data number	reference number	comment	common formula of materials	chemical formula	element name of materials	composition of MA1	element name of materials	composition of MA2	element name of materials	composition of MA3	element name of materials	composition of MA4	element name of materials	composition of MA5	element name of materials	composition of MA6	element name of materials	composition of MA7	element name of materials	composition of MA8	element name of materials	composition of MA9	element name of materials	composition of MA10	oxygen	common formula of oxygen	measured value of Oxygen content	shape	publication year of reference	unit of KAIZERO	temperature independent term in susceptibility	unit of CURIEC	Curie constant	unit of MOMENT	magnetic moment per formula	Curie temperature	Neel temperature	density (gcm-3)	unit of hardness 	hardness at 300 K 	unit of Young's modulus 	Young's modulus at 4.2 K 	Young's modulus at 300 K 	unit of shear modulus 	shear modulus at 4.2 K 	shear modulus at 300 K 	unit of bulk modulus 	unit of bulk modulus at 4.2 K 	unit of bulk modulus at 300 K 	Poisson ratio at 4.2 K 	Poisson ratio at 300 K 	unit of sound velocity 	sound velocity at 4.2 K 	sound velocity at 300 K 	figure number for SV(T) 	*crystal structure, symmetry	common name of structure	space group	international table number	unit of lattice constant	lattice constant a	lattice constant b	lattice constant c	*method of analysis for structure	figure number of structure model	unit of D(L)DT	temperature dependence of LATA	temperature dependence of LATB	temperature dependence of LATC	unit of D(L)DP	pressure dependence of LATA	pressure dependence of LATB	pressure dependence of LATC	comments for structure	unit of Tc	transition temperature (R = 0)	transition temperature (mid point)	transition temperature (R = 100%)	Tc from susceptibility measurement	lowest temperature for measurement (not superconducting)	transition width for resistive transition	Tc (of this sample) recommended	figure number for Tc(p, x, etc)	tc measurement method	unit of DTCDP	slope at P = 0 in Tc vs P plot 	maximum pressure applied	alpha in Tc = A * M^(-alpha), isotope effect	isotope element	exchange ratio of isotope(%)	DTC = Tc - Tc0 for isotope element	volume fraction of Meissner effect(%)	unit of Hc1	method of Hc1 derivation	Hc1 at 0 K for poly crystal	Hc1 at 0 K for single crystal for H //ab-plane	Hc1 at 0 K for single crystal for H //c-axis	Hc1 at given temperature for poly crystal	Hc1 at given temperature for single crystal H//ab-plane	Hc1 at given temperature for single crystal H//c-axis	measuring temperature	unit of Hc2	method of Hc2 derivation	Hc2 at 0 K for poly crystal	Hc2 at 0 K for single crystal for H //ab-plane	Hc2 at 0 K for single crystal for H //c-axis	Hc2 at given temperature for poly crystal	Hc2 at given temperature for single crystal H//ab-plane	Hc2 at given temperature for single crystal H//c-axis	measuring temperature	unit of dHc2/dT	method of dHc2/dT derivation	-slope in Hc2 vs T at Tc for poly crystal	-slope in Hc2 vs T at Tc for single crystal for H //ab-plane	-slope in Hc2 vs T at Tc for single crystal for H //c-axis	figure number for Hirr(T), irreversibility field	difinition or method for Hirr	unit of COHERE	method of COHERE derivation	coherence length at 0 K for poly crystal	coherence length at 0 K for single crystal for H //ab-plane	coherence length at 0 K for single crystal for H ⊥ab-plane	unit of PENET	method of PENET derivation	penetration depth at 0 K for poly crystal	penetration depth at 0 K for single crystal for H //ab-plane	penetration depth at 0 K for single crystal for H⊥ab-plane	unit of energy gap	energy gap at 0 K , delta(0)	normarized energy gap at 0 K , 2delta(0)/kTc	method of measuring energy gap	Jc at 4.2 K, H = 0 T	Jc at T = 77 K, H = 0 T	figure number for Jc(T,H)	graph number of specific heat	unit of SPJUMP	specific heat jump at Tc (delta-C)	unit of GAMMA	coefficient of electronic specific heat	comment for derivation of GAMMA	Debye temperature	method for derivation of Debye temperature	unit of thermal conductivity	thermal conductivity at 300 K	thermal conductivity at 300 K for heat flow//c-axis	thermal conductivity at 300 K for heat flow//ab-plane	graph number for thermal conductivity	unit of thermopower	thermopower at 300 K	thermopower at 300 K for normal to ab-plane	thermopower at 300 K for parallel to ab-plane	graph number for thermopower	unit of resistivity	resistivity at 4.2 K for poly crystal	resistivity at 4.2 K for single crystal for J//ab-plane	resistivity at 4.2 K for single crystal for J//c-axis	resistivity at 77 K for poly crystal	resistivity at 77 K for single crystal for J//ab-plane	resistivity at 77 K for single crystal for J//c-axis	resistivity at normal-T for poly crystal	resistivity at normal-T for single crystal for J//ab-plane	resistivity at normal-T for single crystal for J//c-axis	normal temperature	resistivity at RT for poly crystal	resistivity at RT for single crystal for J//ab-plane	resistivity at RT for single crystal for J//c-axis	unit of RH300	Hall coefficient at 300 K	Hall coefficient at 300 K for single, H//c-axis	Hall coefficient at 300 K for single, H//ab-plane	Hall coefficient for single, H//c-axis	magnetic field for Hall effect	graph number for Hall coefficient	unit of carrier density	carrier density at 300 K	raw materials	*preparation method	preparation comments	preparation method for film	substrate	target material	process comments	title of reference	month of reference	keyword	institute	journal	author	sample	comments
num	refno	commt	name	element	ma1	ma2	mb1	mb2	mc1	mc2	md1	md2	me1	me2	mf1	mf2	mg1	mg2	mh1	mh2	mi1	mi2	mj1	mj2	mo1	mo2	oz	shape	year	ukai	kaizero	ucc	curiec	umoment	moment	curiet	neelt	dens	uhv	hv300	uye	yehe	ye300	ug	ghe	g300	ub	bhe	b300	pohe	po300	usv	svhe	sv300	svfig	str1	str3	spaceg	tblno	ulat	lata	latb	latc	analm	model	udldt	dadt	dbdt	dcdt	udldp	dadp	dbdp	dcdp	strcmt	utc	t1	t2	t3	tcsus	tcn	tcwidth	tc	tcfig	tcmeth	udtcdp	dtcdp	pmax	isotope	isoel	isorat	dtc	vols	uhc1	mhc1	hc1zero	phc1zero	nhc1zero	hc1t	phc1t	nhc1t	tempc1	uhc2	mhc2	hc2zero	phc2zero	nhc2zero	hc2t	phc2t	nhc2t	tempc2	udhc2dt	mdhc2dt	dhc2dt	pdhc2dt	ndhc2dt	hirfig	mhirr	ucohere	mcohere	cohere	pcohere	ncohere	upenet	mpenet	penet	ppenet	npenet	ugap	gap	gapene	gapmeth	jche	jc77	figjc	spheat	ujump	spjump	ugamma	gamma	gamcom	debyet	mdebye	uthc	thc300	thc300n	thc300p	thcfig	utp	tp300	tp300n	tp300p	tpfig	ures	reshe	abreshe	creshe	res77	abres77	cres77	resn	abresn	cresn	nort	resrt	abresrt	cresrt	uhall	rh300	rh300n	rh300p	rhn	field	hallfig	ucarr	carrier	rawmat	method	prepcmt	f_prep	subst	target	pr_commt	title	month	keyword	institute	journal	author	sample	comments
2	JJP0260223		(Ba,La)2CuO4	Ba0.2La1.8Cu1O4-Y	Ba	0.2	La	1.8	Cu	1															O	4-Y			1987																												T																			24	29	32				29																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
3	JJP0260223		(Ba,La,Ag)2CuO4	Ba0.1La1.9Ag0.1Cu0.9O4-Y	Ba	0.1	La	1.9	Ag	0.1	Cu	0.9													O	4-Y			1987																												T																			15	26	32				26																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
4	JJP0260223		(Ba,La,)2CuO4	Ba0.1La1.9Cu1O4-Y	Ba	0.1	La	1.9	Cu	1															O	4-Y			1987																												T																			5	19	30				19																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
5	JJP0260223		(Ba,La)2CuO4	Ba0.15La1.85Cu1O4-Y	Ba	0.15	La	1.85	Cu	1															O	4-Y			1987																												T																			4	22	30				22																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
6	JJP0260223		(Ba,La)2CuO4	Ba0.3La1.7Cu1O4-Y	Ba	0.3	La	1.7	Cu	1															O	4-Y			1987																												T																			5	23	34				23																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
7	JJP0260223		(Ba,La)2CuO4	Ba0.5La1.5Cu1O4-Y	Ba	0.5	La	1.5	Cu	1															O	4-Y			1987																												T																			5	23	35				23																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
8	JJP0260223		(Ba,La)2CuO4	Ba1La1Cu1O4-Y	Ba	1	La	1	Cu	1															O	4-Y			1987																												T																				11	21				11																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
9	JJP0260223		La2CuO4	La2Cu1O4-Y	La	2	Cu	1																	O	4-Y			1987																												T																																																																																																																														Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
10	JJP0260223		(La,Sr)2CuO4	Sr0.05La1.95Cu1O4-Y	Sr	0.05	La	1.95	Cu	1															O	4-Y			1987																												T																																																																																																																														Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
11	JJP0260223		(La,Sr)2CuO4	Sr0.1La1.9Cu1O4-Y	Sr	0.1	La	1.9	Cu	1															O	4-Y			1987																												T																			17.5	33	38				33																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
12	JJP0260223		(La,Sr)2CuO4	Sr0.15La1.85Cu1O4-Y	Sr	0.15	La	1.85	Cu	1															O	4-Y			1987																												T																			30	36	40				36																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
13	JJP0260223		(La,Sr)2CuO4	Sr0.2La1.8Cu1O4-Y	Sr	0.2	La	1.8	Cu	1															O	4-Y			1987																												T																			22	31	38				31																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
14	JJP0260223		(La,Sr)2CuO4	Sr0.3La1.7Cu1O4-Y	Sr	0.3	La	1.7	Cu	1															O	4-Y			1987																												T																			5	33	38				33																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
15	JJP0260223		(La,Ba)2(Cu,Hg)O4	Ba0.3La1.7Hg0.3Cu0.7O4-Y	Ba	0.3	La	1.7	Hg	0.3	Cu	0.7													O	4-Y			1987																												T																			4	26	34				26																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
16	JJP0260223		(La,Ba)2(Cu,Hg)O4	Ba0.3La1.7Hg0.5Cu0.5O4-Y	Ba	0.3	La	1.7	Hg	0.5	Cu	0.5													O	4-Y			1987																												T																																																																																																																														Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
17	JJP0260223		(La,Ba)2(Cu,Ag)O4	Ba0.1La1.9Ag0.05Cu0.95O4-Y	Ba	0.1	La	1.9	Ag	0.05	Cu	0.95													O	4-Y			1987																												T																			11.5	27	35				27																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
18	JJP0260223		(La,Ba)2(Cu,Ag)O4	Ba0.1La1.9Ag0.1Cu0.9O4-Y	Ba	0.1	La	1.9	Ag	0.1	Cu	0.9													O	4-Y			1987																												T																			11.5	27	35				27																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
19	JJP0260223		(La,Ba)2(Cu,Ag)O4	Ba0.1La1.9Ag0.25Cu0.75O4-Y	Ba	0.1	La	1.9	Ag	0.25	Cu	0.75													O	4-Y			1987																												T																			10	26	35				26																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
20	JJP0260223		(La,Ba)2(Cu,Ag)O4	Ba0.1La1.9Ag0.5Cu0.5O4-Y	Ba	0.1	La	1.9	Ag	0.5	Cu	0.5													O	4-Y			1987																												T																			10	27	36				27																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
21	SSC0721203		Y(Ba,Ca)2Cu3O7	Y1Ba1.5Ca0.5Cu3O7-Z	Y	1	Ba	1.5	Ca	0.5	Cu	3													O	7-Z			1989																											3	Y123				3.762	3.894	11.697															82				82																																																																																																					MAGNETIC PROPERTIES OF YBA1.5CA0.5CU3-O7-Z SUPERCONDUCTOR	198912	MICROSTRUCTURE      ,SUSCEPTIBILITY      ,CRITICAL CURRENT    ,GRAINS	DEPARTMENT OF PHYSICS, SAURASHTRA UNIVERSITY, RAJIKOT 360 005,INDIA	SOLID STATE COMMUN.72(1989)1203	G. J. BALDHA,H. H. JOSHI,K. V. RAO,R. G. KULKARNI,S. M. JOSHI,V. SKUMRYEV	Y,BA,CA,CU,O	
22	JJP0260123		(La,Ba)2CuO4	Ba0.15La1.85Cu1O4-Y	Ba	0.15	La	1.85	Cu	1															O	4-Y			1987																												T																			24	30	32				30																																																																																																					High-Tc superconductivity of La-Ba-Cu oxides. II.-Specification of the superconducting phase				Jpn.J.Appl.Phys., 26(1987)L123	H.Takagi,S.Uchida,K.Kitazawa,S.Tanaka		
23	JJP0260151		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4			1987																												T																			26	30	32				30																																																																														6																							High-Tc superconductivity of La-Ba-Cu oxides. III. Electrical resistivity measurement				Jpn.J.Appl.Phys., 26(1987)L151	S.Uchida,H.Takagi,K.Kitazawa,S.Tanaka		
24	JJP0260196		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																					39				39																																2																																																																					High-Tc superconductivity of La-Ba(Sr)-Cu oxides. IV Critical magnetic fields				Jpn.J.Appl.Phys., 26(1987)L196	S.Uchida,H.Takagi,S.Tanaka,K.Nakao,N.Miura,K.Kishio,K.Kitazawa,K.Fueki		
36	CL19870547		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4-Y	La	1.95	Sr	0.05	Cu	1															O	4-Y			1987																												T				3.794		13.211															14.8				14.8																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
37	CL19870547		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4-Y	La	1.9	Sr	0.1	Cu	1															O	4-Y			1987																												T				3.786		13.221															30				30																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
38	CL19870547		(La,Sr)2CuO4	La1.775Sr0.225Cu1O4-Y	La	1.775	Sr	0.225	Cu	1															O	4-Y			1987																												T				3.771		13.254															35.5				35.5																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
39	CL19870547		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4-Y	La	1.75	Sr	0.25	Cu	1															O	4-Y			1987																												T				3.774		13.267															23.3				23.3																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
40	CL19870547		(La,Sr)2CuO4	La1.7Sr0.3Cu1O4-Y	La	1.7	Sr	0.3	Cu	1															O	4-Y			1987																												T				3.774		13.246															18.2				18.2																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
41	CL19870547		(La,Sr)2CuO4	La1.65Sr0.35Cu1O4-Y	La	1.65	Sr	0.35	Cu	1															O	4-Y			1987																												T				3.771		13.258															18.3				18.3																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
42	CL19870547		(La,Sr)2CuO4	La1.6Sr0.4Cu1O4-Y	La	1.6	Sr	0.4	Cu	1															O	4-Y			1987																												T				3.769		13.257															18.3				18.3																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
43	CL19870547		(La,Sr)2CuO4	La1.825Sr0.175Cu1O4-Y	La	1.825	Sr	0.175	Cu	1															O	4-Y			1987																												T				3.778		13.243															37.5				37.5																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
44	CL19870429		(La,Sr)2CuO4	La1.85Ca0.15Cu1O4-Y	La	1.85	Ca	0.15	Cu	1															O	4-Y			1987																												T																			18	20	24				20																																																																																																					New High Temperature Superconducting Oxides. (La1-xSrx)2CuO4-d and (La1-xCax)2CuO4-d			Department of Industrial Chemistry, University of Tokyo, Japan	Chem.Lett., 16(1987)429	K.Kishio,K.Kitazawa,S.Kanbe,I.Yasuda,N.Sugii,H.Takagi,S.Uchida,K.Fueki,S.Tanaka		
47	JJP0260325			Yb16Ba1Cu2Oz	Yb	16	Ba	1	Cu	2															O	z			1987																																															26.7	76.9	89.9				76.9																																																																														600																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
48	JJP0260325			Yb1.8Ba0.2Cu1Oz	Yb	1.8	Ba	0.2	Cu	1															O	z			1987																																															44.3	65.3	89.4				65.3																																																																														430																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
49	JJP0260325			Yb6Ba1Cu1Oz	Yb	6	Ba	1	Cu	1															O	z			1987																																															48.6	78.6	89				78.6																																																																														370																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
50	JJP0260325			Yb1.62La0.18Ba0.18Sr0.02Cu1Oz	Yb	1.62	La	0.18	Ba	0.18	Sr	0.02	Cu	1											O	z			1987																																															59.9	79.3	89				79.3																																																																														420																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
51	JJP0260608			Y0.4Ba0.6Cu1OX	Y	0.4	Ba	0.6	Cu	1															O	X			1987																																5.51		5.472													88	90	91				90																																																																																																					MEISSNER EFFECT AND RESISTIVITY OF THE  SUPERCONDUCTING Y-BA-CU-O SYSTEM				JJAP.LETT.,26(1987)L608	I.NAKADA,K.ASAYAMA,T.KOHARA,Y.ODA	Y,BA,CU,O	
52	JJP0260601			Y0.4Ba0.6Cu1OX	Y	0.4	Ba	0.6	Cu	1															O	X			1987																																															87		94				90.5																																																																														2.2				5.2																			BULK SUPERCONDUCTIVITY OF Y-BA-CU-O AND ER-BA-CU-O				JJAP.LETT.,26(1987)L601	H.ISHII,H.SATO,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,S.TANAKA,S.UCHIDA	M,BA,CU,O	
53	JJP0260601			Er0.5Ba0.5Cu1OX	Er	0.5	Ba	0.5	Cu	1															O	X			1987																																															90		94				92																																																																														2.6				5.3																			BULK SUPERCONDUCTIVITY OF Y-BA-CU-O AND ER-BA-CU-O				JJAP.LETT.,26(1987)L601	H.ISHII,H.SATO,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,S.TANAKA,S.UCHIDA	M,BA,CU,O	
54	JJP0260613			Tm0.35Ba0.65Cu1OX	Tm	0.35	Ba	0.65	Cu	1															O	X			1987																																															93	93.2	100				93.2																																																																																																					HIGH TC SUPERCONDUCTIVITY IN TM-BA-CU-O SYSTEM				JJAP.LETT.,26(1987)L613	H.KOINUMA,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,M.AOKI,S.KANBE,S.TANAKA,S.UCHIDA,T.HASEGAWA,T.NAKAMURA	TM,BA,CU,O	
55	JJP0260613			Tm0.3Ba0.7Cu1OX	Tm	0.3	Ba	0.7	Cu	1															O	X			1987																																3.89	3.81	11.68														94.4	96.6				94.4																																																																																																					HIGH TC SUPERCONDUCTIVITY IN TM-BA-CU-O SYSTEM				JJAP.LETT.,26(1987)L613	H.KOINUMA,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,M.AOKI,S.KANBE,S.TANAKA,S.UCHIDA,T.HASEGAWA,T.NAKAMURA	TM,BA,CU,O	
56	JJP0260613			Tm0.25Ba0.75Cu1OX	Tm	0.25	Ba	0.75	Cu	1															O	X			1987																																3.89	3.81	11.68													86	93.2	97				93.2																																																																																																					HIGH TC SUPERCONDUCTIVITY IN TM-BA-CU-O SYSTEM				JJAP.LETT.,26(1987)L613	H.KOINUMA,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,M.AOKI,S.KANBE,S.TANAKA,S.UCHIDA,T.HASEGAWA,T.NAKAMURA	TM,BA,CU,O	
57	JJP0260613			Tm0.2Ba0.8Cu1OX	Tm	0.2	Ba	0.8	Cu	1															O	X			1987																																3.89	3.81	11.68													68.6	80.5	97.5				80.5																																																																																																					HIGH TC SUPERCONDUCTIVITY IN TM-BA-CU-O SYSTEM				JJAP.LETT.,26(1987)L613	H.KOINUMA,H.TAKAGI,K.FUEKI,K.KISHIO,K.KITAZAWA,M.AOKI,S.KANBE,S.TANAKA,S.UCHIDA,T.HASEGAWA,T.NAKAMURA	TM,BA,CU,O	
58	JJP0260615			La2Ba4Cu6O14+X	La	2	Ba	4	Cu	6															O	14+X			1987																											3					5.545		11.73													40	48	55				48																																0.6																																																																					OXYGEN-DEFECT PEROVSKITE STRUCTURE WITH SUPERCONDUCTING TC ABOVE 50K IN LA-BA-CU-O COMPOUND SYSTEM				JJAP.LETT.,26(1987)L615	K.SEMBA,M.HIKITA,S.KURIHARA,S.TSURUMI,T.IWATA	LA,BA,CU,O	
59	JJP0260619		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.824	3.889	11.687													86		94				90																																																																														2				3.2																			X-RAY AND ELECTRON-MICROSCOPIC STUDIES  ON SINGLE-PHASE HIGH TC SUPERCONDUCTOR, Y(1)BA(2)CU(3)O(Z)				JJAP.LETT.,26(1987)L619	E.TAKAYAMA-MUROMACHI,K.KATO,Y.MATSUI,Y.UCHIDA	Y,BA,CU,O	
60	JJP0260624		Y(Y,Ba)2Cu3O7	Y1.6Ba2.4Cu3O10-X	Y	1.6	Ba	2.4	Cu	3															O	10-X			1987																												Y123																			78	90	93				90																																																																																																					SUPERCONDUCTIVITY ABOVE 90K IN Y-BA-CU-O COMPOUNDS AND THEIR CRITICAL CURRENT DENSITIES AT 77K				JJAP.LETT.,26(1987)L624	A.INOUE,H.KIMURA,K.MATSUZAKI,K.MOROISHI,T.MASUMOTO	Y,BA,CU,O	
61	JJP0260624		Y(Y,Ba)2Cu3O7	Y1.2Ba1.8Cu2O7-X	Y	1.2	Ba	1.8	Cu	2															O	7-X			1987																											3	Y123																			85	92	94				92																																																																																																					SUPERCONDUCTIVITY ABOVE 90K IN Y-BA-CU-O COMPOUNDS AND THEIR CRITICAL CURRENT DENSITIES AT 77K				JJAP.LETT.,26(1987)L624	A.INOUE,H.KIMURA,K.MATSUZAKI,K.MOROISHI,T.MASUMOTO	Y,BA,CU,O	
62	JJP0260624			Y0.8Ba1.2Cu1O4-X	Y	0.8	Ba	1.2	Cu	1															O	4-X			1987																											3																					80	92				80																																																																																																					SUPERCONDUCTIVITY ABOVE 90K IN Y-BA-CU-O COMPOUNDS AND THEIR CRITICAL CURRENT DENSITIES AT 77K				JJAP.LETT.,26(1987)L624	A.INOUE,H.KIMURA,K.MATSUZAKI,K.MOROISHI,T.MASUMOTO	Y,BA,CU,O	
63	JJP0260633			La0.4Ba0.6Cu1O3-X	La	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																																																																																																																															SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
64	JJP0260633			Pr0.4Ba0.6Cu1O3-X	Pr	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																																																																																																																															SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
65	JJP0260633			Nd0.4Ba0.6Cu1OX	Nd	0.4	Ba	0.6	Cu	1															O	X			1987																											3																					85	93				85																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
66	JJP0260633			Eu0.4Ba0.6Cu1O3-X	Eu	0.4	Ba	0.6	Cu	1															O	3-X			1987																																																8	16				8																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
67	JJP0260633			Gd0.4Ba0.6Cu1O3-X	Gd	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					13	27				13																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
68	JJP0260633			Dy0.4Ba0.6Cu1O3-X	Dy	0.4	Ba	0.6	Cu	1															O	3-X			1987																																																91	94				91																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
69	JJP0260633			Ho0.4Ba0.6Cu1O3-X	Ho	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					94	95				94																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
70	JJP0260633			Er0.4Ba0.6Cu1O3-X	Er	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					93	95				93																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
71	JJP0260633			Tm0.4Ba0.6Cu1O3-X	Tm	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					93	96				93																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
72	JJP0260633			Lu0.4Ba0.6Cu1O3-X	Lu	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					91	94				91																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
73	JJP0260642		LaBa2Cu3O7	La1Ba2Cu3OX	La	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.923		11.78																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
74	JJP0260642			Pr2Ba3Cu5OX	Pr	2	Ba	3	Cu	5															O	X			1987																											3					3.904		11.716																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
75	JJP0260642			Nd2Ba3Cu5OX	Nd	2	Ba	3	Cu	5															O	X			1987																																3.891		11.678													2.8	18	40				18																																																																																																					HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
76	JJP0260642		SmBa2Cu3O7	Sm1Ba2Cu3OX	Sm	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.901		11.81													24	43	54				43																																																																																																					HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
77	JJP0260642			Eu2Ba3Cu5OX	Eu	2	Ba	3	Cu	5															O	X			1987																																3.861	3.896	11.688																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
78	JJP0260642			Gd2Ba3Cu5OX	Gd	2	Ba	3	Cu	5															O	X			1987																											3					3.852	3.9	11.701													28.6	40	51				40																																																																																																					HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
79	JJP0260642			Dy2Ba3Cu5OX	Dy	2	Ba	3	Cu	5															O	X			1987																											3					3.879		11.679																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
80	JJP0260642		TmBa2Cu3O7	Tm1Ba2Cu3OX	Tm	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.823	3.892	11.674																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
81	JJP0260642		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.829	3.888	11.667																																																																																																																								HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
82	JJP0260642		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																											3	Y123																			48		92				70																																																																																																					HIGH TC SUPERCONDUCTIVITY IN NEW OXIDE  SYSTEMS AND THEIR X-RAY DIFFRACTION STUDY				JJAP.LETT.,26(1987)L642	M.ONODA,M.SATO,S.HOSOYA,S.SHAMOTO		
83	JJP0260645	strong c-axis orientation. surface oxidized by glow discharge and Pb-film-electrode. gap  by tunneling. Tc = 48 K after sample treatments	YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123				3.883	3.822	11.69												K	90						90																																																10.5	1																																																				TUNNELING SPECTROSCOPY OF Y-BA-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L645	A.SUGISHITA,E.YAMAKA,H.WATANABE,I.IGUCHI,T.MOCHIKU,Y.KASAI	Y,BA,CU,O	
85	JJP0260649			Y0.3Ba0.7Cu1O3-X	Y	0.3	Ba	0.7	Cu	1															O	3-X			1987																											3																					95.5					95.5																																																																																																					RIETVELD REFINEMENT OF THE STRUCTURE OF BA(2)Y(1)CU(3)O(7-Z) WITH NEUTRON POWDER DIFFRACTION DATA				JJAP.LETT.,26(1987)L649	E.TAKAYAMA-MUROMACHI,F.IZUMI,H.ASANO,N.WATANABE,T.ISHIGAKI,T.NISHIKAWA,Y.UCHIDA	Y,BA,CU,O	
86	JJP0260657			Y0.8Ba1.2Cu1OX	Y	0.8	Ba	1.2	Cu	1															O	X			1987																											3																					94					94																																																																																																					ELECTRICAL RESISTIVITY, CRITICAL CURRENTAND CRYSTAL ORIENTATION OF THE SINTERED Y-BA-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L657	A.SUGISHITAI.IGUCHI,E.YAMAKA,H.WATANABE,T.MOCHIKU,Y.KASAI	Y,BA,CU,O	
87	JJP0260657			Y0.6Ba0.9Cu1OX	Y	0.6	Ba	0.9	Cu	1															O	X			1987																																															75	88	98				88																																																																																																					ELECTRICAL RESISTIVITY, CRITICAL CURRENTAND CRYSTAL ORIENTATION OF THE SINTERED Y-BA-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L657	A.SUGISHITAI.IGUCHI,E.YAMAKA,H.WATANABE,T.MOCHIKU,Y.KASAI	Y,BA,CU,O	
88	JJP0260223			Ba0.3La1.7Hg0.15Cu0.85O4-Y	Ba	0.3	La	1.7	Hg	0.15	Cu	0.85													O	4-Y			1987																																															22	28	32				28																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
89	JJP0260223			Ba0.3La1.7Hg0.15Cu0.85O4-Y	Ba	0.3	La	1.7	Hg	0.15	Cu	0.85													O	4-Y			1987																																															10	28	36				28																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
93	CL19870547		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T				3.782		13.229														35.5	36				35.5																																																																																																					Superconductivity and lattice parameters in (La1-xSrx)2CuO4-d solid solution system				Chem.Lett., No.3 (1987)547-550	S.Kanbe,K.Kishio,K.Kitazawa,K.Fueki,H.Takagi,S.Tanaka		
94	JJP0260325			Yb1.6La0.2Ba0.2Cu1Oz	Yb	1.6	La	0.2	Ba	0.2	Cu	1													O	z			1987																											3																				53.5	79.2	88.9				79.2																																																																														780																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
95	JJP0260223		(La,Sr)2CuO4	Sr0.35La1.65Cu1O4-Y	Sr	0.35	La	1.65	Cu	1															O	4-Y			1987																												T																				26	32				26																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
97	JJP0260624			Y0.4Ba0.6Cu1OX	Y	0.4	Ba	0.6	Cu	1															O	X			1987																																3.818	3.888	11.667													90	92	93				92																																																																																																					SUPERCONDUCTIVITY ABOVE 90K IN Y-BA-CU-O COMPOUNDS AND THEIR CRITICAL CURRENT DENSITIES AT 77K				JJAP.LETT.,26(1987)L624	A.INOUE,H.KIMURA,K.MATSUZAKI,K.MOROISHI,T.MASUMOTO	Y,BA,CU,O	
98	JJP0260633			Yb0.4Ba0.6Cu1O3-X	Yb	0.4	Ba	0.6	Cu	1															O	3-X			1987																											3																					88	92				88																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
99	JJP0260325			Lu1.8Ba0.2Cu1O4	Lu	1.8	Ba	0.2	Cu	1															O	4			1987																											3																				43	71.9	89				71.9																																																																														4.2																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
100	JJP0260325			Y0.9Ba0.1Cu1O4	Y	0.9	Ba	0.1	Cu	1															O	4			1987																											3																				50	81	92.5				81																																																																														0.7																							High-Tc superconductivity in new oxide systems					S.Hosoya,S.Shamoto,M.Onoda,M.Sato		
105	APL0500543		(La,Ba)2CuO4	Ba0.15La1.85Cu1O4	Ba	0.15	La	1.85	Cu	1															O	4			1987																												T																			21.5	28	34				28																																																																																																					Upper critical fields and high superconducting transition temperatures of La1.85Sr0.15CuO4 and La1.85Ba0.15CuO4				Appl.Phys.Lett., 50(1987)543	D.W.Capone II,D.G.Hinks,J.D.Jorgensen,K.Zhang		
106	APL0500543		(La,Sr)2CuO4	Sr0.15La1.85Cu1O4	Sr	0.15	La	1.85	Cu	1															O	4			1987																												T																			30	34.7	36.7				34.7																																																																																																					Upper critical fields and high superconducting transition temperatures of La1.85Sr0.15CuO4 and La1.85Ba0.15CuO4				Appl.Phys.Lett., 50(1987)543	D.W.Capone II,D.G.Hinks,J.D.Jorgensen,K.Zhang		
108	JJP0260337		(La,Sr)2(Cu,Ti)O4	Sr0.2La1.8Cu0.95Ti0.05O4	Sr	0.2	La	1.8	Cu	0.95	Ti	0.05													O	4			1987																												T																					21				21																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
109	JJP0260337		(La,Sr)2(Cu,V)O4	Sr0.2La1.8Cu0.99V0.01O4	Sr	0.2	La	1.8	Cu	0.99	V	0.01													O	4			1987																												T																					12				12																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
110	JJP0260337		(La,Sr)2(Cu,Cr)O4	Sr0.2La1.8Cu0.99Cr0.01O4	Sr	0.2	La	1.8	Cu	0.99	Cr	0.01													O	4			1987																												T																					22				22																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
111	JJP0260337		(La,Sr)2(Cu,Mn)O4	Sr0.2La1.8Cu0.98Mn0.02O4	Sr	0.2	La	1.8	Cu	0.98	Mn	0.02													O	4			1987																												T																					32				32																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
112	JJP0260337		(La,Sr)2(Cu,Fe)O4	Sr0.2La1.8Cu0.95Fe0.05O4	Sr	0.2	La	1.8	Cu	0.95	Fe	0.05													O	4			1987																												T																					30				30																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
113	JJP0260337		(La,Sr)2(Cu,Co)O4	Sr0.2La1.8Cu0.95Co0.05O4	Sr	0.2	La	1.8	Cu	0.95	Co	0.05													O	4			1987																												T																					16				16																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
114	JJP0260337		(La,Sr)2(Cu,Ni)O4	Sr0.2La1.8Cu0.95Ni0.05O4	Sr	0.2	La	1.8	Cu	0.95	Ni	0.05													O	4			1987																												T																					21				21																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
115	JJP0260337		(La,Sr)2(Cu,Zn)O4	Sr0.2La1.8Cu0.99Zn0.01O4	Sr	0.2	La	1.8	Cu	0.99	Zn	0.01													O	4			1987																												T																					29				29																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
116	JJP0260337		(La,Pr,Sr)2CuO4	Pr0.1La1.7Sr0.2Cu1O4	Pr	0.1	La	1.7	Sr	0.2	Cu	1													O	4			1987																												T																					36				36																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
117	JJP0260337		(La,Nd,Sr)2CuO4	Nd0.1La1.7Sr0.2Cu1O4	Nd	0.1	La	1.7	Sr	0.2	Cu	1													O	4			1987																												T																					35				35																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
118	JJP0260337		(La,Sm,Sr)2CuO4	Sm0.1La1.7Sr0.2Cu1O4	Sm	0.1	La	1.7	Sr	0.2	Cu	1													O	4			1987																												T																					32				32																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
119	JJP0260337		(La,Gd,Sr)2CuO4	Gd0.1La1.7Sr0.2Cu1O4	Gd	0.1	La	1.7	Sr	0.2	Cu	1													O	4			1987																												T																					30				30																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
120	PRB0363923		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7			1987																												Y123																				51					51																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
121	PRB0363923		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7			1987																											3	Y123																				33					33																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
122	PRB0363923		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7			1987																											3	Y123				3.822	3.891	11.67														82					82																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
123	PRB0363923		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O7	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7			1987																											3	Y123																				60					60																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
124	PRB0363923		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7			1987																												Y123																				54					54																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
125	PRB0363923		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																											3	Y123				3.822	3.891	11.67														90					90																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
126	PRB0363923		YBa2Cu3(O,S)7	Y1Ba2Cu3S1O6	Y	1	Ba	2	Cu	3	S	1													O	6			1987																												Y123				3.855	3.919	11.75														90					90																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
127	PRB0363923		Yba2Cu3(O,Cl)7	Y1Ba2Cu3Cl1O6	Y	1	Ba	2	Cu	3	Cl	1													O	6			1987																											3	Y123																				72					72																																																																																																					EFFECTS OF SUBSTITUTION OF O BY S AND CU BY FE ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7)	198709	SUSCEPTIBILITY           ,TC	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM,ISRAEL	PHYS.REV.B,36(1987)3923	I.FELNER,I.NOWIK,Y.YESHURUN	Y,BA,CU,O	
128	PRB0363920		YBa2Cu3O7	Y1Ba2Cu3O7+Y	Y	1	Ba	2	Cu	3															O	7+Y			1987																											3	Y123				3.821	3.885	11.676														92					92																																																																																																					Twins and oriented domains in the orthorhombic superconductor YBa2Cu3O7+-e	1987		Laboratoire de Cristallographie et Sciences des Materiaux, Institut des Sciences de la Matiere et du Rayonnement, Campus 2, Boulevard du Marechal Juin, Universite de Caen, 14032 Caen Cedex, France	Phys.Rev.B.,36(1987)3920	B. Domenges,B. Raveau,C. Michel,G. Heger,J. Provost,M. Hervieu		
129	PRB0363917		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																											3	Y123																			86		100				93																																																																														11				19																			THERMAL CONDUCTIVITY OF SUPERCONDUCTIVE Y-BA-CU-O	198709	THERMAL CONDUCTIVITY	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,36(1987)3917	D.E.SWETS,D.T.MORELLI,J.HEREMANS	Y,BA,CU,O	
130	PRB0363913		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																											3	Y123																				92					92																																																									40										3.24			TP130								0.35																							NORMAL-STATE PROPERTIES OF A(1)BA(2)CU(3)O(7-Y) COMPOUNDS(A=Y AND GD):ELECTRON-ELECTRON CORRELATIONS	198709	THERMOPOWER              ,HALL EFFECT	PHYSICS DIVISION,LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)3913	D.E.PETERSON,E.ZIRNGIEBL,G.GRUNER,G.L.WELLS,J.D.THOMPSON,J.R.COOPER,R.B.SCHWARZ,R.S.KWOK,S-W.CHEONG,S.E.BROWN,Z.FISK	R,BA,CU,O	
131	PRB0363913		GdBa2Cu3O7	Gd1Ba2Cu3O7-Y	Gd	1	Ba	2	Cu	3															O	7-Y			1987																											3	Y123																				94.5					94.5																																																																			6.46			TP131								0.2													RH131										NORMAL-STATE PROPERTIES OF A(1)BA(2)CU(3)O(7-Y) COMPOUNDS(A=Y AND GD):ELECTRON-ELECTRON CORRELATIONS	198709	THERMOPOWER              ,HALL EFFECT	PHYSICS DIVISION,LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)3913	D.E.PETERSON,E.ZIRNGIEBL,G.GRUNER,G.L.WELLS,J.D.THOMPSON,J.R.COOPER,R.B.SCHWARZ,R.S.KWOK,S-W.CHEONG,S.E.BROWN,Z.FISK	R,BA,CU,O	
132	PRB0364011		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																												T																																																																																																																														Low-field magnetic relaxation effects in high-Tc superconductors Sr-La-Cu-O and Ba-La-Cu-O	198709		Laboratorium Fur Festkorperphysik, Eidgenossische Technische Hochschule-Honggerberg, CH-8093 Zurich, Swizerland	Phys.Rev.B,36(1987)4011	A. Pollini,A.C. Mota,J.G. Bednorz,K.A. Muller,P. Visani		
133	PRB0364003		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				36					36																																																																																																					Critical fields and the critical current density of La1.85Sr0.15CuO4	1987		Laboratoire de Physique des Solides Universite de Paris-Sud, Batiment 510, 91405 Orsay Cedex, France	Phys.Rev.B.,36(1987)4003	G. Collin,M. Oussena,M. Ribault,S. Senoussi		
134	PRB0363990	78.8%BA(135),DTC=0.1,ALPHA=0.0+-0.1(RES)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123																			91	91.85	92				91.85																																																																																																					Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity	198709		Department of Physics, University of California, Berkeley, California 94720	Phys.Rev.B,36(1987)3990	A. Zettl,L.C. Bourne,Marvin L. Cohen,T.W. Barbee III		
135	PRB0363990	99.7%BA(138)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123																			91	91.95	92.2				91.95																																																																																																					Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity	198709		Department of Physics, University of California, Berkeley, California 94720	Phys.Rev.B,36(1987)3990	A. Zettl,L.C. Bourne,Marvin L. Cohen,T.W. Barbee III		
136	PRB0363990	99.7%CU(63),DTC=0.2,ALPHA=0.0+-0.07(RES)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																											3	Y123																			87	89.7	91				89.7																																	0.01																																																																				Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity	198709		Department of Physics, University of California, Berkeley, California 94720	Phys.Rev.B,36(1987)3990	A. Zettl,L.C. Bourne,Marvin L. Cohen,T.W. Barbee III		
137	PRB0363990	99.6%CU(65)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																											3	Y123																			87	89.9	91.2				89.9																																																																																																					Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity	198709		Department of Physics, University of California, Berkeley, California 94720	Phys.Rev.B,36(1987)3990	A. Zettl,L.C. Bourne,Marvin L. Cohen,T.W. Barbee III		
138	JPC0200669		HoBa2Cu3O7	Ho1Ba2Cu3O8-X	Ho	1	Ba	2	Cu	3															O	8-X			1987						7.9																					3	Y123																			80		90				85																																																																														15																							SUPERCONDUCTIVITY IN Y(0.1)GD(0.9)BA(2)CU(3)O(8-Z) AND HO(1)BA(2)CU(3)O(8-Z) SYSTEMS	198710	RESISTIVITY              ,TC                       ,MAGNETIZ	SAHA INSTITUTE OF NUCLEAR PHYSICS,CALCUTTA,INDIA	J.PHYS.C,20(1987)669	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	Y,GD,BA,CU,O,HO,BA,CU,O	
139	JPC0200669		(Y,Gd)Ba2Cu3O7	Y0.1Gd0.9Ba2Cu3O8-X	Y	0.1	Gd	0.9	Ba	2	Cu	3													O	8-X			1987						5.26																					3	Y123																			89		92				90.5																																																																														2																							SUPERCONDUCTIVITY IN Y(0.1)GD(0.9)BA(2)CU(3)O(8-Z) AND HO(1)BA(2)CU(3)O(8-Z) SYSTEMS	198710	RESISTIVITY              ,TC                       ,MAGNETIZ	SAHA INSTITUTE OF NUCLEAR PHYSICS,CALCUTTA,INDIA	J.PHYS.C,20(1987)669	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	Y,GD,BA,CU,O,HO,BA,CU,O	
140	JPC0200673		ErBa2Cu3O7	Er1Ba2Cu3O7-X	Er	1	Ba	2	Cu	3															O	7-X			1987																											3	Y123																			260	275	285				275																																																																																																					EVIDENCE FOR TRANSIENT SUPERCONDUCTIVITY NEAR 260 K	198710	RESISTIVITY              ,SUSCEPTIBILITY	TATA INSTITUTE OF FUNDAMENTAL RESEARCH,HOMI BHABHA ROAD,BOMBAY,INDIA	J.PHYS.C,20(1987)673	A.K.RAJARAJAN,L.C.GUPTA,M.S.MULTANI,P.AYYUB,P.GUPTASARMA,R.VIJAYARAGHAVAN	ER,BA,CU,O	
141	PRL0591468		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																												Y123																					130				130																																																																														40																							IMPROVED HIGH-TC SUPERCONDUCTORS	198709	RESISTIVITY              ,PREPARATION	PHILIPS LABORATORIES,NORTH AMERICAN PHILIPS CORPORATION,BRIARCLIFF MANOR,NEW YORK	PHYS.REV.LETT.,59(1987)1468	R.N.BHARGAVA,S.P.HERKO,W.N.OSBORNE	Y,BA,CU,O,F	
142	PRL0591160		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																											3	Y123				3.83	3.89	11.71														88.8					88.8																																2.3	0.71																																																																				ANISOTROPIC NATURE OF HIGH-TEMPERATURE SUPERCONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-X)	198709	HC                       ,ANISOTROPY               ,SINGLE C	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.LETT.,59(1987)1160	T.K.WORTHINGTON,T.R.DINGER,W.J.GALLAGHER	Y,BA,CU,O	
143	PRL0591329		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1987																												T																																																																																																																														SOFT-PHONON BEHAVIOR AND TRANSPORT IN SINGLE-CRYSTAL LA(2)CU(1)O(4)	198709	STRUCTURE                ,PHONON                   ,RESISTIV	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,MASSACHUSETTS INSTITUTE OF TECHNOLOGY,CAMBRIDGE,MASSACHUSETTS	PHYS.REV.LETT.,59(1987)1329	C.J.PETERS,C.Y.CHEN,D.R.GABBE,G.SHIRANE,H.L.TULLER,H.P.JENSSEN,J.D.AXE,M.A.KASTNER,P.BONI,P.J.PICONE,R.J.BIRGENEAU,T.R.THURSTON,TINEKE THIO	LA,CU,O	
144	JPF0170261		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																												Y123																			84	90	92				90																																																																																																					ULTRASONIC ATTENUATION IN THE HIGH-TC SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z)	198710	SOUND VELOCITY           ,PHONON	SCHOOLS OF MATERIALS SCIENCE AND PHYSICS,UNIVERSITY OF BATH,CLAVERTON DOWN,BATH,UK	J.PHYS.F,17(1987)261	D.P.ALMOND,E.F.LAMBSON,G.A.SAUNDERS,WANG HONG	Y,BA,CU,O	
145	JPF0170243		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																											3	Y123																			85.5						85.5																																																																																																					Ultrasonic investigation of lattice instability and superconductivivty in high-Tc systems			Center of Theoretical Physics, CCAST (World Lab.), Beijing, China and Physics Department, Tsinghua University, Beijing, China	J.Phys.F:Met.Phys.17(1987)L243-L248	Chen Haoming,He Yusheng,Lin Sihan,Lou Yongming,Xiang Jiong,Zhang Baiwen		
146	JPF0170243			Y3Ba5Cu4Nb1O18-X	Y	3	Ba	5	Cu	4	Nb	1													O	18-X			1987																											3																				77.3						77.3																																																																																																					Ultrasonic investigation of lattice instability and superconductivivty in high-Tc systems			Center of Theoretical Physics, CCAST (World Lab.), Beijing, China and Physics Department, Tsinghua University, Beijing, China	J.Phys.F:Met.Phys.17(1987)L243-L248	Chen Haoming,He Yusheng,Lin Sihan,Lou Yongming,Xiang Jiong,Zhang Baiwen		
147	PRL0591768		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																											3	Y123																				90					90																																																																														0.18								-0.75			-0.9												MEASUREMENT OF ANISOTROPIC RESISTIVITY AND HALL CONSTANT FOR SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-X)	198710	SINGLE CRYSTAL           ,HALL EFFECT              ,RESISTIVITY              ,AN	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.LETT.,59(1987)1768	A.W.KLEINSASSER,D.KAISER,F.HOLTZBERG,S.W.TOZER,T.PENNEY	Y,BA,CU,O	
148	SSC0631125			Sm0.45Ba0.55Cu1O3-Y	Sm	0.45	Ba	0.55	Cu	1															O	3-Y			1987																											3																				56	69	85.5				69																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
149	SSC0631125			Sm0.4Ba0.6Cu1O3-Y	Sm	0.4	Ba	0.6	Cu	1															O	3-Y			1987																											3																				78.9	84.3	92.8				84.3																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
150	SSC0631125			Sm0.33Ba0.67Cu1O7-X	Sm	0.33	Ba	0.67	Cu	1															O	7-X			1987																																															80.3	86.4	94.8				86.4																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
151	SSC0631125			Sm0.3Ba0.7Cu1O3-Y	Sm	0.3	Ba	0.7	Cu	1															O	3-Y			1987																											3																				79.8	88.8	96.5				88.8																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
152	SSC0631125			Sm0.25Ba0.75Cu1O3-Y	Sm	0.25	Ba	0.75	Cu	1															O	3-Y			1987																											3																				63.4	73.6	89.1				73.6																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
153	SSC0631125			Sm0.2Ba0.8Cu1O3-Y	Sm	0.2	Ba	0.8	Cu	1															O	3-Y			1987																																															41.3	62.5	89.9				62.5																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
154	SSC0631125			Sm0.35Ba0.65Cu1O3-Y	Sm	0.35	Ba	0.65	Cu	1															O	3-Y			1987																											3					3.976	3.998	11.996													90.8	93.1	96.7				93.1																																																																																																					THE HIGH-TC SUPERCONDUCTIVITY IN SM(X)BA(1-X)CU(1)O(3-Y) COMPOUND SYSTEM	198710	RESISTIVITY              ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1125	CAO NING,CHANG YINGCHUAN,CHEN XICHEN,DUAN ZHANGRO,FAN HUI,GUAN WEIYAN,HOU DESEN,LIU JINXIANG,RAN QIZE,SHAO XIUYU,ZHENG JIAQI		
155	SSC0631149		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																											3	Y123				3.817	3.883	11.633														90					90																																																																																																					STRUCTURE OF THE HIGH-TEMPERATURE SUPERCONDUCTOR BA(2)Y(1)CU(3)O(7) BY X-RAY AND NEUTRON POWDER DIFFRACTION	198710	STRUCTURE                ,NEUTRON DIFFRA	LABORATOIRE DE CRISTALLOGRAPHIE AUX RAYONS-X,24 QUAI ERNST ANSERMET,UNIVERSITE DE GENEVE,GENEVE,SWITZERLAND	SOLID STATE COMMUN.,63(1987)1149	E.WALKER,J.-L.JORDA,K.YVON,M.FRANCOIS,P.FISHER		
156	SSC0631129		YBa2Cu3O7	Y1Ba2Cu3O9-X	Y	1	Ba	2	Cu	3															O	9-X			1987																											3					3.818	3.889	11.694													92						92																																																																																																					MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR Y(1)BA(2)CU(3)O(9-X)	198710	MAGNETIZATION	DEPARTMENT OF PHYSICS AND INSTITUTE OF SOLID STATE PHYSICS,PEKING UNIVERSITY,BEIJING,CHINA	SOLID STATE COMMUN.,63(1987)1129	CHIN LIN,CHONG-DE WEI,CUO LU,GUO-ZHONG LI,JIAN LAN,SUN-QI FENG,YUN-XI SUN,ZI-ZHAO GAN,ZUN-XIAO LIU		
157	JPC0200659		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																												T																																																																																																																														EVIDENCE FOR PEROXIDE AND CU1+ SPECIES IN LA1.8SR0.2CUO4 FROMPHOTO-EMISSION STUDIES				J.PHYS.C,20(1987)659	C N R RAO,D D SARMA	LA,SR,CU,O	
158	ZPS0680421			Bi2Sr2Cu2O7+Z	Bi	2	Sr	2	Cu	2															O	7+Z			1987																											3					5.32	26.6	48.8													14	22	27				22																																																																																		25																			SUPERCONDUCTIVITY IN THE BI-SR-CU-O SYSTEM		RESISTIVITY              ,PREPARATION	LABORATOIRE DE CRISTALLOGRAPHIE ET SCIENCES DES MATERIAUX,ISMRA,UNIVERSITE DE CAEN,FRANCE	Z.PHYS.B:CONDENSED MATTER,68(1987)421	A.GRANDIN,B.RAVEAU,C.MICHEL,F.DESLANDES,J.PROVOST,M.HERVIEU,M.M.BOREL	BI,SR,CU,O	
159	JJP0262080			Bi1Sr1Cu1OY	Bi	1	Sr	1	Cu	1															O	Y			1987																											2					5.38	5.38	24.6													4.7	6.5	8.5				6.5																																																																																																					SUPERCONDUCTIVITY IN THE BI-SR-CU-O SYSTEM	198712	RESISTIVITY              ,PREPARATION	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,26(1987)L2080	AKIRA YAMAZAKI,HIDEO FUJIKI,HIROSHI SAWA,JUN AKIMITSU	BI,SR,CU,O	
160	JJP0261837		YBa2Cu3O7	Y1Ba2Cu3O9-Y	Y	1	Ba	2	Cu	3															O	9-Y			1987																												Y123																																																																																																																														Thickness Dependence of Superconductivity in As-Sputtered Er-Ba-Cu-O	198711		Central Research Laboratories, Matsushita Electric Industrial Co.,Ltd., Moriguchi, Osaka 570	Jpn.J.Appl.Phys,26(1987)L1837-L1838	Hideaki Adachi,Kentaro Setsune,Kiyotaka Wasa,Kumiko Hirochi,Osamu Yamazaki		
161	JJP0261837		ErBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X			1987																											3	Y123																			80		91				85.5																																																																														3																							Thickness Dependence of Superconductivity in As-Sputtered Er-Ba-Cu-O	198711		Central Research Laboratories, Matsushita Electric Industrial Co.,Ltd., Moriguchi, Osaka 570	Jpn.J.Appl.Phys,26(1987)L1837-L1838	Hideaki Adachi,Kentaro Setsune,Kiyotaka Wasa,Kumiko Hirochi,Osamu Yamazaki		
162	JJP0261850		HoBa2Cu3O7	Ho1Ba2Cu3OX	Ho	1	Ba	2	Cu	3															O	X			1987																											3	Y123																				91					91																																0.9	3																																																																				Critical Field Anisotropy of a Single Craystal GdBa2Cu3Ox and HoBa2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1850-L1852	Hiroyuki TAKEYA,Humihiko TAKEI,Tsuyoshi TAMEGAI,Yasuhiro IYE		
163	JJP0261850		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X			1987																												Y123																				93					93																																0.9	3																																																																				Critical Field Anisotropy of a Single Craystal GdBa2Cu3Ox and HoBa2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1850-L1852	Hiroyuki TAKEYA,Humihiko TAKEI,Tsuyoshi TAMEGAI,Yasuhiro IYE		
164	JJP0261859		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9		1987							32																				3	Y123																					95				95																																																																																																					Dependence of Magnetic Susceptibility of Ba2YCu3O7-x on the Oxygen Defect Concentration			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1859-L1861	Masayasu ISHIKAWA,Tadashi SUGANO,Toshiro TAKABATAKE		
165	JJP0261859		YBa2Cu3O7	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	6.41	6.41		1987							35																					Y123																																																																																																																														Dependence of Magnetic Susceptibility of Ba2YCu3O7-x on the Oxygen Defect Concentration			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1859-L1861	Masayasu ISHIKAWA,Tadashi SUGANO,Toshiro TAKABATAKE		
166	JJP0261859		YBa2Cu3O7	Y1Ba2Cu3O6.23	Y	1	Ba	2	Cu	3															O	6.23	6.23		1987							38																					Y123																																																																																																																														Dependence of Magnetic Susceptibility of Ba2YCu3O7-x on the Oxygen Defect Concentration			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1859-L1861	Masayasu ISHIKAWA,Tadashi SUGANO,Toshiro TAKABATAKE		
167	JJP0261859		YBa2Cu3O7	Y1Ba2Cu3O6.18	Y	1	Ba	2	Cu	3															O	6.18	6.18		1987							30																					Y123																																																																																																																														Dependence of Magnetic Susceptibility of Ba2YCu3O7-x on the Oxygen Defect Concentration			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appl.Phys.,26(1987)L1859-L1861	Masayasu ISHIKAWA,Tadashi SUGANO,Toshiro TAKABATAKE		
168	JJP0261865		La(Ba,La)2Cu3O7	La1.5Ba1.5Cu3OY	La	1.5	Ba	1.5	Cu	3															O	Y			1987																												Y123				3.913	11.71																																																																																																		120																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
169	JJP0261865		Pr(Ba,Pr)2Cu3O7	Pr1.5Ba1.5Cu3OY	Pr	1.5	Ba	1.5	Cu	3															O	Y			1987																												Y123				3.898	11.66																																																																																																																									Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
170	JJP0261865		Nd(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3OY	Nd	1.5	Ba	1.5	Cu	3															O	Y			1987																												Y123				3.887	11.62																																																																																																		530																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
171	JJP0261865		Sm(Ba,Sm)2Cu3O7	Sm1.5Ba1.5Cu3OY	Sm	1.5	Ba	1.5	Cu	3															O	Y			1987																												Y123				3.865	11.56																																																																																																		950																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
172	JJP0261865		Eu(Ba,Eu)2Cu3O7	Eu1.5Ba1.5Cu3Oz	Eu	1.5	Ba	1.5	Cu	3															O	z			1987																												Y123				3.865		11.56													86		93				89.5																																																																														17																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
173	JJP0261865		Gd(Ba,Gd)2Cu3O7	Gd1.5Ba1.5Cu3Oz	Gd	1.5	Ba	1.5	Cu	3															O	z			1987																												Y123				3.863		11.58													92		93				92.5																																																																														8																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
174	JJP0261865		Y(Ba,Y)Cu3O7	Y1.5Ba1.5Cu3Oz	Y	1.5	Ba	1.5	Cu	3															O	z			1987																												Y123				3.821	3.854	11.67													90						90																																																																														13																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
175	JJP0261865		Tb(Ba,Yb)2Cu3O7	Yb1.5Ba1.5Cu3Oz	Yb	1.5	Ba	1.5	Cu	3															O	z			1987																												Y123																			90						90																																																																														20																							Drystal Structures and Electrical Properties of L1.5ba1.5Cu3Oy (L=La,Pr,Nd,Sm,Eu,Gd,Y, and Yb)	198711		NTT Opto-electronics Laboratories, Tokai, Ibaraki 319-11	Jpn.J.Appl.Phys,26(1987)L1865-L1867	Makoto HIKITA,Rsunekazu Iwata,Shigeyuki TSURUMI,Yukimichi TAJIMA		
176	PRB0368393		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.95Zn0.05O4	La	1.85	Sr	0.15	Cu	0.95	Zn	0.05													O	4			1987																											3	T				3.781		13.135																																																																																																	3																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
177	PRB0368393		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.925Zn0.075O4	La	1.85	Sr	0.15	Cu	0.925	Zn	0.075													O	4			1987						0.56	11																					T				3.793		13.201																																																																																																	15																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
178	PRB0368393		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9Zn0.1O4	La	1.85	Sr	0.15	Cu	0.9	Zn	0.1													O	4			1987						0.5	8																					T				3.785		13.194																																																																																																	10.5																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
179	PRB0368393		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.8Zn0.2O4	La	1.85	Sr	0.15	Cu	0.8	Zn	0.2													O	4			1987						0.46	9																					T				3.794		13.164																																																																																																	20																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
180	PRB0368393		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987						0.29	-21																					Y123				3.824	3.887	11.657														91.6					91.6																																																																														1.8																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
181	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.8Ni0.2O4	La	1.85	Sr	0.15	Cu	0.8	Ni	0.2													O	4			1987																												T				3.787		13.114																																																																																																																								3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
182	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.7Ni0.3O4	La	1.85	Sr	0.15	Cu	0.7	Ni	0.3													O	4			1987						1.72	14																					T				3.797		13.046																																																																																																																								3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
183	PRB0368393		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.75Ni0.25O7	Y	1	Ba	2	Cu	2.75	Ni	0.25													O	7			1987						0.62	14																					Y123				3.819	3.886	11.657														63.9					63.9																																																																														1.36																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
184	PRB0368365		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123				3.851	3.851	11.672															92				92																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
185	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.95Al0.05O7	Y	1	Ba	2	Cu	2.95	Al	0.05													O	7			1987																												Y123				3.835	3.884	11.688															88				88																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
186	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.9Al0.1O7	Y	1	Ba	2	Cu	2.9	Al	0.1													O	7			1987																												Y123				3.844	3.895	11.657														75					75																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
187	PRB0368393		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T				3.777		13.226														39.3					39.3																																																																														2.3																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
188	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4			1987																												T				3.775		13.222														22.6					22.6																																																																														2.38																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
189	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.95Ni0.05O4	La	1.85	Sr	0.15	Cu	0.95	Ni	0.05													O	4			1987																												T				3.776		13.208														4.2					4.2																																																																														3.5																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
190	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.925Ni0.075O4	La	1.85	Sr	0.15	Cu	0.925	Ni	0.075													O	4			1987						0.74	1																					T				3.779		13.187																																																																																																	4																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
191	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.9Ni0.1O4	La	1.85	Sr	0.15	Cu	0.9	Ni	0.1													O	4			1987						0.83	2																					T				3.792		13.167																																																																																																	4.2																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
192	PRB0368393		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.875Ni0.125O4	La	1.85	Sr	0.15	Cu	0.875	Ni	0.125													O	4			1987						1.14	9																					T				3.783		13.158																																																																																																	9.3																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
193	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.89Al0.11O7	Y	1	Ba	2	Cu	2.89	Al	0.11													O	7			1987																												Y123				3.847	3.851	11.659															82				82																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
194	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.88Al0.12O7	Y	1	Ba	2	Cu	2.88	Al	0.12													O	7			1987																												Y123				3.855	3.859	11.684															51				51																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
195	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.87Al0.13O7	Y	1	Ba	2	Cu	2.87	Al	0.13													O	7			1987																												Y123				3.843	3.859	11.667															45				45																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
196	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.865Al0.135O7	Y	1	Ba	2	Cu	2.865	Al	0.135													O	7			1987																												Y123				3.856	3.86	11.674															45				45																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
197	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu2.82Al0.18O7	Y	1	Ba	2	Cu	2.82	Al	0.18													O	7			1987																												Y123				3.854	3.856	11.668															20				20																																																																																																					Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
198	PRB0368365		YBa2(Cu,Al)3O7	Y1Ba2Cu0.78Al0.22O7	Y	1	Ba	2	Cu	0.78	Al	0.22													O	7			1987																												Y123				3.854	3.861	11.672																																																																																																																								Aluminum substitution in Ba2YCu3O7			At&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B.,36(1987)8365	B. Batlogg,D.W. Murphy,J.V. Waszczak,L.F. Schneemeyer,L.W. Rupp,N.P. Singh,R.L. Opila,T. Siegrist		
199	PRB0368329		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																					92.4				92.4																																3.2																																														0.8																							High-magnetic-field study of superconducting YBa2Cu3O7-delta	198712		Francis Bitter National Magnet Laboratory, Cambridge, Massachusetts 02139	Phys.Rev.B,36(1987)8329	J.E. Tkaczyk,J.S. Moodera,P.M. Tedrow		
200	PRB0368786		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-Z	6.8		1987																												Y123																			87	91.6					91.6																																																																																																					LOW-TEMPERATURE THERMAL CONDUCTIVITY OF Y(1)BA(2)CU(3)O(7-Z)	198712	THERMAL CONDUCTIVITY	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN	PHYS.REV.B,36(1987)8786	A.ZANGVIL,D.M.GINSBERG,J.CHEN,J.J.FREEMAN,T.A.FRIEDMANN	Y,BA,CU,O	
201	PRB0368791		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1987						9.67	-10.8																					Y123																			84	86					86																																																																																																					Magnetic ordering and magnetization in the high-temperature superconductor ErBa2Cu3O7-delta	198712		Ames Laboratory and Department of Physics, Iowa State university, Ames, Iowa 50011	Phys.Rev.B,36(1987)8791	H.C. Ku,H.D. Yang,P. Klavins,R.N. Shelton		
202	PRB0368798		YBa2Cu3HxO7	Y1Ba2Cu3H0.14O7	Y	1	Ba	2	Cu	3	H	0.14													O	7			1987																												Y123																				92.5					92.5																																																																																																					SUPERCONDUCTING H(X)Y(1)BA(2)CU(3)O(7): THE ROLE OF H	198712	INFRARED                 ,XAS	DIVISION OF MATERIALS SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)8798	A.R.MOODENBAUGH,C.Y.YANG,J.J.REILLY,M.SUENAGA,S.M.HEALD,T.SKOTHEIM,X.-Q.YANG	H,Y,BA,CU,O	
203	PRB0368798		Yba2Cu3HxO7	Y1Ba2Cu3H0.48O7	Y	1	Ba	2	Cu	3	H	0.48													O	7			1987																												Y123																				93.6					93.6																																																																																																					SUPERCONDUCTING H(X)Y(1)BA(2)CU(3)O(7): THE ROLE OF H	198712	INFRARED                 ,XAS	DIVISION OF MATERIALS SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)8798	A.R.MOODENBAUGH,C.Y.YANG,J.J.REILLY,M.SUENAGA,S.M.HEALD,T.SKOTHEIM,X.-Q.YANG	H,Y,BA,CU,O	
204	PRB0368798		YBa2Cu3HxO7	Y1Ba2Cu3H1O7	Y	1	Ba	2	Cu	3	H	1													O	7			1987																												Y123																				93.2					93.2																																																																																																					SUPERCONDUCTING H(X)Y(1)BA(2)CU(3)O(7): THE ROLE OF H	198712	INFRARED                 ,XAS	DIVISION OF MATERIALS SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)8798	A.R.MOODENBAUGH,C.Y.YANG,J.J.REILLY,M.SUENAGA,S.M.HEALD,T.SKOTHEIM,X.-Q.YANG	H,Y,BA,CU,O	
205	PRB0368798		YBa2Cu3HxO7	Y1Ba2Cu3H4O7	Y	1	Ba	2	Cu	3	H	4													O	7			1987																												Y123																																																																																																																														SUPERCONDUCTING H(X)Y(1)BA(2)CU(3)O(7): THE ROLE OF H	198712	INFRARED                 ,XAS	DIVISION OF MATERIALS SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)8798	A.R.MOODENBAUGH,C.Y.YANG,J.J.REILLY,M.SUENAGA,S.M.HEALD,T.SKOTHEIM,X.-Q.YANG	H,Y,BA,CU,O	
206	PRB0368798		YBa2Cu3HxO7	Y1Ba2Cu3H5O7	Y	1	Ba	2	Cu	3	H	5													O	7			1987																												Y123																																																																																																																														SUPERCONDUCTING H(X)Y(1)BA(2)CU(3)O(7): THE ROLE OF H	198712	INFRARED                 ,XAS	DIVISION OF MATERIALS SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)8798	A.R.MOODENBAUGH,C.Y.YANG,J.J.REILLY,M.SUENAGA,S.M.HEALD,T.SKOTHEIM,X.-Q.YANG	H,Y,BA,CU,O	
207	PRB0368802		YBa2Cu3O7	Y1Ba2Cu3O9-Z	Y	1	Ba	2	Cu	3															O	9-Z			1987																												Y123																				90					90																																																																																																					SUPERCONDUCTING ENERGY GAP OF Y(1)BA(2)CU(3)O(9-Z) MEASURED BY FAR-INFRARED REFLECTION	198712	ENERGY GAP               ,INFRARED	LABORATORY FOR INFRARED PHYSICS,SHANGHAI INSTITUTE OF TECHNICAL PHYSICS,SHANGHAI,CHINA	PHYS.REV.B,36(1987)8802	BAI-CAI MIAO,HONG-JUAN YE,WEI LU,XUE-CHU SHEN,YI-MING CAI,YONG-JIA QIAN,ZHI-YI YU	Y,BA,CU,O	
208	PRB0360226		EuBa2Cu3O7	Eu1Ba2Cu3O7.1	Eu	1	Ba	2	Cu	3															O	7-X	7.1		1987																												Y123				3.845	3.901	11.704													93.7	94.9					94.9																																																																														2.5																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
209	PRB0360226		GdBa2Cu3O7	Gd1Ba2Cu3O7.08	Gd	1	Ba	2	Cu	3															O	7-X	7.08		1987						7.75	-2																					Y123				3.84	3.899	11.703													92.2	93.8					93.8																																																																														1.65																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
210	PRB0360226		DyBa2Cu3O7	Dy1Ba2Cu3O6.82	Dy	1	Ba	2	Cu	3															O	7-X	6.82		1987						10.45	-7																					Y123				3.828	3.889	11.668													91.2	92.7					92.7																																																																														1.55																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
211	PRB0360226		HoBa2Cu3O7	Ho1Ba2Cu3O6.71	Ho	1	Ba	2	Cu	3															O	7-X	6.71		1987						10.48	-16																					Y123				3.822	3.888	11.67													92.2	92.9					92.9																																																																														1.2																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
212	PRB0360226		ErBa2Cu3O7	Er1Ba2Cu3O6.16	Er	1	Ba	2	Cu	3															O	7-X	6.16		1987						9.63	-16																					Y123				3.854		11.796																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
213	PRB0360226		TmBa2Cu3O7	Tm1Ba2Cu3O6.07	Tm	1	Ba	2	Cu	3															O	7-X	6.07		1987						7.69	-38																					Y123				3.849		11.788																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
214	PRB0360226		YbBa2Cu3O7	Yb1Ba2Cu3O6.01	Yb	1	Ba	2	Cu	3															O	7-X	6.01		1987																												Y123				3.841		11.828																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
215	PRB0360226		EuBa2Cu3O7	Eu1Ba2Cu3O6.59	Eu	1	Ba	2	Cu	3															O	7-X	6.59		1987																												Y123				3.883		11.814																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
216	PRB0360226		GdBa2Cu3O7	Gd1Ba2Cu3O6.52	Gd	1	Ba	2	Cu	3															O	7-X	6.52		1987						7.85	-3																					Y123				3.877		11.81																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
217	PRB0360226		DyBa2Cu3O7	Dy1Ba2Cu3O6.28	Dy	1	Ba	2	Cu	3															O	7-X	6.28		1987						10.69	-8																					Y123				3.866		11.783																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
218	PRB0360226		HoBa2Cu3O7	Ho1Ba2Cu3O6.13	Ho	1	Ba	2	Cu	3															O	7-X	6.13		1987						10.6	-19																					Y123				3.86		11.791																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
219	PRB0360226		YBa2Cu3O7	Y1Ba2Cu3O6.19	Y	1	Ba	2	Cu	3															O	7-X	6.19		1987																												Y123				3.859		11.8																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
220	PRB0360226		LaBa2Cu3O7	La1Ba2Cu3O7-X	La	1	Ba	2	Cu	3															O	7-X			1987																												Y123				3.901		11.858																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
221	PRB0360226		SmBa2Cu3O7	Sm1Ba2Cu3O6.64	Sm	1	Ba	2	Cu	3															O	7-X	6.64		1987																												Y123				3.884		11.822																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
222	PRB0360226		ErBa2Cu3O7	Er1Ba2Cu3O6.82	Er	1	Ba	2	Cu	3															O	7-X	6.82		1987						9.93	-15																					Y123				3.815	3.885	11.659													91.5	92.4					92.4																																																																														1.88																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
223	PRB0360226		TmBa2Cu3O7	Tm1Ba2Cu3O6.65	Tm	1	Ba	2	Cu	3															O	7-X	6.65		1987						7.53	-35																					Y123				3.81	3.882	11.656													91.2	92.5					92.5																																																																														1.11																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
224	PRB0360226		YbBa2Cu3O7	Yb1Ba2Cu3O6.71	Yb	1	Ba	2	Cu	3															O	7-X	6.71		1987																												Y123				3.799	3.873	11.65													85.6	87					87																																																																														1																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
225	PRB0360226		LuBa2Cu3O7	Lu1Ba2Cu3O7-X	Lu	1	Ba	2	Cu	3															O	7-X			1987																												Y123																			88.2	89.5					89.5																																																																														17																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
226	PRB0360226		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	7-X	6.72		1987																												Y123				3.824	3.887	11.657													91.5	93.4					93.4																																																																														2.5																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
227	PRB0360226		LaBa2Cu3O7	La1Ba2Cu3O7-X	La	1	Ba	2	Cu	3															O	7-X			1987																												Y123				3.856	3.906	11.783																																																																																																																								Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
228	PRB0360226		NdBa2Cu3O7	Nd1Ba2Cu3O7.16	Nd	1	Ba	2	Cu	3															O	7-X	7.16		1987																												Y123				3.855	3.914	11.736													92	95.3					95.3																																																																														4.2																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
229	PRB0360226		SmBa2Cu3O7	Sm1Ba2Cu3O7.11	Sm	1	Ba	2	Cu	3															O	7-X	7.11		1987																												Y123				3.855	3.899	11.721													88.3	93.5					93.5																																																																														2.8																							Oxygen and rare-earth doping of the 90-K superconducting perovskite YBa2Cu3O7-x	198707		Bell Communications Research, 331 Newman Springs Road, Red Bank, New Jersay 07701-7020	Phys.Rev.B,36(1987)226	E.M. Vogel,G.W. Hull,J.M. Tarascon,L.H. Greene,W.R. McKnnon		
230	SSC0650849		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1988																												T																				37.1					37.1																																1.84																									0.134																																												SUPERCONDUCTNG AND NORMAL STATEPROPERTIES OF Sr0.5La1.85CuO4 DETERMINED FROM MAGNETIZATION MEASUREMENTS			Department of Physics, Brock University St. Cctharines, Ontario, Canada L2S 3AI	Solid State Commun.,65(1988)849-853	B. Mitrovic',F.P. Koffyberg,F.S. Razavi,P.N. Arberg		
231	PRL0591160		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																												Y123																				88.8					88.8																																2.3	0.46																																																																				ANISOTROPIC NATURE OF HIGH-TEMPERATURE SUPERCONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-X)	198709	HC                       ,ANISOTROPY               ,SINGLE C	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.LETT.,59(1987)1160	T.K.WORTHINGTON,T.R.DINGER,W.J.GALLAGHER	Y,BA,CU,O	
232	PRB0365279		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Z	La	1.85	Sr	0.15	Cu	1															O	4-Z			1987																												T																				33					33																																2.2																									7																																												HIGH-FIELD MEASUREMENTS ON THE HIGH-TC SUPERCONDUCTORS LA(1.85)SR(0.15)CU(1)O(4-Z) AND Y(1)BA(2)CU(3)O(7-Z)	198710	HC                       ,MAGNETO-RESIST	RESEARCH INSTITUTE FOR MATERIALS AND HIGH FIELD MAGNET LABORATORY,UNIVERSITY OF NIJMEGEN,TOERNOOIVELD,NL	PHYS.REV.B,36(1987)5279	J.A.A.J.PERENBOOM,L.E.C.VAN DE LEEMPUT,L.W.M.SCHREURS,P.A.A.TEUNISSEN,P.J.M.VAN BENTUM.H.VAN KEMPEN	LA,SR,CU,O,Y,BA,CU,O	
233	SSC0650585		YBa2(Cu,Ni)3O7	Y1Ba2.01Cu2.81Ni0.19O6.7	Y	1	Ba	2.01	Cu	2.81	Ni	0.19													O	6.7			1988																												Y123				3.819	3.888	11.661														65	73				65																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
234	SSC0650585		YBa2(Cu,Zn)3O7	Y1Ba2.02Cu2.18Zn0.82O7	Y	1	Ba	2.02	Cu	2.18	Zn	0.82													O	7			1988																												Y123				3.829	3.887	11.67														30	40				30																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
235	SSC0650585		YBa2(Cu,Ag)3O7	Y1Ba1.99Cu2.847Ag0.153O6.7	Y	1	Ba	1.99	Cu	2.847	Ag	0.153													O	6.7			1988																												Y123				3.827	3.893	11.683														86	92				86																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
236	SSC0650585		YBa2(Cu,Pt)3O7	Y1Ba2Cu2.902Pt0.098O6.4	Y	1	Ba	2	Cu	2.902	Pt	0.098													O	6.4			1988																												Y123				3.82	3.886	11.675														81	92				81																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
237	SSC0650585		Yba2(Cu,Co)3O7	Y1Ba2.01Cu2.7Co0.3O6.8	Y	1	Ba	2.01	Cu	2.7	Co	0.3													O	6.8			1988																												Y123				3.871		11.664														36	50				36																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
238	SSC0650585		YBa2(Cu,Co)3O7	Y1Ba2Cu2.55Co0.45Oz	Y	1	Ba	2	Cu	2.55	Co	0.45													O	z			1988																												Y123				3.878		11.64																																																																																																																								SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
239	SSC0650585		YBa2(Cu,Ni)3O7	Y1.01Ba2.01Cu2.906Ni0.094O6.7	Y	1.01	Ba	2.01	Cu	2.906	Ni	0.094													O	6.7			1988																												Y123				3.819	3.886	11.662														71	76				71																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
240	SSC0650585		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.697Mn0.303O6.9	Y	1	Ba	2	Cu	2.697	Mn	0.303													O	6.9	6.9		1988																												Y123				3.828	3.889	11.673														63	92				63																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
241	SSC0650585		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.844Fe0.156O7	Y	1	Ba	2	Cu	2.844	Fe	0.156													O	7			1988																												Y123				3.863		11.665														57	90				57																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
242	SSC0650585		YBa2(Cu,Fe)3O7	Y1.01Ba2.01Cu2.697Fe0.303O	Y	1.01	Ba	2.01	Cu	2.697	Fe	0.303													O				1988																												Y123				3.869		11.61														36	50				36																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
243	SSC0650585		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9		1988																												Y123				3.823	3.888	11.665														88	92				88																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
244	SSC0650585		YBa2Cu3O7	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	6.2	6.2		1988																												Y123				3.863		11.768																																																																																																																								SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
245	SSC0650585		YBa2(Cu,Li)3O7	Y0.99Ba1.99Cu2.847Li0.153O6.4	Y	0.99	Ba	1.99	Cu	2.847	Li	0.153													O	6.4	6.4		1988																												Y123				3.826	3.889	11.667														62	73				62																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
246	SSC0650585		YBa2(Cu,Li)3O7	Y1.01Ba2.03Cu2.808Li0.192O6.6	Y	1.01	Ba	2.03	Cu	2.808	Li	0.192													O	6.6	6.6		1988																												Y123				3.829	3.884	11.68														33	46				33																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
247	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z			1988																												Y123																				50					50																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
248	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z			1988																												Y123																				57					57																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
249	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7-Z	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7-Z			1988																												Y123																				4					4																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
250	PLA1270231		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91					91																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
251	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O7-Z	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z			1988																												Y123																				74					74																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
252	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O7-Z	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z			1988																												Y123																				59					59																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
253	PLA1270231		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.895Fe0.105O7-Z	Y	1	Ba	2	Cu	2.895	Fe	0.105													O	7-Z			1988																												Y123																				61					61																																																																																																					A MOSSBAUER STUDY OF YBa2(Cu1-xFex)3O7-delta	198802		Department of Physics,University of Manitoba, Winnipeg R3T 2N2, Manitoba, Canada	Phys.Lett.A,127(1988)231	A.H. MORRISH,Q.A. PANKHURST,X.Z. ZHOU		
254	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.825O	Y	1	Ba	2	Cu	3	F	0.825													O				1988																												Y123																				90.5					90.5																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
255	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F1.65O5.675	Y	1	Ba	2	Cu	3	F	1.65													O	5.675	5.675		1988																												Y123																				90.3					90.3																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
256	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.066Oz	Y	1	Ba	2	Cu	3	F	0.066													O	z			1988																												Y123				3.826	3.885	11.68														93.4					93.4																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
257	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.066Oz	Y	1	Ba	2	Cu	3	F	0.066													O	z			1988																												Y123				3.827	3.892	11.73														92.2					92.2																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
258	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.165Oz	Y	1	Ba	2	Cu	3	F	0.165													O	z			1988																												Y123				3.821	3.867	11.77														91.6					91.6																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
259	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.016Oz	Y	1	Ba	2	Cu	3	F	0.016													O	z			1988																											3	Y123				3.818	3.884	11.69														90.8					90.8																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
260	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.033Oz	Y	1	Ba	2	Cu	3	F	0.033													O	z			1988																											3	Y123				3.827	3.893	11.7														92.1					92.1																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
261	APL0520838		YBa2Cu3(O,F)7	Y1Ba2Cu3F0.05Oz	Y	1	Ba	2	Cu	3	F	0.05													O	z			1988																											3	Y123				3.822	3.88	11.7														92.5					92.5																																																																																																					EFFECT OF FLUORIDE DOPING ON THE TRANSITION TEMPERATURE OF Y(1)BA(2)CU(3)O(6.5+Z)	3	FLUORIDE                 ,STRUCTURE                ,TC	MATERIALS DIVISION,NATIONAL AERONAUTICS AND SPACE ADMINISTRATION,LEWIS RESEARCH CENTER,CLEVELAND,OHIO	APPL.PHYS.LETT.,52(1988)838	ANN L.SANDKUHL,D.E.FARRELL,NAROTTAM P.BANSAL	Y,BA,CU,O	
262	PRB0368816		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1987																												Y123																				90					90																																																									1.2		247																			5.2																							SUPERCONDUCTING AND NONSUPERCONDUCTING PHASES OF Y(1)BA(2)CU(3)O(X): MODIFICATIONS AT THE HIGH-TEMPERATURE PHASE TRANSITION	198711	PHASE TRANSITION         ,SPECIFIC HEAT            ,RES	DEPARTMENT OF PHYSICS AND CENTER FEO MATERIALS RESEARCH AND TECHNOLOGY,FLORIDA STATE UNIVERSITY,TALLAHASSEE,FLORIDA	PHYS.REV.B,36(1987)8816	C.M.REY,H.K.NG,H.MATHIAS,L.R.TESTARDI,R.J.KENNEDY,W.G.MOULTON	Y,BA,CU,O	
263	PRB0368816		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1987																												Y123																																																																																		9		248																																										SUPERCONDUCTING AND NONSUPERCONDUCTING PHASES OF Y(1)BA(2)CU(3)O(X): MODIFICATIONS AT THE HIGH-TEMPERATURE PHASE TRANSITION	198711	PHASE TRANSITION         ,SPECIFIC HEAT            ,RES	DEPARTMENT OF PHYSICS AND CENTER FEO MATERIALS RESEARCH AND TECHNOLOGY,FLORIDA STATE UNIVERSITY,TALLAHASSEE,FLORIDA	PHYS.REV.B,36(1987)8816	C.M.REY,H.K.NG,H.MATHIAS,L.R.TESTARDI,R.J.KENNEDY,W.G.MOULTON	Y,BA,CU,O	
264	PRB0368780		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																												T																																																																																		23		400																																										SPECIFIC HEAT OF LA(1.8)SR(0.2)CU(1)O(4): ANOMALY AT THE SUPERCONDUCTING TRANSITION	198712	SPECIFIC HEAT	CENTRO ATOMICO BARILOCHE,RIO NEGRO,ARGENTINA	PHYS.REV.B,36(1987)8780	C.A.D'OVIDIO,D.A.ESPARZA,E.N.MARTINEZ,F.DE LA CRUZ,G.NIEVA	LA,SR,CU,O	
265	JAP0624821		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1987																											3	Y123																				86					86																																																																														1.088																							Evidence for weak link and anistropy limitations on the transport critixal current bulk polycrystalline Y1Ba2Cu3Ox			Electromagnetic Technology Division, National Bureau of Standards, Boulder, Colorado 80303	J.Appl.Phys.62(1987)4821	A.I. Braginski,A.J. Panson,B. Flandermeyer,D.W. Capon II,J. Kwo,M. Hong,M.A. Janocko,N.J. Zaluzec,O.F. de Lima,S.H. Liou		
266	JPS0563805		GdBa2Cu3O7	Gd1Ba2Cu3Oz	Gd	1	Ba	2	Cu	3															O	z			1987																												Y123																				87					87																																																																																																					HEAT CAPACITIES OF BA2RCU3OX(R=GD, HO, ER, DY)	198711	HEAT CAPACITIES     ,MEGNETIC ORDERING	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINNERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,56(1987)3805	KIICHI AMAYA,KOH-ICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TATSUO KOBAYASHI,YASUKAGE ODA,YOH KOHORI	BA,GD,HO,ER,DY,CU,O	
267	JPS0563805		ErBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X			1987																											3	Y123																				90					90																																																																																																					HEAT CAPACITIES OF BA2RCU3OX(R=GD, HO, ER, DY)	198711	HEAT CAPACITIES     ,MEGNETIC ORDERING	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINNERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,56(1987)3805	KIICHI AMAYA,KOH-ICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TATSUO KOBAYASHI,YASUKAGE ODA,YOH KOHORI	BA,GD,HO,ER,DY,CU,O	
268	JPS0563805		DyBa2Cu3O7	Dy1Ba2Cu3OX	Dy	1	Ba	2	Cu	3															O	X			1987																											3	Y123																				92					92																																																																																																					HEAT CAPACITIES OF BA2RCU3OX(R=GD, HO, ER, DY)	198711	HEAT CAPACITIES     ,MEGNETIC ORDERING	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINNERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,56(1987)3805	KIICHI AMAYA,KOH-ICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TATSUO KOBAYASHI,YASUKAGE ODA,YOH KOHORI	BA,GD,HO,ER,DY,CU,O	
269	JPS0563805		HoBa2Cu3O7	Ho1Ba2Cu3OX	Ho	1	Ba	2	Cu	3															O	X			1987																											3	Y123																				90					90																																																																																																					HEAT CAPACITIES OF BA2RCU3OX(R=GD, HO, ER, DY)	198711	HEAT CAPACITIES     ,MEGNETIC ORDERING	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINNERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,56(1987)3805	KIICHI AMAYA,KOH-ICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TATSUO KOBAYASHI,YASUKAGE ODA,YOH KOHORI	BA,GD,HO,ER,DY,CU,O	
270	PRB0364014		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123																				93					93																																2.7																																																																					Longitudinal and transverse magnetoresistances of YBa2cu3O7 in very high field up to 430 kG	198709		Laboratoire de Physique des Solides, Centre d'Orsay, Universite' de Paris-Sud, Batiment 510,91405 Orsay, France	Phys.Rev.B,36(1987)4014	G. Collin,H. Rakoto,J.C. Ousset,J.M. Broto,M. Oussena,S. Askenazy,S. Snoussi		
271	SSC0650059		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1988																												Y123																				92					92																																																																																																					STUDY OF HIGH-TC SUPERCONDUCTING Y-BA-CU-O THIN FILMS	198801	FILM                     ,PREPARATION              ,RESISTIV	INSTITUTE OF PHYSICS,ACADEMIA SINICA,BEIJING,CHINA SURFACE PHYSICS LABORATRY,ACADEMIA SINICA,BEIJING,CHINA	SOLID STATE COMMUN.,65(1988)59	CAO LEI,CUI YU-DE,GUAN WEI-YAN,LI DONG-QI,WANG WEI,XIAO DONG-GUANG,XUE JIN-MIN,ZHENG GUO-GUANG,ZHENG JIA-QI	Y,BA,CU,O	
272	PRB0375132		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-X	La	1.85	Sr	0.15	Cu	1															O	4-X			1988																												T				3.776		13.22														34					34																																																																																																					EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
273	PRB0375132		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.995Ni0.005O4-X	La	1.85	Sr	0.15	Cu	0.995	Ni	0.005													O	4-X			1988																												T				3.776		13.205														30.5					30.5																																																																																																					EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
274	PRB0375132		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4-X	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4-X			1988																												T				3.777		13.22														30.5					30.5																																																																																																					EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
275	PRB0375132		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4-X	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4-X			1988																												T				3.785		13.225														23					23																																																																																																					EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
276	PRB0375132		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03OX	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	X			1988																												T				3.78		13.22														24					24																																																																																																					EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
277	PRB0375132		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.95Ni0.05OX	La	1.85	Sr	0.15	Cu	0.95	Ni	0.05													O	X			1988																												T				3.782		13.2																																																																																																																								EFFECTS OF NI-TO-CU SUBSTITUTION ON THE PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-Y)	198804	RESISTIVITY              ,TC                       ,SUSCEPTIBILITY           ,LA	LABORATOIRE DE PHYSIQUE DES SOLIDES,UNIVERSITE DE PARIS-SUD,FRANCE	PHYS.REV.B,37(1988)5132	D.JEROME,H.J.SCHULZ,J.M.BASSAT,PH.ODIER,S.S.P.PARKIN,W.KANG	LA,SR,CU,O,LA,SR,CU,NI,O	
278	PRL0601657			Tl2Ca2Ba1Cu3OX	Tl	2	Ca	2	Ba	1	Cu	3													O	X			1988																																															106	110	120				110																																																																																																					100-K SUPERCONDUCTING PHASES IN THE TL-CA-BA-CU-O SYSTEM	198804	NEW PHASE                ,RESISTIVITY              ,TEM                      ,ST	GEOPHYSICAL LABORATORY,CARNEGIE INSTITUTION OF WASHINGTON,WASHINGTON,D.C.	PHYS.REV.LETT.,60(1988)1657	A.EL ALI,A.M.HERMANN,C.G.HADIDIACOS,C.T.PREWITT,D.R.VEBLEN,L.W.FINGER,N.L.ROSS,P.J.HEANEY,R.J.ANGEL,R.M.HAZEN,Z.Z.SHENG	TL,CA,BA,CU,O	
279	PRL0601657			Tl2Ca2Ba2Cu3OX	Tl	2	Ca	2	Ba	2	Cu	3													O	X			1988																																5.4		36.25													102	110	120				110																																																																																																					100-K SUPERCONDUCTING PHASES IN THE TL-CA-BA-CU-O SYSTEM	198804	NEW PHASE                ,RESISTIVITY              ,TEM                      ,ST	GEOPHYSICAL LABORATORY,CARNEGIE INSTITUTION OF WASHINGTON,WASHINGTON,D.C.	PHYS.REV.LETT.,60(1988)1657	A.EL ALI,A.M.HERMANN,C.G.HADIDIACOS,C.T.PREWITT,D.R.VEBLEN,L.W.FINGER,N.L.ROSS,P.J.HEANEY,R.J.ANGEL,R.M.HAZEN,Z.Z.SHENG	TL,CA,BA,CU,O	
280	PRL0601657			Tl1Ca4Cu5OX	Tl	1	Ca	4	Cu	5															O	X			1988																																5.4	17.4	43.4																																																																																																																								100-K SUPERCONDUCTING PHASES IN THE TL-CA-BA-CU-O SYSTEM	198804	NEW PHASE                ,RESISTIVITY              ,TEM                      ,ST	GEOPHYSICAL LABORATORY,CARNEGIE INSTITUTION OF WASHINGTON,WASHINGTON,D.C.	PHYS.REV.LETT.,60(1988)1657	A.EL ALI,A.M.HERMANN,C.G.HADIDIACOS,C.T.PREWITT,D.R.VEBLEN,L.W.FINGER,N.L.ROSS,P.J.HEANEY,R.J.ANGEL,R.M.HAZEN,Z.Z.SHENG	TL,CA,BA,CU,O	
281	PRL0601657		Tl2Ba2CaCu2Oz	Tl2Ca1Ba2Cu2Oz	Tl	2	Ca	1	Ba	2	Cu	2													O	z			1988																												Tl2212				5.44		29.3																																																																																																																								100-K SUPERCONDUCTING PHASES IN THE TL-CA-BA-CU-O SYSTEM	198804	NEW PHASE                ,RESISTIVITY              ,TEM                      ,ST	GEOPHYSICAL LABORATORY,CARNEGIE INSTITUTION OF WASHINGTON,WASHINGTON,D.C.	PHYS.REV.LETT.,60(1988)1657	A.EL ALI,A.M.HERMANN,C.G.HADIDIACOS,C.T.PREWITT,D.R.VEBLEN,L.W.FINGER,N.L.ROSS,P.J.HEANEY,R.J.ANGEL,R.M.HAZEN,Z.Z.SHENG	TL,CA,BA,CU,O	
282	JJP0270655		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1988																												Y123																			87		100				93.5																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
283	JJP0270655		YBa(Cu,Ti)3O7	Y1Ba2Cu2.85Ti0.15Oz	Y	1	Ba	2	Cu	2.85	Ti	0.15													O	z			1988																												Y123																			80		108				94																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
284	JJP0270655		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.7Ti0.3Oz	Y	1	Ba	2	Cu	2.7	Ti	0.3													O	z			1988																												Y123																			81		104				92.5																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
285	JJP0270655		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.55Ti0.45Oz	Y	1	Ba	2	Cu	2.55	Ti	0.45													O	z			1988																												Y123																			80		105				92.5																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
286	JJP0270655		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.4Ti0.6Oz	Y	1	Ba	2	Cu	2.4	Ti	0.6													O	z			1988																												Y123																			80		107				93.5																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
287	JJP0270655		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.25Ti0.75Oz	Y	1	Ba	2	Cu	2.25	Ti	0.75													O	z			1988																												Y123																			78		98				88																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
288	JJP0270655		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.1Ti0.9Oz	Y	1	Ba	2	Cu	2.1	Ti	0.9													O	z			1988																												Y123																			77		90				83.5																																																																																																					SUPERCONDUCTIVITY OF BA(2)Y(CU,TI)(3)O(Y) OXIDE	198804	FABRICATION              ,RESISTIVITY              ,SUSCEPTI	RESEARCH & DEVELOPMENT GROUP,SUMITOMO ELECTRIC INDUSTRIES,LTD. OSAKA	JJAP.LETT.,27(1988)L655	HAJIME HITOTSUYANAGI,HIROMI TAKEI,KAZUYA OHMATSU,KENGO OKURA,TSUNEO NAKAHARA	Y,BA,CU,TI,O	
289	JJP0270661			Bi1Sr1Ca1Cu2Oz	Bi	1	Sr	1	Ca	1	Cu	2													O	z			1988																																															75	110					110																																																																														4				10																			PHYSICAL PROPERTIES OF AN 80 K-SUPERCONDUCTOR: BI-SR-CA-CU-O CERAMICS	198804	STRUCTURE                ,SUSCEPTIBILITY	DEPARTMENT OF APPLIED PHYSICS,THE UNIVERSITY OF TOKYO	JJAP.LETT.,27(1988)L661	ATSUTAKA MAEDA,HIROSHI IKUTA,KUNIMITSU UCHINOKURA,MITSURU IZUMI,SHIGERU OKUDA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TAKAHIRO WADA,TAKAO ITOH,TOMOAKI YABE,YOSHIMI NAKAYAMA	BI,SR,CA,CU,O	
290	JJP0270661		Bi2(Sr,Ca)2CaCu2O8	Bi2Sr1.8Ca1.2Cu2Oz	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	z			1988																												Bi2212				5.4	27	30.73													70	75					75																																																																														0.4				1.2																			PHYSICAL PROPERTIES OF AN 80 K-SUPERCONDUCTOR: BI-SR-CA-CU-O CERAMICS	198804	STRUCTURE                ,SUSCEPTIBILITY	DEPARTMENT OF APPLIED PHYSICS,THE UNIVERSITY OF TOKYO	JJAP.LETT.,27(1988)L661	ATSUTAKA MAEDA,HIROSHI IKUTA,KUNIMITSU UCHINOKURA,MITSURU IZUMI,SHIGERU OKUDA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TAKAHIRO WADA,TAKAO ITOH,TOMOAKI YABE,YOSHIMI NAKAYAMA	BI,SR,CA,CU,O	
291	JJP0270674			Bi2Sr3Ca4Cu8Oz	Bi	2	Sr	3	Ca	4	Cu	8													O	z			1988																																															82.5	104	110				104																																																																																																					EFFECT OF PRESSURE ON SUPERCONDUCTING TRANSITION TEMPERATURES IN THE BI-SR-CA-CU-O SYSTEM	198804	PRESSURE EFFECT          ,TC                       ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,TSUKUBA,IBARAKI	JJAP.LETT.,27(1988)L674	BIN OKAI,KOH TAKAHASHI,MASATSUNE OHTA,MICHIKAZU KOSUGE	BI,SR,CA,CU,O	
292	JJP0270668			Bi1Sr1Ca1Cu2Oz	Bi	1	Sr	1	Ca	1	Cu	2													O	z			1988																																																106	112				106																						108										1.5																																																																					UPPER CRITICAL FIELD OF NEW OXIDE SUPERCONDUCTOR BI-SR-CA-CU-O	198804		NATIONAL RESEARCH INSTITUTE FOR METALS,IBARAK-KEYW                      CRITICAL FIELD	JJAP.LETT.,27(1988)L668	HIROAKI KUMAKURA,HIROSHI MAEDA,HITOSHI SHIMIZU,KAZUHIKO TAKAHASHI,KAZUMASA TOGANO	BI,SR,CA,CU,O	
293	PRB0368393		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.925Zn0.025O4	La	1.85	Sr	0.15	Cu	0.925	Zn	0.025													O	4			1987																												T				3.777		13.221														15					15																																																																														3.5																							3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
294	PRB0365279		NdBa2Cu3O7	Nd1Ba2Cu3O6.47	Nd	1	Ba	2	Cu	3															O	7-X	6.47		1987																												Y123				3.893		11.882																																																																																																																								HIGH-FIELD MEASUREMENTS ON THE HIGH-TC SUPERCONDUCTORS LA(1.85)SR(0.15)CU(1)O(4-Z) AND Y(1)BA(2)CU(3)O(7-Z)	198710	HC                       ,MAGNETO-RESIST	RESEARCH INSTITUTE FOR MATERIALS AND HIGH FIELD MAGNET LABORATORY,UNIVERSITY OF NIJMEGEN,TOERNOOIVELD,NL	PHYS.REV.B,36(1987)5279	J.A.A.J.PERENBOOM,L.E.C.VAN DE LEEMPUT,L.W.M.SCHREURS,P.A.A.TEUNISSEN,P.J.M.VAN BENTUM.H.VAN KEMPEN	LA,SR,CU,O,Y,BA,CU,O	
295	PRB0365279		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																				91.5					91.5																																4.2																									48																																												HIGH-FIELD MEASUREMENTS ON THE HIGH-TC SUPERCONDUCTORS LA(1.85)SR(0.15)CU(1)O(4-Z) AND Y(1)BA(2)CU(3)O(7-Z)	198710	HC                       ,MAGNETO-RESIST	RESEARCH INSTITUTE FOR MATERIALS AND HIGH FIELD MAGNET LABORATORY,UNIVERSITY OF NIJMEGEN,TOERNOOIVELD,NL	PHYS.REV.B,36(1987)5279	J.A.A.J.PERENBOOM,L.E.C.VAN DE LEEMPUT,L.W.M.SCHREURS,P.A.A.TEUNISSEN,P.J.M.VAN BENTUM.H.VAN KEMPEN	LA,SR,CU,O,Y,BA,CU,O	
296	SSC0650585		YBa2(Cu,Co)3O7	Y1Ba2Cu2.841Co0.159O6.8	Y	1	Ba	2	Cu	2.841	Co	0.159													O	6.8	6.8		1988																												Y123				3.862		11.664														54	78				54																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
297	SSC0650585		YBa2(Cu,Cr)3O7	Y1Ba2.01Cu2.806Cr0.194O7.3	Y	1	Ba	2.01	Cu	2.806	Cr	0.194													O	7.3	7.3		1988																												Y123				3.831	3.894	11.686														62	86				62																																																																																																					SUPERCONDUCTING PROPERTIES OF SUBSTITUTED Y(1)BA(2)CU(3(1-X))M(3X)O(7-Z)	198802	RESISTIVITY              ,SUBSTITUTION             ,SUSCEPTI	LABORATOIRE DE CRISTALLOGRAPHIE,C.N.R.S.,BP,FRANCE	SOLID STATE COMMUN.,65(1988)585	C.PAULSEN,J.L.THOLENCE,P.STROBEL	Y,BA,CU,MO	
298	JPS0563797		YBa2Cu3O7	Y1Ba2Cu3O6.74	Y	1	Ba	2	Cu	3															O	6.74	6.74		1987																												Y123																				91					91																																																																														4.9																							FAR-INFRARED ABSORPTION BY SMALL PARTICLES OF YBA2CU3O6.74	198711	FAR-INFRARED        ,GAP	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, SENDAI	J.PHYS.SOC.JAPAN,56(1987)3797	AYAKO TOKIWA,FUMIO CHIDA,MASAE KIKUCHI,NORITAKA KURODA,YOSHIRO SASAKI,YUICHIRO NISHINA	Y,BA,CU,O	
299	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.98Fe0.02O6.93	Y	1	Ba	2	Cu	2.98	Fe	0.02													O	X	6.93		1988																											3	Y123				3.819	3.884	11.667														91.8					91.8																																																																																		1.7																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
300	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.92	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	X	6.92		1988																											3	Y123				3.83	3.878	11.666														91.8					91.8																																																																																		1.7																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
301	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.92	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	X	6.92		1988						4.23	13																					Y123				3.86		11.683														76					76																																																																																		5.2																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
302	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.93	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	X	6.93		1988						3.77	5																				2	Y123				3.864		11.684														49					49																																																																																		7.5																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
303	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O6.96	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	X	6.96		1988						3.51	9																					Y123				3.867		11.681																																																																																																					8																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
304	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.6Fe0.4O7	Y	1	Ba	2	Cu	2.6	Fe	0.4													O	X	7		1988						3.48	11																				2	Y123				3.871		11.674														31					31																																																																																		10																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
305	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.5Fe0.5O7.2	Y	1	Ba	2	Cu	2.5	Fe	0.5													O	X	7.2		1988						3.53	16																				2	Y123				3.874		11.667																																																																																																					10																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
306	PRB0377458		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.2Fe0.8O7.25	Y	1	Ba	2	Cu	2.2	Fe	0.8													O	X	7.25		1988						3.23	12																				2	Y123				3.873		11.647																																																																																																					170																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
307	PRB0377458		YBa2(Cu,Al)3O7	Y1Ba2Cu2.95Al0.05O6.93	Y	1	Ba	2	Cu	2.95	Al	0.05													O	X	6.93		1988																											3	Y123				3.835	3.883	11.682														91					91																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
308	PRB0377458		YBa2(Cu,Al)3O7	Y1Ba2Cu2.9Al0.1O6.93	Y	1	Ba	2	Cu	2.9	Al	0.1													O	X	6.93		1988																												Y123				3.86	3.866	11.675														92					92																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
309	PRB0377458		YBa2(Cu,Al)3O7	Y1Ba2Cu2.8Al0.2O6.91	Y	1	Ba	2	Cu	2.8	Al	0.2													O	X	6.91		1988																											2	Y123				3.862		11.673														85					85																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
310	PRB0377458		YBa2(Cu,Al)3O7	Y1Ba2Cu2.7Al0.3O6.99	Y	1	Ba	2	Cu	2.7	Al	0.3													O	X	6.99		1988																												Y123				3.863		11.672														73					73																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
311	PRB0377458		YBa2(Cu,Al)3O7	Y1Ba2Cu2.6Al0.4O7	Y	1	Ba	2	Cu	2.6	Al	0.4													O	X	7		1988																											2	Y123				3.863		11.671														42					42																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
312	PRB0377458		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.87	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	X	6.87		1988																											3	Y123				3.829	3.886	11.637														55					55																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
313	PRB0377458		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.8Ni0.2O6.82	Y	1	Ba	2	Cu	2.8	Ni	0.2													O	X	6.82		1988																											3	Y123				3.835	3.856	11.657														45					45																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
314	PRB0377458	RH FROM (REFNO=PR0397324),RHN =AT 100K	YBa2(Cu,Co)3O7	Y1Ba2Cu2.98Co0.02O6.9	Y	1	Ba	2	Cu	2.98	Co	0.02													O	X	6.9	1	1988																												Y123				3.82	3.883	11.667														93.4					93.4																																																																																		1.1				0.000000000498			0.00000000133		RH314										STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
315	PRB0377458	RH FROM (REFNO=PR0397324),RHN=AT 100K	YBa2(Cu,Co)3O7	Y1Ba2Cu2.95Co0.05O6.92	Y	1	Ba	2	Cu	2.95	Co	0.05													O	X	6.92	1	1988																											3	Y123				3.829	3.88	11.67														94.3					94.3																																																																																		3.8				0.00000000126			0.00000000362		RH315										STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
316	PRB0377458	RH FROM (REFNO=PR0397324),RHN=AT 100K	YBa2(Cu,Co)3O7	Y1Ba2Cu2.9Co0.1O6.82	Y	1	Ba	2	Cu	2.9	Co	0.1													O	X	6.82	1	1988						4.05																						Y123				3.861		11.687														73					73																																																																																		4.5				0.00000000263			0.00000000563		RH316										STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
317	PRB0377458	RH FROM (REFNO=PR0397324),RHN=AT 100K	YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2O6.83	Y	1	Ba	2	Cu	2.8	Co	0.2													O	X	6.83	1	1988						3.74	15																				2	Y123				3.868		11.684														53					53																																																																																		11				0.00000000506			0.00000000968		RH317										STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
318	PRB0377458	RH FROM (REFNO=PR0397324),RHN=AT 100K	YBa2(Cu,Co)3O7	Y1Ba2Cu2.7Co0.3O6.88	Y	1	Ba	2	Cu	2.7	Co	0.3													O	X	6.88	1	1988						3.37	20																				2	Y123				3.872		11.68														22					22																																																																																		20				0.0000000108			0.0000000145		RH318										STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
319	PRB0377458		YBa2(Cu,Co)3O7	Y1Ba2Cu2.6Co0.4O6.95	Y	1	Ba	2	Cu	2.6	Co	0.4													O	X	6.95		1988						3.52	52																				2	Y123				3.877		11.674																																																																																																					77																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
320	PRB0377458		YBa2(Cu,Co)3O7	Y1Ba2Cu2.5Co0.5O6.99	Y	1	Ba	2	Cu	2.5	Co	0.5													O	X	6.99		1988						3.46	66																				2	Y123				3.881		11.671																																																																																																					50																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
321	PRB0377458		YBa2(Cu,Co)3O7	Y1Ba2Cu2.2Co0.8O7.07	Y	1	Ba	2	Cu	2.2	Co	0.8													O	X	7.07		1988						3.52	100																					Y123				3.886		11.661																																																																																																																								STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
322	PRB0377458		YBa2(Cu,Co)3O7	Y1Ba2Cu2Co1O7.2	Y	1	Ba	2	Cu	2	Co	1													O	X	7.2		1988																												Y123				3.887		11.625																																																																																																																								STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
323	PRB0377458		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O6.97	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	X	6.97		1988																											3	Y123				3.833	3.849	11.662														40					40																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
324	PRB0377458		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.81	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	X	6.81		1988																											3	Y123				3.819	3.888	11.682														55					55																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
325	PRB0377458		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2O6.79	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	X	6.79		1988																											3	Y123				3.82	3.889	11.68														45					45																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
326	PRB0377458		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6.74	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	X	6.74		1988																											3	Y123				3.82	3.893	11.68														45					45																																																																																																					STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
327	PRB0377458		YBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	X	6.85		1988																											3	Y123				3.815	3.882	11.67														92					92																																																																																		1.8																			STRUCTURAL AND PHYSICAL PROPERTIES OF THE METAL (M) SUBSTITUTED Y(1)BA(2)CU(3-X)M(X)O(7-Y) PEROVSKITE	198805	STRUCTURE                ,TRANSITION TEMPERATURE   ,LATTICE CONSTANT         ,RESISTIVITY	BELL COMMUNICATIONS RESEARCH INC.,NEW JERSEY	PHYS.REV.B,37(1988)7458	G.W.HULL,J.M.TARASCON,L.H.GREENE,M.EIBSCHUTZ,P.BARBOUX,P.F.MICELI,S.A.SUNSHINE	Y,BA,CU,M,O	
328	SSC0660715		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X			1988																											3	Y123				3.833	3.895	11.681													95	96.4	97.8				96.4																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
329	SSC0660715		Gd(Ba,Sr)2Cu3O7	Gd1Ba1.8Sr0.2Cu3OX	Gd	1	Ba	1.8	Sr	0.2	Cu	3													O	X			1988																												Y123				3.834	3.897	11.69													89.7	94.7	97.5				94.7																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
330	SSC0660715		Gd(Ba,Sr)2Cu3O7	Gd1Ba1.6Sr0.4Cu3OX	Gd	1	Ba	1.6	Sr	0.4	Cu	3													O	X			1988																												Y123				3.831	3.883	11.64													88.3	92.4	95.2				92.4																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
331	SSC0660715		Gd(Ba,Sr)2Cu3O7	Gd1Ba1.4Sr0.6Cu3Oz	Gd	1	Ba	1.4	Sr	0.6	Cu	3													O	z			1988																											2	Y123				3.854		11.615													86	89.4	94.2				89.4																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
332	SSC0660715		Gd(Ba,Sr)2Cu3O7	Gd1Ba1.2Sr0.8Cu3Oz	Gd	1	Ba	1.2	Sr	0.8	Cu	3													O	z			1988																											2	Y123				3.843		11.567														90.7	94.9				90.7																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
333	SSC0660715		Gd(Ba,Sr)2Cu3O7	Gd1Ba1Sr1Cu3Oz	Gd	1	Ba	1	Sr	1	Cu	3													O	z			1988																											2	Y123				3.848		11.569														88.6	94.2				88.6																																																																																																					CRYSTAL SYRUCTURE AND HIGH-TC SUPERCONDUCTIVITY IN THE SYSYEM GD(1)BA(2-X)SR(X)CU(3)O(7-Z)	198805	STRUCTURE                ,RESISTIVITY	CHEMISTRY DEPARTMENT,PAISLEY COLLEGE OF TECHNOLOGY,PAISLEY,SCOTLAND	SOLID STATE COMMUN.,66(1988)715	A.M.FORREST,D.B.CURRIE	GD,BA,SR,CU,O	
334	SSC0660387		(La,Na)2CuO4	La2.89Na0.11Cu1O4-X	La	2.89	Na	0.11	Cu	1															O	4-X			1988																												Y123																				16	21				16																																																																																		4																			SUPERCONDUCTIVITY IN La2-xNaxCuO4-y			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Solid State Commun., 66(1988)387	J. T. Marked,C. L. Seaman,H. Zhou,M. B. Maple		
335	SSC0660387		(La,Na)2CuO4	La2.89Na0.41Cu1O4-X	La	2.89	Na	0.41	Cu	1															O	4-X			1988																												Y123																				18	25				18																																																																																		4																			SUPERCONDUCTIVITY IN La2-xNaxCuO4-y			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Solid State Commun., 66(1988)387	J. T. Marked,C. L. Seaman,H. Zhou,M. B. Maple		
336	SSC0660393			Bi1Ca1Sr1Cu2Oz	Bi	1	Ca	1	Sr	1	Cu	2													O	z			1988																												Y123																			71	75	90				75																																																																														14																							HIGH TEMPERATURE SUPERCONDUCTIVITY IN THE COMPOUND (BICASR)CU(X)O(Y)	198804	FABRICATION              ,RESISTIVITY	LABORATORIUM VOOR VASTE STOF-FYSIKA EN MAGNETISME,KATHOLIEKE UNIVERSITEIT LEUVEN,BELGIUM	SOLID STATE COMMUN.,66(1988)393	C.VAN HAESENDONCK,IVAN K.SCHULLER,J.P.LOCQUET,J.VANACKEN,M.D'HALLE,Y.BRUYNSERAEDE	BI,CA,SR,CU,O	
337	SSC0660393			Bi1Ca1Sr1Cu2Oz	Bi	1	Ca	1	Sr	1	Cu	2													O	z			1988																												Y123																			64	70	84				70																																																																														1.7																							HIGH TEMPERATURE SUPERCONDUCTIVITY IN THE COMPOUND (BICASR)CU(X)O(Y)	198804	FABRICATION              ,RESISTIVITY	LABORATORIUM VOOR VASTE STOF-FYSIKA EN MAGNETISME,KATHOLIEKE UNIVERSITEIT LEUVEN,BELGIUM	SOLID STATE COMMUN.,66(1988)393	C.VAN HAESENDONCK,IVAN K.SCHULLER,J.P.LOCQUET,J.VANACKEN,M.D'HALLE,Y.BRUYNSERAEDE	BI,CA,SR,CU,O	
338	SSC0660421		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																											3	Y123																				91.3					91.3																																																																														7				9.8																			PROBING THERMODYNAMIC FLUCTUATIONS IN HIGH TEMPERATURE SUPERCONDUCTORS	198804	FLUCTUATION              ,RESISTIVITY	LABORATORIO DE FISICA DE MATERIALES,FACULTAD DE FISICA,UNIVERSIDAD DE SANTIAGO DE COMPOSTELA,SPAIN	SOLID STATE COMMUN.,66(1988)421	E.MORAN,F.MIGUELEZ,FELIX VIDAL,J.A.VEIRA,J.MAZA,M.A.ALARIO	R,BA,CU,O	
339	SSC0660421		HoBa2Cu3O7	Ho1Ba2Cu3O7	Ho	1	Ba	2	Cu	3															O	7			1988																											3	Y123																				92.1					92.1																																																																														2.8				5.1																			PROBING THERMODYNAMIC FLUCTUATIONS IN HIGH TEMPERATURE SUPERCONDUCTORS	198804	FLUCTUATION              ,RESISTIVITY	LABORATORIO DE FISICA DE MATERIALES,FACULTAD DE FISICA,UNIVERSIDAD DE SANTIAGO DE COMPOSTELA,SPAIN	SOLID STATE COMMUN.,66(1988)421	E.MORAN,F.MIGUELEZ,FELIX VIDAL,J.A.VEIRA,J.MAZA,M.A.ALARIO	R,BA,CU,O	
340	SSC0660421		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7			1988																												Y123																				92.6					92.6																																																																														1.45				2.6																			PROBING THERMODYNAMIC FLUCTUATIONS IN HIGH TEMPERATURE SUPERCONDUCTORS	198804	FLUCTUATION              ,RESISTIVITY	LABORATORIO DE FISICA DE MATERIALES,FACULTAD DE FISICA,UNIVERSIDAD DE SANTIAGO DE COMPOSTELA,SPAIN	SOLID STATE COMMUN.,66(1988)421	E.MORAN,F.MIGUELEZ,FELIX VIDAL,J.A.VEIRA,J.MAZA,M.A.ALARIO	R,BA,CU,O	
341	SSC0660421		HoBa2Cu3O7	Ho1Ba2Cu3O7	Ho	1	Ba	2	Cu	3															O	7			1988																											3	Y123																				92.1					92.1																																																																														0.85				1.7																			PROBING THERMODYNAMIC FLUCTUATIONS IN HIGH TEMPERATURE SUPERCONDUCTORS	198804	FLUCTUATION              ,RESISTIVITY	LABORATORIO DE FISICA DE MATERIALES,FACULTAD DE FISICA,UNIVERSIDAD DE SANTIAGO DE COMPOSTELA,SPAIN	SOLID STATE COMMUN.,66(1988)421	E.MORAN,F.MIGUELEZ,FELIX VIDAL,J.A.VEIRA,J.MAZA,M.A.ALARIO	R,BA,CU,O	
342	SSC0660623		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																											3	Y123																				88.1					88.1																																																																																		12																			ELECTRICAL RESISTANCE OF Y(1)BA(2)CU(3)O(7-Z) IN THE RANGE 300-500 K AND 0-1.5 GPA	198805	RESISTIVITY              ,PRESSURE	DEPARTMENT OF PHYSICS,UNIVERSITY OF UMEA,SWEDEN	SOLID STATE COMMUN.,66(1988)623	B.SUNDGVIST	Y,BA,CU,O	
343	PRB0377956		EuBa2Cu3O7	Eu1Ba2Cu3OX	Eu	1	Ba	2	Cu	3															O	X			1988																											3	Y123																				94					94																																3.8	0.41																																																	1																			UPPER CRITICAL FIELD AND RESISTIVITY OF SINGLE-CRYSTAL EU(1)BA(2)CU(3)O(Y):DIRECT MEASUREMENTS UNDER HIGH FIELD UP TO 50 T	198805	SINGLE CRYSTAL           ,CRITICAL FIELD           ,RESISTIV	NIPPON TELEGRAPH AND TELEPHONE CORPORATION OPTO-ELECTRONICS LABORATORIES,TOKAI,IBARAKI	PHYS.REV.B,37(1988)7956	AKINORI KATSUI,AKIO YAMAGISHI,HIROYUKI FUKE,KIYOHIRO SUGIYAMA,MAKOTO HIKITA,MUNEYUKI DATE,SHIGEYUKI TSURUMI,TAKAO ISHII,TSUNEKAZU IWATA,YOSHIYUKI HIDATA,YUKIMICHI TAJIMA	EU,BA,CU,O	
344	SSC0650845		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	X	6.8		1988																											3	Y123																				79					79													750									88																																																																															MEISSNER EFFECT, CRITICAL FIELDS, AND SUPERCONDUCTING PARAMETERS OF YBa2Cu3O7-delta	1988		Freie Universitat Berlin, Institut fur Atom-und Festkorperphysik, Arnimallee 14, D-1000 Berlin 33, Federal Republic of Germany	Solid State Cmmun.65(1988)845-848	J.G. Perez-Ramirez,K. Baberschke,W.G. Clark		
345	PRB0377454		NdBa2Cu3O7	Nd1Ba2Cu3OX	Nd	1	Ba	2	Cu	3															O	X			1988						3.57																					3	Y123				3.88	3.874	11.626													75		90				82.5																																																																																		1.8																			RESISTIVE AND MAGNETIC STUDIES OF ND(1)BA(2)CU(3)O(7-Z) AND PR(1)BA(2)CU(3)O(7-Z)	198805	RESISTIVITY              ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS,OHIO STATE UNIVERSITY,COLUMBUS,OHIO	PHYS.REV.B,37(1988)7454	A.J.EPSTEIN,D.L.COX,J.P.GOLBEN,J.R.GAINES,SAILESH CHITTIPEDDI,Y.SONG	ND,BA,CU,O,PR,BA,CU,O	
346	PRB0377454		PrBa2Cu3O7	Pr1Ba2Cu3OX	Pr	1	Ba	2	Cu	3															O	X			1988						3.35	-5																				3	Y123				3.887	3.889	11.654																																																																																																					100																			RESISTIVE AND MAGNETIC STUDIES OF ND(1)BA(2)CU(3)O(7-Z) AND PR(1)BA(2)CU(3)O(7-Z)	198805	RESISTIVITY              ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS,OHIO STATE UNIVERSITY,COLUMBUS,OHIO	PHYS.REV.B,37(1988)7454	A.J.EPSTEIN,D.L.COX,J.P.GOLBEN,J.R.GAINES,SAILESH CHITTIPEDDI,Y.SONG	ND,BA,CU,O,PR,BA,CU,O	
347	JJP0270665			Bi1Sr1Ca1Cu2OX	Bi	1	Sr	1	Ca	1	Cu	2													O	X			1988																																															75	105					105																																																																																																					MAGNETIC PROPERTIES OF BI(1)SR(1)CA(1)CU(2)O(X) SUPERCONDUCTORS	198804		NATIONAL RESEARCH INSTITUTE FOR METALS,TSUKUB-KEYW                      MAGNETIZATION,JC	JJAP.LETT.,27(1988)L665	HIROSHI MAEDA,KEIICHI OGAWA,MITSURU UEHARA,YUJI ASADA	BI,SR,CA,CU,O	
348	PRB0363906		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																												T																				35.7					35.7																																1.53																																														8.07																							Microwave study of the high-Tc superconductor La1.8Sr0.2CuO4	198709		Centre de Recherche en Physique du Solide, De'partement de Physique, Universite' de Sherbrooke, Sherbrooke, Que'bec, Canada JIK 2R1	Phys.Rev.B,36(1987)3906	G. Quirion,J.P. Thiel,K.R. Poeppelmeier,M. Poirier		
349	PRB0363910			Y1.2Ba0.8Cu1O4	Y	1.2	Ba	0.8	Cu	1															O	4			1987																																																75	85				75																																																7																																																					Electron tunneling in the high-Tc superconductor Y-Ba-Cu-O	198709		Instituto de Investigaciones en Materiales, Universidad Nacional Auto'noma de Mexico, Apartado Postal 70-360,04510 Me'xco, Distrito Federal, Me'xico	Phys.Rev.B,36(1987)3910	J. Taguna-Marti'nez,L. Rendo'n,R. Escudero,R.A. Barrio,T. Akachi		
350	PRB0364018			Gd1Ba2Cu2.82Fe0.18O9-Z	Gd	1	Ba	2	Cu	2.82	Fe	0.18													O	9-Z			1987																											3																				31	42	57				42																																																																																																					Magnetic ordering in GdBa2(Cu0.94Fe0.06)3O9-delta below the superconducting transition temperature	9		Department of Phsics and Astronomy, Johns Hopkins University, Baltimore, Maryland 21218	Phys.Rev.B,36(1987)4018	C.L. Chien,Gang Xiao,H. Tang,J.C. Walker,Y.-w. Du,Z.Q. Qiu		
351	PLA1260130			Y1.2Ba0.8Cu1O4-X	Y	1.2	Ba	0.8	Cu	1															O	4-X			1987																											3					3.457	3.815	26.5														94.5					94.5																																																																																																					EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF THE (Y1.2BA0.8)4CU4O16-Z CERAMIC COMPOUND	198712			PHYS.LETT.A,126(1987)130	J.BASZYNSKI,M.MACKOWIAK,M.ZDANOWSKA-FRACZEK	Y,BA,CU,O	
352	JJP0262091		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1987																											3	Y123				3.811	3.878	11.646														90					90																																																																																		1																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
353	JJP0262091		(Er,Yb)Ba2Cu3O7	Er0.75Yb0.25Ba2Cu3O7-Z	Er	0.75	Yb	0.25	Ba	2	Cu	3													O	7-Z			1987																												Y123				3.817	3.887	11.659														87.6					87.6																																																																																		3.8																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
354	JJP0262091		(Er,Yb)Ba2Cu3O7	Er0.62Yb0.38Ba2Cu3O7-Z	Er	0.62	Yb	0.38	Ba	2	Cu	3													O	7-Z			1987																											3	Y123				3.815	3.883	11.675														88.3					88.3																																																																																		1.5																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
355	JJP0262091		(Er,Yb)Ba2Cu3O7	Er0.5Yb0.5Ba2Cu3O7-Z	Er	0.5	Yb	0.5	Ba	2	Cu	3													O	7-Z			1987																												Y123				3.812	3.883	11.674														89.3					89.3																																																																																		0.8																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
356	JJP0262091		(Er,Yb)Ba2Cu3O7	Er0.37Yb0.63Ba2Cu3O7-Z	Er	0.37	Yb	0.63	Ba	2	Cu	3													O	7-Z			1987																											3	Y123				3.809	3.879	11.664														87.8					87.8																																																																																		1.4																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
357	JJP0262091		(Er,Yb)Ba2Cu3O7	Er0.25Yb0.75Ba2Cu3O7-Z	Er	0.25	Yb	0.75	Ba	2	Cu	3													O	7-Z			1987																											3	Y123				3.812	3.879	11.636														86.3					86.3																																																																																		2.4																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
358	JJP0262091		YBa2Cu3O7	Yb1Ba2Cu3O7-Z	Yb	1	Ba	2	Cu	3															O	7-Z			1987																											3	Y123				3.811	3.871	11.635														88.5					88.5																																																																																		2.3																			ELECTRICAL,MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ER(1-X)YB(X)BA(2)CU(3)O(7-Z)	198712	RESISTIVITY              ,TC                       ,MAGNETIZ	DEPARTMENT OF ELECTRICAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TEMPAKU-CHO,TOYOHASHI-SHI,AICHI-KEN	JJAP.LETT.,26(1987)L2091	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI,YOSHIO KIYOSHIMA	ER,YB,BA,CU,O	
359	JJP0262087		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1OX	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	X			1987																												Y123																				90					90																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
360	JJP0262087		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2OX	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	X			1987																												Y123																				66					66																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
361	JJP0262087		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3OX	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	X			1987																												Y123																				44					44																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
362	JJP0262087		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.6Fe0.4OX	Y	1	Ba	2	Cu	2.6	Fe	0.4													O	X			1987																												Y123																				22					22																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
363	JJP0262087		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1OX	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	X			1987																												Y123																				80					80																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
364	JJP0262087		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.8Ni0.2OX	Y	1	Ba	2	Cu	2.8	Ni	0.2													O	X			1987																												Y123																				73					73																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
365	JJP0262087		YBa2(Cu,Co)3O7	Y1Ba2Cu2.9Co0.1OX	Y	1	Ba	2	Cu	2.9	Co	0.1													O	X			1987																												Y123																				88					88																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
366	JJP0262087		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2OX	Y	1	Ba	2	Cu	2.8	Co	0.2													O	X			1987																												Y123																																																																																																																														SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
367	JJP0262087		YBa2(Cu,Co)3O7	Y1Ba2Cu2.7Co0.3OX	Y	1	Ba	2	Cu	2.7	Co	0.3													O	X			1987																												Y123																				50					50																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
368	JJP0262087		YBa2(Cu,Co)3O7	Y1Ba2Cu2.6Co0.4OX	Y	1	Ba	2	Cu	2.6	Co	0.4													O	X			1987																												Y123																				15					15																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
369	JJP0262087		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1OX	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	X			1987																												Y123																				58					58																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
370	JJP0262087		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2OX	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	X			1987																												Y123																				50					50																																																																																																					SUPERCONDUCTIVITY OF Y(1)BA(2)CU(3-X)M(X)O(Y) (M=CO,FE,NI,ZN)	198712	SUSCEPTIBILITY           ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,IBARAKI	JJAP.LETT.,26(1987)L2087	EIJI TAKAYAMA-MUROMACHI,KATSUO KATO,YOSHISHIGE UCHIDA	Y,BA,CU,M,O	
371	JJP0262097		DyBa2Cu3O7	Dy1Ba2Cu3OX	Dy	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.835	3.89	11.69														91.2					91.2																						170										2.77																									15.3																					4.4																							SUPERCONDUCTIVITY AND MAGNETIC PROPERTIES OF DY(1)BA(2)CU(3)O(Y)	198712	HC                       ,MAGNETIZATION            ,SPECIFIC	ELECTROTECHNICAL LABORATORY,IBARAKI	JJAP.LETT.,26(1987)L2097	HIROMI UNOKI,KAZUYOSHI MITSUGI,KUNIHIKO OKA,SHINYA WAKI,YUJI YAMAGUCHI	DY,BA,CU,O	
372	JJP0262097		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																											3	Y123				3.823	3.886	11.68														90.8					90.8																																2.22																									4.4																					2.5				4																			SUPERCONDUCTIVITY AND MAGNETIC PROPERTIES OF DY(1)BA(2)CU(3)O(Y)	198712	HC                       ,MAGNETIZATION            ,SPECIFIC	ELECTROTECHNICAL LABORATORY,IBARAKI	JJAP.LETT.,26(1987)L2097	HIROMI UNOKI,KAZUYOSHI MITSUGI,KUNIHIKO OKA,SHINYA WAKI,YUJI YAMAGUCHI	DY,BA,CU,O	
373	SSC0650465		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1988																											3	Y123																			89	91.5	92				91.5																						50																																																																															ESTIMATION OF MATERIAL PARAMETERS FROM THE OBSERVATION OF PARACONDUCTIVITY IN Y-BA-CU-O	198801	RESISTIVITY	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,USA	SOLID STATE COMMUN.,65(1988)465	D.M.GINSBERG,NIGEL.GOLDENFELD,P.D.OLMSTED,T.A.FRIEDMANN	Y,BA,CU,O	
374	PRL0600542			La4Ba1Cu5O13	La	4	Ba	1	Cu	5															O	13			1988																																																																																																																																																										METALLIC,BUT NOT SUPERCONDUCTING,LA-BA(AND LA-SR) COPPER OXIDES	198802	SUPERCONDUCTIVITY        ,RESISTIVITY	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA	PHYS.REV.LETT.,60(1988)542	A.NAZZAL,J.B.TORRANCE,S.S.P.PARKIN,Y.TOKURA	LA,BA,CU,O,LA,SR,CU,O	
375	PRL0600542		La2SrCu2O6	La2Sr1Cu2O6.2	La	2	Sr	1	Cu	2															O	6.2	6.2		1988																												2126																																																																																																																														METALLIC,BUT NOT SUPERCONDUCTING,LA-BA(AND LA-SR) COPPER OXIDES	198802	SUPERCONDUCTIVITY        ,RESISTIVITY	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA	PHYS.REV.LETT.,60(1988)542	A.NAZZAL,J.B.TORRANCE,S.S.P.PARKIN,Y.TOKURA	LA,BA,CU,O,LA,SR,CU,O	
376	PRL0600542			La5Sr1Cu6O15	La	5	Sr	1	Cu	6															O	15			1988																																																																																																																																																										METALLIC,BUT NOT SUPERCONDUCTING,LA-BA(AND LA-SR) COPPER OXIDES	198802	SUPERCONDUCTIVITY        ,RESISTIVITY	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA	PHYS.REV.LETT.,60(1988)542	A.NAZZAL,J.B.TORRANCE,S.S.P.PARKIN,Y.TOKURA	LA,BA,CU,O,LA,SR,CU,O	
377	PRL0600542		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1988																											3	T																				40					40																																																																																																					METALLIC,BUT NOT SUPERCONDUCTING,LA-BA(AND LA-SR) COPPER OXIDES	198802	SUPERCONDUCTIVITY        ,RESISTIVITY	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA	PHYS.REV.LETT.,60(1988)542	A.NAZZAL,J.B.TORRANCE,S.S.P.PARKIN,Y.TOKURA	LA,BA,CU,O,LA,SR,CU,O	
378	SSC0650487		YBa2(Cu,V)3O7	Y1Ba2Cu2.4V0.6O6.9	Y	1	Ba	2	Cu	2.4	V	0.6													O	6.9	6.9		1988																												Y123																																																																																																																														RAMAN SPECTROSCOPIC STUDY OF AN APPARENT PHASE TRANSITION AT 234 K IN THE HIGH-TC SUPERCONDUCTOR Y(1)BA(2)CU(3-X)V(X)O(7-Y)	198801	RAMAN	NANJING UNIVERSITY,NANJING,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,65(1988)487	CHEN QIANG,J.F.SCOTT,JI RONG-FU,MING-SHENG ZHANG,QIN ZHENG-HAO,SUN DAKUN,YU ZHENG	Y,BA,CU,O	
379	JJP0261997		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																											3	Y123				3.823	3.887	11.684														92					92																																																																																																					TETRAGONAL HIGH-TC SUPERCONDUCTOR IN THE SYSTEM BA(2)Y(CU(1-X)GA(X))(3)O(7-Z)	198712	FABRICATION              ,SUBSTITUTION             ,OXYGEN C	CENTRAL RESEARCH LABORATORY,HITACHI,LTD.,KOKUBUNJI,TOKYO	JJAP.LETT.,26(1987)L1997	KATSUKI MIYAUCHI,MASAHIKO HIRATANI,TETSUICHI KUDO,YUKIO ITO	Y,BA,CU,GA,O	
380	JJP0261997		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.94Ga0.06O7-Z	Y	1	Ba	2	Cu	2.94	Ga	0.06													O	7-Z			1987																											3	Y123				3.848	3.874	11.689														87					87																																																																																																					TETRAGONAL HIGH-TC SUPERCONDUCTOR IN THE SYSTEM BA(2)Y(CU(1-X)GA(X))(3)O(7-Z)	198712	FABRICATION              ,SUBSTITUTION             ,OXYGEN C	CENTRAL RESEARCH LABORATORY,HITACHI,LTD.,KOKUBUNJI,TOKYO	JJAP.LETT.,26(1987)L1997	KATSUKI MIYAUCHI,MASAHIKO HIRATANI,TETSUICHI KUDO,YUKIO ITO	Y,BA,CU,GA,O	
381	JJP0261997		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7-Z	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-Z			1987																											2	Y123				3.855	3.863	11.689														75					75																																																																																																					TETRAGONAL HIGH-TC SUPERCONDUCTOR IN THE SYSTEM BA(2)Y(CU(1-X)GA(X))(3)O(7-Z)	198712	FABRICATION              ,SUBSTITUTION             ,OXYGEN C	CENTRAL RESEARCH LABORATORY,HITACHI,LTD.,KOKUBUNJI,TOKYO	JJAP.LETT.,26(1987)L1997	KATSUKI MIYAUCHI,MASAHIKO HIRATANI,TETSUICHI KUDO,YUKIO ITO	Y,BA,CU,GA,O	
382	JJP0261997		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.7Ga0.3O7-Z	Y	1	Ba	2	Cu	2.7	Ga	0.3													O	7-Z			1987																											2	Y123				3.861	3.866	11.696														66					66																																																																																																					TETRAGONAL HIGH-TC SUPERCONDUCTOR IN THE SYSTEM BA(2)Y(CU(1-X)GA(X))(3)O(7-Z)	198712	FABRICATION              ,SUBSTITUTION             ,OXYGEN C	CENTRAL RESEARCH LABORATORY,HITACHI,LTD.,KOKUBUNJI,TOKYO	JJAP.LETT.,26(1987)L1997	KATSUKI MIYAUCHI,MASAHIKO HIRATANI,TETSUICHI KUDO,YUKIO ITO	Y,BA,CU,GA,O	
383	PRB0370638		YBa2Cu3O7	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	6.98	6.98		1988																											2	Y123																				92					92																																																																																																					DETERMINATION OF THE MAGNETIC FIELD PENETRATION DEPTH IN SUPERCONDUCTING YTTRIUM BARIUM COPPER OXIDE: DEVIATIONS FROM THE BARDEEN-COOPER-SCHRIEFFER LAWS	198801	MAGNETIZATION            ,POWDER                   ,PENETRAT	PHYSICS DEPARTMENT AND SOLID STATE SCIENCE CENTER,UNIVERSITY OF CALIFORNIA,LOS ANGELES,CALIFORNIA	PHYS.REV.B,37(1988)638	B.DUNN,C.T.CHU,G.GRUNER,J.R.COOPER,L.W.ZHOU		
384	JJP0261953		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	6			1987																												Y123																																																																																		16.4																																												LOW TEMPERATURE SPECIFIC HEAT AND ELECTRICAL RESISTIVITY IN ORTHORHOMBIC Y(1)BA(2)CU(3)O(6.8) AND TETRAGONAL Y(1)BA(2)CU(3)O(6.0)	198712	RESISTIVITY              ,SPECIFIC HEAT	NATIONAL RESEARCH INSTITUTE FOR METALS,NAKAMEGURO,TOKYO	JJAP.LETT.,26(1987)L1953	AKIYUKI MATSUSHITA,KAZUHIRO KIMURA,KEIICHI OGAWA,SHIGERU TAKAYANAGI,TAKEHIKO MATSUMOTO,TAKESHI HATANO,TAMIO OGUCHI	Y,BA,CU,O	
385	JJP0261953		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8	6.8		1987																												Y123																																																																																		10.2																																												LOW TEMPERATURE SPECIFIC HEAT AND ELECTRICAL RESISTIVITY IN ORTHORHOMBIC Y(1)BA(2)CU(3)O(6.8) AND TETRAGONAL Y(1)BA(2)CU(3)O(6.0)	198712	RESISTIVITY              ,SPECIFIC HEAT	NATIONAL RESEARCH INSTITUTE FOR METALS,NAKAMEGURO,TOKYO	JJAP.LETT.,26(1987)L1953	AKIYUKI MATSUSHITA,KAZUHIRO KIMURA,KEIICHI OGAWA,SHIGERU TAKAYANAGI,TAKEHIKO MATSUMOTO,TAKESHI HATANO,TAMIO OGUCHI	Y,BA,CU,O	
386	JJP0261982		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7-Z	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7-Z			1987																												Y123																				70					70																																																																																																					SUPERCONDUCTIVITY IN IMPURITY-INDUCED TETRAGONAL Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z)	198712	IMPURITY                 ,STRUCTURE                ,TC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA	JJAP.LETT.,26(1987)L1982	MASATSUN.KATO,TOSHIZO FUJITA,YOSHITERU MAENO,YUJI AOKI	Y,BA,CU,FE,O	
387	JJP0262034		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																				94.7					94.7																																4.1																																																																					UPPER CRITICAL FIELD AND ITS ANISOTROPY OF EU(1)BA(2)CU(3)O(7-X) AND GD(1)BA(2)CU(3)O(7-X) STUDIED IN PREFERENTIALLY ORIENTED PELLETS	198712	HC                       ,ANISOTROPY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP.LETT.,26(1987)L2034	HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	EU,BA,CU,O,GD,BA,CU,O	
388	JJP0262034		ErBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																				94.5					94.5																																4.2	2.6																																																																				UPPER CRITICAL FIELD AND ITS ANISOTROPY OF EU(1)BA(2)CU(3)O(7-X) AND GD(1)BA(2)CU(3)O(7-X) STUDIED IN PREFERENTIALLY ORIENTED PELLETS	198712	HC                       ,ANISOTROPY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP.LETT.,26(1987)L2034	HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	EU,BA,CU,O,GD,BA,CU,O	
389	JJP0262080			Bi1Sr1Cu1OX	Bi	1	Sr	1	Cu	1															O	X			1987																																															4.6	6.5	8				6.5																																																																																																					SUPERCONDUCTIVITY IN THE BI-SR-CU-O SYSTEM	198712	RESISTIVITY              ,PREPARATION	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,26(1987)L2080	AKIRA YAMAZAKI,HIDEO FUJIKI,HIROSHI SAWA,JUN AKIMITSU	BI,SR,CU,O	
390	JJP0262076		NdBa2Cu3O7	Nd1Ba2Cu3OX	Nd	1	Ba	2	Cu	3															O	X			1987																												Y123																				90					90																																																																														4.8																							THE OXYGEN-DEFICIENT PEROVSKITE SOLID SOLUTION ND(1+X)BA(2-X)CU(3)O(Y) AND ITS SUPERCONDUCTIVITY	198712	OXYGEN DEFECT            ,X-RAY                    ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,NAMIKI,IBARAKI	JJAP.LETT.,26(1987)L2076	HIROSHI NOZAKI,NOBUO IYI,SHUNJI TAKEKAWA,YOSHIO ISHIZAW	ND,BA,CU,O	
391	JJP0262076		Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3OX	Nd	1.2	Ba	1.8	Cu	3															O	X			1987																												Y123																				60					60																																																																														2																							THE OXYGEN-DEFICIENT PEROVSKITE SOLID SOLUTION ND(1+X)BA(2-X)CU(3)O(Y) AND ITS SUPERCONDUCTIVITY	198712	OXYGEN DEFECT            ,X-RAY                    ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,NAMIKI,IBARAKI	JJAP.LETT.,26(1987)L2076	HIROSHI NOZAKI,NOBUO IYI,SHUNJI TAKEKAWA,YOSHIO ISHIZAW	ND,BA,CU,O	
392	JJP0262076		Nd(Ba,Nd)Cu3O7	Nd1.08Ba1.92Cu3OX	Nd	1.08	Ba	1.92	Cu	3															O	X			1987																												Y123																				86					86																																																																														1.2																							THE OXYGEN-DEFICIENT PEROVSKITE SOLID SOLUTION ND(1+X)BA(2-X)CU(3)O(Y) AND ITS SUPERCONDUCTIVITY	198712	OXYGEN DEFECT            ,X-RAY                    ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,NAMIKI,IBARAKI	JJAP.LETT.,26(1987)L2076	HIROSHI NOZAKI,NOBUO IYI,SHUNJI TAKEKAWA,YOSHIO ISHIZAW	ND,BA,CU,O	
393	JJP0262076		Nd(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3OX	Nd	1.5	Ba	1.5	Cu	3															O	X			1987																												Y123																																																																																																											20																			THE OXYGEN-DEFICIENT PEROVSKITE SOLID SOLUTION ND(1+X)BA(2-X)CU(3)O(Y) AND ITS SUPERCONDUCTIVITY	198712	OXYGEN DEFECT            ,X-RAY                    ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,NAMIKI,IBARAKI	JJAP.LETT.,26(1987)L2076	HIROSHI NOZAKI,NOBUO IYI,SHUNJI TAKEKAWA,YOSHIO ISHIZAW	ND,BA,CU,O	
394	JJP0262076		Nd(Ba,Nd)2Cu3O7	Nd1.32Ba1.68Cu3OX	Nd	1.32	Ba	1.68	Cu	3															O	X			1987																												Y123																				20					20																																																																														8																							THE OXYGEN-DEFICIENT PEROVSKITE SOLID SOLUTION ND(1+X)BA(2-X)CU(3)O(Y) AND ITS SUPERCONDUCTIVITY	198712	OXYGEN DEFECT            ,X-RAY                    ,RESISTIV	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,NAMIKI,IBARAKI	JJAP.LETT.,26(1987)L2076	HIROSHI NOZAKI,NOBUO IYI,SHUNJI TAKEKAWA,YOSHIO ISHIZAW	ND,BA,CU,O	
395	SSC0660413		YBa2(Cu,Mo)3O7	Y1Ba2Cu2.97Mo0.03OX	Y	1	Ba	2	Cu	2.97	Mo	0.03													O	X			1988																												Y123				3.826	3.882	11.706														76					76																																																																														0.75				1.6																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
396	SSC0660413		YBa2(Cu,Mo)3O7	Y1Ba2Cu2.94Mo0.06OX	Y	1	Ba	2	Cu	2.94	Mo	0.06													O	X			1988																												Y123				3.841	3.878	11.724														63					63																																																																														1.3				2.3																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
397	SSC0660413		YBa2(Cu,Mo)3O7	Y1Ba2Cu2.895Mo0.105OX	Y	1	Ba	2	Cu	2.895	Mo	0.105													O	X			1988																												Y123				3.855	3.868	11.73														52.5					52.5																																																																																		3.25																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
398	SSC0660413		YBa2(Cu,Mo)3O7	Y1Ba2Cu2.85Mo0.15OX	Y	1	Ba	2	Cu	2.85	Mo	0.15													O	X			1988																												Y123				3.362	3.864	11.736														50					50																																																																																		5																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
399	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03OX	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	X			1988																												Y123				3.819	3.885	11.691														79					79																																																																														0.6				1.05																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
400	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06OX	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	X			1988																												Y123				3.818	3.883	11.688														62					62																																																																														0.75				1.2																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
401	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.895Zn0.105OX	Y	1	Ba	2	Cu	2.895	Zn	0.105													O	X			1988																												Y123				3.82	3.886	11.688														52					52																																																																														1				1.3																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
402	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15OX	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	X			1988																												Y123				3.82	3.886	11.685														38					38																																																																														1.4				1.76																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
403	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.775Zn0.225OX	Y	1	Ba	2	Cu	2.775	Zn	0.225													O	X			1988																												Y123				3.823	3.888	11.685																																																																																														4.5							3.2																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
404	SSC0660413		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3OX	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	X			1988																												Y123				3.823	3.883	11.685																																																																																														11							6.5																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
405	SSC0660413		YBa2(Cu,Al)3O7	Y1Ba2Cu2.97Al0.03OX	Y	1	Ba	2	Cu	2.97	Al	0.03													O	X			1988																												Y123				3.826	3.882	11.691														81					81																																																																														0.5				1.1																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
406	SSC0660413		YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06OX	Y	1	Ba	2	Cu	2.94	Al	0.06													O	X			1988																												Y123				3.833	3.88	11.703														58					58																																																																														1.2				2.1																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
407	SSC0660413		YBa2(Cu,Al)3O7	Y1Ba2Cu2.885Al0.105OX	Y	1	Ba	2	Cu	2.885	Al	0.105													O	X			1988																												Y123				3.848	3.871	11.712														42					42																																																																																		3.5																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
408	SSC0660413		YBa2(Cu,Al)3O7	Y1Ba2Cu2.85Al0.15OX	Y	1	Ba	2	Cu	2.85	Al	0.15													O	X			1988																												Y123				3.854	3.866	11.715														33					33																																																																																		3.75																			EFFECT OF NONMAGNETIC IMPURITIES OF AL,MO AND ZN ON THE SUPERCONDUCTIVITY OF BA(2)Y(1)CU(3)O(7)	198804	SUBSTITUTION             ,RESISTIVITY              ,TC	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO	SOLID STATE COMMUN.,66(1988)413	M.ISHIKAWA,T.TAKABATAKE	Y,BA,CU,O	
409	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3OX	Y	1	Ba	1.95	La	0.05	Cu	3													O	X			1988																												Y123				3.82	3.89	11.675														91					91																																																																																		3.5																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
410	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3OX	Y	1	Ba	1.9	La	0.1	Cu	3													O	X			1988																												Y123				3.827	3.893	11.678																																																																																																																								BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
411	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.85La0.15Cu3OX	Y	1	Ba	1.85	La	0.15	Cu	3													O	X			1988																												Y123				3.825	3.892	11.681														88					88																																																																																		1.6																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
412	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3OX	Y	1	Ba	1.8	La	0.2	Cu	3													O	X			1988																												Y123				3.827	3.89	11.669																																																																																																																								BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
413	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.75La0.25Cu3OX	Y	1	Ba	1.75	La	0.25	Cu	3													O	X			1988																												Y123				3.83	3.889	11.669														76					76																																																																																		2.6																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
414	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3OX	Y	1	Ba	1.7	La	0.3	Cu	3													O	X			1988																												Y123				3.843	3.881	11.644																																																																																																					5																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
415	PRB0375912		Y(Ba,La)Cu3O7	Y1Ba1.65La0.35Cu3OX	Y	1	Ba	1.65	La	0.35	Cu	3													O	X			1988																												Y123				3.852	3.873	11.624														64					64																																																																																		5.3																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
416	PRB0375912		Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3O7-Z	Y	1	Ba	1.6	La	0.4	Cu	3													O	7-Z			1988																												Y123				3.867		11.598																																																																																																					8.8																			BA(2-X)LA(X)Y(1)CU(3)O(7+-Z) PEROVSKITE COMPOUNDS:CRYSTAL CHEMISTRY	198804	CRYSTAL STRUCTURE        ,RESISTIVITY              ,X-RAY                    ,OX	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5912	A.RAMIREZ,B.BATLOGG,E.A.RIETMAN,R.B.VAN DOVER,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.M.ZAHURAK	Y,BA,LA,CU,O	
417	JJP0261956		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123				3.83	3.89	11.67													92	92.5	93				92.5																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
418	JJP0261956		NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			1987						3.1	-22.6																					Y123				3.812	3.907	11.741													60	67	75				67																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
419	JJP0261956		SmBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z			1987						0.7	-17.9																					Y123				3.858	3.916	11.704													71	76	90				76																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
420	JJP0261956		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z			1987																												Y123				3.84	3.9	11.704													87	92	94				92																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
421	JJP0261956		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1987						8	-12.7																					Y123				3.843	3.898	11.717													82	86	93				86																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
422	JJP0261956		DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1987						10.7	-12.1																					Y123				3.829	3.895	11.68													90	92	93				92																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
423	JJP0261956		HoBa2Cu3O7	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z			1987						9.7	-10.3																					Y123				3.824	3.89	11.664													90	91	93				91																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
424	JJP0261956		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1987						9.3	-12.3																					Y123				3.829	3.884	11.652													90	91	93				91																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
425	JJP0261956		TmBa2Cu3O7	Tm1Ba2Cu3O7-Z	Tm	1	Ba	2	Cu	3															O	7-Z			1987						7.9	-13																					Y123				3.82	3.88	11.66													90	92	95				92																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
426	JJP0261956		YbBa2Cu3O7	Yb1Ba2Cu3O7-Z	Yb	1	Ba	2	Cu	3															O	7-Z			1987						4.5	-2.4																					Y123				3.382	3.87	11.66													90	91	95				91																																																																																																					EXPERIMENTS ON SUPERCONEDUCTING (RARE EARTH)-BA(2)CU(3)O(7-Z) DOWN TO 30 MK	198712	SUSCEPTIBILITY           ,STRUCTURE	FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	JJAP.LETT.,26(1987)L1956	HARUHISA TOYODA,HIROSHI FUJITA,ICHIRO NAKAD,KOHICHI UEDA,KUNISUKE ASAYAMA,TAKAO KOHARA,TETUYUKI KANEKO,YASUKAGE ODA,YOSHIHIRO YAMADA	R,BA,CU,O	
427	JJP0271123		YBa2(Cu,Co)3O7	Y1Ba2Cu2Co1OX	Y	1	Ba	2	Cu	2	Co	1													O	X			1988							-52.8																					Y123				3.89		11.66																																																																																																																								MAGNETIC PROPERTY OF Y(1)BA(2)CU(2)CO(1)O(Y)	198806	SUSCEPTIBILITY           ,LOW DIMENSIONA	DEPARTMENT OF PHYSICS,FACULTY OF ENGINEERING,YOKOHAMA NATIONAL UNIVERSITY,TOKIWADAI	JJAP.LETT.,27(1988)L1123	NAHONORI MIYATA,SHUICHI HIRABAYASHI,YOSHIHIDE KIMISHIMA	Y,BA,CU,CO,O	
428	JJP0271104		YBa2Cu3HxO7	Y1Ba2Cu3HO7-X	Y	1	Ba	2	Cu	3	H														O	7-X			1988																												Y123				3.822	3.892	11.67													87.5		92.5				90																																																																																		6.3																			EFFECTS OF HYDROGEN ION IMPLANTATION ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7-X)	198806	ION IMPLANTATION         ,RES                      ,STRUCTUR	HITACHI RESEARCH LABORATORY,HITACHI LTD.,HITACHI,IBARAKI	JJAP.LETT.,27(1988)L1104	JIRO KUNIYA,KATSUHISA USAMI,SHIN-PEI MATSUDA,TAKAHIKO KATO	Y,BA,CU,O	
429	JJP0271104		YBa2Cu3HxO7	Y1Ba2Cu3HO7-X	Y	1	Ba	2	Cu	3	H														O	7-X			1988																												Y123				3.862		11.76													34.8		51.3				43.05																																																																																		58																			EFFECTS OF HYDROGEN ION IMPLANTATION ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7-X)	198806	ION IMPLANTATION         ,RES                      ,STRUCTUR	HITACHI RESEARCH LABORATORY,HITACHI LTD.,HITACHI,IBARAKI	JJAP.LETT.,27(1988)L1104	JIRO KUNIYA,KATSUHISA USAMI,SHIN-PEI MATSUDA,TAKAHIKO KATO	Y,BA,CU,O	
430	JJP0271104		YBa2Cu3HxO7	Y1Ba2Cu3HO7-X	Y	1	Ba	2	Cu	3	H														O	7-X			1988																											2	Y123				3.68		11.73																																																																																																					1400																			EFFECTS OF HYDROGEN ION IMPLANTATION ON SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3)O(7-X)	198806	ION IMPLANTATION         ,RES                      ,STRUCTUR	HITACHI RESEARCH LABORATORY,HITACHI LTD.,HITACHI,IBARAKI	JJAP.LETT.,27(1988)L1104	JIRO KUNIYA,KATSUHISA USAMI,SHIN-PEI MATSUDA,TAKAHIKO KATO	Y,BA,CU,O	
431	PRL0591860		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1987																												Y123																				92					92																																																8.3																																																					Evidence for Two Pairing Energies from Nuclear Spin-Lattice Relaxation in Superconducting Ba2YCu3O7-delta	198710		AT & T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.59(1987)1860	G.F. Brennert,G.P. Espinosa,J.P. Remeika,Jr., R.E. Walstedt,W.W. Warren		
432	NU0570030		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1988																												Y123																				92					92																																																12																																																					NUCLEAR RELAXATION AND KNIGHT SHIFT STUDIES OF COPPER IN Y(1)BA(2)CU(3)O(7-Y)	1	NMR                      ,NQR	DEPARTMENT OF MATERIAL PHYSICS,FACULTY OF ENGINEERING SCIENCE,OSAKA UNIVERSITY,TOYONAKA,OSAKA	J.PHYS.SOC.JAPAN,57(1988)30	KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,TAKAYUKI KONDO,YOSHIO KITAOKA	Y,BA,CU,O	
433	PRB0375820		GdBa2Cu3(O,S)7	Gd1Ba2Cu3S1O6	Gd	1	Ba	2	Cu	3	S	1													O	6			1988						8.33	-12																					Y123				3.899		11.85																																																																																																																								EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
434	PRB0375820		TbBa2Cu3O7	Tb1Ba2Cu3O7	Tb	1	Ba	2	Cu	3															O	7			1988						9.7	-50																					Y123				8.572																																																																																																																										EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
435	PRB0375820		TbBa2Cu3(O,S)7	Tb1Ba2Cu3S1O6	Tb	1	Ba	2	Cu	3	S	1													O	6			1988						8.23	-40																					Y123				8.572																																																																																																																										EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
436	PRB0375828		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																			90		96				93																																																																														5.4				7.92																			TRANSPORT CRITICAL CURRENT IN RARE-EARTH-SUBSTITUTED SUPERCONDUCTORS R(1)BA(2)CU(3)O(7-Z)(R=GD,DY,SM,HO,Y)	198804	CRITICAL CURRENT         ,MAGNETIC FIELD	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5828	R.A.FASTNACHT,R.C.SHERWOOD,S.JIN,T.H.TIEFEL	R,BA,CU,O	
437	PRB0375828		DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																			92		96				94																																																																														0.84				1.95																			TRANSPORT CRITICAL CURRENT IN RARE-EARTH-SUBSTITUTED SUPERCONDUCTORS R(1)BA(2)CU(3)O(7-Z)(R=GD,DY,SM,HO,Y)	198804	CRITICAL CURRENT         ,MAGNETIC FIELD	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5828	R.A.FASTNACHT,R.C.SHERWOOD,S.JIN,T.H.TIEFEL	R,BA,CU,O	
438	PRB0375828		SmBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																			90		94				92																																																																														1.8				4.44																			TRANSPORT CRITICAL CURRENT IN RARE-EARTH-SUBSTITUTED SUPERCONDUCTORS R(1)BA(2)CU(3)O(7-Z)(R=GD,DY,SM,HO,Y)	198804	CRITICAL CURRENT         ,MAGNETIC FIELD	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5828	R.A.FASTNACHT,R.C.SHERWOOD,S.JIN,T.H.TIEFEL	R,BA,CU,O	
439	PRB0375828		HoBa2Cu3O7	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																			92		95				93.5																																																																														1.44				3.07																			TRANSPORT CRITICAL CURRENT IN RARE-EARTH-SUBSTITUTED SUPERCONDUCTORS R(1)BA(2)CU(3)O(7-Z)(R=GD,DY,SM,HO,Y)	198804	CRITICAL CURRENT         ,MAGNETIC FIELD	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5828	R.A.FASTNACHT,R.C.SHERWOOD,S.JIN,T.H.TIEFEL	R,BA,CU,O	
440	PRB0375828		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																			91		96				93.5																																																																														0.38				0.81																			TRANSPORT CRITICAL CURRENT IN RARE-EARTH-SUBSTITUTED SUPERCONDUCTORS R(1)BA(2)CU(3)O(7-Z)(R=GD,DY,SM,HO,Y)	198804	CRITICAL CURRENT         ,MAGNETIC FIELD	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)5828	R.A.FASTNACHT,R.C.SHERWOOD,S.JIN,T.H.TIEFEL	R,BA,CU,O	
441	PRB0375820		NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7			1988						3.53	-36																					Y123				3.873	3.906	11.73														88					88																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
442	PRB0375820		NdBa2Cu3(O,S)7	Nd1Ba2Cu3S1O6	Nd	1	Ba	2	Cu	3	S	1													O	6			1988						3.58	-40																					Y123				3.879		11.69														69					69																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
443	PRB0375820		NdBa2Cu3(O,S)7	Nd1Ba2Cu3S1O5	Nd	1	Ba	2	Cu	3	S	1													O	5			1988						3.64	-57																					Y123				3.897		11.69														56					56																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
444	PRB0375820		EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7			1988						3.05	-12																					Y123				3.821	3.884	11.61														92					92																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
445	PRB0375820		EuBa2Cu3(O,S)7	Eu1Ba2Cu3S1O6	Eu	1	Ba	2	Cu	3	S	1													O	6			1988																												Y123				3.884		11.65														85					85																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
446	PRB0375820		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1988						8.03																						Y123				3.844	3.897	11.7														92					92																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
447	PRB0375820		GdBa2Cu3(O,S)7	Gd1Ba2Cu3S1O6	Gd	1	Ba	2	Cu	3	S	1													O	6			1988						8.17																						Y123				3.887	3.911	11.72														92					92																																																																																																					EFFECT OF SULFUR ON THE SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7)	198804	SULFUR                   ,SUSCEPTIBILITY           ,STRUCTUR	LABORATOIRE L.NEEL,FRANCE	PHYS.REV.B,37(1988)5820	B.BARBARA,I.FELNER	R,BA,CU,O	
448	JJP0271101		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1988																												Y123																																																																																																																														FRACTURE TOUGHNESS MEASUREMENTS OF BA(2)Y(1)CU(3)O(7-X) SUPERCONDUCTING OXIDE BY MEANS OF INDENTATION TECHNIQUE	198806	FRACTURE TOUGHNESS       ,HARDNESS	DEPARTMENT OF METALLURGY,KYOTO UNIVERSITY,SAKYO-KU,KYOTO	JJAP.LETT.,27(1988)L1101	KOZO OSAMURA,SHOJIRO OCHIAI,TOMOO TAKAYAMA	Y,BA,CU,O	
449	JJP0271094			Bi2Sr1.8Ca1.6Cu2.3OX	Bi	2	Sr	1.8	Ca	1.6	Cu	2.3													O	X			1988																																																																											440										0.36	7.3																																																																				ANISOTROPIC UPPER CRITICAL FIELDS OF HIGHLY ORIENTED BI-SR-CA-CU-O THIN FILMS PREPARED BY COEVAPORATION	198806	THIN FILM                ,COEVAPORATION            ,CRITICAL	FUNDAMENTAL RESEARCH LABORATORIES,KAWASAKI	JJAP.LETT.,27(1988)L1094	HITOSHI IGARASHI,TAKASHI MANAKO,TETSURO SATOH,TSUTOMU YOSHITAKE,YOSHIMI KUBO	BI,SR,CA,CU,O	
450	PRB0375619		K(Ta,Nb)O3	K1Ta0.992Nb0.008O3	K	1	Ta	0.992	Nb	0.008															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
451	PRB0375619		K(Ta,Nb)O3	K1Ta0.988Nb0.012O3	K	1	Ta	0.988	Nb	0.012															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
452	PRB0375619		K(Ta,Nb)O3	K1Ta0.98Nb0.02O3	K	1	Ta	0.98	Nb	0.02															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
453	PRB0375619		K(Ta,Nb)O3	K1Ta0.91Nb0.09O3	K	1	Ta	0.91	Nb	0.09															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
454	PRB0375619		K(Ta,Nb)O3	K1Ta0.79Nb0.21O3	K	1	Ta	0.79	Nb	0.21															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
455	PRB0375619		K(Ta,Nb)O3	K1Ta0.64Nb0.36O3	K	1	Ta	0.64	Nb	0.36															O	3			1988																												ABO3																																																																																																																														EXPERIMENTAL AND THEORETICAL STUDY OF THE RAMAN SPECTRUM IN K(1)TA(1-X)NB(X)O(3) SOLID SOLUTIONS	198804	RAMAN	CENTRE LORRAIN D'OPTIQUE ET D'ELECTRONIQUE DU SOLIDE,ECOLE SUPERIEURE D'ELECTRICITE,FRANCE	PHYS.REV.B,37(1988)5619	D.RYTZ,G.E.KUGEL,H.MESLI,M.D.FONTANA	K,TA,NB,O	
456	PRB0375845		YBa2Cu3O7	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	X	6.54		1988																												Y123				3.882		11.826																																																																																																																								STRUCTURE OF THE HIGH-TC SUPERCONDUCTOR BA(2)Y(1)CU(3)O(X) AT 750-C USING NEUTRON DIFFRACTION	198804	CRYSTAL STRUCTURE        ,NEUTRON DIFFRA	INSTITUTE OF PHYSICS,ACADEMIA SINICA,CHINA	PHYS.REV.B,37(1988)5845	C.X.LIU,J.K.ZHAO,K.SUN,P.L.ZHANG,Q.W.YAN,S.W.NIU,T.S.NING,Y.N.WEI,Y.REN,Z.G.SHEN	Y,BA,CU,O	
457	PRB0375901		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-Z	6.96		1988																												Y123																																																																																																																														ANOMALOUS ULTRASOUND PROPAGATION IN HIGH-TC SUPERCONDUCTORS:LA(1.8)SR(0.2)CU(1)O(4-Y) AND Y(1)BA(2)CU(3)O(7-Z)	198804	ATTENUATION              ,SOUND VELOCITY	CORPORATE RESEARCH SCIENCE LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,37(1988)5901	A.J.JACOBSON,D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI,M.J.HIGGINS,S.BHATTACHARYA	LA,SR,CU,O,Y,BA,CU,O	
458	PRB0375901		(La,Sr)2CuO4	La1.8Sr0.2Cu1O3.95	La	1.8	Sr	0.2	Cu	1															O	4-Z	3.95		1988																												T																																																																																																																														ANOMALOUS ULTRASOUND PROPAGATION IN HIGH-TC SUPERCONDUCTORS:LA(1.8)SR(0.2)CU(1)O(4-Y) AND Y(1)BA(2)CU(3)O(7-Z)	198804	ATTENUATION              ,SOUND VELOCITY	CORPORATE RESEARCH SCIENCE LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,37(1988)5901	A.J.JACOBSON,D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI,M.J.HIGGINS,S.BHATTACHARYA	LA,SR,CU,O,Y,BA,CU,O	
459	JJP0271080		YBa2Cu3O7	Y1Ba2Cu3O6.89	Y	1	Ba	2	Cu	3															O	6.89	6.89		1988																												Y123																				92					92																																																																																																					EFFECTS OF SULFUR ADDITION ON THE SUPERCONDUCTIVITY OF Y-BA-CU-O COMPOUND	198806	TRANSITION TEMPERATURE   ,CRITICAL CURRENT         ,X-RAY	GOVERNMENT INDUSTRIAL RESEARCH INSTITUTE,OSAKA	JJAP.LETT.,27(1988)L1080	HIDEO TANIGAWA,ICHIRO MATSUBARA,SABURO KOSE,TORU OGURA	Y,BA,CU,O	
460	JJP0271080		YBa2Cu3(O,S)7	Y1Ba2Cu3S0.03O7.12	Y	1	Ba	2	Cu	3	S	0.03													O	7.12	7.12		1988																												Y123																				90					90																																																																																																					EFFECTS OF SULFUR ADDITION ON THE SUPERCONDUCTIVITY OF Y-BA-CU-O COMPOUND	198806	TRANSITION TEMPERATURE   ,CRITICAL CURRENT         ,X-RAY	GOVERNMENT INDUSTRIAL RESEARCH INSTITUTE,OSAKA	JJAP.LETT.,27(1988)L1080	HIDEO TANIGAWA,ICHIRO MATSUBARA,SABURO KOSE,TORU OGURA	Y,BA,CU,O	
461	JJP0271080		YBa2Cu3(O,S)7	Y1Ba2Cu3S0.06O7.23	Y	1	Ba	2	Cu	3	S	0.06													O	7.23	7.23		1988																												Y123																				89					89																																																																																																					EFFECTS OF SULFUR ADDITION ON THE SUPERCONDUCTIVITY OF Y-BA-CU-O COMPOUND	198806	TRANSITION TEMPERATURE   ,CRITICAL CURRENT         ,X-RAY	GOVERNMENT INDUSTRIAL RESEARCH INSTITUTE,OSAKA	JJAP.LETT.,27(1988)L1080	HIDEO TANIGAWA,ICHIRO MATSUBARA,SABURO KOSE,TORU OGURA	Y,BA,CU,O	
462	JJP0271080		YBa2Cu3(O,S)7	Y1Ba2Cu3S0.12O7.28	Y	1	Ba	2	Cu	3	S	0.12													O	7.28	7.28		1988																												Y123																				89					89																																																																																																					EFFECTS OF SULFUR ADDITION ON THE SUPERCONDUCTIVITY OF Y-BA-CU-O COMPOUND	198806	TRANSITION TEMPERATURE   ,CRITICAL CURRENT         ,X-RAY	GOVERNMENT INDUSTRIAL RESEARCH INSTITUTE,OSAKA	JJAP.LETT.,27(1988)L1080	HIDEO TANIGAWA,ICHIRO MATSUBARA,SABURO KOSE,TORU OGURA	Y,BA,CU,O	
463	SSC0661215		YBa2Cu3O7	Y1Ba2Cu3OY	Y	1	Ba	2	Cu	3															O	Y			1988																												Y123				3.813	3.882	11.656														91.9					91.9																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
464	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.975Zn0.025OY	Y	1	Ba	2	Cu	2.975	Zn	0.025													O	Y			1988																												Y123				3.809	3.882	11.653														82.8					82.8																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
465	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.95Zn0.05OY	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	Y			1988																												Y123				3.805	3.876	11.626														74.7					74.7																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
466	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.925Zn0.075OY	Y	1	Ba	2	Cu	2.925	Zn	0.075													O	Y			1988																												Y123				3.815	3.888	11.663														64.9					64.9																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
467	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1OY	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	Y			1988																												Y123				3.816	3.884	11.644														57.6					57.6																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
468	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15OY	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	Y			1988																												Y123				3.816	3.887	11.666														56					56																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
469	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2OY	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	Y			1988																												Y123				3.818	3.885	11.651														56.5					56.5																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
470	SSC0661215		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3OY	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	Y			1988																												Y123				3.825	3.885	11.644														47.6					47.6																																																																																																					ELECTRONIC STATE AND SUPERCONDUCTIVITY IN Y(1)BA(2)CU(3-X)ZN(X)O(Y) SYSTEM	198806	X-RAY                    ,RES                      ,HALL EFF	DEPARTMENT OF PHYSICS,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,P.R.CHINA	SOLID STATE COMMUN.,66(1988)1215	CHEN ZUYAO,HE ZHENHUI,SUN SHIFANG,XIA JIANSHENG,ZHANG HAN,ZHANG QIRUI	Y,BA,CU,ZN,O	
471	JJP0271307		GdBa2Cu3O7	Gd1Ba2Cu3O6.9	Gd	1	Ba	2	Cu	3															O	Z	6.9		1988						7.79																						Y123																				92					92																																																																																																					MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
472	JJP0271307		GdBa2Cu3O7	Gd1Ba2Cu3O6.3	Gd	1	Ba	2	Cu	3															O	Z	6.3		1988						7.82	2.35																				2	Y123				3.886		11.808																																																																																																																								MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
473	JJP0271307		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O6.9	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	Z	6.9		1988																												Y123																				41					41																																																																																																					MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
474	JJP0271307		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O6.3	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	Z	6.3		1988						8.29	2.3																				2	Y123				3.892		11.778																																																																																																																								MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
475	JJP0271307		GdBa2(Cu,Co)3O7	Gd1Ba2Cu2.7Co0.3O6.9	Gd	1	Ba	2	Cu	2.7	Co	0.3													O	Z	6.9		1988						8.07																					2	Y123																				33					33																																																																																																					MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
476	JJP0271307		GdBa2(Cu,Co)3O7	Gd1Ba2Cu2.7Co0.3O6.3	Gd	1	Ba	2	Cu	2.7	Co	0.3													O	Z	6.3		1988						8.04	2.25																				2					3.892		11.76																																																																																																																								MAGNETIC PROPERTIES OF GD(1)BA(2)CU(2.7)M(0.3)O(Y) (M=CU,FE AND CO): MAGNETIC ORDERING OF M IN CU(1) SITE	198807	MAGNETIZATION            ,SUSCEPTIBILITY	ELECTROTECHNICAL LABORATORY,TSUKUBA	JJAP.LETT.,27(1988)L1307	SHINYA WAKI,YUJI YAMAGUCHI	GD,BA,CU,M,O	
477	PRB0380889		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9		1988																												Y123				3.846	3.883	11.661														91					91																																																																																																					ANOMALOUS VARIATION OF THE C LATTICE PARAMETER OF A SAMPLE OF Y(1)BA(2)CU(3)O(7-Z) THROUGH THE SUPERCONDUCTING TRANSITION	198807	LATTICE CONSTANT         ,X-RAY	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS,INDIA	PHYS.REV.B,38(1988)889	G.V.SUBBA RAO,K.S.GIRIRAJAN,R.SRINIVASAN,V.GANESAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,O	
478	PRB0380893		Bi2Sr2CaCu2O8	Bi2.2Sr2Ca0.8Cu2O8+Z	Bi	2.2	Sr	2	Ca	0.8	Cu	2													O	8+Z			1988																												Bi2212				5.414	5.418	30.89													84		90				87																																																																														0.04				0.13																			STRUCTURE AND PHYSICAL PROPERTIES OF SINGLE CRYSTALS OF THE 84-K SUPERCONDUCTOR BI(2.2)SR(2)CA(0.8)CU(2)O(8+Z)	198807	SINGLE CRYSTAL           ,X-RAY                    ,SUSCEPTIBILITY           ,RESISTIVITY	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,38(1988)893	B.BATLOGG,D.W.MURPHY,J.H.MARSHALL,J.J.KRAJEWSKI,J.V.WASZCZAK,JR.,L.F.SCHNEEMEYER,L.W.RUPP,P.MARSH,R.B.VAN DOVER,R.FARROW,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.H.GLARUM,S.M.ZAHURAK,S.NAKAHARA,T.SIEGRIST,W.F.PECK	BI,SR,CA,CU,O	
479	PRB0380893		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.5Ni0.5O7	Y	1	Ba	2	Cu	2.5	Ni	0.5													O	7			1988						0.87	-4																					Y123				3.82	3.883	11.647														52.3					52.3																																																																														2.5																							STRUCTURE AND PHYSICAL PROPERTIES OF SINGLE CRYSTALS OF THE 84-K SUPERCONDUCTOR BI(2.2)SR(2)CA(0.8)CU(2)O(8+Z)	198807	SINGLE CRYSTAL           ,X-RAY                    ,SUSCEPTIBILITY           ,RESISTIVITY	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,38(1988)893	B.BATLOGG,D.W.MURPHY,J.H.MARSHALL,J.J.KRAJEWSKI,J.V.WASZCZAK,JR.,L.F.SCHNEEMEYER,L.W.RUPP,P.MARSH,R.B.VAN DOVER,R.FARROW,R.J.CAVA,R.M.FLEMING,S.A.SUNSHINE,S.H.GLARUM,S.M.ZAHURAK,S.NAKAHARA,T.SIEGRIST,W.F.PECK	BI,SR,CA,CU,O	
480	PHF0180095		La(Ba,La)2Cu3O7	La3Ba3Cu6O14.37	La	3	Ba	3	Cu	6															O	X	14.37		1988																												Y123				3.9		11.696																																																																																																																								SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
481	PHF0180095		La(Ba,La)2Cu3O7	La2.8Ba3.2Cu6O14.07	La	2.8	Ba	3.2	Cu	6															O	X	14.07		1988																												Y123				3.902		11.713														13					13																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
482	PHF0180095		La(Ba,La)2Cu3O7	La2.6Ba3.4Cu6O14.06	La	2.6	Ba	3.4	Cu	6															O	X	14.06		1988																												Y123				3.903		11.714														26					26																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
483	PHF0180095		La(Ba,La)2Cu3O7	La2.4Ba3.6Cu6O14.01	La	2.4	Ba	3.6	Cu	6															O	X	14.01		1988																												Y123				3.904		11.738														39					39																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
484	PHF0180095		La(Ba,La)2Cu3O7	La2.2Ba3.8Cu6O13.86	La	2.2	Ba	3.8	Cu	6															O	X	13.86		1988																												Y123				3.905		11.758														52					52																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
485	PHF0180095		LaBa2Cu3O7	La2Ba4Cu6O13.8	La	2	Ba	4	Cu	6															O	X	13.8		1988																												Y123				3.909		11.78														65					65																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
486	PHF0180095			Y1La2Ba3Cu6O14.53	Y	1	La	2	Ba	3	Cu	6													O	X	14.53		1988																																3.861		11.603														25.6					25.6																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
487	PHF0180095			Y1La1.8Ba3.2Cu6O14.49	Y	1	La	1.8	Ba	3.2	Cu	6													O	X	14.49		1988																												Y123				3.875		11.645														41.9					41.9																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
488	PHF0180095			Y1La1.6Ba3.4Cu6O14.38	Y	1	La	1.6	Ba	3.4	Cu	6													O	X	14.38		1988																												Y123				3.844	3.877	11.673														53.1					53.1																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
489	PHF0180095			Y1La1.4Ba3.6Cu6O14.2	Y	1	La	1.4	Ba	3.6	Cu	6													O	X	14.2		1988																												Y123				3.873	3.882	11.668														64					64																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
490	PHF0180095			Y1La1.2Ba3.8Cu6O14.07	Y	1	La	1.2	Ba	3.8	Cu	6													O	X	14.07		1988																											3	Y123				3.852	3.861	11.682														70.4					70.4																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
491	PHF0180095			Y1La1Ba4Cu6O13.95	Y	1	La	1	Ba	4	Cu	6													O	X	13.95		1988																											3	Y123				3.853	3.863	11.687														72.2					72.2																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
492	PHF0180095			Y2La2Ba2Cu6O14.45	Y	2	La	2	Ba	2	Cu	6													O	X	14.45		1988																												Y123																																																																																																																														SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
493	PHF0180095			Y2La1.8Ba2.2Cu6O14.54	Y	2	La	1.8	Ba	2.2	Cu	6													O	X	14.54		1988																												Y123				3.835	3.864	11.622																																																																																																																								SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
494	PHF0180095			Y2La1.6Ba2.4Cu6O14.39	Y	2	La	1.6	Ba	2.4	Cu	6													O	X	14.39		1988																												Y123				3.846	3.869	11.634																																																																																																																								SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
495	PHF0180095			Y2La1.4Ba2.6Cu6O14.42	Y	2	La	1.4	Ba	2.6	Cu	6													O	X	14.42		1988																												Y123				3.821	3.839	11.619																																																																																																																								SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
496	PHF0180095			Y2La1.2Ba2.8Cu6O14.27	Y	2	La	1.2	Ba	2.8	Cu	6													O	X	14.27		1988																												Y123				3.832	3.843	11.574																																																																																																																								SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
497	PHF0180095			Y2La1Ba3Cu6O14.17	Y	2	La	1	Ba	3	Cu	6													O	X	14.17		1988																												Y123				3.84	3.849	11.569														28					28																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
498	PHF0180095			Y2La0.8Ba3.2Cu6O14.2	Y	2	La	0.8	Ba	3.2	Cu	6													O	X	14.2		1988																												Y123				3.848		11.567														46					46																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
499	PHF0180095			Y2La0.6Ba3.4Cu6O14.02	Y	2	La	0.6	Ba	3.4	Cu	6													O	X	14.02		1988																												Y123				3.87		11.647														60					60																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
500	PHF0180095			Y2La0.4Ba3.6Cu6O13.91	Y	2	La	0.4	Ba	3.6	Cu	6													O	X	13.91		1988																												Y123				3.812	3.874	11.624														78					78																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
501	PHF0180095			Y2La0.2Ba3.8Cu6O13.92	Y	2	La	0.2	Ba	3.8	Cu	6													O	X	13.92		1988																												Y123				3.81	3.876	11.64														93					93																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
502	PHF0180095			Y2La0.15Ba3.85Cu6O13.99	Y	2	La	0.15	Ba	3.85	Cu	6													O	X	13.99		1988																												Y123																				93.2					93.2																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
503	PHF0180095			Y2La0.1Ba3.9Cu6O13.94	Y	2	La	0.1	Ba	3.9	Cu	6													O	X	13.94		1988																												Y123																				90					90																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
504	PHF0180095		YBa2Cu3O7	Y2Ba4Cu6O13.9	Y	2	Ba	4	Cu	6															O	X	13.9		1988																												Y123				3.817	3.884	11.666														93					93																																																																																																					SUPERCONDUCTIVITY IN THE SOLID SOLUTIONS Y(N)LA(2-N+X)BA(4-X)CU(6)O(14+Y) (N=0,1,2)	6	FABRICATION              ,SOLID SOLUTION           ,RESISTIV	DEPARTMENT OF CHEMISTRY,THE UNIVERSITY,SOUTHAMPTON,UK	J.PHYS.F,18(1988)95	C.E.MEATS,J.R.GRASMEDER,M.T.WELLER,P.C.LANCHESTER	Y,LA,BA,CU,O	
505	PRB0373734		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	X	6.94		1988																												Y123				3.824	3.89	11.679															97				97																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
506	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.975La0.025Cu3O6.95	Y	1	Ba	1.975	La	0.025	Cu	3													O	X	6.95		1988																												Y123				3.82	3.889	11.67															99				99																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
507	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3O6.9	Y	1	Ba	1.95	La	0.05	Cu	3													O	X	6.9		1988																												Y123				3.821	3.889	11.672															99				99																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
508	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.925La0.075Cu3O6.9	Y	1	Ba	1.925	La	0.075	Cu	3													O	X	6.9		1988																												Y123				3.827	3.885	11.659															99				99																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
509	PRB0373734		Y(Ba,La,)2Cu3O7	Y1Ba1.9La0.1Cu3O6.9	Y	1	Ba	1.9	La	0.1	Cu	3													O	X	6.9		1988																												Y123				3.83	3.883	11.653															95				95																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
510	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O6.95	Y	1	Ba	1.8	La	0.2	Cu	3													O	X	6.95		1988																												Y123				3.839	3.872	11.618															78				78																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
511	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3O7	Y	1	Ba	1.7	La	0.3	Cu	3													O	X	7		1988																												Y123				3.858	3.859	11.582															67				67																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
512	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3O7.05	Y	1	Ba	1.6	La	0.4	Cu	3													O	X	7.05		1988																												Y123				3.858	3.858	11.58															52				52																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
513	PRB0373734		Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3O7.08	Y	1	Ba	1.5	La	0.5	Cu	3													O	X	7.08		1988																												Y123				3.858		11.572															38				38																																																																																																					EVIDENCE FOR PEROXIDE FORMATION IN SUPERCONDUCTING Y(1)BA(2-X)LA(X)CU(3)O(7+-Z)	198803	OXYGEN CONTENT           ,LATTICE CONSTANT         ,RESISTIVITY              ,ST	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC,TEXAS	PHYS.REV.B,37(1988)3734	A.MANTHIRAM,J.B.GOODENOUGH,X.X.TANG	Y,BA,LA,CU,O	
514	SSC0670521		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X			1988						7.89	3.4																					Y123				3.838	3.9	11.699														89					89																																																																																																					SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
515	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.925Fe0.075OX	Gd	1	Ba	2	Cu	2.925	Fe	0.075													O	X			1988						8.08	1.8																					Y123				3.871	3.897	11.684														64					64																																																																																																					SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
516	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.85Fe0.15OX	Gd	1	Ba	2	Cu	2.85	Fe	0.15													O	X			1988						8.13	-4.3																					Y123				3.874	3.891	11.67														47					47																																																																																																					SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
517	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.775Fe0.225OX	Gd	1	Ba	2	Cu	2.775	Fe	0.225													O	X			1988						8.18	-3.8																					Y123				3.884	3.884	11.661														33					33																																																																																																					SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
518	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3OX	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	X			1988						8.23	2.7																					Y123				3.882	3.886	11.652														11					11																																																																																																					SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
519	SSC0640209		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123																				92					92																																																							3.036		21		400																																										SPECIFIC HEAT STUDIES OF HIGH-T(C) SUPERCONDUCTOR Y(1)BA(2)CU(3)0(7-X)		SPECIFIC HEAT            ,SUS                      ,RES	NATIONAL INSTITUTE OF METROLOGY,BEIJING,CHINA	SOLID STATE COMMUN.,64(1987)209	C.LI,D.YIN,F.LI,G.LU,K.WU,Q.LI,Y.ZHOU	Y,BA,CU,O	
520	SSC0640247		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123																				93					93																																2																							6.417		33		383																																										THERMAL AND MAGNETIC PROPERTIES OF SOME YBA2CU3O7-Z SAMPLES				SOLID STATE COMMUN.64(1987)247	B.BARBARA,C.AYACHE,E.BONJOUR,J.H.HENRY,J.ROSSAT-MIGNOD,M.COUACH,R.CALEMCZUK	Y,BA,CU,O	
521	PRB0362401		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123																			90.1	91.6					91.6																																																							4.129		37.3		440																																										MEASUREMENT OF THE SPECIFIC-HEAT ANOMALY AT THE SUPERCONDUCTING TRANSITION OF Y(1)BA(2)CU(3)O(7-Z)	198708	SPECIFIC HEAT            ,SUSCEPTIBILITY           ,SP                       ,SUS	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,URBANA,ILLINOIS	PHYS.REV.B,36(1987)2401	D.M.GINSBERG,M.B.SALAMON,S.E.INDERHEES,T.A.FRIEDMANN	Y,BA,CU,O	
522	SSC0661085		LaBa2Cu3O7	La1Ba2Cu3OX	La	1	Ba	2	Cu	3															O	X			1988																												Y123				3.913		11.617														34.5					34.5																																																																																																					RAMAN STUDIES ON LA(1)BA(2-X)CA(X)CU(3)O(Y) SYSTEM	198806	RAMAN	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY BEIJING,CHINA	SOLID STATE COMMUN.,66(1988)1085	CHONGDE WEI,HE-TIAN ZHOU,QIN LIN,SHU-LIN ZHANG	LA,BA,CA,CU,O	
523	SSC0661085		La(Ba,Ca)2Cu3O7	La1Ba1.75Ca0.25Cu3OX	La	1	Ba	1.75	Ca	0.25	Cu	3													O	X			1988																												Y123				3.885	3.892	11.54														71.7					71.7																																																																																																					RAMAN STUDIES ON LA(1)BA(2-X)CA(X)CU(3)O(Y) SYSTEM	198806	RAMAN	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY BEIJING,CHINA	SOLID STATE COMMUN.,66(1988)1085	CHONGDE WEI,HE-TIAN ZHOU,QIN LIN,SHU-LIN ZHANG	LA,BA,CA,CU,O	
524	SSC0661085		La(Ba,Ca)2Cu3O7	La1Ba1.25Ca0.75Cu3OX	La	1	Ba	1.25	Ca	0.75	Cu	3													O	X			1988																												Y123				3.858	3.875	11.488														78.2					78.2																																																																																																					RAMAN STUDIES ON LA(1)BA(2-X)CA(X)CU(3)O(Y) SYSTEM	198806	RAMAN	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY BEIJING,CHINA	SOLID STATE COMMUN.,66(1988)1085	CHONGDE WEI,HE-TIAN ZHOU,QIN LIN,SHU-LIN ZHANG	LA,BA,CA,CU,O	
525	SSC0661085		La(Ba,Ca)2Cu3O7	La1Ba1Ca1Cu3OX	La	1	Ba	1	Ca	1	Cu	3													O	X			1988																												Y123				3.827	3.844	11.474														80					80																																																																																																					RAMAN STUDIES ON LA(1)BA(2-X)CA(X)CU(3)O(Y) SYSTEM	198806	RAMAN	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY BEIJING,CHINA	SOLID STATE COMMUN.,66(1988)1085	CHONGDE WEI,HE-TIAN ZHOU,QIN LIN,SHU-LIN ZHANG	LA,BA,CA,CU,O	
526	SSC0661085		La(Ba,Ca)2Cu3O7	La1Ba0.5Ca1.5Cu3OX	La	1	Ba	0.5	Ca	1.5	Cu	3													O	X			1988																												Y123				3.846	3.865	11.476														36.7					36.7																																																																																																					RAMAN STUDIES ON LA(1)BA(2-X)CA(X)CU(3)O(Y) SYSTEM	198806	RAMAN	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY BEIJING,CHINA	SOLID STATE COMMUN.,66(1988)1085	CHONGDE WEI,HE-TIAN ZHOU,QIN LIN,SHU-LIN ZHANG	LA,BA,CA,CU,O	
527	SSC0661079		EuBa2Cu3O7	Eu1Ba2Cu3OX	Eu	1	Ba	2	Cu	3															O	X			1988																											3	Y123				3.845	3.903	11.71																																																																																																																								CRYSTAL-FIELD EFFECT ON MAGNETIC SUSCEPTIBILITY OF EU(1)BA(2)CU(3)O(Y)	198806	SUSCEPTIBILITY           ,SINGLE CRYSTAL           ,CRYSTAL	ELECTROTECHNICAL LABORATORY,TSUKUBA,IBARAKI	SOLID STATE COMMUN.,66(1988)1079	K.HAYASHI,M.TOKUMOTO,S.WAKI,Y.YAMAGUCHI	EU,BA,CU,O	
528	SSC0661079		EuBa2Cu3O7	Eu1Ba2Cu3OX	Eu	1	Ba	2	Cu	3															O	X			1988																											2	Y123				3.885		11.79																																																																																																																								CRYSTAL-FIELD EFFECT ON MAGNETIC SUSCEPTIBILITY OF EU(1)BA(2)CU(3)O(Y)	198806	SUSCEPTIBILITY           ,SINGLE CRYSTAL           ,CRYSTAL	ELECTROTECHNICAL LABORATORY,TSUKUBA,IBARAKI	SOLID STATE COMMUN.,66(1988)1079	K.HAYASHI,M.TOKUMOTO,S.WAKI,Y.YAMAGUCHI	EU,BA,CU,O	
529	PRB0375932		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2O7.04	Y	1	Ba	2	Cu	2.8	Co	0.2													O	X	7.04		1988																												Y123																				53					53																																																																																																					ROLE OF BOND LENGTHS IN THE 90-K SUPERCONDUCTOR: A NEUTRON POWDER-DIFFRACTION STUDY OF Y(1)BA(2)CU(3-X)CO(X)O(7-Y)	198804	NEUTRON DIFFRACTION      ,CU-O BOND	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,37(1988)5932	F.J.ROTELLA,J.D.JORGENSEN,J.M.TARASCON,L.H.GREENE,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
530	PRB0375932		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2O6.45	Y	1	Ba	2	Cu	2.8	Co	0.2													O	X	6.45		1988																												Y123																																																																																																																														ROLE OF BOND LENGTHS IN THE 90-K SUPERCONDUCTOR: A NEUTRON POWDER-DIFFRACTION STUDY OF Y(1)BA(2)CU(3-X)CO(X)O(7-Y)	198804	NEUTRON DIFFRACTION      ,CU-O BOND	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,37(1988)5932	F.J.ROTELLA,J.D.JORGENSEN,J.M.TARASCON,L.H.GREENE,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
531	PRB0375932		YBa2(Cu,Co)3O7	Y1Ba2Cu2.2Co0.8O7.3	Y	1	Ba	2	Cu	2.2	Co	0.8													O	X	7.3		1988																												Y123																																																																																																																														ROLE OF BOND LENGTHS IN THE 90-K SUPERCONDUCTOR: A NEUTRON POWDER-DIFFRACTION STUDY OF Y(1)BA(2)CU(3-X)CO(X)O(7-Y)	198804	NEUTRON DIFFRACTION      ,CU-O BOND	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,37(1988)5932	F.J.ROTELLA,J.D.JORGENSEN,J.M.TARASCON,L.H.GREENE,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
532	PRB0375932		YBa2(Cu,Co)3O7	Y1Ba2Cu2.2Co0.8O6.91	Y	1	Ba	2	Cu	2.2	Co	0.8													O	X	6.91		1988																												Y123																																																																																																																														ROLE OF BOND LENGTHS IN THE 90-K SUPERCONDUCTOR: A NEUTRON POWDER-DIFFRACTION STUDY OF Y(1)BA(2)CU(3-X)CO(X)O(7-Y)	198804	NEUTRON DIFFRACTION      ,CU-O BOND	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,37(1988)5932	F.J.ROTELLA,J.D.JORGENSEN,J.M.TARASCON,L.H.GREENE,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
533	JJP0271094			Bi2Sr2Ca2Cu3O	Bi	2	Sr	2	Ca	2	Cu	3													O				1988																																															103	111	115				111																						500										0.34	7																																																																				ANISOTROPIC UPPER CRITICAL FIELDS OF HIGHLY ORIENTED BI-SR-CA-CU-O THIN FILMS PREPARED BY COEVAPORATION	198806	THIN FILM                ,COEVAPORATION            ,CRITICAL	FUNDAMENTAL RESEARCH LABORATORIES,KAWASAKI	JJAP.LETT.,27(1988)L1094	HITOSHI IGARASHI,TAKASHI MANAKO,TETSURO SATOH,TSUTOMU YOSHITAKE,YOSHIMI KUBO	BI,SR,CA,CU,O	
534	JJP0271094			Bi2Sr2Ca1Cu2O	Bi	2	Sr	2	Ca	1	Cu	2													O				1988																																															82	87	91				87																						400										0.36	7.3																																																																				ANISOTROPIC UPPER CRITICAL FIELDS OF HIGHLY ORIENTED BI-SR-CA-CU-O THIN FILMS PREPARED BY COEVAPORATION	198806	THIN FILM                ,COEVAPORATION            ,CRITICAL	FUNDAMENTAL RESEARCH LABORATORIES,KAWASAKI	JJAP.LETT.,27(1988)L1094	HITOSHI IGARASHI,TAKASHI MANAKO,TETSURO SATOH,TSUTOMU YOSHITAKE,YOSHIMI KUBO	BI,SR,CA,CU,O	
535	PRB0382432		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	X	6		1988																												Y123				3.857		11.819																																																																																																																								SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
536	PRB0382432		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	X	7		1988																												Y123				3.822	3.892	11.674														92					92																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
537	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.97Co0.03O6.96	Y	1	Ba	2	Cu	2.97	Co	0.03													O	X	6.96		1988																												Y123				3.824	3.889	11.677														92					92																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
538	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.925Co0.075O6.97	Y	1	Ba	2	Cu	2.925	Co	0.075													O	X	6.97		1988																												Y123																				92					92																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
539	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15O7.03	Y	1	Ba	2	Cu	2.85	Co	0.15													O	X	7.03		1988																												Y123				3.869		11.701														65					65																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
540	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.775Co0.225O6.99	Y	1	Ba	2	Cu	2.775	Co	0.225													O	X	6.99		1988																												Y123				3.873		11.647														58					58																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
541	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.7Co0.3O7.11	Y	1	Ba	2	Cu	2.7	Co	0.3													O	X	7.11		1988							-17																					Y123				3.878		11.648														36					36																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
542	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.55Co0.45O7.26	Y	1	Ba	2	Cu	2.55	Co	0.45													O	X	7.26		1988																												Y123				3.88		11.659																																																																																																																								SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
543	PRB0382432		YBa2(Cu,Co)3O7	Y1Ba2Cu2.4Co0.6OX	Y	1	Ba	2	Cu	2.4	Co	0.6													O	X			1988																												Y123				3.884		11.647																																																																																																																								SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
544	PRB0382432		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7.01	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	X	7.01		1988																												Y123				3.835	3.897	11.686														85					85																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
545	PRB0382432		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.84	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	X	6.84		1988																												Y123				3.832	3.894	11.684														75					75																																1.5																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
546	PRB0382432		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O6.88	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	X	6.88		1988							20																					Y123				3.827	3.889	11.671														73					73																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
547	PRB0382432		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.4Ni0.6O6.94	Y	1	Ba	2	Cu	2.4	Ni	0.6													O	X	6.94		1988																												Y123				3.822	3.88	11.61														66					66																																																																																																					SYNTHESIS AND CHARACTERIZATION OF Y(1)BA(2)(CU(1-X)M(X))(3)O(7-Z) (M=CO,NI): CRYSTAL SYMMETRY,SUPERCONDUCTIVITY,AND THE ROLE OF OXYGEN	198808	OXYGEN CONTENT           ,PHASE TRANSITION         ,SUSCEPTIBILITY           ,CR	DEPARTMENT OF CHEMISTRY,UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)2432	B.A.AVERILL,J.F.BRINGLEY,K.M.WONG,S.J.POON,T.-M.CHEN	Y,BA,CU,M,O	
548	PRB0364047		La2SrO4	La2Sr1O4.003	La	2	Sr	1																	O	X	4.003		1987																												T																																																																																																																														CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
549	PRB0364047		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4.002	La	1.96	Sr	0.04	Cu	1															O	X	4.002		1987																												T																																																																																																																														CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
550	PRB0364047		(La,Sr)2CuO4	La1.94Sr0.06Cu1O3.995	La	1.94	Sr	0.06	Cu	1															O	X	3.995		1987																												T																				6.5					6.5																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
551	PRB0364047		(La,Sr)2CuO4	La1.92Sr0.08Cu1O3.994	La	1.92	Sr	0.08	Cu	1															O	X	3.994		1987																												T																				20.3					20.3																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
552	PRB0364047		(La,Sr)2CuO4	La1.89Sr0.11Cu1O3.986	La	1.89	Sr	0.11	Cu	1															O	X	3.986		1987																												T																				29.2					29.2																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
553	PRB0364047		(La,Sr)2CuO4	La1.855Sr0.145Cu1O4	La	1.855	Sr	0.145	Cu	1															O	X	4		1987																												T																				34.9					34.9																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
554	PRB0364047		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	X	4		1987																												T																				35.2					35.2																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
555	PRB0364047		(La,Sr)2CuO4	La1.815Sr0.185Cu1O3.964	La	1.815	Sr	0.185	Cu	1															O	X	3.964		1987																												T																				33.2					33.2																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
556	PRB0364047		(La,Sr)2CuO4	La1.81Sr0.19Cu1O3.949	La	1.81	Sr	0.19	Cu	1															O	X	3.949		1987																												T																																																																																																																														CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
557	PRB0364047		(La,Sr)2CuO4	La1.78Sr0.22Cu1O3.945	La	1.78	Sr	0.22	Cu	1															O	X	3.945		1987																												T																				34.8					34.8																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
558	PRB0364047		(La,Sr)2CuO4	La1.75Sr0.25Cu1O3.921	La	1.75	Sr	0.25	Cu	1															O	X	3.921		1987																												T																				19.6					19.6																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
559	PRB0364047		(La,Sr)2CuO4	La1.73Sr0.27Cu1O3.913	La	1.73	Sr	0.27	Cu	1															O	X	3.913		1987																												T																				30.6					30.6																																																																																																					CORRELATION OF TC WITH HOLE CONCENTRATION IN LA(2-X)SR(X)CU(1)O(4-Z) SUPERCONDUCTORS	198709	TC	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,36(1987)4047	B.L.OLSON,M.W.SHAFER,T.PENNEY	LA,SR,CU,O	
560	PRB0357129			La1Ba2Cu2.9O6.8	La	1	Ba	2	Cu	2.9															O	6.8	6.8		1987																																3.892	3.936	11.814														45					45																																																																																																					MAGNETIC PENETRATION DEPTH AND FLUX-PINNING EFFECT IN HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4)	198705	MUON                     ,PENETRATION DEPTH        ,CARRIER DENSITY          ,FL	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,35(1987)7129	D.R.NOAKES,E.J.ANSALDO,G.AEPPLI,G.M.LUKE,J.H.BREWER,R.F.KIEFL,R.J.CAVA,S.R.KREITZMAN	LA,SR,CU,O	
561	PRB0357129		La(Ba,La)2Cu3O7	La1.6Ba1.4Cu2.9O6.98	La	1.6	Ba	1.4	Cu	2.9															O	6.98	6.98		1987																												Y123				3.918	3.928	11.742																																																																																																																								MAGNETIC PENETRATION DEPTH AND FLUX-PINNING EFFECT IN HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4)	198705	MUON                     ,PENETRATION DEPTH        ,CARRIER DENSITY          ,FL	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,35(1987)7129	D.R.NOAKES,E.J.ANSALDO,G.AEPPLI,G.M.LUKE,J.H.BREWER,R.F.KIEFL,R.J.CAVA,S.R.KREITZMAN	LA,SR,CU,O	
562	PRB0357129		La(Ba,La)2Cu3O7	La1.2Ba1.8Cu3O6.98	La	1.2	Ba	1.8	Cu	3															O	6.98			1987																												Y123				3.895	3.927	11.778														80					80																																																																																																					MAGNETIC PENETRATION DEPTH AND FLUX-PINNING EFFECT IN HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4)	198705	MUON                     ,PENETRATION DEPTH        ,CARRIER DENSITY          ,FL	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,35(1987)7129	D.R.NOAKES,E.J.ANSALDO,G.AEPPLI,G.M.LUKE,J.H.BREWER,R.F.KIEFL,R.J.CAVA,S.R.KREITZMAN	LA,SR,CU,O	
563	JJP0271425		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1988																												Y123				3.823	3.894	11.684														92					92																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
564	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.875Lu0.125Ba2Cu3OX	Y	0.875	Lu	0.125	Ba	2	Cu	3													O	X			1988																												Y123				3.82	3.893	11.672														89.7					89.7																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
565	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.75Lu0.25Ba2Cu3OX	Y	0.75	Lu	0.25	Ba	2	Cu	3													O	X			1988																												Y123				3.817	3.888	11.676														88.2					88.2																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
566	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.625Lu0.375Ba2Cu3OX	Y	0.625	Lu	0.375	Ba	2	Cu	3													O	X			1988																												Y123				3.812	3.888	11.676														88					88																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
567	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.5Lu0.5Ba2Cu3OX	Y	0.5	Lu	0.5	Ba	2	Cu	3													O	X			1988																												Y123				3.818	3.891	11.679														86.7					86.7																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
568	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.375Lu0.625Ba2Cu3OX	Y	0.375	Lu	0.625	Ba	2	Cu	3													O	X			1988																												Y123				3.81	3.89	11.668														86.9					86.9																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
569	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.25Lu0.75Ba2Cu3OX	Y	0.25	Lu	0.75	Ba	2	Cu	3													O	X			1988																												Y123				3.807	3.883	11.659														86					86																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
570	JJP0271425		(Y,Lu)Ba2Cu3O7	Y0.125Lu0.875Ba2Cu3OX	Y	0.125	Lu	0.875	Ba	2	Cu	3													O	X			1988																												Y123				3.803	3.88	11.65														87.9					87.9																																																																																																					SUPERCONDUCTING AND MAGNETIC PROPERTIES OF THE HIGH-T(C) AND HIGH-DENSITY SUPERCONDUCTOR Y(1-X)LU(X)BA(2)CU(3)O(7-Z)	198808	X-RAY                    ,RESISTIVITY              ,MAGNETIZ	DEPARTMENT OF ELECTRACAL AND ELECTRONIC ENGINEERING,TOYOHASHI UNIVERSITY OF TECHNOLOGY,TOYOHASHI-SHI,AICHI-KEN	JJAP LETT.,27(1988)L1425	AKIO OOTA,MASATAKA OHKUBO,TATSUMI HIOKI,YOSHINOBU SASAKI	Y,LU,BA,CU,O	
571	JJP0271449		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	Z	4		1988																												T																																																																																																																														CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
572	JJP0271449		(La,Ba)2CuO4	La1.95Ba0.05Cu1O3.98	La	1.95	Ba	0.05	Cu	1															O	Z	3.98		1988																												T				3.787	3.801	13.192																																																																																																																								CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
573	JJP0271449		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	Z	4		1988																												T				3.785		13.244														26.9					26.9																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
574	JJP0271449		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	Z	4		1988																												T				3.784		13.285																																																																																																																								CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
575	JJP0271449		(La,Ba)2CuO4	La1.785Ba0.215Cu1OZ	La	1.785	Ba	0.215	Cu	1															O	Z			1988																												T																				25.5					25.5																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
576	JJP0271449		(La,Sr)2CuO4	La1.95Sr0.05Cu1O3.98	La	1.95	Sr	0.05	Cu	1															O	Z	3.98		1988																												T				3.783	3.801	13.163																																																																																																																								CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
577	JJP0271449		(La,Sr)2CuO4	La1.9Sr0.1Cu1O3.98	La	1.9	Sr	0.1	Cu	1															O	Z	3.98		1988																												T				3.783		13.209														29.5					29.5																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
578	JJP0271449		(La,Sr)2CuO4	La1.875Sr0.125Cu1OZ	La	1.875	Sr	0.125	Cu	1															O	Z			1988																												T																				34.3					34.3																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
579	JJP0271449		(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.98	La	1.85	Sr	0.15	Cu	1															O	Z	3.98		1988																												T				3.773		13.224														37.9					37.9																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
580	JJP0271449		(La,Sr)2CuO4	La1.825Sr0.175Cu1OZ	La	1.825	Sr	0.175	Cu	1															O	Z			1988																												T																				35					35																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
581	JJP0271449		(La,Sr)2CuO4	La1.8Sr0.2Cu1O3.99	La	1.8	Sr	0.2	Cu	1															O	Z	3.99		1988																												T																				27.5					27.5																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
582	JJP0271449		(La,Sr)2CuO4	La1.75Sr0.25Cu1OZ	La	1.75	Sr	0.25	Cu	1															O	Z			1988																												T																				11.9					11.9																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
583	JJP0271449		(La,Sr)2CuO4	La1.7Sr0.3Cu1O3.99	La	1.7	Sr	0.3	Cu	1															O	Z	3.99		1988																												T																																																																																																																														CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
584	JJP0271449		(La,Sr)2CuO4	La1.5Sr0.5Cu1O3.96	La	1.5	Sr	0.5	Cu	1															O	Z	3.96		1988																												T																																																																																																																														CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
585	JJP0271449		(La,Ca)2CuO4	La1.95Ca0.05Cu1O3.975	La	1.95	Ca	0.05	Cu	1															O	Z	3.975		1988																												T				3.781	3.802	13.149																																																																																																																								CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
586	JJP0271449		(La,Ca)2CuO4	La1.9Ca0.1Cu1O3.967	La	1.9	Ca	0.1	Cu	1															O	Z	3.967		1988																												T				3.78		13.158														20					20																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
587	JJP0271449		(La,Ca)2CuO4	La1.85Ca0.15Cu1O3.942	La	1.85	Ca	0.15	Cu	1															O	Z	3.942		1988																												T				3.779		13.166														19					19																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
588	JJP0271449		(La,Ca)2CuO4	La1.8Ca0.2Cu1O3.917	La	1.8	Ca	0.2	Cu	1															O	Z	3.917		1988																												T																				19.5					19.5																																																																																																					CRYTAL STRUCTIRE,OXYGEN CONTENT AND SUPERCONDUCTIVITY OF M(X)LA(2-X)CU(1)O(4-Y) (M=BA,SR AND CA)	198808	OXYGEN CONTENT           ,STRUCTURE                ,RESISTIVITY              ,TC	TOHOKU UNIVERSITY,SENDAI	JJAP LETT.,27(1988)L1449	HIROSHI YAMAUCHI,KATSUYOSHI OH-ISHII,MASAE KIKUCHI,NORIO KOBAYASHI,TAKAAKI SASAOKA,TOMOKAZU MATSUHIRA,YASUHIKOSYONO,YOSHIO MUTO	M,LA,CU,O	
589	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	Z	6.94		1988																											3	Y123																				92.5					92.5																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
590	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.89	Y	1	Ba	2	Cu	3															O	Z	6.89		1988																											3	Y123																				92.1					92.1																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
591	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.84	Y	1	Ba	2	Cu	3															O	Z	6.84		1988																											3	Y123																				91					91																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
592	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.83	Y	1	Ba	2	Cu	3															O	Z	6.83		1988																											3	Y123																				89.3					89.3																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
593	SSC0680221		YBa2CuO7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	Z	6.75		1988																												Y123																				92.3					92.3																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
594	SSC0680221		YBa3Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	Z	6.7		1988																											3	Y123																				83					83																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
595	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	Z	6.4		1988																												Y123																				33					33																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
596	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.31	Y	1	Ba	2	Cu	3															O	Z	6.31		1988																											2	Y123																																																																																																																														LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
597	SSC0680221		YBa2Cu3O7	Y1Ba2Cu3O6.22	Y	1	Ba	2	Cu	3															O	Z	6.22		1988																											2	Y123																																																																																																																														LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
598	SSC0680221		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O6.89	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	Z	6.89		1988																											2	Y123																				72					72																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
599	SSC0680221		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.92	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	Z	6.92		1988																											2	Y123																				48					48																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
600	SSC0680221		YBa2(Cu,Al)3O7	Y1Ba2Cu2.52Al0.48O6.74	Y	1	Ba	2	Cu	2.52	Al	0.48													O	Z	6.74		1988																												Y123																				68					68																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
601	SSC0680221		YBa2(Cu,Al)3O7	Y1Ba2Cu2.05Al0.95O6.7	Y	1	Ba	2	Cu	2.05	Al	0.95													O	Z	6.7		1988																											2	Y123																				63					63																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
602	SSC0680221		YBa2(Cu,Al)3O7	Y1Ba2Cu2.095Al0.095O6.81	Y	1	Ba	2	Cu	2.095	Al	0.095													O	Z	6.81		1988																												Y123																				83.3					83.3																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
603	SSC0680221		YBa2(Cu,Zr)3O7	Y1Ba2Cu2.98Zr0.02O6.84	Y	1	Ba	2	Cu	2.98	Zr	0.02													O	Z	6.84		1988																											3	Y123																				90.2					90.2																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
604	SSC0680221		YBa2(Cu,Zr)3O7	Y1Ba2Cu2.94Zr0.06O6.81	Y	1	Ba	2	Cu	2.94	Zr	0.06													O	Z	6.81		1988																											3	Y123																				92.3					92.3																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
605	SSC0680221		YBa2(Cu,Zr)3O7	Y1Ba2Cu2.98Zr0.2O6.75	Y	1	Ba	2	Cu	2.98	Zr	0.2													O	7-z	6.75		1988																												Y123																				89.8					89.8																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
606	SSC0680221		EuBa2Cu3O7	Eu1Ba2Cu3O6.76	Eu	1	Ba	2	Cu	3															O	Z	6.76		1988																											3	Y123																				77					77																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
607	SSC0680221		EuBa2Cu3O7	Eu1Ba2Cu3O6.88	Eu	1	Ba	2	Cu	3															O	Z	6.88		1988																												Y123																				94					94																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
608	SSC0680221		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.98Fe0.02O6.93	Y	1	Ba	2	Cu	2.98	Fe	0.02													O	Z	6.93		1988																											3	Y123																				89					89																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
609	SSC0680221		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.994Zn0.006O6.63	Y	1	Ba	2	Cu	2.994	Zn	0.006													O	Z	6.63		1988																											3	Y123																				60					60																																																																																																					LABILE CU(3) IONS CORRELATED WITH SUPERCONDUCTING PROPERTIES IN Y(1)BA(2)CU(3)O(7-X)	198810	CU(3) IONS               ,Tc                       ,DOPANT                   ,CH	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING UNIVERSITY OF NEW SOUTH WALES KENSINGTON,AUSTRALIA	SOLID STATE COMMUN.,68(1988)0221	A.J.BOURDILLON,C.C.SORRELL,H.K.LIU,J.P.ZHOU,N.SAVVIDES,S.X.DOU	Y,BA,CU,O	
610	JJP0260223		(La,Sr)2CuO4	Sr0.25La1.75Cu1O4-Y	Sr	0.25	La	1.75	Cu	1															O	4-Y			1987																												T																			7.5	33	37				33																																																																																																					Composition dependence of the high temperature superconductivity in (Ba,Sr)-La-(Hg,Ag)-Cu-O system with K2NiF4-type structure				Jpn.J.Appl.Phys., 26(1987)L223	Y.Saito,T.Noji,A.Endo,N.Matsuzaki,M.Katsumata		
613	JJP0260633			Sm0.4Ba0.6Cu1OX	Sm	0.4	Ba	0.6	Cu	1															O	X			1987																																																18	35				18																																																																																																					SUPERCONDUCTIVITY IN BA-LN(LANTHANOID)-CU-O COMPOUNDS				JJAP.LETT.,26(1987)L633	A.MATSUDA,K.KINOSHITA,T.WATANA T.WATANABE,T.YAMADA,Y.ASANO	M,BA,CU,O	
614	JJP0260337		(La,Sr,Eu)2CuO4	Eu0.1La1.7Sr0.2Cu1O4	Eu	0.1	La	1.7	Sr	0.2	Cu	1													O	4			1987																												T																					33				33																																																																																																					HIGH TC SUPERCONDUCTIVITY OF (LA(1-X)SR(X))(2)CU(1)O(4)EFFECT OF SUBSTITUTION OF FOREIGN IONS FOR CU AND LA ON SUPERCONDUCTIVITY	198704		DEPARTMENT OF INDUSTRIAL CHEMISTRY,FACULTY OFENGINEERING,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L337	KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,MAKOTO AOKI,NAOKI OOBA,SHIN-ICHI UCHIDA,SHOJI TANAKA,TETSUYA HASEGAWA	LA,SR,CU,O	
615	PRB0364025		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																											3	Y123																				92.3					92.3																																0.23																																																																					SUPERCONDUCTING PROPERTIES OF ALIGNED CRYSTALLINE GRAINS OF Y(1)BA(2)CU(3)O(7-Z)	198709	MAGNETIZATION            ,JC	DEPARTMENT OF PHYSICS,CASE WESTERN RESERVE UNIVERSITY,CLEVELAND,OHIO	PHYS.REV.B,36(1987)4025	B.S.CHANDRASEKHAR,D.E.FARRELL,J.R.CLEM.D.K.FINNEMORE,M.M.FANG,M.R.DEGUIRE,V.G.KOGAN	Y,BA,CU,O	
616	PRB0368393		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.75Ni0.25O7	Y	1	Ba	2	Cu	2.75	Ni	0.25													O	7			1987						0.66	-3																					Y123				3.859		11.8																																																																																																																								3d-metal doping of the high-temperature superconducting perovskites La-Sr-Cu-O and Y-Ba-Cu-O	198712		Bell Communications Reserch, Red Bank, New Jersey 07701	Phys.Rev.B,36(1987)8393	E.J. McNiff, Jr,G.W. Hull,J.M. Tarascon,K.A. Delin,L.H. Greene,P. Barboux,S. Foner,T.P. Orlando,W.R. Mckinnon		
617	JPS0572261		La2CuO4	La2O4	La	2																			O	4		1	1988																												T																																																																																																																														EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
618	JPS0572261		(La,Ba)2CuO4	La1.99Ba0.01Cu1O4	La	1.99	Ba	0.01	Cu	1															O	4		1	1988																												T																																																																																		0.5																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
619	JPS0572261		(La,Ba)2CuO4	La1.98Ba0.02Cu1O4	La	1.98	Ba	0.02	Cu	1															O	4		1	1988																												T																																																																																		1.6																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
620	JPS0572261		(La,Ba2)2CuO4	La1.97Ba0.03Cu1O4	La	1.97	Ba	0.03	Cu	1															O	4		1	1988																												T																																																																																		2.8																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
621	JPS0572261		(La,ba)2CuO4	La1.965Ba0.035Cu1O4	La	1.965	Ba	0.035	Cu	1															O	4		1	1988																												T																																																																																		5																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
622	JPS0572261		(La,Ba)2CuO4	La1.955Ba0.045Cu1O4	La	1.955	Ba	0.045	Cu	1															O	4		1	1988																												T																																																																																		5.8																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
623	JPS0572261		(La,Ba)2CuO4	La1.94Ba0.06Cu1O4	La	1.94	Ba	0.06	Cu	1															O	4		1	1988																												T																																																																																		3.8																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
624	JPS0572261		(La,Ba)2CuO4	La1.93Ba0.07Cu1O4	La	1.93	Ba	0.07	Cu	1															O	4		1	1988																												T																																																																																		3.8																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
625	JPS0572261		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4		1	1988																												T																																																																																		2.7																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
626	JPS0572261		(La,Ba)2CuO4	La1.91Ba0.09Cu1O4	La	1.91	Ba	0.09	Cu	1															O	4		1	1988																												T																																																																																		3																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
627	JPS0572261		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4		1	1988																												T																																																																																		2.9																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
628	JPS0572261		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1988																												T																																																																																		4																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
629	JPS0572261		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4		1	1988																												T																																																																																		5.9																																												EXISTENCE OF THE MINIMUM COEFFICIENT IN TEMPERATURE LINEAR TERM OF HEAT CAPACITY IN SUPERCONDUCTING (LA1-XBAX)2CUO4	198807		DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY	J.PHYS.SOC.JAPAN,57(1988)2261	KENJI ISHIDA,KIICHI AMAYA,KUNISUKE ASAYAMA,SATOSHI KUMAYASU,TATSUO KOBAYASHI,YOSHIO KITAOKA	LA,BA,CU,O	
630	PRB0362404		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123																												K/GPa	0.9																																																																																																	COMPARISON OF THE PRESSURE DEPENDENCIES OF Tc IN THE 90-K SUPERCONDUCTORS R(1)BA(2)CU(3)O(X) (R=GD,ER,AND YB) AND Y(1)BA(2)CU(3)O(X)	198708	RESISTANCE               ,Tc                       ,PRESSURE	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)2404	D.E.PETERSON,G.L.WELLS,H.A.BORGES,J.D.THOMPOSON,J.L.SMITH,R.KWOK,Z.FISK	GD,ER,YB,Y,BA,CU,O	
631	PRB0362404		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X			1987																												Y123																												K/GPa	1.3																																																																																																	COMPARISON OF THE PRESSURE DEPENDENCIES OF Tc IN THE 90-K SUPERCONDUCTORS R(1)BA(2)CU(3)O(X) (R=GD,ER,AND YB) AND Y(1)BA(2)CU(3)O(X)	198708	RESISTANCE               ,Tc                       ,PRESSURE	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)2404	D.E.PETERSON,G.L.WELLS,H.A.BORGES,J.D.THOMPOSON,J.L.SMITH,R.KWOK,Z.FISK	GD,ER,YB,Y,BA,CU,O	
632	PRB0362404		ErBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X			1987																												Y123																												K/GPa	1.4																																																																																																	COMPARISON OF THE PRESSURE DEPENDENCIES OF Tc IN THE 90-K SUPERCONDUCTORS R(1)BA(2)CU(3)O(X) (R=GD,ER,AND YB) AND Y(1)BA(2)CU(3)O(X)	198708	RESISTANCE               ,Tc                       ,PRESSURE	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)2404	D.E.PETERSON,G.L.WELLS,H.A.BORGES,J.D.THOMPOSON,J.L.SMITH,R.KWOK,Z.FISK	GD,ER,YB,Y,BA,CU,O	
633	PRB0362404		YbBa2Cu3O7	Yb1Ba2Cu3OX	Yb	1	Ba	2	Cu	3															O	X			1987																												Y123																												K/GPa	1.9																																																																																																	COMPARISON OF THE PRESSURE DEPENDENCIES OF Tc IN THE 90-K SUPERCONDUCTORS R(1)BA(2)CU(3)O(X) (R=GD,ER,AND YB) AND Y(1)BA(2)CU(3)O(X)	198708	RESISTANCE               ,Tc                       ,PRESSURE	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,36(1987)2404	D.E.PETERSON,G.L.WELLS,H.A.BORGES,J.D.THOMPOSON,J.L.SMITH,R.KWOK,Z.FISK	GD,ER,YB,Y,BA,CU,O	
634	PRB0392788		Y(Ba,Sr)2Cu3O7	Y1Ba1.48Sr0.52Cu3O7-Z	Y	1	Ba	1.48	Sr	0.52	Cu	3													O	7-Z		1	1989																											3	Y123				3.79	3.84	11.52														95					95																																																																																																					LOCAL STRUCTURE DISTORTION IN A Y(1)BA(2-0.52)SR(0.52)CU(3)O(7) SUPERCONDUCTOR	198902	STRUCTURE                ,XAFS	INSTITUTE FOR STRUCTURE AND FUNCTION STUDIES,PHILADELPHIA	PHYS.REV.B,39(1989)2788	B.CHANCE,C.F.GALLO,G.BUNKER,K.ZHANG	Y,BA,SR,CU,O	
635	PRB0392788		Y(Ba,Sr)2Cu3O7	Y1Ba1.48Sr0.52Cu3O7-Z	Y	1	Ba	1.48	Sr	0.52	Cu	3													O	7-Z		1	1989																											3	Y123				3.812	3.862	11.586														85					85																																																																																																					LOCAL STRUCTURE DISTORTION IN A Y(1)BA(2-0.52)SR(0.52)CU(3)O(7) SUPERCONDUCTOR	198902	STRUCTURE                ,XAFS	INSTITUTE FOR STRUCTURE AND FUNCTION STUDIES,PHILADELPHIA	PHYS.REV.B,39(1989)2788	B.CHANCE,C.F.GALLO,G.BUNKER,K.ZHANG	Y,BA,SR,CU,O	
636	PRB0392748		EuBa2Cu3O7	Eu1Ba2Cu3OX	Eu	1	Ba	2	Cu	3															O	X		1	1989									5.31																		3	Y123																				93	95				93										31																															A		1700																																																										MUON-SPIN-ROTATION MEASUREMENT OF MAGNETIC FIELD PENETRATION AND FLUX PINNING IN SUPERCONDUCTING EU(1)BA(2)CU(3)O(X)	198902	MUON                     ,PENETRATION DEPTH        ,FLUX PIN	LOS ALAMOS NATIONAL LABORATORY,NEW MEXICO	PHYS.REV.B,39(1989)2748	C.BOEKEMA,D.W.COOKE,H.REMPP,J.L.SMITH,J.O.WILLIS,J.OOSTENS,K.C.B.CHAN,M.E.SCHILLACI,M.MAEZ,R.L.HUTSON,R.L.LICHTI,R.S.KWOK,S.P.WEATHERSBY	EU,BA,CU,O	
637	JJP0272274		SmBa2Cu3O7	Sm1Ba2Cu3O6.85	Sm	1	Ba	2	Cu	3															O	7-Z	6.85	1	1988																											3	Y123				3.858	3.909	11.754													91.4		94.2				92.8																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
638	JJP0272274		Sm(Ba,Sm)2Cu3O7	Sm1.05Ba1.95Cu3O6.87	Sm	1.05	Ba	1.95	Cu	3															O	7-Z	6.87	1	1988																											3	Y123				3.853	3.903	11.743													86.5		93				89.75																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
639	JJP0272274		Sm(Ba,Sm)2Cu3O7	Sm1.15Ba1.85Cu3O6.95	Sm	1.15	Ba	1.85	Cu	3															O	7-Z	6.95	1	1988																											3	Y123				3.859	3.902	11.741													73.5		81.1				77.3																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
640	JJP0272274		Sm(Ba,Sm)2Cu3O7	Sm1.2Ba1.8Cu3O7.01	Sm	1.2	Ba	1.8	Cu	3															O	7-Z	7.01	1	1988																											3	Y123				3.87	3.88	11.658													51.4		61.6				56.5																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
641	JJP0272274		Sm(Ba,Sm)2Cu3O7	Sm1.28Ba1.72Cu3O7.03	Sm	1.28	Ba	1.72	Cu	3															O	7-Z	7.03	1	1988																												Y123						11.639													33.7		53.5				43.6																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
642	JJP0272274		Sm(Ba,Sm)2CuO7	Sm1.35Ba1.65Cu3O7.07	Sm	1.35	Ba	1.65	Cu	3															O	7-Z	7.07	1	1988																												Y123						11.639													10.5		41.9				26.2																																																																																																					OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
643	JJP0272274		Sm(Ba,Sm)2CuO7	Sm1.5Ba1.5Cu3O7.14	Sm	1.5	Ba	1.5	Cu	3															O	7-Z	7.14	1	1988																												Y123				3.863	3.872	11.574																																																																																																																								OXYGEN CONTENT AND TRANSITION TEMPERATURE (TC) IN BA(2-X)LN(1+X)CU(3)O(7-Z) (LN=SM,EU)	198812	OXYGEN CONTENT           ,VALENCE                  ,DOPANT	R&D CENTER,TDK CORPORATION,ICHIKAWA,CHIBA	JJAP LETT.,27(1988)L2274	MAKOTO KOBAYASHI,SATOSHI MARUYAMA,TAKAHIRO KODAMA	BA,SM,EU,CU,O	
644	JJP0272283		(Nd,Ce,Sr)2CuO4	Nd1.32Ce0.27Sr0.41Cu1OY	Nd	1.32	Ce	0.27	Sr	0.41	Cu	1													O	Y		1	1988																												T'				3.856		12.487															20				20																																																																																																					IDENTIFICATION OF THE SUPERCONDUCTING PHASE IN THE ND-CE-SR-CU0O SYSTEM	198812	SINGLE PHASE             ,SUSCEPTIBILITY           ,CONDUCTIVITY             ,TE	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS,TSUKUBA IBARAKI	JJAP LETT.,27(1988)L2283	EIJI TAKAYAMA-MUROMACHI,FUJIO IZUMI,KATSUO KATO,MITSUKO ONODA,YOSHIO MATSUI,YOSHISHIGE UCHIDA	ND,CE,SR,CU,O	
645	PRB0394299		YBa2Cu3O7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	X	6.75		1989																												Y123																				89.1					89.1																																																																																																					PHASE TRANSFORMATIONS IN YBA(2)CU(3)O(7-Z)	198903	ANNEALING                ,PHASE TRANSFORMATION     ,TWINNING	MATERIALS SCIENCE DIVISION,BUILDING 223,ARGONNE NATIONAL LABORA-TORY, ARGONNE,ILLINOIS	PHYSICAL REVIEW B.,39(1989)4299	DONGLU SHI	Y,BA,CU,O	
646	PRB0394299		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	X	6.72		1989																												Y123																				62					62																																																																																																					PHASE TRANSFORMATIONS IN YBA(2)CU(3)O(7-Z)	198903	ANNEALING                ,PHASE TRANSFORMATION     ,TWINNING	MATERIALS SCIENCE DIVISION,BUILDING 223,ARGONNE NATIONAL LABORA-TORY, ARGONNE,ILLINOIS	PHYSICAL REVIEW B.,39(1989)4299	DONGLU SHI	Y,BA,CU,O	
647	PRB0394299		YBa2Cu3O7	Y1Ba2Cu3O6.62	Y	1	Ba	2	Cu	3															O	X	6.62		1989																												Y123																				62					62																																																																																																					PHASE TRANSFORMATIONS IN YBA(2)CU(3)O(7-Z)	198903	ANNEALING                ,PHASE TRANSFORMATION     ,TWINNING	MATERIALS SCIENCE DIVISION,BUILDING 223,ARGONNE NATIONAL LABORA-TORY, ARGONNE,ILLINOIS	PHYSICAL REVIEW B.,39(1989)4299	DONGLU SHI	Y,BA,CU,O	
648	PRB0394291		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1989								0.55																				Y123				3.828	3.89															88	89.5				88																																																																																																					MAGNETIC ORDERING IN THE HIGH-TEMPERATURE SUPERCONDUCTOR ERBA(2-)CU(3)O(7-Z)	198903	NEUTRON DIFFRACTION      ,MAGNETIC ORDERING        ,SPECIFIC HEAT            ,SI	DEPARTMENT OF PHYSICS,UNIVERSITY OF WARWICK,COVENTRY CV 4 7 AL,-UNITED KINGDOM	PHYS. REV. B.,39(1989)4291	B.C.SALES,D.MCK.PAUL,H.A.MOOK,J.O.RAMEY,L.A.BOATNER,L.CUSSEN	ER,BA,CU,O	
649	PRB0394693		Bi2Sr2CaCu2O8	Bi2Ca1Sr2Cu2O8	Bi	2	Ca	1	Sr	2	Cu	2													O	8			1989																												Bi2212																			82	88.5	96				88.5																																																3.4																																																					TUNNELING MEASUREMENTS ON BI(2)CASR(2)CU(2)O(8)	198903	TUNNELING                ,I-V CHARACTERI	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA CITY,IOWA	PHYS. REV. B.,39(1989)4693	ROBERT E.JOHNSON	BI,CA,SR,CU,O	
650	JPS0570734		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1988								240																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
651	JPS0570734		(La,Ba)2CuO4	La1.996Ba0.004Cu1O4	La	1.996	Ba	0.004	Cu	1															O	4			1988								189																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
652	JPS0570734		(La,Ba)2CuO4	La1.99Ba0.01Cu1O4	La	1.99	Ba	0.01	Cu	1															O	4			1988								129																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
653	JPS0570734		(La,Ba)2CuO4	La1.987Ba0.014Cu1O4	La	1.987	Ba	0.014	Cu	1															O	4			1988								88																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
654	JPS0570734		(La,Ba)2CuO4	La1.986Ba0.014Cu1O4	La	1.986	Ba	0.014	Cu	1															O	4			1988								15																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
655	JPS0570734		(La,Ba)2CuO4	La1.984Ba0.016Cu1O4	La	1.984	Ba	0.016	Cu	1															O	4			1988								12																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
656	JPS0570734		(La,Ba)2CuO4	La1.98Ba0.02Cu1O4	La	1.98	Ba	0.02	Cu	1															O	4			1988								8.8																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
657	JPS0570734		(La,Ba)2CuO4	La1.95Ba0.05Cu1O4	La	1.95	Ba	0.05	Cu	1															O	4			1988								1.5																				T																																																																																																																														MAGNETIC PHASE DIAGRAM AND SUPERCONDUCTIVITY IN HIGH-TC(LA1-XBAX)2CUO4	198803	PHASE DIAGRAM       ,NQR                 ,ANTIFERROMAGNETISM	DEPARTMENT OF MATERIAL PHYSICS, FACULTY OF ENGINEERING SCIENCE, OSAKA UNIVERSITY, TOYONAKA, OSAKA	J.PHYS.SOC.JAPAN,57(1988)734	KENJI ISHIDA,KUNISUKE ASAYAMA,SHIGERU HIRAMATSU,YOSHIO KITAOKA	LA,BA,CU,O	
658	PHC1570237		(Ba,K)BiO3	Ba0.65K0.35Bi1O3	Ba	0.65	K	0.35	Bi	1															O	3			1989																												BKBO																				23					23			K/GPa	0.8																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
659	PHC1570237		La2CuO4	La2Cu1O4.13	La	2	Cu	1																	O	4.13			1989																												T																				28					28			K/GPa	2.7																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
660	PHC1570237		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1989																												T																				26					26			K/GPa	2																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
661	PHC1570237		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1989																												T																				39					39			K/GPa	3.5																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
662	PHC1570237		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4			1989																												T																				30					30			K/kbar	0																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
663	PHC1570237		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X			1989																												Bi2212																				85					85			K/GPa	2.4																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
664	PHC1570237		BiSr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OX	Bi	2	Sr	2	Ca	2	Cu	3													O	X			1989																												Bi2212																				108					108			K/GPa	1.6																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
665	PHC1570237		TlBa2CaCu2O8	Tl2Ca1Ba2Cu2OX	Tl	2	Ca	1	Ba	2	Cu	2													O	X			1989																												Tl2212																				106					106			K/GPa	2																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
666	PHC1570237		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8			1989																												Y123																				92					92			K/GPa	0.7																																																																																																	EFFECT OF PRESSURE ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF BA(1-X)K(X)BI(1)O(3)	198902	TC                       ,PRESSURE	SANDIA NATIONAL LABORATORIES,ALBUQUERQUE,USA	PHYSICA C,157(1989)237	B.MOROSIN,D.S.GINLEY,J.E.SCHIRBER	BA,K,BI,O	
667	SSC0651355	RH300 BY LOW FREQ. AC TECHNIQUE	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	Z	7		1988																												Y123																				91				5	91																																																																														0.9								0.00000000112			0.000000002	1	RH667										HALL-EFFECT OF THE HIGH TC SUPERCONDUCTORS Y-BA-CU-O AND GD-BA-CU-O	198804	HALL EFFECT              ,HEAT TREATMENT	INSTITUTE OF PHYSICS OF THE UNIVERSITY,P.O.B.YUGOSLAVIA	SOLID STATE COMMUN.,65(1988)1355	B.LEONTIC,L.FORRO,M.PETRAVIC	Y,BA,CU,O,GD,BA,CU,O	
668	SSC0651355		YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	Z	6.6		1988																												Y123																							4.2																																																																																1.7								0.0000000169			0.000000002		RH668										HALL-EFFECT OF THE HIGH TC SUPERCONDUCTORS Y-BA-CU-O AND GD-BA-CU-O	198804	HALL EFFECT              ,HEAT TREATMENT	INSTITUTE OF PHYSICS OF THE UNIVERSITY,P.O.B.YUGOSLAVIA	SOLID STATE COMMUN.,65(1988)1355	B.LEONTIC,L.FORRO,M.PETRAVIC	Y,BA,CU,O,GD,BA,CU,O	
669	SSC0641287		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1987																												Y123																				89					89																																																																														2																							HALL EFFECT MEASUREMENTS ON A BULK Y(1)BA(2)CU(3)O(7) SAMPLE	198712	HALL EFFECT              ,RESISTIVITY	CSIRO DIVISION OF APPLIED PHYSICS,LINDFIELD,AUSTRALIA	SOLID STATE COMMUN.,64(1987)1287	B.W.RICKETTS,H.K.WELSH,R.B.ROBERTS,R.DRIVER	Y,BA,CU,O	
670	PRB0380844		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	X	7		1988																												Y123																				92					92																																																																																		0.8																			HALL COEFFICIENT AND OXYGEN STOICHIOMETRY IN Y(1)BA(2)CU(3)O(7-Z) CERAMICS AT ELEVATED TEMPERATURES	198807	RESISTIVITY              ,OXYGEN CONTENT           ,HALL EFF	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,38(1988)844	A.T.FIORY,G.S.GRADER,P.K.GALLAGHER	Y,BA,CU,O	
671	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	X	6.94		1988																												Y123																																																																																																															0.0000000004			0.0000000008												RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
672	PLA1320217	RHN AT 100K,DENS CALCULATED BY XRD	YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X			1988									4.86																			Y123																				91.9					91.9																																																																																						0.00000000184			0.00000000184												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
673	PRB0389280		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1988																											3	Y123																				91.2					91.2																																2.34	0.32																																																																				ORIENTATIONAL ANISOTROPY OF THE UPPER CRITICAL FIELD IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7) AND BI(2.2)CA(1)SR(1.9)CU(2)O(8+X)	198811	SINGLE-CRYSTAL           ,Hc                       ,ANISOTRO	DEPARTMENT OF PHYSICS AND LABORATORY FOR RESEARCH ON THE STRUCTURE OF MATTER,UNIVERSITY OF PENNSYLVANIA,PHILADELPHIA,PENNSYLVANIA	PHYS.REV.B,38(1988)9280	J.E.FISCHER,M.J.NAUGHTON,N.P.ONG,P.K.DAVIES,P.M.CHAIKIN,R.C.YU,R.V.CHAMBERLIN,T.W.JING,Z.Z.WANG	Y,BA,CU,O,BI.CA.SR	
674	PRB0389280		Bi2Sr2CaCu2O8	Bi2.2Ca1Sr1.9Cu2O8+X	Bi	2.2	Ca	1	Sr	1.9	Cu	2													O	8+X		2	1988																												Bi2212																			82		91				86.5																																																																																																					ORIENTATIONAL ANISOTROPY OF THE UPPER CRITICAL FIELD IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7) AND BI(2.2)CA(1)SR(1.9)CU(2)O(8+X)	198811	SINGLE-CRYSTAL           ,Hc                       ,ANISOTRO	DEPARTMENT OF PHYSICS AND LABORATORY FOR RESEARCH ON THE STRUCTURE OF MATTER,UNIVERSITY OF PENNSYLVANIA,PHILADELPHIA,PENNSYLVANIA	PHYS.REV.B,38(1988)9280	J.E.FISCHER,M.J.NAUGHTON,N.P.ONG,P.K.DAVIES,P.M.CHAIKIN,R.C.YU,R.V.CHAMBERLIN,T.W.JING,Z.Z.WANG	Y,BA,CU,O,BI.CA.SR	
675	PRB0394316			Bi4Sr4La2Cu4OZ	Bi	4	Sr	4	La	2	Cu	4													O	Z		1	1989																																3.875		30.592																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
676	PRB0394316			Bi4Sr4Pr2Cu4OZ	Bi	4	Sr	4	Pr	2	Cu	4													O	Z		1	1989						2.96	16																									3.877		30.366																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
677	PRB0394316			Bi4Sr4Nd2Cu4OZ	Bi	4	Sr	4	Nd	2	Cu	4													O	Z		1	1989						2.97	30																					Bi2212				3.872		30.287																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
678	PRB0394316			Bi4Sr4Sm2Cu4OZ	Bi	4	Sr	4	Sm	2	Cu	4													O	Z		1	1989																												Bi2212				3.867		30.296																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
679	PRB0394316			Bi4Sr4Eu2Cu4OZ	Bi	4	Sr	4	Eu	2	Cu	4													O	Z		1	1989																												Bi2212				3.863		30.138																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
680	PRB0394316			Bi4Sr4Gd2Cu4OZ	Bi	4	Sr	4	Gd	2	Cu	4													O	Z		1	1989						7.84	2																					Bi2212				3.855		30.248																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
681	PRB0394316			Bi4Sr4Dy2Cu4OZ	Bi	4	Sr	4	Dy	2	Cu	4													O	Z		1	1989						10.23	8																					Bi2212				3.853		30.162																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
682	PRB0394316			Bi4Sr4Y2Cu4OZ	Bi	4	Sr	4	Y	2	Cu	4													O	Z		1	1989																												Bi2212				3.853		30.152																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
683	PRB0394316			Bi4Sr4Tb2Cu4OZ	Bi	4	Sr	4	Tb	2	Cu	4													O	Z		1	1989						7.66	13																					Bi2212				3.85		30.232																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
684	PRB0394316			Bi4Sr4Ho2Cu4OZ	Bi	4	Sr	4	Ho	2	Cu	4													O	Z			1989						10.23	13																					Bi2212				3.843		30.025																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
685	PRB0394316			Bi4Sr4Er2Cu4OZ	Bi	4	Sr	4	Er	2	Cu	4													O	Z			1989						9.39	14																					Bi2212				3.841		30.156																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
686	PRB0394316			Bi4Sr4Tm2Cu4OZ	Bi	4	Sr	4	Tm	2	Cu	4													O	Z			1989						7.66	32																					Bi2212				3.824		30.173																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
687	PRB0394316			Bi4Sr4Yb2Cu4OZ	Bi	4	Sr	4	Yb	2	Cu	4													O	Z			1989																												Bi2212				3.85		30.474																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
688	PRB0394316			Bi4Sr4Lu2Cu4OZ	Bi	4	Sr	4	Lu	2	Cu	4													O	Z			1989																												Bi2212				3.812		30.316																																																																																																																								BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
689	PHC1580230		Bi2(Sr,Ca)2CuO6	Bi2Sr1.3Ca0.7Cu1O6.15	Bi	2	Sr	1.3	Ca	0.7	Cu	1													O	6.15			1989																												Bi2201																				84					84																																									A	MUON-SPIN RELAXATION	3550																																																			BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-CAL(750C 15H)-SIN(830C 15H)					MAGNETIC PENETRATION DEPTH IN BI(2)(SR,CA)(2)CUO(8-Z)	198904		INSTITUT FUR MITTELENERGIEPHYSIK,ETHZ,CH-5232 VILLIGEN PSI,SWITZERLAND	PHYSICA C ,158(1989)230	A.SCHENCK,B.HETTICH,B.HITTI,E.LIPPELT,F.N.GYGAX,H.MALETTA,M.WEBER,P.BIRRER	BI,SR,CA,CU,O	
690	PHC1580097			Bi0.8Pb0.2Sb0.05Sr1Ca1Cu2OX	Bi	0.8	Pb	0.2	Sb	0.05	Sr	1	Ca	1	Cu	2									O	X			1989																																5.23	5.18	35.98														93	107				93																																																																																														(BI,SR,CA,CU,PB)-NITRATE,SB2O5	0	MIXTURE-CAL(800C 12H+840C 24H)-SIN(850C 60-100H IN (N2+O2) GAS)					EFFECT OF SB SUBSTITUTION ON TC IN BI-PB-SR-CA-CU-O SYSTEMS	198904	MATERIAL                 ,SB SUBSTITUTION          ,SUPERLAT	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING,UNIVERSITY OF NEWSOUTH WALES,P.O.BOX 1 KENSINGTON,NSW 2033,AUSTRALIA	PHISICA C ,158(1989)97	H.K.LIU,N.X.TAN,S.X.DOU,W.K.JONES,Y.J.SHENG	SB,BI,PB,SR,CA,CU,O	
691	PHC1580097			Bi0.8Pb0.2Sr1Ca1Cu2OZ	Bi	0.8	Pb	0.2	Sr	1	Ca	1	Cu	2											O	Z			1989																																5.26	5.23	36.45														108					108																																																																																														(BI,SR,CA,CU,PB)-NITRATE,SB2O5	0	MIXTURE-CAL(800C 12H+840C 24H)-SIN(850C 60-100H IN (N2+O2) GAS)					EFFECT OF SB SUBSTITUTION ON TC IN BI-PB-SR-CA-CU-O SYSTEMS	198904	MATERIAL                 ,SB SUBSTITUTION          ,SUPERLAT	SCHOOL OF MATERIALS SCIENCE AND ENGINEERING,UNIVERSITY OF NEWSOUTH WALES,P.O.BOX 1 KENSINGTON,NSW 2033,AUSTRALIA	PHISICA C ,158(1989)97	H.K.LIU,N.X.TAN,S.X.DOU,W.K.JONES,Y.J.SHENG	SB,BI,PB,SR,CA,CU,O	
692	PHC1580265		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1989																												Y123																				92					92																																																																																															0						NEUTRON DIFFRACTION STUDY OF THE SUPERCONDUCTOR YBA(2)(CU(1-X)FE(X))(3)O(7-Z) AT X=0.06 AND 0.10,Z=0	198904	NEUTRON DIFFRACTION      ,RIETVELD	LABORATORY OF NEUTRON PHYSICS,JOINT INSTITUTE FOR NUCLEAR RESEARCH,DUBNA,USSR	PHYSICA C ,158(1989)265	A.M.BALAGUROV,A.PAJACZKOWSKA,G.M.MIRONOVA,H.SZYMCZAK	Y,BA,CU,FE,O	
693	PHC1580265		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18OZ	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	Z			1989																												Y123																				55					55																																																																																															0						NEUTRON DIFFRACTION STUDY OF THE SUPERCONDUCTOR YBA(2)(CU(1-X)FE(X))(3)O(7-Z) AT X=0.06 AND 0.10,Z=0	198904	NEUTRON DIFFRACTION      ,RIETVELD	LABORATORY OF NEUTRON PHYSICS,JOINT INSTITUTE FOR NUCLEAR RESEARCH,DUBNA,USSR	PHYSICA C ,158(1989)265	A.M.BALAGUROV,A.PAJACZKOWSKA,G.M.MIRONOVA,H.SZYMCZAK	Y,BA,CU,FE,O	
694	PHC1580265		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3OZ	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	Z			1989																												Y123																				39					39																																																																																															0						NEUTRON DIFFRACTION STUDY OF THE SUPERCONDUCTOR YBA(2)(CU(1-X)FE(X))(3)O(7-Z) AT X=0.06 AND 0.10,Z=0	198904	NEUTRON DIFFRACTION      ,RIETVELD	LABORATORY OF NEUTRON PHYSICS,JOINT INSTITUTE FOR NUCLEAR RESEARCH,DUBNA,USSR	PHYSICA C ,158(1989)265	A.M.BALAGUROV,A.PAJACZKOWSKA,G.M.MIRONOVA,H.SZYMCZAK	Y,BA,CU,FE,O	
695	PHC1580237			Bi4.4Sr3.6Ca2Cu4OY	Bi	4.4	Sr	3.6	Ca	2	Cu	4													O	Y			1989																																																83.6					83.6			K/kbar	0.2																																																																															2.3	630											0	CRYSTAL GROWN BY CUO FLUX METHOD					PRESSURE-EFFECT STUDY ON HIGH-TC SUPERCONDUCTING SINGLE CRYSTAL OF 84 K BI-SR-CA-CU-O SYSTEM	198904	PRESSURE EFFECT          ,TC                       ,RESISTIVITY              ,SI	NIPPON TELEGRAPH AND TELEPHONE CORPORATION,OPTO-ELECTRONICS LABORATORIES,TOKAI IBARAKI 319-11,JAPAN	PHYSICA C ,158(1989)237	MAKOTO HIKITA,MINORU SUZUKI,YOSHIKAZU HIDAKA,YUKIMICHI TASHIMA	BI,SR,CA,CU,O	
696	PHC1580255		(Bi,Pb)2Sr2Ca2Cu3O10	Pb0.3Bi1.7Sr2Ca2Cu3O10+Z	Pb	0.3	Bi	1.7	Sr	2	Ca	2	Cu	3											O	10+Z			1989																												Bi2223				5.418	5.346	37.1														107					107																																																					SP696		5.3		34.6		418																																			PBO,BI2O3,SRCO3,CACO3,CUO	0	CAL(800-810C 12H)-SIN(870-880C 240H IN AIR)-FC TO 500C-Q					THE SPECIFIC HEAT OF THE SINGLE-PHASE (BI,PB)(2)SR(2)CA(2)CU(3)O(10+Y) SUPERCONDUCTOR	198904	SPECIFIC HEAT       ,SINGLE-PHASE	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCE,BEIJING,P.R.CHINA	PHYSICA C ,158(1989)255	JIN RONG-YING,QI-ZE RAN,SHI FAN,SHI NI-CHENG,SHI ZHEN-HUA,ZHOU SHOU-ZENG	BI,PB,SR,CA,CU,O	
697	PRB0399069		YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	1	1989																											3	Y123				3.817	3.884	11.671														91					91																																																																																																					OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
698	PRB0399069		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	Z	6.4	1	1989																											2	Y123				3.861		11.803																																																																																																																								OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
699	PRB0399069		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	Z	6.4	1	1989																											2	Y123				3.858		11.81																																																																																																																								OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
700	PRB0399069		YBa2Cu3Oz	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O	Z	6.55	1	1989																											3	Y123				3.82	3.89	11.714														89					89																																																																																																					OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
701	PRB0399069		YBa2Cu3Oz	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Z	6.66	1	1989																											3	Y123				3.82	3.89	11.681																																																																																																																								OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
702	PRB0399069		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1989																											3	Y123				3.817	3.885	11.674														90					90																																																																																																					OXYGEN IN-DIFFUSION PROCESSES IN TETRAGONAL YBA(2)CU(3)O(7-X)OXIDE	198905	RESISTANCE          ,DIFFUSION           ,OXYGEN CONTENT      ,DISORDER-ORDER	PHYSICS DEPARTMENT,UNIVERSITA DEGLI STUDI DI MODENA,VIA CAMPI213/A,I-41100,MODENA,ITALY	PHYS.REV.B.,39(1989)9069	C.NOBILI,E.GALLI,F.C.MATACOTTA,F.NAVA,G.OTTAVIANI,M.AFFRONTE,T.MANFREDINI	Y,BA,CU,O	
703	PRB0399682		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1989									8.1																			BKBO																				31.5					31.5																															0.52																								27.09		1.5																																												HEAT CAPACITY OF SUPERCONDUCTING BA0.6K0.4BIO3NEAR TC	198905	HEAT CAPACITY            ,SINGLE CRYSTALS          ,MAGNETIZATION            ,BA	AT&T BELL LABORATORIES,MURRY HILL,NEW JERSEY 07974	PHYS.REV.B.39(1989)9682	J.E.GRAEBNER,K.J.THOMAS,L.F.SCHNEEMEYER	BA,K,BI,O	
704	SSC0700547		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		5	1989																												Y123																				90					90																																																3.2																																																					INFRARED REFLECTANCE OF ANISOTROPIC(110)YBCO EPITAXIAL FILM	198905	IR                       ,REFLECTANCE              ,SINGLE CRYSTAL           ,FI	INSTITUTE OF PHTSICS,CZECHOSLIVAK ACAD.SCI.,NASLIVANCE 2,18040PRAGUE 8,CZECHOSLOVAKIA	SOLID STATE COMMUN.,70(1989)547	B.P.GORSHUNOV,E.V.PECHEN,J.PETZELT,S.I.KRASNISVOBODTSEV,S.KAMBA,V.ZELEZNY	Y,BA,CU,O	
705	SSC0700553		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																												Y123																				92					92										82																																																																																											DETERMINARION OF FLUX PINNING POTENTIALS FROM FIELD-INDUCED ANISOTROPY IN OXIDE SUPERCONDUCTORS	198905	MAGNETIZATION            ,PINNING                  ,RAYLEIGH	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY,BEIJING 100871,PRC	SOLID STATE COMMUN.,70(1989)553	HONG MA,QINGRONG FENG,SHOUSHENG YAN,SUICHEN LIANG,YI GAO,YUNXI SUN		
706	SSC0700553		YBa2(Cu,Ag)3O7	Y1Ba2Cu2.85Ag0.15O7	Y	1	Ba	2	Cu	2.85	Ag	0.15													O	7		1	1989																												Y123																				90					90										58																																																																																											DETERMINARION OF FLUX PINNING POTENTIALS FROM FIELD-INDUCED ANISOTROPY IN OXIDE SUPERCONDUCTORS	198905	MAGNETIZATION            ,PINNING                  ,RAYLEIGH	DEPARTMENT OF PHYSICS,PEKING UNIVERSITY,BEIJING 100871,PRC	SOLID STATE COMMUN.,70(1989)553	HONG MA,QINGRONG FENG,SHOUSHENG YAN,SUICHEN LIANG,YI GAO,YUNXI SUN		
707	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	1	1989																											3	Y123																				90.6					90.6																																																																																																					THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
708	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	Z	6.82	1	1989																											3	Y123																				91.2					91.2																																																																																																					THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
709	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Z	6.66	1	1989																											3	Y123																				88.9					88.9																																																																																																					THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
710	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.47	Y	1	Ba	2	Cu	3															O	Z	6.47	1	1989																												Y123																				43.6					43.6																																																																																																					THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
711	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.46	Y	1	Ba	2	Cu	3															O	Z	6.46	1	1989																												Y123																				45					45																																																																																																					THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
712	SSC0700561		YBa2Cu3O7	Y1Ba2Cu3O6.19	Y	1	Ba	2	Cu	3															O	Z	6.19	1	1989																												Y123																																																																																																																														THE EFFECT OF A MODERATE-TEMPERATURE ANNEALING ON THE STRUCTURE AND TEMPERATURE OF A SUPERCONDUCTIVE CONVERSION OF CERAMICSYBA2CU3OY	198905		INSTITUTE OF SOLID STATE PHYSICS,CHERNOGOLOVKA,MOSCOW IBL.142432,USSR	SOLID STATE COMMUN.,70(1989)561	A.V.PALNICHENKO,I.N.KREMENSKAYA,M.A.NEVEDOMSKAYA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAYEV,V.F.DEGTYARYOVA,V.SH.SHEHTMAN,YU.A.OSIPIAN	Y,BA,CU,O	
713	SSC0700631	NOT S/C	CeBa2Cu3O7	Ce1Ba2Cu3O7.4	Ce	1	Ba	2	Cu	3															O	7.4	7.4	1	1989																												Y123	PMMM			6.208	6.232	8.759																																																																																																																								STRUCTURE STUDY OF BA2CECU3O7.4	198905	EXAFS	RECEIVED 25 JANUARY 1989 BY W.Y.KUAN	SOLID STATE COMMUN.,70(1989)631	CHEN ZHUYAO,CHENG TINGZHU,GAO CHEN,LIN YING,LIU WENHAN,QIAN YITAI,WANG HSIN	BA,CE,CU,O	
714	SSC0700661		TlSr2(Ca,Sm)Cu2O7	Tl1Sr2Ca0.5Sm0.5Cu2O6.75	Tl	1	Sr	2	Ca	0.5	Sm	0.5	Cu	2											O	6.75	6.75	1	1989																												Tl1212				3.817		12.054														37.6					37.6																																																																																														TL2O3,SRO,CAO,SM2O3	0	SIN(900C 4H IN O2)-FURNACE COOL TO RT					THE CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY OF NEW SUPERCONDUCTING PHASE TISR2CA0.5SM0.5CU2O6.75	198905	STRUCTURE                ,XRY	INSTITUTE OF PHYSICS,ACADEMIA SINICA,BEIJING 100080,CHINA	SOLID STATE COMMUN.,70(1989)661	G.H.RAO,J.K.LIANG,S.S.XIE,X.R.CHENG,Y.L.ZHANG,Z.X.ZHAO	TL,SR,CA,SM,CU,O	
715	PRB0399689			Bi1.84Pb0.34Sr2Cu3O10	Bi	1.84	Pb	0.34	Sr	2	Cu	3													O	10			1989									6.5			GPa		82	GPa		34.2	GPa		45.7		0.2			253000			Bi2212				5.396		37.18																																																																														312																																										ELASTIC CONSTANTS OF THE POLYCRYSTALLINE BI-PB-SR-CA-CU-O SUPERCONDUCTOR	198905	ELASTIC CONSTANTS        ,SHEAR MODULUS            ,DEBYE	NATIONAL INSTITUTE OF STANDARDS AND TECHNOLOGY,BOULDER,COLORADO 80303	PHYS.REV.B.,39(1989)9689	H.M.LEDBETTER,K.TOGANO,R.B.GOLDFARD,S.A.KIM	BI,PB,SR,CA,CU,O	
716	PRB0399611		YBa2Cu4O8	Y1Ba2Cu4O8+-Z	Y	1	Ba	2	Cu	4															O	8+-Z			1989																												Y124																			82						82																																																			1								500																																										NONLINEAR TEMPERATURE DEPENDENCE OF THE NORMAL-STATE RESISTIVITY IN YBA2CU4O8+-ZFILMS	198905	RESISITIVITY             ,FILMS                    ,NONLINEA	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.B.,39(1989)9611	A.F.HEBARD,A.T.FIORY,C.E.RICE,M.GURVITCH,P.L.GAMMEL,R.M.FIEMING,S.MARTIN	Y,BA,CU,O	
717	PRB0399611		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1989																												Y123																			91.5						91.5																																																			3																																																		NONLINEAR TEMPERATURE DEPENDENCE OF THE NORMAL-STATE RESISTIVITY IN YBA2CU4O8+-ZFILMS	198905	RESISITIVITY             ,FILMS                    ,NONLINEA	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.B.,39(1989)9611	A.F.HEBARD,A.T.FIORY,C.E.RICE,M.GURVITCH,P.L.GAMMEL,R.M.FIEMING,S.MARTIN	Y,BA,CU,O	
718	PHC1580143		Tl(Ba,La)2CuO5	Tl1Ba1La1Cu1O5	Tl	1	Ba	1	La	1	Cu	1													O	5			1989																												Tl1201				3.843		9.01																																																																																																					25.7																			SUPERCONDUCTIVITY OF TLBA(1+X)LA(1-X)CUO(5) WITH 1201 STRUCTURE	198904	MATERIAL                 ,XRY                      ,RES                      ,SUS	FUNDAMENTAL RESEARCH LABORATORIES,RESOURCE AND ENVIORONMENT PROTECTION RESEARCH LABORATORIES,NEC CORPORATION,4-1-1,MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYSICA C ,158(1989)143	H.IGARASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,LA,CU,O	
719	PHC1580143		Tl(Ba,La)2CuO5	Tl1Ba1.1La0.9Cu1O5	Tl	1	Ba	1.1	La	0.9	Cu	1													O	5			1989																												Tl1201				3.84		9.054														39.6					39.6																																																																																		3.6																			SUPERCONDUCTIVITY OF TLBA(1+X)LA(1-X)CUO(5) WITH 1201 STRUCTURE	198904	MATERIAL                 ,XRY                      ,RES                      ,SUS	FUNDAMENTAL RESEARCH LABORATORIES,RESOURCE AND ENVIORONMENT PROTECTION RESEARCH LABORATORIES,NEC CORPORATION,4-1-1,MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYSICA C ,158(1989)143	H.IGARASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,LA,CU,O	
720	PHC1580143		Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5			1989																												Tl1201				3.834		9.107														41.1					41.1																																																																																		3.6																			SUPERCONDUCTIVITY OF TLBA(1+X)LA(1-X)CUO(5) WITH 1201 STRUCTURE	198904	MATERIAL                 ,XRY                      ,RES                      ,SUS	FUNDAMENTAL RESEARCH LABORATORIES,RESOURCE AND ENVIORONMENT PROTECTION RESEARCH LABORATORIES,NEC CORPORATION,4-1-1,MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYSICA C ,158(1989)143	H.IGARASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,LA,CU,O	
721	PHC1580143		Tl(Ba2La)2CuO5	Tl1Ba1.4La0.6Cu1O5	Tl	1	Ba	1.4	La	0.6	Cu	1													O	5			1989																												Tl1201				3.838		9.223																																																																																																					8.3																			SUPERCONDUCTIVITY OF TLBA(1+X)LA(1-X)CUO(5) WITH 1201 STRUCTURE	198904	MATERIAL                 ,XRY                      ,RES                      ,SUS	FUNDAMENTAL RESEARCH LABORATORIES,RESOURCE AND ENVIORONMENT PROTECTION RESEARCH LABORATORIES,NEC CORPORATION,4-1-1,MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYSICA C ,158(1989)143	H.IGARASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,LA,CU,O	
722	PHC1580148		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-X	Nd	1.85	Ce	0.15	Cu	1															O	4-X			1989																												T'				3.946		12.081														21					21																																																																																																					SINTHESIS AND X-RAY CHARACTERIZATION OF SUPERCONDUCTING AND RELATED Ln2-xCexCuO4-y(Ln=Nd AND GD) COMPOUNDS			IBM Research Division, Almaden Research Center, 650 Harry Road, San Jose, CA 95120-6099, USA	Physica C, 159(1989)148-152	A.I. NAZZAL,E. MORAN,J.B. TORRANCE,T.C. HUANG		
723	PHC1580148		(Gd,Ce)2CuO4	Gd1.85Ce0.15Cu1O4-X	Gd	1.85	Ce	0.15	Cu	1															O	4-X			1989																												T'				3.902		11.831																																																																																																																								SINTHESIS AND X-RAY CHARACTERIZATION OF SUPERCONDUCTING AND RELATED Ln2-xCexCuO4-y(Ln=Nd AND GD) COMPOUNDS			IBM Research Division, Almaden Research Center, 650 Harry Road, San Jose, CA 95120-6099, USA	Physica C, 159(1989)148-152	A.I. NAZZAL,E. MORAN,J.B. TORRANCE,T.C. HUANG		
724	PHC1530026		YBa2Cu3Oz	Y1Ba2Cu3O6.86	Y	1	Ba	2	Cu	3															O	7-X	6.86		1988																											3	Y123				3.818	3.891	11.674													91						91																																3.3	0.88																																														0.28	11			0.68	23		0.000000000156			0.00000000045												THE ANISOTROPIC SUPERCONDUCTIVITY OF R(1)BA(2)CU(3)O(7-X) (R:Y,GD AND HO) SINGLE CRYSTALS		SINGLE CRYSTAL           ,ANISOTROPY               ,RES                      ,HALL EFFECT	THE INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,TOKYO	PHYSICA C, 153(1988)26	HIROYUKI TAKEYA,HUMIHIKO TAKEI,NOBORU MIURA,TOSHIRO SAKAKIBARA,TSUNEAKI GOTO,TSUYOSHI TAMEGAI,YASUHIKO IYE	Y,GD,HO,BA,CU,O	
725	PHC1531357		YBa2Cu3Oz	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-X	6.96		1988																											3	Y123																				85					85																																3.12	0.32						46	4.6																											12.5												0.2				0.6	18		0.0000000023			0.0000000041												TRANSPORT PROPERTIES OF A Y(1)BA(2)CU(3)O(7-Z) SINGLE CRYSTAL		SINGLE CRYSTAL           ,ANISOTROPY               ,HC                       ,HALL EFFECT	CENTRE D'ETUDES NUCLEAIRES,DEPARTMENT DE RECHERCHE FONDAMENTALE,38041 GRENOBLE CEDEX-F	Physica C,153(1988)1357	C.AYACHE,J.ROSSAT-MIGNOD,J.Y.HENRY,L.FORRO,M.RAKI,P.C.E.STAMP	Y,BA,CU,O	
726	PRB0387016			Tl2Ca2Ba2Cu3OX	Tl	2	Ca	2	Ba	2	Cu	3													O	X			1988																												Tl2223				3.85		36														120					120																																																																																						0.0000000026			5.3		RH726										HALL EFFECT OF THE HIGH-TcSUPERCONDUCTING OXIDES BI-CA-SR-CU-O AND TL(2)CA(2)BA(2)CU(3)O(X)	198810	HALL EFFECT              ,RES	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,38(1988)7016	C.W.CHU,J.CLAYHOLD,N.P.ONG,P.H.HOR	BI,CA,SR,CU,O,TL,CA,BA,CU,O	
727	PRB0390729			Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X			1989																												Bi2212																																																																																																							0.16				0.29				2.2			2.8												HALL COEFFICIENT OF SINGLE-CRYSTAL BI(2)SR(2)CA(1)CU(2)O(Y)	198901	SINGLE CRYSTAL           ,CARRIER DENSITY          ,HALL EFF	INSTITUTE OF PHYSICS,ACADEMIA SINICA,BEIJING,CHINA	PHYS.REV.B,39(1989)729	H.M.DUAN,L.LI,L.LU,Y.F.YAN,Y.LU	BI,SR,CA,CU,O	
728	SSC0700725		YBa2Cu3Oz	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X		1	1989																											3	Y123				3.82	3.886	11.67														91.9					91.9																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
729	SSC0700725		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.95Ni0.05OX	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	X		1	1989																											3	Y123				3.826	3.886	11.67														86.8					86.8																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
730	SSC0700725		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1OX	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	X		1	1989																											3	Y123				3.818	3.88	11.66														82.9					82.9																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
731	SSC0700725		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.95Zn0.05OX	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	X		1	1989																											3	Y123				3.822	3.881	11.68														72.2					72.2																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
732	SSC0700725		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1OX	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	X		1	1989																											3	Y123				3.825	3.881	11.68														54.3					54.3																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
733	SSC0700725		NdBa2Cu3O7	Nd1Ba2Cu3OX	Nd	1	Ba	2	Cu	3															O	X		1	1989						3.4	-30.7																				3	Y123				3.859	3.913	11.76														93					93																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
734	SSC0700725		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.95Ni0.05OX	Nd	1	Ba	2	Cu	2.95	Ni	0.05													O	X		1	1989						3.4	-38.6																				3	Y123				3.878	3.919	11.73														85					85																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
735	SSC0700725		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.9Ni0.1OX	Nd	1	Ba	2	Cu	2.9	Ni	0.1													O	X		1	1989						3.2	-43.1																				3	Y123				3.863	3.906	11.74														70.9					70.9																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
736	SSC0700725		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.95Zn0.05OX	Nd	1	Ba	2	Cu	2.95	Zn	0.05													O	X		1	1989						3.2	-33.1																				3	Y123				3.868	3.895	11.74														65					65																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
737	SSC0700725		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.9Zn0.1OX	Nd	1	Ba	2	Cu	2.9	Zn	0.1													O	X		1	1989						3.2	-22.1																				3	Y123				3.873	3.905	11.75														36.9					36.9																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
738	SSC0700725		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X		1	1989						7.9	5.4																				3	Y123				3.844	3.896	11.7														93.4					93.4																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
739	SSC0700725		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.95Ni0.05OX	Gd	1	Ba	2	Cu	2.95	Ni	0.05													O	X		1	1989						7.4	2.7																				3	Y123				3.85	3.885	11.68														86.2					86.2																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
740	SSC0700725		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.9Ni0.1OX	Gd	1	Ba	2	Cu	2.9	Ni	0.1													O	X		1	1989						7.7	4.5																				3	Y123				3.845	3.883	11.69														84.5					84.5																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
741	SSC0700725		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.95Zn0.05OX	Gd	1	Ba	2	Cu	2.95	Zn	0.05													O	X		1	1989						7.8	5.1																				3	Y123				3.845	3.89	11.7														72.5					72.5																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
742	SSC0700725		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.9Zn0.1OX	Gd	1	Ba	2	Cu	2.9	Zn	0.1													O	X		1	1989						7.8	0.9																				3	Y123				3.842	3.89	11.7														53.6					53.6																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
743	SSC0700725		DyBa2Cu3O7	Dy1Ba2Cu3OX	Dy	1	Ba	2	Cu	3															O	X		1	1989						10.5	-5.2																				3	Y123				3.83	3.892	11.67														91.3					91.3																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
744	SSC0700725		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.95Ni0.05OX	Dy	1	Ba	2	Cu	2.95	Ni	0.05													O	X		1	1989						10.6	-6.1																				3	Y123				3.827	3.89	11.67														87.5					87.5																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
745	SSC0700725		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.9Ni0.1OX	Dy	1	Ba	2	Cu	2.9	Ni	0.1													O	X		1	1989						10.5	-6.4																				3	Y123				3.831	3.87	11.66														81.8					81.8																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
746	SSC0700725		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.95Zn0.05OX	Dy	1	Ba	2	Cu	2.95	Zn	0.05													O	X		1	1989						10.8	-5.2																				3	Y123				3.83	3.877	11.66														71.5					71.5																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
747	SSC0700725		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.9Zn0.1OX	Dy	1	Ba	2	Cu	2.9	Zn	0.1													O	X		1	1989						10.7	-7.1																				3	Y123				3.831	3.881	11.67														49.3					49.3																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
748	SSC0700725		ErBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X		1	1989						9.3	-5.6																				3	Y123				3.818	3.881	11.67														91.7					91.7																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
749	SSC0700725		ErBa2(Cu,Ni)3O7	Er1Ba2Cu2.95Ni0.05OX	Er	1	Ba	2	Cu	2.95	Ni	0.05													O	X		1	1989						9.6	-8.5																				3	Y123				3.819	3.88	11.67														87.8					87.8																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
750	SSC0700725		ErBa2(Cu,Ni)3O7	Er1Ba2Cu2.9Ni0.1OX	Er	1	Ba	2	Cu	2.9	Ni	0.1													O	X		1	1989						9.4	-7.9																				3	Y123				3.819	3.879	11.66														83.3					83.3																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
751	SSC0700725		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.95Zn0.05OX	Er	1	Ba	2	Cu	2.95	Zn	0.05													O	X		1	1989						9.5	-8																				3	Y123				3.815	3.877	11.66														73.1					73.1																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
752	SSC0700725		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.9Zn0.1OX	Er	1	Ba	2	Cu	2.9	Zn	0.1													O	X		1	1989						9.5	-5.8																				3	Y123				3.818	3.874	11.66														51.8					51.8																																																																																														R2O3,BACO3,CUO,NIO,ZNO	0	CAL(930C 10H IN AIR)-SIN(930C 10H IN AIR)-COOL(140C/H)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF RBA(2)CU(3-X)M(X)O(Y) (R=Y,ND,GD,DY AND ER; M=NI AND ZN)	198906	TC                       ,SUS                      ,SUBSTITUTION             ,CU	DEPARTMENT OF PHYSICS,COLLEGE OF SCIENCE & TECHNOLOGY,NIHON UNIVERSITY,KANDA-SURUGADAI 1-8,CHIYODA-KU,TOKYO 101,JAPAN	SOLID STATE COMMUN.,70(1989)725	KAZUKO SEKIZAWA,TAKAMICHI INABA,YOSHIKI TAKANO	Y,ND,GD,DY,ER,NI,ZN,CU,BA,O	
753	PHC1580230			Bi2Sr1.3Ca0.7Cu1O8-Z	Bi	2	Sr	1.3	Ca	0.7	Cu	1													O	8-Z			1989																																5.392	5.394	24.537													62	84	82				84																																																																																																					MAGNETIC PENETRATION DEPTH IN BI(2)(SR,CA)(2)CUO(8-Z)	198904		INSTITUT FUR MITTELENERGIEPHYSIK,ETHZ,CH-5232 VILLIGEN PSI,SWITZERLAND	PHYSICA C ,158(1989)230	A.SCHENCK,B.HETTICH,B.HITTI,E.LIPPELT,F.N.GYGAX,H.MALETTA,M.WEBER,P.BIRRER	BI,SR,CA,CU,O	
754	PR0399074		La(Ba,Ca)2Cu3O7	La1Ba1Ca1Cu3O6.98	La	1	Ba	1	Ca	1	Cu	3													O	7+Z	6.98		1989																												Y123				3.87		11.61													74.2		78.5				76.35																															1.07							20			A		640																																																										PREPARATION,CHARACTERIZATION,AND SUPERCONDUCTING PROPERTIES OFTETRAGONAL LABACACU(3)O(7+X)	5	HC                  ,OXYGEN CONTENT      ,MAGNETIZATION       ,RESISTIVITY	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA 95616	PHYS.REV.B.,39(1989)9074	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,M.COSTANTINO,P.A.HAHN,P.KLAVINS,R.N.SHELTON	LA,BA,CA,CU,O	
755	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.12	Er	1	Ba	2	Cu	3															O	X	6.12		1989																												Y123				3.836		11.733																																																																																																																								LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
756	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.23	Er	1	Ba	2	Cu	3															O	X	6.23		1989																												Y123				3.85		11.772																																																																																																																								LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
757	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.15	Er	1	Ba	2	Cu	3															O	X	6.15		1989																												Y123				3.839	3.868	11.762														35					35																																																																																																					LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
758	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.34	Er	1	Ba	2	Cu	3															O	X	6.34		1989																												Y123				3.836	3.864	11.754														20					20																																																																																																					LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
759	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.31	Er	1	Ba	2	Cu	3															O	X	6.31		1989								0.54																				Y123				3.822	3.876	11.713														55					55																																																																																																					LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
760	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.67	Er	1	Ba	2	Cu	3															O	X	6.67		1989								0.57																				Y123				3.812	3.89	11.67														85					85																																																																																																					LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
761	PRB0399099		ErBa2Cu3Oz	Er1Ba2Cu3O6.91	Er	1	Ba	2	Cu	3															O	X	6.91		1989								0.6																				Y123				3.814	3.887	11.661														92					92																																																																																																					LOW-DEMENSIONAL MAGNETIC ORDERING AND ISING- AND XY-LINK ANISOTROPY OF ER(3+) IN THE SYSTEM ERBA(2)CU(3)O(X) WITH 6<X<7	198905	OXYGEN CONTENT      ,MAGNETIC ORDERING   ,SUSCEPTIBILITY      ,HEAT-CAPACITY	DEPERTMENT OF PYSICS,CARNEGIE-MELLON UNIVERSITY,PITTSBURGH,PENNSYIVANIA 15213	PHYS.REV.B.,39(1989)9099	G.H.BELLESIS,H.S.LESSURE,J.LUKIN,M.GREENBLATT,S.A.FRIEDBERG,S.M.FINE,S.SIMIZU	ER,BA,CU,O	
762	PHC1710181	LARGE MEASURING CURRENT CAUSES A RE-ENTRANT BEHAVIOUR,TC(SUS)=31K	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1990																											1	BKBO				4.285																28.9	30.6			2.8	28.9																						18									0.87							43															SP762				0.06		324																							12																			AC SUSCEPTIBILITY, RESISTIVITY AND SPECIFIC HEAT OF THE CUBICSUPERCONDUCTOR BA0.6K0.4BIO3			CSIRO DIVISION OF APPLIED PHYSICS, SYDNEY, AUSTRALIA 2070	PHYSICA C,171(1990)181	C.ANDRIKIDIS,E.R.VANCE,K.-H.MULLER,N.SAVVIDES,S.J.COLLOCOTT	BA,K,BI,O	
763	PRB0358807		(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4			1987																												T																																																																																																																		0.00000000038												HALL EFFECT OF LA(2-X)SR(X)CU(1)O(4): IMPLIC ATIONS FOR THE ELECTRONIC STRUCTURE IN THE NORMAL STATE		HALL EFFECT	PRINCETON UNIV.,PRINCETON,NEW JERSEY,USA	PHYS.REV.B,35(1987)8807	J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG		
764	PRB0358807		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4			1987																												T																																																																																																																		0.000000002												HALL EFFECT OF LA(2-X)SR(X)CU(1)O(4): IMPLIC ATIONS FOR THE ELECTRONIC STRUCTURE IN THE NORMAL STATE		HALL EFFECT	PRINCETON UNIV.,PRINCETON,NEW JERSEY,USA	PHYS.REV.B,35(1987)8807	J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG		
765	PRB0358807		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																																																																																																																		0.000000003												HALL EFFECT OF LA(2-X)SR(X)CU(1)O(4): IMPLIC ATIONS FOR THE ELECTRONIC STRUCTURE IN THE NORMAL STATE		HALL EFFECT	PRINCETON UNIV.,PRINCETON,NEW JERSEY,USA	PHYS.REV.B,35(1987)8807	J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG		
766	PRB0358807		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4			1987																												T																																																																																																				0.82														0.0000000048												HALL EFFECT OF LA(2-X)SR(X)CU(1)O(4): IMPLIC ATIONS FOR THE ELECTRONIC STRUCTURE IN THE NORMAL STATE		HALL EFFECT	PRINCETON UNIV.,PRINCETON,NEW JERSEY,USA	PHYS.REV.B,35(1987)8807	J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG		
767	PRB0358807		(La,Sr)2CuO4	La1.5Sr0.5Cu1O4	La	1.5	Sr	0.5	Cu	1															O	4			1987																												T																																																																																																				7.2														0.000000013												HALL EFFECT OF LA(2-X)SR(X)CU(1)O(4): IMPLIC ATIONS FOR THE ELECTRONIC STRUCTURE IN THE NORMAL STATE		HALL EFFECT	PRINCETON UNIV.,PRINCETON,NEW JERSEY,USA	PHYS.REV.B,35(1987)8807	J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG		
768	SSC0650573		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1988																												T																																																																																																																		0.000000158												HALL EFFECT MEASUREMENTS IN LA2-XSRXCUO4				SOLID STATE COMMUN.65(1988)573	A.HAMZIC,E.TUTIS,L.FORRO,M.PETRAVIC	LA,SR,CU,O	
769	SSC0650573		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1988																												T																																																																																																																		0.0000000063												HALL EFFECT MEASUREMENTS IN LA2-XSRXCUO4				SOLID STATE COMMUN.65(1988)573	A.HAMZIC,E.TUTIS,L.FORRO,M.PETRAVIC	LA,SR,CU,O	
770	SSC0650573		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1988																												T																																																																																																																		0.0000000013												HALL EFFECT MEASUREMENTS IN LA2-XSRXCUO4				SOLID STATE COMMUN.65(1988)573	A.HAMZIC,E.TUTIS,L.FORRO,M.PETRAVIC	LA,SR,CU,O	
771	SSC0650573		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1988																												T																																																																																																																		0.00000000093												HALL EFFECT MEASUREMENTS IN LA2-XSRXCUO4				SOLID STATE COMMUN.65(1988)573	A.HAMZIC,E.TUTIS,L.FORRO,M.PETRAVIC	LA,SR,CU,O	
772	SSC0650573		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4			1988																												T																																																																																																																		0.00000000056												HALL EFFECT MEASUREMENTS IN LA2-XSRXCUO4				SOLID STATE COMMUN.65(1988)573	A.HAMZIC,E.TUTIS,L.FORRO,M.PETRAVIC	LA,SR,CU,O	
773	PRB0392312		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1989																												T																																																																																																							7800				346																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
774	PRB0392312		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O	4			1989																												T																																																																																																							3.4				6.31				0.0000000133			0.0000000137												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
775	PRB0392312		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1989																												T																				26.2					26.2																																																																														0.287				0.958				0.00000000373			0.00000000517												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
776	PRB0392312		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1989																												T																				28.6					28.6																																																																														0.236				0.75				0.0000000016			0.0000000023												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
777	PRB0392312		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1989																												T																				18.9					18.9																																																																														0.165				0.531				0.00000000074			0.00000000103												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
778	PRB0392312		(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4			1989																												T																				15.2					15.2																																																																														0.109				0.333				0.0000000003			0.000000000395												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
779	PRB0392312		(La,Sr)2CuO4	La1.66Sr0.36Cu1O4	La	1.66	Sr	0.36	Cu	1															O	4			1989																												T																																																																																																							0.096				0.299				0.000000000037			0.000000000035												HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
780	PRB0382910		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90					90																																																																																						0.00000000062															ELECTRONIC PROPERTIES OF BA(2)Y(1-X)PR(X)CU(3)O(7-Z)	198808	HALL EFFECT              ,RESISTIVITY              ,OXYGEN CONTENT           ,TC	NTT BASIC RESEARCH LABORATORIES,MUSASHINO-SHI,TOKYO,JAPAN	PHYS.REV.B,38(1988)2910	A.MATSUDA,H.SHIBATA,K.KINOSHITA,T.ISHII,T.WATANABE,T.YAMADA	Y,PR,BA,CU,O	
781	SSC0680929		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91.7					91.7																																																																																						0.0000000008			0.0000000026		RH781			Y203,BACO3,CUO	0	SIN(925C 12H IN O2)-COOL TO RT IN 5H					HALL-EFFECT OF BULK Y(1)BA(2)CU(3)O(7-Z)	198812	HALL-EFFECT              ,RESISTIVITY              ,MAGNETO-	II.PHYS.INST.,UNIV.KOLN,ZULPICHER STR.77,KOLN,FRG	SOLID STATE COMMUN.,68(1988)929	E.ZIRNGIEBL,M.GALFFY	Y,BA,CU,O	
782	PRB0367124		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																				91					91																																																																																						0.0000000015															REEXAMINATION OF THE Y(2)O(3)-BA(1)O(1)-CU(1)O(1) PHASE DIAGRAM FOR SOLID SOLUTIONS NEAR Y(1)BA(2)CU(3)O(7)	198711	HALL EFFECT              ,SOLID SOLUTION           ,PHASE DIAGRAM            ,TC	WESTINGHOUSE RESEARCH AND DEVELOPMENT CENTER,PITTSBURGH,PENNSYLVANIA	PHYS.REV.B,36(1987)7124	A.I.BRAGINSKI,A.J.PANSON,G.R.WAGNER	Y,BA,CU,O	
783	PRB0390777		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1989																												Y123																				94					94																																																																																						0.0000000005			0.00000000136												CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
784	PHC1570083		YBa2Cu3O7	Y1Ba2Cu3O6.962	Y	1	Ba	2	Cu	3															O	Z	6.962		1989																												Y123				3.82	3.886	11.68													89.5	92.2	92.8				92.2																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
785	PHC1570083		YBa2Cu3Oz	Y1Ba2La1.94Cu3O6.963	Y	1	Ba	2	La	1.94	Cu	3													O	Z	6.963		1989																																3.818	3.887	11.669													90.7	91.8	92.7				91.8																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
786	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.92La0.08Cu3O6.965	Y	1	Ba	1.92	La	0.08	Cu	3													O	Z	6.965		1989																												Y123				3.817	3.887	11.664													91.6	92.6	93.2				92.6																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
787	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.975	Y	1	Ba	1.9	La	0.1	Cu	3													O	Z	6.975		1989																												Y123				3.816	3.887	11.664													92.6	93.9	94.7				93.9																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
788	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.86La0.14Cu3O6.98	Y	1	Ba	1.86	La	0.14	Cu	3													O	Z	6.98		1989																												Y123				3.818	3.887	11.651													86.6	89.4	92				89.4																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
789	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O7.013	Y	1	Ba	1.8	La	0.2	Cu	3													O	Z	7.013		1989																												Y123				3.821	3.886	11.643													77.3	80.5	82.5				80.5																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
790	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.76La0.24Cu3O7.024	Y	1	Ba	1.76	La	0.24	Cu	3													O	Z	7.024		1989																												Y123				3.823	3.883	11.636													70.2	73.4	78				73.4																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
791	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.7La0.3Cu3O7.059	Y	1	Ba	1.7	La	0.3	Cu	3													O	Z	7.059		1989																												Y123				3.837	3.869	11.618													58.8	61.4	64				61.4																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
792	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.66La0.34Cu3O7.073	Y	1	Ba	1.66	La	0.34	Cu	3													O	Z	7.073		1989																												Y123				3.851	3.859	11.597													54	56	59.2				56																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
793	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.6La0.4Cu3O7.083	Y	1	Ba	1.6	La	0.4	Cu	3													O	Z	7.083		1989																												Y123				3.855		11.581													45.5	49.4	53.5				49.4																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
794	PHC1570083		Y(Ba,La)2Cu3Oz	Y1Ba1.54La0.46Cu3O7.118	Y	1	Ba	1.54	La	0.46	Cu	3													O	Z	7.118		1989																												Y123				3.856		11.566													41.1	44.1	49.5				44.1																																																																																																					THE EFFECT OF LA SUBSTITUTION ON THE SUPERCONDUCTIVITY OF BA(2)-YCU(3)O(Y)	198901	HALL EFFECT              ,VALENCE                  ,OXYGEN CONTENT           ,CARRIER CONCENTRATION	RESEARCH LABORATORY OF ENG.MATERIALS,TOKYO INSTITUTE OF TECHNOL-OGY,NAGATSUTA 4259,MIDORI-KU,YOKOHAMA	PHYSICA C,157(1989)83	MITSURU ITOH,RUIXING LIANG,RYOZO AOKI,TETSURO NAKAMURA	LA,BA,Y,CU,O	
795	PHC1590141		YBa2(Cu,Co)3Oz	Y1Ba2Cu2.95Co0.05O6.88	Y	1	Ba	2	Cu	2.95	Co	0.05													O	Z	6.88		1989																												Y123				3.832	3.884	11.687														91.2					91.2																																																																																																					STRUCTURAL CHANGES OF THE SUPERCONDUCTOR YBA(2)CU(3)O(7) BY COBALT SUBSTITUTION.A HIGH-RESOLUTION NEUTRON POWDER DIFFRACTIONSTUDY	198906		INSTITUT FUR KRISTALLOGRAPHIE DER UNIVERSITAT,7400 TUBINGEN,FED.REP.GERMANY	PHYSICA C ,159(1989)141	A.HOSER,A.W.HEWAT,D.HOHLWEIN,M.SCHLICHENMAIER,R.KIEMEL,R.SONNTAG,S.KEMMLER-SACK,S.LOSCH,W.PRANDL,W.SCHAFER	Y,BA,CU,O	
796	PHC1590141		YBa2(Cu,Co)3Oz	Y1Ba2Cu2.9Co0.1O6.89	Y	1	Ba	2	Cu	2.9	Co	0.1													O	Z	6.89		1989																												Y123				3.866		11.674														55.3					55.3																																																																																																					STRUCTURAL CHANGES OF THE SUPERCONDUCTOR YBA(2)CU(3)O(7) BY COBALT SUBSTITUTION.A HIGH-RESOLUTION NEUTRON POWDER DIFFRACTIONSTUDY	198906		INSTITUT FUR KRISTALLOGRAPHIE DER UNIVERSITAT,7400 TUBINGEN,FED.REP.GERMANY	PHYSICA C ,159(1989)141	A.HOSER,A.W.HEWAT,D.HOHLWEIN,M.SCHLICHENMAIER,R.KIEMEL,R.SONNTAG,S.KEMMLER-SACK,S.LOSCH,W.PRANDL,W.SCHAFER	Y,BA,CU,O	
797	PHC1590141		YBa2(Cu,Co)3Oz	Y1Ba2Cu2.8Co0.2O6.9	Y	1	Ba	2	Cu	2.8	Co	0.2													O	Z	6.9		1989																												Y123				3.87		11.675																																																																																																																								STRUCTURAL CHANGES OF THE SUPERCONDUCTOR YBA(2)CU(3)O(7) BY COBALT SUBSTITUTION.A HIGH-RESOLUTION NEUTRON POWDER DIFFRACTIONSTUDY	198906		INSTITUT FUR KRISTALLOGRAPHIE DER UNIVERSITAT,7400 TUBINGEN,FED.REP.GERMANY	PHYSICA C ,159(1989)141	A.HOSER,A.W.HEWAT,D.HOHLWEIN,M.SCHLICHENMAIER,R.KIEMEL,R.SONNTAG,S.KEMMLER-SACK,S.LOSCH,W.PRANDL,W.SCHAFER	Y,BA,CU,O	
798	PHC1590141		YBa2(Cu,Co)3Oz	Y1Ba2Cu2.7Co0.3O6.93	Y	1	Ba	2	Cu	2.7	Co	0.3													O	Z	6.93		1989																												Y123				3.875		11.683														16.9					16.9																																																																																																					STRUCTURAL CHANGES OF THE SUPERCONDUCTOR YBA(2)CU(3)O(7) BY COBALT SUBSTITUTION.A HIGH-RESOLUTION NEUTRON POWDER DIFFRACTIONSTUDY	198906		INSTITUT FUR KRISTALLOGRAPHIE DER UNIVERSITAT,7400 TUBINGEN,FED.REP.GERMANY	PHYSICA C ,159(1989)141	A.HOSER,A.W.HEWAT,D.HOHLWEIN,M.SCHLICHENMAIER,R.KIEMEL,R.SONNTAG,S.KEMMLER-SACK,S.LOSCH,W.PRANDL,W.SCHAFER	Y,BA,CU,O	
799	PHC1590141		YBa2(Cu,Co)3Oz	Y1Ba2Cu2.35Co0.65O6.99	Y	1	Ba	2	Cu	2.35	Co	0.65													O	Z	6.99		1989																												Y123				3.889		11.651																																																																																																																								STRUCTURAL CHANGES OF THE SUPERCONDUCTOR YBA(2)CU(3)O(7) BY COBALT SUBSTITUTION.A HIGH-RESOLUTION NEUTRON POWDER DIFFRACTIONSTUDY	198906		INSTITUT FUR KRISTALLOGRAPHIE DER UNIVERSITAT,7400 TUBINGEN,FED.REP.GERMANY	PHYSICA C ,159(1989)141	A.HOSER,A.W.HEWAT,D.HOHLWEIN,M.SCHLICHENMAIER,R.KIEMEL,R.SONNTAG,S.KEMMLER-SACK,S.LOSCH,W.PRANDL,W.SCHAFER	Y,BA,CU,O	
800	PHC1590124		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18O7	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	7			1989																												Y123																				74					74																																																																																																					DYNAMICS OF FE IN SUPERCONDUCTING YBA(2)(CU(1-X)FE(X))(3)O(Y)BY NEUTRON SCATTERING	198906	TIME OF FLIGHT           ,NEUTRON DIFFRACTION      ,ELASTIC INTENSITY        ,PR	LABORATOIRE LEON BRILLOUIN,CEN-SACLAY,91191 GIF-SUR-YVETTE CEDEX,FRANCE	PHYSICA C ,159(1989)124	A.MENELLE,G.CODDENS,I.MIREBEAU,K.MOORJANI,M.HENNION,M.HERVIEU,T.E.PHILLIPS	Y,BA,CU,FE,O	
801	PHC1590124		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.64Fe0.36O7	Y	1	Ba	2	Cu	2.64	Fe	0.36													O	7			1989																												Y123																				32					32																																																																																																					DYNAMICS OF FE IN SUPERCONDUCTING YBA(2)(CU(1-X)FE(X))(3)O(Y)BY NEUTRON SCATTERING	198906	TIME OF FLIGHT           ,NEUTRON DIFFRACTION      ,ELASTIC INTENSITY        ,PR	LABORATOIRE LEON BRILLOUIN,CEN-SACLAY,91191 GIF-SUR-YVETTE CEDEX,FRANCE	PHYSICA C ,159(1989)124	A.MENELLE,G.CODDENS,I.MIREBEAU,K.MOORJANI,M.HENNION,M.HERVIEU,T.E.PHILLIPS	Y,BA,CU,FE,O	
802	PHC1590137		YBa2Cu3(I,O)7	Y1Ba2Cu3IOZ	Y	1	Ba	2	Cu	3	I														O	Z			1989																												Y123				3.84	3.887	11.721																																																																																																																								OXYGEN-IODINE ISOMORPHISM IN THE Y-BA-CU-O CERAMICS	198906	XRY                      ,SUBSTITUTION             ,IODINE                   ,MO	INSTITUTE OF SOLID STATE PHYSICS AND INSTITUTE OFEXPERIMENTALMINEROLOGY,USSR AC.SCI.,CHERNOGOLOVKA,MOSCOW DISTRICT,142432,USSR	PHYSICA C ,159(1989)137	A.M.GROMOV,G.V.NOVIKOV,L.V.SYPAVINA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAEV,V.I.KULAKOV,YU.A.OSIPYAN	Y,BA,CU,O	
803	PHC1590137		YBa2(Cu,Fe)3(I,O)7	Y1Ba2Cu2.94Fe0.06IOZ	Y	1	Ba	2	Cu	2.94	Fe	0.06	I												O	Z			1989																												Y123																																																																																																																														OXYGEN-IODINE ISOMORPHISM IN THE Y-BA-CU-O CERAMICS	198906	XRY                      ,SUBSTITUTION             ,IODINE                   ,MO	INSTITUTE OF SOLID STATE PHYSICS AND INSTITUTE OFEXPERIMENTALMINEROLOGY,USSR AC.SCI.,CHERNOGOLOVKA,MOSCOW DISTRICT,142432,USSR	PHYSICA C ,159(1989)137	A.M.GROMOV,G.V.NOVIKOV,L.V.SYPAVINA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAEV,V.I.KULAKOV,YU.A.OSIPYAN	Y,BA,CU,O	
804	PHC1590137		YBa2(Cu,Fe)3(I,O)7	Y1Ba2Cu2.7Fe0.3IOZ	Y	1	Ba	2	Cu	2.7	Fe	0.3	I												O	Z			1989																												Y123				3.872		11.736																																																																																																																								OXYGEN-IODINE ISOMORPHISM IN THE Y-BA-CU-O CERAMICS	198906	XRY                      ,SUBSTITUTION             ,IODINE                   ,MO	INSTITUTE OF SOLID STATE PHYSICS AND INSTITUTE OFEXPERIMENTALMINEROLOGY,USSR AC.SCI.,CHERNOGOLOVKA,MOSCOW DISTRICT,142432,USSR	PHYSICA C ,159(1989)137	A.M.GROMOV,G.V.NOVIKOV,L.V.SYPAVINA,N.S.SIDOROV,O.V.ZHARIKOV,R.K.NIKOLAEV,V.I.KULAKOV,YU.A.OSIPYAN	Y,BA,CU,O	
805	PHC1590087		Bi2Sr2CaCu2O8	Bi2Ca1Sr2Cu2O8+Z	Bi	2	Ca	1	Sr	2	Cu	2													O	8+Z			1989																												Bi2212				5.376	5.423	30.72														81					81																																																																																																					NEUTRON DIFFRACTION EVIDENCE FOR OXYGEN DIMERS IN Bi-Ca-Sr-Cu-O SUPERCONDUCTORS			Neutron Physics Division, Bhabha Atomic Research Centre, Trombay, Bombay 400 085, India	Physica C159(1989)87	A. SWQUEIRA,C.N.R. RAO,H. RAJAGOPAL,R. NAGARAJAN		
806	PHC1590087			Bi2Ca2Sr1Cu2O8+Z	Bi	2	Ca	2	Sr	1	Cu	2													O	8+Z			1989																												Bi2212				5.356	5.409	30.37														70					70																																																																																																					NEUTRON DIFFRACTION EVIDENCE FOR OXYGEN DIMERS IN Bi-Ca-Sr-Cu-O SUPERCONDUCTORS			Neutron Physics Division, Bhabha Atomic Research Centre, Trombay, Bombay 400 085, India	Physica C159(1989)87	A. SWQUEIRA,C.N.R. RAO,H. RAJAGOPAL,R. NAGARAJAN		
807	PHC1590087			Bi2Ca1.5Y0.5Sr1Cu2O8+Z	Bi	2	Ca	1.5	Y	0.5	Sr	1	Cu	2											O	8+Z			1989																																5.386	5.403	30.37														65					65																																																																																																					NEUTRON DIFFRACTION EVIDENCE FOR OXYGEN DIMERS IN Bi-Ca-Sr-Cu-O SUPERCONDUCTORS			Neutron Physics Division, Bhabha Atomic Research Centre, Trombay, Bombay 400 085, India	Physica C159(1989)87	A. SWQUEIRA,C.N.R. RAO,H. RAJAGOPAL,R. NAGARAJAN		
808	PHC1590075		Tl2Ba2Ca2Cu3Oz	Tl2Ca2Ba2Cu3OZ	Tl	2	Ca	2	Ba	2	Cu	3													O	Z			1989																												Tl2223																				125					125																																																																																																					NATURE OF THE SUPERCONDUCTING TRANSITION IN HIGH T(C) TL-CA-BA-CU-O COMPOUNDS:POSITION ANNIHILATION STUDIES	198906	POSITRON ANNIHILATION    ,OXYGEN VALENCE	CHEMICAL GROUP,BHABHA ATOMIC RESEARCH CENTRE,TROMAY,BOMBAY 400085,INDIA	PHYSICA C ,159(1989)75	G.M.PHATAK,I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.K.PUJARI,P.V.P.S.S.SASTRY,R.M.IYER,S.B.MANOHAR,SATYA PRAKASH,T.DATTA	TL,CA,BA,CU,O	
809	PHC1590075		Tl2Ba2CaCu2Oz	Tl2Ca1Ba2Cu2OZ	Tl	2	Ca	1	Ba	2	Cu	2													O	Z			1989																												Tl2212				3.847		29.22														108					108																																																																																																					NATURE OF THE SUPERCONDUCTING TRANSITION IN HIGH T(C) TL-CA-BA-CU-O COMPOUNDS:POSITION ANNIHILATION STUDIES	198906	POSITRON ANNIHILATION    ,OXYGEN VALENCE	CHEMICAL GROUP,BHABHA ATOMIC RESEARCH CENTRE,TROMAY,BOMBAY 400085,INDIA	PHYSICA C ,159(1989)75	G.M.PHATAK,I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.K.PUJARI,P.V.P.S.S.SASTRY,R.M.IYER,S.B.MANOHAR,SATYA PRAKASH,T.DATTA	TL,CA,BA,CU,O	
810	NAT3390293		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1989																											2	T'																				22.3					22.3																																																																																																					Anomalous absence of pressure effect on transition temperature in the electron-doped superconductor Nd1.85Ce0.15CuO4-d				Nature 339(1989)293-294	C.Murayama,H.Takagi,N.Mori,S.Uchida,S.Yomo,Y.Tokura		
811	NAT3390293		(Nd,Ce,Sr)2CuO4	Nd1.3Ce0.2Sr0.5Cu1O4-Z	Nd	1.3	Ce	0.2	Sr	0.5	Cu	1													O	4-Z		1	1989																											2	T*																				24					24			K/GPa	3																																																																																																	Anomalous absence of pressure effect on transition temperature in the electron-doped superconductor Nd1.85Ce0.15CuO4-d				Nature 339(1989)293-294	C.Murayama,H.Takagi,N.Mori,S.Uchida,S.Yomo,Y.Tokura		
812	PHC1590093			Bi2Sr3Cu2OZ	Bi	2	Sr	3	Cu	2															O	Z			1989																																4.888	5.396	24.804																																																																																																																								PHASES AND THEIR RELATIONS IN THE BI-SR-CU-O SYSTEM	198906	PHASE DIAGRAM            ,MAG                      ,XRD                      ,TEM	INSTITUTE FOR CHEMICAL RESEARCH,KYOTO UNIVERSITY,UJI,KYOTO-FU611,JAPAN	PHYSICA C ,159(1989)93	HIROYUKI ITO,KAZUHISA INABA,MIKIO TAKANO,SHINICHI SHIMOMURA,YASUNORI IKEDA,YASUSHI OUE,ZENJI HIROI	BI,SR,CU,O	
813	PHC1590093			Bi4Sr8Cu5OZ	Bi	4	Sr	8	Cu	5															O	Z			1989																																34.035	24.05	5.389																																																																																																																								PHASES AND THEIR RELATIONS IN THE BI-SR-CU-O SYSTEM	198906	PHASE DIAGRAM            ,MAG                      ,XRD                      ,TEM	INSTITUTE FOR CHEMICAL RESEARCH,KYOTO UNIVERSITY,UJI,KYOTO-FU611,JAPAN	PHYSICA C ,159(1989)93	HIROYUKI ITO,KAZUHISA INABA,MIKIO TAKANO,SHINICHI SHIMOMURA,YASUNORI IKEDA,YASUSHI OUE,ZENJI HIROI	BI,SR,CU,O	
814	PHC1590093			Bi1Sr3OZ	Bi	1	Sr	3																	O	Z			1989																																17.147	16.758	16.998																																																																																																																								PHASES AND THEIR RELATIONS IN THE BI-SR-CU-O SYSTEM	198906	PHASE DIAGRAM            ,MAG                      ,XRD                      ,TEM	INSTITUTE FOR CHEMICAL RESEARCH,KYOTO UNIVERSITY,UJI,KYOTO-FU611,JAPAN	PHYSICA C ,159(1989)93	HIROYUKI ITO,KAZUHISA INABA,MIKIO TAKANO,SHINICHI SHIMOMURA,YASUNORI IKEDA,YASUSHI OUE,ZENJI HIROI	BI,SR,CU,O	
815	PR03911445		La2CuO4	La2Cu1O4+Z	La	2	Cu	1																	O	4+Z			1989								272																				T																				35	39.8				35																																																																																																					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING AND NEEL TENPERATURES IN A LA(2)CUO(4+Z) CRYSTAL	6	RESISTANCE          ,SINGLE CRYSTAL      ,PRESSURE            ,ANTIFERROMAGNETIC	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO 87545	PHYS.REV.B.,39(1989)11445	F.H.GARZON,J.D.THOMPSON,M.C.ARONSON,S-W.CHEONG,Z.FISK	LA,CU,O	
816	JJP0280060			Tb1Pb1Sr2Ca3Cu4OZ	Tb	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																																36	60				36																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
817	JJP0280060			Dy1Pb1Sr2Ca3Cu4OZ	Dy	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																																																																																																																																										SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
818	JJP0280060			Ho1Pb1Sr2Ca3Cu4OZ	Ho	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																	3.886														26	41	61				41																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
819	JJP0280060			Er1Pb1Sr2Ca3Cu4OZ	Er	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																															16	33	54				33																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
820	JJP0280060			Tm1Pb1Sr2Ca3Cu4OZ	Tm	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																															34	38	58				38																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
821	JJP0280060			Yb1Pb1Sr2Ca3Cu4OZ	Yb	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																															48	48	70				48																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
822	JJP0280060			Lu1Pb1Sr2Ca3Cu4OZ	Lu	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																															38	33	75				33																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
823	JJP0280060			Y1Pb1Sr2Ca3Cu4OZ	Y	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.845															16	31	49				31																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
824	JJP0280060			La1Pb1Sr2Ca3Cu4OZ	La	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.848																22	39				22																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
825	JJP0280060			Ce1Pb1Sr2Ca3Cu4OZ	Ce	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.85																	62				62																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
826	JJP0280060			Pr1Pb1Sr2Ca3Cu4OZ	Pr	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.857																18	47				18																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
827	JJP0280060			Nd1Pb1Sr2Ca3Cu4OZ	Nd	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.861																40	51				40																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
828	JJP0280060			Sm1Pb1Sr2Ca3Cu4OZ	Sm	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																3.88															27	35	60				35																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
829	JJP0280060			Eu1Pb1Sr2Ca3Cu4OZ	Eu	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																																38					38																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
830	JJP0280060			Gd1Pb1Sr2Ca3Cu4OZ	Gd	1	Pb	1	Sr	2	Ca	3	Cu	4											O	Z			1989																																															50	42	70				42																																																																																																					SUPERCONDUCTIVITY IN A LN-PB-SR-CA-CU-O SYSTEM	198901	CRYSTAL STRUCTURE        ,TC                       ,RES                      ,XR	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.OSAKA	JJAP LETT.,28(1989)L60	HIROFUMI HIRANO,OSAMU INOUE,SEIJI ADACHI,SYUNICHIRO KAWASHIMA,YUKIHIRO TAKAHASHI	Y,PB,SR,CA,CU,O,LN	
831	JJP0280049		(Nd,Ce,Sr)2CuO4	Nd1.2Ce0.35Sr0.45Cu1O4-Z	Nd	1.2	Ce	0.35	Sr	0.45	Cu	1													O	4-Z			1989																												T*				3.86		12.5														21.2					21.2																																																																																																					PREPARATION OF AN ALMOST SINGLE PHASE SUPERCONDUCTOR IN THE ND-CE-SR-CU-O SYSTEM	198901	SINGLE PFASE             ,STRUCTURE                ,OXYGEN PRESSURE          ,FA	YOKOHAMA R & D LABORATORIES,FURUKAWA ELECTRIC,YOKOHAMA	JJAP LETT.,28(1989)L49	MICHIKAZU KOSUGE	ND,CE,SR,CU,O	
832	JJP0270607		NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				94.2					94.2																																																																																									0.00000000151												CORRELATION OF TC WITH HOLE CONCENTRATION IN COPPER-OXIDE SUPERCONDUCTORS;HALL EFFECT MEASUREMENT IN ND(1+X)BA(2-X)CU(3)O(7-Z)	198804	HOLE CONCENTRATION       ,HALL EFFECT              ,TC	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA CITY,IBARAKI	JJAP.LETT.,27(1988)L607	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	ND,BA,CU,O	
833	JJP0270607		Nd(Ba,Nd)2Cu3O7	Nd1.1Ba1.9Cu3O7-Z	Nd	1.1	Ba	1.9	Cu	3															O	7-Z			1988																												Y123																				78.5					78.5																																																																																									0.00000000265												CORRELATION OF TC WITH HOLE CONCENTRATION IN COPPER-OXIDE SUPERCONDUCTORS;HALL EFFECT MEASUREMENT IN ND(1+X)BA(2-X)CU(3)O(7-Z)	198804	HOLE CONCENTRATION       ,HALL EFFECT              ,TC	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA CITY,IBARAKI	JJAP.LETT.,27(1988)L607	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	ND,BA,CU,O	
834	JJP0270607		Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3O7-Z	Nd	1.2	Ba	1.8	Cu	3															O	7-Z			1988																												Y123																				48.8					48.8																																																																																									0.00000000437												CORRELATION OF TC WITH HOLE CONCENTRATION IN COPPER-OXIDE SUPERCONDUCTORS;HALL EFFECT MEASUREMENT IN ND(1+X)BA(2-X)CU(3)O(7-Z)	198804	HOLE CONCENTRATION       ,HALL EFFECT              ,TC	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA CITY,IBARAKI	JJAP.LETT.,27(1988)L607	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	ND,BA,CU,O	
835	JJP0270607		Nd(Ba,Nd)2Cu3O7	Nd1.3Ba1.7Cu3O7-Z	Nd	1.3	Ba	1.7	Cu	3															O	7-Z			1988																												Y123																				34.2					34.2																																																																																									0.00000000735												CORRELATION OF TC WITH HOLE CONCENTRATION IN COPPER-OXIDE SUPERCONDUCTORS;HALL EFFECT MEASUREMENT IN ND(1+X)BA(2-X)CU(3)O(7-Z)	198804	HOLE CONCENTRATION       ,HALL EFFECT              ,TC	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA CITY,IBARAKI	JJAP.LETT.,27(1988)L607	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	ND,BA,CU,O	
836	PHC1590181			La6.4Sr1.6Cu8O20-Y	La	6.4	Sr	1.6	Cu	8															O	20-Y			1989																																																																																																																																											-0.0000000004			-0.0000000042												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
837	PHC1590181			La6.13Sr1.87Cu8O20-Y	La	6.13	Sr	1.87	Cu	8															O	20-Y			1989																																																																																																																																											-0.0000000004			-0.0000000006												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
838	PHC1590181			La5.87Sr2.13Cu8O20-Y	La	5.87	Sr	2.13	Cu	8															O	20-Y			1989																																																																																																																																											-0.0000000007			-0.0000000008												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
839	PHC1590181			La1.9Sr1.1Cu2O6+Y	La	1.9	Sr	1.1	Cu	2															O	6+Y		1	1989																																																																																																																																1.76							1.7				0.00000000035			0.00000000035												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
840	PHC1590181			La4Ba1Cu5O13-Y	La	4	Ba	1	Cu	5															O	13-Y			1989																																																																																																																													0.5			0.8							3.6				-0.0000000005			-0.00000000025												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
841	PHC1590181		(La,Ca)2CaCu2O6	La1.9Ca1.1Cu2O6+Y	La	1.9	Ca	1.1	Cu	2															O	6+Y			1989																												2126																																																																																																				40							45				0.0000000112			0.0000000112												TRANSPORT PROPERTIES OF NON-SUPERCONDUCTING LA-CUPRATES	198906	MAGNETRORESISTANCE  ,TRANSPORT PROPERTIES,RESISTIVITY         ,HALL COEFFICIENT	THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI MINATO-KU,TOKYO 106,JAPAN	PHYSICA C.,159(1989)181	TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,CA,CU,O,SR,BA	
842	PHC1590215	(dC/Tc) = 67 mJ/K2.mol	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1989	emu/g	0.00000042																										Y123																						89.8			89.8										65																																														mJ/mol.K2	4		438																																										SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
843	PHC1590215		Tl2Ba2CuOz	Tl2Ba2Cu1OX	Tl	2	Ba	2	Cu	1															O	X			1989	emu/g	0.00000005																										Tl2201																							12												8																																														mJ/mol.K2	0		238																																										SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
844	PHC1590215	(dC/Tc) = 35 mJ/K2.mol	Tl2Ba2CaCu2Oz	Tl2Ba2Ca1Cu2OX	Tl	2	Ba	2	Ca	1	Cu	2													O	X			1989	emu/g	0.00000029																										Tl2212																			101	106		99.5			106										51																																																	254																																										SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
845	PHC1590215	(dC/Tc) = 20 mJ/K2.mol	Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3OX	Tl	2	Ba	2	Ca	2	Cu	3													O	X			1989	emu/g	0.0000004																										Tl2223																			125	129		121.4			129										24																																																	290																																										SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
846	PRB03911587			Bi8Sr8Co4O25	Bi	8	Sr	8	Co	4															O	25			1989																																21.836	5.462	23.45																																																																																																																								Sturacture and magnetic properties of nonsuperconducting doped Co and Fe Bi2Sr2Cu1-xMxOy phases	1989		Bell Communications Research, Red Bank, New Jersey 07701	Phys.Rev.B.,39(1989)11587	D.A. Neumann,D.M. Hwang,E. Tselepis,G. Pleizier,G.W. Hull,J.J. Rhyne,J.M. Tarascon,L.H. Greene,M. Eibschuts,M. giroud,P. Barboux,P.F. Miceli,W.R. McKinnon,Yvon Lepage		
847	PRB03911587		Bi2Sr2CuO4	Bi2Sr2Cu1OX	Bi	2	Sr	2	Cu	1															O	X			1989																																5.376		24.56																																																																																																																								Sturacture and magnetic properties of nonsuperconducting doped Co and Fe Bi2Sr2Cu1-xMxOy phases	1989		Bell Communications Research, Red Bank, New Jersey 07701	Phys.Rev.B.,39(1989)11587	D.A. Neumann,D.M. Hwang,E. Tselepis,G. Pleizier,G.W. Hull,J.J. Rhyne,J.M. Tarascon,L.H. Greene,M. Eibschuts,M. giroud,P. Barboux,P.F. Miceli,W.R. McKinnon,Yvon Lepage		
848	PRB03911587			Bi2Sr2Co1OX	Bi	2	Sr	2	Co	1															O	X			1989						2.4	-130	150																								5.464		23.47																																																																																																																								Sturacture and magnetic properties of nonsuperconducting doped Co and Fe Bi2Sr2Cu1-xMxOy phases	1989		Bell Communications Research, Red Bank, New Jersey 07701	Phys.Rev.B.,39(1989)11587	D.A. Neumann,D.M. Hwang,E. Tselepis,G. Pleizier,G.W. Hull,J.J. Rhyne,J.M. Tarascon,L.H. Greene,M. Eibschuts,M. giroud,P. Barboux,P.F. Miceli,W.R. McKinnon,Yvon Lepage		
849	PRB03911587		Bi2Sr2(Cu,Co)Oz	Bi2Sr2Cu0.5Co0.5OX	Bi	2	Sr	2	Cu	0.5	Co	0.5													O	X			1989																												Bi2201				5.411		23.99																																																																																																																								Sturacture and magnetic properties of nonsuperconducting doped Co and Fe Bi2Sr2Cu1-xMxOy phases	1989		Bell Communications Research, Red Bank, New Jersey 07701	Phys.Rev.B.,39(1989)11587	D.A. Neumann,D.M. Hwang,E. Tselepis,G. Pleizier,G.W. Hull,J.J. Rhyne,J.M. Tarascon,L.H. Greene,M. Eibschuts,M. giroud,P. Barboux,P.F. Miceli,W.R. McKinnon,Yvon Lepage		
850	PHC1590173		GdBa2(Cu,Fe)3Oz	Gd1Ba2Cu2.64Fe0.36O6.99	Gd	1	Ba	2	Cu	2.64	Fe	0.36													O	Z	6.99		1989																												Y123				3.891		11.679														21					21																																																																																																					DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
851	PHC1590173		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.55Fe0.45OZ	Gd	1	Ba	2	Cu	2.55	Fe	0.45													O	Z			1989																												Y123				3.891		11.69																																																																																																																								DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
852	PHC1590173		GdBa2(Cu,Fe)3Oz	Gd1Ba2Cu2.46Fe0.54O7.06	Gd	1	Ba	2	Cu	2.46	Fe	0.54													O	Z	7.06		1989																												Y123				3.889		11.685																																																																																																																								DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
853	PHC1590173		GdBa2Cu3Oz	Gd1Ba2Cu3O6.99	Gd	1	Ba	2	Cu	3															O	Z	6.99		1989																												Y123				3.84	3.904	11.71														94					94																																																																																																					DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
854	PHC1590173		GdBa2(Cu,Fe)3Oz	Gd1Ba2Cu2.91Fe0.09O6.94	Gd	1	Ba	2	Cu	2.91	Fe	0.09													O	Z	6.94		1989																												Y123				3.878		11.71														75					75																																																																																																					DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
855	PHC1590173		GdBa2(Cu,Fe)3Oz	Gd1Ba2Cu2.82Fe0.18O6.91	Gd	1	Ba	2	Cu	2.82	Fe	0.18													O	Z	6.91		1989																												Y123				3.88		11.672														41					41																																																																																																					DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
856	PHC1590173		GdBa2(Cu,Fe)3Oz	Gd1Ba2Cu2.73Fe0.27O6.98	Gd	1	Ba	2	Cu	2.73	Fe	0.27													O	Z	6.98		1989																												Y123				3.887		11.699														40					40																																																																																																					DEPENDENCE OF STRUCTURE AND T(C) UPON THE DISTRIBUTION OF IRONOVER THE COPPER SITES IN GDBA(2)(CU(1-X)FE(X))(3)0(Z)	198906	TC                  ,STRUCTURE           ,IRON DOPED          ,OXYGEN CONTENT	KERNFORSCHUNGSZENTRUM KARLSRUHE,INSTITUT FUR NUKLEARE FESTKORPERPHYSIK,P.O.B.3640,D-7500 KARLSRUHE,FED.REP.GERMANY	PHYSICA C.,159(1989)173	A.SEIDEL,G.CZJZEK,H.J.BORNEMANN,P.ADELMANN,R.KMIEC	GD,BA,CU,FE,O	
857	PHC1590195		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7			1989							38																					Y123				3.853	3.908	11.73														88.1					88.1													580									137																9			A		680														10																																												MAGNETIC CHARACTERISTICS OF NORMAL AND SUPERCONDUCTIVE STATES IN SmBa2Cu3O7			Institute of Physics, Chinese Academy of Sciences Beijing, P.O. Box P.R. China	Physica.C,159(1989)195-200	J.Q. ZHENG,N. CAO,W.Y. GUAN,X.S. CHEN		
858	PHC1590188		GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z			1989																											3	Y123				3.814	3.904	11.73														92.7					92.7																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
859	PHC1590188	KAIZERO=EMU/G.OE,CURIEC=EMU.K/G.OE	GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.972Fe0.03OZ	Gd	1	Ba	2	Cu	2.972	Fe	0.03													O	Z			1989			EMU.K/G.OE	0.0115		7.42	3.1																				3	Y123				3.826	3.904	11.733														90					90																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
860	PHC1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.95Fe0.05OZ	Gd	1	Ba	2	Cu	2.95	Fe	0.05													O	Z			1989																											3	Y123				3.862	3.897	11.727														89.1					89.1																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
861	PHC1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.93Fe0.07OZ	Gd	1	Ba	2	Cu	2.93	Fe	0.07													O	Z			1989																											3	Y123				3.874	3.894	11.718														86.9					86.9																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
862	PHC1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.9Fe0.1OZ	Gd	1	Ba	2	Cu	2.9	Fe	0.1													O	Z			1989						6	-7																				2	Y123				3.891		11.688														75.3					75.3																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
863	CR1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.85Fe0.15OZ	Gd	1	Ba	2	Cu	2.85	Fe	0.15													O	Z			1989		-57180000000000000000000000				5.21	-6.7																				2	Y123				3.896		11.688														69.1					69.1																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
864	PHC1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.8Fe0.2OZ	Gd	1	Ba	2	Cu	2.8	Fe	0.2													O	Z			1989						4.39	-4.3																				2	Y123				3.897		11.697														58.7					58.7																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
865	PHC1590188		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3OZ	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	Z			1989						3.32	-2.1																				2	Y123				3.9		11.7														36.2					36.2																																																																																																					CRYSTAL STRUCTURE,TC,MAGNETIC PROPERTIES AND MOSSBAUER SPECTRUM OF FE-DOPED GDBA2CU3O7-Z	198906	MAGNETIC PROPERTY   ,SUBSTITUTION        ,STRUCTURE           ,MASSBAUER           ,MAGNETIC MOMENT	DEPARTMENT OF PHYSICS,NATIONAL CHENG KUNG UNIVERSITY,TAINAN,TAIWAN	PHYSICA C,159(1989)188	C.L.LIN,C.TIEN,K.C.LIN,S.T.LIN	GD,BA,CU,O,FE	
866	PRB0375901		YBa2Cu3Oz	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-Z	6.96		1988																											3	Y123																				88.1					88.1																																																																																																					ANOMALOUS ULTRASOUND PROPAGATION IN HIGH-TC SUPERCONDUCTORS:LA(1.8)SR(0.2)CU(1)O(4-Y) AND Y(1)BA(2)CU(3)O(7-Z)	198804	ATTENUATION              ,SOUND VELOCITY	CORPORATE RESEARCH SCIENCE LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,37(1988)5901	A.J.JACOBSON,D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI,M.J.HIGGINS,S.BHATTACHARYA	LA,SR,CU,O,Y,BA,CU,O	
867	PRB0375901		(La,Sr)2CuO4	La1.8Sr0.2Cu1O3.95	La	1.8	Sr	0.2	Cu	1															O	4-Z	3.95		1988																											3	T																				30.4					30.4																																																																																																					ANOMALOUS ULTRASOUND PROPAGATION IN HIGH-TC SUPERCONDUCTORS:LA(1.8)SR(0.2)CU(1)O(4-Y) AND Y(1)BA(2)CU(3)O(7-Z)	198804	ATTENUATION              ,SOUND VELOCITY	CORPORATE RESEARCH SCIENCE LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,37(1988)5901	A.J.JACOBSON,D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI,M.J.HIGGINS,S.BHATTACHARYA	LA,SR,CU,O,Y,BA,CU,O	
868	PHC1590105		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1989																											2	Bi2212				5.408		30.83													69.5	72.5	77.5				72.5																																																																																													3220000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
869	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.9Lu0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Lu	0.1	Cu	2											O	8+Z			1989																											2	Bi2212				5.399		30.68													76	83.5	93				83.5																																																																																													3010000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
870	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.8Lu0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Lu	0.2	Cu	2											O	8+Z			1989																											2	Bi2212				5.407		30.69													79.5	89.5	100				89.5																																																																																													2610000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
871	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.7Lu0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Lu	0.3	Cu	2											O	8+Z			1989																											2	Bi2212				5.414		30.57													70.5	87	102.5				87																																																																																													2100000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
872	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.6Lu0.4Cu2O8+Z	Bi	2	Sr	2	Ca	0.6	Lu	0.4	Cu	2											O	8+Z			1989																											3	Bi2212				5.421	5.402	30.44													49	65	87				65																																																																																													1120000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
873	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.5Lu0.5Cu2O8+Z	Bi	2	Sr	2	Ca	0.5	Lu	0.5	Cu	2											O	8+Z			1989																											3	Bi2212				5.422	5.401	30.36													18.5	29	60.5				29																																																																																													631000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
874	PHC1590105		Bi2Sr2(Ca,Lu)O8	Bi2Sr2Ca0.4Lu0.6Cu2O8+Z	Bi	2	Sr	2	Ca	0.4	Lu	0.6	Cu	2											O	8+Z			1989																											3	Bi2212				5.429	5.406	30.31																																																																																																																661000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
875	PHC1590105		Bi2Sr2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.3Lu0.7Cu2O8+Z	Bi	2	Sr	2	Ca	0.3	Lu	0.7	Cu	2											O	8+Z			1989																											3	Bi2212				5.445	5.397	30.32																																																																																																																330000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
876	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.9Na0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Na	0.1	Cu	2											O	8+Z			1989																											2	Bi2212				5.404		30.88													65	70.5	74.5				70.5																																																																																													2990000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
877	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.8Na0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Na	0.2	Cu	2											O	8+Z			1989																											2	Bi2212				5.408		30.81													68	73.5	79				73.5																																																																																													3120000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
878	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.7Na0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Na	0.3	Cu	2											O	8+Z			1989																											2	Bi2212				5.401		30.75													65.5	72.5	79				72.5																																																																																													2840000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
879	PHC1590105		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1989																											2	Bi2212				5.395		30.77													55	60	63.5				60																																																																																													3710000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
880	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.9Na0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Na	0.1	Cu	2											O	8+Z			1989																											2	Bi2212				5.396		30.64													59.5	63.5	68.5				63.5																																																																																													3230000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
881	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.8Na0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Na	0.2	Cu	2											O	8+Z			1989																											2	Bi2212				5.391		30.8													62	66	72.5				66																																																																																													2880000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
882	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.7Na0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Na	0.3	Cu	2											O	8+Z			1989																											2	Bi2212				5.404		30.71													60.5	65.5	71				65.5																																																																																													3110000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
883	PHC1590105		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1989																											2	Bi2212				5.391		30.73													44	49.5	54				49.5																																																																																													3670000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
884	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.9Na0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Na	0.1	Cu	2											O	8+Z			1989																											2	Bi2212				5.387		30.67													46.5	51	56				51																																																																																													3750000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
885	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.8Na0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Na	0.2	Cu	2											O	8+Z			1989																											2	Bi2212				5.398		30.64													49	53	58.5				53																																																																																													3690000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
886	PHC1590105		Bi2Sr2(Ca,Na)Cu2O8	Bi2Sr2Ca0.7Na0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Na	0.3	Cu	2											O	8+Z			1989																											2	Bi2212				5.406		30.86													49.5	54	60				54																																																																																													3380000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
887	PRB0404503		YBa2Cu3Oz	Y1Ba2Cu3O6.15	Y	1	Ba	2	Cu	3															O	6+X	6.15	3	1989						0.35		370																			2	Y123				3.863		11.82																																																																																																																								NEUTRON SCATTERING STUDY OF MAGNETIC EXCITATIONS IN YBA2CU3O6+X	198909	NEUTRON SCATTERING  ,SINGLE CRYSTALS     ,SPIN WAVES          ,ACOUSTIC MODES	PHYSICS DEPARTMENT,BROOKHAVEN NATIONAL LAVORATORY,UPTON,NEW YORK 11973	PHYS.REV.B,40(1989)4503	B.KEIMER,G.SHIRANE,J.M.TRANQUADA,M.SATO,S.SHAMOTO	Y,BA,CU,O	
888	PRB0404503		YBa2Cu3Oz	Y1Ba2Cu3O6.3	Y	1	Ba	2	Cu	3															O	6+X	6.3	3	1989						0.36		260																			2	Y123				3.863		11.8																																																																																																																								NEUTRON SCATTERING STUDY OF MAGNETIC EXCITATIONS IN YBA2CU3O6+X	198909	NEUTRON SCATTERING  ,SINGLE CRYSTALS     ,SPIN WAVES          ,ACOUSTIC MODES	PHYSICS DEPARTMENT,BROOKHAVEN NATIONAL LAVORATORY,UPTON,NEW YORK 11973	PHYS.REV.B,40(1989)4503	B.KEIMER,G.SHIRANE,J.M.TRANQUADA,M.SATO,S.SHAMOTO	Y,BA,CU,O	
889	PRB0404503		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	6+X	6.45	3	1989																											3	Y123						11.75														40					40																																																																																																					NEUTRON SCATTERING STUDY OF MAGNETIC EXCITATIONS IN YBA2CU3O6+X	198909	NEUTRON SCATTERING  ,SINGLE CRYSTALS     ,SPIN WAVES          ,ACOUSTIC MODES	PHYSICS DEPARTMENT,BROOKHAVEN NATIONAL LAVORATORY,UPTON,NEW YORK 11973	PHYS.REV.B,40(1989)4503	B.KEIMER,G.SHIRANE,J.M.TRANQUADA,M.SATO,S.SHAMOTO	Y,BA,CU,O	
890	PRB0404503		YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	6+X	6.5	3	1989																											3	Y123						11.73														20					20																																																																																																					NEUTRON SCATTERING STUDY OF MAGNETIC EXCITATIONS IN YBA2CU3O6+X	198909	NEUTRON SCATTERING  ,SINGLE CRYSTALS     ,SPIN WAVES          ,ACOUSTIC MODES	PHYSICS DEPARTMENT,BROOKHAVEN NATIONAL LAVORATORY,UPTON,NEW YORK 11973	PHYS.REV.B,40(1989)4503	B.KEIMER,G.SHIRANE,J.M.TRANQUADA,M.SATO,S.SHAMOTO	Y,BA,CU,O	
891	PRB0404503		YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6+X	6.8	3	1989																											3	Y123						11.7														83					83																																																																																																					NEUTRON SCATTERING STUDY OF MAGNETIC EXCITATIONS IN YBA2CU3O6+X	198909	NEUTRON SCATTERING  ,SINGLE CRYSTALS     ,SPIN WAVES          ,ACOUSTIC MODES	PHYSICS DEPARTMENT,BROOKHAVEN NATIONAL LAVORATORY,UPTON,NEW YORK 11973	PHYS.REV.B,40(1989)4503	B.KEIMER,G.SHIRANE,J.M.TRANQUADA,M.SATO,S.SHAMOTO	Y,BA,CU,O	
892	PRB03911680		YBa2Cu3Oz	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	Z	6	1	1989								395																			2	Y123																																																																																																																														INFLUENCE OF NI,FE,AND ZN SUBSTITUTION ON THE SUPERCONDUCTINGAND ANTIFERROMAGNETIC STATE OF YBA(2)CU(3)0(7-Z)	198906	SUBSTITUTION        ,SUSCEPTIBILITY      ,RES                 ,ANTIFERROMAGNETIC	INSTITUT FUR EXPERIMENTALPHYSIK IV,RUHR-UNIVERSITAT,D-4630 BOCHUM,WEST GERMANY	PHYS.REV.B.,39(1989)11680	H.BACH,H.J.WULLER,K.WESTERHOLT,P.STAUCHE	Y,BA,CU,O,NI,FE,ZN	
893	PRB03911680		YBa2Cu3Oz	Y1Ba2Cu3O6.1	Y	1	Ba	2	Cu	3															O	Z	6.1	1	1989								390																			2	Y123																																																																																																																														INFLUENCE OF NI,FE,AND ZN SUBSTITUTION ON THE SUPERCONDUCTINGAND ANTIFERROMAGNETIC STATE OF YBA(2)CU(3)0(7-Z)	198906	SUBSTITUTION        ,SUSCEPTIBILITY      ,RES                 ,ANTIFERROMAGNETIC	INSTITUT FUR EXPERIMENTALPHYSIK IV,RUHR-UNIVERSITAT,D-4630 BOCHUM,WEST GERMANY	PHYS.REV.B.,39(1989)11680	H.BACH,H.J.WULLER,K.WESTERHOLT,P.STAUCHE	Y,BA,CU,O,NI,FE,ZN	
894	PRB03911680		YBa2Cu3Oz	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	Z	6.35	1	1989								300																			2	Y123																																																																																																																														INFLUENCE OF NI,FE,AND ZN SUBSTITUTION ON THE SUPERCONDUCTINGAND ANTIFERROMAGNETIC STATE OF YBA(2)CU(3)0(7-Z)	198906	SUBSTITUTION        ,SUSCEPTIBILITY      ,RES                 ,ANTIFERROMAGNETIC	INSTITUT FUR EXPERIMENTALPHYSIK IV,RUHR-UNIVERSITAT,D-4630 BOCHUM,WEST GERMANY	PHYS.REV.B.,39(1989)11680	H.BACH,H.J.WULLER,K.WESTERHOLT,P.STAUCHE	Y,BA,CU,O,NI,FE,ZN	
895	PRB0404478		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1989																											3	Y123																				82					82																																																2.4																																																					QUASIPARTICLE DENSITY OF STATES IN THE PERPENDICULAR DIRECTIONTO THE CU-O PLANES IN YBA2CU3O7-X SINGLE-CRYSTAL THIN FILMS	198909	FILMS               ,ENERGY GAP	INSTITUTE FOR CHEMICAL RESEARCH,KYOTO UNIVERSITY,UJI 611,JAPAN	PHYS.REV.B,40(1989)4478	H.MAZAKI,J.TAKADA,K.HIRATA,K.IIJIMA,K.YAMAMOTO,T.TERASHIMA,Y.BANDO	TUNNELING SPECTRASINGLE-CRYSTAL	
896	SSC0710505		YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-Z	6.8	1	1989																											3	Y123																					91.4				91.4														113	340																										A			1400	6000																																																								MAGNETIC PENETRATION DEPTH IN ORIENTED YBACUO POWDER SAMPLES	198908	PENETRATION DEPTH   ,MAGNETIZATION	FREIE UNIVERSITAT BERLIN,FACHBEREICH PHYSIK,ARNIMALLEE 14,D-1000 BERLIN 33,WEST-GERMANY	SOLID STATE COMMUN.,71(1989)505	C.HUCHO,E.-W.SCHEIDT,K.LUDERS,V.MULLER	Y,BA,CU,O	
897	PRB0402170		YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95		1989																											3	Y123				3.82	3.889	11.676													89						89										90																																						2.6																																																					PHONON ANOMALIES AND RANGE OF SUPERCONDUCTING ENERGY GAPS FROMINFRARED STUDIES OF YBA2CU3O7-Z	198908	INFRARED            ,PHONONS             ,LATTICE-DYNAMICS    ,DIELECTRIC          ,ENERGY GAP	MAX-PLANCK-INSTIFUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE1,D-7000 STUTTART 80,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)2170	A.SIMON,A.WITTLIN,E.SCHONHERR,L.GENZEL,M.BAUER,M.CARDONA	Y,BA,CU,O	
898	PRB0402187		La2NiO4	La2Ni1O4	La	2	Ni	1																	O	4+Z	4	1	1989																											3	T	BMAB			5.466	5.533	12.555																																																																																																																								STRUCTURE OF THE INTERSTITIAL OXYGEN DEFECT IN LA2NIO4+Z	198908	RIETVELD REFINEMENT ,NEUTRON DIFFRACTION ,EXCESS OXYGEN       ,STRUCTURE	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.B,40(1989)2187	B.DABROWSKIFRACTION,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,SHIYOU PEIGEN	LA,NI,O	
899	PRB0402187		La2NiO4	La2Ni1O4.18	La	2	Ni	1																	O	4+Z	4.18	1	1989																											3	T	FMMM			5.461	5.472	12.714																																																																																																																								STRUCTURE OF THE INTERSTITIAL OXYGEN DEFECT IN LA2NIO4+Z	198908	RIETVELD REFINEMENT ,NEUTRON DIFFRACTION ,EXCESS OXYGEN       ,STRUCTURE	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.B,40(1989)2187	B.DABROWSKIFRACTION,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,SHIYOU PEIGEN	LA,NI,O	
900	SSC0710819			Bi1.84Pb0.34Sr1.91Ca2.03Cu3.06OZ	Bi	1.84	Pb	0.34	Sr	1.91	Ca	2.03	Cu	3.06											O	Z		1	1989									4.96																		2	Bi2223				5.42		37.16															105				105																																																																																						0.0000000022			0.00000000446				2840000000000000000000								RESISTIVITY,HALL COEFFICIENT AND TRANSITION TEMPERATURES IN DOPED 80K AND 110K BI-SR-CA-CU-O SUPERCONDUCTORS	198909	RESISTIVITY         ,HALL EFFECT         ,TC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OSAKA UNIVERSITY 1-1MACHIKANEYAMA,TOYONAKA,560 JAPAN	SOLID STATE COMMUN.,71(1989)819	K.MURASE,K.OTO,S.TAKAOKA	BI,SR,CA,CU,O	
901	SSC0710187			Bi0.7Pb0.3Sr1Ca1Cu1.8O6	Bi	0.7	Pb	0.3	Sr	1	Ca	1	Cu	1.8											O	6		1	1989																											2							37.6													73						73																																																									73		230																																										SPECIFIC HEAT AND RESISTIVITY OF THE HIGH-Tc SUPERCONDUCTOR BiCaSrCu2Ox FROM 2.5 TO 300K			Reserch Institute of Electricl Engineering, 190 11 Prague 9 - Bechovice	Solid State Commun.,71(1989)187-190	A. Belling,H. Hejdova',J. Bischof,J. Hrebi'k,V. Plechacek,Z. Trejbalova'		
902	SSC0710187			Bi1Sr1Ca1Cu2OX	Bi	1	Sr	1	Ca	1	Cu	2													O	X		1	1989																											2	Bi1112						30.8													80						80																																																											230																																										SPECIFIC HEAT AND RESISTIVITY OF THE HIGH-Tc SUPERCONDUCTOR BiCaSrCu2Ox FROM 2.5 TO 300K			Reserch Institute of Electricl Engineering, 190 11 Prague 9 - Bechovice	Solid State Commun.,71(1989)187-190	A. Belling,H. Hejdova',J. Bischof,J. Hrebi'k,V. Plechacek,Z. Trejbalova'		
903	PRB03911563		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4+Y	4	3	1989								320																				T																																																																																																																														Conductivity and Hall coefficient in La2CuO4+y near the insulator-metal transtion	1989		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B.,39(1989)	C.Y. Chen,D.R. Gabbe,H.P. Jenssen,M.A. Kastner,N.W. Preyer,P.J. Pikone,R.J. Birgeneau,Tineke Thio		
904	PRB03911563		La2CuO4	La2Cu1O4.02	La	2	Cu	1																	O	4+Y	4.02	3	1989								310																				T																																																																																																																														Conductivity and Hall coefficient in La2CuO4+y near the insulator-metal transtion	1989		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B.,39(1989)	C.Y. Chen,D.R. Gabbe,H.P. Jenssen,M.A. Kastner,N.W. Preyer,P.J. Pikone,R.J. Birgeneau,Tineke Thio		
905	PRB03911563		La2CuO4	La2Cu1O4.04	La	2	Cu	1																	O	4+Y	4.04	3	1989								285																				T																																																																																																																														Conductivity and Hall coefficient in La2CuO4+y near the insulator-metal transtion	1989		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B.,39(1989)	C.Y. Chen,D.R. Gabbe,H.P. Jenssen,M.A. Kastner,N.W. Preyer,P.J. Pikone,R.J. Birgeneau,Tineke Thio		
906	PRB03911563		La2CuO4	La2Cu1O4.052	La	2	Cu	1																	O	4+Y	4.052	3	1989								260																				T																																																																																																																														Conductivity and Hall coefficient in La2CuO4+y near the insulator-metal transtion	1989		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B.,39(1989)	C.Y. Chen,D.R. Gabbe,H.P. Jenssen,M.A. Kastner,N.W. Preyer,P.J. Pikone,R.J. Birgeneau,Tineke Thio		
907	PRB03911563		La2CuO4	La2Cu1O4.056	La	2	Cu	1																	O	4+Y	4.056	3	1989								240																				T																																																																																																																														Conductivity and Hall coefficient in La2CuO4+y near the insulator-metal transtion	1989		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B.,39(1989)	C.Y. Chen,D.R. Gabbe,H.P. Jenssen,M.A. Kastner,N.W. Preyer,P.J. Pikone,R.J. Birgeneau,Tineke Thio		
908	PHC1590105		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.8La0.2Ca1Cu2O8+X	Bi	2	Sr	1.8	La	0.2	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.411		30.64													73	85	92.5				85																																																																																													2310000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
909	PHC1590105		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.6La0.4Ca1Cu2O8+X	Bi	2	Sr	1.6	La	0.4	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.428		30.52													57	74	93.5				74																																																																																													1620000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
910	PHC1590105		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.4La0.6Ca1Cu2O8+X	Bi	2	Sr	1.4	La	0.6	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.442		30.41													18	25.5	39.5				25.5																																																																																													985000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
911	PHC1590105		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.2La0.8Ca1Cu2O8+X	Bi	2	Sr	1.2	La	0.8	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.45		30.31																																																																																																																								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
912	PHC1590105		Bi2(Sr,K)2CaCu2O8	Bi2Sr1.8K0.2Ca1Cu2O8+X	Bi	2	Sr	1.8	K	0.2	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.4		30.69													69.5	75	78.5				75																																																																																													3340000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
913	PHC1590105		Bi2(Sr,K)2CaCu2O8	Bi2Sr1.6K0.4Ca1Cu2O8+X	Bi	2	Sr	1.6	K	0.4	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.399		30.64													73.5	78	85.5				78																																																																																													2910000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
914	PHC1590105	600C,1BAR	Bi2(Sr,K)2CaCu2O8	Bi2Sr1.8K0.2Ca1Cu2O8+X	Bi	2	Sr	1.8	K	0.2	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.399		30.7													61.5	66.5	70.5				66.5																																																																																													3300000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
915	PHC1590105	48H, O2 ANNEAL	Bi2(Sr,K)2CaCu2O8	Bi2Sr1.6K0.4Ca1Cu2O8+X	Bi	2	Sr	1.6	K	0.4	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.396		30.6													69	73	78.5				73																																																																																													3470000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
916	PHC1590105	430C,250BAR	Bi2(Sr,K)2CaCu2O8	Bi2Sr1.8K0.2Ca1Cu2O8+X	Bi	2	Sr	1.8	K	0.2	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.391		30.69													49	55.5	60				55.5																																																																																													3530000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
917	PHC1590105	80H,O2 ANNEAL	Bi2(Sr,K)2CaCu2O8	Bi2Sr1.6K0.4Ca1Cu2O8+X	Bi	2	Sr	1.6	K	0.4	Ca	1	Cu	2											O	8+X			1989																												Bi2212				5.393		30.64													60	64	68				64																																																																																													3940000000000000000000								CORRELATION BETWEEN T(C) AND HOLE CONCENTRATION IN THE CATION-SUBSTITUTED BI(2)SR(2)CACU(2)O(8+Z) SYSTEM	198905	HIOE CONTENT        ,TC                  ,RES                 ,CATION	INSTITUTE FOR MATERIALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980,JAPAN	PHYSICA C.,159(1989)105	NORIO KOBAYASHI,SYOICHI HOSOYA,TETSUO FUKASE,YOJI KOIKE,YOSHIHIRO IWABUCHI	LA,K,NA,LU,BI,SR,CA,CU,O	
918	PRB0404453		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1989																											3	Y123				3.819		11.678														92					92																																																																																																					MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
919	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-Z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		1	1989																											3	Y123				3.824	3.888	11.677														83.3					83.3																																																									23.6																																												MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
920	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1989																											3	Y123				3.83	3.89	11.679														75.2					75.2																																																									57.5																																												MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
921	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z		1	1989																											3	Y123				3.834	3.895	11.686														59.1					59.1																																																									101																																												MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
922	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7-Z	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z		1	1989																											3	Y123				3.841	3.896	11.691														49.4					49.4																																																									150.6																																												MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
923	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-Z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z		1	1989								2.1																			3	Y123					3.901	11.691														28.9					28.9																																																																																																					MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
924	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O7-Z	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z		1	1989								3.5																			3	Y123					3.901	11.695																																																																																																																								MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
925	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.3Pr0.7Ba2Cu3O7-Z	Y	0.3	Pr	0.7	Ba	2	Cu	3													O	7-Z		1	1989								5.3																			3	Y123					3.91	11.703																																																																																																																								MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
926	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O7-Z	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7-Z		1	1989								11.4																			3	Y123					3.916	11.697																																																																																																																								MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
927	PRB0404453		(Y,Pr)Ba2Cu3O7	Y0.1Pr0.9Ba2Cu3O7-Z	Y	0.1	Pr	0.9	Ba	2	Cu	3													O	7-Z		1	1989								14																			3	Y123					3.919	11.697																																																																																																																								MAGNETIC ORDERING AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7-Y	198909	ANTIFERROMAGNETIC   ,SPECIFIC HEAT       ,SUSCEPTIBILITY      ,RESISTIVITY	CENTER FOR MATERIALS RESEARCH,TEMPLE UNIVERSITY,PHILADELPHIA,PENNSYLVANIA 19122	PHYS.REV.B,40(1989)4453	A.KEBEDE,C.S.JEE,G.H.MYER,J.E.CROW,J.SCHWEGLER,M.V.KURIC,P.SCHLOTTMANN,R.E.SALOMON,R.P.GUERTIN,S.H.BLOOM,T.MIHALISIN	Y,PR,BA,CU,O	
929	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.11	Er	1	Ba	2	Cu	3															O	Z	6.11		1989																											2	Y123	P4/MMM	123		3.846		11.792																																																																																																																								NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
930	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.34	Er	1	Ba	2	Cu	3															O	Z	6.34		1989																											3	Y123	PMMM	47		3.844	3.851	11.76																																																																																																																								NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
931	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.53	Er	1	Ba	2	Cu	3															O	Z	6.53		1989																											3	Y123				3.823	3.865	11.694														54.3					54.3																																																																																																					NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
932	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.64	Er	1	Ba	2	Cu	3															O	Z	6.64		1989																											3	Y123				3.82	3.869	11.676														61.3					61.3																																																																																																					NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
933	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.78	Er	1	Ba	2	Cu	3															O	Z	6.78		1989																											3	Y123				3.817	3.874	11.653														78.2					78.2																																																																																																					NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
934	PRB0404472		ErBa2Cu3Oz	Er1Ba2Cu3O6.87	Er	1	Ba	2	Cu	3															O	Z	6.87		1989																											3	Y123				3.812	3.877	11.65														94.5					94.5																																																																																																					NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
935	PRB0404472		ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	Z	7		1989																											3	Y123				3.803	3.873	11.62														92.5					92.5																																																																																																					NEUTRON-DIFFRACTION STUDY OF ERBA2CU3OX IN THE COMPOSITION RANGE 6.1<-X<-7.0	198909	REUTRON SCATTERING  ,OXYGEN CONTENT	INSTITUT FUR FESTKORPERFORSCHUNG,KERNFORSCHUNGSANLAGE JULICH G.M.B.H.,D-5170 JULICH,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)4472	B.RUPP,E.PORSCHKE,P.ALLENSPACH,P.FISCHER,P.MEUFFELS	ER,BA,CU,O	
936	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8+Z			1989																												Bi2212				5.417		30.805													69.6	81.5	90				81.5																																																																																		4.58				0.00000000208			0.000000003												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
937	JJP0280112		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1989																												Bi2212				5.396		30.774													63.6	70.7	81.9				70.7																																																																																		2.41				0.00000000166			0.0000000021												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
938	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+Z			1989																												Bi2212				5.412		30.693													70	84.5	91.2				84.5																																																																																		5.68				0.0000000023			0.0000000032												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
939	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+Z			1989																												Bi2212				5.414		30.549													66.5	80	92				80																																																																																		3.36				0.00000000309			0.0000000045												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
940	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8+Z	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+Z			1989																												Bi2212				5.42		30.469													53.1	71.5	88				71.5																																																																																		11.1				0.0000000052			0.0000000066												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
941	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8+Z	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8+Z			1989		-0.001																										Bi2212				5.426	5.434	30.401													4	12	57				12																																																																																		23				0.0000000087															METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
942	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.45Y0.55Cu2O8+Z	Bi	2	Sr	2	Ca	0.45	Y	0.55	Cu	2											O	8+Z			1989																												Bi2212																																																																																																															0.000000013			0.0000000178												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
943	ME0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.4Y0.6Cu2O8+Z	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	8+Z			1989																												Bi2212				5.425	5.441	30.369																																																																																																					70.7																			Metal-Insulator Transition in the Bi2Sr2Ca1-xYxCu2O8+y System	198901		Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn.J.Appi.Phys,28(1989)L112-L115	Fumiko SAKAI,Kei-ichi KOGA,Kunio SUZUKI,Masaki ICHIHARA,Tsuyoshi TAMEGAI,Yasuhiro IYE		
944	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.3Y0.7Cu2O8+Z	Bi	2	Sr	2	Ca	0.3	Y	0.7	Cu	2											O	8+Z			1989																												Bi2212				5.427	5.443	30.268																																																																																																					95.2				0.000000021			0.0000000226												METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
945	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8+Z	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8+Z			1989								2.05																				Bi2212				5.43	5.452	30.238																																																																																																					713				0.0000000574															METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
946	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.1Y0.9Cu2O8+Z	Bi	2	Sr	2	Ca	0.1	Y	0.9	Cu	2											O	8+Z			1989								2.03																				Bi2212				5.428	5.458	30.201																																																																																																									0.000000156															METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
947	JJP0280112		Bi2Sr2YCu2O8	Bi2Sr2Y1Cu3O8+Z	Bi	2	Sr	2	Y	1	Cu	3													O	8+Z			1989								2																				Bi2212				5.428	5.465	30.175																																																																																																																								METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
948	JJP0280112		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.55Y0.45Cu2O8+Z	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	2											O	8+Z			1989																												Bi2212																			17	42	64				42																																																																																																					METAL-INSULATOR TRANSITION IN THE BI2SR2CA1-XYXCU2O8+Y SYSTEM	198901	METAL-INSULATOR TRAN,PHASE DIAGRAM       ,RES                 ,HALL EFFECT	INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106	JJAP LETT.,28(1989)L112	FUMIKO SAKAI,KEI-ICHI KOGA,KUNIO SUZUKI,MASAKI ICHIHARA,TSUYOSHI TAMEGAI,YASUHIRO IYE	BI,SR,CA,Y,CU,O	
949	PRB0404517		YBa2Cu3Oz	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-Z	6.96	1	1989	emu/g	0.00000048	emu/g	0.000129			10																				3	Y123				3.831	3.875	11.646														88.5				2	88.5																															2.73							12			A	calculated from resistivity	726														56.3																					0.1133																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
950	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.9Pr0.1Ba2Cu3O6.91	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z	6.91	1	1989	emu/g	0.0000006	emu/g	0.00032			0.2																				3	Y123				3.839	3.879	11.668														81				9.8	81																															1.6							16			A	calculated from resistivity	540														65.6																					0.0573																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
951	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O6.91	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z	6.91		1989	emu/g	0.00000066	emu/g	0.000375			-5.2																				3	Y123				3.845	3.879	11.662														62.7				8.3	62.7																															1.16							21			A	calculated from resistivity	506														70.1																					0.0389																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
952	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.7Pr0.3Ba2Cu3O6.88	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z	6.88	1	1989	emu/g	0.00000069	emu/g	0.000592			-11.7																				3	Y123				3.847	3.883	11.672														47.5				9.2	47.5																															0.69							32			A	calculated from resistivity	439														73.2																					0.0222																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
953	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.65Pr0.35Ba2Cu3O7.01	Y	0.65	Pr	0.35	Ba	2	Cu	3													O	7-Z	7.01	1	1989	emu/g	0.00000064	emu/g	0.00063			-4.2																				3	Y123				3.857	3.882	11.652														44.5				10.8	44.5																															0.6							35			A	calculated from resistivity	435														69.4																					0.0204																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
954	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.9	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z	6.9	1	1989	emu/g	0.00000075	emu/g	0.000668			-8.4																				3	Y123				3.856	3.882	11.662														32				7	32																															0.41							50			A	calculated from resistivity	400														78																					0.0124																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
955	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.55Pr0.45Ba2Cu3O7.01	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	7-Z	7.01	1	1989	emu/g	0.00000072	emu/g	0.000829			-6																				3	Y123				3.859	3.882	11.655														29.2				9.6	29.2																															0.22							71			A	calculated from resistivity	312														75.7																					0.0069																							UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
956	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O7.01	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z	7.01	1	1989	emu/g	0.00000078	emu/g	0.00081			-8.5																				3	Y123				3.868	3.888	11.669																																																																												80.7																																												UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
957	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.4Pr0.6Ba2Cu3O7.03	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z	7.03	1	1989	emu/g	0.00000093	emu/g	0.00082			-4.4																				3	Y123				3.867	3.889	11.682																																																																												92.7																																												UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
958	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.3Pr0.7Ba2Cu3O7.03	Y	0.3	Pr	0.7	Ba	2	Cu	3													O	7-Z	7.03	1	1989	emu/g	0.00000106	emu/g	0.00104			-5.2																				3	Y123				3.874	3.892	11.686																																																																												102.9																																												UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
959	PRB0404517		(Y,Pr)Ba2Cu3Oz	Y0.1Pr0.9Ba2Cu3O7.03	Y	0.1	Pr	0.9	Ba	2	Cu	3													O	7-Z	7.03	1	1989	emu/g	0.0000012	emu/g	0.00119			-4.6																				2	Y123				3.892		11.675																																																																												115.9																																												UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
960	PRB0404517		PrBa2Cu3Oz	Pr1Ba2Cu3O6.96	Pr	1	Ba	2	Cu	3															O	7-Z	6.96	1	1989	emu/g	0.00000151	emu/g	0.00153			-7.3																				2	Y123				3.896		11.688																																																																												139.7																																												UPPER CRITICAL FIELD AND NORMAL-STATE PROPERTIES OF SINGLE-PHASE Y1-XPRXBA2CU3O7Z COMPOUNDS	198909	SINGLE-PHASE        ,ANNEALING CONDITIONS,MAGNETIZATION       ,CRITICAL FIELDS	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,CALIFORNIA,CALIFORNIA 95616	PHYS.REV.B,40(1989)4517	H.B.RADOUSKY,J.L.PENG,L.BERNARDEZ,P.A.HAHN,P.KLAVINS,R.N.SHELTON	Y,PR,BA,CU,O	
961	PRL0582333	75%O(18),DTC=0.3K(RES),  O<18> exchange analyzed by mass spectroscopy.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																		K		92.1					92.1						0	O	75	0.1																																																																																							exchange cycle : heat(500-550C,12h, in vac) - heat(500C,12h in 1 atm-O<18>).  after three exchange cycle, 75% exchange.					ISOTOPE EFFECT IN THE HIGH-TC SUPERCONDUCTORS BA(2)Y(1)CU(3)O(7) AND BA(2)EU(1)CU(3)O(7)		ISOTOPE EFFECT           ,RAMAN                    ,MAGNETIZ	ATT & ELL LAB.,MURRY HILL,NEW JERSEY,USA	PHYS.REV.LETT.,58(1987)2333	A.JAYARAMAN,A.M.MUJSCE,A.WHITE,B.BATLOGG,D.W.MURPHY,E.A.RIETMAN,G.A.KOUROUKLIS,H.S.CHEN,K.T.SHORT,L.W.RUPP,R.B.VAN DOVER,R.J.CAVA,S.SUNSHINE		
962	PRL0582333	75%O(18),DTC=0.4K(RES). O<18> exchange analyzed by mass spectroscopy.	EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																		K		92.15					92.15						0	O	75	0.1																																																																																							exchange cycle : heat(500-550C,12h, in vac) - heat(500C,12h in 1 atm-O<18>).  after three exchange cycle, 75% exchange.					ISOTOPE EFFECT IN THE HIGH-TC SUPERCONDUCTORS BA(2)Y(1)CU(3)O(7) AND BA(2)EU(1)CU(3)O(7)		ISOTOPE EFFECT           ,RAMAN                    ,MAGNETIZ	ATT & ELL LAB.,MURRY HILL,NEW JERSEY,USA	PHYS.REV.LETT.,58(1987)2333	A.JAYARAMAN,A.M.MUJSCE,A.WHITE,B.BATLOGG,D.W.MURPHY,E.A.RIETMAN,G.A.KOUROUKLIS,H.S.CHEN,K.T.SHORT,L.W.RUPP,R.B.VAN DOVER,R.J.CAVA,S.SUNSHINE		
963	PRL0582337	90%O(18),ALPHA=0.0+-0.027(RES)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																		K		90					90						0	O	90																																																																																								O-exchange condition (950C,12h, in O<18> atmosphere) - slow cool to RT(over 6h)					SEARCH FOR ISOTOPE EFFECT IN SUPERCONDUCTING Y-BA-CU-O	198706	ISOTOPE EFFECT           ,RESISTIVITY              ,SUSCEPTI	UNIV. OF CALIFORNIA,BERKELEY,CALIFORNIA,USA	PHYS.REV.LETT.,58(1987)2337	A.ZETTL,ANGELICA M.STACY,DONALD E.MORRIS,HANS-CONRAD ZUR LOYE,K.J.CHANG,K.L.LEARY,L.C.BOURNE,M.F.CROMMIE,MARVIN L.COHEN,S.W.KELLER		
964	PRL0591236	90%O(18) substitution, DTC=0.5K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																				92.1					92.1						0.046	O	90	0.5																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN Y(1)BA(2)CU(3)O(7)	198709	ISOTOPE EFFECT           ,SUSCEPTIBILITY           ,OXYGEN C	COLLEGE OF CHEMISTRY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.LETT.,59(1987)1236	ANGELICA M.STACY,HANS CONRAD ZUR LOYE,JAMES N.MICHAELS,KEVIN J.LEARY,STEVEN W.KELLER,TANYA A.FALTENS,WILLIAM K.HAM	Y,BA,CU,O	
965	SSC0650869	alpha=zero, CU(65),DTC=0.0+-0.2	YBa2Cu3Oz	Y1Ba2Cu3O7.1	Y	1	Ba	2	Cu	3															O	7	7.1	1	1988																											3	Y123																				91.3					91.3						0	Cu																																																																																														THE COPPER ISOTOPE EFFECT IN BA(2)Y(1)CU(3)O(7)	198802	ISOTOPE EFFECT           ,SUSCEPTIBILITY           ,TC	INSTITUTE OF PHYSICS,ACADEMY OF SCIENCES,BEIJING,CHINA	SOLID STATE COMMUN.,65(1988)869	CHEN GENG-HUA,HAN SHUN-HUI,LI JING-YUAN,LIN QUAN(C.LIN),LIU CHAO-XIN,NI YONG-MING,NING TAI-SHANG,SHAO YOU-YU,SHEN ZHI-GONG,WEI YU-NIAN,YAN QI-WEI,YANG QIAN-SHENG,ZHANG PAN-LIN,ZHAO JIN-KUE	Y,BA,CU,O	
966	JJP0270553	85%BA(134),DTC=0.1(INDUCTANCE)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123																				89.9					89.9																																																																																																					BA ISOTOPE EFFECT IN A BA(2)Y(1)CU(3)O(7-Z) SUPERCONDUCTOR	198804	ISOTOPE EFFECT           ,MEISSNER EFFEC	ELECTROTECHNICAL LABORATORY,IBARAKI	JJAP.LETT.,27(1988)L553	TAKEHIKO HIDAKA,TOSHIMI MATSUI,YOSHIHIKO NAKAGAWA	Y,BA,CU,O	
967	PRB0375936	DTC=0.18+-0.04K WITH 85%O(18),ALPHA=0.019+-0.005	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988									4.8																		3	Y123																				91.6					91.6						0.019																																																																																															SMALL OXYGEN ISOTOPE SHIFT IN Y(1)BA(2)CU(3)O(7)	198804	OXYGEN ISOTOPE EFFECT    ,TC	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)5936	ANDREA G.MARKELZ,DONALD E.MORRIS,JANICE H.NICKEL,JOHN Y.T.WEI,RANDY M.KURODA	Y,BA,CU,O	
968	SSC0670707	80%O(18),DTC=0.41+-0.2K,ALPHA=0.14+-0.08(SUS)	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1988																												T																				35					35						0.14																																																																																															MAGNETIC AND RESISTIVE DETERMINATION OF THE OXYGEN ISOTOPE EFFECT IN La1.85Sr0.15CuO4			Department of Physics, University of California at Berkeley, and Materials and Chemical Sciences Division, Lawrence Berkeley Laboratories, Berkeley, California 94720	Solid State Commun.,67(1988)707-711	A. Zettl,Donald E. Morris,John Kinney,L.C. Bourne,Luis Bernardez,M.F. Crommie,Marvin L. Cohen,S. Hoen,W.N. Creager		
969	PRB0392269	DTC=0.17K,ALPHA=0.019+-0.004(SUS),ALPHA=0.028+-0.003(RES)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																				92					92						0.019																																																																																															OXYGEN ISOTOPE STUDY OF Y(1)BA(2)CU(3)O(7)	198902	OXYGEN                   ,ISOTOPE EFFECT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA AT BERKELEY,AND MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,CALIFORNIA	PHYS.REV.B,39(1989)2269	A.ZETTL,JOHN KINNEY,L.C.BOURNE,LUIS BERNARDEZ,M.F.CROMMIE,MARVIN L.COHEN,S.HOEN,T.W.BARBEE III,W.N.CREAGER	Y,BA,CU,O	
970	JJP0281769			Bi2La0.5Ca1.5Cu2OZ	Bi	2	La	0.5	Ca	1.5	Cu	2													O	Z		1	1989																											2	Bi2212				5.409		39.6														39.6					39.6																																																																																		6.3																			SUPERCONDUCTIVITY IN THE BI2LNXCA3-XCU2OZ	198910	NEW FAMILY          ,RESISTIVITY         ,SINGLE PHASE        ,XRY	DEPARTMENT OF MATERIALS SCIENCE, UNIVERSITY OF OSAKA PREFECTURE, SAKAI, OSAKA 591	JJAP LETT 28(1989)L1769	AKIRA YANASE,HIROYUKI SASAKURA,KIYOTAKA NAKAHIGASHI,MINEO KOGACHI,NOBUO FUKUOKA,SHIGEMITSU NAKANISHI,SHINNOSUKE MINAMIGAWA	BI,R,CU,CA,O	
971	JJP0281769			Bi2La0.3Ca2.7Cu2OZ	Bi	2	La	0.3	Ca	2.7	Cu	2													O	Z		1	1989																											2	Bi2212																				20.2					20.2																																																																																		30.7																			SUPERCONDUCTIVITY IN THE BI2LNXCA3-XCU2OZ	198910	NEW FAMILY          ,RESISTIVITY         ,SINGLE PHASE        ,XRY	DEPARTMENT OF MATERIALS SCIENCE, UNIVERSITY OF OSAKA PREFECTURE, SAKAI, OSAKA 591	JJAP LETT 28(1989)L1769	AKIRA YANASE,HIROYUKI SASAKURA,KIYOTAKA NAKAHIGASHI,MINEO KOGACHI,NOBUO FUKUOKA,SHIGEMITSU NAKANISHI,SHINNOSUKE MINAMIGAWA	BI,R,CU,CA,O	
972	JJP0281769			Bi2Pr0.5Ca1.5Cu2OZ	Bi	2	Pr	0.5	Ca	1.5	Cu	2													O	Z		1	1989																											2	2212				5.41		29.98													46.8						46.8																																																																																		5.1																			SUPERCONDUCTIVITY IN THE BI2LNXCA3-XCU2OZ	198910	NEW FAMILY          ,RESISTIVITY         ,SINGLE PHASE        ,XRY	DEPARTMENT OF MATERIALS SCIENCE, UNIVERSITY OF OSAKA PREFECTURE, SAKAI, OSAKA 591	JJAP LETT 28(1989)L1769	AKIRA YANASE,HIROYUKI SASAKURA,KIYOTAKA NAKAHIGASHI,MINEO KOGACHI,NOBUO FUKUOKA,SHIGEMITSU NAKANISHI,SHINNOSUKE MINAMIGAWA	BI,R,CU,CA,O	
973	PRB0406862		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1989																											1	BKBO																				29					29																																																3.5																																																					SUPERCONDUCTING ENERGY GAP AND A NORMAL-STATE EXCITATION IN BA0.6K0.4BIO3	198910	ENERGY GAP          ,INFRARED            ,REFLECTIVITY	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK10598	PHYS.REV.B,40(1989)6862	A.W.MITCHELL,B.DABROWSKI,D.G.HINKS,D.J.SCALAPINO,J.A.CALISE,N.E.BICKERS,R.T.COLLINS,Y.ZHENG,Z.SCHLESINGER	BA,K,BI,O	
974	PRB0406810			Bi10Sr15Fe10O46	Bi	10	Sr	15	Fe	10															O	46		1	1989																											3		B222			27.245	5.462	31.696																																																																																																																								ORGIN OF THE INCOMMENSURATE MODULATION OF THE 80-K SUPERCONDUCTOR BI2SR2CACU2O8.21 DERIVED FROM ISOSTRUCTURAL COMMENSURATE BI10SR15FE10O46	198910	INCOMMENSURATE      ,MODULATION          ,STRUCTURE           ,OXYGEN DISTRIBUTI	DIVISION OF CHEMISTRY, NATIONAL RESEARCH COUNCIL OF CANADA, OTTAWA, CANADA K1A OR9	PHYS.REV.B,40(1989)6810	J. -M. TARASCON,P. BARBOUX,W. R. MCKINNON,Y. LE PAGE	FE,BI,SR,CA,CU,O	
975	PRB0406771		LaBa2Cu3Oz	La1Ba2Cu2.9O6.82	La	1	Ba	2	Cu	2.9															O	6.82	6.82	1	1989																											3	Y123	PMMM			3.894	3.937	11.816													20	45	52				45										30																																																																																											STRUCTURAL PROPERTIES OF THE SUPERCONDUCTOR LABA2CU3-YO7-Z INTHE SOLID SOLUTION SYSTEM LA1+XBA2-XCU3-YO7-Z	198910	TIME-OF-FLIGHT      ,NEUTRON             ,CRYSTAL STRUCTURES  ,CRYSTAL PARAMENTRS  ,SOLID-SOLUTION	DEPARTMENT OF PHYSICS, TOKYO UNIVERSITY OF MERCANTILE MARINE,2-1-6, ETCHU-JIMA, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,40(1989)6771	ATSUTAKA MAEDA,HAJIME ASANO,KUNIMITSU UCHINOKURA,MITSURU IZUMI,SHOJI TANAKA,TAKAHIRO WADA,TOMIAKI YABE	KA,BA,CU,O	
976	PRB0406771			La1.56Ba1.44Cu2.86O6.98	La	1.56	Ba	1.44	Cu	2.86															O	6.98	6.98		1989																													PMMM			3.918	3.928	11.742																																																																																																																								STRUCTURAL PROPERTIES OF THE SUPERCONDUCTOR LABA2CU3-YO7-Z INTHE SOLID SOLUTION SYSTEM LA1+XBA2-XCU3-YO7-Z	198910	TIME-OF-FLIGHT      ,NEUTRON             ,CRYSTAL STRUCTURES  ,CRYSTAL PARAMENTRS  ,SOLID-SOLUTION	DEPARTMENT OF PHYSICS, TOKYO UNIVERSITY OF MERCANTILE MARINE,2-1-6, ETCHU-JIMA, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,40(1989)6771	ATSUTAKA MAEDA,HAJIME ASANO,KUNIMITSU UCHINOKURA,MITSURU IZUMI,SHOJI TANAKA,TAKAHIRO WADA,TOMIAKI YABE	KA,BA,CU,O	
977	PRB0406717	NO. OF CU-O SHEETS=INFINITY, IR AND RAMAN		Ca1Cu1O2	Ca	1	Cu	1																	O	2			1989																													P4/MMM																																																																																																																													PHONONS IN CACUO2	198910	INFRARED REFLECTIVIT,PHONONS             ,GROUP THEORY        ,RAMAN	IBM THOMAS J. WATSON RESEARCH CENTER, YORKTOWN HEIGHTS, NEW YORK 10598-0218	PHYS.REV.B,40(1989)6717	E. M. MCCARRON III,F. H. DACOL,G. BURNS,M. K. CRAWFORD,T. M. SHAW	SR,CA,CU,O	
978	PH0406717			Ca0.86Sr0.14Cu1O2	Ca	0.86	Sr	0.14	Cu	1															O	2		1	1989																												IL																																																																																																																														PHONONS IN CACUO2	198910	INFRARED REFLECTIVIT,PHONONS             ,GROUP THEORY        ,RAMAN	IBM THOMAS J. WATSON RESEARCH CENTER, YORKTOWN HEIGHTS, NEW YORK 10598-0218	PHYS.REV.B,40(1989)6717	E. M. MCCARRON III,F. H. DACOL,G. BURNS,M. K. CRAWFORD,T. M. SHAW	SR,CA,CU,O	
979	PRB0406771		LaBa2Cu3Oz	La1Ba2Cu3O6.85	La	1	Ba	2	Cu	3															O	6.85	6.85	1	1989																											3	Y123	PMMM			3.893	3.938	11.818														93					93										30																																																																																											STRUCTURAL PROPERTIES OF THE SUPERCONDUCTOR LABA2CU3-YO7-Z INTHE SOLID SOLUTION SYSTEM LA1+XBA2-XCU3-YO7-Z	198910	TIME-OF-FLIGHT      ,NEUTRON             ,CRYSTAL STRUCTURES  ,CRYSTAL PARAMENTRS  ,SOLID-SOLUTION	DEPARTMENT OF PHYSICS, TOKYO UNIVERSITY OF MERCANTILE MARINE,2-1-6, ETCHU-JIMA, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,40(1989)6771	ATSUTAKA MAEDA,HAJIME ASANO,KUNIMITSU UCHINOKURA,MITSURU IZUMI,SHOJI TANAKA,TAKAHIRO WADA,TOMIAKI YABE	KA,BA,CU,O	
980	SSC0710939	THERMAL CONDUCTIVITY, UNIT=W/M.K	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.90	6.9		1989																											3	Y123																				92					92																																																																																																					CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
981	SSC0710939		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.9Zn0.1O6.94	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	6.94	6.94		1989																												Y123																				57					57																																																																																																					CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
982	SSC0710939		YBa2(Cu,Al)3Oz	Y1Ba2Cu2.9Al0.1O7.1	Y	1	Ba	2	Cu	2.9	Al	0.1													O	7.10	7.1		1989																												Y123																				85					85																																																																																																					CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
983	SSC0710939		YBa2(Cu,Sn)3Oz	Y1Ba2Cu2.9Sn0.1O7.28	Y	1	Ba	2	Cu	2.9	Sn	0.1													O	7.28	7.28		1989																												Y123																				90					90																																																																																																					CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
984	PLA1390265	ANOMALY IN THERMAL CONDUCTIVITY AT 155 AND 225K	Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3OZ	Tl	2	Ba	2	Ca	2	Cu	3													O	Z			1989																											2	Tl2223																				119	128			11	119																															1.6																															2.4																				8.1																			ANOMALOUS BEHAVIOUR OF THERMAL CONDUCTIVITY OF TL-BA-CA-CU-O	198908	THERMAL CONDUCTIVITY     ,PHASE TRANSITION         ,OXYGEN V	INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCES,2 OKOLNA ST.,50-422 WROCLAW,POLAND	PHYS.LETT.A,139(1989)265	A.J.ZALESKI,A.JEZOWSKI,E.P.KHLYBOV,H.MISIOREK,V.V.EVDOKIMOVA	TL,BA,CA,CU,O	
985	PRL0582482		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1987																											2	T																			3		40				21.5																																																																			300																																		EVIDENCE FOR SUPERCONDUCTIVITY IN LA(2)CU(1)O(4)		RESISTIVITY              ,THERMOPOWER	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA,USA	PHYS.REV.LETT.,58(1987)2482	E.M.ENGLER,G.LIM,J.E.VAZQUEZ,M.L.RAMIREZ,P.M.GRANT,R.D.JACOWITZ,R.L.GREENE,S.S.P.PARKIN,V.Y.LEE		
986	SSC0700303	THPOW300 = AT 240K	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1989																											2	T						13.222																																																																																						25.4			TP986																								LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
987	SSC0700303	THPOW300 = AT 240K	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1989																											2	T						13.232																																																																																						15.8			TP987																								LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
988	SSC0700303	THPOW300 = AT 240K	(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1989																											2	T						13.245																																																																																						12.6			TP988																								LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
989	SSC0690851	STRUCTURAL TRANSFORMATION AT TM=52K	(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4		1	1989																												T																																																																																												35.7			TP989																0.000000004			0.00000000663		RH989			LA2O3,BACO3,CUO	1	CAL(900C 12H)-SIN(1100C 12H)-ANN(600C 12H)					TRANSPORT AND MAGNETIC ANOMALIES AT THE STRUCTURAL TRANSITION T-O THE NEW LOW TEMPERATURE PHASE IN LA(2-X)BA(X)CUO(4)	198902	RES                      ,HALL EFFECT              ,THERMOPOWER              ,ST	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI 444,JAPAN	SOLID STATE COMMUN.,69(1989)851	I.WATANAGE,K-.KUMAGAI,K.FUKUDA,M.SATO,M.SERA,S.KONDOH,S.NAKASHIMA,Y.ANDO	LA,BA,CU,O	
990	SSC0690851	STRUCTURAL TRANSFORMATION AT TM=61K	(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1989																												T																					35				35																																																																			27.7			TP990					2							3.5				0.00000000283			0.00000000423		RH990			LA2O3,BACO3,CUO	1	CAL(900C 12H)-SIN(1100C 12H)-ANN(600C 12H)					TRANSPORT AND MAGNETIC ANOMALIES AT THE STRUCTURAL TRANSITION T-O THE NEW LOW TEMPERATURE PHASE IN LA(2-X)BA(X)CUO(4)	198902	RES                      ,HALL EFFECT              ,THERMOPOWER              ,ST	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI 444,JAPAN	SOLID STATE COMMUN.,69(1989)851	I.WATANAGE,K-.KUMAGAI,K.FUKUDA,M.SATO,M.SERA,S.KONDOH,S.NAKASHIMA,Y.ANDO	LA,BA,CU,O	
991	SSC0690851	STRUCTURAL TRANSFORMATION AT TM=61K	(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4		1	1989																												T																																																																																												24.3			TP991																0.00000000224			0.00000000358		RH991			LA2O3,BACO3,CUO	1	CAL(900C 12H)-SIN(1100C 12H)-ANN(600C 12H)					TRANSPORT AND MAGNETIC ANOMALIES AT THE STRUCTURAL TRANSITION T-O THE NEW LOW TEMPERATURE PHASE IN LA(2-X)BA(X)CUO(4)	198902	RES                      ,HALL EFFECT              ,THERMOPOWER              ,ST	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI 444,JAPAN	SOLID STATE COMMUN.,69(1989)851	I.WATANAGE,K-.KUMAGAI,K.FUKUDA,M.SATO,M.SERA,S.KONDOH,S.NAKASHIMA,Y.ANDO	LA,BA,CU,O	
992	SSC0700303	THPOW300=AT 240K,RHN=AT 50K	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		1	1989																											2	T						13.268																																																																																						2.7			TP992																0.00000000016			0.000000000246		RH992			LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
993	SSC0700303	THPOW300=AT 240K,RHN=AT 50K	(La,Sr)2CuO4	La1.65Sr0.35Cu1O4	La	1.65	Sr	0.35	Cu	1															O	4		1	1989																											2	T						13.277																																																																																																									0.000000000051			0.000000000105		RH993			LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
994	SSC0700303	THPOW300=AT 240K,RHN=AT 50K	(La,Sr)2CuO4	La1.6Sr0.4Cu1O4	La	1.6	Sr	0.4	Cu	1															O	4		1	1989																											2	T						13.277																																																																																						1.1																						0.000000000047		RH994			LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
995	SSC0700303	THPOW300=AT 240K,RHN=AT 50K	(LA,SR)2CUO4	La1.5Sr0.5Cu1O4	La	1.5	Sr	0.5	Cu	1															O	4		1	1989																											2	T						13.279																																																																																						1.3																			-0.000000000256			-0.000000000302		RH995			LA2O3,SRCO3,CUO	1	CAL(1000C 30H)-SIN(1100C 60H)-FC-ANN(1080C 6H IN 200ATM O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
996	PRB0397324		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4		1	1989																												T																				37					37																																																																																									0.00000000121		RH996										HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
997	PRB0397324		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.987Ni0.013O4	La	1.84	Sr	0.16	Cu	0.987	Ni	0.013													O	4		1	1989																												T																				25					25																																																																																									0.00000000136		RH997										HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
998	PRB0397324		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.975Ni0.025O4	La	1.84	Sr	0.16	Cu	0.975	Ni	0.025													O	4		1	1989																												T																				15					15																																																																																									0.00000000141		RH998										HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
999	PRB0397324		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.95Ni0.05O4	La	1.84	Sr	0.16	Cu	0.95	Ni	0.05													O	4		1	1989																												T																																																																																																																		0.00000000141		RH999										HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1000	PRB0389194		BI4SR3CA3CU4O16	Bi4Ca3Sr3Cu4O16	Bi	4	Ca	3	Sr	3	Cu	4													O	16			1988																												Bi4334																			76		93				84.5													240																									44			A		1585																																							4.78												BI2O3,CACO3,SRCO3,CUO	0	CAL(850C 1-2H IN AIR)-SIN(865C12H IN O2)-C TO RT WITHIN 12H					MAGNETIZATION AND RESISTIVITY OF BI(4)CA(3)SR(3)CU(4)O(16)-TYPE MATERIALS HAVING TWO SUPERCONDUCTIVITY ONSET TEMPERATURES	198811	MAG                      ,RES                      ,Tc                       ,Hc	CPRNING GLASS WORKS,SULLIVAN PRAK,CORNING,NEW YORK	PHYS.REV.B,38(1988)9194	M.GRAYSON ALEXANDER	BI,CA,SR,CU,O	
1001	PRB0389194		Bi4Sr3Ca3Cu4O16	Bi4Ca3Sr3Cu4O16	Bi	4	Ca	3	Sr	3	Cu	4													O	16			1988																												Bi4334																			76		111				93.5													90																									2.7					3650																																							1.09												BI2O3,CACO3,SRCO3,CUO	0	CAL(850C 1-2H IN AIR)-SIN(865C12H IN O2)-C TO RT WITHIN 12H					MAGNETIZATION AND RESISTIVITY OF BI(4)CA(3)SR(3)CU(4)O(16)-TYPE MATERIALS HAVING TWO SUPERCONDUCTIVITY ONSET TEMPERATURES	198811	MAG                      ,RES                      ,Tc                       ,Hc	CPRNING GLASS WORKS,SULLIVAN PRAK,CORNING,NEW YORK	PHYS.REV.B,38(1988)9194	M.GRAYSON ALEXANDER	BI,CA,SR,CU,O	
1002	PRB0389194		Bi4Sr3Ca3Cu4O16	Bi4Ca3Sr3Cu4O16	Bi	4	Ca	3	Sr	3	Cu	4													O	16			1988																												Bi4334																			58		115				86.5													110																									7					3040																																							5.59												BI2O3,CACO3,SRCO3,CUO	0	CAL(850C 1-2H IN AIR)-SIN(865C12H IN O2)-C TO RT WITHIN 12H					MAGNETIZATION AND RESISTIVITY OF BI(4)CA(3)SR(3)CU(4)O(16)-TYPE MATERIALS HAVING TWO SUPERCONDUCTIVITY ONSET TEMPERATURES	198811	MAG                      ,RES                      ,Tc                       ,Hc	CPRNING GLASS WORKS,SULLIVAN PRAK,CORNING,NEW YORK	PHYS.REV.B,38(1988)9194	M.GRAYSON ALEXANDER	BI,CA,SR,CU,O	
1003	PR0388885		Bi2Sr2CuO6	Bi2Sr2Cu1O6+Y	Bi	2	Sr	2	Cu	1															O	6+Y			1988																											2	Bi2201				5.39		24.6														10					10										10																																																																																				BI2O3,SRCO3,SRO2,CUO	0	VARIOUS HEAT TREATMENT					PREPARATION,STRUCTURE,AND PROPERTIES OF THE SUPERCONDUCTING COMPOUND SERIES BI(2)SR(2)CA(N-1)CU(N)O(Y) WITH N=1,2,AND 3	11	STRUCTURES               ,PREPARATION              ,TEM                      ,SUS	BELLCORE,331 NEWMAN SPRINGS ROAD,RED BANK,NEW JERSEY	PHYS.REV.B,38(1988)8885	B.G.BAGLEY,D.M.HWANG,G.W.HULL,J.M.TARASCON,L.H.GREEN,P.BARBOUX,W.R.MCKINNON,Y.LEPAGE	BI,SR,CA,CU,O	
1004	PR0388885		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Y			1988																											2	Bi2212				5.39		30.7														85					85										50																																																																																				BI2O3,SRCO3,SRO2,CUO	0	VARIOUS HEAT TREATMENT					PREPARATION,STRUCTURE,AND PROPERTIES OF THE SUPERCONDUCTING COMPOUND SERIES BI(2)SR(2)CA(N-1)CU(N)O(Y) WITH N=1,2,AND 3	11	STRUCTURES               ,PREPARATION              ,TEM                      ,SUS	BELLCORE,331 NEWMAN SPRINGS ROAD,RED BANK,NEW JERSEY	PHYS.REV.B,38(1988)8885	B.G.BAGLEY,D.M.HWANG,G.W.HULL,J.M.TARASCON,L.H.GREEN,P.BARBOUX,W.R.MCKINNON,Y.LEPAGE	BI,SR,CA,CU,O	
1005	PR0388885		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10+Y	Bi	2	Sr	2	Ca	2	Cu	3													O	10+Y			1988																											2	Bi2223				5.39		37.1														110					110										50																																																																																				BI2O3,SRCO3,SRO2,CUO	0	VARIOUS HEAT TREATMENT					PREPARATION,STRUCTURE,AND PROPERTIES OF THE SUPERCONDUCTING COMPOUND SERIES BI(2)SR(2)CA(N-1)CU(N)O(Y) WITH N=1,2,AND 3	11	STRUCTURES               ,PREPARATION              ,TEM                      ,SUS	BELLCORE,331 NEWMAN SPRINGS ROAD,RED BANK,NEW JERSEY	PHYS.REV.B,38(1988)8885	B.G.BAGLEY,D.M.HWANG,G.W.HULL,J.M.TARASCON,L.H.GREEN,P.BARBOUX,W.R.MCKINNON,Y.LEPAGE	BI,SR,CA,CU,O	
1006	PRB0389205			Bi1Sr1Ca1Cu2OX	Bi	1	Sr	1	Ca	1	Cu	2													O	X			1988																																5.384	26.951	30.608														110					110																															1.98																																				19																											BI2O3,SRCO3,CACO3,CUO	0	CAL(850C,16H IN O2)-SIN(882C 20MIN)-ANN(872C 12H IN O2)-C					MAGNETORESISTANCE AND THERMOELECTRIC POWER OF THE BI-SR-CA-CU-O SYSTEM	198811	MAGNETORESISTANCE        ,RES                      ,Hc                       ,TH	SAHA INSTITUTE OF NUCLEAR PHYSICS,CALCUTTA,INDIA	PHYS.REV.B,38(1988)9205	A.CHAKRABORTY,A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL,S.K.LAHIRI	BI,SR,CA,CU,O	
1007	PRB0389205		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X			1988																												Bi2212																				80					80																																																																																														BI2O3,SRCO3,CACO3,CUO	0	CAL(850C,16H IN O2)-SIN(882C 20MIN)-ANN(872C 12H IN O2)-C					MAGNETORESISTANCE AND THERMOELECTRIC POWER OF THE BI-SR-CA-CU-O SYSTEM	198811	MAGNETORESISTANCE        ,RES                      ,Hc                       ,TH	SAHA INSTITUTE OF NUCLEAR PHYSICS,CALCUTTA,INDIA	PHYS.REV.B,38(1988)9205	A.CHAKRABORTY,A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL,S.K.LAHIRI	BI,SR,CA,CU,O	
1008	PRB0389209		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2O6.45	Y	1	Ba	2	Cu	2.8	Co	0.2													O	6.45	6.45		1988								415																				Y123																																																																																																																								0						ANTIFERROMAGNETIC ORDER IN Y(1)BA(2)CU(3-X)CO(X)O(6+Y)	198811	NEUTRON SCATTERING       ,ANTIFERROMAGNE	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,38(1988)9209	D.A.NEUMANN,J.J.RHYNE,J.M.TARASCON,J.V.WASZCZAK,L.F.SCHNEEMEYER,L.H.GREENE,M.GIROUD,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
1009	PRB0389209		YBa2(Cu,Co)3O7	Y1Ba2Cu2.2Co0.8O6.91	Y	1	Ba	2	Cu	2.2	Co	0.8													O	6.91	6.91		1988								435																			3	Y123																																																																																																																								0						ANTIFERROMAGNETIC ORDER IN Y(1)BA(2)CU(3-X)CO(X)O(6+Y)	198811	NEUTRON SCATTERING       ,ANTIFERROMAGNE	BELL COMMUNICATIONS RESEARCH,RED BANK,NEW JERSEY	PHYS.REV.B,38(1988)9209	D.A.NEUMANN,J.J.RHYNE,J.M.TARASCON,J.V.WASZCZAK,L.F.SCHNEEMEYER,L.H.GREENE,M.GIROUD,P.BARBOUX,P.F.MICELI	Y,BA,CU,CO,O	
1010	PRB0389220		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z		1	1988																												Y123																				90					90													250																																			3.3																																														BACO3,EUO,CUO	0	CAL(950C IN O2)-PELLET-(750C OVERNIGHT)-(425C 8H+OVER NIGHT IN O2)					THERMAL CONDUCTIVITY AND SUPERCONDUCTIVITY IN EU(1)BA(2)CU(3)O(7-X)	198811	THERMAL                  ,CONDUCTIVITY             ,ENRRGY G	CENTRO ATOMICO BARILOCHE,RIO NEGRO,REPUBLIC OF ARGENTINA	PHYS.REV.B,38(1988)9220	C.FAINSTEIN,M.A.IZBIZKY,M.NUNEZ REGUEIRO,P.ESQUINAZI	EU,BA,CU,O	
1011	PRB0389272			Bi2Sr2Ca2Cu6OZ	Bi	2	Sr	2	Ca	2	Cu	6													O	Z		3	1988																											2																																																																																																																									0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1012	PRB0389272		Bi2Sr2CaCu2O8	Bi2.15Sr1.68Ca1.17Cu2OZ	Bi	2.15	Sr	1.68	Ca	1.17	Cu	2													O	Z		3	1988																											2	Bi2212																				68					68																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1013	PRB0389272		Bi2Sr2(Ca,Bi)2Cu3O10	Bi2.4Sr2Ca1.6Cu3OZ	Bi	2.4	Sr	2	Ca	1.6	Cu	3													O	Z		3	1988																											2	Bi2223																				70					70																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1014	PHC1620427	CDW INSTABILITY AT ABOUT 30K		Li0.9Mo6O17	Li	0.9	Mo	6																	O	17		3	1989																												bronze																				1.7					1.7			K/GPa	2																																																																																											0						PRESSURE EFFECT ON THE TRANSPORT PROPERTIES OF SUPERCONDUCTING Li0.9Mo6O17 BRONZE			Laboratoire d'Etudes des Proprietes Electroniques des Solides+ *Laboratoire Louis Nee+-C.N.R.S. B.P. 166-38042 Grenoble Cedex-France	Physica.C,162-164(1989)427-428	C. ESCRIBE FILPPINI,C. SCHLENKER,J. BEILLE,J. MARCUS,M. BOUJIDA		
1015	PRB0389272		Bi2Sr2(Ca,Bi)2Cu3O10	Bi2.2Sr2Ca1.8Cu3OZ	Bi	2.2	Sr	2	Ca	1.8	Cu	3													O	Z		3	1988																											2	Bi2223																				30					30																																																																																																					INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1016	PRB0389272		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OZ	Bi	2	Sr	2	Ca	2	Cu	3													O	Z		3	1988																											2	Bi2223																				76					76																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1017	PRB0389272		Bi2Sr2Ca2Cu3O10	Bi1.95Sr2Ca2Cu3OZ	Bi	1.95	Sr	2	Ca	2	Cu	3													O	Z		3	1988																											2	Bi2223																				58					58																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1018	PRB0389272		Bi2Sr2Ca2Cu3O10	Bi1.8Sr2Ca2Cu3OZ	Bi	1.8	Sr	2	Ca	2	Cu	3													O	Z		3	1988																											2	Bi2223																				95					95																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1019	PRB0389272		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.7Sr2Ca2Cu3Pb0.3OZ	Bi	1.7	Sr	2	Ca	2	Cu	3	Pb	0.3											O	Z		3	1988																											2	Bi2223																				106					106																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1020	PRB0389272		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.9Sr2Ca2Cu3Pb0.3OZ	Bi	1.9	Sr	2	Ca	2	Cu	3	Pb	0.3											O	Z		3	1988																											2	Bi2223																				104					104																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1021	PRB0389272		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Sr2Ca2Cu3Pb0.6OZ	Bi	1.8	Sr	2	Ca	2	Cu	3	Pb	0.6											O	Z		3	1988																											2	Bi2223																				104					104																																																																																															0						INFLUENCE OF LEAD ON THE FORMATION OF THE 110-K SUPERCONDUCTING PHASE IN THE BI-SR-CA-CU-O COMPOUNDS	198811	FABRICATION              ,XRY                      ,RES                      ,ST	INSTITUTO DE INVESTIGACIONES EN MATERIALER,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO,DISTRITO FEDERAL,MEXICO	PHYS.REV.B,38(1988)9272	D.RIOS-JARA,E.CHAVIRA,L.M.LEON,R.ESCUDERO	BI,SR,CA,CU,O,PB	
1022	PRB0365680		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																				92					92																																																																														0.6				1.2							2.3						0						THERMAL TRANSPORT PROPERTIES OF Y(1)BA(2)CU(3)O(7) SUPERCONDUCTORS	198710	THERMAL CONDUCTIVITY     ,THERMOPOWER              ,HALL EFFECT              ,RE	MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,FEDERAL REPUBLIC OF GERMANY AND PHYSICS DEPARTMENT,THE UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN	PHYS.REV.B,36(1987)5680	A.B.KAISER,C.UHER	Y,BA,CU,O	
1023	PRB0365676		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1987																												T																																																																																												7			TP1023					0.4			0.28				1.2				1.7									0						ELECTRONIC TRANSPORT IN HIGHLY DOPED LA(2-X)SR(X)CU(1)O(4) SUPERCONDUCTORS	198710	THERMOPOWER              ,HALL EFFECT              ,RES	MAX-PLANCK-INSTITUT FUR RESTKORPERFORSCHUNG,FEDERAL REPUBLIC OF GERMANY AND PHYSICS DEPARTMENT,THE UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN	PHYS.REV.B,36(1987)5676	A.B.KAISER,C.UHER,E.GMELIN,L.WALZ	LA,SR,CU,O	
1024	PRB0365676		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1987																												T																																																																																												0.5			TP1024					0.42			0.18				1.2				0.45									0						ELECTRONIC TRANSPORT IN HIGHLY DOPED LA(2-X)SR(X)CU(1)O(4) SUPERCONDUCTORS	198710	THERMOPOWER              ,HALL EFFECT              ,RES	MAX-PLANCK-INSTITUT FUR RESTKORPERFORSCHUNG,FEDERAL REPUBLIC OF GERMANY AND PHYSICS DEPARTMENT,THE UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN	PHYS.REV.B,36(1987)5676	A.B.KAISER,C.UHER,E.GMELIN,L.WALZ	LA,SR,CU,O	
1025	PHC1480342		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123				3.828	3.896	11.7														92.6					92.6																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1026	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.97Al0.03O7-Z	Y	1	Ba	2	Cu	2.97	Al	0.03													O	7-Z		1	1987																											3	Y123				3.838	3.896	11.701														86.1					86.1																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1027	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06O7-Z	Y	1	Ba	2	Cu	2.94	Al	0.06													O	7-Z		1	1987																											3	Y123				3.848	3.891	11.675														80.3					80.3																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1028	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.91Al0.09O7-Z	Y	1	Ba	2	Cu	2.91	Al	0.09													O	7-Z		1	1987																											3	Y123				3.852	3.889	11.686																																																																																																																		0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1029	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.88Al0.12O7-Z	Y	1	Ba	2	Cu	2.88	Al	0.12													O	7-Z		1	1987																												Y123				3.87		11.59														68.6					68.6																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1030	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.82Al0.18O7-Z	Y	1	Ba	2	Cu	2.82	Al	0.18													O	7-Z		1	1987																												Y123																				72.1					72.1																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1031	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.76Al0.24O7-Z	Y	1	Ba	2	Cu	2.76	Al	0.24													O	7-Z		1	1987																												Y123																				72.1					72.1																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1032	PHC1480342		YBa2(Cu,Al)3O7	Y1Ba2Cu2.7Al0.3O7-Z	Y	1	Ba	2	Cu	2.7	Al	0.3													O	7-Z		1	1987																												Y123																				59.4					59.4																																																																																															0						HIGH-TC OXIDE Y-BA-CU-O NORMAL AND SUPERCONDUCTING PROPERTIES AND PHASES	198712		NATIONAL RESEARCH INSTITUTE FOR METALS,TOKYO	PHYSICA  B+C,148(1987)342	A.MATSUSHITA,H.AOKI,K.KIMURA,K.NAKAMURA,K.OGAWA,T.HATANO,T.MATSUMOTO,Y.ASADA	Y,BA,CU,O	
1033	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7-Z	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z		1	1988																											3	Y123																				89					89																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1034	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.949Fe0.051O7-Z	Y	1	Ba	2	Cu	2.949	Fe	0.051													O	7-Z		1	1988																											3	Y123																				78					78																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1035	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.901Fe0.099O7-Z	Y	1	Ba	2	Cu	2.901	Fe	0.099													O	7-Z		1	1988																											2	Y123																				62					62																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1036	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.799Fe0.201O7-Z	Y	1	Ba	2	Cu	2.799	Fe	0.201													O	7-Z		1	1988																											2	Y123																				39					39																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1037	PHF0181547		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																											3	Y123																				89					89																																						5					3800																																			0.85				1.7													0										J.Phys. F, 18(1988)1547-1562	A.Porch,J.R.Waldram,Lesley Cohen		
1038	JPF0182069		YBa2Cu3O7	Y0.33Ba0.67Cu3OX	Y	0.33	Ba	0.67	Cu	3															O	X		1	1988																											3	Y123				3.809	3.861	11.663														97					97																																																																			8											2.5																	0						A STIDY OF THE Y(X)BA(1-X)CU(1)O(Y) SUPERCONDUCTORS FOR 0.3<X<0.42	198809	TC                       ,XRY                      ,THERMOPO	ADVANCED ELECTRONIC MATERIALS GROUP,UNIVERSITY OF NEW SOUTH WALES,PO BOX 1 KENSINGTON,NSW 2033,AUSTRALIA	J.PHYS.F,18(1988)2069	A BAILEY,B HUNTER,D N MATTHEWS,G J RUSSELL,J COCHRANE,K N R TAYLOR,R A VAILE	Y,BA,CU,O	
1039	JPF0182069		YBa2Cu3O7	Y2Ba3Cu5OX	Y	2	Ba	3	Cu	5															O	X		1	1988																											3	Y123				3.812	3.869	11.633														97					97																																																																			4.5											2.6																	0						A STIDY OF THE Y(X)BA(1-X)CU(1)O(Y) SUPERCONDUCTORS FOR 0.3<X<0.42	198809	TC                       ,XRY                      ,THERMOPO	ADVANCED ELECTRONIC MATERIALS GROUP,UNIVERSITY OF NEW SOUTH WALES,PO BOX 1 KENSINGTON,NSW 2033,AUSTRALIA	J.PHYS.F,18(1988)2069	A BAILEY,B HUNTER,D N MATTHEWS,G J RUSSELL,J COCHRANE,K N R TAYLOR,R A VAILE	Y,BA,CU,O	
1040	PR0365602	FOR TC(ON),DTCDP=-0.7 FOR TC(END)	YBa2Cu3O7	Y1Ba2Cu3O7.1	Y	1	Ba	2	Cu	3															O	7	7.1	1	1987																											3	Y123				3.824	3.888	11.679															92				92			K/GPa	0.43																																																																																											0						PRESSURE DEPENDENCE OF THE TC OF Y(1)BA(2)CU(3)O(7) UP TO 170 KBAR	10	PRESSURE DEPENDENCE      ,TC	NATUURKUNDIG LABORATORIUM DER VRIJE UNIVERSITEIT,AMSTERDAM,THE NETHERLANDS	PHYS.REV.B,36(1987)5602	A.DRIESSEN,D.G.DE GROOT,E.SALOMONS,H.HEMMES,J.RECTOR,K.HEECK,N.KOEMAN,R.BROUWER,R.GRIESSEN	Y,BA,CU,O	
1041	PRB0365586		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																					90				90										90																																						5																																															0						MEASUREMENT OF THE ENERGY GAP OF Y(1)BA(2)CU(3)O(7) USING AC SUSCEPTIBILITY	198710	ENERGY GAP               ,SUSCEPTIBILITY	PHYSICS DEPARTMENT,THE TECHNION,ISRAEL	PHYS.REV.B,36(1987)5586	B.FISHER,E.POLTURAK	Y,BA,CU,O	
1042	PRB0365592		YBa2Cu3O7	Y1.1Ba2Cu3OX	Y	1.1	Ba	2	Cu	3															O	X		4	1987																											3	Y123																			70		85				77.5																																																3.4																																																					RAMAN DETECTION OF THE SUPERCONDUCTING GAP IN BA-Y-CU-O SUPERCONDUCTORS	198710	RAMAN                    ,THIN FILM                ,ANISOTROPY               ,EN	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5592	H.S.CHEN,J.KWO,K.B.LYONS,M.HONG,S.H.LIOU,T.J.NEGRAN	BA,Y,CU,O	
1043	PRB0389284		Ba(Pb,Bi)O3	Ba1Pb0.8Bi0.2O3	Ba	1	Pb	0.8	Bi	0.2															O	3	3		1988																											1	BPBO																				9.5					9.5																																																3.2																																																					SUPERCONDUCTING ENERGY GAP OF BA(1)PB(1-X)BI(X)O(3)	198811	INFRARED                 ,ENERGY GAP               ,POLYCRYS	IBM RESEARCH DIVISION,THOMAS J.WATSON RESEARCH CENTER.P.O.YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,38(1988)9284	B.A.SCOTT,J.A.CALISE,R.T.COLLINS,Z.SCHLESINGER	BA,BI,PB,O	
1044	PRB0387084		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123				3.82	3.885	11.675														92.2					92.2																																																																																		0.8												Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1045	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.94Ga0.06O7-Z	Y	1	Ba	2	Cu	2.94	Ga	0.06													O	7-Z			1988																												Y123				3.843	3.878	11.695														86.9					86.9																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1046	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.91Ga0.09O7-Z	Y	1	Ba	2	Cu	2.91	Ga	0.09													O	7-Z			1988																												Y123				3.857	3.869	11.692														77.5					77.5																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1047	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.88Ga0.12O7-Z	Y	1	Ba	2	Cu	2.88	Ga	0.12													O	7-Z			1988																												Y123				3.863		11.689														68.2					68.2																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1048	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7-Z	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-Z			1988																												Y123																				68.2					68.2																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1049	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.82Ga0.18O7-Z	Y	1	Ba	2	Cu	2.82	Ga	0.18													O	7-Z			1988																												Y123				3.864		11.702														58.2					58.2																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1050	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.76Ga0.24O7-Z	Y	1	Ba	2	Cu	2.76	Ga	0.24													O	7-Z			1988																												Y123				3.866		11.735														45.7					45.7																																																																																		8.6												Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1051	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.7Ga0.3O7-Z	Y	1	Ba	2	Cu	2.7	Ga	0.3													O	7-Z			1988																												Y123				3.865		11.739														24.7					24.7																																																																																														Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1052	PRB0387084		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.97Ga0.03O7-Z	Y	1	Ba	2	Cu	2.97	Ga	0.03													O	7-Z			1988																												Y123				3.824	3.881	11.679																																																																																																																	Y2O3,BACO3,CUO,GA2O3	0	CAL(900C 20H)-(962C 48H+865C 8H IN O2)-C TO 100C IN O2					EFFECT OF GA SDDITION TO Y(1)BA(2)CU(3)O(7)	198810	SUBSTITUTION             ,LATTICE PARAMETER        ,XRY	DIVISION OF MATERIALS SCIENCE,SROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)7084	A.R.MOODENBAUGH,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,O	
1053	PRB0387080		LaBa2Cu3O7	La1Ba2Cu3O7-Z	La	1	Ba	2	Cu	3															O	7-Z			1988																											3	Y123				3.885	3.938	11.817													92						92																																																																																														LA2O3,BACO3,CUO	0	CAL(900-950C)-SIN(980C 40H IN N2)-ANN(300C 40H IN DRIED O2)					ORTHORHOMBIC-TETRAGONAL PHASE TRANSITION IN LA(1)BA(2)CU(3)O(7-Y) WITH ZERO RESISTANCE AT 92 K	198810	PHASE TRANSITION         ,OXYGEN CONTENT           ,DTA                      ,TG	CENTRAL RESEARCH LABORATORY,MATSUSHITA ELECTRIC INDUSTRIAL CO.LTD.,OSAKA AND DEPARTMENT OF APPLIED PHYSICS,UNIVERSITY OF TOKYO,TOKYO	PHYS.REV.B,38(1988)7080	A.MAEDA,K.UCHINOKURA,N.SUZUKI,S.TANAKA,S.UCHIDA,T.MAEDA,T.WADA	LA,BA,CU,O	
1054	PRB0387074		Tl2Sr2Ca2Cu3O10	Tl2Sr2Ca2Cu3O10+X	Tl	2	Sr	2	Ca	2	Cu	3													O	10+X			1988																												Tl2223																			10		22				16																																																																																														TL2O3,SRO,CAO,CUO	0	(900-950C,3-5MIN IN O2)					SUPERCONDUCTIVITY IN THE TL-SR-CA-CU-O SYSTEM	198810	MECHANISM                ,RES                      ,SUS                      ,NE	DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,ARKANSAS	PHYS.REV.B,38(1988)7074	A.M.HERMANN,D.C.VIER,D.J.GEORGE,R.M.HAZEN,S.B.OSEROFF,S.SCHULTZ,Z.Z.SHENG	TL,SR,CA,CU,O	
1055	PRB0387074		Tl2Sr2Ca2Cu3O10	Tl2Sr1Ca2Cu3O9+X	Tl	2	Sr	1	Ca	2	Cu	3													O	9+X			1988																												Tl2223																					70				70																																																																																														TL2O3,SRO,CAO,CUO	0	(900-950C,3-5MIN IN O2)					SUPERCONDUCTIVITY IN THE TL-SR-CA-CU-O SYSTEM	198810	MECHANISM                ,RES                      ,SUS                      ,NE	DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,ARKANSAS	PHYS.REV.B,38(1988)7074	A.M.HERMANN,D.C.VIER,D.J.GEORGE,R.M.HAZEN,S.B.OSEROFF,S.SCHULTZ,Z.Z.SHENG	TL,SR,CA,CU,O	
1056	PRB0387064		Tl2Ba2Ca2Cu3O10	Tl2.2Ca2Ba2.14Cu3.72OY	Tl	2.2	Ca	2	Ba	2.14	Cu	3.72													O	Y			1988																												Tl2223																			104	110	120				110																																																																			4.5			TP1056																									0						THERMOELECTRIC POWER OF THE TL-CA-BA-CU-O SUPERCONDUCTOR	198810	THERMO POWER	DEPARTMENT OF PHYSICS,COLORADO SCHOOL OF MINES,GOLDEN,COLORADO	PHYS.REV.B,38(1988)7064	A.M.HERMANN,B.YARAR,G.PINE,J.TREFNY,N.MITRA,Z.Z.SHENG	TL,CA,BA,CU,O	
1057	PRB0387101			Bi1.7Sr1.3Ca2Cu3OX	Bi	1.7	Sr	1.3	Ca	2	Cu	3													O	X		3	1988																																															75		115				95										40																					4																																																																						MAGNETIC FIELD DEPENDENCE OF THE RESISTIVITY AND SUSCEPTIBILITY OF THE ABOVE-100-K BI-SR-CA-CU SUPERCONDUCTOR	198810	MAGNETIC FIELD           ,MAG                      ,SUS                      ,RE	IBM RESEARCH DIVISION,ALMADEN RESEACH CENTER,SAN JOSE,CALIFORNIA	PHYS.REV.B,38(1988)7101	A.I.NAZZAL,E.M.ENGLER,J.B.TORRANCE,P.M.GRANT,S.S.P.PARKIN,V.Y.LEE,Y.TOKURA	BI,SR,CA,CU,O	
1058	PRB0387200		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	7-Z	6.94		1988									6.1																		3	Y123				3.825	3.889	11.674														95					95																																																																																															0						NEW ANELASTIC RELAXATION EFFECT IN Y-BA-CU-O AT LOW TEMPERATURE: A SNOEK-TYPE PEAK DUE TO OXYGEN DIFFUSION	198810	INTERNAL FRICTION        ,ACTIVATION ENE	"INSTITUTO DI ACUSTICA ""O.M.CORBINO,""CONSIGLIO NAZIONALE DELLE RICERCHE,ROMA,ITALY"	PHYS.REV.B,38(1988)7200	F.CORDERO,G.CANNELLI,R.CANTELLI		
1059	PRB0387200		YBa2Cu3O7	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	7-Z	6.2		1988																											2	Y123				3.854		11.8																																																																																																																		0						NEW ANELASTIC RELAXATION EFFECT IN Y-BA-CU-O AT LOW TEMPERATURE: A SNOEK-TYPE PEAK DUE TO OXYGEN DIFFUSION	198810	INTERNAL FRICTION        ,ACTIVATION ENE	"INSTITUTO DI ACUSTICA ""O.M.CORBINO,""CONSIGLIO NAZIONALE DELLE RICERCHE,ROMA,ITALY"	PHYS.REV.B,38(1988)7200	F.CORDERO,G.CANNELLI,R.CANTELLI		
1060	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7-Z	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z			1988																												Y123																				89					89																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1061	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.949Fe0.051O7-Z	Y	1	Ba	2	Cu	2.949	Fe	0.051													O	7-Z			1988							6																					Y123																				78					78																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1062	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.901Fe0.099O7-Z	Y	1	Ba	2	Cu	2.901	Fe	0.099													O	7-Z			1988							10																					Y123																				62					62																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1063	SSC0650043		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.799Fe0.201O7-Z	Y	1	Ba	2	Cu	2.799	Fe	0.201													O	7-Z			1988							20																					Y123																				39					39																																																																																															0						MOSSBAUER STUDY OF Y(1)BA(2)(CU(1-X)FE(X))(3)O(7-Z) : SUPERCONDUCTIVITY AND MAGNETIC ORDER	198801	MOSSBAUER                ,SUBSTITUTION             ,SITE ASS	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,OCHANOMIZU UNIVERSITY,TOKYO	SOLID STATE COMMUN.,65(1988)0043	A.ITO,T.FUJITA,T.KOMAI,T.TAMAKI,Y.MAENO	Y,BA,CU,FE,O	
1064	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	Z	7	1	1987																											3	Y123				3.822	3.891	11.677														91.8					91.8																																																																																		1.5												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1065	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O	Z	6.78	1	1987																											3	Y123				3.827	3.895	11.722														85.4					85.4																																																																																		5												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1066	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.76	Y	1	Ba	2	Cu	3															O	Z	6.76	1	1987																											3	Y123				3.83	3.898	11.728														77.8					77.8										39																																																																								4.9												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1067	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	Z	6.72	1	1987																											3	Y123				3.835	3.89	11.716														60.8					60.8										94																																																																								3.8												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1068	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	Z	6.6	1	1987																											3	Y123				3.831	3.889	11.736														58.9					58.9																																																																																		3.5												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1069	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.53	Y	1	Ba	2	Cu	3															O	Z	6.53	1	1987																											3	Y123				3.838	3.887	11.747														54.8					54.8																																																																																		4.7												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1070	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.51	Y	1	Ba	2	Cu	3															O	Z	6.51	1	1987																											3	Y123				3.845	3.887	11.768														45.4					45.4																																																																																		5.4												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1071	PRB0365719		YBa2Cu3O7	Y1Ba2Cu3O6.3	Y	1	Ba	2	Cu	3															O	Z	6.3	1	1987																											3	Y123				3.851	3.883	11.789														28					28										62																																																																								9.2												BACO3,Y2O3,CUO	0	(900+950C 3DAYS IN AIR)-(1000C 16H IN O2)-ANN(500C 12H IN O2)					SINGLE-PHASE 60-K BULK SUPERCONDUCTOR IN ANNEALED BA(2)Y(1)CU(3)O(7-Z)(0.3<Z<0.4) WITH CORRELATED OXYGEN VACANCIES IN THE CU-O CHAINS	198710	RESISTIVITY              ,TC                       ,MAG                      ,LATTICE CONSTANT	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5719	B.BATLOGG,C.H.CHEN,D.WERDER,E.A.RIETMAN,R.J.CAVA,S.M.ZAHURAK	BA,Y,CU,O	
1072	PRB0390225		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.73Fe0.27O6.1	Y	1	Ba	2	Cu	2.73	Fe	0.27													O	X	6.1	1	1989							-1																				2	Y123				3.874		11.7																																																																																																																		0						SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND SPECIFIC-HEAT STUDIES OF THE HIGH-TC SUPERCONDUCTOR AND QUENCHED Y(1)BA(2)(CU(0.91)FE(0.09))(3)O(X)	198901	SUSCEPTIBILITY           ,SPECIFIC HEAT            ,XRY	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEMISRAEL	PHYS.REV.B,39(1989)225	G.HILSCHER,I.FELNER,N.PILLMAYR,Y.WOLFUS	Y,BA,CU,FE,O	
1073	PRB0390225		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.73Fe0.27O7.1	Y	1	Ba	2	Cu	2.73	Fe	0.27													O	X	7.1	1	1989						3.2	2.8																				2	Y123				3.874		11.7														69					69										26																																																																																					0						SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND SPECIFIC-HEAT STUDIES OF THE HIGH-TC SUPERCONDUCTOR AND QUENCHED Y(1)BA(2)(CU(0.91)FE(0.09))(3)O(X)	198901	SUSCEPTIBILITY           ,SPECIFIC HEAT            ,XRY	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEMISRAEL	PHYS.REV.B,39(1989)225	G.HILSCHER,I.FELNER,N.PILLMAYR,Y.WOLFUS	Y,BA,CU,FE,O	
1074	PRB0390729		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OY	Bi	2	Sr	2	Ca	1	Cu	2													O	Y		2	1989																												Bi2212																																																																																																							0.16				0.29				2.1															HALL COEFFICIENT OF SINGLE-CRYSTAL BI(2)SR(2)CA(1)CU(2)O(Y)	198901	SINGLE CRYSTAL           ,CARRIER DENSITY          ,HALL EFF	INSTITUTE OF PHYSICS,ACADEMIA SINICA,BEIJING,CHINA	PHYS.REV.B,39(1989)729	H.M.DUAN,L.LI,L.LU,Y.F.YAN,Y.LU	BI,SR,CA,CU,O	
1075	PRB0390315		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1989																												T				3.776		13.237														37.8					37.8																																																																														0.372				1.8												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1076	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.995Zn0.005O4	La	1.85	Sr	0.15	Cu	0.995	Zn	0.005													O	4		1	1989																												T				3.777		13.23														35.1					35.1																																																																														0.464				1.64												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1077	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01O4	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	4		1	1989																												T				3.777		13.23														30.1					30.1																																																																														0.505				1.56												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1078	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.985Zn0.015O4	La	1.85	Sr	0.15	Cu	0.985	Zn	0.015													O	4		1	1989																												T				3.778		13.229														22.1					22.1																																																																														0.545				1.55												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1079	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.98Zn0.02O4	La	1.85	Sr	0.15	Cu	0.98	Zn	0.02													O	4		1	1989																												T				3.779		13.221														6.5					6.5																																																																														0.669				1.5												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1080	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.97Zn0.03O4	La	1.85	Sr	0.15	Cu	0.97	Zn	0.03													O	4		1	1989																												T				3.78		13.221																																																																																																	0.761				1.64												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1081	PRB0390315		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.96Zn0.04O4	La	1.85	Sr	0.15	Cu	0.96	Zn	0.04													O	4		1	1989																												T				3.779		13.22																																																																																																	0.788				1.48												LA2O3,SRCO3,CUO,ZNO	0	PELLET-SIN(1000C+1000C+1050C TOTAL 100H IN O2)-C(3C/MIN)					CORRELATION BETWEEN SUPERCONDUCTIVITY AND NORMAL-STATE PROPERTIES IN THE LA(1.85)SR(0.15)(CU(1-X)ZN(X))O(4) SYSTEM	198901	RESISTIVITY              ,TC                       ,DOPANT	DEPARTMENT OF PHYSICS AND ASTRONOMY,THE JOHNS HOPKINS UNIVERSITY,BALTIMORE,MARYLAND	PHYS.REV.B,39(1989)315	A.BAKHSHAI,C.L.CHIEN,GANG XIAO,MARTA Z.CIEPLAK,Z.TESANOVIC	LA,SR,CU,ZN,O	
1082	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	7	6.41	1	1987																											2	Y123																				22.5					22.5										10.8																																																																															0.00000001318						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1083	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.34	Y	1	Ba	2	Cu	3															O	7	6.34	1	1987																											2	Y123																																			0.5																																																																															0.00000002328						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1084	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7	7	1	1987																											3	Y123																				92.5					92.5										35.4																																																																												0.00000000036			0.00000000212						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1085	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.89	Y	1	Ba	2	Cu	3															O	7	6.89	1	1987																											3	Y123																				64.7					64.7										28.4																																																																												0.00000000165			0.00000000419						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1086	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.67	Y	1	Ba	2	Cu	3															O	7	6.67	1	1987																											3	Y123																				52.5					52.5										27.1																																																																												0.00000000212			0.00000000505						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1087	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.56	Y	1	Ba	2	Cu	3															O	7	6.56	1	1987																											3	Y123																				50.4					50.4										27.1																																																																															0.0000000041						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1088	PRB0367222		YBa2Cu3O7	Y1Ba2Cu3O6.49	Y	1	Ba	2	Cu	3															O	7	6.49	1	1987																											3	Y123																				37.5					37.5										20.3																																																																															0.00000001052						0						VARIATION OF SUPERCONDUCTIVITY WITH CARRIER CONCENTRATION IN OXYGEN-DOPED Y(1)BA(2)CU(3)O(7-Y)	198711	HALL EFFECT              ,TC                       ,OXYGEN C	DEPARTMENT OF PHYSICS,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,36(1987)7222	G.W.HULL,J.CLAYHOLD,J.M.TARASCON,L.H.GREENE,N.P.ONG,W.R.MCKINNON,Z.Z.WANG	Y,BA,CU,O	
1089	PRB0367230		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																											3	Y123				3.826	3.886	11.671														90					90																																																																																														Y2O3,CUO,BAO,FE2O3	0	(750C 3H IN AIR)-(970C 6H IN 1 ATM O2)					SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND MOSSBAUER STUDY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z) DOPED WITH IRON	198711	MOSSBAUER                ,CRYSTAL STRUCTURE        ,MAGNETIC ORDERING        ,TC	DEPARTMENTS OF PHYSICS AND GEOLOGICAL SCIENCES,UNIVERSITY OF MANITOBA,WINNIPEG,MANITOBA,CANADA	PHYS.REV.B,36(1987)7230	A.H.MORRISH,I.MAARTENSE,M.RAUDSEPP,Q.A.PANKHURST,X.Z.ZHOU,Y.L.LUO	Y,BA,CU,O,FE,	
1090	PRB0367230		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O7-Z	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z			1987																											3	Y123				3.856	3.868	11.654														82.6					82.6																																																											455																																			Y2O3,CUO,BAO,FE2O3	0	(750C 3H IN AIR)-(970C 6H IN 1 ATM O2)					SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND MOSSBAUER STUDY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z) DOPED WITH IRON	198711	MOSSBAUER                ,CRYSTAL STRUCTURE        ,MAGNETIC ORDERING        ,TC	DEPARTMENTS OF PHYSICS AND GEOLOGICAL SCIENCES,UNIVERSITY OF MANITOBA,WINNIPEG,MANITOBA,CANADA	PHYS.REV.B,36(1987)7230	A.H.MORRISH,I.MAARTENSE,M.RAUDSEPP,Q.A.PANKHURST,X.Z.ZHOU,Y.L.LUO	Y,BA,CU,O,FE,	
1091	PRB0367230		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.895Fe0.105O7-Z	Y	1	Ba	2	Cu	2.895	Fe	0.105													O	7-Z			1987																											3	Y123				3.861	3.867	11.652														67					67																																																																																														Y2O3,CUO,BAO,FE2O3	0	(750C 3H IN AIR)-(970C 6H IN 1 ATM O2)					SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND MOSSBAUER STUDY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z) DOPED WITH IRON	198711	MOSSBAUER                ,CRYSTAL STRUCTURE        ,MAGNETIC ORDERING        ,TC	DEPARTMENTS OF PHYSICS AND GEOLOGICAL SCIENCES,UNIVERSITY OF MANITOBA,WINNIPEG,MANITOBA,CANADA	PHYS.REV.B,36(1987)7230	A.H.MORRISH,I.MAARTENSE,M.RAUDSEPP,Q.A.PANKHURST,X.Z.ZHOU,Y.L.LUO	Y,BA,CU,O,FE,	
1092	PRB0367230		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z			1987																											3	Y123				3.869	3.872	11.634														61					61																																																																																														Y2O3,CUO,BAO,FE2O3	0	(750C 3H IN AIR)-(970C 6H IN 1 ATM O2)					SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND MOSSBAUER STUDY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z) DOPED WITH IRON	198711	MOSSBAUER                ,CRYSTAL STRUCTURE        ,MAGNETIC ORDERING        ,TC	DEPARTMENTS OF PHYSICS AND GEOLOGICAL SCIENCES,UNIVERSITY OF MANITOBA,WINNIPEG,MANITOBA,CANADA	PHYS.REV.B,36(1987)7230	A.H.MORRISH,I.MAARTENSE,M.RAUDSEPP,Q.A.PANKHURST,X.Z.ZHOU,Y.L.LUO	Y,BA,CU,O,FE,	
1093	PRB0367230		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7-Z	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7-Z			1987																											3	Y123				3.87	3.869	11.629														2					2																																																																																														Y2O3,CUO,BAO,FE2O3	0	(750C 3H IN AIR)-(970C 6H IN 1 ATM O2)					SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND MOSSBAUER STUDY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7-Z) DOPED WITH IRON	198711	MOSSBAUER                ,CRYSTAL STRUCTURE        ,MAGNETIC ORDERING        ,TC	DEPARTMENTS OF PHYSICS AND GEOLOGICAL SCIENCES,UNIVERSITY OF MANITOBA,WINNIPEG,MANITOBA,CANADA	PHYS.REV.B,36(1987)7230	A.H.MORRISH,I.MAARTENSE,M.RAUDSEPP,Q.A.PANKHURST,X.Z.ZHOU,Y.L.LUO	Y,BA,CU,O,FE,	
1094	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.829Zn0.171O7-Z	Y	1	Ba	2	Cu	2.829	Zn	0.171													O	7-Z			1988																												Y123																				2.2					2.2																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1095	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-Z			1988																												Y123																				12.5					12.5																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1096	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.868Zn0.132O7-Z	Y	1	Ba	2	Cu	2.868	Zn	0.132													O	7-Z			1988																												Y123																				19.3					19.3																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1097	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.901Zn0.099O7-Z	Y	1	Ba	2	Cu	2.901	Zn	0.099													O	7-Z			1988																												Y123																				37.5					37.5																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1098	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.919Zn0.081O7-Z	Y	1	Ba	2	Cu	2.919	Zn	0.081													O	7-Z			1988																												Y123																				47.4					47.4																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1099	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.949Zn0.051O7-Y	Y	1	Ba	2	Cu	2.949	Zn	0.051													O	7-Y			1988																												Y123																				62.7					62.7																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1100	PRB0382903		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7-Y	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-Y			1988																												Y123																				72.3					72.3																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1101	PRB0382903		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1988																												Y123																				87.8					87.8																																																																																															0						ANOMALOUSLY LARGE T(C)DEPRESSION BY ZN SUBSTITUTION IN Y-BA-CU-O	198808	TC                       ,SUBSTITUTION	NATIONAL PHYSICAL LABORATORY,NEW DELHI,INDIA	PHYS.REV.B,38(1988)2903	A.V.NARLIKAR,B.JAYARAM,C.V.NARASIMHA RAO,S.K.AGARWAL	Y,BA,CU,O	
1102	JJP0272342		YBa2Cu3O7	Y1Ba2Cu3O7-X	Y	1	Ba	2	Cu	3															O	7-X			1988																											2	Y123				3.83	3.89	11.68													89.5		93				91.25																																																																																															0						EFFECT OF S,SE AND TE ADDITION ON THE SUPERCONDUCTIVE PROPERTIES OF BA(2)Y(1)CU(3)O(7-Y)	198812		THE INSTITUTE OF PHYSICAL AND CHEMICAL RESEARCH,WAKO,SAITAMA	JJAP LATT.,27(1988)L2342	MAKI KAWAI,SHIRO KAMBE		
1103	JJP0272342		YBa2Cu3(S,O)7	Y1Ba2Cu3S0.001O7-X	Y	1	Ba	2	Cu	3	S	0.001													O	7-X			1988																											2	Y123				3.83	3.87	11.67													90.5		93.5				92																																																																																															0						EFFECT OF S,SE AND TE ADDITION ON THE SUPERCONDUCTIVE PROPERTIES OF BA(2)Y(1)CU(3)O(7-Y)	198812		THE INSTITUTE OF PHYSICAL AND CHEMICAL RESEARCH,WAKO,SAITAMA	JJAP LATT.,27(1988)L2342	MAKI KAWAI,SHIRO KAMBE		
1104	JJP0272342		YBa2Cu3(S,O)7	Y1Ba2Cu3S0.05O7-X	Y	1	Ba	2	Cu	3	S	0.05													O	7-X			1988																											2	Y123				3.84	3.87	11.62													93		94				93.5																																																																																															0						EFFECT OF S,SE AND TE ADDITION ON THE SUPERCONDUCTIVE PROPERTIES OF BA(2)Y(1)CU(3)O(7-Y)	198812		THE INSTITUTE OF PHYSICAL AND CHEMICAL RESEARCH,WAKO,SAITAMA	JJAP LATT.,27(1988)L2342	MAKI KAWAI,SHIRO KAMBE		
1105	JJP0272342		YBa2Cu3(S,O)7	Y1Ba2Cu3Se0.05O7-X	Y	1	Ba	2	Cu	3	Se	0.05													O	7-X			1988																											2	Y123																			91						91																																																																																															0						EFFECT OF S,SE AND TE ADDITION ON THE SUPERCONDUCTIVE PROPERTIES OF BA(2)Y(1)CU(3)O(7-Y)	198812		THE INSTITUTE OF PHYSICAL AND CHEMICAL RESEARCH,WAKO,SAITAMA	JJAP LATT.,27(1988)L2342	MAKI KAWAI,SHIRO KAMBE		
1106	PRB0362386		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	9-Z	6.9		1987																											3	Y123																				80					80																																											1400																																																										TEMPERATURE DEPENDENCE OF THE MAGNETIC PWNETRATION DEPTH IN THE HIGH-TC SUPERCONDUCTOR BA2YCU3O9-Z: EVIDENCE FOR CONVENTIONAL S-WAVE PAIRING	198708	MUON                     ,PENETRAT DEPTH           ,ANISOTRO	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	RHYS.REV.B., 36(1987)2386	B.BATLOGG,D.R.HARSHMAN,G.AEPPLI,J.F.CAROLAN,J.H.BREWER,M.CELIO,R.J.CAVA	Y,BA,CU,O	
1107	JJP0280031		SmBa2Cu3O7	Sm1Ba2Cu3O6.944	Sm	1	Ba	2	Cu	3															O	7-Z	6.944		1989																												Y123																				94					94																																																																																															0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1108	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.05Ba1.95Cu3O6.94	Sm	1.05	Ba	1.95	Cu	3															O	7-Z	6.94		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1109	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.15Ba1.85Cu3O6.955	Sm	1.15	Ba	1.85	Cu	3															O	7-Z	6.955		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1110	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.2Ba1.8Cu3O6.965	Sm	1.2	Ba	1.8	Cu	3															O	7-Z	6.965		1989																												Y123																				47					47																																																																																															0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1111	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.25Ba1.75Cu3O6.972	Sm	1.25	Ba	1.75	Cu	3															O	7-Z	6.972		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1112	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.3Ba1.7Cu3O6.996	Sm	1.3	Ba	1.7	Cu	3															O	7-Z	6.996		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1113	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.1Ba1.9Cu3O7-Z	Sm	1.1	Ba	1.9	Cu	3															O	7-Z			1989																												Y123																				73					73																																																																																															0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1114	JJP0280031		Sm(Ba,Sm)2Cu3O7	Sm1.35Ba1.65Cu3O7-Z	Sm	1.35	Ba	1.65	Cu	3															O	7-Z			1989																												Y123																				8.5					8.5																																																																																															0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1115	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.25Ba1.75Cu3O6.959	Eu	1.25	Ba	1.75	Cu	3															O	7-Z	6.959		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1116	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.3Ba1.7Cu3O6.983	Eu	1.3	Ba	1.7	Cu	3															O	7-Z	6.983		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1117	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.35Ba1.65Cu3O6.995	Eu	1.35	Ba	1.65	Cu	3															O	7-Z	6.995		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1118	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.4Ba1.6Cu3O7.006	Eu	1.4	Ba	1.6	Cu	3															O	7-Z	7.006		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1119	JJP0280031		EuBa2Cu3O7	Eu1Ba2Cu3O6.962	Eu	1	Ba	2	Cu	3															O	7-Z	6.962		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1120	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.05Ba1.95Cu3O6.93	Eu	1.05	Ba	1.95	Cu	3															O	7-Z	6.93		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1121	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.1Ba1.9Cu3O6.932	Eu	1.1	Ba	1.9	Cu	3															O	7-Z	6.932		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1122	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.15Ba1.85Cu3O6.937	Eu	1.15	Ba	1.85	Cu	3															O	7-Z	6.937		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1123	JJP0280031		Eu(Ba,Eu)2Cu3O7	Eu1.2Ba1.8Cu3O6.956	Eu	1.2	Ba	1.8	Cu	3															O	7-Z	6.956		1989																												Y123																																																																																																																								0						RELATION OF TC WITH HOLE CONCENTRATION IN LN(1+X)BA(2-X)CU(3)O(7-Z) (LN=SM AND EU); HALL EFFECT MEASUREMENT AND CHEMICAL ANALYSIS	198901	HALL EFFECT              ,HOLE CONCENTRA	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,IBARAKI	JJAP LETT.,28(1989)L31	HIDEO KATOH,HIROYUKI AKINAGA,KOHZOH MASUDA,KOKI TAKITA	SM,EU,BA,CU,O	
1124	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.67Y0.33Cu2O8+Z	Bi	2	Sr	2	Ca	0.67	Y	0.33	Cu	2											O	8+Z			1988																												Bi2212						30.58														34.3					34.3																																																																																																					ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1125	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.83Y0.17Cu2O8+Z	Bi	2	Sr	2	Ca	0.83	Y	0.17	Cu	2											O	8+Z			1988																												Bi2212																				48.4					48.4																																																																																																					ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1126	JJP0271432		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1988																												Bi2212						30.85														52.4					52.4																																																																																																					ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1127	JJP0271432		Bi2Sr2CaCu2O8	Bi2Sr2Y1Cu2O8+Z	Bi	2	Sr	2	Y	1	Cu	2													O	8+Z			1988								15.4																				Bi2212						30.25																																																																																																																								ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1128	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8+Z	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8+Z			1988								13.2																				Bi2212						30.25																																																																																																																								ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1129	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.25Y0.75Cu2O8+Z	Bi	2	Sr	2	Ca	0.25	Y	0.75	Cu	2											O	8+Z			1988																												Bi2212						30.27																																																																																																																								ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1130	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.33Y0.67Cu2O8+Z	Bi	2	Sr	2	Ca	0.33	Y	0.67	Cu	2											O	8+Z			1988																												Bi2212						30.31																																																																																																																								ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1131	JJP0271432		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8+Z	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8+Z			1988																												Bi2212						30.55														17					17																																																																																																					ELECTRICAL AND MAGNETIC PROPERTIES IN BI(2)SR(2)CA(1-X)Y(X)CU(2)O(8+Z)	198808	STRUCTURE                ,ANTIFERROMAGNE	TOSHIBA CORPORATION RESEARCH AND DEVELOPMENT CENTER,KAWASAKI	JJAP LETT.,27(1988)L1432	HIROMI NIU,KEN ANDO,NOBURU FUKUSHIMA	BI,SR,CA,Y,CU,O	
1132	JJP0280037			Bi1Pb0.1Sr1Ca1Cu2OX	Bi	1	Pb	0.1	Sr	1	Ca	1	Cu	2											O	X		3	1989																																															102		120				111																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1133	JJP0280037			Bi1Pb0.2Sr1Ca1Cu2OX	Bi	1	Pb	0.2	Sr	1	Ca	1	Cu	2											O	X		3	1989																																															99		119				109																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1134	JJP0280037			Bi1Pb0.3Sr1Ca1Cu2OX	Bi	1	Pb	0.3	Sr	1	Ca	1	Cu	2											O	X		3	1989																																															92		118				105																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1135	JJP0280037			Bi1Pb0.4Sr1Ca1Cu2OX	Bi	1	Pb	0.4	Sr	1	Ca	1	Cu	2											O	X		3	1989																																															88		115				101.5																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1136	JJP0280037			Bi0.8Pb0.1Sr0.8Ca1Cu1.4OX	Bi	0.8	Pb	0.1	Sr	0.8	Ca	1	Cu	1.4											O	X		3	1989																																															82		120				101																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1137	JJP0280037			Bi0.8Pb0.2Sr0.8Ca1Cu1.4OX	Bi	0.8	Pb	0.2	Sr	0.8	Ca	1	Cu	1.4											O	X		3	1989																																															92		119				105.5																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1138	JJP0280037			Bi0.8Pb0.3Sr0.8Ca1Cu1.4OX	Bi	0.8	Pb	0.3	Sr	0.8	Ca	1	Cu	1.4											O	X		3	1989																																															90		118				104																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1139	JJP0280037			Bi0.8Pb0.4Sr0.8Ca1Cu1.4OX	Bi	0.8	Pb	0.4	Sr	0.8	Ca	1	Cu	1.4											O	X		3	1989																																															86		115				100.5																																																																																															0						PREPARATION AND CRYSTALLIZATION PROCESS OF THE HIGH-TC SUPERCONDUCTING PHASE (TC(END)>100 K)IN BI,PB-SR-CA-CU-O GLASS-CERAMICS	198901	GLASSY STATE             ,FABRICATION              ,THERMAL	DEPARTMENT OF ELECTRICAL ENGINEERING,FACULTY OF ENGINEERING,HIROSHIMA UNIVERSITY,HIGASHI-HIROSHIMA	JJAP LETT.,28(1989)L37	HIROYUKI NASU,TAKESHI IMURA,YOSHIKAZU IBARA,YUKIO OSAKA	BI,PB,SR,CA,CU,O	
1140	PRB0392729		Y(Ba,Cs)2Cu3O7	Y1Ba1.95Cs0.05Cu3O7-Z	Y	1	Ba	1.95	Cs	0.05	Cu	3													O	7-Z		3	1989																												Y123				3.827	3.876	11.632													78	85.5	90.5				85.5																																																																																															0						SUPERCONDUCTIVITY IN Y(1)BA(1.95)CS(0.05)CU(3)O(7-Y) GRANULAR CERAMICS	198902	RESISTIVITY              ,GRANULAR	INSTITUT DE PHYSIQUE B5,UNIVERSITE DE LIEGE,BELGIUM	PHYS.REV.B,39(1989)2729	A.RULMONT,CH.LAURENT,H.W.VANDERSCHUEREN,M.AUSLOOS,P.TARTE	Y,BA,CS,CU,O	
1141	PRB0392251		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		2	1989								280																				T																																																																																																																								0						INFRARED STUDY OF ANISOTROPY IN SINGLE-CRYSTAL LA(2-X)SR(X)CU(1)O(4)	198902	INFRARED                 ,SINGLE CRYSTAL           ,ANISOTRO	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,39(1989)2251	G.V.CHANDRASHEKHAR,M.W.SHAFER,R.T.COLLINS,Z.SCHLESINGER	LA,SR,CU,O	
1142	PRB0392251		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		2	1989																												T																																																																																																																								0						INFRARED STUDY OF ANISOTROPY IN SINGLE-CRYSTAL LA(2-X)SR(X)CU(1)O(4)	198902	INFRARED                 ,SINGLE CRYSTAL           ,ANISOTRO	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,39(1989)2251	G.V.CHANDRASHEKHAR,M.W.SHAFER,R.T.COLLINS,Z.SCHLESINGER	LA,SR,CU,O	
1143	PRB0392255		Bi2(Sr,Bi)2CaCu2O8	Bi2.2Sr1.8Ca1Cu2OY	Bi	2.2	Sr	1.8	Ca	1	Cu	2													O	Y		2	1989																												Bi2212																				90					90																																																																																															0						PHOTOEMISSION STUDY OF BI(2)(SR,CA)(3)CU(2)O(Y)	198902	ELECTRONIC STRUCTURE     ,PHOTOEMISSION            ,EELS	DEPARTMENT OF PHYSICS,UNIVERSITY OF TOKYO,TOKYO	PHYS.REV.B,39(1989)2255	A.FUJIMORI,A.ONO,E.TAKAYAMA-MUROMACHI,H.KATAYAMA-YOSHIDA,S.TAKEKAWA,T.TAKAHASHI,Y.OKABE,Y.UCHIDA	BI,SR,CA,CU,O	
1144	PRB0392255		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4-Z	La	1.92	Sr	0.08	Cu	1															O	4-Z		2	1989																												T																																																																																																																								0						PHOTOEMISSION STUDY OF BI(2)(SR,CA)(3)CU(2)O(Y)	198902	ELECTRONIC STRUCTURE     ,PHOTOEMISSION            ,EELS	DEPARTMENT OF PHYSICS,UNIVERSITY OF TOKYO,TOKYO	PHYS.REV.B,39(1989)2255	A.FUJIMORI,A.ONO,E.TAKAYAMA-MUROMACHI,H.KATAYAMA-YOSHIDA,S.TAKEKAWA,T.TAKAHASHI,Y.OKABE,Y.UCHIDA	BI,SR,CA,CU,O	
1145	PRB0392336		La2CoO4	La2Co1O4	La	2	Co	1																	O	4		2	1989								275																				T				5.473	5.606	12.656																																																																																																																		0						SUCCESSIVE ANTIFERROMAGNETIC PHASE TRANSITIONS IN SINGLE-CRYSTAL LA(2)CO(1)O(4)	198902	PHASE TRANSITION         ,SINGLE CRYSTAL           ,NEUTRON SCATTERING       ,AN	DEPARTMENT OF PHYSICS,TOHOKU UNIVERSITY,SENDAI	PHYS.REV.B,39(1989)2336	B.KEIMER,G.SHIRANE,J.MIZUSAKI,K.YAMADA,M.MATSUDA,R.J.BIRGENEAU,S.ONODERA,T.MATSUURA,Y.ENDOH	LA,CO,O	
1146	PRB0390785		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1989																												Y123																																																																				3000							1																												0.09																							POWER-LAW TEMPERATURE DEPENDENCE OF THE ELECTRODYNAMIC PROPERTIES IN ORIENTED Y(1)BA(2)CU(3)O(7-Z) AND Y(2)BA(4)CU(8)O(16-Z) FILMS	198901	SURFACE RESISTANCE       ,SURFACE REACTANCE        ,FILM	DEPARTMENT OF PHYSICS AND SOLID STATE SCIENCE CENTER,UNIVERSITY OF CALIFORNIA,LOS ANGELES,CALIFORNIA	PHYS.REV.B,39(1989)785	GEORGE GRUNER,JOHN P.CARINI,K.CHAR,LAWRENCE DRABECK,M.R.BEASLEY,T.HYLTON	Y,BA,CU,O	
1147	PRB0390851		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	2	1989																											3	Y123																				82					82																																											1415																																																										MAGNETIC PENETRATION DEPTH IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-Z)	198901	PENETRATION              ,SINGLE CRYSTAL           ,MAGNETIZ	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,39(1989)851	B.BATLOGG,D.LL.WILLIAMS,D.R.HARSHMAN,E.J.ANSALDO,G.AEPPLI,J.V.WASZCZAK,L.F.SCHNEEMEYER,L.W.RUPP,R.J.CAVA	Y,BA,CU,O	
1148	PRB0380909		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	Z	6.95		1988																											3	Y123																				89.9					89.9																																											1656																																																										SYSTEMATIC VARIATION OF MAGNETIC-FIELD PENETRATION DEPTH IN HIGH-TC SUPERCONDUCTORS STUDIED BY MUON-SPIN RELAXATION	198807	MUON                     ,PENETRATION DE	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)909	A.J.JACOBSON,A.R.MOODENBAUGH,C.E.STRONACH,D.C.JOHNSTON,D.OPIE,G.M.LUKE,H.E.SCHONE,J.H.BREWER,J.R.KEMPTON,J.T.LEWANDOWEKI,M.SUENAGA,R.F.KIEFL,S.R.KREITZMAN,T.RISEMAN,V.J.EMERY,W.J.KOSSLER,X.H.YU,Y.J.UEMURA	Y,BA,CU,O,LA,SR,CU,O	
1149	PRB0380909		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	Z	7		1988																											3	Y123																				91.1					91.1																																											1472																																																										SYSTEMATIC VARIATION OF MAGNETIC-FIELD PENETRATION DEPTH IN HIGH-TC SUPERCONDUCTORS STUDIED BY MUON-SPIN RELAXATION	198807	MUON                     ,PENETRATION DE	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)909	A.J.JACOBSON,A.R.MOODENBAUGH,C.E.STRONACH,D.C.JOHNSTON,D.OPIE,G.M.LUKE,H.E.SCHONE,J.H.BREWER,J.R.KEMPTON,J.T.LEWANDOWEKI,M.SUENAGA,R.F.KIEFL,S.R.KREITZMAN,T.RISEMAN,V.J.EMERY,W.J.KOSSLER,X.H.YU,Y.J.UEMURA	Y,BA,CU,O,LA,SR,CU,O	
1150	PRB0367199		EuBa2Cu3O7	Eu1Ba2Cu3OY	Eu	1	Ba	2	Cu	3															O	Y			1987																											3	Y123																				94.8					94.8																							190	45								3	0.7						27	6																																						0.41				0.72																			ELECTRICAL PROPERTIES OF HIGH-TC SUPERCONDUCTING SINGLE-CRYSTAL EU(1)BA(2)CU(3)O(Y)	198711	RESISTIVITY              ,SINGLE CRYSTAL           ,HC                       ,AN	NIPPON TELEGRAPH AND TELEPHONE ELECTRICAL COMMUNICATIONS LABORATORIES,TOKAI,IBARAKI	PHYS.REV.B,36(1987)7199	AKINORI KATSUI,MAKOTA HIKITA,SHIGEYUKI TSURUMI,TSUNEKAZU IWATA,YOSHIKAZU HIDAKA,YUKIMICHI TAJIMA	EU,BA,CU,O	
1151	JJP0272339		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988																												Y123																			92.5		93.8				93.15																																																																																																					ELECTRON IRRADIATION EFFECT ON A BA(2)Y(1)CU(3)O(7) SUPERCONDUCTOR	198812	IRRADIATION              ,RESISTIVITY              ,CRITICAL CURRENT         ,TC	TAKASAKI RADIATION CHEMISTRY RESEARCH ESTABLISHMENT,JAPAN ATOMIC ENERGY RESEARCH INSTITUTE,GUNMA	JJAP LETT.,27(1988)L2339	HIROSHI ITOH,KENSUKE SHIRAISHI,OSAMU YODA	Y,BA,CU,O	
1152	PRB0390801		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X			1989																												Bi2212																				85					85																																																6.3																																																					ELECTRON TUNNELING AND THE ENERGY GAP IN BI(2)SR(2)CA(1)CU(2)O(X)	198901	TUNNELING                ,SINGLE CRYSTAL           ,ENERGY G	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,CALIFORNIA	PHYS.REV.B,39(1989)801	A.KAPITULNIK,D.B.MITZI,M.R.BEASLEY,MARK LEE	BI,SR,CA,CU,O	
1153	SSC0650997		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123																																																																									4																																																					ELECTRON TUNNELING STUDIES OF HIGH-TC SUPERCONDUCTOR YBA2CU3O7-Z				SOLID STATE COMMUN.,65(1988)997	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O	
1154	SSC0670057		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123				3.82	3.889	11.668														92.11					92.11																																																																																																					SUPERCONDUCTIVITY IN YTTRIUM-TERBIUM-BARIUM-COPPER OXIDE	198810	LATTICE CONSTANT         ,Tc                       ,RES	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA,IOWA,USA	SOLID STATE COMMUN.,68(1988)0057	JAMES E.KASPER,JOHN W.SCHWEITZER,LEE S.MARTINSON,NORMAN G.BAENZIGER,WILLIAM R.SAVAGE	Y,TB,BA,CU,O	
1155	SSC0670057		(Y,Tb)Ba2Cu3O7	Y0.96Tb0.04Ba2Cu3O7-Z	Y	0.96	Tb	0.04	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.819	3.889	11.677														92.01					92.01																																																																																																					SUPERCONDUCTIVITY IN YTTRIUM-TERBIUM-BARIUM-COPPER OXIDE	198810	LATTICE CONSTANT         ,Tc                       ,RES	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA,IOWA,USA	SOLID STATE COMMUN.,68(1988)0057	JAMES E.KASPER,JOHN W.SCHWEITZER,LEE S.MARTINSON,NORMAN G.BAENZIGER,WILLIAM R.SAVAGE	Y,TB,BA,CU,O	
1156	SSC0670057		(Y,Tb)Ba2Cu3O7	Y0.92Tb0.08Ba2Cu3O7-Z	Y	0.92	Tb	0.08	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.82	3.889	11.672														92.01					92.01																																																																																																					SUPERCONDUCTIVITY IN YTTRIUM-TERBIUM-BARIUM-COPPER OXIDE	198810	LATTICE CONSTANT         ,Tc                       ,RES	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA,IOWA,USA	SOLID STATE COMMUN.,68(1988)0057	JAMES E.KASPER,JOHN W.SCHWEITZER,LEE S.MARTINSON,NORMAN G.BAENZIGER,WILLIAM R.SAVAGE	Y,TB,BA,CU,O	
1157	SSC0670057		(Y,Tb)Ba2Cu3O7	Y0.88Tb0.12Ba2Cu3O7-Z	Y	0.88	Tb	0.12	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.831	3.891	11.666														92.1					92.1																																																																																																					SUPERCONDUCTIVITY IN YTTRIUM-TERBIUM-BARIUM-COPPER OXIDE	198810	LATTICE CONSTANT         ,Tc                       ,RES	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA,IOWA,USA	SOLID STATE COMMUN.,68(1988)0057	JAMES E.KASPER,JOHN W.SCHWEITZER,LEE S.MARTINSON,NORMAN G.BAENZIGER,WILLIAM R.SAVAGE	Y,TB,BA,CU,O	
1158	PRL0601446		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123				3.822	3.888	11.681														91.06					91.06																																																																																		1.588																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1159	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.97Ga0.03O7	Y	1	Ba	2	Cu	2.97	Ga	0.03													O	7			1988																												Y123				3.835	3.882	11.687														90.88					90.88																																																																																		1.805																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1160	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.94Ga0.06O7	Y	1	Ba	2	Cu	2.94	Ga	0.06													O	7			1988																												Y123				3.851	3.874	11.681														87.99					87.99																																																																																		2.473																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1161	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.91Ga0.09O7	Y	1	Ba	2	Cu	2.91	Ga	0.09													O	7			1988																												Y123				3.858	3.866	11.686														83.71					83.71																																																																																		3.05																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1162	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.88Ga0.12O7	Y	1	Ba	2	Cu	2.88	Ga	0.12													O	7			1988																												Y123				3.861	3.866	11.681														79.89					79.89																																																																																		3.538																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1163	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7			1988																												Y123				3.861	3.866	11.684														78.49					78.49																																																																																		4.332																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1164	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.82Ga0.18O7	Y	1	Ba	2	Cu	2.82	Ga	0.18													O	7			1988																												Y123				3.863	3.863	11.686														79.24					79.24																																																																																		4.296																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1165	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.79Ga0.21O7	Y	1	Ba	2	Cu	2.79	Ga	0.21													O	7			1988																												Y123				3.864	3.864	11.686														76.91					76.91																																																																																		4.585																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1166	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.76Ga0.24O7	Y	1	Ba	2	Cu	2.76	Ga	0.24													O	7			1988																												Y123				3.865	3.865	11.683														71.79					71.79																																																																																		7.022																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1167	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.73Ga0.27O7	Y	1	Ba	2	Cu	2.73	Ga	0.27													O	7			1988																												Y123				3.866	3.866	11.683														67.04					67.04																																																																																		7.166																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1168	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.67Ga0.33O7	Y	1	Ba	2	Cu	2.67	Ga	0.33													O	7			1988																												Y123				3.866	3.866	11.679														65.64					65.64																																																																																		9.206																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1169	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.61Ga0.39O7	Y	1	Ba	2	Cu	2.61	Ga	0.39													O	7			1988																												Y123				3.865	3.865	11.677														64.8					64.8																																																																																		12.67																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1170	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.55Ga0.45O7	Y	1	Ba	2	Cu	2.55	Ga	0.45													O	7			1988																												Y123				3.867	3.867	11.677														65.36					65.36																																																																																		20.94																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1171	PRL0601446		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.4Ga0.6O7	Y	1	Ba	2	Cu	2.4	Ga	0.6													O	7			1988																												Y123				3.868	3.868	11.675														63.31					63.31																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1172	PRL0601446		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123				3.822	3.888	11.683														89.66					89.66																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1173	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7			1988																												Y123				3.827	3.883	11.683														78.21					78.21																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1174	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7			1988																												Y123				3.829	3.883	11.683														67.04					67.04																																																																																		1.877																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1175	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7			1988																												Y123				3.829	3.883	11.683														55.87					55.87																																																																																		1.877																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1176	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O7	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7			1988																												Y123				3.834	3.886	11.681														47.02					47.02																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1177	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7			1988																												Y123				3.833	3.883	11.681														45.53					45.53																																																																																		2.256																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1178	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.82Zn0.18O7	Y	1	Ba	2	Cu	2.82	Zn	0.18													O	7			1988																												Y123				3.833	3.883	11.681														46.18					46.18																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1179	PRL0601446		YBa2(Cyu,Zn)3O7	Y1Ba2Cu2.885Zn0.195O7	Y	1	Ba	2	Cu	2.885	Zn	0.195													O	7			1988																												Y123				3.833	3.885	11.679														32.4					32.4																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1180	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O7	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	7			1988																												Y123				3.834	3.884	11.68														35.2					35.2																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1181	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.73Zn0.27O7	Y	1	Ba	2	Cu	2.73	Zn	0.27													O	7			1988																												Y123				3.835	3.887	11.681																																																																																																																								HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1182	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O7	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	7			1988																												Y123				3.837	3.89	11.686														27					27																																																																																																					HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1183	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.67Zn0.33O7	Y	1	Ba	2	Cu	2.67	Zn	0.33													O	7			1988																												Y123				3.836	3.888	11.683																																																																																																																								HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1184	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.76Zn0.24O7	Y	1	Ba	2	Cu	2.76	Zn	0.24													O	7			1988																												Y123																				29.05					29.05																																																																																		3.899																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1185	PRL0601446		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.58Zn0.42O7	Y	1	Ba	2	Cu	2.58	Zn	0.42													O	7			1988																												Y123																																																																																																											8.881																			HIGH-TEMPERATURE SUPERCONDUCTIVITY IN TETRAGONAL PEROVSKITE STRUCTURES:IS OXYGEN-VACANCY ORDER IMPORTANT?	198804			PHYS.REV.LETT.,60(1988)1446	A.BAKHSHAI,A.GAVRIN,C.L.CHIEN,F.T.STREITZ,GANG XIAO,M.Z.CIEPLAK	Y,BA,CU,O,ZN,GA,	
1186	PRB0392312		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		4	1989																												T																																																																																																							7800				3460																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1187	PRB0392312		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O	4		4	1989																												T																																																																																																							3.7				6.31																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1188	PRB0392312		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		4	1989																												T																				26.2					26.2																																																																														0.287				0.958																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1189	PRB0392312		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		4	1989																												T																				28.6					28.6																																																																														0.236				0.75																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1190	PRB0392312		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		4	1989																												T																				18.9					18.9																																																																														0.165				0.531																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1191	PRB0392312		(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		4	1989																												T																				15.2					15.2																																																																														0.109				0.333																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1192	PRB0392312		(La,Sr)2CuO4	La1.64Sr0.36Cu1O4	La	1.64	Sr	0.36	Cu	1															O	4		4	1989																												T																																																																																																							0.096				0.299																			HALL COEFFICIENTS AND OPTICAL PROPERTIES OF LA(2-X)SR(X)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198902	THIN FILM                ,FILM                     ,HALL EFFECT              ,OP	NIPPON TELEGRAPH AND TELEPHONE OPTO-ELECTRONICS LABORATORIES,IBARAKI	PHYS.REV.B,39(1989)2312	MINORU SUZUKI	LA,SR,CU,O	
1193	JJP0280193		Bi2Sr2(Sr,Nd)Cu2O8	Bi2Sr2.9Nd0.1Cu2OY	Bi	2	Sr	2.9	Nd	0.1	Cu	2													O	Y			1989																												Bi2212																																																																																																																														SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1194	JJP0280193		Bi2Sr2(Sr,Nd)Cu2O8	Bi2Sr2.8Nd0.2Cu2OY	Bi	2	Sr	2.8	Nd	0.2	Cu	2													O	Y			1989																												Bi2212																				62.94					62.94																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1195	JJP0280193		Bi2Sr2(Sr,Nd)Cu2O8	Bi2Sr2.7Nd0.3Cu2OY	Bi	2	Sr	2.7	Nd	0.3	Cu	2													O	Y			1989																												Bi2212																				63.38					63.38																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1196	JJP0280193		Bi2Sr2(Sr,Nd)Cu2O8	Bi2Sr2.6Nd0.4Cu2OY	Bi	2	Sr	2.6	Nd	0.4	Cu	2													O	Y			1989																												Bi2212																				55.28					55.28																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1197	JJP0280193		Bi2Sr2(Sr,Nd)Cu2O8	Bi2Sr2.5Nd0.5Cu2OY	Bi	2	Sr	2.5	Nd	0.5	Cu	2													O	Y			1989																												Bi2212																				50.09					50.09																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1198	JJP0280193		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OY	Bi	2	Sr	2	Ca	1	Cu	2													O	Y			1989																												Bi2212																				72.18					72.18																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1199	JJP0280193		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.9La0.1Ca1Cu2OY	Bi	2	Sr	1.9	La	0.1	Ca	1	Cu	2											O	Y			1989																												Bi2212																				85.04					85.04																																																																																																					SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1200	JJP0280193		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.8La0.2Ca1Cu2OY	Bi	2	Sr	1.8	La	0.2	Ca	1	Cu	2											O	Y			1989																												Bi2212																				90.58					90.58																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1201	JJP0280193		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.7La0.3Ca1Cu2OY	Bi	2	Sr	1.7	La	0.3	Ca	1	Cu	2											O	Y			1989																												Bi2212																				86					86																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1202	JJP0280193		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.6La0.4Ca1Cu2OY	Bi	2	Sr	1.6	La	0.4	Ca	1	Cu	2											O	Y			1989																												Bi2212																				75.18					75.18																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1203	JJP0280193		Bi2(Sr,La)2CaCuO8	Bi2Sr1.5La0.5Ca1Cu2OY	Bi	2	Sr	1.5	La	0.5	Ca	1	Cu	2											O	Y			1989																												Bi2212																				55.63					55.63																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1204	JJP0280193		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.4La0.6Ca1Cu2OY	Bi	2	Sr	1.4	La	0.6	Ca	1	Cu	2											O	Y			1989																												Bi2212																				39.44					39.44																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1205	JJP0280193		BiSrCuOZ	Bi1Sr1Cu1OY	Bi	1	Sr	1	Cu	1															O	Y			1989																																																5.28					5.28																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1206	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.95Nd0.05Cu1OY	Bi	1	Sr	0.95	Nd	0.05	Cu	1													O	Y			1989																																																8.01					8.01																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1207	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.9Nd0.1Cu1OY	Bi	1	Sr	0.9	Nd	0.1	Cu	1													O	Y			1989																																																10.74					10.74																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1208	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.85Nd0.15Cu1OY	Bi	1	Sr	0.85	Nd	0.15	Cu	1													O	Y			1989																																																13.56					13.56																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1209	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.8Nd0.2Cu1OY	Bi	1	Sr	0.8	Nd	0.2	Cu	1													O	Y			1989																																																14.79					14.79																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1210	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.75Nd0.25Cu1OY	Bi	1	Sr	0.75	Nd	0.25	Cu	1													O	Y			1989																																																14.96					14.96																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1211	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.7Nd0.3Cu1OY	Bi	1	Sr	0.7	Nd	0.3	Cu	1													O	Y			1989																																																13.2					13.2																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1212	JJP0280193		Bi2(Sr,Nd)3Cu2O8	Bi1Sr0.65Nd0.35Cu1OY	Bi	1	Sr	0.65	Nd	0.35	Cu	1													O	Y			1989																																																10.21					10.21																																																																																															0						SUPERCONDUCTIVITY IN THE BI(2)SR(3-X)LN(X)CU(2)O(Y) SYSTEM AND THE EXCESS OF HOLE CONCENTRATION IN BI(2)SR(2)CA(N)CU(1+N)O(Y) (N=0 AND 1)	198902	MATERIAL                 ,RES                      ,SUS                      ,TC	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,TOKYO	JJAP.LETT.,28(1989)L193	JUN AKIMITSU,TOHRU DEN	PR,ND,BI,SR,LN,CU,O	
1213	JJP0280200			Tl2.5Nd1Sr2Cu2.5OX	Tl	2.5	Nd	1	Sr	2	Cu	2.5													O	X			1989																																															16.37		40.78				28.575																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1214	JJP0280200			Tl2.5Pb0.2Nd1Sr2Cu2.5OX	Tl	2.5	Pb	0.2	Nd	1	Sr	2	Cu	2.5											O	X			1989																																															30.97		41.99				36.48																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1215	JJP0280200			Tl2.5Pb0.5Nd1Sr2Cu2.5OX	Tl	2.5	Pb	0.5	Nd	1	Sr	2	Cu	2.5											O	X			1989																																															36.94		42.8				39.87																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1216	JJP0280200			Tl2.5Pb0.6Nd1Sr2Cu2.5OX	Tl	2.5	Pb	0.6	Nd	1	Sr	2	Cu	2.5											O	X			1989																																															36.99		42.58				39.785																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1217	JJP0280200			Tl2.5Pb0.7Nd1Sr2Cu2.5OX	Tl	2.5	Pb	0.7	Nd	1	Sr	2	Cu	2.5											O	X			1989																																															30.89		42.28				36.585																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1218	JJP0280200			Tl2.5Pb1Nd1Sr2Cu2.5OX	Tl	2.5	Pb	1	Nd	1	Sr	2	Cu	2.5											O	X			1989																																																	41.26				41.26																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1219	JJP0280200			Tl2.5Pb0.3Pr1Sr2Cu2.5OX	Tl	2.5	Pb	0.3	Pr	1	Sr	2	Cu	2.5											O	X			1989																																																	39.06				39.06																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1220	JJP0280200			Tl2.5Pb0.5Pr1Sr2Cu2.5OX	Tl	2.5	Pb	0.5	Pr	1	Sr	2	Cu	2.5											O	X			1989																																															15.54		40.24				27.89																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1221	JJP0280200			Tl2.5Pb0.65Pr1Sr2Cu2.5OX	Tl	2.5	Pb	0.65	Pr	1	Sr	2	Cu	2.5											O	X			1989																																															20		40.56				30.28																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1222	JJP0280200			Tl2.5Pb0.8Pr1Sr2Cu2.5OX	Tl	2.5	Pb	0.8	Pr	1	Sr	2	Cu	2.5											O	X			1989																																															15.54		40.08				27.81																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1223	JJP0280200			Tl2.5Pb1Pr1Sr2Cu2.5OX	Tl	2.5	Pb	1	Pr	1	Sr	2	Cu	2.5											O	X			1989																																																	39.22				39.22																																																																																														TL2O3,PBO,SRCO3,CUO,R2O3	0	SIN(850-870C 8-12H IN AIR)-ANN(860-880C 40-80MIN)-C(10-15C/MIN)					SUPERCONDUCTIVITY OF NEW COMPOUNDS IN THE SYSTEMS TL-LN-SR-CU-O (LN=PR AND ND) AND TL-PB-LN-SR-CU-O (LN=PR,ND AND SM)	198902	RESISTIVITY              ,NEW MATERIAL             ,TC	CERAMICS RESEARCH LABORATORY,ONODA CEMENT CO.,LTD.,TOKYO	JJAP.LETT.,28(1989)L200	HIROSHI UCHIKAWA,TAKAO ITOH	PR,ND,SM,TL,PB,SR,CU,O	
1224	PRB0390777		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.98Ni0.02O7	Y	1	Ba	2	Cu	2.98	Ni	0.02													O	7			1989																												Y123																		K		91.6					91.6																																																																		uV/K	-1.293																												0						CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
1225	PRB0390777		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.95Ni0.05O7	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	7			1989																												Y123																		K		90.6					90.6																																																																		uV/K	-3.142																												0						CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
1226	PRB0390777		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O7	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7			1989																												Y123																		K		83					83																																																																		uV/K	-3.95																												0						CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
1227	PRB0390777		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.8Ni0.2O7	Y	1	Ba	2	Cu	2.8	Ni	0.2													O	7			1989																												Y123																		K		79.4					79.4																																																																		uV/K	-3.849																												0						CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
1228	PRB0390777		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.6Ni0.4O7	Y	1	Ba	2	Cu	2.6	Ni	0.4													O	7			1989																												Y123																		K		71					71																																																																		uV/K	-2.164																												0						CHAIN-SITE VERSUS PLANE-SITE CU SUBSTITUTION IN Y(1)BA(2)CU(3-X)M(X)O(7) (M=CO,NI): HALL AND THERMOPOWER STUDIES	198901	SUBSTITUTION             ,HALL EFFECT              ,THERMOPO	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY	PHYS.REV.B,39(1989)777	J.CLAYHOLD,J.M.TARASCON,N.P.ONG,P.BARBOUX,S.HAGEN,Z.Z.WANG	Y,BA,CU,CO,NI,O	
1229	PRB0394693	POINT CONTACT	Bi2Sr2CaCu2O8	Bi2Ca1Sr2Cu2O8	Bi	2	Ca	1	Sr	2	Cu	2													O	8		1	1989																												Bi2212																				88					88																																																3.4	1																																													BI2O3,SRCO3,CA(NO3)2,CUO	0	CAL(860C 48H IN AIR)-SIN(850C 24H IN AIR)					TUNNELING MEASUREMENTS ON BI(2)CASR(2)CU(2)O(8)	198903	TUNNELING                ,I-V CHARACTERI	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA CITY,IOWA	PHYS. REV. B.,39(1989)4693	ROBERT E.JOHNSON	BI,CA,SR,CU,O	
1230	PSA1030113			Ba1Y1Cu2OX	Ba	1	Y	1	Cu	2															O	X			1987																																3.82	3.888	11.616																																																																																																																								LA AND LI DOPED HIGH-TC SUPERCONDUCTOR OF Y-BA-CU-O CERAMICS	198709	DOPING EFFECT            ,XRY                      ,RES                      ,SU	DEPARTMENT OF PHYSICS,ZHONGSHAN UNIVERSITY,GUANGZHOU	PHYS.STAT.SOL.A,103(1987)K113	CHAORUI LI,HONG WANG,WU LI,XIANDUAN LIN,YUHUAN XU,ZHONGRONG LI	Y,BA,CU,O,LA,LI	
1231	PSA1030113			Ba1Y1Cu1.6Li0.4OX	Ba	1	Y	1	Cu	1.6	Li	0.4													O	X			1987																																3.82	3.885	11.664																																																																																																																								LA AND LI DOPED HIGH-TC SUPERCONDUCTOR OF Y-BA-CU-O CERAMICS	198709	DOPING EFFECT            ,XRY                      ,RES                      ,SU	DEPARTMENT OF PHYSICS,ZHONGSHAN UNIVERSITY,GUANGZHOU	PHYS.STAT.SOL.A,103(1987)K113	CHAORUI LI,HONG WANG,WU LI,XIANDUAN LIN,YUHUAN XU,ZHONGRONG LI	Y,BA,CU,O,LA,LI	
1232	PSA1030113			Ba1Y0.67La0.33Cu1.8Li0.2OX	Ba	1	Y	0.67	La	0.33	Cu	1.8	Li	0.2											O	X			1987																																3.888	3.895	11.598													82	90					90																																																																																																					LA AND LI DOPED HIGH-TC SUPERCONDUCTOR OF Y-BA-CU-O CERAMICS	198709	DOPING EFFECT            ,XRY                      ,RES                      ,SU	DEPARTMENT OF PHYSICS,ZHONGSHAN UNIVERSITY,GUANGZHOU	PHYS.STAT.SOL.A,103(1987)K113	CHAORUI LI,HONG WANG,WU LI,XIANDUAN LIN,YUHUAN XU,ZHONGRONG LI	Y,BA,CU,O,LA,LI	
1233	PRB0394690			Tl1.5Pb0.3Nd2Sr2Cu2OX	Tl	1.5	Pb	0.3	Nd	2	Sr	2	Cu	2											O	X			1989																																															29.6	37.5	43.1				37.5																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1234	PRB0394690			Tl1.5Pb0.5Nd2Sr2Cu2OX	Tl	1.5	Pb	0.5	Nd	2	Sr	2	Cu	2											O	X			1989																																															31.7		44.1				37.9																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1235	PRB0394690			Tl1.5Pb0.7Nd2Sr2Cu2OX	Tl	1.5	Pb	0.7	Nd	2	Sr	2	Cu	2											O	X			1989																																															16.8		44.1				30.45																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1236	PRB0394690			Tl1.5Pb1Nd2Sr2Cu2OX	Tl	1.5	Pb	1	Nd	2	Sr	2	Cu	2											O	X			1989																																																	44.1				44.1																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1237	PRB0394690			Tl1.5Pb0.5Sm2Sr2Cu2OX	Tl	1.5	Pb	0.5	Sm	2	Sr	2	Cu	2											O	X			1989																																																23.6					23.6																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1238	PRB0394690			Tl1.5Pb0.5Pr2Sr2Cu2OX	Tl	1.5	Pb	0.5	Pr	2	Sr	2	Cu	2											O	X			1989																																																16.7					16.7																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1239	PRB0394690			Tl1.5Pb0.5La2Sr2Cu2OX	Tl	1.5	Pb	0.5	La	2	Sr	2	Cu	2											O	X			1989																																																																																																																																																			PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1240	PRB0394690			Tl1.5Nd1Sr2Cu3OX	Tl	1.5	Nd	1	Sr	2	Cu	3													O	X			1989																																																36.1					36.1																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1241	PRB0394690			Tl1.5Nd2Sr2Cu3OX	Tl	1.5	Nd	2	Sr	2	Cu	3													O	X			1989																																																29.8					29.8																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1242	PRB0394690			Tl1.5Pb0.5Nd1Sr2Cu3OX	Tl	1.5	Pb	0.5	Nd	1	Sr	2	Cu	3											O	X			1989																																																39.6					39.6																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1243	PRB0394690			Tl1.5Pb0.5Nd2Sr2Cu3OX	Tl	1.5	Pb	0.5	Nd	2	Sr	2	Cu	3											O	X			1989																																																38.8					38.8																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1244	PRB0394690			Tl1.5Nd2Sr2Cu2OX	Tl	1.5	Nd	2	Sr	2	Cu	2													O	X			1989																																															15.5		41.8				28.65																																																																																														PBO,ND2O3,SRCO3,CUO,TL2O3	0	CAL(860C 9H IN AIR)-MIX WITH TL2O3-(860C 70MIN IN PT CRUCIBLE)-C(15C/MIN) TO 300C					SUPERCONDUCTIVITY IN THE TI-ND-SR-CU-O AND THE TI-PB-ND-SR-CU-O- SYSTEMS	198903	RESISTIVITY              ,SUSCEPTIBILITY           ,MATERIAL	CERAMICS RESEARCH LABORATORY,ONODA CEMENT COMPANY,LTD.,TOKYO 13-5,JAPAN	PHYS.REV. B.,39(1989)4690	HIROSHI UCHIKAWA,TAKAO ITOH	TL,ND,SR,CU,O,PB	
1245	AS3370345		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.93	Nd	1.85	Ce	0.15	Cu	1															O	4-X	3.93	1	1989																												T'				3.95		12.07															24				24																																																																																						-0.65															A SUPERCONDUCTING COPPER OXIDE COMPOUND WITH ELECTRONS AS THECHARGE CARRIERS	1	RES                      ,STRUCTURE                ,SUS	DEPARTMENT OF PHYSICS AND ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,TOKYO	NATURE,337(1989)345	H.TAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,SR,CU,O	
1246	AS3370345		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-X	Pr	1.85	Ce	0.15	Cu	1															O	4-X		1	1989																												T'																					17				17																																																																																																					A SUPERCONDUCTING COPPER OXIDE COMPOUND WITH ELECTRONS AS THECHARGE CARRIERS	1	RES                      ,STRUCTURE                ,SUS	DEPARTMENT OF PHYSICS AND ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,TOKYO	NATURE,337(1989)345	H.TAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,SR,CU,O	
1247	AS3370345		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-X	Sm	1.85	Ce	0.15	Cu	1															O	4-X		1	1989																												T*																					15				15																																																																																																					A SUPERCONDUCTING COPPER OXIDE COMPOUND WITH ELECTRONS AS THECHARGE CARRIERS	1	RES                      ,STRUCTURE                ,SUS	DEPARTMENT OF PHYSICS AND ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,TOKYO	NATURE,337(1989)345	H.TAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,SR,CU,O	
1248	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.98Ni0.02O7	Y	1	Ba	2	Cu	2.98	Ni	0.02													O	7			1989																												Y123																																																																																																															0.000000000504			0.00000000125		RH1248				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1249	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.95Ni0.05O7	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	7			1989																												Y123																																																																																																															0.000000000448			0.000000000835		RH1249				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1250	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O7	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7			1989																												Y123																																																																																																															0.000000000478			0.000000000854		RH1250				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1251	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.8Ni0.2O7	Y	1	Ba	2	Cu	2.8	Ni	0.2													O	7			1989																												Y123																																																																																																															0.000000000604			0.0000000011		RH1251				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1252	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O7	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	7			1989																												Y123																																																																																																															0.000000000636			0.00000000115		RH1252				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1253	PRB0397324	RH300=AT 250K,RHN=AT 100K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.6Ni0.4O7	Y	1	Ba	2	Cu	2.6	Ni	0.4													O	7			1989																												Y123																				58					58																																																																																						0.000000000793			0.0000000012		RH1253				0						HALL-EFFECT ANOMALY IN THE HIGH-TC COPPER-BASED PEROVSKITES	198904	HALL EFFECT         ,ANOMALY	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B.,39(1989)7324	J.CLAYHOLD,N.P.ONG,Z.Z.WANG	CO,NI,Y,BA,CU,O,LA,SR	
1254	PRB0402568	RH300 = FOR (SR=0.30)	(Sm,La,Sr)2CuO4	Sm1La0.75Sr0.25Cu1O3.95	Sm	1	La	0.75	Sr	0.25	Cu	1													O	3.95	3.95		1989																											2		P4/NMM			3.859		12.572															20				20										10																																																																												0.000000002								LA2O3,SM2O3,CUO,SRCO3	0	CAL(950C10H IN AIR)-SIN(1130C 15H IN AIR)-Q TO RT IN AIR-ANN(550C IN O2 UPTO 80 ATM)					NEW FAMILI OF LAYERED COPPER OXIDE COMPOUNDS WITH ORDERED CATIONS:PROSPECTIVE HIGH-TEMPERATURE SUPERCONDUCTORS	198908	NEW FAMILY          ,FABRICATION         ,HREM                ,HALL EFFECT	DEPARTMENT OF PHYSICS,UNIVERSITY OF TOKYO,7-3-1 HONGO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2568	H.ASANO,H.MATSUBAR,H.TAKAGI,H.WATABE,K.HIRAGA,S.UCHIDA,T.MOCHIKU,T.OKU,Y.TOKURA	SM,LA,SR,CU,O	
1255	SSC0660189	RHN=AT 77K,HC2 FIGURE	BiSrCuOZ	Bi1Sr1Cu1OY	Bi	1	Sr	1	Cu	1															O	Y			1988																											2					5.381		24.65														6.7					6.7																																																																																						0.00000000625			0.0000000149						0						SUPERCONDUCTING AND ELECTRONIC PROPERTIES OF BI(1-X)LA(X)SR(1)CU(1)O(Y) SYSTEM	198804	RESISTIVITY              ,HALL EFFECT              ,HC                       ,SU	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI NATIONAL RESEARCH INSTITUTES,MYODAIJI,OKAZAKI	SOLID STATE COMMUN.,66(1988)189	H.SAWA,J.AKIMITSU,K.FUKUDA,M.ONODA,M.SATO,M.SERA,S.KONDOH,T.DEN	BI,LA,SR,CU,O	
1256	SSC0660189		(Bi,La)SrCuOZ	Bi1.95La0.05Sr1Cu1OY	Bi	1.95	La	0.05	Sr	1	Cu	1													O	Y			1988																											2							24.398														20					20										7.5																																																																																					0						SUPERCONDUCTING AND ELECTRONIC PROPERTIES OF BI(1-X)LA(X)SR(1)CU(1)O(Y) SYSTEM	198804	RESISTIVITY              ,HALL EFFECT              ,HC                       ,SU	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI NATIONAL RESEARCH INSTITUTES,MYODAIJI,OKAZAKI	SOLID STATE COMMUN.,66(1988)189	H.SAWA,J.AKIMITSU,K.FUKUDA,M.ONODA,M.SATO,M.SERA,S.KONDOH,T.DEN	BI,LA,SR,CU,O	
1257	PRB0377963		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Z	La	1.85	Sr	0.15	Cu	1															O	4-Z		1	1988																											2	T																				35					35																																																																			55			TP1257																									1						OBSERVATIONS ON THE THERMOPOWER OF THE HIGH-TC SUPERCONDUCTORS	198805	THERMOPOWER              ,SEEBECK EFFECT	DEPARTMENT OF PHYSICS AND LABORATORY FOR RESEARCH ON THE STRUCTURE OF MATTER,UNIVERSITY OF PENNSYLVANIA,PHILADELPHIA,PENNSYLVANIA	PHYS.REV.B,37(1988)7963	F.HOLTZBERG,J.STUART,M.J.NAUGHTON,P.DAVIES,P.M.CHAIKIN,R.C.YU,R.L.GREENE,X.YAN	SR,LA,CU,O,Y,BA,CU,O	
1258	PRB0377963		YBa2Cu307	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				92					92																																																																			-0.19			TP1258																									1						OBSERVATIONS ON THE THERMOPOWER OF THE HIGH-TC SUPERCONDUCTORS	198805	THERMOPOWER              ,SEEBECK EFFECT	DEPARTMENT OF PHYSICS AND LABORATORY FOR RESEARCH ON THE STRUCTURE OF MATTER,UNIVERSITY OF PENNSYLVANIA,PHILADELPHIA,PENNSYLVANIA	PHYS.REV.B,37(1988)7963	F.HOLTZBERG,J.STUART,M.J.NAUGHTON,P.DAVIES,P.M.CHAIKIN,R.C.YU,R.L.GREENE,X.YAN	SR,LA,CU,O,Y,BA,CU,O	
1259	PRB0377963		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																				92					92																																																																			-2.05			TP1259																									1						OBSERVATIONS ON THE THERMOPOWER OF THE HIGH-TC SUPERCONDUCTORS	198805	THERMOPOWER              ,SEEBECK EFFECT	DEPARTMENT OF PHYSICS AND LABORATORY FOR RESEARCH ON THE STRUCTURE OF MATTER,UNIVERSITY OF PENNSYLVANIA,PHILADELPHIA,PENNSYLVANIA	PHYS.REV.B,37(1988)7963	F.HOLTZBERG,J.STUART,M.J.NAUGHTON,P.DAVIES,P.M.CHAIKIN,R.C.YU,R.L.GREENE,X.YAN	SR,LA,CU,O,Y,BA,CU,O	
1260	PRB0358794		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1987																											3	T																																																																																												308																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1261	PRB0358794		(La,Ba)2CuO4	La1.95Ba0.05Cu1O4	La	1.95	Ba	0.05	Cu	1															O	4		1	1987																												T																																																																																												137																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1262	PRB0358794		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4		1	1987																											2	T																																																																																												97																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1263	PRB0358794		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4		1	1987																												T																																																																																												50																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1264	PRB0358794		(La,Ba)2CuO4	La1.725Ba0.275Cu1O4	La	1.725	Ba	0.275	Cu	1															O	4		1	1987																												T																																																																																												13																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1265	PRB0358794		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		1	1987																												T																																																																																												117																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1266	PRB0358794		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1987																											2	T																																																																																												54																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1267	PRB0358794		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4		1	1987																											2	T																				29					29																																																																			13.6																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1268	PRB0358794		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1987																											2	T																				36					36																																																																			4																											LA2O3,BACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 17H IN AIR)-C TO RT WITHIN 4H					THERMOELECTRIC POWER OF SOME HIGH-TC OXIDES		THERMOPOWER	UNIV. OF CALIFORNIA,LOS ANGELES,CALIFORNIA,USA	PHYS.REV.B,35(1987)8794	B.ALAVI,G.GRUNER,J.R.COOPER,L-W.ZHOU,W.P.BEYERMANN		
1269	PLA1270228		Y(Ba,La)2Cu3O7	Y1Ba1La1Cu3OZ	Y	1	Ba	1	La	1	Cu	3													O	Z		1	1988																											3	Y123				3.84	3.856	11.55																																																																																						103																											Y2O3,BACO3,LA2O3,CUO	1	CAL(IN AIR)-SIN(1080C IN O2)-C TO 400C					EVIDENCE FOR ELECTRONIC LOCALIZATION IN Y(1)BA(2-Y)LA(Y)CU(3)O(X)	198802	ELECTRICAL PROPERTIES    ,THERMOPOWER	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NM	PHYS.LETT.A,127(1988)228	C.B.PIERCE,J.A.O'ROURKE,J.D.THOMPSON,J.L.SMITH,R.S.KWOK,Z.FISK	Y,BA,LA,CU,O	
1270	JJP0280762	RHN=AT 60K,PRESS. DEP. OF TC AND HC2 ALSO SHOWN	(La,Sr)2CuO4	La1.92Sr0.08Cu1OZ	La	1.92	Sr	0.08	Cu	1															O	Z		1	1989																												T																				21.8	25.2				21.8			K/GPa	3.75																																																																							4.77							5.5							0.00000000636						1	SPRAY-DRY TECKNIQUE					THE STRONTIUM CONTENT DEPENDENCE OF PRESSURE EFFECT IN (LA(1-X)SR(X))(2)CUO(4)	198905	PRESSURE EFFECT     ,HALL COEFFICIENT    ,TC	INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106	JJAP LETT.,28(1989)L762	CHIZUKO MURAYAMA,KOICHI KITAZAWA,NOBUKATSU TANAHASHI,NOBUO MOHRI,NORIAKI OKAZAKI,SHUSUKE YOMO,TSUYOSHI TAMEGAI,YASUHIRO YRE	LA,SR,CU,O	
1271	JJP0280762		(La,Sr)2CuO4	La1.88Sr0.12Cu1OZ	La	1.88	Sr	0.12	Cu	1															O	Z		1	1989																												T																				30.3	33.4				30.3			K/GPa	3.66																																																																							1.08							2.96							0.00000000312						1	SPRAY-DRY TECKNIQUE					THE STRONTIUM CONTENT DEPENDENCE OF PRESSURE EFFECT IN (LA(1-X)SR(X))(2)CUO(4)	198905	PRESSURE EFFECT     ,HALL COEFFICIENT    ,TC	INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106	JJAP LETT.,28(1989)L762	CHIZUKO MURAYAMA,KOICHI KITAZAWA,NOBUKATSU TANAHASHI,NOBUO MOHRI,NORIAKI OKAZAKI,SHUSUKE YOMO,TSUYOSHI TAMEGAI,YASUHIRO YRE	LA,SR,CU,O	
1272	JJP0280762		(La,Sr)2CuO4	La1.84Sr0.16Cu1OZ	La	1.84	Sr	0.16	Cu	1															O	Z		1	1989																												T																				38	38.7				38			K/GPa	3.26																																																																							0.67							2.09							0.00000000147						1	SPRAY-DRY TECKNIQUE					THE STRONTIUM CONTENT DEPENDENCE OF PRESSURE EFFECT IN (LA(1-X)SR(X))(2)CUO(4)	198905	PRESSURE EFFECT     ,HALL COEFFICIENT    ,TC	INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106	JJAP LETT.,28(1989)L762	CHIZUKO MURAYAMA,KOICHI KITAZAWA,NOBUKATSU TANAHASHI,NOBUO MOHRI,NORIAKI OKAZAKI,SHUSUKE YOMO,TSUYOSHI TAMEGAI,YASUHIRO YRE	LA,SR,CU,O	
1273	JJP0280762		(La,Sr)2CuO4	La1.8Sr0.2Cu1OZ	La	1.8	Sr	0.2	Cu	1															O	Z		1	1989																												T																				32.7	34.4				32.7			K/GPa	2.43																																																																							0.33							1.05							0.00000000071						1	SPRAY-DRY TECKNIQUE					THE STRONTIUM CONTENT DEPENDENCE OF PRESSURE EFFECT IN (LA(1-X)SR(X))(2)CUO(4)	198905	PRESSURE EFFECT     ,HALL COEFFICIENT    ,TC	INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106	JJAP LETT.,28(1989)L762	CHIZUKO MURAYAMA,KOICHI KITAZAWA,NOBUKATSU TANAHASHI,NOBUO MOHRI,NORIAKI OKAZAKI,SHUSUKE YOMO,TSUYOSHI TAMEGAI,YASUHIRO YRE	LA,SR,CU,O	
1274	JJP0280762		(La,Sr)2CuO4	La1.76Sr0.24Cu1OZ	La	1.76	Sr	0.24	Cu	1															O	Z		1	1989																												T																				18.7	20.2				18.7			K/GPa	3.02																																																																							0.23							0.84							0.00000000043						1	SPRAY-DRY TECKNIQUE					THE STRONTIUM CONTENT DEPENDENCE OF PRESSURE EFFECT IN (LA(1-X)SR(X))(2)CUO(4)	198905	PRESSURE EFFECT     ,HALL COEFFICIENT    ,TC	INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106	JJAP LETT.,28(1989)L762	CHIZUKO MURAYAMA,KOICHI KITAZAWA,NOBUKATSU TANAHASHI,NOBUO MOHRI,NORIAKI OKAZAKI,SHUSUKE YOMO,TSUYOSHI TAMEGAI,YASUHIRO YRE	LA,SR,CU,O	
1275	SSC0680649		(La,Sr)2CuO4	La1.99Sr0.01Cu1O4	La	1.99	Sr	0.01	Cu	1															O	4		3	1988																												T																																																																																												102			TP1275																									1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1276	SSC0680649		(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	1988																												T																			11						11																																																																			31.6			TP1276																									1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1277	SSC0680649		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		3	1988																												T																																																																																												121			TP1277																									1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1278	SSC0680649	THPOW ALONG C AXIS ALSO SHOWN	YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	3	1988																											3	Y123																			92					1	92																																																																			2.1			TP1278									1.9	36			6.7	50											1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1279	SSC0680649		YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	Z	6.7	3	1988																												Y123																			73	85.4					85.4																																																																			13.4			TP1279									26.8	307			19.5	146											1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1280	SSC0680649		YBa2Cu3O7	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	Z	6.2	3	1988																												Y123																																																																																												64.4			TP1280																									1	USING CUO FLUX					ANISOTROPIC THERMOELECTRIC POWERS OF Y(1)BA(2)CU(3)O(7-Z) AND (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE CRYSTALS	198811	SINGLE CRYSTAL           ,ANISOTROPY               ,THERMOPO	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)649	M.SATO,M.SERA,S.SHAMOTO	Y,BA,CU,O,LA,SR	
1281	PRB0357124	CULAO3 PHASE OBSERVED, THPOW UP TO 160K	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4-Y	La	1.8	Ba	0.2	Cu	1															O	4-Y		2	1987																												T																			28						28																																																																						TP1281																								LA2O3,BACO3,CUO	1	CAL(900C 8H IN AIR)-SIN(1100C 4H IN AIR)					DETERMINATION OF CHARGE CARRIERS IN SUPERCONDUCTING LA-BA-CU-O BY THERMOELECTRIC MEASUREMENTS	198705	CHARGE CARRIER           ,THERMOPOWER	DEPARTMENT OF PHYSICS,WAYNE STATE UNIVERSITY,DETROIT,MICHIGAN	PHYS.REV.B,35(1987)7124	C.J.MCEWAN,E.M.LOGOTHETIS,J.T.CHEN,L.E.WENGER	LA,BA,CU,O	
1282	PRB0375916	RES BY MONTGOMERY METHOD. S=A*T**(1/2)	La2CuO4	La2Cu1O4-Y	La	2	Cu	1																	O	4-Y		3	1988																												T				5.358	5.403	13.181															33				33																																																																			160						1230			8.6	9100						14.1	4200		0.000000115									1	USING PBO FLUX, CHEM.ANAL.=LA1.75CUO4.3+2AT%PB					ELECTRONIC ANISOTROPY IN SINGLE-CRYSTAL LA(2)CU(1)O(4)	198804	RESISTIVITY              ,ANISOTROPY               ,THERMOEP	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO	PHYS.REV.B,37(1988)5916	G.GRUNER,J.D.THOMPSON,J.P.REMEIKA,R.S.KWOK,S-W.CHEONG,Z.FISK	LA,CU,O	
1283	PRB0364007		La2CuO4	La2Cu1O3.985	La	2	Cu	1																	O	4-Y	3.985	1	1987								230																				T																																																																																												118																												1	CAL(950C IN AIR)-FC-HEAT(500C UNDER 600PSI O2)					INFLUENCE OF OXYGEN DEFECTS ON THE PHYSICAL PROPERTIES OF LA(2)CU(1)O(4-Y)	198709	SUS                      ,SPECIFIC HEAT            ,RESISTIVITY              ,TH	CORPORATE RESEARCH LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,36(1987)4007	D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI	LA,CU,O	
1284	PRB0364007		La2CuO4	La2Cu1O3.97	La	2	Cu	1																	O	4-Y	3.97	1	1987								290																				T																																																																																																																								1	CAL(950C IN AIR)-FC-HEAT(500C UNDER 600PSI O2)					INFLUENCE OF OXYGEN DEFECTS ON THE PHYSICAL PROPERTIES OF LA(2)CU(1)O(4-Y)	198709	SUS                      ,SPECIFIC HEAT            ,RESISTIVITY              ,TH	CORPORATE RESEARCH LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,36(1987)4007	D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI	LA,CU,O	
1285	PRB0364007		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4-Y	4	1	1987																												T																																																																																												729																												1	CAL(950C IN AIR)-FC-HEAT(500C UNDER 600PSI O2)					INFLUENCE OF OXYGEN DEFECTS ON THE PHYSICAL PROPERTIES OF LA(2)CU(1)O(4-Y)	198709	SUS                      ,SPECIFIC HEAT            ,RESISTIVITY              ,TH	CORPORATE RESEARCH LABORATORIES,EXXON RESEARCH AND ENGINEERING COMPANY,ANNANDALE,NEW JERSEY	PHYS.REV.B,36(1987)4007	D.C.JOHNSTON,D.P.GOSHORN,J.P.STOKES,J.T.LEWANDOWSKI	LA,CU,O	
1286	PR0410769	USING BRANDT'S FORMULA	Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3OX	Tl	2	Ba	2	Ca	2	Cu	3													O	X			1990																												Tl2223																				119					119																																									A	EPR SPECTRA	2520																																																				0						MEASUREMENT BY EPR OF THE PENETRATION DEPHT IN THE HIGH-TC SUPERCONDUCTORS TL2BA2CA2CU3OX AND BI2CA2SRCU2OX	199001	EPR                 ,PENTERATION DEPHT	CHEMISTRY DEPARTMENT, WEST VIRGINIA UNIVERSITY, MORGANTOWN, WEST VIRGINIA 26506	PHYS.REV.B,41(1990)769	A.S.BHALLA,B.RAKNIN,N.S.DALAL,T.A.MAHL,Z.Z.SHENG	TL,BA,CA,CU,O,BI,SR	
1287	PR0410769		Bi2Sr2CaCu2O8	Bi2Sr2Ca2Cu2OX	Bi	2	Sr	2	Ca	2	Cu	2													O	X			1990																												Bi2212																				84					84																																									A	EPR	2700																																																				0						MEASUREMENT BY EPR OF THE PENETRATION DEPHT IN THE HIGH-TC SUPERCONDUCTORS TL2BA2CA2CU3OX AND BI2CA2SRCU2OX	199001	EPR                 ,PENTERATION DEPHT	CHEMISTRY DEPARTMENT, WEST VIRGINIA UNIVERSITY, MORGANTOWN, WEST VIRGINIA 26506	PHYS.REV.B,41(1990)769	A.S.BHALLA,B.RAKNIN,N.S.DALAL,T.A.MAHL,Z.Z.SHENG	TL,BA,CA,CU,O,BI,SR	
1288	PR0410282	85%O(18),NON-SUPER	(La,Sr)2CuO4	La1.962Sr0.038Cu1O4	La	1.962	Sr	0.038	Cu	1															O	4		1	1990																												T																																																																																																																								1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1289	PR0410282	90%O(18),TC0-TC=0.84	(La,Sr)2CuO4	La1.925Sr0.075Cu1O4	La	1.925	Sr	0.075	Cu	1															O	4		1	1990																												T																				21.2					21.2						0.4	O	90	0.84																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1290	PR0410282	88%O(18),TC0-TC=1.91	(La,Sr)2CuO4	La1.887Sr0.113Cu1O4	La	1.887	Sr	0.113	Cu	1															O	4		1	1990																												T																				29.7					29.7						0.64	O	88	1.91																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1291	PR0410282	87%O(18),TC0-TC=0.32	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				37.8					37.8						0.08	O	87	0.32																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1292	PR0410282	84%O(18),TC0-TC=0.21	(La,Sr)2CuO4	La1.812Sr0.188Cu1O4	La	1.812	Sr	0.188	Cu	1															O	4		1	1990																												T																				34.4					34.4						0.06	O	84	0.21																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1293	PR0410282	88%O(18),TC0-TC=0.23	(La,Sr)2CuO4	La1.775Sr0.225Cu1O4	La	1.775	Sr	0.225	Cu	1															O	4		1	1990																												T																				23					23						0.1	O	88	0.23																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1294	PR0410282	86%O(18),TC0-TC=0.22	(La,Sr)2CuO4	La1.737Sr0.263Cu1O4	La	1.737	Sr	0.263	Cu	1															O	4		1	1990																												T																				8					8						0.12	O	86	0.22																																																																																						1	SIN(1100C 12H IN O2)-FC					ANOMALOUS OXYGEN ISOTOPE EFFECT IN LA2-XSRXCUO4	199001	ISOTOPE EFFECT	E.I.DU PONT DENEMOURS AND CO., INC., CENTRAL RESEARCH AND DEVELOPMENT DEPARTMENT, EXPERIMENTAL STATION, WILMINGTON, DELAWARE 19880-0356	PHYS.REV.B,41(1990)282	E.M.MCCARRON 3,M.K.CRAWFORD,M.N.KUNCHUR,S.J.POON,W.E.FARNETH	LA,SR,CU,O	
1295	PR04011406	980C,P(O2)=20BAR	Y2Ba4Cu7Oz	Y2Ba4Cu7O15-X	Y	2	Ba	4	Cu	7															O	15-X		1	1989																											3	Y247				3.854	3.874	50.4														55					55																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1296	PR04011406	CONTAIN 124 PHASE,980C P(O2)=35BAR	Eu2Ba4Cu7Oz	Eu2Ba4Cu7O15-X	Eu	2	Ba	4	Cu	7															O	15-X		2	1989																											3	Y247				3.879	3.886	50.39														45					45																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1297	PR04011406	CONTAIN 124 PHASE,930C P(O2)=35BAR	Gd2Ba4Cu7Oz	Gd2Ba4Cu7O15-X	Gd	2	Ba	4	Cu	7															O	15-X		2	1989																											3	Y247				3.872	3.879	50.36														45					45																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1298	PR04011406		Dy2Ba4Cu7Oz	Dy2Ba4Cu7O15-X	Dy	2	Ba	4	Cu	7															O	15-X		1	1989																											3	Y247				3.864	3.879	50.39														50					50																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1299	PR04011406		Ho2Ba4Cu7Oz	Ho2Ba4Cu7O15-X	Ho	2	Ba	4	Cu	7															O	15-X		2	1989																											3	Y247				3.857	3.879	50.4														55					55																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1300	PR04011406		Er2Ba4Cu7Oz	Er2Ba4Cu7O15-X	Er	2	Ba	4	Cu	7															O	15-X		1	1989																											3	Y247				3.847	3.873	50.44														55					55																																																																																														R2O3,BAO,CU0	1	SIN(930-980C 8H IN 18.6BAR O2)-C(5C/MIN) TO RT IN O2					SYNTHESIS AND PROPERTIES OF THE 2:4:7 SUPERCONDUCTORS R2BA4CU7O15-X (R=Y,EU,GD,DY,HO,ER)	198912	SYNTHESIZED         ,OXYGEN CONTENT      ,HOLE CONCENTRATION	LAWRENCE BERKELEY LABORATORY 2-300,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11406	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY E.POST,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR,RANDY L.SID	R,BA,CU,O,Y	
1301	SSC0680647	THPOW=MINIMUM AT 100K	(Ba,K)BiO3	Ba0.77K0.23Bi1O3	Ba	0.77	K	0.23	Bi	1															O	3			1988																												BKBO																			28						28										10																																																									3.22			TP1301					700							78													0	USING AG-TUBE					THERMOELECTRIC POWER OF SUPERCONDUCTING BA-K-BI-O WITH PEROVSKITE STRUCTURE	198811	THERMOPOWER	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI	SOLID STATE COMMUN.,68(1988)647	M.SATO,M.SERA,S.KONDOH	BA,K,BI,O	
1302	APL0531753	X-RAY DIFFRACTION, STRUCTURE FACTOR	(Ba,K)BiO3	Ba0.87K0.13Bi1O3	Ba	0.87	K	0.13	Bi	1															O	3		3	1988																											1	BKBO	PM3M			4.322																																																																																																																			BA(OH)2.8H2O,BI2O3,KOH	0	HEAT(360C IN AIR) USING AU BOAT,EXCESS KOH WAS DISSOLVED IN WATER					OXYGEN ATOM THERMAL VIBRATION ANISOTROPY IN BA(0.87)K(0.13)BI(1)O(3)	10	STRUCTURE                ,THERMAL VIBRAT	CENTER FOR MATERIALS SCIENCE AND ENGINEERING,THE UNIVERSITY OF TEXAS AT AUSTIN TEXAS	APPL.PHYS.LETT.,53(1988)1753	H.STEINFINK,J.B.GOODENOUGH,J.P.WIGNACOURT,J.S.SWINNEA	BA,K,BI,O	
1303	SSC0670879		(Ba,K)BiO3	Ba0.7K0.75Bi1OY	Ba	0.7	K	0.75	Bi	1															O	Y			1988																											1	BKBO																				29					29										9.1																																																																	700							78												BAO,KO2,BI2O3	1	SEALED IN AG TUBE-HEAT(675C 3DAYS)-FC					SYNTHESIS OF SUPERCONDUCTING BA-K-BI-O SYSTEM WITH PEROVSKITE STRUCTURE	198809	FABRICATION              ,SUS                      ,RES	INSTITUTE FOR MOLECULAR SCIENCE,OKAZAKI JAPAN	SOLID STATE COMMUN.,67(1988)879	K.FUKUDA,M.SATO,M.SERA,S.KONDOH,Y.ANDO	BA,K,BI,O	
1304	PRB0373745	BAND STRUCTURE IN EL0602681	(Ba,K)BiO3	Ba0.9K0.2Bi1O3-Z	Ba	0.9	K	0.2	Bi	1															O	3-Z		2	1988																											1	BKBO																				20					20																																																																																														BACO3,K2CO3,BI2O3	1	MIX-HEAT(900C 2H IN PT CRUCIBLE)-SIN(900C 2H IN O2)					SUPERCONDUCTIVITY ABOVE 20 K IN THE BA-K-BI-O SYSTEM	198803	FABRICATION              ,SUSCEPTIBILITY	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)3745	D.W.JOHNSON,E.M.GYORGY,JR.,L.F.MATTHEISS	BA,K,BI,O	
1305	PRB0373745		(Ba,K)BiO3	Ba0.9K0.24Bi1O3-Z	Ba	0.9	K	0.24	Bi	1															O	3-Z		2	1988																											1	BKBO																				22					22																																																																																														BACO3,K2CO3,BI2O3	1	MIX-HEAT(900C 2H IN PT CRUCIBLE)-SIN(900C 2H IN O2)					SUPERCONDUCTIVITY ABOVE 20 K IN THE BA-K-BI-O SYSTEM	198803	FABRICATION              ,SUSCEPTIBILITY	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)3745	D.W.JOHNSON,E.M.GYORGY,JR.,L.F.MATTHEISS	BA,K,BI,O	
1306	PRB0373745		(Ba,Rb)BiO3	Ba0.9Rb0.2Bi1O3-Z	Ba	0.9	Rb	0.2	Bi	1															O	3-Z		2	1988																											1	BKBO																				15					15																																																																																														BACO3,K2CO3,BI2O3	1	MIX-HEAT(900C 2H IN PT CRUCIBLE)-SIN(900C 2H IN O2)					SUPERCONDUCTIVITY ABOVE 20 K IN THE BA-K-BI-O SYSTEM	198803	FABRICATION              ,SUSCEPTIBILITY	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,37(1988)3745	D.W.JOHNSON,E.M.GYORGY,JR.,L.F.MATTHEISS	BA,K,BI,O	
1307	PRB0397339	FLUX CREEP	(Ba,K)BiO3	Ba0.6K0.4Bi1O3-Z	Ba	0.6	K	0.4	Bi	1															O	3-Z		1	1989																											1	BKBO	IM3M			4.287																26	29				26										98																																								300000																																												BANO3,BI2O3,KNO3	1	(700K 1H IN N2)-ANN(450C 3H+375C 4H IN O2)-FC					Flux creep in a polycrystalline Ba0.6K0.4BiO3 superconductor	198904		Los Alomos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B,39(1989)7339	G.H. Kwei,J.D. Thompson,M.E. McHenry,M.P. Maley		
1308	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.941	Sm	1	Ba	2	Cu	3															O	Z	6.941		1989																											3	Y123																				90.7					90.7																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1309	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	Z	7		1989																											3	Y123																				95.5					95.5																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1310	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.927	Sm	1	Ba	2	Cu	3															O	Z	6.927		1989																											3	Y123																				88.1					88.1																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1311	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.9	Sm	1	Ba	2	Cu	3															O	Z	6.9		1989																											3	Y123																				87					87																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1312	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.878	Sm	1	Ba	2	Cu	3															O	Z	6.878		1989																											3	Y123																				91.1					91.1																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1313	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.813	Sm	1	Ba	2	Cu	3															O	Z	6.813		1989																											3	Y123																				83.6					83.6																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1314	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.773	Sm	1	Ba	2	Cu	3															O	Z	6.773		1989																											3	Y123																				87.8					87.8																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1315	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.734	Sm	1	Ba	2	Cu	3															O	Z	6.734		1989																											3	Y123																				67.6					67.6																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1316	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.709	Sm	1	Ba	2	Cu	3															O	Z	6.709		1989																											3	Y123																				59.8					59.8																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1317	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.554	Sm	1	Ba	2	Cu	3															O	Z	6.554		1989																											3	Y123																				44.7					44.7																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1318	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3O6.467	Sm	1	Ba	2	Cu	3															O	Z	6.467		1989																											3	Y123																																																																			MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)																																																					0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1319	PRB0399203		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1989									6.324																		3	Y123																					90.53				90.53																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	3910																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1320	PRB0399203		LaBa2Cu3O7	La1Ba2Cu3OZ	La	1	Ba	2	Cu	3															O	Z			1989									6.577																		3	Y123																					47.73				47.73																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	10780																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1321	PRB0399203		NdBa2Cu3O7	Nd1Ba2Cu3OZ	Nd	1	Ba	2	Cu	3															O	Z			1989									6.746																		3	Y123																					87.63				87.63																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	8020																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1322	PRB0399203		SmBa2Cu3O7	Sm1Ba2Cu3OZ	Sm	1	Ba	2	Cu	3															O	Z			1989									6.853																		3	Y123																					92.33				92.33																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	6830																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1323	PRB0399203		EuBa2Cu3O7	Eu1Ba2Cu3OZ	Eu	1	Ba	2	Cu	3															O	Z			1989									6.88																		3	Y123																					93.83				93.83																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	6910																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1324	PRB0399203		DyBa2Cu3O7	Dy1Ba2Cu3OZ	Dy	1	Ba	2	Cu	3															O	Z			1989									7.057																		3	Y123																					91.23				91.23																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	5280																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1325	PRB0399203		HoBa2Cu3O7	Ho1Ba2Cu3OZ	Ho	1	Ba	2	Cu	3															O	Z			1989									7.095																		3	Y123																					89.43				89.43																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	5930																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1326	PRB0399203		ErBa2Cu3O7	Er1Ba2Cu3OZ	Er	1	Ba	2	Cu	3															O	Z			1989									7.139																		3	Y123																					91.1				91.1																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	3560																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1327	PRB0399203		TmBa2Cu3O7	Tm1Ba2Cu3OZ	Tm	1	Ba	2	Cu	3															O	Z			1989									7.186																		3	Y123																					90.1				90.1																																										MAGNETIZATION OF PARTICLE(ABOUT 10MICRON)	4090																																																				0						HIGH-TEMPERATURE RESISTIVITY OF RBA(2)CU(3)0(7-Y),WHERE R=LA,PR,ND,SM,EU,DY,HO,ER,AND TM	198905	RESISTIVITY         ,OXYGEN CONTENTS	DEPRTMENT OF PHYSICS,NATIONAL TAIWAN UNIVERSITY,TAIPEI,TAIWAN,REPUBRIC OF CHINA	PHYS.REV.B.,39(1989)9203	C.H.CHEN,H.C.CHEN,H.C.YANG,H.H.HORNG,H.H.SUNG,J.C.JAO,M.H.HSIEH,Y.S.KAN	SM,EU,DY,HO,ER,R,BA,CU,O	
1328	PR04011352		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-X	Bi	2	Sr	2	Ca	1	Cu	2													O	8-X		3	1989																												Bi2212																			83						83																																																																																											RH1328		3020000000000000000000	BI2O3,SRCO3,CACO3,CUO	0	5H AT 650C, FOLLOWED BY 12H RAMP TO 25C IN 1 ATM O2 FLOW					VARIABLE HALL COEFFICIENT IN BI2SR2CACU2O8-X ACROSS THE METAL-INSULATOR TRANSITION	198912	HALL COEFFICIENT    ,SINGLE-CRYSTAL      ,OXYGEN CONTENT      ,HALL MOBILITY	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA ATBERKELEY,ANDMATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11352	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
1329	PR04011352	1/RH=A+BT.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-X	Bi	2	Sr	2	Ca	1	Cu	2													O	8-X			1989																												Bi2212																				25					25																																																																																											RH1329		1050000000000000000000	BI2O3,SRCO3,CACO3,CUO	0	5H AT 650C, FOLLOWED BY 12H RAMP TO 25C IN 1 ATM O2 FLOW					VARIABLE HALL COEFFICIENT IN BI2SR2CACU2O8-X ACROSS THE METAL-INSULATOR TRANSITION	198912	HALL COEFFICIENT    ,SINGLE-CRYSTAL      ,OXYGEN CONTENT      ,HALL MOBILITY	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA ATBERKELEY,ANDMATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11352	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
1330	SSC0711079		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Y	Nd	1.85	Ce	0.15	Cu	1															O	4-Y		2	1989																											2	T'																			14	20.9	22.3				20.9																																																																			-1.49								24.5			36.7				9												ND2O3,CEO2,CUO	0	IMPURITY PHASE=NDCEO3.5,NDCE3O7.5,CU2O,CAL(950C 24H IN AIR)-SIN(1050C 48H IN O2)-ANN(900C 24H IN AIR)-Q TO RT					COMPOSITIONAL PROPERTIES AND THERMOELECTRIC POWER OF THE SUPERCONDUCTING CERAMIC ND2-XCEXCUO4-Y	198909	THERMOELECTRIC POWER,RES                 ,SUS	IBM RESEARCH DIVISION, ALMADEN RESEARCH CENTER SAN JOSE, CALIFORUNIA 95120-6099	SOLID STATE COMMUN.71(1989)1079	M. E. LOPEZ-MORALES,P. M. GRANT,R. J. SAVOR	ND,CE,CU,O	
1331	SSC0711099		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1989																												Y123																				91.5					91.5																																																																											0.082							0.27				0.00000000057			0.00000000145		RH1331		10000000000000000000000		0	GRAIN GROWTH					FLUX-FLOW HALL EFFECT IN YBA2CU3O7 AND BI2SR2CACU2O8 HIGH TEMPERATURE SUPERCONDUCTORS				SOLID STATE COMMUN.,71(1989)1099	A.HAMZIC,L.FORRO	Y,BA,CU,O,BI,SR,CA,	
1332	SSC0711099		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1989																												Bi2212																				82					82																																																																											0.048							0.19				0.00000000104			0.00000000153				5950000000000000000000		0	GRAIN GROWTH					FLUX-FLOW HALL EFFECT IN YBA2CU3O7 AND BI2SR2CACU2O8 HIGH TEMPERATURE SUPERCONDUCTORS				SOLID STATE COMMUN.,71(1989)1099	A.HAMZIC,L.FORRO	Y,BA,CU,O,BI,SR,CA,	
1333	SSC0710939		Y(Ba,Ca)2Cu3O7	Y1Ba1.9Ca0.1Cu3O6.84	Y	1	Ba	1.9	Ca	0.1	Cu	3													O	Z	6.84		1989																											3	Y123																				85					85																																																																																															0						CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
1334	SSC0710939		Y(Ba,Sr)2Cu3O7	Y1Ba1.9Sr0.1Cu3O6.89	Y	1	Ba	1.9	Sr	0.1	Cu	3													O	Z	6.89		1989																											3	Y123																				89					89																																																																																															0						CORRELATION BETWEEN ELECTRONIC STATES OF OXYGEN AND COPPER INY-BA-CU-O DOPED SYSTEMS		XPS                 ,OXYGEN CONTENTS     ,ELECTRONIC STATES	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA (USTC),HEFEI,ANHUI,CHINA	SOLID STATE COMMUN.71(1989)939	H. ZHANG,M. R. JI,Q. R. ZHANG,S. X. WANG,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,SR,CA,ZN,AL,SN	
1335	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.975Zn0.025O6.93	Y	1	Ba	2	Cu	2.975	Zn	0.025													O	Z	6.93	1	1989																											3	Y123																				82.8					82.8																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1336	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.95Zn0.05O6.94	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	Z	6.94	1	1989																											3	Y123																				73.9					73.9																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1337	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.925Zn0.075O6.94	Y	1	Ba	2	Cu	2.925	Zn	0.075													O	Z	6.94	1	1989																											3	Y123																				65					65																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1338	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.94	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	Z	6.94	1	1989																											3	Y123																				56.9					56.9																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1339	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.9	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	Z	6.9	1	1989																											3	Y123																																																																																																																								1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1340	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2O6.88	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	Z	6.88	1	1989																											3	Y123																				54.7					54.7																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1341	SSC0720075		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6.92	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	Z	6.92	1	1989																											3	Y123																				47.2					47.2																																																																																															1	930C QUENCH IN O2, OZ BY TGA					OXYGEN CONTENT IS NOT THE PROEDOMINANT FACTOR FOR HIGH TC SUPERCONDUCTIVITY IN Y-BA-CU-O SYSTEM	198910	OXYGEN CONTENT      ,TC	DEPARTMENT OF APPLIED CHEMISTRY, UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA(USTC), HEFEI, ANHUI, CHINA	SOLID STATE COMMUN. 72(1989)75	H. ZHANG,Q. R. ZHANG,S. H. LIU,X. Y. ZHOU,Y. ZHAO	Y,BA,CU,O,M,R	
1342	SSC0720085		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7-Z	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z		1	1989																											3	Y123																				91					91																																																2.9	2																																													Y2O3,BAO2,CUO,FE2O3	1						OBSERVATION OF AN ENERGY GAP IN THE FAR INFRARED SPECTRA OF IRON-DOPED YBA2CU3OX SUPERCONDUCTORS	198910	FAR INFRARED        ,REFLECTANCE         ,ENERGY GAP          ,OXYGEN CONTENT	MAX-PLANCE-INSTITUT FUR FESTKORPERFORSCHUNG HEISENBERGSTR. 1,7000 STUTTGART 80	SOLID STATE COMMUN.72(1989)85	A. JANSEN,C. RICHTER,E. SEIDER,L. GENZEL,M. BAUER,P. WYDER	Y,BA,CU,O,FE	
1343	SSC0720085		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18O7-Z	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	7-Z		1	1989																											2	Y123																				72.2					72.2																																																1.1	2																																													Y2O3,BAO2,CUO,FE2O3	1						OBSERVATION OF AN ENERGY GAP IN THE FAR INFRARED SPECTRA OF IRON-DOPED YBA2CU3OX SUPERCONDUCTORS	198910	FAR INFRARED        ,REFLECTANCE         ,ENERGY GAP          ,OXYGEN CONTENT	MAX-PLANCE-INSTITUT FUR FESTKORPERFORSCHUNG HEISENBERGSTR. 1,7000 STUTTGART 80	SOLID STATE COMMUN.72(1989)85	A. JANSEN,C. RICHTER,E. SEIDER,L. GENZEL,M. BAUER,P. WYDER	Y,BA,CU,O,FE	
1344	SSC0720273		Pr2NiO4	Pr2Ni1O4	Pr	2	Ni	1																	O	4		1	1989						3.73	-16.3																				3		BMAB			5.404	5.578	12.22																																																																																																																		1	BY REDUCING NONSTOICHIOMETRIC R2NI04+Z UNDER H FLOW AT 583K					MAGNETIC AND X-RAY DIFFRACTION CHARACTERIZATION OF STOICHIOMETRIC PR2NIO4 AND ND2NIO4OXIDES	198910	SRYSTAL STRUCTURE   ,ANTIFERROMAGNETIC   ,SUSCEPTIBILITY	DEPT. QULMICA LNORGANICA. FACULTAD CIENCIAS QULMICAS, UNIVERSIDAD COMPLUTENSE. E-28040. MADRID. SPAIN	SOLID STATE COMMUN.72(1989)273	F. FERNANDEZ,J. L. MARTINEZ,J. RODRIGUEZ CARVAJAL,R. SAEZ PUCHE	PR,NI,O,ND	
1345	SSC0720273		Nd2NiO4	Nd2Ni1O4	Nd	2	Ni	1																	O	4		1	1989						3.83	-17.9																				3		BMAB			5.381	5.585	12.114																																																																																																																		1	BY REDUCING NONSTOICHIOMETRIC R2NI04+Z UNDER H FLOW AT 583K					MAGNETIC AND X-RAY DIFFRACTION CHARACTERIZATION OF STOICHIOMETRIC PR2NIO4 AND ND2NIO4OXIDES	198910	SRYSTAL STRUCTURE   ,ANTIFERROMAGNETIC   ,SUSCEPTIBILITY	DEPT. QULMICA LNORGANICA. FACULTAD CIENCIAS QULMICAS, UNIVERSIDAD COMPLUTENSE. E-28040. MADRID. SPAIN	SOLID STATE COMMUN.72(1989)273	F. FERNANDEZ,J. L. MARTINEZ,J. RODRIGUEZ CARVAJAL,R. SAEZ PUCHE	PR,NI,O,ND	
1346	SSC0720117	HC1 MEASURED BY EPR X-BAND	(Y,Er)(Ba,Sr)2Cu3O7	Y0.9Er0.1Ba1.9Sr0.1Cu3O7-Z	Y	0.9	Er	0.1	Ba	1.9	Sr	0.1	Cu	3											O	7-Z		1	1989																												Y123																				88					88													190									83																15					1400																																																			CUO,Y2O3,BACO3,ER2O3,SR2CO3	1	CAL(800C 12H)-SIN(960C 7H IN O2)-C					ELECTRON PARAMAGNETIC RESONANCE OF THE HIGH-TC SUPERCONDUCTORY0.9ER0.1BA1.9SR0.1CU3O7-Z	198910	EPR                 ,JOSEPHSON JUNCTIONS ,CRITICAL FIELD      ,MICROWAVE ABSORPT	PHYSICS DEPARTMENT, CONCORDIA UNIVIRSITY, 1455 DE MAISONNEUVE.BLVD, WEST, MONTREAL,	SOLID STATE COMMUN.72(1989)117	L. E. MISIAK,S. K. MISRA	Y,ER,BA,SR,CU,O	
1347	SSC0720351	HC1 MEASURED BY EPR, X-BAND	(Y,Ho)Ba2Cu3O7	Y0.9Ho0.1Ba2Cu3O7-Z	Y	0.9	Ho	0.1	Ba	2	Cu	3													O	7-Z		1	1989																											3	Y123																				60					60												EPR MEASUREMENT	750								ESTIMATED FROM HC1	173																																																																									1						EPR STUDY OF HIGH-TC SUPERCONDUCTOR Y0.9HO0.1BA2CU3O7-Z	198910	EPR                 ,MICROWAVE ABSORPTION,CRITICAL FIELD      ,OXYGEN VACANCIES	PHYSICS DEPARTMENT, CONCORDIA UNIVERSITY, 1455 DE MAISONNEUVEBLVD. WEST, MONTREAL, QUEBEC, CANADA	SOLID STATE COMMUN.72(1989)351	L. E. MISIAK,S. K. MISRA	Y,HO,BA,CU,O	
1348	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.975Zn0.025O6.85	Y	1	Ba	2	Cu	2.975	Zn	0.025													O	7-Y	6.85	1	1989																											3	Y123																			72.85						72.85																																																																						TP1348																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1349	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.95Zn0.05O6.85	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Y	6.85	1	1989																											3	Y123																			66.19						66.19																																																																						TP1349																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1350	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.925Zn0.075O6.85	Y	1	Ba	2	Cu	2.925	Zn	0.075													O	7-Y	6.85	1	1989																											3	Y123																			63.6						63.6																																																																						TP1350																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1351	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.85	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	7-Y	6.85	1	1989																											3	Y123																			50.08						50.08																																																																						TP1351																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1352	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.85	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-Y	6.85	1	1989																											3	Y123																			47.6						47.6																																																																						TP1352																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1353	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2O6.85	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	7-Y	6.85	1	1989																											3	Y123																			30.69						30.69																																																																						TP1353																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1354	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6.85	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	7-Y	6.85	1	1989																												Y123																																																																																															TP1354																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1355	PRB0406850		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.6Zn0.4O6.85	Y	1	Ba	2	Cu	2.6	Zn	0.4													O	7-Y	6.85	1	1989																												Y123																																																																																															TP1355																									1						THERMOPOWER OF ZINC-DOPED Y-BA-CU-O	198910	THERMOPOWER         ,SINGLE PHASE        ,PHONON DRAG	LOW TEMPERATURE LABORATORY,DEPARTMENT OF PHYSICS,INDIA AND MATERIAL SCIENCE RESEARCH CENTER,INDIAN INSTITUTE OF TECHNOLOGY,MADRAS 600036,INDIA	EATCH CENTER,IN	C.K.SUBRAMANIAM,G.V.SUBBA RAO,R,SRINIVASAN,V.SANKARANARAYANAN,VIJAYASHREE RADHAKRISHNAN	Y,BA,CU,ZN,O	
1356	PR0408861		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																																																																														SP1356				28.4		322																																				1	<2% CUO ,SIN(975C IN O2)					THERMAL EXPANSIVITY BELOW 300 K AND LOW-TEMPERATURE HEAT CAPACITY OF YBA2CU3O7	198911	THEMAL EXPANSIVITIES,HEAT CAPACITIES     ,LATTICE SOFTENING   ,ELASTIC CONSTANTS	AMES LABORATORY,U.S.DEPARTMET OF ENERGY,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)8861	C.A.SWENSON,K.NO,R.W.MCCALLUM	Y,BA,CU,O	
1357	PR0408861		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																																																																														SP1357				8.2		415																																				1	<2% CUO ,SIN(975C IN O2)					THERMAL EXPANSIVITY BELOW 300 K AND LOW-TEMPERATURE HEAT CAPACITY OF YBA2CU3O7	198911	THEMAL EXPANSIVITIES,HEAT CAPACITIES     ,LATTICE SOFTENING   ,ELASTIC CONSTANTS	AMES LABORATORY,U.S.DEPARTMET OF ENERGY,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)8861	C.A.SWENSON,K.NO,R.W.MCCALLUM	Y,BA,CU,O	
1358	PR0408861		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																																																																														SP1358				5.74		435																																				1	<2% CUO ,SIN(975C IN O2)					THERMAL EXPANSIVITY BELOW 300 K AND LOW-TEMPERATURE HEAT CAPACITY OF YBA2CU3O7	198911	THEMAL EXPANSIVITIES,HEAT CAPACITIES     ,LATTICE SOFTENING   ,ELASTIC CONSTANTS	AMES LABORATORY,U.S.DEPARTMET OF ENERGY,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)8861	C.A.SWENSON,K.NO,R.W.MCCALLUM	Y,BA,CU,O	
1359	SSC0720089		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.8Ni0.2O7	Y	1	Ba	2	Cu	2.8	Ni	0.2													O	7		1	1989																												Y123																				63.5				1.5	63.5																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1360	SSC0720089		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.12O7	Y	1	Ba	2	Cu	2.88	Ni	0.12													O	7		1	1989																												Y123																				74.3				0.8	74.3																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1361	SSC0720089		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.75Ni0.25O7	Y	1	Ba	2	Cu	2.75	Ni	0.25													O	7		1	1989																												Y123																				54				1.5	54																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1362	SSC0720089		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.72Ni0.28O7	Y	1	Ba	2	Cu	2.72	Ni	0.28													O	7		1	1989																												Y123																				51				1.6	51																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1363	SSC0720089		YBa2(Cu,Co)3O7	Y1Ba2Cu2.89Co0.11O7	Y	1	Ba	2	Cu	2.89	Co	0.11													O	7		1	1989																												Y123																				64				4	64																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1364	SSC0720089		YBa2(Cu,Co)3O7	Y1Ba2Cu2.82Co0.18O7	Y	1	Ba	2	Cu	2.82	Co	0.18													O	7		1	1989																												Y123																				46				5	46																																																																																														Y2O3,BACO3,CUO,NI OR CO OXIDE	0	CAL(900C 24H IN AIR)-ANN(600C 6H IN AIR)-FC					EFFECTIVE CONCENTRATION OF CO AND NI IMPURITIES AND THEIR INFLUENCE ON THE SUPERCONDUCTING YBA2 CU3 O7 COMPOUND	198910	SQUID               ,TC                  ,SUS                 ,EPMA	INSTITUT D'ELECTRONIQUE FONDAMENTALE, BATIMENT 220, URA 022, UNIVERSITE PARIS SUD, F91405-ORSAY	SOLID STATE COMMUN.72(1989)89	E. VELU,J. P. RENARD,K. LE DANG,R. LAVAL	Y,VA,CU,O,CO,NI	
1365	SSC0680331		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X		3	1988																											3	Bi2212				5.14	5.42	30.78													86						86														450	2800																																			150000																																												BI2O3,SR(NO3)2,CACO3,CUO	5	MELT(1025C 16H)-COOL TO 925C(80C/H)-HOLD(8H)-COOL TO 835C(1C/H)-COOL TO RT(10C/H)					ANISOTROPIC MAGNETIZATION IN SINGLE CRYSTAL BI(2)SR(2)CA(1)CU(2)O(Y)	198810	SINGLE CRYSTAL           ,ANISOTROPY               ,MAG                      ,HC	INSTITUTE OF PHYSICS,ACADEMIA SINICA,BEIJING,CHINA	SOLID STATE COMMUN.,68(1988)331	CHANG-GENG CUI,HONG YIN,JI-HONG WANG,JIN-LONG ZHANG,KE-CHEN WU,SHAN-LIN LI,YI-FENG YAN	BI,SR,CA,CU,O	
1366	PRB0385102		Bi2Sr2(Ca,Bi)Cu2O8	Bi2.2Sr2Ca0.8Cu2O8+Z	Bi	2.2	Sr	2	Ca	0.8	Cu	2													O	8+Z		3	1988																												Bi2212																																														RESISTIVE		44	2640								45	0.75						27	0.45																																											0.22												5						ANGULAR DEPENDENCE OF THE UPPER CRITICAL FIELD OF BI(2.2)SR(2)CA(0.8)CU(2)O(8+Z)	198809	ANISOTROPY               ,RES                      ,HC	AT&T BELL LABORATORIES,600 MOUNTAIN AVENUE,MURRAY HILL,NEW JERSEY	PHYS.REV.B,38(1988)5102	B.BATLOGG,J.V.WASZCZAK,L.F.SCHNEEMEYER,R.B.VAN DOVER,T.T.M.PALSTRA	BI,SR,CA,CU,O	
1367	PRB0392936	single crystal.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1989																												Y123																			91	89.5					89.5												DEVIATION FROM LINEAR MAGNETIZATION		180	530																								13	2				1300	4500																																																		0	not described					TEMPERATURE DEPENDENCE OF LOWER CRITICAL FIELDS IN Y-BA-CU-O CRYSTALS	198902	ANISOTROPY               ,LOWER CRITICAL FIELD     ,SINGLE CRYSTAL           ,MA	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,39(1989)2936	A.P.MALOZEMOFF,D.C.CRONEMEYER,F.HOLTZBERG,L.KRUSIN-ELBAUM,Y.YESHURUN	Y,BA,CU,O	
1368	PLA1280283		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																												Y123						11.71													81						81																																3.12	0.32						44.8	4.6																																											0.6																		RESISTIVITY AND UPPER CRITICAL FIELD ANISOTROPY IN Y(1)BA(2)CU(3)O(7-Z) SINGLE CRYSTALS	198804	SINGLE CRYSTAL           ,ANISOTROPY               ,CRITICAL	CENTRE D'ETUDES NUCLEAIRES DE GRENOBLE,DEPARTEMENT DE RECHERCHE FONDAMENTALE,FRANCE	PHYS.LETT.A,128(1988)283	C.AYACHE,J.Y.HENRY,L.FORRO,P.STAMP	Y,BA,CU,O	
1369	PRB0380252		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																												Y123																			91						91																					RESISTIVE		210	35								3.3	0.56						31	5.1																																																						Y2O3,BACO3,CUO	5	CUO FLUX METHOD					ANISOTROPIC SUPERCONDUCTING PROPERTIES OF BA(2)Y(1)CU(3)O(7-Y)	198807	HC                       ,SINGLE CRYSTAL           ,ANISOTRO	NTT OPTO-ELECTRONICS LABORATORIES,IBARAKI,JAPAN	PHYS.REV.B,38(1988)252	M.ODA,M.SUZUKI,T.MURAKAMI,Y.HIDAKA	Y,BA,CU,O	
1370	SSC0670609		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1988																											3	Bi2212				5.4	27.01	30.82													90						90																																																																																		0.45												BI2O3,SRCO3,CACO3,CUO	1	HEAT(900C 2H IN PT)-C(5C/H) TO 800C-FC					ANISOTROPY OF THE SUPERCONDUCTING PROPERTIES OF Bi2Sr2CaCu2O8			Service National des Champs Intenses, Centre National de la Recherche Scientifique, BP 166 X, 38042 Grenoble-Ce'dex, France	Solid State Commun.,67(1988)609-611	H. Noel,J. Padiou,J.C. Levet,M. Potel,O. Laborde,P. Gougeon,P. Monceau		
1371	ZPB0690151		Y(Ba,K)2Cu3O7	Y1Ba1.9K0.1Cu3O6.9	Y	1	Ba	1.9	K	0.1	Cu	3													O	6.9	6.9	1	1987																											3	Y123																					91.5				91.5																																																									7.74		397																																										A SPEDIFIC HEAT AND MAGNETIZATION STUDY OF HIGH TC CERAMIC SUPERCONDUCTORS			RUHR-UNIVERSITAT BOCHUM, EXPERIMENTALPHYSIK VI, BOCHUM, FEDERAL REPUBLIC JOF GERMANY	Z.PHYS.B,69(1987)151	H.SABROWSKY,M.MITTAG,M.ROSENBERG,R.JOB,R.NEUBARER,R.WERNHARBT,W.CHOJETZKI	LA,SR,CU,O,Y,BA	
1372	ZPB0690151		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1987																												T																																																																														SP1372						396																																										A SPEDIFIC HEAT AND MAGNETIZATION STUDY OF HIGH TC CERAMIC SUPERCONDUCTORS			RUHR-UNIVERSITAT BOCHUM, EXPERIMENTALPHYSIK VI, BOCHUM, FEDERAL REPUBLIC JOF GERMANY	Z.PHYS.B,69(1987)151	H.SABROWSKY,M.MITTAG,M.ROSENBERG,R.JOB,R.NEUBARER,R.WERNHARBT,W.CHOJETZKI	LA,SR,CU,O,Y,BA	
1373	ZPB0690151		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1987																												T																				37.2					37.2																															0.85																										4.02		394																																										A SPEDIFIC HEAT AND MAGNETIZATION STUDY OF HIGH TC CERAMIC SUPERCONDUCTORS			RUHR-UNIVERSITAT BOCHUM, EXPERIMENTALPHYSIK VI, BOCHUM, FEDERAL REPUBLIC JOF GERMANY	Z.PHYS.B,69(1987)151	H.SABROWSKY,M.MITTAG,M.ROSENBERG,R.JOB,R.NEUBARER,R.WERNHARBT,W.CHOJETZKI	LA,SR,CU,O,Y,BA	
1374	TH1531507		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123																			90		92			0.5	91																																																																																																					On the influence of the heat treatment on the diamagnetic and thermodynamic properties of sintered YBa2Cu3O7				PHYSICA C,153-155(1988)1507			
1375	PHC1531089		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123				3.817	3.884	11.68																																																																								SP1375				4.2		371																																										SPECIFIC HEAT STUDY ON BA2YCU3O7 SAMPLES WITH A DOUBLE SUPERCONDUCTING TRANSITION			INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA C,153-155(1988)1089	A.KISHI,A.MAESONO,M.ISHIKAWA,R.KATO,T.TAKABATAKE,Y.NAKAZAWA	BA,Y,CU,O	
1376	PHC1531092		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123																				92					92																						160																															SP1376				6.95		457																																										SPECIFIC HEAT OF BYA2CU3O7			MATERIALS AND CHEMICAL SCIENCE DIVISION, LAWRENCE BERKELEY LABORATORY, UNIVERSITY OF CALIFORNIA, BERKELEY, CA 94720, USA	PHYSICA C,153-155(1988)1092	A.M.STACY,J.E.GORDON,N.E.PHILLIPS,R.A.FISHER,S.KIM	Y,BA,CU,O	
1377	PHB1480332	TETRA-I	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																											2	Y123				3.87		11.63																																																																																																																								CHARACTERIZATION OF THE HIGH-TX PHASE AND ITS METAMORPHIC PHASES, BA2YCU3O7-Z			INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA B,148(1987)332	M.ISHISAWA,T.TAKABATAKE,Y.NAKAZAWA	BA,Y,CU,O	
1378	PHB1480332	TETRA-II	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1987																											2	Y123				3.864		11.803																																																																								SP1378																																																CHARACTERIZATION OF THE HIGH-TX PHASE AND ITS METAMORPHIC PHASES, BA2YCU3O7-Z			INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA B,148(1987)332	M.ISHISAWA,T.TAKABATAKE,Y.NAKAZAWA	BA,Y,CU,O	
1379	PHB1480332	ORTHO-I	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123				3.825	3.893	11.676																																																																								SP1379				8																					0.35				0.82																			CHARACTERIZATION OF THE HIGH-TX PHASE AND ITS METAMORPHIC PHASES, BA2YCU3O7-Z			INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA B,148(1987)332	M.ISHISAWA,T.TAKABATAKE,Y.NAKAZAWA	BA,Y,CU,O	
1380	PHB1480332	ORTHO-II	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123				3.846	3.883	11.763																																																																								SP1380				8																					44				12																			CHARACTERIZATION OF THE HIGH-TX PHASE AND ITS METAMORPHIC PHASES, BA2YCU3O7-Z			INSTITUTE FOR SOLID STATE PHYSICS, UNIVERSITY OF TOKYO, ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA B,148(1987)332	M.ISHISAWA,T.TAKABATAKE,Y.NAKAZAWA	BA,Y,CU,O	
1381	PHC1580102		Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4			1989						3.68	-61																						I4/MMM																																																																													SP1381				2.6		361																																				0	PBO,CUO FLUX,PB<1% IF ANY,NO MAGNETIC ORDER :GROWN FROM PBO- AND CUO-BASED FLUX					SPECIFIC HEAT AND ANISOTROPIC MAGNETIC SUSCEPTIBILITY OF PR(2)CUO(4),ND(2)CUO(4) AND SM(2)CUO(4) CRYSTALS	198904	SINGLE CRYSTAL           ,ANTIFERROMAGNETIC ORDER  ,ANISOTRO	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO 87545,USA	PHYSICA C ,158(1989)102	J.D.THOMPSON,M.F.HUNDLEY,S-W.CHEONG,S.B.OSEROFF,Z.FISK	PR,CU,O,ND,SM	
1382	PHC1580102		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4			1989						3.56	-62	1																																																																																																		SP1382						319																																				0	PBO,CUO FLUX,PB<1% IF ANY,NO MAGNETIC ORDER :GROWN FROM PBO- AND CUO-BASED FLUX					SPECIFIC HEAT AND ANISOTROPIC MAGNETIC SUSCEPTIBILITY OF PR(2)CUO(4),ND(2)CUO(4) AND SM(2)CUO(4) CRYSTALS	198904	SINGLE CRYSTAL           ,ANTIFERROMAGNETIC ORDER  ,ANISOTRO	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO 87545,USA	PHYSICA C ,158(1989)102	J.D.THOMPSON,M.F.HUNDLEY,S-W.CHEONG,S.B.OSEROFF,Z.FISK	PR,CU,O,ND,SM	
1383	PHC1580102	SP FITTING RANGE:15< T<25K	Sm2CuO4	Sm2Cu1O4	Sm	2	Cu	1																	O	4			1989								5.95																				T'																																																																														SP1383				164		353																																				0	PBO,CUO FLUX,PB<1% IF ANY,NO MAGNETIC ORDER :GROWN FROM PBO- AND CUO-BASED FLUX					SPECIFIC HEAT AND ANISOTROPIC MAGNETIC SUSCEPTIBILITY OF PR(2)CUO(4),ND(2)CUO(4) AND SM(2)CUO(4) CRYSTALS	198904	SINGLE CRYSTAL           ,ANTIFERROMAGNETIC ORDER  ,ANISOTRO	LOS ALAMOS NATIONAL LABORATORY,LOS ALAMOS,NEW MEXICO 87545,USA	PHYSICA C ,158(1989)102	J.D.THOMPSON,M.F.HUNDLEY,S-W.CHEONG,S.B.OSEROFF,Z.FISK	PR,CU,O,ND,SM	
1384	LTP0730241		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				92					92																																																					SP1384			mJ/mol.K2	13.8		356																																				1						Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1385	LTP0730241		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				92					92																																																					SP1385			mJ/mol.K2	11.7		387																																				1						Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1386	LTP0730241		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				90.5					90.5																																																					SP1386			mJ/mol.K2	3.9		392																																				1						Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1387	PHC1590215	FITTING C=AT**(-2)+BT**3+CT**5+DT**7	Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3OX	Tl	2	Ba	2	Ca	2	Cu	3													O	X		2	1989																											2	Tl2223																				125	129			9.8	125										24																																																	290																																				1						SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
1388	PHC1590215	FITTING C=AT**(-2)+BT**3+CT**5+DT**7	Tl2Ba2CaCu2Oz	Tl2Ba2Ca1Cu2OX	Tl	2	Ba	2	Ca	1	Cu	2													O	X		1	1989																											2	Tl2212																				101	106			8.8	101										51																																											SP1388				6.8		254																																				1						SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
1389	SP1590215	FITTING C=AT**(-2)+BT**3+CT**5+DT**7	Tl2Ba2CuOz	Tl2Ba2Cu1OX	Tl	2	Ba	2	Cu	1															O	X		1	1989		-17340000000000000000000000																									2	Tl2201																					10				10																																																					SP1389						238																																				1						SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
1390	PHC1590215		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																				89.9				0.8	89.9										65																																															4		438																																				1						SPECIFIC HEAT(1-330 K),MEISSNER EFFECT AND MAGNETIC SUSCEPTIBILITY OF TL(2)BA(2)CA(2)CU(3)O(10),TL(2)BA(2)CACU(2)O(8) AND TL(2)BA(2)CUO(6) CERAMIC SAMPLES	198906	SPECIFIC HEAT       ,SUSCEPTIBILITY      ,MEISSNER EFFECT	DEPARTMENT DE PHYSIOUE DE LA MATIERE CONDENSEE,UNIVERSITE DE GENEVE,CH-1211 GENEVE 4,SWIZERLAND	PHYSICA C.,159(1989)215	A.JUNOD,D.ECKERT,G.TRISCONE,J.MULLER,V.Y.LEE	TL,BA,CA,CU,O	
1391	PHC1520495		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1988									5.74																		3	Y123				3.818	3.887	11.676														91.4				1.8	91.4										66																																											SP1391				10.6		457																																			CUO,Y2O3,BACO3,FE2O3	1	CITRATE PYROLYSIS TECHNIQUE,DISSOLVED IN HOT H2NO3-MIXTURE-CAL(950C 14H)-SIN(980C 17H IN O2)-C(50C/H) TO RT					SPECIFIC HEAT, MAGNETIC SUSCEPTIBILITY AND SUPERCONDUCTIVITY OF YBA2CU3O7-Z DOPED WITH IRON				PHYSICA C,152(1988)495	BEZINGE.A,ECKERT.D,GRAF.T,JUNOD.A,MULLER.J		
1392	PHC1520495	MOMENT PER FE ATOM	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7		1	1988						4.07																					3	Y123				3.825	3.885	11.683														91.2				1	91.2										66																																											SP1392																																									CUO,Y2O3,BACO3,FE2O3	1	CITRATE PYROLYSIS TECHNIQUE,DISSOLVED IN HOT H2NO3-MIXTURE-CAL(950C 14H)-SIN(980C 17H IN O2)-C(50C/H) TO RT					SPECIFIC HEAT, MAGNETIC SUSCEPTIBILITY AND SUPERCONDUCTIVITY OF YBA2CU3O7-Z DOPED WITH IRON				PHYSICA C,152(1988)495	BEZINGE.A,ECKERT.D,GRAF.T,JUNOD.A,MULLER.J		
1393	PHC1520495	MOMENT PER FE ATOM	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O7	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7		1	1988						4.07																					3	Y123				3.834	3.881	11.681														89.3				1.7	89.3										47																																											SP1393																																									CUO,Y2O3,BACO3,FE2O3	1	CITRATE PYROLYSIS TECHNIQUE,DISSOLVED IN HOT H2NO3-MIXTURE-CAL(950C 14H)-SIN(980C 17H IN O2)-C(50C/H) TO RT					SPECIFIC HEAT, MAGNETIC SUSCEPTIBILITY AND SUPERCONDUCTIVITY OF YBA2CU3O7-Z DOPED WITH IRON				PHYSICA C,152(1988)495	BEZINGE.A,ECKERT.D,GRAF.T,JUNOD.A,MULLER.J		
1394	PHC1520495	MOMENT PER FE ATOM	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7		1	1988						3.96																					2	Y123				3.863		11.685														77.3				13	77.3										14																																											SP1394																																									CUO,Y2O3,BACO3,FE2O3	1	CITRATE PYROLYSIS TECHNIQUE,DISSOLVED IN HOT H2NO3-MIXTURE-CAL(950C 14H)-SIN(980C 17H IN O2)-C(50C/H) TO RT					SPECIFIC HEAT, MAGNETIC SUSCEPTIBILITY AND SUPERCONDUCTIVITY OF YBA2CU3O7-Z DOPED WITH IRON				PHYSICA C,152(1988)495	BEZINGE.A,ECKERT.D,GRAF.T,JUNOD.A,MULLER.J		
1395	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									5.24																		3	Y123																				90.5					90.5																																																									6.96		413																			0.665																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1396	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									5.39																		3	Y123																				92					92																																																									7.53		439																			0.401																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1397	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									5.2																		3	Y123																				91.5					91.5																																																									6.65		435																			0.695																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1398	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									4.48																		3	Y123																				95					95																																																									7.51		426																			6.89																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1399	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									4.37																		3	Y123																																																																																		5.6		330																																			Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1400	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									4.13																		3	Y123																				91					91																																																									11.5		431																			12.85																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1401	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									4.49																		3	Y123																				92					92																																																									5.63		427																			4.7																Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1402	PHC1520401	FITTING C=AT**(-2)+BT +CT**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988									4.38																		3	Y123																																																																																		4.47		333																																			Y2O3,BACO3,CUO	1	SINTER 945C,13H-ANNEAL 350C,10H IN AIR					THE HEAT CAPACITY OF YBA2CU3O7 AND YBA2CU3O6 IN RTHE RANGE 0.4TO 20 K: EVIDENCE FOR AN INTRINSIC T-TERM				PHYSICA C,152(1988)401	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,WELSH.H.K		
1403	PHC1520065		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1403				5.5		391																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1404	PHC1520065		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1404				5.5		391																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1405	PHC1520065		SmBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1405						350																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1406	PHC1520065		LuBa2Cu3O7	Lu1Ba2Cu3O7-Z	Lu	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1406				5.5		292																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1407	PHC1520065		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1407				5.5		316																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1408	PHC1520065		YbBa2Cu3O7	Yb1Ba2Cu3O7-Z	Yb	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1408				5.5		316																																				1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1409	PHC1520065		HoBa2Cu3O7	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1409																																										1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1410	PHC1520065		DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1410																																										1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1411	PHC1520065		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1411																																										1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1412	PHC1520065		TmBa2Cu3O7	Tm1Ba2Cu3O7-Z	Tm	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1412																																										1						LOW-TEMPRETURE SPECIFIC HEAT OF REBA2CU3O7 IN MAGNETIC FIELDSUP TO 5T(RE=Y,PR,SM,EU,GD,DY,HO,ER,TM,YB AND LU)				PHYSICA C,152(1988)65	BANDER MEULEN.H.P,FRANSE.J.J.M,KADOWAKI.K,KLASSE.P.C.P,MENOVSKY.A.A,TARNAWSKI.Z		
1413	PHC1560395	FITTING C(H)/T=A(H)*T**(-3)+B(H)+D*T**2+E*T**4,D=1944NTD**3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7-Z	7	1	1988																											3	Y123				3.823	3.895	11.694														91					91																																																					SP1413				5.1		443																																			Y2O3,BACO3,CUO	1	SIN(930C 12H IN AIR)-SIN(930C 15H IN AIR)-OXYGEN CONTROL(Q,ANN(IN N2),ANN(690C))					SPECIFIC HEAT OF YBA2CU3O7-Z AND BACUO2+C IN MAGNETIC FIELDS UP TO 6 T				PHYSICA C,156(1988)	HIRAGA.K,KIKUCHI.M,KOBAYASHI.N,LIU.A,MUTO.Y,NAKATSU.O,SASAKI.T,SYONO.Y,TOKIWA.A		
1414	PHC1560395		YBa2Cu3O7	Y1Ba2Cu3O6.31	Y	1	Ba	2	Cu	3															O	7-Z	6.31	1	1988																											2	Y123				3.859		11.711																																																																								SP1414				10		394																																			Y2O3,BACO3,CUO	1	SIN(930C 12H IN AIR)-SIN(930C 15H IN AIR)-OXYGEN CONTROL(Q,ANN(IN N2),ANN(690C))					SPECIFIC HEAT OF YBA2CU3O7-Z AND BACUO2+C IN MAGNETIC FIELDS UP TO 6 T				PHYSICA C,156(1988)	HIRAGA.K,KIKUCHI.M,KOBAYASHI.N,LIU.A,MUTO.Y,NAKATSU.O,SASAKI.T,SYONO.Y,TOKIWA.A		
1415	PHC1560395		YBa2Cu3O7	Y1Ba2Cu3O6.09	Y	1	Ba	2	Cu	3															O	7-Z	6.09	1	1988																											2	Y123				3.856		11.833																																																																								SP1415				4.1		354																																			Y2O3,BACO3,CUO	1	SIN(930C 12H IN AIR)-SIN(930C 15H IN AIR)-OXYGEN CONTROL(Q,ANN(IN N2),ANN(690C))					SPECIFIC HEAT OF YBA2CU3O7-Z AND BACUO2+C IN MAGNETIC FIELDS UP TO 6 T				PHYSICA C,156(1988)	HIRAGA.K,KIKUCHI.M,KOBAYASHI.N,LIU.A,MUTO.Y,NAKATSU.O,SASAKI.T,SYONO.Y,TOKIWA.A		
1416	PHC1560395		Y(Ba,Y)2Cu3O7	Y1.1Ba1.9Cu3O7-Z	Y	1.1	Ba	1.9	Cu	3															O	7-Z		1	1988																											3	Y123																				91					91																																																					SP1416				6.2		440																																			Y2O3,BACO3,CUO	1	SIN(930C 12H IN AIR)-SIN(930C 15H IN AIR)-OXYGEN CONTROL(Q,ANN(IN N2),ANN(690C))					SPECIFIC HEAT OF YBA2CU3O7-Z AND BACUO2+C IN MAGNETIC FIELDS UP TO 6 T				PHYSICA C,156(1988)	HIRAGA.K,KIKUCHI.M,KOBAYASHI.N,LIU.A,MUTO.Y,NAKATSU.O,SASAKI.T,SYONO.Y,TOKIWA.A		
1417	PHC1560395			Ba1Cu1O2+X	Ba	1	Cu	1																	O	2+X		1	1988																																																																																																										SP1417				98																																					Y2O3,BACO3,CUO	1	SIN(930C 12H IN AIR)-SIN(930C 15H IN AIR)-OXYGEN CONTROL(Q,ANN(IN N2),ANN(690C))					SPECIFIC HEAT OF YBA2CU3O7-Z AND BACUO2+C IN MAGNETIC FIELDS UP TO 6 T				PHYSICA C,156(1988)	HIRAGA.K,KIKUCHI.M,KOBAYASHI.N,LIU.A,MUTO.Y,NAKATSU.O,SASAKI.T,SYONO.Y,TOKIWA.A		
1418	PHC1520424		YBa2Cu3O7	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	6.5	6.5	1	1988																											3	Y123				3.834	3.873	11.738														50					50																															1.5																						SP1418				4		359																																				1	SINTERING-QUENCH,PREFERRED ORIENTATION , (885-900C)-SIN(920C 50H IN AIR)-C TO 690C-ANN(690C 24H)-Q-ANN(600-300C 6DAYS IN EVAC. TUBE)					SUPERCONCDUCTING AND MAGNETIC PROPERTIES OF THE OXYGEN-VACANCYORDERED ORTHO-2 PHASE OF BA2YCU3O6.5				PHYSICA C,152(1988)424	ISHIKAWA.M,K,KOGA,NAKAZAWA.Y,TAKABATAKE.T		
1419	PHB1480305		YBa2Cu3O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	7-Z	6.92	1	1987																											3	Y123																				91					91																																																					SP1419				10		350																																			BACO3,CUO,Y2O3	1	ANNEAL 480C,1.2BAR O2 , (950C 12H IN AIR)-Q-ANN(480C IN 1.2BAR O2)-C(WITHIN 12H) TO RT					SPECIFIC HEAT, SUSCEPTIBILITY AND RESISTIVITY MEASUREMENTS OFHIGH-TC SUPERCONDUCTORS YBA2CU3O7-X			DEPARTMENT DE RECHERCHE FONDAMENTALE, C.E.N. GRENOBLE, 85X-38041 GRENOBLE CEDEX, FRANCE	PHYSICA B,148(1987)305	B.BARBARA,C.AYACHE,E.BONJOUR,J.ROSSAT-MIGNOD,J.Y.HENRY,M.COUACH,M.J.G.M.JURGENS,P.BURLET,R.CALEMCZUK	Y,BA,CU,O	
1420	PHB1480305		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	7-Z	6	1	1987																											2	Y123				3.857		11.83																																																																								SP1420				10		350																																			BACO3,CUO,Y2O3	1	ANNEAL 480C,1.2BAR O2 , (950C 12H IN AIR)-Q-ANN(480C IN 1.2BAR O2)-C(WITHIN 12H) TO RT					SPECIFIC HEAT, SUSCEPTIBILITY AND RESISTIVITY MEASUREMENTS OFHIGH-TC SUPERCONDUCTORS YBA2CU3O7-X			DEPARTMENT DE RECHERCHE FONDAMENTALE, C.E.N. GRENOBLE, 85X-38041 GRENOBLE CEDEX, FRANCE	PHYSICA B,148(1987)305	B.BARBARA,C.AYACHE,E.BONJOUR,J.ROSSAT-MIGNOD,J.Y.HENRY,M.COUACH,M.J.G.M.JURGENS,P.BURLET,R.CALEMCZUK	Y,BA,CU,O	
1421	PHB1480305		YBa2Cu3O7	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	7-Z	6.66	1	1987																											3	Y123																				50					50																																																					SP1421				10		350																																			BACO3,CUO,Y2O3	1	ANNEAL 480C,1.2BAR O2 , (950C 12H IN AIR)-Q-ANN(480C IN 1.2BAR O2)-C(WITHIN 12H) TO RT					SPECIFIC HEAT, SUSCEPTIBILITY AND RESISTIVITY MEASUREMENTS OFHIGH-TC SUPERCONDUCTORS YBA2CU3O7-X			DEPARTMENT DE RECHERCHE FONDAMENTALE, C.E.N. GRENOBLE, 85X-38041 GRENOBLE CEDEX, FRANCE	PHYSICA B,148(1987)305	B.BARBARA,C.AYACHE,E.BONJOUR,J.ROSSAT-MIGNOD,J.Y.HENRY,M.COUACH,M.J.G.M.JURGENS,P.BURLET,R.CALEMCZUK	Y,BA,CU,O	
1422	PHB1480442	GAMMA FROM KAIZERO=36.0 DIAMAG CORRECTION	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7	6.95	1	1987																											3	Y123				3.824	3.886	11.676														91				0.9	91																																																					SP1422				5.53		389																			0.127				0.35													1	<1% BACUO2,BAO,Y2O3 , STANDARD CERAMICS TECHNIQUE					PHYSICAL PROPERTIES OF SINGLE-PHASE HIGH-TC SUPERCONDUCTOR YBA2CU3O7			NATUURKUNDIG LABORATORIUM DER UNIVERSITEIT VAN AMSTERDAM, VALCKENIERSTRAAT 65, 1018 XE, AMSTERDAM, THE NETHERLANDS	PHYSICA B,148(1987)442	A.A.MENOVSKY,A.SCHUIJFF,H.BARTEN,H.P.VAN DER MEULEN,J.C.P.KLAASSE,J.C.VAN MILTENBURG,J.J.M.FRANSE,J.Q.A.KOSTER,K.KADOWAWKI,M.VAN SPRANG,P.W.LEDNOR,R.DE RUITER,T.T.M.PALSTRA,Y.K.HUANG,Z.TARNAWSKI	Y,BA,CU,O	
1423	PHB1480360	FITTING C(H)=A(H)/T**2+B(H)*T+B3*T**3+B5*T**5	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																					92			8	92																																																					SP1423				7.1		430																																				1						SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS (LA,M)2CUO4 AND YBA2CU3O7 IN MAGNETIC FIELDS			MATERIALS AND CHEMICAL SCIENCES, LAWRENCE BERKELEY, UNIVERSITYOF CALIFORNIA, BERKELEY, CA 94720, USA	PHYSICA B,148(1987)360	A.M.STACY,C.MARCENAT,F.A.OLSEN,J.E.GORDON,M.L.TAN,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,W.K.HAM	LA,CA,CU,O,SR,Y,BA	
1424	PHB1480155		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123																																																																																		8.2		161																																				1						RBA2CU3O7-Z (R=RARE EATTH) HIGH-TC MAGNETIC SUPERCONDUCTORS			DEPARTMENT OF PHYDICS AND INSTUTUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093, USA	PHYSICA B,148(1987)155	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,M.V.KURIC,R.P.GUERTIN,R.R.HAKE,Y.DALICHAOUCH	R,BA,CU,O	
1425	PHB1480155		HoBa2Cu3O7	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123																																																								2.4																																																																1						RBA2CU3O7-Z (R=RARE EATTH) HIGH-TC MAGNETIC SUPERCONDUCTORS			DEPARTMENT OF PHYDICS AND INSTUTUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093, USA	PHYSICA B,148(1987)155	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,M.V.KURIC,R.P.GUERTIN,R.R.HAKE,Y.DALICHAOUCH	R,BA,CU,O	
1426	PHB1480155		TmBa2Cu3O7	Tm1Ba2Cu3O7-Z	Tm	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123																																																								2.8																																																																1						RBA2CU3O7-Z (R=RARE EATTH) HIGH-TC MAGNETIC SUPERCONDUCTORS			DEPARTMENT OF PHYDICS AND INSTUTUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093, USA	PHYSICA B,148(1987)155	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,M.V.KURIC,R.P.GUERTIN,R.R.HAKE,Y.DALICHAOUCH	R,BA,CU,O	
1427	PHB1480155		YbBa2Cu3O7	Yb1Ba2Cu3O7-Z	Yb	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123																																																								2.7																																																																1						RBA2CU3O7-Z (R=RARE EATTH) HIGH-TC MAGNETIC SUPERCONDUCTORS			DEPARTMENT OF PHYDICS AND INSTUTUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093, USA	PHYSICA B,148(1987)155	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,M.V.KURIC,R.P.GUERTIN,R.R.HAKE,Y.DALICHAOUCH	R,BA,CU,O	
1428	PHB1480155		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123																																																								2.86																										12.9		370																																				1						RBA2CU3O7-Z (R=RARE EATTH) HIGH-TC MAGNETIC SUPERCONDUCTORS			DEPARTMENT OF PHYDICS AND INSTUTUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093, USA	PHYSICA B,148(1987)155	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,M.V.KURIC,R.P.GUERTIN,R.R.HAKE,Y.DALICHAOUCH	R,BA,CU,O	
1429	PRB0368816		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X		1	1987																											3	Y123																																																																																		1.2		247																																				1						SUPERCONDUCTING AND NONSUPERCONDUCTING PHASES OF Y(1)BA(2)CU(3)O(X): MODIFICATIONS AT THE HIGH-TEMPERATURE PHASE TRANSITION	198711	PHASE TRANSITION         ,SPECIFIC HEAT            ,RES	DEPARTMENT OF PHYSICS AND CENTER FEO MATERIALS RESEARCH AND TECHNOLOGY,FLORIDA STATE UNIVERSITY,TALLAHASSEE,FLORIDA	PHYS.REV.B,36(1987)8816	C.M.REY,H.K.NG,H.MATHIAS,L.R.TESTARDI,R.J.KENNEDY,W.G.MOULTON	Y,BA,CU,O	
1430	PRB0368816		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X		1	1987																											3	Y123																																																																																		9		248																																				1						SUPERCONDUCTING AND NONSUPERCONDUCTING PHASES OF Y(1)BA(2)CU(3)O(X): MODIFICATIONS AT THE HIGH-TEMPERATURE PHASE TRANSITION	198711	PHASE TRANSITION         ,SPECIFIC HEAT            ,RES	DEPARTMENT OF PHYSICS AND CENTER FEO MATERIALS RESEARCH AND TECHNOLOGY,FLORIDA STATE UNIVERSITY,TALLAHASSEE,FLORIDA	PHYS.REV.B,36(1987)8816	C.M.REY,H.K.NG,H.MATHIAS,L.R.TESTARDI,R.J.KENNEDY,W.G.MOULTON	Y,BA,CU,O	
1431	SSC0640247		YBa2Cu3O7	Y1Ba2Cu3OX	Y	1	Ba	2	Cu	3															O	X		1	1987																											3	Y123																				93					93																																						15					1000														33		383																																				1	SIN(950C)-Q-ANN(500C IN O2)-C					THERMAL AND MAGNETIC PROPERTIES OF SOME YBA2CU3O7-Z SAMPLES				SOLID STATE COMMUN.64(1987)247	B.BARBARA,C.AYACHE,E.BONJOUR,J.H.HENRY,J.ROSSAT-MIGNOD,M.COUACH,R.CALEMCZUK	Y,BA,CU,O	
1432	PRB0371580		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4-Z	La	1.8	Sr	0.2	Cu	1															O	4-Z		1	1988																											2	T																				35					35																																																					SP1432				3.35		376																																			LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1433	PRB0371580		YBa2Cu3O7	Y1Ba2Cu3O1	Y	1	Ba	2	Cu	3															O	7-Z	1	1	1988																											3	Y123																																																																														SP1433				8.21		383																																			LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1434	PRB0371580		HoBa2Cu3O7	Ho1Ba2Cu3O1	Ho	1	Ba	2	Cu	3															O	7-Z	1	1	1988																											3	Y123																																																																														SP1434																																									LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1435	PRB0371580		TmBa2Cu3O7	Tm1Ba2Cu3O1	Tm	1	Ba	2	Cu	3															O	7-Z	1	1	1988																											3	Y123																																																																														SP1435																																									LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1436	PRB0371580		YbBa2Cu3O7	Yb1Ba2Cu3O1	Yb	1	Ba	2	Cu	3															O	7-Z	1	1	1988																											3	Y123																																																																														SP1436																																									LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1437	PRB0371580		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																														SP1437				12.9		370																																			LA(NO3)3,SR(NO3)2,CU(NO3)2	0	COPRECIPITATION					LOW-TEMPERATURE SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTORS LA(1.8)SR(0.2)CU(1)O(4-Z) AND R(1)BA(2)CU(3)O(7-Z)(R=Y,EU,HO,TM,AND YB)	198802	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA	PHYS.REV.B,37(1988)1580	B.W.LEE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	LA,SR,CU,O,R,BA,CU,O	
1438	PLA1290185		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																																																																																																																								0	ANN(450C 12H IN O2)					LOW TEMPERATURE SPECIFIC HEAT OF YBA2CU3O7 SINGLE CRYSTALS	198805			PHYS.LETT.A,129(1988)185	H.NOEL,J.C.LASJAUNIAS,J.C.LEVET,M.POTEL,P.GOUGEON	Y,BA,CU,O	
1439	JJP0270333	ORTHO-I	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		3	1988								2.26																			3	Y123																				92.7					92.7																																																					SP1439			mJ/mol.K2	4.57		355																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1440	JJP0270333	ORTHO-II	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1988								2.27																			3	Y123																				49					49																																																					SP1440			mJ/mol.K2	4.46		326																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1441	JJP0270333	TETRA-II	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1988								2.23																			2	Y123																																																																														SP1441			mJ/mol.K2	6.28		313																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1442	JJP0270333		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.925Fe0.075O7-Z	Gd	1	Ba	2	Cu	2.925	Fe	0.075													O	7-Z		1	1988								2.23																			3	Y123																				81.3					81.3																																																					SP1442			mJ/mol.K2	21.7		348																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1443	JJP0270333		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.85Fe0.15O7-Z	Gd	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z		1	1988								2.2																			3	Y123																				63.1					63.1																																																					SP1443			mJ/mol.K2	41.4		347																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1444	JJP0270333		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O7-Z	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	7-Z		1	1988								2.14																			3	Y123																				2.9					2.9																																																					SP1444			mJ/mol.K2	73.6		349																																			GD2O3,BACO3,CUO,FE2O3	0	CAL(930C 12H)-SIN(930C 12H)-SIN(940C 12H)-C,ALL IN O2					Specific heat on metamorphic and iron-doped GdBa2Cu3O7-z			Department of Electrical and Electronic Engineering, Toyohashi University of Technology, Japan	Jpn.J.Appl.Phys., 27(1988)L333	A.Oota,T.Kojima		
1445	JPF0180009		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				88.9					88.9																																																																																														Y2O3,BACO3,CUO	1	SIN(900C 12H IN AIR)-ANN(600C+500C+400C 12H)-FC					MEASUREMENTS OF THE LOW TEMPERATURE HEAT CAPACITY OF YBA2CU3O7-Y IN MAGNETIC FIELDS UP TO 4.5T				J.PHYS. F:MET.PHYS.18(1988)L9	C.E.GOUGH,C.GIBBS,C.GREAVES,E.M.FORGAN,F.WELLHOFER,J.S.ABELL,S.SUTTON	Y,BA,CU,O	
1446	JPF0180009		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				89.2					89.2																																																									8.27		465																																			Y2O3,BACO3,CUO	1	SIN(900C 12H IN AIR)-ANN(600C+500C+400C 12H)-FC					MEASUREMENTS OF THE LOW TEMPERATURE HEAT CAPACITY OF YBA2CU3O7-Y IN MAGNETIC FIELDS UP TO 4.5T				J.PHYS. F:MET.PHYS.18(1988)L9	C.E.GOUGH,C.GIBBS,C.GREAVES,E.M.FORGAN,F.WELLHOFER,J.S.ABELL,S.SUTTON	Y,BA,CU,O	
1447	JPF0180009		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				90.1					90.1																																																																																														Y2O3,BACO3,CUO	1	SIN(900C 12H IN AIR)-ANN(600C+500C+400C 12H)-FC					MEASUREMENTS OF THE LOW TEMPERATURE HEAT CAPACITY OF YBA2CU3O7-Y IN MAGNETIC FIELDS UP TO 4.5T				J.PHYS. F:MET.PHYS.18(1988)L9	C.E.GOUGH,C.GIBBS,C.GREAVES,E.M.FORGAN,F.WELLHOFER,J.S.ABELL,S.SUTTON	Y,BA,CU,O	
1448	PRB0377917	C=7.326*T+0.315*T**3+0.00222*T**5	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																			92					2.5	92																																																									7.326		431																																				1						SCHOTTKY ANOMALY IN THE HEAT CAPACITY OF THE HIGH-TC SUPERCNDUCTOR Y(1)BA(2)CU(3)O(7)	198805	SPECIFIC HEAT	DIVISION OF APPLIED PHYSICS,COMMONWEALTH SCIENTIFIC AND INDUSTRIAL RESEARCH ORGANIZATION,LINDFIELD,AUSTRALIA	PHYS.REV.B,37(1988)7917	L.DALE,R.DRIVER,S.J.COLLOCOTT,S.X.DOU	Y,BA,CU,O	
1449	PRB0377917	C=10.273*T**(-2)+11.380*T+0.0248*T**3	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																			91					2.5	91																																																									11.38																																						1						SCHOTTKY ANOMALY IN THE HEAT CAPACITY OF THE HIGH-TC SUPERCNDUCTOR Y(1)BA(2)CU(3)O(7)	198805	SPECIFIC HEAT	DIVISION OF APPLIED PHYSICS,COMMONWEALTH SCIENTIFIC AND INDUSTRIAL RESEARCH ORGANIZATION,LINDFIELD,AUSTRALIA	PHYS.REV.B,37(1988)7917	L.DALE,R.DRIVER,S.J.COLLOCOTT,S.X.DOU	Y,BA,CU,O	
1450	SSC0661101			Bi4.1Sr2.4Ca2.4Cu4OX	Bi	4.1	Sr	2.4	Ca	2.4	Cu	4													O	X		1	1988																											2					5.4		30.79													70	75	110				75																																																					SP1450						290																																			BI2O3,SRCO3,CACO3,CUO	1	IMPURITY=(CA,SR)2CUOX,BI-SR-CA-OX, HEAT(820C 12H IN AIR)-SIN(820C 375H)-C TO 450C IN FURNACE					ABSENCE OF THE T-LINEAR TERM IN LOW TEMPERATURE SPECIFIC HEAT OF HIGH-TC OXIDE,BI-SR-CA-CU-O SYSTEM	198806	SPECIFIC HEAT            ,RESISTIVITY              ,MAGNETIZ	INSTITUTE FOR MOLECULAR SCIENCE,MYODAIJI,OKAZAKI	SOLID STATE COMMUN.,66(1988)1101	K.FUKUDA,M.SATO,M.SERA,S.KONDOH	BI,SR,CA,CU,O	
1451	LES1510191	FOR DEBYET/45< T,DEVIATION FROM T**3 LAW		Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		2	1989																											2	Bi2212																																																																																		7		233																																				1						LOW-TEMPERATURE SPECIFIC HEAT OF BI2SU2CACU2O8: COMPARISON WITH SOME OTHER LAYERED OXIDES			OB, RESEARCH CENTER, YORKTOWN HEIGHTS, NY 10598 (U.S.A.)	J.LESS-COMMON METALES,151(1989)191	A.TORRESSEN,J.M.D.COEY,S.VON MOLNAR	BI,CR,CA,CU,O	
1452	LES1510191			Sr14Cu24O41	Sr	14	Cu	24																	O	41			1989																																																																																																														100		296																																				1						LOW-TEMPERATURE SPECIFIC HEAT OF BI2SU2CACU2O8: COMPARISON WITH SOME OTHER LAYERED OXIDES			OB, RESEARCH CENTER, YORKTOWN HEIGHTS, NY 10598 (U.S.A.)	J.LESS-COMMON METALES,151(1989)191	A.TORRESSEN,J.M.D.COEY,S.VON MOLNAR	BI,CR,CA,CU,O	
1453	LTP0730241		(Y,Ba)Ba2Cu3O7	Y0.9Ba2.1Cu3O7-Z	Y	0.9	Ba	2.1	Cu	3															O	7-Z			1988																												Y123																				92					92																																																					SP1453				63		372																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1454	LTP0730241		Y(Ba,Y)2Cu3O7	Y1.1Ba1.9Cu3O7-Z	Y	1.1	Ba	1.9	Cu	3															O	7-Z			1988																												Y123																				92					92																																																					SP1454				14.1		362																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1455	LTP0730241		Y2BaCuO5	Y2Ba1Cu1O5	Y	2	Ba	1	Cu	1															O	5			1988																												Y211																																																																														SP1455				9		292																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1456	LTP0730241		YBa3Cu2O7	Y1Ba3Cu2O7	Y	1	Ba	3	Cu	2															O	7			1988																																																																																																										SP1456				28.6		244																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1457	LTP0730241		BaCuO2	Ba1Cu1O2+X	Ba	1	Cu	1																	O	2+X			1988																																																																																																										SP1457				52		278																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1458	LTP0730241		BaCuO2	Ba1Cu1O2+X	Ba	1	Cu	1																	O	2+X			1988																																																																																																										SP1458				140		291																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1459	LTP0730241		BaCuO2	Ba1Cu1O2+X	Ba	1	Cu	1																	O	2+X			1988																																																																																																										SP1459				107		290																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1460	LTP0730241		BaCuO2	Ba1Cu1O2+X	Ba	1	Cu	1																	O	2+X			1988																																																																																																										SP1460				151		293																																										Low-temperature Specific Heat of YBa2Cu3O7, YBa2Cu3O6, Y2Ba2CuO5, YBa3Cu2O7, BaCuO2, and CuO	198803		De'partement de Physique de la Matie're Condense'e, Universite' de Gene've, CH-1211 Geneva 4, Swizerland	J.Low Temp.Phys., 73(1988)241	A. Bezinge,A. Junod,D. Eckert,J. Muller,T. Graf		
1461	SSC0701155	BA0.58K0.42BIO3.03 BY NEUTRON DIFFR.	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1989																											1	BKBO				4.29																27					27										22																					0.39																						SP1461						210																																			BANO3,BI2O3,KNO3	1	(BANO3+BI2O3)-(700C 12H)-MIX WITH KNO3-(700C 1H IN N2)-ANN(450C 2H+375C 4H IN O2)-C					SPECIFIC HEAT OF THE CUBIC HIGH-TC SUPERCONDUCTOR BA0.6K0.4BIO3			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545	SOLID STATE COMMUN,70(1989)1155	G.H.KWEI,J.D.THOMPSON,M.F.HUNDLEY	BA,K,BI,O	
1464	SSC0630721		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4-Y	La	1.8	Ba	0.2	Cu	1															O	4-Y			1987																												T																				31	35				31																																						67															SP1464				6		330																																				0						MAGNETIC AND THERMAL MEASUREMENTS ON HIGH-TC  (LA0.9BA0.1)2CUO4-Y			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545	SOLID STATE COMMUN,063(1987)721	C.W.CHU,C.Y.HUANG,E.ZIRNGIEBL,J.D.THOMPSON,J.L.SMITH,J.O.WILLIS,M.K.WU,P.H.HOR,R.L.MENG,Z.FISK	LA,BA,CU,O	
1465	SSC0650111		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1988						0.21	37.5	240																			3	T				5.358	5.403	13.181																																																																								SP1465				1		320																																				0	PBO BASED FLUX					NOVEL PHASE TRANSITION IN NON-ANTIFERROMAGNETICALLY ORDERED CRYSTALS OF LA2CUO4			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545	SOLID STATE COMMUN,065(1988)111	A.S.COOPER,D.SCHIFERL,G.GRUNER,J.D.THOMPSON,J.O.WILLIS,J.P.REMEIKA,R.M.AIKIN,S-W.CHENG,S.E.BROWN,Z.FISK	LA,CU,O	
1466	SSC0630635		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4-Z	La	1.8	Sr	0.2	Cu	1															O	4-Z			1987																												T																			27		38				32.5																																																									4		367																																				0	SIN(1100C 12H)-ANN(925C 18-24H IN 1ATM O2)					HIGH TEMPERATUER SUPERCONDUCTIVITY IN(M1-XM'X)2CUO4-Z AND RELATED COMPOUNDS(M=Y,LA,EU,SM; M=BA,SR)			DEPERTMENT OF PHYSICS AND INSTITUTE FO PURE AND APPLIEDPHYSICAL SCIENSE UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093	SOLID STATE COMMUN,063(1987)635	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	CU,O,Y,LA,EU,SM,BA,SR	
1467	TH1380136	LATC=37,30A TWO PHASES	(Bi,Pb,Sb)2Sr2Ca2Cu3Oz	Bi1.7Pb0.2Sb0.1Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.2	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			116						116																						181									2.43																																																															BI2O3,CU0,SB2O5,PBO,SRCO3,CACO3	1	MATERIALS CONTAIN CU3,BI-PB-SB-SR-CA-CU-O , MIXTURE-HEAT(830C 15H)-SIN(865C 60H)-FC IN AIR					THE INFLUENCE OF PB COMPOSITION ON THE UPPER CRITICAL MAGNETICFIELD OF BI1.9-XPBXSB0.1SR2CA2CU3OY SYSTEM	198906	UPPER CRITICAL FIELD,PB CONTENT          ,MAGNETORESISTANCE	DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE AND TECHNOLOGY OFCHINA, HEFEI, PR CHINA	PHYS. A,138(1989)136	HONGBAO LIU,LING ZHOU,QUAN DU,WEIJIE ZHANG,XIANGLEI MAO,YU WANG,YUHENG ZHANG,ZHIQIANG MAO	BI,PB,SB,SR,CA,CU,O	
1468	TH1380136	LATC=37,30A TWO PHASES	(Bi,Pb,Sb)2Sr2Ca2Cu3Oz	Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			116						116																						370									4.9																																																															BI2O3,CU0,SB2O5,PBO,SRCO3,CACO3	1	MATERIALS CONTAIN CU3,BI-PB-SB-SR-CA-CU-O , MIXTURE-HEAT(830C 15H)-SIN(865C 60H)-FC IN AIR					THE INFLUENCE OF PB COMPOSITION ON THE UPPER CRITICAL MAGNETICFIELD OF BI1.9-XPBXSB0.1SR2CA2CU3OY SYSTEM	198906	UPPER CRITICAL FIELD,PB CONTENT          ,MAGNETORESISTANCE	DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE AND TECHNOLOGY OFCHINA, HEFEI, PR CHINA	PHYS. A,138(1989)136	HONGBAO LIU,LING ZHOU,QUAN DU,WEIJIE ZHANG,XIANGLEI MAO,YU WANG,YUHENG ZHANG,ZHIQIANG MAO	BI,PB,SB,SR,CA,CU,O	
1469	TH1380136	LATC=37,30A TWO PHASES	(Bi,Pb,Sb)2Sr2Ca2Cu3Oz	Bi1.5Pb0.4Sb0.1Sr2Ca2Cu3OZ	Bi	1.5	Pb	0.4	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			110						110																						416									5.36																																																															BI2O3,CU0,SB2O5,PBO,SRCO3,CACO3	1	MATERIALS CONTAIN CU3,BI-PB-SB-SR-CA-CU-O , MIXTURE-HEAT(830C 15H)-SIN(865C 60H)-FC IN AIR					THE INFLUENCE OF PB COMPOSITION ON THE UPPER CRITICAL MAGNETICFIELD OF BI1.9-XPBXSB0.1SR2CA2CU3OY SYSTEM	198906	UPPER CRITICAL FIELD,PB CONTENT          ,MAGNETORESISTANCE	DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE AND TECHNOLOGY OFCHINA, HEFEI, PR CHINA	PHYS. A,138(1989)136	HONGBAO LIU,LING ZHOU,QUAN DU,WEIJIE ZHANG,XIANGLEI MAO,YU WANG,YUHENG ZHANG,ZHIQIANG MAO	BI,PB,SB,SR,CA,CU,O	
1470	TH1380136	LATC=37,30A TWO PHASES	(Bi,Pb,Sb)2Sr2Ca2Cu3Oz	Bi1.4Pb0.5Sb0.1Sr2Ca2Cu3OZ	Bi	1.4	Pb	0.5	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			109						109																						195									2.5																																																															BI2O3,CU0,SB2O5,PBO,SRCO3,CACO3	1	MATERIALS CONTAIN CU3,BI-PB-SB-SR-CA-CU-O , MIXTURE-HEAT(830C 15H)-SIN(865C 60H)-FC IN AIR					THE INFLUENCE OF PB COMPOSITION ON THE UPPER CRITICAL MAGNETICFIELD OF BI1.9-XPBXSB0.1SR2CA2CU3OY SYSTEM	198906	UPPER CRITICAL FIELD,PB CONTENT          ,MAGNETORESISTANCE	DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE AND TECHNOLOGY OFCHINA, HEFEI, PR CHINA	PHYS. A,138(1989)136	HONGBAO LIU,LING ZHOU,QUAN DU,WEIJIE ZHANG,XIANGLEI MAO,YU WANG,YUHENG ZHANG,ZHIQIANG MAO	BI,PB,SB,SR,CA,CU,O	
1471	PRB0368780		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																											2	T																					41.5				41.5																																																					SP1471				4		400																																				0	<5% LA2SRCU2O6, CAL(1130C IN AIR)-ANN(1000C 12H IN O2)					SPECIFIC HEAT OF LA(1.8)SR(0.2)CU(1)O(4): ANOMALY AT THE SUPERCONDUCTING TRANSITION	198712	SPECIFIC HEAT	CENTRO ATOMICO BARILOCHE,RIO NEGRO,ARGENTINA	PHYS.REV.B,36(1987)8780	C.A.D'OVIDIO,D.A.ESPARZA,E.N.MARTINEZ,F.DE LA CRUZ,G.NIEVA	LA,SR,CU,O	
1472	JPF0170329		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1987																												T																																																																														SP1472				0.16		406																																				0						EVIDENCE ON THE NATURE OF SUPERCONDUCTIVITY IN LA1.85BA0.15CUO4 FROM SPECIFIC HEAT MEASUREMENTS			SCHOOL OF MATHEMATICAL AND PHYSICAL SCEINCES, UNIVERSITY OF SUSSEX, BRIGHTON BN19QH, UK	J.PHYS.F,17(1987)L329	D.VCK PAUL,G.BALAKRISHNAN,J.W.LORMAN,K.A.MIRZA	LA,BA,CU,O	
1473	JPF0170329		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4			1987																												T																				29					29																																																					SP1473				0.76		418																																				0						EVIDENCE ON THE NATURE OF SUPERCONDUCTIVITY IN LA1.85BA0.15CUO4 FROM SPECIFIC HEAT MEASUREMENTS			SCHOOL OF MATHEMATICAL AND PHYSICAL SCEINCES, UNIVERSITY OF SUSSEX, BRIGHTON BN19QH, UK	J.PHYS.F,17(1987)L329	D.VCK PAUL,G.BALAKRISHNAN,J.W.LORMAN,K.A.MIRZA	LA,BA,CU,O	
1474	SSC0651555	THER.EXPAN.=1.03E-9*T+5.75E-11*T**3	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																			87		90				88.5																																																					SP1474				9.4		346																																										LOW TEMPERATURE THERMAL EXPANSION AND SPECIFIC HEAT OF A HIGH TC CERAMIC Y(1)BA(2)CU(3)O(7-Z)	198804	SPECIFIC HEAT            ,THERMAL EXPANS	DPTO.DE FISICA DE LA MATERIA CONDENSADA,C-III UNIVERSIDAD AUTONOMA DE MADRID CANTOBLANCO	SOLID STATE COMMUN.,65(1988)1555	A.AGUILO,C.MOURE,M.A.RAMOS,P.DURAN,R.VILLAR,S.BOURGEAL,S.VIEIRA	Y,BA,CU,O	
1475	PRB03912391	0.75X0.75X0.1 MM3	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z		3	1989																											2	Tl2223																				105					105																																																					SP1475				1		242																																				9						LOW-TEMPERATURE SPECIFIC HEAT OF SINGLE-CRYSTAL BI(2)CASR(2)CU(2)O(8) AND TL(2)CA(2)BA(2)CU(3)O(10)	198906	SPECIFIC-HEAT       ,SINGLE CRYSTALS	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,STANFORD,CALIFORNIA 94305	PHYS.REV.B.,39(1989)12391	A.KAPITULNIK,D.B.MITZI,D.E.MORRIS,J.S.URBACH,J.Y.T.WEI	BI,CA,SR,CU,O,TL,BA	
1476	PRB03912391		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z		1	1989																											2	Tl2223																				105					105																																																					SP1476				5		225																																				9						LOW-TEMPERATURE SPECIFIC HEAT OF SINGLE-CRYSTAL BI(2)CASR(2)CU(2)O(8) AND TL(2)CA(2)BA(2)CU(3)O(10)	198906	SPECIFIC-HEAT       ,SINGLE CRYSTALS	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,STANFORD,CALIFORNIA 94305	PHYS.REV.B.,39(1989)12391	A.KAPITULNIK,D.B.MITZI,D.E.MORRIS,J.S.URBACH,J.Y.T.WEI	BI,CA,SR,CU,O,TL,BA	
1477	PRB03912391		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1989																											2	Bi2212																				98					98																																																					SP1477				0.6		230																																				9						LOW-TEMPERATURE SPECIFIC HEAT OF SINGLE-CRYSTAL BI(2)CASR(2)CU(2)O(8) AND TL(2)CA(2)BA(2)CU(3)O(10)	198906	SPECIFIC-HEAT       ,SINGLE CRYSTALS	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,STANFORD,CALIFORNIA 94305	PHYS.REV.B.,39(1989)12391	A.KAPITULNIK,D.B.MITZI,D.E.MORRIS,J.S.URBACH,J.Y.T.WEI	BI,CA,SR,CU,O,TL,BA	
1478	PRB03811942	TC=110K + 80K, TWO PHASES	Bi2Sr2Ca6Cu8O19	Bi2Sr2Ca6Cu8O19	Bi	2	Sr	2	Ca	6	Cu	8													O	19			1988																												Bi2268																				80					80																																																											293																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1479	PRB03811942		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1988																												Bi2212																				84					84																																																											256																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1480	PRB03811942		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1988																												Bi2212																				84				30	84																																																											252																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1481	PRB03811942	TC=95K+110K		Bi2Sr2Ca2Cu4O11	Bi	2	Sr	2	Ca	2	Cu	4													O	11			1988																												Bi2224																				95					95																																																											249																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1482	PRB03811942			Tl1Ba1Ca1Cu2O5.5	Tl	1	Ba	1	Ca	1	Cu	2													O	5.5		1	1988																											2																					114				20	114																																																					SP1482				16		268																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1483	PRB03811942			Bi2.15Sr1.68Ca1.17Cu2O8	Bi	2.15	Sr	1.68	Ca	1.17	Cu	2													O	8			1988																											2																					80				20	80																																																					SP1483						228																																				0						SPECIFIC-HEAT MEASUREMENTS ON SUPERCONDUCTING BI-CA-SR-CU AND TL-CA-BA-CU OXIDES: ABSENCE OF A LINEAR TERM IN THE SPECIFIC HEAT OF BI-CA-SR-CU OXIDES	198812	SPECIFIC HEAT	MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,38(1988)11942	A.G.MARKELZ,D.E.MORRIS,D.S.GINLEY,J.Y.T.WEI,N.E.PHILLIPS,R.A.FISHER,S.E.LACY,S.KIM	BI,CA,SR,CU,TL,BA,O	
1484	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.876	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.876	1	1989																												Tl2212																				110					110																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1485	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.833	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.833	1	1989																												Tl2212																				112					112																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1486	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	8	1	1989																												Tl2212																				87					87																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1487	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.984	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.984	1	1989																												Tl2212																				92					92																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1488	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.978	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.978	1	1989																												Tl2212																				95					95																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1489	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.958	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.958	1	1989																												Tl2212																				107					107																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1490	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.946	Tl	2	Ba	2	Ca	1	Cu	2													O	Z	7.946	1	1989																												Tl2212																				107					107																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1491	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1989																												Tl2223																				115					115																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1492	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.964	Tl	2	Ba	2	Ca	2	Cu	3													O	10	9.964		1989																												Tl2223																				112					112																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1493	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.877	Tl	2	Ba	2	Ca	2	Cu	3													O	10	9.877		1989																												Tl2223																				111					111																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1494	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.841	Tl	2	Ba	2	Ca	2	Cu	3													O	10	9.841		1989																												Tl2223																				110					110																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1495	PHC1660405	SOUND VELOCITY	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212						30.86															85				85																																																																																															0	PT CRUCIBLE AT 900 C 2H					SOUND VELOCITY IN BI2SR2CACU2O8 SINGLE CRYSTALS		SOUND VELOCITY      ,SINGLE CRYSTALS     ,SHERA MODULUS	CENTRE DE RECHERCHES SUR LES TRES BASSED TEMPREATURES,CNRS,BP166 X,38042 GRENOBLE-CEKEX,FRANCE	PHYSICA C,166(1990)405	J.L.THOLENCE,M.SAINT-PAUL	BI,SR,CA,CU,O	
1496	JJP0282175		(Tl,Pb)Sr2(Ca,Er)Cu2Oz	Tl0.5Pb0.5Ca0.8Er0.2Sr2Cu2OX	Tl	0.5	Pb	0.5	Ca	0.8	Er	0.2	Sr	2	Cu	2									O	X		1	1989						9.76	-8.5																				2	Tl1212				3.81		11.97														110					110																																																																																														CACO3,ER2O3,SRCO3,CUO,TL2O3,PBO	1	CAL(920-970C 12H IN AIR)-ADD(TL2O3+PBO)-WRAPPED IN AU FOIL-SIN(950C 3H IN O2)-C(2C/MIN) TO RT					MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR TL0.5PB0.5CA0.8ER0.2SR2CU2 OXUDE	198912	MAGNETISATION       ,ESR                 ,PARAMAGNETISM       ,MAGNETIC PROPERTI	RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,WEST CAMBRIDGE SITE,MADINGLEY ROAD,CAMBRIDGE,U.K.	JJAP LETT.,28(1989)L2175	P.P.EDWARDS,P.T.WU,R.JANES,R.S.LIU,T.J.WATSON-YANG	TL,PB,CA,ER,SR,CU,O	
1497	PR04011403	TUNNELING USING STM,I-V CURVE USING PT-RH TIP	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z			1989																												Tl2223																			105	110					110																																																4																																															0						TUNNELING MEASUREMENTS OF THE ENERGY GAP IN THE HIGH-TC SUPERCONDUCTOR TL2BA2CA2CU3O10+Z	198912	TUNNELING           ,I-V CHARACTERISTIC  ,ENERGY GAP          ,STEM	LABORATORIO DE FISICA DE BAJAS TEMPERATURAS,C-III,UNIVERSIDADAUTONOMA DE MADRLD,CANTOBLANCO,28049-MADRID,SPAIN	PHYS.REV.B,40(1989)11403	J.G.RODRIGO,K.V.RAO,M.A.RAMOS,S.VIEIRA,Y.MAKINO	TL,BA,CA,CU,O	
1498	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	Z	6	1	1989																												Tl2201						23.14																																																																																																																	TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1499	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.989	Tl	2	Ba	2	Cu	1															O	Z	5.989	1	1989																												Tl2201						23.15														10					10																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1500	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	X	6		1989																												Y123				3.862		11.813																																																																																																																	Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1501	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.16	Y	1	Ba	2	Cu	3															O	X	6.16		1989																												Y123				3.855	3.871	11.792																																																																																																																	Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1502	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.29	Y	1	Ba	2	Cu	3															O	X	6.29		1989																												Y123				3.842	3.872	11.767														21.9					21.9																																																																																		345												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1503	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.34	Y	1	Ba	2	Cu	3															O	X	6.34		1989																												Y123				3.838	3.875	11.747														23.5					23.5																																																																																		210												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1504	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.43	Y	1	Ba	2	Cu	3															O	X	6.43		1989																												Y123				3.837	3.875	11.747														26.4					26.4																																																																																		157												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1505	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	X	6.5		1989																												Y123				3.831	3.879	11.738														50.1					50.1																																																																																		48.8												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1506	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	X	6.54		1989																												Y123				3.831	3.876	11.732														54					54																																																																																		27.9												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1507	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.58	Y	1	Ba	2	Cu	3															O	X	6.58		1989																												Y123				3.829	3.88	11.723														56.3					56.3																																																																																		22.4												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1508	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.64	Y	1	Ba	2	Cu	3															O	X	6.64		1989																												Y123				3.826	3.882	11.719														59.7					59.7																																																																																		17.6												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1509	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	X	6.72		1989																												Y123				3.824	3.881	11.707														85					85																																																																																		9.75												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1510	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	X	6.8		1989																												Y123				3.82	3.884	11.697														93.9					93.9																																																																																		7.56												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1511	JJP0280368		YBa2Cu3O7	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	X	6.87		1989																												Y123				3.818	3.885	11.684														93.2					93.2																																																																																		3.28												Y2O3,BACO3,CUO	0	SIN(900C)-ANN(500C IN AIR),OXYGEN CONTROLED BY HEATING UPTO 400-700C AT 10C/MIN AND COOLING(2.5C/MIN)					POSSIBLE EXISTENCE OF A SUPERCONDUCTING PHASE IN HIGHLY OXYGEN--DEFICIENT YBA(2)CU(3)O(Y)(Y<6.5)	198903	OXYGEN CONTENT           ,SUSCEPTIBILITY           ,RES	DEPARTMENT OF MATHENATICS AND PHYSICS,THE NATIONAL DEFENSE ACAD-EMY,YOKOSUKA	JJAP LETT.,28(1989)L368	HIROMASA MAZAKI,KOJI -KOSUGE,TAKAYOSHI KUBOZOE,YUJI AIHARA,YUTAKA UEDA	Y,BA,CU,O	
1512	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.957	Tl	2	Ba	2	Cu	1															O	Z	5.957	1	1989																												Tl2201						23.17														38					38																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1513	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.947	Tl	2	Ba	2	Cu	1															O	Z	5.947	1	1989																												Tl2201						23.176														50					50																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1514	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.943	Tl	2	Ba	2	Cu	1															O	Z	5.943	1	1989																												Tl2201						23.2														56					56																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1515	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.984	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.984	1	1989																												Tl2212																				90					90																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1516	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.978	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.978	1	1989																												Tl2212																				95					95																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1517	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.958	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.958	1	1989																												Tl2212																				107					107																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1518	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.946	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.946	1	1989																												Tl2212																				107					107																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1519	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.876	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.876	1	1989																												Tl2212																				110					110																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1520	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O7.833	Tl	2	Ba	2	Ca	1	Cu	2													O	8	7.833	1	1989																												Tl2212																				112					112																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1521	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.94	Tl	2	Ba	2	Cu	1															O	Z	5.94	1	1989																												Tl2201																				58					58																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1522	PR04011400		TL2BA2CUO6	Tl2Ba2Cu1O5.929	Tl	2	Ba	2	Cu	1															O	Z	5.929	1	1989																												Tl2201																				70					70																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1523	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.912	Tl	2	Ba	2	Cu	1															O	Z	5.912	1	1989																												Tl2201																				82					82																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1524	PR04011400		Tl2Ba2CuO6	Tl2Ba2Cu1O5.876	Tl	2	Ba	2	Cu	1															O	Z	5.876	1	1989																												Tl2201																				87					87																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1525	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	Z	10	1	1989																												Tl2223																				115					115																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1526	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.964	Tl	2	Ba	2	Ca	2	Cu	3													O	Z	9.964	1	1989																												Tl2223																				112					112																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1527	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.877	Tl	2	Ba	2	Ca	2	Cu	3													O	Z	9.877	1	1989																												Tl2223																				111					111																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1528	PR04011400		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O9.841	Tl	2	Ba	2	Ca	2	Cu	3													O	Z	9.841	1	1989																												Tl2223																				110					110																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1529	PR04011400		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8	8	1	1989																												Tl2212																				87					87																																																																																														TL2O3,BAO,CAO,CUO	1	WRAPPED IN AU FOIL-SIN(860C 5-10H IN O2)-SIN(880-890C 5-10H IN O2)-OXYGEN CONTROL BY ANN(350-600C 3-5H IN AR)					VARIATION IN TC AND CARRIER CONCENTRATION IN TL-BASED SUPERCONDUCTORS	198912	CARRIER CONCETRATION,OXYGEN CONTENT      ,TC	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,40(1989)11400	H.IGARASHI,T.MANAKO,Y.KUDO,Y.SHIMAKAWA	TL,BA,CA,CU,O	
1530	PHC1570279		Tl2Ba2CuO6	Tl2Ba2Cu1O5.963	Tl	2	Ba	2	Cu	1															O	6	5.963	1	1989																											2	Tl2201	I4/MMM	139		3.86		23.201														53					53																																																																																															0	890C 3H QUENCH TO LN					VARIATION IN TC,STRUCTURE AND OXYGEN CONTENT IN TL(2)BA(2)CU(1)O(6) AND THEIR CORRELATIONS	198902	FABRICATION              ,STRUCTURE                ,TC                       ,OX	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,KAWASAKI	PHYSICA C,157(1989)279	H.IGARASHI,S.IIJIMA,T.ICHIHASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
1531	PHC1570279		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6	6	1	1989																											2	Tl2201	I4/MMM	139		3.859		23.127																																																																																																																		0	890C 3H QUENCH TO LN					VARIATION IN TC,STRUCTURE AND OXYGEN CONTENT IN TL(2)BA(2)CU(1)O(6) AND THEIR CORRELATIONS	198902	FABRICATION              ,STRUCTURE                ,TC                       ,OX	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,KAWASAKI	PHYSICA C,157(1989)279	H.IGARASHI,S.IIJIMA,T.ICHIHASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
1532	PHC1570279		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1989																											3	Tl2201	FMMM	69		5.455	5.493	23.176														50					50																																																																																															0	890C 3H QUENCH TO LN					VARIATION IN TC,STRUCTURE AND OXYGEN CONTENT IN TL(2)BA(2)CU(1)O(6) AND THEIR CORRELATIONS	198902	FABRICATION              ,STRUCTURE                ,TC                       ,OX	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,KAWASAKI	PHYSICA C,157(1989)279	H.IGARASHI,S.IIJIMA,T.ICHIHASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
1533	PHC1570279		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1989																											3	Tl2201	FMMM	69		5.44	5.496	23.141																																																																																																																		0	890C 3H QUENCH TO LN					VARIATION IN TC,STRUCTURE AND OXYGEN CONTENT IN TL(2)BA(2)CU(1)O(6) AND THEIR CORRELATIONS	198902	FABRICATION              ,STRUCTURE                ,TC                       ,OX	FUNDAMENTAL RESEARCH LABORATORIES,NEC CORPORATION,KAWASAKI	PHYSICA C,157(1989)279	H.IGARASHI,S.IIJIMA,T.ICHIHASHI,T.MANAKO,T.SATOH,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
1534	PHC1650340	GAMMA=43MJ/MOLE.K2 FROM KAIZERO	(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3O10	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	10		1	1990		-8148000000000000000000					215																				2	Bi2223				5.261		37.1														109					109																																																																																																					SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY OF THE HIGH-TC SUPERCONDUCTOR (VI,PB,SB)2SR2CA2CU3O10			CENTER FOR MATERIALS RESEARCH, TEMPLE UNIVERSITY, PHILADELPHIA, PA 19122, USA	PHYSICA C,165(1990)340	G.H.MYER,J.E.CROW,J.SCHWEGLER,NICHOLAS D.SPENCER,P.SCHLOTTMANN,Y.GAO	BI,PB,SB,SR,CA,CU,O	
1535	PHC1670067	NOT SUPER BUT HAVE CUO5 PYRAMIDS		Pb3Ba3Cu3Cl1O8	Pb	3	Ba	3	Cu	3	Cl	1													O	8			1990																											3					5.55	5.59	20.11																																																																																																																		0						PB2SR3CU3O8ZCL: A NEW LAYERED COPPER EXYCHLORIDE		CRYSTAL STRUCTURE   ,OXYGEN STOICHIOMETR	AT&T BELL LABORATORIES,600 MOUNJTAIN AVENUE,MURRAY HILL,NJ USA	PHYSICA C,167(1990)67	B.BATLOGG,C.CHAILLOUT,E.A.HEWAT,J.CHENAVAS,J.J.CAPPONI,J.L.HODEAU,J.P.LEVY,L.W.RUPP JR.,M.MAREZIO,P.BORDET,R.J.CAVA,T.FOURNIER	PB,SR,CU,O,CL	
1536	PHC1670067	NOT SUPER BUT HAVE CUO5 PYRAMIDS		Pb3Sr3Cu3Cl1O9.5	Pb	3	Sr	3	Cu	3	Cl	1													O	9.5			1990																											3					3.88	3.95	19.53																																																																																																																		0						PB2SR3CU3O8ZCL: A NEW LAYERED COPPER EXYCHLORIDE		CRYSTAL STRUCTURE   ,OXYGEN STOICHIOMETR	AT&T BELL LABORATORIES,600 MOUNJTAIN AVENUE,MURRAY HILL,NJ USA	PHYSICA C,167(1990)67	B.BATLOGG,C.CHAILLOUT,E.A.HEWAT,J.CHENAVAS,J.J.CAPPONI,J.L.HODEAU,J.P.LEVY,L.W.RUPP JR.,M.MAREZIO,P.BORDET,R.J.CAVA,T.FOURNIER	PB,SR,CU,O,CL	
1537	PHC1670067			Pb3Sr3Cu3Cl1O8	Pb	3	Sr	3	Cu	3	Cl	1													O	8			1990																											3		C-MMM			5.444	5.495	19.49																																																																																																																		0						PB2SR3CU3O8ZCL: A NEW LAYERED COPPER EXYCHLORIDE		CRYSTAL STRUCTURE   ,OXYGEN STOICHIOMETR	AT&T BELL LABORATORIES,600 MOUNJTAIN AVENUE,MURRAY HILL,NJ USA	PHYSICA C,167(1990)67	B.BATLOGG,C.CHAILLOUT,E.A.HEWAT,J.CHENAVAS,J.J.CAPPONI,J.L.HODEAU,J.P.LEVY,L.W.RUPP JR.,M.MAREZIO,P.BORDET,R.J.CAVA,T.FOURNIER	PB,SR,CU,O,CL	
1538	PHC1670067			Pb3Ba2Sr1Cu3Cl1O8	Pb	3	Ba	2	Sr	1	Cu	3	Cl	1											O	8			1990																											3					5.53	5.56	19.87																																																																																																																		0						PB2SR3CU3O8ZCL: A NEW LAYERED COPPER EXYCHLORIDE		CRYSTAL STRUCTURE   ,OXYGEN STOICHIOMETR	AT&T BELL LABORATORIES,600 MOUNJTAIN AVENUE,MURRAY HILL,NJ USA	PHYSICA C,167(1990)67	B.BATLOGG,C.CHAILLOUT,E.A.HEWAT,J.CHENAVAS,J.J.CAPPONI,J.L.HODEAU,J.P.LEVY,L.W.RUPP JR.,M.MAREZIO,P.BORDET,R.J.CAVA,T.FOURNIER	PB,SR,CU,O,CL	
1539	PHC1660393			Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		1	1990						10.4	-14																					Y124																			76		81				78.5																																																											380																																										SPECIFIC HEAT, MAGNETIZATION AND RESISTIVITY MEASUREMENTS ON HOBA2CU4O8		SPECIFIC HEAT       ,RESISTIVETY         ,MAGNETIZATION	LABRATORIUM FUR FESTKORPRPHYSIK,ETHZ,HC-8093 ZURICH,SWIZRELAND	PHYSICA C,166(1990)393	A.BERNASCONI,A.SCHILLING,H.R.OTT,J.D.GUO	HO,BA,CU,O	
1540	PHC1670102		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1990									6.72																			Y124																				77					77										68.6																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1541	PHC1670102		(Ho,Ca)Ba2Cu4O8	Ho0.95Ca0.05Ba2Cu4O8	Ho	0.95	Ca	0.05	Ba	2	Cu	4													O	8			1990																												Y124																				81					81										94.1																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1542	PHC1670102		(Ho,Ca)Ba2Cu4O8	Ho0.9Ca0.1Ba2Cu4O8	Ho	0.9	Ca	0.1	Ba	2	Cu	4													O	8			1990																												Y124																				87					87										98																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1543	PHC1670102		(Ho,Ca)Ba2Cu4O8	Ho0.85Ca0.15Ba2Cu4O8	Ho	0.85	Ca	0.15	Ba	2	Cu	4													O	8			1990																												Y124																				87					87										93.3																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1544	PHC1670102		(Ho,Ca)Ba2Cu4O8	Ho0.8Ca0.2Ba2Cu4O8	Ho	0.8	Ca	0.2	Ba	2	Cu	4													O	8			1990																												Y124																				87					87										73.5																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1545	PHC1670102		(Ho,Ca)Ba2Cu4O8	Ho0.7Ca0.3Ba2Cu4O8	Ho	0.7	Ca	0.3	Ba	2	Cu	4													O	8			1990																												Y124																				87					87										64.6																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1546	PHC1670102		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990									6.13																			Y124																				81					81										72.2																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1547	PHC1670102		(Y,Ca)Ba2Cu4O8	Y0.95Ca0.05Ba2Cu4O8	Y	0.95	Ca	0.05	Ba	2	Cu	4													O	8		1	1990																												Y124																				84					84										89.3																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1548	PHC1670102		(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8		1	1990																												Y124																				89.5					89.5										94.7																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1549	PHC1670102		(Y,Ca)Ba2Cu4O8	Y0.85Ca0.15Ba2Cu4O8	Y	0.85	Ca	0.15	Ba	2	Cu	4													O	8		1	1990																												Y124																				90					90										73																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1550	PHC1670102		(Y,Ca)Ba2Cu4O8	Y0.8Ca0.2Ba2Cu4O8	Y	0.8	Ca	0.2	Ba	2	Cu	4													O	8		1	1990																												Y124																				90					90										65																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1551	PHC1670102		(Y,Ca)Ba2Cu4O8	Y0.7Ca0.3Ba2Cu4O8	Y	0.7	Ca	0.3	Ba	2	Cu	4													O	8		1	1990																												Y124																				90					90										48.9																																																																																				Y2O3,HO2O3,CACO3,BACO3,CUO	1	CAL(880C 16H IN AIR)-O2-HIP IN 20%O2+80%AR					BULK SYNTHESIS OF LN1-XCAXBA2CU4O8(LN=Y,HO)BY THE OXYGEN-HIPTHCHNIQUE		SYNTHESIS           ,HIGH PRESSURE OXYGEN,CA-SUBSTIUTION      ,CRITICALCURRENT	SUPERCONDUCTING AND CRYOGENIC TECHNOLOGY CENTER,KOBE STEEL LTD.,1-5-5,TAKATSUKADAI,NISHI-KU,KOBE 673-02,JAPAN	PHYSICA C,167(1990)102	K.SHIBUTANI,R.OGAWA,S.HAYASHI,Y.FUKUMOTO,Y.KAWATE	Y,HO,CA,BA,CU,O	
1552	SSC0630721	DEFINITION OF HC1 AMBIGUOUS,GAMMA=2.23 FROM SUS	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4-Y	La	1.8	Ba	0.2	Cu	1															O	4-Y			1987																												T																				31					31										10			400																																												6		330																																				0						MAGNETIC AND THERMAL MEASUREMENTS ON HIGH-TC  (LA0.9BA0.1)2CUO4-Y			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545	SOLID STATE COMMUN,063(1987)721	C.W.CHU,C.Y.HUANG,E.ZIRNGIEBL,J.D.THOMPSON,J.L.SMITH,J.O.WILLIS,M.K.WU,P.H.HOR,R.L.MENG,Z.FISK	LA,BA,CU,O	
1553	SSC0650111	KAI= /MOLE.CU		La2Cu1O	La	2	Cu	1																	O				1988						0.21	37.5	240																			3	T				5.358	5.403	13.181																																																																																																																		0	PBO BASED FLUX					NOVEL PHASE TRANSITION IN NON-ANTIFERROMAGNETICALLY ORDERED CRYSTALS OF LA2CUO4			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545	SOLID STATE COMMUN,065(1988)111	A.S.COOPER,D.SCHIFERL,G.GRUNER,J.D.THOMPSON,J.O.WILLIS,J.P.REMEIKA,R.M.AIKIN,S-W.CHENG,S.E.BROWN,Z.FISK	LA,CU,O	
1554	SSC0630635	BETA=0.274MJ/MOLE.K4, TEMP.<80K	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4-Z	La	1.8	Sr	0.2	Cu	1															O	4-Z			1987																												T																				34					34																																																							11		4		367																																				0	SIN(1100C 12H)-ANN(925C 18-24H IN 1ATM O2)					HIGH TEMPERATUER SUPERCONDUCTIVITY IN(M1-XM'X)2CUO4-Z AND RELATED COMPOUNDS(M=Y,LA,EU,SM; M=BA,SR)			DEPERTMENT OF PHYSICS AND INSTITUTE FO PURE AND APPLIEDPHYSICAL SCIENSE UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA 92093	SOLID STATE COMMUN,063(1987)635	B.W.LEE,H.ZHOU,J.J.NEUMEIRE,J.M.FERREIRA,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	CU,O,Y,LA,EU,SM,BA,SR	
1555	ST0280576	OMEGA-P=8700CM-1,TAW=4.9E-15 FR PLASMA FREQ.		Bi1.85Pb0.35Sr1.9Ca2.1Cu3.1OY	Bi	1.85	Pb	0.35	Sr	1.9	Ca	2.1	Cu	3.1											O	Y		1	1989																											2	Bi2223				5.413		37.1													107	112					112																																																																																		0.8				0.00000000125			0.0000000027	1.8				BI2O3,PB3O4,SRCO3,CACO3,CUO	1	BI-PB-SR-CA-CU=1.85-0.35-1.9-2.1-3.1 NOMINAL COMP.					STUDY ON THE PREPARATION AND THE PHYSICAL PROPERTIES OF A 110K (BI,PB)(2)SR(2)CA(2)CU(3)O(Y) SUPERCONDUCTOR	198904	PLASMA FREQUENCY         ,HALL EFFECT              ,SINGLE PHASE             ,PR	DEPARTMENT OF APPLIED PHYSICS,THE UNIVERSITY OF TOKYO,7-3-1 HON-GO,BUNKYO-KU,TOKYO	JJAP LETT.,28(1989)L576	ATSUTAKA MAEDA,KAZUYOSHI NODA,KUNIMITSU UCHINOKURA,SHOJI TANAKA	BI,PB,SR,CA,CU,O	
1556	PHC1560761	THPOW77=100K	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123				3.82	3.89	11.68													88	89.5					89.5																																																																																															0	FINAL TREATMENT=SINGLE CRYSTAL ANN(950C 70H)					STUDU OF THE SUPERCONDUCTING TRANSITION IN YBA2CU3O7-Z SINGLECRYSTAL BY THERMOPOWRT MEASUREMENTS				PHYSICA C,156(1988)761	DUAN HONG-MIN,LIN SHU-YUAN,LU LI,MA BEI-HAI,ZHANG DIAN-LIN		
1557	PHC1670107	LN=PR,SM,LA, SAME STRUCTURE,NOT SUPERCOND.		Pb2Sr2Nd1Ce1Cu3O10+Y	Pb	2	Sr	2	Nd	1	Ce	1	Cu	3											O	10+Y		1	1990																												Pb3222	FMMM			5.442	5.462	36.9																																																																																																																	PBO,SR2CUO3,LN2O3,CEO2,CUO	1	(900C 12H IN N2)					PB2SR2LNCECU3O10+Z A NEW MEMBER OF THE LAYERED CUPRATES FAMILY, BUILT UP FROM DOUBLE FLUORITE-TYPE LAYERS		LAYERED CUPRATES    ,FLUORITE-TYPE	LABORATOIRE CRISMAT,ISMRA CAMPUS 2,UNIVERSITE DE CAEN,BOULEVARD DU MARECHAL JUIN,14032 CAEN CEDEX,FRANCE	PHYSICA C,167(1990)107	B.RAVEAU,C.MICHEL,D.GROULT,M.HERVIEU,T.ROUILLON	PB,SR,LN,SE,CU,O	
1558	PRB0394316		Bi2Sr2CaCu2O8	Bi4Sr4Ca2Cu4O16.25	Bi	4	Sr	4	Ca	2	Cu	4													O	16+Y	16.25		1989																												Bi2212				5.412		30.843														82.4					82.4																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1559	PRB0394316		Bi2Sr2(Ca,Tm)Cu2O8	Bi4Sr4Ca1.9Tm0.1Cu4O16.28	Bi	4	Sr	4	Ca	1.9	Tm	0.1	Cu	4											O	16+Y	16.28		1989																												Bi2212				5.406		30.777														83.9					83.9																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1560	PRB0394316		Bi2Sr2(Ca,Tm)CuO8	Bi4Sr4Ca1.8Tm0.2Cu4O16.38	Bi	4	Sr	4	Ca	1.8	Tm	0.2	Cu	4											O	16+Y	16.38		1989																												Bi2212				5.403		30.738														83.9					83.9																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1561	PRB0394316		Bi2Sr2(Ca,Tm)Cu2O8	Bi4Sr4Ca1.5Tm0.5Cu4O16.5	Bi	4	Sr	4	Ca	1.5	Tm	0.5	Cu	4											O	16+Y	16.5		1989																												Bi2212				5.405		30.671														84.3					84.3																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1562	PRB0394316		Bi2Sr2(Ca,Tm)Cu2O8	Bi4Sr4Ca1Tm1Cu4O16.67	Bi	4	Sr	4	Ca	1	Tm	1	Cu	4											O	16+Y	16.67		1989																												Bi2212				5.419		30.452														37.7					37.7																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1563	PRB0394316		Bi2Sr2(Ca,Tm)Cu2O8	Bi4Sr4Ca0.5Tm1.5Cu4O16.91	Bi	4	Sr	4	Ca	0.5	Tm	1.5	Cu	4											O	16+Y	16.91		1989																												Bi2212				5.423		30.252														1.5					1.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1564	PRB0394316		Bi2Sr2(Ca,Eu)Cu2O8	Bi4Sr4Ca1.5Eu0.5Cu4O16+Y	Bi	4	Sr	4	Ca	1.5	Eu	0.5	Cu	4											O	16+Y			1989																												Bi2212																				84.3					84.3																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1565	PRB0394316		Bi2Sr2(Ca,Eu)Cu2O8	Bi4Sr4Ca1Eu1Cu4O16+Y	Bi	4	Sr	4	Ca	1	Eu	1	Cu	4											O	16+Y			1989																												Bi2212																				28.5					28.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1566	PRB0394316		Bi2Sr2(Ca,Eu)Cu2O8	Bi4Sr4Ca0.5Eu1.5Cu4O16+Y	Bi	4	Sr	4	Ca	0.5	Eu	1.5	Cu	4											O	16+Y			1989																												Bi2212																				1.5					1.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1567	PRB0394316		Bi2Sr2(Ca,Er)Cu2O8	Bi4Sr4Ca1.5Er0.5Cu4O16+Y	Bi	4	Sr	4	Ca	1.5	Er	0.5	Cu	4											O	16+Y			1989																												Bi2212																				84.3					84.3																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1568	PRB0394316		Bi2Sr2(Ca,Er)Cu2O8	Bi4Sr4Ca1Er1Cu4O16+Y	Bi	4	Sr	4	Ca	1	Er	1	Cu	4											O	16+Y			1989																												Bi2212																				32.9					32.9																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1569	PRB0394316		Bi2Sr2(Ca,Er)Cu2O8	Bi4Sr4Ca0.5Er1.5Cu4O16+Y	Bi	4	Sr	4	Ca	0.5	Er	1.5	Cu	4											O	16+Y			1989																												Bi2212																				1.5					1.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1570	PRB0394316		Bi2Sr2(Ca,Ho)Cu2O8	Bi4Sr4Ca1.5Ho0.5Cu4O16+Y	Bi	4	Sr	4	Ca	1.5	Ho	0.5	Cu	4											O	16+Y			1989																												Bi2212																				84.3					84.3																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1571	PRB0394316		Bi2Sr2(Ca,Ho)Cu2O8	Bi4Sr4Ca1Ho1Cu4O16+Y	Bi	4	Sr	4	Ca	1	Ho	1	Cu	4											O	16+Y			1989																												Bi2212																				40.7					40.7																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1572	PRB0394316		Bi2Sr2(Ca,Ho)Cu2O8	Bi4Sr4Ca0.5Ho1.5Cu4O16+Y	Bi	4	Sr	4	Ca	0.5	Ho	1.5	Cu	4											O	16+Y			1989																												Bi2212																				1.5					1.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1573	PRB0394316			Bi4Sr4Ca3Cu4O16.29	Bi	4	Sr	4	Ca	3	Cu	4													O	16+Y	16.29		1989																																5.404		30.693														81					81																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1574	PRB0394316			Bi4Sr3Ca2.9Tm0.1Cu4O16.36	Bi	4	Sr	3	Ca	2.9	Tm	0.1	Cu	4											O	16+Y	16.36		1989																																5.4		30.667														80					80																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1575	PRB0394316			Bi4Sr3Ca2.8Tm0.2Cu4O16.41	Bi	4	Sr	3	Ca	2.8	Tm	0.2	Cu	4											O	16+Y	16.41		1989																																5.393		30.596														83					83																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1576	PRB0394316			Bi4Sr3Ca2.5Tm0.5Cu4O16.52	Bi	4	Sr	3	Ca	2.5	Tm	0.5	Cu	4											O	16+Y	16.52		1989																																5.399		30.465														81					81																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1577	PRB0394316			Bi4Sr3Ca2Tm1Cu4O16.73	Bi	4	Sr	3	Ca	2	Tm	1	Cu	4											O	16+Y	16.73		1989																																5.399		30.309														46.5					46.5																																																																																														CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1578	PRB0394316			Bi4Sr3Ca1.5Tm1.5Cu4O16.88	Bi	4	Sr	3	Ca	1.5	Tm	1.5	Cu	4											O	16+Y	16.88		1989																																5.408		30.265																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1579	PRB0394316			Bi4Sr3Ca1Tm2Cu4O17.18	Bi	4	Sr	3	Ca	1	Tm	2	Cu	4											O	16+Y	17.18		1989																																5.409		30.187																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1580	PRB0394316		BI4SR4ER2CU4O16	Bi4Sr4Er2Cu4O16+Y	Bi	4	Sr	4	Er	2	Cu	4													O	16+Y			1989						9.39	14																					Bi2212				3.841		30.156																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1581	PRB0394316		BI4SR4TM2CU4O16	Bi4Sr4Tm2Cu4O17.14	Bi	4	Sr	4	Tm	2	Cu	4													O	16+Y	17.14		1989						7.66	32																					Bi2212				3.824		30.173																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1582	PRB0394316		BI4SR4YB2CU4O16	Bi4Sr4Yb2Cu4O16+Y	Bi	4	Sr	4	Yb	2	Cu	4													O	16+Y			1989																												Bi2212				3.85		30.474																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1583	PRB0394316		BI4SR4LU2CU4O16	Bi4Sr4Lu2Cu4O16+Y	Bi	4	Sr	4	Lu	2	Cu	4													O	16+Y			1989																												Bi2212				3.812		30.316																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1584	PRB0394316	NOT SUPERCOND.	BI4SR4GD2CU4O16	Bi4Sr4Gd2Cu4O16+Y	Bi	4	Sr	4	Gd	2	Cu	4													O	16+Y			1989						7.84	2																					Bi2212				3.855		30.248																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1585	PRB0394316		BI4SR4DY2CU4O16	Bi4Sr4Dy2Cu4O16+Y	Bi	4	Sr	4	Dy	2	Cu	4													O	16+Y			1989						10.23	8																					Bi2212				3.853		30.162																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1586	PRB0394316		BI4SR4Y2CU4O16	Bi4Sr4Y2Cu4O16+Y	Bi	4	Sr	4	Y	2	Cu	4													O	16+Y			1989						0.5																						Bi2212				3.853		30.152																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1587	PRB0394316		BI4SR4TB2CU4O16	Bi4Sr4Tb2Cu4O16+Y	Bi	4	Sr	4	Tb	2	Cu	4													O	16+Y			1989						7.66	13																					Bi2212				3.85		30.232																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1588	PRB0394316		BI4SR4HO2CU4O16	Bi4Sr4Ho2Cu4O16+Y	Bi	4	Sr	4	Ho	2	Cu	4													O	16+Y			1989						10.23	13																					Bi2212				3.843		30.025																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1589	PRB0394316		BI4SR4LA2CU4O16	Bi4Sr4La2Cu4O16+Y	Bi	4	Sr	4	La	2	Cu	4													O	16+Y			1989																												Bi2212				3.875		30.592																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1590	PRB0394316		BI4SR4PR2CU4O16	Bi4Sr4Pr2Cu4O16+Y	Bi	4	Sr	4	Pr	2	Cu	4													O	16+Y			1989						2.96	16																					Bi2212				3.877		30.366																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1591	PRB0394316		BI4SR4ND2CU4O16	Bi4Sr4Nd2Cu4OZ	Bi	4	Sr	4	Nd	2	Cu	4													O	Z			1989						2.97	30																				2	Bi2212				3.872		30.287																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1592	PRB0394316		BI4SR4SM2CU4O16	Bi4Sr4Sm2Cu4OZ	Bi	4	Sr	4	Sm	2	Cu	4													O	Z			1989																											2	Bi2212				3.867		30.296																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1593	PRB0394316		BI4SR4EU2CU4O16	Bi4Sr4Eu2Cu4OZ	Bi	4	Sr	4	Eu	2	Cu	4													O	Z			1989																											2	Bi2212				3.863		30.138																																																																																																																	CACO3,SRCO3,BI2O3,CUO,R2O3	0	HEAT TREATMENT IN AIR,ANN(860C) EXCEPT FOR TM AND LU COMPOUND ANN(900C)					BISMUTH CUPRATE HIGH-T(C) SUPERCONDUCTORS USING CATIONIC SUBSTI-TUTION	198903	TC                       ,STRUCTURE                ,VALENCE                  ,SU	BELLCORE,RED BANK,NEW JERSEY	PHYSICAL REVIEW B.,39(1989)4316	G.W.HULL,J.-M.TARASCON,L.H.GREENE,M-.S.HEGDE,M.GIROUD,P.BARBOUX,R.RAMESH,W.R.MCKINNON	R,BI,SR,CA,CU,O,FE,CO	
1594	PHC1650055		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.7Y0.3Cu2O8.25	Bi	1.7	Pb	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	8+Z	8.25		1990																												Bi2212				5.411	5.414	30.471														71					71																																																																																														BI2O3,PBO,SR(NO3)2,CA(OH)2,CUO	0	MOTHER COMPOUND PREPARED BY:(850C 16H IN AIR)-(850C 72H IN AIR)-Q,OXYGEN CONTROL BY ANN(600C IN VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1595	PHC1650055		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.7Y0.3Cu2O8.25	Bi	1.7	Pb	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	8+Z	8.25		1990																												Bi2212				5.409	5.424	30.456														72					72																																																																																														BI2O3,PBO,SR(NO3)2,CA(OH)2,CUO	0	MOTHER COMPOUND PREPARED BY:(850C 16H IN AIR)-(850C 72H IN AIR)-Q,OXYGEN CONTROL BY ANN(600C IN VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1596	PHC1650055		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.7Y0.3Cu2O8.26	Bi	1.7	Pb	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	8+Z	8.26		1990																												Bi2212				5.407	5.411	30.446														73					73																																																																																														BI2O3,PBO,SR(NO3)2,CA(OH)2,CUO	0	MOTHER COMPOUND PREPARED BY:(850C 16H IN AIR)-(850C 72H IN AIR)-Q,OXYGEN CONTROL BY ANN(600C IN VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1597	PHC1520223			Tl5Ba5Ca2Cu6OX	Tl	5	Ba	5	Ca	2	Cu	6													O	X		1	1988									7.43																		3	Tl5526				3.862	3.863	29.306														106	110				106			K/kbar	0.23						60																																																																																				TL2O3,BAO,CAO,CUO	1	TL-BA-CA-CU=2-1-1-2 IN PT CRUCIBLE - HEAT TO 950C-HOLD 30MIN-COOL TO 900C-HOLD 1H-C(10C/H) TO 750C-FC					SINGLE CRYSTALS OF TL5BA5CA2CU6OX:106 K SUPERCONDUCTOR				PHYSICA C,152(1988)223	BAUGHMAN.R.J,GINLEY.D.S,HLAVA.P.F,KWAK.J.F,MOROSIN.B,SCHIRBER.J.E,VENTURINI.E.L		
1598	PHC1520339		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7-Z	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z		1	1988																											3	Y123																				84					84			K/kbar	0.19																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1599	PHC1520339		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				91					91			K/kbar	0.11																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1600	PHC1610123		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OX	Bi	2	Sr	2	Ca	2	Cu	3													O	X		2	1989																											2	Bi2223				3.822		37.04													105.7						105.7													65																									7					400										SP1600																																	0.00000000382					RH1600			BI2O3,PBO,SRCO3,CACO3,CUO	1	6-7%2212 PHASE,7%CU2PBO4,<5%CUO					SUPERCONDUCTING FLUCTUATIONS IN Bi2Sr2Ca2Cu3Ox			"II. Physikalisches Institut der Universitat zu Ko""ln, 5000 Ko""ln 41, Fed. Rep. Germany"	Physica.C,161(1989)123-135	A. WALDORF,D. WOHLLEBEN,E. BRAUN,F. SEIDLER,H. BROICHER,H. GEUS,H. WEISS,M. GALFFY,S. RUPPEL,W. BRAUNISCH,W. SCHNELLE		
1601	PHC1520339		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O7-Z	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z		1	1988																											3	Y123																												K/kbar	0.26																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1602	PHC1520339		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.895Fe0.105O7-Z	Y	1	Ba	2	Cu	2.895	Fe	0.105													O	7-Z		1	1988																											2	Y123																				63					63			K/kbar	0.56																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1603	PHC1520339		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18O7-Z	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	7-Z		1	1988																											2	Y123																												K/kbar	0.61																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1604	PHC1520339		YBa2(Cu,Co)3O7	Y1Ba2Cu2.901Co0.099O7-Z	Y	1	Ba	2	Cu	2.901	Co	0.099													O	7-Z		1	1988																											2	Y123																				70					70			K/kbar	0.62																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1605	PHC1520339		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.955Zn0.045O7-Z	Y	1	Ba	2	Cu	2.955	Zn	0.045													O	7-Z		1	1988																											3	Y123																				67					67			K/kbar	0.14																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1606	PHC1520339		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.82Zn0.18O7-Z	Y	1	Ba	2	Cu	2.82	Zn	0.18													O	7-Z		1	1988																											3	Y123																				35					35			K/kbar	0.16																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1607	PHC1520339		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7-Z	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7-Z		1	1988																											3	Y123																				83					83																																																																																														Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1608	PHC1520339		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.82Ni0.18O7-Z	Y	1	Ba	2	Cu	2.82	Ni	0.18													O	7-Z		1	1988																											3	Y123																												K/kbar	0.14																																																																																										Y2O3,BACO3,CUO,FE2O3,CO2O3,NIO,ZNO	1						PRESSURE DEPENDENCES OF SUPERCONDUCTING TRANSITION TEMPERATURETC IN ORTHORHOMBIC AND IMPURITY-INDUCED TETRAGONAL YBA2(CU1-XMX)3O7-Y(M=FE,CO,NI AND ZN)				PHYSICA C,152(1988)339	FUJITA.T,KUMAGAI.K,KURISU.M,MAENO.Y		
1609	PHC1560113		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1988																											2	Tl2212				3.847		29.43													109.2	113.1	117.1			8.1	113.1			K/kbar	0.2																																																																																										TL2O3,BAO,CAO,CUO	1	SIN(820C 10H)-C					PRESSURE EFFECTS ON THE NEW HIGH-TC SUPERCONDUCTOR TL-BA-CA-CU-O				PHYSICA C,156(1988)113	HAN.H,HAN.S.H,LIU.Y,ZHANG.Y.L		
1610	PHC1560448	PLATE LIKE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X		3	1988									6.5																		3	Bi2212				5.427	5.441	30.77													80	85					85			K/kbar	0.2																			410	40								7	0.7						9	29																																											1.6	600										SRCO3,CUO,BI2O3,CAO	1	NOMINAL SR-CA-BI-CU=1-1-1-2,(800-850C 6H IN AIR)-SIN(820C 6H)					PRESSURE EFFECTS, ANISOTROPIC TRANSPORT PROPERTIES AND UPPER CRITICAL FIELDS OF BI2SR2CACU2O8+C SINGLE CRYSTALS-CHARACTERIZATION OF NEEDLE-LIKE BI-SR-CA-CU-O CRYSTALS				PHYSICA C,156(1988)448	BEILLE.J,DUPENDANT.H,LABORDE.O,LEFUR.Y,PERROUX.M,TOURNIER.R,WANG.J.H,YEN.Y.F,ZHAO.Z,ZHENG.D.N		
1611	PHC1560448	SEMI-COND. LIKE RESISTIVITY. IN SOLDER CONTACT	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X		3	1988																											3	Bi2212				5.427	5.441	30.77														82					82			K/kbar	0.2																																																																																																	PRESSURE EFFECTS, ANISOTROPIC TRANSPORT PROPERTIES AND UPPER CRITICAL FIELDS OF BI2SR2CACU2O8+C SINGLE CRYSTALS-CHARACTERIZATION OF NEEDLE-LIKE BI-SR-CA-CU-O CRYSTALS				PHYSICA C,156(1988)448	BEILLE.J,DUPENDANT.H,LABORDE.O,LEFUR.Y,PERROUX.M,TOURNIER.R,WANG.J.H,YEN.Y.F,ZHAO.Z,ZHENG.D.N		
1612	PHC1660019	LAT=305K,LATA=3.8444,LATC=9.0744(15K)		Tl1Ba1.2La0.8Cu1O5	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5			1990																													P4/MMM			3.848		9.091														52					52																																																																																														TL2O3,CUO,LA2O3,BA-PEROXIDE	0						TLBA1.2LA0.8CUO5: A SUPERCONDUCTOR PRODUCED BY REDUCTION, RATHER THAN OXIDATION, OF THE CUO2 PLANES			E.I. DU PONT DE NEMOURS, EXPERIMENTAL STATION, P.O. BOX 80262,WILMINGTON, DE 19880-0262, USA	PHYSICA C,166(1990)19	G.H.KWEI,J.A.GOLDSTONE,J.B.PARISE,M.A.SUBRAMANIAN,R.B.VON DREELE	TL,BA,LA,CU,O	
1613	PHC1660015	1X1.5X0.3MM3 TUNGSTEN NEEDLE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X		3	1990																												Bi2212																			80						80																																																7.8	1																																														0	MIXTURE-(950C IN AIR)-C(1C/H) TO BELOW 600C					SUPERCONDUCTING ENERGY GAP OF SINGLE-CRYSTAL BI2XR2CA1CU2O8+ZBY ELECTRON TUNNELING			INSTITUTO DE INVESTIGACIONES EN MATERIALES. UNIJVERSIDAD NACIONAL AUTONOMA DE MEXICO, A. POSTAL 70-360 MEXICO.	PHYSICA C,166(1990)15	E.GUARNER,F.MORALES,R.ESCUDERO	BI,SR,CA,CU,O	
1614	PHC1650055		Bi2(Sr,Ca)2Cu2O8	Bi2Sr1.5Ca1.5Cu2O8.19	Bi	2	Sr	1.5	Ca	1.5	Cu	2													O	8+X	8.19		1990																											3	Bi2212				5.402	5.408	30.699														83					83																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1615	PHC1650055		Bi2(Sr,Ca)2Cu2O8	Bi2Sr1.5Ca1.5Cu2O8.22	Bi	2	Sr	1.5	Ca	1.5	Cu	2													O	8+X	8.22		1990																											3	Bi2212				5.396	5.4	30.635														73					73																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1616	PHC1650055		Bi2(Sr,Ca)2Cu2O8	Bi2Sr1.5Ca1.5Cu2O8.25	Bi	2	Sr	1.5	Ca	1.5	Cu	2													O	8+X	8.25		1990																											3	Bi2212				5.396	5.404	30.618														67					67																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1617	PHC1650055		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X			1990																											3	Bi2212				5.407	5.415	30.874														83					83																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1618	PHC1650055		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X			1990																											3	Bi2212				5.401	5.408	30.788														68					68																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1619	PHC1650055		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X			1990																											3	Bi2212				5.401	5.412	30.781														64					64																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1620	PHC1650055		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8.33	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8+Z	8.33	1	1990																											3	Bi2212	FMMM	69		5.416	5.439	30.43														40					40																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1621	PHC1650055	T2<4K	Bi2SR2(Ca,Y)Cu2O8	Bi2Sr2Ca0.25Y0.75Cu2O8.41	Bi	2	Sr	2	Ca	0.25	Y	0.75	Cu	2											O	8+Z	8.41	1	1990																											3	Bi2212				5.424	5.454	30.28																																																																																																																		0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1622	PHC1650055	T2<4K	Bi2Sr2YCu2O8	Bi2Sr2Y1Cu2O8.51	Bi	2	Sr	2	Y	1	Cu	2													O	8+Z	8.51	1	1990																											3	Bi2212				5.432	5.471	30.204																																																																																																																		0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1623	PHC1650055	DENS=60% OF X-RAY DENS	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.23	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.23	1	1990																											3	Bi2212		69		5.403	5.407	30.851														70					70																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1624	PHC1650055		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8.23	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8+Z	8.23	1	1990																											3	Bi2212				5.407	5.416	30.807														90					90																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1625	PHC1650055		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8.3	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+Z	8.3	1	1990																											3	Bi2212				5.41	5.425	30.619														86					86																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1626	PHC1650055		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.65Y0.35Cu2O8.3	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	2											O	8+Z	8.3	1	1990																											3	Bi2212				5.412	5.428	30.54														74					74																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1627	PHC1650055		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8.29	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+Z	8.29	1	1990																											3	Bi2212				5.414	5.431	30.52														64					64																																																																																															0	SPRAY-DRYING TECHNIQUE,METAL NITRATE-SPRAY(200C)-CAL(850C16H)-OXYGEN CONTROL BY ANN(600C AT VARIOUS O2 PRESSURE)					HOLE CONCENTRATION AND TC IN BI2SR2CACU2O8+Z				PHYSICA C,165(1990)55	DE LEEUW.D.M,FEINER.L.F,GROEN.W.A		
1628	PHC1660009	MOMENT/ER	ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	Z	7	1	1990						4.8		0.62																			3	Y123																				92					92																																																																																														ER2O3,BACO3,CUO	1	HEAT(4K/MIN) TO 1228K-(1228K 24H IN O2)-ANN(1228K 24H IN AIR)-C(0.5K/MIN),OXYGEN CONTROL BY ANN(IN VARIOUS O2 PRESSURE)					2-D AND 3-D MAGNETIC ORDERING OF ER IN ERBA2CU3OX(6-<X-<7)			INSTITUTE FUR FESTLORPERFORSCHUNG, KFA JULICH, 5170 JULICH, FED. REP. GERMANY	PHYSICA C,166(1990)9	E.PORSCHKE,H.MALETTA,P.J.BROWN,T.CHATTOPADHYAY	ER,BA,CU,O	
1629	PHC1660009	MOMENT/ER	ErBa2Cu3O7	Er1Ba2Cu3O6.87	Er	1	Ba	2	Cu	3															O	Z	6.87	1	1990						4.4		0.585																			3	Y123																																																																																																																							ER2O3,BACO3,CUO	1	HEAT(4K/MIN) TO 1228K-(1228K 24H IN O2)-ANN(1228K 24H IN AIR)-C(0.5K/MIN),OXYGEN CONTROL BY ANN(IN VARIOUS O2 PRESSURE)					2-D AND 3-D MAGNETIC ORDERING OF ER IN ERBA2CU3OX(6-<X-<7)			INSTITUTE FUR FESTLORPERFORSCHUNG, KFA JULICH, 5170 JULICH, FED. REP. GERMANY	PHYSICA C,166(1990)9	E.PORSCHKE,H.MALETTA,P.J.BROWN,T.CHATTOPADHYAY	ER,BA,CU,O	
1630	PHC1660009	MOMENT/ER	ErBa2Cu3O7	Er1Ba2Cu3O6.64	Er	1	Ba	2	Cu	3															O	Z	6.64	1	1990						3.9		0.53																				Y123																																																																																																																							ER2O3,BACO3,CUO	1	HEAT(4K/MIN) TO 1228K-(1228K 24H IN O2)-ANN(1228K 24H IN AIR)-C(0.5K/MIN),OXYGEN CONTROL BY ANN(IN VARIOUS O2 PRESSURE)					2-D AND 3-D MAGNETIC ORDERING OF ER IN ERBA2CU3OX(6-<X-<7)			INSTITUTE FUR FESTLORPERFORSCHUNG, KFA JULICH, 5170 JULICH, FED. REP. GERMANY	PHYSICA C,166(1990)9	E.PORSCHKE,H.MALETTA,P.J.BROWN,T.CHATTOPADHYAY	ER,BA,CU,O	
1631	PHC1660009	MOMENT/ER	ErBa2Cu3O7	Er1Ba2Cu3O6.53	Er	1	Ba	2	Cu	3															O	Z	6.53	1	1990						3.7		0.46																				Y123																																																																																																																							ER2O3,BACO3,CUO	1	HEAT(4K/MIN) TO 1228K-(1228K 24H IN O2)-ANN(1228K 24H IN AIR)-C(0.5K/MIN),OXYGEN CONTROL BY ANN(IN VARIOUS O2 PRESSURE)					2-D AND 3-D MAGNETIC ORDERING OF ER IN ERBA2CU3OX(6-<X-<7)			INSTITUTE FUR FESTLORPERFORSCHUNG, KFA JULICH, 5170 JULICH, FED. REP. GERMANY	PHYSICA C,166(1990)9	E.PORSCHKE,H.MALETTA,P.J.BROWN,T.CHATTOPADHYAY	ER,BA,CU,O	
1632	PHC1660185		TmBa2Cu3O7	Tm1Ba2Cu3OZ	Tm	1	Ba	2	Cu	3															O	Z		3	1990																												Y123																					92				92												DEVIATION FROM LINEAR M-H CURVE		410	1800																																																																																0						TEMPERATURE DEPENDENCES OF THE FIRST CRITICAL FIELD AND CRITICAL CURRENT IN THE UNTWINNED TMBA2CU3OX SUPERCONDUCTING SINGLECRYSTALS			LABORATORY OF HIGH-TC SUPERCONDUCTIVITY,PHYSICS DEPARTMENT, MOSCOW STATE UMIVERSITY, MOSCOW 117234, USSR	PHYSICA C,166(1990)185	A.A.ZHUKOV,D.K.PETROV,V.I.VORONKOVA,V.K.YANOVSKII,V.V.MOSHCHALKOV	TM,BA,CU,O	
1633	PHC1480404	MAGNETIC CONTRIBUTION TO SP. HEAT	GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z		1	1987								2.29																			3	Y123				3.845	3.908	11.728														91.1					91.1																																																																																														R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1634	PHC1480404		GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z		1	1987								2.23																			2	Y123				3.88		11.85																																																																																																																	R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1635	PHC1480404		DyBa2Cu3O7	Dy1Ba2Cu3OZ	Dy	1	Ba	2	Cu	3															O	Z		1	1987								0.88																			3	Y123				3.831	3.894	11.693														91.8					91.8																																																																																														R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1636	PHC1480404		DyBa2Cu3O7	Dy1Ba2Cu3OZ	Dy	1	Ba	2	Cu	3															O	Z		1	1987								0.82																			2	Y123				3.869		11.827																																																																																																																	R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1637	PHC1480404		HoBa2Cu3O7	Ho1Ba2Cu3OZ	Ho	1	Ba	2	Cu	3															O	Z		1	1987																											3	Y123				3.828	3.89	11.683														92.4					92.4																																																																																														R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1638	PHC1480404		HoBa2Cu3O7	Ho1Ba2Cu3OZ	Ho	1	Ba	2	Cu	3															O	Z		1	1987																											2	Y123				3.867		11.827																																																																																																																	R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1639	PHC1480404	MAGNETIC CONTRIBUTION TO SP HEAT	ErBa2Cu3O7	Er1Ba2Cu3OZ	Er	1	Ba	2	Cu	3															O	Z		1	1987								0.62																			3	Y123				3.823	3.887	11.668														92.5					92.5																																																																																														R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1640	PHC1480404		ErBa2Cu3O7	Er1Ba2Cu3OZ	Er	1	Ba	2	Cu	3															O	Z		1	1987								0.61																			2	Y123				3.862		11.822																																																																																																																	R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1641	PHC1480404		TmBa2Cu3O7	Tm1Ba2Cu3OZ	Tm	1	Ba	2	Cu	3															O	Z		1	1987																											3	Y123				3.814		11.676														91.8					91.8																																																																																														R2O3,BACO3,CUO	1	SIN(900C)-SLOW COOL OR Q					Low-temperature specific heat of orthorhombic and tetragonal phases of Ba2(RE)Cu3O7-d (RE=Gd, Dy, Ho, ErandTm)				Physica C,148(1987)404-407	Y.Nakazawa,M.Ishikawa,T.Takabatake		
1642	PR04111209		YBa2Cu4O8	Y1Ba2Cu4O7.8	Y	1	Ba	2	Cu	4															O	8	7.8	1	1990																											3	Y124				3.836	3.872	27.224													75		80				77.5																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1643	PR04111209		Y(Ba,Sr)2Cu4O8	Y1Ba1.9Sr0.1Cu4O7.9	Y	1	Ba	1.9	Sr	0.1	Cu	4													O	8	7.9	1	1990																											3	Y124				3.823	3.868	27.194													75		81				78																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1644	PR04111209		Y(Ba,Sr)2Cu4O8	Y1Ba1.8Sr0.2Cu4O7.9	Y	1	Ba	1.8	Sr	0.2	Cu	4													O	8	7.9	1	1990																											3	Y124				3.82	3.866	27.176													74		82				78																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1645	PR04111209		Y(Ba,Sr)2Cu4O8	Y1Ba1.6Sr0.4Cu4O7.9	Y	1	Ba	1.6	Sr	0.4	Cu	4													O	8	7.9	1	1990																											3	Y124				3.805	3.862	27.122													76		82				79																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1646	PR04111673		(Eu,Ce)4(La,Ba,Sr)4Cu6Oz	Eu2.67Ce1.33La1.33Ba1.33Sr1.33Cu6OZ	Eu	2.67	Ce	1.33	La	1.33	Ba	1.33	Sr	1.33	Cu	6									O	Z		1	1990																												446																				28.5					28.5																																																																											3.04							3.56									HA1646				1	HEAT IN 3ATM O2-STEP-WISE COOLING AS (900C 1H)+(600C 10H)+(400C 20H)					ANOMALOUS TEMPERATURE DEPENDENCE OF HALL COEFFICIENTS FOR (L2/3CE1/3)4(LA1/3BA1/3SR1/3)4CU6OY(L=EU,DY,Y,AND HO)	199006	HALL EFFECT         ,CRYSTAL STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,41(1990)11673	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,S.IKEGAWA,S.TANAKA,T.KANEKO,T.SAKURAI,T.WADA,T.YAMASHITA,Y.YAEGUSHI	CE,LA,BA,SR,CU,O,EU,DY,Y,HO	
1647	PR04111673		(Dy,Ce)4(La,Ba,Sr)4Cu6Oz	Dy2.67Ce1.33La1.33Ba1.33Sr1.33Cu6OZ	Dy	2.67	Ce	1.33	La	1.33	Ba	1.33	Sr	1.33	Cu	6									O	Z		1	1990																												446																				6					6																																																																											4							4.52									HA1647				1	HEAT IN 3ATM O2-STEP-WISE COOLING AS (900C 1H)+(600C 10H)+(400C 20H)					ANOMALOUS TEMPERATURE DEPENDENCE OF HALL COEFFICIENTS FOR (L2/3CE1/3)4(LA1/3BA1/3SR1/3)4CU6OY(L=EU,DY,Y,AND HO)	199006	HALL EFFECT         ,CRYSTAL STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,41(1990)11673	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,S.IKEGAWA,S.TANAKA,T.KANEKO,T.SAKURAI,T.WADA,T.YAMASHITA,Y.YAEGUSHI	CE,LA,BA,SR,CU,O,EU,DY,Y,HO	
1648	PR04111673	T2<6K	(Y,Ce)4(La,Ba,Sr)4Cu6OZ	Y2.67Ce1.33La1.33Ba1.33Sr1.33Cu6OZ	Y	2.67	Ce	1.33	La	1.33	Ba	1.33	Sr	1.33	Cu	6									O	Z		1	1990																												446																																																																																																				4							4.52									HA1648				1	HEAT IN 3ATM O2-STEP-WISE COOLING AS (900C 1H)+(600C 10H)+(400C 20H)					ANOMALOUS TEMPERATURE DEPENDENCE OF HALL COEFFICIENTS FOR (L2/3CE1/3)4(LA1/3BA1/3SR1/3)4CU6OY(L=EU,DY,Y,AND HO)	199006	HALL EFFECT         ,CRYSTAL STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,41(1990)11673	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,S.IKEGAWA,S.TANAKA,T.KANEKO,T.SAKURAI,T.WADA,T.YAMASHITA,Y.YAEGUSHI	CE,LA,BA,SR,CU,O,EU,DY,Y,HO	
1649	PR04111673	T2<6K	(Ho,Ce)4(La,Ba,Sr)4Cu6Oz	Ho2.67Ce1.33La1.33Ba1.33Sr1.33Cu6OZ	Ho	2.67	Ce	1.33	La	1.33	Ba	1.33	Sr	1.33	Cu	6									O	Z		1	1990																												446																																																																																																				5.8							5.25									HA1649				1	HEAT IN 3ATM O2-STEP-WISE COOLING AS (900C 1H)+(600C 10H)+(400C 20H)					ANOMALOUS TEMPERATURE DEPENDENCE OF HALL COEFFICIENTS FOR (L2/3CE1/3)4(LA1/3BA1/3SR1/3)4CU6OY(L=EU,DY,Y,AND HO)	199006	HALL EFFECT         ,CRYSTAL STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,41(1990)11673	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,S.IKEGAWA,S.TANAKA,T.KANEKO,T.SAKURAI,T.WADA,T.YAMASHITA,Y.YAEGUSHI	CE,LA,BA,SR,CU,O,EU,DY,Y,HO	
1650	PR04111209		Y(Ba,Sr)2Cu4O8	Y1Ba1.4Sr0.6Cu4O7.8	Y	1	Ba	1.4	Sr	0.6	Cu	4													O	8	7.8	1	1990																											3	Y124				3.802	3.86	27.068													74		83				78.5																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1651	PR04111209		Y(Ba,Sr)2Cu4O8	Y1Ba1.2Sr0.8Cu4O7.9	Y	1	Ba	1.2	Sr	0.8	Cu	4													O	8	7.9	1	1990																											3	Y124				3.799	3.856	27.021													75		83				79																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1652	PR04111209		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	1	1990																											3	Y123				3.823	3.892	11.684													91		94				92.5																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1653	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba1.8Sr0.2Cu3O6.8	Y	1	Ba	1.8	Sr	0.2	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.815	3.883	11.656													87		94				90.5																																																																																														Y2O3,CACO3,BA(NO3)2,SR(NO3)2,CUO	1	HIP,(AR+O2) 100MPA AT 1000C,CAL(900C 24H IN O2)-SIN(900C IN O2)-ANN(1000C (80%AR+20%O2) OF 100MPA) USING HIP					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1654	PR04111299	thermal expansion(figure): p=1 means ab-axis, p=2 means c-axis	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1990																											3	Y123																				90				2	90			K/GPa	1.77																																																	SP1654		27																																								5	AL2O3 CRUCIBLE,CUO-BAO FLUX FOR SINGLE CRYSTAL					ANISOTROPIC PRESSURE DEPENDENCE OF TC IN SINGLE-CRYSTAL YBA2CU3O7 VIA THERMAL EXPANSION	199006	THERMAL-EXPANSION   ,SINGLE-CRYSTALLINE	KERNFORSCHUNGSZENTRUM KARLSRUHE, INSTITUT FUR TECHNISCHE PHYSIK, AND UNIFERSITAT KARLSRUHE, 7500 KARLSRUHE, FEDERAL REPUBLICOF GERMANY	PHYS.REV.B,41(1990)11299	B.BLANK,B.OBST,C.MEINGAST,H.BURKLE,H.WUHL,K.SALAMA,T.WOLF,V.SELVAMANICKAM	Y,BA,CU,O	
1655	PR04111299	PRESSURE DEPENDENCE CALCULATED FROM THERMAL EXPANSION COEFF.,thermal expansion (figure): p=1 means a-axis oriented, p=2 for c-axis oriented	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1990																											3	Y123																				93.4				1	93.4			K/GPa	0.73																																																			43																																								5	AL2O3 CRUCIBLE,CUO-BAO FLUX FOR SINGLE CRYSTAL					ANISOTROPIC PRESSURE DEPENDENCE OF TC IN SINGLE-CRYSTAL YBA2CU3O7 VIA THERMAL EXPANSION	199006	THERMAL-EXPANSION   ,SINGLE-CRYSTALLINE	KERNFORSCHUNGSZENTRUM KARLSRUHE, INSTITUT FUR TECHNISCHE PHYSIK, AND UNIFERSITAT KARLSRUHE, 7500 KARLSRUHE, FEDERAL REPUBLICOF GERMANY	PHYS.REV.B,41(1990)11299	B.BLANK,B.OBST,C.MEINGAST,H.BURKLE,H.WUHL,K.SALAMA,T.WOLF,V.SELVAMANICKAM	Y,BA,CU,O	
1656	PR04111209		(Y,Ca)(Ba,Sr)2Cu4O8	Y0.95Ca0.05Ba1.6Sr0.4Cu4O7.8	Y	0.95	Ca	0.05	Ba	1.6	Sr	0.4	Cu	4											O	8	7.8	1	1990																											3	Y124				3.813	3.861	27.13													79		85				82																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1657	PR04111209		(Y,Ca)(Ba,Sr)2Cu4O8	Y0.9Ca0.1Ba1.6Sr0.4Cu4O7.8	Y	0.9	Ca	0.1	Ba	1.6	Sr	0.4	Cu	4											O	8	7.8	1	1990																											3	Y124				3.812	3.859	27.155													84		87				85.5																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1658	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba1.6Sr0.4Cu3O6.8	Y	1	Ba	1.6	Sr	0.4	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.805	3.875	11.624													86		91				88.5																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1659	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba1.4Sr0.6Cu3O6.8	Y	1	Ba	1.4	Sr	0.6	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.803	3.869	11.61													84		88				86																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1660	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba1.2Sr0.8Cu3O6.8	Y	1	Ba	1.2	Sr	0.8	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.792	3.859	11.578													84		88				86																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1661	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba1Sr1Cu3O6.8	Y	1	Ba	1	Sr	1	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.792	3.85	11.553													82		85				83.5																																																																																															1						PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1662	PR04111209		Y(Ba,Sr)2Cu3O7	Y1Ba0.8Sr1.2Cu3O6.8	Y	1	Ba	0.8	Sr	1.2	Cu	3													O	Z	6.8	1	1990																											3	Y123				3.781	3.842	11.527													81		83				82																																																																																																					PREPARATION AND PROPERTIES OF SUPERCONDUCTING Y(BA1-XSRX)2CU4O8	199006	SINGLE-PHASE        ,TC	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVIRY TECHNOLOGY CENTER, 10-13 SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.BA,41(1990)11209	HISAO YAMAUCHI,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKESHI SAKURAI	Y,BA,SR,CU,O	
1663	PHC1690237	SP FITTING FOR 4.5-9.5 K,SP MEASURED FOR T<90	YBa2Cu4O8	Y1Ba2Cu4O7.96	Y	1	Ba	2	Cu	4															O	8	7.96		1990																												Y124																			81	86	90				86		3								8		DEVIATION FROM LINEAR MAGNETIZATION	130																																								SP1663				5.7		380																			470				960													0	CITRATE-PYROLYSIS TECHNIQUE,SIN(825C 50H IN O2)					SPECIFIC-HEAT,RESISTIVITY AND MAGNETIZATION STUDY ON POLYCRYSTALLINE YBA2CU4O8			LABORATORIUM FUR FESKORPERPHYSIK, ETHZ,CH-8093 ZURICH, SWITZERLAND	PHYSICA C,169(1990)237	A.BERNASCONI,A.SCHILLING,F.HULLIGER,H.R.OTT	Y,BA,CU,O	
1664	PHC1680546		YBa2(Cu,W)3Oz	Y1Ba2Cu2W1O9-Z	Y	1	Ba	2	Cu	2	W	1													O	9-Z		1	1990																											1	Y123				8.332																																																																																																																			Y2O3,BACO3,CUO,WO3	0	(950C 24H IN AIR)-SIN(1050C 24H IN O2)-ANN(480C IN O2)-C					SYNTHESIS, STRUCTURE AND PROPERTIES OF THE NONSUPERCONDUCTOR YBA2 CU2 WO9-Z			THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JURUSALEM, JURUSALEM 91904, ISRAEL	PHYSICA C,168(1990)546	D.KOWAL,I.FELNER,M.EINAV,U.YARON	Y,BA,CU,W,O	
1665	PHC1680530		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z			1990																												T'																					18.4				18.4			K/GPa	0.07																											0.48																																																																0						EFFECT OF PRESSURE ON CRITICAL PARAMETERS OF ELECTRON-DOPED SUPERCONDUCTORS LN2-XMXCUO4-Y(LN=ND,SM,PR,M=CE,TH)			INSTITUTE FOR HIGH PRESSURE PHYSICS, USSR ACADEMY OF SCIENCES,TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C, 168(1990)530	A.E.LUPPOV,A.G.GAPOTCHENKO,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,S.L.BUD'KO	ND,SM,PR,CE,TH,CU,O	
1666	PHC1680530		(Nd,Th)2CuO4	Nd1.85Th0.15Cu1O4-Z	Nd	1.85	Th	0.15	Cu	1															O	4-Z			1990																												T'																					15.9				15.9			K/GPa	-0.4																											0.41																																																																0						EFFECT OF PRESSURE ON CRITICAL PARAMETERS OF ELECTRON-DOPED SUPERCONDUCTORS LN2-XMXCUO4-Y(LN=ND,SM,PR,M=CE,TH)			INSTITUTE FOR HIGH PRESSURE PHYSICS, USSR ACADEMY OF SCIENCES,TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C, 168(1990)530	A.E.LUPPOV,A.G.GAPOTCHENKO,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,S.L.BUD'KO	ND,SM,PR,CE,TH,CU,O	
1667	PHC1680530		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-Z	Sm	1.85	Ce	0.15	Cu	1															O	4-Z			1990																												T'																					21.1				21.1			K/GPa	-0.5																											0.49																																																																0						EFFECT OF PRESSURE ON CRITICAL PARAMETERS OF ELECTRON-DOPED SUPERCONDUCTORS LN2-XMXCUO4-Y(LN=ND,SM,PR,M=CE,TH)			INSTITUTE FOR HIGH PRESSURE PHYSICS, USSR ACADEMY OF SCIENCES,TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C, 168(1990)530	A.E.LUPPOV,A.G.GAPOTCHENKO,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,S.L.BUD'KO	ND,SM,PR,CE,TH,CU,O	
1668	PHC1680530		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Z	Pr	1.85	Ce	0.15	Cu	1															O	4-Z			1990																												T'																					22.4				22.4			K/GPa	0.2																											0.53																																																																0						EFFECT OF PRESSURE ON CRITICAL PARAMETERS OF ELECTRON-DOPED SUPERCONDUCTORS LN2-XMXCUO4-Y(LN=ND,SM,PR,M=CE,TH)			INSTITUTE FOR HIGH PRESSURE PHYSICS, USSR ACADEMY OF SCIENCES,TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C, 168(1990)530	A.E.LUPPOV,A.G.GAPOTCHENKO,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,S.L.BUD'KO	ND,SM,PR,CE,TH,CU,O	
1669	PHC1680530		(Pr,Th)2CuO4	Pr1.85Th0.15Cu1O4-Z	Pr	1.85	Th	0.15	Cu	1															O	4-Z			1990																												T'																					15.5				15.5			K/GPa	0.03																											0.43																																																																0						EFFECT OF PRESSURE ON CRITICAL PARAMETERS OF ELECTRON-DOPED SUPERCONDUCTORS LN2-XMXCUO4-Y(LN=ND,SM,PR,M=CE,TH)			INSTITUTE FOR HIGH PRESSURE PHYSICS, USSR ACADEMY OF SCIENCES,TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C, 168(1990)530	A.E.LUPPOV,A.G.GAPOTCHENKO,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,S.L.BUD'KO	ND,SM,PR,CE,TH,CU,O	
1670	PHC1680499	MELT PROCESS,Y FROM	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.11	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.11		1990																												Bi2212																		K				86.4			86.4			K/kbar	0.14																																																																																											0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1671	PHC1680499		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.16		1990																												Bi2212																		K				92.7			92.7			K/kbar	0.15																																																																																											0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1672	PHC1680499		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.19	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.19		1990																												Bi2212																		K				88			88																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1673	PHC1680499		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.22	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.22		1990																												Bi2212																		K				78.5			78.5																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1674	PHC1680499		Tl2Ba2CuO6	Tl2Ba2Cu1O6.1	Tl	2	Ba	2	Cu	1															O	6+Y	6.1	1	1990									6.1																			Tl2201																		K				92.4			92.4																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1675	SSC0750315		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1990																												Y124																																					DEVIATION FROM LINEAR MAGNETIZATIN,USING EXTRACTION MAGNETOMETER																																																																																			0						DETERMINATION OF HC1(T) ON A Y2BA4CU8O16 SINGLE CRYSTAL		MAGNETIZATION       ,HC1                 ,SINGLE CRYSTAL	CENTRE DE RECHERCHES SUR LES TRES BASSES TEMPERATURES, C.N.R.S., BP 166 X, 38042	SOLID STATE COMMUN.,75(1990)315	E.KALDIS,J.C.MARTINEZ,J.J.PREJEAN,J.KARPINSKI,P.BORDET	Y,BA,CU,O	
1676	PHC1680499		Tl2Ba2CuO6	Tl2Ba2Cu1O6.12	Tl	2	Ba	2	Cu	1															O	6+Y	6.12		1990																												Tl2201																		K				87.8			87.8																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1677	PHC1680499		Tl2Ba2CuO6	Tl2Ba2Cu1O6.16	Tl	2	Ba	2	Cu	1															O	6+Y	6.16		1990																												Tl2201																		K				64.9			64.9																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1678	PHC1680499		Tl2Ba2CuO6	Tl2Ba2Cu1O6.19	Tl	2	Ba	2	Cu	1															O	6+Y	6.19		1990																												Tl2201																		K				45.3			45.3																																																																																															0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1679	PHC1680499		Tl2Ba2CuO6	Tl2Ba2Cu1O6.23	Tl	2	Ba	2	Cu	1															O	6+Y	6.23		1990																												Tl2201																		K					4.2																																																																																																	0						CORRELATION BETWEEN THE MAGNITUDE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE AND THE NORMAL-STATE MAGNETIC SUSCEPTIBILITYIN BI2SR2CACU2O8+Y AS A FUNCTION OF OXYGEN CONTENT			SEKITION PHYSIK, UNIVERSITAT MUNCHEN, SCHELLINGSTR. 4, D-8000MUNCHEN 40, FRG,AND WALTHER-MEISSNER-INSTITUT FUR TIEFTEMPERATURFORSCHUNG,D-8046 GARCHING,FRG	PHYSICA C, 186(1990)499	C.ALLGEIER,J.S.SCHILLING	TL,BI,SR,CA,CU,O	
1680	PHC1680482		YBa2Cu4O8	Y1Ba2Cu4O7.986	Y	1	Ba	2	Cu	4															O	8	7.986		1990																												Y124				3.841	3.871	27.24														80					80																																																																																															0						SUPERCONDUCTIVITY AT 108 K IN YBA2CU4O8 AT PRESSURES UP TO 12GPA			DEPARTMENT OF PHYSICS AND ASTRONOMY OF THE FREE UNIVERSITY, 1081 HV AMSTERDAM, THE NETHERLANDS	PHYSICA C,186(1990)482	E.JILEK,E.KALDIS,E.N.VAN EENIGE,J.KARPINSKI,R.GRIESSEN,R.J.WIJNGAARDEN,S.RUSIECKI	Y,BA,CU,O	
1681	PHC1680465		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1990		0																									3	Y123																			91.8	92.4	92.7				92.4																																																					SP1681				24.8																																						0	MIXTURE-SIN(925C 50H)-C(IN O2)					FLUCTUATION SPECIFIC HEAT AND THERMAL EXPANSION OF YBACUO ANDDYBACUO			II.PHYSIKALISCHES INSTITUT DER UNIVERSITAT ZU KOLN, ZULPICHERSTRASSE 77, D-5000 KOLN 41, FRG	PHYSICA C,168(1990)465	D.WOHLLEBEN,E.BRAUN,H.BROICHER,J.HARNISCHMACHER,R.DOMEL,S.RUPPEL,W.BRAUNISCH,W.SCHNELLE	DY,Y,BA,CU,O	
1682	PHC1680465		DyBa2Cu3O7	Dy1Ba2Cu3OZ	Dy	1	Ba	2	Cu	3															O	Z		1	1990						10.5																					3	Y123																			91.8		92.4				92.1																																																					SP1682				21.6																																						0	MIXTURE-SIN(925C 50H)-C(IN O2)					FLUCTUATION SPECIFIC HEAT AND THERMAL EXPANSION OF YBACUO ANDDYBACUO			II.PHYSIKALISCHES INSTITUT DER UNIVERSITAT ZU KOLN, ZULPICHERSTRASSE 77, D-5000 KOLN 41, FRG	PHYSICA C,168(1990)465	D.WOHLLEBEN,E.BRAUN,H.BROICHER,J.HARNISCHMACHER,R.DOMEL,S.RUPPEL,W.BRAUNISCH,W.SCHNELLE	DY,Y,BA,CU,O	
1683	SSC0741321		(La,Ba)2CuO4	La1.926Ba0.074Cu1O4	La	1.926	Ba	0.074	Cu	1															O	4			1990																												T																																																																																		5.6																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1684	SSC0741321		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4			1990																												T																																																																																		6.62																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1685	SSC0741321		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4			1990																												T																																																																																		7.52																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1686	SSC0741321		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4			1990																												T																																																																																		8.38																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1687	SSC0741321		(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4			1990																												T																																																																																		9.55																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1688	SSC0741321		(La,Ba)2CuO4	La1.826Ba0.174Cu1O4	La	1.826	Ba	0.174	Cu	1															O	4			1990																												T																																																																																		10.45																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1689	SSC0741321		(La,Ba)2CuO4	La1.826Ba0.174Cu1O4	La	1.826	Ba	0.174	Cu	1															O	4			1990																												T																																																																																		10.45																																						0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1690	SSC0741321			Bi4Sr3Ca2Y1Cu4O16	Bi	4	Sr	3	Ca	2	Y	1	Cu	4											O	16			1990																												Bi2212																				43.5					43.5										24.1																																																																																				BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1691	SSC0741321			Bi4Sr3Ca1.6Y1.4Cu4O16	Bi	4	Sr	3	Ca	1.6	Y	1.4	Cu	4											O	16			1990																												Bi2212																				79.8					79.8																																																																																														BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1692	SSC0741321			Bi4Sr3Ca1.5Y1.5Cu4O16	Bi	4	Sr	3	Ca	1.5	Y	1.5	Cu	4											O	16			1990																												Bi2212																				86.1					86.1										41.9																																																																																				BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1693	SSC0741321			Bi4Sr3Ca1.4Y1.6Cu4O16	Bi	4	Sr	3	Ca	1.4	Y	1.6	Cu	4											O	16			1990																												Bi2212																				85.8					85.8										41																																																																																				BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1694	SSC0741321			Bi4Sr3Ca1.2Y1.8Cu4O16	Bi	4	Sr	3	Ca	1.2	Y	1.8	Cu	4											O	16			1990																												Bi2212																				79.3					79.3										49.6																																																																																				BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1695	SSC0741321			Bi4Sr3Ca1Y2Cu4O16	Bi	4	Sr	3	Ca	1	Y	2	Cu	4											O	16			1990																												Bi2212																				64.1					64.1										55.7																																																																																				BI2O3,SRCO3,CACO3,Y2O3,CUO	0	CAL(850C 10-30H IN O2)-SIN(890-920C)-C					COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1696	SSC0741321		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8			1990																												Bi2212																				41					41										16																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1697	SSC0741321		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8			1990																												Bi2212																				62.7					62.7										31																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1698	SSC0741321		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8			1990																												Bi2212																				81.4					81.4										37.4																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1699	SSC0741321		BISr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.75Y0.25Cu2O8	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	2											O	8			1990																												Bi2212																				89.4					89.4										33																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1700	PHC1650221		NdBa2Cu3O7	Nd1Ba2Cu3O6.84	Nd	1	Ba	2	Cu	3															O	7-Z	6.84	1	1990																												Y123																			91	93					93																																																																			6.1																			0.000000000904			0.0000000025		HA1700			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1701	PHC1650221	PARAMETER=ND CONTENT IN 1+2X, N=100K	Nd(Ba,Nd)2Cu3O7	Nd1.1Ba1.9Cu3O6.9	Nd	1.1	Ba	1.9	Cu	3															O	7-Z	6.9	1	1990																												Y123																			90	92					92																																																																			10.3																			0.00000000126			0.00000000333		HA1701			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1702	PHC1650221	PARAMETER=ND CONTENT IN 1+2X, N=100K	Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3O6.96	Nd	1.2	Ba	1.8	Cu	3															O	7-Z	6.96	2	1990																												Y123																			72	80					80																																																																			25.8																			0.00000000271			0.00000000514		HA1702			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1703	PHC1650221	PARAMETER=ND CONTENT IN 1+2X, N=100K	Nd(Ba,Nd)2Cu3O7	Nd1.3Ba1.7Cu3O7	Nd	1.3	Ba	1.7	Cu	3															O	7-Z	7	2	1990																												Y123																			49	69					69																																																																			48.7																			0.00000000498			0.00000000741		HA1703			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1704	PHC1650221	PARAMETER=ND CONTENT IN 1+2X, N=100K	Nd(Ba,Nd)2Cu3O7	Nd1.4Ba1.6Cu3O7.09	Nd	1.4	Ba	1.6	Cu	3															O	7-Z	7.09	2	1990																												Y123																			30	38					38																																																																			58.4																			0.00000000524			0.00000000802		HA1704			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1705	PHC1650221	PARAMETER=ND CONTENT IN 1+2X, N=100K	Nd(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3O7.14	Nd	1.5	Ba	1.5	Cu	3															O	7-Z	7.14	2	1990																												Y123																			10	20					20																																																																			85.2																			0.00000000761			0.0000000116		HA1705			ND2O3,BAO2,CUO	0	(950C IN AIR)-ANN(950C IN 1 BAR O2)-C(8C/H) TO RT					TRANSPORT PROPERTIES AND HOLE DISTRIBUTION OF ND(BA1-XNDX)2CUO7+Z				PHYSICA C,165(1990)221	DE LEEUW.D.M,VAN WOERDEN.R.A.M		
1706	SSC0741321		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8			1990																												Bi2212																				89.6					89.6										42.1																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1707	SSC0741321		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8			1990																												Bi2212																				76					76										37.2																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1708	SSC0741321		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1990																												Bi2212																				71.8					71.8										47.5																																																																																					0						COMMON FEATURES OF MAGNETIC AND SUPERCONDUCTING PROPERTIES INY-DOPED BI2(SR,CA)3CU2O8 AND BA(SR)-DOPED LA2CUO4			DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE HOKKAIDO UNIVERSITY,SAPPORO, 060, JAPAN	SOLID STATE COMMUN.,74(1990)1321	H.MATSUKI,M.IDO,M.ODA	Y,BI,SR,CA,CU,O,BA,LA	
1709	SSC0740767	GAMMA FR SP.HEAT	(La,Ba)2CuO4	La1.976Ba0.024Cu1O4	La	1.976	Ba	0.024	Cu	1															O	4			1990																												T																																																																																		2.37																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1710	SSC0740767	GAMMA FR SP HEAT	(La,Ba)2CuO4	La1.946Ba0.054Cu1O4	La	1.946	Ba	0.054	Cu	1															O	4			1990																												T																																																																																		4.14																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1711	SSC0740767	GAMMA FR SP.HEAT	(La,Ba)2CuO4	La1.91Ba0.09Cu1O4	La	1.91	Ba	0.09	Cu	1															O	4			1990																												T																				28.8					28.8																																																									2.26																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1712	SSC0740767	GAMMA FR SP.HEAT,TWO STEP TRANSITION	(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4			1990																												T																				4.2	29				4.2																																																									2																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1713	SSC0740767	GAMMA FR SP.HEAT	(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4			1990																												T																				28.8					28.8																																																									5.5																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1714	SSC0740767	GAMMA FR SP.HEAT	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4			1990																												T																																																																																		8.72																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1715	SSC0740767	GAMMA FR SP.HEAT,TWO STEP TRANSITION	(La,Ba)2CuO4	La1.78Ba0.22Cu1O4	La	1.78	Ba	0.22	Cu	1															O	4			1990																												T																					32				32																																																									12.2																																					LA2O3,BACO3,CUO	0	CAL(1050C 10H IN O2)-SIN(1050C 44H IN O2)-C(1.5C/MIN) TO 500C-ANN(500C 24H)					REDUCTION OF THE ELECTRONIC COEFFICIENT OF THE SPECIFIC HEAT AROUND X=0.065 IN (LA1-XBAX)2CUO4		SPECIFIC HEAT	DEPARTMENT OF NUCLEAR ENGINEERING, HOKKAIDO UNIVERSITY, SAPPORO 060, JAPAN	SOLID STATE COMMUN.,74(1990)767	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
1716	SSC0740951		(La,Sr)2CuO4	La1.65Sr0.35Cu1O4	La	1.65	Sr	0.35	Cu	1															O	4		1	1990																											1	T																																																																																										THC1716																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1717	SSC0740951		(La,Sr)2CuO4	La1.6Sr0.4Cu1O4	La	1.6	Sr	0.4	Cu	1															O	4		1	1990																											1	T																																																																																										THC1717																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1718	SSC0740951		(La,Sr)2CuO4	La1.5Sr0.5Cu1O4	La	1.5	Sr	0.5	Cu	1															O	4		1	1990																											1	T																																																																																										THC1718																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1719	SSC0740951		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1990																											1	T																																																																																										THC1719																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1720	SSC0740951		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1990																											1	T																																																																																										THC1720																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1721	SSC0740951		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																											1	T																				36.4					36.4																																																																	THC1721																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1722	SSC0740951		YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	6.7	6.7	3	1990																											3	Y123																				60					60																																																																	THC1722																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1723	SSC0740951		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4		3	1990																												T'																																																																																										THC1723																													LA2O3,SRCO3,CUO	0	CAL(900C 30H)-SIN(1100C 60H)-FC,FOR X>0.35 ANN(1080C 6H IN 300ATM O2)					THERMAL CONDUCTIVITY OF HIGH-TC OXIDES		THERMAL CONDUCTIVITY	INSTITUTE FOR MOLECULAR SCIENCE, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.,74(1990)951	I.WATANABE,K.KUMAGAI,M.SATO,M.SERA,S.NAKASHIMA,S.SHAMOTO	LA,BA,SR,CU,O	
1724	PR0422554		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.925Zn0.075Oz	Gd	1	Ba	2	Cu	2.925	Zn	0.075													O	z		1	1990						7.91	1.7	2.12																			3	Y123				3.836	3.891	11.682														54					54																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1725	PR0422554		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.85Zn0.15Oz	Gd	1	Ba	2	Cu	2.85	Zn	0.15													O	z		1	1990						7.91	-0.7	2.06																			3	Y123				3.833	3.887	11.662														37					37																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1726	PR0422554		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.775Zn0.225Oz	Gd	1	Ba	2	Cu	2.775	Zn	0.225													O	z		1	1990						7.9	-2.4	2.05																			3	Y123				3.841	3.894	11.662														35					35																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1727	PR0422554		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.7Zn0.3Oz	Gd	1	Ba	2	Cu	2.7	Zn	0.3													O	z		1	1990						7.93	1.1	1.99																			3	Y123				3.845	3.889	11.647																																																																																																																		0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1728	PR0422554		GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z		1	1990						7.98	0.6	2.19																			3	Y123				3.834	3.897	11.675														91					91																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1729	PR0422554		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.925Ni0.075OZ	Gd	1	Ba	2	Cu	2.925	Ni	0.075													O	Z		1	1990						7.95	2.2	2.11																			3	Y123				3.821	3.876	11.633														79					79																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1730	PR0422554		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.85Ni0.15OZ	Gd	1	Ba	2	Cu	2.85	Ni	0.15													O	Z		1	1990						8.01	0.5	2.06																			3	Y123				3.834	3.888	11.677														71					71																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1731	PR0422554		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.775Ni0.225OZ	Gd	1	Ba	2	Cu	2.775	Ni	0.225													O	Z		1	1990						7.93	3.2	1.99																			3	Y123				3.833	3.882	11.65														65					65																																																																																															0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1732	PR0422554		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.7Ni0.3OZ	Gd	1	Ba	2	Cu	2.7	Ni	0.3													O	Z		1	1990						8	-0.2	1.9																			3	Y123				3.833	3.878	11.641																																																																																																																		0	USUAL SOLID STATE REACTION					EFFECTS OF NI AND ZN SUBSTITUTION ON MAGNETIC PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR GDBA2CU3O7-Y	199008		DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING, PEOPLE'S REPUBLIC OF CHINA	PHYS.REV.B,42(1990)2554	CHIN LIN,JIAN LAN,ZUN-XIAO LIU	GD,BA,CU,O	
1733	PR0422551		(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3		1	1990									7.29																		1	BKBO				4.29															23	24					24																						15.4									0.916							45.3				FROM MAGNETIZATION,400 MESH PARTICLE	803							150000																																												BAO,K2O,BI2O3	0	ANN(700C 1H IN N2)-ANN(450C 2H IN O2)-FC					MAGNETIC PROPERTIES OF POLYCRYSTALLINE BA0.5K0.5BIO3	199008	MAGNETIZATION	DEPARTMENT OF PHYSICS, NATIONAL TAIWAN UNIVERSITY, TAIPEI, TAIWAN	PHY.REV.B,42(1990)2551	D.S. Lee,D.S.LEE,H.C. Yang,H.C.YANG,H.E. Horng,H.E.HORNG,M.H. Hsieh,M.H.HSIEH	BA,K,BI,O	
1734	PR0416541		(Bi,Pb)2Sr2Ca3Cu4Oz	Bi1.7Pb0.3Sr2Ca3Cu4OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	3	Cu	4											O	Z		1	1990																											4	Bi2223				3.779	3.834	37.15													107	110					110													900									184									2.43							13.5					880							48000					5.3		34.6		418																																			PBO,BI2O3,SRCO3,CACO3,CUO	0	CAL(800-810C 12H)-SIN(870-880C 60+180H IN AIR)-FC TO 500C-Q IN AIR					PREPARATION PROCESS, CRYSTAL STRUCTURE, AND PHYSICAL PROPERTIES OF THE 110-K SINGLE-PHASE PB-BI-SR-CA-CU-O SUPERCONDUCTOR	199004		DEPARTMENT OF MATERIALS SCIENCE AND ENGINEERING, UNIVERSITY OFSCIENCE AND TECHNOLOGY, BEIJING, BEIJING, 10083, CHINA	PHYS.REV.B,41(1990)6541	C.G.CUI,F.SHI,J.DU,J.L.ZHANG,N.C.SHI,Q.Z.RAN,R.Y.JIN,S.Z.ZHOU,T.S.RONG,X.F.WU,Z.H.SHI	PB,BI,SR,CA,CU,O	
1735	PR04111681		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1990																												Y123																				93					93																																																3.5																														100																	0						Infrared absorptivity of YBa2Cu3O7-x crystal	199006		Center for Superconductivity Research, Physics Department, University of Maryland, College Park, Maryland 20742 and Laboratory for Physical Sciences, College Park, Maryland 20740	Phys.Rev.B,41(1990)11681	H.D. Drew,J.Z. Liu,S.H. Moseley,T. Pham		
1736	PR0422558	NEELT BY ESR	GdBa2(Cu,Ni)3O7	Gd1Ba2CuNiOY	Gd	1	Ba	2	Cu		Ni														O	Y		1	1990																											1	Y123																																																																																																																							GD2O3,BACO3,NIO,CUO	0	SIN(850C 2H IN N2)-C-SIN(950C 24H IN O2)-C(20C/H) TO 600C-C(10C/H) TO RT					MAGNETIC INTERACTIONOS OF GD IN GDBA2 (CU1-XNIX)3OY COMPOUNDS	199008		INSTITUTE OF PHYSICS, UNIVERSITY OF TSUKUBA, TSUKUBA, IBARAKI305, JAPAN	PHY.REV.B,42(1990)2558	F.NAKAMURA,H.SHIMIZU,Y.NARAHARA,Y.OCHIAI	GD,BA,CU,NI,O	
1737	PR0416605		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1990									5.24																		3	Y123																				90					90																																																																	TC1737																													BACO3,Y2O3,CUO	1	YBA2CUO5 ABOUT 2%,CUO 1% , (950C 24H IN AIR)-(900C 24H IN O2)-C(12C/H) TO RT-(930C 24H IN O2)-C(12C/H) TO RT					THERMAL CONDUCTIVITY OF POLYCRYSTALLINE YBA2CU3O7-Z IN A MAGNETIC FIELD	199004		DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY, UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN, URBANA, ILLINOIS 61801	PHYS.REV.B,41(1990)6605	A.C.ANDERSON,D.M.GINSBERG,DA-MING ZHU,T.A.FRIENDMANN	Y,BA,CU,O	
1738	PR0416418			Bi2.05Pb0.05Sr1.9Cu1OY	Bi	2.05	Pb	0.05	Sr	1.9	Cu	1													O	Y		1	1990																																5.362		24.616														9.4					9.4																																																																																															1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1739	PR0416418			Bi2Pb0.1Sr1.9Cu1OY	Bi	2	Pb	0.1	Sr	1.9	Cu	1													O	Y			1990																																5.361		24.625														8.4					8.4																																																																																															1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1740	PR0416418			Bi1.95Pb0.15Sr1.9Cu1OY	Bi	1.95	Pb	0.15	Sr	1.9	Cu	1													O	Y			1990																																5.34	5.37	24.654														6.4					6.4																																																																																															1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1741	PR0416418			Bi1.9Pb0.2Sr1.9Cu1OY	Bi	1.9	Pb	0.2	Sr	1.9	Cu	1													O	Y			1990																																5.336	5.385	24.649														4.7					4.7																																																																																															1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1742	PR0416418			Bi1.8Pb0.3Sr1.9Cu1OY	Bi	1.8	Pb	0.3	Sr	1.9	Cu	1													O	Y			1990																																5.303	5.371	24.53																																																																																																																		1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1743	PR0416418			Bi1.7Pb0.4Sr1.9Cu1OY	Bi	1.7	Pb	0.4	Sr	1.9	Cu	1													O	Y			1990																																5.284	5.391	24.584																																																																																																																		1						PHYSICAL PROPERTIES OF BI2SU2CAN-1CUNOY (N=1,2,3)	199004	HOLE CONCENTRATIONS ,SUSCEPTIBILITIES    ,INFRARED	DEPARTMENT OF APPLIED PHYSICS, THE UNIVERSITY OF TOKYO, 7-3-1HONGO, BUNKYO-KU, TOKYO 113, JAPAN	PHYS.REV.B,41(1990)6418	A.MAEDA,I.TSUKADA,K.NODA,K.UCHINOKURA,M.HASE,S.TAKEBAYASHI	BI,SR,CA,CU,O,PB	
1744	SSC0640727		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123				3.822	3.885	11.66																																																																			3.66	4																																														0						INFRARED AND RAMAN SPECTRA OF THE MBA2CU3O7-TYPE HIGH-TC SUPERCONDUCTORS			MAX-PLANK-INSTITUT FUR FESKORPEFORSCHUNG, HEISENGERGSTR. 1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,64(1987)727	A.WITTLIN,E.GARCIA-GONALEZ,F.GARCIA-ALVARADO,HJ.MATTAUSCH,L.GENZEL,M.CARDONA,R.LIU		
1745	SSC0640727		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1987																												Y123																																																																									3.33	4																																														0						INFRARED AND RAMAN SPECTRA OF THE MBA2CU3O7-TYPE HIGH-TC SUPERCONDUCTORS			MAX-PLANK-INSTITUT FUR FESKORPEFORSCHUNG, HEISENGERGSTR. 1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,64(1987)727	A.WITTLIN,E.GARCIA-GONALEZ,F.GARCIA-ALVARADO,HJ.MATTAUSCH,L.GENZEL,M.CARDONA,R.LIU		
1746	SSC0640727		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7			1987																												Y123				3.85	3.902	11.708																																																																			3.17	4																																														0						INFRARED AND RAMAN SPECTRA OF THE MBA2CU3O7-TYPE HIGH-TC SUPERCONDUCTORS			MAX-PLANK-INSTITUT FUR FESKORPEFORSCHUNG, HEISENGERGSTR. 1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,64(1987)727	A.WITTLIN,E.GARCIA-GONALEZ,F.GARCIA-ALVARADO,HJ.MATTAUSCH,L.GENZEL,M.CARDONA,R.LIU		
1747	SSC0640727		HoBa2Cu3O7	Ho1Ba2Cu3O7	Ho	1	Ba	2	Cu	3															O	7			1987																												Y123				3.818	3.89	11.669													93		97				95																																																3.36	4																																														0						INFRARED AND RAMAN SPECTRA OF THE MBA2CU3O7-TYPE HIGH-TC SUPERCONDUCTORS			MAX-PLANK-INSTITUT FUR FESKORPEFORSCHUNG, HEISENGERGSTR. 1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,64(1987)727	A.WITTLIN,E.GARCIA-GONALEZ,F.GARCIA-ALVARADO,HJ.MATTAUSCH,L.GENZEL,M.CARDONA,R.LIU		
1748	SSC0640727		EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7			1987																												Y123																																																																									3.18	4																																														0						INFRARED AND RAMAN SPECTRA OF THE MBA2CU3O7-TYPE HIGH-TC SUPERCONDUCTORS			MAX-PLANK-INSTITUT FUR FESKORPEFORSCHUNG, HEISENGERGSTR. 1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,64(1987)727	A.WITTLIN,E.GARCIA-GONALEZ,F.GARCIA-ALVARADO,HJ.MATTAUSCH,L.GENZEL,M.CARDONA,R.LIU		
1749	SSC0650219		(Y,Ho)Ba2Cu3O7	Y0.5Ho0.5Ba2Cu3O7-Z	Y	0.5	Ho	0.5	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.827	3.896	11.688																																																																			3.6	2																																														0						HIGH SUPERCONDUCTORS MBA2CU3O7-X WITH M=MIXED RARE EARTHS ANDY: LOW FREQUENCY PHONON PEAK ENGINEERING			MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE1, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.65(1990)219	A.WITTLIN,C.THOMSEN,E.GARCIA,L.GENZEL,M.CARDONA,M.V.CABANAS,R.LIU,W.KONIG	Y,SM,HO,BA,CU,O	
1750	PRB0370652		DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90					90																																																3.2																																															0						SUPERCONDUCTING ENERGY GAP IN M(1)BA(2)CU(3)O(7-Z)-TYPE MATERIALS	198801	ENERGY GAP               ,FAR-INFRARED             ,REFLECTA	MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE,GERMANY	PHYS.REV.B,37(1988)652	A.WITTLIN,E.GARCIA,L.GENZEL,M.BARAHONA,M.BAUER,M.CARDONA,M.V.CABANAS,W.KONIG	R,BA,CU,O	
1751	PRB0370652		(Sm,Y)Ba2Cu3O7	Sm0.5Y0.5Ba2Cu3O7-Z	Sm	0.5	Y	0.5	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.836	3.891	11.681																																																																			3.2	2																																														0						SUPERCONDUCTING ENERGY GAP IN M(1)BA(2)CU(3)O(7-Z)-TYPE MATERIALS	198801	ENERGY GAP               ,FAR-INFRARED             ,REFLECTA	MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE,GERMANY	PHYS.REV.B,37(1988)652	A.WITTLIN,E.GARCIA,L.GENZEL,M.BARAHONA,M.BAUER,M.CARDONA,M.V.CABANAS,W.KONIG	R,BA,CU,O	
1752	PRB0370652		(Sm,Ho)Ba2Cu3O7	Sm0.5Ho0.5Ba2Cu3O7-Z	Sm	0.5	Ho	0.5	Ba	2	Cu	3													O	7-Z			1988																												Y123				3.841	3.899	11.699																																																																			3.2	2																																														0						SUPERCONDUCTING ENERGY GAP IN M(1)BA(2)CU(3)O(7-Z)-TYPE MATERIALS	198801	ENERGY GAP               ,FAR-INFRARED             ,REFLECTA	MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE,GERMANY	PHYS.REV.B,37(1988)652	A.WITTLIN,E.GARCIA,L.GENZEL,M.BARAHONA,M.BAUER,M.CARDONA,M.V.CABANAS,W.KONIG	R,BA,CU,O	
1753	SSC0720085		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12OZ	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	Z			1989																												Y123																				76.1					76.1																																																1.17	2																																														0	USUAL SINTERING PROCESS					OBSERVATION OF AN ENERGY GAP IN THE FAR INFRARED SPECTRA OF IRON-DOPED YBA2CU3OX SUPERCONDUCTORS	198910	FAR INFRARED        ,REFLECTANCE         ,ENERGY GAP          ,OXYGEN CONTENT	MAX-PLANCE-INSTITUT FUR FESTKORPERFORSCHUNG HEISENBERGSTR. 1,7000 STUTTGART 80	SOLID STATE COMMUN.72(1989)85	A. JANSEN,C. RICHTER,E. SEIDER,L. GENZEL,M. BAUER,P. WYDER	Y,BA,CU,O,FE	
1754	SSC0720085		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.91Fe0.09OZ	Y	1	Ba	2	Cu	2.91	Fe	0.09													O	Z			1989																												Y123																																																																									1.51	2																																														0	USUAL SINTERING PROCESS					OBSERVATION OF AN ENERGY GAP IN THE FAR INFRARED SPECTRA OF IRON-DOPED YBA2CU3OX SUPERCONDUCTORS	198910	FAR INFRARED        ,REFLECTANCE         ,ENERGY GAP          ,OXYGEN CONTENT	MAX-PLANCE-INSTITUT FUR FESTKORPERFORSCHUNG HEISENBERGSTR. 1,7000 STUTTGART 80	SOLID STATE COMMUN.72(1989)85	A. JANSEN,C. RICHTER,E. SEIDER,L. GENZEL,M. BAUER,P. WYDER	Y,BA,CU,O,FE	
1755	SSC0720085		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06OZ	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	Z			1989																												Y123																																																																									2.09	2																																														0	USUAL SINTERING PROCESS					OBSERVATION OF AN ENERGY GAP IN THE FAR INFRARED SPECTRA OF IRON-DOPED YBA2CU3OX SUPERCONDUCTORS	198910	FAR INFRARED        ,REFLECTANCE         ,ENERGY GAP          ,OXYGEN CONTENT	MAX-PLANCE-INSTITUT FUR FESTKORPERFORSCHUNG HEISENBERGSTR. 1,7000 STUTTGART 80	SOLID STATE COMMUN.72(1989)85	A. JANSEN,C. RICHTER,E. SEIDER,L. GENZEL,M. BAUER,P. WYDER	Y,BA,CU,O,FE	
1756	PRB0360843		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				84					84																																																3.2	1																																														0						TUNNELING MEASUREMENTS ON THE HIGH-TC SUPERCONDUCTORS LA(1.85)SR(0.15)CU(1)O(4-Z) AND Y(1)BA(2)CU(3)O(7-Z)	198707	TUNNELING	RESEARCH INST. FOR MATERIALS,UNIV. OF NIJMEGEN,TOERNOOIVELD,NIJMEGEN,THE NETHERLANDS	PHYS.REV.B,36(1987)843	H.VAN KEMPEN,L.E.C.VAN DE LEEMPUT,L.W.M.SCHREURS,P.A.A.TEUNISSEN,P.J.M.VAN BENTUM		
1757	PRB0358853		YBa2Cu3O7	Y1Ba2Cu3O9-Y	Y	1	Ba	2	Cu	3															O	9-Y			1987																												Y123																				90					90																																																3.9	1																																														0						TUNNELING MEASUREMENT OF THE ENERGY GAP IN Y-BA-CU-O	198706	TUNNELING	UNIV. OF CALIFORNIA,BERKELEY,CALIFORNIA,USA	PHYS.REV.B,35(1987)8853	A.STACY,A.ZETTL,L.C.BOURNE,M.F.CROMMIE,MARVIN L.COHEN		
1758	PRB0375920		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1988																												Y123																				90					90																																																2.8	4																																														0						RAMAN SCATTERING FROM SUPERCONDUCTING GAP EXCITATIONS IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-Z)	198804	SINGLE CRYSTAL           ,RAMAN                    ,ENERGY G	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,ILLINOIS	PHYS.REV.B,37(1988)5920	B.G.PAZOL,D.M.GINSBERG,J.P.RICE,M.V.KLEIN,S.L.COOPER	Y,BA,CU,O	
1759	PRL0582249			Y1Ba2Cu3.85O6.85	Y	1	Ba	2	Cu	3.85															O	6.85	6.85		1987																												Y123																				93					93																																																3.1	2																																														0						FAR-INFRARED CONDUCTIVITY OF THE HIGH-TC SUPERCONDUCTOR YBA2CU3O7	198705	GAP	INSTITUTE OF MATERIALS RESEARCH, MCMASTER UNIVERSITY,HAMILTON,ONTARIO L8S 4M1, CANADA	PHYS.REV.LETT.,58(1987)2249	C.V.STAGER,D.A.BONN,D.B.TANNER,J.E.GREEDAN,K.KAMARAS,M.G.DOSS,S.L.HERR,T.TIMUSK	Y,BA,CU,O	
1760	PR04111237	C-AXIS GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																												Y123																				93					93																																																3	2																																														0						infrared studies of the superconducting energy gap and normal-state dynamics of the high-Tc superconductor YBa2Cu3O7	1990		IBM Thomas J. Watson Research Center, Yorktown Heights, New York 10598	Phys.Rev.B.,41(1990)11237	A. Gupta,C. Feild,F. Holtzberg,G. Koren,R.T. Collins,Z. Schlesinger		
1761	PR04111237	AB PLANE GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																												Y123																				93					93																																																8	2																																														0						infrared studies of the superconducting energy gap and normal-state dynamics of the high-Tc superconductor YBa2Cu3O7	1990		IBM Thomas J. Watson Research Center, Yorktown Heights, New York 10598	Phys.Rev.B.,41(1990)11237	A. Gupta,C. Feild,F. Holtzberg,G. Koren,R.T. Collins,Z. Schlesinger		
1762	PRB0365586		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123																				90					90																																																5	5																																														0						MEASUREMENT OF THE ENERGY GAP OF Y(1)BA(2)CU(3)O(7) USING AC SUSCEPTIBILITY	198710	ENERGY GAP               ,SUSCEPTIBILITY	PHYSICS DEPARTMENT,THE TECHNION,ISRAEL	PHYS.REV.B,36(1987)5586	B.FISHER,E.POLTURAK	Y,BA,CU,O	
1763	PR0352378		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4			1987																												T																				37					37																																																1.3	6																																														0						Energy gap and Korringa constant in the high-temperature superconductor La1.83Sr0.17CuO4 determined by NMR				Phys.Rev.B, 36(1987)2378			
1764	PRB0358826		(La,Sr)2CuO4	La1.8Ba0.2Cu1O4-Y	La	1.8	Ba	0.2	Cu	1															O	4-Y			1987																												T																				25.6					25.6																																																3.5	7																																														0						SURFACE IMPEDANCE MEASUREMENTS IN LA(1.8)BA(0.2)CU(1)O(4-Y)	198706		UNIV. OF CALIFORNIA,LOS ANGELES,LOS ANGELES,CALIFORNIA ,USA	PHYS.REV.B,35(1987)8826	B.ALAVI,G.GRUNER,W.P.BEYERMANN		
1765	PRB0358829		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4-Y	La	1.84	Sr	0.16	Cu	1															O	4-Y			1987																												T																				38.5					38.5																																																2.7	2																																														0						FAR-INFRARED MEASUREMENT OF A2(Q)F(Q) IN SUPERCONDUCTING LA(1.85)SR(0.15)CU(1)O(4-Y)	098706		CORNELL UNIV. ITHACA,NEW YORK,USA	PHYS.REV.B,35(1987)8829	A.J.SIEVERS,J.M.TARASCON,L.H.GREENE,P.E.SULEWSKI,R.A.BUHRMAN,W.A.CURTIN		
1766	PRB0357228		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				32					32																																																8	1																																														0						ELECTRON-TUNNELING STUDIES OF THIN FILMS OF HIGH-TC SUPERCONDUCTING LA-SR-CU-O	198705	TUNNELING                ,THIN FILM                ,POINTCON	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,CALIFORNIA	PHYS.REV.B,35(1987)7228	A.KAPITULNIK,B.OH,C.F.QUATE,D.B.MITZI,D.J.WEBB,D.P.E.SMITH,J.Z.SUN,K.CHAR,M.D.KIRK,M.NAITO,M.R.BEASLEY,M.R.HAHN,O.FISCHER,R.H.HAMMOND,T.H.GEBALLE	LA,SR,CU,O	
1767	PRB0358850		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				35					35																																																13	1																																														0						POINT-CONTACT ELECTRON TUNNELING INTO THE HIGH-TC SUPERCONDUCTOR Y-BA-CU-O	198706	TUNNELING	STANFORD UNIV.,STANFORD,CALIFORNIA,USA	PHYS.REV.B,35(1987)8850	A.KAPITLUNIK,B.OH,C.F.QUATE,D.B.MITZI,D.J.WEBB,D.P.E.SMITH,J.Z.SUN,K.CHAR,M.D.KIRK,M.NAITO,M.R.BEASLEY,M.R.HAHN,R.H.HAMMOND,T.H.GEBALLE		
1768	PRB0358850		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y124																				90					90																																																13	1																																														0						POINT-CONTACT ELECTRON TUNNELING INTO THE HIGH-TC SUPERCONDUCTOR Y-BA-CU-O	198706	TUNNELING	STANFORD UNIV.,STANFORD,CALIFORNIA,USA	PHYS.REV.B,35(1987)8850	A.KAPITLUNIK,B.OH,C.F.QUATE,D.B.MITZI,D.J.WEBB,D.P.E.SMITH,J.Z.SUN,K.CHAR,M.D.KIRK,M.NAITO,M.R.BEASLEY,M.R.HAHN,R.H.HAMMOND,T.H.GEBALLE		
1769	PRB0355327		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				36					36																																																2.4	2																																														0						ENERGY GAP IN THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4)	198704	FAR-INFRARED             ,ENERGY GAP	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,35(1987)5327	A.STACY,A.ZETTL,M.S.SHERWIN,P.L.RICHARDS,U.WALTER	LA,SR,CU,O	
1770	PRB0357224		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				35.9					35.9																																																5.2	1																																														0						ENERGY GAP IN LA(1.85)SR(0.15)CU(1)O(4-Y) FROM POINT-CONTACT TUNNELING	198705	TUNNELING                ,ENERGY GAP	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ILLINOIS	PHYS.REV.B,35(1987)7224	D.G.HINKS,D.W.CAPONE II,K.E.GRAY,M.E.HAWLEY	LA,SR,CU,O	
1771	PRB0355330		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4			1987																												T																				28					28																																																1.95	2																																														0						MEASUREMENT OF THE SUPERCONDUCTING ENERGY GAP IN LA-BA-CU OXIDE AND LA-SR-CU OXIDE	198704	FAR-INFRARED             ,ENERGY GAP	LABORATORY OF ATOMIC AND SOLID STATE PHYSICS AND MATERIALS SCIENCE CENTER,CORNELL UNIVERSITY,ITHACA,NEW YORK	PHYS.REV.B,35(1987)5330	A.J.SIEVERS,D.K.LATHROP,H.D.HALLEN,P.E.SULEWSKI,R.A.BUHRMAN,S.E.RUSSEK	LA,BA,CU,O,SR	
1772	PRB0355330		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				36					36																																																2.7	2																																														0						MEASUREMENT OF THE SUPERCONDUCTING ENERGY GAP IN LA-BA-CU OXIDE AND LA-SR-CU OXIDE	198704	FAR-INFRARED             ,ENERGY GAP	LABORATORY OF ATOMIC AND SOLID STATE PHYSICS AND MATERIALS SCIENCE CENTER,CORNELL UNIVERSITY,ITHACA,NEW YORK	PHYS.REV.B,35(1987)5330	A.J.SIEVERS,D.K.LATHROP,H.D.HALLEN,P.E.SULEWSKI,R.A.BUHRMAN,S.E.RUSSEK	LA,BA,CU,O,SR	
1773	PRB0357220		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				40					40																																																7	1																																														0						MEASUREMENTS OF THE SUPERCONDUCTING GAP OF LA-SR-CU-O WITH A SCANNING-TUNNELING MICROSCOPE	198705	STM                      ,ENERGY GAP	DEPARTMENT OF PHYSICS,UNIVERSITY OF TEXAS,AUSTIN,TEZAS	PHYS.REV.B,35(1987)7220	A.L.DE LOZANNE,J.M.TARASCON,K.W.NG,L.H.GREENE,S.PAN	LA,SR,CU,O	
1774	PRB0357216		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				36					36																																																6.3	1																																														0						LOCAL TUNNELING MEASUREMENTS OF THE HIGH-TC SUPERCONDUCTOR LA(2-X)SR(X)CU(1)O(4-Y)	198705	TUNNELING                ,I-V CHARACTERISTIC       ,STM	IBM THOMAS J.WATSON LABORATORY,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,35(1987)7216	C.C.CHI,C.C.TSUEI,J.R.KIRTLEY,J.ROZEN,M.W.SHAFER,SUNG I.PARK	LA,SR,CU,O	
1775	PRB0360736		(La,Sr)2CuO4	La1.825Sr0.175Cu1O4	La	1.825	Sr	0.175	Cu	1															O	4			1987																												T																				36					36																																																3.5	2																																														0						FAR-INFRARED REFLECTIVITY OF LA(2-X)SR(X)CU(1)O(4)	198707	REFLECTANCE              ,FAR-INFRARED	AT&T BELL LAB.,MURRAY HILL,NEW JERSEY,USA	PHYS.REV.B,36(1987)736	A.J.MILLIS,E.A.RIETMAN,G.A.THOMAS,R.J.CAVA,R.N.BHATT		
1776	PRB0355334		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987																												T																				30					30																																																2.5	2																																														0						FAR-INFRARED MEASUREMENT OF THE ENERGY GAP OF LA(1.8)SR(0.2)CU(1)O(4)	198704	FAR-INFRARED             ,ENERGY GAP	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,35(1987)5334	J.G.BEDNORZ,K.A.MULLER,R.L.GREENE,Z.SCHLESINGER	LA,SR,CU,O	
1777	PRB0357232		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				35					35																																																1.65	2																																														0						OBSERVATION OF A LOW-ENERGY INFRARED ANOMOLY IN SUPERCONDUCTING LA(1.85)SR(0.15)CU(1)O(4)	198705	INFRARED                 ,PLASMA EDGE	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,35(1987)7232	M.W.SHAFER,R.T.COLLINS,Z.SCHLESINGER	LA,SR,CU,O	
1778	SSC0650873		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1988																												T																				34					34																																																2.7	2																																														0						SPECIFIC HEAT AND FLUX CREEP FEATURE ON Y-BA-CU-O SYSTEM	198802	THEORY                   ,SPECIFIC HEAT            ,FLUX CRE	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING CHINA	SOLID STATE COMMUN.,65(1988)873	CHEN SHI-GANG,CHEN XIAO-LAN	Y,BA,CU,O	
1779	PRB0358843		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				37					37																																																4.5	2																																														0						FAR-INFRARED MEASUREMENT OF THE GAP OF THE HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4-X)	198706	GAP	MCMASTER UNIV.,HAMILTON,ONTARIO,CANADA	PHYS.REV.B,35(1987)8843	C.D.PORTER,C.V.STAGER,D.A.BONN,D.B.TANNER,J.E.GREEDAN,J.M.TARASCON,K.KAMARAS,L.H.GREENE,M.G.DOSS,S.L.HERR,T.TIMUSK,W.R.MCKINNON		
1780	PRB0360843		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				33					33																																																4	1																																														0						TUNNELING MEASUREMENTS ON THE HIGH-TC SUPERCONDUCTORS LA(1.85)SR(0.15)CU(1)O(4-Z) AND Y(1)BA(2)CU(3)O(7-Z)	198707	TUNNELING	RESEARCH INST. FOR MATERIALS,UNIV. OF NIJMEGEN,TOERNOOIVELD,NIJMEGEN,THE NETHERLANDS	PHYS.REV.B,36(1987)843	H.VAN KEMPEN,L.E.C.VAN DE LEEMPUT,L.W.M.SCHREURS,P.A.A.TEUNISSEN,P.J.M.VAN BENTUM		
1781	PRB0371587		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1988																												T																				36					36																																																2.4	2																																														0						TEMPERATURE-DEPENDENT FAR-INFRARED REFLECTANCE OF LA-SR-CU-O AND LA-CA-CU-O:BARDEEN-COOPER-SCHRIEFFER ELECTRODYNAMICS BUT UNCERTAIN ENERGY GAP	198802	FAR-INFRARED             ,ENERGY GAP	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)1587	A.ZETTL,M.S.SHERWIN,P.L.RICHARDS	LA,SR,CU,O,LA,CA,CU,O	
1782	PRB0371587		(La,Ca)2CuO4	La1.85Ca0.15Cu1O4	La	1.85	Ca	0.15	Cu	1															O	4			1988																												T																				17					17																																																2.4	2																																														0						TEMPERATURE-DEPENDENT FAR-INFRARED REFLECTANCE OF LA-SR-CU-O AND LA-CA-CU-O:BARDEEN-COOPER-SCHRIEFFER ELECTRODYNAMICS BUT UNCERTAIN ENERGY GAP	198802	FAR-INFRARED             ,ENERGY GAP	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)1587	A.ZETTL,M.S.SHERWIN,P.L.RICHARDS	LA,SR,CU,O,LA,CA,CU,O	
1783	PRB0389284			Ba1Pb0.8Bi0.2O3	Ba	1	Pb	0.8	Bi	0.2															O	3			1988																												T																				9.5					9.5																																																3.2	2																																														0						SUPERCONDUCTING ENERGY GAP OF BA(1)PB(1-X)BI(X)O(3)	198811	INFRARED                 ,ENERGY GAP               ,POLYCRYS	IBM RESEARCH DIVISION,THOMAS J.WATSON RESEARCH CENTER.P.O.YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,38(1988)9284	B.A.SCOTT,J.A.CALISE,R.T.COLLINS,Z.SCHLESINGER	BA,BI,PB,O	
1784	PR0365275		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				35					35																																																2	2																																														0						NORMAL-STATE REFLECTIVITY AND SUPERCONDUCTING ENERGY-GAP MEASUREMENT OF LA2-XSRXCUO4	10	REFLECTIVITY        ,GAP	IBM THOMAS J. WATSON RESEARCH CENTER, YORKTOWN HEIGHTS, NEW YORK 10598	PHYS.REV.B,36(1987)5275	E.M.ENGLER,M.W.SHAFER,R.T.COLLINS,Z.SCHLESINGER	LA,SR,CU,O	
1785	PRL0630330		(La,Sr)2CuO4	La1.89Sr0.11Cu1O4	La	1.89	Sr	0.11	Cu	1															O	4			1989																												T																				10					10																																																3.48	8																																														0						TEMPERATURE DEPARTMENT OF THE MAGNETIC EXCITATIONS IN LA1.85SR0.15CUO4 (TC=33 K)	198907	ENERGY GAP	BROOKHAVEN NATIONAL LABORATORY, UPTON, NEW YOIRK 11973	PHYS.REV.LETT.,63(1989)330	G.SHIRANE,H.KOJIMA,I.TANAKA,K.KITAZAWA,K.YAMADA,M.A.KASTNER,P.GEHRING,R.J.BIRGENEAU,T.R.THURSTON,Y.ENDOH	LA,SR,CU,O	
1786	PRL0630330		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1989																												T																				33					33																																																3.52	8																																														0						TEMPERATURE DEPARTMENT OF THE MAGNETIC EXCITATIONS IN LA1.85SR0.15CUO4 (TC=33 K)	198907	ENERGY GAP	BROOKHAVEN NATIONAL LABORATORY, UPTON, NEW YOIRK 11973	PHYS.REV.LETT.,63(1989)330	G.SHIRANE,H.KOJIMA,I.TANAKA,K.KITAZAWA,K.YAMADA,M.A.KASTNER,P.GEHRING,R.J.BIRGENEAU,T.R.THURSTON,Y.ENDOH	LA,SR,CU,O	
1787	PRL0641067		(Nd,Th)2CuO4	Nd1.85Th0.15Cu1O4-Y	Nd	1.85	Th	0.15	Cu	1															O	4-Y			1990																												T'				3.955		12.116														18					18																																																3.9	2																																														0						ENERGY GAPS OF ND1.85CE0.15CUO4-Y AND ND1.85TH0.15CUO4-Y DETERMINED BY FAR-INFRARED SPECTROSCOPY	199002		DEPARTMENT OF PHYSICS, SIMON FRASER UNIVERSITY, BURNABY, BRITISH COLUMBIA, CANADA V5A 1S6	PHYS.REV.LETT.,64(1990)1067	B.P.CLAYMAN,J.L.PENG,L.ZHANG,Q.SONG,R.N.SHELTON,S.H.WANG	ND,CE,CU,O,TH	
1788	PRL0641067		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Y	Nd	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'				3.959		12.11														23					23																																																3.1	2																																														0						ENERGY GAPS OF ND1.85CE0.15CUO4-Y AND ND1.85TH0.15CUO4-Y DETERMINED BY FAR-INFRARED SPECTROSCOPY	199002		DEPARTMENT OF PHYSICS, SIMON FRASER UNIVERSITY, BURNABY, BRITISH COLUMBIA, CANADA V5A 1S6	PHYS.REV.LETT.,64(1990)1067	B.P.CLAYMAN,J.L.PENG,L.ZHANG,Q.SONG,R.N.SHELTON,S.H.WANG	ND,CE,CU,O,TH	
1789	PR0365735		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1987																												T																				37					37																																																2.6	2																																														0						FAR-INFRARED COMPOSITE-MEDIUM STUDY OF SINTERED LA2NIO4 AND LA1.85SR0.15CUO4-Y	10	INFRARED            ,GAP	LABORATORY OF ATOMIC AND SOLID STATE PHYSICS AND MATERIALS SCIENCE CENTER, CORNELL UNIVERSITY, ITHACA, NEW YORK 14853-2501	PHYS.REV.B,36(1987)5735	A.J.SIEVERS,J.T.MCWHIRTER,P.E.SULEWSKI,T.W.NOH	LA,NI,O,SR,CU	
1790	PRL0641067		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Y	La	1.85	Sr	0.15	Cu	1															O	4-Y			1990																												T'																				36					36																																																3.2	2																																														0						ENERGY GAPS OF ND1.85CE0.15CUO4-Y AND ND1.85TH0.15CUO4-Y DETERMINED BY FAR-INFRARED SPECTROSCOPY	199002		DEPARTMENT OF PHYSICS, SIMON FRASER UNIVERSITY, BURNABY, BRITISH COLUMBIA, CANADA V5A 1S6	PHYS.REV.LETT.,64(1990)1067	B.P.CLAYMAN,J.L.PENG,L.ZHANG,Q.SONG,R.N.SHELTON,S.H.WANG	ND,CE,CU,O,TH	
1791	PRB0367121		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				92.4					92.4																																																4.8	1																																														0						INVESTIGATION OF THE ENERGY GAP OF Y-BA-CU-O BY POINT-CONTACT JOSEPHSON-JUNCTION TECHNIQUES	198711	POINT CONTACT            ,ENERGY GAP               ,I-V CHAR	DIPARTIMENTO DI FISICA NUCLEARE,STRUTTURA DELLA MATERIA E FISICA APPLICATA,UNIVERSITA DI NAPOLI,NAPOLI,ITALY	PHYS.REV.B,36(1987)7121	A.BARONE,A.DI CHIARA,A.M.CUCOLO,E.OLZI,F.C.MATACOTTA,G.PELUSO,R.VAGLIO,U.SCOTTI DI UCCIO	Y,BA,CU,O	
1792	PRB0396571		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1989																												Y123																				92					92																																																8	2																																														0						REFLECTIVTY AND CONDUCTIVITY OF YBA2CU3O7	198904		IBM THOMAS J.WATSON RESEARCH CENTER,YOKTOWN HEIGHTS,NEW YORK 10598	PHYS.REV.B.,39(1989)6571	C.FEILD,F.HOLTZBERG,P.CHAUDHARI,R.T.COLLINS,Z.SCHLESINGER	INFRARED,REFLECTIVITY	
1793	PRB0402170	GAPENE,2.6-6.0	YBa2Cu3O7	Y1Ba2Cu3O9-Y	Y	1	Ba	2	Cu	3															O	9-Y			1989																												Y123																				89					89																																																6	2																																														0						PHONON ANOMALIES AND RANGE OF SUPERCONDUCTING ENERGY GAPS FROMINFRARED STUDIES OF YBA2CU3O7-Z	198908	INFRARED            ,PHONONS             ,LATTICE-DYNAMICS    ,DIELECTRIC          ,ENERGY GAP	MAX-PLANCK-INSTIFUT FUR FESTKORPERFORSCHUNG,HEISENBERGSTRASSE1,D-7000 STUTTART 80,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,40(1989)2170	A.SIMON,A.WITTLIN,E.SCHONHERR,L.GENZEL,M.BAUER,M.CARDONA	Y,BA,CU,O	
1794	PRL0631008	AB PLANE GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1989																												Y123																				89					89																																																4.95	1																																														0						REPRODUCIBLE TUNNELING DATA ON CHEMICALLY ETCHED SINGLE CRYSTALS OF YBA2CU3O7	198908	TUNNEL JUNCTIONS    ,SINGLE CRYSTALS     ,CONDUCTANCE	AT & BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.LETT., 63(1989)1008	A.M.CUCOLO,J.M.VALLES,J.P.GARNO,J.V.WASZCZAK,JR.,L.F.SCHNEEMEYER,M.GURVITCH,R.C.DYNES	Y,BA,CU,O	
1795	PRL0631008	C AXIS GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1989																												Y123																				89					89																																																1.04	1																																														0						REPRODUCIBLE TUNNELING DATA ON CHEMICALLY ETCHED SINGLE CRYSTALS OF YBA2CU3O7	198908	TUNNEL JUNCTIONS    ,SINGLE CRYSTALS     ,CONDUCTANCE	AT & BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.LETT., 63(1989)1008	A.M.CUCOLO,J.M.VALLES,J.P.GARNO,J.V.WASZCZAK,JR.,L.F.SCHNEEMEYER,M.GURVITCH,R.C.DYNES	Y,BA,CU,O	
1796	PRB0358846	GAP,3.7-5.6	YBa2Cu3O7	Y1Ba2Cu3O9-Y	Y	1	Ba	2	Cu	3															O	9-Y			1987																												Y123																				90					90																																																5.6	1																																														0						TUNNELING AND INFRARED MEASUREMENTS OF THE ENERGY GAP IN THE HIGH-CRITICAL-TEMPERATURE SUPERCONDUCTOR Y-BA-CU-O	198706		IBM THOMAS J. WATSON LAB.,YORKTOWN HEIGHTS,NEW YORK,USA	PHYS.REV.B,35(1987)8846	D.A.CHANCE,J.R.KIRTLEY,R.L.SANDSTROM,R.T.COLLINS,T.R.DINGER,W.J.GALLAGHER,Z.SCHLESINGER		
1797	PRL0631008		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1989																												Y123																				89					89																																																4.1	1																																														0						REPRODUCIBLE TUNNELING DATA ON CHEMICALLY ETCHED SINGLE CRYSTALS OF YBA2CU3O7	198908	TUNNEL JUNCTIONS    ,SINGLE CRYSTALS     ,CONDUCTANCE	AT & BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.LETT., 63(1989)1008	A.M.CUCOLO,J.M.VALLES,J.P.GARNO,J.V.WASZCZAK,JR.,L.F.SCHNEEMEYER,M.GURVITCH,R.C.DYNES	Y,BA,CU,O	
1798	PRB03811955	GAP,4-7	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		2	1988																												Bi2212																				90					90																																																7	4																																														0						Raman scattering spectra of superconducting Bi2Sr2CaCu2O8 single crystals	198812		Varian Research Center, 611 Hansen Way, Palo Alto, California 94303	Phys.Rev.B,38(1988)11955	A. Kapitulnik,D. Kirillov,D.B. Mitzi,I. Bozovic,T.H. Geballe		
1799	PRL0611313	GAP,3-4	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1988																												Y123																				90					90																																																4	2																																														0						BA(2)TCU(3)O(7-Z): ELECTRODYNAMICS OF CRYSTALS WITH HIGH REFLECTIVITY	198809	REFLECTANCE              ,OPTICS                   ,ENERGY G	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.LETT.,61(1988)1313	A.J.MILLIS,D.H.RAPKINE,G.A.THOMAS,J.ORENSTEIN,J.V.WASZCZAK,L.F.SCHNEEMEYER,M.CAPIZZI,R.N.BHATT	Y,BA,CU,O	
1800	PRL0620336		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1989																												Bi2212																				88					88																																																8	9																																														0						HIGH-RESOLUTION PHOTOEMISSION STUDY OF THE LOW-ENERGY EXCITATIONS REFLECTING THE SUPERCONDUCTING STATE OF BI-SR-CA-CU-O SINGLE CRYSTALS	198901	SINGLE CRYSTAL           ,ULTRA VIOLET             ,PES                      ,EN	INSTITUT DE PHYSIQUE,UNIVERSITE DE NEUCHATEL,SWITZERLAND	PHYS.REV.LETT.,62(1989)336	A.ZETTL,B.DARDEL,F.PATTHEY,J.-M.IMER,W.-D.SCHNEIDER,Y.BAER,Y.PETROFF	BI,SR,CA,CU,O	
1801	PRB0365592		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1987																												Y123																				85					85																																																3.4	4																																														0						RAMAN DETECTION OF THE SUPERCONDUCTING GAP IN BA-Y-CU-O SUPERCONDUCTORS	198710	RAMAN                    ,THIN FILM                ,ANISOTROPY               ,EN	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)5592	H.S.CHEN,J.KWO,K.B.LYONS,M.HONG,S.H.LIOU,T.J.NEGRAN	BA,Y,CU,O	
1802	PHC1660015	GAP=7.8-9.3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1990																												Bi2212																				80					80																																																9.3	1																																														0	MIXTURE-(950C IN AIR)-C(1C/H) TO BELOW 600C					SUPERCONDUCTING ENERGY GAP OF SINGLE-CRYSTAL BI2XR2CA1CU2O8+ZBY ELECTRON TUNNELING			INSTITUTO DE INVESTIGACIONES EN MATERIALES. UNIJVERSIDAD NACIONAL AUTONOMA DE MEXICO, A. POSTAL 70-360 MEXICO.	PHYSICA C,166(1990)15	E.GUARNER,F.MORALES,R.ESCUDERO	BI,SR,CA,CU,O	
1803	PRB03811970	GAP=1.3-6.5	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1988																												Y123																				90					90																																																6.5	10																																														0						MICROWAVE TRANSMISSION THROUGH FILMS OF Y(1)BA(2)CU(3)O(7-Z)	198812	MICROWAVE                ,THIN FILM                ,CONDUCTIVITY             ,PENETRATION DEPTH	IBM RESEARCH DIVISION,THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,38(1988)11970	C.S.NICHOLS,N.S.SHIREN,R.B.LAIBOWITZ,T.G.KAZYAKA	Y,BA,CU,O	
1804	PRL0630422	AB PLANE GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1989																												Y123																				92					92																																																8	2																																														0						INFRARED EVIDENCE FOR GAP ANISOTROPY IN YBA(2)CU(3)O(7)	198907	INFRARED            ,ENERGY GAP          ,ANISOTROPY	IBM T.J.WATSON RESEACH CENTER,YORKTOWN HEIGHTS,NEW YORK 10598	PHYS.REV.LETT.,63(1989)422	C.FIELD,F.HOLTZBERG,R.T.COLLINS,Z.SCHLESINGER	Y,BA,CU,O	
1805	PRL0630422	C-AXIS GAP	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1989																												Y123																				92					92																																																3	2																																														0						INFRARED EVIDENCE FOR GAP ANISOTROPY IN YBA(2)CU(3)O(7)	198907	INFRARED            ,ENERGY GAP          ,ANISOTROPY	IBM T.J.WATSON RESEACH CENTER,YORKTOWN HEIGHTS,NEW YORK 10598	PHYS.REV.LETT.,63(1989)422	C.FIELD,F.HOLTZBERG,R.T.COLLINS,Z.SCHLESINGER	Y,BA,CU,O	
1806	PR0368903	EPITAXIAL FILM	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y		4	1987																												Y123																				92					92																																																4.5	1																																														0						PROPERTIES OF EPITAXIAL FILMS OF Y(1)BA(2)CU(3)O(7-Z)	12		IBM RESEARCH CENTER,P.O.BOX,NEW YORK	PHYS.REV.B,36(1987)8903	ARMIN P.SEGMULLER,E.J.MCNIFF,F.K.LEGOUES,J.R.KIRTLEY,JR.,P.CHAUDHARI,P.FREITAS,R.B.LAIBOWITZ,R.H.KOCH,R.J.GAMBINO,R.T.COLLINS,S.FONER,T.PENNEY,T.R.MCGUIRE,Z.SCHLESINGER	Y,BA,CU,O	
1807	PR0368903		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				92					92																																																4.5	2																																														0						PROPERTIES OF EPITAXIAL FILMS OF Y(1)BA(2)CU(3)O(7-Z)	12		IBM RESEARCH CENTER,P.O.BOX,NEW YORK	PHYS.REV.B,36(1987)8903	ARMIN P.SEGMULLER,E.J.MCNIFF,F.K.LEGOUES,J.R.KIRTLEY,JR.,P.CHAUDHARI,P.FREITAS,R.B.LAIBOWITZ,R.H.KOCH,R.J.GAMBINO,R.T.COLLINS,S.FONER,T.PENNEY,T.R.MCGUIRE,Z.SCHLESINGER	Y,BA,CU,O	
1808	PRL0591860	CU(1) SITEGAP	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				92					92																																																8.3	6																																														0						Evidence for Two Pairing Energies from Nuclear Spin-Lattice Relaxation in Superconducting Ba2YCu3O7-delta	198710		AT & T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.59(1987)1860	G.F. Brennert,G.P. Espinosa,J.P. Remeika,Jr., R.E. Walstedt,W.W. Warren		
1809	PRL0591860	CU(2) SITE GAP	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				92					92																																																2.4	6																																														0						Evidence for Two Pairing Energies from Nuclear Spin-Lattice Relaxation in Superconducting Ba2YCu3O7-delta	198710		AT & T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.59(1987)1860	G.F. Brennert,G.P. Espinosa,J.P. Remeika,Jr., R.E. Walstedt,W.W. Warren		
1810	PRB0387133		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1988																												Y123																				88					88																																																14.8	4																																														0						LIGHT-SCATTERING STUDY OF THE SUPERCONDUCTING ENERGY GAP IN Y(1)BA(2)CU(3)O(7) SINGLE CRYSTALS	198810	RAMAN                    ,SINGLE-CRYSTAL           ,ENERGY G	PHYSIK DEPARTMENT E21,TECHNISCHE UNIVERSITAT MUNCHEN,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,38(1988)7133	D.EINZEL,K.ANDRES,P.MULLER,R.HACKL,W.GLASER		
1811	PRB0387133		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1988																												Y123																				83					83																																																2.6	4																																														0						LIGHT-SCATTERING STUDY OF THE SUPERCONDUCTING ENERGY GAP IN Y(1)BA(2)CU(3)O(7) SINGLE CRYSTALS	198810	RAMAN                    ,SINGLE-CRYSTAL           ,ENERGY G	PHYSIK DEPARTMENT E21,TECHNISCHE UNIVERSITAT MUNCHEN,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,38(1988)7133	D.EINZEL,K.ANDRES,P.MULLER,R.HACKL,W.GLASER		
1812	PRB0371574	GAP=2.98-4.8	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1988																												Y123																				94					94																																																4.8	2																																														0						FAR-INFRARED PROPERTIES OF AB-PLANE ORIENTED Y(1)BA(2)CU(3)O(7-Z)	198802	FAR-INFRARED             ,PHONON	INSTITUTE FOR MATERIALS RESARCH,MCMASTER UNIVERSITY,HAMILTON,ONTARIO,CANADA	PHYS.REV.B,37(1988)1574	A.H.O'REILLY,C.V.STAGER,D.A.BONN,D.B.TANNER,J.E.GREEDAN,K.KAMARAS,T.TIMUSK	Y,BA,CU,O	
1813	PRB0360846		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				93					93																																																3.5	2																																														0						FAR-INFRARED SPECTRA OF POLYCRYSTALLINE BA(2)Y(1)CU(3)O(9-Z)	198707	REFLECTANCE              ,FAR-INFRARED	AT&T BELL LAB.,MURRAY HILL,NEW JERSEY,USA	PHYS.REV.B,36(1987)846	A.J.MILLIS,D.W.JOHNSON.JR.,E.A.RIETMAN,G.A.THOMAS,G.P.ESPINOSA,H.K.NG,J.M.VANDENBERG,R.J.CAVA,R.N.BHATT		
1814	PRL0590704	EPITAXIAL FILM	YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y		4	1987																												Y123																				90					90																																																4.7	2																																														0						COMPARATIVE STUDY OF SUOERCONDUCTING ENERGY GAPS IN ORIENTED FILMS AND POLYCRYSTALLINE BULK SAMPLES OF Y-BA-CU-O	198710		IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.LETT.,59(1987)704	P.FREITAS,R.B.LAIBOWITZ,R.H.KOCH,R.L.SANDSTROM,R.T.COLLINS,T.R.DINGER,T.S.PLASKETT,W.J.GALLAGHER,Z.SCHLESINGER		
1815	PRB0358856		YBa2Cu3O7	Y1Ba2Cu3O7-Y	Y	1	Ba	2	Cu	3															O	7-Y			1987																												Y123																				93					93																																																4.8	1																																														0						BREAK-JUNCTION TUNNELING MEASUREMENTS OF THE HIGH-TC SUPERCONDUCTOR Y(1)BA(2)CU(3)O(9-Z)	198706	TUNNELING	NBS,BOULDER,COLORADO,USA	PHYS.REV.B,35(1987)8856	A.F.CLARK,J.KWO,J.MORELAND,J.W.EKIN,L.F.GOODRICH,M.HONG,S.H.LIOU,T.E.CAPOBIANCO		
1816	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7-Z	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7-Z			1989																												Y123				3.861		11.682														77.3					77.3																																																																																		3.19												Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1817	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z			1989																												Y123				3.861		11.676														73.7					73.7																																																																																		4.89												Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1818	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.775Fe0.225O7-Z	Y	1	Ba	2	Cu	2.775	Fe	0.225													O	7-Z			1989																												Y123				3.865		11.68														57.6					57.6																																																																																														Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1819	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7.15	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7-Z	7.15		1989																												Y123	P4/MMM			3.865		11.668														36					36																																																																																														Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1820	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.55Fe0.45O7-Z	Y	1	Ba	2	Cu	2.55	Fe	0.45													O	7-Z			1989																												Y123				3.873		11.66																																																																																																																	Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1821	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.5Fe0.5O7.23	Y	1	Ba	2	Cu	2.5	Fe	0.5													O	7-Z	7.23		1989																												Y123	P4/MMM			3.871		11.661																																																																																																																	Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1822	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2Fe1O7-Z	Y	1	Ba	2	Cu	2	Fe	1													O	7-Z			1989																												Y123				3.866		11.66																																																																																																																	Y2O3,BACO3,CUO,FE2O3	0	CAL(900C IN AIR)-SIN(970C 40H IN O2)-ANN(665C 8H)-FC					MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1823	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.95Mo0.05OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.95	Mo	0.05											O	Y			1990																																																107.1					107.1																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1824	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.9Mo0.1OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.9	Mo	0.1											O	Y			1990																																																107					107																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1825	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.85Mo0.15OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.85	Mo	0.15											O	Y			1990																																																98.5					98.5																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1826	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.8Mo0.2OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.8	Mo	0.2											O	Y			1990																																																98.4					98.4																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1827	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.75Mo0.25OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.75	Mo	0.25											O	Y			1990																																																96.9					96.9																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1828	PHC1700035		(BI,PB)2SR2CA2(CU,MO)3O10	Bi1.6Pb0.4Sr2Cu2.7Mo0.3OY	Bi	1.6	Pb	0.4	Sr	2	Cu	2.7	Mo	0.3											O	Y			1990																																																96.9					96.9																																																																																															0						SUPERDONDUCTING PROPERTIES OF SUBSTITUTED BI1.6PB0.4SR2CA2(CU3-XMOX)OY			UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA, HEFEI, PR CHINA	PHYSICA C,170(1990)35	CHEN ZHAOJIA,DONG YI,FENG GUOBIN,HAN ZHIYI,MAO ZHIQIANG,WANG HAIQIAN,WANG YU,ZHANG YUHENG,ZHOU GUIEN	BI,PB,SR,CA,CU,MO,O	
1829	PHC1700245	TWO PHASE Y123,(A=3.84,B=3.86,C=11.68),(	YBA2CU2PBOZ	Y1Ba2Cu2Pb1OX	Y	1	Ba	2	Cu	2	Pb	1													O	X			1990																																															80	90	93				90																																																																																															0	PREPARED BY PYROPHORIC PROCESS                                  SIN(885C 20H IN AIR)					LATTICE AND ELECTRONIC STRUCTURE OF YBA2CU2PBOX SUPERCONDUCTOR			MATERIALS SCIENCE CENTRE, INDIAN INSTITUTE OF TECHNOLOGY, KHARAGPUR, KHARAGPUR-721302, INDIA	PHYSICA C,170(1990)245	D.BHATTCHARYA,D.K.PANDYA,D.SEN,K.L.CHOPRA,L.C.PATHAK,S.C.KASHYAP,S.MISHRA	Y,BA,CU,PB,O	
1830	PHC1700139	NO SUP/CON	YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8	6.8		1990																											2	Y123	P4/MMM			6.871		11.626																																																																																																																		0						"YBA2CU3O6.8: AN OXYGEN-RICH ""123""-TYPE PHASE SWITH TETRAGONALSYMMETRY"			LABORATOIRE CRISMAT, ISMRA, UNIVERSITE DE CAEN, BOULEVARD DU MARECHAL JUIN, 14032 CAEN CEDEX, FRANCE	PHYSICA C,170(1990)139	B.RAVEAU,F.BOTEREL,G.DESGARDIN,J.M.HAUSSONNE,J.WANG,M.HERVIEU,V.CAIGNAERT	Y,BA,CU,O	
1831	PHC1690391	S-I-N JUNCTION I=AU	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		4	1990																											1	BKBO																				16					16																																																3.7	1																																														16	EPITAXIAL FILM, FILMS((110) ORIENTED) ON STTIO3(110) SUBSTRATE BY RF MAGNETRON SPUTTERING					GAP OBSERVATION BY TUNNELING MEASUREMENT ON SUPERCONDUCTING BA1-XKXBIO3 THIN FILM: A FINITE ENERGY GAP IN BA1-XKXBIO3			DEPARTMENT OF APPLIED PHYSICS, UNIVERSITY OF TOKYO, BUNKYO-KU,TOKYO 113, JAPAN	PHYSICA C,169(1990)391	H.SATO,H.TAKAGI,S.UCHIDA	BA,K,BI,O	
1832	PHC1690464	EXCESS O IN THE INTERLAYER SITE,NO S/C	(LA,SR)2CU2O6	La1.85Sr1.15Cu2O6.25	La	1.85	Sr	1.15	Cu	2															O	6.25			1990																											2	2126	I4/MMM			3.853		20.083																																																																																																																	LA2O3,SRCO3,CUO	1	(1000C 20H IN 1ATM O2)-G-(1050C 20H IN 1ATM O2)-ANN(500+450+400+350+300+250C EACH 12H)-C TO 100C					OXYGEN-DEFECT STRUCTURE OF NON-SUPERCONDUCTING LA1.85SR1.15CU2O6.25: EXCESS OXYGEN IN THE INTERLAYER SITE			MATERIALS SCIENCE  DIVISION AND SCIENCE AND TECHNOLOGY CENTERFOR SUPERCONDUCTIVITY, ARGONNE NATIONALLABORATORY, ARGONNE,1L60439, USA	PHYSICA C,169(1990)464	A.MANTHIRAM,J.B.GOODENOUGH,J.D.JORGENSEN,P.LIGHTFOOT,SHIYOU PEI,X.-X. TANG	LA,SR,CU,O	
1833	PHC1690377	NO S/C,CRYSTAL TYPE=0212	(LA,SR)2CACU2OZ	La1.6Sr0.4Ca1Cu2OY	La	1.6	Sr	0.4	Ca	1	Cu	2													O	Y		1	1990																											2	2126	I4/MMM			3.822		19.545																																																																																																																	LA2O3,SRCO3,CUO,CACO3	1	CAL(900C 5H IN AIR)-SIN(1050C 24H IN O2)-C(100C/H)					"X-RAY RIETVELD STUDY OF NONSUPERCONDUCTING ""0212"" CUPRATE; LA1.6SR0.4CACU2OY"			CENTRAL RESEARCH LABORATORIES, MATSUSHITA ELECTRIC INDUSTRIALCO., LTD., 3-15 YAGUMO-NAKAMACHI, MORIGUCHI, OSAKA 570, JAPAN	PHYSICA C,169(1990)377	HIDEAKI ADACHI,KENTARO SETSUNE,KIYOTAKE WASA,SEIJI ADACH	LA,SR,CA,CU,O	
1834	PHC1680521		Tl(Sr,Nd)2CaCu2Oz	Tl1Sr1.3Nd0.7Ca1Cu2O7	Tl	1	Sr	1.3	Nd	0.7	Ca	1	Cu	2											O	7		1	1990																											2	Tl1212	P4/MMM			3.828		11.987															81				81																																																																																														TL2O3,CUO,ND2O3,(SR,CA)-PEROXIDE	1	HEAT IN SEALED AU TUBE(890C 12H)					STRUCTURE OF TI(SR0.65ND0.35)2CACU2O7NEUTRON POWDER DEFFRACTION STUDY OF CATI0N ORDERING AND OXYGENSTOICHIOMETRY			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545-1663, USA	PHYSICA C,186(1990)521	GEORGE H. KWEI,M.A.SUBRAMANIAN	TL,SR,ND,CA,CU,O	
1835	PHC1590245		(Tl,Pb)Sr2CaCu2Oz	Tl0.5Pb0.5Sr2Ca1Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2											O	7			1989																												Tl1212				3.802		12.107															85				85																																																																																														TL2O3,PBO2,SRO2,CAO2,CUO	0	(850-915C 3-12H IN SEALED AU TUBE)					THE SUPERCONDUCTORS (Tl,Pb)SrCaCu2O7 AND (Tl,Pb)Sr2Ca2Cu3O9: neutron POWDER DIFFRACTION, HIGH RESOLUTION ELECTRON MICROSCOPY AND X-RAY ABSORPTION STUDIES			E.I. du Pont de Nemours & Company, Central Research and Development Department, Experimental Station, P.O. Box 80356, Wilmington, Delaware 19880-0356, USA	Physica.C,159(1989)245-254	A.W. SLEIGHT,J. GOPALAKRISHNAN,J.B. PARISE,M.A. SUBRAMANIAN,P.L. GAI		
1836	PRB0396667		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1989																												Y123				3.82	3.885	11.676														89.8				0.2	89.8																																																																																		0.8													0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1837	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.985Fe0.015O7-Z	Y	1	Ba	2	Cu	2.985	Fe	0.015													O	7-Z			1989																												Y123				3.822	3.885	11.68														90				7	90																																																																																															0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1838	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.97Fe0.03O7-Z	Y	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z			1989																												Y123				3.825	3.885	11.672														89.2					89.2																																																																																		1.24													0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1839	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O7-Z	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z			1989																												Y123				3.829	3.881	11.678														86.7					86.7																																																																																															0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1840	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O7-Z	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7-Z			1989																												Y123				3.834	3.879	11.677														86.4					86.4																																																																																		1.91													0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1841	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.925Fe0.075O7-Z	Y	1	Ba	2	Cu	2.925	Fe	0.075													O	7-Z			1989																												Y123				3.842	3.868	11.678														86.4					86.4																																																																																															0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1842	PRB0396667		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.91Fe0.09O7-Z	Y	1	Ba	2	Cu	2.91	Fe	0.09													O	7-Z			1989																												Y123				3.852	3.861	11.686														82.8					82.8																																																																																		3.19													0						MICROSTRUCTURE,LATTICE PARAMETERS,AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3O7-Z	198904	TC                  ,TEM                 ,LATTICE PARAMETERS  ,DISTORTION          ,TWIN BOUNDARY	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK 11973	PHYS.REV.B.,39(1989)6667	A.R.MOODENBAUGH,J.TAFTO,M.SUENAGA,R.L.SABATINI,YOUWEN XU	Y,BA,CU,FE,O	
1843	PRB0394756		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		2	1989																												Y123																			90.71					0.3	90.71																																2.7	0.72						26	5.5																																																							0						MAGNETORESISTANCE AND THERMODYNAMIC FLUCTUATIONS IN SINGLE-CRYS-TAL YBA(2)CU(3)O(Y)	198903	MAGNETORESISTANCE        ,SINGLE CRYSTAL           ,FLUCTUAT	NIPPON TELEGRAPH AND TELEPHONE CORPORATION OPTO-ELECTRONICS LAB-ORATORIES,TOKAI,IBARAKI 319-11,JAPAN	PHYS. REV. B., 39(1989)4756	MAKOTO HIKITA,MINORU SUAUKI	Y,BA,CU,O	
1844	PRB0370619		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1988																												Y123																				92.5					92.5																																																																																			0.4												0						CRITICAL-MAGNETIC-FIELD ANISOTROPY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7)	198801	HC                       ,SINGLE CRYSTAL	FRANCIS BITTER NATIONAL MAGNET LABORATORY,MASSACHUSETTS INSTITUTE OF TECHNOLOGY,CAMBRIDGE,MASSACHUSETTS	PHYS.REV.B,37(1988)619	C.X.HAO,G.A.GIBSON,J.E.TKACZYK,J.S.MOODERA,P.M.TEDROW,R.MESERVEY	Y,BA,CU,O	
1845	PRL0591160		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		2	1987																												Y123																				88.8					88.8																																2.3	0.71						34	7																																																							0						ANISOTROPIC NATURE OF HIGH-TEMPERATURE SUPERCONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-X)	198709	HC                       ,ANISOTROPY               ,SINGLE C	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.LETT.,59(1987)1160	T.K.WORTHINGTON,T.R.DINGER,W.J.GALLAGHER	Y,BA,CU,O	
1846	PHC1680023		Bi2Sr2(Y,Ca)Cu2O8	Bi2Sr2Y0.9Ca0.1Cu2OY	Bi	2	Sr	2	Y	0.9	Ca	0.1	Cu	2											O	Y		1	1990								300																				Bi2212																																																																																																																							BI2O3,CACO3,Y2O3,CUO	1	CAL(800C)-(860C FOR X=1,900C FOR X=0)-SIN(100H)					INTERNAL MAGNETIC FIELDS AT (MYU+) SITES AND THE MAGNETIC PHASE DIAGRAM OF BI2SR2Y1-XCAXCU2OYSYSTEM STUDIED BY THE (MYU)SR METHOD			DEPT.OF PHYSICS,TOKYO INST.OF TECHNOLOGY,MEGURO-KU,TOKYO 152,JAPAN	PHYSICA C,168(1990)23	H.MIYATAKE,J.H.BREWER,K.NAGAMINE,K.NISHIYAMA,N.NISHIDA,R.KADONO,R.YOSHIZAKI,S.OKUMA,T.TAMEGAI,Y.IYE	BI,SR,Y,CA,CU,O	
1847	PHC1680023		Bi2Sr2(Y,Ca)Cu2O8	Bi2Sr2Y0.8Ca0.2Cu2OY	Bi	2	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	Y		1	1990								257																				Bi2212																																																																																																																							BI2O3,CACO3,Y2O3,CUO	1	CAL(800C)-(860C FOR X=1,900C FOR X=0)-SIN(100H)					INTERNAL MAGNETIC FIELDS AT (MYU+) SITES AND THE MAGNETIC PHASE DIAGRAM OF BI2SR2Y1-XCAXCU2OYSYSTEM STUDIED BY THE (MYU)SR METHOD			DEPT.OF PHYSICS,TOKYO INST.OF TECHNOLOGY,MEGURO-KU,TOKYO 152,JAPAN	PHYSICA C,168(1990)23	H.MIYATAKE,J.H.BREWER,K.NAGAMINE,K.NISHIYAMA,N.NISHIDA,R.KADONO,R.YOSHIZAKI,S.OKUMA,T.TAMEGAI,Y.IYE	BI,SR,Y,CA,CU,O	
1848	PHC1680023		Bi2Sr2(Y,Ca)Cu2O8	Bi2Sr2Y0.7Ca0.3Cu2OY	Bi	2	Sr	2	Y	0.7	Ca	0.3	Cu	2											O	Y		1	1990								16																				Bi2212																																																																																																																							BI2O3,CACO3,Y2O3,CUO	1	CAL(800C)-(860C FOR X=1,900C FOR X=0)-SIN(100H)					INTERNAL MAGNETIC FIELDS AT (MYU+) SITES AND THE MAGNETIC PHASE DIAGRAM OF BI2SR2Y1-XCAXCU2OYSYSTEM STUDIED BY THE (MYU)SR METHOD			DEPT.OF PHYSICS,TOKYO INST.OF TECHNOLOGY,MEGURO-KU,TOKYO 152,JAPAN	PHYSICA C,168(1990)23	H.MIYATAKE,J.H.BREWER,K.NAGAMINE,K.NISHIYAMA,N.NISHIDA,R.KADONO,R.YOSHIZAKI,S.OKUMA,T.TAMEGAI,Y.IYE	BI,SR,Y,CA,CU,O	
1849	PHC1690107	JC DETERMINED AT 1 UV INRESISTANCE MEASUREMENT	YBa2Cu3O7	Y1Ba2Cu3OY	Y	1	Ba	2	Cu	3															O	Y			1990																												Y123																				92					92																																																		81																																												Y2O3,BACO3,CUO,AG2O	1	(920C 10H)-SIN(960C 12H IN O2)					CRITICAL CURRENT DENSITY OF AG-DOPED Y-BA-CU-O SUPERCONDUCTORSIN LOW MAGNETIC FIELDS			DEPARTMENT OF PHYSICS,STATE UNIVERSITY OF NEW YORK AT BUFFALO,BUFFALO, NY 14260, USA	PHYSICA C,169(1990)107	L.W.SONG,Y.H.KAO	AG,Y,BA,CU,O	
1850	PHC1690107		YBa2(Cu,Ag)3O7	Y1Ba2Cu2.85Ag0.15OY	Y	1	Ba	2	Cu	2.85	Ag	0.15													O	Y			1990																												Y123																				91.3					91.3																																																		480																																												Y2O3,BACO3,CUO,AG2O	1	(920C 10H)-SIN(960C 12H IN O2)					CRITICAL CURRENT DENSITY OF AG-DOPED Y-BA-CU-O SUPERCONDUCTORSIN LOW MAGNETIC FIELDS			DEPARTMENT OF PHYSICS,STATE UNIVERSITY OF NEW YORK AT BUFFALO,BUFFALO, NY 14260, USA	PHYSICA C,169(1990)107	L.W.SONG,Y.H.KAO	AG,Y,BA,CU,O	
1851	PHC1690107	IMPURITY,BACUO2,Y2O3,Y2BACUO5	YBa2(Cu,Ag)3O7	Y1Ba2Cu2.7Ag0.3OY	Y	1	Ba	2	Cu	2.7	Ag	0.3													O	Y			1990																												Y123																				90.2					90.2																																																		170																																												Y2O3,BACO3,CUO,AG2O	1	(920C 10H)-SIN(960C 12H IN O2)					CRITICAL CURRENT DENSITY OF AG-DOPED Y-BA-CU-O SUPERCONDUCTORSIN LOW MAGNETIC FIELDS			DEPARTMENT OF PHYSICS,STATE UNIVERSITY OF NEW YORK AT BUFFALO,BUFFALO, NY 14260, USA	PHYSICA C,169(1990)107	L.W.SONG,Y.H.KAO	AG,Y,BA,CU,O	
1852	PHC1690107		YBa2(Cu,Ag)3O7	Y1Ba2Cu2.55Ag0.45OY	Y	1	Ba	2	Cu	2.55	Ag	0.45													O	Y			1990																												Y123																				87.6					87.6																																																		3																																												Y2O3,BACO3,CUO,AG2O	1	(920C 10H)-SIN(960C 12H IN O2)					CRITICAL CURRENT DENSITY OF AG-DOPED Y-BA-CU-O SUPERCONDUCTORSIN LOW MAGNETIC FIELDS			DEPARTMENT OF PHYSICS,STATE UNIVERSITY OF NEW YORK AT BUFFALO,BUFFALO, NY 14260, USA	PHYSICA C,169(1990)107	L.W.SONG,Y.H.KAO	AG,Y,BA,CU,O	
1853	PHC1680493		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu1O8+Y	Bi	2	Sr	2	Ca	1	Cu	1													O	8+Y			1990																												Bi2212	I4/MMM			3.814		30.52													69	77	89			17	77																																																																																														BI2O3,CUO,FE2O3,CACO3,SRCO3	0	(800C 20H IN AIR)-(875C 20H IN AIR)-Q					IRON DOPING AND MOSSBAUER SPECTROSCOPY IN BI-SR-CA-CU CERAMICSUPERCONDUCTORS			DEPARTAMENTO DE FISICA,COMISION NACIONAL DE ENERGIA ATOMICA,AVDA. LIBERTADOR 8250, 1429 BUENOS AIRES, ARGENTINA	PHUSOCA C,185(1990)493	CARLOS FAINSTEIN,CELIA SARAGOVI,PABLO ETCHEGOIN,STELLA DUHALDE	BI,SR,CA,CU	
1854	PHC1680493		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu0.995Fe0.005O8+Y	Bi	2	Sr	2	Ca	1	Cu	0.995	Fe	0.005											O	8+Y			1990																												Bi2212																			69	77	89			17	77																																																																																														BI2O3,CUO,FE2O3,CACO3,SRCO3	0	(800C 20H IN AIR)-(875C 20H IN AIR)-Q					IRON DOPING AND MOSSBAUER SPECTROSCOPY IN BI-SR-CA-CU CERAMICSUPERCONDUCTORS			DEPARTAMENTO DE FISICA,COMISION NACIONAL DE ENERGIA ATOMICA,AVDA. LIBERTADOR 8250, 1429 BUENOS AIRES, ARGENTINA	PHUSOCA C,185(1990)493	CARLOS FAINSTEIN,CELIA SARAGOVI,PABLO ETCHEGOIN,STELLA DUHALDE	BI,SR,CA,CU	
1855	PHC1680493		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu0.98Fe0.02O8+Y	Bi	2	Sr	2	Ca	1	Cu	0.98	Fe	0.02											O	8+Y			1990																												Bi2212																			54	66	79			26	66																																																																																														BI2O3,CUO,FE2O3,CACO3,SRCO3	0	(800C 20H IN AIR)-(875C 20H IN AIR)-Q					IRON DOPING AND MOSSBAUER SPECTROSCOPY IN BI-SR-CA-CU CERAMICSUPERCONDUCTORS			DEPARTAMENTO DE FISICA,COMISION NACIONAL DE ENERGIA ATOMICA,AVDA. LIBERTADOR 8250, 1429 BUENOS AIRES, ARGENTINA	PHUSOCA C,185(1990)493	CARLOS FAINSTEIN,CELIA SARAGOVI,PABLO ETCHEGOIN,STELLA DUHALDE	BI,SR,CA,CU	
1856	PHC1680493		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu0.95Fe0.05O8+Y	Bi	2	Sr	2	Ca	1	Cu	0.95	Fe	0.05											O	8+Y		1	1990																												Bi2212																			33	52	70			37	52																																																																																														BI2O3,CUO,FE2O3,CACO3,SRCO3	0	(800C 20H IN AIR)-(875C 20H IN AIR)-Q					IRON DOPING AND MOSSBAUER SPECTROSCOPY IN BI-SR-CA-CU CERAMICSUPERCONDUCTORS			DEPARTAMENTO DE FISICA,COMISION NACIONAL DE ENERGIA ATOMICA,AVDA. LIBERTADOR 8250, 1429 BUENOS AIRES, ARGENTINA	PHUSOCA C,185(1990)493	CARLOS FAINSTEIN,CELIA SARAGOVI,PABLO ETCHEGOIN,STELLA DUHALDE	BI,SR,CA,CU	
1857	PHC1690179		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1990																		GPa		147								T														-0.002	-0.002																																																																																																									0						PRESSURE-INDUCED STRUCTURAL CHANGES IN LA1.85SR0.15CUO4			MATERIAL SCIENCE DIVISION AND SCIENCE AND TECHNOLOGY CENTER FOR SUPERCONDUCTIVITY,ARGONNE NATIONAL LABORATORY, ARGONNE, IL 60439, USA	PHYSICA C,169(1990)179	B.DABROWSKI,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,P.LIGHTFOOT,SHIYOU PEI	LA,SR,CU,O	
1858	PHC1690250			Bi1.84Pb0.34Sr1.91Ca2.03Cu3OX	Bi	1.84	Pb	0.34	Sr	1.91	Ca	2.03	Cu	3											O	X		1	1990																												Bi2223																			101.4	107				6	107																															1.1																																																			2.9													1						STUDY OF UPPER CRITICAL FIELD HC2(T) IN DOPED BI-SR-CA-CU-O SUPERCONDUCTORS WITH 100 K PHASE			DEPARTMENT OF SOLID STATE PHYSICS, THE ROYAL INSTITUTE OF TECHNOLOGY, S-100 44 STOCKHOLM, SWEDEN	PHYSICA C,169(1990)250	M.NYGREN,O.RAPP,Q.CHEN,S.H.HAN,U.ANDERSSON,Y.F.YAN,Y.N.WEI,Y.S.HE,Z.HEGEDUS	BI,SR,CA,CU,O	
1859	PHC1690250			Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3OX	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	X		1	1990																												Bi2223																			102.3	109.6				6	109.6																															2.26																																																																1						STUDY OF UPPER CRITICAL FIELD HC2(T) IN DOPED BI-SR-CA-CU-O SUPERCONDUCTORS WITH 100 K PHASE			DEPARTMENT OF SOLID STATE PHYSICS, THE ROYAL INSTITUTE OF TECHNOLOGY, S-100 44 STOCKHOLM, SWEDEN	PHYSICA C,169(1990)250	M.NYGREN,O.RAPP,Q.CHEN,S.H.HAN,U.ANDERSSON,Y.F.YAN,Y.N.WEI,Y.S.HE,Z.HEGEDUS	BI,SR,CA,CU,O	
1860	PHC1690250		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.2Sr2Ca2Cu3OX	Bi	1.8	Pb	0.2	Sr	2	Ca	2	Cu	3											O	X		1	1990																												Bi2223																			99.6	107				9	107																															0.81																																																			5.3													1						STUDY OF UPPER CRITICAL FIELD HC2(T) IN DOPED BI-SR-CA-CU-O SUPERCONDUCTORS WITH 100 K PHASE			DEPARTMENT OF SOLID STATE PHYSICS, THE ROYAL INSTITUTE OF TECHNOLOGY, S-100 44 STOCKHOLM, SWEDEN	PHYSICA C,169(1990)250	M.NYGREN,O.RAPP,Q.CHEN,S.H.HAN,U.ANDERSSON,Y.F.YAN,Y.N.WEI,Y.S.HE,Z.HEGEDUS	BI,SR,CA,CU,O	
1861	PHC1690250			Bi3.7Pb0.3Sr3Ca3Cu4OX	Bi	3.7	Pb	0.3	Sr	3	Ca	3	Cu	4											O	X		1	1990																																															103.1	107				7	107																															1.1																																																			6.1													1						STUDY OF UPPER CRITICAL FIELD HC2(T) IN DOPED BI-SR-CA-CU-O SUPERCONDUCTORS WITH 100 K PHASE			DEPARTMENT OF SOLID STATE PHYSICS, THE ROYAL INSTITUTE OF TECHNOLOGY, S-100 44 STOCKHOLM, SWEDEN	PHYSICA C,169(1990)250	M.NYGREN,O.RAPP,Q.CHEN,S.H.HAN,U.ANDERSSON,Y.F.YAN,Y.N.WEI,Y.S.HE,Z.HEGEDUS	BI,SR,CA,CU,O	
1862	PHC1690294	GAP(T) AGREE WITH BCS THORY,GAP(4.2K)=2.9MEV, BYTUNNELING SAMPLE-I-SN JUNCTION	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1990																												BKBO																				18					18																																																3.75	1																																														0	BY MELT-PROCESS					ELECTRON TUNNELING IN SUPERCONDUCTING BA0.6K0.4BIO3			INSTITUTO DE INVESTIGACIONES EN MATERIALES,UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO, APARTADO POSTAL 70-360, MEXICO, D.F. 04510, MEXICO	PHYSICA C,169(1990)294	D.G.HINKS,F.MORALES,R.ESCUDERO,Y.ZHENG	BA,K,BI,O	
1863	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.97	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	Y	6.97	1	1990																											3	Y123																				39					39																																																																																									0.00000000078					BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1864	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.9	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	Y	6.9	1	1990																											3	Y123																				32.5					32.5																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1865	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.76	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	Y	6.76	1	1990																											3	Y123																																																																																																																							BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1866	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O6.97	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	Y	6.97	1	1990																											3	Y123																				14.2					14.2																																																																																									0.00000000083					BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1867	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O6.9	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	Y	6.9	1	1990																											3	Y123																																																																																																																							BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1868	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6.97	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	Y	6.97	1	1990																											3	Y123																																																																																																																		0.00000000164					BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1869	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.97	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.97	1	1990																											3	Y123																				67.6					67.6																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1870	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.9	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.9	1	1990																											3	Y123																				67.1					67.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1871	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.76	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.76	1	1990																											3	Y123																				41.1					41.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1872	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.59	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.59	1	1990																											3	Y123																				18.6					18.6																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1873	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.47	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.47	1	1990																											3	Y123																																																																																																																							BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1874	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.97	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.97	1	1990																											3	Y123																				79.1					79.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1875	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.9	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.9	1	1990																											3	Y123																				81					81																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1876	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.76	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.76	1	1990																												Y123																				61.4					61.4																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1877	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.59	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.59	1	1990																												Y123																				38.7					38.7																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1878	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.47	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.47	1	1990																												Y123																				29.8					29.8																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1879	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.85	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.85	1	1990																												Y123																				77					77																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1880	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.67	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	Y	6.67	1	1990																												Y123																				39.8					39.8																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1881	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.84	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.84	1	1990																												Y123																				60.8					60.8																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1882	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.65	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.65	1	1990																												Y123																				18.9					18.9																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1883	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.59	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.59	1	1990																												Y123																				18.9					18.9																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1884	PHC1700307		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.48	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	Y	6.48	1	1990																												Y123																																																																																																																							BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1885	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.97	Y	1	Ba	2	Cu	3															O	Y	6.97	1	1990																												Y123																				91.6					91.6																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1886	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Y	6.9	1	1990																												Y123																				94.1					94.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1887	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.76	Y	1	Ba	2	Cu	3															O	Y	6.76	1	1990																												Y123																				82					82																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1888	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.59	Y	1	Ba	2	Cu	3															O	Y	6.59	1	1990																												Y123																				61.2					61.2																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1889	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.47	Y	1	Ba	2	Cu	3															O	Y	6.47	1	1990																												Y123																				51.4					51.4																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1890	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Y	6.66	1	1990																												Y123																				68					68																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1891	PHC1700307		YBa2Cu3O7	Y1Ba2Cu3O6.33	Y	1	Ba	2	Cu	3															O	Y	6.33	1	1990																												Y123																				18.6					18.6																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1892	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.97	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.97	1	1990						2.22	-34.1																					Y123																				85					85																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1893	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.9	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.9	1	1990						2.33	-7.8																					Y123																				86.3					86.3																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1894	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.78	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.78	1	1990						2.29	15.4																					Y123																				64.6					64.6																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1895	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.6	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.6	1	1990						2.3	18.2																					Y123																				40.1					40.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1896	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.47	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.47	1	1990																												Y123																				23					23																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1897	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.7	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.7	1	1990																												Y123																				47.4					47.4																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1898	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.64	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.64	1	1990																												Y123																				43.1					43.1																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1899	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.56	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	Y	6.56	1	1990																												Y123																				37.5					37.5																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1900	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.97	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	Y	6.97	1	1990						2.36	-44.4																					Y123																				77.2					77.2																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1901	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.9	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	Y	6.9	1	1990						2.37	-12.8																					Y123																				73					73																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1902	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.78	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	Y	6.78	1	1990																												Y123																				41.3					41.3																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1903	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.6	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	Y	6.6	1	1990						2.52	-14.3																					Y123																																																																																																																							BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1904	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O6.97	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	Y	6.97	1	1990						2.42	-43.6																					Y123																				60.4					60.4																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1905	PHC1700307		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O6.9	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	Y	6.9	1	1990						2.38	-23.2																					Y123																				46					46																																																																																														BA(NO3)2,Y2O3,CUO,ZNO,NICO3.XH2O	0	CAL(900C 24H IN AIR)-SIN(960C 12H IN O2)-STEP WISE COOLING BETWEEN 800 AND 350C-ANN(5H)-Q,OXYGEN CONTROL BY ANNEALING TEMPERATURE					SUPERCONDUCTIVITY, MAGNETISM AND OXYGEN NONSTOICHIOMETRY OF BA2Y(CU1-XMX)3OY(M=ZN AND NI)			RESEARCH LABORATORY OF ENGINEERING MEATERIALS, TOKYO INSTITUTEOF TECHNOLOGY, 4259 NAGATSUTA, MIDORI-KU, YOKOHAMA 227, JAPAN	PHYSICA C,170(1990)307	HITOSHI KAWAJI,MITSURU ITOH,RUIXING LIANG,TAKAHIRO NAKAMURA,TETSURO NAKAMURA	BA,Y,CU,O,ZN,NI	
1906	PHC1700130	LEAD WIRE=IN SOLDER OR AG PASTE	Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.85Ca0.15Cu3O8+Z	Pb	2	Sr	2	Y	0.85	Ca	0.15	Cu	3											O	8+Z		1	1990																											3	Pb3212				5.403	5.442	15.773														46					46																						22									1.06							38																																												43.5				0.000000162				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1907	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.8Ca0.2Cu3O8+Z	Pb	2	Sr	2	Y	0.8	Ca	0.2	Cu	3											O	8+Z		1	1990				0																							3	Pb3212				5.4	5.435	15.786														58.9					58.9																						42									1.16							27.8																																												55.1				0.0000000687				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1908	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.75Ca0.25Cu3O8+Z	Pb	2	Sr	2	Y	0.75	Ca	0.25	Cu	3											O	8+Z		1	1990																											3	Pb3212				5.396	5.435	15.777														70.6					70.6																																																																																		49.5				0.0000000406								SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1909	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.7Ca0.3Cu3O8+Z	Pb	2	Sr	2	Y	0.7	Ca	0.3	Cu	3											O	8+Z		1	1990		-24860																									3	Pb3212				5.395	5.435	15.803														76.8					76.8																						45									0.92							27																																												11.5				0.0000000108				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1910	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.65Ca0.35Cu3O8+Z	Pb	2	Sr	2	Y	0.65	Ca	0.35	Cu	3											O	8+Z		1	1990																											3	Pb3212				5.394	5.432	15.799														79.1					79.1																						75									1.45							21																																												15.9				0.0000000167				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1911	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.6Ca0.4Cu3O8+Z	Pb	2	Sr	2	Y	0.6	Ca	0.4	Cu	3											O	8+Z		1	1990		-1062000000000000000000000000000000																									3	Pb3212				5.392	5.43	15.806														79.1					79.1																						79									1.51							20																																												12.8				0.0000000118				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1912	PHC1700130		Pb2CuSr2YCu2O8	Pb2Sr2Y1Cu3O8+Z	Pb	2	Sr	2	Y	1	Cu	3													O	8+Z		1	1990				-0.002																							3	Pb3212				5.409	5.447	15.765																																																																																																					82.9				0.00000026				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1913	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.55Ca0.45Cu3O8+Z	Pb	2	Sr	2	Y	0.55	Ca	0.45	Cu	3											O	8+Z		1	1990																											3	Pb3212				5.391	5.43	15.806														79.7					79.7																																																																																		7.98				0.0000000128				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1914	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.5Ca0.5Cu3O8+Z	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8+Z		1	1990				0																							3	Pb3212				5.388	5.428	15.808														79.7					79.7																						78									1.51							20																																												6.3				0.0000000123				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1915	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.45Ca0.55Cu3O8+Z	Pb	2	Sr	2	Y	0.45	Ca	0.55	Cu	3											O	8+Z		1	1990																											3	Pb3212				5.385	5.424	15.804														78.8					78.8																						79									1.52							20																																												26.5				0.0000000174				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1916	PHC1700130		Pb2CuSr2(Y,Ca)Cu3O8	Pb2Sr2Y0.4Ca0.6Cu3O8+Z	Pb	2	Sr	2	Y	0.4	Ca	0.6	Cu	3											O	8+Z		2	1990		-0.002																									3	Pb3212				5.396	5.434	15.836														79.1					79.1																																																																																		14.8				0.000000353				1.5				SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1917	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.3Ca0.7Cu3O8+Z	Pb	2	Sr	2	Y	0.3	Ca	0.7	Cu	3											O	8+Z		2	1990		-375300000000																									3	Pb3212				5.393	5.429	15.818														73					73																																																																																		1570												SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1918	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.2Ca0.8Cu3O8+Z	Pb	2	Sr	2	Y	0.2	Ca	0.8	Cu	3											O	8+Z		2	1990		-82170000000000000000000000																									3	Pb3212				5.392	5.425	15.8														73.2					73.2																																																																																		1066												SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1919	PHC1700130		Pb2CuSr2(Y,Ca)Cu2O8	Pb2Sr2Y0.9Ca0.1Cu3O8+Z	Pb	2	Sr	2	Y	0.9	Ca	0.1	Cu	3											O	8+Z		1	1990		-82170000000000000000000000																									3	Pb3212				5.411	5.448	15.783																																																																																																					27.7												SRCO3,Y2O3,CACO3,CUO,PBO	1	PRECURSOR SR2Y1-XCAXCU3OZ+PBO - SIN(925-955C 2H IN 1%O2+99%N2)-ANN(800-840C 12H IN 1%O2+99%N2)-Q					NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZI:DEPENDENCE ON THE CA CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,170(1990)130	HIROMU SUNAGAWA,HISASHI KAWABE,MASAHIRO MASUZAWA,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
1920	PRB0377476		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																			92.9	93.5	94.4				93.5																																																																			1.75			TP1920												1.18													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1921	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O7-Z	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																																																																																												1.65			TP1921												1.2													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1922	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-Z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																			89	90	90.8				90																																																																			2.15			TP1922												1.23																			TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1923	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																			77.2	78.4	79.6				78.4																																																																																		1.52																			TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1924	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																			61.9	64	68				64																																																																																		2.1													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1925	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7-Z	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																			46	48	57.2				48																																																																			15.2			TP1925												2.5													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1926	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-Z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																			29.2	33	38				33																																																																			18.5			TP1926												2.7													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1927	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O7-Z	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																																																																																												41.7			TP1927												5.5													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1928	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.3Pr0.7Ba2Cu3O7-Z	Y	0.3	Pr	0.7	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																																																																																																											15													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1929	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O7-Z	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																																																																																																											27													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1930	PRB0377476		(Y,Pr)Ba2Cu3O7	Y0.1Pr0.9Ba2Cu3O7-Z	Y	0.1	Pr	0.9	Ba	2	Cu	3													O	7-Z		1	1988																												Y123																																																																																												68.1			TP1930												61													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1931	PRB0377476		PrBa2Cu3O7	Pr1Ba2Cu3O7-Z	Pr	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																																																																																												120			TP1931												85.4													1						TRANSPORT PROPERTIES OF THE OXIDES Y(1-X)PR(X)BA(2)CU(3)O(7-Z)(0<-X<-1): EFFECTS OF BAND FILLING AND LATTICE DISTORTION ON SUPERCONDUCTIVITY	198805	RESISTIVITY              ,THERMOPOWER	DEPARTAMENTO DE QUIMICA,INSTITUTO DE CIENCASEE ENGENHARIA NUCLEAR-LABORATORIO NACIONAL DE ENGENHARIA E TECNOLGIA INDUSTRIAL,PORTUGAL	PHYS.REV.B,37(1988)7476	A.P.GONCALVES,E.B.LOPES,I.C.SANTOS,M.ALMEIDA,M.O.FIGUEIREDO,R.T.HENRIQUES	Y,PR,BA,CU,O	
1932	PR0426801	MUON SPIN,H=3.9KOE	(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.97	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	6.97	6.97	1	1990																											3	Y123	PMMM																			91.5					91.5																																											1500																																																				1						MAGNETIC PENETRATION DEPTH OF Y1-XPRXBA2CU3O6.97 MEASURED BY MUON-SPIN RELAXATION	199010		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.B,42(1990)6801	B.J.STERNLIEB,C.L.SEAMAN,G.M.LUKE,J.H.BREWER,J.J.NEUMEIER,L.P.LE,M.B.MAPLE,R.F.KIEFL,R.KADONO,S.R.KRIETZMAN,T.M.RISEMAN,Y.J.UEMURA	Y,PR,BA,CU,O	
1933	PR0426801	MUON SPIN,H=3.9KOE	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.97	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6.97	6.97	1	1990																											3	Y123	PMMM																			40					40																																						40					2900																																																				1						MAGNETIC PENETRATION DEPTH OF Y1-XPRXBA2CU3O6.97 MEASURED BY MUON-SPIN RELAXATION	199010		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.B,42(1990)6801	B.J.STERNLIEB,C.L.SEAMAN,G.M.LUKE,J.H.BREWER,J.J.NEUMEIER,L.P.LE,M.B.MAPLE,R.F.KIEFL,R.KADONO,S.R.KRIETZMAN,T.M.RISEMAN,Y.J.UEMURA	Y,PR,BA,CU,O	
1934	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.85Ca0.05Pr0.1Ba2Cu3O6.95	Y	0.85	Ca	0.05	Pr	0.1	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				84.6					84.6																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1935	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.8Ca0.1Pr0.1Ba2Cu3O6.95	Y	0.8	Ca	0.1	Pr	0.1	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				81.4					81.4																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1936	PRL0632516		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	1	1989																												Y123																				92.2					92.2																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1937	PRL0632516		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.95	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	6.95	6.95	1	1989																												Y123																				91.5					91.5																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1938	PRL0632516		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.95	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	6.95	6.95	1	1989																												Y123																				88.1					88.1																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1939	PRL0632516		(Y,Pr)Ba2Cu3O7	Y0.85Pr0.15Ba2Cu3O6.95	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	6.95	6.95	1	1989																												Y123																				81.6					81.6																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1940	PRL0632516		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.95	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	6.95	6.95	1	1989																												Y123																				74.6					74.6																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1941	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.83Ca0.02Pr0.15Ba2Cu3O6.95	Y	0.83	Ca	0.02	Pr	0.15	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				83					83																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1942	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.8Ca0.05Pr0.15Ba2Cu3O6.95	Y	0.8	Ca	0.05	Pr	0.15	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				82.7					82.7																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1943	PRL0632516		(Y,Pr,Pr)Ba2Cu3O7	Y0.77Ca0.08Pr0.15Ba2Cu3O6.95	Y	0.77	Ca	0.08	Pr	0.15	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				81.7					81.7																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1944	PRL0632516		(Y,Pr,Ca)Ba2Cu3O7	Y0.75Ca0.1Pr0.15Ba2Cu3O6.95	Y	0.75	Ca	0.1	Pr	0.15	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				79.6					79.6																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1945	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.7Ca0.15Pr0.15Ba2Cu3O6.95	Y	0.7	Ca	0.15	Pr	0.15	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				77.6					77.6																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1946	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.75Ca0.05Pr0.2Ba2Cu3O6.95	Y	0.75	Ca	0.05	Pr	0.2	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				76.4					76.4																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1947	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.7Ca0.1Pr0.2Ba2Cu3O6.95	Y	0.7	Ca	0.1	Pr	0.2	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				77.1					77.1																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1948	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.6Ca0.2Pr0.2Ba2Cu3O6.95	Y	0.6	Ca	0.2	Pr	0.2	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				72.9					72.9																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1949	PRL0632516		(Y,Ca,Pr)Ba2Cu3O7	Y0.65Ca0.15Pr0.2Ba2Cu3O6.95	Y	0.65	Ca	0.15	Pr	0.2	Ba	2	Cu	3											O	6.95	6.95	1	1989																												Y123																				77.1					77.1																																																																																																					HOLE FILLING AND PAIR BREAKING BY PR IONS IN YBA2CU3O6.95+-0.02	198911		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA,SAN DIEGO,LA,JOLLA,CALIFORNIA 92093	PHYS,REV.LETT.63(1989)2516	IVAN K.SCHULLER,J.J.NEUMEIER,M.B.MAPLE,T.BJw RNHOLM	Y,BA,CU,O,PR	
1950	PHC1680057		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.9Gd0.1Cu2O7	Tl	1	Ba	2	Ca	0.9	Gd	0.1	Cu	2											O	7			1990																											2	Tl1212				3.872		12.675														91.8					91.8																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1951	PHC1680057		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.8Gd0.2Cu2O7	Tl	1	Ba	2	Ca	0.8	Gd	0.2	Cu	2											O	7			1990																											2	Tl1212				3.887		12.63														93.6					93.6																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1952	PHC1680057		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.7Gd0.3Cu2O7	Tl	1	Ba	2	Ca	0.7	Gd	0.3	Cu	2											O	7			1990																											2	Tl1212																				84.5					84.5																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1953	PHC1680057		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.6Gd0.4Cu2O7	Tl	1	Ba	2	Ca	0.6	Gd	0.4	Cu	2											O	7			1990																											2	Tl1212				3.922		12.595																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1954	PHC1680057		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.2Gd0.8Cu2O7	Tl	1	Ba	2	Ca	0.2	Gd	0.8	Cu	2											O	7			1990																											2	Tl1212				3.955		12.508																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1955	PHC1680057		TlBa2GdCu2O7	Tl1Ba2Gd1Cu2O7	Tl	1	Ba	2	Gd	1	Cu	2													O	7			1990																											2	Tl1212				3.954		12.492																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1956	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.9Y0.1Cu2O7	Tl	1	Ba	2	Ca	0.9	Y	0.1	Cu	2											O	7			1990																											2	Tl1212																				86.1					86.1																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1957	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.8Y0.2Cu2O7	Tl	1	Ba	2	Ca	0.8	Y	0.2	Cu	2											O	7			1990																											2	Tl1212				3.861		12.729														97.6					97.6																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1958	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.65Y0.35Cu2O7	Tl	1	Ba	2	Ca	0.65	Y	0.35	Cu	2											O	7			1990																											2	Tl1212				3.865		12.649														102					102																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1959	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.6Y0.4Cu2O7	Tl	1	Ba	2	Ca	0.6	Y	0.4	Cu	2											O	7			1990																											2	Tl1212				3.868		12.623														95.8					95.8																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1960	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.5Y0.5Cu2O7	Tl	1	Ba	2	Ca	0.5	Y	0.5	Cu	2											O	7			1990																											2	Tl1212				3.87		12.607																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1961	PHC1680057		TlBa2(Ca,Y)Cu2O7	Tl1Ba2Ca0.2Y0.8Cu2O7	Tl	1	Ba	2	Ca	0.2	Y	0.8	Cu	2											O	7			1990																											2	Tl1212				3.902		12.492																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1962	PHC1680057		TlBa2YCu2O7	Tl1Ba2Y1Cu2O7	Tl	1	Ba	2	Y	1	Cu	2													O	7			1990																											2	Tl1212				3.91		12.466																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1963	PHC1680057		TlBa2CaCu2O7	Tl1Ba2Ca1Cu2O7	Tl	1	Ba	2	Ca	1	Cu	2													O	7			1990																											2	Tl1212				3.847		12.771														81.6					81.6																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1964	PHC1680057		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.9Nd0.1Cu2O7	Tl	1	Ba	2	Ca	0.9	Nd	0.1	Cu	2											O	7			1990																											2	Tl1212				3.868		12.729														90.8					90.8																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1965	PHC1680057		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.8Nd0.2Cu2O7	Tl	1	Ba	2	Ca	0.8	Nd	0.2	Cu	2											O	7			1990																											2	Tl1212				3.888		12.697														96.3					96.3																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1966	PHC1680057		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.7Nd0.3Cu2O7	Tl	1	Ba	2	Ca	0.7	Nd	0.3	Cu	2											O	7			1990																											2	Tl1212				3.905																95.5					95.5																																																																																														TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1967	PHC1680057		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.6Nd0.4Cu2O7	Tl	1	Ba	2	Ca	0.6	Nd	0.4	Cu	2											O	7			1990																											2	Tl1212				3.931		12.655																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1968	PHC1680057		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.2Nd0.8Cu2O7	Tl	1	Ba	2	Ca	0.2	Nd	0.8	Cu	2											O	7			1990																											2	Tl1212				3.972		12.556																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1969	PHC1680057		TlBa2NdCu2O7	Tl1Ba2Nd1Cu2O7	Tl	1	Ba	2	Nd	1	Cu	2													O	7			1990																											2	Tl1212				3.972		12.534																																																																																																																	TL2O3,BACUO2,BAO2,CAO,CUO,R2O3,Y2O3	0	PELLET WRAPPED IN AU FOIL-CAL(890C 1-3H IN O2)-SLOW COOL IN O2					SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
1970	PHC1690015		(La,Dy)2Cu(F,O)4	La1.25Dy0.75Cu1F0.5O3.75	La	1.25	Dy	0.75	Cu	1	F	0.5													O	3.75			1990																											3	T*	CMMA			5.461	5.509	12.484																																																																																																																	LA2O3,DY2O3,CUO,ZNF2	0	LOW TEMP. ANION-EXCHANGE REACTION,USING ZNF, (950C 12H)-(1050C 20H),FLUORINATION BY (LA,DY)2CUO4+ZNF2(IN GLASS TUBE)-HEAT(280C 48H IN VAC)-ANN(400C 24H)					INTERSTITIAL ANIONS IN THE T STRUCTURE			MATERIALS SCIENCE DIVISION, AND SCIENCE AND TECHNOLOGY CENTERFOR SUPERCONDUCTIVITY, ARGONNE NATIONAL LABORATORY, ARGONNE, IL 60439, USA	PHYSICA C,169(1990)15	A.MANTHIRAM,J.B.GOODENOUGH,J.D.JORGENSEN,P.LIGHTFOOT,SHINYOU PEI,X.-X.TANG		
1971	PHC1690015		(La,Dy)2CuO4	La1.25Dy0.75Cu1O4	La	1.25	Dy	0.75	Cu	1															O	4			1990																											2		P4/MMM			3.866		12.447																																																																																																																	LA2O3,DY2O3,CUO,ZNF2	0	LOW TEMP. ANION-EXCHANGE REACTION,USING ZNF, (950C 12H)-(1050C 20H),FLUORINATION BY (LA,DY)2CUO4+ZNF2(IN GLASS TUBE)-HEAT(280C 48H IN VAC)-ANN(400C 24H)					INTERSTITIAL ANIONS IN THE T STRUCTURE			MATERIALS SCIENCE DIVISION, AND SCIENCE AND TECHNOLOGY CENTERFOR SUPERCONDUCTIVITY, ARGONNE NATIONAL LABORATORY, ARGONNE, IL 60439, USA	PHYSICA C,169(1990)15	A.MANTHIRAM,J.B.GOODENOUGH,J.D.JORGENSEN,P.LIGHTFOOT,SHINYOU PEI,X.-X.TANG		
1972	TH1220431		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	9-Z	6.8	1	1987									6.35																		3	Y123				3.82	3.886	11.66													85	89.5				4.2	89.5																																																																	TC1972																	0.74																			THERMAL CONDUCTIVITY AND ELECTRICAL RESISTIVITY OF THE HIGH-TC SUPERCONDUCTOR Y(1)BA(2)CU(3)O(9-Z)	198706	RESISTIVITY              ,THERMAL CONDUC	INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCE,POLAND	PHYS.REV.A,122(1987)431	A.J.ZALESKI,A.JEZOWSKI,C.SULKOWSKI,E.TROJNAR,J.KLAMUT,J.MUCHA,J.RAFALOWICZ,J.STEPIEN-DAMM,K.ROGACKI,M.HOROBIOWSKI,R.HORYN,Z.BUKOWSKI	Y,BA,CU,O	
1973	PHC1700071		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7-Z	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7-Z		1	1990																											3	Y123				3.826	3.888	11.668														82.7					82.7																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1974	PHC1700071		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O7-Z	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	7-Z		1	1990																											3	Y123				3.827	3.887	11.668														74.6					74.6																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1975	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.97Fe0.03O7-Z	Gd	1	Ba	2	Cu	2.97	Fe	0.03													O	7-Z		1	1990																												Y123																				88.2					88.2																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1976	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.94Fe0.06O7-Z	Gd	1	Ba	2	Cu	2.94	Fe	0.06													O	7-Z		1	1990																												Y123																				85					85																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1977	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.82Fe0.18O7-Z	Gd	1	Ba	2	Cu	2.82	Fe	0.18													O	7-Z		1	1990																												Y123																				55.2					55.2																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1978	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.76Fe0.24O7-Z	Gd	1	Ba	2	Cu	2.76	Fe	0.24													O	7-Z		1	1990																												Y123																				40.6					40.6																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1979	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.73Fe0.27O7-Z	Gd	1	Ba	2	Cu	2.73	Fe	0.27													O	7-Z		1	1990																												Y123																				36.4					36.4																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1980	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.67Fe0.33O7-Z	Gd	1	Ba	2	Cu	2.67	Fe	0.33													O	7-Z		1	1990																												Y123																				11.8					11.8																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1981	PHC1700071		GDBA2(CU,FE)3O7	Gd1Ba2Cu2.64Fe0.36O7-Z	Gd	1	Ba	2	Cu	2.64	Fe	0.36													O	7-Z		1	1990																												Y123																				18.6					18.6																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1982	PHC1700071	GAMMA FROM SUSCEPTIBILITY	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	1	1990																											3	Y123																				92					92																															2.7							11.5					890														97																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1983	PHC1700071	GAMMA FROM SUSCEPTIBILITY	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.955Fe0.045O6.93	Y	1	Ba	2	Cu	2.955	Fe	0.045													O	7-Z	6.93	1	1990																											3	Y123																				91.4					91.4																															2							13.4					731														107																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1984	PHC1700071	GAMMAFROM SUSCEPTIBILITY	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.835Fe0.165O6.98	Y	1	Ba	2	Cu	2.835	Fe	0.165													O	7-Z	6.98	1	1990																											2	Y123				3.864		11.676														69.3					69.3																															0.5							30.7					334														169																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1985	PHC1700071	GAMMA FROM SUSCEPTIBILITY	YBAa(Cu,Fe)3O7	Y1Ba2Cu2.745Fe0.255O7.08	Y	1	Ba	2	Cu	2.745	Fe	0.255													O	7-Z	7.08	1	1990																											2	Y123																				53					53																															0.25							49.7					230														233																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1986	PHC1700071	GAMMA FROM SUSCEPTIBILITY	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.64Fe0.36O7.12	Y	1	Ba	2	Cu	2.64	Fe	0.36													O	7-Z	7.12	1	1990																											2	Y123																				32					32																																						71					228														312																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1987	PHC1700071	GAMMA FROM SUSCEPTIBILITY	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.52Fe0.48O7.08	Y	1	Ba	2	Cu	2.52	Fe	0.48													O	7-Z	7.08		1990																											2	Y123																																																																																		337																																					Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1988	PHC1700071		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.58Fe0.42O7-Z	Y	1	Ba	2	Cu	2.58	Fe	0.42													O	7-Z		1	1990																											2	Y123				3.865		11.627														24.7					24.7																																																																																														Y2O3,GD2O3,BACO3,CUO,FE2O3,NIO	0	SIN(960C IN O2)-FC(1.4C/MIN) IN O2)					ASPECTS OF SUBSTITUTION OF MAGNETIC IONS FE, NI AND GD IN YBCOHTSC			INSTITUT FUR METALLPHYSIK,HOSPITALSTRASSE 3-7, 3400 GOTTINGEN,FRG	PHYSICA C,179(1990)71	B.ULLMANN,H.C.FREYHARDT,K.HEINEMANN,R.WORDENWEBER	FE,NI,GD,Y,BA,CU,O	
1989	PRB0397347		DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.846	3.873	27.237														77.2					77.2																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1990	PR0394316			Bi4Sr4Pr2Cu4OZ	Bi	4	Sr	4	Pr	2	Cu	4													O	Z			1989																											2																																																																																																																															Bismuth cuprate high-Tc superconductors using cationic substitution	3		Bellcore, Red Bank, New Jersey 07701	Phys.Rev.B,39(1989)4316	G.W. Hull,J.-M. Tarascon,L.H. Green,M. Giroud,M.S. Hegde,P. Barboux,R. Ramesh,W.R. McKinnon		
1991	PRB0397347		ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.837	3.869	27.23														78.3					78.3																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1992	PRB0397347		TmBa2Cu4O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.827	3.864	27.18														78.6					78.6																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1993	PRB0397347		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.84	3.87	27.231														80.4					80.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1994	PRB0397347	Y123(70%),Y124(30%)	SmBa2Cu4O8	Sm1Ba2Cu4O8	Sm	1	Ba	2	Cu	4															O	8		2	1989																											3	Y124				3.872	3.886	27.308														69.3					69.3																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1995	PRB0397347	Y124(60%),Y247(40%)	EuBa2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		2	1989																											3	Y124				3.865	3.884	27.279														68.9					68.9																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1996	PRB0397347	Y124(40%),Y247(60%)	GdBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8		2	1989																											3	Y124				3.863	3.881	27.259														73.4					73.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
1997	PHC1680047	CUO CLUSTER(<1%VOLUME)	YBa2Cu4O8	Y1Ba2Cu4O8.045	Y	1	Ba	2	Cu	4															O	8	8.045		1990									5.74																			Y124				3.84	3.869	27.23														81.4					81.4										55																																															4.9		350																																				0						SPECIFIC HEAT OF THE SUPERCONDUCTOR YBA2CU4O8FROM 1.5 TO 330 K			DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITE DEGENEVE, CH-1211 GENEVE 4, SWIZERLAND	PHYSICA C,168(1990)47	A.JUNOD,D.ECKERT,D.SANCHEZ,E.KALDIS,G.TRISCONE,J.KARPINSKI,J.MULLER,S.RUSIECKI,T.GRAF	Y,BA,CU,O	
1998	PHC1680047		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1990																												Y124				3.837	3.87	27.216														79.7					79.7										31																																															13		260																																				0						SPECIFIC HEAT OF THE SUPERCONDUCTOR YBA2CU4O8FROM 1.5 TO 330 K			DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITE DEGENEVE, CH-1211 GENEVE 4, SWIZERLAND	PHYSICA C,168(1990)47	A.JUNOD,D.ECKERT,D.SANCHEZ,E.KALDIS,G.TRISCONE,J.KARPINSKI,J.MULLER,S.RUSIECKI,T.GRAF	Y,BA,CU,O	
1999	PHC1680047		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1990																												Y124				3.843	3.872	27.237														80.6					80.6										14																																															15		200																																				0						SPECIFIC HEAT OF THE SUPERCONDUCTOR YBA2CU4O8FROM 1.5 TO 330 K			DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITE DEGENEVE, CH-1211 GENEVE 4, SWIZERLAND	PHYSICA C,168(1990)47	A.JUNOD,D.ECKERT,D.SANCHEZ,E.KALDIS,G.TRISCONE,J.KARPINSKI,J.MULLER,S.RUSIECKI,T.GRAF	Y,BA,CU,O	
2000	PRB0397347		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1989																												Y124				3.84	3.87	27.221														77.4					77.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2001	PHC1700112	TP IS NOT INFLUENCED BY THE POROCITY,RH DEPENDS ON THE POROC	ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		1	1990									3.3																		3	Y124				3.836	3.867	27.22													73	78				5	78																																																																			7.52			TP2001																			0.0000000004												NORMAL-STATE TRANSPORT PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ERBA2CU4O8			LABORATORY OF INORGANIC CHEMISTRY, UNIVERSITY OF GRONINGEN, NIJENBORGH 216, 9747 GRONINGEN, THE NETHERLANDS	PHYUSICA C,170(1990)112	C.F.VAN BRUGGEN,D.M.DE LEEUW,H.J.TERPSTRA,M.KRAAN,R.A.M.VAN WOERDEN	ER,BA,CU,O	
2002	PHC1700112	TP IS NOT INFLUENCED BY THE POROCITY,RH DEPENDS ON POROCITY	ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		1	1990									5.1																		3	Y124				3.838	3.871	27.25																																																																																									RH2001																					RH2002										NORMAL-STATE TRANSPORT PROPERTIES OF THE HIGH-TC SUPERCONDUCTOR ERBA2CU4O8			LABORATORY OF INORGANIC CHEMISTRY, UNIVERSITY OF GRONINGEN, NIJENBORGH 216, 9747 GRONINGEN, THE NETHERLANDS	PHYUSICA C,170(1990)112	C.F.VAN BRUGGEN,D.M.DE LEEUW,H.J.TERPSTRA,M.KRAAN,R.A.M.VAN WOERDEN	ER,BA,CU,O	
2003	PHC1650391	T(SUS)=77.0	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990																											3	Y124				3.835	3.856	27.215														82.9					82.9																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2004	PHC1650391	T(SUS)=80.4,TC PROPORTINAL TO LATC	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.981Ba1.994Ca0.025Cu4O8	Y	0.981	Ba	1.994	Ca	0.025	Cu	4													O	8		1	1990																											3	Y124						27.233														87.1					87.1																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2005	PHC1650391	T(SUS)=83.9	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.962Ba1.987Ca0.05Cu4O8	Y	0.962	Ba	1.987	Ca	0.05	Cu	4													O	8		1	1990																											3	Y124						27.248														91.5					91.5																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2006	PHC1650391	T(SUS)=86.2	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.925Ba1.975Ca0.1Cu4O8	Y	0.925	Ba	1.975	Ca	0.1	Cu	4													O	8		2	1990																											3	Y124						27.261														92.3					92.3																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2007	PHC1650391	T(SUS)=82.8	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.887Ba1.962Ca0.15Cu4O8	Y	0.887	Ba	1.962	Ca	0.15	Cu	4													O	8		2	1990																											3	Y124																				91.8					91.8																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2008	PHC1650391	T(SUS)=83.2	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.85Ba1.95Ca0.2Cu4O8	Y	0.85	Ba	1.95	Ca	0.2	Cu	4													O	8		2	1990																											3	Y124						27.262														91.6					91.6																																																																																																					CALCIUM-SUBSTITUTED SUPERCONDUCTING RBA2CU4O8 WITH TC-90K PREPARED AT ONE ATMOSPHERE			PHYSICS AND ENGINEERING LABORATORY, DSIR, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYSICA C,165(1990)391	D.M.POOKE,J.L.TALLON,M.R.PORESLAND,R.G.BUCKLEY	Y,ER,CU,O,BA	
2009	SSC0690531		YBa2Cu4O8	Y1Ba2Cu4O8.043	Y	1	Ba	2	Cu	4															O	8	8.043	1	1989																											3	Y124	AMMM			3.841	3.871	27.24														80					80																																																																																															0	400 BAR O2,1040C,IMPURITY YCUO2 OR Y2BACUO5					HIGHPRESSURE PREPARATION AND NEUTRON-DIFFRACTION STUDY OF THE HIGH Tc SUPERCONDUCTOR YBa2Cu4O8+-x			"Laboratorium fu""r Festko""rperphysik ETH, CH-8093 Zu""rich"	Solid State Commun.,69(1989)531-533	E. Jilek,E. Kaldis,J. Karpinski,P. Fischer,S. Rusiecki		
2010	SSC0750315	SWEEP RATE=10MOE/SEC,DEMAG.FACTOR(N=0.8,L=0.179,M=0.022)	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1990																												Y124																				74					74														44	197																																																																																						DETERMINATION OF HC1(T) ON A Y2BA4CU8O16 SINGLE CRYSTAL		MAGNETIZATION       ,HC1                 ,SINGLE CRYSTAL	CENTRE DE RECHERCHES SUR LES TRES BASSES TEMPERATURES, C.N.R.S., BP 166 X, 38042	SOLID STATE COMMUN.,75(1990)315	E.KALDIS,J.C.MARTINEZ,J.J.PREJEAN,J.KARPINSKI,P.BORDET	Y,BA,CU,O	
2011	PHC1670335	(dL/dP) shows (1/L)*(dL/dP). B(30K)=122GPA,SEE PHC1590668	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1990																		GPa		112								Y124														0.003	0.001	0.004				80					80																																																																																																					X-RAY INVESTIGATIONS OF Y1BA2CU4O8 UNDER HIGH PRESSURE			UNIVERSITAT KARLSRUHE UND KERNFORSCHUNGSZENTRUM KARLSRUHE, INSTITUTE FUR TECHNISCHE PHYSIK, D-7500 KARLSRUHE, FRG	PHYSICA C,167(1990)335	E.KALDIS,H.A.LUDWIG,H.WUHL,J.KARPINSKI,M.R.DIETRICH,S.RUSIECKI,W.H.FIETZ	Y,BA,CU,O	
2012	PHC1700521	DTCDP=K/GPA. Tc defined as midpoint value in resistive transition,?@POROCITY=1.5	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990																												Y124																				75					75			K/GPa	7.5																																														900																																0.63																			ELECTRICAL TRANSPORT PROPERTIES OF DENSE BULK YBA2CU4O8 PRODUCED BY HOT ISOSTATIC PRESSING			DEPARTMENT OF PHYSICS, UMEA UNIVERSITY, S-90187 UMEA, SWEDEN	PHYSICA C,170(1990)521	B.LOBERG,B.M.ANDERSSON,B.SUNDQVIST,J.NISKA,K.EASTERLING	Y,BA,CU,O	
2013	PRB03811337		La2CuO4	La2Cu1O4.13	La	2	Cu	1																	O	4.13	4.13	1	1988																											3	T	FMMM			3.772	3.816	13.165														34					34										30																																																																																											SUPERCONDUCTING PHASE OF LA(2)CU(1)O(4+Z): A SUPERCONDUCTING COMPOSITION RESULTING FROM PHASE SEPARATION	198812	NEUTRON DIFFRACTION      ,OXYGEN CONTENT           ,TWQ PHAS	MATERIALS SCIENCE AND CHEMISTRY DIVISIONS,ARGONNE NATIONAL LABORATORY,ILLINOIS	PHYS.REV.B,38(1988)11337	B.DABROWSKI,B.MOROSIN,D.G.HINKS,D.S.GINLEY,E.L.VENTURINI,J.D.JORGENSEN,J.E.SCHIRBER,L.SODERHOLM,SHIYOU PEI	LA,CU,O	
2014	PRB03811337		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4.0	4	1	1988																											3	T	BMAB			3.772	3.833	13.107																																																																																																																								SUPERCONDUCTING PHASE OF LA(2)CU(1)O(4+Z): A SUPERCONDUCTING COMPOSITION RESULTING FROM PHASE SEPARATION	198812	NEUTRON DIFFRACTION      ,OXYGEN CONTENT           ,TWQ PHAS	MATERIALS SCIENCE AND CHEMISTRY DIVISIONS,ARGONNE NATIONAL LABORATORY,ILLINOIS	PHYS.REV.B,38(1988)11337	B.DABROWSKI,B.MOROSIN,D.G.HINKS,D.S.GINLEY,E.L.VENTURINI,J.D.JORGENSEN,J.E.SCHIRBER,L.SODERHOLM,SHIYOU PEI	LA,CU,O	
2015	PHC1580183	EXCESS OXYGEN OCCUPY AN INTERSTITIAL SITE	La2CuO4	La2Cu1O4.32	La	2	Cu	1																	O	4.32	4.32	3	1989																											3	T	CMCA			3.79	3.813	13.181															37.5				37.5										70																																																																																											THE CRYSTAL STRUCTURE OF SUPERCONDUCTING LA(2)CUO(4.032) BY NEUTRON DIFFRACTION	198904	CRYSTAL STRUCTURE   ,NEUTRON-DIFFRECTION	LABORATOIRE DE CRISTALLOGRAPHIE,CNRS,ASSOCIE A UNIVERSITE J.FOURIER,166X,38042 GRENOBLEN CEDEX,FRANCE	PHYSICA C ,158(1989)183	B.MOROSIN,C.CHAILLOUT,J.E.SCHIRBER,M.MAREZIO,M.S.LEHMANN,S.W.CHEONG,Z.FISK	LA,CU,O	
2016	SSC0750897		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Y	Nd	1.85	Ce	0.15	Cu	1															O	4-Y		1	1990																												T'																			24						24																																																																																											RH2016										RESISTIVITY, HALL CONSTANT AND MASNETISATION OF ND1.85CE0.15CUO4-Y		PREPARATION         ,HALL CONSTANT       ,MAGNETISATION	LABORATOIRE DE PHYSIQUE DES SOLIDES DE BELLEVUE, CNRS, 92195 MEUDON FRANCE.	SOLID STATE COMMUN.,75(1990)897	C.QUITMANN,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN,U.EBELS	ND,CE,CU,O	
2017	SSC0750779		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.4Pb0.5Sb0.1Sr2Ca2Cu3O10-X	Bi	1.4	Pb	0.5	Sb	0.1	Sr	2	Ca	2	Cu	3									O	10-X		1	1990																																																106.9					106.9																																																																																																					THERMAL CONDUCTIVITY OF BI-BASED HIGH-TC SUPERCONDUCTORS IN THE VICINITY OF SUPERCONDUCTING TRANSITION		THERMAL CONDUCTIVITY	INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCE,OKOLNA 2,50-422 WROCLAW, P.O. BOX 937, POLAND	SOLID STATE COMMUN.,75(1990)779	A.JEZOWSKI	BI,PB,SB,SR,CA,CU,O	
2018	SSC0750753	PENET FROM NMR MEASUREMENT	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1990																												Tl2201																				85					85																																											1800																																																										MAGNETIC FIELD DISTRIBUTION OF THE VORTEX LATTICE IN THE SUPERCONDUCTOR TL2BA2CUO6 (TC=85K): 205TL NMR INVESTIGATION		NMR                 ,PENETRATION DEPTH	2. PHYSIKALISCHES INSTITUT, UNIVERSITAT STUTTGART, D-7000 STUTTGART 80, FEDERAL REPUBLIC OF GERMANY	SOLID STATE COMMUN.,75(1990)753	A.SIMON,F.HENTSCH,HJ.MATTAUSCH,M.MEHRING	TL,BA,CU,O	
2019	SSC0750617		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sb0.1Sr2Ca2Cu2OZ	Bi	1.6	Pb	0.4	Sb	0.1	Sr	2	Ca	2	Cu	2									O	Z			1990																												Bi2223																			132		140				136																																																																																																					THE EFFECT OF CONSTITUENT CONTENT ON SUPERCONDUCTIVITY AND PHASE IN BI-PB-SB-SR-CA-CU-O SYSTEM			DEPARTMENT OF APPLIED CHEMISTRY, DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE & TECHNOLOGY OF CHINA, HEFEI, ANHUI,P.R.CHINA)	SOLID STATE COMMUN.,75(1990)617	CAO LIEZHAO,CHEN ZHAOJIA,CHEN ZUYAO,LIN RONG,MAO XINGLEI,QIAN YITAI,ZHANG YUHENG,ZHOU LING	BI,PB,SB,SR,CA,CU,O	
2020	SSC0750617		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sb0.1Sr2Ca2Cu2OZ	Bi	1.6	Pb	0.4	Sb	0.1	Sr	2	Ca	2	Cu	2									O	Z			1990																																															130		134.5				132.25																																																																																																					THE EFFECT OF CONSTITUENT CONTENT ON SUPERCONDUCTIVITY AND PHASE IN BI-PB-SB-SR-CA-CU-O SYSTEM			DEPARTMENT OF APPLIED CHEMISTRY, DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE & TECHNOLOGY OF CHINA, HEFEI, ANHUI,P.R.CHINA)	SOLID STATE COMMUN.,75(1990)617	CAO LIEZHAO,CHEN ZHAOJIA,CHEN ZUYAO,LIN RONG,MAO XINGLEI,QIAN YITAI,ZHANG YUHENG,ZHOU LING	BI,PB,SB,SR,CA,CU,O	
2021	SSC0750617		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.8Pb0.2Sb0.1Sr2Ca2Cu2OZ	Bi	1.8	Pb	0.2	Sb	0.1	Sr	2	Ca	2	Cu	2									O	Z			1990																																															130		142				136																																																																																																					THE EFFECT OF CONSTITUENT CONTENT ON SUPERCONDUCTIVITY AND PHASE IN BI-PB-SB-SR-CA-CU-O SYSTEM			DEPARTMENT OF APPLIED CHEMISTRY, DEPARTMENT OF PHYSICS, UNIVERSITY OF SCIENCE & TECHNOLOGY OF CHINA, HEFEI, ANHUI,P.R.CHINA)	SOLID STATE COMMUN.,75(1990)617	CAO LIEZHAO,CHEN ZHAOJIA,CHEN ZUYAO,LIN RONG,MAO XINGLEI,QIAN YITAI,ZHANG YUHENG,ZHOU LING	BI,PB,SB,SR,CA,CU,O	
2022	SSC0750579		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1990									4.4																		3	Y123																				91.7					91.7													460																																																																																								LOW MAGNETIC FIELD DEPENDENCE OF A.C. SUSCEPTIBILITY IN SUPERCONDUCTING YBA2CU3O7-Z		SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, UNIVERSITY OF WISCONSIN-MILWAUKEE, MILWAUKEE, WI 53201, U.S.A	SOLID STATE COMMUN.,75(1990)579	AHMAD KOMPANY,H-P.BAUM,M-F.XU,M.LEVY,W.MILLMAN,Y.J.QIAN	Y,BA,CU,O	
2023	SSC0750981	NEELT FROM MOSSBAUER	(Pr,Gd)Ba2Cu3O7	Gd0.075Pr0.925Ba2Cu3O6.9	Gd	0.075	Pr	0.925	Ba	2	Cu	3													O	7-Z	6.9	1	1990								16.5																			3	Y123				3.874	3.912	11.74																																																																																																																								MAGNETIC ORDER OF THE PR SUBLATTICE IN TETRAGONAL AND ORTHORHOMBIC PR1-XGDXBA2CU3O7-Z OBSERVBED BY 155GD-MOSSBAUER SPECTROSCOPY		MOSSBAUER           ,MAGNETIC ORDER	INSTITUT FUR EXPERIMENTALPHYSIK, FREIE UNIVERSITAT BERLIN, D-1000 BERLIN 33, GERMANY	SOLID STATE COMMUN.,75(1990)981	G.WORTMANN,I.FELNER	PR,GD,BA,CU,O	
2024	SSC0750981	NEELT FROM MOSSBAUER	(Pr,Gd)Ba2Cu3O7	Gd0.075Pr0.925Ba2Cu3O6.1	Gd	0.075	Pr	0.925	Ba	2	Cu	3													O	7-Z	6.1	1	1990								7.5																			2	Y123				3.909		11.84																																																																																																																								MAGNETIC ORDER OF THE PR SUBLATTICE IN TETRAGONAL AND ORTHORHOMBIC PR1-XGDXBA2CU3O7-Z OBSERVBED BY 155GD-MOSSBAUER SPECTROSCOPY		MOSSBAUER           ,MAGNETIC ORDER	INSTITUT FUR EXPERIMENTALPHYSIK, FREIE UNIVERSITAT BERLIN, D-1000 BERLIN 33, GERMANY	SOLID STATE COMMUN.,75(1990)981	G.WORTMANN,I.FELNER	PR,GD,BA,CU,O	
2025	SSC0750987		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-Z			1990																												Y123				3.835	3.874	11.621														42.8					42.8																																																																																																					SIMULTANEOUS DOPING AT THE CHAIN- AND PLANE-SITES OF CU IN YBA2CU3O7-Y			TATA INSITITUTE OF FUNDAMENTAL RESEARCH, BOMBAY-400 005, INDIA	SOLID STATE COMMUN.,75(1990)987	A.K.RAJARAJAN,K.PATNAIK,L.C.GUPTA,N.C.MISHRA,R.VIJAYARAGHAVAN	Y,BA,CU,O,ZN,GA	
2026	SSC0750987		YBa2(Cu,Zn,Ga)3O7	Y1Ba2Cu2.85Zn0.114Ga0.036O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.114	Ga	0.036											O	7-Z			1990																												Y123				3.842	3.874	11.62														40.2					40.2																																																																																																					SIMULTANEOUS DOPING AT THE CHAIN- AND PLANE-SITES OF CU IN YBA2CU3O7-Y			TATA INSITITUTE OF FUNDAMENTAL RESEARCH, BOMBAY-400 005, INDIA	SOLID STATE COMMUN.,75(1990)987	A.K.RAJARAJAN,K.PATNAIK,L.C.GUPTA,N.C.MISHRA,R.VIJAYARAGHAVAN	Y,BA,CU,O,ZN,GA	
2027	SSC0750987		YBa2(Cu,Zn,Ga)3O7	Y1Ba2Cu2.85Zn0.075Ga0.075O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.075	Ga	0.075											O	7-Z			1990																												Y123				3.853	3.874	11.623														42.3					42.3																																																																																																					SIMULTANEOUS DOPING AT THE CHAIN- AND PLANE-SITES OF CU IN YBA2CU3O7-Y			TATA INSITITUTE OF FUNDAMENTAL RESEARCH, BOMBAY-400 005, INDIA	SOLID STATE COMMUN.,75(1990)987	A.K.RAJARAJAN,K.PATNAIK,L.C.GUPTA,N.C.MISHRA,R.VIJAYARAGHAVAN	Y,BA,CU,O,ZN,GA	
2028	SSC0750987		YBa2(Cu,Zn,Ga)3O7	Y1Ba2Cu2.85Zn0.036Ga0.114O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.036	Ga	0.114											O	7-Z			1990																												Y123				3.85	3.869	11.614														55.1					55.1																																																																																																					SIMULTANEOUS DOPING AT THE CHAIN- AND PLANE-SITES OF CU IN YBA2CU3O7-Y			TATA INSITITUTE OF FUNDAMENTAL RESEARCH, BOMBAY-400 005, INDIA	SOLID STATE COMMUN.,75(1990)987	A.K.RAJARAJAN,K.PATNAIK,L.C.GUPTA,N.C.MISHRA,R.VIJAYARAGHAVAN	Y,BA,CU,O,ZN,GA	
2029	SSC0750987		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7-Z	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-Z			1990																												Y123				3.855	3.876	11.633														75.2					75.2																																																																																																					SIMULTANEOUS DOPING AT THE CHAIN- AND PLANE-SITES OF CU IN YBA2CU3O7-Y			TATA INSITITUTE OF FUNDAMENTAL RESEARCH, BOMBAY-400 005, INDIA	SOLID STATE COMMUN.,75(1990)987	A.K.RAJARAJAN,K.PATNAIK,L.C.GUPTA,N.C.MISHRA,R.VIJAYARAGHAVAN	Y,BA,CU,O,ZN,GA	
2030	PRB0357129	MUON SPIN RESONANCE,ANOMOLOUS TEMP DEPENDENCE	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				37					37													150																														2500																																																										MAGNETIC PENETRATION DEPTH AND FLUX-PINNING EFFECT IN HIGH-TC SUPERCONDUCTOR LA(1.85)SR(0.15)CU(1)O(4)	198705	MUON                     ,PENETRATION DEPTH        ,CARRIER DENSITY          ,FL	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,35(1987)7129	D.R.NOAKES,E.J.ANSALDO,G.AEPPLI,G.M.LUKE,J.H.BREWER,R.F.KIEFL,R.J.CAVA,S.R.KREITZMAN	LA,SR,CU,O	
2031	PRB0357133	MUON SPIN RESONANCE	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				37					37																																											2000																																																										MAGNETIC FIELD PENETRATION DEPTH OF LA(1.85)SR(0.15)CU(1)O(4)MEASURED BY MUON SPIN RELAXATION	198705	MUON                     ,PENETRATION DEPTH        ,CARRIER	PHYSICS DEPARTMENT,COLLEGE OF WILLIAM AND MARY,WILLIAMSBURG,VIRGINIA	PHYS.REV.B,35(1987)7133	A.R.MOODENBAUGH,C.E.STRONACH,H.E.SCHONE,J.R.KEMPTON,M.SUENAGA,W.J.KOSSLER,X.H.YU,Y.J.UEMURA	LA,SR,CU,O	
2032	JJP0260443		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1987		0																										T																			38	39	40			1	39																						50									1.8							20					1000																																			0.3				1.8																			SUPERCONDUCTING PROPERTIES OF (LA(1-X)SR(X))(2)CU(1)O(4)	198704		DEPARTMENT OF APPLIED PHYSICS,UNIVERSITY OF TOKYO,TOKYO	JJAP.LETT.,26(1987)L443	HIDENORI TAKAGI,KAZUO FUEKI,KOHJI KISHIO,KOICHI KITAZAWA,SHIN-ICHI UCHIDA,SHOJI TANAKA	LA,SR,CU,O	
2033	LES1640824	5X5X0.15MM3,HALL=H//C-AXIS	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1990																												T'																				22.9				0.4	22.9																																																																																		0.55							-0.0000000048		RH2033										CRYSTAL GROWTH AND PHYSICAL PROPERTIES OF ND2-XCEXCUO4-Y SINGLE CRYSTALS.		SINGLE CRYSTALS     ,RESISTIVITY         ,HALL COEFFICIENT	DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE	LESS-COMM.METALS,164(1990)824	E.KOLLER,E.WALKER,M.AFFRONTE,M.FRANCOIS,W.SADOWSKI	ND,CE,CU,O	
2034	LES1640824	X DEPEND. OF TC IN FIGURE	(Nd,Ce)2CuO4	Nd1.847Ce0.153Cu1O4	Nd	1.847	Ce	0.153	Cu	1															O	4		3	1990																																														K		22.5					22.5	TC2034																																																																																																				CRYSTAL GROWTH AND PHYSICAL PROPERTIES OF ND2-XCEXCUO4-Y SINGLE CRYSTALS.		SINGLE CRYSTALS     ,RESISTIVITY         ,HALL COEFFICIENT	DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE	LESS-COMM.METALS,164(1990)824	E.KOLLER,E.WALKER,M.AFFRONTE,M.FRANCOIS,W.SADOWSKI	ND,CE,CU,O	
2035	LES1640808			Pb2.04Sr2.07Y0.61Ca0.38Cu3O8	Pb	2.04	Sr	2.07	Y	0.61	Ca	0.38	Cu	3											O	8		3	1990																											3					5.383	5.413	15.79														65					65																																																																																																					PREPARATION AND CHARACTERIZATION OF 80 K SUPERCONDUCTING PB2SR2Y1-XCAXCU3O8+Z SINGLE CRYSTALS		PREPARATION         ,SINGLE CRYSTALS	LABORATOIRE DE CRISTALLOGRAPHIE, CNRS-UJF, 166X, 38042 GRENOBLE CEDEX, FRANCE	LESS-COMM.METALS,164(1990)808	J.J.CAPPONI,J.L.THOLENCE,M.F.GORIUS,M.MAREZIO,O.CHMAISSEM,S.KORCZAK,T.FOURNIER	PB,SR,Y,CA,CU,O	
2036	LES1640808	SEE PHC162-164(1989)53		Pb2Sr2Y0.5Ca0.5Cu3O9.4	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	9.4	9.4	3	1990																											3	Pb3212				3.84	3.87	15.89																	4.2																																																																																																							PREPARATION AND CHARACTERIZATION OF 80 K SUPERCONDUCTING PB2SR2Y1-XCAXCU3O8+Z SINGLE CRYSTALS		PREPARATION         ,SINGLE CRYSTALS	LABORATOIRE DE CRISTALLOGRAPHIE, CNRS-UJF, 166X, 38042 GRENOBLE CEDEX, FRANCE	LESS-COMM.METALS,164(1990)808	J.J.CAPPONI,J.L.THOLENCE,M.F.GORIUS,M.MAREZIO,O.CHMAISSEM,S.KORCZAK,T.FOURNIER	PB,SR,Y,CA,CU,O	
2037	LES1640884	METALLIC,DEFORMRD PEROVSKITE	(Sr,La)2TiO4	Sr1.78La0.22Ti1O4	Sr	1.78	La	0.22	Ti	1															O	4			1990																																																			4.2																																																																																																							SEARCH OF SUPERCONDUCTIVITY IN TERNARY OXIDES BASED ON D1IONS			CERN, 1211 GENEVE 23, SWITZERLAND	LESS-COMM.METALS,164(1990)884	CRISTOFORO BENVENUTI,REMI CHIPAUX	K,RB,CS,CA,SR,BA,LA,CU,O	
2038	LES1640884	SEMICONDUCTOR LIKE	(Sr,La)2TiO4	Sr1.89La0.19Ti1O4	Sr	1.89	La	0.19	Ti	1															O	4			1990																																																			4.2																																																																																																							SEARCH OF SUPERCONDUCTIVITY IN TERNARY OXIDES BASED ON D1IONS			CERN, 1211 GENEVE 23, SWITZERLAND	LESS-COMM.METALS,164(1990)884	CRISTOFORO BENVENUTI,REMI CHIPAUX	K,RB,CS,CA,SR,BA,LA,CU,O	
2039	SSC0730291		La2Sr6Cu8O18	La2Sr6Cu8O17.56	La	2	Sr	6	Cu	8															O	18-Z	17.56		1989	emu/mol	0.000736	emu.K/mol	0.0376			2.23																				2				A	3.764		10.861																	4																																																																																																							PROPERTIES OF A NEW COPPER TERNARY COMPOUND LA2SR6CU8O18-Z		STRUCFTURE          ,TED                 ,XRY                 ,OXYGEN CONTENT      ,SUSCEPTIBILITY	KAMERLINGH ONNES LABORATORY AND CORLAEUS LABORATORIES, LEIDENUNIVERSITY P.O. BOC 9506, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN,73(1989)291	A.A.VERHEIJEN,H.W.ZANDBERGEN,J.M.VAN RUITENBEEK,L.J.DE JONGH,Q.XU,W.T.FU	LA,SR,CU,O	
2040	SSC0730291		La2Sr6Cu8O18	La2Sr6Cu8O16.02	La	2	Sr	6	Cu	8															O	18-Z	16.02		1989	emu/mol	0.000388		0.0512			3.11																				2				A	3.652		11.055																	4																																																																																																							PROPERTIES OF A NEW COPPER TERNARY COMPOUND LA2SR6CU8O18-Z		STRUCFTURE          ,TED                 ,XRY                 ,OXYGEN CONTENT      ,SUSCEPTIBILITY	KAMERLINGH ONNES LABORATORY AND CORLAEUS LABORATORIES, LEIDENUNIVERSITY P.O. BOC 9506, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN,73(1989)291	A.A.VERHEIJEN,H.W.ZANDBERGEN,J.M.VAN RUITENBEEK,L.J.DE JONGH,Q.XU,W.T.FU	LA,SR,CU,O	
2041	SSC0670391		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.85	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z	6.85	1	1988																											3	Y123																				89				18.4	89																																																					SP2041																																																SPECIFIC HEAT OF PRASEODYMIUM DOPED YTTRIUM BARIUM COPPER OXIDE	198808	SPECIFIC HEAT            ,SCHOTTKY ANOMALIES       ,DOPANT	DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,INDIA	SOLID STATE COMMUN.,67(1988)391	D R.SRINIVASAN,G.RANGARAJAN,G.V.SUBBA RAO,K.A.THOMAS,L.S.VAIDHYANATHAN,N.SANKAR,U.V.VARADARAJU,V.SANKARANARAYANAN	Y,BA,CU,O	
2042	SSC0670391		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.82	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z	6.82	1	1988																											3	Y123																				71.6				33.3	71.6																																																																																																					SPECIFIC HEAT OF PRASEODYMIUM DOPED YTTRIUM BARIUM COPPER OXIDE	198808	SPECIFIC HEAT            ,SCHOTTKY ANOMALIES       ,DOPANT	DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,INDIA	SOLID STATE COMMUN.,67(1988)391	D R.SRINIVASAN,G.RANGARAJAN,G.V.SUBBA RAO,K.A.THOMAS,L.S.VAIDHYANATHAN,N.SANKAR,U.V.VARADARAJU,V.SANKARANARAYANAN	Y,BA,CU,O	
2043	SSC0670391		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																				67.4				25.4	67.4																																																					SP2043																																																SPECIFIC HEAT OF PRASEODYMIUM DOPED YTTRIUM BARIUM COPPER OXIDE	198808	SPECIFIC HEAT            ,SCHOTTKY ANOMALIES       ,DOPANT	DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,INDIA	SOLID STATE COMMUN.,67(1988)391	D R.SRINIVASAN,G.RANGARAJAN,G.V.SUBBA RAO,K.A.THOMAS,L.S.VAIDHYANATHAN,N.SANKAR,U.V.VARADARAJU,V.SANKARANARAYANAN	Y,BA,CU,O	
2044	SSC0670391		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.76	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z	6.76	1	1988																											3	Y123																				44.3				20.9	44.3																																																																																																					SPECIFIC HEAT OF PRASEODYMIUM DOPED YTTRIUM BARIUM COPPER OXIDE	198808	SPECIFIC HEAT            ,SCHOTTKY ANOMALIES       ,DOPANT	DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,INDIA	SOLID STATE COMMUN.,67(1988)391	D R.SRINIVASAN,G.RANGARAJAN,G.V.SUBBA RAO,K.A.THOMAS,L.S.VAIDHYANATHAN,N.SANKAR,U.V.VARADARAJU,V.SANKARANARAYANAN	Y,BA,CU,O	
2045	SSC0670391		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-Z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z		1	1988																											3	Y123																				25.4				12.2	25.4																																																					SP2045																																																SPECIFIC HEAT OF PRASEODYMIUM DOPED YTTRIUM BARIUM COPPER OXIDE	198808	SPECIFIC HEAT            ,SCHOTTKY ANOMALIES       ,DOPANT	DEPARTMENT OF PHYSICS,INDIAN INSTITUTE OF TECHNOLOGY,INDIA	SOLID STATE COMMUN.,67(1988)391	D R.SRINIVASAN,G.RANGARAJAN,G.V.SUBBA RAO,K.A.THOMAS,L.S.VAIDHYANATHAN,N.SANKAR,U.V.VARADARAJU,V.SANKARANARAYANAN	Y,BA,CU,O	
2046	APJ0291259	ESTIMATED BY TYPE-II S/C THEORY	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.4Pb0.6Ca2Sr2Cu3OZ	Bi	1.4	Pb	0.6	Ca	2	Sr	2	Cu	3											O	Z			1991																											2	Bi2223				5.415		37.044													108						108													111									61									0.81							23					2600																																																										MAGNETIC PROPERTIES OF HIGH-TC BI1.4PB0.6CA2SR2CU3OY SUPERCONDUCTOR	7	MAGNETIZATION       ,COHERENCE LENGTH    ,PENETRATION DEPTH	DEPARTMENT OF PHYSICS,SUNG KYUN KWAN UNIVERSITY,SUWAN 440-746,KOREA	JPN.J,APPL.PHYS.,29(1991)1259	CHONG-YUN PARK,KYUNG-SOO Y,MIN-SU JANG,SANG-GEUN LEE,SEONG-CHO YU,YOUNG-CHEOL KIM	BI,PB,CA,SR,CU,O	
2047	JJP0261231		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123				3.819	3.891	11.672														92.5					92.5																																																																																		3.8																			SUPERCONDUCTIVITY IN METAMORPHIC PHASES OF BA(2)ER(1)CU(3)O(7-Z)		RESISTIVITY              ,SUSCEPTIBILITY           ,LATTICE	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,JAPAN	JJAP LETT.,26(1987)L1231	M.ISHIKAWA,T.TAKABATAKE,Y.NAKAZAWA		
2048	JJP0261231		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z		1	1987																											3	Y123				3.84	3.877	11.763														51.8					51.8																																																																																		9.5																			SUPERCONDUCTIVITY IN METAMORPHIC PHASES OF BA(2)ER(1)CU(3)O(7-Z)		RESISTIVITY              ,SUSCEPTIBILITY           ,LATTICE	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,JAPAN	JJAP LETT.,26(1987)L1231	M.ISHIKAWA,T.TAKABATAKE,Y.NAKAZAWA		
2049	JJP0261231		ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z		1	1987																											2	Y123				3.862		11.823																	4.2																																																																																																							SUPERCONDUCTIVITY IN METAMORPHIC PHASES OF BA(2)ER(1)CU(3)O(7-Z)		RESISTIVITY              ,SUSCEPTIBILITY           ,LATTICE	INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,JAPAN	JJAP LETT.,26(1987)L1231	M.ISHIKAWA,T.TAKABATAKE,Y.NAKAZAWA		
2050	PRB0390225	KAIZERO=EMU/MOLE.OE	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.73Fe0.27O7.1	Y	1	Ba	2	Cu	2.73	Fe	0.27													O	7.1	7.1	1	1989		-65230000000				3.2	2.8																				3	Y123																				69					69													200																																								SP2050				73																																												SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND SPECIFIC-HEAT STUDIES OF THE HIGH-TC SUPERCONDUCTOR AND QUENCHED Y(1)BA(2)(CU(0.91)FE(0.09))(3)O(X)	198901	SUSCEPTIBILITY           ,SPECIFIC HEAT            ,XRY	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEMISRAEL	PHYS.REV.B,39(1989)225	G.HILSCHER,I.FELNER,N.PILLMAYR,Y.WOLFUS	Y,BA,CU,FE,O	
2051	PRB0390225	KAIZERO=EMU/MOLE.OE	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.73Fe0.27O6.1	Y	1	Ba	2	Cu	2.73	Fe	0.27													O	6.1	6.1	1	1989		-57670000000000000000000					-1	410																			2	Y123																							4.2																																																																																																							SUSCEPTIBILITY,CRYSTAL-STRUCTURE,AND SPECIFIC-HEAT STUDIES OF THE HIGH-TC SUPERCONDUCTOR AND QUENCHED Y(1)BA(2)(CU(0.91)FE(0.09))(3)O(X)	198901	SUSCEPTIBILITY           ,SPECIFIC HEAT            ,XRY	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEMISRAEL	PHYS.REV.B,39(1989)225	G.HILSCHER,I.FELNER,N.PILLMAYR,Y.WOLFUS	Y,BA,CU,FE,O	
2052	PRL0640080	OZ=3.99-3.              97	(Pr,Th)2CuO4	Pr1.85Th0.15Cu1O3.98	Pr	1.85	Th	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.981		12.214														17.2					17.2			K/GPa	-0.18																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2053	PRL0640080	OZ=3.99-3.              97	(Nd,Th)2CuO4	Nd1.85Th0.15Cu1O3.98	Nd	1.85	Th	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.958		12.127														17					17			K/GPa	-0.33																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2054	PRL0640080	OZ=3.99-3.              97	(Sm,Th)2CuO4	Sm1.85Th0.15Cu1O3.98	Sm	1.85	Th	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.932		11.948														1.8					1.8			K/GPa	-0.27																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2055	PRL0640080	OZ=3.99-3.              97	(Eu,Th)2CuO4	Eu1.85Th0.15Cu1O3.98	Eu	1.85	Th	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.919		11.877																	4.2																																																																																																							PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2056	PRL0640080	OZ=3.99-3.              97	(Gd,Th)2CuO4	Gd1.85Th0.15Cu1O3.98	Gd	1.85	Th	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.91		11.865																	4.2																																																																																																							PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2057	PRL0640080	OZ=3.99-3.              97	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O3.98	Pr	1.85	Ce	0.15	Cu	1															O	4-Z	3.98		1990																											2	T'				3.973		12.166														19.4					19.4			K/GPa	-0.1																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2058	PRL0640080	OZ=3.99-3.              97	(Nd,Th)2CuO4	Nd1.85Ce0.15Cu1O3.98	Nd	1.85	Ce	0.15	Cu	1															O	4-z	3.98		1990																											2	T'				3.952		12.091														21.2					21.2			K/GPa	-0.01																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2059	PRL0640080	OZ=3.99-3.              97	(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O3.98	Sm	1.85	Ce	0.15	Cu	1															O	4-z	3.98		1990																											2	T'				3.924		11.909														19.7					19.7			K/GPa	-0.49																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2060	PRL0640080	OZ=3.99-3.              97	(Eu,Ce)2CuO4	Eu1.85Ce0.15Cu1O3.98	Eu	1.85	Ce	0.15	Cu	1															O	4-z	3.98		1990																											2	T'				3.918		11.85														7.3					7.3			K/GPa	-0.37																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2061	PRL0640080	OZ=3.99-3.              97	(Gd,Ce)2CuO4	Gd1.85Ce0.15Cu1O3.99	Gd	1.85	Ce	0.15	Cu	1															O	4-z	3.99		1990																											2	T'				3.906		11.834																	4.2																																																																																																							PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2062	SSC0750059		EuBa2Cu3O7	Eu1Ba2Cu3O6.9	Eu	1	Ba	2	Cu	3															O	Z	6.9	1	1990																											3	Y123				3.844	3.899	11.7													88						88																																																																																																					MAGNETIC SUSCEPTIBILITY, RESISTIVITY AND 151EU MOSSBAUER STUDIES ON ZN-SUBSTITUTED EUBA2CU3O7-Y		MOSSBAUER	TATA INSTITUTE OF FUNDAMENTAL RESEARCH, BOMBAY 400 005, INDIA	SOLID STATE COMMUN.,75(1990)59	C.V.TOMY,KALYAN ADHIKARY,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.MALIK	EU,BA,CU,O,ZN	
2063	SSC0750059		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.925Zn0.075OZ	Eu	1	Ba	2	Cu	2.925	Zn	0.075													O	Z		1	1990																											3	Y123				3.848	3.901	11.71													27						27																																																																																																					MAGNETIC SUSCEPTIBILITY, RESISTIVITY AND 151EU MOSSBAUER STUDIES ON ZN-SUBSTITUTED EUBA2CU3O7-Y		MOSSBAUER	TATA INSTITUTE OF FUNDAMENTAL RESEARCH, BOMBAY 400 005, INDIA	SOLID STATE COMMUN.,75(1990)59	C.V.TOMY,KALYAN ADHIKARY,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.MALIK	EU,BA,CU,O,ZN	
2064	SSC0750059		EuBa2(Cu,Zn)307	Eu1Ba2Cu2.85Zn0.15OZ	Eu	1	Ba	2	Cu	2.85	Zn	0.15													O	Z		1	1990																											3	Y123				3.853	3.904	11.7																	12																																																																																																							MAGNETIC SUSCEPTIBILITY, RESISTIVITY AND 151EU MOSSBAUER STUDIES ON ZN-SUBSTITUTED EUBA2CU3O7-Y		MOSSBAUER	TATA INSTITUTE OF FUNDAMENTAL RESEARCH, BOMBAY 400 005, INDIA	SOLID STATE COMMUN.,75(1990)59	C.V.TOMY,KALYAN ADHIKARY,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.MALIK	EU,BA,CU,O,ZN	
2065	SSC0750059		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.775Zn0.225OZ	Eu	1	Ba	2	Cu	2.775	Zn	0.225													O	Z		1	1990																											3	Y123				3.858	3.902	11.71																	12																																																																																																							MAGNETIC SUSCEPTIBILITY, RESISTIVITY AND 151EU MOSSBAUER STUDIES ON ZN-SUBSTITUTED EUBA2CU3O7-Y		MOSSBAUER	TATA INSTITUTE OF FUNDAMENTAL RESEARCH, BOMBAY 400 005, INDIA	SOLID STATE COMMUN.,75(1990)59	C.V.TOMY,KALYAN ADHIKARY,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.MALIK	EU,BA,CU,O,ZN	
2066	SSC0750059		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.7Zn0.3OZ	Eu	1	Ba	2	Cu	2.7	Zn	0.3													O	Z		1	1990																											2	Y123				3.888		11.67																	12																																																																																																							MAGNETIC SUSCEPTIBILITY, RESISTIVITY AND 151EU MOSSBAUER STUDIES ON ZN-SUBSTITUTED EUBA2CU3O7-Y		MOSSBAUER	TATA INSTITUTE OF FUNDAMENTAL RESEARCH, BOMBAY 400 005, INDIA	SOLID STATE COMMUN.,75(1990)59	C.V.TOMY,KALYAN ADHIKARY,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.MALIK	EU,BA,CU,O,ZN	
2067	PHC1670097	HEAT TREATED AT 200C IN F2(1.3BAR),MAYBE F IS CORPORATED	La2CuFoO4	La2Cu1FO4	La	2	Cu	1	F																O	4			1990																											3					5.342	5.436	13.192														40					40													700																																																																																								STABILIZATION OF A NEW SUPERCONDUCTING PHASE BY LOW TEMPERATURE FLUORINATION OF LA2CUO4		HC1                 ,F2 GAS              ,NEW COMPOUND        ,SUSCEPTIBILITY	LABORATOIRE DE CHIMIE DU SOLIDE DU CNRS,UNIVERSITE BORDEAUX 1,33405 TALENCE CEDEX,FRANCE	PHYSICA C,167(1990)97	A.TRESSAUD,B.CHEVALIER,B.LEPINE,E.HICKEY,J.ETOURNEAU,J.M.DANCE,K.AMINE,L.LOZANO	LA,CU,O,F	
2068	PHC1660393	NO 123,247 PHASES	HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1990						10.4	-14																					Y124																			76		76				76										9																																											SP2068						380																							5.8																			SPECIFIC HEAT, MAGNETIZATION AND RESISTIVITY MEASUREMENTS ON HOBA2CU4O8		SPECIFIC HEAT       ,RESISTIVETY         ,MAGNETIZATION	LABRATORIUM FUR FESTKORPRPHYSIK,ETHZ,HC-8093 ZURICH,SWIZRELAND	PHYSICA C,166(1990)393	A.BERNASCONI,A.SCHILLING,H.R.OTT,J.D.GUO	HO,BA,CU,O	
2069	PHC1670236	DTC/DP=-0.434(B-A)/A *E3 + 7.93,DTCDP=K/GPA	Y2Ba4Cu7O15	Y2Ba4Cu7O15	Y	2	Ba	4	Cu	7															O	15			1990																												Y247																				93				4	93			K/GPa	3																																																																																																	HIGH-PRESSURE STUDIES ON THE 90 K SUPERCONDUCTORS Y2BA4CU7O15AND (Y/CA)BA2CU4O8		HELIUM PRESSURES    ,RESISTIV            ,SUSCEPTIBILITY	PHYSICS AND ENGINEERING LABORATORY,DEPARTMENT OF SINENIFIC ANDINDUSTRIAL RESEARCH,PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,167(1990)236	J.L.TALLON,J.LUSK	Y,BA,CU,CA	
2070	PHC1670236	CA 75% ON Y-            SITE	(Y,Ca)Ba2Cu4O8	Y0.93Ca0.07Ba2Cu4O8	Y	0.93	Ca	0.07	Ba	2	Cu	4													O	8			1990																												Y124																			85.5	89				4	89			K/GPa	4.5																																																																																																	HIGH-PRESSURE STUDIES ON THE 90 K SUPERCONDUCTORS Y2BA4CU7O15AND (Y/CA)BA2CU4O8		HELIUM PRESSURES    ,RESISTIV            ,SUSCEPTIBILITY	PHYSICS AND ENGINEERING LABORATORY,DEPARTMENT OF SINENIFIC ANDINDUSTRIAL RESEARCH,PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,167(1990)236	J.L.TALLON,J.LUSK	Y,BA,CU,CA	
2071	SSC0750779	TWO STEP CHANGE IN THERMAL CONDUCTIVITY	((Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.4Pb0.5Sb0.1Sr2Ca2Cu3O10-X	Bi	1.4	Pb	0.5	Sb	0.1	Sr	2	Ca	2	Cu	3									O	10-X			1990																																																106.9	108.6				106.9																																																																	TC2071																																				THERMAL CONDUCTIVITY OF BI-BASED HIGH-TC SUPERCONDUCTORS IN THE VICINITY OF SUPERCONDUCTING TRANSITION		THERMAL CONDUCTIVITY	INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCE,OKOLNA 2,50-422 WROCLAW, P.O. BOX 937, POLAND	SOLID STATE COMMUN.,75(1990)779	A.JEZOWSKI	BI,PB,SB,SR,CA,CU,O	
2072	SSC0750785		Yb2Cu2O5	Yb2Cu2O5	Yb	2	Cu	2																	O	5			1990																													PN2(1)A			10.724	12.337	3.432																																																																																																																								CRYSTAL STRUCTURE REFINEMENT AND MAGNETIC ORDERING IN R2CU2O5(R=HO,TM,YB) COMPOUNDS		CRYSTAL STRUCTURES  ,NEUTRON DIFFRACTION ,MAGNETIC ORDERING	LABOR FUR NEUTRONENSTREUUNG ETHZ, CH-5232 VILLIGEN PSI, SWITZERLAND	SOLID STATE COMMUN.,75(1990)785	A.MURASIK,P.FISCHER,R.TROC,Z.BUKOWSKI	HO,TM,YB,CU,O	
2073	SSC0750785		Tm2Cu2O5	Tm2Cu2O5	Tm	2	Cu	2																	O	5			1990																																10.741	12.371	3.459																																																																																																																								CRYSTAL STRUCTURE REFINEMENT AND MAGNETIC ORDERING IN R2CU2O5(R=HO,TM,YB) COMPOUNDS		CRYSTAL STRUCTURES  ,NEUTRON DIFFRACTION ,MAGNETIC ORDERING	LABOR FUR NEUTRONENSTREUUNG ETHZ, CH-5232 VILLIGEN PSI, SWITZERLAND	SOLID STATE COMMUN.,75(1990)785	A.MURASIK,P.FISCHER,R.TROC,Z.BUKOWSKI	HO,TM,YB,CU,O	
2074	SSC0750785		Ho2Cu2O5	Ho2Cu2O5	Ho	2	Cu	2																	O	5			1990																																																																																																																																																										CRYSTAL STRUCTURE REFINEMENT AND MAGNETIC ORDERING IN R2CU2O5(R=HO,TM,YB) COMPOUNDS		CRYSTAL STRUCTURES  ,NEUTRON DIFFRACTION ,MAGNETIC ORDERING	LABOR FUR NEUTRONENSTREUUNG ETHZ, CH-5232 VILLIGEN PSI, SWITZERLAND	SOLID STATE COMMUN.,75(1990)785	A.MURASIK,P.FISCHER,R.TROC,Z.BUKOWSKI	HO,TM,YB,CU,O	
2075	JJP0291396	B=GPA	(Bi2Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.4Sr1.85Ca2.05Cu3O10.26	Bi	1.8	Pb	0.4	Sr	1.85	Ca	2.05	Cu	3											O	10+X	10.26		1990																		GPa		73								Bi2223														-0.003		-0.008				107					107			K/GPa	2																																																																																																	PRESSURE-EFFECT STUDY ON THE HIGH-TC SUPERCONDUCTOR BI(PB)-SR-CA-CU-O SYSTEM	199008	PRESSURE EFFECT     ,X-RAY               ,COMPRESSIBILITY	DEPARTMENT OF MATERIAL SCIENCE, HIMEJI INSTITUTE OF TECHNOLOGY, HIMEJI 670	JJAP LETT,29(1990)L1396	HARUKI KAWAMURA,MOTOTADA KOBAYASHI,TAKUJI YONEDA,YOSHIHISA MORI,YUICHI AKAHAMA	BI,PB,SR,CA,CU,O	
2076	JJP0291396	B=GPA	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z			1990																		GPa		61								Bi2212														-0.004		-0.008				85					85			K/GPa	2																																																																																																	PRESSURE-EFFECT STUDY ON THE HIGH-TC SUPERCONDUCTOR BI(PB)-SR-CA-CU-O SYSTEM	199008	PRESSURE EFFECT     ,X-RAY               ,COMPRESSIBILITY	DEPARTMENT OF MATERIAL SCIENCE, HIMEJI INSTITUTE OF TECHNOLOGY, HIMEJI 670	JJAP LETT,29(1990)L1396	HARUKI KAWAMURA,MOTOTADA KOBAYASHI,TAKUJI YONEDA,YOSHIHISA MORI,YUICHI AKAHAMA	BI,PB,SR,CA,CU,O	
2077	JJP0291079	HIGH O2 PRESS,HIP PROCESS	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1990																											3	Y124				3.842	3.863	27.19														83					83										50			140									114									2							17					2400																																																										CRITICAL CURRENT DENSITIES OF Y1-XCAXBA2CU4O8 (X=0 AND 0.1) SUPERCONDUCTING CERAMICS	199007	CRITICAL CURRENT    ,CRITICAL FIELD	SUPERCONDUCTIVITY RESEARCH LABORATORY, ISTEC, 1-10-13 SHINONOME, KOTO-KU, TOKYO 135	JJAP LETT,29(1990)L1079	KOJI YAMAGUCHI,NAOKI KOSHIZUKA,SATOSHI GOTOH,SHOJI TANAKA,TAKAYUKI MIYATAKE,TSUTOMU TAKATA	Y,CA,BA,CU,O	
2078	JJP0291079	HIGH O2 PRESS,HIP PROCESS	(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8			1990																											3	Y124				3.841	3.864	27.21														91					91										45			185									172									2.77							14					2100																																																										CRITICAL CURRENT DENSITIES OF Y1-XCAXBA2CU4O8 (X=0 AND 0.1) SUPERCONDUCTING CERAMICS	199007	CRITICAL CURRENT    ,CRITICAL FIELD	SUPERCONDUCTIVITY RESEARCH LABORATORY, ISTEC, 1-10-13 SHINONOME, KOTO-KU, TOKYO 135	JJAP LETT,29(1990)L1079	KOJI YAMAGUCHI,NAOKI KOSHIZUKA,SATOSHI GOTOH,SHOJI TANAKA,TAKAYUKI MIYATAKE,TSUTOMU TAKATA	Y,CA,BA,CU,O	
2079	PR0409389	THC FOR OUT-OF PLANE,THC(C)	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																											3																					92				0.2	92																																																														8.2			THC2079																																				ANISOTROPY OF THE THERMAL CONDUCTIVITY OF YBA2CU3O7-Y	198911	THERMAL CONDUCTIVITY,ANISOTROPIC         ,ELECTRON-PHONON	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B,40(1989)9389	N.P.ONG,S.J.HAGEN,Z.Z.WANG	Y,BA,CU,O	
2080	PR0409389	THC FOR AB PLANE,THC(AB)	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																											2																								4.2																																																																7.25			THC2080																																				ANISOTROPY OF THE THERMAL CONDUCTIVITY OF YBA2CU3O7-Y	198911	THERMAL CONDUCTIVITY,ANISOTROPIC         ,ELECTRON-PHONON	JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	PHYS.REV.B,40(1989)9389	N.P.ONG,S.J.HAGEN,Z.Z.WANG	Y,BA,CU,O	
2081	PRB0402694	NEUTRON IRRADIATED, Tc is for fluence = 30 E+17. FLUENCE DEP. OF TC IN FIGURE(TC2081)	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		2	1989																											3	Y123																		K		86.5					86.5	TC2081																																																													7			THC2081		-4.05			TP2081																															THERMOELECTRIC POWER AND THERMAL CONDUCTIVITY OF NEUTRON-IRRADIATED YBA2CU3O7-Z	198908	THERMOELECTRIC POWER,THERMAL CONDUCTIVITY,FAST-NEUTRON        ,IRRADIATION	DEPARTMENT OF PHYSICS,UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,40(1989)2694	C.UHER,W.-N.HUANG	Y,BA,CU,O	
2082	PSA1030037		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1987																											2					3.774		13.253														34.2				6	34.2																																																																	THC2082													0.8																							THERMAL AND ELECTRICAL CONDUCTIVITY OF LA(1.8)SR(0.2)CU(1)O(4) SAMPLES	198709	THERMAL CONDUCTIVITY     ,RES	INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCES,WROCLAW	PHYS.STAT.SOL..A, 103(1987)K37	A.J.ZALESKI,A.STEPIEN-DAMM,C.MARUCHA,C.SULKOWSKI,E.TROJNAR,J.KLAMUT,J.RAFALOWICZ,K.BARTKOWSKI,K.ROGACKI,M.HOROBIOWSKI,R.HORYN,Z.BUKOWSKI	LA,SR,CU,O	
2083	PRB0400841	K=0.15*T**2.0 FOR T<1.6K, AB-PLANE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1989																											2	Bi2212																				84					84																																																																	THC2083																																				LOW-TEMPERATURE THERMAL CONDUCTIVITY OF SINGLE-CRYSTAL BI(2)SR(2)CACU(2)O(8)	198907	THERMAL CONDUCTIVITY,SINGLE CRYSTAL	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,1110 WEST GREEN STREET,URBANA,ILLINOIS 61801	PHYS.REV.B.,40(1989)841	A.C.ANDERSON,D.M.GINSBERG,DA-MING ZHU,E.D.BUKOWSKI	BI,SR,CA,CU,O	
2084	PRL0622885	TWO FLUID MODEL,PENET=879A BY USING WEAK-COUPLING MODEL	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1989																												Y123																				89.6					89.6																																											1705																																																										MAGNETIC PENETRATION DEPTH OF YBA2CU3O7	6		AT&T BELL LABORATORIES MURRY HILL,NEW JERSEY 07974	PHYS.REV.LETT.,62(1989)2885	A.F.HEBARD,A.T.FIORY,D.R.HARSHMAN	Y,BA,CU,O	
2085	PRL0611419	FROM SUSCEPTIBILITY USING  =1-(2P/D)TANH(D/2P)	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																												Y123																				89.7				0.2	89.7																																											1400																																																										RENORMALIZATION OF THE MEAN-FIELD SUPERCONDUCTING PENETRATION DEPTH IN EPITAXIAL Y(1)BA(2)CU(3)O(7) FILMS	198809	PENETRATION DEPTH        ,KOSTERLITZ-THO	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.LETT.,61(1988)1419	A.F.HEBARD,A.T.FIORY,P.M.MANKIEWICH,R.E.HOWARD	Y,BA,CU,O	
2086	PHC1600541	HC2 ESTIMATED HY WHH THEORY	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.842	3.863	27.19													79.6	82.5	82.6				82.5										50			140									114									2							17					2400																																			0.75				3																			PREPARATION AND SUPERCONDUCTING PROPERTIES OF YBA2CU4O8	198910			PHYS.C.160(1989)541	GOTOH,K.,KOSHIZUKA,MIYATAKE,N.,S.,T.,TAKATA,TANAKA,YAMAGUCHI		
2087	PHC1531515	THC BELOW 7K,FIELD DEP. OF THC AND MAGNETIZATION	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1988								2.2																				Y123																				95.5				1.5	95.5																																																																														0.6																							THERMAL TRANSPORT AND MAGNETIC PROPERTIES OF GdBa2Cu3O7-y SUPERCONDUCTOR			College of Liberal Arts, Toyama University, 3190 Gofuku, Toyama 930 Japan	Physica.C,153-155(1988)1515-1516	Katsunori MORI,Kiyoo SATO,Koshichi NOTO,Masahiro SASAKAWA,Norio KOBAYASHI,Yoshikazu ISHIKAWA,Yoshio MUTO		
2088	PHC1700259	H//AB-PLANE,SLIGHTLY DIFFERENT FOR ANOTHER DIRECTION	YBa2Cu4O8	Y1Ba2Cu4OZ	Y	1	Ba	2	Cu	4															O	Z		3	1990																											4	Y124																			73.6	74.6	76.7			3	74.6			K/GPa	6.8																																																																																																	CHANGE OF CRITICAL PARAMETERS OF YBA2CU4OX AND YBA2CU3.5OX SINGLE CRYSTALS UNDER PRESSURE			INSTITUTE FOR HIGH PRESSURE PHYSICS, ACADEMY OF SCIENCES OF THE USSR, TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C,170(1990)259	A.E.LUPPOV,A.G.GAPOTCHENKO,S.L.BUD'KO	Y,BA,CU,O	
2089	PHC1700259	H//AB-PLANE,SLIGHTLY DIFFERENT FOR ANOTHER DIRECTION	Y2Ba4Cu7O15	Y2Ba4Cu7OZ	Y	2	Ba	4	Cu	7															O	Z		3	1990																											4	Y247																			45.3	51.3	53.3				51.3			K/GPa	5.6																																																																																																	CHANGE OF CRITICAL PARAMETERS OF YBA2CU4OX AND YBA2CU3.5OX SINGLE CRYSTALS UNDER PRESSURE			INSTITUTE FOR HIGH PRESSURE PHYSICS, ACADEMY OF SCIENCES OF THE USSR, TROITSK, MOSCOW REGION, 142092, USSR	PHYSICA C,170(1990)259	A.E.LUPPOV,A.G.GAPOTCHENKO,S.L.BUD'KO	Y,BA,CU,O	
2090	PR04111681		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1990																												Y123																					93				93																																																3.5	2																																																				Infrared absorptivity of YBa2Cu3O7-x crystal	199006		Center for Superconductivity Research, Physics Department, University of Maryland, College Park, Maryland 20742 and Laboratory for Physical Sciences, College Park, Maryland 20740	Phys.Rev.B,41(1990)11681	H.D. Drew,J.Z. Liu,S.H. Moseley,T. Pham		
2091	HPA0610438	ERROR BELOW 1.5%	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				92.7				2.5	92.7																																																														3.32			THC2091																	2.4																							Helvetica Phys.Acta, 61(19??) 438			
2092	HPA0610438	ERROR BELOW 1.5%	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				89.5				4.2	89.5																																																														4.74			THC2092																	0.74																							Helvetica Phys.Acta, 61(19??) 438			
2093	HPA0610438	ERROR BELOW 1.5%	SmBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																				92				2.2	92																																																														5.13			THC2093																	1.5																							Helvetica Phys.Acta, 61(19??) 438			
2094	SST0010296		YBa2Cu3O7	Y1Ba2Cu3O6.81	Y	1	Ba	2	Cu	3															O	Z	6.81	1	1989																											3	Y123																				89.5					89.5																																																														4.96			THC2094																																				Thermal conductivity of the Y-Ba-Cu-O tetragonal structure: phase transitions and hysteresis behaviour			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw, Poland	Supercond.Scie.Technol., 1(1989)296	A.Jezowski,J.Klamut,R.Horyn,K.Rogacki		
2095	SST0010296		YBa2Cu3O7	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	Z	6.54	1	1989																											3	Y123																				58					58																																																														4.49			THC2095																																				Thermal conductivity of the Y-Ba-Cu-O tetragonal structure: phase transitions and hysteresis behaviour			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw, Poland	Supercond.Scie.Technol., 1(1989)296	A.Jezowski,J.Klamut,R.Horyn,K.Rogacki		
2096	SST0010296		YBa2Cu3O7	Y1Ba2Cu3O6.1	Y	1	Ba	2	Cu	3															O	Z	6.1	1	1989																											2	Y123				3.858		11.811																																																																																	2.76			THC2096																																				Thermal conductivity of the Y-Ba-Cu-O tetragonal structure: phase transitions and hysteresis behaviour			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw, Poland	Supercond.Scie.Technol., 1(1989)296	A.Jezowski,J.Klamut,R.Horyn,K.Rogacki		
2097	PHC1560574	SEE SSC0651001	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				92.4					92.4			K/kbar	0.07																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2098	PHC1560574	SEE SSC0651001	(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-Z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z			1988																												Y123																				85.5					85.5			K/kbar	0.18																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2099	PHC1560574	SEE SSC0651001	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1988																												Y123																				79.6					79.6			K/kbar	0.3																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2100	PHC1560574	SEESSC0651001	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z			1988																												Y123																				56					56			K/kbar	0.32																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2101	PHC1560574	SEESSC0651001	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7-Z	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z			1988																												Y123																				48.5					48.5			K/kbar	-0.21																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2102	PHC1560574	SEESSC0651001	(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-Z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z			1988																												Y123																				28.9					28.9			K/kbar	-0.68																																																																																																	PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF (Y1-XPRX)BA2CU3O7-Z COMPOUNDS; EVIDENCE FOR 4F ELECTRONHYBRIDIZATION				PHYSICA C,156(1988)574	MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S		
2103	PHC1710315		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.824		30.678														92					92																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2104	PHC1710315		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.8La0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	La	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.831		30.786														87.9					87.9																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2105	PHC1710315		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.8Nd0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Nd	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.829		30.752														88.8					88.8																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2106	PHC1710315		Bi2Sr2(Ca,Eu)Cu2O8	Bi2Sr2Ca0.8Eu0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Eu	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.826		30.688														90.4					90.4																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2107	PHC1710315		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.826		30.709														89.8					89.8																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2108	PHC1710315		Bi2Sr2(Ca,Dy)Cu2O8	Bi2Sr2Ca0.8Dy0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Dy	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.824		30.685														90.8					90.8																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2109	PHC1710315		Bi2Sr2(Ca,Yb)Cu2O8	Bi2Sr2Ca0.8Yb0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Yb	0.2	Cu	2											O	8+Z	8.26		1990																											2					3.821		30.657														91.2					91.2																																																																																																					SUBSTITUTION EFFECT OF RARE EARTH (R) FOR CA IN THE BI2SR2CA1-XRXCU2O8+Y SYSTEM		IONIC RADIUS        ,TC	INSTITUTE OF APPLIED PHYSICS AND CRYOGENICS CENTER,UNIVERSITYOF TSUKUBA, TSUKUBA, IBARAKI 305,JAPAN	PHYSICA C,171(1990)315	H.ASANO,J.FUJIKAMI,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R,	
2110	PHC1710287		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z			1990																											3																					95.8					95.8																																																																																																					INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2111	PHC1710287	DTC/DP IN K/GPA	(Eu,Pr)Ba2Cu3O7	Eu0.9Pr0.1Ba2Cu3O7-Z	Eu	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z			1990																											3	Y123				3.838	3.885	11.673													74	77.8	81.7				77.8			K/GPa	1																																																																																																	INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2112	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O7-Z	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1990																											3					3.843	3.885	11.68													48.3	53.5	60.2				53.5																																																																																																					INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2113	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.7Pr0.3Ba2Cu3O7-Z	Eu	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z			1990																											3					3.841	3.889	11.681													29.4	35.2	41.3				35.2																																																																																																					INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2114	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.65Pr0.35Ba2Cu3O7-Z	Eu	0.65	Pr	0.35	Ba	2	Cu	3													O	7-Z			1990																											3																				10.4	19.1	26.5				19.1																																																																																																					INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2115	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.6Pr0.4Ba2Cu3O7-Z	Eu	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z			1990																											3																								4.2																																																																																																							INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2116	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.5Pr0.5Ba2Cu3O7-Z	Eu	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z			1990																											3																								4.2																																																																																																							INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2117	PHC1710287		(Eu,Pr)Ba2Cu3O7	Eu0.1Pr0.9Ba2Cu3O7-Z	Eu	0.1	Pr	0.9	Ba	2	Cu	3													O	7-Z			1990																											3																								4.2																																																																																																							INVESTIGATION OF THE PRASEODYMIUM ROLE IN SUPERCONDUCTIVITY OF(EU1-XPRX)BA2CU3O7-Z AND RELATED COMPOUNDS		X-RAY               ,RESISTIVITY         ,MOSSBAUER	INSTITUTE OF PHYSICS, JAGELLONIAN UNIVERSITY, REYMONTA 4,30-059 CRACOW,POLAND	PHYSICA C,171(1990)287	A.SZYTUTA,A.ZYGMUNT,K.LATKA,R.DURAJ,Z.TOMKOWICZ	EU,PR,BA,CU,O	
2118	PHC1710523		(La,Ca)2CaCu2O6	La1.9Ca1.1Cu2O6-Z	La	1.9	Ca	1.1	Cu	2															O	6-Z		1	1990																												2126																				39.5					39.5																																																																																																					HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING LA2-XCA1+XCU2O6-X/2+Z		SYNTHESIS           ,MEISSNER VOLUME	NTT BASIC RESEARCH LABORATORIES, MIDORI-CHO, MUSASHINO-SHI, TOKYO 180, JAPAN	PHYSICA C,171(1990)523	HIROYUKI SHIBATA,KYOICHI KINOSHITA,TOMOAKI YAMADA	LA,CA,CU,O	
2119	PHC1710523		(La,Ca)2CaCu2O6	La1.85Ca1.15Cu2O6-Z	La	1.85	Ca	1.15	Cu	2															O	6-Z		1	1990																												2126				38.2		19.419														45.5					45.5																																																																																																					HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING LA2-XCA1+XCU2O6-X/2+Z		SYNTHESIS           ,MEISSNER VOLUME	NTT BASIC RESEARCH LABORATORIES, MIDORI-CHO, MUSASHINO-SHI, TOKYO 180, JAPAN	PHYSICA C,171(1990)523	HIROYUKI SHIBATA,KYOICHI KINOSHITA,TOMOAKI YAMADA	LA,CA,CU,O	
2120	PHC1710523		(La,Ca)2CaCu2O6	La1.75Ca1.25Cu2O5.99	La	1.75	Ca	1.25	Cu	2															O	6-Z	5.99	1	1990																												2126																			44.7	47.7					47.7										12																																																																																											HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING LA2-XCA1+XCU2O6-X/2+Z		SYNTHESIS           ,MEISSNER VOLUME	NTT BASIC RESEARCH LABORATORIES, MIDORI-CHO, MUSASHINO-SHI, TOKYO 180, JAPAN	PHYSICA C,171(1990)523	HIROYUKI SHIBATA,KYOICHI KINOSHITA,TOMOAKI YAMADA	LA,CA,CU,O	
2121	PHC1710523		(La,Ca)2CaCu2O6	La1.4Ca1.6Cu2O6-Z	La	1.4	Ca	1.6	Cu	2															O	6-Z		2	1990																												2126																				47.7					47.7																																																																																																					HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING LA2-XCA1+XCU2O6-X/2+Z		SYNTHESIS           ,MEISSNER VOLUME	NTT BASIC RESEARCH LABORATORIES, MIDORI-CHO, MUSASHINO-SHI, TOKYO 180, JAPAN	PHYSICA C,171(1990)523	HIROYUKI SHIBATA,KYOICHI KINOSHITA,TOMOAKI YAMADA	LA,CA,CU,O	
2122	PHC1710223	PENET DEPENDS ON PARTICLE SIZE AND PARTICLE SHAPE	YBa2Cu3O7	Y1Ba2Cu3O6.83	Y	1	Ba	2	Cu	3															O	7-Z	6.83	5	1990																											3	Y123				3.83	3.88	11.16																																																														1430																																																										TEMPERATURE DEPENDENCE OF THE MAGNETIC FIELD PENETRATION DEPTHIN YBA2CU3O7-Z MEASURED ON ULTRA FINE POWDER		PENETRATION DEPTH   ,SUSCEPTIBILITY      ,FINE POWDER	INSTITUTE OF SOLID STATE PHYSICS, ACADEMY OF THE USSR, CHERNOGOLOVKA, MOSCOW DISTRICT, 142432, USSR	PHYSICA C,171(1990)223	A.M.NEMINSKY,A.V.PETINOVA,I.G.NAUMENKO,N.I.GOLOVKO,V.F.GANTMAKHER	Y,BA,CU,O	
2123	JJP0261304		LaBa2Cu3O7	La1Ba2Cu3OX	La	1	Ba	2	Cu	3															O	X		1	1987																											3																					62.5	69			15	62.5																															2.1																																															5.4																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2124	JJP0261304		NdBa2Cu3O7	Nd1Ba2Cu3OX	Nd	1	Ba	2	Cu	3															O	X		1	1987																											3																					93.6	94.6			2.3	93.6																															2																																															0.69																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2125	JJP0261304		SmBa2Cu3O7	Sm1Ba2Cu3OX	Sm	1	Ba	2	Cu	3															O	X		1	1987																											3																					94.2	94.6			1	94.2																															2.1																																															0.43																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2126	JJP0261304		EuBa2Cu3O7	Eu1Ba2Cu3OX	Eu	1	Ba	2	Cu	3															O	X		1	1987																											3																					93.9	94.4			2.6	93.9																															2																																															1.5																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2127	JJP0261304		GdBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X		1	1987																											3																					93.6	93.9			0.6	93.6																															2.9																																															0.35																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2128	JJP0261304		DyBa2Cu3O7	Dy1Ba2Cu3OX	Dy	1	Ba	2	Cu	3															O	X		1	1987																											3																					91.8	92.3			2	91.8																															2.7																																															0.68																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2129	JJP0261304		HoBa2Cu3O7	Ho1Ba2Cu3OX	Ho	1	Ba	2	Cu	3															O	X		1	1987																											3																					91.7	92.3			2.5	91.7																															2.6																																															0.84																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2130	JJP0261304		ErBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X		1	1987																											3																					91.4	92.3			1.5	91.4																															2																																															0.73																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2131	JJP0261304		TmBa2Cu3O7	Tm1Ba2Cu3OX	Tm	1	Ba	2	Cu	3															O	X		1	1987																											3																					90.2	91			1.9	90.2																															2.1																																															0.36																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2132	JJP0261304		YbBa2Cu3O7	Yb1Ba2Cu3OX	Yb	1	Ba	2	Cu	3															O	X		1	1987																											3																					88.7	89.8			2.3	88.7																															2.4																																															0.6																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2133	JJP0261304		LuBa2Cu3O7	Lu1Ba2Cu3OX	Lu	1	Ba	2	Cu	3															O	X		1	1987																											3																					86.9	88.7			3	86.9																															2.4																																															0.64																							Structure and Upper Critical Fields of High Tc Superconductors (RE)Ba2Cu3Ox			The Institute for Solid State Physics, The University of Tokyo, Roppongi, Minato-ku, Tokyo 106	Jpn. J.Appl.Phys., 26(1987)L1304	Akiko WATANABE,Isamu OGURO,Tsuyoshi TAMEGAI,Yasuhiro IYE		
2134	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8	Pb	2	Sr	2	Y	1	Cu	3													O	8.0	8		1990																											3					5.407	5.448	15.731																	4.2																																																																																								0.000000256															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2135	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8.5	Pb	2	Sr	2	Y	1	Cu	3													O	8.5	8.5		1990																											3					5.419	5.457	15.848																	4.2																																																																																								0.0000285															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2136	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8.8	Pb	2	Sr	2	Y	1	Cu	3													O	8.8	8.8		1990																											3	Pb3212				5.412	5.459	15.933																	4.2																																																																																								0.0000856															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2137	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8.0	8		1990	emu/g	0.00000017																									3	Pb3212				5.398	5.434	15.825														78.4					78.4																																																																																						0.0000000118															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2138	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8.6	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8.6	8.6		1990	emu/g	0.00000036																									3	Pb3212				5.408	5.438	15.848														65					65																																																																																						0.000000331															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2139	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O9	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	9.0	9		1990																												Pb3212						15.99																	4.2																																																																																								0.00000765															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2140	PHC1710331	ALMOST SINGLE PHASE,KAI=EMU/G	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O9.47	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	9.47	9.47		1990																											2	Pb3212				5.47		15.002																	4.2																																																																																								0.00011															NORMAL AND SUPERCONDUCTING PROPERTIES OF PB2SR2Y1-XCAXCU3O8+ZII.DEPENDENCE ON THE OXYGEN CONCENTRATION			DEPARTMENT OF APPLIED PHYSICS, FACULTY OF ENGINEERING, TOHOKUUNIVERSITY, ARAMAKI AOBA, AOBA-KU, SENDAI 980, JAPAN	PHYSICA C,171(1990)331	HIROMU SUNAGAWA,KICHINOSUKE HIROKAWA,MASAHIRO MASUZAWA,MICHIKO NAMIKI,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	PB,SR,Y,CA,CU,O	
2141	PRB0363917	LORENTZ NO.=2.45E-8W.OHM./K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1987																																															86					5	86																																																																	THC2141																	19																			THERMAL CONDUCTIVITY OF SUPERCONDUCTIVE Y-BA-CU-O	198709	THERMAL CONDUCTIVITY	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,36(1987)3917	D.E.SWETS,D.T.MORELLI,J.HEREMANS	Y,BA,CU,O	
2142	PRB0368786	THC VARIES AS T**2 FOR T<0.3K	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987									4.43																																						87	91.6				2.6	91.6																																																																	THC2142																																				LOW-TEMPERATURE THERMAL CONDUCTIVITY OF Y(1)BA(2)CU(3)O(7-Z)	198712	THERMAL CONDUCTIVITY	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN	PHYS.REV.B,36(1987)8786	A.ZANGVIL,D.M.GINSBERG,J.CHEN,J.J.FREEMAN,T.A.FRIEDMANN	Y,BA,CU,O	
2143	PRB0368813	SDW=150K,SOUND VELOCITY=4E+5CM/S	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1987																											3	T																																																																																				300						THC2143																																				ANOMALOUS THERMAL CONDUCTIVITY OF LA(2-X)SR(X)CU(1)O(4): POSSIBILITY OF A POLARONIC GLASS	198712	THERMAL                  ,CONDUCTIVITY	CENTRO ATOMICO BARILOCHE,COMISION NACIONAL DE ENERGIA ATOMICA,ARGENTINA	PHYS.REV.B,36(1987)8813	C.D'OVIDIO,D.CASTELLO,D.ESPARZA,M.A.IZBIZKY,M.NUNEZ REGUEIORO	LA,SR,CU,O	
2144	PRB0368813		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																																																35.5				2	35.5																																																																	THC2144																																				ANOMALOUS THERMAL CONDUCTIVITY OF LA(2-X)SR(X)CU(1)O(4): POSSIBILITY OF A POLARONIC GLASS	198712	THERMAL                  ,CONDUCTIVITY	CENTRO ATOMICO BARILOCHE,COMISION NACIONAL DE ENERGIA ATOMICA,ARGENTINA	PHYS.REV.B,36(1987)8813	C.D'OVIDIO,D.CASTELLO,D.ESPARZA,M.A.IZBIZKY,M.NUNEZ REGUEIORO	LA,SR,CU,O	
2145	PRB0365680	LORENTZ NO.=2.45E-8V**2/K**2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1987																												Y123																				90.5					90.5																																																														4.5			THC2145		2.3			TP2145																															THERMAL TRANSPORT PROPERTIES OF Y(1)BA(2)CU(3)O(7) SUPERCONDUCTORS	198710	THERMAL CONDUCTIVITY     ,THERMOPOWER              ,HALL EFFECT              ,RE	MAX-PLANCK-INSTITUT FUR FESTKORPERFORSCHUNG,FEDERAL REPUBLIC OF GERMANY AND PHYSICS DEPARTMENT,THE UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN	PHYS.REV.B,36(1987)5680	A.B.KAISER,C.UHER	Y,BA,CU,O	
2146	SSC0630983		YBa2Cu3O7	Y1.04Ba1.96Cu3O6.8	Y	1.04	Ba	1.96	Cu	3															O	6.8	6.8	1	1987																												Y123																			90	90.6				1	90.6																																																														2.31			THC2146		5.62			TP2146																															STRONG ELECTRON-PHONON COUPLING FROM THERMAL CONDUCTIVITY MEASUREMENTS IN A YBA2CU3O7-TYPE SUPERCONDUCTING COMPOUND				SOLID STATE COMMUN.,63(1987)983	A.JONAS,C.DEWITTE,F.DELANNAY,J-P.ERAUW,J-P.ISSI,J-P.MICHENAUD,J-P.MINET,L.PIRAUX,M.KINANY-ALAOUI,M.LAMBRICHT,V.BAYOT,X.GONZE	Y,BA,CU,O	
2147	PRB0407310	R NOT GO TO ZERO AT 4.2K,TEP HAVE + SIGN CONTRAST TAKAGI ET.AL	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z			1989																												T'																				24					24																																																																			0.96			TP2147																															THERMOELECTRIC POWER OF ND1.85CE0.15CUO4-Y AND PR1.85CE0.15CUO4-Y	198910	THEMOELECTRIC POWER ,RESISTANCE	PHYSICS DIVISION,RESEARCH INSTITUTE OF INDUSTRIAL SCIENCE ANDTECHNOLOGY,POHANG,790-330,KOREA	PHYS.REV.B,40(1989)7310	K.H.HAN,S.H.SALK,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	ND,CE,CU,O,PR	
2148	PRB0407310		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Z	Pr	1.85	Ce	0.15	Cu	1															O	4-Z			1989																												Y123																			7	23					23																																																																			0.12			TP2148																															THERMOELECTRIC POWER OF ND1.85CE0.15CUO4-Y AND PR1.85CE0.15CUO4-Y	198910	THEMOELECTRIC POWER ,RESISTANCE	PHYSICS DIVISION,RESEARCH INSTITUTE OF INDUSTRIAL SCIENCE ANDTECHNOLOGY,POHANG,790-330,KOREA	PHYS.REV.B,40(1989)7310	K.H.HAN,S.H.SALK,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	ND,CE,CU,O,PR	
2149	SSC0681011		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	1	1988																											3	Y123				3.821	3.887	11.666														92					92																																																																			6			TP2500												1.1												NITRATES OF Y,BA,CU	1	CRYO-CHEMICAL TECHNOLOGY					THERMOELECTRIC POWER OF Y(1)BA(2)CU(3)O(X) SUPERCONDUCTORS	198812	THERMO POWER             ,OXYGEN CONTENT	INSTITUTE OF ATOMIC ENERGY MOSCOW	SOLID STATE COMMUN.,68(1988)1011	A.A.SIKOV,E.ZSOLDOS,J.TOTH,M.N.HLOPKIN	Y,BA,CU,O	
2150	SSC0681011		YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	7-Z	6.7	1	1988																											3	Y123				3.822	3.881	11.701														56					56																																																																			22			TP2501												4												NITRATES OF Y,BA,CU	1	CRYO-CHEMICAL TECHNOLOGY					THERMOELECTRIC POWER OF Y(1)BA(2)CU(3)O(X) SUPERCONDUCTORS	198812	THERMO POWER             ,OXYGEN CONTENT	INSTITUTE OF ATOMIC ENERGY MOSCOW	SOLID STATE COMMUN.,68(1988)1011	A.A.SIKOV,E.ZSOLDOS,J.TOTH,M.N.HLOPKIN	Y,BA,CU,O	
2151	SSC0681011		YBa2Cu3O7	Y1Ba2Cu3O6.3	Y	1	Ba	2	Cu	3															O	7-Z	6.3	1	1988																											2	Y123				3.858		11.786																																																																																						200															118												NITRATES OF Y,BA,CU	1	CRYO-CHEMICAL TECHNOLOGY					THERMOELECTRIC POWER OF Y(1)BA(2)CU(3)O(X) SUPERCONDUCTORS	198812	THERMO POWER             ,OXYGEN CONTENT	INSTITUTE OF ATOMIC ENERGY MOSCOW	SOLID STATE COMMUN.,68(1988)1011	A.A.SIKOV,E.ZSOLDOS,J.TOTH,M.N.HLOPKIN	Y,BA,CU,O	
2152	PRB0387160	2*2*0.08MM3,CRES HAS SHALLOW MINIMUM NEAR 150K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1988																												Y123																				91					91																																																																			9.6			TP2152						0.05							0.15																		ANISOTROPIC THERMOPOWER IN SINGLE CRYSTALS OF THE HIGH-Tc SUPERCONDUCTOR Y(1)BA(2)CU(3)O(7)	198810	THERMOPOWER              ,SINGLE CRYSTAL	JOSEPH HENRY LABORATORIES,PRINCETON UNIVERSITY,NEW JERSEY	PHYS.REV.B,38(1988)7160	N.P.ONG,Z.Z.WANG	Y,BA,CU,O	
2153	PR0387160		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1988																												Y123																				92					92																																																																			2.75			TP2153																															Anisotoropic thermopower in single crystals of the high-Tc superconductor YBa2Cu3O7			Joseph Henry Laboratories, Princeton University, Princeton, New Jersey 08544	Phys.Rev.B.,38(1988)7106	N.P. Ong,Z.Z. Wang		
2154	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	Z	6.94		1988																												Y123																				91.7					91.7																																																																			-3.11			TP2154								0.2				0.7																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2155	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	Z	6.85		1988																												Y123																				90.9					90.9																																																																			-2.66			TP2155												1.1																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2156	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	Z	6.65		1988																												Y123																				79.3					79.3																																																																			7.5			TP2156												2.1																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2157	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O	Z	6.55		1988																												Y123																				58.3					58.3																																																																			21.1			TP2157												3.9																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2158	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45		1988																												Y123																				52.5					52.5																																																																			37.4			TP2158												3.3																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2159	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.36	Y	1	Ba	2	Cu	3															O	Z	6.36		1988																												Y123																				8.3					8.3																																																																			72.8			TP2159												3.58																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2160	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6.15	Y	1	Ba	2	Cu	3															O	Z	6.15		1988																												Y123																																																																																												128			TP2160												14.9																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2161	PLA1310203		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	Z	6		1988																												Y123																																																																																												228			TP2161		5300										30.6																			RESISTIVITY AND THERMOELECTRIC POWER IN Y(1)BA(2)CU(3)O(X) SAMPLES WITH DIFFERENT OXYGEN CONTENT	198808	RESISTIVITY              ,THERMOPOWER              ,OXYGEN CONTENT           ,HA	URAL DIVISION OF THE USSR ACADEMY OF SCIENCES,SVERDLOVSK,USSR	PHYS.LETT.A,131(1988)203	A.I.PONOMAREV,G.V.BAZUEV,I.M.TSIDILKOVSKI,K.R.KRYLOV,S.M.CHESHNITSKI,V.I.TSIDILKOVSKI,V.L.KOZHEVNIKOV	Y,BA,CU,O	
2162	PRB0379734	0.75*0.75*0.15MM3,TEP ALONG C-AXIS	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1988																												Y123																				81					81																																																																			7			TP2162																															ANISOTROPIC THERMOELECTRIC POWER AND CONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(Y)	198806	THERMOPOWER              ,ELECTRICAL CONDUCTIVITY  ,SINGLE C	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,AND MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)9734	A.ZETTL,M.F.CROMMIE,MARVIN L.COHEN,T.W.BARBEE III	Y,BA,CU,O	
2163	PRB0379734	TEP ALONG AB-PLANE	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1988																												Y123																				81					81																																																																			13.5			TP2163																															ANISOTROPIC THERMOELECTRIC POWER AND CONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(Y)	198806	THERMOPOWER              ,ELECTRICAL CONDUCTIVITY  ,SINGLE C	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,AND MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)9734	A.ZETTL,M.F.CROMMIE,MARVIN L.COHEN,T.W.BARBEE III	Y,BA,CU,O	
2164	PRB0379734	POLYCRYSTAL	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1988																												Y123																				91					91																																																																			6.3			TP2164																															ANISOTROPIC THERMOELECTRIC POWER AND CONDUCTIVITY IN SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(Y)	198806	THERMOPOWER              ,ELECTRICAL CONDUCTIVITY  ,SINGLE C	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,AND MATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA	PHYS.REV.B,37(1988)9734	A.ZETTL,M.F.CROMMIE,MARVIN L.COHEN,T.W.BARBEE III	Y,BA,CU,O	
2165	PRB0372285		ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	7			1988																												Y123				3.821	3.895	11.705													88.8	91.1	93.2			2.8	91.1																																																																			-3																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2166	PRB0372285		TmBa2Cu3O7	Tm1Ba2Cu3O7	Tm	1	Ba	2	Cu	3															O	7			1988																												Y123				3.844	3.915	11.783													89.4	92.1	94.6			2.5	92.1																																																																			-2.2																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2167	PRB0372285		YbBa2Cu3O7	Yb1Ba2Cu3O7	Yb	1	Ba	2	Cu	3															O	7			1988																												Y123				3.828	3.906	11.746													91.7	96.1	97.8			2.5	96.1																																																																			-4.9			TP2167																															THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2168	PRB0372285		LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7			1988																												Y123				3.797	3.879	11.663													89.8	92.4	95.8			4	92.4																																																																			-4.7																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2169	PRB0372285		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123				3.815	3.891	11.673													92.2	94	95.5			2	94																																																																			-2.7																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2170	PRB0372285		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7			1988																												Y123				3.87	3.893	11.727													61	73	85			12	73																																																																			21.9																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2171	PRB0372285		NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7			1988																												Y123				3.869	3.92	11.78													86	93.5	96.7			5.5	93.5																																																																			8.8																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2172	PRB0372285		EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7			1988																												Y123				3.859	3.914	11.753													70	82.2	86.5			7	82.2																																																																			1.6																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2173	PRB0372285		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1988																												Y123				3.84	3.914	11.743													94.4	95.7	96.6			1.2	95.7																																																																			3.4			TP2173																															THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2174	PRB0372285		DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	7			1988																												Y123				3.834	3.905	11.726													93.4	95.1	96.1			1.3	95.1																																																																			-1.2																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2175	PRB0372285		HoBa2Cu3O7	Ho1Ba2Cu3O7	Ho	1	Ba	2	Cu	3															O	7			1988																												Y123				3.831	3.897	11.7													88.8	91.3	93.5			2.5	91.3																																																																			-2.7																																		THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2176	PRB0368881		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1987																												Y123																				90					90																																																																			10.5			TP2176																															THERMOPOWER OF Y(1)BA(2)CU(3)O(7) AND RELATED SUPERCONDUCTING OXIDES	198712	THERMOPOWER              ,RESISTIVITY	DEPARTMENT,VICTORIA UNIVERSITY OF WELLINGTON,PRIVATE BAG,WELLINGTON,NEW ZEALAND	PHYS.REV.B,36(1987)8881	A.MAWDSLEY,H.J.TRODAHL	Y,BA,CU,O	
2177	SSC0641285	RH300=2.6*E-11 V.CM/A.OE	YBa2Cu3O7	Y1Ba2Cu3O6.88	Y	1	Ba	2	Cu	3															O	6.5+Z	6.88		1987																												Y123				3.824	3.889	11.694														90.6					90.6																																																																			4.2			TP2177												1.05																			NORMAL STATE THERMOPOWER OF THE HIGH TEMPERATURE SUPERCONDUCTOR Y(1)BA(2)CU(3)O(6.5+Z)	198711		INSTITUTE FOR LOW TEMPERATURE AND STRUCTURE RESEARCH,POLISH ACADEMY OF SCIENCES,PL.KATEDRALNY,POLAND	SOLID STATE COMMUN.,64(1987)1285	J.KLAMUT,P.J.MARDOWSKI,R.HORYN,Z.BUKOWSKI,Z.HENKIE	Y,BA,CU,O	
2178	MPL0020923		Tl2Ba2Ca2Cu3O10	Tl2Ca2Ba2Cu3O10	Tl	2	Ca	2	Ba	2	Cu	3													O	10			1988																												Tl2223																			114.9		125				119.95																																																																			2.5			TP2178												10																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER IN TL(2)CA(2)BA(2)CU(3)O(10) AND TL(1)CA(3)BA(1)CU(3)O(9)	8	SYNTHESIS                ,TEP                      ,RES                      ,SU	DEPT.QUIMICA,ICEN-LNETI,P-2686 SACAVE CODEX,PORTUGAL	MOD.PHYS.LETT.B,2(1988)923	A.P.GONCALVES,C.POLITIS,E.B.LOPESH.L.LUO,L.ALCACER,M.ALMEIDA,S.M.GREEN,U.BRAUN	TL,CA,BA,CU,O	
2179	MPL0020923			Th1Ca3Ba1Cu3O9	Th	1	Ca	3	Ba	1	Cu	3													O	9			1988																																															122		127				124.5																																																																			1.75			TP2179												25																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER IN TL(2)CA(2)BA(2)CU(3)O(10) AND TL(1)CA(3)BA(1)CU(3)O(9)	8	SYNTHESIS                ,TEP                      ,RES                      ,SU	DEPT.QUIMICA,ICEN-LNETI,P-2686 SACAVE CODEX,PORTUGAL	MOD.PHYS.LETT.B,2(1988)923	A.P.GONCALVES,C.POLITIS,E.B.LOPESH.L.LUO,L.ALCACER,M.ALMEIDA,S.M.GREEN,U.BRAUN	TL,CA,BA,CU,O	
2180	PR0414002		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1990									5																		3	Y123																				93					93																																																																			6			TP2180												1																			THERMOPOWER OF RBA2CU3O7-X (R=Y,ER)	199003	THERMOPOWER         ,RESISTANCE	PHYSICS DEPARTMENT, TEXAS A&M UNIVERSITY, COLLEGE STATION, TEXAS 77843	PHYS.REV.B,41(1990)4002	A.K.BHATNAGAR,D.G.NAUGLE,G.R.GILBERT,R.K.PANDEY,R.PAN	Y,ER,BA,CU,O	
2181	PR0414002	NON-ZERO BELOW TC BY AG-LEAD	ErBa2Cu3O7	Er1Ba2Cu3OZ	Er	1	Ba	2	Cu	3															O	Z		1	1990									5.8																		3	Y123																				90					90																																																																			5.5			TP2181												3																			THERMOPOWER OF RBA2CU3O7-X (R=Y,ER)	199003	THERMOPOWER         ,RESISTANCE	PHYSICS DEPARTMENT, TEXAS A&M UNIVERSITY, COLLEGE STATION, TEXAS 77843	PHYS.REV.B,41(1990)4002	A.K.BHATNAGAR,D.G.NAUGLE,G.R.GILBERT,R.K.PANDEY,R.PAN	Y,ER,BA,CU,O	
2182	PR0419551		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																			83						83		1	K/GPa	1.5																																																																															0.15	0.006																	HIGH-PRESSURE STYDY OF BI2SR2CACU2O8 SINGLE CRYSTALS	199005		INSTITUTE OF PHYSICS OF THE UNIVERSITY, BIJENICKA CESTA 46, P.O. BOX 304, 41001 ZAGREB, YUGOSLAVIA	PHYS.REV.B,41(1990)9551	B.KESZEI,L.FORRO,V.ILAKOVAC	BI,SR,CA,CU,O	
2183	PR0418757		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7-Z	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z			1990																												Y123																				69					69		3	K/GPa	1																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2184	PR0418757		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O7-Z	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-Z			1990																												Y123																				41					41		3	K/GPa	4																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2185	PR0418757		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7-Z	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7-Z			1990																												Y123																				84					84		3	K/GPa	1																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2186	PR0418757		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.12O7-Z	Y	1	Ba	2	Cu	2.88	Ni	0.12													O	7-Z			1990																												Y123																				78					78		3	K/GPa	1																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2187	PR0418757		YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7-Z	Y	1	Ba	2	Cu	2.88	Co	0.12													O	7-Z			1990																												Y123																				72.5					72.5		3	K/GPa	11																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2188	PR0418757		YBa2(Cu,Cr)3O7	Y1Ba2Cu2.94Cr0.06O7-Z	Y	1	Ba	2	Cu	2.94	Cr	0.06													O	7-Z			1990																												Y123																				84					84		3	K/GPa	2																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2189	PR0418757		YBa2(Cu,Al)3O7	Y1Ba2Cu2.88Al0.12O7-Z	Y	1	Ba	2	Cu	2.88	Al	0.12													O	7-Z			1990																												Y123																				78					78		3	K/GPa	4																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2190	PR0418757		YBa2(Cu,Al)3O7	Y1Ba2Cu2.82Al0.18O7-Z	Y	1	Ba	2	Cu	2.82	Al	0.18													O	7-Z			1990																												Y123																				66					66		3	K/GPa	7																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2191	PR0418757		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z			1990																												Y123																				75					75		3	K/GPa	5																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2192	PR0418757		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.775Fe0.225O7-Z	Y	1	Ba	2	Cu	2.775	Fe	0.225													O	7-Z			1990																												Y123																				59					59		3	K/GPa	8.5																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2193	PR0418757		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8	6.8		1990																												Y123				3.822	3.889	11.712														64					64		3	K/GPa	8																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2194	PR0418757		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																												Y123				3.817	3.885	11.681														89					89		3	K/GPa	-0.1																																																																																																	SUPERCONDUCTIVITY UNDER HIGH PRESSURE OF YBA2(CU1-XMX)3O7-Z(M=FE,CO,AL,CR,NI, AND ZN)	199005		PHYSICS DEPARTMENT, VIRGINIA COMMONWEALTH UNIVERSITY, RICHMOND, VIRGINIA 23284	PHYS.REV.B,41(1990)8757	A.R.VOODENBAUGH,J.G.HUBER,W.J.LIVERMAN,YOUWEN XU	Y,BA,CU,O,FE,CO,AL,CR,NI,ZN	
2195	PR0416655	CURIEC=EMU.K/MOL	PrBa2Cu3O7	Pr1Ba2Cu3O6.93	Pr	1	Ba	2	Cu	3															O	6.93	6.93	1	1990							3																				3	Y123				3.865	3.931	11.725																																																																																						60																																		ROLE OF OXYGEN IN PRBA2CU3O7-Y: EFFECT OF STRUCTURAL AND PHYSICAL PROPERTIES	199004		INSTITUTO DE INVESTIGACIONES EN MATERIALES, UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO, APARTADO POSTAL70-360, MEXICO, DISTRITO FEDERAL, MIXICO	PHYS.REV.B,41(1990)6655	A/BEZINGE,D.RIOS-JARA,E.M.ENGLER,J.TAGUENA,M.E.LOPEZ-MORALES,P.M.GRANT,R.ESCUDERO,S.LA PLACA,V.Y.LII	PR,BA,CU,O	
2196	PR0416655	CURIEC=EMU.K/MOL	PrBa2Cu3O7	Pr1Ba2Cu3O6.6	Pr	1	Ba	2	Cu	3															O	6.6	6.6	1	1990							7																																																																																																																																																			ROLE OF OXYGEN IN PRBA2CU3O7-Y: EFFECT OF STRUCTURAL AND PHYSICAL PROPERTIES	199004		INSTITUTO DE INVESTIGACIONES EN MATERIALES, UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO, APARTADO POSTAL70-360, MEXICO, DISTRITO FEDERAL, MIXICO	PHYS.REV.B,41(1990)6655	A/BEZINGE,D.RIOS-JARA,E.M.ENGLER,J.TAGUENA,M.E.LOPEZ-MORALES,P.M.GRANT,R.ESCUDERO,S.LA PLACA,V.Y.LII	PR,BA,CU,O	
2197	PR0416655	CURIEC=EMU.K/MOL	PrBa2Cu3O7	Pr1Ba2Cu3O6.46	Pr	1	Ba	2	Cu	3															O	6.46	6.46	1	1990							8																																																																																																																																																			ROLE OF OXYGEN IN PRBA2CU3O7-Y: EFFECT OF STRUCTURAL AND PHYSICAL PROPERTIES	199004		INSTITUTO DE INVESTIGACIONES EN MATERIALES, UNIVERSIDAD NACIONAL AUTONOMA DE MEXICO, APARTADO POSTAL70-360, MEXICO, DISTRITO FEDERAL, MIXICO	PHYS.REV.B,41(1990)6655	A/BEZINGE,D.RIOS-JARA,E.M.ENGLER,J.TAGUENA,M.E.LOPEZ-MORALES,P.M.GRANT,R.ESCUDERO,S.LA PLACA,V.Y.LII	PR,BA,CU,O	
2198	PR0416616		YBa2Cu3O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990																											3					3.842	3.871	27.244													78		84				81																																																																																																					BULK SUPERCONDUCTING Y2BA4CU7O15-ZX AND YBA2CU4O8 PREPARDE INOXYGEN AT 1 ATM	199004		PHYSICS AND ENGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC AND INDUSTRIAL RESEARCH, P.O.BOX 31313, LAWER HUTT, NEW ZAALAND	PHYS.REV.B,41(1990)6616	D.M.POOKE,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	Y,BA,CU,O	
2199	PR0416616		Er2Ba4Cu7O15	Er2Ba4Cu7O15-Z	Er	2	Ba	4	Cu	7															O	15-Z		1	1990																											3					3.838	3.867	50.624													80		90				85																																																																																																					BULK SUPERCONDUCTING Y2BA4CU7O15-ZX AND YBA2CU4O8 PREPARDE INOXYGEN AT 1 ATM	199004		PHYSICS AND ENGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC AND INDUSTRIAL RESEARCH, P.O.BOX 31313, LAWER HUTT, NEW ZAALAND	PHYS.REV.B,41(1990)6616	D.M.POOKE,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	Y,BA,CU,O	
2200	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O15	Y	2	Ba	4	Cu	7															O	15-Z	15	1	1990																											3	Y247																					92				92		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2201	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.98	Y	2	Ba	4	Cu	7															O	15-Z	14.98	1	1990																											3	Y247																					88				88		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2202	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.92	Y	2	Ba	4	Cu	7															O	15-Z	14.92	1	1990																											3	Y247																					82				82		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2203	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.85	Y	2	Ba	4	Cu	7															O	15-Z	14.85	1	1990																											3	Y247																					78				78		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2204	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.78	Y	2	Ba	4	Cu	7															O	15-Z	14.78	1	1990																											3	Y247																					70				70		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2205	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.68	Y	2	Ba	4	Cu	7															O	15-Z	14.68	1	1990																											3	Y247																					60				60		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2206	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.46	Y	2	Ba	4	Cu	7															O	15-Z	14.46	1	1990																											3	Y247																					46				46		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2207	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.38	Y	2	Ba	4	Cu	7															O	15-Z	14.38	1	1990																											3	Y247																					50				50		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2208	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.16	Y	2	Ba	4	Cu	7															O	15-Z	14.16	1	1990																											3	Y247																					34				34		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2209	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14.04	Y	2	Ba	4	Cu	7															O	15-Z	14.04	1	1990																											3	Y247																					36				36		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2210	PR0417220		Y2Ba4Cu7O15	Y2Ba4Cu7O14	Y	2	Ba	4	Cu	7															O	15-Z	14	1	1990																											3	Y247																					30				30		2																																																																																																			R2BA4CU7O15-Z: A 92-K BULK SUPERCONDUCTOR	199004		PHYSICS AND INGINEERING LABORATORY, DEPARTMENT OF SCIENTIFIC &INDUSTRIAL RESEARCH, P.O. BOX 31313, LOWER HUTT, NEW ZEALAND	PHYS.REV.B,41(1990)7220	D.M.POOKE,F.J.BLUNT,J.L.TALLON,M.R.PRESLAND,R.G.BUCKLEY	BA,CU,O,Y,ER	
2211	PR0426813		Dy2CuO4	Dy2Cu1O4	Dy	2	Cu	1																	O	4			1990							-22.1																				2																																																																																																																															Magnetic properties of Nd2CuO4-type R2CuO4(R=Y,Dy,Ho,Er,Tm) synthesized under high pressure: Weak ferromagnetism of Y2CuO4	199010		Materials Researchi Laboratory, Kobe Steel, Ltd.,Kobe 651, Japan	Phys.Rev.B,42(1990)6813	Hiroshi Okada,Mikio Takano,Yasuo Takeda		
2212	PR0426813		Ho2CuO4	Ho2Cu1O4	Ho	2	Cu	1																	O	4			1990							-12.2																				2																																																																																																																															Magnetic properties of Nd2CuO4-type R2CuO4(R=Y,Dy,Ho,Er,Tm) synthesized under high pressure: Weak ferromagnetism of Y2CuO4	199010		Materials Researchi Laboratory, Kobe Steel, Ltd.,Kobe 651, Japan	Phys.Rev.B,42(1990)6813	Hiroshi Okada,Mikio Takano,Yasuo Takeda		
2213	PR0426813		Er2CuO4	Er2Cu1O4	Er	2	Cu	1																	O	4			1990							-23.9																				2																																																																																																																															Magnetic properties of Nd2CuO4-type R2CuO4(R=Y,Dy,Ho,Er,Tm) synthesized under high pressure: Weak ferromagnetism of Y2CuO4	199010		Materials Researchi Laboratory, Kobe Steel, Ltd.,Kobe 651, Japan	Phys.Rev.B,42(1990)6813	Hiroshi Okada,Mikio Takano,Yasuo Takeda		
2214	PR0426813		Tm2CuO4	Tm2Cu1O4	Tm	2	Cu	1																	O	4			1990							-20.6																				2																																																																																																																															Magnetic properties of Nd2CuO4-type R2CuO4(R=Y,Dy,Ho,Er,Tm) synthesized under high pressure: Weak ferromagnetism of Y2CuO4	199010		Materials Researchi Laboratory, Kobe Steel, Ltd.,Kobe 651, Japan	Phys.Rev.B,42(1990)6813	Hiroshi Okada,Mikio Takano,Yasuo Takeda		
2215	PHC1680079		Bi2Sr2(Nd,Ce)Cu2O8	Bi2Sr2Nd1.64Ce0.36Cu2O10.23	Bi	2	Sr	2	Nd	1.64	Ce	0.36	Cu	2											O	10.23	10.23	2	1990																											2					3.881		17.93															14				14		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2216	PHC1680079		Bi2Sr2(Sm,Ce)Cu2O8	Bi2Sr2Sm1.64Ce0.36Cu2O10.24	Bi	2	Sr	2	Sm	1.64	Ce	0.36	Cu	2											O	10.24	10.24	2	1990																											2					3.863		17.9															16				16		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2217	PHC1680079		Bi2Sr2(Eu,Ce)Cu2O8	Bi2Sr2Eu1.64Ce0.36Cu2O10.26	Bi	2	Sr	2	Eu	1.64	Ce	0.36	Cu	2											O	10.26	10.26	2	1990																											2					3.854		17.88															27				27		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2218	PHC1680079		Bi2Sr2(Gd,Ce)Cu2O8	Bi2Sr2Gd1.64Ce0.36Cu2O10.24	Bi	2	Sr	2	Gd	1.64	Ce	0.36	Cu	2											O	10.24	10.24	2	1990																											2					3.851		17.88															34				34		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2219	PHC1680079		Bi2Sr2(Dy,Ce)Cu2O8	Bi2Sr2Dy1.64Ce0.36Cu2O10.26	Bi	2	Sr	2	Dy	1.64	Ce	0.36	Cu	2											O	10.26	10.26	2	1990																											2					3.844		17.87															27				27		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2220	PHC1680079		Bi2Sr2(Ho,Ce)Cu2O8	Bi2Sr2Ho1.64Ce0.36Cu2O10.22	Bi	2	Sr	2	Ho	1.64	Ce	0.36	Cu	2											O	10.22	10.22	2	1990																											2					3.84		17.86															24				24		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2221	PHC1680079		Bi2Sr2(Y,Ce)Cu2O8	Bi2Sr2Y1.64Ce0.36Cu2O10.22	Bi	2	Sr	2	Y	1.64	Ce	0.36	Cu	2											O	10.22	10.22	2	1990																											2					3.836		17.85															20				20		2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2222	PHC1680079		Bi2Sr2(Er,Ce)Cu2O8	Bi2Sr2Er1.64Ce0.36Cu2O10.21	Bi	2	Sr	2	Er	1.64	Ce	0.36	Cu	2											O	10.21	10.21	2	1990																											2					3.837		17.84																	5				2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2223	PHC1680079		Bi2Sr2(Tm,Ce)Cu2O8	Bi2Sr2Tm1.64Ce0.36Cu2O10.2	Bi	2	Sr	2	Tm	1.64	Ce	0.36	Cu	2											O	10.2	10.2	2	1990																											2					3.827		17.84																	5				2																																																																																																			EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
2224	PHC1680057		TlBa2CaCu2O7	Tl1Ba2Ca1Cu2O7	Tl	1	Ba	2	Ca	1	Cu	2													O	7		1	1990																											2					3.85		12.76															80				80		1																																																																																																			SUPERCONDUCTIVITY OF HIGH-TC TLBA2CA1-XREXCU2O7(RE=ND,GD OR Y)SYSTEM			INSTITUTE FOR METALS RESEARCH,TOHOKU UNIVERSITY,KATAHIRA,AOBA-KU,SENDAI 980 JAPAN	PHYSICA C,168(1990)57	M.KIKUCHI,N.KOBAYASHI,S.NAKAJIMA,Y.MUTO,Y.SYONO	TL,BA,CA,ND,GD,Y,CU,O	
2225	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.88Ce0.12Cu0.98IN0.02O4-Z	Nd	1.88	Ce	0.12	Cu	0.98	IN	0.02													O	4-Z		1	1990																																															10.7	15.4	21			10.3	15.4		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2226	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.88Ce0.12Cu0.97IN0.03O4-Z	Nd	1.88	Ce	0.12	Cu	0.97	IN	0.03													O	4-Z		1	1990																																															12.2	17	23			10.8	17		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2227	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.88Ce0.12Cu0.96IN0.04O4-Z	Nd	1.88	Ce	0.12	Cu	0.96	IN	0.04													O	4-Z		1	1990																																															2.6	10.5	22			19.4	10.5		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2228	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.87Ce0.13Cu0.98IN0.02O4-Z	Nd	1.87	Ce	0.13	Cu	0.98	IN	0.02													O	4-Z		1	1990																																															17.8	19.5	23.8			6	19.5		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2229	PHC1700211		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1990																												T'																			20.8	22.7	24.8			4	22.7		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2230	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.85Ce0.15Cu0.99IN0.01O4-Z	Nd	1.85	Ce	0.15	Cu	0.99	IN	0.01													O	4-Z		1	1990																																															19.2	20.5	24.3			5.1	20.5		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2231	PHC1700211		(Nd,Ce)2(Cu,In)O4	Nd1.85Ce0.15Cu0.98IN0.02O4-Z	Nd	1.85	Ce	0.15	Cu	0.98	IN	0.02													O	4-Z		1	1990																																															17	19.5	24.3			7.3	19.5		1																																																																																																			THE EFFECT OF INDIUM SUBSTITUTION FOR COPPER ON THE SUPERCONDUCTIVITY OF THE ELECTRON-DOPED SYSTEM ND-CE-CU-O			DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CA92093, USA	PHYSICA C,170(1990)211	C.C.ALMASAN,C.L.SEAMAN,E.A.EARLY,J.T.MARKERT,M.B.MAPLE,N.Y.AYOUB	ND,CE,CU,O	
2232	PR0437955	R30/R273=7.5	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1991																											1	BKBO																			24.5		26.5				25.5																																																																						TP2232												231																			THERMOELECTRIC POWER OF BA1-XKXBIO3	199104		DEPARTMENT OF PHYSICS,UNIVERSITY OF MACHIGAN,ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,43(1991)7955	A.B.KAISER,C.UHER,S.D.PEACOR	BA,K,BI,O	
2233	PR0437955	R30/R273=1.2	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1991																											1	BKBO																			24.5		26.5				25.5																																																																						TP2233												19.1																			THERMOELECTRIC POWER OF BA1-XKXBIO3	199104		DEPARTMENT OF PHYSICS,UNIVERSITY OF MACHIGAN,ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,43(1991)7955	A.B.KAISER,C.UHER,S.D.PEACOR	BA,K,BI,O	
2234	MPL0030295		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1989																											3	Bi2212				5.42	5.44	30.6													85						85																																																																						TP2234																															MEASUREMENT OF ANISOTROPIC THERMOPOWER IN SINGLE CTYSTALS BI2SR2CACU2OY		THERMOPOWER	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	MOD.PHYS.LETT.B,3(1989)295	D.N.ZHENG,G.H.CHEN,J.H.WANG,Q.S.YANG,S.L.JIA,Y.F.YAN,Y.M.NI,Z.X.ZHAO		
2235	IJM0030409	150X150X80MICRO-M 3	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																											3	Y123				3.82	3.89	11.68														92				1.5	92																																																																						TP2235																															THERMOPOWER ANISOTROPY OF YBA2CU3O7-Z SINGLE CRYSTALS			INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,CHINA	INT'L J.MOD.PHYS.B,3(1989)409	DUAN HONG-MIN,LIN SHU-YUAN,LU LI,MA BEI-HAI,ZHANG DIAN-LIN	Y,BA,CU,O	
2236	PHC1621627	HIGHLY ORIENTED CRYSTAL	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123																				91.5					91.5													1490									141									2.2																																																																						CRITICAL MAGNETIC FIELDS(Hc2Hcl)AND k IN YBa2(Cu0.98M0.02)3O7+delta,M=Ni,Al, AND Cu			Material Science Division, Brookhaven National Laboratory, Upton, New York 1973	Physica.C,162-164(1989)1627-1628	A.R. MOODENBAUGH,J.L. PENG,M. SUENAGA,R.N. SHELTON,Youwen XU		
2237	PHC1621627	HIGHLY ORIENTED CRYSTAL	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7		1	1989																											3	Y123																				83.5					83.5													900									140									2.4																																																																						CRITICAL MAGNETIC FIELDS(Hc2Hcl)AND k IN YBa2(Cu0.98M0.02)3O7+delta,M=Ni,Al, AND Cu			Material Science Division, Brookhaven National Laboratory, Upton, New York 1973	Physica.C,162-164(1989)1627-1628	A.R. MOODENBAUGH,J.L. PENG,M. SUENAGA,R.N. SHELTON,Youwen XU		
2238	PHC1621627	HIGHLY ORIENTED CRYSTAL	YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06O7	Y	1	Ba	2	Cu	2.94	Al	0.06													O	7		1	1989																											3	Y123																				87					87													190									150									2.8																																																																						CRITICAL MAGNETIC FIELDS(Hc2Hcl)AND k IN YBa2(Cu0.98M0.02)3O7+delta,M=Ni,Al, AND Cu			Material Science Division, Brookhaven National Laboratory, Upton, New York 1973	Physica.C,162-164(1989)1627-1628	A.R. MOODENBAUGH,J.L. PENG,M. SUENAGA,R.N. SHELTON,Youwen XU		
2239	PHC1621619		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10		1	1989																												Tl2223																				118.5				2	118.5																																3	0.55																																																																				ANISOTROPIC PROPERTIES OF SINGLE CRYSTALS OF (TIO)mBa2Ca2Cu3O8			Sevice National des Champs Intenses, C.N.R.S.,BP 166 X, 38042 Grenoble-Ce'dex, France	Physica.C,162-164(1989)1619-1620	H. NOEL,J. PADIOU,J.C. LEVET,M. POTEL,O. LABORDE,P. GOUGEON,P. MONCEAU		
2240	PHC1621619			Th1Ba2Ca2Cu3OZ	Th	1	Ba	2	Ca	2	Cu	3													O	Z		1	1989																												Tl1223																				114				2	114																																3.7	0.98																																																																				ANISOTROPIC PROPERTIES OF SINGLE CRYSTALS OF (TIO)mBa2Ca2Cu3O8			Sevice National des Champs Intenses, C.N.R.S.,BP 166 X, 38042 Grenoble-Ce'dex, France	Physica.C,162-164(1989)1619-1620	H. NOEL,J. PADIOU,J.C. LEVET,M. POTEL,O. LABORDE,P. GOUGEON,P. MONCEAU		
2241	PHC1520293	GAMMA FROM DHC2DT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				92.2				1.7	92.2																						108									1.72							14.3																			1.12																					3.65																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2242	PHC1520293	GAMMA FROM DHC2DT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90.9				3.3	90.9																						71									1.14							18																			1.33																					2																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2243	PHC1520293	GAMMA FROM DHC2DT	NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91.9				4.2	91.9																						88									1.41							14.4																			1.13																					2.96																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2244	PHC1520293	GAMMA FROM DHC2DT	SmBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90.9				3	90.9																						87									1.41							15.8																			1.35																					2.48																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2245	PHC1520293	GAMMA FROM DHC2DT	EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				93.8				1	93.8																						183									2.86							11																			10																					0.68																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2246	PHC1520293	GAMMA FROM DHC2DT	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				94.2				1.2	94.2																						162									2.52							11.6																			6.72																					0.89																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2247	PHC1520293	GAMMA FROM DHC2DT	DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90				4	90																						92									1.5							15.5																			1.98																					1.8																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2248	PHC1520293	GAMMA FROM DHC2DT	DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91				2.9	91																						62									1							18.8																			0.78																					3.2																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2249	PHC1520293	GAMMA FROM DHC2DT	HoBa2Cu3O7	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				92.7				1	92.7																						153									2.4							12.1																			8.16																					0.7																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2250	PHC1520293	GAMMA FROM DHC2DT	ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				92.2				2.7	92.2																						58									1.01							18.7																			0.47																					5.04																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2251	PHC1520293	GAMMA FROM DHC2DT	ErBa2Cu3O7	Er1Ba2Cu3O7-Z	Er	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				89.3				10	89.3																						46									0.76							21.8																			0.063																					26.3																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2252	PHC1520293	GAMMA FROM DHC2DT	TmBa2Cu3O7	Tm1Ba2Cu3O7-Z	Tm	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91.5				0.8	91.5																						177									2.8							11.3																			3.54																					1.9																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2253	PHC1520293	GAMMA FROM DHC2DT	YbBa2Cu3O7	Yb1Ba2Cu3O7-Z	Yb	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90.1				1.8	90.1																						166									2.7							11.6																			8.67																					0.74																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2254	PHC1520293	GAMMA FROM DHC2DT	LuBa2Cu3O7	Lu1Ba2Cu3O7-Z	Lu	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				90				7.9	90																						50									0.81							21.1																			0.063																					30.2																							UPPER CRITICAL MAGNETIC FIELD MEASUREMENTS IN RBA2CU3O7-Z(R=RARE EARTH) COMPOUNDS				PHYSICA C,152(1988)293	DALICHAOUCH.Y,GUERTIN.R.P,HAKE.R.R,KURIC.M.V,LEE.B.W,MAPLE.M.B,NEUMEIER.J.J,TORIKACHVILI.M.S,YANG.K.N		
2255	PR0437875	RHN=120K	Tl2Ba2CuO6	Tl2Ba2Cu1O6.01	Tl	2	Ba	2	Cu	1															O	6+Z	6.01		1991																																															81						81																																																																																						0.00000000176			0.00000000238		RH2255										TRANSPORT AND MAGNETIC PROPERTIES OF TL2BA2CUO6+Z SHOWING A Z-DEPENDENT GRADUAL TRANSITION FROM AN 85-K SUPERCONDUCTING METAL	199104	TRANSPORT           ,HALL	FUNDAMENTAL RESEACH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,43(1991)7875	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
2256	PR0437875	RHN=120K	Tl2Ba2CuO6	Tl2Ba2Cu1O6.03	Tl	2	Ba	2	Cu	1															O	6+Z	6.03		1991																																															62						62																																																																																						0.00000000136			0.00000000169		RH2256										TRANSPORT AND MAGNETIC PROPERTIES OF TL2BA2CUO6+Z SHOWING A Z-DEPENDENT GRADUAL TRANSITION FROM AN 85-K SUPERCONDUCTING METAL	199104	TRANSPORT           ,HALL	FUNDAMENTAL RESEACH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,43(1991)7875	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
2257	PR0437875	RHN=120K	Tl2Ba2CuO6	Tl2Ba2Cu1O6.05	Tl	2	Ba	2	Cu	1															O	6+Z	6.05		1991																																															47						47																																																																																						0.00000000119			0.00000000147		RH2257										TRANSPORT AND MAGNETIC PROPERTIES OF TL2BA2CUO6+Z SHOWING A Z-DEPENDENT GRADUAL TRANSITION FROM AN 85-K SUPERCONDUCTING METAL	199104	TRANSPORT           ,HALL	FUNDAMENTAL RESEACH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,43(1991)7875	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
2258	PR0437875	RHN=120K	Tl2Ba2CuO6	Tl2Ba2Cu1O6.08	Tl	2	Ba	2	Cu	1															O	6+Z	6.08		1991																																															16						16																																																																																						0.00000000103			0.00000000115		RH2258										TRANSPORT AND MAGNETIC PROPERTIES OF TL2BA2CUO6+Z SHOWING A Z-DEPENDENT GRADUAL TRANSITION FROM AN 85-K SUPERCONDUCTING METAL	199104	TRANSPORT           ,HALL	FUNDAMENTAL RESEACH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,43(1991)7875	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
2259	PR0437875	RHN=120K	Tl2Ba2CuO6	Tl2Ba2Cu1O6.1	Tl	2	Ba	2	Cu	1															O	6+Z	6.1		1991																																																			4.2																																																																																								0.00000000093			0.00000000108		RH2259										TRANSPORT AND MAGNETIC PROPERTIES OF TL2BA2CUO6+Z SHOWING A Z-DEPENDENT GRADUAL TRANSITION FROM AN 85-K SUPERCONDUCTING METAL	199104	TRANSPORT           ,HALL	FUNDAMENTAL RESEACH LABORATORIES,NEC CORPORATION,4-1-1 MIYAZAKI,MIYAMAE-KU,KAWASAKI 213,JAPAN	PHYS.REV.B,43(1991)7875	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
2260	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.95Ce0.05Cu1O3.97	Nd	1.95	Ce	0.05	Cu	1															O	4	3.97		1989																												T'																							4.2																																																																																								-0.00000000425			-0.0000000129												SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2261	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.92Ce0.08Cu1O3.97	Nd	1.92	Ce	0.08	Cu	1															O	4	3.97		1989																												T'				3.948		12.125																	4.2																																																																																								-0.00000000261			-0.00000000543												SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2262	PRL0621197	RHN=80K	(Nd.Ce)2CuO4	Nd1.88Ce0.12Cu1O3.94	Nd	1.88	Ce	0.12	Cu	1															O	4	3.94		1989																												T'				3.945		12.099																	4.2																																																																																								-0.0000000013			-0.00000000333												SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2263	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.86Ce0.14Cu1O3.96	Nd	1.86	Ce	0.14	Cu	1															O	4	3.96		1989																												T'				3.949		12.089														21.3					21.3																																																																																																					SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2264	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.95	Nd	1.85	Ce	0.15	Cu	1															O	4	3.95		1989																												T'				3.947		12.1														22.1					22.1																																																																																						-0.000000000235			-0.000000000783		RH2264										SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2265	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.84Ce0.16Cu1O3.96	Nd	1.84	Ce	0.16	Cu	1															O	4	3.96		1989																												T'				3.948		12.077														16.1					16.1																																																																																						-0.000000000111			-0.0000000003												SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2266	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.83Ce0.17Cu1O4	Nd	1.83	Ce	0.17	Cu	1															O	4			1989																												T'																				9.9					9.9																																																																																																					SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2267	PRL0621197	RHN=80K	(Nd,Ce)2CuO4	Nd1.82Ce0.18Cu1O4	Nd	1.82	Ce	0.18	Cu	1															O	4			1989																												T'																																																																																																																														SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2268	PR0437866			Pb1Sr4Y1Cu5OZ	Pb	1	Sr	4	Y	1	Cu	5													O	Z		1	1991																											2	Pb1212				3.814		11.796																	4.2																																																																																																							SYNTHESIS AND CHARACTERIZATION OF THE SUPERCONDUVTING CUPTATES(PB,CU)SR2(Y,CA)CU2OZ	199104		SUPERCONDUCTIVITY RESEACH LABORATORY,ISTEC,10-13,SINONOME 1-CYOME,KOTO-KU,YOKYO135,LAPAN	PHYS.REV.B,43(1991)7866	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,SR,Y,CA,CU,O	
2269	PR0437866			Pb1.3Sr4Y1.4Ca0.6Cu4.7OZ	Pb	1.3	Sr	4	Y	1.4	Ca	0.6	Cu	4.7											O	Z		2	1991																											2	Pb1212				3.817		11.854														22					22																																																																																																					SYNTHESIS AND CHARACTERIZATION OF THE SUPERCONDUVTING CUPTATES(PB,CU)SR2(Y,CA)CU2OZ	199104		SUPERCONDUCTIVITY RESEACH LABORATORY,ISTEC,10-13,SINONOME 1-CYOME,KOTO-KU,YOKYO135,LAPAN	PHYS.REV.B,43(1991)7866	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,SR,Y,CA,CU,O	
2270	PR0437866			Pb1.35Sr4Y1.3Ca0.7Cu4.65OZ	Pb	1.35	Sr	4	Y	1.3	Ca	0.7	Cu	4.65											O	Z		2	1991																											2	Pb1212				3.817		11.864														41					41																																																																																																					SYNTHESIS AND CHARACTERIZATION OF THE SUPERCONDUVTING CUPTATES(PB,CU)SR2(Y,CA)CU2OZ	199104		SUPERCONDUCTIVITY RESEACH LABORATORY,ISTEC,10-13,SINONOME 1-CYOME,KOTO-KU,YOKYO135,LAPAN	PHYS.REV.B,43(1991)7866	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,SR,Y,CA,CU,O	
2271	PR0437866			Pb1.4Sr4Y1.2Ca0.8Cu4.6OZ	Pb	1.4	Sr	4	Y	1.2	Ca	0.8	Cu	4.6											O	Z		2	1991																												Pb1212																				52					52																																																																																																					SYNTHESIS AND CHARACTERIZATION OF THE SUPERCONDUVTING CUPTATES(PB,CU)SR2(Y,CA)CU2OZ	199104		SUPERCONDUCTIVITY RESEACH LABORATORY,ISTEC,10-13,SINONOME 1-CYOME,KOTO-KU,YOKYO135,LAPAN	PHYS.REV.B,43(1991)7866	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,SR,Y,CA,CU,O	
2272	PHC1710243		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1990																											3	Y123																				92.5					92.5																																																					SP2272				1.95		405																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2273	PHC1710243		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7		1	1990																											3	Y123																				79.5					79.5																																																					SP2273				5.2		405																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2274	PHC1710243		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7		1	1990																											3	Y123																				56					56																																																					SP2274				12.35		403																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2275	PHC1710243		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7		1	1990																											3	Y123																				43.5					43.5																																																					SP2275				14.3		403																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2276	PHC1710243		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O7	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	7		1	1990																											3	Y123																				27					27																																																					SP2276				17.55		395																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2277	PHC1710243		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O7	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	7		1	1990																											3	Y123																				19					19																																																					SP2277				19.5		381																																										THE ELECTRONIC SPECIFIC HEAT OF YBA2(CU1-ZNX)3O7 FROM 1.6 K TO300 K		SPECIFIC HEAT       ,DENSITY OF STATES	IRC IN SUPERCONDUCTIVITY, MADINGLEY ROAD, CAMBRIDGE CB3 OHE,UK	PHYSICA C,171(1990)243	J.W.LORAM,K.A.MIRZA,P.F.FREEMAN	Y,BA,CU,ZN,O	
2278	JJP0271631		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3OZ	Tl	2	Ba	2	Ca	2	Cu	3													O	Z			1988																											2	Tl2223				5.45		35.59														114					114													500									100									1.3							18					1400																																																										Upper and Lower Critical Fields of High-Tc Tl-Ba-Ca-Cu-O System	198809		Institute for Materials Research, Tohoku University, Katahira, sendai 980	Jpn.J.Appl.Phys,27(1988)L1631-L1633	Hideo IWASAKI,Koshichi NOTO,Masae KIKUCHI,Norio KOBAYASHI,Yasuhiko SYONO,Yoji KOIKE,Yoshio MUTO		
2279	APJ0300474		Y2Ba4Cu7O15	Y2Ba4Cu7O15-Z	Y	2	Ba	4	Cu	7															O	15-Z		1	1991																																																41					41																																																																																																					Effect of Annealing Conditions on the Tc of the Y2Ba4Cu7O15-x Superconductor	3		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135	Jpn.J.Appl.Phys.30(1991)474-475	Hirohiko Murakami,Seiji Yaegahi,Shoji Tanaka,Yuh Shiohara		
2280	APJ0300474		Y2Ba4Cu7O15	Y2Ba4Cu7O15-Z	Y	2	Ba	4	Cu	7															O	15-Z		1	1991																																																66					66																																																																																																					Effect of Annealing Conditions on the Tc of the Y2Ba4Cu7O15-x Superconductor	3		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135	Jpn.J.Appl.Phys.30(1991)474-475	Hirohiko Murakami,Seiji Yaegahi,Shoji Tanaka,Yuh Shiohara		
2281	APJ0300474		Y2Ba4Cu7O15	Y2Ba4Cu7O15-Z	Y	2	Ba	4	Cu	7															O	15-Z		1	1991																																																75					75																																																																																																					Effect of Annealing Conditions on the Tc of the Y2Ba4Cu7O15-x Superconductor	3		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135	Jpn.J.Appl.Phys.30(1991)474-475	Hirohiko Murakami,Seiji Yaegahi,Shoji Tanaka,Yuh Shiohara		
2282	APJ0300474		Y2Ba4Cu7O15	Y2Ba4Cu7O15-Z	Y	2	Ba	4	Cu	7															O	15-Z		1	1991																																																82					82																																																																																																					Effect of Annealing Conditions on the Tc of the Y2Ba4Cu7O15-x Superconductor	3		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135	Jpn.J.Appl.Phys.30(1991)474-475	Hirohiko Murakami,Seiji Yaegahi,Shoji Tanaka,Yuh Shiohara		
2283	APJ0300472			Dy0.35Ba0.65Cu1O3-Z	Dy	0.35	Ba	0.65	Cu	1															O	3-Z		1	1991									5.2																		3	Y123				3.821	3.876	11.629													92		106.5				99.25																																																																																																					SUPERCONDUCTIVITY IN PB2+ DOPED DY-BA-CUO SYSTEM	3			JAPANESE J.APPL.PHYS.30(1991)472	A.BHANUMATHI,K.LINGA MURTY,K.UMAKANTHAM,S.NARAYAMA MURTY		
2284	APJ0300472			Dy0.35Ba0.65Pb0.1Cu0.9O3-Z	Dy	0.35	Ba	0.65	Pb	0.1	Cu	0.9													O	3-Z		1	1991									6.1																		3	Y123				3.813	3.887	11.662													80		100.5				90.25																																																																																																					SUPERCONDUCTIVITY IN PB2+ DOPED DY-BA-CUO SYSTEM	3			JAPANESE J.APPL.PHYS.30(1991)472	A.BHANUMATHI,K.LINGA MURTY,K.UMAKANTHAM,S.NARAYAMA MURTY		
2285	PHC1720131	HALL=H PARALLEL C-AXIS	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1990																											3	Y123																			85.5					0.7	85.5																																																																																		0.27				0.0000000011					RH2285										COMPARISON OF HALL EFFECT NEAR TC IN YBCO 123 SINGLE CRYSTAL AND 124 CERAMICS			DEPARTEMENT DE LA PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITEDE GENEVE, CH-1211 GENEVE, CH-1211 GENEVE 4, SWITZERLAND	PHYSICA C,172(1990)131	M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF,W.SADOWSKI	Y,BA,CU,O	
2286	PHC1720131		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990									5.8																		3	Y124	AMMM			3.84	3.87	27.227															79.6			2.5	79.6																																																																																		0.42									RH2286										COMPARISON OF HALL EFFECT NEAR TC IN YBCO 123 SINGLE CRYSTAL AND 124 CERAMICS			DEPARTEMENT DE LA PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITEDE GENEVE, CH-1211 GENEVE, CH-1211 GENEVE 4, SWITZERLAND	PHYSICA C,172(1990)131	M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF,W.SADOWSKI	Y,BA,CU,O	
2287	PHC1560027		(Ba,K)BiO3	Ba0.65K0.35Bi1O3	Ba	0.65	K	0.35	Bi	1															O	3			1988																																																27				10	27										25																																																																																											THE UPPER CRITICAL FIELD OF BA1-XKXBIO3				PHYSICA C,156(1988)27	CLAUS.H,CRABTERR.G.W,DABROWSKI.B,HINKS.D.G,KWOK.W.K,MARX.D.T,MITCHELL.A.W,RICHARDS.D.R,VANDERVOORT.K.G,WELP.U		
2288	PHC1560027		(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3			1988																																																27.7				7.5	27.7										85												21									0.86																																																																						THE UPPER CRITICAL FIELD OF BA1-XKXBIO3				PHYSICA C,156(1988)27	CLAUS.H,CRABTERR.G.W,DABROWSKI.B,HINKS.D.G,KWOK.W.K,MARX.D.T,MITCHELL.A.W,RICHARDS.D.R,VANDERVOORT.K.G,WELP.U		
2289	PHC1560027	RE-ENTRANT BEHAVIOR BELOW 9K AT H=0.25,I=1MA	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1988																																																28				2.6	28										60												16									0.63																																																																						THE UPPER CRITICAL FIELD OF BA1-XKXBIO3				PHYSICA C,156(1988)27	CLAUS.H,CRABTERR.G.W,DABROWSKI.B,HINKS.D.G,KWOK.W.K,MARX.D.T,MITCHELL.A.W,RICHARDS.D.R,VANDERVOORT.K.G,WELP.U		
2290	PHC1560027		(Ba,K)BiO3	Ba0.55K0.45Bi1O3	Ba	0.55	K	0.45	Bi	1															O	3			1988																																																25.6				1.7	25.6										35												11									0.52																																																																						THE UPPER CRITICAL FIELD OF BA1-XKXBIO3				PHYSICA C,156(1988)27	CLAUS.H,CRABTERR.G.W,DABROWSKI.B,HINKS.D.G,KWOK.W.K,MARX.D.T,MITCHELL.A.W,RICHARDS.D.R,VANDERVOORT.K.G,WELP.U		
2291	PR0416582		(Nd,Th)2CuO4	Nd1.85Th0.15Cu1O4	Nd	1.85	Th	0.15	Cu	1															O	4		1	1990																											2					3.952		12.11															22.5				22.5																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2292	PR0416582		(Nd,La,Th)2CuO4	Nd1.55La0.3Th0.15Cu1O4	Nd	1.55	La	0.3	Th	0.15	Cu	1													O	4		1	1990																											2					3.961		12.16															22				22																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2293	PR0416582		(Nd,La,Th)2CuO4	Nd1.25La0.6Th0.15Cu1O4	Nd	1.25	La	0.6	Th	0.15	Cu	1													O	4		1	1990																											2					3.97		12.22															18				18																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2294	PR0416582		(Nd,La,Th)2CuO4	Nd0.95La0.9Th0.15Cu1O4	Nd	0.95	La	0.9	Th	0.15	Cu	1													O	4		1	1990																											2					3.981		12.26															16				16																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2295	PR0416582		(Nd,La,Th)2CuO4	Nd0.85La1Th0.15Cu1O4	Nd	0.85	La	1	Th	0.15	Cu	1													O	4		1	1990																											2					3.984		12.28															16				16																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2296	PR0416582		(Eu,La,Ce)2CuO4	Eu1.55La0.3Ce0.15Cu1O4	Eu	1.55	La	0.3	Ce	0.15	Cu	1													O	4		1	1990																											2					3.923		11.93															10				10																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2297	PR0416582		(Eu,La,Ce)2CuO4	Eu1.25La0.6Ce0.15Cu1O4	Eu	1.25	La	0.6	Ce	0.15	Cu	1													O	4		1	1990																											2					3.938		12.02															15				15																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2298	PR0416582		(Eu,La,Ce)2CuO4	Eu0.95La0.9Ce0.15Cu1O4	Eu	0.95	La	0.9	Ce	0.15	Cu	1													O	4		1	1990																											2					3.952		12.1															17.5				17.5																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2299	PR0416582		(Eu,La,Ce)2CuO4	Eu0.85La1Ce0.15Cu1O4	Eu	0.85	La	1	Ce	0.15	Cu	1													O	4		1	1990																											2					3.958		12.14															15				15																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2300	PR0416582		(Eu,La,Ce)2CuO4	Eu0.65La1.2Ce0.15Cu1O4	Eu	0.65	La	1.2	Ce	0.15	Cu	1													O	4		1	1990																											2					3.97		12.2															11				11																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2301	PR0416582		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1990																											2	T'				3.944		12.09															24				24																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2302	PR0416582		(Nd,La,Ce)2CuO4	Nd1.55La0.3Ce0.15Cu1O4	Nd	1.55	La	0.3	Ce	0.15	Cu	1													O	4		1	1990																											2					3.954		12.12															25.2				25.2																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2303	PR0416582		(Nd.La,Ce)2CuO4	Nd1.25La0.6Ce0.15Cu1O4	Nd	1.25	La	0.6	Ce	0.15	Cu	1													O	4		1	1990																											2					3.963		12.16															23				23																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2304	PR0416582		(Nd,La,Ce)2CuO4	Nd0.95La0.9Ce0.15Cu1O4	Nd	0.95	La	0.9	Ce	0.15	Cu	1													O	4		1	1990																											2					3.972		12.22															22				22																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2305	PR0416582		(Nd,La,Ce)2CuO4	Nd0.85La1Ce0.15Cu1O4	Nd	0.85	La	1	Ce	0.15	Cu	1													O	4		1	1990																											2					3.978		12.25															15				15																																																																																																					CATIONIC SUBSTITUTION AND ROLE OF OXYGEN IN THE N-TYPE SUPERCONDUCTING T' SYSTEM ND2-YCEYCUOZ	199004		BELLCORE, 331 NEWMAN SPRINGS ROAD, RED BAND, NEW JERSEY 07701	PHYS.REV.B,41(1990)6582	E.WANG,G.W.HULL,J.-M.TARASCON,L.H.GREENE,W.R.MCLINNON	ND,CE,CU,O	
2306	PHC1620476	KAI=EMU/G	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1989		-17340000000000000000000000																										Tl2201																																																																																				238																																										SPECIFIC HEAT (1-330K), MAGNETIC SUSCEPTIBILITY AND MEISSNER EFFECT OF Tl-Ba-Ca-Cu-O SAMPLES			Departement de physique de la matiere condense'e, Universite' de Gene've, CH-1211 Gene've 4, Switzerland	Physica.C,162-164(1989)476-477	A. JUNOD,D. ECKERT,G. TRISCONE,J. MULLER,V.Y. LEE		
2307	PHC1620476	KAI=EMU/G,GAMMA<6.8	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+Z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+Z		1	1989																												Tl2212																				106				8.8	106										51																																																	254																																										SPECIFIC HEAT (1-330K), MAGNETIC SUSCEPTIBILITY AND MEISSNER EFFECT OF Tl-Ba-Ca-Cu-O SAMPLES			Departement de physique de la matiere condense'e, Universite' de Gene've, CH-1211 Gene've 4, Switzerland	Physica.C,162-164(1989)476-477	A. JUNOD,D. ECKERT,G. TRISCONE,J. MULLER,V.Y. LEE		
2308	PHC1620476	KAI=EMU/G	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z		2	1989																												Tl2223																				129				9.8	129										24																																																	290																																										SPECIFIC HEAT (1-330K), MAGNETIC SUSCEPTIBILITY AND MEISSNER EFFECT OF Tl-Ba-Ca-Cu-O SAMPLES			Departement de physique de la matiere condense'e, Universite' de Gene've, CH-1211 Gene've 4, Switzerland	Physica.C,162-164(1989)476-477	A. JUNOD,D. ECKERT,G. TRISCONE,J. MULLER,V.Y. LEE		
2309	PRB0397347		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1989																												Y124				3.84	3.87	27.231														80.4					80.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2310	PRB0397347		SmBa2Cu4O8	Sm1Ba2Cu4O8	Sm	1	Ba	2	Cu	4															O	8		2	1989																												Y124				3.872	3.886	27.308														69.3					69.3																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2311	PRB0397347		EuBa2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		2	1989																												Y124				3.865	3.884	27.279														68.9					68.9																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2312	PRB0397347		GdBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8		2	1989																												Y124				3.863	3.881	27.259														73.4					73.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2313	PRB0397347		DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		1	1989																												Y124				3.846	3.873	27.237														77.2					77.2																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2314	PHC1650251		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1990																												T'																				19.5					19.5													133									5.1									0.38																																																																						MAGNETIC PROPERTIES OF LN2-XCEXCUO4-Z(LN=ND,PR,SM) IN THE SUPERCONDUCTING AND NORMAL-CONDUCTING STATE			PHYSIKALISCHES INSTITUTE, UNIVERSITAT ERLANGEN, 8520 ERLANGEN,FED.TEP. GERMANY	PHYSICA C,165(1990)251	G.SAEMANN-ISCHENKO,H.-W.NEUMULLER,J.P.STROBEL,M.KLAUDA,M.LIPPERT,W.GERHAUSER	ND,PR,SM,CE,CU,O	
2315	PRB0397347		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.84	3.87	27.221														77.4					77.4																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2316	PRB0397347		ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.837	3.869	27.23														78.3					78.3																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2317	PRB0397347		TmBa2Cu4O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8		1	1989																											3	Y124				3.827	3.864	27.18														78.6					78.6																																																																																																					EIGHT NEW HIGH-TEMPERATURE SUPERCONDUCTORS WITH THE 1:2:4 STRUCTURE	198904	TC                  ,SUS                 ,COMPOUNDS           ,NEW PHASE           ,STOICHIOMETRY	PHYSICS DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B.,39(1989)7347	DONALD E.MORRIS,JANICE H.NICKEL,JEFFREY S.SCOTT,JOHN Y.T.WEI,NAGGI G.ASMAR	ND,SM,BA,CU,O,R	
2318	PHC1590195	E-PH COUPLING CONST.=2.8,KAIZERO=EMU/MOLE	SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7		1	1989							38																				3	Y123				3.853	3.908	11.73														88.1				3.3	88.1										42			580									137																9					680																																																										MAGNETIC CHARACTERISTICS OF NORMAL AND SUPERCONDUCTIVE STATES IN SmBa2Cu3O7			Institute of Physics, Chinese Academy of Sciences Beijing, P.O. Box P.R. China	Physica.C,159(1989)195-200	J.Q. ZHENG,N. CAO,W.Y. GUAN,X.S. CHEN		
2319	PRL0621197		(Pr,Ce)2CuO4	Pr1.86Ce0.14Cu1O4-Z	Pr	1.86	Ce	0.14	Cu	1															O	4-Z		1	1989																											2	T'																				20					20																																																																																																					SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2320	PRL0621197		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Z	Pr	1.85	Ce	0.15	Cu	1															O	4-Z		1	1989																											2	T'																				17.8					17.8																																																																																																					SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2321	PRL0621197		(Pr,Ce)2CuO4	Pr1.84Ce0.16Cu1O4-Z	Pr	1.84	Ce	0.16	Cu	1															O	4-Z		1	1989																											2	T'																				12.3					12.3																																																																																																					SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2322	PRL0621197		(Pr,Ce)2CuO4	Pr1.82Ce0.18Cu1O4-Z	Pr	1.82	Ce	0.18	Cu	1															O	4-Z		1	1989																											2	T'																																																																																																																														SUPERCONDUCTIVITY PRODUCED BY ELECTRON DOPING IN CUO2-LAYEREDCOMPOUNDS	198903		ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.LETT.62(1989)1197	H.RAKAGI,S.UCHIDA,Y.TOKURA	ND,CE,CU,O	
2323	NAT3370345		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.93	Nd	1.85	Ce	0.15	Cu	1															O	3.93	3.93	1	1989																											2	T'																				24					24																																																																																						-0.00000000065			-0.0000000023												A superconducting copper oxide compound with electrons as the charge carriers			Department of Physics and Engineering Research Institute, University of Tokyo, Tokyo, Japan	Nature, 337(1989)345	Y.Tokura,H.Takagi,S.Uchida		
2324	NAT3390293		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1989																											2	T'																				22.3					22.3																																																																																																					Anomalous absence of pressure effect on transition temperature in the electron-doped superconductor Nd1.85Ce0.15CuO4-d				Nature 339(1989)293-294	C.Murayama,H.Takagi,N.Mori,S.Uchida,S.Yomo,Y.Tokura		
2325	NAT3390293		(Nd,Ce,Sr)2CuO4	Nd1.3Ce0.2Sr0.15Cu1O4-Z	Nd	1.3	Ce	0.2	Sr	0.15	Cu	1													O	4-Z		1	1989																											2	T'																				23.76					23.76			K/GPa	3																																																																																																	Anomalous absence of pressure effect on transition temperature in the electron-doped superconductor Nd1.85Ce0.15CuO4-d				Nature 339(1989)293-294	C.Murayama,H.Takagi,N.Mori,S.Uchida,S.Yomo,Y.Tokura		
2326	PHC1620957		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.98	Nd	1.85	Ce	0.15	Cu	1															O	3.98	3.98	1	1989																											2	T'																				19.5					19.5													400																		1.5																																																																						PROCESSING AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y(Ln=Pr,Nd,Sm,Eu,Gd;=Ce,Th)			Institute for Pure and Applied Physical Sciences and Department of Physics, University of California, San Diego, La Jolla, CA 92093 USA	Physica.C,162-164(1989)957-958	C.L. Seaman,E.A. Early,J.T. Markert,M.B. Maple,N.Y. Ayoub,P.K. Tsai,T. Bjornholm		
2327	PRB0406739		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																											3	Y123				3.825	3.9	11.66														91					91																																																									17																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2328	PRB0406739		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1989																											3	Y123				3.83	3.905	11.67														67					67																																																									64																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2329	PRB0406739		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1989																											3	Y123				3.83	3.921	11.68														35					35																																																									138																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2330	PRB0406739	NEELT=PR ORDER	(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O7	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1989								6.4																			3	Y123				3.845	3.906	11.69																																																																												180																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2331	PRB0406739	NEELT=PR ORDER	(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O7	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1989								12																			3	Y123				3.852	3.916	11.69																																																																												216																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2332	PRB0406739	NEELT=PR ORDER	PrBa2Cu3O7	Pr1Ba2Ba2Cu3O7	Pr	1	Ba	2	Ba	2	Cu	3													O	7		1	1989								17																			3	Y123				3.873	3.915	11.67																																																																												300																																												MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2333	PR0435430		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95	1	1991																											3	Y123	PMMM																			92.2				0.7	92.2																																																																																																					LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2334	PR0435430		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.95	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z	6.95	1	1991																											3	Y123	PMMM																			73.3				2.7	73.3																																																									49.4																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2335	PR0435430		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.95	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z	6.95	1	1991																											3	Y123	PMMM																			62.5				3.9	62.5																																																									70.5																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2336	PR0435430		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.95	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z	6.95	1	1991																											3	Y123	PMMM																			45.3				2.8	45.3																																																									40.4																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2337	PR0435430		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O6.95	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z	6.95	1	1991																											3	Y123	PMMM																			9				9.6	9																																																									84.6																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2338	PR0435430		(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O6.95	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7-Z	6.95	1	1991																											3	Y123	PMMM																																																																																	104																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2339	PR0435430		PrBa2Cu3O7	Pr1Ba2Cu3O6.95	Pr	1	Ba	2	Cu	3															O	7-Z	6.95	1	1991																											3	Y123	PMMM																																																																																	94																																												LOW-TEMPERATURE SPECIFIC HEAT OF THE Y1-XPRXBA2CU3O7-Z SISTEM	199103		DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,43(1991)5430	B.W.LEE,G.NIEVA,J.J.NEUMEIER,M.B.MAPLE,S.GHAMATY	Y,PR,BA,CU,O	
2340	PRL0651945	MOSSBAUER,0.1%FE	YBa2Cu3O7	Y1Ba2Cu3O6+Z	Y	1	Ba	2	Cu	3															O	6+Z		1	1990								410																				Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2341	PRL0651945	MOSSBAUER,0.1%FE	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.93Zn0.07O6+Z	Y	1	Ba	2	Cu	2.93	Zn	0.07													O	6+Z		1	1990								270																				Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2342	PRL0651945	MOSSBAUER,0.1%FE	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.87Zn0.13O6+Z	Y	1	Ba	2	Cu	2.87	Zn	0.13													O	6+Z		1	1990								240																				Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2343	PRL0651945	MOSSBAUER,0.1%FE	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.81Zn0.19O6+Z	Y	1	Ba	2	Cu	2.81	Zn	0.19													O	6+Z		1	1990								217																				Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2344	PRL0651945	MOSSBAUER,0.1%FE	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.75Zn0.25O6+Z	Y	1	Ba	2	Cu	2.75	Zn	0.25													O	6+Z		1	1990								148																				Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2345	PRL0651945	MOSSBAUER,0.1%FE	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6+Z	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	6+Z		1	1990																												Y123																																																																																																																														COMPETITION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETISMINCU(2) LAYERS OF Y1-XPRXBA2CU3-YMYOZ,M=FE,CO,ZN	199010	ANTIFERROMAGNETIC   ,PHASE TRANSITION    ,MOSSBAUER	THE RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM 91904,ISRAEL	PHYS.REV.LETT.,65(1990)1945	D.HECHEL,E.R.BAUMINGER,I.FELNER,I.NOWID,U.YARON	Y,PR,BA,CU,FE,CO,ZN,O	
2346	PRB0406739		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7.1	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7.1	7.1	1	1989																											2	Y123				3.875		11.68														69					69																																																																																																					MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2347	PRB0406739		(Y,Pr)Ba2(Cu,Fe)3O7	Y0.8Pr0.2Ba2Cu2.7Fe0.3O7.1	Y	0.8	Pr	0.2	Ba	2	Cu	2.7	Fe	0.3											O	7.1	7.1	1	1989																											2	Y123				3.879		11.69														25					25																																																																																																					MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2348	PRB0406739	NEELT=CU(2)	(Y,Pr)Ba2(Cu,Fe)3O7	Y0.6Pr0.4Ba2Cu2.7Fe0.3O7.1	Y	0.6	Pr	0.4	Ba	2	Cu	2.7	Fe	0.3											O	7.1	7.1	1	1989								30																			2	Y123				3.881		11.7																																																																																																																								MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2349	PRB0406739	NEELT=CU(2) ORDER,PR ORDER=5.5K	(Y,Pr)Ba2(Cu,Fe)3O7	Y0.4Pr0.6Ba2Cu2.7Fe0.3O7.1	Y	0.4	Pr	0.6	Ba	2	Cu	2.7	Fe	0.3											O	7.1	7.1	1	1989								230																			2	Y123				3.884		11.7																																																																																																																								MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2350	PRB0406739	NEELT=CU(2) ORDER,PR ORDER=7.5K	(Y,Pr)Ba2(Cu,Fe)3O7	Y0.2Pr0.8Ba2Cu2.7Fe0.3O7.1	Y	0.2	Pr	0.8	Ba	2	Cu	2.7	Fe	0.3											O	7.1	7.1	1	1989								300																			2	Y123				3.909		11.73																																																																																																																								MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2351	PRB0406739	NEELT=CU(2) ORDER,PR ORDER=12K	PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.7Fe3O7.1	Pr	1	Ba	2	Cu	2.7	Fe	3													O	7.1	7.1	1	1989								325																			2	Y123				3.917		11.75																																																																																																																								MAGNETIC ORDER AND SUPERCONDUCTIVITY IN Y1-XPRXBA2CU3O7	198910	MOSSBAUER           ,ANTIFERROMAGNETIC   ,SPECIFIC-HEAT	THE RACAH INSTITUTE OF PHYSICS, THE HEBREW UNIVERSITY OF JERUSALEM, 91904 JERUSALEM, ISRAEL	PHYS.REV.B,40(1989)6739	E. R. BAUMINGER,E. R. YACOBY,G. HILSCHER,I. FELNER,I. NOWIK,N. PILLMAYR,U. YARON,Y. WOLFUS	Y,PR,BA,CU,O,FE	
2352	PHC1580178		Nd2CuO4	Nd2Cu1O3.93	Nd	2	Cu	1																	O	4	3.93	1	1989																											2	T'																																																																														SP2352																																																TWO NEW ELECTRON CUPRATE SUPERCONDUCTORS,PR(1.85)TH(0.15)CUO(4-Y) AND EU(1.85)CE(0.15)CUO(4-Y),AND PROPERTIES OF ND(2-X)CE(X)O(4-Y)	198904	NEW MATERIAL             ,RES                      ,SUS                      ,OXYGEN CONTENT           ,SPECIFIC HEAT	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCE,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CA 92093,USA	PHYSICA C ,158(1989)178	B.W.LEE,C.L.SERMAN,E.A.EARLY,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,R.D.PRICE,S.GHAMATY,T.BJORNHOLM	EU,CE,CU,O,PR,TH,ND	
2353	PHC1580178		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.98	Nd	1.85	Ce	0.15	Cu	1															O	4	3.98	1	1989																											2	T'																																																																														SP2353																																																TWO NEW ELECTRON CUPRATE SUPERCONDUCTORS,PR(1.85)TH(0.15)CUO(4-Y) AND EU(1.85)CE(0.15)CUO(4-Y),AND PROPERTIES OF ND(2-X)CE(X)O(4-Y)	198904	NEW MATERIAL             ,RES                      ,SUS                      ,OXYGEN CONTENT           ,SPECIFIC HEAT	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCE,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CA 92093,USA	PHYSICA C ,158(1989)178	B.W.LEE,C.L.SERMAN,E.A.EARLY,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,R.D.PRICE,S.GHAMATY,T.BJORNHOLM	EU,CE,CU,O,PR,TH,ND	
2354	PHC1580178		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		1	1989																											2	T'																				19				2	19																																																																																																					TWO NEW ELECTRON CUPRATE SUPERCONDUCTORS,PR(1.85)TH(0.15)CUO(4-Y) AND EU(1.85)CE(0.15)CUO(4-Y),AND PROPERTIES OF ND(2-X)CE(X)O(4-Y)	198904	NEW MATERIAL             ,RES                      ,SUS                      ,OXYGEN CONTENT           ,SPECIFIC HEAT	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCE,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CA 92093,USA	PHYSICA C ,158(1989)178	B.W.LEE,C.L.SERMAN,E.A.EARLY,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,R.D.PRICE,S.GHAMATY,T.BJORNHOLM	EU,CE,CU,O,PR,TH,ND	
2355	PHC1580178		(Eu,Ce)2CuO4	Eu1.85Ce0.15Cu1O4	Eu	1.85	Ce	0.15	Cu	1															O	4		1	1989																											2	T'																				8	12.5			6	8																																																																																																					TWO NEW ELECTRON CUPRATE SUPERCONDUCTORS,PR(1.85)TH(0.15)CUO(4-Y) AND EU(1.85)CE(0.15)CUO(4-Y),AND PROPERTIES OF ND(2-X)CE(X)O(4-Y)	198904	NEW MATERIAL             ,RES                      ,SUS                      ,OXYGEN CONTENT           ,SPECIFIC HEAT	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCE,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CA 92093,USA	PHYSICA C ,158(1989)178	B.W.LEE,C.L.SERMAN,E.A.EARLY,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,R.D.PRICE,S.GHAMATY,T.BJORNHOLM	EU,CE,CU,O,PR,TH,ND	
2356	PR0438620	THPOWER300(C)=14UV/K,FIG P=1 FOR AB PLANE,P=2 FOR C-PLANE	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95	3	1991																											3	Y123																				90					90																																																																			10.5			TP2356																															ANISOTROPIC THERMOELECTRIC POWER IN YBA2CU307-X SINGLE CRYSTALS UNDER PRESSURES UP TO 8 GPA	199104	THERMOELECTRIC POWER,SINGLE CRYSTALS     ,PRESSURE	MATERIALS SCIENCE DIVISION,NATIONAL AERONAUTICAL LABORATORY,BANGALORE 560 017,INDIA	PHYS.REV.B,43(1991)8620	ANIL K SINGH,P.MURUGARAJ,SHEELA K.RAMASESHA	Y,BA,CU,O	
2357	PR0438721	FIELD DEPENDENCE OF THC,PCOHERE/NCOHERE=3..5	YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	3	1991																											3	Y123																				92					92																																																																	TC2357																																				EFFECT OF MAGNETIC 0N THERMAL CONDUCTIVITY OF YBA2CU3O7-Z SINGLE CRYSTALS	199104	THERMAL CONDUCTIVITY,MAGNETIC FIELD      ,SINGLE CRYSTALS	DEPARTMENT OF PHYSICS,UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,43(1991)8721	C.UHER,J.L.COHN,S.D.PEACOR	Y,BA,CU,O	
2358	APL0542361	MUON SR	EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7			1989																											3	Y123																				95					95																																											1310																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2359	APL0542361	MUON SR	GdBa2Cu3O7	Gd1Ba2Cu3O6.8	Gd	1	Ba	2	Cu	3															O	7	6.8		1989																											3	Y123																				81					81																																											1770																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2360	APL0542361	MUON SR	GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1989																											3	Y123																				96					96																																											1430																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2361	APL0542361	MUON SR	ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	7			1989																											3	Y123																				92					92																																											1340																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2362	APL0542361	MUON SR	ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	7			1989																											3	Y123																				93					93																																											1400																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2363	APL0542361	MUON SR	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1989																												Bi2212																				82					82																																											1950																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2364	APL0542361	MUON SR	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1989																												Tl2223																				105					105																																											1850																																																										COUPLING STRENGTHS AND FLUX PINNING IN OXIDE SUPERCONDUCTORS	6	MUON SPIN RELAXATION,PENETRATION DEPPTH	TEXAS TECH UNIVERSITY,LUBBOCK,TEXAS 79409	APPL.PHYS.LETT.,54(1989)2361	C.BOEKEMA,D.W.COOKE,K.C.B.CHAN,R.L.LICHTI	Y,BA,CU,O,EU,GD,ER,BI,SR,CA,TL	
2365	TL1590255	TC DEPENDS ON RAW MATERIAL BAO OR BA2O	(Tl,Cd)2Ba2CuO6	Tl1.75Cd0.25Ba2Cu1O6	Tl	1.75	Cd	0.25	Ba	2	Cu	1													O	6			1989																																3.851		23.313														88					88																																																																																																					TL(2-X)CD(X)BA(2)CUO(6+Z):VARIATION OF T(C) WITH CADMIUM SUBSTITUTION	198906	HREM                ,TC                  ,CATION DOPING       ,NEUTRON DIFFRACTION ,STRUCTURE	CENTRAL RESEARCH & DEVELOPMENT DEPARTMENT,E.I.DUPONT DE NEMOURS,EXPERIMENTAL STATION,P.O.BOX 80356,WILMINGTON,DE 19880-0356,USA	PHYSICA C.,159(1989)255	JOHN B.PARISE,MICHAEL K.CRAWFORD,NORMAN HERRON,PRATIBHA L.GAI	TL,CD,BA,CU,O	
2366	PR0428039		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1990																												T'																				18.4					18.4																																																																																																					ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2367	PR0428039	TC OBEY A-G THEORY	(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.999Co0.001O4	Nd	1.85	Ce	0.15	Cu	0.999	Co	0.001													O	4		1	1990																												T'																				15.5					15.5																																																																																																					ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2368	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.998Co0.002O4	Nd	1.85	Ce	0.15	Cu	0.998	Co	0.002													O	4		1	1990																												T'																				14.4					14.4																																																																																																					ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2369	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.996Co0.004O4	Nd	1.85	Ce	0.15	Cu	0.996	Co	0.004													O	4		1	1990																												T'																				9.6					9.6																																																																																																					ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2370	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.994Co0.006O4	Nd	1.85	Ce	0.15	Cu	0.994	Co	0.006													O	4		1	1990																												T'																							3																																																																																																							ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2371	PR0430448	BELOW 120K ORTHORHOMBIC(BMAB),SPIN GLASS BELOW 17K	(La,Sr)2NiO4	La1.8Sr0.2Ni1O4	La	1.8	Sr	0.2	Ni	1															O	4		3	1991																											2		I4/MMM			5.346		12.4																	4.2																																																																																																							MAGNETIC AND STRUCTURAL STUDY OF LA1.8SR0.2NIO4	199101	NEUTRON-DEFFRACTION ,SINGLE CRYSTALS     ,STRUCTURAL PARAMETER,MAGNETIC ORDER	INSTITUT LAUE-LANGEVIN, 156X, 38042 GRENOBLE, FRANCE	PHYS.REV.B,43(1991)448	C.STASSIS,G.H.LANDER,G.HONIG,J.SPALEK,P.GOPALAN,P.J.BROWN	LA,SR,NI,O	
2372	PR0437936	TC VARIES FOR ANNEALING CONDITION,SINGLE PHASE FOR X=<0.5		Pb0.5Sr2Ca0.5Y0.5Cu2.5O7-Z	Pb	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2.5											O	7-Z		1	1991																											2					3.818		11.882														65					65																																																																																																					SUPERCONDUCTIVITY AT 67 K IN (PB,CU)SR2(CA,Y)CU2O7 BY PRECISEADJUDTMENT OF OXYGEN	199104		MORRIS RESEACH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA94704	PHYS.REV.B,43(1991)7936	A.P.B.SINHA,D.E.MORRIS,X.X.TANG	PB,CU,SR,CA,Y,O	
2373	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.99Co0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Co	0.01													O	4		1	1990						9.6	-72																					T'																							3																																																																																																							ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2374	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.98Co0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Co	0.02													O	4		1	1990						6.9	-152																					T'																							3																																																																																																							ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2375	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.95Co0.05O4	Nd	1.85	Ce	0.15	Cu	0.95	Co	0.05													O	4		1	1990						6.52	-133																					T'																							3																																																																																																							ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2376	PR0428039		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.9Co0.1O4	Nd	1.85	Ce	0.15	Cu	0.9	Co	0.1													O	4		1	1990						6.12	-320																					T'																							3																																																																																																							ANNIHILATION OF SUPERCONDUCTIVITY BY CO SUBSTITUTION FOR CU INND1.85CE0.15CUO4	199011	ANTIFERROMAGNETIC   ,PAIR-BREAKING	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8039	H.YAMAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,SHOJI TANAKA,TAKESHI SAKURAI	ND,CE,CU,O	
2377	PR0438686		(Bi,Pb)2Sr2(Y,Ca)Cu2O8	Bi1Pb1Sr2Y0.65Ca0.35Cu2O8	Bi	1	Pb	1	Sr	2	Y	0.65	Ca	0.35	Cu	2									O	8			1991																											3	Bi2212				5.395	5.407	30.35														76					76																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2378	PR0438686		(Bi,Pb)2Sr2(Y,Ca)Cu2O8	Bi1Pb1Sr2Y0.6Ca0.4Cu2O8	Bi	1	Pb	1	Sr	2	Y	0.6	Ca	0.4	Cu	2									O	8			1991																											3	Bi2212				5.391	5.395	30.392														83					83																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2379	PR0438686		(Bi,Pb)2Sr2(Y,Ca)Cu2O8	Bi1Pb1Sr2Y0.5Ca0.5Cu2O8	Bi	1	Pb	1	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	8			1991																											2	Bi2212				5.389		30.44														85					85																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2380	PR0438686		(Bi,Pb)2Sr2(Y,Ca)Cu2O8	Bi1Pb1Sr2Y0.4Ca0.6Cu2O8	Bi	1	Pb	1	Sr	2	Y	0.4	Ca	0.6	Cu	2									O	8			1991																											2	Bi2212				5.389		30.463														79.5					79.5																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2381	PR0438686		(Bi,Pb)2Sr2(Y,Ca)Cu2O8	Bi1Pb1Sr2Y0.3Ca0.7Cu2O8	Bi	1	Pb	1	Sr	2	Y	0.3	Ca	0.7	Cu	2									O	8			1991																											2	Bi2212				5.387		30.535														75					75																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2382	PR0438737	SQUID 20OE,DTCDX=23K/AT%FE	YBa2Cu4O8	Y1Ba2Cu4O8+Z	Y	1	Ba	2	Cu	4															O	8+Z			1991																											3					3.833	3.873	27.19														82					82																																																																																																					SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2383	PR0438737		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8+Z	Y	1	Ba	2	Cu	3.96	Fe	0.04													O	8+Z			1991																											3																					59					59																																																																																																					SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2384	PR0438737		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.9Fe0.1O8+Z	Y	1	Ba	2	Cu	3.9	Fe	0.1													O	8+Z			1991																											3					3.83	3.87	27.131														26					26																																																																																																					SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2385	PR0438737		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8+Z	Y	1	Ba	2	Cu	3.84	Fe	0.16													O	8+Z			1991																											2					3.86		27.08																	4.2																																																																																																							SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2386	PR0438737		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.72Fe0.28O8+Z	Y	1	Ba	2	Cu	3.72	Fe	0.28													O	8+Z			1991								110																			2					3.86		27.08																	4.2																																																																																																							SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2387	PR0438737		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.6Fe0.4O8+Z	Y	1	Ba	2	Cu	3.6	Fe	0.4													O	8+Z			1991								380																			2					3.86		27.08																	4.2																																																																																																							SUPERCONDUCTIVITY AND MAGNETIC ORDER IN THE CU(2) PLANES IN FE-DOPED YBA2CU4O8	199104	MOSSBAUER           ,SUSCEPTIBILITY      ,AUTIFERROMAGNETISM  ,PHASE DIAGRAM	RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)8737	B.BROSH,D.HECHCL,E.R.BAUMINGER,I.FELNER,I.NOWIK	Y,BA,CU,O,FE	
2388	PR0438686		(Bi,Pb)2(Sr,La)2CuO6	Bi1Pb1Sr1.2La0.2Cu1O6	Bi	1	Pb	1	Sr	1.2	La	0.2	Cu	1											O	6			1991																											3					5.288	5.4	24.557														24					24																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2389	PR0438686		(Bi,Pb)2(Sr,La)2CuO6	Bi1Pb1Sr1.26La0.26Cu1O6	Bi	1	Pb	1	Sr	1.26	La	0.26	Cu	1											O	6			1991																											3					5.283	5.409	24.591														26					26																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2390	PR0438686		(Bi,Pb)2(Sr,La)2CuO6	Bi1Pb1Sr1.5La0.5Cu1O6	Bi	1	Pb	1	Sr	1.5	La	0.5	Cu	1											O	6			1991																											3					5.273	5.419	24.662														16.3					16.3																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2391	PR0438686		(Bi,Pb)2(Sr,Pr)2CuO6	Bi1Pb1Sr0.12Pr0.12Cu1O6	Bi	1	Pb	1	Sr	0.12	Pr	0.12	Cu	1											O	6			1991																											3					5.273	5.407	24.207														11					11																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2392	PR0438686		(Bi,Pb)2(Srr,Pr)2CuO6	Bi1Pb1Sr0.2Pr0.2Cu1O6	Bi	1	Pb	1	Sr	0.2	Pr	0.2	Cu	1											O	6			1991																											3					5.268	5.418	24.262														15					15																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2393	PR0438686		(Bi,Pb)2(Sr,Pr)2CuO6	Bi1Pb1Sr0.3Pr0.3Cu1O6	Bi	1	Pb	1	Sr	0.3	Pr	0.3	Cu	1											O	6			1991																											3					5.263	5.433	24.333														14					14																																																																																																					MODULATION-FREE BISMUTH-LEAD CUPRATE SUPERCONDUCTORS:BIPBSR1+XL1-XCUO6 AND BIPBSR2Y1-XCAXCU2O8	199104		SOLID STATE AND STRUCTURAL CHEMISTRY UNIT,INDIAN INSUTITUTE OFSCIENCE,BANGALORE,560 012,INDIA	PHYS.REV.B,43(1991)8686	C.N.R.RAO,J.GOPALAKRISHNAN,V.MANIVANNAN	BI,PB,SR,CU,Y,CA,LA,O	
2394	PHC1590111		(La,Ba)2CuO4	La1.94Ba0.04Cu1O4	La	1.94	Ba	0.04	Cu	1															O	4		1	1989																											2	T																				4					4																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2395	PHC1590111		(La,Ba)2CuO4	La1.922Ba0.078Cu1O4	La	1.922	Ba	0.078	Cu	1															O	4		1	1989																											2	T																				27					27																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2396	PHC1590111	T-O AT 272K,O-T AT 25K,STRUCTURE CHANGE	(La,Ba)2CuO4	La1.906Ba0.094Cu1O4	La	1.906	Ba	0.094	Cu	1															O	4		1	1989																											2	T																				32					32																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2397	PHC1590111		(La,Ba)2CuO4	La1.898Ba0.102Cu1O4	La	1.898	Ba	0.102	Cu	1															O	4		1	1989																											2	T																				29					29																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2398	PHC1590111	T-O AT 206K,O-T AT 68K,STRUCTURE CHANGE	(La,Ba)2CuO4	La1.882Ba0.118Cu1O4	La	1.882	Ba	0.118	Cu	1															O	4		1	1989																											2	T																				9					9																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2399	PHC1590111	T-O AT 137K,O-T AT 68K,STRUCTURE CHANGE	(La,Ba)2CuO4	La1.858Ba0.142Cu1O4	La	1.858	Ba	0.142	Cu	1															O	4		1	1989																											2	T																				29					29																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2400	PHC1590111	T-O AT 94K,O-T AT 25K,STRUCTURE CHANGE	(La,Ba)2CuO4	La1.842Ba0.158Cu1O4	La	1.842	Ba	0.158	Cu	1															O	4		1	1989																											2	T																																																																																																																														STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2401	PHC1590111		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4		1	1989																											3																					21					21																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2402	PHC1590111		(La,Ba)2CuO4	La1.76Ba0.24Cu1O4	La	1.76	Ba	0.24	Cu	1															O	4		1	1989																											3																					14					14																																																																																																					STRUCTURAL PHASE TRANSITION IN (LA(1-X)BA(X))(2)CUO(4-Z)	198906	STRUCTURE                ,XRY                      ,PHASE TRANSITION         ,FERROELASTIC	DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,HIROSHIMA UNIVERSITY,HIROSHIMA 730,JAPAN	PHYSICA C ,159(1989)111	TAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
2403	PHB1651331	F CONC. IS NOMINAL VALUE	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7			1990																												T'																																																																																		40																																												LOW TEMPERATURE SPECIFIC HEAT OF ND2CUO4 AND ND2CUO4-XFX	8		IPCMS, GROUPE DES MATERIAUX INORGANIQUES, EHICS, 1 RUE BLAISEPASCAL, 67008 STRASBOURG CEDEX, FRANCE	PHYSICA B,165(1990)1331	A.TIGHEZA,G.POURROY,M.DRILLON,R.KUENTZLER,Y.DOSSMANN	ND,CU,O,F	
2404	PHB1651331	F CONC. IS NOMINAL VALUE	Nd2Cu(O,F)4	Nd2Cu1F0.4O3.6	Nd	2	Cu	1	F	0.4															O	3.6			1990																												T'																																																																																		30																																												LOW TEMPERATURE SPECIFIC HEAT OF ND2CUO4 AND ND2CUO4-XFX	8		IPCMS, GROUPE DES MATERIAUX INORGANIQUES, EHICS, 1 RUE BLAISEPASCAL, 67008 STRASBOURG CEDEX, FRANCE	PHYSICA B,165(1990)1331	A.TIGHEZA,G.POURROY,M.DRILLON,R.KUENTZLER,Y.DOSSMANN	ND,CU,O,F	
2405	PHB1651331	F CONC. IS NOMINAL VALUE	Nd2Cu(O,F)4	Nd2Cu1F0.5O3.5	Nd	2	Cu	1	F	0.5															O	3.5			1990																												T'																																																																																		42																																												LOW TEMPERATURE SPECIFIC HEAT OF ND2CUO4 AND ND2CUO4-XFX	8		IPCMS, GROUPE DES MATERIAUX INORGANIQUES, EHICS, 1 RUE BLAISEPASCAL, 67008 STRASBOURG CEDEX, FRANCE	PHYSICA B,165(1990)1331	A.TIGHEZA,G.POURROY,M.DRILLON,R.KUENTZLER,Y.DOSSMANN	ND,CU,O,F	
2406	PHB1651331		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4			1990								2.1																				T'																																																																																		50		300																																										LOW TEMPERATURE SPECIFIC HEAT OF ND2CUO4 AND ND2CUO4-XFX	8		IPCMS, GROUPE DES MATERIAUX INORGANIQUES, EHICS, 1 RUE BLAISEPASCAL, 67008 STRASBOURG CEDEX, FRANCE	PHYSICA B,165(1990)1331	A.TIGHEZA,G.POURROY,M.DRILLON,R.KUENTZLER,Y.DOSSMANN	ND,CU,O,F	
2407	PHB1651331		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4			1990								1.6																				T'																																																																																		225		410																																										LOW TEMPERATURE SPECIFIC HEAT OF ND2CUO4 AND ND2CUO4-XFX	8		IPCMS, GROUPE DES MATERIAUX INORGANIQUES, EHICS, 1 RUE BLAISEPASCAL, 67008 STRASBOURG CEDEX, FRANCE	PHYSICA B,165(1990)1331	A.TIGHEZA,G.POURROY,M.DRILLON,R.KUENTZLER,Y.DOSSMANN	ND,CU,O,F	
2408	PHB1651283		SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3			1990									5.11			GPa		190	GPa		118	GPa		180		0.23			812000		1	ABO3																							4.2																																																													690																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2409	PHB1651283		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1990									6.22			GPa		124	GPa		50.1	GPa		78.5		0.24			483400		2	T																				38					38																																																											410																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2410	PHB1651283		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1990									5.69			GPa		92.2	GPa		38.4	GPa		51.2		0.2			424200		3	Y123																				90					90																																																											480																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2411	PHB1651283		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1990									5.35			GPa		38.8	GPa		16.1	GPa		21.9		0.2			284600		2	Bi2212																				74					74																																																											250																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2412	PHB1651283		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1990									5.02			GPa		37.3	GPa		16	GPa		18.6		0.17			282100		2	Bi2212																				80					80																																																											270																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2413	PHB1651283		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OZ	Bi	2	Sr	2	Ca	2	Cu	3													O	Z			1990									4.35			GPa		33.7	GPa		14.3	GPa		17.4		0.18			289400		2	Bi2223																				108					108																																																											280																																										Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
2414	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2OZ	Y	1	Ba	2	Cu	2.8	Co	0.2													O	Z			1988									3.8																		3	Y123				3.86	3.862	11.668														50.2					50.2																																																																																									0.0000000137												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2415	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.75Co0.25OZ	Y	1	Ba	2	Cu	2.75	Co	0.25													O	Z			1988									4.28																		3	Y123				3.862	3.868	11.669														39.3					39.3																																																																																									0.00000001596												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2416	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.725Co0.275OZ	Y	1	Ba	2	Cu	2.725	Co	0.275													O	Z			1988									5.17																		3	Y123				3.86	3.862	11.662														31					31																																																																																									0.00000001396												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2417	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.7Co0.3OZ	Y	1	Ba	2	Cu	2.7	Co	0.3													O	Z			1988									5.36																		3	Y123				3.871	3.878	11.655														23.2					23.2																																																																																									0.0000000127												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2418	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.675Co0.325OZ	Y	1	Ba	2	Cu	2.675	Co	0.325													O	Z			1988									5.33																		3	Y123				3.873	3.884	11.671														7					7																																																																																									0.00000001555												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2419	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.65Co0.35OZ	Y	1	Ba	2	Cu	2.65	Co	0.35													O	Z			1988									5.19																		3	Y123				3.868	3.87	11.646																	4.2																																																																																											0.00000002222												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2420	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.625Co0.375OZ	Y	1	Ba	2	Cu	2.625	Co	0.375													O	Z			1988									5.15																		2	Y123				3.879		11.669																	4.2																																																																																											0.00000002462												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2421	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.6Co0.4OZ	Y	1	Ba	2	Cu	2.6	Co	0.4													O	Z			1988																											2	Y123				3.869		11.869																	4.2																																																																																																							LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2422	PR0430457	COHERE BY MAGNETIC FLUCTUATION,KAIZERO IN CM3/MOLE	(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+Z			1991		-17300																										Bi2212																				91.1					91.1																																							20.4	0.37																																																													MAGNETIC PROPERTIES AND SUPERCONDUCTING-FLUCTUATION DIAMAGNETISM ABOVE TC IN BI2-XPBXSR2CACU2O8+Z(X=0.0,0.1,0.2,0.3,0.5)ANDBI2-XPBXSR2CA2CU3O10+Z(X=0.2,0.25)	199101	SUSCEPTIBILITIES    ,FLUCTUATION         ,ORDER PARAMETER	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS, IOWA STATE UNIVERSITY, AMES, IOWA 50011	PHYS.REV.B,43(1991)457	D.C.JOHNSTON,J.H.CHO,W.C.LEE	BI,PB,SR,CA,CU,O	
2423	PR0430457	COHERE BY MAGNETIC FLUCTUATION,KAIZERO IN CM3/MOLE	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.2Sr2Ca2Cu3O10+Z	Bi	1.8	Pb	0.2	Sr	2	Ca	2	Cu	3											O	10+Z			1991		0																										Bi2223																				103					103																																							18																																																														MAGNETIC PROPERTIES AND SUPERCONDUCTING-FLUCTUATION DIAMAGNETISM ABOVE TC IN BI2-XPBXSR2CACU2O8+Z(X=0.0,0.1,0.2,0.3,0.5)ANDBI2-XPBXSR2CA2CU3O10+Z(X=0.2,0.25)	199101	SUSCEPTIBILITIES    ,FLUCTUATION         ,ORDER PARAMETER	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS, IOWA STATE UNIVERSITY, AMES, IOWA 50011	PHYS.REV.B,43(1991)457	D.C.JOHNSTON,J.H.CHO,W.C.LEE	BI,PB,SR,CA,CU,O	
2424	PR0430457	COHERE BY MAGNETIC FLUCTUATION,KAIZERO IN CM3/MOLE	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.75Pb0.25Sr2Ca2Cu3O10+Z	Bi	1.75	Pb	0.25	Sr	2	Ca	2	Cu	3											O	10+Z			1991																												Bi2223																				108					108																																							11.8																																																														MAGNETIC PROPERTIES AND SUPERCONDUCTING-FLUCTUATION DIAMAGNETISM ABOVE TC IN BI2-XPBXSR2CACU2O8+Z(X=0.0,0.1,0.2,0.3,0.5)ANDBI2-XPBXSR2CA2CU3O10+Z(X=0.2,0.25)	199101	SUSCEPTIBILITIES    ,FLUCTUATION         ,ORDER PARAMETER	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS, IOWA STATE UNIVERSITY, AMES, IOWA 50011	PHYS.REV.B,43(1991)457	D.C.JOHNSTON,J.H.CHO,W.C.LEE	BI,PB,SR,CA,CU,O	
2425	PHC1710031		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7	7	1	1990																											3	Y123				3.82	3.886	11.688														92.1					92.1																																																																																																					RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2426	PHC1710031		(Y,Eu)Ba2Cu3O7	Y0.8Eu0.2Ba2Cu3O7	Y	0.8	Eu	0.2	Ba	2	Cu	3													O	7	7	1	1990																											3	Y123				3.823	3.89	11.697																																																																																																																								RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2427	PHC1710031		(Y,Eu)Ba2Cu3O7	Y0.6Eu0.4Ba2Cu3O7	Y	0.6	Eu	0.4	Ba	2	Cu	3													O	7	7	1	1990																											3	Y123				3.828	3.893	11.696														92.6					92.6																																																																																																					RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2428	PHC1710031		(Y,Eu)Ba2Cu3O7	Y0.4Eu0.6Ba2Cu3O7	Y	0.4	Eu	0.6	Ba	2	Cu	3													O	7	7	1	1990																											3	Y123				3.831	3.895	11.705																																																																																																																								RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2429	PHC1710031		(Y,Eu)Ba2Cu3O7	Y0.2Eu0.8Ba2Cu3O7	Y	0.2	Eu	0.8	Ba	2	Cu	3													O	7	7	1	1990																											3	Y123				3.836	3.896	11.71														93.8					93.8																																																																																																					RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2430	PHC1710031		EuBa2Cu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7	7	1	1990																											3	Y123				3.845	3.905	11.719														95.2					95.2																																																																																																					RAMAN MEASUREMENTS OF Y1-XEUXBA2CU3O7: COMPARISON WITH Y1-XPRXBA2CU307			IBM RESEARCH DIVISION, THOMAS J. WATSON RESEARCH CENTER, P.O.BOX 218, YORKTOWN HEIGHTS, NY 10598, USA	PHYSICA C,171(1990)31	F.H.DACOL,G.BURNS,IN-SANG YANG,J.F.BRINGLEY,S.S.TRAIL	Y,EU,BA,CU,O,PR	
2431	PHC1710093	0.0065HOLES/GPA	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	6.93	6.93	1	1990																		GPa		123							3	Y123				3.818	3.884	11.683														91					91																																																																																																					PRESSURE-INDUCED CHARGE TRANSFER AND DTC/DP IN YBA2CU3O7-X			MATERIALS SCIENCE DIVISION AND SCIENCE AND TECHNOLOGY CENTER FOR SUPERCONDUCTIVITY, ARGONNE NATIONAL LABORATORY, ARGONNE, IL60439, USA	PHYSICA C,171(1990)93	A.P.PAULIKAS,B.DABROWSKI,B.W.VEAL,D.G.HINKS,I.D.BROWN,J.D.JORGENSEN,P.LIGHTFOOT,R.KLEB,SHIYOU PEI	Y,BA,CU,O	
2432	PHC1710093	0.008HOLES/GPA	YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1990																		GPa		112							3	Y123				3.83	3.885	11.709														58					58																																																																																																					PRESSURE-INDUCED CHARGE TRANSFER AND DTC/DP IN YBA2CU3O7-X			MATERIALS SCIENCE DIVISION AND SCIENCE AND TECHNOLOGY CENTER FOR SUPERCONDUCTIVITY, ARGONNE NATIONAL LABORATORY, ARGONNE, IL60439, USA	PHYSICA C,171(1990)93	A.P.PAULIKAS,B.DABROWSKI,B.W.VEAL,D.G.HINKS,I.D.BROWN,J.D.JORGENSEN,P.LIGHTFOOT,R.KLEB,SHIYOU PEI	Y,BA,CU,O	
2433	PHC1660413			Pb0.5Sr2Y1Cu2.5OZ	Pb	0.5	Sr	2	Y	1	Cu	2.5													O	Z			1990																											2	Pb1212																							4.2																																																																																				60																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2434	PHC1660413			Pb0.5Sr1.5Ba0.5Y1Cu2.5OZ	Pb	0.5	Sr	1.5	Ba	0.5	Y	1	Cu	2.5											O	Z			1990																											2	Pb1212																							4.2																																																																																				28																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2435	PHC1660413			Pb0.5Sr1Ba1Y1Cu2.5OZ	Pb	0.5	Sr	1	Ba	1	Y	1	Cu	2.5											O	Z			1990																											2	Pb1212																							4.2																																																																																				18																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2436	PHC1660413			Pb0.5Sr1Ba1Y0.75Ca0.25Cu2.5OZ	Pb	0.5	Sr	1	Ba	1	Y	0.75	Ca	0.25	Cu	2.5									O	Z			1990																											2	Pb1212																			53		70				61.5																																																																																		8																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2437	PHC1660413			Pb0.5Sr1.5Ba0.5Y0.75Ca0.25Cu2.5OZ	Pb	0.5	Sr	1.5	Ba	0.5	Y	0.75	Ca	0.25	Cu	2.5									O	Z			1990																											2	Pb1212																			26		37				31.5																																																																																		17																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2438	PHC1660413			Pb0.5Sr2Y0.75Ca0.25Cu2.5OZ	Pb	0.5	Sr	2	Y	0.75	Ca	0.25	Cu	2.5											O	Z			1990																											2	Pb1212																							4.2																																																																																				34																			SUPERCONDUCTIVITY IN PB-BASED LAYERED COPPER OXIDES, (PB0.5CU0.5)(SR,BA)2(Y,CA)CU2O7		NEW MATERIAL        ,SUBSTITUTION        ,SOLUBILITY          ,STRUCTURE	SUPERCONDUCTIVITY RESEARCH LABRATORY INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KOTO-KU,TOKYO	PHYSICA C,166(1990)413	H,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOHSIHIKO MAEDA,YAMAUCHI	PB,CU,SR,BA,Y,CA,CU,O	
2439	PR0437852	DIAMAG APPEAR BUT NO ZERO RESISTANCE,TETRA(HIGH)-ORTHO(LOW) AT 100K	(La,Sr)2NiO4	La1.8Sr0.2Ni1O4+Z	La	1.8	Sr	0.2	Ni	1															O	4+Z		1	1991																																																			4.2																																																																																																							STRUCTURAL AND TRANSPORT MEASUREMENTS IN LA1.8SR0.2NIO4+Z	199104	LATTICE CONSTANTS   ,RESISTIVITY         ,MAGNETIZATION       ,SINGLE CRYSTALS	DEPARTMENT OF PHYSICS,PURDUE UNIVERSITY,WEST LAFAYETTE,INDIANA47907	PHYS.REV.B,43(1991)7852	C.VENKATRAMAN,G.L.LIEDL,S.A.HOFFMAN,S.M.DURBIN,S.N.EHRLICH	LA,SR,NI,O	
2440	PR0436242		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1991																												Y123																																																																																																												0.15								RH2440										UNUSUAL I/T3 TEMPERATURE DEPENDENCE OF THE HALL CONDUCTIVITY IN YBA2CU3O7-Z	199103		JOSPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JORSEY 08544	PHYS.REV.B,43(1991)6242	D.A.BRAWNER,N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,O	
2441	PR0436242		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1991																												Y123																																																																																																												0.15								RH2441										UNUSUAL I/T3 TEMPERATURE DEPENDENCE OF THE HALL CONDUCTIVITY IN YBA2CU3O7-Z	199103		JOSPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JORSEY 08544	PHYS.REV.B,43(1991)6242	D.A.BRAWNER,N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,O	
2442	PR0436242		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1991																												Y123																																																																																																												0.3								RH2442										UNUSUAL I/T3 TEMPERATURE DEPENDENCE OF THE HALL CONDUCTIVITY IN YBA2CU3O7-Z	199103		JOSPH HENRY LABORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JORSEY 08544	PHYS.REV.B,43(1991)6242	D.A.BRAWNER,N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,O	
2443	PR04310364	ZN PREFERENTIALLY SUBSTITUTE FOR CU(2)	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O	8		1	1991																											3	Y124																				52.2					52.2																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2444	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.94Zn0.06O8	Y	1	Ba	2	Cu	3.94	Zn	0.06													O	8		1	1991																											3	Y124																				39.6					39.6																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2445	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.92Zn0.08O8	Y	1	Ba	2	Cu	3.92	Zn	0.08													O	8		1	1991																											3	Y124																				27.7					27.7																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2446	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.88Zn0.12O8	Y	1	Ba	2	Cu	3.88	Zn	0.12													O	8		1	1991																											3	Y124																				25.7					25.7																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2447	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.7Zn0.3O8	Y	1	Ba	2	Cu	3.7	Zn	0.3													O	8		1	1991																											3	Y124																				22.5					22.5																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2448	PR04310364		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1991																											3	Y124				3.833	3.873	27.19														81.3					81.3																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2449	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O	8		1	1991																											3	Y124																				55.8					55.8																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2450	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.9Zn0.1O8	Y	1	Ba	2	Cu	3.9	Zn	0.1													O	8		1	1991																											3	Y124				3.83	3.869	27.133														25.3					25.3																																																																																																					EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2451	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.8Zn0.2O8	Y	1	Ba	2	Cu	3.8	Zn	0.2													O	8		1	1991																											2	Y124				3.86		27.08																	4.2																																																																																																							EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2452	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.72Zn0.28O8	Y	1	Ba	2	Cu	3.72	Zn	0.28													O	8		1	1991																											2	Y124				3.86		27.08																	4.2																																																																																																							EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2453	PR04310364		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.6Zn0.4O8	Y	1	Ba	2	Cu	3.6	Zn	0.4													O	8		1	1991																											2	Y124				3.86		27.08																	4.2																																																																																																							EFFECTS OF FE AND ZN SUBSTITUTION UPON SUPERCONDUCTIVITY IN YBA2CU4O8	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,91904,ISRAEL	PHYS.REV.43(1991)10364	B.BROSH,I.FELNER	Y,BA,CU,O	
2454	PR0435516		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.12O7+Z	Y	1	Ba	2	Cu	2.88	Ni	0.12													O	7+Z			1991																												Y123																				76.3					76.3																						123									2.3								16.4																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2455	PR0435516		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.82Ni0.18O7+Z	Y	1	Ba	2	Cu	2.82	Ni	0.18													O	7+Z			1991																												Y123																				72.2					72.2																						126									2.5								16.2																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2456	PR0435516		YBa2Cu3O7	Y1Ba2Cu3O7+Z	Y	1	Ba	2	Cu	3															O	7+Z			1991																												Y123																				90.5					90.5																						133									2.1								15.7																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2457	PR0435516		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7+Z	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7+Z			1991																												Y123																				83.5					83.5																						123									2.1								16.4																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2458	PR0435516		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7+Z	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7+Z			1991																												Y123																				68					68																						100									2.1								18.2																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2459	PR0435516		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O7+Z	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7+Z			1991																												Y123																				86					86																						114									1.9								17																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2460	PR0435516		YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06O6	Y	1	Ba	2	Cu	2.94	Al	0.06													O	6			1991																												Y123																				86					86																						148									2.4								14.9																																																														IRREVERSIBILITY REMPERATURES IN SUPERCONDUCTING OXIDES:THE FLUX-LINE-LATTICE MELTING,THE GLASS-LIQUID TRANSITION,OR THE DEPINNING TEMPERATURES	199103		DIVISION OF MATERIALS SCIENCE,BRPOOKHAVEN NATIONAL LABORATORY,UPTOWN,NEW YORK 11973	PHYS.REV.B,(1991)5516	M.SUENAGA,YOUWEN XU		
2461	PHC1740028	ANN(970C, 50h,P(O2)=20 bar) 	(La,Sr)2CaCu2O6	La1.7Sr0.3Ca1Cu2O6	La	1.7	Sr	0.3	Ca	1	Cu	2													O	6			1991																												2126																				34					34																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2462	PHC1740028	ANN(970C, 50h,P(O2)=50 bar)  	(La,Sr)2CaCu2O6	La1.7Sr0.3Ca1Cu2O6	La	1.7	Sr	0.3	Ca	1	Cu	2													O	6			1991																												2126																				44					44																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2463	PHC1740028	ANN(970C, 50h,P(O2)=100 bar)   	(La,Sr)2CaCu2O6	La1.7Sr0.3Ca1Cu2O6	La	1.7	Sr	0.3	Ca	1	Cu	2													O	6			1991																												2126																				50					50																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2464	PHC1740028	ANN(970C, 50h,P(O2)=200 bar)  	(La,Sr)2CaCu2O6	La1.7Sr0.3Ca1Cu2O6	La	1.7	Sr	0.3	Ca	1	Cu	2													O	6			1991																												2126																				54					54																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2465	PHC1740028	ANN(970C, 50h,P(O2)=20 bar)  	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O6	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6		2	1991																												2126				3.82		19.43														27					27																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2466	PHC1740028	ANN(970C, 50h,P(O2)=50 bar)  	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O6	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6		2	1991																												2126																				38					38																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2467	PHC1740028	ANN(970C, 50h,P(O2)=100 bar)  	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O6	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6		2	1991																												2126																				45					45																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2468	PHC1740028	ANN(970C, 50h,P(O2)=200 bar)  	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O6	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6		2	1991																												2126																				53					53																																																																																																					SUPERCONDUCTIVITY IN LA2-XSRXCACU2O6 AT 60 K INVESTIGATION OFDOPING AND HIGH PRESSURE ANNEALING			MORRIS RESEARCH INC.,1918 UNIVERSITY AVE.,BERKELEY,CA 94704,USA	PHYSCA C,174(1991)28	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,X.X.TANG	LA,SR,CA,CU,O	
2469	PHC1680309	SUBSTITUTION OF ALKALINE METAL RESULTS IN THE INCREASE OF TC		Bi2.2Sr1.8Ca1.05Cu1.45Li0.7OZ	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.45	Li	0.7											O	Z		2	1990																											2	Bi2212				5.4		30.82													91						91																																																																																																					LI SUBSTITUTION IN THE BI2SR2CA1CU2O8 SUPERCONDUCTOR		SUBSTITUTION        ,MEISSNER EFFECT     ,ANNEALING	THE INSTITUTE OF SCIENTIFIC AND INDUSTRIAL RESEARCH, OSAKA UNIVERSITY, MIHOGAOKA, IBARAKI, OSAKA 567, JAPAN	PHYSICA C,168(1990)309	KATSUTOKI MITSUI,KIYOSHI OGURA,SHICHIO KAWAI,TAKESHI HORIUCHI,TOMOJI KAWAI	LI,BI,SR,CA,CU,O	
2470	PHC1700015		(La,Sr)2SrCu2O6	La1.9Sr1.1Cu2O6.251	La	1.9	Sr	1.1	Cu	2															O	6+Z	6.251	1	1990																											2	2126				3.856		20.068																	4.2																																																																																																							CARRIER DENSITY DEPENDENCE OF THE TRANSPORT PROPERTIES OF LA2-XSR1+XCU2O6+Y			THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA C,170(1990)15	CHIHO OKADA,TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,SR,CU,O	
2471	PHC1700015		(La,Sr)2SrCu2O6	La1.8Sr1.2Cu2O6.213	La	1.8	Sr	1.2	Cu	2															O	6+Z	6.213	1	1990																											2	2126				3.85		20.074																	4.2																																																																																																							CARRIER DENSITY DEPENDENCE OF THE TRANSPORT PROPERTIES OF LA2-XSR1+XCU2O6+Y			THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA C,170(1990)15	CHIHO OKADA,TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,SR,CU,O	
2472	PHC1700015		(La,Sr)2SrCu2O6	La2Sr1Cu2O6.315	La	2	Sr	1	Cu	2															O	6+Z	6.315		1990																											2	2126				3.86		20.063																	4.2																																																																																																							CARRIER DENSITY DEPENDENCE OF THE TRANSPORT PROPERTIES OF LA2-XSR1+XCU2O6+Y			THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA C,170(1990)15	CHIHO OKADA,TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,SR,CU,O	
2473	PHC1700015		(La,Sr)2SrCu2O6	La1.9Sr1.1Cu2O6.05	La	1.9	Sr	1.1	Cu	2															O	6+Z	6.05	1	1990																											2	2126				3.862		19.949																	4.2																																																																																								0.0000000058															CARRIER DENSITY DEPENDENCE OF THE TRANSPORT PROPERTIES OF LA2-XSR1+XCU2O6+Y			THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI, MINATO-KU, TOKYO 106, JAPAN	PHYSICA C,170(1990)15	CHIHO OKADA,TSUYOSHI TAMEGAI,YASUHIRO IYE	LA,SR,CU,O	
2474	PR04011352	RH FOR AB-PLANE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z		3	1989																											2	Bi2212																			81						81																																																																																			1			0.00000000392					RH2474										VARIABLE HALL COEFFICIENT IN BI2SR2CACU2O8-X ACROSS THE METAL-INSULATOR TRANSITION	198912	HALL COEFFICIENT    ,SINGLE-CRYSTAL      ,OXYGEN CONTENT      ,HALL MOBILITY	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA ATBERKELEY,ANDMATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11352	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
2475	PR04011352	RH FOR AB-PLANE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z		3	1989																											2	Bi2212																				62					62																																																																																			1.8			0.00000000498					RH2475										VARIABLE HALL COEFFICIENT IN BI2SR2CACU2O8-X ACROSS THE METAL-INSULATOR TRANSITION	198912	HALL COEFFICIENT    ,SINGLE-CRYSTAL      ,OXYGEN CONTENT      ,HALL MOBILITY	DEPARTMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA ATBERKELEY,ANDMATERIALS AND CHEMICAL SCIENCES DIVISION,LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,40(1989)11352	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
2476	PRB0402254		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1989																											3	T				3.785	3.818	13.148																	4.2																																																																																								0.00000000445					RH2476										SUPERCONDUCTOR-TO-NONSUPERCONDUCTOR TRANSITION INLA1-XSRX)2CUO4 AS INVESTIGATED BY TRANSPORT AND MAGNETIC MEASUREMENTS	198908	HALL COEFFICIENT    ,SUSCEPTIBILITY      ,RES                 ,SUPER-SEMI TRANSI	ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,YAYOI, BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2254	H.TAKAGI,M.UOTA,S.ISHIBASHI,S.UCHIDA,T.IDO,Y.TOKURA	LA,SR,CU,O	
2477	PRB0402254		(La,Sr)2CuO4	La1.964Sr0.036Cu1O4	La	1.964	Sr	0.036	Cu	1															O	4		1	1989																											3	T				3.783	3.812	13.166																	4.2																																																																																													RH2477										SUPERCONDUCTOR-TO-NONSUPERCONDUCTOR TRANSITION INLA1-XSRX)2CUO4 AS INVESTIGATED BY TRANSPORT AND MAGNETIC MEASUREMENTS	198908	HALL COEFFICIENT    ,SUSCEPTIBILITY      ,RES                 ,SUPER-SEMI TRANSI	ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,YAYOI, BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2254	H.TAKAGI,M.UOTA,S.ISHIBASHI,S.UCHIDA,T.IDO,Y.TOKURA	LA,SR,CU,O	
2478	PRB0402254		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		1	1989																											3	T				3.782	3.809	13.174																	4.2																																																																																													RH2478										SUPERCONDUCTOR-TO-NONSUPERCONDUCTOR TRANSITION INLA1-XSRX)2CUO4 AS INVESTIGATED BY TRANSPORT AND MAGNETIC MEASUREMENTS	198908	HALL COEFFICIENT    ,SUSCEPTIBILITY      ,RES                 ,SUPER-SEMI TRANSI	ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,YAYOI, BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2254	H.TAKAGI,M.UOTA,S.ISHIBASHI,S.UCHIDA,T.IDO,Y.TOKURA	LA,SR,CU,O	
2479	PRB0402254		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1989																											2	T				3.776		13.229														37					37																																																																																											RH2479										SUPERCONDUCTOR-TO-NONSUPERCONDUCTOR TRANSITION INLA1-XSRX)2CUO4 AS INVESTIGATED BY TRANSPORT AND MAGNETIC MEASUREMENTS	198908	HALL COEFFICIENT    ,SUSCEPTIBILITY      ,RES                 ,SUPER-SEMI TRANSI	ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,YAYOI, BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2254	H.TAKAGI,M.UOTA,S.ISHIBASHI,S.UCHIDA,T.IDO,Y.TOKURA	LA,SR,CU,O	
2480	PRB0402254		(La,Sr)2CuO4	La1.774Sr0.226Cu1O4	La	1.774	Sr	0.226	Cu	1															O	4		1	1989																											2					3.767		13.25														19.8					19.8																																																																																						0.000000000312					RH2480										SUPERCONDUCTOR-TO-NONSUPERCONDUCTOR TRANSITION INLA1-XSRX)2CUO4 AS INVESTIGATED BY TRANSPORT AND MAGNETIC MEASUREMENTS	198908	HALL COEFFICIENT    ,SUSCEPTIBILITY      ,RES                 ,SUPER-SEMI TRANSI	ENGINEERING RESEARCH INSTITUTE,UNIVERSITY OF TOKYO,YAYOI, BUNKYO-KU,TOKYO 113,JAPAN	PHYS.REV.B,40(1989)2254	H.TAKAGI,M.UOTA,S.ISHIBASHI,S.UCHIDA,T.IDO,Y.TOKURA	LA,SR,CU,O	
2481	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.2	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.2	1	1991																											2	Bi2212																				65					65																																																																																						0.0000000015															OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2482	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.199	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.199	1	1991																											2	Bi2212																				70					70																																																																																																					OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2483	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.198	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.198	1	1991																											2	Bi2212																				78					78																																																																																						0.00000000283															OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2484	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.196	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.196	1	1991																											2	Bi2212																				85					85																																																																																						0.00000000312															OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2485	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.195	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.195	1	1991																											2	Bi2212																				91					91																																																																																						0.00000000298															OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2486	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.194	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.194	1	1991																											2	Bi2212																				92					92																																																																																						0.00000000278															OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2487	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.118	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.118	1	1991																											2	Bi2212																				91					91																																																																																																					OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2488	PR04310445		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.1	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z	8.1	1	1991																											2	Bi2212																				90					90																																																																																																					OXYGEN-LOSS EFFECTS ON SUPERCONDUCTIVITY OF BI2SR2CACU2OY SISTEM	199105		STEEL RESEACH CENTER,NKK CORPORATION,KAWASAKI 210,JAPAN	PHYS.REV.B,43(1991)10445	A.TOKIWA,K.TERASHIMA,M.NAGOSHI,M.OGITA,M.TACHIKI,T.SUZUKI,Y.FUKUDA,Y.NAKANISHI,Y.SYONO	BI,SR,CA,CU,O	
2489	PR04310489		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1991																											2	T'																				21.6					21.6																																																																																						-0.00000000038					RH2489										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2490	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.998Co0.002O4	Nd	1.85	Ce	0.15	Cu	0.998	Co	0.002													O	4		1	1991																											2	T'																				16.5					16.5																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2491	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.996Co0.004O4	Nd	1.85	Ce	0.15	Cu	0.996	Co	0.004													O	4		1	1991																											2	T'																				11.2					11.2																																																																																											RH2491										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2492	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.995Co0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Co	0.005													O	4		1	1991																											2	T'																				7.3					7.3																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2493	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.994Co0.006O4	Nd	1.85	Ce	0.15	Cu	0.994	Co	0.006													O	4		1	1991																											2	T'																				4.3					4.3																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2494	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.993Co0.007O4	Nd	1.85	Ce	0.15	Cu	0.993	Co	0.007													O	4		1	1991																											2	T'																							2																																																																																																							COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2495	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.99Co0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Co	0.01													O	4		1	1991																											2	T'																							2																																																																																												6	RH2495										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2496	PR04310489		(Nd,Ce)2(Cu,Co)O4	Nd1.85Ce0.15Cu0.98Co0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Co	0.02													O	4		1	1991																											2	T'																							2																																																																																												6	RH2496										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2497	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.999Ni0.001O4	Nd	1.85	Ce	0.15	Cu	0.999	Ni	0.001													O	4		1	1991																												T'																				19.5					19.5																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2498	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.998Ni0.002O4	Nd	1.85	Ce	0.15	Cu	0.998	Ni	0.002													O	4		1	1991																												T'																				17.3					17.3																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2499	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.997Ni0.003O4	Nd	1.85	Ce	0.15	Cu	0.997	Ni	0.003													O	4		1	1991																												T'																				15.3					15.3																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2500	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.996Ni0.004O4	Nd	1.85	Ce	0.15	Cu	0.996	Ni	0.004													O	4		1	1991																												T'																				13.5					13.5																																																																																						-0.00000000028				6	RH2500										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2501	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.995Ni0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Ni	0.005													O	4		1	1991																												T'																				11.2					11.2																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2502	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.994Ni0.006O4	Nd	1.85	Ce	0.15	Cu	0.994	Ni	0.006													O	4		1	1991																												T'																				8.4					8.4																																																																			195																																		COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2503	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.993Ni0.007O4	Nd	1.85	Ce	0.15	Cu	0.993	Ni	0.007													O	4		1	1991																												T'																				5.6					5.6																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2504	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.99Ni0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Ni	0.01													O	4		1	1991																												T'																							2																																																																																								-0.000000000175				6	RH2504										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2505	PR04310489		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.98Ni0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Ni	0.02													O	4		1	1991																												T'																							2																																																																																								-0.00000000012				6	RH2505										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2506	PR04310489		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.996Zn0.004O4	Nd	1.85	Ce	0.15	Cu	0.996	Zn	0.004													O	4		1	1991																												T'																				18.1					18.1																																																																																										6	RH2506										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2507	PR04310489		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.99Zn0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Zn	0.01													O	4		1	1991																												T'																				15.1					15.1																																																																																										6	RH2507										COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2508	PR04310489		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.98Zn0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Zn	0.02													O	4		1	1991																												T'																				8.7					8.7																																																																																																					COMPARISPON OF PARAMAGNETIC- AND NONMAGNETIC-IMPURITY EFFECT ON SUPERCONDUCTIVITY IN ND1.85CE0.15CUO4	199105		SUPERCONDUCTIVITY RESEACH LABORATOTY,INTERNATIONALSUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO135,JAPAN	PHYS.REV.B,43(1991)10489	H.YAMAUCHI,JUN SUGIYAMA,SHINICHI KORIYAMA,SHINYA TOKUONO,SHOJI TANAKA	ZN,ND,CE,CU,O,CO,NA	
2509	PLA1320217	RHN AT 100K,DENS CALCULATED FROM XRD	YBa2(Cu,Co)3O7	Y1Ba2Cu2.975Co0.025OZ	Y	1	Ba	2	Cu	2.975	Co	0.025													O	Z		1	1988									4.08																		3	Y123				3.824	3.889	11.678														90.3					90.3																																																																																									0.00000000406												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2510	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.95Co0.05OZ	Y	1	Ba	2	Cu	2.95	Co	0.05													O	Z		1	1988									4.07																		3	Y123				3.826	3.876	11.665														86.1					86.1																																																																																									0.00000000422												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2511	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.95Co0.05OZ	Y	1	Ba	2	Cu	2.95	Co	0.05													O	Z		1	1988																											3	Y123				3.833	3.872	11.651														84					84																																																																																																					LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2512	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.925Co0.075OZ	Y	1	Ba	2	Cu	2.925	Co	0.075													O	Z		1	1988																											3	Y123				3.853	3.882	11.669														77					77																																																																																																					LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2513	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.9Co0.1OZ	Y	1	Ba	2	Cu	2.9	Co	0.1													O	Z		1	1988									4.04																		3	Y123				3.85	3.87	11.665														70					70																																																																																									0.00000000579												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2514	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.875Co0.125OZ	Y	1	Ba	2	Cu	2.875	Co	0.125													O	Z		1	1988									4.83																		3	Y123				3.851	3.858	11.677														64.3					64.3																																																																																									0.00000000841												LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2515	PLA1320217		YBa2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15OZ	Y	1	Ba	2	Cu	2.85	Co	0.15													O	Z		1	1988																											3	Y123				3.861	3.864	11.865														58.9					58.9																																																																																																					LOCALIZATION EFFECTS IN THE Y(1)BA(2)CU(3-X)CO(X)O(Y) SYSTEM	198810	HALL EFFECT              ,LOCALIZATION             ,XRY                      ,RE	UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI,PR CHINA	PHYS.LETT.A,132(1988)217	QIRUI ZHANG,YITAI QIAN,ZHANCHUEN ZHAO,ZHENHUI HE,ZHUAN XU,ZUYAO CHEN	Y,BA,CU,CO,O	
2516	PR0379401		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123																																																																				1550																																																										Muon depolarization and magnetic field penetration depth in superconducting GdBa2Cu3Ox	6		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B,37(1988)9401	C. Boekema,D.W. Cooke,H. Rempp,J. Oostens,J.A. Flint,J.L. Smith,J.O. Willis,K-C.B. Chan,M. Maez,M.E. Schillaci,R.L. Hutson,R.L. Lichti,R.S. Kwok,S.P. Weathersby		
2517	PR0379401		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7		1	1988																											3	Y123																																																																				1900																																																										Muon depolarization and magnetic field penetration depth in superconducting GdBa2Cu3Ox	6		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B,37(1988)9401	C. Boekema,D.W. Cooke,H. Rempp,J. Oostens,J.A. Flint,J.L. Smith,J.O. Willis,K-C.B. Chan,M. Maez,M.E. Schillaci,R.L. Hutson,R.L. Lichti,R.S. Kwok,S.P. Weathersby		
2518	JJP0270538			Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1988																												Bi2212																				83					83																							812	19								14	0.32						42	1																																																													LARGE ANISOTROPY OF THE UPPER CRITICAL MAGNETIC FIELD IN SINGLE CRYSTAL BI-(SR,CA)-CU-O	198804	SINGLE CRYSTAL           ,HC	NTT LABORATORIES,IBARAKI	JJAP.LETT.,27(1988)L538	MIGAKU ODA,MINORU SUZUKI,TOSHIAKI MURAKAMI,YASUSHI MAEDA,YOSHIKAZU HIDAKA,YOUICHI ENOMOTO	BI,SR,CA,CU,O	
2519	JJP0261921	substrate temp.=800C Films were grown on SrTiO3 by magnetron sputtering.		La1.92Sr0.08Cu1OZ	La	1.92	Sr	0.08	Cu	1															O	Z		4	1987																												T																				19.8					19.8																				T	mid point in the resistive transition		125	24					T/K			6.3	1.2			A			37	7.1																																																													ANISOTROPIC PROPERTIES OF SUPERCONDUCTING (LA(1-X)SR(X))(2)CU(1)O(4) SINGLE-CRYSTAL THIN FILMS	198711	FILM                     ,SINGLE CRYSTAL           ,HC                       ,RE	NTT LABORATORIES,TOKAI,IBARAKI	JJAP.LETT.,26(1987)L1921	KAZUYUKI MORIWAKI,MINORU SUZUKI,TOSHIAKI MURAKAMI,YOUICHI ENOMOTO	LA,SR,CU,O	
2520	JJP0261057		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1987																												Y123																				90.8					90.8																							190	56								3	0.9							10																																																													THE ANISOTROPIC UPPER CRITICAL FIELD OF SINGLE CRYSTAL Y(1)BA(2)CU(3)O(X)		HC                       ,ANISOTROPY	ISSP UNIV. OF TOKYO	JJAP LETT.,26(1987)L1057	H.TAKEI,H.TAKEYA,T.TAMEGAI,Y.IYE		
2521	PR0426172		Pr2CuO4	Pr2Cu1O3.49	Pr	2	Cu	1																	O	3.49	3.49		1990																											3	214S				4.254	3.794	12.005																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2522	PR0426172		Nd2CuO4	Nd2Cu1O3.5	Nd	2	Cu	1																	O	3.50	3.5		1990																											3	214S				4.238	3.768	11.919																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2523	PR0426172		La2CuO4	La2Cu1O4.1	La	2	Cu	1																	O	4.10	4.1		1990																											2	T				4.004		12.546																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2524	PR0426172		La2CuO4	La2Cu1O4.2	La	2	Cu	1																	O	4.20	4.2		1990																											2	T				4.007		12.549																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2525	PR0426172		La2CuO4	La2Cu1O4.33	La	2	Cu	1																	O	4.33	4.33		1990																											2	T				4.009		12.547																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2526	PR0426172		La2CuO4	La2Cu1O4.06	La	2	Cu	1																	O	4.06	4.06		1990																											2	T				3.804		13.152																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2527	PR0426172		La2CuO4	La2Cu1O4.03	La	2	Cu	1																	O	4.03	4.03		1990																											2	T				3.802		13.15																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2528	PR0426172		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4.00	4		1990																											3	T				3.792	3.825	13.17																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2529	PR0426172		Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4.00	4		1990																											2	T'				3.958		12.288																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2530	PR0426172		Nd2CuO4	Nd2Cu1O3.99	Nd	2	Cu	1																	O	3.99	3.99		1990																											2	T'				3.937		12.15																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2531	PR0426172		Sr2CuO4	Sr2Cu1O3	Sr	2	Cu	1																	O	3	3		1990																											3	T				3.906	3.496	12.684																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2532	PR0426172		La2CuO4	La2Cu1O3.67	La	2	Cu	1																	O	3.67	3.67		1990																											2	T				4.278	3.87	12.241																	5																																																																																																							NEW PHASES INDUCED BY HYDROGEN REDUCTION AND BY SUBSEQUENT OXIDATION OF L2CUO4(L=LA,PR,ND,SM,EU,GD)	199010		AMES LABORATORY U.S.DEPARTMENT OF ENERGY AND DEVELOPMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA50011	PHYS.REV.B,42(1990)6172	D.C.JOHNSTON,F.C.CHOU,J.H.CHO,L.L.MILLER	LA,PR,ND,SM,EU,GD,CU,O	
2533	PHC1740071		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1991																											3	Y123				3.838	3.89	11.695														93.5					93.5																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2534	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.95Pr0.05Ba2Cu3O7-Z	Gd	0.95	Pr	0.05	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				88					88																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2535	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3O7-Z	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				76					76																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2536	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.85Pr0.15Ba2Cu3O7-Z	Gd	0.85	Pr	0.15	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.841	3.887	11.678														63					63																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2537	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7-Z	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.841	3.893	11.678														56					56																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2538	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.75Pr0.25Ba2Cu3O7-Z	Gd	0.75	Pr	0.25	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.839	3.894	11.682														51					51																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2539	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.7Pr0.3Ba2Cu3O7-Z	Gd	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.846	3.904	11.687														43.2					43.2																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2540	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.65Pr0.35Ba2Cu3O7-Z	Gd	0.65	Pr	0.35	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				30.4					30.4																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2541	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.6Pr0.4Ba2Cu3O7-Z	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.85	3.905	11.693														16					16																																																																																																					SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2542	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.55Pr0.45Ba2Cu3O7-Z	Gd	0.55	Pr	0.45	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																							4.2																																																																																																							SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2543	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.3Pr0.7Ba2Cu3O7-Z	Gd	0.3	Pr	0.7	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.856	3.898	11.68																	4.2																																																																																																							SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2544	PHC1740071		(Gd,Pr)Ba2Cu3O7	Gd0.1Pr0.9Ba2Cu3O7-Z	Gd	0.1	Pr	0.9	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.864	3.928	11.689																	4.2																																																																																																							SUPERCONDUCTIVITY IN THE (GD1-XPRX)BA2CU307-Z SYSTEM			INSTITUTE OF PHYSICS,JAGELLONIAN UNIVERSITY,REYMONTA 4,30-059CRACOW,POLAND	PHYSICA C174(1991)71	A.BAJOREK,A.SZYTUTA,A.ZYGMUNT,K.BATANDA,K.LATKA,R.KMIEC,R.KRUK,Z.TOMOKOWICZ	GD,PR,BA,CU,O	
2545	PHC1690174		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1990																												Bi2212						30.75														93					93																																																																																		1																			TRANSPORT PROPERTIES OF BI2SR2CACU2OX SINGLE CRYSTALS WITH TC=95 K			INSTITUTE FOR PHYSICAL PROBLEMS, U. KOSYGINA 2, MOSCOW 117334,USSR	PHYSICA C,169(1990)174	A.A.YURGENS,A.V.SAMOILOV,N.V.ZAVARITSKY	BI,SR,CA,CU,O	
2546	PHC1610001	NO-POSITIVE CURVATURE IN HC2 VS T	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																											3	Y123				3.82	3.891	11.679														93					93																																10	1.8																																																																				THE UPPER CRITICAL FIELD OF UNTWINNED YBA2CU3O7-Z CRYSTALS	198910			PHYS.C.161(1989)1	FANG M.M.,GRABTREE G.W.,GRIMSDITCH M.,KWOK W.K.,LIU J.Z.,WELP U.,YOU H.		
2547	MSTEC1		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1990																											3	Y123																				91.5				0.2	91.5			K/GPa	-2.5																																																																																																			TC                  ,PRESSURE DEPENDENCE		MEAS.SCI.TECHNOL.,1(1990)1347		Y,BA,CU,O	
2548	MSTEC1		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1990																											3	Y123																				90					90			K/GPa	-1.1																																																																																																			TC                  ,PRESSURE DEPENDENCE		MEAS.SCI.TECHNOL.,1(1990)1347		Y,BA,CU,O	
2549	PR04310568		(La,Pr)Ba2Cu3O7	La0.8Pr0.2Ba2Cu3O7-Z	La	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				20.5					20.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2550	PR04310568		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O7-Z	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				25.8					25.8																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2551	PR04310568		(Sm,Pr)Ba2Cu3O7	Sm0.8Pr0.2Ba2Cu3O7-Z	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				49.4					49.4																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2552	PR04310568		(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O7-Z	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				47					47																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2553	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7-Z	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				58.5					58.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2554	PR04310568		(Dy,Pr)Ba2Cu3O7	Dy0.8Pr0.2Ba2Cu3O7-Z	Dy	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				66.7					66.7																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2555	PR04310568		(Ho,Pr)Ba2Cu3O7	Ho0.8Pr0.2Ba2Cu3O7-Z	Ho	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				79.5					79.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2556	PR04310568		(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3O7-Z	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				76.5					76.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2557	PR04310568		(Tm,Pr)Ba2Cu3O7	Tm0.8Pr0.2Ba2Cu3O7-Z	Tm	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				81.8					81.8																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2558	PR04310568		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O7-Z	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				82.4					82.4																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2559	PR04310568		(Lu,Pr)Ba2Cu3O7	Lu0.8Pr0.2Ba2Cu3O7-Z	Lu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				75.2					75.2																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2560	PR04310568		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123																				71.7					71.7																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2561	PR04310568	KAIZERO=EMU/MOLE	GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1991	emu/mol	0.00071			myu-B/mol	7.79	-0.4																				3	Y123				3.84	3.899	11.702														91.5					91.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2562	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3O7-Z	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.845	3.899	11.701														73.5					73.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2563	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7-Z	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1991	emu/mol	0.00052			myu-B/mol	7.06	-2.3																				3	Y123				3.85	3.895	11.7														58					58																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2564	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.7Pr0.3Ba2Cu3O7-Z	Gd	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z		1	1991	emu/mol	0.00015			myu-B/mol	6.65	-16.1																				3	Y123				3.857	3.898	11.699														35					35																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2565	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.65Pr0.35Ba2Cu3O7-Z	Gd	0.65	Pr	0.35	Ba	2	Cu	3													O	7-Z		1	1991																											3	Y123				3.859	3.899	11.697														15.5					15.5																																																																																																					SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2566	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.6Pr0.4Ba2Cu3O7-Z	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z		1	1991	emu/mol	0.00045			myu-B/mol	6.27	-4.6																				3	Y123				3.862	3.9	11.698																																																																																																																								SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2567	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.4Pr0.6Ba2Cu3O7-Z	Gd	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z		1	1991	emu/mol	0.00037			myu-B/mol	5.51	-6.3																				3	Y123				3.874	3.898	11.695																																																																																																																								SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2568	PR04310568		(Gd,Pr)Ba2Cu3O7	Gd0.2Pr0.8Ba2Cu3O7-Z	Gd	0.2	Pr	0.8	Ba	2	Cu	3													O	7-Z		1	1991	emu/mol	0.00042			myu-B/mol	4.14	-6.7																				3	Y123				3.885	3.897	11.69																																																																																																																								SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2569	PR04310568		PrBa2Cu3O7	Pr1Ba2Cu3O7-Z	Pr	1	Ba	2	Cu	3															O	7-Z		1	1991	emu/mol	0.00036			myu-B/mol	3.02	-6																				3	Y123				3.896	3.903	11.699																																																																																																																								SUPPRESSION OF SUPERCONDUVTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Z SYSTEMS	199105		DEPARTMENT OF PHYSICS,NATIONAL SUN YAT-SEN UNIVERSITY,KAOHSIUNG,TAIWAN 80424,REQUBLIC OF CHINA	PHYS.REV.B,43(1991)10568	C.C.PENG,C.L.LI,C.R.HSU,C.W.LEE,H.D.YANG,P.F.CHEN	GD,PR,BA,CU,O,R	
2570	PR04310589		Bi2Sr2(Ca,Gd)(Cu,Li)2O8	Bi2Sr2Ca0.6Gd0.4Cu1.96LI0.04O8+Z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	1.96	LI	0.04									O	8+Z			1991																												Bi2212																			54	74	87.8				74																																																																																																					DESTRUCTION OF SUPERCONDUCTIVITY IN THE BI2SR2CA1-XGDXCU2-YLIYO8+D SYSTEM	199105		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA,OMAHA,NEBRASKA 68182-0266	PHYS.REV.B,43(1991)10589	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,LI,O	
2571	PR04310589		Bi2Sr2(Ca,Gd)(Cu,Li)2O8	Bi2Sr2Ca0.6Gd0.4Cu1.85LI0.15O8+Z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	1.85	LI	0.15									O	8+Z			1991																												Bi2212																			39	64	91				64																																																																																																					DESTRUCTION OF SUPERCONDUCTIVITY IN THE BI2SR2CA1-XGDXCU2-YLIYO8+D SYSTEM	199105		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA,OMAHA,NEBRASKA 68182-0266	PHYS.REV.B,43(1991)10589	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,LI,O	
2572	PR04310589		Bi2Sr2(Ca,Gd)(Cu,Li)2O8	Bi2Sr2Ca0.6Gd0.4Cu1.8LI0.2O8+Z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	1.8	LI	0.2									O	8+Z			1991																												Bi2212																			24	44	81				44																																																																																																					DESTRUCTION OF SUPERCONDUCTIVITY IN THE BI2SR2CA1-XGDXCU2-YLIYO8+D SYSTEM	199105		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA,OMAHA,NEBRASKA 68182-0266	PHYS.REV.B,43(1991)10589	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,LI,O	
2573	PR04310589		Bi2Sr2(Ca,Gd)(Cu,Li)2O8	Bi2Sr2Ca0.6Gd0.4Cu1.8LI0.2O8+Z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	1.8	LI	0.2									O	8+Z			1991																												Bi2212																				5	24				5																																																																																																					DESTRUCTION OF SUPERCONDUCTIVITY IN THE BI2SR2CA1-XGDXCU2-YLIYO8+D SYSTEM	199105		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA,OMAHA,NEBRASKA 68182-0266	PHYS.REV.B,43(1991)10589	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,LI,O	
2574	PR04310589		Bi2Sr2(Ca,Gd)(Cu,Li)2O8	Bi2Sr2Ca0.6Gd0.4Cu1.6LI0.4O8+Z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	1.6	LI	0.4									O	8+Z			1991																												Bi2212																							5																																																																																																							DESTRUCTION OF SUPERCONDUCTIVITY IN THE BI2SR2CA1-XGDXCU2-YLIYO8+D SYSTEM	199105		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA,OMAHA,NEBRASKA 68182-0266	PHYS.REV.B,43(1991)10589	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,LI,O	
2575	PHC1740155		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.985Zn0.015O7	Y	1	Ba	2	Cu	2.985	Zn	0.015													O	7		1	1991																											3	Y123																																																																																		11		416																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2576	PHC1740155		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7		1	1991																											3	Y123																																																																																		12.48		419																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2577	PHC1740155		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7		1	1991																											3	Y123																																																																																		17.56		394																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2578	PHC1740155		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7		1	1991																											3	Y123																																																																																		18.93		412																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2579	PHC1740155		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7		1	1991																											3	Y123																																																																																		25.7		410																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2580	PHC1740155		YBa2(Cu,Al)3O7	Y1Ba2Cu2.985Al0.015O7	Y	1	Ba	2	Cu	2.985	Al	0.015													O	7		1	1991																											3	Y123																																																																																		4.9																																												EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2581	PHC1740155		YBa2(Cu,Al)3O7	Y1Ba2Cu2.97Al0.03O7	Y	1	Ba	2	Cu	2.97	Al	0.03													O	7		1	1991																											3	Y123																																																																																		8.4																																												EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2582	PHC1740155		YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06O7	Y	1	Ba	2	Cu	2.94	Al	0.06													O	7		1	1991																											3	Y123																																																																																		12.2																																												EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2583	PHC1740155		YBa2Cu3O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	Z	6.92	1	1991																											3	Y123																																																																																		3.54		394																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2584	PHC1740155		YBa2Cu3O7	Y1Ba2Cu3O6.84	Y	1	Ba	2	Cu	3															O	Z	6.84	1	1991																											3	Y123																																																																																		4.15		390																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2585	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	Z	6.7	1	1991																											3	Y123																																																																																		4.32		383																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2586	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	Z	6.5	1	1991																											3	Y123																																																																																		3.66		375																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2587	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	Z	6.4	1	1991																											3	Y123																																																																																		4.54		364																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2588	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.3	Y	1	Ba	2	Cu	3															O	Z	6.3	1	1991																												Y123																																																																																		10.73		355																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2589	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.24	Y	1	Ba	2	Cu	3															O	Z	6.24	1	1991																												Y123																																																																																		12.29		351																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2590	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6.16	Y	1	Ba	2	Cu	3															O	Z	6.16	1	1991																												Y123																																																																																		4.46		347																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2591	PHC1740155		YBa2Cu3Oz	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	Z	6	1	1991																												Y123																																																																																		4.27		320																																										EFFECTS OF OXYGEN STOICHIOMETRY AND ZN(AL) SUBSTITUTION ON LOWTEMPERATURE SPECIFIC HEAT ANOMALY OF THE BA2YCU3OY SYSTEM			INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN		J.TAKEYA,M.ISHIKAWA,Y.NAKAZAWA	AL,BA,Y,CU,O	
2592	MATLET10	TWO STEP TRANSITION	(Bi,Pb)SrCaCu1.5POz	Bi0.7Pb0.3Sr1Ca1Cu1.5POZ	Bi	0.7	Pb	0.3	Sr	1	Ca	1	Cu	1.5	P										O	Z			1990																																															70		100				85																																																																																																									MATERIALS LETTERS,10(1990)133		BI,PB,SR,CA,CU,P,O	
2593	PRB0397320	RH230(=230K),CALCULATED BY ASSUMING V=440A~3	Bi4Sr3(Ca,Tm)3Cu4O16	Bi4Sr3Ca3Cu4O16.25	Bi	4	Sr	3	Ca	3	Cu	4													O	16+Z	16.25		1989																																																83					83																																																																																						0.00000000196					RH2593										APPROACHING THE MOTT-HUBBARS INSULATOR IN THE 85-K SUPERCONDUCTOR BI2(SR,CA)3CU2O8+D BY DOPING WITH TM	198904	HALL EFFECT              ,MOTT-HUBBARD             ,CARRIER	JOSEPH HENRY LODORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	RHYS.REV.B,39(1989)7320	J.CLAYHOLD,N.P.ONG,S.J.HAGEN	BI,SR,CA,CU,O,TM	
2594	PRB0397320	RH300(=230K)	Bi4Sr3(Ca,Tm)3Cu4O16	Bi4Sr3Ca2.8Tm0.2Cu4O16+Z	Bi	4	Sr	3	Ca	2.8	Tm	0.2	Cu	4											O	16+Z			1989																																																88					88																																																																																						0.00000000179					RH2594										APPROACHING THE MOTT-HUBBARS INSULATOR IN THE 85-K SUPERCONDUCTOR BI2(SR,CA)3CU2O8+D BY DOPING WITH TM	198904	HALL EFFECT              ,MOTT-HUBBARD             ,CARRIER	JOSEPH HENRY LODORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	RHYS.REV.B,39(1989)7320	J.CLAYHOLD,N.P.ONG,S.J.HAGEN	BI,SR,CA,CU,O,TM	
2595	PRB0397320	RH300(=230K)	Bi4Sr3(Ca,Tm)3Cu4O16	Bi4Sr3Ca2.5Tm0.5Cu4O16+Z	Bi	4	Sr	3	Ca	2.5	Tm	0.5	Cu	4											O	16+Z			1989																																																91.5					91.5																																																																																						0.0000000014					RH2595										APPROACHING THE MOTT-HUBBARS INSULATOR IN THE 85-K SUPERCONDUCTOR BI2(SR,CA)3CU2O8+D BY DOPING WITH TM	198904	HALL EFFECT              ,MOTT-HUBBARD             ,CARRIER	JOSEPH HENRY LODORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	RHYS.REV.B,39(1989)7320	J.CLAYHOLD,N.P.ONG,S.J.HAGEN	BI,SR,CA,CU,O,TM	
2596	PRB0397320	RH300(=230K)	Bi4Sr3(Ca,Tm)3Cu4O16	Bi4Sr3Ca2Tm1Cu4O16+Z	Bi	4	Sr	3	Ca	2	Tm	1	Cu	4											O	16+Z			1989																																																49					49																																																																																						0.000000000566					RH2596										APPROACHING THE MOTT-HUBBARS INSULATOR IN THE 85-K SUPERCONDUCTOR BI2(SR,CA)3CU2O8+D BY DOPING WITH TM	198904	HALL EFFECT              ,MOTT-HUBBARD             ,CARRIER	JOSEPH HENRY LODORATORIES OF PHYSICS,PRINCETON UNIVERSITY,PRINCETON,NEW JERSEY 08544	RHYS.REV.B,39(1989)7320	J.CLAYHOLD,N.P.ONG,S.J.HAGEN	BI,SR,CA,CU,O,TM	
2597	SSC0780413	TWO PHASES ZNFE2O4 TYPE(A=8.441) + CAFE2O4 TYPE(A=9.277,B=10.714,C=3.049),PHASE TRANSITION AT 200K,SUGGEST SUPERCOND. AT 200K		Ca0.5Zn0.5Fe2O4	Ca	0.5	Zn	0.5	Fe	2															O	4		2	1991																																																			4.2																																																																																																							MAGNETIC ORIGINS OF THE PHASE TRANSITIONAL BEHAVIOUR AT 200K IN CA0.5ZN0.5FE2O4	199105		SCHOOLS OF PHYSICS AND MATERIALS SCIENCE,UNIVERSITY OF BATH,CLVERTON DOWN,BATH BA27AY,UK	SOLID STATE COMMUN.,78(1991)413	B.F.CHAPMAN,CHANG FANGGAO,D.A.LADDS,D.P.ALMOND,G.A.SAUNDERS,LL.MANOSA,P.J.FORD,Q.A.PANKHURST,R.A.L.SULLIVAN,S.J.BENDING,S.SMITH,Z.OTHAMAN	CA,ZN,FE,O	
2598	SSC0780391		PbSr(Ba,La)Cu2O6	Pb1Sr1Ba0.5La0.5Cu2O6-Z	Pb	1	Sr	1	Ba	0.5	La	0.5	Cu	2											O	6-Z			1991																											3					10.772	11.856	6.93													24.8		29.2				27																																																																																																					A NEW SUPERCONDUCTOR IN THE SYSTEM PB-SR-BA-LA-CU-O	199105		SHANGHAI INSTITUTE OF CERAMICS,CHINESEACADEMY OF SCIENCES,1295DING XI ROAD,SHANGHAI 200050,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,78(1991)391	TU HENG-YONG,WU JIN-DI	PB,SR,BA,LA,CU,O	
2599	SSC0780605		(Bi,Pb,Sb)2Sr2Cu3O10	Bi1.5Pb0.4Sb0.06Sr2Ca2Cu2OZ	Bi	1.5	Pb	0.4	Sb	0.06	Sr	2	Ca	2	Cu	2									O	Z		2	1991																												Bi2212																					113				113																																																																																																					SUPERCONDUCTIVITY IN BI1.5PB0.4SBXSR2CA2CU2OY SYSTEM (X=0-0.32)	199105	EFFECT OF DOPING	CHANGCHUN INSTITUTE OF APPLIED CHEMISTRY,ACADEMIA SINICA 130022 CHANGCHUN,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,78(1991)605	HONG GUANGYAN,LI YANRONG,LI YOUMO	BI,PB,SB,SR,CA,CU,O	
2600	SSC0780605		(Bi,Pb,Sb)2Sr2Cu3O10	Bi1.5Pb0.4Sb0.1Sr2Ca2Cu2OZ	Bi	1.5	Pb	0.4	Sb	0.1	Sr	2	Ca	2	Cu	2									O	Z		2	1991																												Bi2223																					114.7				114.7																																																																																																					SUPERCONDUCTIVITY IN BI1.5PB0.4SBXSR2CA2CU2OY SYSTEM (X=0-0.32)	199105	EFFECT OF DOPING	CHANGCHUN INSTITUTE OF APPLIED CHEMISTRY,ACADEMIA SINICA 130022 CHANGCHUN,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,78(1991)605	HONG GUANGYAN,LI YANRONG,LI YOUMO	BI,PB,SB,SR,CA,CU,O	
2601	SSC0780605		(Bi,Pb,Sb)2Sr2Cu3O10	Bi1.5Pb0.4Sb0.18Sr2Ca2Cu2OZ	Bi	1.5	Pb	0.4	Sb	0.18	Sr	2	Ca	2	Cu	2									O	Z		2	1991																												Bi2223																					114				114																																																																																																					SUPERCONDUCTIVITY IN BI1.5PB0.4SBXSR2CA2CU2OY SYSTEM (X=0-0.32)	199105	EFFECT OF DOPING	CHANGCHUN INSTITUTE OF APPLIED CHEMISTRY,ACADEMIA SINICA 130022 CHANGCHUN,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,78(1991)605	HONG GUANGYAN,LI YANRONG,LI YOUMO	BI,PB,SB,SR,CA,CU,O	
2602	SSC0780605		(Bi,Pb,Sb)2Sr2Cu3O10	Bi1.5Pb0.4Sb0.32Sr2Ca2Cu2OZ	Bi	1.5	Pb	0.4	Sb	0.32	Sr	2	Ca	2	Cu	2									O	Z		2	1991																												Bi2223																					116.5				116.5																																																																																																					SUPERCONDUCTIVITY IN BI1.5PB0.4SBXSR2CA2CU2OY SYSTEM (X=0-0.32)	199105	EFFECT OF DOPING	CHANGCHUN INSTITUTE OF APPLIED CHEMISTRY,ACADEMIA SINICA 130022 CHANGCHUN,PEOPLE'S REPUBLIC OF CHINA	SOLID STATE COMMUN.,78(1991)605	HONG GUANGYAN,LI YANRONG,LI YOUMO	BI,PB,SB,SR,CA,CU,O	
2603	PRL0663217	NEUTRON DIFFRACTION AND MOLECULAR DYNAMICS,SIMULATION	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1991																											1	BKBO																															0.42																																																																																															OXYGEN ISOTOPE EFFECT IN SUPERFONDUCTING BA1-XKXBIO3 FROM PHONON DENSITY OF STATES	199106	PHONON SPECTRUM     ,OXYGEN ISOTOPE      ,NEUTRON SCATTERING	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.LETT.,66(1991)3217	A.W.MITCHELL,B.DABROWSKI,C.-K.LOONG,D.G.HINKS,D.L.PRICE,D.R.RICHARDS,J.D.JORGENSEN,M.H.DEGANI,P.VASHISHTA,R.K.KALIA,W.JIN,Y.ZHENG	BA,K,BI,O	
2604	PR04311488	GAMMA=7.6+200*X(=PR MOLE)	(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.95	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	6.95	6.95	1	1991																											3	Y123																				86					86																																																									27.6																																												MAGNETIC-ORDERING,HYPERFINE,AND LINEAR CONTRIBUTIONS TO THE LOW-TEMPERATURE SPECIFIC HEAT OF (Y1-XPRX) BA2CU3O7-Z	199105		MATERIALS AND CHEMICAL SCIENCE DIVISION,LAWRENCE BERKLEY LABORATORY,UNIVERSITY OF CALIFORNIA,BARKELEY,CALIFORNIA 94550	PHYS.REV.B,43(1991)11488	A.AMATO,H.B.RADOUSKY,J.L.PENG,L.ZHANG,N.E.PHILLIPS,R.A.FISHER,R.CASPARY,R.N.SHELTON	Y,PR,BA,CU,O	
2605	PHC1590087		Pb2(Sr,La)LaCu2O6	Pb2Sr0.8La1.2Cu2O6+Z	Pb	2	Sr	0.8	La	1.2	Cu	2													O	6+Z		2	1989																											3	Pb3201	P22(1)2			5.333	5.421	12.609													26	31	32				31		1																																																																																				0.0000000014															NEUTRON DIFFRACTION EVIDENCE FOR OXYGEN DIMERS IN Bi-Ca-Sr-Cu-O SUPERCONDUCTORS			Neutron Physics Division, Bhabha Atomic Research Centre, Trombay, Bombay 400 085, India	Physica C159(1989)87	A. SWQUEIRA,C.N.R. RAO,H. RAJAGOPAL,R. NAGARAJAN		
2606	PHC1590210	SEMICONDUCTOR LIKE BEHAVIOR IN RESISTIVITY	Pb2Ba2YCu3O8	Pb2Ba2Y1Cu3O8+Z	Pb	2	Ba	2	Y	1	Cu	3													O	8+Z		1	1989																											3	Pb2212	P22(1)2			5.465	5.497	16.173																																																																																																																								PREPARATION AND CRYSTAL STRUCTURE OF PB(2)BA(2)YCU(3)O(8+Z)	198906	TED                 ,XRY                 ,STRUCTURE           ,NEUTRON DIFFRACTION ,NEW FAMILY	KAMERLINGH ONNES LABORATORY,LEIDEN UNIVERSITY,P.O.BOX 9506,2300 RA LEIDEN,THE NETHERLANDS	PHYSICA C.,159(1989)210	H.W.ZANDBERGEN,L.J.DE JONGH,W.G.HAIJE,W.T.FU	PB,BA,Y,CU,O	
2607	PHC1590201		(Pb,Sr)Sr2(Y,Ca)Cu2O7	Pb0.5Sr2.5Y0.5Ca0.5Cu2O7-Z	Pb	0.5	Sr	2.5	Y	0.5	Ca	0.5	Cu	2											O	7-Z			1989																											2	Tl1212				3.817		11.907													50		100				75		1																																																																																																			SUPERCONDUCTIVITY UP TO 100 K IN LEAD CUPRATES:A NEW SUPERCONDUCTOR PB(0.5)SR(2.5)Y(0.5)CA(0.5)CU(2)O(7-Z)	198906	FABRICATION         ,TED                 ,HREM                ,MAGNETIZATION       ,STRUCTURE           ,OXYGEN VACANCIE	LABORATOIRE CRISMAT-ISMRA-BD DU MARECHAL JUIN,14032 CAEN CEDEX,FRANCE	PHYSICA C.,159(1989)201	B.RAVEAU,C.MICHEL,D.GROULT,J.PROVOST,M.HERVIEU,T.ROUILLON	PB,SR,Y,CA,CU,O	
2608	PHC1590087	ORTHO WAS TRANSFORMED TO TETRA BY HEATING IN AIR AT 500C		Pb1.8Bi0.2Sr1.1La0.9Cu2O6+Z	Pb	1.8	Bi	0.2	Sr	1.1	La	0.9	Cu	2											O	6+Z		2	1989																											3					5.297	5.415	12.686													24						24		1																																																																																																			NEUTRON DIFFRACTION EVIDENCE FOR OXYGEN DIMERS IN Bi-Ca-Sr-Cu-O SUPERCONDUCTORS			Neutron Physics Division, Bhabha Atomic Research Centre, Trombay, Bombay 400 085, India	Physica C159(1989)87	A. SWQUEIRA,C.N.R. RAO,H. RAJAGOPAL,R. NAGARAJAN		
2609	JJP0281378	SINGLE SIZE=2X2 MM2		Tl1.9Ca0.03Ba2Cu1OZ	Tl	1.9	Ca	0.03	Ba	2	Cu	1													O	Z		3	1989																											2	Tl2202						23.4														84					84		2																																																																																																			CRYSTAL GROWTH AND SUPERCONDUCTIVITY OF TL-CA-BA-CU-O SYSTEM	198908	GROWTH              ,SINGLE CRYSTAL      ,PHASE DIAGRAM       ,EDX                 ,DTA	BASIC HIGH-TECHNOLOGY LABORATORIES,SUMITOMO ELECTRIC INDUSTRIES,LTD.,1-3,SHIMAYA 1-CHOME,KONOHANA-KU,OSAKA 554	JJAP LETT.,28(1989)L1378	HIROMI TAKEI,KOJI TADA,TETSUYUKI KANEKO,TOSHIHIRO KOTANI	TL,CA,BA,CU,O	
2610	JJP0281378	SINGLE SIZE=2X2.5 MM2		Tl2Ca0.67Ba2Cu2OZ	Tl	2	Ca	0.67	Ba	2	Cu	2													O	Z		3	1989																											2	Tl2213						29.2														110					110		2																																																																																																			CRYSTAL GROWTH AND SUPERCONDUCTIVITY OF TL-CA-BA-CU-O SYSTEM	198908	GROWTH              ,SINGLE CRYSTAL      ,PHASE DIAGRAM       ,EDX                 ,DTA	BASIC HIGH-TECHNOLOGY LABORATORIES,SUMITOMO ELECTRIC INDUSTRIES,LTD.,1-3,SHIMAYA 1-CHOME,KONOHANA-KU,OSAKA 554	JJAP LETT.,28(1989)L1378	HIROMI TAKEI,KOJI TADA,TETSUYUKI KANEKO,TOSHIHIRO KOTANI	TL,CA,BA,CU,O	
2611	JJP0281378	SINGLE SIZE=1X1.5 MM2		Tl1.8Ca1.6Ba2Cu2.9OZ	Tl	1.8	Ca	1.6	Ba	2	Cu	2.9													O	Z		3	1989																											2	Tl2223						35.8														118					118		2																																																																																																			CRYSTAL GROWTH AND SUPERCONDUCTIVITY OF TL-CA-BA-CU-O SYSTEM	198908	GROWTH              ,SINGLE CRYSTAL      ,PHASE DIAGRAM       ,EDX                 ,DTA	BASIC HIGH-TECHNOLOGY LABORATORIES,SUMITOMO ELECTRIC INDUSTRIES,LTD.,1-3,SHIMAYA 1-CHOME,KONOHANA-KU,OSAKA 554	JJAP LETT.,28(1989)L1378	HIROMI TAKEI,KOJI TADA,TETSUYUKI KANEKO,TOSHIHIRO KOTANI	TL,CA,BA,CU,O	
2612	JJP0281378	SINGLE SIZE=0.8X0.8 MM2		Tl2.1Ca2.6Ba2Cu3.8OZ	Tl	2.1	Ca	2.6	Ba	2	Cu	3.8													O	Z		3	1989																											2	Tl2324						42														115					115		2																																																																																																			CRYSTAL GROWTH AND SUPERCONDUCTIVITY OF TL-CA-BA-CU-O SYSTEM	198908	GROWTH              ,SINGLE CRYSTAL      ,PHASE DIAGRAM       ,EDX                 ,DTA	BASIC HIGH-TECHNOLOGY LABORATORIES,SUMITOMO ELECTRIC INDUSTRIES,LTD.,1-3,SHIMAYA 1-CHOME,KONOHANA-KU,OSAKA 554	JJAP LETT.,28(1989)L1378	HIROMI TAKEI,KOJI TADA,TETSUYUKI KANEKO,TOSHIHIRO KOTANI	TL,CA,BA,CU,O	
2613	PR0440249	THICKNESS=2810A,COHERE AB/C=13.8	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		5	1991																												T																				30.4					30.4																																							33	2.4																																							0.0996																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2614	PR0440249	THICKNESS=3410A,COHERE AB/C=17.2	(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		5	1991																												T																				19					19																																							39	2.5																																							0.104																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2615	PR0440249	THICKNESS=3550A,COHERE AB/C=17,NO PHASE SEPARATION	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		5	1991																												T																				17.8					17.8																																							52	3																																							0.116																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2616	PR0440249	THICKNESS=3360A,COHERE AB/C=56	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		5	1991																												T																				29.7					29.7																																							31	0.55																																							0.474																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2617	PR0440249	THICKNESS=3630A,COHERE AB/C=17	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		5	1991																												T																				31.6					31.6																																							31	1.8																																							0.643																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2618	PR0440249	THICKNESS=2780A,COHERE AB/C=22	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		5	1991																												T																				25.2					25.2																																							37	1.7																																							0.5																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2619	PR0440249	THICKNESS=3700A,COHERE AB/C=35	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		5	1991																												T																				29.1					29.1																																							31.5	0.9																																							0.284																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2620	PR0440249	THICKNESS=3700A,COHERE AB/C=14.5	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1991																												T																				31.6					31.6																																							32	2.2																																							0.217																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2621	PR0440249	THICKNESS=3350A,COHERE AB/C=15	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1991																												T																				31.4					31.4																																							33	2.2																																							0.176																						RESISTIVE TRANSITION,MAGNETORESISTANCE,AND ANISOTROPY IN LA2-XSRXCU04 SINGLE-CRYSTAL THIN FILMS	199107		NTT APPLIED ELECTRONICS LABORATORIES,NTT IBARAKI RESEARCH ANDDEVELOPMENT CENTER,NIPPON TELEGRAPH ANDTELEPHONE CORPORATION,162 TOKAI,IBARAKI 319-11,JAPAN	PHYS.REV.B,44(1991)249	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2622	PHC1480411		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.97Zn0.03OZ	Eu	1	Ba	2	Cu	2.97	Zn	0.03													O	Z			1987																											3	Y123																				70.6					70.6			K/GPa	9.4																																																																																																	RESISTIVITY OF EUBA2(CU1-YZNY)3OX AS A FUNCTION OF TEMPERATURE, MAGNETIC FIELD, PRESSURE AND ZN CONCENTRATION			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545. USA	PHYSICA C,148(1987)411	G.L.WELLS,H.A.BORGES,J.D.THOMPSON,J.L.SMITH,R.S.KWOK,S.-W.CHEONG,S.B.OSEROFF,Z.FISK	EU,BA,CU,ZN,O	
2623	PHC1480411		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.895Zn0.105OZ	Eu	1	Ba	2	Cu	2.895	Zn	0.105													O	Z			1987																											3	Y123																				25.4					25.4																																																																																																					RESISTIVITY OF EUBA2(CU1-YZNY)3OX AS A FUNCTION OF TEMPERATURE, MAGNETIC FIELD, PRESSURE AND ZN CONCENTRATION			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545. USA	PHYSICA C,148(1987)411	G.L.WELLS,H.A.BORGES,J.D.THOMPSON,J.L.SMITH,R.S.KWOK,S.-W.CHEONG,S.B.OSEROFF,Z.FISK	EU,BA,CU,ZN,O	
2624	PHC1480411		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.85Zn0.15OZ	Eu	1	Ba	2	Cu	2.85	Zn	0.15													O	Z			1987																											3	Y123																							4.2																																																																																																							RESISTIVITY OF EUBA2(CU1-YZNY)3OX AS A FUNCTION OF TEMPERATURE, MAGNETIC FIELD, PRESSURE AND ZN CONCENTRATION			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545. USA	PHYSICA C,148(1987)411	G.L.WELLS,H.A.BORGES,J.D.THOMPSON,J.L.SMITH,R.S.KWOK,S.-W.CHEONG,S.B.OSEROFF,Z.FISK	EU,BA,CU,ZN,O	
2625	PHC1480411		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu3OZ	Eu	1	Ba	2	Cu	3															O	Z			1987																											3	Y123																				93					93			K/GPa	1.2																																																																																																	RESISTIVITY OF EUBA2(CU1-YZNY)3OX AS A FUNCTION OF TEMPERATURE, MAGNETIC FIELD, PRESSURE AND ZN CONCENTRATION			LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NM 87545. USA	PHYSICA C,148(1987)411	G.L.WELLS,H.A.BORGES,J.D.THOMPSON,J.L.SMITH,R.S.KWOK,S.-W.CHEONG,S.B.OSEROFF,Z.FISK	EU,BA,CU,ZN,O	
2626	JJP0281368	D=3000-4000A	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		5	1989																												T																				28.5					28.5																																38.5	1.8						25.4	1.19																																						0.3																							ANOMALOUS FIELD-INDUCED RESISTIVE TRANSITION IN LA2-XSRXCUO4	198908	RESISTIVE TRANSITION     ,COHERENCE LENGRH         ,LA2-XSRXCUO4             ,HC	NTT OPTO-ELECTRONICS LABORATORIES,162 TOKAI,IBARAKI 319-11	JJAP LETT.,28(1989)L1368	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2627	JJP0281368	D=3000-4000A	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1989																												T																				31.4					31.4																																12	0.96						33	2.6																																						0.24																							ANOMALOUS FIELD-INDUCED RESISTIVE TRANSITION IN LA2-XSRXCUO4	198908	RESISTIVE TRANSITION     ,COHERENCE LENGRH         ,LA2-XSRXCUO4             ,HC	NTT OPTO-ELECTRONICS LABORATORIES,162 TOKAI,IBARAKI 319-11	JJAP LETT.,28(1989)L1368	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2628	JJP0281368	D=3000-4000A	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		5	1989																												T																				18.3					18.3																																5.17	0.089						144	2.5																																						0.097																							ANOMALOUS FIELD-INDUCED RESISTIVE TRANSITION IN LA2-XSRXCUO4	198908	RESISTIVE TRANSITION     ,COHERENCE LENGRH         ,LA2-XSRXCUO4             ,HC	NTT OPTO-ELECTRONICS LABORATORIES,162 TOKAI,IBARAKI 319-11	JJAP LETT.,28(1989)L1368	MAKOTO HIKITA,MINORU SUZUKI	LA,SR,CU,O	
2629	PRB0402674	RANDOMLY ORIENTED POWDER PELLET,PENET FROM MAGNETIZATION	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1989																											3	Y123																			89.2	91.2	92.1				91.2																																											2900																																																										MAGNETIC FIELD PENETRATION DEPTH OF POLYCRYSTALLINE (Y,GD)BA2CU3O7,GRAIN-ALIGNED YBA2CU3O7,AND SINGLE-CRYSTAL BI2SR2CACU2O8	198908	PENETRATION DEPTHS  ,MAGNETIZATION	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)2674	D.C.JOHSTON,J.H.CHO,SREEPARNA MITRA,V.G.KOGAN,W.C.LEE	Y,GD,BA,CU,O,BI,SR,CA	
2630	PRB0402674	FREE-FLOWING POWDER ORIENTED WITH H//ABPLANE,PENET FROM MAGNETIZATION	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1989																											3	Y123																			87.5	91.1	92.1				91.1																																											2200																																																										MAGNETIC FIELD PENETRATION DEPTH OF POLYCRYSTALLINE (Y,GD)BA2CU3O7,GRAIN-ALIGNED YBA2CU3O7,AND SINGLE-CRYSTAL BI2SR2CACU2O8	198908	PENETRATION DEPTHS  ,MAGNETIZATION	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)2674	D.C.JOHSTON,J.H.CHO,SREEPARNA MITRA,V.G.KOGAN,W.C.LEE	Y,GD,BA,CU,O,BI,SR,CA	
2631	PRB0402674	PENET FROM MAGNETIZATION	GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z		1	1989																											3	Y123																			90.7	91.4	92.2				91.4																																											2500																																																										MAGNETIC FIELD PENETRATION DEPTH OF POLYCRYSTALLINE (Y,GD)BA2CU3O7,GRAIN-ALIGNED YBA2CU3O7,AND SINGLE-CRYSTAL BI2SR2CACU2O8	198908	PENETRATION DEPTHS  ,MAGNETIZATION	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)2674	D.C.JOHSTON,J.H.CHO,SREEPARNA MITRA,V.G.KOGAN,W.C.LEE	Y,GD,BA,CU,O,BI,SR,CA	
2632	PRB0402674	PENET FROM MAGNETIZATION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1989																												Bi2212																			81.3	84	84.8				84																																												3000																																																									MAGNETIC FIELD PENETRATION DEPTH OF POLYCRYSTALLINE (Y,GD)BA2CU3O7,GRAIN-ALIGNED YBA2CU3O7,AND SINGLE-CRYSTAL BI2SR2CACU2O8	198908	PENETRATION DEPTHS  ,MAGNETIZATION	AMES LABORATORY-U.S. DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS,IOWA STATE UNIVERSITY,AMES,IOWA 50011	PHYS.REV.B,40(1989)2674	D.C.JOHSTON,J.H.CHO,SREEPARNA MITRA,V.G.KOGAN,W.C.LEE	Y,GD,BA,CU,O,BI,SR,CA	
2633	PHC1670020	RESISTIVITY AND SUSCEPTIBILITY ARE MEASURED FROM4.2 TO 300K	BiPbSr2CoO6	Bi1Pb1Sr2Co1O6	Bi	1	Pb	1	Sr	2	Co	1													O	6		3	1990																																5.326	5.396	23.521																	4.2																																																																																																							NEW NON-SUPERCONDUCTING MODULATION-FREE BIPBSR2MOY PHASES (M=CO,MN,FE) ISOTYPC WITH THE 10 K BI2SR2CUOY SUPERCONDUCTOR		ISOSTRUCTURAL       ,SINGLE CRYSTALS     ,ELECTRICAL PROPERTIE,STRUCTURE           ,MOSSBAURE           ,MAGNETIC PHASE	BELL COMMUNICATIONS RESARCH,RED BANK,NJ 07701,USA	PHYSICA C,167(1990)20	E.TSELEPIS,E.WANG,G.W.HULL,J.M.TARASCON,M.EIBSCHUTZ,R.RAMESH,W.R.MCKINNON,Y.LEPAGE	BI,PB,SR,CO,MN,FE,O	
2634	PHC1670020	RESISTIVITY AND SUSCEPTIBILITY ARE MEASURED FROM4.2 TO 300K	BiPbSr2MnO6	Bi1Pb1Sr2Mn1O6	Bi	1	Pb	1	Sr	2	Mn	1													O	6		3	1990																																5.331	5.399	23.751																	4.2																																																																																																							NEW NON-SUPERCONDUCTING MODULATION-FREE BIPBSR2MOY PHASES (M=CO,MN,FE) ISOTYPC WITH THE 10 K BI2SR2CUOY SUPERCONDUCTOR		ISOSTRUCTURAL       ,SINGLE CRYSTALS     ,ELECTRICAL PROPERTIE,STRUCTURE           ,MOSSBAURE           ,MAGNETIC PHASE	BELL COMMUNICATIONS RESARCH,RED BANK,NJ 07701,USA	PHYSICA C,167(1990)20	E.TSELEPIS,E.WANG,G.W.HULL,J.M.TARASCON,M.EIBSCHUTZ,R.RAMESH,W.R.MCKINNON,Y.LEPAGE	BI,PB,SR,CO,MN,FE,O	
2635	PHC1670042	COHERE OBTAINED FROM FITTING CURVE USING FLUCTUATION EQUATION	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1990																												Y123																				89.5					89.5																																4.7	1.4						12.5																																																														MAGNETORESISTANCE ABOVE AND BELOW TC IN C-ACIS-ORIENTED YBA2XU3O7Z		RESISTIBITY         ,THIN FILMS          ,MAGNETORESISTANCE   ,ANISOTROPIC         ,FLUCTUATION COND	INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SCIENCES,BEIJING,PR CHINA	PHYSICA C,167(1990)42	BAI-RU ZHAO,KAZUYUKI SHIRAKI,LAN-FONG CHEN,LIN LI,PO XU,SHOICHI MASE,YIN-ZI ZHANG,YU-YING ZHAO,YUUJI HORIE	Y,BA,CU,O	
2636	PRL0640080		(Sm,Ce)2CuO4	Sm1.88Ce0.12Cu1O4	Sm	1.88	Ce	0.12	Cu	1															O	4			1990																												T'																				3.9					3.9			K/GPa	-0.62																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2637	PRL0640080		(Sm,Ce)2CuO4	Sm1.8Ce0.2Cu1O4	Sm	1.8	Ce	0.2	Cu	1															O	4			1990																												T'																				14.7					14.7			K/GPa	-0.19																																																																																																	PRESSUR DEPARTMENT OF TC IN L2-XMXCUO4-Y (L=PR,ND,SM,EU;M=CE,TH): ANTISYMMETRIC BEHAVIOR OF ELECTRON - VERSUS HOLE-DOPED COPPER-OXIDE SUPERCONDUCTORS	199001	TC                  ,PRESSURE	DEPARTMENT OF PHYSICS AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES, UNIVERSITY OF CALIFORNIA, SAN DIEGO, LA JOLLA, CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)80	C.L.SEAMAN,E.A.EARLY,J.BEILLE,J.J.NEUMEIER,J.T.MARKERT,M.B.MAPLE,T.MORAN	PR,ND,SM,EU,CE,TH,CU,O	
2638	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				35.8					35.8																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2639	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.996Fe0.004O4	La	1.85	Sr	0.15	Cu	0.996	Fe	0.004													O	4		1	1990																												T																				29.4					29.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2640	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.992Fe0.008O4	La	1.85	Sr	0.15	Cu	0.992	Fe	0.008													O	4		1	1990																												T																				20.4					20.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2641	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.988Fe0.012O4	La	1.85	Sr	0.15	Cu	0.988	Fe	0.012													O	4		1	1990						4.8																						T																				11.6					11.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2642	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.985Fe0.015O4	La	1.85	Sr	0.15	Cu	0.985	Fe	0.015													O	4		1	1990																												T																				5.2					5.2																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2643	PR0428752		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.982Fe0.018O4	La	1.85	Sr	0.15	Cu	0.982	Fe	0.018													O	4		1	1990																												T																				0.2					0.2																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2644	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				35.3					35.3																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2645	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.996Zn0.004O4	La	1.85	Sr	0.15	Cu	0.996	Zn	0.004													O	4		1	1990																												T																				31					31																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2646	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.992Zn0.008O4	La	1.85	Sr	0.15	Cu	0.992	Zn	0.008													O	4		1	1990																												T																				25.5					25.5																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2647	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.988Zn0.012O4	La	1.85	Sr	0.15	Cu	0.988	Zn	0.012													O	4		1	1990						0.95																						T																				20.2					20.2																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2648	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.985Zn0.015O4	La	1.85	Sr	0.15	Cu	0.985	Zn	0.015													O	4		1	1990																												T																				16.6					16.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2649	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.982Zn0.018O4	La	1.85	Sr	0.15	Cu	0.982	Zn	0.018													O	4		1	1990																												T																				12.6					12.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2650	PR0428752		(La.Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.979Zn0.021O4	La	1.85	Sr	0.15	Cu	0.979	Zn	0.021													O	4		1	1990																												T																				10.4					10.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2651	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.976Zn0.024O4	La	1.85	Sr	0.15	Cu	0.976	Zn	0.024													O	4		1	1990																												T																				6.6					6.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2652	PR0428752		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.973Zn0.027O4	La	1.85	Sr	0.15	Cu	0.973	Zn	0.027													O	4		1	1990																												T																				2.8					2.8																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2653	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				34.7					34.7																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2654	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.996Co0.004O4	La	1.85	Sr	0.15	Cu	0.996	Co	0.004													O	4		1	1990																												T																				30					30																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2655	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.992Co0.008O4	La	1.85	Sr	0.15	Cu	0.992	Co	0.008													O	4		1	1990																												T																				23.1					23.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2656	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.988Co0.012O4	La	1.85	Sr	0.15	Cu	0.988	Co	0.012													O	4		1	1990																												T																				18.6					18.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2657	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.985Co0.015O4	La	1.85	Sr	0.15	Cu	0.985	Co	0.015													O	4		1	1990																												T																				16					16																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2658	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.982Co0.018O4	La	1.85	Sr	0.15	Cu	0.982	Co	0.018													O	4		1	1990																												T																				8.9					8.9																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2659	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.979Co0.021O4	La	1.85	Sr	0.15	Cu	0.979	Co	0.021													O	4		1	1990						1.2																						T																				6					6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2660	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.976Co0.024O4	La	1.85	Sr	0.15	Cu	0.976	Co	0.024													O	4		1	1990																												T																				4.4					4.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2661	PR0428752		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.973Co0.027O4	La	1.85	Sr	0.15	Cu	0.973	Co	0.027													O	4		1	1990																												T																				2.5					2.5																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2662	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				36					36																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2663	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.995Ga0.005O4	La	1.85	Sr	0.15	Cu	0.995	Ga	0.005													O	4		1	1990																												T																				29.8					29.8																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2664	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.99Ga0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ga	0.01													O	4		1	1990																												T																				24.1					24.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2665	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.985Ga0.015O4	La	1.85	Sr	0.15	Cu	0.985	Ga	0.015													O	4		1	1990																												T																				13.7					13.7																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2666	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.98Ga0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ga	0.02													O	4		1	1990						0.8																						T																				8.3					8.3																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2667	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.977Ga0.023O4	La	1.85	Sr	0.15	Cu	0.977	Ga	0.023													O	4		1	1990																												T																				0.9					0.9																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2668	PR0428752		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.975Ga0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ga	0.025													O	4		1	1990																												T																				0.7					0.7																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2669	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				38.1					38.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2670	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.993Ni0.007O4	La	1.85	Sr	0.15	Cu	0.993	Ni	0.007													O	4		1	1990																												T																				32.6					32.6																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2671	PR0428752		(La.Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.986Ni0.014O4	La	1.85	Sr	0.15	Cu	0.986	Ni	0.014													O	4		1	1990																												T																				27.9					27.9																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2672	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4		1	1990																												T																				22.2					22.2																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2673	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4		1	1990																												T																				17.4					17.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2674	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4		1	1990						0.6																						T																				13.4					13.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2675	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.966Ni0.034O4	La	1.85	Sr	0.15	Cu	0.966	Ni	0.034													O	4		1	1990																												T																				9.4					9.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2676	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15CuNi0.037O4	La	1.85	Sr	0.15	Cu		Ni	0.037													O	4		1	1990																												T																				6.1					6.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2677	PR0428752		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15CuNi0.04O4	La	1.85	Sr	0.15	Cu		Ni	0.04													O	4		1	1990																												T																				2.5					2.5																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2678	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1990																												T																				34.4					34.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2679	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.996Al0.004O4	La	1.85	Sr	0.15	Cu	0.996	Al	0.004													O	4		1	1990																												T																				30.4					30.4																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2680	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.992Al0.008O4	La	1.85	Sr	0.15	Cu	0.992	Al	0.008													O	4		1	1990																												T																				27.1					27.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2681	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.988Al0.012O4	La	1.85	Sr	0.15	Cu	0.988	Al	0.012													O	4		1	1990																												T																				17.9					17.9																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2682	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.985Al0.015O4	La	1.85	Sr	0.15	Cu	0.985	Al	0.015													O	4		1	1990																												T																				15					15																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2683	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.982Al0.018O4	La	1.85	Sr	0.15	Cu	0.982	Al	0.018													O	4		1	1990																												T																				9.1					9.1																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2684	PR0428752		(La,Sr)2(Cu,Al)O4	La1.85Sr0.15Cu0.979Al0.021O4	La	1.85	Sr	0.15	Cu	0.979	Al	0.021													O	4		1	1990						1.1																						T																				3.7					3.7																																																																																																					MAGNECTIC PAIR-BREAKING EFFECTS: MOMENT FORMATION AND CRITICALDOPING LEVEL IN SUPERCONDUCTING LA1.85SR0.15CU1-XAXO4 SYSTEMS(A=FE,CO,NI,ZU,GA,AL)	199011	CU-SITE DOPING      ,MAGNETIC MOMENT     ,PAIR-BREAKING EFFE	DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, PROVIDENCE, PHODE ISLAND 02912	PHYS.RE.V,42(1990)8752	C.L.CHIEN,GANG XIAO,J.Q.XIAO,MARTA Z. CIEPLAK	LA,SR,CU,O,FE,CO,NI,ZN,GA,AL	
2685	PR04312989		YBa2(Cu,Fe)3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																											3	Y123																				91.2	92.7			2.6	91.2															3500																																																																																						EFFECT OF CU SUBSTITUTION BY FE ON THE MAGNETIC PROPERTIES OFYBA2CU3O7-Y SINGLE CRYSTALS	199106		DEPATMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,DAVIS,CALIFORNIA 95616	PHYS.REV.B,43(1991)12989	J.Z.LIU,M.D.LAN,R.N.SHELTON	Y,BA,CU,O,FE	
2686	PR04312989		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O7-Z	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7-Z		3	1991																											3	Y123																				82.1	87.2			8.4	82.1															2500																																																																																						EFFECT OF CU SUBSTITUTION BY FE ON THE MAGNETIC PROPERTIES OFYBA2CU3O7-Y SINGLE CRYSTALS	199106		DEPATMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,DAVIS,CALIFORNIA 95616	PHYS.REV.B,43(1991)12989	J.Z.LIU,M.D.LAN,R.N.SHELTON	Y,BA,CU,O,FE	
2687	PR04312989		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7-Z	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7-Z		3	1991																											2	Y123																				76	86.1			14.6	76															2300																																																																																						EFFECT OF CU SUBSTITUTION BY FE ON THE MAGNETIC PROPERTIES OFYBA2CU3O7-Y SINGLE CRYSTALS	199106		DEPATMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,DAVIS,CALIFORNIA 95616	PHYS.REV.B,43(1991)12989	J.Z.LIU,M.D.LAN,R.N.SHELTON	Y,BA,CU,O,FE	
2688	PR04312989		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.76Fe0.24O7-Z	Y	1	Ba	2	Cu	2.76	Fe	0.24													O	7-Z		3	1991																											2	Y123																				48.3	70			22.2	48.3															800																																																																																						EFFECT OF CU SUBSTITUTION BY FE ON THE MAGNETIC PROPERTIES OFYBA2CU3O7-Y SINGLE CRYSTALS	199106		DEPATMENT OF PHYSICS,UNIVERSITY OF CALIFORNIA,DAVIS,DAVIS,CALIFORNIA 95616	PHYS.REV.B,43(1991)12989	J.Z.LIU,M.D.LAN,R.N.SHELTON	Y,BA,CU,O,FE	
2689	JML0090033		(In,Pb)Sr2(Y,Ca)Cu2OZ	In0.5Pb0.5Sr2Y0.5Ca0.5Cu2OZ	In	0.5	Pb	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z		1	1990																											2					3.82		11.89														36					36																																																																																																					CONFIRMATION OF SUPERCONDUCTIVITY IN (INPB)SR2(YCA)CU2OZ			LABORATOIRE DE PHYSIQUE DES SOLIDES DE BELLEVUE,CNRS,92195 MEUDON,FRANCE	J.MATER.SCI.LETT.,9(1990)33	A.HALLI,H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	IN,PB,SR,Y,CA,CU,O	
2690	JML0090033		(In,Pb)Sr2(Y,Ca)Cu2OZ	In0.4Pb0.6Sr2Y0.5Ca0.5Cu2OZ	In	0.4	Pb	0.6	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z		1	1990																											2																					47					47																																																																																		15				0.000000006															CONFIRMATION OF SUPERCONDUCTIVITY IN (INPB)SR2(YCA)CU2OZ			LABORATOIRE DE PHYSIQUE DES SOLIDES DE BELLEVUE,CNRS,92195 MEUDON,FRANCE	J.MATER.SCI.LETT.,9(1990)33	A.HALLI,H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	IN,PB,SR,Y,CA,CU,O	
2691	JML0090033		(In,Pb)Sr2(Y,Ca)Cu2OZ	In0.3Pb0.7Sr2Y0.5Ca0.5Cu2OZ	In	0.3	Pb	0.7	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z		1	1990																											2																				38	40	50				40																																																																																																					CONFIRMATION OF SUPERCONDUCTIVITY IN (INPB)SR2(YCA)CU2OZ			LABORATOIRE DE PHYSIQUE DES SOLIDES DE BELLEVUE,CNRS,92195 MEUDON,FRANCE	J.MATER.SCI.LETT.,9(1990)33	A.HALLI,H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	IN,PB,SR,Y,CA,CU,O	
2692	PR0428019	PENET BY MUON SPIN RESONANCE	YBa2Cu3O7	Y1Ba2Cu3O6.97	Y	1	Ba	2	Cu	3															O	6.97	6.97		1990									5.3																		3	Y123																				89.5				8	89.5										60																																	1550																																																										MUON-SPIN-ROTATION MEASUREMENTS OF THE LONDON PENETRATION DEPTHS IN YBA2CU3O6.79	199011	MUON-SPIN-ROTATION  ,PENTRATION DEPTH	PHYSIK-INSTITUT DER UNIVERSITAT ZURICH, H-8001 ZURICH, SWITZERLAND	PHYS.REV.B,42(1990)8019	B.PUMPIN,C.ROSSEL,E.KALDIS,H.KELLER,H.SIMMLER,I.M.SAVIC,J.W.SCHNEIDER,P.ZIMMERMANN,S.RUSIECKI,W.KUNDIG,W.ODERMATT,Y.MAENO	B,BA,CU,O	
2693	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba2Cu4O7.9	Y	1	Ba	2	Cu	4															O	7.9	7.9	1	1990																											3	Y124				3.836	3.872	27.224													74	78.3	80				78.3																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2694	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.95La0.05Cu4OZ	Y	1	Ba	1.95	La	0.05	Cu	4													O	Z		1	1990																											3	Y124				3.832	3.872	27.213													68	74.3	75				74.3																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2695	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.9La0.1Cu4O7.8	Y	1	Ba	1.9	La	0.1	Cu	4													O	7.8	7.8	1	1990																											3	Y124				3.832	3.873	27.196													60	67.8	71				67.8																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2696	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.85La0.15Cu4OZ	Y	1	Ba	1.85	La	0.15	Cu	4													O	Z		1	1990																											3	Y124				3.835	3.875	27.173													54	63.4	67				63.4																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2697	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.8La0.2Cu4O7.9	Y	1	Ba	1.8	La	0.2	Cu	4													O	7.9	7.9	1	1990																											3	Y124				3.834	3.875	27.145													43	60.1	62				60.1																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2698	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.75La0.25Cu4OZ	Y	1	Ba	1.75	La	0.25	Cu	4													O	Z			1990																											3	Y124				3.828	3.876	27.151													44	60.1	63				60.1																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2699	PR0428030		Y(Ba,La)2Cu4O8	Y1Ba1.7La0.3Cu4O7.8	Y	1	Ba	1.7	La	0.3	Cu	4													O	7.8	7.8		1990																											3	Y124				3.835	3.878	27.143													37	62.7	59				62.7																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2700	PR0428030		(Y,Ca)(Ba,La)2Cu4O8	Y0.95Ca0.05Ba1.9La0.1Cu4O7.9	Y	0.95	Ca	0.05	Ba	1.9	La	0.1	Cu	4											O	7.9	7.9	1	1990																											3	Y124				3.828	3.874	27.155													46	68.8	68				68.8																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2701	PR0428030		(Y,Ca)(Ba,La)2Cu4O8	Y0.9Ca0.1Ba1.9La0.1Cu4O7.8	Y	0.9	Ca	0.1	Ba	1.9	La	0.1	Cu	4											O	7.8	7.8	1	1990																											3	Y124				3.827	3.873	27.174													60	79	80				79																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2702	PR0428030		(Y,Ca)(Ba,La)2Cu4O8	Y0.85Ca0.15Ba1.9La0.1Cu4OZ	Y	0.85	Ca	0.15	Ba	1.9	La	0.1	Cu	4											O	Z			1990																											3	Y124				3.825	3.871	27.183													70	79.3	81				79.3																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2703	PR0428030		(Y,Ca)(Ba,La)2Cu4O8	Y0.8Ca0.2Ba1.9La0.1Cu4OZ	Y	0.8	Ca	0.2	Ba	1.9	La	0.1	Cu	4											O	Z			1990																																															74	80.7	83				80.7																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2704	PR0428030		(Y,Ca)(Ba,La)2Cu4O8	Y0.75Ca0.25Ba1.9La0.1Cu4OZ	Y	0.75	Ca	0.25	Ba	1.9	La	0.1	Cu	4											O	Z			1990																																															71	80.4	83				80.4																																																																																																					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF Y(BA1-YLAY)2CU4O8AND (Y1-XCAX)(BA1-YLAY)2CU4O8	199011	SYNTHESIZED         ,SINGLE-PHASE	SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTO-KU,TOKYO 135, JAPAN	PHYS.REV.B,42(1990)8030	H.YAMAUCHI,NAOKI KOSHIZUKA,NOBUO SUZUKI,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TAKAHIRO WADA,TAKAYUKI MIYATAKE,TAKESHI SAKURAI	Y,BA,LA,CU,O,CA	
2705	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.7	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	6.7	6.7	1	1991																											2	Y123																							4.2																																																																																																							CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2706	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.76	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	6.76	6.76	1	1991																											2	Y123																				27.8					27.8										0.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2707	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.8	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	6.8	6.8	1	1991																											2	Y123																				43.9					43.9										5.1																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2708	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.85	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	6.85	6.85	1	1991																											2	Y123																				57.7					57.7										9.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2709	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O6.9	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	6.9	6.9	1	1991																											2	Y123																				58.8					58.8										9.2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2710	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.58	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.58	6.58	1	1991																											2	Y123																							4.2																																																																																																							CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2711	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.64	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.64	6.64	1	1991																											2	Y123																				20.5					20.5										0.9																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2712	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.7	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.7	6.7	1	1991																											2	Y123																				28.5					28.5										2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2713	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.75	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.75	6.75	1	1991																											2	Y123																				37.4					37.4										4																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2714	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.8	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.8	6.8	1	1991																											2	Y123																				53.1					53.1										9.1																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2715	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.85	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.85	6.85	1	1991																											2	Y123																				63.8					63.8										11.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2716	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.9	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	6.9	6.9	1	1991																											2	Y123				3.859		11.659														74.9					74.9										14.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2717	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.52	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.52	6.52	1	1991																											3	Y123				3.858	3.872																		4.2																																																																																																							CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2718	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.55	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.55	6.55	1	1991																											3	Y123																				17.8					17.8										0.8																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2719	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.6	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.6	6.6	1	1991																											3	Y123				3.85	3.876															26.2					26.2										6																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2720	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.64	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.64	6.64	1	1991																											3	Y123				3.847	3.877															37.4					37.4										4.1																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2721	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.69	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.69	6.69	1	1991																											3	Y123				3.843	3.877															43.5					43.5										5																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2722	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.73	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.73	6.73	1	1991																											3	Y123				3.84	3.878															52.7					52.7										9																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2723	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.79	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.79	6.79	1	1991																											3	Y123				3.837	3.878															67.6					67.6																																																																			5.38																																		CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2724	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.84	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.84	6.84	1	1991																											3	Y123				3.837	3.879															76.4					76.4										14.2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2725	PHC1740316		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.95Fe0.05O6.9	Y	1	Ba	2	Cu	2.95	Fe	0.05													O	6.9	6.9	1	1991																											3	Y123				3.833	3.877	11.663														88.7					88.7										19.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2726	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.44	Y	1	Ba	2	Cu	3															O	6.44	6.44	1	1991																											3	Y123																							4.2																																																																																																							CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2727	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.48	Y	1	Ba	2	Cu	3															O	6.48	6.48	1	1991																											3	Y123																				19.7					19.7										0.8																																																									1.5																																		CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2728	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.53	Y	1	Ba	2	Cu	3															O	6.53	6.53	1	1991																											3	Y123																				40					40										5.8																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2729	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.58	Y	1	Ba	2	Cu	3															O	6.58	6.58	1	1991																											3	Y123																				43.5					43.5										9																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2730	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.62	Y	1	Ba	2	Cu	3															O	6.62	6.62	1	1991																											3	Y123																				50.4					50.4										10																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2731	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	6.68	6.68	1	1991																											3	Y123																				54.6					54.6										9																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2732	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.71	Y	1	Ba	2	Cu	3															O	6.71	6.71	1	1991																											3	Y123																				59.6					59.6										10.1																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2733	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	6.75	6.75	1	1991																											3	Y123																				68.8					68.8										14.2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2734	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8	6.8	1	1991																											3	Y123																				81.8					81.8										12.3																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2735	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	6.85	6.85	1	1991																											3	Y123																				89					89										19.2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2736	PHC1740316		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1991																											3	Y123				3.821	3.881	11.666														91					91										24.2																																																																																											CRYSTALLOGRAPHIC,THERMOGRAVIMETRIC AND MAGNETIZATION STUDY OFTHE YBA2CU3-XFEXOY SUPERCONDUCTOR (O=<X=<0.2,6=<Y=<7)			INSTITUTE OF MATERIALS SCIENCE,N.C.S.R. DEMOKRITOS ,15310,ATHENS,GREECE	PHYSICA C,174(1991)316	D.NIARCNOS,G.KALLIAS,M.PISSAS,V.PSYHARIS	Y,BA,CU,O,FE	
2737	PRL0620217	PENET FROM SUSCEPTIBILITY,KAI/KAIZERO=1-(2*PENET)*TANH(D/2*PENET)	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1989																											3	Y123																				89.5					89.5																																																																																																					Direct Measurement of the Temperature-Dependent Magnetic Penetration Depth in Y-Ba-Cu-O Crystals	198901		IBM Tomas J. Watson Research center, Yorktown Heights, New York10598-0218	Phys.Rev.Lett.62(1989)217	A.P. Malozemoff,F. Holtzberg,L. Krusin-Elbaum,R.L. Greene,Y. Yeshurun		
2738	PR0440741	COHERE FITTED BY 3D AL MODEL.ANOTHER MODEL ALSO ADOPTED	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1991																											3	Y123																			90.2	90.5					90.5																																						1.5						1400																																		0.078				0.224																			ANALYSIS OF THE FLUCTUATION-INDUCED EXCESS DC CONDUCTIVITY OFEPITAXIAL YBA2CU3O7 FILMS:INFLUENCE OF A SHORT-WAVELENGTH CUTOFF IN THE FLUCTUATION SPECTRUM	199107		PHYSIKALOSCHES INSTITUT,UNIVERSITAT ERLANGEN,ERWIN-ROMME-STRASSE 1,D-8520 ERLANGEN,FEDERAL REPUBLIC OF GERMANY	PHYS.REV.B,44(1991)741	B.HENSEL,G.SAEMANN-ISCHENKO,R.HOPFENGARTNER	Y,BA,CU,O	
2739	PHC1750165		La2Sr6Cu8O17	La2Sr6Cu8O17.6	La	2	Sr	6	Cu	8															O	17.6	17.6	1	1991		-3895000000000000000																											P42(1)2																																																																																											3.6			TP2739					1.78							2.45				0.0000000016					RH2739										TRANSPORT PROPERTIES AND CRYSTAL STRUCTURES OF NEW CONDUCTIVECOPPER OXIDES LA2SR6CU8O16+Z (Z=0.0 AND 1.6)	199106	TRANSPORT PROPERTIES,CRYSTAL STRUCTURES	DEPARTMENT OF PHYSICS,COLLEGE OF LUBERAL ARTS,WANAZAWA UNIVERSITY,KANAZAWA 920,JAPAN	PHYSICA C,175(1991)165	HIDESHI FUJISHITA,MASAFUMI SERA,MASATOSHI SATO	LA,SR,CU,O	
2740	PHC1740359		Bi2(Sr,Ca)2(Ca,Lu)Cu2O8	Bi2Sr1.6Ca1.2Lu0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Lu	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.397		30.531														88.6					88.6																																																																																						0.00000000181															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2741	PHC1740359		Bi2(Sr,Ca)2(Ca,Yb)Cu2O8	Bi2Sr1.6Ca1.2Yb0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Yb	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.397		30.542														88.3					88.3																																																																																						0.00000000213															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2742	PHC1740359		Bi2(Sr,Ca)2(Ca,Y)Cu2O8	Bi2Sr1.6Ca1.2Y0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Y	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.402		30.571														89.1					89.1																																																																																						0.00000000224															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2743	PHC1740359		Bi2(Sr,Ca)2(Ca,Dy)Cu2O8	Bi2Sr1.6Ca1.2Dy0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Dy	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.401		30.596														88					88																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2744	PHC1740359		Bi2(Sr,Ca)2(Ca,Gd)Cu2O8	Bi2Sr1.6Ca1.2Gd0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Gd	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.407		30.59														87.1					87.1																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2745	PHC1740359		Bi2(Sr,Ca)2(Ca,Eu)Cu2O8	Bi2Sr1.6Ca1.2Eu0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Eu	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.408		30.608														87.1					87.1																																																																																						0.00000000177															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2746	PHC1740359		Bi2(Sr,Ca)2(Ca,Nd)Cu2O8	Bi2Sr1.6Ca1.2Nd0.2Cu2O8.26	Bi	2	Sr	1.6	Ca	1.2	Nd	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.413		30.65														86					86																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2747	PHC1740359		Bi2(Sr,Ca)2(Ca,La)Cu2O8	Bi2Sr1.6Ca1.2La0.2Cu2O8.27	Bi	2	Sr	1.6	Ca	1.2	La	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.413		30.652														86					86																																																																																						0.00000000173															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2748	PHC1740359		Bi2(Sr,Ca)2(Ca,Lu)Cu2O8	Bi2Sr1.8Ca1Lu0.2Cu2O8.27	Bi	2	Sr	1.8	Ca	1	Lu	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.398		30.625														91.1					91.1																																																																																						0.00000000184															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2749	PHC1740359		Bi2(Sr,Ca)2(Ca,Yb)Cu2O8	Bi2Sr1.8Ca1Yb0.2Cu2O8.26	Bi	2	Sr	1.8	Ca	1	Yb	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.398		30.615														90.1					90.1																																																																																						0.00000000181															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2750	PHC1740359		Bi2(Sr,Ca)2(Ca,Y)Cu2O8	Bi2Sr1.8Ca1Y0.2Cu2O8.25	Bi	2	Sr	1.8	Ca	1	Y	0.2	Cu	2											O	8.25	8.25	1	1991																											2	Bi2212				5.404		30.623														90.4					90.4																																																																																						0.00000000198															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2751	PHC1740359		Bi2(Sr,Ca)2(Cu,Dy)Cu2O8	Bi2Sr1.8Ca1Dy0.2Cu2O8.26	Bi	2	Sr	1.8	Ca	1	Dy	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.405		30.639														89.2					89.2																																																																																						0.00000000195															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2752	PHC1740359		Bi2(Sr,Ca)2(Ca,Gd)Cu2O8	Bi2Sr1.8Ca1Gd0.2Cu2O8.26	Bi	2	Sr	1.8	Ca	1	Gd	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.407		30.647														88.9					88.9																																																																																						0.00000000177															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2753	PHC1740359		Bi2(Sr,Ca)2(Ca,Eu)Cu2O8	Bi2Sr1.8Ca1Eu0.2Cu2O8.25	Bi	2	Sr	1.8	Ca	1	Eu	0.2	Cu	2											O	8.25	8.25	1	1991																											2	Bi2212				5.41		30.656														88.9					88.9																																																																																						0.00000000217															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2754	PHC1740359		Bi2(Sr,Ca)2(Ca,Nd)Cu2O8	Bi2Sr1.8Ca1Nd0.2Cu2O8.26	Bi	2	Sr	1.8	Ca	1	Nd	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.414		30.685														87.7					87.7																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2755	PHC1740359		Bi2(Sr,Ca)2(Ca,La)Cu2O8	Bi2Sr1.8Ca1La0.2Cu2O8.27	Bi	2	Sr	1.8	Ca	1	La	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.416		30.727														87.8					87.8																																																																																						0.00000000167															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2756	PHC1740359		Bi2(Sr,Ca)2(Ca,Lu)Cu2O8	Bi2Sr2Ca0.8Lu0.2Cu2O8.27	Bi	2	Sr	2	Ca	0.8	Lu	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.4		30.666														92.5					92.5																																																																																						0.00000000192															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2757	PHC1740359		Bi2(Sr,Ca)2(Ca,Yb)Cu2O8	Bi2Sr2Ca0.8Yb0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Yb	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.403		30.658														92.1					92.1																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2758	PHC1740359		Bi2(Sr,Ca)2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8.27	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.408		30.677														92.6					92.6																																																																																						0.00000000217															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2759	PHC1740359		Bi2(Sr,Ca)2(Ca,Dy)Cu2O8	Bi2Sr2Ca0.8Dy0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Dy	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.408		30.683														91.7					91.7																																																																																						0.0000000017															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2760	PHC1740359		Bi2(Sr,Ca)2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8.27	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8.27	8.27	1	1991																											2	Bi2212				5.411		30.705														90.9					90.9																																																																																						0.00000000203															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2761	PHC1740359		Bi2(Sr,Ca)2(Ca,Eu)Cu2O8	Bi2Sr2Ca0.8Eu0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Eu	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.412		30.723														90.9					90.9																																																																																						0.00000000195															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2762	PHC1740359		Bi2(Sr,Ca)2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.8Nd0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	Nd	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.416		30.746														89.7					89.7																																																																																						0.00000000209															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2763	PHC1740359		Bi2(Sr,Ca)2(Ca,La)Cu2O8	Bi2Sr2Ca0.8La0.2Cu2O8.26	Bi	2	Sr	2	Ca	0.8	La	0.2	Cu	2											O	8.26	8.26	1	1991																											2	Bi2212				5.419		30.774														89					89																																																																																						0.00000000159															SITE-SELECTIVE SUBSTITUTION EFFECT ON TC IN THE BI2(SR2-XCAX)(CA0.8R0.2)CU2O8+Y SISTEM(R=RARE-EARTH)			INSTITUTE OF APPLIED PHYSICS,UNIVERSITY OF TSUKUBA,IBARAKI 305,JAPAN	PHYSICA C,174(1991)359	H.ASANO,J.FUJIKAMI,M.AKAMATSU,R.YOSHIZAKI,T.ISHIGAKI	BI,SR,CA,CU,O,R	
2764	JJP0281926		TlLaSrCuO5	Tl1La1Sr1Cu1O5	Tl	1	La	1	Sr	1	Cu	1													O	5		1	1989																											2		P4/MMM			3.78		8.806													30		38				34																																																																																		109																			CRYSTAL STRUCTURE AND CHARACTERIZATION OF THE NEW TL(LA,SR)2 CUO5-TYPE SUPERCONDUCTOR	198911	XRY                 ,STRUCTURE           ,RESISTIVITY         ,SUSCEPTIVILITY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA,IBARAKI 305	JJAP LETT 28(1989)L1926	MASAYA WATAHIKI,TAKASHI MOCHIKU,TOSHIO NAGASHIMA,YUH FUKAI	TL,LA,SR,CU,O	
2765	JJP0281926			Tl0.8La1Sr1Cu1.2O5	Tl	0.8	La	1	Sr	1	Cu	1.2													O	5		1	1989																											2		P4/MMM			3.773		8.827													32		42				37																																																																																		44																			CRYSTAL STRUCTURE AND CHARACTERIZATION OF THE NEW TL(LA,SR)2 CUO5-TYPE SUPERCONDUCTOR	198911	XRY                 ,STRUCTURE           ,RESISTIVITY         ,SUSCEPTIVILITY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA,IBARAKI 305	JJAP LETT 28(1989)L1926	MASAYA WATAHIKI,TAKASHI MOCHIKU,TOSHIO NAGASHIMA,YUH FUKAI	TL,LA,SR,CU,O	
2766	JJP0281926			Tl0.6La1Sr1Cu1.4O5	Tl	0.6	La	1	Sr	1	Cu	1.4													O	5		1	1989																											2		P4/MMM			3.771		8.853													26		40				33																																																																																		80																			CRYSTAL STRUCTURE AND CHARACTERIZATION OF THE NEW TL(LA,SR)2 CUO5-TYPE SUPERCONDUCTOR	198911	XRY                 ,STRUCTURE           ,RESISTIVITY         ,SUSCEPTIVILITY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA,IBARAKI 305	JJAP LETT 28(1989)L1926	MASAYA WATAHIKI,TAKASHI MOCHIKU,TOSHIO NAGASHIMA,YUH FUKAI	TL,LA,SR,CU,O	
2767	JJP0281926			Tl0.4La1Sr1Cu1.6O5	Tl	0.4	La	1	Sr	1	Cu	1.6													O	5		1	1989																											2		P4/MMM			3.771		8.856													22		38				30																																																																																		153																			CRYSTAL STRUCTURE AND CHARACTERIZATION OF THE NEW TL(LA,SR)2 CUO5-TYPE SUPERCONDUCTOR	198911	XRY                 ,STRUCTURE           ,RESISTIVITY         ,SUSCEPTIVILITY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA,IBARAKI 305	JJAP LETT 28(1989)L1926	MASAYA WATAHIKI,TAKASHI MOCHIKU,TOSHIO NAGASHIMA,YUH FUKAI	TL,LA,SR,CU,O	
2768	JJP0281926			Tl0.7La1Sr1Cu1O5	Tl	0.7	La	1	Sr	1	Cu	1													O	5		1	1989																											2		P4/MMM			3.774		8.831													37		40				38.5																																																																																																					CRYSTAL STRUCTURE AND CHARACTERIZATION OF THE NEW TL(LA,SR)2 CUO5-TYPE SUPERCONDUCTOR	198911	XRY                 ,STRUCTURE           ,RESISTIVITY         ,SUSCEPTIVILITY	INSTITUTE OF MATERIALS SCIENCE,UNIVERSITY OF TSUKUBA,TSUKUBA,IBARAKI 305	JJAP LETT 28(1989)L1926	MASAYA WATAHIKI,TAKASHI MOCHIKU,TOSHIO NAGASHIMA,YUH FUKAI	TL,LA,SR,CU,O	
2769	PHC1750250		(Bi,Pb)2Sr2(Eu,Ca)Cu2O8	Bi1.55Pb0.45Sr2Eu0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Eu	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.489													91						91																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2770	PHC1750250		(Bi,Pb)2Sr2(Gd,Ca)Cu2O8	Bi1.55Pb0.45Sr2Gd0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Gd	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.685													93						93																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2771	PHC1750250		(Bi,Pb)2Sr2(Tb,Ca)Cu2O8	Bi1.55Pb0.45Sr2Tb0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Tb	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.181													94						94																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2772	PHC1750250		(Bi,Pb)2Sr2(Dy,Ca)Cu2O8	Bi1.55Pb0.45Sr2Dy0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Dy	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.407													95						95																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2773	PHC1750250		(Bi,Pb)2Sr2(Ho,Ca)Cu2O8	Bi1.55Pb0.45Sr2Ho0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Ho	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.51													94						94																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2774	PHC1750250		(Bi,Pb)2Sr2(Er,Ca)Cu2O8	Bi1.55Pb0.45Sr2Er0.2Ca0.8Cu2O8+Z	Bi	1.55	Pb	0.45	Sr	2	Er	0.2	Ca	0.8	Cu	2									O	8+Z		1	1991																											2	Bi2212						30.531													94						94																																																																																																					LANTHANIDE SUBSTITUTION INTO LOW HOLE CONCENTRATION BISMUTH SUPERCONDUCTORS			DEPARTMENT OF PHYSICS,FACULTY OF SCIENCE,MAHIDOL UNIVERSITY,BANGKOK 10400 ,THAILAND	PHYSICA C,175(1991)250	C.SOANKWAN,I.M.TANG,N.CHIENGPRATOOM,S.LEELAPRUTE	BI,PB,SR,CA,CU,O,R	
2775	PHC1750183		TlBa2CuO5	Tl1Ba2Cu1O5	Tl	1	Ba	2	Cu	1															O	5		1	1991																											2					3.859		9.261													95						95																																																																																																					STABILIZATION OF SUPERCONDUCTIVITY IN TLBA2CUO5-Z AT 9.5K ANDITS ENHANCEMENT TO 43 K IN TLBASRCUO5-Z			CHEMISTRY DIVISION,BHABHA ATOMIC RESERACH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,175(1991)183	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.LYER	TL,BA,CU,O,SR	
2776	PHC1750183		TlBaSrCuO5	Tl1Ba1Sr1Cu1O5	Tl	1	Ba	1	Sr	1	Cu	1													O	5		1	1991																											2					3.805		9.12													33		50				41.5																																																																																																					STABILIZATION OF SUPERCONDUCTIVITY IN TLBA2CUO5-Z AT 9.5K ANDITS ENHANCEMENT TO 43 K IN TLBASRCUO5-Z			CHEMISTRY DIVISION,BHABHA ATOMIC RESERACH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,175(1991)183	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.LYER	TL,BA,CU,O,SR	
2777	PHC1750183		TlBaSrCuO5	Tl1Ba1Sr1Cu1O5	Tl	1	Ba	1	Sr	1	Cu	1													O	5		1	1991																											2					3.805		9.12													43		70				56.5																																																																																																					STABILIZATION OF SUPERCONDUCTIVITY IN TLBA2CUO5-Z AT 9.5K ANDITS ENHANCEMENT TO 43 K IN TLBASRCUO5-Z			CHEMISTRY DIVISION,BHABHA ATOMIC RESERACH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,175(1991)183	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.LYER	TL,BA,CU,O,SR	
2778	PR04313042	520C IN O2-N2 ATMOSPHERE,QUENCH TO L-N2	YBa2Cu3O7	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	6.65	6.65	3	1991																											3	Y123																				62.2					62.2														25	83								380	87								8.7	2						20	4.5				3180	13600																																																								MAGNETIC MEASUREMENTS OF THE UPPER AND LOWER CRITICAL FIELDS OF OXYGEN-DEFICIENT YBA2CU3O7-Z SINGLE CRYSTALS	199106	MAGNETIZATION       ,SINGLE CRYSTALS     ,CRITICAL-FIELD	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.B,43(1991)13042	A.P.PAULIKAS,A.UMEZAWA,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.E.KESSLER,J.W.DOWNEY,J.Z.LIU,K.G.VANDERVOORT,U.WELP,W.K.KWOK	Y,BA,CU,O	
2779	PHC1750081	SPJUMP=MJ/MOLE.K2	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1991																											3	Y124				3.843	3.873	27.254														80				2.9	80																																																							16				467																																										SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY MEASUREMENTS OF YBA2CU4O8    A STUDY OF THE DENSITY OF ELECTRONIC STATE	199106	SPECIFIC HEAT       ,SUSCEPTIBILITY	SUPERCONDUVTIVITY RESEATCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KATK-KU,TOKYO135,JAPAN	PHYSICA C,175(1991)81	IZUMI TOMENO,J.O.WILLIS,KEISHI TAI,NAOKI KOSHIZUKA,SHOJI TANAKA,T.R.NICHOLS,TAKAO ITOH,TAKAYUKI MIYATAKE	Y,BA,CU,O	
2780	PHC1750081	SPJUMP=MJ/MOLE.K2	DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		1	1991						10.49	-6.4																				3	Y124				3.848	3.876	27.261														75				3.3	75																																																							15				445																																										SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY MEASUREMENTS OF YBA2CU4O8    A STUDY OF THE DENSITY OF ELECTRONIC STATE	199106	SPECIFIC HEAT       ,SUSCEPTIBILITY	SUPERCONDUVTIVITY RESEATCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KATK-KU,TOKYO135,JAPAN	PHYSICA C,175(1991)81	IZUMI TOMENO,J.O.WILLIS,KEISHI TAI,NAOKI KOSHIZUKA,SHOJI TANAKA,T.R.NICHOLS,TAKAO ITOH,TAKAYUKI MIYATAKE	Y,BA,CU,O	
2781	PHC1750081	SPJUMP=MJ/MOLE.K2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1991																											3	Y123																				90.7				5.8	90.7																																																							45				466																																										SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY MEASUREMENTS OF YBA2CU4O8    A STUDY OF THE DENSITY OF ELECTRONIC STATE	199106	SPECIFIC HEAT       ,SUSCEPTIBILITY	SUPERCONDUVTIVITY RESEATCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13,SHINONOME 1-CHOME,KATK-KU,TOKYO135,JAPAN	PHYSICA C,175(1991)81	IZUMI TOMENO,J.O.WILLIS,KEISHI TAI,NAOKI KOSHIZUKA,SHOJI TANAKA,T.R.NICHOLS,TAKAO ITOH,TAKAYUKI MIYATAKE	Y,BA,CU,O	
2782	JML0100210	GREEN PHASE(211)+YBC(123),COARSE GRAIN,SV(T)=2.21E+5 CM/S	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1991									4.98			GPa		60	GPa		24	GPa		38		0.237			377000		3	Y123																																																																																																																														Ultrasonic characterization of ceramic superconductors			Ultran Laboratories, Inc., State Cllege, PA 16801, USA	J.Material Science Lett.(1991)210-213	A.S. BHALLA,M.C. BHARDWAJ		
2783	JML0100210	70%YBCO+30%LOW-MELTING GLASS,COMPOSITE,MEDIUM GRAIN,SV(T)=1.96E+5 CM/S	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		2	1991									4.15			GPa		39	GPa		16	GPa		23.5		0.224			329000		3	Y123																				90					90																																																																																																					Ultrasonic characterization of ceramic superconductors			Ultran Laboratories, Inc., State Cllege, PA 16801, USA	J.Material Science Lett.(1991)210-213	A.S. BHALLA,M.C. BHARDWAJ		
2784	JML0100210	COMMERCIAL SINGLE PHASE,FINE GRAIN,SV(T)=2.06E+5 CM/S	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1991									5.37			GPa		93	GPa		38	GPa		58		0.231			449000		3	Y123																				87					87																																																																																																					Ultrasonic characterization of ceramic superconductors			Ultran Laboratories, Inc., State Cllege, PA 16801, USA	J.Material Science Lett.(1991)210-213	A.S. BHALLA,M.C. BHARDWAJ		
2785	JML0100210	FINE GRAIN,HIGH PURITY,HIGH DENSITY,SV(T)=2.54E+5 CM/S	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1991									5.58			GPa		92	GPa		36	GPa		69		0.279			450000		3	Y123																				93					93																																																																																																					Ultrasonic characterization of ceramic superconductors			Ultran Laboratories, Inc., State Cllege, PA 16801, USA	J.Material Science Lett.(1991)210-213	A.S. BHALLA,M.C. BHARDWAJ		
2786	PR0442757	R=EXP(T0/T)**N	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+Z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+Z		1	1991																											2	Tl2212				3.865		29.266													87	98					98																																																																																		15.1				0.00000000568					RH2786										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2787	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.9Y0.1Cu2O8+Z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.859		29.247																																																																																																					23									RH2787										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2788	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.8Y0.2Cu2O8+Z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.865		29.172													71	85					85																																																																																		19.8																			EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2789	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.75Y0.25Cu2O8+Z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.865		29.073													58	73.2					73.2																																																																																		38.4				0.00000000759					RH2789										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2790	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.7Y0.3Cu2O8+Z	Tl	2	Ba	2	Ca	0.7	Y	0.3	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.868		29.113													54.5	73.2					73.2																																																																																		47.3				0.00000000971					RH2790										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2791	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.65Y0.35Cu2O8+Z	Tl	2	Ba	2	Ca	0.65	Y	0.35	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.868		28.979													31.2	58					58																																																																																		68.7																			EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2792	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.6Y0.4Cu2O8+Z	Tl	2	Ba	2	Ca	0.6	Y	0.4	Cu	2											O	8+Z		1	1991																											2	Tl2212																			25	45					45																																																																																		113.9				0.0000000145					RH2792										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2793	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.52Y0.48Cu2O8+Z	Tl	2	Ba	2	Ca	0.52	Y	0.48	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.869		28.932														22					22																																																																																		172.1				0.0000000187					RH2793										EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2794	PR0442757		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.4Y0.6Cu2O8+Z	Tl	2	Ba	2	Ca	0.4	Y	0.6	Cu	2											O	8+Z		1	1991																											2	Tl2212				3.878		28.926																	23																																																																																																							EFFECT OF CARRIER CONCENTRATION ON THE NORMAL TRANSPORT PROPERTIES AND THE SUPERCONDUCTING TRANSITION TEMPERATURE IN THE TL2BA2CA1-XYXCU2O8+Y SYSTEM	199108		SAHA ONSTITUTE OF NUCLEAR PHYSICS,SECTOR I,BLOCK AF,BIDHGANNAGAR,CALCUTTA 700 064,INDIA	PHYS.REV.B,44(1991)2757	A.N.DAS,A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAL	TL,BA,CA,Y,CU,O	
2795	PR04313606	HALL COEFF. IN PLANE	(Nd,Ce)2CuO4	Nd1.89Ce0.11Cu1O3.97	Nd	1.89	Ce	0.11	Cu	1															O	4-Z	3.97	3	1991																												T'																																																																																																															0.00000000161					RH2795										IN-PLANE TRANSPORT PROPERTIES OF SINGLE-CRYSTAL R2-XCEXCUO4-Y(R=ND,SM)			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND 20742-4111	PHYS.REV.43(1991)13606	J.L.PENG,R.L.GREENE,S.J.HAGEN,Z.Y.LI		
2796	PR04313606	HALL COEFF. IN PLANE	(Nd,Ce)2CuO4	Nd1.86Ce0.14Cu1O4-Z	Nd	1.86	Ce	0.14	Cu	1															O	4-Z		3	1991																												T'																				21.7					21.7																																																																																						0.00000000051					RH2796										IN-PLANE TRANSPORT PROPERTIES OF SINGLE-CRYSTAL R2-XCEXCUO4-Y(R=ND,SM)			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND 20742-4111	PHYS.REV.43(1991)13606	J.L.PENG,R.L.GREENE,S.J.HAGEN,Z.Y.LI		
2797	PR04313606	HALL COEFF. IN PLANE	(Nd,Ce)2CuO4	Nd1.83Ce0.17Cu1O4-Z	Nd	1.83	Ce	0.17	Cu	1															O	4-Z		3	1991																												T'																				23.3					23.3																																																																																						0.00000000061					RH2797										IN-PLANE TRANSPORT PROPERTIES OF SINGLE-CRYSTAL R2-XCEXCUO4-Y(R=ND,SM)			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND 20742-4111	PHYS.REV.43(1991)13606	J.L.PENG,R.L.GREENE,S.J.HAGEN,Z.Y.LI		
2798	PR04313606	HALL COEFF. IN PLANE	(Nd,Ce)2CuO4	Nd1.78Ce0.22Cu1O4-Z	Nd	1.78	Ce	0.22	Cu	1															O	4-Z		3	1991																												T'																																																																																																																				RH2798										IN-PLANE TRANSPORT PROPERTIES OF SINGLE-CRYSTAL R2-XCEXCUO4-Y(R=ND,SM)			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND 20742-4111	PHYS.REV.43(1991)13606	J.L.PENG,R.L.GREENE,S.J.HAGEN,Z.Y.LI		
2799	PR04313102	LATB IS SLIGHTLY LARGER THAN LATA	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		1	1991																											3	Bi2212				5.388		30.82													65.5	70.8					70.8																																																																																						0.0000000016					RH2799										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2800	PR04313102		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		1	1991																											3	Bi2212																			82.7	85.8					85.8																																																																																						0.00000000199					RH2800										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2801	PR04313102		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.75Y0.25Cu2O8+Z	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	2											O	8+Z		1	1991																											3	Bi2212				5.402		30.672													70.8	86.3					86.3																																																																																						0.00000000245					RH2801										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2802	PR04313102		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.65Y0.35Cu2O8+Z	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	2											O	8+Z		1	1991																											3	Bi2212				5.407		30.527													54.9	79.6					79.6																																																																																						0.00000000269					RH2802										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2803	PR04313102		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8+Z	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+Z		1	1991																											3	Bi2212				5.424		30.473																																																																																																									0.0000000041					RH2803										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2804	PR04313102		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.55Y0.45Cu2O8+Z	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	2											O	8+Z		1	1991																											3	Bi2212				5.414		30.402													38	54.9					54.9																																																																																						0.00000000596					RH2804										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2805	PR04313102		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.45Y0.55Cu2O8+Z	Bi	2	Sr	2	Ca	0.45	Y	0.55	Cu	2											O	8+Z		1	1991																											3	Bi2212				5.421		30.351																																																																																																									0.0000000092					RH2805										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2806	PR04313102	2223 DOMINANT,A=5.396,B=5.388,C=30.730 FOR LOW-TC PHASE	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.75Pb0.25Sr2Ca2Cu3O10+Z	Bi	1.75	Pb	0.25	Sr	2	Ca	2	Cu	3											O	10+Z		2	1991																											3	Bi2223																			103						103																																																																																						0.00000000395					RH2806										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2807	PR04313102		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.7Pb0.3Sr2Ca2Cu3O10+Z	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	10+Z		2	1991																												Bi2223																			107						107																																																																																						0.00000000313					RH2807										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2808	PR04313102		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.66Pb0.34Sr2Ca2Cu3O10+Z	Bi	1.66	Pb	0.34	Sr	2	Ca	2	Cu	3											O	10+Z		2	1991																												Bi2223																			100						100																																																																																						0.00000000286					RH2808										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2809	PR04313102		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.65Pb0.35Sr2Ca2Cu3O10+Z	Bi	1.65	Pb	0.35	Sr	2	Ca	2	Cu	3											O	10+Z		2	1991																												Bi2223																			93						93																																																																																						0.00000000211					RH2809										VARIATION OF TC AND TRANSPORT PROPERTIES WITH CARRIER CONCENTRATION IN Y-AND PB-DOPED BI-BASED SI@ERCONDUCTORS	199106		SAHA INSTITUTE OF NUCLEAR PHYSICS,92 ACHARYA CHANDRA ROAD,CALCUTTA 700 009,INDIA	PHYS.REV.B,43(1991)13102	A.PODDAR,B.GHOSH,P.CHOUDHURY,P.MANDAI	Y,PB,BI,SR,CA,CU,O	
2810	PHC1750587		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.85Zn0.15O7	Er	1	Ba	2	Cu	2.85	Zn	0.15													O	7		1	1991																											3	Y123				3.81	3.881	11.629													53		57				55																																																																																											RH2810										NEUTRON SPECTROSCOPIC STUDIES OF CRYSTALLINE ELECTRIC FIELDS IN HIGH-TC ERBA2CU3O7 DOPED WITH ZN AND NI			INSTITUTE FOR METAL PHYSICS,USSR ACADEMY OF SCIENCES, URAL BRANCH,SVERDLOVSK GSP-170,USSR	PHYSICA C,175(1991)587	A.D.TAYLOR,A.FURRER,A.MIRMELSTEIN,A.PODLESNYAK,J.MESOT,P.ALLENSPACH,R.OSBORN,S.M.BENNINGTN,U.STAUB,V.KOZHEVNIKOV	ER,BA,CU,O,ZN,NI	
2811	PHC1750587		ErBa2(Cu,Ni)3O7	Er1Ba2Cu2.82Ni0.18O7	Er	1	Ba	2	Cu	2.82	Ni	0.18													O	7		1	1991																											3	Y123				3.812	3.874	11.601													53		77				65																																																																																						0.00000000145					RH2811										NEUTRON SPECTROSCOPIC STUDIES OF CRYSTALLINE ELECTRIC FIELDS IN HIGH-TC ERBA2CU3O7 DOPED WITH ZN AND NI			INSTITUTE FOR METAL PHYSICS,USSR ACADEMY OF SCIENCES, URAL BRANCH,SVERDLOVSK GSP-170,USSR	PHYSICA C,175(1991)587	A.D.TAYLOR,A.FURRER,A.MIRMELSTEIN,A.PODLESNYAK,J.MESOT,P.ALLENSPACH,R.OSBORN,S.M.BENNINGTN,U.STAUB,V.KOZHEVNIKOV	ER,BA,CU,O,ZN,NI	
2812	PHC1750523	247,123 ,OTHER IMPURITY PFASESEXIST	EuBa2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8			1991																												Y124				3.868	3.882	27.271													63	67	69				67																																																																																																					SYNTHESIS OF LNBA2CU4O8 (LN=RARE EARTH ELEMENTS) CERAMICS AT ONE ATMOSPHERE OXZGEN PRESSURE			CENTRAL RESEARCH LABORATORIES,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.,3-15 YAGUMO-NAKAMACHI,MORIGUCHI,OSAKA 570,JAPAN	PHYCICA C,175(1991)523	HIDEAKI ADACHI,KENTARO SETSUNE,KIYOTAKA WASA,SEIJI ADACHI	R,BA,CU,O	
2813	PHC1750523		GdBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8			1991																												Y124				3.861	3.881	27.257													66	69	72				69																																																																																																					SYNTHESIS OF LNBA2CU4O8 (LN=RARE EARTH ELEMENTS) CERAMICS AT ONE ATMOSPHERE OXZGEN PRESSURE			CENTRAL RESEARCH LABORATORIES,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.,3-15 YAGUMO-NAKAMACHI,MORIGUCHI,OSAKA 570,JAPAN	PHYCICA C,175(1991)523	HIDEAKI ADACHI,KENTARO SETSUNE,KIYOTAKA WASA,SEIJI ADACHI	R,BA,CU,O	
2814	PHC1750523		DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8			1991																												Y124				3.847	3.874	27.239													70	71	74				71																																																																																																					SYNTHESIS OF LNBA2CU4O8 (LN=RARE EARTH ELEMENTS) CERAMICS AT ONE ATMOSPHERE OXZGEN PRESSURE			CENTRAL RESEARCH LABORATORIES,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.,3-15 YAGUMO-NAKAMACHI,MORIGUCHI,OSAKA 570,JAPAN	PHYCICA C,175(1991)523	HIDEAKI ADACHI,KENTARO SETSUNE,KIYOTAKA WASA,SEIJI ADACHI	R,BA,CU,O	
2815	PHC1750523		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1991																												Y124				3.841	3.868	27.214													72	74	77				74																																																																																																					SYNTHESIS OF LNBA2CU4O8 (LN=RARE EARTH ELEMENTS) CERAMICS AT ONE ATMOSPHERE OXZGEN PRESSURE			CENTRAL RESEARCH LABORATORIES,MATSUSHITA ELECTRIC INDUSTRIAL CO.,LTD.,3-15 YAGUMO-NAKAMACHI,MORIGUCHI,OSAKA 570,JAPAN	PHYCICA C,175(1991)523	HIDEAKI ADACHI,KENTARO SETSUNE,KIYOTAKA WASA,SEIJI ADACHI	R,BA,CU,O	
2816	PHC1750407		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	3	1991																												Y123																																							230	950																																																																																						ANISOTROPY OF THE FIRST CRITICAL FIELD AND CRITICAL CURRENT INYBA2CU3O6.9 SINGLE CRYSTALS			CENTRE D'ENTUDES NUCLEAIRES,DRF/SPH-MDN (#DRF/SBT-LCP)85X,38041 GRENOBLE CEDEX,FRANCE	PHYSICA C,175(1991)407	C.MARIN,J.F.JACQUOT,J.ROSSAT-MIGNOD,J.Y.HENRY,V.V.MOSHCHALKOV	Y,BA,CU,O	
2817	PR04313073	GAMMA,DEBYE FROM SPHEAT,2-4 K FITTING,	YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	6.7	6.7	1	1991		0.000002478	K	0.0001399					4.75																		3	Y123				3.822	3.888	11.663														67					67										33																																											SP2817				4.71		392																																										LOW-TEMPERETURE SPECIFIC HEAT OF POLYCRYSTALLINE YBA2CU3O6.7 IN APPLIED MAGNETIC FIELDS OF 0,1,2,AND 3 T	199106		DEPARTMENTOF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILL	Phys. Rev. B., 43(1991)13073	D.J.VAN HARLINGEN,D.M.GINSBERG,J.P.RICE,R.A.SCHWEINFURTH,S.E.STUPP,T.A.FRIEDMANN	Y,BA,CU,O	
2818	PHC1780110		Bi2Sr2CuO6	Bi2Sr2Cu1O6+Z	Bi	2	Sr	2	Cu	1															O	6+Z			1991																												Bi2201																				9.8					9.8																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2819	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z			1991																												Bi2201																				13.3					13.3																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2820	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.8La0.2Cu1O6+Z	Bi	2	Sr	1.8	La	0.2	Cu	1													O	6+Z			1991																												Bi2201																				16.2					16.2																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2821	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.7La0.3Cu1O6+Z	Bi	2	Sr	1.7	La	0.3	Cu	1													O	6+Z			1991																												Bi2201																				17.8					17.8																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2822	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+Z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z			1991																												Bi2201																				19.1					19.1																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2823	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6+Z	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+Z			1991																												Bi2201																							4.2																																																																																																							SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2824	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.4La0.6Cu1O6+Z	Bi	2	Sr	1.4	La	0.6	Cu	1													O	6+Z			1991																												Bi2201																							4.2																																																																																																							SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2825	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1.2La0.8Cu1O6+Z	Bi	2	Sr	1.2	La	0.8	Cu	1													O	6+Z			1991																												Bi2201																							4.2																																																																																																							SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2826	PHC1780110		Bi2(Sr,La)2CuO6	Bi2Sr1La1Cu1O6+Z	Bi	2	Sr	1	La	1	Cu	1													O	6+Z			1991																												Bi2201																							4.2																																																																																																							SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2827	PHC1780110		(Bi,Pb)2(Sr,La)2CuO6	Bi1.9Pb0.1Sr1.9La0.1Cu1OY	Bi	1.9	Pb	0.1	Sr	1.9	La	0.1	Cu	1											O	Y			1991																												Bi2201				5.356	5.371	24.625														16					16																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2828	PHC1780110		(Bi,Pb)2(Sr,La)2CuO6	Bi1.8Pb0.2Sr1.8La0.2Cu1OY	Bi	1.8	Pb	0.2	Sr	1.8	La	0.2	Cu	1											O	Y			1991																												Bi2201				5.352	5.38	24.6														21					21																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2829	PHC1780110		(Bi,Pb)2(Sr,La)2CuO6	Bi1.7Pb0.3Sr1.7La0.3Cu1OY	Bi	1.7	Pb	0.3	Sr	1.7	La	0.3	Cu	1											O	Y			1991																												Bi2201				5.334	5.386	24.561														23					23																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2830	PHC1780110		(Bi,Pb)2(Sr,La)2CuO6	Bi1.6Pb0.4Sr1.6La0.4Cu1OY	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	1											O	Y			1991																												Bi2201				5.322	5.399	24.497														26					26																																																																																																					SUPERCONDUCTIVITY OF BI-2201 (N=1) AS INFLUENCED BY THE SUBSTITUTION OF PB AND/OR RARE-EARTHS (R=LA,ND AND PR)			CHEMISTRY DIVISION,BHABHA ATOMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,178(1991)110	C.K.SUBRAMANIAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN	BI,SR,CU,O,LA,ND,PR	
2831	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.7La0.3Cu1O5-Y	Tl	1	Ba	1.7	La	0.3	Cu	1													O	5-Y		1	1991																											2	Tl1201																				42					42																																																																																																					STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2832	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.6La0.4Cu1O5-Y	Tl	1	Ba	1.6	La	0.4	Cu	1													O	5-Y		1	1991																											2	Tl1201				3.848		9.234														39.1					39.1																																																																																																					STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2833	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.5La0.5Cu1O5-Y	Tl	1	Ba	1.5	La	0.5	Cu	1													O	5-Y		1	1991																											2	Tl1201				3.847		9.195														33.3					33.3																																																																																																					STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2834	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.4La0.6Cu1O5-Y	Tl	1	Ba	1.4	La	0.6	Cu	1													O	5-Y		1	1991																											2	Tl1201				3.844		9.104														23.5					23.5																																																																																																					STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2835	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5-Y	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5-Y		1	1991																											2	Tl1201				3.84		9.064																	20																																																																																																							STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2836	PHC1780075	MEASURED UP TO 9GPA.TC SATURATE ABOVE 5GPA(TC-108K)	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1991																												Y124																												K/GPa	5.5																																																																																																	THE SUPERCONDUCTING PROPERTIES OF YBA2CU4O8 SINGLE CTYSTALS UNDER HYDROSTATIC PRESSURE (UP TO 9.5 GPA)			SERVICE NATIONAL DES CHANPS INTENSES,CNRS,166X,38042 GRENOBLECODEX,FRANCE	PHYSICA C,178(1991)75	D.BRAITHWAITE,E.JILEK,E.KALDIS,G.CHOUTEAU,G.MARTINEZ,J.KARPINSKI,J.L.HODEAU,M.MAREZIO,S.RUSIECKI	Y,BA,CU,O	
2837	SSC0760923		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4			1990																											2	T				3.793		13.297																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2838	SSC0760923		(La,Ba)2(Cu,Li)O4	La1.87Ba0.13Cu0.99Li0.01O4	La	1.87	Ba	0.13	Cu	0.99	Li	0.01													O	4			1990																											2	T				3.79		13.3																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2839	SSC0760923		(La,Ba)2(Cu,Li)O4	La1.87Ba0.13Cu0.98Li0.02O4	La	1.87	Ba	0.13	Cu	0.98	Li	0.02													O	4			1990																											2	T				3.787		13.279																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2840	SSC0760923		(La,Ba)2(Cu,Li)O4	La1.87Ba0.13Cu0.96Li0.04O4	La	1.87	Ba	0.13	Cu	0.96	Li	0.04													O	4			1990																											2	T				3.789		13.284																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2841	SSC0760923		(La,Ba)2(Cu,Li)O4	La1.87Ba0.13Cu0.94Li0.06O4	La	1.87	Ba	0.13	Cu	0.94	Li	0.06													O	4			1990																											2	T				3.785		13.282																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2842	SSC0760923		(La,Ba)2(Cu,Li)O4	La1.87Ba0.13Cu0.92Li0.08O4	La	1.87	Ba	0.13	Cu	0.92	Li	0.08													O	4			1990																											2	T				3.786		13.284																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2843	SSC0760923		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4		1	1990																											2	T				3.796		13.257																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2844	SSC0760923		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4		1	1990																											2	T				3.792		13.259																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2845	SSC0760923		(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4		1	1990																											2	T				3.795		13.288																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2846	SSC0760923		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1990																											2	T				3.792		13.291																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2847	SSC0760923		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4		1	1990																											2	T				3.792		13.298																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2848	SSC0760923		(La,Ba)2CuO4	La1.865Ba0.135Cu1O4	La	1.865	Ba	0.135	Cu	1															O	4		1	1990																											2	T				3.791		13.292																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2849	SSC0760923		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4		1	1990																											2	T				3.793		13.301																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2850	SSC0760923		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4		1	1990																											2	T				3.789		13.302																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2851	SSC0760923		(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4		1	1990																											2	T				3.788		13.302																																																																																																																								ON THE POSSIBLE MECHANISM OF THE SUCCESSIVE STRUCTURAL TRANSITIONS OF LA2-XBAXCUO4: STUDY BY THE LI SUBSTITUTION FOR CU	199011		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE, NAGOYA UNIVERSITY,CHIKUSA-KU, NAGOYA 464-01, JAPAN	SOLID STATE COMMUN.,76(1990)923	M.SATO,M.SERA,S.SHAMOTO	LA,BA,CU,O	
2852	PRL0640599	POSITIVE CURVATURE,ANISOTROPIC FACTOR=5	(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-Y	Sm	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																				11.4				2.7	11.4										43													28.2	5.23								3.6	0.1						79	14.7																																						0.38				1																			UPPER CRITICAL FIELD OF A SM1.85CE0.15CUO4-Y SINGLE CRYSTAL: INTERACTION BETWEEN SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDER IN COPPERCOXIDES	199001		DEPARTMENT OF PHYSICS,AND INSTITUTE FOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SAN DIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.LETT.,64(1990)599	B.Q.LEE,C.L.SEAMAN,J.T.MARKERT,M.B.MAPLE,Y.DALICHAOUCH	SM,CE,CU,O	
2853	PR0410300	USING PB REFERENCE LEADS.PEAK AROUND TC COMES FROM FLUCTUATION EFFECT.SIGN OF TEP SHOWS ELECTRON LIKE FERMI SURFACE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1990																											3	Y123																				92.6					92.6																																																																																																					ANOMALOUS PEAK IN THE THERMOPOWER OF YBA2CU3O7-Z SINGLE CRYSTALS: A POSSIBLE FLUCTUATION EFFECT	199001	THERMOPOWRE         ,FLUCTUATION         ,SINGLE CRYSTALS:	DEPARTMENT OF PHYSICS, UNIVERSITY OF LEEDS, LEEDS LS2 9JT, UNITED KINGDOM	PHYS.REV.B,41(1990)300	D.GINSBERG,J.P.RICE,M.A.HOWSON,MAB.SALAMON,T.A.FRIEDMANN	Y,BA,CU,O	
2854	PR04111029	// MEANS TEMPERATURE GRADIENT//H,FIG=S//,H=0,5T	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.76Pb0.24Sr2Ca2Cu3OZ	Bi	1.76	Pb	0.24	Sr	2	Ca	2	Cu	3											O	Z		1	1990																												Bi2223																			108.5						108.5																																																																																																					UNUSUAL SEEBECK AND NERNST EFFECTS IN THE MIXED STATE OF BI2-XPBXSR2CA2CU3OZ	199011		II. PHYSIKALISCHES INSTITUT, UNIVERSITAT KOLN, 5000 KOLN 41, WEST GERMANY	PHYS.REV.B,41(1990)11029	A.FREIMUTH,M.GALFFY,U.MUREK	BI,PB,SR,CA,CU,O	
2855	SSC0660445	GREEN PHASE<5%		Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123																			89.5	90.4					90.4																																																																						TP2855																															THERMOELECTRIC POWER AND MAGNETO SEEBECK-EFFECT NEAR THE CRITICAL TEMPERATURE OF GRANULAR CERAMIC OXIDE SUPERCONDUCTORS Y1Ba2Ca3O7-y			Institut de Physique B5, Universite' de Lie'ge, Sart Tilman B-4000 Lie'ge, Belgium	Solid Stste Commun.,66(1988)445-450	A. Rulmont,Ch. Laurent,H.W. Vanderschueren,M. Ausloos,M. Laguesse,R. Tarte,S.K. Patapis		
2856	PRB0408814			Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1989																												Bi2212																				85					85																																																																						TP2856																															MAGNETIC FIELD DEPENDENCE OF THE THERMOELECTRIC POWER OF SUPERCONDUCTING BI-SR-CA-CU-O	198911	MAGNETIC FIELD      ,THERMOPOWER	DEPARTMENT OF PHYSICS, MCMASTER UNIVERSITY, HAMILTON, ONTARIO,CANADA L8S 4M1	PHYS.REV.B,40(1989)8814	C. G. TRENDALL,J. D. GARRETT,P. PERNAMBUCO-WISE,VLADIMIR V.,W. R. DATARS	BI,SR,CA,CU,O	
2857	PHC1780029		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.8Nd0.2Cu2O6.86	Tl	1	Ba	2	Ca	0.8	Nd	0.2	Cu	2											O	7-Z	6.86	1	1991																											2	Tl1212	P4/MMM			3.856		12.653														100					100										60																																																																																											"MEUTRON DIFFRACTION STRUCTURE DETERMINATION OF THE ""1212"" -SERIES TLBA2CA1-XCU2O7-Z"			LABORATOIRE DE CRISTALLOGRAPHIE ET SCIENCES DES MATERIAUX,CRISMAT,ISMRA,BOULEVARD DU MARECHAL JUIN,14050 CAEN CEDEX,FRANCE	PHYSICA C,178(1991)29	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,E.SUARD,M.HERVIEU,V.CAIGNAERT	TL,BA,CA,ND,CU,O	
2858	PHC1780029		TlBa2(Ca,Nd)Cu2O7	Tl1Ba2Ca0.5Nd0.5Cu2O6.86	Tl	1	Ba	2	Ca	0.5	Nd	0.5	Cu	2											O	7-Z	6.86	1	1991																											2	Tl1212	P4/MMM			3.877		12.604														40					40										30																																																																																											"MEUTRON DIFFRACTION STRUCTURE DETERMINATION OF THE ""1212"" -SERIES TLBA2CA1-XCU2O7-Z"			LABORATOIRE DE CRISTALLOGRAPHIE ET SCIENCES DES MATERIAUX,CRISMAT,ISMRA,BOULEVARD DU MARECHAL JUIN,14050 CAEN CEDEX,FRANCE	PHYSICA C,178(1991)29	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,E.SUARD,M.HERVIEU,V.CAIGNAERT	TL,BA,CA,ND,CU,O	
2859	PHC1780029		TlBa2NdCu2O7	Tl1Ba2Nd1Cu2O6.96	Tl	1	Ba	2	Nd	1	Cu	2													O	7-Z	6.96	1	1991																											2	Tl1212	P4/MMM			3.91		12.492																	4.2																																																																																																							"MEUTRON DIFFRACTION STRUCTURE DETERMINATION OF THE ""1212"" -SERIES TLBA2CA1-XCU2O7-Z"			LABORATOIRE DE CRISTALLOGRAPHIE ET SCIENCES DES MATERIAUX,CRISMAT,ISMRA,BOULEVARD DU MARECHAL JUIN,14050 CAEN CEDEX,FRANCE	PHYSICA C,178(1991)29	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,E.SUARD,M.HERVIEU,V.CAIGNAERT	TL,BA,CA,ND,CU,O	
2860	PHC1760257	AC RESISTIVITY,16HZ INSULATOR	(La,Ce)2CuO4	La1.85Ce0.15Cu1O4-Z	La	1.85	Ce	0.15	Cu	1															O	4-Z			1991																																																																																																																																																										SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2861	PHC1760257		(La,Ce)2(Cu,Ag)O4	La1.85Ce0.15Cu0.9Ag0.1O4-Z	La	1.85	Ce	0.15	Cu	0.9	Ag	0.1													O	4-Z			1991																																																	22				22																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2862	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.8Ag0.2O4-Z	La	1.85	Ce	0.15	Cu	0.8	Ag	0.2													O	4-Z			1991																																															12.9	16.5	22.7				16.5																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2863	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.7Ag0.3O4-Z	La	1.85	Ce	0.15	Cu	0.7	Ag	0.3													O	4-Z			1991																																															9.9	17.2	22				17.2																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2864	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.6Ag0.4O4-Z	La	1.85	Ce	0.15	Cu	0.6	Ag	0.4													O	4-Z			1991																																															15.3	19	21.8			7	19																						3.2									0.24																																																																						SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2865	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.55Ag0.45O4-Z	La	1.85	Ce	0.15	Cu	0.55	Ag	0.45													O	4-Z			1991																																															7.4	17.1	19				17.1																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2866	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.5Ag0.5O4-Z	La	1.85	Ce	0.15	Cu	0.5	Ag	0.5													O	4-Z			1991																																															8.4	15.2	18.7				15.2																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2867	PHC1760257		(La,Ce)2CuO4	La1.85Ce0.15Cu0.4Ag0.6O4-Z	La	1.85	Ce	0.15	Cu	0.4	Ag	0.6													O	4-Z			1991																																																	11.1				11.1																																																																																																					SUPERCONDUCTIVITY IN THE LA1.85CE0.15CU1-XAGXO4-Z SYSTEM			DEPARTMENT OF PHYSICS,NATIONAL RAIWAN UNIVERSITY,TAIPEI,TAIWAN	PHYSICA C,176(1991)257	FU-AN YANG,J.W.CHEN	LA,CE,CU,AG,O	
2868	PHC1780193		Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5-Z	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5-Z		1	1991																											2	Tl1201																				35.9					35.9																																																																																																					STUDIES OF THE SUPERCONDUCTING BEHAVIOUR OF TLBA2-XLAXCUO5-Y			DEPARTMENT OF CHEMISTRY,INDIAN INSTITUTE OF TECHNOLOGY,BOMBAY400076,INDIA	PHYSICA C,178(1991)193	A.K.RAJARAJAN,A.SUNDARESAN,L.C.GUPTA,M.SHARON,R.VIJAYATAGHAVAN	TL,BA,CU,O,LA	
2869	PR0433020	MAGNETORESISTANCE POSITIVE,RH AT VARIOUS FIELD,	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.97	Nd	1.85	Ce	0.15	Cu	1															O	4	3.97		1991																												T'																				20					20										60																																																																	0.8								1.5								RH2869										POSITIVE COEFFICIENT OBSERVED IND SINGLE-CRYSTAL ND2-XCEXCUO4-Z AT LOW TEMPERATURES	199102		JOSEPH HENRY LABORATORIES OF PHYSICS, PRINCETON UNIVERSITY, PRINCETON, NEW JERSEY 08544	PHYS.REV.B,43(1991)3020	E.WANG,J.M.TARASCON,N.P.ONG,T.R.CHIEN,Z.Z.WANG	ND,CE,CU,O	
2870	APJ0291632			La1.85Ca0.989Sr0.161Cu2O5.93	La	1.85	Ca	0.989	Sr	0.161	Cu	2													O	5.93	5.93		1990																											2					3.825		19.51														13					13																																																																																																					Preparation and Superconducting Properties of La2-x(Ca1-ySry)1+xCu2O6-x/2+delta	9		NTT Basic Research Laboratories, Midori-cho, Musashino-shi, Tokyo 180	Japanese J.Appl.Phys.29(1990)L1632-L1634	Hiroyuki SHIBATA,Kyoichi KINOSHITA,Tomoaki YAMADA		
2871	APJ0291632			La1.83Ca1.006Sr0.164Cu2O6.08	La	1.83	Ca	1.006	Sr	0.164	Cu	2													O	6.08	6.08		1990																											2					3.824		19.505														14.1					14.1																																																																																																					Preparation and Superconducting Properties of La2-x(Ca1-ySry)1+xCu2O6-x/2+delta	9		NTT Basic Research Laboratories, Midori-cho, Musashino-shi, Tokyo 180	Japanese J.Appl.Phys.29(1990)L1632-L1634	Hiroyuki SHIBATA,Kyoichi KINOSHITA,Tomoaki YAMADA		
2872	APJ0291632			La1.8Ca1.032Sr0.168Cu2O6.08	La	1.8	Ca	1.032	Sr	0.168	Cu	2													O	6.08	6.08		1990																											2					3.824		19.505														15					15																																																																																																					Preparation and Superconducting Properties of La2-x(Ca1-ySry)1+xCu2O6-x/2+delta	9		NTT Basic Research Laboratories, Midori-cho, Musashino-shi, Tokyo 180	Japanese J.Appl.Phys.29(1990)L1632-L1634	Hiroyuki SHIBATA,Kyoichi KINOSHITA,Tomoaki YAMADA		
2873	PR0444526	magnetic properties for H perpendicular for c-axis.	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O6.85	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7-Z	6.85		1991	cm3/mol	0.0000001					-21																				3	Y123				3.821	3.889	11.724														85					85																																																																																																					MAGNETIC AND STRUCTURAL PROPERTIES OF FE IN SINGLE CRYSTALS OFYBA2CU3-XFEXO7-Z	199109		DEPARTMENT OF CHEMISTRY,NORTHERN ILLINOIS UNIVERSITY,DEKALB,ILLINOIS 60115	PHYS.REV.B,44(1991)4526	A.UMEZAWA,G.W.CRABTREE,K.VANDERVOORT,L.NUNEZ,R.D.ROGERS,U.FANG,U.WELP	Y,BA,CU,FE,O	
2874	PR0444526	magnetic properties for H perpendicular for c-axis.	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.91Fe0.09O6.83	Y	1	Ba	2	Cu	2.91	Fe	0.09													O	7-Z	6.83		1991	cm3/mol	0.0000016			myu-B/mol	1.015	-25																				3	Y123				3.83	3.875	11.734														60					60																																																																																																					MAGNETIC AND STRUCTURAL PROPERTIES OF FE IN SINGLE CRYSTALS OFYBA2CU3-XFEXO7-Z	199109		DEPARTMENT OF CHEMISTRY,NORTHERN ILLINOIS UNIVERSITY,DEKALB,ILLINOIS 60115	PHYS.REV.B,44(1991)4526	A.UMEZAWA,G.W.CRABTREE,K.VANDERVOORT,L.NUNEZ,R.D.ROGERS,U.FANG,U.WELP	Y,BA,CU,FE,O	
2875	PR0444526	magnetic properties for H perpendicular for c-axis.	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7.02	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-Z	7.02		1991	cm3/mol	0.0000012			myu-B/mol	1.192	-27.4																				3	Y123				3.846	3.855	11.709														76					76																																																																																																					MAGNETIC AND STRUCTURAL PROPERTIES OF FE IN SINGLE CRYSTALS OFYBA2CU3-XFEXO7-Z	199109		DEPARTMENT OF CHEMISTRY,NORTHERN ILLINOIS UNIVERSITY,DEKALB,ILLINOIS 60115	PHYS.REV.B,44(1991)4526	A.UMEZAWA,G.W.CRABTREE,K.VANDERVOORT,L.NUNEZ,R.D.ROGERS,U.FANG,U.WELP	Y,BA,CU,FE,O	
2876	PR0444526	magnetic properties for H perpendicular for c-axis.	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.76Fe0.24O7-Z	Y	1	Ba	2	Cu	2.76	Fe	0.24													O	7-Z			1991	cm3/mol	0.0000045			myu-B/mol	1.269	-14.8																				2	Y123				3.854	3.858	11.718														49					49																																																																																																					MAGNETIC AND STRUCTURAL PROPERTIES OF FE IN SINGLE CRYSTALS OFYBA2CU3-XFEXO7-Z	199109		DEPARTMENT OF CHEMISTRY,NORTHERN ILLINOIS UNIVERSITY,DEKALB,ILLINOIS 60115	PHYS.REV.B,44(1991)4526	A.UMEZAWA,G.W.CRABTREE,K.VANDERVOORT,L.NUNEZ,R.D.ROGERS,U.FANG,U.WELP	Y,BA,CU,FE,O	
2877	PHC1770271	N=1,2,3,4,5,7 PHASES ARE EXIST,67VOL%= N=3 PHASE	Bi2Sr2Ca3Cu4OZ	Bi2Sr2Ca3Cu4OZ	Bi	2	Sr	2	Ca	3	Cu	4													O	Z		2	1991																												Bi2234				5.4		37														110.9					110.9																																																																																																					STRUCTURAL SNALYSIS AND SUPERCONDUCTINGPROPERTIES OF PB-FREE BI2SR2CA3CU4OY (N=4,NOMINAL COMPOSITION)			INSTITUT FUR ANORGANISCHE CHEMIE DER UNIVERSITAT,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,177(1991)271	H.BUDOM,M.HARTMANN,M.RYGULA,O.EIBL,R.P.HUEBENER,S.KEMMLER-SACK,S.LOSCH,T.RENTSCHLER	PB,BI,SR,CA,CU,O	
2878	PHC1770373	MECHANICAL PROPTY BY SOUND VELOCITY,VL(5K)=2.26(KM/S),VT(5K)=1.46	Bi2Sr2CuO6	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O	6		1	1991									5.36				25			11			12		0.14			0.251				Bi2201																				8.9				4.4	8.9																																																																																																					VELOCITY AND ATTENUATION OF ULTRASOUND IN THE BI2SR2CUO6 SUPERCONDUCTOR			INSTITUTE OF PHYSICS,CZEOCHOSL.ACAD.SCI.,NA SLAVANCE 2,18040 PRAHA 8,CZECHOSLOVAKIA	PHYSICA C,177(1991)373	C.LAERMANS,C.PLECHACEK,J.DOMINEC	BI,SR,CU,O	
2879	PHC1770373	MECHANICAL PROPTY BY SOUND VELOCITY,VL(5K)=1.84(KM/S),VT(5K)=1.46	Bi2Sr2CuO6	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O	6		1	1991									5.04				29			14			11		0.55			0.251				Bi2201																				8				5.1	8																																																																																																					VELOCITY AND ATTENUATION OF ULTRASOUND IN THE BI2SR2CUO6 SUPERCONDUCTOR			INSTITUTE OF PHYSICS,CZEOCHOSL.ACAD.SCI.,NA SLAVANCE 2,18040 PRAHA 8,CZECHOSLOVAKIA	PHYSICA C,177(1991)373	C.LAERMANS,C.PLECHACEK,J.DOMINEC	BI,SR,CU,O	
2880	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.8Pb0.2Sr1.8Ca1Nd0.2Cu2O8.2	Bi	1.8	Pb	0.2	Sr	1.8	Ca	1	Nd	0.2	Cu	2									O	8.20	8.2	1	1991																											3	Bi2212				5.396	5.41	30.66													83	86					86																																																																																		2																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2881	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.8Pb0.2Sr2Ca0.8Nd0.2Cu2O8.21	Bi	1.8	Pb	0.2	Sr	2	Ca	0.8	Nd	0.2	Cu	2									O	8.21	8.21	1	1991																											3	Bi2212				5.401	5.409	30.74													84	87					87																																																																																		1.4																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2882	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.6Pb0.4Sr1.6Ca1Nd0.4Cu2O8.17	Bi	1.6	Pb	0.4	Sr	1.6	Ca	1	Nd	0.4	Cu	2									O	8.17	8.17	1	1991																											3	Bi2212				5.4	5.416	30.6													72	79					79																																																																																		2.5																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2883	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.6Pb0.4Sr2Ca0.6Nd0.4Cu2O8.26	Bi	1.6	Pb	0.4	Sr	2	Ca	0.6	Nd	0.4	Cu	2									O	8.26	8.26	1	1991																											3	Bi2212				5.412	5.43	30.66													81	85					85																																																																																		3.5																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2884	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.4Pb0.6Sr1.4Ca1Nd0.6Cu2O8.22	Bi	1.4	Pb	0.6	Sr	1.4	Ca	1	Nd	0.6	Cu	2									O	8.22	8.22	1	1991																											3	Bi2212				5.416	5.432	30.5															25				25																																																																																		30.5																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2885	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.4Pb0.6Sr2Ca0.4Nd0.6Cu2O8.24	Bi	1.4	Pb	0.6	Sr	2	Ca	0.4	Nd	0.6	Cu	2									O	8.24	8.24	1	1991																											3	Bi2212				5.422	5.441	30.61															65				65																																																																																		12.1																			SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2886	PHC1790405		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.26	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z	6.26		1991																											3	Bi2201				5.392	5.412	24.49														14.3					14.3																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2887	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.8Pb0.2Sr1.6La0.4Cu1O6.182	Bi	1.8	Pb	0.2	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.182		1991																											3	Bi2201				5.374	5.402	24.535														13.7					13.7																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2888	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.7Pb0.3Sr1.6La0.4Cu1O6.141	Bi	1.7	Pb	0.3	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.141		1991																											3	Bi2201				5.349	5.393	24.529														20.2					20.2																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2889	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.6Pb0.4Sr1.6La0.4Cu1O6.082	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.082		1991																											3	Bi2201				5.34	5.399	24.517														23					23																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2890	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.6La0.4Cu1O6.055	Bi	1.5	Pb	0.5	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.055		1991																											3	Bi2201				5.306	5.399	24.479														28.4					28.4																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2891	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.4Pb0.6Sr1.6La0.4Cu1O6.068	Bi	1.4	Pb	0.6	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.068		1991																											3	Bi2201				5.293	5.407	24.481														28					28																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2892	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.2Pb0.8Sr1.6La0.4Cu1O6.014	Bi	1.2	Pb	0.8	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.014		1991																											3	Bi2201				5.27	5.399	24.477														17.3					17.3																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2893	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1Pb1Sr1.6La0.4Cu1O6.065	Bi	1	Pb	1	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.065		1991																											3	Bi2201				5.277	5.407	24.422														19.8					19.8																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2894	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.8La0.2Cu1O5.983	Bi	1.5	Pb	0.5	Sr	1.8	La	0.2	Cu	1											O	6+Z	5.983		1991																											3	Bi2201				5.278	5.384	24.53														9.2					9.2																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2895	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.7La0.3Cu1O5.993	Bi	1.5	Pb	0.5	Sr	1.7	La	0.3	Cu	1											O	6+Z	5.993		1991																											3	Bi2201				5.293	5.401	24.5														15.6					15.6																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2896	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.6La0.4Cu1O6.044	Bi	1.5	Pb	0.5	Sr	1.6	La	0.4	Cu	1											O	6+Z	6.044		1991																											3	Bi2201				5.303	5.398	24.475														28.1					28.1																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2897	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.5La0.5Cu1O6.074	Bi	1.5	Pb	0.5	Sr	1.5	La	0.5	Cu	1											O	6+Z	6.074		1991																											3	Bi2201				5.325	5.401	24.466														18.1					18.1																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2898	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.4La0.6Cu1O6.118	Bi	1.5	Pb	0.5	Sr	1.4	La	0.6	Cu	1											O	6+Z	6.118		1991																											3	Bi2201				5.341	5.399	24.435														10.8					10.8																																																																																																					STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2899	PHC1790405		(Bi,Pb)2(Sr,La)2CuO6	Bi1.5Pb0.5Sr1.2La0.8Cu1O6.183	Bi	1.5	Pb	0.5	Sr	1.2	La	0.8	Cu	1											O	6+Z	6.183		1991																											3	Bi2201				5.383	5.411	24.382																																																																																																																								STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2900	PHC1790405		(BI,PB)2(SR,LA)2CUO6	Bi1.5Pb0.5Sr1La1Cu1O6.295	Bi	1.5	Pb	0.5	Sr	1	La	1	Cu	1											O	6+Z	6.295		1991																											3	Bi2201				5.412	5.42	24.285																																																																																																																								STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2901	PHC1790405		(Bi,Pb)2Sr2CuO6	Bi1.5Pb0.5Sr2Cu1O5.959	Bi	1.5	Pb	0.5	Sr	2	Cu	1													O	6+Z	5.959		1991																											3	Bi2201				5.282	5.383	24.564																																																																																																																								STRUCTURE AND SUPERCONDUCTIVITY IN THE SINGLE CU-O LAYERED (BI2-XPBX)(SR2-YLAY) CUO6+Z SYSTEM			THE JAMES FRANCK INSTITUTE AND THE SCIENCE AND TECHNOLOGY CENTRE FOR SUPERCONDUCTIVITY,THE UNIVERSITY OF CHICAGO,CHICAGO,IL60637,USA	PHYSICA C,179(1991)405	B.H.MA,C.U.SEGRE,G.SEIDLER,K.ZHANG	BI,PB,SR,LA,CU,O	
2902	PHC1800331	HC2 BY WHH THEORY,GAMMA BY BCS THEORY	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	1991																												BKBO																				32					32													100									12.6									0.57							51					2500														2.4																																												STUDY OF THE MAGNETIC PROPERTIES OF SINGLE-CRYSTAL BA0.6K0.4BIO3			TEXAS CENTER FOR SUPERCONDUCTIVITY,UNIVERSITY OF HOUSTON,TX 77204-5932,USA	PHYSICA C,180(1991)331	C.W.CHU,H.H.FANG,H.Y.TANG,M.L.NORTON,P.H.HOR,Y.Y.XUE,Z.J.HUANG	BA,K,BI,O	
2903	PHC1790358	NEELT DECREASES WITH PRESSURE,DTC/DP=+0.50K/KBAR FOR P>3KBAR	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1991								204																				T																				37.7					37.7			K/GPa	4																																																																																																	TWO-STEP SUPERCONDUCTING TRANSITION AND ANOMALOUS PRESSURE DEPENDENCE OF TC IN LA2CUO4			FACULTY OF ENGINEERING,IWATE UNIVERSITY,MORIOKA 020,JAPAN	PHYSICA C,179(1991)358	M.KURISU,S.MATSUDA,T.FUJITA,T.SUZUKI	LA,CU,O	
2904	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1Ba2Cu3O7+Z	Nd	1	Ba	2	Cu	3															O	7+Z		1	1991																												Y123																				92.9					92.9																																																																																						0.000000000854					RH2904										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2905	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1.1Ba1.9Cu3O7+Z	Nd	1.1	Ba	1.9	Cu	3															O	7+Z		1	1991																												Y123																				82.3					82.3																																																																																						0.00000000151					RH2905										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2906	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3O7+Z	Nd	1.2	Ba	1.8	Cu	3															O	7+Z		1	1991																												Y123																				56.5					56.5																																																																																						0.00000000292					RH2906										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2907	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1.3Ba1.7Cu3O7+Z	Nd	1.3	Ba	1.7	Cu	3															O	7+Z		1	1991																												Y123																				39.4					39.4																																																																																						0.0000000058					RH2907										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2908	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1.4Ba1.6Cu3O7+Z	Nd	1.4	Ba	1.6	Cu	3															O	7+Z		1	1991																												Y123																				23.5					23.5																																																																																						0.0000000081					RH2908										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2909	PR04410167		(Nd,Ba)(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3O7+Z	Nd	1.5	Ba	1.5	Cu	3															O	7+Z		1	1991																												Y123																							4.2																																																																																								0.0000000084					RH2909										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2910	PR04410167		YBa2(Cu,Co)3O7	Y1Ba2Cu2.97Co0.03O7+Z	Y	1	Ba	2	Cu	2.97	Co	0.03													O	7+Z		1	1991																												Y123																				90.5					90.5																																																																																						0.000000000741					RH2910										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2911	PR04410167		YBa2(Cu,Co)3O7	Y1Ba2Cu2.91Co0.09O7+Z	Y	1	Ba	2	Cu	2.91	Co	0.09													O	7+Z		1	1991																												Y123																				70					70																																																																																						0.00000000204					RH2911										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2912	PR04410167		YBa2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15O7+Z	Y	1	Ba	2	Cu	2.85	Co	0.15													O	7+Z		1	1991																												Y123																				57.1					57.1																																																																																											RH2912										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2913	PR04410167		YBa2(Cu,Co)3O7	Y1Ba2Cu2.79Co0.21O7+Z	Y	1	Ba	2	Cu	2.79	Co	0.21													O	7+Z		1	1991																												Y123																				41.1					41.1																																																																																						0.00000000464					RH2913										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2914	PR04410167		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7-Z	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-Z		1	1991																												Y123																				80.2					80.2																																																																																						0.00000000035					RH2914										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2915	PR04410167		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7-Z	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z		1	1991																												Y123																				58.7					58.7																																																																																						0.00000000048					RH2915										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2916	PR04410167		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O7-Z	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	7-Z		1	1991																												Y123																				21					21																																																																																						0.00000000046					RH2916										UNIVERSAL TRANSPORT ANOMALY IN YBA2CU3O7-TYPE SYSTEMS WITH REDUCED CARRIER DENSITY	199111		THE INSTITUTE FOR SOLID STATE PHYSICS,THE UNIVERSITY OF TOKYO,ROPPONGI,MINATO-KU,TOKYO 106,JAPAN	PHYS.REV.B,44(1991)10167	T.TAMEGAI,Y.IYE	Y,BA,CU,O,CO,ND,ZN	
2917	SSC0700951	RESRT=280K	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1989									5.3																		3	Y123				3.82	3.889	11.672														91					91																																																																																		1.33				0.00000000076					RH2917			Y2O3,BACO3,CUO,ZNO	1	SIN(950C 24H IN O2)-FC(IN O2)					EFFECTS OF CU SUBSTITUTION BY ZN ON TRANSPORT PRAPERTIES OF YBA(2)CU(3)O(7-Z)	198906	RESISTIVITY              ,HALL COEFFICIENT         ,HALL MOB	DEPARTMENT DE PHYSIOUE I.M.O.ECOLE POLYTECHNIQUE FEDERALE CH-1015 LAUSANNE SWITZERLAND	SOLID STATE COMMUN.,70(1989)951	D.PAVUNA,F.LICCI,M.AFFRONTE,O.MARTIN,S.CATTANI,T.BESAGNI	Y,BA,CU,O	
2918	SSC0700951	RESRT=280K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.925Zn0.075O7-Z	Y	1	Ba	2	Cu	2.925	Zn	0.075													O	7-Z		1	1989									5.2																		3	Y123				3.82	3.89	11.673														59					59																																																																																		1.43				0.000000000821					RH2918			Y2O3,BACO3,CUO,ZNO	1	SIN(950C 24H IN O2)-FC(IN O2)					EFFECTS OF CU SUBSTITUTION BY ZN ON TRANSPORT PRAPERTIES OF YBA(2)CU(3)O(7-Z)	198906	RESISTIVITY              ,HALL COEFFICIENT         ,HALL MOB	DEPARTMENT DE PHYSIOUE I.M.O.ECOLE POLYTECHNIQUE FEDERALE CH-1015 LAUSANNE SWITZERLAND	SOLID STATE COMMUN.,70(1989)951	D.PAVUNA,F.LICCI,M.AFFRONTE,O.MARTIN,S.CATTANI,T.BESAGNI	Y,BA,CU,O	
2919	SSC0700951	RESRT=280K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-Z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-Z		1	1989									5.05																		3	Y123				3.82	3.885	11.671														49					49																																																																																		1.88				0.000000000857					RH2919			Y2O3,BACO3,CUO,ZNO	1	SIN(950C 24H IN O2)-FC(IN O2)					EFFECTS OF CU SUBSTITUTION BY ZN ON TRANSPORT PRAPERTIES OF YBA(2)CU(3)O(7-Z)	198906	RESISTIVITY              ,HALL COEFFICIENT         ,HALL MOB	DEPARTMENT DE PHYSIOUE I.M.O.ECOLE POLYTECHNIQUE FEDERALE CH-1015 LAUSANNE SWITZERLAND	SOLID STATE COMMUN.,70(1989)951	D.PAVUNA,F.LICCI,M.AFFRONTE,O.MARTIN,S.CATTANI,T.BESAGNI	Y,BA,CU,O	
2920	SSC0700951	MAYBE SECONDARY PHASE,RESRT AT 280K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.775Zn0.225O7-Z	Y	1	Ba	2	Cu	2.775	Zn	0.225													O	7-Z			1989									4.95																		3	Y123				3.826	3.893	11.689														46					46																																																																																		7.35				0.00000000103					RH2920			Y2O3,BACO3,CUO,ZNO	1	SIN(950C 24H IN O2)-FC(IN O2)					EFFECTS OF CU SUBSTITUTION BY ZN ON TRANSPORT PRAPERTIES OF YBA(2)CU(3)O(7-Z)	198906	RESISTIVITY              ,HALL COEFFICIENT         ,HALL MOB	DEPARTMENT DE PHYSIOUE I.M.O.ECOLE POLYTECHNIQUE FEDERALE CH-1015 LAUSANNE SWITZERLAND	SOLID STATE COMMUN.,70(1989)951	D.PAVUNA,F.LICCI,M.AFFRONTE,O.MARTIN,S.CATTANI,T.BESAGNI	Y,BA,CU,O	
2921	PR04410408	SLIGHTLY UNTWINNED,SPHEAT JUMP=MJ/G.K2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1991																											3	Y123																				91.6					91.6																																																					SP2921		2.75																																														HEAT-CAPACITY INVESTIGATIONS  NEAR THE NORMAL-SUPERCONDUCTINGTRANSITION OF YBA2CU3O7	199111		CENTER FOR THE SCIENCE AND APPLICATION OF SUPERCONDUCTIVITY AND SCHOOL OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MINNESOTA,MINNESOTA 55455	PHYS.REV.B,44(1991)10408	B.ZHOU,C.C.HUANG,J.BUAN,J.V.WASZCZAK,L.F.SCHNEEMEYER	Y,BA,CU,O	
2922	PRL0582482	LA2.01CUO4.6 BY EPMA	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1987																											3	T																			16		40				28																																																																			294			TP2922																															EVIDENCE FOR SUPERCONDUCTIVITY IN LA(2)CU(1)O(4)		RESISTIVITY              ,THERMOPOWER	IBM ALMADEN RESEARCH CENTER,SAN JOSE,CALIFORNIA,USA	PHYS.REV.LETT.,58(1987)2482	E.M.ENGLER,G.LIM,J.E.VAZQUEZ,M.L.RAMIREZ,P.M.GRANT,R.D.JACOWITZ,R.L.GREENE,S.S.P.PARKIN,V.Y.LEE		
2923	PHC1790353	MAJOR 2223+IMPURITY TL0.2CA0.8CUOZ PHASE	TlBaCa3Cu3OZ	Tl1Ba1Ca3Cu3OZ	Tl	1	Ba	1	Ca	3	Cu	3													O	Z			1991																																															116		130				123										29.6																																																																								5.58																			SYNTHESIS OF MONOPHASIC TL2BA2CA2CU3O10 (TC=120K) SUPERCONDUCTOR			IRC IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIGE CB30HE,UK	PHYSICA C,179(1991)353	P.P.EDWARDS,R.S.LIU	TL,BA,CA,CU,O	
2924	PHC1790353	HOMOGENEOUS 2223	Tl2Ba2Ca2Cu3O10	Tl1.8Ba2Ca2.2Cu3OZ	Tl	1.8	Ba	2	Ca	2.2	Cu	3													O	Z		1	1991																											2	Tl2223				3.859		35.94													117	120	130				120										58																																																																								3.47																			SYNTHESIS OF MONOPHASIC TL2BA2CA2CU3O10 (TC=120K) SUPERCONDUCTOR			IRC IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIGE CB30HE,UK	PHYSICA C,179(1991)353	P.P.EDWARDS,R.S.LIU	TL,BA,CA,CU,O	
2925	PHC1790353	MAJOR 2223 + MINOR 2212	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3OZ	Tl	2	Ba	2	Ca	2	Cu	3													O	Z			1991																												Tl2223																			110		130				120										48.9																																																																								3.17																			SYNTHESIS OF MONOPHASIC TL2BA2CA2CU3O10 (TC=120K) SUPERCONDUCTOR			IRC IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIGE CB30HE,UK	PHYSICA C,179(1991)353	P.P.EDWARDS,R.S.LIU	TL,BA,CA,CU,O	
2926	PRB0372285	SLIGHTLY OFF-STOICHIOMETRY,LESS CUO	YBa2Cu3O7	Y1Ba2Cu3O9-Z	Y	1	Ba	2	Cu	3															O	9-Z		1	1988																											3	Y123																				92					92																																																																			4.44			TP2926																															THERMOELECTRIC POWER AND SUPERCONDUCTING PROPERTIES OF Y(1)BA(2)CU(3)O(7-Z) AND R(1)BA(2)CU(3)O(7-Z)	198802	THERMOPOWER	DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL,KOREA	PHYS.REV.B,37(1988)2285	B.J.SUH,C.J.LIM,J.H.LEE,S.C.LEE,S.H.MOON,Z.G.KHIM	R,BA,CU,O	
2927	SSC0700303	NOT SUPERCONDUCTING	La2SrCu2O6	La2Sr1Cu2OZ	La	2	Sr	1	Cu	2															O	Z		1	1989																												2126																							4.2																																																																								TP2927																					RH2927			LA2O3,SRCO3,CUO	1	CAL(1050C)-SIN(1050C 2DAYS)-ANN(450C 4DAYS IN O2)					NORMAL STATE PROPERTIES OF LA2-XSRXCUO4 AND LA2SRCU2OY				SOLID STATE COMMUN.,70(1989)303	M.ONODA,M.SATO,M.SERA,S.KONDOH,S.YAMAGATA,Y.ANDO	LA,SR,CU,O	
2928	PHC1770183		TlSr2(Sr,Y)Cu2O7	Tl1Sr2Sr0.5Y0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Y	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.736		12.05													77		90				83.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2929	PHC1770183	MAJOR 1201(TC=40K) + MINOR 1212(TC=90K)	TlSr2(Sr,La)Cu2O7	Tl1Sr2Sr0.5La0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	La	0.5	Cu	2											O	7-Z		2	1991																											2	Tl1212				3.736																	90				90																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2930	PHC1770183		TlSr2(Sr,Pr)Cu2O7	Tl1Sr2Sr0.5Pr0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Pr	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.843		12.166													79		90				84.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2931	PHC1770183		TlSr2(Sr,Nd)Cu2O7	Tl1Sr2Sr0.5Nd0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Nd	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.836		12.135													82		90				86																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2932	PHC1770183		TlSr2(Sr,Sm)Cu2O7	Tl1Sr2Sr0.5Sm0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Sm	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.833		12.078													60		90				75																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2933	PHC1770183		TlSr2(Sr,Eu)Cu2O7	Tl1Sr2Sr0.5Eu0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Eu	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.825		12.074													55		87				71																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2934	PHC1770183		TlSr2(Sr,Gd)Cu2O7	Tl1Sr2Sr0.5Gd0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Gd	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.825		12.093													77		90				83.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2935	PHC1770183		TlSr2(Sr,Tb)Cu2O7	Tl1Sr2Sr0.5Tb0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Tb	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.818		12.078													75		90				82.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2936	PHC1770183		TlSr2(Sr,Dy)Cu2O7	Tl1Sr2Sr0.5Dy0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Dy	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.817		12.068													74		90				82																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2937	PHC1770183		TlSr2(Sr,Ho)Cu2O7	Tl1Sr2Sr0.5Ho0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Ho	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.814		12.05													77		90				83.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2938	PHC1770183		TlSr2(Sr,Er)Cu2O7	Tl1Sr2Sr0.5Er0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Er	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.81		12.04													77		90				83.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2939	PHC1770183		TlSr2(Sr,Tm)Cu2O7	Tl1Sr2Sr0.5Tm0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Tm	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.805		12.035													79		90				84.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2940	PHC1770183		TlSr2(Sr,Yb)Cu2O7	Tl1Sr2Sr0.5Yb0.5Cu2O7-Z	Tl	1	Sr	2	Sr	0.5	Yb	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.796		12.034													73		90				81.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2941	PHC1770183		TlSr2(Sr,Lu)Cu2O7	Tl2Sr2Sr0.5Lu0.5Cu2O7-Z	Tl	2	Sr	2	Sr	0.5	Lu	0.5	Cu	2											O	7-Z		1	1991																											2	Tl1212				3.8		12.037													73		90				81.5																																																																																																					FORMATION AND SUPERCONDUCTIVITY OF 1212-TYPE PHASE TLSR2(SR0.5R0.5)SU2O7-Z WITH R=SC,Y AND LANTHANIDES			DEPARTMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,177(1991)183	D.O.PEDERSON,D.X.GU,Y.XIN,Z.Z.SHENG	TL,SR,SC,Y,CU,O,R	
2942	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.6Pb0.4Sr1.8Ca1Nd0.2Cu2O8.11	Bi	1.6	Pb	0.4	Sr	1.8	Ca	1	Nd	0.2	Cu	2									O	8.11		2	1991																											3	Bi2212				5.39	5.413	30.73													84	87					87																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2943	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.6Pb0.4Sr2Ca0.8Nd0.2Cu2O8.16	Bi	1.6	Pb	0.4	Sr	2	Ca	0.8	Nd	0.2	Cu	2									O	8.16		2	1991																											3	Bi2212				5.401	5.409	30.74													85	87					87																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2944	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.4Pb0.6Sr1.8Ca1Nd0.2Cu2O8+Z	Bi	1.4	Pb	0.6	Sr	1.8	Ca	1	Nd	0.2	Cu	2									O	8+Z		2	1991																											3	Bi2212				5.377	5.424	30.71													77	84					84																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2945	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.4Pb0.6Sr2Ca0.8Nd0.2Cu2O8+Z	Bi	1.4	Pb	0.6	Sr	2	Ca	0.8	Nd	0.2	Cu	2									O	8+Z		2	1991																											3	Bi2212				5.384	5.421	30.74													84	87					87																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2946	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi1.4Pb0.6Sr1.6Ca1Nd0.4Cu2O8+Z	Bi	1.4	Pb	0.6	Sr	1.6	Ca	1	Nd	0.4	Cu	2									O	8+Z		2	1991																											3	Bi2212				5.383	5.424	30.6													52	62					62																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2947	PHC1760445		(Bi,Pb)2(Sr,Nd)2(Ca,Nd)Cu2O8	Bi2.4Pb0.6Sr2Ca0.6Nd0.4Cu2O8+Z	Bi	2.4	Pb	0.6	Sr	2	Ca	0.6	Nd	0.4	Cu	2									O	8+Z		2	1991																											3	Bi2212				5.398	5.434	30.69													65	77					77																																																																																																					SUPERCONDUCTING PROPERTIES OF CERAMICS IN THE 2212 SYSTEM BI2-WPBWSR2-XCA1-YNDX+YCU2O8+Z			INSTITUT FUR ANORGANISCH CHEMIE DER UNIVERSITAT TUBINFEN,AUF DER MORGENSTELLE 18,W-7400 TUBINGEN,GERMANY	PHYSICA C,176(1991)445	S.KEMMLER-SACK,T.RENTSHLER	BI,PB,SR,CA,ND,CU,O	
2948	NAT3510549		SrCuO2	Sr1Cu1O2	Sr	1	Cu	1																	O	2		1	1991																											2					3.925		3.43																	2																																																																																																							ELECTRON-DOPED SUPERCONDUCTIVITY AT 40 K IN THE INFINITE-LAYERCOMPOUND SR1-YNDYCUO2	6		CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC#5160,UNIVERSITY OF TEXAS AT AUSTIN,AUSTIN,TEXAS 78712-1084,USA	NATURE,351(1991)549	A.MANTHIRAM,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,PR,CU,O	
2949	NAT3510549	INFINITE LAYER COMPOUND,SR1-XLNXCUO2=NEARLY SINGLE PHASE FOR 0<=X<=0.16 FOR LN=PR,ND	(Sr,Nd)CuO2	Sr0.95Nd0.05Cu1O2	Sr	0.95	Nd	0.05	Cu	1															O	2		1	1991																											2	IL				3.932		3.408															38				38																																																																																																					ELECTRON-DOPED SUPERCONDUCTIVITY AT 40 K IN THE INFINITE-LAYERCOMPOUND SR1-YNDYCUO2	6		CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC#5160,UNIVERSITY OF TEXAS AT AUSTIN,AUSTIN,TEXAS 78712-1084,USA	NATURE,351(1991)549	A.MANTHIRAM,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,PR,CU,O	
2950	NAT3510549		(Sr,Nd)CuO2	Sr0.86Nd0.14Cu1O2	Sr	0.86	Nd	0.14	Cu	1															O	2		1	1991																											2	IL				3.942		3.384													25	35	40				35																																																																																																					ELECTRON-DOPED SUPERCONDUCTIVITY AT 40 K IN THE INFINITE-LAYERCOMPOUND SR1-YNDYCUO2	6		CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC#5160,UNIVERSITY OF TEXAS AT AUSTIN,AUSTIN,TEXAS 78712-1084,USA	NATURE,351(1991)549	A.MANTHIRAM,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,PR,CU,O	
2951	NAT3510549		(Sr,Nd)CuO2	Sr0.84Nd0.16Cu1O2	Sr	0.84	Nd	0.16	Cu	1															O	2		1	1991																											2	IL				3.944		3.386															40				40																																																																																																					ELECTRON-DOPED SUPERCONDUCTIVITY AT 40 K IN THE INFINITE-LAYERCOMPOUND SR1-YNDYCUO2	6		CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC#5160,UNIVERSITY OF TEXAS AT AUSTIN,AUSTIN,TEXAS 78712-1084,USA	NATURE,351(1991)549	A.MANTHIRAM,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,PR,CU,O	
2952	NAT3510549		(Sr,Pr)CuO2	Sr0.85Pr0.15Cu1O2	Sr	0.85	Pr	0.15	Cu	1															O	2		1	1991																											2					3.942		3.393															39				39																																																																																																					ELECTRON-DOPED SUPERCONDUCTIVITY AT 40 K IN THE INFINITE-LAYERCOMPOUND SR1-YNDYCUO2	6		CENTER FOR MATERIALS SCIENCE AND ENGINEERING,ETC#5160,UNIVERSITY OF TEXAS AT AUSTIN,AUSTIN,TEXAS 78712-1084,USA	NATURE,351(1991)549	A.MANTHIRAM,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,PR,CU,O	
2953	PR0444539	Y- and Ca-content not described. Then, Y- and Ca-content are tentative values. anisotropy factor = 2.5	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8+Z	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8+Z		3	1991																											3	Pb3212				5.383	5.423	15.765														75					75											Oe	deviation from linear in M-H curve.		95	505																										A	magnetization		2575	6425																																																			single crystals were grown using a PbO-NaCl flux method.  ANN(600C,40h in N2)					TEMPERATURE DEPENDENCE OF THE ANISOTROPIC MAGNETIC PENETRATIONDEPTH AND LOWER CRITICAL FIELD OF SINGLE-CRYSTAL PB2SR2(Y,CA)CU3O8-Z	199109		DEPARTMENT OF PHYSICS,MCMASTER UNIVERSITY,HAMILTON,ONTARIO,CANADA L8S4M1	PHYS.REV.B,44(1991)4539	C.V.STAGER,J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,CA,CU,O	
2954	PR0445046	TETRA-ORTHO PHASE TRANSITION >300K	La2NiO4	La2Ni1O4	La	2	Ni	1																	O	4+Z	4	3	1991								300																			3					5.473	5.532	12.541																																																																																																																								Magnetic correlations and their dependence on excess oxygen in La2NiO4+delta	199109		Corporate R&D, NKT, DK-2605 Brondby, Denmark	Phys.Rev.B,44(1991)5046	D. Vaknin,D.J. Buttrey,G. Aeppli,G. Shirane,T. Freltoft		
2955	PR0445046	TETRA-ORTHO PHASE TRANSITION 232-240K	La2NiO4	La2Ni1O4.067	La	2	Ni	1																	O	4+Z	4.067	3	1991								68																			2					3.869		12.625																																																																																																																								Magnetic correlations and their dependence on excess oxygen in La2NiO4+delta	199109		Corporate R&D, NKT, DK-2605 Brondby, Denmark	Phys.Rev.B,44(1991)5046	D. Vaknin,D.J. Buttrey,G. Aeppli,G. Shirane,T. Freltoft		
2956	PR0445046		La2NiO4	La2Ni1O4.077	La	2	Ni	1																	O	4+Z	4.077	3	1991								49																			2					3.869		12.635																																																																																																																								Magnetic correlations and their dependence on excess oxygen in La2NiO4+delta	199109		Corporate R&D, NKT, DK-2605 Brondby, Denmark	Phys.Rev.B,44(1991)5046	D. Vaknin,D.J. Buttrey,G. Aeppli,G. Shirane,T. Freltoft		
2957	PR0445046	TETRA-ORTHO PHASE TRANSITION 220-250K	La2NiO4	La2Ni1O4	La	2	Ni	1																	O	4+Z	4	1	1991						0.85		74																			2					3.871		12.63																																																																																																																								Magnetic correlations and their dependence on excess oxygen in La2NiO4+delta	199109		Corporate R&D, NKT, DK-2605 Brondby, Denmark	Phys.Rev.B,44(1991)5046	D. Vaknin,D.J. Buttrey,G. Aeppli,G. Shirane,T. Freltoft		
2958	PR0445046		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4+Z	4	1	1991								265																			3					5.375	5.399	13.156																																																																																																																								Magnetic correlations and their dependence on excess oxygen in La2NiO4+delta	199109		Corporate R&D, NKT, DK-2605 Brondby, Denmark	Phys.Rev.B,44(1991)5046	D. Vaknin,D.J. Buttrey,G. Aeppli,G. Shirane,T. Freltoft		
2959	PR0445318	DELTA-TC=0.9	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1991																												Y123																			71						71						0.1			0.9																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2960	PR0445318	DELTA-TC=0.76K,84%O(18)	(Y,Pr,Ca)Ba2Cu3O7	Y0.75Pr0.2Ca0.05Ba2Cu3O7-Z	Y	0.75	Pr	0.2	Ca	0.05	Ba	2	Cu	3											O	7-Z			1991																												Y123																			73.6						73.6		1				0.09	O	84	0.76																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2961	PR0445318	DELTA-TC=0.47K,78%O(18)	(Y,Pr,Ca)Ba2Cu3O7	Y0.7Pr0.2Ca0.1Ba2Cu3O7-Z	Y	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7-Z			1991																												Y123																			77.8						77.8		1				0.05	O	78	0.47																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2962	PR0445318	DELTA-TC=0.42K,76%O(18)	(Y,Pr,Ca)Ba2Cu3O7	Y0.6Pr0.2Ca0.2Ba2Cu3O7-Z	Y	0.6	Pr	0.2	Ca	0.2	Ba	2	Cu	3											O	7-Z			1991																												Y123																			71.2						71.2		1				0.05	O	76	0.42																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2963	PR0445318	DELTA-TC=0.8K,84.6%O(18)	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1991																												Y123																				75.6					75.6		1				0.09	O	84.6	0.8	24																																																																																											OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2964	PR0445318	DELTA=TC=1.07K,79%O(18)	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z			1991																												Y123																				60.4					60.4		1				0.15	O	79	1.07	21																																																																																											OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2965	PR0445318	DELTA-TC=1.50K,85.5%O(18)	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7-Z	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z			1991																												Y123																				46.2					46.2		1				0.27	O	85.5	1.5	14																																																																																											OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2966	PR0445318	DELTA-TC=1.65K,85.9%O(18)	(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-Z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z			1991																												Y123																				30.6					30.6		1				0.45	O	85.9	1.65	7																																																																																											OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2967	PR0445318	DELTA-TC=1.16K,72.1%O(18)	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-Z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z			1991																												Y123																				60					60		1				0.17	O	72.1	1.16																																																																																												OBSERVATION OF AN OXYGEN ISOTOPE EFFECT IN SUPERCONDUCTING (Y1-XPRX)BA2CU3O7-Z	199109		DEPARTMENTOF PHYSICS,UNIVERSITY OF AOBERTA,CANADA T6G2J1	PHYS.REV.B,44(1991)5318	G.I.SPROULE,J.JUNG,J.P.FRANCK,M.A-K.MOHAMED,S.GYGAX	Y,PR,BA,CU,O	
2968	PR0445326	COMPARED WITH 97%LI(6),99%LI(7)	LiTiO4	Li1Ti1O4	Li	1	Ti	1																	O	4			1991																												LTO																				12.15					12.15		2				0.013	Li	99																																																																																													LI-LI ISOTOPE EFFECT IN SUPERCONDUCTING LITI2O4	199109	ISOTOPE EFFECT	DEPARTMENT OF PHYSICS AND ASTRONOMY,LOUISIANA STATE UNIVERSITY,BATON ROUGE,LOUISIANA 70803-4001	PHYS.REV.B,44(1991)5326	R.G.GOODRICH	LI,TI,O	
2969	PR0444553			Pb1Sr0.8Ba1.2Y0.7Ca0.3Cu3O8.41	Pb	1	Sr	0.8	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z	8.41		1991																												Pb1213				3.845		27.92														42					42																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2970	PR0444553			Pb1Sr0.8Ba1.2Y0.7Ca0.3Cu3O7+Z	Pb	1	Sr	0.8	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z			1991																												Pb3212																				78					78																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2971	PR0444553			Pb1Sr0.8Ba1.2Y0.7Ca0.3Cu3O9.63	Pb	1	Sr	0.8	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z	9.63		1991																												Pb3212																							6																																																																																																							77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2972	PR0444553			Pb0.5Sr2Y0.6Ca0.4Cu2.5O6.97	Pb	0.5	Sr	2	Y	0.6	Ca	0.4	Cu	2.5											O	7-Z	6.97		1991																																																67					67																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2973	PR0444553			Pb0.5Sr2Y0.6Ca0.4Cu2.5O6.99	Pb	0.5	Sr	2	Y	0.6	Ca	0.4	Cu	2.5											O	7-Z	6.99		1991																																																			6																																																																																																							77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2974	PR0444553			Pb0.8Sr1Ba1.2Y0.7Ca0.3Cu3O7.59	Pb	0.8	Sr	1	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z	7.59		1991																											2	Pb1213				4.839		27.72														40					40																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2975	PR0444553			Pb0.8Sr1Ba1.2Y0.7Ca0.3Cu3O8.28	Pb	0.8	Sr	1	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z	8.28		1991																											2	Pb1213				3.844		27.96														74					74																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2976	PR0444553			Pb0.8Sr1Ba1.2Y0.7Ca0.3Cu3O8.35	Pb	0.8	Sr	1	Ba	1.2	Y	0.7	Ca	0.3	Cu	3									O	7+Z	8.35		1991																											2	Pb1213				3.845		27.96														77					77																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2977	PR0444553			Pb0.8Sr0.8Ba1.2Y0.7Ca0.3Cu3.2O8.3	Pb	0.8	Sr	0.8	Ba	1.2	Y	0.7	Ca	0.3	Cu	3.2									O	7+Z	8.3		1991																											2	Pb1213				3.845		27.9														75					75																																																																																																					77-K SUPERCONDUCTOR PB0.8SRBA1.2Y0.7CA0.3CU3O7+Z:COMPARISON WITH OTHER PB-BASED SUPERCONDUCTORS	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)4553	D.E.MORRIS,X.X.TANG	PB,SR,BA,Y,CA,CU,O	
2978	JPS0583890	NEELT INCREASES AS +18.5K/GPA BY NED	La2CuO4	La2Cu1O4-Z	La	2	Cu	1																	O	4-Z		3	1989								222																			3	T				5.353	5.402	13.136																																																																																																																								PRESSURE EFFECT ON THE ANTIFERROMAGNETISM IN LA2CUO4-Y	198911		DEPARTMENT OF PHYSICS,JAPAN ATOMIC ENERGY RESEARCH INSTITUTE,TOKAI,IBARAKI 319-11	J.PHYS.SOC.JAPAN.58(1989)3890	HIROKI RAKAHASHI,NOBUO MORI,SUSUMU KATANO	LA,CU,O	
2979	PR0362305	TWO STEP TRANSITION 95.5,93K,RES/T=1.94MICRO-OHM/K	YBa2Cu3O7	Y1Ba2Cu3O9-Z	Y	1	Ba	2	Cu	3															O	9-Z		1	1987																											3	Y123				3.819	3.882	11.665													91	93	96			3	93										50																																																			1.17						1.17			TP2979								0.22				0.52																			SUPERCONDUCTIVITY IN SINGLE-PHASE Y1BA2CU3O9-X AND THERMOELECTRIC POWER MEASUREMENT	8		DEPARTMENT OF PHYSICS,SEOUL NATIONAL UNIVERSITY,SEOUL 151,KOREA	PHPYS.REV.B,36(1991)2305	B.J.SUH,C.PARK,I.S.YU,J.H.LEE,S.C.LEE,Y.W.PARK,Z.G.KHIM	Y,BA,CU,O	
2980	PHC1790376	TP MEASURED IN AIR	(La,Sr)2CuO4	La1.99Sr0.01Cu1O4-Z	La	1.99	Sr	0.01	Cu	1															O	4-Z			1991																												T																																																																																												392			TP2980																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2981	PHC1790376		(La,Sr)2CuO4	La1.97Sr0.03Cu1O4-Z	La	1.97	Sr	0.03	Cu	1															O	4-Z			1991																												T																																																																																						267						267			TP2981																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2982	PHC1790376		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4-Z	La	1.96	Sr	0.04	Cu	1															O	4-Z			1991																												T																																																																																												151			TP2982																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2983	PHC1790376		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4-Z	La	1.86	Sr	0.14	Cu	1															O	4-Z			1991																												T																																																																																												22.8			TP2983																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2984	PHC1790376		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4-Z	La	1.84	Sr	0.16	Cu	1															O	4-Z			1991																												T																																																																																												6.14			TP2984																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2985	PHC1790376		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4-Z	La	1.8	Sr	0.2	Cu	1															O	4-Z			1991																												T																																																																																												-10.3			TP2985																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2986	PHC1790376		(La,Sr)2CuO4	La1.6Sr0.4Cu1O4-Z	La	1.6	Sr	0.4	Cu	1															O	4-Z			1991																												T																																																																																												-3.86			TP2986																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2987	PHC1790376		(Nd,Ce)2CuO4	Nd1.95Ce0.05Cu1O4-Z	Nd	1.95	Ce	0.05	Cu	1															O	4-Z			1991																												T'																																																																																												-14.2			TP2987																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2988	PHC1790376		(Nd,Ce)2CuO4	Nd1.9Ce0.1Cu1O4-Z	Nd	1.9	Ce	0.1	Cu	1															O	4-Z			1991																												T'																																																																																															TP2988																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2989	PHC1790376		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z			1991																												T'																																																																																															TP2989																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2990	PHC1790376		(Nd,Ce)2CuO4	Nd1.8Ce0.2Cu1O4-Z	Nd	1.8	Ce	0.2	Cu	1															O	4-Z			1991																												T'																																																																																																																														THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2991	PHC1790376		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1991																												Y123																																																																																												-12.9			TP2991																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2992	PHC1790376		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1991																												Bi2212																																																																																												-21.1			TP2992																															THERMOELECTRIC POWER OF THE HIGH-TC OXIDE SUPERCONDUCTORS AT ELEVATED TEMPERATURES			LABORATORY FOR SOLID STATE CHEMISTRY,OKAYAMA UNIVERSITY OF SCIENCE,RIDAI-CHO 1-1,OKAYAMA 700,JAPAN	PHYSICA C,179(1991)376	K.KOBATAKE,T.OHTANI,T.TAKEHARA	ND,CE,LA,SR,CU,O,NI,CA	
2993	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.94Ba0.06Cu0.99Ga0.01O4	La	1.94	Ba	0.06	Cu	0.99	Ga	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2994	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.9Ba0.1Cu0.99Ga0.01O4	La	1.9	Ba	0.1	Cu	0.99	Ga	0.01													O	4		1	1991																												T																				14.3					14.3																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2995	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.88Ba0.12Cu0.99Ga0.01O4	La	1.88	Ba	0.12	Cu	0.99	Ga	0.01													O	4		1	1991																												T																				8.2					8.2																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2996	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.87Ba0.13Cu0.99Ga0.01O4	La	1.87	Ba	0.13	Cu	0.99	Ga	0.01													O	4		1	1991																												T																				4.5					4.5																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2997	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.86Ba0.14Cu0.99Ga0.01O4	La	1.86	Ba	0.14	Cu	0.99	Ga	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2998	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.84Ba0.16Cu0.99Ga0.01O4	La	1.84	Ba	0.16	Cu	0.99	Ga	0.01													O	4		1	1991																												T																				8.3					8.3																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
2999	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.82Ba0.18Cu0.99Ga0.01O4	La	1.82	Ba	0.18	Cu	0.99	Ga	0.01													O	4		1	1991																												T																				8.6					8.6																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3000	SSC0780511		(La,Ba)2(Cu,Ga)O4	La1.7Ba0.3Cu0.99Ga0.01O4	La	1.7	Ba	0.3	Cu	0.99	Ga	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3001	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.94Ba0.06Cu0.99Zn0.01O4	La	1.94	Ba	0.06	Cu	0.99	Zn	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3002	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.9Ba0.1Cu0.99Zn0.01O4	La	1.9	Ba	0.1	Cu	0.99	Zn	0.01													O	4		1	1991																												T																				9.8					9.8																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3003	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.88Ba0.12Cu0.99Zn0.01O4	La	1.88	Ba	0.12	Cu	0.99	Zn	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3004	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.86Ba0.14Cu0.99Zn0.01O4	La	1.86	Ba	0.14	Cu	0.99	Zn	0.01													O	4		1	1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3005	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.84Ba0.16Cu0.99Zn0.01O4	La	1.84	Ba	0.16	Cu	0.99	Zn	0.01													O	4		1	1991																												T																				12.4					12.4																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3006	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.82Ba0.18Cu0.99Zn0.01O4	La	1.82	Ba	0.18	Cu	0.99	Zn	0.01													O	4		1	1991																												T																				13.9					13.9																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3007	SSC0780511		(La,Ba)2(Cu,Zn)O4	La1.7Ba0.3Cu0.99Zn0.01O4	La	1.7	Ba	0.3	Cu	0.99	Zn	0.01													O	4		1	1991																												T																				5					5																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3008	SSC0780511		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3009	SSC0780511		(La,Ba)2CuO4	La1.95Ba0.05Cu1O4	La	1.95	Ba	0.05	Cu	1															O	4			1991																												T																																																																																																																														EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3010	SSC0780511		(La,Ba)2CuO4	La1.94Ba0.06Cu1O4	La	1.94	Ba	0.06	Cu	1															O	4			1991																												T																				10.2					10.2																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3011	PHC1800324		La(Ba,Ca)2(Cu,Ni)3O7	Ca1Ba1La1Cu2.5Ni0.5O6.812	Ca	1	Ba	1	La	1	Cu	2.5	Ni	0.5											O	6.812	6.812	1	1991																												Y123				3.877		11.634																	4.2																																																																																																							EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3012	PHC1710419		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.7Ga0.3O6.93	Y	1	Ba	2	Cu	2.7	Ga	0.3													O	Z	6.93	1	1990																											2	Y123																				75					75																																																																																																					ANTIFERROMAGNETISM IN YBA2CU3O6+X: GA AND ZN SUBSTITUTIONS I.89Y NMR DETERMINATION OF THE NEEL TEMPERATURE		NEEL TEMPERATURE    ,NMR                 ,ANTIFERROMAGNETIC	LABORATOIRE DE PHYSIQUE DES SOLIDES AND LABORATOIRE DES COMPOSES NON STOECHIOMETRIQUES, UNIVERSITE PARIS SUD, 91405 ORSAY, FRANCE	PHYSICA C,171(1990)419	G.COLLIN,H.ALLOUL,H.CASALTA,J.ARABSKI,J.F.MARUCCO,M.MEHBOD,P.MENDELS,T.OHNO	Y,BA,CU,O,GA,ZN	
3013	PHC1710419		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.7Ga0.3O6.2	Y	1	Ba	2	Cu	2.7	Ga	0.3													O	Z	6.2	1	1990								404																			2	Y123																																																																																																																														ANTIFERROMAGNETISM IN YBA2CU3O6+X: GA AND ZN SUBSTITUTIONS I.89Y NMR DETERMINATION OF THE NEEL TEMPERATURE		NEEL TEMPERATURE    ,NMR                 ,ANTIFERROMAGNETIC	LABORATOIRE DE PHYSIQUE DES SOLIDES AND LABORATOIRE DES COMPOSES NON STOECHIOMETRIQUES, UNIVERSITE PARIS SUD, 91405 ORSAY, FRANCE	PHYSICA C,171(1990)419	G.COLLIN,H.ALLOUL,H.CASALTA,J.ARABSKI,J.F.MARUCCO,M.MEHBOD,P.MENDELS,T.OHNO	Y,BA,CU,O,GA,ZN	
3014	PHC1710419	X=0.102 BY EDAX	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O6.92	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	Z	6.92	1	1990																											3	Y123																				53					53																																																																																																					ANTIFERROMAGNETISM IN YBA2CU3O6+X: GA AND ZN SUBSTITUTIONS I.89Y NMR DETERMINATION OF THE NEEL TEMPERATURE		NEEL TEMPERATURE    ,NMR                 ,ANTIFERROMAGNETIC	LABORATOIRE DE PHYSIQUE DES SOLIDES AND LABORATOIRE DES COMPOSES NON STOECHIOMETRIQUES, UNIVERSITE PARIS SUD, 91405 ORSAY, FRANCE	PHYSICA C,171(1990)419	G.COLLIN,H.ALLOUL,H.CASALTA,J.ARABSKI,J.F.MARUCCO,M.MEHBOD,P.MENDELS,T.OHNO	Y,BA,CU,O,GA,ZN	
3015	PHC1710419	X=0.102 BY EDAX	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O6.01	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	Z	6.01	1	1990								401																				Y123																																																																																																																														ANTIFERROMAGNETISM IN YBA2CU3O6+X: GA AND ZN SUBSTITUTIONS I.89Y NMR DETERMINATION OF THE NEEL TEMPERATURE		NEEL TEMPERATURE    ,NMR                 ,ANTIFERROMAGNETIC	LABORATOIRE DE PHYSIQUE DES SOLIDES AND LABORATOIRE DES COMPOSES NON STOECHIOMETRIQUES, UNIVERSITE PARIS SUD, 91405 ORSAY, FRANCE	PHYSICA C,171(1990)419	G.COLLIN,H.ALLOUL,H.CASALTA,J.ARABSKI,J.F.MARUCCO,M.MEHBOD,P.MENDELS,T.OHNO	Y,BA,CU,O,GA,ZN	
3016	PHC1710419	X=0.201 BY EDAX	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.76Zn0.24O6.02	Y	1	Ba	2	Cu	2.76	Zn	0.24													O	Z	6.02		1990								404																				Y123																																																																																																																														ANTIFERROMAGNETISM IN YBA2CU3O6+X: GA AND ZN SUBSTITUTIONS I.89Y NMR DETERMINATION OF THE NEEL TEMPERATURE		NEEL TEMPERATURE    ,NMR                 ,ANTIFERROMAGNETIC	LABORATOIRE DE PHYSIQUE DES SOLIDES AND LABORATOIRE DES COMPOSES NON STOECHIOMETRIQUES, UNIVERSITE PARIS SUD, 91405 ORSAY, FRANCE	PHYSICA C,171(1990)419	G.COLLIN,H.ALLOUL,H.CASALTA,J.ARABSKI,J.F.MARUCCO,M.MEHBOD,P.MENDELS,T.OHNO	Y,BA,CU,O,GA,ZN	
3017	PHC1720043	NEARLY SINGLE PHASE	(Tl,Pb)(Sr,Pr)3Cu2OZ	Tl0.8Pb0.2Sr2.5Pr0.5Cu2OZ	Tl	0.8	Pb	0.2	Sr	2.5	Pr	0.5	Cu	2											O	Z		1	1990																											2	Tl1302				3.841		12.195														90	105				90																																																																																																					SUPERCONDUCTIVITY ABOVE 100 K IN THE CA-FREE TL-PB-SR-PR-CU-OSYSTEM			DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS, FAYETTEVILLE, AR 72701 USA	PHYSICA C,172(1990)43	J.M.MEASON,L.A.BURCHFIELD,Y.XIN,Z.Z.SHENG	TL,PB,SR,PR,CU,O	
3018	PHC1760368	IMPURITIS PRESENT	Tl2Ba2CuO6	Tl2Ba2Cu1O6-X	Tl	2	Ba	2	Cu	1															O	6-X		1	1991																												Tl2201				3.87		23.238													73		90				81.5																																																																						TP3018																															THERMOPOWER OF TL2BA2CUO6-X BULK SUPERCONDUCTORS			HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYSICA C,176(1991)368	A.M.HERMANN,C.DONG,D.E.WEEKS,W.KIEHL	TL,BA,CU,O	
3019	RSI0621801	BY MICROSTRIP RESONATOR TECHNIQUE,PENE(LONDON)=1400A	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1991																												Y123																				90					90																																						15					1700					4.5																																																					MAGNETIC PENETRATION DEPTH MEASUREMENTS OF SUPERCONDUCTING THIN FILMS BY A MICROSTRIP RESONATOR TECHNIQUE	199107			REV.SCI.INSTRUM.,62(1991)1801	B.W.LANGLEY,M.R.BEASLEY,R.F.W.PEASE,S.M.ANLAGE		
3020	SSC0780511		(La,Ba)2CuO4	La1.93Ba0.07Cu1O4	La	1.93	Ba	0.07	Cu	1															O	4			1991																												T																				19					19																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3021	SSC0780511		(La,Ba)2CuO4	La1.922Ba0.078Cu1O4	La	1.922	Ba	0.078	Cu	1															O	4			1991																												T																				22.9					22.9																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3022	SSC0780511		(La,Ba)2CuO4	La1.903Ba0.097Cu1O4	La	1.903	Ba	0.097	Cu	1															O	4			1991																												T																				26					26																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3023	SSC0780511		(La,Ba)2CuO4	La1.892Ba0.108Cu1O4	La	1.892	Ba	0.108	Cu	1															O	4			1991																												T																				22.1					22.1																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3024	SSC0780511		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4			1991																												T																				9.5					9.5																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3025	SSC0780511		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4			1991																												T																				9.7					9.7																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3026	SSC0780511		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4			1991																												T																				13.3					13.3																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3027	SSC0780511		(La,Ba)2CuO4	La1.843Ba0.157Cu1O4	La	1.843	Ba	0.157	Cu	1															O	4			1991																												T																				25.3					25.3																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3028	SSC0780511		(La,Ba)2CuO4	La1.823Ba0.177Cu1O4	La	1.823	Ba	0.177	Cu	1															O	4			1991																												T																				25.5					25.5																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3029	SSC0780511		(La,Ba)2CuO4	La1.801Ba0.199Cu1O4	La	1.801	Ba	0.199	Cu	1															O	4			1991																												T																				23.5					23.5																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3030	SSC0780511		(LA,BA)2CUO4	La1.782Ba0.218Cu1O4	La	1.782	Ba	0.218	Cu	1															O	4			1991																												T																				21.6					21.6																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3031	SSC0780511		(La,Ba)2CuO4	La1.751Ba0.249Cu1O4	La	1.751	Ba	0.249	Cu	1															O	4			1991																												T																				13.7					13.7																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3032	SSC0780511		(La,Ba)2CuO4	La1.7Ba0.3Cu1O4	La	1.7	Ba	0.3	Cu	1															O	4			1991																												T																				9.7					9.7																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3033	SSC0780511		(La,Ba)2CuO4	La1.65Ba0.35Cu1O4	La	1.65	Ba	0.35	Cu	1															O	4			1991																												T																					4.2		4.2		4.2																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3034	SSC0780511		(La,Ba)2CuO4	La1.6Ba0.4Cu1O4	La	1.6	Ba	0.4	Cu	1															O	4			1991																												T																					4.2		4.2		4.2																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3035	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.94Ba0.06Cu0.99Ni0.01O4	La	1.94	Ba	0.06	Cu	0.99	Ni	0.01													O	4			1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3036	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.9Ba0.1Cu0.99Ni0.01O4	La	1.9	Ba	0.1	Cu	0.99	Ni	0.01													O	4			1991																												T																				17					17																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3037	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.882Ba0.118Cu0.99Ni0.01O4	La	1.882	Ba	0.118	Cu	0.99	Ni	0.01													O	4			1991																												T																				12.7					12.7																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3038	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.869Ba0.131Cu0.99Ni0.01O4	La	1.869	Ba	0.131	Cu	0.99	Ni	0.01													O	4			1991																												T																				7					7																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3039	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.86Ba0.14Cu0.99Ni0.01O4	La	1.86	Ba	0.14	Cu	0.99	Ni	0.01													O	4			1991																												T																				11					11																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3040	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.842Ba0.158Cu0.99Ni0.01O4	La	1.842	Ba	0.158	Cu	0.99	Ni	0.01													O	4			1991																												T																				19					19																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3041	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.822Ba0.178Cu0.99Ni0.01O4	La	1.822	Ba	0.178	Cu	0.99	Ni	0.01													O	4			1991																												T																				18.2					18.2																																																																																																					EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3042	SSC0780511		(La,Ba)2(Cu,Ni)O4	La1.7Ba0.3Cu0.99Ni0.01O4	La	1.7	Ba	0.3	Cu	0.99	Ni	0.01													O	4			1991																												T																							4.2																																																																																																							EFFECTS OF THE CU-SITE SUBSTITUTION ON THE ANOMALOUS X DEPENDENCE OF TC IN LA2-XBAXCUO4	199105		DEPARTMENT OF APPLIED PHYSICS,FACULTY OF ENGINEERING,TOHOKU UNIVERSITY,ARAMAKI AOBA,AOBA-KU,SENDEI 980,JAPAN	SOLID STATE COMMUN.,78(1991)511	N.WATANABE,T.NOJI,Y.KOIKE,Y.SAITO	LA,BA,CU,O	
3043	PRB0365694	TC BY INDUCTIVE METHOD		Ba2Cu3O7	Ba	2	Cu	3																	O	7		1	1987																											3	Y123				3.82	3.886	11.683														92					92																																																																																																					SUPERCONDUCTIVITY IN H(X) Y(1)BA(2)CU(3)O(7)	198710	PREPARATION              ,SOLID SOLUTION           ,TC	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)5694	A.R.MOOODENBAUGH,J.J.REILLY,J.R.JOHNSON,M.SUENAGA,P.THOMPSON	H,Y,BA,CU,O	
3044	PRB0365694			Y1Ba2Cu3H0.13O7	Y	1	Ba	2	Cu	3	H	0.13													O	7		1	1987																											3	Y123				3.821	3.887	11.688														93.5					93.5																																																																																																					SUPERCONDUCTIVITY IN H(X) Y(1)BA(2)CU(3)O(7)	198710	PREPARATION              ,SOLID SOLUTION           ,TC	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)5694	A.R.MOOODENBAUGH,J.J.REILLY,J.R.JOHNSON,M.SUENAGA,P.THOMPSON	H,Y,BA,CU,O	
3045	PRB0365694			Y1Ba2Cu3H0.19O7	Y	1	Ba	2	Cu	3	H	0.19													O	7		1	1987																											3	Y123				3.825	3.886	11.691														93.5					93.5																																																																																																					SUPERCONDUCTIVITY IN H(X) Y(1)BA(2)CU(3)O(7)	198710	PREPARATION              ,SOLID SOLUTION           ,TC	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)5694	A.R.MOOODENBAUGH,J.J.REILLY,J.R.JOHNSON,M.SUENAGA,P.THOMPSON	H,Y,BA,CU,O	
3046	PRB0365694			Y1Ba2Cu3H0.38O7	Y	1	Ba	2	Cu	3	H	0.38													O	7		1	1987																											3	Y123				3.825	3.886	11.69														93.8					93.8																																																																																																					SUPERCONDUCTIVITY IN H(X) Y(1)BA(2)CU(3)O(7)	198710	PREPARATION              ,SOLID SOLUTION           ,TC	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)5694	A.R.MOOODENBAUGH,J.J.REILLY,J.R.JOHNSON,M.SUENAGA,P.THOMPSON	H,Y,BA,CU,O	
3047	PRB0365694			Y1Ba2Cu3H0.49O7	Y	1	Ba	2	Cu	3	H	0.49													O	7		1	1987																											3	Y123				3.826	3.886	11.694														93.6					93.6																																																																																																					SUPERCONDUCTIVITY IN H(X) Y(1)BA(2)CU(3)O(7)	198710	PREPARATION              ,SOLID SOLUTION           ,TC	DEPARTMENT OF APPLIED SCIENCE,BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,36(1987)5694	A.R.MOOODENBAUGH,J.J.REILLY,J.R.JOHNSON,M.SUENAGA,P.THOMPSON	H,Y,BA,CU,O	
3048	JJP0280923	SMALL AMOUNT OF BA2CUO3	TlBa2CuO4	Tl1Ba2Cu1O5-Z	Tl	1	Ba	2	Cu	1															O	5-Z			1989																												Tl1201				3.859		9.229														15					15																																																																																																					THE OCCURRENCE OF SUPERCONDUCTIVITY IN THE TLBA(2)CUO(5-Z)-TYPE (1021) SYSTEM	198906	METASTABLE               ,METAL-INSULATOR TRANSITIO,RES	DEPARTMENT OF PHYSICS,NATIONAL TSING HUA UNIVERSITY,HSINCHU,TAIWAN 30043,R.O.C.	JJAP LETT ,28(1989)L923	D.C.LING,G.H.HWANG,H.C.KU,HSU,J.B.SHI,M.F.TAI,M.J.SHIH,S,T.J.WATSON-YANG,T.Y.LIN,W	TL,BA,CU,O	
3049	JJP0280923		Tl(Ba,La)2CuO4	Tl1Ba1.8La0.2Cu1O5-Z	Tl	1	Ba	1.8	La	0.2	Cu	1													O	5-Z			1989																												Tl1201																				42	57				42																																																																																																					THE OCCURRENCE OF SUPERCONDUCTIVITY IN THE TLBA(2)CUO(5-Z)-TYPE (1021) SYSTEM	198906	METASTABLE               ,METAL-INSULATOR TRANSITIO,RES	DEPARTMENT OF PHYSICS,NATIONAL TSING HUA UNIVERSITY,HSINCHU,TAIWAN 30043,R.O.C.	JJAP LETT ,28(1989)L923	D.C.LING,G.H.HWANG,H.C.KU,HSU,J.B.SHI,M.F.TAI,M.J.SHIH,S,T.J.WATSON-YANG,T.Y.LIN,W	TL,BA,CU,O	
3050	JJP0280923		Tl(Ba,La)2CuO4	Tl1Ba1.6La0.4Cu1O5-Z	Tl	1	Ba	1.6	La	0.4	Cu	1													O	5-Z			1989																												Tl1201																				40					40																																																																																																					THE OCCURRENCE OF SUPERCONDUCTIVITY IN THE TLBA(2)CUO(5-Z)-TYPE (1021) SYSTEM	198906	METASTABLE               ,METAL-INSULATOR TRANSITIO,RES	DEPARTMENT OF PHYSICS,NATIONAL TSING HUA UNIVERSITY,HSINCHU,TAIWAN 30043,R.O.C.	JJAP LETT ,28(1989)L923	D.C.LING,G.H.HWANG,H.C.KU,HSU,J.B.SHI,M.F.TAI,M.J.SHIH,S,T.J.WATSON-YANG,T.Y.LIN,W	TL,BA,CU,O	
3051	JJP0280923		Tl(Ba,La)2CuO4	Tl1Ba1.4La0.6Cu1O5-Z	Tl	1	Ba	1.4	La	0.6	Cu	1													O	5-Z			1989																												Tl1201																			42	45					45																																																																																																					THE OCCURRENCE OF SUPERCONDUCTIVITY IN THE TLBA(2)CUO(5-Z)-TYPE (1021) SYSTEM	198906	METASTABLE               ,METAL-INSULATOR TRANSITIO,RES	DEPARTMENT OF PHYSICS,NATIONAL TSING HUA UNIVERSITY,HSINCHU,TAIWAN 30043,R.O.C.	JJAP LETT ,28(1989)L923	D.C.LING,G.H.HWANG,H.C.KU,HSU,J.B.SHI,M.F.TAI,M.J.SHIH,S,T.J.WATSON-YANG,T.Y.LIN,W	TL,BA,CU,O	
3052	JJP0290586		(Y,Ca)Sr2(Cu,Pb)3O7	Sr2Y0.7Ca0.3Cu2.35Pb0.65O6.89	Sr	2	Y	0.7	Ca	0.3	Cu	2.35	Pb	0.65											O	Y	6.89	1	1990																											2					3.815		11.85														17					17																																																																																																					PREPARATION OF A NEW SUPERCONDUCTOR SR2Y0.7CA0.3CU2.35PB0.65OY	199004	SINGLE PHASE        ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS, NAMIKI, TSUKUBA, IBARAKI 305	JJAP,29(1990)L586	AKIRA ONO,YOSHISHIGE UCHIDA	SR,Y,CA,CU,PB,O	
3053	JJP0290586		(Y,Ca)Sr2(Cu,Pb)3O7	Sr2Y0.7Ca0.3Cu2.35Pb0.65O7.11	Sr	2	Y	0.7	Ca	0.3	Cu	2.35	Pb	0.65											O	Y	7.11	1	1990																											2					3.818		11.86																	4.2																																																																																																							PREPARATION OF A NEW SUPERCONDUCTOR SR2Y0.7CA0.3CU2.35PB0.65OY	199004	SINGLE PHASE        ,TC	NATIONAL INSTITUTE FOR RESEARCH IN INORGANIC MATERIALS, NAMIKI, TSUKUBA, IBARAKI 305	JJAP,29(1990)L586	AKIRA ONO,YOSHISHIGE UCHIDA	SR,Y,CA,CU,PB,O	
3054	DE0611670	65% O(18) replaced. -(dHc1/dT)=4.5 Oe/K. -(dHc/dT)=75 Oe/K. G-L = 45	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1988																											1	BKBO																		K		28					28						0.21	O	65			Oe		107																T/K		0.5			HC3054																																																																			DENSITY OF STATES AND ISOTOPE EFFECT IN BI(1)O(1) SUPERCONDUCTORS: EVIDENCE FOR NONPHONON MECHANISM	198810	ISOTOPE EFFECT           ,HC                       ,SUS                      ,MA	AT&T BELL LABORATIRIES,MURRAY HILL,NEW JERSEY	PHYS.REV.LETT.,61(1988)1670	A.M.MUJSCE,A.S.COOPER,B.BATLOGG,G.P.ESPINOSA,J.J.KRAJEWSKI,J.P.REMEIKA,JR.,L.W.RUPP,R.J.CAVA,W.F.PECK		
3055	DE0611670	85% O(18) replaced. -(dHc/dT)=50 Oe/K. G-L = 80.	Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3		3	1988																											1	BPBO																				10.5					10.5						0.22	O	85																																																																																													DENSITY OF STATES AND ISOTOPE EFFECT IN BI(1)O(1) SUPERCONDUCTORS: EVIDENCE FOR NONPHONON MECHANISM	198810	ISOTOPE EFFECT           ,HC                       ,SUS                      ,MA	AT&T BELL LABORATIRIES,MURRAY HILL,NEW JERSEY	PHYS.REV.LETT.,61(1988)1670	A.M.MUJSCE,A.S.COOPER,B.BATLOGG,G.P.ESPINOSA,J.J.KRAJEWSKI,J.P.REMEIKA,JR.,L.W.RUPP,R.J.CAVA,W.F.PECK		
3056	PHC1760087	AS-PREPARED	Bi2Sr2CuO6	Bi2Sr2Cu1O6+Z	Bi	2	Sr	2	Cu	1															O	6+Z		1	1991																											3	Bi2201				5.362	5.374	24.622																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3057	PHC1760087	ANNEALED IN AIR AT 500C	Bi2(Sr,Pb)2CuO6	Bi2Sr1.9Pb0.1Cu1O6+Z	Bi	2	Sr	1.9	Pb	0.1	Cu	1													O	6+Z		1	1991																											3	Bi2201				5.363	5.37	24.652														8					8																																																																																																					STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3058	PHC1760087	AS-PREPARED	Bi2(Sr,Pb)2CuO6	Bi2Sr1.85Pb0.15Cu1O6+Z	Bi	2	Sr	1.85	Pb	0.15	Cu	1													O	6+Z		1	1991																											3	Bi2201				5.36	5.376	24.621																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3059	PHC1760087	AS-PREPARED	Bi2(Sr,Pb)2CuO6	Bi2Sr1.8Pb0.2Cu1O6.129	Bi	2	Sr	1.8	Pb	0.2	Cu	1													O	6+Z	6.129	1	1991																											3	Bi2201				5.355	5.382	24.6																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3060	PHC1760087	AS-PREPARED	Bi2(Sr,Pb)2CuO6	Bi2Sr1.7Pb0.3Cu1O6.152	Bi	2	Sr	1.7	Pb	0.3	Cu	1													O	6+Z	6.152	1	1991																											3	Bi2201				5.351	5.397	24.529																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3061	PHC1760087	AS-PREPARED	Bi2(Sr,Pb)2CuO6	Bi2Sr1.6Pb0.4Cu1O6.172	Bi	2	Sr	1.6	Pb	0.4	Cu	1													O	6+Z	6.172	1	1991																											3	Bi2201				5.349	5.404	24.501																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3062	PHC1760087	AS-PREPARED	Bi2(Sr,Pb)2CuO6	Bi2Sr1.5Pb0.5Cu1O6+Z	Bi	2	Sr	1.5	Pb	0.5	Cu	1													O	6+Z		1	1991																											3	Bi2201				5.35	5.404	24.486																	2																																																																																																							STRUCTURAL AND TRANSPORT PROPERTIES OF BI2SR2-XMXCUO6+-Z (M=BIAND PB)			DEPARTMENT OF CHEMISTRY,RUTGERS,THE STATE UNIVERSITY OF NEW JERSEY,NEW BRUNSWICK,NJ 08903,USA	PHYSICA C,176(1991)87	H.T.SHIH,K.V.RAMANUJACHARY,M.GREENBLATT	BI,SR,CU,O,PB	
3063	CA0271623	SEMICONDUCTOR LIKE CONDUCTIVITY	LaBa2CuTaO8	La1Ba2Cu2Ta1O8+Y	La	1	Ba	2	Cu	2	Ta	1													O	8+Y			1988																											2		P4/MMM			3.967		12.052																	77																																																																																																							CATION ORDERING IN LA(1)BA(2)CU(3)TA(1)O(8+Y)	198809	CATION ORDERING          ,SEMICONDUCTIVITY         ,XRY                      ,RE	COVERNMENT INDUSTRIAL RESEARCH INSTITUTE,NAGOYA	JJAP LETT.,27(1988)L1623	AKIHIRO TSUZUKI,EIICHI SUDO,KEIKO KANI,MASANOBU AWANO,NORIMITSU MURAYAMA,SHOJI KAWAKAMI,YASUYOSHI TORII	LA,BA,CU,TA,O	
3064	PHC1760019	SEMICONDUCTOR LIKE BEHAVIOUR,UNIT CELL MODEL		Ta1Sr2Nd1.5Ce0.5Cu2O10	Ta	1	Sr	2	Nd	1.5	Ce	0.5	Cu	2											O	10		1	1991																											2	Ml1222	I4/MMM			3.881		28.93																																																																																																																								THE PREPARATION AND STRUCTURE OF A NEW LAYERED CUPRATE:TASR2(NDCE)2CU2OY,THE TA ANALOG OF THE TL-1222 PHASE			DEPARTMENT OF APPLIED CHEMISTRY,UNIVERSITY OF SCIENCE AND TECHNOLOGY OF CHINA,HEFEI,ANHUI 230026,CHINA	PHYSICA C,176(1991)19	CHEN ZUYAO,LI RUKANG,QIAN YITAI,ZHU YINGJIE	TA,SR,ND,CE,CU,O	
3065	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																					11				11																																																																			8			TP3065												4.5																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3066	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																																																																																												-3.87			TP3066												6.2																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3067	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																																																																																												-3.55			TP3067												6.8																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3068	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																			10		23				16.5																																																																			0.04			TP3068												25.3																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3069	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																																																																																												0.19			TP3069																															SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3070	PR0412623		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-Y	Pr	1.85	Ce	0.15	Cu	1															O	4-Y			1990																												T'																			7		25				16																																																																			-0.46			TP3070												12.5																			SUPERCONDUCTIVITY AND THERMOELECTRIC POWER OF PR1.85CE0.15CUO4-Y	199002	OXYGEN CONTENTS     ,RESISTANCE          ,THERMOELECTRIC POW	DEPARTMENT OF PHYSICS AND BASIC SCIENCE RESEARCH CENTER, POHANG INSTITUTE OF SCIENCE AND TECHNOLOGY, POHANG, 790-330, KOREA	PHYS.REV.B,41(1990)2623	K.H.HAN,SUNG-IK LEE,Y.S.SONG,Y.W.PARK,YOON H.JEONG,Z.S.LIM	PR,CE,CU,O	
3071	SSC0730637		TlBa2CaCu2O	Tl1Ba2Ca1Cu2O8	Tl	1	Ba	2	Ca	1	Cu	2													O	8		1	1990																												Tl2212																			104.33		111.66				107.995																																																																			0.89			TP3071												11.37																			THERMOPOWER OF 2122 THALLIUM THGH TEMPERATURE SUPERCONDUCTORS		THERMOPOWER         ,SINGLE PHASE	LOW TEMPERATURE LABORATORY, DEPARTMENT OF PHYSICS, INKIAN INSTITUTE OF TECHNOLOGY, MADRAS 600 036, INDIA,	SOLID STATE COMMUN,73(1990)637	C.K.SUBRAMANIAM,I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN,VIJAYASHREE RADHAKRISHNAN	TL,CA,BA,CU,O	
3072	SSC0730637		TlBa2CaCu2O	Tl1Ba2Ca1Cu2O8	Tl	1	Ba	2	Ca	1	Cu	2													O	8		1	1990																												Tl2212																			102.74		107.16			2.9	104.95																																																																			5.59			TP3072												1.609																			THERMOPOWER OF 2122 THALLIUM THGH TEMPERATURE SUPERCONDUCTORS		THERMOPOWER         ,SINGLE PHASE	LOW TEMPERATURE LABORATORY, DEPARTMENT OF PHYSICS, INKIAN INSTITUTE OF TECHNOLOGY, MADRAS 600 036, INDIA,	SOLID STATE COMMUN,73(1990)637	C.K.SUBRAMANIAM,I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.M.IYER,R.SRINIVASAN,VIJAYASHREE RADHAKRISHNAN	TL,CA,BA,CU,O	
3073	SSC0730501	S//=6UV/K,SN=2UV/K,SAMPLE=4X0.2X0.005MM3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																			84	85					85																																																																			6			TP3073													0.15	6000																	THERMOELECTRIC POWER OF BI2SR2CACU2O8 SINGLE CRYSTALS WITH VARYING OXYGEN STOICHIOMETRY		THERMOELECTRIC POWER,SINGLE CRYSTALS     ,OXYGEN STOICHIOMET	INSTITUTE OF PHYSICS OF THE UNIVERSITY, ZAGREB, P.O.B. 304, ZAGREB, YUGOSLAVIA	SOLID STATE COMMUN,73(1990)501	B.KESZEI,J.LUKATELA,L.FORRO	BI,SR,CA,CU,O	
3074	SSC0730501		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																				60					60																																																																			18.9			TP3074																															THERMOELECTRIC POWER OF BI2SR2CACU2O8 SINGLE CRYSTALS WITH VARYING OXYGEN STOICHIOMETRY		THERMOELECTRIC POWER,SINGLE CRYSTALS     ,OXYGEN STOICHIOMET	INSTITUTE OF PHYSICS OF THE UNIVERSITY, ZAGREB, P.O.B. 304, ZAGREB, YUGOSLAVIA	SOLID STATE COMMUN,73(1990)501	B.KESZEI,J.LUKATELA,L.FORRO	BI,SR,CA,CU,O	
3075	SSC0730501		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																				71.5					71.5																																																																			14.5			TP3075																															THERMOELECTRIC POWER OF BI2SR2CACU2O8 SINGLE CRYSTALS WITH VARYING OXYGEN STOICHIOMETRY		THERMOELECTRIC POWER,SINGLE CRYSTALS     ,OXYGEN STOICHIOMET	INSTITUTE OF PHYSICS OF THE UNIVERSITY, ZAGREB, P.O.B. 304, ZAGREB, YUGOSLAVIA	SOLID STATE COMMUN,73(1990)501	B.KESZEI,J.LUKATELA,L.FORRO	BI,SR,CA,CU,O	
3076	SSC0730053	2223+2212(MAJOR)	Tl2Ba2Ca2Cu3O10	Tl2Ca2Ba2Cu3O10	Tl	2	Ca	2	Ba	2	Cu	3													O	10		2	1990																												Tl2223																			112	118	122			10	118																																																																			5.3			TP3076												5																			THERMOELECTRIC POWER OF TL-CA-BA-CU-O AND PR-TL-SR-CA-CU-O HIGH TC SUPERCONDUCTORS	199001	RESISTANCE          ,THERMOELECTRIC POWE	PHYSICS DEPARTMENT; CHEMISTRY DEPARTMENT, TEXAS A&M UNIVERSITY, COLLEGE STATION, TX 77843 USA	SOLID STATE COMMUN.,73(1990)53	A.CLEARFIELD,A.K.BAHATNAGAR,A.M.HERMANN,D.G.NAUGLE,P.J.SQUATTRITO,Q.A.SHAMS,R.PAN,Z.Z.SHENG	TL,CA,BA,CU,O,PR,SR	
3077	SSC0730053	2223+2212LARGE AMOUNT OF 2223	Tl2Ba2Ca2Cu3O10	Tl2Ca2Ba2Cu3O10	Tl	2	Ca	2	Ba	2	Cu	3													O	10		2	1990																												Tl2223																			112	118	122				118																																																																			1.3			TP3077																															THERMOELECTRIC POWER OF TL-CA-BA-CU-O AND PR-TL-SR-CA-CU-O HIGH TC SUPERCONDUCTORS	199001	RESISTANCE          ,THERMOELECTRIC POWE	PHYSICS DEPARTMENT; CHEMISTRY DEPARTMENT, TEXAS A&M UNIVERSITY, COLLEGE STATION, TX 77843 USA	SOLID STATE COMMUN.,73(1990)53	A.CLEARFIELD,A.K.BAHATNAGAR,A.M.HERMANN,D.G.NAUGLE,P.J.SQUATTRITO,Q.A.SHAMS,R.PAN,Z.Z.SHENG	TL,CA,BA,CU,O,PR,SR	
3078	SSC0730053		PrTl2Sr2Ca4Cu5O	Pr1Tl2Sr2Ca4Cu5O2	Pr	1	Tl	2	Sr	2	Ca	4	Cu	5											O	X	2		1990																																															79		97				88																																																																			13			TP3078																															THERMOELECTRIC POWER OF TL-CA-BA-CU-O AND PR-TL-SR-CA-CU-O HIGH TC SUPERCONDUCTORS	199001	RESISTANCE          ,THERMOELECTRIC POWE	PHYSICS DEPARTMENT; CHEMISTRY DEPARTMENT, TEXAS A&M UNIVERSITY, COLLEGE STATION, TX 77843 USA	SOLID STATE COMMUN.,73(1990)53	A.CLEARFIELD,A.K.BAHATNAGAR,A.M.HERMANN,D.G.NAUGLE,P.J.SQUATTRITO,Q.A.SHAMS,R.PAN,Z.Z.SHENG	TL,CA,BA,CU,O,PR,SR	
3079	SU1590081		Pr2(Sr,La)2Cu2O6	Pr2Sr0.8La1.2Cu2O6+Z	Pr	2	Sr	0.8	La	1.2	Cu	2													O	6+Z			1989																											3	Pb3201				5.333	5.421	12.609													26	31	32				31																																																																																																					SUPERCONDUCTIVITY IN (PB,BI)(2)SR(2-X)LA(X)CU(2)O(6+Z)	198906	HREM                     ,FABRICATION              ,STRUCTUR	GORLAEUS LABORATORIES,LEIDEN UNIVERSITY,P.O.BOX 9502,2300RA LEIDEN,THE NETHERLANDS	PHISICA C ,159(1989)81	G.VAN TENDELOO,H.W.ZANDBERGEN,J.M.VAN RUITENBEEK,L.J.DE JONGH,S.AMELINCKX,W.T.FU	PB,BI,SR,LA,CU,O,	
3080	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.7Pb0.3Sr2Ca2Cu3OX	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	X		2	1991																											3					5.425	5.313	37.049													104		116				110																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3081	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.3Pb0.7Sr2Ca2Cu3OX	Bi	1.3	Pb	0.7	Sr	2	Ca	2	Cu	3											O	X			1991																											3					5.4	5.374	37.101													112		120				116																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3082	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.7Pb0.2Sb0.1Sr2Ca2Cu3OX	Bi	1.7	Pb	0.2	Sb	0.1	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.397	5.38	36.976													105		116				110.5																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3083	PHC1760179	SEMICONDUCTOR-LIKE,2223 PHASE DOMINANT	(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.3Pb0.5Sb0.2Sr2Ca2Cu3OX	Bi	1.3	Pb	0.5	Sb	0.2	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.397	5.344	36.921													70		115				92.5																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3084	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.7Pb0.2V0.1Sr2Ca2Cu3OX	Bi	1.7	Pb	0.2	V	0.1	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.425	5.406	37.105													105		115				110																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3085	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.3Pb0.5V0.2Sr2Ca2Cu3OX	Bi	1.3	Pb	0.5	V	0.2	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.408	5.374	37.084													106		117				111.5																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3086	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,Mo)2Sr2Ca2Cu3O10	Bi1.7Pb0.2Mo0.1Sr2Ca2Cu3OX	Bi	1.7	Pb	0.2	Mo	0.1	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.416	5.401	37.026													105		115				110																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3087	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,Mo)2Sr2Ca2Cu3O10	Bi1.3Pb0.5Mo0.2Sr2Ca2Cu3OX	Bi	1.3	Pb	0.5	Mo	0.2	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.402	5.371	37.053													105		122				113.5																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3088	PHC1760179	METALLIC,2223 PHASE DOMINANT	(Bi,Pb,W)2Sr2Ca2Cu3O10	Bi1.7Pb0.2W0.1Sr2Ca2Cu3OX	Bi	1.7	Pb	0.2	W	0.1	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.39	5.358	36.978													93		113				103																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3089	PHC1760179	METALLIC,2223 DOMINANT,PB0.2W0.1 SEEMS TO BE FAVOR THE FORMATIONOF 2223 PHASE MORE THAN PB0.5W0.2	(Bi,Pb,W)2Sr2Ca2Cu3O10	Bi1.3Pb0.5W0.2Sr2Ca2Cu3OX	Bi	1.3	Pb	0.5	W	0.2	Sr	2	Ca	2	Cu	3									O	X		2	1991																											3					5.383	5.352	37.018													71		118				94.5																																																																																																					COMPARISON OF PB,PB-SB,PB-V,PB-MO AND PB-W SUBSTITUTED BI-SR-CA-CU-O			DEPAERMENT OF PHYSICS,UNIVERSITY OF ARKANSAS,FAYETTEVILLE,AR 72701,USA	PHYSICA C,176(1991)179	S.NASRAZADANI,XIN,Y,Z.Z.SHENG	PB,SB,V,MO,W,BI,SR,CA,CU,O	
3090	PHC1770310	HC1 FROM M VS H CURVE	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Y	Nd	1.85	Ce	0.15	Cu	1															O	4-Y		3	1991																												T'																				16.5	22				16.5														20	1900																																																																																						AN UPPER LIMIT ON THE LOWER CRITICAL FIELD IN SINGLE CRYSTAL ND1.85CE0.15CUO4-Y			TATA INSTITUTE OF FUNDAMENTAL RESEARCH,HOMI BHABHA ROAD,BOMBAY400005,INDIA	PHYSICA C,177(1991)310	C.K.SUBRAMANIAM,D.MCK.PAUL,G.BALAKRISHNAN,R.VIJAYARAGHAVAN,S.PINOL	ND,CE,CU,O	
3091	PR04311508			Eu2.667Ce1.333La1.333Ba1.333Sr1.333Cu6OY	Eu	2.667	Ce	1.333	La	1.333	Ba	1.333	Sr	1.333	Cu	6									O	Y			1991																												446																			28.5						28.5																																																																			22			TP3091																															thermoelectric power of the (Eu,Ce)4(Ba,Eu)4Cu6Oy phase and the T* phase: Comparison between superconducting and nonsuperconducting compounds	199105		Supercoductivity Reserch Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)11508	A. Ichinose,H. Yamauchi,K. Kudo,K. Matsuura,S. Ikegawa,S. Tanaka,T. Wada,T. Yamashita		
3092	PR04311508			Y2.667Ce1.333La1.333Ba1.333Sr1.333Cu6OY	Y	2.667	Ce	1.333	La	1.333	Ba	1.333	Sr	1.333	Cu	6									O	Y			1991																												446																							2																																																																					33.2			TP3092																															thermoelectric power of the (Eu,Ce)4(Ba,Eu)4Cu6Oy phase and the T* phase: Comparison between superconducting and nonsuperconducting compounds	199105		Supercoductivity Reserch Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)11508	A. Ichinose,H. Yamauchi,K. Kudo,K. Matsuura,S. Ikegawa,S. Tanaka,T. Wada,T. Yamashita		
3093	PR04311508			Nd1.4Ce0.2Sr0.4Cu1O4-Z	Nd	1.4	Ce	0.2	Sr	0.4	Cu	1													O	4-Z			1991																												T*																			23.1						23.1																																																																			22.3			TP3093																0.00000000304					RH3093										thermoelectric power of the (Eu,Ce)4(Ba,Eu)4Cu6Oy phase and the T* phase: Comparison between superconducting and nonsuperconducting compounds	199105		Supercoductivity Reserch Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)11508	A. Ichinose,H. Yamauchi,K. Kudo,K. Matsuura,S. Ikegawa,S. Tanaka,T. Wada,T. Yamashita		
3094	PR04311508			Nd1.4Ce0.2Sr0.4Cu0.985Zn0.015O4-Z	Nd	1.4	Ce	0.2	Sr	0.4	Cu	0.985	Zn	0.015											O	4-Z			1991																												T*																							2																																																																					36			TP3094																0.00000000317					RH3094										thermoelectric power of the (Eu,Ce)4(Ba,Eu)4Cu6Oy phase and the T* phase: Comparison between superconducting and nonsuperconducting compounds	199105		Supercoductivity Reserch Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)11508	A. Ichinose,H. Yamauchi,K. Kudo,K. Matsuura,S. Ikegawa,S. Tanaka,T. Wada,T. Yamashita		
3095	PR0442815	PENET FROM MAGNETIZATION AFTER CORRECTION	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																											2	Y123																				66					66																																												2600																																																									MAGNETIC PENETRATION DEPTH OF OXYGEN-DEFICIENT YBA2CU3O7-Z SINGLE CRYSTALS (TC=66K)	199108		DEPARTMENT OF PHYSICS AND MATERIALS RESEARTCH LABORATORY,UNIVERSITY OF ILLINOIS AT URABANA-CHAMPAIGN,1110 WEST GREEN STREET,URBANA,ILLINOIS 61801	PHYS.REV.B,44(1991)2815	D.M.GINSBERG,W.C.LEE	Y,BA,CU,O	
3096	CEM0780192		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.1	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	6.1		1	1989																											2	Y123				3.861		11.826														50					50																																																																																																					LETTER TO THE EDITOROBSERVATION OF SUKPERCONDUCTIVITY IN (Y1-XCAX)BA2CU3O6			E.I.DU PONT DE NEMOURS AND CO.,INC.,CENTRAL RESEARCH AND DEVELOPMENT,EXPERIMENTAL STATION,WILMINGTON,DELAWARE 19880-0356	J.SOL.STATE CHEM.,78(1989)192	E.M.MCCARRON III,J.B.PARISE,M.K.CRAWFORD	Y,CA,BA,CU,O	
3097	JML0100760			Sb1Pb1Ca1Ba2Cu2OX	Sb	1	Pb	1	Ca	1	Ba	2	Cu	2											O	X		2	1991																											3					5.11	6.321	18.512													25						25																																																																																																					SYNTHESIS AND STRUCTURE OF (SBPB)CABA2CU2OX)			CHEMISTRY,RADIOCHEMISTRY AND APPLIED CHEMISTRY DIVISIONS,CHEMICAL GROUP,BHABHA ATOMIC RESEARCH CENTRE,TROMBAY,BOMBAY 400085,INDIA	J.MATER.SCI.LETT.,10(1991)760	G.M.PHATAK,M.D.SASTRY,R.A.GUNASEKARAN,R.M.IYER,U.R.K.RAO	SB,PB,CA,BA,CU,O	
3098	PHC1750119	TWO PHASES,NO MEISSNER EFFECT,NO Y123 PHASE		Y1Ba2Cu2W1OY	Y	1	Ba	2	Cu	2	W	1													O	Y		2	1991																																																	60				60																																																																																																					Superconductivity in the Ba-Y-Cu-W-O system			Instituto Fisica, Universidad Nacional Auto'noma de Me'xico, a.p. 20-364, 01000 Me'xico D.F., Me'xco	Physica.c,175(1991)119-126	Bokhimi		
3099	PHC1750119	TWO PHASES,NO MEISSNER EFFECT,NO Y123 PHASE		Y1Ba2Cu2W1OY	Y	1	Ba	2	Cu	2	W	1													O	Y		2	1991																																															65		92				78.5																																																																																																					Superconductivity in the Ba-Y-Cu-W-O system			Instituto Fisica, Universidad Nacional Auto'noma de Me'xico, a.p. 20-364, 01000 Me'xico D.F., Me'xco	Physica.c,175(1991)119-126	Bokhimi		
3100	PHC1800358	NEELT BY MUON-SR	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1991								258																																																																																																																																																		DISRUPTION OF ANTIFERROMAGNETIC ORDER IN ZN-DOPED LA2CUO4			TEXAS TECH UNIVERSITY,LUBBOCK,TX 79409,USA	PHYSICA C,180(1991)358	C.BOEKEMA,D.W.COOKE,J.C.LAM,J.E.CROW,R.L.LICHTI,S.F.J.COX,S.T.TING	ZN,LA,CU,O	
3101	PHC1800358	NEELT BY MUON-SR	La2(Cu,Zn)O4	La2Cu0.98Zn0.02O4	La	2	Cu	0.98	Zn	0.02															O	4		1	1991								208																																																																																																																																																		DISRUPTION OF ANTIFERROMAGNETIC ORDER IN ZN-DOPED LA2CUO4			TEXAS TECH UNIVERSITY,LUBBOCK,TX 79409,USA	PHYSICA C,180(1991)358	C.BOEKEMA,D.W.COOKE,J.C.LAM,J.E.CROW,R.L.LICHTI,S.F.J.COX,S.T.TING	ZN,LA,CU,O	
3102	PHC1800358	NEELT BY MUON-SR	La2(Cu,Zn)O4	La2Cu0.96Zn0.04O4	La	2	Cu	0.96	Zn	0.04															O	4		1	1991								194																																																																																																																																																		DISRUPTION OF ANTIFERROMAGNETIC ORDER IN ZN-DOPED LA2CUO4			TEXAS TECH UNIVERSITY,LUBBOCK,TX 79409,USA	PHYSICA C,180(1991)358	C.BOEKEMA,D.W.COOKE,J.C.LAM,J.E.CROW,R.L.LICHTI,S.F.J.COX,S.T.TING	ZN,LA,CU,O	
3103	PHC1800358	NEELT BY MUON-SR	La2(Cu,Zn)O4	La2Cu0.92Zn0.08O4	La	2	Cu	0.92	Zn	0.08															O	4		1	1991								181																																																																																																																																																		DISRUPTION OF ANTIFERROMAGNETIC ORDER IN ZN-DOPED LA2CUO4			TEXAS TECH UNIVERSITY,LUBBOCK,TX 79409,USA	PHYSICA C,180(1991)358	C.BOEKEMA,D.W.COOKE,J.C.LAM,J.E.CROW,R.L.LICHTI,S.F.J.COX,S.T.TING	ZN,LA,CU,O	
3104	PHC1800358	NEELT BY MUON-SR	La2(Cu,Zn)O4	La2Cu0.9Zn0.1O4	La	2	Cu	0.9	Zn	0.1															O	4		1	1991								103																																																																																																																																																		DISRUPTION OF ANTIFERROMAGNETIC ORDER IN ZN-DOPED LA2CUO4			TEXAS TECH UNIVERSITY,LUBBOCK,TX 79409,USA	PHYSICA C,180(1991)358	C.BOEKEMA,D.W.COOKE,J.C.LAM,J.E.CROW,R.L.LICHTI,S.F.J.COX,S.T.TING	ZN,LA,CU,O	
3105	PHC1800324		La(Ca,Ba)2(Cu,Zn)3O7	La1Ca1Ba1Cu2.95Zn0.05O7-Z	La	1	Ca	1	Ba	1	Cu	2.95	Zn	0.05											O	7-Z			1991																											2	Y123				3.87		11.634													55						55																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3106	PHC1800324		La(Ca,Ba)2(Cu,Zn)3O7	La1Ca1Ba1Cu2.9Zn0.1O7-Z	La	1	Ca	1	Ba	1	Cu	2.9	Zn	0.1											O	7-Z			1991																											2	Y123				3.867		11.622													37						37																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3107	PHC1800324		La(Ca,Ba)2(Cu,Zn)3O7	La1Ca1Ba1Cu2.8Zn0.2O7-Z	La	1	Ca	1	Ba	1	Cu	2.8	Zn	0.2											O	7-Z			1991																											2	Y123				3.868		11.628													30						30																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3108	PHC1800324		La(Ca,Ba)2(Cu,Zn)3O7	La1Ca1Ba1Cu2.7Zn0.3O7-Z	La	1	Ca	1	Ba	1	Cu	2.7	Zn	0.3											O	7-Z			1991																											2	Y123				3.879		11.662													20						20																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3109	PHC1800324		La(Ca,Ba)2(Cu,Zn)3O7	La1Ca1Ba1Cu2.6Zn0.4O7-Z	La	1	Ca	1	Ba	1	Cu	2.6	Zn	0.4											O	7-Z			1991																											2	Y123				3.877		11.628																	42																																																																																																							EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3110	PHC1800324		LaBaCaCu3O7	La1Ba1Ca1Cu3O6.856	La	1	Ba	1	Ca	1	Cu	3													O	7-Z	6.856	1	1991																											2	Y123				3.871		11.61													66						66																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3111	PHC1800324		La(Ca,Ba)2(Cu,Ni)3O7	La1Ba1Ca1Cu2.9Ni0.1O6.85	La	1	Ba	1	Ca	1	Cu	2.9	Ni	0.1											O	7-Z	6.85	1	1991																											2	Y123				3.866		11.628													45						45																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3112	PHC1800324		La(Ca,Ba)2(Cu,Ni)3O7	La1Ba1Ca1Cu2.8Ni0.2O6.837	La	1	Ba	1	Ca	1	Cu	2.8	Ni	0.2											O	7-Z	6.837	1	1991																											2	Y123				3.871		11.624													30						30																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3113	PHC1800324		La(Ca,Ba)2(Cu,Ni)3O7	La1Ba1Ca1Cu2.7Ni0.3O6.848	La	1	Ba	1	Ca	1	Cu	2.7	Ni	0.3											O	7-Z	6.848	1	1991																											2	Y123				3.875		11.639													28						28																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3114	PHC1800324		La(Ca,Ba)2(Cu,Ni)3O7	La1Ba1Ca1Cu2.6Ni0.4O6.854	La	1	Ba	1	Ca	1	Cu	2.6	Ni	0.4											O	7-Z	6.854	1	1991																											2	Y123				3.876		11.622													24						24																																																																																																					EFFECT OF PARTIAL SUBSTITUTION OF NI AND ZN FOR CU IN CABALACU3O7-Z SUPERCONDUCTOR			CHEMISTRY DIVISION,BHABHA AROMIC RESEARCH CENTRE,BOMBAY-400085,INDIA	PHYSICA C,180(1991)324	C.V.TOMY,I.K.GOPALAKRISHINAN,J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER,S.K.MALIK	ZN,NI,CA,BA,LA,CU,O	
3115	PHC1770159		YBa2Cu3O6	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	6		1	1991																											2	Y123																																																																																															TP3115																															VARIABLE-RANGE HOPPING IN YBA2(CU1-XMX)3O6+Z  M=FE,ZN!			CENTRE DE RECHERCHE EN PHYSIQUE DU SOLIDE AND DEPARTMENT DE PHYSIQUE,UNIVERSITE DE SHERBROOKE,SHERBROOKE,QUE.,CANADA JIK2R1	PHYSICA C,177(1991)159	M.AUBIN,P.FOURNIER,R.GAGNON	Y,BA,CU,FE,ZN,O	
3116	PHC1770023	2223 IS DOMINANT,SECOND PHASE<5% BY XRD		Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1991																												Tl2223																					121				121																																																																	THC3116																																				THERMAL CONDUCTIVITY OF TL2BA2CA2CU3O10 CERAMICS FROM 300K DOWN TO 0.1K			DEPARTMENT OF PHYSICS,UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN 48109,USA	PHYSICA C,177(1991)23	C.UHER,J.SHEWCHUN,S.D.PEACOR	TL,BA,CA,CU,O	
3117	PHC1770023	SAME AS 3116 DATA		Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1991																												Tl2223																					121				121																																																																	THC3117																																				THERMAL CONDUCTIVITY OF TL2BA2CA2CU3O10 CERAMICS FROM 300K DOWN TO 0.1K			DEPARTMENT OF PHYSICS,UNIVERSITY OF MICHIGAN,ANN ARBOR,MICHIGAN 48109,USA	PHYSICA C,177(1991)23	C.UHER,J.SHEWCHUN,S.D.PEACOR	TL,BA,CA,CU,O	
3118	JPS0581883	X=0.082(EPMA),TD1=275,TD2=26,PHASE TRANSITION	(La,Ba)2CuO4	La1.906Ba0.094Cu1O4-Z	La	1.906	Ba	0.094	Cu	1															O	4-Z		1	1989																											2	T																				32					32																																																																																																					ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3119	JPS0581883	X=0.102(EPMA),TD1=210,TD2=49	(La,Ba)2CuO4	La1.882Ba0.118Cu1O4-Z	La	1.882	Ba	0.118	Cu	1															O	4-Z		1	1989																											2	T				3.78		13.27														9.2					9.2	TC3119																																																																		6.5			TP3119																															ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3120	JPS0581883	X=0.142(EPMA),TD1=137,TD2=49	(La,Ba)2CuO4	La1.858Ba0.142Cu1O4-Z	La	1.858	Ba	0.142	Cu	1															O	4-Z		1	1989																											2	T																				28.9					28.9																																																																																																					ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3121	JPS0581883	X=0.158(EPMA),TD1=95.5,TD2=24.3	(La,Ba)2CuO4	La1.842Ba0.158Cu1O4-Z	La	1.842	Ba	0.158	Cu	1															O	4-Z		1	1989																											2	T																																																																																																																														ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3122	JPS0581883	X=0.064(EPMA)	(La,Ba)2CuO4	La1.922Ba0.078Cu1O4-Z	La	1.922	Ba	0.078	Cu	1															O	4-Z		1	1989																											2	T																				26.6					26.6																																																																																																					ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3123	JPS0581883	X=0.174(EPMA)	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4-Z	La	1.8	Ba	0.2	Cu	1															O	4-Z		1	1989																											2	T																				20.9					20.9																																																																																																					ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3124	JPS0581883	X=0.212(EPMA)	(LA,BA)2CUO4	La1.76Ba0.24Cu1O4-Z	La	1.76	Ba	0.24	Cu	1															O	4-Z		1	1989																											2	T																				14					14																																																																																																					ANOMALOUS CHANGE IN CRYSTALLINE STRUCTURE OF (LA1-XBAX)2CUO4-Z	198906		DEPARTMENT OF PHYSICS,HIROSHIMA UNIVERSITY,HIROSHIMA 730	J.PHYS.SOC.JAPAN,58(1989)1883	RAKASHI SUZUKI,TOSHIZO FUJITA	LA,BA,CU,O	
3125	PHC1760373			Nd1.42Ce0.18Sr0.4Cu1O4-Z	Nd	1.42	Ce	0.18	Sr	0.4	Cu	1													O	4-Z		1	1991																												T*																				17.3					17.3																																																																																											RH3125										HALL EFFECT AND SUPERCONDUCTING PROPERTIES OF (ND0.8-XCEXSR0.2)2CUO4-Z WITH T STRUCTURE			SUPERCONDUCTIVITY RESEARCH LAVORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,176(1991)373	MICHIKAZU KOSUGE,NAOKI KOSHIZUKA,SHOJI TANAKA,SUMIO IKEGAWA	ND,CE,SR,CU,O	
3126	PHC1760373	HHC1 BY M VS H CURVE		Nd1.4Ce0.2Sr0.4Cu1O4-Z	Nd	1.4	Ce	0.2	Sr	0.4	Cu	1													O	4-Z		1	1991																												T*																			21.8	22.7					22.7													40									15									0.91							46					4200																																																RH3126										HALL EFFECT AND SUPERCONDUCTING PROPERTIES OF (ND0.8-XCEXSR0.2)2CUO4-Z WITH T STRUCTURE			SUPERCONDUCTIVITY RESEARCH LAVORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,176(1991)373	MICHIKAZU KOSUGE,NAOKI KOSHIZUKA,SHOJI TANAKA,SUMIO IKEGAWA	ND,CE,SR,CU,O	
3127	PHC1760373			Nd1.38Ce0.22Sr0.4Cu1O4-Z	Nd	1.38	Ce	0.22	Sr	0.4	Cu	1													O	4-Z		1	1991																												T*																				18.2					18.2																																																																																											RH3127										HALL EFFECT AND SUPERCONDUCTING PROPERTIES OF (ND0.8-XCEXSR0.2)2CUO4-Z WITH T STRUCTURE			SUPERCONDUCTIVITY RESEARCH LAVORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,176(1991)373	MICHIKAZU KOSUGE,NAOKI KOSHIZUKA,SHOJI TANAKA,SUMIO IKEGAWA	ND,CE,SR,CU,O	
3128	PHC1760373	SEMICONDUCTOR LIKE		Nd1.3Ce0.3Sr0.4Cu1O4-Z	Nd	1.3	Ce	0.3	Sr	0.4	Cu	1													O	4-Z		1	1991																												T*																							4.2																																																																																													RH3128										HALL EFFECT AND SUPERCONDUCTING PROPERTIES OF (ND0.8-XCEXSR0.2)2CUO4-Z WITH T STRUCTURE			SUPERCONDUCTIVITY RESEARCH LAVORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,176(1991)373	MICHIKAZU KOSUGE,NAOKI KOSHIZUKA,SHOJI TANAKA,SUMIO IKEGAWA	ND,CE,SR,CU,O	
3129	PHC1810068	OZ BY TGA	Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Pr0.5Cu2O8.53	Bi	2	Ca	2.5	Pr	0.5	Cu	2													O	8+Z	8.53	1	1991									6.5																		2	Bi2212																				45	56				45										38																																																																												0.0000000019					RH3129										PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3130	PHC1810068		Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Nd0.5Cu2O8.43	Bi	2	Ca	2.5	Nd	0.5	Cu	2													O	8+Z	8.43	1	1991																											2	Bi2212																				33.5	52				33.5																																																																																																					PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3131	PHC1810068		Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Sm0.5Cu2O8.33	Bi	2	Ca	2.5	Sm	0.5	Cu	2													O	8+Z	8.33	1	1991																											2	Bi2212																				22	59				22																																																																																						0.0000000019					RH3131										PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3132	PHC1810068		Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Eu0.5Cu2O8.31	Bi	2	Ca	2.5	Eu	0.5	Cu	2													O	8+Z	8.31	1	1991																											2	Bi2212																				7	35				7																																																																																																					PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3133	PHC1810068		Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Gd0.5Cu2O8.33	Bi	2	Ca	2.5	Gd	0.5	Cu	2													O	8+Z	8.33	1	1991																											2	Bi2212																				4	25				4																																																																																						0.000000003					RH3133										PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3134	PHC1810068	OZ BY TGA	Bi2(Ca,R)2CaCu2O8	Bi2Ca2.5Pr0.5Cu2O8.41	Bi	2	Ca	2.5	Pr	0.5	Cu	2													O	8+Z	8.41	1	1991																											2	Bi2212																																																																																																															0.00000000265					RH3134										PREPARATION AND PROPERTIES OF SUPERCONDUCTING BI2CA3-XRXCU2O8+Z			CENTER FOR SUPERCONDUCTIVITY RESEARCH,DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF MARYLAND,COLLEGE PARK,MD 20742,USA	PHYSICA C,181(1991)68	R.L.GREENE,S.M.GREEN,W.JIANG	BI,CA,CU,O,R	
3135	PHC1810063	+2201+CUO	Bi2(Sr,Li)2CaCu2O8	Bi2Sr1.8Li0.2Ca1Cu2O8	Bi	2	Sr	1.8	Li	0.2	Ca	1	Cu	2											O	8+Z	8		1991																											2	Bi2212				5.429		30.811													77						77																																																																																																					"LITHIUM/STRONTIUM EXCHANGE IN ""2212"" BISMUTH SUPERCONDUCTORS"			FACULTY OF SCIENCE AND TECHNOLOGY,THAMMASAT UNIVERSITY,RANGSIT,PATUM THANI 12121,THAILAND	PHYSICA C,181(1991)63	C.ENGKAGUL,I.M.TANG,J.LAKSANABOONSONG,K.EAIPRASERTSAK,K.TREECHAIRUSME,N.CHAICHIT,N.CHIENGPRATOOM,S.LEELAPRUTE	LA,SR,BI,CA,CU,O	
3136	PHC1810063	+2201+CUO	Bi2(Sr,Li)2CaCu2O8	Bi2Sr1.6Li0.4Ca1Cu2O7.87	Bi	2	Sr	1.6	Li	0.4	Ca	1	Cu	2											O	8+Z	7.87		1991																											2	Bi2212				5.408		30.795													86						86																																																																																																					"LITHIUM/STRONTIUM EXCHANGE IN ""2212"" BISMUTH SUPERCONDUCTORS"			FACULTY OF SCIENCE AND TECHNOLOGY,THAMMASAT UNIVERSITY,RANGSIT,PATUM THANI 12121,THAILAND	PHYSICA C,181(1991)63	C.ENGKAGUL,I.M.TANG,J.LAKSANABOONSONG,K.EAIPRASERTSAK,K.TREECHAIRUSME,N.CHAICHIT,N.CHIENGPRATOOM,S.LEELAPRUTE	LA,SR,BI,CA,CU,O	
3137	PHC1810063		Bi2(Sr,Li)2CaCu2O8	Bi2Sr1.4Li0.6Ca1Cu2O7.7	Bi	2	Sr	1.4	Li	0.6	Ca	1	Cu	2											O	8+Z	7.7		1991																											2	Bi2212				5.398		30.806													94						94																																																																																																					"LITHIUM/STRONTIUM EXCHANGE IN ""2212"" BISMUTH SUPERCONDUCTORS"			FACULTY OF SCIENCE AND TECHNOLOGY,THAMMASAT UNIVERSITY,RANGSIT,PATUM THANI 12121,THAILAND	PHYSICA C,181(1991)63	C.ENGKAGUL,I.M.TANG,J.LAKSANABOONSONG,K.EAIPRASERTSAK,K.TREECHAIRUSME,N.CHAICHIT,N.CHIENGPRATOOM,S.LEELAPRUTE	LA,SR,BI,CA,CU,O	
3138	PHC1800407	+BI2212+CA2PBO4+CUO	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.4Pb0.6Sr2Ca2Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	2	Cu	3											O	7		2	1991																											2	Bi2223																			74.5	108.5					108.5																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3139	PHC1800407	+2212+CA2PBO4+CUO	(Bi,Pb)2Sr2(CaGa)2Cu3O10	Bi1.4Pb0.6Sr2Ca1.9Ga0.1Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.9	Ga	0.1	Cu	3									O	7		2	1991																											2	Bi2223																			65.5	104.4					104.4																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3140	PHC1800407	+2223+2212+CA2PBO4		Bi1.4Pb0.6Sr2Ca1.8Ga0.2Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.8	Ga	0.2	Cu	3									O	7		2	1991																											2																					68.2	103.4				68.2																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3141	PHC1800407	+CA2PBO4	(Bi,Pb)2Sr2(Ca,Ga)Cu2O8	Bi1.4Pb0.6Sr2Ca1.7Ga0.3Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.7	Ga	0.3	Cu	3									O	7		2	1991																											2	Bi2212																				67.4					67.4																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3142	PHC1800407	+CA2PBO4	(Bi,Pb)2Sr2(Ca,Ga)Cu2O8	Bi1.4Pb0.6Sr2Ca1.6Ga0.4Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.6	Ga	0.4	Cu	3									O	7		2	1991																											2	Bi2212																				69.4					69.4																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3143	PHC1800407	+2201+CA2PBO4+CUO	(Bi,Pb)2Sr2(Ca,Ga)Cu2O8	Bi1.4Pb0.6Sr2Ca1.4Ga0.6Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.4	Ga	0.6	Cu	3									O	7		2	1991																											2	Bi2212																				70.6					70.6																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3144	PHC1800407	+2201+CA2PBO4	(Bi,Pb)2Sr2(Ca,Ga)Cu2O8	Bi1.4Pb0.6Sr2Ca1.2Ga0.8Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1.2	Ga	0.8	Cu	3									O	7		2	1991																											2	Bi2212																				67.7					67.7																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3145	PHC1800407	+2212+2201+CA2PBO4	(Bi,Pb)2Sr2(Ca,Ga)Cu2O8	Bi1.4Pb0.6Sr2Ca1Ga1Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ca	1	Ga	1	Cu	3									O	7		2	1991																											2																					66.5					66.5																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3146	PHC1800407	+CA2PBO4+CUO		Bi1.4Pb0.6Sr2Ga2Cu3O7	Bi	1.4	Pb	0.6	Sr	2	Ga	2	Cu	3											O	7		2	1991																											2	Bi2201																				62.7					62.7																																																																																																					THE EFFECT OF GALLIUM SUBSTITUTION ON THE SUPERCONDUCTIVITY OFTHE BISRCACUO SYSTEM			DEPARTMENT OF PHYSICS & ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONT.,L8S4M1 CANADA	PHYSICA C,180(1991)407	P.K.UMMAT,R.K.NKUM,W.R.DATARS	GA,BI,SR,CA,CU,O	
3147	PHC1730322	T(D1)=204.7,TD2=49.7,PHASE TRANSITION	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		1	1991																											2	T																				4.4					4.4																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3148	PHC1730322	TD1=214.7,TD2=39.7	(La,Ba,Sr)2CuO4	La1.875Ba0.1Sr0.025Cu1O4	La	1.875	Ba	0.1	Sr	0.025	Cu	1													O	4		1	1991																											2	T																				6					6																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3149	PHC1730322	TD1=217.7,TD2=25.7	(La,Ba,Sr)2CuO4	La1.875Ba0.075Sr0.05Cu1O4	La	1.875	Ba	0.075	Sr	0.05	Cu	1													O	4		1	1991																											2	T																				8					8																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3150	PHC1730322	TD1=225.	(La,Ba,Sr)2CuO4	La1.875Ba0.05Sr0.075Cu1O4	La	1.875	Ba	0.05	Sr	0.075	Cu	1													O	4		1	1991																											2	T																				17					17																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3151	PHC1730322	TD1=214.7	(La,Ba,Sr)2CuO4	La1.875Ba0.025Sr0.1Cu1O4	La	1.875	Ba	0.025	Sr	0.1	Cu	1													O	4		1	1991																											2	T																				29.1					29.1																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3152	PHC1730322	TD1=225K	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		1	1991																											2	T																				30					30																																																																																																					STRUCTURAL, NORMAL-STATE, AND SUPERCONDUCTING PROPERTIES OF (LA1-XBAX-YSRY)2CUO4	199102			PHYSICA C,173(1991)322	A.ODAGAWA,MAENO,N.KAKEHI,T.FUJITA,T.SUZUKI,Y	LA,BA,SR,CU,O	
3153	PR04411971	RES IS UNDER 0.1 MPA,OZ BY COULOMETRIC TITRATION	(Yb,Ca)(Ba,Sr)2Cu3O7	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.78	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	Z	6.78	1	1991																											3	Y123				3.794	3.851	11.622														44.6					44.6			K/GPa	-1.25																																																																														0.516																			COMPOSITION DEPENDENCE OF THE PRESSURE EFFECT ON TC IN (YB0.7CA0.3)(BA0.8SR0.2)2CU3OZ	199112		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,SHINONOME,KOTO-KU,TOKYO 135,JAPAN	PHYS.REV.B,44(1991)11971	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,N.KOSHIZUKA,N.MORI,S.TANAKA,T.MIYATAKE,T.WADA,Y.YAEGASHI	YB,CA,BA,SR,CU,O	
3154	PR04411971		(Yb,Ca)(Ba,Sr)2Cu3O7	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.73	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	Z	6.73	1	1991																											3	Y123				3.797	3.856	11.594														67.6					67.6			K/GPa	-1.25																																																																														0.926																			COMPOSITION DEPENDENCE OF THE PRESSURE EFFECT ON TC IN (YB0.7CA0.3)(BA0.8SR0.2)2CU3OZ	199112		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,SHINONOME,KOTO-KU,TOKYO 135,JAPAN	PHYS.REV.B,44(1991)11971	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,N.KOSHIZUKA,N.MORI,S.TANAKA,T.MIYATAKE,T.WADA,Y.YAEGASHI	YB,CA,BA,SR,CU,O	
3155	PR04411971		(Yb,Ca)(Ba,Sr)2Cu3O7	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.56	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	Z	6.56	1	1991																											2	Y123				3.83		11.677														80.3					80.3			K/GPa	0.95																																																																														1.3																			COMPOSITION DEPENDENCE OF THE PRESSURE EFFECT ON TC IN (YB0.7CA0.3)(BA0.8SR0.2)2CU3OZ	199112		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,SHINONOME,KOTO-KU,TOKYO 135,JAPAN	PHYS.REV.B,44(1991)11971	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,N.KOSHIZUKA,N.MORI,S.TANAKA,T.MIYATAKE,T.WADA,Y.YAEGASHI	YB,CA,BA,SR,CU,O	
3156	PR04411971		(Yb,Ca)(Ba,Sr)2Cu3O7	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.43	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	Z	6.43	1	1991																											2	Y123				3.822		11.708														66.3					66.3			K/GPa	6.16																																																																														1.59																			COMPOSITION DEPENDENCE OF THE PRESSURE EFFECT ON TC IN (YB0.7CA0.3)(BA0.8SR0.2)2CU3OZ	199112		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,SHINONOME,KOTO-KU,TOKYO 135,JAPAN	PHYS.REV.B,44(1991)11971	A.ICHINOSE,H.YAMAUCHI,M.KOSUGE,N.KOSHIZUKA,N.MORI,S.TANAKA,T.MIYATAKE,T.WADA,Y.YAEGASHI	YB,CA,BA,SR,CU,O	
3157	PHC1850573	VOLUME INCREASES FROM 5.353*5.404*13.164 TO 5.35*5.379*13.216 BYOXIDIZATION,TC(SUS)=35K	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1991																											3	T				5.35	5.371	13.216													36	37					37																																																																																		4.5				0.0000000025				7	RH3157										SUPERCONDUCTING PROPERTIES AND HALL EFFECT IN ELECTROCHEMICALLLY OXIDISED LaCuO4 .			Laboratoire de Physique des Solides de Bellevue, CNRS, 92195 Meudon, France	Physica.C,185-189(1991)573-574	G. HEGER,L. OUHAMMOU,Mamidanna S.R. RAO,O. GOROCHOV,R. SURYANARAYANAN,W. PAULUS		
3158	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.975	Y	1	Ba	2	Cu	3															O	7-Z	6.975	1	1991																											3	Y123																																																																																																															0.000000000354				7	RH3158										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3159	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	7-Z	6.6	1	1991																											3	Y123																				56.5					56.5																																																																			33.9																			0.0000000018				7	RH3159										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3160	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.32	Y	1	Ba	2	Cu	3															O	7-Z	6.32	1	1991																											3	Y123																																																																																												68.5																			0.00000000789				7	RH3160										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3161	PR04412086	AVERAGE GRAIN SIZE 20-30MICRON-M,Z DEDUCED FROM THE WEIGHT CHANGE,RES BY AC METHOD(77HZ)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	Z	7	1	1991									5.1																		3	Y123																				90.2					90.2																																							11	2.8																											-2.33			TP3161												0.6								7	RH3161										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3162	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	Z	6.95	1	1991																											3	Y123																				90.9					90.9																																								1.8																											-0.02			TP3162												0.78				0.00000000041				7	RH3162										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3163	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	Z	6.9	1	1991																											3	Y123																				91.6					91.6																																							9.9	1.4																											1.51			TP3163												0.83								7	RH3163										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3164	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	Z	6.82	1	1991																											3	Y123																				86.7					86.7																																								1.5																											3.69			TP3164												1.16				0.00000000072				7	RH3164										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3165	PR04412086		YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	Z	6.7	1	1991																											3	Y123																				63.9					63.9																																																																			8.63			TP3165																0.00000000128				7	RH3165										EFFECT OF OXYGEN ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199112		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY,UNIVERSITY OF CAMBRIDGE,MADINGLEY ROAD,CAMBRIDGE,ENGLAND CB30HE	PHYS.REV.B,44(1991)12086	A.CARRINGRON,J.R.COOPER,J.W.LORAM,S.D.OBERTELLI	Y,BA,CU,O	
3166	PR04412516		(Bi,Pb)2(Sb)Sr2Ca2Cu3O10	Bi1.7Pb0.3Sb0.05Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.3	Sb	0.05	Sr	2	Ca	2	Cu	3									O	Z			1991																												Bi2223																				106.2					106.2																																						8.73																																																															FLUCTUATION-ENHANCED CONDUCTIVITY IN THE SB-DOPED BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199112		DEPARTMENT OF PHYSICS AND ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONTARIO L8S4M1,CANADA	PHYS.REV.B,44(1991)12516	R.K.NKUM,W.R.DATARS	SB,BI,PB,SR,CA,CU,O	
3167	PR04412516			Bi1.7Pb0.3Sb0.05Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.3	Sb	0.05	Sr	2	Ca	2	Cu	3									O	Z		1	1991																												Bi2223																				105.8					105.8																																						7.7																																																															FLUCTUATION-ENHANCED CONDUCTIVITY IN THE SB-DOPED BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199112		DEPARTMENT OF PHYSICS AND ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONTARIO L8S4M1,CANADA	PHYS.REV.B,44(1991)12516	R.K.NKUM,W.R.DATARS	SB,BI,PB,SR,CA,CU,O	
3168	PR04412516			Bi1.7Pb0.3Sb0.1Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		1	1991																												Bi2223																				106.3					106.3																																						7.26																																																															FLUCTUATION-ENHANCED CONDUCTIVITY IN THE SB-DOPED BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199112		DEPARTMENT OF PHYSICS AND ASTRONOMY,MCMASTER UNIVERSITY,HAMILTON,ONTARIO L8S4M1,CANADA	PHYS.REV.B,44(1991)12516	R.K.NKUM,W.R.DATARS	SB,BI,PB,SR,CA,CU,O	
3169	PHC1810303	FERRIMAGNETIC,NEGATIVE M BELLOW 35K,INFLECTION POINT AT 45K,METALLIC RESISTIVITY	TlSrVOZ	Tl1Sr1V1OZ	Tl	1	Sr	1	V	1															O	Z		2	1991							87																																												5																																																																																				1.75																			ELECTRICAL AND MAGNETIC PROPERTIES OF THE TL-SR-V-O SYSTEM	199110		IRC IN SUPERCONDUCTIVITY,UNIIVERSITY OF CAMBRIDGE,MADINGLY ROAD,CAMBRIDGE CB30HE,UNITED KINGDOM	PHYSICA C,181(1991)303	J.D.JOHNSON,P.P.EDWARDS,R.S.LIU	TL,SR,V,O	
3170	PRL0681058	DELTA-TC=0.65K,75% SUBSTITUTION OF C(13)	Rb3C60	C60Rb3	C	60	Rb	3																					1992																																																29.8					29.8																																											4000																																																										ISOTOPE EFFECT IN SUPERCONDUCTING RB3C60	199202			PHYS.REV.LETT.,68(1992)1058	A.M.MUJSCE,A.M.Mujsce,A.P.RAMIREZ,A.P.Ramirez,A.R.KORTAN,A.R.Kortan,A.V.MAKHIJA,A.V.Makhija,D.W.MURPHY,D.W.Murphy,K.B.LYONS,K.B.Lyons,M.J.ROSSEINSKY,M.J.Rosseinsky,R.C.HADDON,R.C.Haddon,S.J.DUCLOS,S.J.Duclos,S.M.ZAHURAK,S.M.Zahurak	RB,C	
3171	PRL0681054	D=1600A,GRAIN SIZE=70A	K3C60	C60K3	C	60	K	3																				4	1992																												fullerene																				12.8					12.8																						47									5.5							26																																																					RH3171										ELECTRONIC TRANSPORT PROPERTIES OF K3C60 FILMS	199202			PHYS.REV.LETT.,68(1992)1054	A.F.HEBARD,J.ZAANEN,R.C.HADDON,T.T.M.PALSTRA	K,C	
3172	JJP0310166	FILMS OF C60 BY VACUUM EVAP. OF C60 ONTO QUALTZ SUBSTRATE,D=1000A		C60Rb3	C	60	Rb	3																				3	1992																																															26		30				28																																																																																		80																			Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
3173	JJP0310166			C60Rb3	C	60	Rb	3																				4	1992																																															2.5		22				12.25																																																																																		140																			Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
3174	JJP0310166			C60K3	C	60	K	3																				4	1992																																															2.5		14.5				8.5																																																																																		20																			Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
3175	NAT3520223	(CSMX)3C60 (M=HG,TL,BI) HAVING ALL THE SAME TC	Cs3C60	Cs3C60	Cs	3	C	60																					1991																																																29.5					29.5																																																																																																					Superconductivity at 30K in cesium-doped C60	7		Department of Chemistry and Division of Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA	Nature 352(1991)223	Charles M. Lieber,Chia-Chun Chen,Stephen P. Kelty		
3176	NAT3520222	COMPOSITION IS NOMINAL VALUE	(Cs,Rb)3C60	Cs2Rb1C60	Cs	2	Rb	1	C	60																			1991																																																33					33										60																																																																																											SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
3177	NAT3520222	COMPOSITION IS NOMINAL VALUE	(Cs,Rb)3C60	Cs1Rb2C60	Cs	1	Rb	2	C	60																			1991																																																31					31										30																																																																																											SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
3178	NAT3520222	COMPO. IS NOMINAL	Rb3C60	Rb3C60C60	Rb	3	C	60	C	60																			1991																																																29					29										10																																																																																											SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
3179	NAT3520222	COMPO. IS NOMINAL	Rb2C60	C60Rb2	C	60	Rb	2																					1991																																																29					29										14																																																																																											SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
3180	NAT3520222	COMPOSITION IS NOMINAL VALUE	Rb4C60	C60Rb4	C	60	Rb	4																					1991																																																29					29										18																																																																																											SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
3181	PRL0670271		K3C60	C60K3	C	60	K	3																					1991									1.91																			fullerene																				19.3					19.3													132									49									3.73							26					2400																																																										CRITICAL MAGNETIC FIELDS IN THE SUPERCONDUCTING STATE OF K3C60	199107			PHYS.REV.LETT.,67(1991)271	F.DIEDERICH,G.GRUNER,J.D.THOMPSON,K.HOLCZER,O.KLEIN,R.L.WHETTEN	K,C	
3182	NAT3500600	VAN DER PAUW'S METHOD FOR AC RESISTIVITY,D=960A	K3C60	C60K3	C	60	K	3																				4	1991																																															8		18				13																																																																																																					Superconductivity at 18K in potassium-doped C60	6		AT&T Bell Laboratories, Murray Hill, New Jersey 07974-2070, USA	Nature.35(1991)600	A.F. Hebard,A.R. Kortan,D.W. Murphy,D.W. Ramirez,M.J. Rosseinsky,R.C. Haddon,S.H. Glarum,T.T.M. Palstra		
3183	NAT3500600	TC BY MEISSNER EFFECT	K3C60	C60K3	C	60	K	3																				1	1991																																																18					18																																																																																																					Superconductivity at 18K in potassium-doped C60	6		AT&T Bell Laboratories, Murray Hill, New Jersey 07974-2070, USA	Nature.35(1991)600	A.F. Hebard,A.R. Kortan,D.W. Murphy,D.W. Ramirez,M.J. Rosseinsky,R.C. Haddon,S.H. Glarum,T.T.M. Palstra		
3184	PR04412632	MAXIMUM TC=122.7K(3.7GPA)	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1991																												Tl2212																				112.1					112.1			K/GPa	4																																																																																																	PRESSURE DEPENDENCE OF TC IN TL2BA2CACU2O8 AT HYDROSTATIC PRESSURES TO 6 GPA	199112		U.S.NAVAL RESEARCH LABORATORY,WASHINGTON,D.C.20375-5000	PHYS.REV.B,44(1991)12632	A.M.HERMANN,D.H.LIEBENBERG,E.F.SKELTON,H.M.DUAN,N.E.MOULTON,S.A.WOLF,T.A.VANDERAH	TL,BA,CA,CU,O	
3185	PR04412632		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1991																												Tl2212																				107.2					107.2			K/GPa	1.6																																																																																																	PRESSURE DEPENDENCE OF TC IN TL2BA2CACU2O8 AT HYDROSTATIC PRESSURES TO 6 GPA	199112		U.S.NAVAL RESEARCH LABORATORY,WASHINGTON,D.C.20375-5000	PHYS.REV.B,44(1991)12632	A.M.HERMANN,D.H.LIEBENBERG,E.F.SKELTON,H.M.DUAN,N.E.MOULTON,S.A.WOLF,T.A.VANDERAH	TL,BA,CA,CU,O	
3186	PR04412632		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1991																												Tl2212																				106.7					106.7			K/GPa	2.4																																																																																																	PRESSURE DEPENDENCE OF TC IN TL2BA2CACU2O8 AT HYDROSTATIC PRESSURES TO 6 GPA	199112		U.S.NAVAL RESEARCH LABORATORY,WASHINGTON,D.C.20375-5000	PHYS.REV.B,44(1991)12632	A.M.HERMANN,D.H.LIEBENBERG,E.F.SKELTON,H.M.DUAN,N.E.MOULTON,S.A.WOLF,T.A.VANDERAH	TL,BA,CA,CU,O	
3187	PR04412632		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1991																												Tl2212																				114.1					114.1			K/GPa	2																																																																																																	PRESSURE DEPENDENCE OF TC IN TL2BA2CACU2O8 AT HYDROSTATIC PRESSURES TO 6 GPA	199112		U.S.NAVAL RESEARCH LABORATORY,WASHINGTON,D.C.20375-5000	PHYS.REV.B,44(1991)12632	A.M.HERMANN,D.H.LIEBENBERG,E.F.SKELTON,H.M.DUAN,N.E.MOULTON,S.A.WOLF,T.A.VANDERAH	TL,BA,CA,CU,O	
3188	PR0450355	GRAIN SIZE 2-4MICRON,89.4% O(18)	(La,Sr)2CuO4	La1.87Sr0.125Cu1.07O4	La	1.87	Sr	0.125	Cu	1.07															O	4			1992																												T																				26.4					26.4						0.65	O	89.4																																																																																													ISOTOPE EFFECT IN LA2-XSRXCUO4 SUPERCONDUCTORS	199201			PHYS.REV.B,45(1992)355	M.A.FRISCH,MARIA RONAY,T.R.MCGUIRE	LA,SR,CU,O	
3189	PR0450355	92.2,91.6% O(18)	(La,Sr)2CuO4	La1.88Sr0.125Cu0.97O4	La	1.88	Sr	0.125	Cu	0.97															O	4			1992																												T																				28.4					28.4						0.44	O	91.6																																																																																													ISOTOPE EFFECT IN LA2-XSRXCUO4 SUPERCONDUCTORS	199201			PHYS.REV.B,45(1992)355	M.A.FRISCH,MARIA RONAY,T.R.MCGUIRE	LA,SR,CU,O	
3190	PR04313118	SUS PEAK AT 70K	Ba(V,Ti)S3	Ba1V1S3	Ba	1	V	1	S	3																			1991																																																																																																																								-43			TP3190																			-0.0000000025	10											Magnetic and transport properties of BaV1-xTixS3(0%$x<0.2)	199106		Superonductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)13118	H. Yamauchi,Kiyotaka Matsuura,Shoji Tanaka,Takahiro Wada,Takashi Nakamizo		
3191	PR04313118	SEMICON-LIKE	Ba(V,Ti)S3	Ba1V0.8TI0.2S3	Ba	1	V	0.8	TI	0.2	S	3																	1991																																																																																																																											TP3191																															Magnetic and transport properties of BaV1-xTixS3(0%$x<0.2)	199106		Superonductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,43(1991)13118	H. Yamauchi,Kiyotaka Matsuura,Shoji Tanaka,Takahiro Wada,Takashi Nakamizo		
3192	PHC1790131	F DISTRIBUTE HOMOGENEOUSLY,F CONTENT = 0.85*NOMINAL	Nd2Cu(O,F)4	Nd2Cu1F0.1O3.9	Nd	2	Cu	1	F	0.1															O	3.9		1	1991																											2	T'				3.946		12.129																	10																																																																																													RH3192										TEM OBSERVATION AND HALL MEASUREMENTS ONSUPERCONDUCTIVE ND2CUO4-XFX			SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,179(1991)131	H.YAMAUCHI,JUN SUGIUAMA,MICHIKAZU KOSUGE,SHOJI TANAKA,YOSHIHUMI OJIMA	ND,CU,O,F	
3193	PHC1790131	SAME AS 3192	Nd2Cu(O,F)4	Nd2Cu1F0.16O3.84	Nd	2	Cu	1	F	0.16															O	3.84		1	1991																											2	T'																							10																																																																																													RH3193										TEM OBSERVATION AND HALL MEASUREMENTS ONSUPERCONDUCTIVE ND2CUO4-XFX			SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,179(1991)131	H.YAMAUCHI,JUN SUGIUAMA,MICHIKAZU KOSUGE,SHOJI TANAKA,YOSHIHUMI OJIMA	ND,CU,O,F	
3194	PHC1790131	SAME AS 3192	Nd2Cu(O,F)4	Nd2Cu1F0.2O3.8	Nd	2	Cu	1	F	0.2															O	3.8		1	1991																											2	T'				3.95		12.12															27				27																																																																																		25				-0.00000000083					RH3194										TEM OBSERVATION AND HALL MEASUREMENTS ONSUPERCONDUCTIVE ND2CUO4-XFX			SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,179(1991)131	H.YAMAUCHI,JUN SUGIUAMA,MICHIKAZU KOSUGE,SHOJI TANAKA,YOSHIHUMI OJIMA	ND,CU,O,F	
3195	PHC1790131	SAME AS 3192	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7		1	1991																											2	T'				3.951		12.116															27				27																																																																																											RH3195										TEM OBSERVATION AND HALL MEASUREMENTS ONSUPERCONDUCTIVE ND2CUO4-XFX			SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,179(1991)131	H.YAMAUCHI,JUN SUGIUAMA,MICHIKAZU KOSUGE,SHOJI TANAKA,YOSHIHUMI OJIMA	ND,CU,O,F	
3196	PHC1730103	SMALL GRAIN,HIGH DENSITY OF PORES	Nd2Cu(O,F)4	Nd2Cu1F0.2O3.8	Nd	2	Cu	1	F	0.2															O	3.8		1	1991																											2	T'																							10																																																																																																							SUPERCONDUCTIVITY IN ND2CUO4-XFX	199101		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CERNTER, 10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYSICA C,173(1991)103	H.YAMAUCHI,JUN SUGIYAMA,KAZUHIRO SAKUYAMA,TUTOMU TAKATA,YOSHIHUMI OJIMA	ND,CU,O,F	
3197	PHC1730103	SAME AS 3192	Nd2Cu(O,F)4	Nd2Cu1F0.4O3.6	Nd	2	Cu	1	F	0.4															O	3.6		2	1991																											2	T'				3.95		12.116													10		27				18.5																																																																																																					SUPERCONDUCTIVITY IN ND2CUO4-XFX	199101		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CERNTER, 10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYSICA C,173(1991)103	H.YAMAUCHI,JUN SUGIYAMA,KAZUHIRO SAKUYAMA,TUTOMU TAKATA,YOSHIHUMI OJIMA	ND,CU,O,F	
3198	PHC1730103	SAME AS 3192	Nd2Cu(O,F)4	Nd2Cu1F0.5O3.5	Nd	2	Cu	1	F	0.5															O	3.5		2	1991																											2	T'				3.95		12.115													8		27				17.5																																																																																																					SUPERCONDUCTIVITY IN ND2CUO4-XFX	199101		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CERNTER, 10-13 SHINONOME 1-CHOME, KOTO-KU, TOKYO 135, JAPAN	PHYSICA C,173(1991)103	H.YAMAUCHI,JUN SUGIYAMA,KAZUHIRO SAKUYAMA,TUTOMU TAKATA,YOSHIHUMI OJIMA	ND,CU,O,F	
3199	PHC1820157	SEMICON-LIKE,(PB0.5,CU0.5)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y1Cu2.5OZ	Pb	0.5	Sr	2	Y	1	Cu	2.5													O	Z			1991																												Pb2212																																																																																																																				RH3199										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3200	PHC1820157	SEMICON-LIKE,(PB0.6,CU0.4)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.6Sr2Y0.8Ca0.2Cu2.4OZ	Pb	0.6	Sr	2	Y	0.8	Ca	0.2	Cu	2.4											O	Z			1991																												Pb2212																																																																																																																				RH3200										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3201	PHC1820157	SEMICON-LIKE,(PB0.6,CU0.4)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.6Sr2Y0.8Ca0.2Cu2.4OZ	Pb	0.6	Sr	2	Y	0.8	Ca	0.2	Cu	2.4											O	Z			1991																												Pb1212																																																																																																															0.00000000899					RH3201										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3202	PHC1820157	SEMICON-LIKE,(PB0.65,CU0.35)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.65Sr2Y0.7Ca0.3Cu2.35OZ	Pb	0.65	Sr	2	Y	0.7	Ca	0.3	Cu	2.35											O	Z			1991																												Pb1212																																																																																												76.6			TP3202																0.00000000821					RH3202										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3203	PHC1820157	SEMICON-LIKE,(PB0.65,CU0.35)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.65Sr2Y0.7Ca0.3Cu2.35OZ	Pb	0.65	Sr	2	Y	0.7	Ca	0.3	Cu	2.35											O	Z			1991																												Pb1212																					20				20																																																																			63.7			TP3203																0.00000000715					RH3203										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3204	PHC1820157	SEMICON-LIKE,(PB0.675,CU0.325)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.675Sr2Y0.65Ca0.35Cu2.325OZ	Pb	0.675	Sr	2	Y	0.65	Ca	0.35	Cu	2.325											O	Z			1991																												Pb1212																																																																																												60.8			TP3204																0.00000000761					RH3204										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3205	PHC1820157	(PB0.675,CU0.325)	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.675Sr2Y0.65Ca0.35Cu2.325OZ	Pb	0.675	Sr	2	Y	0.65	Ca	0.35	Cu	2.325											O	Z			1991																												Pb1212																					40				40																																																																			51.7			TP3205																0.00000000657					RH3205										TRANSPORT PROPERTIES OF THE PB-BASED SUPERCONDUCTING SUPRATE  PB(1+X)/2CU(1-X)/2 SR(Y1-XCAX)CU2OY	199110		SUPERCONDUCTIVITY RESEARCH LABORATORY,INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER,10-13 SHINONOME 1-CHOME,KOTO-KU,TOKYO 135,JAPAN	PHYSICA C,182(1991)))157	H.YAMAUCHI,K.SAKUYAMA,M.KOSUGE,N.KOSHIZUKA,S.TANAKA,T.MAEDA	PB,CU,SR,Y,CA,O	
3206	CEM0940294	METALLIC,PAULI PARAMAGNETISM	BaNb2O5	Ba1Nb2S5	Ba	1	Nb	2	S	5																			1991																											7					3.32		24.88																	1.9																																																																					-11			TP3206												1.3																			Physical Properties of a New Barium Niobium Sulfide, BaNd2S5			Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	J.Solid State Chem.94(1991)294-297	H. YAMAUCHI,KIYOTAKA MATSUURA,SHOJI TANAKA,TAKAHIRO WADA,TAKASHI NAKAMIZO		
3207	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.5Ca2.5Cu2OZ	Bi	2	La	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															30		57				43.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3208	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2Pr0.5Ca2.5Cu2OZ	Bi	2	Pr	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															37		57				47																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3209	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2Nd0.5Ca2.5Cu2OZ	Bi	2	Nd	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															33		54				43.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3210	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2Sm0.5Ca2.5Cu2OZ	Bi	2	Sm	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															27		46				36.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3211	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2Eu0.5Ca2.5Cu2OZ	Bi	2	Eu	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															21		42				31.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3212	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2Gd0.5Ca2.5Cu2OZ	Bi	2	Gd	0.5	Ca	2.5	Cu	2													O	Z		1	1991																																															21		36				28.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3213	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.25Pr0.25Ca2.5Cu2OZ	Bi	2	La	0.25	Pr	0.25	Ca	2.5	Cu	2											O	Z		1	1991																																															45		62				53.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3214	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.25Nd0.25Ca2.5Cu2OZ	Bi	2	La	0.25	Nd	0.25	Ca	2.5	Cu	2											O	Z		1	1991																																															40		62				51																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3215	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.25Sm0.25Ca2.5Cu2OZ	Bi	2	La	0.25	Sm	0.25	Ca	2.5	Cu	2											O	Z		1	1991																																															35		60				47.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3216	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.25Eu0.25Ca2.5Cu2OZ	Bi	2	La	0.25	Eu	0.25	Ca	2.5	Cu	2											O	Z		1	1991																																															33		60				46.5																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3217	CTR0180157		Bi2(R,Ca)2CaCu2O8	Bi2La0.25Gd0.25Ca2.5Cu2OZ	Bi	2	La	0.25	Gd	0.25	Ca	2.5	Cu	2											O	Z		1	1991																																															40		58				49																																																																																																					Sr-free Bi-Ln-Ca-Cu-O Superconductors				Cer.Trans.,18(1991)157			
3218	PR0450527	SUPERCON. IS SEEN ONLY FOR X<0.2 IN BI(2+X),REDUCED SAMPLE 3220		Bi2.15Sr1.85Cu1O5.4+Z	Bi	2.15	Sr	1.85	Cu	1															O	5.4+Z			1992																												Bi2201																				6					6																																																																																						0.00000000131					RH3218										LOW-TEMPERATURE HALL EFFECT IN BI2SR2CUO6-Z	199201			PHYS.REV.B,45(1992)527	A.CARRINGTON,A.P.MACKENZIE,B.M.WANKLYN,C.CHEN,J.R.COOPER,S.D.HUGHES	BI,SR,CU,O	
3219	PR0450527			Bi2.25Sr1.75Cu1O5.4+Z	Bi	2.25	Sr	1.75	Cu	1															O	5.4+Z			1992																												Bi2201																																																																																																															0.00000000276					RH3219										LOW-TEMPERATURE HALL EFFECT IN BI2SR2CUO6-Z	199201			PHYS.REV.B,45(1992)527	A.CARRINGTON,A.P.MACKENZIE,B.M.WANKLYN,C.CHEN,J.R.COOPER,S.D.HUGHES	BI,SR,CU,O	
3220	PR0450527			Bi2.15Sr1.85Cu1O5.4+Z	Bi	2.15	Sr	1.85	Cu	1															O	5.4+Z			1992																												Bi2201																																																																																																															0.00000000257					RH3220										LOW-TEMPERATURE HALL EFFECT IN BI2SR2CUO6-Z	199201			PHYS.REV.B,45(1992)527	A.CARRINGTON,A.P.MACKENZIE,B.M.WANKLYN,C.CHEN,J.R.COOPER,S.D.HUGHES	BI,SR,CU,O	
3221	PR0450515	NON-SUPER	(Nd,Ce)2CuO4	Nd1.975Ce0.025Cu1O4-Z	Nd	1.975	Ce	0.025	Cu	1															O	4-Z		3	1992																												T'																																																																																												-108			TP3221																					RH3221										TRANSPORT AND LOCALIZATION IN ND2-XCEXCUO4-Y CRYSTALS AT LOW DOPING	199201			PHYS.REV.B,45(1992)515	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.Q.XU,Z.Y.LI	ND,CE,CU,O	
3222	PR0450511		YBa2Cu3O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	7-Z	6.92	3	1992																																															92					0.5	92																																																														8			THC3222																	0.25																			EVIDENCE FOR STRONG ELECTRON-PHONON COUPLING IN THE THERMAL CONDUCTIVITY OF YBA2CU3O7-Z	199201			PHYS.REV.B,45(1992)511	JOSHUA L.COHN,STUART A.WOLF,TERRELL A.VANDERAH	Y,BA,CU,O	
3223	PHC1900099	(INXPB0.75-XCU0.25)SR2(CA0.5Y0.5)CU2O7-Z,X=0	(Pb,Cu,In)Sr2(Ca,Y)Cu2O7	Pb0.75Sr2Ca0.5Y0.5Cu2.25O7-Z	Pb	0.75	Sr	2	Ca	0.5	Y	0.5	Cu	2.25											O	7-Z			1991																											2	Pb1212				3.8		11.8														45					45																																																																			21.7			TP3223																															BULK NEW HIGH-TC SUPERCONDUCTORS IN THE (PB,CU)SR2(CA,Y)CU2O7-Z AND (IN,PB,CU)SR2(CA,Y)CU2O7-Z SYSTEMS	199112			PHYSICA C,190(1991)99	B.RAVEAU,C.MICHEL,D.A.JEFFERSON,D.GROULT,I.GAMESON,J.PROVOST,M.HERVIEU,P.P.EDWARDS,R.S.LIU,S.D.OBERTELLI,S.F.HU,T.ROUILLON	PB,CU,SR,CA,Y,O,IN	
3224	PHC1900099	SAME AS 3223,X=0.2	(Pb,Cu,In)Sr2(Ca,Y)Cu2O7	In0.2Pb0.55Sr2Ca0.5Y0.5Cu2.25O7-Z	In	0.2	Pb	0.55	Sr	2	Ca	0.5	Y	0.5	Cu	2.25									O	7-Z			1991																											2	Pb1212				3.8		11.8														60					60																																																																			19.1			TP3224																															BULK NEW HIGH-TC SUPERCONDUCTORS IN THE (PB,CU)SR2(CA,Y)CU2O7-Z AND (IN,PB,CU)SR2(CA,Y)CU2O7-Z SYSTEMS	199112			PHYSICA C,190(1991)99	B.RAVEAU,C.MICHEL,D.A.JEFFERSON,D.GROULT,I.GAMESON,J.PROVOST,M.HERVIEU,P.P.EDWARDS,R.S.LIU,S.D.OBERTELLI,S.F.HU,T.ROUILLON	PB,CU,SR,CA,Y,O,IN	
3225	PHC1840041	1.8*1.7*1.2MM2,92.25% FREE OF TWIN,HC1(4K)=164 OE FOR H//B-AXIS,HC1(4K)=1250 OE FOR H//C-AXIS	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																												Y123																																																																																																																														A-B ANISOTROPY PROPERTIES OF MILLIMETER-SIZED MONODOMAIN YBA2CU3O7I-X SINGLE CRYSTALS	12		SIEMENS AG,CORPORATE RESEARCH AND DEVELOPMENT,D-8000 MUNICH,GERMANY	PHYSICA C,184(1991)41	B.SEEBACHER,K.ANDRES,K.SCHONMANN	Y,BA,CU,O	
3226	PHC1840041	SAME AS 3225,HC1(4K)=117 OE FOR H//B-AXIS,HC1(4K)=520 OE FOR H//C-AXIS	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																												Y123																																																																																																																														A-B ANISOTROPY PROPERTIES OF MILLIMETER-SIZED MONODOMAIN YBA2CU3O7I-X SINGLE CRYSTALS	12		SIEMENS AG,CORPORATE RESEARCH AND DEVELOPMENT,D-8000 MUNICH,GERMANY	PHYSICA C,184(1991)41	B.SEEBACHER,K.ANDRES,K.SCHONMANN	Y,BA,CU,O	
3227	PHC1840113			Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z		1	1991																											3	Y123																				91.2				0.7	91.2																																																					SP3227				37																																												SPECIFIC HEAT OF A HIGH-TEMPERATURE SUPERCONDUCTOR:DYBA2CU3O7	199112			PHYSICA C,184(1991)113	A.KOTODZIEJCZYK,A.KOZTOWSKI,J.CHMIST,R.ZALECKI,T.SCIEZOR,Z.TARNAWSKI	DY,BA,CU,O	
3228	PRL0683240	GAP=46MEV BY HREELS	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1992																												Bi2212																				88.5				5	88.5																																																6																																																					TEMPERATURE DEPENDENCE OF THE ENERGY GAP IN BI2SR2CACU2O8 SUPERCONDUCTORS BY HIGH-RESOLUTION ELECTRON-ENERGY-LOSS SPECTROSCOPY	199205			PHYS.REV.LETT.68(1992)3240	CHARLES M.LIEBER,JIN LIN HUANG,YONGHONG LI	BI,SR,CA,CU,O	
3229	PHC1900104		Sr4(V,Ti)3O10	Sr4V2.7TI0.3O9.51	Sr	4	V	2.7	TI	0.3															O	10-Z	9.51		1991																																																			4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3230	PHC1900104		Sr4(V,Ti)3O10	Sr4V2.82TI0.18O9.47	Sr	4	V	2.82	TI	0.18															O	10-Z	9.47		1991																																																			4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3231	PHC1900104		Sr4(V,Ti)3O10	Sr4V2.85TI0.15O9.6	Sr	4	V	2.85	TI	0.15															O	10-Z	9.6		1991																																																			4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3232	PHC1900104	CURIEC=EMU.K/MOLE,KAIZERO=EMU/MOLE	(La,Sr)RhO3	La1Rh1O3	La	1	Rh	1																	O	3			1991							-1.3																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3233	PHC1900104		(La,Sr)RhO3	La0.9Sr0.1Rh1O3	La	0.9	Sr	0.1	Rh	1															O	3			1991																																																			4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3234	PHC1900104		(La,Ca)RhO3	La0.8Ca0.2Rh1O3	La	0.8	Ca	0.2	Rh	1															O	3			1991																																																			4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3235	PHC1900104	SAME AS 3232	LaCoO3	La1Co1O3	La	1	Co	1																	O	3			1991		-22600000000000000000000000000000					-218																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3236	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.9Pr0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Pr	0.1	Cu	2											O	8			1992																											2	Bi2212				5.404		30.706																																																																																																																								SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3237	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8			1992																											2	Bi2212				5.451		30.628														73					73																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3238	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.7Pr0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Pr	0.3	Cu	2											O	8			1992																											2	Bi2212				5.437		30.654														61					61																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3239	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8			1992																											2	Bi2212				5.454		30.697														41					41																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3240	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.5Pr0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Pr	0.5	Cu	2											O	8			1992																											2	Bi2212				5.446		30.697																																																																												16																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3241	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2O8	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	8			1992																											2	Bi2212				5.465		30.74																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3242	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.3Pr0.7Cu2O8	Bi	2	Sr	2	Ca	0.3	Pr	0.7	Cu	2											O	8			1992																											2	Bi2212				5.463		30.774																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3243	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.2Pr0.8Cu2O8	Bi	2	Sr	2	Ca	0.2	Pr	0.8	Cu	2											O	8			1992																											2	Bi2212				5.479		30.757																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3244	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.1Pr0.9Cu2O8	Bi	2	Sr	2	Ca	0.1	Pr	0.9	Cu	2											O	8			1992																											2	Bi2212				5.478		30.731																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3245	PR0457436		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Pr1Cu2O8	Bi	2	Sr	2	Pr	1	Cu	2													O	8			1992																											2	Bi2212						30.748																	4.2																																																											26																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3246	PR0457436		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1992																											2	Bi2212																				81					81																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3247	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.9Gd0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Gd	0.1	Cu	2											O	8			1992																											2	Bi2212				5.425																80					80																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3248	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8			1992																											2	Bi2212				5.418		30.586														73					73																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3249	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.7Gd0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Gd	0.3	Cu	2											O	8			1992																											2	Bi2212				5.433		30.586														48					48																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3250	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.6Gd0.4Cu2O8	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	2											O	8			1992																											2	Bi2212				5.437		30.465														30					30																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3251	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.5Gd0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Gd	0.5	Cu	2											O	8			1992																											2	Bi2212				5.449		30.465																	4.2																																																											19																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3252	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.4Gd0.6Cu2O8	Bi	2	Sr	2	Ca	0.4	Gd	0.6	Cu	2											O	8			1992																											2	Bi2212				5.449		30.369																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3253	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.3Gd0.7Cu2O8	Bi	2	Sr	2	Ca	0.3	Gd	0.7	Cu	2											O	8			1992																											2	Bi2212				5.444		30.352																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3254	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.2Gd0.8Cu2O8	Bi	2	Sr	2	Ca	0.2	Gd	0.8	Cu	2											O	8			1992																											2	Bi2212				5.447		30.265																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3255	PR0457436		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Gd1Cu2O8	Bi	2	Sr	2	Gd	1	Cu	2													O	8			1992																											2	Bi2212						30.265																	4.2																																																											30.7																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3256	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8			1992																											2	Bi2212				5.403		30.8														77					77																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3257	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8			1992																											2	Bi2212				5.405		30.714														70					70																																																									1.7																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3258	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8			1992																											2	Bi2212				5.408		30.62														48					48																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3259	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8			1992																											2	Bi2212				5.416		30.414														37					37																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3260	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8			1992																											2	Bi2212				5.418		30.414														22					22																																																									2.3																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3261	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.4Y0.6Cu2O8	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	8			1992																											2	Bi2212				5.421		30.371														9					9																																																																																																					SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3262	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.1Y0.9Cu2O8	Bi	2	Sr	2	Ca	0.1	Y	0.9	Cu	2											O	8			1992								358																			2	Bi2212				5.436		30.31																	4.2																																																											6.5																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3263	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8			1992								296																			2	Bi2212				5.432		30.242																	4.2																																																																																																							SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3264	PR0457436		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Y1Cu2O8	Bi	2	Sr	2	Y	1	Cu	2													O	8			1992								368																			2	Bi2212																							4.2																																																											10.2																																												SUPERCONDUCTING AND MAGNETIC PHASE BOUNDARIES IN BI2SR2CA1-XMXCU2O8,WITH M=Y,GD, AND PR	199204			PHYS.REV.B,45(1992)7436	H.CHEN,J.E.CROW,J.O'REILLY,N.SPENCER,P.PERNAMBUCO-WISE,R.E.SALOMON,Y.GAO	BA,SR,CA,Y,GD,PR,CU,O	
3265	SSC0810253	GRAIN SIZE=9MICRON	YBa2(Cu,Li)3O7	Y1Ba2Cu2.95Li0.05OZ	Y	1	Ba	2	Cu	2.95	Li	0.05													O	Z			1992																												Y123																			82						82																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3266	SSC0810253	26 MICRON	YBa2(Cu,Li)3O7	Y1Ba2Cu2.9Li0.1OZ	Y	1	Ba	2	Cu	2.9	Li	0.1													O	Z			1992																												Y123																			78						78																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3267	SSC0810253	32MICRON	YBa2(Cu,Li)3O7	Y1Ba2Cu2.98Li0.2OZ	Y	1	Ba	2	Cu	2.98	Li	0.2													O	Z			1992																												Y123																			77						77																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3268	SSC0810253	7 MICRON		Y1BaNa0.05Cu3OZ	Y	1	Ba		Na	0.05	Cu	3													O	Z			1992																												Y123																			84						84																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3269	SSC0810253	17 MICRON		Y1BaNa0.1Cu3OZ	Y	1	Ba		Na	0.1	Cu	3													O	Z			1992																												Y123																			84						84																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3270	SSC0810253	23MICRON		Y1BaNa0.2Cu3OZ	Y	1	Ba		Na	0.2	Cu	3													O	Z			1992																												Y123																			84						84																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3271	SSC0810253	6 MICRON	Y(Ba,K)2Cu3O7	Y1Ba1.95K0.05Cu3OZ	Y	1	Ba	1.95	K	0.05	Cu	3													O	Z			1992																												Y123																			86						86																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3272	SSC0810253	10 MICRON	Y(Ba,K)2Cu3O7	Y1Ba1.9K0.1Cu3OZ	Y	1	Ba	1.9	K	0.1	Cu	3													O	Z			1992																												Y123																			86						86																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3273	SSC0810253	16 MICRON	Y(Ba,K)2Cu3O7	Y1Ba1.8K0.2Cu3OZ	Y	1	Ba	1.8	K	0.2	Cu	3													O	Z			1992																												Y123																			86						86																																																																																																					ORIENTED GRAIN GROWTH IN YBA2CU3O7-Z BY ALKALI METALS (LI,NA &K) SUBSTITUTION	199201			J.SOLID STATE COMMUN.,81(1992)253	A.D.DAMODARAN,A.SIMON,M.S.SARMA,P.S.MUKHERJEE	Y,BA,CU,O,LI,NA,K	
3274	SSC0810109	UNKNOWN IMPURITY	(BI,GA)2(SR,CA)2CACU2O8	Bi2Sr1.8Ca1.2Cu2O8	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	8			1992																												Bi2212																			68.4						68.4																																																																																																					EFFECT OF GA2O3 SUBSTITUTION IN BI-2212 SUPERCONDUCTOR	199201			J.SOLID STATE COMMUN.,81(1992)109	C.BANSAL,G.RAJARAM,N.KANNAN	BI,SR,CA,CU,GA,O	
3275	SSC0810109	BI SITE SUBSTITUTE BY GA	(BI,CA)2(SR,CA)2CACU208	Bi1.8Ga0.2Sr1.8Ca1.2Cu2O8	Bi	1.8	Ga	0.2	Sr	1.8	Ca	1.2	Cu	2											O	8			1992																												Bi2212																			56.5						56.5																																																																																																					EFFECT OF GA2O3 SUBSTITUTION IN BI-2212 SUPERCONDUCTOR	199201			J.SOLID STATE COMMUN.,81(1992)109	C.BANSAL,G.RAJARAM,N.KANNAN	BI,SR,CA,CU,GA,O	
3276	SSC0810109	SAME AS 3275	(BI,CA)2(SR,CA)2CACU2O8	Bi1.5Ga0.5Sr1.8Ca1.2Cu2O8	Bi	1.5	Ga	0.5	Sr	1.8	Ca	1.2	Cu	2											O	8			1992																												Bi2212																			41						41																																																																																																					EFFECT OF GA2O3 SUBSTITUTION IN BI-2212 SUPERCONDUCTOR	199201			J.SOLID STATE COMMUN.,81(1992)109	C.BANSAL,G.RAJARAM,N.KANNAN	BI,SR,CA,CU,GA,O	
3277	SSC0810109	SAME AS 3275	(BI,GA)2(SR,CA)2CACU2O8	Bi1Ga1Sr1.8Ca1.2Cu2O8	Bi	1	Ga	1	Sr	1.8	Ca	1.2	Cu	2											O	8			1992																												Bi2212																			24.8						24.8																																																																																																					EFFECT OF GA2O3 SUBSTITUTION IN BI-2212 SUPERCONDUCTOR	199201			J.SOLID STATE COMMUN.,81(1992)109	C.BANSAL,G.RAJARAM,N.KANNAN	BI,SR,CA,CU,GA,O	
3278	SSC0810081	GAP=13 MEV AT 4.2K,BSCCO/IN2O3/PB0.5IN0.5 JUNCTION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1992																											3	Bi2212				5.406	5.436	30.87														77.8					77.8																																																3.8																																																					SINGLE PARTICLE TUNNELING STUDIES ON BI2SR2CA1CU2OY	199201			J.SOLID STATE COMMUN.,81(1992)81	G.RANGARAJAN,G.V.SUBBA RAO,S.KASIVISWANATHAN,S.LAKSHMIRAGHAVAN	BI,SR,CA,CU,O	
3279	PR0457414	WHISKER	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OZ	Bi	2	Sr	2	Ca	2	Cu	3													O	Z			1992																												Bi2223																			106.5						106.5																							1210	39								16	0.51						29	0.93																																										0.38																			UPPER CRITICAL FIELD AND ANISOTROPY OF THE HIGH-TC BI2SR2CA2CU3OX PHASE	199204			PHYS.REV.B,45(1992)7414	HIDEO TANIGAWA,HIROSHI YAMASHITA,ICHIRO MATSUBARA,MAKOTO KINOSHITA,TOMOJI KAWAI,TORU OGURA	BI,SR,CA,CU,O	
3280	PR0457402	IMPURITY=CUO,NO Y123,NO Y247 PHASES DETERMINED BY XRD,PENET CALCULATED BY HC1,PENET ESTIMATED FROM HC1 AND G-L PARAMETER	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1992																												Y124																				79.2					79.2										67														87									1.57						19.5					1960																																																									MAGNETIC MEASUREMENTS OF THE UPPER CRITICAL FIELD,IRREVERSIBILITY LINE,ANISOTROPY,AND MAGNETIC PENETRATION DEPTH OF GRAIN-ALIGNED YBA2CU4O8	199204			PHYS.REV.B,45(1992)7402	D.M.GINSBERG,W.C.LEE	Y,BA,CU,O	
3281	PR0457406	SEMICONDUCTOR	Pb2Sr2RCu3O8	Pb2Sr2Pr1Cu3O8	Pb	2	Sr	2	Pr	1	Cu	3													O	8		3	1992																												Pb3212																							60																																																																																																							OPTICAL INVESTIGATION OF THE METAL-INSULATOR TRANSITION IN THECA-FREE PB2SR2LCU3O8 (L=Y,DY,EU,SM,ND,AND PR)SERIES	199204			PHYS.REV.B,45(1992)7406	J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,DY,EU,SM,ND,PR,CU,O	
3282	PR0457406	SEMICONDUCTOR	Pb2Sr2RCu3O8	Pb2Sr2Sm1Cu3O8	Pb	2	Sr	2	Sm	1	Cu	3													O	8		3	1992																												Pb3212																							60																																																																																																							OPTICAL INVESTIGATION OF THE METAL-INSULATOR TRANSITION IN THECA-FREE PB2SR2LCU3O8 (L=Y,DY,EU,SM,ND,AND PR)SERIES	199204			PHYS.REV.B,45(1992)7406	J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,DY,EU,SM,ND,PR,CU,O	
3283	PR0457406		Pb2Sr2RCu3O8	Pb2Sr2Eu1Cu3O8	Pb	2	Sr	2	Eu	1	Cu	3													O	8		3	1992																												Pb3212																			67		75				71																																																																																																					OPTICAL INVESTIGATION OF THE METAL-INSULATOR TRANSITION IN THECA-FREE PB2SR2LCU3O8 (L=Y,DY,EU,SM,ND,AND PR)SERIES	199204			PHYS.REV.B,45(1992)7406	J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,DY,EU,SM,ND,PR,CU,O	
3284	PR0457406		Pb2Sr2RCu3O8	Pb2Sr2Dy1Cu3O8	Pb	2	Sr	2	Dy	1	Cu	3													O	8		3	1992																												Pb3212																			71		82				76.5																																																																																																					OPTICAL INVESTIGATION OF THE METAL-INSULATOR TRANSITION IN THECA-FREE PB2SR2LCU3O8 (L=Y,DY,EU,SM,ND,AND PR)SERIES	199204			PHYS.REV.B,45(1992)7406	J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,DY,EU,SM,ND,PR,CU,O	
3285	PR0457406		Pb2Sr2RCu3O8	Pb2Sr2Y1Cu3O8	Pb	2	Sr	2	Y	1	Cu	3													O	8		3	1992																												Pb3212																			71		80				75.5																																																																																																					OPTICAL INVESTIGATION OF THE METAL-INSULATOR TRANSITION IN THECA-FREE PB2SR2LCU3O8 (L=Y,DY,EU,SM,ND,AND PR)SERIES	199204			PHYS.REV.B,45(1992)7406	J.E.GREEDAN,J.S.XUE,M.REEDYK,T.TIMUSK	PB,SR,Y,DY,EU,SM,ND,PR,CU,O	
3286	PR04412571	THC300=AB-PLANE,FOR C-AXIS,ANISOTROPY=9	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1991																												Tl2212																																																																																							1.5			THC3286																																				ANISOTROPIC THERMAL CONDUCTIVITY OF TL2BA2CACU2O8 AND YBA2CU3O7 SINGLE CRYSTALS: ANOMALY IN BOTH IN-PLANE DIRECTIONS	199112		INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SEIENCIES,BEIJING 100080,CHINA	PHYS.REV.B,44(1991)12571	A.M.HERMANN,CAO SHAO-CHUN,H.M.DUAN,ZHANG DIAN-LIN,ZHANG DONG-MING	TL,BA,CA,CU,O,Y	
3287	PR04412571	SAME AS 3286,ANISOTROPY=17	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1991																												Y123																																																																																							3			THC3287																																				ANISOTROPIC THERMAL CONDUCTIVITY OF TL2BA2CACU2O8 AND YBA2CU3O7 SINGLE CRYSTALS: ANOMALY IN BOTH IN-PLANE DIRECTIONS	199112		INSTITUTE OF PHYSICS,CHINESE ACADEMY OF SEIENCIES,BEIJING 100080,CHINA	PHYS.REV.B,44(1991)12571	A.M.HERMANN,CAO SHAO-CHUN,H.M.DUAN,ZHANG DIAN-LIN,ZHANG DONG-MING	TL,BA,CA,CU,O,Y	
3288	PHC1620572	2*0.5*0.2 MM3	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3OX	Tl	2	Ba	2	Ca	2	Cu	3													O	X		3	1989																												Tl2223																				120					120																																																																	THC3288																																				Thermal conductivity of the Bi2(Ca0.5Sr0.5)3Cu2Ox, Tl2Ba2Ca2Cu3Ox ceramics and ErBa2Cu3Ox single crystal				Physica.C,162-164(1989)572-a	F.G. ALIEV,V.V. MOSHCHALKOV,V.V. PRYADUN		
3289	PHC1620572	TWO TC(80K,110K)	Bi2(Ca,Sr)3Cu2O8	Bi2Sr1.5Ca1.5Cu2OX	Bi	2	Sr	1.5	Ca	1.5	Cu	2													O	X		2	1989																												Bi2212																			80		110				95																																																																	THC3289																																				Thermal conductivity of the Bi2(Ca0.5Sr0.5)3Cu2Ox, Tl2Ba2Ca2Cu3Ox ceramics and ErBa2Cu3Ox single crystal				Physica.C,162-164(1989)572-a	F.G. ALIEV,V.V. MOSHCHALKOV,V.V. PRYADUN		
3290	PRL0673856	TWINNED SAMPLE,H//C-AXIS,HEAT FLOW ALONG A-B PLANE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																											3	Y123																																																																																										THC3290																																				THERMAL CONDUCTIVITY OF YBA2CU3O7-Z IN A MAGNETIC FIELD: CAN K(H) PROBE THE VORTEX STATE?	199112			PHYS.REV.LETT.67(1991)3856	C.UHER,FRANCO NORI,R.A.RICHARDSON,S.D.PEACOR	Y,BA,CU,O	
3291	PRL0673856	UNTWINNED SAMPLE,H//C-AXIS,HEAT FLOW ALONG A-B PLANE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																											3	Y123																																																																																										THC3291																																				THERMAL CONDUCTIVITY OF YBA2CU3O7-Z IN A MAGNETIC FIELD: CAN K(H) PROBE THE VORTEX STATE?	199112			PHYS.REV.LETT.67(1991)3856	C.UHER,FRANCO NORI,R.A.RICHARDSON,S.D.PEACOR	Y,BA,CU,O	
3292	PHC1920161	TL=1.78 BY CHEMICAL ANALYSIS		Tl2Ba2Ca2Cu3O9.83	Tl	2	Ba	2	Ca	2	Cu	3													O	10	9.83	1	1992																											2	Tl2223				3.859		35.72														114					114																																																																																																					HOLE CONCENTRATION AND CRITICAL TEMPERATURE IN THE TL2-X-ZBA2CA2+XCU3O10-Y SYSTEM	199203			PHYSICA C,192(1992)161	A.M.HERMANN,M.FOLDEAKI,M.PARANTHAMAN	TL,BA,CA,CU,O	
3293	PHC1920161	TL=1.66 BY CHEMICAL ANALYSIS		Tl1.8Ba2Ca2.2Cu3O9.92	Tl	1.8	Ba	2	Ca	2.2	Cu	3													O	10	9.92	1	1992																											2	Tl2223				3.861		35.76														112					112																																																																																																					HOLE CONCENTRATION AND CRITICAL TEMPERATURE IN THE TL2-X-ZBA2CA2+XCU3O10-Y SYSTEM	199203			PHYSICA C,192(1992)161	A.M.HERMANN,M.FOLDEAKI,M.PARANTHAMAN	TL,BA,CA,CU,O	
3294	PHC1920161	TL=1.52		Tl1.7Ba2Ca2.3Cu3O9.82	Tl	1.7	Ba	2	Ca	2.3	Cu	3													O	10	9.82	1	1992																											2	Tl2223				3.858		35.71														116					116																																																																																																					HOLE CONCENTRATION AND CRITICAL TEMPERATURE IN THE TL2-X-ZBA2CA2+XCU3O10-Y SYSTEM	199203			PHYSICA C,192(1992)161	A.M.HERMANN,M.FOLDEAKI,M.PARANTHAMAN	TL,BA,CA,CU,O	
3295	PHC1920161	TL=1.33,TC INCREASE UPTO 128K BY POST ANNEALING AT 750 C FOR 10DAYS		Tl1.6Ba2Ca2.4Cu3O9.67	Tl	1.6	Ba	2	Ca	2.4	Cu	3													O	10	9.67	1	1992																											2	Tl2223				3.856		35.72														118					118																																																																																																					HOLE CONCENTRATION AND CRITICAL TEMPERATURE IN THE TL2-X-ZBA2CA2+XCU3O10-Y SYSTEM	199203			PHYSICA C,192(1992)161	A.M.HERMANN,M.FOLDEAKI,M.PARANTHAMAN	TL,BA,CA,CU,O	
3296	PHC1920161	TL=1.10 BY CHEMICAL ANALYSIS,IMPURITY = TL0.2CA0.8CUOZ		Tl1.4Ba2Ca2.6Cu3O9.53	Tl	1.4	Ba	2	Ca	2.6	Cu	3													O	10	9.53	1	1992																											2	Tl2223				3.857		35.7														118					118																																																																																																					HOLE CONCENTRATION AND CRITICAL TEMPERATURE IN THE TL2-X-ZBA2CA2+XCU3O10-Y SYSTEM	199203			PHYSICA C,192(1992)161	A.M.HERMANN,M.FOLDEAKI,M.PARANTHAMAN	TL,BA,CA,CU,O	
3297	PHC1920137	FIGURE=TC VS OZ,247 DECOMPOSES INTO 123 + CUO AT HIGH T AND LOW O2 PRESSURE	YBa2Cu3O7	Y2Ba4Cu7OZ	Y	2	Ba	4	Cu	7															O	Z		1	1992																											3	Y247																																																																																																																														VARIATION OF THE SUPERCONDUCTING AND STRUCTURAL PROPERTIES OFY2BA4CU7OZ WITH OXYGEN CONTENT (14.1<Z<15.3,30K<-TC<-95K)	199203			PHYSICA C,192(1992)137	A.JUNOD,G.TRISCONE,J.-Y.GENOUD,J.MULLER,T.GRAF	Y,BA,CU,O	
3298	PHC1920103		YBa2Cu4(Li)O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1992																											3	Y124				3.837	3.867	27.23														80					80										27																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3299	PHC1920103	LI SUBSTITUTES FOR CU,SOLUBILITY LIMIT IS ABOUT X = 0.13	YBa2Cu4(Li)O8	Y1Ba2Cu4Li0.016O8	Y	1	Ba	2	Cu	4	Li	0.016													O	8			1992																											3	Y124				3.838	3.869	27.21														77					77										25																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3300	PHC1920103		YBa2Cu4(Li)O8	Y1Ba2Cu4Li0.031O8	Y	1	Ba	2	Cu	4	Li	0.031													O	8			1992																											3	Y124				3.838	3.868	27.2														72					72										20																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3301	PHC1920103		YBa2Cu4(Li)O8	Y1Ba2Cu4Li0.062O8	Y	1	Ba	2	Cu	4	Li	0.062													O	8			1992																											3	Y124				3.83	3.869	27.2														64					64										32																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3302	PHC1920103		YBa2Cu4(Li)O8	Y1Ba2Cu4Li0.125O8	Y	1	Ba	2	Cu	4	Li	0.125													O	8			1992																											3	Y124				3.827	3.869	27.2														58					58										28																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3303	PHC1920103		YBa2Cu4(Li)O8	Y1Ba2Cu4Li0.25O8	Y	1	Ba	2	Cu	4	Li	0.25													O	8			1992																											3	Y124				3.818	3.868	27.18														58					58										20																																																																																											LITHIUM SUBSTITUTED SUPERCONDUCTING Y1BA2CU4O8 FORMED IN ELEVATED OXYGEN PRESSURE	199203			PHYSICA C,192(1992)103	A.P.B.SINHA,D.E.MORRIS,J.S.SURNOW,M.R.CHANDRACHOOD	Y,BA,CU,O,LI	
3304	PHC1690386	TC SHARPLY DECREASES WITH DOPED FE,124 SINGLE PHASE OBSERVED ONLY UPTO X-0.025,BEYOND THIS MIXTURE WITH Y123	YBa2(Cu,Fe)4O8	Y1Ba2CuFeO8	Y	1	Ba	2	Cu		Fe														O	8			1990																											3	Y124				3.835	3.87	27.17																																																																																																																								DESTABILISATION OF 124 AND 247 PHASES OF Y-BA-CU-O BY FE SUBSTITUTION AT ELEVATED OXYGEN PRESSURES			2-300 LAWRENCE BERKELY LABORATORY, BERKELEY CA 94720, USA	PHYSICA C,169(1990)386	A.P.B.SINHA,A.P.MARATHE,D.E.MORRIS	Y,BA,CU,O,FE	
3305	PHC1920013	INFINITE LAYER,NEARLY(95%) SINGLE PHASE, UPTO 200KBAR	(Sr,Nd)2CuO2	Sr0.84Nd0.16Cu1O2	Sr	0.84	Nd	0.16	Cu	1															O	2		1	1992																											2	IL				3.944		3.383														24				6	24			K/GPa	0.6						25																																																																																											THE PRESSURE DEPENDENCE OF TC IN THE INFINITE-LAYER ELECTRON-DOPED COMPOUND SR0.84ND0.16CUO2	199203			PHYSICA C,192(1992)13	A MANTHIRAM,BEOM-HOAN O,C.L.WOOTEN,J.B.GOODENOUGH,J.T.MARKERT,J.ZHOU,M.G.SMITH	SR,ND,CU,O	
3306	JPS0593839	TC DEPENDS ON Z,SEE 'PR04011400'	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				87					87			K/GPa	-0.88																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3307	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				82					82			K/GPa	-1.3																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3308	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				61					61			K/GPa	-3.2																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3309	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				51					51			K/GPa	-5.9																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3310	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				49					49			K/GPa	-6																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3311	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				20					20			K/GPa	-3.3																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3312	JPS0593839		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				16					16			K/GPa	-2.8																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3313	JPS0593839	TC=MAXIMUM AT 2GPA		Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z			1990																												Tl2201																				117					117			K/GPa	1.7																																																																																																	APPEARANCE OF A MAXIMUM OF TC AND A LARGE NEGATIVE DTC/DP IN THE SUPERCONDUCTING TL-BA-CA-CU-O COMPOUNDS UNDER PRESSURE	199011			J.PHYS.SOC.JAPAN,59(1990)3839	HIROKI TAKAHASHI,NOBUO MORI,TAKASHI MANAKO,YOSHIMI KUBO,YUICHI SHIMAKAWA	TL,BA,CA,CU,O	
3314	PHC1900104		Sr4V3O10	Sr4V3O9.8	Sr	4	V	3																	O	10-Z	9.8		1991	emu/mol	0.00035	emu/mol.K	0.02			-72																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3315	PHC1900104		Sr4V3O10	Sr4V3O9.73	Sr	4	V	3																	O	10-Z	9.73		1991	emu/mol	0.000402	emu/mol.K	0.016			-22																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3316	PHC1900104		Sr4V3O10	Sr4V3O9.51	Sr	4	V	3																	O	10-Z	9.51		1991	emu/mol	0.000532	emu/mol.K	0.013			5.78																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3317	PHC1900104		Sr4V3O10	Sr4V3O9.49	Sr	4	V	3																	O	10-Z	9.49		1991	emu/mol	0.00044	emu/mol.K	0.018			13.2																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3318	PHC1900104		Sr4V3O10	Sr4V3O9.44	Sr	4	V	3																	O	10-Z	9.44		1991	emu/mol	0.000434	emu/mol.K	0.019			14																																												4.2																																																																																																							CANDIDATE COMPOUNDS FOR SUPERCONDUCTIVITY	199112			PHYCA C,190(1991)104	MASAHIRO SHIKANO,MITSURU ITOH,TETSUO SHIMURA,TETSURO NAKAMURA		
3319	PR0445322	97%(O(18)),DTC=0.28K	Y(Ba,La)2Cu3O7	Y1Ba2Cu3O6.99	Y	1	Ba	2	Cu	3															O	Z	6.99		1991									4.5																			Y123																				92.3					92.3						0.025	O	97	0.28																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3320	PR0445322	97%(O(18)),DTC=0.41K	Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O7.06	Y	1	Ba	1.9	La	0.1	Cu	3													O	Z	7.06		1991																												Y123																				91.9					91.9						0.039	O	97	0.41																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3321	PR0445322	97%(O(18)),DTC=1.29K	Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O7.05	Y	1	Ba	1.8	La	0.2	Cu	3													O	Z	7.05		1991																												Y123																				77.3					77.3						0.14	O	97	1.29																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3322	PR0445322	97%(O(18)),DTC=1.86K	Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3OZ	Y	1	Ba	1.7	La	0.3	Cu	3													O	Z			1991																												Y123																				73					73						0.213	O	97	1.86																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3323	PR0445322	95%(O(18)),DTC=1.92K	Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3O7.11	Y	1	Ba	1.6	La	0.4	Cu	3													O	Z	7.11		1991																												Y123																				49.3					49.3						0.324	O	95	1.92																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3324	PR0445322	94%(O(18)),DTC=1.75K	Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3O7.19	Y	1	Ba	1.5	La	0.5	Cu	3													O	Z	7.19		1991																												Y123																				38.3					38.3						0.38	O	94	1.75																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3325	PR0445322	97%(O(18)),DTC=1.93K		Y1Ba1.7La0.3Cu3O7.1	Y	1	Ba	1.7	La	0.3	Cu	3													O	Z	7.1		1991																												Y123																				60					60						0.269	O	97	1.93																																																																																												ISOTOPE EFFECT YBA2-XLAXCU3OZ:EVIDENCE FOR PHONON-MEDIATED HIGH-TEMPERATURE SUPERCONDUCTIVITY	199109		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5322	D.E.MORRIS,H.J.BORNEMANN	Y,BA,LA,CU,O	
3326	PR0445369	ALMOST SINGLE PASE,(PB0.5CU0.5)SR2(CA0.5ND0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Nd0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Nd	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.83		11.892														60					60																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3327	PR0445369	(PB0.5CU0.5)SR2(CA0.5SM0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Sm0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Sm	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.827		11.888														62					62																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3328	PR0445369	(PB0.5CU0.5)SR2(CA0.5EU0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Eu0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Eu	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.821		11.871														60					60																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3329	PR0445369	(PB0.5CU0.5)SR2(CA0.5GD0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Gd0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Gd	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.821		11.854														60					60																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3330	PR0445369	(PB0.5CU0.5)SR2(CA0.5DY0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Dy0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Dy	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.812		11.853														65.9					65.9																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3331	PR0445369	(PB0.5CU0.5)SR2(CA0.5HO0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Ho0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Ho	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.809		11.842														67.9					67.9																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3332	PR0445369	(PB0.5CU0.5)SR2(CA0.5ER0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Er0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Er	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.807		11.845														70					70																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3333	PR0445369	(PB0.5CU0.5)SR2(CA0.5TM0.5)CU2O7	(Pb,Cu)Sr2(Ca,R)Cu2O7	Pb0.5Sr2Ca0.5Tm0.5Cu2.5O7	Pb	0.5	Sr	2	Ca	0.5	Tm	0.5	Cu	2.5											O	7		1	1991																												Pb1212				3.804		11.838														72					72																																																																																																					EIGHT RARE-EARTH-SUBSTITUTED PB-BASED 1:2:1:2 SUPERCONDUCTINGCOMPOUNDS:(PB,CU)SR2(CA,R)CU2O7 (R=ND,SM,EU,GD,DY,HO,ER,TM)	199109		MORRIS RESEARCH INCORPORATED,1918 UNIVERSITY AVENUE,BERKELEY,CALIFORNIA 94704	PHYS.REV.B,44(1991)5369	D.E.MORRIS,H.B.LIU	PB,CU,SR,CA,R,O	
3334	PHC1830277	D(LNTC)/DP=4.6%,RH300=250K	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1991																												Y124																				72.9					72.9			K/GPa	3.55																																																																																		0.00000000013					RH3334										CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3335	PHC1830277	D(LNTC)/DP=0.72%,RH300=250K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1991																												Y123																				91.4					91.4			K/GPa	0.66																																																																																		0.00000000069					RH3335										CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3336	PHC1830277	D(LNTC)/DP=-0.91%,RH300=250K	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		1	1991																												Bi2212																				84.9					84.9			K/GPa	-0.77																																																																																		0.00000000141					RH3336										CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3337	PHC1830277	D(LNTC)/DP=-9.3%,RH300=250K	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1991																												Tl2201																				47					47			K/GPa	-4.2																																																																																		0.00000000143					RH3337										CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3338	PHC1830277	D(LNTC)/DP=13.8%/GPA,RH300=250K	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		1	1991																												T																				22.4					22.4			K/GPa	3.3																																																																																		0.0000000072															CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3339	PHC1830277	D(LNTC)/DP=9.1%/GPA,RH300=250K	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		1	1991																												T																				31					31			K/GPa	2.95																																																																																		0.00000000286															CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3340	PHC1830277	D(LNTC)/DP=5.5%/GPA,RH300=250K	(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4		1	1991																												T																				38					38			K/GPa	2.15																																																																																		0.00000000083															CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3341	PHC1830277	D(LNTC)/DP=5.6%/GPA,RH300=250K	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1991																												T																				32.6					32.6			K/GPa	1.88																																																																																		0.00000000054															CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3342	PHC1830277	D(LNTC)/DP=10.2%/GPA,RH300=250K	(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		1	1991																												T																				19.3					19.3			K/GPa	2.07																																																																																		0.00000000018															CORRELATION BETWEEN THE PRESSURE-INDUCED CHANGES IN THE HALL COEFFICIENT AND TC IN SUPERCONDUCTING CUPRATES	199111		INSTITUTE FOR SOLID STATE PHYSICS,UNIVERSITY OF TOKYO,ROPPONGI,TOKYO 106,JAPAN	PHYSICA C,183(1991)277	C.MURAYAMA,N.MORI,T.ENOMOTO,T.MANAKO,T.MATSUMOTO,Y.IYE,Y.KUBO,Y.SHIMAKAWA,Y.YAMADA	Y,BA,CU,O,BI,SR,CA,TL	
3343	PR0460448		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.9Ni0.1O7-Z	Gd	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z		1	1992																											3	Y123																				77.7					77.7																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3344	PR0460448		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.8Ni0.2O7-Z	Gd	1	Ba	2	Cu	2.8	Ni	0.2													O	7-Z		1	1992																											3	Y123																				55.1					55.1																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3345	PR0460448		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.7Ni0.3O7-Z	Gd	1	Ba	2	Cu	2.7	Ni	0.3													O	7-Z		1	1992																											3	Y123																				32.3					32.3																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3346	PR0460448		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.9Fe0.1O7-Z	Gd	1	Ba	2	Cu	2.9	Fe	0.1													O	7-Z		1	1992						8.04	2																					Y123																				75					75																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3347	PR0460448		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.8Fe0.2O7-Z	Gd	1	Ba	2	Cu	2.8	Fe	0.2													O	7-Z		1	1992						8.2	4																					Y123																				49					49																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3348	PR0460448		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O7-Z	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	7-Z		1	1992						8.35	3																					Y123																				29					29																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3349	PR0460448		GdBa2(Cu,Co)3O7	Gd1Ba2Cu2.9Co0.1O7-Z	Gd	1	Ba	2	Cu	2.9	Co	0.1													O	7-Z			1992																												Y123																				76					76																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3350	PR0460448		GdBa2(Cu,Co)3O7	Gd1Ba2Cu2.8Co0.2O7-Z	Gd	1	Ba	2	Cu	2.8	Co	0.2													O	7-Z			1992																												Y123																				49					49																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3351	PR0460448		GdBa2(Cu,Co)3O7	Gd1Ba2Cu2.7Co0.3O7-Z	Gd	1	Ba	2	Cu	2.7	Co	0.3													O	7-Z			1992																												Y123																				13					13																																																																																																					TRANSITION-METAL REDISTRIBUTION IN GDBA2CU3-XMXO7-Z AND YBA2CU3-XMXO7-Z (M=FE,CO,AND NI):EVIDENCE FOR GD-FE(2) MAGNETIC INTERACTIONS	199207			PHYS.REV.B,46(1992)448	G.KALONJI,R.C.O'HANDLEY,R.CHATTERJEE,T.R.S.PRASANNA	GD,BA,CU,O,FE,CO,NI	
3352	PR0460443	F SUBSTITUTE FOR O(2) SITE IN FLUORITE-TYPE NDO LAYERS	Nd2Cu(O,F)4	Nd2Cu1F0.15O3.85	Nd	2	Cu	1	F	0.15															O	3.85			1992																												T'																							4.2																																																																																																							LOCAL STRUCTURE AROUND F IN THE FLUORINE-DOPED ND2CUO4 SUPERCONDUCTOR	199207			PHYS.REV.B,46(1992)443	A.KROL,S.HUANG,Y.H.KAO,Y.L.SOO,Z.H.MING	ND,CU,O,F	
3353	PR0460443	SAME AS 3352	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.70			1992																												T'																			10		27				18.5																																																																																																					LOCAL STRUCTURE AROUND F IN THE FLUORINE-DOPED ND2CUO4 SUPERCONDUCTOR	199207			PHYS.REV.B,46(1992)443	A.KROL,S.HUANG,Y.H.KAO,Y.L.SOO,Z.H.MING	ND,CU,O,F	
3354	PR0460398	M-H CURVE ANALYSED BY HAO AND CLEM'S EQUATION,HC(O)=1.18E+4 OE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1992																											3	Y123																				92.5					92.5																															1.9							18					1310																																																										CRITICAL FIELDS AND VORTEX STRUCTURE OF YBA2CU3O7-Z DERIVED FROM REVERSIBLE MAGNETIZATION	199207			PHYS.REV.B,46(1992)398	D.K.FINNEMORE,JUNHO GOHNG	Y,BA,CU,O	
3355	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.975Ca0.025Ba2Cu2.975Al0.025O6.89	Y	0.975	Ca	0.025	Ba	2	Cu	2.975	Al	0.025											O	6.89	6.89		1991																												Y123																				94.5					94.5																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3356	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.95Ca0.05Ba2Cu2.95Al0.05O6.88	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Al	0.05											O	6.88	6.88		1991																												Y123																				92					92																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3357	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.9Ca0.1Ba2Cu2.9Al0.1O6.88	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Al	0.1											O	6.88	6.88		1991																												Y123																				91.1					91.1																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3358	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.85Ca0.15Ba2Cu2.85Al0.15O6.87	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Al	0.15											O	6.87	6.87		1991																												Y123																				90.5					90.5																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3359	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.8Ca0.2Ba2Cu2.8Al0.2O6.88	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Al	0.2											O	6.88	6.88		1991																												Y123																				89.1					89.1																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3360	PHC1900160		(Y,Ca)Ba2(Cu,Al)3O7	Y0.75Ca0.25Ba2Cu2.75Al0.25O6.86	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Al	0.25											O	6.86	6.86		1991																												Y123																				88.2					88.2																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3361	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu2.15O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	2.15													O	8+Z			1991																												Bi2212						3.078														82					82																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3362	PHC1900160	NA SUBSTITUTION REDUCES OXYGEN CONTENT	Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu2.05Na0.1O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	2.05	Na	0.1											O	8+Z			1991																												Bi2212						3.078														86					86																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3363	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.95Na0.2O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.95	Na	0.2											O	8+Z			1991																												Bi2212						3.083														87					87																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3364	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.85Na0.3O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.85	Na	0.3											O	8+Z			1991																												Bi2212																				88					88																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3365	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.75Na0.4O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.75	Na	0.4											O	8+Z			1991																												Bi2212						3.088														89					89																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3366	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.65Na0.5O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.65	Na	0.5											O	8+Z			1991																												Bi2212						3.089														90					90																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3367	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.55Na0.6O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.55	Na	0.6											O	8+Z			1991																												Bi2212						3.088														91					91																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3368	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.45Na0.7O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.45	Na	0.7											O	8+Z			1991																												Bi2212						3.086														90					90																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3369	PHC1900160		Bi2Sr2Ca(Cu,Na)2O8	Bi2.2Sr1.8Ca1.05Cu1.25Na0.9O8+Z	Bi	2.2	Sr	1.8	Ca	1.05	Cu	1.25	Na	0.9											O	8+Z			1991																												Bi2212																				86					86																																																																																																					EFFECT OF CHEMICAL SUBSTITUTION ON SUPERCONDUCTIVITY IN YBA2CU3O7-Z,BI2SR2YCU2O8+Z,AND BI2SR2CACU2O8+Z	199112			PHYSICA C,190(1991)160	C.C.SORRELL,H.K.LIU,S.X.DOU,W.M.WU,Y.C.GUO,Y.ZHAO	Y,BA,CU,O,BI,SR,CA,NA,AL	
3370	PHC1900255		(Y,Ca,Pr)Ba2Cu3O7	Y1Ba2Cu3O6.99	Y	1	Ba	2	Cu	3															O	6.99	6.99	1	1992																											3	Y123				3.818	3.885	11.682														91.4					91.4																															2.78																																																																						STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Y1-2XCAXPRXBA2CU3O7-Z	199201			PHYSICA C,190(1992)255	M.ANDERSSON,M.NYGREN,O.RAPP,T.L.WEN,Z.HEGEDUS	Y,CA,PR,BA,CU,O	
3371	PHC1900255	ANAL. CA0.1PR0.1	(Y,Ca,Pr)Ba2Cu3O7	Y0.8Ca0.1Pr0.1Ba2Cu3O7.01	Y	0.8	Ca	0.1	Pr	0.1	Ba	2	Cu	3											O	7.01	7.01	1	1992																											3	Y123				3.823	3.887	11.679														78.4					78.4																															2.93																																																																						STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Y1-2XCAXPRXBA2CU3O7-Z	199201			PHYSICA C,190(1992)255	M.ANDERSSON,M.NYGREN,O.RAPP,T.L.WEN,Z.HEGEDUS	Y,CA,PR,BA,CU,O	
3372	PHC1900255	ANAL. CA0.2PR0.2,IMPURITY 1.1%BACUO2	(Y,Ca,Pr)Ba2Cu3O7	Y0.6Ca0.2Pr0.2Ba2Cu3O7	Y	0.6	Ca	0.2	Pr	0.2	Ba	2	Cu	3											O	7.00	7	1	1992																											3	Y123				3.829	3.888	11.679														67.1					67.1																															3.06																																																																						STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Y1-2XCAXPRXBA2CU3O7-Z	199201			PHYSICA C,190(1992)255	M.ANDERSSON,M.NYGREN,O.RAPP,T.L.WEN,Z.HEGEDUS	Y,CA,PR,BA,CU,O	
3373	PHC1900255	ANAL. CA0.25PR0.32,IMPURITY 4.3%BACUO2	(Y,Ca,Pr)Ba2Cu3O7	Y0.4Ca0.3Pr0.3Ba2Cu3O7.02	Y	0.4	Ca	0.3	Pr	0.3	Ba	2	Cu	3											O	7.02	7.02	1	1992																											3	Y123				3.832	3.89	11.681														53.6					53.6																															2.6																																																																						STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Y1-2XCAXPRXBA2CU3O7-Z	199201			PHYSICA C,190(1992)255	M.ANDERSSON,M.NYGREN,O.RAPP,T.L.WEN,Z.HEGEDUS	Y,CA,PR,BA,CU,O	
3374	PHC1900255	ANAL. CA0.25PR0.5,IMPURITY 4.8%BACUO2	(Y,Ca,Pr)Ba2Cu3O7	Y0.2Ca0.4Pr0.4Ba2Cu3O7	Y	0.2	Ca	0.4	Pr	0.4	Ba	2	Cu	3											O	7.00	7	1	1992																											3	Y123				3.834	3.896	11.68														36.5					36.5																															1.83																																																																						STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Y1-2XCAXPRXBA2CU3O7-Z	199201			PHYSICA C,190(1992)255	M.ANDERSSON,M.NYGREN,O.RAPP,T.L.WEN,Z.HEGEDUS	Y,CA,PR,BA,CU,O	
3375	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	8.28	8.28	1	1992																												Bi2212																			61	76					76																																																																			-8.12			TP3375																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3376	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8.34	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8.34	8.34	1	1992																												Bi2212																			71	86					86																																																																			-1.54			TP3376																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3377	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8.36	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8.36	8.36	1	1992																												Bi2212																			50	76					76																																																																			19.3			TP3377																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3378	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8.39	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8.39	8.39	1	1992																												Bi2212																			20	66					66																																																																			37.4			TP3378																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3379	PR04510604	ANTIFERRO,INSULATOR	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8.45	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8.45	8.45	1	1992																												Bi2212																							4.2																																																																					232			TP3379																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3380	PR04510604	ANTIFERRO,INSULATOR	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Y1Cu2O8.53	Bi	2	Sr	2	Y	1	Cu	2													O	8.53	8.53	1	1992																												Bi2212																							4.2																																																																					473			TP3380																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3381	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca1Cu2O8.15	Bi	2	Sr	2	Ca	1	Cu	2													O	8.15	8.15	1	1992																												Bi2212																			40	87					87																																																																			-3.75			TP3381																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3382	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8.36	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8.36	8.36	1	1992																												Bi2212																				18					18																																																																			137			TP3382																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3383	PR04510604		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8.38	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8.38	8.38	1	1992																												Bi2212																							4.2																																																																					276			TP3383																															THERMOELECTRIC POWER OF BI2SR2CA1-XYXCU2O8+Y	199205			PHYS.REV.B,45(1992)10604	F.MUNAKATA,H.YAMAUCHI,K.KUBO,K.MATSUURA,T.KAWANO	BI,SR,CA,Y,CU,O	
3384	PHC1950373	NO UPWARD CURVATURE IN HC2(T)	(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	1992																											1	BKBO																				29.1					29.1													419									9.6									0.48							58					1200																																																										CRITICAL FIELDS AND FLUX PINNING IN SINGLE CRYSTAL BA1-XKXBIO3	199206			PHYSICA C,195(1992)373	B.W.VEAL,D.A.PAYNE,G.T.SEIDLER,P.D.HAN,T.F.ROSENBAUM	BA,K,BI,O	
3385	PHC1950373		(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	1992																											1	BKBO																				30					30																						11									0.55							54																																																															CRITICAL FIELDS AND FLUX PINNING IN SINGLE CRYSTAL BA1-XKXBIO3	199206			PHYSICA C,195(1992)373	B.W.VEAL,D.A.PAYNE,G.T.SEIDLER,P.D.HAN,T.F.ROSENBAUM	BA,K,BI,O	
3386	JJP0310471	DEBYE TEMP. OBTAINED FROM MOSSBAUER SHIFT		Bi4Sr3.5Ca2.5Cu4Sn0.015O16-Y	Bi	4	Sr	3.5	Ca	2.5	Cu	4	Sn	0.015											O	16-Y		1	1992																												Bi2212																				77					77																																																											340																																										Low-Temperature 119Sn-Mossbauer Study of Superconducting Bi4Sr3.5Ca2.5Cu4Sn0.015O16-y Ceramic (2212 Phase)	199204		Department of Chemistry, Faculty of Science, Kyushu University, Hakozaki, Higashiku, Fukuoka 812	Jpn.J.Appl.Phys.Lett.31(1992)L471-473	Motomi KATADA,Noboru YAMAZOE,Norio MIURA,Ttsuaki NISHIDA,Yasukuni MATSUMOTO,Yoshimasa TAKASHIMA,Yuichi DESHIMARU		
3387	JJP0310471			Bi4Sr3.5Ca2.5Cu4O16-Y	Bi	4	Sr	3.5	Ca	2.5	Cu	4													O	16-Y		1	1992																												Bi2212																				80					80																																																																																																					Low-Temperature 119Sn-Mossbauer Study of Superconducting Bi4Sr3.5Ca2.5Cu4Sn0.015O16-y Ceramic (2212 Phase)	199204		Department of Chemistry, Faculty of Science, Kyushu University, Hakozaki, Higashiku, Fukuoka 812	Jpn.J.Appl.Phys.Lett.31(1992)L471-473	Motomi KATADA,Noboru YAMAZOE,Norio MIURA,Ttsuaki NISHIDA,Yasukuni MATSUMOTO,Yoshimasa TAKASHIMA,Yuichi DESHIMARU		
3388	PR04510609	1*0.8*0.05 MM3	(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1992																												Y123																				92					92																							639	112								9.9	1.7						17	3																																																													UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3389	PR04510609	1*0.8*0.05 MM3	(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-Z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		3	1992																												Y123																				86					86																							252	79								4.2	1.3						20	6.4																																																													UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3390	PR04510609	1*0.8*0.05 MM3	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		3	1992																												Y123																				73					73																							174	56								3.4	1.1						24	7.8																																																													UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3391	PR04510609	1*0.8*0.02MM3	(Y,Pr)Ba2Cu3O7	Y0.72Pr0.28Ba2Cu3O7-Z	Y	0.72	Pr	0.28	Ba	2	Cu	3													O	7-Z		3	1992																												Y123																				60					60																								33									0.79						32																																																														UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3392	PR04510609	1*0.8*0.02MM3	(Y,Pr)Ba2Cu3O7	Y0.56Pr0.44Ba2Cu3O7-Z	Y	0.56	Pr	0.44	Ba	2	Cu	3													O	7-Z		3	1992																												Y123																				36					36																							83.2	13.4								3.3	0.53						50	8																																																													UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3393	PR04510609	1*0.8*0.02 MM3	(Y,Pr)Ba2Cu3O7	Y0.44Pr0.56Ba2Cu3O7-Z	Y	0.44	Pr	0.56	Ba	2	Cu	3													O	7-Z		3	1992																												Y123																				11					11																							10	2								1.3	0.25						130	25																																																													UPPER CRITICAL FIELD HC2 OF SINGLE-CRYSTAL Y1-XPRXBA2CU3O7-Z	199205			PHYS.REV.B,45(1992)10609	H.B.RADOUSKY,J.Z.LIU,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.X.JIA	Y,PR,BA,CU,O	
3394	SCI2541487		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1991																												Bi2212																				93					93																																																																																																					TUNNING HIGH-TC SUPERCONDUCTORS VIA MULTISTAGE INTERCALATION	199112			SCIENCE,254(1991)1487	A.ZETTI,J.L.CORKILL,MARVIN L.COHEN,N.KIJIMA,R.GRONSKY,T.W.BARBEE III,W.A.VAREKA,X-D XIANG	I,BI,SR,CA,CU,O	
3395	SCI2541487	INTERCALATE I BY USING A GAS DIFFUSION	IBa2Sr2CaCu2OZ	I1Bi2Sr2Ca1Cu2OZ	I	1	Bi	2	Sr	2	Ca	1	Cu	2											O	Z			1991																																																81.5					81.5																																																																																																					TUNNING HIGH-TC SUPERCONDUCTORS VIA MULTISTAGE INTERCALATION	199112			SCIENCE,254(1991)1487	A.ZETTI,J.L.CORKILL,MARVIN L.COHEN,N.KIJIMA,R.GRONSKY,T.W.BARBEE III,W.A.VAREKA,X-D XIANG	I,BI,SR,CA,CU,O	
3396	SCI2541487	SAME AS 3395	IBi4Sr4Ca2Cu4OZ	I1Bi4Sr4Ca2Cu4OZ	I	1	Bi	4	Sr	4	Ca	2	Cu	4											O	Z			1991																																																86					86																																																																																																					TUNNING HIGH-TC SUPERCONDUCTORS VIA MULTISTAGE INTERCALATION	199112			SCIENCE,254(1991)1487	A.ZETTI,J.L.CORKILL,MARVIN L.COHEN,N.KIJIMA,R.GRONSKY,T.W.BARBEE III,W.A.VAREKA,X-D XIANG	I,BI,SR,CA,CU,O	
3397	ST0382918	TWIN PHASE WITH <110>	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																				92				0.3	92																																																																																											RH3397										STRONGLY ANISOTROPIC ELECTRICAL PROPERTIES OF SINGLE-CRYSTAL Y(1)BA(2)CU(3)O(7-Z)	198808	RESISTIVITY              ,HALL EFFECT              ,ANISOTRO	IBM RESEARCH DIVISION,THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YOWK,USA	PHYS.REV.B,38(1988)2918	A.W.KLEINSASSER,D.KAISER,F.HOLTZBERG,S.VON MOLNAR,T.PENNEY	Y,BA,CU,O	
3398	PHC1940076		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1992																											3	Y123				3.827	3.888	11.645														92.8					92.8																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3399	PHC1940076	CRITICAL CONC.=0.57 FOR Y1-XPRXBA2CU3O7 SYSTEM	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3OZ	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				71.3					71.3																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3400	PHC1940076		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3OZ	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				58.4					58.4																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3401	PHC1940076		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3OZ	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				43.3					43.3																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3402	PHC1940076		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3OZ	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				21.9					21.9																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3403	PHC1940076		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3OZ	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	Z		1	1992																											3	Y123				3.844	3.9	11.702																	3.75																																																																																																							ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3404	PHC1940076		(Y,Pr)Ba2Cu3O7	Pr1Ba2Cu3OZ	Pr	1	Ba	2	Cu	3															O	Z		1	1992																											3	Y123				3.861	3.907	11.722																	3.75																																																																																																							ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3405	PHC1940076		(Er,Pr)Ba2Cu3O7	Er1Ba2Cu3OZ	Er	1	Ba	2	Cu	3															O	Z		1	1992																											3	Y123				3.825	3.884	11.653														92.4					92.4																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3406	PHC1940076	CRITICAL CONC.=0.60 FOR ER1-XPRXBA2CU3O7	(Er,Pr)Ba2Cu3O7	Er0.9Pr0.1Ba2Cu3OZ	Er	0.9	Pr	0.1	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				84.1					84.1																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3407	PHC1940076		(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3OZ	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				73.7					73.7																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3408	PHC1940076		(Er,Pr)Ba2Cu3O7	Er0.7Pr0.3Ba2Cu3OZ	Er	0.7	Pr	0.3	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				66.7					66.7																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3409	PHC1940076		(Er,Pr)Ba2Cu3O7	Er0.6Pr0.4Ba2Cu3OZ	Er	0.6	Pr	0.4	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				55					55																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3410	PHC1940076		(Er,Pr)Ba2Cu3O7	Er0.5Pr0.5Ba2Cu3OZ	Er	0.5	Pr	0.5	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				24.8					24.8																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3411	PHC1940076		(Er,Pr)Ba2Cu3O7	Er0.4Pr0.6Ba2Cu3OZ	Er	0.4	Pr	0.6	Ba	2	Cu	3													O	Z		1	1992																											3	Y123				3.845	3.895	11.665																	3.75																																																																																																							ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3412	PHC1940076		(Gd,Pr)Ba2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z		1	1992																											3	Y123				3.841	3.901	11.702														92.8					92.8																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3413	PHC1940076	CRITICAL CONC.=0.45 FOR GD1-XPRXBA2CU3O7	(Gd,Pr)Ba2Cu3O7	Gd0.95Pr0.05Ba2Cu3OZ	Gd	0.95	Pr	0.05	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				79					79																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3414	PHC1940076		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3OZ	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				69					69																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3415	PHC1940076		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3OZ	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				43.4					43.4																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3416	PHC1940076		(Gd,Pr)Ba2Cu3O7	Gd0.6Pr0.4Ba2Cu3OZ	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	Z		1	1992																											3	Y123				3.85	3.9	11.694														18					18																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3417	PHC1940076		(Gd,Pr)Ba2Cu3O7	Gd0.5Pr0.5Ba2Cu3OZ	Gd	0.5	Pr	0.5	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																							3.75																																																																																																							ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3418	PHC1940076		(Sm,Pr)Ba2Cu3O7	Sm1Ba2Cu3OZ	Sm	1	Ba	2	Cu	3															O	Z		1	1992																											3	Y123				3.849	3.911	11.729														92					92																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3419	PHC1940076	CRITICAL CONC.=0.40 FOR SM1-XPRXBA2CU3O7	(Sm,Pr)Ba2Cu3O7	Sm0.95Pr0.05Ba2Cu3OZ	Sm	0.95	Pr	0.05	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				65.8					65.8																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3420	PHC1940076		(Sm,Pr)Ba2Cu3O7	Sm0.9Pr0.1Ba2Cu3OZ	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				58.3					58.3																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3421	PHC1940076		(Sm,Pr)Ba2Cu3O7	Sm0.8Pr0.2Ba2Cu3OZ	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				39					39																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3422	PHC1940076		(Sm,Pr)Ba2Cu3O7	Sm0.7Pr0.3Ba2Cu3OZ	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	Z		1	1992																											3	Y123																				31.1					31.1																																																																																																					ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3423	PHC1940076		(Sm,Pr)Ba2Cu3O7	Sm0.6Pr0.4Ba2Cu3OZ	Sm	0.6	Pr	0.4	Ba	2	Cu	3													O	Z		1	1992																											3	Y123				3.851	3.904	11.722																	3.75																																																																																																							ON THE SUPERCONDUCTIVITY SUPPRESSION IN LN1-XPRXBA2CU3O7	199205			PHYSICA C,194(1992)76	EMILIO ORGAZ,ENRIQUE RUIZ-TREJO		
3424	PHC1940066	NEEL-T FOR CU	(Gd,Nd,Ce)2CuO4	Gd1.85Ce0.15Cu1O4	Gd	1.85	Ce	0.15	Cu	1															O	4			1992								155																				T'																							4.2																																																																																																							SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3425	PHC1940066	NEEL-T FOR CU	(Gd,Nd,Ce)2CuO4	Gd1.65Nd0.2Ce0.15Cu1O4	Gd	1.65	Nd	0.2	Ce	0.15	Cu	1													O	4			1992								140																				T'																							4.2																																																																																																							SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3426	PHC1940066	NEEL-T FOR CU	(Gd,Nd,Ce)2CuO4	Gd1.5Nd0.35Ce0.15Cu1O4	Gd	1.5	Nd	0.35	Ce	0.15	Cu	1													O	4			1992								96																				T'																							4.2																																																																																																							SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3427	PHC1940066	NEEL-T FOR CU	(Gd,Nd,Ce)2CuO4	Gd1.3Nd0.55Ce0.15Cu1O4	Gd	1.3	Nd	0.55	Ce	0.15	Cu	1													O	4			1992																												T'																							4.2																																																																																																							SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3428	PHC1940066		(Gd,Nd,Ce)2CuO4	Gd1.1Nd0.75Ce0.15Cu1O4	Gd	1.1	Nd	0.75	Ce	0.15	Cu	1													O	4			1992																												T'																																																																																																																														SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3429	PHC1940066		(Gd,Nd,Ce)2CuO4	Gd1Nd0.85Ce0.15Cu1O4	Gd	1	Nd	0.85	Ce	0.15	Cu	1													O	4			1992																												T'																				5.9					5.9																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3430	PHC1940066		(Gd,Nd,Ce)2CuO4	Gd0.75Nd1.1Ce0.15Cu1O4	Gd	0.75	Nd	1.1	Ce	0.15	Cu	1													O	4			1992																												T'																				10.1					10.1																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3431	PHC1940066		(Gd,Nd,Ce)2CuO4	Gd0.5Nd1.35Ce0.15Cu1O4	Gd	0.5	Nd	1.35	Ce	0.15	Cu	1													O	4			1992																												T'																				14.3					14.3																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3432	PHC1940066		(Gd,Nd,Ce)2CuO4	Gd0.2Nd1.65Ce0.15Cu1O4	Gd	0.2	Nd	1.65	Ce	0.15	Cu	1													O	4			1992																												T'																				18.5					18.5																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3433	PHC1940066		(GD,ND,CE)2CUO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4			1992																												T'				3.953		12.109														20					20																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3434	PHC1940066		(Nd,Y,Ce)2CuO4	Nd1.75Y0.1Ce0.15Cu1O4	Nd	1.75	Y	0.1	Ce	0.15	Cu	1													O	4			1992																												T'																				21					21																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3435	PHC1940066		(Nd,Y,Ce)2CuO4	Nd1.65Y0.2Ce0.15Cu1O4	Nd	1.65	Y	0.2	Ce	0.15	Cu	1													O	4			1992																												T'				3.942		12.042														17.3					17.3																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3436	PHC1940066		(Nd,Y,Ce)2CuO4	Nd1.5Y0.35Ce0.15Cu1O4	Nd	1.5	Y	0.35	Ce	0.15	Cu	1													O	4			1992																												T'				3.936		12.001																																																																																																																								SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3438	PHC1940066		(Nd,La,Ce)2CuO4	Nd1.75La0.1Ce0.15Cu1O4	Nd	1.75	La	0.1	Ce	0.15	Cu	1													O	4			1992																												T'				3.958		12.139														20					20																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3439	PHC1940066		(Nd,La,Ce)2CuO4	Nd1.65La0.2Ce0.15Cu1O4	Nd	1.65	La	0.2	Ce	0.15	Cu	1													O	4			1992																												T'																				21.2					21.2																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3440	PHC1940066		(Nd,La,Ce)2CuO4	Nd1.55La0.3Ce0.15Cu1O4	Nd	1.55	La	0.3	Ce	0.15	Cu	1													O	4			1992																												T'				3.968		12.149														21.5					21.5																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3441	PHC1940066		(Nd,La,Ce)2CuO4	Nd1.35La0.5Ce0.15Cu1O4	Nd	1.35	La	0.5	Ce	0.15	Cu	1													O	4			1992																												T'				3.968		12.195														19.1					19.1																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3442	PHC1940066		(Nd,La,Ce)2CuO4	Nd1.15La0.7Ce0.15Cu1O4	Nd	1.15	La	0.7	Ce	0.15	Cu	1													O	4			1992																												T'				3.968		12.23														19					19																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3443	PHC1940066		(Nd,La,Ce)2CuO4	Nd0.95La0.9Ce0.15Cu1O4	Nd	0.95	La	0.9	Ce	0.15	Cu	1													O	4			1992																												T'				3.981		12.294														18.4					18.4																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3444	PHC1940066		(Nd,La,Ce)2CuO4	Nd0.65La1.2Ce0.15Cu1O4	Nd	0.65	La	1.2	Ce	0.15	Cu	1													O	4			1992																												T'				3.985		12.284														5.8					5.8																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,ND,CE)2CUO4	199205			PHYSICA C,194(1992)66	CHIN LIN,GUO LU,YU-FEN ZHANG,ZUN-XIAO LIU		
3445	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.925Ni0.075OZ	Pr	1	Ba	2	Cu	2.925	Ni	0.075													O	Z			1992								15.4																			3	Y123				3.868	3.894																		4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3446	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.85Ni0.15OZ	Pr	1	Ba	2	Cu	2.85	Ni	0.15													O	Z			1992								14.5																			2	Y123				3.889																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3447	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.775Ni0.225OZ	Pr	1	Ba	2	Cu	2.775	Ni	0.225													O	Z			1992								13																			2	Y123				3.892																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3448	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.7Ni0.3OZ	Pr	1	Ba	2	Cu	2.7	Ni	0.3													O	Z			1992								12																			2	Y123				3.893																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3449	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.55Ni0.45OZ	Pr	1	Ba	2	Cu	2.55	Ni	0.45													O	Z			1992								11.6																			2	Y123				3.893																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3450	PR0461176		PrBa2(Cu,Ni)3O7	Pr1Ba2Cu2.4Ni0.6OZ	Pr	1	Ba	2	Cu	2.4	Ni	0.6													O	Z			1992								11.7																			2	Y123				3.892																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3451	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.925Co0.075OZ	Pr	1	Ba	2	Cu	2.925	Co	0.075													O	Z			1992								16.9																			2	Y123				3.897																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3452	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.85Co0.15OZ	Pr	1	Ba	2	Cu	2.85	Co	0.15													O	Z			1992								13.9																			2	Y123				3.902																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3453	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.775Co0.225OZ	Pr	1	Ba	2	Cu	2.775	Co	0.225													O	Z			1992								12.1																			2	Y123				3.906																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3454	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.7Co0.3OZ	Pr	1	Ba	2	Cu	2.7	Co	0.3													O	Z			1992								10.2																			2	Y123				3.909																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3455	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.55Co0.45OZ	Pr	1	Ba	2	Cu	2.55	Co	0.45													O	Z			1992								7.6																			2	Y123				3.919																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3456	PR0461176		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.4Co0.6OZ	Pr	1	Ba	2	Cu	2.4	Co	0.6													O	Z			1992								7.2																			2	Y123				3.921																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3457	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu3OZ	Pr	1	Ba	2	Cu	3															O	Z			1992								17.5																			3	Y123				3.865	3.9																		4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3458	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.925Fe0.075OZ	Pr	1	Ba	2	Cu	2.925	Fe	0.075													O	Z			1992								15.4																			2	Y123				3.897																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3459	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.85Fe0.15OZ	Pr	1	Ba	2	Cu	2.85	Fe	0.15													O	Z			1992								14.5																			2	Y123				3.899																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3460	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.775Fe0.225OZ	Pr	1	Ba	2	Cu	2.775	Fe	0.225													O	Z			1992								12.5																			2	Y123				3.9																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3461	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.7Fe0.3OZ	Pr	1	Ba	2	Cu	2.7	Fe	0.3													O	Z			1992								11																			2	Y123				3.899																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3462	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.55Fe0.45OZ	Pr	1	Ba	2	Cu	2.55	Fe	0.45													O	Z			1992								9.5																			2	Y123				3.892																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3463	PR0461176		PrBa2(Cu,Fe)3O7	Pr1Ba2Cu2.4Fe0.6OZ	Pr	1	Ba	2	Cu	2.4	Fe	0.6													O	Z			1992								8.1																			2	Y123				3.89																			4.2																																																																																																							MAGNETIC ORDERING AND CHAIN TRANSPORT OF PRBA2CU3O7-Y	199207			PHYS REV B,46(1992)1176	C.K.CHIOU,H.D.YANG,M.W.LIN,W.H.LEE	PR,BA,CU,O,FE,CO,NI,ZN,GA,GD	
3464	PR0461166		CaGdCuO3Cl	Ca1Gd1Cu1Cl1O3	Ca	1	Gd	1	Cu	1	Cl	1													O	3			1992						8.3	-13																					T*																																																																																																																														MAGNETIC ORDERING OF GD3+ AND SM3+ IN THE T' AND T* COPPER OXIDES AND OXYCHLORIDES	199207			PHYS.REV.B,46(1992)1166	K.V.RAMANUJACHARY,MARTHA GREENBLATT,ROBERT L.FULLER	LA,GD,CU,O,SR,CA,SM,CL	
3465	PR0461166		(La,Gd)2CuO4	La1.15Gd0.85Cu1O4	La	1.15	Gd	0.85	Cu	1															O	4			1992						7.9	-8																					T*																																																																																																																														MAGNETIC ORDERING OF GD3+ AND SM3+ IN THE T' AND T* COPPER OXIDES AND OXYCHLORIDES	199207			PHYS.REV.B,46(1992)1166	K.V.RAMANUJACHARY,MARTHA GREENBLATT,ROBERT L.FULLER	LA,GD,CU,O,SR,CA,SM,CL	
3466	PR0461166		(Sr,La,Gd)2CuO4	Sr0.2La0.9Gd0.9Cu1O4	Sr	0.2	La	0.9	Gd	0.9	Cu	1													O	4			1992						8.1	-10																					T*																																																																																																																														MAGNETIC ORDERING OF GD3+ AND SM3+ IN THE T' AND T* COPPER OXIDES AND OXYCHLORIDES	199207			PHYS.REV.B,46(1992)1166	K.V.RAMANUJACHARY,MARTHA GREENBLATT,ROBERT L.FULLER	LA,GD,CU,O,SR,CA,SM,CL	
3467	PR0460585	EPITAXIAL SINGLE PHASE FILM,123 PHASE STABLE ONLY IN FILM STATE		Tb0.7Pr0.3Ba2Cu3OZ	Tb	0.7	Pr	0.3	Ba	2	Cu	3													O	Z		4	1992																												Y123																				50					50																																																																																																					SUPERCONDUCTING FILMS OF TB1-XPRXBA2CU3O7-Z	199207			PHYS.REV.B,46(1992)585	B.FISHER,G.KOREN,G.M.REISNER,J.GENOSSAR,L.PATLAGAN,S.ISRAELIT	TB,PR,BA,CU,O	
3468	PR0460585	SAME AS 3467		Tb0.6Pr0.4Ba2Cu3OZ	Tb	0.6	Pr	0.4	Ba	2	Cu	3													O	Z		4	1992																												Y123																				43					43																																																																																																					SUPERCONDUCTING FILMS OF TB1-XPRXBA2CU3O7-Z	199207			PHYS.REV.B,46(1992)585	B.FISHER,G.KOREN,G.M.REISNER,J.GENOSSAR,L.PATLAGAN,S.ISRAELIT	TB,PR,BA,CU,O	
3469	PR0460585	SAME AS 3467		Tb0.5Pr0.5Ba2Cu3OZ	Tb	0.5	Pr	0.5	Ba	2	Cu	3													O	Z		4	1992																												Y123																				30					30																																																																																																					SUPERCONDUCTING FILMS OF TB1-XPRXBA2CU3O7-Z	199207			PHYS.REV.B,46(1992)585	B.FISHER,G.KOREN,G.M.REISNER,J.GENOSSAR,L.PATLAGAN,S.ISRAELIT	TB,PR,BA,CU,O	
3470	PR0460585	SAME AS 3467		Tb0.4Pr0.6Ba2Cu3OZ	Tb	0.4	Pr	0.6	Ba	2	Cu	3													O	Z		4	1992																												Y123																							4.2																																																																																																							SUPERCONDUCTING FILMS OF TB1-XPRXBA2CU3O7-Z	199207			PHYS.REV.B,46(1992)585	B.FISHER,G.KOREN,G.M.REISNER,J.GENOSSAR,L.PATLAGAN,S.ISRAELIT	TB,PR,BA,CU,O	
3471	SUP0040029		Bi2Sr2(Ca,K)Cu2O8	Bi2Sr2Ca0.95K0.05Cu2OZ	Bi	2	Sr	2	Ca	0.95	K	0.05	Cu	2											O	Z			1991																												Bi2212																				78					78																																																																																																					Effect of Oxygen Concentration on Superconductivity of Bi-Sr-Ca-K-Cu-O Compounds	1991		Department of Physics, University of Science and Technology of China, Hefei, Anhui, China.	J.Superconductivity,4(1991)29	Chao LieZhao,Chen Qun,Cheng Zhaojia,Han Zhiyi,Mao Zhiqiang,Wang Yu,Zhang Ning,Zhang Yuheng,Zhou Guien,Zhou Zhe		
3472	SUP0040029		Bi2Sr2(Ca,K)Cu2O8	Bi2Sr2Ca0.9K0.1Cu2OZ	Bi	2	Sr	2	Ca	0.9	K	0.1	Cu	2											O	Z			1991																												Bi2212																				76					76																																																																																																					Effect of Oxygen Concentration on Superconductivity of Bi-Sr-Ca-K-Cu-O Compounds	1991		Department of Physics, University of Science and Technology of China, Hefei, Anhui, China.	J.Superconductivity,4(1991)29	Chao LieZhao,Chen Qun,Cheng Zhaojia,Han Zhiyi,Mao Zhiqiang,Wang Yu,Zhang Ning,Zhang Yuheng,Zhou Guien,Zhou Zhe		
3473	SUP0040029		Bi2Sr2(Ca,K)Cu2O8	Bi2Sr2Ca0.8K0.2Cu2OZ	Bi	2	Sr	2	Ca	0.8	K	0.2	Cu	2											O	Z			1991																												Bi2212																				76					76																																																																																																					Effect of Oxygen Concentration on Superconductivity of Bi-Sr-Ca-K-Cu-O Compounds	1991		Department of Physics, University of Science and Technology of China, Hefei, Anhui, China.	J.Superconductivity,4(1991)29	Chao LieZhao,Chen Qun,Cheng Zhaojia,Han Zhiyi,Mao Zhiqiang,Wang Yu,Zhang Ning,Zhang Yuheng,Zhou Guien,Zhou Zhe		
3474	SUP0040029		Bi2Sr2(Ca,K)Cu2O8	Bi2Sr2Ca0.7K0.3Cu2OZ	Bi	2	Sr	2	Ca	0.7	K	0.3	Cu	2											O	Z			1991																												Bi2212																				71					71																																																																																																					Effect of Oxygen Concentration on Superconductivity of Bi-Sr-Ca-K-Cu-O Compounds	1991		Department of Physics, University of Science and Technology of China, Hefei, Anhui, China.	J.Superconductivity,4(1991)29	Chao LieZhao,Chen Qun,Cheng Zhaojia,Han Zhiyi,Mao Zhiqiang,Wang Yu,Zhang Ning,Zhang Yuheng,Zhou Guien,Zhou Zhe		
3475	SUP0040029		Bi2Sr2(Ca,K)Cu2O8	Bi2Sr2Ca0.6K0.4Cu2OZ	Bi	2	Sr	2	Ca	0.6	K	0.4	Cu	2											O	Z			1991																												Bi2212																				75					75																																																																																																					Effect of Oxygen Concentration on Superconductivity of Bi-Sr-Ca-K-Cu-O Compounds	1991		Department of Physics, University of Science and Technology of China, Hefei, Anhui, China.	J.Superconductivity,4(1991)29	Chao LieZhao,Chen Qun,Cheng Zhaojia,Han Zhiyi,Mao Zhiqiang,Wang Yu,Zhang Ning,Zhang Yuheng,Zhou Guien,Zhou Zhe		
3476	PLA1640355	C<13> 60% substitution.  ISOTOPE=2.0-2.25	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																				28.6					28.6						2	C	60																																																																																													Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
3477	PLA1640355	C<13> 60% substitution. ISOTOPE EFFECT=1.2-1.43	K3C60	C60K3	C	60	K	3																					1992																												fullerene																				20					20						1.2	C	60																																																																																													Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
3478	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.6K0.4Bi0.9Pb0.1O3	Ba	0.6	K	0.4	Bi	0.9	Pb	0.1													O	3			1992																												BKBO																				21.5					21.5																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3479	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.6K0.4Bi0.8Pb0.2O3	Ba	0.6	K	0.4	Bi	0.8	Pb	0.2													O	3			1992																												BKBO																				14.7					14.7																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3480	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.7K0.3Bi0.7Pb0.3O3	Ba	0.7	K	0.3	Bi	0.7	Pb	0.3													O	3			1992																												BKBO																				14.6					14.6																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3481	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.6K0.4Bi0.7Pb0.3O3	Ba	0.6	K	0.4	Bi	0.7	Pb	0.3													O	3			1992																												BKBO																				11.3					11.3																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3482	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.9K0.1Bi0.4Pb0.6O3	Ba	0.9	K	0.1	Bi	0.4	Pb	0.6													O	3			1992																												BKBO																				11.3					11.3																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3483	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.6K0.4Bi0.6Pb0.4O3	Ba	0.6	K	0.4	Bi	0.6	Pb	0.4													O	3			1992																												BKBO																				9.2					9.2																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3484	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.9K0.1Bi0.3Pb0.7O3	Ba	0.9	K	0.1	Bi	0.3	Pb	0.7													O	3			1992																												BKBO																				9.3					9.3																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3485	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.6K0.4Bi0.5Pb0.5O3	Ba	0.6	K	0.4	Bi	0.5	Pb	0.5													O	3			1992																												BKBO																				7.2					7.2																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3486	PR0461144		(Ba,K)(Bi,Pb)O3	Ba0.8K0.2Bi0.3Pb0.7O3	Ba	0.8	K	0.2	Bi	0.3	Pb	0.7													O	3			1992																												BKBO																				7.2					7.2																																																																																																					METASTABLE BEHAVIOR OF THE SUPERCUNDUCTING PHASE IN THE BABI1-XPBXO3 SYSTEM	199207			PHYS.REV.B,46(1992)1144	B.DABROWSKI,D.G.HINKS,D.T.MARX,J.D.JORGENSEN,P.G.RADAELLI,R.L.HITTERMAN,SHIYOU PEI	BA,BI,PB,O	
3487	JAP0685289		(M,Tl)BaCuO4.5	Tl0.76Ba1Cu1O4.5	Tl	0.76	Ba	1	Cu	1															O	4.5			1990																																3.853		23.14													82		90				86																																																																																																					STUDY ON ZN-, CD-, OR HG-ADDITION INTO TLBACUO			DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS, FAYETTEVILLE, ARKANSAS 72701	J.APPL.PHYS.,68(1990)5289	Y.XIN,Z.Z.SHENG	TL,BA,CU,O,ZN,CD,HG,	
3488	JAP0685289		(M,Tl)BaCuO4.5	Zn1Tl0.78Ba1Cu1O4.5	Zn	1	Tl	0.78	Ba	1	Cu	1													O	4.5			1990																																3.865		23.218													77		85				81																																																																																																					STUDY ON ZN-, CD-, OR HG-ADDITION INTO TLBACUO			DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS, FAYETTEVILLE, ARKANSAS 72701	J.APPL.PHYS.,68(1990)5289	Y.XIN,Z.Z.SHENG	TL,BA,CU,O,ZN,CD,HG,	
3489	JAP0685289		(M,Tl)BaCuO4.5	Cd1Tl0.7Ba1Cu1O4.5	Cd	1	Tl	0.7	Ba	1	Cu	1													O	4.5			1990																																3.853		23.241													45		60				52.5																																																																																																					STUDY ON ZN-, CD-, OR HG-ADDITION INTO TLBACUO			DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS, FAYETTEVILLE, ARKANSAS 72701	J.APPL.PHYS.,68(1990)5289	Y.XIN,Z.Z.SHENG	TL,BA,CU,O,ZN,CD,HG,	
3490	JAP0685289		(M,Tl)BaCuO4.5	Hg0.76Tl0.76Ba1Cu1O4.5	Hg	0.76	Tl	0.76	Ba	1	Cu	1													O	4.5			1990																																3.875		23.217													85		90				87.5																																																																																																					STUDY ON ZN-, CD-, OR HG-ADDITION INTO TLBACUO			DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS, FAYETTEVILLE, ARKANSAS 72701	J.APPL.PHYS.,68(1990)5289	Y.XIN,Z.Z.SHENG	TL,BA,CU,O,ZN,CD,HG,	
3491	PR0446999		(Eu,Pr)Ba2Cu3O7	Eu1Ba2Cu3O6.97	Eu	1	Ba	2	Cu	3															O	Z	6.97	1	1991																											3	Y123				3.843	3.902	11.714													94.75	94.77	94.9				94.77																																																																																		0.857																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3492	PR0446999		(Eu,Pr)Ba2Cu3O7	Eu0.95Pr0.05Ba2Cu3OZ	Eu	0.95	Pr	0.05	Ba	2	Cu	3													O	Z		1	1991																											3	Y123																			91.05	91.35	91.8				91.35																																																																																		0.792																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3493	PR0446999	KONDO-T=2.1K,NEELT,GAMMA,KONDO-T FROM SPECIFIC HEAT	(Eu,Pr)Ba2Cu3O7	Eu0.9Pr0.1Ba2Cu3O6.95	Eu	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	6.95	1	1991								1.15																			3	Y123				3.842	3.895	11.696													78.2	79.45	81.5				79.45																																																									40																									0.973																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3494	PR0446999	KONDO-T=4.5K,FROM SPECIFIC HEAT	(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O6.97	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	Z	6.97	1	1991								2.63																			3	Y123				3.847	3.904	11.714													57.2	57.9	59.4				57.9																																																									90																									1.56																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3495	PR0446999		(Eu,Pr)Ba2Cu3O7	Eu0.7Pr0.3Ba2Cu3O6.95	Eu	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123				3.846	3.899	11.701													37.2	38.8	42.2				38.8																																																																																		2.24																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3496	PR0446999	KONDO-T=7.0K,FROM SPECIFIC HEAT	(Eu,Pr)Ba2Cu3O7	Eu0.6Pr0.4Ba2Cu3O6.97	Eu	0.6	Pr	0.4	Ba	2	Cu	3													O	Z	6.97	1	1991								9.1																			3	Y123				3.856	3.894	11.722													10.1	15	20.1				15																																																									112.5																									2.28																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3497	PR0446999	NEELT FROM SPECIFIC HEAT	(Eu,Pr)Ba2Cu3O7	Eu0.4Pr0.6Ba2Cu3O6.95	Eu	0.4	Pr	0.6	Ba	2	Cu	3													O	Z	6.95	1	1991								10.1																			3	Y123				3.86	3.898	11.711																																																																																																					7.9																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3498	PR0446999	NEELT FROM SPHEAT	(Eu,Pr)Ba2Cu3O7	Eu0.2Pr0.8Ba2Cu3O7.01	Eu	0.2	Pr	0.8	Ba	2	Cu	3													O	Z	7.01	1	1991								12.9																			3	Y123				3.868	3.893	11.734																																																																																																					11.93																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3499	PR0446999	NEELT FROM SPHEAT	(Eu,Pr)Ba2Cu3O7	Pr1Ba2Cu3O6.95	Pr	1	Ba	2	Cu	3															O	Z	6.95	1	1991								15.9																			3	Y123				3.878	3.928	11.719																																																																																																					15.1																			SUPERCONDUCTIVITY AND MAGNETISM IN EU1-XPRXBA2CU3O7-Z	199110		DEPARTMENT OF PHYSICS AND INSTITUTEFOR PURE AND APPLIED PHYSICAL SCIENCES,UNIVERSITY OF CALIFORNIA,SANDIEGO,LA JOLLA,CALIFORNIA 92093	PHYS.REV.B,44(1991)6999	B.W.LEE,G.NIEVA,IVAN K.SCHULLER,M.B.MAPLE,S.GHAMATY	EU,PR,BA,CU,O	
3500	PR0457424	KAIZERO,CURIEC IN EMU/CM3.OE	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y1Cu2.5O6.98	Pb	0.5	Sr	2	Y	1	Cu	2.5													O	Z	6.98		1992		-419700000000				0.41	10.7																				2	Pb1212				3.817		11.802																																																																																																					15				0.0000000161					RH3500										SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3501	PR0457424		(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y0.95Ca0.05Cu2.5OZ	Pb	0.5	Sr	2	Y	0.95	Ca	0.05	Cu	2.5											O	Z			1992																											2	Pb1212				3.815		11.804																																																																																																					9.7																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3502	PR0457424	IMPURITY=SRCUO2	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y0.9Ca0.1Cu2.5OZ	Pb	0.5	Sr	2	Y	0.9	Ca	0.1	Cu	2.5											O	Z			1992																											2	Pb1212				3.815		11.818																																																																																																					7.1																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3503	PR0457424	IMPURITY=SRCUO2	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y0.85Ca0.15Cu2.5OZ	Pb	0.5	Sr	2	Y	0.85	Ca	0.15	Cu	2.5											O	Z			1992																											2	Pb1212				3.814		11.821																																																																																																					7.1																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3504	PR0457424	IMPURITY=SRCUO2	(Pb,Cu)Sr2(Y,Ca)Cu2OZ	Pb0.5Sr2Y0.8Ca0.2Cu2.5OZ	Pb	0.5	Sr	2	Y	0.8	Ca	0.2	Cu	2.5											O	Z			1992																											2	Pb1212				3.814		11.823																																																																																																					7.1																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3505	PR0457424	KAIZERO,CURIEC IN EMU/CM3.OE	(Pb,Cu)(Sr,Ba)2(Y,Ca)Cu2OZ	Pb0.5Sr1.8Ba0.2Y1Cu2.5O6.98	Pb	0.5	Sr	1.8	Ba	0.2	Y	1	Cu	2.5											O	Z	6.98		1992						0.24	-5.5																				2	Pb1212				3.823		11.839																																																																																																					12.5				0.00000000926					RH3505										SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3506	PR0457424		(Pb,Ca)(Sr,Ba)2(Y,Ca)Cu2OZ	Pb0.5Sr1.8Ba0.2Y0.95Ca0.05Cu2.5OZ	Pb	0.5	Sr	1.8	Ba	0.2	Y	0.95	Ca	0.05	Cu	2.5									O	Z			1992																											2	Pb1212				3.823		11.85																																																																																																					8.3																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3507	PR0457424		(Pb,Cu)(Sr,Ba)2(Y,Ca)Cu2OZ	Pb0.5Sr1.8Ba0.2Y0.9Ca0.1Cu2.5OZ	Pb	0.5	Sr	1.8	Ba	0.2	Y	0.9	Ca	0.1	Cu	2.5									O	Z			1992																											2	Pb1212				3.822		11.853																																																																																																					5.2																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3508	PR0457424	KAIZERO,CURIEC IN EMU/CM3.OE	(Pb,Cu)(Sr,Ba)2(Y,Ca)Cu2OZ	Pb0.5Sr1.8Ba0.2Y0.85Ca0.15Cu2.5O6.98	Pb	0.5	Sr	1.8	Ba	0.2	Y	0.85	Ca	0.15	Cu	2.5									O	Z	6.98		1992		-26750				0.22	-3																				2	Pb1212				3.821		11.861															25				25										11																																																																								4.1				0.00000000365					RH3508										SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3509	PR0457424	IMPURITY=SRCUO2 BY XRD	(Pb,Cu)(Sr,Ba)2(Y,Ca)Cu2OZ	Pb0.5Sr1.8Ba0.2Y0.8Ca0.2Cu2.5OZ	Pb	0.5	Sr	1.8	Ba	0.2	Y	0.8	Ca	0.2	Cu	2.5									O	Z			1992																											2	Pb1212				3.821		11.869																																																																																																					4.1																			SUPERCONDUCTING LEAD CUPRATES (PB0.5CU0.5)(SR1-YBAY)2(Y1-XCAX)CU2OW	199204			PHYS.REV.B,45(1992)7424	H.YAMAUCHI,KAZUHIRO SAKUYAMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,SR,BA,Y,CA,O	
3510	PR0458189	NO Y123,NO Y124 PHASES	YBa2Cu4O15	Y2Ba4Cu7O15.09	Y	2	Ba	4	Cu	7															O	15.09	15.09	1	1992																												Y247																				89					89																																																																																		1.1				0.00000000006					RH3510										HALL EFFECT IN Y2BA4CU7OX CERAMICS WITH 14.1<X<15.1	199204			PHYS.REV.B,45(1992)8189	J.Y.GENOUD,M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF	Y,BA,CU,O	
3511	PR0458189	SAME AS 3510	YBa2Cu4O15	Y2Ba4Cu7O15.03	Y	2	Ba	4	Cu	7															O	15.03	15.03	1	1992																												Y247																				87					87																																																																																		1.2				0.00000000005					RH3511										HALL EFFECT IN Y2BA4CU7OX CERAMICS WITH 14.1<X<15.1	199204			PHYS.REV.B,45(1992)8189	J.Y.GENOUD,M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF	Y,BA,CU,O	
3512	PR0458189	SAME AS 3510	YBa2Cu4O15	Y2Ba4Cu7O14.53	Y	2	Ba	4	Cu	7															O	14.53	14.53	1	1992																												Y247																				60					60																																																																																		1.3				0.00000000025					RH3512										HALL EFFECT IN Y2BA4CU7OX CERAMICS WITH 14.1<X<15.1	199204			PHYS.REV.B,45(1992)8189	J.Y.GENOUD,M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF	Y,BA,CU,O	
3513	PR0458189	SAME AS 3510	YBa2Cu4O15	Y2Ba4Cu7O14.13	Y	2	Ba	4	Cu	7															O	14.13	14.13	1	1992																												Y247																				37					37																																																																																		1.8				0.00000000041					RH3513										HALL EFFECT IN Y2BA4CU7OX CERAMICS WITH 14.1<X<15.1	199204			PHYS.REV.B,45(1992)8189	J.Y.GENOUD,M.AFFRONTE,M.DECROUX,O.FISCHER,T.GRAF	Y,BA,CU,O	
3514	PR0457356		(Nd,Ce)2CuO4	Nd1.99Ce0.01Cu1O4	Nd	1.99	Ce	0.01	Cu	1															O	4		1	1992																												T'																																																																																												-16.5			TP3514																															THERMOELECTRIC POWER OF ND2-XCEXCUO4 CRYSTALS	199204			PHYS.REV.B,45(1992)7356	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.-Q.XU,Z.Y.LI	ND,CE,CU,O	
3515	PR0457356		(Nd,Ce)2CuO4	Nd1.975Ce0.025Cu1O4	Nd	1.975	Ce	0.025	Cu	1															O	4		1	1992																												T'																																																																																												-10.9			TP3515																															THERMOELECTRIC POWER OF ND2-XCEXCUO4 CRYSTALS	199204			PHYS.REV.B,45(1992)7356	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.-Q.XU,Z.Y.LI	ND,CE,CU,O	
3516	PR0457356		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1992																												T'																					24				24																																																																			-0.92			TP3516												0.6				-0.00000000087					RH3516										THERMOELECTRIC POWER OF ND2-XCEXCUO4 CRYSTALS	199204			PHYS.REV.B,45(1992)7356	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.-Q.XU,Z.Y.LI	ND,CE,CU,O	
3517	PR0457356		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1992																												T'																					24				24																																																																						TP3517												0.3				-0.00000000042					RH3517										THERMOELECTRIC POWER OF ND2-XCEXCUO4 CRYSTALS	199204			PHYS.REV.B,45(1992)7356	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.-Q.XU,Z.Y.LI	ND,CE,CU,O	
3518	PR0457356		(Nd,Ce)2CuO4	Nd1.78Ce0.22Cu1O4	Nd	1.78	Ce	0.22	Cu	1															O	4		1	1992																												T'																																																																																															TP3518																															THERMOELECTRIC POWER OF ND2-XCEXCUO4 CRYSTALS	199204			PHYS.REV.B,45(1992)7356	J.L.PENG,R.L.GREENE,S.J.HAGEN,W.JIANG,X.-Q.XU,Z.Y.LI	ND,CE,CU,O	
3519	PHC1940321	2223PHASE DOMINANT	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.05Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.05	Cu	3									O	Z		2	1992																																															75		113				94																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3520	PHC1940321	2223 PHASE DOMINANT	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.1Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.1	Cu	3									O	Z		2	1992																																															77		110				93.5																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3521	PHC1940321	2223 PHASE DOMINANT	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.2Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.2	Cu	3									O	Z		2	1992																																															73		110				91.5																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3522	PHC1940321	2223 PHASE DOMINANT	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.25Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.25	Cu	3									O	Z		2	1992																																															74		112				93																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3523	PHC1940321	2212 PHASE DOMINANT,TWO TC	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.3Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.3	Cu	3									O	Z		2	1992																																															69	81	110				81																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3524	PHC1940321		(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	Cu	3											O	Z		1	1992																																															82		110				96																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3525	PHC1940321	2212 PHASE DOMINANT,TWO TC	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.4Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.4	Cu	3									O	Z		2	1992																																															73	83	106				83																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3526	PHC1940321	2212 PHASE DOMINANT,TWO TC	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In0.6Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	0.6	Cu	3									O	Z		2	1992																																															72	84	105				84																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3527	PHC1940321	2212 PHASE DOMINANT,TWO TC	(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In1Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	1	Cu	3									O	Z		2	1992																																															72	85	105				85																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3528	PHC1940321		(Bi,Pb)2Sr2Ca2(In)XCu3OZ	Bi1.8Pb0.2Sr2Ca2In2Cu3OZ	Bi	1.8	Pb	0.2	Sr	2	Ca	2	In	2	Cu	3									O	Z		1	1992																																															73		87				80																																																																																																					INDIUM DOPING IN THE BI-PB-SR-CA-CU-O SUPERCONDUCTING SYSTEM	199205			PHYSICA C,194(1992)321	A.PUNNETT,P.K.UMMAT,R.K.NKUM,W.R.DATARS	BI,PB,SR,CA,CU,O	
3529	PR0447042		(Sm,Pr)Ba2Cu3O7	Sm1Ba2Cu3O6.95	Sm	1	Ba	2	Cu	3															O	Z	6.95	1	1991																											3	Y123																				90					90																																																																																		1.41																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3530	PR0447042		(Sm,Pr)Ba2Cu3O7	Sm0.9Pr0.1Ba2Cu3O6.95	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				65.7					65.7																																																																																		2.23																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3531	PR0447042		(Sm,Pr)Ba2Cu3O7	Sm0.8Pr0.2Ba2Cu3O6.95	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				38.3					38.3																																																																																		2.75																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3532	PR0447042		(Sm,Pr)Ba2Cu3O7	Sm0.7Pr0.3Ba2Cu3O6.95	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				11.9					11.9																																																																																		4.1																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3533	PR0447042		(Sm,Pr)Ba2Cu3O7	Sm0.6Pr0.4Ba2Cu3O6.95	Sm	0.6	Pr	0.4	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																							4.2																																																																																				5.4																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3534	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm1Ba2Cu3O6.95	Tm	1	Ba	2	Cu	3															O	Z	6.95	1	1991																											3	Y123																				89					89																																																																																		4.42																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3535	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.9Pr0.1Ba2Cu3O6.95	Tm	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				87.9					87.9																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3536	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.8Pr0.2Ba2Cu3O6.95	Tm	0.8	Pr	0.2	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				77.9					77.9																																																																																		5.83																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3537	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.7Pr0.3Ba2Cu3O6.95	Tm	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				64.1					64.1																																																																																		7.5																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3538	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.6Pr0.4Ba2Cu3O6.95	Tm	0.6	Pr	0.4	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				50.3					50.3																																																																																		11.3																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3539	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.5Pr0.5Ba2Cu3O6.95	Tm	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				28.9					28.9																																																																																		12.1																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3540	PR0447042		(Tm,Pr)Ba2Cu3O7	Tm0.4Pr0.6Ba2Cu3O6.95	Tm	0.4	Pr	0.6	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																							4.2																																																																																				15																			SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3541	PR0447042		(Gd,Pr)Ba2Cu3O7	Gd1Ba2Cu3O6.95	Gd	1	Ba	2	Cu	3															O	Z	6.95	1	1991																											3	Y123																				90					90																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3542	PR0447042		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3O6.95	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				74.3					74.3																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3543	PR0447042		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O6.95	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				53.1					53.1																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3544	PR0447042		(Gd,Pr)Ba2Cu3O7	Gd0.7Pr0.3Ba2Cu3O6.95	Gd	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				30.6					30.6																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3545	PR0447042		(Gd,Pr)Ba2Cu3O7	Gd0.6Pr0.4Ba2Cu3O6.95	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	Z	6.95	1	1991																											3	Y123																				11.2					11.2																																																																																																					SUPPRESSION OF SUPERCONDUCTIVITY IN THE OXIDE SYSTEMS R1-XPRXBA2CU3O7-Y  (R=SM,GD,AND TM)	199110		TATA INSTITUTE OF FUNDAMENTAL RESEARCH,BOMBAY 400005,INDIA	PHYS.REV.B,44(1991)7042	C.V.TOMY,PARAG BHARGAVA,S.K.MALIK	SM,GD,TM,PR,BA,CU,O	
3546	PHC1940337		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.32	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6.32	6.32		1992																												Bi2201				5.384	5.407	24.491														23.2				6.8	23.2										14																																																																								1.8																			STRONG INFLUENCE OF THE OXYGEN CONTENT ON THE ELECTRICAL AND MAGNETIC PROPERTIES OF BI2SR1.6LA0.4CUOY	199205			PHYSICA C,194(1992)337	C.ALLGEIER,J.J.NEUMEIER,J.S.SCHILLING	BI,SR,LA,CU,O	
3547	PHC1940337	SEMICON-LIKE	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.26	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6.26	6.26	1	1992																											3	Bi2201				5.4	5.42	24.563																													5																																																																																											STRONG INFLUENCE OF THE OXYGEN CONTENT ON THE ELECTRICAL AND MAGNETIC PROPERTIES OF BI2SR1.6LA0.4CUOY	199205			PHYSICA C,194(1992)337	C.ALLGEIER,J.J.NEUMEIER,J.S.SCHILLING	BI,SR,LA,CU,O	
3548	PHC1940337	MAXIMUM TC IN THIS SYSTEM	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.29	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6.29	6.29	1	1992																											3	Bi2201																				30.6					30.6										18																																																																								2.8																			STRONG INFLUENCE OF THE OXYGEN CONTENT ON THE ELECTRICAL AND MAGNETIC PROPERTIES OF BI2SR1.6LA0.4CUOY	199205			PHYSICA C,194(1992)337	C.ALLGEIER,J.J.NEUMEIER,J.S.SCHILLING	BI,SR,LA,CU,O	
3549	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.9Pb0.1Sr2Ca1Cu2O8+Z	Bi	1.9	Pb	0.1	Sr	2	Ca	1	Cu	2											O	8+Z			1992																												Bi2212																			79.8		96.8				88.3																																																																			4.02			TP3549																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3550	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.85Pb0.15Sr2Ca1Cu2O8+Z	Bi	1.85	Pb	0.15	Sr	2	Ca	1	Cu	2											O	8+Z			1992																												Bi2212																			85.5		96.3				90.9																																																																			4.16			TP3550																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3551	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+Z			1992																												Bi2212																			86.8		97				91.9																																																																			2			TP3551																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3552	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.75Pb0.25Sr2Ca1Cu2O8+Z	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	2											O	8+Z			1992																												Bi2212																			85.9		95.7				90.8																																																																			1.62			TP3552																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3553	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8+d	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	8+d			1992																												Bi2212																			87.2		93.6				90.4																																																																			0.26			TP3553																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3554	PR0460463		(Bi,Pb)2Sr2CaCu2O8	Bi1.65Pb0.35Sr2Ca1Cu2O8+Z	Bi	1.65	Pb	0.35	Sr	2	Ca	1	Cu	2											O	8+Z			1992																												Bi2212																			85.9		91.5				88.7																																																																			0.44			TP3554																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3555	PR0460463	Z0+0.23	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O0.23	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	+0.23			1992																												Bi2212																			74.1		77.4				75.75																																																																						TP3555																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3556	PR0460463	Z0+0.27	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O0.27	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	+0.27			1992																												Bi2212																			64.3		70.9				67.6																																																																						TP3556																															THERMOPOWER OF BI2-XPBXSR2CACU2O8+Z	199207			PHYS.REV.B,46(1992)463	C.R.VAROY,H.J.TRODAHL	BI,PB,SR,CA,CU,O	
3557	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.85Re0.15O7	Y	1	Sr	2	Cu	2.85	Re	0.15													O	7.0	7	1	1992																											2	Y123				3.81		11.522													53						53																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3558	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.8Re0.2O6.9	Y	1	Sr	2	Cu	2.8	Re	0.2													O	6.9	6.9	1	1992																											2	Y123				3.814		11.524													43						43																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3559	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.75Re0.25O7	Y	1	Sr	2	Cu	2.75	Re	0.25													O	7.0	7	1	1992																											2	Y123				3.821		11.527													37						37																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3560	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.7Re0.3O7.1	Y	1	Sr	2	Cu	2.7	Re	0.3													O	7.1	7.1	1	1992																											2	Y123				3.823		11.529													33						33																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3561	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.85Re0.15O7.1	Y	1	Sr	2	Cu	2.85	Re	0.15													O	7.1	7.1	1	1992																											2	Y123				3.811		11.495													73						73																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3562	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.8Re0.2O7.2	Y	1	Sr	2	Cu	2.8	Re	0.2													O	7.2	7.2	1	1992																											2	Y123				3.815		11.496													63						63																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3563	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.75Re0.25O7.3	Y	1	Sr	2	Cu	2.75	Re	0.25													O	7.3	7.3	1	1992																											2	Y123				3.822		11.496													49						49																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3564	PHC1960141		YSr2(Cu,Re)3O7	Y1Sr2Cu2.7Re0.3O7.2	Y	1	Sr	2	Cu	2.7	Re	0.3													O	7.2	7.2	1	1992																											2	Y123				3.824		11.499													44						44																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3565	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.8W0.2O6.9	Y	1	Sr	2	Cu	2.8	W	0.2													O	6.9	6.9	1	1992																											2	Y123			A	3.805		11.522												K	45						45																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3566	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.75W0.25O6.9	Y	1	Sr	2	Cu	2.75	W	0.25													O	6.9	6.9	1	1992																											2	Y123				3.809		11.526													33						33																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3567	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.7W0.3O6.9	Y	1	Sr	2	Cu	2.7	W	0.3													O	6.9	6.9	1	1992																											2	Y123				3.812		11.535													24						24																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3568	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.8W0.2O7.2	Y	1	Sr	2	Cu	2.8	W	0.2													O	7.2	7.2	1	1992																											2	Y123				3.804		11.491													66						66																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3569	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.75W0.25O7.1	Y	1	Sr	2	Cu	2.75	W	0.25													O	7.1	7.1	1	1992																											2	Y123				3.809		11.492													51						51																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3570	PHC1960141		YSr2(Cu,W)3O7	Y1Sr2Cu2.7W0.3O6.9	Y	1	Sr	2	Cu	2.7	W	0.3													O	6.9	6.9	1	1992																											2	Y123				3.811		11.522													28						28																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3571	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.8Mo0.2O7	Y	1	Sr	2	Cu	2.8	Mo	0.2													O	7.0	7	1	1992																											2	Y123				3.807		11.521													40						40																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3572	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.75Mo0.25O7.1	Y	1	Sr	2	Cu	2.75	Mo	0.25													O	7.1	7.1	1	1992																											2	Y123				3.812		11.537													31						31																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3573	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.7Mo0.3O7.1	Y	1	Sr	2	Cu	2.7	Mo	0.3													O	7.1	7.1	1	1992																											2	Y123				3.816		11.534													30						30																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3574	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.65Mo0.35O7.2	Y	1	Sr	2	Cu	2.65	Mo	0.35													O	7.2	7.2	1	1992																											2	Y123				3.819		11.537													29						29																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3575	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.8Mo0.2O7.1	Y	1	Sr	2	Cu	2.8	Mo	0.2													O	7.1	7.1	1	1992																											2	Y123				3.807		11.49													71						71																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3576	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.75Mo0.25O7.1	Y	1	Sr	2	Cu	2.75	Mo	0.25													O	7.1	7.1	1	1992																											2	Y123				3.812		11.499													55						55																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3577	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.7Mo0.3O7.1	Y	1	Sr	2	Cu	2.7	Mo	0.3													O	7.1	7.1	1	1992																											2	Y123				3.816		11.496													43						43																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3578	PHC1960141		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.65Mo0.35O7.4	Y	1	Sr	2	Cu	2.65	Mo	0.35													O	7.4	7.4	1	1992																											2	Y123				3.819		11.499													43						43																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3579	PHC1960141		YSr2(Cu,Co)3O7	Y1Sr2Cu2.7Co0.3O6.7	Y	1	Sr	2	Cu	2.7	Co	0.3													O	6.7	6.7	1	1992																											2	Y123				3.808		11.414													27						27																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3580	PHC1960141		YSr2(Cu,Co)3O7	Y1Sr2Cu2.6Co0.4O6.8	Y	1	Sr	2	Cu	2.6	Co	0.4													O	6.8	6.8	1	1992																											2	Y123				3.812		11.412																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3581	PHC1960141		YSr2(Cu,Ga)3O7	Y1Sr2Cu2.65Ga0.35O6.6	Y	1	Sr	2	Cu	2.65	Ga	0.35													O	6.6	6.6	1	1992																											2	Y123				3.811		11.453													17						17																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3582	PHC1960141		YSr2(Cu,Ga)3O7	Y1Sr2Cu2.6Ga0.4O6.7	Y	1	Sr	2	Cu	2.6	Ga	0.4													O	6.7	6.7	1	1992																											2	Y123				3.813		11.447																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3583	PHC1960141		YSr2(Cu,Ga)3O7	Y1Sr2Cu2.65Ga0.35O6.7	Y	1	Sr	2	Cu	2.65	Ga	0.35													O	6.7	6.7	1	1992																											2	Y123				3.812		11.439													21						21																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3584	PHC1960141		YSr2(Cu,Ga)3O7	Y1Sr2Cu2.6Ga0.4O6.8	Y	1	Sr	2	Cu	2.6	Ga	0.4													O	6.8	6.8	1	1992																											2	Y123				3.815		11.437																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3585	PHC1960141		YSr2(Cu,Ge)3O7	Y1Sr2Cu2.8Ge0.2O	Y	1	Sr	2	Cu	2.8	Ge	0.2													O			1	1992																											2	Y123				3.815		11.474																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3586	PHC1960141		YSr2(Cu,Ge)3O7	Y1Sr2Cu2.8Ge0.2O	Y	1	Sr	2	Cu	2.8	Ge	0.2													O			1	1992																											2	Y123				3.817		11.436													18						18																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3587	PHC1960141		YSr2(Cu,Ge)3O7	Y1Sr2Cu2.75Ge0.25O	Y	1	Sr	2	Cu	2.75	Ge	0.25													O			1	1992																											2	Y123				3.817		11.439																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3588	PHC1960141		YSR2(Cu,Fe)3O7	Y1Sr2Cu2.7Fe0.3O6.9	Y	1	Sr	2	Cu	2.7	Fe	0.3													O	6.9	6.9	1	1992																											2	Y123				3.807		11.41													43						43																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3589	PHC1960141		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.65Fe0.35O6.7	Y	1	Sr	2	Cu	2.65	Fe	0.35													O	6.7	6.7	1	1992																											2	Y123				3.805		11.411													34						34																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3590	PHC1960141		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.6Fe0.4O7	Y	1	Sr	2	Cu	2.6	Fe	0.4													O	7.0	7	1	1992																											2	Y123				3.807		11.412													21						21																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3591	PHC1960141		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.7Fe0.3O7.1	Y	1	Sr	2	Cu	2.7	Fe	0.3													O	7.1	7.1	1	1992																											2	Y123				3.801		11.394													51						51																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3592	PHC1960141		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.65Fe0.35O7.1	Y	1	Sr	2	Cu	2.65	Fe	0.35													O	7.1	7.1	1	1992																											2	Y123				3.801		11.394													46						46																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3593	PHC1960141		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.6Fe0.4O7	Y	1	Sr	2	Cu	2.6	Fe	0.4													O	7.0	7	1	1992																											2	Y123				3.803		11.388													37						37																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3594	PHC1960141		YSr2(Cu,Co)3O7	Y1Sr2Cu2.7Co0.3O6.5	Y	1	Sr	2	Cu	2.7	Co	0.3													O	6.5	6.5	1	1992																											2	Y123				3.811		11.434													13						13																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3595	PHC1960141		YSr2(Cu,Co)3O7	Y1Sr2Cu2.6Co0.4O6.5	Y	1	Sr	2	Cu	2.6	Co	0.4													O	6.5	6.5	1	1992																											2	Y123				3.814		11.432																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3596	PHC1960141		YSr2(Cu,Li)3O7	Y1Sr2Cu2.7Li0.3O	Y	1	Sr	2	Cu	2.7	Li	0.3													O			2	1992																											2	Y123				3.86		11.086																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3597	PHC1960141		YSr2(Cu,V)3O7	Y1Sr2Cu2.8V0.2O6.5	Y	1	Sr	2	Cu	2.8	V	0.2													O	6.5	6.5	1	1992																											2	Y123				3.822		11.431													16						16																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3598	PHC1960141		YSr2(Cu,V)3O7	Y1Sr2Cu2.75V0.25O6.5	Y	1	Sr	2	Cu	2.75	V	0.25													O	6.5	6.5	1	1992																											2	Y123				3.829		11.452																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3599	PHC1960141	METALLIC	YSr2(Cu,V)3O7	Y1Sr2Cu2.8V0.2O6.8	Y	1	Sr	2	Cu	2.8	V	0.2													O	6.8	6.8	1	1992																											3	Y123				3.816	3.84	11.358																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3600	PHC1960141		YSr2(Cu,V)3O7	Y1Sr2Cu2.75V0.25O6.7	Y	1	Sr	2	Cu	2.75	V	0.25													O	6.7	6.7	1	1992																											3	Y123				3.823	3.841	11.377																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3601	PHC1960141		YSr2(Cu,Cr)3O7	Y1Sr2Cu2.8Cr0.2O7	Y	1	Sr	2	Cu	2.8	Cr	0.2													O	7.0	7	1	1992																											3	Y123				3.814	3.856	11.343																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3602	PHC1960141		YSr2(Cu,Cr)3O7	Y1Sr2Cu2.75Cr0.25O7.1	Y	1	Sr	2	Cu	2.75	Cr	0.25													O	7.1	7.1	1	1992																											3	Y123				3.828	3.862	11.347																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3603	PHC1960141		YSr2(Cu,Cr)3O7	Y1Sr2Cu2.7Cr0.3O7.1	Y	1	Sr	2	Cu	2.7	Cr	0.3													O	7.1	7.1	1	1992																											3	Y123				3.839	3.863	11.358																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3604	PHC1960141		YSr2(Cu,Al)3O7	Y1Sr2Cu2.6Al0.4O6.5	Y	1	Sr	2	Cu	2.6	Al	0.4													O	6.5	6.5	1	1992																											2	Y123				3.82		11.325																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3605	PHC1960141		YSr2(Cu,Al)3O7	Y1Sr2Cu2.4Al0.6O6.4	Y	1	Sr	2	Cu	2.4	Al	0.6													O	6.4	6.4	1	1992																											2	Y123				3.833		11.268																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3606	PHC1960141		YSr2(Cu,Al)3O7	Y1Sr2Cu2.2Al0.8O6.3	Y	1	Sr	2	Cu	2.2	Al	0.8													O	6.3	6.3	1	1992																											2	Y123				3.855		11.191																	4.2																																																																																																							PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3607	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O6.7	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	6.7	6.7	1	1992																											2	Y123				3.814		11.471													26						26																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3608	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.675Ti0.325O6.6	Y	1	Sr	2	Cu	2.675	Ti	0.325													O	6.6	6.6	1	1992																											2	Y123				3.816		11.477													21						21																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3609	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.65Ti0.35O6.8	Y	1	Sr	2	Cu	2.65	Ti	0.35													O	6.8	6.8	1	1992																											2	Y123				3.816		11.48													21						21																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3610	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7.0	7	1	1992																											2	Y123				3.809		11.458													58						58																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3611	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.675Ti0.325O7.1	Y	1	Sr	2	Cu	2.675	Ti	0.325													O	7.1	7.1	1	1992																											2	Y123				3.81		11.46													56						56																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3612	PHC1960141		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.65Ti0.35O7.1	Y	1	Sr	2	Cu	2.65	Ti	0.35													O	7.1	7.1	1	1992																											2	Y123				3.81		11.461													53						53																																																																																																					PREPARATION AND PROPERTIES OF YSR2CU3-XMXOY (M=LI,AL,TI,V,CR,FE,CO,GA,GE,MO,W AND RE)	199206			PHYSICA C,196(1992)141	TAMAKI KOBAYASHI,TOHRU DEN	Y,SR,CU,M,O	
3613	PHC1960271	SMALL AMOUNT OF IMPURITY	(Sr,La)CuO2	Sr0.95La0.05Cu1O2.01	Sr	0.95	La	0.05	Cu	1															O	2	2.01	1	1992																											2					3.937		3.422													18	42.4	43.5				42.4																																																																																		95																			STRUCTURAL,ELECTRICAL AND MAGNETIC STUDIES OF INFINITE-LAYEREDSR1-XLAXCUO2 SUPERCONDUCTOR	199206			PHYSICA C,196(1992)271	F.KANAMARU,G.ER.S.KIKKAWA,M.SATO,M.SERA,M.TAKANO,S.TANAKA,Y.BANDO,Y.MIYAMOTO,Z.HIROI	SR,LA,CU,O	
3614	PHC1960271	SAME AS 3613	(Sr,La)CuO2	Sr0.9La0.1Cu1O1.96	Sr	0.9	La	0.1	Cu	1															O	2	1.96	1	1992																											2					3.947		3.412													30.5	42.5	43.5				42.5																																																																			-0.86			TP3614												42									RH3614										STRUCTURAL,ELECTRICAL AND MAGNETIC STUDIES OF INFINITE-LAYEREDSR1-XLAXCUO2 SUPERCONDUCTOR	199206			PHYSICA C,196(1992)271	F.KANAMARU,G.ER.S.KIKKAWA,M.SATO,M.SERA,M.TAKANO,S.TANAKA,Y.BANDO,Y.MIYAMOTO,Z.HIROI	SR,LA,CU,O	
3615	PHC1960271	SAME AS 3613,SOLUBILITY LIMIT>X=0.15	(Sr,La)CuO2	Sr0.88La0.12Cu1O1.97	Sr	0.88	La	0.12	Cu	1															O	2	1.97	1	1992																											2					3.948		3.409													22.5	42.4	42				42.4																																																																																		50																			STRUCTURAL,ELECTRICAL AND MAGNETIC STUDIES OF INFINITE-LAYEREDSR1-XLAXCUO2 SUPERCONDUCTOR	199206			PHYSICA C,196(1992)271	F.KANAMARU,G.ER.S.KIKKAWA,M.SATO,M.SERA,M.TAKANO,S.TANAKA,Y.BANDO,Y.MIYAMOTO,Z.HIROI	SR,LA,CU,O	
3616	PHC1960271		(Sr,La)CuO2	Sr1Cu1O2	Sr	1	Cu	1																	O	2		1	1992																											2					3.928		3.434																																																																																																																								STRUCTURAL,ELECTRICAL AND MAGNETIC STUDIES OF INFINITE-LAYEREDSR1-XLAXCUO2 SUPERCONDUCTOR	199206			PHYSICA C,196(1992)271	F.KANAMARU,G.ER.S.KIKKAWA,M.SATO,M.SERA,M.TAKANO,S.TANAKA,Y.BANDO,Y.MIYAMOTO,Z.HIROI	SR,LA,CU,O	
3617	PHC1960247		DyBaSrCu3O7	Dy1Ba1Sr1Cu3O6.94	Dy	1	Ba	1	Sr	1	Cu	3													O	6.94	6.94	1	1992																											2	Y123				3.828		11.533													80						80																																																																																		1.74																			OXYGEN ORDERING AND SUPERCONDUCTIVITY IN DYBASRCU3OY	199206			PHYSICA C,196(1992)247	M.REISSNER,P.L.STEGER,W.STEINER,X.Z.WANG	DY,BA,SR,CU,O	
3618	PHC1960247		DyBaSrCu3O7	Dy1Ba1Sr1Cu3O6.93	Dy	1	Ba	1	Sr	1	Cu	3													O	6.93	6.93	1	1992																											3	Y123				3.816	3.838	11.542													83						83																																																																																		1.11																			OXYGEN ORDERING AND SUPERCONDUCTIVITY IN DYBASRCU3OY	199206			PHYSICA C,196(1992)247	M.REISSNER,P.L.STEGER,W.STEINER,X.Z.WANG	DY,BA,SR,CU,O	
3619	PHC1950195	MEASURING CURRENT //<100>DIRECTION,G-L PARAMETER=82,HC2(0) BY WHH THEORY	(Ba,K)BiO3	Ba0.62K0.38Bi1O3	Ba	0.62	K	0.38	Bi	1															O	3		3	1992																												BKBO																			28.5		30.5				29.5																						16.1									0.79							45					3690																																																										ELECTRICAL RESISTIVITY OF SINGLE CRYSTAL BA1-XKXBIO3	199205			PHYSICA C,195(1992)195	N.SUZUKI,P.KLAVINS,R.N.SHELTON,T.UCHIDA,W.D.MOSLEY,Y.NAGATA	BA,K,BI,O	
3620	PR0414126		(Ba,K)BiO3	Ba1Bi1O3	Ba	1	Bi	1																	O	3			1990																											4	BKBO	I2/M			6.186	6.141	8.672																	4.2																																																																																																							STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3621	PR0414126		(Ba,K)BiO3	Ba0.9K0.1Bi1O3	Ba	0.9	K	0.1	Bi	1															O	3			1990																											4	BKBO	IBMM			6.158	6.126	8.657																	4.2																																																																																																							STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3622	PR0414126		(Ba,K)BiO3	Ba0.8K0.2Bi1O3	Ba	0.8	K	0.2	Bi	1															O	3			1990																											4	BKBO	IBMM			6.128	6.104	8.629																	4.2																																																																																																							STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3623	PR0414126		(Ba,K)BiO3	Ba0.75K0.25Bi1O3	Ba	0.75	K	0.25	Bi	1															O	3			1990																											4	BKBO	IBMM			6.112	6.093	8.613																	4.2																																																																																																							STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3624	PR0414126		(Ba,K)BiO3	Ba0.7K0.3Bi1O3	Ba	0.7	K	0.3	Bi	1															O	3			1990																											1	BKBO	PM3-M			4.301																	29.9				29.9																																																																																																					STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3625	PR0414126		(Ba,K)BiO3	Ba0.65K0.35Bi1O3	Ba	0.65	K	0.35	Bi	1															O	3			1990																											1	BKBO	PM3-M			4.295															28.5		29.9				29.2																																																																																																					STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3626	PR0414126		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1990																											1	BKBO	PM3-M			4.283															27.6		29.4				28.5																																																																																																					STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3627	PR0414126		(Ba,K)BiO3	Ba0.575K0.425Bi1O3	Ba	0.575	K	0.425	Bi	1															O	3			1990																											1	BKBO	PM3-M			4.279															26.6		28				27.3																																																																																																					STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3628	PR0414126		(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3			1990																											1	BKBO	PM3-M			4.27															17.2		21.9				19.55																																																																																																					STRUCTURAL PHASE DIAGRAM OF THE BA1-XKXBIO3 SYSTEM	199003	STRUCTURES          ,NEUTRON DIFFRACTION	MATERIALS SCIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARGONNE, ILLINOIS 60439	PHYS.REV.B,41(1990)4126	A.J.JACOBSON,A.W.MITCHELL,B.DABROWSKI,D.BAKNIN,D.G.HINKS,D.R.RICHARDS,J.D.JORGENSEN,J.M.NEWSAM,S.K.SINHA,SHIYOU PEI	BA,K,BI,O	
3629	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd1Ba2Cu3O6.86	Nd	1	Ba	2	Cu	3															O	Z	6.86	1	1988																											3	Y123				3.866	3.908	11.766													77.1	78.6	80.2				78.6																																																																																		1.65																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3630	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.9Pr0.1Ba2Cu3OZ	Nd	0.9	Pr	0.1	Ba	2	Cu	3													O	Z		1	1988																											3	Y123				3.865	3.917	11.755													45.1	48.9	52.9				48.9																																																																																		1.59																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3631	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3OZ	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	Z		1	1988																											3	Y123				3.863	3.912	11.742													23.9	28.6	33.1				28.6																																																																																		2.14																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3632	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.75Pr0.25Ba2Cu3O6.96	Nd	0.75	Pr	0.25	Ba	2	Cu	3													O	Z	6.96	1	1988																											3	Y123				3.861	3.906	11.758													4.2	11.7	19.3				11.7																																																																																		3.79																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3633	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.7Pr0.3Ba2Cu3O6.98	Nd	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.98	1	1988																											3	Y123				3.866	3.91	11.747																	4.2																																																																																				3.45																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3634	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.65Pr0.35Ba2Cu3O6.87	Nd	0.65	Pr	0.35	Ba	2	Cu	3													O	Z	6.87	1	1988																											3	Y123				3.869	3.913	11.744																	4.2																																																																																				3.48																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3635	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.5Pr0.5Ba2Cu3O6.95	Nd	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.95	1	1988																											3	Y123				3.859	3.902	11.767																	4.2																																																																																				4.31																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3636	APJ0271862		(Nd,Pr)Ba2Cu3O7	Nd0.25Pr0.75Ba2Cu3O6.91	Nd	0.25	Pr	0.75	Ba	2	Cu	3													O	Z	6.91	1	1988																											3	Y123				3.865	3.903	11.769																	4.2																																																																																				7.18																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3637	APJ0271862		(Nd,Pr)Ba2Cu3O7	Pr1Ba2Cu3O6.88	Pr	1	Ba	2	Cu	3															O	Z	6.88	1	1988																											3	Y123				3.875	3.911	11.757																	4.2																																																																																				12																			Electrical, Magnetic and Superconducting Properties of the High-Tc Superconductor Ba2Nd1-xPrxCu3O7-delta	10		Technology Development Center, Toyohashi University of Technology, Tempaku-cho, Toyohashi 440	Japanese J.Appl.Phys.27(1988)1862-1866	Kuniyuki KOYAMA,Seiichiro NOGUCHI,Yasuji SUZUKI		
3638	PHC1960090	TC RELATED TO AVERAGE ION RADIUS OF R	(Lu,Pr)Ba2Cu3O7	Lu0.5Pr0.5Ba2Cu3O6.75	Lu	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.75	1	1992																											3	Y123				3.826	3.891	11.683													37.5	40.1					40.1																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3639	PHC1960090		(Pr,R)Ba2Cu3O7	Yb0.5Pr0.5Ba2Cu3O6.67	Yb	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.67	1	1992																											3	Y123				3.826	3.893	11.676													37	38.7					38.7																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3640	PHC1960090		(Pr,R)Ba2Cu3O7	Tm0.5Pr0.5Ba2Cu3O6.64	Tm	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.64	1	1992																											3	Y123				3.829	3.895	11.679													35	36					36																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3641	PHC1960090		(Pr,R)Ba2Cu3O7	Er0.5Pr0.5Ba2Cu3O6.82	Er	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.82	1	1992																											3	Y123				3.832	3.893	11.682													33	34.4					34.4																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3642	PHC1960090		(Pr,R)Ba2Cu3O7	Ho0.5Pr0.5Ba2Cu3O6.67	Ho	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.67	1	1992																											3	Y123				3.834	3.898	11.691													23	24.3					24.3																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3643	PHC1960090		(Pr,R)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O6.68	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.68	1	1992																											3	Y123				3.837	3.896	11.7													26	27.1					27.1																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3644	PHC1960090		(Pr,R)Ba2Cu3O7	Dy0.5Pr0.5Ba2Cu3O6.85	Dy	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.85	1	1992																											3	Y123				3.844	3.906	11.709													18	19					19																																																																																																					SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3645	PHC1960090		(Pr,R)Ba2Cu3O7	Gd0.5Pr0.5Ba2Cu3O6.79	Gd	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.79	1	1992																											3	Y123				3.836	3.902	11.712																																																																																																																								SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3646	PHC1960090		(Pr,R)Ba2Cu3O7	Eu0.5Pr0.5Ba2Cu3O6.79	Eu	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.79	1	1992																											3	Y123				3.848	3.907	11.709																																																																																																																								SUPERCONDUCTIVITY OF PR0.5R0.5BA2CU3O7-Y SYSTEM AND THE EXISTENCE OF A CRITICAL ION RADIUS FOR SUPPRESSION OF SUPERCONDUCTIVITY IN R1-XPRXBA2CU3O7-Y	199206			PHYSICA C,196(1992)90	A.KUFUDAKIS,CH.MITROS,D.NIARCHOS,D.ZEMANOVA,E.POLLERT,H.GAMARI-SEALE,P.SVOBODA,P.VASEK	PR,BA,CU,O,R	
3647	PHC1960125	MULTI-PHASE FOR 0<X<=0.3,TETRA FOR 0.3<X<=0.7,ORTHO FOR 0.7<X<1.0,AS-SINTERED SAMPLE NOT S/C,STR=1212(Y123)	YSr2(Cu,Ga)3O7	Y1Sr2Cu2.6Ga0.4OZ	Y	1	Sr	2	Cu	2.6	Ga	0.4													O	Z		1	1992																											2	1212				3.813		11.439														10	15				10																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF CUPRATES IN THE YSR2CU3OY-GASR2YCU2OY SYSTEM	199206			PHYSICA C,196(1992)125	H.YAMAUCHI,SATOSHI TAKANO,SEIJI ADACHI	Y,SR,CU,O,GA	
3648	PHC1970303		La2CuO4	La2Cu1O4.03	La	2	Cu	1																	O	4.03	4.03		1992																											3	T				5.361	5.383	13.184														32					32																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3649	PHC1970303		La2CuO4	La2Cu1O4.11	La	2	Cu	1																	O	4.11	4.11		1992																											3	T				5.341	5.404	13.219														45					45																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3650	PHC1970303		La2CuO4	La2Cu1O4.18	La	2	Cu	1																	O	4.18	4.18		1992																											3	T				5.339	5.409	13.214																																																																																																																								SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3651	PHC1970303		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4.07	La	1.75	Sr	0.25	Cu	1															O	4.07	4.07		1992																											2	T				3.77		13.249														37					37																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3652	PHC1970303		(La,Sr)2CuO4	La1.67Sr0.33Cu1O4	La	1.67	Sr	0.33	Cu	1															O	4			1992																												T																				37					37																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3653	PHC1970303		(La,Sr)2CuO4	La1.99Sr0.01Cu1O4.13	La	1.99	Sr	0.01	Cu	1															O	4.13	4.13		1992																											3	T				5.337	5.395	13.198														40					40																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3654	PHC1970303		(La,Sr)2CuO4	La1.98Sr0.02Cu1O4.09	La	1.98	Sr	0.02	Cu	1															O	4.09	4.09		1992																												T																				40					40																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3655	PHC1970303		(La,Sr)2CuO4	La1.97Sr0.03Cu1O4.06	La	1.97	Sr	0.03	Cu	1															O	4.06	4.06		1992																												T																				39					39																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3656	PHC1970303		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4.05	La	1.96	Sr	0.04	Cu	1															O	4.05	4.05		1992																												T																				40					40																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3657	PHC1970303		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4.07	La	1.92	Sr	0.08	Cu	1															O	4.07	4.07		1992																											2	T				3.785		13.221																																																																																																																								SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3658	PHC1970303		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4.05	La	1.85	Sr	0.15	Cu	1															O	4.05	4.05		1992																											2	T				3.775		13.227														39					39																																																																																																					SYNTHESIS,CHARACTERIZATION,AND SUPERCONDUCTING AND MAGNETIC PROPERTIES OF ELECTROCHEMICALLY OXIDIZED LA2CUO4+Z AND LA2-XSRXCUO4+Z (0.01<-X<-0.33,0.01<-Z<-0.36)	199207			PHYSICA C,197(1992)303	D.C.JOHNSTON,F.C.CHOU,J.H.CHO	LA,SR,CU,O	
3659	PHC1970101		(Pb,Ca)Sr2(Ca,Y)Cu2O7	Pb0.5Ca1Sr2Y0.5Cu2O6.93	Pb	0.5	Ca	1	Sr	2	Y	0.5	Cu	2											O	6.93	6.93		1992																												1212																			16	30	40				30										5																																																																																											ENHANCEMENT OF TC TO 60 K IN (PB,CA)SR2(CA,Y)CU2O7-Z BY HIGH PRESSURE OXYGEN TREATMENT AND QUENCHING	199207			PHYSICA C,197(1992)101	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,J.C.HO,X.W.CAO	PB,CA,SR,Y,CU,O	
3660	PHC1970101		(Pb,Ca)Sr2(Ca,Y)Cu2O7	Pb0.5Ca1Sr2Y0.5Cu2O6.95	Pb	0.5	Ca	1	Sr	2	Y	0.5	Cu	2											O	6.95	6.95		1992																												1212																			30	50					50																																																																																																					ENHANCEMENT OF TC TO 60 K IN (PB,CA)SR2(CA,Y)CU2O7-Z BY HIGH PRESSURE OXYGEN TREATMENT AND QUENCHING	199207			PHYSICA C,197(1992)101	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,J.C.HO,X.W.CAO	PB,CA,SR,Y,CU,O	
3661	PHC1970101		(Pb,Ca)Sr2(Ca,Y)Cu2O7	Pb0.5Ca1Sr2Y0.5Cu2O6.97	Pb	0.5	Ca	1	Sr	2	Y	0.5	Cu	2											O	6.97	6.97		1992																												1212																			40	55					55										15																																																																																											ENHANCEMENT OF TC TO 60 K IN (PB,CA)SR2(CA,Y)CU2O7-Z BY HIGH PRESSURE OXYGEN TREATMENT AND QUENCHING	199207			PHYSICA C,197(1992)101	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,J.C.HO,X.W.CAO	PB,CA,SR,Y,CU,O	
3662	PHC1970101		(Pb,Ca)Sr2(Ca,Y)Cu2O7	Pb0.5Ca1Sr2Y0.5Cu2O7	Pb	0.5	Ca	1	Sr	2	Y	0.5	Cu	2											O	7.00	7		1992																												1212																			50	62					62										20																																																																																											ENHANCEMENT OF TC TO 60 K IN (PB,CA)SR2(CA,Y)CU2O7-Z BY HIGH PRESSURE OXYGEN TREATMENT AND QUENCHING	199207			PHYSICA C,197(1992)101	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,J.C.HO,X.W.CAO	PB,CA,SR,Y,CU,O	
3663	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.85Sr0.15Cu1O4+Z	La	1.85	Sr	0.15	Cu	1															O	4+Z			1992																												T																				37.5					37.5																																																																																																					EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3664	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.85Sr0.15Cu0.995Sn0.005O4+Z	La	1.85	Sr	0.15	Cu	0.995	Sn	0.005													O	4+Z			1992																												T																				28					28																																																																																																					EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3665	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.85Sr0.15Cu0.99Sn0.01O4+Z	La	1.85	Sr	0.15	Cu	0.99	Sn	0.01													O	4+Z			1992																												T																				15.8					15.8																																																																																																					EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3666	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.85Sr0.15Cu0.985Sn0.015O4+Z	La	1.85	Sr	0.15	Cu	0.985	Sn	0.015													O	4+Z			1992																												T																				5.2					5.2																																																																																																					EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3667	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.85Sr0.15Cu0.98Sn0.02O4+Z	La	1.85	Sr	0.15	Cu	0.98	Sn	0.02													O	4+Z			1992																												T																							4.2																																																																																																							EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3668	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.992Sr0.008Cu1O4+Z	La	1.992	Sr	0.008	Cu	1															O	4+Z		1	1992								162																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3669	PHC1960315		(La,Sr)2(Cu,Sn)O4	La1.992Sr0.008Cu0.99Sn0.01O4+Z	La	1.992	Sr	0.008	Cu	0.99	Sn	0.01													O	4+Z		1	1992								153																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3670	PHC1960315		La2(Cu,Sn)O4	La2Cu1O4+Z	La	2	Cu	1																	O	4+Z		1	1992								226																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3671	PHC1960315		La2(Cu,Sn)O4	La2Cu0.995Sn0.005O4+Z	La	2	Cu	0.995	Sn	0.005															O	4+Z		1	1992								290																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3672	PHC1960315		La2(Cu,Sn)O4	La2Cu0.99Sn0.01O4+Z	La	2	Cu	0.99	Sn	0.01															O	4+Z		1	1992								230.5																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3673	PHC1960315		La2(Cu,Sn)O4	La2Cu0.97Sn0.03O4+Z	La	2	Cu	0.97	Sn	0.03															O	4+Z		1	1992								232.5																				T																																																																																																																														EFFECT OF SN SUBSTITUTION FOR CU ON THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF LA2-XSRX(CU1-YSNY)O4+Z (0<-X<-0.15)	199206			PHYSICA C,196(1992)315	CH.SAUER,J.OLEJNICZAK,M.M.ABD-ELMEGUID,U.KOBLER,W.ZINN	LA,SR,CU,SN,O	
3674	PHC1960276	SEMICONDUCTOR	(Ca,Sr,Y)CuO2	Ca0.84Sr0.14Y0.02CuO2	Ca	0.84	Sr	0.14	Y	0.02	Cu														O	2		1	1992																											2					3.866		3.209																	4.2																																																																																																							CARRIER DOPING AND RESISTIVE AND MAGNETIC ANOMALIES IN PARTIALLY SUBSTITUTED CA1-XSRXCUO2	199206			PHYSICA C,196(1992)276	HIDEKI MATSUO,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	CA,SR,CU,O	
3675	PHC1960276	SEMICONDUCTOR	(Ca,Sr)(Cu,Ga)O2	Ca0.86Sr0.14Cu0.96Ga0.04O2	Ca	0.86	Sr	0.14	Cu	0.96	Ga	0.04													O	2		1	1992																											2					3.866		3.212																	4.2																																																																																																							CARRIER DOPING AND RESISTIVE AND MAGNETIC ANOMALIES IN PARTIALLY SUBSTITUTED CA1-XSRXCUO2	199206			PHYSICA C,196(1992)276	HIDEKI MATSUO,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	CA,SR,CU,O	
3676	PHC1960276	F CONTENT NOT CLEAR,SEMICONDUCTOR	(Ca,Sr)Cu(O,F)2	Ca0.86Sr0.14Cu1F0.2O1.8	Ca	0.86	Sr	0.14	Cu	1	F	0.2													O	1.8		1	1992																											2					3.861		3.203																	4.2																																																																																																							CARRIER DOPING AND RESISTIVE AND MAGNETIC ANOMALIES IN PARTIALLY SUBSTITUTED CA1-XSRXCUO2	199206			PHYSICA C,196(1992)276	HIDEKI MATSUO,NORIO KOBAYASHI,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	CA,SR,CU,O	
3677	PHC1960291	COMPO.=NOMINAL,	Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1992																											2	Tl2201				3.867		23.186													80		90				85																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3678	PHC1960291		Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8			1992																											2	Tl2212				3.856		29.328													109	109	114				109																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3679	PHC1960291	2223(MAJOR)+2212(MINOR)	Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10		2	1992																											2	Tl2223				3.857		35.711													115	115					115																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3680	PHC1960291	2223(MAJOR)+2212(MINOR)	Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Ca3Cu4O12	Tl	2	Ba	2	Ca	3	Cu	4													O	12		2	1992																											2	Tl2223				3.823		35.373													115	120	126				120																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3681	PHC1960291	2223(MAJOR)+CUO	Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Ca4Cu5O14	Tl	2	Ba	2	Ca	4	Cu	5													O	14		2	1992																											2	Tl2223				3.816		35.346													121	124	130				124																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3682	PHC1960291	IMPURITY=CA2CUO3,CUO+UNKNOWN	Tl2Ba2Ca(N-1)Cu(N)O(2N+1)	Tl2Ba2Ca5Cu6O16	Tl	2	Ba	2	Ca	5	Cu	6													O	16		2	1992																											2					3.831		35.356													116	120	128				120																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING PROPERTIES OF THE TL-BA-CA-CU-O SYSTEM	199206			PHYSICA C,196(1992)291	ALI NAZIRIPOUR,ALLEN M.HERMANN,CHENG DONG,HONG MIN DUAN,JOHN.W.DREXLER,WILLIAM KIEHL	TL,BA,CA,CU,O	
3683	PHC1980033	NON-S/C PHASES ARE CONTAINED,GAP=FOE // PLANE	Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1992																												Bi2212				5.414	5.426	30.921														88					88																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+Z SINGLE CRYSTALS	199207			PHYSICA C,198(1992)33	G.GUNTHERODT,L.BUSCHMANN,M.BOEKHOLT,M.FLEUSTER,TH.BOLLMEIER	BI,SR,CA,CU,CO,O	
3684	PHC1980033	3683,2GAP//=39MEV,2GAP(PERPENDICULAR)=20MEV	Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.96Co0.04O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	8+Z		3	1992																												Bi2212				5.379	5.414	30.89														78					78																																																5.8	1																																																				STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+Z SINGLE CRYSTALS	199207			PHYSICA C,198(1992)33	G.GUNTHERODT,L.BUSCHMANN,M.BOEKHOLT,M.FLEUSTER,TH.BOLLMEIER	BI,SR,CA,CU,CO,O	
3685	PHC1980033	3683,2GAP//=36MEV	Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.92Co0.08O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	8+Z		3	1992																												Bi2212				5.362	5.405	30.718														68					68																																																6.1	1																																																				STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+Z SINGLE CRYSTALS	199207			PHYSICA C,198(1992)33	G.GUNTHERODT,L.BUSCHMANN,M.BOEKHOLT,M.FLEUSTER,TH.BOLLMEIER	BI,SR,CA,CU,CO,O	
3686	PHC1980033	3683,2GAP//=26MEV	Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.88Co0.12O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	8+Z		3	1992																												Bi2212				5.342	5.397	30.69														56					56																																																5.4	1																																																				STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+Z SINGLE CRYSTALS	199207			PHYSICA C,198(1992)33	G.GUNTHERODT,L.BUSCHMANN,M.BOEKHOLT,M.FLEUSTER,TH.BOLLMEIER	BI,SR,CA,CU,CO,O	
3687	PHC1980033	3683,2GAP//=19MEV	Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.84Co0.16O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	8+Z		3	1992																												Bi2212																				45					45																																																4.9	1																																																				STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA(CU1-YCOY)2O8+Z SINGLE CRYSTALS	199207			PHYSICA C,198(1992)33	G.GUNTHERODT,L.BUSCHMANN,M.BOEKHOLT,M.FLEUSTER,TH.BOLLMEIER	BI,SR,CA,CU,CO,O	
3688	PHC1980070		YSr2(Cu,Mo)3O7	Y1Sr2Cu2.8Mo0.2OZ	Y	1	Sr	2	Cu	2.8	Mo	0.2													O	Z		1	1992																											2	Y123				3.803		11.5													42	45	48				45			K/GPa	8.4																																																																																																	HIGH-PRESSURE STUDY ON MO-STABILIZED SR-BASED 123 COMPOUNDS YSR2CU2.8MO0.2OY AND TBSR2CU2.7MO0.3OY	199207			PHYSICA C,198(1992)70	C.W.CHU,H.H.FENG,J.W.CHU,K.MATSUISHI,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN	Y,SR,CU,MO,O,TB	
3689	PHC1980070		TbSr2(Cu,Mo)3O7	Tb1Sr2Cu2.7Mo0.3OZ	Tb	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1992																											2	Y123				3.821		11.53													28	31	34				31			K/GPa	4																																																																																																	HIGH-PRESSURE STUDY ON MO-STABILIZED SR-BASED 123 COMPOUNDS YSR2CU2.8MO0.2OY AND TBSR2CU2.7MO0.3OY	199207			PHYSICA C,198(1992)70	C.W.CHU,H.H.FENG,J.W.CHU,K.MATSUISHI,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN	Y,SR,CU,MO,O,TB	
3690	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr6Ca6Cu9O33.964	Bi	8	Sr	6	Ca	6	Cu	9													O	Z	33.964		1992																											2	Bi2212																				80					80																																																																			-2.36			TP3690																															THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3691	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr6Ca6Cu9O33.912	Bi	8	Sr	6	Ca	6	Cu	9													O	Z	33.912		1992																											2	Bi2212																				85					85																																																																			2.2			TP3691												3.8																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3692	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr6Ca6Cu9O33.85	Bi	8	Sr	6	Ca	6	Cu	9													O	Z	33.85		1992																											2	Bi2212																				72.5					72.5																																																																			7.34			TP3692												17																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3693	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr6Ca6Cu9O34	Bi	8	Sr	6	Ca	6	Cu	9													O	Z	34		1992																											2	Bi2212																				74.3					74.3																																																																			-3.31			TP3693												2.2																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3694	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr8Ca4Cu9O34.16	Bi	8	Sr	8	Ca	4	Cu	9													O	Z	34.16		1992																											2	Bi2212																				94.2					94.2																																																																			1.79			TP3694																															THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3695	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr8Ca4Cu9O34.25	Bi	8	Sr	8	Ca	4	Cu	9													O	Z	34.25		1992																											2	Bi2212				5.388		30.406														73.5					73.5																																																																			-4.02			TP3695												2.4																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3696	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr7Ca5Cu9O34.13	Bi	8	Sr	7	Ca	5	Cu	9													O	Z	34.13		1992																											2	Bi2212				5.392		30.568														72.5					72.5																																																																			-4.38			TP3696												2																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3697	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr6Ca6Cu9O33+X	Bi	8	Sr	6	Ca	6	Cu	9													O	33+X			1992																											2	Bi2212				5.392		30.577														74.3					74.3																																																																			-3.53			TP3697												2.2																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3698	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr5Ca7Cu9O34.94	Bi	8	Sr	5	Ca	7	Cu	9													O	Z	34.94		1992																											2	Bi2212				5.389		30.686														74.4					74.4																																																																			-2.44			TP3698												2.6																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3699	PHC1980162		Bi2Sr2CaCu2O8	Bi8Sr4Ca8Cu9O33+X	Bi	8	Sr	4	Ca	8	Cu	9													O	33+X			1992																											2	Bi2212				5.399		30.769														69					69																																																																			-1.91			TP3699												11.6																			THE EFFECT OF ISOELECTRONIC CATION SUBSTITUTION AND DEOXYGENATION OF BI8SR8-XCA4+XCU9O33+E-Z SUPERCONDUCTORS ON THE THERMOPOWER AND RESISTIVITY	199207			PHYSICA C,198(1992)162	R.HORYN,T.CICHOREK,W.WOJAKOWSKI,Z.HENKIE	BI,SR,CA,CU,O	
3700	PHC1980209	PRECURSOR=OXALATE	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7			1992																											2					3.952		12.12														26					26																																																																																																					THE OXYFLUORIDE ND2CUO4-XFX	199208			PHYSICA C,198(1992)209	A.TIGHEZZA,J.L.REHSPRINGER,M.DRILLON	ND,CU,O,F	
3701	PHC1980209	PRECURSOR=PROPINATE	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7			1992																											2																					37					37																																																																																																					THE OXYFLUORIDE ND2CUO4-XFX	199208			PHYSICA C,198(1992)209	A.TIGHEZZA,J.L.REHSPRINGER,M.DRILLON	ND,CU,O,F	
3702	PHC1980209	PRECURSOR=HYDROXIDE	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7			1992																											2																					28					28																																																																																																					THE OXYFLUORIDE ND2CUO4-XFX	199208			PHYSICA C,198(1992)209	A.TIGHEZZA,J.L.REHSPRINGER,M.DRILLON	ND,CU,O,F	
3703	PHC1980209	PRECURSOR=OXIDE	Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7			1992																											2																					25					25																																																																																																					THE OXYFLUORIDE ND2CUO4-XFX	199208			PHYSICA C,198(1992)209	A.TIGHEZZA,J.L.REHSPRINGER,M.DRILLON	ND,CU,O,F	
3704	PHC1980231		CaLaBaCu3O7	Ca1La1Ba1Cu3O7	Ca	1	La	1	Ba	1	Cu	3													O	7			1992																											2	Y123				3.865		11.635															80				80																																																																																																					PRESSURE DEPENDENCE OF TC AND HC2 OF CALABACU3O7 UP TO 50 GPA	199208			PHYSICA C,198(1992)231	D.M.DE LEEUW,E.N.VAN EENIGE,J.J.SCHOLZ,R.GRIESSEN,R.J.WIJNGAARDEN	CA,LA,BA,CU,O	
3705	PHC1980318			Tl0.5Pb0.5Sr1.6Ca2.4Cu3O9	Tl	0.5	Pb	0.5	Sr	1.6	Ca	2.4	Cu	3											O	9			1992																												Tl2223																			107	113	115				113																																																																																																					SUPERCONDUCTIVITY AT 124 K IN (TL,PB)SR2CA2CU3O9	199208			PHYSICA C,198(1992)318	D.A.JEFFERSON,P.P.EDWARDS,R.S.LIU,S.F.HU	TL,PB,SR,CA,CU,O	
3706	PHC1980318			Tl0.5Pb0.5Sr1.6Ca2.4Cu3O9	Tl	0.5	Pb	0.5	Sr	1.6	Ca	2.4	Cu	3											O	9			1992																												Tl2223																			115	117	120				117																																																																																																					SUPERCONDUCTIVITY AT 124 K IN (TL,PB)SR2CA2CU3O9	199208			PHYSICA C,198(1992)318	D.A.JEFFERSON,P.P.EDWARDS,R.S.LIU,S.F.HU	TL,PB,SR,CA,CU,O	
3707	PHC1980318			Tl0.5Pb0.5Sr1.6Ca2.4Cu3O9	Tl	0.5	Pb	0.5	Sr	1.6	Ca	2.4	Cu	3											O	9			1992																												Tl2223				3.82		15.28													122.5	124	130				124																																																																																																					SUPERCONDUCTIVITY AT 124 K IN (TL,PB)SR2CA2CU3O9	199208			PHYSICA C,198(1992)318	D.A.JEFFERSON,P.P.EDWARDS,R.S.LIU,S.F.HU	TL,PB,SR,CA,CU,O	
3708	PHC1990023	RANDOM ORIENTED MULTI-GRAIN(8*8*4 MM3),EXTENSIVE TWIN	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1992																											3	Y123																				94					94																																																		16000																																																			TRANSPORT CRITICAL CURRENTS AND FLUX PINNING IN MELT-GROWN YBA2CU3O7-Z	199208			PHYSICA C,199(1992)23	C.BEDUZ,R.G.SCURLOCK,Y.YANG,Z.YI	Y,BA,CU,O	
3709	PHC1990032	DEMAG.FACTOR=0.87,HC1 FROM MAGNETIZATION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1992																												Bi2212																				87					87													340																																																																																								TEMPERATURE DEPENDENCE OF THE LOWER CRITICAL FIELD UNDER THE EFFECT OF SURFACE BARRIES IN BI2SR2CACU2O8 CRYSTAL	199208			PHYSICA C,199(1992)32	K.KISHIO,M.KONCZYKOWSKI,N.CHIKUMOTO,N.MOTOHIRA	BI,SR,CA,CU,O	
3710	PHC1990037	AC(80HZ) RESISTIVITY	(Y,Ca)SrBa(Cu,Co)3O7	Y1Sr1Ba1Cu2.7Co0.3O6+Z	Y	1	Sr	1	Ba	1	Cu	2.7	Co	0.3											O	6+Z		1	1992																											2	Y123				3.84		11.502														22				11	22																																																																																		27				0.00000000368				11											REMARKABLE INFLUENCE OF CA ON THE NORMAL STATE AND THE SUPERCONDUCTING PROPERTIES OF YSRBACU3-YCOYO6+Z (Y=0.3)	199208			PHYSICA C,199(1992)37	H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	Y,SR,BA,CU,CO,O,CA	
3711	PHC1990037		(Y,Ca)SrBa(Cu,Co)3O7	Y0.9Ca0.1Sr1Ba1Cu2.7Co0.3O6+Z	Y	0.9	Ca	0.1	Sr	1	Ba	1	Cu	2.7	Co	0.3									O	6+Z		1	1992																											2	Y123				3.83		11.531														40					40																																																																																		2				0.00000000231															REMARKABLE INFLUENCE OF CA ON THE NORMAL STATE AND THE SUPERCONDUCTING PROPERTIES OF YSRBACU3-YCOYO6+Z (Y=0.3)	199208			PHYSICA C,199(1992)37	H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	Y,SR,BA,CU,CO,O,CA	
3712	PHC1990037		(Y,Ca)SrBa(Cu,Co)3O7	Y0.8Ca0.2Sr1Ba1Cu2.7Co0.3O6+Z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.7	Co	0.3									O	6+Z		1	1992																											2	Y123				3.82		11.538														58				9	58																																																																																		1.74				0.00000000145															REMARKABLE INFLUENCE OF CA ON THE NORMAL STATE AND THE SUPERCONDUCTING PROPERTIES OF YSRBACU3-YCOYO6+Z (Y=0.3)	199208			PHYSICA C,199(1992)37	H.PANKOWSKA,L.OUHAMMOU,O.GOROCHOV,R.SURYANARAYANAN	Y,SR,BA,CU,CO,O,CA	
3713	PHC1990130	MAIN PHASE=Y124(>95%)	YBa2(Cu,Fe)4O8	Y1Ba2Cu3.975Fe0.025O8	Y	1	Ba	2	Cu	3.975	Fe	0.025													O	8		1	1992																											3	Y124				3.835	3.87	27.17														64.6					64.6																																																																																																					MAGNETIZATION MEASUREMENTS AND MOSSBAUER SPECTROSCOPY IN IRONDOPED YBA2CU4O8	199208			PHYSICA C,199(1992)130	D.E.MORRIS,H.J.BORNMANN,M.A.CHUEV,V.M.CHELEPANOV	FE,Y,BA,CU,O	
3714	PHC1990130		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.987Fe0.013O8	Y	1	Ba	2	Cu	3.987	Fe	0.013													O	8		1	1992																												Y124																				70.3					70.3																																																																																																					MAGNETIZATION MEASUREMENTS AND MOSSBAUER SPECTROSCOPY IN IRONDOPED YBA2CU4O8	199208			PHYSICA C,199(1992)130	D.E.MORRIS,H.J.BORNMANN,M.A.CHUEV,V.M.CHELEPANOV	FE,Y,BA,CU,O	
3715	PHC1990130		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.925Fe0.075O8	Y	1	Ba	2	Cu	3.925	Fe	0.075													O	8		1	1992																												Y124																				44.2					44.2																																																																																																					MAGNETIZATION MEASUREMENTS AND MOSSBAUER SPECTROSCOPY IN IRONDOPED YBA2CU4O8	199208			PHYSICA C,199(1992)130	D.E.MORRIS,H.J.BORNMANN,M.A.CHUEV,V.M.CHELEPANOV	FE,Y,BA,CU,O	
3716	PHC1990143	TC DEPEND ON HOLE DENSITY	(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4.00	4		1992																												T																				37					37																																																																																																					EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3717	PHC1990143		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.994	La	1.82	Sr	0.18	Cu	1															O	3.994	3.994		1992																												T																				34					34																																																																																																					EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3718	PHC1990143		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.987	La	1.82	Sr	0.18	Cu	1															O	3.987	3.987		1992																												T																				33					33																																																																																																					EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3719	PHC1990143		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.972	La	1.82	Sr	0.18	Cu	1															O	3.972	3.972		1992																												T																				28					28																																																																																																					EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3720	PHC1990143		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.967	La	1.82	Sr	0.18	Cu	1															O	3.967	3.967		1992																												T																				22					22																																																																																																					EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3721	PHC1990143		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.957	La	1.82	Sr	0.18	Cu	1															O	3.957	3.957		1992																												T																							4.2																																																																																																							EFFECT OF 0XYGEN VACANCY ON MAGNETIC AND SUPERCONDUCTING PROPERTIES IN LA1.82SR0.18CUO4	199208			PHYSICA C,199(1992)143	N.ISHIKAWA,N.KURODA,R.YOSHIZAKI,S.NAKAMURA	LA,SR,CU,O	
3722	PHC1990177	NEARLY SINGLE PHASE	Yb(Ba,Sr)2Cu4O8	Yb1Ba1.8Sr0.2Cu4O8	Yb	1	Ba	1.8	Sr	0.2	Cu	4													O	8		1	1992																											3	Y124				3.814	3.857	27.129													77	80	82				80																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3723	PHC1990177		Yb(Ba,Sr)2Cu4O8	Yb1Ba1.6Sr0.4Cu4O8	Yb	1	Ba	1.6	Sr	0.4	Cu	4													O	8		1	1992																											3	Y124				3.805	3.855	27.072													78	80	83				80																																																																			5.47			TP3723																															"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3724	PHC1990177		Yb(Ba,Sr)2Cu4O8	Yb1Ba1.4Sr0.6Cu4O8	Yb	1	Ba	1.4	Sr	0.6	Cu	4													O	8		1	1992																											3	Y124				3.796	3.851	27.022													77	80	83				80																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3725	PHC1990177	Y124+OTHER PHASES	Yb(Ba,Sr)2Cu4O8	Yb1Ba1.2Sr0.8Cu4O8	Yb	1	Ba	1.2	Sr	0.8	Cu	4													O	8		2	1992																											3	Y124				3.794	3.851	27.007													76	80	81				80																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3726	PHC1990177	NEARLY SINGLE PHASE	(Yb,Ca)(Ba,Sr)2Cu4O8	Yb0.9Ca0.1Ba1.8Sr0.2Cu4O8	Yb	0.9	Ca	0.1	Ba	1.8	Sr	0.2	Cu	4											O	8		1	1992																											3	Y124				3.814	3.854	27.128													86	87	88				87																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3727	PHC1990177		(Yb,Ca)(Ba,Sr)2Cu4O8	Yb0.9Ca0.1Ba1.6Sr0.4Cu4O8	Yb	0.9	Ca	0.1	Ba	1.6	Sr	0.4	Cu	4											O	8		1	1992																											3	Y124				3.805	3.851	27.076													85	86	87				86																																																																			1.37			TP3727																															"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3728	PHC1990177		(Yb,Ca)(Ba,Sr)2Cu4O8	Yb0.9Ca0.1Ba1.4Sr0.6Cu4O8	Yb	0.9	Ca	0.1	Ba	1.4	Sr	0.6	Cu	4											O	8		1	1992																											3	Y124				3.8	3.851	27.046													83	85	86				85																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3729	PHC1990177	Y124+OTHER PHASES	(Yb,Ca)(Ba,Sr)2Cu4O8	Yb0.9Ca0.1Ba1.2Sr0.8Cu4O8	Yb	0.9	Ca	0.1	Ba	1.2	Sr	0.8	Cu	4											O	8		2	1992																											3	Y124				3.798	3.85	27.036													80	84	85				84																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3730	PHC1990177	Y124+OTHER PHASES	(Yb,Ca)(Ba,Sr)2Cu4O8	Yb1Ca0.2Ba1.6Sr0.4Cu4O8	Yb	1	Ca	0.2	Ba	1.6	Sr	0.4	Cu	4											O	8		2	1992																											3	Y124				3.809	3.852	27.106													86	86	87				86																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3731	PHC1990177	Y124+OTHER PHASES	(Yb,Ca)(Ba,Sr)2Cu4O8	Yb1Ca0.4Ba1.6Sr0.4Cu4O8	Yb	1	Ca	0.4	Ba	1.6	Sr	0.4	Cu	4											O	8		2	1992																											3	Y124				3.809	3.852	27.106													84	85	87				85																																																																																																					"PREPARATION AND PROPERTIES OF CA-DOPED ""YB-124"" SUPERCONDUCTORS"	199208			PHYSICA C,199(1992)177	AKIKO NARA,H.YAMAUCHI,KIYOTAKA MATSUURA,SATOSHI TAKANO,SEIJI ADACHI,YUJI YAEGASHI	CA,YB,BA,SR,CU,O	
3732	PR0469250	COUNTER ELECTRODE=PB FILM,ANOTHER PEAK=+-5MEV	YBa2(Cu,Fe)O7	Y1Ba2Cu2.88Fe0.12O7	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7		3	1992																											2	Y123				3.866		11.729														57					57																																															25	5.09	1																																														9						TUNNELING SPECTROSCOPY OF FE-DOPED YBA2CU3O7 SINGLE CRYSTALS	199210		DEPARTIMENTO DI FISICA, UNIVERSITA DI SALERNO, ITALY	PHYS.REV.B,46(1992)9250	A.M.CUCOLO,A.NIGRO,F.LICCI,R.DI LEO	Y,BA,CU,O,FE	
3733	PR0469116		La(2-x)Ca(1+x)Cu2O6	La1.9Ca1.1Cu2O6+Z	La	1.9	Ca	1.1	Cu	2															O	6+Z		1	1992																												2126																				42.5					42.5																																																																																														LA2O3,CACO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400 ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3734	PR0469116		La(2-x)Ca(1+x)Cu2O6	La1.85Ca1.15Cu2O6+Z	La	1.85	Ca	1.15	Cu	2															O	6+Z		1	1992																												2126																				48					48																																																																																														LA2O3,CACO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400 ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3735	PR0469116		La(2-x)Ca(1+x)Cu2O6	La1.82Ca1.18Cu2O6+Z	La	1.82	Ca	1.18	Cu	2															O	6+Z		1	1992			EMU.K/MOLE			0.63	-141																					2126																			49	50	60				50																																																																																														LA2O3,CACO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400 ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3736	PR0469116		La(2-x)Ca(1+x)Cu2O6	La1.75Ca1.25Cu2O6+Z	La	1.75	Ca	1.25	Cu	2															O	6+Z		1	1992																												2126																				51					51																																																																																														LA2O3,CACO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400 ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3737	PR0469116		(La,Sr)2CaCu2O6	La1.9Sr0.1Ca1Cu2O6.03	La	1.9	Sr	0.1	Ca	1	Cu	2													O	6+Z	6.03	1	1992																												2126																				43					43																																																																																														LA2O3,CACO3,SRCO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3738	PR0469116		(La,Sr)2CaCu2O6	La1.85Sr0.15Ca1Cu2O6.03	La	1.85	Sr	0.15	Ca	1	Cu	2													O	6+Z	6.03	1	1992																												2126																				47.5					47.5																																																																																														LA2O3,CACO3,SRCO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3739	PR0469116		(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O6.03	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6+Z	6.03	1	1992																												2126																				51					51																																																																																														LA2O3,CACO3,SRCO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3740	PR0469116		(La,Sr)2CaCu2O6	La1.77Sr0.23Ca1Cu2O6.03	La	1.77	Sr	0.23	Ca	1	Cu	2													O	6+Z	6.03	1	1992																												2126																				51.5					51.5																																																																																														LA2O3,CACO3,SRCO3,CUO	0	SIN(1050-1080C 50H IN AIR 1-8ATM)-SIN(20%O2+80%AR 50-2000ATM) USING HIP,SYNTHESIZED UNDER 400ATM O2					SUPERCONDICTIVITY AND ANTIFERROMAGNETISM IN LA2-XCA1-XCU2O6+-ZAND LA2-XSRXCACU2O6+-Z	199210		NTT BASIC RESEARCH LABORATORIES, TOKYO	PHYS.REV.B,46(1992)9116	K.KINOSHITA,T.YAMADA	LA,CA,CU,O,SR	
3741	SSC0691097	1.7*0.37*0.03 MM3	YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6.8	6.8	3	1989																											3	Y123																				84					84																																																																			12			TP3741																0.0000000022				7.5	RH3741										HALL EFFECT AND THERMOELECTRIC POWER OF AN YBa2Cu3O6.8 SINGLE CRYSTAL			Centre d'Etudes Nucle'aires, De'partement de Recherche Fondamentale BP 85 x-38041 GRENOBLE Cedex-France	Solid State Commun.,69(1989)1097-1101	C. AYACHE,J.Y. HENRY,L. FORRO,M. RAKI		
3742	SSC0691093		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+Z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z		1	1989																											3	Bi2201				5.411	5.378	24.41													17	27	36	29			27										20																																																																																				SRCO3,BI2O3,LA2O3,CUO	1	SIN(920C)-ANN(800C 1DAY IN O2)-FC					SUPERCONDUCTING PHASES IN THE SERIES Bi2Sr2-xLaxCuO6+d  (0< x <1)			Laboratoire de chimie du Solide du CNRS, 351,Cours de la Libe'ration Universite' de BORDEAUXI, 33405 TALENCE Cedex, France	Solid State Commun.,69(1989)1093-1096	B. Chevalier,C.J.P. Soethout,J. Darriet,J. Etourneau		
3743	SSC0691079	POSSIBILITY THAT ZN IS SUBSTITUTED ON CU SITE	(Y,Zn)Ba2Cu3O7	Y0.9Zn0.1Ba2Cu3O7	Y	0.9	Zn	0.1	Ba	2	Cu	3													O	7			1989																												Y123																			50.6	54.9	58.1				54.9																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3744	SSC0691079		(Y,Zn)Ba2Cu3O7	Y0.8Zn0.2Ba2Cu3O7	Y	0.8	Zn	0.2	Ba	2	Cu	3													O	7			1989																												Y123																			33.1	43	50.6				43																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3745	SSC0691079		(Y,Zn)Ba2Cu3O7	Y0.7Zn0.3Ba2Cu3O7	Y	0.7	Zn	0.3	Ba	2	Cu	3													O	7			1989																												Y123																			11.3	23.5	33.1				23.5																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3746	SSC0691079		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989																												Y123																				92.1					92.1																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3747	SSC0691079		(Y,Cd)Ba2Cu3O7	Y0.9Cd0.1Ba2Cu3O7	Y	0.9	Cd	0.1	Ba	2	Cu	3													O	7		1	1989																												Y123																				89.9					89.9																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3748	SSC0691079		(Y,Cd)Ba2Cu3O7	Y0.8Cd0.2Ba2Cu3O7	Y	0.8	Cd	0.2	Ba	2	Cu	3													O	7		1	1989																												Y123																				92.8					92.8																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3749	SSC0691079		(Y,Cd)Ba2Cu3O7	Y0.7Cd0.3Ba2Cu3O7	Y	0.7	Cd	0.3	Ba	2	Cu	3													O	7		1	1989																												Y123																				92.8					92.8																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3750	SSC0691079		(Y,Cd)Ba2Cu3O7	Y0.6Cd0.4Ba2Cu3O7	Y	0.6	Cd	0.4	Ba	2	Cu	3													O	7		1	1989																												Y123																				91.7					91.7																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3751	SSC0691079		(Y,Cd)Ba2Cu3O7	Y0.5Cd0.5Ba2Cu3O7	Y	0.5	Cd	0.5	Ba	2	Cu	3													O	7		1	1989																												Y123																				93.2					93.2																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3752	SSC0691079	IMPURITY=BACUO2	(Y,Cd)Ba2Cu3O7	Y0.4Cd0.6Ba2Cu3O7	Y	0.4	Cd	0.6	Ba	2	Cu	3													O	7		2	1989																												Y123																				91.7					91.7																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3753	SSC0691079	IMPURITY=BACUO2	(Y,Cd)Ba2Cu3O7	Y0.3Cd0.7Ba2Cu3O7	Y	0.3	Cd	0.7	Ba	2	Cu	3													O	7		2	1989																												Y123																			82.9	87	90.6				87																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3754	SSC0691079	IMPURITY=BACUO2	(Y,Cd)Ba2Cu3O7	Y0.25Cd0.75Ba2Cu3O7	Y	0.25	Cd	0.75	Ba	2	Cu	3													O	7		2	1989																												Y123																			29.7	53.2	74.5				53.2																																																																																														Y2O3,BACO3,CUO,ZNO,CDO	1	SIN(900C 1DAY)-ANN(850-930C 24H IN O2)-SLOW COOL(IN O2)					Superconductivity in (Y1-xMx)Ba2Cu3O7-delta(M=Cd and Zn)Systems			Department of Physics National Taiwan University Taipei, Taiwan, Republic of China	Solid State Commun.,69(1989)1079-1083	C.F. Chen,J.W. Chen		
3755	SSC0690867	STABLE FOR LOW TEMP.(77-200K) CYCLE	(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			132						132																																																																																														BI2O3,PBO,SB2O5,SRCO3,CACO3,CUO	1	SIN(820C 12H IN AIR)-SIN(865C 60H IN AIR)-Q					Zero Resistance at 132K in the Multiphase System of Bi1,9-xPbxSb0.1Sr2Ca2Cu3Oy with x=0.3,0.4			Department of Physics, University of Science and Technology of China, Hefei, Anhui, P.R. China	Solid State Commun.,69(1989)867-868	Cao Liezhao,Chen Zhaojia,Li Xiaoxian,Liu Hongbao,Mao Xianglei,Mao Zhiqiang,Run Yaozhong,Xue Bai,Yu Zhidong,Zhang Yuheng,Zhou Guien,Zhou Ling		
3756	SSC0690867		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.5Pb0.4Sb0.1Sr2Ca2Cu3OZ	Bi	1.5	Pb	0.4	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z		2	1989																												Bi2223																			132						132																																																																																														BI2O3,PBO,SB2O5,SRCO3,CACO3,CUO	1	SIN(820C 12H IN AIR)-SIN(865C 60H IN AIR)-Q					Zero Resistance at 132K in the Multiphase System of Bi1,9-xPbxSb0.1Sr2Ca2Cu3Oy with x=0.3,0.4			Department of Physics, University of Science and Technology of China, Hefei, Anhui, P.R. China	Solid State Commun.,69(1989)867-868	Cao Liezhao,Chen Zhaojia,Li Xiaoxian,Liu Hongbao,Mao Xianglei,Mao Zhiqiang,Run Yaozhong,Xue Bai,Yu Zhidong,Zhang Yuheng,Zhou Guien,Zhou Ling		
3757	SSC0690739	SEMICON	Bi2MLaCuO6.5	Bi2Ca1La1Cu1O6.5	Bi	2	Ca	1	La	1	Cu	1													O	6.5			1989									7.12																		3					5.451	5.412	23.64																	4.2																																																																																																	1	SIN(920C 16H IN AIR)-SLOW COOL					NEW SERIES OF COMPOUNDS Bi2AlaCuO6.5(A=Ca,Sr, or Ba) ISOSTRUCTURAL TO THE SUPERCONDUCTING PHASE Bi2Sr2CuO6			Laboratoire de Chimie du Solide du CNRS, 351, cours de la Libe'ration Universite' de BORDEAUX I, 33405 TALENCE Cedex, France	Solid State Commun.,69(1989)739-742	A. Le Lirzin,B. Chevalier,B. Lepine,E. Marquestaut,J. Darriet,J. Etourneau		
3758	SSC0690739	SEMICON	Bi2MLaCuO6.5	Bi2Sr1La1Cu1O6.5	Bi	2	Sr	1	La	1	Cu	1													O	6.5			1989																											3					5.459	5.432	23.92																	4.2																																																																																																	1	SIN(920C 16H IN AIR)-SLOW COOL					NEW SERIES OF COMPOUNDS Bi2AlaCuO6.5(A=Ca,Sr, or Ba) ISOSTRUCTURAL TO THE SUPERCONDUCTING PHASE Bi2Sr2CuO6			Laboratoire de Chimie du Solide du CNRS, 351, cours de la Libe'ration Universite' de BORDEAUX I, 33405 TALENCE Cedex, France	Solid State Commun.,69(1989)739-742	A. Le Lirzin,B. Chevalier,B. Lepine,E. Marquestaut,J. Darriet,J. Etourneau		
3759	SSC0690739	SEMICON	Bi2MLaCuO6.5	Bi2Ba1La1Cu1O6.5	Bi	2	Ba	1	La	1	Cu	1													O	6.5			1989																											3					5.553	5.477	24.006																	4.2																																																																																																	1	SIN(850C 16H IN AIR)-SLOW COOL					NEW SERIES OF COMPOUNDS Bi2AlaCuO6.5(A=Ca,Sr, or Ba) ISOSTRUCTURAL TO THE SUPERCONDUCTING PHASE Bi2Sr2CuO6			Laboratoire de Chimie du Solide du CNRS, 351, cours de la Libe'ration Universite' de BORDEAUX I, 33405 TALENCE Cedex, France	Solid State Commun.,69(1989)739-742	A. Le Lirzin,B. Chevalier,B. Lepine,E. Marquestaut,J. Darriet,J. Etourneau		
3760	SSC0690379		(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1989					/PR ION																						3	Y123																				95.5		96			95.5																																																									8.68																					0.13				0.39												PR6O11	1	SIN(950-980C)					DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3761	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7		1	1989					/PR ION	2.39																					3	Y123																				84.1		88.2			84.1																																																									34.3																																					PR6O11	1	SIN(950-980C)					DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3762	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1989					/PR	2.55																					3	Y123																			73.5	75.8	78.8	82.1			75.8																																																									67.4																					0.46				1.19												PR6O11	1	SIN(950-980C)					DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3763	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1989					/PR	2.63																					3	Y123																			56.4	59.2	62.8	70.3			59.2																																																									110.3																																					PR6O11	1	SIN(950-980C)					DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3764	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1989					/PR	2.58																					3	Y123																				48.7	54.2	46.5			48.7																																																									162.4																					0.78				1.28												PR6O11	1	SIN(950-980C)					DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3765	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1989					/PR	2.39																					3	Y123																			24.6	28.5		35.1			28.5																																																									231.8																					1.81				2.03													1						DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3766	SSC0690379		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O7	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1989					/PR	2.76																					3	Y123																																																																																		282			C=A*T+B*T(3)																																			1						DEPRESSION OF SUPERCONDUCTIVITY, HEAVY FERMION BEHAVIOR AND VALENCE FLUCTUATIONS IN Y1-xPrxba2Cu3O7			Center for Materials Reserch, Temple University, Philadelphia, PA 19122, USA	Solid State Commun.,69(1989)379-384	A. Kabede,Chan-Soo Jee,D. Nichols,G.H. Myer,I. Perez,J.E. Crow,P. Schlottmann,R.E. Salomon,T. Mihalisin		
3767	SSC0690387	DHC1/DP=3 OE/KBAR AT 4.2K,DHC2/DP=1.3 KOE/KBAR AT 25K	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1989																												T																					32.5				32.5			K/KBAR	0.17																																																																																																	EFFECT OF PRESSURE ON CRITICAL FIELDS AND Tc OF La1.8Sr0.2CuO4 AND YBa2Cu3O7 HIGH-Tc CERAMICS			Institute for High Pressure Physics, USSR Academy of Sciences, Troisk, Moscow region, 142092, USSR	Solid State Commun.,69(1989)387-389	A.G. Gapotchenko,E.S. Itskevich,S.L. Bud'ko		
3768	SSC0690387	DHC1/DP=0 OE/KBAR AT 10K,DHC2/DP=1.3 KOE/KBAR AT 80K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1989																												Y123																					88.9				88.9			K/KBAR	0.22																																																																																																	EFFECT OF PRESSURE ON CRITICAL FIELDS AND Tc OF La1.8Sr0.2CuO4 AND YBa2Cu3O7 HIGH-Tc CERAMICS			Institute for High Pressure Physics, USSR Academy of Sciences, Troisk, Moscow region, 142092, USSR	Solid State Commun.,69(1989)387-389	A.G. Gapotchenko,E.S. Itskevich,S.L. Bud'ko		
3769	SSC0690387		YBa2Cu3O7(H)	Y1Ba2Cu3H0.2O7-Z	Y	1	Ba	2	Cu	3	H	0.2													O	7-Z			1989																											3	Y123																				92					92																																										PROTON NMR	2500																																																			Y2O3,BA(OH)2.H2O,CUO	1	CAL(950C 20H IN AIR)-ANN(900C 10H IN O2)-ANN(400C)-Q(TO RT)					EFFECT OF PRESSURE ON CRITICAL FIELDS AND Tc OF La1.8Sr0.2CuO4 AND YBa2Cu3O7 HIGH-Tc CERAMICS			Institute for High Pressure Physics, USSR Academy of Sciences, Troisk, Moscow region, 142092, USSR	Solid State Commun.,69(1989)387-389	A.G. Gapotchenko,E.S. Itskevich,S.L. Bud'ko		
3770	SSC0701151	PRESSURE GENERATED BY WC PISTON, TC BY RESISTANCE. structural phase transition temperature T0, dT0/dP = 5 K/kbar.  	(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1989																												T																			12						12																																																																																														LA2O3,BACO3,CUO	1	CAL(1050C 10H IN O2)-SIN(1050C4H)-COOL(1.5C/MIN)TO 500C-ANN(500C 24H)					PRESSURE EFFECT ON THE LOW TEMPERATURE TETRAGONAL PHASE AND THE SUPERCONDUCTIVITY IN (LA1-XBAX)2CUO4				SOLID STATE COMMUN.,70(1989)1151	K.YAMAYA,M.IDO,M.ODA,N.YAMADA,Y.OKAJIMA	LA,BA,CU,O	
3771	SSC0701141	four samples (average oxygen isotope mass: M=16.00, 16.61, 17.23, 17.84) are measured.	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4			1989																												T'																		K				23.6			23.6						0.15	O																																																																																									synthsized using Nd2<18>O3, Cu<18>O.					OXYGEN ISOTOPE EFFECT OF SUPERCONDUCTING (ND1-XCEX)2CUO4-Z SYSTEM				SOLID STATE COMMUN.,70(1989)1141	MASASHIGE ONODA,MASATOSHI SATO,SHINJI KONDOH	ND,CE,CU,O	
3772	SSC0701055	POINT CONTACT, GAP(C)=12MEV,2*GAP(C)/KTC=3.3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1989																												Bi2212																				85					85																																														MEV	23	6.2	1																																														0						TUNNELING SPECTROSCOPY IN BI2SR2CACU2O8: IS THE ENERGY GAP ANISOTROPIC?				SOLID STATE COMMUN.,70(1989)1055	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
3773	SSC0700287		(Bi,Pb)2Sr2Ca3Cu4OZ	Pb0.3Bi1.7Sr2Ca3Cu4OZ	Pb	0.3	Bi	1.7	Sr	2	Ca	3	Cu	4											O	Z		1	1989																											3	Bi2234				5.418	5.346	37.1													107	110					110													900									184									2.43							13.5					880							48000																																												PBO,BI2O3,SRCO3,CACO3,CUO	1	CAL(800C 12H)-SIN(870C 60H IN AIR)-ANN(880C 180H)					Properties of 107K supercomducting single phase in PbBiSrCaCu oxide			Institute of Physics, Academia Sinica, Beijing, China	Solid State COmmun.,70(1989)287-289	C.G. Cui,F. Shi,J. Dou,J. Li,J.L. Zhang,S.L. Li,S.Z. Zhou,Z.H. Shi		
3774	SSC0700145		(Nd,Th)2CuO4	Nd1.85Th0.15Cu1O4-Z	Nd	1.85	Th	0.15	Cu	1															O	4-Z			1989									7.5																			T*																				16		17		4	16										4																																																																																				ND2O3,CEO2,THO2,CUO	0	SIN(900C 20H IN AIR)-(1100C 16H)-Q TO RT IN AIR-ANN(910C IN HE)-Q					HIGH TEMPERATURE SUPERCONDUCTIVITY IN Th-DOPED Nd2CuO4-y			Department of Physics and Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun.,70(1989)145-147	J.T. Markert,M.B. Maple		
3775	SSC0700129		(Bi,Pb)4Sr3Ca3Cu4OZ	Bi3Pb1Ca3Sr3Cu4OZ	Bi	3	Pb	1	Ca	3	Sr	3	Cu	4											O	Z			1989																												Bi4334																			103			105			105																																																																																											RH3775				0						Pculiar Behavior of Hall Effect on single-Phase Bi3PbCa3Sr3 cu4Oy			Department of Physics, University of Science and Technology of China, Hefei, China	Solid State Commun.,70(1989)129-131	Cao Liezhao,Chen Xianhui,Chen Zuyao,Fang Minghu,He zhenhui,Qian Yitai,Wang Shunxi,Xia Jiansheng,Zhang Qirui		
3776	SSC0710663		Bi2M3Co2OZ	Bi2Ca3Co2OZ	Bi	2	Ca	3	Co	2															O	Z			1989																																																			4.2																																																																																																	1	ANN(1200C 1.5H)-C(8C/H) TO 800C					NEW NON-SUPERCONDUCTING LAYERED Bi-OXIDEPHASES OF FORMULA Bi2M3Co2Oy CONTAINING Co INSTEAD OF Cu			Bellcore, Red Bank, New Jerscy 07701	Solid State Commun.,71(1989)663-668	G.W. Hull,J.-M. Trascon,J.V. Waszcak,L.F. Schnccmeyer,M.S. Hcdge,P. Barboux,R. Ramcsh,W.R. McKinnon,Y. LePage		
3777	SSC0710663		Bi2M3Co2OZ	Bi2Sr3Co2OZ	Bi	2	Sr	3	Co	2															O	Z			1989																																																			4.2																																																																																																	1	ANN(1000C 2H)-C(6C/H) TO 700C					NEW NON-SUPERCONDUCTING LAYERED Bi-OXIDEPHASES OF FORMULA Bi2M3Co2Oy CONTAINING Co INSTEAD OF Cu			Bellcore, Red Bank, New Jerscy 07701	Solid State Commun.,71(1989)663-668	G.W. Hull,J.-M. Trascon,J.V. Waszcak,L.F. Schnccmeyer,M.S. Hcdge,P. Barboux,R. Ramcsh,W.R. McKinnon,Y. LePage		
3778	SSC0710663		Bi2M3Co2OZ	Bi2Ba3Co2OZ	Bi	2	Ba	3	Co	2															O	Z			1989																																																			4.2																																																																																																	1	ANN(1150C 2.5H)-C(8C/H) TO 750C					NEW NON-SUPERCONDUCTING LAYERED Bi-OXIDEPHASES OF FORMULA Bi2M3Co2Oy CONTAINING Co INSTEAD OF Cu			Bellcore, Red Bank, New Jerscy 07701	Solid State Commun.,71(1989)663-668	G.W. Hull,J.-M. Trascon,J.V. Waszcak,L.F. Schnccmeyer,M.S. Hcdge,P. Barboux,R. Ramcsh,W.R. McKinnon,Y. LePage		
3779	SSC0710419		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.90	6.9	1	1989									5.6																		3	Y123				3.822	3.88	11.66														89.6				4	89.6																																																														5.29			THC3779																	1.1													1						FIVIDENCE FOR HYSTERESIS BEHAVIOUR AND ANOMALY OF THERMAL CONDUCTIVITY IN Y-Ba-Cu-O SUPERCONDUCTOR			Institute for Low Temperature and Structure Research, Polish Academy of Sciences, 2 Oko lna str., 50-422 Wrociaw, Poland	Solid State Commun.,71(1989)419-424	A. Jez'owski		
3780	SSC0710419		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	1	1989									5.45																		3	Y123				3.816	3.99	11.646														91				1.4	91																																																														2.95			THC3780																	1.11													1						FIVIDENCE FOR HYSTERESIS BEHAVIOUR AND ANOMALY OF THERMAL CONDUCTIVITY IN Y-Ba-Cu-O SUPERCONDUCTOR			Institute for Low Temperature and Structure Research, Polish Academy of Sciences, 2 Oko lna str., 50-422 Wrociaw, Poland	Solid State Commun.,71(1989)419-424	A. Jez'owski		
3781	SSC0710419		CuO	Cu1O	Cu	1																			O				1989								225																																																																																																											12.4			THC3781																														1						FIVIDENCE FOR HYSTERESIS BEHAVIOUR AND ANOMALY OF THERMAL CONDUCTIVITY IN Y-Ba-Cu-O SUPERCONDUCTOR			Institute for Low Temperature and Structure Research, Polish Academy of Sciences, 2 Oko lna str., 50-422 Wrociaw, Poland	Solid State Commun.,71(1989)419-424	A. Jez'owski		
3782	SSC0710739		R2Tl2Sr2Cu3O11	La2Tl2Sr2Cu3O11	La	2	Tl	2	Sr	2	Cu	3													O	11		1	1989																											2					3.775		35.35													34	37	41				37																																																																																														TL2O3,SRO,CUO,R2O3	1	MIXTURE PELLET HEATED(930C 3-5MIN) IN TUBE IN O2-FC					SUPERCONDUCTIVITY IN THE R-Tl-Sr-Cu-O SYSTEM WITH R= RARE EARTHS			Department of Physics, University of Arkansas, Fayetteville, AR 72701, USA	Solid State Commun.,71(1989)739-741	C. Dong,J.H. Wang,L. Sheng,X. Fei,Y.H. Liu,Z.Z. Sheng		
3783	SSC0710739		R2Tl2Sr2Cu3O11	Pr2Tl2Sr2Cu3O11	Pr	2	Tl	2	Sr	2	Cu	3													O	11		1	1989																											2					3.762		35.34													37	43	46				43																																																																																														TL2O3,SRO,CUO,R2O3	1	MIXTURE PELLET HEATED(930C 3-5MIN) IN TUBE IN O2-FC					SUPERCONDUCTIVITY IN THE R-Tl-Sr-Cu-O SYSTEM WITH R= RARE EARTHS			Department of Physics, University of Arkansas, Fayetteville, AR 72701, USA	Solid State Commun.,71(1989)739-741	C. Dong,J.H. Wang,L. Sheng,X. Fei,Y.H. Liu,Z.Z. Sheng		
3784	SSC0710739		R2Tl2Sr2Cu3O11	Nd2Tl2Sr2Cu3O11	Nd	2	Tl	2	Sr	2	Cu	3													O	11		1	1989																																															25	44	65				44																																																																																														TL2O3,SRO,CUO,R2O3	1	MIXTURE PELLET HEATED(930C 3-5MIN) IN TUBE IN O2-FC					SUPERCONDUCTIVITY IN THE R-Tl-Sr-Cu-O SYSTEM WITH R= RARE EARTHS			Department of Physics, University of Arkansas, Fayetteville, AR 72701, USA	Solid State Commun.,71(1989)739-741	C. Dong,J.H. Wang,L. Sheng,X. Fei,Y.H. Liu,Z.Z. Sheng		
3785	SSC0710739		R2Tl2Sr2Cu3O11	Y2Tl2Sr2Cu3O11	Y	2	Tl	2	Sr	2	Cu	3													O	11		1	1989																																																	45		15		45																																																																																														TL2O3,SRO,CUO,R2O3	1	MIXTURE PELLET HEATED(930C 3-5MIN) IN TUBE IN O2-FC					SUPERCONDUCTIVITY IN THE R-Tl-Sr-Cu-O SYSTEM WITH R= RARE EARTHS			Department of Physics, University of Arkansas, Fayetteville, AR 72701, USA	Solid State Commun.,71(1989)739-741	C. Dong,J.H. Wang,L. Sheng,X. Fei,Y.H. Liu,Z.Z. Sheng		
3786	SSC0651333	C-AXIS ORIENTED GRAIN,THERMOPOWER IS // TO AB-PLANE,VALUES ARE FOR // TO THE PRESSING DIRECTION	EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z		1	1988																											3	Y123				3.82	3.884	11.681													76.9	85.1	95.3				85.1																																																																						TP3786								61																	1	CAL(930C)-COOL TO 550C-Q IN AIR					STRUCTURAL AND ELECTRONIC ANISOTROPY IN POLYCRYSTALLINE COMPACTIONS OF THE HIGH-Tc SUPERCONDUCTOR EuBa2Cu3O7-delta			Department of Chemistry and the Materials Research Center, Northwestern University, Evanston, IL 60208, USA	Solid State Commnu.,65(1988)1333-1337	C.R. Kannewurf,H.O. Marcy,M.G. Kanatzidis,T.J. Marks,W.J. McCarthy		
3787	SSC0651001	BACUO2,CUO,BACO3=IMPURITY	(Y,Na)Ba2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1988		-90780000000000000000000000000					4.41																				3	Y123																				90.6					90.6																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3788	SSC0651001		(Y,Na)Ba2Cu3O7	Y0.9Na0.1Ba2Cu3OZ	Y	0.9	Na	0.1	Ba	2	Cu	3													O	Z		1	1988							24.22																				3	Y123																				90.2					90.2																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3789	SSC0651001		(Y,Na)Ba2Cu3O7	Y0.8Na0.2Ba2Cu3OZ	Y	0.8	Na	0.2	Ba	2	Cu	3													O	Z		1	1988							29.04																				3	Y123																			84.9	89.5	90.6				89.5																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3790	SSC0651001		(Y,Na)Ba2Cu3O7	Y0.7Na0.3Ba2Cu3OZ	Y	0.7	Na	0.3	Ba	2	Cu	3													O	Z		1	1988																											3	Y123																			69.6	81.8	88.3				81.8																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3791	SSC0651001		(Y,Na)Ba2Cu3O7	Y0.6Na0.4Ba2Cu3OZ	Y	0.6	Na	0.4	Ba	2	Cu	3													O	Z		1	1988																											3	Y123																			43.6	52.8	61.6				52.8																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3792	SSC0651001		(Y,Na)Ba2Cu3O7	Y0.5Na0.5Ba2Cu3OZ	Y	0.5	Na	0.5	Ba	2	Cu	3													O	Z		1	1988																											3	Y123																			23.7	41.3	56.6				41.3																																																																																														Y2O3,NACO3,CUO	1	CAL(800C 3H IN AIR)-ANN(900C IN AIR)-ANN(950C 18H IN O2)-COOL TO RT WITHIN 9H					SUPERCONDUCTING AND NORMAL STATE PROPERTIES OF Y1-XMXBA2CU3O7-Z (M=PR,NA)				SOLID STATE COMMUN.,65(1988)1001	B.W.LEE,C.L.SEAMAN,E.A.EARLY,H.ZHOU,K.N.YANG,M.B.MAPLE,M.S.TORIKACHVILI,Y.DALICHAOUCH	Y,PR,NA,CU,O,BA	
3793	SSC0650973		YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7-Z	Y	1	Ba	2	Cu	2.88	Co	0.12													O	7-Z			1988									6.46																		2	Y123	PMM2								E-6%	8.3		1.97								84				8	84										44																																																																																				Y2O3,BACO3,CUO,CO3O4	1	CAL(950C IN AIR)-SIN(950C 12H IN O2)-C TO RT WITHIN 5H					BULK SUPERCONDUCTIVITY AT 70 K IN TETRAGONAL YBA2(CU0.96CO0.04)3O7-Y				SOLID STATE COMMUN.,65(1988)973	A.ERLE,E.ZIRNGIEBL,H.-D.JOSTARNDT,H.SCHMIDT,J.LANGEN,M.GALFFY,M.VEIT,S.BLUMENRODER	Y,BA,CU,CO,O	
3794	SSC0650849	GRAIN SIZE =10 MICRON	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1988																												T																				37.1					37.1										20			250																		1.84							30					2600																																			0.14																SRCO3,LACO3,CU-NITRATE	0	DISSOLVING IN NITRIC ACID-DECOMPOSED AT 600C-SIN(900C 54H,950C 24H)-SIN(1000C 38H IN O2)-FAST COOL IN O2					SUPERCONDUCTNG AND NORMAL STATEPROPERTIES OF Sr0.5La1.85CuO4 DETERMINED FROM MAGNETIZATION MEASUREMENTS			Department of Physics, Brock University St. Cctharines, Ontario, Canada L2S 3AI	Solid State Commun.,65(1988)849-853	B. Mitrovic',F.P. Koffyberg,F.S. Razavi,P.N. Arberg		
3795	SSC0650333		DyBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z		1	1988			EMU/K.OE	0.0193	/CELL	10.68	-8.4																				3	Y123				3.849	3.889	11.739																													33		DEVIATION FROM LINEAR MAGNETIZATION	500								RESISTIVE TRANSITION,WHH THEORY	103									1.6						FROM HC2(O)	10.4					735																																			0.208																	1						THE MAGNETIC AND SUPERCONDUCTING PROPERTIES OF DyBa2Cu3O7-x			Institute of Physics, Chinese Academy of Sciences, Beijing, China	Solid State Commun.,65(1988)333-337	Cao Ning,Chen Xichen,Guan Weiyan,Zheng Jiaqi		
3796	SSC0651529		CuO	Cu1O1	Cu	1																			O	1			1988																																																																																																										SP3796																																										1	MIXTURE HEATED (950C 2DAYS IN AIR)					ORIGIN OF THE RESIDUAL LINEAR SPECIFIC HEAT TERM IN YBa2Cu3O7-x			I.P.C.M.S. 1. L.M.S.E.S. LA 306 Du CNRS, 3 rue de 1' Universite', 67084 STRASBOURG (France)	Solid State Commun.,65(1988)1529-1530	R. KUENTZLER,S. VILMINOT,S.EL HADIGUI,Y. DOSSMANN		
3797	SSC0651529		Y2BaCuO5	Y2Ba1Cu1O5	Y	2	Ba	1	Cu	1															O	5			1988																											3																																																																															SP3797																																										1	MIXTURE HEATED (950C 2DAYS IN AIR)					ORIGIN OF THE RESIDUAL LINEAR SPECIFIC HEAT TERM IN YBa2Cu3O7-x			I.P.C.M.S. 1. L.M.S.E.S. LA 306 Du CNRS, 3 rue de 1' Universite', 67084 STRASBOURG (France)	Solid State Commun.,65(1988)1529-1530	R. KUENTZLER,S. VILMINOT,S.EL HADIGUI,Y. DOSSMANN		
3798	SSC0651529		Y2CuO5	Y2Cu5O5	Y	2	Cu	5																	O	5			1988																																																																																																										SP3798																																										1	MIXTURE HEATED (950C 2DAYS IN AIR)					ORIGIN OF THE RESIDUAL LINEAR SPECIFIC HEAT TERM IN YBa2Cu3O7-x			I.P.C.M.S. 1. L.M.S.E.S. LA 306 Du CNRS, 3 rue de 1' Universite', 67084 STRASBOURG (France)	Solid State Commun.,65(1988)1529-1530	R. KUENTZLER,S. VILMINOT,S.EL HADIGUI,Y. DOSSMANN		
3799	SSC0651339		(Y,Gd)Ba2Cu3O7	Y1Gd0.5Ba2Cu3OZ	Y	1	Gd	0.5	Ba	2	Cu	3													O	Z			1988			EMU/G				-1.1																					Y123																																																																																																																							GD2O3,Y2O3,BACO3,CUO	0	ANN(900C 10H IN AIR)-Q TO LN2					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3800	SSC0651339		(Y,Gd)Ba2Cu3O7	Y1Gd0.8Ba2Cu3OZ	Y	1	Gd	0.8	Ba	2	Cu	3													O	Z			1988							-1.92	1.93																				Y123																																																																																																																							GD2O3,Y2O3,BACO3,CUO	0	ANN(900C 10H IN AIR)-Q TO LN2					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3801	SSC0651339		(Y,Gd)Ba2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z			1988			EMU/G				-2.7	2.37																				Y123																																																																																																																							GD2O3,Y2O3,BACO3,CUO	0	ANN(900C 10H IN AIR)-Q TO LN2					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3802	SSC0651339		(Y,Gd)Ba2Cu3O7	Y0.7Gd0.3Ba2Cu3OZ	Y	0.7	Gd	0.3	Ba	2	Cu	3													O	Z			1988			EMU/G																									Y123																			93						93																																																																																														GD2O3,Y2O3,BACO3,CUO	0	SIN(950C IN O2)-ANN(800C 10H IN AIR)					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3803	SSC0651339		(Y,Gd)Ba2Cu3O7	Y0.4Gd0.6Ba2Cu3OZ	Y	0.4	Gd	0.6	Ba	2	Cu	3													O	Z			1988			EMU/G																									Y123																			93						93																																																																																														GD2O3,Y2O3,BACO3,CUO	0	SIN(950C IN O2)-ANN(800C 10H IN AIR)					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3804	SSC0651339		(Y,Gd)Ba2Cu3O7	Y0.2Gd0.8Ba2Cu3OZ	Y	0.2	Gd	0.8	Ba	2	Cu	3													O	Z			1988			EMU/G	0.00753				1.8																				Y123																			93						93																																																																																														GD2O3,Y2O3,BACO3,CUO	0	SIN(950C IN O2)-ANN(800C 10H IN AIR)					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3805	SSC0651339		GdBa2Cu3O7	Gd1Ba2Cu3OZ	Gd	1	Ba	2	Cu	3															O	Z			1988			EMU/G					2.27																				Y123																			93						93																																																																																														GD2O3,Y2O3,BACO3,CUO	0	SIN(950C IN O2)-ANN(800C 10H IN AIR)					THE GADOLINIUM ORDERING IN SUPERCONDUCTING AND NON-SUPERCONDUCTING Gdxy1-xBa2Cu3Oy COMPOUNDS			Instittue of Physcs, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Solid State Commun.,65(1988)1339-1341	A. Tominaga,F. Nakanura,M. Akisue,T. Fukuda,T. Uchiyama,Y. Ochiai		
3806	SSC0680827	// CURRENT TO AB-PLANE GIVES HIGHER TC TAN N-CURRENT, SIZE=3X1X1MM3	GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	Z	7	3	1988																												Y123																				78	84				78																																																																																			1.47	36.5		0.00000000133				1	RH3806										Reserch on Anisotropy for Single Craystal GdBa2Cu3O7-y			Deaprtment of Physics, Department of Applied Chemistry, University of Science and Technology of China, Hefei, P.R. China	Solid State Commun.,68(1988)827-829	Chen Zuyao,Fang Minghu,Qian Yitai,Sun Dunming,Xia Jiansheng,Xu Zhuan,Zhang Qirui,Zhao Zhanchun		
3807	SSC0680753	GAPENE=5.4 FOR TC1, =3.9 FOR TC3	YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	Z	6.6	4	1988																												Y123																			68		93				80.5																																																5.4	1																																					0.0000000222				1	RH3807										TUNNELING SPECTROSCOPY IN THIN FILM SUPERCONDUCTING JUNCTTIONS YBCO/Pb			Institute of Electrical Engineering EPRC SAS, 842 39 Bratislava, Czechoslovakia	Solid State Commun.,68(1988)	A. Plecenik,S. Benacka,S. Chromik,S. Gazi,V.M. Svistunov		
3808	PHC1990240		CaBa(La,Eu)Cu3O7	Ca1Ba1La0.8Eu0.2Cu3O7-Z	Ca	1	Ba	1	La	0.8	Eu	0.2	Cu	3											O	7-Z		1	1992																											2	1113				3.866		11.587														69					69																																																																																		8.61																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3809	PHC1990240		CaBa(La,Eu)Cu3O7	Ca1Ba1La0.6Eu0.4Cu3O7-Z	Ca	1	Ba	1	La	0.6	Eu	0.4	Cu	3											O	7-Z		1	1992																											2	1113				3.863		11.573														65					65																																																																																		10.17																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3810	PHC1990240		CaBa(La,Eu)Cu3O7	Ca1Ba1La0.4Eu0.6Cu3O7-Z	Ca	1	Ba	1	La	0.4	Eu	0.6	Cu	3											O	7-Z		1	1992																											2	1113				3.857		11.595														62					62																																																																																		6.92																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3811	PHC1990240		CaBaEuCu3O7	Ca1Ba1Eu1Cu3O7-Z	Ca	1	Ba	1	Eu	1	Cu	3													O	7-Z			1992																												Y123																				53					53																																																																																		31.37																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3812	PHC1990240	NOT SUPERCOND.	CaBaPrCu3O7	Ca1Ba1Pr1Cu3O7-Z	Ca	1	Ba	1	Pr	1	Cu	3													O	7-Z			1992																												1113																							4.2																																																																																				251.4																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3813	PHC1990240		CaBaGdCu3O7	Ca1Ba1Gd1Cu3O7-Z	Ca	1	Ba	1	Gd	1	Cu	3													O	7-Z			1992																												Y123																				49					49																																																																																		89.64																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3814	PHC1990240		CaBa(La,Sm)Cu3O7	Ca1Ba1La0.8Sm0.2Cu3O7-Z	Ca	1	Ba	1	La	0.8	Sm	0.2	Cu	3											O	7-Z		1	1992																											2	1113				3.865		11.637														71					71																																																																																		2.7																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3815	PHC1990240		CaBa(La,Sm)Cu3O7	Ca1Ba1La0.6Sm0.4Cu3O7-Z	Ca	1	Ba	1	La	0.6	Sm	0.4	Cu	3											O	7-Z		1	1992																											2					3.861		11.626														68					68																																																																																		5.81																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3816	PHC1990240		CaBa(La,Sm)Cu3O7	Ca1Ba1La0.4Sm0.6Cu3O7-Z	Ca	1	Ba	1	La	0.4	Sm	0.6	Cu	3											O	7-Z		1	1992																											2					3.859		11.612														64					64																																																																																		4.45																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3817	PHC1990240		CaBa(La,Sm)Cu3O7	Ca1Ba1La0.2Sm0.8Cu3O7-Z	Ca	1	Ba	1	La	0.2	Sm	0.8	Cu	3											O	7-Z		1	1992																											2	1113				3.853		11.613														56					56																																																																																		8.72																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3818	PHC1990240		CaBaSmCu3O7	Ca1Ba1Sm1Cu3O7-Z	Ca	1	Ba	1	Sm	1	Cu	3													O	7-Z			1992																												Y123																				39					39																																																																																		33.39																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3819	PHC1990240		CaBaLaCu3O7	Ca1Ba1La1Cu3O7-Z	Ca	1	Ba	1	La	1	Cu	3													O	7-Z		1	1992																											2	1113				3.871		11.61														72					72																																																																																		1.84																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3820	PHC1990240		CaBa(La,Nd)Cu3O7	Ca1Ba1La0.8Nd0.2Cu3O7-Z	Ca	1	Ba	1	La	0.8	Nd	0.2	Cu	3											O	7-Z		1	1992																											2					3.866		11.606														71					71																																																																																		3.96																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3821	PHC1990240		CaBa(La,Nd)Cu3O7	Ca1Ba1La0.6Nd0.4Cu3O7-Z	Ca	1	Ba	1	La	0.6	Nd	0.4	Cu	3											O	7-Z		1	1992																											2					3.864		11.617														67					67																																																																																		3.52																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3822	PHC1990240		CaBa(La,Nd)Cu3O7	Ca1Ba1La0.4Nd0.6Cu3O7-Z	Ca	1	Ba	1	La	0.4	Nd	0.6	Cu	3											O	7-Z		1	1992																											2					3.86		11.622														63					63																																																																																		4.64																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3823	PHC1990240		CaBa(La,Nd)Cu3O7	Ca1Ba1La0.2Nd0.8Cu3O7-Z	Ca	1	Ba	1	La	0.2	Nd	0.8	Cu	3											O	7-Z		1	1992																											2					3.857		11.628														57					57																																																																																		12.23																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3824	PHC1990240		CaBaNdCu3O7	Ca1Ba1Nd1Cu3O7-Z	Ca	1	Ba	1	Nd	1	Cu	3													O	7-Z		1	1992																											2					3.854		11.629														46					46																																																																																		20.15																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3825	PHC1990240		CaBaDyCu3O7	Ca1Ba1Dy1Cu3O7-Z	Ca	1	Ba	1	Dy	1	Cu	3													O	7-Z			1992																																																65					65																																																																																		95.02																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3826	PHC1990240		CaBaHoCu3O7	Ca1Ba1Ho1Cu3O7-Z	Ca	1	Ba	1	Ho	1	Cu	3													O	7-Z			1992																																																57					57																																																																																		31.6																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3827	PHC1990240		CaBaErCu3O7	Ca1Ba1Er1Cu3O7-Z	Ca	1	Ba	1	Er	1	Cu	3													O	7-Z			1992																																																66					66																																																																																		28.75																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3828	PHC1990240		CaBaTmCu3O7	Ca1Ba1Tm1Cu3O7-Z	Ca	1	Ba	1	Tm	1	Cu	3													O	7-Z			1992																																																67					67																																																																																		32.77																			PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3829	PHC1990240	NOT SUPERCOND.,RESRT>1.0E+6	CaBaYbCu3O7	Ca1Ba1Yb1Cu3O7-Z	Ca	1	Ba	1	Yb	1	Cu	3													O	7-Z			1992																																																																																																																																																										PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
3830	SSC0680239		(Y,Sc)Ba2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1988						0.12	20																					Y123																				90					90																																																																																		1.35																			ANOMALOUS MAGNETIC PROPERTIES OF Y1-XSCXBA2CU3O7-Z				SOLID STATE COMMUN.,68(1988)239	A.CHAKRABORTY,A.J.EPSTEIN,B.R.PATTON,F.ZUO,J.R.GAINES,X.D.CHEN	Y,SC,BA,CU,O	
3831	SSC0680239		(Y,Sc)Ba2Cu3O7	Y0.75Sc0.25Ba2Cu3O7-Z	Y	0.75	Sc	0.25	Ba	2	Cu	3													O	7-Z		1	1988						0.65	36																					Y123																				87					87																																																																																		2.2																			ANOMALOUS MAGNETIC PROPERTIES OF Y1-XSCXBA2CU3O7-Z				SOLID STATE COMMUN.,68(1988)239	A.CHAKRABORTY,A.J.EPSTEIN,B.R.PATTON,F.ZUO,J.R.GAINES,X.D.CHEN	Y,SC,BA,CU,O	
3832	SSC0680239	AT LEAST 90% Y123 PHASE	(Y,Sc)Ba2Cu3O7	Y0.5Sc0.5Ba2Cu3O7-Z	Y	0.5	Sc	0.5	Ba	2	Cu	3													O	7-Z			1988						1.37	32																					Y123																				83					83																																																																																		9.8																			ANOMALOUS MAGNETIC PROPERTIES OF Y1-XSCXBA2CU3O7-Z				SOLID STATE COMMUN.,68(1988)239	A.CHAKRABORTY,A.J.EPSTEIN,B.R.PATTON,F.ZUO,J.R.GAINES,X.D.CHEN	Y,SC,BA,CU,O	
3833	SSC0680835	RESN=AT 115K	YBa2(Cu,Mn)3O7	Y1Ba2Cu2.85Mn0.15O7-Z	Y	1	Ba	2	Cu	2.85	Mn	0.15													O	7-Z			1988																												Y123																			90.5	91.1					91.1										80																																																																				1.38																							MICROSTRUCTURE AND SUPERCONDUCTING FRACTION IN THE YBa2(Cu1-xMnx)3O7-delta			Fundacao de Tecnologia Industrial Po'lo Urbo Industrial, s/n -Gleba AI-6 - CP.16 12600 - Lorena -SP - Brasil	Solid State Commun.,68(1988)	O.F. de Lima,R.F. Jardim,S. Gama,S. Zacarelli		
3834	SSC0680835		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.7Mn0.3O7-Z	Y	1	Ba	2	Cu	2.7	Mn	0.3													O	7-Z			1988																												Y123																			88.7	89					89										60																																																																				2.19																							MICROSTRUCTURE AND SUPERCONDUCTING FRACTION IN THE YBa2(Cu1-xMnx)3O7-delta			Fundacao de Tecnologia Industrial Po'lo Urbo Industrial, s/n -Gleba AI-6 - CP.16 12600 - Lorena -SP - Brasil	Solid State Commun.,68(1988)	O.F. de Lima,R.F. Jardim,S. Gama,S. Zacarelli		
3835	SSC0680835		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.55Mn0.45O7-Z	Y	1	Ba	2	Cu	2.55	Mn	0.45													O	7-Z			1988																												Y123																			78	86					86										30																																																																				2.38																							MICROSTRUCTURE AND SUPERCONDUCTING FRACTION IN THE YBa2(Cu1-xMnx)3O7-delta			Fundacao de Tecnologia Industrial Po'lo Urbo Industrial, s/n -Gleba AI-6 - CP.16 12600 - Lorena -SP - Brasil	Solid State Commun.,68(1988)	O.F. de Lima,R.F. Jardim,S. Gama,S. Zacarelli		
3836	SSC0680835		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.4Mn0.6O7-Z	Y	1	Ba	2	Cu	2.4	Mn	0.6													O	7-Z			1988																												Y123																			73	84					84										20																																																																				2.99																							MICROSTRUCTURE AND SUPERCONDUCTING FRACTION IN THE YBa2(Cu1-xMnx)3O7-delta			Fundacao de Tecnologia Industrial Po'lo Urbo Industrial, s/n -Gleba AI-6 - CP.16 12600 - Lorena -SP - Brasil	Solid State Commun.,68(1988)	O.F. de Lima,R.F. Jardim,S. Gama,S. Zacarelli		
3837	SSC0680391	HIGHLY TEXTURED,J NORMAL TO FORGING AXIS	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91.5					91.5													700										190	50							3.2																																																			0.838																			ANISOTROPIC PROPERTIES OF SINTER-FORGED YBA2CU3O7-Z				SOLID STATE COMMUN.,68(1988)391	D.J.JOHNSON,J.B.KETTERSON,Q.ROBINSON,S.N.SONG	Y,BA,CU,O	
3838	SSC0680391	HIGHLY TEXTURED,J//FORGING AXIS	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																												Y123																				91.5					91.5													1300										190	50							1.15																																																			6.4																			ANISOTROPIC PROPERTIES OF SINTER-FORGED YBA2CU3O7-Z				SOLID STATE COMMUN.,68(1988)391	D.J.JOHNSON,J.B.KETTERSON,Q.ROBINSON,S.N.SONG	Y,BA,CU,O	
3839	SSC0680539		Y(Ba,M)2Cu3O7	Y1Ba1.95Li0.05Cu3OZ	Y	1	Ba	1.95	Li	0.05	Cu	3													O	Z			1988																											3	Y123																			66		72				69																																																																																																					EFFECTS OF ALKALI CATION(Li,Na,K,Cs)SUBSTITUTION ON THE MAGNETO-ELECTRICAL PROPERTIES OF Y1Ba2Cu3O7-y GRANULAR SUPERCONDUCTORS			Institut de Physique, B5, Universite' de Lie'ge, 4000. Belgium                              E-mail address: U2150MA at BLIULGII	Solid State Commun.,68(1988)539-545	A. Rulmont,Ch. Laurent,H.W. Vanderschueren,M. Ausloos,P. Tarte		
3840	SSC0680539		Y(Ba,M)2Cu3O7	Y1Ba1.95Na0.05Cu3OZ	Y	1	Ba	1.95	Na	0.05	Cu	3													O	Z			1988																											3	Y123																			78	90					90																																																																																																					EFFECTS OF ALKALI CATION(Li,Na,K,Cs)SUBSTITUTION ON THE MAGNETO-ELECTRICAL PROPERTIES OF Y1Ba2Cu3O7-y GRANULAR SUPERCONDUCTORS			Institut de Physique, B5, Universite' de Lie'ge, 4000. Belgium                              E-mail address: U2150MA at BLIULGII	Solid State Commun.,68(1988)539-545	A. Rulmont,Ch. Laurent,H.W. Vanderschueren,M. Ausloos,P. Tarte		
3841	SSC0680539		Y(Ba,M)2Cu3O7	Y1Ba1.95K0.05Cu3OZ	Y	1	Ba	1.95	K	0.05	Cu	3													O	Z			1988																											3	Y123																			83						83																																																																																																					EFFECTS OF ALKALI CATION(Li,Na,K,Cs)SUBSTITUTION ON THE MAGNETO-ELECTRICAL PROPERTIES OF Y1Ba2Cu3O7-y GRANULAR SUPERCONDUCTORS			Institut de Physique, B5, Universite' de Lie'ge, 4000. Belgium                              E-mail address: U2150MA at BLIULGII	Solid State Commun.,68(1988)539-545	A. Rulmont,Ch. Laurent,H.W. Vanderschueren,M. Ausloos,P. Tarte		
3842	SSC0680539		Y(Ba,M)2Cu3O7	Y1Ba1.95Cs0.05Cu3OZ	Y	1	Ba	1.95	Cs	0.05	Cu	3													O	Z			1988																											3	Y123																			78	84.5					84.5																																																																																																					EFFECTS OF ALKALI CATION(Li,Na,K,Cs)SUBSTITUTION ON THE MAGNETO-ELECTRICAL PROPERTIES OF Y1Ba2Cu3O7-y GRANULAR SUPERCONDUCTORS			Institut de Physique, B5, Universite' de Lie'ge, 4000. Belgium                              E-mail address: U2150MA at BLIULGII	Solid State Commun.,68(1988)539-545	A. Rulmont,Ch. Laurent,H.W. Vanderschueren,M. Ausloos,P. Tarte		
3843	SSC0680519	TWO STEP TRANSITION IN SUSCEPTIBILITY		Tl1.7Sr3Ca0.7Cu4.3OZ	Tl	1.7	Sr	3	Ca	0.7	Cu	4.3													O	Z			1988																											2					3.805		12.14													104		109				106.5																																																																																																					BLUK SUPERCONDUCTIVITY ABOVE 100 K IN THE Tl-Sr-Ca-Cu SYSTEM			Naval Research Laboratory Washington, DC 20375-5000	Solid State Commun.,68(1988)519-521	A.K. Singh,C. Skowronek,E.F. Skelton,H.A. Hoff,J.V. Gilfrich,L. Humphreys,L.E. Toth,M.S. Osofsky,R.A. Hein,R.J. Soulen, Jr,S.A. Wolf,S.B. Qadri,V.M. LeTourneau,W.L. Lechter,W.T. Elam		
3844	ME0382455		HoBa2Cu3O7	Ho1Ba2Cu3O6.9	Ho	1	Ba	2	Cu	3															O	7-Z	6.9		1988			EMU/mol	15.1		10.9	-16.1																				3	Y123				3.819	3.9	11.669														91.5				1.5	91.5																					MAGNETIZATION REACHES TO PARA-MAG VALUE										0.39																																																															BACO3,HO2O3,CU(NO3)2	1	MIXTURE-(950C IN AIR)-PELLET-ANN(700C 2H IN O2)-C(IN O2) TO RT					Meissner effect and critical fields in an inhomogeneous BaHoCu3O7-x high-Tc superconductor	198808		Departament de Fisica Fonamental, Universitat de Barcelona, Diagonal, 647 08028 Barcelona, Spain	Phys.Rev.B,38(1988)2455	A. Labarta,J. Tejada,J.M. Gonzalez-Calbet,M. Vallet,X. Obradors		
3845	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1Ba2Cu3O7.04	Nd	1	Ba	2	Cu	3															O	7+Z	7.04	1	1988																											3	Y123				3.871	3.914	11.756													77		88				82.5																																																																																														ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3846	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1.1Ba1.9Cu3O7.05	Nd	1.1	Ba	1.9	Cu	3															O	7+Z	7.05	1	1988																											3	Y123				3.871	3.914	11.732													50		81				65.5																																																																																														ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3847	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3O7.1	Nd	1.2	Ba	1.8	Cu	3															O	7+Z	7.1	1	1988																											3	Y123				3.89	3.892	11.696													33		54				43.5																																																																																														ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3848	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1.3Ba1.7Cu3O7.14	Nd	1.3	Ba	1.7	Cu	3															O	7+Z	7.14	1	1988																											2	Y123				3.89		11.661													14		50				32																																																																																														ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3849	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1.4Ba1.6Cu3O7.19	Nd	1.4	Ba	1.6	Cu	3															O	7+Z	7.19	1	1988																											2	Y123				3.874		11.659																																																																																																																	ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3850	PR0382450		Nd(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3O7.3	Nd	1.5	Ba	1.5	Cu	3															O	7+Z	7.3	1	1988																											2	Y123				3.876		11.649																																																																																																																	ND2O3,BACO3,CUO	1	MIXTURE-CAL(950C IN AIR)-PELLET-SIN(950C 24H)-ANN(450-500C 24H IN O2)-FC					ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3851	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1Ba2Cu3O7.01	Sm	1	Ba	2	Cu	3															O	7+Z	7.01	1	1988																											3	Y123				3.858	3.91	11.741													82		92				87																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3852	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1.1Ba1.9Cu3O7.05	Sm	1.1	Ba	1.9	Cu	3															O	7+Z	7.05	1	1988																											3	Y123				3.86	3.906	11.729													70		87				78.5																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3853	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1.2Ba1.8Cu3O7.09	Sm	1.2	Ba	1.8	Cu	3															O	7+Z	7.09	1	1988																											2	Y123				3.881		11.654													29		47				38																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3854	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1.3Ba1.7Cu3O7.16	Sm	1.3	Ba	1.7	Cu	3															O	7+Z	7.16	1	1988																											2	Y123				3.879		11.63																																																																																																																	SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3855	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1.4Ba1.6Cu3O7.19	Sm	1.4	Ba	1.6	Cu	3															O	7+Z	7.19	1	1988																											2	Y123				3.871		11.599																																																																																																																	SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3856	PR0382450		Sm(Ba,Sm)2Cu3O7	Sm1.5Ba1.5Cu3O7.22	Sm	1.5	Ba	1.5	Cu	3															O	7+Z	7.22	1	1988																											2	Y123				3.861		11.603																																																																																																																	SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3857	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1Ba2Cu3O7.01	Eu	1	Ba	2	Cu	3															O	7+Z	7.01	1	1988																											3	Y123				3.859	3.904	11.709													88		92				90																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3858	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1.1Ba1.9Cu3O7.07	Eu	1.1	Ba	1.9	Cu	3															O	7+Z	7.07	1	1988																											3	Y123				3.873	3.887	11.679													70		92				81																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3859	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1.2Ba1.8Cu3O7.18	Eu	1.2	Ba	1.8	Cu	3															O	7+Z	7.18	1	1988																											2	Y123				3.867		11.631													28		56				42																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3860	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1.3Ba1.7Cu3O7.15	Eu	1.3	Ba	1.7	Cu	3															O	7+Z	7.15	1	1988																											2	Y123				3.873		11.624													26		53				39.5																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3861	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1.4Ba1.6Cu3O7.16	Eu	1.4	Ba	1.6	Cu	3															O	7+Z	7.16	1	1988																											2	Y123				3.854		11.619													13		43				28																																																																																														SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3862	PR0382450		Eu(Ba,Eu)2Cu3O7	Eu1.5Ba1.5Cu3O7.32	Eu	1.5	Ba	1.5	Cu	3															O	7+Z	7.32	1	1988																											2	Y123				3.844		11.579																																																																																																																	SM2O3,BACO3,CUO	1						ORTHORHOMBIC-TO-TETRAGONAL TRANSITION IN R1+XBA2-XCU3O7-Z (R=NS,SM, AND FU)	8		DEPARTMENT OF CHEMISTRY, RUTGERS-THE STATE UNIVERSITY, NEW JERSEY	PHYS.REV.B,38(1988)2450	E.A.HAYRI,K.V.RAMANUJACHARY,MARTHA GREENBLATT,S.LI	ND,SM,EU,BA,CU,O	
3863	PRB0384596	TWO STEP TC2=9.3K	(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1988																											2	T																				30					30																																																																																		0.852												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3864	PRB0384596	RESISTIVE PEAK AT TC(ON), IMPURITY PHASES EXIST	(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4		1	1988																											2	T																				30					30																																																																																		1.22												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3865	PRB0384596		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4		1	1988																											2	T																				32.2					32.2																																																																																		0.235												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3866	PRB0384596	TWO STEP TC2=17.0	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4		1	1988																											2	T																				32.5					32.5																																																																																		0.497												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3867	PRB0384596		(La,Ba)2CuO4	La1.825Ba0.175Cu1O4	La	1.825	Ba	0.175	Cu	1															O	4		1	1988																											2	T																				28.3					28.3																																																																																		0.443												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3868	PRB0384596		(La,Ba)2CuO4	La1.855Ba0.145Cu1O4	La	1.855	Ba	0.145	Cu	1															O	4		1	1988																											2	T																				30					30																																																																																		1.03												LA2O3,BACO3,CUO	0	MIXTURE-PRESS-(1000C 12H IN AIR)-(1100C 12H IN AIR)-FC					SUPERCONDUCTING PROPERTIES OF LA(2-X)BA(X)CU(1)O(4)	198809	TC                       ,RES                      ,INDUCTANCE               ,LA	BROOKHAVEN NATIONAL LABORATORY,UPTON,NEW YORK	PHYS.REV.B,38(1988)4596	A.R.MOODENBAUGH,M.SUENAGA,R.N.SHELTON,T.J.FOLKERTS,YOUWEN XU	LA,BA,CU,O	
3869	OX0385025	91%O(18),DTC=0.16K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123																				91.2					91.2						0.016	O	91	0.16																																																																																					BAO2,Y2O3,CUO	0	MIXTURE-HEAT(850C 3H IN AIR)-(950C 12H IN O2)-C-REGROUND-(950C 12H IN O2)-(350C 48H IN O2)-O(18) EXCHANGE					OXYGEN ISOTOPE EFFECT ON CRITICAL TEMPERATURE AND PHONON MODES IN Y(1)BA(2)CU(3)O(7)	198809	FAR-INFRARED             ,ISOTOPE EFFECT           ,SUS                      ,TC	UNIVERSITY OF VIRGINIA,CHARLOTTESVILLE,VIRGINIA	PHYS.REV.B,38(1988)5025	E.L.BENITEZ,E.M.MCCARRON,J.J.LIN,M.K.CRAWFORD,S.J.POON,W.E.FARNETH	Y,BA,CU,O	
3870	HI0379730		EuBa2Cu3O7	Eu1Ba2Cu3OZ	Eu	1	Ba	2	Cu	3															O	Z			1988																											3	Y123				3.849	3.901	11.704														90					90			K/KBAR	0.16																																																																																											1	MIXTURE-CAL(950C IN AIR)-SIN(950C IN O2)-SLOW C IN O2					HIGH-PRESSURE STUDY ON 60- AND 90-K EU(1)BA(2)CU(3)O(7-Z)	198806	PRESSURE EFFECT          ,RESISTIVITY              ,TC	DEPARTMENT OF PHYSICS,TEXAS CENTER FOR SUPERCONDUCTIVITY AT THE UNIVERSITY OF HOUSTON,HOUSTON,TEXAS	PHYS.REV.B,37(1988)9730	C.W.CHU,L.GAO,P.H.HOR,R.L.MENG,Z.J.HUANG	EU,BA,CU,O	
3871	HI0379730		EuBa2Cu3O7	Eu1Ba2Cu3OZ	Eu	1	Ba	2	Cu	3															O	Z			1988																											3	Y123				3.859	3.904	11.712														55					55			K/KBAR	0.9																																																																																											1	3870 SAMPLE-ANN(300-500C 30MIN IN VACUUM)					HIGH-PRESSURE STUDY ON 60- AND 90-K EU(1)BA(2)CU(3)O(7-Z)	198806	PRESSURE EFFECT          ,RESISTIVITY              ,TC	DEPARTMENT OF PHYSICS,TEXAS CENTER FOR SUPERCONDUCTIVITY AT THE UNIVERSITY OF HOUSTON,HOUSTON,TEXAS	PHYS.REV.B,37(1988)9730	C.W.CHU,L.GAO,P.H.HOR,R.L.MENG,Z.J.HUANG	EU,BA,CU,O	
3872	PR0465880		K3C60	C60K3	C	60	K	3																					1992																												fullerene																				18					18																						28									2							34																																																									1						UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
3873	PR0465880		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																				30					30																						38									2							30																																																									1						UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
3874	PR0465876	HC2 FOLLOWS LINEAR RELATION, NOT WHH THEORY	K3C60	C60K3	C	60	K	3																				1	1992																												fullerene																				18.7					18.7																						38									2.14							29																																																									0	C60 POWDER + K-(350C SEVERAL DAYS IN SEALED PYREX AMPOULE),NOMINAL(K2.5 C60)					EVIDENCE OF UPPER-CRITICAL-FIELD ENHAMCEMENT IN K3C60 POWDERS	199209		AT&T BELL LABORATORIES, NEW JERSEY	PHYS.REN.B,46(1992)5876	A.PASSNER,D.W.MURPHY,G.S.BOEBINGER,I.I.MAZIN,M.J.ROSSEINSKY,T.T.PALSTRA	K,C	
3875	HE0370552	GAMMA BY SPHEAT, BCS THEORY	DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	7		1	1988																												Y123																				92.5				3.7	92.5																																																						J/MOLE.K	3.7		28																																					DY2O3,BA(NO3)2,CUO	0	MIXTURE-(1173K 12H IN AIR)-PELLET-SIN(1223K 16H IN O2)-ANN(1173K 1H+1073K 2H+973K 4H)-C TO RT					HEAT CAPACITY OF THE HIGH-TEMPERATURE SUPERCONDUCTOR BA(2)DY(1)CU(3)O(7)	198801	SPECIFIC HEAT            ,MAGNETIZATION	RESEARCH LABORATORY OF ENGINEEING MATERIALS,TOKYO INSTITUTE OF TECHNOLOGY,YOKOHAMA	PHYS.REV.B,37(1988)552	TETSURO NAKAMURA,TOORU ATAKE,YASUTOSHI SAITO,YOSHIKI TAKAGI	DY,BA,CU,O	
3876	SP0367145	NEEL-T DETERMINED BY SPHEAT	NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7		1	1987																											3	Y123																																																																																																																								1						SPECIFIC HEAT NEAR T(N) IN(PR,ND,SM,GD,AND DY)BA(2)CU(3)O(7): EVIDENCE FOR SPIN-EXCHANGE-DRIVEN ORDERING	198711	MAGNETIC ORDERING        ,SPECIFIC HEAT            ,ANTIFERR	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)7145	A.P.RAMIREZ,J.V.WASZCZAK,L.F.SCHNEEMEYER	PR,ND,SM,GD,DY,BA,CU,O	
3877	SP0367145	NEEL-T DETERMINED BY SPHEAT, NO ORDERING	SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O	7		1	1987								0.6																			3	Y123																																																																																																																								1						SPECIFIC HEAT NEAR T(N) IN(PR,ND,SM,GD,AND DY)BA(2)CU(3)O(7): EVIDENCE FOR SPIN-EXCHANGE-DRIVEN ORDERING	198711	MAGNETIC ORDERING        ,SPECIFIC HEAT            ,ANTIFERR	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)7145	A.P.RAMIREZ,J.V.WASZCZAK,L.F.SCHNEEMEYER	PR,ND,SM,GD,DY,BA,CU,O	
3878	SP0367145	NEEL-T BY SPHEAT	GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7		1	1987								2.2																			3	Y123																																																																																																																								1						SPECIFIC HEAT NEAR T(N) IN(PR,ND,SM,GD,AND DY)BA(2)CU(3)O(7): EVIDENCE FOR SPIN-EXCHANGE-DRIVEN ORDERING	198711	MAGNETIC ORDERING        ,SPECIFIC HEAT            ,ANTIFERR	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)7145	A.P.RAMIREZ,J.V.WASZCZAK,L.F.SCHNEEMEYER	PR,ND,SM,GD,DY,BA,CU,O	
3879	SP0367145	NEEL-T BY SPHEAT	DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	7		1	1987								0.92																			3	Y123																																																																																																																								1						SPECIFIC HEAT NEAR T(N) IN(PR,ND,SM,GD,AND DY)BA(2)CU(3)O(7): EVIDENCE FOR SPIN-EXCHANGE-DRIVEN ORDERING	198711	MAGNETIC ORDERING        ,SPECIFIC HEAT            ,ANTIFERR	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,36(1987)7145	A.P.RAMIREZ,J.V.WASZCZAK,L.F.SCHNEEMEYER	PR,ND,SM,GD,DY,BA,CU,O	
3880	SP0366915		GdBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1987					/GD	7.98	-5.89																					Y123																			89	94				2	94																																																						MJ/GAT.K	301				374																																				1	MIXTURE-(950C 24H)-(900C 16H IN O2)-C(100C/C) TO 400C-C(200C/H)-TO RT					SPECIFIC HEAT OF GD(1)BA(2)CU(3)O(7-Z) IN THE NORMAL AND SUPERCONDUCTING STATES	198711	SPECIFIC HEAT            ,ANTIFERROMAGNETIC        ,RES                      ,SU	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,URBANA,ILLINOIS	PHYS.REV.B,36(1987)6915	B.G.PAZOL,D.M.GINSBERG,D.S.CITRIN,M.E.REEVES,T.A.FRIEDMANN	GD,BA,CU,O	
3881	SP0366915		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																			90.3	92.1				1.79	92.1																																																											374																																				1	MIXTURE-(950C 24H)-(900C 16H IN O2)-C(100C/C) TO 400C-C(200C/H)-TO RT					SPECIFIC HEAT OF GD(1)BA(2)CU(3)O(7-Z) IN THE NORMAL AND SUPERCONDUCTING STATES	198711	SPECIFIC HEAT            ,ANTIFERROMAGNETIC        ,RES                      ,SU	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,URBANA,ILLINOIS	PHYS.REV.B,36(1987)6915	B.G.PAZOL,D.M.GINSBERG,D.S.CITRIN,M.E.REEVES,T.A.FRIEDMANN	GD,BA,CU,O	
3882	SP0366915		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																																																																																		4.17		356																																				1	MIXTURE-(950C 24H)-(900C 16H IN O2)-C(100C/C) TO 400C-C(200C/H)-TO RT					SPECIFIC HEAT OF GD(1)BA(2)CU(3)O(7-Z) IN THE NORMAL AND SUPERCONDUCTING STATES	198711	SPECIFIC HEAT            ,ANTIFERROMAGNETIC        ,RES                      ,SU	DEPARTMENT OF PHYSICS AND MATERIALS RESEARCH LABORATORY,UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN,URBANA,ILLINOIS	PHYS.REV.B,36(1987)6915	B.G.PAZOL,D.M.GINSBERG,D.S.CITRIN,M.E.REEVES,T.A.FRIEDMANN	GD,BA,CU,O	
3883	EF0365258		(La,Nd,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																											2	T				3.778		13.222													24	34.4	37				34.4																															1.33																																															0.98																	0	NITRATE-CAL(1000C)-PELLET-SIN(1000C OVERNIGHT)					EFFECT OF MAGNETIC IMPURITIES ON HIGH-TEMPERATURE SUPERCONDUCTIVITY IN LA(1.85)SR(0.15)CU(1)O(4)	198710	MAGNETIC IMPURITY        ,RESISTIVITY              ,SUS                      ,HC	MATERIALS SCIENCE AND CHEMISTRY DISISIONS,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS	PHYS.REV.B,36(1987)5258	A.UMEZAWA,E.E.ALP,G.W.GRABTREE,L.MORSS,L.SODERHOLM,W.K.KWOK	LA,SR,CU,O,ND	
3884	EF0365258		(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4			1987																											2	T				3.768		13.173													9	22.5	30				22.5																															0.97																																															4.8																	0	NITRATE-CAL(1000C)-PELLET-SIN(1000C OVERNIGHT)					EFFECT OF MAGNETIC IMPURITIES ON HIGH-TEMPERATURE SUPERCONDUCTIVITY IN LA(1.85)SR(0.15)CU(1)O(4)	198710	MAGNETIC IMPURITY        ,RESISTIVITY              ,SUS                      ,HC	MATERIALS SCIENCE AND CHEMISTRY DISISIONS,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS	PHYS.REV.B,36(1987)5258	A.UMEZAWA,E.E.ALP,G.W.GRABTREE,L.MORSS,L.SODERHOLM,W.K.KWOK	LA,SR,CU,O,ND	
3885	EF0365258		(La,Nd,Sr)2CuO4	La1.82Nd0.03Sr0.15Cu1O4	La	1.82	Nd	0.03	Sr	0.15	Cu	1													O	4			1987					/ND	3.9																					2	T																				34.2	38				34.2																															1.26																																																																0	NITRATE-CAL(1000C)-PELLET-SIN(1000C OVERNIGHT)					EFFECT OF MAGNETIC IMPURITIES ON HIGH-TEMPERATURE SUPERCONDUCTIVITY IN LA(1.85)SR(0.15)CU(1)O(4)	198710	MAGNETIC IMPURITY        ,RESISTIVITY              ,SUS                      ,HC	MATERIALS SCIENCE AND CHEMISTRY DISISIONS,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS	PHYS.REV.B,36(1987)5258	A.UMEZAWA,E.E.ALP,G.W.GRABTREE,L.MORSS,L.SODERHOLM,W.K.KWOK	LA,SR,CU,O,ND	
3886	MA0364028	O IS REPLACED BY S	YBa2Cu3(O,S)7	Y1Ba2Cu3S1O6	Y	1	Ba	2	Cu	3	S	1													O	6		1	1987																											3	Y123				3.855	3.914	11.75														89					89										80		ESR MEASUREMENT	600								ESTIMATED FROM HC1ZERO,KAPPA	138																																																																									0	SLOW COOLING					MAGNETISM AND CRITICAL FIELDS IN THE HIGH-TC SUPERCONDUCTORS Y(1)BA(2)CU(3)O(7-X)S(X)(X=0,1):AN ESR STUDY	198709	SUSCEPTIBILITY           ,HC                       ,ESR	RACAH INSTITUTE OF PHYSICS,HEBREW UNIVERSITY OF JERUSALEM,JERUSALEM,ISRAEL	PYHS.REV.B,36(1987)4028	CARLOS RETTORI,DAN DAVIDOV,IGAL BELAISH,ISRAEL FELNER	Y,BA,CU,O,S	
3887	TE0387026	THERMAL EXPANSION=10.5E-6 K(-1)	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1988																												BKBO				4.286						4.5																																																																																																														0	SEE NAT3320814					TEMPERTURE DEPENDENCE OF THE LATTICE PARAMETERS IN THE 30-K SUPERCONDUCTOR BA(0.6)K(0.4)BI(1)O(3)	198810	XRY                      ,STRUCTURE	AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY	PHYS.REV.B,38(1988)7026	J.J.KRAJEWSKI,P.MARSH,R.J.CAVA,R.M.FLEMING	BA,K,BI,O	
3888	MA03811828		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1988																												Y123																				91.5					91.5												MAGNETIC RELAXATION		250	950																																																																																0	SEE J.CRYST.GROWTH,85(1987)593					MAGNETIC RELAXATION AND THE LOWER CRITICAL FIELDS IN A Y-BA-CU-O CRYSTAL	198812	MAGNETIC RELAXATION      ,LOWER CRITICAL FIELD     ,FLUX CREEP               ,MA	IBM THOMAS J.WATSON RESEARCH CENTER,YORKTOWN HEIGHTS,NEW YORK	PHYS.REV.B,38(1988)11828	A.P.MALPZERMOFF,F.HOLTZBERG,T.R.DINGER,Y.YESHURUN	Y,BA,CU,O	
3889	LO0387041	SPJUMP=6MJ/K2.MOLE	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1988																												T																				36.7					36.7																																																							6		1.8		285																																				0	SEE SSC0620383					LOW-TEMPERATURE SPECIFIC HEAT OF LA(1.85)SR(0.15)CU(1)O(4) AND LA(2)CU(1)O(4)	198810	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,THE PENNSYLVANIA STATE UNIVERSITY,UNIVERSITY PARK,PENNSYLVANIA	PHYS.REV.B,38(1988)7041	A.JIN,D.FINOTELLO,J.E.GREEDAN,K.A.GILLIS,M.H.W.CHAN,Y.P.FENG	LA,SR,CU,O	
3890	LO0387041	OZ>3.97	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1988								250																				T																																																																																		0.2		280																																				0	SEE SSC0620383					LOW-TEMPERATURE SPECIFIC HEAT OF LA(1.85)SR(0.15)CU(1)O(4) AND LA(2)CU(1)O(4)	198810	SPECIFIC HEAT	DEPARTMENT OF PHYSICS,THE PENNSYLVANIA STATE UNIVERSITY,UNIVERSITY PARK,PENNSYLVANIA	PHYS.REV.B,38(1988)7041	A.JIN,D.FINOTELLO,J.E.GREEDAN,K.A.GILLIS,M.H.W.CHAN,Y.P.FENG	LA,SR,CU,O	
3891	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Nd1Cu3O8+Z	Pb	2	Sr	2	Nd	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.437	5.48	15.782																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3892	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Sm1Cu3O8+Z	Pb	2	Sr	2	Sm	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.424	5.466	15.758																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3893	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Eu1Cu3O8+Z	Pb	2	Sr	2	Eu	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.417	5.459	15.741																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3894	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Gd1Cu3O8+Z	Pb	2	Sr	2	Gd	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.413	5.454	15.734																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3895	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Dy1Cu3O8+Z	Pb	2	Sr	2	Dy	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.399	5.44	15.719																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3896	JPS0610881		Pb2Sr2MCu3O8+Z	Pb2Sr2Ho1Cu3O8+Z	Pb	2	Sr	2	Ho	1	Cu	3													O	8+Z		1	1992																											3	Pb3212				5.394	5.436	15.721																																																																																																																		1						CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3897	JPS0610881		Pb2Sr2ErCu3O8	Pb2Sr2Er1Cu3O8+Z	Pb	2	Sr	2	Er	1	Cu	3													O	8+Z		1	1992																											3	Pb3212	CMMM			5.387	5.428	15.708																																																																																																																	PBO,SRCO3,LN2O3,CACO3,CUO	1	MIX-(800C12H)-Q TO RT-PELLET-SIN(850C12H)-Q TO RT-ANN(800C24H IN N2)					CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3898	JPS0610881		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.7Ca0.3Cu3O8+Z	Pb	2	Sr	2	Y	0.7	Ca	0.3	Cu	3											O	8+Z		1	1992																											3	Pb3212				5.383	5.419	15.75																																																																																																																	PBO,SRCO3,LN2O3,CACO3,CUO	1	MIX-(800C12H)-Q TO RT-PELLET-SIN(850C12H)-Q TO RT-ANN(800C24H IN N2)					CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3899	JPS0610881		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8+Z	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8+Z		1	1992																											3	Pb3212				5.378	5.415	15.778																																																																																																																	PBO,SRCO3,LN2O3,CACO3,CUO	1	MIX-(800C12H)-Q TO RT-PELLET-SIN(850C12H)-Q TO RT-ANN(800C24H IN N2)					CRYSTAL STRUCTURE OF PB2SR2MCU3O8+Z SYSTEN (M=ND, SM, EU, GD,DY, Y1-XCAX,HO AND ER)	199203	CRYSTAL STRUCTURE   ,X-RAY               ,COMPRESSIBILITY		J.PHYS.SOC.JAPAN,61(1992)881	KAZUO KADOWAKI,TAKASHI MOCHIKU	PB,SR,LN,CU,O	
3900	JPS0582252	Ln:Ba:Ce:Cu=6:4:2:9, Tc strongly depends on annealing condition	Cu(Eu,Ce)2(Ba,Eu)2Cu2O10-z	Eu6Ba4Ce2Cu9OZ	Eu	6	Ba	4	Ce	2	Cu	9													O	Z		1	1989			EMU/G																								2	Cu1222	I4/MMM		A	3.85		28.46														20					20										22																																																																																				ND2O3,SM2O3,CEO2,EU2O3+BACO3,CUO	1	MIX-PELLET-(1020C15H IN O2)-REPEAT 2 TIMES-ANN(650C 24H IN O2(80KG/CM2))					A new family of superconducting copper oxides: (Ln1-xCex)2(Ba1-yLny)2Cu3O10-z) (Ln: Nd,Sm,Eu) 	198907		DEPARTMENT OF PHYSICS, AOYAMA-GAKUIN UNIVERSIRY	J.PHYS.SOC.JAPAN,58(1989)3363	HIROSHI SAWA,JUN AKIMITSU,KAZUHIKO OBARA,SHIGEO HORIUCHI,YOSHIO MATSUI	ND,SM,EU,CE,BA,CU,O	
3901	JPS0582252		Cu(Sm,Ce)2(Ba,Sm)2Cu2O10-z	Sm6Ba4Ce2Cu9OZ	Sm	6	Ba	4	Ce	2	Cu	9													O	Z		1	1989																											2	Cu1222																				12					12																																																																																														ND2O3,SM2O3,CEO2,EU2O3+BACO3,CUO	1	MIX-PELLET-(1020C15H IN O2)-REPEAT 2 TIMES-ANN(650C 24H IN O2(80KG/CM2))					A new family of superconducting copper oxides: (Ln1-xCex)2(Ba1-yLny)2Cu3O10-z) (Ln: Nd,Sm,Eu) 	198907		DEPARTMENT OF PHYSICS, AOYAMA-GAKUIN UNIVERSIRY	J.PHYS.SOC.JAPAN,58(1989)3363	HIROSHI SAWA,JUN AKIMITSU,KAZUHIKO OBARA,SHIGEO HORIUCHI,YOSHIO MATSUI	ND,SM,EU,CE,BA,CU,O	
3902	JPS0582252		Cu(Nd,Ce)2(Ba,Nd))2Cu2O10-z	Nd6Ba4Ce2Cu9OZ	Nd	6	Ba	4	Ce	2	Cu	9													O	Z		1	1989																											2	Cu1222																				27					27																																																																																														ND2O3,SM2O3,CEO2,EU2O3+BACO3,CUO	1	MIX-PELLET-(1020C15H IN O2)-REPEAT 2 TIMES-ANN(650C 24H IN O2(80KG/CM2))					A new family of superconducting copper oxides: (Ln1-xCex)2(Ba1-yLny)2Cu3O10-z) (Ln: Nd,Sm,Eu) 	198907		DEPARTMENT OF PHYSICS, AOYAMA-GAKUIN UNIVERSIRY	J.PHYS.SOC.JAPAN,58(1989)3363	HIROSHI SAWA,JUN AKIMITSU,KAZUHIKO OBARA,SHIGEO HORIUCHI,YOSHIO MATSUI	ND,SM,EU,CE,BA,CU,O	
3903	OH0563805	NEEL TEMP. BY SPECIFIC HEAT	RBa2Cu3O7	Gd1Ba2Cu3OX	Gd	1	Ba	2	Cu	3															O	X			1987								2.25																				Y123																				87					87																																																																																														R2O3,BACO3,CUO	1	MIXTURE-PELLET-(920C 15H)-SLOW C-REPEAT(940C)					Heat Capacities of Ba2RCu3Ox (R=Gd, Ho, Er, Dy)	1987		Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Phys.Soc.Jpn,56(1987)3805-3807	Kiichi AMAYA,Koh-ichi UEDA,Kunisuke ASAYAMA,Takao KOHARA,Tatsuo KOBAYASHI,Yasukage ODA,Yoh KOHORI		
3904	OH0563805		RBa2Cu3O7	Er1Ba2Cu3OX	Er	1	Ba	2	Cu	3															O	X			1987								0.55																				Y123																				90					90																																																																																														R2O3,BACO3,CUO	1	MIXTURE-PELLET-(920C 15H)-SLOW C-REPEAT(940C)					Heat Capacities of Ba2RCu3Ox (R=Gd, Ho, Er, Dy)	1987		Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Phys.Soc.Jpn,56(1987)3805-3807	Kiichi AMAYA,Koh-ichi UEDA,Kunisuke ASAYAMA,Takao KOHARA,Tatsuo KOBAYASHI,Yasukage ODA,Yoh KOHORI		
3905	OH0563805		RBa2Cu3O7	Dy1Ba2Cu3OX	Dy	1	Ba	2	Cu	3															O	X			1987								0.95																				Y123																				92					92																																																																																														R2O3,BACO3,CUO	1	MIXTURE-PELLET-(920C 15H)-SLOW C-REPEAT(940C)					Heat Capacities of Ba2RCu3Ox (R=Gd, Ho, Er, Dy)	1987		Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Phys.Soc.Jpn,56(1987)3805-3807	Kiichi AMAYA,Koh-ichi UEDA,Kunisuke ASAYAMA,Takao KOHARA,Tatsuo KOBAYASHI,Yasukage ODA,Yoh KOHORI		
3906	OH0563805		RBa2Cu3O7	Ho1Ba2Cu3OX	Ho	1	Ba	2	Cu	3															O	X			1987								0.1																				Y123																				90					90																																																																																														R2O3,BACO3,CUO	1	MIXTURE-PELLET-(920C 15H)-SLOW C-REPEAT(940C)					Heat Capacities of Ba2RCu3Ox (R=Gd, Ho, Er, Dy)	1987		Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Phys.Soc.Jpn,56(1987)3805-3807	Kiichi AMAYA,Koh-ichi UEDA,Kunisuke ASAYAMA,Takao KOHARA,Tatsuo KOBAYASHI,Yasukage ODA,Yoh KOHORI		
3907	SSC0820673		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z			1992									2.871																		2	Bi2223																			99.2		115				107.1																																																														4.941			THC3907																	3.841													1						INFLUENCE OF DENSITY OF BI0.6PB0.4SR2CA2CU3OX SUPEERCONDUCTINGPELLETS ON THEIR TEMPERATURE DEPENDENCE OF THERMAL CONDUCTIVITY				SOLID STATE COMMUN.82(1992)673	H.K.BARIK,T.K.DEY	BI,PB,SR,CA,CU,O	
3908	SSC0820673		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z			1992									3.595																		2	Bi2223																			99.5		115				107.25																																																														5.2			THC3908																	3.637													1						INFLUENCE OF DENSITY OF BI0.6PB0.4SR2CA2CU3OX SUPEERCONDUCTINGPELLETS ON THEIR TEMPERATURE DEPENDENCE OF THERMAL CONDUCTIVITY				SOLID STATE COMMUN.82(1992)673	H.K.BARIK,T.K.DEY	BI,PB,SR,CA,CU,O	
3909	SSC0820673		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z			1992									3.821																		2	Bi2223																			100.5		115				107.75																																																														5.4			THC3909																	2.934													1						INFLUENCE OF DENSITY OF BI0.6PB0.4SR2CA2CU3OX SUPEERCONDUCTINGPELLETS ON THEIR TEMPERATURE DEPENDENCE OF THERMAL CONDUCTIVITY				SOLID STATE COMMUN.82(1992)673	H.K.BARIK,T.K.DEY	BI,PB,SR,CA,CU,O	
3910	SSC0820673		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z			1992									4.252																		2	Bi2223																			101.2		115				108.1																																																														5.576			THC3910																	2.543													1						INFLUENCE OF DENSITY OF BI0.6PB0.4SR2CA2CU3OX SUPEERCONDUCTINGPELLETS ON THEIR TEMPERATURE DEPENDENCE OF THERMAL CONDUCTIVITY				SOLID STATE COMMUN.82(1992)673	H.K.BARIK,T.K.DEY	BI,PB,SR,CA,CU,O	
3911	SSC0820775		(Bi,Pb)2Sr2Ca3Cu4O10	Bi1.6Pb0.4Sr2Ca3Cu4O10+Z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	4											O	10+Z			1992																												Bi2234																			90	100	110				100																																																																						TP3911																									1						THERMOELECTRIC POWER OF BULK AND THIN FILM BISMUTH HIGH TC SUPERCONDUCTORS				SOLID STATE COMMUN.82(1992)775	A.MARINO,J.E.RODRIGUEZ	BI,PB,SR,CA,CU,O	
3912	SSC0820241		TmBa2Cu3O7	Tm1Ba2Cu3O7	Tm	1	Ba	2	Cu	3															O	7		3	1992																												Y123																				90					90																																																																	THC3912					TP3912																									0						THERMAL CONDUCTIVITY OF TMBA2CU3OX AND BI2SR2CACU2OX SINGLE CRYSTALS IN THE VICINITY OF THE SUPERCONDUCTING TRANSITION				SOLID STATE COMMUN.82(1992)241	F.G.ALIEV,M.A.ARRANZ MONGE,V.V.MOSHCHALKOV,V.V.PRYADUN	TM,BA,CU,O,BI,SR,CA	
3913	SSC0820241		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X		3	1992																												Bi2212																				89					89																																																																	THC3913					TP3913																									0						THERMAL CONDUCTIVITY OF TMBA2CU3OX AND BI2SR2CACU2OX SINGLE CRYSTALS IN THE VICINITY OF THE SUPERCONDUCTING TRANSITION				SOLID STATE COMMUN.82(1992)241	F.G.ALIEV,M.A.ARRANZ MONGE,V.V.MOSHCHALKOV,V.V.PRYADUN	TM,BA,CU,O,BI,SR,CA	
3914	PHC1990032	SIZE 1.0*1.0*0.093MM3,DEMAG.FACTOR=0.87,	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1992																												Bi2212																				87					87													340																																																																																		7	FLOATING ZONE FROM SINTERED FEED					TEMPERATURE DEPENDENCE OF THE LOWER CRITICAL FIELD UNDER THE EFFECT OF SURFACE BARRIES IN BI2SR2CACU2O8 CRYSTAL	199208			PHYSICA C,199(1992)32	K.KISHIO,M.KONCZYKOWSKI,N.CHIKUMOTO,N.MOTOHIRA	BI,SR,CA,CU,O	
3915	PHC1990023	RANDOM ORIENTED MULTI-GRAIN(8*8*4MM3),EXTENSIVE TWIN, JC CRITERIA=3.3UV/CM,JC(77K,H=1T)=3000A/CM2	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1992																											3	Y123																				94					94																																																			16000																																												0	MELT-GROWN BULK,SIN-1100C 15H-RAPID COOL TO 1030C-SLOW C TO 980C-HOLD(980C 15H)					TRANSPORT CRITICAL CURRENTS AND FLUX PINNING IN MELT-GROWN YBA2CU3O7-Z	199208			PHYSICA C,199(1992)23	C.BEDUZ,R.G.SCURLOCK,Y.YANG,Z.YI	Y,BA,CU,O	
3916	SSC0721207		Y(Ba,K)2Cu3O7	Y1Ba1.9K0.1Cu3O7-Z	Y	1	Ba	1.9	K	0.1	Cu	3													O	7-Z		1	1989																											3	Y123				3.83	3.895	11.6																																315									73																																																																								CUO,Y2O3,BACO3,KHCO3	1	MIXTURE-CAL(800C 12H)-PRESS-SIN(960C SEV H IN O2)-SLOW C					EPR OF POLYCRYSTALLINE HIGH-TC SUPERCONDUCTOR YBA1.9K0.1CU3O7-Z	198912	ERP                 ,MICROWAVEABSORPTION ,CRITICAL FIELD	PHYSICS DEPARTMENT CONCORDIA UNIVERSITY, 1455 DE MAISONNEUVE BOULEVARD WEST MONTREAL, QUEBEC, CANADA H3G 1M8	SOLID STATE COMMUN.72(1989)1207	LUCJAN E. MISIAK,SUSHIL K. MISRA	Y,BA,K,CU,O	
3917	SSC0720749	GAMMA BY LOW TEMP SP.HEAT	(Pr,Ce)2CuO4	Pr1.95Ce0.05Cu1O4	Pr	1.95	Ce	0.05	Cu	1															O	4		1	1989																												T'																																																																																		2.08																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3918	SSC0720749		(Pr,Ce)2CuO4	Pr1.9Ce0.1Cu1O4	Pr	1.9	Ce	0.1	Cu	1															O	4		1	1989																												T'																																																																																		2.34																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3919	SSC0720749		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		1	1989																												T'						12.15																																																																												2.75																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3920	SSC0720749		(Pr,Ce)2CuO4	Pr1.82Ce0.18Cu1O4	Pr	1.82	Ce	0.18	Cu	1															O	4		1	1989																												T'																																																																																		4.13																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3921	SSC0720749		(Pr,Ce)2CuO4	Pr1.8Ce0.2Cu1O4	Pr	1.8	Ce	0.2	Cu	1															O	4			1989																												T'																																																																																		5.02																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3922	SSC0720749		(Pr,Ce)2CuO4	Pr1.75Ce0.25Cu1O4	Pr	1.75	Ce	0.25	Cu	1															O	4			1989																												T'																																																																																		6.96																																						0						SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3923	SSC0720749	GAMMA ESTIMATED BY BCS TYPE JUMP(1.43)	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1989																												T'						12.25														22					22																																																							37.75		1.2																																						0	HEAT(900C 18H IN AIR)-PRESS-HEAT(1000C 20H+1100C 40H IN AIR)-PRESS-HEAT-ANN(900C 44H+550C 50H IN 1E-5 TORR)					SMALL ELECTRONIC SPECIFIC HEAT IN THE ELECTRON DOPED CU-OXIDESUPERCONDUCTORS	198911	SPECIFIC HEAT	INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444 JAPAN	SOLID STATE COMMUN.72(1989)749	M. SATO,M. SERA,S. SHAMOTO	PR,ND,CE,CU,O	
3924	SSC0720697	DENSITY=60% OF X-RAY DENSITY,SMALL AMOUNT OF BI4SR8CU5O19+Z	Bi2Sr2CuO6	Bi2Sr2Cu1O6.17	Bi	2	Sr	2	Cu	1															O	6+Z	6.17	1	1989																												Bi2201				5.365	5.369	24.69																	4.2																																																																																																	1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3925	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6.2	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z	6.2	1	1989																												Bi2201				5.374	5.379	24.63														12					12																																																																																															1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3926	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1.8La0.2Cu1O6.3	Bi	2	Sr	1.8	La	0.2	Cu	1													O	6+Z	6.3	1	1989																												Bi2201				5.375	5.388	24.59														18					18																																																																																															1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3927	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.35	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z	6.35	1	1989																												Bi2201				5.381	5.417	24.42														20					20																																																																																															1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3928	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6.38	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+Z	6.38	1	1989																												Bi2201				5.387	5.421	24.31														21					21																																																																																															1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3929	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1.4La0.6Cu1O6.42	Bi	2	Sr	1.4	La	0.6	Cu	1													O	6+Z	6.42	1	1989																												Bi2201				5.389	5.43	24.13														5					5																																																																																															1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3930	SSC0720697		Bi2(Sr,La)2CuO6	Bi2Sr1La1Cu1O6.6	Bi	2	Sr	1	La	1	Cu	1													O	6+Z	6.6	1	1989																												Bi2201				5.417	5.445	24																	4.2																																																																																																	1						OXYGEN CONTENT, LATTICE CONSTANTS AND TC OF BI2SR2-XLAXCUO6+ZWHTH 0.0<X<1.0	198911	LETTICE CONSTANT    ,OXYGEN CONTENTS	GORLAEUS LABORATORIES, LEIDEN UNIVERSITY, P.O.BOX 9502, 2300 RA LEIDEN, THE NETHERLANDS	SOLID STATE COMMUN.72(1989)697	D. M. DE LEEUW,G. M. STOLLMAN,W. A. GROEN	BI,SR,LA,CU,O	
3931	SSC0730771	C-ORIENTED SINGLE PHASE FILM	(Pb,Bi)2Sr2Ca2Cu3O10	Pb2Bi2Sr2Ca2Cu3O8+Z	Pb	2	Bi	2	Sr	2	Ca	2	Cu	3											O	8+Z		4	1990																												Bi2223																				107					107																																2.4	0.59						11.3	6																																																							0						MAGNETORESISTANCE AND THE COHERENCE LENGHT IN C-AXIS-ORIENTEDHIGH-TC PHASE (BI1-XPBX)2SR2CA2CU3O10+Y		COHERENCE LINGTH    ,FLUCTUATION	DEPARTMENT OF PHYSICS, KYUSHU UNIVERSITY, FUKUOKA 812, JAPAN	SOLID STATE COMMUN,73(1990)771	A.A.A.YOUSSEF,S.MASE,Y.HORIE	BI,PB,SR,CA,CU,O	
3932	SSC0720689		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1989																												T																			17		31.5				24.25													111																																																																																		1						ON THE ANOMALOUS MAGNETIC BEHAVIORS OF HIGH-TC OXIDES	198911		INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.72(1989)689	H. FUJISHITA,M. SATO,M. SERA,S. SHAMOTO	LA,SR,CU,O,NI,ND	
3933	SSC0720689		(La,Sr)2Cu04	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1989																												T																			24		36				30													105																																																																																		1						ON THE ANOMALOUS MAGNETIC BEHAVIORS OF HIGH-TC OXIDES	198911		INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.72(1989)689	H. FUJISHITA,M. SATO,M. SERA,S. SHAMOTO	LA,SR,CU,O,NI,ND	
3934	SSC0720689		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1989																												T'																			16	22	22				22													298																																																																																		1						ON THE ANOMALOUS MAGNETIC BEHAVIORS OF HIGH-TC OXIDES	198911		INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.72(1989)689	H. FUJISHITA,M. SATO,M. SERA,S. SHAMOTO	LA,SR,CU,O,NI,ND	
3935	SSC0720689		(La,Sr)2(Cu,Ni)04	La1.85Sr0.15Cu0.98Ni0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4		1	1989																												T																			12		25				18.5													38																																																																																		1						ON THE ANOMALOUS MAGNETIC BEHAVIORS OF HIGH-TC OXIDES	198911		INSTITUTE FOR MOLECULAR SCIENCE, MYODAIJI, OKAZAKI 444, JAPAN	SOLID STATE COMMUN.72(1989)689	H. FUJISHITA,M. SATO,M. SERA,S. SHAMOTO	LA,SR,CU,O,NI,ND	
3936	PHC1990001	SOLUBILITY LIMIT 0=< X =< 0.02	YBa2(Cu,Co)4O8	Y1Ba2Cu3.96Co0.04O8	Y	1	Ba	2	Cu	3.96	Co	0.04													O	8			1992	emu/g	-0.00000011			myu-B/mol	2.93	-16																					Y124				3.842	3.873	27.227													61		64			3	62.5																																																																																															0						SUBSTITUTION EFFECTS OF FE AND CO FOR CU IN YBA2(CU1-XMX)4O8 SUPERCONDUCTORS	199208			PHYSICA C,199(1992)1	S.TANEMURA,Y.KODAMA	FE,CO,Y,BA,CU,O	
3937	PHC1990001		YBa2(Cu,Co)4O8	Y1Ba2Cu3.92Co0.08O8	Y	1	Ba	2	Cu	3.92	Co	0.08													O	8			1992	emu/g	-0.00000006			myu-B/mol	3.18	7.4																					Y124				3.842	3.873	27.214													47.5		53.7			5	50.6																																																																																															0						SUBSTITUTION EFFECTS OF FE AND CO FOR CU IN YBA2(CU1-XMX)4O8 SUPERCONDUCTORS	199208			PHYSICA C,199(1992)1	S.TANEMURA,Y.KODAMA	FE,CO,Y,BA,CU,O	
3938	PHC1990001		YBa2(Cu,Fe)O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1992	emu/g	0.00000036			myu-B/mol	0.08	-34																					Y124				3.841	3.872	27.227															76.9			3.5	76.9																																																																																															0						SUBSTITUTION EFFECTS OF FE AND CO FOR CU IN YBA2(CU1-XMX)4O8 SUPERCONDUCTORS	199208			PHYSICA C,199(1992)1	S.TANEMURA,Y.KODAMA	FE,CO,Y,BA,CU,O	
3939	PHC1990001		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O	8			1992	emu/g	-0.00000004			myu-B/mol	3.58	-2.8																					Y124				3.842	3.873	27.221															64.6			12	64.6																																																																																															0						SUBSTITUTION EFFECTS OF FE AND CO FOR CU IN YBA2(CU1-XMX)4O8 SUPERCONDUCTORS	199208			PHYSICA C,199(1992)1	S.TANEMURA,Y.KODAMA	FE,CO,Y,BA,CU,O	
3940	PHC1990001		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.92Fe0.08O8	Y	1	Ba	2	Cu	3.92	Fe	0.08													O	8			1992	emu/g	-0.00000012			myu-B/mol	3.92	8.1																					Y124				3.843	3.874	27.195															50.4			24.3	50.4																																																																																															0						SUBSTITUTION EFFECTS OF FE AND CO FOR CU IN YBA2(CU1-XMX)4O8 SUPERCONDUCTORS	199208			PHYSICA C,199(1992)1	S.TANEMURA,Y.KODAMA	FE,CO,Y,BA,CU,O	
3941	PR04614101		Ba3(Pb,Bi)2O7	Ba3Pb2BiO7	Ba	3	Pb	2	Bi																O	7		1	1992																											2					4.293		21.732																	1.8																																																																																																	0						SYNTHESIS AND CHARACTERIZATION OF BA3(PB1-XBIX)2O7	199212			PHYS.REV.B,46(1992)14101	B.HESSEN,H.TAKAGI,H.W.ZANDBERGEN,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK	BA,PB,BI,O	
3942	PR04614101		Ba3(Pb,Bi)2O7	Ba3Pb1.6Bi0.4O7	Ba	3	Pb	1.6	Bi	0.4															O	7		1	1992																											2					4.304		21.795																	1.8																																																																																																	0						SYNTHESIS AND CHARACTERIZATION OF BA3(PB1-XBIX)2O7	199212			PHYS.REV.B,46(1992)14101	B.HESSEN,H.TAKAGI,H.W.ZANDBERGEN,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK	BA,PB,BI,O	
3943	PR04614101		Ba3(Pb,Bi)2O7	Ba3Pb1.4Bi0.6O7	Ba	3	Pb	1.4	Bi	0.6															O	7		1	1992																											2					4.311		21.814																	1.8																																																																																																	0						SYNTHESIS AND CHARACTERIZATION OF BA3(PB1-XBIX)2O7	199212			PHYS.REV.B,46(1992)14101	B.HESSEN,H.TAKAGI,H.W.ZANDBERGEN,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK	BA,PB,BI,O	
3944	PR04614101		Ba3(Pb,Bi)2O7	Ba3Pb1.2Bi0.8O7	Ba	3	Pb	1.2	Bi	0.8															O	7		1	1992																											2					4.313		21.827																	1.8																																																																																																	0						SYNTHESIS AND CHARACTERIZATION OF BA3(PB1-XBIX)2O7	199212			PHYS.REV.B,46(1992)14101	B.HESSEN,H.TAKAGI,H.W.ZANDBERGEN,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK	BA,PB,BI,O	
3945	PR04614101		Ba3(Pb,Bi)2O7	Ba3Pb1Bi1O7	Ba	3	Pb	1	Bi	1															O	7		1	1992																											2					4.318		21.859																	1.8																																																																																																	0						SYNTHESIS AND CHARACTERIZATION OF BA3(PB1-XBIX)2O7	199212			PHYS.REV.B,46(1992)14101	B.HESSEN,H.TAKAGI,H.W.ZANDBERGEN,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK	BA,PB,BI,O	
3946	PR04614230		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		4	1992																												T																				27.9					27.9																																100	0.67						42	0.28																																																							0						THERMALLY ACTIVATED RESISTIVE BEHAVIOR AND FLUX MOTION IN LA2-XSRXCUO4 SINGLE-CRYSTAL THIN FILMS	199212			PHYS.REV.B,46(1992)14230	MINORU SUZUKI	LA,SR,CU,O	
3947	PR04614230		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		4	1992																												T																				31.6					31.6																																13.9	0.98						32.6	2.31																																																							0						THERMALLY ACTIVATED RESISTIVE BEHAVIOR AND FLUX MOTION IN LA2-XSRXCUO4 SINGLE-CRYSTAL THIN FILMS	199212			PHYS.REV.B,46(1992)14230	MINORU SUZUKI	LA,SR,CU,O	
3948	PR04614230		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		4	1992																												T																				29.5					29.5																																10.53	0.9						35.2	3.01																																																							0						THERMALLY ACTIVATED RESISTIVE BEHAVIOR AND FLUX MOTION IN LA2-XSRXCUO4 SINGLE-CRYSTAL THIN FILMS	199212			PHYS.REV.B,46(1992)14230	MINORU SUZUKI	LA,SR,CU,O	
3949	PRL0673152		Bi2Sr2CaCu2O8	Bi2.1Sr1.94Ca0.88Cu2.07O8+Z	Bi	2.1	Sr	1.94	Ca	0.88	Cu	2.07													O	8+Z		1	1991																												Bi2212																				90					90																							9.76									0.738							48.4					4200																																																			0						MAGNETIC PENETRATION DEPTH AND FLUX DYUNAMICS IN SINGLE-CRYSTAL BI2SR2CACU2O8+Z	199111		AT&T BELL LABORATORIES,MURRAY HILL,NEW JERSEY 07974	PHYS.REV.LETT.,67(1991)3152	A.KAPITULNIK,D.B.MITZI,D.LI.WILLIAMS,D.R.HARSHMAN,G.P.ESPINOSA,M.INUI,R.N.KLEIMAN,T.PFIZ	BI,SR,CA,CU,O	
3950	PR04614290		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-Z	Sm	1.85	Ce	0.15	Cu	1															O	4-Z		3	1992																												T'																				19					19																																																																																															0						DETERMINATION OF THE UPPER CRITICAL FIELD OF THE ELECTRON-DOPED SUPERCONDUCTOR SM1.85CE0.15CUO4-Y FROM RESISTIVE FLUCTUATIONS	199212			PHYS.REV.B,46(1992)14290	C.C.ALMASAN,M.B.MAPLE,M.C.DE ANDRADE,S.H.HAN,Y.DALICHAOUCH	SM,CE,CU,O	
3951	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988																											3	Y123																				89.1					89.1																																																																														1.1																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3952	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.975Ni0.025O7-Z	Y	1	Ba	2	Cu	2.975	Ni	0.025													O	7-Z			1988																											3	Y123																				86.5					86.5																																																																														1.45																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3953	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.95Ni0.05O7-Z	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	7-Z			1988																											3	Y123																				84.7					84.7																																																																														1.9																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3954	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.925Ni0.075O7-Z	Y	1	Ba	2	Cu	2.925	Ni	0.075													O	7-Z			1988																											3	Y123																				82.1					82.1																																																																														2.42																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3955	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O7-Z	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z			1988																											3	Y123																				80.3					80.3																																																																														2.7																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3956	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.75Ni0.25O7-Z	Y	1	Ba	2	Cu	2.75	Ni	0.25													O	7-Z			1988																											3	Y123																				73.8					73.8																																																																														3.49																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3957	SSC0670031		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.5Ni0.5O7-Z	Y	1	Ba	2	Cu	2.5	Ni	0.5													O	7-Z			1988																											3	Y123																				61.8					61.8																																																																														5.05																	1						LACALIZATION OF THE ELECTRONS AND SUPERCONDUCTIVITY IN YBa2Cu3-xNixO7-y			Department of Physics, University of Science and Technology of China, Anhui, PR China	Solid State Commun.,67(1988)31-33	Chen Zuyao,Su Zhenpeng,Sun Shifang,Zhang Han,Zhang Qirui,Zhao Yong		
3958	SSC0670055	CURIET=-100K FROM EPR	Y2BaCuO5	Y2Ba1Cu1O5	Y	2	Ba	1	Cu	1															O	5			1988						1.7	-38	35																				Y211																																																																																																																								1						CONPARISON OF THE EPR OF THE ANTIFERROMAGNETS Y2BaCuO5 AND GdBaCuO5 AND THE HIGH Tc SUPERCONDUCTORS YBa2Cu3O7 AND GdBa2Cu3O7			IBM Research Division, T.J. Watson Reserch Center Yorktown Heights, NY 10598	Solid State Commun.,67(1988)55-59	E.A. Giess,F. Mehran,S.E. Barnes,T.R. McGuire		
3959	SSC0670055	CURIET=-20K FROM EPR	Gd2BaCuO5	Gd2Ba1Cu1O5	Gd	2	Ba	1	Cu	1															O	5			1988						8.4	-26	12																				Y211																																																																																																																								1						CONPARISON OF THE EPR OF THE ANTIFERROMAGNETS Y2BaCuO5 AND GdBaCuO5 AND THE HIGH Tc SUPERCONDUCTORS YBa2Cu3O7 AND GdBa2Cu3O7			IBM Research Division, T.J. Watson Reserch Center Yorktown Heights, NY 10598	Solid State Commun.,67(1988)55-59	E.A. Giess,F. Mehran,S.E. Barnes,T.R. McGuire		
3960	SSC0670119	DISTORTED RUTILE STRUCTURE		Nb1O2	Nb	1																			O	2			1988																																13.704		5.992																	4.2																																																																					-570																												0						SEARCH FOR SUPERCONDUCTIVITY IN NbO2-B SYSTEM			Chemistry Division, Bhabha Atomic Research Center, Bombay 400 085, India	Solid State Commun.,67(1988)119-122	C.V. Tomy,D.T. Adroja,M.P. Srinivasan,S.K. Malik,S.N. Vaidya		
3961	SSC0670119			Nb1B0.25O2	Nb	1	B	0.25																	O	2			1988																																13.683		5.99																	4.2																																																																					-130																												0						SEARCH FOR SUPERCONDUCTIVITY IN NbO2-B SYSTEM			Chemistry Division, Bhabha Atomic Research Center, Bombay 400 085, India	Solid State Commun.,67(1988)119-122	C.V. Tomy,D.T. Adroja,M.P. Srinivasan,S.K. Malik,S.N. Vaidya		
3962	SSC0670119			Nb1B0.4O2	Nb	1	B	0.4																	O	2			1988																																13.687		5.989																	4.2																																																																					5.2															20													0						SEARCH FOR SUPERCONDUCTIVITY IN NbO2-B SYSTEM			Chemistry Division, Bhabha Atomic Research Center, Bombay 400 085, India	Solid State Commun.,67(1988)119-122	C.V. Tomy,D.T. Adroja,M.P. Srinivasan,S.K. Malik,S.N. Vaidya		
3963	SSC0670119			Nb1B0.6O2	Nb	1	B	0.6																	O	2			1988																																13.733		6																	4.2																																																																					4															320													0						SEARCH FOR SUPERCONDUCTIVITY IN NbO2-B SYSTEM			Chemistry Division, Bhabha Atomic Research Center, Bombay 400 085, India	Solid State Commun.,67(1988)119-122	C.V. Tomy,D.T. Adroja,M.P. Srinivasan,S.K. Malik,S.N. Vaidya		
3964	SSC0670119			Nb1B2O2	Nb	1	B	2																	O	2			1988																																13.707		5.988																																																																																						-15																												0						SEARCH FOR SUPERCONDUCTIVITY IN NbO2-B SYSTEM			Chemistry Division, Bhabha Atomic Research Center, Bombay 400 085, India	Solid State Commun.,67(1988)119-122	C.V. Tomy,D.T. Adroja,M.P. Srinivasan,S.K. Malik,S.N. Vaidya		
3965	SSC0670257		La2CuO4	La2Cu1O4-Z	La	2	Cu	1																	O	4-Z		3	1988								230																				T				5.35	5.39	13.1																																																																																																						490												0	CUO FLUX METHOD,AS-GROWN					Electric Properties of La2CuO4-y			NTT Opto-Electronics Labolatories Ibaraki-ken Tokai 162, 319-11, Japan	Solid State Commun.,67(1988)257-261	K. Yamada,M. Oda,M. Suzuki,T. Murakami,Y. Endoh,Y. Enomoto,Y. Hidaka		
3966	SSC0670257		La2CuO4	La2Cu1O4-Z	La	2	Cu	1																	O	4-Z		3	1988								115																				T																																																																																																																								0	CUO FLUX METHOD,AS-GROWN					Electric Properties of La2CuO4-y			NTT Opto-Electronics Labolatories Ibaraki-ken Tokai 162, 319-11, Japan	Solid State Commun.,67(1988)257-261	K. Yamada,M. Oda,M. Suzuki,T. Murakami,Y. Endoh,Y. Enomoto,Y. Hidaka		
3967	SSC0670257		La2CuO4	La2Cu1O4-Z	La	2	Cu	1																	O	4-Z		3	1988								300																				T																																																																																																																								0	CUO FLUX METHOD,AS-GROWN					Electric Properties of La2CuO4-y			NTT Opto-Electronics Labolatories Ibaraki-ken Tokai 162, 319-11, Japan	Solid State Commun.,67(1988)257-261	K. Yamada,M. Oda,M. Suzuki,T. Murakami,Y. Endoh,Y. Enomoto,Y. Hidaka		
3968	SSC0670521		GdBa2Cu3O7	Gd1Ba2Cu3O7+Z	Gd	1	Ba	2	Cu	3															O	7+Z		1	1988						7.89	3.4																				3	Y123				3.838	3.9	11.699														89					89																																																																																															0						SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
3969	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.925Fe0.075O7+Z	Gd	1	Ba	2	Cu	2.925	Fe	0.075													O	7+Z		1	1988						8.08	1.8																				3	Y123				3.871	3.897	11.684														64					64																																																																																															0						SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
3970	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.85Fe0.15O7+Z	Gd	1	Ba	2	Cu	2.85	Fe	0.15													O	7+Z		1	1988						8.13	-4.3																				3	Y123				3.874	3.891	11.67														47					47																																																																																															0						SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
3971	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.775Fe0.225O7+Z	Gd	1	Ba	2	Cu	2.775	Fe	0.225													O	7+Z		1	1988						8.18	-3.8																				2	Y123				3.884		11.661														33					33																																																																																															0						SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
3972	SSC0670521		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O7+Z	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	7+Z		1	1988						8.23	2.7																				2	Y123				3.886	3.882	11.652														11					11																																																																																															0						SUPERCONDUCTING AND MAGNETIC STUDIES ON GDBA2(CU1-XFEX)3O7+Z OXIDE SYSTEM				SOLID STATE COMMUN.67(1988)521	C.V.TOMY,D.T.ADROJA,N.C.SONI,R.NAGARAJAN,RAM PRASAD,S.K.DHAR,S.K.MALIK	GD,BA,CU,FE,O	
3973	SSC0670609		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1988																												Bi2212				5.4	27.01	30.82													90	93					93																																																																																			0.45											BI2O3,SRCO3,CACO3,CUO	0	HEAT(900C 2H IN PT CRUCIBLE)-COOL TO 800C AT 5C/H-FC					ANISOTROPY OF THE SUPERCONDUCTING PROPERTIES OF Bi2Sr2CaCu2O8			Service National des Champs Intenses, Centre National de la Recherche Scientifique, BP 166 X, 38042 Grenoble-Ce'dex, France	Solid State Commun.,67(1988)609-611	H. Noel,J. Padiou,J.C. Levet,M. Potel,O. Laborde,P. Gougeon,P. Monceau		
3974	SSC0670707	81% O(18), DELTA TC=0.41K	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1988																												T																				37					37						0.14	O	81	0.41																																																																																					LA2O3,SRCO3,CUO	1	O(18) BY GAS DIFFUSION METHOD					MAGNETIC AND RESISTIVE DETERMINATION OF THE OXYGEN ISOTOPE EFFECT IN La1.85Sr0.15CuO4			Department of Physics, University of California at Berkeley, and Materials and Chemical Sciences Division, Lawrence Berkeley Laboratories, Berkeley, California 94720	Solid State Commun.,67(1988)707-711	A. Zettl,Donald E. Morris,John Kinney,L.C. Bourne,Luis Bernardez,M.F. Crommie,Marvin L. Cohen,S. Hoen,W.N. Creager		
3975	SSC0670815	CARRIER=E+21/CM3	Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca3Cu4OY	Bi	4	Sr	3	Ca	3	Cu	4													O	Y		1	1988																											2					5.39		30.628														75.6					75.6																																																																																		4.44				0.00000000188				1.5			3.309	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3976	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca2.7Y0.3Cu4OY	Bi	4	Sr	3	Ca	2.7	Y	0.3	Cu	4											O	Y		1	1988																																5.405		30.645														81.7					81.7																																																																																		9.21				0.00000000313				1.5			1.991	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3977	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca2.55Y0.45Cu4OY	Bi	4	Sr	3	Ca	2.55	Y	0.45	Cu	4											O	Y		1	1988																																5.411		30.69														85.8					85.8																																																																																		11.26				0.0000000026				1.5			2.4	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3978	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca2.4Y0.6Cu4OY	Bi	4	Sr	3	Ca	2.4	Y	0.6	Cu	4											O	Y		1	1988																																5.413		30.579														79.7					79.7																																																																																		35.15				0.00000000364				1.5			1.714	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3979	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca2.25Y0.75Cu4OY	Bi	4	Sr	3	Ca	2.25	Y	0.75	Cu	4											O	Y		1	1988																																5.414		30.394														89.8					89.8																																																																																		16.72				0.00000000447				1.5			1.397	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3980	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca2.1Y0.9Cu4OY	Bi	4	Sr	3	Ca	2.1	Y	0.9	Cu	4											O	Y		1	1988																																5.425		30.538														66.2					66.2																																																																																		18.77												BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3981	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca1.95Y1.05Cu4OY	Bi	4	Sr	3	Ca	1.95	Y	1.05	Cu	4											O	Y		1	1988																																5.428		30.449														25.6					25.6																																																																																		83.61												BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3982	SSC0670815		Bi4Sr3(Ca,Y)3Cu4OZ	Bi4Sr3Ca1.8Y1.2Cu4OY	Bi	4	Sr	3	Ca	1.8	Y	1.2	Cu	4											O	Y		1	1988																																5.428		30.422														0.3					0.3																																																																																		142.3				0.00000000697				1.5			0.896	BI2O3,SRCO3,CACO3,Y2O3,CUO	0						STUDY ON NORMAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3(Ca1-xYx)3 Cu4Oy			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Solid State Commun.,67(1988)815-819	K. Fukuda,M. Onoda,M. Sato,M. Sera,S. Kondoh,Y. Ando		
3983	SSC0670959		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1988																											3	Y123																				83				7	83			K/GPa	0.8																																																																																											1	PREPARED BY ASSUMIE ET.AL.(AL2O3 CRUCIBLE)					PRESSURE DEPENDENCE OF Tc FOR SINGLE CRYSTAL YBa2Cu3O7-x UP TO 10 GPa			"Institut fu""r Festko""rperforschung, KFA Ju""lich, D-5170 Ju""lich"	Solid State Commun.,67(1988)959-963	B. Gegenheimer,J. Wittg,K. Winzer,N. Lotter,U. Koch,W. Assmus		
3984	SSC0670959		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1988																											3	Y123																				91				1	91			K/GPA	-0.8																																																																																											1	PREPARED BY WINZER ET.AL.(PT CRUCIBLE)					PRESSURE DEPENDENCE OF Tc FOR SINGLE CRYSTAL YBa2Cu3O7-x UP TO 10 GPa			"Institut fu""r Festko""rperforschung, KFA Ju""lich, D-5170 Ju""lich"	Solid State Commun.,67(1988)959-963	B. Gegenheimer,J. Wittg,K. Winzer,N. Lotter,U. Koch,W. Assmus		
3987	SSC0730511	NEW TYPE S/C	Y2(Ba,Ca)2Cu3O8	Y2Ba1.5Ca0.5Cu3O8+Z	Y	2	Ba	1.5	Ca	0.5	Cu	3													O	8+Z			1990																											3	Y223				4.059	3.722	13.065													78	80	82			4	80																																																																																															1	MIXTURE HEATED IN AIR AT 950C,THEN SLOW COOLED TO RT					NEW HIGH-TC 2-2-3 TYPE SUPERCONDUCTOR Y2BA1.5CA0.5CU3O8+Z		NEW MATERIAL        ,SINGLE-PHASE        ,SUSCEPTIBILITY      ,RESISTANCE	PHYSICS DEPARTMENT, SAURASHTRA UNIVERSITY, RAJKOT-360 005, INDIA	SOLID STATE COMMUN,73(1990)511	BV.SKUMRYEV,G.J.BALDHA,H.H.JOSHI,H.MOHAN,K.V.RAO,R.B.JOTANIA,R.G.KULKARNI	Y,BA,CA,CU,O	
3988	SSC0730515	SE SUBSTITUTED BY O FOR X=0.3,CONTENTS ANALYZED BY MASS SPECTR.	YBa2Cu3(O,Se)7	Y1Ba2Cu3Se0.25OZ	Y	1	Ba	2	Cu	3	Se	0.25													O	Z		1	1990																											2	Y123																				40					40																																																																																														BACO3,CUO,CUSE	0						EFFECT OF SUBSTITUTION OF O BY SE ON THE SUPERCONDUCTIVITY OFYBA2CU3O7		MAGNETOMETRY        ,SELENIUM            ,XRY	INSTITUTE OF PHUSICS, SILESIAN UNIVERSITY, UNIWERSYTECKA 4, 40-007 KATOWICE, POLAND	SOLID STATE COMMUN,73(1990)515	A,A.CHELKOWSKI,A.SLEBARSKI,J.JELONEK,KASPRZYK	SE,Y,BA,CU,O	
3989	SSC0730515		YBa2Cu3(O,Se)7	Y1Ba2Cu3Se0.5OZ	Y	1	Ba	2	Cu	3	Se	0.5													O	Z		2	1990																											2	Y123																				92					92																																																																																															0						EFFECT OF SUBSTITUTION OF O BY SE ON THE SUPERCONDUCTIVITY OFYBA2CU3O7		MAGNETOMETRY        ,SELENIUM            ,XRY	INSTITUTE OF PHUSICS, SILESIAN UNIVERSITY, UNIWERSYTECKA 4, 40-007 KATOWICE, POLAND	SOLID STATE COMMUN,73(1990)515	A,A.CHELKOWSKI,A.SLEBARSKI,J.JELONEK,KASPRZYK	SE,Y,BA,CU,O	
3990	SSC0730629	NOT S/C, STRUCTURE BY NEUTRON DIFFRACTION	Ba4CaCu3O8	Ba4Ca1Cu3O8.61	Ba	4	Ca	1	Cu	3															O	8.61		1	1990																											1					8.124																																																																																																																				0	MIXTURE-HEATED AT 980C 14H IN O2,THEN REHEATED AT 1015C 14H IN O2					SYNTHESIS AND STRUCTURAL CHARACTERISATION OF A NEW PEROVSKITEPHASE, BA4CACU3O8.61		NEW PHASE           ,STRUCTURE           ,NEUTRON DIFFRACTION ,OXYGEN VACANCIES	SUPERCONDUCTIVITY RESEARCH GROUP, SCHOOL OF CHEMISTRY, UNIVERSITY OF BIRMINGHAM, BIRMINGHAM B15 2TT, ENGLAND	SOLID STATE COMMUN,73(1990)629	C.GREAVES,P.R.SLATER	CA,BA,CU,O	
3991	SSC0720529	CARRIER IN E+21/CM3		La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1989																											2					3.784		13.22														31					31																																																																																						0.00000000344							1.816								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
3992	SSC0720529	CARRIER IN E+21/CM3		La1.9Sr0.1Cu0.975Ni0.025O4	La	1.9	Sr	0.1	Cu	0.975	Ni	0.025													O	4		1	1989																											2					3.785		13.197														3.65					3.65																																																																																						0.00000000382							1.632								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
3993	SSC0720529	CARRIER IN E+21/CM3		La1.9Sr0.1Cu0.97Ni0.03O4	La	1.9	Sr	0.1	Cu	0.97	Ni	0.03													O	4		1	1989																											2					3.786		13.194														3.65					3.65																																																																																						0.00000000369							1.693								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
3994	SSC0720529	CARRIER IN E+21/CM3		La1.9Sr0.1Cu0.96Ni0.04O4	La	1.9	Sr	0.1	Cu	0.96	Ni	0.04													O	4		1	1989																											2					3.788		13.197																																																																																																									0.00000000422							1.478								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
3995	PR0468694	CARRIER IN E+21/CM3		Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1992																											3	Y123																				91.4					91.4																																																																																			0.237										2.01								HALL-EFFECT STUDIES OF Y1-XPRXBA2CU3O7 CRYSTALS	199210		CENTER FOR SUPERCONDUCTIVITY RESEARCH, DEPARTMENT OF PHYSICS,UNIVERSITY OF MARYLAND	PHYS.REV.B,46(1992)8694	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU JIANG	Y,PR,BA,CU,O	
3996	PR0468694	CARRIER IN E+21/CM3		Y0.87Pr0.13Ba2Cu3O7	Y	0.87	Pr	0.13	Ba	2	Cu	3													O	7		3	1992																											3	Y123																				78.35					78.35																																																																																			0.275										1.66								HALL-EFFECT STUDIES OF Y1-XPRXBA2CU3O7 CRYSTALS	199210		CENTER FOR SUPERCONDUCTIVITY RESEARCH, DEPARTMENT OF PHYSICS,UNIVERSITY OF MARYLAND	PHYS.REV.B,46(1992)8694	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU JIANG	Y,PR,BA,CU,O	
3997	PR0468694	CARRIER IN E+21/CM3		Y0.7Pr0.3Ba2Cu3O7	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7		3	1992																											3	Y123																				55.67					55.67																																																																																			0.459										1.1								HALL-EFFECT STUDIES OF Y1-XPRXBA2CU3O7 CRYSTALS	199210		CENTER FOR SUPERCONDUCTIVITY RESEARCH, DEPARTMENT OF PHYSICS,UNIVERSITY OF MARYLAND	PHYS.REV.B,46(1992)8694	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU JIANG	Y,PR,BA,CU,O	
3998	PR0468694	CARRIER IN E+21/CM3		Y0.5Pr0.5Ba2Cu3O7	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7		3	1992																											3	Y123																				23.36					23.36																																																																																			0.632										0.87								HALL-EFFECT STUDIES OF Y1-XPRXBA2CU3O7 CRYSTALS	199210		CENTER FOR SUPERCONDUCTIVITY RESEARCH, DEPARTMENT OF PHYSICS,UNIVERSITY OF MARYLAND	PHYS.REV.B,46(1992)8694	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU JIANG	Y,PR,BA,CU,O	
3999	PR0468694	CARRIER IN E+21/CM3		Y0.45Pr0.55Ba2Cu3O7	Y	0.45	Pr	0.55	Ba	2	Cu	3													O	7		3	1992																											3	Y123																																																																																																																						0.351								HALL-EFFECT STUDIES OF Y1-XPRXBA2CU3O7 CRYSTALS	199210		CENTER FOR SUPERCONDUCTIVITY RESEARCH, DEPARTMENT OF PHYSICS,UNIVERSITY OF MARYLAND	PHYS.REV.B,46(1992)8694	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU JIANG	Y,PR,BA,CU,O	
4000	SSC0820889	FIGURE=TC VS SR-CONTENT	(La,Sr)2(Cu,Ni)O4	La1.855Sr0.145Cu0.99Ni0.01O4	La	1.855	Sr	0.145	Cu	0.99	Ni	0.01													O	4		1	1992																												T																		K		33					33	TC4000																																																																																																				ANOMALOUS X DEPENDENCE OF TC AND POSSIBILITY OF LOW-TEMPERATURE STRUCTURAL PHASE TRANSITION IN LA2-XSRXCU0.99M0.01O4 (M=NI,ZN,GA)				SOLID STATE COMMUN.82(1992)889	A.KOBAYASHI,M.KATO,T.HIKITA,T.KAWAGUCHI,T.NOJI,Y.KOIKE,Y.ONO,Y.SAITO	LA,SR,CU,NI,ZN,GA,O	
4001	SSC0820889	FIGURE=TC VS SR-CONTENT	(La,Sr)2(Cu,Zn)O4	La1.855Sr0.145Cu0.99Zn0.01O4	La	1.855	Sr	0.145	Cu	0.99	Zn	0.01													O	4		1	1992																												T																		K		24.7					24.7	TC4001																																																																																																				ANOMALOUS X DEPENDENCE OF TC AND POSSIBILITY OF LOW-TEMPERATURE STRUCTURAL PHASE TRANSITION IN LA2-XSRXCU0.99M0.01O4 (M=NI,ZN,GA)				SOLID STATE COMMUN.82(1992)889	A.KOBAYASHI,M.KATO,T.HIKITA,T.KAWAGUCHI,T.NOJI,Y.KOIKE,Y.ONO,Y.SAITO	LA,SR,CU,NI,ZN,GA,O	
4002	SSC0820889	FIGURE=TC VS SR-CONTENT	(La,Sr)2CuO4	La1.836Sr0.164Cu1O4	La	1.836	Sr	0.164	Cu	1															O	4		1	1992																												T																		K		36.9					36.9	TC4002																																																																																																				ANOMALOUS X DEPENDENCE OF TC AND POSSIBILITY OF LOW-TEMPERATURE STRUCTURAL PHASE TRANSITION IN LA2-XSRXCU0.99M0.01O4 (M=NI,ZN,GA)				SOLID STATE COMMUN.82(1992)889	A.KOBAYASHI,M.KATO,T.HIKITA,T.KAWAGUCHI,T.NOJI,Y.KOIKE,Y.ONO,Y.SAITO	LA,SR,CU,NI,ZN,GA,O	
4003	SSC0820889	FIGURE=TC VS SR-CONTENT	(La,Sr)2(Cu,Ga)O4	La1.836Sr0.164Cu0.99Ga0.01O4	La	1.836	Sr	0.164	Cu	0.99	Ga	0.01													O	4		1	1992																												T																		K		26.9					26.9	TC4003																																																																																																				ANOMALOUS X DEPENDENCE OF TC AND POSSIBILITY OF LOW-TEMPERATURE STRUCTURAL PHASE TRANSITION IN LA2-XSRXCU0.99M0.01O4 (M=NI,ZN,GA)				SOLID STATE COMMUN.82(1992)889	A.KOBAYASHI,M.KATO,T.HIKITA,T.KAWAGUCHI,T.NOJI,Y.KOIKE,Y.ONO,Y.SAITO	LA,SR,CU,NI,ZN,GA,O	
4004	PR04614293	AS-GROWN,HALLFIG(P=1 FOR //PLANE,P=2 FOR NORMAL TO PLANE)		Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1992																											3	Y123																				91					91																																																																																											RH4004										EXPERIMENTAL TEST OF THE T2 LAW FOR THE HALL ANGLE FROM TC TO500 K IN OXYGEN-REDUCED YBA2CU3O6+X CRYSTALS	199212			PHYS.REV.B,46(1992)14293	J.M.HARRIS,N.P.ONG,Y.F.YAN	Y,BA,CU,O	
4005	PR04614293	QUENCH FROM 620K		Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1992																											3	Y123																				74					74																																																																																											RH4005										EXPERIMENTAL TEST OF THE T2 LAW FOR THE HALL ANGLE FROM TC TO500 K IN OXYGEN-REDUCED YBA2CU3O6+X CRYSTALS	199212			PHYS.REV.B,46(1992)14293	J.M.HARRIS,N.P.ONG,Y.F.YAN	Y,BA,CU,O	
4006	PR04614293	QUENCH FROM 650K		Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1992																											3	Y123																				60					60																																																																																											RH4006										EXPERIMENTAL TEST OF THE T2 LAW FOR THE HALL ANGLE FROM TC TO500 K IN OXYGEN-REDUCED YBA2CU3O6+X CRYSTALS	199212			PHYS.REV.B,46(1992)14293	J.M.HARRIS,N.P.ONG,Y.F.YAN	Y,BA,CU,O	
4007	PR0465841	Structural phase transition at 77K. 		La1.6Nd0.4Cu1O4	La	1.6	Nd	0.4	Cu	1															O	4		3	1992								306																				T																							10																																																																																												5											ANISOTROPIC TRANSPORT PROPERTIES OF SINGLE-CRYSTAL LA2-X-YNDYSRXCUO4: EFFECT OF THE STRUCTURAL PHASE TRANSITION	199209		SUPERCONDUCTIVITY RESEARCH COURSE, THE UNIVERSITY OF TOKYO	PHYS.REV.B,46(1992)5841	S.UCHIDA,Y.NAKAMURA	LA,ND,SR,CU,O	
4008	PR0465841	TRANSPORT PROPERTIES JUMP AT T0,T0=71K(LTO TO LTT)		La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	1992																												T																				8.3					8.3																																																																						TP4008				230									0.63							5	RH4008										ANISOTROPIC TRANSPORT PROPERTIES OF SINGLE-CRYSTAL LA2-X-YNDYSRXCUO4: EFFECT OF THE STRUCTURAL PHASE TRANSITION	199209		SUPERCONDUCTIVITY RESEARCH COURSE, THE UNIVERSITY OF TOKYO	PHYS.REV.B,46(1992)5841	S.UCHIDA,Y.NAKAMURA	LA,ND,SR,CU,O	
4009	PR0465841	T0=79K(LTO TO LTT)		La1.4Nd0.4Sr0.2Cu1O4	La	1.4	Nd	0.4	Sr	0.2	Cu	1													O	4		3	1992																												T																				21.7					21.7																																																																						TP4009				45									0.27							5	RH4009										ANISOTROPIC TRANSPORT PROPERTIES OF SINGLE-CRYSTAL LA2-X-YNDYSRXCUO4: EFFECT OF THE STRUCTURAL PHASE TRANSITION	199209		SUPERCONDUCTIVITY RESEARCH COURSE, THE UNIVERSITY OF TOKYO	PHYS.REV.B,46(1992)5841	S.UCHIDA,Y.NAKAMURA	LA,ND,SR,CU,O	
4010	SSC0830895		TlSr2CaCu2(O,F)z	Tl1Sr2Ca1Cu2OZ	Tl	1	Sr	2	Ca	1	Cu	2													O	Z			1992																											2	Tl1212				3.781		12.06													35						35																																																																																														TL2O3,SRO,CAO,SRF2	0	MIXTURE-(900-1000C 24H IN AIR)-PELLET-(950-1000C 10-30MIN IN O2 IN ALUMINA)-Q IN AIR					EFFECTS OF F-DOPING AND CL-DOPING ON FORMATION AND SUPERCONDUCTIVITY OF THE 1212-TYPE PHASE TISR2CACU2O7	199209	TL                  ,SR                  ,CA                  ,CU                  ,O                   ,F                   ,CL	DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS	SOLID STATE COMMUN.,83(1992)895	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG		
4011	SSC0830895		TlSr2CaCu2(O,F)z	Tl1Sr2Ca1Cu2F0.2OZ	Tl	1	Sr	2	Ca	1	Cu	2	F	0.2											O	Z			1992																											2	Tl1212				3.782		12.04													40						40																																																																																														TL2O3,SRO,CAO,SRF2	0	MIXTURE-(900-1000C 24H IN AIR)-PELLET-(950-1000C 10-30MIN IN O2 IN ALUMINA)-Q IN AIR					EFFECTS OF F-DOPING AND CL-DOPING ON FORMATION AND SUPERCONDUCTIVITY OF THE 1212-TYPE PHASE TISR2CACU2O7	199209	TL                  ,SR                  ,CA                  ,CU                  ,O                   ,F                   ,CL	DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS	SOLID STATE COMMUN.,83(1992)895	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG		
4012	SSC0830895		TlSr2CaCu2(O,F)z	Tl1Sr2Ca1Cu2F0.5OZ	Tl	1	Sr	2	Ca	1	Cu	2	F	0.5											O	Z			1992																											2	Tl1212				3.783		12.04													50						50																																																																																														TL2O3,SRO,CAO,SRF2	0	MIXTURE-(900-1000C 24H IN AIR)-PELLET-(950-1000C 10-30MIN IN O2 IN ALUMINA)-Q IN AIR					EFFECTS OF F-DOPING AND CL-DOPING ON FORMATION AND SUPERCONDUCTIVITY OF THE 1212-TYPE PHASE TISR2CACU2O7	199209	TL                  ,SR                  ,CA                  ,CU                  ,O                   ,F                   ,CL	DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS	SOLID STATE COMMUN.,83(1992)895	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG		
4013	SSC0830895		TlSr2CaCu2(O,F)z	Tl1Sr2Ca1Cu2F1OZ	Tl	1	Sr	2	Ca	1	Cu	2	F	1											O	Z			1992																											2	Tl1212				3.788		12.03													50						50																																																																																														TL2O3,SRO,CAO,SRF2	0	MIXTURE-(900-1000C 24H IN AIR)-PELLET-(950-1000C 10-30MIN IN O2 IN ALUMINA)-Q IN AIR					EFFECTS OF F-DOPING AND CL-DOPING ON FORMATION AND SUPERCONDUCTIVITY OF THE 1212-TYPE PHASE TISR2CACU2O7	199209	TL                  ,SR                  ,CA                  ,CU                  ,O                   ,F                   ,CL	DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS	SOLID STATE COMMUN.,83(1992)895	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG		
4014	SSC0830895		TlSr2CaCu2(O,F)z	Tl1Sr2Ca1Cu2F1.5OZ	Tl	1	Sr	2	Ca	1	Cu	2	F	1.5											O	Z			1992																											2	Tl1212				3.789		12.04													50						50																																																																																														TL2O3,SRO,CAO,SRF2	0	MIXTURE-(900-1000C 24H IN AIR)-PELLET-(950-1000C 10-30MIN IN O2 IN ALUMINA)-Q IN AIR					EFFECTS OF F-DOPING AND CL-DOPING ON FORMATION AND SUPERCONDUCTIVITY OF THE 1212-TYPE PHASE TISR2CACU2O7	199209	TL                  ,SR                  ,CA                  ,CU                  ,O                   ,F                   ,CL	DEPARTMENT OF PHYSICS, UNIVERSITY OF ARKANSAS	SOLID STATE COMMUN.,83(1992)895	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG		
4015	SSC0720529	CARRIER(N)=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1989																												T				3.78		13.241														35.7					35.7																																																																																						0.00000000126							4.937								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4016	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4			1989																												T				3.779		13.235														30.1					30.1																																																																																						0.0000000013							4.786								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4017	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4			1989																												T				3.78		13.227														23.7					23.7																																																																																						0.00000000161							3.881								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4018	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4			1989																												T				3.779		13.22														16.3					16.3																																																																																						0.00000000178							3.505								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4019	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.96Ni0.04O4	La	1.85	Sr	0.15	Cu	0.96	Ni	0.04													O	4			1989																												T				3.783		13.222														6.4					6.4																																																																																						0.00000000146							4.258								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4020	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.95Ni0.05O4	La	1.85	Sr	0.15	Cu	0.95	Ni	0.05													O	4			1989																												T				3.783		13.215																																																																																																									0.00000000195							3.203								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4021	SSC0720529		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.99Ni0.01O4	La	1.78	Sr	0.22	Cu	0.99	Ni	0.01													O	4			1989																												T																				21.3					21.3																																																																																																					COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4022	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.98Ni0.02O4	La	1.78	Sr	0.22	Cu	0.98	Ni	0.02													O	4			1989																												T																				17.7					17.7																																																																																						0.000000000414							15.1								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4023	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.97Ni0.03O4	La	1.78	Sr	0.22	Cu	0.97	Ni	0.03													O	4			1989																												T																				14					14																																																																																						0.000000000481							13								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4024	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.96Ni0.04O4	La	1.78	Sr	0.22	Cu	0.96	Ni	0.04													O	4			1989																												T																				7.9					7.9																																																																																						0.000000000481							13								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4025	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.95Ni0.05O4	La	1.78	Sr	0.22	Cu	0.95	Ni	0.05													O	4			1989																												T																				4.1					4.1																																																																																						0.00000000059							10.6								COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4026	SSC0720529	N=IN E+21/CM3	(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4			1989																												T																				24.6					24.6																																																																																																					COMPARISON OF THE NORMAL STATE PROPERTIES BETWEEN THE SUPERCONDUCTING AND THE NONSUPERCONDUCTING METALLIC PHASES IN LA2-YSRYCUL-XNIXO4	198911	STRUCTURE           ,RESISTIVITY         ,LOCALIZATION        ,HALL COEFFICIENT    ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS, COLLEGE OF LIBERAL ARTS, KANAZAWA UNIVERSITY, KANAZAWA 920 JAPAN	SOLID STATE COMMUN.,72(1989)529	HIDESHI FUJISHITA,MASATOSHI SATO	LA,SR,CU,NI,O	
4027	SSC0820885		Bi2Sr2(Ca,Ho)Cu2O8	Bi2Sr2Ca0.9Ho0.1Cu2OZ	Bi	2	Sr	2	Ca	0.9	Ho	0.1	Cu	2											O	Z		1	1992																												Bi2212																																																																																																																							BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4028	SSC0820885		Bi2Sr2(Cu,Ho)Cu2O8	Bi2Sr2Ca0.8Ho0.2Cu2OZ	Bi	2	Sr	2	Ca	0.8	Ho	0.2	Cu	2											O	Z		1	1992																												Bi2212																			80						80																																																																						TP4028																								BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4029	SSC0820885		Bi2Sr2(Ca,Ho)Cu2O8	Bi2Sr2Ca0.7Ho0.3Cu2OZ	Bi	2	Sr	2	Ca	0.7	Ho	0.3	Cu	2											O	Z		1	1992																												Bi2212																																																																																															TP4029																								BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4030	SSC0820885		Bi2Sr2(Ca,Ho)Cu2O8	Bi2Sr2Ca0.6Ho0.4Cu2OZ	Bi	2	Sr	2	Ca	0.6	Ho	0.4	Cu	2											O	Z		1	1992																												Bi2212																																																																																																																							BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4031	SSC0820885		Bi2Sr2(Ca,Ho)Cu2O8	Bi2Sr2Ca0.5Ho0.5Cu2OZ	Bi	2	Sr	2	Ca	0.5	Ho	0.5	Cu	2											O	Z		1	1992																												Bi2212																																																																																																																							BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4032	SSC0820885		Bi2Sr2(Ca,Ho)Cu2O8	Bi2Sr2Ca0.4Ho0.6Cu2OZ	Bi	2	Sr	2	Ca	0.4	Ho	0.6	Cu	2											O	Z		1	1992																												Bi2212																																																																																																																							BI2O3,SRCO3,CACO3,HO2O3,CUO	1	MIXTURE-CAL(830C 12H)-SIN(900-910C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4033	SSC0820885		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		1	1992																												Bi2212																			74						74																																																																						TP4033																									0	MIXTURE-CAL(860C 12H)-SIN(870C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4034	SSC0820885	INSULATOR,NO MAGNETIC ORDERING FROM 300 TO 5K	Bi2Sr2HoCu2O8	Bi2Sr2Ho1Cu2OZ	Bi	2	Sr	2	Ho	1	Cu	2													O	Z		1	1992																												Bi2212																																																																																																																								0	MIXTURE-CAL(860C 12H)-SIN(870C 12H)					NORMAL STATE AND SUPERCONDUCTING PROPERTIES OF BI2SR2CA1-XHOXCU2OY COMPOUNDS				SOLID STATE COMMUN.82(1992)885	C.SCHLENKER,G.V.SUBBA RAO,S.LAKSHMI RAGHAVAN	BI,SR,CA,HO,CU,O	
4035	PR04614928		YBa2(Cu,Co)3O7	Y1Ba2Cu2.79Co0.21O7-Z	Y	1	Ba	2	Cu	2.79	Co	0.21													O	7-Z			1992																												Y123																																																																																												29.1			TP4035																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4036	PR04614928		YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7-Z	Y	1	Ba	2	Cu	2.88	Co	0.12													O	7-Z			1992																												Y123																																																																																												11.7			TP4036																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4037	PR04614928		YBa2(Cu,Co)3O7	Y1Ba2Cu2.916Co0.084O7-Z	Y	1	Ba	2	Cu	2.916	Co	0.084													O	7-Z			1992																												Y123																																																																																												8.86			TP4037																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4038	PR04614928		YBa2(Cu,Co)3O7	Y1Ba2Cu2.955Co0.045O7-Z	Y	1	Ba	2	Cu	2.955	Co	0.045													O	7-Z			1992																												Y123																																																																																												8.56			TP4038																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4039	PR04614928		YBa2(Cu,Co)3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1992																												Y123																																																																																												-3.13			TP4039																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4040	PR04614928		YBa2Cu3O7	Y1Ba2Cu3O6.13	Y	1	Ba	2	Cu	3															O	6.13			1992																												Y123																																																																																																																														SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4041	PR04614928		YBa2Cu3O7	Y1Ba2Cu3O6.23	Y	1	Ba	2	Cu	3															O	6.23			1992																												Y123																																																																																																																														SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4042	PR04614928		YBa2Cu3O7	Y1Ba2Cu3O6.36	Y	1	Ba	2	Cu	3															O	6.36			1992																												Y123																																																																																												74.8			TP4042																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4043	PR04614928		YBa2Cu3O7	Y1Ba2Cu3O6.48	Y	1	Ba	2	Cu	3															O	6.48			1992																												Y123																				48					48																																																																																																					SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4044	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.077	Bi	2	Sr	2	Ca	1	Cu	2													O	8.077			1992																												Bi2212																																																																																												-5.75			TP4044																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4045	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.051	Bi	2	Sr	2	Ca	1	Cu	2													O	8.051			1992																												Bi2212																																																																																												-4			TP4045																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4046	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.01	Bi	2	Sr	2	Ca	1	Cu	2													O	8.01			1992																												Bi2212																																																																																												2.71			TP4046																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4047	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O7.93	Bi	2	Sr	2	Ca	1	Cu	2													O	7.93			1992																												Bi2212																																																																																												3.63			TP4047																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4048	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O7.975	Bi	2	Sr	2	Ca	1	Cu	2													O	7.975			1992																												Bi2212																																																																																												5.66			TP4048																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4049	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O7.965	Bi	2	Sr	2	Ca	1	Cu	2													O	7.965			1992																												Bi2212																																																																																												7.37																																		SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4050	PR04614928		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1992																												Bi2212																																																																																												1.16			TP4050																															SYSTEMATICS IN THE THERMOELECTRIC POWER OF HIGH-TC OXIDES	199212		INTERDISCIPLINARY RESEARCH CENTRE IN SUPERCONDUCTIVITY, UNITEDKINGDOM	PHYS.REV.B,46(1992)14928	J.L.TALLON,J.R.COOPER,S.D.OBERTELLI	BI,SR,CA,CU,TL,BA,O	
4051	PR04614936		K3C60	C60K3	C	60	K	3																					1992																												K3C60																				19.5					19.5																					RF TECHNIQUE IN PULSED FIELD,SPIN-ORBIT PARAMETER=1	32.7									2.8							31																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
4052	PR04614936		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												K3C60																				28.4					28.4																					RF TECHNIQUE IN PULSED FIELD, SPIN-ORBIT PARAMETER=0.7	57.4									3.86							24																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
4053	SSC0830689		Bi2Sr2(Ca,Dy)Cu2O8	Bi2Sr2Ca0.9Dy0.1Cu2O8+Z	Bi	2	Sr	2	Ca	0.9	Dy	0.1	Cu	2											O	8+Z		1	1992	emu/g	-0.0019					-10																				2	Bi2212			A	5.413		30.871														93		93			93																																																																																														BI2O3,SRCO3,CACO3,DY2CO3,CUO	1	MIXTURE-CAL(800C 24H)-SIN(850C-900C)-Q TO LN2					MGNETISM AND SUPERCONDUCTIVITY IN THE 2:2:1:2 BISMUTH CUPRATEBY DYSPROSIUM SUBSTITUTION (BI2SR2CA1-XDYXCU2O8+Z)				SOLID STATE COMMUN.83(1992)689	E.LAXMI NARSAIAH,U.V.SUBBA RAO	BI,SR,CA,DY,CU,O	
4054	SSC0830689		Bi2Sr2(Ca,Dy)Cu2O8	Bi2Sr2Ca0.8Dy0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	Dy	0.2	Cu	2											O	8+Z		1	1992	emu/g	-0.0012					-7																				2	Bi2212			A	5.418		30.809														89		89			89																																																																																														BI2O3,SRCO3,CACO3,DY2CO3,CUO	1	MIXTURE-CAL(800C 24H)-SIN(850C-900C)-Q TO LN2					MGNETISM AND SUPERCONDUCTIVITY IN THE 2:2:1:2 BISMUTH CUPRATEBY DYSPROSIUM SUBSTITUTION (BI2SR2CA1-XDYXCU2O8+Z)				SOLID STATE COMMUN.83(1992)689	E.LAXMI NARSAIAH,U.V.SUBBA RAO	BI,SR,CA,DY,CU,O	
4055	SSC0830689		Bi2Sr2(Ca,Dy)Cu2O8	Bi2Sr2Ca0.7Dy0.3Cu2O8+Z	Bi	2	Sr	2	Ca	0.7	Dy	0.3	Cu	2											O	8+Z		1	1992	emu/g	-0.0002					-6																				2	Bi2212			A	5.423		30.746														88		88			88																																																																																														BI2O3,SRCO3,CACO3,DY2CO3,CUO	1	MIXTURE-CAL(800C 24H)-SIN(850C-900C)-Q TO LN2					MGNETISM AND SUPERCONDUCTIVITY IN THE 2:2:1:2 BISMUTH CUPRATEBY DYSPROSIUM SUBSTITUTION (BI2SR2CA1-XDYXCU2O8+Z)				SOLID STATE COMMUN.83(1992)689	E.LAXMI NARSAIAH,U.V.SUBBA RAO	BI,SR,CA,DY,CU,O	
4056	SSC0830127	SOLUBILITY LIMIT (BA/SR)=0.15	(Bi,Pb)2(Sr,Ba)2Ca2Cu3O10	Bi1.5Pb0.52Sr1.63Ba0.29Ca2.04Cu3OZ	Bi	1.5	Pb	0.52	Sr	1.63	Ba	0.29	Ca	2.04	Cu	3									O	Z		1	1992																											3	Bi2223																			109.3			109.6			109.6																																																																																														BI2O3,PBO,SRCO3,BACO3,CACO3,CUO	1	SIN(838C 120H)					SUPERCONDUCTIVITY OF THE BA-DOPED BI2PBSR2CA2CU3OY SYSTEM				SOLID STATE COMMUN.83(1992)127	HONG SEOK KIM,KEU HONG KIM,SEONG HAN KIM,SUNG HAN LEE	BA,BI,PB,SR,CA,CU,O	
4057	SSC0830205	MAIN PHASE =TL1201	(Tl,Cr)Sr2CuO6	Tl0.5Cr0.5Sr2Cu1OZ	Tl	0.5	Cr	0.5	Sr	2	Cu	1													O	Z			1992																											2	Tl1201	P4/MMM			3.795		8.88													40		50				45																																																																																														TL2O3,CR2O3,SRO,CUO	1	MIXTURE-PELLET-SIN(950C 5-30MIN IN O2)-Q					A NEW SUPERCONDUCTING 1201-TYPE PHASE (TL,CR)SR2CUO5				SOLID STATE COMMUN.83(1992)205	D.O.PEDERSON,Y.F.LI,Y.Q.TANG,Z.Y.CHEN,Z.Z.SHENG	TL,CR,SR,CU,O	
4058	SSC0830123	TWO STEP TRANSITION	(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z			1992																																															72		114				93																																																																														3.25				6.42												BI2O3,PBO,CACO3,SRCO3	0	SIN(860C 12H)					110K BI2SR2CA2CU3OY SUPERCONDUCTORS BY PB AND SB DOPING				SOLID STATE COMMUN.83(1992)123	K.SHAHI,V.P.N.PADMANABAN	BI,SR,CA,CU,O,PB,SB	
4059	SSC0830123		(Bi,Pb,Sb)2Sr2Ca2Cu3O10	Bi1.6Pb0.3Sb0.1Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.3	Sb	0.1	Sr	2	Ca	2	Cu	3									O	Z			1992																																															101		114				107.5																																																																														2				4.31													0	SIN(850C 12H)					110K BI2SR2CA2CU3OY SUPERCONDUCTORS BY PB AND SB DOPING				SOLID STATE COMMUN.83(1992)123	K.SHAHI,V.P.N.PADMANABAN	BI,SR,CA,CU,O,PB,SB	
4060	PR0465581	1.80*0.95*0.03MM3,DEMAG.FACTOR=0.946	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1992																												T'																				19.2		19.2			19.2												DEVIATION FROM LINEAR M-H CURVE			920						REVERSIBLE MAGNETIZATIONNEAR HC2(T)			7															70					700																																																			0	BY SELF-FLUX METHOD					CRITICAL FIELDS AND FUNDAMENTAL LENGTHS IN A SUPERCONDUCTING ELECTRON-DOPED PR1.85CE0.15CUO4-Y SINGLE CRYSTAL	199209	CRITICAL FIELDS     ,SINGLE CRYSTAL      ,PENETRATION	INSTITUT DE CIENCIA DE MATERIALS DE BARCELONA	PHYS.REV.B,46(1992)5581	B.MARTINEZ,J.FONTCUBERTA,L.FABREGA,S.PINOL,X.OBRADORS	PR,CE,CU,O	
4062	PR0463195			Bi1.8Pb0.4Sr2Ca2.2Cu3OZ	Bi	1.8	Pb	0.4	Sr	2	Ca	2.2	Cu	3											O	Z			1992																												Bi2223																				107.5		107.5			107.5																								297									3.68						10.5					1940																																																			0	FORMED IN AG TUBE, HIGHLY ORIENTED C-AXIS PERPRNDICULAR TO TAPE SURFACE					REVERSIBLE MAGNETIC PROPERTIES OF C-AXIS-ORIENTED SUPERCONDUCTING BI2SR2CA2CU3O10	199208	MAGNETIZATION       ,ANISOTROPY          ,CRITICAL FIELD	DIVISION OF MATERIALS SCIENCES, BROOKHAVEN NATIONAL LABORATORY, NY	PHYS.REV.B,46(1992)3195	D.K.FINNEMORE,JUNHO GOHNG,K.SATO,M.SUENAGA,QIANG LI,T.HIKATA	BI,SR,CA,CU,O	
4063	PR0422684		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1990																												BKBO																					25.5				25.5																																																																	THC4063																													BAO,BI2O3,KO2	0						THERMAL CONDUCTIVITY OF BA-K-BI-O: A CONTRAST TO COPPER OXIDESUPERCONDUCTORS	199008		DEPARTMENT OF PHYSICS, THE UNIVERSITY OF MICHIGAN, ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,42(1990)2684	A.B.KAISER,C.UHER,J.BURM,R.A.RICHADSON,S.D.PEACOR	BA,K,BI,O	
4064	LES1690017		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4.03	Nd	1.85	Ce	0.15	Cu	1															O	4+Z	4.03	1	1991																											2	T'																				19.3					19.3										40																																																																																											THERMAL CONDUCTIVITY OF ND-CE-CU-O SUPERCONDUCTORS				J.LESS-COMMON METALS,169(1991)L17	A.JEZOWSKI,P.W.KLAMUT	ND,CE,CU,O	
4065	LES1690017	SEMICONDUCTIVE	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+Z	Nd	1.85	Ce	0.15	Cu	1															O	4+Z		1	1991																											2	T'																																																																																										THC4065																														1	ANN(900C 15H IN AIR)					THERMAL CONDUCTIVITY OF ND-CE-CU-O SUPERCONDUCTORS				J.LESS-COMMON METALS,169(1991)L17	A.JEZOWSKI,P.W.KLAMUT	ND,CE,CU,O	
4066	PRB03911559	LONG AXIS PERPENDICULAR TO PRESS DIRECTION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1989									6.3																			Bi2212																				91					91																																																																	THC4066																	9.25													0						THERMAL CONDUCTIVITY OF BI-SR-CA-CU-O SUPERCONDUCTORS: CORRELATION WITH THE LOW-TEMPERATURE SPECIFIC-HEAT BEHAVIOR	198906	THERMAL CONDUCTIVITY	DEPARTMENT OF PHYSICS,THE UNIVERSITY OF MICHIGAN 48109-1120	PHYS.REV.B.,39(19879)11559	C.UHER,S.D.PEACOR	BI,SR,CA,CU,O	
4067	PRB03911559	LONG AXIS // PRESS DIRECTION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1989									6.3																			Bi2212																				91					91																																																																	THC4067																	40													0						THERMAL CONDUCTIVITY OF BI-SR-CA-CU-O SUPERCONDUCTORS: CORRELATION WITH THE LOW-TEMPERATURE SPECIFIC-HEAT BEHAVIOR	198906	THERMAL CONDUCTIVITY	DEPARTMENT OF PHYSICS,THE UNIVERSITY OF MICHIGAN 48109-1120	PHYS.REV.B.,39(19879)11559	C.UHER,S.D.PEACOR	BI,SR,CA,CU,O	
4068	PRB03911559		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3OZ	Bi	2	Sr	2	Ca	2	Cu	3													O	Z			1989																												Bi2223																				107					107																																																																																		5.8													0	BI:SR:CA:CU=1:1:1:2,MIXTURE-ANN(820C 12H)-PRESS					THERMAL CONDUCTIVITY OF BI-SR-CA-CU-O SUPERCONDUCTORS: CORRELATION WITH THE LOW-TEMPERATURE SPECIFIC-HEAT BEHAVIOR	198906	THERMAL CONDUCTIVITY	DEPARTMENT OF PHYSICS,THE UNIVERSITY OF MICHIGAN 48109-1120	PHYS.REV.B.,39(19879)11559	C.UHER,S.D.PEACOR	BI,SR,CA,CU,O	
4069	SSC0770773	SEMICONDUCTIVE,HEAT FLOW // P=1 FOR CUO2 PLANE,P=2 FOR HEAT FLOW PERPENDICULAR TO CU-O PLANE	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		3	1991																												T																																																																																										THC4069																														0						THERMAL CONDUCTIVITY OF SINGLE CRYSTAL LANTHANUM CUPRATES AT VERY LOW TEMPERATURE	199103		PHYSICS DEPARTMENT GENERAL MOTORS RESEARCH LABORATORIES WWARREN,MI 48090-9055	SOLID STATE COMMUN,77(1991)773	A.CASSANHO,C.UHER,D.R.GABBE,D.T.MORELLI,G.L.DOLL,H.P.JENSSEN,J.HEREMANS,M.S.DRESSELHAUS,S.D.PEACOR	LA,SR,CU,O	
4070	SSC0770773		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		3	1991																												T																			9						9																																																																	THC4070																														0						THERMAL CONDUCTIVITY OF SINGLE CRYSTAL LANTHANUM CUPRATES AT VERY LOW TEMPERATURE	199103		PHYSICS DEPARTMENT GENERAL MOTORS RESEARCH LABORATORIES WWARREN,MI 48090-9055	SOLID STATE COMMUN,77(1991)773	A.CASSANHO,C.UHER,D.R.GABBE,D.T.MORELLI,G.L.DOLL,H.P.JENSSEN,J.HEREMANS,M.S.DRESSELHAUS,S.D.PEACOR	LA,SR,CU,O	
4071	SSC0770773		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1991																												T																			33						33																																																																	THC4071																														0						THERMAL CONDUCTIVITY OF SINGLE CRYSTAL LANTHANUM CUPRATES AT VERY LOW TEMPERATURE	199103		PHYSICS DEPARTMENT GENERAL MOTORS RESEARCH LABORATORIES WWARREN,MI 48090-9055	SOLID STATE COMMUN,77(1991)773	A.CASSANHO,C.UHER,D.R.GABBE,D.T.MORELLI,G.L.DOLL,H.P.JENSSEN,J.HEREMANS,M.S.DRESSELHAUS,S.D.PEACOR	LA,SR,CU,O	
4072	PR0412520	P=1 FOR HEAT FLOW // CUO2 PLANE, THEORY=BARDEEN-RICKEYZEN-TEWORDT(BRT)	(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O	4		3	1990																												T																			9.5						9.5																																																											380			1.7			THC4072																																				Anisotropic thermal conductivity of superconducting lanthanum lanthanum cuprate	199002		Physics Department, General Motors Research Laboratories, Warren, Michigan 48090-9055	Phys.Rev.B,41(1990)2520	A. Cassanho,D.R. Gabbe,D.T. Morelli,G.L. Doll,H.P. Jenssen,J. Heremans,M.S. Dresselhaus		
4073	PRB0390804	P=1 FOR HEAT FLOW//<001>,P=2 FOR HEAT FLOW //<221>,P=3 FOR HEAT FLOW //<110>	La2CuO4	La2Cu1O4-Z	La	2	Cu	1																	O	4-Z		3	1989																											2																																																																																											THC4073																														0	SEE J.CRYST.GROWTH 85(1987)576					THERMAL PROPERTIES OF SINGLE-CRYSTAL LA(2)CU(1)O(4-Z)	198901	THERMAL CONDUCTIVITY     ,RAMAN                    ,SUSCEPTIBILITY           ,SPECIFIC HEAT	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,39(1989)804	D.T.MORELLI,G.DOLL,H.P.JENSSEN,J.HEREMANS,M.S.DRESSELHAUS,P.J.PICONE	LA,CU,O	
4074	PRB0371604	90%Y123STRUCTURE	RBa2Cu3O7	Gd1Ba1.98Cu3.05O7	Gd	1	Ba	1.98	Cu	3.05															O	7			1988									3.83																			Y123																			89.4						89.4																																																											614	BY FITTING OF DEBYE FUNCTION TO SPHEAT					THC4074																														0	SEE PHYS.REV.B 36(1987)3917					THERMAL AND ELECTRONIC PROPERTIES OF RARE-EARTH BA(2)CU(3)O(X) SUPERCONDUCTORS	198802	THERMAL CONDUCTIVITY     ,RESISTIVITY              ,SPECIFIC	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,37(1988)1604	D.T.MORELLI,G.W.SMITH,J.HEREMANS,S.C.STRITE III	R,BA,CU,O	
4075	PRB0371604	90%Y123 STRUCTURE	RBa2Cu3O7	Dy1Ba1.97Cu3.06O7	Dy	1	Ba	1.97	Cu	3.06															O	7			1988									4.48																			Y123																			87.1						87.1																																																											595	BY SP.HEAT					THC4075																														0	SEE PHYS.REV.B 36(1987)3917					THERMAL AND ELECTRONIC PROPERTIES OF RARE-EARTH BA(2)CU(3)O(X) SUPERCONDUCTORS	198802	THERMAL CONDUCTIVITY     ,RESISTIVITY              ,SPECIFIC	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,37(1988)1604	D.T.MORELLI,G.W.SMITH,J.HEREMANS,S.C.STRITE III	R,BA,CU,O	
4076	PRB0371604	90%Y123 STRUCTURE	RBa2Cu3O7	Eu1Ba1.93Cu2.92O7	Eu	1	Ba	1.93	Cu	2.92															O	7			1988									3.69																			Y123																			83.2						83.2																																																											595	BY SP.HEAT					THC4076																														0	SEE PHYS.REV.B 36(1987)3917					THERMAL AND ELECTRONIC PROPERTIES OF RARE-EARTH BA(2)CU(3)O(X) SUPERCONDUCTORS	198802	THERMAL CONDUCTIVITY     ,RESISTIVITY              ,SPECIFIC	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,37(1988)1604	D.T.MORELLI,G.W.SMITH,J.HEREMANS,S.C.STRITE III	R,BA,CU,O	
4077	PRB0371604	90%Y123 STRUCTURE,TWO CURVES ARE FOR DIFFERENT SAMPLES	RBa2Cu3O7	Y1Ba2.01Cu3.11O7	Y	1	Ba	2.01	Cu	3.11															O	7			1988									2.72																			Y123																			86						86																																																											606	BY SP.HEAT					THC4077																														0	SEE PHYS.REV.B 36(1987)3917					THERMAL AND ELECTRONIC PROPERTIES OF RARE-EARTH BA(2)CU(3)O(X) SUPERCONDUCTORS	198802	THERMAL CONDUCTIVITY     ,RESISTIVITY              ,SPECIFIC	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,37(1988)1604	D.T.MORELLI,G.W.SMITH,J.HEREMANS,S.C.STRITE III	R,BA,CU,O	
4078	PRB0371604		RBa2Cu3O7	Er1Ba2.03Cu3.05O7	Er	1	Ba	2.03	Cu	3.05															O	7			1988									3.01																			Y123																			90						90																																																											614	BY SP.HEAT					THC4078																														0	SEE PHYS.REV.B 36(1987)3917					THERMAL AND ELECTRONIC PROPERTIES OF RARE-EARTH BA(2)CU(3)O(X) SUPERCONDUCTORS	198802	THERMAL CONDUCTIVITY     ,RESISTIVITY              ,SPECIFIC	PHYSICS DEPARTMENT,GENERAL MOTORS RESEARCH LABORATORIES,WARREN,MICHIGAN	PHYS.REV.B,37(1988)1604	D.T.MORELLI,G.W.SMITH,J.HEREMANS,S.C.STRITE III	R,BA,CU,O	
4079	PRL0643090	THERMAL COND. MEASURED FOR MAGNETIC FIELD PARRALLEL TO C-AXIS,SINGLE=1.80*0.71*0.02MM3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1990																												Y123																			87.5						87.5																								400							7								9																										THC4079																														0	USING CUO FLUX, SEE NAT3280601					Transport Entropy of Vortex Motion in YBa2Cu3O7	1990		AT&T Bell Laboratories,600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.rev.Lett.64(1990)3090	B. Batlogg,J.V. Waszczak,L.F. Schneemeyer,T.T.M. Palstra		
4080	PR0382892		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1988									5.22																			Y123																																																																																										THC4080																	2.01													0	ANN(600C)-SLOW COOL TO RT(IN O2)					THERMAL CONDUCTIVITY OF YBA2CU3O7-Z BELOW 1 K: EVIDENCE FOR NORMAL-CARRIER TRANSPORT WELL BELOW TC	8		DEPARTMENT OF PHYSICS, UNIVERSITY OF MICHIGAN	PHYS.REV.B,38(1988)2892	C.UHER,J.L.COHN,S.D.PEACOR	Y,BA,CU,O	
4081	PR0382892		YBa2Cu3O7	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	7-Z	6.2		1988																												Y123																																																																																										THC4081																														0	ANN(600C)-SLOW COOL TO RT(IN O2)-VAVUUM ANN					THERMAL CONDUCTIVITY OF YBA2CU3O7-Z BELOW 1 K: EVIDENCE FOR NORMAL-CARRIER TRANSPORT WELL BELOW TC	8		DEPARTMENT OF PHYSICS, UNIVERSITY OF MICHIGAN	PHYS.REV.B,38(1988)2892	C.UHER,J.L.COHN,S.D.PEACOR	Y,BA,CU,O	
4082	PR0422684	INSULATOR	(Ba,K)BiO3	Ba0.8K0.2Bi1O3	Ba	0.8	K	0.2	Bi	1															O	3		1	1990																												BKBO																																																																																																																							BAO,BI2O3,KO2	0						THERMAL CONDUCTIVITY OF BA-K-BI-O: A CONTRAST TO COPPER OXIDESUPERCONDUCTORS	199008		DEPARTMENT OF PHYSICS, THE UNIVERSITY OF MICHIGAN, ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,42(1990)2684	A.B.KAISER,C.UHER,J.BURM,R.A.RICHADSON,S.D.PEACOR	BA,K,BI,O	
4083	PR0471053	80% SINGLE DOMAIN,SPJUMP BY ASSUMING 3D GAUSSIAN FLUCTUATION,HC2 BY LINEAR DEPENDENCE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1993									6.4																		3	Y123																				90.6					90.6																							1000	250															11.5	2.9														MJ/G.K																																									0	(CA,SR,CU,O)MIXTURE-HEAT(1200K,24H)+(TL2O3,PBO2)-HEAT(1170K,3H IN SEALED AG TUBE IN AIR)					HEAT CAPACITY OF YBA2CU3O7-Z CRYSTALS ALONG THE HC2 LINE	199301		NAVAL RESEARCH LABORATORY, WASHINGTON, D.C.	PHYS.REV.B,(1993)1053	D.M.GINSBERG,J.P.RICE,M.B.SALAMON,S.E.INDERHEES	Y,BA,CU,O	
4084	SSC0830073		(Tl,Pb)Sr2CaCu2O7	Tl0.75Pb0.25Ca1Sr2Cu2O7	Tl	0.75	Pb	0.25	Ca	1	Sr	2	Cu	2											O	7		1	1992																											2	Tl1212				3.8		12.145																	20																																																																																																	0						SUPERCONDUCTING PROPERTIES OF TL1-YPBYCASR2CU2O7: ROLE OF PB AND OXYGEN STOICHIOMETRY				SOLID STATE COMMUN.83(1992)73	C.N.R.RAO,R.VIJAYARAGHAVAN	TL,PB,CA,SR,CU,O	
4085	SSC0830073		(Tl,Pb)Sr2CaCu2O7	Tl0.7Pb0.3Ca1Sr2Cu2O7	Tl	0.7	Pb	0.3	Ca	1	Sr	2	Cu	2											O	7		1	1992																											2	Tl1212				3.794		12.115													22		40				31																																																																																															0						SUPERCONDUCTING PROPERTIES OF TL1-YPBYCASR2CU2O7: ROLE OF PB AND OXYGEN STOICHIOMETRY				SOLID STATE COMMUN.83(1992)73	C.N.R.RAO,R.VIJAYARAGHAVAN	TL,PB,CA,SR,CU,O	
4086	SSC0830073		(Tl,Pb)Sr2CaCu2O7	Tl0.5Pb0.5Ca1Sr2Cu2O7	Tl	0.5	Pb	0.5	Ca	1	Sr	2	Cu	2											O	7		1	1992																											2	Tl1212				3.81		12.16													78		91				84.5																																																																																															0						SUPERCONDUCTING PROPERTIES OF TL1-YPBYCASR2CU2O7: ROLE OF PB AND OXYGEN STOICHIOMETRY				SOLID STATE COMMUN.83(1992)73	C.N.R.RAO,R.VIJAYARAGHAVAN	TL,PB,CA,SR,CU,O	
4087	SSC0830073		(Tl,Pb)Sr2CaCu2O7	Tl0.75Pb0.25Ca1Sr2Cu2O7	Tl	0.75	Pb	0.25	Ca	1	Sr	2	Cu	2											O	7		1	1992																												Tl1212																				80					80																																																																																															0	4083+ANN IN SILICA TUBE UNDER VAC(E-3 TORR)					SUPERCONDUCTING PROPERTIES OF TL1-YPBYCASR2CU2O7: ROLE OF PB AND OXYGEN STOICHIOMETRY				SOLID STATE COMMUN.83(1992)73	C.N.R.RAO,R.VIJAYARAGHAVAN	TL,PB,CA,SR,CU,O	
4088	SSC0710187	2212(MAJOR)+2223(MINOR)+OTHERS,GAMMA BY ASSUMING BCS	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		2	1989																												Bi2212																			84		90				87																																																						J/MOLE.K	1.6	MJ/MOLE.K2	14		230																																				0	SIN(880C,12H IN O2)					SPECIFIC HEAT AND RESISTIVITY OF THE HIGH-Tc SUPERCONDUCTOR BiCaSrCu2Ox FROM 2.5 TO 300K			Reserch Institute of Electricl Engineering, 190 11 Prague 9 - Bechovice	Solid State Commun.,71(1989)187-190	A. Belling,H. Hejdova',J. Bischof,J. Hrebi'k,V. Plechacek,Z. Trejbalova'		
4089	SSC0710187	2212(MAJOR)+2223(MINOR)+OTHERS,TWO STEP TRANSITION IN SUS AND RES	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		2	1989																												Bi2212																			76		110				93																																																							1.83		17.5																																						0	SIN(880C,12H IN AIR)					SPECIFIC HEAT AND RESISTIVITY OF THE HIGH-Tc SUPERCONDUCTOR BiCaSrCu2Ox FROM 2.5 TO 300K			Reserch Institute of Electricl Engineering, 190 11 Prague 9 - Bechovice	Solid State Commun.,71(1989)187-190	A. Belling,H. Hejdova',J. Bischof,J. Hrebi'k,V. Plechacek,Z. Trejbalova'		
4090	SSC0710187	2223(MAJOR)+2212(MINOR),2223>85 VOL %	(Bi,Pb)2Sr2Ca2Cu3O10	Bi0.7Pb0.3Sr1Ca1Cu1.8O6	Bi	0.7	Pb	0.3	Sr	1	Ca	1	Cu	1.8											O	6		2	1989																												Bi2223																																																																																		73																																						0						SPECIFIC HEAT AND RESISTIVITY OF THE HIGH-Tc SUPERCONDUCTOR BiCaSrCu2Ox FROM 2.5 TO 300K			Reserch Institute of Electricl Engineering, 190 11 Prague 9 - Bechovice	Solid State Commun.,71(1989)187-190	A. Belling,H. Hejdova',J. Bischof,J. Hrebi'k,V. Plechacek,Z. Trejbalova'		
4091	PR04614234	1.5*1.5*0.05MM3,PENET ANDHC1 HAVE THE SAME TEMP. DEPENDENCE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OY	Bi	2	Sr	2	Ca	1	Cu	2													O	Y		3	1992																												Bi2212																				90				1.3	90														800																												LC RESONANCE WITH 10MHZ		5000																																							0.23												0						MAGNETIC-FIELD PENETRATION DEPTH AND THE LOWER CRITICAL FIELDOF THE QUASI-TWO-DIMENSIONAL SUPERCONDUCTOR BI2SR2CACU2OY	199212			PHYS.REV.B,46(1992)14234	A.MAEDA,K.UCHINOKURA,M.KOBAYASHI,N.KONDO,T.SHIBAUCHI	BI,SR,CA,CU,O	
4092	PR0466422		Bi2Sr2CaCu2O8	Bi2.15Sr1.8Ca1Cu2O8.15	Bi	2.15	Sr	1.8	Ca	1	Cu	2													O	8.15	8.15	3	1992																												Bi2212																				93					93																																																																																															0	(870C,45H IN PT CRUCIBLE)-Q,PLATELET-ANN(725C)					MAGNETIC PROPERTIES OF BI2SR2CACU2O8+Z SINGLE CRYSTALS WITH VARIABLE OXYGEN CONTENT	199209		IBM THOMAS J.WATSON RESEARCH CENTER, NEW YORK	PHYS.REV.B,46(1992)6422	G.V.CHANDRASHEKHAR,M.DAUMLING	BI,SR,CA,CU,O	
4093	PR0430408	AB PLANE 1MM,5-10 MICRON IN C-DIRECTION,CREAVED,HEAT FLOW//C AXIS, THC300(NORMAL)=0=87W/M.K	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1991																																																85				2	85																																																														0.87			THC4093																														0	SEE PRL0620336					THERMAL-CONDUCTIVITY ANISOTROPY OF SINGLE-CRYSTAL BI2SR2CACU2O8	199101	THERMAL CONDUCTIVITY,SINGLE-CRYSTAL	DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT BERKELEY,AND MATERIALS AND CHEMICAL SCIENCES DIVISION OF THE LAWRENCE BERKELEY LABORATORY,BERKELEY,CALIFORNIA 94720	PHYS.REV.B,43(1991)408	A.ZETTL,M.F.CROMMIE	BI,SR,CA,CU,O	
4094	PR04110978	HEAT FLOW FOR AB DIRECTION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z		3	1990																												Bi2212																			81		89				85																																																														6.8			THC4094																		0.37												0	SEE PRL0620336					THERMAL CONDUCTIVITY OF SINGLE-CRYSTAL BI-SR-CA-CU-O	199006		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT BERKELEY,BERKELEY, CALIFORNIA 94720 AND MATERIALS AND CHEMICAL SCIENCES DIVISION OF THE LAWRENCE BERKELEY LABORATORY, BERKELEY, CALIFORNIA 94720	PHYS.REV.B,41(1990)10978	A.ZETTL,M.F.CROMMIE	BI,SR,CA,CU,O	
4095	PR04110978	HEAT FLOW FOR AB DIRECTION	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8-Z		3	1990																												Bi2212																				55					55																																																														3.2			THC4095																		4.5												0	SEE PRL0620336					THERMAL CONDUCTIVITY OF SINGLE-CRYSTAL BI-SR-CA-CU-O	199006		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT BERKELEY,BERKELEY, CALIFORNIA 94720 AND MATERIALS AND CHEMICAL SCIENCES DIVISION OF THE LAWRENCE BERKELEY LABORATORY, BERKELEY, CALIFORNIA 94720	PHYS.REV.B,41(1990)10978	A.ZETTL,M.F.CROMMIE	BI,SR,CA,CU,O	
4096	PR0382843	AS-GROWN, MEASURED AT 11K	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																																					DEVIATION FROM LINEAR M VS H CURVE		120	690						CALCULATED FROM HC1 AND WHH THEORY		230	35															31	4.8		CALCULATED FROM HC1		900																																																			0	SEE PHYS.LETT. 121(1987)305					ANISOTROPY OF THE LOWER CRITICAL FIELD, MAGNETIC PENETRATION DEPTH, AND EQUILIBRIUM SHIELDING CURRENT IN SINGLE-CRYSTAL YBA2CUO7-Z	8		MATERIALS SCIENCES DIVISION, ARGONNE NATIONAL LABORATORY, ILLINOIS	PHYS.REV.B,38(1988)2843	A.UMEZAWA,C.H.SOWERS,G.W.CRABTREE,J.Z.LIU,L.H.NUNEZ,S.K.MALIK,T.J.MORAN,W.L.KWOK	Y,BA,CU,O	
4097	PR0382843	AS-GROWN AND ANN(550C,72H IN O2)	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																																					DEVIATION FROM LINEAR M VS H CURVE		80	375						CALCULATED FROM HC1 AND WHH THEORY																																																																										0	SEE PHYS.LETT. 121(1987)305					ANISOTROPY OF THE LOWER CRITICAL FIELD, MAGNETIC PENETRATION DEPTH, AND EQUILIBRIUM SHIELDING CURRENT IN SINGLE-CRYSTAL YBA2CUO7-Z	8		MATERIALS SCIENCES DIVISION, ARGONNE NATIONAL LABORATORY, ILLINOIS	PHYS.REV.B,38(1988)2843	A.UMEZAWA,C.H.SOWERS,G.W.CRABTREE,J.Z.LIU,L.H.NUNEZ,S.K.MALIK,T.J.MORAN,W.L.KWOK	Y,BA,CU,O	
4098	PR0382843	AS-GROWN-IRRADIATED BY FAST NEUTRON,FLUENCE OF 8.16E+17 N/CM2	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1988																											3	Y123																																					DEVIATION FROM LINEAR M VS H CURVE		90	325						CALCULATED FROM HC1 AND WHH THEORY																																																																										0	SEE PHYS.LETT. 121(1987)305					ANISOTROPY OF THE LOWER CRITICAL FIELD, MAGNETIC PENETRATION DEPTH, AND EQUILIBRIUM SHIELDING CURRENT IN SINGLE-CRYSTAL YBA2CUO7-Z	8		MATERIALS SCIENCES DIVISION, ARGONNE NATIONAL LABORATORY, ILLINOIS	PHYS.REV.B,38(1988)2843	A.UMEZAWA,C.H.SOWERS,G.W.CRABTREE,J.Z.LIU,L.H.NUNEZ,S.K.MALIK,T.J.MORAN,W.L.KWOK	Y,BA,CU,O	
4099	PR0382900	NATURAL ABANDANCE OF O(18)	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																											3					3.816	3.884	11.679														90.85					90.85										94																																																																																					0						SYNTHSIS AND SUPERCONDUCTING CRITICAL TEMPERATURE OF YBA2CU3 18O7-Z	8		LOS ALAMOS NATIONAL LABORATORY, NEW MEXICO	PHYS.REN.B,38(1988)2900	B.PIERCE,E.GARCIA,L.BERNARDEZ,M.FLUSS,N.N.SAUER,R.R.RYAN,Z.FISK	Y,BA,CU,O	
4100	PR0382900	44% O(18),NO INDICATION OF ISOTOPE EFFECT	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																											3					3.815	3.887	11.667														91.15					91.15										95																																																																																					0						SYNTHSIS AND SUPERCONDUCTING CRITICAL TEMPERATURE OF YBA2CU3 18O7-Z	8		LOS ALAMOS NATIONAL LABORATORY, NEW MEXICO	PHYS.REN.B,38(1988)2900	B.PIERCE,E.GARCIA,L.BERNARDEZ,M.FLUSS,N.N.SAUER,R.R.RYAN,Z.FISK	Y,BA,CU,O	
4101	PR0382900	90% O(18),NO INDICATION OF ISOTOPE EFFECT	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																											3					3.818	3.884	11.664														90.6					90.6										82																																																																																					0						SYNTHSIS AND SUPERCONDUCTING CRITICAL TEMPERATURE OF YBA2CU3 18O7-Z	8		LOS ALAMOS NATIONAL LABORATORY, NEW MEXICO	PHYS.REN.B,38(1988)2900	B.PIERCE,E.GARCIA,L.BERNARDEZ,M.FLUSS,N.N.SAUER,R.R.RYAN,Z.FISK	Y,BA,CU,O	
4102	EN0406902	TWO STEP TRANSITION	Bi2Sr2Ca2Cu3O10	Bi1Sr1Ca1Cu1O1	Bi	1	Sr	1	Ca	1	Cu	1													O	1		1	1989																												Bi2223																			76	105	111				105																																															40.5	10	1																																														0	FIRED(800C,5H)-(880C,12-20H IN AIR),BI:SR:CA:CU=1:1:1:2					ENERGY GAPS IN BI-SR-CA-CU-O AND BI-SR-CU-O SYSTEMS BY ELECTRON TUNNELING	198910	ELECTRON TUNNELING  ,POINT-CONTACT       ,ENERGY GAPS         ,ANISOTROPIES	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1 CHITOSEDAI,SETAGAYA,TOKYO 157 JAPAN	PHYS.REV.B,40(1989)6902	J.AKIMITSU,T.EKINO	BI,SR,CA,CU,O	
4103	EN0406902	TUNNEL//CUO2 PLANE	Bi2Sr2CaCu2O8	Bi1Sr1Ca1Cu1O1	Bi	1	Sr	1	Ca	1	Cu	1													O	1		2	1989																												Bi2212																			76	84	88				84																																															36.5	9.6	1																																														0	BI:SR:CA:CU=1:2:2:4,FROM 900C TO 800C COOL AT RATE 2C/H IN AIR					ENERGY GAPS IN BI-SR-CA-CU-O AND BI-SR-CU-O SYSTEMS BY ELECTRON TUNNELING	198910	ELECTRON TUNNELING  ,POINT-CONTACT       ,ENERGY GAPS         ,ANISOTROPIES	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1 CHITOSEDAI,SETAGAYA,TOKYO 157 JAPAN	PHYS.REV.B,40(1989)6902	J.AKIMITSU,T.EKINO	BI,SR,CA,CU,O	
4104	PR0428890	THE TIP IS PERPENDICULAR TO THE AB PLANE	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																																																																								37.9	8.5	1																																														0						Energy gaps measured by scanning tunneling microscopy	199011		Department of Physics, University of Virginia, Charlottesville, Virginia 22901	Phys.rev.B,42(1990)8890	B. Giambattista,C.G. Slough,Chen Wang,M.A. Subramanian,R.V. Coleman		
4105	PO0392261	POINT CONTACT NB/SAMPLE	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	1	1989																											3	Y123				3.821	3.885	11.675														90.5				4.5	90.5																																															21.3	5.46	1																																													BA(NO3)2,Y2O3,CU2O	1	PELLET-SIN(950C,10H IN O2)-ANN(850C,2H)-SLOW COOL IN O2					POINT-CONTACT TUNNELING IN MONOPHASIC AND POLYPHASIC Y-BA-CU-O SAMPLES:EXPERIMENT AND MODEL	198902	TUNNELING                ,POINT-CONTACT	DIPARTIMENTO DI FISICA,POLITECNICO DI TORINO,ITALY	PHYS.REV.B,39(1989)2261	D.ANDREONE,F.ABBATTISTA,M.VALLINO,R.S.GONNELLI,V.LACQUANITI	Y,BA,CU,O	
4106	PO0392261	11VOL % Y2BACUO7	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		2	1989																											3	Y123																				90.9				8.8	90.9																																															22	5.62	1																																													BA(NO3)2,Y2O3,CU2O	1	PELLET-SIN(950C,10H IN O2)-ANN(850C,2H)-SLOW COOL IN O2					POINT-CONTACT TUNNELING IN MONOPHASIC AND POLYPHASIC Y-BA-CU-O SAMPLES:EXPERIMENT AND MODEL	198902	TUNNELING                ,POINT-CONTACT	DIPARTIMENTO DI FISICA,POLITECNICO DI TORINO,ITALY	PHYS.REV.B,39(1989)2261	D.ANDREONE,F.ABBATTISTA,M.VALLINO,R.S.GONNELLI,V.LACQUANITI	Y,BA,CU,O	
4107	PR0409286	POINT CONTACT,ELECTRODE=AL,TIP AREA=0.001MM2,GAP AT 4.2-15K	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1OX	Nd	1.85	Ce	0.15	Cu	1															O	X		2	1989																												T'																				20	22.5				20																																															4.75	5.5	1																																														1	SIN(1050C,10H IN O2)-ANN(800C,8H+400C,4H IN O2)					TUNNELING MEASUREMENTS OF ND1.85CE0.15CUOX	198911	TUNNELING           ,POINT-CONTACT       ,ENERGY GAP	MICROELECTRONICS RESEATCH LABORATORIES,NEC CORPORATION,34 MIYUKIGOKA,TSUKUBA,IBARAKI 305,JAPAN	PHYS.REV.B,40(1989)9286	I.TAKEUCHI,J.S.TSAI,T.MANAKO,Y.KUDO	ND,CE,CU,O	
4108	TU0394693	2212 PHASE=90%,ETCHED W TIP, CONTACT RESISTANCE=100-200OHM	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1989																												Bi2212																				88					88																																															25	3.4	1																																													BI2O3,SR2CO3,CA(NO3)2,CUO	1	HEAT(860C,48H IN AIR)-HEAT(850C,24H IN AIR)					TUNNELING MEASUREMENTS ON BI(2)CASR(2)CU(2)O(8)	198903	TUNNELING                ,I-V CHARACTERI	DEPARTMENT OF PHYSICS AND ASTRONOMY,UNIVERSITY OF IOWA CITY,IOWA	PHYSICAL REVIEW B.,39(1989)4693	ROBERT E.JOHNSON	BI,CA,SR,CU,O	
4109	EL0390801	GAP AT 4.2K,ELECTRODE=PB,NB,GAP CLOSING AT 81-85K	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OX	Bi	2	Sr	2	Ca	1	Cu	2													O	X		3	1989																												Bi2212																				90				1	90																																															25	7	1																																														0	MIXTURE OF OXIDE AND CARBONATE-MELT(950C IN AIR)-COOL(7C/) TO 800C					ELECTRON TUNNELING AND THE ENERGY GAP IN BI(2)SR(2)CA(1)CU(2)O(X)	198901	TUNNELING                ,SINGLE CRYSTAL           ,ENERGY G	DEPARTMENT OF APPLIED PHYSICS,STANFORD UNIVERSITY,CALIFORNIA	PHYS.REV.B,39(1989)801	A.KAPITULNIK,D.B.MITZI,M.R.BEASLEY,MARK LEE	BI,SR,CA,CU,O	
4110	PR0417217	PB/SIO/BSCCO SANDWITCH		Bi2Pb0.4Sr2Ca2.5Cu3.5OZ	Bi	2	Pb	0.4	Sr	2	Ca	2.5	Cu	3.5											O	Z			1990																																																105					105																																															49.6	5.5	1																																														1	CAL(820C,20H IN AIR)-HEAT(840C,100H IN 0.1ATM O2+520C,50H IN 1ATM O2)					TUNNELING STUDY OF BI2PB0.4SR2CA2.5CU3.5OY WITH TC=105K	199004		DEPARTMENT OF PHYSICS, FACULTY OF SCIENCE AND ENGINEERING, SAGA UNIVERSITY, SAGA 840, JAPAN	PHYS.REV.B,41(1990)7217	H.INOUE,L.RINDERER,M.SUZUKI	BI,PB,SR,CA,CU,O	
4111	TU0407364	TWO STEP TRANSITION,T1=26.1,T2=21.5K,POINT CONTACT=PT ELECTRODE	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		1	1989																												T'				3.95		12.1													15		26.1				20.55																																															4	5.2	1																																														1	ANN(900C,20H IN N2)-Q TO RT					TUNNELING STUDY ON THE ELECTRON-DOPED SUPERCONDUCTOR ND1.85CE0.15CUO4-Y	198910	TUNNELING           ,ENERGY GAP	DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1,CHITOSEDAI,SETAGAYA,TOKYO 157,JAPAN	PHYS.REV.B,40(1989)7364	J.AKIMITSU,T.EKINO	ND,CE,CU,O	
4112	IN0367121	ELECTRODE=1MM DIA NB, GAP ESTIMATED FROM DI/DV	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																												Y123																				92.4				0.8	92.4																																															19.5	4.8	1																																														1	PELLET-SIN(950C, IN O2)					INVESTIGATION OF THE ENERGY GAP OF Y-BA-CU-O BY POINT-CONTACT JOSEPHSON-JUNCTION TECHNIQUES	198711	POINT CONTACT            ,ENERGY GAP               ,I-V CHAR	DIPARTIMENTO DI FISICA NUCLEARE,STRUTTURA DELLA MATERIA E FISICA APPLICATA,UNIVERSITA DI NAPOLI,NAPOLI,ITALY	PHYS.REV.B,36(1987)7121	A.BARONE,A.DI CHIARA,A.M.CUCOLO,E.OLZI,F.C.MATACOTTA,G.PELUSO,R.VAGLIO,U.SCOTTI DI UCCIO	Y,BA,CU,O	
4113	TU0358711	BREAK-JUNCTION METHOD	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																				36					36																																															3.5	2.26	1																																														1						TUNNELING SPECTROSCOPY OF A LA-SR-CU-O BREAK JUNCTION: EVIDENCE FOR STRONG-COUPLING SUPERCONDUCTIVITY		TUNNELING	NBS BOULDER,COLORADO,USA	PHYS.REV.B,35(1987)8711	A.F.CLARK,H.C.KU,JOHN MORELAND,L.F.GOODRICH,N.SHELTON		
4114	PR04010954	ELECTRODE=1000A DIA W	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1989																											3	Y123																				92					92																																															16	4	1																																														1	SURFACE WERE POLISHED WITH SAND PAPER AND CUTTED, THEN CLEANED					TUNNELING MEASUREMENT OF THE ENERGY GAPS IN THE SUPERCONDUCTORS Y-BA-CU-O AND TI-BA-CA-CU-O	198912	POINT-CONTACT       ,TUNNELING           ,ENERGY GAPS	PHYSICS DEPARTMENT,PEKING UNIVERSITY,BEIJING,CHINA	PHYS.REV.B,40(1989)10954	HE JIAN,WANG GUOWEN,WANG LANPING	Y,BA,CU,O,TL,CA	
4115	PR04010954	ELECTRODE=1000A DIA W	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z			1989																												Tl2223																				116					116																																															23	4.6	1																																														1	SURFACE WERE POLISHED WITH SAND PAPER AND CUTTED, THEN CLEANED					TUNNELING MEASUREMENT OF THE ENERGY GAPS IN THE SUPERCONDUCTORS Y-BA-CU-O AND TI-BA-CA-CU-O	198912	POINT-CONTACT       ,TUNNELING           ,ENERGY GAPS	PHYSICS DEPARTMENT,PEKING UNIVERSITY,BEIJING,CHINA	PHYS.REV.B,40(1989)10954	HE JIAN,WANG GUOWEN,WANG LANPING	Y,BA,CU,O,TL,CA	
4116	TU0389295	UNIT CELL=80 CUBIC CELL,USING LOW TEMP. STM,TIP=PT-RH WIRE		Bi4Ca3Sr3Cu4O16.32	Bi	4	Ca	3	Sr	3	Cu	4													O	16+Z	16.32		1988																											3					5.405	27.03	30.6														80				5	80																																															15	4.5	1																																														1	MIXTURE-HEAT(810C,13H IN AIR)-COOL TO RT-ANN(840C,14H+860C,15H)-FC					TUNNELING MEASUREMENTS OF THE ENERGY GAP IN BI(4)CA(3)SR(3)CU(4)O(16+Z)	198811	TUNNELING                ,STM                      ,ENERGY G	DEPARTMENT DE FISICA DE LA MATERIA CONDENSADA,UNIVERSIDAD AUTONOMA DE MADRID,SPAIN	PHYS.REV.B,38(1988)9295	J.M.GONZALEZ-CALBET,M.A.RAMOS,M.VALLET-REGI,S.VIEIRA	BI,CA,SR,CU,O	
4117	PR0410842	BSCCO/AL2O3(60A)/AL JUNCTION	Bi2Sr2CaCu2O8	Bi1Sr1Ca1Cu1O1	Bi	1	Sr	1	Ca	1	Cu	1													O	1		4	1990																												Bi2212																				85					85																																															18	5.5																																															16						QUASIPARTICLE TUNNELING IN BI-SR-CA-CU-O THIN FILMS	199001	TUNNEL JUNCTIONS    ,THIN                ,GAP PARAMETER	FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY, CAMBIRDGE, MASSACHUSETTS 02139	PHYS.REV.B,41(1990)842	A.KUSSMAUL,G.M.ROESLER.JR.,J.S.MOODERA,P.M.TEDROW	BI,SR,CA,CU,O	
4118	PR0410842	BSCCO/AL2O3(60A)/AL JUNCTION	Bi2Sr2Ca2Cu3O10	Bi1Sr1Ca1Cu1O1	Bi	1	Sr	1	Ca	1	Cu	1													O	1		4	1990																												Bi2223																			78	110					110																																															25	5.5																																															16						QUASIPARTICLE TUNNELING IN BI-SR-CA-CU-O THIN FILMS	199001	TUNNEL JUNCTIONS    ,THIN                ,GAP PARAMETER	FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY, CAMBIRDGE, MASSACHUSETTS 02139	PHYS.REV.B,41(1990)842	A.KUSSMAUL,G.M.ROESLER.JR.,J.S.MOODERA,P.M.TEDROW	BI,SR,CA,CU,O	
4119	TU0379738	POINT CONTACT(ELECTRODE=PT-RH ALLOY),GAP AT 4.2K	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4-Z	La	1.92	Sr	0.08	Cu	1															O	4-Z		1	1988																												T																				12					12																																															3	5.79	1																																														0						TUNNELING MEASUREMENTS OF THE DEPENDENCE OF THE ENERGY GAP ON CRITICAL TEMPERATURE IN LA(2-X)SR(X)CU(1)O(4-Y)	198806	TUNNELING                ,ENERGY GAP	IBM THOMAS J.WATSON RESEARCH CENTER,NEW YORK	PHYS.REV.B,37(1988)9738	A.P.FEIN,J.R.KIRTLEY,M.W.SHAFER	LA,SR,CU,O	
4120	TU0379738	ELECTRODE=PT-RH ALLOY,GAP AT 4.2K	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4-Z	La	1.9	Sr	0.1	Cu	1															O	4-Z		1	1988																												T																				18					18																																															4	5.15	1																																														0						TUNNELING MEASUREMENTS OF THE DEPENDENCE OF THE ENERGY GAP ON CRITICAL TEMPERATURE IN LA(2-X)SR(X)CU(1)O(4-Y)	198806	TUNNELING                ,ENERGY GAP	IBM THOMAS J.WATSON RESEARCH CENTER,NEW YORK	PHYS.REV.B,37(1988)9738	A.P.FEIN,J.R.KIRTLEY,M.W.SHAFER	LA,SR,CU,O	
4121	TU0379738	ELECTRODE=PT-RH ALLOY,GAP AT 4.2K	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4-Z	La	1.85	Sr	0.15	Cu	1															O	4-Z		1	1988																												T																				30					30																																															7	5.41	1																																														0						TUNNELING MEASUREMENTS OF THE DEPENDENCE OF THE ENERGY GAP ON CRITICAL TEMPERATURE IN LA(2-X)SR(X)CU(1)O(4-Y)	198806	TUNNELING                ,ENERGY GAP	IBM THOMAS J.WATSON RESEARCH CENTER,NEW YORK	PHYS.REV.B,37(1988)9738	A.P.FEIN,J.R.KIRTLEY,M.W.SHAFER	LA,SR,CU,O	
4122	PR0409366	POINT CONTACT(AU TIP),GAP VALUES BETWEEN 17 AND 31 MEV	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	Z		3	1989																												Bi2212																				96					96																																															17		1																																														0						ELECTRON TUNNELING STUDY OF THE NORMAL AND SUPERCONDUCTING STATES OF BI1.7PB0.3SR2CACU2OX	198911	POINT-CONTACT       ,TUNNELING           ,CONDUCTANCE	MATERIALS SCIENCE DIVISION AND SCIENCE AND TECHNOLOGY CENTER FOR SUPERCONDUCTIVITY,ARGONNE NATIONALLOBORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.B,40(1989)9366	H.CLAUS,J.F.ZASADZINSKI,J.Z.LIU,K.E.GRAY,QIANG HUANG	BI,PB,SR,CA,CU,O	
4123	PR0428049	GAP AT 4.2K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																												Y123																				90					90																																															12	3.2																																															0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4124	PR0428049	GAP AT 6.3K	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																												Y123																				50					50																																															9.7	4.1																																															0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4125	PR0428049	GAP AT 5.1K	GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7			1990																												Y123																				90					90																																															12.4	4.2																																															0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4126	PR0428049	GAP AT 9.8K	ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	7			1990																												Y123																				90					90																																															11.4	4.1																																															0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4127	PR0428049	POINT CONTACT(ELECTRODE=AL OR PT)	(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4			1990																																															10		20				15																																															2.5	4.5	1																																														0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4128	PR0428049	POINT CONTACT(ELECTRODE=AL OR PT)	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4			1990																																																	30				30																																															6	4.6	1																																														0						ELECTRON-TUNNELING STUDIES ON THE SUPERCONDUCTING (LA1-XSRX)2CUO4 AND YBA2CU3OY SYSTEMS	199011	TUNNELING           ,GAPS	FACULTY OF INTEGRATED ARTS AND SCIENCE, HIROSHIMA UNIVERSITY,HIROSHIMA 730, JAPAN	PHYS.REV.B,42(1990)8049	JUN AKIMITSU,TOSHIKAZU EKINO	LA,SR,CU,O,Y,BA	
4129	QU0404478	GAP VALUE AT 4.6K, NORMAL TO CU-O PLANE	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1989																												Y123																				87				3.7	87																																															9	3	1																																														17	SINGLE CRYSTAL FILMS WERE GROWN ON SRTIO3(100) AT 600C					QUASIPARTICLE DENSITY OF STATES IN THE PERPENDICULAR DIRECTIONTO THE CU-O PLANES IN YBA2CU3O7-X SINGLE-CRYSTAL THIN FILMS	198909	FILMS               ,ENERGY GAP	INSTITUTE FOR CHEMICAL RESEARCH,KYOTO UNIVERSITY,UJI 611,JAPAN	PHYS.REV.B,40(1989)4478	H.MAZAKI,J.TAKADA,K.HIRATA,K.IIJIMA,K.YAMAMOTO,T.TERASHIMA,Y.BANDO	TUNNELING SPECTRASINGLE-CRYSTAL	
4130	SSC0701055	GAP VALUES FOR AB-PLANE, FOR C-AXIS DIRECTION GAP=12MEV,GAPENE=3.3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1989																												Bi2212																				85					85																																															23	6.2	1																																														0	ANN(IN O2) AFTER THE SYNTHESIS					TUNNELING SPECTROSCOPY IN BI2SR2CACU2O8: IS THE ENERGY GAP ANISOTROPIC?				SOLID STATE COMMUN.,70(1989)1055	A.ZETTL,G.BRICENO	BI,SR,CA,CU,O	
4131	SSC0620535	POINT CONTACT(ELECTRODE=AL)	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1987																												T																			34		40				37																																															7	4.07	1																																														1						ELECTRON TUNNELING STUDY OF HIGH-Tc SUPERCONDUCTOR La-Sr-Cu-O SYSTEM			Department of Physics, Aoyama-gakuin University, 6-16-1 Chitosedai, Setagaya, Tokyo 157 Japan	Solid State Commun.,62(1987)535-537	J. Akimitsu,M. Sato,S. Hosoya,T. Ekino		
4132	SSC0780809	POINT CONTACT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1991																												Y123																			80						80																																															30	7.6	1																																														0	DISORDERED GRANULAR OR ORIENTED FILMS WITH C-AXIS NORMAL TO SUBSTRATE					THE ENERGY GAP DEPRESSION IN YBA2CU3O7-X/METAL CONTACTS	199106		INSTITUTE OF ELECTRICAL ENGINEERING,SLOVAK ACADEMY OF SCIENCES,84239 BRATISLAVA,CZECHO-SLOVAKIA	SOLID STATE COMMUN.,78(1991)809	A.PLECENIK,M.DARULA,M.GRAJCAR,P.MIKUSIK,S.BENACKA,S.CHROMIK	Y,BA,CU,O	
4133	SSC0671179	POINT CONTACT(MO,NB TIPS)	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1988																												Bi2212																			84						84																																															23	6.4	1																																														5						Electron tunnelling Spectroscopy of Bi2Ca1Sr2Cu2Oy Superconductor			Institute of Physics, Chinese Academy of Sciences, Beijing, China	Solid State Commun.,67(1988)1179-1182	Chen Yinfel,Tao Hongjie,Yan Yifen,Yang Qiansheng,Zhao Shiping		
4134	SSC0770519	CLEAVED SURFACE,BREAK JUNCTION(PB ELECTRODE),GAPENE ESTIMATED USING TC=80K(GAP OPENING)	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1991																												Bi2212																				90					90																																															25	7.3	1																																														0						TUNNELING EVIDENCE OF STRONG COOPER-PAIR-BREAKING NEAR TC IN CUPRATE SUPERCONDUCTORS				SOLID STATE COMMUN.,77(1991)519	B.SUSLA,E.L.WOLF,H.J.TAO		
4135	JJP0271038	BSCCO/ALPHA-SI(160A)/AG JUNCTION,GAP AT 8.2K	Bi2(Sr,Ca)2CaCu2O8	Bi2Sr1.8Ca1.2Cu2OZ	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	Z			1988																												Bi2212																				80					80																																															30	8.7	1																																														1	MIXTURE-CAL(850C,10H IN AIR)-PELLET-SIN(860C,5H IN AIR)					Tunneling Spectroscopy of the 80 K Superconducting Phase of the Bi-Sr-Ca-Cu-O System	198806		Department of Applied Physics, The University of Tokyo 7-3-1 Hongo, Bunkyo-ku, Tokyo 113	Jpn.J.Appl.Phys.Lett.27(1988)L1038-L1040	Atsutaka MAEDA,Hiroshi IKUTA,Kunimitsu UCHINOKURA,Shoji TANAKA		
4136	JJP0290614	YBCO/MGO/PB PLANAR JUNCTION	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		4	1990																											3	Y123																			75		85				80																																															20	6.2	1																																														17	COEVAPORATION ON MGO(100),SRTIO3(100) AT 600C					TUNNELING CHARACTERISTICS OF YBACUO/MGO/PB PLANAR TUNNEL JUNCTIONS AND PBSERVATION OF JOSEPHSON EFFECT	199004	TUNNEL JUNCTION     ,GAP STRUCTURE       ,JOSEPHSON	INSTITUTE OF MATERIALS SCIENCE, UNIVERSITY OF TSUKUBA, TSUKUBA, IBARAKI 305	JJAP LETT.,29(1990)L614	HIROAKI OHTAKE,IENARI IGUCHI,KOJI SHIRAI,MASAFUMI FURUYAMA,MASAKO NASU,SHOJI TOMURA,TAKESHI KUSUMORI	Y,BA,CU,O	
4137	APL0532689	PT(1000A)/ALOX(60A)/YBCO JUNCTION	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1988																												Y123																			74	83					83																																															11.5	3.2	1																																														0	FILMS PREPARED BY REACTIVE EVAPORATION ON SRTIO3(100)					Tunnel junctions using oxide superconducting thin films epitaxially grown on SrTiO3	12		Institute for Chemical reserch, Kyoto University Uji 611, Japan	Appl.Phys.Lett.53(1988)2689	H. Mazaki,J. Takada,K. Hirata,K. Iijima,K. Yamamoto,T. Terashima,Y. Bando		
4138	APL0560683	YBCO(001)Y2O3(001)/YBCO(001) JUNCTION,GAP AT 4.5K	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1990																												Y123																			86						86																																															9	3.5	1																																														0	EPITAXIAL GROWTH ON MGO(100) AT 650C					Tunneling measurement on superconductor/insulator/superconductor junctions using single-crystal YBa2Cu3O7-x thin films	2		Reserch Institute for Production Development, Kyoto 606, Japan	Appl.Phys.Lett.56(1990)683	H. Mazaki,J. Takada,K. Hirata,K. Iijima,K. Yamamoto,T. Terashima,Y. Bando		
4139	APL0572356	POINT CONTACT(AU OR NB ELECTRODE),USING TC=21.5K	(Ba,K)BiO3	Ba0.625K0.375Bi1O3	Ba	0.625	K	0.375	Bi	1															O	3			1990																												BKBO																			21.5	27.5	28.5				27.5																																															3.6	3.8	1																																														1	MELT PROCESS,SURFACE WAS POLISHED BY DIAMOND PAPER,					Ideal tunneling characteristics in Ba1-xKxBiO3 point-contact junctions with Au and Nd tips	11		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne, Illinois 60439	Appl.phys.Lett.57(1990)2356	D.G. Hinks,D.R. Richards,J.F. Zasadzinski,K.E. Gray,Qiang Huang		
4140	APL0551463	10-18% TL2BA2CA2CU3O10, BREAK JUNCTION	Tl2Ba2CaCu2O7	Tl2Ba2Ca1Cu2O7	Tl	2	Ba	2	Ca	1	Cu	2													O	7		2	1989																												Tl2212																			105	108	115				108																																															30	6.1	1																																														0	CRYSTAL GROWN FROM MELT OF TL2BA0.5CA1.5CU2OZ					Break junction measurement of the tunneling gap of a thallium-based high temperature superconductor crystal	10		Electromagnetic technology Division, National Institute of Standards and Technology, Boulder, Clorado 80303	Appl.Phys.Lett.55(1989)1463	B. Morosin,D.S. Ginley,E.L. Venturini,John Mareland		
4141	PHB1651567	POINT CONTACT(W TIP)	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1990																												Bi2212																				85					85																																															21.5	6.3	1																																														0										Physica B, 165(1990)1567	G.Guntherodt,M.Hoffmann,P.C.Splittgerber-Hunnekes,R.Koltun		
4142	PHB1651567	BREAK JUNCTION	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10+Z	Bi	2	Sr	2	Ca	2	Cu	3													O	10+Z		1	1990																												Bi2223																				107					107																																															32.5	7.3	1																																														0										Physica B, 165(1990)1567	G.Guntherodt,M.Hoffmann,P.C.Splittgerber-Hunnekes,R.Koltun		
4143	PHB1651503	POINT CONTACT(W TIP)	(Y,Pr)Ba2Cu3O7	Y0.57Pr0.43Ba2Cu3O7	Y	0.57	Pr	0.43	Ba	2	Cu	3													O	7			1990																																															22					7	22																																															38	4	1																																														0	FILMS PREPARED USING TWO TARGET DC MAGNETRON SPUTTERING					Properties of homogeneous Y1-xPrxBa2Cu3O7 alloy thin films prepared using layer by layer growth				Physica B, 165(1990)1503	A.D.Kent,Ch.Renner,F.Fischer,J.-M.Triscone,L.Antognazza,M.G.Karkut,O.Brunner,Ph Niedermann		
4144	PHB1651601	SIS tunneling ( high-Tc/SiO/Pb). Tunneling were measured after 4 days from fabrication.  compositions and structure of films not given. target compositions are in DB.	Bi2212-film	Bi2Pb1Sr2Ca2Cu4OZ	Bi	2	Pb	1	Sr	2	Ca	2	Cu	4											O	Z		4	1990																																														K		65					65																																															10.5	3.8	1																																														16	Films were deposited on SrTiO3(110) substrates using magnetron sputtering. Target: Bi2PbSr2Ca2Cu4Oz. Films were annealed (830C, 1h) with PbO.					TUNING INVESTGATION OF HIFG TcBi-SYSTEM FILMS ON SrTiO3(110)			Instute of Experimental Physics, University of Lausanne, CH-1015 Lausanne, Swizerland	Physica B, 165(1990)1601	Hiroshi NAKANO,Le'o RINDERER,Morio SUZUKI,Serge NICOUD		
4145	PHB1651601	SIS tunneling ( high-Tc/SiO/Pb). As-grown film. compositions and structure of films not given. target compositions are in DB.	Bi2212-film	Bi2Pb1Sr2Ca2Cu4OZ	Bi	2	Pb	1	Sr	2	Ca	2	Cu	4											O	Z		4	1990																																														K		65					65																																															23.5	8.4	1																																														16	Films were deposited on SrTiO3(110) substrates using magnetron sputtering. Target: Bi2PbSr2Ca2Cu4Oz. Films were annealed (830C, 1h) with PbO.					TUNING INVESTGATION OF HIFG TcBi-SYSTEM FILMS ON SrTiO3(110)			Instute of Experimental Physics, University of Lausanne, CH-1015 Lausanne, Swizerland	Physica B, 165(1990)1601	Hiroshi NAKANO,Le'o RINDERER,Morio SUZUKI,Serge NICOUD		
4146	PHB1690705	BKBO/OXIDE/SN JUNCTION,GAP AT 4K,GAPENE USING TC=18K(GAP DISAPPEAR)	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		1	1990																												BKBO																			21		30				25.5																																															2.9	3.75	1																																														0						The temperature energy gap evolution of Ba0.6K0.4BiO3 by electron tunneling				Physica B, 169(1990)705	D.G.Hinks,F.Morales,R.Escudero,Y.Zheng		
4147	JPS0582135	POINT CONTACT(ELECTRODE=AL)	Ba(Pb,Bi)O3	Ba1Pb0.78Bi0.22O3	Ba	1	Pb	0.78	Bi	0.22															O	3		3	1989																												BPBO																				10.3					10.3																																															1.71	3.85	1																																														5	USING PBO2+BI2O3 AS A SOLVENT					SUPERCONDUCTING ENERGY GAP IN BAPB1-XBIXO3 DETAERMINED FROM POINT-CONTACT TUNNELING	198906		DEPARTMENT OF PHYSICS, AOYAMA-GAKUEN UNIVERSITY, SETAGAYA, TOKYO	J.PHYS.SOC.JAPAN,58(1989)2135	JUN AKIMITSU,TOSHIKAZU EKINO	BA,PB,BI,O	
4148	JPS0582135	POINT CONTACT(ELECTRODE=AL)	Ba(Pb,Bi)O3	Ba1Pb0.83Bi0.17O3	Ba	1	Pb	0.83	Bi	0.17															O	3		3	1989																												BPBO																				7.6					7.6																																															0.71	2.17	1																																														5	USING PBO2+BI2O3 AS A SOLVENT					SUPERCONDUCTING ENERGY GAP IN BAPB1-XBIXO3 DETAERMINED FROM POINT-CONTACT TUNNELING	198906		DEPARTMENT OF PHYSICS, AOYAMA-GAKUEN UNIVERSITY, SETAGAYA, TOKYO	J.PHYS.SOC.JAPAN,58(1989)2135	JUN AKIMITSU,TOSHIKAZU EKINO	BA,PB,BI,O	
4149	JPS0580383	POINT CONTACT(ELECTRODE=GAAS), USING TC=76.2K	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1989																												Bi2212																			76.2		87.2				81.7																																															22	6.7																																															0						FINE STRUCTURE IN THE TUNNELING CONDUCTANCE OF A BI2SR2CACU2O8-GAAS JUNCTION	198902		DEPARTMENT OF APPLIED PHYSICS, SCIENCE UNIVERSITY OF TOKYO	J.PHYS.SOC.JAPAN,58(1989)383	DAISUKE SHIMADA,NOBUAKI MIYAKAWA,NOBUO TSUDA,TADAHARU KIDO	BI,SR,CA,SU,O	
4150	JPS0592473	BSCCO/GAAS:ZN JUNCTION, GAPENE USING TC=85K	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																				84	89				84																																															28	7.1																																															0						TUNNELING CONDUCTANCE OF A BI2SR2CACU2O8-GAAS JUNCTION:TEMPERATURE DEPENDENCE OF THE GAP	199007			J.PHYS.SOC.JAPAN,59(1990)2473	DAISUKE SHIMADA,NOBUAKI MIYAKAWA,NOBUO TSUDA,TADAHARU KIDO	BI,SR,CA,CU,O	
4151	JPC0201009	CERAMIC DISC WITH GRAIN SIZE=5-20MICRON, POINT CONTACT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1987																											3	Y123																			89	91.7					91.7																																															20	5	1																																														1						Electron tunneling spectroscopy of YBaCu3O7-x ceramics			Cavendish Laboratory, Madingley Road, Cambridge CB3 OAE, UK	J.Phys.C,20(1987)L1009-L1015	A Edgar,C J Adkins,S J Chandler		
4152	PRL0672195	STM	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1991																												Bi2212																				85				2	85																																															30	8.2	1																																														0	CLEAVED SURFACE					Features of the Density of States of High-Tc Superconductors Probed by Vacuum Tunneling	199110		Center for the Science and Application of Superconductivity and School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455	Phys.Rev.Lett.67(1991)2195	A.M. Goldman,Ji-Chun Wan,Jin-Xiang Liu		
4153	PR0418904	POINT CONTACT	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990																											3	Y123																			80	85	95				85																																															27		1																																														16						TUNNELING SPECTROSCOPY STUDY OF YBA2CU3O7 THIN FILMS USING A CRYOGENIC SCANNING TUNNELING MICROSCOPE	199005		DEPARTMENT OF PHYSICS, THE UNIVERSITY OF MICHIGAN, ANN ARBOR,MICHIGAN 48109	PHYS.REV.B,41(1990)8904	M.AMMAN,R.BEN-JACOB,R.C.JAKLEVIC,R.WILKINS	Y,BA,CU,O	
4154	PHC2040194		Ba(Pb,Sb)O3	Ba1Pb0.9Sb0.1O3-Z	Ba	1	Pb	0.9	Sb	0.1															O	3-Z			1992																											3	ABO3				6.022	6.061	8.506												K					2																																																																																				0.0318				-0.0000000156								BACO3,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1073K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,6H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4155	PHC2040194		Ba(Pb,Sb)O3	Ba1Pb0.8Sb0.2O3-Z	Ba	1	Pb	0.8	Sb	0.2															O	3-Z			1992																											3	ABO3																		K					2																																																																																				0.0424				-0.0000000122								BACO3,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1073K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,6H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4156	PHC2040194		Ba(Pb,Sb)O3	Ba1Pb0.75Sb0.25O3-Z	Ba	1	Pb	0.75	Sb	0.25															O	3-Z			1992																											3	ABO3																		K	2.3						2.3																																																																																		0.0531				-0.0000000104								BACO3,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1073K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,6H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4157	PHC2040194		Ba(Pb,Sb)O3	Ba1Pb0.7Sb0.3O3-Z	Ba	1	Pb	0.7	Sb	0.3															O	3-Z			1992																											3	ABO3																		K					2																																																																																				0.0763				-0.00000001								BACO3,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1073K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,6H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4158	PHC2040194		Sr(Pb,Sb)O3	Sr1Pb1SbO3-Z	Sr	1	Pb	1	Sb																O	3-Z			1992																											3	ABO3				5.859	5.957	8.325												K					2																																																																																				4.23				-0.00000213								SRCO3,SR(NO3)2,PBO,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1023K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,12H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4159	PHC2040194		Sr(Pb,Sb)O3	Sr1Pb0.95Sb0.05O3-Z	Sr	1	Pb	0.95	Sb	0.05															O	3-Z			1992																											3	ABO3				5.859	5.953	8.325												K					2																																																																																				0.0659				-0.000000698								SRCO3,SR(NO3)2,PBO,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1023K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,12H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4160	PHC2040194		Sr(Pb,Sb)O3	Sr1Pb0.9Sb0.1O3-Z	Sr	1	Pb	0.9	Sb	0.1															O	3-Z			1992																											3	ABO3				5.861	5.951	8.325												K					2																																																																																				0.0511				-0.000000205								SRCO3,SR(NO3)2,PBO,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1023K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,12H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4161	PHC2040194		Sr(Pb,Sb)O3	Sr1Pb0.85Sb0.15O3-Z	Sr	1	Pb	0.85	Sb	0.15															O	3-Z			1992																											3	ABO3				5.862	5.954	8.326												K					2																																																																																				0.108				-0.00000026								SRCO3,SR(NO3)2,PBO,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1023K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,12H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4162	PHC2040194		Sr(Pb,Sb)O3	Sr1Pb0.8Sb0.2O3-Z	Sr	1	Pb	0.8	Sb	0.2															O	3-Z			1992																											3	ABO3				5.861	5.954	8.327												K					2																																																																																				0.42				-0.000000456								SRCO3,SR(NO3)2,PBO,PB(NO3)2,SB2O3	1	MIXTURE-CAL(1023K,12H IN AIR)-PELLET-PRESS(300MPA)-SIN(1123K,12H IN O2)-COOL TO RT(300K/H)					ELECTRICAL PROPERTIES OF THE A(PB1-XBX)O3-Z (A=BA,SR,B=SB,BI)SYSTEM	199212			PHYSICA C,204(1992)194	IN-SEON KIM,MITSURU ITOH,TETSURO NAKAMURA,TOHRU SAWADA,YOSHIYUKI INAGUMA	BA,SR,SB,BI,PB,O	
4163	PHC2040384		DyBa2Cu3O7	Dy1Ba2Cu3O6.94	Dy	1	Ba	2	Cu	3															O	7-Z	6.94		1993									6.07																		3					3.826	3.896	11.688													87.3	88.7				2.6	88.7																																																																																		0.88													0						A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4164	PHC2040384		Dy(Ba,Sr)2Cu3O7	Dy1Ba1.8Sr0.2Cu3O6.89	Dy	1	Ba	1.8	Sr	0.2	Cu	3													O	7-Z	6.89		1993									6.06																		3					3.822	3.888	11.661													83	84.2				2	84.2																																																																																		1.78													0						A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4165	PHC2040384		Dy(Ba,Sr)2Cu3O7	Dy1Ba1.6Sr0.4Cu3O6.89	Dy	1	Ba	1.6	Sr	0.4	Cu	3													O	7-Z	6.89		1993									5.91																		3					3.818	3.882	11.647													79.1	80.6				2.8	80.6																																																																																		1.25													0						A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4166	PHC2040384		Dy(Ba,Sr)2Cu3O7	Dy1Ba1.4Sr0.6Cu3O6.91	Dy	1	Ba	1.4	Sr	0.6	Cu	3													O	7-Z	6.91		1993									5.91																		3					3.81	3.874	11.624													84.5	85.2				1	85.2																																																																																		0.71													0						A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4167	PHC2040384		Dy(Ba,Sr)2Cu3O7	Dy1Ba1.2Sr0.8Cu3O6.9	Dy	1	Ba	1.2	Sr	0.8	Cu	3													O	7-Z	6.9		1993									5.86																		3					3.799	3.863	11.588													84.4	84.7				0.8	84.7																																																																																		0.59													0	4164+SIN(970+980C)					A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4168	PHC2040384		Dy(Ba,Sr)2Cu3O7	Dy1Ba1Sr1Cu3O6.89	Dy	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.89		1993									5.51																		3					3.83	3.849	11.559													78.5	79.5					79.5																																																																																		0.76													0	4164+SIN(960+980C)					A POWDER X-RAY DIFFRACTION AND ELECTRICAL STUDY OF DY(BA2-XSRX)CU3O7-Z SUPERCONDUCTING CUPRATES	199301			PHYSICA C,204(1993)384	CLARE GLORIOSO,GREG W.BOOK,JAMES M.ROZELL JR.,JANNETTE CUNNINGHAM,JOHN P.GOLBEN,MARCUS VLASSE	DY,BA,SR,CU,O	
4169	PHC2050118	SRCUO2,SRY2O5,(SR,Y)14CU24O41 CONTAINED,NOT S/C	YSr2(Cu,B)3O7	Y1Sr2Cu2.9B0.1O7	Y	1	Sr	2	Cu	2.9	B	0.1													O	7			1993																												1212						11.15																																																																																																																	CUO,SRCO3,Y2O3,H3BO3	1	PELLET-HEAT(900C,20H IN AIR)-PELLET-CAL(1000C,24H IN AIR)-ANN(550C)					(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4170	PHC2050118	NOT S/C	YSr2(Cu,B)3O7	Y1Sr2Cu2.7B0.3O7	Y	1	Sr	2	Cu	2.7	B	0.3													O	7		1	1993																												1212						11.029																																																																																																																	CUO,SRCO3,Y2O3,H3BO3	1	PELLET-HEAT(900C,20H IN AIR)-PELLET-CAL(1000C,24H IN AIR)-ANN(550C)					(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4171	PHC2050118	NOT S/C	YSr2(Cu,B)3O7	Y1Sr2Cu2.5B0.5O7	Y	1	Sr	2	Cu	2.5	B	0.5													O	7		1	1993																											2	1212	P4/MMM			3.817		10.961																																																																																																																	CUO,SRCO3,Y2O3,H3BO3	1	PELLET-HEAT(900C,20H IN AIR)-PELLET-CAL(1000C,24H IN AIR)-ANN(550C)					(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4172	PHC2050118	SEMICOND.	YSr2(Cu,B)3O7	Y1Sr2Cu2.3B0.7O7	Y	1	Sr	2	Cu	2.3	B	0.7													O	7		1	1993																												1212						10.93																																																																																																																	CUO,SRCO3,Y2O3,H3BO3	1	PELLET-HEAT(900C,20H IN AIR)-PELLET-CAL(1000C,24H IN AIR)-ANN(550C)					(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4173	PHC2050118	SEMICOND.	YSr2(Cu,B)3O7	Y1Sr2Cu2.1B0.9O7	Y	1	Sr	2	Cu	2.1	B	0.9													O	7		1	1993																												1212						10.942																																																																																																																	CUO,SRCO3,Y2O3,H3BO3	1	PELLET-HEAT(900C,20H IN AIR)-PELLET-CAL(1000C,24H IN AIR)-ANN(550C)					(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4174	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1.85Ba0.15Cu2.5B0.5O7	Y	1	Sr	1.85	Ba	0.15	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.834		11.079																																																																																																																		0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4175	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1.7Ba0.3Cu2.5B0.5O7	Y	1	Sr	1.7	Ba	0.3	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.838		11.186																																																																																																																		0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4176	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1.55Ba0.45Cu2.5B0.5O7	Y	1	Sr	1.55	Ba	0.45	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.848		11.212														16					16																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4177	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1.4Ba0.6Cu2.5B0.5O7	Y	1	Sr	1.4	Ba	0.6	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.86		11.247														24					24																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4178	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1.2Ba0.8Cu2.5B0.5O7	Y	1	Sr	1.2	Ba	0.8	Cu	2.5	B	0.5											O	7			1993																											2	1212				0.865		11.269														35					35																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4179	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr1Ba1Cu2.5B0.5O7	Y	1	Sr	1	Ba	1	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.87		11.3														44					44																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4180	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr0.8Ba1.2Cu2.5B0.5O7	Y	1	Sr	0.8	Ba	1.2	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.877		11.33														51					51																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4181	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr0.6Ba1.4Cu2.5B0.5O7	Y	1	Sr	0.6	Ba	1.4	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.879		11.369														47					47																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4182	PHC2050118		Y(Sr,Ba)2(Cu,B)3O7	Y1Sr0.4Ba1.6Cu2.5B0.5O7	Y	1	Sr	0.4	Ba	1.6	Cu	2.5	B	0.5											O	7			1993																											2	1212				3.879		11.399														35					35																																																																																															0						(B,CU)SR2YCU2O7,A NEW LAYERED COPPER-OXIDE BASED ON THE BORON-OXYGEN GROUP	199301			PHYSICA C,205(1993)118	J.J.YUE,W.J.ZHU,Y.Z.HUANG,Z.X.ZHAO	B,CU,SR,Y,O	
4183	PHC2040299	2223 DOMINANT(85% 2223)	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.7Pb0.3Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	Z			1993																											2	Bi2223				5.41		37.07													108		116			8	112																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4184	PHC2040299	41%2223	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.99Sm0.01Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1.99	Sm	0.01	Cu	3									O	Z			1993																											2																				107		115			8	111																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4185	PHC2040299	38% 2223	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.98Sm0.02Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1.98	Sm	0.02	Cu	3									O	Z			1993																											2																				105		115			10	110																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4186	PHC2040299	4% 2223	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.95Sm0.05Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1.95	Sm	0.05	Cu	3									O	Z			1993																											2	Bi2223																			76		100			24	88																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4187	PHC2040299		(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.925Sm0.075Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1.925	Sm	0.075	Cu	3									O	Z			1993																											2	Bi2223																					86				86																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4188	PHC2040299		(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.9Sm0.1Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	1.9	Sm	0.1	Cu	3									O	Z			1993																											2	Bi2223				5.41		30.69															85				85																																																																																														BI2O3,PBO,SRCO3,CAO,SM2O3,CUO	1	MIXTURE-CAL(800C,24H)-SIN(800C,SEVERAL H)-PELLET-SIN(850C,200H)					EFFECT OF RARE-EARTH SM3+ SUBSTITUTION ON THE SUPERCONDUCTINGPROPERTIES OF THE BI1.7PB0.3SR2CA2-XSMXCU3OY SYSTEM	199301			PHYSICA C,204(1993)299	F.BENIERE,K.NANDA KISHORE,M.MURALIDHAR,M.SERGENT,O.PENA,V.HARI BABU	BI,PB,SR,CA,SM,CU,O	
4189	PHC2040212	INSULATING,20 KOHM.CM AT 100K,KAIZERO IN EMU/CM3.OE	(R,Ce)2Sr2Cu2NbO10	Pr1.5Ce0.5Sr2Cu2Nb1O10	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1992	emu/cm3.Oe	0.0000137				2.6	-3.01		6.39																			RCSCNO				3.887		28.752																																																																																																																		0						SUPERCONDUCTING,MAGNETIC,ELECTRONIC TRANSPORT,AND STRUCTURAL PROPERTIES OF (R1.5CE0.5)SR2CU2NBO10,R=PR,ND,SM,EU	199212			PHYSICA C,204(1992)212	H.B.RADOUSKY,R.N.SHELTON,T.J.GOODWIN	R,CE,SR,CU,NB,O	
4190	PHC2040212	KAIZERO IN EMU/CM3.OE	(R,Ce)2Sr2Cu2NbO10	Sm1.5Ce0.5Sr2Cu2Nb1O10	Sm	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1992	emu/cm3.Oe	0.000012				0.42	-7.79		6.55																			RCSCNO				3.871		28.791															23			5	23										57																																																																																					0						SUPERCONDUCTING,MAGNETIC,ELECTRONIC TRANSPORT,AND STRUCTURAL PROPERTIES OF (R1.5CE0.5)SR2CU2NBO10,R=PR,ND,SM,EU	199212			PHYSICA C,204(1992)212	H.B.RADOUSKY,R.N.SHELTON,T.J.GOODWIN	R,CE,SR,CU,NB,O	
4191	PHC2040212		(R,Ce)2Sr2Cu2NbO10	Eu1.5Ce0.5Sr2Cu2Nb1O10	Eu	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1992									6.58																			RCSCNO				3.869		28.774															23			5	23										56																																																																																					0						SUPERCONDUCTING,MAGNETIC,ELECTRONIC TRANSPORT,AND STRUCTURAL PROPERTIES OF (R1.5CE0.5)SR2CU2NBO10,R=PR,ND,SM,EU	199212			PHYSICA C,204(1992)212	H.B.RADOUSKY,R.N.SHELTON,T.J.GOODWIN	R,CE,SR,CU,NB,O	
4192	PHC2040212		(Nd,Ce)2Sr2Cu2NbO10	Nd1.5Ce0.5Sr2Cu2Nb1O10	Nd	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1992	emu/cm3.Oe	0.0000164				2.97	-19.6		6.42																			RCSCNO				3.882		28.843														20	25			10	20										63																																																																																				CEO2,ND2O3,SRCO3,CUO,ND2O5	1	PELLET IN ALUMINA-SIN(1120C,80H IN 5 PSI O2)-FC TO RT-REPEAT					SUPERCONDUCTING,MAGNETIC,ELECTRONIC TRANSPORT,AND STRUCTURAL PROPERTIES OF (R1.5CE0.5)SR2CU2NBO10,R=PR,ND,SM,EU	199212			PHYSICA C,204(1992)212	H.B.RADOUSKY,R.N.SHELTON,T.J.GOODWIN	R,CE,SR,CU,NB,O	
4193	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1Ca2Cu2O8.229	Bi	2	Sr	1	Ca	2	Cu	2													O	Z	8.229		1993																											2	Bi2212				5.396		30.487														76.4					76.4																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4194	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.1Ca1.9Cu2O8.22	Bi	2	Sr	1.1	Ca	1.9	Cu	2													O	Z	8.22		1993																											2					5.396		30.547														76.5					76.5																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4195	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.2Ca1.8Cu2O8.199	Bi	2	Sr	1.2	Ca	1.8	Cu	2													O	Z	8.199		1993																											2					5.399		30.579														76.5					76.5																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4196	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.3Ca1.7Cu2O8.19	Bi	2	Sr	1.3	Ca	1.7	Cu	2													O	Z	8.19		1993																											2					5.399		30.608														76.5					76.5																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4197	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.4Ca1.6Cu2O8.2	Bi	2	Sr	1.4	Ca	1.6	Cu	2													O	Z	8.2		1993																											2					5.399		30.649														81.1					81.1																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4198	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.5Ca1.5Cu2O8.19	Bi	2	Sr	1.5	Ca	1.5	Cu	2													O	Z	8.19		1993																											2					5.403		30.699														78.5					78.5																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4199	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.6Ca1.4Cu2O8.16	Bi	2	Sr	1.6	Ca	1.4	Cu	2													O	Z	8.16		1993																																5.399		30.862														77.6					77.6																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4200	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.7Ca1.3Cu2O8.211	Bi	2	Sr	1.7	Ca	1.3	Cu	2													O	Z	8.211		1993																																5.409		30.832														78.7					78.7																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4201	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.8Ca1.2Cu2O8.211	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	Z	8.211		1993																																5.402		30.81														73.7					73.7																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4202	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr1.9Ca1.1Cu2O8.181	Bi	2	Sr	1.9	Ca	1.1	Cu	2													O	Z	8.181		1993																																5.402		30.8														71.8					71.8																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4203	JPS0621017		Bi2(Sr,Ca)3Cu2O8	Bi2Sr2Ca1Cu2O8.212	Bi	2	Sr	2	Ca	1	Cu	2													O	Z	8.212		1993																																5.407		30.72														73					73																																																																																														BI2O3,SRCO3,CACO3,CUO	0	MIXTURE-(760-780C,24H)-(790-830C,72H)-(820-870C,48H)					Normal-State Uniform Mgnetic Susceptibility and Superconductivity in Bi2SrzCa3-zCu2Oy	199303		Institute of Applied Physics, University of Tsukuba, Tennoudai 1-1-1, Tsukuba, Ibaraki 305	J.Phys.Soc.Japan62(1993)1017-1024	Hiromoto Uwe,Takayuki IWAMATSU		
4204	NAT3620226		HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z			1993																											2	Hg1201	P4/MMM			3.88		9.509													35		94				64.5																																																																																														BA2CUO3,HGO	1	MIXTURE OF BA2CUO3+HGO-SEALED IN SILICA TUBE-HEAT(800C,5H)-FC TO RT AFTER 10H					SUPERCONDUCTIVITY AT 94K IN HGBA2CUO4+Z	3			NATURE,362(1993)226	E.V.ANTIPOV,M.MAREZIO,O.CHMAISSEM,S.N.PUTILIN	HG,BA,CU,O	
4205	NAT3630056	PLATE-LIKE GRAIN,HG1223+HG1212,LATTICE CONST. IS FOR HG1223	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z		2	1993																											2	Hg1223				3.93		16.1													95	132.5	133.5				132.5																																																																																															1	BA2CACU2O5+HGO-MIX-PELLET IN SEALED QUAETZ-(800C,5H)-ANN(300C,5H IN O2)					SUPERCONDUCTIVITY ABOVE 130 K IN THE HG-BA-CA-CU-O SYSTEM	5			NATURE,363(1993)56	A.SCHILLING,H.R.OTT,J.D.GUO,M.CANTONI	HG,BA,CA,CU,O	
4206	PHC2000043	OZ BY TGA	(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.94Co0.06O6.81	Y	0.76	Ca	0.24	Ba	2	Cu	2.94	Co	0.06											O	Z	6.81	1	1992																											2	Y123				3.857		11.695														82					82										100																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4207	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.85Co0.15O6.8	Y	0.76	Ca	0.24	Ba	2	Cu	2.85	Co	0.15											O	Z	6.8	2	1992																											2	Y123				3.862		11.691														86					86										71																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4208	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.76Co0.24O6.84	Y	0.76	Ca	0.24	Ba	2	Cu	2.76	Co	0.24											O	Z	6.84	2	1992																											2	Y123				3.863		11.709														85					85										82																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4209	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.64Co0.36O6.96	Y	0.76	Ca	0.24	Ba	2	Cu	2.64	Co	0.36											O	Z	6.96	2	1992																											2	Y123				3.87		11.689														66					66										63																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4210	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.34Ba2Cu2.55Co0.45O6.95	Y	0.76	Ca	0.34	Ba	2	Cu	2.55	Co	0.45											O	Z	6.95	2	1992																											2	Y123				3.874		11.687														51					51										43																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4211	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y1Ba2Cu2.55Co0.45O7	Y	1	Ba	2	Cu	2.55	Co	0.45													O	Z	7	2	1992																											2	Y123				3.878		11.666																																																																																																																	BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4212	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.9Ca0.1Ba2Cu2.55Co0.45O7.02	Y	0.9	Ca	0.1	Ba	2	Cu	2.55	Co	0.45											O	Z	7.02	2	1992																											2	Y123				3.879		11.677														18					18										4																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4213	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.85Ca0.15Ba2Cu2.55Co0.45O7.08	Y	0.85	Ca	0.15	Ba	2	Cu	2.55	Co	0.45											O	Z	7.08	2	1992																											2	Y123				3.876		11.685														30					30										28																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4214	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.55Co0.45O6.93	Y	0.76	Ca	0.24	Ba	2	Cu	2.55	Co	0.45											O	Z	6.93	2	1992																											2	Y123				3.874		11.687														51					51										43																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4215	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.7Ca0.3Ba2Cu2.55Co0.45O6.84	Y	0.7	Ca	0.3	Ba	2	Cu	2.55	Co	0.45											O	Z	6.84	2	1992																											2	Y123				3.874		11.689														53					53										49																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4216	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15O6.92	Y	1	Ba	2	Cu	2.85	Co	0.15													O	Z	6.92	2	1992																											2	Y123				3.864		11.678														71					71										55																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4217	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.95Ca0.05Ba2Cu2.85Co0.15O6.82	Y	0.95	Ca	0.05	Ba	2	Cu	2.85	Co	0.15											O	Z	6.82	2	1992																											2	Y123				3.864		11.684														83					83										51																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4218	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.9Ca0.1Ba2Cu2.85Co0.15O6.91	Y	0.9	Ca	0.1	Ba	2	Cu	2.85	Co	0.15											O	Z	6.91	2	1992																											2	Y123				3.863		11.69														84					84										57																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4219	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.85Ca0.15Ba2Cu2.85Co0.15O6.83	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z	6.83	2	1992																											2	Y123				3.861		11.694														86					86										58																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4220	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.8Ca0.2Ba2Cu2.85Co0.15O6.84	Y	0.8	Ca	0.2	Ba	2	Cu	2.85	Co	0.15											O	Z	6.84	2	1992																											2	Y123				3.86		11.75														86					86										71																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4221	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.85Co0.15O6.8	Y	0.76	Ca	0.24	Ba	2	Cu	2.85	Co	0.15											O	Z	6.8	2	1992																											2	Y123				3.862		11.691														86					86										71																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4222	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.88Ca0.12Ba2Cu2.88Co0.12O6.78	Y	0.88	Ca	0.12	Ba	2	Cu	2.88	Co	0.12											O	Z	6.78	2	1992																											2	Y123				3.861		11.687														87					87										85																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4223	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.85Ca0.15Ba2Cu2.85Co0.15O6.83	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z	6.83	2	1992																											2	Y123				3.861		11.694														86					86										58																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4224	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.76Ca0.24Ba2Cu2.76Co0.24O6.84	Y	0.76	Ca	0.24	Ba	2	Cu	2.76	Co	0.24											O	Z	6.84	2	1992																											2	Y123				3.863		11.709														85					85										82																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4225	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.7Ca0.3Ba2Cu2.7Co0.3O6.93	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z	6.93	2	1992																											2	Y123				3.865		11.715														84					84										80																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4226	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.64Ca0.36Ba2Cu2.64Co0.36O6.87	Y	0.64	Ca	0.36	Ba	2	Cu	2.64	Co	0.36											O	Z	6.87	2	1992																											2	Y123				3.866		11.717														82					82										77																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4227	PHC2000043		(Y,Ca)Ba2(Cu,Co)3O7	Y0.58Ca0.42Ba2Cu2.52Co0.48OZ	Y	0.58	Ca	0.42	Ba	2	Cu	2.52	Co	0.48											O	Z		2	1992																											2	Y123				3.868		11.716														79					79										65																																																																																				BACO3,Y2O3,CACO3,CUO,CO3O4	0	MIXTURE-CAL(950C,SEVERAL DAYS IN AIR)-PELLET-ANN(980C,24H+400C,12H IN O2)-FC TO RT					EFFECT OF Y-CA SUBSTITUTION UPON SUPERCONDUCTIVITY IN THE OXIDE YBA2CU3-XCOXO7-Z	199209			PHYSICA C,200(1992)43	A.MAIGNAN,B.RAVEAU,E.SUARD,V.CAIGNAERT	CA,Y,BA,CU,CO,O	
4228	PHC2030411		Bi2Sr2CaCu2O8I	Bi2Sr2Ca1Cu2I1O8	Bi	2	Sr	2	Ca	1	Cu	2	I	1											O	8		1	1992																											2					5.393		18.95														58		55			58																																																																											50							80												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4229	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.9Y0.1Cu2I1O8	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2	I	1									O	8		1	1992																											2					5.403		18.975														67		72			67																																																																											240							300												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4230	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.8Y0.2Cu2I1O8	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2	I	1									O	8		1	1992																											2					5.411		19														75		76			75																																																																											270							300												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4231	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.7Y0.3Cu2I1O8	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2	I	1									O	8		1	1992																											2					5.421		19														79		79			79																																																																											200							220												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4232	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.6Y0.4Cu2I1O8	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2	I	1									O	8		1	1992																											2					5.425		19														66		65			66																																																																											250							22												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4233	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.55Y0.45Cu2I1O8	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	2	I	1									O	8		1	1992																											2					5.426		19														55		55			55																																																																											530							470												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4234	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.5Y0.5Cu2I1O8	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2	I	1									O	8		1	1992																											2					5.433		19														31		43			31																																																																											500							300												BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4235	PHC2030411		Bi2Sr2(Ca,Y)Cu2O8I	Bi2Sr2Ca0.4Y0.6Cu2I1O8	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2	I	1									O	8		1	1992																											2					5.439		19																																																																																																																	BI2O3,SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-FIRE(800C,12H IN AIR)-PELLET-SIN(860-880C,24H)					TWO EFFECTS OF IODINE INTERCALATION ON TC IN BI2SR2CA1-XYXCU2O8	199212			PHYSICA C,203(1992)411	AKIHIKO FUJIWARA,KEIICHI SASAAKI,MITSUNORI MOCHIDA,TAKASHI NOJI,YOJI KOIKE,YOSHITAMI SAITO	BI,SR,CA,CU,O,Y	
4236	PHC2020371			Bi1.6Pb0.4Sr2Ca2Cu2.99Fe0.01OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.99	Fe	0.01									O	Z			1992																											2					5.4		37													96.8		109.7				103.25																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4237	PHC2020371			Bi1.6Pb0.4Sr2Ca2Cu2.95Fe0.05OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.95	Fe	0.05									O	Z			1992																											2					5.39		37.14													85.6		101.9				93.75																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4238	PHC2020371			Bi1.6Pb0.4Sr2Ca2Cu2.93Fe0.07OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.93	Fe	0.07									O	Z			1992																											2					5.39		37.08													79.9		98.8				89.35																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4239	PHC2020371			Bi1.6Pb0.4Sr2Ca2Cu2.9Fe0.1OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.9	Fe	0.1									O	Z			1992																																5.38		36.89															94.2				94.2																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4240	PHC2020371	2223+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.99Zn0.01OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.99	Zn	0.01									O	Z		2	1992																											2	Bi2223				5.4		37.03													95.9		101.1				98.5																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4241	PHC2020371	2223+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.95Zn0.05OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.95	Zn	0.05									O	Z			1992																																5.42		37.09													86.5		107.7				97.1																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4242	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.93Zn0.07OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.93	Zn	0.07									O	Z			1992																																															79		107.1				93.05																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4243	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.9Zn0.1OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.9	Zn	0.1									O	Z			1992																																															78.1		105.2				91.65																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4244	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.8Zn0.2OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.8	Zn	0.2									O	Z			1992																																5.42		37.16													78		106				92																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4245	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.6Zn0.4OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.6	Zn	0.4									O	Z			1992																																5.38		37.09													63.8		108.1				85.95																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4246	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Zn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.5Zn0.5OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.5	Zn	0.5									O	Z			1992																												Bi2212																			55		74.3				64.65																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4247	PHC2020371	2223(MAJOR)+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z		2	1992																											2	Bi2223				5.41		37.12													99.7	105.3	110.1				105.3																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4248	PHC2020371	2223(MAJOR)+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.99Mn0.01OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.99	Mn	0.01									O	Z		2	1992																											2	Bi2223				5.4		37																																																																																																																	BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4249	PHC2020371	2223(MAJOR)+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.95Mn0.05OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.95	Mn	0.05									O	Z		2	1992																											2	Bi2223				5.39		36.81													95.7	103.8	109.7				103.8																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4250	PHC2020371	2223(MAJOR)+2212(MINOR)	(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.8Mn0.2OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.8	Mn	0.2									O	Z		2	1992																											2	Bi2223				5.41		37.04													95		108.4				101.7																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4251	PHC2020371	2223+2212	(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.7Mn0.3OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.7	Mn	0.3									O	Z		2	1992																											2	Bi2223				5.4		36.98													88.4		106.8				97.6																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4252	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.6Mn0.4OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.6	Mn	0.4									O	Z		2	1992																											2	Bi2223				5.41		36.94													65.9		106.8				86.35																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4253	PHC2020371		(Bi,Pb)2Sr2Ca2(Cu,Mn)3O10	Bi1.6Pb0.4Sr2Ca2Cu2.5Mn0.5OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	2.5	Mn	0.5									O	Z			1992																											2	Bi2223				5.4		36.8													63	95.5	106.8				95.5																																																																																														BI2O3,PBO,SRCO3,CACO3,CUO,MXOZ	0	MIXTURE-CAL(820C,5H IN AIR)-PELLET-SIN(850C,100H)-COOL TO 700C(0.2C/MIN)-COOL TO 200C(0.1C/MIN)-FC TO RT					Substitution of 3d metals for Cu in (Bi,Pb)2Sr2Ca2U3Oy			Department of Physics & Astronomy, McMaster University, Hamilton, Ont. L8S 4M1. China	Physica.C,202(1992)371-378	A. Punnett,R.K. NKum,W.R. Datars		
4254	PHC2020162		(C,Cu)Sr2(Y,Ce)2Cu2O9	Sr2.02Y1.4Ce0.55Cu2.59C0.41OZ	Sr	2.02	Y	1.4	Ce	0.55	Cu	2.59	C	0.41											O	Z			1992																											3	1222	I4/MMM			3.827	3.831	27.708													5	18					18										10																																																																																					0	SR:Y:CE:CU=2:1.46:0.54:2.65-PELLET-ANN(1303K,20H IN 80%O2+20%CO2 UNDER 0.02MPA)-Q-ANN(773-1023K, UNDER 0.1MPA O2)					(C0.35CU0.65)SR2(Y0.73CE0.27)2CU2OX	199211			PHYSICA C,202(1992)162	H.NAKATA,H.YAMANE,J.AKIMITSU,K.TOMIMOTO,N.KOBAYASHI,T.HIRAI,Y.MIYAZAKI	C,CU,SR,Y,CE,O	
4255	SSC0850579		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.61Ca0.39Cu3O8	Pb	2	Sr	2	Y	0.61	Ca	0.39	Cu	3											O	8			1993																											2	Pb3212				5.393	5.394	15.815															79				79										50																																																																																					0						PRESSURE EFFECTS,ANISOTROPIC TRANSPORT PROPERTIES AND IRREVERSIBILITY LINE OF PB2SR2Y1-XCAXCU3O8 CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)579	B.SOULETIE,H.BORGES,J.BEILLE,J.C.MARTINEZ,J.J.CAPPONI,O.CHMAISSEM,O.LABORDE	PB,SR,Y,CA,CU,O	
4256	SSC0850579	CA CONTENT NOT MEASURED,UNDER HYDROSTATIC PRESSURE	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.61Ca0.39Cu3O8	Pb	2	Sr	2	Y	0.61	Ca	0.39	Cu	3											O	8			1993																											3	Pb3212				5.379	5.416	15.775															75				75			K/kbar	0.15																																																																															0.16	0.75											0						PRESSURE EFFECTS,ANISOTROPIC TRANSPORT PROPERTIES AND IRREVERSIBILITY LINE OF PB2SR2Y1-XCAXCU3O8 CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)579	B.SOULETIE,H.BORGES,J.BEILLE,J.C.MARTINEZ,J.J.CAPPONI,O.CHMAISSEM,O.LABORDE	PB,SR,Y,CA,CU,O	
4257	SSC0850579		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.64Ca0.36Cu3O8	Pb	2	Sr	2	Y	0.64	Ca	0.36	Cu	3											O	8			1993																											3	Pb3212				5.382	5.412	15.783															65				65																																																																																															0						PRESSURE EFFECTS,ANISOTROPIC TRANSPORT PROPERTIES AND IRREVERSIBILITY LINE OF PB2SR2Y1-XCAXCU3O8 CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)579	B.SOULETIE,H.BORGES,J.BEILLE,J.C.MARTINEZ,J.J.CAPPONI,O.CHMAISSEM,O.LABORDE	PB,SR,Y,CA,CU,O	
4258	PR0470457		YBa2(Cu,Fe)3O7	Y1Ba2Cu3FeO7-Z	Y	1	Ba	2	Cu	3	Fe														O	7-Z		3	1993																												Y123																			92.5	92					92																							481	112								7.5	1.75						17.2	4																																																							0	SELF-FLUX METHOD, CRYSTAL-ANN(400C,2-4H IN O2)					RESISTIVITY AND UPPER CRITICAL FIELD OF YBA2CU3-XFEXO7-Y SINGLE CRYSTALS	199301		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA, DAVIS	PHYS.REV.B,47(1993)457	J.Z.LIU,LU ZHANG,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.NAGATA,Y.X.JIA	Y,BA,CU,FE,O	
4259	PR0470457		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.96Fe0.04O7-Z	Y	1	Ba	2	Cu	2.96	Fe	0.04													O	7-Z		3	1993																												Y123																				89.5					89.5																							215	56								3.45	0.91						24.3	6.3																																																							0	SELF-FLUX METHOD, CRYSTAL-ANN(400C,2-4H IN O2)					RESISTIVITY AND UPPER CRITICAL FIELD OF YBA2CU3-XFEXO7-Y SINGLE CRYSTALS	199301		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA, DAVIS	PHYS.REV.B,47(1993)457	J.Z.LIU,LU ZHANG,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.NAGATA,Y.X.JIA	Y,BA,CU,FE,O	
4260	PR0470457		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.87Fe0.13O7-Z	Y	1	Ba	2	Cu	2.87	Fe	0.13													O	7-Z		3	1993																												Y123																			79	73.5					73.5																							129	31								2.35	0.58						32.7	7.8																																																							0	SELF-FLUX METHOD, CRYSTAL-ANN(400C,2-4H IN O2)					RESISTIVITY AND UPPER CRITICAL FIELD OF YBA2CU3-XFEXO7-Y SINGLE CRYSTALS	199301		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA, DAVIS	PHYS.REV.B,47(1993)457	J.Z.LIU,LU ZHANG,M.D.LAN,P.KLAVINS,R.N.SHELTON,Y.NAGATA,Y.X.JIA	Y,BA,CU,FE,O	
4261	PR0481266	LATTICE CONST. BY NEUTRON DIFFRACTION AT 20K,NO PRECIPITATION OBSERVED BY XAFS	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O6.95	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-Z	6.95	1	1993																											3					3.817	3.888	11.642														39.2				3.7	39.2																																																																																															1						DISTORTED LOCAL ENVIRONMENT AROUND ZN ON CU(2) SITES IN YBA2CU3O7: AN X-RAY-ABSORPTION STUDY	199307			PHYS.REV.B,48(1993)1266	FRANK BRIDGES,GUOGUANG LI,JAMES B.BOYCE,TORD CLAESON		
4262	PR0481266		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.775Zn0.225O6.93	Y	1	Ba	2	Cu	2.775	Zn	0.225													O	7-Z	6.93	1	1993																											3					3.819	3.89	11.64														25				5.8	25																																																																																															1						DISTORTED LOCAL ENVIRONMENT AROUND ZN ON CU(2) SITES IN YBA2CU3O7: AN X-RAY-ABSORPTION STUDY	199307			PHYS.REV.B,48(1993)1266	FRANK BRIDGES,GUOGUANG LI,JAMES B.BOYCE,TORD CLAESON		
4263	PR0481266		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O6.89	Y	1	Ba	2	Cu	2.7	Zn	0.3													O	7-Z	6.89	1	1993																											3					3.823	3.891	11.649																																																																																																																		1						DISTORTED LOCAL ENVIRONMENT AROUND ZN ON CU(2) SITES IN YBA2CU3O7: AN X-RAY-ABSORPTION STUDY	199307			PHYS.REV.B,48(1993)1266	FRANK BRIDGES,GUOGUANG LI,JAMES B.BOYCE,TORD CLAESON		
4264	PR0481148	ASSUMPTION(OXYGEN CONTENT DOES NOT CHANGE BY BROMINATION),BR CONTENT MEASURED		Y1Ba2Cu3Br0.9O6.2	Y	1	Ba	2	Cu	3	Br	0.9													O	6.2		3	1993																												Y123																				92				1	92																					HC2(0)=0.69DHC2/DT AT 14T		776	53															25	1.7																																																							0	DEOXYGENATE(600C,12H)-BROMINATE(260C,24H)					TRANSPORT AND MAGNETIC PROPERTIES OF YBA2CU3O7-ZBRY SINGLE CRYSTALS	199307			PHYS.REV.B,48(1993)1148	A.M.RAO,G.DRESSELHAUS,H.B.RADOUSKY,J.S.MOODERA,J.Z.LIU,M.S.DRESSELHAUS,P.P.NGUYEN,R.S.GLASS,Z.H.WANG		
4265	PR0481148		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1993																											3	Y123																				92					92																							313	78															21	5.1																																																							0						TRANSPORT AND MAGNETIC PROPERTIES OF YBA2CU3O7-ZBRY SINGLE CRYSTALS	199307			PHYS.REV.B,48(1993)1148	A.M.RAO,G.DRESSELHAUS,H.B.RADOUSKY,J.S.MOODERA,J.Z.LIU,M.S.DRESSELHAUS,P.P.NGUYEN,R.S.GLASS,Z.H.WANG		
4266	PR0480607	SOUND VELOCITY AND SPECIFIC HEAT SHOW JUMP AT 150K	(Y,Ca)Ba2Cu4O8	Y0.975Ca0.025Ba2Cu4O8	Y	0.975	Ca	0.025	Ba	2	Cu	4													O	8		1	1993																												Y124																				82		82			82																																																																																															1	HIP USING AR+O2 GAS					CA-INDUCED PHASE TRANSITION AT 150 K IN Y1-XCAXBA2CU4O8 SINGLE-PHASE HIGH-TC SUPERCONDUCTING MATERIAL	199307			PHYS.REV.B,48(1993)607	H.YAMAUCHI,K.FOSSHEIM,M.G.KARKUT,O.-M.NES,S.TANAKA,T.SUZUKI,WU.TING,Y.YAEGASHI		
4267	PR0480607	SEE 4266	(Y,Ca)Ba2Cu4O8	Y0.95Ca0.05Ba2Cu4O8	Y	0.95	Ca	0.05	Ba	2	Cu	4													O	8			1993																												Y124																				87		87			87																																																																																															1	HIP USING AR+O2 GAS					CA-INDUCED PHASE TRANSITION AT 150 K IN Y1-XCAXBA2CU4O8 SINGLE-PHASE HIGH-TC SUPERCONDUCTING MATERIAL	199307			PHYS.REV.B,48(1993)607	H.YAMAUCHI,K.FOSSHEIM,M.G.KARKUT,O.-M.NES,S.TANAKA,T.SUZUKI,WU.TING,Y.YAEGASHI		
4268	PR0480607	SEE 4266	(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8			1993																												Y124																				89		89			89																																																																																															1	HIP USING AR+O2 GAS					CA-INDUCED PHASE TRANSITION AT 150 K IN Y1-XCAXBA2CU4O8 SINGLE-PHASE HIGH-TC SUPERCONDUCTING MATERIAL	199307			PHYS.REV.B,48(1993)607	H.YAMAUCHI,K.FOSSHEIM,M.G.KARKUT,O.-M.NES,S.TANAKA,T.SUZUKI,WU.TING,Y.YAEGASHI		
4269	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.3Ba1.45Cu3O7.11	La	1.25	Ca	0.3	Ba	1.45	Cu	3													O	Z	7.11	1	1993																											2	Y123				3.883		11.649															74.6	67.1		3.9	67.1																																																																																		1.92													0						TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4270	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.35Ba1.4Cu3O7.108	La	1.25	Ca	0.35	Ba	1.4	Cu	3													O	Z	7.108		1993																												Y123																					78.5	74.3		2.6	74.3																																																																																		1.29													0						TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4271	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.4Ba1.35Cu3O7.141	La	1.25	Ca	0.4	Ba	1.35	Cu	3													O	Z	7.141		1993																												Y123				3.876		11.634															80.6	77.8		1.3	77.8																																																																																		1.48													0						TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4272	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.45Ba1.3Cu3O7.135	La	1.25	Ca	0.45	Ba	1.3	Cu	3													O	Z	7.135		1993																												Y123																					81.4	79.2		0.9	79.2																																																																																		1.04													0						TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4273	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.5Ba1.25Cu3O7.137	La	1.25	Ca	0.5	Ba	1.25	Cu	3													O	Z	7.137		1993																												Y123				3.873		11.622															81.3	79.2		0.7	79.2																																																																																		1.04													0						TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4274	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ba1.75Cu3O7.07	La	1.25	Ba	1.75	Cu	3															O	Z	7.07	1	1993																											2	Y123				3.917		11.751															47.8	40		5.3	40																																																																																		3.54												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4275	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.05Ba1.7Cu3O7.03	La	1.25	Ca	0.05	Ba	1.7	Cu	3													O	Z	7.03		1993																												Y123																					46.7	38.6		6.1	38.6																																																																																		3.47												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4276	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.1Ba1.65Cu3O7.06	La	1.25	Ca	0.1	Ba	1.65	Cu	3													O	Z	7.06		1993																												Y123				3.906		11.718															48.3	38.8		5.4	38.8																																																																																		3.02												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4277	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.15Ba1.6Cu3O7.052	La	1.25	Ca	0.15	Ba	1.6	Cu	3													O	Z	7.052		1993																												Y123																					51.9	45.6		5.1	45.6																																																																																		2.5												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4278	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.2Ba1.55Cu3O7.082	La	1.25	Ca	0.2	Ba	1.55	Cu	3													O	Z	7.082		1993																												Y123				3.894		11.685															61.7	50.2		5.4	50.2																																																																																		2.53												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4279	PR0480532		(Ca,La)(Ba,La)2Cu3O7	La1.25Ca0.25Ba1.5Cu3O7.087	La	1.25	Ca	0.25	Ba	1.5	Cu	3													O	Z	7.087		1993																												Y123																					70	62.9		5.4	62.9																																																																																		1.6												CACO3,LA2O3,BACO3,CUO	1	MIXTURE-HEAT(950C,1-2DAYS IN AIR)-PELLET-SIN(960C,60H IN O2)-COOL(10C/H) TO RT					TETRAGONAL SUPERCONDUCTING FAMILY (CAXLA1-X)(BA1.75-XLA0.25+X)CU3OY: THE EFFECT OF COSUBSTITUTION ON THE TRANSITION TEMPERATURE	199307			PHYS.REV.B,48(1993)532	A.KNIZHNIK,D.GOLDSCHMIDT,E.GARTSTEIN,G.KIMMEL,G.M.REISNER,Y.DIREKTOVITCH,Y.ECKSTEIN		
4280	PR04711525		BaPbO	Ba1Pb1O1	Ba	1	Pb	1																	O	1		1	1993																											3					6.056	6.024	8.506																	4.2																																																																																				1.2				-0.00000002				1				BA(OH)2.8H2O,PB3O4	1	SLOW HEAT TO 750C-PELLET-(825C,2H IN O2)+(500C,5H)					OXYGEN-DEFICIENT BARIUM LEAD OXIDE PEROVSKITES	199305			PHYS.REV.B,47(1993)11525	H.TAKAGI,H.Y.HWANG,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK		
4281	PR04711525		Ba4Pb3O10	Ba4Pb3O10	Ba	4	Pb	3																	O	10		1	1993																											2					4.289		30.278																	4.2																																																																																				3.5				-0.000000018				1				BACO3,PB(NO3)2	0	HEAT(825C,15H IN O2)-(950C,48H)-PELLET-(950C,48H+850C,5H+500C,5H IN O2)					OXYGEN-DEFICIENT BARIUM LEAD OXIDE PEROVSKITES	199305			PHYS.REV.B,47(1993)11525	H.TAKAGI,H.Y.HWANG,J.J.KRAJEWSKI,JR.,R.J.CAVA,W.F.PECK		
4282	PR04711544	EFFECTIVE O2 PRESSURE DURING ANN=20 ATM	(La,Ca)2CaCu2O6	La1.89Ca1.11Cu2OZ	La	1.89	Ca	1.11	Cu	2															O	Z		3	1993																												2126																							4.2																																																																																					7.2							6					0	CRYSTAL GROWN IN AIR FROM CUO-RICH MELT-ANN(1040-1080C,200H IN 20%O2+80%AR AT PRESSURE OF 100-1500 ATM)					EFFECTS OF HIGH-OXYGEN-PRESSURE ANNEALING ON TRANSPORT PROPERTIES FOR LA1.89CA1.11CU2O6+-Z SINGLE CRYSTALS	199305			PHYS.REV.B,47(1993)11544	AZUSA MATSUDA,KYOICHI KINOSHITA,TAKAO WATANABE		
4283	PR04711544	EFFECTIVE O2 PRESSURE DURING ANN=100 ATM	(La,Ca)2CaCu2O6	La1.89Ca1.11Cu2OZ	La	1.89	Ca	1.11	Cu	2															O	Z		3	1993																												2126																			13						13																																																																																			1.914							6					0	CRYSTAL GROWN IN AIR FROM CUO-RICH MELT-ANN(1040-1080C,200H IN 20%O2+80%AR AT PRESSURE OF 100-1500 ATM)					EFFECTS OF HIGH-OXYGEN-PRESSURE ANNEALING ON TRANSPORT PROPERTIES FOR LA1.89CA1.11CU2O6+-Z SINGLE CRYSTALS	199305			PHYS.REV.B,47(1993)11544	AZUSA MATSUDA,KYOICHI KINOSHITA,TAKAO WATANABE		
4284	PR04711544	EFFECTIVE O2 PRESSURE DURING ANN=300 ATM	(La,Ca)2CaCu2O6	La1.89Ca1.11Cu2OZ	La	1.89	Ca	1.11	Cu	2															O	Z		3	1993																												2126																			40						40																																																																																			0.819							6					0	CRYSTAL GROWN IN AIR FROM CUO-RICH MELT-ANN(1040-1080C,200H IN 20%O2+80%AR AT PRESSURE OF 100-1500 ATM)					EFFECTS OF HIGH-OXYGEN-PRESSURE ANNEALING ON TRANSPORT PROPERTIES FOR LA1.89CA1.11CU2O6+-Z SINGLE CRYSTALS	199305			PHYS.REV.B,47(1993)11544	AZUSA MATSUDA,KYOICHI KINOSHITA,TAKAO WATANABE		
4285	PR0476177	211 PHASE INCLUDED,HC(0)=0.78 T, G-L PARAMETER=63	YBa2(Cu,Au)3O7	Y1Ba1.97Cu2.55Au0.13OX	Y	1	Ba	1.97	Cu	2.55	Au	0.13													O	X		2	1993																											3	Y123																				93.3				1	93.3																															1.5																																																																1	ADDING METALLIC AU POWDER-MIX-PELLET-SIN-ANN(400C)-Q					UPPER CRITICAL FIELD OF GOLD-DOPED YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6177	K.H.KELLEHER,M.DAUMLING,P.R.DUNCOMBE,R.A.FIGAT,T.M.SHAW	Y,BA,CU,O	
4286	PLA1420300		La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			1989																											2	T														0.002	0.002	0.002																																																																																																								1	MIXTURE-PELLET BY 10KBAR-HEAT(1323K IN O2)-HEAT(1223K,2 DAYS)-COOL TO RT IN AIR					X-RAY INVESTIGATION OF La2CuO4 AND Pr2CuO4 UNDER HIGH PRESSURE	198911		Kernforschungszentrum Karlsruhe and Universitat Karlsruhe, Postfach 3640, D-7500 Karlsruhe, FRG	Phys.Lett.A,142(1989)300	"C.A. WASSILEW,D. EWERT,D. HOCHHEIMER,H. WU""HL,M.R. DIETRICH,W.H. FIETZ,Z. FISK"		
4287	PLA1420300		Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4			1989																											2	T'														0.002	0.002	0.003																																																																																																								0	CRYSTAL GROWN FROM PB-O BASED FLUX-MIXTURE-HEAT(1520K,2H IN AIR)-COOL TO 1070K(7K/H)					X-RAY INVESTIGATION OF La2CuO4 AND Pr2CuO4 UNDER HIGH PRESSURE	198911		Kernforschungszentrum Karlsruhe and Universitat Karlsruhe, Postfach 3640, D-7500 Karlsruhe, FRG	Phys.Lett.A,142(1989)300	"C.A. WASSILEW,D. EWERT,D. HOCHHEIMER,H. WU""HL,M.R. DIETRICH,W.H. FIETZ,Z. FISK"		
4288	PR0475524	TC(MAX)=131.5K AT 7.4GPA	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10-Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10-Z		3	1993																												Tl2223																				116					116			K/GPa	4.8																																																																																										TL2O3,BAO2,CAO2,CUO	0	TL:BA:CA:CU=2:2:3:4, IN AU CAPSULE,)917C,4H)-COOL TO 697C IN 12H-FC-REMOVED AT 350C					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE IN SINGLE CRYSTALS OF TL2BA2CA2CU3O10-X	199303			PHYS.REV.B,47(1993)5524	D.D.BERKLEY,E.F.SKELTON,M.S.OSOFSKY,N.E.MOULTON,V.M.BROWNING,W.T.LECHTER	TL,BA,CA,CU,O	
4289	PR0476154	ABOUT 10% OF CHAIN CU WERE REPLACED BY AU,9 INDEPENDENT ELASTIC CONST. C(I,I) ARE DETERMINED	YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	3	1993									6.333			GPa		154.3	GPa		58.7	GPa		138.2		0.314			0.251		3	Y123																				91.4				0.7	91.4																																																											414																																				0	SELF-FLUX METHOD IN AU CRUCIBLE					ELASTIC CONSTANTS OF A MONOCRYSTAL OF SUPERCONDUCTING YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6154	A.MOGLIORI,B.W.VEAL,J.D.THOMPSON,J.L.SARRAO,MING LEI,T.M.BELL,U.W.WELP,WILLIAM M.VISSCHER	Y,BA,CU,O	
4290	PR04711337		RSr2(Cu,Mo)3O7	Yb1Sr2Cu2.7Mo0.3OZ	Yb	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				34	35.9				34				5.9																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4291	PR04711337		RSr2(Cu,Mo)3O7	Tm1Sr2Cu2.7Mo0.3OZ	Tm	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				33.9	35.4				33.9			K/GPa	5.7																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4292	PR04711337		RSr2(Cu,Mo)3O7	Er1Sr2Cu2.7Mo0.3OZ	Er	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				35.1	36.7				35.1			K/GPa	6.1																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4293	PR04711337		RSr2(Cu,Mo)3O7	Ho1Sr2Cu2.7Mo0.3OZ	Ho	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				34.1	35.7				34.1			K/GPa	6.4																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4294	PR04711337		RSr2(Cu,Mo)3O7	Dy1Sr2Cu2.7Mo0.3OZ	Dy	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				31.9	35.8				31.9				4.7																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4295	PR04711337		RSr2(Cu,Mo)3O7	Gd1Sr2Cu2.7Mo0.3OZ	Gd	1	Sr	2	Cu	2.7	Mo	0.3													O	Z		1	1993																												Y123																				31.1	33.6				31.1			K/GPa	4																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4296	PR04711337		RSr2(Cu,Mo)3O7	Eu1Sr2Cu2.7Mo0.3OZ	Eu	1	Sr	2	Cu	2.7	Mo	0.3													O	Z			1993																												Y123																				27.1	30				27.1			K/GPa	3.7																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4297	PR04711337		RSr2(Cu,Mo)3O7	Sm1Sr2Cu2.7Mo0.3OZ	Sm	1	Sr	2	Cu	2.7	Mo	0.3													O	Z			1993																												Y123																		K		31.5	33.6				31.5			K/GPa	3.9																																																																																											0						HIGH-PRESSURE STUDY OF RSR2CU2.7MO0.3OY WITH R=SM,EU,GD,TB,DY,HO,ER,TM,AND YB	199305			PHYS.REV.B,47(1993)11337	C.W.CHU,J.W.CHU,P.H.HOR,Q.XIONG,Y.Q.WANG,Y.Y.SUN,Y.Y.XUE		
4298	PHC1990430	YB<0.8-X>ND<X>PR0.2BA2CU3O<7-Z>,FIGURE SHOWS TC VS X	(Yb,Nd,Pr)Ba2Cu3O7	Yb0.6Nd0.2Pr0.2Ba2Cu3O7-Z	Yb	0.6	Nd	0.2	Pr	0.2	Ba	2	Cu	3											O	7-Z		1	1992																											3	Y123																		K		70.3					70.3	TC4298																																																																																														0						ION SIZE EFFECT ON TC IN THE (YB0.8-ZNDZPR0.2)BA2CU3O7-Y AND (ER0.7-ZEUZPR0.3)BA2CU3O7-Y SYSTEMS	199209			PHYSICA C,199(1992)430	WEIYAN GUAN,YUNHUI XU	ER,EU,YB,ND,PR,BA,CU,O	
4299	PHC1990430	ER<0.7-X>EU<X>PR0.3BA2CU3O<7-Z>,FIGURE SHOWS TC VS X	(Er,Eu,Pr)Ba2Cu3O7	Er0.5Eu0.2Pr0.3Ba2Cu3O7-Z	Er	0.5	Eu	0.2	Pr	0.3	Ba	2	Cu	3											O	7-Z		1	1992																											3	Y123																		K		52.1					52.1	TC4299																																																																																														0						ION SIZE EFFECT ON TC IN THE (YB0.8-ZNDZPR0.2)BA2CU3O7-Y AND (ER0.7-ZEUZPR0.3)BA2CU3O7-Y SYSTEMS	199209			PHYSICA C,199(1992)430	WEIYAN GUAN,YUNHUI XU	ER,EU,YB,ND,PR,BA,CU,O	
4300	PHC1990430		(Yb,Nd,Pr)Ba2Cu3O7	Yb0.4Nd0.4Pr0.2Ba2Cu3O7-Z	Yb	0.4	Nd	0.4	Pr	0.2	Ba	2	Cu	3											O	7-Z		1	1992																											3	Y123																		K	54.1	56.6		57			56.6																																																																																		4													0						ION SIZE EFFECT ON TC IN THE (YB0.8-ZNDZPR0.2)BA2CU3O7-Y AND (ER0.7-ZEUZPR0.3)BA2CU3O7-Y SYSTEMS	199209			PHYSICA C,199(1992)430	WEIYAN GUAN,YUNHUI XU	ER,EU,YB,ND,PR,BA,CU,O	
4301	PHC1990430		(Er,Eu,Pr)Ba2Cu3O7	Er0.4Eu0.3Pr0.3Ba2Cu3O7-Z	Er	0.4	Eu	0.3	Pr	0.3	Ba	2	Cu	3											O	7-Z		1	1992																											3	Y123																		K	44.6	47.8		48			47.8																																																																																		4													0						ION SIZE EFFECT ON TC IN THE (YB0.8-ZNDZPR0.2)BA2CU3O7-Y AND (ER0.7-ZEUZPR0.3)BA2CU3O7-Y SYSTEMS	199209			PHYSICA C,199(1992)430	WEIYAN GUAN,YUNHUI XU	ER,EU,YB,ND,PR,BA,CU,O	
4302	PHC1990285	Tc/Tc0 = 0.709 for x=0.1	(Sm,Pr)Ba2Cu3O7	Sm0.9Pr0.1Ba2Cu3O7-Z	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z			1992																												Y123																		K								TC4302																																																																																													CUO,BACO3,PR6O11,R2O3	1	MIXTURE-CAL(920C,20H IN AIR)-PELLET-CAL(940C,3DAYS IN O2)-COOL TO RT(1C/MIN)					RARE-EARTH IONIC SIZE EFFECT ON THE PR-INDUCED TC DEPRESSION IN THE SERIES R1-XPRXBA2CU3O7-Z (R=SM,GD,Y,ER,TM)	199209			PHYSICA C,199(1992)285	P.LIU,W.J.ZHU,Z.X.ZHAO	SM,GD,Y,ER,TM,PR,BA,CU,O	
4303	PHC1990285	Tc/Tc0 = 0.835 for x=0.1	(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3O7-Z	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z			1992																												Y123																		K								TC4303																																																																																													CUO,BACO3,PR6O11,R2O3	1	MIXTURE-CAL(920C,20H IN AIR)-PELLET-CAL(940C,3DAYS IN O2)-COOL TO RT(1C/MIN)					RARE-EARTH IONIC SIZE EFFECT ON THE PR-INDUCED TC DEPRESSION IN THE SERIES R1-XPRXBA2CU3O7-Z (R=SM,GD,Y,ER,TM)	199209			PHYSICA C,199(1992)285	P.LIU,W.J.ZHU,Z.X.ZHAO	SM,GD,Y,ER,TM,PR,BA,CU,O	
4304	PHC1990285	Tc/Tc0 = 0.638 for x=0.2	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1992																												Y123																		K								TC4304																																																																																													CUO,BACO3,PR6O11,R2O3	1	MIXTURE-CAL(920C,20H IN AIR)-PELLET-CAL(940C,3DAYS IN O2)-COOL TO RT(1C/MIN)					RARE-EARTH IONIC SIZE EFFECT ON THE PR-INDUCED TC DEPRESSION IN THE SERIES R1-XPRXBA2CU3O7-Z (R=SM,GD,Y,ER,TM)	199209			PHYSICA C,199(1992)285	P.LIU,W.J.ZHU,Z.X.ZHAO	SM,GD,Y,ER,TM,PR,BA,CU,O	
4305	PHC1990285	Tc/Tc0 = 0.823 for x=0.2	(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3O7-Z	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1992																												Y123																		K								TC4305																																																																																													CUO,BACO3,PR6O11,R2O3	1	MIXTURE-CAL(920C,20H IN AIR)-PELLET-CAL(940C,3DAYS IN O2)-COOL TO RT(1C/MIN)					RARE-EARTH IONIC SIZE EFFECT ON THE PR-INDUCED TC DEPRESSION IN THE SERIES R1-XPRXBA2CU3O7-Z (R=SM,GD,Y,ER,TM)	199209			PHYSICA C,199(1992)285	P.LIU,W.J.ZHU,Z.X.ZHAO	SM,GD,Y,ER,TM,PR,BA,CU,O	
4306	PHC1990285	Tc/Tc0 = 0.871 for x=0.2	(Tm,Pr)Ba2Cu3O7	Tm0.8Pr0.2Ba2Cu3O7-Z	Tm	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1992																												Y123																		K								TC4306																																																																																													CUO,BACO3,PR6O11,R2O3	1	MIXTURE-CAL(920C,20H IN AIR)-PELLET-CAL(940C,3DAYS IN O2)-COOL TO RT(1C/MIN)					RARE-EARTH IONIC SIZE EFFECT ON THE PR-INDUCED TC DEPRESSION IN THE SERIES R1-XPRXBA2CU3O7-Z (R=SM,GD,Y,ER,TM)	199209			PHYSICA C,199(1992)285	P.LIU,W.J.ZHU,Z.X.ZHAO	SM,GD,Y,ER,TM,PR,BA,CU,O	
4307	PHC1990276	HALL EFFECT BY VAN DER PAUW, NOT S/C	Bi2Sr2CuO6	Bi2Sr2Cu1O6.17	Bi	2	Sr	2	Cu	1															O	6+Z	6.17		1992																												Bi2201																							4.2																																																																					-8.5			TP4307																0.0000000008				5	RH4307				1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4308	PHC1990276		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6.2	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z	6.2		1992																												Bi2201																				12					12																																																																			-11.9			TP4308																0.0000000024				5	RH4308				1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4309	PHC1990276		Bi2(Sr,La)2CuO6	Bi2Sr1.8La0.2Cu1O6.3	Bi	2	Sr	1.8	La	0.2	Cu	1													O	6+Z	6.3		1992																												Bi2201																				18					18																																																																			-10.8			TP4309																									1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4310	PHC1990276		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.35	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z	6.35		1992																												Bi2201																				20					20																																																																			-7.3			TP4310																									1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4311	PHC1990276		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6.38	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+Z	6.38		1992																												Bi2201																				21					21																																																																			-1			TP4311																									1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4312	PHC1990276		Bi2(Sr,La)2CuO6	Bi2Sr1.4La0.6Cu1O6.42	Bi	2	Sr	1.4	La	0.6	Cu	1													O	6+Z	6.42		1992																												Bi2201																				5					5																																																																			1.2			TP4312																									1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4313	PHC1990276	NOT S/C	Bi2(Sr,La)2CuO6	Bi2Sr1La1Cu1O6.6	Bi	2	Sr	1	La	1	Cu	1													O	6+Z	6.6		1992																												Bi2201																							4.2																																																																																																	1	SEE SSC0720697					TRANSPORT PROPERTIES OF BI2SR2-XLAXCUO6+Z	199209			PHYSICA C,199(1992)276	A.J.SMITS,J.M.VAN RUITENBEEK,L.J.DE JONGH,W.A.GROEN,W.J.ELION	BI,SR,LA,CU,O	
4314	PRL0711238	LINEAR REGION IN HC2(T) NOT EXIST, FIGURE SHOWS HC2(T)	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	1993																												Tl2201																				15				1.8	15																				T	resistive transition 	15.8																																																					0.025							0.195																			RESISTIVE UPPER CRITICAL FIELD OF TL2BA2CUO6 AT LOW TEMPERATURES AND HIGH MAGNETIC FIELDS	199308			PHYS.REV.LETT.,71(1993)1238	A.CARRINGTON,A.P.MACKENZIE,D.C.SINCLAIR,G.G.LONZARICH,R.S.LIU,S.D.HUGHES,S.R.JULIAN		
4315	PHC1990240		(La,Eu)CaBaCu3O7	La0.8Eu0.2Ca1Ba1Cu3OZ	La	0.8	Eu	0.2	Ca	1	Ba	1	Cu	3											O	Z		1	1992																											2	Y123				3.866		11.587														69					69																																																																																		8.61													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4316	PHC1990240		(La,Eu)CaBaCu3O7	La0.6Eu0.4Ca1Ba1Cu3OZ	La	0.6	Eu	0.4	Ca	1	Ba	1	Cu	3											O	Z		1	1992																											2	Y123				3.863		11.573														65					65																																																																																		10.17													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4317	PHC1990240		(La,Eu)CaBaCu3O7	La0.4Eu0.6Ca1Ba1Cu3OZ	La	0.4	Eu	0.6	Ca	1	Ba	1	Cu	3											O	Z		1	1992																											2	Y123				3.857		11.595														62					62																																																																																		6.92													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4318	PHC1990240		(La,Eu)CaBaCu3O7	Eu1Ca1Ba1Cu3OZ	Eu	1	Ca	1	Ba	1	Cu	3													O	Z		1	1992																												Y123				3.865		11.637														53					53																																																																																		31.37													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4319	PHC1990240		(La,Sm)CaBaCu3O7	La0.8Sm0.2Ca1Ba1Cu3O7-Z	La	0.8	Sm	0.2	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.861		11.626														71					71																																																																																		2.7													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4320	PHC1990240		(La,Sm)CaBaCu3O7	La0.6Sm0.4Ca1Ba1Cu3O7-Z	La	0.6	Sm	0.4	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.859		11.612														68					68																																																																																		5.81													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4321	PHC1990240		(La,Sm)CaBaCu3O7	La0.4Sm0.6Ca1Ba1Cu3O7-Z	La	0.4	Sm	0.6	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.853		11.613														64					64																																																																																		4.45													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4322	PHC1990240		(La,Sm)CaBaCu3O7	La0.2Sm0.8Ca1Ba1Cu3O7-Z	La	0.2	Sm	0.8	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123																				56					56																																																																																		8.72													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4323	PHC1990240		(La,Sm)CaBaCu3O7	Sm1Ca1Ba1Cu3O7-Z	Sm	1	Ca	1	Ba	1	Cu	3													O	7-Z		1	1992																												Y123																				39					39																																																																																		33.39													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4324	PHC1990240	STRUCTURE CALLED ALSO AS 1113 PHASE	(La,Nd)CaBaCu3O7	La1Ca1Ba1Cu3O7-Z	La	1	Ca	1	Ba	1	Cu	3													O	7-Z		1	1992																											2	Y123				3.871		11.61														72					72																																																																																		1.84													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4325	PHC1990240	4324	(La,Nd)CaBaCu3O7	La0.8Nd0.2Ca1Ba1Cu3O7-Z	La	0.8	Nd	0.2	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.866		11.606														71					71																																																																																		3.96													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4326	PHC1990240	4324	(La,Nd)CaBaCu3O7	La0.6Nd0.4Ca1Ba1Cu3O7-Z	La	0.6	Nd	0.4	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.864		11.617														67					67																																																																																		3.52													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4327	PHC1990240	4324	(La,Nd)CaBaCu3O7	La0.4Nd0.6Ca1Ba1Cu3O7-Z	La	0.4	Nd	0.6	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.86		11.622														63					63																																																																																		4.64													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4328	PHC1990240	4324	(La,Nd)CaBaCu3O7	La0.2Nd0.8Ca1Ba1Cu3O7-Z	La	0.2	Nd	0.8	Ca	1	Ba	1	Cu	3											O	7-Z		1	1992																											2	Y123				3.857		11.628														57					57																																																																																		12.23													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4329	PHC1990240	4324	(La,Nd)CaBaCu3O7	Nd1Ca1Ba1Cu3O7-Z	Nd	1	Ca	1	Ba	1	Cu	3													O	7-Z		1	1992																											2	Y123				3.854		11.629														46					46																																																																																		20.15													1						PHASE STABILITY AND SUPERCONDUCTING CHARACTERISTICS OF CABA(LA1-XRX)CU3O7-Z(R=RARE EARTH) SYSTEM	199209		CHEMISTRY DIVISION, BHABHA ATOMIC RESEARCH CENTRE, INDIA	PHYSICA C,199(1992)240	I.K.GOPALAKRISHNAN,J.V.YAKHMI,P.V.P.S.S.SASTRY,R.A.GUNASEKARAN,R.M.IYER	CA,BA,LA,R,CU,O	
4330	PHC2030144	SEMICOND.-LIKE,FERROMAGNETIC,COERCIVE FORCE=7960 OE, MOMENT PER CO CALCULATED FROM CURIE CONST.	Bi2Ca2(Ca,La)Co2OZ	Bi2Ca2.5La0.5Co2OZ	Bi	2	Ca	2.5	La	0.5	Co	2													O	Z			1992						1.8	147																				3	Bi2212				5.54	5.36	29.32																																																																																																					900												BI2O3,LA2O3,CACO3,CO3O4	1	MIXTURE-CAL(840C IN AIR)-SIN(870-910,50H IN AIR)					MAGNETIC PROPERTIES OF BI-BASED LAYERED COBALT OXIDES, BAI2CA3-XLAXCO2OY	199212		SUPERCONDUCTIVITY RESEARCH LABORATORY, TOKYO	PHYSICA C,203(1992)144	H.YAYAUCHI,HIROAKI HIDAKA,HIROSHI YOSHIKAWA,JUN SUGIYAMA,KOICHI NAKAO	BI,CA,LA,CO,O	
4331	PHC2020209	PHASE DIAGRAM FOR 4<4+Z<4.09	La2CuO4	La2Cu1O4.09	La	2	Cu	1																	O	4+Z	4.09		1992																												T																				32					32													640																																																																																	BACO3,Y2O3,CUO	1						TRANSPORT AND MAGNETIC PROPERTIES OF THE SUPERCONDUCTING LA2CUO4-Z PHASE (0<Z<0.09) PREPARED BY ELECTROCHEMICAL OXIDATION	199211		LABORATOIRE DE CHIMIE DU SOLIDE DU CNRS, UNIVERSITE DE BORDEAUX, FRANCE	PHYSICA C,202(1992)209	A.WATTIAUX,J-P.DOUMERC,J.-C.GRENIER,J.ETOURNEAU,M.POUCHARD,N.LAGUEYTE,P.DORDOR	LA,CU,O	
4332	PHC2010305	F CONTENT NOT MEASURED,TRANSPORT PROPERTIES ARE NOT CHANGED DRASTICALLY BY F	YBa2Cu3(O,F)7	Y1Ba2Cu3FOZ	Y	1	Ba	2	Cu	3	F														O	Z			1992																											3	Y123																			91	92	93				92																																																																	THC4332		4.11			TP4332																									0	(900C IN AIR)-ANN(500C,24H IN O2)-COOL TO RT(100C/H)-FLUORINATION BELOW 100C					INFLUENCE OF LOW-TEMPERATURE FLUORINATION ON THE TRANSPORT PROPERTIES OF YBA2CU3O7-Z	199210		UNIVERSITE CATHOLIQUE DE LOUVAIN, BELGIUM	PHYSICA C,201(1992)305	A.TRESSAUD,B.CHEVALIER,J.ETOURNEAU,J.P.ISSI,M.CASSART	Y,BA,CU,O,F	
4333	PHC2010320		(Y,Ca)Sr2Cu2(CO3)OZ	Y0.475Ca0.475Sr2.05Cu2.4C0.6OZ	Y	0.475	Ca	0.475	Sr	2.05	Cu	2.4	C	0.6											O	Z			1992																											2	Y123				3.846		11.081													37		66	63		29	63										5																																																																	36							50												SRCO3,CACO3,Y2O3,CUO	1	MIXTURE-PELLET-CAL(1050C,15H IN 80%O2+20%CO2)-Q TO RT-HIP AT 10MPA(700C,30H IN 0.1%CO2-O2)				an excess amount of CO3 in raw materials was dissociated during calcination	SUPERCONDUCTIVITY IN THE NEW COMPOUND (Y1-XCAX)0.95SR2.05CU2.4(CO3)0.6OY	199210		DEPARTMENT OF PHYSICAS, AOYAMA-GAKUIN UNIVERSITY, TOKYO	PHYSICA C,201(1992)320	H.NAKATA,H.YAMANE,J.AKIMITSU,K.KINOSHITA,K.TOMIMOTO,M.OGAWA,M.UEHARA,T.HIRAI,Y.MATSUI,Y.MIYAZAKI	Y,CA,SR,CU,C,O	
4334	PHC2010403	NEARLY SINGLE PHASE	(Ga,Cu)(Sr,Eu)2(Eu,Ce)2Cu2OZ	Ga0.5Sr1.5Eu2Ce0.5Cu2.5OZ	Ga	0.5	Sr	1.5	Eu	2	Ce	0.5	Cu	2.5											O	Z			1992																											2	1222				3.84		28.14													22		28				25										10																																																																																				GA2O3,SRCO3,CEO2,EU2O3,CUO	1	MIXTURE-CAL(960C,24H IN AIR)-PELLET-SIN(1050C,24H IN1 ATM O2)-ANN(1000C,5H IN AR-20%O2 OF 2000 ATM) USING HIP					SYNTHESIS OF (GA/CU)(SR/E)2(EU/CE)2CU2OY SUPERCONDUCTOR	199210		SUPERCONDUCTIVITY RESEARCH RABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYSICA C,201(1992)403	AKIKO NARA,H.YAMAUCHI,SEIJI ADACHI	GA,CU,SR,EU,CE,O	
4335	PHC1980273		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1992																																																																																																					4.7	1																																														0						TUNNELING SPECTRA OF A BI2SR2CACU2O8 SINGLE CRYSTAL WITH WELLDEFINED BI2SR2CUO6 ARTIFICIAL BARRIER	199208			PHYSICA C,198(1992)273	KATSUKI KITAHAMA,SHICHIO KAWAI,TAKUYA MATSUMOTO,TOMOJI KAWAI	BI,SR,CA,CU,O	
4336	PHC1970053	1.2*0.9*0.03 MM3	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1992																											3	Y123																				92				0.5	92																																										BY ESR BROADENING			6250																																																		5	FROM DR. P.HOR					MEASUREMENT OF MAGNETIC FIELD PENETRATION DEPTH IN YBA2CU3O7-ZSINGLE CRYSTALS BY SURFACE PARAMAGNETIC PROBES	199207			PHYSICA C,197(1992)53	LARRY KEVAN,MICKY PURI	Y,BA,CU,O	
4337	PHC2040413		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1993																											3	Y124	AMMM			3.839	3.869	27.243														81.5		81.5			81.5																																																																																															1	BACU2O3+Y2O3(OR DY2O3)+CEO2-SIN(1085K IN O2)					THE INFLUENCE OF SUBSTITUTION OF CE ON THE SUPERCONDUCTING BEHAVIOUR OF YBA2CU4O8 AND DYBA2CU4O8	199301			PHYSICA C,204(1993)413	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.IYER	Y,BA,CU,O,DY	
4338	PHC2040413		(Y,Ce)Ba2Cu4O8	Y0.9Ce0.1Ba2Cu4O8	Y	0.9	Ce	0.1	Ba	2	Cu	4													O	8		1	1993																											3	Y124				3.845	3.871	27.236														56.5		56.5			56.5																																																																																															1	BACU2O3+Y2O3(OR DY2O3)+CEO2-SIN(1085K IN O2)					THE INFLUENCE OF SUBSTITUTION OF CE ON THE SUPERCONDUCTING BEHAVIOUR OF YBA2CU4O8 AND DYBA2CU4O8	199301			PHYSICA C,204(1993)413	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.IYER	Y,BA,CU,O,DY	
4339	PHC2040413		DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		1	1993																											3	Y124				3.844	3.872	27.223														76		76			76																																																																																															1	BACU2O3+Y2O3(OR DY2O3)+CEO2-SIN(1085K IN O2)					THE INFLUENCE OF SUBSTITUTION OF CE ON THE SUPERCONDUCTING BEHAVIOUR OF YBA2CU4O8 AND DYBA2CU4O8	199301			PHYSICA C,204(1993)413	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.IYER	Y,BA,CU,O,DY	
4340	PHC2040413		(Dy,Ce)Ba2Cu4O8	Dy0.9Ce0.1Ba2Cu4O8	Dy	0.9	Ce	0.1	Ba	2	Cu	4													O	8		1	1993																											3	Y124				3.846	3.876	27.205														44		44			44																																																																																															1	BACU2O3+Y2O3(OR DY2O3)+CEO2-SIN(1085K IN O2)					THE INFLUENCE OF SUBSTITUTION OF CE ON THE SUPERCONDUCTING BEHAVIOUR OF YBA2CU4O8 AND DYBA2CU4O8	199301			PHYSICA C,204(1993)413	I.K.GOPALAKRISHNAN,J.V.YAKHMI,R.M.IYER	Y,BA,CU,O,DY	
4341	PHC1970157	CU-O LENGTH=1.898A IN PLANE,KAIZERO(C//)=1.2 E-5 CM3/MOLE	Bi2Sr2CuO6	Bi2Sr2Cu1O6+Z	Bi	2	Sr	2	Cu	1															O	6+Z		3	1992	CM3/MOLE		CM3.K/MOLE				1.1																				3	Bi2201				5.364	5.375	24.62																																																																																																																		0	GROWN BY SELF-FLUX METHOD, HEAT(1000C,1H IN ALUMINA CRUCIBLE IN AIR)-SLOWWLY COOLED TO 800C AT 5C/H-FC TO RT AT 100C/H					ANISOTROPIC MAGNETIC PROPERTIES OF BI2SR2CUO6+Z SINGLE CRYSTAL	199207			PHYSICA C,197(1992)157	B.S.CHIOU,H.C.KU,J.B.SHI,J.C.HO	BI,SR,CU,O	
4342	PR0471153	94% DENSE,GRAIN SIZE=2-3MICRON,POROCITY=5%,SOUND VELOCITY V(L)=5.10KM/S,V(S)=2.69KM/S	YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z			1993									5.96									GPa		96							3	Y123																				60					60																																																											370	FROM SOUND VELOCITY																																			1	SIN(950C)-BALL MILLING-HIP(900C,80MPA IN STAINLESS					ULTRASONIC VELOCITIES IN DENSE YBA2CU3O7-Z AT HIGH PRESSURE	199301		RESEARCH SCHOOL OF EARTH SCIENCES, AUSTRALIAN NATIONAL UNIVERSITY	PHYS.REV.B,47(1993)1153	E.R.VANCE,GUY K.WHITE,SALLY RIGDEN	Y,BA,CU,O	
4343	PR0471123	IMPURITY PHASE EXISTS,NQR EXPERIMENT	(Lu,Pr)Ba2Cu3O7	Lu0.9Pr0.1Ba2Cu3O2	Lu	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	2		1993																											3	Y123				3.806	3.875	11.601														85					85																																																																																														LU2O3,PR6O11,BACO3,CUO	1	MIXTURE-SIN(900C,24H)-PELLET-HEAT(800C,1H IN O2)-ANN(450C,24H)-SLOW COOL TO RT					NQR STUDY OF COPPER IN LU0.9PR0.1BA2CU3O7	199301		TATA INSTITUTE OF FUNDAMENTAL RESEARCH, INDIA	PHYS.REV.B,47(1993)1123	A.K.RAJARAJAN,A.S.TAMHANE,G.MARKANDEYULU,K.I.GNANASEKAR,K.V.GOPALAKRISHNAN,L.C.GUPTA,R.PINTO,R.VIJAYARAGHAVAN	LU,PR,BA,CU,O	
4344	PHC2010043	OZ CHANGES BY ANNEALING TEMPERATURE,FOLLOWS LATTICE CONST. CHANGE	(Ba,K)BiO3	Ba0.65K0.35Bi1O2.99	Ba	0.65	K	0.35	Bi	1															O	Z	2.99		1992																												BKBO																			11.8		25.6				18.7																																																																																															0						OXYGEN CONTENT AND TC OF BA0.6K0.4BIO3-Z	199210		DEPARTMENT OF INDUSTRIAL CHEMISTRY, FACULTY OF SCIENCE AND TECHNOLOGY, SCIENCE UNIVERSITY OF TOKYO, CHIBA	PHYSICA C,201(1992)43	KAZUO FUEKI,YASUSHI IDEMOTO,YOSHIKI IWATA	BA,K,BI,O	
4345	PHC2010043		(Ba,K)BiO3	Ba0.59K0.41Bi1O2.96	Ba	0.59	K	0.41	Bi	1															O	Z	2.96		1992																												BKBO																			13.5		27.3				20.4																																																																																															0						OXYGEN CONTENT AND TC OF BA0.6K0.4BIO3-Z	199210		DEPARTMENT OF INDUSTRIAL CHEMISTRY, FACULTY OF SCIENCE AND TECHNOLOGY, SCIENCE UNIVERSITY OF TOKYO, CHIBA	PHYSICA C,201(1992)43	KAZUO FUEKI,YASUSHI IDEMOTO,YOSHIKI IWATA	BA,K,BI,O	
4346	PHC2010043		(Ba,K)BiO3	Ba0.52K0.48Bi1O2.93	Ba	0.52	K	0.48	Bi	1															O	Z	2.93		1992																												BKBO																			14.5		26.7				20.6																																																																																															0						OXYGEN CONTENT AND TC OF BA0.6K0.4BIO3-Z	199210		DEPARTMENT OF INDUSTRIAL CHEMISTRY, FACULTY OF SCIENCE AND TECHNOLOGY, SCIENCE UNIVERSITY OF TOKYO, CHIBA	PHYSICA C,201(1992)43	KAZUO FUEKI,YASUSHI IDEMOTO,YOSHIKI IWATA	BA,K,BI,O	
4347	PHC2010043		(Ba,K)BiO3	Ba0.48K0.52Bi1O2.9	Ba	0.48	K	0.52	Bi	1															O	Z	2.9		1992																												BKBO																			15.2		27				21.1																																																																																															0						OXYGEN CONTENT AND TC OF BA0.6K0.4BIO3-Z	199210		DEPARTMENT OF INDUSTRIAL CHEMISTRY, FACULTY OF SCIENCE AND TECHNOLOGY, SCIENCE UNIVERSITY OF TOKYO, CHIBA	PHYSICA C,201(1992)43	KAZUO FUEKI,YASUSHI IDEMOTO,YOSHIKI IWATA	BA,K,BI,O	
4348	PHC2010043		(Ba,K)BiO3	Ba0.45K0.55Bi1O2.83	Ba	0.45	K	0.55	Bi	1															O	Z	2.83		1992																												BKBO																			14.2		23.7				18.95																																																																																															0						OXYGEN CONTENT AND TC OF BA0.6K0.4BIO3-Z	199210		DEPARTMENT OF INDUSTRIAL CHEMISTRY, FACULTY OF SCIENCE AND TECHNOLOGY, SCIENCE UNIVERSITY OF TOKYO, CHIBA	PHYSICA C,201(1992)43	KAZUO FUEKI,YASUSHI IDEMOTO,YOSHIKI IWATA	BA,K,BI,O	
4349	PHC2030320		PrBa2Cu3O7	Pr1Ba2Cu3OZ	Pr	1	Ba	2	Cu	3															O	Z			1992								17.5																			3	Y123				3.867	3.903	11.742																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4350	PHC2030320		(Pr,Ca)Ba2Cu3O7	Pr0.95Ca0.05Ba2Cu3OZ	Pr	0.95	Ca	0.05	Ba	2	Cu	3													O	Z			1992								17.5																			3	Y123				3.864	3.901	11.728																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4351	PHC2030320		(Pr,Ca)Ba2Cu3O7	Pr0.9Ca0.1Ba2Cu3OZ	Pr	0.9	Ca	0.1	Ba	2	Cu	3													O	Z			1992								17																			3	Y123				3.867	3.9	11.719																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4352	PHC2030320		(Pr,Ca)Ba2Cu3O7	Pr0.85Ca0.15Ba2Cu3OZ	Pr	0.85	Ca	0.15	Ba	2	Cu	3													O	Z			1992								16.5																			3	Y123				3.865	3.902	11.717																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4353	PHC2030320		(Pr,Ca)Ba2Cu3O7	Pr0.8Ca0.2Ba2Cu3OZ	Pr	0.8	Ca	0.2	Ba	2	Cu	3													O	Z			1992								16																			3	Y123				3.865	3.897	11.701																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4354	PHC2030320	NEELT DETERMINED BY SLOPE CHANGE IN M-T CURVE	Pr(Ba,Ca)2Cu3O7	Pr1Ba1.9Ca0.1Cu3Oz	Pr	1	Ba	1.9	Ca	0.1	Cu	3													O	z			1992								17.5																			3	Y123				3.855	3.895	11.706																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4355	PHC2030320	4354	Pr(Ba,Ca)2Cu3O7	Pr1Ba1.8Ca0.2Cu3Oz	Pr	1	Ba	1.8	Ca	0.2	Cu	3													O	z			1992								16.5																			2	Y123				3.88		11.648																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4356	PHC2030320	4354	Pr(Ba,Ca)2Cu3O7	Pr1Ba1.7Ca0.3Cu3Oz	Pr	1	Ba	1.7	Ca	0.3	Cu	3													O	z			1992								14																			2	Y123				3.873		11.63																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4357	PHC2030320	4354	Pr(Ba,Ca)2Cu3O7	Pr1Ba1.6Ca0.4Cu3Oz	Pr	1	Ba	1.6	Ca	0.4	Cu	3													O	z			1992								12																			2	Y123				3.871		11.624																	10																																																																																																	1						EFFECTS OF SUBSTITUTION ON THE STRUCTURAL,ELECTRICAL AND MAGNETIC PROPERTIES OF PRBA2CU3O7-Y	199212			PHYSICA C,203(1992)320	C.H.LUO,H.D.YANG,H.L.TSAY,M.W.LIN,T.F.YOUNG	PR,BA,CU,O,CA	
4358	PHC2000215	HYDROSTATIC PRESSURE UPTO 1GPA	(Bi,Pb)2Sr2CaCu2O8	Bi1.9Pb0.1Sr2Ca1Cu2O8.2	Bi	1.9	Pb	0.1	Sr	2	Ca	1	Cu	2											O	8+Z	8.2	1	1992																											3	Bi2212				5.39	5.44	31														73.5					73.5			K/GPa	2																																																																																											1	MIXTURE-ANN(800C,3DAYS IN AIR)-ANN(820C,7DAYS INO2)					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF COMPOUNDS BI2-YPBYSR2CA1-XYXCU2O8+Z	199209			PHYSICA C,200(1992)215	A.STRUK,K.WESTERHOLT	BI,PB,SR,CA,Y,CU,O	
4359	PHC2000215	4358	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca1Cu2O8.2	Bi	2	Sr	2	Ca	1	Cu	2													O	8.2	8.2	1	1992																											3	Bi2212				5.4	5.45	31.1														85.2					85.2			K/GPa	1.8																																																																																											1	MIXTURE-ANN(800C,3DAYS IN AIR)-ANN(820C,7DAYS INO2)					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF COMPOUNDS BI2-YPBYSR2CA1-XYXCU2O8+Z	199209			PHYSICA C,200(1992)215	A.STRUK,K.WESTERHOLT	BI,PB,SR,CA,Y,CU,O	
4360	PHC2000215	4358	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8.2	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8.2	8.2	1	1992																											3	Bi2212				5.41	5.44	30.7														89					89			K/GPa	1																																																																																											1	MIXTURE-ANN(800C,3DAYS IN AIR)-ANN(820C,7DAYS INO2)					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF COMPOUNDS BI2-YPBYSR2CA1-XYXCU2O8+Z	199209			PHYSICA C,200(1992)215	A.STRUK,K.WESTERHOLT	BI,PB,SR,CA,Y,CU,O	
4361	PHC2000215	4358	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8.2	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8.2	8.2	1	1992																											3	Bi2212				5.4	5.45	31														87.8					87.8			K/GPa	0.9																																																																																											1	MIXTURE-ANN(800C,3DAYS IN AIR)-ANN(820C,7DAYS INO2)					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF COMPOUNDS BI2-YPBYSR2CA1-XYXCU2O8+Z	199209			PHYSICA C,200(1992)215	A.STRUK,K.WESTERHOLT	BI,PB,SR,CA,Y,CU,O	
4362	PHC2000012		RBaSrCu3O7	Dy1Ba1Sr1Cu3O6.94	Dy	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	1	1992																											3	Y123				3.816	3.838	11.542														83					83																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4363	PHC2000012		RBaSrCu3O7	Y1Ba1Sr1Cu3O6.94	Y	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	1	1992																											3	Y123				3.791	3.845	11.542														79					79																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4364	PHC2000012		RBaSrCu3O7	Ho1Ba1Sr1Cu3O6.94	Ho	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	1	1992																											3	Y123				3.789	3.851	11.546														79					79																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4365	PHC2000012	IMPURITY R2BACUO5(GREEN PHASE)	RBaSrCu3O7	Er1Ba1Sr1Cu3O6.94	Er	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	1	1992																											3	Y123				3.791	3.847	11.56														78					78																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4366	PHC2000012	4365	RBaSrCu3O7	Tm1Ba1Sr1Cu3O6.94	Tm	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	1	1992																											3	Y123				3.821	3.836	11.55														70					70																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4367	PHC2000012	4365	RBaSrCu3O7	Lu1Ba1Sr1Cu3O6.94	Lu	1	Ba	1	Sr	1	Cu	3													O	Z	6.94	4	1992																											3	Y123						11.61														54					54																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4368	PHC2000012		RBaSrCu3O7	La1Ba1Sr1Cu3O6.94	La	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.877		11.728														57					57																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4369	PHC2000012	SEMICONDUCTOR	RBaSrCu3O7	Pr1Ba1Sr1Cu3O6.94	Pr	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.859		11.551																																																																																																																		1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4370	PHC2000012		RBaSrCu3O7	Nd1Ba1Sr1Cu3O6.94	Nd	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.87		11.622														74					74																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4371	PHC2000012		RBaSrCu3O7	Sm1Ba1Sr1Cu3O6.94	Sm	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.851		11.591														80					80																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4372	PHC2000012		RBaSrCu3O7	Eu1Ba1Sr1Cu3O6.94	Eu	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.844		11.579														80					80																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4373	PHC2000012		RBaSrCu3O7	Gd1Ba1Sr1Cu3O6.94	Gd	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.94	1	1992																											2	Y123				3.845		11.554														86					86																																																																																															1						CRYSTAL STRUCTURE AND SUPERCONDUCTIVITY IN REBASRCU3OX	199209			PHYSICA C,200(1992)12	B.HELLEBRAND,D.BAUERLE,X.Z.WANG	R,BA,CU,SR,O	
4374	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9Pr0.1Sr2Ca2Cu3OZ	Bi	1.9	Pr	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			81		113				97																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4375	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9In0.1Sr2Ca2Cu3OZ	Bi	1.9	In	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			80		111				95.5																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4376	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9Sb0.1Sr2Ca2Cu3OZ	Bi	1.9	Sb	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			83		115				99																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4377	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9Pb0.1Sr2Ca2Cu3OZ	Bi	1.9	Pb	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			98		115				106.5																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4378	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9Sn0.1Sr2Ca2Cu3OZ	Bi	1.9	Sn	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			103		116				109.5																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4379	PHC1990333		(Bi,M)2Sr2Ca2Cu3O10	Bi1.9Ge0.1Sr2Ca2Cu3OZ	Bi	1.9	Ge	0.1	Sr	2	Ca	2	Cu	3											O	Z			1992																												Bi2223																			88.5		112				100.25																																																																																															1						STUDY OF HIGH-TC SUPERCONDUCTOR (BIM)-SR-CA-CU-O (M=PB+GE,PB+SN,PB,ETC.)	199209			PHYSICA C,199(1992)333	CHANGJIANG LI,GUANLIANG QIU,HUA LI,MINHUA FU,MOUYUAN CHEN,QI YAO,QINGYUN MENG,XIUHAI LI	PB,GE,SN,BI,SR,CA,CU,O	
4380	PHC2010053	BACUO2 IMPURITY,CU-O APICAL=2.66A,TC DEPENDS ON REACTION CODITION	Tl2Ba2Ca3Cu4O12	Tl2Ba2Ca3Cu4O12	Tl	2	Ba	2	Ca	3	Cu	4													O	12		1	1992																											2	Tl2234	I4/MMM			3.849		42.049														109					109																																																																																														TL2O3,BAO2,CAO,CUO	1	TL:BA:CA:CU=1.5:2.0:3.5:4,MIXTURE IN AU TUBE-(860C,10H IN AIR)-Q TO RT					THE STRUCTURE OF TL2BA2CA3CU4O12	199210		DEPARTMENT OF CHMISTRY, THE UNIVERSITY OF SOUTHAMPTON, UK	PHYSICA C,201(1992)53	D.M.OGBORNE,M.T.WELLER	TL,BA,CA,CU,O	
4381	PHC1980007		(C,Cu)Sr2(Y,Sr)Cu2O7	C0.4Cu0.6Sr2Y0.86Sr0.14Cu2O7	C	0.4	Cu	0.6	Sr	2	Y	0.86	Sr	0.14	Cu	2									O	7			1992																											3	Cu1212	PMMM			3.828	3.851	11.185																																																																																																																		0						THE CRYSTAL STRUCTURE OF (C0.4CU0.6)SR2(Y0.86SR0.14)CU2O7	199207			PHYSICA C,198(1992)7	H.YAMANE,K.HIRAGA,N.OHNISHI,S.FUNAHASHI,T.HIRAI,T.KAJITANI,Y.MIYAZAKI,Y.MORII	C,CU,SR,Y,O	
4382	PHC1960259	TL CONTENT AND TC DEPENDS ON SINTERING CONDITION,TL1234 OR TL2234		Tl1.4Ba2Ca3Cu4O11.4	Tl	1.4	Ba	2	Ca	3	Cu	4													O	11.4			1992																																															118						118																																																																																															1	CAL(600C)-UNIAXIALLY COMPACTED AT 7000KBAR-SIN(880-915C)					TLXBA2CA3CU4OY SUPERCONDUCTORS FROM COPRECIPITATED OXALATE PRECURSORS	199206			PHYSICA C,196(1992)259	GERHARD GRITZNER,KLAUS BERNHARD	TL,BA,CU,O,CA	
4383	PHC1980053	STRUCTURE SIMULAR TO Y123,AVERAGE CU VALENCE=2.13		Y2Sr5Cu6C0.9O16.2	Y	2	Sr	5	Cu	6	C	0.9													O	16.2	16.2		1992									5.6																		2					3.848		11.185																	15																																																																																				83												Y2O3,SRCO3,CUO	1	MIXTURE-HEAT(1273K,20H IN AIR OR O2+10%CO2 UNDER 0.01MPA)-Q TO RT-REPEAT					PREPARATION OF A NEW COMPOUND,Y2.0SR5.0CU6.0C0.9O16.2	199207			PHYSICA C,198(1992)53	HISANORI YAMANE,TOSHIO HIRAI,YUZURU MIYAZAKI	Y,SR,CU,C,O	
4384	PHC1980027	NOT S/C,SEMICON-LIKE	Sr2(Nd,Ce)2MCu2O9	Sr2Nd1.35Ce0.65Ga1Cu2O9	Sr	2	Nd	1.35	Ce	0.65	Ga	1	Cu	2											O	9		1	1992																											3					5.456	5.529	28.34																																																																																																																	SRCO3,ND2O3,CE2(CO3)3.5H20	0	SLOWLY HEATED TO 1000C IN O2-HOLD SEVERAL DAYS, ANN(  )					SR2(ND,CE)2MCU2O9,M=AL,CO,GA	199207			PHYSICA C,198(1992)27	B.HESSEN,H.W.ZANDBERGEN,J.J.KRAJEWSKI,R.B.VAN DOVER,R.J.CAVA,S.-W.CHEONG,W.F.PECK JR.	AL,CO,GA,SR,ND,CE,CU,O	
4385	PHC1980027	NOT S/C	Sr2(Nd,Ce)2MCu2O9	Sr2Nd1.2Ce0.8Co1Cu2O9	Sr	2	Nd	1.2	Ce	0.8	Co	1	Cu	2											O	9		2	1992																											2					3.869		28.33																																																																																																																	SRCO3,ND2O3,CE2(CO3)3.5H20	0	SLOWLY HEATED TO 1000C IN O2-HOLD SEVERAL DAYS, ANN(  )					SR2(ND,CE)2MCU2O9,M=AL,CO,GA	199207			PHYSICA C,198(1992)27	B.HESSEN,H.W.ZANDBERGEN,J.J.KRAJEWSKI,R.B.VAN DOVER,R.J.CAVA,S.-W.CHEONG,W.F.PECK JR.	AL,CO,GA,SR,ND,CE,CU,O	
4386	PHC1980007	40% OF CUO CHAIN ARE REPLACED BY CO3 GROUPS,STRUCTURE RESEMBLE TO CU1212	(C,Cu)Sr2(Y,Sr)Cu2O7	C0.4Sr2.14Y0.86Cu2.6O7	C	0.4	Sr	2.14	Y	0.86	Cu	2.6													O	7			1992																												C1212	PMMM			3.828	3.851	11.185																	15																																																																																																Y2O3,SRCO3,CUO	0	MIXTURE(Y:SR:CU=0.84:2.16:2.60)-HEAT(1270K,20H IN(O2+CO2) 0.01MPA)-Q TO RT-PELLET					THE CRYSTAL STRUCTURE OF (C0.4CU0.6)SR2(Y0.86SR0.14)CU2O7	199207			PHYSICA C,198(1992)7	H.YAMANE,K.HIRAGA,N.OHNISHI,S.FUNAHASHI,T.HIRAI,T.KAJITANI,Y.MIYAZAKI,Y.MORII	C,CU,SR,Y,O	
4387	PHC1980019		RBa8Cu4OZ	Dy1Ba8Cu4OZ	Dy	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.152		8.076																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4388	PHC1980019		RBa8Cu4OZ	Gd1Ba8Cu4OZ	Gd	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.162		8.08																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4389	PHC1980019		RBa8Cu4OZ	Eu1Ba8Cu4OZ	Eu	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.172		8.088																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4390	PHC1980019		RBa8Cu4OZ	Sm1Ba8Cu4OZ	Sm	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.177		8.104																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4391	PHC1980019		RBa8Cu4OZ	Nd1Ba8Cu4OZ	Nd	1	Ba	8	Cu	4															O	Z		2	1992																											1	Y184				8.095																																																																																																																				0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4392	PHC1980019		RBa8Cu4OZ	Sc1Ba8Cu4OZ	Sc	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.063		7.991																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4393	PHC1980019		RBa8Cu4OZ	Lu1Ba8Cu4OZ	Lu	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.086		8.058																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4394	PHC1980019		RBa8Cu4OZ	Yb1Ba8Cu4OZ	Yb	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.101		8.067																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4395	PHC1980019		RBa8Cu4OZ	Tm1Ba8Cu4OZ	Tm	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.111		8.072																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4396	PHC1980019		RBa8Cu4OZ	Er1Ba8Cu4OZ	Er	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.126		8.058																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4397	PHC1980019		RBa8Cu4OZ	Ho1Ba8Cu4OZ	Ho	1	Ba	8	Cu	4															O	Z			1992																											2	Y184				8.146		8.065																																																																																																																		0						"THE LN-BA-CU ""184"" OXIDE PHASE"	199207			PHYSICA C,198(1992)19	E,H.A.EICK,HODOROWICZ,S.A.HODOROWICZ	BA,CU,SM,LU,SC,R	
4398	JPS0591921	ALMOST SINGLE PHASE,SEMICON-LIKE RESISTIVITY,NEELT BY MUON-SR	Bi2(Sr,La)2CuO6	Bi2Sr1La1Cu1O6+Z	Bi	2	Sr	1	La	1	Cu	1													O	6+Z		1	1990								10																			2	Bi2201				3.858		24.02																	4.2																																																																																																	1						OBSERVATION OF AN ANTIFERROMAGNETIC PHASE IN THE BI2SR2CUO6+YSYSTEM BY THE U+SR TECHNIQUE	199006			J.PHYS.SOC.JAPAN,59(1990)1921	AKIRA YAMAZAKI,HIDEAKI MIYATAKE,JUN AKIMITSU,NOBUHIKO NISHIDA,SATOSHI OKUMA	BI,SR,CU,O	
4399	JPS0591921	4398	Bi2(Sr,La)2CuO6	Bi2Sr0.9La1.1Cu1O6+Z	Bi	2	Sr	0.9	La	1.1	Cu	1													O	6+Z		1	1990								33																			2	Bi2201				3.863		23.9																	4.2																																																																																																	1						OBSERVATION OF AN ANTIFERROMAGNETIC PHASE IN THE BI2SR2CUO6+YSYSTEM BY THE U+SR TECHNIQUE	199006			J.PHYS.SOC.JAPAN,59(1990)1921	AKIRA YAMAZAKI,HIDEAKI MIYATAKE,JUN AKIMITSU,NOBUHIKO NISHIDA,SATOSHI OKUMA	BI,SR,CU,O	
4400	JPS0591921	4398	Bi2(Sr,La)2CuO6	Bi2Sr0.8La1.2Cu1O6+Z	Bi	2	Sr	0.8	La	1.2	Cu	1													O	6+Z		1	1990								140																			2	Bi2201				3.868		23.84																	4.2																																																																																																	1						OBSERVATION OF AN ANTIFERROMAGNETIC PHASE IN THE BI2SR2CUO6+YSYSTEM BY THE U+SR TECHNIQUE	199006			J.PHYS.SOC.JAPAN,59(1990)1921	AKIRA YAMAZAKI,HIDEAKI MIYATAKE,JUN AKIMITSU,NOBUHIKO NISHIDA,SATOSHI OKUMA	BI,SR,CU,O	
4401	JPD0260281		RBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1993																											3	Y123																					90				90																																																																			3.7																			0.0000000011			0.00000000319	0.5					0						Normal state transport properties in superconducting oxides RBa2Cu3O7-z (R=Y, Gd, Sm, Nd, and Dy)			Department of Physics and Meteorology, Indian Institute of Technology, Kharagpur-721 302, India	J.Phys.D, 26(1993)281	P C Jana,R C Bhuniya		
4402	JPD0260281		RBa2Cu3O7	Gd1Ba2Cu3O7-Z	Gd	1	Ba	2	Cu	3															O	7-Z			1993																											3	Y123																			92						92																																																																			6																			0.000000000543			0.00000000185	0.5					0						Normal state transport properties in superconducting oxides RBa2Cu3O7-z (R=Y, Gd, Sm, Nd, and Dy)			Department of Physics and Meteorology, Indian Institute of Technology, Kharagpur-721 302, India	J.Phys.D, 26(1993)281	P C Jana,R C Bhuniya		
4403	JPD0260281		RBa2Cu3O7	Sm1Ba2Cu3O7-Z	Sm	1	Ba	2	Cu	3															O	7-Z			1993																											3	Y123																			86						86																																																																			0.1																			0.0000000008			0.00000000231	0.5					0						Normal state transport properties in superconducting oxides RBa2Cu3O7-z (R=Y, Gd, Sm, Nd, and Dy)			Department of Physics and Meteorology, Indian Institute of Technology, Kharagpur-721 302, India	J.Phys.D, 26(1993)281	P C Jana,R C Bhuniya		
4404	JPD0260281		RBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			1993																											3	Y123																			92						92																																																																			5.4																			0.0000000005			0.00000000141	0.5					0						Normal state transport properties in superconducting oxides RBa2Cu3O7-z (R=Y, Gd, Sm, Nd, and Dy)			Department of Physics and Meteorology, Indian Institute of Technology, Kharagpur-721 302, India	J.Phys.D, 26(1993)281	P C Jana,R C Bhuniya		
4405	JPD0260281		RBa2Cu3O7	Dy1Ba2Cu3O7-Z	Dy	1	Ba	2	Cu	3															O	7-Z			1993																											3	Y123																			92						92																																																																			3																			0.000000000901			0.00000000283	0.5					0						Normal state transport properties in superconducting oxides RBa2Cu3O7-z (R=Y, Gd, Sm, Nd, and Dy)			Department of Physics and Meteorology, Indian Institute of Technology, Kharagpur-721 302, India	J.Phys.D, 26(1993)281	P C Jana,R C Bhuniya		
4406	PR0472854	X=0.092 BY ICP,PENET FOR H//C-AXIS. Hc(0)=1430 Oe 	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1993																												T																					26.2			0.9	26.2																																										Using Hao et al model from magnetization. 		4400																																																			0						MAGNETIC PENETRATION DEPTH OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS	199302			PHYS.REV.B,47(1993)2854	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA	LA,SR,CU,O	
4407	PR0472854	X=0.118 BY ICP,PENET FOR H//C-AXIS. Hc(0)=1430 Oe 	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		3	1993																												T																					32.4			3.7	32.4																																										Using Hao & Clem analysis from magnetization		3730																																																			0						MAGNETIC PENETRATION DEPTH OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS	199302			PHYS.REV.B,47(1993)2854	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA	LA,SR,CU,O	
4408	PR0472854	X=0.154 BY ICP,PENET FOR H//C-AXIS. Hc(0)=2510 Oe 	(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		3	1993																												T																					35.1			1.8	35.1																																										Using Hao & Clem analysis from magnetization		2545																																																			0						MAGNETIC PENETRATION DEPTH OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS	199302			PHYS.REV.B,47(1993)2854	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA	LA,SR,CU,O	
4409	PR0472854	X=0.18 BY ICP,PENET FOR H//C-AXIS. Hc(0)=2170 Oe 	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	1993																												T																					29.8				29.8																																										Using Hao & Clem analysis from magnetization		2830																																																			0						MAGNETIC PENETRATION DEPTH OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS	199302			PHYS.REV.B,47(1993)2854	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA	LA,SR,CU,O	
4410	SSC0850925	TWINNED CRYSTAL,IMPURITY PHASE Y2BACUO5 INCLUDED,FIELD INDUCED TC APPEARS AT 74K	YBa2Cu3O7	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	6.45	6.45	3	1993																												Y123						11.76														47					47																																2.2	1.7																																																														0	GRAIN GROWTH TECHNIQUE					FIELD ENHANCEMENT OF THE DIAMAGNETIC ONSET TEMPERATURE IN A YBA2CU3O6.45 SINGLE CRYSTAL	199303			SOLID STATE COMMUN.,85(1993)925	C.MARIN,J.ROSSAT-MIGNOD2,J.Y.HENRY,V.V.MOSHCHALKOV	Y,BA,CU,O	
4411	PR04712190	NOT S/C	La2CaCu2O6	La2Ca1Cu2O6	La	2	Ca	1	Cu	2															O	6		1	1993							-27.5	13.5																			2	2126				3.827		19.42																																																																																																																		1	MIX-PRESS-PELLET-HEAT(950C,1DAY)-REGROUND-CAL(1050C-1100C,48H)-FC TO RT					MAGNETIC PROPERTIES,MOSSBAUER MEASUREMENTS,AND SPECIFIC-HEAT STUDIES OF LA2MCU2O6 (M=CA OR SR) COMPOUNDS	199305			PHYS.REV.B,47(1993)12190	D.HECHEL,E.R.YACOBY,G.HILSCHER,G.SCHAUDY,I.FELNER,T.HOLUBAR		
4412	PR04712190	NOT S/C	La2SrCu2O6	La2Sr1Cu2O6	La	2	Sr	1	Cu	2															O	6		1	1993							-57	18.5																			2	2126				3.866		19.92																																																																																																																		1	MIX-PRESS-PELLET-HEAT(950C,1DAY)-REGROUND-CAL(1050C-1100C,48H)-FC TO RT					MAGNETIC PROPERTIES,MOSSBAUER MEASUREMENTS,AND SPECIFIC-HEAT STUDIES OF LA2MCU2O6 (M=CA OR SR) COMPOUNDS	199305			PHYS.REV.B,47(1993)12190	D.HECHEL,E.R.YACOBY,G.HILSCHER,G.SCHAUDY,I.FELNER,T.HOLUBAR		
4413	PR04712190	NOT S/C	(La,Sr)2CaCu2O6	La1.6Sr0.4Ca1Cu2O6	La	1.6	Sr	0.4	Ca	1	Cu	2													O	6		1	1993							-3.2	10																			2	2126				3.843		19.68																																																																																																																		1	MIX-PRESS-PELLET-HEAT(950C,1DAY)-REGROUND-CAL(1050C-1100C,48H)-FC TO RT					MAGNETIC PROPERTIES,MOSSBAUER MEASUREMENTS,AND SPECIFIC-HEAT STUDIES OF LA2MCU2O6 (M=CA OR SR) COMPOUNDS	199305			PHYS.REV.B,47(1993)12190	D.HECHEL,E.R.YACOBY,G.HILSCHER,G.SCHAUDY,I.FELNER,T.HOLUBAR		
4414	PR0472849		SrNbO3	Sr0.75Nb1O3	Sr	0.75	Nb	1																	O	3	3	1	1993																											1					3.993																																																																																													1.3										1.8													1	(1050C,80-160H)					SYNTHESIS AND TRANSPORT PROPERTIES OF SRXNBO3 (0.75<-X<-0.90)	199302			PHYS.REV.B,47(1993)2849	AYUMI NOZAKI,H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,KIYOTAKA MATSUURA	SR,NB,O	
4415	PR0472849		SrNbO3	Sr0.9Nb1O3	Sr	0.9	Nb	1																	O	3	3	1	1993				0		0.24	1.2																				1					4.005																																																																																																							6													1	(1050C,80-160H)					SYNTHESIS AND TRANSPORT PROPERTIES OF SRXNBO3 (0.75<-X<-0.90)	199302			PHYS.REV.B,47(1993)2849	AYUMI NOZAKI,H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,KIYOTAKA MATSUURA	SR,NB,O	
4416	PR0480657	IN-PLANE THERMOPOWER	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1993																												T'																				24		24			24																																																																			-0.94																												0	DIRECTIONAL SOLIDIFICATION TECHNIQUE,SEE PHC1770079					ANISOTROPIC NORMAL-STATE MAGNETOTHERMOPOWER OF SUPERCONDUCTINGND1.85CE0.15CUO4 CRYSTALS	199307			PHYS.REV.B,48(1993)657	J.L.PENG,R.L.GREENE,S.J.HAGEN,WU.JIANG,X.Q.XU,Z.Y.LI		
4417	PHC2050039		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18O6.95	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	6.95	6.95	1	1993																											2	Y123				3.885		11.718												K		75.6					75.6																																																																																															1						STRUCTURE AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3OY PREPAREDBY VACUUM CALCINATION AT 673 K (X=0.02 AND 0.06)	199301			PHYSICA C,205(1993)39	KAZUYOSHI YOSHIMURA,KOJI KOSUGE,NOBUYA MACHIDA,NORIHIKO NAKANISHI,TOMOHIRO FURUKAWA,TOSHIHIKO SHIGEMATSU	Y,BA,CU,FE,O	
4418	PHC2050039	TC AND LATTICE PARAMETERS ARE GIVEN AS A FUNCTION OF OXYGEN CONTENT	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.82Fe0.18O6.895	Y	1	Ba	2	Cu	2.82	Fe	0.18													O	Z	6.895	1	1993																											2	Y123																		K		87.7					87.7	TC4418																																																																																														1						STRUCTURE AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3OY PREPAREDBY VACUUM CALCINATION AT 673 K (X=0.02 AND 0.06)	199301			PHYSICA C,205(1993)39	KAZUYOSHI YOSHIMURA,KOJI KOSUGE,NOBUYA MACHIDA,NORIHIKO NAKANISHI,TOMOHIRO FURUKAWA,TOSHIHIKO SHIGEMATSU	Y,BA,CU,FE,O	
4419	PHC2050039		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O6.89	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	6.89	6.89		1993																											3	Y123				3.849	3.88	11.681												K		87.5					87.5																																																																																															1						STRUCTURE AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3OY PREPAREDBY VACUUM CALCINATION AT 673 K (X=0.02 AND 0.06)	199301			PHYSICA C,205(1993)39	KAZUYOSHI YOSHIMURA,KOJI KOSUGE,NOBUYA MACHIDA,NORIHIKO NAKANISHI,TOMOHIRO FURUKAWA,TOSHIHIKO SHIGEMATSU	Y,BA,CU,FE,O	
4420	PHC2050039	TC AND LATTICE PARAMETERS ARE GIVEN AS A FUNCTION OF OXYGEN CONTENT	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Fe0.06O6.954	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	Z	6.954		1993																												Y123																		K		76.6					76.6	TC4420																																																																																														1						STRUCTURE AND SUPERCONDUCTIVITY OF YBA2(CU1-XFEX)3OY PREPAREDBY VACUUM CALCINATION AT 673 K (X=0.02 AND 0.06)	199301			PHYSICA C,205(1993)39	KAZUYOSHI YOSHIMURA,KOJI KOSUGE,NOBUYA MACHIDA,NORIHIKO NAKANISHI,TOMOHIRO FURUKAWA,TOSHIHIKO SHIGEMATSU	Y,BA,CU,FE,O	
4421	PR04715265		YBA2(Cu,Zn)3O7	Y1Ba2Cu3ZnO6.91	Y	1	Ba	2	Cu	3	Zn														O	7-Z	6.91	1	1993																												Y123																																																																																																																			5	RH4421			BACO3,Y2O3,CUO,ZNO	1	PELLET-CAL(905C,160H IN O2)-COOL(0.5C/MIN)-(930C,12H IN O2)-COOL(0.5C/MIN)-SIN(950C,12H IN O2)-ANN(500C,12H IN O2)					HALL EFFECT IN BULK YBA2(CU1-XZNX)3O7-Z	199306			PHYS.REV.B,47(1993)15265	A.LANCKBEEN,G.ILONCA,M.MEHBOD,R.DELTOUR		
4422	PR04715265		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.91	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.91	1	1993																												Y123																																																																																																																			5	RH4422			BACO3,Y2O3,CUO,ZNO	1	PELLET-CAL(905C,160H IN O2)-COOL(0.5C/MIN)-(930C,12H IN O2)-COOL(0.5C/MIN)-SIN(950C,12H IN O2)-ANN(500C,12H IN O2)					HALL EFFECT IN BULK YBA2(CU1-XZNX)3O7-Z	199306			PHYS.REV.B,47(1993)15265	A.LANCKBEEN,G.ILONCA,M.MEHBOD,R.DELTOUR		
4423	PR04715265		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.883Zn0.117O6.9	Y	1	Ba	2	Cu	2.883	Zn	0.117													O	7-Z	6.9	1	1993																												Y123																																																																																																																			5	RH4423			BACO3,Y2O3,CUO,ZNO	1	PELLET-CAL(905C,160H IN O2)-COOL(0.5C/MIN)-(930C,12H IN O2)-COOL(0.5C/MIN)-SIN(950C,12H IN O2)-ANN(500C,12H IN O2)					HALL EFFECT IN BULK YBA2(CU1-XZNX)3O7-Z	199306			PHYS.REV.B,47(1993)15265	A.LANCKBEEN,G.ILONCA,M.MEHBOD,R.DELTOUR		
4424	PR04715265		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.841Zn0.159O6.89	Y	1	Ba	2	Cu	2.841	Zn	0.159													O	7-Z	6.89	1	1993																												Y123																																																																																																																			5	RH4424			BACO3,Y2O3,CUO,ZNO	1	PELLET-CAL(905C,160H IN O2)-COOL(0.5C/MIN)-(930C,12H IN O2)-COOL(0.5C/MIN)-SIN(950C,12H IN O2)-ANN(500C,12H IN O2)					HALL EFFECT IN BULK YBA2(CU1-XZNX)3O7-Z	199306			PHYS.REV.B,47(1993)15265	A.LANCKBEEN,G.ILONCA,M.MEHBOD,R.DELTOUR		
4425	PR04715265		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.826Zn0.174O6.89	Y	1	Ba	2	Cu	2.826	Zn	0.174													O	7-Z	6.89	1	1993																												Y123																																																																																																																			5	RH4425			BACO3,Y2O3,CUO,ZNO	1	PELLET-CAL(905C,160H IN O2)-COOL(0.5C/MIN)-(930C,12H IN O2)-COOL(0.5C/MIN)-SIN(950C,12H IN O2)-ANN(500C,12H IN O2)					HALL EFFECT IN BULK YBA2(CU1-XZNX)3O7-Z	199306			PHYS.REV.B,47(1993)15265	A.LANCKBEEN,G.ILONCA,M.MEHBOD,R.DELTOUR		
4426	PR04712178	NOT S/C,NEELT BY SPECIFIC HEAT	TlBa2GdCu2O7	Tl1Ba2Gd1Cu2O7-Z	Tl	1	Ba	2	Gd	1	Cu	2													O	7-Z		1	1993							2.35	2.3																			2	Tl1212	P4/MMM			3.888		12.48																	2																																																																																																TL2O3,BACO3,GD2O3,CUO	1	SOLID STATE REACTION METHOD,ANN(870C,10H IN O2)-SLOW COOL TO RT					MAGNETIC AND CALORIMETRIC STUDIES OF GD ORDERING IN TLBA2GDCU2O7-Z	199305			PHYS.REV.B,47(1993)12178	B.S.CHIOU,C.C.LAI,H.C.KU,J.C.HO,Y.Y.CHEN		
4427	SSC0870289		PrBa2Cu3O7	Pr1Ba2Cu3O7-Z	Pr	1	Ba	2	Cu	3															O	7-Z		3	1993	EMU/MOLE		EMU.K/MOLE	1.47			-8.2																					Y123	P4/MMM																																																																																																																							0	FLUX METHOD,FLUX=BAO-CUO					STRUCTURAL AND CRYSTAL FIELD STUDIES ON A SINGLE CRYSTAL OF PRBA2CU3O7-Z				SOLID STATE COMMUN.,87(1993)289	G.RANGARAJAN,M.SESHASAYEE,S.UMA,T.SARKAR	PR,BA,CU,O	
4428	SSC0870425			Bi2.19Sr2Ca0.81Cu1.93OZ	Bi	2.19	Sr	2	Ca	0.81	Cu	1.93													O	Z			1993																												Bi2212																				89					89																																																																																															0						THE EFFECT YTTRIUM ON THE CA AND SR PLANES OF Y-DOPED BI2SR2CA1CU2O8				SOLID STATE COMMUN.,87(1993)425	G.MARGARITONDO,H.BERGER,P.ALMERAS	BI,SR,CA,CU,O,Y	
4429	SSC0870425			Bi2.01Sr1.93Ca0.79Y0.24Cu1.94OZ	Bi	2.01	Sr	1.93	Ca	0.79	Y	0.24	Cu	1.94											O	Z			1993																												Bi2212																				85					85																																																																																															0						THE EFFECT YTTRIUM ON THE CA AND SR PLANES OF Y-DOPED BI2SR2CA1CU2O8				SOLID STATE COMMUN.,87(1993)425	G.MARGARITONDO,H.BERGER,P.ALMERAS	BI,SR,CA,CU,O,Y	
4430	SSC0870425			Bi2.02Sr1.81Ca0.74Y0.37Cu1.93OZ	Bi	2.02	Sr	1.81	Ca	0.74	Y	0.37	Cu	1.93											O	Z			1993																												Bi2212																				80					80																																																																																															0						THE EFFECT YTTRIUM ON THE CA AND SR PLANES OF Y-DOPED BI2SR2CA1CU2O8				SOLID STATE COMMUN.,87(1993)425	G.MARGARITONDO,H.BERGER,P.ALMERAS	BI,SR,CA,CU,O,Y	
4431	SSC0870551	STRUCTURE LIKE 1223 PHASE	(Tl,Pb)Sr4Cu2(SO4)OZ	Tl0.5Pb0.5Sr4Cu2S1OZ	Tl	0.5	Pb	0.5	Sr	4	Cu	2	S	1											O	Z			1993																											2		P4/MMM			3.852		16.596																																																																																																																	TL2O3,PBO2,SR2CUO3,SRO2,SRSO4,CUO	0	MIXTURE-HEAT(1190K,1H IN AG TUBE)-Q TO RT					OXYANION DERIVATIVES OF CUPRATE SUPERCONDUCTORS:SUPERCONDUCTING THALLIUM CUPRATE OXYSUFATE,TL0.5PB0.5SR4CU2(SO4)OY				SOLID STATE COMMUN.,87(1993)551	C.N.R.RAO,G.N.SUBBANNA,S.AYYAPPAN,V.MANIVANNAN	TL,PB,SR,CU,S,O	
4432	PR04711384	HC2 ETC CALCULATED BY HAO-CLEM MODEL	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1993																												T																				28	26.2				28																						33									1.6								32					4400																																																			0						REVERSIBLE MAGNETIC PROPERTIES OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS WITH 0.05<-X<-0.10	199305			PHYS.REV.B,47(1993)11384	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA		
4433	PR04711384	4432	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		3	1993																												T																				32	32.4				32																						23									1								38					3730																																																			0						REVERSIBLE MAGNETIC PROPERTIES OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS WITH 0.05<-X<-0.10	199305			PHYS.REV.B,47(1993)11384	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA		
4434	PR04711384	4432	(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		3	1993																												T																				34	35.1				34																						34									1.35								32					2545																																																			0						REVERSIBLE MAGNETIC PROPERTIES OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS WITH 0.05<-X<-0.10	199305			PHYS.REV.B,47(1993)11384	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA		
4435	PR04711384	4432	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	1993																												T																				29.8	29.8				29.8																						33									1.5								33					2830																																																			0						REVERSIBLE MAGNETIC PROPERTIES OF (LA1-XSRX)2CUO4 SINGLE CRYSTALS WITH 0.05<-X<-0.10	199305			PHYS.REV.B,47(1993)11384	K.KISHIO,M.SUENAGA,QIANG LI,T.KIMURA		
4436	PHC2050032	TWINNED SAMPLE,DTC/DP CALCULATED FROM THERMAL EXPANSION COEFFICIENT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1993																											3	Y123																				87.3				1.3	87.3			K/GPa	3.2																																																																																											5	SELF-FLUX METHOD IN AL2O3 CRUCIBLE					ANISOTROPIC STRESS DEPENDENCE OF TC IN YBA2CU3O7-Z SINGLE CRYSTALS DEDUCED FROM THERMAL EXPANSION,MEASURED WITH A CAPACITIVEQUARTZ-DILATOMETER	199301			PHYSICA C,205(1993)32	K.ANDRES,M.KUND	Y,BA,CU,O	
4437	PHC2050032	UNTWINNED SAMPLE,DTC/DP CALCULATED FROM THERMAL EXPANSION COEFFICIENT	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1993																											3	Y123																				89.4				0.8	89.4			K/GPa	0.31																																																																																											5	SELF-FLUX METHOD IN AL2O3 CRUCIBLE					ANISOTROPIC STRESS DEPENDENCE OF TC IN YBA2CU3O7-Z SINGLE CRYSTALS DEDUCED FROM THERMAL EXPANSION,MEASURED WITH A CAPACITIVEQUARTZ-DILATOMETER	199301			PHYSICA C,205(1993)32	K.ANDRES,M.KUND	Y,BA,CU,O	
4438	PR0473347		(Bi,Pb)2Sr2CuO6	Bi1.7Pb0.3Sr2Cu1OZ	Bi	1.7	Pb	0.3	Sr	2	Cu	1													O	Z		1	1993																												Bi2201																																																																																																																				RH4438				0	SIN(880C-850C)-PELLET-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4439	PR0473347		Bi2Sr2CuO6	Bi2.1Sr1.9Cu1OZ	Bi	2.1	Sr	1.9	Cu	1															O	Z		1	1993																												Bi2201																																																																																																																								0	SIN(880-910C)-REPEAT-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4440	PR0473347		Bi2(Sr,La)2CuO6	Bi2.1Sr1.7La0.2Cu1OZ	Bi	2.1	Sr	1.7	La	0.2	Cu	1													O	Z		1	1993																												Bi2201																																																																																																																								0	SIN(880-910C)-REPEAT-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4441	PR0473347		Bi2(Sr,La)2CuO6	Bi2.1Sr1.5La0.4Cu1OZ	Bi	2.1	Sr	1.5	La	0.4	Cu	1													O	Z		1	1993																																																																																																																																																				0	SIN(880-910C)-REPEAT-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4442	PR0473347		Bi2(Sr,La)2CuO6	Bi2.1Sr1.3La0.6Cu1OZ	Bi	2.1	Sr	1.3	La	0.6	Cu	1													O	Z		1	1993																												Bi2201																																																																																																																								0	SIN(880-910C)-REPEAT-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4443	PR0473347		Bi2(Sr,La)2CuO6	Bi2.1Sr0.9La1Cu1OZ	Bi	2.1	Sr	0.9	La	1	Cu	1													O	Z		1	1993																																																																																																																																																				0	SIN(880-910C)-REPEAT-ANN(400C,12H)					DOPING DEPENDENCE OF NORMAL-STATE TRANSPORT PROPERTIES IN LA-AND PB-DOPED BI2SR2CUOY	199302			PHYS.REV.B,47(1993)3347	C.Y.WANG,D.J.HUANG,L.Z.CAO,N.L.WANG,Y.CHONG,Z.J.CHEN,Z.Q.MAO	BI,SR,CU,O,LA,PB	
4444	PR0487636	orthorhombically distorted perovskite,Debye temperature=500K +-50K	(La,Sr)TiO3	La0.9Sr0.1Ti1O3	La	0.9	Sr	0.1	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	11.4		500	specific heat																																			7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4445	PR0487636	4444	(La,Sr)TiO3	La0.7Sr0.3Ti1O3	La	0.7	Sr	0.3	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	7.82		500	specific heat																																			7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4446	PR0487636	4444	(La,Sr)TiO3	La0.5Sr0.5Ti1O3	La	0.5	Sr	0.5	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	5.44		500	specific heat																																			7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4447	PR0487636	4444	(La,Sr)TiO3	La0.3Sr0.7Ti1O3	La	0.3	Sr	0.7	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	4.36		500	specific heat																																			7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4448	PR0487636	4444	(La,Sr)TiO3	La0.1Sr0.9Ti1O3	La	0.1	Sr	0.9	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	3.54		500	specific heat																																			7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4449	PR0487636	4444, insulator	(Y,Ca)TiO3	Y0.9Ca0.1Ti1O3	Y	0.9	Ca	0.1	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	137.5																																						7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4450	PR0487636	4444, insulator	(Y,Ca)TiO3	Y0.7Ca0.3Ti1O3	Y	0.7	Ca	0.3	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	90.6																																						7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4451	PR0487636	4444,metallic	(Y,Ca)TiO3	Y0.5Ca0.5Ti1O3	Y	0.5	Ca	0.5	Ti	1															O	3		1	1993																												GdFeO3																		K					1.2																																																										mJ/K2fu	9.3																																						7	see Phys.Rev.B,46(1992)11167					METAL-INSULATOR TRANSITION IN LA1-XSRXTIO3 AND Y1-XCAXTIO3 INVESTIGATED BY SPECIFIC-HEAT MEASUREMENTS	199309			PHYS.REV.B,48(1993)7636	K.KUMAGAI,T.SUZUKI,Y.FUJISHIMA,Y.OKADA,Y.TAGUCHI,Y.TOKURA		
4452	PHC1920001	nearly single phase	(Ho,Ce)2Sr2Cu3O8+z	Ho1.11Ce0.89Sr2Cu3O8.6	Ho	1.11	Ce	0.89	Sr	2	Cu	3													O	8+z	8.6	1	1992																											2	223			A	3.826		29.1												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4453	PHC1920001	nearly single phase	(Eu,Ce)2(Eu,Sr)2(Cu,Co)3O8+z	Eu2.17Ce0.5Sr1.33Cu2Co1O9.03	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2	Co	1											O	8+z	9.03	1	1992																											2	223			A	3.86		27.95												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4454	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Fe)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.75Fe0.25O9.11	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.75	Fe	0.25											O	8+z	9.11		1992																											2	223			A	3.836		28.192												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4455	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Fe)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.5Fe0.5O9.23	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.5	Fe	0.5											O	8+z	9.23		1992																											2	223			A	3.845		28.06												K		25.7		25.7			25.7																																																																																														Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4456	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Fe)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.25Fe0.75O9.41	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.25	Fe	0.75											O	8+z	9.41		1992																											2	223			A	3.852		27.994												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4457	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Fe)3O8+z	Eu2.17Ce0.5Sr1.33Cu2Fe1O9.43	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2	Fe	1											O	8+z	9.43		1992																											2	223			A	3.857		27.969												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4458	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Co)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.75Co0.25O9.02	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.75	Co	0.25											O	8+z	9.02		1992																											2	223			A	3.839		28.215												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4459	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Co)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.5Co0.5O9.08	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.5	Co	0.5											O	8+z	9.08		1992																											2	223			A	3.849		28.104												K		34.9		34.9			34.9																																																																																														Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4460	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Co)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.25Co0.75O9.09	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.25	Co	0.75											O	8+z	9.09		1992																											2	223			A	3.859		28.034												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4461	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Co)3O8+z	Eu2.17Ce0.5Sr1.33Cu2Co1O9.2	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2	Co	1											O	8+z	9.2		1992																											2	223			A	3.862	27.96													K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4462	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Al)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.75Al0.25O8.88	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.75	Al	0.25											O	8+z	8.88		1992																											2	223			A	3.846		27.953												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4463	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Al)3O8+	Eu2.17Ce0.5Sr1.33Cu2.5Al0.5O9.02	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.5	Al	0.5											O	8+z	9.02		1992																											2	223			A	3.853		27.871												K		16.4		16.4			16.4																																																																																														Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4464	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Al)3O8+z	Eu2.17Ce0.5Sr1.33Cu2.25Al0.75O9.04	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2.25	Al	0.75											O	8+z	9.04		1992																											2	223			A	3.871		27.621												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4465	PHC1920001		(Eu,Ce)2(Eu,Sr)2(Cu,Al)3O8+z	Eu2.17Ce0.5Sr1.33Cu2Al1O9.11	Eu	2.17	Ce	0.5	Sr	1.33	Cu	2	Al	1											O	8+z	9.11		1992																											2	223			A	3.875		27.584												K					4.2																																																																																																Ho2O3,CeO2,SrCO3,CuO,(Co,Fe,Al)-oxide	1	mixture-CAL(1000-1020C in O2)-ANN(600C,4H+400C,4H underthe pressure of p(O2)=200 atm by O2 HIP)					"BA-FREE ""223"" LAYERED COPPER OXIDES,(HO,CE)2SR2CU3O8+Z AND (EU,CE)2(EU,SR)2CU3-XMXO8+Z (M=FE,CO AND AL)"	199203			PHYSICA C,192(1992)1	AKIKO NARA,ATARU ICHINOSE,H.YAMAUCHI,SHOJI TANAKA,TAKAHIRO WADA,YUJI YAEGASHI	EU,CE,SR,CU,FE,CO,AL,HO,O	
4466	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd0.71Sm1.14Ce0.15Cu1O4	Gd	0.71	Sm	1.14	Ce	0.15	Cu	1													O	4			1992																																														K		0.01					0.01																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4467	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd0.51Sm1.34Ce0.15Cu1O4	Gd	0.51	Sm	1.34	Ce	0.15	Cu	1													O	4			1992																																														K		10.9					10.9																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4468	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd0.31Sm1.54Ce0.15Cu1O4	Gd	0.31	Sm	1.54	Ce	0.15	Cu	1													O	4			1992																																														K		14.2					14.2																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4469	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd0.11Sm1.74Ce0.15Cu1O4	Gd	0.11	Sm	1.74	Ce	0.15	Cu	1													O	4			1992																																														K		17.8					17.8																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4470	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd0.05Sm1.8Ce0.15Cu1O4	Gd	0.05	Sm	1.8	Ce	0.15	Cu	1													O	4			1992																																														K		19.1					19.1																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4471	SSC0840721		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4			1992																																														K		20					20																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4472	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd1.8Sm0.05Ce0.15Cu1O4	Gd	1.8	Sm	0.05	Ce	0.15	Cu	1													O	4			1992								162																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4473	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd1.75Sm0.1Ce0.15Cu1O4	Gd	1.75	Sm	0.1	Ce	0.15	Cu	1													O	4			1992								165																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4474	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd1.55Sm0.3Ce0.15Cu1O4	Gd	1.55	Sm	0.3	Ce	0.15	Cu	1													O	4			1992								150																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4475	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd1.3Sm0.55Ce0.15Cu1O4	Gd	1.3	Sm	0.55	Ce	0.15	Cu	1													O	4			1992								143																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4476	SSC0840721		(Gd,Sm,Ce)2CuO4	Gd1.1Sm0.75Ce0.15Cu1O4	Gd	1.1	Sm	0.75	Ce	0.15	Cu	1													O	4			1992								0.001																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4477	SSC0840721		(Gd,Ce)2CuO4	Gd1.85Ce0.15Cu1O4	Gd	1.85	Ce	0.15	Cu	1															O	4			1992								155																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4478	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd1.8Pr0.05Ce0.15Cu1O4	Gd	1.8	Pr	0.05	Ce	0.15	Cu	1													O	4			1992								155																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4479	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd1.75Pr0.1Ce0.15Cu1O4	Gd	1.75	Pr	0.1	Ce	0.15	Cu	1													O	4			1992								154																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4480	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd1.55Pr0.3Ce0.15Cu1O4	Gd	1.55	Pr	0.3	Ce	0.15	Cu	1													O	4			1992								144																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4481	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd1.3Pr0.55Ce0.15Cu1O4	Gd	1.3	Pr	0.55	Ce	0.15	Cu	1													O	4			1992								0.001																																																																																																																																																		SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4482	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.9Pr0.95Ce0.15Cu1O4	Gd	0.9	Pr	0.95	Ce	0.15	Cu	1													O	4			1992																																														K		0.001					0.001																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4483	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.71Pr1.14Ce0.15Cu1O4	Gd	0.71	Pr	1.14	Ce	0.15	Cu	1													O	4			1992																																														K		8.1					8.1																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4484	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.51Pr1.34Ce0.15Cu1O1	Gd	0.51	Pr	1.34	Ce	0.15	Cu	1													O	1			1992																																														K		12.1					12.1																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4485	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.32Pr1.53Ce0.15Cu1O4	Gd	0.32	Pr	1.53	Ce	0.15	Cu	1													O	4			1992																																														K		13.6					13.6																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4486	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.12Pr1.73Ce0.15Cu1O4	Gd	0.12	Pr	1.73	Ce	0.15	Cu	1													O	4			1992																																														K		15.8					15.8																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4487	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.07Pr1.78Ce0.15Cu1O4	Gd	0.07	Pr	1.78	Ce	0.15	Cu	1													O	4			1992																																														K		17.4					17.4																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4488	SSC0840721		(Gd,Pr,Ce)2CuO4	Gd0.02Pr1.83Ce0.15Cu1O4	Gd	0.02	Pr	1.83	Ce	0.15	Cu	1													O	4			1992																																														K		18.5					18.5																																																																																																					SUPERCONDUCTIVITY AND ANTIFERROMAGNETIC ORDERING IN (GD,R)1.85CE0.15CUO4 WITH R=PR AND SM	199211	ANTIFERROMAGNETIC OR,PHASE DIAGRAM	DEPARTMENT OF PHYSICS, PEKING UNIVERSITY, BEIJING	SOLID STATE COMMUN.,84(1992)721	CHIN LIN,GUO LU,ZUN-XIAO LIU	GD,CE,CU,O,PR,SM	
4489	SSC0860441	highly textured Bi2223/Ag tape,Jc was also measured	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10	Bi	2	Sr	2	Ca	2	Cu	3													O	10			1993																												Bi2223																		K	106.5					6	106.5			K/GPa	1.6																																																																																												hydrostatic pressure up to 14kBar,					NONLINEAR PRESSURE DEPENDENCE OF THE TRANSPORT CRITICAL CURRENT DENSITY IN BSCCO-2223 TAPES	199305			SOLID STATE COMMUN.,86(1993)441	C.W.CHU,P.H.HOR,S.L.BUD'KO,Y.K.TAO,Y.Q.WANG	BI,SR,CA,CU,O	
4490	SSC0860199	size=1.5*1*0.1 mm3, magnetoresistance of x=0.3,0.37,0.4 in (Y1-xPrx) samples also measured in this paper	(Y,Pr)Ba2Cu3O7	Y0.85Pr0.15Ba2Cu3O7-z	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z		3	1993																												Y123																		K	75	80					80																													T/K			1.7	0.9																																																														5	self-flux method using BaO,CuO flux					MAGNETORESISTANCE AND UPPER CRITICAL FIELDS IN SINGLE CRYSTALY1-XPRXBA2CU3O7-Y	199304			SOLID STATE COMMUN.,86(1993)199	A.K.PRADHAN,B.M.WANKLYN,C.CHEN,J.W.HODBY,S.J.HAZELL,Y.HU	Y,PR,BA,CU,O	
4491	PHC2160181			Ca1Ba1La1Cu3O6.85	Ca	1	Ba	1	La	1	Cu	3													O	7-z	6.85		1993																											2				A	3.871		11.61												K		76		69.8			76																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4492	PHC2160181			Ca0.95Ce0.05Ba1La1Cu3O6.91	Ca	0.95	Ce	0.05	Ba	1	La	1	Cu	3											O	7-z	6.91		1993																											2				A	3.864		11.55												K		64.8		55.9			64.8																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4493	PHC2160181			Ca0.9Ce0.1Ba1La1Cu3O7.02	Ca	0.9	Ce	0.1	Ba	1	La	1	Cu	3											O	7-z	7.02		1993																											2				A	3.849		11.586												K	53	60.5		45.7			60.5																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4494	PHC2160181			Ca0.85Ce0.15Ba1La1Cu3O7.07	Ca	0.85	Ce	0.15	Ba	1	La	1	Cu	3											O	7-z	7.07		1993																											2				A	3.848		11.593												K		52.4		38.3			52.4																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4495	PHC2160181			Ca0.9Nd0.1Ba1La1Cu3O6.87	Ca	0.9	Nd	0.1	Ba	1	La	1	Cu	3											O	7-z	6.87		1993																											2				A	3.869		11.591												K	68.5	73.8		70.4			73.8																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4496	PHC2160181			Ca0.8Nd0.2Ba1La1Cu3O6.99	Ca	0.8	Nd	0.2	Ba	1	La	1	Cu	3											O	7-z	6.99		1993																											2				A	3.87	11.583													K		73.8		69.6			73.8																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4497	PHC2160181			Ca0.7Nd0.3Ba1La1Cu3O7.04	Ca	0.7	Nd	0.3	Ba	1	La	1	Cu	3											O	7-z	7.04		1993																											2				A	3.86		11.541												K		73.8		62.5			73.8																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4498	PHC2160181			Ca0.6Nd0.4Ba1La1Cu3O7.1	Ca	0.6	Nd	0.4	Ba	1	La	1	Cu	3											O	7-z	7.1		1993																											2				A	3.857		11.531												K		48.6		37.2			48.6																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4499	PHC2160181			Ca0.5Nd0.5Ba1La1Cu3O7.17	Ca	0.5	Nd	0.5	Ba	1	La	1	Cu	3											O	7-z	7.17		1993																											2				A	3.852		11.594												K		41.4					41.4																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4500	PHC2160181			Ca0.4Nd0.6Ba1La1Cu3O7.19	Ca	0.4	Nd	0.6	Ba	1	La	1	Cu	3											O	7-z	7.19		1993																											2				A	3.868		11.524												K		21.9					21.9																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4501	PHC2160181			Ca0.3Nd0.7Ba1La1Cu3O7.24	Ca	0.3	Nd	0.7	Ba	1	La	1	Cu	3											O	7-z	7.24		1993																											2				A	3.867		11.517												K		14.3					14.3																																																																																														CaCO3,Ba(NO3)2,La2O3,CuO,CeO2,Nd2O3	1	mixture-CAL(1220-1235K,24H)-SIN(1250K,48H)-pellet-SIN(1250-1270K,24H)-cool to 400K(1K/min in flowing O2)-FC to RT					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF CA1-XRXBALACU3O7-Z (R=CA AND ND) SYSTEMS	199310			PHYSICA C,216(1993)181	J.V.YAKHMI,R.A.GUNASEKARAN,R.M.IYER	CA,CE,ND,BA,LA,CU,O	
4502	PHC2160187	THCFIG shows lattice thermal conductivity, UHV shows thermal diffusivity as a function of T at 1 GPa,rod along HIP cylinder axis, 0.7*0.9*13.8 mm3	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1993																												Y124																		K			79			4	79																																																																	THC4502						m.ohm.cm											0.63														HIP					THERMAL CONDUCTIVITY OF YBA2CU4O8 UNDER HIGH PRESSURE	199310			PHYSICA C,216(1993)187	B.M.ANDERSSON,B.SUNDQVIST	Y,BA,CU,O	
4503	PHC2160169	Hc1(77K)=7.8 Oe, Hc1(86.5K)=3.2 Oe	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1993																																														K		90					90											Oe	remanent second harmonic generation																																																																																			1						HC1 MEASUREMENTS IN SINTERED YBACUO AND BI(PB)SRCACUO USIMG REMANENT SECOND-HARMONIC GENERATION	199310			PHYSICA C,216(1993)169	A.K.PRADHAN,KALYAN ADHIKARI,N.C.SONI,P.CHADDAH,RAM PRASAD,S.B.ROY,SHAILENDRA KUMAR	BI,PB,SR,CA,CU,O,Y,BA	
4504	PHC2160169	Hc1(77K)=3.3 Oe, Hc1(102K)=0.2 Oe	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.7Pb0.3Sr2Ca2Cu3O10+z	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	10+z			1993																																														K		105					105											Oe	remanent second harmonic generation																																																																																			1						HC1 MEASUREMENTS IN SINTERED YBACUO AND BI(PB)SRCACUO USIMG REMANENT SECOND-HARMONIC GENERATION	199310			PHYSICA C,216(1993)169	A.K.PRADHAN,KALYAN ADHIKARI,N.C.SONI,P.CHADDAH,RAM PRASAD,S.B.ROY,SHAILENDRA KUMAR	BI,PB,SR,CA,CU,O,Y,BA	
4505	PHC2160147		(Cu,Ce)Sr2(Y,Ce)2Cu2Oz	Sr2Y1.2Ce1.2Cu2.6Oz	Sr	2	Y	1.2	Ce	1.2	Cu	2.6													O	z		1	1993																											2	Cu1222			A	3.82		29.094												K					4.2																																																																																																Y2O3,CeO2,CuO,SrCO3	1	mixture-CAL(960C,1H in air)-ANN(450C,12H in air)					ROLE OF SB DOPING IN GOVERNING THE THERMAL CONDUCTIVITY OF BI-PB-SR-CA-CU-O SUPERCONDUCTORS BETWEEN 10 AND 150 K	199310			PHYSICA C,216(1993)147	DIPTEN BHATTACHARYA,H.S.MAITI	BI,PB,SR,CA,CU,O	
4506	PHC2160147	high-pressure sample, secondary phase detected	(Cu,Ce)Sr2(Y,Ce)2Cu2Oz	Sr2Y1.2Ce1.2Cu2.6Oz	Sr	2	Y	1.2	Ce	1.2	Cu	2.6													O	z			1993																											3	Cu1222			A	3.804	3.838	28.929												K		40					40																																																																																															1	4505 sample-sealed in Au capsule with KClO3-heat(880-1000C,1-2H under 1.7-2.0GPa O2)-ANN(750C,30min+420C,30min under high pressure O2)-Q					ROLE OF SB DOPING IN GOVERNING THE THERMAL CONDUCTIVITY OF BI-PB-SR-CA-CU-O SUPERCONDUCTORS BETWEEN 10 AND 150 K	199310			PHYSICA C,216(1993)147	DIPTEN BHATTACHARYA,H.S.MAITI	BI,PB,SR,CA,CU,O	
4507	PHC2160140	oxygen content by TGA	Dy2Ba4Cu7O14	Dy2Ba4Cu7O14.61	Dy	2	Ba	4	Cu	7															O	14+z	14.61	1	1993																											2	Y247			A	3.857	3.875	50.36												K		29					29																																																																																														Dy(or Nd)2O3,BaCO3,CuO	1	mixture-fire(930C,24H in Alumina crucible)-reground-(930C,24H)-heat(1030C,in 400 atm of flowing O2, several times)-reduced in 5%H2-N2					THE CRYSTAL STRUCTURES OF DY2BA4CU7O14+Z AND ND2BA4CU7O14+Z	199310			PHYSICA C,216(1993)140	D.B.CURRIE,M.T.WELLER	DY,BA,CU,O,ND	
4508	PHC2160140		Nd2Ba4Cu7O14	Nd2Ba4Cu7O15.38	Nd	2	Ba	4	Cu	7															O	14+z	15.38	1	1993																											2	Y247			A	3.891	3.9	50.62												K		35					35																																																																																														Dy(or Nd)2O3,BaCO3,CuO	1	mixture-fire(930C,24H in Alumina crucible)-reground-(930C,24H)-heat(1030C,in 400 atm of flowing O2, several times)-reduced in 5%H2-N2					THE CRYSTAL STRUCTURES OF DY2BA4CU7O14+Z AND ND2BA4CU7O14+Z	199310			PHYSICA C,216(1993)140	D.B.CURRIE,M.T.WELLER	DY,BA,CU,O,ND	
4509	PHC2160124	Tc(x),Lat-c(x),Tc(Lat-c) good relation	Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.26Cd0.74La1Cu3Oz	Ba	1	Ca	0.26	Cd	0.74	La	1	Cu	3											O	z			1993																											2				A			11.67												K			7.6				7.6																																																																																														CaCO3,CdO,CuO,BaCO3,La2O3	1	mixture-(900C,12H)-cool to 600C(5C/min)-FC to RT-reground-SIN(1000C,24H in flowing O2)-cool to 600C-FC to RT					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
4510	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.3Cd0.7La1Cu3Oz	Ba	1	Ca	0.3	Cd	0.7	La	1	Cu	3											O	z			1993																											2				A			11.67												K			13.2				13.2																																																																																														CaCO3,CdO,CuO,BaCO3,La2O3	1	mixture-(900C,12H)-cool to 600C(5C/min)-FC to RT-reground-SIN(1000C,24H in flowing O2)-cool to 600C-FC to RT					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
4511	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.4Cd0.6La1Cu3Oz	Ba	1	Ca	0.4	Cd	0.6	La	1	Cu	3											O	z			1993																											2				A			11.66												K			24				24																																																																																														CaCO3,CdO,CuO,BaCO3,La2O3	1	mixture-(900C,12H)-cool to 600C(5C/min)-FC to RT-reground-SIN(1000C,24H in flowing O2)-cool to 600C-FC to RT					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
4512	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.5Cd0.5La1Cu3Oz	Ba	1	Ca	0.5	Cd	0.5	La	1	Cu	3											O	z			1993																											2				A			11.651												K			34.1				34.1																																																																																														CaCO3,CdO,CuO,BaCO3,La2O3	1	mixture-(900C,12H)-cool to 600C(5C/min)-FC to RT-reground-SIN(1000C,24H in flowing O2)-cool to 600C-FC to RT					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
4513	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.6Cd0.4La1Cu3Oz	Ba	1	Ca	0.6	Cd	0.4	La	1	Cu	3											O	z			1993																											2				A			11.641												K			45.3				45.3																																																																																														CaCO3,CdO,CuO,BaCO3,La2O3	1	mixture-(900C,12H)-cool to 600C(5C/min)-FC to RT-reground-SIN(1000C,24H in flowing O2)-cool to 600C-FC to RT					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
4514	PHC2160017	380.0 mg for specific heat, 65K<T<200K, volume fraction of Hg1223 is about 30%	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8	Hg	1	Ba	2	Ca	2	Cu	3													O	8			1993																												Hg1223																		K		133					133																																																					SP4514			mJ/K2fu	18	for T>Tc C=C(L)+r*T, for T<Tc C=C(L)+r*T+(3*r/Tc**2)*T**3																																					1	Ba2Ca2Cu3Oz+HgO-press into pelet-seal in quartz tube-heat(800C,5H)-cool to RT-ANN(300C,several hours in flowing O2)					SPECIFIC HEAT OF SUPERCONDUCTING HGBA2CA2CU3O8 BETWEEN 65 AND200 K	199310			PHYSICA C,216(1993)17	A.SCHILLING,H.R.OTT,O.JEANDUPEUX	HG,BA,CA,CU,O	
4515	PHC2160006	majority phase is Hg1223	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8	Hg	1	Ba	2	Ca	2	Cu	3													O	8		2	1993																											2	Hg1223	P4/mmm		A	3.851		15.847												K	130	132	134	134			132																																																																																															1	Ba2Ca2Cu3Oz+HgO-press into pelet-seal in quartz tube-heat(800C,5H)-cool to RT-ANN(300C,several hours in flowing O2)					MAGNETIZATION AND RESISTIVITY STUDY ON THE 130 K SUPERCONDUCTOR IN THE HG-BA-CA-CU-O SYSTEM	199310			PHYSICA C,216(1993)6	A.SCHILLING,H.R.OTT,J.D.GUO,O.JEANDUPEUX	HG,BA,CA,CU,O	
4516	PHC2160001	for 0.4<=x<=0.6 in Nd(1-x)Ca(x)Ba2Cu2HgO6+z , single phase obtained	HgBa2(Nd,Ca)Cu2O6	Nd0.5Ca0.5Ba2Cu2HgO6+z	Nd	0.5	Ca	0.5	Ba	2	Cu	2	Hg												O	6+z		1	1993																											2	Hg1212			A	3.877	12.607													K			110				110										25																																																																																						mixture(NdBa2Cu3O7,CaO,Ba2),CuO,HgO)-heat upto 800C in quartz tube-(800C,5-8H)-cool to RT within 12H					SUPERCONDUCTIVITY UP TO 110 K IN THE 1212-HG BASED CUPRATE ND1-XCAXBA2HG1-X'CU2+X'O6+Y	199310			PHYSICA C,216(1993)1	A.MAIGNAN,B.RAVEAU,C.MICHEL,G.VAN TENDELOO,M.HERVIEU	ND,CA,BA,HG,CU,O	
4517	PHC2160001		(Hg,Cu)Ba2(Nd,Ca)Cu2O6	Nd0.6Ca0.4Ba2Cu2.2Hg0.8O6+z	Nd	0.6	Ca	0.4	Ba	2	Cu	2.2	Hg	0.8											O	6+z		1	1993																											2	Hg1212																		K			108				108										25																																																																																						mixture(NdBa2Cu3O7,CaO,Ba2),CuO,HgO)-heat upto 800C in quartz tube-(800C,5-8H)-cool to RT within 12H					SUPERCONDUCTIVITY UP TO 110 K IN THE 1212-HG BASED CUPRATE ND1-XCAXBA2HG1-X'CU2+X'O6+Y	199310			PHYSICA C,216(1993)1	A.MAIGNAN,B.RAVEAU,C.MICHEL,G.VAN TENDELOO,M.HERVIEU	ND,CA,BA,HG,CU,O	
4518	PHC2160029	moisture,CO2 are harmful when synthesized	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z		2	1993																											2	Hg1212	P4/mmm		A	3.85		12.66												K	126		128	128			128										90																																																																																					1	mixture(BaO,CaO,CuO,HgO)-ground in glove(N2)-pellet-seal in quartz tube-heat to 800C(2C/min)-(800C,8H)-cool to RT					STRUCTURE,DOPING AND SUPERCONDUCTIVITY IN HGBA2CACU2O6+Z (TC<-128K)	199310			PHYSICA C,216(1993)29	B.A.HUNTER,D.G.HINKS,G.S.KNAPP,J.D.JORGENSEN,J.L.WAGNER,M.A.BENO,P.G.RADAELLI	HG,BA,CA,CU,O	
4519	PHC2160029	sample reduced in Ar	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z		2	1993																											2	Hg1212	P4/mmm		A	3.863		12.698												K				92			92										40																																																																																					1	mixture(BaO,CaO,CuO,HgO)-ground in glove(N2)-pellet-seal in quartz tube-heat to 800C(2C/min)-(800C,8H)-cool to RT					STRUCTURE,DOPING AND SUPERCONDUCTIVITY IN HGBA2CACU2O6+Z (TC<-128K)	199310			PHYSICA C,216(1993)29	B.A.HUNTER,D.G.HINKS,G.S.KNAPP,J.D.JORGENSEN,J.L.WAGNER,M.A.BENO,P.G.RADAELLI	HG,BA,CA,CU,O	
4520	PHC1590391	Hc2 was defined as mid-point of normal resistivity	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.98	Nd	1.85	Ce	0.15	Cu	1															O	4	3.98		1989																												T'																		K		19					19																													T/K		1.8			HC4520																																																																			MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y     (Ln=Pr,Nd,Sm,Eu,Gd:M=Ce,Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Physica.C,159(1989)391-403	B.W. LEE,C.L. SEAMAN,E.A. EARLY,J.J. NEUMEIER,J.T. MARKERT,M.B. MAPLE,N.Y. AYOUB,P.K. TSAI,S. GHAMATY,T. BJORNHOLM		
4521	PHC1590391		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4			1989							-23	1.7																																																																																																																																												1	ANN(1000C IN O2)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y     (Ln=Pr,Nd,Sm,Eu,Gd:M=Ce,Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Physica.C,159(1989)391-403	B.W. LEE,C.L. SEAMAN,E.A. EARLY,J.J. NEUMEIER,J.T. MARKERT,M.B. MAPLE,N.Y. AYOUB,P.K. TSAI,S. GHAMATY,T. BJORNHOLM		
4522	PHC1590391		Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4			1989							-81																																																																																																																																													1	ANN(1000C IN O2)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y     (Ln=Pr,Nd,Sm,Eu,Gd:M=Ce,Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Physica.C,159(1989)391-403	B.W. LEE,C.L. SEAMAN,E.A. EARLY,J.J. NEUMEIER,J.T. MARKERT,M.B. MAPLE,N.Y. AYOUB,P.K. TSAI,S. GHAMATY,T. BJORNHOLM		
4523	PHC1590391		Sm2CuO4	Sm2Cu1O4	Sm	2	Cu	1																	O	4			1989					/Sm	0.33	-8.3	5.95																				T'																																																																																																																								1	ANN(1000C IN O2)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y     (Ln=Pr,Nd,Sm,Eu,Gd:M=Ce,Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Physica.C,159(1989)391-403	B.W. LEE,C.L. SEAMAN,E.A. EARLY,J.J. NEUMEIER,J.T. MARKERT,M.B. MAPLE,N.Y. AYOUB,P.K. TSAI,S. GHAMATY,T. BJORNHOLM		
4524	PHC1590391		Gd2CuO4	Gd2Cu1O4	Gd	2	Cu	1																	O	4			1989					/Gd	7.79	-15.3																																																																																																																																													1	ANN(1000C IN O2)					MAGNETIC AND SUPERCONDUCTING PROPERTIES OF THE ELECTRON-DOPED COMPOUNDS Ln2-xMxCuO4-y     (Ln=Pr,Nd,Sm,Eu,Gd:M=Ce,Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Physica.C,159(1989)391-403	B.W. LEE,C.L. SEAMAN,E.A. EARLY,J.J. NEUMEIER,J.T. MARKERT,M.B. MAPLE,N.Y. AYOUB,P.K. TSAI,S. GHAMATY,T. BJORNHOLM		
4525	NAT3380635	(anisotropy factor for Hc2) = 21. Hc2-Fig: p=1 and p=2 show for H// and Hn to CuO2 plane.	(Nd,Ce)2CuO4	Nd1.84Ce0.16Cu1O4	Nd	1.84	Ce	0.16	Cu	1															O	4		3	1989																											2	T'			A	3.956		12.108												K	21		22.5				21.75																				T	resistivity, WHH theory		137	6.69					T/K			8.85	0.43			A			70.2	3.4																																																						Nd2O3,CeO2,CuO	1	mixture-heat(1300C,2H)-slowly cool to 700C(1.2C/H)-FC to RT-ANN(950C,8H in air)					Growth and anisotropic superconducting properties of Nd2-xCexCuO4-y single crystals				Nature 338(1989)635-637	M.Suzuki,Y.Hidaka		
4526	PHC2220278		(Tl,Pb,Bi)(Sr,Ba)Ca2Cu3O9	Tl0.6Pb0.2Bi0.2Sr1.8Ba0.2Ca2Cu3O9	Tl	0.6	Pb	0.2	Bi	0.2	Sr	1.8	Ba	0.2	Ca	2	Cu	3							O	9			1994																											2	Tl1223			A	3.822		15.348												K		122		122			122																																																																																														SrCO3,BaCO3,CaCO3,CuO,PbO,Tl2O3,Bi2O3	1	mixture-CAL(920C,10H in air)-precursor(Sr-Ba-Ca-Cu-O)+Tl;Pb;Bi;-oxide-pellet-wrapped in Au foil-(920C,3H in O2)-cool(2C/min)					Improvement of phase purity and accelerated formation of the Tl-1223 phase from the stoichiometric compositions (Tl0.6Pb0.2Bi0.2)(Sr2-xBax)Ca2Cu3O9 (x=0.2-0.3)	199403			Physica C, 222(1994)278-282	D.A.Jefferson,D.S.Shy,R.S.Liu,S.F.Hu,S.F.Wu	Tl,Pb,Bi,Sr,Ba,Ca,Cu,O	
4527	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.92Ca0.08Sr2Cu2.5Fe0.5O6.74	Y	0.92	Ca	0.08	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.74		1994	emu/mole	0.001	emu.K/mole	0.749	micro.B/Mo	2.5	-8.7	22																			2	Y123			A	3.804		11.42												K					4.2																																																																																																	1	4530-reduce(800C in flowing N2)-ANN(400C,24H in flowing O2)					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4528	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.9Ca0.1Sr2Cu2.5Fe0.5O6.75	Y	0.9	Ca	0.1	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.75		1994	emu/mole	0.001	emu.K/mole	0.737	micro.B/Mo	2.4	-9	21																			2	Y123			A	3.801		11.41												K					4.2																																																																																																	1	4530-reduce(800C in flowing N2)-ANN(400C,24H in flowing O2)					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4529	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.88Ca0.12Sr2Cu2.5Fe0.5O6.67	Y	0.88	Ca	0.12	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.67		1994	emu/mole	0.001	emu.K/mole	0.755	micro.B/Mo	2.5	-8.6	21																			2	Y123			A	3.797		11.4												K					4.2																																																																																																	1	4530-reduce(800C in flowing N2)-ANN(400C,24H in flowing O2)					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4530	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.92Ca0.08Sr2Cu2.5Fe0.5O6.92	Y	0.92	Ca	0.08	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.92		1994	emu/mole	0.001	emu.K/mole	0.715	micro.B/Mo	2.4	-8.7																				2	Y123			A	3.86		11.39												K		8					8																																																																																														Y2O3,CaCO3,SrCO3,CuO,Fe2O3	1	mixture-SIN(950C,16-20H in air)-ground-pellet-SIN(990C,70H)-ANN(1040C,75H in flowing O2)-slow cool(1C/min) to RT in air					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4531	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.9Ca0.1Sr2Cu2.5Fe0.5O6.9	Y	0.9	Ca	0.1	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.9		1994	emu/mole	0.001	emu.K/mole	0.746	micro.B/Mo	2.4	-10.9																				2	Y123			A	3.798		11.39												K		20					20																																																																																														Y2O3,CaCO3,SrCO3,CuO,Fe2O3	1	mixture-SIN(950C,16-20H in air)-ground-pellet-SIN(990C,70H)-ANN(1040C,75H in flowing O2)-slow cool(1C/min) to RT in air					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4532	PHC2220157		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.88Ca0.12Sr2Cu2.5Fe0.5O6.89	Y	0.88	Ca	0.12	Sr	2	Cu	2.5	Fe	0.5											O	6+z	6.89		1994	emu/mole	0.001	emu.K/mole	0.747	micro.B/Mo	2.4	-10.8																				2	Y123			A	3.803		11.41												K		19					19																																																																																														Y2O3,CaCO3,SrCO3,CuO,Fe2O3	1	mixture-SIN(950C,16-20H in air)-ground-pellet-SIN(990C,70H)-ANN(1040C,75H in flowing O2)-slow cool(1C/min) to RT in air					Fe migration, magnetic order, and the suppression of superconductivity in Y1-zCazSr2Cu2.5Fe0.5O6+x	199403			Physica C, 222(1994)157-165	J.B.Goodenough,J.J.Neumeier,J.O.Willis,M.G.Smith,R.D.Taylor	Y,Ca,Sr,Cu,Fe,O	
4533	PHC2220052		CuBa2Ca2Cu2O8	Ba2Ca2Cu3O8+z	Ba	2	Ca	2	Cu	3															O	8+z		2	1994																												Cu1223			A			15												K		75					75																																																																																															1	precursor(Ba2Ca2Cu3Oz)+Ag-mix-high pressure(5GPa) synthesis, for detail  see Physica C 215(1993)1					A new HTSC family: the copper analogs of the single-layer Hg or Tl copper oxide superconductors	199403		Laboratoire de Cristallographie,CNRS,Grenoble,Cedex,France	Physica C, 222(1994)52-56	B.Souletie,C.Chaillout,J.-L.Tholence,J.J.Capponi,M.A.Alario-Franco	Hg,Ba,Ca,Cu,O,Tl	
4534	PHC2220052		CuBa2Ca3Cu4O10	Ba2Ca3Cu5O10+z	Ba	2	Ca	3	Cu	5															O	10+z		2	1994																												Cu1234			A			18												K		80					80																																																																																															1	precursor(Ba2Ca2Cu3Oz)+Ag-mix-high pressure(5GPa) synthesis, for detail  see Physica C 215(1993)1					A new HTSC family: the copper analogs of the single-layer Hg or Tl copper oxide superconductors	199403		Laboratoire de Cristallographie,CNRS,Grenoble,Cedex,France	Physica C, 222(1994)52-56	B.Souletie,C.Chaillout,J.-L.Tholence,J.J.Capponi,M.A.Alario-Franco	Hg,Ba,Ca,Cu,O,Tl	
4535	PHC2220052		CuBa2Ca4Cu5O12	Ba2Ca4Cu6O12+z	Ba	2	Ca	4	Cu	6															O	12+z		2	1994																												Cu1245			A			21												K		95					95																																																																																															1	precursor(Ba2Ca2Cu3Oz)+Ag-mix-high pressure(5GPa) synthesis, for detail  see Physica C 215(1993)1					A new HTSC family: the copper analogs of the single-layer Hg or Tl copper oxide superconductors	199403		Laboratoire de Cristallographie,CNRS,Grenoble,Cedex,France	Physica C, 222(1994)52-56	B.Souletie,C.Chaillout,J.-L.Tholence,J.J.Capponi,M.A.Alario-Franco	Hg,Ba,Ca,Cu,O,Tl	
4536	PHC2220052		CuBa2Ca5Cu6O14	Ba2Ca5Cu7O14+z	Ba	2	Ca	5	Cu	7															O	14+z		2	1994																												Cu1256			A			24												K		120					120																																																																																															1	precursor(Ba2Ca2Cu3Oz)+Ag-mix-high pressure(5GPa) synthesis, for detail  see Physica C 215(1993)1					A new HTSC family: the copper analogs of the single-layer Hg or Tl copper oxide superconductors	199403		Laboratoire de Cristallographie,CNRS,Grenoble,Cedex,France	Physica C, 222(1994)52-56	B.Souletie,C.Chaillout,J.-L.Tholence,J.J.Capponi,M.A.Alario-Franco	Hg,Ba,Ca,Cu,O,Tl	
4537	PHC2220007	90%Hg1223, <5%Ba-Cu-O, >5%CaHgO2	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																											2	Hg1223	P4/mmm		A	3.852		15.83												K		134.5		134.5			134.5																																																																																															1	Ba2Ca2Cu3O7+HgO-mix-pellet-quartz tube-heat(860C,6H)-ANN(300C,6H in O2)					Single-step synthesis of bulk HgBa2Ca2Cu3O8+z	199403		Chemistry Division,Oal Ridge National Laboratory, Oak Ridge,TN,USA	Physica C, 222(1994)7	M.Paranthaman	Hg,Ba,Ca,Cu,O	
4538	PHC2220013		(Pb,Hg)Sr2(Ca,Y)Cu2O7	Pb0.5Hg0.5Sr2Ca0.8Y0.2Cu2O7-z	Pb	0.5	Hg	0.5	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	7-z			1994																											2	Pb1212																																																																																																																							PbO,HgO,SrO2,CaO,Y2O3,CuO		see Solid  State Chem. 103(1993)280					Crystal structure of the (Pb,Hg)Sr2(Ca,Y)Cu2O7-z superconductor	199403		Material Research Laboratories, Industrial Technology Research Institute,Hsinchu,Taiwan	Phisica C, 222(1994)13	D.A.Jefferson,D.H.Chen,D.S.Shy,R.S.Liu,S.F.Hu	Pb,Hg,Sr,Ca,Y,Cu,O	
4539	PHC2220013		(Pb,Hg)Sr2(Ca,Y)Cu2O7	Pb0.5Hg0.5Sr2Ca0.7Y0.3Cu2O7-z	Pb	0.5	Hg	0.5	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	7-z			1994																											2	Pb1212																																																																																																																							PbO,HgO,SrO2,CaO,Y2O3,CuO		see Solid  State Chem. 103(1993)280					Crystal structure of the (Pb,Hg)Sr2(Ca,Y)Cu2O7-z superconductor	199403		Material Research Laboratories, Industrial Technology Research Institute,Hsinchu,Taiwan	Phisica C, 222(1994)13	D.A.Jefferson,D.H.Chen,D.S.Shy,R.S.Liu,S.F.Hu	Pb,Hg,Sr,Ca,Y,Cu,O	
4540	PHC2220013		(Pb,Hg)Sr2(Ca,Y)Cu2O7	Pb0.5Hg0.5Sr2Ca0.6Y0.4Cu2O7-z	Pb	0.5	Hg	0.5	Sr	2	Ca	0.6	Y	0.4	Cu	2									O	7-z			1994																											2	Pb1212																																																																																																																							PbO,HgO,SrO2,CaO,Y2O3,CuO		see Solid  State Chem. 103(1993)280					Crystal structure of the (Pb,Hg)Sr2(Ca,Y)Cu2O7-z superconductor	199403		Material Research Laboratories, Industrial Technology Research Institute,Hsinchu,Taiwan	Phisica C, 222(1994)13	D.A.Jefferson,D.H.Chen,D.S.Shy,R.S.Liu,S.F.Hu	Pb,Hg,Sr,Ca,Y,Cu,O	
4541	PHC2220013		(Pb,Hg)Sr2(Ca,Y)Cu2O7	Pb0.5Hg0.5Sr2Ca0.5Y0.5Cu2O7-z	Pb	0.5	Hg	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	7-z			1994																											2	Pb1212			A	3.817		11.948																																																																																																																	PbO,HgO,SrO2,CaO,Y2O3,CuO		see Solid  State Chem. 103(1993)280					Crystal structure of the (Pb,Hg)Sr2(Ca,Y)Cu2O7-z superconductor	199403		Material Research Laboratories, Industrial Technology Research Institute,Hsinchu,Taiwan	Phisica C, 222(1994)13	D.A.Jefferson,D.H.Chen,D.S.Shy,R.S.Liu,S.F.Hu	Pb,Hg,Sr,Ca,Y,Cu,O	
4542	PHC2220019	for oz=7.6  sample has T1=65K and T3=90K	(Pb,Hg)Sr2(Nd,Ca)Cu2O7	Pb0.7Hg0.3Sr2Nd0.3Ca0.7Cu2O6.6	Pb	0.7	Hg	0.3	Sr	2	Nd	0.3	Ca	0.7	Cu	2									O	7	6.6		1994																											2	Pb1212	P4/mmm		A	3.812		12.134												K	80		100				90																																																																																														PbO2,HgO,SrO2,SrCuO2,CuO,CaO,Nd2O3	1	mixtre-heat(800C)					Lead-mercury-based superconductors. The 1212 cuprate Pb0.7Hg0.3Sr2+xCa0.7Nd0.3-xCu2O7-z and the new oxycarbonate Pb0.7Hg0.3Sr4Cu2CO3O7	199403		CNRS, Universite de Caen, Caen, France	Physica C, 222(1994)19	A.Maignan,B.Raveau,C.Martin,C.Michel,G.Van Tendeloo,M.Hervieu,M.Huve	Pb,Hg,Sr,Ca,Nd,Cu,O,C	
4543	PHC2220019		(Pb,Hg)Sr4Cu2(CO3)O7	Pb0.7Hg0.3Sr4Cu2C1O10	Pb	0.7	Hg	0.3	Sr	4	Cu	2	C	1											O	10			1994																											2	Pb1212	P4/mmm		A	3.824		16.468												K		68		68			68																																																																																															1	mixture-heat(800C)-ANN(400C,30min in 90%Ar+10%H2)					Lead-mercury-based superconductors. The 1212 cuprate Pb0.7Hg0.3Sr2+xCa0.7Nd0.3-xCu2O7-z and the new oxycarbonate Pb0.7Hg0.3Sr4Cu2CO3O7	199403		CNRS, Universite de Caen, Caen, France	Physica C, 222(1994)19	A.Maignan,B.Raveau,C.Martin,C.Michel,G.Van Tendeloo,M.Hervieu,M.Huve	Pb,Hg,Sr,Ca,Nd,Cu,O,C	
4544	PR04900572	film	YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-z	6.9	4	1994																												Y123																		K	89.8						89.8																													T/K		1.7																																																																	films grown by BaF2 process. for resistivity, they were patterned photolithographically. O-content was controlled by isobaric sequential anneals at 550C under reduced partial O2 pressure					Upper-critical fields of YBa2Cu3O7-z epitaxial thin films with variable oxygen deficiency z	1		Department of Physics,University of Tennessee,Knoxville,Tennessee,USA	Phys.Rev.B, 49(1994)572	D.K.Christen,E.C.Jones,J.G.Ossandon,J.R.Thompson,Julia M.Phillips,M.P.Siegal,R.Feenstra	Y,Ba,Cu,O	
4546	PR04900572	film	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7-z	7	4	1994																												Y123																		K	90		90.5				90.25																													T/K		1.7																																																																	films grown by BaF2 process. for resistivity, they were patterned photolithographically. O-content was controlled by isobaric sequential anneals at 550C under reduced partial O2 pressure					Upper-critical fields of YBa2Cu3O7-z epitaxial thin films with variable oxygen deficiency z	1		Department of Physics,University of Tennessee,Knoxville,Tennessee,USA	Phys.Rev.B, 49(1994)572	D.K.Christen,E.C.Jones,J.G.Ossandon,J.R.Thompson,Julia M.Phillips,M.P.Siegal,R.Feenstra	Y,Ba,Cu,O	
4547	PR04900572	film	YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	4	1994																												Y123																		K	89.1						89.1																													T/K		1.7																																																																	films grown by BaF2 process. for resistivity, they were patterned photolithographically. O-content was controlled by isobaric sequential anneals at 550C under reduced partial O2 pressure					Upper-critical fields of YBa2Cu3O7-z epitaxial thin films with variable oxygen deficiency z	1		Department of Physics,University of Tennessee,Knoxville,Tennessee,USA	Phys.Rev.B, 49(1994)572	D.K.Christen,E.C.Jones,J.G.Ossandon,J.R.Thompson,Julia M.Phillips,M.P.Siegal,R.Feenstra	Y,Ba,Cu,O	
4548	PR04900580		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1994																												Y123																				92					92																																																																																					m3/C			0.00000000073		5	RH4548				5	ANN(420C,1 week in flowing O2)					Normal-state Hall effect in YBa2Cu3-xFexO7-z single crystals	1		Department of Physics,University of California,Davis,California,USA	Phys.Rev.B, 49(1994)580	J.Z.Liu,Lu Zhang,M.D.Lan,R.N.Shelton,Y.X.Jia	Y,Ba,Cu,Fe,O	
4549	PR04900580		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.98Fe0.02O7-z	Y	1	Ba	2	Cu	2.98	Fe	0.02													O	7-z		3	1994																												Y123																				93.4					93.4																																																																																					m3/C			0.000000001		5	RH4549				5	ANN(420C,1 week in flowing O2)					Normal-state Hall effect in YBa2Cu3-xFexO7-z single crystals	1		Department of Physics,University of California,Davis,California,USA	Phys.Rev.B, 49(1994)580	J.Z.Liu,Lu Zhang,M.D.Lan,R.N.Shelton,Y.X.Jia	Y,Ba,Cu,Fe,O	
4550	PR04900580		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.96Fe0.04O7-z	Y	1	Ba	2	Cu	2.96	Fe	0.04													O	7-z		3	1994																												Y123																				90.5					90.5																																																																																					m3/C			0.0000000011		5	RH4550				5	ANN(420C,1 week in flowing O2)					Normal-state Hall effect in YBa2Cu3-xFexO7-z single crystals	1		Department of Physics,University of California,Davis,California,USA	Phys.Rev.B, 49(1994)580	J.Z.Liu,Lu Zhang,M.D.Lan,R.N.Shelton,Y.X.Jia	Y,Ba,Cu,Fe,O	
4551	PR04900580		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7-z	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7-z		3	1994																												Y123																		K		75					75																																																																																					m3/C			0.0000000016		5	RH4551				5	ANN(420C,1 week in flowing O2)					Normal-state Hall effect in YBa2Cu3-xFexO7-z single crystals	1		Department of Physics,University of California,Davis,California,USA	Phys.Rev.B, 49(1994)580	J.Z.Liu,Lu Zhang,M.D.Lan,R.N.Shelton,Y.X.Jia	Y,Ba,Cu,Fe,O	
4552	PR04900580		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2O7-z	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	7-z		3	1994																												Y123																		K		64					64																																																																																					m3/C			0.0000000023			RH4552				5	ANN(420C,1 week in flowing O2)					Normal-state Hall effect in YBa2Cu3-xFexO7-z single crystals	1		Department of Physics,University of California,Davis,California,USA	Phys.Rev.B, 49(1994)580	J.Z.Liu,Lu Zhang,M.D.Lan,R.N.Shelton,Y.X.Jia	Y,Ba,Cu,Fe,O	
4553	PHC2210039		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.98Zn0.02O7-z	Yb	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		83.3					83.3	TC4553																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4554	PHC2210039		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.98Zn0.02O7-z	Er	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		85.5					85.5	TC4554																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4555	PHC2210039		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.98Zn0.02O7-z	Y	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		84.7					84.7	TC4555																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4556	PHC2210039		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.98Zn0.02O7-z	Dy	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		84.8					84.8	TC4556																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4557	PHC2210039		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.98Zn0.02O7-z	Gd	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		86					86	TC4557																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4558	PHC2210039		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.98Zn0.02O7-z	Eu	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		86					86	TC4558																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4559	PHC2210039		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.98Zn0.02O7-z	Sm	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		86.3					86.3	TC4559																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4560	PHC2210039		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.98Zn0.02O7-z	Nd	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z		1	1994																												Y123																		K		85.5					85.5	TC4560																																																																																													R2O3,BaCO3,CuO,ZnO	1	mixture-CAL(915C,24H)-ground-pellet-SIN(925C,72H in flowing O2)-ANN(680C,10H + 400C,10H)-FC to RT in flowing O2					Effect of Zn doping on the superconductivity of RBa2Cu3-xZnxO7-z (R=Yb,Er,Y,Dy,Gd,Eu,Sm,Nd)	199402			Physica C, 221(1994)39-45	Ch. Heiden,S.S.Ata-Allah,Yunhui Xu	Ba,Cu,O,Zn,Yb,Er,Y,Dy,Gd,Eu,Sm,Nd	
4561	PHC2200001		(Bi,Hg)Sr2YCu2O7	Bi0.33Hg0.67Sr2Y1Cu2O7	Bi	0.33	Hg	0.67	Sr	2	Y	1	Cu	2											O	7		1	1994																											2	Hg1212			A	3.816		12.02												K		74		74			74																																																																																														Bi2O3,CuO,SrCO3,CaCO3,Y2O3,HgO	1	precursor(Bi-Sr-Ca-Cu-Y-O)+HgO-wrapped in Au foil-ANN(in quartz tube)					Studies on (Hg,Bi)-1212: A 92K superconductor	199402			Physica C, 220(1994)1-6	A.P.B.Sinha,D.E.Morris,K.K.Singh,V.Kirtikar	Hg,Bi,Sr,Y,Ca,Cu,O	
4562	PHC2200001		(Bi,Hg)Sr2(Y,Ca)Cu2O7	Bi0.33Hg0.67Sr2Y0.5Ca0.5Cu2O7	Bi	0.33	Hg	0.67	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7		1	1994																											2	Hg1212			A	3.811		12												K		92		92			92																																																																																														Bi2O3,CuO,SrCO3,CaCO3,Y2O3,HgO	1	precursor(Bi-Sr-Ca-Cu-Y-O)+HgO-wrapped in Au foil-ANN(in quartz tube)					Studies on (Hg,Bi)-1212: A 92K superconductor	199402			Physica C, 220(1994)1-6	A.P.B.Sinha,D.E.Morris,K.K.Singh,V.Kirtikar	Hg,Bi,Sr,Y,Ca,Cu,O	
4563	PHC2200001	not superconducting	(Bi,Hg)Sr2CaCu2O7	Bi0.33Hg0.67Sr2Ca1Cu2O7	Bi	0.33	Hg	0.67	Sr	2	Ca	1	Cu	2											O	7		3	1994																											2	Hg1212			A	5.345		24.329												K					4.2																																																																																																Bi2O3,CuO,SrCO3,CaCO3,Y2O3,HgO	1	precursor(Bi-Sr-Ca-Cu-Y-O)+HgO-wrapped in Au foil-ANN(in quartz tube)					Studies on (Hg,Bi)-1212: A 92K superconductor	199402			Physica C, 220(1994)1-6	A.P.B.Sinha,D.E.Morris,K.K.Singh,V.Kirtikar	Hg,Bi,Sr,Y,Ca,Cu,O	
4564	PHC2220027	as-grown,this system has a superstructure a=24.71, b=5.49, c=16.94	HgBa2Sr2Cu2O6(CO3)	Hg1Ba2Sr2Cu2C1O9+z	Hg	1	Ba	2	Sr	2	Cu	2	C	1											O	9+z			1994																											2				A	3.88		16.94												K	46	58	58	58			58										20																																																																																				HgO,Ba2CuO3,Sr2CuO2(CO3)	1	mixture-pellet-seal in evacuated quartz ampoule-fire(800C,5H)-Q					New Hg based oxycarbonate superconductor HgBa2Sr2Cu2O6+z(CO3)	199403		Department of Physics, Aoyama-Gakuen University, Tokyo,Japan	Physica C, 222(1994)27-32	H.Nakata,J.Akimitsu,M.Uehara,S.Sahoda,Y.Matsui	Hg,Ba,Sr,Cu,O,C	
4565	PHC2220027		HgBa2Sr2Cu2O6(CO3)	Hg1Ba2Sr2Cu2C1O9+z	Hg	1	Ba	2	Sr	2	Cu	2	C	1											O	9+z			1994																											2																			K	58	66	66	66			66										20																																																																																				HgO,Ba2CuO3,Sr2CuO2(CO3)	1	mixture-pellet-seal in evacuated quartz ampoule-fire(800C,5H)-Q					New Hg based oxycarbonate superconductor HgBa2Sr2Cu2O6+z(CO3)	199403		Department of Physics, Aoyama-Gakuen University, Tokyo,Japan	Physica C, 222(1994)27-32	H.Nakata,J.Akimitsu,M.Uehara,S.Sahoda,Y.Matsui	Hg,Ba,Sr,Cu,O,C	
4566	PHC2220047	as-sintered	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1994																												Hg1201																		K	50	75					75																																																																		micro.V/K	36			TP4566	m.ohm.cm											600												BaO,HgO,CuO	1	mixture-SIN					Thermoelectric power and resistivity of bulk HgBa2CuO4+y superconductors and the effects of annealing	199403		Phys.Dept.,Victoria University of Wellington,Wellington,New Zealand	Physica C, 222(1994)47-51	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Cu,O	
4567	PHC2220047	as-annealing	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1994																												Hg1201																		K		97					97																																																																		micro.V/K	0.9			TP4567	m.ohm.cm											2												BaO,HgO,CuO	1	mixture-SIN--ANN(500C,12H in flowing O2)					Thermoelectric power and resistivity of bulk HgBa2CuO4+y superconductors and the effects of annealing	199403		Phys.Dept.,Victoria University of Wellington,Wellington,New Zealand	Physica C, 222(1994)47-51	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Cu,O	
4568	PHC2190047		(Eu,Sr)2(Eu,Ce)2Cu3O8	Eu1.6Sr1.8Ce0.6Cu3O8.6	Eu	1.6	Sr	1.8	Ce	0.6	Cu	3													O	8.6	8.6		1994																											2	223			A	3.844		28.09												K		30					30																																																																																														R2O3,SrCO3,CuO	1	mixture-pellet-ANN(1000C,20H)-heat(600C,25H under 120 atm O2)					Synthesis and investigation of Sr-containing 223 and 1222 complex oxides in the R-Sr-Ce-Cu-O system (R=Pr,Nd,Sm-Gd,Dy-Yb and Y)	199401		Department of Chemistry,Moscow State University, Moscow,Russian Federation	Physica C, 219(1994)47-56	A.L.Kharlanov,E.M.Kopnin,E.V.Antipov,I.Bryntse	Sr,Ce,Cu,O,Pr,Nd,Sm,Gd,Dy,Yb,Y	
4569	PHC2190047		(Y,Cu)(Y,Sr)2(Ce,Sr)2Cu2O8	Y1.5Sr1.8Ce1Cu2.7O8.6	Y	1.5	Sr	1.8	Ce	1	Cu	2.7													O	8.6	8.6		1994																											2	Cu1222			A	3.816		29.12												K					4.2																																																																																																R2O3,SrCO3,CuO	1	mixture-pellet-ANN(1000C,20H)-heat(600C,25H under 120 atm O2)					Synthesis and investigation of Sr-containing 223 and 1222 complex oxides in the R-Sr-Ce-Cu-O system (R=Pr,Nd,Sm-Gd,Dy-Yb and Y)	199401		Department of Chemistry,Moscow State University, Moscow,Russian Federation	Physica C, 219(1994)47-56	A.L.Kharlanov,E.M.Kopnin,E.V.Antipov,I.Bryntse	Sr,Ce,Cu,O,Pr,Nd,Sm,Gd,Dy,Yb,Y	
4570	PHC2190047		(Sm,Sr)2(Sm,Ce)2Cu3O8	Sm1.6Sr1.7Ce0.7Cu3O8+z	Sm	1.6	Sr	1.7	Ce	0.7	Cu	3													O	8+z			1994																											2	223			A	3.856		28.18												K		36					36																																																																																														R2O3,SrCO3,CuO	1	mixture-pellet-ANN(1000C,20H)-heat(600C,25H under 120 atm O2)					Synthesis and investigation of Sr-containing 223 and 1222 complex oxides in the R-Sr-Ce-Cu-O system (R=Pr,Nd,Sm-Gd,Dy-Yb and Y)	199401		Department of Chemistry,Moscow State University, Moscow,Russian Federation	Physica C, 219(1994)47-56	A.L.Kharlanov,E.M.Kopnin,E.V.Antipov,I.Bryntse	Sr,Ce,Cu,O,Pr,Nd,Sm,Gd,Dy,Yb,Y	
4571	PHC2210001	measured under He-gas pressure(hydrostatic)	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1994																		GPa		69.9							2	Hg1201			A	3.879		9.516							A/GPa	4.26		5.83	DLDP=(1/L)(dL/dP) in e-3 unit, by NED	K		97		97			97										95																																																																																					1	Ba2CuO3+HgO-pellet-sealed in evacuated quartz-heat(840C,8H)-ANN(in flowing O2)					Pressur-induced structural changes in superconducting HgBa2Cun-1CunO2n+2+z (n=1,2,3) compounds	199402			Physica C,221(1994)1-10	B.A.Hunter,D.G.Hinks,H.Shaked,J.D.Jorgensen,J.L.Wagner,P.G.Radaelli,R.B.Von Dreele,R.L.Hitterman	Hg,Ba,Ca,Cu,O	
4572	PHC2210001	measured under He-gas pressure(hydrostatic)	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1994																		GPa		84.1							2	Hg1212	p4/mmm	123	A	3.849		12.646							A/GPa	2.94		6.04	DLDP=(1/L)(dL/dP) in e-3 unit, by NED	K		128		128			128										95																																																																																				HgO,BaO,CaO,CuO	1	mixture-pellet-sealed in evacuated quartz-heat(810 or 860C, 8 or 6H)-ANN in 2%O2+Ar or O2					Pressur-induced structural changes in superconducting HgBa2Cun-1CunO2n+2+z (n=1,2,3) compounds	199402			Physica C,221(1994)1-10	B.A.Hunter,D.G.Hinks,H.Shaked,J.D.Jorgensen,J.L.Wagner,P.G.Radaelli,R.B.Von Dreele,R.L.Hitterman	Hg,Ba,Ca,Cu,O	
4573	PHC2210001	measured under He-gas pressure(hydrostatic)	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																		GPa		93							2	Hg1223	p4/mmm	123	A	3.846		15.773							A/GPa	2.57		5.62	DLDP=(1/L)(dL/dP) in e-3 unit, by NED	K		135		135			135										95																																																																																				HgO,BaO,CaO,CuO	1	mixture-pellet-sealed in evacuated quartz-heat(810 or 860C, 8 or 6H)-ANN in 2%O2+Ar or O2					Pressur-induced structural changes in superconducting HgBa2Cun-1CunO2n+2+z (n=1,2,3) compounds	199402			Physica C,221(1994)1-10	B.A.Hunter,D.G.Hinks,H.Shaked,J.D.Jorgensen,J.L.Wagner,P.G.Radaelli,R.B.Von Dreele,R.L.Hitterman	Hg,Ba,Ca,Cu,O	
4574	PRL0720128	gap is for a-axis direction, for direction 45 degree from a-axis  gap=23 meV	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1994																											3	Bi2212			A	5.399	5.457	30.724												K		85					85																																														meV	36.6	5	1																																															see Phys.Rev.B, 41(1990)6564					Observation of a-b Plane Gap Anisotropy in BiSr2CaCu2O8 with a Low Temperature Scanning Tunneling Microscope	199401		Department of Physics and Astronomy,University of Kentucky,Lexington,Kentucky 40506-0055	Rhys.Rev.Lett.,72(1994)0128	Jeffrey Kane,K.-W.Ng,Qun Chen		
4575	PHC2210278	impurity Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2GdCu2O7	Bi0.35In0.65Sr2Gd1Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	1	Cu	2											O	z			1994																											2	Tl1212			A	3.838		11.76												K					4.2																																																																																																Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4576	PHC2210278	impurity=Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2(Gd,Ca)Cu2O7	Bi0.35In0.65Sr2Gd0.9Ca0.1Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	0.9	Ca	0.1	Cu	2									O	z			1994																											2	Tl1212			A	3.837		11.762												K					4.2																																																																																																Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4577	PHC2210278	impurity=Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2(Gd,Ca)Cu2O7	Bi0.35In0.65Sr2Gd0.8Ca0.2Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	0.8	Ca	0.2	Cu	2									O	z			1994																											2	Tl1212			A	3.836		11.784												K					4.2																																																																																																Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4578	PHC2210278	impurity=Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2(Gd,Ca)Cu2O7	Bi0.35In0.65Sr2Gd0.7Ca0.3Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	0.7	Ca	0.3	Cu	2									O	z			1994																											2	Tl1212			A	3.835		11.8												K					4.2																																																																																																Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4579	PHC2210278	impurity=Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2(Gd,Ca)Cu2O7	Bi0.35In0.65Sr2Gd0.6Ca0.4Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	0.6	Ca	0.4	Cu	2									O	z			1994																											2	Tl1212			A	3.834		11.779												K	18		42				30																																																																																														Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4580	PHC2210278	impurity=Sr-Cu-O,GdInO3,Sr-Bi-O	(Bi,In)Sr2(Gd,Ca)Cu2O7	Bi0.35In0.65Sr2Gd0.5Ca0.5Cu2Oz	Bi	0.35	In	0.65	Sr	2	Gd	0.5	Ca	0.5	Cu	2									O	z			1994																											2	Tl1212			A	3.835		11.779												K	22		50				36																																																																																														Bi2O3,In2O3,SrCO3,Gd2O3,Ln2O3,CaCO3,CuO	1	mixture-CAL(1103K,5H in air with cover)-pellet-SIN(1283K,1H in flowing O2)-FC-ANN(973K,1H in flowing O2) -cool to 473K(1K/min)					Synthesis and characterization of new cuprates with a (Bi,In)O monolayer: (Bi,In)Sr2(Gd,Ca)Cu2Oz	199403			Physica C, 221(1994)278-282	Cao Guanghan,Chen Zuyao,Huang Yonglan,Qian Yitai,Wang Shizhong,Yu Weichao,Zhang Yuheng	Bi,In,Sr,Gd,Ca,Cu,O	
4581	PRL0721537	photon dose=1.5e+25 photon/cm2, before photon dose Tc=73K	YBa2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	6.70	6.7	4	1994																												Y123																		K	77						77																																																																							m.ohm.cm																								17	film grown on SrTiO3(100) substrate by coevaporation method, heat treatment for each oxygen content					Effects of Photoinduced Hole Doping on Normal-State and Superconducting Transport in Oxygen-Deficient YBa2Cu3Oy	199403		NTT Interdisciplinary Research Laboratories,Tokai,Ibaraki 319-11,Japan	Phys.Rev.Lett.,72(1994)1537	F.Hosseini Teherani,H.Asano,K.Tanabe,M.Suzuki,S.Kubo		
4582	PRL0721537	photon dose=1.5e+25 photon/cm2, before photon dose Tc=45K, resistivity=0.3 mOhm.cm(77K)	YBa2Cu3O7	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	6.45	6.45	4	1994																												Y123																		K	49						49																																																																							m.ohm.cm				0.25																				17	film grown on SrTiO3(100) substrate by coevaporation method, heat treatment for each oxygen content					Effects of Photoinduced Hole Doping on Normal-State and Superconducting Transport in Oxygen-Deficient YBa2Cu3Oy	199403		NTT Interdisciplinary Research Laboratories,Tokai,Ibaraki 319-11,Japan	Phys.Rev.Lett.,72(1994)1537	F.Hosseini Teherani,H.Asano,K.Tanabe,M.Suzuki,S.Kubo		
4583	PRL0721537	photon dose=1.5e+25 photon/cm2, before photon dose Tc=26K, resistivity=0.55 mOhm.cm(77K)	YBa2Cu3O7	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	6.40	6.4	4	1994																												Y123																		K	34						34																																																																							m.ohm.cm				0.4																				17	film grown on SrTiO3(100) substrate by coevaporation method, heat treatment for each oxygen content					Effects of Photoinduced Hole Doping on Normal-State and Superconducting Transport in Oxygen-Deficient YBa2Cu3Oy	199403		NTT Interdisciplinary Research Laboratories,Tokai,Ibaraki 319-11,Japan	Phys.Rev.Lett.,72(1994)1537	F.Hosseini Teherani,H.Asano,K.Tanabe,M.Suzuki,S.Kubo		
4584	PRL0721537	photon dose=1.5e+25 photon/cm2, before photon dose Tc lower than 1.5K, resistivity=1.4 mOhm.cm(77K)	YBa2Cu3O7	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	6.35	6.35	4	1994																												Y123																		K	15						15																																																																							m.ohm.cm				0.8																				17	film grown on SrTiO3(100) substrate by coevaporation method, heat treatment for each oxygen content					Effects of Photoinduced Hole Doping on Normal-State and Superconducting Transport in Oxygen-Deficient YBa2Cu3Oy	199403		NTT Interdisciplinary Research Laboratories,Tokai,Ibaraki 319-11,Japan	Phys.Rev.Lett.,72(1994)1537	F.Hosseini Teherani,H.Asano,K.Tanabe,M.Suzuki,S.Kubo		
4585	PHC2200041		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1994	emu/g	0.00000182																									3	Y124			A	3.837	3.868	27.203												K		80				2	80																																																																							m.ohm.cm											0.88												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4586	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.9Pr0.1Ba2Cu4O8	Y	0.9	Pr	0.1	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000045			uB/Pr	3.53	6																				3	Y124			A	3.841	3.871	27.206												K		75				3	75																																																																							m.ohm.cm											1.03												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4587	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000041			uB/Pr	3.55	3																				3	Y124			A	3.845	3.875	27.214												K		68				4	68																																																																							m.ohm.cm											1.09												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4588	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.7Pr0.3Ba2Cu4O8	Y	0.7	Pr	0.3	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000044			uB/Pr	2.88	4																				3	Y124			A	3.849	3.879	27.215												K		61				4.5	61																																																																							m.ohm.cm											1.18												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4589	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.6Pr0.4Ba2Cu4O8	Y	0.6	Pr	0.4	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000037			uB/Pr	3.17	5																				3	Y124			A	3.853	3.882	27.227												K		58				5	58																																																																							m.ohm.cm											1.28												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4590	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.5Pr0.5Ba2Cu4O8	Y	0.5	Pr	0.5	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000097			uB/Pr	2.95	7																				3	Y124			A	3.858	3.885	27.236												K		49				6	49																																																																							m.ohm.cm											1.36												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4591	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.4Pr0.6Ba2Cu4O8	Y	0.4	Pr	0.6	Ba	2	Cu	4													O	8		1	1994	emu/g	0.0000013			uB/Pr	3.05	9																				3	Y124			A	3.863	3.889	27.248												K		39				6.5	39																																																																							m.ohm.cm											1.56												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4592	PHC2200041	trace of BaCuO2 and CuO	(Y,Pr)Ba2Cu4O8	Y0.3Pr0.7Ba2Cu4O8	Y	0.3	Pr	0.7	Ba	2	Cu	4													O	8		1	1994	emu/g	0.00000148			uB/Pr	3.09	13																				3	Y124			A	3.867	3.892	27.251												K		23				12	23																																																																							m.ohm.cm											2.22												Y2O3,Pr6O11,BaO2,CuO	1	mix in N2-pellet-SIN(900-980C24H in O2 of 38 atm)-cool to RT within 2H, repeat several times					Superconducting properties of (Y1-xPrx)Ba2Cu4O8 compounds	199402			Physica C, 220(1994)41-49	Kay Kohn,Ken Ichiro Gondaira,Nobuyoshi Yamada,Takeo Iri,Zhen Guo	Y,Pr,Ba,Cu,O	
4593	PHC2190183		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.8Ce0.1Ca0.1Ba2Cu3O7-z	Lu	0.8	Ce	0.1	Ca	0.1	Ba	2	Cu	3											O	7-z			1994																												Y123																		K	73						73																																																																																														Lu2O3,CeO2,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4594	PHC2190183	impurity=BaCeO2	(Lu,Ce,Ca)Ba2Cu3O7	Lu0.75Ce0.15Ca0.1Ba2Cu3O7-z	Lu	0.75	Ce	0.15	Ca	0.1	Ba	2	Cu	3											O	7-z			1994																												Y123																		K	70						70																																																																																														Lu2O3,CeO2,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4595	PHC2190183	impurity=BaCeO2	(Lu,Ce,Ca)Ba2Cu3O7	Lu0.7Ce0.15Ca0.15Ba2Cu3O7-z	Lu	0.7	Ce	0.15	Ca	0.15	Ba	2	Cu	3											O	7-z			1994																												Y123																		K	66						66																																																																																														Lu2O3,CeO2,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4596	PHC2190183		(Lu,Ce)Ba2Cu3O7	Lu0.9Ce0.1Ba2Cu3O7-z	Lu	0.9	Ce	0.1	Ba	2	Cu	3													O	7-z			1994																												Y123																		K	60						60																																																																																														Lu2O3,CeO2,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4597	PHC2190183	impurity phase	(Lu,Pr)Ba2Cu3O7	Lu0.93Pr0.07Ba2Cu3O7-z	Lu	0.93	Pr	0.07	Ba	2	Cu	3													O	7-z		2	1994																												Y123																		K	78						78																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4598	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.9Pr0.1Ba2Cu3O7-z	Lu	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	86						86																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4599	PHC2190183		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.8Pr0.1Ca0.1Ba2Cu3O7-z	Lu	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	7-z		1	1994																												Y123																		K	78						78																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4600	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.85Pr0.15Ba2Cu3O7-z	Lu	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	82.5						82.5																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4601	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.8Pr0.2Ba2Cu3O7-z	Lu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	80						80																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4602	PHC2190183		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.7Pr0.2Ca0.1Ba2Cu3O7-z	Lu	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7-z		1	1994																												Y123																		K	74						74																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4603	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.7Pr0.3Ba2Cu3O7-z	Lu	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	71						71																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4604	PHC2190183		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.6Pr0.3Ca0.1Ba2Cu3O7-z	Lu	0.6	Pr	0.3	Ca	0.1	Ba	2	Cu	3											O	7-z		1	1994																												Y123																		K	60.5						60.5																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4605	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.6Pr0.4Ba2Cu3O7-z	Lu	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	49						49																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4606	PHC2190183		(Lu,Pr)Ba2Cu3O7	Lu0.5Pr0.5Ba2Cu3O7-z	Lu	0.5	Pr	0.5	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	29						29																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4607	PHC2190183	semicon-like	(Lu,Pr)Ba2Cu3O7	Lu0.45Pr0.55Ba2Cu3O7-z	Lu	0.45	Pr	0.55	Ba	2	Cu	3													O	7-z		1	1994																												Y123																		K	13						13																																																																																														Lu2O3,Pr6O11,BaCO3,CaCO3,CuO	1	solid state reaction					Superconductivity and valence states of Ce,Pr and Tb in bulk Lu1-xMxBa2Cu3O7-z(M=Ce,Pr and Tb) systems	199401			Physica C, 219(1994)184-190	A.S.Tamhane,K.I.Gnanasekar,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Ce,Pr,Tb,Lu,Ba,Cu,O	
4608	PHC2230207	minor(<5%) impurity	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1994																											2	Hg1201	p4/mm		A	3.879		9.51												K	91.5	94					94																				T	using WHH theory, resistive transition	44							T/K		0.68					A		27												160000																																												HgO,BaO,CuO	1	grind- mixture  in Ar-drybox-sealed in quartz tube-heat-two step cooling					Magnetic and transport properties of HgBa2CuO4+z	199404			Physica C, 223(1994)207-212	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton,T.J.Goodwin	Hg,Ba,Cu,O	
4609	PHC2230238	two step transition in SUS, Cu1234(dominant) + Cu1223 + BaCuO2 +BaCuO2+x	Ba-Ca-Cu-O	Ba2Ca3Cu5O	Ba	2	Ca	3	Cu	5															O			2	1994									6																																					K	107.6		117	106			106																																																																																														BaO2,CaO,CuO	1	Ba:Ca:Cu=2:3:4, mixture-CAL(920C,50H in flowing O2)-SIN-pellet-(5.0GPa-950C)-pressure release					117K superconductivity in the Ba-Ca-Cu-O system	199404			Physica C, 223(1994)238-242	C.-Q.Jin,H.Yamauchi,S.Adachi,S.Tanaka,X.-J.Wu	Ba,Cu,O,Ca	
4610	PHC2230267	not s/c	TlBa2PrCu2O7	Tl1Ba2Pr1Cu2O7-z	Tl	1	Ba	2	Pr	1	Cu	2													O	7-z			1994								8.03																			2	Tl1212	p4/mmm		A	3.919		12.552												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4611	PHC2230267	not s/c	Tl(Ba,Sr)2PrCu2O7	Tl1Ba1.6Sr0.4Pr1Cu2O7-z	Tl	1	Ba	1.6	Sr	0.4	Pr	1	Cu	2											O	7-z			1994								6.22																			2	Tl1212	p4/mmm		A	3.908		12.49												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4612	PHC2230267	not s/c	Tl(Ba,Sr)2PrCu2O7	Tl1Ba1.2Sr0.8Pr1Cu2O7-z	Tl	1	Ba	1.2	Sr	0.8	Pr	1	Cu	2											O	7-z			1994								5.74																			2	Tl1212	p4/mmm		A	3.895		12.384												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4613	PHC2230267	not s/c	Tl(Ba,Sr)2PrCu2O7	Tl1Ba1Sr1Pr1Cu2O7-z	Tl	1	Ba	1	Sr	1	Pr	1	Cu	2											O	7-z			1994								5.44																			2	Tl1212	p4/mmm		A	3.889		12.309												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4614	PHC2230267	not s/c	Tl(Ba,Sr)2PrCu2O7	Tl1Ba0.8Sr1.2Pr1Cu2O7-z	Tl	1	Ba	0.8	Sr	1.2	Pr	1	Cu	2											O	7-z			1994								5.24																			2	Tl1212	p4/mmm		A	3.882		12.275												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4615	PHC2230267	not s/c	Tl(Ba,Sr)2PrCu2O7	Tl1Ba0.4Sr1.6Pr1Cu2O7-z	Tl	1	Ba	0.4	Sr	1.6	Pr	1	Cu	2											O	7-z			1994								4.53																			2	Tl1212	p4/mmm		A	3.868		12.195												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4616	PHC2230267	not s/c	TlSr2PrCu2O7	Tl1Sr2Pr1Cu2O7-z	Tl	1	Sr	2	Pr	1	Cu	2													O	7-z			1994								4.03																			2	Tl1212	p4/mmm		A	3.854		12.102												K					4.2																																																																																																	1						Structures and antiferromagnetic Pr ordering mechanism of Tl(Ba2-xSrx)PrCu2O7-z compounds by Rietveld analysis	199404			Physica C, 223(1994)267-275	Chiou-Chu Lai,Hoong-Kun Fun,Huan-Chiu Ku,Ping Yang,Tsong-Jen Lee	Tl,Ba,Sr,Pr,Cu,O	
4617	PHC2230037	not s/c	Ba4YCu2.37O7.85(SO4)0.5	Ba4Y1Cu2.37S0.5O9.85	Ba	4	Y	1	Cu	2.37	S	0.5													O	9.85	9.85	1	1994																											2		p4/mmm		A	5.854		8.082												K					4.2																																																																																																BaO,BaSO4,CaO,Y2O3,CuO	1	mixture-heat(1000C)-ANN(400C,12H in O2)					Synthesis and structure of the perovskite oxy-sulphates Ba4MCu2+xO6+y(SO4)z (M=Ca,Y)	199404			Physica C, 223(1994)37-45	C.Greaves,P.R.Slater	Ba,Cu,O,Ca,Y	
4618	PHC2230037	not s/c	Ba4CaCu2.38O7.52(SO4)0.5	Ba4Ca1Cu2.38S0.5O9.52	Ba	4	Ca	1	Cu	2.38	S	0.5													O	9.52	9.52	1	1994																											2		p4/mmm		A	5.838		8.143												K					4.2																																																																																																BaO,BaSO4,CaO,Y2O3,CuO	1	mixture-heat(1000C)-ANN(400C,12H in O2)					Synthesis and structure of the perovskite oxy-sulphates Ba4MCu2+xO6+y(SO4)z (M=Ca,Y)	199404			Physica C, 223(1994)37-45	C.Greaves,P.R.Slater	Ba,Cu,O,Ca,Y	
4619	PHC2230037	not s/c	Ba4YCu2.15O6.90(SO4)0.8	Ba4Y1Cu2.15S0.8O10.1	Ba	4	Y	1	Cu	2.15	S	0.8													O	10.1	10.1	1	1994																											2		p4/mmm		A	5.887		8.102												K					4.2																																																																																																BaO,BaSO4,CaO,Y2O3,CuO	1	mixture-heat(1000C)-ANN(400C,12H in O2)					Synthesis and structure of the perovskite oxy-sulphates Ba4MCu2+xO6+y(SO4)z (M=Ca,Y)	199404			Physica C, 223(1994)37-45	C.Greaves,P.R.Slater	Ba,Cu,O,Ca,Y	
4620	PHC2230313	hydrostatic pressure, Figure is Tc vs P	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1994																												Hg1212																		K		126.6					126.6	TC4620	2	K/GPa	1.8																																																																																										HgO,BaO,CaO,CuO		see Physica C 216(1993)29					Hydrostatic pressure dependence of the superconducting transition temperature of HgBa2CaCu2O6+z and HgBa2Ca2Cu3O8+z	199404			Physica C, 223(1994)313-320	A.-K.Klehe,D.G.Hinks,J.L.Wagner,J.S.Schilling	Hg,Ba,Ca,Cu,O	
4621	PHC2230313	hydrostatic pressure, Figure is Tc vs P	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																												Hg1223																		K		133.9					133.9	TC4621	2	K/GPa	1.71																																																																																										HgO,BaO,CaO,CuO		see Physica C 216(1993)29					Hydrostatic pressure dependence of the superconducting transition temperature of HgBa2CaCu2O6+z and HgBa2Ca2Cu3O8+z	199404			Physica C, 223(1994)313-320	A.-K.Klehe,D.G.Hinks,J.L.Wagner,J.S.Schilling	Hg,Ba,Ca,Cu,O	
4622	PR0478167		Bi2CuO4	Bi2Cu1O4	Bi	2	Cu	1																	O	4		3	1993					uB/Cu	0.63		44																			2		p4/ncc	130	A	8.51		5.814																																																																																																																		7	grown from the melt by floating zone method with an image furnace					MAGNON DISPERSION CURVE OF ANTIFERROMAGNETIC BI2CUO4	199304			PHYS.REV.B,47(1993)8167	A.REVCOLEVSCHI,B.HENNION,G.DHALENNE,M.AIN,O.GUISELIN	BI,CU,O	
4623	PHC2230051		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1994																											3	Y124			A	3.833	3.861	27.189												K		79.7					79.7																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4624	PHC2230051		(Y,Pr)Ba2Cu4O8	Y0.95Pr0.05Ba2Cu4O8	Y	0.95	Pr	0.05	Ba	2	Cu	4													O	8		1	1994																											3	Y124			A	3.834	3.863	27.172												K		77					77																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4625	PHC2230051		(Y,Pr)Ba2Cu4O8	Y0.9Pr0.1Ba2Cu4O8	Y	0.9	Pr	0.1	Ba	2	Cu	4													O	8		1	1994																											3	Y124			A	3.837	3.867	27.174												K		74.6					74.6																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4626	PHC2230051		(Y,Pr)Ba2Cu4O8	Y0.85Pr0.15Ba2Cu4O8	Y	0.85	Pr	0.15	Ba	2	Cu	4													O	8		1	1994																											3	Y124			A	3.839	3.867	27.184												K		72.3					72.3																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4627	PHC2230051		(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		1	1994																											3	Y124			A	3.841	3.869	27.184												K		70.8					70.8																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4628	PHC2230051		(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8		1	1994																											3	Y124			A	3.833	3.861	27.189												K		88.8					88.8																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4629	PHC2230051		(Y,Pr,Ca)Ba2Cu4O8	Y0.85Pr0.05Ca0.1Ba2Cu4O8	Y	0.85	Pr	0.05	Ca	0.1	Ba	2	Cu	4											O	8		1	1994																											3	Y124			A	3.83	3.86	27.169												K		83.8					83.8																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4630	PHC2230051		(Y,Pr,Ca)Ba2Cu4O8	Y0.8Pr0.1Ca0.1Ba2Cu4O8	Y	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	4											O	8		1	1994																											3	Y124			A	3.832	3.862	27.174												K		80					80																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4631	PHC2230051		(Y,Pr,Ca)Ba2Cu4O8	Y0.75Pr0.15Ca0.1Ba2Cu4O8	Y	0.75	Pr	0.15	Ca	0.1	Ba	2	Cu	4											O	8		1	1994																											3	Y124			A	3.834	3.864	27.18												K		76.2					76.2																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4632	PHC2230051		(Y,Pr,Ca)Ba2Cu4O8	Y0.7Pr0.2Ca0.1Ba2Cu4O8	Y	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	4											O	8		1	1994																											3	Y124			A	3.836	3.867	27.173												K		73.4					73.4																																																																																														Pr6O11,BaO2,CuO,CaO	1	mixture-dry-press-fire(930-950C,30H in O2 of 200bar)-repeat					Effect of praseodymium substitution in YBa2Cu4O8(1:2:4)	199404			Physica C, 223(1994)51-56	A.P.B.Sinha,D.E.Morris,George H.Kwei,H.B.Liu	Y,Ba,Cu,O,Pr	
4633	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.91Ce0.09Cu1O3.97	La	1	Nd	0.91	Ce	0.09	Cu	1													O	4	3.97	1	1994																												T'																		K		15.7					15.7																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4634	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.9Ce0.1Cu1O3.974	La	1	Nd	0.9	Ce	0.1	Cu	1													O	4	3.974	1	1994																												T'																		K		19.9					19.9																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4635	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.89Ce0.11Cu1O3.978	La	1	Nd	0.89	Ce	0.11	Cu	1													O	4	3.978	1	1994																												T'																		K		19.8					19.8																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4636	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.87Ce0.13Cu1O3.975	La	1	Nd	0.87	Ce	0.13	Cu	1													O	4	3.975	1	1994																												T'																		K		16.8					16.8																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4637	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.86Ce0.14Cu1O3.978	La	1	Nd	0.86	Ce	0.14	Cu	1													O	4	3.978	1	1994																												T'																		K		16					16																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4638	PR04906293		(La,Nd,Ce)2CuO4	La1Nd0.85Ce0.15Cu1O4	La	1	Nd	0.85	Ce	0.15	Cu	1													O	4		1	1994																												T'																		K		8.8					8.8																																																																																															1	L2O3,ceric ammonium nitrate, Cu were dissolved in dilute nitric acid,-CAL(500C,6H in air)-SIN(1000C,24H)-ANN(950C, in N2)					Role of boud-length mismatch in L2-xCexCuO4(L=lanthanide)	3		Center for Materials Science and Engineering, ETC 9.104, The University of Texas at Austin, Austin, Texas 78712	Phys.Rev.B,49(1994)6293	A. Manthiram,Y.T. Zhu		
4639	PR0455628	Figure=Hirr vs T,Hirr determined by dc magnetization	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8			1992																												Tl2212																		K		102					102																																		HIR4639																																																													1						Field-modulated microwave surface resistance in a single-crystal Tl2Ca2BaCu2O8 superconductor	199203		Department of phisics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801	Phys.Rev.B,45(1992)5628	A.M. Hermann,H.M. Duan,M.B. Salamon,N.T. Tea,T. Datta		
4640	PR0455547	4%Tl2Ba2CaCu2O8 phase,grain size=20-30micron-meter,thickness=1micron-meter,Jc(100K,0T)=5E+5 A/cm2	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+z		4	1992																												Tl2223																		K		116					116																																		HIR4640																																																													17	substrate=LaAlO3, epitaxial film by single target rf magnetron sputtering					MAGNETIC RELAXATION AND IRREVERSIBILITY IN A SUPERCONDUCTING TL2BA2CA2CU3O10+-X THIN FILM	199203			PHYS.REV.B,45(1992)5547	S.H.LIOU,V.K.CHAN	TL,BA,CA,CU,O	
4641	PR0426797	Figure=Hirr vs T for H//c-axis,platelet=1.5*1*0.3mm3,Hirr by ac-permiability measurement using freq. from 10 to E+5 Hz	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1990																												Y123																		K		87.5					87.5																																		HIR4641																																																																			FLUX PINNING AND IRREVERSIBILITY IN YBA2CU3O7 SUPERCONDUCTINGCRYSTAL	199010		DIVISION OF PHYSICS, THE NORWEGIAN INSTITUTE OF TECHNOLOGY ANDSINTEF APPLIED PHYSICS, 7034 TRONDHEIM, NORWAY	PHYS.REV.B,42(1990)6797	K.FOSSHEIM,L.T.SAGDAHL,S.GJOLMESLI,T.LAEGREID,W.ASSMUS	Y,BA,CU,O	
4642	APL0630693	Figure= Hirr vs T, Jc(10K,2T)=1.6E+3 A/cm2	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1993																												Hg1201	p4/mmm		A	3.878		9.527												K	94			94			94																																		HIR4642																																																												HgO,PbO,Ba2CuO3	1	see Physica C 210(1993)447					The irreversibility line of HgBa2CuO4+z	8		Argonne National Laboratory, Argonne,Illinois,USA	Appl.Phys.Lett., 63(1993)693	B.Dabrowski,D.G.Hinks,G.W.Crabtree,J.D.Jorgensen,J.F.Mitchell,J.L.Wagner,P.G.Radaelli,U.Welp	Hg,Ba,Pb,Cu,O	
4643	APL0630693	Figure=Hirr vs T	(Hg,Pb)Ba2CuO4	Hg0.8Pb0.2Ba2Cu1O4+z	Hg	0.8	Pb	0.2	Ba	2	Cu	1													O	4+z			1993																											2	Hg1201	p4/mmm		A	3.881		9.531												K	96			96			96																																		HIR4643																																																												HgO,PbO,Ba2CuO3	1	see Physica C 210(1993)447					The irreversibility line of HgBa2CuO4+z	8		Argonne National Laboratory, Argonne,Illinois,USA	Appl.Phys.Lett., 63(1993)693	B.Dabrowski,D.G.Hinks,G.W.Crabtree,J.D.Jorgensen,J.F.Mitchell,J.L.Wagner,P.G.Radaelli,U.Welp	Hg,Ba,Pb,Cu,O	
4644	PR0428704	1*1mm *300A,electrical contact by silver epoxy	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																		K	82						82																																																																																					m3/C					7	RH4644										HALL-EFFECT MEASUREMENTS ON SUPERCONDUCTING AND NONSUPERCONDUCTING COPPER-OXIDE-BASED METALS	199011	HALL EFFECT         ,SINGLE CRYSTALS	DEPARTMENT OF PHYSICS, STATE UNIVERSITY OF NEW YORK AT STONY BROOK, NEW YORK 11794	PHYS.RE,B,42(1990)8704	C.KENDZIORA,D.MANDRUS,L.FORRO,L.MIHALY,R.REEDER	BI,SR,CA,CU,O	
4645	PR0428704	metallic	Bi2Sr2CuO6	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O	6			1990																												Bi2201																		K					3																																																																																							m3/C					7	RH4645										HALL-EFFECT MEASUREMENTS ON SUPERCONDUCTING AND NONSUPERCONDUCTING COPPER-OXIDE-BASED METALS	199011	HALL EFFECT         ,SINGLE CRYSTALS	DEPARTMENT OF PHYSICS, STATE UNIVERSITY OF NEW YORK AT STONY BROOK, NEW YORK 11794	PHYS.RE,B,42(1990)8704	C.KENDZIORA,D.MANDRUS,L.FORRO,L.MIHALY,R.REEDER	BI,SR,CA,CU,O	
4646	PRL0672088		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.984Zn0.016O7-z	Y	1	Ba	2	Cu	2.984	Zn	0.016													O	7-z		3	1991																												Y123																		K	83	84					84																																																																																					m3/C						RH4646				5	Zn-doped ceramic is crushed and dissolved in the ratio 1:5 in BaCuO2+z flux at 1025C, slow cool in flowing O2--ANN in O2 of 3 bar					EFFECT OF ZN IMPURITIES ON THE NORMAL-STATE HALL ANGLE IN SINGLE-CRYSTAL YBA2CU3-XZNXO7-Z	199110		JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCERON UNIVERSITY,PRINCETON UNIVERSITY,PRINCERON,NEW JERSEY 08544	PHYS.REV.LETT.,67(1991)2088	N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,ZN,O	
4647	PRL0672088		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.948Zn0.052O7-z	Y	1	Ba	2	Cu	2.948	Zn	0.052													O	7-z		3	1991																												Y123																		K	72	73					73																																																																																					m3/C						RH4647				5	Zn-doped ceramic is crushed and dissolved in the ratio 1:5 in BaCuO2+z flux at 1025C, slow cool in flowing O2--ANN in O2 of 3 bar					EFFECT OF ZN IMPURITIES ON THE NORMAL-STATE HALL ANGLE IN SINGLE-CRYSTAL YBA2CU3-XZNXO7-Z	199110		JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCERON UNIVERSITY,PRINCETON UNIVERSITY,PRINCERON,NEW JERSEY 08544	PHYS.REV.LETT.,67(1991)2088	N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,ZN,O	
4648	PRL0672088		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.909Zn0.091O7-z	Y	1	Ba	2	Cu	2.909	Zn	0.091													O	7-z		3	1991																												Y123																		K	50	55					55																																																																																					m3/C						RH4648				5	Zn-doped ceramic is crushed and dissolved in the ratio 1:5 in BaCuO2+z flux at 1025C, slow cool in flowing O2--ANN in O2 of 3 bar					EFFECT OF ZN IMPURITIES ON THE NORMAL-STATE HALL ANGLE IN SINGLE-CRYSTAL YBA2CU3-XZNXO7-Z	199110		JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCERON UNIVERSITY,PRINCETON UNIVERSITY,PRINCERON,NEW JERSEY 08544	PHYS.REV.LETT.,67(1991)2088	N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,ZN,O	
4649	PRL0672088		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.892Zn0.108O7-z	Y	1	Ba	2	Cu	2.892	Zn	0.108													O	7-z		3	1991																												Y123																		K	40	48					48																																																																																					m3/C						RH4649				5	Zn-doped ceramic is crushed and dissolved in the ratio 1:5 in BaCuO2+z flux at 1025C, slow cool in flowing O2--ANN in O2 of 3 bar					EFFECT OF ZN IMPURITIES ON THE NORMAL-STATE HALL ANGLE IN SINGLE-CRYSTAL YBA2CU3-XZNXO7-Z	199110		JOSEPH HENRY LABORATORIES OF PHYSICS,PRINCERON UNIVERSITY,PRINCETON UNIVERSITY,PRINCERON,NEW JERSEY 08544	PHYS.REV.LETT.,67(1991)2088	N.P.ONG,T.R.CHIEN,Z.Z.WANG	Y,BA,CU,ZN,O	
4650	PHC2220257	Tc measured by resistivity,lattice const. linearly decreases with Ocontent	(Ba,K)BiO3	Ba0.65K0.35Bi1O2.984	Ba	0.65	K	0.35	Bi	1															O	z	2.984		1994																												BKBO																		K		27.9					27.9	TC4650																																																																																													BaO,KO2,Bi2O3	1	mixture-heat(700C,1H in N2)-C-heat(500C,2H)-ANN in O2 for various O-content					Defect chemistry of Ba1-xKxBiOy superconductors	199403			Physica C, 222(1994)257-266	Kazuo Fueki,Yasushi Idemoto,Yoshiki Iwata	Ba,K,Bi,O	
4651	PHC2220257	Fig=Tc vs O-content	(Ba,k)BiO3	Ba0.525K0.475Bi1O2.917	Ba	0.525	K	0.475	Bi	1															O	z	2.917		1994																												BKBO																		K		25.9					25.9	TC4651																																																																																													BaO,KO2,Bi2O3	1	mixture-heat(700C,1H in N2)-C-heat(500C,2H)-ANN in O2 for various O-content					Defect chemistry of Ba1-xKxBiOy superconductors	199403			Physica C, 222(1994)257-266	Kazuo Fueki,Yasushi Idemoto,Yoshiki Iwata	Ba,K,Bi,O	
4652	PHC2220257	Fig=Tc vs O-content	(Ba,K)BiO3	Ba0.6K0.4Bi1O2.926	Ba	0.6	K	0.4	Bi	1															O	z	2.926		1994																												BKBO																		K		27.6					27.6	TC4652																																																																																													BaO,KO2,Bi2O3	1	mixture-heat(700C,1H in N2)-C-heat(500C,2H)-ANN in O2 for various O-content					Defect chemistry of Ba1-xKxBiOy superconductors	199403			Physica C, 222(1994)257-266	Kazuo Fueki,Yasushi Idemoto,Yoshiki Iwata	Ba,K,Bi,O	
4653	PR0489747	SUS(Pauli)=1.51E-4 cm3/mole	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.29	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6.29	6.29		1993																												Bi2201																		K		30.6		30.6			30.6																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4654	PR0489747	SUS(Pauli)=2.86E-4 cm3/mole	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	8.16	8.16		1993																												Bi2212																		K		92.8		92.8			92.8																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4655	PR0489747	SUS(Pauli)=1.47E-4 cm3/mole	Tl2Ba2CuO6	Tl2Ba2Cu1O6.1	Tl	2	Ba	2	Cu	1															O	6.10	6.1		1993																												Tl2201																		K		92.5		92.5			92.5																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4656	PR0489747	SUS(Pauli)=2.73E-4 cm3/mole	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+z			1993																												Tl2212																		K		106.8		106.8			106.8																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4657	PR0489747	SUS(Pauli=3.77 E-4 cm3/mole	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+z			1993																												Tl2223																		K		120		120			120																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4658	PR0489747	SUS(Pauli)=2.06 E-4 cm3/mole	Bi2Sr2Ca1Cu2O8	Bi2Sr2Ca1Cu2O8.11	Bi	2	Sr	2	Ca	1	Cu	2													O	8.11	8.11		1993	cm3/mole				micro.B/Mo	0.834																						Bi2212																		K		86.5		86.5			86.5																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4659	PR0489747	SUS(Pauli)=2.27E-4 cm3/mole	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	8.16	8.16		1993	cm3/mole				micro.B/Mo	0.709																						Bi2212																		K		92.8		92.8			92.8																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4660	PR0489747	SUS(Pauli)=2.37E-4 cm3/mole	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.19	Bi	2	Sr	2	Ca	1	Cu	2													O	8.19	8.19		1993	cm3/mole				micro.B/Mo	0.682																						Bi2212																		K		87.1		87.1			87.1																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4661	PR0489747	SUS(Pauli)=2.45E-4 cm3/mole	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.22	Bi	2	Sr	2	Ca	1	Cu	2													O	8.22	8.22		1993	cm3/mole				micro.B/Mo	0.702																						Bi2212																		K		77.6		77.6			77.6																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4662	PR0489747	SUS(Pauli)=2.69E-4 cm3/mole	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.24	Bi	2	Sr	2	Ca	1	Cu	2													O	8.24	8.24		1993	cm3/mole				micro.B/Mo	0.616																						Bi2212																		K		71.1		71.1			71.1																																																																																																SEE PHYSICA C,194(1992)337					MAGNETIC SUSCEPTIBILITY IN THE NORMAL STATE: A TOOL TO OPTIMIZE TC WITHIN A GIVEN SUPERCONDUCTING OXIDE SYXTEM	199310			PHYS.REV.B,48(1993)9747	C.ALLGEIER,J.S.SCHILLING		
4663	JJP0330503	as-sintered it contains Cu1245,BaCuO2 and other phases	CuBa2Ca3Cu4O12	Cu5Ba2Ca3O12-z	Cu	5	Ba	2	Ca	3															O	12-z		2	1994																											2	Cu1234			A	7.711		35.986												K	109.3	116.3		116.4			116.3										20																																																																																				BaCO3,CaCO3,CuO	1	mixture of some kind of Ba-Ca-Cu-O -mix with CaO2-pellet-sealed in Au capsule-heat(1100C,3H in graphite tube under 5GPa-ANN(300C,5-10H in flowing O2)					New High-Tc Superconductor Family oof Cu-Based Cu1-xBa2Can-1CunO2n+4-z with Tc>116K	199404			Jpn.J.Apll.Phys.Lett.,33(1994)L503-506	Akira Negishi,Hideo Ihara,Hirofumi Matuhata,Hirotomo Ozawa,Kazuyasu Tokiwa,Masayuki Hirabayashi,Young Seok Song	Cu,Ba,Ca,O	
4664	PHC2270160		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1994																											2	T			A	3.371		13.222												K		27.8					27.8																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4665	PHC2270160	semiconductor-like	(La,Sr)2(Cu,Ni)O4	La0.9Sr0.1Cu1.98Ni0.02O4	La	0.9	Sr	0.1	Cu	1.98	Ni	0.02													O	4		1	1994																											2	T																		K					4.2																																																																																																La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4666	PHC2270160	semiconductor-like	(La,Sr)2(Cu,Ni)O4	La0.9Sr0.1Cu0.965Ni0.035O4	La	0.9	Sr	0.1	Cu	0.965	Ni	0.035													O	4		1	1994																											2	T																		K					4.2																																																																																																La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4667	PHC2270160		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1994																											2	T			A	3.786		13.246												K		37					37																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4668	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.965Ni0.035O4	La	1.85	Sr	0.15	Cu	0.965	Ni	0.035													O	4		1	1994																											2	T																		K		2.1					2.1																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4669	PHC2270160		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		1	1994																											2	T			A	3.782		13.252												K	37						37																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4670	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.98Ni0.02O4	La	1.83	Sr	0.17	Cu	0.98	Ni	0.02													O	4		1	1994																											2	T																		K	22.1						22.1																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4671	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.97Ni0.03O4	La	1.83	Sr	0.17	Cu	0.97	Ni	0.03													O	4		1	1994																											2	T																		K	14.4						14.4																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4672	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.96Ni0.04O4	La	1.83	Sr	0.17	Cu	0.96	Ni	0.04													O	4		1	1994																											2	T																		K	5.8						5.8																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4673	PHC2270160		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1994																											2	T			A	3.78		13.261												K	31						31																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4674	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.98Ni0.02O4	La	1.8	Sr	0.2	Cu	0.98	Ni	0.02													O	4		1	1994																											2	T																		K	17.1						17.1																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4675	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.97Ni0.03O4	La	1.8	Sr	0.2	Cu	0.97	Ni	0.03													O	4		1	1994																											2	T																		K	11.1						11.1																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4676	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.96Ni0.04O4	La	1.8	Sr	0.2	Cu	0.96	Ni	0.04													O	4		1	1994																											2	T																		K	7						7																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4677	PHC2270160		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1994																											2	T			A	3.777		13.263												K	16.2						16.2																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4678	PHC2270160	resistivity not to zero at 0K.	(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.96Ni0.04O4	La	1.75	Sr	0.25	Cu	0.96	Ni	0.04													O	4		1	1994																											2	T																		K			33.6				33.6																																																																																														La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4679	PHC2270160	semiconductor-like	(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.92Ni0.08O4	La	1.75	Sr	0.25	Cu	0.92	Ni	0.08													O	4		1	1994																											2	T																		K					4.2																																																																																																La2O3,SrCo3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C,in air)-ANN(500C,10H in flowing O2)-cool to RT(1C/min)					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4680	PHC2260243	oxygen content by iodometry, linear dependence of R on T	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.231	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.231		1994																												Bi2212																		K		83.7					83.7																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture-fire(800C,12H)-pellet-SIN(825C,24H in air)-FC-ANN(300-400,100H in 1-1080 atm O2) or (600C,24H in flowing N2)					Dependence of Tc on the excess oxygen content z in Bi2Sr2CaCu2O8+z annealed under high pressures of oxygen	199406			Physica C, 226(1994)243-249	Masatsune Kato,Takashi Noji,Wataru Ito,Yoji Koike,Yoshitami Saito	Bi,Sr,Ca,Cu,O	
4681	PHC2260243		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.329	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.329		1994			emu.K/mole	0.048																								Bi2212																		K		47.3					47.3																																																																							m.ohm.cm											0.835												Bi2O3,SrCO3,CaCO3,CuO	1	mixture-fire(800C,12H)-pellet-SIN(825C,24H in air)-FC-ANN(300-400,100H in 1-1080 atm O2) or (600C,24H in flowing N2)					Dependence of Tc on the excess oxygen content z in Bi2Sr2CaCu2O8+z annealed under high pressures of oxygen	199406			Physica C, 226(1994)243-249	Masatsune Kato,Takashi Noji,Wataru Ito,Yoji Koike,Yoshitami Saito	Bi,Sr,Ca,Cu,O	
4682	PHC2260243	linear dependence of R on T	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.373	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.373		1994			emu.K/mole	0.079																								Bi2212																		K		47.2					47.2																																																																							m.ohm.cm											0.745												Bi2O3,SrCO3,CaCO3,CuO	1	mixture-fire(800C,12H)-pellet-SIN(825C,24H in air)-FC-ANN(300-400,100H in 1-1080 atm O2) or (600C,24H in flowing N2)					Dependence of Tc on the excess oxygen content z in Bi2Sr2CaCu2O8+z annealed under high pressures of oxygen	199406			Physica C, 226(1994)243-249	Masatsune Kato,Takashi Noji,Wataru Ito,Yoji Koike,Yoshitami Saito	Bi,Sr,Ca,Cu,O	
4683	PHC2260243		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.428	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.428		1994																												Bi2212																		K		42.1					42.1																																																																							m.ohm.cm											0.677												Bi2O3,SrCO3,CaCO3,CuO	1	mixture-fire(800C,12H)-pellet-SIN(825C,24H in air)-FC-ANN(300-400,100H in 1-1080 atm O2) or (600C,24H in flowing N2)					Dependence of Tc on the excess oxygen content z in Bi2Sr2CaCu2O8+z annealed under high pressures of oxygen	199406			Physica C, 226(1994)243-249	Masatsune Kato,Takashi Noji,Wataru Ito,Yoji Koike,Yoshitami Saito	Bi,Sr,Ca,Cu,O	
4684	PHC2260243		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.256	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.256		1994			emu.K/mole	0.045																								Bi2212																		K		67.2					67.2																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture-fire(800C,12H)-pellet-SIN(825C,24H in air)-FC-ANN(300-400,100H in 1-1080 atm O2) or (600C,24H in flowing N2)					Dependence of Tc on the excess oxygen content z in Bi2Sr2CaCu2O8+z annealed under high pressures of oxygen	199406			Physica C, 226(1994)243-249	Masatsune Kato,Takashi Noji,Wataru Ito,Yoji Koike,Yoshitami Saito	Bi,Sr,Ca,Cu,O	
4685	PHC2270254		Y2Ba4Cu7O14	Y2Ba4Cu7O15-z	Y	2	Ba	4	Cu	7															O	15-z			1994																											3	Y247			A	3.841	3.884	50.42												K		78.8				6.5	78.8		1	K/GPa	5																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(900C,48H at 2 MPa(for x=0), 24H at 0.8 MPa (for x=0.1,0.4,0.6) O2)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4686	PHC2270254		(Y,Pr)2Ba4Cu7O14	Y1.8Pr0.2Ba4Cu7O15-z	Y	1.8	Pr	0.2	Ba	4	Cu	7													O	15-z			1994																											3	Y247			A	3.839	3.877	50.5												K		64.3				13	64.3		1	K/GPa	3.5																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(900C,48H at 2 MPa(for x=0), 24H at 0.8 MPa (for x=0.1,0.4,0.6) O2)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4687	PHC2270254		(Y,Pr)2Ba4Cu7O14	Y1.2Pr0.8Ba4Cu7O15-z	Y	1.2	Pr	0.8	Ba	4	Cu	7													O	15-z			1994																											3	Y247			A	3.855	3.886	50.57												K		54				9.3	54		1	K/GPa	-1.8																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(900C,48H at 2 MPa(for x=0), 24H at 0.8 MPa (for x=0.1,0.4,0.6) O2)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4688	PHC2270254		(Y,Pr)2Ba4Cu7O14	Y0.8Pr1.2Ba4Cu7O15-z	Y	0.8	Pr	1.2	Ba	4	Cu	7													O	15-z			1994																											3	Y247			A	3.861	3.893	50.6												K		40				13	40		1	K/GPa	-15																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(900C,48H at 2 MPa(for x=0), 24H at 0.8 MPa (for x=0.1,0.4,0.6) O2)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4689	PHC2270237	Cl occupies both at apical and interstitial sites	(La,Sr)2Cu(O,Cl)4	La1.935Sr0.065Cu1Cl0.05O4-z	La	1.935	Sr	0.065	Cu	1	Cl	0.05													O	4-z		1	1994																												T																		K		14					14																																																																							m.ohm.cm											11.8												LaOCl,Cu,SrCO3,La2O3	1	sintered sample					Chlorination effects in electrical transport properties of ceramic La2-xSrxCuO4-z-yCly	199407			Physica C, 227(1994)237-244	C.Acha,F.de la Cruz,G.Leyva,G.Polla,L.Urba,M.A.R.de Benyacar,P.Levy,V.Bekeris	La,Sr,Cu,O,Cl	
4690	PHC2270237		(La,Sr)2Cu(O,Cl)4	La1.9Sr0.1Cu1Cl0.1O3.9-z	La	1.9	Sr	0.1	Cu	1	Cl	0.1													O	3.9-z		1	1994																												T																		K		21					21																																																																							m.ohm.cm											8.2												LaOCl,Cu,SrCO3,La2O3	1	sintered sample					Chlorination effects in electrical transport properties of ceramic La2-xSrxCuO4-z-yCly	199407			Physica C, 227(1994)237-244	C.Acha,F.de la Cruz,G.Leyva,G.Polla,L.Urba,M.A.R.de Benyacar,P.Levy,V.Bekeris	La,Sr,Cu,O,Cl	
4691	PHC2270237	R is not zero at Tc	(La,Sr)2Cu(O,Cl)4	La1.8Sr0.2Cu1Cl0.2O3.8-z	La	1.8	Sr	0.2	Cu	1	Cl	0.2													O	3.8-z		1	1994																												T																		K		32					32																																																																							m.ohm.cm											2.73												LaOCl,Cu,SrCO3,La2O3	1	sintered sample					Chlorination effects in electrical transport properties of ceramic La2-xSrxCuO4-z-yCly	199407			Physica C, 227(1994)237-244	C.Acha,F.de la Cruz,G.Leyva,G.Polla,L.Urba,M.A.R.de Benyacar,P.Levy,V.Bekeris	La,Sr,Cu,O,Cl	
4692	PHC2200265		Bi2Sr2(Y,Ce)2Cu2O10	Bi2Sr2Y1.65Ce0.35Cu2O10+z	Bi	2	Sr	2	Y	1.65	Ce	0.35	Cu	2											O	10+z		1	1994																											2	Bi2222			A	3.819		17.831												K		17.9					17.9																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4693	PHC2200265		(Bi,Pb)2Sr2(Y,Ce)2Cu2O10	Bi1.8Pb0.2Sr2Y1.65Ce0.35Cu2O10+z	Bi	1.8	Pb	0.2	Sr	2	Y	1.65	Ce	0.35	Cu	2									O	10+z		1	1994																											2	Bi2222			A	3.816		17.812												K		20					20																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4694	PHC2200265		(Bi,Pb)2Sr2(Y,Ce)2Cu2O10	Bi1.6Pb0.4Sr2Y1.65Ce0.35Cu2O10+z	Bi	1.6	Pb	0.4	Sr	2	Y	1.65	Ce	0.35	Cu	2									O	10+z		1	1994																											2	Bi2222			A	3.821		17.811												K		21.4					21.4																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4695	PHC2200265		(Bi,Pb)2Sr2(Y,Ce)2Cu2O10	Bi1.4Pb0.6Sr2Y1.65Ce0.35Cu2O10+z	Bi	1.4	Pb	0.6	Sr	2	Y	1.65	Ce	0.35	Cu	2									O	10+z		1	1994																											2	Bi2222			A	3.809		17.861												K		23.5					23.5																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4696	PHC2200265		(Bi,Pb)2Sr2(Y,Ce)2Cu2O10	Bi1.2Pb0.8Sr2Y1.65Ce0.35Cu2O10+z	Bi	1.2	Pb	0.8	Sr	2	Y	1.65	Ce	0.35	Cu	2									O	10+z		1	1994																											2	Bi2222			A	3.813		17.881												K		27					27																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4697	PHC2200265		(Bi,Pb)2Sr2(Y,Ce)2Cu2O10	Bi1Pb1Sr2Y1.65Ce0.35Cu2O10+z	Bi	1	Pb	1	Sr	2	Y	1.65	Ce	0.35	Cu	2									O	10+z		1	1994																											2	Bi2222			A	3.813		17.827												K		25					25																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					Effect of lead addition to Bi-based 2222 superconducting cuprates Bi2-xPbxSr2(Y,Ce)2Cu2O10+z	199402			Physca C, 220(1994)265-270	A.P.B.Sinha,D.E.Morris,H.B.Liu,X.D.Chen,X.P.Jiang	Bi,Sr,Pb,Y,Ce,Cu,O	
4698	PHC1680079		Bi2Sr2(Pr,Ce)Cu2O10	Bi2Sr2Pr1.64Ce0.36Cu2O10.27	Bi	2	Sr	2	Pr	1.64	Ce	0.36	Cu	2											O	10+z	10.27	1	1990																											2	Bi2222			A	3.885		17.87												K					4.2																																																																																																Bi2O3,SrCO3,CeO2,CuO,R2O3	1	mixture-fire(800C,10H in air)-pellet-heat(900-990C,60H in air)-SIN(slightly below M.P.)-FC-ANN(500C,10H in 80 atm O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4699	PHC1680079		Bi2Sr2(Nd,Ce)2Cu2O10	Bi2Sr2Nd1.64Ce0.36Cu2O10.23	Bi	2	Sr	2	Nd	1.64	Ce	0.36	Cu	2											O	10+z	10.23	1	1990																											2	Bi2222			A	3.881		17.93												K		14					14																																																																																														Bi2O3,SrCO3,CeO2,CuO,R2O3	1	mixture-fire(800C,10H in air)-pellet-heat(900-990C,60H in air)-SIN(slightly below M.P.)-FC-ANN(500C,10H in 80 atm O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4700	PHC1680079		Bi2Sr2(Sm,Ce)2Cu2O10	Bi2Sr2Sm1.64Ce0.36Cu2O10.24	Bi	2	Sr	2	Sm	1.64	Ce	0.36	Cu	2											O	10+z	10.24	1	1990																											2	Bi2222			A	3.863		17.9												K		16					16																																																																																														Bi2O3,SrCO3,CeO2,CuO,R2O3	1	mixture-fire(800C,10H in air)-pellet-heat(900-990C,60H in air)-SIN(slightly below M.P.)-FC-ANN(500C,10H in 80 atm O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4701	PHC1680079		Bi2Sr2(Eu,Ce)2Cu2O10	Bi2Sr2Eu1.64Ce0.36Cu2O10.26	Bi	2	Sr	2	Eu	1.64	Ce	0.36	Cu	2											O	10+z	10.26	1	1990																											2	Bi2222			A	3.854		17.88												K		27					27																																																																																														Bi2O3,SrCO3,CeO2,CuO,R2O3	1	mixture-fire(800C,10H in air)-pellet-heat(900-990C,60H in air)-SIN(slightly below M.P.)-FC-ANN(500C,10H in 80 atm O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4702	PHC1680079		Bi2Sr2(Gd,Ce)2Cu2O10	Bi2Sr2Gd1.64Ce0.36Cu2O10.24	Bi	2	Sr	2	Gd	1.64	Ce	0.36	Cu	2											O	10+z	10.24	1	1990																											2	Bi2222			A	3.851		17.88												K		34					34										20																																																																																				Bi2O3,SrCO3,CeO2,CuO,R2O3	1	mixture-fire(800C,10H in air)-pellet-heat(900-990C,60H in air)-SIN(slightly below M.P.)-FC-ANN(500C,10H in 80 atm O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4703	PHC1680079		Bi2Sr2(Tb,Ce)2Cu2O10	Bi2Sr2Tb1.64Ce0.36Cu2O10.26	Bi	2	Sr	2	Tb	1.64	Ce	0.36	Cu	2											O	10+z	10.26	1	1990																											2	Bi2222			A	3.847		17.83												K					4.2																																																																																																Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4704	PHC1680079		Bi2Sr2(Dy,Ce)2Cu2O10	Bi2Sr2Dy1.64Ce0.36Cu2O10.26	Bi	2	Sr	2	Dy	1.64	Ce	0.36	Cu	2											O	10+z	10.26	1	1990																											2	Bi2222			A	3.844		17.87												K		27					27																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4705	PHC1680079		Bi2Sr2(Ho,Ce)2Cu2O10	Bi2Sr2Ho1.64Ce0.36Cu2O10.22	Bi	2	Sr	2	Ho	1.64	Ce	0.36	Cu	2											O	10+z	10.22	1	1990																											2	Bi2222			A	3.84		17.86												K		24					24																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4706	PHC1680079		Bi2Sr2(Y,Ce)2Cu2O10	Bi2Sr2Y1.64Ce0.36Cu2O10.22	Bi	2	Sr	2	Y	1.64	Ce	0.36	Cu	2											O	10+z	10.22	1	1990																											2	Bi2222			A	3.836		17.85												K		20					20																																																																																														Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4707	PHC1680079		Bi2Sr2(Er,Ce)2Cu2O10	Bi2Sr2Er1.64Ce0.36Cu2O10.21	Bi	2	Sr	2	Er	1.64	Ce	0.36	Cu	2											O	10+z	10.21	1	1990																											2	Bi2222			A	3.837		17.84												K					5																																																																																																Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4708	PHC1680079		Bi2Sr2(Tm,Ce)2Cu2O10	Bi2Sr2Tm1.64Ce0.36Cu2O10.2	Bi	2	Sr	2	Tm	1.64	Ce	0.36	Cu	2											O	10+z	10.2	1	1990																											2	Bi2222			A	3.827		17.84												K					5																																																																																																Bi2O3,PbO,SrCO3,CeO2,Y2O3,CuO	1	mixture-fire(750C,20H)-pellet-heat(900C,60H in air)-ANN(500C,10H in 100 bar O2)					EXTENDED FAMILY OF NEW Bi-2222 SUPERCONDUCTING CUPRATES Bi2Sr2(RE1-xCex)2Cu2O10+y9 RE=rare earth			Department of Physics, University of Tokyo, Bunkyo 113, Japan	Physica.C,168(1990)79-84	H. TAKAGI,J.B. TORRANCE,R. BEYERS,S. UCHIDA,T. ARIMA,Y. TOKURA		
4709	PHC2200187			La1.4Ba1.27Ca0.33Cu3Oz	La	1.4	Ba	1.27	Ca	0.33	Cu	3													O	z		1	1994																											2																			K		68					68																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4710	PHC2200187			La1.3Ba1.37Ca0.33Cu3Oz	La	1.3	Ba	1.37	Ca	0.33	Cu	3													O	z		1	1994																											2																			K		61					61																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4711	PHC2200187			La1.2Ba1.47Ca0.33Cu3Oz	La	1.2	Ba	1.47	Ca	0.33	Cu	3													O	z		1	1994																											2																			K		53					53																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4712	PHC2200187			La1.1Ba1.57Ca0.33Cu3Oz	La	1.1	Ba	1.57	Ca	0.33	Cu	3													O	z		1	1994																											2																			K		43					43																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4713	PHC2200187			La1.4Ba1.4Ca0.2Cu3Oz	La	1.4	Ba	1.4	Ca	0.2	Cu	3													O	z		1	1994																											2																			K		30					30																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4714	PHC2200187			La1.3Ba1.3Ca0.4Cu3Oz	La	1.3	Ba	1.3	Ca	0.4	Cu	3													O	z		1	1994																											2																			K		58					58																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4715	PHC2200187			La1Ba1.5Ca0.5Cu3Oz	La	1	Ba	1.5	Ca	0.5	Cu	3													O	z		1	1994																											2																			K		77					77																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4716	PHC2200187			La1.5Ba1Ca0.5Cu3Oz	La	1.5	Ba	1	Ca	0.5	Cu	3													O	z		1	1994																											2																			K		50					50																																																																																														La2O3,BaCO3,CaCO3,CuO	1	mixture-(900C,12H for decarbonate)-(900C)					Superconducting La1.5-xBa1.5+x-yCayCu3Oz solid solutions: I. Phase diagram,cation stoichiometry and Tc data	199402			Physica C, 220(1994)187-194	A.R.West,J.M.S.Skakle	La,Ba,Ca,Cu,O	
4717	PHC2230075	constant current=0.50mA,Cu-valence2.145	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1994																											3	T			A	5.336	5.421	13.164												K		41.2					41.2																																																																						TP4717																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4718	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.178	(La,Ba)2CuO4	La1.95Ba0.05Cu1O4	La	1.95	Ba	0.05	Cu	1															O	4		1	1994																											3	T			A	5.332	5.4	13.187												K		33.6					33.6																																																																						TP4718																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4719	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.171	(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4		1	1994																											2	T			A	5.361		13.258												K		31.1					31.1																																																																						TP4719																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4720	PHC2230075	constant current=0.25mA(oxize),Cu-valence=2.145	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		1	1994																											2	T			A	5.354		13.281												K		28.4					28.4																																																																						TP4720																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4721	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.155	(La,Ba)2CuO4	La1.855Ba0.145Cu1O4	La	1.855	Ba	0.145	Cu	1															O	4		1	1994																											2	T			A	5.354		13.289												K		30.3					30.3																																																																						TP4721																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4722	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.150	(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4		1	1994																											2	T			A	5.353		13.301												K		29.8					29.8																																																																						TP4722																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4723	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.190	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4		1	1994																											2	T			A	5.352		13.327												K		16.5					16.5																																																																						TP4723																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4724	PHC2230075	constant current=0.50mA(oxidize),Cu-valence=2.235	(La,Ba)2CuO4	La1.75Ba0.25Cu1O4	La	1.75	Ba	0.25	Cu	1															O	4		1	1994																											2	T			A	5.352		13.356												K					4.2																																																																								TP4724																								La2O3,Ba(NO3)2,CuO		mixture-CAL(1173K,12H in air)-SIN(1320K,24H)-oxidized electrochemically					Preparation, magnetization, Seebeck coefficient, and electrical resistivity of electrochemically oxidized La2-xBaxCuO4 (0=<x=<0.25)	199404			Physica C, 223(1994)75-82	Mitsuru Itoh,Shigeru Sakamoto,Tetsuro Nakamura,Yoshiyuki Inaguma,Yue-Jin Shan	La,Ba,Cu,O	
4725	SSC0870375		Na-N-C60	Na1N1C60	Na	1	N	1	C	60																			1993																											1	fullerene			A	14.204														K		14.7					14.7																																																																																																mixture of C60+NaN3-ESR quartz tube-evacuate-heat(370-390C,20 min)-heat(410C)-cool					NEW SUPERCONDUCTING SODIUM-NITROGEN-C60 THRNARY COMPOUND				SOLID STATE COMMUN.,87(1993)375	H.INOKUCHI,H.KITAGAWA,I.I.KHAIRULLIN,K.IMAEDA,K.YAKUSHI,M.NAGATA,N.MIZUTANI	C,NA,N	
4726	PR0473423		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1993																												Bi2212																		K		85.4					85.4																																														meV	50	6.8	1																																															single crystals were grown from CuO-rich melts-ANN(540C,18H in 12 atm O2)-(540C,2 weeks in 1 atm O2)					MEASUREMENT OF THE ENERGY GAP IN OXYGEN-ANNEALED BI2SR2CACU2O8+Z HIGH-TC SUPERCONDUCTORS BY TUNNELING SPECTROSCOPY	199302			PHYS.REV.B,47(1993)3423	CHARLES M.LIEBER,ZHE ZHANG	BI,SR,CA,CU,O	
4727	PR0478385		(Y,Ca)Ba2Cu3O7	Y0.985Ca0.015Ba2Cu3O6.98	Y	0.985	Ca	0.015	Ba	2	Cu	3													O	7-z	6.98	1	1993																												Y123																		K		89.9					89.9			K/GPa	-0.13																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4728	PR0478385		(Y,Ca)Ba2Cu3O7	Y0.97Ca0.03Ba2Cu3O6.97	Y	0.97	Ca	0.03	Ba	2	Cu	3													O	7-z	6.97	1	1993																												Y123																		K		86.7					86.7			K/GPa	-0.55																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4729	PR0478385		(Y,Ca)Ba2Cu3O7	Y0.94Ca0.06Ba2Cu3O6.97	Y	0.94	Ca	0.06	Ba	2	Cu	3													O	7-z	6.97	1	1993																												Y123																		K		83.4					83.4			K/GPa	-0.59																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4730	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O6.96	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.5					93.5			K/GPa																																																																																													see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4731	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.89La0.11Cu3O6.96	Y	1	Ba	1.89	La	0.11	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.6					93.6			K/GPa	1.64																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4732	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.88La0.12Cu3O6.96	Y	1	Ba	1.88	La	0.12	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.2					93.2			K/GPa	1.84																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4733	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.86La0.14Cu3O6.96	Y	1	Ba	1.86	La	0.14	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		91.9					91.9			K/GPa	2.1																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4734	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.96La0.04Cu3O6.96	Y	1	Ba	1.96	La	0.04	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.6					93.6																																																																																																see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4735	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3O6.96	Y	1	Ba	1.95	La	0.05	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.8					93.8																																																																																																see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4736	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.94La0.06Cu3O6.96	Y	1	Ba	1.94	La	0.06	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		94					94			K/GPa	0.37																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4737	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.92La0.08Cu3O6.96	Y	1	Ba	1.92	La	0.08	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		94					94			K/GPa	0.78																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4738	PR0478385		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-z	6.96	1	1993																												Y123																		K		91.3					91.3			K/GPa	0.471																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4739	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.99La0.01Cu3O6.96	Y	1	Ba	1.99	La	0.01	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		92.1					92.1																																																																																																see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4740	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.98La0.02Cu3O6.96	Y	1	Ba	1.98	La	0.02	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		92.6					92.6																																																																																																see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4741	PR0478385		Y(Ba,La)2Cu3O7	Y1Ba1.97La0.03Cu3O6.96	Y	1	Ba	1.97	La	0.03	Cu	3													O	7-z	6.96	1	1993																												Y123																		K		93.2					93.2			K/GPa	0.114																																																																																												see Appl.Phys.Lett.,61(1992)1852					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF YBA2CU3O7 AS A FUNCTION OF CARRIER CONCENTRATION: A TEST FOR A SIMPLE CHARGE-TRANSFER MODEL	199304			PHYS.REV.B,47(1993)8385	H.A.ZIMMERMANN,J.J.NEUMEIER	Y,BA,CU,O	
4742	PR0486569	LTT phase,LTO-LTT phase transition at 74K, dTc/dP=10 K/GPa at P=0.5GPa	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		1	1993																											2	T																		K		4					4			K/GPa																																																																																											La2O3,BaCO3,CuO	1	mixture-CAL(900C,24H)-SIN(1050C,several days in air)-ANN(500C,24H in flowing O2)					PRESSURE EFFECTS ON THE STRUCTURAL PHASE TRANSITIONS AND SUPERCONDUCTIVITY OF LA2-XBAXCUO4 (X=0.125)	199309			PHYS.REV.B,48(1993)6569	JAIME A.FERNANDEZ-BACA,NOBUO MORI,SATORU FUNAHASHI,SUSUMU KATANO,YUTAKA UEDA		
4743	PR0486569	LTO phase, HTT-LTO phase transition at 200K,	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		1	1993																											3	T																		K		30					30			K/GPa	8																																																																																										La2O3,BaCO3,CuO	1	mixture-CAL(900C,24H)-SIN(1050C,several days in air)-ANN(500C,24H in flowing O2)					PRESSURE EFFECTS ON THE STRUCTURAL PHASE TRANSITIONS AND SUPERCONDUCTIVITY OF LA2-XBAXCUO4 (X=0.125)	199309			PHYS.REV.B,48(1993)6569	JAIME A.FERNANDEZ-BACA,NOBUO MORI,SATORU FUNAHASHI,SUSUMU KATANO,YUTAKA UEDA		
4744	PR0486617	thickness=3000A	(Ba,K)BiO3	Ba0.55K0.45Bi1O3	Ba	0.55	K	0.45	Bi	1															O	3		4	1993																											1	BKBO																		K		22.5					22.5																					resistive transition	23							T/K		1					A	from Hc2	37								meV	3.45	3.8	1																						m.ohm.cm											0.58				-0.000000000245					RH4744				16	target=Ba:K:Bi=0.3:0.7:0.7,sputtered in 1%O2-Ar of 5-20 mTorr--ANN(450-500C,1H in flowing O2),substrate=(110) or (100)SrTiO3					SUPERCONDUCTING AND NORMAL STATES OF BA1-XKXBIO3 STUDIED WITHUSE OF HIGH-QUALITY THIN FILMS	199309			PHYS.REV.B,48(1993)6617	H.SATO,K.TANABE,K.TATSUHARA,M.YOSHIDA,N.MIURA,S.TAJIMA,S.UCHIDA,T.IDO		
4745	PR0486617		(Ba,K)BiO3	Ba0.55K0.45Bi1O3	Ba	0.55	K	0.45	Bi	1															O	3		4	1993																											1	BKBO																		K		20					20																													T/K		1.6																																								m.ohm.cm											1.1													16	target=Ba:K:Bi=0.3:0.7:0.7,sputtered in 1%O2-Ar of 5-20 mTorr--ANN(450-500C,1H in flowing O2),substrate=(110) or (100)SrTiO3					SUPERCONDUCTING AND NORMAL STATES OF BA1-XKXBIO3 STUDIED WITHUSE OF HIGH-QUALITY THIN FILMS	199309			PHYS.REV.B,48(1993)6617	H.SATO,K.TANABE,K.TATSUHARA,M.YOSHIDA,N.MIURA,S.TAJIMA,S.UCHIDA,T.IDO		
4746	PHC2270395	p-type superconductor	SrCuO2	Sr1Cu1O2	Sr	1	Cu	1																	O	2		1	1994																												IL																		K		91		91			91			K/GPa	2.1																																																																																												prepared by high pressure synthesis					Effect of pressure on Tc of hole- and electron-doped infinite-layer compounds up to 8GPa	199407			Physica C, 227(1994)395-398	H.Takahashi,M.Azuma,M.Takano,N.Mori,Z.Hiroi	Sr,Cu,O,Ca	
4747	PHC2270395	p-type superconductor	(Ca,Sr)CuO2	Ca0.285Sr0.665Cu1O2	Ca	0.285	Sr	0.665	Cu	1															O	2		1	1994																												IL																		K		110		110			110			K/GPa	1.2																																																																																												prepared by high pressure synthesis					Effect of pressure on Tc of hole- and electron-doped infinite-layer compounds up to 8GPa	199407			Physica C, 227(1994)395-398	H.Takahashi,M.Azuma,M.Takano,N.Mori,Z.Hiroi	Sr,Cu,O,Ca	
4748	PHC2270395	n-type superconductor, dTc/dP=0 K/GPa	(Sr,Sm)CuO2	Sr0.92Sm0.08Cu1O2	Sr	0.92	Sm	0.08	Cu	1															O	2		1	1994																												IL																		K		43		43			43			K/GPa																																																																																													prepared by high pressure synthesis					Effect of pressure on Tc of hole- and electron-doped infinite-layer compounds up to 8GPa	199407			Physica C, 227(1994)395-398	H.Takahashi,M.Azuma,M.Takano,N.Mori,Z.Hiroi	Sr,Cu,O,Ca	
4749	PHC2270254		Y2Ba4Cu7O15	Y2Ba4Cu7O15-z	Y	2	Ba	4	Cu	7															O	15-z		1	1994																											3	Y247			A	3.841	3.884	50.42												K		78.8				6.5	78.8			K/GPa	5																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(990C,24H under 2MPa O2 for non-doped, 0.8MPa O2 for doped sample)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4750	PHC2270254		(Y,Pr)2Ba4Cu7O15	Y1.8Pr0.2Ba4Cu7O15-z	Y	1.8	Pr	0.2	Ba	4	Cu	7													O	15-z		1	1994																											3	Y247			A	3.839	3.877	50.5												K		64.3				13	64.3			K/GPa	3.5																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(990C,24H under 2MPa O2 for non-doped, 0.8MPa O2 for doped sample)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4751	PHC2270254		(Y,Pr)2Ba4Cu7O15	Y1.2Pr0.8Ba4Cu7O15-z	Y	1.2	Pr	0.8	Ba	4	Cu	7													O	15-z		1	1994																											3	Y247			A	3.855	3.866	50.57												K		54				9.3	54			K/GPa	-1.8																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(990C,24H under 2MPa O2 for non-doped, 0.8MPa O2 for doped sample)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4752	PHC2270254		(Y,Pr)2Ba4Cu7O15	Y1.2Pr0.8Ba4Cu7O15-z	Y	1.2	Pr	0.8	Ba	4	Cu	7													O	15-z		1	1994																											3	Y247			A	3.861	3.893	50.6												K		40				13	40			K/GPa	-15																																																																																										Y2O3,BaCO3,CuO,Pr2O3	1	mixture-CAL(900C,12H in flowing O2)-SIN(990C,24H under 2MPa O2 for non-doped, 0.8MPa O2 for doped sample)					Pressure effects on the electrical resistivities of (Y1-xPrx)2Ba4Cu7O15-z with x=0,0.1,0.4 and 0.6	199407			Physica C, 227(1994)254-258	A.Matsushita,I.Hirabayashi,K.Kawamoto,M.Otsuki,N.Yamada,S.Horii,S.Takashima,T.Matsumoto,T.Yamanishi,Y.Kodama,Y.Yamada	Y,Pr,Ba,Cu,O	
4753	PHC1810206	single phase obtained for x<0.15	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	1991																											2	IL			A	3.946		3.412												K		43		43			43										30																																																																																				SrCO3,La2O3,CuO	1	mixture-fire(950C,30-48H)-react(950-1000C,1-2H under the pressure of 3-5 GPa					SUPERCONDUCTIVITY IN THE INFINITE-LAYER COMOPOUND SR1-XLAX CUO2 PREPARED UNDER HIGH PRESSURE			INSTITUTE OF SCIENTIFIC AND INDUSTRIAL RESEARCH,OSAKA UNIVERSITY,OSAKA 567,JAPAN	PHYSICA C,181(1991)206	F.KANAMARU,G.ER,S.KIKKAWA,Y.MIUAMOTO	SR,LA,CU,O	
4754	PHC2280401		(Bi,Sr)2(Sr,La)2CuO6	Bi1.95Sr1.65La0.4Cu1O6+z	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	6+z		3	1994																												Bi2201																		K		15		15			15																				T	magnetization			8.2					T/K				0.52			A			63		A			10000																																																			7	CuO-rich sample-furnace-heat upto 1100C at 150C/H-(1100C,10H)-cool to 850C at 2C/H-(850C,3H)-FC, heating cycle in air-ANN(660C,15H in air)					Magnetization of superconducting Bi1.95Sr1.65La0.4CuO6+z single crystals near Tc	199407			Physica C,228 (1994) 401-407	A.Schilling,H.R.Ott,R.Jin		
4755	PHC2280323		(Tl,Pb)Sr2CaCu2O7	Tl0.5Pb0.5Sr2Ca1Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2											O	7		3	1994																											2	Tl1212	P4/mmm		A	3.799		12.109												K		82		82			82											Oe				250					T				89					T/K				1.71			A			19.2		A			1739																																																			1	precursor=mixture of CuO,CaO,SrCO3-addition of Tl2O3, PbO-(750C,6H)-(1050C,1H)-cool to RT(0.1C/min)					Magnetic properties of a Tl0.5Pb0.5Sr2CaCu2O7 single crystal	199407			Physica C,228 (1994) 323-330	A.Maignan,C.Martin,Ch,Simom,V,Hardy		
4756	PHC2260184	impurity phase=CaHgO2,CaTlOz	(Hg,Tl)2Ba2CaCu2O8	Hg0.67Tl1.33Ba2Ca1Cu2O8+z	Hg	0.67	Tl	1.33	Ba	2	Ca	1	Cu	2											O	8+z			1994																											2	Tl2212			A	3.854		29.385												K			100				100																																																																																														BaO2,Ca(NO3)2.4H2O,Cu(NO3)2.3H2O	1	powder-dry(150C,12H)-pellet-heat(925C,14H in flowing O2)=precursor +HgO+Tl2O3-react					(Hg2/3Tl4/3)Ba2CaCu2 O8+z, a 2212 type superconductor	199406			Physica C,226 (1994)184-187	I.Bryntse		
4757	PHC2260147		(La,Sr)2CuO4H	La1.9Sr0.1Cu1H0.1O4	La	1.9	Sr	0.1	Cu	1	H	0.1													O	4			1994																												T																		K		28.9					28.9																																																																																															1	pure H2 gas was admitted into the cell under pressure upto 600 Torr , adsorption was carried out at 180C					Effect of hydrogen on the transition temperature in La2-x Srx Cu O4 high-Tc superconductors from underdoped to overdoped regimes	199406			Physica C,226 (1994) 147-152	A.D.Shengelaya,A.Zygmunt,H.Drulis,J.Klamut,N.M.Sulemanov		
4758	PHC2260147		(La,Sr)2CuO4H0.1	La1.85Sr0.15Cu1H0.1O4	La	1.85	Sr	0.15	Cu	1	H	0.1													O	4			1994																												T																		K		35.4					35.4																																																																																															1	pure H2 gas was admitted into the cell under pressure upto 600 Torr , adsorption was carried out at 180C					Effect of hydrogen on the transition temperature in La2-x Srx Cu O4 high-Tc superconductors from underdoped to overdoped regimes	199406			Physica C,226 (1994) 147-152	A.D.Shengelaya,A.Zygmunt,H.Drulis,J.Klamut,N.M.Sulemanov		
4759	PHC2260147		(La,Sr)2CuO4H0.1	La1.8Sr0.2Cu1H0.1O4	La	1.8	Sr	0.2	Cu	1	H	0.1													O	4			1994																												T																		K		35.5					35.5																																																																																															1	pure H2 gas was admitted into the cell under pressure upto 600 Torr , adsorption was carried out at 180C					Effect of hydrogen on the transition temperature in La2-x Srx Cu O4 high-Tc superconductors from underdoped to overdoped regimes	199406			Physica C,226 (1994) 147-152	A.D.Shengelaya,A.Zygmunt,H.Drulis,J.Klamut,N.M.Sulemanov		
4760	PHC2260147		(La,Sr)2CuO4H0.1	La1.75Sr0.25Cu1H0.1O4	La	1.75	Sr	0.25	Cu	1	H	0.1													O	4			1994																												T																		K		26.8					26.8																																																																																															1	pure H2 gas was admitted into the cell under pressure upto 600 Torr , adsorption was carried out at 180C					Effect of hydrogen on the transition temperature in La2-x Srx Cu O4 high-Tc superconductors from underdoped to overdoped regimes	199406			Physica C,226 (1994) 147-152	A.D.Shengelaya,A.Zygmunt,H.Drulis,J.Klamut,N.M.Sulemanov		
4761	PHC2260121	narrow gap semiconductor	(Cd,Ce)Sr2(Y,Ce,Sr)Cu2Oz	Cd0.844Ce0.832Sr2.076Y1.248Cu2Oz	Cd	0.844	Ce	0.832	Sr	2.076	Y	1.248	Cu	2											O	z			1994																											2	Pb1212			A	3.801		29.31												K					4																																																																																																SrCO3,CeO2,CuO,CdO,Y2O3 or Nd2O3	1	nominal compositions are CdSr2Y1.2Ce0.8Cu2Oz or CdSr2Nd1.1Ce0.9Cu2Oz, compositions were measured by ICP					A new type of layered cuprates with 1222 structure.(CdCe)Sr2(LnCeSr)2 Cu2 Oy (Ln=Nd, Y)	199406			Physica C, 226 (1994) 121-124	Chen Zuyao,Qian Yitai,Tang Kaibin,Wang Shizhong,Yang Peidong,Yu weichao,Zhou Guien		
4762	PHC2260121	narrow gap semiconductor	(Cd,Ce)Sr2(Nd,Ce,Sr)Cu2Oz	Cd0.797Ce0.946Sr2.101Nd1.156Cu2Oz	Cd	0.797	Ce	0.946	Sr	2.101	Nd	1.156	Cu	2											O	z			1994																											2	Pb1212			A	3.844		29.38												K					4																																																																																																SrCO3,CeO2,CuO,CdO,Y2O3 or Nd2O3	1	nominal compositions are CdSr2Y1.2Ce0.8Cu2Oz or CdSr2Nd1.1Ce0.9Cu2Oz, compositions were measured by ICP					A new type of layered cuprates with 1222 structure.(CdCe)Sr2(LnCeSr)2 Cu2 Oy (Ln=Nd, Y)	199406			Physica C, 226 (1994) 121-124	Chen Zuyao,Qian Yitai,Tang Kaibin,Wang Shizhong,Yang Peidong,Yu weichao,Zhou Guien		
4763	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.224	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	z	7.224	1	1994																											2	Y123			A	3.811		11.459												K	33	35					35																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in Al2O3)-pellet-SIN(1000C,5H in air)-ANN(300-700,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4764	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.152	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	z	7.152	1	1994																											2	Y123			A	3.816		11.483												K	9	23					23																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in Al2O3)-pellet-SIN(1000C,5H in air)-ANN(300-700,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4765	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.144	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	z	7.144	1	1994																											2	Y123			A	3.815		11.477												K		12					12																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in Al2O3)-pellet-SIN(1000C,5H in air)-ANN(300-700,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4766	PHC2260037	semiconductor,ferromagnetic	YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.123	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	z	7.123	1	1994																											2	Y123			A	3.81		11.465												K					4																																																																																																Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in Al2O3)-pellet-SIN(1000C,5H in air)-ANN(300-700,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4767	PHC2260037	semiconductor,ferromagnetic	YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.098	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	z	7.098	1	1994																											2	Y123			A	3.808		11.459												K					4																																																																																																Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in Al2O3)-pellet-SIN(1000C,5H in air)-ANN(300-700,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4768	PHC2190123	R=not zero at 4.2K	SrCuO2	Sr1Cu1O2	Sr	1	Cu	1																	O	2			1994																											2	IL			A	3.935		3.436												K					4.2																																																																																																SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4769	PHC2190123	R=not zero at 4.2K	(Sr,Y)CuO2	Sr0.95Y0.05Cu1O2	Sr	0.95	Y	0.05	Cu	1															O	2			1994																											2	IL			A	3.937		3.431												K			38.6				38.6										1																																																																																				SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4770	PHC2190123	R=not zero at 4.2K	(Sr,Y)CuO2	Sr0.9Y0.1Cu1O2	Sr	0.9	Y	0.1	Cu	1															O	2			1994																											2	IL			A	3.933		3.424												K			36.6				36.6																																																																																														SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4771	PHC2190123	R=not zero at 4.2K	(Sr,Y)CuO2	Sr0.85Y0.15Cu1O2	Sr	0.85	Y	0.15	Cu	1															O	2			1994																											2	IL			A	3.933		3.426												K			36.6				36.6																																																																																														SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4772	PHC2190123	R=not zero at 4.2K	(Sr,Y)CuO2	Sr0.8Y0.2Cu1O2	Sr	0.8	Y	0.2	Cu	1															O	2			1994																											2	IL			A	3.936		3.43												K			38.6				38.6																																																																																														SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4773	PHC2190123	impurity phase included, R=not zero at 4.2K	(Sr,Y)CuO2	Sr0.75Y0.25Cu1O2	Sr	0.75	Y	0.25	Cu	1															O	2			1994																											2	IL			A	3.936		3.424												K			38.6				38.6																																																																																														SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4774	PHC2190123	impurity phase included , R=not ero at 4.2K	(Sr,Y)CuO2	Sr0.7Y0.3Cu1O2	Sr	0.7	Y	0.3	Cu	1															O	2			1994																											2	IL			A	3.928		3.424												K			32.6				32.6										0.1																																																																																				SrCO3,CuO,Y2O3	1	mixture-CAL(960C,48H)-pellet-wrapped with Ag or Au foil-compress-heat(850-1000C,45min at 3.5GPa)					Superconductivity in the (Sr1-xYx)CuO2 (x=0.00-0.30) system synthesized under high pressure				Physica C, 219(1994)123-128	Cheng Dong,Jingwei Li,Shunlian Jia,Xingjiang Zhou,Yushu Yao,Zhongxian Zhao		
4775	PHC2020199		Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z			1992																											2	Tl2201			A	3.861		23.117			/K				/GPa	-0.004		-0.003	dL/dT=(1/L)(dL/dT),dL/dP=(1/L)(dL/dP)	K					4.2																																																																																																	1	ANN(in O2)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4776	PHC2020199		Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z			1992																											2	Tl2201			A	3.864		23.201			/K				/GPa					K		78					78																																																																																															1	ANN(550C,5H in Ar)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4777	PHC2020199		Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z			1992																											3	Tl2201			A	5.498	5.44	23.148			/K									K					4.2																																																																																																	1	ANN(in O2)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4778	PHC2020199		Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z			1992																											3	Tl2201			A	5.489	5.46	23.209			/K									K		83					83																																																																																															1	ANN(550C,5H in Ar)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4779	PHC2020199		TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7	Tl	1	Sr	2	Ca	1	Cu	2													O	7			1992																											2	Tl1212			A	3.786		12.115			/K								dL/dT=(1/L)(dL/dT)	K					4.2																																																																																																	1	ANN(in O2)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4780	PHC2020199		TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7	Tl	1	Sr	2	Ca	1	Cu	2													O	7			1992																											2	Tl1212			A	3.796		12.122			/K									K		73					73																																																																																															1	ANN(550C,5H in Ar)					LOW-TEMPERATURE CRYSTAL STRUCTURES OF TL2BA2CUO6-Z AND TLSR2CACU2O7-Z	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYSICA C,202(1992)199	YUICHI SHIMAKAWA	TL,BA,CU,O,SR,CA	
4781	PHC2130051		(Bi,Pb)2Sr6Cu2(CO3)Oz	Bi1.6Pb0.4Sr4Cu2C1O11	Bi	1.6	Pb	0.4	Sr	4	Cu	2	C	1											O	11		1	1993																											2				A	3.821		39.444	1											K	31		40	41		9	41										23																																																													m.ohm.cm				0.8							1.4												Bi2O3,PbO,SrCO3,CuO	1	SIN(850C,20H in flowing gas mixture of 92%Ar+7.5%O2+0.5%CO2)-Q				an excess amount of CO3 in raw materials was dissociated during sintering	SUPERCONDUCTIVITIES IN THE (BI,PB)-OXYCARBONATE SYSTEM	199308			PHYSICA C,213(1993)51	H.NAKATA,J.AKIMITSU,M.UEHARA,T.DEN,T.KOBAYASHI,Y.MATSUI	BI,PB,SR,CU,C,O	
4782	PHC2130051	metastable phase	(Bi,Pb)2Sr6Cu3(CO3)2O10	Bi1.6Pb0.4Sr6Cu3C2O16	Bi	1.6	Pb	0.4	Sr	6	Cu	3	C	2											O	16		2	1993																											2				A	3.88		54.52	1											K			55	54			54																																																																							m.ohm.cm				4.8							4.3												Bi2O3,PbO,SrCO3,CuO	1	SIN(870C,20H in flowing gas mixture of 79%Ar+20%O2+1%CO2)-Q					SUPERCONDUCTIVITIES IN THE (BI,PB)-OXYCARBONATE SYSTEM	199308			PHYSICA C,213(1993)51	H.NAKATA,J.AKIMITSU,M.UEHARA,T.DEN,T.KOBAYASHI,Y.MATSUI	BI,PB,SR,CU,C,O	
4783	PHC2160453		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.85B0.15O5	Sr	2	Cu	1	C	0.85	B	0.15													O	5		1	1993																											2				A	7.788		14.968	1											K	26		35	32		9	32										10																																																													m.ohm.cm				80							100												SrCO3,CuO,H3BO3	1	CAL(750C,20H in air)-SIN(900C,20H in flowing gas mixture of 98%O2+2%CO3-Q					SUPERCONDUCTIVITY IN THE NEW COMPOUND SR2CUO2(CO3)1-X(BO3)X	199311			PHYSICA C,216(1993)453	H.NAKATA,J.AKIMITSU,M.UEHARA	SR,CU,O,C,B	
4784	PHC2290310	mainly single phase	Sr2(Ca,Sr)Cu2(CO3)1-x(BO3)xOz	Sr15.9Ca7.6Cu17.6C3.3B2.6O53	Sr	15.9	Ca	7.6	Cu	17.6	C	3.3	B	2.6											O	53		1	1994																											2	M1212			A	3.86		10.62	1										(B,C)1212	K	90		105	105		15	105										20																																																													m.ohm.cm											280												Sr2CuO2(CO3),Sr2CuO3,Ca2CuO3,CuO,B2O3	1	SIN(1050-1150C,0.5-1H,  under 5GPa with KClO4 as oxidizer					A new homologous series of oxycarbonate superconductors Sr2(Ca,Sr)n-1Cun(CO3)1-x(BO3)xOy (n=1,2 and 3)	199408			Physica C, 229(1994)310-314	H.Nakata,J.Akimitsu,M.Uehara,M.Uoshima,N.Mori,S.Ishiyama,T.Arima,Y.Matsui,Y.Tokura	Sr,Ca,Cu,C,O,B	
4785	PHC2290310	mainly single phase	Sr2(Ca,Sr)2Cu3(CO3)1-x(BO3)xOz	Sr16.7Ca7.7Cu19.4C1.9B2.9O51.7	Sr	16.7	Ca	7.7	Cu	19.4	C	1.9	B	2.9											O	51.7		1	1994																											2	M1223			A	3.87		13.98	1										(B,C)1223	K	105		115	115		10	115										40																																																													m.ohm.cm											6.4												Sr2CuO2(CO3),Sr2CuO3,Ca2CuO3,CuO,B2O3	1	SIN(1050-1150C,0.5-1H,  under 5GPa with KClO4 as oxidizer					A new homologous series of oxycarbonate superconductors Sr2(Ca,Sr)n-1Cun(CO3)1-x(BO3)xOy (n=1,2 and 3)	199408			Physica C, 229(1994)310-314	H.Nakata,J.Akimitsu,M.Uehara,M.Uoshima,N.Mori,S.Ishiyama,T.Arima,Y.Matsui,Y.Tokura	Sr,Ca,Cu,C,O,B	
4786	PHC2260311	ABRES minimum at 50K,CRES minimum at 56K, Tc(in CRES)=19.4K	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	1994																												T'																		K		20.9					20.9																																																																							m.ohm.cm												4	3200											5	single crystal grown by self-flux method, then ANN(900C,12H in Ar)-FC to RT					Anisotropic low-temperature magnetoresistivity in the normal state of L2-xCexCuO4 single crystals	199406			Physica C, 226(1994)311-319	J.Fontcuberta,M.A.Crusellas,S.Pinol	Pr,Sm,Nd,Ce,Cu,O	
4787	PHC2260311	ABRES minimum at 33K,CRES minimum at 43K, Tc(in CRES)=17.3K	(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4		3	1994																												T'																		K		21.9					21.9																																																																							m.ohm.cm												4.9	2600											5	single crystal grown by self-flux method, then ANN(900C,12H in Ar)-FC to RT					Anisotropic low-temperature magnetoresistivity in the normal state of L2-xCexCuO4 single crystals	199406			Physica C, 226(1994)311-319	J.Fontcuberta,M.A.Crusellas,S.Pinol	Pr,Sm,Nd,Ce,Cu,O	
4788	PHC2260311	ABRES minimum at 43K, CRES minimum at 14.5K, Tc(in CRES)=26.1K	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1994																												T'																		K		26.4					26.4																																																																							m.ohm.cm												6.6	1350											5	single crystal grown by self-flux method, then ANN(900C,12H in Ar)-FC to RT					Anisotropic low-temperature magnetoresistivity in the normal state of L2-xCexCuO4 single crystals	199406			Physica C, 226(1994)311-319	J.Fontcuberta,M.A.Crusellas,S.Pinol	Pr,Sm,Nd,Ce,Cu,O	
4789	PHC2260311	ABRES minimum at 33K, CRES minimum at 38K, Tc(in CRES)=24.5K	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1994																												T'																		K		22					22																																																																							m.ohm.cm												0.6	4600											5	single crystal grown by self-flux method, then ANN(900C,12H in Ar)-FC to RT					Anisotropic low-temperature magnetoresistivity in the normal state of L2-xCexCuO4 single crystals	199406			Physica C, 226(1994)311-319	J.Fontcuberta,M.A.Crusellas,S.Pinol	Pr,Sm,Nd,Ce,Cu,O	
4790	PHC2260235	impurity phase =<1%,aligned under H=1T,KAIZERO=6.8e-7 emu/g for perpendicular field, G-L parameter=97 for // field and =63 for normal	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	1994	emu/g																											IL																		K		40.7					40.7											Oe			42	59					T	magnetization measurement and calculation using GLAG theory		23.8	15.5					T/K			0.85	0.55			A	GLAG theory		46	30	A			2900	4500																																																	SrCO3,La2O3,CuO	1	mixture-SIN(900C,7days in air)-pellet-sealed in Pt crucible-press to 25kbar-SIN(1045C,2H)-Q to RT					Reversible magnetization measurements of the anisotropic superconducting parameters of the infinite-layer electron-doped compound Sr0.9La0.1CuO2: Apparent anisotropy crossover	199406			Physica C, 226(1994)235-242	J.L.Cobb,J.T.Markert	Sr,La,Cu,O	
4791	PHC2260235	impurity phase=<1%,aligned under H=1T	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	1994																												IL																		K		40.6					40.6														69	95					T	magnetization and calculation using GLAG theory		8.6	13.4					T/K			0.31	0.48			A			50	77	A			2630	1700																																																	SrCO3,La2O3,CuO	1	mixture-SIN(900C,7days in air)-pellet-sealed in Pt crucible-press to 25kbar-SIN(1045C,2H)-Q to RT					Reversible magnetization measurements of the anisotropic superconducting parameters of the infinite-layer electron-doped compound Sr0.9La0.1CuO2: Apparent anisotropy crossover	199406			Physica C, 226(1994)235-242	J.L.Cobb,J.T.Markert	Sr,La,Cu,O	
4792	PHC2260235	impurity phase=<1%,aligned under H=1T	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	1994																												IL																		K		40.8					40.8											Oe			40	79					T	magnetization and calculation using GLAG theory		33.8	13.9					T/K			1.2	0.49			A			49	20	A			2440	5900																																																	SrCO3,La2O3,CuO	1	mixture-SIN(900C,7days in air)-pellet-sealed in Pt crucible-press to 25kbar-SIN(1045C,2H)-Q to RT					Reversible magnetization measurements of the anisotropic superconducting parameters of the infinite-layer electron-doped compound Sr0.9La0.1CuO2: Apparent anisotropy crossover	199406			Physica C, 226(1994)235-242	J.L.Cobb,J.T.Markert	Sr,La,Cu,O	
4793	PHC2260222	Hirr is determined as Jc=1e+3 A/cm2	(Cu,C)Ba2Ca2Cu3O9	C0.5Ba2Ca2Cu3.5O9+z	C	0.5	Ba	2	Ca	2	Cu	3.5													O	9+z			1994																												Cu1223																		K		67					67																					magnetization													HIR4793																																																														heat treatment under the pressure of 5GPa at 1200C					Critical current densities and irreversibility lines of new oxycarbonate superconductors (Cu0.5C0.5)Ba2Can-1CunO2n+3 (n=3,4)	199406			Physica C, 226(1994)222-226	E.Takayama-Muromachi,H.Kumakura,K.Togano,T.Kawashima	Cu,C,Ba,Ca,Cu,O	
4794	PHC2260222	Hirr is determined as Jc=1e+3 A/cm2	(Cu,C)Ba2Ca3Cu4O11	C0.5Ba2Ca3Cu4.5O11+z	C	0.5	Ba	2	Ca	3	Cu	4.5													O	11+z			1994																												Cu1234																		K		117					117																					magnetization													HIR4794																																																														heat treatment under the pressure of 5GPa at 1200C					Critical current densities and irreversibility lines of new oxycarbonate superconductors (Cu0.5C0.5)Ba2Can-1CunO2n+3 (n=3,4)	199406			Physica C, 226(1994)222-226	E.Takayama-Muromachi,H.Kumakura,K.Togano,T.Kawashima	Cu,C,Ba,Ca,Cu,O	
4795	PHC2260353		(La,Rb)2CuO4	La1.945Rb0.055Cu1O4	La	1.945	Rb	0.055	Cu	1															O	4		3	1994									7.051																		2	T	I4/mmm		A	3.786		13.276												K		22		22			22																																																																																																(mixture of CuO,La2O3)+RbOH-in Al2O3 crucible-heat(400C,24H)-cool to RT at 150C/H					Synthesis, single-crystal structure, and superconductivity of the rubidium-substituted La2CuO4	199406			Physica C, 226(1994)353-359	D.G.Hinks,J.M.Williams,P.M.Keane,U.Geiser	La,Cu,O,Rb	
4796	PHC2260353		(La,K)2CuO4	La1.935K0.065Cu1O4	La	1.935	K	0.065	Cu	1															O	4		3	1994																											2	T																		K		20		20			20										50																																																																																						(mixture of CuO,La2O3)+RbOH-in Al2O3 crucible-heat(400C,24H)-cool to RT at 150C/H					Synthesis, single-crystal structure, and superconductivity of the rubidium-substituted La2CuO4	199406			Physica C, 226(1994)353-359	D.G.Hinks,J.M.Williams,P.M.Keane,U.Geiser	La,Cu,O,Rb	
4797	PHC2260353		(La,Na)2CuO4	La1.929Na0.071Cu1O4	La	1.929	Na	0.071	Cu	1															O	4		3	1994																											2	T																		K		28		28			28										55																																																																																						(mixture of CuO,La2O3)+RbOH-in Al2O3 crucible-heat(400C,24H)-cool to RT at 150C/H					Synthesis, single-crystal structure, and superconductivity of the rubidium-substituted La2CuO4	199406			Physica C, 226(1994)353-359	D.G.Hinks,J.M.Williams,P.M.Keane,U.Geiser	La,Cu,O,Rb	
4798	PHC2300184	after annealing as-grown sample in flowing O2 at 400C, 24H	(Ba,K)BiO3	Ba0.62K0.38Bi1O3	Ba	0.62	K	0.38	Bi	1															O	3		1	1994																											1	BKBO																																																																																											micro.V/K	-0.44			TP4798																										sample obtained by a low temperature anodic electrocrystalization method in a potassium hydroxide molten flux					Thermoelectric power of superconducting Ba-K-Bi-O crystals	199409			Physica C, 230(1994)184-188	A.B.Kaiser,C.K.Subramanian,H.Y.Tang	Ba,K,Bi,O	
4799	PHC2300031	single crystal=0.5*0.3*0.2mm3	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1994																											3	Y123																		K		87		87			87																																																																																															5	flux is BaCO3+CuO-(mixture+Co3O4)-(980C,15-20H in air using Au-crucible)-cool to 930C at 1C/H and to 870C at 2C/H-FC-oxidize					Structural deformation in oxidized and reduced YBa2(Cu1-yCoy)3O6+z compounds (0<y=<0.05)	199409			Physica C, 230(1994)31-41	E.Elkaim,H.Renevier,J.L.Hodeau,M.Bessiere,M.Marezio,S.Lefebvre	Y,Ba,Cu,Co,O	
4800	PHC2300031	single crystal=0.7*0.8*0.1mm3	YBa2(Cu,Co)3O7	Y1Ba2Cu2.949Co0.051O7-z	Y	1	Ba	2	Cu	2.949	Co	0.051													O	7-z		3	1994																											3	Y123																		K		81		81			81																																																																																															5	flux is BaCO3+CuO-(mixture+Co3O4)-(980C,15-20H in air using Au-crucible)-cool to 930C at 1C/H and to 870C at 2C/H-FC-oxidize					Structural deformation in oxidized and reduced YBa2(Cu1-yCoy)3O6+z compounds (0<y=<0.05)	199409			Physica C, 230(1994)31-41	E.Elkaim,H.Renevier,J.L.Hodeau,M.Bessiere,M.Marezio,S.Lefebvre	Y,Ba,Cu,Co,O	
4801	PHC2300031	single crystal=0.5*0.5*0.2mm3	YBa2(Cu,Co)3O7	Y1Ba2Cu2.871Co0.129O7-z	Y	1	Ba	2	Cu	2.871	Co	0.129													O	7-z		3	1994																											2	Y123																		K		68		68			68																																																																																															5	flux is BaCO3+CuO-(mixture+Co3O4)-(980C,15-20H in air using Au-crucible)-cool to 930C at 1C/H and to 870C at 2C/H-FC-oxidize					Structural deformation in oxidized and reduced YBa2(Cu1-yCoy)3O6+z compounds (0<y=<0.05)	199409			Physica C, 230(1994)31-41	E.Elkaim,H.Renevier,J.L.Hodeau,M.Bessiere,M.Marezio,S.Lefebvre	Y,Ba,Cu,Co,O	
4802	PHC2300177	oxygen content by TGA	YBa2Cu3O7	Y1Ba2Cu3O7.01	Y	1	Ba	2	Cu	3															O	7.01	7.01		1994																											3	Y123			A	3.823	3.883	11.68												K	88.5	89.5	90.5	89.5			89.5																																																																																															1	solid state reaction					Hole state density and superconductivity in oxygen-deficient La2-xSrxCuO4-y and YBa2Cu3O7-z	199409			Physica C, 230(1994)177-183	A.R.Moodenbaugh,D.A.Fischer	La,Sr,Cu,O,Y,Ba	
4803	PHC2300177	quench from 530C	YBa2Cu3O7	Y1Ba2Cu3O6.84	Y	1	Ba	2	Cu	3															O	6.84	6.84		1994																											3	Y123			A	3.828	3.882	11.714												K	60	67	71	67			67																																																																																															1	solid state reaction					Hole state density and superconductivity in oxygen-deficient La2-xSrxCuO4-y and YBa2Cu3O7-z	199409			Physica C, 230(1994)177-183	A.R.Moodenbaugh,D.A.Fischer	La,Sr,Cu,O,Y,Ba	
4804	PHC2300177	quench from 650C	YBa2Cu3O7	Y1Ba2Cu3O6.63	Y	1	Ba	2	Cu	3															O	6.63	6.63		1994																											3	Y123			A	3.835	3.877	11.733												K	45	51	53	51			51																																																																																															1	solid state reaction					Hole state density and superconductivity in oxygen-deficient La2-xSrxCuO4-y and YBa2Cu3O7-z	199409			Physica C, 230(1994)177-183	A.R.Moodenbaugh,D.A.Fischer	La,Sr,Cu,O,Y,Ba	
4805	PHC2300177	quench from 900C	YBa2Cu3O7	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	6.4	6.4		1994																											3	Y123			A	3.86	3.863	11.798												K					5																																																																																																	1	solid state reaction					Hole state density and superconductivity in oxygen-deficient La2-xSrxCuO4-y and YBa2Cu3O7-z	199409			Physica C, 230(1994)177-183	A.R.Moodenbaugh,D.A.Fischer	La,Sr,Cu,O,Y,Ba	
4806	PHC2300177	quench from 950C	YBa2Cu3O7	Y1Ba2Cu3O6.27	Y	1	Ba	2	Cu	3															O	6.27	6.27		1994																											2	Y123			A	3.861		11.815												K					5																																																																																																	1	solid state reaction					Hole state density and superconductivity in oxygen-deficient La2-xSrxCuO4-y and YBa2Cu3O7-z	199409			Physica C, 230(1994)177-183	A.R.Moodenbaugh,D.A.Fischer	La,Sr,Cu,O,Y,Ba	
4807	PHC2300153		TlBa2Ca3Cu4O11	Tl1Ba2Ca3Cu4O11	Tl	1	Ba	2	Ca	3	Cu	4													O	11			1994																											2	Tl1234			A	3.848		19												K		114		114			114																																																																																														Tl2O3,BaO2,CaO,CuO	1						The structure of TlBa2Ca3Cu4O11	199409			Physica C, 230(1994)153-158	D.M.Ogborne,M.T.Weller	Tl,Ba,Ca,Cu,O	
4808	PHC2250173		Bi2(Sr,La)2CuO4	Bi1.95Sr1.85La0.2Cu1O4	Bi	1.95	Sr	1.85	La	0.2	Cu	1													O	4			1994																												Bi2201																		K		27					27																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4809	PHC2250173		Bi2(Sr,La)2CuO4	Bi1.95Sr1.75La0.3Cu1O4	Bi	1.95	Sr	1.75	La	0.3	Cu	1													O	4			1994																												Bi2201																		K		33					33																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4810	PHC2250173		Bi2(Sr,La)2CuO4	Bi1.95Sr1.65La0.4Cu1O4	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	4			1994																												Bi2201																		K		36					36																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4811	PHC2250173		Bi2(Sr,La)2CuO4	Bi1.95Sr1.45La0.6Cu1O4	Bi	1.95	Sr	1.45	La	0.6	Cu	1													O	4			1994																												Bi2201																		K		24					24																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4812	PHC2250173		Bi2(Sr,La)2CuO4	Bi1.95Sr1.25La0.8Cu1O4	Bi	1.95	Sr	1.25	La	0.8	Cu	1													O	4			1994																												Bi2201																		K		19					19																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4813	PHC2250173		Bi2(Sr,Pr)2CuO4	Bi1.95Sr1.85Pr0.2Cu1O4	Bi	1.95	Sr	1.85	Pr	0.2	Cu	1													O	4			1994																												Bi2201																		K		28					28																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4814	PHC2250173		Bi2(Sr,Pr)2CuO4	Bi1.95Sr1.75Pr0.3Cu1O4	Bi	1.95	Sr	1.75	Pr	0.3	Cu	1													O	4			1994																												Bi2201																		K		32					32																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4815	PHC2250173		Bi2(Sr,Pr)2CuO4	Bi1.95Sr1.65Pr0.4Cu1O4	Bi	1.95	Sr	1.65	Pr	0.4	Cu	1													O	4			1994																												Bi2201																		K		35					35																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4816	PHC2250173		Bi2(Sr,Pr)2CuO4	Bi1.95Sr1.45Pr0.6Cu1O4	Bi	1.95	Sr	1.45	Pr	0.6	Cu	1													O	4			1994																												Bi2201																		K		22					22																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4817	PHC2250173		Bi2(Sr,Pr)2CuO4	Bi1.95Sr1.25Pr0.8Cu1O4	Bi	1.95	Sr	1.25	Pr	0.8	Cu	1													O	4			1994																												Bi2201																		K		17					17																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4818	PHC2250173		Bi2(Sr,Nd)2CuO4	Bi1.95Sr1.85Nd0.2Cu1O4	Bi	1.95	Sr	1.85	Nd	0.2	Cu	1													O	4			1994																												Bi2201																		K		26					26																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4819	PHC2250173		Bi2(Sr,Nd)2CuO4	Bi1.95Sr1.75Nd0.3Cu1O4	Bi	1.95	Sr	1.75	Nd	0.3	Cu	1													O	4			1994																												Bi2201																		K		30					30																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4820	PHC2250173		Bi2(Sr,Nd)2CuO4	Bi1.95Sr1.65Nd0.4Cu1O4	Bi	1.95	Sr	1.65	Nd	0.4	Cu	1													O	4			1994																												Bi2201																		K		35					35																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4821	PHC2250173		Bi2(Sr,Nd)2CuO4	Bi1.95Sr1.45Nd0.6Cu1O4	Bi	1.95	Sr	1.45	Nd	0.6	Cu	1													O	4			1994																												Bi2201																		K		18					18																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4822	PHC2250173	quench to RT	(Bi,Pb)2(Sr,La)2CuO4	Bi1.6Pb0.4Sr1.6La0.4Cu1O4	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	1											O	4			1994																												Bi2201																		K		36					36																																																																																														Bi2O3,SrCO3,CuO,CaCO3,R2O3,Pr6O11,PbO	1	mixture-CAL(700C,15H in air)-pellet-SIN(840C-940C for higher rare earth content)					Stoichiometry and Tc of Bi-2201 doped with La,Pr,Nd and Pb	199405			Physica C, 225(1994)173-180	A.R.West,P.V.P.S.S.Sastry	Bi,Sr,Cu,La,Pr,Nd,Pb	
4823	PHC2290239		YbBa2Cu3O7	Yb1Ba2Cu3O6.95	Yb	1	Ba	2	Cu	3															O	7-z	6.95		1994																											3	Y123			A	3.8	3.866	11.634												K		88.4					88.4																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4824	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.95Pr0.05Ba2Cu3O6.9	Yb	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z	6.9		1994																											3	Y123			A	3.801	3.87	11.64												K		89.1					89.1																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4825	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.9Pr0.1Ba2Cu3O6.92	Yb	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.92		1994																											3	Y123			A	3.803	3.878	11.655												K		88					88																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4826	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O6.88	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.88		1994																											3	Y123			A	3.809	3.881	11.65												K		79.9					79.9																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4827	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.7Pr0.3Ba2Cu3O6.87	Yb	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.87		1994																											3	Y123			A	3.812	3.886	11.648												K		67.2					67.2																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4828	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.6Pr0.4Ba2Cu3O6.91	Yb	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.91		1994																											3	Y123			A	3.817	3.888	11.679												K		50.5					50.5																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4829	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.5Pr0.5Ba2Cu3O6.9	Yb	0.5	Pr	0.5	Ba	2	Cu	3													O	7-z	6.9		1994																											3	Y123			A	3.822	3.894	11.699												K		34.8					34.8																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4830	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.45Pr0.55Ba2Cu3O6.92	Yb	0.45	Pr	0.55	Ba	2	Cu	3													O	7-z	6.92		1994																											3	Y123			A	3.83	3.897	11.7												K		18.3					18.3																																																																																														Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4831	PHC2290239		(Yb,Pr)Ba2Cu3O7	Yb0.3Pr0.7Ba2Cu3O6.94	Yb	0.3	Pr	0.7	Ba	2	Cu	3													O	7-z	6.94		1994																											3	Y123			A	3.836	3.9	11.701												K					5																																																																																																Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4832	PHC2290239		PrBa2Cu3O7	Pr1Ba2Cu3O6.95	Pr	1	Ba	2	Cu	3															O	7-z	6.95		1994																											3	Y123			A	3.865	3.92	11.722												K					5																																																																																																Yb2O3,Pr6O11,BaO2,CuO	1	mixture-heat(930C,60H)-pellet-heat(850C,4H in flowing O2)-cool to 500C(0.5C/min in O2)-ANN(500C,12H in O2)-cool to RT(1C/min)					Superconducting properties of Yb1-x Prx Ba2 Cu3O7-z	199408			Physica C, 229(1994)239-243	H.Zhang,J.L.Peng,M.S.Hegde,R.L.Greene,S.M.Green,X.Q.Xu	Yb,Pr,Ba,Cu,O	
4833	PHC2270160		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		1	1994																												T																		K		36.4					36.4																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4834	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.98Ni0.02O4	La	1.83	Sr	0.17	Cu	0.98	Ni	0.02													O	4		1	1994																												T																		K		22.8					22.8																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4835	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.97Ni0.03O4	La	1.83	Sr	0.17	Cu	0.97	Ni	0.03													O	4		1	1994																												T																		K		15.2					15.2																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4836	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.65Ni0.35O4	La	1.83	Sr	0.17	Cu	0.65	Ni	0.35													O	4		1	1994																												T																		K		13.5					13.5																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4837	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.96Ni0.04O4	La	1.83	Sr	0.17	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		7.7					7.7																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4838	PHC2270160		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1994																												T																		K		28					28																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4839	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.99Ni0.01O4	La	1.8	Sr	0.2	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		23.4					23.4																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4840	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.98Ni0.02O4	La	1.8	Sr	0.2	Cu	0.98	Ni	0.02													O	4		1	1994																												T																		K		16.8					16.8																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4841	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.97Ni0.03O4	La	1.8	Sr	0.2	Cu	0.97	Ni	0.03													O	4		1	1994																												T																		K		10.9					10.9																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4842	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.65Ni0.35O4	La	1.8	Sr	0.2	Cu	0.65	Ni	0.35													O	4		1	1994																												T																		K		8					8																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4843	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.96Ni0.04O4	La	1.8	Sr	0.2	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		5.1					5.1																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4844	PHC2270160		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1994																												T																		K		29.4					29.4																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4845	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.9Sr0.1Cu0.99Ni0.01O4	La	1.9	Sr	0.1	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		11.5					11.5																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4846	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.9Sr0.1Cu0.98Ni0.02O4	La	1.9	Sr	0.1	Cu	0.98	Ni	0.02													O	4		1	1994																												T																		K																																																																																																					La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4847	PHC2270160		(La,Sr)2CuO4	La0.75Sr0.25Cu1O4	La	0.75	Sr	0.25	Cu	1															O	4		1	1994																												T																		K		14.4					14.4																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4848	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.98Ni0.02O4	La	1.75	Sr	0.25	Cu	0.98	Ni	0.02													O	4		1	1994																												T																		K		8.1					8.1																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4849	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.97Ni0.03O4	La	1.75	Sr	0.25	Cu	0.97	Ni	0.03													O	4		1	1994																												T																		K		4.7					4.7																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4850	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.96Ni0.04O4	La	1.75	Sr	0.25	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		2.5					2.5																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4851	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.96Ni0.04O4	La	1.85	Sr	0.15	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		0.001					0.001																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4852	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.96Ni0.04O4	La	1.83	Sr	0.17	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		8.2					8.2																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4853	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.96Ni0.04O4	La	1.8	Sr	0.2	Cu	0.96	Ni	0.04													O	4		1	1994																												T																		K		7.6					7.6																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4854	PHC2270160		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		1	1994																												T																		K		0.001					0.001																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4855	PHC2270160		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1994																												T																		K		27.8					27.8																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4856	PHC2270160		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1994																												T																		K		37					37																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4857	PHC2270160		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		1	1994																												T																		K		37.2					37.2																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4858	PHC2270160		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1994																												T																		K		31.4					31.4																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4859	PHC2270160		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1994																												T																		K		16.8					16.8																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4860	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.92Sr0.08Cu0.99Ni0.01O4	La	1.92	Sr	0.08	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		0.001					0.001																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4861	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.9Sr0.1Cu0.99Ni0.01O4	La	1.9	Sr	0.1	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		13.1					13.1																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4862	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.99Ni0.01O4	La	1.83	Sr	0.17	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		31.2					31.2																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4863	PHC2270160		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.99Ni0.01O4	La	1.8	Sr	0.2	Cu	0.99	Ni	0.01													O	4		1	1994																												T																		K		24.5					24.5																																																																																														La2O3,SrCO3,CuO,NiO	1	mixture-heat(900C,48H in air)-heat(1000-1150C, in air)-ANN(500C,10H in flowing O2)-cool to RT at 1K/min					Effect of a change in the carrier concentration and disorder on the superconducting transition temperature of the La2-xSrxCu1-yNiyO4 system	199406			Physica C, 227(1994)160-168	J.M.Honig,K.Sreedhar,P.A.Metcalf	La,Sr,Cu,Ni,O	
4864	PHC2270095	starting mixture=C0.6Ba2Ca4Cu5.5O13.2	(Cu,C)2Ba3Ca3Cu4O13	C1Ba3Ca3Cu5O13	C	1	Ba	3	Ca	3	Cu	5													O	13		1	1994																											2	Cu2334			A	3.855		21.87												K		113		113			113																																																																																															1	precursor(Ba2Ca3Cu4O9)+(CaCO3+Ca2CuO3+CuO+Ag2O) in a dry box-(C0.5Ba2Ca4Cu5.5O13+C0.5Ba2Ca4Cu5.5O13.2)-seal in Au capsule-(5GPa,1250C,1H)-Q to RT					A new series of oxycarbonate superconductors (Cu0.5C0.5)2Ba3Can-1CunO2n+5 (n=4,5) prepared at high pressure	199406		National Institute for Research in Inorganic Materials,Tsukuba,Ibaraki,Japan	Physica C, 227(1994)95-101	E.Takayama-Muromachi,T.Kawashima,Y.Matsui	Cu,C,Ba,Ca,O	
4865	PHC2270095	starting mixture=C0.5Ba2Ca4Cu5.5O13, mix-phase of (Cu,C)2334+(Cu,C)2345	(Cu,C)2Ba3Ca3Cu4O13	C1Ba3Ca3Cu5O13	C	1	Ba	3	Ca	3	Cu	5													O	13		2	1994																											2	Cu2334			A	3.857		25.067												K	107	110	113				110																																																																																															1	precursor(Ba2Ca3Cu4O9)+(CaCO3+Ca2CuO3+CuO+Ag2O) in a dry box-(C0.5Ba2Ca4Cu5.5O13+C0.5Ba2Ca4Cu5.5O13.2)-seal in Au capsule-(5GPa,1250C,1H)-Q to RT					A new series of oxycarbonate superconductors (Cu0.5C0.5)2Ba3Can-1CunO2n+5 (n=4,5) prepared at high pressure	199406		National Institute for Research in Inorganic Materials,Tsukuba,Ibaraki,Japan	Physica C, 227(1994)95-101	E.Takayama-Muromachi,T.Kawashima,Y.Matsui	Cu,C,Ba,Ca,O	
4866	PHC2310004	small amount of impurity included	(Hg,Tl)Ba2(Ca,Sr)Cu2O6	Hg0.5Tl0.5Ba2Ca0.86Sr0.14Cu2O6+z	Hg	0.5	Tl	0.5	Ba	2	Ca	0.86	Sr	0.14	Cu	2									O	6+z		1	1994																											2	Hg1212			A	3.85		12.655												K		122		122			122																																																																																														HgO,Tl2O3,Ba2CuO3,Ca0.86Sr0.14CuO2	1	mixture-pellet-silica tube-heat(860C,8H)-SIN(860C,10H)-slow cool to RT					Synthesis and characterization of a new mercury-based superconductor,Hg0.5Tl0.5Ba2Ca1-xSrxCu2O6+z	7			Physica C.,231(1994) 4-8	Jong C.Park,Kyu W.Lee,Nae H.Kim,Nam H. Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
4867	PHC2310004		(Hg,Tl)Ba2(Ca,Sr)Cu2O6	Hg0.5Tl0.5Ba2Ca0.86Sr0.14Cu2O6+z	Hg	0.5	Tl	0.5	Ba	2	Ca	0.86	Sr	0.14	Cu	2									O	6+z		1	1994																												Hg1212																		K		100		100			100																																																																																															1	4866 sample - ANN(350C,8H in O2)					Synthesis and characterization of a new mercury-based superconductor,Hg0.5Tl0.5Ba2Ca1-xSrxCu2O6+z	7			Physica C.,231(1994) 4-8	Jong C.Park,Kyu W.Lee,Nae H.Kim,Nam H. Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
4868	PHC2300354	oxygen content by iodometric titration	SmBa2Cu3O7	Sm1Ba2Cu3O6.85	Sm	1	Ba	2	Cu	3															O	z	6.85	1	1994																												Y123																		K		90.4					90.4																																																								mJ/K2fu	16	from sp.heat measurement	494	from sp.heat measurement																																			1	citrate pyrolysis process, details see					Specific herat of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199409			Physica C 230 (1994) 354-560	D.Wlosewicz,K.Rogacki,T.Plackowski,Z.Bukowski	Sm,Ba,Cu,O	
4869	PHC2300354		SmBa2Cu3O7	Sm1Ba2Cu3O6.73	Sm	1	Ba	2	Cu	3															O	z	6.73	1	1994																												Y123																		K		45					45																																																								mJ/K2fu	15	from sp.heat	488	from sp.heat																																			1	citrate pyrolysis process, details see					Specific herat of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199409			Physica C 230 (1994) 354-560	D.Wlosewicz,K.Rogacki,T.Plackowski,Z.Bukowski	Sm,Ba,Cu,O	
4870	PHC2300354		SmBa2Cu3O7	Sm1Ba2Cu3O6.11	Sm	1	Ba	2	Cu	3															O	z	6.11	1	1994																												Y123																		K					4																																																										mJ/K2fu		from sp.heat	487	from sp.heat																																			1	citrate pyrolysis process, details see					Specific herat of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199409			Physica C 230 (1994) 354-560	D.Wlosewicz,K.Rogacki,T.Plackowski,Z.Bukowski	Sm,Ba,Cu,O	
4871	PHC2300354		Sm(Ba,Sm)2Cu3O7	Sm1.27Ba1.73Cu3O7.05	Sm	1.27	Ba	1.73	Cu	3															O	z	7.05	1	1994																												Y123																		K		50					50																																																											493	from sp.heat																																			1	citrate pyrolysis process, details see					Specific herat of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199409			Physica C 230 (1994) 354-560	D.Wlosewicz,K.Rogacki,T.Plackowski,Z.Bukowski	Sm,Ba,Cu,O	
4872	PHC2300354		Sm(Ba,Sm)2Cu3O7	Sm1.6Ba1.4Cu3O7.11	Sm	1.6	Ba	1.4	Cu	3															O	z	7.11	1	1994																												Y123																		K					4																																																										mJ/K2fu		from sp.heat, gamma=zero	518	from sp.heat																																			1	citrate pyrolysis process, details see					Specific herat of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199409			Physica C 230 (1994) 354-560	D.Wlosewicz,K.Rogacki,T.Plackowski,Z.Bukowski	Sm,Ba,Cu,O	
4873	PHC2300385	impurity phases=Tm2O3,Tm2Cu2O5, superconductivity and antiferro coexist?	(Tm,Ca)2CuO4	Tm1.83Ca0.17Cu1O3.99	Tm	1.83	Ca	0.17	Cu	1															O	4	3.99	1	1994								9.5																			2	T'			A	3.831		11.642												K		30		30			30										27																																																																																				R2O3,CaO,CuO	1	mixture-SIN(100C,24H in air)-reground-pellet-wrapped in Au foil-heat(1100C,0.5H under 6GPa O2 atmosphere using KClO4)					Superconductivity at 30 K in the Nd2CuO4-type cuprate Tm1.83Ca0.17CuO4	199409			Physica C (1994)385-388	B.Yin,C.Dong,W.L.Zhu,X.J.Zhou,Y.S.Yao,Y.Z.Huang,Z.X.Zhao	Tm,Ca,Cu,O	
4874	PHC2300385	semicon-like	(Dy,Ca)2CuO4	Dy1.83Ca0.17Cu1O4	Dy	1.83	Ca	0.17	Cu	1															O	4	4	1	1994								9																			2	T'			A	3.864		11.772												K					4																																																																																																R2O3,CaO,CuO	1	mixture-SIN(100C,24H in air)-reground-pellet-wrapped in Au foil-heat(1100C,0.5H under 6GPa O2 atmosphere using KClO4)					Superconductivity at 30 K in the Nd2CuO4-type cuprate Tm1.83Ca0.17CuO4	199409			Physica C (1994)385-388	B.Yin,C.Dong,W.L.Zhu,X.J.Zhou,Y.S.Yao,Y.Z.Huang,Z.X.Zhao	Tm,Ca,Cu,O	
4875	PHC2300385	semicon-like, magnetic anomaly at 20K, weak ferro	(Gd,Ca)2CuO4	Gd1.83Ca0.17Cu1O3.98	Gd	1.83	Ca	0.17	Cu	1															O	4	3.98	1	1994																											2	T'			A	3.885		11.893												K					4																																																																																																R2O3,CaO,CuO	1	mixture-SIN(100C,24H in air)-reground-pellet-wrapped in Au foil-heat(1100C,0.5H under 6GPa O2 atmosphere using KClO4)					Superconductivity at 30 K in the Nd2CuO4-type cuprate Tm1.83Ca0.17CuO4	199409			Physica C (1994)385-388	B.Yin,C.Dong,W.L.Zhu,X.J.Zhou,Y.S.Yao,Y.Z.Huang,Z.X.Zhao	Tm,Ca,Cu,O	
4876	PHC2310131	impurity phase=PrBaO3,BaCuO2, there are broad maximum at 150K in resistivity	PrBa2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		1	1994	emu/g				micro.B/Mo	2.67	7.25																				3	Y124	Ammm		A	3.885	3.902	27.308												K					2																																																																									m.ohm.cm											4												Pr2O3,BaO2,CuO	1	mixture-CAL(900C,12H in flowing O2)-SIN twice -(Pr123+BaCuO2+CuO)-pellet-react(950-970C,24H in O2 of 5 atm)					Hihg oxygen pressure synthesis of the PrBa2Cu4O8 compound	199409			Physica C 231 (1994) 131-136	I.Hirabayashi,K.Kawamoto,N.Yamsda,S.Horii,U.MIzutani,Y.kodama,Yuh Yamada,Z.Guo	Pr,Ba,Cu,O	
4877	PHC2310109	not superconducting	YSr2(Cu,Se)3O7	Y1Sr2Cu2.5Se0.5O7-z	Y	1	Sr	2	Cu	2.5	Se	0.5													O	7-z			1994																											3	Y123			A	3.806	3.869	11.461												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4878	PHC2310109		(Y,Ca)Sr2(Cu,Se)3O7	Y0.7Ca0.3Sr2Cu2.5Se0.5O7-z	Y	0.7	Ca	0.3	Sr	2	Cu	2.5	Se	0.5											O	7-z			1994																											3	Y123			A	3.848	3.86	11.391												K			45				45																																																																																														Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4879	PHC2310109	high-pressure O2 process	YSr2(Cu,Se)3O7	Y1Sr2Cu2.5Se0.5O7-z	Y	1	Sr	2	Cu	2.5	Se	0.5													O	7-z			1994																											3	Y123			A	3.8	3.866	11.46												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4880	PHC2310109		(Y,Ce)2Sr2(Cu,Se)3O9	Y1.5Ce0.5Sr2Cu2.5Se0.5O9-z	Y	1.5	Ce	0.5	Sr	2	Cu	2.5	Se	0.5											O	9-z			1994																											2				A	3.835		28.43												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4881	PHC2310109	high-pressure O2 process	(Y,Ce)2Sr2(Cu,Se)3O9	Y1.5Ce0.5Sr2Cu2.5Se0.5O9-z	Y	1.5	Ce	0.5	Sr	2	Cu	2.5	Se	0.5											O	9-z			1994																											2				A	3.829		28.41												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4882	PHC2310109		(Y,Ce)2Sr2(Cu,Se)3O9	Y1.5Ce0.5Sr2Cu2Se1O9-z	Y	1.5	Ce	0.5	Sr	2	Cu	2	Se	1											O	9-z			1994																											2				A	3.83		28.65												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4883	PHC2310109	high-pressure O2 process	(Y,Ce)2Sr2(Cu,Se)3O9	Y1.5Ce0.5Sr2Cu2Se1O9-z	Y	1.5	Ce	0.5	Sr	2	Cu	2	Se	1											O	9-z			1994																											2				A	3.82		28.65												K					10																																																																																																Y2O3,CeO2,SrCO3,SrSeO4,CuO	1	mixture-pellet-heat(1060C,12H in O2)-reground-heat(1060C,12H in O2)-slow cool					Se and Te subsititutions in YSr2Cu3O7-y and [Y/Ce]2 Sr2 Cu3 O9-y	199409			Pyhsica C 231 (1994) 109-112	C.Greaves,E.Z.Kurmaev,M.Neumann,M.Slaski,P.R.Slater,St.Uhlenbrock	Y,Sr,Cu,O,Ce,Te	
4884	PHC2310161	coherence length anisotropy = 15	Tl2Ba2CuO6	Tl1.7Ba2Cu1O6	Tl	1.7	Ba	2	Cu	1															O	6		3	1994																											2	Tl2201			A	3.867		23.175												K		24					24																																																																																														Tl2O3,BaO2,CuO,	5	mixture of (Tl:Ba:Ca:Cu=2:2:0:2)-seal in Au capsule-heat to 915C with soaking time=10H in flowing O2-cool to 895K at 2C/H-Q to RT					Growth and anisotropic superconducting properties of Tl2Ba2CuO6 and Tl2Ba2CaCu2O8 single crystals	199409			Physica C 231 (1994) 161-166	Humihiko Takei,Masashi Hasegawa,Yasuhiro Iye,Yoshitaka Matsushita	Tl,Ba,Cu,O,Ca	
4885	PHC2310161	single crystal=0.8*0.8mm*50micron, coherence length anisotropy = 33	Tl2Ba2CaCu2O8	Tl1.8Ba2Ca0.85Cu2.2O8	Tl	1.8	Ba	2	Ca	0.85	Cu	2.2													O	8		3	1994																											2	Tl2212			A	3.857		29.35												K		104					104																																																																																														Tl2O3,CuO,BaO2,CaO	5	mixture of (Tl:Ba:Ca:Cu=1.5:2:3:1.5)-seal in Au capsule -heat to 930C with soaking time=3H in flowing O2 -cool to 860C at 2C/H -Q to RT					Growth and anisotropic superconducting properties of Tl2Ba2CuO6 and Tl2Ba2CaCu2O8 single crystals	199409			Physica C 231 (1994) 161-166	Humihiko Takei,Masashi Hasegawa,Yasuhiro Iye,Yoshitaka Matsushita	Tl,Ba,Cu,O,Ca	
4886	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.1Sr1.9Cu1Oz	Bi	2.1	Sr	1.9	Cu	1															O	z			1994																											2	Bi2201			A	5.372		24.66												K					14																																																																									m.ohm.cm											4			m3/C	0.0000000025								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4887	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.15Sr1.85Cu1O6.18	Bi	2.15	Sr	1.85	Cu	1															O	z	6.18		1994																											2	Bi2201			A	5.375		24.62												K					14																																																																									m.ohm.cm											4			m3/C	0.0000000027								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4888	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.2Sr1.8Cu1Oz	Bi	2.2	Sr	1.8	Cu	1															O	z			1994																											2	Bi2201			A	5.375		24.59												K					14																																																																									m.ohm.cm											4.4			m3/C	0.0000000048								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4889	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.25Sr1.75Cu1O6.21	Bi	2.25	Sr	1.75	Cu	1															O	z	6.21		1994																											2	Bi2201			A	5.387		24.58												K					14																																																																									m.ohm.cm											6.3			m3/C	0.0000000052								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4890	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.3Sr1.7Cu1Oz	Bi	2.3	Sr	1.7	Cu	1															O	z			1994																											2	Bi2201			A	5.391		24.55												K					14																																																																									m.ohm.cm											8.9			m3/C	0.0000000082								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4891	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.35Sr1.65Cu1O6.23	Bi	2.35	Sr	1.65	Cu	1															O	z	6.23		1994																											2	Bi2201			A	5.398		24.53												K					14																																																																									m.ohm.cm											1.6			m3/C	0.0000000083								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4892	PR04913119		Bi2(Sr,Bi)2CuO6	Bi2.4Sr1.6Cu1Oz	Bi	2.4	Sr	1.6	Cu	1															O	z			1994																											2	Bi2201			A	5.397		24.47												K					14																																																																									m.ohm.cm											2.6			m3/C	0.000000012								Bi2O3,SrCO3,CuO	1	mixture-CAL(800C,12H + 820C,12H in air)-pellet-SIN(850-870C,15H in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
4893	PRL0731845	penetration depth(T) = A*(1-t)**(-0.33) , t=T/Tc	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7	6.95		1994																												Y123																		K		92.74					92.74																																									A	rf-field normal to c-axis, using microwave technique		1400																																																			5	flux growth technique, see Physica C, 195(1992)51					Penetration Depth Measurements of 3D XY Critical Behavior in YBa2Cu3O6.95 Crystals	199409		Department of Physics,Unversity of British Columbia,Vancouver,British Columbia,Canada V6T1Z1	Phys.Rev.Lett.,73(1994)1845	D.A.Bonn,Nigel Goldenfeld,P.J.Hirschfeld,Ruxing Liang,S.Kamal,W.N.Hardy	Y,Ba,Cu,O	
4894	PHC2280190	superconducting phase = about 80 volume percent	(Hg,Bi)Sr2(Y,Ca)Cu2O6	Hg0.67Bi0.33Sr2Y0.67Ca0.33Cu2O6+z	Hg	0.67	Bi	0.33	Sr	2	Y	0.67	Ca	0.33	Cu	2									O	6+z		2	1994																											2	Hg1212	P4/mmm		A	3.81		12.016												K	55		100				77.5																																																																																														Bi2O3,Sr(NO3)2,Y2O3,CaO,CuO	1	using the sealed quartz method, precursor(Bi-Sr-Ca-Cu-O) + HgO -sealed in quartz tube - heat(865C,8H)-cool to RT(2.5C/min)					Synthesis and characterization of (Hg,Bi)-based 1212-type cuprate superconductor (Hg0.67Bi0.33)Sr2(Y0.67Ca0.33)Cu2O6+z (z=0.68)	199407			Physica C, 228(1994)190-194	L.Wessels,O.Chmaissem,Z.Z.Sheng	Hg,Bi,Sr,Y,Ca,Cu,O	
4895	PHC2280115	single crystal=420*280*30 micrometer, G-L parameter=159	(Bi,La)2(Sr,La)2CuO6	Bi1.95Sr1.65La0.4Cu1O6+z	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	6+z		3	1994																												Bi2201																		K		13					13											Oe	magnetization, linear extraporation to 0K			9.4																					A			63		A			10000																																																									Measurements of Hc1 and Jc in Bi1.95Sr1.65La0.4CuO6+z with a micro-Hall probe	199407			Physica C, 228(1994)115-121	D.A.Brawner,H.R.Ott,R.Jin	Bi,Sr,La,Cu,O	
4896	PHC2250235		Bi2Sr2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8+z	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+z			1994																												Bi2212			A			30.8												K		85		85			85																																		HIR4896																																																												Bi2O3,SrCO3,CaCO3,CuO,Yb2O3	1	mixture-heat(1040C,24H)-cool to 970C at (50C/H) - cool to 830C (1C/H) -FC to RT					Irreversibility lines of Yb and Pb substituted Bi-2212 single crystals	199405			Physica C, 225 (1994) 235-239	A.Maignan,A.Ruyter,Ch.Simon,M.Hervieu,V.Hardy		
4897	PHC2250235		Bi2Sr2(Ca,Yb)Cu2O8	Bi2Sr2Ca0.7Yb0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Yb	0.3	Cu	2											O	8+z			1994																												Bi2212			A			30.5												K		89		89			89																																		HIR4897																																																												Bi2O3,SrCO3,CaCO3,CuO,Yb2O3	1	mixture-heat(1040C,24H)-cool to 970C at (50C/H) - cool to 830C (1C/H) -FC to RT					Irreversibility lines of Yb and Pb substituted Bi-2212 single crystals	199405			Physica C, 225 (1994) 235-239	A.Maignan,A.Ruyter,Ch.Simon,M.Hervieu,V.Hardy		
4898	PHC2250235		Bi2(Sr,Pb)2CaCu2O8	Bi2Pb0.25Sr1.75Ca1Cu2O8+z	Bi	2	Pb	0.25	Sr	1.75	Ca	1	Cu	2											O	8+z			1994																												Bi2212			A			30.75												K		77		77			77																																		HIR4898																																																												Bi2O3,SrCO3,CaCO3,CuO,Yb2O3,PbO	1	mixture-heat to 800c at 150C/H - hold(800C,15H)-heat to 1040C at 50C/H-cool to 970C (50C/H)-cool to 830C(1C/H)-FC to RT					Irreversibility lines of Yb and Pb substituted Bi-2212 single crystals	199405			Physica C, 225 (1994) 235-239	A.Maignan,A.Ruyter,Ch.Simon,M.Hervieu,V.Hardy		
4899	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.224	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7+z	7.224	1	1994																											2	Y123			A	3.811		11.459												K	33	35		35			35																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in alumina crucible)-SIN(1000C,5H in air)-ANN(300-700C,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4900	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.152	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7+z	7.152	1	1994																											2	Y123			A	3.816		11.483												K	9	23		23			23																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in alumina crucible)-SIN(1000C,5H in air)-ANN(300-700C,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4901	PHC2260037		YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.144	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7+z	7.144	1	1994																											2	Y123			A	3.815		11.477												K		12		12			12																																																																																														Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in alumina crucible)-SIN(1000C,5H in air)-ANN(300-700C,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4902	PHC2260037	semicon-like, ferromagnetic	YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.123	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7+z	7.123	1	1994																											2	Y123			A	3.81		11.465												K					4.2																																																																																																Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in alumina crucible)-SIN(1000C,5H in air)-ANN(300-700C,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4903	PHC2260037	semicon-like, ferromagnetic	YSr2(Cu,Ti)3O7	Y1Sr2Cu2.7Ti0.3O7.098	Y	1	Sr	2	Cu	2.7	Ti	0.3													O	7+z	7.098	1	1994																											2	Y123			A	3.808		11.459												K					4.2																																																																																																Y2O3,SrCO3,CuO,TiO2	1	mixture-CAL(900C in alumina crucible)-SIN(1000C,5H in air)-ANN(300-700C,60H in flowing O2)-FC to RT					The superconducting properties and crystal structure of YSr2(Cu0.9 Ti0.1)3 O7+z	199406			Physica C, 226 (1994) 37-42	C.H.Cheng,C.T.Chang,D.H.Chen,M.K.Wu,S.J.Wuu,S.R.Sheen,T.W.Liu		
4904	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.46Sr2Ca0.3Y0.7Cu2.52O6.98	C	0.46	Sr	2	Ca	0.3	Y	0.7	Cu	2.52											O	z	6.98		1994																											3	C1212			A	3.836	3.853	11.123																																																																																																																	SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4905	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.47Sr2Ca0.35Y0.65Cu2.48O6.96	C	0.47	Sr	2	Ca	0.35	Y	0.65	Cu	2.48											O	z	6.96		1994																											3	C1212			A	3.833	3.853	11.119												K			40				40																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4906	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.48Sr2Ca0.4Y0.6Cu2.46O6.97	C	0.48	Sr	2	Ca	0.4	Y	0.6	Cu	2.46											O	z	6.97		1994																											3	C1212			A	3.831	3.851	11.116												K			41.1				41.1																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4907	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.5Sr2.01Ca0.44Y0.55Cu2.44O6.94	C	0.5	Sr	2.01	Ca	0.44	Y	0.55	Cu	2.44											O	z	6.94		1994																											3	C1212			A	3.833	3.85	11.116												K			45.5				45.5																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4908	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.51Sr2Ca0.5Y0.5Cu2.42O6.92	C	0.51	Sr	2	Ca	0.5	Y	0.5	Cu	2.42											O	z	6.92		1994																											3	C1212			A	3.834	3.849	11.108												K			48.9				48.9																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4909	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.53Sr1.99Ca0.56Y0.45Cu2.39O6.94	C	0.53	Sr	1.99	Ca	0.56	Y	0.45	Cu	2.39											O	z	6.94		1994																											3	C1212			A	3.831	3.848	11.108												K			54.2				54.2																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4910	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.54Sr2Ca0.6Y0.4Cu2.38O6.89	C	0.54	Sr	2	Ca	0.6	Y	0.4	Cu	2.38											O	z	6.89		1994																											3	C1212			A	3.835	3.849	11.074												K			56.7				56.7																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4911	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.55Sr2.03Ca0.62Y0.35Cu2.35O6.79	C	0.55	Sr	2.03	Ca	0.62	Y	0.35	Cu	2.35											O	z	6.79		1994																											3	C1212			A	3.836	3.853	11.009												K			60				60																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4912	PHC2300089		(C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	C0.57Sr2Ca0.7Y0.3Cu2.33O6.78	C	0.57	Sr	2	Ca	0.7	Y	0.3	Cu	2.33											O	z	6.78		1994																											3	C1212			A	3.838	3.858	10.973												K			60.3				60.3																																																																																														SrCO3,CaCO3,Y2O3,CuO	1	mixture-pellet-heat(1323K,20H in flowing O2+CO3)-Q to RT-ANN by HIP(1273K,30H in 80%Ar+20%O2)					Preparation, crystal structure and superconductivity of (C,Cu)(Sr,Ca)2(Y,Ca,Sr)Cu2O7	199409		Institute for Materials Research, Tohoku University	Physica C, 230(1994)89-96	H.Yamane,K.Hiraga,N.Kobayashi,S.Funahashi,T.Hirai,T.Kajitani,Y.Miyazaki,Y.Morii	C,Cu,Sr,Ca,Y,O	
4913	PHC2200143		YBa2(Cu,Co)3O7	Y1Ba2Cu2.655Co0.345O7.29	Y	1	Ba	2	Cu	2.655	Co	0.345													O	z	7.29	1	1994																											2	Y123	P4/mmm		A	3.868		11.66																																																																																																																	BaCO3,Y2O3,CuO,Co3O4	1	mixture in alumina crucible-heat(930C,15H)-heat(930C,10H in O2)-Q to 600C-cool to 300C(50C/H)-hold(5H)-RT					Electron- and powder neutron-diffraction studies of YBa2(Cu1-yCoy)3O6+z with 0.05<y<0.33	199402			Physica C, 220(1994)143-159	A.Santoro,H.Renevier,J.L.Hodeau,M.Marezio	Y,Ba,Cu,Co,O	
4914	PHC2200143		YBa2(Cu,Co)3O7	Y1Ba2Cu2.43Co0.57O7.34	Y	1	Ba	2	Cu	2.43	Co	0.57													O	z	7.34	1	1994																											2	Y123	P4/mmm		A	3.886		11.643																																																																																																																	BaCO3,Y2O3,CuO,Co3O4	1	mixture in alumina crucible-heat(930C,15H)-heat(930C,10H in O2)-Q to 600C-cool to 300C(50C/H)-hold(5H)-RT					Electron- and powder neutron-diffraction studies of YBa2(Cu1-yCoy)3O6+z with 0.05<y<0.33	199402			Physica C, 220(1994)143-159	A.Santoro,H.Renevier,J.L.Hodeau,M.Marezio	Y,Ba,Cu,Co,O	
4915	PHC2200143		YBa2(Cu,Co)3O7	Y1Ba2Cu2.61Co0.39O6.91	Y	1	Ba	2	Cu	2.61	Co	0.39													O	z	6.91	1	1994																											2	Y123	P4/mmm		A	3.877		11.735																																																																																																																	BaCO3,Y2O3,CuO,Co3O4	1	mixture in alumina crucible-heat(930C,15H)-heat(930C,10H in O2)-Q to 600C-cool to 300C(50C/H)-hold(5H)-RT					Electron- and powder neutron-diffraction studies of YBa2(Cu1-yCoy)3O6+z with 0.05<y<0.33	199402			Physica C, 220(1994)143-159	A.Santoro,H.Renevier,J.L.Hodeau,M.Marezio	Y,Ba,Cu,Co,O	
4916	PHC2200143		YBa2(Cu,Co)3O7	Y1Ba2Cu2.445Co0.555O7.12	Y	1	Ba	2	Cu	2.445	Co	0.555													O	z	7.12	1	1994																											2	Y123	P4/mmm		A	3.885		11.706																																																																																																																	BaCO3,Y2O3,CuO,Co3O4	1	mixture in alumina crucible-heat(930C,15H)-heat(930C,10H in O2)-Q to 600C-cool to 300C(50C/H)-hold(5H)-RT					Electron- and powder neutron-diffraction studies of YBa2(Cu1-yCoy)3O6+z with 0.05<y<0.33	199402			Physica C, 220(1994)143-159	A.Santoro,H.Renevier,J.L.Hodeau,M.Marezio	Y,Ba,Cu,Co,O	
4917	PHC2160029	Cu-O2 distance=2.775 A	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6.24	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z	6.24		1993									6																		2	Hg1212	P4/mmm		A	3.855		12.665												K		126		126			126										90																																																																																						as-synthesized -ANN(300C in flowing O2)					STRUCTURE,DOPING AND SUPERCONDUCTIVITY IN HGBA2CACU2O6+Z (TC<-128K)	199310			PHYSICA C,216(1993)29	B.A.HUNTER,D.G.HINKS,G.S.KNAPP,J.D.JORGENSEN,J.L.WAGNER,M.A.BENO,P.G.RADAELLI	HG,BA,CA,CU,O	
4918	PHC2160029	Cu-O2 distance = 2.824 A	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6.08	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z	6.08		1993									6																		2	Hg1212			A	3.863		12.698												K		92		92			92										40																																																																																						as-synthesized - heat(600C in flowing Ar)					STRUCTURE,DOPING AND SUPERCONDUCTIVITY IN HGBA2CACU2O6+Z (TC<-128K)	199310			PHYSICA C,216(1993)29	B.A.HUNTER,D.G.HINKS,G.S.KNAPP,J.D.JORGENSEN,J.L.WAGNER,M.A.BENO,P.G.RADAELLI	HG,BA,CA,CU,O	
4919	PHC2270215	[Bi0.5Hg0.5Sr2CuO5]n[Sr2CuO2CO3]m series	(Bi,Hg)Sr4(Cu2,CO3)O7	Bi0.5Hg0.5Sr4Cu2C1O10-z	Bi	0.5	Hg	0.5	Sr	4	Cu	2	C	1											O	10-z			1994																											2				A	3.826		16.474												K		17					17																																																																																														HgO,(BiO)2CO3,SrO2,SrCO3,Sr2CuO3,CuO	1	mixture-heat(800C,6H)-hold 12H-slow cool to RT					A new superconducting oxycarbonate Bi0.5Hg0.5Sr4Cu2CO3O7-z	199407			Physica C, 227(1994)215-224	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu	Bi,Hg,Sr,Cu,O,C	
4920	PHC2250149	2223 phase is dominant	(Bi,Pb,Te)2Sr2Ca3Cu4O12	Bi1.6Pb0.3Te0.1Sr2Ca3Cu4Oz	Bi	1.6	Pb	0.3	Te	0.1	Sr	2	Ca	3	Cu	4									O	z		2	1994																												Bi2223																		K	102.7						102.7																				T		201.4							T/K		2.79			HIR4920		A		12.8																																																									1	ANN(835C,72H in air					Superconducting and magnetic properties of melt-quenched Bi-2223 superconductors doped with Pb and Te	199405			Physica C, 225(1994)149-157	A.Zaleski,E.S.Vlakhov,K.A.Nenkov,M.Ciszek,Y.B.Dimitriev	Bi,Sr,Ca,Cu,O,Pb,Te	
4921	PHC2250149	2223 phase is dominant, Jc(77K,1T)=1.3 A/cm2, Jc(77K,0T)=316 A/cm2	(Bi,Pb,Te)2Sr2Ca3Cu4Oz	Bi1.6Pb0.3Te0.1Sr2Ca3Cu4Oz	Bi	1.6	Pb	0.3	Te	0.1	Sr	2	Ca	3	Cu	4									O	z		2	1994																												Bi2223																		K	102.7						102.7																				T		76.2							T/K		1.05			HIR4921		A		21																																																									1	ANN(835C, 192H in air)					Superconducting and magnetic properties of melt-quenched Bi-2223 superconductors doped with Pb and Te	199405			Physica C, 225(1994)149-157	A.Zaleski,E.S.Vlakhov,K.A.Nenkov,M.Ciszek,Y.B.Dimitriev	Bi,Sr,Ca,Cu,O,Pb,Te	
4922	PHC2230057	non-superconducting phase included, sp.heat C=A*T**(-2)+a*T+b*T**3 for 2<T<20K, A=6.6 E-2 J.K/mole	Bi2(Sr,Bi)2CuO4	Bi2.1Sr1.9Cu1Oz	Bi	2.1	Sr	1.9	Cu	1															O	z		2	1994			emu.K/mole	0.004																								Bi2201																		K		7					7																																																								mJ/K2fu	0.1	from sp.heat	211	from sp.heat measurement																																		Bi2O3,PbO,SrCO3,CuO	1	mixture-CAL(800C,24H in air)-SIN(850C,52H in air)-FC to RT					The specific heat of the 2201 BISCO high-Tc superconductor	199404			Physica C, 223(1994)57-61	J.P.Franck,M.K.Yu	Bi,Cu,O,Sr	
4923	PHC2230057	sp.heat C=A*T**(-2)+a*T+b*T**3, A=7.0**(-2) J.K/mole	Bi2(Sr,Pb,Bi)2Cu1O4	Bi2.05Pb0.05Sr1.9Cu1Oz	Bi	2.05	Pb	0.05	Sr	1.9	Cu	1													O	z		1	1994																												Bi2201																		K		10.5					10.5																																																								mJ/K2fu	0.3	from sp.heat	206	from sp.heat																																		Bi2O3,PbO,SrCO3,CuO	1	mixture-CAL(800C,24H in air)-SIN(850C,52H in air)-FC to RT					The specific heat of the 2201 BISCO high-Tc superconductor	199404			Physica C, 223(1994)57-61	J.P.Franck,M.K.Yu	Bi,Cu,O,Sr	
4924	PHC2310167		(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.9Cd0.1Sr2Y0.5Ca0.5Cu2Oz	Pb	0.9	Cd	0.1	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		1	1994																											2	Pb1212	P4/mmm		A	3.83		11.958												K			18				18																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,8H in air)-pellet-SIN(950C,2H +1000C,2H in flowing O2)-cool to RT at 1C/min - ANN(560C,1H in air)					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4925	PHC2310167		(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.8Cd0.2Sr2Y0.5Ca0.5Cu2Oz	Pb	0.8	Cd	0.2	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		1	1994																											2	Pb1212			A	3.829		11.951												K			22.5				22.5																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,*H in air)-pellet-SIN(950C,2H+1000C,2H in flowing O2)-cool to RT at 1C/min					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4926	PHC2310167		(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.7Cd0.3Sr2Y0.5Ca0.5Cu2Oz	Pb	0.7	Cd	0.3	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		1	1994																											2	Pb1212			A	3.827		11.929												K			26.5				26.5																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,*H in air)-pellet-SIN(950C,2H+1000C,2H in flowing O2)-cool to RT at 1C/min					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4927	PHC2310167		(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.6Cd0.4Sr2Y0.5Ca0.5Cu2Oz	Pb	0.6	Cd	0.4	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		1	1994																											2	Pb1212			A	3.825		11.905												K			22.5				22.5																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,*H in air)-pellet-SIN(950C,2H+1000C,2H in flowing O2)-cool to RT at 1C/min					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4928	PHC2310167	impurity phase=SrPbO3	(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.5Cd0.5Sr2Y0.5Ca0.5Cu2Oz	Pb	0.5	Cd	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		2	1994																											2	Pb1212			A	3.822		11.892												K			22.5				22.5																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,*H in air)-pellet-SIN(950C,2H+1000C,2H in flowing O2)-cool to RT at 1C/min					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4929	PHC2310167	Pb1212 phase + impurity phase(SrPbO3)	(Pb,Cd)Sr2(Y,Ca)Cu2Oz	Pb0.4Cd0.6Sr2Y0.5Ca0.5Cu2Oz	Pb	0.4	Cd	0.6	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	z		2	1994																											2	Pb1212			A	3.822		11.887												K			22.5				22.5																																																																																														PbO,CdO,SrCO3,CaCO3,Y2O3,CuO	1	mixture-CAL(880C,*H in air)-pellet-SIN(950C,2H+1000C,2H in flowing O2)-cool to RT at 1C/min					Superconductivity in Cd-doped Pb-based layered copper oxides,(Pb1-xCdx)Sr2(Y0.5Ca0.5)Cu2Oy	199409			Physica C 231 (1994)167-171	H,Jin,K.Q.Ruan,L.Z.Cao,N.L.Wang,Y.Cheng,Z.J.Ghen	Cd,Pb,Sr,Y,Ca,Cu,O	
4930	SSC0850037	oxygen content by Raman spectroscopy	YBa2(Cu,In)3O7	Y1Ba2Cu2.7In0.3O6.9	Y	1	Ba	2	Cu	2.7	In	0.3													O	z	6.9		1993																												Y123																		K		90					90																																																																																																					THE CONNECTION BETWEEN THE OXYGEN CONTENT AND IONIC RADIUS OF DOPANTS SUBSTITUTING Cu(1) IN Y(123)			Institute of Inorganic Chemistry, Russian Academy of Sciences, Novosibirsk, 630090, Lavrentyev av., Russia	Solid State Commun.,85(1993)37-38	B.A. Kolesov,L.I. Yudanova,L.P. Kozeeva		
4931	PR0468687	Hall effect measured at 100mA, H=8T, 80<T<300K	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1992																												T																																																																																																																				RH4931				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4932	PR0468687		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.992Fe0.008O4	La	1.85	Sr	0.15	Cu	0.992	Fe	0.008													O	4		1	1992																												T																																																																																																																								1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4933	PR0468687		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.982Fe0.018O4	La	1.85	Sr	0.15	Cu	0.982	Fe	0.018													O	4		1	1992																												T																																																																																																																				RH4933				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4934	PR0468687		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.973Fe0.027O4	La	1.85	Sr	0.15	Cu	0.973	Fe	0.027													O	4		1	1992																												T																																																																																																																				RH4934				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4935	PR0468687		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.979Zn0.021O4	La	1.85	Sr	0.15	Cu	0.979	Zn	0.021													O	4		1	1992																												T																																																																																																																				RH4935				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4936	PR0468687		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.963Zn0.037O4	La	1.85	Sr	0.15	Cu	0.963	Zn	0.037													O	4		1	1992																												T																																																																																																																				RH4936				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4937	PR0468687		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.992Co0.008O4	La	1.85	Sr	0.15	Cu	0.992	Co	0.008													O	4		1	1992																												T																																																																																																																				RH4937				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4938	PR0468687		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.979Co0.021O4	La	1.85	Sr	0.15	Cu	0.979	Co	0.021													O	4		1	1992																												T																																																																																																																				RH4938				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4939	PR0468687		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.97Co0.03O4	La	1.85	Sr	0.15	Cu	0.97	Co	0.03													O	4		1	1992																												T																																																																																																																				RH4939				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4940	PR0468687		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.99Ga0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ga	0.01													O	4		1	1992																												T																																																																																																																				RH4940				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4941	PR0468687		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.98Ga0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ga	0.02													O	4		1	1992																												T																																																																																																																				RH4941				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4942	PR0468687		(La,Sr)2(Cu,Ga)O4	La1.85Sr0.15Cu0.975Ga0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ga	0.025													O	4		1	1992																												T																																																																																																																				RH4942				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4943	PR0468687		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4		1	1992																												T																																																																																																																				RH4943				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4944	PR0468687		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.94Ni0.06O4	La	1.85	Sr	0.15	Cu	0.94	Ni	0.06													O	4		1	1992																												T																																																																																																																				RH4944				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4945	PR0468687		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.94Ni0.06O4	La	1.85	Sr	0.15	Cu	0.94	Ni	0.06													O	4		1	1992																												T																																																																																																																				RH4945				1	see Phys.Rev.B, 42(1990)8752					UNIVERSAL HALL EFFECT IN LA1.85SR0.15CU1-XAXO4 SYSTEMS (A=FE,CO,NI,ZN,GA)	199210		DEPARTMENT OF PHYSICS, BROWN UNIVERSITY, RHODE ISLAND	PHYS.REV.B,46(1992)8687	GANG XIAO,MARTA Z. CIEPLAK,PENG XIONG	LA,SR,CU,O,FE,CO,NI,ZN,GA	
4946	PHC2250051	Hc1 value in DB is for intra-grain, for intergrain Hc1=9 Oe	Dy(Ba,Sr)2Cu3O7	Dy1Ba1Sr1Cu3O6.9	Dy	1	Ba	1	Sr	1	Cu	3													O	z	6.9		1994																											3	Y123																		K	73		81.1				77.05											Oe	defined as deviation from linearity in M vs H curves	620																																																										m.ohm.cm											21												Dy2O3,CuO,Sr-nitrate,BaCO3	1	mixture-CAL(900-950C in flowing O2)-reground-pellet-SIN-ANN(950C,15H + 420C,12H in flowing O2)-cool to RT,for different O2 content ANN(898,650,570C in air)					Influence of strontium on superconducting and magnetic properties of DyBa2-xSrxCu3O7-z	199405			Physica C, 225(1994)51-58	H.Szymczak,N.A.Doroshenko,R.Puzniak,V.I.Markovich,V.P.Dyakonov,Ya.I.Yuzhelevskii	Dy,Ba,Sr,Cu,O	
4947	PHC2250051		Dy(Ba,Sr)2Cu3O7	Dy1Ba1Sr1Cu3O6.7	Dy	1	Ba	1	Sr	1	Cu	3													O	z	6.7		1994																												Y123																		K	24.6		35.2				29.9																																																																							m.ohm.cm											23												Dy2O3,CuO,Sr-nitrate,BaCO3	1	mixture-CAL(900-950C in flowing O2)-reground-pellet-SIN-ANN(950C,15H + 420C,12H in flowing O2)-cool to RT,for different O2 content ANN(898,650,570C in air)					Influence of strontium on superconducting and magnetic properties of DyBa2-xSrxCu3O7-z	199405			Physica C, 225(1994)51-58	H.Szymczak,N.A.Doroshenko,R.Puzniak,V.I.Markovich,V.P.Dyakonov,Ya.I.Yuzhelevskii	Dy,Ba,Sr,Cu,O	
4948	PHC2250051		Dy(Ba,Sr)2Cu3Oz	Dy1Ba1Sr1Cu3O6.6	Dy	1	Ba	1	Sr	1	Cu	3													O	z	6.6		1994																												Y123																		K	9.5		20.2				14.85																																																																							m.ohm.cm											41												Dy2O3,CuO,Sr-nitrate,BaCO3	1	mixture-CAL(900-950C in flowing O2)-reground-pellet-SIN-ANN(950C,15H + 420C,12H in flowing O2)-cool to RT,for different O2 content ANN(898,650,570C in air)					Influence of strontium on superconducting and magnetic properties of DyBa2-xSrxCu3O7-z	199405			Physica C, 225(1994)51-58	H.Szymczak,N.A.Doroshenko,R.Puzniak,V.I.Markovich,V.P.Dyakonov,Ya.I.Yuzhelevskii	Dy,Ba,Sr,Cu,O	
4949	PHC2250051		Dy(Ba,Sr)2Cu3O7	Dy1Ba1Sr1Cu3O6.4	Dy	1	Ba	1	Sr	1	Cu	3													O	z	6.4		1994																												Y123																		K					10																																																																									m.ohm.cm											180												Dy2O3,CuO,Sr-nitrate,BaCO3	1	mixture-CAL(900-950C in flowing O2)-reground-pellet-SIN-ANN(950C,15H + 420C,12H in flowing O2)-cool to RT,for different O2 content ANN(898,650,570C in air)					Influence of strontium on superconducting and magnetic properties of DyBa2-xSrxCu3O7-z	199405			Physica C, 225(1994)51-58	H.Szymczak,N.A.Doroshenko,R.Puzniak,V.I.Markovich,V.P.Dyakonov,Ya.I.Yuzhelevskii	Dy,Ba,Sr,Cu,O	
4950	PHC2250051	Hc1 value in DB is for intra-grain, for intergrain Hc1=24Oe	Dy(Ba,Sr)2Cu3O7	Dy1Ba1.5Sr0.5Cu3O6.9	Dy	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.9		1994																												Y123																		K	85.3		87.3				86.3											Oe	defined as deviation from linearity in M vs H curves	420																																																										m.ohm.cm											6.4												Dy2O3,CuO,Sr-nitrate,BaCO3	1	mixture-CAL(900-950C in flowing O2)-reground-pellet-SIN-ANN(950C,15H + 420C,12H in flowing O2)-cool to RT,for different O2 content ANN(898,650,570C in air)					Influence of strontium on superconducting and magnetic properties of DyBa2-xSrxCu3O7-z	199405			Physica C, 225(1994)51-58	H.Szymczak,N.A.Doroshenko,R.Puzniak,V.I.Markovich,V.P.Dyakonov,Ya.I.Yuzhelevskii	Dy,Ba,Sr,Cu,O	
4951	PHC2330061	Tq=400C	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O7	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	z	7	1	1994																											2	Y123			A	3.861		11.669												K	80.5						80.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4952	PHC2330061	Tq=500C	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.8	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	z	6.8	1	1994																											2	Y123			A	3.864		11.701												K	48						48																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4953	PHC2330061	Tq=600C	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.72	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	z	6.72	1	1994																											2	Y123			A	3.864		11.719												K	33						33																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4954	PHC2330061	Tq=700C	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.62	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	z	6.62	1	1994																											2	Y123			A	3.865		11.736												K	4.2						4.2																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4955	PHC2330061	Tq=800C, not s/c	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.9Fe0.1O6.52	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	z	6.52	1	1994																											2	Y123																		K					4.2																																																																																																Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4956	PHC2330061	Tq=400C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O7	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	7	1	1994																											3	Y123			A	3.822	3.888	11.665												K	81.5						81.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4957	PHC2330061	Tq=450C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.88	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.88	1	1994																											3	Y123																		K	69.5						69.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4958	PHC2330061	Tq=500C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.85	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.85	1	1994																											3	Y123			A	3.825	3.889	11.684												K	54.5						54.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4959	PHC2330061	Tq=550C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.77	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.77	1	1994																											3	Y123			A	3.828	3.887	11.682												K	44						44																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4960	PHC2330061	Tq=650C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.71	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.71	1	1994																											3	Y123			A	3.833	3.887	11.682												K	29						29																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4961	PHC2330061	Tq=700C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.61	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.61	1	1994																											3	Y123			A	3.839	3.881	11.722												K	20.5						20.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4962	PHC2330061	Tq=750C	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.56	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.56	1	1994																											3	Y123			A	3.841	3.88	11.722												K	4.3						4.3																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4963	PHC2330061	Tq=800C, not s/c	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.9Ni0.1O6.48	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	z	6.48	1	1994																											3	Y123																		K					4.2																																																																																																Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4964	PHC2330061	Tq=400C	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O7	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	z	7	1	1994																											3	Y123			A	3.825	3.891	11.674												K	51.5						51.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4965	PHC2330061	Tq=450C	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.99	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	z	6.99	1	1994																											3	Y123			A	3.826	3.889	11.678												K	43.5						43.5																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4966	PHC2330061	Tq=500C	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.93	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	z	6.93	1	1994																											3	Y123			A	3.828	3.89	11.687												K	23						23																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4967	PHC2330061	Tq=550C	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.88	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	z	6.88	1	1994																											3	Y123			A	3.833	3.891	11.702												K	4.3						4.3																																																																																														Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4968	PHC2330061	Tq=600C, not s/c	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O6.82	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	z	6.82	1	1994																											3	Y123			A	3.83	3.893	11.691												K					4.2																																																																																																Y2O3,BaCO3,NiO,ZnO,Fe2O3,CuO	1	mixture-fire(940C,20H in air)-pellet-SIN(940C,6H)-slow cool to 400C - ANN(400C,16H in flowing O2)-cool to RT, different oz from different quenching temp. see commt column					On the distinct Tc decrease behaviours in Fe,Ni and Zn doped YBa2Cu3O7-z	199411			Physica C,233 (1994) 61-66	Nianhua Peng,W.Y.Liang	Y,Ba,Cu,O,Fe,Ni,Zn	
4969	PHC2320269	550C,30H in 8 atm O2	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		3.46					3.46																																																								mJ/K2fu	7.5		212	C=A*T+B*T**3+C*T**5+D*T**(-2)																																		Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4970	PHC2320269	200C,12H in vacuum	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		7.05					7.05																																																								mJ/K2fu	4.89		202																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4971	PHC2320269	200C,24H in vacuum	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		5.33					5.33																																																								mJ/K2fu	2.39		203																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4972	PHC2320269	200C,36H in vacuum	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K																																																															mJ/K2fu		gamma=0.0 mJ/K2.mole	201																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4973	PHC2320269	200C,18H in 1 atm O2	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		5.74					5.74																																																								mJ/K2fu	4.86		206																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4974	PHC2320269	200C,36H in 1 atm O2	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		6.05					6.05																																																								mJ/K2fu	5.75		209																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4975	PHC2320269	200C,54H in 1 atm O2	Bi2Sr2CuO6	Bi2.1Sr1.85Cu1O6-z	Bi	2.1	Sr	1.85	Cu	1															O	6-z		1	1994																												Bi2201																		K		5.46					5.46																																																								mJ/K2fu	6.27		208																																			Bi2O3,Sr2CO3,CuO2	1	best quarity samples were formed by usual solid state reaction method. final heat treatment are  described  in COMMT column					Low-temperature specific-heat studies of Bi-Sr-Cu-O	199410			Physica C,232 (1994) 269-276	Izumi Hirabayashi,Tetushi Okamoto,Uichiro Mizutani,Yuh Yamada	Bi,Sr,Cu,O	
4976	PHC2320136	small amount of 2212 phase	(Bi,Pb,)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O9.91	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	z	9.91		1994																											2	Bi2223			A	5.399		36.97																																																																																						0.6			TP4976																									1	usual ceramic technique					Normal state thermoelectric power of vanadium-substitued(Bi0.8Pb0.2-yVy)2Sr2Ca2Cu3Ox superconducting pellets	199410			Physica C, 232 (1994) 136-144	Bitasta Chanda,S.K.Chatak,T.K.Dey	Bi,Pb,V,Sr,Ca,Cu,O	
4977	PHC2320136		(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.35V0.05Sr2Ca2Cu3O9.92	Bi	1.6	Pb	0.35	V	0.05	Sr	2	Ca	2	Cu	3									O	z	9.92		1994																											2	Bi2223			A	5.403		36.983																																																																																						0.84			TP4977																									1	usual ceramic technique					Normal state thermoelectric power of vanadium-substitued(Bi0.8Pb0.2-yVy)2Sr2Ca2Cu3Ox superconducting pellets	199410			Physica C, 232 (1994) 136-144	Bitasta Chanda,S.K.Chatak,T.K.Dey	Bi,Pb,V,Sr,Ca,Cu,O	
4978	PHC2320136		(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.3V0.1Sr2Ca2Cu3O9.92	Bi	1.6	Pb	0.3	V	0.1	Sr	2	Ca	2	Cu	3									O	z	9.92		1994																											2	Bi2223			A	5.406		36.975																																																																																						1.36			TP4978																									1	usual ceramic technique					Normal state thermoelectric power of vanadium-substitued(Bi0.8Pb0.2-yVy)2Sr2Ca2Cu3Ox superconducting pellets	199410			Physica C, 232 (1994) 136-144	Bitasta Chanda,S.K.Chatak,T.K.Dey	Bi,Pb,V,Sr,Ca,Cu,O	
4979	PHC2320136		(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.25V0.15Sr2Ca2Cu3O9.91	Bi	1.6	Pb	0.25	V	0.15	Sr	2	Ca	2	Cu	3									O	z	9.91		1994																											2	Bi2223			A	5.409		36.978																																																																																						1.89			TP4979																									1	usual ceramic technique					Normal state thermoelectric power of vanadium-substitued(Bi0.8Pb0.2-yVy)2Sr2Ca2Cu3Ox superconducting pellets	199410			Physica C, 232 (1994) 136-144	Bitasta Chanda,S.K.Chatak,T.K.Dey	Bi,Pb,V,Sr,Ca,Cu,O	
4980	PHC2320075	Bi2Sr2CuO6(Sr2CuO2CO3)n  n=3	Bi2Sr2CuO6(Sr2CuO2CO3)3	Bi2Sr8Cu4C3O21	Bi	2	Sr	8	Cu	4	C	3													O	21			1994																															A	5.494	5.478	69.49												K		34		34			34										7																																																																																				Bi2O3,SrCO3,CuO		mixture-wrapped in Au sheet -heat(910C,1H in air)-Q to RT					The 34 superconductor Bi2-xPbxSr8Cu4(CO3)3O12.A new oxycarbonate, third member of the series (Bi2-xPbxSr2CuO6)(Sr2CuO2CO3)n	199410			Physica C,232 (1994) 75-81	A.Maignan,B.Ravesu,C.Michel,D.Pelloquin,M.Hervieu,M.T.Caldes	Bi,Pb,Sr,Cu,C,O	
4981	PHC2320075	Bi2Sr2CuO6(Sr2CuO2CO3)n   n=1	Bi2Sr2CuO6(Sr2CuO2CO3)	Bi2Sr8Cu4C3O21	Bi	2	Sr	8	Cu	4	C	3													O	21			1994																																														K		30		30			30																																																																																														Bi2O3,SrCO3,CuO		mixture-wrapped in Au sheet -heat(910C,1H in air)-Q to RT					The 34 superconductor Bi2-xPbxSr8Cu4(CO3)3O12.A new oxycarbonate, third member of the series (Bi2-xPbxSr2CuO6)(Sr2CuO2CO3)n	199410			Physica C,232 (1994) 75-81	A.Maignan,B.Ravesu,C.Michel,D.Pelloquin,M.Hervieu,M.T.Caldes	Bi,Pb,Sr,Cu,C,O	
4982	PHC2320075	Bi2Sr2CuO6(Sr2CuO2CO3)n  n=2	Bi2Sr2CuO6(Sr2CuO2CO3)2	Bi2Sr8Cu4C3O21	Bi	2	Sr	8	Cu	4	C	3													O	21			1994																																														K		40		40			40																																																																																														Bi2O3,SrCO3,CuO		mixture-wrapped in Au sheet -heat(910C,1H in air)-Q to RT					The 34 superconductor Bi2-xPbxSr8Cu4(CO3)3O12.A new oxycarbonate, third member of the series (Bi2-xPbxSr2CuO6)(Sr2CuO2CO3)n	199410			Physica C,232 (1994) 75-81	A.Maignan,B.Ravesu,C.Michel,D.Pelloquin,M.Hervieu,M.T.Caldes	Bi,Pb,Sr,Cu,C,O	
4983	PHC2250025	oz by iodometry	Nd(Ba,Nd)2Cu3O7	Nd1Ba2Cu3O6.81	Nd	1	Ba	2	Cu	3															O	z	6.81	1	1994																											3	Y123			A	3.863	3.916	11.745														91.7		91.7			91.7																																																																																														Nd2O3,CuO,BaCO3	1	mixture-pellet-ANN(950C,50H)-ANN(400C,20H in flowing O2)					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4984	PHC2250025		Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3O6.91	Nd	1.2	Ba	1.8	Cu	3															O	z	6.91	1	1994																											2	Y123			A	3.89		11.684												K		47.6	57.9	47.6			47.6																																																																																														Nd2O3,CuO,BaCO3	1	mixture-pellet-ANN(950C,50H)-ANN(400C,20H in flowing O2)					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4985	PHC2250025	not s/c	Nd(Ba,Nd)2Cu3O7	Nd1.5Ba1.5Cu3O7.05	Nd	1.5	Ba	1.5	Cu	3															O	z	7.05	1	1994																											2	Y123			A	3.88		11.636																																																																																																																	Nd2O3,CuO,BaCO3	1	mixture-pellet-ANN(950C,50H)-ANN(400C,20H in flowing O2)					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4986	PHC2250025	not s/c	Nd(Ba,Nd)2Cu3O7	Nd1.7Ba1.3Cu3O7.15	Nd	1.7	Ba	1.3	Cu	3															O	z	7.15	1	1994																											2	Y123			A	3.883		11.541																																																																																																																	Nd2O3,CuO,BaCO3	1	mixture-pellet-ANN(950C,50H)-ANN(400C,20H in flowing O2)					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4987	JML0111639		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1992																												Y123																																																																																																																							Y2O3,BaCO3,CuO,(Nb2O5)	1	mixture-CAL(1175K,overnight in air)-SIN(1223K,12H in air)-cool to RT					Substitution of copper by niobium in superconducting YBa2Cu3O7-d				J.Mater.Sci.Lett.,11(1992)1639	A.M. GEORGE,C.G.S. PILLAI		
4988	JML0111639	Y123+YBa2NbO6+CuO	YBa2(Cu,Nb)3O7	Y1Ba2Cu2.98Nb0.02O7-z	Y	1	Ba	2	Cu	2.98	Nb	0.02													O	7-z		2	1992																												Y123																																																																																																																							Y2O3,BaCO3,CuO,(Nb2O5)	1	mixture-CAL(1175K,overnight in air)-SIN(1223K,12H in air)-cool to RT					Substitution of copper by niobium in superconducting YBa2Cu3O7-d				J.Mater.Sci.Lett.,11(1992)1639	A.M. GEORGE,C.G.S. PILLAI		
4989	JML0111639	Y123+YBa2NbO6+CuO, volume of YBa2NbO6 increases as increasing Nb content	YBa2(Cu,Nb)3O7	Y1Ba2Cu2.95Nb0.05O7-z	Y	1	Ba	2	Cu	2.95	Nb	0.05													O	7-z		2	1992																												Y123																																																																																																																							Y2O3,BaCO3,CuO,(Nb2O5)	1	mixture-CAL(1175K,overnight in air)-SIN(1223K,12H in air)-cool to RT					Substitution of copper by niobium in superconducting YBa2Cu3O7-d				J.Mater.Sci.Lett.,11(1992)1639	A.M. GEORGE,C.G.S. PILLAI		
4990	PHC2270001	sample contains impurity phases of 20 wt% Hg1256 and 2 wt% CaO, structure analysis by neutron diffraction	HgBa2Ca4Cu5O12	Hg1Ba2Ca4Cu5O12.32	Hg	1	Ba	2	Ca	4	Cu	5													O	12+z	12.32		1994																												Hg1245	p4/mmm		A	3.851		22.107																																																																																																																	Ba(NO3)2,Ca(NO3)2.4H2O,Cu(NO3).3H2O,HgO		precursor from powder mixture without Hg-(+HgO)-press in Au cupsule-18kbar, 20min-heat(900C,1.6H)-power off-press off					Neutron powder diffraction study of the crystal structure of HgBa2Ca4Cu5O12+z at room temperature and at 10K	199406			Physica C, 227(1994)1-9	A.Santoro,C.Chaillout,J.J.Capponi,J.L.Tholence,M.Marezio,O.Chmaissem,Q.Huang	Hg,Ba,Ca,Cu,O	
4991	PHC2320075		(Bi,Pb)2Sr8Cu4(CO3)3O12	Bi1.75Pb0.25Sr8Cu4C3O21	Bi	1.75	Pb	0.25	Sr	8	Cu	4	C	3											O	21		1	1994																											3		Fmmm		A	5.499	5.478	69.507																																																																																																																	Bi2O3,PbO,SrCO3,Sr2CuO3,CuO	1	mixture-heat(810C,4H in evacuated silica tube) -Q to RT					The 34 superconductor Bi2-xPbxSr8Cu4(CO3)3O12.A new oxycarbonate, third member of the series (Bi2-xPbxSr2CuO6)(Sr2CuO2CO3)n	199410			Physica C,232 (1994) 75-81	A.Maignan,B.Ravesu,C.Michel,D.Pelloquin,M.Hervieu,M.T.Caldes	Bi,Pb,Sr,Cu,C,O	
4992	PHC2250025		Nd(Ba,Nd)2Cu3O7	Nd1.05Ba1.95Cu3O6.68	Nd	1.05	Ba	1.95	Cu	3															O	7	6.68	3	1994									6.635																		2	Y123	p4/mmm		A	3.9		11.785																																																																																																																			mixture was placed in a BeO crucible-heat(1100C,4H)-cool to 900C at 10C/H-FC to RT					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4993	PHC2250025		Nd(Ba,Nd)2Cu3O7	Nd1.22Ba1.78Cu3O6.84	Nd	1.22	Ba	1.78	Cu	3															O	7	6.84	3	1994									6.763																		2	Y123	p4/mmm		A	3.892		11.677																																																																																																																			mixture was placed in a BeO crucible-heat(1100C,4H)-cool to 900C at 10C/H-FC to RT					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4994	PHC2250025		Nd(Ba.Nd)2Cu3O7	Nd1.42Ba1.58Cu3O6.94	Nd	1.42	Ba	1.58	Cu	3															O	7	6.94	3	1994									6.816																		2	Y123	p4/mmm		A	3.899		11.588																																																																																																																			mixture was placed in a BeO crucible-heat(1100C,4H)-cool to 900C at 10C/H-FC to RT					The structures of Nd1+xBa2-xCu3O7-z (x=0.05,0.22,0.42) phases refined from X-ray single-crystal data	199405			Physica C, 225(1994)25-33	A.V.Mironov,D.V.Fomichev,E.V.Antipov,O.G.D'yachenko	Nd,Ba,Cu,O	
4996	PR05013744		YBa2(CU,Ni,Zn)3O7	Y1Ba2Cu2.85Ni0.075Zn0.075O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.075	Zn	0.075											O	7-z		1	1994																												Y123																		K		58					58																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
4997	PR05013744		YBa2(Cu,Ni,Zn)3O7	Y1Ba2Cu2.85Ni0.101Zn0.049O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.101	Zn	0.049											O	7-z		1	1994																												Y123																		K		62					62																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
4998	PR05013744		YBa2(Cu,Ni,Zn)3O7	Y1Ba2Cu2.85Ni0.124Zn0.025O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.124	Zn	0.025											O	7-z		1	1994																												Y123																		K		64.6					64.6																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
4999	PR05013744		YBa2(cu,Ni)3O7	Y1Ba2Cu285Ni0.15O7-z	Y	1	Ba	2	Cu	285	Ni	0.15													O	7-z		1	1994																												Y123																		K		73.4					73.4																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
5000	PR0478089	twinned rectangular bar,unload pressure=0.36GPa. Tc(P=0.36Gpa)=89.99K. Tc(max)=95.8K(P=10.3GPa)	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1993																											3	Y123																		K		87.7					87.7			K/GPa	0.64																																																																			m.ohm.cm												0.485													grown in irconia crucible					VARIATION OF THE AB-PLANE NORMAL-STATE RESISTANCE AND THE SUPERCONDUCTING TRANSITION TEMPERATURE OF A YBA2CU3O7-Z SINGLE CRYSTAL TO PRESSURES OF 13 GPA	199304			PHYS.REV.B,47(1993)8089	E.M.MCCARRON III,J.L.KOSTON,S.W.TOZER	Y,BA,CU,O	
5001	SSC0850501	0.4<x<0.4, K-content not measured	(Ba,K)BiO3	Ba1K1Bi1O3	Ba	1	K	1	Bi	1															O	3		3	1993																												BKBO																		K		30.9				0.8	30.9																																																											233	from resis											m.ohm.cm											1.11			m3/C	-0.00000000122					RH5001					electrochemical synthesis, see SSC0780967					TRANSPORT PROPERTIES OF BA1-XKXBIO3 SINGLE CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)501	C.ESCRIBE-FILIPPINI,J.MARCUS,M.AFFRONTE	BA,K,BI,O	
5002	SSC0850501	K-content not measured	(Ba,K)BiO3	Ba1K1Bi1O3	Ba	1	K	1	Bi	1															O	3		3	1993																												BKBO																		K		28				2.5	28																																																																							ohm.cm											3.75			m3/C	-0.00000000273					RH5002			KOH,Bi2O3,Ba(OH)2.8H2O	5	flux method, mixture of raw powders using ZrO2 crucible-heat(100C/H) to 200C-heat(80C/H) to 430C-cool(100C/H)					TRANSPORT PROPERTIES OF BA1-XKXBIO3 SINGLE CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)501	C.ESCRIBE-FILIPPINI,J.MARCUS,M.AFFRONTE	BA,K,BI,O	
5003	SSC0850501	K-content not measured	(Ba,K)BiO3	Ba1K1Bi1O3	Ba	1	K	1	Bi	1															O	3		3	1993																												BKBO																		K		32				0.2	32																																																											224	from resis											m.ohm.cm											1.71			m3/C	-0.00000000336					RH5003			KOH+RbOH,Bi2O3,Ba(OH)2.8H2O	5	same as 5002					TRANSPORT PROPERTIES OF BA1-XKXBIO3 SINGLE CRYSTALS	199302			SOLID STATE COMMUN.,85(1993)501	C.ESCRIBE-FILIPPINI,J.MARCUS,M.AFFRONTE	BA,K,BI,O	
5004	SSC0870213		(Pr,Ce)2CuO4	Pr1.87Ce0.13Cu1O4-z	Pr	1.87	Ce	0.13	Cu	1															O	4-z		1	1993																											2	T'																		K		17		17			17																																																																						TP5004																								Pr6O11,CeO2,CuO	1	mixture-(950C,14H in air)-pellet-(1100C,18H in air)-cool to RT(20C/min)-reduce(920C,7H in vac)-cool to RT(10C/min)					THERMOELECTRIC POWER OF PR2-YCEYCUO4-Z SUPERCONDUCTORS WITH VARIOUS CONTENT OF CE				SOLID STATE COMMUN.,87(1993)213	G.KH.PANOVA,J.A.ARNOLD,J.TOTH,M.N.KHLOPKIN,N.A.BABUSHKINA,R.O.ZAITSEV,S.E.VOINOVA	PR,CE,CU,O	
5005	SSC0870213		(Pr,Ce)2CuO4	Pr1.86Ce0.14Cu1O4-z	Pr	1.86	Ce	0.14	Cu	1															O	4-z		1	1993																											2	T'																		K		25		25			25																																																																						TP5005																								Pr6O11,CeO2,CuO	1	mixture-(950C,14H in air)-pellet-(1100C,18H in air)-cool to RT(20C/min)-reduce(920C,7H in vac)-cool to RT(10C/min)					THERMOELECTRIC POWER OF PR2-YCEYCUO4-Z SUPERCONDUCTORS WITH VARIOUS CONTENT OF CE				SOLID STATE COMMUN.,87(1993)213	G.KH.PANOVA,J.A.ARNOLD,J.TOTH,M.N.KHLOPKIN,N.A.BABUSHKINA,R.O.ZAITSEV,S.E.VOINOVA	PR,CE,CU,O	
5006	SSC0870213		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-z	Pr	1.85	Ce	0.15	Cu	1															O	4-z		1	1993																											2	T'																		K		22.5		22.5			22.5																																																																						TP5006																								Pr6O11,CeO2,CuO	1	mixture-(950C,14H in air)-pellet-(1100C,18H in air)-cool to RT(20C/min)-reduce(920C,7H in vac)-cool to RT(10C/min)					THERMOELECTRIC POWER OF PR2-YCEYCUO4-Z SUPERCONDUCTORS WITH VARIOUS CONTENT OF CE				SOLID STATE COMMUN.,87(1993)213	G.KH.PANOVA,J.A.ARNOLD,J.TOTH,M.N.KHLOPKIN,N.A.BABUSHKINA,R.O.ZAITSEV,S.E.VOINOVA	PR,CE,CU,O	
5007	SSC0870213		(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O4-z	Pr	1.83	Ce	0.17	Cu	1															O	4-z		1	1993																											2	T'																		K		12		12			12																																																																						TP5007																								Pr6O11,CeO2,CuO	1	mixture-(950C,14H in air)-pellet-(1100C,18H in air)-cool to RT(20C/min)-reduce(920C,7H in vac)-cool to RT(10C/min)					THERMOELECTRIC POWER OF PR2-YCEYCUO4-Z SUPERCONDUCTORS WITH VARIOUS CONTENT OF CE				SOLID STATE COMMUN.,87(1993)213	G.KH.PANOVA,J.A.ARNOLD,J.TOTH,M.N.KHLOPKIN,N.A.BABUSHKINA,R.O.ZAITSEV,S.E.VOINOVA	PR,CE,CU,O	
5008	PR0481211		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.95Ce0.05Cu2O8	Bi	2	Sr	2	Ca	0.95	Ce	0.05	Cu	2											O	8		1	1993																											2	Bi2212																			80						80																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5009	PR0481211		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.9Ce0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Ce	0.1	Cu	2											O	8		1	1993																											2	Bi2212			A		5.39	30.579													57.3		93.61				75.455																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5010	PR0481211		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.8Ce0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Ce	0.2	Cu	2											O	8		1	1993																											2	Bi2212			A	5.369	5.38	30.521													17						17																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5011	PR0481211		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.7Ce0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Ce	0.3	Cu	2											O	8		1	1993																											2	Bi2212			A	5.354	5.37	30.394																																																																																																																		1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5012	PR0481211		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1993																											2	Bi2212			A			30.674													89.3						89.3																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5013	PR0481211		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.95Pr0.05Cu2O8	Bi	2	Sr	2	Ca	0.95	Pr	0.05	Cu	2											O	8		1	1993																											2	Bi2212			A	5.38	5.39	30.62													72.1		94.2				83.15																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5014	PR0481211		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.9Pr0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Pr	0.1	Cu	2											O	8		1	1993																											2	Bi2212				5.37		30.542													60.5						60.5																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5015	PR0481211		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.85Pr0.15Cu2O8	Bi	2	Sr	2	Ca	0.85	Pr	0.15	Cu	2											O	8		1	1993																											2	Bi2212				5.37	5.38	30.498													42.2		94.5				68.35																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5016	PR0481211		(Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8		1	1993																											2	Bi2212					5.391	30.44													27.1		89.8				58.45																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5017	PR0481211		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.7Pr0.3Cu2O8	Bi	2	Sr	2	Ca	0.7	Pr	0.3	Cu	2											O	8		1	1993																											2	Bi2212				5.366	5.385	30.361													7.1		53.5				30.3																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5018	PR0481211		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8		1	1993																											2	Bi2212					5.369	30.268															43.4				43.4																																																																																															1	CAL(820+830+840C,12H)-press-pellet-SIN(930-980C,860C,12H in air)-Q to RT					SUPERCONDUCTIVITY IN PR- AND CE-DOPED BI2CASR2CU2OY SYSTEMS	199307			PHYS.REV.B,48(1993)1211	A.V.NARLIKAR,M.P.DAS,S.K.AGARWAL,V.P.S.AWANA		
5019	PR0475367	Neel Temp by Mossbauer effect of Fe(57),1% Fe doped sample	La2Sr6Cu8O16	La2Sr6Cu8O16	La	2	Sr	6	Cu	8															O	16		1	1993								295																			2		p4/mbm		A	11.043		3.64												K					4.2																																																																																																La2O3,SrCO3,CuO,Fe(57)2O3	1	mixture-CAL(900C,24H in air)-pellet-SIN(1000C or 1050C,24H)-Q in air-ANN(800C in air)-slow cool to RT					OXYGEN DEPENDENCE OF THE ANTIFERROMAGNETIC ORDER IN LA8-XSRXCU8OY	199303			PHYS.REV.B,47(1993)5367	D.HECHEL,I.FELNER,I.NOWIK	LA,SR,CA,O	
5020	PR0475367	Neel Temp by Mossbauer effect of Fe(57), 1% Fe doped sample	La2Sr6Cu8O17.6	La2Sr6Cu8O17.6	La	2	Sr	6	Cu	8															O	17.6		1	1993								9																			2		p4/mbm		A	10.844		3.76												K					4.2																																																																																																La2O3,SrCO3,CuO,Fe(57)2O3	1	mixture-CAL(900C,24H in air)-pellet-SIN(1000C or 1050C,24H)-Q in air-ANN(800C in air)-slow cool to RT					OXYGEN DEPENDENCE OF THE ANTIFERROMAGNETIC ORDER IN LA8-XSRXCU8OY	199303			PHYS.REV.B,47(1993)5367	D.HECHEL,I.FELNER,I.NOWIK	LA,SR,CA,O	
5021	PR0475367	Neel Temp by Mossbauer effect of Fe(57), 1% Fe doped sample		La6.72Sr1.28Cu8O20-z	La	6.72	Sr	1.28	Cu	8															O	20-z		1	1993								215																			2		p4/mbm		A	10.898		3.893												K					4.2																																																																																																La2O3,SrCO3,CuO,Fe(57)2O3	1	mixture-CAL(900C,24H in air)-pellet-SIN(1000C or 1050C,24H)-Q in air-ANN(800C in air)-slow cool to RT					OXYGEN DEPENDENCE OF THE ANTIFERROMAGNETIC ORDER IN LA8-XSRXCU8OY	199303			PHYS.REV.B,47(1993)5367	D.HECHEL,I.FELNER,I.NOWIK	LA,SR,CA,O	
5022	PR0475367	anneald sample, Neel temp. by Mossbauer effect of Fe(57), 1% Fe doped sample		La6Sr2Cu8O19+z	La	6	Sr	2	Cu	8															O	19+z		1	1993								140																			2		p4/mbm		A	10.844		3.861												K					4.2																																																																																																La2O3,SrCO3,CuO,Fe(57)2O3	1	mixture-CAL(900C,24H in air)-pellet-SIN(1000C or 1050C,24H)-Q in air-ANN(800C in air)-slow cool to RT					OXYGEN DEPENDENCE OF THE ANTIFERROMAGNETIC ORDER IN LA8-XSRXCU8OY	199303			PHYS.REV.B,47(1993)5367	D.HECHEL,I.FELNER,I.NOWIK	LA,SR,CA,O	
5023	PR0475367	quenched sample, Neel temp. by Mossbauer effect of Fe(57), 1% Fe doped sample		La6Sr2Cu8O19+z	La	6	Sr	2	Cu	8															O	19+z		1	1993								235																			2		p4/mbm		A	10.865		3.86												K					4.2																																																																																																La2O3,SrCO3,CuO,Fe(57)2O3	1	mixture-CAL(900C,24H in air)-pellet-SIN(1000C or 1050C,24H)-Q in air-ANN(800C in air)-slow cool to RT					OXYGEN DEPENDENCE OF THE ANTIFERROMAGNETIC ORDER IN LA8-XSRXCU8OY	199303			PHYS.REV.B,47(1993)5367	D.HECHEL,I.FELNER,I.NOWIK	LA,SR,CA,O	
5025	PR0487618	metallic	(Sr,Ca)NbO3	Sr0.8Ca0.1Nb1O3	Sr	0.8	Ca	0.1	Nb	1															O	3		1	1993																											1	ABO3			A	3.998														K					4.2																																																																																																SrO,CaO,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5026	PR0487618	metallic	(Sr,Ca)NbO3	Sr0.7Ca0.2Nb1O3	Sr	0.7	Ca	0.2	Nb	1															O	3		1	1993																											1	ABO3			A	3.989														K					4.2																																																																																																SrO,CaO,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5027	PR0487618	metallic	(Sr,Eu)NbO3	Sr0.7Eu0.2Nb1O3	Sr	0.7	Eu	0.2	Nb	1															O	3		1	1993			emu.K/mole		micro.B/Mo	3.3	0.4																				1	ABO3			A	4.003														K					4.2																																																																																																SrO,Eu2O5,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5028	PR0487618	metallic	(Sr,Eu)NbO3	Sr0.5Eu0.4Nb1O3	Sr	0.5	Eu	0.4	Nb	1															O	3		1	1993					micro.B/Mo	4.2	1.5																				1	ABO3			A	4.003														K					4.2																																																																																																SrO,Eu2O5,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5029	PR0487618	metallic	(Sr,Eu)NbO3	Sr0.3Eu0.6Nb1O3	Sr	0.3	Eu	0.6	Nb	1															O	3		1	1993					micro.B/Mo	4.8	2.3																				1	ABO3			A	4.003														K					4.2																																																																																																SrO,Eu2O5,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5030	PR0487618	metallic	(Sr,Eu)NbO3	Sr0.1Eu0.8Nb1O3	Sr	0.1	Eu	0.8	Nb	1															O	3		1	1993					micro.B/Mo	5.2	2.9																				1	ABO3			A	4.004														K					4.2																																																																																																SrO,Eu2O5,Nb2O5	1	mixture in evacuated silica tube-fire(1050C,80-160H)					EFFECTS OF CA AND EU SUBSTITUTION FOR SR IN SRXNBO3	199309			PHYS.REV.B,48(1993)7618	H.YAMAUCHI,JUN SUGIYAMA,KAZUYUKI ISAWA,NAOKI KOSHIZUKA,RITTAPORN ITTI		
5031	PR0487712	hydrostatic pressure upto 1.6GPa, Tc(max)=87.5K(p=1.1GPa)	Bi2Sr2CaCu2O8	Bi2.2Sr1.8Ca1Cu2O8+z	Bi	2.2	Sr	1.8	Ca	1	Cu	2													O	8+z		3	1993																											2	Bi2212			A	5.13		30.54												K		83.5					83.5			K/GPa	3.85																																																																																	m3/C	0.00000000285						/cm3		Bi2O3,Sr(NO3)2,CaCO3,CuO	7	mixed(Bi:Sr:Ca:Cu=2.2:1.8:1:2 for feed and =2.4:1.5:1:1.8 for solvent)-CAL(750C,12H in air)-pellet-SIN(860C,12H in O2)-TSFZ(using infrared heating)					APPEARANCE OF A MAXIMUM IN THE SUPERCONDUCTING TRANSITION TEMPERATURE OF A BI2.2SR1.8CACU2O8+Y SINGLE CRYSTAL UNDER PRESSURE	199309			PHYS.REV.B,48(1993)7712	JIANDING YU,MITSURU ITOH,TETSURO NAKAMURA,TONGKAI HUANG,YOSHIYUKI INAGUMA		
5032	PR0489799	dominant phase(90%)=(Bi0.4Cu0.6)Sr1.9(Nd1.03Ce2)Cu2Oz	(Bi,Cu)Sr2(Nd,Ce)3Cu2Oz	Bi0.5Sr2Nd1Ce1.6Cu2.5Oz	Bi	0.5	Sr	2	Nd	1	Ce	1.6	Cu	2.5											O	z			1993																											2	Bi1232			A	3.848		17.246												K		15					15																																																																																																					(BI,M)SR2(R,CE)NCU2OY (M=CU,CD;R=ND,GD;N=1,2,AND3): A FAMILY OF SUPERCONDUCTORS THAT EXHIBIT SUPERCONDUCTIVITY AT TC-20 K FOR N=3 WITH DOUBLE FLUORITE BLOCKS AND MONOLAYER (BI,M)O SHEETS	199310			PHYS.REV.B,48(1993)9799	CAO LIEZHAO,CHEN XIANHUI,CHEN ZHAOJIA,CHEN ZUYAO,DING ZHONGFEN,QIAN YITAI		
5033	PR0489799	dominant phase=(Bi0.53Cu0.5)Sr1.78(Gd1.09Ce2.07)Cu2Oz	(Bi,Cu)Sr2(Gd,Ce)3Cu2Oz	Bi0.5Sr2Gd1Ce1.6Cu2.5Oz	Bi	0.5	Sr	2	Gd	1	Ce	1.6	Cu	2.5											O	z			1993																												Bi1232																		K		20					20																																																																																																					(BI,M)SR2(R,CE)NCU2OY (M=CU,CD;R=ND,GD;N=1,2,AND3): A FAMILY OF SUPERCONDUCTORS THAT EXHIBIT SUPERCONDUCTIVITY AT TC-20 K FOR N=3 WITH DOUBLE FLUORITE BLOCKS AND MONOLAYER (BI,M)O SHEETS	199310			PHYS.REV.B,48(1993)9799	CAO LIEZHAO,CHEN XIANHUI,CHEN ZHAOJIA,CHEN ZUYAO,DING ZHONGFEN,QIAN YITAI		
5034	PR0489803	O(18)=94%, Tc shift =1.94K, dTc/dx=20K/at.%	YBa2(Cu,Ni)4O8	Y1Ba2Cu3.98Ni0.02O8	Y	1	Ba	2	Cu	3.98	Ni	0.02													O	8			1993																												Y124																		K		67.1					67.1						0.249	O	94	1.94																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5035	PR0489803	O(18)=94%, Tc shift=2.32K	YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8			1993																												Y124																		K		53					53						0.38	O	94	2.32																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5036	PR0489803	O(18)=89%, Tc shift=1.75K	YBa2(Cu,Ni)4O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8			1993																												Y124																		K		25.1					25.1						0.62	O	89	1.75																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5037	PR0489803	O(18)=93%, Tc shift=0.76K, dTc/dx=18K/at.%	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O	8			1993																												Y124																		K		63.8					63.8						0.102	O	93	0.76																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5038	PR0489803	O(18)=93%, Tc shift=0.52K	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.06O8	Y	1	Ba	2	Cu	3.96	Zn	0.06													O	8			1993																												Y124																		K		50.1					50.1						0.089	O	93	0.52																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5039	PR0489803	O(18)=93%, Tc shift=0.62K	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.92Zn0.08O8	Y	1	Ba	2	Cu	3.92	Zn	0.08													O	8			1993																												Y124																		K		40.5					40.5						0.131	O	93	0.62																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5040	PR0489803	O(18)=93%, Tc shift=0.80K, dTc/dx=20K/at.%	YBa2(Cu,Fe)4O8	Y1Ba2Cu3.987Fe0.013O8	Y	1	Ba	2	Cu	3.987	Fe	0.013													O	8			1993																												Y124																		K		70		70			70						0.098	O	93	0.8																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5041	PR0489803	O(18)=92%, Tc shift=1.04K	YBa2(Cu,Fe)4O8	Y1Ba2Cu3.975Fe0.025O8	Y	1	Ba	2	Cu	3.975	Fe	0.025													O	8			1993																												Y124																		K		64.6		64.6			64.6						0.138	O	92	1.04																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5042	PR0489803	O(18)=86%, Tc shift=0.87K	YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8	Y	1	Ba	2	Cu	3.84	Fe	0.16													O	8			1993																												Y124																		K		38.6		38.6			38.6						0.19	O	86	0.87																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-press-wrapped in Au foil-furnace with high-pressure O2-Heat(930C,15H)-Cool to RT-ground-press-refired under high O2 pressure-C					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5043	PR0489803	O(18)=96%,Tc shift=0.5K, dTc/dx=6K/at.%	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.98Fe0.02O7	Y	1	Ba	2	Cu	2.98	Fe	0.02													O	7		1	1993																												Y123																		K		90.7		90.7			90.7						0.047	O	96	0.5																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5044	PR0489803	O(18)=96%,Tc shift=0.60K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.93Fe0.03O7	Y	1	Ba	2	Cu	2.93	Fe	0.03													O	7		1	1993																												Y123																		K		90.1		90.1			90.1						0.056	O	96	0.6																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5045	PR0489803	O(18)=96%, Tc shift=1.7K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.94Cu0.6O7	Y	1	Ba	2	Cu	2.94	Cu	0.6													O	7		1	1993																												Y123																		K		89.1		89.1			89.1						0.16	O	96	1.7																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5046	PR0489803	O(18)=96%, Tc shift=2.1K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.92Fe0.08O7	Y	1	Ba	2	Cu	2.92	Fe	0.08													O	7		1	1993																												Y123																		K		86.2		86.2			86.2						0.209	O	96	2.1																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5047	PR0489803	O(18)=95%, Tc shift=2.24K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.88Fe0.12O7	Y	1	Ba	2	Cu	2.88	Fe	0.12													O	7		1	1993																												Y123																		K		79		79			79						0.24	O	95	2.24																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5048	PR0489803	O(18)=95%, Tc shift=2.29K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.74Fe0.26O7	Y	1	Ba	2	Cu	2.74	Fe	0.26													O	7		1	1993																												Y123																		K		55.6		55.6			55.6						0.357	O	95	2.29																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5049	PR0489803	O(18)=93%, Tc shift=2.2K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7		1	1993																												Y123																		K		50.8		50.8			50.8						0.376	O	93	2.2																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5050	PR0489803	O(18)=96%, Tc shift=0.34K, dTc/dx=18K/at.%	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.985Zn0.015O7	Y	1	Ba	2	Cu	2.985	Zn	0.015													O	7		1	1993																												Y123																		K		83.2		83.2			83.2						0.04	O	96	0.34																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5051	PR0489803	O(18)=96%, Tc shift=0.58K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7		1	1993																												Y123																		K		75.2		75.2			75.2						0.07	O	96	0.58																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5052	PR0489803	O(18)=96%, Tc shift=0.55K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7		1	1993																												Y123																		K		57.4		57.4			57.4						0.082	O	96	0.55																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5053	PR0489803	O(18)=96%, Tc shift=0.74K	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O7	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7		1	1993																												Y123																		K		50.4		50.4			50.4						0.126	O	96	0.74																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5054	PR0489803	O(18)=96%,Tc shift=0.41K,dTc/dx=2.5K/at.%	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	7		1	1993																												Y123																		K		85.9		85.9			85.9						0.04	O	96	0.41																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5055	PR0489803	O(18)=96%,Tc shift=0.42K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.18O7	Y	1	Ba	2	Cu	2.88	Ni	0.18													O	7		1	1993																												Y123																		K		77.2		77.2			77.2						0.046	O	96	0.42																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5056	PR0489803	O(18)=96%, Tc shift=0.45K	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.76Ni0.24O7	Y	1	Ba	2	Cu	2.76	Ni	0.24													O	7		1	1993																												Y123																		K		71.5		71.5			71.5						0.054	O	96	0.45																																																																																					Y2O3,BaO2,CuO,TM-oxide	1	mixture-pellet-Heat(930C,15H in 1 bar flowing O2)-FC to RT in O2-ground-press-Heat(930C,24H)-C at 1 C/min to 420C-ANN(420C,40H)-FC					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5057	PR0489803	O(18)=91%, Tc shift=0.69K	Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.99Fe0.01O8	Bi	2	Sr	2	Ca	1	Cu	1.99	Fe	0.01											O	8		1	1993																												Bi2212																		K		74.1		74.1			74.1						0.079	O	91	0.69																																																																																					Bi2O3,SrCO3,CaO,CuO,Fe2O3	1	mixture-CAL(800C,15H in air)-ground-pellet-SIN(860C,20H in air)-FC-once more					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5058	PR0489803	O(18)=91%, Tc shift=o.oK	Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.98Fe0.02O8	Bi	2	Sr	2	Ca	1	Cu	1.98	Fe	0.02											O	8		1	1993																												Bi2212																		K		71.5		71.5			71.5						0	O	91	0																																																																																					Bi2O3,SrCO3,CaO,CuO,Fe2O3	1	mixture-CAL(800C,15H in air)-ground-pellet-SIN(860C,20H in air)-FC-once more					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5059	PR0489803	O(18)=91%, Tc shift=-0.79K	Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.96Fe0.04O8	Bi	2	Sr	2	Ca	1	Cu	1.96	Fe	0.04											O	8		1	1993																												Bi2212																		K		65.7		65.7			65.7						-0.101	O	91	-0.79																																																																																					Bi2O3,SrCO3,CaO,CuO,Fe2O3	1	mixture-CAL(800C,15H in air)-ground-pellet-SIN(860C,20H in air)-FC-once more					MODIFICATION OF THE OXYGEN-ISOTOPE EFFECT IN HIGH-TEMPERATURESUPERCONDUCTORS DUE TO TRANSITION-METAL DOPING	199310			PHYS.REV.B,48(1993)9803	A.P.B.SINHA,D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,M.R.CHANDRACHOOD		
5060	NAT3650323	Hg1223=90%,remaining was a mixture of CaHgO2,Ba2Ca3O5.9, BaCuO2, hydrostatic 17kbar, qusi-hydrostatic 150kbar	HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z		2	1993																												Hg1223																		K	134	135					135			K/GPa	1.8						75																																																																																						(HgBa2Ca2Cu3Oz+Ba2Ca2Cu3Oz) were sealed in qualtz tube-HEAT(850C,5H)-cool-ANN(300C,10H in flowing O2)					SUPERCONDUCTIVITY ABOVE 150 K IN HGBA2CA2CU3O8+Z AT HIGH PRESSURES	9			NATURE,365(1993)323	C.W.CHU,F.CHEN,L.GAO,R.L.MENG,Y.Y.XUE,Z.J.HUANG	HG,BA,CA,CU,O	
5061	PHC2150191		(Y,Ca)Sr2(Cu,BO3)3Oz	Y0.85Ca0.15Sr2Cu2.5B0.5O7	Y	0.85	Ca	0.15	Sr	2	Cu	2.5	B	0.5											O	7			1993																												Y123																		K					4.2																																																																																																Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5062	PHC2150191			Y0.85Ca0.15Sr1.5Ba0.5Cu2.5B0.5O7	Y	0.85	Ca	0.15	Sr	1.5	Ba	0.5	Cu	2.5	B	0.5									O	7			1993																												Y123																		K		35.5					35.5																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5063	PHC2150191			Y0.85Ca0.15Sr1Ba1Cu2.5B0.5O7	Y	0.85	Ca	0.15	Sr	1	Ba	1	Cu	2.5	B	0.5									O	7			1993																												Y123																		K		43.6					43.6																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5064	PHC2150191			Y0.85Ca0.15Sr0.5Ba1.5Cu2.5B0.5O7	Y	0.85	Ca	0.15	Sr	0.5	Ba	1.5	Cu	2.5	B	0.5									O	7			1993																												Y123																		K		55.6					55.6																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5065	PHC2150191			Y0.85Ca0.15Ba2Cu2.5B0.5O7	Y	0.85	Ca	0.15	Ba	2	Cu	2.5	B	0.5											O	7			1993																												Y123																		K					4.2																																																																																																Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5066	PHC2150191	samples treated in ambient O2 pressure were not s/c		Y1Sr1Ba1Cu2.5B0.5O7	Y	1	Sr	1	Ba	1	Cu	2.5	B	0.5											O	7			1993																												Y123																		K		25					25																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5067	PHC2150191			Y1Sr0.5Ba1.5Cu2.5B0.5O7	Y	1	Sr	0.5	Ba	1.5	Cu	2.5	B	0.5											O	7			1993																												Y123																		K		15					15																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,H3BO3		mixture-HEAT(14H,930C(x=2.0),960C(x=1.5),1000C(x=1.0), 1050C(x=0.5), 1065C(x=0.0))-pellet-HEAT-C in 250bar O2					BO3- 3 SUBSTITUTIONS IN PHASES RELATED TO YBA2CU3O7. SUPERCONDUCTING PROPERTIES OF (Y,CA)(BA,SR)2CU3-Z(BO3)ZOY	199309			PHYSICA C,215(1993)191	C.GREAVES,P.R.SLATER	Y,BA,CU,O,CA,SR,B	
5068	PHC2140307	impurity phase=CaHgO,Hg1201,Ba2Cu3O5.9,BaCuO2, after full oxygenation Tc reach 117K	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z		2	1993																											2	Hg1212	P4/mmm		A	3.862		12.707												K	107	113	116				113			K/GPa							60																																																																																					1	mixture(Ba2CaCu2O5:HgO=1:1)-pellet-sealed in evacuated qualtz tube-Heat to 800C(160C/H)-(800C,9H)-cool-ANN(300C in 1 bar O2)					SUPERCONDUCTIVITY AT 112-117 K IN HGBA2CACU2O6+Z	199309			PHYSICA C,214(1993)307	C.W.CHU,F.CHEN,J.KULIK,R.L.MENG,Y.Y.SUN,Y.Y.XUE,Z.J.HUANG	HG,BA,CA,CU,O	
5069	PHC2150001	Tc maybe 126K	HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O10+z	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z		2	1993																											2	Hg1234			A	3.854		19.006												K		126					126																																																																																															1	mixture of Ba2Ca2Cu3Oz and HgO were sealed in Pt capsule-pressurize to 50 kbar, then HEAT(950C,3H)-cool then depressure					THE SYNTHESIS AND CHARACTERIZATION OF THE HGBA2CA2CU3O8+Z ANDHGBA2CA3CU4O10+Z PHASES	199309			PHYSICA C,215(1993)1	C.CHAILLOUT,E.V.ANTIPOV,J.J.CAPPONI,J.L.THOLENCE,M.MAREZIO,P.BORDET,S.M.LOUREIRO,S.N.PUTILIN	HG,BA,CA,CU,O	
5070	PHC2150001		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z		2	1993																											2	Hg1223			A	3.853		15.818												K		133					133																																																																																															1	mixture of Ba2Ca2Cu3Oz and HgO were sealed in Pt capsule-pressurize to 50 kbar, then HEAT(950C,3H)-cool then depressure					THE SYNTHESIS AND CHARACTERIZATION OF THE HGBA2CA2CU3O8+Z ANDHGBA2CA3CU4O10+Z PHASES	199309			PHYSICA C,215(1993)1	C.CHAILLOUT,E.V.ANTIPOV,J.J.CAPPONI,J.L.THOLENCE,M.MAREZIO,P.BORDET,S.M.LOUREIRO,S.N.PUTILIN	HG,BA,CA,CU,O	
5071	PHC2150011	100% Hg1212 phase, Hg1223 and Hg2435 phases not observed	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2Oz	Hg	1	Ba	2	Ca	1	Cu	2													O	z			1993																											2	Hg1212			A	3.85		12.75												K		125		125			125										20																																																																																						see NAT3620226					CHARACTERISATION OF SUPERCONDUCTING HG-BA-CA-CU-OXIDES	199309			PHYSICA C,215(1993)11	A.SCHILLING,H.-U.NISSEN,H.R.OTT,M.CANTONI	HG,BA,CA,CU,O	
5072	PHC2150011	Hg1223>60%,Hg1212=5%, Hg2435=30%	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1993																											2	Hg1223			A	3.85		15.95												K	130	133		133			133										20																																																																																						see NAT3620226					CHARACTERISATION OF SUPERCONDUCTING HG-BA-CA-CU-OXIDES	199309			PHYSICA C,215(1993)11	A.SCHILLING,H.-U.NISSEN,H.R.OTT,M.CANTONI	HG,BA,CA,CU,O	
5073	PHC1620151		YBa2Cu3Oz	Y1Ba2Cu3O6.97	Y	1	Ba	2	Cu	3															O	z	6.97	1	1989																											3	Y123																		K		89.9		89.9			89.9										60																															A	muon-spin resonance	1550																																																				1						MEASUREMENT OF THE LONDON PENETRATION DEPTHSIN IN YBa2Cu3Ox BY MEANS OF MUON SPIN ROTATION (%*SR) EXPERIMENTS			"Physik-Institut der Universita""t Zu""rich, CH-8001 Zurich"	Physica.C,162-164(1989)151-152	"B. PU""MPIN,H. KELLER,H. SIMMLER,I.M. SAVIC,J.W. SCHNEIDER,P. ZIMMERMANN,W. KU""NDIG,W. ODERMATT"		
5074	PHC1620151	c-axis oriented sample	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	z	6.9	1	1989																											3	Y123																		K		89		89			89										23																															A	muon-spin resonance		5000	1300																																																		1						MEASUREMENT OF THE LONDON PENETRATION DEPTHSIN IN YBa2Cu3Ox BY MEANS OF MUON SPIN ROTATION (%*SR) EXPERIMENTS			"Physik-Institut der Universita""t Zu""rich, CH-8001 Zurich"	Physica.C,162-164(1989)151-152	"B. PU""MPIN,H. KELLER,H. SIMMLER,I.M. SAVIC,J.W. SCHNEIDER,P. ZIMMERMANN,W. KU""NDIG,W. ODERMATT"		
5075	PHC2140350		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1993																											3	Y123																		K		92.9					92.9																																									A	susceptibility of highly oriented grain	1400	10400																																																		Y2O3,BaCO3,CuO,Co3O4,ZnO	1	mixture-CAL(850C,12H)-pellet-SIN(900C+940C,36H)-ANN-slow cool(1C/min) in O2 to RT					TEMPERATURE DEPENDENT MAGNETIC PENETRATION DEPTH OF CO AND ZNDOPED YBA2CU3O7 OBTAINED FROM THE AC SUSCEPTIBILITY OF MAGNETICALLY ALIGNED POWDERS	199309			PHYSICA C,214(1993)350	A.M.CAMPBELL,A.PORCH,D.N.ZHENG,J.R.COOPER,J.R.WALDRAM,P.A.FREEMAN	CO,ZN,Y,BA,CU,O	
5076	PHC2140350		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-z			1993																												Y123																		K		41.5					41.5																																									A		3300	15000																																																		Y2O3,BaCO3,CuO,Co3O4,ZnO	1	mixture-CAL(850C,12H)-pellet-SIN(900C+940C,36H)-ANN-slow cool(1C/min) in O2 to RT					TEMPERATURE DEPENDENT MAGNETIC PENETRATION DEPTH OF CO AND ZNDOPED YBA2CU3O7 OBTAINED FROM THE AC SUSCEPTIBILITY OF MAGNETICALLY ALIGNED POWDERS	199309			PHYSICA C,214(1993)350	A.M.CAMPBELL,A.PORCH,D.N.ZHENG,J.R.COOPER,J.R.WALDRAM,P.A.FREEMAN	CO,ZN,Y,BA,CU,O	
5077	PHC2140350		YBa2(Cu,Co)3O7	Y1Ba2Cu2.955Co0.045O7-z	Y	1	Ba	2	Cu	2.955	Co	0.045													O	7-z			1993																												Y123																		K		94.4					94.4																																									A	susceptibility of highly oriented grain	2020	11600																																																		Y2O3,BaCO3,CuO,Co3O4,ZnO	1	mixture-CAL(850C,12H)-pellet-SIN(900C+940C,36H)-ANN-slow cool(1C/min) in O2 to RT					TEMPERATURE DEPENDENT MAGNETIC PENETRATION DEPTH OF CO AND ZNDOPED YBA2CU3O7 OBTAINED FROM THE AC SUSCEPTIBILITY OF MAGNETICALLY ALIGNED POWDERS	199309			PHYSICA C,214(1993)350	A.M.CAMPBELL,A.PORCH,D.N.ZHENG,J.R.COOPER,J.R.WALDRAM,P.A.FREEMAN	CO,ZN,Y,BA,CU,O	
5078	PHC2140350		YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7-z	Y	1	Ba	2	Cu	2.88	Co	0.12													O	7-z			1993																												Y123																		K		80					80																																									A	susceptibility of highly oriented grain	2000	20000																																																		Y2O3,BaCO3,CuO,Co3O4,ZnO	1	mixture-CAL(850C,12H)-pellet-SIN(900C+940C,36H)-ANN-slow cool(1C/min) in O2 to RT					TEMPERATURE DEPENDENT MAGNETIC PENETRATION DEPTH OF CO AND ZNDOPED YBA2CU3O7 OBTAINED FROM THE AC SUSCEPTIBILITY OF MAGNETICALLY ALIGNED POWDERS	199309			PHYSICA C,214(1993)350	A.M.CAMPBELL,A.PORCH,D.N.ZHENG,J.R.COOPER,J.R.WALDRAM,P.A.FREEMAN	CO,ZN,Y,BA,CU,O	
5079	PR0486525		(Nd,Ce)2Sr2Cu2NbO10	Nd1.5Ce0.5Sr2Cu2Nb1O10	Nd	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1993																											2	RCSCNO																		K		24.2					24.2											Oe		89																																																																																	CeO2,R2O3,SrCO3,CuO,Nb2O3	1	pellet in Al2O3-SIN(1120C,80H in 30kbar O2)-FC to RT					MAGNETIC PROPERTIES OF POLYCRYSTALLINE R1.5CE0.5SR2CU2NBO10 (R=EU,ND,AND SM) HIGH-TC SUPERCONDUCTING CERAMICS	199309			PHYS.REV.B,48(1993)6525	A.F.BELLO,D.BACK,H.B.RADOUSKY,M.BENNAHMIAS,P.KLAVINS,R.N.SHELTON,T.J.GOODWIN		
5080	PR0486525		(Eu,Ce)2Sr2Cu2NbO10	Eu1.5Ce0.5Sr2Cu2Nb1O10	Eu	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1993																											2	RCSCNO																		K		24					24											Oe		70.5																																																																																	CeO2,R2O3,SrCO3,CuO,Nb2O3	1	pellet in Al2O3-SIN(1120C,80H in 30kbar O2)-FC to RT					MAGNETIC PROPERTIES OF POLYCRYSTALLINE R1.5CE0.5SR2CU2NBO10 (R=EU,ND,AND SM) HIGH-TC SUPERCONDUCTING CERAMICS	199309			PHYS.REV.B,48(1993)6525	A.F.BELLO,D.BACK,H.B.RADOUSKY,M.BENNAHMIAS,P.KLAVINS,R.N.SHELTON,T.J.GOODWIN		
5081	PR0486525		(Sm,Ce)2Sr2Cu2NbO10	Sm1.5Ce0.5Sr2Cu2Nb1O10	Sm	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10			1993																											2	RCSCNO																		K		27					27											Oe		92.5																																																																																	CeO2,R2O3,SrCO3,CuO,Nb2O3	1	pellet in Al2O3-SIN(1120C,80H in 30kbar O2)-FC to RT					MAGNETIC PROPERTIES OF POLYCRYSTALLINE R1.5CE0.5SR2CU2NBO10 (R=EU,ND,AND SM) HIGH-TC SUPERCONDUCTING CERAMICS	199309			PHYS.REV.B,48(1993)6525	A.F.BELLO,D.BACK,H.B.RADOUSKY,M.BENNAHMIAS,P.KLAVINS,R.N.SHELTON,T.J.GOODWIN		
5082	PR0486519	Hc(0)=0.92T, G-L parameter=143	(Tl,Pb)Sr2Ca2Cu3O9	Tl0.5Pb0.5Sr2Ca2Cu3O9	Tl	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	9		1	1993																												Tl1223																		K		115				3	115											Oe		231							T	using WHH theory	240							T/K		2.8					A			11.7		A	Hao et al method from magnetization		1800																																																			1	sample sealed in Au foil, SIN(950C or 910C in O2), average grain size 2 micron powders were solidified with wax in a field of 8T					REVERSIBLE MAGNETIC PROPERTIES OF SUPERCONDUCTING (TL,PB)SR2CA2CU3O9 AND TL2BA2CA2CU3O10	199309			PHYS.REV.B,48(1993)6519	A.M.CAMPBELL,D.N.ZHENG,R.S.LIU		
5083	PR0486519	Hc(0)=0.79T, G-L parameter=151	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10		1	1993																												Tl2223																		K		118				3	118											Oe		186								WHH theory	212							T/K		2.4					A			12.4		A	Hao et al method from magnetization		2100																																																			1	sample sealed in Au foil, SIN(950C or 910C in O2), average grain size 2 micron powders were solidified with wax in a field of 8T					REVERSIBLE MAGNETIC PROPERTIES OF SUPERCONDUCTING (TL,PB)SR2CA2CU3O9 AND TL2BA2CA2CU3O10	199309			PHYS.REV.B,48(1993)6519	A.M.CAMPBELL,D.N.ZHENG,R.S.LIU		
5084	PR0486506	Tc measured by rf technique,pressure was changed at RT	La2CuO4	La2Cu1O4.08	La	2	Cu	1																	O	4+z	4.08	1	1993																												T																		K		32					32			K/GPa	2.5																																																																																											1	electro-chemically charged sample using NaOH electrolyte					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SUPEROXYGENATED LA2CUO4+Z	199309			PHYS.REV.B,48(1993)6506	D.C.JOHNSTON,F.C.CHOU,J.E.SCHIRBER,P.C.CANFIELD,W.R.BAYLESS,Z.FISK		
5085	PR0486506	Tc measured rf technique, pressure was changed at RT	La2CuO4	La2Cu1O4.12	La	2	Cu	1																	O	4+z	4.12	1	1993																												T																		K		43					43			K/GPa	0.1																																																																																											1	electro-chemically charged sample using NaOH electrolyte					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SUPEROXYGENATED LA2CUO4+Z	199309			PHYS.REV.B,48(1993)6506	D.C.JOHNSTON,F.C.CHOU,J.E.SCHIRBER,P.C.CANFIELD,W.R.BAYLESS,Z.FISK		
5086	PR0486506	Tc was measured by rf technique,pressure was changed at RT	La2CuO4	La2Cu1O4+z	La	2	Cu	1																	O	4+z		3	1993																												T																		K		28					28			K/GPa	0.1																																																																																											5	high pressure charged sample					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SUPEROXYGENATED LA2CUO4+Z	199309			PHYS.REV.B,48(1993)6506	D.C.JOHNSTON,F.C.CHOU,J.E.SCHIRBER,P.C.CANFIELD,W.R.BAYLESS,Z.FISK		
5087	PR0486506	Tc was measured by rf technique,pressure was changed at RT	La2CuO4	La2Cu1O4+z	La	2	Cu	1																	O	4+z		3	1993																												T																		K		39					39			K/GPa	-1																																																																																											5	high pressure charged sample					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SUPEROXYGENATED LA2CUO4+Z	199309			PHYS.REV.B,48(1993)6506	D.C.JOHNSTON,F.C.CHOU,J.E.SCHIRBER,P.C.CANFIELD,W.R.BAYLESS,Z.FISK		
5088	PR0486431	z<0.1(OZ>6.9),Tc(max)=96.5K(p=5.6GPa), Tc for dTc/dP determined by Tc(on)	NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	1993																											3	Y123																		K		87				7	87			K/GPa	3.6																																																																																												diamond anvil method					PRESSURE DEPENDENCE OF TC IN NDBA2CU3O7-Z TO 6 GPA	199309			PHYS.REV.B,48(1993)6431	CHARLES C.KIM,D.H.LIEBENBERG,E.F.SKELTON,M.S.OSOFSKY		
5089	PR0486431	z<0.1, Tc for dTc/dP determined by Tc(on)	NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	1993																											3	Y123																		K		87.5				7	87.5			K/GPa	3.4																																																																																												diamond anvil method					PRESSURE DEPENDENCE OF TC IN NDBA2CU3O7-Z TO 6 GPA	199309			PHYS.REV.B,48(1993)6431	CHARLES C.KIM,D.H.LIEBENBERG,E.F.SKELTON,M.S.OSOFSKY		
5090	PR0484095	thermal cond. measured by using transient plane source technique, porocity=0.20	YBa2Cu3O7	Y1Ba2Cu3O6.99	Y	1	Ba	2	Cu	3															O	7-z	6.99	1	1993									5.08																		3	Y123			A	3.821	3.887	11.68																																																																														400	from thermal conductivity		2.8			THC5090						m.ohm.cm											1.3										/cm3		Y2O3,Er2O3,CuO,BaCO3	1	mixture-CAL(900C,20H in air)-pellet-SIN(920C,20H in air)-SIN(940C,20-24H in air)-FC to RT-ANN(400C,48H in O2)-c to RT					THERMAL CONDUCTIVITY AND ELECTRICAL RESISTIVITY OF THE Y- ANDER-SUBSTITUTED 1:2:3 SUPERCONDUCTING COMPOUNDS IN THE VICINITYOF THE TRANSITION TEMPERATURE	199308			PHYS.REV.B,48(1993)4095	A.MAQSOOD,B.M.SULEIMAN,E.KARAWACKI,I.UL-HAQ,S.E.GUSTAFSSON		
5091	PR0484095	porocity=0.24, thermal cond. by transient plane source technique	ErBa2Cu3O7	Er1Ba2Cu3O6.88	Er	1	Ba	2	Cu	3															O	7-z	6.88	1	1993									5.4																		3	Y123			A	3.817	3.89	11.648																																																																														350	from thermal conductivity		1.8			THC5091						m.ohm.cm											2.6										/cm3		Y2O3,Er2O3,CuO,BaCO3	1	mixture-CAL(900C,20H in air)-pellet-SIN(920C,20H in air)-SIN(940C,20-24H in air)-FC to RT-ANN(400C,48H in O2)-c to RT					THERMAL CONDUCTIVITY AND ELECTRICAL RESISTIVITY OF THE Y- ANDER-SUBSTITUTED 1:2:3 SUPERCONDUCTING COMPOUNDS IN THE VICINITYOF THE TRANSITION TEMPERATURE	199308			PHYS.REV.B,48(1993)4095	A.MAQSOOD,B.M.SULEIMAN,E.KARAWACKI,I.UL-HAQ,S.E.GUSTAFSSON		
5092	PR0483575	porocity<2%	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1993																												Y124																		K			79			4	79																																																											185	analyzed by relaxation time model		7.3			THC5092						m.ohm.cm											630													1	by HIP CuO with Y123					THERMAL CONDUCTIVITY OF YBA2CU4O8 DOMINATED BY PHONON-PHONON INTERACTIONS	199308			PHYS.REV.B,48(1993)3575	B.M.ANDERSSON,B.SUNDQVIST		
5093	PR0483531	Bi:Sr:Ca:Cu=2.14:1.93:0.92:2.02, oxygen content not measured	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1993																												Bi2212																		K	85						85																																																																							m.ohm.cm												0.3	2800								/cm3			9	1 bar air annealing(500C,12-24H)					WIDE-RANGE OXYGEN DOPING OF BI2SR2CACU2O8+Z	199308			PHYS.REV.B,48(1993)3531	C.KENDZIORA,J.HARTGE,L.FORRO,L.MIHALY,MICHAEL C.MARTIN		
5094	PR0483531		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1993																												Bi2212																		K	59						59																																																																							m.ohm.cm												0.18	1580								/cm3			9	2 kbar O2 annealing(500C,12-24H)					WIDE-RANGE OXYGEN DOPING OF BI2SR2CACU2O8+Z	199308			PHYS.REV.B,48(1993)3531	C.KENDZIORA,J.HARTGE,L.FORRO,L.MIHALY,MICHAEL C.MARTIN		
5095	PHC1970131	major phase=Tl-1222, impurity phase=Eu2CuO4	TlBa2(Eu,Ce)2Cu2O9	Tl1Ba1.75Eu1.75Ce0.5Cu2O9-z	Tl	1	Ba	1.75	Eu	1.75	Ce	0.5	Cu	2											O	9-z		2	1992																											2	Tl1222	I4/mmm		A	3.878		30.423												K			40	40			40										5																																																																																				Tl2O3,BaO2,Eu2O3,CeO2,CuO	1	ANN(500C,10H in 100bar O2), sample(5096)=SIN(890-910C,6H)					TLBA2(EU,CE)2CU2O9+Z, A NEW MEMBER OF THE DOUBLE FLUORITE-TYPECUPRATE FAMILY	199207			PHYSICA C,197(1992)131	A.MAIGNAN,B.RAVEAU,C,C.MICHEL,M.HERVIEU,MARTIN,P.P.EDWARDS,R.S.LIU	TL,EU,CE,CU,O	
5096	PHC1970131	major=Tl-1222, impurity phase=Eu2CuO4	TlBa2(Eu,Ce)2Cu2O9	Tl1Ba1.75Eu1.75Ce0.5Cu2O9-z	Tl	1	Ba	1.75	Eu	1.75	Ce	0.5	Cu	2											O	9-z		2	1992																											2	Tl1222	I4/mmm		A	3.878		30.423												K		25.5		25.5			25.5										0.3																																																																																				Tl2O3,BaO2,Eu2O3,CeO2,CuO	1	ANN(500C,10H in 100bar O2), sample(5096)=SIN(890-910C,6H)					TLBA2(EU,CE)2CU2O9+Z, A NEW MEMBER OF THE DOUBLE FLUORITE-TYPECUPRATE FAMILY	199207			PHYSICA C,197(1992)131	A.MAIGNAN,B.RAVEAU,C,C.MICHEL,M.HERVIEU,MARTIN,P.P.EDWARDS,R.S.LIU	TL,EU,CE,CU,O	
5097	PHC1970042	main phase=ortho-Pb2Sr2YCu3O8, X-Ray shows weak Ag + unknown phase	((Pb,Ag)La,Cu)Sr2LaCu2Oz	Pb0.9AgSr2La2Cu3.1Oz	Pb	0.9	Ag		Sr	2	La	2	Cu	3.1											O	z		2	1992																											3	Pb3212			A	5.402	5.367	15.7												K	55	70		69			70																																																																																															11	sol-gel precursor-powder-fired(350C)-pellet-SIN(800C,12H in flowing Ar)-Quench					SUPERCONDUCTIVITY AT 55 K ENHANCED BY SILVER-DOPING IN PB0.9AGXSR2LA2CU3.1OY	199207			PHYSICA C,197(1992)42	CHENGYUN WANG,GUANGHAN CAO,GUIEN ZHOU,HE HUANG,MINGRONG JI,YITAI QIAN,ZUYAO CHEN	PB,AG,SR,LA,CU,O	
5098	PHC1900433	lattice parameter decreases with increasing Sr content	Yb(Ba,Sr)2Cu4O8	Yb1Ba1.8Sr0.2Cu4O8	Yb	1	Ba	1.8	Sr	0.2	Cu	4													O	8		1	1992																											3	Y124			A	3.814	3.857	27.129		xray										K	77	82		80			82																																																																							m.ohm.cm											4.3												Yb2O3,BaCO3,SrCO3,CuO	1	mixture-pellet-CAL(900c,120H in flowing O20-ground-long bar-SIN(920C in flowing O2)-ANN(1070C,6H in 80%Ar+20%O2 of 200MPa)					"YB(BA,SR)2CU4O8:A""124"" PHASE SUPERCONDUCTOR WITH A REDUCED UNIT CELL VOLUME"	199201			PHYSICA C,190(1992)433	H.YAMAUCHI,SATOSHI TAKANO,SEIJI ADACHI,TAKAHIRO WADA,YUJI YAEGASHI	YB,BA,SR,CU,O	
5099	PHC1900433		Yb(Ba,Sr)2Cu4O8	Yb1Ba1.6Sr0.4Cu4O8	Yb	1	Ba	1.6	Sr	0.4	Cu	4													O	8		1	1992																											3	Y124			A	3.805	3.855	27.072		x-ray										K	78		83	80			80																																																																							m.ohm.cm											2.9												Yb2O3,BaCO3,SrCO3,CuO	1	mixture-pellet-CAL(900c,120H in flowing O20-ground-long bar-SIN(920C in flowing O2)-ANN(1070C,6H in 80%Ar+20%O2 of 200MPa)					"YB(BA,SR)2CU4O8:A""124"" PHASE SUPERCONDUCTOR WITH A REDUCED UNIT CELL VOLUME"	199201			PHYSICA C,190(1992)433	H.YAMAUCHI,SATOSHI TAKANO,SEIJI ADACHI,TAKAHIRO WADA,YUJI YAEGASHI	YB,BA,SR,CU,O	
5100	PHC1900433		Yb(Ba,Sr)2Cu4O8	Yb1Ba1.4Sr0.6Cu4O8	Yb	1	Ba	1.4	Sr	0.6	Cu	4													O	8		1	1992																											3	Y124			A	3.796	3.851	27.022		x-ray										K	77		83	80			80																																																																							m.ohm.cm											4												Yb2O3,BaCO3,SrCO3,CuO	1	mixture-pellet-CAL(900c,120H in flowing O20-ground-long bar-SIN(920C in flowing O2)-ANN(1070C,6H in 80%Ar+20%O2 of 200MPa)					"YB(BA,SR)2CU4O8:A""124"" PHASE SUPERCONDUCTOR WITH A REDUCED UNIT CELL VOLUME"	199201			PHYSICA C,190(1992)433	H.YAMAUCHI,SATOSHI TAKANO,SEIJI ADACHI,TAKAHIRO WADA,YUJI YAEGASHI	YB,BA,SR,CU,O	
5101	PHC1900433		Yb(Ba,Sr)2Cu4O8	Yb1Ba1.2Sr0.8Cu4O8	Yb	1	Ba	1.2	Sr	0.8	Cu	4													O	8		2	1992																											3	Y124			A	3.794	3.851	27.007		x-ray										K	76		81	80			80																																																																							m.ohm.cm											6.8												Yb2O3,BaCO3,SrCO3,CuO	1	mixture-pellet-CAL(900c,120H in flowing O20-ground-long bar-SIN(920C in flowing O2)-ANN(1070C,6H in 80%Ar+20%O2 of 200MPa)					"YB(BA,SR)2CU4O8:A""124"" PHASE SUPERCONDUCTOR WITH A REDUCED UNIT CELL VOLUME"	199201			PHYSICA C,190(1992)433	H.YAMAUCHI,SATOSHI TAKANO,SEIJI ADACHI,TAKAHIRO WADA,YUJI YAEGASHI	YB,BA,SR,CU,O	
5102	PRL0700085	gap by microwave, gap=3.9-4.5	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1993																												T'																		K		22		22			22																																				A					A	micro wave		1100				3.9	10																																																				Temperature Dependence of Penetration Depth and Surface Resistance of Nd1.85Ce0.15CuO4	199301		Center for Superconductivity Reserch, Department of Physics, University of Maryland, College Park, Maryland 207 42	Phys.Rev.Lett.70(1993)85	Dong Ho Wu,J.L. Peng,Jian Mao,R.L. Greene,S.N. Mao,Steven M. Anlage,T. Venkatesan,X.X. Xi		
5103	PRL0700085	gap=3.9-4.3	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1993																												T'																		K		21.5		21.5			21.5																																				A			80		A			1250				3.9	10																																																				Temperature Dependence of Penetration Depth and Surface Resistance of Nd1.85Ce0.15CuO4	199301		Center for Superconductivity Reserch, Department of Physics, University of Maryland, College Park, Maryland 207 42	Phys.Rev.Lett.70(1993)85	Dong Ho Wu,J.L. Peng,Jian Mao,R.L. Greene,S.N. Mao,Steven M. Anlage,T. Venkatesan,X.X. Xi		
5104	PRL0700085	thin film, gap=4-4.3	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		4	1993																												T'																		K		21					21																																				A			72		A			1300				4	10																																																				Temperature Dependence of Penetration Depth and Surface Resistance of Nd1.85Ce0.15CuO4	199301		Center for Superconductivity Reserch, Department of Physics, University of Maryland, College Park, Maryland 207 42	Phys.Rev.Lett.70(1993)85	Dong Ho Wu,J.L. Peng,Jian Mao,R.L. Greene,S.N. Mao,Steven M. Anlage,T. Venkatesan,X.X. Xi		
5105	PRB03600836	impurity phase<5%	HoBa2Cu3O7	Ho1Ba2Cu3Oz	Ho	1	Ba	2	Cu	3															O	z		1	1987					micro.B/Mo	10.6	13																					Y123																		K	90.2	91.5		86.6			91.5										90																																																													ohm.cm							0.4				1												Ho2O3,BaCO3,CuO	1	mixture-fired(895C,20H in flowing O2)-ground-pellet-HEAT(2C/min) to 945C-SIN(945C,16H)-cool(0.5C/min) to 500C-FC					Independent superconductivity and paramagnetism in HoBa2Cu3Oz				PHYS.REV.B,36(1987)836			
5106	SSC0850849	apical Cu-O=2.333A,in-plane Cu-O=1.9902A	PrBa2Cu2NbOz	Pr1Ba2Cu2Nb1O8-z	Pr	1	Ba	2	Cu	2	Nb	1													O	8-z		1	1993	emu/mole	0.001			/Pr	2.85	-6	10																			2	Y123	P4/mmm		A	3.965		12.003		x-ray																																																																																																															Pr6O11,CuO,Nb2O5,BaCO3	1	mixture-HEAT(1000C,24H)-ground-pellet-SIN(1000C,12H in flowing O2)					STRUCTURAL AND MAGNETIC STUDIES ON PRBA2CU2NBO8-Y	199303			SOLID STATE COMMUN.,85(1993)849	H.JHANS,J.J.RHYNE,S.K.MALIK,W.B.YELON	PR,BA,CU,NB,O	
5107	PHC2040043	O2 press =23.4GPa, quenching sample		Sr2Dy1Cu3Oz	Sr	2	Dy	1	Cu	3															O	z			1992																											2	Y123			A	3.797		11.395												K					40																																																																																																SrCO3,R2O3,CuO	1	synthesized at 2GPa under various O2 pressure					SUPERCONDUCTIVITY IN SR2RCU3OZ (R=DY,HO,ER,TM AND YB)	199212			PHYSICA C,204(1992)43	A.ONO,M.TSUTSUMI	SR,R,CU,O	
5108	PHC2040043	O2 pressure=12.9GPa	HoSr2Cu3Oz	Sr2Ho1Cu3O	Sr	2	Ho	1	Cu	3															O				1992																											2	Y123			A	3.792		11.384												K		62		62			62																																																																																														SrCO3,R2O3,CuO	1	synthesized at 2GPa under various O2 pressure					SUPERCONDUCTIVITY IN SR2RCU3OZ (R=DY,HO,ER,TM AND YB)	199212			PHYSICA C,204(1992)43	A.ONO,M.TSUTSUMI	SR,R,CU,O	
5109	PHC2040043	O2 pressure = 19.1GPa	ErSr2Cu3Oz	Er1Sr2Cu3Oz	Er	1	Sr	2	Cu	3															O	z			1992																											2	Y123																		K		60		60			60																																																																																														SrCO3,R2O3,CuO	1	synthesized at 2GPa under various O2 pressure					SUPERCONDUCTIVITY IN SR2RCU3OZ (R=DY,HO,ER,TM AND YB)	199212			PHYSICA C,204(1992)43	A.ONO,M.TSUTSUMI	SR,R,CU,O	
5110	PHC2040043	O2 pressure=16.1GPa	TmSr2Cu3Oz	Tm1Sr2Cu3Oz	Tm	1	Sr	2	Cu	3															O	z			1992																											2	Y123																		K		45		45			45																																																																																														SrCO3,R2O3,CuO	1	synthesized at 2GPa under various O2 pressure					SUPERCONDUCTIVITY IN SR2RCU3OZ (R=DY,HO,ER,TM AND YB)	199212			PHYSICA C,204(1992)43	A.ONO,M.TSUTSUMI	SR,R,CU,O	
5111	PHC2040065		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1992																											2	Bi2212	Bbmb		A	5.41		30.88												K		75	85	75			75																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5112	PHC2040065	I content =0.97	IBi2Sr2YCu2O8	I1Bi2Sr2Y1Cu2Oz	I	1	Bi	2	Sr	2	Y	1	Cu	2											O	z			1992																											2				A	5.448		37.76		x-ray										K					4.2																																																																																																							STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5113	PHC2040065	I content =0.96	IBi2Sr2(Ca,Y)Cu2O8	I1Bi2Sr2Ca0.4Y0.6Cu2Oz	I	1	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2									O	z			1992																											2				A	5.428		37.76		x-ray										K					4.2																																																																																																							STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5114	PHC2040065	I content =0.96	IBi2Sr2(Ca,Y)Cu2O8	I1Bi2Sr2Ca0.5Y0.5Cu2Oz	I	1	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	z			1992																											2				A	5.423		37.85		x-ray										K		79	79	79			79																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5115	PHC2040065		IBi2Sr2(Ca,Y)Cu2O8	I1Bi2Sr2Ca0.6Y0.4Cu2Oz	I	1	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2									O	z		3	1992																											2				A	5.421		37.9		x-ray										K		86	88	86			86																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5116	PHC2040065		IBi2Sr2(Ca,Y)Cu2O8	I1Bi2Sr2Ca0.8Y0.2Cu2Oz	I	1	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	z		3	1992																											2				A	5.408		38.06		x-ray										K		84	98	84			84																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5117	PHC2040065	lattice const. c linearly decreases with decreasing I content. I atom found between Bi-O layers.	IBi2Sr2CaCu2O8	I1Bi2Sr2Ca1Cu2Oz	I	1	Bi	2	Sr	2	Ca	1	Cu	2											O	z		3	1992																											2		Pbmb		A	5.4		38.15		x-ray										K		65	75	65			65																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5118	PHC2040065		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	z		3	1992																											2	Bi2212			A	5.408		30.7												K		87	100	87			87																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5119	PHC2040065		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2Oz	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	z		3	1992																											2	Bi2212			A	5.422		30.52												K		86	98	86			86																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5120	PHC2040065		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	z			1992																											3	Bi2212			A	5.423	5.432	30.46												K		80	83	80			80																																																																																																					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5121	PHC2040065		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.4Y0.6Cu2Oz	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	z			1992																											3	Bi2212			A	5.424	5.438	30.38												K					4.2																																																																																																							STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5122	PHC2040065		Bi2Sr2YCu2O8	Bi2Sr2Y1Cu2Oz	Bi	2	Sr	2	Y	1	Cu	2													O	z			1992																											3	Bi2212			A	5.438	5.468	30.2												K					4.2																																																																																																							STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF IODINE-INTERCALATED BI2SR2CA1-XYXCU2OZ	199212			PHYSICA C,204(1992)65	K.HIRAGA,M.KIKUCHI,N.KOBAYASHI,N.OHNISHI,R.SUZUKI,Y.MURAOKA,Y.SHONO	BI,SR,CA,Y,CU,O	
5123	SSC0850073	80%C60+18%C70+2%solvent, Debye temp. estimated from specific heat below 9K. two anomalies(90K ,250K) in specific heat	C60	C60	C	60																							1993																												fullerene																																																																																	uJ/g.K2	893		188	from specific heat																																									SPECIFIC HEAT OF FULLERENES EXTRACT	199301			SOLID STATE COMMUN.,85(1993)73	A.DEMAIN,B.NYSTEN,E.GRIVEI,J-P.ISSI,M.CASSART	C,	
5124	SSC0850849		PrBa2Cu3NbO8	Pr1Ba2Cu2Nb1O8-z	Pr	1	Ba	2	Cu	2	Nb	1													O	8-z			1993	emu/mole	0.001			micro.B/Mo	2.85	-6	10																			2	Y123	P4/mmm		A	3.965		12.003											structure analyzed by neutron diffraction																																																																																																						Pr6O11,CuO,Nb2O5,BaCo2	1	mixture-Heat(1000C,24H)-reground-pellet-Heat(12H in flowing O2)-slow cool					STRUCTURAL AND MAGNETIC STUDIES ON PRBA2CU2NBO8-Y	199303			SOLID STATE COMMUN.,85(1993)849	H.JHANS,J.J.RHYNE,S.K.MALIK,W.B.YELON	PR,BA,CU,NB,O	
5125	PR0479048		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+z		1	1993																											3	Tl2212																		K		85					85																																																																		micro.V/K	-3.1			TP5125																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5126	PR0479048		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+z		1	1993																											3	Tl2212																		K		105					105																																																																			2.63			TP5126																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5127	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.9Y0.1Cu2O8+z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	2											O	8+z		1	1993																											3	Tl2212																		K		88					88																																																																			2.46			TP5127																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5128	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.8Y0.2Cu2O8+z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	2											O	8+z		1	1993																											3	Tl2212																		K		74					74																																																																			12.3			TP5128																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5129	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.75Y0.25Cu2O8+z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	2											O	8+z		1	1993																											3	Tl2212																		K		58					58																																																																			27			TP5129																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5130	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.65Y0.35Cu2O8+z	Tl	2	Ba	2	Ca	0.65	Y	0.35	Cu	2											O	8+z		1	1993																											3	Tl2212																		K		30					30																																																																			62.6			TP5130																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5131	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.5Y0.5Cu2O8+z	Tl	2	Ba	2	Ca	0.5	Y	0.5	Cu	2											O	8+z		1	1993																											3	Tl2212																																																																																												121.5			TP5131																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5132	PR0479048		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.4Y0.6Cu2O8+z	Tl	2	Ba	2	Ca	0.4	Y	0.6	Cu	2											O	8+z		1	1993																											3	Tl2212																																																																																												180			TP5132																										see PR0442757					THERMOELECTRIC POWER OF TL2BA2CA1-XYXCU2O8+Y (0<-X<-0.6) SAMPLES	199304			PHYS.REV.B,47(1993)9048	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	TL,BA,CA,Y,CU,O	
5133	PR0478008	structure comfirmed by x-ray diffraction	(Ba,K)2(Pb,Bi)O4	Ba1.7K0.3Pb0.95Bi0.05O4	Ba	1.7	K	0.3	Pb	0.95	Bi	0.05													O	4			1993																											2	T																		K		11		11			11																																																																																															11	modified sol-gel method was used for nominal powders					BA2-XKXPB1-YBIYO4-Z: LAYERED OXIDES WITH INSULATING OR CONDUCTING PROPERTIES AND POSSIBLE SUPERCONDUCTING PROPERTIES	199304			PHYS.REV.B,47(1993)8008	FRANCOIS GERVAIS,MARINA LICHERON	BA,K,PB,BI,O	
5134	PR0478008	structure by x-ray diffraction	(Ba.K)2(Pb,Bi)O4	Ba1.9K0.1Pb0.85Bi0.15O4	Ba	1.9	K	0.1	Pb	0.85	Bi	0.15													O	4			1993																											2	T																		K		12.5		12.5			12.5																																																																																															11	modified sol-gel method was used for nominal powders					BA2-XKXPB1-YBIYO4-Z: LAYERED OXIDES WITH INSULATING OR CONDUCTING PROPERTIES AND POSSIBLE SUPERCONDUCTING PROPERTIES	199304			PHYS.REV.B,47(1993)8008	FRANCOIS GERVAIS,MARINA LICHERON	BA,K,PB,BI,O	
5135	PR0478008	structure by x-ray diffraction	(Ba,K)2(Pb,Bi)O4	Ba1.7K0.3Pb0.9Bi0.1O4	Ba	1.7	K	0.3	Pb	0.9	Bi	0.1													O	4			1993																											2	T																		K		11		11			11																																																																																															11	modified sol-gel method was used for nominal powders					BA2-XKXPB1-YBIYO4-Z: LAYERED OXIDES WITH INSULATING OR CONDUCTING PROPERTIES AND POSSIBLE SUPERCONDUCTING PROPERTIES	199304			PHYS.REV.B,47(1993)8008	FRANCOIS GERVAIS,MARINA LICHERON	BA,K,PB,BI,O	
5136	PR0478151	1.3*0.8*0.02mm3, Ce distribution is uniform	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+z	Nd	1.85	Ce	0.15	Cu	1															O	4+z		3	1993																												T'																		K					4.2																																																																																							m3/C	-0.0000000027					RH5136				5	as-grown					TRANSPORT PROPERTIES OF ND1.85CE0.15CUO4+Z CRYSTALS BEFORE ANDAFTER REDUCTION	199304			PHYS.REV.B,47(1993)8151	J.L.PENG,R.L.GREENE,WU JIANG,Z.Y.LI	ND,CE,CU,O	
5137	PR0478151	1.3*0.8*0.02mm3, Ce distribution is uniform	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+z	Nd	1.85	Ce	0.15	Cu	1															O	4+z		3	1993																												T'																		K		24				2	24																																																																																					m3/C	-0.000000001					RH5137				5	annealing in N2(900c,15H)					TRANSPORT PROPERTIES OF ND1.85CE0.15CUO4+Z CRYSTALS BEFORE ANDAFTER REDUCTION	199304			PHYS.REV.B,47(1993)8151	J.L.PENG,R.L.GREENE,WU JIANG,Z.Y.LI	ND,CE,CU,O	
5138	PR0478324	reverse slope 1/B (B=dS/dT for in-plane thermopower S) decreases linearly with increasing Tc	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	1993																												Tl2201																		K	80		92				86																																																																			-4			TP5138	m.ohm.cm												0.1	10												by using double-crucible technique					THERMOPOWER OF TL2BA2CUO6 SINGLE CRYSTALS	199304			PHYS.REV.B,47(1993)8324	A.M.HERMANN,H.M.DUAN,LIN SHU-YUAN,LU LI,WILLIAM KIEHL,ZHANG DIAN-LIN	TL,BA,CU,O	
5139	PR0478212	anisotropy parameter > 31	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.67Ca0.33Cu3O8+z	Pb	2	Sr	2	Y	0.67	Ca	0.33	Cu	3											O	8+z		3	1993																												Pb3212																		K		80		80			80											Oe	linear extraporation in root(M) vs H		16	500																										A	using 2D layered s/c model, measurement of M		1860																																																			5	crucible-quickly heat up to 1030C-hold for 30min-cool to 800C at 5C/H-cool to 550C at 20C/H-FC to RT in N2					LOWER CRITICAL FIELDS,CRITICAL CURRENTS,AND FLUX CREEP IN PB2SR2R1-XCAXCU3O8+Y (R=Y,DY) SINGLE CRYSTALS	199304			PHYS.REV.B,47(1993)8212	G.GUNTHERODT,M.M.LUKINA,V.V.METLUSHKO,V.V.MOSHCHALKOV,Y.BRUYNSERAEDE	PB,SR,Y,DY,CA,CU,O	
5140	PHC2170265	95%Hg1223, 5%Hg1234, impurity=CaHgO2,BaCuO2, oxygen content by neutron diffraction	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8.41	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z	8.41	2	1993																											2	Hg1223	P4/mmm		A	3.85		15.784											analized by multi-phase program	K		133		133			133																																																																																														Ba2Ca2Cu3Oz,HgO	1	precursor prepared by mixing metal-nitrate,mix(precursor+HgO)-Au crucible-press(18kbar,20min)-Heat(880C,40min)-react(18kbar,880C,1.8H)-cool to RT at 1 atm					Neutron powder diffraction study at room temperature and at 10 K of the crystal structure of the 133 K superconductor HgBa2Ca2Cu3O8+z	199311		NIST,Gaithersburg,USA	Physica C, 217(1993)265	A.Santoro,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,O.Chmaissem,Q.Huang,S.M.Loureiro,S.N.Putilin	Hg,Ba,Ca,Cu,O	
5141	PHC2170253	oxygen content evaluated by neutron diffraction,synthesis condition of precursor is important	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6.22	Hg	1	Ba	2	Ca	1	Cu	2													O	6	6.22		1993									6.45																		2	Hg1212	P4/mmm		A	6.858		12.68												K			127				127																																																																																														Ba2CaCu2Oz,HgO	1	mixture of precursor +yellow HgO-pellet-sealed in silica tube-SIN(750C,16H)-ANN(300C,10H),precursor made by 600+800+925C with intermediate ground(starting=Nitrate)					Synthesis and structural characterization of the 127 K HgBa2CaCu2O6.22 superconductor: Tc variations upon different atmosphere annealings	199311			Physica C, 217(1993)253	E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,O.Chmaissem,Q.Huang,S.M.Loureiro	Hg,Ba,Ca,Cu,O	
5142	PHC2170294	Y124+Ag, Ag addition improves structural completeness and increases s/c volume fraction	(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8			1993																											3	Y124			A	3.846	3.869	27.25												K	77		90				83.5																																																																																															1	mixture-CAL(750C,24H)-cool to RT-mix(powder+50wt%Ag2O)-pellet under 100MPa-SIN(800C,72H)-FC to RT,all press under flowing O2					Synthesis of 90 K superconducting Y0.9Ca0.1Ba2Cu4O8 in oxygen at ordinary pressure by Ag2O addition	199311		Department of Electical Engineering,Nagaoka University of Technology,Nagaoka,Japan	Physica C, 217(1993)294	Ben Huybrechts,Masasuke Takata,Sadao Mori,Satoshi Ohara,Yuichi Watanabe	Y,Ca,Ba,Cu,O	
5143	PHC2170342		(Sr,Bi)2(Y,Ce)2Cu2O8	Sr1.5Bi0.5Y1.15Ce0.85Cu2O8-z	Sr	1.5	Bi	0.5	Y	1.15	Ce	0.85	Cu	2											O	8-z			1993																											2	T*	P4/mmm		A	3.822		12.659												K	30	32	40	32			32																																																																																														Bi2O3,SrCO3,Y2O3,CeO2,CuO	1	mixture-CAL(950C,several days in flowing O2)-ground-pellet-SIN(980C,36H in flowing O2)-cool to 500C(0.25C/min)-ANN(500C,10H)-cool to RT					Synthesis and structure of superconductors, (Sr2-xBix)(Ln2-yCey)Cu2O8-z of T* phase	199311		Department of Physics, University of Science & Technology of China,Hefei,China	Physica C, 217(1993)342	G.E.Zhou,H.Chen,L.Z.Cao,X.H.Chen,Z.J.Chen	Sr,Bi,Ln,Ce,Cu,O	
5144	PHC2170439	for Pr,Tb, single phase for 0<x<0.3, Tc(FIG)  for Tc vs Pr or Tb content	(Tl,Pb)Sr2(Ca,Pr)Cu2Oz	Tl0.5Pb0.5Sr2CaPrCu2Oz	Tl	0.5	Pb	0.5	Sr	2	Ca		Pr		Cu	2									O	z		1	1993																												Tl1212																																																																																																																							SrCO3,CaO,Cu,CeO2,Pr6O11,Tb4O7		two step solid state reaction, precursor=Sr2Ca1-xRxCu2O5, mixture-heat(920C,40H in air)/precursor+Tl2O3+PbO-mix-pellet-sandwitch between Au-SIN(900C,5H)					Superconductivity in Tl0.5Pb0.5Sr2Ca1-xRxCu2Oy (R=Ce,Pr,or Tb)	199311		Superconducting Materials Lab. Acheson Hall,State University of New York at Buffalo,USA	Physica C, 217(1993)439	Jui H.Wang,Q.Hong	Tl,Pb,Sr,Ca,Ce,Pr,Tb,Cu,O	
5145	PHC2170439		(Tl,Pb)Sr2(Ca,Tb)Cu2Oz	Tl0.5Pb0.5Sr2CaTbCu2Oz	Tl	0.5	Pb	0.5	Sr	2	Ca		Tb		Cu	2									O	z		1	1993																												Tl1212																																																																																																																							SrCO3,CaO,Cu,CeO2,Pr6O11,Tb4O7		two step solid state reaction, precursor=Sr2Ca1-xRxCu2O5, mixture-heat(920C,40H in air)/precursor+Tl2O3+PbO-mix-pellet-sandwitch between Au-SIN(900C,5H)					Superconductivity in Tl0.5Pb0.5Sr2Ca1-xRxCu2Oy (R=Ce,Pr,or Tb)	199311		Superconducting Materials Lab. Acheson Hall,State University of New York at Buffalo,USA	Physica C, 217(1993)439	Jui H.Wang,Q.Hong	Tl,Pb,Sr,Ca,Ce,Pr,Tb,Cu,O	
5146	SSC0880629	oxygen content by iodometry	ErBa2Cu3O7	Er1Ba2Cu3O6.935	Er	1	Ba	2	Cu	3															O	z	6.935	1	1993																											3	Y123			A	3.82	3.886	11.671												K	87	88	92				88																																																																							m.ohm.cm											0.32												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5147	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.95Ca0.05Ba2Cu3O6.935	Er	0.95	Ca	0.05	Ba	2	Cu	3													O	z	6.935	1	1993																											3	Y123			A	3.76	3.8	11.671												K	84.5	86	90				86																																																																							m.ohm.cm											2.2												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5148	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.9Ca0.1Ba2Cu3O6.93	Er	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.93	1	1993																											3	Y123			A	3.821	3.883	11.663												K	79	82.5	87.7				82.5																																																																							m.ohm.cm											1.4												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5149	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.85Ca0.15Ba2Cu3O6.93	Er	0.85	Ca	0.15	Ba	2	Cu	3													O	z	6.93	1	1993																											3	Y123			A	3.827	3.885	11.674												K	77	79.5	84.5				79.5																																																																							m.ohm.cm											2.5												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5150	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.8Ca0.2Ba2Cu3O6.91	Er	0.8	Ca	0.2	Ba	2	Cu	3													O	z	6.91	1	1993																											3	Y123			A	3.828	3.992	11.664												K	71.5	76.5	84.3				76.5																																																																							m.ohm.cm											0.2												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5151	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.75Ca0.25Ba2Cu3O6.88	Er	0.75	Ca	0.25	Ba	2	Cu	3													O	z	6.88	1	1993																											3	Y123			A	3.835	3.882	11.662												K	62	67.5	73				67.5																																																																																														Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5152	SSC0880629		(Er,Ca)Ba2Cu3O7	Er0.7Ca0.3Ba2Cu3O6.83	Er	0.7	Ca	0.3	Ba	2	Cu	3													O	z	6.83	1	1993																											3	Y123			A	3.791	3.941	11.91												K	51.5	55.7	60				55.7																																																																							m.ohm.cm											0.35												Er2O3,BaCO3,CuO,CaCO3	1	mixture-heat(950C,24H in air in Pt crucible)-reground-pellet-SIN(950C,24H in air)-ANN(450C,24H in flowing O2)-cool to RT(1C/min)					SUPPRESSION OF SUPERCONDUCTIVITY IN Er1-xCaxBa2Cu3Oy BY HOLE DOPING AND PAIR BREAKING			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun.,88(1993)629-632	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5153	SUP0060265		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1993																											3	Y124	Ammm		A	3.839	3.871	27.259												K		80					80																																																																																														Y2O3,CeO2,CuO,Ba(NO3)2	1	CuO+Ba(NO3)2-heat(1175K,48H)-precursor(BaCu2O3 or Ba1.1Cu2O3)+Y2O3(or CeO2)-mix-pellet-SIN(1085K,1 week in flowing O2 at 1 atm)					Inflence of Ba Content and Ce Doping on the Structural Features of YBa2Cu4O8 Superconductor-a Neutron Study	1993		Solid State Physics Division, Bhabha Atomic Reserch Center, Bombay-400 085, India	J.Superconductivity,6(1993)265	A. Sequeira,H. Rajagopal,I.K. Gopalakrishnan,J.V. Yakhmi,R.M. Iyer		
5154	SUP0060265		(Y,Ce)Ba2Cu4O8	Y0.9Ce0.1Ba2Cu4O8	Y	0.9	Ce	0.1	Ba	2	Cu	4													O	8			1993																											3	Y124	Ammm		A	3.829	3.86	27.152												K		55					55																																																																																														Y2O3,CeO2,CuO,Ba(NO3)2	1	CuO+Ba(NO3)2-heat(1175K,48H)-precursor(BaCu2O3 or Ba1.1Cu2O3)+Y2O3(or CeO2)-mix-pellet-SIN(1085K,1 week in flowing O2 at 1 atm)					Inflence of Ba Content and Ce Doping on the Structural Features of YBa2Cu4O8 Superconductor-a Neutron Study	1993		Solid State Physics Division, Bhabha Atomic Reserch Center, Bombay-400 085, India	J.Superconductivity,6(1993)265	A. Sequeira,H. Rajagopal,I.K. Gopalakrishnan,J.V. Yakhmi,R.M. Iyer		
5155	SUP0060265		YBa2Cu4O8	Y1Ba2.2Cu4O8	Y	1	Ba	2.2	Cu	4															O	8			1993																											3	Y124	Ammm		A	3.845	3.869	27.265												K		80					80																																																																																														Y2O3,CeO2,CuO,Ba(NO3)2	1	CuO+Ba(NO3)2-heat(1175K,48H)-precursor(BaCu2O3 or Ba1.1Cu2O3)+Y2O3(or CeO2)-mix-pellet-SIN(1085K,1 week in flowing O2 at 1 atm)					Inflence of Ba Content and Ce Doping on the Structural Features of YBa2Cu4O8 Superconductor-a Neutron Study	1993		Solid State Physics Division, Bhabha Atomic Reserch Center, Bombay-400 085, India	J.Superconductivity,6(1993)265	A. Sequeira,H. Rajagopal,I.K. Gopalakrishnan,J.V. Yakhmi,R.M. Iyer		
5156	SSC0880813	addition of W and Mo stabilizes Sr base 123 phase	YSr2(Cu,Mo,W)3Oz	Y1Sr2Cu2.8Mo0.1W0.1Oz	Y	1	Sr	2	Cu	2.8	Mo	0.1	W	0.1											O	z			1993																											2				A	3.793		11.495												K	29.3	40.5	51.4	40.5			40.5																																																																																														Y2O3,SrCO3,CuO,MoO3,WO3	1	mixture-heat(800C,6H+920-960C,14H)-ground-pellet-heat(1000C,18H+500C,18H in air)-(500C,120H in flowing O2)					T(I)-O-T-(II) STRUCTURAL TRANSITION AND SUPERCONDUCTIVITY IN THE Sr-BASED 123 COMPOUNDS YSrCu2.8Mo0.1W0.1Oy			School of Materials Science and Engineering, University of New South Wales, PO Box 1, Kensington, NSW 2033, Australia	Solid State Commun.,88(1993)813-819	C. Andrikidis,F. Shi,H.K. Liu,J.A. Xia,S.X. Dou,Y. Zhao		
5157	PHC2320184		TlSr2Ca2Cu3Oz	Tl1Sr2Ca2Cu3Oz	Tl	1	Sr	2	Ca	2	Cu	3													O	z			1994																											2	Tl1223			A	3.814		15.267														107					107																																		HIR5157																																																												Tl2O3,V2O3,Sr2Ca2Cu3Oz	1	nominal Tl2V0.5Sr2Ca2Cu3Oz-pellet in covered Al2O3 crucible-heat(970C,5H in flowing O2)-cool to RT					Synthesis and properties of Tl0.6V0.5Sr2Ca2Cu3Ox	199410			Physica C,232 (1994) 184-188	K.C.Goretta,P.E.D.Morgan,S.Sengupta,Y.F.Li,Z.Z.Sheng	Tl,V,Sr,Ca,Cu,O	
5158	PHC2320184		TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3Oz	Tl	1	Ba	2	Ca	2	Cu	3													O	z			1994																											2	Tl1223			A	3.853		15.922														118					118																																		HIR5158																																																												Tl2O3,V2O3,Sr2Ca2Cu3Oz	1	nominal Tl2V0.5Sr2Ca2Cu3Oz-pellet in covered Al2O3 crucible-heat(970C,5H in flowing O2)-cool to RT					Synthesis and properties of Tl0.6V0.5Sr2Ca2Cu3Ox	199410			Physica C,232 (1994) 184-188	K.C.Goretta,P.E.D.Morgan,S.Sengupta,Y.F.Li,Z.Z.Sheng	Tl,V,Sr,Ca,Cu,O	
5159	PHC2320184		(Tl,V)Sr2Ca2Cu3Oz	Tl0.6V0.5Sr2Ca2Cu3Oz	Tl	0.6	V	0.5	Sr	2	Ca	2	Cu	3											O	z			1994																											2	Tl1223			A	3.824		15.16														110					110																																		HIR5159																																																												Tl2O3,V2O3,Sr2Ca2Cu3Oz	1	nominal Tl2V0.5Sr2Ca2Cu3Oz-pellet in covered Al2O3 crucible-heat(970C,5H in flowing O2)-cool to RT					Synthesis and properties of Tl0.6V0.5Sr2Ca2Cu3Ox	199410			Physica C,232 (1994) 184-188	K.C.Goretta,P.E.D.Morgan,S.Sengupta,Y.F.Li,Z.Z.Sheng	Tl,V,Sr,Ca,Cu,O	
5160	PHC2330209		Bi2Sr4Cu2(CO3)Oz	Bi2Sr4Cu2C1Oz	Bi	2	Sr	4	Cu	2	C	1													O	z			1994																											2				A	5.45		39.45																	10																																																																																																Bi2O3,Sr2CuO3	1	mixture-fire(850C,20H in flowing Ar(82%),O2(16%),2%CO2)-Q to RT-intercalate(180-250C, 1-6days)					Strcture and superconductivity of iodine-intercalated Bi2Sr4Cu2CO3Oz	199411			Physica C, 233 (1994) 209-213	H.Nameki,M.Kikuchi,N.Kobayashi,S.Awaji,Y.Muraoka,Y.Syono	Bi,Sr,Cu,C,O	
5161	PHC2330209		IBi2Sr4Cu2(CO3)Oz	I0.52Bi2Sr4Cu2C1Oz	I	0.52	Bi	2	Sr	4	Cu	2	C	1											O	z			1994																											2				A	5.45		23.36												K			20	23			23																																																																																														Bi2O3,Sr2CuO3	1	mixture-fire(850C,20H in flowing Ar(82%),O2(16%),2%CO2)-Q to RT-intercalate(180-250C, 1-6days)					Strcture and superconductivity of iodine-intercalated Bi2Sr4Cu2CO3Oz	199411			Physica C, 233 (1994) 209-213	H.Nameki,M.Kikuchi,N.Kobayashi,S.Awaji,Y.Muraoka,Y.Syono	Bi,Sr,Cu,C,O	
5162	PR04915993		NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7		1	1994																												Y123																		K		92.2					92.2																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5163	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.97Pr0.03Ba2Cu3O7	Nd	0.97	Pr	0.03	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		85.1					85.1																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5164	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.92Pr0.08Ba2Cu3O7	Nd	0.92	Pr	0.08	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		68.2					68.2																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5165	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.85Pr0.15Ba2Cu3O7	Nd	0.85	Pr	0.15	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		40.7					40.7																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5166	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O7	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		31.4					31.4																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5167	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.7Pr0.3Ba2Cu3O7	Nd	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		5.6					5.6																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5168	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.5Pr0.5Ba2Cu3O7	Nd	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1994								12.2																				Y123																		K																																																																																																					R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5169	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.4Pr0.6Ba2Cu3O7	Nd	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1994								13.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5170	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.3Pr0.7Ba2Cu3O7	Nd	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	1994								14.7																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5171	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.2Pr0.8Ba2Cu3O7	Nd	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								16.2																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5172	PR04915993		(Nd,Pr)Ba2Cu3O7	Nd0.1Pr0.9Ba2Cu3O7	Nd	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								16.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5173	PR04915993		PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		1	1994								17.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5174	PR04915993		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O	7		1	1994																												Y123																		K		96.2					96.2																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5175	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.97Pr0.03Ba2Cu3O7	Gd	0.97	Pr	0.03	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		93.1					93.1																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5176	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.922Pr0.078Ba2Cu3O7	Gd	0.922	Pr	0.078	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		84					84																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5177	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.85Pr0.15Ba2Cu3O7	Gd	0.85	Pr	0.15	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		67.9					67.9																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5178	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		57.7					57.7																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5179	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.7Pr0.3Ba2Cu3O7	Gd	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		39.6					39.6																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5180	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.6Pr0.4Ba2Cu3O7	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		20.9					20.9																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5181	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.4Pr0.6Ba2Cu3O7	Gd	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1994																												Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5182	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.3Pr0.7Ba2Cu3O7	Gd	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	1994																												Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5183	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.2Pr0.8Ba2Cu3O7	Gd	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994																												Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5184	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.1Pr0.9Ba2Cu3O7	Gd	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994																												Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5185	PR04915993		(Gd,Pr)Ba2Cu3O7	Gd0.5Pr0.5Ba2Cu3O7	Gd	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1994																												Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5186	PR04915993		ErBa2Cu3O7	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	7		1	1994																												Y123																		K		93.6					93.6																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5187	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.97Pr0.03Ba2Cu3O7	Er	0.97	Pr	0.03	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		93.9					93.9																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5188	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.924Pr0.076Ba2Cu3O7	Er	0.924	Pr	0.076	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		91.1					91.1																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5189	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.85Pr0.15Ba2Cu3O7	Er	0.85	Pr	0.15	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		82.9					82.9																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5190	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3O7	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		76.4					76.4																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5191	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.7Pr0.3Ba2Cu3O7	Er	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		61.1					61.1																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5192	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.6Pr0.4Ba2Cu3O7	Er	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		45.8					45.8																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5193	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.5Pr0.5Ba2Cu3O7	Er	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		28.6					28.6																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5194	PR04915993		(Eu,Pr)Ba2Cu3O7	Eu0.4Pr0.6Ba2Cu3O7	Eu	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1994								11.6																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5195	PR04915993		(Eu,Pr)Ba2Cu3O7	Eu0.3Pr0.7Ba2Cu3O7	Eu	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	1994								12.5																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5196	PR04915993		(Eu,Pr)Ba2Cu3O7	Eu0.2Pr0.8Ba2Cu3O7	Eu	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								14.6																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5197	PR04915993		(Eu,Pr)Ba2Cu3O7	Eu0.1Pr0.9Ba2Cu3O7	Eu	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								16.3																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5198	PR04915993		(Eu,Pr)Ba2Cu3O7	Eu0.5Pr0.5Ba2Cu3O7	Eu	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1994								9.6																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5199	PR04915993		(Sm,Pr)Ba2Cu3O7	Sm0.5Pr0.5Ba2Cu3O7	Sm	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	1994								11.1																																																																																																																																											R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5200	PR04915993		(Sm,Pr)Ba2Cu3O7	Sm0.4Pr0.6Ba2Cu3O7	Sm	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	1994								13.1																																																																																																																																											R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5201	PR04915993		(Sm,Pr)Ba2Cu3O7	Sm0.3Pr0.7Ba2Cu3O7	Sm	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	1994								13.4																																																																																																																																											R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5202	PR04915993		(Sm,Pr)Ba2Cu3O7	Sm0.2Pr0.8Ba2Cu3O7	Sm	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								15.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5203	PR04915993		(Sm,Pr)Ba2Cu3O7	Sm0.1Pr0.9Ba2Cu3O7	Sm	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								16.6																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5204	PR04915993		LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		1	1994																												Y123																		K		90.8					90.8																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5205	PR04915993		(Lu,Pr)Ba2Cu3O7	Lu0.85Pr0.15Ba2Cu3O7	Lu	0.85	Pr	0.15	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		89.7					89.7																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5206	PR04915993		(Lu,Pr)Ba2Cu3O7	Lu0.8Pr0.2Ba2Cu3O7	Lu	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		86.8					86.8																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5207	PR04915993		(Lu,Pr)Ba2Cu3O7	Lu0.7Pr0.3Ba2Cu3O7	Lu	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		73.5					73.5																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5208	PR04915993		(Lu,Pr)Ba2Cu3O7	Lu0.6Pr0.4Ba2Cu3O7	Lu	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1994																												Y123																		K		59.1					59.1																																																																																														R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5209	PR04915993		(Dy,Pr)Ba2Cu3O7	Dy0.3Pr0.7Ba2Cu3O7	Dy	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	1994								10.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5210	PR04915993		(Dy,Pr)Ba2Cu3O7	Dy0.2Pr0.8Ba2Cu3O7	Dy	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								13.2																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5211	PR04915993		(Dy,Pr)Ba2Cu3O7	Dy0.1Pr0.9Ba2Cu3O7	Dy	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								15.8																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5212	PR04915993		(Ho,Pr)Ba2Cu3O7	Ho0.2Pr0.8Ba2Cu3O7	Ho	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								12.7																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5213	PR04915993		(Ho,Pr)Ba2Cu3O7	Ho0.1Pr0.9Ba2Cu3O7	Ho	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								15.5																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5214	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.2Pr0.8Ba2Cu3O7	Er	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	1994								12.5																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5215	PR04915993		(Er,Pr)Ba2Cu3O7	Er0.1Pr0.9Ba2Cu3O7	Er	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								15																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5216	PR04915993		(Yb,Pr)Ba2Cu3O7	Yb0.1Pr0.9Ba2Cu3O7	Yb	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	1994								14																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5217	PR04915993		(Lu,Pr)Ba2Cu3O7	Lu0.1Py0.9Ba2Cu3O7	Lu	0.1	Py	0.9	Ba	2	Cu	3													O	7		1	1994								11.9																				Y123																																																																																																																							R2O3,Pr6O11,BaCO3,CuO	1	mixture-fired(940-960C,2days in air-reground-pellet-fire(940C-960C,2days)-slow cool to 450C-hold 10H-slow cool to RT-ANN(in flowing O2)					Ion-size effect on TN in (R1-xPrx)Ba2Cu3O7-z systems (R=Lu,Yb,Tm,Er,Y,Ho,Dy,Gd,Eu,Sm, and Nd)	199406			Phys.Rev.B, 49(1994)15993	H.F. Lai,H.F.Lai,J.C. Ho,J.Y.T. Wei,J.Y.T.Wei,M.K. Wu,M.K.Wu,S.R. Sheen,S.R.Sheen,Weiyan Guan,Y.C. Chen,Y.C.Chen,Yunhui Xu	R,Pr,Ba,Cu,O	
5218	PHC2320022	granular, grain size=150A	K3C60	K3C60	K	3	C	60																					1994																																														K						0.9																					T		40							T/K		2.8																																																																	C60 by sublimation method-K3C60 using two-zone high-temperature doping- annealing cell					Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
5219	PHC2320022	granular, grain size=250A	K3C60	K3C60	K	3	C	60																					1994																																														K						0.5																					T		33							T/K		2.33																																																																	C60 by sublimation method-K3C60 using two-zone high-temperature doping- annealing cell					Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
5220	PHC2320022	granular, grain size=310A	K3C60	K3C60	K	3	C	60																					1994																																														K						0.35																					T		28							T/K		2.18																																																																	C60 by sublimation method-K3C60 using two-zone high-temperature doping- annealing cell					Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
5221	PHC2320015	successive reducing , annealing 310C	(Hg,Ce)Sr2(Sr,Ca)Cu2O7	Hg0.4Ce0.6Sr2.5Ca0.4Cu2.1O7-z	Hg	0.4	Ce	0.6	Sr	2.5	Ca	0.4	Cu	2.1											O	7-z			1994																											3	Hg1212			A	3.818	7.606	24.379												K				51			51			K/GPa							90																																																																																				HgO,CeO2,SrO2,CaO,Nd2O3,CuO	1	mixture-in evacuated silica-heat(800C in 10H + hold 10H)-cool to 400C  in 10H					Cerium-mercury '1212' cuprates Hg0.4Ce0.5Sr3-xMxCu2.1O7-z  (M=Ca,Ce,Nd). A new series of superconductors	199410			Physica C,232 (1994) 15-21	A.Maignan,B.Raveau,C.Martin,C.Michel,M.Hervieu	Hg,Ce,Sr,Ca,Nd,Cu,O	
5222	PHC2320015		(Hg,Ce)Sr2(Sr,Ca,Nd)Cu2O7	Hg0.4Ce0.6Sr2.5Ca0.2Nd0.2Cu2.1O7-z	Hg	0.4	Ce	0.6	Sr	2.5	Ca	0.2	Nd	0.2	Cu	2.1									O	7-z			1994																																														K				65			65																																																																																														HgO,CeO2,SrO2,CaO,Nd2O3,CuO	1	mixture-in evacuated silica-heat(800C in 10H + hold 10H)-cool to 400C  in 10H					Cerium-mercury '1212' cuprates Hg0.4Ce0.5Sr3-xMxCu2.1O7-z  (M=Ca,Ce,Nd). A new series of superconductors	199410			Physica C,232 (1994) 15-21	A.Maignan,B.Raveau,C.Martin,C.Michel,M.Hervieu	Hg,Ce,Sr,Ca,Nd,Cu,O	
5223	PHC2320015	volume fraction is very small, x=0.5 in Ca<0.4-x>Nd<x>	(Hg,Ce)Sr2(Sr,Ca,Nd)Cu2O7	Hg0.4Ce0.6Sr2.5Ca-0.1Nd0.5Cu2.1O7-z	Hg	0.4	Ce	0.6	Sr	2.5	Ca	-0.1	Nd	0.5	Cu	2.1									O	7-z			1994																																														K				60			60																																																																																														HgO,CeO2,SrO2,CaO,Nd2O3,CuO	1	mixture-in evacuated silica-heat(800C in 10H + hold 10H)-cool to 400C  in 10H					Cerium-mercury '1212' cuprates Hg0.4Ce0.5Sr3-xMxCu2.1O7-z  (M=Ca,Ce,Nd). A new series of superconductors	199410			Physica C,232 (1994) 15-21	A.Maignan,B.Raveau,C.Martin,C.Michel,M.Hervieu	Hg,Ce,Sr,Ca,Nd,Cu,O	
5224	PHC2320277	after annealing over 20H, Tc remains constant	Ca(La,Ba)2Cu3O7	Ca1La1Ba1Cu3Oz	Ca	1	La	1	Ba	1	Cu	3													O	z		1	1994																												Y123																		K	77.9	79.1	80.1				79.1																																																																							m.ohm.cm											2.39												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5225	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.9Cd0.1La1Ba1Cu3Oz	Ca	0.9	Cd	0.1	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	75.9	76.7	77.8				76.7																																																																							m.ohm.cm											2.87												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5226	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.8Cd0.2La1Ba1Cu3Oz	Ca	0.8	Cd	0.2	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	75	76	76.9				76																																																																							m.ohm.cm											3.27												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5227	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.7Cd0.3La1Ba1Cu3Oz	Ca	0.7	Cd	0.3	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	69	70.8	72.6				70.8																																																																							m.ohm.cm											3.63												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5228	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.6Cd0.4La1Ba1Cu3Oz	Ca	0.6	Cd	0.4	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	69.4	67.3	70				67.3																																																																							m.ohm.cm											6												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5229	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.5Cd0.5La1Ba1Cu3Oz	Ca	0.5	Cd	0.5	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	55.9	58.4	61.5				58.4																																																																							m.ohm.cm											16.37												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5230	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.4Cd0.6La1Ba1Cu3Oz	Ca	0.4	Cd	0.6	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	44.8	47.8	51.3				47.8																																																																							m.ohm.cm											23.85												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5231	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.3Cd0.7La1Ba1Cu3Oz	Ca	0.3	Cd	0.7	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	31.5	36	39.8				36																																																																							m.ohm.cm											34.5												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5232	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.25Cd0.75La1Ba1Cu3Oz	Ca	0.25	Cd	0.75	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K	25.8	31.3	35.8				31.3																																																																							m.ohm.cm											48.7												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5233	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.2Cd0.8La1Ba1Cu3Oz	Ca	0.2	Cd	0.8	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K					10																																																																									m.ohm.cm											103.5												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5234	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Ca0.1Cd0.9La1Ba1Cu3Oz	Ca	0.1	Cd	0.9	La	1	Ba	1	Cu	3											O	z		1	1994																												Y123																		K					10																																																																									m.ohm.cm											160.1												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5235	PHC2320277		(Ca,Cd)(La,Ba)2Cu3O7	Cd1La1Ba1Cu3Oz	Cd	1	La	1	Ba	1	Cu	3													O	z		1	1994																												Y123																		K					10																																																																									m.ohm.cm											245.1												CaCO3,CdO,La2O3,BaCO3,CuO	1	mixture-CAL(900C,20H in air)-press-pellet-SIN(900C,24H in flowing O2)-cool to 600C(5C/min)-ANN(600C,20H in flowing O2)-FC to RT					Normal and superconducting properties in the Ca1-xCdxLaBaCu3Oy system	199410			Physica C,232 (1994) 277-282	J.-S.Wang,Q.R.Zhang,X.-J.Zhang,Z.-A.Xe,Z.-K.Jiao	Ca,Cd,La,Ba,Cu,O	
5236	PHC2330021	grain oriented sample, G-L parameter=127	HgBa2CuO4+z	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1994																												Hg1201			A															K		96					96											Oe	calculated from magnetization curve			123					T	calculated from magnetization curve			72					T/K				1.75			A	from Hc2		21.1		A			2680																																																			1	poly crystal-powder-grain oriented in a resin, in a magnetic field of 8 T for 24H at RT					Superconducting-state thermodynamic paramenters of HgBa2Can-1CunOy(N=1,2,and 3)	199411			Physica C,233 (1994) 21-29	H.Yamauchi,K.Isawa,R.Puzniak,R.Usami	Hg,Ba,Ca,Cu,O	
5237	PHC2330021	grain oriented sample, G-L parameter=126	HgBa2CaCu2O6+z	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1994																												Hg1212			A															K		127					127											Oe	calculated from magnetization curve			201					T	from magnetization curve			113					T/K				1.4			A	from Hc2		16.6		A			2090																																																			1	poly crystal-powder-grain oriented in a resin, in a magnetic field of 8 T for 24H at RT					Superconducting-state thermodynamic paramenters of HgBa2Can-1CunOy(N=1,2,and 3)	199411			Physica C,233 (1994) 21-29	H.Yamauchi,K.Isawa,R.Puzniak,R.Usami	Hg,Ba,Ca,Cu,O	
5238	PHC2330021	grain oriented sample, G-L parameter=80	HgBa2Ca2Cu3O8+z	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																												Hg1223			A															K		135					135			K/GPa								Oe	from magnetization curve			335					T	from magnetization curve			88					T/K				1.2			A	from Hc2		19.3		A			1550																																																			1	poly crystal-powder-grain oriented in a resin, in a magnetic field of 8 T for 24H at RT					Superconducting-state thermodynamic paramenters of HgBa2Can-1CunOy(N=1,2,and 3)	199411			Physica C,233 (1994) 21-29	H.Yamauchi,K.Isawa,R.Puzniak,R.Usami	Hg,Ba,Ca,Cu,O	
5239	PHC2330001		(Hg,Mo)Sr2CuOz	Hg0.7Mo0.3Sr2Cu1Oz	Hg	0.7	Mo	0.3	Sr	2	Cu	1													O	z			1994																											2	Hg1201			A	3.8		8.86															58	56			56			K/GPa							1.5																																																																																				SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5240	PHC2330001		(Hg,Re)Sr2(Ca,Y)Cu2Oz	Hg0.8Re0.2Sr2Ca0.7Y0.3Cu2Oz	Hg	0.8	Re	0.2	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	z		1	1994																											2	Hg1212			A	3.818		11.879												K	83		100				91.5																																																																																														SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5241	PHC2330001		HgSr2(Ca,Y)(Cu,Re)2Oz	Hg1Sr2Ca0.7Y0.3Cu1.8Re0.2Oz	Hg	1	Sr	2	Ca	0.7	Y	0.3	Cu	1.8	Re	0.2									O	z		1	1994																											2	Hg1212			A	3.818		11.879												K	83		100				91.5																																																																																														SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5242	PHC2330001	resistivity did not show zero down to 4.2K	HgSr2(Cu,Re)Oz	Hg1Sr2Cu0.9Re0.1Oz	Hg	1	Sr	2	Cu	0.9	Re	0.1													O	z			1994																											2	Hg1201			A	3.783		8.883												K			70	62			62										9.5																																																																																				SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5243	PHC2330001	Tirr = 55.1K, for 0.3=<Y content =<0.7 nearly single phase, vols for H=1 Oe,	(Hg,Mo)Sr2(Ca,Y)Cu2Oz	Hg0.7Mo0.3Sr2Ca0.7Y0.3Cu2Oz	Hg	0.7	Mo	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	z			1994																															A	3.821		11.927												K	73		95	96			96										92																																																																																				SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5244	PHC2330001	Tirr = 34.8K, vols for H=1 Oe	(Hg,Mo)Sr2(Ca,Y)Cu2Oz	Hg0.7Mo0.3Sr2Ca0.5Y0.5Cu2Oz	Hg	0.7	Mo	0.3	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	z			1994																															A	3.823		11.898												K			89.3				89.3										69																																																																																				SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5245	PHC2330001	Tirr = 30.3 K, vols for H=1 Oe	(Hg,Mo)Sr2(Ca,Y)Cu2Oz	Hg0.7Mo0.3Sr2Ca0.3Y0.7Cu2Oz	Hg	0.7	Mo	0.3	Sr	2	Ca	0.3	Y	0.7	Cu	2									O	z			1994																															A	3.823		11.806												K			84				84										3																																																																																				SrCO3,CaCO3,CuO,MoO3	1	precursor Mo-Sr-(Ca,Y)-Cu-O + HgO - mix - press-pellet-seal in evacuated quartz tube-SIN(860-940C,10-40H)-Q to RT					New barium-free mercury-based high-Tc superconductors (Hg,Mo)Sr2(Ca,Y)n-1CunOy and HgSr2(Ca,Y)n-1(Cu,Re)nOy (n=1 and 2)	199411			Physica C,233 (1994) 1-7	J.Shimoyama,K.Kishio,O.Shiino,S.Hahakura	Re,Hg,Mo,Sr,Ca,Y,Cu,O	
5246	SUP0070853			Y1Ba2Cu3O6.83	Y	1	Ba	2	Cu	3															O	7-Z	6.83	1	1994																											3	Y123			A	3.822	3.888	11.667																																																																																																																								Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5247	SUP0070853			Y1Ba2Cu2.97Zr0.03O6.94	Y	1	Ba	2	Cu	2.97	Zr	0.03													O	7-z	6.94	1	1994																											3	Y123			A	3.859	3.88	11.86																																																																																																																								Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5248	SUP0070853			Y1Ba2Cu2.94Zr0.06O6.82	Y	1	Ba	2	Cu	2.94	Zr	0.06													O	7-z	6.82	1	1994																											3	Y123			A	3.859	3.88	11.86																																																																																																																								Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5249	SUP0070853			Y1Ba2Cu2.91Zr0.09O6.73	Y	1	Ba	2	Cu	2.91	Zr	0.09													O	7-z	6.73	1	1994																											3	Y123			A	3.859	3.88	11.86																																																																																																																								Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5250	SUP0070853			Y1Ba2Cu2.88Zr0.12O7-z	Y	1	Ba	2	Cu	2.88	Zr	0.12													O	7-z			1994																											3	Y123			A	3.858	3.88	11.86													84.4			84			84																																																																																																					Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5251	SUP0070853			Y1Ba2Cu2.85Zr0.15O7-z	Y	1	Ba	2	Cu	2.85	Zr	0.15													O	7-z			1994																											3	Y123			A	3.859	3.881	11.86													82.5						82.5																																																																																																					Influence of Zr Substitution on Superconductity of YBa2Cu3O7-delta	1994		Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity,7(1994)853	D.G. Kuberkar,G.J. Baldha,I.A. Shaikh,J.A. Bhalodia,R.G. Kulkarni		
5252	PHC2310009	multi-phases. small amount of Hg1201-phase.	HgSr2CuO4	Hg1Sr2Cu1O4+z	Hg	1	Sr	2	Cu	1															O	4+z			1994																											2	Hg1201																		K		56					56																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5253	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.95Mo0.05Sr2Cu1O4+z	Hg	0.95	Mo	0.05	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.782		8.846												K		58					58																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5254	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.9Mo0.1Sr2Cu1O4+z	Hg	0.9	Mo	0.1	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.785		8.841												K		72					72																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5255	PHC2310009	highest Tc in (Hg,Mo)Sr2CuO4.	(Hg,Mo)Sr2CuO4	Hg0.85Mo0.15Sr2Cu1O4+z	Hg	0.85	Mo	0.15	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.787		8.844												K		78					78																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5256	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.8Mo0.2Sr2Cu1O4+z	Hg	0.8	Mo	0.2	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.797		8.818												K		72					72																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5257	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.75Mo0.25Sr2Cu1O4+z	Hg	0.75	Mo	0.25	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.795		8.816												K		50					50																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5258	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.7Mo0.3Sr2Cu1O4+z	Hg	0.7	Mo	0.3	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.798		8.81												K		20					20																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5259	PHC2310009		(Hg,Mo)Sr2CuO4	Hg0.65Mo0.35Sr2Cu1O4+z	Hg	0.65	Mo	0.35	Sr	2	Cu	1													O	4+z			1994																											2	Hg1201			A	3.798		8.801												K		9					9																																																																																														SrCO3,Sr(NO3)2,CuO	1	precursor(Sr2CuO3,SrCuO2,Sr14Cu24O41) + (MoO3,HgO) - (sealed quartz tube) - heat(850-880C,8h) - cool to RT(150C/h)					A new 78 K superconductor by Mo substitution	199409			Physica C,231(1994) 9-14	A.P.B.Sinha,D.E.Morris,K.K.Singh,K.Ksingh,V.Kirtikar	Mo,Hg,Sr,Cu,O	
5260	PHC2310015			Hg0.5Pb0.5Sr3Ba1Cu3C1O7	Hg	0.5	Pb	0.5	Sr	3	Ba	1	Cu	3	C	1									O	7			1994																											2				A	3.845		16.728																																																																																																																								Structural and physical properties of the new superconductor Hg0.5Pb0.5Sr4-xBaxCu2(CO3)O7-z	199409			Physica C,231(1994) 15-20	A.Maignan,B.Raveau,G.Van Tendeloo,M.Hervieu,M.Huve	Hg,Pb,Sr,Ba,Cu,C,O	
5261	PHC2310015			Hg0.5Pb0.5Sr3Ba1Cu3C1O7	Hg	0.5	Pb	0.5	Sr	3	Ba	1	Cu	3	C	1									O	7			1994																											2				A	3.845		16.728																																																																																																																								Structural and physical properties of the new superconductor Hg0.5Pb0.5Sr4-xBaxCu2(CO3)O7-z	199409			Physica C,231(1994) 15-20	A.Maignan,B.Raveau,G.Van Tendeloo,M.Hervieu,M.Huve	Hg,Pb,Sr,Ba,Cu,C,O	
5262	PHC2330143		(Cu,C)2(Ba,Ca)Ca2Cu3O11	C1Ba2.5Ca2.5Cu4Oz	C	1	Ba	2.5	Ca	2.5	Cu	4													O	z			1994																											2	Cu2323			A	3.852		18.61														113		91			113																																																																																																					A new oxycarbonate superconductor (Cu0.5C0.5)2Ba3Ca2Cu3O11 (Tc=91K) prepared at high pressure	199411			Physica C,233(1994) 143-148	T.Kawashima,Takayama-Muromachi,Y.Matsui	C,Ba,Ca,Cu,O	
5263	PHC2310293		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4			1994																												T																																																																																												83.8			TP5263																					RH5263			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5264	PHC2310293		(La,Sr)2(Cu,Zn)O4	La1.92Sr0.08Cu0.994Zn0.006O4	La	1.92	Sr	0.08	Cu	0.994	Zn	0.006													O	4			1994																												T																																																																																																																				RH5264			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5265	PHC2310293		(La,Sr)2(Cu,Zn)O4	La1.92Sr0.08Cu0.96Zn0.04O4	La	1.92	Sr	0.08	Cu	0.96	Zn	0.04													O	4			1994																												T																																																																																												75			TP5265																					RH5265			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5266	PHC2310293		(La,Sr)2(Cu,Zn)O4	La1.92Sr0.08Cu0.94Zn0.06O4	La	1.92	Sr	0.08	Cu	0.94	Zn	0.06													O	4			1994																												T																																																																																												72			TP5266																					RH5266			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5267	PHC2310293		(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O	4			1994																												T																																																																																																																				RH5267			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5268	PHC2310293		(La,Sr)2CuO4	La1.94Sr0.06Cu1O4	La	1.94	Sr	0.06	Cu	1															O	4			1994																												T																																																																																												103			TP5268																					RH5268			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5269	PHC2310293		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1994																												T																																																																																												57.3			TP5269																					RH5269			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5270	PHC2310293		(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4			1994																												T																																																																																												38.7			TP5270																					RH5270			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5271	PHC2310293		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1994																												T																																																																																															TP5271																					RH5271			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5272	PHC2310293		(Nd,Ce)2CuO4	Nd1.84Ce0.16Cu1O4	Nd	1.84	Ce	0.16	Cu	1															O	4			1994																												T'																																																																																												-2.64			TP5272																								La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5273	PHC2310293		(Nd,Ce)2CuO4	Nd1.87Ce0.13Cu1O4	Nd	1.87	Ce	0.13	Cu	1															O	4			1994																												T'																																																																																												-10.4			TP5273																								La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5274	PHC2310293		(Nd,Ce)2CuO4	Nd1.9Ce0.1Cu1O4	Nd	1.9	Ce	0.1	Cu	1															O	4			1994																												T'																																																																																												-24.4			TP5274																					RH5274			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5275	PHC2310293		(Nd,Ce)2CuO4	Nd1.93Ce0.07Cu1O4	Nd	1.93	Ce	0.07	Cu	1															O	4			1994																												T'																																																																																												-45.5			TP5275																					RH5275			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5276	PHC2310293		(Nd,Ce)2CuO4	Nd1.96Ce0.04Cu1O4	Nd	1.96	Ce	0.04	Cu	1															O	4			1994																												T'																																																																																												-115			TP5276																					RH5276			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5277	PHC2310293		(La,Sr)2(Cu,Ni)O4	La1.92Sr0.08Cu0.98Ni0.02O4	La	1.92	Sr	0.08	Cu	0.98	Ni	0.02													O	4			1994																												T																																																																																																																				RH5277			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5278	PHC2310293		(La,Sr)2(Cu,Ni)O4	La1.92Sr0.08Cu0.96Ni0.04O4	La	1.92	Sr	0.08	Cu	0.96	Ni	0.04													O	4			1994																												T																																																																																												130			TP5278																					RH5278			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5279	PHC2310293		(La,Sr)2(Cu,Ni)O4	La1.92Sr0.08Cu0.94Ni0.06O4	La	1.92	Sr	0.08	Cu	0.94	Ni	0.06													O	4			1994																												T																																																																																																																				RH5279			La2O3,SrCO3,CuO,MO	1	mixture-heat(1000C,12H)-reground-pellet-SIN(1080C,2days in air)-FC					Transport studies of La1.92Sr0.08Cu1-xMxO4(M=Ni and Zn) and Nd2-yCeyCuO4 up to about 900 K	199409			Physica C,231 (1994) 293-299	J.Takeda,M.Sato,T.Nishikawa	Ce,Nd,La,Sr,Cu,Ni,Zn,O	
5280	SUP0070773	reduced crystal, in-plane thermopower	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+z	Nd	1.85	Ce	0.15	Cu	1															O	4+z			1994																												T'																																																																																												-0.85			TP5280																										crystal was grown by a directional solidification technique-ANN(in reduced atmosphere)					Anomalous Normal State Magnetothermopower of Electron-Doped Nd1.85Ce0.15CuO4+delta Crystals	1994		Center for Superconductivity Reserch, Department of physics, University of Maryland, College Park, Maryland 20742	J.Superconductivity,7(1994)773	J. L. Peng,R. L. Greene,S. J. Hagen,Wu jiang,X. Q. Xu,Z. Y. Li		
5281	SUP0070773	as-grown crystal, in-plane thermopower	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+z	Nd	1.85	Ce	0.15	Cu	1															O	4+z			1994																												T'																																																																																												-14.4			TP5281																										crystal was grown by a directional solidification technique-ANN(in reduced atmosphere)					Anomalous Normal State Magnetothermopower of Electron-Doped Nd1.85Ce0.15CuO4+delta Crystals	1994		Center for Superconductivity Reserch, Department of physics, University of Maryland, College Park, Maryland 20742	J.Superconductivity,7(1994)773	J. L. Peng,R. L. Greene,S. J. Hagen,Wu jiang,X. Q. Xu,Z. Y. Li		
5282	SUP0070813		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1994																											2	T			A	3.78		13.22													33.8		37.1				35.45																																																																	THC5282																													La2O3,SrCO3(or CaCO3),CuO		mixture-CAL(1000C,12H in air)-pellet-SIN(1000C,12H in flowing O2)-cool to RT(1000C/H)					Thermal Coductivity and Electrical Resistivity of the T' Phase and the T Phase in 2-1-4 Oxide Superconductors	1994		Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930, Japan	J.Superconductivity,7(1994)813	Atsushi Tanaka,Junji Sakurai,Katsuhiko Nishimura,Katsunori Mori,Koshichi Noto,Michiaki Matsukawa,Yoshikazu Isikawa		
5283	SUP0070813		(La,Ca)2CuO4	La1.935Ca0.065Cu1O4	La	1.935	Ca	0.065	Cu	1															O	4		1	1994																											2	T			A	3.78		13.14													2.3		8.8				5.55																																																																	THC5283																													La2O3,SrCO3(or CaCO3),CuO		mixture-CAL(1000C,12H in air)-pellet-SIN(1000C,12H in flowing O2)-cool to RT(1000C/H)					Thermal Coductivity and Electrical Resistivity of the T' Phase and the T Phase in 2-1-4 Oxide Superconductors	1994		Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930, Japan	J.Superconductivity,7(1994)813	Atsushi Tanaka,Junji Sakurai,Katsuhiko Nishimura,Katsunori Mori,Koshichi Noto,Michiaki Matsukawa,Yoshikazu Isikawa		
5284	SUP0070813		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4			1994																												T'			A	3.95		12.09													14.3		26.4				20.35																																																											450	calculated from thermal conductivity					THC5284																													Nd2O3,CeO2,CuO		mixture-CAL(900C,2H in air)-pellet-SIN(1100C,18H in flowing O2)-cool to RT-ANN(910C,16H in Ar)-Q to RT					Thermal Coductivity and Electrical Resistivity of the T' Phase and the T Phase in 2-1-4 Oxide Superconductors	1994		Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930, Japan	J.Superconductivity,7(1994)813	Atsushi Tanaka,Junji Sakurai,Katsuhiko Nishimura,Katsunori Mori,Koshichi Noto,Michiaki Matsukawa,Yoshikazu Isikawa		
5285	SUP0070813		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4			1994																												T'			A	3.96		12.16													16		23				19.5																																																											550	calculated from thermal conductivity					THC5285																													Pr2O11,CeO2,CuO		CAL(900C,20H in air)-SIN(1050C,16H in air)-ANN(850C,60H in Ar)-Q to RT					Thermal Coductivity and Electrical Resistivity of the T' Phase and the T Phase in 2-1-4 Oxide Superconductors	1994		Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930, Japan	J.Superconductivity,7(1994)813	Atsushi Tanaka,Junji Sakurai,Katsuhiko Nishimura,Katsunori Mori,Koshichi Noto,Michiaki Matsukawa,Yoshikazu Isikawa		
5286	APJ0331314		EuBa2Cu3O7	Eu1Ba2Cu3OZ	Eu	1	Ba	2	Cu	3															O	Z			1994																												Y123																										TC5286																																																																																													BaCo3,Eu2O3,CuO	1	mix using wet ball mill-CAL(960C,6H in air)-ground-pellet-SIN(960C,24H in O2)-ANN(500-800C,10-1e+5 Pa O2)					Relationship between Tc and Cu Valence and Bond Lengths of Cu-Cu and Cu-O for Ba2-xEu1+xCu3O7-y Compounds	3			Jpn.J.Appl.Phys.,33A (1994) 1314-1319	Katsuro Okuyama,Nobuo Tanaka,Shigetoshi Ohshima,Shiro Kambe	Ba,Eu,Cu,O	
5287	JJP0331149	compositions analyzed by EDX	(Cu,C)(Ba,Ca)2(Y,Ca)Cu2Oz	Ba1.96Ca0.12Y0.92C0.21Cu2.79Oz	Ba	1.96	Ca	0.12	Y	0.92	C	0.21	Cu	2.79											O	z			1994																												Cu1212			A	3.858		11.665												K		85		85			85																																																																																														BaCO3,CaCO3,Y2O3,CuO		(mixture+KClO3 as O-resource)-sealed in Au capsule-heat(980-1010C,5H under 2 GPa)-Q to RT					High-Pressure Synthesis of Superconducting(Cu,C)-1212 Compound (Cu,C)Ba2(Y,Ca)Cu2Oz	199408			Jpn.J.Appl.Phys.Lett.,33(1994)l1149-1152	Akira Ono,Shigeo Horiuchi	Cu,C,Ba,Y,Ca,O	
5288	JJP0331399	almost single phase	GaSr2Ca3Cu4O11	Ga1Sr2Ca3Cu4O10.8	Ga	1	Sr	2	Ca	3	Cu	4													O	10.8		1	1994																											3	Ga1234			A	5.462	5.417	35.78												K				93			93																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5289	JJP0331399		GaSr2Ca3Cu4O11	Ga1Sr2Ca3Cu4O10.9	Ga	1	Sr	2	Ca	3	Cu	4													O	10.9			1994																											3	Ga1234																		K				100			100																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5290	JJP0331399	two step transition lower=70-80 K, Ga1223 phase included	GaSr2Ca3Cu4O11	Ga1Sr2Ca3Cu4O11.	Ga	1	Sr	2	Ca	3	Cu	4													O	11.0			1994																											3	Ga1234																		K				107			107																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5291	JJP0331399	two step transition , lower=70-80 K, Ga1223 phase included	GaSr2Ca3Cu4O11	Ga1Sr2Ca3Cu4O11.1	Ga	1	Sr	2	Ca	3	Cu	4													O	11.1			1994																											3	Ga1234																		K				107			107																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5292	JJP0331399	single step transition	GaSr2Ca3Cu4O11	Ga1Sr2Ca3Cu4O11.5	Ga	1	Sr	2	Ca	3	Cu	4													O	11.5			1994																											3	Ga1234																		K				63			63																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5293	JJP0331399	upper transition at about 100K, maybe Ga1234 phase included though it's not detected by x-ray diffraction	GaSr2Ca3Cu4O9	Ga1Sr2Ca3Cu4OZ	Ga	1	Sr	2	Ca	3	Cu	4													O	Z			1994																											3	Ga1223			A	5.454	5.391	29.371												K				70			70																																																																																														Ca2CuO3,SrCuO2,CuO,Ga2O3,SrO2	1	conventional solid state reaction, oxygen content was controlled by the amount of SrO2,(1250C,6GPa in a belt-type high-pressure apparatus)					New Series of High Tc Superconductors,GaSr2Can-1CunO2n+3(n=3; Tc=70 K,n=4; Tc=107 K) Prepared at High Pressure	199409			Jpn.J.Appl.Phys.Lett.,33(1994)L1399-1402	Eiji Takayama-Muromachi,Masaki Isobe	Ga,Sr,Ca,Cu,O	
5294	APJ0332515	precursor(Sr-Ho-Ca-Cu-O) + PbO+flux(NaCl)	Pb2Sr2(Ho,Ca)Cu3O8	Pb2Sr2Ho0.5Ca0.5Cu3O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	3											O	8		3	1994																												Pb3212																		K		78.5				0.7	78.5																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5295	APJ0334583		YBa2Cu3O7	Y1Ba2Cu3O6.887	Y	1	Ba	2	Cu	3															O	z	6.887		1994																											3	Y123			A	3.84	3.886	11.666												K	89.8					1.2	89.8																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5296	APJ0334583		YBa2Cu3O7	Y1Ba2Cu3O6.791	Y	1	Ba	2	Cu	3															O	z	6.791		1994																											3	Y123			A	3.824	3.891	11.683												K	86.9					1.7	86.9																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5297	APJ0334583		YBa2Cu3O7	Y1Ba2Cu3O6.821	Y	1	Ba	2	Cu	3															O	z	6.821		1994																											3	Y123			A	3.821	3.89	11.678												K	91.1					2	91.1																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5298	APJ0334583	ANN(350C,10H)	YBa2Cu3O7	Y1Ba2Cu3O6.869	Y	1	Ba	2	Cu	3															O	z	6.869		1994																											3	Y123			A	3.829	3.889	11.669												K	90					2	90																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5299	APJ0334583	ANN(400C,10H)	YBa2Cu3O7	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	z	6.87		1994																											3	Y123			A	3.82	3.891	11.669												K	88.7					2.2	88.7																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5300	APJ0334583		YBa2Cu3O7	Y1Ba2Cu3O6.852	Y	1	Ba	2	Cu	3															O	z	6.852		1994																											3	Y123			A	3.841	3.887	11.672												K	89.2					2.4	89.2																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5301	APJ0334583		YBa2Cu3OZ	Y1Ba2Cu3O6.858	Y	1	Ba	2	Cu	3															O	Z	6.858		1994																											3	Y123			A	3.831	3.885	11.671												K	87.4					3.9	87.4																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5302	APJ0334583	ANN(400C,10H)	YBa2Cu3Oz	Y1Ba2Cu3O6.937	Y	1	Ba	2	Cu	3															O	z	6.937		1994																											3	Y123			A	3.828	3.915	11.656												K	84.8					5.3	84.8																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5303	APJ0334583	ANN(300C,10H)	YBa2Cu3Oz	Y1Ba2Cu3O6.838	Y	1	Ba	2	Cu	3															O	z	6.838		1994																											3	Y123			A	3.827	3.889	11.675												K	84.8					6.4	84.8																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5304	APJ0334583		YBa2Cu3Oz	Y1Ba2Cu3O6.861	Y	1	Ba	2	Cu	3															O	z	6.861		1994																											3	Y123			A	3.854	3.888	11.671												K	80.5					7.9	80.5																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5305	APJ0334583		YBa2Cu3Oz	Y1Ba2Cu3O6.894	Y	1	Ba	2	Cu	3															O	z	6.894		1994																											3	Y123			A	3.835	3.886	11.664												K	80.5					9.2	80.5																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5306	APJ0334583		YBa2Cu3Oz	Y1Ba2Cu3O6.876	Y	1	Ba	2	Cu	3															O	z	6.876		1994																											3	Y123			A	3.852	3.885	11.668												K	78.1					11.2	78.1																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5307	APJ0334583	ANN(375C,10H)	YBa2Cu3Oz	Y1Ba2Cu3O6.883	Y	1	Ba	2	Cu	3															O	z	6.883		1994																											3	Y123			A	3.886	3.886	11.666												K	74					11.6	74																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5308	APJ0334583	ANN(400C,10H)	YBa2Cu3Oz	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	z	6.87		1994																											3	Y123			A	3.846	3.886	11.669												K	75.1					11.7	75.1																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5309	APJ0334583	ANN(850C,10H)	YBa2Cu3Oz	Y1Ba2Cu3O6.829	Y	1	Ba	2	Cu	3															O	z	6.829		1994																											3	Y123			A	3.869	3.894	11.676												K	57.7					23.4	57.7																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5310	APJ0334583		YBa2Cu3Oz	Y1Ba2Cu3O6.729	Y	1	Ba	2	Cu	3															O	z	6.729		1994																											3	Y123			A	3.861	3.889	11.695												K	56.8					28.2	56.8																																																																																															1	pellet-heat to (900-950C) at 300C/H-cool to RT at 300C/H or Q to LN2)-some were annealed or quenched, oxygen content estimated from lattice constant					Examinations of Superconducting Transition Width, Oxygen Deficiency and Crystallographic Quality in YBa2Cu3O7-z	8			Jpn.J.Appl.Phys.,33(1994) 4583-4592	Akihiko Nishida,Kauzumi Forai,Kouki Furuya,Nobuhiro Fuketa	Y,Ba,Cu,O	
5311	JJP0330507		YBa2Cu3O7Hx	Y1Ba2Cu3H0.2O6.98	Y	1	Ba	2	Cu	3	H	0.2													O	7	6.98		1994																											3	Y123																		K	94.2	94.5	94.7				94.5																																																																																																YBa2Cu3O7-ground to fine grains-hydrogenation using the Sievelt gas absorption system(1.25 atm H2, 200C)					Hydrogen-Absorption Effect on YBa2Cu3Ox	199404			Jpn.J.Appl.Phys.Lett.,33(1994)L507-509	Hiroyuki Kaneko,Hitoshi Taimatsu,Katsuyuki Fujiwara,Takeji Kebukawa,Yoshitaka Kumaki,Yukichi Tatsumi	Y,Ba,Cu,O	
5312	JJP0330507		YBaCu3O7Hx	Y1Ba2Cu3H1.4O6.98	Y	1	Ba	2	Cu	3	H	1.4													O	7	6.98		1994																											3	Y123																		K	91.5	92	92.4				92																																																																																																YBa2Cu3O7-ground to fine grains-hydrogenation using the Sievelt gas absorption system(1.25 atm H2, 200C)					Hydrogen-Absorption Effect on YBa2Cu3Ox	199404			Jpn.J.Appl.Phys.Lett.,33(1994)L507-509	Hiroyuki Kaneko,Hitoshi Taimatsu,Katsuyuki Fujiwara,Takeji Kebukawa,Yoshitaka Kumaki,Yukichi Tatsumi	Y,Ba,Cu,O	
5313	JJP0330503	as-sintered sample, minor phase=Cu1245,BaCuO2, unknown and amorphous phases are included	CuBa2Ca3Cu4O12	Cu5Ba2Ca3O12-z	Cu	5	Ba	2	Ca	3															O	12-z		1	1994																											2	Cu1234	P4/mmm		A	3.856		17.993												K	109.3	116.3	117.1	116.4			116.3			K/GPa							70																																																																																				BaCO3,CaCO3,CuO	1	mixture of Ba2CaCu5O8,Ba2Ca2Cu5O9,Ba2CaCu4O7,Ba2Ca2Cu4O8, Ba2Ca3Cu4O9, CaO2,-SIN(1100C,3H under a pressure of 5GPa)					New High-Tc Superconductor Family oof Cu-Based Cu1-xBa2Can-1CunO2n+4-z with Tc>116K	199404			Jpn.J.Apll.Phys.Lett.,33(1994)L503-506	Akira Negishi,Hideo Ihara,Hirofumi Matuhata,Hirotomo Ozawa,Kazuyasu Tokiwa,Masayuki Hirabayashi,Young Seok Song	Cu,Ba,Ca,O	
5314	JJP0330219		(Y,K)Ba2Cu3O7	Y0.95K0.05Ba2Cu3O6.6	Y	0.95	K	0.05	Ba	2	Cu	3													O	z	6.6		1994																											3	Y123			A	3.825	3.896	11.688												K	86.7		92.1			5.4	89.4																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5315	JJP0330219		(Y.K)Ba2Cu3O7	Y0.9K0.1Ba2Cu3O6.51	Y	0.9	K	0.1	Ba	2	Cu	3													O	z	6.51	1	1994																											3	Y123			A	3.825	3.896	11.692												K	89.8		94.3			4.5	92.05																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5316	JJP0330219		(Y,K)Ba2Cu3O7	Y0.85K0.15Ba2Cu3O6.48	Y	0.85	K	0.15	Ba	2	Cu	3													O	z	6.48	1	1994																											3	Y123			A	3.823	3.896	11.69												K	88.7		91.6			2.9	90.15																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5317	JJP0330219		(Y,Rb)Ba2Cu3O7	Y0.95Rb0.05Ba2Cu3O6.59	Y	0.95	Rb	0.05	Ba	2	Cu	3													O	z	6.59	1	1994																											3	Y123			A	3.824	3.897	11.694												K	90.3		93.8			3.5	92.05																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5318	JJP0330219		(Y,Rb)Ba2Cu3O7	Y0.9Rb0.1Ba2Cu3O6.42	Y	0.9	Rb	0.1	Ba	2	Cu	3													O	z	6.42	1	1994																											3	Y123			A	3.825	3.896	11.693												K	91		93.8			2.8	92.4																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5319	JJP0330219		(Y,Rb)Ba2Cu3O7	Y0.85Rb0.15Ba2Cu3O6.48	Y	0.85	Rb	0.15	Ba	2	Cu	3													O	z	6.48	1	1994																											3	Y123			A	3.822	3.896	11.694												K	89.5		94.4			4.9	91.95																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5320	JJP0330219		(Y,Cs)Ba2Cu3O7	Y0.95Cs0.05Ba2Cu3O6.61	Y	0.95	Cs	0.05	Ba	2	Cu	3													O	z	6.61	1	1994																											3	Y123			A	3.823	3.896	11.69												K	89.4		95.5			6.1	92.45																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5321	JJP0330219		(Y,Cs)Ba2Cu3O7	Y0.9Cs0.1Ba2Cu3O6.47	Y	0.9	Cs	0.1	Ba	2	Cu	3													O	z	6.47	1	1994																											3	Y123			A	3.827	3.895	11.685												K	89		93.6			4.6	91.3																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5322	JJP0330219		(Y,Cs)Ba2Cu3O7	Y0.85Cs0.15Ba2Cu3O6.5	Y	0.85	Cs	0.15	Ba	2	Cu	3													O	z	6.5	1	1994																											3	Y123			A	3.823	3.897	11.696												K	87.9		92.9			5	90.4																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5323	JJP0330219		Y(Ba,K)2Cu3O7	Y1Ba1.9K0.1Cu3O6.61	Y	1	Ba	1.9	K	0.1	Cu	3													O	z	6.61	1	1994																											3	Y123			A	3.829	3.896	11.693												K	91.8		93.6			1.8	92.7																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5324	JJP0330219		Y(Ba,K)2Cu3O7	Y1Ba1.8K0.2Cu3O6.57	Y	1	Ba	1.8	K	0.2	Cu	3													O	z	6.57	1	1994																											3	Y123			A	3.836	3.896	11.691												K	92.4		93.6			1.2	93																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5325	JJP0330219		Y(Ba,K)2Cu3O7	Y1Ba1.7K0.3Cu3O6.54	Y	1	Ba	1.7	K	0.3	Cu	3													O	z	6.54	1	1994																											3	Y123			A	3.828	3.895	11.687												K	92		93.7			1.7	92.85																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5326	JJP0330219		Y(Ba,Rb)2Cu3O7	Y1Ba1.9Rb0.1Cu3O6.52	Y	1	Ba	1.9	Rb	0.1	Cu	3													O	z	6.52	1	1994																											3	Y123			A	3.825	3.895	11.687												K	92.4		94.3			1.9	93.35																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5327	JJP0330219		Y(Ba,Rb)2Cu3O7	Y1Ba1.8Rb0.2Cu3O6.56	Y	1	Ba	1.8	Rb	0.2	Cu	3													O	z	6.56	1	1994																											3	Y123			A	3.825	3.893	11.684												K	89		92.1			3.1	90.55																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5328	JJP0330219		Y(Ba,Rb)2Cu3O7	Y1Ba1.7Rb0.3Cu3O6.52	Y	1	Ba	1.7	Rb	0.3	Cu	3													O	z	6.52	1	1994																											3	Y123			A	3.826	3.895	11.684												K	89.7		92.4			2.7	91.05																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5329	JJP0330219		Y(Ba,Cs)2Cu3O7	Y1Ba1.9Cs0.1Cu3O6.65	Y	1	Ba	1.9	Cs	0.1	Cu	3													O	z	6.65	1	1994																											3	Y123			A	3.826	3.895	11.688												K	91.9		95			3.1	93.45																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5330	JJP0330219		Y(Ba,Cs)2Cu3O7	Y1Ba1.8Cs0.2Cu3O6.58	Y	1	Ba	1.8	Cs	0.2	Cu	3													O	z	6.58	1	1994																											3	Y123			A	3.827	3.893	11.684												K	91.9		94.7		2.8		93.3																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5331	JJP0330219		Y(Ba,Cs)Cu3O7	Y1Ba1.7Cs0.3Cu3O6.6	Y	1	Ba	1.7	Cs	0.3	Cu	3													O	z	6.6	1	1994																											3	Y123			A	3.826	3.896	11.69												K	92.2		95.3			3.1	93.75																																																																																														Y2O3,BaCO3,CuO,K2CO3,RbOH.H2O,CsOH	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5332	JJP0330219		(Y,Sc)Ba2Cu3O7	Y0.95Sc0.05Ba2Cu3O6.63	Y	0.95	Sc	0.05	Ba	2	Cu	3													O	z	6.63	1	1994																											3	Y123			A	3.831	3.895	11.69												K	90.8		92.6			1.8	91.7																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5333	JJP0330219		(Y,Sc)Ba2Cu3O7	Y0.9Sc0.1Ba2Cu3O6.56	Y	0.9	Sc	0.1	Ba	2	Cu	3													O	z	6.56	1	1994																											3	Y123			A	3.833	3.896	11.687												K	89.9		92.9			3	91.4																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5334	JJP0330219		(Y,La)Ba2Cu3O7	Y0.95La0.05Ba2Cu3O6.58	Y	0.95	La	0.05	Ba	2	Cu	3													O	z	6.58	1	1994																											3	Y123			A	3.829	3.896	11.7												K	92.1		95.2			3.1	93.65																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5335	JJP0330219		(Y,La)Ba2Cu3O7	Y0.9La0.1Ba2Cu3O6.62	Y	0.9	La	0.1	Ba	2	Cu	3													O	z	6.62	1	1994																											3	Y123			A	3.834	3.896	11.69												K	90.7		94			3.3	92.35																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5336	JJP0330219		Y(Ba,Sc)2Cu3O7	Y1Ba1.9Sc0.1Cu3O6.55	Y	1	Ba	1.9	Sc	0.1	Cu	3													O	z	6.55	1	1994																											3	Y123			A	3.837	3.895	11.689												K	86.9		91			4.7	88.95																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5337	JJP0330219		Y(Ba,Sc)2Cu3O7	Y1Ba1.8Sc0.2Cu3O6.64	Y	1	Ba	1.8	Sc	0.2	Cu	3													O	z	6.64	1	1994																											3	Y123			A	3.827	3.893	11.681												K	87		90.6			3.6	88.8																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5338	JJP0330219		Y(Ba,Y)2Cu3O7	Y1.1Ba1.9Cu3O6.65	Y	1.1	Ba	1.9	Cu	3															O	z	6.65	1	1994																											3	Y123			A	3.831	3.892	11.68												K	90.3		92.2			1.9	91.25																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5339	JJP0330219		Y(Ba,Y)2Cu3O7	Y1.2Ba1.8Cu3O6.68	Y	1.2	Ba	1.8	Cu	3															O	z	6.68	1	1994																											3	Y123			A	3.83	3.894	11.696												K	89.6		95			5.4	92.3																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5340	JJP0330219		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O6.73	Y	1	Ba	1.9	La	0.1	Cu	3													O	z	6.73	1	1994																											3	Y123			A	3.836	3.888	11.668												K	90.4		95.3			4.9	92.85																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5341	JJP0330219		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O6.81	Y	1	Ba	1.8	La	0.2	Cu	3													O	z	6.81	1	1994																											3	Y123			A	3.826	3.887	11.661												K	87.4		96			8.6	91.7																																																																																														Y2O3,BaCO3,CuO,Sc2O3,La2O3	1	solid state reaction, for details see Jpn.J.Appl.Phys.31(1992)L392					Effects of Substitution by Group Ia and IIIa Elements on Superconducting Properties of YBa2Cu3Oy	199402			Jpn.J.Appl.Phys.Lett.,33 (1994) L219-222	Fumihiko Kimura,Katsuyuki Fujiwara,Yukichi Tatsumi	Y,Ba,Cu,O,K,Rb,Cs,Sc,La	
5342	JJP0330300	impurity phase=BaCuO2, unknown,amorphous, Ag site = disorder	(Ag,Cu)Ba2Ca3Cu4O11	Ag0.25Cu0.75Ba2Ca3Cu4O11-z	Ag	0.25	Cu	0.75	Ba	2	Ca	3	Cu	4											O	11-z			1994																											2	Ag1234	P4/mmm		A	7.727		36.222												K	116.4	117.1	117.6	117			117.1																																																																																															1	mixture of precursor(Ba-Ca-Cu-O) and AgO - pellet-seal in Au capsule-heat(1100C,1-3H under 5GPa) ANN(300C,5-10H in flowing O2)					New Hihg-Tc Superconductor Ag1-xCuxBa2Can-1CunO2n+3-z Family with Tc>117 K	199403			Jpn.J.Appl.Phys.Lett.,33 (1994) L300-303	Akira Negishi,HIdeo Ihara,Hirofumi Matuhata,Hirotomi Ozawa,Kazurasu Tokiwa,Msayuki Hirabayashi,Young Seok Song	Ag,Cu,Ba,Ca,O	
5343	JJP0330715	Hir defined as the peak of imaginary part of susceptibility during sweeping DC field	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1994																												Y123																		K		92					92																																		HIR5343																																																														MPMG method, final melt growth process was performed in the mixed gas of 1 %O2 and 99%Ar					Flux Pinning in Melt-Grown NdBa2Cu3Oy and SmBa2Cu3Oy Superconductors	199405			Jpn.J.Appl.Phys.Lett.,33(1994)L715-717	Jurgen Weltz,Masato Murakami,Naoki Koshizuka,Naomichi Sakai,Sang-Im Yoo,Shoji Tanaka,Takamitsu Higuchi	Nd,Ba,Cu,O,Sm	
5344	JJP0330715	Nd4Ba2Cu2O10 phase included	NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7			1994																												Y123																		K		94.5					94.5																																		HIR5344																																																														MPMG method, final melt growth process was performed in the mixed gas of 1 %O2 and 99%Ar					Flux Pinning in Melt-Grown NdBa2Cu3Oy and SmBa2Cu3Oy Superconductors	199405			Jpn.J.Appl.Phys.Lett.,33(1994)L715-717	Jurgen Weltz,Masato Murakami,Naoki Koshizuka,Naomichi Sakai,Sang-Im Yoo,Shoji Tanaka,Takamitsu Higuchi	Nd,Ba,Cu,O,Sm	
5345	PHC2280181	AC susceptibility measurement, BCS coherence = 150A	K3C60	C60K3	C	60	K	3																					1994																												fullerene																		K		17.8		17.8			17.8			K/GPa							44										T		17							T/K		1.4					A		44																																																										(C60+excess K or Rb)-seal in quartz ampoule-react(300C,5days) using two zone method-pelletize-ANN(35)c,5days)					Inter- and intragrain AC response of the granular superconductors K3C60 and Rb3C60	199407			Physica C, 228(1994)181-189	E.Straube,H.-J.Guntherodt,H.Werner,K.Luders,M.Baenitz,M.Heinze,R.Schlogl,V.Thommen	K,C,Rb	
5346	PHC2280181	single grain, BCS coherence = 50A	Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		29.5		29.5			29.5			K/GPa							29										T		44							T/K		2.3					A		27																																																										(C60+excess K or Rb)-seal in quartz ampoule-react(300C,5days) using two zone method-pelletize-ANN(35)c,5days)					Inter- and intragrain AC response of the granular superconductors K3C60 and Rb3C60	199407			Physica C, 228(1994)181-189	E.Straube,H.-J.Guntherodt,H.Werner,K.Luders,M.Baenitz,M.Heinze,R.Schlogl,V.Thommen	K,C,Rb	
5347	PHC2280175	BCS coherence = 44 A	Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		30					30																				T	analizing R(H) curve using fluctuation theory	62							T/K		3.28					A		24			A		3200																																																					high quality C60 single crystals were grown by vapor transport, Rb doping using similar method of Science 352(1992)1900					Magnetotransport in single-crystal Rb3C60	199407			Physica C, 228(1994)175-180	A.Zettl,J.G.Hou,Marvin L.Cohen,Vincent H.Crespi,X.-D.Xiang	Rb,C	
5348	PHC2330247	intercalated sample,24.6A for host c-axis	(Hg2Cl2)Bi2Sr2CuO8	Hg1.38Cl1.38Bi2.2Sr1.8Cu1Oz	Hg	1.38	Cl	1.38	Bi	2.2	Sr	1.8	Cu	1											O	z			1994																												Bi2201			A			27.8																																																																																																																			HgCl2  was intercalated into Bi2201,Bi2212, Bi2223 single phase of Bi22(n-1)n + HgCl2 in evacuated pyrex-heat(360C,4days)					Synthesis and superconductivity of 'Hg2Cl2'-intercalated Bi2Sr2Can-1CunOz(n=1-3) compounds	199411			Physica C.,233(1994) 247-252	K.Hiraga,M.Kikuchi,N.Kobayashi,N.Ohnishi,Y.Muraoka,Y.Syono	Hg,Cl,Bi,Sr,Ca,O,Cu	
5349	PHC2330247		(Hg2Cl2)Bi2Sr2CaCu2O8	Hg1.76Cl1.76Bi2Sr2Ca1Cu2Oz	Hg	1.76	Cl	1.76	Bi	2	Sr	2	Ca	1	Cu	2									O	z			1994																												Bi2212			A			34.3																																																																																																																								Synthesis and superconductivity of 'Hg2Cl2'-intercalated Bi2Sr2Can-1CunOz(n=1-3) compounds	199411			Physica C.,233(1994) 247-252	K.Hiraga,M.Kikuchi,N.Kobayashi,N.Ohnishi,Y.Muraoka,Y.Syono	Hg,Cl,Bi,Sr,Ca,O,Cu	
5350	PHC2330247		(Hg2Cl2)(Bi,Pb)2Sr2Ca2Cu3O10	Hg2.9Cl2.9Bi1.65Pb0.35Sr2Ca2Cu3Oz	Hg	2.9	Cl	2.9	Bi	1.65	Pb	0.35	Sr	2	Ca	2	Cu	3							O	z			1994																												Bi2223			A			40.8																																																																																																																								Synthesis and superconductivity of 'Hg2Cl2'-intercalated Bi2Sr2Can-1CunOz(n=1-3) compounds	199411			Physica C.,233(1994) 247-252	K.Hiraga,M.Kikuchi,N.Kobayashi,N.Ohnishi,Y.Muraoka,Y.Syono	Hg,Cl,Bi,Sr,Ca,O,Cu	
5351	PHC2330247		(Hg2Cl2)Bi2Sr2CaCu2O8	Hg1.46Cl1.46Bi2Sr2Ca1Cu2Oz	Hg	1.46	Cl	1.46	Bi	2	Sr	2	Ca	1	Cu	2									O	z			1994																																														K				86			86																																																																																																					Synthesis and superconductivity of 'Hg2Cl2'-intercalated Bi2Sr2Can-1CunOz(n=1-3) compounds	199411			Physica C.,233(1994) 247-252	K.Hiraga,M.Kikuchi,N.Kobayashi,N.Ohnishi,Y.Muraoka,Y.Syono	Hg,Cl,Bi,Sr,Ca,O,Cu	
5352	PHC2330327		(Bi,Pb)2Sr2Ca2Cu3O<z>F<x>	Bi1.6Pb0.4Sr2Ca2Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	z			1994																																														K	79		107				93																																																																																																					Effect of F doping in the (Bi,Pb)-Sr-Ca-Cu-O system	199411			Physica C.,233(1994) 327-331	P.-Y.Hu,R.-D.Wang,X.-G.Wang,X.-Z.Gao,Z.-M.Huang	Bi,Pb,Sr,Cu,Ca,O	
5354	PHC2330327		(Bi,Pb)2Sr2Ca2Cu3O<z>F<x>	Bi1.6Pb0.4Sr2Ca2Cu3F0.65Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3	F	0.65									O	z			1994																																														K	93		107				100																																																																																																					Effect of F doping in the (Bi,Pb)-Sr-Ca-Cu-O system	199411			Physica C.,233(1994) 327-331	P.-Y.Hu,R.-D.Wang,X.-G.Wang,X.-Z.Gao,Z.-M.Huang	Bi,Pb,Sr,Cu,Ca,O	
5355	PHC2330327		(Bi,Pb)2Sr2Ca2Cu3O<z>F<x>	Bi1.6Pb0.4Sr2Ca2Cu3F0.85Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3	F	0.85									O	z			1994																																														K	97		107				102																																																																																																					Effect of F doping in the (Bi,Pb)-Sr-Ca-Cu-O system	199411			Physica C.,233(1994) 327-331	P.-Y.Hu,R.-D.Wang,X.-G.Wang,X.-Z.Gao,Z.-M.Huang	Bi,Pb,Sr,Cu,Ca,O	
5356	PHC2330327		(Bi,Pb)2Sr2Ca2Cu3O<z>F<x>	Bi1.6Pb0.4Sr2Ca2Cu3F0.85Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3	F	0.85									O	z			1994																												Bi2223																		K	112		120				116																																																																																																					Effect of F doping in the (Bi,Pb)-Sr-Ca-Cu-O system	199411			Physica C.,233(1994) 327-331	P.-Y.Hu,R.-D.Wang,X.-G.Wang,X.-Z.Gao,Z.-M.Huang	Bi,Pb,Sr,Cu,Ca,O	
5357	NAT3450324			Li1Nb1O2	Li	1	Nb	1																	O	2			1990																											2				A	2.906		10.447												K					2					K/GPa																																																																																																		Superconductivity in the layered compound LixNbO2	5			Nature.345 (1990)324-325	Angelica M.Stacy,MargretJ.Geselbracht,Thomas J.Richardson	Li,Nb,O	
5358	NAT3450324			Li0.5Nb1O2	Li	0.5	Nb	1																	O	2			1990																											2	MoS2			A	2.919		10.453												K		5		5			5																																																																																																					Superconductivity in the layered compound LixNbO2	5			Nature.345 (1990)324-325	Angelica M.Stacy,MargretJ.Geselbracht,Thomas J.Richardson	Li,Nb,O	
5359	NAT3450324			Li0.45Nb1O2	Li	0.45	Nb	1																	O	2			1990									6																		2				A	2.9227		10.455												K		5.5		5.5			5.5			K/GPa							15																																																																																											Superconductivity in the layered compound LixNbO2	5			Nature.345 (1990)324-325	Angelica M.Stacy,MargretJ.Geselbracht,Thomas J.Richardson	Li,Nb,O	
5360	PHC2310021		HgBa2(Ca,Sr)2Cu3O8	Hg1Ba2CaSrCu3O8+z	Hg	1	Ba	2	Ca		Sr		Cu	3											O	8+z			1994																												Hg1223																		K		132					132																																		HIR5360																																																																			Critical currents and irreversibility lines in HgBa2(Ca1-xSrx)2Cu3O8+z and Hg0.5Tl0.5Ba2(Ca1-xSrx)2Cu3O8+z	199409			Physica C,231(1994) 21-25	J.C.Park,K.-H.Yoo,N.H.Hur,S.C.Yu,Y.K.Park,Y.Y.Song	Tl,Hg,Ca,Sr,Cu,O	
5361	PHC2310021		(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.5Tl0.5Ba2CaSrCu3O8+z	Hg	0.5	Tl	0.5	Ba	2	Ca		Sr		Cu	3									O	8+z			1994																												Hg1223																		K		132					132																																		HIR5361																																																																			Critical currents and irreversibility lines in HgBa2(Ca1-xSrx)2Cu3O8+z and Hg0.5Tl0.5Ba2(Ca1-xSrx)2Cu3O8+z	199409			Physica C,231(1994) 21-25	J.C.Park,K.-H.Yoo,N.H.Hur,S.C.Yu,Y.K.Park,Y.Y.Song	Tl,Hg,Ca,Sr,Cu,O	
5362	PHC2220233		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			1994																											2	Bi2212			A	5.392		30.854												K		66.5					66.5																																																																																												E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5363	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.9Gd0.1Ca1Cu2O8+z	Bi	2	Sr	1.9	Gd	0.1	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.396		30.715												K		76					76																																																																																																					Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5364	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.8Gd0.2Ca1Cu2O8+z	Bi	2	Sr	1.8	Gd	0.2	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.398		30.572												K		71.6					71.6																																																																																												E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5365	PHC2220233		Bi2(Sr.Gd)2CaCu2O8	Bi2Sr1.7Gd0.3Ca1Cu2O8+z	Bi	2	Sr	1.7	Gd	0.3	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.394		30.384												K		60.4					60.4																																																																																																					Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5366	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.6Gd0.4Ca1Cu2O8+z	Bi	2	Sr	1.6	Gd	0.4	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.394		30.329												K		50					50																																																																																												E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5367	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.5Gd0.5Ca1Cu2O8+z	Bi	2	Sr	1.5	Gd	0.5	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A															K		21.6					21.6																																																																																												E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5368	PHC2220233		Bi2(Sr.Gd)2CaCu2O8	Bi2Sr1.44Gd0.56Ca1Cu2O8+z	Bi	2	Sr	1.44	Gd	0.56	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.418		30.165												K		4					4																																																																																												E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5369	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.4Gd0.6Ca1Cu2O8+z	Bi	2	Sr	1.4	Gd	0.6	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.387		30.102												K					10																																																																																														E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5370	PHC2220233		Bi2(Sr,Gd)2CaCu2O8	Bi2Sr1.35Gd0.65Ca1Cu2O8+z	Bi	2	Sr	1.35	Gd	0.65	Ca	1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.391		29.997												K					10																																																																																														E+21/cm3									Study of Hall effect, electrical resistivity and magnetoresistance in Bi2Sr2-xGdxCa1Cu2O8+z(x=0.00-0.65) systems	199403			Physica C, 222(1994)233-240	D.C.Khan,Sandeep Singh	Bi,Sr,Gd,Ca,Cu,O	
5371	PHC2340361		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1994																											3	Y124			A	3.842	3.863	27.204												K		80.4		81.8			80.4																																																																																																					Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5372	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8		1	1994																											3	Y124			A	3.843	3.859	27.227												K		45.4			45		45.4																																																																																																					Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5373	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8		1	1994																											3	Y124			A	3.843	3.858	27.207												K		17		15.3			17																																																																																																					Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5374	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.88Ni0.12O8	Y	1	Ba	2	Cu	3.88	Ni	0.12													O	8		1	1994																											3	Y124			A	3.842	3.861	27.197												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5375	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.84Ni0.16O8	Y	1	Ba	2	Cu	3.84	Ni	0.16													O	8		1	1994																											3	Y124			A	3.845	3.858	27.178												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5376	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.8Ni0.2O8	Y	1	Ba	2	Cu	3.8	Ni	0.2													O	8			1994																											3	Y124			A	3.845	3.858	27.18												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5377	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.76Ni0.24O8	Y	1	Ba	2	Cu	3.76	Ni	0.24													O	8			1994																											3	Y124			A	3.844	3.86	27.159												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5378	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.68Ni0.32O8	Y	1	Ba	2	Cu	3.68	Ni	0.32													O	8			1994																											3	Y124			A	3.845	3.861	27.153												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5379	PHC2340361		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.6Ni0.4O8	Y	1	Ba	2	Cu	3.6	Ni	0.4													O	8			1994																											3	Y124			A	3.843	3.861	27.144												K					4.2																																																																																																							Effects of Ni substitution on the superconducting and Raman spectra in YBa2Cu4O8	199412			Physica C.,234(1994) 361-367	H.Yamauchi,N.Koshizuka,N.Seiji,N.Watanabe	Y,Ba,Cu,O	
5380	PHC2340269		YBa2Cu3O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	6.92	6.92		1994																											3	Y123																		K		92.4				0.14	92.4																				T	from specific heat measurement	212							T/K		3.2					A		12.4																																																															Specific heat up to 14 tesla of a YBa2Cu3O6.92 single crystal	199412			Physica C.,234(1994) 269-279	A.Junod,E.Janod,G.Triscone,J.-Y.Henry,K.-Q.Wang,R.Calemczuk	Y,Ba,Cu,O	
5381	PHC2340255		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.307	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z	6.307		1994																											2	Bi2201			A	5.38														K				27.6			27.6																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5382	PHC2340255		Bi2(Sr,Pr)2CuO6	Bi2Sr1.6Pr0.4Cu1O6.313	Bi	2	Sr	1.6	Pr	0.4	Cu	1													O	z	6.313		1994																											2	Bi2201			A	5.382														K				21.8			21.8																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5383	PHC2340255		Bi2(Sr,Nd)2CuO6	Bi2Sr1.6Nd0.4Cu1O6.32	Bi	2	Sr	1.6	Nd	0.4	Cu	1													O	z	6.32		1994																											2	Bi2201			A	5.382														K				23.1			23.1																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5384	PHC2340255		Bi2(Sr,Sm)2CuO6	Bi2Sr1.6Sm0.4Cu1O6.3	Bi	2	Sr	1.6	Sm	0.4	Cu	1													O	z	6.3		1994																											2	Bi2201			A	5.378														K				17			17																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5385	PHC2340255		Bi(Sr,Eu)2CuO6	Bi2Sr1.6Eu0.4Cu1O6.301	Bi	2	Sr	1.6	Eu	0.4	Cu	1													O	z	6.301		1994																											2	Bi2201			A	5.374														K				12.5			12.5																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5386	PHC2340255		Bi(Sr,Gd)2CuO6	Bi2Sr1.6Gd0.4Cu1O6.328	Bi	2	Sr	1.6	Gd	0.4	Cu	1													O	z	6.328		1994																											2	Bi2201			A	5.373														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5387	PHC2340255		Bi(Sr,Tb)2CuO6	Bi2Sr1.6Tb0.4Cu1O6.331	Bi	2	Sr	1.6	Tb	0.4	Cu	1													O	z	6.331		1994																											2	Bi2201			A	5.379														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5388	PHC2340255		Bi2(Sr,La)2CuO6	Bi2Sr1.3La0.7Cu1O6.422	Bi	2	Sr	1.3	La	0.7	Cu	1													O	z	6.422		1994																											2	Bi2201			A	5.414														K			22.6				22.6																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5389	PHC2340255		Bi2(Sr,Pr)2CuO6	Bi2Sr1.3Pr0.7Cu1O6.412	Bi	2	Sr	1.3	Pr	0.7	Cu	1													O	z	6.412		1994																											2	Bi2201			A	5.406														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5390	PHC2340255		Bi2(Sr,Nd)2CuO6	Bi2Sr1.3Nd0.7Cu1O6.417	Bi	2	Sr	1.3	Nd	0.7	Cu	1													O	z	6.417		1994																											2	Bi2201			A	5.403														K			14.2				14.2																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5391	PHC2340255		Bi2(Sr,Sm)2CuO6	Bi2Sr1.3Sm0.7Cu1O6.405	Bi	2	Sr	1.3	Sm	0.7	Cu	1													O	z	6.405		1994																											3	Bi2201			A	5.406														K				8			8																																																																																																					Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5392	PHC2340255		Bi2(Sr,Eu)2CuO6	Bi2Sr1.3Eu0.7Cu1O6.408	Bi	2	Sr	1.3	Eu	0.7	Cu	1													O	z	6.408		1994																											2	Bi2201			A	5.408														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5393	PHC2340255		Bi2(Sr,Gd)2CuO6	Bi2Sr1.3Gd0.7Cu1O6.402	Bi	2	Sr	1.3	Gd	0.7	Cu	1													O	z	6.402		1994																											2	Bi2201			A	5.407														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5394	PHC2340255		Bi2(Sr,Tb)2CuO6	Bi2Sr1.3Tb0.7Cu1O6.399	Bi	2	Sr	1.3	Tb	0.7	Cu	1													O	z	6.399		1994																											2	Bi2201			A	5.398														K					5																																																																																																							Effects of lanthanoid substitution on superconductivity and modulated structure of Bi2Sr2CuOy	199412			Physica C.,234(1994) 255-262	H.Nameki,M.Kikuchi,Y.Syono	Bi,Sr,Cu,O	
5395	PHC2340120			Al1Sr2Ca3Cu4Oz	Al	1	Sr	2	Ca	3	Cu	4													O	z			1994																												Al1234			A	3.839		17.72												K	108			110			110																																																																																																					A new series of high-Tc superconductors AlSr2Can-1CunO2n+3(n=4,Tc=110 K;n=5,Tc=83 K )prepared at high pressure	199412			Physica C,.234(1994) 120-126	E.Takayama-Muromachi,K.Kosuda,M.Isobe,T.Kawashima,Y.Matsui	Al,Sr,Cu,O.Ca	
5396	PHC2340120			Al1Sr2Ca5Cu5Oz	Al	1	Sr	2	Ca	5	Cu	5													O	z			1994																												Al1245			A	3.845		20.87												K	80			83			83																																																																																																					A new series of high-Tc superconductors AlSr2Can-1CunO2n+3(n=4,Tc=110 K;n=5,Tc=83 K )prepared at high pressure	199412			Physica C,.234(1994) 120-126	E.Takayama-Muromachi,K.Kosuda,M.Isobe,T.Kawashima,Y.Matsui	Al,Sr,Cu,O.Ca	
5397	NAT3690382	grain size is about 700A 	Sr2Cu(O2F2)	Sr2Cu1F2.6O2	Sr	2	Cu	1	F	2.6															O		2		1994																											3	T				5.394	5.513	13.468												K					4.2																																																																																																		Sr2CuO3-Ni furnacetube(10%F2+90%N2)-heat(21OC,15min)-cool in N2 or air after flushing all F2 from the system					Synthesis and superconducting properties of the strontium copper oxy-fluoride Sr2CuO2F2+z	6			Nature,369(1994) 382-384	C.Greaves,M.Al-Mamouri,M.Slaski,P.P.Edwards	Sr,Cu,O,F	
5398	NAT3690382		Sr2Cu(O2F2)	Sr2Cu1F2.33O2	Sr	2	Cu	1	F	2.33															O		2		1994																																														K		46		48			46										3.5																																																																																						Sr2CuO3-Ni furnacetube(10%F2+90%N2)-heat(21OC,15min)-cool in N2 or air after flushing all F2 from the system					Synthesis and superconducting properties of the strontium copper oxy-fluoride Sr2CuO2F2+z	6			Nature,369(1994) 382-384	C.Greaves,M.Al-Mamouri,M.Slaski,P.P.Edwards	Sr,Cu,O,F	
5399	NAT3690382	F-content depence of Tc is shown in Figure.	Sr2Cu(O2F2)	Sr2Cu1F2O2	Sr	2	Cu	1	F	2															O	2			1994																																																						TC5399																																																																																															Sr2CuO3-Ni furnacetube(10%F2+90%N2)-heat(21OC,15min)-cool in N2 or air after flushing all F2 from the system					Synthesis and superconducting properties of the strontium copper oxy-fluoride Sr2CuO2F2+z	6			Nature,369(1994) 382-384	C.Greaves,M.Al-Mamouri,M.Slaski,P.P.Edwards	Sr,Cu,O,F	
5400	APJ0332515		Pb2Sr2(Ho,Ca)(Cu,Al)3O8	Pb2Sr2Ho0.05Ca0.5Cu2.994Al0.006O8	Pb	2	Sr	2	Ho	0.05	Ca	0.5	Cu	2.994	Al	0.006									O		8		1994																												Pb3212																		K		76.4					76.4																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5401	APJ0332515		Pb2SR2(Ho,Ca)(Cu,Al)3O8	Pb2Sr2Ho0.5Ca0.5Cu2.982Al0.018O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	2.982	Al	0.018									O		8		1994																												Pb3212																		K		63.6					63.6																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5402	APJ0332515		Pb2Sr2(Ho,Ca)(Cu,Al)3O8	Pb2Sr2Ho0.5Ca0.5Cu2.97Al0.03O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	2.97	Al	0.03									O		8		1994																												Pb3212																		K		59.1					59.1																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5403	APJ0332515		Pb2Sr2(Ho,Ca)(Cu,Al)3O8	Pb2Sr2Ho0.5Ca0.5Cu2.94Al0.06O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	2.94	Al	0.06									O		8		1994																												Pb3212																		K		51.8					51.8																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5404	APJ0332515	Tc is independent of Pt-doping	Pb2Sr2(Ho,Ca)(Cu,Pt)3O8	Pb2Sr2Ho0.5Ca0.5Cu2.94Pt0.06O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	2.94	Pt	0.06									O		8		1994																												Pb3212																		K			80.4				80.4																																																																																														SrCO3,Ho2O3,CaCO3,CuO,PbO,NaCl	5	Pb:Sr:Ho:Ca:Cu:NaCl=7:1.5:0.3:1:4:17, 1050C in Pt crucible, PbO,NaCl as a flux					Growth,Superconductivity and Anisotropy in the Electrical Resistivity of Pb2Sr2Ho0.5Ca0.5Cu3O8 Single Crystals:The Effect of Contamination from theCrucible on Tc	5			Jpn.J.Appl.Phys.,33(1994)2515-2520	Akihiko Fujiwara,Kunihiro Ohtsubo,Masatsune Kato,Shunsuke Shiga,Takashi Noji,Yoji Koike,Yoshitami saito	Pb,Sr,Ho, Ca,Cu,O	
5405	NAT3710139	impurity phane=CaCl2 Ca(OH)2 H2O,CuO insulator	Ca2CuO2Cl2	Ca2Cu1Cl2O2	Ca	2	Cu	1	Cl	2															O		2		1994																																3.864		15.049																																																																																																																			mixture of (Ca2CuO2Cl2+NaClO4+CuO)in dry box-heat(1173K,30min under 6 G Pa)					Probable hole-doped superconductivity without apical oxygens in (Ca,Na)2CuO2Cl2	10			Nature.371(1994) 139-141	M.Takano,N.Kobayashi,Z.Hiroi	Ca,Na,Cu,O,Cl	
5406	NAT3710139		(Ca,Na)2CuO2Cl2	Ca1.883Cu0.941Cl1.941Na0.059O2.117	Ca	1.883	Cu	0.941	Cl	1.941	Na	0.059													O		2.117		1994																																3.855		15.096												K		26		26			26																																																																																																mixture of (Ca2CuO2Cl2+NaClO4+CuO)in dry box-heat(1173K,30min under 6 G Pa)					Probable hole-doped superconductivity without apical oxygens in (Ca,Na)2CuO2Cl2	10			Nature.371(1994) 139-141	M.Takano,N.Kobayashi,Z.Hiroi	Ca,Na,Cu,O,Cl	
5407	NAT3710139		(Ca,Na)2CuO2Cl2	Ca1.808Cu0.904Cl1.904Na0.096O2.192	Ca	1.808	Cu	0.904	Cl	1.904	Na	0.096													O		2.192		1994																																3.852		15.121												K				26			26																																																																																																mixture of (Ca2CuO2Cl2+NaClO4+CuO)in dry box-heat(1173K,30min under 6 G Pa)					Probable hole-doped superconductivity without apical oxygens in (Ca,Na)2CuO2Cl2	10			Nature.371(1994) 139-141	M.Takano,N.Kobayashi,Z.Hiroi	Ca,Na,Cu,O,Cl	
5408	NAT3710139		(Ca,Na)2CuO2Cl2	Ca1.737Cu0.868Cl1.868Na0.132O2.263	Ca	1.737	Cu	0.868	Cl	1.868	Na	0.132													O		2.263		1994																																3.849		15.143												K				21			21																																																																																																mixture of (Ca2CuO2Cl2+NaClO4+CuO)in dry box-heat(1173K,30min under 6 G Pa)					Probable hole-doped superconductivity without apical oxygens in (Ca,Na)2CuO2Cl2	10			Nature.371(1994) 139-141	M.Takano,N.Kobayashi,Z.Hiroi	Ca,Na,Cu,O,Cl	
5409	NAT3710139		(Ca,Na)2CuO2Cl2	Ca1.702Cu0.851Cl1.851Na0.149O2.404	Ca	1.702	Cu	0.851	Cl	1.851	Na	0.149													O		2.404		1994																																3.844	15.13													K				15			15																																																																																																mixture of (Ca2CuO2Cl2+NaClO4+CuO)in dry box-heat(1173K,30min under 6 G Pa)					Probable hole-doped superconductivity without apical oxygens in (Ca,Na)2CuO2Cl2	10			Nature.371(1994) 139-141	M.Takano,N.Kobayashi,Z.Hiroi	Ca,Na,Cu,O,Cl	
5410	PHC2340001	Hall const n     by van der Pa   method maybeunderdoped sample,OHV=Hall angle.	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z		3	1994																												Hg1223																		K	130		134				132																																				A			16	1																										micro.V/K	5.4			TP5410	m.ohm.cm												0.35							7				HgO,BaO,CaO,CuO		Hg:Ba:Ca:Cu=1:2:2:3,pellet+pellet(=0:2:2:3)are placed in evacuated tube-heat(800C,10H)-slow cool to RT					Transport properties of single-crystal HgBa2Ca2Cu3O8+z	199412			Physica C.,234(1994) 1-9	A.Bertinotti,A.Carrington,C.Ayache,D.Colson,J.F.Marucco,Y.Dumont	Hg,Ba,Ca,Cu,O	
5411	PHC2340001	Hall coust nea       by van der Pa   method maybe under doped sample,OHV=Hall angle	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																												Hg1223																		K	123		125				124																																																																		micro.V/K	9.2			TP5411	m.ohm.cm												0.35											HgO,BaO,CaO,CuO		Hg:Ba:Ca:Cu=1:2:2:3,pellet+pellet(=0:2:2:3)are placed in evacuated tube-heat(800C,10H)-slow cool to RT					Transport properties of single-crystal HgBa2Ca2Cu3O8+z	199412			Physica C.,234(1994) 1-9	A.Bertinotti,A.Carrington,C.Ayache,D.Colson,J.F.Marucco,Y.Dumont	Hg,Ba,Ca,Cu,O	
5412	PHC2340019	imp rity pheses=CaHgO2,BaCuO2	(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.75Tl0.25Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.75	Tl	0.25	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z		1	1994																											2	Hg1223			A	3.873		16.006												K				128			128																																																																																														HgO,Tl2O3,Ba2CuO3,Ca0.86 Sr0.14 CuO2		mixture of vaw materials-pellet- lanced in a alumin a tube in evacuateel qwartg-heat(88C,6H)-SIN(880C,10H)-slow cool-ANN(400C,10H in O2)					New members in the family of Hg and Tl based superconductors Hg1-xTlxBa2(Ca0.86Sr0.14)2Cu3O8+z	199412			Physica C.,234(1994) 19-23	Jong C.Park,Kyu W.Lee,Kyung H.Yoo,Nae H.Kim,Nam H.Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
5413	PHC2340019		(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.5Tl0.5Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.5	Tl	0.5	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z		1	1994																											2	Hg1223				3.865		15.957												K				124			124																																																																																														HgO,Tl2O3,Ba2CuO3,Ca0.86 Sr0.14 CuO2		mixture of vaw materials-pellet- lanced in a alumin a tube in evacuateel qwartg-heat(88C,6H)-SIN(880C,10H)-slow cool-ANN(400C,10H in O2)					New members in the family of Hg and Tl based superconductors Hg1-xTlxBa2(Ca0.86Sr0.14)2Cu3O8+z	199412			Physica C.,234(1994) 19-23	Jong C.Park,Kyu W.Lee,Kyung H.Yoo,Nae H.Kim,Nam H.Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
5414	PHC2340019		(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.25Tl0.75Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.25	Tl	0.75	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z		1	1994																											2	Hg1223			A	3.863		15.869												K				122			122										90																																																																																				HgO,Tl2O3,Ba2CuO3,Ca0.86 Sr0.14 CuO2		mixture of vaw materials-pellet- lanced in a alumin a tube in evacuateel qwartg-heat(88C,6H)-SIN(880C,10H)-slow cool-ANN(400C,10H in O2)					New members in the family of Hg and Tl based superconductors Hg1-xTlxBa2(Ca0.86Sr0.14)2Cu3O8+z	199412			Physica C.,234(1994) 19-23	Jong C.Park,Kyu W.Lee,Kyung H.Yoo,Nae H.Kim,Nam H.Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
5415	PHC2340019		(Hg,Tl)Ba2(Ca,Sr)2Cu3O2	Hg0.75Tl0.25Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.75	Tl	0.25	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z		1	1994																											2	Hg1223																		K						132																																																																																																	sample #( )-ANN(400C,10H in Ar)					New members in the family of Hg and Tl based superconductors Hg1-xTlxBa2(Ca0.86Sr0.14)2Cu3O8+z	199412			Physica C.,234(1994) 19-23	Jong C.Park,Kyu W.Lee,Kyung H.Yoo,Nae H.Kim,Nam H.Hur,Yong K.Park	Hg,Tl,Ba,Ca,Sr,Cu,O	
5416	PHC2340024		(Tl,Hg)2Ba2Ca2Cu3O10	Tl2HgBa2Ca2Cu3O10-Z	Tl	2	Hg		Ba	2	Ca	2	Cu	3											O	10-Z			1994																											2	Tl2223			A	3.849		35.662												K	115		122				118.5																																																																																														Ba(NO3)2,Ca(NO3)2 4H2O,Cu(NO3)2 3H2O		prearor(Ba2Ca2Cu3O7)was prepered from solut on of metal nitrate,powder of preansor+HgO+Tl2O3-heat(860-870C,5H in vacuumquarty tube)					Stabilization of the Tl2Ba2Ca2Cu3O10 superconductor by Hg doping	199412			Physica C.,234(1994) 24-28	A.Zettl,C.S.Lee,Y.X.Jia	Hg,Tl,Ba,Ca,Cu,O	
5417	PHC2340024		(Tl,Hg)2Ba2Ca2Cu3O10	Tl1.7Hg0.3Ba2Ca2Cu3O10-z	Tl	1.7	Hg	0.3	Ba	2	Ca	2	Cu	3											O	10-z			1994																											2	Tl2223			A	3.846		35.74												K	122.1		125.9				124																																																																																														Ba(NO3)2,Ca(NO3)2 4H2O,Cu(NO3)2 3H2O		prearor(Ba2Ca2Cu3O7)was prepered from solut on of metal nitrate,powder of preansor+HgO+Tl2O3-heat(860-870C,5H in vacuumquarty tube)					Stabilization of the Tl2Ba2Ca2Cu3O10 superconductor by Hg doping	199412			Physica C.,234(1994) 24-28	A.Zettl,C.S.Lee,Y.X.Jia	Hg,Tl,Ba,Ca,Cu,O	
5418	PHC2340024		(Tl,Hg)2Ba2Ca2Cu3O10	Tl1.6Hg0.4Ba2Ca2Cu3O10-z	Tl	1.6	Hg	0.4	Ba	2	Ca	2	Cu	3											O	10-z			1994																											2	Tl2223			A	3.843		35.754												K	125.9		129.9	127			127										89																																																																																				Ba(NO3)2,Ca(NO3)2 4H2O,Cu(NO3)2 3H2O		prearor(Ba2Ca2Cu3O7)was prepered from solut on of metal nitrate,powder of preansor+HgO+Tl2O3-heat(860-870C,5H in vacuumquarty tube)					Stabilization of the Tl2Ba2Ca2Cu3O10 superconductor by Hg doping	199412			Physica C.,234(1994) 24-28	A.Zettl,C.S.Lee,Y.X.Jia	Hg,Tl,Ba,Ca,Cu,O	
5419	PHC2340024		(Tl,Hg)2Ba2Ca2Cu3O10/	Tl1.4Hg0.6Ba2Ca2Cu3O10-z	Tl	1.4	Hg	0.6	Ba	2	Ca	2	Cu	3											O	10-z			1994																											2	Tl2223			A	3.841		35.816												K	122.1		124.9				123.5																																																																																														Ba(NO3)2,Ca(NO3)2 4H2O,Cu(NO3)2 3H2O		prearor(Ba2Ca2Cu3O7)was prepered from solut on of metal nitrate,powder of preansor+HgO+Tl2O3-heat(860-870C,5H in vacuumquarty tube)					Stabilization of the Tl2Ba2Ca2Cu3O10 superconductor by Hg doping	199412			Physica C.,234(1994) 24-28	A.Zettl,C.S.Lee,Y.X.Jia	Hg,Tl,Ba,Ca,Cu,O	
5420	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.15O6.7	Y	1	Ba	2	Cu	3	F	0.15													O		6.7		1994																																														K				89.5			89.5																																																																																																					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
5421	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.25O6.7	Y	1	Ba	2	Cu	3	F	0.25													O		6.7		1994																																														K				91			91																																																																																																					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
5422	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.29O6.7	Y	1	Ba	2	Cu	3	F	0.29													O		6.7		1994																																														K				91			91																																																																																																					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
5423	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.38O6.7	Y	1	Ba	2	Cu	3	F	0.38													O		6.7		1994																																														K				91			91																																																																																																					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
5424	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F1.5O6	Y	1	Ba	2	Cu	3	F	1.5													O		6		1994																																																																																																																																																										NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
5425	PR05000496	Authors say sample is Bi2201. compositions determined by EDX. 	Bi2Sr2Cu1Ox	Bi2Sr1.9Cu2.1Ox	Bi	2	Sr	1.9	Cu	2.1															O	x		3	1994																																														K			5.3	7.5			7.5																																																																							mic.ohm.cm												267		m3/C	0.000000001				5		/cm3									Anisotropic resistivity of Bi2Sr2CuO crystals	199407		National laboratory Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, China	Phys.Rev.B,50(1994)496	F. Wu,J.Q. Li,J.W. Li,J.W. Xiong,W.J. Zhu,X.H. Hou,Y.Z. Huang,Z.X. Zhao		
5426	PR05000462		ErBa2Cu3O7-y	Er1Ba2Cu3O7-y	Er	1	Ba	2	Cu	3															O	7-y		1	1994																											3	Y123			A	3.82	3.89	11.63												K	92.5		94.1	90.5			90.5																																																											440	See Physeca C 165,29(1990).																																									Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5427	PR05000462		ErBa2(Cu,Ni)3O7-y	Er1Ba2Cu2.85Ni0.15O7-y	Er	1	Ba	2	Cu	2.85	Ni	0.15													O	7-y		1	1994																											3				A	3.82	3.89	11.62												K	89.1		92.2	89.5			89.5																																																																																																					Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5428	PR05000462		ErBa2(Cu,Zn)3O7-y	Er1Ba2Cu2.85Zn0.15O7-y	Er	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1994																											3				A	3.82	0.89	11.63												K	86.2		87.7	86			86																																																																																																					Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5429	PR05000462		ErBa2(Cu,Fe)3O7-y	Er1Ba2Cu2.85Fe0.15O7-y	Er	1	Ba	2	Cu	2.85	Fe	0.15													O	7-y		1	1994																											3				A	3.83	3.86	11.64												K	88.5		88.5	90			90																																																																																																					Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5430	PR05000462		ErBa2(Cu,Co)3O7-y	Er1Ba2Cu2.85Co0.15O7-y	Er	1	Ba	2	Cu	2.85	Co	0.15													O	7-y		1	1994																											3				A	3.83	3.87	11.63												K	89.9		91.8	88.5			88.5																																																																																																					Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5431	PR05000462		ErBa2(Cu,Ga)3O7-y	Er1Ba2Cu2.85Ga0.15O7-y	Er	1	Ba	2	Cu	2.85	Ga	0.15													O	7-y		1	1994																											3				A	3.84	3.86	11.64												K	89.5		90.9	89.6			89.6																																																																																																					Resistivity, magnetic-susceptibility, and specific-heat studies of ErBa2(Cu(1-x)Mx)3O7-y [(M=Ni,Zn,Fe,Co, and Ga) and x =0.005]: The effect of site-dependent substitutional disorder	199407		National Physical laboratory, New Delhi 110012, India	Phys.Rev.B,50(1994)462	A.K. Bandyopadhyay,A.V. Narlikar,Deepak Varandani,E. Gmelin		
5432	PHC2430389	demagnetization factor between0.7and0,95	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1995																												Bi2212																		K		85					85			K/GPa								Oe	first penetration field		220						kT																A					A			2200																																																				crystal was grown from the melt by modified Bridgman-stockbarger tacknique,Before measurements homoginized by ANN(8%O2+92%Ar,800C,1week)					Flux penetration in Bi(2212) single crystals at low magnetic fields	199503		Institut fur Experimentalphysik IV, Ruhr-Universitat Bochum,D-44780 Bochum,Germany	Physica C.,243(1995)389-396	B.vom Hedt,K.Westerholt	Bi,Sr,Ca,Cu,O	
5433	PHC2430001	Cu-valence=2.28	HgBa2CuO4	Hg1Ba2Cu1O4.14	Hg	1	Ba	2	Cu	1															O	4+Z	4.14	1	1995																											2	Hg1201			A	3.871		9.497												K																																																																																																							Precusor(Ba2CuOz) was prepared by mixing nitrates,+HgO-heat to 920C(P=18kbar)in Au capsule					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5434	PHC2430001		HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1995																											2	Hg1201			A	3.875		9.5												K				59			59																																																																																																Precusor(Ba2CuOz) was prepared by mixing nitrates,+HgO-heat to 920C(P=18kbar)in Au capsule					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5435	PHC2430001		HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1995																											2	Hg1201			A	3.878		9.51												K				87			87																																																																																																Precusor(Ba2CuOz) was prepared by mixing nitrates,+HgO-heat to 920C(P=18kbar)in Au capsule					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5436	PHC2430001	precursor(800C,10H in O2)Cu-valence=2.20	HgBa2CuO4	Hg1Ba2Cu1O4.1	Hg	1	Ba	2	Cu	1															O	4+z	4.1	1	1995																											2	Hg1201			A	3.874		9.5												K				35			35																																																																																																Precusor(Ba2CuOz) was prepared by mixing nitrates,+HgO-heat to 920C(P=18kbar)in Au capsule					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5437	PHC2430001	Cu-valence=2.18	HgBa2CuO4+z	Hg1Ba2Cu1O4.09	Hg	1	Ba	2	Cu	1															O	4+z	4.09	1	1995																											2	Hg1201			A	3.874		9.507												K				36			36																																																																																																Prearsor was heat-treated(800C,20H in O2)-heat(300C,15H in O2)-					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5438	PHC2430001	Cu-valence=2.13	HgBa2CuO4+z	Hg1Ba2Cu1O4.07	Hg	1	Ba	2	Cu	1															O	4+z	4.07	1	1995																											2	Hg1201			A	3.88		9.512												K				91			91																																																																																																Prearsor was heat-treated(800C,20H in O2)-heat(300C,15H in O2)-					Suppression of superconductivity and the overdoped region in HgBa2CuO4+z	199502		Laboratoire de Cristallographie,CNRS-UJF BP 166,38042 Grenoble Cedex 09,France	Physica C.,243(1995)1-9	A.Santoro,B.Souletie,E.T.Alexandre,E.V.Antipov,J.J.Capponi,J.L.Tholence,M.Marezio,Q.Huang,S.M.Loureiro,S.de.Brion	Hg,Ba,Cu,O	
5439	PHC2430019	post anneal (200C,6H in flowing O2), grain oriented sample	HgBa2CuO4	Hg1Ba2Cu1O4.117	Hg	1	Ba	2	Cu	1															O	4+z	4.117		1995																											2	Hg1201			A			9.516												K				82			82												Hc1 at 40K	124							kT														HIR5439		A																																																										HgO,BaO,CuO		(Hg:Ba:Cu=1:2:1)-sealed in quartz tube (P=2E-4 Torr)-heat(750C,1H)-Q to water					The oxygen-content dependence of the magnetization anisotropy of HgBaCuO4+z	199502		Superconductivity Research Laboratory,ISTEC,10-13 Shinome,1-chome,Tokyo 135,Japan	Physica C.,243(1995)19-23	A.Fukuoka,H.Kubota,H.Yamauchi,R.Usami	Hg,Ba,Cu,O	
5440	PHC2430019		HgBa2CuO4	Hg1Ba2Cu1O4.09	Hg	1	Ba	2	Cu	1															O	4+Z	4.09		1995																											2	Hg1201						9.511												K				96			96																																																																																														HgO,BaO,CuO		(Hg:Ba:Cu=1:2:1)-sealed in quartz tube (P=2E-4 Torr)-heat(750C,1H)-Q to water					The oxygen-content dependence of the magnetization anisotropy of HgBaCuO4+z	199502		Superconductivity Research Laboratory,ISTEC,10-13 Shinome,1-chome,Tokyo 135,Japan	Physica C.,243(1995)19-23	A.Fukuoka,H.Kubota,H.Yamauchi,R.Usami	Hg,Ba,Cu,O	
5441	PHC2430019	post anneale(400C,6H in flowing Ar), grain oriented sample	HgBa2CuO4	Hg1Ba2Cu1O4.043	Hg	1	Ba	2	Cu	1															O	4+z	4.043		1995																											2	Hg1201			A			9.516												K				87			87												Hc1 at 40K	80																					HIR5441																																																												HgO,BaO,CuO		(Hg:Ba:Cu=1:2:1)-sealed in quartz tube (P=2E-4 Torr)-heat(750C,1H)-Q to water					The oxygen-content dependence of the magnetization anisotropy of HgBaCuO4+z	199502		Superconductivity Research Laboratory,ISTEC,10-13 Shinome,1-chome,Tokyo 135,Japan	Physica C.,243(1995)19-23	A.Fukuoka,H.Kubota,H.Yamauchi,R.Usami	Hg,Ba,Cu,O	
5442	PHC2430134	void free somple,sound velocity = 2909 m/s for shear velocity	ErBa2Cu3O7	Er1Ba2Cu3O6.92	Er	1	Ba	2	Cu	3															O	7-Z	6.92	1	1995									7.12						GPa		52.4						m/s		5509		3	Y123			A	3.821	3.888	11.669												K		90					90																																																											480	calculated from sound velocity																																		Er2O3,BaCO3,CuO		mixture-heat(930C,24H)-press in to pellett-heat(930C,24(+)in air)					Ultrasonic velocity studies on superconducting and non-superconducting ErBa2Cu3O7-z	199502		Department of Physics,Universiti Kebangsaan Malaysia,43600 Bangi,Selangor Darul Ehsan,Malaysia	Physica C.,243(1995)134-138	M.Yahya,R.Abd-Shukor,S.S.Lee	Er,Ba,Cu,O	
5443	PHC2430134	Q from 930C. void-free sample Q from semicon-like		Er1Ba2Cu3O6.25	Er	1	Ba	2	Cu	3															O	7-Z	6.25	1	1995									6.94						GPa		46.1										2	Y123			A	3.854		11.792												K					80																																																																																																Er2O3,BaCO3,CuO		mixture-heat(930C,24H)-press in to pellett-heat(930C,24(+)in air)					Ultrasonic velocity studies on superconducting and non-superconducting ErBa2Cu3O7-z	199502		Department of Physics,Universiti Kebangsaan Malaysia,43600 Bangi,Selangor Darul Ehsan,Malaysia	Physica C.,243(1995)134-138	M.Yahya,R.Abd-Shukor,S.S.Lee	Er,Ba,Cu,O	
5444	PHC2430160		(Y,Ca)Ba2(Cu,Ni)3O7	Y1CaBa2Cu3NiO6.89	Y	1	Ca		Ba	2	Cu	3	Ni												O	7-z	6.89	1	1995																											3	Y123			A	3.825	3.879	11.683												K	92			91			91																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5445	PHC2430160		(Y,Ca)Ba2(Cu,Ni)3O7	Y0.95Ca0.05Ba2Cu2.95Ni0.05O6.83	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Ni	0.05											O	7-z	6.83	1	1995																											3	Y123			A	3.827	3.896	11.669												K	78			82			82																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5446	PHC2430160		(Y,Ca)Ba2(Cu,Ni)3O7	Y0.9Ca0.1Ba2Cu2.9Ni0.1O6.86	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Ni	0.1											O	7-z	6.86	1	1995																											3	Y123			A	3.829	3.88	11.682												K	69			74			74																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5447	PHC2430160		(Y,Ca)Ba2(Cu,Ni)3O7	Y0.85Ca0.15Ba2Cu2.85Ni0.15O6.85	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Ni	0.15											O	7-z	6.85	1	1995																											3	Y123			A	3.823	3.885	11.671												K	63			67			67																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5448	PHC2430160		(Y,Ca)Ba2(Cu,Ni)3O7	Y0.8Ca0.2Ba2Cu2.8Ni0.2O6.77	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Ni	0.2											O	7-Z	6.77		1995																											3	Y123			A	3.825	3.872	11.663												K	59			64			64																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5449	PHC2430160	in homogeneous	(Y,Ca)Ba2(Cu,Ni)3O7	Y0.75Ca0.25Ba2Cu2.75Ni0.25O6.77	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Ni	0.25											O	7-Z	6.77		1995																											3	Y123			A	3.829	3.891	11.65												K	62			62			62																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5450	PHC2430160	in homogeneous	(Y,Ca)Ba2(Cu,Ni)3O7	Y0.7Ca0.3Ba2Cu2.7Ni0.3O7-z	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Ni	0.3											O	7-z			1995																											3	Y123																		K	64			65			65																																																																																														Y2O3,Ba(NO3)2,CaCO3,CuO,NiO,ZnO		mixture-heat(1190-1210K,24H in air)-SIN(1200-1225K,48H)-cool to 450K(1K/min)-FC					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5451	PHC2430214		(Hg,V)Ba2CuO4	Hg0.8V0.2Ba2Cu1O4.3	Hg	0.8	V	0.2	Ba	2	Cu	1													O	4+z	4.3		1995																											2	Hg1201			A	3.886		9.339												K				90			90																																		HIR5451																100000																																												HgO,V2O5,BaO,CuO,CaO		mix(in dry box)-Alumina crucible sealed in quartg tube(vacwum)-heat(800C at 100C/H)-keep(800C,12H)-cool to RT(50C/H)					New superconducting vanadomercury cuorates Hg0.8V0.2Ba2Cam-1CumO2m+2+z	199503		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen Cedex,France	Physica C.,243(1995)214-221	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu	Hg,V,Ba,Ca,Cu,O	
5452	PHC2430214		(Hg,V)Ba2CaCu2O6	Hg0.8V0.2Ba2Ca1Cu2O6.3	Hg	0.8	V	0.2	Ba	2	Ca	1	Cu	2											O	6+z	6.3		1995																											2	Hg1212			A	3.869		12.5												K				115			115																																		HIR5452																1000000																																												HgO,V2O5,BaO,CuO,CaO		mix(in dry box)-Alumina crucible sealed in quartg tube(vacwum)-heat(800C at 100C/H)-keep(800C,12H)-cool to RT(50C/H)					New superconducting vanadomercury cuorates Hg0.8V0.2Ba2Cam-1CumO2m+2+z	199503		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen Cedex,France	Physica C.,243(1995)214-221	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu	Hg,V,Ba,Ca,Cu,O	
5453	PHC2430214	ANN in flowing Oz.	(Hg,V)Ba2CaCu2O6	Hg0.8V0.2Ba2Ca1Cu2O6.3	Hg	0.8	V	0.2	Ba	2	Ca	1	Cu	2											O	6+z	6.3		1995																											2	Hg1212																		K				125			125																																																																																														HgO,V2O5,BaO,CuO,CaO		mix(in dry box)-Alumina crucible sealed in quartg tube(vacwum)-heat(800C at 100C/H)-keep(800C,12H)-cool to RT(50C/H)					New superconducting vanadomercury cuorates Hg0.8V0.2Ba2Cam-1CumO2m+2+z	199503		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen Cedex,France	Physica C.,243(1995)214-221	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu	Hg,V,Ba,Ca,Cu,O	
5454	PHC2430160		(Y,Ca)Ba2(Cu,Zn)3O7	Y0.95Ca0.05Ba2Cu2.95Zn0.05O6.89	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Zn	0.05											O	7-z	6.89		1995																											3	Y123			A	3.819	3.876	11.658												K	62			65			65																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5455	PHC2430160		(Y,Ca)Ba2(Cu,Zn)3O7	Y0.9Ca0.1Ba2Cu2.9Zn0.1O6.81	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Zn	0.1											O	7-z	6.81		1995																											3	Y123			A	3.814	3.885	11.661												K	47			50			50																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5456	PHC2430160		(Y,Ca)Ba2(Cu,Zn)3O7	Y0.85Ca0.15Ba2Cu2.85Zn0.15O6.85	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Zn	0.15											O	7-Z	6.85		1995																											3	Y123			A	3.816	3.879	11.666												K	42			43			43																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5457	PHC2430160		(Y,Ca)Ba2(Cu,Zn)3O7	Y0.8Ca0.2Ba2Cu2.8Zn0.2O6.73	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Zn	0.2											O	7-Z	6.73		1995																											3	Y123			A	3.824	3.875	11.674												K	41			43			43																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5458	PHC2430160		(Y,Ca)Ba2(Cu,Zn)3O7	Y0.75Ca0.25Ba2Cu2.75Zn0.25O6.76	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Zn	0.25											O	7-Z	6.76		1995																											3	Y123			A	3.82	3.868	11.67												K	40			42			42																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5459	PHC2430160	winor amount of impusity p  ase.	(Y,Ca)Ba2(Cu,Zn)3O7	Y0.7Ca0.3Ba1Cu2.7Zn0.3O7-z	Y	0.7	Ca	0.3	Ba	1	Cu	2.7	Zn	0.3											O	7-z			1995																											3	Y123																		K	43			45			45																																																																																																					Superconducting behaviour of co-doped Y1-xCaxBa2Cu3-xMxO7-z(M=Ni or Zn and 0.0 x 0.30)	199502		Chemistry Division,Bhabha Atomic Research Centre,Bombay 400 085,India	Physica C.,243(1995)160-166	J.V.Yakhmi,R.A.Gunasekaran,R.Ganguly	Yi,Ca,Ba,Cu,O,Ni,Zn	
5460	PR05004051		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95		1994																												Y123																																																													A					A	surface impedace	1400																																																					flux growth technique					Comparison of the influence of Ni and Zn impurities on the electromagnetic properties of YBa2Cu3O6.95	199408			Phys.Rev.B, 50(1994)4051	D.A.Bonn,D.J.Baar,E.Klein,Kuan Zhang,Ruixing Liang,S.Kamal,W.N.Hardy	Y,Ba,Cu,O,Zn,Ni	
5461	PHC2460001	[Hg1201]n(Sr2CuO2CO3)m	(Hg,Mo)Sr4Cu2(CO3)O6	Hg0.5Mo0.5Sr4Cu2C1O9+z	Hg	0.5	Mo	0.5	Sr	4	Cu	2	C	1											O	9+z			1995																											2	Hg1201		123	A	3.845		16.317												K				74			74			K/GPa							35																																																																																				SrCO3,Cr2O3,MoO3,CuO,HgO		mixtube-pellet-sealed in evacuated tube-heat(880C,12H)-Q to RT					Two transition-metal-substituted superconducting mercury-based oxycarbonates,Hg1-xMxSr4Cu2(CO3)O6+z(M=Cr and Mo)	199504		Laboratoire CRISMAT-CNRS URA 1318,ISMRA et Universite de Caen,Boulevard du Marechal Juin,14050 Caen cedex,France	Physica C.,246(1995)1-10	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo		
5462	PHC2460001	[Hg1201]n(Sr2CuO2CO3)m	(Hg,Cr)Sr4Cu2(CO3)O6	Hg0.4Cr0.6Sr4Cu2C1O9+z	Hg	0.4	Cr	0.6	Sr	4	Cu	2	C	1											O	9+z			1995																											2	Hg1201	P4/mmm	123	A	3.875		16.155												K				37			37			K/GPa							60																																																																																				SrCO3,Cr2O3,MoO3,CuO,HgO		mixtube-pellet-sealed in evacuated tube-heat(880C,12H)-Q to RT					Two transition-metal-substituted superconducting mercury-based oxycarbonates,Hg1-xMxSr4Cu2(CO3)O6+z(M=Cr and Mo)	199504		Laboratoire CRISMAT-CNRS URA 1318,ISMRA et Universite de Caen,Boulevard du Marechal Juin,14050 Caen cedex,France	Physica C.,246(1995)1-10	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo		
5463	PHC2460011	magnetic properties by inelastic neutron scatlering	Pb2Sr2EuCu3O8	Pb2Sr2Eu1Cu3O8	Pb	2	Sr	2	Eu	1	Cu	3													O		8		1995		0.01	emu.K/mole		micro.B/Mo	9.89	9.5																					Pb3212																																																																																																																							PbO,R2O3,CuO,CaCO3,SrCuO2		mixyube-prefire(950C,12H)-pellet-heat(890C,2days in Pt boat under N2 atmosphere)-cool to RT(1.5C/min)					The magnetic properties of R in Pb2Sr2(R/Ca)Cu3O8 (R = Ho and Er)	199504		Argonne  National Laboratory,Argonne IL 60439,USA	Physica C.,246(1995)11-21	C.-K.Loong,J.E.Greedan,J.P.Hammonds,J.Simon Xue,L.Soderholm,M.Maric,S.Skanthakumar,U.Staub		
5464	PHC2460011	magnetic properties by inelastic nsutron scatlering	Pb2Sr2H0Cu3O8	Pb2Sr2HCu3O8	Pb	2	Sr	2	H		Cu	3													O		8		1995			emu.K/mole		micro.B/Mo	10.1	9																					Pb3212																																																																																																																							PbO,R2O3,CuO,CaCO3,SrCuO2		mixyube-prefire(950C,12H)-pellet-heat(890C,2days in Pt boat under N2 atmosphere)-cool to RT(1.5C/min)					The magnetic properties of R in Pb2Sr2(R/Ca)Cu3O8 (R = Ho and Er)	199504		Argonne  National Laboratory,Argonne IL 60439,USA	Physica C.,246(1995)11-21	C.-K.Loong,J.E.Greedan,J.P.Hammonds,J.Simon Xue,L.Soderholm,M.Maric,S.Skanthakumar,U.Staub		
5465	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.197	Y	1	Ba	2	Cu	3															O	z	6.197		1995																												Y123																																																																																												649			TP5465																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5466	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.215	Y	1	Ba	2	Cu	3															O	z	6.215		1995																												Y123																																																																																															TP5466																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5467	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.24	Y	1	Ba	2	Cu	3															O	z	6.24		1995																												Y123																																																																																												416			TP5467																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5468	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.28	Y	1	Ba	2	Cu	3															O	z	6.28		1995																												Y123																																																																																												313			TP5468																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5469	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	z	6.35		1995																												Y123																																																																																												170			TP5469																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5470	PHC2460145	semiconductor	YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	z	6.4		1995																												Y123																																																																																												124			TP5470																										see RHC1960297					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
5471	SUP0080021		(Y,Ca)(Sr,Ba)2Cu2GaO7	Y0.6Ca0.4Sr1.8Ba0.2Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	1.8	Ba	0.2	Cu	2	Ga	1									O		7		1995																																														K		45					45																																																																																																					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5472	SUP0080021		(Y,Ca)(Sr,Ba)2Cu2GaO7	Y0.6Ca0.4Sr1.7Ba0.3Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	1.7	Ba	0.3	Cu	2	Ga	1									O		7		1995																																														K		50					50																																																																																																					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5473	SUP0080021		(Y,Ca)(Sr,Ba)2Cu2GaO7	Y0.6Ca0.4Sr1.6Ba0.4Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	1.6	Ba	0.4	Cu	2	Ga	1									O		7		1995																																														K		56					56																																																																																																					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5474	SUP0080021	long anneating 500C,180H in 350 bar O2	(Y,Ca)(Sr,Ba)2Cu2GaO7	Y0.6Ca0.4Sr1.8Ba0.2Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	1.8	Ba	0.2	Cu	2	Ga	1									O		7		1995																																														K		68					68																																																																																																					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5475	SUP0080021		(Y,Ca)Sr2Cu2GaO7	Y0.65Ca0.35Sr2Cu2Ga1O7	Y	0.65	Ca	0.35	Sr	2	Cu	2	Ga	1											O		7		1995																													Ima2		A	5.384	5.474	22.815														27					27																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3		mixture-heat(1050C,2OH in air)-pellet-SIN(1050C,in O2)-hold(460C,30H)-cool to RT-(500C,100H under pres of 350bar Oz)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5476	SUP0080021		(Y,Ca)Sr2Cu2GaO7	Y0.6Ca0.4Sr2Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	2	Cu	2	Ga	1											O		7		1995																													Ima2		A	5.382	5.472	22.805												K		41					41																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3		mixture-heat(1050C,2OH in air)-pellet-SIN(1050C,in O2)-hold(460C,30H)-cool to RT-(500C,100H under pres of 350bar Oz)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5477	SUP0080067	G-L parameter=15,e-ph coupling=0.8	Ba6C60	Ba6C60	Ba	6	C	60																					1995																												fullerene																		K			7				7											Oe	deviation from linear magnetization	130							T		2.2							T/K		0.45					A		120			A		1800																																																										On the Normal and Superconducting Properties of Ba6C60	1995		Department of Condensed Matter Physics, Royal Institute of Technology, S-100 44 Stockholm, Sweden	J.Superconductivity,8(1995)67	K.V. Rao,Vladislav Korenivski		
5478	PHC2430252	semiconductoo	Y(Sr,Ba)2(Cu,Cr)3O7	Y1CaSr1.5Ba0.5Cu2.8Cr0.2O7	Y	1	Ca		Sr	1.5	Ba	0.5	Cu	2.8	Cr	0.2									O		7		1995																																																			4.2																																																																					54.2			TP5478																									1	see physica C 207(1993)44					Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5479	PHC2430252		(Y,Ca)(Sr,Ba)2(Cu,Cr)3O7	Y0.8Ca0.2Sr1.5Ba0.5Cu2.8Cr0.2O7	Y	0.8	Ca	0.2	Sr	1.5	Ba	0.5	Cu	2.8	Cr	0.2									O		7		1995																																														K	23	28					28																																																																			25.7			TP5479	ohm.cm											5.6													1	see physica C 207(1993)44					Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5480	PHC2430252		(Y,Ca)(Sr,Ba)2(Cu,Cr)3O7	Y0.7Ca0.3Sr1.5Ba0.5Cu2.8Cr0.2O7	Y	0.7	Ca	0.3	Sr	1.5	Ba	0.5	Cu	2.8	Cr	0.2									O		7		1995																																														K	37	41					41																																																																			19.8			TP5480	ohm.cm											6.5													1	see physica C 207(1993)44					Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5481	PHC2430252		YBa2(Cu,Cr)3O7	Y1Ba2Cu2.8Cr0.2O7	Y	1	Ba	2	Cu	2.8	Cr	0.2													O		7		1995																												Y123																		K	82	87.5					87.5																																																																			8.76			TP5481	ohm.cm											2.5																			Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5482	PHC2430252	two step transition in thermopower.	YBa2(Cu,Co)3O7	Y1Ba2Cu2.79Co0.21O7	Y	1	Ba	2	Cu	2.79	Co	0.21													O		7		1995																												Y123																		K	22						22																																																																			47.7			TP5482																															Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5483	PHC2430252		(Y,Ca)(Sr,Ba)2(Cu,Ga)3O7	Y0.8Ca0.2Sr1Ba1Cu2.7Ga0.3O7	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.7	Ga	0.3									O		7		1995																												Y123																		K	60	64					64																																																																			11.4			TP5483	ohm.cm											2.16																			Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5484	PHC2430252		(Y,Ca)(Sr,Ba)2(Cu,Ga)3O7	Y0.8Ca0.2Sr1.6Ba0.4Cu2.7Ga0.3O7	Y	0.8	Ca	0.2	Sr	1.6	Ba	0.4	Cu	2.7	Ga	0.3									O		7		1995																												Y123																		K	47.9	53.9					53.9																																																																			12.6			TP5484	ohm.cm											7.53																			Comparison of carrier concentration determined by structural and electrical studies of substituted YSr2Cu3O7-z	199503		Interdisciplinary Research centre in Superconductivity,Madingley Road,Cambridge,CB3 OHE,UK	Physica C.,243(1995)252-256	A.Janossy,C.Greaves,J.R.Cooper,P.S.I.P.N.de Silva,T.G.N.Babu	Y,Sr,Cu,O	
5485	PHC2430233	as-synthesized.	(Hg,W)Ba2CuO4	Hg0.9W0.1Ba2Cu1O4.2	Hg	0.9	W	0.1	Ba	2	Cu	1													O		4.2		1995																											2	Hg1201			A	3.875		9.45												K				89			89										40																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5486	PHC2430233	as-synthesized. not SC. nominal (Hg0.8Cr0.2)-1201	(Hg,Cr)Ba2CuO4	Hg0.6Cr0.4Ba2Cu1O4.1	Hg	0.6	Cr	0.4	Ba	2	Cu	1													O		4.1		1995																											2	Hg1201			A	3.926		9.306												K					30																																																																																																M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5487	PHC2430233	after annealing in O2 flow. nominal (Hg0.8Cr0.2)-1201	(Hg,Cr)Ba2CuO4	Hg0.6Cr0.4Ba2Cu1O4.1	Hg	0.6	Cr	0.4	Ba	2	Cu	1													O		4.1		1995																											2	Hg1201			A	3.926		9.306												K				70			70										55																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5488	PHC2430233	(Hg0.75Mo0.25)by EDS	(Hg,Mo)Ba2CuO4	Hg0.8Mo0.2Ba2Cu1O4.4	Hg	0.8	Mo	0.2	Ba	2	Cu	1													O		4.4		1995																											2	Hg1201			A	3.882		9.378												K				74			74										60																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5489	PHC2430233		(Hg,Mo)Ba2CuO4	Hg0.9Mo0.1Ba2Cu1O4.2	Hg	0.9	Mo	0.1	Ba	2	Cu	1													O		4.2		1995																											2	Hg1201			A	3.875		9.435												K				75			75										60																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5490	PHC2430233	secondary phese Ba2CuWO6 exists	(Hg,W)Ba2CuO4	Hg0.8W0.2Ba2Cu1O4.4	Hg	0.8	W	0.2	Ba	2	Cu	1													O		4.4		1995																											2	Hg1201			A	3.871		9.416												K				45			45										30																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5491	PHC2430233		HgBa2CuO4	Hg0.9Ba2Cu1O4+z	Hg	0.9	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201			A	3.883		9.536												K				91			91										51																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5492	PHC2430233		(Hg,V)Ba2CuO4	Hg0.8V0.2Ba2Cu1O4.3	Hg	0.8	V	0.2	Ba	2	Cu	1													O		4.3		1995																											2	Hg1201			A	3.8863		9.338												K				96			96										65																																																																																				M-oxide,BaO,CaO,CuO,HgO		mixture - heat to 800					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5493	PHC2430233		HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1995																											2	Hg1212			A	3.862		12.704												K				117			117																																																																																																					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5494	PHC2430233	after annealing in O2 flow	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1995																											2	Hg1212																		K				127			127																																																																																																					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5495	PHC2430233		(Hg,V)Ba2CaCu2O6	Hg0.8V0.2Ba2Ca1Cu2O6.3	Hg	0.8	V	0.2	Ba	2	Ca	1	Cu	2											O		6.3		1995																											2	Hg1212			A	3.869		12.5												K				119			119			K/GPa							60																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5496	PHC2430233	after annealing in O2 flow	(Hg,V)Ba2CaCu2O6	Hg0.8V0.2Ba2Ca1Cu2O6.3	Hg	0.8	V	0.2	Ba	2	Ca	1	Cu	2											O		6.3		1995																											2	Hg1212																		K				128			128			K/GPa							75																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5497	PHC2430233	(Hg0.75Mo0.25)by EDS	(Hg,Mo)Ba2CaCu2O6	Hg0.8Mo0.2Ba2Ca1Cu2O6.4	Hg	0.8	Mo	0.2	Ba	2	Ca	1	Cu	2											O		6.4		1995																											2	Hg1212			A	3.86		12.576												K				127			127			K/GPa							75																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5498	PHC2430233	(Hg0.75W0.25)by EDS	(Hg,Mo)Ba2CaCu2O6	Hg0.8W0.2Ba2Ca1Cu2O6.4	Hg	0.8	W	0.2	Ba	2	Ca	1	Cu	2											O		6.4		1995																											2	Hg1212			A	3.861		12.661												K				118			118			K/GPa							58																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5499	PHC2430233		(Hg,W)Ba2CaCu2O6	Hg0.9W0.1Ba2Ca1Cu2O6.2	Hg	0.9	W	0.1	Ba	2	Ca	1	Cu	2											O		6.2		1995																											2	Hg1212			A	3.864		12.685												K				118			118			K/GPa							40																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5500	PHC2430233	(Hg0.7,Ti0.3)by EDS	(Hg,Ti)Ba2Ca1Cu2O6	Hg0.8Ti0.2Ba2Ca1Cu2O6.2	Hg	0.8	Ti	0.2	Ba	2	Ca	1	Cu	2											O		6.2		1995																											2	Hg1212			A	3.857		12.581												K				127			127			K/GPa							80																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5501	PHC2430233	(Hg0.6,Cr0.4)by EDS	(Hg,Cr)Ba2CaCu2O6	Hg0.8Cr0.2Ba2Ca1Cu2O6.1	Hg	0.8	Cr	0.2	Ba	2	Ca	1	Cu	2											O		6.1		1995																											2	Hg1212			A	3.875		12.488												K				110			110			K/GPa							75																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5502	PHC2430233	after annealing in O2 flow	(Hg,Cr)Ba2CaCu2O6	Hg0.8Cr0.2Ba2Ca1Cu2O6.1	Hg	0.8	Cr	0.2	Ba	2	Ca	1	Cu	2											O		6.1		1995																											2	Hg1212																		K				115			115			K/GPa							98																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5503	PHC2430233	Compositions are nominal values. 	HgBa2Ca2Cu3O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1995																											2	Hg1212			A	3.856		15.856												K				105			105																																																																																																					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5504	PHC2430233	Sample was  annealed in O2 flow. Compositions are nominal values. 	HgBa2Ca2Cu3O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1995																											2	Hg1223																		K				134			134																																																																																																					The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5505	PHC2430233	(Hg0.7V0.3)by EDS	(Hg,V)Ba2Ca2Cu3O8	Hg0.8V0.2Ba2Ca2Cu3O8.3	Hg	0.8	V	0.2	Ba	2	Ca	2	Cu	3											O		8.3		1995																											2	Hg1223			A	3.863		15.652												K				120			120			K/GPa							80																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5506	PHC2430233	after annealing in O2 Flow 	(Hg,V)Ba2Ca2Cu3O8	Hg0.8V0.2Ba2Ca2Cu3O8.3	Hg	0.8	V	0.2	Ba	2	Ca	2	Cu	3											O		8.3		1995																											2	Hg1223																		K				127			127			K/GPa							80																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5507	PHC2430233	(Hg0.75Mo0.25)by EDS	(Hg,Mo)Ba2Ca2Cu3O8	Hg0.8Mo0.2Ba2Ca2Cu3O8.4	Hg	0.8	Mo	0.2	Ba	2	Ca	2	Cu	3											O		8.4		1995																											2	Hg1223			A	3.854		15.731												K				129			129			K/GPa							62																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5508	PHC2430233	after annealing in O2 flow	(Hg,Mo)Ba2Ca2Cu3O8	Hg0.8Mo0.2Ba2Ca2Cu3O8.4	Hg	0.8	Mo	0.2	Ba	2	Ca	2	Cu	3											O		8.4		1995																											2	Hg1223																		K				134			134			K/GPa							67																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5509	PHC2430233	(Hg0.7Ti0.3)by EDS	(Hg,Ti)Ba2Ca2Cu3O8	Hg0.6Ti0.4Ba2Ca2Cu3O8.4	Hg	0.6	Ti	0.4	Ba	2	Ca	2	Cu	3											O		8.4		1995																											2	Hg1223			A	3.851		15.707												K				128			128			K/GPa							58																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5510	PHC2430233	after annealing in O2 flow	(Hg,Ti)Ba2Ca2Cu3O8	Hg0.6Ti0.4Ba2Ca2Cu3O8.4	Hg	0.6	Ti	0.4	Ba	2	Ca	2	Cu	3											O		8.4		1995																											2	Hg1223																		K				134			134			K/GPa							60																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5511	PHC2430233	(Hg0.6Cr0.4)by EDS	(Hg,Cr)Ba2Ca2Cu3O8	Hg0.8Cr0.2Ba2Ca2Cu3O8.1	Hg	0.8	Cr	0.2	Ba	2	Ca	2	Cu	3											O		8.1		1995																											2	Hg1223			A	3.863		15.625												K				95			95			K/GPa							68																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5512	PHC2430233	after annealing in O2 flow	(Hg,Cr)Ba2Ca2Cu3O8	Hg0.8Cr0.2Ba2Ca2Cu3O8.1	Hg	0.8	Cr	0.2	Ba	2	Ca	2	Cu	3											O		8.1		1995																											2	Hg1223																		K				110			110			K/GPa							76																																																																																											The great ability of mercury-based cuprates to accommodate transition elements	199503		Laboratoire CRIMAT-ISMRA-Universite de Caen,6 boulevard du Marec Juin,14050 Caen Cedex,France	Physica C.,243(1995)233-242	A.Maignan,B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,S.Malo	Hg,Ba,Ca,Cu,O,V,Mo,W,Ti,Cr	
5513	PHC2410383	pressure effect of JC.was measured	(Y,Ca)(Ba,Ca)2Cu4O8	Y0.95Ba1.95Ca0.1Cu4O8	Y	0.95	Ba	1.95	Ca	0.1	Cu	4													O		8	1	1995																												Y124																		K				80			80			K/GPa	5.5																																																																																											1	Ca was added to stabilige Y124 phase. Ca replaces both Y and Ba.					Comparative study of the pressure effect on critical parameters of GdBa2Cu4O8 and YBa2Cu4O8	199501		Institute of Physics Academy of Sciences Al. Lotnikow 32/46,02-668 Warszawa,Poland	Physica C.,241(1995)383-388	G.Levchenko,H.Szymczak,L.Gladczuk,M.Baran,S.Piechota,V.Dyakonov	Gd,Ba,Cu,O,Y	
5514	PHC2410383	pressure effect of JC was measured	(Gd,Ca)(Ba,Ca)2Cu4O8	Gd0.95Ba1.95Ca0.1Cu4O8	Gd	0.95	Ba	1.95	Ca	0.1	Cu	4													O		8	1	1995																												Y124																		K				80			80			K/GPa	4.5																																																																																											1	Ca was added to stabilige Y124 phase. Ca replaces both Y and Ba.					Comparative study of the pressure effect on critical parameters of GdBa2Cu4O8 and YBa2Cu4O8	199501		Institute of Physics Academy of Sciences Al. Lotnikow 32/46,02-668 Warszawa,Poland	Physica C.,241(1995)383-388	G.Levchenko,H.Szymczak,L.Gladczuk,M.Baran,S.Piechota,V.Dyakonov	Gd,Ba,Cu,O,Y	
5515	PRL0741202	delta-ramda increases linearly with H	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																		K																																																A			2600																																																									Magnetic Field Dependnce of the London Penetration Depth of Bi2Sr2CaCu2Oy	199502		Department of Pure and Applied Sciences,The University of Tokyo,3-8-1,Komaba,Meguro-ku,Tokyo153, Japan	Phys.Rev.Lett.,74(1995)1202	A.Maeda,K.Kishio,N.Motohira,T.Fukase,T.Hanaguri,Y.Iino	Bi,Sr,Ca,Cu,O	
5516	PRL0740598	untwinned sample,ppenet=800 A for b-axis	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	3	1995																												Y124			A															K		80				0.5	80																																									A			2000																																																				under high-O2 pressure,see Physica C 202(1992)271					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
5517	PRL0740598	detwinned under uniaxial stress,anisotropy factor in a-,b- direction = 2.3 , from surface resistance penet= 1000A for b-axis,	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1995																												Y123																		K		93.5				0.2	93.5																																									A	far infrared reflectance		1600																																																			5	see Physica C 195(1992)51					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
5518	PRL0740598	anisotropy factor in a-,b-,direction = 2.1 from dc resistivity, penet=1200A for b-axis from surface resistance	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1995																												Y123																		K	92						92																																									A		1200	1600																																																				see Phys.Rev.42(1990)6217					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
5519	PHC2410001	as-Synthesized,XRD shows not-pure Hg1201	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1995																												Hg1201																		K				90			90										60																																																																																											Stabilization of mercury cuprates by bismuth  The supercounductor Hg1-xBixBa2Cam-1CumO2m+2+z	199501		Laboratoire CRISMAT,ISMRA,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,241(1995)1-9	B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,V.Badri	Hg,Bi,Ba,Ca,Cu,O	
5520	PHC2410001	as-synthesized.,XRD shows pure Hg1201	HgBa2CuO4	Hg0.9Ba2Cu1O4	Hg	0.9	Ba	2	Cu	1															O		4		1995																												Hg1201																		K				73			73										60																																																																																											Stabilization of mercury cuprates by bismuth  The supercounductor Hg1-xBixBa2Cam-1CumO2m+2+z	199501		Laboratoire CRISMAT,ISMRA,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,241(1995)1-9	B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,V.Badri	Hg,Bi,Ba,Ca,Cu,O	
5521	PHC2410001	as-synthesized	(Hg,Bi)Ba2CuO4	Hg0.8Bi0.2Ba2Cu1O4.2	Hg	0.8	Bi	0.2	Ba	2	Cu	1													O		4.2		1995																											2	Hg1201			A	3.876		9.475												K				85			85																																																																																																					Stabilization of mercury cuprates by bismuth  The supercounductor Hg1-xBixBa2Cam-1CumO2m+2+z	199501		Laboratoire CRISMAT,ISMRA,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,241(1995)1-9	B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,V.Badri	Hg,Bi,Ba,Ca,Cu,O	
5522	PHC2410001	as-synthesized	(Hg,Bi)Ba2Ca2Cu3O8	Hg0.8Bi0.2Ba2Ca2Cu3O8.2	Hg	0.8	Bi	0.2	Ba	2	Ca	2	Cu	3											O		8.2		1995																											2	Hg1223			A	3.85		15.813												K				130			130										75																																																																																											Stabilization of mercury cuprates by bismuth  The supercounductor Hg1-xBixBa2Cam-1CumO2m+2+z	199501		Laboratoire CRISMAT,ISMRA,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,241(1995)1-9	B.Raveau,C.Michel,D.Pelloquin,M.Hervieu,V.Badri	Hg,Bi,Ba,Ca,Cu,O	
5523	PHC2410301	nominal Y:Ba:Cu=1.02:2:3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7		1995																											3	Y123			A	3.818	3.886	11.679												K		92.03					92.03																																																								mJ/K2fu	0.71	SP-heat	509																																				1	mixture-CAL(920C,24H)-pellet-heat(935C,120H)-Ann(300C,240H)in flowing Oz					Specific heat of YBa2Cu3O7-z ceramics with single and double superconducting transitions in magnetic fields up to 14 T	199501		Departement de Physique de la Matiere Condensee,Universite de Geneve,CH-1211 Geneve  4,Swizerland	Physica C.,241(1995)301-310	A.Junod,A.Mirmelstein,E.Janod,J.Muller,K.-Q.Wang	Y,Ba,Cu,O	
5524	PHC2410301	nominal Y:Ba:Cu=1:2:3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7		1995																											3	Y123			A	3.818	3.885	11.677														92.83					92.83																																																						mJ/mole.K		mJ/K2fu			460																																					mixture-CAL(920C,24H)-pellet-heat(950C,120H)-ANN(300C,240H in flowing O2)-ANN(460C,24H)-Q to liquid Ga					Specific heat of YBa2Cu3O7-z ceramics with single and double superconducting transitions in magnetic fields up to 14 T	199501		Departement de Physique de la Matiere Condensee,Universite de Geneve,CH-1211 Geneve  4,Swizerland	Physica C.,241(1995)301-310	A.Junod,A.Mirmelstein,E.Janod,J.Muller,K.-Q.Wang	Y,Ba,Cu,O	
5525	PHC2410211	Ts=970C,P=3.0GPa	(Hg,Mo)Sr2Ca2Cu3O8	Hg0.95Mo0.05Sr2Ca2Cu3Oz	Hg	0.95	Mo	0.05	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223			A	3.829		15.294												K			106				106																																																																																																(precursor+HgO+MoO3)-pellet-encapsuled in Au forl-react(Ts,P)					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5526	PHC2410211	Ts=970C, P=3.0GPa	(Hg,Mo)Sr2Ca2Cu3O8	Hg0.75Mo0.05Sr2Ca2Cu3O	Hg	0.75	Mo	0.05	Sr	2	Ca	2	Cu	3											O				1995																											2	Hg1223			A	3.83		15.323												K				106			106																																																																																																(precursor+HgO+MoO3)-pellet-encapsuled in Au forl-react(Ts,P)					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5527	PHC2410211	pressure=2.0GPa Ts=880C	Hg(Ba,Sr)2Ca2Cu3O8	Hg0.75SrBa2Ca2Cu3O8+z	Hg	0.75	Sr		Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Hg1223			A	3.855		15.83												K			133	133.5			133.5																																																																																																mix(precursor Ba2Ca2Cu3O7,Sr2Ca2Cu3O7+HgO)-pellet-Aufoil-high pressure using BaCO3 medium T>1000C					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5528	PHC2410211	2.5GPa Ts=980C	Hg(Ba,Sr)2Ca2Cu3O8	Hg0.75Sr0.5Ba1.5Ca2Cu3O8+z	Hg	0.75	Sr	0.5	Ba	1.5	Ca	2	Cu	3											O	8+z			1995																											2	Hg1223			A	3.846		15.68												K			127.5	126.2			126.2																																																																																																mix(precursor Ba2Ca2Cu3O7,Sr2Ca2Cu3O7+HgO)-pellet-Aufoil-high pressure using BaCO3 medium T>1000C					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5529	PHC2410211	2.5GPa 1000C	Hg(Ba,Sr)2Ca2Cu3O8	Hg0.75Sr1Ba1Ca2Cu3O8+z	Hg	0.75	Sr	1	Ba	1	Ca	2	Cu	3											O	8+z			1995																											2	Hg1223			A	3.837		15.552												K			123	122			122																																																																																																mix(precursor Ba2Ca2Cu3O7,Sr2Ca2Cu3O7+HgO)-pellet-Aufoil-high pressure using BaCO3 medium T>1000C					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5530	PHC2410211	2.5GPa 980C	Hg(Ba,Sr)2Ca2Cu3O8	Hg0.5Pb0.5Sr2Ca2Cu3Oz	Hg	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223			A	3.838		15.54												K			123.5	121			121																																																																																																mix(precursor Ba2Ca2Cu3O7,Sr2Ca2Cu3O7+HgO)-pellet-Aufoil-high pressure using BaCO3 medium T>1000C					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5531	PHC2410211	3.0GPa 970C	Hg(Ba,Sr)2Ca2Cu3O8	Hg0.5Pb0.5Sr2Ca2Cu3Oz	Hg	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223			A	3.815		15.327												K			107.5	107			107																																																																																																mix(precursor Ba2Ca2Cu3O7,Sr2Ca2Cu3O7+HgO)-pellet-Aufoil-high pressure using BaCO3 medium T>1000C					High-pressure synthesis of single-phase superconductors HgzSrxBa2-xCa2Cu3O8+zand(Hg,M)Sr2Ca2CU3Oy with M=Pb and Mo	199501		Department of Physics,Zhougshan University,Guandzhou 510 275,People's Republic of China	Physica C.,241(1995)211-218	C.W.Chu,L.Gao,Q.M.Lin,Y.Y.Sun,Y.Y.Xue,Z.H.He	Hg,Sr,Ba,Ca,Cu,O,Pb,Mo	
5532	PHC2410181	optimum fluorination condition is at 180C	Sr2CuO2F2	Sr2Cu1F2O2	Sr	2	Cu	1	F	2															O		2		1995																													Fmmm																					47			47																																																																																																Sr2CuO3(from mixed SrO+CuO)-react in flowing F2/Ne gas at 180 C for 20 min					Supercondusting properties of strontium copper oxyfluoride,Sr2CuO2F2+z	199501		Sandia National Laboratory,Albuquerque,NM87185-0345,USA	Physica C 241(1995)181-186	B.Morosin,E.L.Venturini,J.E.Schirber,P.P.Newcomer,R.G.Dunn	Sr,Cu,O,F	
5533	PHC2410151		(Sr,Ba)2CuO2F2	Sr2BaCu1F2O2	Sr	2	Ba		Cu	1	F	2													O		2		1995																											3				A	5.405	5.513	13.46												K				46			46																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5534	PHC2410151		(Sr,Ba)2CuO2F2	Sr1.9Ba0.1Cu1F2O2	Sr	1.9	Ba	0.1	Cu	1	F	2													O		2		1995																											3				A	5.409	5.504	13.49												K				54			54																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5535	PHC2410151		(Sr,Ba)2CuO2F2	Sr1.75Ba0.25Cu1F2O2	Sr	1.75	Ba	0.25	Cu	1	F	2													O		2		1995																											3				A	5.431	5.498	13.56												K				58			58																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5536	PHC2410151		(Sr,Ba)2CuO2F2	Sr1.6Ba0.4Cu1F2O2	Sr	1.6	Ba	0.4	Cu	1	F	2													O		2		1995																											2				A	5.475		13.64												K				60			60																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5537	PHC2410151		(Sr,Ba)2CuO2F2	Sr1.5Ba0.5Cu1F2O2	Sr	1.5	Ba	0.5	Cu	1	F	2													O		2		1995																											2				A	5.475		13.64												K				62			62																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5538	PHC2410151		(Sr,Ba)2CuO2F2	Sr1.4Ba0.6Cu1F2O2	Sr	1.4	Ba	0.6	Cu	1	F	2													O		2		1995																											2				A	5.48		13.69												K				64			64																																																																																														SrCO3,BaCO3,CaCO3,CuO	1	NH4F was added to Sr<2-x>(Ca,Ba)<x>CuO<3>-mixture-pellet-heat(225C,6H under O2 or N2 or air)-cool to RT in N2					Superconductivity up to 64 K in the copper oxyfluorides Sr2-xAxCuO2F2+z(A=Ca,Ba) prepared using NH4F as a fluorinating reagent	199501		Shool of Chemsity of Birmingham,Edgbaston,Birmingham B15 2TT,UK	Physica C.,241(1995)151-157	C.Greaves,I.Gameson,J.P.Hodges,M.Al-Mamouri,M.G.Francesconi,M.Slaski,P.P.Edwards,P.R.Slater	Sr,Ca,Ba,Cu,O,F	
5539	PHC2410137	impurity=CuO	BSr2Ca3Cu4O11	B1Sr2Ca3Cu4O11	B	1	Sr	2	Ca	3	Cu	4													O		11	1	1995																											2	B1234	P4/mmm		A	3.836		17.082												K	105	110	118	110			110																																																																																														SrCuO2,CaCuO3,SrO2CuO,B2O3	1	mixture-sealed in Au capsule-heat(1200C,1H under 6GPa)					New oxyborate superconductor,BSr2Ca3Cu4O11(Tc=110K) prepared at high pressure	199501		National Instiute for Research in Inorganic Materials(NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan	Physica C.,241(1995)137-141	E.Takayama-Muromachi,K.Kosuda,Y.Matsui	B,Sr,Ca,Cu,O	
5540	PRL0730166	epitaxial film	SrCuO2	Sr0.85Cu1O2	Sr	0.85	Cu	1																	O		2	4	1994																												IL																		K					10																																																																									m.ohm.cm											3.47			m3/C					8	RH5540					thin films were grown by pulsed laser ablation,see Phys.Rev.B.47(1993)8986					Anomalpus T3 Inverse Hall Mobilities Observed in Sr1-xCuO2 and Sr0.9Nd0.1CuO2 Infinite-Layer Thin Films	199407		Solid State Division,Oak Ridge National Laboratory,Oak Ridge,Tennessee 37831-6061	Phys.Rev.Lett.,73(1994)0166	David K.Christen,David P.Norton,Douglas H.Lowdes,Edwin C.Jones	Sr,Cu,O,Nd	
5541	PRL0730166	epitaxial film	(Sr,Nd)CuO2	Sr0.9Nd0.1Cu1O2	Sr	0.9	Nd	0.1	Cu	1															O		2	4	1994																												IL																																																																																																m.ohm.cm											0.79			m3/C					8	RH5541					thin films were grown by pulsed laser ablation,see Phys.Rev.B.47(1993)8986					Anomalpus T3 Inverse Hall Mobilities Observed in Sr1-xCuO2 and Sr0.9Nd0.1CuO2 Infinite-Layer Thin Films	199407		Solid State Division,Oak Ridge National Laboratory,Oak Ridge,Tennessee 37831-6061	Phys.Rev.Lett.,73(1994)0166	David K.Christen,David P.Norton,Douglas H.Lowdes,Edwin C.Jones	Sr,Cu,O,Nd	
5542	PRL0730166	epitaxial film	YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O		6.4	4	1994																												Y123																																																																																																m.ohm.cm											1.91			m3/C					8	RH5542					thin films were grown by pulsed laser ablation,see Phys.Rev.B.47(1993)8986					Anomalpus T3 Inverse Hall Mobilities Observed in Sr1-xCuO2 and Sr0.9Nd0.1CuO2 Infinite-Layer Thin Films	199407		Solid State Division,Oak Ridge National Laboratory,Oak Ridge,Tennessee 37831-6061	Phys.Rev.Lett.,73(1994)0166	David K.Christen,David P.Norton,Douglas H.Lowdes,Edwin C.Jones	Sr,Cu,O,Nd	
5543	NAT3470369	point contact tunneling counter electrode=Au	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		1	1990																												T'																		K		23					23																																														meV	3.7	3.9	1																																													Nd2O3,CeO2,CuO	1	ANN in a reduced at mosphere					Tunnelling evidence for predominantly electron-phonon coupling in superconducting Ba1-xKxBiO3and Nd2-xCexCuO4-y	9		Materials Science Division,and Science and Technology Center for Superconductivity,Argonne National Laboratory,Argonne,lllinois 60439,USA	NATURE.,347(1990)369	D.G.Hinks,J.F.Zasadzinski,J.L.Peng,K.E.Gray,N.Tralshawala,Q.Huang,R.L.Greene	Ba,K,Bi,O,Nd,Ce,Cu	
5544	NAT3470369	point contact tunneling counter electrode=Au	(Ba,K)BiO3	Ba0.625K0.375Bi1O3	Ba	0.625	K	0.375	Bi	1															O		3	1	1990																												BKBO																		K		30					30																																														meV	3.8	3.8																																														Bi2O3,BaO,KO2		Melt-process technique					Tunnelling evidence for predominantly electron-phonon coupling in superconducting Ba1-xKxBiO3and Nd2-xCexCuO4-y	9		Materials Science Division,and Science and Technology Center for Superconductivity,Argonne National Laboratory,Argonne,lllinois 60439,USA	NATURE.,347(1990)369	D.G.Hinks,J.F.Zasadzinski,J.L.Peng,K.E.Gray,N.Tralshawala,Q.Huang,R.L.Greene	Ba,K,Bi,O,Nd,Ce,Cu	
5545	APL0591905	gap=3.8-4.0,SIS tunneling,barrie is native surface oxide	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O		3	4	1991																											1	BKBO																		K	26.5		28				27.25																																														meV	4.5	3.8	1																																															grown by pulsed laser,substrate=LaAlO3					In situ pulsed laser deposition of superconducting Ba1-xKxBiO3 thin films	10		Science and Technology Center for Superconductivity and Department of Physics,University Illinois at Urbana-Champaign, Urbana, Illinois 61801	Appl.phys.Lett.59(1991)1905	B.M. Moon,C.E. Platt,D.J. Van Harlingen,R.A. Schweinfurth		
5546	APL0610480	target=Ba0.6K0.4BiO3,thickness=1500A	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O		3	4	1992																												BKBO																		K	28					0.3	28																				T	WHH theory	15.2							T/K		0.78					A		46												3.1																					m.ohm.cm							0.25				0.52														ArF excimer laser,substrate=MgO(100)					Electrical and magnetic transport properties of laser-deposited Ba1-xKxBiO3 thin films	7		Science and Technology Center for Superconductivity and Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801	Appl.Phys.Lett.61(1992)480	C.E. Platt,D.J. van Harlingen,M.R. Teepe,R.A. Schweinfurth		
5547	PR05108624	rhombohed BaRuO3 structure	Ba(Ru,Rh)O3	Ba1Ru0.67Rh0.33O3	Ba	1	Ru	0.67	Rh	0.33															O		3	1	1995			emu.K/mole		micro.B/Mo	5.8	-920																						R-3m		A	5.747		21.726												K					4.2																																																																																																RuO2,Rh2O3,BaCO3,SrCO3		1200C,several days in air inAlumina,for Ba-Ru-Rh-O,1200C,in flowing O2 for Sr-Ru-Rh-O					Magnetic properties of BaRu1-xRhxO3 and Sr2Ru1-xRhxO4	199504		Inorganic Chemistry Laboratory,Oxford University,South Parks Road,Oxford OX1 3QR,United Kingdom	Phys.Rev.B.,51(1995)8624	J.G.Gore,J.R.Frost,P.D.Battle	Ba,Ru,Rh,O,Sr	
5548	PR05108624	rhombohedral BaRuO3 structure	Ba(Ru,Rh)O3	Ba1Ru0.5Rh0.5O3	Ba	1	Ru	0.5	Rh	0.5															O		3	1	1995			emu.K/mole		micro.B/Mo	2.9	-375																						R-3m		A	5.753		21.762												K					4.2																																																																																																RuO2,Rh2O3,BaCO3,SrCO3		1200C,several days in air inAlumina,for Ba-Ru-Rh-O,1200C,in flowing O2 for Sr-Ru-Rh-O					Magnetic properties of BaRu1-xRhxO3 and Sr2Ru1-xRhxO4	199504		Inorganic Chemistry Laboratory,Oxford University,South Parks Road,Oxford OX1 3QR,United Kingdom	Phys.Rev.B.,51(1995)8624	J.G.Gore,J.R.Frost,P.D.Battle	Ba,Ru,Rh,O,Sr	
5549	PR05108624		Sr2(Ru,Rh)O4	Sr2Ru0.5Rh0.5O4	Sr	2	Ru	0.5	Rh	0.5															O		4	1	1995			emu.K/mole		micro.B/Mo	2.3	-259																				2		I4/mmm		A	3.877		12.782												K					4.2																																																																																																RuO2,Rh2O3,BaCO3,SrCO3		1200C,several days in air inAlumina,for Ba-Ru-Rh-O,1200C,in flowing O2 for Sr-Ru-Rh-O					Magnetic properties of BaRu1-xRhxO3 and Sr2Ru1-xRhxO4	199504		Inorganic Chemistry Laboratory,Oxford University,South Parks Road,Oxford OX1 3QR,United Kingdom	Phys.Rev.B.,51(1995)8624	J.G.Gore,J.R.Frost,P.D.Battle	Ba,Ru,Rh,O,Sr	
5550	PR05108624		Sr2(Ru,Rh)O4	Sr2Ru0.33Rh0.67O4	Sr	2	Ru	0.33	Rh	0.67															O		4	1	1995			emu.K/mole		micro.B/Mo	2.51	-323																				2		I4/mmm		A	3.871		12.812			A/K									K					4.2																																																																									m.ohm.cm														m3/C									RuO2,Rh2O3,BaCO3,SrCO3		1200C,several days in air inAlumina,for Ba-Ru-Rh-O,1200C,in flowing O2 for Sr-Ru-Rh-O					Magnetic properties of BaRu1-xRhxO3 and Sr2Ru1-xRhxO4	199504		Inorganic Chemistry Laboratory,Oxford University,South Parks Road,Oxford OX1 3QR,United Kingdom	Phys.Rev.B.,51(1995)8624	J.G.Gore,J.R.Frost,P.D.Battle	Ba,Ru,Rh,O,Sr	
5551	CRY0350271	Bi2212+Bi2223	(Bi,Pb)2Sr2Ca2Cu3O16	Bi1.82Pb0.18Sr2Ca2Cu3O16+z	Bi	1.82	Pb	0.18	Sr	2	Ca	2	Cu	3											O	16+z		2	1995																											2	Bi2223																		K		102.98					102.98																																																																		micro.V/K	3.482				m.ohm.cm											4.11												Bi2O3,PbO,CuO,CaCO3,Sr2CO3	1	mixture-CAL(820C,48H in air)-SIN(840C,110H in air)-FC to Rt					Influence of lead content on temperature dependence of thermoelectric power of 2223(Bi-Pb) sintered cuprates			High Temperature Superconductivity Laboratory,Cryogenic Engineering Centre, and Department of Physics,Indian Institute of Tachnology,Khaeagpur 721 302, India	Cryogenics 35 (1995)271-275	B.Chanda,S.K.Ghatak,T.K.Dey	Bi,Pb,Sr,Ca,Cu,O	
5552	CRY0350271	Bi2212+Bi2223	(Bi,Pb)2Sr2Ca2Cu3O16	Bi1.72Pb0.28Sr2Ca2Cu3O16+z	Bi	1.72	Pb	0.28	Sr	2	Ca	2	Cu	3											O	16+z		2	1995																											2	Bi2223																		K		102.98					102.98																																																						mJ/mole.K		mJ/K2fu					W/K.M					micro.V/K	2.451				ohm.cm											3.64												Bi2O3,PbO,CuO,CaCO3,Sr2CO3	1	mixture-CAL(820C,48H in air)-SIN(840C,110H in air)-FC to Rt					Influence of lead content on temperature dependence of thermoelectric power of 2223(Bi-Pb) sintered cuprates			High Temperature Superconductivity Laboratory,Cryogenic Engineering Centre, and Department of Physics,Indian Institute of Tachnology,Khaeagpur 721 302, India	Cryogenics 35 (1995)271-275	B.Chanda,S.K.Ghatak,T.K.Dey	Bi,Pb,Sr,Ca,Cu,O	
5553	CRY0350271	Bi2212+Bi2223	(Bi,Pb)2Sr2Ca2Cu3O16	Bi1.62Pb0.38Sr2Ca2Cu3O16+z	Bi	1.62	Pb	0.38	Sr	2	Ca	2	Cu	3											O	16+z		2	1995																											2	Bi2223																		K		104.44					104.44																																																						mJ/mole.K		mJ/K2fu					W/K.M					micro.V/K	1.399				ohm.cm											2.851												Bi2O3,PbO,CuO,CaCO3,Sr2CO3	1	mixture-CAL(820C,48H in air)-SIN(840C,110H in air)-FC to Rt					Influence of lead content on temperature dependence of thermoelectric power of 2223(Bi-Pb) sintered cuprates			High Temperature Superconductivity Laboratory,Cryogenic Engineering Centre, and Department of Physics,Indian Institute of Tachnology,Khaeagpur 721 302, India	Cryogenics 35 (1995)271-275	B.Chanda,S.K.Ghatak,T.K.Dey	Bi,Pb,Sr,Ca,Cu,O	
5554	CRY0350271	Bi2212+Bi2223  Bi2223 is dominant	(Bi,Pb)2Sr2Ca2Cu3O16	Bi1.52Pb0.48Sr2Ca2Cu3O16+z	Bi	1.52	Pb	0.48	Sr	2	Ca	2	Cu	3											O	16+z		2	1995																											2	Bi2223			A	5.411		37.03												K		107.17					107.17																																																						mJ/mole.K		mJ/K2fu					W/K.M					micro.V/K	2.358				ohm.cm											2.358												Bi2O3,PbO,CuO,CaCO3,Sr2CO3	1	mixture-CAL(820C,48H in air)-SIN(840C,110H in air)-FC to Rt					Influence of lead content on temperature dependence of thermoelectric power of 2223(Bi-Pb) sintered cuprates			High Temperature Superconductivity Laboratory,Cryogenic Engineering Centre, and Department of Physics,Indian Institute of Tachnology,Khaeagpur 721 302, India	Cryogenics 35 (1995)271-275	B.Chanda,S.K.Ghatak,T.K.Dey	Bi,Pb,Sr,Ca,Cu,O	
5555	NAT3750126	Z=32formula units per unit cell,calcuted density=2.92g/cm3	Yb3C60	C60Yb2.75	C	60	Yb	2.75																					1995																													Pcab		A	27.874	27.98	27.873												K		6		6			6			K/GPa							5.6																																																																																						(Y6+C60)-seeled in quartz tube (E-7 Torr)-heat (630C,6H)-cool to RT(5C/min)					Superconductivity and cation-vacancy ordering in the rare-earth fulleride Yb2.75C60	5		AT&T Bell Laboratories, Murray Hill, new Jersey 07974, USA	Nature 375(1995)126	A.P. Ramirez,A.R. Kortan,E. Ozdas,H.E. Bair,K.M. Rabe,N. Kopylov,P.H. Cltrin,S. Schuppler,T. Siegrist		
5556	PLA1960263	Oxygen content=6.91-6.95 in dependent of x	(Y,Pr)BaSrCu3O7	Y1PrBa1Sr1Cu3O6.95	Y	1	Pr		Ba	1	Sr	1	Cu	3											O	7-z	6.95	1	1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5557	PLA1960263	Oxygen content=6.91-6.95 independent of x	(Y,Pr)BaSrCu3O7	Y0.8Pr0.2Ba1Sr1Cu3O6.95	Y	0.8	Pr	0.2	Ba	1	Sr	1	Cu	3											O	7-z	6.95	1	1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5558	PLA1960263	Oxygen content=6.91-6.95 independent of x	(Y,Pr)BaSrCu3O7	Y0.6Pr0.4Ba1Sr1Cu3O6.95	Y	0.6	Pr	0.4	Ba	1	Sr	1	Cu	3											O	7-z	6.95	1	1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5559	PLA1960263	Oxygen content=6.91-6.95 independent of x	(Y,Pr)BaSrCu3O7	Y0.5Pr0.5Ba1Sr1Cu3O6.95	Y	0.5	Pr	0.5	Ba	1	Sr	1	Cu	3											O	7-z	6.95	1	1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5560	PLA1960263	Oxygen content=6.91-6.95 independent of x	(Y,Pr)BaSrCu3O7	Y0.4Pr0.6Ba1Sr1Cu3O6.95	Y	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7-z	6.95	1	1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5561	PLA1960263		(Y,Pr)BaSrCu3O7	Y0.35Pr0.65Ba1Sr1Cu3O6.95	Y	0.35	Pr	0.65	Ba	1	Sr	1	Cu	3											O	7-z	6.95		1994																												Y123																																																																																																																							Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5562	PLA1960263		(Y,Pr)BaSrCu3O7	Y0.3Pr0.7Ba1Sr1Cu3O6.95	Y	0.3	Pr	0.7	Ba	1	Sr	1	Cu	3											O	7-z	6.95		1994																												Y123																		K				14			14																																																																																														Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5563	PLA1960263		(Y,Pr)BaSrCu3O7	Y0.2Pr0.8Ba1Sr1Cu3O6.95	Y	0.2	Pr	0.8	Ba	1	Sr	1	Cu	3											O	7-z	6.95		1994																												Y123																		K					14																																																																																																Y2O3,Pr6O11,BaCO3,SrCo3,CuO	1	mixture-fire(1203-1223K,24H in air)-press to bar -SIN(1243-1253K,24H in flowing O2-ANN(773K,24H)cool to RT (1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5564	PHC2410191		La(Ba,Sr)2Cu3O7	La1.5Ba1.5Sr1.5Cu3Oz	La	1.5	Ba	1.5	Sr	1.5	Cu	3													O	z			1995																											2	Y123			A															K		18					18																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5565	PHC2410191		La(Ba,Sr)2Cu3O7	La1.5Ba1.3Sr0.2Cu3Oz	La	1.5	Ba	1.3	Sr	0.2	Cu	3													O	z			1995																											2	Y123			A	3.909		11.759												K		31.8					31.8																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5566	PHC2410191		La(Ba,Sr)2Cu3O7	La1.5Ba1.2Sr0.3Cu3Oz	La	1.5	Ba	1.2	Sr	0.3	Cu	3													O	z			1995																											2	Y123			A	3.911		11.759												K		38					38																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5567	PHC2410191		La(Ba,Sr)2Cu3O7	La1.5Ba1.1Sr0.4Cu3Oz	La	1.5	Ba	1.1	Sr	0.4	Cu	3													O	z			1995																											2	Y123			A	3.91		11.759												K		35					35																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5568	PHC2410191		La(Ba,Sr)2Cu3O7	La1.5Ba1Sr0.5Cu3O6.955	La	1.5	Ba	1	Sr	0.5	Cu	3													O	z	6.955		1995																											2	Y123			A	3.907		11.741												K		26.9					26.9																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5569	PHC2410191		La(Ba,Sr)2Cu3O7	La1.1Ba1.7Sr0.2Cu3Oz	La	1.1	Ba	1.7	Sr	0.2	Cu	3													O	z			1995																											2	Y123			A	3.921		11.786												K		54.3					54.3																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5570	PHC2410191		La(Ba,Sr)2Cu3O7	La1.1Ba1.6Sr0.3Cu3Oz	La	1.1	Ba	1.6	Sr	0.3	Cu	3													O	z			1995																											2	Y123			A	3.914		11.764												K		63.1					63.1																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5571	PHC2410191		La(Ba,Sr)2Cu3O7	La1.1Ba1.5Sr0.4Cu3Oz	La	1.1	Ba	1.5	Sr	0.4	Cu	3													O	z			1995																											2	Y123			A	3.906		11.747												K		56.1					56.1																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5572	PHC2410191		La(Ba,Sr)2Cu3O7	La1.1Ba1.4Sr0.5Cu3O6.954	La	1.1	Ba	1.4	Sr	0.5	Cu	3													O	z	6.954		1995																											2	Y123			A	3.902		11.731												K		50.1					50.1																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5573	PHC2410191		La(Ba,Sr)2Cu3O7	La1Ba1.6Sr0.4Cu3Oz	La	1	Ba	1.6	Sr	0.4	Cu	3													O	z			1995																											2	Y123			A	3.91		11.759												K		65.3					65.3																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5574	PHC2410191		La(Ba,Sr)2Cu3O7	La1Ba1.5Sr0.5Cu3O6.948	La	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.948		1995																											2	Y123			A	3.907		11.741												K		57.1					57.1																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5575	PHC2410191		La(Ba,Sr)2Cu3O7	La1.2Ba1.8SrCu3Oz	La	1.2	Ba	1.8	Sr		Cu	3													O	z			1995																											2	Y123			A	3.926		11.793												K		44					44																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5576	PHC2410191		La(Ba,Sr)2Cu3O7	La1.2Ba1.6Sr0.2Cu3Oz	La	1.2	Ba	1.6	Sr	0.2	Cu	3													O	z			1995																											2	Y123			A	3.916		11.767												K		47.9					47.9																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5577	PHC2410191		La(Ba,Sr)2Cu3O7	La1.2Ba1.5Sr0.3Cu3Oz	La	1.2	Ba	1.5	Sr	0.3	Cu	3													O	z			1995																											2	Y123			A	3.91		11.748												K		55.2					55.2																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5578	PHC2410191		La(Ba,Sr)2Cu3O7	La1.2Ba1.4Sr0.4Cu3Oz	La	1.2	Ba	1.4	Sr	0.4	Cu	3													O	z			1995																											2	Y123			A	3.903		11.734												K		52					52																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5579	PHC2410191		La(Ba,Sr)2Cu3O7	La1.2Ba1.3Sr0.5Cu3O6.943	La	1.2	Ba	1.3	Sr	0.5	Cu	3													O	z	6.943		1995																											2	Y123			A	3.899		11.722												K		45.1					45.1																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5580	PHC2410191		La(Ba,Sr)2Cu3O7	La1.3Ba1.7SrCu3O6.885	La	1.3	Ba	1.7	Sr		Cu	3													O	z	6.885		1995																											2	Y123			A	3.921		11.773												K		32					32																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5581	PHC2410191		La(Ba,Sr)2Cu3O7	La1.3Ba1.5Sr0.2Cu3O6.901	La	1.3	Ba	1.5	Sr	0.2	Cu	3													O	z	6.901		1995																											2	Y123			A	3.911		11.746												K		43.8					43.8																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5582	PHC2410191		La(Ba,Sr)2Cu3O7	La1.3Ba1.4Sr0.3Cu3O6.91	La	1.3	Ba	1.4	Sr	0.3	Cu	3													O	z	6.91		1995																											2	Y123			A	3.906		11.734												K		50					50																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5583	PHC2410191		La(Ba,Sr)2Cu3O7	La1.3Ba1.3Sr0.4Cu3O6.928	La	1.3	Ba	1.3	Sr	0.4	Cu	3													O	z	6.928		1995																											2	Y123			A	3.9		11.722												K		45.2					45.2																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5584	PHC2410191		La(Ba,Sr)2Cu3O7	La1.3Ba1.2Sr0.5Cu3O6.955	La	1.3	Ba	1.2	Sr	0.5	Cu	3													O	z	6.955		1995																											2	Y123			A	3.895		11.709												K		38					38																																																																																														La2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(930-980C)-reground-SIN-ANN(400C,in flowing Oz)-slow cool to RT					Superconducting La1.5-xBa1.5+x-ySryCu3Ozsolid solutions.Stoichiometry,structure and properties	199501		Department of Chemistry,University of Aberdeen,Meston walk,Aberdeen AB9 2UE,Scotland,UK	Physica C.,241(1995)191-197	A.R.West,J.M.S.Skakle	La,Ba,Sr,Cu,O	
5585	PHC2420012		(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl1HgSr2Ba2Cu2Co3Oz	Tl	1	Hg		Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											3	Tl1222			A	3.843	3.879	16.95												K		70.3					70.3																																																																																														Tl2O3,HgO,Ba2CuO3,BaO,Sr2CuO2(CO3)		pellet-sealed in evacuated quartz-fire(800C,5H)-Q toRT					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5586	PHC2420012	Tl(Sr,Ba)2CuOz impurity phase=	(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.8Hg0.2Sr2Ba2Cu2Co3Oz	Tl	0.8	Hg	0.2	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											3	Tl1222			A	3.85	3.876	16.959												K		70				10.6	70																																																																																														Tl2O3,HgO,Ba2CuO3,BaO,Sr2CuO2(CO3)		pellet-sealed in evacuated quartz-fire(800C,5H)-Q toRT					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5587	PHC2420012		(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.7Hg0.3Sr2Ba2Cu2Co3Oz	Tl	0.7	Hg	0.3	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											3	Tl1222			A	3.851	3.873	16.936												K		71					71																																																																																														Tl2O3,HgO,Ba2CuO3,BaO,Sr2CuO2(CO3)		pellet-sealed in evacuated quartz-fire(800C,5H)-Q toRT					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5588	PHC2420012		(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.5Hg0.5Sr2Ba2Cu2Co3Oz	Tl	0.5	Hg	0.5	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											3	Tl1222			A	3.854	3.869	16.934												K		72.9					72.9																																																																																														Tl2O3,HgO,Ba2CuO3,BaO,Sr2CuO2(CO3)		pellet-sealed in evacuated quartz-fire(800C,5H)-Q toRT					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5589	PHC2420012		(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.3Hg0.7Sr2Ba2Cu2Co3Oz	Tl	0.3	Hg	0.7	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											2	Tl1222			A	3.872		16.921												K		73					73																																																																																														Tl2O3,HgO,Ba2CuO3,BaO,Sr2CuO2(CO3)		pellet-sealed in evacuated quartz-fire(800C,5H)-Q toRT					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5590	PHC2420012	impurity phase=(Sr,Ba)2CuO2(CO3)	(Tl,,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.2Hg0.8Sr2Ba2Cu2Co3Oz	Tl	0.2	Hg	0.8	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											2	Tl1222			A	3.883														K		60				10.5	60																																																																																																					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5591	PHC2420012	impurity phase=(Sr,Ba)2CuO2(CO3)	(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl0.1Hg0.9Sr2Ba2Cu2Co3Oz	Tl	0.1	Hg	0.9	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											2	Tl1222			A	3.879		16.929												K		66					66																																																																																																					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5592	PHC2420012		(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl1Hg1Sr2Ba2Cu2Co3Oz	Tl	1	Hg	1	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																											2	Tl1222			A	3.883		16.928												K		57.3					57.3																																																																																																					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5593	PHC2420012	ANN(400C,in O2)	(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl1Hg1Sr2Ba2Cu2Co3Oz	Tl	1	Hg	1	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																																														K		73					73																																																																																																					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5594	PHC2420012	ANN(400C,in O2)	(Tl,Hg)Sr2Ba2Cu2(CO3)Oz	Tl1Hg1Sr2Ba2Cu2Co3Oz	Tl	1	Hg	1	Sr	2	Ba	2	Cu	2	Co	3									O	z			1995																																														K		66					66																																																																																																					Synthesis of oxycarbonate solid solutions (Tl1-xHgx)Sr2Ba2Cu2(CO3)Oy(x=0-1.0)and superconductivity	199502		Department of Physics,Aoyama-Gakuin University,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,242(1995)12-16	E.Ohshima,J.Akimitsu,M.Kikuchi,M.Ogawa,T.Noda,Y.Syono		
5595	SSC0920535		(Ba,K)BiO3	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O	6			1995																											3	Bi2201			A	5.344	5.392	24.574																																																																																																																								THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5596	SSC0920535		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1995																											3	Bi2212			A	5.408	5.416	30.919																																																																																																																								THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5597	SSC0920535		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10	Bi	2	Sr	2	Ca	2	Cu	3													O	10			1995																											3	Bi2223			A	5.403	5.427	37.243																																																																																																																	Bi2O3,SrCO3,CuO,CaCO3	1	conventional solid state reaction					THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5598	SSC0920535		BaBiO3	Ba1Bi1O3	Ba	1	Bi	1																	O	3			1995																											3	ABO3			A	6.172	6.123	8.672																																																																																																																		1						THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5599	SSC0920535		Ba0.6K0.4BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1995																											1	BKBO			A	4.271																																																																																																																				1						THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5600	SSC0920535		Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			1995																											3	BPBO			A	6.069	6.041	8.543																																																																																																																	BaO,KO2,Bi2O3	1	heat(700C,1H)-heat(425C,1H in O2)					THE EFFECT OF PRESSURE ON THE CRISTAL STRUCTURES OF SOME BISMUTH BASED SUPERCONDUCTORS				Solid State Commun.,93(1995)269	C.R.A. Catlow,M.J. Akhtar,S.M. Clark,Z.N. Akhtar	Bi, Ba, K, O, Pb, Sr, Ca	
5601	PHC2420228		(Ga, Hg )Sr2( Y, Ca )Cu2 Oz	Ga0.3Hg0.7Sr2Y0.3Ca0.7Cu2OZ	Ga	0.3	Hg	0.7	Sr	2	Y	0.3	Ca	0.7	Cu	2									O	Z			1995																												Ga1212			A															K			86				86																																																																																																					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5602	PHC2420228		(Ga,Hg) Sr2 (Y,Ca) Cu2 Oz	Ga0.5Hg0.5Sr2Y0.3Ca0.7Cu2OZ	Ga	0.5	Hg	0.5	Sr	2	Y	0.3	Ca	0.7	Cu	2									O	Z			1995																											3	Ga1212			A	23.115	5.448	5.38												K	30		78				54																																																																																																precursor(Sr2(Y,Ca)Cu2Oz)-mix with Ga2O3-heat(920C,2-3H)-mix with HgO-seal in evacuated quartz-heat(910C,6H)-ANN(350C,in flowing O2)					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5603	PHC2420228		(Ga,Hg) Sr2 (Y,Ca) Cu2 Oz	Ga0.7Hg0.3Sr2Y0.3Ca0.7Cu2OZ	Ga	0.7	Hg	0.3	Sr	2	Y	0.3	Ca	0.7	Cu	2									O	Z			1995																												Ga1212			A															K	40		73				56.5																																																																																																precursor(Sr2(Y,Ca)Cu2Oz)-mix with Ga2O3-heat(920C,2-3H)-mix with HgO-seal in evacuated quartz-heat(910C,6H)-ANN(350C,in flowing O2)					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5604	PHC2420228	Tc(zero)<20K	(Ga,Hg) Sr2 (Y,Ca) Cu2 Oz	Ga0.3Hg0.7Sr2Y0.5Ca0.5Cu2OZ	Ga	0.3	Hg	0.7	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z			1995																												Ga1212			A															K			88				88																																																																																																					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5605	PHC2420228	Tc(zero)<20K	(Ga,Hg) Sr2 (Y,Ca) Cu2 Oz	Ga0.5Hg0.5Sr2Y0.5Ca0.5Cu2OZ	Ga	0.5	Hg	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z			1995																												Ga1212			A															K			86				86																																																																																																					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5606	PHC2420228		(Ga,Hg) Sr2 (Y,Ca) Cu2 Oz	Ga0.7Hg0.3Sr2Y0.5Ca0.5Cu2OZ	Ga	0.7	Hg	0.3	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	Z			1995																												Ga1212			A															K	35		75				55																																																																																																					Enhancement of T c onset in (Ga,Hg)Sr2(Y,Ca)Cu2O7 by Hg doping	199502		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)228-232	O.Chmaissem,Z.Z.Sheng	Ga,Hg,Sr,Y,Ca,Cu,O	
5607	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl1Ba4Ca2Cu4OZ	Hg	1	Tl	1	Ba	4	Ca	2	Cu	4											O	Z			1995																											2	Tl2223			A	3.85		35.85												K	106		110				108																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5608	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl1Ba4Ca4Cu6OZ	Hg	1	Tl	1	Ba	4	Ca	4	Cu	6											O	Z			1995																											2	Tl2223			A	3.85		36.1												K	119		126				122.5																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5609	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl2Ba4Ca2Cu4OZ	Hg	1	Tl	2	Ba	4	Ca	2	Cu	4											O	Z			1995																											2	Tl2212			A	3.85		29.5												K	110		125				117.5																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5610	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl2Ba4Ca4Cu6OZ	Hg	1	Tl	2	Ba	4	Ca	4	Cu	6											O	Z			1995																											2	Tl2223			A	3.86		35.86													121		123				122																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5611	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl2Ba4Ca4Cu6OZ	Hg	1	Tl	2	Ba	4	Ca	4	Cu	6											O	Z		2	1995																											2	Tl2212			A	3.86		29.6													85		130				107.5																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5612	PHC2420221		(Hg,Tl) (Ba,Sr) Ca Cu Oz	Hg1Tl1Sr4Ca2Cu4OZ	Hg	1	Tl	1	Sr	4	Ca	2	Cu	4											O	Z		2	1995																											2				A																95		110				102.5																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5613	PHC2420221		(Hg,Tl)(Ba,Sr) CA Cu Oz	Hg1Tl2Sr4Ca2Cu4OZ	Hg	1	Tl	2	Sr	4	Ca	2	Cu	4											O	Z		2	1995																											2				A	3.79		28.3													85		98				91.5																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5614	PHC2420221		(Hg,Tl)(Ba,Sr) Ca Cu Oz	Hg1Tl2Sr4Cu6OZ	Hg	1	Tl	2	Sr	4	Cu	6													O	Z		2	1995																											2				A	3.83		28.6													70		110				90																																																																																																					Superconductivity in (Hg,Tl)(Ba,Sr)CaCuOx	199502		Materials Science and Technology Division,Naval Research Laboratory,Washington,DC 20375-5000 USA	Physica C.,242(1995)221-227	A.W.Webb,B.Das,R.J.Soulen Jr,S.B.Qadri	Hg,Tl,Ba,Sr,Ca,Cu,O	
5615	PHC2420155		Y Ba2 Cu3 O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1995						0	-2.2		5.78																			Y123			A																			92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5616	PHC2420155		(Y,Gd) Ba2 Cu3 O7	Y0.8Gd0.2Ba2Cu3O7-z	Y	0.8	Gd	0.2	Ba	2	Cu	3													O	7-z			1995						8.31	-7.1																					Y123																						92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5617	PHC2420155		(Y,Gd) Ba2 Cu3 O7	Y0.6Gd0.4Ba2Cu3O7-z	Y	0.6	Gd	0.4	Ba	2	Cu	3													O	7-z			1995						8.09	-5.6																					Y123																						92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5618	PHC2420155		(Y,Gd) Ba2 Cu3 O7	Y0.4Gd0.6Ba2Cu3O7-z	Y	0.4	Gd	0.6	Ba	2	Cu	3													O	7-z			1995						8.06	-5																					Y123																						92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5619	PHC2420155		(Y,Gd) Ba2 Cu3 O7	Y0.2Gd0.8Ba2Cu3O7-z	Y	0.2	Gd	0.8	Ba	2	Cu	3													O	7-z			1995						8.15	-4.6																					Y123																						92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5620	PHC2420155		Gd Ba2 Cu3 O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			1995						7.98	-3.1		6.39																			Y123																						92			92																																																																																																					Magnetic properties of Y1-xGdxBa2Cu3O7-z Polycrystals	199502		Institut fuir Physik,Max-Planck-Institut fuir Meisenbergstr.1,Pf800665,70569 Stuttgart,Germany	Physica C.,242(1995)155-163	H.Kronmuller,H.Theuss		
5621	SUP0080329		Cd Ba2 (Ca,Y)Cu2 Oz	Cd1Ba2Ca0.7Y0.3Cu2Oz	Cd	1	Ba	2	Ca	0.7	Y	0.3	Cu	2											O	z			1995																												Cd1212			A																				70																																																																																																							Superconductivity at 103 K in CdBa2(Ca0.7Y0.3)Cu2Oy			Institute of Solid State Physics, 1784 Sofia, Gulgaria	J.Superconductivity,8(1995)329	A. Staneva,E. Gattef,J. Pirov,K. Konstantinov,N. Balchev,V. Lovchinov		
5622	SUP0080329		Cd Ba2(Ca,Y)Cu2 Oz	Cd1Ba2Ca0.7Y0.3Cu2Oz	Cd	1	Ba	2	Ca	0.7	Y	0.3	Cu	2											O	z			1995																																															72		103	103			103																																																																																																					Superconductivity at 103 K in CdBa2(Ca0.7Y0.3)Cu2Oy			Institute of Solid State Physics, 1784 Sofia, Gulgaria	J.Superconductivity,8(1995)329	A. Staneva,E. Gattef,J. Pirov,K. Konstantinov,N. Balchev,V. Lovchinov		
5623	PHC2480011		Hg0.75Nb0.25Sr2Nd1-xCaxCu2Oz	Hg0.75Nd0.25Sr2Nd1Cu2Oz	Hg	0.75	Nd	0.25	Sr	2	Nd	1	Cu	2											O	z		1	1995																											2	Hg1212	P4/mmm		A	3.852		11.966	3																																																																																																																							Superconductivity of a new series of mercury-based cuprates (Hg,M)Sr2(Nd,Ca)Cu2Oz(M=Nb,Ta)	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China,Academia Sinica;Hefei 230026, China	Physica C.,248(1995)11-14	K.-B.Tang,L.Yang,Y.-H.Zhang,Y.-T.Qian,Z.-Y.Chen		
5624	PHC2480011		Hg0.75 Nb0.25 Sr2 Nd1-x Cax Cu2 Oz	Hg0.75Nb0.25Sr2Nd0.7Ca0.3Cu2Oz	Hg	0.75	Nb	0.25	Sr	2	Nd	0.7	Ca	0.3	Cu	2									O	z		1	1995																											2	Hg1212	P4/mmm		A	3.84		11.979	3																																																																																																																							Superconductivity of a new series of mercury-based cuprates (Hg,M)Sr2(Nd,Ca)Cu2Oz(M=Nb,Ta)	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China,Academia Sinica;Hefei 230026, China	Physica C.,248(1995)11-14	K.-B.Tang,L.Yang,Y.-H.Zhang,Y.-T.Qian,Z.-Y.Chen		
5625	PHC2480011		Hg0.75 Nb0.25 Sr2 Nd1-x Cax Cu2 Oz	Hg0.75Nb0.25Sr2Nd0.6Ca0.4Cu2Oz	Hg	0.75	Nb	0.25	Sr	2	Nd	0.6	Ca	0.4	Cu	2									O	z		1	1995																											2	Hg1212	P4/mmm		A	3.839		11.988	3																																																																																																																							Superconductivity of a new series of mercury-based cuprates (Hg,M)Sr2(Nd,Ca)Cu2Oz(M=Nb,Ta)	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China,Academia Sinica;Hefei 230026, China	Physica C.,248(1995)11-14	K.-B.Tang,L.Yang,Y.-H.Zhang,Y.-T.Qian,Z.-Y.Chen		
5626	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z		1	1995																												RPr123			A	3.843	3.903	11.71	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5627	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd0.9Pr0.1Ba2Cu3O7-z	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.846	3.905	11.713	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5628	PHC2480092		(Gd,Pr)Ba2 Cu3 O7	Gd0.8Pr0.2Ba2Cu3O7-z	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.848	3.907	11.715	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5629	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd0.7Pr0.3Ba2Cu3O7-z	Gd	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.852	3.909	11.718	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5630	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd0.65Pr0.35Ba2Cu3O7-z	Gd	0.65	Pr	0.35	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.853	3.909	11.72	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5631	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd0.6Pr0.4Ba2Cu3O7-z	Gd	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.855	3.911	11.724	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5632	PHC2480092		(Gd,Pr) Ba2 Cu3 O7	Gd0.5Pr0.5Ba2Cu3O7-z	Gd	0.5	Pr	0.5	Ba	2	Cu	3													O	7-z		1	1995																												RPr123			A	3.858	3.912	11.728	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5633	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd1Ba1Sr1Cu3O7-z	Gd	1	Ba	1	Sr	1	Cu	3													O	7-z		1	1995																												RPr123			A	3.847	3.864	11.582	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5634	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.9Pr0.1Ba1Sr1Cu3O7-z	Gd	0.9	Pr	0.1	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.857		11.575	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5635	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.8Pr0.2Ba1Sr1Cu3O7-z	Gd	0.8	Pr	0.2	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.857		11.577	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5636	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.7Pr0.3Ba1Sr1Cu3O7-z	Gd	0.7	Pr	0.3	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.858		11.581	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5637	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.6Pr0.4Ba1Sr1Cu3O7-z	Gd	0.6	Pr	0.4	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.859		11.58	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5638	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.5Pr0.5Ba1Sr1Cu3O7-z	Gd	0.5	Pr	0.5	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.861		11.583	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5639	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.45Pr0.55Ba1Sr1Cu3O7-z	Gd	0.45	Pr	0.55	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.862		11.584	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5640	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 P7	Gd0.4Pr0.6Ba1Sr1Cu3O7-z	Gd	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.864		11.587	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5641	PHC2480092		(Gd,Pr)  Ba2 Cu3 O7	Gd0.55Pr0.45Ba1Cu3O7-z	Gd	0.55	Pr	0.45	Ba	1	Cu	3													O	7-z		1	1995																												RPr123			A	3.856	3.911	11.725	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5642	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.55Pr0.45Ba1.5Sr0.5Cu3O7-z	Gd	0.55	Pr	0.45	Ba	1.5	Sr	0.5	Cu	3											O	7-z		1	1995																												RPr123			A	3.854	3.885	11.633	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5643	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.55Pr0.45Ba1.25Sr0.75Cu3O7-z	Gd	0.55	Pr	0.45	Ba	1.25	Sr	0.75	Cu	3											O	7-z		1	1995																												RPr123			A	3.856	3.875	11.606	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5644	PHC2480092		(Gd,Pr)(Ba,Sr)2 Cu3 O7	Gd0.55Pr0.45Ba1Sr1Cu3O7-z	Gd	0.55	Pr	0.45	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																												RPr123			A	3.86		11.583	3																																																																																																																							The suppression of superconductivity in the Gd1-xPrxBa2-ySryCu3O7-z system	199506		Department of Applied Chemistry,University of Science and Tecnology of China,Hefei 230026,P.R.China	Physica C.,248(1995)92-96	Guanghan Cao,Hongkai Wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5645	PHC2480167		(CA,NA)2 CA Cu2 O4 Cl2	Ca1.9Na0.1Ca1Cu2Cl2O4	Ca	1.9	Na	0.1	Ca	1	Cu	2	Cl	2											O	4		1	1995																											2	2126	I4/mmm		A	3.85		21.45	3																																																																																																																							Superconductivity in (Ca,Na)2CaCu2O4Cl2 The new simplest double-layer cuprate with apical chlorine	199506		Department of Physics,Aoyama-Gakuin,University,6-16-1,Chitosedai,Setagaya-ku,Tokyo 157,Japan	Physica C.,248(1995)167-170	J.Akimitsu,K.Inari,M.Ayabe,M.Uehara,N.Kubota,S.Sahoda,Y.Zenitani		
5646	PHC2420055	isomer shift(Gd)=0.507 mm/s linewidth=0.42 mm/s at 4.2K	GD(Ba, Sr)2 Cu3 O7	Gd1Ba1Sr1Cu3O7	Gd	1	Ba	1	Sr	1	Cu	3													O	7-x	7	1	1995																											2	Y123			A	3.839		11.572													80.8			82			82																																																																							m.ohm.cm											1.97				0.0000000009				0.7	RH5646			Gd2O3,BaCO3,SrCO3,CuO	1	ANN(T>920C)-slow cooling in O2					Oxygen ordering and superconductivity in GdBaSrCu3O7-x	199502		Angewandte Physik,Johannes-Keplera-Universitat Linz,A-4040 Linz,Austria	Physica C.,242(1995)55-62	B.Hellebrand,D.Bauerle,G.Wortmann,M.Strecker,W.Lang,X.Z.Wang		
5647	PHC2420055	isomer shift=0.512 mm/s, HWHM=0.46 mm/s at 4.2K	Gd(Ba, Sr)2 Cu3 O7	Gd1Ba1Sr1Cu3O7-z	Gd	1	Ba	1	Sr	1	Cu	3													O	7-z		1	1995																											3	Y123				3.804	3.863	11.588													82.6			85			85																																																																							m.ohm.cm											0.68				0.0000000014				0.7	RH5647				1	ANN(T>920C)-slow cooling in O2-ANN(500C,in O2)					Oxygen ordering and superconductivity in GdBaSrCu3O7-x	199502		Angewandte Physik,Johannes-Keplera-Universitat Linz,A-4040 Linz,Austria	Physica C.,242(1995)55-62	B.Hellebrand,D.Bauerle,G.Wortmann,M.Strecker,W.Lang,X.Z.Wang		
5648	PHC2420023	(Hg0.7 Cr0.3) Sanple also non- superconducting	(Hg, Cr) Sr (CA, Y) Ca2 O7	Hg0.49Cr0.51Sr2Ca0.44Yo0.56Cu2O7.28	Hg	0.49	Cr	0.51	Sr	2	Ca	0.44	Yo	0.56	Cu	2									O	7.28	7.28		1995																											2	Hg1212				3.853		11.819																	10																																																																																																HgO,Cr,O3,Sr(NO3)2,Y2O3,CaO,CuO	1	mix ture of precursorand Hg-sealed in evacucted quartz tube mix ture of precursorand HgO-seald in evacucted quartz tube					New1212-type(Hg,Cr)-based cuprate (Hg1-xCrx)Sr2(Ca1-yYy)Cu2O6+z	199502		Department of Physics,and High Density Electronics Center,Unversity of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)23-29	O.Chmaissem,Z.Z.Sheng		
5649	PHC2470091	using HIP apparatus,not superconducting		Ga1.78Cu4.22Sr3.16Nd3.84O16-z	Ga	1.78	Cu	4.22	Sr	3.16	Nd	3.84													O	16-z		2	1995																											3	Ga2434				5.458	5.535	51.3																																																																																																																	Ga2O3,PbO,SrCO3,Nd2O3,CuO	1	CAL(920-1180C,15-30H,in ai)-Interrittent grindings-ANN(1000C,2H,under 20Mpa of Oxgen)-C to RT(at-10C/min)					Preparation and structure of a new layered cuprate Ga2(Sr,Nd)4Nd3Cu4)z	199505		National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba,305,Japan	Physica C.,247(1995)91-95	A.Ono,A.Watanabe,L.L.He,S.Horiuchi		
5650	PHC2470125	90%1212 phase	(Hg, Pb) Sr2 (Ca,Y) Cu2  Oz	Hg0.7Pb0.3Sr2Ca0.7Y0.3Cu2Oz	Hg	0.7	Pb	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	z		1	1995																											2	Hg1212			A	3.808		12.005															100				100																																																																																														Sr(NO3)2,Y2O3,Ca,O,CuO,HgO,PbO	1	(Precursor(Sr2Ca1-yYyCu2Oz)+HgO+PbO in dry box)-sealed in quarty tube-heat to 920C(3.5C/min)-SIN(900-920,6-8H)-ANN(300C,20H in O2)					Electrical properties and crystal structure of (Hg,Pb)Sr2(Ca,Y)Cu2O6+z	199505		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,247(1995)125-132	O.Chmaissem,Z.Z.Sheng		
5651	PHC2470125	95%1212 phase	(Hg, Pb) Sr2 (Ca, Y) Cu2 Oz	Hg0.5Pb0.5Sr2Ca0.5Y0.5Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	z		1	1995																												Hg1212			A																80		100				90																																																																																														Sr(NO3)2,Y2O3,Ca,O,CuO,HgO,PbO	1	(Precursor(Sr2Ca1-yYyCu2Oz)+HgO+PbO in dry box)-sealed in quarty tube-heat to 920C(3.5C/min)-SIN(900-920,6-8H)-ANN(300C,20H in O2)					Electrical properties and crystal structure of (Hg,Pb)Sr2(Ca,Y)Cu2O6+z	199505		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,247(1995)125-132	O.Chmaissem,Z.Z.Sheng		
5652	PHC2470125	95%1212 phase	(Hg, Pb) Sr2 (Ca, Y) Cu2 Oz	Hg0.5Pb0.5Sr2Ca0.7Y0.3Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	z		1	1995																												Hg1212																			80		100				90																																																																																														Sr(NO3)2,Y2O3,Ca,O,CuO,HgO,PbO	1	(Precursor(Sr2Ca1-yYyCu2Oz)+HgO+PbO in dry box)-sealed in quarty tube-heat to 920C(3.5C/min)-SIN(900-920,6-8H)-ANN(300C,20H in O2)					Electrical properties and crystal structure of (Hg,Pb)Sr2(Ca,Y)Cu2O6+z	199505		Department of Physics,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,247(1995)125-132	O.Chmaissem,Z.Z.Sheng		
5653	PHC2470062	Semiconducter like, not Superconducter	(Ca O) (Ba Ti O3)2 (Gd,Ce)3 Cu2 O7	Ti2Ba2Ca1Gd2.25Ce0.75Cu2O14	Ti	2	Ba	2	Ca	1	Gd	2.25	Ce	0.75	Cu	2									O	14		1	1995																											2	Ti2322			A	3.884		20.463																	15																																																																									m.ohm.cm				270							70												TiO2,BaCO3,CaCO3,Gd2O3,CeO2,CuO	1	Mxture-CAL(950C,24H, in air)-ground-CAL(1000C,24H, in air)-FC-grand-Pellet-SIN(1050C,48H, in air)-FC-SIN(1050C,72H,in air or  flowing O2)-step cooling					Design and synthesis of a new layered cuprate Ti2Ba2Ca(Gd,Ce)3Cu2O14	199505		Department of Applied Chemistry,University of Science and Technology of China,Hefei,Anhui 230026,P.R.China	Physica C.,247(1995)62-66	Dong Chen,Li Rukang,Yang Li		
5654	PHC2420216		(Hg,Mo) Sr2 (Y,Ca) Cu2 O6	Hg0.8Mo0.2Sr2Y0.6Ca0.4Ca2O6+z	Hg	0.8	Mo	0.2	Sr	2	Y	0.6	Ca	0.4	Ca	2									O	6+z		1	1995																																3.827		11.888													55		94				74.5																																																																																														MoO3,Sr(NO3)2,Y2O3,CaCO3,CuO,HgO		Precursor(Mo-Sr-Y-Ca-Cu-O)+HgO-Prees into pellet  -seald in quartz tube-heat to  850C(3C/min)-hold(10H)-					(Hg,Mo)Sr2Y1-xCaxCu2O6+z A new series of mercury-based high-Tc superconductor	199502		Department of Applied Chemistry,University of Science and Technology of China.Structure Reseach Laboratory,University of Science and Technology of China,Academia Sinica,Hefei,Anhui 230026,P.R.China	Physica C.,242(1995)216-220	Kaibin Tang,Li Yang,Liangbin Wang,Yitai Qian,Yuheng Zhang,Zuyao Chen	Hg,MO,Sr,Y,Ca,Cu,O	
5655	PHC2420216		(Hg,Mo) Sr2 (Y,Ca) Cu2 O6	Hg0.8Mo0.2Sr2Y0.5Ca0.5Ca2O6+z	Hg	0.8	Mo	0.2	Sr	2	Y	0.5	Ca	0.5	Ca	2									O	6+z		1	1995																																3.825		11.912													54		93				73.5																																																																																														MoO3,Sr(NO3)2,Y2O3,CaCO3,CuO,HgO		Precursor(Mo-Sr-Y-Ca-Cu-O)+HgO-Prees into pellet  -seald in quartz tube-heat to  850C(3C/min)-hold(10H)-					(Hg,Mo)Sr2Y1-xCaxCu2O6+z A new series of mercury-based high-Tc superconductor	199502		Department of Applied Chemistry,University of Science and Technology of China.Structure Reseach Laboratory,University of Science and Technology of China,Academia Sinica,Hefei,Anhui 230026,P.R.China	Physica C.,242(1995)216-220	Kaibin Tang,Li Yang,Liangbin Wang,Yitai Qian,Yuheng Zhang,Zuyao Chen	Hg,MO,Sr,Y,Ca,Cu,O	
5656	PHC2420216		(Hg,Mo) Sr2 (Y,Ca) Cu2 O6	Hg0.8Mo0.2Sr2Y0.35Ca0.65Ca2O6+z	Hg	0.8	Mo	0.2	Sr	2	Y	0.35	Ca	0.65	Ca	2									O	6+z		1	1995																																3.82		11.93													75		96				85.5																																																																																																					(Hg,Mo)Sr2Y1-xCaxCu2O6+z A new series of mercury-based high-Tc superconductor	199502		Department of Applied Chemistry,University of Science and Technology of China.Structure Reseach Laboratory,University of Science and Technology of China,Academia Sinica,Hefei,Anhui 230026,P.R.China	Physica C.,242(1995)216-220	Kaibin Tang,Li Yang,Liangbin Wang,Yitai Qian,Yuheng Zhang,Zuyao Chen	Hg,MO,Sr,Y,Ca,Cu,O	
5657	PHC2450301		(Bi,Pb,Cu) Sr2 (Dy,Ca) Cu2 O	Bi0.3Pb0.5Cu0.2Sr2Dy0.75Ca0.25Cu2Oz	Bi	0.3	Pb	0.5	Cu	0.2	Sr	2	Dy	0.75	Ca	0.25	Cu	2							O	z			1995																											2	Pb1212																				80					80																																																																																														Bi2O3,Dy2O3,Pbo,CuO,SrCO3,CaCO3	1	Mixture-CAL(900C,16H+920C,24H)-pellet-SIN(940C,20H)-Q to cold Cu plate-ANN(600C 48H in flowing N)					Preparation and superconductivity of (Bi,Pb,Cu)Sr2(RE,Ca)CuOd ceramics	199504		Max-Planck-Institut fur Metallforschung,Pulvermetallurgisches Laboratorium,Heisenbergstr.5,D-70569 Stuttgart,Germany	Physica C.,245(1995)301-307	F.Aldinger,M.Ritschel,P.Majewski		
5658	PHC2450301		(Bi,Pb,Cu) Sr2 (Dy,Ca) Cu2 O	Bi0.3Pb0.5Cu0.2Sr2Dy0.5Ca0.5Oz	Bi	0.3	Pb	0.5	Cu	0.2	Sr	2	Dy	0.5	Ca	0.5									O	z			1995																											2	Pb1212																				80					80																																																																																														Bi2O3,Dy2O3,Pbo,CuO,SrCO3,CaCO3	1	Mixture-CAL(900C,16H+920C,24H)-pellet-SIN(940C,20H)-Q to cold Cu plate-ANN(600C 48H in flowing N)					Preparation and superconductivity of (Bi,Pb,Cu)Sr2(RE,Ca)CuOd ceramics	199504		Max-Planck-Institut fur Metallforschung,Pulvermetallurgisches Laboratorium,Heisenbergstr.5,D-70569 Stuttgart,Germany	Physica C.,245(1995)301-307	F.Aldinger,M.Ritschel,P.Majewski		
5659	PHC2490139	Optimally doped	Bi2 Sr2 Ca Cu2 O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																				86.1					86.1																																																																						TP5659																										using floating qone(infra-red image furnace)					Thermoelectric power and the hole concentration in indine-intercalated Bi2Sr2CaCu2Ox crystals	199506		Department of Physics,Victoria University of Wellington,PO.Box 600,Wellington,New Zealand	Physica C.,249(1995)139-143	C.K.Subramaniam,D.Pooke,H.J.Trodahl,K.Kishio		
5660	PHC2490139	Optimally doped	I Bi2 Sr2 Ca Cu2 O8	I1Bi2Sr2Ca1Cu2O8	I	1	Bi	2	Sr	2	Ca	1	Cu	2											O	8		3	1995																												Bi2212																				58.3					58.3																																																																						TP5660																										single cristal (floating qone)-seal in glass anpoule (excess I)-ANN (180C,1week)					Thermoelectric power and the hole concentration in indine-intercalated Bi2Sr2CaCu2Ox crystals	199506		Department of Physics,Victoria University of Wellington,PO.Box 600,Wellington,New Zealand	Physica C.,249(1995)139-143	C.K.Subramaniam,D.Pooke,H.J.Trodahl,K.Kishio		
5661	PHC2490139	under doped	Bi2 Sr2 Ca Cu2 O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																				72.2					72.2																																																																						TP5661																										using floating qone(infra-red image furnace)					Thermoelectric power and the hole concentration in indine-intercalated Bi2Sr2CaCu2Ox crystals	199506		Department of Physics,Victoria University of Wellington,PO.Box 600,Wellington,New Zealand	Physica C.,249(1995)139-143	C.K.Subramaniam,D.Pooke,H.J.Trodahl,K.Kishio		
5662	PHC2490139	under doped	I Bi2 Sr2 Ca Cu2 O8	I1Bi2Sr2Ca1Cu2O8	I	1	Bi	2	Sr	2	Ca	1	Cu	2											O	8		3	1995																												Bi2212																				72.2					72.2																																																																						TP5662																										single cristal (floating qone)-seal in glass anpoule (excess I)-ANN (180C,1week)					Thermoelectric power and the hole concentration in indine-intercalated Bi2Sr2CaCu2Ox crystals	199506		Department of Physics,Victoria University of Wellington,PO.Box 600,Wellington,New Zealand	Physica C.,249(1995)139-143	C.K.Subramaniam,D.Pooke,H.J.Trodahl,K.Kishio		
5663	PHC2490196	Semi-con	Pb(Sr,La)2 Gd2 Cu2 Oz	Pb1Sr1.2La0.8Gd2Cu2Oz	Pb	1	Sr	1.2	La	0.8	Gd	2	Cu	2											O	z			1995																											2	Pb1222			A	3.843		29.119																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5664	PHC2490196	semi-con	Pb(Sr,La)2 Dy2 Cu2 Oz	Pb1Sr14La0.6Dy2Cu2Oz	Pb	1	Sr	14	La	0.6	Dy	2	Cu	2											O	z			1995																											2	Pb1222			A	3.825		29.119																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5665	PHC2490196	Semi-con	Pb(Sr,La)2 Eu2 Cu2 Oz	Pb1Sr1La1Eu2Cu2Oz	Pb	1	Sr	1	La	1	Eu	2	Cu	2											O	z			1995																											2	Pb1222			A	3.859		29.203																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5666	PHC2490196		Pb(Sr,La)2 Pr2 Cu2 Oz	Pb1Sr1.6La0.4Pr2Cu2Oz	Pb	1	Sr	1.6	La	0.4	Pr	2	Cu	2											O	z			1995																											2	Pb1222				3.873		29.194																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5667	PHC2490196		(Pb,Cd)(Sr,La)2 Gd2 Cu2 Oz	Pb0.5Cd0.5Sr1.2La0.8Gd2Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.2	La	0.8	Gd	2	Cu	2									O	z			1995																											2	Pb1222				3.842		29.29																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5668	PHC2490196	anneal (920,in O2)	(Pb,Cd)(Sr,La)2 Gd2 Cu2 Oz	Pb0.5Cd0.5Sr1.2La0.8Gd2Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.2	La	0.8	Gd	2	Cu	2									O	z			1995																											2	Pb1222				3.836		29.274																	4.2																																																																																																PbO,SrCO3,Ln2O3,CuO	1	mixtuo-cal(850C,overnight,in air)-pellet-SIN(900-970C,20H in air)-FC to RT					A new family of Pb-based 1222 cuprates Pb(Sr,La)2Ln2Cu2Oz(Ln=Gd,Dy,Eu, and Pr)	199506		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,249(1995)196-201	C.Dong,C.Wang,G.H.Rao,H.Chen,H.Jin,J.K.Liang,J.R.Min,Y.D.Yu		
5669	PHC2450281	annealing(970C,2H in O2),inprity phase=Sr Cu O2,Sr2 Cu O3,CdO	(Pb,Cd) Sr2 (Y,Ca) Cu2 O7	Pb0.5Cd0.5Sr2Y0.5Ca0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7			1995																												Pb1212				3.817		11.966													51		76				63.5																																																																																														PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	mixture-CAL(850C,15H in air)-pellet-SIN(910C,10H in air)					Synthesis and superconducting properties of (Pb0.5Cd0.5)Sr2(Y0.5Ca0.5)Cu2O7	199504		Institutr of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,245(1995)281-286	C.Dong,C.Wang,G.H.Rao,J.K.Chen,J.R.Min,X.R.Cheng,Y.D.Yu		
5670	PHC2450281	annealing(970C,2H, in air),inprity phase=Sr Cu O2,Sr2 Cu O3,Cd O	(Pb,Cd) Sr2 (Y,Ca) Cu2 O7	Pb0.5Cd0.5Sr2Y0.5Ca0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7			1995																											2	Pb1212																			12		32				22																																																																																														PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	mixture-CAL(850C,15H in air)-pellet-SIN(910C,10H in air)					Synthesis and superconducting properties of (Pb0.5Cd0.5)Sr2(Y0.5Ca0.5)Cu2O7	199504		Institutr of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,245(1995)281-286	C.Dong,C.Wang,G.H.Rao,J.K.Chen,J.R.Min,X.R.Cheng,Y.D.Yu		
5671	PHC2450281	annerling(970C,2H in N2),inprity phase=Sr Cu O2,Sr2 Cu O3,Cd O	(Pb,Cd) Sr2 (Y,Ca) Cu2 O7	Pb0.5Cd0.5Sr2Y0.5Ca0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7			1995																											2	Pb1212																		K	58		83				70.5																																																																																														PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	mixture-CAL(850C,15H in air)-pellet-SIN(910C,10H in air)					Synthesis and superconducting properties of (Pb0.5Cd0.5)Sr2(Y0.5Ca0.5)Cu2O7	199504		Institutr of Physics,Chinese Academy of Sciences,Beijing 100080,China	Physica C.,245(1995)281-286	C.Dong,C.Wang,G.H.Rao,J.K.Chen,J.R.Min,X.R.Cheng,Y.D.Yu		
5672	PHC2490293		La2(Sr,Ca)Cu2 O6	La1.9Sr1.1Cu2O6.311	La	1.9	Sr	1.1	Cu	2															O	6+z	6.311		1995																												2126				3.853		20.036																	4.2																																																																																				2.889												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5673	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr1Ca0.1Cu2O6.242	La	1.9	Sr	1	Ca	0.1	Cu	2													O	6+z	6.242		1995																												2126				3.853		19.96																	4.2																																																																																				5.859												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5674	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.9Ca0.2Cu2O6.202	La	1.9	Sr	0.9	Ca	0.2	Cu	2													O	6+z	6.202		1995																												2126				3.851		19.892																	4.2																																																																																				8.695												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5675	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.8Ca0.3Cu2O6.122	La	1.9	Sr	0.8	Ca	0.3	Cu	2													O	6+z	6.122		1995																												2126				3.848		19.82																	4.2																																																																																				7.75												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5676	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.7Ca0.4Cu2O6.091	La	1.9	Sr	0.7	Ca	0.4	Cu	2													O	6+z	6.091		1995																												2126				3.845		19.764																	4.2																																																																																				9.441												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5677	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.6Ca0.5Cu2O6.062	La	1.9	Sr	0.6	Ca	0.5	Cu	2													O	6+z	6.062		1995																												2126				3.842		19.72																	4.2																																																																																				23.33												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5678	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.5Ca0.6Cu0.6O6.055	La	1.9	Sr	0.5	Ca	0.6	Cu	0.6													O	6+z	6.055		1995																												2126				3.838		19.66																																																																																																					28.42												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5679	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.4Ca0.7Cu2O6.042	La	1.9	Sr	0.4	Ca	0.7	Cu	2													O	6+z	6.042		1995																												2126				3.854		19.608																																																																																																					24.11												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5680	PHC2490293		La2(Sr,Ca)Cu2 O6	La1.9Sr0.3Ca0.8Cu2O6.04	La	1.9	Sr	0.3	Ca	0.8	Cu	2													O	6+z	6.04		1995																												2126				3.832		19.56																																																																																																					23.33												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5681	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.2Ca0.9Cu2O6.029	La	1.9	Sr	0.2	Ca	0.9	Cu	2													O	6+z	6.029		1995																												2126				3.829		19.508																																																																																																					24.51												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5682	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Sr0.1Ca1Cu2O6.02	La	1.9	Sr	0.1	Ca	1	Cu	2													O	6+z	6.02		1995																												2126				3.827		19.448																																																																																																					18.23												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5683	PHC2490293		La2(Sr,Ca)Cu2O6	La1.9Ca1.1Cu2O6+z	La	1.9	Ca	1.1	Cu	2															O	6+z			1995																												2126				3.824		19.396																																																																																																					16.79												La2O3,SrCO3,CaCO3,CuO		mixture-CAL(1000-1070C,12H in latm O2)-pellet-SIN(1070C,12H,in O2 flow)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5684	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr1.1Cu2O6.11	Pr	1.9	Sr	1.1	Cu	2															O	6+z	6.11		1995	emu/mol	0.000597	emu.K/mol	1.37	myu-B/Pr	3.31	-31.7																									3.84		19.728																																																																																																					84.14												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5685	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr1Ca0.1Cu2O6.078	Pr	1.9	Sr	1	Ca	0.1	Cu	2													O	6+z	6.078		1995																																3.84		19.652																																																																																																					86.95												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5686	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr0.9Ca0.2Cu2O6.061	Pr	1.9	Sr	0.9	Ca	0.2	Cu	2													O	6+z	6.061		1995	emu/mol	0.000605	emu.K/mol	1.34	myu-B/Pr	3.27	-31.4																									3.839		19.58																																																																																																					53.09												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5687	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr0.8Ca0.3Cu2O6.052	Pr	1.9	Sr	0.8	Ca	0.3	Cu	2													O	6+z	6.052		1995																																3.836		19.524																																																																																																					48.1												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5688	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr0.7Ca0.4Cu2O6.034	Pr	1.9	Sr	0.7	Ca	0.4	Cu	2													O	6+z	6.034		1995	emu/mol	0.000605	emu.K/mol	1.34	myu-B/Pr	3.26	-29.1																									3.834		19.476																																																																																																					44.3												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5689	PHC2490293		Pr2(Sr,Ca)Cu2O6	Pr1.9Sr0.6Ca0.5Cu2O6.023	Pr	1.9	Sr	0.6	Ca	0.5	Cu	2													O	6+z	6.023		1995																																3.832		19.42																																																																																																					42.87												Pr6O11,SrCO3,CaCO3,CuO		mixtwo-CAL(1000-1070C,12H in O2 flow)-pellet-SIN(1050C,12H in air)					Structural and electrical changes in Ln1.9Sr1.1-xCaxCu2O6+z(Ln=La,Pr)systems	199507		Depertment of Inorganic Materials,Faculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro,Tokyo,152 Japan	Physica C.,249(1995)293-303	Fujio Izumi,Hiroyuki Ikawa,Junzo Tanaka,Naoki Ohashi,Osamu Fukunaga,Takashi Ohyama		
5691	PHC2490220	(100)-collapsed Sr2CuO2(CO3)-1201 phase, as-synthesized	TlBa2Sr2Cu2(CO3)O7	Tl1Ba2Sr2Cu2C1O10	Tl	1	Ba	2	Sr	2	Cu	2	C	1											O	10			1995																																																		61			61																																																																																														Tl2O3,Cr2O3,V2O5,CuO,Sr-oxide	1	mixture-press into pellet-sealed in evacuated silica ampoule-heat(850c,12H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5692	PHC2490220	(100)-collapsed Sr2CuO2(CO3)-1201 phase, as-synthesized	(Tl,Cr)Sr4Cu2(CO3)O7	Tl0.67Cr0.33Sr4Cu2C1O10	Tl	0.67	Cr	0.33	Sr	4	Cu	2	C	1											O	10			1995																													I 222			5.418	27.108	16.668														77		72			77																																																																																														Tl2O3,Cr2O3,V2O5,CuO,Sr-oxide	1	mixture-press into pellet-sealed in evacuated silica ampoule-heat(850c,12H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5693	PHC2490220		(Tl,V)Sr4Cu2(CO3)O7	Tl0.8V0.2Sr4Cu2C1O10	Tl	0.8	V	0.2	Sr	4	Cu	2	C	1											O	10			1995																											3		I222	23		5.401	27.076	16.628														50		54			50										90																																																																																				Tl2O3,Cr2O3,V2O5,CuO,Sr-oxide	1	mixture-press into pellet-sealed in evacuated silica ampoule-heat(850c,12H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5694	PHC2490220		(Tl,Pb)Sr4Cu2(CO3)O7	Tl0.5Pb0.5Sr4Cu2C1O10	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C1												O	10			1995																																																		71			71																																																																																														Tl2O3,Cr2O3,V2O5,CuO,Sr-oxide	1	mixture-press into pellet-sealed in evacuated silica ampoule-heat(850c,12H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5695	PHC2490220	as-synthesized	(Hg,V)Sr4Cu2(CO3)O6	Hg0.6V0.4Sr4Cu2C1O9+z	Hg	0.6	V	0.4	Sr	4	Cu	2	C1												O	9+z			1995																											2		P4/mmm	123		3.85		16.24														76		76			76										55																																																																																				HgO,V2O5,CuO,SrO2		mixture-pellet-heat(850c,20H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5696	PHC2490220	as-synthesized	(Hg,Mo)Sr4Cu2(CO3)O6	Hg0.5Mo0.5Sr4Cu2C1O9+z	Hg	0.5	Mo	0.5	Sr	4	Cu	2	C	1											O	9+z			1995																																														K				74			74										45																																																																																				HgO,V2O5,CuO,SrO2		mixture-pellet-heat(850c,20H)-Q to RT					Stabilisation of three new oxycarbonates by V and Cr substitutions The superconductors(Tl,M)1Sr4Cu2(CO3)O7(M=Cr,V) and (Hg,V)1Sr4Cu2(CO3)O6+z	199507		Laboratoire CRISMAT,URA 1318 associee au CNRS,ISMRA et Universite de Caen,Bd du Marechal Juin 14050,Caen cedex,France	Physica C.,249(1995)220-233	A.Maignan,B. Raveau,B.Raveau,C. Michel,C.Michel,D. Pelloquin,D.Pelloquin,M. Hervieu,M.Hervieu,S. Malo,S.Malo		
5697	PHC2420342			La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1995																											2	T			A	3.776		13.247													33			28			28																																																																																														La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5698	PHC2420342			La1.65Sm0.15Sr0.2Cu1O4	La	1.65	Sm	0.15	Sr	0.2	Cu	1													O	4		1	1995																											2	T				3.775		13.217													25			24			24																																																																																														La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5699	PHC2420342			La1.5Sm0.3Sr0.2Cu1O4	La	1.5	Sm	0.3	Sr	0.2	Cu	1													O	4		1	1995																											2	T				3.77		13.153													17			17			17																																																																																														La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5700	PHC2420342	two phases T+T		La1.35Sm0.45Sr0.2Cu1O4	La	1.35	Sm	0.45	Sr	0.2	Cu	1													O	4		2	1995																																															4			12			12																																																																																														La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5701	PHC2420342			La1Sm0.8Sr0.2Cu1O4	La	1	Sm	0.8	Sr	0.2	Cu	1													O	4			1995																											2	T				3.878		12.583																	4																																																																																																La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5702	PHC2420342			La1Sm0.8Sr0.2Cu1O4	La	1	Sm	0.8	Sr	0.2	Cu	1													O	4			1995																											2					3.873		12.605													35			35			35																																																																																														La2O3,Sm2O3,SrCO3,CuO		mixture-heat(950C,24H in air in almina boat)-pellet-heat(1150C,2days in flowing O2)					Structural and superconducting properties of the La1.8-xSmxSr0.2CuO4 system (0 x 1)	199502		Laboratoire de Chimie du Solide du CNRS,Universite Bordeaux I,351 cours de la Liberation,F-33405 Talence Cedex,France	Physica C.,242(1995)342-350	A.Tressaud,B.Chevalier,E.Ben Salem,F.Weill,J.Etourneau,P.Gravereau	La,Sm,Sr,Cu,O	
5703	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.98Fe0.02O8	Y	1	Ba	2	Cu	3.98	Fe	0.02													O	8			1995																											3	Y124				3.839	3.861	27.184													59		82				70.5																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5704	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O	8			1995																											3	Y124				3.847	3.86	27.132													48.5		81				64.75																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5705	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.92Fe0.08O8	Y	1	Ba	2	Cu	3.92	Fe	0.08													O	8			1995																											3	Y124				3.85	3.86	27.104													41		80				60.5																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5706	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.88Fe0.12O8	Y	1	Ba	2	Cu	3.88	Fe	0.12													O	8			1995	emu/mol	0.00043			myu-B/mol	5.63	-5.39																				2	Y124				3.855		27.079													19.1		77				48.05																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5707	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8	Y	1	Ba	2	Cu	3.84	Fe	0.16													O	8			1995																											2	Y124				3.855		27.08													11.6		70				40.8																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5708	PHC2420373		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.8Fe0.2O8	Y	1	Ba	2	Cu	3.8	Fe	0.2													O	8			1995																											2	Y124				3.855		27.08															64				64																																																																																														Y2O3,Ba(NO3)2,CuO,Fe2O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5709	PHC2420373		YBa2(Cu,Co)4O8	Y1Ba2Cu3.98Co0.02O8	Y	1	Ba	2	Cu	3.98	Co	0.02													O	8			1995																											3	Y124				3.845	3.86	37.193													66.6		80				73.3																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5710	PHC2420373		YBa2(Cu,Co)4O8	Y1Ba2Cu3.96Co0.04O8	Y	1	Ba	2	Cu	3.96	Co	0.04													O	8			1995																											3	Y124				3.847	3.858	27.158													59		78				68.5																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5711	PHC2420373		YBa2(Cu,Co)4 O8	Y1Ba2Cu3.92Co0.08O8	Y	1	Ba	2	Cu	3.92	Co	0.08													O	8			1995																											3	Y124				3.85	3.857	27.125													55.5		72				63.75																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5712	PHC2420373		YBa2(Cu,Co)4 O8	Y1Ba2Cu3.88Co0.12O8	Y	1	Ba	2	Cu	3.88	Co	0.12													O	8			1995	emu/mole	0.0006			myu-B/mol	3.91	3.36																				2	Y124				3.856		27.109													48		68				58																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5713	PHC2420373		YBa2(Cu,Co)4 O8	Y1Ba2Cu3.84Co0.16O8	Y	1	Ba	2	Cu	3.84	Co	0.16													O	8			1995																											2	Y124				3.858		27.098													43.6		65				54.3																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5714	PHC2420373		YBa2(Cu,Co)4 O8	Y1Ba2Cu3.8Co0.2O8	Y	1	Ba	2	Cu	3.8	Co	0.2													O	8			1995																											2	Y124				3.86		27.09													37		63				50																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5715	PHC2420373		YBa2(Cu,Co)4 O8	Y1Ba2Cu1O8	Y	1	Ba	2	Cu	1															O	8			1995																											3	Y124				3.842	3.861	27.207													79		90				84.5																																																																																														Y2O3,Ba(NO3)2,CuO,Co2O3		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in Flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5716	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.98Ni0.02O8	Y	1	Ba	2	Cu	3.98	Ni	0.02													O	8			1995																											3	Y124				3.844	3.862	27.202													62.1		80				71.05																																																																																														Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5717	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8			1995																											3	Y124				3.848	3.864	27.196													52.4		75				63.7																																																																																														Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5718	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8			1995																											3	Y124				3.851	3.865	27.192													31.5		67				49.25																																																																																														Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5719	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.88Ni0.12O8	Y	1	Ba	2	Cu	3.88	Ni	0.12													O	8			1995	emu/mole	0.00045			myu-B/mol	3.37	-3.4																				3	Y124				3.855	3.866	27.187															50				50																																																																																														Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5720	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.84Ni0.16O8	Y	1	Ba	2	Cu	3.84	Ni	0.16													O	8			1995																											3	Y124				3.859	3.867	27.182																	10																																																																																																Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5721	PHC2420373		YBa2(Cu,Ni)4 O8	Y1Ba2Cu3.8Ni0.2O8	Y	1	Ba	2	Cu	3.8	Ni	0.2													O	8			1995																											3	Y124				3.862	3.868	27.181																	10																																																																																																Y2O3,Ba(NO3)2,CuO,NiO		mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5722	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O	8			1995																											3	Y124				3.841	3.861	27.2													58.1		77				67.55																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5723	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O	8			1995																											3	Y124				3.845	3.862	27.195													45.5		67				56.25																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5724	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.92Zn0.08O8	Y	1	Ba	2	Cu	3.92	Zn	0.08													O	8			1995																											3	Y124				3.847	3.862	27.191													37		61				49																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5725	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.88Zn0.12O8	Y	1	Ba	2	Cu	3.88	Zn	0.12													O	8			1995																											3	Y124				3.848	3.863	27.185													27		42				34.5																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5726	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.84Zn0.16O8	Y	1	Ba	2	Cu	3.84	Zn	0.16													O	8			1995																											3	Y124				3.852	3.864	27.185													21		42				31.5																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5727	PHC2420373		YBa2(Cu,Zn)4 O8	Y1Ba2Cu3.8Zn0.2O8	Y	1	Ba	2	Cu	3.8	Zn	0.2													O	8			1995																											3	Y124				3.857	3.865	27.186													19		42				30.5																																																																																														Y2O3,Ba(NO3)2CuO,ZnO	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5728	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.98Ga0.02O8	Y	1	Ba	2	Cu	3.98	Ga	0.02													O	8			1995																											3	Y124				3.844	3.86	27.197													70.5		85				77.75																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5729	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.96Ga0.04O8	Y	1	Ba	2	Cu	3.96	Ga	0.04													O	8			1995																											3	Y124				3.848	3.859	27.172													70		85				77.5																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5730	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.92Ga0.08O8	Y	1	Ba	2	Cu	3.92	Ga	0.08													O	8			1995																											3	Y124				3.85	3.858	27.152													66		83				74.5																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5731	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.88Ga0.12O8	Y	1	Ba	2	Cu	3.88	Ga	0.12													O	8			1995																											3	Y124				3.855	3.857	27.129													65		82				73.5																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5732	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.84Ga0.16O8	Y	1	Ba	2	Cu	3.84	Ga	0.16													O	8			1995																											2	Y124				3.856		27.12													61.5		81				71.25																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5733	PHC2420373		YBa2(Cu,Ga)4 O8	Y1Ba2Cu3.8Ga0.2O8	Y	1	Ba	2	Cu	3.8	Ga	0.2													O	8			1995																											2	Y124				3.858		27.11													59.5		81				70.25																																																																																														Y2O3, Ba(NO3)2, CuO,Ga2 O3	1	mixture-CAL(750C,6H in O2)-pellet-SIN(800C,24H in flowing O2)					Structure,superconductivity and magnetism of YBa2(Cu1-xMx)4O8(M=Fe,Co,Ni,Zn and Ga)	199502		Department of Physics,National Sun Yat-Sen University,Kaohsiung 80424,Taiwan	Physica C.,242(1995)373-380	F.L.Juang,H.D.Yang,K.C.Huang,T.H.Meen,W.J.Huang,Y.C.Chen	Y,Ba,Cu,O,Fe,Co,Ni,Zn,Ga	
5734	PHC2420017	as-synthesized. semiconductor-like. RRR<1	(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1OZ	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	Z			1995																											2	Hg1201	P4/mmm			3.841		8.701												K	56	59.5	67				59.5																																																																																																two step process, precursor(Cr-Sr-Cu-O) - ADD(HgO) - pellet - sealed in quartz tube - heat to 870C(3.5C/min) hold(870C,5-8h) - cool to RT					Synthesis and study of (Hg,Cr)-based 1201-type superconducting cuprate (Hg,Cr)Sr2CuO4+z	199502		Department of Physics,and High Density Electronics Center,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)17-22	O.Chmaissem,T.Z.Deng,Z.A.Sheng		
5735	PHC2420017	annealed in O2. metallic behaviour. sharp transition	(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1Oz	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	z			1995																												Hg1201																		K		59.5					59.5																																																																																																two step process, precursor(Cr-Sr-Cu-O) - ADD(HgO) - pellet - sealed in quartz tube - heat to 870C(3.5C/min) hold(870C,5-8h) - cool to RT					Synthesis and study of (Hg,Cr)-based 1201-type superconducting cuprate (Hg,Cr)Sr2CuO4+z	199502		Department of Physics,and High Density Electronics Center,University of Arkansas,Fayetteville,AR 72701,USA	Physica C.,242(1995)17-22	O.Chmaissem,T.Z.Deng,Z.A.Sheng		
5736	PHC2440305		Bi2Sr2CaCu2O8-(ZnPc)xBi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1995																												Bi2212																					97				97																																																																						TP5736																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5737	PHC2440305	intercalated	Br2Sr2CaCu2O8-(Zn Pc)x Bi2Sy2CaCu2O8	Zn0.005Pc0.005Bi2Sr2Ca1Cu2Oz	Zn	0.005	Pc	0.005	Bi	2	Sr	2	Ca	1	Cu	2									O	z			1995																												Bi2212																					79				79																																																																						TP5737																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5738	PHC2440305		Bi2Sr2CaCu2O8-(Zn Pc)xBi2Sr2CaCu2O8	Zn0.01Pc0.01Bi2Sr2Ca1Cu2Oz	Zn	0.01	Pc	0.01	Bi	2	Sr	2	Ca	1	Cu	2									O	z			1995																																																	74				74																																																																						TP5738																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5739	PHC2440305		Bi2Sr2CaCu2O8-(Zn Pc)xBi2Sr2CaCu2O8	Zn0.02Pc0.02Bi2Sr2Ca1Cu2Oz	Zn	0.02	Pc	0.02	Bi	2	Sr	2	Ca	1	Cu	2									O	z			1995																																																	67				67																																																																						TP5739																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5740	PHC2440305		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3Oz	Bi	2	Sr	2	Ca	2	Cu	3													O	z			1995																												Bi2223																			110						110																																																																						TP5740																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5741	PHC2440305		(Zn Pc)xBi2Sr2Ca2Cu3O10	Zn0.005Pc0.005Bi2Ca2Cu3Oz	Zn	0.005	Pc	0.005	Bi	2	Ca	2	Cu	3											O	z			1995																												Bi2223																			94						94																																																																						TP5741																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5742	PHC2440305		(Zn Pc)xBi2Sr2Ca2Cu3O10	Zn0.01Pc0.01Bi2Sr2Ca2Cu3Oz	Zn	0.01	Pc	0.01	Bi	2	Sr	2	Ca	2	Cu	3									O	z			1995																												Bi2223																			88						88																																																																						TP5742																										(Bi2212+single cryotal Zn Pc)-pellet-Pyrextube(10E-2TON)-heat(490C,15min-several hours)					Thermoelectric power study on high-Tc Bi2122 and -2223 oxides intercalated with organic molecules zincphtalocyanine	199503		Department of physics,National Taiwan University,Taipei,Taiwan	Physica C.,244(1995)305-310	C.Y.Huang,J.G.Lin,J.J.Lin,K.Yakushi,L.Grigoryan,Z.J.Huang		
5743	PHC2440341	ANN(300C,6H under 90 bar O2)	Tl(Ba,Sr)2 Ca2 Cu3 O9	Tl1Ba0.8Sr1.2Ca2Cu3O9-z	Tl	1	Ba	0.8	Sr	1.2	Ca	2	Cu	3											O	9-z		3	1995																												Tl1223																		K		95					95														90																				HIR5743				19.1						1660																																																		SrCuO2,Tl2O3,CuO,BaO2,CaO		sealed in silica ampoule-heatin vertical furnace					Magnetic study of an overdoped %a1223%a system: TlBa0.8Sr1.2Ca2Cu3O9-delta single crystals			Laboratoire CRISMAT-CNRS URA 1318-ISMRa-Universite' de Caen, Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	Physica.C,244(1995)341-348	A. Maignan,A. Wahl,B. Raveau,Ch. Simon,J. Provost,V. Hardy		
5744	PHC2440341	ANN(360C,30min in H2-Ar Fl)ow	Tl(Ba,Sr)2 Ca2 Cu3 O9	Tl1Ba0.8Sr1.2Ca2Cu3O9-z	Tl	1	Ba	0.8	Sr	1.2	Ca	2	Cu	3											O	9-z		3	1995																												Tl1223																				115					115														105																				HIR5744					17.7				1660																																																			SrCuO2,Tl2O3,CuO,BaO2,CaO		sealed in silica ampoule-heatin vertical furnace					Magnetic study of an overdoped %a1223%a system: TlBa0.8Sr1.2Ca2Cu3O9-delta single crystals			Laboratoire CRISMAT-CNRS URA 1318-ISMRa-Universite' de Caen, Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	Physica.C,244(1995)341-348	A. Maignan,A. Wahl,B. Raveau,Ch. Simon,J. Provost,V. Hardy		
5745	PHC2440341	as-grown	Tl(Ba,Sr)2 Ca2 Cu3 O9	Tl1Ba0.8Sr1.2Ca2Cu3O9-z	Tl	1	Ba	0.8	Sr	1.2	Ca	2	Cu	3											O	9-z		3	1995																												Tl1223																				98					98														90																				HIR5745					19.1				1640																																																			SrCuO2,Tl2O3,CuO,BaO2,CaO		sealed in silica ampoule-heatin vertical furnace					Magnetic study of an overdoped %a1223%a system: TlBa0.8Sr1.2Ca2Cu3O9-delta single crystals			Laboratoire CRISMAT-CNRS URA 1318-ISMRa-Universite' de Caen, Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	Physica.C,244(1995)341-348	A. Maignan,A. Wahl,B. Raveau,Ch. Simon,J. Provost,V. Hardy		
5746	PHC2440389	epitaxial film,G-L parameter=31	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z			1995																												T'																				21.7					21.7																				T		5.2							T/K		0.35					A			80		A			2480																																																				target=Nd1.85 Ce0.15 Cu Oz,substrate=(100)Sr Ti O3 T(sub)=795C,sputtering(0.35mbar Ar+0.25mbar O2)					Fabrication and electrical transprot properties of epitaxial Nd1.85Ce0.15CuO4-y films	199503		Physikalisches Institut,Lehrstuhl Experimentalphysik II,University of Tubingen Morgenstelle 14,D-72076 Tubingen,Germany	Physica C.,244(1995)389-399	A.Beck,F.Gollnuk,H.Heansel,K.Knorr,R.Gross,R.P.Huebener		
5747	PHC2450270		Sr2 Cu(O2 F2)	Sr2Cu1F2O2	Sr	2	Cu	1	F	2															O	2			1995																																															40						40																																																																																																subjecting Sr2 Cu O3 to flowing 95% Ne/5% F2 at 180C for 20 min					Anomalous pressure dependence of the superconducting transition temperature of Sr2CuO2F2+z	199504		Sandia National Laboratories,Albuquerque,NM 87185-0345,USA	Physica C.,245(1995)270-272	B.Morosin,E.L.Venturini,J.E.Schirber,W.R.Bayless		
5748	PHC2450036		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	7-z	6.92	1	1995																												Y123																				92.2				1.1	92.2										70																																											SP5748				25.091		446.7																																			Y2O3,BaCo3,CuO		ANN(930C,12H in air )-final ANN(500C,10-12H in flowing O2)-FC					Electron and phonon characteristics of YBa2Cu3O7-z	199504		Institute of Inorganic Chemistry,Novosibirsk,630090,Russian Federation	Physica C.,245(1995)36-40	G.I.Frolova,V.G.Bessergenev,V.N.Naumov,Yu.A.Kovalevskaya		
5749	PHC2450207	prepared immdiately	(Hg,Cu)Ba2 Cu O4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1995																											2	Hg1201				3.872		9.479														50					50																																																																																																high pressure synthesis,pellet-Au capsule-prees(18Kbar,900C,0.6H)					On the possibility of replacing Hg by Cu in the Hgba2CuO4+z phase synthesized under high-pressure	199504		Laboratoire de Cristallographie,CNRS-UJF,BP 166,38042 Grenoble cedex 09,France	Physica C.,245(1995)207-211	E.T.Alexandre,E.V.Antipov,J.J.Capponi,M.Marezio,P.Bordet,S.M.Loureiro,S.de Brion		
5750	PHC2450207	Hg1201+unknown inpuriq	(Hg,Cu)Ba2 Cu O4	Hg0.75Ba2Cu1.25O4+z	Hg	0.75	Ba	2	Cu	1.25															O	4+z		1	1995																											2	Hg1201				3.868		9.485																	4.2																																																																																																		high pressure synthesis,pellet-Au capsule-prees(18Kbar,900C,0.6H)					On the possibility of replacing Hg by Cu in the Hgba2CuO4+z phase synthesized under high-pressure	199504		Laboratoire de Cristallographie,CNRS-UJF,BP 166,38042 Grenoble cedex 09,France	Physica C.,245(1995)207-211	E.T.Alexandre,E.V.Antipov,J.J.Capponi,M.Marezio,P.Bordet,S.M.Loureiro,S.de Brion		
5751	PHC2450001	85%Hg1234+3% Hg1223+7% Hg1245,data for Hg1234, Tc=3step(132K,116K,96K)	Hg Ba2 Ca3 Cu4 O10	Hg1Ba2Ca3Cu4O10+z	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z			1995																											2	Hg1234				3.852		18.943														116	132				116																																		HIR5751																																																													1	precursor(Ba2 Cu3 Cu4 Oz)-mixed with HgO-Au capsule-prees up to 18kbar-heat(920C,1.7H)-standuid state					Magnetic properties of the HgBa2Ca3Cu4O10+z superconducting phase	199504		Departmento de Fisica,FCUL,Campo Grande,Ed.C1,1700 Lisboa,Portugal	Physica C.,245(1995)1-5	C.C.Abilio,J.J.Capponi,M.Godinho,S.M.Loureiro		
5752	PHC2460351	ANN(763K)	Hg Sr2 Ca (Cu,Re)2 Oz	Hg1Sr2Ca1Cu1.8Re0.2Oz	Hg	1	Sr	2	Ca	1	Cu	1.8	Re	0.2											O	z			1995																											2	Hg1212				3.816		12.066														90					90																																																																																																Precursor +HgO					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
5753	PHC2460351	as-prepared	(Hg,Re)Sr2 Ca2 Cu3 Oz	Hg0.75Re0.25Sr2Ca2Cu3Oz	Hg	0.75	Re	0.25	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223				3.816		15.213														100					100																																																																																																Precursor +HgO					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
5754	PHC2460351	ANN(783C,in evacuated quartz ampoule)	(Hg,Re)Sr2 Ca2 Cu3 Oz	Hg0.75Re0.25Sr2Ca2Cu3Oz	Hg	0.75	Re	0.25	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223				3.83		15.227														120					120																																																																																																Precursor +HgO					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
5758	JSC1100032	semicon-like	Nb Sr2 Sm Cu2 O8	Nb1Sr2Sm1Cu2O8-z	Nb	1	Sr	2	Sm	1	Cu	2													O	8-z		1	1994																											2	1212	P4/mmm			3.877		11.636																	10																																																																																				980												M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5759	JSC1100032	in purity phase=SrCuO2,semicon	Ta Sr2  Sm Cu2 O8	Ta1Sr2Sm1Cu1O8-z	Ta	1	Sr	2	Sm	1	Cu	1													O	8-z			1994																											2	1212				3.872		11.676																	10																																																																																					4790											M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5760	JSC1100032	semicon	Nb Sr2 Pr Cu2 O8	Nb1Sr2Pr1Cu2O8.01	Nb	1	Sr	2	Pr	1	Cu	2													O	8-z	8.01		1994																											2	1212				3.892		11.681																	10																																																																																				670												M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5761	JSC1100032	semicon	TaSr2PrCu2O8	Ta1Sr1Pr1Cu2O8-z	Ta	1	Sr	1	Pr	1	Cu	2													O	8-z			1994																											2	1222	P/4mmm			3.89		11.713																																																																																																																	M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5762	JSC1100032	semicon	NbBa2PrCu2O8	Nb1Ba2Pr1Cu2O7.96	Nb	1	Ba	2	Pr	1	Cu	2													O	8-z	7.96		1994																											2	1222	P/4mmm			3.95		11.947																																																																																																																	M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5763	JSC1100032	semicon	(Nb,Ru)Sr2 Sm Cu2 O8	Nb0.9Ru0.1Sr2Sm1Cu2O8-z	Nb	0.9	Ru	0.1	Sr	2	Sm	1	Cu	2											O	8-z			1994																											2	1212				3.8741		11.626																	10																																																																																																M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5764	JSC1100032	semicon	(Nb,Ru)Sr2 Sm Cu2 O8	Nb0.8Ru0.2Sr2Sm1Cu2O8-z	Nb	0.8	Ru	0.2	Sr	2	Sm	1	Cu	2											O	8-z			1994																											2	1212				3.8712		11.617																	10																																																																																																M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5765	JSC1100032	semicon	(Nb,Ru)Sr2 Sm Cu2 O8	Nb0.7Ru0.3Sr2Sm1Cu2O8-z	Nb	0.7	Ru	0.3	Sr	2	Sm	1	Cu	2											O	8-z			1994																											2	1212				3.8688		11.609																	10																																																																																																M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5766	JSC1100032	semicon	(Nb,Ru)Sr2 Sm Cu2 O8	Nb0.6Ru0.4Sr2Sm1Cu2O8-z	Nb	0.6	Ru	0.4	Sr	2	Sm	1	Cu	2											O	8-z			1994																											2	1212				3.8624		11.59																	10																																																																																																M2O5,RuO2,BaCO3,SrCO3,Pr6O11,Sm2O3,CuO	1	CAL,SIN(1040,1050C,20H in air					Preparation and Characterization of New 1-2-1-2 Compounds MA2RECu2O8-z (M=Nb or Ta, A=Ba or Sr, and RE=Pr or Sm )			"Angewandte Physik, Johannes-Kepler Uniersita""t Linz, A4040 Linz, Austria"	J.Solid State Chem(1994)32-35	B. Hellebrand,P.L. Steger,X.Z. Wang		
5767	SUP0080021	not SIc	(Y,Ca)Sr2(Cu2,Ga)O7	Y0.65Ca0.35Sr2Cu2Ga1O6.94	Y	0.65	Ca	0.35	Sr	2	Cu	2	Ga	1											O	7-z	6.94		1995																											3	Y123				5.386	5.474	22.814																	10																																																																																																Y2O3,CaCo3,SrCO3,BaCO3,CuO,Ga2O3	1	mixture-CAL(1050C,20H in air)-pellet-SIN(1050 or1000C,in O2)-ANN(460C,30H in O2)-cool to RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5768	SUP0080021	ANN in 350 bar O2 at 500c	(Y,Ca)Sr2(Cu2,Ga)O7	Y0.65Ca0.35Sr2Cu2Ga1O6.99	Y	0.65	Ca	0.35	Sr	2	Cu	2	Ga	1											O	7-Z	6.99		1995																											3	Y123				5.384	5.474	22.815														27					27																																																																																														Y2O3,CaCo3,SrCO3,BaCO3,CuO,Ga2O3	1	mixture-CAL(1050C,20H in air)-pellet-SIN(1050 or1000C,in O2)-ANN(460C,30H in O2)-cool to RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5769	SUP0080021	not  S/C	(Y,Ca)Sr2(Cu2,Ga)O7	Y0.6Ca0.4Sr2Cu2Ga1O0.92	Y	0.6	Ca	0.4	Sr	2	Cu	2	Ga	1											O	7-z	0.92		1995																											3	Y123				5.386	5.475	22.816																	10																																																																																																Y2O3,CaCo3,SrCO3,BaCO3,CuO,Ga2O3	1	mixture-CAL(1050C,20H in air)-pellet-SIN(1050 or1000C,in O2)-ANN(460C,30H in O2)-cool to RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5770	SUP0080021	ANN in 350 bar O2 at 500C	(Y,Ca)Sr2(Cu2,Ga)O7	Y0.6Ca0.4Sr2Cu2Ga1O7	Y	0.6	Ca	0.4	Sr	2	Cu	2	Ga	1											O	7-z	7		1995																											3	Y123				5.382	5.472	22.805														41					41																																																																																														Y2O3,CaCo3,SrCO3,BaCO3,CuO,Ga2O3	1	mixture-CAL(1050C,20H in air)-pellet-SIN(1050 or1000C,in O2)-ANN(460C,30H in O2)-cool to RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5771	SUP0080021		(Y,Ca)(Sr,Ba)2(Cu2,Ga)O7	Y0.6Ca0.4Sr1.8Ba0.2Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.8	Ba	0.2	Cu	2	Ga	1									O	7-z			1995																												Y123																				45					45																																																																																															1	ANN(500C,100H in 350bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5772	SUP0080021		(Y,Ca)(Sr,Ba)2(Cu2,Ga)O7	Y0.6Ca0.4Sr1.7Ba0.3Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.7	Ba	0.3	Cu	2	Ga	1									O	7-z			1995																												Y123																				50					50																																																																																															1	ANN(500C,100H in 350bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5773	SUP0080021		(Y,Ca)(Sr,Ba)2(Cu2,Ga)O7	Y0.6Ca0.4Sr1.6Ba0.4Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.6	Ba	0.4	Cu	2	Ga	1									O	7-z			1995																												Y123																				56					56																																																																																															1	ANN(500C,100H in 350bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5774	SUP0080021		(Y,Ca)Sr2 Ga Cu2 O7	Y0.6Ca0.4Sr2Ga1Cu2O7	Y	0.6	Ca	0.4	Sr	2	Ga	1	Cu	2											O	7			1995																											3					22.816	5.475	5.386																	4.2																																																																																																Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5775	SUP0080021		(Y,Ca)Sr2 Cu2 Ga O7	Y0.6Ca0.4Sr2Ga1Cu2O7	Y	0.6	Ca	0.4	Sr	2	Ga	1	Cu	2											O	7			1995																											3					22.805	5.472	5.382														41					41																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT-heat(500C,100H in 350 bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5776	SUP0080021		(Y,Ca)Sr2 Ga Cu2 O7	Y0.65Ca0.35Sr2Ga1Cu2O7	Y	0.65	Ca	0.35	Sr	2	Ga	1	Cu	2											O	7			1995																											3	Y123				22.814	5.474	5.386																	4.2																																																																																																Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5777	SUP0080021		(Y,Ca)Sr2 Ga Cu2 O7	Y0.65Ca0.35Sr2Ga1Cu2O7	Y	0.65	Ca	0.35	Sr	2	Ga	1	Cu	2											O	7			1995																											3	Y123				22.815	5.474	5.384														27					27																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT-heat(500C,100H in 350 bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5778	SUP0080021		(Y,Ca)(Sr,Ba)Cu2 Ga O7	Y0.6Ca0.4Sr1.8Ba0.2Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.8	Ba	0.2	Cu	2	Ga	1									O	7-z			1995																												Y123																				45					45																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT-heat(500C,100H in 350 bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5779	SUP0080021		(Y,Ca)(Sr,Ba)Cu2 Ga O7	Y0.6Ca0.4Sr1.7Ba0.3Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.7	Ba	0.3	Cu	2	Ga	1									O	7-z			1995																												Y123																				50					50																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT-heat(500C,100H in 350 bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5780	SUP0080021		(Y,Ca)(Sr,Ba)Cu2 Ga O7	Y0.6Ca0.4Sr1.6Ba0.4Cu2Ga1O7-z	Y	0.6	Ca	0.4	Sr	1.6	Ba	0.4	Cu	2	Ga	1									O	7-z			1995																												Y123																				56					56																																																																																														Y2O3,CaCO3,SrCO3,BaCO3,CuO,Ga2O3	1	pellet-SIN(1050C in O2)-ANN(460C,30min)-RT-heat(500C,100H in 350 bar O2)					Synthesis,Composition,and Structure of Superconducting (Y,Ca)(Sr,Ba)2GaO7-z	199501		Superconductivity Research Group,School of Chemistry,University of Birmingham,Birmingham B15 2TT,United kingdom.	J.Supercomductivity.,8(1995)21-25	C.Greaves,T.G.N.Babu		
5781	PHC2490111	Two step transitions in SUS. Tc shows higher value (minor phase Pb1223). The lower is 70K (major phase Pb1212: a=3.81, b=3.83, c=12.1). O-content is nominal value. impurity phase: Sr3Pb2.03Cu0.73O7.70	(Pb,Cu)Sr2CaCu2Oz	Pb0.5Sr2Ca1Cu2.5O6.8	Pb	0.5	Sr	2	Ca	1	Cu	2.5													O	z	6.8		1995																											3	Pb1223				3.82		15.5																115			115																																																																																														PbO,SrCuO2,Ca2CuO3,KClO4		K Cl O4 is doled as oxidiqing agent,pellet-press to 5.0GPa-heat(900C,0.5H)-FC					115 K superconductivity in the Pb-Sr-Ca-Cu-O system and formation of a new homologous series consisting of Pb-based layered cuprates	199506		Superconductivity Research Laboratory,International Superconductivity Technoligy Center,10-13 Shinonome 1-chome,Koto-ku,Tokyo 135,Japan	Physica C.,249(1995)111-116	Chang-Qing Jin,H.Yamauchi,Seiji Adachi,Tadashi Tatsuki,Toshiyuki Tamura,Xiao-Jing Wu		
5782	PHC2490001	Tc(zero)below 13K	(Hg,Pb)Sr2(R,Ce)2Cu2Oz	Hg0.5Pb0.5Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	1995																											2	Hg1222				3.846		29.418															38				38																																																																																															1	precursor(Sr2(Ln,Ce)2 Cu2 Oz)by citrate gel process-mix with PbO,HgO-pellet-seal in quartz tubu-heat(920C,10H)-ANN(400,in O2 flow or 10bar O2)					(Hg,Pb)Sr2(Ln,Ce)2Cu2Oz(Ln=Gd,Nd),a new family of mercury-lesd-based superconducting cuprates	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China Academia Sinica,Hefei 230026,China	Physica C.,249(1995)1-4	Kaibin Tang,Li Yang,Xiaowen Xu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5783	PHC2490001	dominant phase=1222	(Hg,Pb)Sr2(R,Ce)2 Cu2 Oz	Hg0.5Pb0.5Sr2Eu1.5Ce0.5Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	z			1995																											2	Hg1222				3.851		29.43																	4.2																																																																																																	1	precursor(Sr2(Ln,Ce)2 Cu2 Oz)by citrate gel process-mix with PbO,HgO-pellet-seal in quartz tubu-heat(920C,10H)-ANN(400,in O2 flow or 10bar O2)					(Hg,Pb)Sr2(Ln,Ce)2Cu2Oz(Ln=Gd,Nd),a new family of mercury-lesd-based superconducting cuprates	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China Academia Sinica,Hefei 230026,China	Physica C.,249(1995)1-4	Kaibin Tang,Li Yang,Xiaowen Xu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5784	PHC2490001	dominant phase=1222	(Hg,Pb)Sr2(R,Ce)2 Cu2 Oz	Hg0.5Pb0.5Sr2Sm1.5Ce0.5Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Sm	1.5	Ce	0.5	Cu	2									O	z			1995																											2	Hg1222				3.853		29.439																	4.2																																																																																																	1	precursor(Sr2(Ln,Ce)2 Cu2 Oz)by citrate gel process-mix with PbO,HgO-pellet-seal in quartz tubu-heat(920C,10H)-ANN(400,in O2 flow or 10bar O2)					(Hg,Pb)Sr2(Ln,Ce)2Cu2Oz(Ln=Gd,Nd),a new family of mercury-lesd-based superconducting cuprates	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China Academia Sinica,Hefei 230026,China	Physica C.,249(1995)1-4	Kaibin Tang,Li Yang,Xiaowen Xu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5785	PHC2490001	semiconductor	(Hg,Pb)Sr2(R,Ce)2 Cu2 Oz	Hg0.5Pb0.5Sr2Nd1.5Ce0.5Cu2Oz	Hg	0.5	Pb	0.5	Sr	2	Nd	1.5	Ce	0.5	Cu	2									O	z		1	1995																											2	Hg1222				3.872		29.496																	4.2																																																																																																	1	precursor(Sr2(Ln,Ce)2 Cu2 Oz)by citrate gel process-mix with PbO,HgO-pellet-seal in quartz tubu-heat(920C,10H)-ANN(400,in O2 flow or 10bar O2)					(Hg,Pb)Sr2(Ln,Ce)2Cu2Oz(Ln=Gd,Nd),a new family of mercury-lesd-based superconducting cuprates	199506		Department of Applied Chemistry,University of Science and Technology of China;Structure Research Laboratory,University of Science and Technology of China Academia Sinica,Hefei 230026,China	Physica C.,249(1995)1-4	Kaibin Tang,Li Yang,Xiaowen Xu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
5786	PHC2030115	450-470C Na OH react at	(La,Na)2CuO4	La1.96Na0.4Cu1O4	La	1.96	Na	0.4	Cu	1															O	4			1992																											2	T				5.361		13.158																31			31																																																																																														La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5787	PHC2030115	react at 390C KOH	(La,K)2CuO4	La1.8K0.2Cu1O4	La	1.8	K	0.2	Cu	1															O	4			1992																											2	T				5.334		13.324																41			41																																																																																														La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5788	PHC2030115	react at 700C KOH	(La,K)2CuO4	La1.92K0.08Cu1O4	La	1.92	K	0.08	Cu	1															O	4			1992																											2	T				5.342		13.238																21			21																																																																																														La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5789	PHC2030115	react in 460C RbOH	(La,Rb)2CuO4	La1.84Rb0.16Cu1O4	La	1.84	Rb	0.16	Cu	1															O	4			1992																											2	T				5.346		13.314																	13																																																																																																La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5790	PHC2030115	react in 370C CsOH	(La,Cs)2CuO4	La1Cs1Cu1O	La	1	Cs	1	Cu	1															O				1992																											2	T				5.362		13.238																	13																																																																																																La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5791	PHC2030115	react in 520C CsOH	(La,Cs)2CuO4	La1Cs1Cu1O	La	1	Cs	1	Cu	1															O				1992																											3	T				5.361	5.391	13.155																	13																																																																																																La2 O3,Cu O,R OH		low temperature hydroxide melt technique. La2 O3,Cu O in Na OH,KOH,RbOH,CsOH,melt under air					LOW TEMPERATURE SYNTHESIS AND PROPERTIES OF SUPERCONDUCTING ALKALI SUBSTITUTED LA2CUO4 PHASE	199212		INSTITUT FUR ANORGANISCHE UND ANALYTISCHE CHEMIE, TECHNISCHE UNIVERSITAT BERLIN, GERMANY	PHYSICA C,203(1992)115	R.SCHOLLHORN,W.GUNTHER	LA,CU,O,NA,K,RB,CS	
5792	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2O8.21	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.21	1	1995																												Bi2212																				90.6					90.6																																																																																																reduced host(z=8.210 Bi2212)+I in evacuated gloss tube,host temp=150C,I-temp=40-150C for various content of I					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5793	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.03O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.03											O	z	8.21	1	1995																												Bi2212																				86.6					86.6																																																																																																reduced host(z=8.210 Bi2212)+I in evacuated gloss tube,host temp=150C,I-temp=40-150C for various content of I					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5794	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.1O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.1											O	z	8.21	1	1995																												Bi2212																				83.9					83.9																																																																																																reduced host(z=8.210 Bi2212)+I in evacuated gloss tube,host temp=150C,I-temp=40-150C for various content of I					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5795	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.25O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.25											O	z	8.21	1	1995																												Bi2212																				71.6					71.6																																																																																																reduced host(z=8.210 Bi2212)+I in evacuated gloss tube,host temp=150C,I-temp=40-150C for various content of I					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5796	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.43O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.43											O	z	8.21	2	1995																												Bi2212																				63.1					63.1																																																																																																					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5797	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.61O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.61											O	z	8.21	2	1995																												Bi2212																				56.3					56.3																																																																																																					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5798	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca2Cu2I0.86O8.21	Bi	2	Sr	2	Ca	2	Cu	2	I	0.86											O	z	8.21	1	1995																												Bi2212																				50.6					50.6																																																																																																					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5799	PHC2450332		Bi2 Sr2Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.98O8.21	Bi	2	Sr	2	Ca	1	Cu	2	I	0.98											O	z	8.21	1	1995																												Bi2212																				49.3					49.3																																																																																																					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5800	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2O8.242	Bi	2	Sr	2	Ca	1	Cu	2													O		8.242	1	1995																												Bi2212																				73.9					73.9																																																																			-3.22																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5801	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1I0.06O8.242	Bi	2	Sr	2	Ca	1	I	0.06													O		8.242	1	1995																												Bi2212																																																																																												-3.57																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5802	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.2O8.242	Bi	2	Sr	2	Ca	1	Cu	2	I	0.2											O		8.242	1	1995																												Bi2212																				64.6					64.6																																																																			-4.75																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5803	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.4O8.242	Bi	2	Sr	2	Ca	1	Cu	2	I	0.4											O		8.242	1	1995																												Bi2212																				56.7					56.7																																																																			-5.26																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5804	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.69O8.242	Bi	2	Sr	2	Ca	1	Cu	2	I	0.69											O		8.242	2	1995																												Bi2212																				53.1					53.1																																																																			-4.69																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5805	PHC2450332		Bi2Sr2CaCu2O8Ix	Bi2Sr2Ca1Cu2I0.86O8.242	Bi	2	Sr	2	Ca	1	Cu	2	I	0.86											O		8.242	1	1995																												Bi2212																				55.5					55.5																																																																			-3.6																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5806	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I1O8.242	Bi	2	Sr	2	Ca	1	Cu	2	I	1											O		8.242	1	1995																												Bi2212																				53					53																																																																			-3.35																													as sintered host(z=8.242 Bi2212)+I in evacuated glass tube,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5807	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.28	1	1995																												Bi2212																																																																																																																									oxidiqed host (z=8.280 Bi2212)+I in evacuated glass tubu,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5808	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.23O8.28	Bi	2	Sr	2	Ca	1	Cu	2	I	0.23											O	z	8.28	1	1995																												Bi2212																																																																																																																									oxidiqed host (z=8.280 Bi2212)+I in evacuated glass tubu,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5809	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.47O8.28	Bi	2	Sr	2	Ca	1	Cu	2	I	0.47											O	Z	8.28	2	1995																												Bi2212																																																																																																																									oxidiqed host (z=8.280 Bi2212)+I in evacuated glass tubu,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5810	PHC2450332		Bi2 Sr2 Ca Cu2 O8 Ix	Bi2Sr2Ca1Cu2I0.95O8.28	Bi	2	Sr	2	Ca	1	Cu	2	I	0.95											O	z	8.28	1	1995																												Bi2212																																																																																																																									oxidiqed host (z=8.280 Bi2212)+I in evacuated glass tubu,host temp=150C,I-temp=40-150C for various content of I,24H					Carrier doping through iodine intercalation into Bi2Sr2CaCu2O8+z with different z values	199504		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,245(1995)332-340	Akihiko Fujiwara,Kei Wataanabe,Keniichi Sasaki,Masatsune Kato,Takashi Noji,Yoji Koike,Yoshitami Saito		
5811	SUP0080373		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	z	6.92	1	1995																											3	Y123				3.822	3.888	11.667																91.5			91.5																																																																																														Y2O3,BaCO3,CuO,TiO2	1	mixture-heat(950C,24H in Pt crucible)-pellet-SIN(950C,24H in air)-ANN(450C,12H in O2 flow)-cool to RT(1 C/min)					Influence of Hole Filling by Ti on the Superconductivity of YBa2Cu3O7-delta	1995		Department of Physics, Dr. Babasahed Ambedkar Marathwada University, Aurangabad 431 004, India	J.Superconductivity,8(1995)373	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5812	SUP0080373		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.97Ti0.03O6.92	Y	1	Ba	2	Cu	2.97	Ti	0.03													O	z	6.92	1	1995																											3	Y123				3.873	3.895	11.652																82			82																																																																																														Y2O3,BaCO3,CuO,TiO2	1	mixture-heat(950C,24H in Pt crucible)-pellet-SIN(950C,24H in air)-ANN(450C,12H in O2 flow)-cool to RT(1 C/min)					Influence of Hole Filling by Ti on the Superconductivity of YBa2Cu3O7-delta	1995		Department of Physics, Dr. Babasahed Ambedkar Marathwada University, Aurangabad 431 004, India	J.Superconductivity,8(1995)373	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5813	SUP0080373		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.94Ti0.06O6.91	Y	1	Ba	2	Cu	2.94	Ti	0.06													O	z	6.91	1	1995																											3	Y123				3.867	3.883	11.632																77			77																																																																																														Y2O3,BaCO3,CuO,TiO2	1	mixture-heat(950C,24H in Pt crucible)-pellet-SIN(950C,24H in air)-ANN(450C,12H in O2 flow)-cool to RT(1 C/min)					Influence of Hole Filling by Ti on the Superconductivity of YBa2Cu3O7-delta	1995		Department of Physics, Dr. Babasahed Ambedkar Marathwada University, Aurangabad 431 004, India	J.Superconductivity,8(1995)373	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5814	SUP0080373		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.91Ti0.09O6.9	Y	1	Ba	2	Cu	2.91	Ti	0.09													O	z	6.9	1	1995																											3	Y123				3.877	3.902	11.673																74.1			74.1																																																																																														Y2O3,BaCO3,CuO,TiO2	1	mixture-heat(950C,24H in Pt crucible)-pellet-SIN(950C,24H in air)-ANN(450C,12H in O2 flow)-cool to RT(1 C/min)					Influence of Hole Filling by Ti on the Superconductivity of YBa2Cu3O7-delta	1995		Department of Physics, Dr. Babasahed Ambedkar Marathwada University, Aurangabad 431 004, India	J.Superconductivity,8(1995)373	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5815	SUP0080373		YBa2(Cu,Ti)3O7	Y1Ba2Cu2.88Ti0.12O6.88	Y	1	Ba	2	Cu	2.88	Ti	0.12													O	z	6.88	1	1995																											3	Y123				3.871	3.894	11.653																68.4			68.4																																																																																														Y2O3,BaCO3,CuO,TiO2	1	mixture-heat(950C,24H in Pt crucible)-pellet-SIN(950C,24H in air)-ANN(450C,12H in O2 flow)-cool to RT(1 C/min)					Influence of Hole Filling by Ti on the Superconductivity of YBa2Cu3O7-delta	1995		Department of Physics, Dr. Babasahed Ambedkar Marathwada University, Aurangabad 431 004, India	J.Superconductivity,8(1995)373	D.G. Kuberkar,G.K. Bichile,K.M. Jadhav,R.G. Kulkarni,R.L. Raibagkar		
5817	SSC0930269		Na2(Rb,Cs)C60	Na2Rb1C60	Na	2	Rb	1	C	60																		2	1995																											1	ABO3				14.096																		3.4			3.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
5818	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.75Cs0.25C60	Na	2	Rb	0.75	Cs	0.25	C	60																2	1995																											1																							5.2			5.2																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
5819	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.5Cs0.5C60	Na	2	Rb	0.5	Cs	0.5	C	60																2	1995																											1																							8.4			8.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
5820	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.25Cs0.75C60	Na	2	Rb	0.25	Cs	0.75	C	60																2	1995																											1																							9.4			9.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
5821	SSC0930269		Na2(Rb,Cs)C60	Na2Cs1C60	Na	2	Cs	1	C	60																		2	1995																											1																							11.7			11.7																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
5822	JJP0341121		(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	Nb1Sr2Sm1.2Ce0.8Cu2OZ	Nb	1	Sr	2	Sm	1.2	Ce	0.8	Cu	2											O	Z		1	1995																											2	1212				3.872		28.731																25			25																																																																																														RuO2,Nb2O5,SrCO3,Sm2O3,CeO2,CuO	1	mixture-heat(1000-1050C,3H in air)-pellet-heat(1050C,12H in air)-ANN(550C,2H in 0.4MPa O2)-cool to RT					Preparation of New Superconducting Cuprate(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	199509			Jpn.J.Appl.phys.Lett.,34(1995)L1121-L1122	Akira ONO	Ru, Nb, Sr, Sm, Ce, Cu,O	
5823	JJP0341121		(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	Ru0.32Nb0.68Sr2Sm1.2Ce0.8Cu2Oz	Ru	0.32	Nb	0.68	Sr	2	Sm	1.2	Ce	0.8	Cu	2									O	z		2	1995																												1212																						30			30																																																																																														RuO2,Nb2O5,SrCO3,Sm2O3,CeO2,CuO	1	mixture-heat(1000-1050C,3H in air)-pellet-heat(1050C,12H in air)-ANN(550C,2H in 0.4MPa O2)-cool to RT					Preparation of New Superconducting Cuprate(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	199509			Jpn.J.Appl.phys.Lett.,34(1995)L1121-L1122	Akira ONO	Ru, Nb, Sr, Sm, Ce, Cu,O	
5824	JJP0341121		(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	Ru0.5Nb0.5Sr2Sm1.2Ce0.8Cu2Oz	Ru	0.5	Nb	0.5	Sr	2	Sm	1.2	Ce	0.8	Cu	2									O	z		1	1995																											2	1212				3.859		28.663																32			32																																																																																														RuO2,Nb2O5,SrCO3,Sm2O3,CeO2,CuO	1	mixture-heat(1000-1050C,3H in air)-pellet-heat(1050C,12H in air)-ANN(550C,2H in 0.4MPa O2)-cool to RT					Preparation of New Superconducting Cuprate(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	199509			Jpn.J.Appl.phys.Lett.,34(1995)L1121-L1122	Akira ONO	Ru, Nb, Sr, Sm, Ce, Cu,O	
5825	JJP0341121		(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	Ru0.76Nb0.24Sr2Sm1.2Ce0.8Cu2Oz	Ru	0.76	Nb	0.24	Sr	2	Sm	1.2	Ce	0.8	Cu	2									O	z		1	1995																											2	1212				3.851		28.61																25			25																																																																																														RuO2,Nb2O5,SrCO3,Sm2O3,CeO2,CuO	1	mixture-heat(1000-1050C,3H in air)-pellet-heat(1050C,12H in air)-ANN(550C,2H in 0.4MPa O2)-cool to RT					Preparation of New Superconducting Cuprate(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	199509			Jpn.J.Appl.phys.Lett.,34(1995)L1121-L1122	Akira ONO	Ru, Nb, Sr, Sm, Ce, Cu,O	
5826	JJP0341121		(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	Ru1Sr2Sm1.2Ce0.8Cu2Oz	Ru	1	Sr	2	Sm	1.2	Ce	0.8	Cu	2											O	z		1	1995																											2	1212				3.847		28.559																	4.2																																																																																																RuO2,Nb2O5,SrCO3,Sm2O3,CeO2,CuO	1	mixture-heat(1000-1050C,3H in air)-pellet-heat(1050C,12H in air)-ANN(550C,2H in 0.4MPa O2)-cool to RT					Preparation of New Superconducting Cuprate(Ru,Nb)Sr2(Sm,Ce)2Cu2Oz	199509			Jpn.J.Appl.phys.Lett.,34(1995)L1121-L1122	Akira ONO	Ru, Nb, Sr, Sm, Ce, Cu,O	
5827	PHC2490111	O-content is nominal value. impurity phase: Sr3Pb2.03Cu0.73O7.70.	(Pb,Cu)Sr2CaCu2Oz	Pb0.5Sr2Ca1Cu2.5O7.4	Pb	0.5	Sr	2	Ca	1	Cu	2.5													O	z	7.4		1995																											3	Pb1212				3.76	3.85	12.3												K					4.2																																																																																																PbO,SrCuO2,Ca2CuO3,KClO4		K Cl O4 is doled as oxidiqing agent,pellet-press to 5.0GPa-heat(900C,0.5H)-FC					115 K superconductivity in the Pb-Sr-Ca-Cu-O system and formation of a new homologous series consisting of Pb-based layered cuprates	199506		Superconductivity Research Laboratory,International Superconductivity Technoligy Center,10-13 Shinonome 1-chome,Koto-ku,Tokyo 135,Japan	Physica C.,249(1995)111-116	Chang-Qing Jin,H.Yamauchi,Seiji Adachi,Tadashi Tatsuki,Toshiyuki Tamura,Xiao-Jing Wu		
5828	PHC2510219	grain siqe< 20micron	Y Ba2 Cu3 O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1995																												Y123																						89.8			89.8																																										from AC Suspeptibity		1.3	1.2																																																	Y2 O3, Ba Co3, Cu O	1	final heat treatment(920C,several days)-slow cool (320C to 280C,150H),separate through sieves					Possible origin for the T2 dependence of the penetration depth detected by susceptibility measurements in aligned YBa2Cu3O7 powder samples	199509		Physique des Solides, URA 2 CNRS, Universite' Paris-Sud, Orsay, France	Physica C,251(1995)219-230	G. Collin (b),H. Alloul (a),L. Guerrin (a)	Y, Ba, Cu, O	
5829	PHC2510219	20<grain siqe<40 micron	Y Ba2 Cu3 O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1995																												Y123																						90.3			90.3																																												1.4	0.8																																																	Y2 O3, Ba Co3, Cu O	1	final heat treatment(920C,several days)-slow cool (320C to 280C,150H),separate through sieves					Possible origin for the T2 dependence of the penetration depth detected by susceptibility measurements in aligned YBa2Cu3O7 powder samples	199509		Physique des Solides, URA 2 CNRS, Universite' Paris-Sud, Orsay, France	Physica C,251(1995)219-230	G. Collin (b),H. Alloul (a),L. Guerrin (a)	Y, Ba, Cu, O	
5830	PHC2510219	50<grain siqe<100 miclon	Y Ba2 Cu3 O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1995																												Y123																						90.7			90.7																																												1.3	1																																																	Y2 O3, Ba Co3, Cu O	1	final heat treatment(920C,several days)-slow cool (320C to 280C,150H),separate through sieves					Possible origin for the T2 dependence of the penetration depth detected by susceptibility measurements in aligned YBa2Cu3O7 powder samples	199509		Physique des Solides, URA 2 CNRS, Universite' Paris-Sud, Orsay, France	Physica C,251(1995)219-230	G. Collin (b),H. Alloul (a),L. Guerrin (a)	Y, Ba, Cu, O	
5831	PHC2510255		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	z	6.6	3	1995																												Y123																																																											HIR5831																																																														grown by slow cooling of a solid-melt mixture,-ANN (appropriat temp. for 1-2weeks in flowing O2)-Q to RT or LN2					Anisotropic properties of the anomalous second peak in the magnetization curves and the irreversibility field of YBa2Cu3Oy (6.6%$y%$6.9)single crystals	199509		Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-77, Japan	Physica C,251(1995)255-262	H. Asaoka (b),H. Iwasaki (a),H. Takei (c),K. Hirono (a),K. Watanabe (a),N. Kobayashi (a),S. Awaji (a),T. Nishizaki (a),T. Sasaki (a)	Y, Ba, Cu, O	
5832	PHC2510255		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7	3	1995																												Y123																																																											HIR5832																																																														grown by slow cooling of a solid-melt mixture,-ANN (appropriat temp. for 1-2weeks in flowing O2)-Q to RT or LN2					Anisotropic properties of the anomalous second peak in the magnetization curves and the irreversibility field of YBa2Cu3Oy (6.6%$y%$6.9)single crystals	199509		Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-77, Japan	Physica C,251(1995)255-262	H. Asaoka (b),H. Iwasaki (a),H. Takei (c),K. Hirono (a),K. Watanabe (a),N. Kobayashi (a),S. Awaji (a),T. Nishizaki (a),T. Sasaki (a)	Y, Ba, Cu, O	
5833	PHC2510255		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	3	1995																												Y123																																																											HIR5833																																																														grown by slow cooling of a solid-melt mixture,-ANN (appropriat temp. for 1-2weeks in flowing O2)-Q to RT or LN2					Anisotropic properties of the anomalous second peak in the magnetization curves and the irreversibility field of YBa2Cu3Oy (6.6%$y%$6.9)single crystals	199509		Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-77, Japan	Physica C,251(1995)255-262	H. Asaoka (b),H. Iwasaki (a),H. Takei (c),K. Hirono (a),K. Watanabe (a),N. Kobayashi (a),S. Awaji (a),T. Nishizaki (a),T. Sasaki (a)	Y, Ba, Cu, O	
5834	PHC2510255		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	z	6.85	3	1995																												Y123																																																											HIR5834																																																														grown by slow cooling of a solid-melt mixture,-ANN (appropriat temp. for 1-2weeks in flowing O2)-Q to RT or LN2					Anisotropic properties of the anomalous second peak in the magnetization curves and the irreversibility field of YBa2Cu3Oy (6.6%$y%$6.9)single crystals	199509		Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-77, Japan	Physica C,251(1995)255-262	H. Asaoka (b),H. Iwasaki (a),H. Takei (c),K. Hirono (a),K. Watanabe (a),N. Kobayashi (a),S. Awaji (a),T. Nishizaki (a),T. Sasaki (a)	Y, Ba, Cu, O	
5835	PHC2510255		Y Ba2 Cu3 O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	z	6.9	3	1995																												Y123																																																											HIR5835																																																														grown by slow cooling of a solid-melt mixture,-ANN (appropriat temp. for 1-2weeks in flowing O2)-Q to RT or LN2					Anisotropic properties of the anomalous second peak in the magnetization curves and the irreversibility field of YBa2Cu3Oy (6.6%$y%$6.9)single crystals	199509		Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-77, Japan	Physica C,251(1995)255-262	H. Asaoka (b),H. Iwasaki (a),H. Takei (c),K. Hirono (a),K. Watanabe (a),N. Kobayashi (a),S. Awaji (a),T. Nishizaki (a),T. Sasaki (a)	Y, Ba, Cu, O	
5836	PHC2520013		R Ba2 Cu4 O8	Yb1Ba2Cu4O8	Yb	1	Ba	2	Cu	4															O	8		3	1995																											3	Y124	Ammm			3.821	3.859	27.109														78.8					78.8																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5837	PHC2520013		R Ba2 Cu4 O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8		3	1995																											3	Y124	Ammm			3.822	3.856	27.113														80					80																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5838	PHC2520013		R Ba2 Cu4 O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		3	1995																											3	Y124	Ammm			3.825	3.86	27.11														80.1					80.1																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5839	PHC2520013		R Ba2 Cu4 O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		3	1995																											3	Y124	Ammm			3.832	3.865	27.128														79.2					79.2																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5840	PHC2520013		R Ba2 Cu4 O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		3	1995																											3	Y124	Ammm			3.833	3.864	27.115														74					74																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5841	PHC2520013		(Y,Ca) Ba2 Cu4 O8	Y0.98Ca0.02Ba2Cu4O8	Y	0.98	Ca	0.02	Ba	2	Cu	4													O	8		3	1995																											3	Y124	Ammm			3.834	3.864	27.156														87					87																																																																																														R123, BaCuO2,CuO		flux method, 20% Oz/ Ar at 3K bar using HIP furnace heat to 1100C (12C/min)  -hold (1100C,30min)-1060C (5C/H)-RT (60C/H)-P=0					Single-crystal growth and characterization of REBa2Cu4O8 and Y1-xCaxBa2Cu4O8	199510		(a)Department of Chemistry,Northwestern University,Evanston,IL 60208, USA (b)The Science and Technology Center for Superconductivity,Northwesten University,Evanston,IL 60208, USA (c)Department of Physics and The Science and Technology Center for Superconductivity,Northern Illinois University,Decalb,IL 60115, USA	Physica C,252(1995)13-21	B. Dabrowski (c),C.A. Hijar (a,b),C.L. Stern (a),K. Rogacki (c),K.R. Poeppelmeier (a,b),Z. Chen (c)	Y, Ca, Ba, Cu, O	
5842	PHC2510110		(Pb,Cd) Sr2 Tb Cu2 O7	Pb5Cd0.5Sr2Tb1Cu2O7	Pb	5	Cd	0.5	Sr	2	Tb	1	Cu	2											O	7			1995																											2	Pb1212	P4/mmm			3.822		11.951																	4.2																																																																																																							New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5843	PHC2510110		(Pb,Cd)Sr2 (Tb,Ca)Cu2 O7	Pb0.5Cd0.5Sr2Tb0.65Ca0.15Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Tb	0.65	Ca	0.15	Cu	2									O	7			1995																											2	Pb1212				3.8209		11.959																	4.2																																																																																																							New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5844	PHC2510110		(Pb,Cd)Sr2(Tb,Ca)Cu2 O7	Pb0.5Cd0.5Sr2Tb0.78Ca0.22Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Tb	0.78	Ca	0.22	Cu	2									O	7			1995																											2	Pb1212				3.8214		11.963																	4.2																																																																																																							New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5845	PHC2510110		(Pb,Cd)Sr2(Tb,Ca)Cu2 O7	Pb0.5Cd0.5Sr2Tb0.7Ca0.3Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Tb	0.7	Ca	0.3	Cu	2									O	7			1995																											2	Pb1212				3.8228		11.963																	4.2																																																																																																							New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5846	PHC2510110		(Pb,Cd)Sr2(Tb,Ca)Cu2 O7	Pb0.5Cd0.5Sr2Tb0.6Ca0.4Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Tb	0.6	Ca	0.4	Cu	2									O	7			1995																											2	Pb1212				3.826		11.972														19					19										5																																																																																											New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5847	PHC2510110		(Pb,Cd)Sr2(Tb,Ca)Cu2 O7	Pb0.5Cd0.5Sr2Tb0.5Ca0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Tb	0.5	Ca	0.5	Cu	2									O	7			1995																											2	Pb1212				3.8277		11.97														19					19										5																																																																																											New 1212 type (Pb,Cd) based cuprate superconducting system (Pb0.5Cd0.5)Sr2(Tb1-xCax)Cu2O7	199509		National Laboratory for Superconductivity,Institute of Physics, Chinese Academy of Sciences,Beijing 100080, China	Physica C,251(1995)110-114	B. Yin,C. Dong,F. Wu,G.C. Che,H. Chen,S.L. Jia,Y.C. Lan,Z.X. Zhao	Pb, Cd, Sr, Tb, Ca, Cu, O	
5848	JPC0019067		Gd Ba2 Cu3 O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z		1	1989									5.549									GPa		47.5					3955			Y123																																																																																																																							Gd2 O3, Ba O, Cu O	1	mixtwo-CAL(940C,48H in air)-pellet-SIN(940C,48H in flowing O2)-slow cool to RT(20C/H)				prosity=0.22,mearning ultorasonic wave by pulse echo method.elastivity C11=86.8, C44=29.5 GPa	The effect of hydrostatic Pressure on the elastic behaviour of GdBa2Cu3O7-x			School of Physics and Materials Science,University of Bath,Claverton Down,Bath BA27AY,UK	J.Phys.Codens.Matter 1(1989)9067-9076	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper	Gd, Ba, Cu, O	
5849	PHC2530102	R(T,H)curve anisotropy parometer=250	Bi2 Sr2 Ca(Cu,Zn)2 OZ	Bi2.1Sr1.9Ca1Cu2Oz	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	z		3	1995																												Bi2212																				90					90																																																																															0.85																	Using TSFZ method,					Zn substitution effect for Cu on the anisotropic transport properties in Bi2Sr2CaCu2O8+z single crystals	199510		Institute of Applied Physics, University of Tsukuba, Lbaraki 305, Japan	Physica C,253(1995)102-108	Dong-Seong Jeon,Hiroshi Ikeda,Masahiro Akamatsu,Ryozo Yoshizaki	Bi, Sr, Ca, Cu, O, Zn	
5850	PHC2530102	R(T,H)curve anisotropy parameter=70	Bi2 Sr2 Ca (Cu,Zn)2 O8	Bi2.1Sr1.9Ca1Cu1.988Zn0.012OZ	Bi	2.1	Sr	1.9	Ca	1	Cu	1.988	Zn	0.012											O	Z		3	1995																												Bi2212																				84					84																																																																															0.14																	Using TSFZ method,					Zn substitution effect for Cu on the anisotropic transport properties in Bi2Sr2CaCu2O8+z single crystals	199510		Institute of Applied Physics, University of Tsukuba, Lbaraki 305, Japan	Physica C,253(1995)102-108	Dong-Seong Jeon,Hiroshi Ikeda,Masahiro Akamatsu,Ryozo Yoshizaki	Bi, Sr, Ca, Cu, O, Zn	
5851	PHC2530102	R(T,H)curve anisotropy parameter=50	Bi2Sr2Ca(Cu,Zn)2O8	Bi2.1Sr1.9Ca1Cu1.98Zn0.02Oz	Bi	2.1	Sr	1.9	Ca	1	Cu	1.98	Zn	0.02											O	z		3	1995																												Bi2212																				82					82																																																																															0.17																	Using TSFZ method,					Zn substitution effect for Cu on the anisotropic transport properties in Bi2Sr2CaCu2O8+z single crystals	199510		Institute of Applied Physics, University of Tsukuba, Lbaraki 305, Japan	Physica C,253(1995)102-108	Dong-Seong Jeon,Hiroshi Ikeda,Masahiro Akamatsu,Ryozo Yoshizaki	Bi, Sr, Ca, Cu, O, Zn	
5852	PHC2530401		Sr2 Cu (O5,C)	Sr2Cu1C1O5	Sr	2	Cu	1	C	1															O	5			1995																											2					3.906		7.492																	4.2																																																																																																SrCO3, SrCuO2, NaCuO2, KCuO2		mixture-Pt or Au capsul-pressure(40Kbar)-heat(1000C,IH)-normal cond.(in 30 min), all operation in dyy box					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5853	PHC2530401		(Sr,Na)2(O2,CO3)	Sr1.85Na0.15Cu1C1O5	Sr	1.85	Na	0.15	Cu	1	C	1													O	5			1995																											2					3.902		7.484																	4.2																																																																																																SrCO3, SrCuO2, NaCuO2, KCuO2		mixture-Pt or Au capsul-pressure(40Kbar)-heat(1000C,IH)-normal cond.(in 30 min), all operation in dyy box					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5854	PHC2530401		(Sr,Na)2Cu(O2,CO3)	Sr1.7Na0.3Cu1C1O5	Sr	1.7	Na	0.3	Cu	1	C	1													O	5			1995																											2					3.893		7.491																	4.2																																																																																																SrCO3, SrCuO2, NaCuO2, KCuO2		mixture-Pt or Au capsul-pressure(40Kbar)-heat(1000C,IH)-normal cond.(in 30 min), all operation in dyy box					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5855	PHC2530401		(Sr,Na)2Cu(O2,Co3)	Sr1.4Na0.6Cu11O5	Sr	1.4	Na	0.6	Cu	11															O	5			1995																											2					3.889		7.493																	4.2																																																																																																SrCO3, SrCuO2, NaCuO2, KCuO2		mixture-Pt or Au capsul-pressure(40Kbar)-heat(1000C,IH)-normal cond.(in 30 min), all operation in dyy box					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5856	PHC2530401		(Sr,Na)2Cu(O2,CO3)	Sr1Na1Cu1C1O5	Sr	1	Na	1	Cu	1	C	1													O	5			1995																											2					3.885		7.493																	4.2																																																																																																SrCO3, SrCuO2, NaCuO2, KCuO2		mixture-Pt or Au capsul-pressure(40Kbar)-heat(1000C,IH)-normal cond.(in 30 min), all operation in dyy box					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5857	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.9K0.1Cu1CO5	Sr	1.9	K	0.1	Cu	1	C														O	5			1995																											2					3.897		7.507																	4.2																																																																																																							Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5858	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.8K0.2Cu1C1O5	Sr	1.8	K	0.2	Cu	1	C	1													O	5			1995																											2					3.896		7.519																	4.2																																																																																																							Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5859	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.75K0.25Cu1C1O5	Sr	1.75	K	0.25	Cu	1	C	1													O	5			1995																											2					3.892		7.52																13			13																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5860	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.7K0.3Cu1C1O5	Sr	1.7	K	0.3	Cu	1	C	1													O	5			1995																											2					3.891		7.519																16			16																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5861	PHC2530401	average x=0.16 by EDS analysis	(Sr,K)2Cu(O2,CO3)	Sr1.6K0.4Cu1C1O5	Sr	1.6	K	0.4	Cu	1	C	1													O	5			1995																											2					3.891		7.522																23			23																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5862	PHC2530401		(Sr,K)2Cu(O,CO3)	Sr1.5K0.5Cu1C1O5	Sr	1.5	K	0.5	Cu	1	C	1													O	5			1995																											2					3.889		7.523																20			20																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5863	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.4K0.6Cu1C1O5	Sr	1.4	K	0.6	Cu	1	C	1													O	5			1995																											2					3.888		7.528																21			21																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5864	PHC2530401		(Sr,K)2Cu(O2,CO3)	Sr1.3K0.7Cu1C1O5	Sr	1.3	K	0.7	Cu	1	C	1													O	5			1995																											2					3.888		7.524																20			20																																																																																																					Synthesis of alkali-substituted Sr,Cu oxycarbonates Superconductivity in Sr2-xKxCuO2CO3(0.25%$ x %$0.7)	199511		Department pf Chemistry, Moscow State University,119899 Moscow, Russian Federation	Physica C,253(1995)401-406	C. Chaillout,E.V. Antipov,J.J. Capponi,J.L. Tolence,M. Brunner,M. Marezio,S.M. Kazakov	Sr, K, Cu, O, C	
5865	PHC2530243		LaBa2(Cu,Co)3 O7	La1Ba2Cu3O6.89	La	1	Ba	2	Cu	3															O	z	6.89		1995																											3	Y123				3.893	3.925	11.775													70		82				76																																																																																														R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5866	PHC2530243		LaBa2(Cu,Co)3O7	La1Ba2Cu2.95Co0.05O6.94	La	1	Ba	2	Cu	2.95	Co	0.05													O	z	6.94		1995						3.7	30																				2	Y123				3.914		11.758													35		46				40.5																																																																																														R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5867	PHC2530243		LaBa2(Cu,Co)3O7	La1Ba2Cu2.9Co0.1O7.04	La	1	Ba	2	Cu	2.9	Co	0.1													O	z	7.04		1995						3.1	33																				2	Y123				3.918		11.743																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5868	PHC2530243	semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2.8Co0.2O7.01	La	1	Ba	2	Cu	2.8	Co	0.2													O	z	7.01		1995						3	35																				2	Y123				3.919		11.759																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5869	PHC2530243	semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2.7Co0.3O7.05	La	1	Ba	2	Cu	2.7	Co	0.3													O	z	7.05		1995						3.2	39																				3	Y123				3.916	3.922	11.763																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5870	PHC2530243	Semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2.5Co0.5O7.21	La	1	Ba	2	Cu	2.5	Co	0.5													O	z	7.21		1995						3.5	44																				3	Y123				3.915	3.93	11.765																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5871	PHC2530243	Semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2.3Co0.7O7.14	La	1	Ba	2	Cu	2.3	Co	0.7													O	z	7.14		1995						3.3	57																				3	Y123				3.906	3.936	11.771																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5872	PHC2530243	Semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2.1Co0.9O7.24	La	1	Ba	2	Cu	2.1	Co	0.9													O	z	7.24		1995						3.3	75																				3	Y123				3.902	3.939	11.796																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5873	PHC2530243	Semicon	LaBa2(Cu,Co)3O7	La1Ba2Cu2Co1O7.39	La	1	Ba	2	Cu	2	Co	1													O	z	7.39		1995						2.8	104																				3	Y123				3.892	3.932	11.808																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5874	PHC2530243		RBa2(Cu2Co)O7	Pr1Ba2Cu2Co1O7.33	Pr	1	Ba	2	Cu	2	Co	1													O	7+z	7.33		1995																											3	Y123				3.889	3.94	11.797																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5875	PHC2530243		RBa2(Cu2Co)O7	Nd1Ba2Cu2Co1O7.24	Nd	1	Ba	2	Cu	2	Co	1													O	7+z	7.24		1995																											3	Y123				3.896	3.918	11.777																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5876	PHC2530243		RBa2(Cu2Co)O7	Sm1Ba2Cu2Co1O7.12	Sm	1	Ba	2	Cu	2	Co	1													O	7+z	7.12		1995																											3	Y123				3.896	3.919	11.752																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5877	PHC2530243		RBa2(Cu2Co)O7	Gd1Ba2Cu2Co1O7.16	Gd	1	Ba	2	Cu	2	Co	1													O	7+z	7.16		1995																											3	Y123				3.893	3.911	11.716																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5878	PHC2530243		RBa2(Cu2Co)O7	Er1Ba2Cu2Co1O7.07	Er	1	Ba	2	Cu	2	Co	1													O	7+z	7.07		1995																											3	Y123				3.891	3.893	11.679																	4.2																																																																																																R2O3,BaO2,CuO,Co(C2O4).2H2O	1	mixture-CAL(925-950C,48H)-Q to RT(1C/min)-pellet-SIN(930C,10H)-ANN(350C,24H inflowing O2)-RT					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5879	PHC2530243		RBa2(Cu2Co)O7	La1Ba2Cu2Co1O7.01	La	1	Ba	2	Cu	2	Co	1													O	7-z	7.01		1995																											3	Y123				3.916	3.959	11.858																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5880	PHC2530243		RBa2(Cu2Co)O7	La1Ba2Cu2Co1O6.71	La	1	Ba	2	Cu	2	Co	1													O	7-z	6.71		1995																											2	Y123				3.951		11.843																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5881	PHC2530243		RBa2(Cu2Co)O7	Pr1Ba2Cu2Co1O7.02	Pr	1	Ba	2	Cu	2	Co	1													O	7-z	7.02		1995																											3	Y123				3.88	3.923	11.736																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5882	PHC2530243		RBa2(Cu2Co)O7	Pr1Ba2Cu2Co1O6.55	Pr	1	Ba	2	Cu	2	Co	1													O	7-z	6.55		1995																											2	Y123				3.927		11.753																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5883	PHC2530243		RBa2(Cu2Co)O7	Sm1Ba2Cu2Co1O6.62	Sm	1	Ba	2	Cu	2	Co	1													O	7-z	6.62		1995																											2	Y123				3.911		11.725																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5884	PHC2530243		RBa2(Cu2Co)O7	Gd1Ba2Cu2Co1O6.76	Gd	1	Ba	2	Cu	2	Co	1													O	7-z	6.76		1995																											2	Y123				3.898		11.701																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5885	PHC2530243		RBa2(Cu2Co)O7	Er1Ba2Cu2Co1O6.64	Er	1	Ba	2	Cu	2	Co	1													O	7-z	6.64		1995																											2	Y123				3.888		11.66																	4.2																																																																																																		desorption condition=heat (15C/min at E-5 torr)					Structural anomalies in RBa2Cu3-xCoxO7+-z (R= rare earth) defect perovskites	199511		Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore-560 012, India	Physica C,253(1995)243-253	A. Sequiera,G.N. Subbanna,H. Rajagopal,M.S. Hegde,N.Y. Vasanthacharya,S. Ramesh,S.K. Paranjpe	R, Ba, Cu, Co, O	
5886	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1995																												Hg1212																			92			110.7			110.7																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5887	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.1Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.1											O	z			1995																												Hg1212																						127.8			127.8																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5888	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.2Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.2											O	z			1995																												Hg1212																						128.8			128.8																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5889	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.3Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.3											O	z			1995																												Hg1212																						128.8			128.8																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5890	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.4Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.4											O	z			1995																												Hg1212																			126			131.4			131.4																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5891	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.5Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.5											O	z			1995																												Hg1212																						128.5			128.5																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5892	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.6Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.6											O	z			1995																												Hg1212																						130.1			130.1																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5893	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F0.8OZ	Hg	1	Ba	2	Ca	2	Cu	3	F	0.8											O	Z			1995																												Hg1212																						128.4			128.4																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5894	PHC2530357	Hirr for H//C	TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9	Tl	1	Ba	2	Ca	2	Cu	3													O	9		1	1995																												Tl1223																				118					118																																		HIR5894																																																														mixture-wraped in Au foil-heat(860-870C,30min in air)-Q to liq, N2-grain aligned in epoxy					Enhanced irreversibility fild and curret stabilization by Pb substitution in aligned Tl-1223 high-Tc superconductor	199511		Department of Physics, University of Tennessee, Knoxville TN 37996-1200,USA	Physica C,253(1995)357-366	D.K. Christen,E.D. Specht,J.R. Thompson,M. Paranthaman,Y.C. Kim	Ca, Pb, Tl, Ba, Cu, O	
5895	PHC2530357	Hirr for H//C	Tl(Ba,Sr)2Ca2Cu3O9	Tl1Ba1Sr1Ca2Cu3O9	Tl	1	Ba	1	Sr	1	Ca	2	Cu	3											O	9		1	1995																												Tl1223																				105					105																																		HIR5895																																																														mixture-wraped in Au foil-heat(860-870C,30min in air)-Q to liq, N2-grain aligned in epoxy					Enhanced irreversibility fild and curret stabilization by Pb substitution in aligned Tl-1223 high-Tc superconductor	199511		Department of Physics, University of Tennessee, Knoxville TN 37996-1200,USA	Physica C,253(1995)357-366	D.K. Christen,E.D. Specht,J.R. Thompson,M. Paranthaman,Y.C. Kim	Ca, Pb, Tl, Ba, Cu, O	
5896	PHC2530357	Hirr for H//C (P=2)  Hirr for H//ab (P=1)	(Tl,Pb)Sr2Ca2Cu3O9	Tl0.5Pb0.5Sr2Ca2Cu3O9	Tl	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	9		1	1995																												Tl1223																				112					112																																		HIR5896																																																														mixture-wraped in Au foil-heat(860-870C,30min in air)-Q to liq, N2-grain aligned in epoxy					Enhanced irreversibility fild and curret stabilization by Pb substitution in aligned Tl-1223 high-Tc superconductor	199511		Department of Physics, University of Tennessee, Knoxville TN 37996-1200,USA	Physica C,253(1995)357-366	D.K. Christen,E.D. Specht,J.R. Thompson,M. Paranthaman,Y.C. Kim	Ca, Pb, Tl, Ba, Cu, O	
5897	PHC2530271	as-grown crystal	Tl2Ba2CuO6	Tl2Ba2Cu2O6-z	Tl	2	Ba	2	Cu	2															O	6-z		3	1995																											2	Tl2201				3.86		23.2														80					80																																																																						TP5897																										using self-flux method,oxgen content by different heat treatment see comment					Anisotropic Seebeck coefficient in Tl2Ba2CuO6-z single crystals	199511		University of Arkansas, Fayetteville, AR 72701, USA	Physica C,253(1995)271-278	A.M. Hermann,H.M. Duan,W. Kiehl	Tl, Ba, Cu, O	
5898	PHC2530271	heat to 350C in air-then furnace cool	Tl2Ba2CuO6	Tl2Ba2Cu1O6-z	Tl	2	Ba	2	Cu	1															O	6-z		3	1995																												Tl2201																				20					20																																																																						TP5898																										using self-flux method,oxgen content by different heat treatment see comment					Anisotropic Seebeck coefficient in Tl2Ba2CuO6-z single crystals	199511		University of Arkansas, Fayetteville, AR 72701, USA	Physica C,253(1995)271-278	A.M. Hermann,H.M. Duan,W. Kiehl	Tl, Ba, Cu, O	
5899	PHC2530271	heat (350-450C,4H in air)-Q to RT	Tl2Ba2CuO6	Tl2Ba2Cu1O6-z	Tl	2	Ba	2	Cu	1															O	6-z		3	1995																												Tl2201																				55					55																																																																						TP5899																										using self-flux method,oxgen content by different heat treatment see comment					Anisotropic Seebeck coefficient in Tl2Ba2CuO6-z single crystals	199511		University of Arkansas, Fayetteville, AR 72701, USA	Physica C,253(1995)271-278	A.M. Hermann,H.M. Duan,W. Kiehl	Tl, Ba, Cu, O	
5900	PHC2530156		TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-z	Tl	1	Sr	2	Ca	1	Cu	2													O	7-z			1995																											2	Tl212				3.771		12.092																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5901	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.8Ce0.2Ca1Cu2O7-z	Tl	1	Sr	1.8	Ce	0.2	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.79		12.059																35			35																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5902	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.75Ce0.25Ca1Cu2O7-z	Tl	1	Sr	1.75	Ce	0.25	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.796		12.052																46.3			46.3																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5903	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.7Ce0.3Ca1Cu2O7-z	Tl	1	Sr	1.7	Ce	0.3	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.799		12.045																57.1			57.1																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5904	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.65Ce0.35Ca1Cu2O7-z	Tl	1	Sr	1.65	Ce	0.35	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.802		12.038																59.3			59.3																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5905	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.6Ce0.4Ca1Cu2O7-z	Tl	1	Sr	1.6	Ce	0.4	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.804		12.034																38.9			38.9																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5906	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.55Ce0.45Ca1Cu2O7-z	Tl	1	Sr	1.55	Ce	0.45	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.806		12.031																19.4			19.4																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5907	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.5Ce0.5Ca1Cu2O7-z	Tl	1	Sr	1.5	Ce	0.5	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.808		12.029																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5908	PHC2530156		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.4Ce0.6Ca1Cu2O7-z	Tl	1	Sr	1.4	Ce	0.6	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.807		12.028																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5909	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.7Ce0.3Cu2O7-z	Tl	1	Sr	2	Ca	0.7	Ce	0.3	Cu	2											O	7-z			1995																											2	Tl1212				3.801		12.086																51.5			51.5																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5910	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.65Ce0.35Cu2O7-z	Tl	1	Sr	2	Ca	0.65	Ce	0.35	Cu	2											O	7-z			1995																											2	Tl1212				3.806		12.085																60			60																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5911	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.6Ce0.4Cu2O7-z	Tl	1	Sr	2	Ca	0.6	Ce	0.4	Cu	2											O	7-z			1995																											2	Tl1212				3.81		12.084																35			35																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5912	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.55Ce0.45Cu2O7-z	Tl	1	Sr	2	Ca	0.55	Ce	0.45	Cu	2											O	7-z			1995																											2	Tl1212				3.814		12.084																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5913	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.5Ce0.5Cu2O7-z	Tl	1	Sr	2	Ca	0.5	Ce	0.5	Cu	2											O	7-z			1995																											2	Tl1212				3.818		12.084																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5914	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.4Ce0.6Cu2O7-z	Tl	1	Sr	2	Ca	0.4	Ce	0.6	Cu	2											O	7-z			1995																											2	Tl1212				3.825		12.083																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5915	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca3Ce0.7Cu2O7-z	Tl	1	Sr	2	Ca	3	Ce	0.7	Cu	2											O	7-z			1995																											2	Tl1212				3.827		12.082																	10																																																																																																Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5916	PHC2530156		TlSr2(Ca,Ce)Cu2O7	Tl1Sr2Ca0.8Ce0.2Cu2O7-z	Tl	1	Sr	2	Ca	0.8	Ce	0.2	Cu	2											O	7-z			1995																											2	Tl1212																						29.4			29.4																																																																																														Tl2O3,CeO2,SrCO3,CuO	1	mixture of Sr-Ce-Ca-Cu-O  CAl(800-850C,12H in Al2O3 crucibul)-(+Tl2O3)-pellet-wrapped in Au foil sealed (Iatm O2 in quartz)-heat(950C,2H)-air quench to RT					Effects of Ce on the crystal structure and supercoductivity in TlSr2CaCu2O7-z	199510		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica C,253(1995)156-164	D.C. Wang,W.H. Lee	Tl, Sr, Ca, Cu, O	
5917	PHC2440263			Pb2Sr0.9La1.1Cu2O6.31	Pb	2	Sr	0.9	La	1.1	Cu	2													O	6+z	6.31		1995																											3	Pb3201				5.305	5.416	12.655														33.2					33.2																																																																						TP5917												8.42												Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5918	PHC2440263			Pb2Sr0.9La1.1Cu2O6.65	Pb	2	Sr	0.9	La	1.1	Cu	2													O	6+z	6.65		1995																											3	Pb3201				5.309	5.42	12.655														30.3					30.3																																																																						TP5918																								Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5919	PHC2440263			Pb2Cu0.9La1.1Cu2O7.42	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	7.42		1995																											3	Pb3201				5.296	5.431	12.62														18.1					18.1																																																																						TP5919												31.6												Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5920	PHC2440263			Pb2Cu0.9La1.1Cu2O6.28	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	6.28		1995																											3	Pb3201				5.317	5.419	12.622														33.4					33.4																																																																						TP5920												9.47												Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5921	PHC2440263			Pb2Cu0.9La1.1Cu2O6.24	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	6.24		1995																											3	Pb3201				5.221	5.42	12.622														31.3					31.3																																																																						TP5921												21.47												Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5922	PHC2440263			Pb2Cu0.9La1.1Cu2O6.19	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	6.19		1995																																5.328	5.422	12.607														19.8					19.8																																																																						TP5922												20.84												Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5923	PHC2440263			Pb2Cu0.9La1.1Cu2O7.87	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	7.87		1995																											2					5.461		12.627																																																																																									TP5923																								Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5924	PHC2440263			Pb2Cu0.9La1.1Cu2O8.05	Pb	2	Cu	0.9	La	1.1	Cu	2													O	6+z	8.05		1995																											2					5.463		12.615																	4.2																																																																								TP5924																								Pb(NO3)2,Sr(CH3COO)2,H2O,La2O3,Cu(CH3COO		gel-method-pellet-SIN(750C,20H in flowingO2)-rapid cool to Liq,N2-ANN(475C,20H in flowing N2)-ANN for various z				ortho=100%	Effects of extra oxygen on the physical properties in the Pb3201 phase of (Pb2Cu)Sr0.9La1.1CuO6+z prepared by the polymerized complex method	199503		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan	Physica C.,244(1995)263-270	Akihoko Fujiwara,Atsushi Sakuma,Masatsune Kato,Takashi Noji,Toyoo Miyajima,Yoji Koike,Yoshitami Saito		
5925	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu3O6.899	Y	1	Ba	1	Sr	1	Cu	3													O	z	6.899		1995																											3					3.808	3.843	11.491														80.2					80.2																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5926	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.975Sn0.025O6.91	Y	1	Ba	1	Sr	1	Cu	2.975	Sn	0.025											O	z	6.91		1995																											3					3.81	3.847	11.489														76.3					76.3																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5927	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.95Sn0.05O6.96	Y	1	Ba	1	Sr	1	Cu	2.95	Sn	0.05											O	z	6.96		1995																											3					3.809	3.84	11.469														73.9					73.9																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5928	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.9Sn0.1O7.001	Y	1	Ba	1	Sr	1	Cu	2.9	Sn	0.1											O	z	7.001		1995																											3					3.812	3.842	11.471														68.6					68.6																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5929	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.85Sn0.15O7.062	Y	1	Ba	1	Sr	1	Cu	2.85	Sn	0.15											O	z	7.062		1995																											3					3.814	3.848	11.478														63.7					63.7																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5930	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.8Sn0.2O7.122	Y	1	Ba	1	Sr	1	Cu	2.8	Sn	0.2											O	z	7.122		1995																											3					3.815	3.852	11.477														49.3					49.3																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5931	PHC2520381		YBaSr(Cu,Sn)3O7	Y1Ba1Sr1Cu2.75Sn0.25O7.163	Y	1	Ba	1	Sr	1	Cu	2.75	Sn	0.25											O	z	7.163		1995																											3					3.815	3.853	11.49														40.9					40.9																																																																																														Y2O3,BaCo3,SrCO3,CuO,SnO2		mixture-fire(930C,20H in air)-reground-heat(935C,24H)-pellet-SIN(950C,20H)-ANN(500C,60H in flowing O2)cool to RT(25C/H)					The mechanism of superconductivity suppression in the YBaSrCu3-xSnxOy system	199510		(a)Superconductivity Research Group,School of Materials Sciense and Engineering,University of New South Wales, Sydney	Physica c,252(1995)381-388	B. Chen,F. Wang,H. Kennedy,H. Zhang,Y. Zhao	Y, Ba, Sr, Cu, Sn, O	
5932	PHC2530254		HgBa2Ca2Cu3(F,O)z	Hg1Ba2Ca2Cu3F1Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	1											O	z			1995																												Hg1212																						124.9			124.9																																																																																														Ba(NO3)2,Ca(NO3)2,4H2O,Cu(ND3)2,H2O	1	Powder mixture+HgO+CuF2-seal in quartz-SIN(650-800C,10H)-Fc to RT, F-content by ion-chosen cathode				F occupy O-site	effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
5933	PHC2540355			Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	1995																												Bi2212																				92					92																																										estimated from ESR	3100																																																			Bi2Sr2CaCu2O8		sol-gel method					Magnetic penetration depth in polycrystalline Bi-2212 Bi2Sr2Ca1-xNaxCu2O8+z (x=0-0.3)	199511		School of Physics, Univarecity of Hyderabad, Hyderabad-505 134, India	Physica.C,254(1995)355-358	Ajay Mohan Suvarna,C.S. Sunandana	Bi, Sr, Ca, Na, Cu, O	
5934	PHC2540355			Bi2Sr2Ca0.9Na0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Na	0.1	Cu	2											O	8+z		2	1995																												Bi2212																				81					81																																										estimated from ESR	2782																																																			Bi2Sr2CaCu2O8		sol-gel method					Magnetic penetration depth in polycrystalline Bi-2212 Bi2Sr2Ca1-xNaxCu2O8+z (x=0-0.3)	199511		School of Physics, Univarecity of Hyderabad, Hyderabad-505 134, India	Physica.C,254(1995)355-358	Ajay Mohan Suvarna,C.S. Sunandana	Bi, Sr, Ca, Na, Cu, O	
5935	PHC2540355			Bi2Sr2Ca0.8Na0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Na	0.2	Cu	2											O	8+z		2	1995																												Bi2212																				83					83																																										estimated from ESR	2587																																																			Bi2Sr2CaCu2O8		sol-gel method					Magnetic penetration depth in polycrystalline Bi-2212 Bi2Sr2Ca1-xNaxCu2O8+z (x=0-0.3)	199511		School of Physics, Univarecity of Hyderabad, Hyderabad-505 134, India	Physica.C,254(1995)355-358	Ajay Mohan Suvarna,C.S. Sunandana	Bi, Sr, Ca, Na, Cu, O	
5936	PHC2540355			Bi2Sr2Ca0.7Na0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Na	0.3	Cu	2											O	8+z		2	1995																												Bi2212																				86					86																																										estimated from ESR	2152																																																			Bi2Sr2CaCu2O8		sol-gel method					Magnetic penetration depth in polycrystalline Bi-2212 Bi2Sr2Ca1-xNaxCu2O8+z (x=0-0.3)	199511		School of Physics, Univarecity of Hyderabad, Hyderabad-505 134, India	Physica.C,254(1995)355-358	Ajay Mohan Suvarna,C.S. Sunandana	Bi, Sr, Ca, Na, Cu, O	
5937	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95	3	1995																											3	Y123																				93.2					93.2																																										calculated from reflectance measurement	10600																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5938	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	z	6.9	3	1995																											3	Y123																				91.5					91.5																																										calculated from reflectance measurement	15800																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5939	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	z	6.85	3	1995																											3	Y123																				89					89																																										calculated from reflectance measurement	20300																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5940	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	3	1995																											3	Y123																				78					78																																										calculated from reflectance measurement	33700																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5941	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7	3	1995																											3	Y123																				63					63																																										calculated from reflectance measurement	51700																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5942	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	z	6.6	3	1995																											3	Y123																				58					58																																										calculated from reflectance measurement	65200																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5943	PHC2540265		YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	z	6.5	3	1995																											3	Y123																				53					53																																										calculated from reflectance measurement	78000																																																			Y2O3,CuO,BaCO3		Crystals were grown by flux method in YSZ crucible,heat (1010C,4H)-(990C,8-16H)-cool to 950-970C (0.3-0.8C/H)-cool to RT (150C/H)-ANN for O-control					Optical properties along the c-axis of YBaCu3O6+x, for x =0.50-0.95 Evolution of the pseudogap	199511		(a)Department of Physics and Astronomy,McMaster University, Hamilton, Ont.,L8S 4M1, Canada (b)Department of Physics, University of British Columbia, Vancouver,B.C. V6T 2A6, Canada	Physica. C,254(1995)265-280	C.C. Homes,D.A. Bonn,R. Liang,T. Timusk,W.N. herdy	Y, Ba, Cu, O	
5944	PHC2550037			Nd2Ba2Ti1.9Cu2.1O11	Nd	2	Ba	2	Ti	1.9	Cu	2.1													O	11		1	1995				2.6		3.2	-60																				2		P4/mmm			3.91		15.759																	15																																																																																																Nd2O3,BaCO3,CaCO3,CeO2,TiO2,CuO		mixture-pellet-heat (920-940C,30min in alumina crucible in air					Electrical properties and crystal structures of homologous series of oxides   Nd2Ba2CamCenTi2-zCu2+zO11+m+2n (m,n=0 or 1)	199512		(a)Canon Research Center,5-1Morinosato-Wakamiya,Atsugi,Kanagawa243-01,Japan (b)National Insutute for Research in Inorganic Matelials,1-1 Namiki, Thukuba, Ibaraki,Japan	Physica.C,255(1995)37-52	F. Izumi,T. Den,T. Kamiyama,T. Kobatashi,Y. Shimakawa	Nd, Ba, Ca, Ce, Ti, Cu, O	
5945	PHC2550037			Nd2Ba2Ca1Ti1.92Cu2.08O12	Nd	2	Ba	2	Ca	1	Ti	1.92	Cu	2.08											O	12		1	1995				2.8		3.3	-56																				2		I4/mmm			3.905		35.863																	15																																																																																																Nd2O3,BaCO3,CaCO3,CeO2,TiO2,CuO		mixture-pellet-heat (920-940C,30min in alumina crucible in air					Electrical properties and crystal structures of homologous series of oxides   Nd2Ba2CamCenTi2-zCu2+zO11+m+2n (m,n=0 or 1)	199512		(a)Canon Research Center,5-1Morinosato-Wakamiya,Atsugi,Kanagawa243-01,Japan (b)National Insutute for Research in Inorganic Matelials,1-1 Namiki, Thukuba, Ibaraki,Japan	Physica.C,255(1995)37-52	F. Izumi,T. Den,T. Kamiyama,T. Kobatashi,Y. Shimakawa	Nd, Ba, Ca, Ce, Ti, Cu, O	
5946	PHC2550037			Nd2Ba2Ce1Ti2Cu2O13	Nd	2	Ba	2	Ce	1	Ti	2	Cu	2											O	13		1	1995				2.7		3.3	-54																				2		I4/mmm			3.9		36.962																	15																																																																																																Nd2O3,BaCO3,CaCO3,CeO2,TiO2,CuO		mixture-pellet-heat (920-940C,30min in alumina crucible in air					Electrical properties and crystal structures of homologous series of oxides   Nd2Ba2CamCenTi2-zCu2+zO11+m+2n (m,n=0 or 1)	199512		(a)Canon Research Center,5-1Morinosato-Wakamiya,Atsugi,Kanagawa243-01,Japan (b)National Insutute for Research in Inorganic Matelials,1-1 Namiki, Thukuba, Ibaraki,Japan	Physica.C,255(1995)37-52	F. Izumi,T. Den,T. Kamiyama,T. Kobatashi,Y. Shimakawa	Nd, Ba, Ca, Ce, Ti, Cu, O	
5947	PHC2550037			Nd2Ba2Ca1Ce1Ti1.9Cu2.1O14	Nd	2	Ba	2	Ca	1	Ce	1	Ti	1.9	Cu	2.1									O	14		1	1995				2.7		3.3	-60																				2		P4/mmm			3.897		20.604																	15																																																																																																Nd2O3,BaCO3,CaCO3,CeO2,TiO2,CuO		mixture-pellet-heat (920-940C,30min in alumina crucible in air					Electrical properties and crystal structures of homologous series of oxides   Nd2Ba2CamCenTi2-zCu2+zO11+m+2n (m,n=0 or 1)	199512		(a)Canon Research Center,5-1Morinosato-Wakamiya,Atsugi,Kanagawa243-01,Japan (b)National Insutute for Research in Inorganic Matelials,1-1 Namiki, Thukuba, Ibaraki,Japan	Physica.C,255(1995)37-52	F. Izumi,T. Den,T. Kamiyama,T. Kobatashi,Y. Shimakawa	Nd, Ba, Ca, Ce, Ti, Cu, O	
5948	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.3Ba1.45La1.25Cu3O6.96	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	6.96		1995																											2	Y123																			9.6						9.6																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5949	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.3Ba1.45La1.25Cu3O7	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	7		1995																											2	Y123																			28.3						28.3																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5950	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.3Ba1.45La1.25Cu3O7.05	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	7.05		1995																											2	Y123																			46.4						46.4																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5951	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.3Ba1.45La1.25Cu3O7.11	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	7.11		1995																											2	Y123																			65.3						65.3																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5952	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.3Ba1.45La1.25Cu3O7.12	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	7.12		1995																											2	Y123																			69.3						69.3																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5953	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O6.98	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	6.98		1995																											2	Y123																			10.4						10.4																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5954	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O6.99	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	6.99		1995																											2	Y123																			14.4						14.4																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5955	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.01	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.01		1995																											2	Y123																			25.1						25.1																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5956	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.03	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.03		1995																											2	Y123																			34.7						34.7																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5957	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.05	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.05		1995																											2	Y123																			41.1						41.1																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5958	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.07	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.07		1995																											2	Y123																			46.1						46.1																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5959	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.11	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.11		1995																											2	Y123																			59.7						59.7																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5960	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.25La1.35Cu3O6.99	Ca	0.4	Ba	1.25	La	1.35	Cu	3													O	z	6.99		1995																											2	Y123																							4.2																																																																																																							Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5961	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.25La1.35Cu3O7.04	Ca	0.4	Ba	1.25	La	1.35	Cu	3													O	z	7.04		1995																											2	Y123																			21.3						21.3																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5962	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.25La1.35Cu3O7.11	Ca	0.4	Ba	1.25	La	1.35	Cu	3													O	z	7.11		1995																											2	Y123																			47.1						47.1																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5963	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.25La1.35Cu3O7.16	Ca	0.4	Ba	1.25	La	1.35	Cu	3													O	z	7.16		1995																											2	Y123																			63.5						63.5																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5964	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.25La1.35Cu3O7.19	Ca	0.4	Ba	1.25	La	1.35	Cu	3													O	z	7.19		1995																											2	Y123																			72.9						72.9																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5965	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.1Ba1.65La1.25Cu3O7.01	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O	z	7.01		1995																											2	Y123																			19.5						19.5																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5966	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.1Ba1.65La1.25Cu3O7.02	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O	z	7.02		1995																											2	Y123																			26.4						26.4																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5967	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.1Ba1.65La1.25Cu3O7.03	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O	z	7.03		1995																											2	Y123																			29.9						29.9																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5968	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.1Ba1.65La1.25Cu3O7.08	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O	z	7.08		1995																											2	Y123																			45.9						45.9																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5969	PR05212982		(La,Ca)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.9	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O	z	6.9		1995																											2	Y123																			5						5																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5970	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.92	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O	z	6.92		1995																											2	Y123																			14.4						14.4																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5971	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.95	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O	z	6.95		1995																											2	Y123																			24.8						24.8																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5972	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.35La1.25Cu3O7.08	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O	z	7.08		1995																											2	Y123																			68.6						68.6																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5973	PR05212982		(La,Ca)(Ba,La)2 Cu3O7	Ca0.4Ba1.35La1.25Cu3O7.15	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O	z	7.15		1995																											2	Y123																			78.8						78.8																																																																																																					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
5974	PHC2520079			Y1Sr2Cu2.7Mo0.3O7-z	Y	1	Sr	2	Cu	2.7	Mo	0.3													O	7-z		1	1995																											2	Y123			A	3.81		11.538														33.2					33.2																																																																																														Y2O3,Pr6O11,Gd2O3,Tb4O7,CuO,SrCO3,MoO3		mixture-SIN(1020C,3H in O2)-slow cool to RT in flowing O2					Superconductivity and magnetic order in RSr2Mo0.3O7-z (R=Y,Pr,Gd,and Tb)	199510		(a)Department of Electrical Engineering,National Sun Yat-Sen University, 80424, Taiwan (b)Department of Physics, National Sun  Yat-Sen University, Kaohsiung 80424,Taiwan (c)Department of Physics,National Chung University,Ming-Hsiung,China-Yi 621,Taiwan	Physica C,252(1995)79-86	C.R. Shih (a,b),H.D. Yang (b),H.L. Tsay (a,b),T.H. Meen (b),W.H. Lee (c),Y.C. Chen (a)	Y, Pr, Gd, Tb, Sr, Cu, O, Mo	
5975	PHC2520079			Pr1Sr2Cu2.7Mo0.3O7-z	Pr	1	Sr	2	Cu	2.7	Mo	0.3													O	7-z		1	1995	emu/g	0.00075			myu-B/mol	3.05	-17.8																				2	Y123			A	3.858		11.616																	10																																																																																																Y2O3,Pr6O11,Gd2O3,Tb4O7,CuO,SrCO3,MoO3		mixture-SIN(1020C,3H in O2)-slow cool to RT in flowing O2					Superconductivity and magnetic order in RSr2Mo0.3O7-z (R=Y,Pr,Gd,and Tb)	199510		(a)Department of Electrical Engineering,National Sun Yat-Sen University, 80424, Taiwan (b)Department of Physics, National Sun  Yat-Sen University, Kaohsiung 80424,Taiwan (c)Department of Physics,National Chung University,Ming-Hsiung,China-Yi 621,Taiwan	Physica C,252(1995)79-86	C.R. Shih (a,b),H.D. Yang (b),H.L. Tsay (a,b),T.H. Meen (b),W.H. Lee (c),Y.C. Chen (a)	Y, Pr, Gd, Tb, Sr, Cu, O, Mo	
5976	PHC2520079			Gd1Sr2Cu2.7Mo0.3O7-z	Gd	1	Sr	2	Cu	2.7	Mo	0.3													O	7-z		1	1995	emu/g	0.001			myu-B/mol	7.92	-4.5	2.27																			2	Y123			A	3.829		11.551														25.7					25.7																																																																																														Y2O3,Pr6O11,Gd2O3,Tb4O7,CuO,SrCO3,MoO3		mixture-SIN(1020C,3H in O2)-slow cool to RT in flowing O2					Superconductivity and magnetic order in RSr2Mo0.3O7-z (R=Y,Pr,Gd,and Tb)	199510		(a)Department of Electrical Engineering,National Sun Yat-Sen University, 80424, Taiwan (b)Department of Physics, National Sun  Yat-Sen University, Kaohsiung 80424,Taiwan (c)Department of Physics,National Chung University,Ming-Hsiung,China-Yi 621,Taiwan	Physica C,252(1995)79-86	C.R. Shih (a,b),H.D. Yang (b),H.L. Tsay (a,b),T.H. Meen (b),W.H. Lee (c),Y.C. Chen (a)	Y, Pr, Gd, Tb, Sr, Cu, O, Mo	
5977	PHC2520079			Tb1Sr2Cu2.7Mo0.3O7-z	Tb	1	Sr	2	Cu	2.7	Mo	0.3													O	7-z		1	1995	emu/g	0			myu-B/mol	9.75	-16.1	5.43																			2	Y123			A	3.825		11.547														29.8					29.8																																																																																														Y2O3,Pr6O11,Gd2O3,Tb4O7,CuO,SrCO3,MoO3		mixture-SIN(1020C,3H in O2)-slow cool to RT in flowing O2					Superconductivity and magnetic order in RSr2Mo0.3O7-z (R=Y,Pr,Gd,and Tb)	199510		(a)Department of Electrical Engineering,National Sun Yat-Sen University, 80424, Taiwan (b)Department of Physics, National Sun  Yat-Sen University, Kaohsiung 80424,Taiwan (c)Department of Physics,National Chung University,Ming-Hsiung,China-Yi 621,Taiwan	Physica C,252(1995)79-86	C.R. Shih (a,b),H.D. Yang (b),H.L. Tsay (a,b),T.H. Meen (b),W.H. Lee (c),Y.C. Chen (a)	Y, Pr, Gd, Tb, Sr, Cu, O, Mo	
5978	PHC2520221		(Cu,S)Sr2Can-1CunOz	Cu0.5S0.5Sr2Ca2Cu3O12	Cu	0.5	S	0.5	Sr	2	Ca	2	Cu	3											O	z	12		1995																											2	Cu1223				3.85		14.322											(Cu,S)-1223					100			100																																																																																														SrCuO2,Ca2CuO3,SrO2,CuSO4,CuO		starting materials were prepared by solid state reaction nominal 1234-mixtuo-seal(Au capsule)-react(1250C,6GPa)					New series of oxysulphate superconductors (Cu0.5S0.5)sr2Can-1CunOy (n=3-7),prepared at high pressure	199510		(a)Ntional Institute for Reserch in Inorganic Materials (NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan (b)Institute of Applied Physics, University of Tsukuba,Ibaraki,305 Japan	Physica C,252(1995)221-228	E. Takayama-Muromachi (a),J. Ramirez-Castellanos (a,b),Y. Matsui (a)	Cu, S, Sr, Ca, Cu, O	
5979	PHC2520221		(Cu,S)Sr2Can-1CunOz	Cu0.5S0.5Sr2Ca4Cu5Oz	Cu	0.5	S	0.5	Sr	2	Ca	4	Cu	5											O	z			1995																											2	Cu1245				3.854		20.883											(Cu,S)-1245				100	74			74																																																																																														SrCuO2,Ca2CuO3,SrO2,CuSO4,CuO		starting materials were prepared by solid state reaction nominal 1234-mixtuo-seal(Au capsule)-react(1250C,6GPa)					New series of oxysulphate superconductors (Cu0.5S0.5)sr2Can-1CunOy (n=3-7),prepared at high pressure	199510		(a)Ntional Institute for Reserch in Inorganic Materials (NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan (b)Institute of Applied Physics, University of Tsukuba,Ibaraki,305 Japan	Physica C,252(1995)221-228	E. Takayama-Muromachi (a),J. Ramirez-Castellanos (a,b),Y. Matsui (a)	Cu, S, Sr, Ca, Cu, O	
5980	PHC2520221		(Cu,S)Sr2Can-1CunOz	Cu0.5S0.5Sr2Ca5Cu6Oz	Cu	0.5	S	0.5	Sr	2	Ca	5	Cu	6											O	z			1995																											2	Cu1256				3.855		24.163											(Cu,S)-1256				100	67			67																																																																																														SrCuO2,Ca2CuO3,SrO2,CuSO4,CuO		starting materials were prepared by solid state reaction nominal 1234-mixtuo-seal(Au capsule)-react(1250C,6GPa)					New series of oxysulphate superconductors (Cu0.5S0.5)sr2Can-1CunOy (n=3-7),prepared at high pressure	199510		(a)Ntional Institute for Reserch in Inorganic Materials (NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan (b)Institute of Applied Physics, University of Tsukuba,Ibaraki,305 Japan	Physica C,252(1995)221-228	E. Takayama-Muromachi (a),J. Ramirez-Castellanos (a,b),Y. Matsui (a)	Cu, S, Sr, Ca, Cu, O	
5981	PHC2520221		(Cu,S)Sr2Can-1CunOz	Cu0.5S0.5Sr2Ca6Cu7Oz	Cu	0.5	S	0.5	Sr	2	Ca	6	Cu	7											O	z			1995																											2	Cu1267				3.857		27.326											(Cu,S)-1267				100	63			63																																																																																														SrCuO2,Ca2CuO3,SrO2,CuSO4,CuO		starting materials were prepared by solid state reaction nominal 1234-mixtuo-seal(Au capsule)-react(1250C,6GPa)					New series of oxysulphate superconductors (Cu0.5S0.5)sr2Can-1CunOy (n=3-7),prepared at high pressure	199510		(a)Ntional Institute for Reserch in Inorganic Materials (NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan (b)Institute of Applied Physics, University of Tsukuba,Ibaraki,305 Japan	Physica C,252(1995)221-228	E. Takayama-Muromachi (a),J. Ramirez-Castellanos (a,b),Y. Matsui (a)	Cu, S, Sr, Ca, Cu, O	
5982	PHC2520100		(Y,Ca)Ba2Cu3O6	Y1Ba2Cu3O6.007	Y	1	Ba	2	Cu	3															O	6	6.007		1995																											2					3.86		11.834																	4.2																																																																																																BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5983	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.95Ca0.05Ba2Cu3O6.06	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	6	6.06		1995																											2					3.858		11.836																	4.2																																																																																																BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5984	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.9Ca0.1Ba2Cu3O6.049	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	6	6.049		1995																											2					3.858		11.827																	4.2																																																																																																BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5985	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.82Ca0.18Ba2Cu3O6.008	Y	0.82	Ca	0.18	Ba	2	Cu	3													O	6	6.008		1995																											2					3.856		11.83																	4.2																																																																																																BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5986	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.8Ca0.2Ba2Cu3O6	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	6	6		1995																											2					3.855		11.831													14.7		33.3				24																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5987	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.77Ca0.23Ba2Cu3O6	Y	0.77	Ca	0.23	Ba	2	Cu	3													O	6	6		1995																											2					3.855		11.831													15.8		34.5				25.15																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5988	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.75Ca0.25Ba2Cu3O6.008	Y	0.75	Ca	0.25	Ba	2	Cu	3													O	6	6.008		1995																											2					3.856		11.833													24.4		45.3				34.85																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
5989	PHC2520049	TEP(max)=112K(2.8microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	z			1995																												Bi2223																				110					110																																																																			-2.5																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5990	PHC2520049	TEP(max)=114K(3.0microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.99Sm0.01Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.99	Sm	0.01	Cu	3									O	z			1995																												Bi2223																				107					107																																																																			-2.4																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5991	PHC2520049	114k(4.0microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.98Sm0.02Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.98	Sm	0.02	Cu	3									O	z			1995																												Bi2223																				105					105																																																																			-2.1																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5992	PHC2520049	112K(7.2microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.95Sm0.05Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.95	Sm	0.05	Cu	3									O	z			1995																												Bi2223																				76					76																																																																			-1.8																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5993	PHC2520049	124K(9.0microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca0.925Sm0.075Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	0.925	Sm	0.075	Cu	3									O	z			1995																												Bi2223																				75					75																																																																			-1.2																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5994	PHC2520049	130K(13microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.9Sm0.1Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.9	Sm	0.1	Cu	3									O	z			1995																												Bi2223																																																																																												-0.8																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5995	PHC2520049	TEP(max)=132K(28.4microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.8Sm0.2Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.8	Sm	0.2	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					1.4																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5996	PHC2520049	TEP(max)=132K(28.4microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.7Sm0.3Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.7	Sm	0.3	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					4.2																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5997	PHC2520049	TEP(max)=150K(20.0microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.5Sm0.5Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.5	Sm	0.5	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					15																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5998	PHC2520049	TEP(max)=132K(28,4microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca1.25Sm0.75Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1.25	Sm	0.75	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					22																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
5999	PHC2520049	TEP(max)=150K(30microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2cu3O10	Bi1.7Pb0.3Sr2Ca1Sm1Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Sm	1	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					40																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
6000	PHC2520049	TEP(max)=150K(60microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Ca0.5Sm1.5Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	0.5	Sm	1.5	Cu	3									O	z			1995																												Bi2223																							4.2																																																																					60.5																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
6001	PHC2520049	TEP(max)=150K(60microV/K)	(Bi,Pb)2Sr2(Ca,Sm)2Cu3O10	Bi1.7Pb0.3Sr2Sm2Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Sm	2	Cu	3											O	z			1995																												Bi2223																							4.2																																																																					140																												1	see Physica C 204(1993) 299					Thermoelectric power studies on the Sm substituted BPSCCO (2223) superconductors	199510		(a)Dept. of Physics,Osmania University,Hyderabad-500 007, India  (b)Lavoratoire de Dhimie du Solide et Inorganique Moleculaire,URA CNRS 1495,Universite' de Rennes,35942 Rennes Cadex, France	Physica C,252(1995)49-53	K. Nanda Kishore (a),M. Muralidhar (a),O. Pena (b),S. Satyavathi (a),V. Hari Babu (a)	Bi, Pb, Sr, Ca, Cu, O	
6002	PHC2540007		(Hg,Pb)Ba2Ca4Cu5O12	Hg0.5Pb0.5Ba2Ca4Cu5O12.5	Hg	0.5	Pb	0.5	Ba	2	Ca	4	Cu	5											O	12.5		3	1995																											2	Hg1245	P4/mmm			3.853		22.172																110		5	110																																																																																															5	grown by gas-phase high-press technique using PbO flux. 10-20 at % PbO+Hg1223-heat(1050-1070C,Ar P=10kbar)-1020C(5C/min)-860C(5C/min)-ANN(860C,2H)-RT				TCWIDTH by magnetiqation,averag Hg:Pb:Ba:Ca:Cu=0.49:0.48:2.0:3.97:4.98	X-ray single crystal structure analysis of the 1245 type supercoductor Hg0.5Pb0.5Ba2Ca4Cu5O12+z	199511		"Laboratorium fu'r FestKo""rpephysik,ETH Ho""nggerberg, CH-8093 Zu""rich,Swizerland"	Physica C,254(1995)7-14	A. Morawski,A. Paszewin,C. Rossel,H. Schwer,J. Karpinski,L. Lesne,T. Lada	Hg, Pb, Ba, Ca, Cu, O	
6003	PHC2530109		(Tl,Bi)(Sr,Ba)2Ca2Cu3O9	Tl0.8Bi0.2Sr1.6Ba0.4Ca2Cu3O9-z	Tl	0.8	Bi	0.2	Sr	1.6	Ba	0.4	Ca	2	Cu	3									O	9-z			1995									6.017																		2	Tl1223	P4/mmm			3.821		15.424																113			113																																																																																														Tl2O3,Bi2O3,(Sr1.6Ba0.4)Ca2Cu3O7	1	mixture-heat(920C,6H in O2)-pellet-wrapped in Au foil				Jc=1.62 E+7 A/cm2 At 5K, H=1T	Structure and supercoducting properties of (Tl0.8Bi0.2) (Sr1.6Ba0.4) Ca2Cu3O9-z	199510		Solid State Division, Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, TN 37831-6061, USA	Physica C,253(1995)109-114	B.C. Chakoumakos,D.K. Christen,J.R. Thompson,M. Paranthaman,N.H. Hur	Tl, Bi, Sr, Ba, Ca, Cu, O	
6004	PHC1660405		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																										SV6004		Bi2212						30.86															85				85																																																																																														BiO3,SrCO3,CaCO3,CUO		mixture-heat (900C,2H in Pt crucible)-cool to 800C(5C/H)-FC to RT				siqe=3*3*0.5mm3,sound velocity (p=for longtudinal, p=2for shear mode),pulse echo method(15MHz)	SOUND VELOCITY IN BI2SR2CACU2O8 SINGLE CRYSTALS		SOUND VELOCITY      ,SINGLE CRYSTALS     ,SHERA MODULUS	CENTRE DE RECHERCHES SUR LES TRES BASSED TEMPREATURES,CNRS,BP166 X,38042 GRENOBLE-CEKEX,FRANCE	PHYSICA C,166(1990)405	J.L.THOLENCE,M.SAINT-PAUL	BI,SR,CA,CU,O	
6005	PR04816869		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1993																																															74						74																																																																																																high-pressure flux method				Resistivity=0.49 mOhm,cm for I//a,0.145 for I//b at RT, RH (P= for I//a,P=2 for I//2)	Anisotropy and double sign change of the Hall resistivity in YBa2Cu4O8 single crystals	199312		Laboratorium fur Festkorperphysik, Eidgenossische Technische Hochschule-Zurich, CH-8093 Zurich, Swizerland	Phys.Rev.B,48(1993)16869	E. Kaldis,J. Karpinski,J. Schoenes		
6006	PHC2580279		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1996																												Y124																				72					72																																																																																										4	RH6006					high-pressure synthesis,see J,Less-Common Metals 164d165(1990)3				restivity by ac method,single crystal=300*400*20mixo-m3, Hall eflect P=1 foeI//a,P=2 for I//b	Hall effect measurements on YBa2Cu4O8 single crystals			"Laboratorium f""ur Festko""rperphysik, ETH-Zu""rich, zu""rich, Swizerland"	Physica.C.258,(1996)279-283	"H. Schwer,J. Karpinski,J. Lo""hle,P. Wachter"	Y,Ba,Cu,O	
6007	PRL0702012		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1993																												Y124																																																																																																																				RH6007					crystal was grown with a high-pressureflux method using BaO-CuO rich flux (640bar O2, 1040C)				Hall coeff,mearured for I//a-axis,H//c-axis resistivity and hall angle mearured for I//a and I//b	Influence of the Spin Gap on the Normal State Transport in YBa2Cu4O8	199303		Laboratorium Fur Festkorperphysik, Eidgenosssiche, Technische Hochschule Zurich, CH-8093 Zurich, Swizerland	Phys.Rev.Lett.70(1993)2012	B. Bucher,E. Kaldis,J. Karpinski,P. Steiner,P. Wachter		
6008	PHC2460207			Hg1Ba2Ca2Cu3O8.22	Hg	1	Ba	2	Ca	2	Cu	3													O	z	8.22	1	1995																											2	Hg1223																			110						110										25																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6009	PHC2460207			Hg0.9Pb0.1Ba2Ca2Cu3O8.25	Hg	0.9	Pb	0.1	Ba	2	Ca	2	Cu	3											O	z	8.25	1	1995																											2	Hg1223																			118						118										30																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6010	PHC2460207			Hg0.8Pb0.2Ba2Ca2Cu3O8.3	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	z	8.3	1	1995																											2	Hg1223																			125						125										55																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6011	PHC2460207			Hg0.7Pb0.3Ba2Ca2Cu3O8.35	Hg	0.7	Pb	0.3	Ba	2	Ca	2	Cu	3											O	z	8.35	1	1995																											2	Hg1223																			130						130										85																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6012	PHC2460207			Hg0.6Pb0.4Ba2Ca2Cu3O8.4	Hg	0.6	Pb	0.4	Ba	2	Ca	2	Cu	3											O	z	8.4	1	1995																											2	Hg1223																			120						120										42																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6013	PHC2460207			Hg0.5Pb0.5Ba2Ca2Cu3O8.45	Hg	0.5	Pb	0.5	Ba	2	Ca	2	Cu	3											O	z	8.45	1	1995																											2	Hg1223																			103						103										13																																																																																				HgO,PbO,BaO,CaO,CuO	1	Mixture-pellet-seal in vac quarty tube-heat(750-850C) at (4C/min)-SIN(750-850C,3-10H)-cool to 200C(4C/min)-FC				oxygen content by EPMA	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6014	PHC2460207		HgBa2Ca2Cu3Oy	Hg0.66Pb0.34Ba2Ca1.98Cu2.9O8.4	Hg	0.66	Pb	0.34	Ba	2	Ca	1.98	Cu	2.9											O	8.4	8.4	1	1995																											2	Hg1223				3.848		15.918													135			143			143																																																																																															1	6008  +ANN(240C,10H in O2 flow)-Q to RT in dry box				Hg1223 bhace volume fraction>90%	The synthesis and characterization of HgBa2Ca2Cu3O8+z superconductors with substitution of Hg by Pb	199505		Department of Physics and National Laboratory of Solid State Microstructures,Centre for Advanced Studies in Science and Technology of Microstructure,Nanjing University,Nanjing 210093,China	Physica C.,246(1995)207-215	C.C.Lam,G.J.Shen,H.M.Shao,J.C.L.Chow,J.H.Du,K.C.Hung,P.C.W.Fung,S.L.Ho,X.S.Xu,X.X.Yao		
6015	PHC2540151		RuSr2SmCu2O8	Ru1Sr2Sm1Cu2O8	Ru	1	Sr	2	Sm	1	Cu	2													O	8			1995																											2	Ru1212				3.852		11.56																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6016	PHC2540151		RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8			1995																											2	Ru1212				3.843		11.55																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6017	PHC2540151		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			1995																											2	Ru1212				3.838		11.53																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6018	PHC2540151		NbSr2SmCu2O8	Nb1Sr2Sm1Cu2O8	Nb	1	Sr	2	Sm	1	Cu	2													O	8			1995																											2	Nb1212				3.877		11.64																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6019	PHC2540151		NbSr2EuCu2O8	Nb1Sr2Eu2Cu2O8	Nb	1	Sr	2	Eu	2	Cu	2													O	8			1995																											2	Nb1212				3.872		11.63																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6020	PHC2540151		NbSr2GdCu2O8	Nb1Sr2Gd1Cu2O8	Nb	1	Sr	2	Gd	1	Cu	2													O	8			1995																											2	Nb1212				3.869		11.62																	4.2																																																																																																RuO2,Nb2O5,CuO,CeO2,R2O2	1	mixture-CAL(970C,24H)-pellet-SIN(1000-1060C for Nb1050-1080 for Ru,72H)					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6021	PHC2540151		RuSr2(Sm,Ce)2Cu2O10	Ru1Sr2Sm1.5Ce0.5Cu2O10	Ru	1	Sr	2	Sm	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Ru1222				3.846		28.58																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6022	PHC2540151		RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.5Ce0.5Cu2O10	Ru	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Ru1222				3.84		28.59																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6023	PHC2540151		RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.5Ce0.5Cu2O10	Ru	1	Sr	2	Gd	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Ru1222				3.836		28.58																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6024	PHC2540151		NbSr2(Sm,Ce)2Cu2O10	Nb1Sr2Sm1.5Ce0.5Cu2O10	Nb	1	Sr	2	Sm	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Nb1222				3.871		28.791																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6025	PHC2540151		NbSr2(Eu,Ce)Cu2O10	Nb1Sr2Eu1.5Ce0.5Cu2O10	Nb	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Nb1222				3.869		28.774																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6026	PHC2540151		NdSr2(Gd,Ce)2Cu2O10	Nd1Sr2Gd1.5Ce0.5Cu2O10	Nd	1	Sr	2	Gd	1.5	Ce	0.5	Cu	2											O	10			1995																											2	Nb1222				3.867		28.742																	4.2																																																																																																		SIN (1065C)-Q to RT					Ruthenium-based layered cuprates   RuSr2LnCu2O8 and RuSr2(Ln1+xCe1-x)Cu2O10 (Ln=Sm, Eu and Gd)	199511		"Physikalisches Institut, Universita""t Bayreuth, 95440 Bayreuth, Germany"	Physica C,254(1995)151-158	H.F. Braun,L. Bauernfeind,W. Widder	Ru, Sr, Sm, Eu, Gd, Cu, O, Ce	
6027	PHC2540033	Tl0.9 Mo0.2 Sr2 Ca0.9 Cu2 by EDS as synthesiqed	(Tl,Mo)Sr2CaCu2O7	Tl0.8Mo0.2Sr2Ca1Cu2O7-z	Tl	0.8	Mo	0.2	Sr	2	Ca	1	Cu	2											O	7-z			1995																											2	Tl1212				3.79		12.046																40			40																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6028	PHC2540033	ANN(450C,10H under P(02))=100bar	(Tl,Mo)Sr2CaCu2O7	Tl0.8Mo0.2Sr2Ca1Cu2O7-z	Tl	0.8	Mo	0.2	Sr	2	Ca	1	Cu	2											O	7-z			1995																																																		24			24																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6029	PHC2540033	ANN280C,IH under  Ar/H2 flow	(Tl,Mo)Sr2CaCu2O7	Tl0.8Mo0.2Sr2Ca1Cu2O7-z	Tl	0.8	Mo	0.2	Sr	2	Ca	1	Cu	2											O	7-z			1995																																																		86			86																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6030	PHC2540033	as-synthesiqed	(Tl,Mo)(Sr,La)2CuO5	Tl0.9Mo0.1Sr1.2La0.8Cu1O5-z	Tl	0.9	Mo	0.1	Sr	1.2	La	0.8	Cu	1											O	5-z			1995																											2	Tl1201				3.776		8.841																40			40										15																																																																																				Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6031	PHC2540033	redced sample(280C,IH in Ar/H2flow)	(Tl,Mo)(Sr,La)2CuO5	Tl0.9Mo0.1Sr1.2La0.8Cu1O5-z	Tl	0.9	Mo	0.1	Sr	1.2	La	0.8	Cu	1											O	5-z			1995																											2	Tl1201																					40	34			34																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6032	PHC2540033	as-synthesiqed	(Tl,MO)Sr2CuO5/Sr2CuO2(CO3)	Tl0.8Mo0.2Sr4Cu2Co3O7-z	Tl	0.8	Mo	0.2	Sr	4	Cu	2	Co	3											O	7-z			1995																											2		P4/mmm			3.825		16.429																30			30																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6033	PHC2540033	ANN(280C,IH in Ar/H2 flow)	(Tl,Mo)Sr2CuO5/Sr2CuO2(CO3)	Tl0.8Mo0.2Sr4Cu2Co3O7-z	Tl	0.8	Mo	0.2	Sr	4	Cu	2	Co	3											O	7-z			1995																											2																				73	80	85	80			80																																																																																														Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6034	PHC2540033	Tl1201/Sr2CuO2Co3 intergrowth	(Tl,Mo)Sr2CuO5/Sr2CuO2(CO3)	Tl0.8Mo0.2Sr4Cu2Co3O7-z	Tl	0.8	Mo	0.2	Sr	4	Cu	2	Co	3											O	7-z			1995																											2					3.8345		16.5811																																																																																																																	Tl2O3,MoO3,SrO2,CuO,Sr2CuO3,SrCO3		mixture-pellet-seal in evacuated silica tube-heat(900C,10H)-Q to RT					Stabilization of new superconducting thallium cuprates and oxycarbonates bymolybdenum	199511		laboratoire de Cristallographie et Sciences des Mate'riaux(CRISMAT)-U.R.A. 1318-ISMRA-Universite' de Caen, Bd du Mare'chal juin,14050 Caen Cedex, France	Physica C,254(1995)33-43	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Letouz'e,M. Hervieu	Tl, Mo, Sr, Cu, O	
6035	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.74Ca0.26Ba2Cu3O6	Y	0.74	Ca	0.26	Ba	2	Cu	3													O	6	6		1995																											2					3.854		11.831													33.4		56				44.7																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
6036	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.72Ca0.28Ba2Cu3O6	Y	0.72	Ca	0.28	Ba	2	Cu	3													O	6			1995																																															36		59				47.5																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
6037	PHC2520100		(Y,Ca)Ba2Cu3O6	Y0.69Ca0.31Ba2Cu3O6	Y	0.69	Ca	0.31	Ba	2	Cu	3													O	6	6		1995																											2					3.856		11.836													19.4		36				27.7																																																																																														BaCO3,Y2O3,CuO,CaCO3	1	mixture-CAL-pellet-SIN(960C,20H)-deoxygenate(700C,20-40H in Ar)-seal(sample+Zn)in quartz tube-heat(430-450C,5-20H)					Superconducting and electrical properties of Ca-substituted YBa2Cu3O6	199510		Department of AppliedElectronics,Science Univercity of Tokyo, 2641 Yamazaki, Noda, Chiba 278 Japan	Physica C,252(1995)100-106	M. Fujiwara,N. Suzuki,T. watanabe	Y, Ba, Cu, O, Ca	
6038	PHC2540026	two step transition,second is due to Al1223,higher Tc due to Al1234	AlSr2Ca2Cu3Oz	Al1Sr2Ca2Cu3O9.3	Al	1	Sr	2	Ca	2	Cu	3													O	z	9.3	2	1995																											2	Al1223				3.836		14.405														63					63																																																																																																reaact at 6G Pa					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6039	PHC2540026	two step transition second,is due to Al 1223,higher Tc due to Al1234	AlSr2Ca2Cu3Oz	Al1Sr2Ca2Cu3O9.5	Al	1	Sr	2	Ca	2	Cu	3													O	z	9.5	2	1995																											2	Al1223				3.836		14.405														69					69																																																																																																reaact at 6G Pa					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6040	PHC2540026	two step transition, second is due to Al1223, higher Tc due to Al 1234	AlSr2Ca2Cu3Oz	Al1Sr2Ca2Cu3O9.7	Al	1	Sr	2	Ca	2	Cu	3													O	z	9.7	2	1995																											2	Al1223				3.836		14.405														72					72																																																																																																reaact at 6G Pa					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6041	PHC2540026	two step transiyion, second is due to Al1223, Higher Tc due to Al1234	AlSr2Ca2Cu3Oz	Al1Sr2Ca2Cu3O9.9	Al	1	Sr	2	Ca	2	Cu	3													O	z	9.9	2	1995																											2	Al1223				3.836		14.405														77					77																																																																																																reaact at 6G Pa					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6042	PHC2540026	two step transition, second is due to Al1223, higher Tc due to Al 1234	AlSr2Ca2Cu3Oz	Al1Sr2Ca2Cu3O10.1	Al	1	Sr	2	Ca	2	Cu	3													O	z	10.1	2	1995																											2	Al1223				3.836		14.405														76					76																																																																																																reaact at 6G Pa					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6043	PHC2540026		AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.9Y0.1Cu3O9.1	Al	1	Sr	2	Ca	1.9	Y	0.1	Cu	3											O	9	9.1	1	1995																												Al1223				3.836		14.475																																																																																																																			mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6044	PHC2540026	impuriq phase=unknown and Al234	AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.8Y0.2Cu3O9.1	Al	1	Sr	2	Ca	1.8	Y	0.2	Cu	3											O	9	9.1		1995																												Al1223				3.834		14.418																																																																																																																			mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6045	PHC2540026	inpuriq phase=unknown and Al234	AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.7Y0.3Cu3O9.1	Al	1	Sr	2	Ca	1.7	Y	0.3	Cu	3											O	9	9.1		1995																												Al1223				3.836		14.428																																																																																																																			mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6046	PHC2540026	inpuriq phase=unknown and Al1234	AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.6Y0.4Cu3O9.1	Al	1	Sr	2	Ca	1.6	Y	0.4	Cu	3											O	9	9.1		1995																												Al1223				3.838		14.417																																																																																																																			mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6047	PHC2540026	inpuriq phase=unknown and Al1234	AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.5Y0.5Cu3O9.1	Al	1	Sr	2	Ca	1.5	Y	0.5	Cu	3											O	9	9.1		1995																												Al1223				3.839		14.425																																																																																																																			mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6048	PHC2540026		AlSr2(Ca,Y)2Cu3O9	Al1Sr2Ca1.4Y0.6Cu3O9.1	Al	1	Sr	2	Ca	1.4	Y	0.6	Cu	3											O	9	9.1		1995																												Al1212				3.847		14.368														14					14																																																																																																mixture-sealed in Au capsule-react in abelt-type high-press apparatus (5-6GPa,1250C,IH)					High-pressure synthesis of a new superconductor, AlSr2Ca2-xYxCu3O9         The n=3 member of the AlSr2Can-1CunO2n+3 family	199511		National Institute for Reseach in Inorganic Materials(NIRIM), 1-1Namiki, Tsukuba, Ibaraki, 305 Japan	Physica C,254(1995)26-32	A.T. Matveev,E. Takatama-Muromachi	Al, Sr, Ca, Y, Cu, O	
6049	PHC2550061	Ca2CuO2Cl2+x KClO4	(Ca,K)2CuO2Cl2	Ca2Cu1Cl2O2	Ca	2	Cu	1	Cl	2															O	2			1995																											2					3.871		15.114																	5																																																																																																CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6050	PHC2550061	Ca2CuO2Cl2+x KClO4	(Ca,K)2CuO2Cl2	Ca1.9K0.1Cu1Cl2O2	Ca	1.9	K	0.1	Cu	1	Cl	2													O	2			1995																											2					3.859		15.209																18			18																																																																																														CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6051	PHC2550061	Ca2CuO2Cl2+x KClO4	(Ca,K)2CuO2Cl2	Ca0.85K0.15Cu1Cl2O2	Ca	0.85	K	0.15	Cu	1	Cl	2													O	2			1995																											2					3.856		15.271																24			24										50																																																																																				CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6052	PHC2550061	Ca2CuO2Cl2+x KClO4	(Ca,K)2CuO2Cl2	Ca1.8K0.2Cu1Cl2O2	Ca	1.8	K	0.2	Cu	1	Cl	2													O	2			1995																											2					3.857		15.287																24			24										42																																																																																				CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6053	PHC2550061	Ca2CuO2Cl2+x KClO4	(Ca,K)2CuO2Cl2	Ca0.75K0.25Cu1Cl2O2	Ca	0.75	K	0.25	Cu	1	Cl	2													O	2			1995																											2					3.858		15.249																24			24										30																																																																																				CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6054	PHC2550061	Ca2CuO2Cl2+x KclO4	(Ca,K)2CuO2Cl2	Ca1.7K0.3Cu1Cl2O2	Ca	1.7	K	0.3	Cu	1	Cl	2													O	2			1995																											2					3.857		15.28																24			24										25																																																																																				CaCo3, Cucl2		mixture(CaCO3:CuCl2=2:1)-CAL(800C,10H in flowing O2)-pellet-heat(800C,10H)-additiong of KClO4-seal in Au capsule-heat9900C,30min under S G Pa					High-pressure synthesis of superconductig (Ca,K)2CuO2Cl2	199512		Superconductivity Reserch Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome,Koto-ku,Tokyo Japan	Physica.C,255(1995)61-64	C.-Q. Jin,K. Tanabe,M. Itoh,N. Koshizuka,S. Adachi,T. Tamura,X.-J. Wu,t. Tatsuki	Ca, K, Cu, O, Cl	
6055	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y1Ba1Sr1Cu3O6.9	Y	1	Ba	1	Sr	1	Cu	3													O	7-z	6.9		1994																											3	Y123				3.8008	3.8523	11.576														92					92																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6056	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.8Pr0.2Ba1Sr1Cu3O6.9	Y	0.8	Pr	0.2	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											3	Y123				3.8154	3.8546	11.573														79.4					79.4																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6057	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.6Pr0.4Ba1Sr1Cu3O6.9	Y	0.6	Pr	0.4	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											3	Y123				3.8315	3.515	11.573														60.5					60.5																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6058	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.5Pr0.5Ba1Sr1Cu3O6.9	Y	0.5	Pr	0.5	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											2	Y123				3.8438		11.577														36					36																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6059	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1Sr1Cu3O8.9	Y	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7-z	8.9		1994																											2	Y123				3.85		11.578														24.1					24.1																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6060	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.35Pr0.65Ba1Sr1Cu3O6.9	Y	0.35	Pr	0.65	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											2	Y123																				20.3					20.3																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6061	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.3Pr0.7Ba1Sr1Cu3O6.9	Y	0.3	Pr	0.7	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											2	Y123				3.8531		11.582																																																																																																																	Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6062	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.2Pr0.8Ba1Sr1Cu3O6.9	Y	0.2	Pr	0.8	Ba	1	Sr	1	Cu	3											O	7-z	6.9		1994																											2	Y123				3.8585		11.587																																																																																																																	Y2O3,Pr6O11,BaCO3,SrCO3,CuO	1	mixture-fire(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6063	PHC2550010	TP in ab-plane HIR for H//c-axis	Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8	Pb	2	Sr	2	Y	1	Cu	3													O	8		3	1995																												Pb3212																						31			31																																		HIR6063																																				TP6063																										precursor+PbO+Nacl-Pt crucible-heat(1050C,500C/H)-cool to 700C at 5C/H-FC to RT,all procedures are in flowing gas of N2 or 1% O2-99% N2					Carrer dependences of anisotropy and irrversibility field in Pb2Sr2Y1-xCaCu3O8 single srystals	199512		Depertment of Applied Physics,Faculty of Engineering,Tohoku Univercity,        Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan (b)Institute for Materials Research,Tohoku University,2-1-1 Katahira,Aoba-ku,Sendai 980-77.Japan	Physica.C,255(1995)10-18	Masatsune Kato,Takashi Noji,Terukazu Nishizaki,Thutomu Takabayashi	Pb, Sr, Y, Ca, Cu, O	
6064	PHC2550010	TP in ab-plane HIR for H//c-axis	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.85Ca0.15Cu3O8	Pb	2	Sr	2	Y	0.85	Ca	0.15	Cu	3											O	8		3	1995																												Pb3212																						47			47																																		HIR6064																																				TP6064																										precursor+PbO+Nacl-Pt crucible-heat(1050C,500C/H)-cool to 700C at 5C/H-FC to RT,all procedures are in flowing gas of N2 or 1% O2-99% N2					Carrer dependences of anisotropy and irrversibility field in Pb2Sr2Y1-xCaCu3O8 single srystals	199512		Depertment of Applied Physics,Faculty of Engineering,Tohoku Univercity,        Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan (b)Institute for Materials Research,Tohoku University,2-1-1 Katahira,Aoba-ku,Sendai 980-77.Japan	Physica.C,255(1995)10-18	Masatsune Kato,Takashi Noji,Terukazu Nishizaki,Thutomu Takabayashi	Pb, Sr, Y, Ca, Cu, O	
6065	PHC2550010	Tp in ab-plan HIR for H//c-axis	Pb2Sr2(Y,Ca)Cu3O8	Pb1Sr2Y0.62Ca0.38Cu3O8	Pb	1	Sr	2	Y	0.62	Ca	0.38	Cu	3											O	8		3	1995																												Pb3212																						71			71																																		HIR6065																																				TP6065																										precursor+PbO+Nacl-Pt crucible-heat(1050C,500C/H)-cool to 700C at 5C/H-FC to RT,all procedures are in flowing gas of N2 or 1% O2-99% N2					Carrer dependences of anisotropy and irrversibility field in Pb2Sr2Y1-xCaCu3O8 single srystals	199512		Depertment of Applied Physics,Faculty of Engineering,Tohoku Univercity,        Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan (b)Institute for Materials Research,Tohoku University,2-1-1 Katahira,Aoba-ku,Sendai 980-77.Japan	Physica.C,255(1995)10-18	Masatsune Kato,Takashi Noji,Terukazu Nishizaki,Thutomu Takabayashi	Pb, Sr, Y, Ca, Cu, O	
6066	PHC2550010	TP in ab-plane HIR for H//c-axis	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.53Ca0.47Cu3O8	Pb	2	Sr	2	Y	0.53	Ca	0.47	Cu	3											O	8		3	1995																												Pb3212																						76			76																																		HIR6066																																				TP6066																										precursor+PbO+Nacl-Pt crucible-heat(1050C,500C/H)-cool to 700C at 5C/H-FC to RT,all procedures are in flowing gas of N2 or 1% O2-99% N2					Carrer dependences of anisotropy and irrversibility field in Pb2Sr2Y1-xCaCu3O8 single srystals	199512		Depertment of Applied Physics,Faculty of Engineering,Tohoku Univercity,        Aramaki Aoba,Aoba-ku,Sendai 980-77,Japan (b)Institute for Materials Research,Tohoku University,2-1-1 Katahira,Aoba-ku,Sendai 980-77.Japan	Physica.C,255(1995)10-18	Masatsune Kato,Takashi Noji,Terukazu Nishizaki,Thutomu Takabayashi	Pb, Sr, Y, Ca, Cu, O	
6067	PHC2550180		HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1995									6.2																		2	Hg1201	P4/mmm			3.877		9.498																97			97																																																																																																mix(Ba2CuO3+z+HgO)-wrapped in Au foil in quartq tube-heat to 800C(100C/H-800C/H)-hold(5-15H)-cool to RT					Single-step synthesis and crystal structure of HgBa2CuO4+z with a Tc of 97K	199512		a) The school of Chemistry, University of Birmingham, Edgbaston,birmingham,B15 2TT,UK B)The ISIS facility,Rutherford Appleton Lavoratory,Chilton,Didcot,Oxon.,OX11OQX,UK	Physica.C,255(1995)180-187	A. Asab (a),A.R. Armstrong (b1),I. Gemeson (a),P.P. Edwards (a)	Hg, Ba, Cu, O	
6068	PHC2460271		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8.0	8	1	1995																												Bi2212						30.818													83						83																																																																																																using freeqed nitrate precursors					Oxygen stotchiometry,structure and superconductivity in Bi2Sr2CaCu2O8+x	199505		Department of Materials Science and Engineering,University of Pittsburgh,Pittsburgh,PA-15261,USA	Physica C.,246(1995)271-276	M.Lelovic,N.G.Eror,P.Krishnaraj,U.Balachandran		
6069	PHC2460271		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.15	Bi	2	Sr	2	Ca	1	Cu	2													O	8.15	8.15	1	1995																												Bi2212						30.843													87						87																																																																																																using freeqed nitrate precursors					Oxygen stotchiometry,structure and superconductivity in Bi2Sr2CaCu2O8+x	199505		Department of Materials Science and Engineering,University of Pittsburgh,Pittsburgh,PA-15261,USA	Physica C.,246(1995)271-276	M.Lelovic,N.G.Eror,P.Krishnaraj,U.Balachandran		
6070	PHC2460271		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	8.16	8.16	1	1995																												Bi2212						30.832													85						85																																																																																																using freeqed nitrate precursors					Oxygen stotchiometry,structure and superconductivity in Bi2Sr2CaCu2O8+x	199505		Department of Materials Science and Engineering,University of Pittsburgh,Pittsburgh,PA-15261,USA	Physica C.,246(1995)271-276	M.Lelovic,N.G.Eror,P.Krishnaraj,U.Balachandran		
6071	PHC2460271		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.26	Bi	2	Sr	2	Ca	1	Cu	2													O	8.26	8.26	1	1995																												Bi2212						30.796													75						75																																																																																																using freeqed nitrate precursors					Oxygen stotchiometry,structure and superconductivity in Bi2Sr2CaCu2O8+x	199505		Department of Materials Science and Engineering,University of Pittsburgh,Pittsburgh,PA-15261,USA	Physica C.,246(1995)271-276	M.Lelovic,N.G.Eror,P.Krishnaraj,U.Balachandran		
6072	PHC2460271		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	8.28	8.28	1	1995																												Bi2212						30.792													75						75																																																																																																using freeqed nitrate precursors					Oxygen stotchiometry,structure and superconductivity in Bi2Sr2CaCu2O8+x	199505		Department of Materials Science and Engineering,University of Pittsburgh,Pittsburgh,PA-15261,USA	Physica C.,246(1995)271-276	M.Lelovic,N.G.Eror,P.Krishnaraj,U.Balachandran		
6073	PHC2460297		Bi2Sr2Ca(Cu,Li)2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z			1995																												Bi2212																			84.2					9.2	84.2																																																																																														Bi2Sr2CaCu2Oz, Bi2Sr2Ca(Cu0.55Li0.45)2Oz		mixture of precursor-pellet-SIN(870C,10-120H, in air)-cool to 800C (7C/min) -ANN(800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6074	PHC2460297		Bi2Sr2Ca(Cu,Li)2Oz	Bi2Sr2Ca1Cu1.8Li0.2Oz	Bi	2	Sr	2	Ca	1	Cu	1.8	Li	0.2											O	z			1995																												Bi2212																			86.9					8.9	86.9																																																																																														Bi2Sr2CaCu2Oz, Bi2Sr2Ca(Cu0.55Li0.45)2Oz		mixture of precursor-pellet-SIN(870C,10-120H, in air)-cool to 800C (7C/min) -ANN(800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6075	PHC2460297		Bi2Sr2C(Cu,Li)2Oz	Bi2Sr2Ca1Cu1.6Li0.4Oz	Bi	2	Sr	2	Ca	1	Cu	1.6	Li	0.4											O	z			1995																												Bi2212																			91.3					9.1	91.3																																																																																														Bi2Sr2CaCu2Oz, Bi2Sr2Ca(Cu0.55Li0.45)2Oz		mixture of precursor-pellet-SIN(870C,10-120H, in air)-cool to 800C (7C/min) -ANN(800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6076	PHC2460297		Bi2Sr2Ca(Cu,Li)2Oz	Bi2Sr2Ca1Cu1.4Li0.6Oz	Bi	2	Sr	2	Ca	1	Cu	1.4	Li	0.6											O	z			1995																												Bi2212																			89.6					7.3	89.6																																																																																														Bi2Sr2CaCu2Oz, Bi2Sr2Ca(Cu0.55Li0.45)2Oz		mixture of precursor-pellet-SIN(870C,10-120H, in air)-cool to 800C (7C/min) -ANN(800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6077	PHC2460297		Bi2Sr2Ca(Cu,Li)2Oz	Bi2Sr2Ca1Cu1.1Li0.9Oz	Bi	2	Sr	2	Ca	1	Cu	1.1	Li	0.9											O	z			1995																												Bi2212																			82.8					5.6	82.8																																																																																														Bi2Sr2CaCu2Oz, Bi2Sr2Ca(Cu0.55Li0.45)2Oz		mixture of precursor-pellet-SIN(870C,10-120H, in air)-cool to 800C (7C/min) -ANN(800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6078	PHC2460297	T(*)=875C		Bi2Sr2Ca1Cu2Li0.1Oz	Bi	2	Sr	2	Ca	1	Cu	2	Li	0.1											O	z			1995																												Bi2212																			86.9					9.3	86.9																																																																																														Bi2Sr2CaCu2Oz, Li2O2Bi2O3	1	mixture-pellet SIN(T(*),10-120 min, in air)-cool to 800C (7K/min)-ANN (800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6079	PHC2460297	T(*)=865C		Bi2Sr2Ca1Cu2Li0.4Oz	Bi	2	Sr	2	Ca	1	Cu	2	Li	0.4											O	z			1995																												Bi2212																			91.2					8.5	91.2																																																																																														Bi2Sr2CaCu2Oz, Li2O2Bi2O3	1	mixture-pellet SIN(T(*),10-120 min, in air)-cool to 800C (7K/min)-ANN (800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6080	PHC2460297	T(*)=865C		Bi1.8Sr2Ca1Cu2Li0.4Oz	Bi	1.8	Sr	2	Ca	1	Cu	2	Li	0.4											O	z			1995																												Bi2212																			94.1					6.8	94.1																																																																																														Bi2Sr2CaCu2Oz, Li2O2Bi2O3	1	mixture-pellet SIN(T(*),10-120 min, in air)-cool to 800C (7K/min)-ANN (800C,12-48H)-Q to RT					Superconducting properties and microstructural evolution of Li doped Bi2Sr2CaCu2Ox	199505		Science and Tecnology Center for Superconductivity and Department of Nuclear Engineering University of Illinois at Urbana-Champaign,103 South Goodwin Avenue,Urbana,IL 61801,USA	Physica C.,246(1995)297-308	G.W.Raban Jr.,J.Schwartz,S.Wu		
6081	PHC2460203	As-sintered	(Tl,Hg)Ba2Ca2Cu3O8	Tl1Ba2Ca2Cu3O8+z	Tl	1	Ba	2	Ca	2	Cu	3													O	8+z		1	1995																											2	Tl1223				3.845		15.909													123						123																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6082	PHC2460203	as-sintered	(Tl,Hg)Ba2Ca2Cu3O8	Tl0.9Hg0.1Ba2Ca2Cu3O8+z	Tl	0.9	Hg	0.1	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845		15.902													132						132																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6083	PHC2460203	as-sintered	(Tl,Hg)Ba2Ca2Cu3O8	Tl0.7Hg0.3Ba2Ca2Cu3O8+z	Tl	0.7	Hg	0.3	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845		15.89													133						133																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6084	PHC2460203		(Tl,Hg)Ba2Ca2Cu3O8	Tl0.5Hg0.5Ba2Ca2Cu3O8+z	Tl	0.5	Hg	0.5	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845		15.873													134						134																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6085	PHC2460203		(Tl,Hg)Ba2Ca2Cu3O8	Tl0.3Hg0.7Ba2Ca2Cu3O8+z	Tl	0.3	Hg	0.7	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845		15.86													134						134																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6086	PHC2460203		(Tl,Hg)Ba2Ca2Cu3O8	Tl0.1Hg0.9Ba2Ca2Cu3O8+z	Tl	0.1	Hg	0.9	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845		15.851													134						134																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6087	PHC2460203		(Tl,Hg)Ba2Ca2Cu3O8	Tl0.05Hg0.95Ba2Ca2Cu3O8+z	Tl	0.05	Hg	0.95	Ba	2	Ca	2	Cu	3											O	8+z			1995																											2	Tl1223				3.845															134						134																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6088	PHC2460203		(Tl,Hg)Ba2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1995																											2	Tl1223				3.845		15.829													134						134																																																																																														Tl2 O3, Hg O, Ba O, Ca O, Cu O	1	mixture-pellet-wrapping in Au foil-seal in evacuated qurtq tube-heat-SIN(750-850C,2-5H)-RT-ANN(300C,1-2H in flowing O2)					Superconductivity above 130 K in  Tl1-xHgxBa2Ca2Cu3O8+z	199505		Physics Department,University of California,Davis,CA,USA	Physica C.,246(1995)203-206	I.C.Chang,J.Z.Liu,M.D.Lan,P.Klavins,R.N.Shelton		
6089	PHC2550173	as-prepared	HgBa2CuO4	Hg1Ba2Cu1O4.08	Hg	1	Ba	2	Cu	1															O	4+z	4.08		1995																											2	Hg1201				3.882		9.525																94			94																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6090	PHC2550173	ANN(350C 67H in 1 bar Ar)	HgBa2CuO4	Hg1Ba2Cu1O4.01	Hg	1	Ba	2	Cu	1															O	4+z	4.01		1995																											2	Hg1201				3.887		9.54																68			68																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6091	PHC2550173	ANN(250C,24H in 1 Bar O2)	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201				3.881		9.525																95			95																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6092	PHC2550173	ANN(200C,18H in 125 bar O2)	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201				3.88		9.521																97			97																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6093	PHC2550173	ANN(250C,66H in 90 bar O2)	HgBa2CuO4	Hg1Ba2Cu1O4.12	Hg	1	Ba	2	Cu	1															O	4+z	4.12		1995																											2	Hg1201				3.876		9.514																89			89																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6094	PHC2550173	as-prepared	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201				3.884		9.53																85			85																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6095	PHC2550173	ANN(250C,24H in flowing O2),Hg0.89 Ba2 Cu1.06 O4+z from wet analysis	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201				3.879		9.525																96			96																																																																																																react in evacuated silica tube uning extra Ba2CuO3+z in tube,temp.gradient=15-20C					Synthesis of monophase HgBa2CuO4+z under controlled partial oxygen pressure	199512		Department of Chemistry,Moscow State University 119899,Moscow,Russian federation	Physica.C,255(1995)173-179	D.A. Mikhailova,E.V. Antipov,V.A. Alyoshin	Hg, Ba, Cu, O	
6096	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.33Cu0.67Sr2Y1Cu2Oz	Bi	0.33	Cu	0.67	Sr	2	Y	1	Cu	2											O	z		1	1995																												Cu1212				3.8118		11.7123																	10																																																																																																Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6097	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.264Mo0.066Cu0.67Sr2Y1Cu2Oz	Bi	0.264	Mo	0.066	Cu	0.67	Sr	2	Y	1	Cu	2									O	z		1	1995																												Cu1212				3.812		11.6757																	10																																																																																																Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6098	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.198Mo0.132Cu0.67Sr2Y1Cu2Oz	Bi	0.198	Mo	0.132	Cu	0.67	Sr	2	Y	1	Cu	2									O	z		1	1995																												Cu1212				3.8111		11.6226																	10																																																																																																Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6099	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.148Mo0.182Cu0.67Sr2Y1Cu2Oz	Bi	0.148	Mo	0.182	Cu	0.67	Sr	2	Y	1	Cu	2									O	z		1	1995																												Cu1212				3.8137		11.5943															30.1				30.1																																																																																														Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6100	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.099Mo0.231Cu0.67Sr2Y1Cu2Oz	Bi	0.099	Mo	0.231	Cu	0.67	Sr	2	Y	1	Cu	2									O	z		1	1995																												Cu1212																					35.2				35.2																																																																																														Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6101	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Mo0.33Cu0.67Sr2Y1Cu2Oz	Mo	0.33	Cu	0.67	Sr	2	Y	1	Cu	2											O	z		1	1995																												Cu1212																					35.7				35.7																																																																																														Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6102	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.85Ce0.15Cu1O4	Gd	1.85	Ce	0.15	Cu	1															O	4		1	1995								4.73																			2	T'				3.903		11.86																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6103	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.75La0.1Ce0.15Cu1O4	Gd	1.75	La	0.1	Ce	0.15	Cu	1													O	4		1	1995								4.57																			2	T'				3.905		11.86																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6104	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.65La0.2Ce0.15Cu1O4	Gd	1.65	La	0.2	Ce	0.15	Cu	1													O	4		1	1995								4.16																			2	T'				3.911		11.885																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6105	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.55La0.3Ce0.15Cu1O4	Gd	1.55	La	0.3	Ce	0.15	Cu	1													O	4		1	1995								3.76																			2	T'				3.92		11.937																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6106	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.35La0.5Ce0.15Cu1O4	Gd	1.35	La	0.5	Ce	0.15	Cu	1													O	4		1	1995																											2	T'				3.935		11.995																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6107	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.25La0.6Ce0.15Cu1O4	Gd	1.25	La	0.6	Ce	0.15	Cu	1													O	4		1	1995																											2	T'				3.94		12.02																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6108	PHC2550147		(Gd,La,Ce)2CuO4	Gd1.05La0.8Ce0.15Cu1O4	Gd	1.05	La	0.8	Ce	0.15	Cu	1													O	4		1	1995																											2	T'				3.951		12.1																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6109	PHC2550147		(Gd,La,Ce)2CuO4	Gd0.95La0.9Ce0.15Cu1O4	Gd	0.95	La	0.9	Ce	0.15	Cu	1													O	4		1	1995																											2	T'				3.957		12.125																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6110	PHC2550147		(Gd,La,Ce)2CuO4	Gd0.65La1.2Ce0.15Cu1O4	Gd	0.65	La	1.2	Ce	0.15	Cu	1													O	4		1	1995																											2	T'				3.977		12.235																	1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6111	PHC2550147		(Gd,La,Ce)2CuO4	Gd0.35La1.5Ce0.15Cu1O4	Gd	0.35	La	1.5	Ce	0.15	Cu	1													O	4		1	1995																											2	T'																							1.5																																																																																																	1						Stracutural and magnetic properties of (Gd,La)1.85Ce0.15CuO4	199512		(a)Depertment of Physics,Peking Univercity,Beijing,People's Republic of China(b)Depertment of Chemistry,Peking Univercity, Beijing, People's Republik of China	Physica.C,255(1995)147-150	Chin Lin,Guo Lu,Hai-Ying Chen,YU-Fen Zhang,Zun-Xiao Liu	Gd, La, Ce, Cu, O	
6112	PHC2560051		Nd(Ba,Sr)2 Cu3O7	Nd1Ba1Sr1Cu3O6.92	Nd	1	Ba	1	Sr	1	Cu	3													O	7-z	6.92	1	1996																											2	Y123				3.854		11.634													60			64			64																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6113	PHC2560051		(Nd,Ca)(Ba,Sr)2 Cu3O7	Nd0.9Ca0.1Ba1Sr1Cu3O6.85	Nd	0.9	Ca	0.1	Ba	1	Sr	1	Cu	3											O	7-z	6.85	1	1996																											2	Y123				3.866		11.673																71			71																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6114	PHC2560051		(Nd,Ca)(Ba,Sr)2 Cu3 O7	Nd0.8Ca0.2Ba1Sr1Cu3O6.78	Nd	0.8	Ca	0.2	Ba	1	Sr	1	Cu	3											O	7-z	6.78	1	1996																											2	Y123				3.864		11.648																77			77																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6115	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3 O7	Nd1Ba1Sr0.95Ca0.05Cu3O7-z	Nd	1	Ba	1	Sr	0.95	Ca	0.05	Cu	3											O	7-z		1	1996																											2	Y123				3.86		11.627													65			67			67																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6116	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3 O7	Nd1Ba1Sr0.9Ca0.1Cu3O7-z	Nd	1	Ba	1	Sr	0.9	Ca	0.1	Cu	3											O	7-z		1	1996																											2	Y123				3.858		11.62													66			70			70																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6117	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3O7	Nd1Ba1Sr0.85Ca0.15Cu3O7-z	Nd	1	Ba	1	Sr	0.85	Ca	0.15	Cu	3											O	7-z		1	1996																											2	Y123				3.858		11.615													66			69			69																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6118	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3 O7	Nd1Ba1Sr0.8Ca0.2Cu3O7-z	Nd	1	Ba	1	Sr	0.8	Ca	0.2	Cu	3											O	7-z		2	1996																											2	Y123				3.852		11.607													66			69			69																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6119	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3O7	Nd1Ba1Sr0.6Ca0.4Cu3O7-z	Nd	1	Ba	1	Sr	0.6	Ca	0.4	Cu	3											O	7-z		2	1996																											2	Y123				3.854		11.611													62			66			66																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6120	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3O7	Nd1Ba1Sr0.4Ca0.6Cu3O7-z	Nd	1	Ba	1	Sr	0.4	Ca	0.6	Cu	3											O	7-z		2	1996																											2	Y123				3.862		11.64													59			63			63																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6121	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3O7	Nd1Ba1Sr0.2Ca0.8Cu3O7-z	Nd	1	Ba	1	Sr	0.2	Ca	0.8	Cu	3											O	7-z		2	1996																											2	Y123				3.865		11.608													41			51			51																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6122	PHC2560051		Nd(Ba,Sr,Ca)2 Cu3O7	Nd1Ba1Ca1Cu3O7-z	Nd	1	Ba	1	Ca	1	Cu	3													O	7-z		2	1996																											2	Y123				3.864		11.63													47			59			59																																																																																														Nd2O3, SrCO3, CuO, CaCO3, Ba(NO3)2	1	mixture-CAL(1225K,24H)-SIN(1235-1255K,96-180H depending on Ca content) -ANN(450C,72H)					Effect of substitution of Ca for Nd and Sr on the superconducting behaviour of NdBaSrCu3O7-z	199601		Chemistry Division,Bhabha Atomic Research Centre,Bombay-400 085, India	Physica.C,256(1996)51-56	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly	Nd, Ba, Sr, Cu, O, Ca	
6123	PHC2550188	nearly single phase	(Hg,W)(Sr,La)2 Cu Oz	Hg0.8W0.2Sr1.4La0.6Cu1Oz	Hg	0.8	W	0.2	Sr	1.4	La	0.6	Cu	1											O	z		1	1995																											2	Hg1201				3.781		8.828													19		37				28																																																																																														WO3,Sr(NO3)2,La2O3,CuO,HgO		precursor with out HgO-CAL(900C,20H)-cool to RT-mix with HgO-seal in quartq-heat to 830C,2C/min-(830C,10H)-cool to RT					Synthesis and supercoductivity of new barinm-free mercury-based cuprates (Hg,W) (Sr,La)n+1CunOz(n=1,2)	199512		(a)Depertment of Applied Chemistry,Univercity of Science and Technology of china,Hefei230026,PR. China( b)Structure Research Laboratory,Univercity of Science and Technology of China,Hefei230026,P.R.China	Physica.C,255(1995)188-192	K.-B. Tang (a,b),L. Yang (b),X.-W. Xu (a),Y.-H. Zhang (b),Y.-T. Qian (a,b),Z.-Y. Chen (a)	Hg, W, Sr, La, Cu, O	
6124	PHC2550188	nearly single hease,Annealed sample	(Hg,W)Sr2(Sr,La)Cu2Oz	Hg0.8W0.2Sr2.45La0.55Cu2Oz	Hg	0.8	W	0.2	Sr	2.45	La	0.55	Cu	2											O	z			1995																												Hg1212	P4/mmm			3.862		12.108													41		91				66																																																																																														WO3,Sr(NO3)2,La2O3,CuO,HgO		precursor with out HgO-CAL(900C,20H)-cool to RT-mix with HgO-seal in quartq-heat to 830C,2C/min-(830C,10H)-cool to RT					Synthesis and supercoductivity of new barinm-free mercury-based cuprates (Hg,W) (Sr,La)n+1CunOz(n=1,2)	199512		(a)Depertment of Applied Chemistry,Univercity of Science and Technology of china,Hefei230026,PR. China( b)Structure Research Laboratory,Univercity of Science and Technology of China,Hefei230026,P.R.China	Physica.C,255(1995)188-192	K.-B. Tang (a,b),L. Yang (b),X.-W. Xu (a),Y.-H. Zhang (b),Y.-T. Qian (a,b),Z.-Y. Chen (a)	Hg, W, Sr, La, Cu, O	
6125	PHC2560161		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3Oz	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z			1996																											3	Y123																				85.1					85.1																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6126	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.85Pr0.1Ca0.05Ba2Cu3Oz	Y	0.85	Pr	0.1	Ca	0.05	Ba	2	Cu	3											O	z			1996																											3	Y123																				82.2					82.2																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6127	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.8Pr0.1Ca0.1Ba2Cu3Oz	Y	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	z			1996																											3	Y123																				78.1					78.1																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6128	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.75Pr0.1Ca0.15Ba2Cu3Oz	Y	0.75	Pr	0.1	Ca	0.15	Ba	2	Cu	3											O	z			1996																											3	Y123																				70.8					70.8																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6129	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.7Pr0.1Ca0.2Ba2Cu3Oz	Y	0.7	Pr	0.1	Ca	0.2	Ba	2	Cu	3											O	z			1996																											3	Y123																				64					64																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6130	PHC2560161		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3Oz	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	z			1996																											3	Y123																				58.7					58.7																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6131	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.75Pr0.2Ca0.05Ba2Cu3Oz	Gd	0.75	Pr	0.2	Ca	0.05	Ba	2	Cu	3											O	z			1996																											3	Y123																				61.6					61.6																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6132	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.7Pr0.2Ca0.1Ba2Cu3O7	Gd	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7			1996																											3	Y123																				64.4					64.4																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6133	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.65Pr0.2Ca0.15Ba2Cu3Oz	Gd	0.65	Pr	0.2	Ca	0.15	Ba	2	Cu	3											O	z			1996																											3	Y123																				62.5					62.5																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6134	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.6Pr0.2Ca0.2Ba2Cu3Oz	Gd	0.6	Pr	0.2	Ca	0.2	Ba	2	Cu	3											O	z			1996																											3	Y123																				58					58																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6135	PHC2560161		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3Oz	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z			1996																											3	Y123																				69.5					69.5																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6136	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.75Pr0.2Ca0.05Ba2Cu3Oz	Y	0.75	Pr	0.2	Ca	0.05	Ba	2	Cu	3											O	z			1996																											3	Y123																				72.7					72.7																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6137	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.7Pr0.2Ca0.1Ba2Cu3Oz	Y	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	z			1996																											3	Y123																				74.6					74.6																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6138	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.65Pr0.2Ca0.15Ba2Cu3Oz	Y	0.65	Pr	0.2	Ca	0.15	Ba	2	Cu	3											O	z			1996																											3	Y123																				72.2					72.2																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6139	PHC2560161		(Y,Pr,Ca)Ba2Cu3O7	Y0.6Pr0.2Ca0.2Ba2Cu3Oz	Y	0.6	Pr	0.2	Ca	0.2	Ba	2	Cu	3											O	z			1996																											3	Y123																				66.3					66.3																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6140	PHC2560161		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3Oz	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	z			1996																											3	Y123																				80.3					80.3																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6141	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.85Pr0.1Ca0.05Ba2Cu3Oz	Gd	0.85	Pr	0.1	Ca	0.05	Ba	2	Cu	3											O	z			1996																											3	Y123																																																																																																																							R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6142	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.8Pr0.1Ca0.1Ba2Cu3Oz	Gd	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	z			1996																											3	Y123																				78.4					78.4																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6143	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.75Pr0.1Ca0.15Ba2Cu3Oz	Gd	0.75	Pr	0.1	Ca	0.15	Ba	2	Cu	3											O	z			1996																											3	Y123																																																																																																																							R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6144	PHC2560161		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.7Pr0.1Ca0.2Ba2Cu3Oz	Gd	0.7	Pr	0.1	Ca	0.2	Ba	2	Cu	3											O	z			1996																											3	Y123																				67.8					67.8																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6145	PHC2560161		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1996																											3	Y123																				90.4					90.4																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6146	PHC2560161		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3Oz	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	z			1996																											3	Y123																				56.9					56.9																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6147	PHC2560161		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3Oz	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z			1996																											3	Y123																				33.1					33.1																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6148	PHC2560161		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3Oz	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	z			1996																											3	Y123																				0					0																																																																																														R2O3,Pr6O11,BaO,CaCO3,CuO		mixture-CAL(950C,24H)-pellet-heat(950C,24H in flowing O2)-ANN(485C,72H)-cool to RT(3C/min)					Structual properties and solubility of calcium in the compounds R1-x-yPrxCayBa2Cu3O7-z (R=Y,Gd)	199601		Department of Physics,University of Hongkong, Pokfulam Road,Hong Kong	Physica.C,256(1996)161-167	T.C. Poon, J. Gao	Y, Gd, Pr, Ca, Ba, Cu, O	
6149	PHC2550329		Li(Ti,Cu)2O4	Li1Ti1.91Cu0.09O4	Li	1	Ti	1.91	Cu	0.09															O	4			1995																																																14.4					14.4	TC6149																																																																																													Li2CO3,Ti,Ti2O3,TiO2,CuO	1	mixture-pellet-SIN(800-875C,24-48H in vac)					Conductivity and superconductivity in the LiTi2-xCuxO4 spinel system	199512		Dpertment of Physics,Ben-Gurion University of the Negeu, Beer Sheva, Israel	Physica.C,255(1995)329-334	O. Faran,V. Volterra	Li, Ti, Cu, O	
6150	PHC2560033	size=1150*150*5 micron.m3,Pb-stabilized Bi2223 GL=84,Hc(0)=3300G	(Bi,Pb)2Sr2Ca2Cu3O10	Bi2Sr2Ca2Oz	Bi	2	Sr	2	Ca	2															O	z			1996																												Bi2223																						109			109																																																																																																Bi2223 whiskers were prepared by phase conversion of Bi2212 whisker to Bi2223 phase					Lower critical field and reversible magnetization of (Bi, Pb)2 Sr2Ca2Cu3Ox   Superconducting whiskers	199601		(a)Osaka National Reseach Institute, AIST, Ikeda, Osaka 563, Japan (b)The Institute of Scientific and Industrial Reseach, Osaka University,Ibaraki,  Osaka 567,Japan	Physica.C,256(1996)33-38	Hiroshi Yamashita (a),Ichiro Matsubara (a),Kazuo Ueno (a),Ryoji Funahashi (a),Tomoji Kawai (b)	Bi, Pb, Sr, Ca, Cu, O	
6151	PHC2560001	as-prepared,Hg1234,CaO, are included	HgBa2Ca4Cu5O12	Hg1Ba2Ca4Cu5O12+z	Hg	1	Ba	2	Ca	4	Cu	5													O	12+z		2	1996																											2	Hg1245				3.855		22.156																100			100																																																																																														Ba2Ca3Cu4Oz, HgO, CaO,CuO		mixture-in Au capsule-high press(18Kbar)-heat(920C,1.6-4H)-heat cut-press cut					High-pressure synthesis and heat treatments of the HgBa2Ca4Cu5O12+z and HgBa2Ca5Cu6O14+z	199601		Laboratoire de Critallographie, CNRS-UJF, BP 166, 38042 Grenoble Cedex 09, France	Physica.C, 256(1996)1-7	B. Souletie,C. Chaillout,E. Gautier,E.M. Kopin,E.V. Antipov,J.J. Capponi,J.L. Tholence,M. Brunner,M. Marezio,S.M. Loureiro	Hg, Ba, Ca, Cu, O	
6152	PHC2560001	ANN(325C,5H,in 500 bar O2)	HgBa2Ca4Cu5O12	Hg1Ba2Ca4Cu5O12+z	Hg	1	Ba	2	Ca	4	Cu	5													O	12+z		2	1996																											2	Hg1245				3.852		22.141																110			110																																																																																														Ba2Ca3Cu4Oz, HgO, CaO,CuO		mixture-in Au capsule-high press(18Kbar)-heat(920C,1.6-4H)-heat cut-press cut					High-pressure synthesis and heat treatments of the HgBa2Ca4Cu5O12+z and HgBa2Ca5Cu6O14+z	199601		Laboratoire de Critallographie, CNRS-UJF, BP 166, 38042 Grenoble Cedex 09, France	Physica.C, 256(1996)1-7	B. Souletie,C. Chaillout,E. Gautier,E.M. Kopin,E.V. Antipov,J.J. Capponi,J.L. Tholence,M. Brunner,M. Marezio,S.M. Loureiro	Hg, Ba, Ca, Cu, O	
6153	PHC2560001	as-prepared,70%Hg1256+15%Hg1245+10%Hg1234+CaO	HgBa2Ca5Cu6O14	Hg1Ba2Ca5Cu6O14+z	Hg	1	Ba	2	Ca	5	Cu	6													O	14+z		2	1996																											2	Hg1256				3.852		25.23																100			100																																																																																														Ba2Ca3Cu4Oz, HgO, CaO,CuO		mixture-in Au capsule-high press(18Kbar)-heat(920C,1.6-4H)-heat cut-press cut					High-pressure synthesis and heat treatments of the HgBa2Ca4Cu5O12+z and HgBa2Ca5Cu6O14+z	199601		Laboratoire de Critallographie, CNRS-UJF, BP 166, 38042 Grenoble Cedex 09, France	Physica.C, 256(1996)1-7	B. Souletie,C. Chaillout,E. Gautier,E.M. Kopin,E.V. Antipov,J.J. Capponi,J.L. Tholence,M. Brunner,M. Marezio,S.M. Loureiro	Hg, Ba, Ca, Cu, O	
6154	PHC2560001	ANN(280C,10H in 13000bar O2)	HgBa2Ca5Cu6O14	Hg1Ba2Ca5Cu6O14+z	Hg	1	Ba	2	Ca	5	Cu	6													O	14+z			1996																											2	Hg1256				3.852		25.26																107			107																																																																																														Ba2Ca3Cu4Oz, HgO, CaO,CuO		mixture-in Au capsule-high press(18Kbar)-heat(920C,1.6-4H)-heat cut-press cut					High-pressure synthesis and heat treatments of the HgBa2Ca4Cu5O12+z and HgBa2Ca5Cu6O14+z	199601		Laboratoire de Critallographie, CNRS-UJF, BP 166, 38042 Grenoble Cedex 09, France	Physica.C, 256(1996)1-7	B. Souletie,C. Chaillout,E. Gautier,E.M. Kopin,E.V. Antipov,J.J. Capponi,J.L. Tholence,M. Brunner,M. Marezio,S.M. Loureiro	Hg, Ba, Ca, Cu, O	
6155	PHC2240001		HgSr2(Cu,Cr)Oz	Hg1Sr2Cu0.7Cr0.3Oz	Hg	1	Sr	2	Cu	0.7	Cr	0.3													O	z		2	1994																												Hg1201																						56			56																																																																																														HgO,SrCO3,CuO,Cr2O3		SrCo3+CuO+Cr2O3-mix and CAL(950C,24H)-mix with HgO-pellet-SIN(880C,8H in evacuated quartq am poule)-Q to RT					A new mercury-based superconductor : (Hg,Cr)Sr2CuOz			Department of Industrial Chemistry,University of Tokyo,Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 224(1994)1-5	J.Shimoyama,K.Kishio,K.Kitazawa,K.Yamafuji,S.Hahakura	Hg,Cr,Sr,Cu,O	
6156	PHC2240001		(Hg,Cr)Sr2CuOz	Hg0.7Cr0.3Sr2Cu1Oz	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	z		1	1994																												Hg1201																			56.5			58			58																																																																																														HgO,SrCO3,CuO,Cr2O3		SrCo3+CuO+Cr2O3-mix and CAL(950C,24H)-mix with HgO-pellet-SIN(880C,8H in evacuated quartq am poule)-Q to RT					A new mercury-based superconductor : (Hg,Cr)Sr2CuOz			Department of Industrial Chemistry,University of Tokyo,Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 224(1994)1-5	J.Shimoyama,K.Kishio,K.Kitazawa,K.Yamafuji,S.Hahakura	Hg,Cr,Sr,Cu,O	
6157	PHC2240001		HgSr2CuOz	Hg1Sr2Cu1Oz	Hg	1	Sr	2	Cu	1															O	z			1994																												Hg1201																						62.4			62.4																																																																																														HgO,SrCO3,CuO,Cr2O3		SrCo3+CuO+Cr2O3-mix and CAL(950C,24H)-mix with HgO-pellet-SIN(880C,8H in evacuated quartq am poule)-Q to RT					A new mercury-based superconductor : (Hg,Cr)Sr2CuOz			Department of Industrial Chemistry,University of Tokyo,Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 224(1994)1-5	J.Shimoyama,K.Kishio,K.Kitazawa,K.Yamafuji,S.Hahakura	Hg,Cr,Sr,Cu,O	
6158	PHC2140087		(Hg,Bi)(Sr,La)2 Cu O5	Hg0.5Bi0.5Sr2Cu1O5-z	Hg	0.5	Bi	0.5	Sr	2	Cu	1													O	5-z			1993																											2	Hg1201				3.765		8.945																																																																																																																	HgO,Bi2O3,La2O3,SrO2,CuO	1	mixture-heat(800C,several aours in quartq tubu)-cool to RT					"A NEW ""1201"" MERCURY CUPRATE"	199309			PHYSICA C,214(1993)87	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,LA,CU,O	
6159	PHC2140087		(Hg,Bi)(Sr,La)2 Cu O5	Hg0.5Bi0.5Sr1.75La0.25Cu1O5-z	Hg	0.5	Bi	0.5	Sr	1.75	La	0.25	Cu	1											O	5-z			1993																											2	Hg1201				3.773		8.906																27			27										7																																																																																				HgO,Bi2O3,La2O3,SrO2,CuO	1	mixture-heat(800C,several aours in quartq tubu)-cool to RT					"A NEW ""1201"" MERCURY CUPRATE"	199309			PHYSICA C,214(1993)87	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,LA,CU,O	
6160	PHC2140087		(Hg,Bi)(Sr,La)2 Cu O5	Hg0.5Bi0.5Sr0.5La0.5Cu1O5-z	Hg	0.5	Bi	0.5	Sr	0.5	La	0.5	Cu	1											O	5-z			1993																											2	Hg1201				3.775		8.877																27			27										7																																																																																				HgO,Bi2O3,La2O3,SrO2,CuO	1	mixture-heat(800C,several aours in quartq tubu)-cool to RT					"A NEW ""1201"" MERCURY CUPRATE"	199309			PHYSICA C,214(1993)87	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,LA,CU,O	
6161	PHC2140087		(Hg,Bi)(Sr,La)2 Cu O5	Hg0.5Bi0.5Sr1.25La0.75Cu1O5-z	Hg	0.5	Bi	0.5	Sr	1.25	La	0.75	Cu	1											O	5-z			1993																											2	Hg1201				3.778		8.841																27			27										7																																																																																				HgO,Bi2O3,La2O3,SrO2,CuO	1	mixture-heat(800C,several aours in quartq tubu)-cool to RT					"A NEW ""1201"" MERCURY CUPRATE"	199309			PHYSICA C,214(1993)87	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,LA,CU,O	
6162	PHC2160273		(Pb,Hg)(Sr,La)2CuO2	Pb0.5Hg0.5Sr1.2La0.8Cu1O5-z	Pb	0.5	Hg	0.5	Sr	1.2	La	0.8	Cu	1											O	5-z		1	1993																											2	Hg1201				3.791		8.691													17	24	38	32			24																																																																																														Pbo,HgO,SrO,CuO		mixture-pellet-wrapped in Au foil in evacuated quartq tube-heat to 930C(5C/min)-hold(12H)-cool to RT (SC/min)					VAN HOVE SINGULARITIES AND THE ROLE OF DOPING IN THE STABILIZATION,SYNTHESIS AND SUPERCONDUCTIVITY OF HGBA2CAN-1CUNO2N+2+Z	199311			PHYSICA C,216(1993)273	A.J.FREEMAN,D.L.NOVIKOV	HG,BA,CA,CU,O	
6163	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.3Pb0.7Sr2Cu1O4+z	Hg	0.3	Pb	0.7	Sr	2	Cu	1													O	4+z			1993																											2	Hg1201				3.749		8.986																	4.2																																																																																																PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6164	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.3Pb0.7Sr1.75La0.25Cu1O4+2	Hg	0.3	Pb	0.7	Sr	1.75	La	0.25	Cu	1											O	4+2			1993																											2	Hg1201				3.76		8.947														30					30																																																																																														PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6165	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.3Pb0.7Sr1.5La0.5Cu1O4+z	Hg	0.3	Pb	0.7	Sr	1.5	La	0.5	Cu	1											O	4+z			1993																											2	Hg1201				3.772		8.894														39					39																																																																																														PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6166	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.3Pb0.7Sr1.35La0.65Cu1O4+z	Hg	0.3	Pb	0.7	Sr	1.35	La	0.65	Cu	1											O	4+z			1993																											2	Hg1201				3.768		8.874																																																																																																																	PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6167	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.3Pb0.7Sr1La1Cu1O4+z	Hg	0.3	Pb	0.7	Sr	1	La	1	Cu	1											O	4+z			1993																											2	Hg1201																				41					41																																																																																														PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6168	PHC2160243		(Hg,Pb)(Sr,La)2CuO4	Hg0.4Pb0.6Sr1.95Pr0.05Cu1O4+z	Hg	0.4	Pb	0.6	Sr	1.95	Pr	0.05	Cu	1											O	4+z			1993																											3	Hg1201				7.606	3.683	8.881																	4.2																																																																																																PbO2,Pr6O11,La2O3,SrCuO2,Sr2CuO3,HgO	1	mixture-slowly heat to 800C in silica tube-several hours-slow cool to RT					"NEW MERCURY-BASED SUPERCONDUCTORS WITH THE ""1201"" STRUCTURE"	199311			PHYSICA C,216(1993)243	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU,P.DANIEL	HG,PR,SR,CU,O,LA	
6169	PHC2500235		TlBa2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6			1995																												Tl2201																						12			12																																																																			-6			TP6169																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6170	PHC2500235		TlBa2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6			1995																												Tl2201																							4.2																																																																					-10			TP6170																										ANN(500C in O2)					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6171	PHC2500235		TlBa2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6			1995																												Tl2201																						88			88																																																																			-0.5			TP6171																										ANN(270C, in 90%Ar-10%H2 )          flow					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6172	PHC2500235		TlBa2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8			1995																												Tl2212																						106			106																																																																			1			TP6172																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6173	PHC2500235		TlBa2CaCu2O8	Tl1Ba2Ca1Cu2O8	Tl	1	Ba	2	Ca	1	Cu	2													O	8			1995																												Tl2212																						105			105																																																																						TP6173																										ANN(500C in O2)					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6174	PHC2500235		TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9	Tl	1	Ba	2	Ca	2	Cu	3													O	9			1995																												Tl1223																						114			114																																																																			-1			TP6174																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6175	PHC2500235		TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9	Tl	1	Ba	2	Ca	2	Cu	3													O	9			1995																												Tl1223																						108			108																																																																						TP6175																										ANN(500C in O2)					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6176	PHC2500235		TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9	Tl	1	Ba	2	Ca	2	Cu	3													O	9			1995																												Tl1223																						123			123																																																																			1			TP6176																										ANN(270C, in 90%Ar-10%H2 )          flow					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6177	PHC2500235		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1995																												Tl2223																						125			125																																																																						TP6177																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6178	PHC2500235		Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10	Tl	2	Ba	2	Ca	2	Cu	3													O	10			1995																												Tl2223																						123			123																																																																						TP6178																										ANN(500C in O2)					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6179	PHC2500235		TlbaSrCaCu2O7	Tl1Ba1Sr1Ca1Cu2O7	Tl	1	Ba	1	Sr	1	Ca	1	Cu	2											O	7			1995																												Tl1212																						16			16																																																																						TP6179																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6180	PHC2500235		TlBaSrCaCu2O7	Tl1Ba1Sr1Ca1Cu2O7	Tl	1	Ba	1	Sr	1	Ca	1	Cu	2											O	7			1995																												Tl1212																						80			80																																																																						TP6180																										ANN(270C, in 90%Ar-10%H2 )          flow					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6181	PHC2500235		TlBaSrCa2Cu3O9	Tl1Ba1Sr1Ca2Cu3O9	Tl	1	Ba	1	Sr	1	Ca	2	Cu	3											O	9			1995																												Tl1223																						97			97																																																																						TP6181																										as-synthesiqed,react(850-950C in silica ampoule) see.Physica C168(1990)8					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6182	PHC2500235		TlBaSrCa2Cu3O9	Tl1Ba2Sr1Ca2Cu3O9	Tl	1	Ba	2	Sr	1	Ca	2	Cu	3											O	9			1995																												Tl1223																						92			92																																																																																																ANN(500C in O2)					Systematic thermopower measurements of the thallium cuprates  Tl(Ba,Sr)2Cam-xCumO2m+3-z and tl2Ba2Cam-1CumO2m+4+z	199508		(a)Laboratoire CRISMAT,CNRS 1318,ISMRA,Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Ce'dex,France (b)Institute of Physics,Cukrovarnicka 10,16200 Prague 6,Czech Republic	Physica C,250(1995)235-239	A. Maignan (a),B. Raveau (a),C. Martin (a),Ch. Simon (a),J. Hejtmanek (b)	Tl, Ba, Sr, Ca, Cu, O	
6183	PHC2150001	impurity=Hg1212,CaO,CuO,CaHgO2	Hg Ba2 Ca2 Cu3 Oz	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1993																											2	Hg1223				3.853	15.818																	133			133																																																																																														Ba2Ca2Cu3Oz,HgO		mixture-seald in Pt capsul-pressure(50Kbar)-heat(950C)-hold(1-4H)-furnace cool					THE SYNTHESIS AND CHARACTERIZATION OF THE HGBA2CA2CU3O8+Z ANDHGBA2CA3CU4O10+Z PHASES	199309			PHYSICA C,215(1993)1	C.CHAILLOUT,E.V.ANTIPOV,J.J.CAPPONI,J.L.THOLENCE,M.MAREZIO,P.BORDET,S.M.LOUREIRO,S.N.PUTILIN	HG,BA,CA,CU,O	
6184	PHC2150001	imprity=Hg1223,CaO,unknown phase.,Tc=132K(for Hg1223)is observed	Hg Ba2 Ca3 Cu4 O10	Hg1Ba2Ca3Cu4O10+z	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z			1993																											2	Hg1234				3.854		19.006																126			126																																																																																																					THE SYNTHESIS AND CHARACTERIZATION OF THE HGBA2CA2CU3O8+Z ANDHGBA2CA3CU4O10+Z PHASES	199309			PHYSICA C,215(1993)1	C.CHAILLOUT,E.V.ANTIPOV,J.J.CAPPONI,J.L.THOLENCE,M.MAREZIO,P.BORDET,S.M.LOUREIRO,S.N.PUTILIN	HG,BA,CA,CU,O	
6185	PHC2550151		(Bi,Mo,Cu)Sr2YCu2O7	Bi0.066Mo0.264Cu0.67Sr2Y1Cu2Oz	Bi	0.066	Mo	0.264	Cu	0.67	Sr	2	Y	1	Cu	2									O	z		1	1995																												Cu1212				3.8125		11.5472															37.5				37.5																																																																																														Bi2 O3, Mo O3, Sr Co3, Y2 O3, CuO	1	mixtuo-CAL(900C,10H in air )-pellet-SIN(980-1000C, 60H in air)-Q to RT-ANN(500-600C, in O2)					prepration and physical properties of the superconductor [(Bi1-xMox)0.33Cu0.67] Sr2YCu2Oy	199512		Faculry of Engineering,Yamagata Univercity,4-3-16,Japan, Yonezawa, Yamagata 992, Japan	Physica.C,255(1995)151-156	Katsuro Okuyama,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao	Bi, Mo, Cu, Sr, Y, Cu, O	
6186	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3O6.19	Y	1	Ba	2	Cu	3															O	6.19			1989																											3	Y123				3.818	3.882	11.643													91		95.4				93.2																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6187	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.14O6.91	Y	1	Ba	2	Cu	3	H	0.14													O	6.91			1989																											3	Y123				3.819	3.885	11.645													88.7		93.2				90.95																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6188	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.32O6.91	Y	1	Ba	2	Cu	3	H	0.32													O	6.91			1989																											3	Y123				3.848	3.888	11.646													88.4		94.1				91.25																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6189	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.43O6.91	Y	1	Ba	2	Cu	3	H	0.43													O	6.91			1989																											3	Y123				3.83	3.886	11.644																																																																																																																		1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6190	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H1.15O6.91	Y	1	Ba	2	Cu	3	H	1.15													O	6.91			1989																																															62.4		91				76.7																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6191	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H1.46O6.91	Y	1	Ba	2	Cu	3	H	1.46													O	6.91			1989																																																																																																																																																				1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6192	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	6.54			1989																											3	Y123				3.841	3.886	11.666													48.1		61.7				54.9																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6193	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.16O6.54	Y	1	Ba	2	Cu	3	H	0.16													O	6.54			1989																											3	Y123				3.849	3.888	11.662													38.2		57.6				47.9																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6194	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.31O6.54	Y	1	Ba	2	Cu	3	H	0.31													O	6.54			1989																											3	Y123				3.859	3.884	11.66													39.5		55.1				47.3																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6195	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.53O6.54	Y	1	Ba	2	Cu	3	H	0.53													O	6.54			1989																											3	Y123				3.874	3.882	11.655													34.1		53.5				43.8																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6196	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.64O6.54	Y	1	Ba	2	Cu	3	H	0.64													O	6.54			1989																											2	Y123				3.882		11.65													34.4		49.7				42.05																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6197	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.6O6.91	Y	1	Ba	2	Cu	3	H	0.6													O	6.91			1989																											3	Y123																			82.1		90.9				86.5																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6198	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.69O6.91	Y	1	Ba	2	Cu	3	H	0.69													O	6.91			1989																											3	Y123				3.847	3.886	11.646													79.2		92.2				85.7																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6199	SPS0312056		YBa2Cu3HxOz	Y1Ba2Cu3H0.92O6.91	Y	1	Ba	2	Cu	3	H	0.92													O	6.91			1989																											3	Y123				3.867	3.888	11.647													71		90.6				80.8																																																																																															1	powders of YBCO(z=6.91,6.54)-spread as thin layer in PT container-slow pumping at 50-60-H2(300-350 torr from TiH2)-(360K,1-2H)					Influence of hydrogen on the superconducting ceramic YBa2Cu3Oy (y=6.91 and 6.54)	198912		Institute of Solid-State Physics, Academy of Sciences of the USSR, Chernogolovka, Moscow Province	Soviet Phys.;Solid State 31(1989)2056	E.G. Ponyatovskii,I.N. Kremenskaya,I.O. Bashkin,M.A. Nevedomskaya,N.S. Sidorov,R.A. Dilanyan,R.K. Nikolaev,V.M. Prokopenko,V.Sh. Shekhtman,V.V. Sinitsyn,Zh.D. Sokolovskaya		
6200	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-z	6.93		1990																											3	Y123				3.823	3.887	11.68													89.9		91.8				90.85																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6201	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.84	Y	1	Ba	2	Cu	3															O	7-z	6.84		1990																											3	Y123																			88		89.7				88.85																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6202	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	7-z	6.82		1990																											3	Y123																			85		89.1				87.05																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6203	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O	7-z	6.78		1990																											3	Y123																			80.4		84.8				82.6																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6204	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	7-z	6.73		1990																											3	Y123				3.828	3.888	11.706													66		71.5				68.75																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6205	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.69	Y	1	Ba	2	Cu	3															O	7-z	6.69		1990																											3	Y123																			62.8		66.6				64.7																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6206	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.67	Y	1	Ba	2	Cu	3															O	7-z	6.67		1990																											3	Y123																			57.9		60.3				59.1																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6207	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.64	Y	1	Ba	2	Cu	3															O	7-z	6.64		1990																											3	Y123																			55.7		57.6				56.65																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6208	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	7-z	6.6		1990																											3	Y123				3.835	3.886	11.728													57		58.7				57.85																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6209	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.57	Y	1	Ba	2	Cu	3															O	7-z	6.57		1990																											3	Y123																			56		58.4				57.2																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6210	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O	7-z	6.55		1990																											3	Y123				3.837	3.881	11.728													53.8		57.3				55.55																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6211	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	7-z	6.52		1990																											3	Y123																			51.1		57.6				54.35																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6212	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.48	Y	1	Ba	2	Cu	3															O	7-z	6.48		1990																											3	Y123				3.842	3.878	11.746													47		55.4				51.2																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6213	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	7-z	6.45		1990																											3	Y123				3.844	3.877	11.751													24.1		29.6				26.85																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6214	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	7-z	6.4		1990																											3	Y123				3.852	3.871														23.4		49.7				36.55																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6215	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	7-z	6.4		1990																											3	Y123																			14.4		32.3				23.35																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6216	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.38	Y	1	Ba	2	Cu	3															O	7-z	6.38		1990																												Y123																			13.6		34.2				23.9																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6217	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.48	Y	1	Ba	2	Cu	3															O	7-z	6.48		1990																											3	Y123																			36.4		43.7				40.05																																																																																														Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6218	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.28	Y	1	Ba	2	Cu	3															O	7-z	6.28		1990																											2	Y123				3.863		11.796																																																																																																																	Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6219	PR04611923	RES(200K)=5.72m,Ohm,cm	(Yb,Ca)(Ba,Sr)2Cu3Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.1	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.1		1992																											2	Y123				3.818		11.744														48.3					48.3																																																																			34.51																													annealed for various temp,for oxygen control					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6220	PR04611923	RES(200K)=4.05m,Ohm,cm	(Yb,Ca)(Ba,Sr)2 Cu3Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.43	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.43		1992																											2	Y123				3.823		11.707														64.3					64.3																																																																			12.2																													annealed for various temp,for oxygen control					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6221	PR04611923	RES(200K)=2.16m,Ohm,cm	(Yb,Ca)(Ba,Sr)2 Cu3Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.56	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.56		1992																											2	Y123				3.83		11.675														82.4					82.4																																																																			1.24																													annealed for various temp,for oxygen control					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6222	PR04611923	RES(200K)=1.36m,Ohm,cm	(Yb,Ca)(Ba,Sr)2 Cu3Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.73	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.73		1992																											3	Y123				3.799	3.857	11.591														68.5					68.5																																																																			-6.19																													annealed for various temp,for oxygen control					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6223	PR04611923	RES(200K)=1.18m,Ohm,cm	(Yb,Ca)(Ba,Sr)2 Cu3 Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.78	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.78		1992																												Y123				3.793	3.853	11.612														40.7					40.7																																																																			-7.96																													annealed for various temp,for oxygen control					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6224	PR04611923		(Yb,Ca)(Ba,Sr)2Cu3Oz	Yb1Ba1.6Sr0.4Cu3O6.88	Yb	1	Ba	1.6	Sr	0.4	Cu	3													O	z	6.88		1992																											3	Y123				3.788	3.863	11.588														80.2					80.2																																																																																														Yb2O3,CaCO3,BaCO3,SrCO3,SrCO3,CuO	1	mixture-CAL-formed into bar-SIN(850C,20H in flowing (99%N2+1%O2)) -ANN  (400C,20H+300C,2OH in flowing O2)					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6225	PR04611923		(Yb,Ca)(Ba,Sr)2Cu3Oz	Yb0.9Ca0.1Ba1.6Sr0.4Cu3O6.89	Yb	0.9	Ca	0.1	Ba	1.6	Sr	0.4	Cu	3											O	z	6.89		1992																											3	Y123				3.788	3.854	11.588														62.1					62.1																																																																																														Yb2O3,CaCO3,BaCO3,SrCO3,SrCO3,CuO	1	mixture-CAL-formed into bar-SIN(850C,20H in flowing (99%N2+1%O2)) -ANN  (400C,20H+300C,2OH in flowing O2)					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6226	PR04611923		(Yb,Ca)(Ba,Sr)2Cu3Oz	Yb0.8Ca0.2Ba0.8Sr0.4Cu3O6.85	Yb	0.8	Ca	0.2	Ba	0.8	Sr	0.4	Cu	3											O	z	6.85		1992																											3	Y123				3.796	3.854	11.599														35					35																																																																																														Yb2O3,CaCO3,BaCO3,SrCO3,SrCO3,CuO	1	mixture-CAL-formed into bar-SIN(850C,20H in flowing (99%N2+1%O2)) -ANN  (400C,20H+300C,2OH in flowing O2)					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6227	PR04611923		(Yb,Ca)(Ba,Sr)2Cu3Oz	Yb0.7Ca0.3Ba1.6Sr0.4Cu3O6.78	Yb	0.7	Ca	0.3	Ba	1.6	Sr	0.4	Cu	3											O	z	6.78		1992																											3	Y123				3.797	3.85	11.61														24.4					24.4																																																																																														Yb2O3,CaCO3,BaCO3,SrCO3,SrCO3,CuO	1	mixture-CAL-formed into bar-SIN(850C,20H in flowing (99%N2+1%O2)) -ANN  (400C,20H+300C,2OH in flowing O2)					THERMOELECTRIC POWER FOR THE OVERDOPED SUPERCONDUCTORS (YB,CA)(BA,SR)2CU3OZ	199211		SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY TECHNOLOGY CENTER, TOKYO	PHYS.REV.B,46(1992)11923	H.YAMAUCHI,KIYOTAKA MATSUURA,S.TAJIMA,TAKAHIRO WADA,YUJI YAEGASHI	YB,CA,BA,SR,CU,O	
6228	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1994																												Y123																				90.4		89		0.8	90.4																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6229	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.16Y1Ba2Cu3Oz	H	0.16	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						86.4			86.4																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6230	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.24Y1Ba2Cu3Oz	H	0.24	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						82.4			82.4																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6231	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.28Y1Ba2Cu3Oz	H	0.28	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						78.8			78.8																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6232	PR0490600	188<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.32Y1Ba2Cu3Oz	H	0.32	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						72.1			72.1																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6233	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.38Y1Ba2Cu3Oz	H	0.38	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						60.7			60.7																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6234	PR0490600	18oo<d<3000,RH for a-b-plane	YBa2Cu3HxOz	H0.42Y1Ba2Cu3Oz	H	0.42	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						56.6			56.6																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6235	PR0490600	1800<d<3000,RH for a-b-plane	YBa2Cu3HxOz	H0.54Y1Ba2Cu3Oz	H	0.54	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																						43.9			43.9																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6236	PR0490600	1800<d<3000,RH for a-b plane	YBa2Cu3HxOz	H0.6Y1Ba2Cu3Oz	H	0.6	Y	1	Ba	2	Cu	3													O	z		4	1994																												Y123																					38	37.6		6.2	37.6																																																																																																films on SrTiO3(100)by laser ablation-hydrogenation (100mbar,463K abaut50H in vac chamber),conc.by (15)N method					Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH, Bereich Schwerionenphysik, Glienicker Strasse 100, D-14109 Berlin, germany	Phys.Rev.B,49(1994)600	A. Weidinger,B. Stritzker,G. Dortmann,H. Karl,J. Erxmeyer,J. Steiger,S. Blasser,T. Paatsch		
6237	PHC2352777	fluence=3E+13/cm2	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		4	1994																												Y123																			86.2						86.2																																																																																										4						The film sputtered on Sr Ti O3(001)-irradiated by H(t) with 3 Me5					Flux-Flow Hall coefficient in YBa2Cu3Oy Films with Proton Irradiation			Department of Phyisics, National Taiwan Normal University. Taipei, Taiwan, R.O.C.	Physica.C,235-240(1994)2777-2778	C.S. Chen,C.Y. Huang,H.C. Yang,H.E. Horng,H.M. Cho,L.M. Wang,Y.C. Liu		
6238	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	6.91	6.91		1988																											3	Y123				3.817	3.886	11.669																93.1			93.1																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6239	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3H0.06O6.91	Y	1	Ba	2	Cu	3	H	0.06													O	7	6.91		1988																											3	Y123																						92.8			92.8																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6240	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3H0.27O6.91	Y	1	Ba	2	Cu	3	H	0.27													O	6.91	6.91		1988																											3	Y123				3.825	3.885	11.656																91.1			91.1																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6241	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3H0.52O6.91	Y	1	Ba	2	Cu	3	H	0.52													O	6.91	6.91		1988																											3	Y123				3.865	3.887	11.619																91.7			91.7																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6242	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3H0.91O6.91	Y	1	Ba	2	Cu	3	H	0.91													O	6.91	6.91		1988																											2	Y123				3.871		11.625																91.4			91.4																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6243	JJP0270525		YBa2Cu3HxO7	Y1Ba2Cu3H1.68O6.91	Y	1	Ba	2	Cu	3	H	1.68													O	6.91	6.91		1988																											2	Y123				3.889		11.589																	4.2																																																																																																		Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6244	JJP0270525		GdBa2Cu3HxO7	Gd1Ba2Cu3O6.89	Gd	1	Ba	2	Cu	3															O	6.89	6.89		1988																											3	Y123				3.844	3.889	11.667																92.9			92.9																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6245	JJP0270525		GdBa2Cu3HxO7	Gd1Ba2Cu3H0.12O6.89	Gd	1	Ba	2	Cu	3	H	0.12													O	6.89	6.89		1988																											3	Y123				3.846	3.898	11.692																84			84																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6246	JJP0270525		GdBa2Cu3HxO7	Gd1Ba2Cu3H0.43O6.89	Gd	1	Ba	2	Cu	3	H	0.43													O	6.89	6.89		1988																											3	Y123				3.849	3.904	11.697																82			82																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6247	JJP0270525		GdBa2Cu3HxO7	Gd1Ba2Cu3H1.32O6.89	Gd	1	Ba	2	Cu	3	H	1.32													O	6.89	6.89		1988																											2	Y123				3.901		11.681																78.2			78.2																																																																																																Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6248	JJP0270525		GdBa2Cu3HxO7	Gd1Ba2Cu3H1.68O6.89	Gd	1	Ba	2	Cu	3	H	1.68													O	6.89	6.89		1988																											2	Y123				3.906		11.694																	4.2																																																																																																		Hydrogenation was performed by exposing powders of YBCO,GDBCO to H2 gas (0.9bar,530K)					Effect of Hydrogen Absorption on Superconductivity in YBa2Cu3O6.91 and GdBa2Cu3O6.89	198804		Faculty of Integrated Arts and Sciences, Hiroshima University, Hiroshima 730	Jpn.J.Appl.Phys.Lett.27(1988)L252-L258	Hirofumi KAWANAKA,Hironobu FUJII,Hitoshi FUKUBA,Shinichi ORIMO,Wei YE		
6249	LES1720425		YBa2Cu3HxOz	Eu1Ba2Cu3O7-z	Eu	1	Ba	2	Cu	3															O	7-z			1991																											3	Y123				3.842	3.905	11.714																																																																																																																			see J.Less-Common Met, 151(1989)183					Static and dynamic dilatation of the high-Tc superconductor EuBa2Cu3O7-deltaHx			U.A. 803 du CNRS, Hydrogene dans les Metaux, Bat. 350, Universite Paris-Sud, F-91405 Orsay (France)	J.Less Common Metals,172-174(1991)425-432	J.N. Daou,J.P. Burger,P. Vajda		
6250	LES1720425		YBa2Cu3HxOz	Eu1Ba2Cu3H0.23O7-z	Eu	1	Ba	2	Cu	3	H	0.23													O	7-z			1991																											3	Y123				3.847	3.9074	11.721																																																																																																																			see J.Less-Common Met, 151(1989)183					Static and dynamic dilatation of the high-Tc superconductor EuBa2Cu3O7-deltaHx			U.A. 803 du CNRS, Hydrogene dans les Metaux, Bat. 350, Universite Paris-Sud, F-91405 Orsay (France)	J.Less Common Metals,172-174(1991)425-432	J.N. Daou,J.P. Burger,P. Vajda		
6251	LES1720425		YBa2Cu3HxOz	Eu1Ba2Cu3H0.54O7-z	Eu	1	Ba	2	Cu	3	H	0.54													O	7-z			1991																											3	Y123				3.85	3.909	11.726																																																																																																																			see J.Less-Common Met, 151(1989)183					Static and dynamic dilatation of the high-Tc superconductor EuBa2Cu3O7-deltaHx			U.A. 803 du CNRS, Hydrogene dans les Metaux, Bat. 350, Universite Paris-Sud, F-91405 Orsay (France)	J.Less Common Metals,172-174(1991)425-432	J.N. Daou,J.P. Burger,P. Vajda		
6252	LES1720425		YBa2Cu3HxOz	Eu1Ba2Cu3H0.79O7-z	Eu	1	Ba	2	Cu	3	H	0.79													O	7-z			1991																											3	Y123				3.85	3.91	11.73																																																																																																																			see J.Less-Common Met, 151(1989)183					Static and dynamic dilatation of the high-Tc superconductor EuBa2Cu3O7-deltaHx			U.A. 803 du CNRS, Hydrogene dans les Metaux, Bat. 350, Universite Paris-Sud, F-91405 Orsay (France)	J.Less Common Metals,172-174(1991)425-432	J.N. Daou,J.P. Burger,P. Vajda		
6253	LES1720425		YBa2Cu3HxOz	Eu1Ba2Cu3H1.5O7-z	Eu	1	Ba	2	Cu	3	H	1.5													O	7-z			1991																											2	Y123				3.907		11.736																																																																																																																			see J.Less-Common Met, 151(1989)183					Static and dynamic dilatation of the high-Tc superconductor EuBa2Cu3O7-deltaHx			U.A. 803 du CNRS, Hydrogene dans les Metaux, Bat. 350, Universite Paris-Sud, F-91405 Orsay (France)	J.Less Common Metals,172-174(1991)425-432	J.N. Daou,J.P. Burger,P. Vajda		
6254	PR04310368		YBa2(Cu,Fe)HxO7	Y1Ba2Cu2.94Fe0.06O7	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7			1991																																3.843	3.858	11.66														73					73																																																																																															1	H-absorption by direct contact with H2-gas(200C),H-content measured by change of gas pressure					SUPERCONDUCTIVITY AND ANTIFERROMAGNETISM IN THE CU(2) PLANES OF YBA2CU3O7HX	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)10368	B.BROSH,C.KORN,I.FELNER,S.D.GOREN,V.VOLTERRA	Y,BA,CU,O,H	
6255	PR04310368		YBa2(Cu,Fe)HxO7	Y1Ba2Cu2.94Fe0.06H0.4O7	Y	1	Ba	2	Cu	2.94	Fe	0.06	H	0.4											O	7			1991																																		11.72														47					47																																																																																															1	H-absorption by direct contact with H2-gas(200C),H-content measured by change of gas pressure					SUPERCONDUCTIVITY AND ANTIFERROMAGNETISM IN THE CU(2) PLANES OF YBA2CU3O7HX	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)10368	B.BROSH,C.KORN,I.FELNER,S.D.GOREN,V.VOLTERRA	Y,BA,CU,O,H	
6256	PR04310368		YBa2(Cu,Fe)HxO7	Y1Ba2Cu2.94Fe0.06H1O7	Y	1	Ba	2	Cu	2.94	Fe	0.06	H	1											O	7			1991								415																										11.72														30					30																																																																																															1	H-absorption by direct contact with H2-gas(200C),H-content measured by change of gas pressure					SUPERCONDUCTIVITY AND ANTIFERROMAGNETISM IN THE CU(2) PLANES OF YBA2CU3O7HX	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)10368	B.BROSH,C.KORN,I.FELNER,S.D.GOREN,V.VOLTERRA	Y,BA,CU,O,H	
6257	PR04310368		YBa2(Cu,Fe)HxO7	Y1Ba2Cu2.94Fe0.06H1.3O7	Y	1	Ba	2	Cu	2.94	Fe	0.06	H	1.3											O	7			1991								415																										11.72																																																																																																																		1	H-absorption by direct contact with H2-gas(200C),H-content measured by change of gas pressure					SUPERCONDUCTIVITY AND ANTIFERROMAGNETISM IN THE CU(2) PLANES OF YBA2CU3O7HX	199105		RACAH INSTITUTE OF PHYSICS,THE HEBREW UNIVERSITY,JERUSALEM 91904,ISRAEL	PHYS.REV.B,43(1991)10368	B.BROSH,C.KORN,I.FELNER,S.D.GOREN,V.VOLTERRA	Y,BA,CU,O,H	
6258	SSC0661157		EuBa2Cu3HxOz	Eu1Ba2Cu3Oz	Eu	1	Ba	2	Cu	3															O	z			1988																												Y123																						96.2			96.2										83																																																																																					1	H.doping(180-210C,10-30 torr H2)					EFFECT OF HYDOROGEN ON HIGH Tc GRANULAR SUPERCONDUCTORS: OBSERVATION OF PERCOLATING BEHAVIOUR			U.A. 803 du CNRS %aHydrog'ene et De'fauts dans les Metaux%a, Bat. 350, 91405 Orsay, France	Solid State Commun.,66(1988)1157-1160	I. Vedel,J. Lesueur,J.N. Daou,J.P. Burger,L. Dumoulin,M. Nicolas,P. Vajda		
6259	SSC0661157		EuBa2Cu3HxOz	Eu1Ba2Cu3H0.09Oz	Eu	1	Ba	2	Cu	3	H	0.09													O	z			1988																												Y123																						95.1			95.1																																																																																															1	H.doping(180-210C,10-30 torr H2)					EFFECT OF HYDOROGEN ON HIGH Tc GRANULAR SUPERCONDUCTORS: OBSERVATION OF PERCOLATING BEHAVIOUR			U.A. 803 du CNRS %aHydrog'ene et De'fauts dans les Metaux%a, Bat. 350, 91405 Orsay, France	Solid State Commun.,66(1988)1157-1160	I. Vedel,J. Lesueur,J.N. Daou,J.P. Burger,L. Dumoulin,M. Nicolas,P. Vajda		
6260	SSC0661157		EuBa2Cu3HxOz	Eu1Ba2Cu3H0.24Oz	Eu	1	Ba	2	Cu	3	H	0.24													O	z			1988																												Y123																						92.8			92.8																																																																																															1	H.doping(180-210C,10-30 torr H2)					EFFECT OF HYDOROGEN ON HIGH Tc GRANULAR SUPERCONDUCTORS: OBSERVATION OF PERCOLATING BEHAVIOUR			U.A. 803 du CNRS %aHydrog'ene et De'fauts dans les Metaux%a, Bat. 350, 91405 Orsay, France	Solid State Commun.,66(1988)1157-1160	I. Vedel,J. Lesueur,J.N. Daou,J.P. Burger,L. Dumoulin,M. Nicolas,P. Vajda		
6261	PR0411863		YBa2Cu3Oz	Y1Ba2Cu3O6.09	Y	1	Ba	2	Cu	3															O	7-z	6.09		1990																											2	Y123				3.861		11.817																																																																																																																	Y2O3,BaCO3,CuO		mixture-pellet-CAL(960C,24H in flowing Oz)-SIN(960C,24H in flowing O2)-ANN(520C,various O2 presure for various O2 content)					STRUCTURAL PROPERTIES OF OXYGEN-DEFICIENT YBA2CU3O7-Z	199002		MATERIALS CSIENCE DIVISION, ARGONNE NATIONAL LABORATORY, ARNONNE, ILLIONIS 60439	PHYS.REV.B,41(1990)1863	A.P.PAULIKAS,B.W.VEAL,G.W.CRABTREE,H.CLAUS,J.D.JORGENSEN,L.J.NOWICKI,W.K.KWOK	Y,BA,CU,O	
6262	PHC2610038	not s/c		Ba2Cu1.2Co2.4O2,4	Ba	2	Cu	1.2	Co	2.4															O	2,4		3	1996																											2		P4/mmm			3.99		8.073																																																																																																																								Synthesis, crystal growth and structural characterisation of barium-copper oxycarbonates Ba2MxCu2-x-y(CO3)yO2+z  (M=Cu,Cd,Ca;0.05<x<0.25)			Dip. Dhimica Fisica ed Inorganica, Universita' di Bologna, 40136 Bologna, Italy	Physica.C,261(1996)38-55	A. Migliori,F.C. Matacotta,G. Calestani,K.A. Thomas,L. Righi,P. Nozar		
6263	PHC2610038	not s/c		Ba2Cd0.21Cu1.04Co2.25O2+z	Ba	2	Cd	0.21	Cu	1.04	Co	2.25													O	2+z		3	1996																											2		P4/mmm			8.13		8.107																																																																																																																								Synthesis, crystal growth and structural characterisation of barium-copper oxycarbonates Ba2MxCu2-x-y(CO3)yO2+z  (M=Cu,Cd,Ca;0.05<x<0.25)			Dip. Dhimica Fisica ed Inorganica, Universita' di Bologna, 40136 Bologna, Italy	Physica.C,261(1996)38-55	A. Migliori,F.C. Matacotta,G. Calestani,K.A. Thomas,L. Righi,P. Nozar		
6264	PHC2610038	not s/c		Ba2Ca0.25Cu0.9Co2.55O2.3	Ba	2	Ca	0.25	Cu	0.9	Co	2.55													O	2.3		3	1996																											2		P4/mmm			4.082		7.986																																																																																																																								Synthesis, crystal growth and structural characterisation of barium-copper oxycarbonates Ba2MxCu2-x-y(CO3)yO2+z  (M=Cu,Cd,Ca;0.05<x<0.25)			Dip. Dhimica Fisica ed Inorganica, Universita' di Bologna, 40136 Bologna, Italy	Physica.C,261(1996)38-55	A. Migliori,F.C. Matacotta,G. Calestani,K.A. Thomas,L. Righi,P. Nozar		
6265	PHC2610038	not s/c		Ba2Ca0.2Cu1.2Co1.8O3	Ba	2	Ca	0.2	Cu	1.2	Co	1.8													O	3		3	1996																											1		Pm3m			8.11																																																																																																																										Synthesis, crystal growth and structural characterisation of barium-copper oxycarbonates Ba2MxCu2-x-y(CO3)yO2+z  (M=Cu,Cd,Ca;0.05<x<0.25)			Dip. Dhimica Fisica ed Inorganica, Universita' di Bologna, 40136 Bologna, Italy	Physica.C,261(1996)38-55	A. Migliori,F.C. Matacotta,G. Calestani,K.A. Thomas,L. Righi,P. Nozar		
6266	PHC2610033		(Ca,La)(Ba,La)2Cu3O7	Ca0.49La0.51Ba1.26La0.74Cu3Oz	Ca	0.49	La	0.51	Ba	1.26	La	0.74	Cu	3											O	z		4	1996																												Y123																				53.4					53.4																																																																																																prepared by lasen ablation from x=0.45 target Ca-content by changing the distance between target and substrate   substrate+ SrTiO3(100)					Characterization of tetragonal 1:2:3  (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy thin films prepared by laser ablasion deposition			Department of Physics and Crown Center for Superconductivity, Technion-Israel Institute of Technology,Haifa 32000, Israel	Physica.C,261(1996)33-37	A. Knizhnik,C. Chabaud,D. Goldschmidt,G. Koren,G.M. Reisner,I. Gertner,Y. Direktovitch,Y. Eckstein		
6267	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr2Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	7			1996																											2	Pb1212				3.812		11.941																																																																																																																	PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6268	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr1.9Ba0.1Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	1.9	Ba	0.1	Ca	0.5	Y	0.5	Cu	2							O	7			1996																											2	Pb1212				3.813		11.95																																																																																																																	PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6269	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr1.8Ba0.2Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	1.8	Ba	0.2	Ca	0.5	Y	0.5	Cu	2							O	7			1996																											2	Pb1212				3.816		11.963																																																																																																																	PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6270	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr1.7Ba0.3Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	1.7	Ba	0.3	Ca	0.5	Y	0.5	Cu	2							O	7			1996																											2	Pb1212				3.82		11.975																																																																																																																	PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6271	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr1.6Ba0.4Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	1.6	Ba	0.4	Ca	0.5	Y	0.5	Cu	2							O	7			1996																											2	Pb1212				3.822		12.028													32		40				36																																																																																														PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6272	PHC2610027	not s/c	(Pb,Cd)(Sr,Ba)2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr1.5Ba0.5Ca0.5Y0.5Cu2O7	Pb	0.5	Cd	0.5	Sr	1.5	Ba	0.5	Ca	0.5	Y	0.5	Cu	2							O	7			1996																											2	Pb1212				3.824		12.054													47		51				49																																																																																														PbO,CdO,SrCO3,BaO2,CaCO3,Y2O3,CuO	1	mixture-SIN(920C,40H, in air)					Electonic structure of the Ba-doped (Pb,Cd)-1212 cuprates			faculty of Chemistry and Chemical Engineering, Suzhou University, Suzhou 215006, China	Physica.C,261(1996)27-32	G.E. Zhou,M.L. Tian,W.J. Yu,X.M. Liu,Y.H. Zhang,Z.Q. Mao		
6273	SSC0840183	semicon-like	(Pr,Ca)Ba2Cu3O7	Pr1Ba2Cu3O6.849	Pr	1	Ba	2	Cu	3															O	7-z	6.849		1992																											3					3.874	3.928	11.76																	4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6274	SSC0840183	semicon-like	(Pr,Ca)Ba2Cu3O7	Pr0.9Ca0.1Ba2Cu3O6.806	Pr	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.806		1992																											3					3.875	3.92	11.729																	4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6275	SSC0840183	semicon-like	(Pr,Ca)Ba2Cu3O7	Pr0.8Ca0.2Ba2Cu3O6.785	Pr	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.785		1992																											3					3.867	3.919	11.738																	4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6276	SSC0840183	semicon-like	(Pr,Ca)Ba2Cu3O7	Pr0.7Ca0.3Ba2Cu3O6.7	Pr	0.7	Ca	0.3	Ba	2	Cu	3													O	7-z	6.7		1992																											3					3.871	3.896	11.698																	4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6277	SSC0840183	semicon-like	Pr(Ba,La)2Cu3O7	Pr1Ba1.75La0.25Cu3O6.976	Pr	1	Ba	1.75	La	0.25	Cu	3													O	7-z	6.976		1992																											2					3.899																			4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6278	SSC0840183	semicon-like	Pr(Ba,La)2Cu3O7	Pr1Ba1.5La0.5Cu3O7.16	Pr	1	Ba	1.5	La	0.5	Cu	3													O	7-z	7.16		1992																											2																								4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6279	SSC0840183	semicon-like	Pr(Ba,La)2Cu3O7	Pr1Ba1.25La0.75Cu3O7.28	Pr	1	Ba	1.25	La	0.75	Cu	3													O	7-z	7.28		1992																											2																								4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6280	SSC0840183	semicon-like	Pr(Ba,La)2Cu3O7	Pr1Ba1La1Cu3O7.42	Pr	1	Ba	1	La	1	Cu	3													O	7-z	7.42		1992																											2					3.855		11.62																	4.2																																																																																																Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6281	SSC0840183	semicon	(Pr,Ca)(Ba,La)Cu3O7	Pr0.8Ca0.2Ba1La1Cu3O7.34	Pr	0.8	Ca	0.2	Ba	1	La	1	Cu	3											O	7-z	7.34		1992																											2	Y123				3.873		11.653																																																																																																																	Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6282	SSC0840183	semicon	(Pr,Ca)(Ba,La)Cu3O7	Pr0.6Ca0.4Ba1La1Cu3O7.29	Pr	0.6	Ca	0.4	Ba	1	La	1	Cu	3											O	7-z	7.29		1992																											2	Y123				3.871		11.637																																																																																																																	Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6283	SSC0840183	semicon	(Pr,Ca)(Ba,La)Cu3O7	Pr0.5Ca0.5Ba1La1Cu3O7.2	Pr	0.5	Ca	0.5	Ba	1	La	1	Cu	3											O	7-z	7.2		1992																											2	Y123				3.863		11.621																																																																																																																	Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6284	SSC0840183	semicon	(Pr,Ca)(Ba,La)Cu3O7	Pr0.4Ca0.6Ba1La1Cu3O7.21	Pr	0.4	Ca	0.6	Ba	1	La	1	Cu	3											O	7-z	7.21		1992																											2	Y123				3.883		11.629																																																																																																																	Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6285	SSC0840183		(Pr,Ca)(Ba,La)Cu3O7	Pr0.2Ca0.8Ba1La1Cu3O7.1	Pr	0.2	Ca	0.8	Ba	1	La	1	Cu	3											O	7-z	7.1		1992																											2	Y123				3.89		11.641													21		46				33.5																																																																																														Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6286	SSC0840183		(Pr,Ca)(Ba,La)Cu3O7	Ca1Ba1La1Cu3O6.97	Ca	1	Ba	1	La	1	Cu	3													O	7-z	6.97		1992																											2	Y123				3.897		11.669													62		66				64																																																																																														Pr6O11,La2P3,BaO2,CaCO3,CuO	1	Mixture-CAL(1200K,24H in air)-pellet -heat(1225K,48H in air)-FC to RT-heat (773C in air)					INVESTIGATIONS OF STRUCTURE AND SUPERCONDUCTING PROPERTIES OFTHE PR(CA)-BA(LA)-CU-O SYSTEM : PR1-XCAXBA2CU3O7-Z, PRBA2-XLAXCU3O7-Z AND PR1-XCAXBALACU3O7-Z	199210	TC                  ,STRUCTURE	SOLID STATE AND STRUCTURAL CHEMISTRY UNIT AND CSIR CENTRE OF EXCELLANCE IN CHEMISTRY, INDIAN INSTITUTE OF SCIENCE	SOLID STATE COMMUN.,84(1992)183	C. N. R. RAO,R. NAGARAJAN,VIKRAM PAVATE	PR,CA,BA,CU,O,LA	
6287	NAT3750126	Yb occupy off-centred interstitial stes	Yb3C60	C60Tb2.75	C	60	Tb	2.75																					1995																											3	fullerene	Pcab	61		27.874	27.98	27.873																5.4			5.4																																																																																																Sample sealed in quartz tubu-heat(630C,6H)-cool to RT(5C/min)					Superconductivity and cation-vacancy ordering in the rare-earth fulleride Yb2.75C60	5		AT&T Bell Laboratories, Murray Hill, new Jersey 07974, USA	Nature 375(1995)126	A.P. Ramirez,A.R. Kortan,E. Ozdas,H.E. Bair,K.M. Rabe,N. Kopylov,P.H. Cltrin,S. Schuppler,T. Siegrist		
6288	JPC0070287		(Y,Pr)(Ba,Sr)Cu3O7	Y0.4Pr0.6Ba2Cu3O6.92	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-z	6.92		1974																											3	Y123				3.862	3.918	11.719																	15																																																																																																Y2O3,Pr6O11,BaCO3,SrCO3CuO	1	mixture-fire(1203-1223K,24H in air)-pellet(4000Kg/cm2)-SIN(1243K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Soft mode dynamics of the singlet-triplet ferromagnet			Bell Laboratories, Murray Hill, New Jersey 07974, USA	J.Phys.C,7(1974)L287	M E Lines		
6289	JPC0070287		(Y,Pr)(Ba,Sr)Cu3O7	Y0.4Pr0.6Ba1.5Sr0.5Cu3O6.92	Y	0.4	Pr	0.6	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.92		1974																											3	Y123				3.861	3.881	11.661																	15																																																																																																Y2O3,Pr6O11,BaCO3,SrCO3CuO	1	mixture-fire(1203-1223K,24H in air)-pellet(4000Kg/cm2)-SIN(1243K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Soft mode dynamics of the singlet-triplet ferromagnet			Bell Laboratories, Murray Hill, New Jersey 07974, USA	J.Phys.C,7(1974)L287	M E Lines		
6290	JPC0070287		(Y,Pr)(Ba,Sr)Cu3O7	Y0.4Pr0.6Ba1.25Sr0.75Cu3O6.92	Y	0.4	Pr	0.6	Ba	1.25	Sr	0.75	Cu	3											O	7-z	6.92		1974																											2	Y123				3.86	3.862	11.597															17				17																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3CuO	1	mixture-fire(1203-1223K,24H in air)-pellet(4000Kg/cm2)-SIN(1243K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Soft mode dynamics of the singlet-triplet ferromagnet			Bell Laboratories, Murray Hill, New Jersey 07974, USA	J.Phys.C,7(1974)L287	M E Lines		
6291	JPC0070287		(Y,Pr)(Ba,Sr)Cu3O7	Y0.4Pr0.6Ba1Sr1Cu3O6.92	Y	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7-z	6.92		1974																											2	Y123					3.849	11.574													18						18																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3CuO	1	mixture-fire(1203-1223K,24H in air)-pellet(4000Kg/cm2)-SIN(1243K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Soft mode dynamics of the singlet-triplet ferromagnet			Bell Laboratories, Murray Hill, New Jersey 07974, USA	J.Phys.C,7(1974)L287	M E Lines		
6292	JPC0070287	Sr-Cu-O phase inprity	(Y,Pr)(Ba,Sr)Cu3O7	Y0.4Pr0.6Ba0.75Sr1.25Cu3O6.92	Y	0.4	Pr	0.6	Ba	0.75	Sr	1.25	Cu	3											O	7-z	6.92		1974																											2	Y123					3.841	11.543													23						23																																																																																														Y2O3,Pr6O11,BaCO3,SrCO3CuO	1	mixture-fire(1203-1223K,24H in air)-pellet(4000Kg/cm2)-SIN(1243K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Soft mode dynamics of the singlet-triplet ferromagnet			Bell Laboratories, Murray Hill, New Jersey 07974, USA	J.Phys.C,7(1974)L287	M E Lines		
6293	PR05215534		Sm3C60	C60Sm3	C	60	Sm	3																					1995																											3		P cab			28.17	28.07	28.27																8			8																																																																																																C60 powder was purchased from Hoechst company,mixture of C60+Sm-pellet-wrapped in Ta-sealed in quartz tube-heat(550-600C,several hours)					Supercondutivity at 8 K in samarium-doped C60	199512			Phys.Rev.B,52(1995)15534	G. Roth,X.H. Chen		
6294	PR05215517			C60K3	C	60	K	3																					1995																																																		19.3			19.3												deviation from linearity at H-M curve	42																																																																																			single crystal was synthesized by vaporizing method. Doping was carried out in a tubu at165C for K,at 200C for Rb-ANN for 1-48H					Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
6295	PR05215517			C60Rb3	C	60	Rb	3																					1995																																																		30			30													32																																																																																			single crystal was synthesized by vaporizing method. Doping was carried out in a tubu at165C for K,at 200C for Rb-ANN for 1-48H					Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
6296	SUP0080591	delta Tc < 0.04	Yba2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	z	6.94		1995																												Y123																				91.2					91.2						0.013	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6297	SUP0080591	delta Tc=-0.84	YBa2Cu3O7	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	7	6.68		1995																												Y123																				66.9					66.9						-0.4	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6298	SUP0080591	delta Tc=-0.32	YBa2Cu3O7	Y1Ba2Cu3O6.64	Y	1	Ba	2	Cu	3															O	z	6.64		1995																												Y123																				62.25					62.25						-0.16	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6299	SUP0080591	delta Tc=-0.30	YBa2Cu3O7	Y1Ba2Cu3O6.61	Y	1	Ba	2	Cu	3															O	z	6.61		1995																												Y123																				61.3					61.3						-0.16	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6300	SUP0080591	delta Tc=-0.24	YBa2Cu3O7	Y1Ba2Cu3O6.62	Y	1	Ba	2	Cu	3															O	z	6.62		1995																												Y123																				60.9					60.9						-0.13	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6301	SUP0080591	delta Tc=-0.27	YBa2Cu3O7	Y1Ba2Cu3O6.61	Y	1	Ba	2	Cu	3															O	z	6.61		1995																												Y123																				61.38					61.38						-0.14	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6302	SUP0080591	delta Tc=-0.30	YBa2Cu3O7	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O	z	6.55		1995																												Y123																				59.9					59.9						-0.16	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6303	SUP0080591	delta Tc=-0.21	YBa2Cu3O7	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	z	6.52		1995																												Y123																				61.34					61.34						-0.11	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6304	SUP0080591	delta Tc=-0.35	YBa2Cu3O7	Y1Ba2Cu3O6.61	Y	1	Ba	2	Cu	3															O	z	6.61		1995																												Y123																				61.25					61.25						-0.18	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6305	SUP0080591	delta Tc=-0.58	YBa2Cu3O7	Y1Ba2Cu3O6.76	Y	1	Ba	2	Cu	3															O	z	6.76		1995																												Y123																				85.23					85.23						-0.22	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6306	SUP0080591	delta Tc=-0.67	YBa2Cu3O7	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	z	6.68		1995																												Y123																				67.4					67.4						-0.32	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6307	SUP0080591	delta Tc=6.75	YBa2Cu3O7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	z	6.75		1995																												Y123																				83.65					83.65						-0.25	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6308	SUP0080591	delta Tc=-0.67	YBa2Cu3O7	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	z	6.73		1995																												Y123																				80					80						-0.27	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6309	SUP0080591	delta Tc=-0.73	Yba2Cu3O7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7		1995																												Y123																				73.62					73.62						-0.32	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6310	SUP0080591	delta Tc=-0.15	YBa2Cu3O7	Y1Ba2Cu3O6.49	Y	1	Ba	2	Cu	3															O	z	6.49		1995																												Y123																				59.53					59.53						-0.08	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6311	SUP0080591	delta Tc=-0.49	YBa2Cu3O7	Y1Ba2Cu3O6.37	Y	1	Ba	2	Cu	3															O	z	6.37		1995																												Y123																				40.87					40.87						-0.38	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6312	SUP0080591	delta Tc=-0.26	YBa2Cu3O7	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	z	6.41		1995																												Y123																				49.5					49.5						-0.17	Cu																																																																																							Y2O3,BaCO3,CuO	1	using Cu(65)O and Cu(63)O, isotopic enrichment=99.67% and 99.72%,mejor impurity=0.01 at% Si,oxygen by weighing					The Copper Isotope Effect in Oxygen-Deficient YBa2Cu3O7-delta			Department of Physics, University of Alberta, Edmonton, AB, Canada, T6G 2J1	J.Superconductivity,8(1995)591	D.D. Lawrie,J.P. Franck		
6313	SUP0080615	diamond anvil cell,up to 6G Pa, Tc=144.4K at p=6Gpa Figure shows Tc deviation from P=0	(Tl,Hg)Ba2Ca2Cu3Oz	Tl0.2Hg0.8Ba2Ca2Cu3Oz	Tl	0.2	Hg	0.8	Ba	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223				3.858		15.915																						K/GPa	1.4																																																																																												standard quartz tube method					Pressure Dependence of Tc in Tl0.2Hg0.8Ba2Ca2Cu3Ox			Naval Research Laboratory, Washington, DC 20375	J.Superconductivity,8(1995)615	A.R. Drews,D.H. Liebenberg,E.F. Skelton,G.F. Sun,K.W. Wong,M.S. Osofsky,S.B. Qadri,Y. Xin		
6314	SUP0080333	CaCdO2,BaCuO2,Cd1111,Cd1121,Cd2333 phase included	CdBa2Ca2Cu3Oz	Cd1Ba2Ca2Cu3Oz	Cd	1	Ba	2	Ca	2	Cu	3													O	z		2	1995																																																107		107			107																																																																																														CdO,BaCO3,CaCO3,CuO	1	mixture-pellet-heat(900C,17H)-cool to 300C in O2-ANN(300C,12H in O2)					Superconductivity at Different Tc in CdBa2Ca2Cu3Oy			Institute of Solid State Physics, 1784 Sofia, Bulgaria	J.Superconductivity,8(1995)333	A. Staneva,E. Gattef,N. Balchev,V. Lovchinov		
6315	SSC0930053	intergrowth of adouble perovskite slice(Ba Cu2 Pr O5)with a triple rock salt layer, R(RT)=1 E+5 Ohm.om	(Hg,Cu,Pr)2 Ba2PrCu2O8	Hg1.5Ba2Pr1.3Cu2.2O8-z	Hg	1.5	Ba	2	Pr	1.3	Cu	2.2													O	8-z			1995																											2	Hg2212				3.924		28.993																	4.2																																																																																																HgO,BaO2,Pr6O11,CuO		mixture-in evacuated tubu-heat(800C-850C,30-60H)-slow cool to RT					AMERCURY BASED CUPRATE WITH THE %a2212%a STRUCTURE: Hg2-x(Cu,Pr)xBa2PrCu2O8-delta			Lboratoire CRISMAT-URA 1318-ISMRa/Universite' de Caen Bd du Marechal Juin, 14050 Caen Cedex, France	Solid State Commun.,93(1995)53-56	A. Maignan,B. Raveau,C. Martin,C. Michel,F. Goutenoire,G.Van Tendeloo,M. Hervieu		
6316	PR04712197	Longitudinal veloaty shows a peak around 160K, sound velocity-VT=1802.4 m/s	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1993									3.97			GPa		31.8	GPa		12.9	GPa		19.7					3048.3			Y124																						76			76																																																											364																																										ULTRASONIC MEASUREMENTS ON TWO SINGLE-PHASE POLYCRYSTALLINE YBA2CU4O8 SUPERCONDUCTING SAMPLES	199305			PHYS.REV.B,47(1993)12197	H.YAMAUCHI,K.FOSSHEIM,S.TANAKA,T.WADA,WU TING,Y.YAEGASHI		
6317	PR0435526	porosity=0.13,C11=136GPa sound velocity VT=2.609	Nd2CuO4	Nd2Cu1O4-z	Nd	2	Cu	1																	O	4-z		1	1991									6.425			GPa		111	GPa		44	GPa		77		0.263			4.602			T'																																																																																				347																																										ULTRASONIC EVIDENCE OF STRONG VIBRATIONAL ANHARMONICITY IN HIGH-TC SUPERCONDUCTORS AND ITS EFFECT ON DETERMINATION OF THEIRELASTIC PROPERTIES	199103		SCHOOLS OF PHYSICS AND MATERIALS SCIENCE,UNIVERSITY OF BATH,CLAVERTON DOWN,BATH BA2 7AY,UNITED KINGDAM	PHYS.REV.B,43(1991)5526	A.AL-KHEFFAJI,CHANG FANGGAO,D.A.LADDS,D.P.ALMOND,G.A.SAUNDERS,M.CANKURTARAN,P.J.FORD	ND,CE,CU,O,LA,SR	
6318	PR0435526	prosity=0.12 C11=143GPa sound velocity VY=2.609	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		1	1991									6.481			GPa		128	GPa		53	GPa		72		0.207			4.694			T'																				21					21																																																											379																																										ULTRASONIC EVIDENCE OF STRONG VIBRATIONAL ANHARMONICITY IN HIGH-TC SUPERCONDUCTORS AND ITS EFFECT ON DETERMINATION OF THEIRELASTIC PROPERTIES	199103		SCHOOLS OF PHYSICS AND MATERIALS SCIENCE,UNIVERSITY OF BATH,CLAVERTON DOWN,BATH BA2 7AY,UNITED KINGDAM	PHYS.REV.B,43(1991)5526	A.AL-KHEFFAJI,CHANG FANGGAO,D.A.LADDS,D.P.ALMOND,G.A.SAUNDERS,M.CANKURTARAN,P.J.FORD	ND,CE,CU,O,LA,SR	
6319	PR0435526	prosity=0.09 C11=140GPa sound velocity, VT=2.609	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1991									6.495			GPa		124	GPa		51	GPa		72					4.641			T																																																																																				377																																										ULTRASONIC EVIDENCE OF STRONG VIBRATIONAL ANHARMONICITY IN HIGH-TC SUPERCONDUCTORS AND ITS EFFECT ON DETERMINATION OF THEIRELASTIC PROPERTIES	199103		SCHOOLS OF PHYSICS AND MATERIALS SCIENCE,UNIVERSITY OF BATH,CLAVERTON DOWN,BATH BA2 7AY,UNITED KINGDAM	PHYS.REV.B,43(1991)5526	A.AL-KHEFFAJI,CHANG FANGGAO,D.A.LADDS,D.P.ALMOND,G.A.SAUNDERS,M.CANKURTARAN,P.J.FORD	ND,CE,CU,O,LA,SR	
6320	PR0435526	prosity=0.16 C11=133GPa sound velocity, VT=2.609	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1991									6			GPa		121	GPa		51	GPa		65		0.188			4.706			T																				32					32																																																											383																																										ULTRASONIC EVIDENCE OF STRONG VIBRATIONAL ANHARMONICITY IN HIGH-TC SUPERCONDUCTORS AND ITS EFFECT ON DETERMINATION OF THEIRELASTIC PROPERTIES	199103		SCHOOLS OF PHYSICS AND MATERIALS SCIENCE,UNIVERSITY OF BATH,CLAVERTON DOWN,BATH BA2 7AY,UNITED KINGDAM	PHYS.REV.B,43(1991)5526	A.AL-KHEFFAJI,CHANG FANGGAO,D.A.LADDS,D.P.ALMOND,G.A.SAUNDERS,M.CANKURTARAN,P.J.FORD	ND,CE,CU,O,LA,SR	
6321	JPC0016853	ultra sonic palse echo method x-ray dinsity=7.138,porosity=0.22, thermal expcnsion a11=1.22 a22=1.12 a33=1.64 (E-5K)	GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			1989									5.549						GPa		64.5	GPa		84.64							3	Y123				3.862	3.925	11.753														89					89																																																											426																																					SIN(940C,48H in O2 flow)-slowcool					An ultrasonic study of superconducting and non-superconducting GdBa2Cu3O7-x			School of Physics and Materials Science, University of Bath, Claverton Down, Bath BA2 7AY, UK	J.Phys.C,1(1989)6853-6864	B.Chapman,D.P.Almond,E.F.Lambson,G.A.Saunders,J.Freestone,Qingxian Wang		
6322	PHC2620001		(Hg,Tl)Ba2CuOz	Hg1Ba2Cu1Oz	Hg	1	Ba	2	Cu	1															O	z		1	1996																											2	Hg1201				3.884		9.519														92.3					92.3																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6323	PHC2620001		(Hg,Tl)Ba2CuOz	Hg0.9Tl0.1Ba2Cu1Oz	Hg	0.9	Tl	0.1	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.885		9.52													69.7	79.8	84.7				79.8																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6324	PHC2620001		(Hg,Tl)Ba2CuOz	Hg0.8Tl0.2Ba2Cu1Oz	Hg	0.8	Tl	0.2	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.883		9.529													50	61.3	75.8				61.3																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6325	PHC2620001		(Hg,Tl)Ba2CuOz	Hg0.7Tl0.3Ba2Cu1Oz	Hg	0.7	Tl	0.3	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.885		9.53													32.7	40.7	64.9				40.7																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6326	PHC2620001		(Hg,Tl)Ba2CuOz	Hg0.6Tl0.4Ba2Cu1Oz	Hg	0.6	Tl	0.4	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.883		9.53																	10																																																																																																HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6327	PHC2620001		(Hg,Tl)Ba2CuOz	Hg0.5Tl0.5Ba2Cu1Oz	Hg	0.5	Tl	0.5	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.882		9.54																	10																																																																																																HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6328	PHC2620001		Hg(Ba,La)2CuOz	Hg1Ba1.9La0.1Cu1Oz	Hg	1	Ba	1.9	La	0.1	Cu	1													O	z			1996																											2	Hg1201																				90.6					90.6																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6329	PHC2620001		Hg(Ba,La)2CuOz	Hg1Ba1.8La0.2Cu1Oz	Hg	1	Ba	1.8	La	0.2	Cu	1													O	z			1996																											2	Hg1201																				88.1					88.1																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6330	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.9Tl0.1Ba1.95La0.05Cu1Oz	Hg	0.9	Tl	0.1	Ba	1.95	La	0.05	Cu	1											O	z			1996																											2	Hg1201																				69.3					69.3																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6331	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.9Tl0.1Ba1.9La0.1Cu1Oz	Hg	0.9	Tl	0.1	Ba	1.9	La	0.1	Cu	1											O	z			1996																											2	Hg1201																				71.8					71.8																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6332	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.9Tl0.1Ba1.8La0.2Cu1Oz	Hg	0.9	Tl	0.1	Ba	1.8	La	0.2	Cu	1											O	z			1996																											2	Hg1201																				75.9					75.9																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6333	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.99	Sm	1	Ba	2	Cu	3															O	z	6.99		1995																											3					3.849	3.91	11.724														90.7					90.7																																																																																														BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6334	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.86	Sm	1	Ba	2	Cu	3															O	z	6.86		1995																											3					3.861	3.914	11.737														91					91																															1.57																																				11.6															1.305												BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6335	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.82	Sm	1	Ba	2	Cu	3															O	z	6.82		1995																											3					3.859	3.914	11.755														59.2					59.2																															1.59																																				37.6															2.952					1.97					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6336	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.73	Sm	1	Ba	2	Cu	3															O	z	6.73		1995																											3					3.86	3.912	11.748														44.9					44.9																															1.6																																				65.1															4.762					0.922					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6337	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.62	Sm	1	Ba	2	Cu	3															O	z	6.62		1995																											3					3.872	3.908	11.787														34.2					34.2																															0.35																																				98.1															7.02					0.736					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6338	PHC2540331		SmBa2Cu3Oz	Sm1Ba2Cu3O6.53	Sm	1	Ba	2	Cu	3															O	z	6.53		1995																																																																																																																								205															30.58												BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6339	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.05Ba1.95Cu3O6.99	Sm	1.05	Ba	1.95	Cu	3															O	z	6.99		1995																											3					3.862	3.897	11.694														88.5					88.5																																																																			21.1															1.709					2.04					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6340	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.15Ba1.85Cu3O7	Sm	1.15	Ba	1.85	Cu	3															O	z	7		1995																											3					3.851	3.899	11.703														83					83																															1.25																																				15.4															1.81												BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6341	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.27Ba1.73Cu3O7.05	Sm	1.27	Ba	1.73	Cu	3															O	z	7.05		1995																											2					3.876		11.656														50.1					50.1																															1.09																																				31.6															3.14					1.05					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6342	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.39Ba1.61Cu3O7.07	Sm	1.39	Ba	1.61	Cu	3															O	z	7.07		1995																											2					3.873		11.619														31.8					31.8																															0.47																																				60.4															5.46					0.64					/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6343	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.45Ba1.55Cu3O7.09	Sm	1.45	Ba	1.55	Cu	3															O	z	7.09		1995																											2																																																																																													115.9															14.03										/cm3		BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6344	PHC2540331		(Sm,Ba)(Ba,Sm)2Cu3O7	Sm1.6Ba1.4Cu3O7.11	Sm	1.6	Ba	1.4	Cu	3															O	z	7.11		1995																											2					3.864		11.569																																																																																						235.9															40.82												BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,20H)-ANN(800C,5H in flowing O2)-slow cool to RT,ANN(48H in Ar) diferent T for varion O-content					Electronic structure parameters of Sm1+xBa2-xCu3Oy solid solution of orthorhombic and tetragonal structure	199511		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,254(1995)331-341	C. Sul,kowski,D. Wl,osewicz,K. Rogacki,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
6345	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba2Cu3O7-z	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7-z		1	1996																											3	Y123				3.862	3.919	11.725																																																																																																																	Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6346	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba1.9Ca0.1Cu3O7-z	Y	0.4	Pr	0.6	Ba	1.9	Ca	0.1	Cu	3											O	7-z		1	1996																											3	Y123				3.856	3.907	11.699																																																																																																																	Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6347	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba1.8Ca0.2Cu3O7-z	Y	0.4	Pr	0.6	Ba	1.8	Ca	0.2	Cu	3											O	7-z		1	1996																											3	Y123				3.859	3.887	11.676													23.9						23.9																																																																																														Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6348	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba1.7Ca0.3Cu3O7-z	Y	0.4	Pr	0.6	Ba	1.7	Ca	0.3	Cu	3											O	7-z		1	1996																											3	Y123				3.863	3.873	11.657													29						29																																																																																														Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6349	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba1.6Ca0.4Cu3O7-z	Y	0.4	Pr	0.6	Ba	1.6	Ca	0.4	Cu	3											O	7-z		1	1996																											2	Y123				3.859		11.629													30.3						30.3																																																																																														Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6350	SUP0090089		(Y,Pr)(Ba,Ca)2Cu3O7	Y0.4Pr0.6Ba1.5Ca0.5Cu3O7-z	Y	0.4	Pr	0.6	Ba	1.5	Ca	0.5	Cu	3											O	7-z			1996																											2																				26.7						26.7																																																																																														Y2O3,Pr6O11,BaCO3,CaCO3,CuO	1	mixture-CAL(1193K,24H in air)-SIN(1238K,24H in flowing O2)-ANN (773K,24H)-slow cool					Structural Variation and Recovery of Superconductivity by Ca Substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta			Department of Applied Chemistry, University of Science and Technology of China, Hefei 23006, P.R. China	J.Superconductivty,9(1996)	Guanghan Cao,Hongkai Wu,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6351	SUP0090065		Pb2Sr2(Ho,Ca)Cu3O8	Pb2Sr2Ho0.5Ca0.5Cu3O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	3											O	8		3	1996																												Pb3212																				73.2					73.2																							390	48								8.1	1						26	3.3																																																								single drystal grown in PT crucible from molten materials uning excess PbO,NaCl as flux-ANN(450C,100H inflowing N2), typical size=1*1*0.1mm3					Anisotropy in the Resistive Superconducting Transition under Magnetic Fields in Single Crystal Pb2Sr2Ho0.5Ca0.5Cu3O8			Department of Applied Physics,Faculty of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai, 980-77 Japan	J.Superconductivity,9(1996)65	Hideo Iwasaki,Masatsune Kato,Norio Kobayashi,Takashi Noji,Yoji Koike,Yoshitami Saito		
6352	SUP0090065		Pb2Sr2(Ho,Ca)Cu3O8	Pb2Sr2Ho0.5Ca0.5Cu3O8	Pb	2	Sr	2	Ho	0.5	Ca	0.5	Cu	3											O	8		3	1996																												Pb3212																				75					75																							650	70								13	1.4						22	2.3																																																								single drystal grown in PT crucible from molten materials uning excess PbO,NaCl as flux-ANN(450C,100H inflowing N2), typical size=1*1*0.1mm3					Anisotropy in the Resistive Superconducting Transition under Magnetic Fields in Single Crystal Pb2Sr2Ho0.5Ca0.5Cu3O8			Department of Applied Physics,Faculty of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai, 980-77 Japan	J.Superconductivity,9(1996)65	Hideo Iwasaki,Masatsune Kato,Norio Kobayashi,Takashi Noji,Yoji Koike,Yoshitami Saito		
6353	SUP0090027	TP300 is for ab-plane, fgure p=1 for//, p=2 for c-axis //	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		3	1996																												T'																				17				2	17																																																																						TP6348													0.165	2300												single crystal grown by L.I.Leonyuk (MOSCOW State Univ)					Transport Properties of Nd1.85Ce0.15CuO4-delta Single Crystals: The Narrow-Band Model			Institute of Metal Physics, Russian Academy of Sciences, Ekaterinburg, Russia	J.Superconductivity,9(1996)27	A.A. Lakhtin,A.I. Ponomarev,K.R. Krylov,L.I. Leonyuk,T.B. Charikova,V.I. Tsidilkovski		
6354	PHC2530071		Tl Sr2(Ca,Tl)Cu2 Oz	Tl1.2Sr2Ca0.8Cu2O6.862	Tl	1.2	Sr	2	Ca	0.8	Cu	2													O	z	6.862		1995																		GPa		112							2	Tl1212				3.793		12.126														60					60																																																																																																					Pressure effects on Tc and structurein overdoped TISr2CaCu2O7-z	199510		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne	Physica C,253(1995)71-78	B.A. Hunter,H. Shaked,H. Takahashi,J.D. Jorgensen,N. Mori,R.L. Hitterman,T. Kondo,T. Manako,Y. Kubo,Y. Shimakawa	Tl, Sr, Ca, Cu, O	
6355	PHC2530071		Tl Sr2(Ca,Tl)Cu2 Oz	Tl1.2Sr2Ca0.8Cu2O6.934	Tl	1.2	Sr	2	Ca	0.8	Cu	2													O	z	6.934		1995																		GPa		114							2	Tl1212				3.784		12.118																	4.2																																																																																																							Pressure effects on Tc and structurein overdoped TISr2CaCu2O7-z	199510		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne	Physica C,253(1995)71-78	B.A. Hunter,H. Shaked,H. Takahashi,J.D. Jorgensen,N. Mori,R.L. Hitterman,T. Kondo,T. Manako,Y. Kubo,Y. Shimakawa	Tl, Sr, Ca, Cu, O	
6356	PHC2530071	hydrostatic 1.5GPa	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-z	Tl	1	Sr	2	Ca	1	Cu	2													O	7-z			1995																												Tl1212																				35.2					35.2			K/GPa	-0.2																																																																																												see Phys.Rev.B,45(1992)5553					Pressure effects on Tc and structurein overdoped TISr2CaCu2O7-z	199510		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne	Physica C,253(1995)71-78	B.A. Hunter,H. Shaked,H. Takahashi,J.D. Jorgensen,N. Mori,R.L. Hitterman,T. Kondo,T. Manako,Y. Kubo,Y. Shimakawa	Tl, Sr, Ca, Cu, O	
6357	PHC2530071	hydrostatic 1.5GPa	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-z	Tl	1	Sr	2	Ca	1	Cu	2													O	7-z			1995																												Tl1212																				51.8					51.8			K/GPa	-0.6																																																																																												see Phys.Rev.B,45(1992)5553					Pressure effects on Tc and structurein overdoped TISr2CaCu2O7-z	199510		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne	Physica C,253(1995)71-78	B.A. Hunter,H. Shaked,H. Takahashi,J.D. Jorgensen,N. Mori,R.L. Hitterman,T. Kondo,T. Manako,Y. Kubo,Y. Shimakawa	Tl, Sr, Ca, Cu, O	
6358	PHC2530071	hydrostatic 1.5GPa	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-z	Tl	1	Sr	2	Ca	1	Cu	2													O	7-z			1995																												Tl1212																				72					72			K/GPa	-1.1																																																																																												see Phys.Rev.B,45(1992)5553					Pressure effects on Tc and structurein overdoped TISr2CaCu2O7-z	199510		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory, Argonne	Physica C,253(1995)71-78	B.A. Hunter,H. Shaked,H. Takahashi,J.D. Jorgensen,N. Mori,R.L. Hitterman,T. Kondo,T. Manako,Y. Kubo,Y. Shimakawa	Tl, Sr, Ca, Cu, O	
6359	SSC0920595			Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1994																											2	Hg1223				3.85		15.85														133				133	133																																																																																																					SYNTHESIS AND X-RAY POWDER DIFFRACTION ANALYSIS OF THE HIGH-Tc SUPERCONDUCTOR HgBa2Ca2Cu3O8+delta			Department of Physics, National Laratory of Solid State Microstructure, Nanjing university, Nanjing, 210008, P.R. China	Solid State Commun.,92(1994)595-599	G.C. Che,G.N. Zhang,H.L. Ji,H.M. Shao,J.C. Shen,K. Zhou,L.J. Shen,X.N. Xu,X.X. Yao,Y. Rui,Z. Wu,Z.J. Li,Z.X. Zhao		
6360	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.03	Hg	1	Ba	2	Cu	1															O	4+z	4.03		1995																												Hg1201																							4.2																																																																																																		precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6361	PHC2610033		(Ca,La)(Ba,La)2Cu3O7	Ca0.63La0.37Ba1.12La0.88Cu3Oz	Ca	0.63	La	0.37	Ba	1.12	La	0.88	Cu	3											O	z			1996																												Y123																				67.4					67.4																																																																																																prepared by lasen ablation from x=0.45 target Ca-content by changing the distance between target and substrate   substrate+ SrTiO3(100)					Characterization of tetragonal 1:2:3  (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy thin films prepared by laser ablasion deposition			Department of Physics and Crown Center for Superconductivity, Technion-Israel Institute of Technology,Haifa 32000, Israel	Physica.C,261(1996)33-37	A. Knizhnik,C. Chabaud,D. Goldschmidt,G. Koren,G.M. Reisner,I. Gertner,Y. Direktovitch,Y. Eckstein		
6362	PHC2610033		(Ca,La)(Ba,La)2Cu3O7	Ca0.49La0.51Ba1.26La0.74Cu3Oz	Ca	0.49	La	0.51	Ba	1.26	La	0.74	Cu	3											O	z			1996																												Y123																				71.9					71.9																																																																																																prepared by lasen ablation from x=0.45 target Ca-content by changing the distance between target and substrate   substrate+ SrTiO3(100)					Characterization of tetragonal 1:2:3  (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy thin films prepared by laser ablasion deposition			Department of Physics and Crown Center for Superconductivity, Technion-Israel Institute of Technology,Haifa 32000, Israel	Physica.C,261(1996)33-37	A. Knizhnik,C. Chabaud,D. Goldschmidt,G. Koren,G.M. Reisner,I. Gertner,Y. Direktovitch,Y. Eckstein		
6363	PHC2610033		(Ca,La)(Ba,La)2Cu3O7	Ca0.46La0.54Ba1.29La0.71Cu3Oz	Ca	0.46	La	0.54	Ba	1.29	La	0.71	Cu	3											O	z			1996																												Y123																				76.3					76.3																																																																																																prepared by lasen ablation from x=0.45 target Ca-content by changing the distance between target and substrate   substrate+ SrTiO3(100)					Characterization of tetragonal 1:2:3  (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy thin films prepared by laser ablasion deposition			Department of Physics and Crown Center for Superconductivity, Technion-Israel Institute of Technology,Haifa 32000, Israel	Physica.C,261(1996)33-37	A. Knizhnik,C. Chabaud,D. Goldschmidt,G. Koren,G.M. Reisner,I. Gertner,Y. Direktovitch,Y. Eckstein		
6364	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.7Tl0.3Ba1.95La0.05Cu1Oz	Hg	0.7	Tl	0.3	Ba	1.95	La	0.05	Cu	1											O	z			1996																											2	Hg1201																				32.1					32.1																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6365	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.7Tl0.3Ba1.9La0.1Cu1Oz	Hg	0.7	Tl	0.3	Ba	1.9	La	0.1	Cu	1											O	z			1996																											2	Hg1201																				40.3					40.3																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6366	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.7Tl0.3Ba1.8La0.2Cu1Oz	Hg	0.7	Tl	0.3	Ba	1.8	La	0.2	Cu	1											O	z			1996																											2	Hg1201																				52.6					52.6																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6367	PHC2620001		(Hg,Tl)(Ba,La)2CuOz	Hg0.6Tl0.4Ba1.6La0.4Cu1Oz	Hg	0.6	Tl	0.4	Ba	1.6	La	0.4	Cu	1											O	z			1996																											2	Hg1201																				21.5					21.5																																																																																														HgO,Yl2O3,BaO2,La2O3,CuO	1	mixture-pellet-sealed in evacuated quartz tubu-heat to 780C (10C/min)-hold (30-60min)-rapid cool to RT					Superconductivity in the overdoping state of (Hg,Tl)(Ba,La)2CuOv and(Hg,Tl)2 Ba2CuOv systems			Department of Chemistry, Tohoku University,Kawauchi,Aoba-ku,sendai 980-77, Japan	Physica.C,262(1996)1-6	Kenzo Nagase,Satoru Nakajima,Takeo Oku,Yasuhiko Syono		
6368	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O7	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	7		1993																												Y123																				81.8					81.8																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6369	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.9	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.9		1993																												Y123																				88.6					88.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6370	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.8	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.8		1993																												Y123																				84.1					84.1																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6371	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.7	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.7		1993																												Y123																				71					71																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6372	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.6	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.6		1993																												Y123																				65.3					65.3																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6373	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.5	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.5		1993																												Y123																				54.5					54.5																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6374	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.4	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.4		1993																												Y123																				41.8					41.8																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6375	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O7	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	7		1993																												Y123																				71.6					71.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6376	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.9	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.9		1993																												Y123																				82.9					82.9																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6377	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.8	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.8		1993																												Y123																				84.1					84.1																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6378	PHC2040237		(Y,Ca)BaCu3Oz	Y0.8Ca0.2Ba2Cu3O6.7	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.7		1993																												Y123																				76.7					76.7																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6379	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.6	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.6		1993																												Y123																				72.1					72.1																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6380	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.5	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.5		1993																												Y123																				61.9					61.9																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6381	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.4	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.4		1993																												Y123																				52.6					52.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6382	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.3	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.3		1993																												Y123																				40.6					40.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6383	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O7	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	7		1993																												Y123																				88.6					88.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6384	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.9	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.9		1993																												Y123																				81.8					81.8																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6385	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.85	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.85		1993																												Y123																				67					67																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6386	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.8	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.8		1993																												Y123																				57.9					57.9																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6387	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.7	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.7		1993																												Y123																				54.5					54.5																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6388	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.6	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.6		1993																												Y123																				50.6					50.6																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6389	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.5	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-z	6.5		1993																												Y123																				32.9					32.9																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6390	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O7	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	7		1993																												Y123																				81.8					81.8																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6391	PHC2040237		Y(BaLa2Cu3Oz)	Y1Ba1.8La0.2Cu3O6.9	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	6.9		1993																												Y123																				61.4					61.4																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6392	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O6.85	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	6.85		1993																												Y123																				51.4					51.4																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6393	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O6.8	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	6.8		1993																												Y123																				47.2					47.2																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6394	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O6.7	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	6.7		1993																												Y123																				44.3					44.3																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6395	PHC2040237		Y(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O6.6	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-z	6.6		1993																												Y123																				28.1					28.1																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6396	PHC1740383	fully oxygenated		Y1Ba1.9La0.1Cu3Oz	Y	1	Ba	1.9	La	0.1	Cu	3													O	z		1	1991																											3	Y123				3.818	3.884	11.672																96.1			96.1																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6397	PHC1740383	fully oxygenated		Y1Ba1.8La0.2Cu3Oz	Y	1	Ba	1.8	La	0.2	Cu	3													O	z		1	1991																											3	Y123				3.8182	3.889	11.65																81.3			81.3																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6398	PHC1740383	fully oxygenated		Y1Ba1.7La0.3Cu3Oz	Y	1	Ba	1.7	La	0.3	Cu	3													O	z		1	1991																											3	Y123				3.824	3.889	11.628																65.6			65.6																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6399	PHC1740383	fully oxygenated		Y1Ba1.6La0.4Cu3Oz	Y	1	Ba	1.6	La	0.4	Cu	3													O	z		1	1991																											2	Y123				3.857		11.585																50.1			50.1																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6400	PHC1740383	fully oxygenated		Y1Ba1.5La0.5Cu3Oz	Y	1	Ba	1.5	La	0.5	Cu	3													O	z		1	1991																											2	Y123				3.86		11.559																42.6			42.6																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6401	PHC1740383	fully oxygenated		Y1Ba1.4La0.6Cu3Oz	Y	1	Ba	1.4	La	0.6	Cu	3													O	z		1	1991																											2	Y123				3.856		11.545																13.2			13.2																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6402	PHC1740383		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O7	Y	1	Ba	1.9	La	0.1	Cu	3													O	7	7		1991																												Y123																						96.1			96.1																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6403	PHC1740383		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O7	Y	1	Ba	1.8	La	0.2	Cu	3													O	7	7		1991																												Y123																						76.3			76.3																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6404	PHC1740383		Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3O7	Y	1	Ba	1.7	La	0.3	Cu	3													O	7	7		1991																												Y123																						54.8			54.8																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6405	PHC1740383		Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3O7	Y	1	Ba	1.6	La	0.4	Cu	3													O	7	7		1991																												Y123																						32.2			32.2																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6406	PHC1740383		Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3O7	Y	1	Ba	1.5	La	0.5	Cu	3													O	7	7		1991																												Y123																						0.3			0.3																																																																																																Samples were folly loaded by slow cooling to 380C in oxygen					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6407	PHC1740383		(Y,Ca)(Ba,Ca)2Cu3O7	Y0.962Ba1.987Ca0.05Cu3Oz	Y	0.962	Ba	1.987	Ca	0.05	Cu	3													O	z			1991																												Y123																						86			86																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6408	PHC1740383		(Y,Ca)(Ba,Ca)2Cu3O7	Y0.925Ba1.975Ca0.1Cu3Oz	Y	0.925	Ba	1.975	Ca	0.1	Cu	3													O	z			1991																											3	Y123				3.819	3.881	11.688																84.2			84.2																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6409	PHC1740383		(Y,Ca)(Ba,Ca)2Cu3O7	Y0.85Ba1.95Ca0.2Cu3Oz	Y	0.85	Ba	1.95	Ca	0.2	Cu	3													O	z			1991																											3	Y123				3.82	3.876	11.697																81.7			81.7																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6410	PHC1740383		(Y,Ca)(Ba,Ca)2Cu3O7	Y0.775Ba1.925Ca0.3Cu3Oz	Y	0.775	Ba	1.925	Ca	0.3	Cu	3													O	z			1991																											3	Y123				3.819	3.878	11.692																81			81																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6411	PHC1740383		(Y,Ca)2(Ba,Ca)4Cu7O15	Y0.961Ba1.987Ca0.052Cu3.5O7.5-z	Y	0.961	Ba	1.987	Ca	0.052	Cu	3.5													O	7.5-z			1991																											3	Y247				3.833	3.876	50.59																93.5			93.5																																																																																																adding 0.2 mole NaNO3 as areaction enhancer, (865C, in flowing O2)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6412	PHC1740383		(Y,Ca)2(Ba,Ca)4Cu7O15	Y0.98Ba1.993Ca0.026Cu3.5O7.5-z	Y	0.98	Ba	1.993	Ca	0.026	Cu	3.5													O	7.5-z			1991																											3	Y247				3.833	3.877	50.58																94.2			94.2																																																																																																adding 0.2 mole NaNO3 as areaction enhancer, (865C, in flowing O2)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6413	PHC1740383		(Y,Ca)2(Ba,Ca)4Cu7O15	Y0.99Ba1.997Ca0.013Cu3.5O7.5-z	Y	0.99	Ba	1.997	Ca	0.013	Cu	3.5													O	7.5-z			1991																											3	Y247				3.835	3.878	50.59																92.8			92.8																																																																																																adding 0.2 mole NaNO3 as areaction enhancer, (865C, in flowing O2)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6414	PHC1740383		(Y,Ca)2(Ba,Ca)4Cu7O15	Y1Ba2Cu3.5O7.5-z	Y	1	Ba	2	Cu	3.5															O	7.5-z			1991																											3	Y247				3.836	3.878	50.583																91			91																																																																																																adding 0.2 mole NaNO3 as areaction enhancer, (865C, in flowing O2)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6415	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.98La0.02Cu3.5O7.5-z	Y	1	Ba	1.98	La	0.02	Cu	3.5													O	7.5-z			1991																											3	Y247				3.834	3.881	50.548																87.8			87.8																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6416	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.925La0.075Cu3.5O7.5-z	Y	1	Ba	1.925	La	0.075	Cu	3.5													O	7.5-z			1991																											3	Y247				3.833	3.878	50.492																77.3			77.3																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6417	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.9La0.1Cu3.5O7.5-z	Y	1	Ba	1.9	La	0.1	Cu	3.5													O	7.5-z			1991																											3	Y247				3.837	3.878	50.443																70.5			70.5																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6418	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.875La0.125Cu3.5O7.5-z	Y	1	Ba	1.875	La	0.125	Cu	3.5													O	7.5-z			1991																											3	Y247																						64			64																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6419	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.85La0.15Cu3.5O7.5-z	Y	1	Ba	1.85	La	0.15	Cu	3.5													O	7.5-z			1991																											3	Y247				3.837	3.877	50.373																62.2			62.2																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6420	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.825La0.175Cu3.5O7.5-z	Y	1	Ba	1.825	La	0.175	Cu	3.5													O	7.5-z			1991																											3	Y247																						54.3			54.3																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6421	PHC1740383		Y2(Ba,La)4Cu7O15	Y1Ba1.8La0.2Cu3.5O7.5-z	Y	1	Ba	1.8	La	0.2	Cu	3.5													O	7.5-z			1991																											3	Y247																						50.7			50.7																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6422	PHC1740383		Y(Ba,Ca)2Cu4O8	Y1Ba1.9Ca0.1Cu4O8	Y	1	Ba	1.9	Ca	0.1	Cu	4													O	8		1	1991																											3	Y124				3.84	3.866	27.247																85.4			85.4																																																																																																reaction (8.24C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6423	PHC1740383		Y(Ba,Ca)2Cu4O8	Y1Ba1.926Ca0.074Cu4O8	Y	1	Ba	1.926	Ca	0.074	Cu	4													O	8		1	1991																											3	Y124				3.84	3.869	27.241																83.3			83.3																																																																																																reaction (8.24C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6424	PHC1740383		Y(Ba,Ca)2Cu4O8	Y1Ba1.972Ca0.028Cu4O8	Y	1	Ba	1.972	Ca	0.028	Cu	4													O	8		1	1991																											3	Y124				3.841	3.87	27.244																79.7			79.7																																																																																																reaction (8.24C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6425	PHC1740383		Y(Ba,Ca)2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1991																											3	Y124				3.842	3.871	27.24																77.9			77.9																																																																																																reaction (8.24C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6426	PHC1740383		Y(Ba,La)2Cu4O8	Y1Ba1.98La0.02Cu4O8	Y	1	Ba	1.98	La	0.02	Cu	4													O	8			1991																											3	Y124				3.843	3.87	27.25																74.3			74.3																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6427	PHC1740383		Y(Ba,La)2Cu4O8	Y1Ba1.9La0.1Cu4O8	Y	1	Ba	1.9	La	0.1	Cu	4													O	8			1991																											3	Y124				3.842	3.875	27.218																61			61																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6428	PHC1740383		Y(Ba,La)2Cu4O8	Y1Ba1.87La0.13Cu4O8	Y	1	Ba	1.87	La	0.13	Cu	4													O	8			1991																											3	Y124				3.841	3.876	27.208																61			61																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6429	PHC1740383		Y(Ba,La)2Cu4O8	Y1Ba1.78La0.22Cu4O8	Y	1	Ba	1.78	La	0.22	Cu	4													O	8			1991																											3	Y124				3.841	3.881	27.174																37.9			37.9																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6430	PHC1740383		Y(Ba,La)2Cu4O8	Y1Ba1.72La0.28Cu4O8	Y	1	Ba	1.72	La	0.28	Cu	4													O	8			1991																											3	Y124				3.841	3.877	27.132																18.9			18.9																																																																																																react(900C,2nights in air)-react(930C)					CA-AND LA-SUBSTITUTION IN YBA2CU3O7-Z,Y2BA4CU7O15-Z AND YBA2CU4O8			DSIR PHYSICAL SCIENCES AND DSIR CHEMISTRY PO BOX 31313,LOWER HUTT,NEW ZEALAND	PHYSICA C,174(1991)383	D.M.POOKE,G.V.M.WILLIAMS,H.L.JOHNSON,J.L.TALLON,M.BOWDEN,M.MEYLAN,M.P.STAINES,M.R.PRESLAND,N.E.FLOWER,R.G.BUCKLEY	Y,BA,CU,O	
6431	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	z	6.94		1989																											3					3.821	3.89	11.678														92					92																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6432	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba1.9La0.1Cu3O6.92	Y	1	Ba	1.9	La	0.1	Cu	3													O	z	6.92		1989																											3																					93					93																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6433	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba1.8La0.2Cu3O6.96	Y	1	Ba	1.8	La	0.2	Cu	3													O	z	6.96		1989																											3																					82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6434	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba1.7La0.3Cu3O7.02	Y	1	Ba	1.7	La	0.3	Cu	3													O	z	7.02		1989																											2																					61					61																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6435	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba1.6La0.4Cu3O7.06	Y	1	Ba	1.6	La	0.4	Cu	3													O	z	7.06		1989																											2																					52					52																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6436	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y1Ba1.5La0.5Cu3O7.1	Y	1	Ba	1.5	La	0.5	Cu	3													O	z	7.1		1989																											2																					30					30																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6437	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.9La0.1Cu3O6.95	Y	0.9	Ca	0.1	Ba	1.9	La	0.1	Cu	3											O	z	6.95		1989																											3					3.817	3.884	11.663														86					86																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6438	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.8La0.2Cu3O6.97	Y	0.9	Ca	0.1	Ba	1.8	La	0.2	Cu	3											O	z	6.97		1989																											3																					87					87																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6439	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.7La0.3Cu3O7.04	Y	0.9	Ca	0.1	Ba	1.7	La	0.3	Cu	3											O	z	7.04		1989																											3																					82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6440	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.6La0.4Cu3O7.09	Y	0.9	Ca	0.1	Ba	1.6	La	0.4	Cu	3											O	z	7.09		1989																											2																					72					72																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6441	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.5La0.5Cu3O7.13	Y	0.9	Ca	0.1	Ba	1.5	La	0.5	Cu	3											O	z	7.13		1989																											2																					60					60																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6442	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.6La6Cu3O7.18	Y	0.9	Ca	0.1	Ba	1.6	La	6	Cu	3											O	z	7.18		1989																											2																					43					43																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6443	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.8La0.2Cu3O6.94	Y	0.8	Ca	0.2	Ba	1.8	La	0.2	Cu	3											O	z	6.94		1989																											3					3.821	3.88	11.653														84					84																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6444	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.5La0.5Cu3O7.11	Y	0.8	Ca	0.2	Ba	1.5	La	0.5	Cu	3											O	z	7.11		1989																											2																					80					80																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6445	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.4La0.6Cu3O7.15	Y	0.8	Ca	0.2	Ba	1.4	La	0.6	Cu	3											O	z	7.15		1989																											2																					66					66																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6446	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.7Ca0.3Ba1.7La0.3Cu3O6.92	Y	0.7	Ca	0.3	Ba	1.7	La	0.3	Cu	3											O	z	6.92		1989																											3					3.828	3.869	11.645														82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6447	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.7Ca0.3Ba1.4La0.6Cu3O7.12	Y	0.7	Ca	0.3	Ba	1.4	La	0.6	Cu	3											O	z	7.12		1989																											2																					82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6448	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.7Ca0.3Ba1.3La0.7Cu3O7.16	Y	0.7	Ca	0.3	Ba	1.3	La	0.7	Cu	3											O	z	7.16		1989																											2																					73					73																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6449	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.6La0.4Cu3O6.95	Y	0.6	Ca	0.4	Ba	1.6	La	0.4	Cu	3											O	z	6.95		1989																											2					3.852		11.63														82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6450	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.4La0.6Cu3O7.07	Y	0.6	Ca	0.4	Ba	1.4	La	0.6	Cu	3											O	z	7.07		1989																											2																					83					83																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6451	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.3La0.7Cu3O7.12	Y	0.6	Ca	0.4	Ba	1.3	La	0.7	Cu	3											O	z	7.12		1989																											2																					82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6452	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.2La0.8Cu3O7.15	Y	0.6	Ca	0.4	Ba	1.2	La	0.8	Cu	3											O	z	7.15		1989																											2																					67					67																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6453	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.1La0.9Cu3O7.18	Y	0.6	Ca	0.4	Ba	1.1	La	0.9	Cu	3											O	z	7.18		1989																											2																					47					47																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6454	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.5Ca0.5Ba1.5La0.5Cu3O6.94	Y	0.5	Ca	0.5	Ba	1.5	La	0.5	Cu	3											O	z	6.94		1989																											2					3.854		11.617														82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6455	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.5Ca0.5Ba1.2La0.8Cu3O7.12	Y	0.5	Ca	0.5	Ba	1.2	La	0.8	Cu	3											O	z	7.12		1989																											2	Y123																				82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6456	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.5Ca0.5Ba1.1La0.9Cu3O7.15	Y	0.5	Ca	0.5	Ba	1.1	La	0.9	Cu	3											O	z	7.15		1989																											2	Y123																				70					70																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6457	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.4Cu0.6Ba1.4La0.6Cu3O6.95	Y	0.4	Cu	0.6	Ba	1.4	La	0.6	Cu	3											O	z	6.95		1989																											2	Y123				3.856		11.594														81					81																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6458	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.4Cu0.6Ba1.3La0.7Cu3O7	Y	0.4	Cu	0.6	Ba	1.3	La	0.7	Cu	3											O	z	7		1989																											2	Y123																				82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6459	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.4Ca0.6Ba1.2La0.8Cu3O7.07	Y	0.4	Ca	0.6	Ba	1.2	La	0.8	Cu	3											O	z	7.07		1989																											2	Y123																				82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6460	FA1590760		(Y,Ca)(Ba,La)2Cu3Oz	Y0.4Ca0.6Ba1.1La0.9Cu3O7.12	Y	0.4	Ca	0.6	Ba	1.1	La	0.9	Cu	3											O	z	7.12		1989																											2	Y123																				82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6461	FA1590760		La(Ba,Ca)2Cu3Oz	La1Ba1.87Ca0.13Cu3O6.923	La	1	Ba	1.87	Ca	0.13	Cu	3													O	z	6.923		1989																																3.905	3.919	11.764														82					82																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6462	FA1590760		La(Ba,Ca)2Cu3Oz	La1Ba1.75Ca0.25Cu3O6.951	La	1	Ba	1.75	Ca	0.25	Cu	3													O	z	6.951		1989																																3.898		11.741														80					80																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6463	FA1590760		La(Ba,Ca)2Cu3Oz	La1Ba1.5Ca0.5Cu3O6.96	La	1	Ba	1.5	Ca	0.5	Cu	3													O	z	6.96		1989																																3.89		11.706														79.9					79.9																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6464	FA1590760		La(Ba,Ca)2Cu3Oz	La1Ba1.25Ca0.75Cu3O6.958	La	1	Ba	1.25	Ca	0.75	Cu	3													O	z	6.958		1989																																3.882		11.655														79.9					79.9																																																																																												/cm3				mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6465	FA1590760		La(Ba,Ca)2Cu3Oz	La1Ba1Ca1Cu3Oz	La	1	Ba	1	Ca	1	Cu	3													O	z			1989																																3.872		11.613														80.1					80.1																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6466	FA1590760		Y(Ba,Sr)2Cu3Oz	Y1Ba2Cu3O6.939	Y	1	Ba	2	Cu	3															O	z	6.939		1989																																3.824	3.89	11.677														91.8					91.8																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6467	FA1590760		Y(Ba,Sr)2Cu3Oz	Y1Ba1.75Sr0.25Cu3O6.928	Y	1	Ba	1.75	Sr	0.25	Cu	3													O	z	6.928		1989																																3.812	3.88	11.642														89.6					89.6																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6468	FA1590760		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.938	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.938		1989																																3.805	3.87	11.615														87.6					87.6																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6469	FA1590760		Y(Ba,Sr)2Cu3Oz	Y1Ba1.25Sr0.75Cu3O6.928	Y	1	Ba	1.25	Sr	0.75	Cu	3													O	z	6.928		1989																																3.799	3.86	11.581														85.5					85.5																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6470	FA1590760		Y(Ba,Sr)2Cu3Oz	Y1Ba1Sr1Cu3O6.947	Y	1	Ba	1	Sr	1	Cu	3													O	z	6.947		1989																																3.793	3.849	11.546														83.3					83.3																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6471	FA1590760		La(Ba,Sr)2Cu3Oz	La1Ba1.75Sr0.25Cu3O6.946	La	1	Ba	1.75	Sr	0.25	Cu	3													O	z	6.946		1989																																3.909		11.782														72.5					72.5																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6472	FA1590760		La(Ba,Sr)2Cu3Oz	La1Ba1.5Sr0.5Cu3O6.967	La	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.967		1989																																3.898		11.759														65.2					65.2																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6473	FA1590760		La(Ba,Sr)2Cu3Oz	La1Ba1.25Sr0.75Cu3O6.996	La	1	Ba	1.25	Sr	0.75	Cu	3													O	z	6.996		1989																																3.894		11.733														54.1					54.1																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6474	FA1590760		La(Ba,Sr)2Cu3Oz	La1Ba1Sr1Cu3O7.01	La	1	Ba	1	Sr	1	Cu	3													O	z	7.01		1989																																3.885		11.714														41.5					41.5																																																																																																mixture-(920-950C,20H)-reground-(920-950C,15H)-ANN(450C,6H in O2)-cool to 200C in O2-hold(10-12H) at each 50C interual					FACTORS INFLUENCING TC IN 123 COPPER-OXIDE SUPERCONDUCTORS	198908			PHYS.C.159(1989)760	GOODENOUGH J.B.,MANTHIRAM A.		
6475	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.03	Hg	1	Ba	2	Cu	1															O	4+z	4.03		1995																												Hg1201																				49.9					49.9																																																																																																precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6476	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.18	Hg	1	Ba	2	Cu	1															O	z	4.18		1995																												Hg1201																				93.2					93.2																																																																																																precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6477	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.27	Hg	1	Ba	2	Cu	1															O	4+z	4.27		1995																												Hg1201																				86.7					86.7																																																																																																precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6478	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.36	Hg	1	Ba	2	Cu	1															O	4+z	4.36		1995																												Hg1201																				40					40																																																																																																precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6479	PHC2510216		HgBa2CuO4	Hg1Ba2Cu1O4.39	Hg	1	Ba	2	Cu	1															O	4+z	4.39		1995																												Hg1201																				24.6					24.6																																																																																																precursor(Ba2CuOz)+Hg-evacuated quart-heat(810C),for details see Physica C 231(1994)233					Dependence of Tc on hole concentration in HgBa2CuO4+delta			Texas Center for Superconductivity at the University of Houston and the Department of Physics, Houston TX 77204-5932, USA	Physica.C,251(1995)216-218	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Xue		
6480	PHC2040237		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.3	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.3		1993																												Y123																				28.1					28.1																																																																																																					STOICHIOMETRIC YBA2CU3O7 IS OVERDOPED	199301			PHYSICA C,204(1993)237	J.L.TALLON,N.E.FLOWER	Y,BA,CU,O	
6481	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.5Ba1.4Cu3OO7.001	Nd	1.5	Ba	1.4	Cu	3	O														O	z	7.001	1	1996																											2	Y123				3.877		11.61																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6482	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.4Ba1.4Ca0.2Cu3O6.976	Nd	1.4	Ba	1.4	Ca	0.2	Cu	3													O	z	6.976	1	1996																											2	Y123				3.88		11.643																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6483	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.3Ba1.5Ca0.2Cu3O6.952	Nd	1.3	Ba	1.5	Ca	0.2	Cu	3													O	z	6.952	1	1996																											2	Y123				3.883		11.663																36			36																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6484	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.2Ba1.6Ca0.2Cu3O6.929	Nd	1.2	Ba	1.6	Ca	0.2	Cu	3													O	z	6.929	1	1996																											2	Y123				3.888		11.697																51			51																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6485	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.1Ba1.7Ca0.2Cu3O6.894	Nd	1.1	Ba	1.7	Ca	0.2	Cu	3													O	z	6.894	1	1996																											2	Y123				3.892		11.732																65			65																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6486	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1Ba1.8Ca0.2Cu3O6.866	Nd	1	Ba	1.8	Ca	0.2	Cu	3													O	z	6.866	1	1996																											2	Y123				3.896		11.759																73			73																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6487	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.5Ba1.1Ca0.4Cu3O6.975	Nd	1.5	Ba	1.1	Ca	0.4	Cu	3													O	z	6.975	1	1996																											2	Y123				3.871		11.579																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6488	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.4Ba1.2Ca0.4Cu3O6.945	Nd	1.4	Ba	1.2	Ca	0.4	Cu	3													O	z	6.945	1	1996																											2	Y123				3.873		11.608																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6489	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.3Ba1.3Ca0.4Cu3O6.912	Nd	1.3	Ba	1.3	Ca	0.4	Cu	3													O	z	6.912	1	1996																											2	Y123				3.876		11.637																13			13																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6490	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.2Ba1.4Ca0.4Cu3O6.888	Nd	1.2	Ba	1.4	Ca	0.4	Cu	3													O	z	6.888	1	1996																											2	Y123				3.88		11.666																40			40																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6491	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1.1Ba1.5Ca0.4Cu3O6.864	Nd	1.1	Ba	1.5	Ca	0.4	Cu	3													O	z	6.864	1	1996																											2	Y123				3.883		11.696																54			54																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6492	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd1Ba1.6Ca0.4Cu3O6.828	Nd	1	Ba	1.6	Ca	0.4	Cu	3													O	z	6.828	1	1996																											2	Y123				3.887		11.719																65			65																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6493	PHC2610105		(Nd,Ba,Ca)3Cu3Oz	Nd0.9Ba1.7Ca0.4Cu3O6.801	Nd	0.9	Ba	1.7	Ca	0.4	Cu	3													O	z	6.801	1	1996																											2	Y123				3.89		11.749																72			72																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6494	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.1Ba1.7Sr0.2Cu3O6.858	Nd	1.1	Ba	1.7	Sr	0.2	Cu	3													O	z	6.858	1	1996																											2	Y123				3.892		11.732																70			70																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6495	PHC2610105		(Nd,Ba,Sr)2Cu3Oz	Nd1Ba1.8Sr0.2Cu3O6.927	Nd	1	Ba	1.8	Sr	0.2	Cu	3													O	z	6.927	1	1996																											2	Y123				3.896		11.76																82			82																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6496	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.5Ba1.1Sr0.4Cu3O6.916	Nd	1.5	Ba	1.1	Sr	0.4	Cu	3													O	z	6.916	1	1996																											2	Y123				3.871		11.58																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6497	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.4Ba1.2Sr0.4Cu3O6.874	Nd	1.4	Ba	1.2	Sr	0.4	Cu	3													O	z	6.874	1	1996																											2	Y123				3.873		11.607																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6498	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.3Ba1.3Sr0.4O6.828	Nd	1.3	Ba	1.3	Sr	0.4															O	z	6.828	1	1996																											2	Y123				3.876		11.635																35			35																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6499	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.2Ba1.4Sr0.4Cu3O6.789	Nd	1.2	Ba	1.4	Sr	0.4	Cu	3													O	z	6.789	1	1996																											2	Y123				3.88		11.665																41			41																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6500	PHC2610105		(Nd,Ba,Sr,)3Cu3Oz	Nd1.2Ba1.4Sr0.4Cu3O6.731	Nd	1.2	Ba	1.4	Sr	0.4	Cu	3													O	z	6.731	1	1996																											2	Y123				3.883		11.695																65			65																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6501	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1Ba1.6Sr0.4Cu3O6.721	Nd	1	Ba	1.6	Sr	0.4	Cu	3													O	z	6.721	1	1996																											2	Y123				3.887		11.719																78.5			78.5																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6502	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd0.9Ba1.7Sr0.4Cu3O6.666	Nd	0.9	Ba	1.7	Sr	0.4	Cu	3													O	z	6.666	1	1996																											2	Y123				3.89		11.748																82			82																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6503	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.6Ba1.2Sr0.2Cu3O7.015	Nd	1.6	Ba	1.2	Sr	0.2	Cu	3													O	z	7.015	1	1996																											2	Y123				3.872		11.584																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6504	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.5Ba1.3Sr0.2Cu3O6.978	Nd	1.5	Ba	1.3	Sr	0.2	Cu	3													O	z	6.978	1	1996																											2	Y123				3.877		11.61																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6505	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.4Ba1.4Sr0.2Cu3O6.956	Nd	1.4	Ba	1.4	Sr	0.2	Cu	3													O	z	6.956	1	1996																											2	Y123				3.88		11.643																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6506	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.3Ba1.5Sr0.2Cu3O6.917	Nd	1.3	Ba	1.5	Sr	0.2	Cu	3													O	z	6.917	1	1996																											2	Y123				3.883		11.661																36			36																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6507	PHC2610105		(Nd,Ba,Sr)3Cu3Oz	Nd1.2Ba1.6Sr0.2Cu3O6.885	Nd	1.2	Ba	1.6	Sr	0.2	Cu	3													O	z	6.885	1	1996																											2	Y123				3.888		11.696																45			45																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6508	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.6Ba1.4Cu3O7.049	Nd	1.6	Ba	1.4	Cu	3															O	z	7.049		1996																											2	Y123				3.879		11.592																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6509	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.5Ba1.5Cu3O7.024	Nd	1.5	Ba	1.5	Cu	3															O	z	7.024		1996																											2	Y123				3.882		11.637																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6510	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.4Ba1.6Cu3O7.002	Nd	1.4	Ba	1.6	Cu	3															O	z	7.002		1996																											2	Y123				3.887		11.658																																																																																																																	ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6511	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.3Ba1.7Cu3O6.987	Nd	1.3	Ba	1.7	Cu	3															O	z	6.987		1996																											2	Y123				3.889		11.696																33			33																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6512	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.2Ba1.8Cu3O6.954	Nd	1.2	Ba	1.8	Cu	3															O	z	6.954		1996																											2	Y123				3.894		11.735																50			50																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6513	PHC2610105		(Nd,Ba)3Cu3Oz	Nd1.1Ba1.9Cu3O6.935	Nd	1.1	Ba	1.9	Cu	3															O	z	6.935		1996																											2	Y123				3.901		11.787																76			76																																																																																														ND2O3,CUO,SrCO3,BaCO3,CaCO3		mixture-CAL-SIN-ANN(400C,4H in O2)					The superconducting solid solutions Nd1.5-xBa1.5+x-yMyCu3Oz (M=Ca,Sr)			Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB9 2UE, UK	Physica.C,261(1996)105-116	A.R. West,J.M.S. Skakle		
6514	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.842	3.87	27.194														79.7					79.7																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6520	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.99Ni0.01O8	Y	1	Ba	2	Cu	3.99	Ni	0.01													O	8			1996																											3	Y124																				78.4					78.4																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6521	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.99Zn0.01O8	Y	1	Ba	2	Cu	3.99	Zn	0.01													O	8			1996																											3	Y124																				73.3					73.3																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6522	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O	8			1996																											3	Y124				3.838	3.869	27.212														66.6					66.6																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6523	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.956Zn0.044O8	Y	1	Ba	2	Cu	3.956	Zn	0.044													O	8			1996																											3	Y124				3.84	3.871	27.21														56.8					56.8																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6524	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.94Zn0.06Oz	Y	1	Ba	2	Cu	3.94	Zn	0.06													O	z			1996																											3	Y124				3.841	3.872	27.21														46.8					46.8																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6525	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.92Zn0.08O8	Y	1	Ba	2	Cu	3.92	Zn	0.08													O	8			1996																											3	Y124																				36.4					36.4																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6526	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.9Zn0.1O8	Y	1	Ba	2	Cu	3.9	Zn	0.1													O	8			1996																											3	Y124				3.841	3.873	27.206														22.1					22.1																																																																																															1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6527	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.8Zn0.2O8	Y	1	Ba	2	Cu	3.8	Zn	0.2													O	8			1996																											3	Y124				3.842	3.874	27.202																	4.2																																																																																																	1	mixture-react+(650C,750C,880C,24H in air)-pellet-SIN(950C in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100 bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6528	PHC2610201		(Hg,Bi)Sr2(Ca,Pr)Cu2O6	Hg0.7Bi0.3Sr2Pr1Cu2O6+z	Hg	0.7	Bi	0.3	Sr	2	Pr	1	Cu	2											O	6+z			1996						3.11	14																				2	Hg1212				3.866		12.093																	4.2																																																																																																	1	precursor(Bi0.3Sr2(Ca,Pr)Cu2Oz)+HgO-mix-press-wrap in Aufoil-seal (evacuated quartz tubu)-heat(825C,8H)-cool to RT(5C/min)					Superconductivity and magnetism of the (Hg0.7Bi0.3)Sr2(Ca1-xPrx)Cu2O6+z system			Department of Electronic Engineering, Feng Chia University, Taichung, 407, Taiwan	Physica.C,261(1996)201-206	H.J. Tsao,J.B. Shi,M.F. Tai		
6529	PHC2610201	Jc(5K)=3.9E+6 A/cm2 for H=O, Jc(5K)=3E+6 A/cm2 for H=5KOe	(Hg,Bi)Sr2(Ca,Pr)Cu2O6	Hg0.7Bi0.3Sr2Ca0.75Pr0.25Cu2O6+z	Hg	0.7	Bi	0.3	Sr	2	Ca	0.75	Pr	0.25	Cu	2									O	6+z			1996																											2	Hg1212				3.833		12.107																91			91										11.2																																																																																					1	precursor(Bi0.3Sr2(Ca,Pr)Cu2Oz)+HgO-mix-press-wrap in Aufoil-seal (evacuated quartz tubu)-heat(825C,8H)-cool to RT(5C/min)					Superconductivity and magnetism of the (Hg0.7Bi0.3)Sr2(Ca1-xPrx)Cu2O6+z system			Department of Electronic Engineering, Feng Chia University, Taichung, 407, Taiwan	Physica.C,261(1996)201-206	H.J. Tsao,J.B. Shi,M.F. Tai		
6530	PHC2610201		(Hg,Bi)Sr2(Ca,Pr)Cu2O6	Hg0.7Bi0.3Sr2Ca0.5Pr0.5Cu2O6+z	Hg	0.7	Bi	0.3	Sr	2	Ca	0.5	Pr	0.5	Cu	2									O	6+z			1996																											2	Hg1212				3.84		12.1																58			58																																																																																															1	precursor(Bi0.3Sr2(Ca,Pr)Cu2Oz)+HgO-mix-press-wrap in Aufoil-seal (evacuated quartz tubu)-heat(825C,8H)-cool to RT(5C/min)					Superconductivity and magnetism of the (Hg0.7Bi0.3)Sr2(Ca1-xPrx)Cu2O6+z system			Department of Electronic Engineering, Feng Chia University, Taichung, 407, Taiwan	Physica.C,261(1996)201-206	H.J. Tsao,J.B. Shi,M.F. Tai		
6531	PHC2610201		(Hg,Bi)Sr2(Ca,Pr)Cu2O6	Hg0.7Bi0.3Sr2Ca0.25Pr0.75Cu2O6+z	Hg	0.7	Bi	0.3	Sr	2	Ca	0.25	Pr	0.75	Cu	2									O	6+z			1996																											2	Hg1212				3.854	12.093																		4.2																																																																																																	1	precursor(Bi0.3Sr2(Ca,Pr)Cu2Oz)+HgO-mix-press-wrap in Aufoil-seal (evacuated quartz tubu)-heat(825C,8H)-cool to RT(5C/min)					Superconductivity and magnetism of the (Hg0.7Bi0.3)Sr2(Ca1-xPrx)Cu2O6+z system			Department of Electronic Engineering, Feng Chia University, Taichung, 407, Taiwan	Physica.C,261(1996)201-206	H.J. Tsao,J.B. Shi,M.F. Tai		
6532	PHC2610090		(Er,Hg)Ba2Cu3Oz	Er1Ba2Cu3O6.953	Er	1	Ba	2	Cu	3															O	z	6.953	1	1996																											3	Y123				3.821	3.885	11.667														90.9					90.9																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6533	PHC2610090		(Er,Hf)Ba2Cu3Oz	Er0.95Hf0.05Ba2Cu3O6.938	Er	0.95	Hf	0.05	Ba	2	Cu	3													O	z	6.938	1	1996																											3	Y123				3.822	3.889	11.667														86					86																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6534	PHC2610090		(Er,Hg)Ba2Cu3Oz	Er0.9Hf0.1Ba2Cu3O6.862	Er	0.9	Hf	0.1	Ba	2	Cu	3													O	z	6.862	1	1996																											3	Y123				3.814	3.879	11.659														82.9					82.9																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6535	PHC2610090		(Er,Hg)Ba2Cu3Oz	Er0.85Hf0.15Ba2Cu3O6.813	Er	0.85	Hf	0.15	Ba	2	Cu	3													O	z	6.813	1	1996																											3	Y123				3.818	3.878	11.652														79.9					79.9																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6536	PHC2610090		(Er,Hg)Ba2Cu3Oz	Er0.8Hf0.2Ba2Cu3O6.772	Er	0.8	Hf	0.2	Ba	2	Cu	3													O	z	6.772	1	1996																											3	Y123				3.817	3.881	11.667														78.8					78.8																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6537	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.8Ca0.05Hf0.15Ba2Cu3O6.706	Er	0.8	Ca	0.05	Hf	0.15	Ba	2	Cu	3											O	z	6.706	1	1996																											3	Y123				3.828	3.876	11.646														64.8					64.8																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6538	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.75Ca0.1Hf0.15Ba2Cu3O6.796	Er	0.75	Ca	0.1	Hf	0.15	Ba	2	Cu	3											O	z	6.796	1	1996																											3	Y123				3.823	3.87	11.658														73.6					73.6																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6539	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.7Ca0.15Hf0.15Ba2Cu3O6.821	Er	0.7	Ca	0.15	Hf	0.15	Ba	2	Cu	3											O	z	6.821	1	1996																											3	Y123				3.825	3.876	11.649														77.3					77.3																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6540	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.65Ca0.2Hf0.15Ba2Cu3O6.83	Er	0.65	Ca	0.2	Hf	0.15	Ba	2	Cu	3											O	z	6.83	1	1996																											3	Y123				3.83	3.877	11.67														80.9					80.9																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6541	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.6Ca0.25Hf0.15Ba2Cu3O7.02	Er	0.6	Ca	0.25	Hf	0.15	Ba	2	Cu	3											O	z	7.02	1	1996																											3	Y123				3.829	3.873	11.702														84.7					84.7																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6542	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.55Ca0.3Hf0.15Ba2Cu3O7.05	Er	0.55	Ca	0.3	Hf	0.15	Ba	2	Cu	3											O	z	7.05	1	1996																											3	Y123				3.825	3.872	11.718														72.2					72.2																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6543	PHC2610090		(Er,Ca,Hf)Ba2Cu3O7	Er0.45Ca0.4Hf0.15Ba2Cu3O7.1	Er	0.45	Ca	0.4	Hf	0.15	Ba	2	Cu	3											O	z	7.1	1	1996																											3	Y123				3.817	3.875	11.718														66					66																																																																																														Er2 O3, Ba Co3, Cu O, Hf O2, Ca O	1	mixture-heat(940C,24H,in air in Pt crucible)-heat(940C,24H)-pellet-SIN(940C,24H in air)-ANN(450C,12H in flowing O2)					Effect of Hf and Hf-Ca substitution on the superconductivity of ErBa2Cu3O7-z			Department of Physics, Saurashtra University, Rajkot-360 005, India	Physica.C,261(1996)90-96	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi		
6544	JSC0950239		YSr2(Cu,Fe)3O7	Y1Sr2Cu2.6Fe0.4O6+z	Y	1	Sr	2	Cu	2.6	Fe	0.4													O	6+z			1991																											2	Y123				3.808		11.397													10						10																																																																																		2.5												Y2 O3, Sr Co3, Cu O, Fe2 O3	1	mixture-CAL(950C,12-18 in air)-pellet-heat(980C,16-24H in air)-ANN(500C,60-72 in O2)					Possible Superconductivity and Microstructuctural Investigation in Y1-xCaxSrCu2.6Fe0.4O6+z(x=0, 0.1)			Laboratoire de Physique des Solides de Belleuve, CNRS, F-92195 Meudon,France;UPR 210, CNRS, F-92195 Meudon, France	Journal solid state Chemistry 95(1991)239-243	L. OUHAMMOU,M. GASGNIER,M.O. RUAULT,MAMIDANNA S.R.RAO,N.LE NAGARD,O. GOROCHOV,P. TREMBLAY,R. SURYANARAYANAN	Y, Ca, Sr, Cu, Fe, O	
6545	JSC0950239		(Y,Ca)Sr2(Cu,Fe)3O7	Y0.9Ca0.1Sr2Cu2.6Fe0.4O6+z	Y	0.9	Ca	0.1	Sr	2	Cu	2.6	Fe	0.4											O	6+z			1991																											2	Y123				3.802		11.41													25			28			28																																																																																		1.5												Y2 O3, Sr Co3, Cu O, Fe2 O3	1	mixture-CAL(950C,12-18 in air)-pellet-heat(980C,16-24H in air)-ANN(500C,60-72 in O2)					Possible Superconductivity and Microstructuctural Investigation in Y1-xCaxSrCu2.6Fe0.4O6+z(x=0, 0.1)			Laboratoire de Physique des Solides de Belleuve, CNRS, F-92195 Meudon,France;UPR 210, CNRS, F-92195 Meudon, France	Journal solid state Chemistry 95(1991)239-243	L. OUHAMMOU,M. GASGNIER,M.O. RUAULT,MAMIDANNA S.R.RAO,N.LE NAGARD,O. GOROCHOV,P. TREMBLAY,R. SURYANARAYANAN	Y, Ca, Sr, Cu, Fe, O	
6546	SSC0990413		(Y,Pr)Sr2(Cu,Re)3O7	Y1Sr2Cu2.8Re2O7	Y	1	Sr	2	Cu	2.8	Re	2													O	7		1	1996																											2	Y123				3.813		11.52																42			42																																																																																														Y2 O3, Pr2 O3, Sr CO3, Re O2, Cu O		mixture-CAL(950C,12-18H in air)-pellet-heat(980C, 16-24H in air)-ANN(1000C,24H in O2)-FC					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6547	SSC0990413		(Y,Pr)Sr2(Cu,Re)3O7	Y0.25Pr0.75Sr2Cu0.2O7	Y	0.25	Pr	0.75	Sr	2	Cu	0.2													O	7		1	1996																											2	Y123				3.845		11.586																	5																																																																																																Y2 O3, Pr2 O3, Sr CO3, Re O2, Cu O		mixture-CAL(950C,12-18H in air)-pellet-heat(980C, 16-24H in air)-ANN(1000C,24H in O2)-FC					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6548	SSC0990413		(Y,Pr)Sr2(Cu,Re)3O7	Y1Sr2Cu2.8Re0.2O7	Y	1	Sr	2	Cu	2.8	Re	0.2													O	7		1	1996																											2	Y123				3.821		11.548																55			55																																																																																																see PREPID=6546 ,and ANN(480C,24H under 200 bar O2)-slow cool (0.1/min)					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6549	SSC0990413		(Y,Pr)Sr2(Cu,Re)3O7	Y0.25Pr0.75Sr2Cu2.8Re0.2O7	Y	0.25	Pr	0.75	Sr	2	Cu	2.8	Re	0.2											O	7		1	1996																											2	Y123				3.854		11.589																14			14																																																																																																see PREPID=6546 ,and ANN(480C,24H under 200 bar O2)-slow cool (0.1/min)					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6550	SSC0980761		RSr2Cu2.8(PO4)0.2Oz	Gd1Sr2Cu2.8P0.2Oz+0.8	Gd	1	Sr	2	Cu	2.8	P	0.2													O	z+0.8			1996																											2					3.841		11.34																	23																																																																																																R2O3, SrCO3, CaCO3, CuO ,NH4H2PO4	1	mixture-pellt-heat(1273-1338K,16H in flowing O2)-RT-heat(1273-1338K,12H in flowing O2)-cool to RT					PHOSHATE DERIVATIVES OF 123 CUPRATES OF THE FORMULA LnSr2Cu3O7(Ln=Gd,Dy,Ho)			Jawaharlal Nehru Centre for Advanced Scientlfic Research Jakkur Campus, Banglore 560 064, India	Solid State Commun.,98(1996)761	C.N.R. Rao,R. Gundakaram,R. Nagarajan	Gd, Dy, Ho, Sr, Cu, O	
6551	SSC0980761		RSr2Cu2.8(PO4)0.2Oz	Dy1Sr2Cu2.8P0.2Oz+0.8	Dy	1	Sr	2	Cu	2.8	P	0.2													O	z+0.8			1996																											2					3.824	11.32																		23																																																																																																R2O3, SrCO3, CaCO3, CuO ,NH4H2PO4	1	mixture-pellt-heat(1273-1338K,16H in flowing O2)-RT-heat(1273-1338K,12H in flowing O2)-cool to RT					PHOSHATE DERIVATIVES OF 123 CUPRATES OF THE FORMULA LnSr2Cu3O7(Ln=Gd,Dy,Ho)			Jawaharlal Nehru Centre for Advanced Scientlfic Research Jakkur Campus, Banglore 560 064, India	Solid State Commun.,98(1996)761	C.N.R. Rao,R. Gundakaram,R. Nagarajan	Gd, Dy, Ho, Sr, Cu, O	
6552	SSC0980761		RSr2Cu2.8(PO4)0.2Oz	Ho1Sr2Cu2.8P0.2Oz+0.8	Ho	1	Sr	2	Cu	2.8	P	0.2													O	z+0.8			1996																											2					3.816		11.27																	23																																																																																																R2O3, SrCO3, CaCO3, CuO ,NH4H2PO4	1	mixture-pellt-heat(1273-1338K,16H in flowing O2)-RT-heat(1273-1338K,12H in flowing O2)-cool to RT					PHOSHATE DERIVATIVES OF 123 CUPRATES OF THE FORMULA LnSr2Cu3O7(Ln=Gd,Dy,Ho)			Jawaharlal Nehru Centre for Advanced Scientlfic Research Jakkur Campus, Banglore 560 064, India	Solid State Commun.,98(1996)761	C.N.R. Rao,R. Gundakaram,R. Nagarajan	Gd, Dy, Ho, Sr, Cu, O	
6553	SSC0980761		(Ho,Ca)Sr2Cu2.8(PO4)0.2Oz	Ho0.8Ca0.2Sr2Cu2.8P0.2Oz+0.8	Ho	0.8	Ca	0.2	Sr	2	Cu	2.8	P	0.2											O	z+0.8			1996																											2					3.82		11.27																34			34																																																																																														R2O3, SrCO3, CaCO3, CuO ,NH4H2PO4	1	mixture-pellt-heat(1273-1338K,16H in flowing O2)-RT-heat(1273-1338K,12H in flowing O2)-cool to RT					PHOSHATE DERIVATIVES OF 123 CUPRATES OF THE FORMULA LnSr2Cu3O7(Ln=Gd,Dy,Ho)			Jawaharlal Nehru Centre for Advanced Scientlfic Research Jakkur Campus, Banglore 560 064, India	Solid State Commun.,98(1996)761	C.N.R. Rao,R. Gundakaram,R. Nagarajan	Gd, Dy, Ho, Sr, Cu, O	
6554	PHC2620135		YSr2(Cu,Re)3Oz	Y1Sr2Cu2.8Re0.2O6+z	Y	1	Sr	2	Cu	2.8	Re	0.2													O	6+z			1996																											2					3.81		11.525																																																																																									TP6554																								Y2O3, Pr2O3, SrCo3, ReO2, CuO	1	mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24 in O2)-fornace cool					Neutron diffraction and thermopower of Y1-xPrxSr2Cu2.8Re0.2O6+z (0 and 0.60 )			School of Chemistry, University of Birmingham,Birmingham B15 2TT, UK	Physica.C,262(1996)135-142	A. Das,C. Greaves,C.R. Taylor,I. Zelenay,R. Suryanarayanan		
6555	PHC2620135		(Y,Pr)Sr2(Cu,Re)3Oz	Y0.4Pr0.6Sr2Cu2.8Re0.2O6+z	Y	0.4	Pr	0.6	Sr	2	Cu	2.8	Re	0.2											O	6+z			1996																											2					3.836	11.563															25					25																																																																						TP6555																								Y2O3, Pr2O3, SrCo3, ReO2, CuO	1	mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24 in O2)-fornace cool					Neutron diffraction and thermopower of Y1-xPrxSr2Cu2.8Re0.2O6+z (0 and 0.60 )			School of Chemistry, University of Birmingham,Birmingham B15 2TT, UK	Physica.C,262(1996)135-142	A. Das,C. Greaves,C.R. Taylor,I. Zelenay,R. Suryanarayanan		
6556	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.5Ca1Ba2.5Cu6O14.146	La	2.5	Ca	1	Ba	2.5	Cu	6													O	z	14.146		1996																												336																			79						79																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6557	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.4Ca1.2Ba2.4Cu6O14.082	La	2.4	Ca	1.2	Ba	2.4	Cu	6													O	z	14.082		1996																												336																			79						79																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6558	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.375Ca1.25Ba2.375Cu6O14.062	La	2.375	Ca	1.25	Ba	2.375	Cu	6													O	z	14.062		1996																												336																			78						78																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6559	PHC2610284		(La,Ca,)3(Ba,Ca)3Cu6O14	La2.25Ca1.5Ba2.25Cu6O13.93	La	2.25	Ca	1.5	Ba	2.25	Cu	6													O	z	13.93		1996																												336																			74						74																																																																																																polymetric citrate precursor method					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6560	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2Ca2Ba2Cu3O13.712	La	2	Ca	2	Ba	2	Cu	3													O	z	13.712		1996																												336																			76						76																																																																																																polymetric citrate precursor method					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6561	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La3Ba3Cu6O14.294	La	3	Ba	3	Cu	6															O	z	14.294		1996																																																																																																																																																										Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6562	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.9Ca2Ba2.9Cu6O14.254	La	2.9	Ca	2	Ba	2.9	Cu	6													O	z	14.254		1996																																																																																																																																																										Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6563	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.85Ca0.3Ba2.85Cu6O14.252	La	2.85	Ca	0.3	Ba	2.85	Cu	6													O	z	14.252		1996																																															22						22																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6564	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.77Ca0.46Ba2.77Cu6O14.246	La	2.77	Ca	0.46	Ba	2.77	Cu	6													O	z	14.246		1996																																															42						42																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6565	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.7Ca0.6Ba2.7Cu6O14.186	La	2.7	Ca	0.6	Ba	2.7	Cu	6													O	z	14.186		1996																																															74						74																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6566	PHC2610284		(La,Ca)3(Ba,Ca)3Cu6O14	La2.57Ca0.86Ba2.57Cu6O14.2	La	2.57	Ca	0.86	Ba	2.57	Cu	6													O	z	14.2		1996																																															80						80																																																																																																					Superconductivity and hole concentration of La3-xCa2xBa3-xCu6Oy compounds			Department of Chemistry, Tamkang University, Tamsui,25137 taiwan	Physica.C,261(1996)284-288	C.M. Wang,H.-C.I. Kao,W.N. Huang,Y.D. Leu		
6567	PHC2620143		HoBa2Cu3O7	Ho1Ba2Cu3O6.87	Ho	1	Ba	2	Cu	3															O	z	6.87	1	1996																												Y123																				92.3					92.3																																																									2.72		554	specific heat																																		Ho2O3, BaCO3, CuO	1	mixture-heat(920C,24H in air)-pellt-heat(930C,48H)-cool to 650C(2-3C/min) -furnace cool					Electoron heat capacity and moments of phonon density of states of HoBa2Cu3O7-z			Institute of Inorganic Chemistry, Novosibirsk, 630090, Russian Federation	Physica.C,262(1996)143-148	E.B. Amitin,G.I. Frolova,P.P. Samoilov,V.E. Fedorov,V.N. Naumov		
6568	PHC2620143	data from ref.6	HoBa2Cu3O7	Ho1Ba2Cu3O6.96	Ho	1	Ba	2	Cu	3															O	z	6.96		1996																												Y123																				91.8					91.8																																																									2.92		551	specific heat																																									Electoron heat capacity and moments of phonon density of states of HoBa2Cu3O7-z			Institute of Inorganic Chemistry, Novosibirsk, 630090, Russian Federation	Physica.C,262(1996)143-148	E.B. Amitin,G.I. Frolova,P.P. Samoilov,V.E. Fedorov,V.N. Naumov		
6569	PHC2620143	data from Physica C 245(1995)36	YBa2Cu3O7	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O	z	6.92		1996																												Y123																				92.2					92.2																																																									2.26		572	specific heat																																									Electoron heat capacity and moments of phonon density of states of HoBa2Cu3O7-z			Institute of Inorganic Chemistry, Novosibirsk, 630090, Russian Federation	Physica.C,262(1996)143-148	E.B. Amitin,G.I. Frolova,P.P. Samoilov,V.E. Fedorov,V.N. Naumov		
6570	PHC2620143	data from Physica C 190(1991)70	YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	z	6.96		1996																												Y123																				92					92																																																									2.02		578	specific heat																																									Electoron heat capacity and moments of phonon density of states of HoBa2Cu3O7-z			Institute of Inorganic Chemistry, Novosibirsk, 630090, Russian Federation	Physica.C,262(1996)143-148	E.B. Amitin,G.I. Frolova,P.P. Samoilov,V.E. Fedorov,V.N. Naumov		
6571	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1996																												Hg1223				3.855		15.842													110						110																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6572	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.9Pb0.1Ba2Ca2Cu3O8+z	Hg	0.9	Pb	0.1	Ba	2	Ca	2	Cu	3											O	8+z			1996																												Hg1223				3.85		15.836													118						118																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6573	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.8Pb0.2Ba2Ca2Cu3O8+z	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	8+z			1996																												Hg1223				3.848		15.831													125						125																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6574	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.7Pb0.3Ba2Ca2Cu3O8+z	Hg	0.7	Pb	0.3	Ba	2	Ca	2	Cu	3											O	8+z			1996																												Hg1223				3.843		15.824													130						130																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6575	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.6Pb0.4Ba2Ca2Cu3O8+z	Hg	0.6	Pb	0.4	Ba	2	Ca	2	Cu	3											O	8+z			1996																												Hg1223				3.842		15.818													120						120																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6576	PHC2610189		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.5Pb0.5Ba2Ca2Cu3O8+z	Hg	0.5	Pb	0.5	Ba	2	Ca	2	Cu	3											O	8+z			1996																												Hg1223				3.84		15.822													103						103																																																																																																precursor(Ba2 Ca2 Cu3 O7)+HgO+PbO-pellet-heat(850C,10H)-(200C,2H)-Fc					Syntheses and neutron powder diffraction studies of the superconductor HgBa2Ca2Cu3O8+z by Pb substitution			National Laboratory of Solid State Microstructures and Center for advanced studies in Science and Technology of Microstructures.Nanjing University, Nanjing 210093, China	Physica.C,261(1996)189-195	C. Gou,D.F. Chen,D.W. Wang,H.M. Shao,S.S. Jiang,X.S. Wu,Z.H. Wu		
6577	PHC2610196	Jc difines by Imicro. V/cm, oriented sample	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.8Pb0.4Sr1.9Ca2Cu3Oz	Bi	1.8	Pb	0.4	Sr	1.9	Ca	2	Cu	3											O	z			1996																												Bi2223																				110					110																																		HIR6577																																																														Ag-sheethad tape-Cut(short tape)-press-SIN(837C,80H in reduced O2)three times					Anisotropy of Bi-2223/Ag tapes by electrical and magnetic characterzations			CISE SpA, PO, Box 12081, 1-20314 Milan, Italy	Physica.C,261(1996)196-200	A. Gandini,L. Martini,L. Rossi,S. Zannella,V. Ottoboni		
6578	PHC2620021		HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z		1	1996																												Hg1234				3.852	19.01																	123			123										83																																																																																					1	precunsor(Ba-Ca-Cu-O)+HgO-heat(800C,4H) in evaceated quartq tube-ANN(300C,30H in flowing O2)					Synthesis of HgBa2Ca3Cu4Oy under ambient pressure			Superconductivity reserch Laboratory,ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135, Japan	Physica.C,262(1996)21-26	A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi,T. Tatsuki		
6579	PHC2610097		Nd(Ba,Sr)2Cu3O7	Nd1Ba1.5Sr0.5Cu3O6.91	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.91		1996																											3	Y123				3.86	3.896	11.697													83						83																																																																																																					Structural analysis of superconducting NdBa1.5Sr0.5Cu3O7-z			"Angewandte Physik, Johannes Kepler Universita""t Linz A-4040 Linz, Austria"	Physica.C,261(1996)97-104	"B. Hellebrand,D. Ba""uerle,M. Guillaume,M. Vybornov,P. Fischer,P. Rogl,X.Z. Wang"		
6580	PHC2610097		Nd(Ba,Sr)2Cu3O7	Nd1Ba1.5Sr0.5Cu3O6.91	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.91		1996																											2	Y123				3.881		11.688													71						71																																																																																																					Structural analysis of superconducting NdBa1.5Sr0.5Cu3O7-z			"Angewandte Physik, Johannes Kepler Universita""t Linz A-4040 Linz, Austria"	Physica.C,261(1996)97-104	"B. Hellebrand,D. Ba""uerle,M. Guillaume,M. Vybornov,P. Fischer,P. Rogl,X.Z. Wang"		
6581	PHC2610071	R(77K)=5.61E+5 Ohm,cm		La2Ba2Cu2Ti2O11	La	2	Ba	2	Cu	2	Ti	2													O	11			1996																											2					3.937		15.75																	4.2																																																																									ohm.cm											1.11													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6582	PHC2610071	R(77)=1.71E+7 Ohm,cm		La2Ba1.7K0.03Cu2Ti2O10.69	La	2	Ba	1.7	K	0.03	Cu	2	Ti	2											O	11-z	10.69		1996																											2					3.94		15.77																	4.2																																																																									ohm.cm											11.9													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6583	PHC2610071	R(77)=1.24E+4 Ohm,cm		La2Ba1.85Cu2Ti2O10.7	La	2	Ba	1.85	Cu	2	Ti	2													O	11-z	10.7		1996																											2					3.942		15.79																	4.2																																																																									ohm.cm											1.03													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6584	PHC2610071	R(77)=2.53E+6 Ohm,cm		La2.3Ba1.7Cu2Ti2O11.15	La	2.3	Ba	1.7	Cu	2	Ti	2													O	11-z	11.15		1996																											2					3.934		15.745																	4.2																																																																									ohm.cm											5.06													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6585	PHC2610071	R(77)=6.2E+3 Ocm, cm		La2Ba2Cu2Ti1.85Zn0.15O10.86	La	2	Ba	2	Cu	2	Ti	1.85	Zn	0.15											O	11-z	10.86		1996																											2					3.937		15.756																	4.2																																																																									ohm.cm											0.71													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6586	PHC2610071	R(77)=5.3E+4 Ohm, cm		La2Ba2Cu2.15Ti1.85O10.85	La	2	Ba	2	Cu	2.15	Ti	1.85													O	11-z	10.85		1996																											2					3.936		15.739																	4.2																																																																									ohm.cm											0.48													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6587	PHC2610071	R(77)=1.3E+3 Ohm, cm		La2Ba2Cu2Ti1.7Co0.3O10.82	La	2	Ba	2	Cu	2	Ti	1.7	Co	0.3											O	11-z	10.82		1996																											2					3.932		15.71																	4.2																																																																									ohm.cm											0.32													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6588	PHC2610071	R(77)=7.43E+5 Ohm, cm		La2Ba2Cu2Ti1.7Al0.3O10.86	La	2	Ba	2	Cu	2	Ti	1.7	Al	0.3											O	11-z	10.86		1996																											2					3.929		15.724																	4.2																																																																									ohm.cm											3.01													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6589	PHC2610071	R(77)=22.9 Ohm, cm		La2Ba2Cu2Ti1.7Sc0.3O10.81	La	2	Ba	2	Cu	2	Ti	1.7	Sc	0.3											O	11-z	10.81		1996																											2					3.953		15.71																	4.2																																																																									ohm.cm											0.22													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6590	PHC2610071	R(77)>E+8 Ohm, cm		Nd2Ba2Cu2Ti2O11	Nd	2	Ba	2	Cu	2	Ti	2													O	11			1996																											2					3.904		15.68																	4.2																																																																									ohm.cm											62.7													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6591	PHC2610071	R(77)>E+8 Ohm,cm, R(300)=9.0E+4 Ohm, cm		Nd2Ba1.7K0.1Cu2Ti2O10.79	Nd	2	Ba	1.7	K	0.1	Cu	2	Ti	2											O	11-z	10.79		1996																											2					3.909		15.69																	4.2																																																																																																	1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6592	PHC2610071	R(77)>E+8 Ohm,cm, R(300)=4.1 E+4 Ohm,cm		Nd2Ba1.85Cu2Ti2O11-z	Nd	2	Ba	1.85	Cu	2	Ti	2													O	11-z			1996																											2					3.898		15.65																	4.2																																																																																																	1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6593	PHC2610071	R(300)=7.3+4 Ohm,cm		Nd2.3Ba1.7Cu2Ti2O11-z	Nd	2.3	Ba	1.7	Cu	2	Ti	2													O	11-z			1996																											2					3.909		15.66																	4.2																																																																									ohm.cm																								1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6594	PHC2610071	R(77)>E+8 Ohm,cm		Nd2Ba2Cu2Ti1.85Zn0.15O11-z	Nd	2	Ba	2	Cu	2	Ti	1.85	Zn	0.15											O	11-z			1996																											2					3.912		15.69																	4.2																																																																									ohm.cm				6.44							0.04													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6595	PHC2610071			Na2Ba2Cu2.15Ti1.85O10.83	Na	2	Ba	2	Cu	2.15	Ti	1.85													O	11-z	10.83		1996																											2					3.907		15.68																	4.2																																																																									ohm.cm				3.14							0.023													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6596	PHC2610071	R(77)=3.9E+5 Ohm, cm		Nd2Ba2Cu2Ti1.7Co0.3O10.85	Nd	2	Ba	2	Cu	2	Ti	1.7	Co	0.3											O	11-z	10.85		1996																											2					3.903		15.66																	4.2																																																																									ohm.cm											0.38													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6597	PHC2610071			Nd2Ba2Cu2Ti1.7Al0.3O10.85	Nd	2	Ba	2	Cu	2	Ti	1.7	Al	0.3											O	11-z	10.85		1996																											2					3.904		15.65																	4.2																																																																									ohm.cm				16.5							0.16													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6598	PHC2610071			Eu2Ba2Cu2Ti2O11	Eu	2	Ba	2	Cu	2	Ti	2													O	11			1996																											2					3.884		15.68																	4.2																																																																									ohm.cm											4.65													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6599	PHC2610071			Eu2Ba1.7K0.1Cu2Ti2O10.74	Eu	2	Ba	1.7	K	0.1	Cu	2	Ti	2											O	11-z	10.74		1996																											2					3.883		15.69																	4.2																																																																									ohm.cm											428.9													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6600	PHC2610071			Eu2Ba2Cu2Ti1.85Zn0.15O10.89	Eu	2	Ba	2	Cu	2	Ti	1.85	Zn	0.15											O	11-z	10.89		1996																											2					3.893		15.67																	4.2																																																																									ohm.cm				22.5							0.026													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6601	PHC2610071			Eu2Ba2Cu2.15Ti1.85O10.85	Eu	2	Ba	2	Cu	2.15	Ti	1.85													O	11-z	10.85		1996																											2					3.885		15.68																	4.2																																																																									m.ohm.cm				48							6.4													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6602	PHC2610071			Eu2Ba2Cu2Ti1.7Co0.3O10.88	Eu	2	Ba	2	Cu	2	Ti	1.7	Co	0.3											O	11-z	10.88		1996																											2					3.885		15.68																	4.2																																																																									m.ohm.cm											274													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6603	PHC2610071			Eu2Ba2Cu2Ti1.7Al0.3O10.89	Eu	2	Ba	2	Cu	2	Ti	1.7	Al	0.3											O	11-z	10.89		1996																											2					3.887		15.65																	4.2																																																																									m.ohm.cm				230							6.7													1	mixture-heat(900C,2H+1100C,24H)-heat(1100C,24H)-ANN(500C,in flowing O2)					Cationic substitutions and doping in the series of layered perovskites Ln2Ba2Cu2Ti2O11 (Ln=La,Nd,Eu,Tb)			Institut de Cie'ncia de Materials de Barcelona(CSIC),Campus UAB, 08193 Bellaterra, Barcelona, Spain	Physica.C,261(1996)71-80	"G. Kra""mer,M. Jansen,M.R. Palac'in,N. Casan-Pastor"		
6604	PHC2610097	single phase	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.5Sr0.5Cu3O6.91	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.91	1	1996																											2	Y123				3.881		11.688													71						71																																																																																														Nd2O3, BaCo3, SrCO3, CuO	1	mixture-CAL(930C,25H in air)-pellet-SIN(1000C,20H in flowing O2)-cool to RT(50C/H)					Structural analysis of superconducting NdBa1.5Sr0.5Cu3O7-z			"Angewandte Physik, Johannes Kepler Universita""t Linz A-4040 Linz, Austria"	Physica.C,261(1996)97-104	"B. Hellebrand,D. Ba""uerle,M. Guillaume,M. Vybornov,P. Fischer,P. Rogl,X.Z. Wang"		
6605	PHC2610097	ANN(940C,5H in Ar)-ANN(350C,10H in flowing O2),Ortho+Tetra	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.5Sr0.5Cu3O6.91	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.91	2	1996																												Y123				3.86	3.896	11.697													83						83																																																																																														Nd2O3, BaCo3, SrCO3, CuO	1	mixture-CAL(930C,25H in air)-pellet-SIN(1000C,20H in flowing O2)-cool to RT(50C/H)					Structural analysis of superconducting NdBa1.5Sr0.5Cu3O7-z			"Angewandte Physik, Johannes Kepler Universita""t Linz A-4040 Linz, Austria"	Physica.C,261(1996)97-104	"B. Hellebrand,D. Ba""uerle,M. Guillaume,M. Vybornov,P. Fischer,P. Rogl,X.Z. Wang"		
6606	PHC2460351	as-prepared,with out oxidiqer	(Hg,Re)Sr2Ca2Cu3Oz	Hg0.75Re0.25Sr2Ca2Cu3Oz	Hg	0.75	Re	0.25	Sr	2	Ca	2	Cu	3											O	z			1995																												Hg1223																						100			100																																																																																																precursor(Ca-Sr-Cu-Re-O)+HgO-press to 6GPa-react(1273K,30min)-pressure release and quench					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
6607	PHC2460351	post-anneal(783K in evacuatecl quartq ampoule)	(Hg,Re)Sr2Ca2Cu3Oz	Hg0.75Re0.25Sr2Ca2Cu3Oz	Hg	0.75	Re	0.25	Sr	2	Ca	2	Cu	3											O	z			1995																											2	Hg1223				3.83		15.227																120			120																																																																																																precursor(Ca-Sr-Cu-Re-O)+HgO-press to 6GPa-react(1273K,30min)-pressure release and quench					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
6608	PHC2460351		HgSr2Ca(Cu,Re)2 Oz	Hg1Sr2Ca1Cu1.8Re0.2Oz	Hg	1	Sr	2	Ca	1	Cu	1.8	Re	0.2											O	z			1995																											2	Hg1212				3.816		12.066																90			90																																																																																																post-anneal(763K)					High-pressure synthesis and superconductivity of a Ba free mercury-based superconductor(Hg0.75Re0.25)Sr2Ca2Cu3Oy	199505		Institute for Chemical Research,kyoto University,Uji.Kyoto-fu 611,Japan	Physica C.,246(1995)351-356	J.Shimoyama,K.Kishio,K.Yamaura,M.Takano,S.Hahakura,Z.Hiroi		
6609	PHC2610117	RES=80micro Ohm.cm at 100K	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.895Fe0.105O7-z	Y	1	Ba	2	Cu	2.895	Fe	0.105													O	7-z		3	1996																												Y123																				81.8				1.5	81.8																																							12.7	0.7																																																							5	self-flux method-ANN(460C,a for days,in flowing O2)siqe=1*0.2*0.02mm3					Fluctuation magnetoconductivity in Fe doped YBa2Cu3O7-z Sign change for B and I parallel to the planes			Department of Solid State Physics, The Royal Institute of Technology, S-100 44 Stockholm, Sweden	Physica.C,261(1996)117-124	"J. Axna""s,O"". Rapp,W. Holm,Yu. Eltsev"		
6610	PHC2610117	RES=180 micro Ohm.cm at rook	YBa2(Cu,Fe)3 O7	Y1Ba2Cu2.805Fe0.195O7-z	Y	1	Ba	2	Cu	2.805	Fe	0.195													O	7-z		3	1996																												Y123																				60				0.9	60																																							15	2.5																																																							5	self-flux method-ANN(460C,a for days,in flowing O2)siqe=1*0.2*0.02mm3					Fluctuation magnetoconductivity in Fe doped YBa2Cu3O7-z Sign change for B and I parallel to the planes			Department of Solid State Physics, The Royal Institute of Technology, S-100 44 Stockholm, Sweden	Physica.C,261(1996)117-124	"J. Axna""s,O"". Rapp,W. Holm,Yu. Eltsev"		
6611	PR0476054		(Y,Ca)Ba2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-z	6.96		1993																												Y123																				89.4					89.4																																																																																																mixture-SIN(950C,24H~960C,60H in flowing O2)sevenal times-ANN(400C,3days in flowing O2-slow cool to RT)					EFFECTS OF SUBSTITUTING CALCIUM FOR YTTRIUM ON THE PROPERTIESOF YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6054	A.KNIZHNIK,B.FISHER,C.G.KUPER,G.M.REISNER,J.GENOSSAR,L.PATLAGAN	Y,BA,CU,O,CA	
6612	PR0476054		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu3O6.91	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.91		1993																												Y123																				84.2					84.2																																																																																																mixture-SIN(950C,24H~960C,60H in flowing O2)sevenal times-ANN(400C,3days in flowing O2-slow cool to RT)					EFFECTS OF SUBSTITUTING CALCIUM FOR YTTRIUM ON THE PROPERTIESOF YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6054	A.KNIZHNIK,B.FISHER,C.G.KUPER,G.M.REISNER,J.GENOSSAR,L.PATLAGAN	Y,BA,CU,O,CA	
6613	PR0476054		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.86	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.86		1993																												Y123																				79					79																																																																																																mixture-SIN(950C,24H~960C,60H in flowing O2)sevenal times-ANN(400C,3days in flowing O2-slow cool to RT)					EFFECTS OF SUBSTITUTING CALCIUM FOR YTTRIUM ON THE PROPERTIESOF YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6054	A.KNIZHNIK,B.FISHER,C.G.KUPER,G.M.REISNER,J.GENOSSAR,L.PATLAGAN	Y,BA,CU,O,CA	
6614	PR0476054		(Y,Ca)Ba2Cu3O7	Y0.7Ca0.3Ba2Cu3O6.78	Y	0.7	Ca	0.3	Ba	2	Cu	3													O	7-z	6.78		1993																												Y123																			68.4	78					78																																																																																																mixture-SIN(950C,24H~960C,60H in flowing O2)sevenal times-ANN(400C,3days in flowing O2-slow cool to RT)					EFFECTS OF SUBSTITUTING CALCIUM FOR YTTRIUM ON THE PROPERTIESOF YBA2CU3O7-Z	199303			PHYS.REV.B,47(1993)6054	A.KNIZHNIK,B.FISHER,C.G.KUPER,G.M.REISNER,J.GENOSSAR,L.PATLAGAN	Y,BA,CU,O,CA	
6615	PHC2610125	hydrostatic, up to 1 Gpa	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.63	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.63		1996																												Y123																						16			16			K/GPa	2.2																																																																																											1	mixture-heat (900-950C in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(IC/min)-ANN(300-600C,20H in N2)					High effect of pressure on the critical temperature in GdBa1.5Sr0.5Cu3Ox			Instiute of Physics, polish Academy of Sciences, Al. Lotniko'w 32/46 Warszawa, Poland	Physica.c,261(1996)125-130	I. Fita,M. Baran		
6616	PHC2610125	hydrostatic, up to 1 Gpa	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.73	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.73		1996																												Y123																						50			50			K/GPa	7																																																																																											1	mixture-heat (900-950C in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(IC/min)-ANN(300-600C,20H in N2)					High effect of pressure on the critical temperature in GdBa1.5Sr0.5Cu3Ox			Instiute of Physics, polish Academy of Sciences, Al. Lotniko'w 32/46 Warszawa, Poland	Physica.c,261(1996)125-130	I. Fita,M. Baran		
6617	PHC2610125	hydrostatic, up to 1Gpa	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.93	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	z	6.93		1996																												Y123																						89			89			K/GPa	13.7																																																																																											1	mixture-heat (900-950C in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(IC/min)-ANN(300-600C,20H in N2)					High effect of pressure on the critical temperature in GdBa1.5Sr0.5Cu3Ox			Instiute of Physics, polish Academy of Sciences, Al. Lotniko'w 32/46 Warszawa, Poland	Physica.c,261(1996)125-130	I. Fita,M. Baran		
6618	PHC1830154		(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O6.83	Y	1	Ba	2	Cu	3															O	7-z	6.83	1	1991																											3	Y123				3.822	3.888	11.667													91	92	93	92			92																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6619	PHC1830154		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.85	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z	6.85	1	1991																											3	Y123				3.814	3.884	11.65													79	85.5	90				85.5																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6620	PHC1830154		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.82	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.82	1	1991																											3	Y123				3.82	3.884	11.648													77	82	86	84			82																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6621	PHC1830154		()Y,Prba2Cu3O7	Y0.85Pr0.15Ba2Cu3O6.84	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z	6.84	1	1991																											3	Y123				3.817	3.887	11.662													68	75	82				75																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6622	PHC1830154		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.81	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.81	1	1991																											3	Y123				3.826	3.889	11.669													62	68	73	70			68																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6623	PHC1830154		(Y,Ca)Ba2Cu3O7	Y0.95Ca0.05Ba2Cu3O6.79	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	7-z	6.79	1	1991																											3	Y123				3.801	3.883	11.646													80	88	91				88																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6624	PHC1830154		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu3O6.67	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.67	1	1991																											3	Y123				3.841	3.89	11.689													79	82	90				82																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6625	PHC1830154		(Y,Ca)Ba2Cu3O7	Y0.85Ca0.15Ba2Cu3O6.65	Y	0.85	Ca	0.15	Ba	2	Cu	3													O	7-z	6.65	1	1991																											3	Y123				3.819	3.887	11.655													80	83	87				83																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6626	PHC1830154		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.64	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.64	1	1991																											3	Y123				3.822	3.872	11.617													78	81	85				81																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6627	PHC1830154		(Y,Pr,Ca)Ba2Cu3O7	Y0.8Pr0.05Ca0.15Ba2Cu3O6.83	Y	0.8	Pr	0.05	Ca	0.15	Ba	2	Cu	3											O	7-z	6.83	1	1991																											3	Y123				3.819	3.881	11.642													85	87	89				87																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6628	PHC1830154		(Y,Pr,Ca)Ba2Cu3O7	Y0.8Pr0.15Ca0.05Ba2Cu3O6.82	Y	0.8	Pr	0.15	Ca	0.05	Ba	2	Cu	3											O	7-z	6.82	1	1991																											3	Y123				3.805	3.873	11.624													75	80	86				80																																																																																														Y2O3, BaCO3, CuO,Pr6O11, CaO	1	mixture-CAL(950C,24H in air in Pt-crucible)-SIN(950C,24H in aie)-ANN(450C,12H in flowing O2)-slow cool to RT					Influence of hole filling and pair breaking by Pr and hole doping by Ca on superconductivity and flux pinning of YBa2Cu3O6.83			Department of Physics, Marathawada University, Aurangabad-431 004, India	Physica.C,183(1991)154-162	D.G. Kuberkar,G.K. Bichile,R.G. Kulkarni,Smida Deshmukh		
6629	PHC1910158		(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-z	6.96		1992																												Y123																			92	92.2	92.7				92.2																																																																																		0.5												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6630	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.96	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z	6.96		1992																												Y123																			91.4	91.5	92.1				91.5																																																																																		0.7												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6631	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.97	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.97		1992																												Y123																			87.7	88.1	88.6				88.1																																																																																		1.08												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6632	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.85Pr0.15Ba2Cu3O6.97	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z	6.97		1992																												Y123																			81.3	81.8	82.7				81.8																																																																																		1.04												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6633	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.96	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.96		1992																												Y123																			74	74.7	76.1				74.7																																																																																		1.17												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6634	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.97	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.97		1992																												Y123																			58.3	59.3	60.9				59.3																																																																																		1.44												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6635	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.98	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.98		1992																												Y123																			44.1	45.4	47.6				45.4																																																																																		1.59												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6636	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O6.95	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-z	6.95		1992																												Y123																			25.7	28.2	32				28.2																																																																																		1.99												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6637	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.47Pr0.53Ba2Cu3O6.96	Y	0.47	Pr	0.53	Ba	2	Cu	3													O	7-z	6.96		1992																												Y123																			9.7	13.5	17.7				13.5																																																																																		2.01												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6638	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.44Pr0.56Ba2Cu3O6.93	Y	0.44	Pr	0.56	Ba	2	Cu	3													O	7-z	6.93		1992																												Y123																					2.1				2.1																																																																																		2.2												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6639	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.42Pr0.58Ba2Cu3O6.94	Y	0.42	Pr	0.58	Ba	2	Cu	3													O	7-z	6.94		1992																												Y123																							4.2																																																																																				2.22												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6640	PHC1910158		(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O6.95	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7-z	6.95		1992																												Y123																							4.2																																																																																				3.89												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6641	PHC1910158		(Y,Pr)Ba2Cu3O7	Pr1Ba2Cu3O6.95	Pr	1	Ba	2	Cu	3															O	7-z	6.95		1992																												Y123																							4.2																																																																																				14.56												Y2O3, Pr6O11, BaCO3, CuO		pellet-ANN(955-970C, 2days in O2)-cool to 450C(1C/min)-ANN(450C,18H)-slow cool to RT					SUPERCONDUCTING CRITICAL TEMPERATURE AND ELECTRICAL RESISTIVITY OF THE SYSTEM Y1-XPRXBA2CU3O6.95(0<-X<-1)	199202			PHYSICA C,191(1992)158	J.J.NEUMEIER,M.B.MAPLE	Y,PR,BA,CU,O	
6642	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	z	6.98	1	1996																												Y123																				92.2					92.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6643	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.9Pr0.1Ba2Cu3O6.98	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				85.9					85.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6644	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.85Pr0.15Ba2Cu3O6.98	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				79.2					79.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6645	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O6.98	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				72.6					72.6																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6646	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.7Pr0.3Ba2Cu3O6.98	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				57.4					57.4																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6647	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.98	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				42.8					42.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6648	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.55Pr0.45Ba2Cu3O6.98	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				33.6					33.6																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6649	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.98	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				21.9					21.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6650	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.45Pr0.55Ba2Cu3O6.98	Y	0.45	Pr	0.55	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				10.1					10.1																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6651	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.4Pr0.6Ba2Cu3O6.98	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6652	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	1	1996																												Y123																				73.2					73.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6653	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.9Pr0.1Ba2Cu3O6.8	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																				65.6					65.6																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6654	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.85Pr0.15Ba2Cu3O6.8	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																				59					59																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6655	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O6.8	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																				56.1					56.1																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6656	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.8	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																				33.9					33.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6657	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.55Pr0.45Ba2Cu3O6.8	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																				23.5					23.5																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6658	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.8	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	z	6.8	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6659	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	z	6.65	1	1996																												Y123																				58.9					58.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6660	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.9Pr0.1Ba2Cu3O6.65	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				56.1					56.1																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6661	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.85Pr0.15Ba2Cu3O6.65	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				52.9					52.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6662	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O6.65	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				51.7					51.7																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6663	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.7Pr0.3Ba2Cu3O6.65	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				46					46																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6664	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.65	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				38					38																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6665	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.55Pr0.45Ba2Cu3O6.65	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				30.7					30.7																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6666	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.65	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				18.7					18.7																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6667	PHC2630336		(Y,Pr)ba2Cu3Oz	Y0.45Pr0.55Ba2Cu3O6.65	Y	0.45	Pr	0.55	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6668	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	z	6.5	1	1996																												Y123																				41.2					41.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6669	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.9Pr0.1Ba2Cu3O6.5	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																				38.7					38.7																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6670	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.85Pr0.15Ba2Cu3O6.5	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																				35.8					35.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6671	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O6.5	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																				33.9					33.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6672	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.7Pr0.3Ba2Cu3O6.5	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																				27.2					27.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6673	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.5	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																				14.9					14.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6674	PHC2630336		(Y,Pr)Ba2Cu3Oz	Y0.55Pr0.45Ba2Cu3O6.5	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	z	6.5	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6675	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd1Ba2Cu3O6.85	Nd	1	Ba	2	Cu	3															O	z	6.85	1	1996																												Y123																				67.4					67.4																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6676	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.95Pr0.05Ba2Cu3O6.85	Nd	0.95	Pr	0.05	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																				57.2					57.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6677	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.9Pr0.1Ba2Cu3O6.85	Nd	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																				48.3					48.3																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6678	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.85Pr0.15Ba2Cu3O6.85	Nd	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																				41.3					41.3																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6679	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O6.85	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																				30.2					30.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6680	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.75Pr0.25Ba2Cu3O6.85	Nd	0.75	Pr	0.25	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																				9.2					9.2																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6681	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.7Pr0.3Ba2Cu3O6.85	Nd	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.85	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6682	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd1Ba2Cu3O6.75	Nd	1	Ba	2	Cu	3															O	z	6.75	1	1996																												Y123																				52.8					52.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6683	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.95Pr0.05Ba2Cu3O6.75	Nd	0.95	Pr	0.05	Ba	2	Cu	3													O	z	6.75	1	1996																												Y123																				45.8					45.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6684	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.9Pr0.1Ba2Cu3O6.75	Nd	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.75	1	1996																												Y123																				35.9					35.9																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6685	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.85Pr0.15Ba2Cu3O6.75	Nd	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.75	1	1996																												Y123																				21.6					21.6																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6686	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O6.75	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.75	1	1996																												Y123																				9.8					9.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6687	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.75Pr0.25Ba2Cu3O6.75	Nd	0.75	Pr	0.25	Ba	2	Cu	3													O	z	6.75	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6688	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd1Ba2Cu3O6.65	Nd	1	Ba	2	Cu	3															O	z	6.65	1	1996																												Y123																				34.3					34.3																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6689	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.95Pr0.05Ba2Cu3O6.65	Nd	0.95	Pr	0.05	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				26.7					26.7																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6690	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.9Pr0.1Ba2Cu3O6.65	Nd	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																				16.8					16.8																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6691	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.85Pr0.15Ba2Cu3O6.65	Nd	0.85	Pr	0.15	Ba	2	Cu	3													O	z	6.65	1	1996																												Y123																							4.2																																																																																																Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6692	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd1Ba2Cu3O6.6	Nd	1	Ba	2	Cu	3															O	z	6.6	1	1996																												Y123																				14					14																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6693	PHC2630336		(Nd,Pr)Ba2Cu3O7	Nd0.95Pr0.05Ba2Cu3O6.6	Nd	0.95	Pr	0.05	Ba	2	Cu	3													O	z	6.6	1	1996																												Y123																				4.1					4.1																																																																																														Y2O3,Nd2O3,Pr6O11,BaCO3,CuO	1	mixture-CAL(950C,24H in air)-pellet-SIN(930C(Nd),950C(Y),12H in flowing O2)-ANN(350C,12H)-verious quenching Temp. for different Oxygen content					Oxygen concentration dependence of superconductivity in Pr-substituted Ln1-xPrxBa2Cu3O7-y (Ln= Y, Nd, Gd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Minamijosanjima, Tokushima 770, Japan	Physica.C,263(1996)336-339	Kiyoshi Mizuno,Kuniyuki Koyama,Takahito Saito,Takashi Tange,Yasuyuki Kitamura		
6694	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.6Ce0.4Cu2Oz	Ru	1	Sr	2	Gd	1.6	Ce	0.4	Cu	2											O	z		2	1996																												Ru1212	I4/mmm																						10																																																																																																RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6695	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.5Ce0.5Cu2Oz	Ru	1	Sr	2	Gd	1.5	Ce	0.5	Cu	2											O	z		2	1996																												Ru1212	I4/mmm																		11	14	28				14																																																																																														RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6696	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.4Ce0.6Cu2Oz	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	z		1	1996																												Ru1212	I4/mmm			3.847		28.649													16	25	34				25																																																																																														RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6697	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.3Ce0.7Cu2Oz	Ru	1	Sr	2	Gd	1.3	Ce	0.7	Cu	2											O	z		1	1996																												Ru1212	I4/mmm																		14	22	30				22																																																																																														RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6698	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.2Ce0.8Cu2Oz	Ru	1	Sr	2	Gd	1.2	Ce	0.8	Cu	2											O	z		1	1996																												Ru1212	I4/mmm																						10																																																																																																RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6699	PHC2590168		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.1Ce0.9Cu2Oz	Ru	1	Sr	2	Gd	1.1	Ce	0.9	Cu	2											O	z		2	1996																												Ru1212	I4/mmm																						10																																																																																																RuO2,Sr(NO3)2,Gd2O3,CeO2,CuO		mixture-CAL(1000C,48H in air)-pellet-SIN(1100C,24H in flowing O2)-FC to RT					Synthesis and characterization of a new layered superconducting cuprate: RuSr2(Gd,Ce)2Cu2Oz			Department of Applied Chemistry,University of Science and Technology of China, Hefei 230026, China	Physica C,259(1996)168-172	Chen Zuyao,Qian Yitai,Tang Kaibin,Yang Li,Zhang Yuheng,Zhao Yadum		
6700	PHC2590036		Hg2Ba2(Y,Ca)Cu2O8	Hg2Ba2Y1Cu2O8-z	Hg	2	Ba	2	Y	1	Cu	2													O	8-z			1996																												Hg2212																						21			21																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6701	PHC2590036		Hg2Ba2(Y,Ca)Cu2O8	Hg2Ba2Y0.7Ca0.3Cu2O8-z	Hg	2	Ba	2	Y	0.7	Ca	0.3	Cu	2											O	8-z			1996																												Hg2212																						58			58																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6702	PHC2590036	small transition at 75K	Hg2Ba2(Y,Ca)Cu2O8	Hg2Ba2Y0.4Ca0.6Cu2O8-z	Hg	2	Ba	2	Y	0.4	Ca	0.6	Cu	2											O	8-z			1996																												Hg2212																						45			45																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6703	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y1Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	1	Cu	2											O	8-z			1996																											2	Hg2212				3.866		28.9																	4.2																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6704	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.7Ca0.3Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	8-z			1996																											2	Hg2212				3.861		28.92													50	60	70	68			60																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6705	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.4Ca0.6Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	8-z			1996																											2	Hg2212				3.856		28.99																84			84																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6706	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Ca1Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Ca	1	Cu	2											O	8-z			1996																											2	Hg2212				3.847		29.27																	4.9																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
6707	PHC2580384	Cu-vacancy	(Cu,C)Ba2Ca3Cu4Oz	Cu0.8C0.2Ba2Ca3Cu4Oz	Cu	0.8	C	0.2	Ba	2	Ca	3	Cu	4											O	z		1	1996																											2	Cu1234						17.93														115.5				2.3	115.5																																																																																											RH6707					high pressure synthesis technique					Hall effect of superconducting copper oxide, Cu-1234			Department of Applied Electronics.Science University of Tokyo 2641 Yamazaki Noda,Chiba 278, Japan	Physica.C.258,(1996)348-388	A. Iyo,H. Ihara,H. Tokiwa,M. Ogino,T. Watanabe	Cu,C,Ba,Ca,Cu,O	
6708	PHC2580384	Cu-vacancy	(Cu,C)Ba2Ca3Cu4Oz	Cu0.9C0.1Ba2Ca3Cu4Oz	Cu	0.9	C	0.1	Ba	2	Ca	3	Cu	4											O	z			1996																											2	Cu1234																				117.2				1.6	117.2																																																																																											RH6708					high pressure synthesis technique					Hall effect of superconducting copper oxide, Cu-1234			Department of Applied Electronics.Science University of Tokyo 2641 Yamazaki Noda,Chiba 278, Japan	Physica.C.258,(1996)348-388	A. Iyo,H. Ihara,H. Tokiwa,M. Ogino,T. Watanabe	Cu,C,Ba,Ca,Cu,O	
6709	PHC2580384	Cu-vacancy	(Cu,C)Ba2Ca3Cu4Oz	Cu5Ba2Ca3Oz	Cu	5	Ba	2	Ca	3															O	z			1996																											2	Cu1234						18														118				1.6	118																																																																																											RH6709					high pressure synthesis technique					Hall effect of superconducting copper oxide, Cu-1234			Department of Applied Electronics.Science University of Tokyo 2641 Yamazaki Noda,Chiba 278, Japan	Physica.C.258,(1996)348-388	A. Iyo,H. Ihara,H. Tokiwa,M. Ogino,T. Watanabe	Cu,C,Ba,Ca,Cu,O	
6710	PHC2580341	EPMA analysis(Tl:Ba:Cu=1.41:4.17:4.59)	Tl2Ba5Cu4Oz	Tl2Ba5Cu4Oz	Tl	2	Ba	5	Cu	4															O	z		3	1996																											2		I4/mmm			5.502		27.257	5															92			92													8																																																																																	Tl2O3,BaO2,CuO	5	heat(950C,10H)-cool to 900C (2C/H)-FC to RV					A new high-Tc cuprate superconductor Tl2Ba5Cu4Ox: growth, structure and superconductivity			Institute for Solid State Physics,University of Tokyo Roppongi,Minato-ku, Tokyo 106, Japan	Physica.C.258,(1996)341-348	Eriko Ohshima,Humihiko Takei,Kengi Hiraga,Masashi Hasegawa,Yoshitaka Matsushita,masae Kikuchi	Tl,Ba,Cu,O	
6711	PHC2580315	Ag-grown	(La,Ba)2CuO4	La1.94Ba0.06Cu1O4-z	La	1.94	Ba	0.06	Cu	1															O	4-z		3	1996																											2	T				3.806		13.241	7												15	15.5	18			3	15.5																																																																																														La2CuO4, BaCuO4	1	see J.cryst.Growth 96(1989)711					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6712	PHC2580315	as-grown	(La,Ba)2CuO4	La1.92Ba0.08Cu1O4-z	La	1.92	Ba	0.08	Cu	1															O	4-z		3	1996																											2	T				3.804		13.258	7												26.5	27	28			1.5	27																																																																																														La2CuO4, BaCuO4	1	see J.cryst.Growth 96(1989)711					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6713	PHC2580315	as-grown	(La,Ba)2CuO4	La1.91Ba0.09Cu1O4-z	La	1.91	Ba	0.09	Cu	1															O	4-z		3	1996																											2	T				3.797		13.272	7												31	31.5	32.5			1.5	31.5																																																																																														La2CuO4, BaCuO4	1	see J.cryst.Growth 96(1989)711					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6714	PHC2580315		(La,Ba)2CuO4	La1.94Ba0.06Cu1O4-z	La	1.94	Ba	0.06	Cu	1															O	4-z		3	1996																																3.799		13.218	7												15	16.5	18.5			3.5	16.5																																																																																															1	ANN(650C,24H in Ar)-cool to RT(1C/min)					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6715	PHC2580315		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4-z	La	1.92	Ba	0.08	Cu	1															O	4-z		3	1996																																3.795		13.232	7												27	28	29			2	28																																																																																															1	ANN(650C,24H in Ar)-cool to RT(1C/min)					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6716	PHC2580315		(La,Ba)2CuO4	La1.91Ba0.09Cu1O4-z	La	1.91	Ba	0.09	Cu	1															O	4-z		3	1996																																3.79		13.25	7												31	32.5	34			3	32.5																																																																																															1	ANN(650C,24H in Ar)-cool to RT(1C/min)					Anisotropic electric resistivity of superconducting La2-xBaxCuO4-z single crystals			Institute of Inorganic Synthesis, Faculty of Engineering, Yamanashi Uniersity, Miyamae 7,Kofu,Yamanashi 400, Japan	Physica.C.258,(1996)315-320	Hideyoshi Tanabe,Hironao Kojima,Isao Tanaka,M.K.R. Khan	La,Ba,Cu,O	
6717	PHC2580227		Ca2Sr2Cu3GaO9	Ca2Sr2Cu3Ga1O9	Ca	2	Sr	2	Cu	3	Ga	1													O	9		2	1996																											3		Imcm			29.36	5.462	5.404	4															73			73																																																																																															1						Crystal structure of the superconductor Ca2Sr2Cu3GaO9 synthesized at high pressure			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C.258,(1996)227-235	A.W. Hewat,E. Takayama-Muromachi,F. Izumi,N.R. Khasanova	Ca,Sr,Cu,Ga,O	
6718	PHC2580279	Fig(Hall effect),1:1/a, 2:1/b sampule is perfect single crystal	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1996																											3	Y124																				72					72																																																																																											RH6718					see NAT336(1988)660					Hall effect measurements on YBa2Cu4O8 single crystals			"Laboratorium f""ur Festko""rperphysik, ETH-Zu""rich, zu""rich, Swizerland"	Physica.C.258,(1996)279-283	"H. Schwer,J. Karpinski,J. Lo""hle,P. Wachter"	Y,Ba,Cu,O	
6719	PHC2590115	ANN(600C)	(Pb,Cu)Sr2(Y,Ca)Cu2O7	Pb0.5Cu0.5Sr2Y0.5Ca0.5Cu2O7-z	Pb	0.5	Cu	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-z		1	1996																												Pb1212																							4.2																																																																																																PbO,CuO,SrCO3,Y2O3,CuCO3							Influence of annealing on the superconductivity in(Pb,Cu)Sr2(Y,Ca)Cu2O7-z ceramics			Department of Electrical Engineering, Nagaoka University of Technology, 1603-1, Kamitomioka, Nagaoka, Niigata, 940-21, Japan	Physica C,259(1996)115-120	Ben Huybrechts,Makoto Nakao,Masasuke Takata,Satoshi Ohara,Yuichi Watanabe		
6720	PHC2590115	ANN(700C)	(Pb,Cu)Sr2(Y,Ca)Cu2O7	Pb0.5Cu0.5Sr2Y0.5Ca0.5Cu2O7-z	Pb	0.5	Cu	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-z		1	1996																												Pb1212																			14	20	31				20																																																																																														PbO,CuO,SrCO3,Y2O3,CuCO3							Influence of annealing on the superconductivity in(Pb,Cu)Sr2(Y,Ca)Cu2O7-z ceramics			Department of Electrical Engineering, Nagaoka University of Technology, 1603-1, Kamitomioka, Nagaoka, Niigata, 940-21, Japan	Physica C,259(1996)115-120	Ben Huybrechts,Makoto Nakao,Masasuke Takata,Satoshi Ohara,Yuichi Watanabe		
6721	PHC2590115	ANN(800C)	(Pb,Cu)Sr2(Y,Ca)Cu2O7	Pb0.5Cu0.5Sr2Y0.5Ca0.5Cu2O7-z	Pb	0.5	Cu	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-z		1	1996																												Pb1212																			25	35	47				35																																																																																														PbO,CuO,SrCO3,Y2O3,CuCO3							Influence of annealing on the superconductivity in(Pb,Cu)Sr2(Y,Ca)Cu2O7-z ceramics			Department of Electrical Engineering, Nagaoka University of Technology, 1603-1, Kamitomioka, Nagaoka, Niigata, 940-21, Japan	Physica C,259(1996)115-120	Ben Huybrechts,Makoto Nakao,Masasuke Takata,Satoshi Ohara,Yuichi Watanabe		
6722	PHC2590115	ANN(900C)	(Pb,Cu)Sr2(Y,Ca)Cu2O7	Pb0.5Cu0.5Sr2Y0.5Ca0.5Cu2O7-z	Pb	0.5	Cu	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-z		1	1996																												Pb1212																			30	38	48				38																																																																																														PbO,CuO,SrCO3,Y2O3,CuCO3							Influence of annealing on the superconductivity in(Pb,Cu)Sr2(Y,Ca)Cu2O7-z ceramics			Department of Electrical Engineering, Nagaoka University of Technology, 1603-1, Kamitomioka, Nagaoka, Niigata, 940-21, Japan	Physica C,259(1996)115-120	Ben Huybrechts,Makoto Nakao,Masasuke Takata,Satoshi Ohara,Yuichi Watanabe		
6723	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y1Sr2Cu2.85Re0.15O6.95	Y	1	Sr	2	Cu	2.85	Re	0.15													O	7	6.95		1995																											2	Y123				3.803		9.081														43.1					43.1																																																																			15.6																											Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6724	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y0.8Pr0.2Sr2Cu2.85Re0.15O7	Y	0.8	Pr	0.2	Sr	2	Cu	2.85	Re	0.15											O	7			1995																											2	Y123				3.804		9.068														39.1					39.1																																																																			22.6																											Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6725	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y0.6Pr0.4Cu2.85Re0.15O7	Y	0.6	Pr	0.4	Cu	2.85	Re	0.15													O	7			1995																											2	Y123				3.814		9.042														33.9					33.9																																																																			28.9																											Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6726	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y0.5Pr0.5Sr2Cu2.85Re0.15O7	Y	0.5	Pr	0.5	Sr	2	Cu	2.85	Re	0.15											O	7			1995																											2	Y123																				26.2					26.2																																																																			30.9																											Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6727	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y0.4Pr0.6Sr2Cu2.85Re0.15O6.8	Y	0.4	Pr	0.6	Sr	2	Cu	2.85	Re	0.15											O	7	6.8		1995																											2	Y123				3.829		9.002														20.2					20.2																																																																			36																											Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6728	JSC1180215		(Y,Pr)Sr2(Cu,Re)3O7	Y0.3Pr0.7Sr2Cu2.85Re0.15O7	Y	0.3	Pr	0.7	Sr	2	Cu	2.85	Re	0.15											O	7			1995																											2	Y123				3.834		9														15.8					15.8																																																																																														Y2O3,Pr2O3,SrCO3,ReO2,CuO		mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-ANN(1000C,24H in O2)-FC to RT					Evidence for Retarded Pr f Hybridization and Tc Suppression in Y1-xPrxSr2Cu2.85Re0.15O7			Laboratoire de Physique des Solides de Bellevue, Centre National de la Recherche Scientifique,92195 Meudon, france	J. Solid State Chem.118(1995)215-218	A. Das,I. Zelenay,L.F. Castro,R. Suryanarayanan		
6729	PRL0740598	Ramda(b)=1000 ppenet=Randa(a)	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95		1995																												Y123																				93.5				0.2	93.5																																										by for infrared(FIR)		1600																																																				by flux growth technique see Physica C 195(1992)51 detwinned under uriaxial stress					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
6730	PRL0740598	Ramda(b)=1200A ppenet=Ramda(a)	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1995																												Y123																			92						92																																										by for infrared(FIR)		1600																																																				Phys.Rev.B,42(1990)6217					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
6731	PRL0740598	Ramda(b)=800A ppenet=Ramda(a)	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1995																												Y123																				80				0.5	80																																										by for infrared(FIR) 		2000																																																				grown under high oxygen pressure					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
6732	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	z	6.94	3	1993																												Y123																				89.5					89.5			K/GPa	-0.85																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6733	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	z	6.93	3	1993																												Y123																				89.7					89.7			K/GPa	-0.64																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6734	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	z	6.91	3	1993																												Y123																				90.1					90.1			K/GPa	-0.27																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6735	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.81	Y	1	Ba	2	Cu	3															O	z	6.81	3	1993																												Y123																				87.3					87.3			K/GPa	1.4																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6736	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7	3	1993																												Y123																				71.2					71.2			K/GPa	1.4																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6737	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.61	Y	1	Ba	2	Cu	3															O	z	6.61	3	1993																												Y123																				58.7					58.7			K/GPa	3.5																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6738	PHC2050139	dtc/dp for C-axial pressure,twinmed sample	YBa2Cu3Oz	Y1Ba2Cu3O6.89	Y	1	Ba	2	Cu	3															O	z	6.89	3	1993																												Y123																				90.8					90.8			K/GPa	-0.27																																																																																												Single crystals were grown in Y2O3-stabiliqed ZrO2 crucible, O-content was varied annealing at 400-520C at I atm O2					UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6739	PHC2050139	twinned sample,dtc/dp for C-axial pressure	YBa2Cu3Oz	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	z	6.82	3	1993																												Y123																				87.7					87.7			K/GPa	1.6																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6740	PHC2050139	twinned sample,dtc/dp for C-axial pressure	YBa2Cu3Oz	Y1Ba2Cu3O6.63	Y	1	Ba	2	Cu	3															O	z	6.63	3	1993																												Y123																				61.1					61.1			K/GPa	4.4																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6741	PHC2050139	untwinned sample,dtc/dp for b-axial presure dtc/dp(a)=-2.7GP/K/2.3/-1.5/-1.0	YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	z	6.93	3	1993																												Y123																				89.7					89.7			K/GPa	3.1																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6742	PHC2050139	untwinned sample,dtc/dp for b-axial presure dtc/dp(a)=-2.7GP/K/2.3/-1.5/-1.0	YBa2Cu3Oz	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	z	6.73	3	1993																												Y123																				76.3					76.3			K/GPa	4.8																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6743	PHC2050139	untwinned sample,dtc/dp fpr b-axial presure dtc/dp(a)=-2.7GP/K/2.3/-1.5/-1.0	YBa2Cu3Oz	Y1Ba2Cu3O6.59	Y	1	Ba	2	Cu	3															O	z	6.59	3	1993																												Y123																				59.9					59.9			K/GPa	2.9																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6744	PHC2050139	untwinned sample,dtc/dp for b-axial presore dtc/dp(a)=-2.7GP/K/2.3/-1.5/-1.0	YBa2Cu3Oz	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	z	6.54	3	1993																												Y123																				55.5					55.5			K/GPa	2.5																																																																																																	UNIAXIAL PRESSURE DEPENDENCE OF TC UNTWINNED YBA2CU3OX SINGLECRYSTALS FOR X=6.5-7	199301			PHYSICA C,205(1993)139	A.ERB,C.MEINGAST,G.BRAUCHLE,G.MULLER-VOGT,H.CLAUS,H.WUHL,O.KRAUT	Y,BA,CU,O	
6745	SSC0981095	R(300)=8.6mOhm	ErBa2(Cu,Co)3O7	Er1Ba2Cu3O6.94	Er	1	Ba	2	Cu	3															O	z	6.94	1	1996																											3	Y123				3.82	3.886	11.671													90	91.5	93				91.5																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air in Pt crucible)-pellet-SIN(930C,24H in air)-ANN(500C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6746	SSC0981095	R(300)=9.9mOhm	ErBa2(Ca,Co)3O7	Er1Ba2Cu2.94Co0.06O6.8	Er	1	Ba	2	Cu	2.94	Co	0.06													O	z	6.8	1	1996																											3	Y123				3.833	3.877	11.655													71	73	75				73																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air in Pt crucible)-pellet-SIN(930C,24H in air)-ANN(500C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6747	SSC0981095	R(300)=67.9mOhm	ErBa2(Ca,Co)3O7	Er1Ba2Cu2.88Co0.12O6.78	Er	1	Ba	2	Cu	2.88	Co	0.12													O	z	6.78	1	1996																											3	Y123				3.833	3.884	11.663													42	46	52				46																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air in Pt crucible)-pellet-SIN(930C,24H in air)-ANN(500C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6748	SSC0981095	R(300)=101.4mOhm	ErBa2(Cu,Co)3O7	Er1Ba2Cu2.28Co0.18O6.74	Er	1	Ba	2	Cu	2.28	Co	0.18													O	z	6.74	1	1996																											3	Y123				3.803	3.88	11.665													26	34	40				34																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air in Pt crucible)-pellet-SIN(930C,24H in air)-ANN(500C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6749	SSC0981095	R(300)=188.0mOhm	ErBa2(Cu,Co)3O7	Er1Ba2Cu2.76Co0.24O6.75	Er	1	Ba	2	Cu	2.76	Co	0.24													O	z	6.75	1	1996																											3	Y123				3.858	3.862	11.672													18	31	53				31																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air in Pt crucible)-pellet-SIN(930C,24H in air)-ANN(500C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6750	SSC0981095	R(300)=57.7mOhm	(Er,Ca)Ba2(Cu,Co)3O7	Er0.94Ca0.06Ba2Cu2.82Co0.18O6.76	Er	0.94	Ca	0.06	Ba	2	Cu	2.82	Co	0.18											O	z	6.76	1	1996																											3	Y123				3.815	3.879	11.66													57	64	71				64																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6751	SSC0981095	R(300)=28.6mOhm	(Er,Ca)Ba2(Cu,Co)3O7	Er0.88Ca0.12Ba2Cu2.82Co0.18O6.93	Er	0.88	Ca	0.12	Ba	2	Cu	2.82	Co	0.18											O	z	6.93	1	1996																											3	Y123				3.823	3.878	11.658													72	77.5	83				77.5																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6752	SSC0981095	R(300)=13.7mOhm	(Er,Ca)Ba2(Cu,Co)3O7	Er0.82Ca0.18Ba2Cu2.82Co0.18O6.71	Er	0.82	Ca	0.18	Ba	2	Cu	2.82	Co	0.18											O	z	6.71	1	1996																											3	Y123				3.827	3.875	11.658													82	84.5	87				84.5																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in flowing O2)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6753	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.8Pr0.2Ba1Sr1Cu3O7-z	Y	0.8	Pr	0.2	Ba	1	Sr	1	Cu	3											O	7-z			1994																											3	Y123				3.823	3.858	11.572														69.1					69.1																																																																																															1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6754	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.6Pr0.4Ba1Sr1Cu3O7-z	Y	0.6	Pr	0.4	Ba	1	Sr	1	Cu	3											O	7-z			1994																											3	Y123				3.839	3.856	11.574														52.4					52.4																																																																																															1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6755	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.5Pr0.5Ba1Sr1Cu3O7-z	Y	0.5	Pr	0.5	Ba	1	Sr	1	Cu	3											O	7-z			1994																											2	Y123				3.849		11.578														32.1					32.1																																																																																															1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6756	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1Sr1Cu3O7-z	Y	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7-z			1994																											2	Y123				3.854		11.576														21.4					21.4																																																																																															1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6757	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.35Pr0.65Ba1Sr1Cu3O7-z	Y	0.35	Pr	0.65	Ba	1	Sr	1	Cu	3											O	7-z			1994																											2	Y123																				17.9					17.9																																																																																															1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6758	PLA1960263		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.3Pr0.7Ba1Sr1Cu3O7-z	Y	0.3	Pr	0.7	Ba	1	Sr	1	Cu	3											O	7-z			1994																											2	Y123				3.857		11.581																																																																																																																		1	mixture-fired(1203-1223K,24H in air)-pellet-SIN(1243-1253K,24H in flowing O2)-ANN(773K,24H)-cool to RT(1K/min)					Structural properties and superconductivity in the Y1-xPrxBaSrCu3O7-delta system	199412		Department of Applied Chemistry, University of Science and Technology of China, Hefei 2300026, China	Phys.Lett.A,196(1994)263-266	Guanghan Cao,Hongkai wu,Xiaojun Li,Yitai Qian,Yuheng Zhang,Zuyao Chen		
6759	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1996																											2	Hg1223				3.853		15.816														132.9					132.9																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6760	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg0.9Au0.1Ba2Ca2Cu3Oz	Hg	0.9	Au	0.1	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.85		15.79														133					133																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6761	PHC2620151		(HG,Au)Ba2Ca2Cu3Oz	Hg0.8Au0.2Ba2Ca2Cu3Oz	Hg	0.8	Au	0.2	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.846		15.739														130.9					130.9																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6762	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg0.7Au0.3Ba2Ca2Cu3Oz	Hg	0.7	Au	0.3	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.846		15.704														121					121																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6763	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg0.6Au0.4Ba2Ca2Cu3Oz	Hg	0.6	Au	0.4	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.843		15.68														118					118																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6764	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg0.5Au0.5Ba2Ca2Cu3Oz	Hg	0.5	Au	0.5	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.842		15.683														100					100																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6765	PHC2620151		(Hg,Au)Ba2Ca2Cu3Oz	Hg0.4Au0.6Ba2Ca2Cu3Oz	Hg	0.4	Au	0.6	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Hg1223				3.841		15.694														100					100																																																																																																precurso(Ba-Ca-Cu-O)+HgO+Au2O3-mixture-seal in Au capsoule-pressure up to 1.8GPA-heat(950C,1.6H)					Gold substitution  in mercury cuprate superconductors	05		Laboratoire de Critallographie CNRS-U.J.F.,BP 166,38042 Grenoble Cedex 9, France	Physica.C.262(1996)151-158	C. Cahaillout,J.J. Capponi,J.L. Tholence,M. Marezio,M.F. Gorius,P. Bordet,P.G. Radaelli,S. LeFloch		
6766	PHC2620261		RBa2Cu4O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.82	3.86	27.187														79.6					79.6																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6767	PHC2620261		RBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.836	3.869	27.197														77.8					77.8																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6768	PHC2620261		RBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.837	3.867	27.204														76.2					76.2																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6769	PHC2620261		RBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.842	3.871	27.229														78.6					78.6																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6770	PHC2620261		RBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.845	3.87	27.236														73.6					73.6																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6771	PHC2620261		RBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.877	3.899	27.274														71.8					71.8																																																																																														R2O3,BaCO3,CuO	1	mixture-CAL(900C,2day in air)-ANN(820C,2-6day in flowing O2)-FC to RT					Synthesis of bulk superconductors RBa2Cu4O8(R=Tm, Er, Ho, Y, Dy, and Gd) by a simple solid-state rection method	05		Department of Applied Chemistry, Faculty of Engineering, Kansai University, Osaka 564, Japan	Physica.C,262(1996)261-265	Makoto Kawazoe,Masakazu Tatsumi,Seika Yamamoto	Tm, Er, Ho, Y, Dy, Gd, Ba, Cu, O	
6772	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.78	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.78		1996																												Tl1212																																																																																																																									annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6773	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.76	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.76		1996																												Tl1212																				21					21																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6774	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.75	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.75		1996																												Tl1212																				37					37																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6775	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.74	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.74		1996																												Tl1212																				43					43																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6776	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.68	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.68		1996																												Tl1212																				75					75																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6777	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.61	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.61		1996																												Tl1212																				52					52																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6778	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.58	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.58		1996																												Tl1212																				43					43																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6779	PHC2630189		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.52	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.52		1996																												Tl1212																				23					23																																																																																																annealed in a fllowing Ar or heated in a evacuated quartz tube with Zr-foil getter					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6780	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca1Cu2O6.78	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.78	1	1996																												Tl1212																							4.2																																																																																																CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6781	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.8Y0.2Cu2O6.82	Tl	1	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	z	6.82	1	1996																												Tl1212																				85					85																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6782	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.7Y0.3Cu2O6.84	Tl	1	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	z	6.84	1	1996																												Tl1212																				87					87																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6783	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.6Y0.4Cu2O6.86	Tl	1	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	z	6.86	1	1996																												Tl1212																				87					87																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6784	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.5Y0.5Cu2O6.89	Tl	1	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	z	6.89	1	1996																												Tl1212																				92					92																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6785	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.4Y0.6Cu2O6.93	Tl	1	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	z	6.93	1	1996																												Tl1212																				92		89.1			92																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6786	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.3Y0.7Cu2O6.97	Tl	1	Sr	2	Ca	0.3	Y	0.7	Cu	2											O	z	6.97	1	1996																												Tl1212																				92					92																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6787	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.2Y0.8Cu2O6.97	Tl	1	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	z	6.97	1	1996																												Tl1212																				93					93																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6788	PHC2630189		TlSr2(Ca,Y)Cu2Oz	Tl1Sr2Ca0.1Y0.9Cu2O6.97	Tl	1	Sr	2	Ca	0.1	Y	0.9	Cu	2											O	z	6.97	1	1996																												Tl1212																				87					87																																																																																														CaO,Y2O3,CuO,Sr2CuO3,Tl2O3	1	mixture with excess Tl2O3-pellet in Au bags-SIN(910C,12H)-wrapped in Au foil-SIN(920-930C,IH in flowing O2)					Cation substitution and deoxygenation effect on superconductivity of Tl-Sr1212 cuprate			Institute for Materials Reserch, Tohoku University, Katahira, Aoba-ku, Sendai 980-77, Japan	Physica.C,263(1996)189-192	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Yasuhiko Syono		
6789	PSS1940371		HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1996																											2	Hg1223				3.848		15.774													119	130		133.7			130																																																																							ohm.cm																				RH6789			Ba(NO3)2,CaO,CuO,HgO		precursor(Ba2Ca2Cu3Oz)-ground and mixed with HgO in glove bix in air-pellet-sealed in quaetz tubu-heat to 800C(1K/min),6H)-ANN(300C,6H in O2flow)					Transport Properties of High-Tc Mercury Cuprates			Department of Physics, University of Colorado, Boulder	Phys,Stat.Sol.(b)194(1996)371	"A. M. Hermann,A. Naziripour,R. Tello,U"". Onbasli,W. Kiehl,Y,T, Wang"	Hg, Ba, Ca, Cu, O	
6790	PSS1940371		HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1996																											2	Hg1223				3.856		15.883													126	132	138	137.8			132																																																																							ohm.cm																				RH6790			Ba(No3)2,CaO,CuO,HgO		precursor+Hgo in a glove box in Ar-sealed in quaetz tube-heat(800C,6H)-ANN(300,6H in O2 flow)					Transport Properties of High-Tc Mercury Cuprates			Department of Physics, University of Colorado, Boulder	Phys,Stat.Sol.(b)194(1996)371	"A. M. Hermann,A. Naziripour,R. Tello,U"". Onbasli,W. Kiehl,Y,T, Wang"	Hg, Ba, Ca, Cu, O	
6791	SSC0990413		YSr2(Cu,Re)3Oz	Y1Sr2Cu2.8Re0.2O6+z	Y	1	Sr	2	Cu	2.8	Re	0.2													O	6+z		1	1996																											2	Y123				3.813		11.52																42			42																																																																																														T2O3,Pr2O3,SrCO3,ReO2,CuO	1	mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-FC					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6792	SSC0990413		(Y,Pr)Sr2(Cu,Re)3Oz	Y0.25Pr0.75Sr2Cu2.8Re0.2O6+z	Y	0.25	Pr	0.75	Sr	2	Cu	2.8	Re	0.2											O	6+z		1	1996																											2	Y123				3.845		11.586																	5																																																																																																T2O3,Pr2O3,SrCO3,ReO2,CuO	1	mixture-CAL(950C,12-18H in air)-pellet-heat(980C,16-24H in air)-FC					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6793	SSC0990413		YSr2(Cu,Re)3Oz	Y1Sr2Cu2.8Re0.2O6+z	Y	1	Sr	2	Cu	2.8	Re	0.2													O	6+z		1	1996																											2	Y123				3.821		11.548																55			55																																																																																																PREPID=(6791)-ANN(480C,24H under 200bar O2)-slow cool to RT					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6794	SSC0990413		(Y,Ca)Sr2(Cu,Re)3Oz	Y0.25Pr0.75Sr2Cu2.8Re0.2O6+z	Y	0.25	Pr	0.75	Sr	2	Cu	2.8	Re	0.2											O	6+z		1	1996																											2	Y123				3.854		11.589																14			14																																																																																																PREPID=(6791)-ANN(480C,24H under 200bar O2)-slow cool to RT					ENHANCEMENT OF Tc IN Y1-xPrxCu2.8Re0.2O6+z(z~1;x=0, 0.75)DUE TO THE ELEVATED OXYGEN PRESSURE ANNEALING			Laboratoire de Physique des Solides, CNRS, 92195 Meudon, France	Solid State 98.,(1996)413	A. Das,B. Dabrowski,R. Suryanarayanan	Y, Pr, CU, Re, O	
6795	SSC0981095		ErBa2(Cu,Co)3Oz	Er1Ba2Cu3O6.94	Er	1	Ba	2	Cu	3															O	z	6.94	1	1996																											3	Y123				3.82	3.886	11.671													90	91.5	93				91.5																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air)-ANN(500C,24H in O2flow)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6796	SSC0981095		ErBa2(Cu,Co)3Oz	Er1Ba2Cu2.94Co0.06O6.8	Er	1	Ba	2	Cu	2.94	Co	0.06													O	z	6.8	1	1996																											3	Y123				3.833	3.877	11.655													71	73	75				73																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air)-ANN(500C,24H in O2flow)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6797	SSC0981095		ErBa2(Cu,Co)3Oz	Er1Ba2Cu2.88Co0.12O6.78	Er	1	Ba	2	Cu	2.88	Co	0.12													O	z	6.78	1	1996																											3	Y123				3.833	3.884	11.663													42	46	52				46																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air)-ANN(500C,24H in O2flow)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6798	SSC0981095		ErBa2(Cu,Co)3Oz	Er1Ba2Cu2.82Co0.18O6.74	Er	1	Ba	2	Cu	2.82	Co	0.18													O	z	6.74	1	1996																											3	Y123				3.803	3.88	11.665													26	34	40				34																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air)-ANN(500C,24H in O2flow)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6799	SSC0981095		ErBa2(Cu,Co)3Oz	Er1Ba2Cu2.76Co0.24O6.75	Er	1	Ba	2	Cu	2.76	Co	0.24													O	z	6.75	1	1996																											3	Y123				3.858	3.862	11.672													18	31	53				31																																																																																														Er2O3,BaCO3,CuO,Co3O4,CaCO3	1	mixture-heat(930C,24H in air)-ANN(500C,24H in O2flow)-cool to RT(1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6800	SSC0981095		(Er,Ca)Ba2(Cu,Co)3Oz	Er0.94Ca0.04Ba2Cu2.82Co0.18O6.76	Er	0.94	Ca	0.04	Ba	2	Cu	2.82	Co	0.18											O	z	6.76	1	1996																											3	Y123				3.815	3.879	11.66													57	64	71				64																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-cool to RT (1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6801	SSC0981095		(Er,Ca)Ba2(Cu,Co)3Oz	Er0.88Ca0.12Ba2Cu2.28Co0.18O6.93	Er	0.88	Ca	0.12	Ba	2	Cu	2.28	Co	0.18											O	z	6.93	1	1996																											3	Y123				3.823	3.878	11.658													72	77.5	83				77.5																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-cool to RT (1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6802	SSC0981095		(Er,Ca)Ba2(Cu,Co)3Oz	Er0.82Ca0.18Ba2Cu2.82Co0.18O6.71	Er	0.82	Ca	0.18	Ba	2	Cu	2.82	Co	0.18											O	z	6.71	1	1996																											3	Y123				3.827	3.875	11.658													82	84.5	87				84.5																																																																																															1	SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-cool to RT (1C/min)					INFLUENCE OF HOLE FILLING BY Co AND HOLE DOPING BY Ca ON THE SUPERCONDUCTIVITY OF ErBa2Cu3O7-z			Department of Physics,Saurashtra University, Rajkot-360005, India	Solid State Commun.98(1996)10095-1098	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni,U.S. Joshi	Ca, Er, Ba, Cu, O, Co	
6803	SSC0980185	Hirr=A*(1-T/Tc)^3.62	HgBa2(Ca,Sr)2Cu3O8	Hg1Ba2Ca1.72Sr0.28Cu3O8+z	Hg	1	Ba	2	Ca	1.72	Sr	0.28	Cu	3											O	8+z			1996																											2	Hg1223				3.86		16.085																																																					HIR6803																																																												HgO,TlO3,Ba2CuO3,Ca0.86Sr0.14CuO2		See Mater,Res.Bull.29(1994)959					CRITICAL CURRENTS AND IRREVERSIBILITY LINES IN Hg1-xTlxBa2 (Ca0.86Sr0.14)2Cu3O8+z			Korea Research Institute of Standards and Science, Yusung, P.O. Box 102,Taejon, 305-600,South Korea	Solid State Commun.98(1996)185-188	I.S. Kim,J.C. Park,K.-H. Yoo,N.H. Hur,S.C. Yu,Y.B. Kim,Y.K. Park,Y.Y. Song	Hg, Tl, Ba, Ca, Sr, Cu, O	
6804	SSC0980185	Hirr=A*(1-T/Tc)^2.6	(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.75Tl0.25Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.75	Tl	0.25	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z			1996																											2	Hg1223				3.855		15.921																																																					HIR6804																																																												HgO,TlO3,Ba2CuO3,Ca0.86Sr0.14CuO2		See Mater,Res.Bull.29(1994)959					CRITICAL CURRENTS AND IRREVERSIBILITY LINES IN Hg1-xTlxBa2 (Ca0.86Sr0.14)2Cu3O8+z			Korea Research Institute of Standards and Science, Yusung, P.O. Box 102,Taejon, 305-600,South Korea	Solid State Commun.98(1996)185-188	I.S. Kim,J.C. Park,K.-H. Yoo,N.H. Hur,S.C. Yu,Y.B. Kim,Y.K. Park,Y.Y. Song	Hg, Tl, Ba, Ca, Sr, Cu, O	
6805	SSC0980185	Hirr=A*(1-T/Tc)^2.51	(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.5Tl0.5Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.5	Tl	0.5	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z			1996																											2	Hg1223				3.85		15.874																																																					HIR6805																																																												HgO,TlO3,Ba2CuO3,Ca0.86Sr0.14CuO2		See Mater,Res.Bull.29(1994)959					CRITICAL CURRENTS AND IRREVERSIBILITY LINES IN Hg1-xTlxBa2 (Ca0.86Sr0.14)2Cu3O8+z			Korea Research Institute of Standards and Science, Yusung, P.O. Box 102,Taejon, 305-600,South Korea	Solid State Commun.98(1996)185-188	I.S. Kim,J.C. Park,K.-H. Yoo,N.H. Hur,S.C. Yu,Y.B. Kim,Y.K. Park,Y.Y. Song	Hg, Tl, Ba, Ca, Sr, Cu, O	
6806	SSC0980185	Hirr=A*(1-T/Tc)^2.41	(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.25Tl0.75Ba2Ca1.72Sr0.28Cu3O8+z	Hg	0.25	Tl	0.75	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+z			1996																											2	Hg1223				3.846		15.832																																																					HIR6806																																																												HgO,TlO3,Ba2CuO3,Ca0.86Sr0.14CuO2		See Mater,Res.Bull.29(1994)959					CRITICAL CURRENTS AND IRREVERSIBILITY LINES IN Hg1-xTlxBa2 (Ca0.86Sr0.14)2Cu3O8+z			Korea Research Institute of Standards and Science, Yusung, P.O. Box 102,Taejon, 305-600,South Korea	Solid State Commun.98(1996)185-188	I.S. Kim,J.C. Park,K.-H. Yoo,N.H. Hur,S.C. Yu,Y.B. Kim,Y.K. Park,Y.Y. Song	Hg, Tl, Ba, Ca, Sr, Cu, O	
6807	SSC0980031		ErBa2Cu3O7	Er1Ba2Cu3O7-z	Er	1	Ba	2	Cu	3															O	7-z		1	1996																												Y123																				91.8					91.8																																																					SP6807	mJ/mole.K	4.4																																							Er2O3, Y2O3, BaCO3, CuO	1	See Phys,Stat,Sol.(a)116(1989)367					SPECIFIC HEAT OF Er1-xYxBa2Cu3O7-z. AN OBSERVATION OF CRYSTALLINE ELECTRIC FIELD CONTRIBUTION			Institute of Low Temperature and Structure Reserch,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclow 2 Poland	Solid State Commun.98(1996)31-34	D. Wlosewicz,T. Plackowski	Er, Y, Ba, Cu, O	
6808	SSC0980031		(Er,Y)Ba2Cu3O7	Er0.5Y0.5Ba2Cu3O7-z	Er	0.5	Y	0.5	Ba	2	Cu	3													O	7-z		1	1996																												Y123																				91.8					91.8																																																					SP6808	mJ/mole.K	3.2																																							Er2O3, Y2O3, BaCO3, CuO	1	See Phys,Stat,Sol.(a)116(1989)367					SPECIFIC HEAT OF Er1-xYxBa2Cu3O7-z. AN OBSERVATION OF CRYSTALLINE ELECTRIC FIELD CONTRIBUTION			Institute of Low Temperature and Structure Reserch,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclow 2 Poland	Solid State Commun.98(1996)31-34	D. Wlosewicz,T. Plackowski	Er, Y, Ba, Cu, O	
6809	SSC0980031		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1996																												Y123																				91					91																																																					SP6809	mJ/mole.K	3.6																																							Er2O3, Y2O3, BaCO3, CuO	1	See Phys,Stat,Sol.(a)116(1989)367					SPECIFIC HEAT OF Er1-xYxBa2Cu3O7-z. AN OBSERVATION OF CRYSTALLINE ELECTRIC FIELD CONTRIBUTION			Institute of Low Temperature and Structure Reserch,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclow 2 Poland	Solid State Commun.98(1996)31-34	D. Wlosewicz,T. Plackowski	Er, Y, Ba, Cu, O	
6810	PLA2070109	Tc and Meissner effect were measured by ESR	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		4	1995																												Y123																				90				20	90										7																																																																																						film was deposited from 99.9% pure material onto 640C (100)MgO substrate					Superconductivity in PrBa2Cu3O7	010		Department of Physics, University of Notre Dame, Notre Dame, IN 46556, USA	Phys,Lett.A,207(1995)109-112	A.E. Klunzinger,D.B. Chrisey,H.A. Blackstead,J.S. Horwitz,John D. Dow	Pr, Ba, Cu, O	
6811	PLA2080257		Y(Ba,Sr)Cu3O7	Y1Ba1Sr1Cu3O6.91	Y	1	Ba	1	Sr	1	Cu	3													O	z	6.91		1995																												Y123																				81					81																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6812	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.975Sn0.025O6.92	Y	1	Ba	1	Sr	1	Cu	2.975	Sn	0.025											O	z	6.92		1995																												Y123																				77					77																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6813	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.95Sn0.05O6.96	Y	1	Ba	1	Sr	1	Cu	2.95	Sn	0.05											O	z	6.96		1995																												Y123																				73.7					73.7																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6814	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.9Sn0.1O7	Y	1	Ba	1	Sr	1	Cu	2.9	Sn	0.1											O	z	7		1995																												Y123																				69.1					69.1																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6815	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.85Sn0.15O7.06	Y	1	Ba	1	Sr	1	Cu	2.85	Sn	0.15											O	z	7.06		1995																												Y123																				63.8					63.8																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6816	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.8Sn0.2O7.12	Y	1	Ba	1	Sr	1	Cu	2.8	Sn	0.2											O	z	7.12		1995																												Y123																				49.8					49.8																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6817	PLA2080257		Y(Ba,Sr)2(Cu,Sn)3Oz	Y1Ba1Sr1Cu2.75Sn0.25O7.16	Y	1	Ba	1	Sr	1	Cu	2.75	Sn	0.25											O	z	7.16		1995																												Y123																				40.9					40.9																																																																																														Y2O3, BaCO3, SrCO3, CUO, SnO2		See Sold State Commun.75(1990)629					Lacalisation of Cu2+ states by Sn4+ ions in the YBaSrCu3Oy system	010		Superconductivity Research Group,School of Materials Science and Engineering, University of NewSouth Wales,Sydney,NSW 2052,Australia	Phys.Lett.A,208(1995)257-260	B. Chen,H. Zhang,Y. Zhao,Z. Xiong	Y, Ba, Sr, Cu, O, Sm	
6818	SSC0980395		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.59	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.59	1	1996																												Y123																				68.8					68.8			K/GPa	8.4																																																																			ohm.cm																			7	RH6818			Y2O3, CaCO3, BaCO3, CuO	1	mixture-fired(900C,6H in air)-pellet-heat(930-940C,10-15H in flowing Oz)-ANN(appropriete temp.in flowing O2)-Q to 77K					EFFECTS OF OXYGEN DOPING AND PRESSURE ON SUPERCONDUCTING TRANSITION TEMPERATUREIN Y0.9Ca0.1Ba2Cu3Oy			Department of Physics, Asahikawa Medical College,Asahikawa 078, Japan	Solid state Commun.98(1996)395-399	K. Yamaya,M. Tanimoto,N. Mo^ri,T. Honma	Y, Ca, Ba, Cu, O	
6819	SSC0980395		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.72	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.72	1	1996																												Y123																				82.6					82.6			K/GPa	4.6																																																																			ohm.cm																				RH6819			Y2O3, CaCO3, BaCO3, CuO	1	mixture-fired(900C,6H in air)-pellet-heat(930-940C,10-15H in flowing Oz)-ANN(appropriete temp.in flowing O2)-Q to 77K					EFFECTS OF OXYGEN DOPING AND PRESSURE ON SUPERCONDUCTING TRANSITION TEMPERATUREIN Y0.9Ca0.1Ba2Cu3Oy			Department of Physics, Asahikawa Medical College,Asahikawa 078, Japan	Solid state Commun.98(1996)395-399	K. Yamaya,M. Tanimoto,N. Mo^ri,T. Honma	Y, Ca, Ba, Cu, O	
6820	SSC0980395		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.87	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.87	1	1996																												Y123																				85.4					85.4			K/GPa	2.4																																																																			ohm.cm																				RH6820			Y2O3, CaCO3, BaCO3, CuO	1	mixture-fired(900C,6H in air)-pellet-heat(930-940C,10-15H in flowing Oz)-ANN(appropriete temp.in flowing O2)-Q to 77K					EFFECTS OF OXYGEN DOPING AND PRESSURE ON SUPERCONDUCTING TRANSITION TEMPERATUREIN Y0.9Ca0.1Ba2Cu3Oy			Department of Physics, Asahikawa Medical College,Asahikawa 078, Japan	Solid state Commun.98(1996)395-399	K. Yamaya,M. Tanimoto,N. Mo^ri,T. Honma	Y, Ca, Ba, Cu, O	
6821	SSC0980395		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.98	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.98	1	1996																												Y123																				81.8					81.8																																																																							ohm.cm																				RH6821			Y2O3, CaCO3, BaCO3, CuO	1	mixture-fired(900C,6H in air)-pellet-heat(930-940C,10-15H in flowing Oz)-ANN(appropriete temp.in flowing O2)-Q to 77K					EFFECTS OF OXYGEN DOPING AND PRESSURE ON SUPERCONDUCTING TRANSITION TEMPERATUREIN Y0.9Ca0.1Ba2Cu3Oy			Department of Physics, Asahikawa Medical College,Asahikawa 078, Japan	Solid state Commun.98(1996)395-399	K. Yamaya,M. Tanimoto,N. Mo^ri,T. Honma	Y, Ca, Ba, Cu, O	
6822	SSC0980333		HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1996																											2	Hg1201				3.877		9.513																87			87																																																																																															1	precursor(Ba2CuO3)+HgO+CeO2-mixture-pellet-seald in quartz tubu-heat(850C,5H)-cool to RT(150C/H)					SUPERCONDUCTING PROPERTIES OF Ce-SUBSTITUTED HgBa2CuO4+z			Institute for Pure and Applied Physical Sciences, University of California, San Diego,La Jolla,CA 92093,U.S.A.	Solid State Commun.98(1996)333-336	J. Herrmann,M.B. Maple,M.S. Chae,M.T. Simnad,S.H. Han	Hg, Ba, Cu, O, Ce	
6823	SSC0980333		(Hg,Ce)Ba2CuO4	Hg0.95Ce0.05Ba2Cu1O4+z	Hg	0.95	Ce	0.05	Ba	2	Cu	1													O	4+z			1996																											2	Hg1201				3.887		9.521													92		94	94			94																																																																																															1	precursor(Ba2CuO3)+HgO+CeO2-mixture-pellet-seald in quartz tubu-heat(850C,5H)-cool to RT(150C/H)					SUPERCONDUCTING PROPERTIES OF Ce-SUBSTITUTED HgBa2CuO4+z			Institute for Pure and Applied Physical Sciences, University of California, San Diego,La Jolla,CA 92093,U.S.A.	Solid State Commun.98(1996)333-336	J. Herrmann,M.B. Maple,M.S. Chae,M.T. Simnad,S.H. Han	Hg, Ba, Cu, O, Ce	
6824	SSC0980333		(Hg,Ce)Ba2CuO4	Hg0.9Ce0.1Ba2Cu1O4+z	Hg	0.9	Ce	0.1	Ba	2	Cu	1													O	4+z			1996																											2	Hg1201				3.885		9.53																96			96																																																																																															1	precursor(Ba2CuO3)+HgO+CeO2-mixture-pellet-seald in quartz tubu-heat(850C,5H)-cool to RT(150C/H)					SUPERCONDUCTING PROPERTIES OF Ce-SUBSTITUTED HgBa2CuO4+z			Institute for Pure and Applied Physical Sciences, University of California, San Diego,La Jolla,CA 92093,U.S.A.	Solid State Commun.98(1996)333-336	J. Herrmann,M.B. Maple,M.S. Chae,M.T. Simnad,S.H. Han	Hg, Ba, Cu, O, Ce	
6825	SSC0980333		(Hg,Ce)Ba2CuO4	Hg0.8Ce0.2Ba2Cu1O4+z	Hg	0.8	Ce	0.2	Ba	2	Cu	1													O	4+z			1996																											2	Hg1201				3.885		9.528													75		94	94			94																																																																																															1	precursor(Ba2CuO3)+HgO+CeO2-mixture-pellet-seald in quartz tubu-heat(850C,5H)-cool to RT(150C/H)					SUPERCONDUCTING PROPERTIES OF Ce-SUBSTITUTED HgBa2CuO4+z			Institute for Pure and Applied Physical Sciences, University of California, San Diego,La Jolla,CA 92093,U.S.A.	Solid State Commun.98(1996)333-336	J. Herrmann,M.B. Maple,M.S. Chae,M.T. Simnad,S.H. Han	Hg, Ba, Cu, O, Ce	
6826	SSC0980333		(Hg,Ce)Ba2CuO4	Hg0.7Ce0.3Ba2Cu1O4+z	Hg	0.7	Ce	0.3	Ba	2	Cu	1													O	4+z			1996																											2	Hg1201				3.886		9.531																94			94																																																																																															1	precursor(Ba2CuO3)+HgO+CeO2-mixture-pellet-seald in quartz tubu-heat(850C,5H)-cool to RT(150C/H)					SUPERCONDUCTING PROPERTIES OF Ce-SUBSTITUTED HgBa2CuO4+z			Institute for Pure and Applied Physical Sciences, University of California, San Diego,La Jolla,CA 92093,U.S.A.	Solid State Commun.98(1996)333-336	J. Herrmann,M.B. Maple,M.S. Chae,M.T. Simnad,S.H. Han	Hg, Ba, Cu, O, Ce	
6828	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.98Ni0.02O8	Y	1	Ba	2	Cu	3.98	Ni	0.02													O	8			1996																											3	Y124				3.84	3.869	27.224														74					74																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6829	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.97Ni0.03O8	Y	1	Ba	2	Cu	3.97	Ni	0.03													O	8			1996																											3	Y124																				70.4					70.4																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6830	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8			1996																											3	Y124																				68.2					68.2																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6831	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.939Ni0.061O8	Y	1	Ba	2	Cu	3.939	Ni	0.061													O	8			1996																											3	Y124				3.839	3.87	27.201														63.5					63.5																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6832	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8			1996																											3	Y124																				55.1					55.1																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6833	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.9Ni0.1O8	Y	1	Ba	2	Cu	3.9	Ni	0.1													O	8			1996																											3	Y124				3.839	3.872	27.187														52.6					52.6																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6834	SSC0980971		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.8Ni0.2O8	Y	1	Ba	2	Cu	3.8	Ni	0.2													O	8			1996																											3	Y124				3.841	3.874	27.185														21					21																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6835	SSC0980971		YBa2Cu4O8	Y1Ba2Cu1O8	Y	1	Ba	2	Cu	1															O	8			1996																											3	Y124				3.842	3.87	27.194														80					80																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6836	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.992Zn0.008O8	Y	1	Ba	2	Cu	3.992	Zn	0.008													O	8			1996																											3	Y124																				74					74																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6837	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O	8			1996																											3	Y124				3.869	3.838	27.212														67					67																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6838	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O	8			1996																											3	Y124				3.871	3.84	27.211														57.6					57.6																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6839	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.938Zn0.062O8	Y	1	Ba	2	Cu	3.938	Zn	0.062													O	8			1996																											3	Y124				3.872	3.841	27.21														47					47																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6840	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.92Zn0.08O8	Y	1	Ba	2	Cu	3.92	Zn	0.08													O	8			1996																											3	Y124																				36.7					36.7																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6841	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.9Zn0.1O8	Y	1	Ba	2	Cu	3.9	Zn	0.1													O	8			1996																											3	Y124				3.873	3.841	27.207														22.4					22.4																																																																																														Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6842	SSC0980971		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.848Zn0.152O8	Y	1	Ba	2	Cu	3.848	Zn	0.152													O	8			1996																											3	Y124																								5																																																																																															Y2O3, BaO, CuO, NiO, ZnO		mixture-CAL(650C,750C,880C, 24H in air)-pellet-SIN(950C,16H in O2)-ANN(500C,16H in O2)-ANN(990C,48H under 100bar O2)					EVIDENCE FOR CHAIN SITE SUBSTTUTION OF NICKEL IN YBa2(Cu1-xNix)4O8			Department of Physics, University of Missouri, Columbia, MO 65211	Solid State Commun.,98(1996)971	B. Jayaram,Dale J. Payne,H.R. Chandrasekhar,J. Ulanday,Meera Chandrasekhar	Zn, Y, Ba, Cu, Ni, O	
6843	PHC2690005		Sr2RCu2O5F	Sr2Yb1Cu2F1O5	Sr	2	Yb	1	Cu	2	F	1													O	5		1	1996																												2126				3.834		19.764																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6844	PHC2690005		Sr2RCu2O5F	Sr2Er1Cu2F1O5	Sr	2	Er	1	Cu	2	F	1													O	5		1	1996																												2126				3.838		19.787																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6845	PHC2690005		Sr2RCu2O5F	Sr2Y1Cu2F1O5	Sr	2	Y	1	Cu	2	F	1													O	5		1	1996																												2126				3.838		19.764																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6846	PHC2690005		Sr2RCu2O5F	Sr2Dy1Cu2F1O5	Sr	2	Dy	1	Cu	2	F	1													O	5		1	1996																												2126				3.845		19.789																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6847	PHC2690005		Sr2RCu2O5F	Sr2Gd1Cu2F1O5	Sr	2	Gd	1	Cu	2	F	1													O	5		1	1996																												2126				3.857		19.808																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6848	PHC2690005		Sr2RCu2O5F	Sr2Sm2Cu2F1O5	Sr	2	Sm	2	Cu	2	F	1													O	5		1	1996																												2126				3.871		19.869																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6849	PHC2690005		Sr2RCu2O5F	Sr2Nd1Cu2F1O5	Sr	2	Nd	1	Cu	2	F	1													O	5		1	1996																												2126				3.876		19.915																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6850	PHC2690005		Sr2RCu2O5F	Sr2La1Cu2F1O5	Sr	2	La	1	Cu	2	F	1													O	5		1	1996																												2126				3.845		20.065																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6851	PHC2690005		Sr2(Nd,Ca)Cu2O5F	Sr2Nd0.7Ca0.3Cu2F1O5	Sr	2	Nd	0.7	Ca	0.3	Cu	2	F	1											O	5		2	1996																												2126				3.879		19.885																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6852	PHC2690005		Sr(Nd,Ca)Cu2O5f	Sr2Nd0.5Ca0.5Cu2F1O5	Sr	2	Nd	0.5	Ca	0.5	Cu	2	F	1											O	5		1	1996																												2126				3.866		19.9														70.9					70.9																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6853	PHC2690005		Sr(Nd,Ca)Cu2O5F	Sr2Nd0.4Ca0.6Cu2F1O5	Sr	2	Nd	0.4	Ca	0.6	Cu	2	F	1											O	5		1	1996																												2126				3.859		20.048														75.1					75.1																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6854	PHC2690005		Sr(Nd,Ca)Cu2O5F	Sr2Nd0.3Ca0.7Cu2F1O5	Sr	2	Nd	0.3	Ca	0.7	Cu	2	F	1											O	5		1	1996																												2126				3.871		20.021														73.1					73.1																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6855	PHC2690005		Sr2(Nd,Ca)Cu2O5F	Sr2Nd0.2Ca0.8Cu2F1O5	Sr	2	Nd	0.2	Ca	0.8	Cu	2	F	1											O	5		1	1996																												2126				3.861		20.073														86					86																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6856	PHC2690005		Sr(Nd,Ca)Cu2O5F	Sr2Nd0.1Ca0.9Cu2F1O5	Sr	2	Nd	0.1	Ca	0.9	Cu	2	F	1											O	5		1	1996																												2126				3.862		20.085														85.8					85.8																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6857	PHC2690005		Sr2CaCu2O5F	Sr2Ca1Cu2F1O5	Sr	2	Ca	1	Cu	2	F	1													O	5		1	1996																											2	2126				3.856		20.14														69.1					69.1																																																																																														R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6858	PHC2690005		Sr2NdCu2O5F	Sr2Nd1Cu2F1O5	Sr	2	Nd	1	Cu	2	F	1													O	5		2	1996																											2	2216				3.876		19.915																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6859	PHC2690005		Sr2(Nd,Ca)Cu2O5F	Sr2Nd0.9Ca0.1Cu2F1O5	Sr	2	Nd	0.9	Ca	0.1	Cu	2	F	1											O	5		2	1996																											2	2216				3.889		19.93																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6860	PHC2690005		Sr2(Nd,Ca)Cu2O5F	Sr2Nd0.8Ca0.2Cu2F1O5	Sr	2	Nd	0.8	Ca	0.2	Cu	2	F	1											O	5		2	1996																											2	2216				3.889		19.907																																																																																																																	R2O3, CuO, SrO2,SrF2, CaCuCO3,SrCuo2,Ca2	1	mixture-seald in Au capsule-(1300c,6GPa,1H)-Q to RT					Synthesis,crystal structures and superconductivity of new copper oxyfluorides,Sr2RCu2O5F(R=Y,La,Nd,Sm,Gd,Dy,Er and Yd)			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	Physica.C,269(1996)5-14	E. Takayama-Muromachi,F. Izumi,J.-Q. Li,M. Isobe,Y. Kanke,Y. Matsui	Sr, R, Cu, O, F	
6861	PHC2690220		Dyba2Cu3O7	Dy1Ba2Cu3O6.9	Dy	1	Ba	2	Cu	3															O	7	6.9		1996																												Y123																				92.3					92.3																																																																																														D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6862	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.95Pr0.05Ba2Cu3O6.9	Dy	0.95	Pr	0.05	Ba	2	Cu	3													O	7	6.9		1996																												Y123																				91.4					91.4																																																																			2.31			TP6862																								D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6863	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.85Pr0.15Ba2Cu3O6.9	Dy	0.85	Pr	0.15	Ba	2	Cu	3													O	7	6.9		1996																												Y123																				77.4					77.4																																																																			8.381			TP6863																								D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6864	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.8Pr0.2Ba2Cu3O6.9	Dy	0.8	Pr	0.2	Ba	2	Cu	3													O	7	6.9		1996																												Y123																																																																																																																							D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6865	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.7Pr0.3Ba2Cu3O6.9	Dy	0.7	Pr	0.3	Ba	2	Cu	3													O	7	6.9		1996																												Y123																				53.9					53.9																																																																			17.92			TP6865																								D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6866	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.6Pr0.4Ba2Cu3O6.9	Dy	0.6	Pr	0.4	Ba	2	Cu	3													O	7	6.9		1996																												Y123																				41.2					41.2																																																																																														D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6867	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.5Pr0.5Ba2Cu3O6.9	Dy	0.5	Pr	0.5	Ba	2	Cu	3													O	7	6.9		1996																												Y123																				27.8					27.8																																																																			37.57			TP6867																								D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6868	PHC2690220		(Dy,Pr)Ba2Cu3O7	Dy0.4Pr0.6Ba2Cu3O6.9	Dy	0.4	Pr	0.6	Ba	2	Cu	3													O	7	6.9		1996																												Y123																								10																																																																				53.7			TP6868																								D2O2,Pr6O11,BaCO3,CuO2	1	mixture-CAL(900C,12H in air)-pellet-SIN(940C,12H)-slow cool to 600C-hold3H-cool to 600C-hold3H-cool to 400C(2H)-RT in flowing O2					Thermoelectric power and superconducting transition in high-temperature superconductors Dy1-xPrxBa2Cu3O7			Department of physics,National Taiwan University,Taipei,Taiwan	Physica.C,269(1996)220-224	C.Y.  Huang,J.C. Ho,J.G. Lin,J.J. Lin,Z.J. Huang	Dy, Pr, Ba, Cu, O	
6869	PHC2690225		TlSr2YbCu2O7	Tl1Sr2Yb1Cu2O7	Tl	1	Sr	2	Yb	1	Cu	2													O	7	7		1996																												Tl1212				3.805		11.989																	5																																																																																																Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6870	PHC2690225		Tl(Sr,Ca)2YbCu2O7	Tl1Sr1.8Ca0.2Yb1Cu2O7	Tl	1	Sr	1.8	Ca	0.2	Yb	1	Cu	2											O	7			1996																												Tl1212				3.794		11.982														45					45																																																																																														Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6871	PHC2690225		Tl(Sr,Ca)2YbCu2O7	Tl1Sr1.7Ca0.3Yb1Cu2O7	Tl	1	Sr	1.7	Ca	0.3	Yb	1	Cu	2											O	7			1996																												Tl1212				3.791		11.973														55					55																																																																																														Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6872	PHC2690225		Tl(Sr,Ca)2YbCu2O7	Tl1Sr1.5Ca0.5Yb1Cu2O7	Tl	1	Sr	1.5	Ca	0.5	Yb	1	Cu	2											O	7			1996																												Tl1212				3.791		11.952														55					55																																																																																														Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6873	PHC2690225		Tl(Sr,Ca)2YbCu2O7	Tl1Sr1Ca1Yb1Cu2O6.8	Tl	1	Sr	1	Ca	1	Yb	1	Cu	2											O	7	6.8		1996																												Tl1212																																																																																																																							Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6874	PHC2690225		Tl(Sr,Ca)2YbCu2O7	Tl1Sr1.9Ca0.1Yb1Cu2O7	Tl	1	Sr	1.9	Ca	0.1	Yb	1	Cu	2											O	7			1996																												Tl1212				3.799		11.979																	5																																																																																																Sr2CuO3,CaO,Yb2O3,Cu),Tl2O3	1	excess Tl2O3 were added, mixture-heat(910-930C, 9-12H in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
6875	PHC2690339		ErBa2Cu3O7	Er1Ba2Cu3Oz	Er	1	Ba	2	Cu	3															O	z		3	1996																												Y123																																					microwave magnets absorption		140	430																																																																															Er2O3(Ho2O3),BaCo3,CuO		R:Ba:Cu=3:6:11, mixture-SIN(900-910C,15H)-heat(1030 in O2),self flux method					Microwave magnetoabsorptions of ErBa2Cu3Oy and HoBa2Cu3Oy single crystals			Department of Materials,Science,University of Osaka Prefecture,Sakai,Osaka 593,Japan	Physica.C,269(1996)339-342	A.D. Caplim,Kimihito Tagaya,L. Cohen,Nobuo Fukuoka,Takahiro Shibayama,Takayuki Yokoo	Er, Ba, Cu, O, Ho	
6876	PHC2690339		HoBa2Cu3O7	Ho1Ba2Cu3Oz	Ho	1	Ba	2	Cu	3															O	z		3	1996																												Y123																																					microwave magnets absorption		150	430																																																																															Er2O3(Ho2O3),BaCo3,CuO		R:Ba:Cu=3:6:11, mixture-SIN(900-910C,15H)-heat(1030 in O2),self flux method					Microwave magnetoabsorptions of ErBa2Cu3Oy and HoBa2Cu3Oy single crystals			Department of Materials,Science,University of Osaka Prefecture,Sakai,Osaka 593,Japan	Physica.C,269(1996)339-342	A.D. Caplim,Kimihito Tagaya,L. Cohen,Nobuo Fukuoka,Takahiro Shibayama,Takayuki Yokoo	Er, Ba, Cu, O, Ho	
6877	PHC2690231	RT=275K	NdBa2Cu3O7	Nd1Ba2Cu3O6.93	Nd	1	Ba	2	Cu	3															O	7-z	6.93		1996																											3	Y123	Pmmm			3.87	3.918	11.763														91.5					91.5																																																																																		1.6												Nd2O3,BaCO3,CuO,Pr6O11,CaCO3	1	tablet-CAL(900C,920C)-pellet-ANN(460C,3days in flowing O2)-cool to RT (10C/H)					Neutron-diffraction studies and interatomic distances in Ca-Pr doped NdBa2Cu3O7-z			Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm Sweden	Physica.C,269(1996)231-241	"C. Tengroth,O"". Rapp,P. Lundqvist,R. Tellgren,Z. Hegedu""s"	Nd, Ba, Cu, O, Ca, Pr	
6878	PHC2690231	RT=275K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.95Ca0.025Pr0.025Ba2Cu3O6.95	Nd	0.95	Ca	0.025	Pr	0.025	Ba	2	Cu	3											O	7-z	6.95		1996																											3	Y123				3.871	3.917	11.761														86.1					86.1																																																																																		1.66												Nd2O3,BaCO3,CuO,Pr6O11,CaCO3	1	tablet-CAL(900C,920C)-pellet-ANN(460C,3days in flowing O2)-cool to RT (10C/H)					Neutron-diffraction studies and interatomic distances in Ca-Pr doped NdBa2Cu3O7-z			Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm Sweden	Physica.C,269(1996)231-241	"C. Tengroth,O"". Rapp,P. Lundqvist,R. Tellgren,Z. Hegedu""s"	Nd, Ba, Cu, O, Ca, Pr	
6879	PHC2690231	RT=275K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.9Ca0.05Pr0.05Ba2Cu3O6.95	Nd	0.9	Ca	0.05	Pr	0.05	Ba	2	Cu	3											O	7-z	6.95		1996																											3	Y123				3.871	3.916	11.755														81.4					81.4																																																																																		1.87												Nd2O3,BaCO3,CuO,Pr6O11,CaCO3	1	tablet-CAL(900C,920C)-pellet-ANN(460C,3days in flowing O2)-cool to RT (10C/H)					Neutron-diffraction studies and interatomic distances in Ca-Pr doped NdBa2Cu3O7-z			Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm Sweden	Physica.C,269(1996)231-241	"C. Tengroth,O"". Rapp,P. Lundqvist,R. Tellgren,Z. Hegedu""s"	Nd, Ba, Cu, O, Ca, Pr	
6880	PHC2690231	RT=275K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.8Ca0.1Pr0.1Ba2Cu3O7.02	Nd	0.8	Ca	0.1	Pr	0.1	Ba	2	Cu	3											O	7-z	7.02		1996																											3	Y123				3.872	3.913	11.747														70.8					70.8																																																																																		2.91												Nd2O3,BaCO3,CuO,Pr6O11,CaCO3	1	tablet-CAL(900C,920C)-pellet-ANN(460C,3days in flowing O2)-cool to RT (10C/H)					Neutron-diffraction studies and interatomic distances in Ca-Pr doped NdBa2Cu3O7-z			Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm Sweden	Physica.C,269(1996)231-241	"C. Tengroth,O"". Rapp,P. Lundqvist,R. Tellgren,Z. Hegedu""s"	Nd, Ba, Cu, O, Ca, Pr	
6881	NAT3430444	Npenet=100 micron meter	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990																												Bi2212																				85					85																																									micron.m				100																																						0.15	6800												see					Direct evidence for a very large penetration depth in superconducying BiSr2CaCu3O8 singl crystals			Institute of Physics of the University. PO Box 304,41000 Zagreb, Yugoslavia	NATURE.343(1990)444	B. Keszei,J.R. Cooper,L. Forro'	Bi, Sr, Ca, Cu, O	
6882	MPL0091387	in purity=CaWOz	(Bi,Pb,W)2Sr2Ca2Cu3Oz	Bi1.6Pb0.3W0.1Sr2Ca2Cu3Oz	Bi	1.6	Pb	0.3	W	0.1	Sr	2	Ca	2	Cu	3									O	z			1995																												Bi2223																					108				108													800																					HIR6882																																																														see Mat.Sci. and Engg.B23,137(1994)					MAGNETIC RELAXATION, LOWER CRITICAL FIELD AND IRREVERSIBILITY LINE OF W DEPED(Bi, PB)-2223 SUPERCONDUCTOR			Department of Physics, Osmania University, Hederabad 500 007, India	Mod.Phys.Lett.B,9(1995)1387-1396	D. SURESH BABU,G. NARSINGA RAO,M. GANNE,P. MOLINIE	Bi, Pb, W, Sr, Ca, Cu, O	
6883	MPL0091027	semi-con like	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z			1995																												T																							4.2																																																																								TP6883																								Nd2O3, CuO, CeO2	1	mixture-CAL(950C,17H in air)-prllet-SIN(1100C,24H)					THERMOELECTRIC POWER IN Nd1.85Ce0.15CuO4-y			Department of Physics, University of Science and Technology of China, Hefei 230026, China	Mod.Phys.Lett.B,9(1995)1027-1031	K.Q. RUAN,L.Z. CAO,M. DENG,N.L. WANG,R.P. WANG,W. ZHOU,Y. CHONG	Nd, Ce, Cu, O	
6884	MPL0091027		(Nd,Ce)2CuO4	Nd185Ce0.15Cu1O4-z	Nd	185	Ce	0.15	Cu	1															O	4-z			1995																												T																					15				15																																																																						TP6884																								Nd2O3, CuO, CeO2	1	as-grown(6883)-ANN(950,7H in N2)					THERMOELECTRIC POWER IN Nd1.85Ce0.15CuO4-y			Department of Physics, University of Science and Technology of China, Hefei 230026, China	Mod.Phys.Lett.B,9(1995)1027-1031	K.Q. RUAN,L.Z. CAO,M. DENG,N.L. WANG,R.P. WANG,W. ZHOU,Y. CHONG	Nd, Ce, Cu, O	
6885	MPL0091027		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z			1995																												T																					20				20																																																																						TP6885																								Nd2O3, CuO, CeO2	1	as-grown(6883)-ANN(950C,42H in N2)					THERMOELECTRIC POWER IN Nd1.85Ce0.15CuO4-y			Department of Physics, University of Science and Technology of China, Hefei 230026, China	Mod.Phys.Lett.B,9(1995)1027-1031	K.Q. RUAN,L.Z. CAO,M. DENG,N.L. WANG,R.P. WANG,W. ZHOU,Y. CHONG	Nd, Ce, Cu, O	
6886	MPL0091027	semi-con like	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z			1995																												T																							4.2																																																																								TP6886																								Nd2O3, CuO, CeO2	1	as-grown(6883)-ANN(950C,17H in O2)					THERMOELECTRIC POWER IN Nd1.85Ce0.15CuO4-y			Department of Physics, University of Science and Technology of China, Hefei 230026, China	Mod.Phys.Lett.B,9(1995)1027-1031	K.Q. RUAN,L.Z. CAO,M. DENG,N.L. WANG,R.P. WANG,W. ZHOU,Y. CHONG	Nd, Ce, Cu, O	
6887	MPL0090805	neariy single phase	(Y,Ca)2Ba4Cu7Oz	Y1.8Ca0.2Ba4Cu7Oz	Y	1.8	Ca	0.2	Ba	4	Cu	7													O	z			1995																												Y247				3.84	3.87	50.5														78					78																																																																																														Y2O3, BaCO3, CaCO3, CuO	1	mixture-CAL(940C,10H in air)-pellet-SIN(940C,20H in air)-FC to RT					ENHANCEMENT OF Tc IN Y2Ba4Cu7O14+y BY CaDOPING			Department of Physics, Anna University Madras 600 025, India	Mod,Phys.Lett.B,9(1995)805-810	K. JEYABALAN,R. ASOKAMANI,S. NATARAJAN,S. RAVIKUMAR	Ca, Y, Ba, Cu, O	
6888	MPL0090805	nearly single phase	(Y,Ca)2Ba4Cu7Oz	Y1.6Ca0.4Ba4Cu7Oz	Y	1.6	Ca	0.4	Ba	4	Cu	7													O	z			1995																												Y247				3.85	3.87	50.4														73					73																																																																																														Y2O3, BaCO3, CaCO3, CuO	1	mixture-CAL(940C,10H in air)-pellet-SIN(940C,20H in air)-FC to RT					ENHANCEMENT OF Tc IN Y2Ba4Cu7O14+y BY CaDOPING			Department of Physics, Anna University Madras 600 025, India	Mod,Phys.Lett.B,9(1995)805-810	K. JEYABALAN,R. ASOKAMANI,S. NATARAJAN,S. RAVIKUMAR	Ca, Y, Ba, Cu, O	
6889	MPL0090805	nearly single phase	(Y,Ca)2Ba4Cu7Oz	Y1Ca1Ba4Cu7Oz	Y	1	Ca	1	Ba	4	Cu	7													O	z			1995																												Y247				3.86	3.86	50.47														53					53																																																																																														Y2O3, BaCO3, CaCO3, CuO	1	mixture-CAL(940C,10H in air)-pellet-SIN(940C,20H in air)-FC to RT					ENHANCEMENT OF Tc IN Y2Ba4Cu7O14+y BY CaDOPING			Department of Physics, Anna University Madras 600 025, India	Mod,Phys.Lett.B,9(1995)805-810	K. JEYABALAN,R. ASOKAMANI,S. NATARAJAN,S. RAVIKUMAR	Ca, Y, Ba, Cu, O	
6890	JPS0652764	Tc is maximen value at 3GPa, not S/C at atm. resistivity proportional to T^2 between 20 and 70K 	(Sr,Ca)14Cu24O41	Sr0.4Ca13.6Cu24O41.84	Sr	0.4	Ca	13.6	Cu	24															O	41.84	41.84		1996																											3	LAD																			8	10	12		0		10																																																																																														SrCO3, CaCO3, CuO		mixture-CAL(1000C,50H in flowing O2)-pellet-SIN(1200C,8H in 20%O2+80%Ar of 2000 atm using HIP)					Superconductivity in the Ladder Material Sr0.4Ca13.6Cu24O41.84	199609		Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157	J.Phys.Soc.Japan,65(1996)2764-2767	Hiroki TAKAHASHI,Jun AKIMITSU,Kyoichi KINOSHITA,Masatomo UEHARA,Nobuo MORI,Takashi NAGATA		
6891	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu4Oz	Bi	4	Sr	3	Ca	3	Cu	4													O	z		1	1995																											2							30.74													74			78			78																																																																																		4.19												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6892	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.975Fe0.025Oz	Bi	4	Sr	3	Ca	3	Cu	3.975	Fe	0.025											O	z		1	1995																											2							30.73													68			72			72																																																																																		4.26												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6893	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.95Fe0.05Oz	Bi	4	Sr	3	Ca	3	Cu	3.95	Fe	0.05											O	z		1	1995																											2							30.71													56			72			72																																																																																		6.07												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6894	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.9Fe1Oz	Bi	4	Sr	3	Ca	3	Cu	3.9	Fe	1											O	z			1995																											2							30.69													52			66			66																																																																																		6.5												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6895	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.8Fe0.2Oz	Bi	4	Sr	3	Ca	3	Cu	3.8	Fe	0.2											O	z			1995																											2							30.66													40			60			60																																																																																		10.13												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6896	JMP0090549		Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.7Fe0.3Oz	Bi	4	Sr	3	Ca	3	Cu	3.7	Fe	0.3											O	z			1995																											2							30.64													36			57			57																																																																																		11.55												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6897	JMP0090549		Bi4Sr3Ca3(Ca,Cr)4Oz	Bi4Sr3Ca3Cu3.975Cr0.025Oz	Bi	4	Sr	3	Ca	3	Cu	3.975	Cr	0.025											O	z			1995																											2							30.73													72			78			78																																																																																		5.55												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6898	JMP0090549		Bi4Sr3Ca3(Ca,Cr)4Oz	Bi4Sr3Ca3Cu3.95Cr0.05Oz	Bi	4	Sr	3	Ca	3	Cu	3.95	Cr	0.05											O	z			1995																											2							30.72													71			76			76																																																																																		7.72												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6899	JMP0090549		Bi4Sr3Ca3(Cu,Cr)4Oz	Bi4Sr3Ca3Cu3.9Cr0.1Oz	Bi	4	Sr	3	Ca	3	Cu	3.9	Cr	0.1											O	z			1995																											2							30.69													50			74			74																																																																																		8.11												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6900	JMP0090549		Bi4Sr3Ca3(Cu,Cr)4Oz	Bi4Sr3Ca3Cu3.8Cr0.2Oz	Bi	4	Sr	3	Ca	3	Cu	3.8	Cr	0.2											O	z			1995																											2							30.68													46			69			69																																																																																		10.98												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6901	JMP0090549		Bi4Sr3Ca3(Cu,Mn)4Oz	Bi4Sr3Ca3Cu3.975Mn0.025Oz	Bi	4	Sr	3	Ca	3	Cu	3.975	Mn	0.025											O	z			1995																											2							30.73													72			78			78																																																																																		4.85												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6902	JMP0090549		Bi4Sr3Ca3(Cu,Mn)4Oz	Bi4Sr3Ca3Cu3.95Mn0.05Oz	Bi	4	Sr	3	Ca	3	Cu	3.95	Mn	0.05											O	z			1995																											2							30.74													64			76			76																																																																																		5.04												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6903	JMP0090549		Bi4Sr3Ca3(Cu,Mn)4Oz	Bi4Sr3Ca3Cu3.9Mn0.1Oz	Bi	4	Sr	3	Ca	3	Cu	3.9	Mn	0.1											O	z			1995																											2							30.72													62			74			74																																																																																		5.38												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6904	JMP0090549		Bi4Sr3Ca3(Cu,Mn)4Oz	Bi4Sr3Ca3Cu3.8Mn0.2Oz	Bi	4	Sr	3	Ca	3	Cu	3.8	Mn	0.2											O	z			1995																											2							30.73													54			72			72																																																																																		5.62												Bi2O3, CuO, SrCO3, CaCO3, M-oxide		mixture-CAL(800C,24H)-melt(1000C,in Pt crucible for 15 mirutes-querch)-heat(820C,4days)-FC to RT					STRUCTURAL AND SUPERCONDUCTING PROPERTIES OF Bi4Sr3Ca3CuyOw AND Bi4Sr3Ca3Cu4-!<M!<Oz (M=Fe, Cr AND Mn) GRASS CERAMICS			School of Physics, University of Hyderabad, Hyderabad-500 134, India	Int.J.Mod.Phys.B,9(1995)549-561	E. Zacharias,R. Singh	Bi, Sr, Ca, Cu, Fe, Cr, Mn	
6905	MPL0090027	as-grown	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O5.92	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6-z	5.92	1	1995																											2	2126				3.821		19.55																	4.2																																																																																																La2O3,SrCO3,CaCO3,CaO	1	mixture-prefine(900C,24H)-pellet-heat(950C,20H)-cool to RT(100C/H)-oxidation(80C,in saturated KMn O4 aqueo us solution,0,1,10H)					Tc ENHANCEMENT OF La1.8Sr0.2CaCu2O6-%+ BY KMnO4 OXIDATION			national Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 10080,China	Mod.Phys.Lett.B,9(1995)27-29	F. WU,L.Q. CHEN,S.L. JIA,S.T. YANG,W.J. ZHU,Y.Z. HUANG,Z.X. ZHAO	La, Sr, Ca, Cu, O	
6906	MPL0090027	IH-oxidation	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O5.96	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6-z	5.96	1	1995																											2	2126				3.818		19.59															54				54																																																																																														La2O3,SrCO3,CaCO3,CaO	1	mixture-prefine(900C,24H)-pellet-heat(950C,20H)-cool to RT(100C/H)-oxidation(80C,in saturated KMn O4 aqueo us solution,0,1,10H)					Tc ENHANCEMENT OF La1.8Sr0.2CaCu2O6-%+ BY KMnO4 OXIDATION			national Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 10080,China	Mod.Phys.Lett.B,9(1995)27-29	F. WU,L.Q. CHEN,S.L. JIA,S.T. YANG,W.J. ZHU,Y.Z. HUANG,Z.X. ZHAO	La, Sr, Ca, Cu, O	
6907	MPL0090027	10H-oxdation	(La,Sr)2CaCu2O6	La1.8Sr0.2Ca1Cu2O5.98	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6-z	5.98	1	1995																											2	2126				3.814		19.62															60				60																																																																																														La2O3,SrCO3,CaCO3,CaO	1	mixture-prefine(900C,24H)-pellet-heat(950C,20H)-cool to RT(100C/H)-oxidation(80C,in saturated KMn O4 aqueo us solution,0,1,10H)					Tc ENHANCEMENT OF La1.8Sr0.2CaCu2O6-%+ BY KMnO4 OXIDATION			national Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 10080,China	Mod.Phys.Lett.B,9(1995)27-29	F. WU,L.Q. CHEN,S.L. JIA,S.T. YANG,W.J. ZHU,Y.Z. HUANG,Z.X. ZHAO	La, Sr, Ca, Cu, O	
6908	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.96B0.04O5	Sr	2	Cu	1	C	0.96	B	0.04													O	5			1996																												SrCuO3																						7			7																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6909	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.95B0.05O5	Sr	2	Cu	1	C	0.95	B	0.05													O	5			1996																												Sr2CuO3																						12.5			12.5																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6910	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.94B0.06O5	Sr	2	Cu	1	C	0.94	B	0.06													O	5			1996																												SrCuO3																						21			21																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6911	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.93B0.07O5	Sr	2	Cu	1	C	0.93	B	0.07													O	5			1996																												SrCuO3																						23			23																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6912	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.92B0.08O5	Sr	2	Cu	1	C	0.92	B	0.08													O	5			1996																												SrCuO3																						25			25																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6913	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.91B0.09O5	Sr	2	Cu	1	C	0.91	B	0.09													O	5			1996																												SrCuO3																						26.5			26.5																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6914	PHC2630344	low temp phase	Sr2CuO2(CO3,BO3)	Sr2Cu1C1O5	Sr	2	Cu	1	C	1															O	5			1996								285																			2	SrCuO3				7.811		14.992																																																																																																																	SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6915	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.985B0.015O5	Sr	2	Cu	1	C	0.985	B	0.015													O	5			1996								210																				Sr2CuO3																																																																																																																							SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6916	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.983B0.018O5	Sr	2	Cu	1	C	0.983	B	0.018													O	5			1996								170																				SrCuO3																																																																																																																							SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6917	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.973B0.027O5	Sr	2	Cu	1	C	0.973	B	0.027													O	5			1996								20																				SrCuO3																																																																																																																							SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6918	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.82B0.12O5	Sr	2	Cu	1	C	0.82	B	0.12													O	5			1996																												SrCuO3																						30			30																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6919	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.86B0.14O5	Sr	2	Cu	1	C	0.86	B	0.14													O	5			1996																												SrCuO3																						31			31																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6920	PHC2630344		Sr2CuO2(CO3,BO3)	Sr2Cu1C0.85B0.15O5	Sr	2	Cu	1	C	0.85	B	0.15													O	5			1996																												SrCuO3																						32			32																																																																																														SrCo3,CuO,H3BO3		mixture-CAL(900C,20H in flowihg gas of 98% O2+2% CO3)-Q to RT					The phase diagram of the new superconductor Sr2CuO(CO3)1-x(BO3)x			Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Physica.C,263(1996)344-348	A. Yamashita,H. Nakata,H. Okajima,J. Akimitsu,S. Katano,T. Yokoo		
6921	PHC2620266		RSr2Cu2NbO7	Y1Sr2Cu2Nb1O7+z	Y	1	Sr	2	Cu	2	Nb	1													O	7+z		1	1996						0.728	-10.6																				3	1212	1mcm			5.534	5.63	22.751																13			13																																																																																														Pr6O11,SrCO3,Nb2O5,CuO	1	mixture-heat(1020C,72H)-pellet-SIN(1050C,in flowing O2)-slow cool to RT					Synthesis, superconductivity and magnetism of RSr2Cu2NbO7+z compounds (R=Y, Pr and Gd)	05		Tata Institute of Fundamental Research, Bombay 400 005, India	Physica.C,262(1996)266-271	Latika Menon,S.K. Malik,V.P.S. Awana	Y, Pr, Gd, Sr, Cu, Nd, O	
6922	PHC2620266		RSr2Cu2NbO7	Pr1Sr2Cu2Nb1O7+z	Pr	1	Sr	2	Cu	2	Nb	1													O	7+z		1	1996						3.11	-4																				3	1212				5.512	5.64	22.803																	1.8																																																																																																Pr6O11,SrCO3,Nb2O5,CuO	1	mixture-heat(1020C,72H)-pellet-SIN(1050C,in flowing O2)-slow cool to RT					Synthesis, superconductivity and magnetism of RSr2Cu2NbO7+z compounds (R=Y, Pr and Gd)	05		Tata Institute of Fundamental Research, Bombay 400 005, India	Physica.C,262(1996)266-271	Latika Menon,S.K. Malik,V.P.S. Awana	Y, Pr, Gd, Sr, Cu, Nd, O	
6923	PHC2620266		RSr2Cu2NbO7	Gd1Sr2Cu2Nb1O7+z	Gd	1	Sr	2	Cu	2	Nb	1													O	7+z		1	1996						7.5	-2.74	2.2																			3	1212				5.506	5.638	22.774																	1.8																																																																																																Pr6O11,SrCO3,Nb2O5,CuO	1	mixture-heat(1020C,72H)-pellet-SIN(1050C,in flowing O2)-slow cool to RT					Synthesis, superconductivity and magnetism of RSr2Cu2NbO7+z compounds (R=Y, Pr and Gd)	05		Tata Institute of Fundamental Research, Bombay 400 005, India	Physica.C,262(1996)266-271	Latika Menon,S.K. Malik,V.P.S. Awana	Y, Pr, Gd, Sr, Cu, Nd, O	
6924	PHC2620159	impurity phase=Sr4Tl2O6CO3,SrCO3	Tl3(CrO4)Sr8Cu4O16	Tl3Cr1Sr8Cu4O20	Tl	3	Cr	1	Sr	8	Cu	4													O	20			1996																											3	Tl1212				3.78	15.257	17.674															30	25			25																																																																																														SrO2,CuO,TlO3,Cr2O3		nominal(Tl:Cr=3:1),mixture-sealed in alumina crucible in evacuated silica ampoule-heat(920C,6H)-Quench to RT					Neutron diffaraction structure determination of the superconducting copper oxychromate Tl(CrO4)Sr8Cu4O16	05		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen,Bd du Mare'chal Juin,14050 Caen Cdex, France	Physica.C,262(1996)159-167	B. Raveau,C. Martin,C. Michel,F. Letouze',M. Hervieu	TL, Cr, O, Sr, Cu, O	
6925	JJP0330583	monoclinic-distorted-defect perovskite	Ca2NbO4	Ca2Nb1O4	Ca	2	Nb	1																	O	4			1994																																																		8.9			8.9																																																																																																heat(1075C,24H)-(1125C,24H)					A2Nb1+xOy(A=Ca,Sr)(O<x<5): New Reduced Niobate Superconductors with the Distored Defect-Perovskite Structure	199404			Jpn.J.Appl.Phys.Lett.,33(1994)L583-586	Akio Nakamura	Ca,Sr,Nb,O	
6926	PHC2620279		(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.5Cu0.5Sr2Ca1.9Y0.1Cu3O9.3	Ge	0.5	Cu	0.5	Sr	2	Ca	1.9	Y	0.1	Cu	3									O	9.3			1996																											2	M1223																			73		90				81.5																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6927	PHC2620279		(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.5Cu0.5Sr2Ca1.8Y0.2Cu3O9.3	Ge	0.5	Cu	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	9.3			1996																											2	M1223				3.831		14.533																77			77																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6928	PHC2620279	lower transition at 50K	(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.5Cu0.5Sr2Ca1.7Y0.3Cu3O9.3	Ge	0.5	Cu	0.5	Sr	2	Ca	1.7	Y	0.3	Cu	3									O	9.3			1996																											2	M1223																						73			73																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6929	PHC2620279		(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.4Cu0.6Sr2Ca1.9Y0.1Cu3O9.3	Ge	0.4	Cu	0.6	Sr	2	Ca	1.9	Y	0.1	Cu	3									O	9.3			1996																											2	M1223																						90			90																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6930	PHC2620279		(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.4Cu0.6Sr2Ca1.8Y0.2Cu3O9.3	Ge	0.4	Cu	0.6	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	9.3			1996																											2	M1223				3.83		14.582																81			81																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6931	PHC2620279	lower transition at 4OK	(Ge,Cu)Sr2(Ca,Y)2Cu3O9	Ge0.4Cu0.6Sr2Ca1.7Y0.3Cu3O9.3	Ge	0.4	Cu	0.6	Sr	2	Ca	1.7	Y	0.3	Cu	3									O	9.3			1996																											2	M1223																						77			77																																																																																														GeO2,CuO,SrCuO2,SrO2,Y2O3,CaCuO3		mixture-sealed in Au capsuee-react in a belt-type high pressure apporatus (6GPa,1300C,IH)-Quench to RT					New high-T superconductor,(Ge,Cu1-z)Sr2Ca2-xYCu3Oy ((Ge,Cu)-1223) prepared under high pressure	05		National Insititute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki,305 Japan	Physica.C,262(1996)279-284	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui	Ge, Cu, Sr, Ca, Y, Cu, O	
6932	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.025	Hg	1	Ba	2	Cu	1															O	4+z	4.025	1	1996																												Hg1201				3.8888		9.533																20			20																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6933	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.045	Hg	1	Ba	2	Cu	1															O	4+z	4.045	1	1996																												Hg1201																						73			73																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6934	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.055	Hg	1	Ba	2	Cu	1															O	4+z	4.055	1	1996																												Hg1201				3.8814		9.5243																80			80																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6935	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.08	Hg	1	Ba	2	Cu	1															O	4+z	4.08	1	1996																												Hg1201				3.88		9.5217																85			85																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6936	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.085	Hg	1	Ba	2	Cu	1															O	4+z	4.085	1	1996																												Hg1201				3.879		9.5124																92			92																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6937	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.09	Hg	1	Ba	2	Cu	1															O	4+z	4.09	1	1996																												Hg1201				3.8753		9.512																97			97																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6938	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.1	Hg	1	Ba	2	Cu	1															O	4+z	4.1	1	1996																											2	Hg1201				3.8732		9.5109																92			92																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6939	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.12	Hg	1	Ba	2	Cu	1															O	4+z	4.12	1	1996																											2	Hg1201				3.8701		9.5078																71			71																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6940	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O4.13	Hg	1	Ba	2	Cu	1															O	4+z	4.13	1	1996																											2	Hg1201				3.8698		9.5048																60			60																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6941	PHC2650013		HgBa2CuOz	Hg1Ba2Cu1O6.932	Hg	1	Ba	2	Cu	1															O	4+z	6.932	1	1996																											2	Hg1201				3.8676		9.4989																50			50																																																																																														HgO,NaO,CuO	1	mixture-pellet-seal in quartz tube-SIN(700C,2.5H),diflerent annealing condition for various oxygen content					Dependence of superconducting properties on the Cu-valence determined by iodometry in HgBa2CuO4+z	07		Superconductivity Research Laboratory,International Superconductivity Technology Center,10-13 Shinonome,1-Chome Koto-ku,Tokyo 135, Japan	Physica.C,265(1996)13-18	A. Fukuoka,A. Tokiwa-Yamamoto,H. Yamauchi,K. Tanabe,M. Itoh,R. Usami,S. Adachi	Hg, Ba, Cu, O	
6942	PHC2640255		(Y,Ca)Ba2Cu3O7	Y0.98Ca0.02Ba2Cu3O7-z	Y	0.98	Ca	0.02	Ba	2	Cu	3													O	7-z			1996																											3	Y123																				86.4					86.4																																																																																														Y2O3,BaCO3,CaCO3,CuO	1	mixture-CAL(900C)-SIN(940C,48H)-ANN(940C,in flowing O2)-ANN(700C,12H)-slow cool to RT					Fluctuation-induced conductivity of polycrystalline Y1-xCaxBa2Cu3O7-z superconductors	6		Condensed Matter Physics Research Centre, Department of Physics,Jadaupur University, Calcutta-700 064, India	Physica.C,264(1996)255-260	A.K. Ghosh,A.N. Basu,P. Barat,Pintu Sen,S.K. Bandyopadhyay	Y, Ca, Ba, Cu, O	
6943	PHC2640255		(Y,Ca)Ba2Cu3O7	Y0.95Ca0.05Ba2Cu3O7-z	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	7-z			1996																											3	Y123																				88.5					88.5																																																																																														Y2O3,BaCO3,CaCO3,CuO	1	mixture-CAL(900C)-SIN(940C,48H)-ANN(940C,in flowing O2)-ANN(700C,12H)-slow cool to RT					Fluctuation-induced conductivity of polycrystalline Y1-xCaxBa2Cu3O7-z superconductors	6		Condensed Matter Physics Research Centre, Department of Physics,Jadaupur University, Calcutta-700 064, India	Physica.C,264(1996)255-260	A.K. Ghosh,A.N. Basu,P. Barat,Pintu Sen,S.K. Bandyopadhyay	Y, Ca, Ba, Cu, O	
6944	PHC2640255		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Cu3O7-z	Y	0.9	Ca	0.1	Cu	3															O	7-z			1996																											3	Y123																				84.4					84.4																																																																																														Y2O3,BaCO3,CaCO3,CuO	1	mixture-CAL(900C)-SIN(940C,48H)-ANN(940C,in flowing O2)-ANN(700C,12H)-slow cool to RT					Fluctuation-induced conductivity of polycrystalline Y1-xCaxBa2Cu3O7-z superconductors	6		Condensed Matter Physics Research Centre, Department of Physics,Jadaupur University, Calcutta-700 064, India	Physica.C,264(1996)255-260	A.K. Ghosh,A.N. Basu,P. Barat,Pintu Sen,S.K. Bandyopadhyay	Y, Ca, Ba, Cu, O	
6945	PHC2640255		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O7-z	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z			1996																											3	Y123																				72.9					72.9																																																																																														Y2O3,BaCO3,CaCO3,CuO	1	mixture-CAL(900C)-SIN(940C,48H)-ANN(940C,in flowing O2)-ANN(700C,12H)-slow cool to RT					Fluctuation-induced conductivity of polycrystalline Y1-xCaxBa2Cu3O7-z superconductors	6		Condensed Matter Physics Research Centre, Department of Physics,Jadaupur University, Calcutta-700 064, India	Physica.C,264(1996)255-260	A.K. Ghosh,A.N. Basu,P. Barat,Pintu Sen,S.K. Bandyopadhyay	Y, Ca, Ba, Cu, O	
6946	PHC2660215	as-prepased	(C,Cu)Ba2Ca2Cu3Oz	C0.15Cu0.5Ba2Ca2Cu3Oz	C	0.15	Cu	0.5	Ba	2	Ca	2	Cu	3											O	z			1996																											2	C1223				3.858		14.766																66			66																																																																																																precursor(Ba2Ca2Cu4Oz)+AgO as a oxidiqihg aqent-react (1100C,0.5H at P=8GPa)					Enhancement of Tc of CyCu1-yBa2Ca2Cu3Ox from 67K to 120K by reduction treatments	08		Laboratoire de Cristallographie, CNRS-UJF, BP166, 38042 Grenoble cedex 9, France	Physica.C,266(1996)215-222	A. Sulpice,C. Acha,C. Chaillout,E. Gautier,J.L. Tholence,M. Marezio,P. Bordet,S.Le Floch,Y. Feng	C, Cu, Ba, Ca, O	
6947	PHC2660215		(C,Cu)Ba2Cu3Oz	C0.15Cu0.5Ba2Ca2Cu3Oz	C	0.15	Cu	0.5	Ba	2	Ca	2	Cu	3											O	z			1996																											2	C1223				3.862		14.78																88			88																																																																																																precursor(Ba2Ca2Cu4Oz)+AgO as a oxidiqihg aqent-react (1100C,0.5H at P=8GPa)					Enhancement of Tc of CyCu1-yBa2Ca2Cu3Ox from 67K to 120K by reduction treatments	08		Laboratoire de Cristallographie, CNRS-UJF, BP166, 38042 Grenoble cedex 9, France	Physica.C,266(1996)215-222	A. Sulpice,C. Acha,C. Chaillout,E. Gautier,J.L. Tholence,M. Marezio,P. Bordet,S.Le Floch,Y. Feng	C, Cu, Ba, Ca, O	
6948	PHC2660215		(C,Cu)Ba2Ca2Cu3Oz	C0.5Cu0.5Ba2Ca2Cu3Oz	C	0.5	Cu	0.5	Ba	2	Ca	2	Cu	3											O	z			1996																											2	C1223				3.862		14.807																118			118																																																																																																precursor(Ba2Ca2Cu4Oz)+AgO as a oxidiqihg aqent-react (1100C,0.5H at P=8GPa)					Enhancement of Tc of CyCu1-yBa2Ca2Cu3Ox from 67K to 120K by reduction treatments	08		Laboratoire de Cristallographie, CNRS-UJF, BP166, 38042 Grenoble cedex 9, France	Physica.C,266(1996)215-222	A. Sulpice,C. Acha,C. Chaillout,E. Gautier,J.L. Tholence,M. Marezio,P. Bordet,S.Le Floch,Y. Feng	C, Cu, Ba, Ca, O	
6949	PHC2660215		(C,Cu)Ba2Ca2Cu3Oz	C0.5Cu0.5Ba2Ca2Cu3Oz	C	0.5	Cu	0.5	Ba	2	Ca	2	Cu	3											O	z			1996																											2	C1223				3.863		14.823																120			120																																																																																																precursor(Ba2Ca2Cu4Oz)+AgO as a oxidiqihg aqent-react (1100C,0.5H at P=8GPa)					Enhancement of Tc of CyCu1-yBa2Ca2Cu3Ox from 67K to 120K by reduction treatments	08		Laboratoire de Cristallographie, CNRS-UJF, BP166, 38042 Grenoble cedex 9, France	Physica.C,266(1996)215-222	A. Sulpice,C. Acha,C. Chaillout,E. Gautier,J.L. Tholence,M. Marezio,P. Bordet,S.Le Floch,Y. Feng	C, Cu, Ba, Ca, O	
6950	PHC2660191		(Ca,Na)2CuO2Cl2	Ca2Cu1Cl2O2	Ca	2	Cu	1	Cl	2															O	2			1996																											2	T				3.869		15.049																	5																																																																																																CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6951	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.92Na0.08Cu1Cl2O2	Ca	1.92	Na	0.08	Cu	1	Cl	2													O	2			1996																											2	T																							5																																																																																																CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6952	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.88Na0.12Cu1Cl2O2	Ca	1.88	Na	0.12	Cu	1	Cl	2													O	2			1996																											2	T				3.85		15.153																7.2			7.2																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6953	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.84Na0.16Cu1Cl2O2	Ca	1.84	Na	0.16	Cu	1	Cl	2													O	2			1996																											2	T																						19.7			19.7																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6954	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.76Na0.24Cu1Cl2O2	Ca	1.76	Na	0.24	Cu	1	Cl	2													O	2			1996																											2	T				3.846		15.186																26.9			26.9																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6955	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.7Na0.3Cu1Cl2O2	Ca	1.7	Na	0.3	Cu	1	Cl	2													O	2			1996																											2	T																						27.5			27.5																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6956	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.6Na0.4Cu1Cl2O2	Ca	1.6	Na	0.4	Cu	1	Cl	2													O	2			1996																											2	T																						27.8			27.8																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6957	PHC2660191		(Ca,Na)2CuO2Cl2	Ca1.5Na0.5Cu1Cl2O2	Ca	1.5	Na	0.5	Cu	1	Cl	2													O	2			1996																											2	T				3.842		15.18																28.5			28.5																																																																																														CaCl2,CaO,CuO,Na2O2,NaClO4		mixture-pellet-CAL(1073K,in N2 flow),addition of diferent ratio of Na2O2/NaClO4,-heat(1073-1173K,30min,at 6GPa)inpurity phase=Ca(OH)2.Call2.H2O					Synthesis, Structure, and superconductivity of Ca2-xNaxCuO2Cl2	08		Institute for Chemical Research, Kyoto University,Uji, Kyoto-fu  611, Japan	Physica.C,266(1996)191-202	M. Takano,N. Kobayashi,Z. Hiroi	Cu, Na, Cu, O, Cl	
6958	PHC2650323	insulator, no magnetic transition for T<300K	Ba2CuO2Cl2	Ba2Cu1Cl2O2	Ba	2	Cu	1	Cl	2															O	2		1	1996																											2	T	14/mmm			4.103		16.442																	4.2																																																																																																BaCl2,BaO2,Cu	1	mixture-pellet-wrapped in capsule-pressed at 6GPa using cubic anil type apparatus-heat(1000C,IH under 6GPa)					A new oxychloride, Ba2CuO2Cl2, prepared under high pressure	07		Superconductivity Research Laboratory, International Superconductivity Technology Center,10-13 Shinonome,1-chome,Koto-ku, Tokyo 135, Japan	Physica.C,265(1996)323-327	A. Tokiwa-Yamamoto,K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki,X.-J. Wu,Y. Moriwaki	Ba, Cu, O, Cl	
6959	PHC2650315		(Bi,In,Pb)Sr2(Gd,Ca)Cu2Oz	Bi0.28In0.52Pb0.2Sr2Gd0.6Ca0.4Cu2Oz	Bi	0.28	In	0.52	Pb	0.2	Sr	2	Gd	0.6	Ca	0.4	Cu	2							O	z		2	1996																											2	1212				3.829		11.762													10		30				20																																																																																		30													1	mixture-SIN(990C),small amount of Bi2212 phase is included					Synthesis, crystal structure and properties of In-containing 1212-type compounds	07		IRC in Superconductivity, University of Cambridge,Madinglay Road,Cambridge CB3 ONS,UK	Physica.C,265(1996)315-322	A. Kharlanov,J.P. Attfield	In, Bi, Pb, Sr, Gd, Ca, Cu, O	
6960	PHC2650315		(Bi,In,Pb)Sr2(Gd,Ca)Cu2Oz	Bi0.245In0.455Pb0.3Sr2Gd0.6Ca0.4Cu2Oz	Bi	0.245	In	0.455	Pb	0.3	Sr	2	Gd	0.6	Ca	0.4	Cu	2							O	z		2	1996																											2	1212				3.837		11.837													40		70				55																																																																																		60													1	mixture-SIN(990C),small amount of Bi2212 phase is included					Synthesis, crystal structure and properties of In-containing 1212-type compounds	07		IRC in Superconductivity, University of Cambridge,Madinglay Road,Cambridge CB3 ONS,UK	Physica.C,265(1996)315-322	A. Kharlanov,J.P. Attfield	In, Bi, Pb, Sr, Gd, Ca, Cu, O	
6961	PHC2650315		(Bi,In,Pb)Sr2(Gd,Ca)Cu2Oz	Bi0.21In0.39Pb0.4Sr2Gd0.6Ca0.4Cu2Oz	Bi	0.21	In	0.39	Pb	0.4	Sr	2	Gd	0.6	Ca	0.4	Cu	2							O	z		2	1996																											2	1212				3.835		11.858													45		70				57.5																																																																																		40													1	mixture-SIN(990C),small amount of Bi2212 phase is included					Synthesis, crystal structure and properties of In-containing 1212-type compounds	07		IRC in Superconductivity, University of Cambridge,Madinglay Road,Cambridge CB3 ONS,UK	Physica.C,265(1996)315-322	A. Kharlanov,J.P. Attfield	In, Bi, Pb, Sr, Gd, Ca, Cu, O	
6962	PHC2650315		(Bi,In,Pb)Sr2(Gd,Ca)Cu2Oz	Bi0.175In0.325Pb0.5Sr2Gd0.6Ca0.4Cu2Oz	Bi	0.175	In	0.325	Pb	0.5	Sr	2	Gd	0.6	Ca	0.4	Cu	2							O	z		2	1996																											2	1212				3.835		11.872													40		75				57.5																																																																																		30													1	mixture-SIN(990C),small amount of Bi2212 phase is included					Synthesis, crystal structure and properties of In-containing 1212-type compounds	07		IRC in Superconductivity, University of Cambridge,Madinglay Road,Cambridge CB3 ONS,UK	Physica.C,265(1996)315-322	A. Kharlanov,J.P. Attfield	In, Bi, Pb, Sr, Gd, Ca, Cu, O	
6963	PR05403580		(Nd,Ca)Ba2Cu3O7	Nd0.9Ca0.1Ba2Cu3O7-z	Nd	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z		1	1996																											3	Y123				3.854	3.911	11.723														86					86																																																																																										7	RH6963			R2O3,BaCO3,CaCo3,CuO	1	mixture-CAL(915,24H in air in Al2O3 crucible)-pellet-heat(925-935C,3days in flowing O2)-ANN(680C,10H)-slow cool to 420C-hold(20H)-slow cool to RT					Ion-size effect on transport properties in R0.9Ca0.1Ba2Cu3O7-z systems(R=Tm,Ho,Gd,and Nd)	199608		Department of Physics, Tamkang University, Tamsui, Taiwan, Republic of China	Phys.Rev.B,54(1996)3580	J.C. Chen,S.H. Cheng,Weiyan Guan		
6964	PR05403580		(Gd,Ca)Ba2Cu3O7	Gd0.9Ca0.1Ba2Cu3O7-z	Gd	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z		1	1996																											3	Y123				3.83	3.889	11.683														88					88																																																																																										7	RH6964			R2O3,BaCO3,CaCo3,CuO	1	mixture-CAL(915,24H in air in Al2O3 crucible)-pellet-heat(925-935C,3days in flowing O2)-ANN(680C,10H)-slow cool to 420C-hold(20H)-slow cool to RT					Ion-size effect on transport properties in R0.9Ca0.1Ba2Cu3O7-z systems(R=Tm,Ho,Gd,and Nd)	199608		Department of Physics, Tamkang University, Tamsui, Taiwan, Republic of China	Phys.Rev.B,54(1996)3580	J.C. Chen,S.H. Cheng,Weiyan Guan		
6965	PR05403580		(Ho,Ca)Ba2Cu3O7	Ho0.9Ca0.1Ba2Cu3O7-z	Ho	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z		1	1996																											3	Y123				3.815	3.878	11.661														89					89																																																																																										7	RH6965			R2O3,BaCO3,CaCo3,CuO	1	mixture-CAL(915,24H in air in Al2O3 crucible)-pellet-heat(925-935C,3days in flowing O2)-ANN(680C,10H)-slow cool to 420C-hold(20H)-slow cool to RT					Ion-size effect on transport properties in R0.9Ca0.1Ba2Cu3O7-z systems(R=Tm,Ho,Gd,and Nd)	199608		Department of Physics, Tamkang University, Tamsui, Taiwan, Republic of China	Phys.Rev.B,54(1996)3580	J.C. Chen,S.H. Cheng,Weiyan Guan		
6966	PR05403580		(Tm,Ca)Ba2Cu3O7	Tm0.9Ca0.1Ba2Cu3O7-z	Tm	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z		1	1996																											3	Y123				3.798	3.862	11.615														86					86																																																																																										7	RH6966			R2O3,BaCO3,CaCo3,CuO	1	mixture-CAL(915,24H in air in Al2O3 crucible)-pellet-heat(925-935C,3days in flowing O2)-ANN(680C,10H)-slow cool to 420C-hold(20H)-slow cool to RT					Ion-size effect on transport properties in R0.9Ca0.1Ba2Cu3O7-z systems(R=Tm,Ho,Gd,and Nd)	199608		Department of Physics, Tamkang University, Tamsui, Taiwan, Republic of China	Phys.Rev.B,54(1996)3580	J.C. Chen,S.H. Cheng,Weiyan Guan		
6967	PR05403610		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+-z	Nd	1.85	Ce	0.15	Cu	1															O	4+-z		4	1996																												T'																				22					22																					magneto resistivity	8									0.37								64																																																									C-axis oriented films were prepared by pulsed laser ablation					Magnetoresistivity of thin films of the electron-doped high-Tc superconductor Nd1.85Ce0.15 CuO4+_ z	199608		Department of Phsics and Institute for pure and Applisd Physical Sciences, University of California, San Diego,La Jolla, California 92093-0360	Phys.Rev.B,54(1996)3610	C.C. Almasan,J. Herrmann,M.B. Maple,M.C. de Andrade,R.P. Dikey		
6968	PHC2620177		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			1996																																																		85			85																																																																																																single crystal was grown in air using the travelling solvent floating zone technique					Thermal expansion,specific heat, and uniaxial pressure dependences of Tc in Bi2Sr2CaCu2)8+z	05		"II.Physikalisches Institut, Universita""t zu Ko""ln, Zu""lpicher Str.77,50937 Ko""ln, Germany"	Physica.C,262(1996)177-186	"A.A. Menovsky,B. Bu""chner,H. Kierspel,H. Winkelmann,J.J.M. Franse,N.T. Hien,T. Auweiler,V.H.M. Duijn,W. Schlabitz"	Bi, Sr, Ca, Cu, O	
6969	PR05311825	Pb0.26 Bi1.74 Sr1.85 Ca0.9 Cu1.95 O8+z by EPMA	(Pb,Bi)2Sr2CaCu2O8	Pb0.24Bi1.76Sr2Ca1Cu2O8+z	Pb	0.24	Bi	1.76	Sr	2	Ca	1	Cu	2											O	8+z		3	1996																												Bi2212																				68					68																																										magnetization	1900																																																					by a self-flux method in alumina crucible ANN(550-650C, 300 bar O2)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
6978	PR05404265	Hg1223=60%,Tc(max)=145K(at 25GPa)	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1996																												Hg1223																					135.5				135.5			K/GPa	0.65																																																																																												precursor(Ba2CaCu2O5+z)-mix with HgO-seale(in evacuated quartz tube)					Prwssure dependence of the superconducting critical temperature of HgBa2Ca2Cu3O8+y and HgBa2Ca3Cu4O10+y up to 30 GPa	199608		Department of Physics and Astronomy, Free University, De Boelelaan 1081,1081 HV Amsterdam, The Netherland	Phys.Rev.B,54(1996)4265	A. Schilling,D. Tristan Jover,H. Wilhelm,H.R. Ott,J.-J. Capponi,R. Griessen,R.J. Wijngaarden,S.M. Loureiro		
6979	PR05404265	Hg1223>95%, Tc(max)=142K(at25GPa),dtc/dp=2K/GPa at P=o	HgBa2Cu3O8+z	Hg1Ba2Ca2Cu3O1	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z	1		1996																												Hg1223																												K/GPa	0.64																																																																																												by a self-flux method in alumina crucible ANN(550-650C, in O2)					Prwssure dependence of the superconducting critical temperature of HgBa2Ca2Cu3O8+y and HgBa2Ca3Cu4O10+y up to 30 GPa	199608		Department of Physics and Astronomy, Free University, De Boelelaan 1081,1081 HV Amsterdam, The Netherland	Phys.Rev.B,54(1996)4265	A. Schilling,D. Tristan Jover,H. Wilhelm,H.R. Ott,J.-J. Capponi,R. Griessen,R.J. Wijngaarden,S.M. Loureiro		
6980	PR05404265	Hg1223>95%,Tc(max)=145K(at 8 GPa)	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1996																												Hg1223																					132.5				132.5			K/GPa	3																																																																																												by a self-flux method in alumina crucible ANN(550-650C, in O2)					Prwssure dependence of the superconducting critical temperature of HgBa2Ca2Cu3O8+y and HgBa2Ca3Cu4O10+y up to 30 GPa	199608		Department of Physics and Astronomy, Free University, De Boelelaan 1081,1081 HV Amsterdam, The Netherland	Phys.Rev.B,54(1996)4265	A. Schilling,D. Tristan Jover,H. Wilhelm,H.R. Ott,J.-J. Capponi,R. Griessen,R.J. Wijngaarden,S.M. Loureiro		
6981	PR05404265	Hg1234>80%, Tc(max)=122K (at20GPa)	HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O1	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z	1	2	1996																												Hg1234																					115				115			K/GPa	0.6																																																																																												by a self-flux method in alumina crucible ANN(550-650C, in O2)					Prwssure dependence of the superconducting critical temperature of HgBa2Ca2Cu3O8+y and HgBa2Ca3Cu4O10+y up to 30 GPa	199608		Department of Physics and Astronomy, Free University, De Boelelaan 1081,1081 HV Amsterdam, The Netherland	Phys.Rev.B,54(1996)4265	A. Schilling,D. Tristan Jover,H. Wilhelm,H.R. Ott,J.-J. Capponi,R. Griessen,R.J. Wijngaarden,S.M. Loureiro		
6982	PR05404265	Hg1234>90%, Yc(max)=122K (at 7GPa)	HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O2	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z	2	2	1996																												Hg1234																					115				115			K/GPa	1.2																																																																																												by a self-flux method in alumina crucible ANN(550-650C, in O2)					Prwssure dependence of the superconducting critical temperature of HgBa2Ca2Cu3O8+y and HgBa2Ca3Cu4O10+y up to 30 GPa	199608		Department of Physics and Astronomy, Free University, De Boelelaan 1081,1081 HV Amsterdam, The Netherland	Phys.Rev.B,54(1996)4265	A. Schilling,D. Tristan Jover,H. Wilhelm,H.R. Ott,J.-J. Capponi,R. Griessen,R.J. Wijngaarden,S.M. Loureiro		
6983	PR05406133	HC2(O) is estimated from HC2=32.2-1.8*T+0.025T, K-content not measured	(Ba,K)BiO3	Ba1K1Bi1O3	Ba	1	K	1	Bi	1															O	3		3	1996																												BKBO																				31.8					31.8																						32.2																																																																								KOH,Ba(OH)2 8H2O,Bi2O3		K:Ba:Bi=72:1:2					Positive curvature in the temperature dependence of Hc2 in KxBa1-xBiO3	199609		Institute of Solid State Physics RAS, 142432 Chernogolovka, Russia	Phys.Rev.B,54(1996)6133	A.K. Geim,G.E. Tsydynzhapov,L.A. Klinkova,N.V. Barkovskii,S. Wiegers,V.F. Gantmakher		
6984	PR05406122	single phase-film,Tc measured by surface resistance,12.92GHz	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		4	1996																												Y123																				92				20	92																																																																																																The film deposited on MgO at 1023K					Observation of superconductivity in PrBa2Cu3O7	199608		Department of Physics, University of Notre Dame,Notre Dame,Indiana 46556	Phys.Rev.B,54(1996)6122	A.E. Klunzinger,D.B. Chrisey,D.B. Pulling,H.A. Blackstead,J.S. Horwitz,John D. Dow,M.A. Black,P.J. McGinn		
6985	PR05406122	impurity=Pr2BaCuO5,Tc by ESR	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7			1996																												Y123																				92					92																																																																																																The powders were prepared in low oxygen environment					Observation of superconductivity in PrBa2Cu3O7	199608		Department of Physics, University of Notre Dame,Notre Dame,Indiana 46556	Phys.Rev.B,54(1996)6122	A.E. Klunzinger,D.B. Chrisey,D.B. Pulling,H.A. Blackstead,J.S. Horwitz,John D. Dow,M.A. Black,P.J. McGinn		
6986	PR05407449	under doping	Bi2(Sr,La)2CuO6	Bi2Sr2Cu1Oz	Bi	2	Sr	2	Cu	1															O	z		3	1996																												Bi2201						24.659														7					7																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6987	PR05407449	under doping	Bi2(Sr,La)2CuO6	Bi2Sr1.975La0.025Cu1Oz	Bi	2	Sr	1.975	La	0.025	Cu	1													O	z		3	1996																												Bi2201						24.668														11					11																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6988	PR05407449	optimal doping	Bi2(Sr,La)2CuO6	Bi2Sr1.95La0.05Cu1Oz	Bi	2	Sr	1.95	La	0.05	Cu	1													O	z		3	1996																												Bi2201						24.5														18					18																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6989	PR05407449	optimal doping	Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1Oz	Bi	2	Sr	1.9	La	0.1	Cu	1													O	z		3	1996																												Bi2201						24.478														18					18																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6990	PR05407449	optimal doping	Bi2(Sr,La)2CuO6	Bi2Sr1.8La0.2Cu1Oz	Bi	2	Sr	1.8	La	0.2	Cu	1													O	z		3	1996																												Bi2201						24.4														18					18																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6991	PR05407449	over doping	Bi2(Sr,La)2CuO6	Bi2Sr1.7La0.3Cu1Oz	Bi	2	Sr	1.7	La	0.3	Cu	1													O	z		3	1996																												Bi2201						24.328														10					10																																																																																														Bi2O3,SrCO3,La2O3,CuO		mixture-melt(1000-1060C depending on La-content,3H)-cool to 850-880C(1-2C/H)-FC to RT					Crystal growth and anisotrope resistivity of Bi2Sr2-xLaxCuOy	199609		"Institut fu""r Festko""rperphysik, Technische Hochschule Darmstadt,Hochshulstra%!e 8,D-64289 Darmstadt, Germany"	Phys.Rev.B,54(1996)7449	B. Buschinger,C. Geibel,F. Steglich,N.L. Wang		
6992	PR05406885	size 12*2*2 mm,K=3.128+0.01104*T(W/mK)for 90<T	Bi2(Sr,Ca)2 CaCu2O8	Bi2Sr1.8Ca1.2Cu2O8	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	8		1	1996																												Bi2212																				79.8					79.8																																																																	THC6992					TP6992																									1	mixture-CAL-pellet-SIN(830C,3days in air)-quench to RT					Superconductivity fluctuation effects on the thermal conductivity of Bi2Sr2CaCuo8	199609		SUPRAS, Insitute ofPhysics, B5, University of Lie'ge, B-4000 Lie'ge, Belgium	Phys.Rev.B,54(1996)R6885	H. Bougrine,M. Ausloos,M. Houssa,R. Cloots,S. Stassen		
6993	PR05407500	penet at 5K,resonance freq(5K)=17.0cm(-1)	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.85Pb0.35Sr2Ca2Cu3.1Oz	Bi	1.85	Pb	0.35	Sr	2	Ca	2	Cu	3.1											O	z			1996																												Bi2223																				107					107																																									micron.m	Josephson plasma frequency  			23																																																								Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6994	PR05407500	penet at 5K,resonance freq(5K)=12cm(-1)	(La,Ca)2CaCu2O6	La1.82Ca1.18Cu2O6+z	La	1.82	Ca	1.18	Cu	2															O	6+z			1996																												2126																				52					52																																									micron.m	Josephson plasma frequency  			15																																																								Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6995	PR05407500	penet at 5K,resonance freq(5K)=22.0cm(-1)	(Nd,Sr,Ce)2CuO4	Nd1.32Sr0.41Ce0.27Cu1O4	Nd	1.32	Sr	0.41	Ce	0.27	Cu	1													O	4			1996																												T*																				24					24																																									micron.m	Josephson plasma frequency  			29																																																								Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6996	PR05407500	penet(5K),resonance freg(5K)=38,5cm(-1)	(Ba,Sr)2CuO2(CO3)	Ba1.12Sr0.88Cu1.1C0.9O4.9+z	Ba	1.12	Sr	0.88	Cu	1.1	C	0.9													O	4.9+z			1996																																																35					35																																									micron.m	 Josephson plasma frequency 			8																																																								Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6997	PR05407500	penet(5K),resonance freg(5K)=7.5cm(-1)	(Pr,Ce)2CuO4	Pr185Ce0.15Cu1O4	Pr	185	Ce	0.15	Cu	1															O	4			1996																												T'																				20					20																																									micron.m	Josephson plasma frequency  	50																																																										Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6998	PR05407500	penet(5K),resonance freq(5K)=8.5cm(-1)	Nd2Cu(O,F)4	Nd2Cu1FO4	Nd	2	Cu	1	F																O		4		1996																																																22					22																																									micron.m	Josephson plasma frequency 	40																																																										Superconducting-plasma resonance along the c axis in various copper oxide superconductors	199609		Nippon Telegraph and Telephon Corporation,Basic Research Laboratories,3-1 Morinosato Wakamiya,Athugi-shi,Kanagawa 243-01, japan	Phys.Rev.B,54(1996)7500	H. Shibata,T. Yamada		
6999	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu2O8.25	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.25		1996																												Bi2212																				68.2					68.2																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7000	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.99Co0.01Oz	Bi	2	Sr	2	Ca	1	Cu	1.99	Co	0.01											O	z			1996																												Bi2212																				66.2					66.2																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7001	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.98Co0.02Oz	Bi	2	Sr	2	Ca	1	Cu	1.98	Co	0.02											O	z			1996																												Bi2212																				63.6					63.6																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7002	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.96Co0.04Oz	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	z			1996																												Bi2212																				58.9					58.9																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7003	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.92Co0.08Oz	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	z			1996																												Bi2212																				51.3					51.3																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7004	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.88Co0.12Oz	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	z			1996																												Bi2212																				44.2					44.2																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7005	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.84Co0.16Oz	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	z			1996																												Bi2212																				37.1					37.1																																																																																															1	as-sintered in air for 24H at 850C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7006	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu2O8.19	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.19		1996																												Bi2212																				92.7					92.7																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7007	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.99Co0.01Oz	Bi	2	Sr	2	Ca	1	Cu	1.99	Co	0.01											O	z			1996																												Bi2212																				88.7					88.7																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7008	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.98Co0.02Oz	Bi	2	Sr	2	Ca	1	Cu	1.98	Co	0.02											O	z			1996																												Bi2212																				85.8					85.8																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7009	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.96Co0.04Oz	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	z			1996																												Bi2212																				78.9					78.9																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7010	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.92Co0.08Oz	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	z			1996																												Bi2212																				68					68																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7011	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.88Co0.12Oz	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	z			1996																												Bi2212																				58					58																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7012	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.84Co0.16Oz	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	z			1996																												Bi2212																				44.2					44.2																																																																																															1	N2 anneald at 600c					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7013	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.28		1996																												Bi2212																				60.7					60.7																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7014	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.99Co0.01Oz	Bi	2	Sr	2	Ca	1	Cu	1.99	Co	0.01											O	z			1996																												Bi2212																				58.9					58.9																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7015	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.98Co0.02Oz	Bi	2	Sr	2	Ca	1	Cu	1.98	Co	0.02											O	z			1996																												Bi2212																				56.2					56.2																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7016	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.96Co0.04Oz	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	z			1996																												Bi2212																				51.1					51.1																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7017	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.92Co0.08Oz	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	z			1996																												Bi2212																				46					46																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7018	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.88Co0.12Oz	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	z			1996																												Bi2212																				38.4					38.4																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7019	PR05400086		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.84Co0.16Oz	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	z			1996																												Bi2212																				31.3					31.3																																																																																															1	O2 annealed at 600C					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7020	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu2I1Oz	Bi	2	Sr	2	Ca	1	Cu	2	I	1											O	z			1996																												Bi2212																				50.7					50.7																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7021	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.99Co0.01I1Oz	Bi	2	Sr	2	Ca	1	Cu	1.99	Co	0.01	I	1									O	z			1996																												Bi2212																				49					49																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7022	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.98Co0.02I1Oz	Bi	2	Sr	2	Ca	1	Cu	1.98	Co	0.02	I	1									O	z			1996																												Bi2212																				46					46																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7023	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.96Co0.04I1Oz	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04	I	1									O	z			1996																												Bi2212																				41.5					41.5																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7024	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.92Co0.08I0.94Oz	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08	I	0.94									O	z			1996																												Bi2212																				34.9					34.9																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7025	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.88Co0.12I0.91Oz	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12	I	0.91									O	z			1996																												Bi2212																				28.4					28.4																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7026	PR05400086		Bi2Sr2Ca(Cu,Co)2OzIx	Bi2Sr2Ca1Cu1.84Co0.16I0.85Oz	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16	I	0.85									O	z			1996																												Bi2212																				21.1					21.1																																																																																															1	as-sintered sample, Tc and Iodine content does not changed by annealing in O2 or N2 gas					Idine intercalation in Bi2Sr2Ca(Cu1-zCoz)2O8+z with different z valus	199607		Department of Applied Physics,Faculty of Engineering,Tohoku University, Aramaki Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,54(1996)86	A. Fujiwara,M. Kato,T. Kluge,Y. Koike		
7027	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.53	Y	1	Ba	2	Cu	3															O	z	6.53		1992																												Y123																				54					54			K/GPa	2.98																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7028	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.59	Y	1	Ba	2	Cu	3															O	z	6.59		1992																												Y123																				61.2					61.2			K/GPa	3.75																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7029	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.67	Y	1	Ba	2	Cu	3															O	z	6.67		1992																												Y123																				61.5					61.5			K/GPa	3.77																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7030	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.71	Y	1	Ba	2	Cu	3															O	z	6.71		1992																												Y123																				67.3					67.3			K/GPa	7.02																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7031	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	z	6.73		1992																												Y123																				73.6					73.6			K/GPa	6.51																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7032	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.77	Y	1	Ba	2	Cu	3															O	z	6.77		1992																												Y123																				86.2					86.2			K/GPa	3.89																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7033	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	z	6.87		1992																												Y123																				90.3					90.3			K/GPa	2.52																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7034	PHC2030293		YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	z	6.93		1992																												Y123																				92.6					92.6			K/GPa	0.44																																																																																										Y2O3, BaCO3,CuO	1	samples were annealed at 400-700c for 24H for narious oxygen content					THE EFFECT OF HIGH HYDROSTATIC PRESSURE ON TC OF YBA2CU3OX ASAFUNCTION OF THE OXYGEN CONTENT	199212			PHYSICA C,203(1992)293	H.WUHL,J.METZGER,K.GRUBE,R.BENISCHKE,T.WEBER,T.WOLF,W.H.FIETZ	Y,BA,CU,O	
7035	PHC2640220		Bi2(Sr,Bi)2CuO6	Bi2.11Sr1.89Cu1O6+z	Bi	2.11	Sr	1.89	Cu	1															O	6+z		3	1996																												Bi2201																				6.8					6.8																																																																																		0.48														by self-flux and travelling solvent flux method, annealing at 700C under O2 for 172H					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7036	PHC2640220		Bi2(Sr,Bi)2CuO6	Bi2.15Sr1.85Cu1O6+z	Bi	2.15	Sr	1.85	Cu	1															O	6+z		3	1996																												Bi2201																				6.5					6.5																																																																			-13.88			TP7036												0.65														by self-flux and travelling solvent flux method, annealing at 700C under O2 for 172H					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7037	PHC2640220		Bi2(Sr,Bi)2CuO6	Bi2.2Sr0.8Cu1O6+z	Bi	2.2	Sr	0.8	Cu	1															O	6+z		3	1996																												Bi2201																								4.2																																																																				-4.94			TP7037												2														by self-flux and travelling solvent flux method, annealing at 700C under O2 for 172H					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7038	PHC2640220		Bi2(Sr,Bi)2CuO6	Bi2.4Sr1.6Cu1O6+z	Bi	2.4	Sr	1.6	Cu	1															O	6+z		3	1996																												Bi2201																								4.2																																																																				29.75			TP7038												60														by self-flux and travelling solvent flux method, annealing at 700C under O2 for 172H					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7039	PHC2640220		Bi2(Sr,Bi)2CuO6	Bi2.11Sr1.89Cu1O6+z	Bi	2.11	Sr	1.89	Cu	1															O	6+z		3	1996																												Bi2201																				8.5					8.5																																																																																		1.9														by self-flux and travelling solvent flux method, ANN(700C,172H in O2)-ANN(700C,172H in Ar)					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7040	PHC2640220	not S/C	Bi2(Sr,Bi)2CuO6	Bi2.15Sr1.85Cu1O6+z	Bi	2.15	Sr	1.85	Cu	1															O	6+z		3	1996																												Bi2201																							4.2																																																																					-9.46			TP7040												1.8														by self-flux and travelling solvent flux method, ANN(700C,172H in O2)-ANN(700C,172H in Ar)					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7041	PHC2640220	not S/C	Bi2(Sr,Bi)2CuO6	Bi2.2Sr0.8Cu1O6+z	Bi	2.2	Sr	0.8	Cu	1															O	6+z		3	1996																												Bi2201																							4.2																																																																																				30														by self-flux and travelling solvent flux method, ANN(700C,172H in O2)-ANN(700C,172H in Ar)					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7042	PHC2640220	not S/C	Bi2(Sr,Bi)2CuO6	Bi2.4Sr1.6Cu1O6+z	Bi	2.4	Sr	1.6	Cu	1															O	6+z		3	1996																												Bi2201																							4.2																																																																																				350														by self-flux and travelling solvent flux method, ANN(700C,172H in O2)-ANN(700C,172H in Ar)					Superconductivity and electric transport of Bi2+xSr2-yCuO6+z single crystals	06		Insitute of Physics, Cukrovarnicka'10, Praha 6,162 00, Czech Republic	Physica.C,264(1996)220-226	D. Sedmidubsky',E. Pollert,J. Hejtma'nek,M. Nevriva,P. Vasek	Bi, Sr, Cu, O	
7043	SUP0090201	minor phase=Bi2212	(Bi,Pb)2Sr2Ca2(Ca,Sc)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Sc0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Sc	0.2									O	z		2	1996																												Bi2223																			104.5		115	109			109																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7044	SUP0090201		(Bi,Pb)2Sr2Ca2(Cu,Ti)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Ti0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Ti	0.2									O	z		2	1996																												Bi2223																			103		113	106			106																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7045	SUP0090201		(Bi,Pb)2Sr2Ca2(Cu,V)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8V0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	V	0.2									O	z		2	1996																												Bi2223																			106.2		114.8	106			106																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7046	SUP0090201		(Bi,Pb)2Sr2Ca2(Cu,Cr)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Cr0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Cr	0.2									O	z		2	1996																												Bi2223																			107.5		113	108			108																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7047	SUP0090201		(Bi,Pb)2Sr2Ca2(Cu,Mn)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Mn0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Mn	0.2									O	z		2	1996																												Bi2223																			105.6		112	107.6			107.6																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7048	SUP0090201		(Bi,Pb)2Sr2Ca2(Cu,Fe)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Fe0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Fe	0.2									O	z		2	1996																												Bi2212																					24				24																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7049	SUP0090201	minor phese=Bi2212 semiconductor	(Bi,Pb)2Sr2Ca2(Cu,Co)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Co0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Co	0.2									O	z			1996																												Bi2212																							4.2																																																																																																		precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7050	SUP0090201	Bi2223 phase diminishes	(Bi,Pb)2Sr2Ca2(Cu,Ni)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2.8Ni0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2.8	Ni	0.2									O	z			1996																												Bi2212																			49		59				54																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7051	SUP0090201	Bi2223 phase diminishes	(Bi,Pb)2Sr2Ca2(Cu,Zn)3Oz	Bi1.5Pb0.2Sr2Ca2Cu2Zn0.2Oz	Bi	1.5	Pb	0.2	Sr	2	Ca	2	Cu	2	Zn	0.2									O	z			1996																												Bi2212																			76.6		88				82.3																																																																																																precursor(Bi-Pb-sr-Ca-Cu-O)+(M-oxide or M-Co3)-mixture-CAL(845-850C,150H in air)-pellet-SIN(845-850C,150H in air)-ANN(400C,24H in air)					Comparative Study on the Doping Effect of 3d Elements in Bi1.5Pb0.2Sr2Ca2Cu2.8M0.2Oy (M=Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn)			Changchun Institute of Applied Chemistry, Chinese Academy of Sciences, Changchun 130022, P.R. China.	J.Superconductivity,9(1996)201-203	Bangchao Yang,E. Marquestaut,Guangyan Hong,J. Etourneau,J.P. Chaminade,P. Dordor,Xingzhao Liu,Yanrong Li,Youmo Li		
7052	SUP0090253		(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1O4.6	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	4+z	4.6	1	1996																											2	Hg1201				3.85		8.715													53			53			53																																																																																																precursor (Cr0.3Sr2CuOz)+HgO-mixture-pellet-sealed in evacuated quartz tube-heat(880C,8H)-Q to RT					Neutron Diffraction Structural Study of 1201 Superconductor (Hg0.7Cr0.3)Sr2CuO4+delta			Saha Institute of Nuclear Physics, Calcutta-700064, India	J.Superconductivity,9(1996)253	A. Sequeira,B. Bandyopadhyay,B. Ghosh,H. Rajagopal,J.B. Mandal,J.V. Yakhmi		
7053	SUP0090181	small amount of Bi2212 phase exists	(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10.11	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	10+z	10.11		1996																											2	Bi2223				5.399		36.97														105.3					105.3																																																																																																					Mixed State Thermoelectric Power of Vanadium Substituted 2223(Bi,Pb)Superconducting Polycrystalline Cuprates			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity,9(1996)181-185	Bitasta Chanda,D.K. Dey		
7054	SUP0090181	small amount of Bi2212 phase exists	(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.35V0.05Sr2Ca2Cu3O10.12	Bi	1.6	Pb	0.35	V	0.05	Sr	2	Ca	2	Cu	3									O	10+z	10.12		1996																											2	Bi2223				5.043		36.983														103.7					103.7																																																																																																					Mixed State Thermoelectric Power of Vanadium Substituted 2223(Bi,Pb)Superconducting Polycrystalline Cuprates			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity,9(1996)181-185	Bitasta Chanda,D.K. Dey		
7055	SUP0090181	small amount of Bi2212 phase exists	(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi1.6Pb0.3Sr2Ca2Cu3V0.1O10.12	Bi	1.6	Pb	0.3	Sr	2	Ca	2	Cu	3	V	0.1									O	10+z	10.12		1996																											2	Bi2223				5.406		36.975														102.5					102.5																																																																																																					Mixed State Thermoelectric Power of Vanadium Substituted 2223(Bi,Pb)Superconducting Polycrystalline Cuprates			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity,9(1996)181-185	Bitasta Chanda,D.K. Dey		
7056	SUP0090161		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z			1996																												Bi2212																			70.5	73.5				1	73.5																																																																																														SrCO3,BaCO3,CaCO3,CuO,Bi2O3	1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7057	SUP0090161		Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.95Ba0.05Ca1Cu2Oz	Bi	2	Sr	1.95	Ba	0.05	Ca	1	Cu	2											O	z			1996																												Bi2212																			69	78.6				3	78.6																																																																																														SrCO3,BaCO3,CaCO3,CuO,Bi2O3	1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7058	SUP0090161		Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.9Ba0.1Ca1Cu2Oz	Bi	2	Sr	1.9	Ba	0.1	Ca	1	Cu	2											O	z			1996																												Bi2212																			68.8	82.6				9	82.6																																																																																														SrCO3,BaCO3,CaCO3,CuO,Bi2O3	1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7059	SUP0090161		Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.85Ba0.15Ca1Cu2Oz	Bi	2	Sr	1.85	Ba	0.15	Ca	1	Cu	2											O	z			1996																												Bi2212																			69.9	83.5				9	83.5																																																																																														SrCO3,BaCO3,CaCO3,CuO,Bi2O3	1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7060	SUP0090161	quench to RT from 865C	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z			1996																												Bi2212																			81	87.6				4.5	87.6																																																																																															1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-Q to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7061	SUP0090161	quench to RT from 865C	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.95Ba0.05Ca1Cu2Oz	Bi	2	Sr	1.95	Ba	0.05	Ca	1	Cu	2											O	z			1996																												Bi2212																			67	88.3				17	88.3																																																																																															1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-Q to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7062	SUP0090161	quench to RT from 865C	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.9Ba0.1Ca1Cu2Oz	Bi	2	Sr	1.9	Ba	0.1	Ca	1	Cu	2											O	z			1996																												Bi2212																			50.2	87.7				35	87.7																																																																																															1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-Q to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7063	SUP0090161	quench to RT from 865C	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.85Ba0.15Ca1Cu2Oz	Bi	2	Sr	1.85	Ba	0.15	Ca	1	Cu	2											O	z			1996																												Bi2212																			43	86.3				43.5	86.3																																																																																															1	mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-Q to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7064	SUP0090161	anneald sample	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z			1996																												Bi2212																			75	78				0.1	78																																																																																																mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT-ANN(865C,20H in air)-cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7065	SUP0090161	anneald sample	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.95Ba0.05Ca1Cu2Oz	Bi	2	Sr	1.95	Ba	0.05	Ca	1	Cu	2											O	z			1996																												Bi2212																			75.9	80				2	80																																																																																																mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT-ANN(865C,20H in air)-cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7066	SUP0090161	anneald sample	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.9Ba0.1Ca1Cu2Oz	Bi	2	Sr	1.9	Ba	0.1	Ca	1	Cu	2											O	z			1996																												Bi2212																			76.7	82.2				3	82.2																																																																																																mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT-ANN(865C,20H in air)-cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7067	SUP0090161	anneald sample	Bi2(Sr,Ba)2CaCu2O8	Bi2Sr1.85Ba0.15Ca1Cu2Oz	Bi	2	Sr	1.85	Ba	0.15	Ca	1	Cu	2											O	z			1996																												Bi2212																			77.3	83.5				3.4	83.5																																																																																																mixture-CAL(800C,20H)-pellet-SIN(865C,20H in air)-slow cool to RT-ANN(865C,20H in air)-cool to RT					Superconductivity of Barium-Doped Bi2Sr2CaCu2Oy			Department of Physics, University of Toront, Toronto, Ontario, Canada M5S 1A7	J.Superconductivity,9(1996)161-165	Airton martin,Beifang Yang,J.M. Perz2,M.J.G. Lee		
7068	PHC2710079	compositions are nominal values	Sr2(Ca,Sr)Cu2(CO3,BO3)Oz	Ca1.3Sr2.7Cu3C0.55B4.5O3+z	Ca	1.3	Sr	2.7	Cu	3	C	0.55	B	4.5											O	3+z			1996																												C1212																						100			100			K/GPa	0.86																																																																																											1	mixtures-seald in Au or Pt capsules,-pressed upto 5GPa-heat(1050-1100C,0.5-1.0H)-Q to RT					Effect of high pressure on Tc of a homologous series of oxycarbonate superconductors Sr2(Ca,Sr)n-1Cun(CO3)1-x(BO3)xOy(n=1,2) and Ba2Ca2Cu3(CO3)1-x(BO3)xOy			Department of Physics, Aoyama-Gakuin Unoversity, Setagaya-ku, Tokyo157, Japan	Physica.C,271(1996)79-82	H. Takahashi,J. Akimitsu,M. Sato,N. Mo^ri		
7069	PHC2710079	compositions are nominal values	Sr2Cu2(CO3,BO3)Oz	Ca0.5Sr2.5Cu2C0.7B0.3O3+z	Ca	0.5	Sr	2.5	Cu	2	C	0.7	B	0.3											O	3+z			1996																												C1201																						52			52			K/GPa	2.25																																																																																											1	mixtures-seald in Au or Pt capsules,-pressed upto 5GPa-heat(1050-1100C,0.5-1.0H)-Q to RT					Effect of high pressure on Tc of a homologous series of oxycarbonate superconductors Sr2(Ca,Sr)n-1Cun(CO3)1-x(BO3)xOy(n=1,2) and Ba2Ca2Cu3(CO3)1-x(BO3)xOy			Department of Physics, Aoyama-Gakuin Unoversity, Setagaya-ku, Tokyo157, Japan	Physica.C,271(1996)79-82	H. Takahashi,J. Akimitsu,M. Sato,N. Mo^ri		
7070	PHC2710079	compositions are nominal values. Tc(max)=128K at 8GPa	Ba2Ca2Cu3(CO3,BO3)Oz	Ba2Ca4Cu5C0.4B0.6O3+z	Ba	2	Ca	4	Cu	5	C	0.4	B	0.6											O	3+z			1996																												C1223																						120			120			K/GPa	1.2																																																																																											1	mixtures-seald in Au or Pt capsules,-pressed upto 5GPa-heat(1050-1100C,0.5-1.0H)-Q to RT					Effect of high pressure on Tc of a homologous series of oxycarbonate superconductors Sr2(Ca,Sr)n-1Cun(CO3)1-x(BO3)xOy(n=1,2) and Ba2Ca2Cu3(CO3)1-x(BO3)xOy			Department of Physics, Aoyama-Gakuin Unoversity, Setagaya-ku, Tokyo157, Japan	Physica.C,271(1996)79-82	H. Takahashi,J. Akimitsu,M. Sato,N. Mo^ri		
7071	JP00810545		YBa2(Cu,Ni)3(O,S)7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1996																																																94					94																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7072	JP00810545		YBa2(Cu,Ni)3(O,S)7	Y1Ba2Cu2.97Ni0.03S0.03Oz	Y	1	Ba	2	Cu	2.97	Ni	0.03	S	0.03											O	z			1996																																																89					89																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7073	JP00810545		YBa2(Cu,Ni)3(O,S)7	Y1Ba2Cu2.91Ni0.09S0.09Oz	Y	1	Ba	2	Cu	2.91	Ni	0.09	S	0.09											O	z			1996																																																85					85																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7074	JP00810545		YBa2(Cu,Ni)3(O,S)7	Y1Ba2Cu2.85Ni0.15S0.15Oz	Y	1	Ba	2	Cu	2.85	Ni	0.15	S	0.15											O	z			1996																																																83					83																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7075	JP00810545		YBa2(Cu,Ni)3(O,S)7	Y1Ba2Cu2.4Ni0.6S0.6Oz	Y	1	Ba	2	Cu	2.4	Ni	0.6	S	0.6											O	z			1996																																																70					70																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7076	JP00810545		YBa2(Cu,Fe)3(O,S)7	Y1Ba2Cu2.94Fe0.06S0.06Oz	Y	1	Ba	2	Cu	2.94	Fe	0.06	S	0.06											O	z			1996																																																85.9					85.9																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7077	JP00810545		YBa2(Cu,Fe)3(O,S)7	Y1Ba2Ca2.85Fe0.15S0.15Oz	Y	1	Ba	2	Ca	2.85	Fe	0.15	S	0.15											O	z			1996																																																61.4					61.4																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7078	JP00810545		YBa2(Cu,Fe)3(O,S)7	Y1Ba2Ca2.55Fe0.3S0.3Oz	Y	1	Ba	2	Ca	2.55	Fe	0.3	S	0.3											O	z			1996																																																41					41																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7079	JP00810545		YBa2(Cu,Fe)3(O,S)7	Y1Ba2Ca2.55Fe0.45S0.45Oz	Y	1	Ba	2	Ca	2.55	Fe	0.45	S	0.45											O	z			1996																																																24.6					24.6																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7080	JP00810545		YBa2(Cu,Zn)3(O,S)7	Y1Ba2Cu1Oz	Y	1	Ba	2	Cu	1															O	z			1996																																																89.6					89.6																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7081	JP00810545		YBa2(Cu,Zn)3(O,S)7	Y1Ba2Cu2.97Zn0.03S0.03Oz	Y	1	Ba	2	Cu	2.97	Zn	0.03	S	0.03											O	z			1996																																																77.7					77.7																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7082	JP00810545		YBa2(Cu,Zn)3(O,S)7	Y1Ba2Cu2.85Zn0.15S0.15Oz	Y	1	Ba	2	Cu	2.85	Zn	0.15	S	0.15											O	z			1996																																																45.7					45.7																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7083	JP00810545		YBa2(Cu,Zn)3(O,S)7	Y1Ba2Cu2.7Zn0.3S0.3Oz	Y	1	Ba	2	Cu	2.7	Zn	0.3	S	0.3											O	z			1996																																																35					35																																																																																															1	mixture-Cal(920C,24H)-pellet-fire(24H)-ANN(940,24H in flowing O2)-slow cool to RT					Structural and superconducting properties of MS(M=Fe,Ni or Zn)-substituted YBa2Cu3O7-z			Departmento de Fisica, Universidade Federal de Pemambuco,50670-901 Recife, PE, Brazill	J.Phys.Condens.Matter, 8(1996)10545-10550	A C Pavao,Alexandre S Ramos,E Chavira,E Z Kurmaev,J Albino Aguiar,J M Ferreira,Leonardo R E Cabral,M Virgi'nia Barbosa,V P S Awana		
7084	APJ0355304	HIR fiqure: P=1 for H//C-axis, P=2 for H// ab plane	(Tl,Pb)Sr2Ca2Cu3O9	Tl0.5Pb0.5Sr2Ca2Cu3O9	Tl	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	9			1996																																																		112			112																																		HIR7084																																																														An aligned sample was produced from monocryslals of 3 micron, in diameter, dis persed in liq. epoxy, aligned in 5T field					Magnetic Properties in Aligned (Tl0.5Pb0.5)Sr2Ca2Cu3O9 High-Tc Superconductor			Department of Physics of Pusan Natioal University, Pusan 609-735, Korea	Jpn.J. Appl.Phys.35(1996)5304	Dae Yeong Jeong,Gun Cheol Kim,Jeong Nam Kim,Myung Hwan Sohn,Yong Dae Paek,Young Cheol Kim		
7085	SSC0970719		(Bi,Pb)2Sr2Ca2Cu3O10	Bi0.16Pb0.4Sr2Ca2Cu3O10.11	Bi	0.16	Pb	0.4	Sr	2	Ca	2	Cu	3											O	10+z	10.11		1996																											2	Bi2223				5.399		36.97													105.3						105.3																																																																																		3.25													1	see cryogenics 33(1993) 980					MIXED STATE THERMOELECTRIC POWER OF VANADIUM SUBSTITUTED 2223 (Bi,Pb) SUPERCONDUCTING POLYCRYSTALLINE CUPRATES			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	Solid State Commun.97(1996)719	Bitasta Chanda,T.K. Dey		
7086	SSC0970719		(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi0.16Pb0.35V0.05Sr2Ca2Cu3O10.12	Bi	0.16	Pb	0.35	V	0.05	Sr	2	Ca	2	Cu	3									O	10+z	10.12		1996																											2	Bi2223				5.403		36.983													103.7						103.7																																																																																		3.3													1	see cryogenics 33(1993) 980					MIXED STATE THERMOELECTRIC POWER OF VANADIUM SUBSTITUTED 2223 (Bi,Pb) SUPERCONDUCTING POLYCRYSTALLINE CUPRATES			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	Solid State Commun.97(1996)719	Bitasta Chanda,T.K. Dey		
7087	SSC0970719		(Bi,Pb,V)2Sr2Ca2Cu3O10	Bi0.16Pb0.3V0.1Sr2Ca2Cu3O10.12	Bi	0.16	Pb	0.3	V	0.1	Sr	2	Ca	2	Cu	3									O	10+z	10.12		1996																											2	Bi2223				5.406		36.975													102.5						102.5																																																																																		3.6													1	see cryogenics 33(1993) 980					MIXED STATE THERMOELECTRIC POWER OF VANADIUM SUBSTITUTED 2223 (Bi,Pb) SUPERCONDUCTING POLYCRYSTALLINE CUPRATES			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	Solid State Commun.97(1996)719	Bitasta Chanda,T.K. Dey		
7088	SSC0970487		LaBa2Cu2NbO8	La1Ba2Cu2Nb1O8	La	1	Ba	2	Cu	2	Nb	1													O	8		1	1996						0.27	2.82																				2	1212	P4/mmm			3.971		12.009																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7089	SSC0970487		(La,Pr)Ba2Cu2NbO8	La0.75Pr0.25Ba22Nb1O8	La	0.75	Pr	0.25	Ba	2		2	Nb	1											O	8		1	1996						1.49	4.49																				2	1212				3.967		12																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7090	SSC0970487		(La,Pr)Ba2Cu2NbO8	La0.5Pr0.5Ba2Cu2Nb1O8	La	0.5	Pr	0.5	Ba	2	Cu	2	Nb	1											O	8		1	1996				0.001		2.06	4.5	2.21																			2	1212				3.961		11.989																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7091	SSC0970487		(La,Pr)Ba2Cu2NbO8	La0.4Pr0.6Ba2Cu2Nb1O8	La	0.4	Pr	0.6	Ba	2	Cu	2	Nb	1											O	8		1	1996				0.001		2.24	5.19	4																			2	1212				3.959		11.984																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7092	SSC0970487		(La,Pr)Ba2Cu2NbO8	La0.25Pr0.75Ba2Cu2Nd1O8	La	0.25	Pr	0.75	Ba	2	Cu	2	Nd	1											O	8		1	1996				0.001		2.45	5.3	6.73																			2	1212				3.957		11.981																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7093	SSC0970487		(La,Pr)Ba2Cu2NbO8	La0.1Pr0.9Ba2Cu2Nb1O8	La	0.1	Pr	0.9	Ba	2	Cu	2	Nb	1											O	8		1	1996				0.001		2.69	5.22	10.3																			2	1212				3.954		11.98																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7094	SSC0970487		PrBa2Cu2NbO8	Pr1Ba2Cu2Nb1O8	Pr	1	Ba	2	Cu	2	Nb	1													O	8		1	1996				0.001		2.81	5.47	12.4																			2	1212				3.954		11.983																	2																																																																																																La2O3,Pr6O11,CuO,BaCO3,Nb2O5	1	mixture-fire (1000C,16H)-Q to RT in air-pellet-fire (1025C,16H)-Q to RT in air					STRUCRURAL CHARACTERIZATION AND MAGNETIC ORDERING IN (La1-xPrx) Ba2Cu2NbO8			Department of Physics, University of California, Davis, CA 95616, U.S.A	Solid State Commun.97(1996)487	B.D. Schrag,C.C. Hoellwarth,P. Klavins,R.N. Shelton,T.J. Goodwin		
7095	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	1992																												Bi2212																																																																																												-5.3			TP7095												2.11														see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7096	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												-0.48			TP7096																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7097	PR04611840		Bi2Se2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												2.75			TP7097																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7098	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												7.6			TP7098																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7099	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												20.6			TP7099												9.9														see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7100	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8+z	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												40			TP7100																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7101	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.45Y0.55Cu2O8+z	Bi	2	Sr	2	Ca	0.45	Y	0.55	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												52.9			TP7101												22.9														see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7102	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.4Y0.6Cu2O8+z	Bi	2	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												73.9			TP7102												58.6														see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7103	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.3Y0.7Cu2O8+z	Bi	2	Sr	2	Ca	0.3	Y	0.7	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												156			TP7103												76.5														see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7104	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.2Y0.8Cu2O8+z	Bi	2	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												279			TP7104																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7105	PR04611840		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.1Y0.9Cu2O8+z	Bi	2	Sr	2	Ca	0.1	Y	0.9	Cu	2											O	8+z		1	1992																												Bi2212																																																																																												397			TP7105																										see phys.Rev.B,43(1991)13102					THERMOELECTRIC POWER OF THE BI2SR2CA1-XYXCU2O8+Y(X=0-1.0) SYSTEM	199211		SAHA INSTITUTE OF NUCLEAR PHYSICS, INDIA	PHYS.REV.B,46(1992)11840	A.N.DAS,A.PODDAR,B.GHOSH,J.B.MANDAL,P.MANDAL,S.KESHRI	BI,SR,CA,Y,CU,O	
7106	JP00802869	band valence sum=2.39	(Pb,Cd)(Sr,Pr)2(Pr,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Pr1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.8	Pr	1.6	Ce	0.6	Cu	2									O	z			1996																											2	Pb1222	I4/mmm			3.87		29.501																	4.2																																																																																																PbO,CdO,SrCO3,CeO2,Pr6O11,TbO2,R2O3,CuO	1	mixture-CAL(900C,overnight in air)-FC to RT -pellet-SIN(1050C,8H in air)-SIN(1050C, in flowing O2)					The crystal structure and superconductivity of (Pb0.5Cd0.5)(Sro.9Ln0.1)2(Ln0.7Ce0.3)2Cu2O9(Ln=Pr,Sm,Eu,Gd and Dy)			Institute of Physics,Chinese Academy of Sciences, Beijing 100080,Peopl's Republic of China	J.Phys.Condens.Matter, 8(1996)2869	C Dong,C Wang,G H Rao,J K Liang,J R Min		
7107	JP00802869	band valence sum=2.63	(Pb,Cd)(Sr,Sm)2(Sm,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Sm1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.8	Sm	1.6	Ce	0.6	Cu	2									O	z			1996																											2	Pb1222	I4/mmm			3.835		29.433													29		41				35																																																																																														PbO,CdO,SrCO3,CeO2,Pr6O11,TbO2,R2O3,CuO	1	mixture-CAL(900C,overnight in air)-FC to RT -pellet-SIN(1050C,8H in air)-SIN(1050C, in flowing O2)					The crystal structure and superconductivity of (Pb0.5Cd0.5)(Sro.9Ln0.1)2(Ln0.7Ce0.3)2Cu2O9(Ln=Pr,Sm,Eu,Gd and Dy)			Institute of Physics,Chinese Academy of Sciences, Beijing 100080,Peopl's Republic of China	J.Phys.Condens.Matter, 8(1996)2869	C Dong,C Wang,G H Rao,J K Liang,J R Min		
7108	JP00802869	band valence sum=2.65	(Pb,Cd)(Sr,Eu)2(Eu,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Eu1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.8	Eu	1.6	Ce	0.6	Cu	2									O	z			1996																											2	Pb1222	I4/mmm			3.831		29.39													35		43				39																																																																																														PbO,CdO,SrCO3,CeO2,Pr6O11,TbO2,R2O3,CuO	1	mixture-CAL(900C,overnight in air)-FC to RT -pellet-SIN(1050C,8H in air)-SIN(1050C, in flowing O2)					The crystal structure and superconductivity of (Pb0.5Cd0.5)(Sro.9Ln0.1)2(Ln0.7Ce0.3)2Cu2O9(Ln=Pr,Sm,Eu,Gd and Dy)			Institute of Physics,Chinese Academy of Sciences, Beijing 100080,Peopl's Republic of China	J.Phys.Condens.Matter, 8(1996)2869	C Dong,C Wang,G H Rao,J K Liang,J R Min		
7109	JP00802869	band valence sum=2.75	(Pb,Cd)(Sr,Gd)2(Gd,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Gd1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.8	Gd	1.6	Ce	0.6	Cu	2									O	z			1996																											2	Pb1222	I4/mmm			3.822		29.354													38		49				43.5																																																																																														PbO,CdO,SrCO3,CeO2,Pr6O11,TbO2,R2O3,CuO	1	mixture-CAL(900C,overnight in air)-FC to RT -pellet-SIN(1050C,8H in air)-SIN(1050C, in flowing O2)					The crystal structure and superconductivity of (Pb0.5Cd0.5)(Sro.9Ln0.1)2(Ln0.7Ce0.3)2Cu2O9(Ln=Pr,Sm,Eu,Gd and Dy)			Institute of Physics,Chinese Academy of Sciences, Beijing 100080,Peopl's Republic of China	J.Phys.Condens.Matter, 8(1996)2869	C Dong,C Wang,G H Rao,J K Liang,J R Min		
7110	JP00802869	band valence sum=2.77	(Pb,Cd)(Sr,Dy)2(Dy,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Dy1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Sr	1.8	Dy	1.6	Ce	0.6	Cu	2									O	z			1996																											2	Pb1222	I4/mmm			3.813		29.289															12		4.2		12																																																																																														PbO,CdO,SrCO3,CeO2,Pr6O11,TbO2,R2O3,CuO	1	mixture-CAL(900C,overnight in air)-FC to RT -pellet-SIN(1050C,8H in air)-SIN(1050C, in flowing O2)					The crystal structure and superconductivity of (Pb0.5Cd0.5)(Sro.9Ln0.1)2(Ln0.7Ce0.3)2Cu2O9(Ln=Pr,Sm,Eu,Gd and Dy)			Institute of Physics,Chinese Academy of Sciences, Beijing 100080,Peopl's Republic of China	J.Phys.Condens.Matter, 8(1996)2869	C Dong,C Wang,G H Rao,J K Liang,J R Min		
7111	JP00801743		(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	4+z			1996																											2	Hg1201	P4/mmm			3.842		8.725														51					51																																																									24.847		234	from SP.heat,coeff=1.1898mj/mole.K(-4)							23																											Sr(NO3)2,Cu(NO3)2.3H2O,HgO,Cr2O3		precursor+Cr2O3-mix and fire(900C,24H)-mix with HgO-pellet-seal in evacuated quartz tube-SIN(880C,8H)-Q to RT-ANN(300C,1H in O2)					Structural, transport and thermal properties of Hg0.7Cr0.3Sr2CuO4+z			Saha Institute of Nuclear Physics, 1/AF Bidhannagar,Calcutta 700 064, India	J.Phys.:Cond.Matter, 8(1996)1743	A Poddar,B Bandyopadhyay,B Ghosh,J B Mandal,P Choudhury		
7112	JJP0350205	small amoount of 2223,1223 phases included,two step resistive transition 	(Hg,Tl)2Ba2Ca3Cu4Oz	Hg1.4Tl0.6Ba2Ca3Cu4Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	3	Cu	4											O	z			1996																											2	Tl2234				3.845		42.06													113		120	114			114																																																																																															1	precursor(Ba2Ca2Cu3Oz)-mix(HgO,Tl2O3,CaO)-pellet-seal in Au capsule-heat(1000C,1-3H at P=5 GPa)					A New Homologous Series of Superconducting Cuprates with the 22(n-1)n Structure, (Hg1-xTlx)2Ba2Can-1CunOy (x~0.4, n=3,4)			Superconductivity Research Laboratory, International Superconductivity Technology Center,1-10-13 Shinonome,Koto-ku, Tokyo 135, Japan	J.Appl.Phys.Lett.35(1996)L205	Atsushi FUKUOKA,Ayako TOKIWA-YAMAMOTO,Keiichi TANABE,Ryo USAMI,Seiji ADACHI,Shoji TANAKA,Tadashi TATSUKI,Toshiyuki TAMURA,Xiao-jing Wu,Yoshiyuki MORIWAKI		
7113	JJP0350205	inpurity phase=HgCaO2,unknown	(Hg,Tl)2Ba2Ca2Cu3Oz	Hg1.4Tl0.6Ba2Ca2Cu3Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	2	Cu	3											O	z			1996																											2	Tl2223				3.84		35.69																45			45																																																																																															1	precursor(Ba2Ca2Cu3Oz)-mix(HgO,Tl2O3,CaO)-pellet-seal in Au capsule-heat(1000C,1-3H at P=5 GPa)					A New Homologous Series of Superconducting Cuprates with the 22(n-1)n Structure, (Hg1-xTlx)2Ba2Can-1CunOy (x~0.4, n=3,4)			Superconductivity Research Laboratory, International Superconductivity Technology Center,1-10-13 Shinonome,Koto-ku, Tokyo 135, Japan	J.Appl.Phys.Lett.35(1996)L205	Atsushi FUKUOKA,Ayako TOKIWA-YAMAMOTO,Keiichi TANABE,Ryo USAMI,Seiji ADACHI,Shoji TANAKA,Tadashi TATSUKI,Toshiyuki TAMURA,Xiao-jing Wu,Yoshiyuki MORIWAKI		
7114	JJP0350974	Yb124+Yb211+CuO	YbBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.82	3.85	27.2																																																																																																																	R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7115	JJP0350974		(Yb,Ca)Ba2Cu4O8	Y0.99Ca0.01Ba2Cu4O8	Y	0.99	Ca	0.01	Ba	2	Cu	4													O	8			1996																											3	Y124				3.823	3.858	27.125													79.4						79.4																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7116	JJP0350974		(Yb,Ca)Ba2Cu4O8	Y0.97Ca0.03Ba2Cu4O8	Y	0.97	Ca	0.03	Ba	2	Cu	4													O	8			1996																											3	Y124				3.822	3.855	27.164													81.9						81.9																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7117	JJP0350974		(Yb,Ca)Ba2Cu4O8	Y0.95Ca0.05Ba2Cu4O8	Y	0.95	Ca	0.05	Ba	2	Cu	4													O	8			1996																											3	Y124				3.822	3.853	27.175													85.4						85.4																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7118	JJP0350974		(Yb,Ca)Ba2Cu4O8	Y0.93Ca0.07Ba2Cu4O8	Y	0.93	Ca	0.07	Ba	2	Cu	4													O	8			1996																											3	Y124				3.82	3.852	27.18													83.5						83.5																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7119	JJP0350974		(Yb,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8			1996																											3	Y123				3.851	3.854	11.579													80.8						80.8																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7120	JJP0350974		TmBa2Cu4O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.829	3.859	27.185													79						79																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7121	JJP0350974		(Tm,Ca)Ba2Cu4O8	Tm0.99Ca0.01Ba2Cu4O8	Tm	0.99	Ca	0.01	Ba	2	Cu	4													O	8			1996																											3	Y124				3.831	3.86	27.186													79.2						79.2																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7122	JJP0350974		(Tm,Ca)Ba2Cu4O8	Tm0.97Ca0.03Ba2Cu4O8	Tm	0.97	Ca	0.03	Ba	2	Cu	4													O	8			1996																											3	Y124				3.829	3.857	27.198													81.2						81.2																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7123	JJP0350974		(Tm,Ca)Ba2Cu4O8	Tm0.95Ca0.05Ba2Cu4O8	Tm	0.95	Ca	0.05	Ba	2	Cu	4													O	8			1996																											3	Y124				3.829	3.857	27.207													84.8						84.8																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7124	JJP0350974		(Tm,Ca)Ba2Cu3O7	Tm0.93Ca0.07Ba2Cu4O8	Tm	0.93	Ca	0.07	Ba	2	Cu	4													O	8			1996																											3	Y123				3.833	3.859	11.628													83.3						83.3																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7125	JJP0350974		ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.836	3.861	27.192													78						78																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7126	JJP0350974		(Er,Ca)Ba2Cu4O8	Er0.99Ca0.01Ba2Cu4O8	Er	0.99	Ca	0.01	Ba	2	Cu	4													O	8			1996																											3	Y124				3.837	3.86	27.196													79.3						79.3																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7127	JJP0350974		(Er,Ca)Ba2Cu4O8	Er0.97Ca0.03Ba2Cu4O8	Er	0.97	Ca	0.03	Ba	2	Cu	4													O	8			1996																											3	Y124				3.834	3.86	27.218													80						80																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7128	JJP0350974		(Er,Ca)Ba2Cu4O8	Er0.95Ca0.05Ba2Cu4O8	Er	0.95	Ca	0.05	Ba	2	Cu	4													O	8		2	1996																											3					3.83	3.85	27.15													83.2						83.2																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7129	JJP0350974		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.836	3.865	27.198													76						76																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7130	JJP0350974		(Ho,Ca)Ba2Cu4O8	Ho0.99Ca0.01Ba2Cu4O8	Ho	0.99	Ca	0.01	Ba	2	Cu	4													O	8			1996																											3	Y124				3.832	3.86	27.202													76.8						76.8																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7131	JJP0350974		(Ho,Ca)Ba2Cu4O8	Ho0.97Ca0.03Ba2Cu4O8	Ho	0.97	Ca	0.03	Ba	2	Cu	4													O	8			1996																											3	Y123				3.828	3.875	11.707													77.4						77.4																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7132	JJP0350974		(YBa2Cu4O8)	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1996																											3	Y124				3.843	3.871	27.23													79.7						79.7																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7133	JJP0350974	Y124+Y123	(Y,Ca)Ba2Cu4O8	Y0.99Ca0.01Ba2Cu4O8	Y	0.99	Ca	0.01	Ba	2	Cu	4													O	8		2	1996																											3	Y124				3.837	3.869	27.23													78						78																																																																																														R2O3,CaCO3,BaCO3,CuO	1	mixrure-pellet-SIN(800C,12H in quartz tube in vac)(P(O2)=1Torr)-ANN(820C,24-48H in flowing O2)-Fc to RT					Preparation of Ceramics (RCa)Ba2Cu4O8 (R=Y,Ho,Er,Tm and Yb) by Conventional Solid-State Reaction			Department of Engineering, Kansai University, 3-3-35 Yamate-cho, Suita-Shi, Osaka 564, Japan	J.Appl.Phys.Lett.35(1996)L974	Masakazu TATSUMI,Miho NISHI,Seika YAMAMOTO,Takenori SHIGETA		
7134	JJP0350012	T=1030C, P=2.0GPa, 9.5H	CuSr2YCu2Oz	Sr2Y1Cu3O7.9	Sr	2	Y	1	Cu	3															O	z	7.9		1996																												Cu1212																						69			69																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7135	JJP0350012	T=1030C, P=2.0GPa, 9.5H	CuSr2YCu2Oz	Sr2Y1Cu3O7.65	Sr	2	Y	1	Cu	3															O	z	7.65		1996																												Cu1212																						70			70																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7136	JJP0350012	T=985C, P=2.1GPa, 2.5H	CuSr2YCu2Oz	Sr2Y1Cu3O7.75	Sr	2	Y	1	Cu	3															O	z	7.75		1996																												Cu1212																						67			67																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7137	JJP0350012	T=990, P=2.1, 8.5H	CuSr2YCu2Oz	Sr2Y1Cu3O7.65	Sr	2	Y	1	Cu	3															O	z	7.65		1996																												Cu1212																						69			69																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7138	JJP0350012	T=1090C, P=2.0GPa, 2.0H	CuSr2YCu2Oz	Sr2Y1Cu3O7.95	Sr	2	Y	1	Cu	3															O	z	7.95		1996																												Cu1212																						62			62																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7139	JJP0350012	T=1050C, P=2.0GPa, 2.5H	Cusr2YCu2Oz	Sr2Y1Cu3O7.45	Sr	2	Y	1	Cu	3															O	z	7.45		1996																												Cu1212																						62			62																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7140	JJP0350012	T=990C, P=2.4GPa, 9.5H	CuSr2TmCu2Oz	Sr2Tm1Cu3O7.65	Sr	2	Tm	1	Cu	3															O	z	7.65		1996																												Cu1212																						62			62																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7141	JJP0350012	T=990, P=2.5GPa, 9.5H	CuSr2TmCu2Oz	Sr2Tm1Cu3O7.2	Sr	2	Tm	1	Cu	3															O	z	7.2		1996																												Cu1212																						62			62																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7142	JJP0350012	T=990C, P=2.5GPa, 2.5H	CuSr2TmCu2Oz	Sr2Tm1Cu3O7.28	Sr	2	Tm	1	Cu	3															O	z	7.28		1996																												Cu1212																						56			56																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7143	JJP0350012	T=970, P=1.6GPa, 8H	CuSr2TmCu2Oz	Sr2Tm1Cu3O7.48	Sr	2	Tm	1	Cu	3															O	z	7.48		1996																												Cu1212																						62			62																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7144	JJP0350012	T=1050, P=2.1, 2H	CuSr2TmCu2Oz	Sr2Tm1Cu3O7.48	Sr	2	Tm	1	Cu	3															O	z	7.48		1996																												Cu1212																						55			55																																																																																														SrCO3,Y2O3,Tm2O3,CuO	1	mixture-seal(Au capsule with K Cl O3)-heat(980-1030C),2.5-9.5H at 1.6-2.5 GPa),heating condition shown in COMMT					Critical-Temperature Optimization in Sr2YCu3Oz and Sr2TmCu3Oz			National Institute for research in Inorganic Materials, 1-1 namiki Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L12	Akira Ono		
7145	JJP0350201		(Cu,Ti)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ti0.2O7	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ti	0.2											O	z	7	1	1996																											2	M1212				3.821		11.513																35			35																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7146	JJP0350201		(Cu,Ga)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ga0.2O7	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ga	0.2											O	z	7	1	1996																											2	M1212				3.817		11.503																38			38																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7147	JJP0350201		(Cu,Ge)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ge0.2O7	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ge	0.2											O	z	7		1996																											2	M1212				3.822		11.503																25			25																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7148	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Al0.2O6.8	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Al	0.2											O	z	6.8		1996																											2	M1212				3.831		11.378																																																																																																																	SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7149	JJP0350201		(Cu,Mo)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Mo0.2O7.03	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Mo	0.2											O	z	7.03	1	1996																											2	M1212				3.821		11.583																26			26																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7150	JJP0350201		(Cu,Cr)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Cr0.2O7	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Cr	0.2											O	z	7		1996																											2	M1212				3.848		11.445																																																																																																																	SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7151	JJP0350201		(Cu,Ga)(Sr,Ba2)YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ga0.2O7.2	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ga	0.2											O	z	7.2		1996																												M1212																						61			61																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7152	JJP0350201		(Cu,Ga)(Sr,Ba2)YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ga0.2O7.14	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ga	0.2											O	z	7.14		1996																												M1212																						56			56																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7153	JJP0350201		(Cu,Ga)(Sr,Ba2)YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ga0.2O7.1	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ga	0.2											O	z	7.1		1996																												M1212																						50			50																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7154	JJP0350201		(Cu,Ga)(Sr,Ba2)YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ga0.2O6.96	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ga	0.2											O	z	6.96		1996																												M1212																						32			32																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7155	JJP0350201		(Cu,Ti)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ti0.2O7.2	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ti	0.2											O	z	7.2		1996																												M1212																						78			78																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7156	JJP0350201		(Cu,Ti)(Sr,Ba)2YCu2O7	Sr1.5Ba0.5Y1Cu2.8Ti0.2O7.08	Sr	1.5	Ba	0.5	Y	1	Cu	2.8	Ti	0.2											O	z	7.08		1996																												M1212																						52			52																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7157	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr0.7Ba1.3Y1Cu2.8Al0.2O6.81	Sr	0.7	Ba	1.3	Y	1	Cu	2.8	Al	0.2											O	z	6.81		1996																											2	M1212				3.86		11.505																																																																																																																	SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7158	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr0.7Ba1.3Y1Cu2.8Al0.2O7.03	Sr	0.7	Ba	1.3	Y	1	Cu	2.8	Al	0.2											O	z	7.03		1996																											2	M1212				3.857		11.487																12			12																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7159	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr0.7Ba1.3Y1Cu2.8Al0.2O7.11	Sr	0.7	Ba	1.3	Y	1	Cu	2.8	Al	0.2											O	z	7.11		1996																											2	M1212				3.858		11.488																20			20																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7160	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr1Ba1Y1Cu2.8Al0.2O7.15	Sr	1	Ba	1	Y	1	Cu	2.8	Al	0.2											O	z	7.15		1996																											2	M1212				3.846		11.446																20			20																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7161	JJP0350201		(Cu,Al)(Sr,Ba)2YCu2O7	Sr1.2Ba0.8Y1Cu2.8Al0.2O7.19	Sr	1.2	Ba	0.8	Y	1	Cu	2.8	Al	0.2											O	z	7.19		1996																											2	M1212				3.841		11.404																16			16																																																																																														SrCO3,BaCO3,Y2O3,CuO,M-oxide	1	mixture-SIN-ANN(500C,1H,P=0.1MPa)-slow cool to RT-seal(Au capsule with K ClO3)-heat(580-800C,3H, P=2GPa)-Q to RT					Oxygenation and Critical-Temperature Optimization in M-1212 Cuprates (Sr,Ba)2 YCu2.8M0.2Oz (M=Ti,Ga,Ge,Al)			National Institute for Research in Inorganic Materials,1-1 Namiki, Tsukuba 305, Japan	J.Appl.Phys.Lett.35(1996)L201	Akira Ono		
7162	APJ0353378	average grain size=5micron	GaSr2Ca2Cu3O9	Ga1Sr2Ca2Cu3O9	Ga	1	Sr	2	Ca	2	Cu	3													O	9			1996																																																		70			70																																		HIR7162																																																														prepared under 6Gpa					Critical Current Densities and Lrreversibility field of High Tc Superconductors, GaSr2Ca2Cu3O9 and BSr2Can-1CunO2n+3 (n=3,4)			Department of Applied Physics, Tokyo Institute of Technology, Oh-okayama, Meguro, Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)3378	Eiji Takayama-Muromachi,Shan Yu,Tetsuya Kawashima,Yuichi Okuda		
7163	APJ0353378	average grain size<10micron	BSr2Ca2Cu3O9	B1Sr2Ca2Cu3O9	B	1	Sr	2	Ca	2	Cu	3													O	9			1996																																																		75			75																																		HIR7163																																																														prepared under 6Gpa					Critical Current Densities and Lrreversibility field of High Tc Superconductors, GaSr2Ca2Cu3O9 and BSr2Can-1CunO2n+3 (n=3,4)			Department of Applied Physics, Tokyo Institute of Technology, Oh-okayama, Meguro, Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)3378	Eiji Takayama-Muromachi,Shan Yu,Tetsuya Kawashima,Yuichi Okuda		
7164	APJ0353378	plate-like grain about 10 micron in size with random orientation	BSr2Ca3Cu4O11	B1Sr2Ca3Cu4O11	B	1	Sr	2	Ca	3	Cu	4													O	11			1996																																																		110			110																																		HIR7164																																																														prepared under 6Gpa					Critical Current Densities and Lrreversibility field of High Tc Superconductors, GaSr2Ca2Cu3O9 and BSr2Can-1CunO2n+3 (n=3,4)			Department of Applied Physics, Tokyo Institute of Technology, Oh-okayama, Meguro, Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)3378	Eiji Takayama-Muromachi,Shan Yu,Tetsuya Kawashima,Yuichi Okuda		
7165	JP00800527		YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7	6.93		1996																											3					3.823	3.889	11.679														91.4					91.4																																																																																														Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7166	JP00800527		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.985Ni0.015O6.92	Y	1	Ba	2	Cu	2.985	Ni	0.015													O	7	6.92		1996																											3					3.824	3.885	11.678														90.5					90.5																																																																																														Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7167	JP00800527		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.97Ni0.03O6.94	Y	1	Ba	2	Cu	2.97	Ni	0.03													O	z	6.94		1996																											3					3.825	3.886	11.674														88.5					88.5																																																																																														Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7168	JP00800527		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.955Ni0.045O6.95	Y	1	Ba	2	Cu	2.955	Ni	0.045													O	z	6.95		1996																											3					3.825	3.881	11.671														86.2					86.2																																																																																														Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7169	JP00800527		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O6.94	Y	1	Ba	2	Cu	2.94	Ni	0.06													O	z	6.94		1996																											3					3.826	3.877	11.668														83.5					83.5																																																																																														Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7170	JP00800527		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O6.96	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	z	6.96		1996																																3.831	3.874	11.664																																																																																																																	Y2O3,BaCO3,CuO,NiO	1	mixture-SIN(930C,48H in air)-pellet-ANN(950C,48H in flowing O2)-slow cool to 450C-ANN(450C,72H in O2)-slow cool to RT					Effect of Ni doping on the thermal expansion of the high-tc superconductor YBa2Cu3Oy			Department of Physics, St Stephen's College, University of Delhi, Delhi-110007, India	J.Phys.Condens,Matter, 8(1996)527	Ashok Rao		
7171	JAP0805169		(Nd,Ce)2CuO4	Nd1.82Ce0.18Cu1Oz	Nd	1.82	Ce	0.18	Cu	1															O	z			1996																												T'																					18				18																																																																						TP7171																									1	see phys.Rev.B,48(1993)13182,reduced sample					Thermoelectric power studies on Nd1.82-xSrxCe0.18CuOy:x%$0.18 superconductors			Department of Physics, Indian Institute of Technology, Powai, Bombay 400 076, India	J.Appl.Phys.80(1996)5169	A.V. Narlikar,B.D. Padalia,Okram G. Singh,Om Prakash,S.K. Agarwal		
7172	JAP0805169		(Nd,Sr,Ce)2CuO4	Nd1.73Sr0.09Ce0.18Cu1Oz	Nd	1.73	Sr	0.09	Ce	0.18	Cu	1													O	z			1996																												T'																			12		20				16																																																																						TP7172																									1	see phys.Rev.B,48(1993)13182,reduced sample					Thermoelectric power studies on Nd1.82-xSrxCe0.18CuOy:x%$0.18 superconductors			Department of Physics, Indian Institute of Technology, Powai, Bombay 400 076, India	J.Appl.Phys.80(1996)5169	A.V. Narlikar,B.D. Padalia,Okram G. Singh,Om Prakash,S.K. Agarwal		
7173	JAP0805169		(Nd,Sr,Ce)2CuO4	Nd1.64Sr0.18Ce0.18Cu1Oz	Nd	1.64	Sr	0.18	Ce	0.18	Cu	1													O	z			1996																												T'																			8		18				13																																																																						TP7173																									1	see phys.Rev.B,48(1993)13182,reduced sample					Thermoelectric power studies on Nd1.82-xSrxCe0.18CuOy:x%$0.18 superconductors			Department of Physics, Indian Institute of Technology, Powai, Bombay 400 076, India	J.Appl.Phys.80(1996)5169	A.V. Narlikar,B.D. Padalia,Okram G. Singh,Om Prakash,S.K. Agarwal		
7174	JAP0805169		(Nd,Sr,Ce)2CuO4	Nd1.64Sr0.18Ce0.18Cu1Oz	Nd	1.64	Sr	0.18	Ce	0.18	Cu	1													O	z			1996																												T'																							5																																																																								TP7174																										oxygenated sample see Phys.Rev.B,48(1993)13182					Thermoelectric power studies on Nd1.82-xSrxCe0.18CuOy:x%$0.18 superconductors			Department of Physics, Indian Institute of Technology, Powai, Bombay 400 076, India	J.Appl.Phys.80(1996)5169	A.V. Narlikar,B.D. Padalia,Okram G. Singh,Om Prakash,S.K. Agarwal		
7175	APJ0353383		Bi2Sr2CuOz	Bi2Sr1.8La0.2Cu1Oz	Bi	2	Sr	1.8	La	0.2	Cu	1													O	z			1996																											2	Bi2201				5.372		24.534														21					21																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7176	APJ0353383		Bi2(Sr,La)(Cu,Ni)Oz	Bi2Sr1.8La2Cu0.98Ni0.02Oz	Bi	2	Sr	1.8	La	2	Cu	0.98	Ni	0.02											O	z			1996																											2	Bi2201				5.374		24.53														17.5					17.5																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7177	APJ0353383		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La2Cu0.96Ni0.04Oz	Bi	2	Sr	1.8	La	2	Cu	0.96	Ni	0.04											O	z			1996																											2	Bi2201				5.376		24.522														12.9					12.9																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7178	APJ0353383		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La2Cu0.94Ni0.06Oz	Bi	2	Sr	1.8	La	2	Cu	0.94	Ni	0.06											O	z			1996																											2	Bi2201				5.378		24.486														10					10																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7179	APJ0353383		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La2Cu0.92Ni0.08Oz	Bi	2	Sr	1.8	La	2	Cu	0.92	Ni	0.08											O	z			1996																											2	Bi2201				5.38		24.405														3.6					3.6																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7180	APJ0353383		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La2Cu0.9Ni0.1Oz	Bi	2	Sr	1.8	La	2	Cu	0.9	Ni	0.1											O	z			1996																											2	Bi2201				5.391		24.392																																																																																																																	Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7181	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.88Zn0.12Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.88	Zn	0.12											O	z			1996																											2	Bi2201																				16.8					16.8																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7182	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.976Zn0.024Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.976	Zn	0.024											O	z			1996																											2	Bi2201				5.373		24.517														11.3					11.3																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7183	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.964Zn0.036Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.964	Zn	0.036											O	z			1996																											2	Bi2201				5.376		24.493														7					7																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7184	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.94Zn0.06Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.94	Zn	0.06											O	z			1996																											2	Bi2201				5.376		24.394														5					5																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7185	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.92Zn0.08Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.92	Zn	0.08											O	z			1996																											2	Bi2201				5.379		24.383														5.1					5.1																																																																																														Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7186	APJ0353383		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.9Zn0.1Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.9	Zn	0.1											O	z			1996																											2	Bi2201				5.39		24.333																																																																																																																	Bi2O3,SrCO3,La2O3,ZnO,NiO,CuO	1	mixture-CAL(810-830C,36H in air)-pellet-SIN(885-920C, in flowing O2)-Q to RT in air					Effect of Ni and Zn Substitutions for Cu in the 25 K Phase of Bi-Sr-La-Cu-O Superconductors			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	Jpn.J.Appl.Phys.35(1996)3383	Cunyi Xu,Gaojie Xu,Mike MCELFRESH,Mingliang Tian,Shi Li,Stephen M. DURBIN,Yu Wang,Yuheng ZHANG,Zhiqiang Mao		
7187	JPS0651548	size=2.6*0.8*0.05 and 2.5*0.9*0.2 mm3	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1996																																																																																																																			29								TP7187																										floating zone method					Thermopower of a Layered Perovskite Superconductor, Sr2RuO4	199606		Electrotechnical Laboratory, Tsukuba 305	J.Phys.Soc.Japan,65(1996)1548-1550	Harukazu YOSHINO,Keizo MURATA,Naoki SHIRAKAWA,Toshizo FUJITA,Yoshikazu NISHIHARA,Yoshiteru MAENO		
7188	JAP0800898		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	z	6.96		1996																											3	Y123				3.819	3.886	11.679														90.7					90.7																																																																						TP7188																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7189	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.975Co0.025Oz	Y	1	Ba	2	Cu	2.975	Co	0.025													O	z			1996																											3	Y123				3.823	3.887	11.685														91.6					91.6																																																																																															1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7190	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.95Co0.05Oz	Y	1	Ba	2	Cu	2.95	Co	0.05													O	z			1996																											3	Y123				3.827	3.886	11.679														92.2					92.2																																																																						TP7190																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7191	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.925Co0.075Oz	Y	1	Ba	2	Cu	2.925	Co	0.075													O	z			1996																											3	Y123				3.85	3.866	11.679														88.3					88.3																																																																																															1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7192	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.9Co0.1Oz	Y	1	Ba	2	Cu	2.9	Co	0.1													O	z			1996																											3	Y123				3.86		11.679														88.6					88.6																																																																																															1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7193	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.875Co0.125Oz	Y	1	Ba	2	Cu	2.875	Co	0.125													O	z			1996																											2					3.861		11.679														77.1					77.1																																																																																															1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7194	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15Oz	Y	1	Ba	2	Cu	2.85	Co	0.15													O	z			1996																											2					3.864		11.679														68.6					68.6																																																																						TP7194																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7195	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.8Co0.2Oz	Y	1	Ba	2	Cu	2.8	Co	0.2													O	z			1996																											2					3.867		11.682														61					61																																																																						TP7195																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7196	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.75Co0.25Oz	Y	1	Ba	2	Cu	2.75	Co	0.25													O	z			1996																											2					3.868		11.676														59.7					59.7																																																																						TP7196																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7197	JAP0800898		YBa2(Cu,Co)2O7	Y1Ba2Cu2.7Co0.3Oz	Y	1	Ba	2	Cu	2.7	Co	0.3													O	z			1996																											2					3.873		11.679														52.6					52.6																																																																						TP7197																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7198	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.6Co0.4O7.03	Y	1	Ba	2	Cu	2.6	Co	0.4													O	z	7.03		1996																											2					3.877		11.676														11.3					11.3																																																																						TP7198																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7199	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.5Co0.5O7.05	Y	1	Ba	2	Cu	2.5	Co	0.5													O	z	7.05		1996																											2					3.882		11.667																	10																																																																								TP7199																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7200	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.4Co0.6O7.08	Y	1	Ba	2	Cu	2.4	Co	0.6													O	z	7.08		1996																											2					3.888		11.658																	10																																																																								TP7200																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7201	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.3Co0.7O7.13	Y	1	Ba	2	Cu	2.3	Co	0.7													O	z	7.13		1996																											2					3.887		11.658																	10																																																																								TP7201																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7202	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.2Co0.8O7.18	Y	1	Ba	2	Cu	2.2	Co	0.8													O	z	7.18		1996																											2					3.89		11.655																	10																																																																								TP7202																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7203	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.1Co0.9O7.21	Y	1	Ba	2	Cu	2.1	Co	0.9													O	z	7.21		1996																											2	Y123				3.891		11.655																	10																																																																								TP7203																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7204	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2.05Co0.95Oz	Y	1	Ba	2	Cu	2.05	Co	0.95													O	z			1996																											2	Y123				3.891		11.637																	10																																																																																																	1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7205	JAP0800898		YBa2(Cu,Co)3O7	Y1Ba2Cu2Co1O7.33	Y	1	Ba	2	Cu	2	Co	1													O	z	7.33		1996																											2	Y123				3.892		11.619																	10																																																																								TP7205																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7206	JAP0800898		EuBa2Cu3O7	Eu1Ba2Cu3O6.94	Eu	1	Ba	2	Cu	3															O	z	6.94		1996																											3	Y123				3.841	3.906	11.712														93.6					93.6																																																																																															1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7207	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.95Co0.05Oz	Eu	1	Ba	2	Cu	2.95	Co	0.05													O	z			1996																											2	Y123				3.877		11.715														88.3					88.3																																																																						TP7207																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7208	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.9Co0.1O6.97	Eu	1	Ba	2	Cu	2.9	Co	0.1													O	z	6.97		1996																											2					3.883		11.718														72.7					72.7																																																																						TP7208																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7209	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.8Co0.2O6.98	Eu	1	Ba	2	Cu	2.8	Co	0.2													O	z	6.98		1996																											2					3.889		11.712														55.3					55.3																																																																						TP7209																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7210	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.7Co0.3O6.95	Eu	1	Ba	2	Cu	2.7	Co	0.3													O	z	6.95		1996																											2					3.895		11.703														29.4					29.4																																																																						TP7210																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7211	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.6Co0.4O7.02	Eu	1	Ba	2	Cu	2.6	Co	0.4													O	z	7.02		1996																											2					3.9		11.703																	10																																																																								TP7211																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7212	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.5Co0.5O7.05	Eu	1	Ba	2	Cu	2.5	Co	0.5													O	z	7.05		1996																											2					3.899		11.706																	10																																																																								TP7212																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7213	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.4Co0.6Oz	Eu	1	Ba	2	Cu	2.4	Co	0.6													O	z			1996																											2					3.906		11.685																	10																																																																								TP7213																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7214	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.3Co0.7O7.12	Eu	1	Ba	2	Cu	2.3	Co	0.7													O	z	7.12		1996																											2	Y123				3.908		11.67																	10																																																																								TP7214																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7215	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.2Co0.8Oz	Eu	1	Ba	2	Cu	2.2	Co	0.8													O	z			1996																											2	Y123				3.911		11.664																	10																																																																								TP7215																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7216	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2Co0.9O7.29	Eu	1	Ba	2	Cu	2	Co	0.9													O	z	7.29		1996																											2	Y123				3.913		11.652																	10																																																																								TP7216																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7217	JAP0800898		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2Co1O7.31	Eu	1	Ba	2	Cu	2	Co	1													O	z	7.31		1996																											2	Y123				3.912		11.634																	10																																																																								TP7217																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7218	JAP0800898		PrBa2Cu3Oz	Pr1Ba2Cu3O6.92	Pr	1	Ba	2	Cu	3															O	z	6.92		1996																											3	Y123				3.865	3.931	11.715																	10																																																																								TP7218																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7219	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.975Co0.025Oz	Pr	1	Ba	2	Cu	2.975	Co	0.025													O	z			1996																											3	Y123				3.879	3.92	11.703																	10																																																																								TP7219																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7220	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.95Co0.05Oz	Pr	1	Ba	2	Cu	2.95	Co	0.05													O	z			1996																											2	Y123				3.902		11.712																	10																																																																								TP7220																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7221	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.925Co0.075Oz	Pr	1	Ba	2	Cu	2.925	Co	0.075													O	z			1996																											2	Y123				3.903		11.712																	10																																																																								TP7221																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7222	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.9Co0.1Oz	Pr	1	Ba	2	Cu	2.9	Co	0.1													O	z			1996																											2	Y123				3.906		11.709																	10																																																																								TP7222																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7223	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.8Co0.2O6.99	Pr	1	Ba	2	Cu	2.8	Co	0.2													O	z	6.99		1996																											2	Y123				3.912		11.721																	10																																																																								TP7223																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7224	JAP0800898		Prba2(Cu,Co)3O7	Pr1Ba2Cu2.7Co0.3Oz	Pr	1	Ba	2	Cu	2.7	Co	0.3													O	z			1996																											2	Y123				3.916		11.712																	10																																																																																																	1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7225	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.6Co0.4O7.02	Pr	1	Ba	2	Cu	2.6	Co	0.4													O	z	7.02		1996																											2	Y123				3.922		11.724																	10																																																																								TP7225																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7226	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.5Co0.5Oz	Pr	1	Ba	2	Cu	2.5	Co	0.5													O	z			1996																											2	Y123				3.927		11.715																	10																																																																																																	1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7227	JAP0800898		Prba2(Cu,Co)3O7	Pr1Ba2Cu2.4Co0.6O7.08	Pr	1	Ba	2	Cu	2.4	Co	0.6													O	z	7.08		1996																											2	Y123				3.929		11.712																	10																																																																																																	1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7228	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba3Cu2.2Co0.8O7.15	Pr	1	Ba	3	Cu	2.2	Co	0.8													O	z	7.15		1996																											2	Y123				3.935		11.703																	10																																																																								TP7228																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7229	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2.1Co0.9Oz	Pr	1	Ba	2	Cu	2.1	Co	0.9													O	z			1996																											2	Y123				3.936		11.694																	10																																																																								TP7229																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7230	JAP0800898		PrBa2(Cu,Co)3O7	Pr1Ba2Cu2Co1O7.29	Pr	1	Ba	2	Cu	2	Co	1													O	z	7.29		1996																											2	Y123				3.939		11.679																	10																																																																								TP7230																									1	fully oxygenated sample,heat treated for several days at 350C under 1 atm O2					Fully oxygenated RBa2Cu3-xCoxOy,(R=Y,Eu,Pr,and 0%$x%$1)-from high-temperature superconductors to high-resistivity nonmetals			Physics Department and Crown Center for Superconductivity, Technion,Haifa 32000, Israel	J.Appl.Phys.80(1996)898	A. Knizhnik,B. Fisher,G. M. Reisner,G.M. Reisner,J. Genossar,L. Patlagan		
7231	PHC2700035	heat(200C,3H)	(Nd,Sr)2Cu(O,F)4	Nd0.7Sr1.3Cu1FO4-z	Nd	0.7	Sr	1.3	Cu	1	F														O	4-z		2	1996																												T				3.89		13.278															44				44																																																																																														nd2O3,SrCO3,CuO	1	precursor(Nd0.7Sr1.3CuO4):CuF2=1.0:1.1 (molar ratio) synthesized at various temp.					Synthesis and superconductivity of Nd0.7Sr1.3Cu(O,F)4-z with Tc=44 K			Institute of Physics,Chinese Academy of Sciences,Beijing 100080, China	Physica.C,270(1996)35-40	Liang Jingkui,Qin Yueling,Rao Guanghui,Shi Ying,Tang Weihua,Yang Jinling	Nd, Sr, Cu, O, F	
7232	PHC2700035	heat(240C,3H)	(Nd,Sr)2Cu(O,F)4	Nd0.7Sr1.3Cu1FO4-z	Nd	0.7	Sr	1.3	Cu	1	F														O	4-z		2	1996																												T				3.929		12.963															44				44																																																																																														nd2O3,SrCO3,CuO	1	precursor(Nd0.7Sr1.3CuO4):CuF2=1.0:1.1 (molar ratio) synthesized at various temp.					Synthesis and superconductivity of Nd0.7Sr1.3Cu(O,F)4-z with Tc=44 K			Institute of Physics,Chinese Academy of Sciences,Beijing 100080, China	Physica.C,270(1996)35-40	Liang Jingkui,Qin Yueling,Rao Guanghui,Shi Ying,Tang Weihua,Yang Jinling	Nd, Sr, Cu, O, F	
7233	PHC2700035	heat(300C,3H)	(Nd,Sr)2Cu(O,F)4	Nd0.7Sr1.3Cu1FO4-z	Nd	0.7	Sr	1.3	Cu	1	F														O	4-z		2	1996																												T				3.932		12.854																																																																																																																	nd2O3,SrCO3,CuO	1	precursor(Nd0.7Sr1.3CuO4):CuF2=1.0:1.1 (molar ratio) synthesized at various temp.					Synthesis and superconductivity of Nd0.7Sr1.3Cu(O,F)4-z with Tc=44 K			Institute of Physics,Chinese Academy of Sciences,Beijing 100080, China	Physica.C,270(1996)35-40	Liang Jingkui,Qin Yueling,Rao Guanghui,Shi Ying,Tang Weihua,Yang Jinling	Nd, Sr, Cu, O, F	
7234	JAP0802317		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1996																																3.822	3.893	11.682													89						89																																																																																														SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7235	JAP0802317		Y(Ba,Sr)2Cu3O7	Y1Ba1.5Sr0.5Cu3Oz	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z			1996																																															84						84																																																																																														SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7236	JAP0802317		Y(Ba,Sr)2Cu3O7	Y1Ba1Sr1Cu3Oz	Y	1	Ba	1	Sr	1	Cu	3													O	z			1996																																															82.5						82.5																																																																																														SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7237	JAP0802317		Y(Ba,Sr)2Cu3O7	Y1Ba0.5Sr1.5Cu3Oz	Y	1	Ba	0.5	Sr	1.5	Cu	3													O	z			1996																																																																																																																																																			SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7238	JAP0802317		Y(Ba,Sr)2Cu3O7	Y1Ba0.4Sr1.6Cu3Oz	Y	1	Ba	0.4	Sr	1.6	Cu	3													O	z			1996																																															79.5						79.5																																																																																														SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7239	JAP0802317	sample contains 5-30% impurities such as YBa2.5Sr0.4Cu4Oz, semiconductor	YSr2Cu3O7	Y1Sr2Cu3Oz	Y	1	Sr	2	Cu	3															O	z			1996																																																			50																																																																																																SrCO3,BaCO3,Y2O3,CuO		mixture-CAL(950C,10H in flowing O2)-SIN(960C,12H)-cool to RT (1C/min)					Semiconductivity in YBa2-xSrxCu3Oy			"Department of Physics, Ino""nu"" University of Arts and Science, Malatya,Turkey"	J.Appl.Phys.80(1996)2317	A. Ulug,B. Ulug,E. Sener		
7240	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	z	6.4		1996																												Y123																												K/GPa	1.6																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7241	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	z	6.45		1996																												Y123																												K/GPa	2.3																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7242	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	z	6.52		1996																												Y123																												K/GPa	3																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7243	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.58	Y	1	Ba	2	Cu	3															O	z	6.58		1996																												Y123																						57.4			57.4			K/GPa	6																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7244	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7		1996																												Y123																												K/GPa	6.8																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7245	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95		1996																												Y123																												K/GPa	0.15																																																																																												For single crystel,see J.Cryst.Growth 132(1993)389					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7246	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	z	6.4		1996																												Y123																												K/GPa	2.33																																																																																												To adjust the oxygen content, annealed at various O2 partial pressure and quenched to Liq,N2					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7247	PHC2700258		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	z	6.45		1996																												Y123																												K/GPa	1.78																																																																																												To adjust the oxygen content, annealed at various O2 partial pressure and quenched to Liq,N2					Giant pressure effect in oxygen deficient YBa2Cu3Ox			"forschungszentrum Karlsruhe, Institut fu""r Technische Physik,Postfach 3640,d-76021 Karlsruhe, Germany"	Physica.C,270(1996)258-266	"A. Erd,F.W. Hornung,G. Mu""ller-Vogt,H.A. Ludwig,K. Grube,M. Kla""ser,R. Quenzel,S.I. Schlachter,T. Wolf,W.H. Fietz"	Y, Ba, Cu, O	
7248	PHC2700327		CaYCuO3Cl	Ca1Y1Cu1Cl1O3	Ca	1	Y	1	Cu	1	Cl	1													O	3		1	1996																											2	T*				3.86		13.349																	5																																																																																																R2O3,CuO,CaO,CuCl2	1	mixture-CAL(800C,15H in flowing O2)-addition(KClO4)-seal in Au capsule-heat(900C,IH under 6GPa using cubic-anvil-tyne apparatus)					New oxychlorides, T*-type CaRCuO3Cl(R=Y, Ho, and Er), prepared under high pressure			Superconductivity Research Laboratory, International Superconductivity Technology Center,10-13 Shinonome 1-Chome,Koto-Ku, Tokyo 135, Japan	Physica.C,270(1996)327-332	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki,X.-J. Wu,Y. Moriwaki	Ca, Y, Ho, Er, Cu, O, Cl	
7249	PHC2700327		CaHoCuO3Cl	Ca1Ho1Cu1Cl1Oz	Ca	1	Ho	1	Cu	1	Cl	1													O	z		1	1996																											2	T*				3.85		13.349																	5																																																																																																R2O3,CuO,CaO,CuCl2	1	mixture-CAL(800C,15H in flowing O2)-addition(KClO4)-seal in Au capsule-heat(900C,IH under 6GPa using cubic-anvil-tyne apparatus)					New oxychlorides, T*-type CaRCuO3Cl(R=Y, Ho, and Er), prepared under high pressure			Superconductivity Research Laboratory, International Superconductivity Technology Center,10-13 Shinonome 1-Chome,Koto-Ku, Tokyo 135, Japan	Physica.C,270(1996)327-332	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki,X.-J. Wu,Y. Moriwaki	Ca, Y, Ho, Er, Cu, O, Cl	
7250	PHC2700327		CaErCuO3Cl	Ca1Er1Cu1Cl1O3	Ca	1	Er	1	Cu	1	Cl	1													O	3		1	1996																											2	T*				3.84		13.34																	5																																																																																																R2O3,CuO,CaO,CuCl2	1	mixture-CAL(800C,15H in flowing O2)-addition(KClO4)-seal in Au capsule-heat(900C,IH under 6GPa using cubic-anvil-tyne apparatus)					New oxychlorides, T*-type CaRCuO3Cl(R=Y, Ho, and Er), prepared under high pressure			Superconductivity Research Laboratory, International Superconductivity Technology Center,10-13 Shinonome 1-Chome,Koto-Ku, Tokyo 135, Japan	Physica.C,270(1996)327-332	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki,X.-J. Wu,Y. Moriwaki	Ca, Y, Ho, Er, Cu, O, Cl	
7251	PHC2690076	annealed at 0.05 mbar O2	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4+z	Pr	1.85	Ce	0.15	Cu	1															O	4+z		3	1996																											2	T'						12.135													23.2						23.2																																																																																															5	standard CuO flux method, the size=about 2*2*0.01 mm3					Residual resistivity and oxygen stoichiometry in Pr2-xCexCuO4+z single crystals			"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universita""t Bochum, Germany"	Physica.C,269(1996)76-82	Henrich Bach,Kurt Westerholt,Markus Stief,Matthias Brinkmann,Thomas Rex	Pr, Ce, Cu, O	
7252	PHC2690076	annealed at 0.05 mbar O2	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4+z	Pr	1.85	Ce	0.15	Cu	1															O	4+z		3	1996																											2	T'						12.137													23.3						23.3																																																																																															5	standard CuO flux method, the size=about 2*2*0.01 mm3					Residual resistivity and oxygen stoichiometry in Pr2-xCexCuO4+z single crystals			"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universita""t Bochum, Germany"	Physica.C,269(1996)76-82	Henrich Bach,Kurt Westerholt,Markus Stief,Matthias Brinkmann,Thomas Rex	Pr, Ce, Cu, O	
7253	PHC2690076	annealed at 0.17 mbar O2	(Pr,Ce)2CuO4	Pr1.9Ce0.1Cu1O4+z	Pr	1.9	Ce	0.1	Cu	1															O	4+z		3	1996																											2	T'						12.175													24.3						24.3																																																																																															5	standard CuO flux method, the size=about 2*2*0.01 mm3					Residual resistivity and oxygen stoichiometry in Pr2-xCexCuO4+z single crystals			"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universita""t Bochum, Germany"	Physica.C,269(1996)76-82	Henrich Bach,Kurt Westerholt,Markus Stief,Matthias Brinkmann,Thomas Rex	Pr, Ce, Cu, O	
7254	PHC2690076	annealed for 3days+5days at 0.05 mbar O2	(Pr,Ce)2CuO4	Pr1.93Ce0.07Cu1O4+z	Pr	1.93	Ce	0.07	Cu	1															O	4+z		3	1996																											2	T'						12.201													22.7						22.7																																																																																															5	standard CuO flux method, the size=about 2*2*0.01 mm3					Residual resistivity and oxygen stoichiometry in Pr2-xCexCuO4+z single crystals			"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universita""t Bochum, Germany"	Physica.C,269(1996)76-82	Henrich Bach,Kurt Westerholt,Markus Stief,Matthias Brinkmann,Thomas Rex	Pr, Ce, Cu, O	
7255	PHC2690225	semiconductor	TlSr2YbCu2O7	Tl1Sr2Yb1Cu2O7	Tl	1	Sr	2	Yb	1	Cu	2													O	z	7	1	1996																											2	Tl1212				3.805		11.988																	5																																																																																																Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7256	PHC2690225		TlSr2(Yb,Ca)Cu2Oz	Tl1Sr2Yb0.7Ca0.3Cu2Oz	Tl	1	Sr	2	Yb	0.7	Ca	0.3	Cu	2											O	z		1	1996																											2	Tl1212				3.7945		12.012														83		80			83																																																																																														Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7257	PHC2690225		TlSr2(Yb,Ca)Cu2Oz	Tl1Sr2Yb0.5Ca0.5Cu2Oz	Tl	1	Sr	2	Yb	0.5	Ca	0.5	Cu	2											O	z		1	1996																											2	Tl1212				3.7905		12.048														67		68			67																																																																																														Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7258	PHC2690225		TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O6.8	Tl	1	Sr	2	Ca	1	Cu	2													O	z	6.8	1	1996																											2	Tl1212				3.7852		12.133																	18																																																																																																Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7259	PHC2690225		TlSr2(Yb,Ca)Cu2Oz	Tl1Sr2Yb0.7Ca0.3Cu2Oz	Tl	1	Sr	2	Yb	0.7	Ca	0.3	Cu	2											O	z		1	1996																											2	Tl1212																				83		80			83																																																																																														Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7260	PHC2690225		TlSr2(Yb,Ca)Cu2Oz	Tl1Sr2Yb0.5Ca0.5Cu2Oz	Tl	1	Sr	2	Yb	0.5	Ca	0.5	Cu	2											O	z		1	1996																											2	Tl1212																				67		68			67																																																																																														Sr2CuO3,CaO,Yb2O3,CuO,Tl2O3	1	(mixture with excess Tl2O3)-pellet-put into Au bags-heat(910-930C,9-12 in flowing O2)					Superconductivity in TlSr2-xCaYbCu2O7 by isovalent cation substitution			Institute for Materials Research,Tohoku University,Katahira,Aoba-ku,Sendai 980-77, Japan	Physica.C,269(1996)225-230	Eriko Ohshima,Masae Kikuchi,Yasuhiko Syono	Tl, Sr, Ca, Yb, Cu, O	
7261	PR05407505			Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		6	1996																												Hg1201																						95.1			95.1										36											from WHH theory	80									1.2			HC7261					2																																																							HgO,BaO,CaO,CuO		mixture-monocastalline powder(about 75m)-dispersion in epexy-magnetically align in 5T					Comparatives study of the characteristic length scales snd filds of Hg-based high-Tc superconductors	199609		Oak Ridge National Laboratory,P.O. box 2008, Oak Ridge, Tennesse 37831-6061	Phys.Rev.B,54(1996)7505	J.G. Ossandon,J.R. Tompson,Y.C. Kim		
7262	PR05407505			Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z		6	1996																												Hg1212																						122.5			122.5										87												135									1.6			HC7262					1.6																																																							HgO,BaO,CaO,CuO		mixture-monocastalline powder(about 75m)-dispersion in epexy-magnetically align in 5T					Comparatives study of the characteristic length scales snd filds of Hg-based high-Tc superconductors	199609		Oak Ridge National Laboratory,P.O. box 2008, Oak Ridge, Tennesse 37831-6061	Phys.Rev.B,54(1996)7505	J.G. Ossandon,J.R. Tompson,Y.C. Kim		
7263	PR05407505			Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z		6	1996																												Hg1223																						133.5			133.5										77												190									1.3			HC7263					1.3																																																							HgO,BaO,CaO,CuO		mixture-monocastalline powder(about 75m)-dispersion in epexy-magnetically align in 5T					Comparatives study of the characteristic length scales snd filds of Hg-based high-Tc superconductors	199609		Oak Ridge National Laboratory,P.O. box 2008, Oak Ridge, Tennesse 37831-6061	Phys.Rev.B,54(1996)7505	J.G. Ossandon,J.R. Tompson,Y.C. Kim		
7264	PR05406881		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1996																												Bi2212																			84						84																																					by fitting the fluchuation-renormalizedGL theory to resistivity data		10	0.1																																																							7	single crystal-annealed in air at 600 c for 24h~36h-cooled under equilibrium oxygen pressure					Evidence of the temperature-dependent interlayer coupling from the anisotropic transport properties in Co-substituted single-crystal Bi2Sr2Ca(Cu1-xCox)2O8+z	199609		NTT Basic research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-Shi, Kanagawa,243-01, Japan	Phys.Rev.B,54(1996)R6881	A. Matsuda,T. Watanabe		
7265	PR05406881		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.92Co0.08O8+z	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	8+z		3	1996																												Bi2212																			60						60																																					by fiting the fluctuation-ronormalized GL theory to resistivity data		13	0.1																																																							7	single crystal-annealed in air at 600 c for 24h~36h-cooled under equilibrium oxygen pressure					Evidence of the temperature-dependent interlayer coupling from the anisotropic transport properties in Co-substituted single-crystal Bi2Sr2Ca(Cu1-xCox)2O8+z	199609		NTT Basic research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-Shi, Kanagawa,243-01, Japan	Phys.Rev.B,54(1996)R6881	A. Matsuda,T. Watanabe		
7266	PR05407455		La2CuO4	La2Cu1O0.001	La	2	Cu	1																	O	4+z	0.001	3	1996																												T																																																																																																																								7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7267	PR05407455		La2CuO4	La2Cu1O4.005	La	2	Cu	1																	O	4+z	4.005	3	1996																												T																				32					32																																																																																															7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7268	PR05407455		La2CuO4	La2Cu1O4.011	La	2	Cu	1																	O	4+z	4.011	3	1996																												T																																																																																																																								7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7269	PR05407455		La2CuO4	La2Cu1O4.015	La	2	Cu	1																	O	4+z	4.015	3	1996																												T																																																																																																																								7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7270	PR05407455		La2CuO4	La2Cu1O4.021	La	2	Cu	1																	O	4+z	4.021	3	1996																												T																																																																																																																								7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7271	PR05407455		La2CuOz	La2Cu1O4.035	La	2	Cu	1																	O	4+z	4.035	3	1996																												T																				35					35																																																																																															7	TSFZ single crystal-high temperature annealing under different partial pressure of oxygen O2z20.035					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7272	PR05407455	TP=in ab-plane,TP(2)-parallel to c-axis	La2CuO4	La2Cu1O4.021	La	2	Cu	1																	O	4+z	4.021	4	1996																												T																				45					45																																																																																																7266-electrochemical oxidation for 40 days.					Effect of oxygen content on the anomalies at successive phase transitions of La2CuO4+z single crystal below 320 K	199609		Reserch Laboratory of Engineering Materials,Tokyo Institute of Technology, 4259 Nagatsuta,Midori-ku Yokohama 226, Japan	Phys.Rev.B,54(1996)7455	Jian Ding Yu,Masaharu Oguni,Mitsuru Itoh,To^ru Kyo^men,Yoshiyuki Inaguma		
7273	PR05414956	delta Tc=0.05K	YBa2Cu3O2	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	z	6.94		1996																											3	Y123				3.821	3.884	11.687																93			93	ISO7273					-0.017	Cu		0.05																																																																																					Y2O3,BaCO2,(63)CuO,(65)CuO	1	mixture-CAL(920C,15H)-pellet-SIN(920C,15H in flowing O2)-ANN(800C,10H in flowing O2)-cool to RT-ANN(670C,12H in O2)-cool to 120C(50C/H)					Large copper isotope effect in oxygen depleted YBa2Cu3Oy: Importance of Cu-dominated phonon modes in the pairing mechanism	199612		Morris Reserch,Inc,44 marguerita Road,Kensington,california 94707	Phys.Rev.B,54(1996)14956	A.P.B. Sinha,A.V. Inyushkin,Donald E. Morris,Guo-meng Zhao,K.K. Singh,Vidula Kirtikar		
7274	PR05414956	delta Tc=-0.57K	YBa2Cu3Oz	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	z	6.75		1996																												Y123																						73			73						0.25	Cu		-0.57																																																																																					Y2O3,BaCO2,(63)CuO,(65)CuO	1	mixture-CAL(920C,15H)-pellet-SIN(920C,15H in flowing O2)-ANN(800C,10H in flowing O2)-cool to RT-ANN(670C,12H in O2)-cool to 120C(50C/H)					Large copper isotope effect in oxygen depleted YBa2Cu3Oy: Importance of Cu-dominated phonon modes in the pairing mechanism	199612		Morris Reserch,Inc,44 marguerita Road,Kensington,california 94707	Phys.Rev.B,54(1996)14956	A.P.B. Sinha,A.V. Inyushkin,Donald E. Morris,Guo-meng Zhao,K.K. Singh,Vidula Kirtikar		
7275	PR05414956	delta Tc=-0.7K	YBa2Cu3Oz	Y1Ba2Cu3O6.63	Y	1	Ba	2	Cu	3															O	z	6.63		1996																												Y123																						60			60						0.37	Cu		-0.7																																																																																					Y2O3,BaCO2,(63)CuO,(65)CuO	1	mixture-CAL(920C,15H)-pellet-SIN(920C,15H in flowing O2)-ANN(800C,10H in flowing O2)-cool to RT-ANN(670C,12H in O2)-cool to 120C(50C/H)					Large copper isotope effect in oxygen depleted YBa2Cu3Oy: Importance of Cu-dominated phonon modes in the pairing mechanism	199612		Morris Reserch,Inc,44 marguerita Road,Kensington,california 94707	Phys.Rev.B,54(1996)14956	A.P.B. Sinha,A.V. Inyushkin,Donald E. Morris,Guo-meng Zhao,K.K. Singh,Vidula Kirtikar		
7276	PR05414956	delta Tc=-0.57	YBa2Cu3Oz	Y1Ba2Cu3O6.48	Y	1	Ba	2	Cu	3															O	z	6.48		1996																												Y123																						48.5			48.5						0.37	Cu		-0.57																																																																																					Y2O3,BaCO2,(63)CuO,(65)CuO	1	mixture-CAL(920C,15H)-pellet-SIN(920C,15H in flowing O2)-ANN(800C,10H in flowing O2)-cool to RT-ANN(670C,12H in O2)-cool to 120C(50C/H)					Large copper isotope effect in oxygen depleted YBa2Cu3Oy: Importance of Cu-dominated phonon modes in the pairing mechanism	199612		Morris Reserch,Inc,44 marguerita Road,Kensington,california 94707	Phys.Rev.B,54(1996)14956	A.P.B. Sinha,A.V. Inyushkin,Donald E. Morris,Guo-meng Zhao,K.K. Singh,Vidula Kirtikar		
7277	PR05406680		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4+z	Pr	1.85	Ce	0.15	Cu	1															O	4+z		3	1996																												T'						12.132														22.9					22.9																																		HC7277																																																													5	Slow cooling CuO self-feux method					Superconductivity of Pr2-xCexCuO4+z single crystals with substitution of Ni and Co on the Cu position	199609		"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universta""t Bochum,D-44780 Bochum, Germany"	Phys.Rev.B,54(1996)6680	Heinrich Bach,Kurt Westerholt,Matthias Brinkmann		
7278	PR05406680		(Pr,Ce)2(Cu,Ni)O4	Pr1.87Ce0.13Cu0.997Ni0.003O4+z	Pr	1.87	Ce	0.13	Cu	0.997	Ni	0.003													O	4+z		3	1996																												T'						12.147														18					18																																		HC7278																																																													5	Slow cooling CuO self-feux method					Superconductivity of Pr2-xCexCuO4+z single crystals with substitution of Ni and Co on the Cu position	199609		"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universta""t Bochum,D-44780 Bochum, Germany"	Phys.Rev.B,54(1996)6680	Heinrich Bach,Kurt Westerholt,Matthias Brinkmann		
7279	PR05406680		(Pr,Ce)2(Cu,Ni)O4	Pr1.84Ce0.16Cu0.993Ni0.007O4+z	Pr	1.84	Ce	0.16	Cu	0.993	Ni	0.007													O	4+z		3	1996																												T'						12.125														12.2					12.2																																		HC7279																																																													5	Slow cooling CuO self-feux method					Superconductivity of Pr2-xCexCuO4+z single crystals with substitution of Ni and Co on the Cu position	199609		"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universta""t Bochum,D-44780 Bochum, Germany"	Phys.Rev.B,54(1996)6680	Heinrich Bach,Kurt Westerholt,Matthias Brinkmann		
7280	PR05406680		(Pr,Ce)2(Cu,Co)O4	Pr1.85Ce0.15Cu0.995Co0.005O4+z	Pr	1.85	Ce	0.15	Cu	0.995	Co	0.005													O	4+z		3	1996																												T'						12.13														14.1					14.1																																		HC7280																																																													5	Slow cooling CuO self-feux method					Superconductivity of Pr2-xCexCuO4+z single crystals with substitution of Ni and Co on the Cu position	199609		"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universta""t Bochum,D-44780 Bochum, Germany"	Phys.Rev.B,54(1996)6680	Heinrich Bach,Kurt Westerholt,Matthias Brinkmann		
7281	PR05406680		(Pr,Ce)2(Cu,Co)O4	Pr1.87Ce0.13Cu0.99Co0.01O4+z	Pr	1.87	Ce	0.13	Cu	0.99	Co	0.01													O	4+z		3	1996																												T'						12.145														8.2					8.2																																																																																															5	Slow cooling CuO self-feux method					Superconductivity of Pr2-xCexCuO4+z single crystals with substitution of Ni and Co on the Cu position	199609		"Institut fu""r Experimentalphysik/Festko""rperphysik,Ruhr-Universta""t Bochum,D-44780 Bochum, Germany"	Phys.Rev.B,54(1996)6680	Heinrich Bach,Kurt Westerholt,Matthias Brinkmann		
7282	SST0090399	Mossbauer:hyperfine parameters of Eu-site,	PbSr2YCu3O8	Pb2Sr2Y1Cu3O8+z	Pb	2	Sr	2	Y	1	Cu	3													O	8+z		1	1996																											3	Pb3212				5.388	5.427	15.712																	77																																																																																																PbO,SrCO3,Y2O3,Eu2O3,CuO		mixture-CAL(800C,15H+900C,IH in air)-pellet-heat(800C,5H in N2),grain alignment(powder) by magnetic field					"Investigations of the Pb2Sr2Y1-xEuxCu3O8+z system by 151Eu Mo""ssbauer resonance and x-ray diffraction"			Department of Technical Physics, Helsinki University of Technology, FIN-02150 Espoo, Finland	Supercond.Sci.Technol.9(1996)399	J Linde'n,L Niinisto,M Karppinen,M Lippmaa,T Karlemo		
7283	SST0090399	Mossbauer: hyperfine parameyers of Eu-site,	Pb2Sr2(Y,Eu)Cu3O8	Pb2Sr2Y0.75Eu0.25Cu3O8+z	Pb	2	Sr	2	Y	0.75	Eu	0.25	Cu	3											O	8+z		1	1996																											3	Pb3212				5.396	5.434	15.727																	77																																																																																																PbO,SrCO3,Y2O3,Eu2O3,CuO		mixture-CAL(800C,15H+900C,IH in air)-pellet-heat(800C,5H in N2),grain alignment(powder) by magnetic field					"Investigations of the Pb2Sr2Y1-xEuxCu3O8+z system by 151Eu Mo""ssbauer resonance and x-ray diffraction"			Department of Technical Physics, Helsinki University of Technology, FIN-02150 Espoo, Finland	Supercond.Sci.Technol.9(1996)399	J Linde'n,L Niinisto,M Karppinen,M Lippmaa,T Karlemo		
7284	SST0090399	Mossbauer: hyperfine parameters of Eu-Site, gamma=2.18mm/s	Pb2Sr2(Y,Eu)Cu3O8	Pb2Sr2Y0.5Eu0.5Cu3O8+z	Pb	2	Sr	2	Y	0.5	Eu	0.5	Cu	3											O	8+z		1	1996																											3	Pb3212				5.403	5.441	15.73																	77																																																																																																PbO,SrCO3,Y2O3,Eu2O3,CuO		mixture-CAL(800C,15H+900C,IH in air)-pellet-heat(800C,5H in N2),grain alignment(powder) by magnetic field					"Investigations of the Pb2Sr2Y1-xEuxCu3O8+z system by 151Eu Mo""ssbauer resonance and x-ray diffraction"			Department of Technical Physics, Helsinki University of Technology, FIN-02150 Espoo, Finland	Supercond.Sci.Technol.9(1996)399	J Linde'n,L Niinisto,M Karppinen,M Lippmaa,T Karlemo		
7285	SST0090399	Mossbauer:hyperfine parameters of Eu-site, gamma=2.20mm/s	Pb2Sr2(Y,Eu)Cu3O8	Pb2Sr2Y0.25Eu0.75Cu3O8+z	Pb	2	Sr	2	Y	0.25	Eu	0.75	Cu	3											O	8+z		1	1996																											3	Pb3212				5.409	5.448	15.744																	77																																																																																																PbO,SrCO3,Y2O3,Eu2O3,CuO		mixture-CAL(800C,15H+900C,IH in air)-pellet-heat(800C,5H in N2),grain alignment(powder) by magnetic field					"Investigations of the Pb2Sr2Y1-xEuxCu3O8+z system by 151Eu Mo""ssbauer resonance and x-ray diffraction"			Department of Technical Physics, Helsinki University of Technology, FIN-02150 Espoo, Finland	Supercond.Sci.Technol.9(1996)399	J Linde'n,L Niinisto,M Karppinen,M Lippmaa,T Karlemo		
7286	SST0090399	Mossbauer:hyperfine parameters of Eu-Site, gamma=2.25mm/s	Pb2Sr2(Y,Eu)Cu3O8	Pb2Sr2Eu1Cu3O8+z	Pb	2	Sr	2	Eu	1	Cu	3													O	8+z		1	1996																											3	Pb3212				5.415	5.454	15.738																	77																																																																																																PbO,SrCO3,Y2O3,Eu2O3,CuO		mixture-CAL(800C,15H+900C,IH in air)-pellet-heat(800C,5H in N2),grain alignment(powder) by magnetic field					"Investigations of the Pb2Sr2Y1-xEuxCu3O8+z system by 151Eu Mo""ssbauer resonance and x-ray diffraction"			Department of Technical Physics, Helsinki University of Technology, FIN-02150 Espoo, Finland	Supercond.Sci.Technol.9(1996)399	J Linde'n,L Niinisto,M Karppinen,M Lippmaa,T Karlemo		
7287	SST0090197		(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.6Pb0.4Sr2Ca3.6Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	3.6													O	z		2	1996																											3	Bi2223				5.451	5.426	36.83													102						102																																																																																														Bi2O3,CuO,SrCO3,CaCO3,PbO	1	mixture-SIN(820C,15H)-SIN(845C,24H in air)-FC to RT-ANN(845C 144H in air)					High-Tc superconductivity in Bi1.6Pb0.4Sr2Ca2Cu2+xOy compounds			Thermal Physics Laboratory, Department of Physics, Quaid-I-Azam University, Islamabad, Pakistan	Supercond.Sci.Technol.9(1996)197	Anwar-ul-Haq,Asghari Maqsood,Mohammad Yousaf,Muhammad Maqsood,S M Ramay,Zahida Ali		
7288	SST0090197		(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.6Pb0.4Sr2Ca2Cu3.8Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3.8											O	z		2	1996																											3	Bi2223				5.413	5.444	37.05													93						93																																																																																														Bi2O3,CuO,SrCO3,CaCO3,PbO	1	mixture-SIN(820C,15H)-SIN(845C,24H in air)-FC to RT-ANN(845C 144H in air)					High-Tc superconductivity in Bi1.6Pb0.4Sr2Ca2Cu2+xOy compounds			Thermal Physics Laboratory, Department of Physics, Quaid-I-Azam University, Islamabad, Pakistan	Supercond.Sci.Technol.9(1996)197	Anwar-ul-Haq,Asghari Maqsood,Mohammad Yousaf,Muhammad Maqsood,S M Ramay,Zahida Ali		
7289	SST0090197		(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.6Pb0.4Sr2Ca2Cu4Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	4											O	z		2	1996																											3	Bi2223				5.416	5.448	37.27													130						130																																																																																														Bi2O3,CuO,SrCO3,CaCO3,PbO	1	mixture-SIN(820C,15H)-SIN(845C,24H in air)-FC to RT-ANN(845C 144H in air)					High-Tc superconductivity in Bi1.6Pb0.4Sr2Ca2Cu2+xOy compounds			Thermal Physics Laboratory, Department of Physics, Quaid-I-Azam University, Islamabad, Pakistan	Supercond.Sci.Technol.9(1996)197	Anwar-ul-Haq,Asghari Maqsood,Mohammad Yousaf,Muhammad Maqsood,S M Ramay,Zahida Ali		
7290	JAC2340207		HgBa2EuCu2O6	Hg1Ba2Eu1Cu2O6+z	Hg	1	Ba	2	Eu	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.893		12.568																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7291	JAC2340207		HgBa2GdCu2O6	Hg1Ba2Gd1Cu2O6+z	Hg	1	Ba	2	Gd	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.893		12.548																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7292	JAC2340207		HgBa2HoCu2O6	Hg1Ba2Ho1Cu2O6+z	Hg	1	Ba	2	Ho	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.877		12.522																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7293	JAC2340207		HgBa2ErCu2O6	Hg1Ba2Er1Cu2O6+z	Hg	1	Ba	2	Er	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.869		12.493																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7294	JAC2340207		HgBa2TmCu2O6	Hg1Ba2Tm1Cu2O6+z	Hg	1	Ba	2	Tm	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.863		12.481																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7295	JAC2340207		HgBa2YbCu2O6	Hg1Ba2Yb1Cu2O6+z	Hg	1	Ba	2	Yb	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.857		12.478																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7296	JAC2340207		HgBa2YCu2O6	Hg1Ba2Y1Cu2O6+z	Hg	1	Ba	2	Y	1	Cu	2													O	6+z		2	1996																											2	Hg1212				3.87		12.515																	12																																																																																																R2O3,Ba(NO3)2,CuO,HgO	1	mixture-heat(500C,in dynamic vacuum)-add(HgO)-ANN(650C,100H),as preparad sample					Synthesis and characterization of HgBa2RCu2O6+z (R=Eu, Gd, Ho, Er, Tm, Yd, and Y)			Department of Inorganic Chemistry, Moscow State University,Moscow 119899, Russia	J.Alloys Compd234(1996)207	E.M. Kopnin,E.V. Antipov,M.G. ROZOVA,M.L. Kovba,M.V. Lobanov,O.I. Lebedev,S.N. Putilin		
7297	MPL0091397	synthesis conditions=55Kbar,870C,1.2H using graphite furnace	(Cu,Ag)Ba2Ca3Cu4Oz	Cu0.75Ag0.25Ba2Ca3Cu4Oz	Cu	0.75	Ag	0.25	Ba	2	Ca	3	Cu	4											O	z		2	1995																																															100		124				112																																																																																																precursor (Cu1-xMxBa2Ca3Cu4Oz,x=0,0.25,0.75:M=Ag or C)-powder-wrapeed in Au-foil-heat (820-1200C,0.5 or 1.5 H under high pressure)-RT(20C/min)					124K superconductivity in Cu-Ba-Ca-Cu-O				Mod.Phys.Lett.B,9(1995)1397-1406	C.W. Chu,I. Rusakova,L. Gao,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
7298	MPL0091397	synthesis conditions=55Kbar,870C,1.3H using Ca-doped Ka2CrO4 furnace	(Cu,Ag)Ba2Ca3Cu4Oz	Cu0.75Ag0.25Ba2Ca3Cu4Oz	Cu	0.75	Ag	0.25	Ba	2	Ca	3	Cu	4											O	z		2	1995																																															80		117				98.5																																																																																																precursor (Cu1-xMxBa2Ca3Cu4Oz,x=0,0.25,0.75:M=Ag or C)-powder-wrapeed in Au-foil-heat (820-1200C,0.5 or 1.5 H under high pressure)-RT(20C/min)					124K superconductivity in Cu-Ba-Ca-Cu-O				Mod.Phys.Lett.B,9(1995)1397-1406	C.W. Chu,I. Rusakova,L. Gao,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
7299	MPL0091397	synthesis conditions=55Kbar,1200C,155H using Ca-doped La2CrO4 furnace	(Cu,C)Ba2Ca3Cu4Oz	Cu0.5C0.5Ba2Ca3Cu4Oz	Cu	0.5	C	0.5	Ba	2	Ca	3	Cu	4											O	z		2	1995																																																110					110																																																																																																precursor (Cu1-xMxBa2Ca3Cu4Oz,x=0,0.25,0.75:M=Ag or C)-powder-wrapeed in Au-foil-heat (820-1200C,0.5 or 1.5 H under high pressure)-RT(20C/min)					124K superconductivity in Cu-Ba-Ca-Cu-O				Mod.Phys.Lett.B,9(1995)1397-1406	C.W. Chu,I. Rusakova,L. Gao,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
7300	MPL0091397	synthesis conditions=60Kbar,1000c,3.0H using Ca=doped La2CrO4 furnace	(Cu,Ag)Ba2Ca3Cu4Oz	Cu0.5Ag0.25Ba2Ca3Cu4Oz	Cu	0.5	Ag	0.25	Ba	2	Ca	3	Cu	4											O	z		2	1995																																																117					117																																																																																																precursor (Cu1-xMxBa2Ca3Cu4Oz,x=0,0.25,0.75:M=Ag or C)-powder-wrapeed in Au-foil-heat (820-1200C,0.5 or 1.5 H under high pressure)-RT(20C/min)					124K superconductivity in Cu-Ba-Ca-Cu-O				Mod.Phys.Lett.B,9(1995)1397-1406	C.W. Chu,I. Rusakova,L. Gao,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
7301	MPL0091397	synthesis conditions=55Kbar,950C,1.0H using graphite furnace	Ba2Ca3Cu4Oz	Ba2Ca3Cu4Oz	Ba	2	Ca	3	Cu	4															O	z		2	1995																																																117					117																																																																																																precursor (Cu1-xMxBa2Ca3Cu4Oz,x=0,0.25,0.75:M=Ag or C)-powder-wrapeed in Au-foil-heat (820-1200C,0.5 or 1.5 H under high pressure)-RT(20C/min)					124K superconductivity in Cu-Ba-Ca-Cu-O				Mod.Phys.Lett.B,9(1995)1397-1406	C.W. Chu,I. Rusakova,L. Gao,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
7302	SST0090297		Bi2(Sr,Pr)2CuO6	Bi1.95Sr1.85Pr0.2Cu1O6+z	Bi	1.95	Sr	1.85	Pr	0.2	Cu	1													O	6+z			1996																												Bi2201																				21					21																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7303	SST0090297		Bi2(Sr,Pr)2CuO6	Bi1.95Sr1.75Pr0.3Cu1O6+z	Bi	1.95	Sr	1.75	Pr	0.3	Cu	1													O	6+z			1996																												Bi2201																				26.1					26.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7304	SST0090297		Bi2(Sr,Pr)2CuO6	Bi1.95Sr1.65Pr0.4Cu1O6+z	Bi	1.95	Sr	1.65	Pr	0.4	Cu	1													O	6+z			1996																												Bi2201																				30.1					30.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7305	SST0090297		Bi2(Sr,Pr)2CuO6	Bi1.95Sr1.55Pr0.5Cu1O6+z	Bi	1.95	Sr	1.55	Pr	0.5	Cu	1													O	6+z			1996																												Bi2201																				27.1					27.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7306	SST0090297		Bi2(Sr,Pr)2CuO6	Bi1.95Sr1.45Pr0.6Cu1O6+z	Bi	1.95	Sr	1.45	Pr	0.6	Cu	1													O	6+z			1996																												Bi2201																				20.1					20.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7307	SST0090297		Bi2(Sr,La)2CuO6	Bi1.95Sr1.85La0.2Cu1O6+z	Bi	1.95	Sr	1.85	La	0.2	Cu	1													O	6+z			1996																											3	Bi2201				5.472	5.332	24.514														22.1					22.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7308	SST0090297		Bi2(Sr,La)2CuO6	Bi1.95Sr1.75La0.3Cu1O6+z	Bi	1.95	Sr	1.75	La	0.3	Cu	1													O	6+z			1996																											3	Bi2201				5.455	5.334	24.539														31.1					31.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7309	SST0090297		Bi2(Sr,La)2CuO6	Bi1.95Sr1.75La0.4Cu1O6+z	Bi	1.95	Sr	1.75	La	0.4	Cu	1													O	6+z			1996																											3	Bi2201				5.425	5.404	24.479														33.1					33.1																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7310	SST0090297		Bi2(Sr,La)2CuO6	Bi1.95Sr1.55La0.5Cu1O6+z	Bi	1.95	Sr	1.55	La	0.5	Cu	1													O	6+z			1996																											3	Bi2201				5.437	5.418	24.442														29.2					29.2																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7311	SST0090297		Bi2(Sr,La)2CuO6	Bi1.95Sr1.45La0.6Ca1O6+z	Bi	1.95	Sr	1.45	La	0.6	Ca	1													O	6+z			1996																											3	Bi2201				5.447	5.433	24.399														25					25																																																																																														Bi2O3,SrCO3,CuO,R2O3	1	mixture-CAL(750C,10H in air)-pellet-SIN(800-850C,35H)-slow cool to RT					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7312	SST0090297		Bi2(Sr,Nd)2CuO6	Bi1.95Sr1.65Nd0.4Cu1O6+z	Bi	1.95	Sr	1.65	Nd	0.4	Cu	1													O	6+z			1996																												Bi2201																				27.4					27.4																																																																																															1	optimal sintering temperature=840C					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7313	SST0090297		Bi2(Sr,Sm)2CuO6	Bi1.95Sr1.65Sm0.4Cu1O6+z	Bi	1.95	Sr	1.65	Sm	0.4	Cu	1													O	6+z			1996																												Bi2201																				19.5					19.5																																																																																															1	optimal sintering teperature=830C					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7314	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.2	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.2		1996																											3	Bi2201																				10					10																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7315	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.28	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.28		1996																											3	Bi2201				5.442	5.404	24.678														32.6					32.6																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7316	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.298	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.298		1996																											3	Bi2201				5.427	5.418	24.639														34					34																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7317	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.311	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.311		1996																											3	Bi2201																				35.5					35.5																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7318	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.334	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.334		1996																											3	Bi2201																				30.5					30.5																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7319	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.343	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.343		1996																											3	Bi2201				5.434	5.418	24.599														26.5					26.5																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7320	SST0090297		Bi2(Sr,la)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.347	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.347		1996																											3	Bi2201																				24					24																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7321	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.36	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.36		1996																											3	Bi2201				5.4216	5.403	24.571														23					23																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7322	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.414	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	z	6.414		1996																											3	Bi2201				5.414	5.407	24.552														10.4					10.4																																																																																																SIN(840C)-Q to liq.N2-heat treatment (700C in O2 or N2 or vacuum for various times)					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7323	SST0090297		Bi2(Sr,La)2CuOz	Bi1.95Sr1.65La0.4Cu1O6.2	Bi	1.95	Sr	1.65	La	0.4	Cu	1													O	6.2	6.2		1996																												Bi2201																				30.5					30.5																																																																																																F was introduced by CuF2, SIN(840C,40H in air) -quenched to liq. N					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7324	SST0090297		Bi2(Sr,La)2Cu(O,F)6	Bi1.95Sr1.65La0.4Cu1F0.2O6	Bi	1.95	Sr	1.65	La	0.4	Cu	1	F	0.2											O	6	6		1996																												Bi2201																				30.1					30.1																																																																																																F was introduced by CuF2, SIN(840C,40H in air) -quenched to liq. N					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7325	SST0090297		Bi2(Sr,La)2Cu(O,F)6	Bi1.95Sr1.65La0.4Cu1F0.4O5.8	Bi	1.95	Sr	1.65	La	0.4	Cu	1	F	0.4											O	5.8	5.8		1996																												Bi2201																				29					29																																																																																																F was introduced by CuF2, SIN(840C,40H in air) -quenched to liq. N					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7326	SST0090297		Bi2(Sr,La)2Cu(O,F)6	Bi1.95Sr1.65La0.4Cu1F0.6O5.6	Bi	1.95	Sr	1.65	La	0.4	Cu	1	F	0.6											O	5.6	5.6		1996																												Bi2201																				25.1					25.1																																																																																																F was introduced by CuF2, SIN(840C,40H in air) -quenched to liq. N					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7327	SST0090297		Bi2(Sr,La)2Cu(O,F)6	Bi1.95Sr1.65La0.4Cu1F0.8O5.4	Bi	1.95	Sr	1.65	La	0.4	Cu	1	F	0.8											O	5.4	5.4		1996																												Bi2201																				13					13																																																																																																F was introduced by CuF2, SIN(840C,40H in air) -quenched to liq. N					The effects of composition, synthesis conditions, oxygen content and F doping on superconductivity and structure for R-substituted Bi-2201			Institute of Physics, Academia Sinica, Beijing 100080, People's Repblic of China	Supercond.Sci.Technol.9(1996)297	C Dong,F Wu,G C Che,H Chen,S L Jia,Y C Lan,Z X Zhao		
7328	SST0090761	2223phase<3%,2212phase>97%,second Tc=78.5K	(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi3.2Pb0.2V0.6Sr4Ca5Cu7Oz	Bi	3.2	Pb	0.2	V	0.6	Sr	4	Ca	5	Cu	7									O	z		2	1996																												Bi2212																				78.5	108.9				78.5																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7329	SST0090761		(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi3.2Pb0.4V0.4Sr4Ca5Cu7Oz	Bi	3.2	Pb	0.4	V	0.4	Sr	4	Ca	5	Cu	7									O	z		2	1996																																																	108.5				108.5																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7330	SST0090761		(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi3.2Pb0.6V0.2Sr4Ca5Cu7Oz	Bi	3.2	Pb	0.6	V	0.2	Sr	4	Ca	5	Cu	7									O	z		2	1996																																																	110.5				110.5																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7331	SST0090761	2223phase=25%, 2212phase=75%	(Bi,Pb)4Sr4Ca5Cu7Oz	Bi3.2Pb0.8Sr4Ca5Cu7Oz	Bi	3.2	Pb	0.8	Sr	4	Ca	5	Cu	7											O	z		2	1996																											2	Bi2212				5.404		37.173																108.9			108.9																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7332	SST0090761	2223phase=87%,2212phase=13%	(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi2.6Pb0.8V0.6Sr4Ca5Cu7Oz	Bi	2.6	Pb	0.8	V	0.6	Sr	4	Ca	5	Cu	7									O	z		2	1996																																5.41		37.079																110.8			110.8																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7333	SST0090761		(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi2.8Pb0.8V0.4Sr4Ca5Cu7Oz	Bi	2.8	Pb	0.8	V	0.4	Sr	4	Ca	5	Cu	7									O	z		2	1996																																																		111			111																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7334	SST0090761	2223phase=62%, 2212phase=38%	(Bi,Pb,V)4Sr4Ca5Cu7Oz	Bi3Pb0.8V0.2Sr4Ca5Cu7Oz	Bi	3	Pb	0.8	V	0.2	Sr	4	Ca	5	Cu	7									O	z		2	1996																																5.411		37.118																110.8			110.8																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7335	SST0090761	2223phase<3%, 2212phase>97%	(Bi,V)4Sr4Ca5Cu7Oz	Bi3.4V0.6Sr4Ca5Cu7Oz	Bi	3.4	V	0.6	Sr	4	Ca	5	Cu	7											O	z		2	1996																																																		82.2			82.2																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7336	SST0090761		(Bi,V)4Sr4Ca5Cu7Oz	Bi3.6V0.4Sr4Ca5Cu7Oz	Bi	3.6	V	0.4	Sr	4	Ca	5	Cu	7											O	z		2	1996																												Bi2212																						84			84																																																																																														Bi2O3,Pb3O4,V2O5,SrCO3,CaCO3,CuO	1	mixture-CAL(800C,24H in air)-pellet-SIN(830C,168H + 840C,168H)-quench to RT.					Preparation and prorerties of Pb-and V-doped Bi-based superconductors			Institute of Chemical Technology, Technicka' 5, 166 28 Prague 6, Czech Republic	Supercond.Sci.Technol.9(1996)761	D Sy'korova',K Nova'kova,O Smrckova',P Vasek		
7337	SST0090706	Hg1212 phase not found	(Hg,Ti)Sr2CaCu2O6	Hg0.8Ti0.2Sr2Ca1Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	1	Cu	2											O	6+z			1996																																																																																																																																																			TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7338	SST0090706	not s/c	(Hg,Ti)Sr2(Ca,Y)Ca2O6	Hg0.8Ti0.2Sr2Ca0.8Y0.2Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	6+z		2	1996																																																			20																																																																																																TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7339	SST0090706	second Tc=52K	(Hg,Ti)Sr2(Ca,Y)Cu2O6	Hg0.8Ti0.2Sr2Ca0.7Y0.3Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	6+z		1	1996																											2	Hg1212				3.822		11.905													31.7		81.8				56.75																																																																			32.8															51												TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7340	SST0090706	second Tc=52K	(Hg,Ti)Sr2(Ca,Y)Cu2O6	Hg0.8Ti0.2Sr2Ca0.6Y0.4Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	0.6	Y	0.4	Cu	2									O	6+z		1	1996																											2	Hg1212																			27.5		80				53.75																																																																			31.8															30												TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7341	SST0090706	second Tc=52K	(Hg,Ti)Sr2(Ca,Y)Cu2O6	Hg0.8Ti0.2Sr2Ca0.5Y0.5Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	6+z		1	1996																											2	Hg1212				3.824		11.901													39.1		82				60.55																																																																			21.9															10												TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7342	SST0090706	second Tc=47K	(Hg,Ti)Sr2(Ca,Y)Cu2O6	Hg0.8Ti0.2Sr2Ca0.4Y0.6Cu2O6+z	Hg	0.8	Ti	0.2	Sr	2	Ca	0.4	Y	0.6	Cu	2									O	6+z		1	1996																											2	Hg1212				3.828		11.888													28.7		81.3				55																																																																			21.7															16												TiO2,Sr(NO3)2,Y2O3,Ca(NO3)2,Cu(NO3)2,HgO	1	two-step solid state rection,orecursor(Ti0.2 Sr2 Ca1-xYx Cu2Oz)-addition of HgO-mixture-pellet-seal in quartz tube-heat(900C,6H+10H)-siow cool to RT					(Hg0.8Ti0.2)Sr2(Ca1-xYx)Cu2O6+z: a new series of mercury-based 1212 superconductors			Saha Institute of Nuclear Physics,1/AF Bidhannagar, Calcutta-700 064, India	Supercond.Sci.Technol.9(1996)706	B Bandyopadhyay,B Ghosh,J B Mandal		
7343	SST0090093		(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8.05	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	z	8.05		1996																											2	Bi2212																					102	80.5			80.5																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7344	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.99Nd0.01Cu2O8.03	Bi	1.7	Pb	0.3	Sr	2	Ca	0.99	Nd	0.01	Cu	2									O	z	8.03		1996																											2	Bi2212																					102	82.5			82.5																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7345	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.98Nd0.02Cu2O8.05	Bi	1.7	Pb	0.3	Sr	2	Ca	0.98	Nd	0.02	Cu	2									O	z	8.05		1996																											2	Bi2212																					97	80.89			80.89																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7346	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.96Y0.04Cu2O8.06	Bi	1.7	Pb	0.3	Sr	2	Ca	0.96	Y	0.04	Cu	2									O	z	8.06		1996																											2	Bi2212																					93	78.5			78.5																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7347	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.94Nd0.06Cu2O8.1	Bi	1.7	Pb	0.3	Sr	2	Ca	0.94	Nd	0.06	Cu	2									O	z	8.1		1996																											2	Bi2212																					90	81.27			81.27																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7348	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.92Nd0.08Cu2O8.16	Bi	1.7	Pb	0.3	Sr	2	Ca	0.92	Nd	0.08	Cu	2									O	z	8.16		1996																											2	Bi2212																					88	84.11			84.11																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7349	SST0090093		(Bi,Pb)2Sr2(Ca,Nd)Cu2O8	Bi1.7Pb0.3Sr2Ca0.9Nd0.1Cu2O8.27	Bi	1.7	Pb	0.3	Sr	2	Ca	0.9	Nd	0.1	Cu	2									O	z	8.27		1996																											2	Bi2212																					84	76.67			76.67																																																																																															1	ANN(450C,2H in vacuum)					Systematics of the physical properties of Bi1.7Pb0.3Sr2(Ca,Nd)1Cu2Oy compounds			Department of Physics,Osmania University, Hyderabad 500007, India	Supercond.Sci.Technol.9(1996)93	K Nanda Kishore,O Pena,S Satyavathi,V Hari Babu		
7350	CEM1250117	metallic	(Pr,Sr)8Cu8O20	Pr5.2Sr2.8Cu8O20	Pr	5.2	Sr	2.8	Cu	8															O	20			1996																													P4/mbm	127		10.8		3.805																	13																																																																																				3.4												CuO,Pr6O11,Nd2O3,SrCO3		moxture-pellet-heat(1273K,40H in flowing O2 in alumina crucible)-Q to RT-heat(1273K,20H in 20% O2+80%Ar,under 100MPa using HIP)					(RE1-xSrx)8Cu8O20(RE=Pr,ND) Synthesized under a High Pressure of Oxygen, Po2=20 MPa			Institute for Materials Research, Tohoku University, Katahira 2-1-1, Aoba-ku, Sendai 980-77, Japan	J.Solid State Chem.125(1996)117	Hisanori Yamane,Toshio Hirai,Yoshiki Amamoto		
7351	CEM1250117		(Nd,Sr)8Cu8O20	Nd4.8Sr3.2Cu8O20	Nd	4.8	Sr	3.2	Cu	8															O	20			1996																													P4/mbm	127		10.796		3.784																	13																																																																																				7												CuO,Pr6O11,Nd2O3,SrCO3		moxture-pellet-heat(1273K,40H in flowing O2 in alumina crucible)-Q to RT-heat(1273K,20H in 20% O2+80%Ar,under 100MPa using HIP)					(RE1-xSrx)8Cu8O20(RE=Pr,ND) Synthesized under a High Pressure of Oxygen, Po2=20 MPa			Institute for Materials Research, Tohoku University, Katahira 2-1-1, Aoba-ku, Sendai 980-77, Japan	J.Solid State Chem.125(1996)117	Hisanori Yamane,Toshio Hirai,Yoshiki Amamoto		
7352	SST0090161	grain size=1-10 micron,intergranulor Hc1=11Oe	(Y,Sm)Ba2Cu3O7	Y0.5Sm0.5Ba2Cu3O7-z	Y	0.5	Sm	0.5	Ba	2	Cu	3													O	7-z			1996																												Y123																						92			92													141																																																																																			liquid mix technique, fire(950C,20H)-ANN(450C,2weeks in flowing O2)					Magnetic flux penetration and creep in a ceramic(Y,Sm)Ba2Cu3O7 superconductor			Institut de Cie'ncia de Materials de Barcelona, CSIC, Campus Universitat Auto'noma de Barcelona,08193 Bellaterra, Spain	Supercond.Sci.Technol.9(1996)161	A Fert,F Pe'rez,J Fontcuberta,X Bozec,X Obradors		
7353	SUP0100059		(Er,Ca)Ba2(Cu,Co)3O7	Er0.76Ca0.24Ba2Cu2.76Co0.24O6.92	Er	0.76	Ca	0.24	Ba	2	Cu	2.76	Co	0.24											O	z	6.92	1	1997																											3	Y123				3.824	3.824	11.611													81	84	87	87			84																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7354	SUP0100059		(Er,Ca)(Ba,Sr)2(Cu,Co)3O7	Er0.76Ca0.24Ba1.8Sr0.2Cu2.76Co0.24O6.91	Er	0.76	Ca	0.24	Ba	1.8	Sr	0.2	Cu	2.76	Co	0.24									O	z	6.91	1	1997																											3	Y123				3.76	3.832	11.787													76	81	85	77			81																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7355	SUP0100059		(Er,Ca)(Ba,Sr)2(Cu,Co)3O7	Er0.76Ca0.24Ba1.6Sr0.4Cu2.76Co0.24O6.88	Er	0.76	Ca	0.24	Ba	1.6	Sr	0.4	Cu	2.76	Co	0.24									O	z	6.88	1	1997																											3	Y123				3.833	3.895	11.61													74	77	80	70			77																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7356	SUP0100059		(Er,Ca)(Ba,Sr)2(Cu,Co)3O7	Er0.76Ca0.24Ba1.4Sr0.6Cu2.76Co0.24O6.84	Er	0.76	Ca	0.24	Ba	1.4	Sr	0.6	Cu	2.76	Co	0.24									O	z	6.84	1	1997																											3	Y123				3.84	3.902	11.585													54	64	74	54			64																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7357	SUP0100059		(Er,Ca)(Ba,Sr)2(Cu,Co)3O7	Er0.64Ca0.36Ba1.4Sr0.6Cu2.76Co0.24O6.8	Er	0.64	Ca	0.36	Ba	1.4	Sr	0.6	Cu	2.76	Co	0.24									O	z	6.8	1	1997																											3	Y123				3.847	3.846	11.611																48			48																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7358	SUP0100059		(Er,Ca)(Ba,Sr)2(Cu,Co)3O7	Er0.52Ca0.48Ba1.4Sr0.6Cu2.76Co0.24O6.77	Er	0.52	Ca	0.48	Ba	1.4	Sr	0.6	Cu	2.76	Co	0.24									O	z	6.77	1	1997																											3	Y123				3.844	3.832	11.63																54			54																																																																																														BaCO3,CuO,Co3O4,CaCO3,SrO		mixture-heat(940C,24H in air)-pellet-SIN(940C,24H in air)-ANN(550C,24H in O2 flow)-slow cool to RT(1C/min)					Effect of Sr and Sr-Ca Substitution on the Superconductivity of (Er0.76Ca0.24)Ba2(Cu2.76Co0.24)Oz	1997		Department of Physics,Saurashtra University, Rajkot-360 005, India	J.Superconductivity,Vol,10(1997)59	D.G. Kuberkar,G.J. Baldha,K.M. Pansuria,R.G. Kulkarni		
7359	SUP0100045		LaBa2Cu3O7	La1Ba2Cu3Oz	La	1	Ba	2	Cu	3															O	z			1997																											3	Y123				3.922	3.942	11.822													70.34						70.34																																																																																														CuO,Y2O3,Fe2O3,BaCO3	1	mixture-heat(930-910C,24H in air)-FC-pellet-SIN(930-910C,24H in flowing O2)-ANN(350C,24H)-FC					A Structural Transition of Fe-Doped Superconducting Cuprates	1997		Department of Physics and National Laboratory of Solid State Microstructure, Nanjing University,Nanjing 210093, Peoples Republic of China	J.Superconductivity,Vol.10,(1997)45	S. Liang,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu,Y. Yu		
7360	SUP0100045		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.97Fe0.03Oz	La	1	Ba	2	Cu	2.97	Fe	0.03													O	z			1997																											3	Y123				3.925	3.935	11.821													55.23						55.23																																																																																														CuO,Y2O3,Fe2O3,BaCO3	1	mixture-heat(930-910C,24H in air)-FC-pellet-SIN(930-910C,24H in flowing O2)-ANN(350C,24H)-FC					A Structural Transition of Fe-Doped Superconducting Cuprates	1997		Department of Physics and National Laboratory of Solid State Microstructure, Nanjing University,Nanjing 210093, Peoples Republic of China	J.Superconductivity,Vol.10,(1997)45	S. Liang,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu,Y. Yu		
7361	SUP0100045		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.94Fe0.06Oz	La	1	Ba	2	Cu	2.94	Fe	0.06													O	z			1997																											2	Y123				3.929		11.812													35.9						35.9																																																																																														CuO,Y2O3,Fe2O3,BaCO3	1	mixture-heat(930-910C,24H in air)-FC-pellet-SIN(930-910C,24H in flowing O2)-ANN(350C,24H)-FC					A Structural Transition of Fe-Doped Superconducting Cuprates	1997		Department of Physics and National Laboratory of Solid State Microstructure, Nanjing University,Nanjing 210093, Peoples Republic of China	J.Superconductivity,Vol.10,(1997)45	S. Liang,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu,Y. Yu		
7362	SUP0100045		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.9Fe0.1Oz	La	1	Ba	2	Cu	2.9	Fe	0.1													O	z			1997																											2	Y123				3.934		11.83																																																																																																																	CuO,Y2O3,Fe2O3,BaCO3	1	mixture-heat(930-910C,24H in air)-FC-pellet-SIN(930-910C,24H in flowing O2)-ANN(350C,24H)-FC					A Structural Transition of Fe-Doped Superconducting Cuprates	1997		Department of Physics and National Laboratory of Solid State Microstructure, Nanjing University,Nanjing 210093, Peoples Republic of China	J.Superconductivity,Vol.10,(1997)45	S. Liang,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu,Y. Yu		
7363	SUP0100045		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.25Fe0.75Oz	La	1	Ba	2	Cu	2.25	Fe	0.75													O	z			1997																											3	Y123				3.913	3.944	11.933																																																																																																																	CuO,Y2O3,Fe2O3,BaCO3	1	mixture-heat(930-910C,24H in air)-FC-pellet-SIN(930-910C,24H in flowing O2)-ANN(350C,24H)-FC					A Structural Transition of Fe-Doped Superconducting Cuprates	1997		Department of Physics and National Laboratory of Solid State Microstructure, Nanjing University,Nanjing 210093, Peoples Republic of China	J.Superconductivity,Vol.10,(1997)45	S. Liang,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu,Y. Yu		
7364	SST0090529		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	1996																											2	Bi2212				5.41		30.984																																																																																									TP7364																								Bi2O3,SrCO3,CaCO3,CeO2,CuO	1	mixture-CAL(800C,13H in air)-pellet-CAL(820C,8H + 840C,12.5H+860C,15H in air with intermediate grindings)-FC to RT					Thermoelectric power of the Bi2Sr2Ca1-xCexCu2O8+y system			School of Science and Engineering, Teikyo University, 1-1 Toyosatodai, Utsunomiya 320, Japan	Supercond.Sci.Technol.9(1996)529	Hisashi Sekine,Hua Jin,Ruiping Wang		
7365	SST0090529		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.95Ce0.05Cu2O8+z	Bi	2	Sr	2	Ca	0.95	Ce	0.05	Cu	2											O	8+z		1	1996																											2	Bi2212				5.415		30.932																																																																																									TP7365																								Bi2O3,SrCO3,CaCO3,CeO2,CuO	1	mixture-CAL(800C,13H in air)-pellet-CAL(820C,8H + 840C,12.5H+860C,15H in air with intermediate grindings)-FC to RT					Thermoelectric power of the Bi2Sr2Ca1-xCexCu2O8+y system			School of Science and Engineering, Teikyo University, 1-1 Toyosatodai, Utsunomiya 320, Japan	Supercond.Sci.Technol.9(1996)529	Hisashi Sekine,Hua Jin,Ruiping Wang		
7366	SST0090529		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.9Ce0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Ce	0.1	Cu	2											O	8+z		1	1996																											2	Bi2212				5.418		30.878																																																																																									TP7366																								Bi2O3,SrCO3,CaCO3,CeO2,CuO	1	mixture-CAL(800C,13H in air)-pellet-CAL(820C,8H + 840C,12.5H+860C,15H in air with intermediate grindings)-FC to RT					Thermoelectric power of the Bi2Sr2Ca1-xCexCu2O8+y system			School of Science and Engineering, Teikyo University, 1-1 Toyosatodai, Utsunomiya 320, Japan	Supercond.Sci.Technol.9(1996)529	Hisashi Sekine,Hua Jin,Ruiping Wang		
7367	SST0090529		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.8Ce0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Ce	0.2	Cu	2											O	8+z		1	1996																											2	Bi2212				5.426		30.529																																																																																									TP7367																								Bi2O3,SrCO3,CaCO3,CeO2,CuO	1	mixture-CAL(800C,13H in air)-pellet-CAL(820C,8H + 840C,12.5H+860C,15H in air with intermediate grindings)-FC to RT					Thermoelectric power of the Bi2Sr2Ca1-xCexCu2O8+y system			School of Science and Engineering, Teikyo University, 1-1 Toyosatodai, Utsunomiya 320, Japan	Supercond.Sci.Technol.9(1996)529	Hisashi Sekine,Hua Jin,Ruiping Wang		
7368	SST0090529		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.6Ce0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Ce	0.4	Cu	2											O	8+z		1	1996																											2	Bi2212				5.434		30.125																																																																																									TP7368																								Bi2O3,SrCO3,CaCO3,CeO2,CuO	1	mixture-CAL(800C,13H in air)-pellet-CAL(820C,8H + 840C,12.5H+860C,15H in air with intermediate grindings)-FC to RT					Thermoelectric power of the Bi2Sr2Ca1-xCexCu2O8+y system			School of Science and Engineering, Teikyo University, 1-1 Toyosatodai, Utsunomiya 320, Japan	Supercond.Sci.Technol.9(1996)529	Hisashi Sekine,Hua Jin,Ruiping Wang		
7369	PHC2780107	semiconductor	Ysr2(Cu,B)3O7	Y1Sr2Cu2.5B0.5Oz	Y	1	Sr	2	Cu	2.5	B	0.5													O	z			1997																											2	1212				3.826		10.984																	5																																																																																																Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7370	PHC2780107	semiconductor	YSr2(Cu,B,S)3O7	Y1Sr2Cu2.5B0.4S0.1Oz	Y	1	Sr	2	Cu	2.5	B	0.4	S	0.1											O	z			1997																											2	1212				3.825		11.052																	5																																																																																																Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7371	PHC2780107	semiconductor	YSr2(Cu,B,S)3O7	Y1Sr2Cu2.5B0.3S0.2Oz	Y	1	Sr	2	Cu	2.5	B	0.3	S	0.2											O	z			1997																											2	1212				3.833		11.108																	5																																																																																																Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7372	PHC2780107	semiconductor	YSr2(Cu,B,S)3O7	Y1Sr2Cu2.5B0.2S0.3Oz	Y	1	Sr	2	Cu	2.5	B	0.2	S	0.3											O	z			1997																											2	1212				3.837		11.164																	5																																																																																																Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7373	PHC2780107	semoconductor	YSr2(Cu,B,S)3O7	Y1Sr2Cu2.5B0.1S0.4Oz	Y	1	Sr	2	Cu	2.5	B	0.1	S	0.4											O	z			1997																											2	1212				3.839		11.189																	5																																																																																																Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7374	PHC2780107		Y(Ba,Sr)(Cu,B)3Oz	Y1Ba1Sr1Cu2.5B0.5Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.5											O	z			1997																											2	1212				3.848		11.281													41.2						41.2																																																																																														Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7375	PHC2780107		Y(Ba,Sr)(Cu,B,S)3Oz	Y1Ba1Sr1Cu2.5B0.1S0.4Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.1	S	0.4									O	z			1997																											2	1212				3.833		11.483													44						44																																																																																														Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7376	PHC2780107		Y(Ba,Sr)(Cu,B,S)3Oz	Y1Ba1Sr1Cu2.5S0.5Oz	Y	1	Ba	1	Sr	1	Cu	2.5	S	0.5											O	z			1997																											2	1212				3.834		11.518													50.9						50.9																																																																																														Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7377	PHC2780107		Y(Ba,Sr)(Cu,B,S)3Oz	Y1Ba1Sr1Cu2.5B0.2S0.3Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.2	S	0.3									O	z			1997																											2	1212				3.838		11.426													25						25																																																																																														Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7378	PHC2780107	smiconductor	Y(Ba,Sr)(Cu,B,S)Oz	Y1Ba1Sr1Cu2.5B0.3S0.2Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.3	S	0.2									O	z			1997																											2	1212				3.842		11.362																		50																																																																																															Y2O3,SrCO3,BaCO3,CuO,H3BO3,S	1	mixture-heat(950C,20H)-mix with S powder-SIN(1040C,or 1010C,20H in air)-slow cool to RT-heat another 20H					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7379	PHC2780107		Y(Sr,Ba)2(Cu,B,S)3)Oz	Y1Sr0.5Ba1.5Cu2.5B0.1S0.4Oz	Y	1	Sr	0.5	Ba	1.5	Cu	2.5	B	0.1	S	0.4									O	z			1997																												1212				3.847		11.533													56.5						56.5																																																																																																					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7380	PHC2780107		Y(Sr,Ba)2(Cu,B,S)2Oz	Y1Sr0.5Ba1.5Cu2.5S0.5Oz	Y	1	Sr	0.5	Ba	1.5	Cu	2.5	S	0.5											O	z			1997																												1212				3.853		11.582													75.6						75.6																																																																																																					The effects of sulphur substitution on Y(Ba,Sr)2Cu2.5B0.5Oz systems	199704		National Laboratory for Superconductivity, Institute of Physics, Academia Sinica, Beijing 100080, China	Physica.C,278(1997)107-112	C. Dong,F. Wu,G.C. Che,H. Chen,H. Deng,J.C. Shen,S.L. Jia,Z.X. Zhao		
7381	PR05111753	films by laser ablation.	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.8Fe0.2Oz	Y	1	Ba	2	Cu	2.8	Fe	0.2													O	z		4	1995																												Y123																				57					57												defined as R/Rn=0.5,extraporete linearly to OK													26.8						0.48																																																																	films were deposited on LaAlO3(001) by pulsed excimen laser ablation, annealed at 500-650C for 1H					Resistivity transitions in apploed mpplied magnetic fields in epitaxial thin films of Fe-and Zn-doped YBa2Cu3O7-z	199505			Phys.Rev.B,51(1995)11753	C. Kwon,D.D. Choughule,M. Rajeswari,R.L. Greene,S.B. Ogale,T. Venkatesan	Fe, Zn, Y, Ba, Cu, O	
7382	PR05111753	films by laser ablation.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.8Zn0.2Oz	Y	1	Ba	2	Cu	2.8	Zn	0.2													O	z		4	1995																												Y123																				51.7					51.7																									50.4					defined as R/Rn=0.5,extraporete linearly to OK	0.98																																																																	films were deposited on LaAlO3(001) by pulsed excimen laser ablation, annealed at 500-650C for 1H					Resistivity transitions in apploed mpplied magnetic fields in epitaxial thin films of Fe-and Zn-doped YBa2Cu3O7-z	199505			Phys.Rev.B,51(1995)11753	C. Kwon,D.D. Choughule,M. Rajeswari,R.L. Greene,S.B. Ogale,T. Venkatesan	Fe, Zn, Y, Ba, Cu, O	
7383	PHC2780113	c-axis oriented film,d=3000A	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		5	1997																												Y123																				87				1	87												defined as R/Rn=0.5,extraporate linearly to OK																				5.6	1.78																																																	0.178														using inverted cylindrical DC magnetron sputtering,films were deposited on MgO(100)sulstrates,T(sub)=770C,oxygenayed in-situ at 450C for 40min.					Thermally activated flux motion in YBa2(Cu1-xZnx)3O7-8 epitaxial thin films: influence of magnetic field and Zn doping	199704		Universite' Libre de Bruxelles, CP-233, Bd, du Triomphe, B1050 Bruxelles, Belgium	Physica.C,278(1997)113-121	A.G.M. Jansen,J. Schroeder,J.F. de Marneffe,M. Mehbad,M. Ye,P. Wyder,R. Deltour		
7384	PHC2780113	c-axis oriented film,d=3000A	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7-z	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-z			1997																												Y123																				73				3	73												defined as R/Rn=0.5,extraporate linearly to OK																				6.3	1.8																																																	0.366														using inverted cylindrical DC magnetron sputtering,films were deposited on MgO(100)sulstrates,T(sub)=770C,oxygenayed in-situ at 450C for 40min.					Thermally activated flux motion in YBa2(Cu1-xZnx)3O7-8 epitaxial thin films: influence of magnetic field and Zn doping	199704		Universite' Libre de Bruxelles, CP-233, Bd, du Triomphe, B1050 Bruxelles, Belgium	Physica.C,278(1997)113-121	A.G.M. Jansen,J. Schroeder,J.F. de Marneffe,M. Mehbad,M. Ye,P. Wyder,R. Deltour		
7385	PHC2780113	c-axis oriented film,d=3000A	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O7-z	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-z			1997																												Y123																				60				5	60												defined as R/Rn=0.5,extraporate linearly to OK																				6.6	1.5																																																	0.497														using inverted cylindrical DC magnetron sputtering,films were deposited on MgO(100)sulstrates,T(sub)=770C,oxygenayed in-situ at 450C for 40min.					Thermally activated flux motion in YBa2(Cu1-xZnx)3O7-8 epitaxial thin films: influence of magnetic field and Zn doping	199704		Universite' Libre de Bruxelles, CP-233, Bd, du Triomphe, B1050 Bruxelles, Belgium	Physica.C,278(1997)113-121	A.G.M. Jansen,J. Schroeder,J.F. de Marneffe,M. Mehbad,M. Ye,P. Wyder,R. Deltour		
7386	PHC2780039		(Gd,Ce)2CuO4	Gd1.85Ce0.15Cu1O4	Gd	1.85	Ce	0.15	Cu	1															O	4		1	1997							158	153																				T'				3.905																																																																																																																				1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7387	PHC2780039		(Gd,Pr,Ce)2CuO4	Gd1.75Pr0.1Ce0.15Cu1O4	Gd	1.75	Pr	0.1	Ce	0.15	Cu	1													O	4			1997							165	154																				T'				3.907		11.841																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7388	PHC2780039		(Gd,Pr,Ce)2CuO4	Gd1.55Pr0.3Ce0.15Cu1O4	Gd	1.55	Pr	0.3	Ce	0.15	Cu	1													O	4			1997							144	145																				T'				3.911		11.873																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7389	PHC2780039		(Gd,Nd,Ce)2CuO4	Gd1.65Nd0.2Ce0.15Cu1O4	Gd	1.65	Nd	0.2	Ce	0.15	Cu	1													O	4			1997							148	140																				T'				3.912		11.864																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7390	PHC2780039		(Gd,Nd,Ce)2CuO4	Gd1.5Nd0.35Ce0.15Cu1O4	Gd	1.5	Nd	0.35	Ce	0.15	Cu	1													O	4			1997							119	97																				T'				3.915		11.883																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7391	PHC2780039		(Gd,Sm,Ce)2CuO4	Gd1.55Sm0.3Ce0.15Cu1O4	Gd	1.55	Sm	0.3	Ce	0.15	Cu	1													O	4		1	1997							154	152																				T'				3.906		11.846																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7392	PHC2780039		(Gd,Sm,Ce)2CuO4	Gd1.3Sm0.55Ce0.15Cu1O4	Gd	1.3	Sm	0.55	Ce	0.15	Cu	1													O	4		1	1997							149	144																				T'				3.907		11.851																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7393	PHC2780039		(Gd,Sm,Ce)2CuO4	Gd1.1Sm0.75Ce0.15Cu1O4	Gd	1.1	Sm	0.75	Ce	0.15	Cu	1													O	4		1	1997							127																					T'				3.91		11.858																																																																																																																		1						Weak ferromagnetism and superconductivity in (Gd,R)1.85Ce0.15CuO4 with R=Pr,Nd, and Sm	199704		Department of Chemistry, Peking University, Beijing, People's Republic of China	Physica.C,278(1997)39-42	Chin Lin,Guo Lu,Hai-Ying Chen,Yu-Fen Zhang,Yun-Xi Sun,Zun-Xiao Liu		
7394	PHC2780011	PPenet=1850A by Hao's model	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1997																												Bi2212																						82			82																															4.5													2220																																																				self-flux method, se Physica C 225(1994)235					Growth and superconductivity of Bi2Sr2Ca1-xYxCu2O8+z single crystals in the Tc optimum region	199704		Laboratoire CRISMAT. ISMRA et Universite' de Caen, UMR 6508, associee' au CNRS, 6 Bd du Marechal Juin, 14050 Caen cedex, France	Physica.C,278(1997)11-22	A. Maignan,A. Wahl,D. Pelloquin,G. Villard		
7395	PHC2780011	ppenet=1580A by Hao's model	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.79Y0.21Cu2O8+z	Bi	2	Sr	2	Ca	0.79	Y	0.21	Cu	2											O	8+z		3	1997																												Bi2212																						89.4			89.4																															2.5													1900																																																				self-flux method, se Physica C 225(1994)235					Growth and superconductivity of Bi2Sr2Ca1-xYxCu2O8+z single crystals in the Tc optimum region	199704		Laboratoire CRISMAT. ISMRA et Universite' de Caen, UMR 6508, associee' au CNRS, 6 Bd du Marechal Juin, 14050 Caen cedex, France	Physica.C,278(1997)11-22	A. Maignan,A. Wahl,D. Pelloquin,G. Villard		
7396	PHC2780011	ppenet=2150A by Hao's model	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.72Y0.28Cu2O8+z	Bi	2	Sr	2	Ca	0.72	Y	0.28	Cu	2											O	8+z		3	1997																												Bi2212																						91.5			91.5																															3.7													2590																																																				self-flux method, se Physica C 225(1994)235					Growth and superconductivity of Bi2Sr2Ca1-xYxCu2O8+z single crystals in the Tc optimum region	199704		Laboratoire CRISMAT. ISMRA et Universite' de Caen, UMR 6508, associee' au CNRS, 6 Bd du Marechal Juin, 14050 Caen cedex, France	Physica.C,278(1997)11-22	A. Maignan,A. Wahl,D. Pelloquin,G. Villard		
7397	PHC2780011	ppenet=2470A by Hao's model	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.64Y0.36Cu2O8+z	Bi	2	Sr	2	Ca	0.64	Y	0.36	Cu	2											O	8+z		3	1997																												Bi2212																						88			88																															1.7													2980																																																				self-flux method, se Physica C 225(1994)235					Growth and superconductivity of Bi2Sr2Ca1-xYxCu2O8+z single crystals in the Tc optimum region	199704		Laboratoire CRISMAT. ISMRA et Universite' de Caen, UMR 6508, associee' au CNRS, 6 Bd du Marechal Juin, 14050 Caen cedex, France	Physica.C,278(1997)11-22	A. Maignan,A. Wahl,D. Pelloquin,G. Villard		
7398	PHC2770119		(Hg,(VO4))Ba2CuOz	Hg0.7V0.3Ba2Cu1O3.4+z	Hg	0.7	V	0.3	Ba	2	Cu	1													O	3.4+z			1997																											2	Hg1201																				70					70										48																																																																																					1	mixture=sealed in quartz tube-heat(720C,16H)-Q to RT					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7399	PHC2770119		(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.75Sr0.25Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.75	Sr	0.25	Cu	1											O	4.6+z			1997																											2	Hg1201																				65					65										44																																																																																					1	mixture=sealed in quartz tube-heat(720C,16H)-Q to RT					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7400	PHC2770119		(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.5Sr0.5Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.5	Sr	0.5	Cu	1											O	4.6+z			1997																											2	Hg1201																				65					65										50																																																																																					1	mixture=sealed in quartz tube-heat(720C,16H)-Q to RT					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7401	PHC2770119		(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.25Sr0.75Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.25	Sr	0.75	Cu	1											O	4.6+z			1997																											2	Hg1201																				55					55										45																																																																																					1	mixture=sealed in quartz tube-heat(720C,16H)-Q to RT					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7402	PHC2770119		(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1Sr1Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1	Sr	1	Cu	1											O	4.6+z			1997																											2	Hg1201																				45					45										39																																																																																					1	mixture=sealed in quartz tube-heat(720C,16H)-Q to RT					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7403	PHC2770119	annealed in Ar 	(Hg,VO4)Ba2CuOz	Hg0.7V0.3Ba2Cu1O4.6+z	Hg	0.7	V	0.3	Ba	2	Cu	1													O	4.6+z			1997																												Hg1201																				95					95										52																																																																																						mixture-sealed in quartz tube-heat(720C,16H)-Q to RT-ANN(400C,72H in Ar flow)					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7404	PHC2770119	annealed in Ar 	(Hg,VO3)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.75Sr0.25Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.75	Sr	0.25	Cu	1											O	4.6+z			1997																												Hg1201																				90					90										60																																																																																						mixture-sealed in quartz tube-heat(720C,16H)-Q to RT-ANN(400C,72H in Ar flow)					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7405	PHC2770119	annealed in Ar 	(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.5Sr0.5Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.5	Sr	0.5	Cu	1											O	4.6+z			1997																												Hg1201																				85					85										67																																																																																						mixture-sealed in quartz tube-heat(720C,16H)-Q to RT-ANN(400C,72H in Ar flow)					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7406	PHC2770119	annealed in Ar 	(Hg,VO4)(Ba,Sr)2CuOz	Hg0.7V0.3Ba1.25Sr0.75Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1.25	Sr	0.75	Cu	1											O	4.6+z			1997																												Hg1201																				75					75										64																																																																																						mixture-sealed in quartz tube-heat(720C,16H)-Q to RT-ANN(400C,72H in Ar flow)					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7407	PHC2770119	annealed in Ar 	(Hg,VO4)(Ba,Sr)2CuO2	Hg0.7V0.3Ba1Sr1Cu1O4.6+z	Hg	0.7	V	0.3	Ba	1	Sr	1	Cu	1											O	4.6+z			1997																												Hg1201																				65					65										68																																																																																						mixture-sealed in quartz tube-heat(720C,16H)-Q to RT-ANN(400C,72H in Ar flow)					The 1201 superconductors Hg1-y(VO4)y(Ba,Sr)2CuO4-2y+z: evidence for VO4 tetrahedra	199704		Laboratoire CRISMAT,CNRS URA 1318,ISMRA et Universite' de Caen, Bd Marechal Juin, 14050 Caen Cedex, France	Physica.C,277(1997)119-132	A. Maignan,B. Raveau,C. Michel,K. Knizek,M. Hervieu,S. Malo		
7408	PHC2770024		(Cu,W)Sr2YCu2O7	Cu0.8W0.2Sr2Y1Cu2O7.3	Cu	0.8	W	0.2	Sr	2	Y	1	Cu	2											O	7.3	7.3		1997																											2	Cu1212	P4/mmm			3.802		11.497													74			77			77																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7409	PHC2770024		(Cu,Mo)Sr2YCu2	Cu0.8Mo0.2Sr2Y1Cu2O7.3	Cu	0.8	Mo	0.2	Sr	2	Y	1	Cu	2											O	7.3	7.3		1997																											2	Cu1212	P4/mmm			3.801		11.486													65						65																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7410	PHC2770024		(Cu,Re)Sr2YCu2O7	Cu0.85Re0.15Sr2Y1Cu2O7.3	Cu	0.85	Re	0.15	Sr	2	Y	1	Cu	2											O	7.3	7.3		1997																											2	Cu1212	P4/mmm			3.8		11.475													69						69																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7411	PHC2770024		(Cu,W)Sr2(Y,Ca)Cu2O7	Cu2.8W0.2Sr2Y0.9Ca0.1Oz	Cu	2.8	W	0.2	Sr	2	Y	0.9	Ca	0.1											O	z			1997																												Cu1212																			75			76			76																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7412	PHC2770024		(Cu,Mo)Sr2(Y,Ca)Cu2O7	Cu2.8Mo0.2Sr2Y0.9Ca0.1Oz	Cu	2.8	Mo	0.2	Sr	2	Y	0.9	Ca	0.1											O	z			1997																												Cu1212																			73			71			71																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7413	PHC2770024		(Cu,Re)Sr2(Y,Ca)Cu2O7	Cu2.85Re0.15Sr2Y0.9Ca0.1Oz	Cu	2.85	Re	0.15	Sr	2	Y	0.9	Ca	0.1											O	z			1997																												Cu1212																			75			73			73																																																																																																mixture-SIN(990C)-ANN(700C,200 atm O2)					Optimized synthesis and properties of chemically stabilized CuSr2YCu2O7	199704		Physics Department, Northern Illinois University, Dekalb, IL 60115, USA	Physica.C,277(1997)24-35	B. Dabrowski,J.D. Jorgensen,J.W. Koenitzer,K. Rogacki,K.R. Poeppelmeier		
7414	PHC2770252	insulator	Pb2Ba2Cu2TaO8Cl	Pb2Ba2Cu2Ta1O8Cl	Pb	2	Ba	2	Cu	2	Ta	1													O	8Cl			1997																											2		P4/mmm			3.951		15.608																																																																																																																	PbO,PbCl2,Ba(NO3)2,Ta2O5(or Nb2O5),CuO		mixture-preheat(550C,650C,12H in air)-pellet-CAL(700C,24H in air)-quickly cooled to RT					Synthesis and structure of layered cuprates contaning Pb2Cl as separating layer, Pb2Ba2Cu2MO8Cl(M=Ta,Nb)	199704		Department of Applied Chemistry, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica.C,277(1997)252-256	Rukang Li		
7415	PHC2770252	insulator	Pb2Ba2Cu2NbO8Cl	Pb2Ba2Cu2Nb1O8Cl	Pb	2	Ba	2	Cu	2	Nb	1													O	8Cl			1997																											2		P4/mmm			3.954		15.571																																																																																																																	PbO,PbCl2,Ba(NO3)2,Ta2O5(or Nb2O5),CuO		mixture-preheat(550C,650C,12H in air)-pellet-CAL(700C,24H in air)-quickly cooled to RT					Synthesis and structure of layered cuprates contaning Pb2Cl as separating layer, Pb2Ba2Cu2MO8Cl(M=Ta,Nb)	199704		Department of Applied Chemistry, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica.C,277(1997)252-256	Rukang Li		
7416	PHC2770265		CaLaBaCu3O7	Ca1La1Ba1Cu3O7	Ca	1	La	1	Ba	1	Cu	3													O	7		1	1997																											2	Y123			A	3.869		11.645																69			69																																																																																														La2O3,BaCO3,CaCO3,CuO,Fe2O3	1	mixture-fire(975C,12H)-Q to RT-heat(975C,12H in air)-FC to RT-pellet-ANN(575C,24H in O2 flow)-FC to RT					Structure, superconductivuty and normal state magnetism of CaLaBaCu3-xFeO7 superconductor, 0.0%$x%$0.24	199704		Departmento de Fisica, Universidad Federal de Pernambuco, 50670-901 Recife PE, Brazil	Physica.C,277(1997)265-270	A.V. Narlikar,D.A. Landinez Tellez,J. Albino Aguiar,J.M. Ferreira,Rajvir Singh,V.P.S. Awana		
7417	PHC2770265		CaLaBa(Cu,Fe)3O7	Ca1La1Ba1Cu2.97Fe0.03O7	Ca	1	La	1	Ba	1	Cu	2.97	Fe	0.03											O	7		1	1997	emu/mole	0.00074	emu.K/mol	3.25	myu-B/Fe	5.09	5.6																				2	Y123			A	3.866		11.643																49			49																																																																																														La2O3,BaCO3,CaCO3,CuO,Fe2O3	1	mixture-fire(975C,12H)-Q to RT-heat(975C,12H in air)-FC to RT-pellet-ANN(575C,24H in O2 flow)-FC to RT					Structure, superconductivuty and normal state magnetism of CaLaBaCu3-xFeO7 superconductor, 0.0%$x%$0.24	199704		Departmento de Fisica, Universidad Federal de Pernambuco, 50670-901 Recife PE, Brazil	Physica.C,277(1997)265-270	A.V. Narlikar,D.A. Landinez Tellez,J. Albino Aguiar,J.M. Ferreira,Rajvir Singh,V.P.S. Awana		
7418	PHC2770265		CaLaBa(Cu,Fe)3O7	Ca1La1Ba1Cu2.94Fe0.06O7	Ca	1	La	1	Ba	1	Cu	2.94	Fe	0.06											O	7		1	1997	emu/mole	0.00039	emu.K/mol	2.58	myu-B/Fe	4.53	1.96																				2	Y123			A	3.864		11.64																44			44																																																																																														La2O3,BaCO3,CaCO3,CuO,Fe2O3	1	mixture-fire(975C,12H)-Q to RT-heat(975C,12H in air)-FC to RT-pellet-ANN(575C,24H in O2 flow)-FC to RT					Structure, superconductivuty and normal state magnetism of CaLaBaCu3-xFeO7 superconductor, 0.0%$x%$0.24	199704		Departmento de Fisica, Universidad Federal de Pernambuco, 50670-901 Recife PE, Brazil	Physica.C,277(1997)265-270	A.V. Narlikar,D.A. Landinez Tellez,J. Albino Aguiar,J.M. Ferreira,Rajvir Singh,V.P.S. Awana		
7419	PHC2770265		CaLaBa(Cu,Fe)3O7	Ca1La1Ba1Cu2.88Fe0.12O7	Ca	1	La	1	Ba	1	Cu	2.88	Fe	0.12											O	7		1	1997	emu/mole	0.00082	emu.K/mol	0.97	myu-B/Fe	2.79	5.76																				2	Y123			A	3.863		11.638																28			28																																																																																														La2O3,BaCO3,CaCO3,CuO,Fe2O3	1	mixture-fire(975C,12H)-Q to RT-heat(975C,12H in air)-FC to RT-pellet-ANN(575C,24H in O2 flow)-FC to RT					Structure, superconductivuty and normal state magnetism of CaLaBaCu3-xFeO7 superconductor, 0.0%$x%$0.24	199704		Departmento de Fisica, Universidad Federal de Pernambuco, 50670-901 Recife PE, Brazil	Physica.C,277(1997)265-270	A.V. Narlikar,D.A. Landinez Tellez,J. Albino Aguiar,J.M. Ferreira,Rajvir Singh,V.P.S. Awana		
7420	PHC2770265		CaLaBa(Cu,Fe)O7	Ca1La1Ba1Cu2.76Fe0.24O7	Ca	1	La	1	Ba	1	Cu	2.76	Fe	0.24											O	7			1997	emu/mole			1.51		3.37	1.42																				2	Y123				3.862		11.635																22			22																																																																																														La2O3,BaCO3,CaCO3,CuO,Fe2O3	1	mixture-fire(975C,12H)-Q to RT-heat(975C,12H in air)-FC to RT-pellet-ANN(575C,24H in O2 flow)-FC to RT					Structure, superconductivuty and normal state magnetism of CaLaBaCu3-xFeO7 superconductor, 0.0%$x%$0.24	199704		Departmento de Fisica, Universidad Federal de Pernambuco, 50670-901 Recife PE, Brazil	Physica.C,277(1997)265-270	A.V. Narlikar,D.A. Landinez Tellez,J. Albino Aguiar,J.M. Ferreira,Rajvir Singh,V.P.S. Awana		
7421	CEM1230313	semiconductor	(Pb,Pb)(Sr,Ho)2(Ho,Ce)2Cu2Oz	Pb1Sr1.8Ho1.6Ce0.6Cu2Oz	Pb	1	Sr	1.8	Ho	1.6	Ce	0.6	Cu	2											O	z		1	1996																											2	Pb1222				3.837		29.189																																																																																																																	PbO,CdO,SrCO3,Ho2O3,CeO2,CuO	1	mixture-heat(830C,24H in air)-pellet-SIN(850C,10H in air)-slow cool to RT (30C/H)					Synthesis and Crystal Structure of New Pb-Based Copper Oxides (Pb0.5M0.5) (Sr0.9Ho0.1) (Ho0.7Ce0.3)2Cu2Oy(M=Pb and Cd)			National Laboratory for Superconductivity, Institute of Physics Academia Sinica, Beijing 100080, People's Republic of China	J.Solid State Chem.123(1996)313	C. Dong,F. Wu,G. C.  Che,H. Chen,H.M. Luo,Y.T. Qian,Z.X. Zhao,Z.Y. Chen		
7422	CEM1230313	semiconductor	(Pb,Cd)(Sr,Ho)2(Ho,Ce)2Cu2Oz	Pb0.5Cd0.5Ho1.6Ce0.6Cu2Oz	Pb	0.5	Cd	0.5	Ho	1.6	Ce	0.6	Cu	2											O	z		1	1996																											2	Pb1222				3.817		29.337																																																																																																																	PbO,CdO,SrCO3,Ho2O3,CeO2,CuO	1	mixture-heat(830C,24H in air)-pellet-SIN(850C,10H in air)-slow cool to RT (30C/H)					Synthesis and Crystal Structure of New Pb-Based Copper Oxides (Pb0.5M0.5) (Sr0.9Ho0.1) (Ho0.7Ce0.3)2Cu2Oy(M=Pb and Cd)			National Laboratory for Superconductivity, Institute of Physics Academia Sinica, Beijing 100080, People's Republic of China	J.Solid State Chem.123(1996)313	C. Dong,F. Wu,G. C.  Che,H. Chen,H.M. Luo,Y.T. Qian,Z.X. Zhao,Z.Y. Chen		
7423	CEM1230313	semiconductor	(Pb,Cu)(Sr,Ho)2(Ho,Ce)2Cu2Oz	Pb0.5Ho1.6Ce0.6Cu2.5Oz	Pb	0.5	Ho	1.6	Ce	0.6	Cu	2.5													O	z		1	1996																											2	Pb1222				3.83		29.081																																																																																																																	PbO,CdO,SrCO3,Ho2O3,CeO2,CuO	1	mixture-heat(830C,24H in air)-pellet-SIN(850C,10H in air)-slow cool to RT (30C/H)					Synthesis and Crystal Structure of New Pb-Based Copper Oxides (Pb0.5M0.5) (Sr0.9Ho0.1) (Ho0.7Ce0.3)2Cu2Oy(M=Pb and Cd)			National Laboratory for Superconductivity, Institute of Physics Academia Sinica, Beijing 100080, People's Republic of China	J.Solid State Chem.123(1996)313	C. Dong,F. Wu,G. C.  Che,H. Chen,H.M. Luo,Y.T. Qian,Z.X. Zhao,Z.Y. Chen		
7424	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La5.8Ca2.2Cu6Ni2O20	La	5.8	Ca	2.2	Cu	6	Ni	2													O	20			1996																											2					10.688		3.86											(8,8,20) structure						4																																																																																				1.11												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7425	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La6Ca2Cu6Ni2O20	La	6	Ca	2	Cu	6	Ni	2													O	20			1996																											2					10.706		3.864											(8,8,20) structure						4																																																																																				0.95												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7426	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La6.1Ca1.9Cu6Ni2O20	La	6.1	Ca	1.9	Cu	6	Ni	2													O	20			1996																											2					10.7		3.866											(8,8,20) structure						4																																																																																				0.95												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7427	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La6.4Ca1.6Cu6Ni2O20	La	6.4	Ca	1.6	Cu	6	Ni	2													O	20			1996																											2					10.719		3.863											(8,8,20) structure						4																																																																																				0.91												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7428	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La6.7Ca1.3Cu6Ni2O20	La	6.7	Ca	1.3	Cu	6	Ni	2													O	20			1996																											2					10.739		3.853											(8,8,20) structure						4																																																																																				2.63												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7429	CEM1210319		(La,Ca)8(Cu,Ni)8O20	La7Ca1Cu6Ni2O20	La	7	Ca	1	Cu	6	Ni	2													O	20			1996																											2					10.749		3.866											(8,8,20) structure						4																																																																																				2.86												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7430	CEM1210319	structure=8-8-20	(La,Ca)8(Cu,Ni)8O20	La6.4Ca1.6Cu6.5Ni1.5O20	La	6.4	Ca	1.6	Cu	6.5	Ni	1.5													O	20		1	1996																											2					10.719		3.862											(8,8,20) structure						4																																																																																																La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7431	CEM1210319	structure=8-8-20	(La,Ca)8(Cu,Ni)8O20	La6.4Ca1.6Ni7Ni1O20	La	6.4	Ca	1.6	Ni	7	Ni	1													O	20		1	1996																											2					10.746		3.863											(8,8,20) structure						4																																																																																				1.67												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7432	CEM1210319	structure=8-8-20	(La,Ca)8(Cu,Ni)8O20	La6.4Ca1.6Cu7.5Ni0.5O20	La	6.4	Ca	1.6	Cu	7.5	Ni	0.5													O	20		1	1996																											2					10.804		3.847											(8,8,20) structure						4																																																																																				2.38												La2O3,CaCO3,CuO,NiO	1	mixture-fire(1000C, in air)-heat(1025C in O2)					Stabilization of the 8-8-20 Structure-Type in La8-xCaxCu8-xNiyO20			AT & T Bell Laboratories, Murray Hill, new Jersey, 07974	J.Solid State Chem.121(1996)319	G.L. Roberts,J.J. Krajewski,R.J. Cava,S.A. Carter,W.F. Peck Jr.		
7433	CEM1210066		HgBa2CuOz	Hg1Ba2Cu1Oz	Hg	1	Ba	2	Cu	1															O	z		1	1996																											2	Hg1201				3.869		9.467																	4																																																																																																		precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7434	CEM1210066		(Hg,S)Ba2CuOz	Hg0.95S0.05Ba2Cu1Oz	Hg	0.95	S	0.05	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.882		9.395																	4																																																																																																		precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7435	CEM1210066		(Hg,S)Ba2CuOz	Hg0.9S0.1Ba2Cu1Oz	Hg	0.9	S	0.1	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.889		9.355																41			41																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7436	CEM1210066		(Hg,S)Ba2CuOz	Hg0.85S0.15Ba2Cu1Oz	Hg	0.85	S	0.15	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.901		9.305																62			62																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7437	CEM1210066		(Hg,S)Ba2CuOz	Hg0.8S0.2Ba2Cu1Oz	Hg	0.8	S	0.2	Ba	2	Cu	1													O	z		1	1996																											2	Hg1201				3.904		9.289																65			65																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7438	CEM1210066		(Hg,S)Ba2CuOz	Hg0.75S0.25Ba2Cu1Oz	Hg	0.75	S	0.25	Ba	2	Cu	1													O	z			1996																											2	Hg1201				3.901		9.3																63			63																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7439	CEM1210066		(Hg,S)Ba2CuOz	Hg0.7S0.3Ba2Cu1Oz	Hg	0.7	S	0.3	Ba	2	Cu	1													O	z			1996																											2	Hg1201				3.907		9.265																73			73																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7440	CEM1210066		(Hg,S)Ba2CuOz	Hg0.5S0.5Ba2Cu1Oz	Hg	0.5	S	0.5	Ba	2	Cu	1													O	z			1996																											2	Hg1201				3.907		9.276																71			71																																																																																																precursor(Ba2CuOz)-mixed with HgO,BaSO4,CuO in glove box-heat(920C, 0.6H)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7441	CEM1210066		(Hg,S)Ba2CuOz	Hg0.85S0.15Ba2Cu1Oz	Hg	0.85	S	0.15	Ba	2	Cu	1													O	z			1996																											2	Hg1201				3.906		9.304																77			77																																																																																																ANN(250C,10H in Ar flow)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7442	CEM1210066		HgBa2CuOz	Hg1Ba2Cu1Oz	Hg	1	Ba	2	Cu	1															O	z			1996																											2	Hg1201				3.88		9.504																88			88																																																																																																ANN(250C,10H in Ar flow)					The Replacement of [HgO2]2- by the Tetrahedral Sulfate Anion [SO4]2- in the Hg-1201 Superconductor			Laboratoir'e de Cristallograplie, CNRS-UJF, BP 166, 38042 Grenodle Cedex 09, France	J.Solid State Chem.121(1996)66	B. Souletie,E.V. Antipov,J.J. Capponi,M. Brunner,M. Marezio,P.G. Radaelli,S.M. Loureiro		
7443	JMR0111120		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.99Zn0.01O6+z	Y	1	Ba	2	Cu	2.99	Zn	0.01													O	6+z		3	1996																												Y123																						89			89																																																																																																solte-rich liquid-crystal pulling method, oxygenation (500C, in O2)					Zn doping in YBCO single crystal by the solute-rich liquid-crystal pulling method			Superconductivity Research Laboratory,ISTEC, 1-10-13 Shinonome Koto-Ku, Tokyo 135, Japan	J.Mater.Res.11(1996)1120	F. Wang,H. Zama,K. Ohtsu,S. Tajima,X. Yao,Y. Shiohara		
7444	JMR0111120		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.979Zn0.021O6+z	Y	1	Ba	2	Cu	2.979	Zn	0.021													O	6+z		3	1996																												Y123																						83			83																																																																																																solte-rich liquid-crystal pulling method, oxygenation (500C, in O2)					Zn doping in YBCO single crystal by the solute-rich liquid-crystal pulling method			Superconductivity Research Laboratory,ISTEC, 1-10-13 Shinonome Koto-Ku, Tokyo 135, Japan	J.Mater.Res.11(1996)1120	F. Wang,H. Zama,K. Ohtsu,S. Tajima,X. Yao,Y. Shiohara		
7445	JMR0111120		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.954Zn0.047O6+z	Y	1	Ba	2	Cu	2.954	Zn	0.047													O	6+z		3	1996																												Y123																						74			74																																																																																																solte-rich liquid-crystal pulling method, oxygenation (500C, in O2)					Zn doping in YBCO single crystal by the solute-rich liquid-crystal pulling method			Superconductivity Research Laboratory,ISTEC, 1-10-13 Shinonome Koto-Ku, Tokyo 135, Japan	J.Mater.Res.11(1996)1120	F. Wang,H. Zama,K. Ohtsu,S. Tajima,X. Yao,Y. Shiohara		
7446	JMR0111120		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.913Zn0.087O6+z	Y	1	Ba	2	Cu	2.913	Zn	0.087													O	6+z		3	1996																												Y123																						57			57																																																																																																solte-rich liquid-crystal pulling method, oxygenation (500C, in O2)					Zn doping in YBCO single crystal by the solute-rich liquid-crystal pulling method			Superconductivity Research Laboratory,ISTEC, 1-10-13 Shinonome Koto-Ku, Tokyo 135, Japan	J.Mater.Res.11(1996)1120	F. Wang,H. Zama,K. Ohtsu,S. Tajima,X. Yao,Y. Shiohara		
7447	JTL0630826		NdBa2Cu3O7	Nd1Ba2Cu3O6.67	Nd	1	Ba	2	Cu	3															O	6.67	6.67		1996																											2	Y123																				29					29																																																																																																not superconducting at 1 atm. it become superconducting at 1GPa holding 92H.					Appeararance of superconductivity in the tetragonal ceramic NdBa2Cu3O6.67 as a result of oxygen ordering under pressure			Donetsk Physicotechnical Institute, Ukrainian National Academy of Sciences, 340114 Donetsk, Ukraine	JETP Lett.63(1996)826	H. Szymczak,I.M. Fita,M. Baran,N.A. Doroshenko,V.P. Dyakonov		
7448	JTL0630561	hydorogenation rise Tc by 2K, Tc(La1.8Sr0.2CuO4)=30K	(La,Sr)2Cu(H,O)4	H0.2La1.8Sr0.2Cu1O4	H	0.2	La	1.8	Sr	0.2	Cu	1													O	4			1996																												T																				32					32																																																																																																La1.8Sr0.2CuO4 by solid state reaction, hydrogenation by ditect reaction with H2 gas (160C,600 Torr)					Spin-lattice relaxation and Knight shift on protons in the hydrogen-doped superconducting system H0.2La1.8Sr0.2CuO4			Kazan Physicotechnical Institute, Kazan Science Center of the Russian Academy of Sciences, 420029 Kazan, Russia	JETP Lett.63(1996)560	A.D. Shengelaya,N. Drulis,N.M. Suleimanov,R.G. Mustafin		
7449	JAC24000L4	semiconductor	(Bi,Cd)Sr2YCu2O7	Bi0.5Cd0.5Sr2Y1Cu2O7-z	Bi	0.5	Cd	0.5	Sr	2	Y	1	Cu	2											O	7-z			1996																											2	1212	P4/mmm			3.812		11.91																	77																																																																																																Bi2o3,CdO,SrO,CuO,R2O3	1	mixture-pellet-fire(1173K,36H in air)-SIN(1223K, 36H in air)					Sithesis and characterization of single Bi-O layered cuprate (Bi,Cd)Sr2YCu2O7-z			Institute of Physics, Chinese Academy of Sciences,Beijing 100080, People's Repblic of China	J.Alloys Compd240(1996)L4	Guanghui Rao,Jingkui Liang,Jinling Yang,Weihua Tang		
7450	MPL0100619		CaBaLaCu3O7	Ca1La1Ba1Cu3O7	Ca	1	La	1	Ba	1	Cu	3													O	7			1996																												Y123																						70			70																																																																																															1	mixture-ANN(400C,12H in air)-cool to RT					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7451	MPL0100619		CaBaLa(Cu,Zn)3O7	Ca1La1Ba1Cu2.97Zn0.03O7	Ca	1	La	1	Ba	1	Cu	2.97	Zn	0.03											O	7			1996	emu/mol	0.00027	emu.K/mol	0.016	myu-B/mol	0.36	20																					Y123																						60			60																																																																																															1	mixture-ANN(400C,12H in air)-cool to RT					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7452	MPL0100619		CaBaLa(Cu,Zn)3O7	Ca1La1Ba1Cu2.85Zn0.045O7	Ca	1	La	1	Ba	1	Cu	2.85	Zn	0.045											O	7			1996	emu/mol	0.00024	emu.K/mol	0.035	myu-B/mol	0.53	3.5																					Y123																						55			55																																																																																															1	mixture-ANN(400C,12H in air)-cool to RT					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7453	MPL0100619		CaBaLa(Cu,Zn)3O7	Ca1La1Ba1Cu2.91Zn0.09O7	Ca	1	La	1	Ba	1	Cu	2.91	Zn	0.09											O	7			1996	emu/mol	0.00023	emu.K/mol	0.039	myu-B/mol	0.56	15																					Y123																						20			20																																																																																															1	mixture-ANN(400C,12H in air)-cool to RT					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7454	MPL0100619		CaBaLa(Cu,Zn)3O7	Ca1La1Ba1Cu2.88Zn0.12O7	Ca	1	La	1	Ba	1	Cu	2.88	Zn	0.12											O	7			1996	emu/mol	0.00022	emu.K/mol	0.047	myu-B/mol	0.61	15																					Y123																						14			14																																																																																															1	mixture-ANN(400C,12H in air)-cool to RT					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7455	MPL0100619		CaBaLaCu3O7	Ca1Ba1La1Cu3O7	Ca	1	Ba	1	La	1	Cu	3													O	7			1996	emu/mol	0.00019	emu.K/mol	0.045	myu-B/mol	0.6	18.6																					Y123																						47			47																																																																																																ANN(400C, 12H in air)-Q to LN2					NORMAL STATE MAGNETISM OF Zn-DOPED AND OXYGEN DEFICIENT CaLaBaCu3O7 SUPERCONDUCTOR			Depto. de Fisica, Universidade Federal de Pernambuco, 50670-901, Recife, PE, Brasil	Mod.Phys.Lett.B(1996)619	A.V. NARLIKAR,D.A. LANDINEZ,J. ALBINO AGUIAR,J.M. FERRERA,RAJVIR SINGH,V.P.S. AWANA		
7456	MPL0100609		(Pb,V)2Sr2(Ca,Y)Cu3Oz	Pb2Sr2Ca0.5Y0.5Cu3Oz	Pb	2	Sr	2	Ca	0.5	Y	0.5	Cu	3											O	z		1	1996																											3	Pb3212				5.408	5.382	15.77													63	71	75				71																																																																																		46												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7457	MPL0100609		(Pb,V)2Sr2(Ca,Y)Cu3Oz	Pb1.8V0.2Sr2Ca0.5Y0.5Cu3Oz	Pb	1.8	V	0.2	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.397	5.37	15.72																																																																																																					54												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7458	MPL0100609		(Pb,V)2Sr2(Ca,Y)Cu3Oz	Pb1.6V0.4Sr2Ca0.5Y0.5Cu3Oz	Pb	1.6	V	0.4	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.401	5.372	15.68																																																																																																					93												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7459	MPL0100609		(Pb,V)2Sr2(Ca,Y)Cu3Oz	Pb1.4V0.6Sr2Ca0.5Y0.5Cu3Oz	Pb	1.4	V	0.6	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.403	5.35	15.7														40	75				40																																																																																		720												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7460	MPL0100609		(Pb,Cr)2Sr2(Ca,Y)Cu3Oz	Pb1.8Cr0.2Sr2Ca0.5Y0.5Cu3Oz	Pb	1.8	Cr	0.2	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.412	5.358	15.7																																																																																																					47												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7461	MPL0100609		(Pb,Cr)2Sr2(Ca,Y)Cu3Oz	Pb1.6Cr0.4Sr2Ca0.5Y0.5Cu3Oz	Pb	1.6	Cr	0.4	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.401	5.35	15.7																																																																																																					110												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7462	MPL0100609		(Pb,Cr)2Sr2(Ca,Y)Cu3Oz	Pb1.4Cr0.6Sr2Ca0.5Y0.5Cu3Oz	Pb	1.4	Cr	0.6	Sr	2	Ca	0.5	Y	0.5	Cu	3									O	z		1	1996																											3	Pb3212				5.397	5.339	15.69													45	67	75				67																																																																																		220												PbO,V2O3,Cr2O3,SrO,Y2O3,CaO,CuO	1	precursor(Sr2Ca0.5Y0.5Cu3Oz)+(PbO,V2O3 or Cr2O3)-pellet-SIN(900C,5H in air)-Q to RT-ANN(800C,2.5H+700C,24H in N2)					EFFECTS OF V-OR Cr-DOPING ON PHASE FORMATION, ELECTRIC PROPERTIES AND SUPERCONDUCTIVITY OF THE 3212-TYPE PHASE PBb2Sr2(Ca0.5Y0.5)Cu3Oz			Structural Reserch Laboratory, University of Science ? Technology of China (USTC),Academia Sinica, Hefei, 230026, China	Mad.Phys.Lett.B10(1996)609	B. Qu,H.M. LUO,L.M. WANG,Y.T. Qian,Z.Y. CHEN,Z.Z. SHENG		
7463	MPL0100573	inpurity phares=YB2CuO5,unknown.,no phase transition up to 80 kbay	(Yb,Sr)Ba2Cu3O7	Yb0.8Sr0.2Ba2Cu3O7-z	Yb	0.8	Sr	0.2	Ba	2	Cu	3													O	7-z			1996																											2	Y123				3.813		11.705																68			68																																																																																														Yb2O3,SrCO3,BaCO3,CuO	1	mixture-SIN()930C,19H-cool to RT					SYNTHESIS, CHARACTERISATION AND HIGH PRESSURE STUDIES OF Yb0.8Sr0.2Ba2Cu3O7-y SUPERCONDUCTOR			Department of Physics, Anna University, Madras 600 025, India	Mod.Phys.Lett.B10(1996)573	A. SEKAR,K. JEYABALAN,N. VICTOR JAYA,V. SARAVANAN		
7464	MPL0100029		Ba5Cu3Oz	Ba5Cu3Oz	Ba	5	Cu	3																	O	z		1	1996																											3					8.664	8.931	9.072																	5																																																																																																BaCO3,CuO	1	mixture-CAL(930C,10H in air)-pellet-SIN(940C,24H in air)-FC					SYNTHESIS AND CHARACTERISATION OF Ba5Cu3Oy			Department of Physics,Bharathidasan Govt. College for Women, Pondicherry, India	Mod.Phys.Lett.B10(1996)29	K. JEYABALAN,L.K. KALIYAPERUMAL		
7465	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Fe)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.98Fe0.02O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.98	Fe	0.02									O	8		1	1996	emu/mol	0.00015	emu/mol	0.05857	myu-B/mol	4.84																						Bi2212																						54.8			54.8																																																																																														Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7466	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Fe)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.96Fe0.04O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.96	Fe	0.04									O	8		1	1996	emu/mol	0.000186	emu/mol	0.106	myu-B/mol	4.6																						Bi2212																						48.5			48.5																																																																																														Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7467	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Fe)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.92Fe0.08O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.92	Fe	0.08									O	8		1	1996	emu/mol	0.00023	emu/mol	0.2079	myu-B/mol	4.56																						Bi2212																						33.8			33.8																																																																																														Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7468	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Fe)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.88Fe0.12O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.88	Fe	0.12									O	8		1	1996	emu/mol	0.00039	emu/mol	279.3	myu-B/mol	4.31																						Bi2212																						30.9			30.9																																																																																														Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7469	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Fe)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.84Fe0.16O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.84	Fe	0.16									O	8		1	1996	emu/mol	0.00047	emu/mol	0.35	myu-B/mol	4.18																						Bi2212																						26.1			26.1																																																																																														Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7470	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Co)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.96Co0.04O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.96	Co	0.04									O	8		1	1996	emu/mol	0.000152	emu/mol	0.0826	myu-B/mol	4.06																						Bi2212																						50.7			50.7																																																									12.6																																					Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7471	PR05308651		(Bu,Pb)2Sr2Ca(Cu,Co)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.94Co0.06O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.94	Co	0.06									O	8		1	1996	emu/mol	0.000218	emu/mol	0.1055	myu-B/mol	3.75																						Bi2212																						48.6			48.6																																																									15.6																																					Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7472	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Co)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.92Co0.08O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.92	Co	0.08									O	8		1	1996	emu/mol	0.000267	emu/mol	0.1315	myu-B/mol	3.62																						Bi2212																						43			43																																																									24.7																																					Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7473	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Co)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.88Co0.12O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.88	Co	0.12									O	8		1	1996	emu/mol	0.00038	emu/mol	0.1715	myu-B/mol	3.38																						Bi2212																						38.8			38.8																																																									18.3																																					Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7474	PR05308651		(Bi,Pb)2Sr2Ca(Cu,Co)2O8	Bi1.8Pb0.2Sr2Ca1Cu1.84Co0.16O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	1.84	Co	0.16									O	8		1	1996	emu/mol	0.00042	emu/mol	0.228	myu-B/mol	3.38																						Bi2212																						35.8			35.8																																																									18.4																																					Bi2O3,PbO,SrO,CaO,CuO,Fe2O3	1	mixture-CAL(800C,24H in air)-SIN(845C,80H in air)four times (reground,sintering)					Comparison of the low-temperature specific heat of Fe- and Co-doped Bi1.8Pb0.2Sr2Ca(Cu1-xMx)2O8(M=Fe or Co): Anomolously enhanced electronic contribution due to Fe doping	04		Department of Physics, University of Alberta, Edomonton, Alberta, Canada T6G2JI	Phys.Rev.B,53(1996)8651	J.P. Franck,M. K. Yu	Bi, Pb, Sr, Ca, Cu, Fe, Co, O	
7475	PHC2660104		HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O10+z	Hg	1	Ba	2	Ca	3	Cu	4													O	10+z		3	1996																												Hg1234																			124		130				127																																		HIR7475																																																									RH7475					high-pressure synthosis technique, see physica C.234(1994)10					Electrical resistivity and Hall effect of single crystal HgBa2Ca3Cu4O10+z	07		"Laboratorium fu""r Fesko""rperphysik, ETH-Zu""rich, 8093 Z""urich, Swezerland"	Physica.C,266(1996)104-108	"A. Morawski,J. Karpinski,J. Lo""hle,P. Wachter"	Hg, Ba, Ca, Cu, O	
7476	PHC2420197		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		4	1995																												Y123																				92					92												analyzing microwave absorption data	165																																																																																			films prepared by the laser ablation on MgO, thickness=5000A					Corrreation of static magnetization and microwave absorption measurements on superconducting films of YBa2Cu3O7-x	199502		Northeastern University,Boston,Massachusetts 02115,USA	Physica C.,242(1995)197-204	A.Drehman,A.Widom,C.Vittoria,D.Chrisey,H.Jiang,J.Horwitz,T.Yuan		
7477	JPM0060399	Kappa=100	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1994																											3	Bi2212	A2aa			5.41	5.412	30.88																92.4			92.4										48					156									67.9									0.95						22					2210																																																									Magnetization scaling below Tc in BiSrCaCuO and TlBaCaCuO superconducting ceramics			Universite' de Gene've, Departement de Physique de la Matie're, 24 Quai Emest Ansermet, CH01211 Gene've 4 , Swizerland	J. Phys.Condens.Matter 6(1994)L399-L404	A Junod,C Opagiste,D. Triscone,J Muller,J-Y Genoud,T. Tsukamoto		
7478	JPM0060399	Kappa=95	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6			1994																											2	Tl2201	I4/mmm			3.87		23.226																92.1			92.1															108									43.2									0.64						27.6					2630																																																									Magnetization scaling below Tc in BiSrCaCuO and TlBaCaCuO superconducting ceramics			Universite' de Gene've, Departement de Physique de la Matie're, 24 Quai Emest Ansermet, CH01211 Gene've 4 , Swizerland	J. Phys.Condens.Matter 6(1994)L399-L404	A Junod,C Opagiste,D. Triscone,J Muller,J-Y Genoud,T. Tsukamoto		
7479	JPM0060399	Kappa=94	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8			1994																											2	Tl2212	I4/mmm			3.855		29.328																108.7			108.7															206									79.7									0.99											1910																																																									Magnetization scaling below Tc in BiSrCaCuO and TlBaCaCuO superconducting ceramics			Universite' de Gene've, Departement de Physique de la Matie're, 24 Quai Emest Ansermet, CH01211 Gene've 4 , Swizerland	J. Phys.Condens.Matter 6(1994)L399-L404	A Junod,C Opagiste,D. Triscone,J Muller,J-Y Genoud,T. Tsukamoto		
7480	CRY0340057	not S/C,P=1,2,3, in THCFIG, are for sintering temperature=1100,1000,950C, respectively	YBaCuO5	Y2Ba1Cu1O5	Y	2	Ba	1	Cu	1															O	5		1	1994																												Y211																																																																																										THC7480																													Y2O3,BaCO3,CuO	1	mixture-CAL(900C,15H in air)-pellet-SIN(950-1100C,15H in air)					Thermal conductivity of YBCO(123) and YBCO(211) mixed crystals prepared by MMTG			Department of Materials Science and Technology, Faculty of Engineering, Iwate University, 4-3-5, Ueda, Morioka 020, Japan	Cryogenics.34(1994)57	H. Fujishiro,K. Noto,M. Ikebe,S. Kohayashi,S. Yoshizawa,T. Naito		
7481	CRY0340057	P=1 for ab-plane, P=2 for c-axis in THC Fig	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1994																												Y123																				90					90																																																																	THC7481																															modified melt texture growth(MMTG),(123):(211)=1:0.4, PT powder was added (0.5 at %) in order to make(211) phase disperse finely.					Thermal conductivity of YBCO(123) and YBCO(211) mixed crystals prepared by MMTG			Department of Materials Science and Technology, Faculty of Engineering, Iwate University, 4-3-5, Ueda, Morioka 020, Japan	Cryogenics.34(1994)57	H. Fujishiro,K. Noto,M. Ikebe,S. Kohayashi,S. Yoshizawa,T. Naito		
7482	PHC2460145			Hg0.7V0.3Sr1.8La0.2Cu1O4+z	Hg	0.7	V	0.3	Sr	1.8	La	0.2	Cu	1											O	4+z			1995																																																41.3					41.3																																																																			-7.44															2.57												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Seebeck coefficient and electrical-resisivity measurements for semiconducting anitiferromagnetic YBa2Cu3Oz,up to 1000 K Evidence for phonon drag and storng electron-phonon coupling	199504		URA 446,Laboratoire des Composes Non-Stoechiomeriques,Batiment 415,Universite Paris-Sud,91405 Orsay Cedex,France	Physica C.,246(1995)145-155	C.Picard,P.Gerdanian		
7483	PHC2640145			Hg0.7V0.3Sr1.7La0.3Cu1O4+z	Hg	0.7	V	0.3	Sr	1.7	La	0.3	Cu	1											O	4+z			1996																																																49.7					49.7																																																																			-6.25															1.53												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7484	PHC2640145			Hg0.7V0.3Sr1.6La0.4Cu1O4+z	Hg	0.7	V	0.3	Sr	1.6	La	0.4	Cu	1											O	4+z			1996																																																47.1					47.1																																																																			-5.29															1.66												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7485	PHC2640145			Hg0.7V0.3Sr1.5La0.5Cu1O4+z	Hg	0.7	V	0.3	Sr	1.5	La	0.5	Cu	1											O	4+z			1996																																																49.7					49.7																																																																			-5.34															2.05												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7486	PHC2640145			Hg0.7V0.3Sr1.4La0.6Cu1O4+z	Hg	0.7	V	0.3	Sr	1.4	La	0.6	Cu	1											O	4+z			1996																																																48.8					48.8																																																																			-4.55															2.96												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7487	PHC2640145			Hg0.7V0.3Sr1.3La0.7Cu1O4+z	Hg	0.7	V	0.3	Sr	1.3	La	0.7	Cu	1											O	4+z			1996																																																51.8					51.8																																																																			-3.59															3.74												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7488	PHC2640145			Hg0.7V0.3Sr1.2La0.8Cu1O4+z	Hg	0.7	V	0.3	Sr	1.2	La	0.8	Cu	1											O	4+z			1996																																																49.7					49.7																																																																			-4.56															4.78												V2O5,Sr(NO3)2,La2O3,CuO,HgO		mixture(V,Sr,La,Cu,O)-heat(750C,3H)-preunrsor +HgO-sealed in evaquated quartq tube-heat(880C,8H)-Q to RT					Anew mercury-based high-Tc cuprate Hg0.7 V0.3 Sr2-x Lax CuO4+z	06		Saha Lnstitute of Nuclear Physics,I/AF Bidhannagar, Calcutta-700064, India	Physica.C,264(1996)145-153	B. Bandyopadhyay,B. Ghosh,F. Fauth,J.B. Mandal,T. Chattopadhyay	Hg, V, Sr, La, Cu, O	
7489	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.346	Y	1	Ba	2	Cu	3															O	z	6.346	3	1992																												Y123																				12.3					12.3			K/GPa	7.16																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7490	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.409	Y	1	Ba	2	Cu	3															O	z	6.409	3	1992																												Y123																				26					26			K/GPa	4.38																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7491	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O	z	6.55	3	1992																												Y123																				54.1					54.1			K/GPa	3.99																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7492	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	z	6.6	3	1992																												Y123																				58.4					58.4			K/GPa	4.54																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7493	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	z	6.72	3	1992																												Y123																				80.7					80.7			K/GPa	4.46																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7494	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.74	Y	1	Ba	2	Cu	3															O	z	6.74	3	1992																												Y123																				82.6					82.6			K/GPa	4.03																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7495	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O	z	6.78	3	1992																												Y123																				88.1					88.1			K/GPa	4.07																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7496	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O4.86	Y	1	Ba	2	Cu	3															O	z	4.86	3	1992																												Y123																				93.2					93.2			K/GPa	1.72																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7497	PRL0690680		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	z	7	3	1992																												Y123																				94.3					94.3			K/GPa	0.62																																																																																												self flux method, typical size=1.2*1.1*0.26 mm3, c-axis is tho shortist.					PRESSURE DEPENDENCE OF TC AND CHARGE TRANSFER IN YBA2CU3OX (6.35<-X<-7) SINGLE CRYSTALS	199207			PHYS.REV.LETT.69(1992)680	A.P.PAULIKAS,B.W.LEE,B.W.VEAL,C.C.ALMASAN,J.E.SCHIRBER,J.W.DOWNEY,L.M.PAULIUS,M.B.MAPLE,S.H.HAN,Z.FISK	Y,BA,CU,O	
7498	SUP0090097		Y(Sr,Ba)2(Cu,B)3Oz	Y1Sr1Ba1Cu2.5B0.5Oz	Y	1	Sr	1	Ba	1	Cu	2.5	B	0.5											O	z			1996																												Y123																				25					25																																																																																														Y2O3,SrCO3,Y2(SO4)3.8H2O,H3BO3,SrSeO4		mixture-heat(1000-1065C,14H in O2)-ANN(425C,24H in 250 bar O2)					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7499	SUP0090097	not SC	(Y,Ce,Sr)Sr2(Cu,S)3Oz	Y1.4Ce0.5Sr2.1Cu2.75S0.25Oz	Y	1.4	Ce	0.5	Sr	2.1	Cu	2.75	S	0.25											O	z			1996																												Y123																							5		20																																																																																														Y2O3,SrCO3,Y2(SO4)3.8H2O,H3BO3,SrSeO4		mixture-heat(1000-1065C,14H in O2)-ANN(425C,24H in 250 bar O2)					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7500	SUP0090097		(Y,Ce)Sr2(Cu,Se)3Oz	Y1.5Ce0.5Sr2Cu2Se1Oz	Y	1.5	Ce	0.5	Sr	2	Cu	2	Se	1											O	z			1996																												Y123																							5																																																																																																Y2O3,SrCO3,Y2(SO4)3.8H2O,H3BO3,SrSeO4		mixture-heat(1000-1065C,14H in O2)-ANN(425C,24H in 250 bar O2)					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7501	SUP0090097	not S/C	(Y,Sr)Sr2(Cu,C)3O7	Y0.86Sr2.14Cu2.6C0.4O7	Y	0.86	Sr	2.14	Cu	2.6	C	0.4													O	7			1996																												Y123																							5																																																																																																Y2O3,SrCO3,CuO		mixture-heat(1273K, in air)-heat(1273K,2H in O2+CO2)-Q to RT					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7502	SUP0090097		(Y,Ca)(Sr,Ba)2(Cu,B)3Oz	Y0.85Ca0.15Sr1Ba1Cu2.5B0.5Oz	Y	0.85	Ca	0.15	Sr	1	Ba	1	Cu	2.5	B	0.5									O	z			1996																												Y123																				36					36																																																																																																mixture-heat(1000-1065C, 14H in O2)					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7503	SUP0090097		(Y,Ca)(Sr,Ba)2(Cu,B)3Oz	Y0.85Ca0.15Sr0.5Ba1.5Cu2.5B0.5Oz	Y	0.85	Ca	0.15	Sr	0.5	Ba	1.5	Cu	2.5	B	0.5									O	z			1996																												Y123																				55					55																																																																																																mixture-heat(1000-1065C, 14H in O2)					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7504	SUP0090097			Y1.4Ce0.5Sr2.1Cu2.75S0.25Oz	Y	1.4	Ce	0.5	Sr	2.1	Cu	2.75	S	0.25											O	z			1996																																																20					20																																																																																																HP treatment					Analysis of oxyanion (BO3(3-), CO3(2-), SO4(2-), PO4(3-), SeO4(4-)) substitution in Y123 compounds studied by X-ray photoelectron spectroscopy			Institute of Metal Physics, Russian Academy of Sciences, Ural Division, 620219 Yekaterinburg, GSP-170, Russia	J.Superconductivity,9(1996)97	C. Greaves,E.Z. Kurmaev,M. Neumann,P.R. Slater,S. Bartkowski,S. Uhlenbrock,V.V. Fedorenko,Y. Miyazaki,V.R. Galakhov		
7505	PHC2750299		NdBa2Cu3O7	Nd1Ba2Cu3Oz	Nd	1	Ba	2	Cu	3															O	z		1	1997																											3	Y123				3.857	3.916	11.755															98.7				98.7																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7506	PHC2750299		Nd(Ba,Nd)2Cu3O7	Nd1.05Ba1.95Cu3Oz	Nd	1.05	Ba	1.95	Cu	3															O	z		1	1997																											3	Y123				3.861	3.911	11.748															98.6				98.6																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7507	PHC2750299		Nd(Ba,Nd)2Cu3O7	Nd1.1Ba1.9Cu3Oz	Nd	1.1	Ba	1.9	Cu	3															O	z		1	1997																											3	Y123				3.862	3.896	11.739															98.3				98.3																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7508	PHC2750299		Nd(Ba,Nd)2Cu3O7	Nd1.15Ba1.85Cu3Oz	Nd	1.15	Ba	1.85	Cu	3															O	z		1	1997																											3	Y123				3.867	3.89	11.724															94				94																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7509	PHC2750299		Nd(Ba,Nd)2Cu3O7	Nd1.2Ba1.8Cu3Oz	Nd	1.2	Ba	1.8	Cu	3															O	z		1	1997																											3	Y123				3.881	3.888	11.719															96.1				96.1																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7510	PHC2750299		Nd(Ba,Nd)2Cu3O7	Nd1.25Ba1.75Cu3Oz	Nd	1.25	Ba	1.75	Cu	3															O	z		1	1997																											3	Y123				3.887	3.887	11.714															97.4				97.4																																																																																																powder mixture from metal acetates-mixture-CAL(780-860C,2-20H in 0,1 or 1% O2 in N2)-ANN(450C,5H in O2)					Relationship of solubility parameter (X), power properties and phase formation in the Nd1+xBa2-xCu3O6.5+z/2+z system	199702		Chemical Engineering Department,Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Physica.C,275(1997)299-310	A. Friedman,G.E. Shter,G.M. Reisner,G.S. Grader,P.Yossefov,Y. Yeshurun		
7511	PHC2750279		Bi2Sr2(Ca,Ce)Cu2O8+z	Bi2Sr2Ca0.9Ce0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Ce	0.1	Cu	2											O	8+z		3	1997																											3	Bi2212				5.393	5.4	30.949													90						90																																																																																														Bi2O3,SrCO3,CaCO3,CuO,CeO2	5	mixture(nominal 2:2:1:2)-heat 750C-kept 10H-heat(1000,1020,1050C for 15H)-cool to 830C (2C/H)					Growth and characterization of superconducting Bi2Sr2Ca(1-x)CexCu2O8+z single crystals	199702		Crystal Growth Centre, Anna University, Madras 600 025, India	Physica.C,275(1997)279-283	A. Thamizhavel,C. Subramanian,D. Prabhakaran,R. Jayavel		
7512	PHC2750279		Bi2Sr2(Ca,Ce)Cu2O8+z	Bi2Sr2Ca0.8Ce0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Ce	0.2	Cu	2											O	8+z		3	1997																											3	Bi2212				5.417	5.42	30.866													81						81																																																																																														Bi2O3,SrCO3,CaCO3,CuO,CeO2	5	mixture(nominal 2:2:1:2)-heat 750C-kept 10H-heat(1000,1020,1050C for 15H)-cool to 830C (2C/H)					Growth and characterization of superconducting Bi2Sr2Ca(1-x)CexCu2O8+z single crystals	199702		Crystal Growth Centre, Anna University, Madras 600 025, India	Physica.C,275(1997)279-283	A. Thamizhavel,C. Subramanian,D. Prabhakaran,R. Jayavel		
7513	PHC2750279		Bi2Sr2(Ca,Ce)Cu2O8+z	Bi2Sr2Ca0.7Ce0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Ce	0.3	Cu	2											O	8+z		3	1997																											3	Bi2212				5.42	5.428	30.849													78						78																																																																																														Bi2O3,SrCO3,CaCO3,CuO,CeO2	5	mixture(nominal 2:2:1:2)-heat 750C-kept 10H-heat(1000,1020,1050C for 15H)-cool to 830C (2C/H)					Growth and characterization of superconducting Bi2Sr2Ca(1-x)CexCu2O8+z single crystals	199702		Crystal Growth Centre, Anna University, Madras 600 025, India	Physica.C,275(1997)279-283	A. Thamizhavel,C. Subramanian,D. Prabhakaran,R. Jayavel		
7514	PHC2750279		Bi2Sr2(Ca,Ce)Cu2O8+z	Bi2Sr2Ca0.6Ce0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Ce	0.4	Cu	2											O	8+z		3	1997																											3	Bi2212				5.427	5.436	30.762													71						71																																																																																														Bi2O3,SrCO3,CaCO3,CuO,CeO2	5	mixture(nominal 2:2:1:2)-heat 750C-kept 10H-heat(1000,1020,1050C for 15H)-cool to 830C (2C/H)					Growth and characterization of superconducting Bi2Sr2Ca(1-x)CexCu2O8+z single crystals	199702		Crystal Growth Centre, Anna University, Madras 600 025, India	Physica.C,275(1997)279-283	A. Thamizhavel,C. Subramanian,D. Prabhakaran,R. Jayavel		
7515	PHC2750279		Bi2Sr2(Ca,Ce)Cu2O8+z	Bi2Sr2Ca0.5Ce0.5Cu2O8+z	Bi	2	Sr	2	Ca	0.5	Ce	0.5	Cu	2											O	8+z		3	1997																											3	Bi2212				5.436	5.448	30.693													60						60																																																																																														Bi2O3,SrCO3,CaCO3,CuO,CeO2	5	mixture(nominal 2:2:1:2)-heat 750C-kept 10H-heat(1000,1020,1050C for 15H)-cool to 830C (2C/H)					Growth and characterization of superconducting Bi2Sr2Ca(1-x)CexCu2O8+z single crystals	199702		Crystal Growth Centre, Anna University, Madras 600 025, India	Physica.C,275(1997)279-283	A. Thamizhavel,C. Subramanian,D. Prabhakaran,R. Jayavel		
7516	EPL0330153	d=1200A, surface resistance=10m ohm	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		4	1996																																																86					86																																										microwave transmission	3400																																																					films are epitaxially grown by laser ablation on MgO					Linear temperature variation of the penetration depth in YBa2Cu3O7-delta thin films	199601		Laboratoire de Physique de la Matiere Condensee, Ecole Normale Superieure 24 rue Lhomond-75231 Paris Cedex 05, France	Europhys.Lett.,33(1996)153-158	J.C. MAGE,J.P. VIEREN,L.A. de VAULCHIER,N. BONTEMPS,R. COMBESCOT,Y. GULDNER,Y. LEMAITRE		
7517	EPL0330153	d=1000A, surface resistance=0.27m Ohm, good quarity	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		4	1996																																																92					92																																										microwave transmission	1570																																																					films are epitaxially grown by laser ablation on MgO					Linear temperature variation of the penetration depth in YBa2Cu3O7-delta thin films	199601		Laboratoire de Physique de la Matiere Condensee, Ecole Normale Superieure 24 rue Lhomond-75231 Paris Cedex 05, France	Europhys.Lett.,33(1996)153-158	J.C. MAGE,J.P. VIEREN,L.A. de VAULCHIER,N. BONTEMPS,R. COMBESCOT,Y. GULDNER,Y. LEMAITRE		
7518	PRL0740598	PENET(a)=1600A,  PENET(b)=1000A	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95	3	1995																												Y123																				93.5				0.2	93.5																																										from Reflectance	1600																																																					single crystal was grown under high oxygen pressure.					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
7519	PRL0740598	PENET(a)=2000A, PENET(b)=800A	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1995																												Y124																				80				0.5	80																																										Kramers-Kronig relation	2000																																																					single crystal was grown under high oxygen pressure					In-Plane Anisotropy of the Penetration Depth in YBa2Cu3O7-x and YBa2Cu4O8 Superconductors	199501		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.Lett.,74(1995)0598	B.Dabrowski,D.A.Bonn,D.B.Tanner,D.M.Ginsberg,D.N.Basov,J.P.Rice,M.Quijada,R.Liang,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
7520	PHC1851089		YBa2Cu3O7	Y1Ba2Cu3O6.97	Y	1	Ba	2	Cu	3															O	z	6.97	1	1991																												Y123																				89.5					89.5																																										muon spin rotation	1300																																																										MOUN-SPIN ROTARION (microSR)STUDY OF THE TEMPERATURE DEPENDENCE OF THE LONDON PETRATION DEPTH IN COPPER OXIDE SUPERCONDUCTORS			Physik-Institut der Universitat Zurich, CH-8001 Zurich	Physica C 185-189(1991)1089	B. STAUBLE-PUMPIN,C. ROSSEL,D. ZECH,E. KALDIS,H. KELLER,H. SIMMLER,I.M. SAVIC,J. KARPINSKI,J.H. BREWER,J.W. SCHNEIDER,M. WARDEN,P. ZIMMERMANN,S. RUSIECKI,T.M. RISEMAN,W. KUNDIG,Y. MAENO		
7521	PHC1851089		YBa2Cu3O7	Y1Ba2Cu3O6.556	Y	1	Ba	2	Cu	3															O	z	6.556	1	1991																												Y123																				59.4					59.4																																										muon spin rotation	2200																																																										MOUN-SPIN ROTARION (microSR)STUDY OF THE TEMPERATURE DEPENDENCE OF THE LONDON PETRATION DEPTH IN COPPER OXIDE SUPERCONDUCTORS			Physik-Institut der Universitat Zurich, CH-8001 Zurich	Physica C 185-189(1991)1089	B. STAUBLE-PUMPIN,C. ROSSEL,D. ZECH,E. KALDIS,H. KELLER,H. SIMMLER,I.M. SAVIC,J. KARPINSKI,J.H. BREWER,J.W. SCHNEIDER,M. WARDEN,P. ZIMMERMANN,S. RUSIECKI,T.M. RISEMAN,W. KUNDIG,Y. MAENO		
7522	PHC1851089		YBa2Cu3O7	Y1Ba2Cu3O6.516	Y	1	Ba	2	Cu	3															O	z	6.516	1	1991																												Y123																				57.7					57.7																																										muon spin rotation	2500																																																										MOUN-SPIN ROTARION (microSR)STUDY OF THE TEMPERATURE DEPENDENCE OF THE LONDON PETRATION DEPTH IN COPPER OXIDE SUPERCONDUCTORS			Physik-Institut der Universitat Zurich, CH-8001 Zurich	Physica C 185-189(1991)1089	B. STAUBLE-PUMPIN,C. ROSSEL,D. ZECH,E. KALDIS,H. KELLER,H. SIMMLER,I.M. SAVIC,J. KARPINSKI,J.H. BREWER,J.W. SCHNEIDER,M. WARDEN,P. ZIMMERMANN,S. RUSIECKI,T.M. RISEMAN,W. KUNDIG,Y. MAENO		
7523	PHC1851089		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1991																												Y124																				80.2					80.2																																										muon spin rotation	1600																																																										MOUN-SPIN ROTARION (microSR)STUDY OF THE TEMPERATURE DEPENDENCE OF THE LONDON PETRATION DEPTH IN COPPER OXIDE SUPERCONDUCTORS			Physik-Institut der Universitat Zurich, CH-8001 Zurich	Physica C 185-189(1991)1089	B. STAUBLE-PUMPIN,C. ROSSEL,D. ZECH,E. KALDIS,H. KELLER,H. SIMMLER,I.M. SAVIC,J. KARPINSKI,J.H. BREWER,J.W. SCHNEIDER,M. WARDEN,P. ZIMMERMANN,S. RUSIECKI,T.M. RISEMAN,W. KUNDIG,Y. MAENO		
7524	PHC1851089		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1991																												Bi2212																				86.4					86.4																																										mon spin rotation	2100																																																										MOUN-SPIN ROTARION (microSR)STUDY OF THE TEMPERATURE DEPENDENCE OF THE LONDON PETRATION DEPTH IN COPPER OXIDE SUPERCONDUCTORS			Physik-Institut der Universitat Zurich, CH-8001 Zurich	Physica C 185-189(1991)1089	B. STAUBLE-PUMPIN,C. ROSSEL,D. ZECH,E. KALDIS,H. KELLER,H. SIMMLER,I.M. SAVIC,J. KARPINSKI,J.H. BREWER,J.W. SCHNEIDER,M. WARDEN,P. ZIMMERMANN,S. RUSIECKI,T.M. RISEMAN,W. KUNDIG,Y. MAENO		
7525	PHC2240263	optimal oxygen content	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1994																											3	Y123	Pmmm			3.817	3.885	11.685															92.3				92.3										41					27.9						curve fitting to M(H,T)			275									4.12				calculated from Hc2(0)		10.9			from magnetization, WHH model	1450																																																										Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7526	PHC2240263	optimal oxygen content	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1994																											3	Y123	Pmmm			3.817	3.886	11.679															91.7				91.7										68					321						curve fitting to M(H,T)			290									4.5				calculated from Hc2(0)		10.6			from magnetization,WHH model	1360																																																										Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7527	PHC2240263		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1994																											3	Y124	Ammm			3.843	3.871	27.242															80.1				80.1										39					166						curve fitting to M(H,T)			89									1.52				calculated from Hc2(0)		19.3			from magnetization,WHH model	1970																																																										Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7528	PHC2240263	optimal oxygen content	YBa4Cu7O14	Y2Ba4Cu7O14	Y	2	Ba	4	Cu	7															O	14		1	1994																											3	Y247				3.832	3.877	50.6															94.2				94.2										45					225						curve fitting to M(H,T)			114									1.76				calculated from Hc2(0)		16.9			from magnetization,WHH model		1930																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7529	PHC2240263	optimal oxygen content	Y2Ba4Cu7O14	Y2Ba4Cu7O14	Y	2	Ba	4	Cu	7															O	14		1	1994																											3	Y247				3.831	3.877	50.591															94.8				94.8										36											curve fitting to M(H,T)			127									1.89				calculated from HC2(0)		16.1			from magnetization,WHH model	1860																																																										Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7530	PHC2240263	optimal oxygen content	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1994																											3	Bi2212	A2aa			5.409	5.411	30.9															93.7				93.7										32		curve fitting to M(H,T)			160						curve fitting to M(H,T)			58.3									0.82				calculated from Hc2(0)		23.8					2770																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7531	PHC2240263	optimal oxygen content	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1994																											3	Bi2212	A2aa			5.41	5.412	30.88															92.4				92.4										48		curve fitting to M(H,T)			156						curve fitting to M(H,T)			67.9									0.95				calculated from Hc2(0)		22			from magnetization,WHH model		2490																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7532	PHC2240263	optimal oxygen content	TlBa2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1994																											2	Tl2201	I4/mmm			3.87		23.226															92.1				92.1										61		curve fitting to M(H,T)			108						curve fitting to M(H,T)			43.2									0.64				calculated from Hc2(0)		27.6			from magnetization,WHH model		2880																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7533	PHC2240263	optimal oxygen content	TlBa2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1994																											2	Tl2201	I4/mmm			3.871		23.224															92.1				92.1										63		curve fitting to M(H,T)			139						curve fitting to M(H,T)			46.7									0.66				calculated from Hc2(0)		26.5			from magnetization,WHH model		2550																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7534	PHC2240263	optimal oxygen content	TlBa2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		1	1994																											2	Tl2212	I4/mmm			3.855		29.328															108.7				108.7										45		curve fitting to M(H,T)			206						curve fitting to M(H,T)			79.7									0.99				calculated from Hc2(0)		20.3			from magnetization,WHH model		1970																																																									Reversible magnetization below Tc in  high-quality superconducting ceramics	199405			Physica C 224 (1994)263-276	A.F.Khoder,A.Junod,C.Opagiste,E.Janod,G.Triscone,J,-Y.Genoud,J.Muller,M.Couach,T.Graf,T.Tsukamoto	Tl,Y,Ba,Cu,O,Bi,Sr,Cu	
7535	PR05106035	c-axis grain-aligned sample with 12-20 micron single crystals. Hc(0)=5225 Oe	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1995																												Y124																						81.8			81.8												clean limit,G-L parametes	220								using clem-Hao thory,M(T),WHHthory	58.1									1.02						from Hc2		23.8					1880																																																				mixture-heat(900C in air )-high pressure(1050C,12H in 20%O2-Ar(600 atm O2))-RT(1.5C/min)					Reversible magnetization, critical, fields, and vortex structure in grain-aligned YBa2Cu4O8	199503		Ames Laboratory, U.S. Department of Enargy and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,51(1995)6035	B. Dabrowski,B.J. Suh,J. Gohng,Junghun Sok,L.A. Schwartzkopf,Ming Xu,Wei Chen		
7536	PR0428710		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1990	cm3/g																											Bi2212																						85		0.8	85										91											calculated from Pcohere	280															calculated from susceptibility		10.9																																																									self-flux method by heating 950C and slowly cooling					MAGNETIC-SUSCEPTIBILITY ANISOTROPY OF SINGLE-CRYSTAL BI2SR2CACU2O8	199011	SUSCEPTIBILITY      ,SINGLE CRYSTAL      ,ANISOTROPIES	AMES LABORATORY, UNITED STATES DEPARTMENT OF ENERGY AND DEPARTMENT OF PHYSICS, IOWA STATE UNIVERSITY, AMES,IOWA 50011	PHYS.REV.B,42(1990)8710	D.C.JOHNSTON,J.H.CHO	BI,SR,CA,CU,O	
7537	SSC1010129			Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3		1	1997																												BPBO																				12					12																																																																																														BaCO3,PbO,Bi2O3,CeO2		mixture-heat(800C, overnight in air)-heat(850C,20H)-bar-SIN(900C,24H in O2 flow)-slow cool to RT					Transport properties of the Ce-doped Ba(Pb,Bi)O3 system			Leiden Institure of Chemistry, Gorlaeus Laboratories, Leiden University, P.O. Box 9502,2300 RA Leiden, The Netherlands	Solid State Commun., 101()129	H.C.F. Martens,W.J.A. Maaskant,W.T. Fu		
7538	SSC1010129	R=RO * exp(TO/T)^(r) R=1/4		Ba1Pb0.7Ce0.05Ni0.25O3	Ba	1	Pb	0.7	Ce	0.05	Ni	0.25													O	3		1	1997																																																			4																																																																																																BaCO3,PbO,Bi2O3,CeO2		mixture-heat(800C, overnight in air)-heat(850C,20H)-bar-SIN(900C,24H in O2 flow)-slow cool to RT					Transport properties of the Ce-doped Ba(Pb,Bi)O3 system			Leiden Institure of Chemistry, Gorlaeus Laboratories, Leiden University, P.O. Box 9502,2300 RA Leiden, The Netherlands	Solid State Commun., 101()129	H.C.F. Martens,W.J.A. Maaskant,W.T. Fu		
7539	SSC1010129			Ba1Pb0.65Ce0.1Bi0.25O3	Ba	1	Pb	0.65	Ce	0.1	Bi	0.25													O	3		1	1997																																																			4																																																																																																BaCO3,PbO,Bi2O3,CeO2		mixture-heat(800C, overnight in air)-heat(850C,20H)-bar-SIN(900C,24H in O2 flow)-slow cool to RT					Transport properties of the Ce-doped Ba(Pb,Bi)O3 system			Leiden Institure of Chemistry, Gorlaeus Laboratories, Leiden University, P.O. Box 9502,2300 RA Leiden, The Netherlands	Solid State Commun., 101()129	H.C.F. Martens,W.J.A. Maaskant,W.T. Fu		
7540	SUP0100013		(La,Sr)2CuO4	La1.85Sr0.15Cu1Oz	La	1.85	Sr	0.15	Cu	1															O	z		1	1997																											2	T				3.771		13.212															38.2				38.2																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7541	SUP0100013		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.95Zn0.05Oz	La	1.85	Sr	0.15	Cu	0.95	Zn	0.05													O	z		1	1997																											2	T				3.778		13.201																	10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7542	SUP0100013		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9Zn0.1Oz	La	1.85	Sr	0.15	Cu	0.9	Zn	0.1													O	z		1	1997																											2	T				3.784		13.17																	10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7543	SUP0100013		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.8Zn0.2Oz	La	1.85	Sr	0.15	Cu	0.8	Zn	0.2													O	z		1	1997																											3	T				3.797	3.803	13.145																	10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7544	SUP0100013		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.7Zn0.3Oz	La	1.85	Sr	0.15	Cu	0.7	Zn	0.3													O	z		1	1997																											3	T				3.806	3.821	13.122																	10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7545	SUP0100013		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01Oz	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	z		1	1997																											3	T																							10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7546	SUP0100013		(La,Sr)2(Cu,Mg))O4	La1.85Sr0.15Cu0.99Mg0.01Oz	La	1.85	Sr	0.15	Cu	0.99	Mg	0.01													O	z		1	1997																											2	T																					30				30																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7547	SUP0100013		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.98Mg0.02Oz	La	1.85	Sr	0.15	Cu	0.98	Mg	0.02													O	z		1	1997																											2	T																					15.9				15.9																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7548	SUP0100013		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.97Mg0.03Oz	La	1.85	Sr	0.15	Cu	0.97	Mg	0.03													O	z		1	1997																											2	T																							10																																																																																																La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7549	SUP0100013		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01Oz	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	z		1	1997																											2	T																					32.1				32.1																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7550	SUP0100013		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02Oz	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	z		1	1997																											2	T																					28				28																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7551	SUP0100013		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03Oz	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	z		1	1997																											2	T																					21.9				21.9																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7552	SUP0100013		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.96Ni0.04Oz	La	1.85	Sr	0.15	Cu	0.96	Ni	0.04													O	z		1	1997																											2	T																					16.1				16.1																																																																																														La2O3,SrCO3,CuO,MO	1	mixture-heat (1000C,12H in air)-pellet SIN(1000-1180C,1 day in O2 flow)-cool to  600C-ANN(600C,1day)					Two-dimensional hole localization induced by Zn, Ni, and Mg dopings in Cu sites in La1.85Sr0.15Cu1-xMxOy				J.Superconductivity , 10(1997)13	Mao Zhiqiang,Tian Mingliang,Wang Yu,Xu Gaojie,Zhang Yuheng		
7553	PHC2290209		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1994																												Bi2212																				85.1		84.5			85.1																																																									2.1		283																																					travelling solvent floating zone method					Specific heat up to 14 tesla magnetization of a Bi2Sr2CaCu2O8 single crystal: Thermodynamics of a 2D superconductor	199408			Physica C, 229(1994)209-230	A.Junod,B.Revaz,E.Walker,G.Triscone,J.Muller,K.-Q.Wang,T.Tsukamoto	Bi,Sr,Ca,Cu,O	
7554	PHC1670598		Ca2CuO3	Ca2Cu1O3	Ca	2	Cu	1																	O	3			1990																																																																																																														1.63		516	specific heat																																									SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7555	PHC1670598		(Ca,Sr)CuO4	Ca0.86Sr0.14Cu1O4	Ca	0.86	Sr	0.14	Cu	1															O	4			1990																												IL																																																																																			gamma=zero	479	specific heat																																									SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7556	PHC1670598		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1990																												Bi2212																																																																																		1.74		246	specific heat																																									SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7557	PHC1670598			Bi1.6Pb0.4Sr1.6Ca2Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.6	Ca	2	Cu	3											O	z			1990																												Bi2223																																																																																		3.18		276	specific heat																																									SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7558	PHC1670598	Bi2223 phase>90%imprity=Bi2212, Ca2CuO3Ca2PbO4		Bi1.6Pb0.4Sr2Ca2.5Cu3.5Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.5	Cu	3.5											O	z			1990																												Bi2223																																																																																		8.41		284	specific heat																																				mixture-react(800+830C+840C,14H)-disc-SIN(859C,60H in aire)-cool to 700C(3C/min)-cool to 400C(1.5C/min)-ANN(2H in O2flow)					SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7559	PHC1670598	equal % of Bi2212,Bi2223 impurity=Ca2CuO3,Ca2PbO4		Bi1.6Pb0.4Sr2Ca2.5Cu3.5Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.5	Cu	3.5											O	z			1990																																																																																																														10.14		283	specific heat																																				mixture-react(800+830C+840C, 14H)-disc-SIN(855C,48H in air)-furnace cool in O2 flow					SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7560	PHC1670598	virtually single phase		Bi16Pb0.4Sr2Ca2.5Cu3.5Oz	Bi	16	Pb	0.4	Sr	2	Ca	2.5	Cu	3.5											O	z			1990																												Bi2223																																																																																			gamma=zero	274	specific heat																																				two step process					SPECIFIC HEAT OF THE HIGH-TC SUPERCONDUCTOR (BI,PB)2SR2CA2CU3O10, AND RELATED PHASES CA2CUO3 AND (CA0.86SR0.14)CUO2 FROM 0.4TO 20K			CSIRO DIVIDION OF APPLIED PHYSICS, LINDFIELD, 2070 AUSTRALIA	PHYSICA C,167(1990)598	R.DRIVER,S.J.COLLOCOTT	CA,CU,O,SR	
7561	PHC1560292		Bi2Sr2CaCu2O8	Bi2.1Sr2Ca1Cu2O8+z	Bi	2.1	Sr	2	Ca	1	Cu	2													O	8+z		1	1988																												Bi2212																			78	89					89																																																									4		260	specific heat																																			1	mixture-heat (790C,4H)-press to pellet-SIN(860C,5H in air)-Q to liq, N2					SPECIFIC HEATAND RESISTIVITY OF THE HIGH-TC SUPERCONDUCTOR BI2SR2CACU2O8+X FROM 0.4 TO 20K: EVIDENCE FOR A T-TERM				PHYSICA C,156(1988)292	ANDRIKIDIS.C,COLLOCOTT.S.J,DRIVER.R,PAVESE.F		
7562	PR03912267		Bi2Sr2CuO6	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O	6			1989																												Bi2201																						12.5			12.5										26																																															0.35		212	specific heat																																		Bi2O3,SrO2,(CaCO3),CuO	1	mixture-heat (950C)-slow cool to 700C-FC					Specific heat of Bi2Sr2CuO6 and Bi2Sr2CaCu2O8 in the superconducting state	6		Department of Physics, The Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B.,39(1989)12267	A. Chakraborty,A.J. Epstein,D.L. Cox,E.M. McCarron,W.E. Farneth		
7563	PR03912267		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1989																												Bi2212																						84			84										26																																															0.6		171	specific heat																																				mixture-heat(850C)					Specific heat of Bi2Sr2CuO6 and Bi2Sr2CaCu2O8 in the superconducting state	6		Department of Physics, The Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B.,39(1989)12267	A. Chakraborty,A.J. Epstein,D.L. Cox,E.M. McCarron,W.E. Farneth		
7564	PR05600802	Gruneizen parameter=0.79	Bi2Sr2CaCu2O8	Bi2Sr1.8Ca1.2Cu2O8	Bi	2	Sr	1.8	Ca	1.2	Cu	2													O	8		1	1997																												Bi2212																					79.5				79.5																																																											288	analyzing thermal expansion																																				See Phys.Rev.B 54(1996)R6885					Superconducting fluctuations in the thermal conductivity of Bi2Sr2CaCu2O8 and DyBa2Cu3O7-x materials	199707		SUPRAS, Institute of Physics B5, University of Lie'ge, B400-4000 Lie'ge, Belgium	Phys.Rev,B56(1997)802	H. Bougrine,M. Ausloos,M. Houssa,R. Cloots		
7565	PR05600802	Gruneizen parameter=2.35	DyBa2Cu3O7	Dy1Ba2Cu3O7-z	Dy	1	Ba	2	Cu	3															O	7-z			1997																												Y123																					83.8				83.8																																																											394	analyzing thermal expansion																																				magnetic field melt-texturing technique,all processes are under the magnetic field, ANN(400C, 1Day)					Superconducting fluctuations in the thermal conductivity of Bi2Sr2CaCu2O8 and DyBa2Cu3O7-x materials	199707		SUPRAS, Institute of Physics B5, University of Lie'ge, B400-4000 Lie'ge, Belgium	Phys.Rev,B56(1997)802	H. Bougrine,M. Ausloos,M. Houssa,R. Cloots		
7566	SSC1010617		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1997																											3	Bi2212																			63						63																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7567	SSC1010617		(Bi,Cd)2Sr2CaCu2O8	Bi1.9Cd0.1Sr2Ca1Cu2Oz	Bi	1.9	Cd	0.1	Sr	2	Ca	1	Cu	2											O	z		1	1997																											3	Bi2212																			60						60																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7568	SSC1010617		(Bi,Cd)2Sr2CaCu2O8	Bi1.8Cd0.2Sr2Ca1Cu2Oz	Bi	1.8	Cd	0.2	Sr	2	Ca	1	Cu	2											O	z		1	1997																											3	Bi2212																			58						58																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7569	SSC1010617		(Bi,Cd)2Sr2CaCu2O8	Bi1.7Cd0.3Sr2Ca1Cu2Oz	Bi	1.7	Cd	0.3	Sr	2	Ca	1	Cu	2											O	z		1	1997																											3	Bi2212																			53						53																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7570	SSC1010617	CdO,SrCuO2 phases detected by XRD	(Bi,Cd)2Sr2CaCu2O8	Bi1.5Cd0.5Sr2Ca1Cu2Oz	Bi	1.5	Cd	0.5	Sr	2	Ca	1	Cu	2											O	z			1997																											3	Bi2212																			45						45																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7571	SSC1010617	CdO,SrCuO2 phases detected by XRD	(Bi,Cd)2Sr2CaCu2O8	Bi1.4Cd0.6Sr2Ca1Cu2Oz	Bi	1.4	Cd	0.6	Sr	2	Ca	1	Cu	2											O	z			1997																											3	Bi2212																			34						34																																																																																															1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7572	SSC1010617	CdO,SrCuO2 phases detected by XRD	(Bi,Cd)2Sr2CaCu2O8	Bi1.2Cd0.2Sr2Ca1Cu2Oz	Bi	1.2	Cd	0.2	Sr	2	Ca	1	Cu	2											O	z			1997																											3	Bi2212																							10																																																																																																	1	See Jpm.J.Apple.Phys.34(1995)5592					STUDY OF NORMALISED RESISTANCE AND THERMOPOWER OF A HOLE DOPED Bi2-xCdxSr2CaCu2Oy (x=0.0-0.8) SUPERCONDUCTING SYSTEM			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Solid State Commun.101(1997)617-620	B.K. Chaudhuri,Souri Banerjee		
7573	SSC1010849		(Tl,Sn)2Ba2Cu(F,O)6	Tl1.9Sm0.1Ba2Cu1FOz	Tl	1.9	Sm	0.1	Ba	2	Cu	1	F												O	z		1	1997																											2	Tl2201	I4/mmm			3.867		23.22													97		100				98.5																																																																																																0.95Tl2O3+0.1SmO2+1.4BaO2+0.6BaF2+CuO,SIN(860C,30min)-FC					EFFECTS OF FLUORINE SUBSTTUTION IN SUPERCONDUCTING TlBa2CuO6+_ delta			Department of Physics,University of Kansas, Lawrence, Kansas 66045, USA	Solid State Commun.101(1997)849-853	D.F. Lu,G.F. Sun,John G. Stevens,K.W. Wong,Y. Xin,Yuchang Zhang		
7574	PR05605631		TbSr2(Cu,Mo)3O7	Tb1Sr2Cu2.69Mo0.31O7	Tb	1	Sr	2	Cu	2.69	Mo	0.31													O	7		1	1997						9.13	7.66	5.4																			3	Y123	Pmmm			3.827	3.825	11.553													32		37				34.5																																																																																														Tb4O7,SrCO3,MoO3,CuO	1	mixture-pellet-heat(1020C,3H in O2)-slow cool to RT in flowing O2					Superconductivity, magnetic fluctuations, and magnetic order in TbSr2Cu2,69Mo0.31O7	199709		Department of Physics, National Central University, Chung-Li, Taiwan 32054, Republic of China	Phys.Rev.B.,56(1997)5631	H.D. Yang,H.L. Tsay,J.W. Lynn,K.C. Lee,S.Y. Wu,W.-H. Li,W.Y. Chuang		
7575	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.06	Y	1	Ba	2	Cu	3															O	7-z	6.06	3	1997																												Y123																							10																																																																																																		self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7576	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.19	Y	1	Ba	2	Cu	3															O	7-z	6.19	3	1997																												Y123																							10																																																																																																		self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7577	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.25	Y	1	Ba	2	Cu	3															O	7-z	6.25	3	1997																												Y123																							10																																																																																																		self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7578	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.34	Y	1	Ba	2	Cu	3															O	7-z	6.34	3	1997																												Y123																							10																																																																																																		self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7579	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	7-z	6.68	3	1997																												Y123																				63					63																																																																																																self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7580	PR05605654	ab-plane THC by steady-state method	YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-z	6.93	3	1997																												Y123																				92					92																																																																																																self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7581	PR05605654	ab-plane THC by steady-state method	YBa2(Cu,Zn)Oz	Y1Ba2Cu2.97Zn0.03O6.93	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	z	6.93	3	1997																												Y123																				80					80																																																																																																self flux method-annealed with 10g polycrystal(same z) in sealed quortz tube (600C,12H)					In-plane thermal conductivity and Lorenz number in YBa2Cu3O7-y	199709		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113, Japan	Phys.Rev.B.,56(1997)5654	H. Asaoka,H. Takei,K. Mizuhashi,K. Takenaka,S. Uchida,Y. Fukuzumi		
7582	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.214	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.214	3	1997																												Bi2212																				70					70																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7583	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.216	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.216	3	1997																												Bi2212																				78					78																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7584	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.22	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.22	3	1997																												Bi2212																				82					82																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7585	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.23	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.23	3	1997																												Bi2212																				86					86																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7586	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.24	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.24	3	1997																												Bi2212																				88					88																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7587	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.25	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.25	3	1997																												Bi2212																				89					89																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7588	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.26	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.26	3	1997																												Bi2212																				86					86																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7589	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.27	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.27	3	1997																												Bi2212																				84					84																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7590	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.28	3	1997																												Bi2212																				81					81																																																																																																crystals were grown by the traveling solvent floating zone method under mixed gas flow(20%O2+80%Ar).					Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
7591	PR05605512		Nd(Ba,Nd)2Cu3O7	Nd1.05Ba1.95Cu3O7+z	Nd	1.05	Ba	1.95	Cu	3															O	7+z			1997																												Y123																						91.9			91.9																																																																																															1						Soppression of superconductivity in the R(ba1-zRz)2Cu3O7+delta (R=Pr,Nd) system	199709		Ames Laboratory, U.S. Department of Enargy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,56(1997)5512	D. Falzgraf,K.W. Dennis,M.J. Kramer,R.W. McCallum,S.K. Malik,W.B. Yelon		
7592	PR05605512		Nd(Ba,Nd)2Cu3O7	Nd1.15Ba1.85Cu3O7+z	Nd	1.15	Ba	1.85	Cu	3															O	7+z			1997																												Y123																						67.1			67.1																																																																																															1						Soppression of superconductivity in the R(ba1-zRz)2Cu3O7+delta (R=Pr,Nd) system	199709		Ames Laboratory, U.S. Department of Enargy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,56(1997)5512	D. Falzgraf,K.W. Dennis,M.J. Kramer,R.W. McCallum,S.K. Malik,W.B. Yelon		
7593	PR05605512		Nd(Ba,Nd)2Cu3O7	Nd1.25Ba1.75Cu3O7+z	Nd	1.25	Ba	1.75	Cu	3															O	7+z			1997																												Y123																						43.8			43.8																																																																																															1						Soppression of superconductivity in the R(ba1-zRz)2Cu3O7+delta (R=Pr,Nd) system	199709		Ames Laboratory, U.S. Department of Enargy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,56(1997)5512	D. Falzgraf,K.W. Dennis,M.J. Kramer,R.W. McCallum,S.K. Malik,W.B. Yelon		
7594	PR05605512		Nd(Ba,Nd)2Cu3O7	Nd1.3Ba1.7Cu3O7+z	Nd	1.3	Ba	1.7	Cu	3															O	7+z			1997																												Y123																						33.8			33.8																																																																																															1						Soppression of superconductivity in the R(ba1-zRz)2Cu3O7+delta (R=Pr,Nd) system	199709		Ames Laboratory, U.S. Department of Enargy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,56(1997)5512	D. Falzgraf,K.W. Dennis,M.J. Kramer,R.W. McCallum,S.K. Malik,W.B. Yelon		
7595	PR05605512		Nd(Ba,Nd)2Cu3O7	Nd1.4Ba1.6Cu3O7+z	Nd	1.4	Ba	1.6	Cu	3															O	7+z			1997																												Y123																						7.9			7.9																																																																																															1						Soppression of superconductivity in the R(ba1-zRz)2Cu3O7+delta (R=Pr,Nd) system	199709		Ames Laboratory, U.S. Department of Enargy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,56(1997)5512	D. Falzgraf,K.W. Dennis,M.J. Kramer,R.W. McCallum,S.K. Malik,W.B. Yelon		
7601	PR05602824	RESRT at 275K	NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		1	1997																											3	Y123				3.862	3.912	11.748												K		93.4				1.1	93.4																																																																							mOhm.cm											1.092												Nd2O3,BaCO3,CuO,ThO2,CaCO3	1	Pellet-CAL(three times at 900,920,920C)-ANN(460C, 3 days in flowing O2)-cool to RT(12C/H)					Neutron-diffraction studies and bond valence sums of charge neutrally doped Nd1-2xCaxThxBa2Cu3O7-delta	199708		Solid State Physics, the Royal Institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,56(1997)2824	I. Bryntse,O. Rapp,P. Landqvist,R. Tellgren		
7602	PR05602824	RESRT is at 275K 	(Nd,Ca,Th)Ba2Cu3O7	Nd0.97Ca0.015Th0.015Ba2Cu3O7-z	Nd	0.97	Ca	0.015	Th	0.015	Ba	2	Cu	3											O	7-z		1	1997																											3	Y123				3.864	3.911	11.741												K		90.4				1.4	90.4																																																																							mOhm.cm											1.25												Nd2O3,BaCO3,CuO,ThO2,CaCO3	1	Pellet-CAL(three times at 900,920,920C)-ANN(460C, 3 days in flowing O2)-cool to RT(12C/H)					Neutron-diffraction studies and bond valence sums of charge neutrally doped Nd1-2xCaxThxBa2Cu3O7-delta	199708		Solid State Physics, the Royal Institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,56(1997)2824	I. Bryntse,O. Rapp,P. Landqvist,R. Tellgren		
7603	PR05602824	RESRT is at 275 K 	(Nd,Ca,Th)Ba2Cu3O7	Nd0.94Ca0.03Th0.03Ba2Cu3O7-z	Nd	0.94	Ca	0.03	Th	0.03	Ba	2	Cu	3											O	7-z		1	1997																											3	Y123				3.867	3.912	11.736												K		86.8				2.6	86.8																																																																							mOhm.cm											1.32												Nd2O3,BaCO3,CuO,ThO2,CaCO3	1	Pellet-CAL(three times at 900,920,920C)-ANN(460C, 3 days in flowing O2)-cool to RT(12C/H)					Neutron-diffraction studies and bond valence sums of charge neutrally doped Nd1-2xCaxThxBa2Cu3O7-delta	199708		Solid State Physics, the Royal Institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,56(1997)2824	I. Bryntse,O. Rapp,P. Landqvist,R. Tellgren		
7604	PR05602824	RESRT is at 275 K 	(Nd,Ca,Th)Ba2Cu3O7	Nd0.9Ca0.05Th0.05Ba2Cu3O7-z	Nd	0.9	Ca	0.05	Th	0.05	Ba	2	Cu	3											O	7-z		1	1997																											3	Y123				3.868	3.91	11.73												K		81.8				6.2	81.8																																																																							mOhm.cm											1.69												Nd2O3,BaCO3,CuO,ThO2,CaCO3	1	Pellet-CAL(three times at 900,920,920C)-ANN(460C, 3 days in flowing O2)-cool to RT(12C/H)					Neutron-diffraction studies and bond valence sums of charge neutrally doped Nd1-2xCaxThxBa2Cu3O7-delta	199708		Solid State Physics, the Royal Institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,56(1997)2824	I. Bryntse,O. Rapp,P. Landqvist,R. Tellgren		
7605	PR05602824	RESRT is at 275 K 	(Nd,Ca,Th)Ba2Cu3O7	Nd0.8Ca0.1Th0.1Ba2Cu3O7-z	Nd	0.8	Ca	0.1	Th	0.1	Ba	2	Cu	3											O	7-z		1	1997																											3	Y123				3.868	3.91	11.732												K		73.4				9.8	73.4																																																																							mOhm.cm											2.02												Nd2O3,BaCO3,CuO,ThO2,CaCO3	1	Pellet-CAL(three times at 900,920,920C)-ANN(460C, 3 days in flowing O2)-cool to RT(12C/H)					Neutron-diffraction studies and bond valence sums of charge neutrally doped Nd1-2xCaxThxBa2Cu3O7-delta	199708		Solid State Physics, the Royal Institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,56(1997)2824	I. Bryntse,O. Rapp,P. Landqvist,R. Tellgren		
7606	PR05602383	Nominal conposition	(Bi,Pb)Sr2Ca3(Cu,Si)4O12	Bi1.6Pb0.4Sr2Ca3Cu4O12-z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	4											O	12-z		1	1997																												Bi2223																				110					110																																																																																														Bi2O3,PbO,SrCO3,CaCO3,CuO,Si	1	mixture-CAL(800C,20H)-pellet-SIN(850C,140H in air)-FC to RT					Electron-phonon contribution to thermopower in Si-doped superconducting Bi Compounds	199708		Departamento de F'isica, Universidad Nacional de Colobia, A.A. 67904, Santafe' de Bogota', Colombia	Phys.Rev.B,56(1997)2383	A. Marino,J. Giraldo,J.E. Rodri'guez		
7607	PR05602383	Nominal conposition	(Bi,Pb)Sr2Ca3(Cu,Si)4O12	Bi1.6Pb0.4Sr2Ca3Cu3.92Si0.08O12-z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.92	Si	0.08									O	12-z		1	1997																												Bi2223																				110					110																																																																																														Bi2O3,PbO,SrCO3,CaCO3,CuO,Si	1	mixture-CAL(800C,20H)-pellet-SIN(850C,140H in air)-FC to RT					Electron-phonon contribution to thermopower in Si-doped superconducting Bi Compounds	199708		Departamento de F'isica, Universidad Nacional de Colobia, A.A. 67904, Santafe' de Bogota', Colombia	Phys.Rev.B,56(1997)2383	A. Marino,J. Giraldo,J.E. Rodri'guez		
7608	PR05602383	Nominal conposition	(Bi,Pb)Sr2Ca3(Cu,Si)4O12	Bi1.6Pb0.4Sr2Ca3Cu3.88Si0.12O12-z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.88	Si	0.12									O	12-z		1	1997																												Bi2223																				110					110																																																																																														Bi2O3,PbO,SrCO3,CaCO3,CuO,Si	1	mixture-CAL(800C,20H)-pellet-SIN(850C,140H in air)-FC to RT					Electron-phonon contribution to thermopower in Si-doped superconducting Bi Compounds	199708		Departamento de F'isica, Universidad Nacional de Colobia, A.A. 67904, Santafe' de Bogota', Colombia	Phys.Rev.B,56(1997)2383	A. Marino,J. Giraldo,J.E. Rodri'guez		
7609	PR05602383	2212+2223 phase and SiO2	(Bi,Pb)Sr2Ca3(Cu,Si)4O12	Bi1.6Pb0.4Sr2Ca3Cu3.86Si0.14O12-z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.86	Si	0.14									O	12-z		2	1997																																																110					110																																																																																														Bi2O3,PbO,SrCO3,CaCO3,CuO,Si	1	mixture-CAL(800C,20H)-pellet-SIN(850C,140H in air)-FC to RT					Electron-phonon contribution to thermopower in Si-doped superconducting Bi Compounds	199708		Departamento de F'isica, Universidad Nacional de Colobia, A.A. 67904, Santafe' de Bogota', Colombia	Phys.Rev.B,56(1997)2383	A. Marino,J. Giraldo,J.E. Rodri'guez		
7610	PR05602383	Nominal conposition	(Bi,Pb)Sr2Ca3(Cu,Si)4O12	Bi1.6Pb0.4Sr2Ca3Cu3.5Si0.5O12-z	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.5	Si	0.5									O	12-z		1	1997																												Bi2223																				110					110																																																																																														Bi2O3,PbO,SrCO3,CaCO3,CuO,Si	1	mixture-CAL(800C,20H)-pellet-SIN(850C,140H in air)-FC to RT					Electron-phonon contribution to thermopower in Si-doped superconducting Bi Compounds	199708		Departamento de F'isica, Universidad Nacional de Colobia, A.A. 67904, Santafe' de Bogota', Colombia	Phys.Rev.B,56(1997)2383	A. Marino,J. Giraldo,J.E. Rodri'guez		
7611	PR05605144		(Eu,,Ce)2Sr2Cu2NbO10	Eu1.5Ce0.5Sr2Cu2Nb1O9.955	Eu	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-z	9.955		1997																												RSCNO																				21					21																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7612	PR05605144		(Eu,Pr,Ce)2Sr2Cu2NbO10	Eu1.45Pr0.05Ce0.5Sr2Cu2Nb1O10=z	Eu	1.45	Pr	0.05	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10=z			1997																												RSCNO																				21.4					21.4																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7613	PR05605144		(Eu,Pr,Ce)2Sr2Cu2NbO10	Eu1.4Pr0.1Ce0.5Sr2Cu2Nb1O10-z	Eu	1.4	Pr	0.1	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				18.4					18.4																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7614	PR05605144		(Eu,Pr,Ce)2SrCu2NbO10	Eu1.35Pr0.15Ce0.5Sr2Cu2Nb1O10-z	Eu	1.35	Pr	0.15	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				18					18																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7615	PR05605144		(Eu,Pr,Ce)2Sr2Cu2NbO10	Eu1.3Pr0.2Ce0.5Sr2Cu2Nb1O10-z	Eu	1.3	Pr	0.2	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				13.4					13.4																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7616	PR05605144		(Eu,Pr,Ce)2Sr2Cu2NbO10	Eu1.25Pr0.25Ce0.5Sr2Cu2Nb1O10-z	Eu	1.25	Pr	0.25	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				7.8					7.8																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7617	PR05605144		(Eu,Pr,Ce)2Sr2Cu2NbO10	Eu1.23Pr0.27Ce0.5Sr2Cu2Nb1O10-z	Eu	1.23	Pr	0.27	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				2.9					2.9																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7618	PR05605144		(Nd,Ce)2Sr2Cu2O10	Nd1.5Ce0.5Sr2Cu2Nb1O10-z	Nd	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-z			1997																												RSCNO																				24					24																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7619	PR05605144		(Nd,Pr,Ce)2Sr2Cu2NbO10	Nd1Pr0.5Ce0.5Sr2Cu2Nb1O10-z	Nd	1	Pr	0.5	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				20.5					20.5																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7620	PR05605144		(Nd,Pr,Ce)2Sr2Cu2NbO10	Nd1.4Pr0.1Ce0.5Sr2Cu2Nb1O10-z	Nd	1.4	Pr	0.1	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				17.2					17.2																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7621	PR05605144		(Nd,Pr,Ce)2Sr2NbO10	Nd1.35Pr0.15Ce0.5Sr2Cu2Nb1O10-z	Nd	1.35	Pr	0.15	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				11.3					11.3																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7622	PR05605144		(Nd,Pr,Ce)2sr2Cu2NdO10	Nd1.3Pr0.2Ce0.5Sr2Cu2Nb1O10-z	Nd	1.3	Pr	0.2	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				4.4					4.4																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7623	PR05605144		(Sm,Ce)2Sr2Cu2NbO10	Sm1.5Ce0.5Sr2Cu2Nb1O10-z	Sm	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-z			1997																												RSCNO																				26					26																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7624	PR05605144		(Sm,Pr,Ce)2SrCu2NbO10	Sm1.45Pr0.05Ce0.5Sr2Cu2Nb1O10-z	Sm	1.45	Pr	0.05	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				25.2					25.2																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7625	PR05605144		(Sm,Pr,Ce)2Sr2Cu2NbO10	Sm1.4Pr0.1Ce0.5Sr2Cu2Nb1O10-z	Sm	1.4	Pr	0.1	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				22.8					22.8																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7626	PR05605144		(Sm,Pr,Ce)2Sr2Cu2O10	Sm0.35Pr0.15Ce0.5Sr2Cu2Nb1O10-z	Sm	0.35	Pr	0.15	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				17.6					17.6																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7627	PR05605144		(Sm,Pr,Ce)2Sr2Cu2NbO10	Sm1.3Pr0.2Ce0.5Sr2Cu2Nb1O10-z	Sm	1.3	Pr	0.2	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				12.8					12.8																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7628	PR05605144		(Sm,Pr,Ce)2Sr2Cu2NbO10	Sm1.25Pr0.25Ce0.5Sr2Cu2Nb1O10-z	Sm	1.25	Pr	0.25	Ce	0.5	Sr	2	Cu	2	Nb	1									O	10-z			1997																												RSCNO																				2.7					2.7																																																																																																See Phys.Rev.B,55(1997)3297					Superconductivity and magnetism in (R1.5-xPrxCe0.5)Sr2Cu2NdO10-delta(R=Nd,Sm,Eu): Criteria for modeling the suppression of superconductivity by Pr in high-Tc cuprates	199709		Department Physics, University of California, Davis, Davis, California 95616	Phys.Rev.B,56(1997)5144	H.B. Radousky,R.N. Shelton,T.J. Goodwin		
7629	PR05412535	G-L parameter=76. Anisotropy factor=12.3 by effective mass. 	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1996																												Y124																						78.8		3	78.8																				T	torque. WHH theory 			90			3.5	76.8	T/K				1.86						19			anisotropie 3D London model for torque data.		1430																																																				crystal was grown in Y2O3 crucible using high-pressure technique					Angle-dependent reversible magnetic torque in singl-crystalline Y2Ba4Cu8O16	199611		"Physik-Institut, University of Zu""rich,Winterthurerstasse 190,8057 Zu""rich, Swizerland"	Phys.Rev.B,54(1996)12535	C. Rossel,D. Zech,H. Keller,J. Karpinski,L. Lesne,S.L. Lee		
7630	PR05403610	C-axis oriented film as-prepared	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4+z	Nd	1.85	Ce	0.15	Cu	1															O	4+z			1996																												T'																				22					22																					analysis of fluctuation coductivity	8									0.37								64																																																									by pulsed laser deposition in N2O					Magnetoresistivity of thin films of the electron-doped high-Tc superconductor Nd1.85Ce0.15 CuO4+_ z	199608		Department of Phsics and Institute for pure and Applisd Physical Sciences, University of California, San Diego,La Jolla, California 92093-0360	Phys.Rev.B,54(1996)3610	C.C. Almasan,J. Herrmann,M.B. Maple,M.C. de Andrade,R.P. Dikey		
7631	PHC2890280		(Lu,Ca)Ba2Cu3O7	Lu0.9Ca0.1Ba2Cu3O6+z	Lu	0.9	Ca	0.1	Ba	2	Cu	3													O	6+z			1997																												Y123																					18				18																																																																																														Lu2o3,CaCO3,BaCO3,CuO	1	mixture-CAL(900C,48H)-grind-fire(905C,24H+910C,24H)-pellet-SIN(905C,48H)-ANN(920C,24H in Ar flow)-cool to 450C(1C/min)-ANN(12H)-cool to RT(1C/min)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7632	PHC2890280		(La,Ca)Ba2Cu3O7	Lu0.8Ca0.2Ba2Cu3O6.13	Lu	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.13		1997																											2	Y123				3.851		11.778															41			2	41																																																																																														Lu2o3,CaCO3,BaCO3,CuO	1	mixture-CAL(900C,48H)-grind-fire(905C,24H+910C,24H)-pellet-SIN(905C,48H)-ANN(920C,24H in Ar flow)-cool to 450C(1C/min)-ANN(12H)-cool to RT(1C/min)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7633	PHC2890280		(Lu,Ca)Ba2Cu3O7	Lu0.7Ca0.3Ba2Cu3O6.15	Lu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.15		1997																											2	Y123	P4/mmm			3.829		11.728															58			2	58																																																																																														Lu2o3,CaCO3,BaCO3,CuO	1	mixture-CAL(900C,48H)-grind-fire(905C,24H+910C,24H)-pellet-SIN(905C,48H)-ANN(920C,24H in Ar flow)-cool to 450C(1C/min)-ANN(12H)-cool to RT(1C/min)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7634	PHC2890280		(Lu,Ca)Ba2Cu3O7	Lu0.6Ca0.4Ba2Cu3O6+z	Lu	0.6	Ca	0.4	Ba	2	Cu	3													O	6+z			1997																												Y123																					74				74																																																																																														Lu2o3,CaCO3,BaCO3,CuO	1	mixture-CAL(900C,48H)-grind-fire(905C,24H+910C,24H)-pellet-SIN(905C,48H)-ANN(920C,24H in Ar flow)-cool to 450C(1C/min)-ANN(12H)-cool to RT(1C/min)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7635	PHC2890280			Lu0.8Ca0.2Ba2Cu3O6.54	Lu	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.54		1997																												Y123																					65				65																																																																																																ANN(920C,24H in air)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7636	PHC2890280			Lu0.7Ca0.3Ba2Cu3O6.4	Lu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.4		1997																											2	Y123				3.852		11.774															68				68																																																																																																ANN(920C,24H in air)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7637	PHC2890280			Lu0.8Ca0.2Ba2Cu3O6.81	Lu	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.81		1997																											3	Y123				3.883	3.815	11.66															52				52																																																																																																ANN(400C,4H in O2)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7638	PHC2890280			Lu0.7Ca0.3Ba2Cu3O6.78	Lu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.78		1997																											3	Y123				3.875	3.814	11.661															54				54																																																																																																ANN(400C,4H in O2)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7639	PHC2890280			Lu0.8Ca0.2Ba2Cu3O6.68	Lu	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.68		1997																												Y123																					78			2	78																																																																																																ANN(920C,24H in air)-Q to RT					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7640	PHC2890280			Lu0.7Ca0.3Ba2Cu3O6.62	Lu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.62		1997																											3	Y123				3.877	3.817	11.707															80			2	80																																																																																																ANN(920C,24H in air)-Q to RT					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7641	PHC2890280			Lu0.8Ca0.2Ba2Cu3O6.91	Lu	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.91		1997																											3	Y123				3.882	3.81	11.665															48				48																																																																																																ANN(920C,24H in O2)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7642	PHC2890280			Lu0.7Ca0.3Ba2Cu3O6.88	Lu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.88		1997																											3	Y123	Pmmm			3.806	3.861	11.654															45				45																																																																																																ANN(920C,24H in O2)					Superconductivity in Lu1-xCaxBa2Cu3O6+delta: holes generated by Ca	199710		Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai400 005, India	Physica.C,289(1997)280-290	A. Sequiera,K.I. Gnanasekar,L.C. Gupta,R. Pinto,Rajni Sharma		
7643	JP00900901		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.7Co0.3Oz	Eu	1	Ba	2	Cu	2.7	Co	0.3													O	z		1	1997																												Y123																			30		36				33																																																																																															1	Standard Solid State recetion					The insulating-to-superconducting transition in europium high-temperature superconducting ceramics			Tel Aviv University, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Ramat Aviv 69978, Israel	J.Phys.:Cond.Matter 9(1997)901-912	Jan Genossar,Ralph Rosenbaum		
7644	JP00900901		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.65Co0.35Oz	Eu	1	Ba	2	Cu	2.65	Co	0.35													O	z		1	1997																												Y123																			4.2		15				9.6																																																																																															1	Standard Solid State recetion					The insulating-to-superconducting transition in europium high-temperature superconducting ceramics			Tel Aviv University, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Ramat Aviv 69978, Israel	J.Phys.:Cond.Matter 9(1997)901-912	Jan Genossar,Ralph Rosenbaum		
7645	JP00900901		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.6Co0.4Oz	Eu	1	Ba	2	Cu	2.6	Co	0.4													O	z		1	1997																												Y123																							15																																																																																																	1	Standard Solid State recetion					The insulating-to-superconducting transition in europium high-temperature superconducting ceramics			Tel Aviv University, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Ramat Aviv 69978, Israel	J.Phys.:Cond.Matter 9(1997)901-912	Jan Genossar,Ralph Rosenbaum		
7646	JP00900901		EuBa2(Cu,Co)3O7	Eu1Ba2Cu2.5Co0.5Oz	Eu	1	Ba	2	Cu	2.5	Co	0.5													O	z		1	1997																												Y123																							15																																																																																																	1	Standard Solid State recetion					The insulating-to-superconducting transition in europium high-temperature superconducting ceramics			Tel Aviv University, School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Ramat Aviv 69978, Israel	J.Phys.:Cond.Matter 9(1997)901-912	Jan Genossar,Ralph Rosenbaum		
7647	SSC0761261		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2Oz	Tl	1	Sr	2	Ca	1	Cu	2													O	z			1990																												Tl1212																																																																																																											7.15														mixrure-pellet-wrapped in Au foil-SIN(950C,3H in flowing Oz)-cool to RT(5C/min)					SUPERCONDUCTIVITY UP TO 105K IN THE NEW HIGH-TC TL-V-SR-CA-CU-O AND TL-V-SR-CA-Y-CU-O SYSTEMS	199012		IRC IN SUPERCONDUCTIVITY, UNIVERSITY OF CAMBRIDGE, MADINGLEY ROAD, CAMBRIDGE CB3 0HE, U.K.	SOLID STATE COMMUN.,76(1990)1261	P.P.EDWARDS,R.JANES,R.S.LIU,W.ZHOU	TL,V,SR,CA,CU,O,Y	
7648	SSC0761261		(Tl,V)Sr2CaCu2Oz	Tl0.5V0.5Sr2Ca1Cu2Oz	Tl	0.5	V	0.5	Sr	2	Ca	1	Cu	2											O	z			1990																												Tl1212				3.801		12.017													57		110				83.5																																																																																		3.2														mixrure-pellet-wrapped in Au foil-SIN(950C,3H in flowing Oz)-cool to RT(5C/min)					SUPERCONDUCTIVITY UP TO 105K IN THE NEW HIGH-TC TL-V-SR-CA-CU-O AND TL-V-SR-CA-Y-CU-O SYSTEMS	199012		IRC IN SUPERCONDUCTIVITY, UNIVERSITY OF CAMBRIDGE, MADINGLEY ROAD, CAMBRIDGE CB3 0HE, U.K.	SOLID STATE COMMUN.,76(1990)1261	P.P.EDWARDS,R.JANES,R.S.LIU,W.ZHOU	TL,V,SR,CA,CU,O,Y	
7649	SSC0761261		(Tl,V)Sr2(Ca,Y)Cu2Oz	Tl0.5V0.5Sr2Ca0.8Y0.2Cu2Oz	Tl	0.5	V	0.5	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	z			1990																												Tl1212																			87	100	110				100																																																																																		17.4														mixrure-pellet-wrapped in Au foil-SIN(950C,3H in flowing Oz)-cool to RT(5C/min)					SUPERCONDUCTIVITY UP TO 105K IN THE NEW HIGH-TC TL-V-SR-CA-CU-O AND TL-V-SR-CA-Y-CU-O SYSTEMS	199012		IRC IN SUPERCONDUCTIVITY, UNIVERSITY OF CAMBRIDGE, MADINGLEY ROAD, CAMBRIDGE CB3 0HE, U.K.	SOLID STATE COMMUN.,76(1990)1261	P.P.EDWARDS,R.JANES,R.S.LIU,W.ZHOU	TL,V,SR,CA,CU,O,Y	
7650	JSC1320073		Nd2Ba4Cu7O14	Nd2Ba4Cu7O14.525	Nd	2	Ba	4	Cu	7															O	14+z	14.525	1	1997																											3	Y247				3.893	3.901	50.68																66			66																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7651	JSC1320073		(Nd,Pr)2Ba4Cu7O14	Nd1.8Pr0.2Ba4Cu7O14.587	Nd	1.8	Pr	0.2	Ba	4	Cu	7													O	14+z	14.587	1	1997																											3	Y247				3.896	3.904	50.709																56			56																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7652	JSC1320073		(Nd,Pr)2Ba4Cu7O14	Nd1.6Pr0.4Ba4Cu7O14.603	Nd	1.6	Pr	0.4	Ba	4	Cu	7													O	14+z	14.603	1	1997																											3	Y247				3.9	3.907	50.749																48			48																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7653	JSC1320073		(Nd,Pr)2Ba4Cu7O14	Nd1.4Pr0.6Ba4Cu7O14.541	Nd	1.4	Pr	0.6	Ba	4	Cu	7													O	14+z	14.541	1	1997																											3	Y247				3.902	3.908	50.77																41			41																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7654	JSC1320073		Eu2Ba4Cu7O14	Eu2Ba4Cu7O14.671	Eu	2	Ba	4	Cu	7															O	14+z	14.671	1	1997																											3	Y247				3.864	3.897	50.571																75			75																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7655	JSC1320073		(Eu,Pr)2Ba4Cu7O14	Eu1.8Pr0.2Ba4Cu7O14.779	Eu	1.8	Pr	0.2	Ba	4	Cu	7													O	14+z	14.779	1	1997																											3	Y247				3.868	3.896	50.608																68			68																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7656	JSC1320073		(Eu,Pr)2Ba4Cu7O14	Eu1.6Pr0.4Ba4Cu7O14.761	Eu	1.6	Pr	0.4	Ba	4	Cu	7													O	14+z	14.761	1	1997																											3	Y247				3.868	3.892	50.646																63			63																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7657	JSC1320073		(Eu,Pr)2Ba4Cu7O14	Eu1.4Pr0.6Ba4Cu7O14.632	Eu	1.4	Pr	0.6	Ba	4	Cu	7													O	14+z	14.632	1	1997																											3	Y247				3.869	3.891	50.677																58			58																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7658	JSC1320073		(Eu,Pr)2Ba4Cu7O14	Eu1.2Pr0.8Ba4Cu7O14.788	Eu	1.2	Pr	0.8	Ba	4	Cu	7													O	14+z	14.788	1	1997																											3	Y247				3.871	3.89	50.699																52			52																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7659	JSC1320073		Tm2Ba4Cu7O14	Tm2Ba4Cu7O14.732	Tm	2	Ba	4	Cu	7															O	14+z	14.732	1	1997																											3	Y247				3.835	3.879	50.419																88			88																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7660	JSC1320073		(Tm,Pr)2Ba4Cu7O14	Tm1.8Pr0.2Ba4Cu7O14.725	Tm	1.8	Pr	0.2	Ba	4	Cu	7													O	14+z	14.725	1	1997																											3	Y247				3.837	3.881	50.471																76			76																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7661	JSC1320073		(Tm,Pr)2Ba4Cu7O14	Tm1.6Pr0.4Ba4Cu7O14.722	Tm	1.6	Pr	0.4	Ba	4	Cu	7													O	14+z	14.722	1	1997																											3	Y247				3.849	3.883	50.498																68			68																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7662	JSC1320073		(Tm,Pr)2Ba4Cu7O14	Tm1.4Pr0.6Ba4Cu7O14.667	Tm	1.4	Pr	0.6	Ba	4	Cu	7													O	14+z	14.667	1	1997																											3	Y247				3.853	3.886	50.53																60			60																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7663	JSC1320073		(Tm,Pr)2Ba4Cu7O14	Tm1.2Pr0.8Ba4Cu7O14.652	Tm	1.2	Pr	0.8	Ba	4	Cu	7													O	14+z	14.652	1	1997																											3	Y247				3.856	3.887	50.567																50			50																																																																																														R2O3,Ba(NO3)2,CuO,Pr6O11		mixture-Al2O3 cricible-heat(900-920C, in O2 flow)-Q to RT-wrapped in Aufoil-heat(980-990 C,24H in 25bar O2)-ANN(300-320C,30H in 120-130 bar O2)					The High-Pressure Synthesis and Characterization of Some Praseodymium-Substituted Rare-Earth-Based R2Ba4Cu7O14+delta (R=Nd,Eu,Tm)			Department of Applied Chemistry, National Chiao-Tung University, Hsinchu 300, Taiwan, Republic of China	J.Solid State Chem.132(1997)73-77	F.S. Kao,Teng-Ming Chen		
7664	JP00901105	optimum(845C,240H in O2)	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O1	Bi	2	Sr	2	Ca	2	Cu	3													O	10+z	1	1	1997																											2	Bi2223				5.393		37.112													108	114		114		6	114																																																		138000																																												Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7665	JP00901105	optimum(850C,80H in O2)	(Bi,V)2Sr2Ca2Cu3O10	Bi1.8V0.2Sr2Ca2Cu3O2	Bi	1.8	V	0.2	Sr	2	Ca	2	Cu	3											O	10+z	2	2	1997																											2	Bi2223				5.413		30.701													92	112				20	112																																																		111000																																												Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7666	JP00901105	optimum(850C,70H in O2)	(Bi,V)2Sr2Ca2Cu3O10	Bi1.6V0.4Sr2Ca2Cu3O10+z	Bi	1.6	V	0.4	Sr	2	Ca	2	Cu	3											O	10+z		2	1997																											2	Bi2223				5.446		30.018													83	92				9	92																																																		97000																																												Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7667	JP00901105	optimum(845C,,60H in O2)	(Bi,V)2Sr2Ca2Cu3O10	Bi1.4V0.6Sr2Ca2Cu3O10+z	Bi	1.4	V	0.6	Sr	2	Ca	2	Cu	3											O	10+z		2	1997																											3	Bi2223				5.99	5.476	29.871													67	67				11	67																																																		71000																																												Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7668	JP00901105	optimum(840C,55H in O2)	(Bi,V)2Sr2Ca2Cu3O10	Bi1.2V0.8Sr2Ca2Cu3O10+z	Bi	1.2	V	0.8	Sr	2	Ca	2	Cu	3											O	10+z		2	1997																											3	Bi2223				6.215	5.49	28.437													30	30				30	30																																																		34000																																												Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7669	JP00901105	optimum(840C,40H in O2)	(Bi,V)2Sr2Ca2Cu3O10	Bi1V1Sr2Ca2Cu3O10+z	Bi	1	V	1	Sr	2	Ca	2	Cu	3											O	10+z		2	1997																											3	Bi2223				6.219	5.495	28.432														15					15																																																																																														Bi2O3,V2O5,SrCO3,CaCO3,CuO	1	two step reaction, precursor(Bi-Sr-Ca-Cu-O) mixed with V2O5-pellet-sealed in evacuated quartz ampoule-SIN( )-ANN(600C in air)					A structural transformation and its effect on the physical properties of the V-substituted Bi2Sr2Ca2Cu3O10+y system			Inonu Universitesi, Fen Edebiyat Fakultesi, Fizik Bolumu, 44069 Malatya, Turkey	J.Phys.:Cond.Matter 9(1997)1105-1121	M E Yakinci		
7670	JSC1300319		Sr2Cu2MnO2S2	Sr2Cu2Mn1S2O2	Sr	2	Cu	2	Mn	1	S	2													O	2			1997						5.3	-28	29.5																			2		I4/mmm			4.002		17.131																																																																																																																	SrS,Mn(Zn),CuO	1	mixture-pellet-sealed in evacuated quartz tube-heat (920C,24H)-FC to RT					Unusual Layered Transition-Metal Oxysulfides: Sr2Cu2MO2S2 (M=Mn,Zn)			Department of Physics and Texas Center for Superconductivity, University of Houston, Texas 77204-5932	J.Solid State Chem.130(1997)319-321	P.H. Hor,W.J. Zhu		
7671	JSC1300319		Sr2Cu2ZnO2S2	Sr2Cu2Zn1S2O2	Sr	2	Cu	2	Zn	1	S	2													O	2			1997																											2		I4/mmm			4.008		17.72																																																																																																																	SrS,Mn(Zn),CuO	1	mixture-pellet-sealed in evacuated quartz tube-heat (920C,24H)-FC to RT					Unusual Layered Transition-Metal Oxysulfides: Sr2Cu2MO2S2 (M=Mn,Zn)			Department of Physics and Texas Center for Superconductivity, University of Houston, Texas 77204-5932	J.Solid State Chem.130(1997)319-321	P.H. Hor,W.J. Zhu		
7672	JSC1300154	impurity phase=Sr2CuTa2Oz, insulator	Pb2Sr2Cu2TaO8Cl	Pb2Sr2Cu2Ta1Cl1O8	Pb	2	Sr	2	Cu	2	Ta	1	Cl	1											O	8			1997																													P4/mmm			3.892		15.383																																																																																																																	PbO,PbCl2,Sr(NO3)2,TaO5,CuO		nixture-heat (500+550+600+650C in air for 12H each with intermittent grindings)-pellet-SIN(700C, 24H in air)-FC to RT					Pb2Sr2Cu2TaO8Cl, a new Layered Cuprate with HematoPhanite Structure			Department of Applied Chemistry, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Solid State Chem.130(1997)154-156	Li Rukang		
7673	JSC1290360	insulator	Ba4CuLiO4Cl4	Ba4Cu1Li1Cl4O4	Ba	4	Cu	1	Li	1	Cl	4													O	4			1997																											2	T	I4/mmm			4.156		16.125																																																																																																																		1	The reactions were carried out in a flowing, CO2 free, O2 at 700-800C, for 24H-FC to RT					New Cu(III) Oxychlorides in the Ba-Cu-M-O-Cl (M=Li,Na) System			CNR, Institute of Structural Chemistry, University of Parma, Italy	J.Solid State Chem.129(1997)360-362	F.C. Matacotta,G. Bocelli,G. Calestani,K.A. Thomas,K.V. Ramanujachary,M. Greenblatt		
7674	JSC1290360	sharp transition in susceptibility was observed around 250C insulator	Ba4CuNaO4Cl4	Ba4Cu1Na1Cl4O4	Ba	4	Cu	1	Na	1	Cl	4													O	4		1	1997																											2	T	I4/mmm			4.218	16.157																																																																																																																			1	The reactions were carried out in a flowing, CO2 free, O2 at 700-800C, for 24H-FC to RT					New Cu(III) Oxychlorides in the Ba-Cu-M-O-Cl (M=Li,Na) System			CNR, Institute of Structural Chemistry, University of Parma, Italy	J.Solid State Chem.129(1997)360-362	F.C. Matacotta,G. Bocelli,G. Calestani,K.A. Thomas,K.V. Ramanujachary,M. Greenblatt		
7675	JSC1280169		(La,Sr)2(Cu,Mn)O4	La1.9Sr0.1Cu0.95Mn0.05O4	La	1.9	Sr	0.1	Cu	0.95	Mn	0.05													O	z	4		1997																											2	T				3.794		13.146																	10																																																																																				0.5												La2O3,SrCO3,CuO,Mn(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7676	JSC1280169		(La,Sr)2(Cu,Mn)O4	La1.8Sr0.2Cu0.9Mn0.1O4.01	La	1.8	Sr	0.2	Cu	0.9	Mn	0.1													O	z	4.01		1997																											2	T				3.793		13.139																	10																																																																																				10												La2O3,SrCO3,CuO,Mn(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7677	JSC1280169		(La,Sr)2(Cu,Mn)O4	La1Sr1Cu0.5Mn0.5O3.99	La	1	Sr	1	Cu	0.5	Mn	0.5													O	z	3.99		1997																											2	T				3.807		12.745																	10																																																																																				4400												La2O3,SrCO3,CuO,Mn(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7678	JSC1280169		(La,Sr)2(Cu,Ru)O4	La1.9Sr0.1Cu0.95Ru0.05O4	La	1.9	Sr	0.1	Cu	0.95	Ru	0.05													O	z	4		1997																											2	T				3.794		13.179																	10																																																																																				0.19												La2O3,SrCO3,CuO,(TiO2,RuO2)		mixture-heat(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7679	JSC1280169		(La,Sr)2(Cu,Ru)O4	La1.8Sr0.2Cu0.9Ru0.1O3.99	La	1.8	Sr	0.2	Cu	0.9	Ru	0.1													O	z	3.99		1997																											2	T				3.795		13.175																	10																																																																																				1.5												La2O3,SrCO3,CuO,(TiO2,RuO2)		mixture-heat(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7680	JSC1280169		(La,Sr)2(Cu,Ti)O4	La1Sr1Cu0.5Ti0.5Oz	La	1	Sr	1	Cu	0.5	Ti	0.5													O	z			1997																											2	T				3.818		13.003																	10																																																																																				650												La2O3,SrCO3,CuO,(TiO2,RuO2)		mixture-heat(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7681	JSC1280169		(La,Sr)2(Cu,Fe)O4	La1.9Sr0.1Cu0.95Fe0.05O4	La	1.9	Sr	0.1	Cu	0.95	Fe	0.05													O	z	4		1997																											2	T				3.795		13.164																	10																																																																																				14												Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7682	JSC1280169		(La,Sr)2(Cu,Fe)O4	La0.8Sr0.2Cu0.9Fe0.1O4	La	0.8	Sr	0.2	Cu	0.9	Fe	0.1													O	z	4		1997																											2	T				3.787		13.173																	10																																																																																																Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7683	JSC1280169		(La,Sr)2(Cu,Fe)O4	La1.7Sr0.3Cu0.85Fe0.15O4	La	1.7	Sr	0.3	Cu	0.85	Fe	0.15													O	z	4		1997																											2	T				3.782		13.169																	10																																																																																				2.3												Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7684	JSC1280169		(La,Sr)2(Cu,Fe)O4	La1.6Sr0.4Cu0.8Fe0.2O4	La	1.6	Sr	0.4	Cu	0.8	Fe	0.2													O	z	4		1997																											2	T				3.784		13.168																	10																																																																																				5.5												Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7685	JSC1280169		(La,Sr)2(Cu,Fe)O4	La1.5Sr0.5Cu1.5Fe0.5O3.94	La	1.5	Sr	0.5	Cu	1.5	Fe	0.5													O	z	3.94		1997																											2	T				3.786		13.166																	10																																																																																																Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7686	JSC1280169		(La,Sr)2(Cu,Fe)O4	La1Sr1Cu0.5Fe0.5O3.9	La	1	Sr	1	Cu	0.5	Fe	0.5													O	z	3.9		1997																											2	T				3.802		12.956																	10																																																																																				270												Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7687	JSC1280169		(La,Sr)2(Cu,Fe)O4	La0.5Sr1.5Cu0.25Fe0.75O3.8	La	0.5	Sr	1.5	Cu	0.25	Fe	0.75													O	Z	3.8		1997																											2	T				3.832		12.678																	10																																																																																																Fe(C2O4).2H2O		decomposition(600C,6H)-mixture-pellet-SIN(1150C,48H)					New La2CuO4 Derivatives La2-2xSr2xCu1-xMxO4(M=Ti,Mn,Fe, or Ru): A Study of Linear Cu-O-M Electronic Interaction in Two Dimensions			Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560 012, India	J.Solid State Chem.128(1997)169-175	J. Gopalakrishnan,K. Ramesha,N.Y. Vasanthacharya,S. Uma		
7688	JSC1280310		Gd(Ba)2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8		1	1997																											3	Y124																				73.1					73.1																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7689	JSC1280310		Gd(Sr,Ba)2Cu4O8	Gd1Sr0.1Ba1.9Cu4O8	Gd	1	Sr	0.1	Ba	1.9	Cu	4													O	8		1	1997																											3	Y124																				73.5					73.5																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7690	JSC1280310		Gd(Sr,Ba)2Cu4O8	Gd1Sr1.8Ba0.2Cu4O8	Gd	1	Sr	1.8	Ba	0.2	Cu	4													O	8		1	1997																											3	Y124																				73.1					73.1																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7691	JSC1280310		Ho(Ba)2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		1	1997																											3	Y124																				68.5					68.5																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7692	JSC1280310		Ho(Ba,Sr)2Cu4O8	Ho1Sr0.2Ba1.8Cu4O8	Ho	1	Sr	0.2	Ba	1.8	Cu	4													O	8		1	1997																											3	Y124																				68.8					68.8																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7693	JSC1280310		HO(Ba,Sr)2Cu4O8	Ho1Sr0.4Ba1.6Cu4O8	Ho	1	Sr	0.4	Ba	1.6	Cu	4													O	8		1	1997																											3	Y124																				68.1					68.1																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7694	JSC1280310		Ho(Ba,Sr)2Cu4O8	Ho1Sr0.6Ba1.4Cu4O8	Ho	1	Sr	0.6	Ba	1.4	Cu	4													O	8		1	1997																											3	Y124																				68.3					68.3																																																																																																See J Am. Ceram, Soc. 76(1993)1618					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
7695	JCG1710409	semiconducting Pr1.06Ba1.93Cu2.95Mg0.05O7-z by ICP	Pr(Ba,Pr)2Cu3O7	Pr1.06Ba1.94Cu3O7-z	Pr	1.06	Ba	1.94	Cu	3															O	7-z		3	1997																												Y123																							15																																																																																																		by inproved top seeded crystal pulling method, starting materials are Pr:Ba:Cu: =5:30:65 forx=0.06,=5:28:67 for x=0.14,=5:24:71 for x=0.29					Control of Pr for Ba substitution in PBCO single crystals by the crystal polling method			SRL-ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	J.Cryst.Growth,171(1997)409-414	Minoru Takagi,Yuh Shiohara		
7696	JCG1710409	semiconducting Pr1.14Ba1.88Cu2.94Mg0.04O7-z by ICP	Pr(Ba,Pr)2Cu3O7	Pr1.14Ba1.86Cu3O7-z	Pr	1.14	Ba	1.86	Cu	3															O	7-z		3	1997																											2	Y123				3.907		11.768																	25																																																																																																		by inproved top seeded crystal pulling method, starting materials are Pr:Ba:Cu: =5:30:65 forx=0.06,=5:28:67 for x=0.14,=5:24:71 for x=0.29					Control of Pr for Ba substitution in PBCO single crystals by the crystal polling method			SRL-ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	J.Cryst.Growth,171(1997)409-414	Minoru Takagi,Yuh Shiohara		
7697	JCG1710409	semiconducting Pr1.29Ba1.67Cu2.95Mg0.05O7-z by ICP	Pr(Ba,Pr)2Cu3O7	Pr1.29Ba1.71Cu3O7-z	Pr	1.29	Ba	1.71	Cu	3															O	7-z		3	1997																												Y123																							60																																																																																																		by inproved top seeded crystal pulling method, starting materials are Pr:Ba:Cu: =5:30:65 forx=0.06,=5:28:67 for x=0.14,=5:24:71 for x=0.29					Control of Pr for Ba substitution in PBCO single crystals by the crystal polling method			SRL-ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	J.Cryst.Growth,171(1997)409-414	Minoru Takagi,Yuh Shiohara		
7698	JCG1710380	anisotropy factor=19.9		Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1997																												Y123																																					SQUID,not in detarls		238	4729																																																																																	flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7699	JCG1710380	anisotropy factor=47.3		Y0.87Pr0.13Ba2Cu3O7-z	Y	0.87	Pr	0.13	Ba	2	Cu	3													O	7-z		3	1997																																																																	SQUID,not in detarls		55	2594																																																																																	flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7700	JCG1710380	anisotropy factor=82.3		Y0.73Pr0.27Ba2Cu3O7-z	Y	0.73	Pr	0.27	Ba	2	Cu	3													O	7-z		3	1997																																																																	SQUID, not in detarls		17	1399																																																																																	flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7701	JCG1710380	anisotropy factor=95.8		Y0.59Pr0.41Ba2Cu3O7-z	Y	0.59	Pr	0.41	Ba	2	Cu	3													O	7-z		3	1997																																																																	SQUID,not in detarls		15	1422																																																																																	flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7702	JCG1710380			Y0.51Pr0.49Ba2Cu3O7-z	Y	0.51	Pr	0.49	Ba	2	Cu	3													O	7-z		3	1997																																																																																																																																																					flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7703	JCG1710380			Y0.41Pr0.59Ba2Cu3O7-z	Y	0.41	Pr	0.59	Ba	2	Cu	3													O	7-z		3	1997																																																																																																																																																					flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7704	JCG1710380			Y0.21Pr0.79Ba2Cu3O7-z	Y	0.21	Pr	0.79	Ba	2	Cu	3													O	7-z		3	1997																																																																																																																																																					flux method, flux-BaCuO2+CuO, starting materials-al2ao3 crucible-heat(Tmax=1050C)-slow cool-renove flux-ANN(420C,7days oxygenation)					Growth and characterization of (Y1-xPrx)Ba2Cu3O7-delta single crystals			Physikalisches Institut, RWTH Aachen, D-52056 Aachen, Germany	J.Cryst.Growth,171(1997)380-386	G. Guntherodt,J. Oebel,L. Winkeler,R. Muller		
7705	JIM0380745	as-grown,not s/c.	Ndba2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	1997																												Y123																							10																																																																																					20													grown by the top-seedad solution-growth method					In-Plane and Out-of-Plane Thermal Conductivities of a Large Single Crystal of NdBa2Cu3O7-x Prepared by the Top-Seeded Solution-Growth Method			Faculty of Engineering, Iwate University, 4-3-5 Ueda, Morioka 020, Japan	Materials Transactions,JIM38(1997)745-748	Hidetaka Sato,Kimiaki Iwasaki,Koshichi Noto,Michiaki Matsukawa,Norio Kobayashi,Xin Yao,Yuh Shiohara		
7706	JIM0380745		NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	1997																												Y123																			94						94																																																																																																top-seedad solution-growth method-ANN(34C,1 mouth in O2 flow of 0.1 MPa)					In-Plane and Out-of-Plane Thermal Conductivities of a Large Single Crystal of NdBa2Cu3O7-x Prepared by the Top-Seeded Solution-Growth Method			Faculty of Engineering, Iwate University, 4-3-5 Ueda, Morioka 020, Japan	Materials Transactions,JIM38(1997)745-748	Hidetaka Sato,Kimiaki Iwasaki,Koshichi Noto,Michiaki Matsukawa,Norio Kobayashi,Xin Yao,Yuh Shiohara		
7707	JP00901451	inpurity phase=CaHgO2, BaCuO2	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1997																											2	Hg1223				3.855		15.842													110						110																																																																																																precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7708	JP00901451	inpurity phase=CaHgO2, BaCuO2	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.9Pb0.1Ba2Ca2Cu3O8+z	Hg	0.9	Pb	0.1	Ba	2	Ca	2	Cu	3											O	8+z			1997																											2	Hg1223				3.85		15.836																																																																																																																			precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7709	JP00901451	inpurity phase=CaHgO2, BaCuO2	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.8Pb0.2Ba2Ca2Cu3O8+z	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	8+z			1997																											2	Hg1223				3.848		15.831																																																																																																																			precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7710	JP00901451	inpurity phase-CaHgO2, BaCuO2	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.7Pb0.3Ba2Ca2Cu3O8+z	Hg	0.7	Pb	0.3	Ba	2	Ca	2	Cu	3											O	8+z			1997																											2	Hg1223				3.842		15.824													135			143			143																																																																																																precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7711	JP00901451	inpurity phase=CaHgO2, BaCuO2	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.6Pb0.4Ba2Ca2Cu3O8+z	Hg	0.6	Pb	0.4	Ba	2	Ca	2	Cu	3											O	8+z			1997																											2	Hg1223				3.842		15.818																																																																																																																			precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7712	JP00901451	inpurity phase=CaHgO2, BaCuO2	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.5Pb0.5Ba2Ca2Cu3O8+z	Hg	0.5	Pb	0.5	Ba	2	Ca	2	Cu	3											O	8+z			1997																											2	Hg1223				3.84		15.822																																																																																																																			precursor(Ba2Ca2Cu3O7)+HgO+PbO-mixture-pellet-sealed in vacum tube-heat(850C,4C/min)-hold IOH-cool to 200C at 4C/min-hold(2H)-ANN(240C,10H in O2)					The crystal structure of the superconductor HgBa2Ca2Cu3O8+delta with Pb substitution			National Laboratory of Solid State Microstrutures, Institute of Solid State, and Centre for Advanced Studies in Science and Technology of Microstructures,Nanging University,Nanjing 210093,People's Repblic of China	J.Phys.;Cond.Matter9(1997)1451-1460	F.M. Pan,H M Shao,Mao Zhiqing,N Xu,SS Jiang,X S Wu,Zhang Yuheng,Zuo Jian		
7713	JP00900075	S/C	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1Oz	Nd	1.85	Ce	0.15	Cu	1															O	z			1997																												T'																																																																																																																							Nd2O3,CaCO3,CuO		mixture-fire(1000C,20H+1120C,20H)-precursor (Nd1.85-xCaxCuOz)+CeO2-mixture-pellet-SIN(1120C,20H)-Q to RT					Anomalies in thermoelectric power at 200 K in the calcium-doped NdCeCuO system			Structure Research Laboratory, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)L75-L82	G E Zhou,K Q Ruan,L Shi,L Z Cao,R P Wang,T F Li,X H Chen,Y B Jia,Y H Zhang,Y M Qiu		
7714	JP00900075	S/C(116) peak in XRD patlern split to two peaks at about 200K	(Nd,Ce,Ca)2CuO4	Nd1.75Ce0.15Ca0.1Cu1Oz	Nd	1.75	Ce	0.15	Ca	0.1	Cu	1													O	z		1	1997																												T'				3.939		12.043																																																																																																																	Nd2O3,CaCO3,CuO		mixture-fire(1000C,20H+1120C,20H)-precursor (Nd1.85-xCaxCuOz)+CeO2-mixture-pellet-SIN(1120C,20H)-Q to RT					Anomalies in thermoelectric power at 200 K in the calcium-doped NdCeCuO system			Structure Research Laboratory, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)L75-L82	G E Zhou,K Q Ruan,L Shi,L Z Cao,R P Wang,T F Li,X H Chen,Y B Jia,Y H Zhang,Y M Qiu		
7715	JP00900075	S/C	(Nd,Ca)2CuO4	Nd1.55Ce0.15Ca0.3Cu1Oz	Nd	1.55	Ce	0.15	Ca	0.3	Cu	1													O	z			1997																												T'																																																																																																																							Nd2O3,CaCO3,CuO		mixture-fire(1000C,20H+1120C,20H)-precursor (Nd1.85-xCaxCuOz)+CeO2-mixture-pellet-SIN(1120C,20H)-Q to RT					Anomalies in thermoelectric power at 200 K in the calcium-doped NdCeCuO system			Structure Research Laboratory, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)L75-L82	G E Zhou,K Q Ruan,L Shi,L Z Cao,R P Wang,T F Li,X H Chen,Y B Jia,Y H Zhang,Y M Qiu		
7716	JP00900075	not s/c	Nd2CuO4	Nd2Cu1O4+z	Nd	2	Cu	1																	O	4+z			1997																												T'																																																																																																																							Nd2O3,CaCO3,CuO		mixture-fire(1000C,20H+11OC, in air)-ANN(950C,in N2)					Anomalies in thermoelectric power at 200 K in the calcium-doped NdCeCuO system			Structure Research Laboratory, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)L75-L82	G E Zhou,K Q Ruan,L Shi,L Z Cao,R P Wang,T F Li,X H Chen,Y B Jia,Y H Zhang,Y M Qiu		
7717	JP00900075	not s/c	(Nd,Ca)2CuO4	Nd1.85Ca0.15Cu1O4+z	Nd	1.85	Ca	0.15	Cu	1															O	4+z			1997																												T'																																																																																																																							Nd2O3,CaCO3,CuO		mixture-fire(1000C,20H+11OC, in air)-ANN(950C,in N2)					Anomalies in thermoelectric power at 200 K in the calcium-doped NdCeCuO system			Structure Research Laboratory, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)L75-L82	G E Zhou,K Q Ruan,L Shi,L Z Cao,R P Wang,T F Li,X H Chen,Y B Jia,Y H Zhang,Y M Qiu		
7718	JP00905137		Bi2(Sr,La)2CuOz	Bi2Sr1.65La0.35Cu1Oz	Bi	2	Sr	1.65	La	0.35	Cu	1													O	z		1	1997																												Bi2201				5.357	5.379	24.549													19.4		34.5				26.95																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7719	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.9Pb0.1Sr1.65La0.35Cu1Oz	Bi	1.9	Pb	0.1	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.369	5.367	24.536													23.8		37.6				30.7																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7720	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.65La0.35Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.358		24.529													30.9		42.7				36.8																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7721	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.7Pb0.3Sr1.65La0.35Cu1Oz	Bi	1.7	Pb	0.3	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.367	5.344	24.52													31.8		43.7				37.75																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7722	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.6Pb0.4Sr1.65La0.35Cu1Oz	Bi	1.6	Pb	0.4	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.361	5.31	24.501													35.8		44.8				40.3																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7723	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.4Pb0.6Sr1.65La0.35Cu1Oz	Bi	1.4	Pb	0.6	Sr	1.65	La	0.35	Cu	1											O	z			1997																												Bi2201				5.381	5.267	24.471													37		45				41																																																																																															1	mixture-preheat(820C,24H in air)-heat(830C,1day in air)-pellet-SIN(840-860C,2days in air)-Q to RT in air-ANN(550C,3H in P(O2)=10E-5 atm)					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7724	JP00905137		Bi2(Sr,La)2CuOz	Bi2Sr1.65La0.35Cu1Oz	Bi	2	Sr	1.65	La	0.35	Cu	1													O	z		1	1997																												Bi2201				5.379	5.377	24.468													25.3		33.4				29.35																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7725	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.9Pb0.1Sr1.65La0.35Cu1Oz	Bi	1.9	Pb	0.1	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.381	5.377	24.459													25.8		34.3				30.05																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7726	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.65La0.35Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.385	5.362	24.459													26.3		35.5				30.9																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7727	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.7Pb0.3Sr1.65La0.35Cu1Oz	Bi	1.7	Pb	0.3	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.387	5.335	24.448													26.7		35.4				31.05																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7728	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.6Pb0.4Sr1.65La0.35Cu1Oz	Bi	1.6	Pb	0.4	Sr	1.65	La	0.35	Cu	1											O	z		1	1997																												Bi2201				5.388	5.303	24.444													22.2		31.5				26.85																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7729	JP00905137		(Bi,Pb)2(Sr,La)2CuOz	Bi1.4Pb0.6Sr1.65La0.35Cu1Oz	Bi	1.4	Pb	0.6	Sr	1.65	La	0.35	Cu	1											O	z			1997																												Bi2201				5.4	5.278	24.421													20.1		30.3				25.2																																																																																															1	mixture-preheat (820C,24H in air)-heat (830C, in air)-pellet-SIN (840-860C, 2days in air)-Q to RT in air					A study on the transport properties in the Bi2-xPbxSr1.65La0.35CuOy system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.;Cond.Matter9(1997)5137-5144	Mao Zhiqiang,Shi Lei,Tian Mingliang,Xu Gaojie,Xu Xiaojun,Zhang Yuheng		
7730	PHC2880057			La3.5Ca2Ba3.5Cu7O16.415	La	3.5	Ca	2	Ba	3.5	Cu	7													O	z	16.415	1	1997																											2	La3137				3.909		11.718																																																																																																					22.4												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7731	PHC2880057			La3.3Gd0.1Ca0.2Ba3.4Cu7O16.449	La	3.3	Gd	0.1	Ca	0.2	Ba	3.4	Cu	7											O	z	16.449	1	1997																											2	La3137				3.905		11.713																																																																																																					18.5												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7732	PHC2880057			La3.1Gd0.2Ca0.4Ba3.3Cu7O16.473	La	3.1	Gd	0.2	Ca	0.4	Ba	3.3	Cu	7											O	z	16.473	1	1997																											2	La3137				3.892		11.667													31	48	55	33			48																																																																																		7.9												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7733	PHC2880057			La2.9Gd0.3Ca0.6Ba3.2Cu0.3O16.503	La	2.9	Gd	0.3	Ca	0.6	Ba	3.2	Cu	0.3											O	z	16.503	1	1997																											2	La3137				3.888		11.659													45	58	70	46			58																																																																																		5.5												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7734	PHC2880057			La2.7Gd0.4Ca0.8Ba3.1Cu7O16.537	La	2.7	Gd	0.4	Ca	0.8	Ba	3.1	Cu	7											O	z	16.537	1	1997																											2	La3137				3.871		11.644													69	74	78	71			74																																																																																		2.5												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7735	PHC2880057			La2.5Gd0.5Ca1Ba3Cu7O16.359	La	2.5	Gd	0.5	Ca	1	Ba	3	Cu	7											O	z	16.359	1	1997																											2	La3137				3.869		11.63													78	80	82				80																																																																																		4.3												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7736	PHC2880057			La2.3Gd0.6Ca1.2Ba2.9Cu7O16.543	La	2.3	Gd	0.6	Ca	1.2	Ba	2.9	Cu	7											O	z	16.543	1	1997																											2	La3137				3.866		11.609													79	80	82	80			80																																																																																		4.2												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7737	PHC2880057			La2.1Gd0.7Ca1.4Ba2.8Cu0.7O16.471	La	2.1	Gd	0.7	Ca	1.4	Ba	2.8	Cu	0.7											O	z	16.471	1	1997																											2	La3137				3.863		11.604													77	79	81				79																																																																																		6												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7738	PHC2880057			La3.3Nd0.1Ca0.2Ba3.4Cu7Oz	La	3.3	Nd	0.1	Ca	0.2	Ba	3.4	Cu	7											O	z		1	1997																												La3137																																																																																																											18.4												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7739	PHC2880057			La2.9Nd0.3Ca0.6Ba3.2Cu7Oz	La	2.9	Nd	0.3	Ca	0.6	Ba	3.2	Cu	7											O	z		1	1997																												La3137																			47	58	68				58																																																																																		10.6												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7740	PHC2880057			La2.7Nd0.4Ca0.8Ba3.1Cu7Oz	La	2.7	Nd	0.4	Ca	0.8	Ba	3.1	Cu	7											O	z		1	1997																												La3137																			73	76	79				76																																																																																		7.2												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7741	PHC2880057			La2.5Nd0.5Ca1Ba3Cu7Oz	La	2.5	Nd	0.5	Ca	1	Ba	3	Cu	7											O	z		1	1997																												La3137																			78	80	81				80																																																																																		5.6												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7742	PHC2880057			La2.1Nd0.7Ca1.4Ba2.8Cu7Oz	La	2.1	Nd	0.7	Ca	1.4	Ba	2.8	Cu	7											O	z		1	1997																												La3137																			77	79	82				79																																																																																		5.8												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7743	PHC2880057			La2.5Dy0.5Ca1Ba3Cu7Oz	La	2.5	Dy	0.5	Ca	1	Ba	3	Cu	7											O	z		1	1997																												La3137																			78	80	82				80																																																																																		5.2												R2O3,BaCO3,CuO,CaCO3	1	mixture-heat (950C,24H in air)-pellet-SIN(940-960C,12H in N2 and O2)-ANN(500C,12H in O2 flow)-cool to RT(1C/mm)					Superconductivity of the La3.5-x-yRyCa2xBa3.5-xCu7Oz system (R=Gd, Nd and Dy)	199708		Department of Physics, Saurashtra University, Rajkpt 3600 005, India	Physica.C,288(1997)57-63	D.G. Kuberkar,G.J. Baldha,M.V. Subbarao,R.G. Kulkarni		
7744	SUP0100231	inprity phase=Li2CuO2, Y2Ba2CuO5	YBa2Cu3LixO7	Y1Ba2Cu3Li0.02O7-z	Y	1	Ba	2	Cu	3	Li	0.02													O	7-z			1997																											3	Y123																				91.18					91.18											kA/m																																																																																			Y2O3,CuO,BaCO3,LiOH		mixture-heat(890C,20H in flowing O2)-grind-pellet-SIN(936C,16H in flowing O2)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
7745	SUP0100231	impurity phase=LiCuO2,Y2BaCuO5	YBa2Cu3LixO7	Y1Ba2Cu3Li0.08O7-z	Y	1	Ba	2	Cu	3	Li	0.08													O	7-z			1997																											3	Y123																				89.2					89.2											kA/m																																																																																			Y2O3,CuO,BaCO3,LiOH		mixture-heat(890C,20H in flowing O2)-grind-pellet-SIN(936C,16H in flowing O2)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
7746	SUP0100231	impurity phase=Li2CuO2,Y2BaCuO5	YBa2Cu3LixO7	Y1Ba2Cu3Li0.1O7-z	Y	1	Ba	2	Cu	3	Li	0.1													O	7-z			1997																											3	Y123																				88.91					88.91											kA/m																																																																																			Y2O3,CuO,BaCO3,LiOH		mixture-heat(890C,20H in flowing O2)-grind-pellet-SIN(936C,16H in flowing O2)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
7747	SUP0100231	imprity phase=Li2CuO2,Y2Ba2CuO5	YBa2Cu3LixO7	Y1Ba2Cu3Li0.3O7-z	Y	1	Ba	2	Cu	3	Li	0.3													O	7-z			1997																											3	Y123																				86					86																																																																																														Y2O3,CuO,BaCO3,LiOH		mixture-heat(890C,20H in flowing O2)-grind-pellet-SIN(936C,16H in flowing O2)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
7748	SUP0100231	impurity phase=Li2CuO2,YBa2CuO5	YBa2Cu3LixO7	Y1Ba2Cu3Li0.5O7-z	Y	1	Ba	2	Cu	3	Li	0.5													O	7-z			1997																											3	Y123																				83.79					83.79																																																																																														Y2O3,CuO,BaCO3,LiOH		mixture-heat(890C,20H in flowing O2)-grind-pellet-SIN(936C,16H in flowing O2)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
7749	SUP0100159		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1997																											2	T				3.771		13.217															37.8				37.8																																																																																		19.8												La2O3,SrCO3,CuO,MgO	1	mixture-heat(1000C,12H in air)-grind-pellet-SIN(1150C,24H in O2 flow)-ANN (600C,24H in O2 flow)-FC to RT					Structure Studies of La1.85Sr0.15CuO4 Doped with Ng at High Doping Level			National Laboratory of Solid State Microstructures, and  Center for Advanced Studies in Science and Technology of Microstructures,nanjing University, Nanjing 210093, China	J.Superconductivity,(1997)159	G. J. Xu,H. Zhang,J. Lin,S.S. Jiang,W.J. Liu,W.M. Chen,X. Jin,X.S. Wu,Z.Q. Mao		
7750	SUP0100159		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.95Mg0.05O4	La	1.85	Sr	0.15	Cu	0.95	Mg	0.05													O	4		1	1997																											2	T				3.777		13.198																																																																																																					24.1												La2O3,SrCO3,CuO,MgO	1	mixture-heat(1000C,12H in air)-grind-pellet-SIN(1150C,24H in O2 flow)-ANN (600C,24H in O2 flow)-FC to RT					Structure Studies of La1.85Sr0.15CuO4 Doped with Ng at High Doping Level			National Laboratory of Solid State Microstructures, and  Center for Advanced Studies in Science and Technology of Microstructures,nanjing University, Nanjing 210093, China	J.Superconductivity,(1997)159	G. J. Xu,H. Zhang,J. Lin,S.S. Jiang,W.J. Liu,W.M. Chen,X. Jin,X.S. Wu,Z.Q. Mao		
7751	SUP0100159		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.9Mg0.1O4	La	1.85	Sr	0.15	Cu	0.9	Mg	0.1													O	4			1997																											2	T				3.779		13.16															29.6				29.6																																																																																		30.4												La2O3,SrCO3,CuO,MgO	1	mixture-heat(1000C,12H in air)-grind-pellet-SIN(1150C,24H in O2 flow)-ANN (600C,24H in O2 flow)-FC to RT					Structure Studies of La1.85Sr0.15CuO4 Doped with Ng at High Doping Level			National Laboratory of Solid State Microstructures, and  Center for Advanced Studies in Science and Technology of Microstructures,nanjing University, Nanjing 210093, China	J.Superconductivity,(1997)159	G. J. Xu,H. Zhang,J. Lin,S.S. Jiang,W.J. Liu,W.M. Chen,X. Jin,X.S. Wu,Z.Q. Mao		
7752	SUP0100159		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.8Mg0.2O4	La	1.85	Sr	0.15	Cu	0.8	Mg	0.2													O	4		1	1997																											2	T				3.786		13.192															15.6				15.6																																																																																		250												La2O3,SrCO3,CuO,MgO	1	mixture-heat(1000C,12H in air)-grind-pellet-SIN(1150C,24H in O2 flow)-ANN (600C,24H in O2 flow)-FC to RT					Structure Studies of La1.85Sr0.15CuO4 Doped with Ng at High Doping Level			National Laboratory of Solid State Microstructures, and  Center for Advanced Studies in Science and Technology of Microstructures,nanjing University, Nanjing 210093, China	J.Superconductivity,(1997)159	G. J. Xu,H. Zhang,J. Lin,S.S. Jiang,W.J. Liu,W.M. Chen,X. Jin,X.S. Wu,Z.Q. Mao		
7753	SUP0100159		(La,Sr)2(Cu,Mg)O4	La1.85Sr0.15Cu0.7Mg0.3O4	La	1.85	Sr	0.15	Cu	0.7	Mg	0.3													O	4		1	1997																											2	T				3.812		13.082																																																																																																																	La2O3,SrCO3,CuO,MgO	1	mixture-heat(1000C,12H in air)-grind-pellet-SIN(1150C,24H in O2 flow)-ANN (600C,24H in O2 flow)-FC to RT					Structure Studies of La1.85Sr0.15CuO4 Doped with Ng at High Doping Level			National Laboratory of Solid State Microstructures, and  Center for Advanced Studies in Science and Technology of Microstructures,nanjing University, Nanjing 210093, China	J.Superconductivity,(1997)159	G. J. Xu,H. Zhang,J. Lin,S.S. Jiang,W.J. Liu,W.M. Chen,X. Jin,X.S. Wu,Z.Q. Mao		
7754	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.01C0.32H0.16N0.08Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.01	C	0.32	H	0.16	N	0.08					O	z			1994																												Bi2212																					68.3				68.3																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7755	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.02C0.64H0.32N0.16Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.02	C	0.64	H	0.32	N	0.16					O	z			1994																																																	65.1				65.1																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7756	MPL0080251		(ZnPc)Bi2Sr2Ca2Cu3Oz	Bi2Sr2Ca2Cu3Zn0.009C0.288H0.144N0.72Oz	Bi	2	Sr	2	Ca	2	Cu	3	Zn	0.009	C	0.288	H	0.144	N	0.72					O	z			1994																												Bi2223																					92.9				92.9																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7757	MPL0080251		(ZnPc)Bi2Sr2Ca2Cu3Oz	Bi2Sr2Ca2Cu3Zn0.013C0.416H0.208N0.104Oz	Bi	2	Sr	2	Ca	2	Cu	3	Zn	0.013	C	0.416	H	0.208	N	0.104					O	z			1994																																																	91				91																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7758	MPL0080251		(ZnPc)Bi2Sr2Ca2Cu3Oz	Bi2Sr2Ca2Cu3Zn0.017C0.544H0.272N0.136Oz	Bi	2	Sr	2	Ca	2	Cu	3	Zn	0.017	C	0.544	H	0.272	N	0.136					O	z			1994																																																	87.1				87.1																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7759	MPL0080251		(ZnPc)Bi2Sr2Ca2Cu3Oz	Bi2Sr2Ca2Cu3Zn0.02C0.64H0.32N0.16Oz	Bi	2	Sr	2	Ca	2	Cu	3	Zn	0.02	C	0.64	H	0.32	N	0.16					O	z			1994																																																	79.8				79.8																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7760	JMR0122907		NdBa2Cu3Oz	Nd1Ba2Cu3O6.95	Nd	1	Ba	2	Cu	3															O	Z	6.95		1997																												Y123				3.865	3.9167	11.754														89					89																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7761	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.1Ba1.9Cu3O6.96	Nd	1.1	Ba	1.9	Cu	3															O	Z	6.96		1997																												Y123				3.8614	3.9144	11.7378														87.6					87.6																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7762	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.15Ba1.85Cu3O6.96	Nd	1.15	Ba	1.85	Cu	3															O	Z	6.96		1997																												Y123				3.8703	3.9077	11.7192														76.8					76.8																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7763	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.25Ba1.75Cu3O6.99	Nd	1.25	Ba	1.75	Cu	3															O	Z	6.99		1997																												Y123				3.889		11.6871														52.7					52.7																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7764	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.35Ba1.65Cu3O7.02	Nd	1.35	Ba	1.65	Cu	3															O	Z	7.02		1997																												Y123				3.8881		11.6643														35.9					35.9																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7765	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.45Ba1.55Cu3O7.08	Nd	1.45	Ba	1.55	Cu	3															O	Z	7.08		1997																												Y123				3.885		11.6244														26.5					26.5																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7766	JMR0122907		Nd(Ba,Nd)2Cu3Oz	Nd1.5Ba1.5Cu3O7.12	Nd	1.5	Ba	1.5	Cu	3															O	Z	7.12		1997																												Y123				3.8855		11.6097														15.4					15.4																																																																																																					The thermopower of Nd1+xBa2-xCu3Oy in a comparative study of effects of Ba-site doping versus chain-Cu-site doping			Department of Physics and Crown Center for Superconductivity, Technion, Haifa, 32000, Israel	J.Mater.Res.12(1997)2907	A. Knizhnik,B. Fisher,G.M. Reisner,J. Genossar,L. Patlagan		
7767	MPL0110311		Pb2Sr2(Y,Ca)Cu3O8Fx	Pb2Sr2Y0.5Ca0.5Cu3O8.1882	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8-X	8.1882		1997																											3	Pb3212				5.395	5.318	15.731													22	62					62																																																																																														Y2O3,CuO,CaCO3,SrCO3,PbO,PbF2		Pb2Sr2Y0.5Ca0.5Cu3Oz was made by sintering(860C,14H)-mixed with PbO+PbF2-pellet-SIN(920C,2H in N2)-SIN(860C)-Q to RT in N2					STRUCTURE AND PROPERTIES OF SUBSTITUTION OF FLUORINE FOR APICAL OXYGEN IN Pb2Sr2Y0.5Ca0.5Cu3O8+delta SUPERCONDUCTOR			Deparment of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, P. R. China	Mod.Phys.Lett.B,11(1997)311-321	BAI-RU ZHAO,DE GAO,SHU-FEN JIANG,SHU-LIAN JIA,XIAO-HUI GAO		
7768	MPL0110311		Pb2Sr2(Y,Ca)Cu3O8Fx	Pb2Sr2Y0.5Ca0.5Cu3F0.253O7.9858	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3	F	0.253									O	8-X	7.9858		1997																											3	Pb3212				5.391	5.119	15.727													23	68					68																																																																																														Y2O3,CuO,CaCO3,SrCO3,PbO,PbF2		Pb2Sr2Y0.5Ca0.5Cu3Oz was made by sintering(860C,14H)-mixed with PbO+PbF2-pellet-SIN(920C,2H in N2)-SIN(860C)-Q to RT in N2					STRUCTURE AND PROPERTIES OF SUBSTITUTION OF FLUORINE FOR APICAL OXYGEN IN Pb2Sr2Y0.5Ca0.5Cu3O8+delta SUPERCONDUCTOR			Deparment of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, P. R. China	Mod.Phys.Lett.B,11(1997)311-321	BAI-RU ZHAO,DE GAO,SHU-FEN JIANG,SHU-LIAN JIA,XIAO-HUI GAO		
7769	MPL0110311		Pb2Sr2(Y,Ca)Cu3O8Fx	Pb2Sr2Y0.5Ca0.5Cu3F0.5612O7.649	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3	F	0.5612									O	8-X	7.649		1997																											3	Pb3212				5.385	5.105	15.718													38	72					72																																																																																														Y2O3,CuO,CaCO3,SrCO3,PbO,PbF2		Pb2Sr2Y0.5Ca0.5Cu3Oz was made by sintering(860C,14H)-mixed with PbO+PbF2-pellet-SIN(920C,2H in N2)-SIN(860C)-Q to RT in N2					STRUCTURE AND PROPERTIES OF SUBSTITUTION OF FLUORINE FOR APICAL OXYGEN IN Pb2Sr2Y0.5Ca0.5Cu3O8+delta SUPERCONDUCTOR			Deparment of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, P. R. China	Mod.Phys.Lett.B,11(1997)311-321	BAI-RU ZHAO,DE GAO,SHU-FEN JIANG,SHU-LIAN JIA,XIAO-HUI GAO		
7770	MPL0110311		Pb2Sr2(Y,Ca)Cu3O8Fx	Pb2Sr2Y0.5Ca0.5Cu3F0.8115O7.3458	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3	F	0.8115									O	8-X	7.3458		1997																											3	Pb3212				5.38	5.098	15.701													52	78					78																																																																																														Y2O3,CuO,CaCO3,SrCO3,PbO,PbF2		Pb2Sr2Y0.5Ca0.5Cu3Oz was made by sintering(860C,14H)-mixed with PbO+PbF2-pellet-SIN(920C,2H in N2)-SIN(860C)-Q to RT in N2					STRUCTURE AND PROPERTIES OF SUBSTITUTION OF FLUORINE FOR APICAL OXYGEN IN Pb2Sr2Y0.5Ca0.5Cu3O8+delta SUPERCONDUCTOR			Deparment of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, P. R. China	Mod.Phys.Lett.B,11(1997)311-321	BAI-RU ZHAO,DE GAO,SHU-FEN JIANG,SHU-LIAN JIA,XIAO-HUI GAO		
7771	MPL0110311		Pb2Sr2(Y,Ca)Cu3O8Fx	Pb2Sr2Y0.5Ca0.5Cu3F1.0031O7.2608	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3	F	1.0031									O	8-X	7.2608		1997																											3	Pb3212				5.376	5.096	15.685													45	73					73																																																																																														Y2O3,CuO,CaCO3,SrCO3,PbO,PbF2		Pb2Sr2Y0.5Ca0.5Cu3Oz was made by sintering(860C,14H)-mixed with PbO+PbF2-pellet-SIN(920C,2H in N2)-SIN(860C)-Q to RT in N2					STRUCTURE AND PROPERTIES OF SUBSTITUTION OF FLUORINE FOR APICAL OXYGEN IN Pb2Sr2Y0.5Ca0.5Cu3O8+delta SUPERCONDUCTOR			Deparment of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, P. R. China	Mod.Phys.Lett.B,11(1997)311-321	BAI-RU ZHAO,DE GAO,SHU-FEN JIANG,SHU-LIAN JIA,XIAO-HUI GAO		
7772	PHC2620021	optimal oxygen condition	HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4OZ	Hg	1	Ba	2	Ca	3	Cu	4													O	Z		1	1996																											2	Hg1234				3.852		19.01																123			123																																																																																														HgO,BaO,CaO,CuO		precursor(Ba-Ca-Cu-O)-HgO-seculed in quartz tube(0223+1223)-heat(800C,4H)-ANN(300C,30H in flowing O2)					Synthesis of HgBa2Ca3Cu4Oy under ambient pressure			Superconductivity reserch Laboratory,ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135, Japan	Physica.C,262(1996)21-26	A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi,T. Tatsuki		
7773	SCI2711255		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-X	Bi	2	Sr	2	Ca	1	Cu	2													O	8-X			1996																												Bi2212																				92					92																																															17	4.3	9																																															Ar-anneald					Doping-Induced Change of Superconducting Gap Anisotropy in Bi2Sr2Ca1Cu2O8+delta	199603		Applied superconductivity Center, University of Wisconsin, Madison, Wl 53706, USA	Science 271(1996)1255	C. Quitmann,G. Margaritondo,H. Berger,M. Onellion,P. Almeras,R.J. Kelley		
7774	SCI2711255		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8-X	Bi	2	Sr	2	Ca	1	Cu	2													O	8-X			1996																												Bi2212																				85					85																																															22	6	9																																															O2-anneald					Doping-Induced Change of Superconducting Gap Anisotropy in Bi2Sr2Ca1Cu2O8+delta	199603		Applied superconductivity Center, University of Wisconsin, Madison, Wl 53706, USA	Science 271(1996)1255	C. Quitmann,G. Margaritondo,H. Berger,M. Onellion,P. Almeras,R.J. Kelley		
7775	SST0100502		(Pb,Cd)LaSrCuO5	Pb0.5Cd0.5La1Sr1Cu1O5-Z	Pb	0.5	Cd	0.5	La	1	Sr	1	Cu	1											O	5-Z		1	1997																											2	M1201				3.757		8.89														35					35																																																																			-4				mOhm.cm											4.9														metal-EDTA complex-dry(500C, in air in muflle furnace-mixture-CAL(750-900C, 0.5-96H in air)-FC to RT					Magnetic and electrical transport properties of (Pb0.5Cd0.5)(La2-xSrx)CuO5-delta			Supercoductivity Group, BICC Cables Ltd, Technology Centre, Wrexham LL13 9XP, UK	Supercond.Sci.Technol.10(1997)502-506	J D Johnson,J M Parberry,T P Beales		
7776	SST0100502		(Pb,Cd)LaSrCuO5	Pb0.5Cd0.5La0.9Sr1.1Cu1O5-Z	Pb	0.5	Cd	0.5	La	0.9	Sr	1.1	Cu	1											O	5-Z		1	1997																											2	M1201																				12					12																																																																			-6				mOhm.cm											2.7														metal-EDTA complex-dry(500C, in air in muflle furnace-mixture-CAL(750-900C, 0.5-96H in air)-FC to RT					Magnetic and electrical transport properties of (Pb0.5Cd0.5)(La2-xSrx)CuO5-delta			Supercoductivity Group, BICC Cables Ltd, Technology Centre, Wrexham LL13 9XP, UK	Supercond.Sci.Technol.10(1997)502-506	J D Johnson,J M Parberry,T P Beales		
7777	SST0100502		(Pb,Cd)LaSrCuO5	Pb0.5Cd0.5La0.8Sr1.2Cu1O5-Z	Pb	0.5	Cd	0.5	La	0.8	Sr	1.2	Cu	1											O	5-Z		1	1997																											2	M1201																							4.2																																																																					-6.2				mOhm.cm											1.9														metal-EDTA complex-dry(500C, in air in muflle furnace-mixture-CAL(750-900C, 0.5-96H in air)-FC to RT					Magnetic and electrical transport properties of (Pb0.5Cd0.5)(La2-xSrx)CuO5-delta			Supercoductivity Group, BICC Cables Ltd, Technology Centre, Wrexham LL13 9XP, UK	Supercond.Sci.Technol.10(1997)502-506	J D Johnson,J M Parberry,T P Beales		
7778	SST0100502		(Pb,Cd)LaSrCuO5	Pb0.5Cd0.5La1.1Sr0.9Cu1O5-Z	Pb	0.5	Cd	0.5	La	1.1	Sr	0.9	Cu	1											O	5-Z		1	1997																											2	M1201																				37					37																																																																																																metal-EDTA complex-dry(500C, in air in muflle furnace-mixture-CAL(750-900C, 0.5-96H in air)-FC to RT					Magnetic and electrical transport properties of (Pb0.5Cd0.5)(La2-xSrx)CuO5-delta			Supercoductivity Group, BICC Cables Ltd, Technology Centre, Wrexham LL13 9XP, UK	Supercond.Sci.Technol.10(1997)502-506	J D Johnson,J M Parberry,T P Beales		
7779	SST0100663	211 and othor phases	(Nd,Eu,Gd)Ba2Cu3O7	Nd0.33Eu0.33Gd0.33Ba2Cu3OZ	Nd	0.33	Eu	0.33	Gd	0.33	Ba	2	Cu	3											O	Z		2	1997																																3.909	3.856	11.724																94.1			94.1																																																																																																OCMG process, mixture-preheat (950C,15H in 0.1%O2-99.9%Ar gas flow)-pellet-OCMG process, see text					Effect of mixing three rare-earth elements on the superconducting properties of REBa2Cu3Oy			International Superconductivity Technology Center,Supercoductivity Reserch Laboratory, 1-16-25, Shibaura, Minato-Ku, Tokyo 105, Japan	Supercond.Sci.Technol.10(1997)663-670	H S Chauhan,K Segawa,K. Komada,M Murakami,M. Muralidhar,T. Saitoh		
7780	SST0100663		(Nd,Sm,Gd)Ba2Cu3O7	Nd0.33Sm0.33Gd0.33Ba2Cu3OZ	Nd	0.33	Sm	0.33	Gd	0.33	Ba	2	Cu	3											O	Z		2	1997																																3.906	3.851	11.727																93.1			93.1																																																																																																OCMG process, mixture-preheat (950C,15H in 0.1%O2-99.9%Ar gas flow)-pellet-OCMG process, see text					Effect of mixing three rare-earth elements on the superconducting properties of REBa2Cu3Oy			International Superconductivity Technology Center,Supercoductivity Reserch Laboratory, 1-16-25, Shibaura, Minato-Ku, Tokyo 105, Japan	Supercond.Sci.Technol.10(1997)663-670	H S Chauhan,K Segawa,K. Komada,M Murakami,M. Muralidhar,T. Saitoh		
7781	SST0100663		(Nd,Sm,Eu)Ba2Cu3O7	Nd0.33Sm0.33Eu0.33Ba2Cu3OZ	Nd	0.33	Sm	0.33	Eu	0.33	Ba	2	Cu	3											O	Z		2	1997																																3.905	3.852	11.728																95.3			95.3																																																																																																OCMG process, mixture-preheat (950C,15H in 0.1%O2-99.9%Ar gas flow)-pellet-OCMG process, see text					Effect of mixing three rare-earth elements on the superconducting properties of REBa2Cu3Oy			International Superconductivity Technology Center,Supercoductivity Reserch Laboratory, 1-16-25, Shibaura, Minato-Ku, Tokyo 105, Japan	Supercond.Sci.Technol.10(1997)663-670	H S Chauhan,K Segawa,K. Komada,M Murakami,M. Muralidhar,T. Saitoh		
7782	SST0100663		(Sm,Eu,Gd)Ba2Cu3O7	Sm0.33Eu0.33Gd0.33Ba2Cu3OZ	Sm	0.33	Eu	0.33	Gd	0.33	Ba	2	Cu	3											O	Z		2	1997																																3.901	3.85	11.711																93.1			93.1																																																																																																OCMG process, mixture-preheat (950C,15H in 0.1%O2-99.9%Ar gas flow)-pellet-OCMG process, see text					Effect of mixing three rare-earth elements on the superconducting properties of REBa2Cu3Oy			International Superconductivity Technology Center,Supercoductivity Reserch Laboratory, 1-16-25, Shibaura, Minato-Ku, Tokyo 105, Japan	Supercond.Sci.Technol.10(1997)663-670	H S Chauhan,K Segawa,K. Komada,M Murakami,M. Muralidhar,T. Saitoh		
7783	MPL0110323		LaCaBaCu3O7	La1Ca1Ba1Cu3O7	La	1	Ca	1	Ba	1	Cu	3													O	7			1997																											2	Y123				3.869		11.645																69			69																																																																																														Pr6O11,La2O3,BaCO3,CaCO3,CuO	1	mixture-heart(975C-995C)-SIN(975-995C)-ANN(575C, 24H)					SUPERCONDUCTIVITY AND MAGNETIC ORDERING OF Pr IN CaLa1-xPrxBaCu3O7 SYSTEM			Depto. de Fisica, Univ. federal de Pernambuco, 50670-901, Recife, RE, Brasil	Mod.Phys.Lett.B,11(1997)323-331	A.V. NARLIKAR,D.A. LANDINES TELLEZ,E. GMERIN,J. ALBINKO AGUIAR,J.M. FERREIRA,RAJVIR SINGH,S. UMA,V.P.S. AWANA		
7784	MPL0110323		(La,Ca)CaBaCu3O7	La0.7Pr0.3Ca1Ba1Cu3O7	La	0.7	Pr	0.3	Ca	1	Ba	1	Cu	3											O	7			1997		0.00039		1.55		3.51	-14.4																				2	Y123				3.866		11.632																40			40																																																																																														Pr6O11,La2O3,BaCO3,CaCO3,CuO	1	mixture-heart(975C-995C)-SIN(975-995C)-ANN(575C, 24H)					SUPERCONDUCTIVITY AND MAGNETIC ORDERING OF Pr IN CaLa1-xPrxBaCu3O7 SYSTEM			Depto. de Fisica, Univ. federal de Pernambuco, 50670-901, Recife, RE, Brasil	Mod.Phys.Lett.B,11(1997)323-331	A.V. NARLIKAR,D.A. LANDINES TELLEZ,E. GMERIN,J. ALBINKO AGUIAR,J.M. FERREIRA,RAJVIR SINGH,S. UMA,V.P.S. AWANA		
7785	MPL0110323		(La,Ca)CaBaCu3O7	La0.3Pr0.7Ca1Ba1Cu3O7	La	0.3	Pr	0.7	Ca	1	Ba	1	Cu	3											O	7			1997		0.00096		1.19		3.07	-17.8	4																			2	Y123				3.872		11.621																	4.2																																																																																																Pr6O11,La2O3,BaCO3,CaCO3,CuO	1	mixture-heart(975C-995C)-SIN(975-995C)-ANN(575C, 24H)					SUPERCONDUCTIVITY AND MAGNETIC ORDERING OF Pr IN CaLa1-xPrxBaCu3O7 SYSTEM			Depto. de Fisica, Univ. federal de Pernambuco, 50670-901, Recife, RE, Brasil	Mod.Phys.Lett.B,11(1997)323-331	A.V. NARLIKAR,D.A. LANDINES TELLEZ,E. GMERIN,J. ALBINKO AGUIAR,J.M. FERREIRA,RAJVIR SINGH,S. UMA,V.P.S. AWANA		
7786	MPL0110323		(La,Ca)CaBaCu3O7	Pr1Ca1Ba1Cu3O7	Pr	1	Ca	1	Ba	1	Cu	3													O	7			1997		0.00041		1.46		3.4	-27.4	8																			2	Y123				3.875		11.603																	4.2																																																																																																Pr6O11,La2O3,BaCO3,CaCO3,CuO	1	mixture-heart(975C-995C)-SIN(975-995C)-ANN(575C, 24H)					SUPERCONDUCTIVITY AND MAGNETIC ORDERING OF Pr IN CaLa1-xPrxBaCu3O7 SYSTEM			Depto. de Fisica, Univ. federal de Pernambuco, 50670-901, Recife, RE, Brasil	Mod.Phys.Lett.B,11(1997)323-331	A.V. NARLIKAR,D.A. LANDINES TELLEZ,E. GMERIN,J. ALBINKO AGUIAR,J.M. FERREIRA,RAJVIR SINGH,S. UMA,V.P.S. AWANA		
7787	JMR0122866	behaviour of Jc(H) depends on the heat treatment, Some showed peak efect	NdBa2cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	7		3	1997																												Y123																						96			96																																																																																																TSSG method, cuptal was grown  in P(O2)=0.01 atm. Then annealed at 340C for 200H, furnace cool to RT					Fabrication of NdBCO single crystal oxide superconductor with enhanced superconductive properties			Departament of Metallurgy, Graduate School of Engineering, The University of Tokyo,7-3-1, Hongo, Bunkyo-ku, Tokyo 113, Japan	J.Mater.Res.12(1997)2866	M. Kambara,M. Nakamura,T. Umeda,X. Yao,Y, Shiohara		
7788	JMR0122526		(Pr,Ce,Sr)2CuO4	Pr1.79Ce0.15Sr0.06Cu1O3.94	Pr	1.79	Ce	0.15	Sr	0.06	Cu	1													O	4+Z	3.94		1997																												T'				3.96		12.16														21					21																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7789	JMR0122526		(Pr,Ce,Sr)2CuO4	Pr1.74Ce0.15Sr0.11Cu1O3.96	Pr	1.74	Ce	0.15	Sr	0.11	Cu	1													O	4+Z	3.96		1997																												T'																				18					18																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7790	JMR0122526		(Pr,Ce)2CuO4	Pr1.9Ce0.1Cu1O3.98	Pr	1.9	Ce	0.1	Cu	1															O	4	3.98		1997																												T'																				9					9																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7791	JMR0122526		(Pr,Ce)2CuO4	Pr1.87Ce0.13Cu1O3.99	Pr	1.87	Ce	0.13	Cu	1															O	4	3.99		1997																												T'																				16					16																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7792	MPL0110593		EuBa2Cu3O7	Eu1Ba2Cu3O7-Z	Eu	1	Ba	2	Cu	3															O	7-Z			1997																												Y123				3.8268																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7793	MPL0110593		(Eu,Ga)Ba2Cu3O7	Eu0.09Ga0.01Ba2Cu3O7-Z	Eu	0.09	Ga	0.01	Ba	2	Cu	3													O	7-Z			1997																												Y123				3.8321																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7794	MPL0110593		(Eu,Ga)Ba2Cu3O7	Eu0.08Ga0.02Ba2Cu3O7-Z	Eu	0.08	Ga	0.02	Ba	2	Cu	3													O	7-Z			1997																												Y123				3.8362																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7795	MPL0110593		(Eu,Ga)Ba2Cu3O7	Eu0.07Ga0.03Ba2Cu3O7-Z	Eu	0.07	Ga	0.03	Ba	2	Cu	3													O	7-Z			1997																												Y123				3.8403																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7796	MPL0110593		(Eu,Ga)Ba2Cu3O7	Eu0.04Ga0.06Ba2Cu3O7-Z	Eu	0.04	Ga	0.06	Ba	2	Cu	3													O	7-Z			1997																												Y123				3.8504																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7797	MPL0110593		(Eu,Ga)Ba2Cu3O7	Eu0.01Ga0.09Ba2Cu3O7-Z	Eu	0.01	Ga	0.09	Ba	2	Cu	3													O	7-Z			1997																												Y123				3.8605																																																																																																																					mixture-CAL(1073K,4H in air)-pellet-SIN(1223K,7Hin O2)-cool to 773K(3K/min)-hold(773K, 1H)-FC					STRUCTURAL AND MAGNETIC CHARACTERISTICS OF (Eu1-xCax)Ba2Cu3O7-delta HIGH-Tc SUPERCONDUCTORS			%aBabes-Boyai%a University, Faculty of Physics, Kogalniceanu 1, Cluj-Nopoca, 3400, Romania	Mod.Phys.Lett.B,11(1997)593-597	GHEORGHE BORODI,IULIU POP,RADU REDAC,VIRGIL IONCU		
7798	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.03C0.96H0.48N0.24Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.03	C	0.96	H	0.48	N	0.24					O	z			1994																												Bi2212																					61.6				61.6																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7799	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.035C1.12H0.56N0.28Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.035	C	1.12	H	0.56	N	0.28					O	z			1994																												Bi2212																					60.6				60.6																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7800	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.05C1.6H0.8N0.4Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.05	C	1.6	H	0.8	N	0.4					O	z			1994																												Bi2212																					55.5				55.5																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7801	MPL0080251		(ZnPc)Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Zn0.067C2.144H1.072N0.536Oz	Bi	2	Sr	2	Ca	1	Cu	2	Zn	0.067	C	2.144	H	1.072	N	0.536					O	z			1994																												Bi2212																					45.3				45.3																																																																																																Pc=C32H16N8,ZnPc molecule were intercalated by varying exposure time, single crystal+ZnPc in sealed Pyrex tube-heat(490C)					CONTRIBUTION OF INTERBLOCK COUPLING TO Tc IN HIGH-Tc BI OXDES			Institute for Molecular Science, Myodaiji, Okazaki 444, Japan	Mod.Phys.Lett.B 8(1994)251-259	A.V. NARLIKAR,K. YASUSHI,L. GRIGORYAN,S.B. SAMANTHA		
7802	JMR0122526		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O3.98	Pr	1.85	Ce	0.15	Cu	1															O	4	3.98		1997																												T'																				18					18																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7803	JMR0122526		(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O3.99	Pr	1.83	Ce	0.17	Cu	1															O	4	3.99		1997																												T'																				13					13																																																																																																see text					Phase indentification and superconductivity transitions in Sr-doped Pr1.85Ce0.15CuO4+delta			Departament de Quimica Inorganica, Facultad de Quimicas, Universidad Complutense, 28040 Madrid, Spain	J.Mater.Res.12(1997)2526	A. Varela,J.M. Gonza'les-Calbet,M. Vallet-Regi'		
7804	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.06	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.06		1997																											3	Y123				3.889	3.825	11.638														48.9					48.9										7																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7805	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.16	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.16		1997																											3	Y123				3.882	3.839	11.632														61.7					61.7										11																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7806	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.26	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.26		1997																											3	Y123				3.876	3.846	11.625														67.6					67.6										14																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7807	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.36	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.36		1997																											3	Y123				3.863	3.851	11.608														89.1					89.1										19																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7808	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.46	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.46		1997																											2	Y123				3.86		11.608														89.8					89.8										19																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7809	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.49	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.49		1997																											2	Y123				3.86		11.595														90.4					90.4										20																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7810	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.57	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.57		1997																											2	Y123				3.861		11.595														89.6					89.6										21																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7811	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.62	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.62		1997																											2	Y123				3.86		11.595														87.9					87.9										25																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7812	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.64	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.64		1997																											2	Y123				3.862		11.601														88.1					88.1										26																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7813	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.74	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.74		1997																											2	Y123				3.861		11.597														89.1					89.1										26																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7814	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.77	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.77		1997																											2	Y123				3.866		11.595														89.8					89.8										26																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7815	JJP0360473		Y(La,Ba)2Cu3Oz	Y1La0.2Ba1.8Cu3O7.79	Y	1	La	0.2	Ba	1.8	Cu	3													O	z	7.79		1997																											2	Y123				3.86		11.59														90.4					90.4										27																																																																																						pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7816	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.2	La	1.2	Ba	1.8	Cu	3															O	z	7.2		1997																											3	Y123				3.924	3.913	11.745														27					27																																																																																																pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7817	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.3	La	1.2	Ba	1.8	Cu	3															O	z	7.3		1997																											3	Y123				3.927	3.918	11.741														27					27																																																																																																pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7818	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.35	La	1.2	Ba	1.8	Cu	3															O	z	7.35		1997																											3	Y123				3.93	3.917	11.717																	4.2																																																																																																		pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7819	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.4	La	1.2	Ba	1.8	Cu	3															O	z	7.4		1997																											3	Y123				3.933	3.922	11.711																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7820	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.45	La	1.2	Ba	1.8	Cu	3															O	z	7.45		1997																											3	Y123				3.928	3.917	11.726																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7821	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.5	La	1.2	Ba	1.8	Cu	3															O	z	7.5		1997																											3	Y123				3.925	3.913	11.745																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7822	JJP0360473		La(Ba,La)2Cu3O8	La1.2Ba1.8Cu3O7.6	La	1.2	Ba	1.8	Cu	3															O	z	7.6		1997																											3	Y123				3.925	3.913	11.74																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7823	JJP0360473		La(Ba,La)2Cu3O8	La1.2Ba1.8Cu3O7.7	La	1.2	Ba	1.8	Cu	3															O	z	7.7		1997																											3	Y123				3.924	3.914	11.715																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7824	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.8	La	1.2	Ba	1.8	Cu	3															O	z	7.8		1997																											3	Y123				3.925	3.921	11.716																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7825	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.9	La	1.2	Ba	1.8	Cu	3															O	z	7.9		1997																											2	Y123				3.925		11.704																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7826	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O7.98	La	1.2	Ba	1.8	Cu	3															O	z	7.98		1997																											2	Y123				3.929		11.704																																																																																																																			pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7827	JJP0360473		La(Ba,La)2Cu3Oz	La1.2Ba1.8Cu3O8	La	1.2	Ba	1.8	Cu	3															O	z	8		1997																											2	Y123				3.935	11.698																																																																																																																				pellet+KClO4-capsuled in Au tube-heat (1150C,2H,5.5 Pa)					Tc of Overdoped YLa0.2Ba1.8Cu3O7.06+y and La1.2Ba1.8Cu3O7.2+y	199704		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)473-475	Bin OKAI,Katsuo KATO		
7828	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7		1997																											3	Y123				3.898	3.834	11.673														58.7					58.7																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7829	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.1	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.1		1997																											3	Y123				3.896	3.841	11.665														57.6					57.6																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7830	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.2	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.2		1997																											3	Y123				3.891	3.846	11.654														63.3					63.3																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7831	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.3	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.3		1997																											3	Y123				3.873	3.861	11.638														62.6					62.6																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7832	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.4	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.4		1997																											2	Y123				3.87		11.635														59.8					59.8																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7833	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.5	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.5		1997																											2	Y123				3.868		11.641														62.9					62.9																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7834	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.55	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.55		1997																											2	Y123				3.869		11.639														68.3					68.3																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7835	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.6	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.6		1997																											2	Y123				3.87		11.637														66.5					66.5																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7836	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.65	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.65		1997																											2	Y123				3.873		11.629														66.5					66.5																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7837	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.67	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.67		1997																											2	Y123				3.868		11.631														67.5					67.5																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7838	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O7.79	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	7.79		1997																											2	Y123				3.868		11.629														65.4					65.4																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7839	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O8.04	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	8.04		1997																											2	Y123				3.873		11.627														64.4					64.4																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7840	JJP0361374		(Y,Pr)Ba2Cu3Oz	Y0.8Pr0.2Ba2Cu3O8.06	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7+z	8.06		1997																											2	Y123				3.875		11.623														65.8					65.8																																																																																																see text					High-Oxygen-Pressure Synthesis of Superconducting Y0.8Pr0.2Ba2Cu3O8	199710		Faculty of General Education, Kogakuin University, 1-24-2 Nishi-Shinjuku, Tokyo 163-91, Japan	Japanese J.Appl.Phys.Lett.36(1997)1374-1375	Bin OKAI,Katsuo KATO		
7841	JSC1270064			Pb1.75Ca0.2Y1Sr2Cu3O8+z	Pb	1.75	Ca	0.2	Y	1	Sr	2	Cu	3											O	8+z			1996																																																		45			45																																																																																																precursor(Sr-Ca-Y-Cu-O)+PbO+Cr2O3-mix-almina crucible-sealed in sill ca tube (10E-2Torr)-heat(1173K,10H)-Q to RT					Substitution of Chromium for Univalent Copper in Superconducting Pb2Sr2(Ca,Y)Cu3O8+delta			Laboratoire CRISMAT, CNRS URA 1318, ISMRA et Universite' de Caen, Bd. du Marechal Juin, 14050 Caen Cedex, France	J.Soild State Chem.127(1996)64-71	A. Maignan,B. Raveau,C. Martin,M. Hervieu,R. Seshadri		
7842	JSC1270064			Pb1.75Ca0.2Y1Sr2Cu2.85Cr0.15O8+z	Pb	1.75	Ca	0.2	Y	1	Sr	2	Cu	2.85	Cr	0.15									O	8+z			1996																													Cmmm			5.386	5.42	15.72																35			35																																																																																																precursor(Sr-Ca-Y-Cu-O)+PbO+Cr2O3-mix-almina crucible-sealed in sill ca tube (10E-2Torr)-heat(1173K,10H)-Q to RT					Substitution of Chromium for Univalent Copper in Superconducting Pb2Sr2(Ca,Y)Cu3O8+delta			Laboratoire CRISMAT, CNRS URA 1318, ISMRA et Universite' de Caen, Bd. du Marechal Juin, 14050 Caen Cedex, France	J.Soild State Chem.127(1996)64-71	A. Maignan,B. Raveau,C. Martin,M. Hervieu,R. Seshadri		
7843	JSC1270064			Pb1.75Ca0.2Y0.8Sr2Cu3O8+z	Pb	1.75	Ca	0.2	Y	0.8	Sr	2	Cu	3											O	8+z			1996																																																		75			75																																																																																																precursor(Sr-Ca-Y-Cu-O)+PbO+Cr2O3-mix-almina crucible-sealed in sill ca tube (10E-2Torr)-heat(1173K,10H)-Q to RT					Substitution of Chromium for Univalent Copper in Superconducting Pb2Sr2(Ca,Y)Cu3O8+delta			Laboratoire CRISMAT, CNRS URA 1318, ISMRA et Universite' de Caen, Bd. du Marechal Juin, 14050 Caen Cedex, France	J.Soild State Chem.127(1996)64-71	A. Maignan,B. Raveau,C. Martin,M. Hervieu,R. Seshadri		
7844	JSC1270064			Pb1.75Ca0.2Y0.8Sr2Cu2.85Cr0.15O8+z	Pb	1.75	Ca	0.2	Y	0.8	Sr	2	Cu	2.85	Cr	0.15									O	8+z			1996																																																		65			65																																																																																																precursor(Sr-Ca-Y-Cu-O)+PbO+Cr2O3-mix-almina crucible-sealed in sill ca tube (10E-2Torr)-heat(1173K,10H)-Q to RT					Substitution of Chromium for Univalent Copper in Superconducting Pb2Sr2(Ca,Y)Cu3O8+delta			Laboratoire CRISMAT, CNRS URA 1318, ISMRA et Universite' de Caen, Bd. du Marechal Juin, 14050 Caen Cedex, France	J.Soild State Chem.127(1996)64-71	A. Maignan,B. Raveau,C. Martin,M. Hervieu,R. Seshadri		
7845	JSC1270056	fully oxygenated	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		1	1996																											3	Y123				3.814	3.881	11.67															90.1				90.1																																																																																																ANN(400C,2 days or longer, in O2)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7846	JSC1270056	fully oxygenated	(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3Oz	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z		1	1996																											3	Y123				3.817	3.878	11.679															85.2				85.2																																																																																																ANN(400C,2 days or longer, in O2)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7847	JSC1270056	fully oxygenated	(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3Oz	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	z		1	1996																											3	Y123				3.825	3.879	11.693															80.9				80.9																																																																																																ANN(400C,2 days or longer, in O2)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7848	JSC1270056	partially oxidiqed	YBa2Cu3Oz	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		1	1996																											3	Y123				3.828	3.881	11.723															63.1				63.1																																																																																																heat (900C in air)-cool to 520C (180C/h)-ANN(520C, 3 days, in 2% O2-Ar gas)-Q to LN2					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7849	JSC1270056	partially oxidiqed	(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.5	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.5	1	1996																											3	Y123				3.834	3.878	11.745															79.3				79.3																																																																																																heat (900C in air)-cool to 520C (180C/h)-ANN(520C, 3 days, in 2% O2-Ar gas)-Q to LN2					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7850	JSC1270056	partially oxidiqed	(Y,Ca)Ba2Cu3O3	Y0.8Ca0.2Ba2Cu3Oz	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	z		1	1996																											3	Y123				3.839	3.868	11.764															77.5				77.5																																																																																																heat (900C in air)-cool to 520C (180C/h)-ANN(520C, 3 days, in 2% O2-Ar gas)-Q to LN2					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7851	JSC1270056	partially oxidiqed	(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.5	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	z	6.5	1	1996																																																	84.8				84.8																																																																																																heat (900C in air)-cool to 520C (180C/h)-ANN(520C, 3 days, in 2% O2-Ar gas)-Q to LN2					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7852	JSC1270056	fully reduced	YBa2Cu3Oz	Y1Ba2Cu3O6.03	Y	1	Ba	2	Cu	3															O	z	6.03	1	1996																											2	Y123				3.859		11.827																	10																																																																																																	1	ANN(640C, in Ar)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7853	JSC1270056	fully redused	(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.03	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.03	1	1996																											2	Y123				3.857		11.835															19.8				19.8																																																																																															1	ANN(640C, in Ar)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7854	JSC1270056	fully reduced	(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.03	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	z	6.03	1	1996																											2	Y123				3.854		11.83															43.5				43.5																																																																																															1	ANN(640C, in Ar)					A Neutron Diffraction Study of Ca Doped and Oxygen Deficient YBa2Cu3O7-delta			Department of Inorganic Chemistry, Chalmers University of Technology and University of Goteborg, Sweden	J.Solid State Chem.127(1996)56-63	H. Mazaki,L.G. Johansson,M. Kakihana,M. Osada,P. Berastegui,S. Tochihara,S.-G. Eriksson		
7855	APJ0366306	91% Hg1212	(Hg,V)Sr2(Ca,Nd)Cu2Oz	Hg0.65V0.35Sr2Ca0.45Nd0.55Cu2Oz	Hg	0.65	V	0.35	Sr	2	Ca	0.45	Nd	0.55	Cu	2									O	z		2	1997																											2																				30		80				55																																																																																																Precursor(V0.35Sr2(Ca,Nd)Cu2Oz)+(Hg,V)Sr2(Ca,Nd)Cu2Oz pellet-sealed in evacuated silica tube-heat(850C,10H)-RT(in 10H)-ANN(350C,24H in O2-flow)-Q to RT					Synthesis, Structure and Superconductivity of (Hg0.65V0.35)Sr2(Ca1-xNdx)Cu2Oz	10		Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Japanese J. Appl.Phys.36(1997)6306-6310	Elsayed KANDYEL,Hajime ASANO,Morsy ABOU-SEKKINA,Saiid AMER,Takashi KAMIYAMA		
7856	APJ0366306	94% Hg1212	(Hg,V)sr2(Ca,Nd)Cu2Oz	Hg0.65V0.35Sr2Ca0.55Nd0.45Cu2O6.8	Hg	0.65	V	0.35	Sr	2	Ca	0.55	Nd	0.45	Cu	2									O	z	6.8	2	1997																											2																				38		96				67																																																																																																Precursor(V0.35Sr2(Ca,Nd)Cu2Oz)+(Hg,V)Sr2(Ca,Nd)Cu2Oz pellet-sealed in evacuated silica tube-heat(850C,10H)-RT(in 10H)-ANN(350C,24H in O2-flow)-Q to RT					Synthesis, Structure and Superconductivity of (Hg0.65V0.35)Sr2(Ca1-xNdx)Cu2Oz	10		Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Japanese J. Appl.Phys.36(1997)6306-6310	Elsayed KANDYEL,Hajime ASANO,Morsy ABOU-SEKKINA,Saiid AMER,Takashi KAMIYAMA		
7857	APJ0366306	90% Hg1212	(Hg,V)Sr2(Ca,Nd)Cu2Oz	Hg0.65V0.35Sr2Ca0.65Nd0.35Cu2Oz	Hg	0.65	V	0.35	Sr	2	Ca	0.65	Nd	0.35	Cu	2									O	z		2	1997																											2																				58		105				81.5																																																																																																Precursor(V0.35Sr2(Ca,Nd)Cu2Oz)+(Hg,V)Sr2(Ca,Nd)Cu2Oz pellet-sealed in evacuated silica tube-heat(850C,10H)-RT(in 10H)-ANN(350C,24H in O2-flow)-Q to RT					Synthesis, Structure and Superconductivity of (Hg0.65V0.35)Sr2(Ca1-xNdx)Cu2Oz	10		Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Japanese J. Appl.Phys.36(1997)6306-6310	Elsayed KANDYEL,Hajime ASANO,Morsy ABOU-SEKKINA,Saiid AMER,Takashi KAMIYAMA		
7858	APJ0366306	79% Hg1212	(Hg,V)Sr2(Ca,Nd)Cu2Oz	Hg0.65V0.35Sr2Ca0.75Nd0.25Cu2Oz	Hg	0.65	V	0.35	Sr	2	Ca	0.75	Nd	0.25	Cu	2									O	z		2	1997																											2																				75		103				89																																																																																																Precursor(V0.35Sr2(Ca,Nd)Cu2Oz)+(Hg,V)Sr2(Ca,Nd)Cu2Oz pellet-sealed in evacuated silica tube-heat(850C,10H)-RT(in 10H)-ANN(350C,24H in O2-flow)-Q to RT					Synthesis, Structure and Superconductivity of (Hg0.65V0.35)Sr2(Ca1-xNdx)Cu2Oz	10		Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki 305, Japan	Japanese J. Appl.Phys.36(1997)6306-6310	Elsayed KANDYEL,Hajime ASANO,Morsy ABOU-SEKKINA,Saiid AMER,Takashi KAMIYAMA		
7859	PHC2890153	befor fluorination	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1997																											2	Hg1201				3.881		9.522																91			91																																																																																															1	mixture-pellet-wrapped in Ag foil-seal in quartz tube in air-heat(650+800C,10H)					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7860	PHC2890153	before fluorination	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			1997																											2	Hg1201				3.921		9.611																35			35																																																																																																prepared under reducing condition					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7861	PHC2890153	befor fluorination	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z			1997																											2	Hg1212				3.87		12.721																120			120																																																																																															1	mixture-pellet-wrapped in Ag foil-seal in quartz tube in air-heat(650+800C,10H)					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7862	PHC2890153	befor fluorination	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1997																											2	Hg1223				3.855		15.826																115			115																																																																																															1	mixture-pellet-wrapped in Ag foil-seal in quartz tube in air-heat(650+800C,10H)					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7863	PHC2890153	F-content was nit determined	HgBa2Cu(O,F)4	Hg1Ba2Cu1FO4+z	Hg	1	Ba	2	Cu	1	F														O	4+z			1997																											2	Hg1201				3.862		9.472															97				97																																																																																															1	prepured under reducing condition+fluorinated by F2 gas flow					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7864	PHC2890153	F-Content was not determined	HgBa2Cu(O,F)4	Hg1Ba2Cu1FO4+z	Hg	1	Ba	2	Cu	1	F														O	4+z			1997																											2	Hg1201				3.64		9.453															97				97																																																																																															1	prepured under reducing condition+fluorinated by F2 gas flow					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7865	PHC2890153	F-content was not determined	HgBa2CaCu2(O,F)6	Hg1Ba2Ca1Cu2FO6+z	Hg	1	Ba	2	Ca	1	Cu	2	F												O	6+z			1997																											2	Hg1212				3.847		12.604															128				128																																																																																																prepured under reducing condition+fluorinated by CuF2 and AgF2					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7866	PHC2890153	F-content was not determined	HgBa2Ca2Cu3(O,F)8	Hg1Ba2Ca2Cu3FO8+z	Hg	1	Ba	2	Ca	2	Cu	3	F												O	8+z			1997																											2	Hg1223				3.848		15.792															135				135																																																																																																prepured under reducing condition+fluorinated by CuF2 and AgF2					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7867	PHC2890153		HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z			1997																												Hg1234																						111			111																																																																																																high pressure synthesis, precursor(Ba2Ca3Cu4Oz)+HgO,CaO,CuO-mixture-in Au capsile-pressure(18Kbar)-heat(920C,4H)-FC to RT					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7868	PHC2890153		HgBa2Ca3Cu4(O,F)z	Hg1Ba2Ca3Cu4FOz	Hg	1	Ba	2	Ca	3	Cu	4	F												O	z			1997																												Hg1234																						114			114																																																																																																prepured under reducing condition+fluorination using CuF2					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7869	PHC2890153	85% Hg1245, 15% Hg1234	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z			1997																												Hg1245																						98			98																																																																																																high pressure synthesis, precursor(Ba2Ca3Cu4Oz)+HgO,CaO,CuO-mixture-in Au capsile-pressure(18Kbar)-heat(920C,4H)-FC to RT					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7870	PHC2890153	85% Hg1245, 15% Hg1234	HgBa2Ca4Cu5(O,F)z	Hg1Ba2Ca4Cu5FOz	Hg	1	Ba	2	Ca	4	Cu	5	F												O	z			1997																												Hg1245																						109			109																																																																																																prepured under reducing condition+fluorination using CuF2					Fluorination of mercury-based high-temperature superconductors	199710		School of Chemistry, University of Biermingham, Edgbaston, Birmingham B15 2TT, UK	Physica.C,289(1997)153-160	G.B. Peacock,I. Gameson,J.J. Capponi,M. Slaski,P.P. Edwards		
7871	APL0712370		TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9	Tl	1	Ba	2	Ca	2	Cu	3													O	9		1	1997																											2	Tl1223				3.853		15.913																110			110																																																																																															1	mixture-alumina crueible-quartz tube(10E-2 Torr)-heat(820-850C,5H and hold 4-6H)-slow cool to RT					Significantly enhanced flux pinning in the Bi-substituted TlBa2Ca2Cu3Oy system	10		Department of Physics, Campus Box 390, University of Colorado, Boulder, Colorado 80309-0390	Appl.Phys.Lett.71(1997)2370	A.M. Hermann,V. Badri,Y.T. Wang		
7872	APL0712370		(Tl,Bi)Ba2Ca2Cu3O9	Tl0.8Bi0.2Ba2Ca2Cu3O9	Tl	0.8	Bi	0.2	Ba	2	Ca	2	Cu	3											O	9		1	1997																											2	Tl1223				3.846		15.816																116			116																																																																																															1	mixture-alumina crueible-quartz tube(10E-2 Torr)-heat(820-850C,5H and hold 4-6H)-slow cool to RT					Significantly enhanced flux pinning in the Bi-substituted TlBa2Ca2Cu3Oy system	10		Department of Physics, Campus Box 390, University of Colorado, Boulder, Colorado 80309-0390	Appl.Phys.Lett.71(1997)2370	A.M. Hermann,V. Badri,Y.T. Wang		
7873	JSC1270315	(Ca2CuO2Cl2)m(Gd2Ca2Cu2O6Cl2)n not s/c	Ca4Gd2Cu3O8Cl4	Ca4Gd2Cu3Cl4O8	Ca	4	Gd	2	Cu	3	Cl	4													O	8		1	1996																											2		I4/mmm			3.886		41.827																																																																																																																			precursor-mixture-alumine crucible-CAL(700C,2H in air)-press-SIN(750C or  800C, 12H)					New Copper Oxychlorides Ca4Ln2Cu3O8Cl4, First Members of the Intergrowth Series (Ca2O2Cl2)m(Ln2Ca2Cu2O6Cl2)n(Ln=Gd,Sm)			Laboratoire CRISMAT, ISMRA et Universite' de Caen, URA 1318 associee' au CNRS, Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	J.Solid State Chem.127(1996)315-324	A. Sundaresan,B. Raveau,C. Michel,D. Pelloquin,M. Hervieu		
7874	JSC1270315	(Ca2CuO2Cl2)m(SmCa2Cu2O6Cl2)n not s/c	Ca4Sm2Cu3O8Cl4	Ca4Sm2Cu3Cl4O8	Ca	4	Sm	2	Cu	3	Cl	4													O	8		1	1996																											2		I4/mmm			3.888		41.825																																																																																																																			precursor-mixture-alumine crucible-CAL(700C,2H in air)-press-SIN(750C or  800C, 12H)					New Copper Oxychlorides Ca4Ln2Cu3O8Cl4, First Members of the Intergrowth Series (Ca2O2Cl2)m(Ln2Ca2Cu2O6Cl2)n(Ln=Gd,Sm)			Laboratoire CRISMAT, ISMRA et Universite' de Caen, URA 1318 associee' au CNRS, Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	J.Solid State Chem.127(1996)315-324	A. Sundaresan,B. Raveau,C. Michel,D. Pelloquin,M. Hervieu		
7875	JP00900307		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1997																												Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7876	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7877	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7-z	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7878	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.25Fe0.45O7-z	Y	1	Ba	2	Cu	2.25	Fe	0.45													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7879	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.4Fe0.6O7-z	Y	1	Ba	2	Cu	2.4	Fe	0.6													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7880	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.25Fe0.75O7-z	Y	1	Ba	2	Cu	2.25	Fe	0.75													O	7-z			1997																																																																																																																																																			Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7881	JP00900307		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.1Fe0.9O7-z	Y	1	Ba	2	Cu	2.1	Fe	0.9													O	7-z			1997																																																																																																																																																			Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7882	JP00900307		YBa2(Cu,Co)3O7	Y1Ba2Cu2.85Co0.15O7-z	Y	1	Ba	2	Cu	2.85	Co	0.15													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7883	JP00900307		YBa2(Cu,Co)3O7	Y1Ba2Cu2.7Co0.3O7-z	Y	1	Ba	2	Cu	2.7	Co	0.3													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7884	JP00900307		YBa2(Cu,Co)3O7	Y1Ba2Cu2.55Co0.45O7-z	Y	1	Ba	2	Cu	2.55	Co	0.45													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7885	JP00900307		YBa2(Cu,Co)3O7	Y1Ba2Cu2.4Co0.6O7-z	Y	1	Ba	2	Cu	2.4	Co	0.6													O	7-z		1	1997																											2	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7886	JP00900307		YBa2(Cu,Ni)3Oz	Y1Ba2Cu2.925Ni0.075O7-z	Y	1	Ba	2	Cu	2.925	Ni	0.075													O	7-z		1	1997																											3	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7887	JP00900307		YBa2(Cu,Ni)3Oz	Y1Ba2Cu2.85Ni0.15O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	7-z		1	1997																											3	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7888	JP00900307		YBa2(Cu,Ni)3Oz	Y1Ba2Cu2.775Ni0.225O7-z	Y	1	Ba	2	Cu	2.775	Ni	0.225													O	7-z		1	1997																											3	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7889	JP00900307		YBa2(Cu,Ni)3Oz	Y1Ba2Cu2.7Ni0.3O7-z	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	7-z		1	1997																											3	Y123																																																																																																																							Fe2O3, Y2O3, BaCO3, CuO		mixture-SIN(925-1000C,2days in air)-wrapped in Au-foil-SIN(915C,24H in 27MPa O2)-slow cool to RT(1C/min)					Metal (M) dopant centred local structures, high-pressure synthesis and bulk superconductivity in YBa2(Cu1-xMx)3O7-delta: M =Fe, Co, Ni			Department of Electrical, Computer Engineering and Computer Science, University of Cincinnati, OH 45221-0030, USA	J.Phys.:Cond.Matter9(1997)307-313	D McDaniel,F Shi,P Boolchand,R Harris,W J Bresser		
7890	NAT3640315		Sr2Cu3	Sr2Cu1O3.1	Sr	2	Cu	1																	O	3.1	3.1	1	1993																											2	T				3.764		12.548																70			70										22																																																																																				Sr2CuO3,CuO		(mixture+K Cl O4)-Au capeule-pressure(6GPa)-heat(1073-1173K,30min)-400K-RT					A new family of copper oxide superconductors Srn+1CunO2n+1+delta stabilized at high pressure	7		Institute for Chemical Research, Kyoto Univercity, Uji, Kyoto-fu 611, Japan	Nature 364(1993)315-317	M. Azuma,M. Takano,Y. Takeda,Z. Hiroi		
7891	NAT3640315		Sr3Cu2O5	Sr3Cu2O5+z	Sr	3	Cu	2																	O	5+z			1993																											2					3.9		21																100			100										4																																																																																				Sr2CuO3,CuO		(mixture+K Cl O4)-Au capeule-pressure(6GPa)-heat(1073-1173K,30min)-400K-RT					A new family of copper oxide superconductors Srn+1CunO2n+1+delta stabilized at high pressure	7		Institute for Chemical Research, Kyoto Univercity, Uji, Kyoto-fu 611, Japan	Nature 364(1993)315-317	M. Azuma,M. Takano,Y. Takeda,Z. Hiroi		
7892	PRL0712315		Bi2Sr2CuOz	Bi2Sr2Cu1Oz	Bi	2	Sr	2	Cu	1															O	z			1993																												Bi2201																			12		19				15.5																					WHH fitting						3.8						0.29						55																																																														Anomalous Temperature Dependence of the Upper Critical Magnetic Field in Bi-Sr-Cu-O	10		Naval Research Laboratory, Washington, D.C. 20375-5000	Phys.Rev.Lett.,71(1993)2315	G. Coffe,G.F. Virshup,H. Rakoto,I. Bozovic,J.C. Ousset,J.M. Broto,J.N. Eckstein,Jr.,S.A. Wolf,M.S. Osofsky,P. Pari,R.J. Soulen,S. Askenazy		
7893	PHC2980066	all nost single phase	YBa2Cu3Oz	Y1Ba2Cu3O8	Y	1	Ba	2	Cu	3															O	8		1	1998																											3	Y123				3.826	3.887	11.682													92		95.5	93			93																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7894	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.95Nd0.05Cu3Oz	Y	1	Ba	1.95	Nd	0.05	Cu	3													O	z		1	1998																											2	Y123				3.843		11.701													92		95	92.5			92.5																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7895	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.9Nd0.1Cu3Oz	Y	1	Ba	1.9	Nd	0.1	Cu	3													O	z		1	1998																											2	Y123				3.859		11.659													92.5		95.5	93			93																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7896	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.85Nd0.15Cu3Oz	Y	1	Ba	1.85	Nd	0.15	Cu	3													O	z		1	1998																											2	Y123				3.847		11.737													91.5		95	92			92																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7897	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.8Nd0.2Cu3Oz	Y	1	Ba	1.8	Nd	0.2	Cu	3													O	z		1	1998																											2	Y123				3.854		11.684													92.5		95	92			92																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7898	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.75Nd0.25Cu3Oz	Y	1	Ba	1.75	Nd	0.25	Cu	3													O	z		1	1998																											2	Y123				3.845		11.732													94		96	93			93																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7899	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.7Nd0.3Cu3Oz	Y	1	Ba	1.7	Nd	0.3	Cu	3													O	z		1	1998																											2	Y123				3.845		11.709													83		95	85			85																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7900	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.65Nd0.35Cu3Oz	Y	1	Ba	1.65	Nd	0.35	Cu	3													O	z		1	1998																											2	Y123				3.855		11.732													86		95	88			88																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7901	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.6Nd0.4Cu3Oz	Y	1	Ba	1.6	Nd	0.4	Cu	3													O	z		1	1998																																															85		95	86			86																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7902	PHC2980066		Y(Ba,Nd)2Cu3Oz	Y1Ba1.5Nd0.5Cu3Oz	Y	1	Ba	1.5	Nd	0.5	Cu	3													O	z		1	1998																																																	30				30																																																																																														Y2O3, Nd2O3, BaCO3, CuO		mixture-CAL(970C,12H in air)-SIN(960C,12H in air)-ANN(500C,10H in flowing O2)-RT(1C/min)					Influence of Nd at Ba-sites on superconductivity of YBa2-x NdxCu3Oy	199803		Department of Physics, The University of Hong Kong Pokfulam Road, Hong Kong, China	Physica.C,298(1998)66-72	J. Gao,W.H. Tang		
7903	NAT3640315	all nost single phase	Sr2CuO3	Sr2Cu1O3.1	Sr	2	Cu	1																	O	3+z	3.1	1	1993																											2	Sr0201				3.764		12.548													4	70	80	70			70										22																																																																																				Sr2CuO3, CuO		mixture-Au capsule-press isostatically to 6GPa-heat to 1073-1173K and hold(30min)-drop to 400K in a flow second-to RT in a minute					A new family of copper oxide superconductors Srn+1CunO2n+1+delta stabilized at high pressure	7		Institute for Chemical Research, Kyoto Univercity, Uji, Kyoto-fu 611, Japan	Nature 364(1993)315-317	M. Azuma,M. Takano,Y. Takeda,Z. Hiroi		
7904	NAT3640315		Sr2CaCu2O5	Sr2.1Ca0.9Cu2O5+z	Sr	2.1	Ca	0.9	Cu	2															O	5+z		2	1993																												Sr0212																			90		100	100			100																																																																																														Sr2CuO3, CuO		mixture-Au capsule-press isostatically to 6GPa-heat to 1073-1173K and hold(30min)-drop to 400K in a flow second-to RT in a minute					A new family of copper oxide superconductors Srn+1CunO2n+1+delta stabilized at high pressure	7		Institute for Chemical Research, Kyoto Univercity, Uji, Kyoto-fu 611, Japan	Nature 364(1993)315-317	M. Azuma,M. Takano,Y. Takeda,Z. Hiroi		
7905	PHC2530254	inpurity phases=CaHgO2, BaCuO2, major phase=Hg-1212 nominal composition	HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1995																											2	Hg1212				3.862		12.708													92			110.3			110.3										44																																																																																						precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7906	PHC2530254	major phase=Hg1212, nominal composition	HgBa2Ca2Cu3(Fe,O)z	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z		1	1995																											2	Hg1212				3.857		12.647													126						126										68																																																																																						precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7907	PHC2530254		HgBa2Ca2Cu3(Fe,O)z	Hg1Ba2Ca2Cu3F0.1Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.1											O	z			1995																												Hg1223																						127.4			127.4																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7908	PHC2530254		HgBa2Ca2Cu3(Fe,O)z	Hg1Ba2Ca2Cu3F0.2Oz	Hg	1	Ba	2	Ca	2	Cu	3	F	0.2											O	z			1995																												Hg1223																						128.4			128.4																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7909	PHC2530254		HgBa2Ca2Cu3(O,Fe)	Hg1Ba2Ca2Cu3Fe0.3Oz	Hg	1	Ba	2	Ca	2	Cu	3	Fe	0.3											O	z			1995																												Hg1223																						128.5			128.5																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7910	PHC2160237	Cu-O=1.815A, Cu-O(2)=2.01A	(Pb,Hg)(Sr,La)2CuO5	Pb0.5Hg0.5Sr1.2La0.8Cu1O5-z	Pb	0.5	Hg	0.5	Sr	1.2	La	0.8	Cu	1											O	5-z		1	1993																												1201	P4/mmm	123		3.791		8.691													17	24	38	32			24										32.3																																																																																				Pb O, Hg O, Sr O, Cu O		mixture-pellet-wrapped in Au foil-quartz tube(O2=10E-4 Torr)-heat to 930C(5C/min)-hold(12H)-RT(5C/min)					SUPERCONDUCTIVITY UP TO 32 K IN A NEW FAMILY OF THE HG-CONTAINING (PB,HG)(SR,LA)2CUO5-Z (1201) SYSTEM	199311			PHYSICA C,216(1993)237	D.A.JEFFERSON,D.S.SHY,R.S.LIU,S.F.HU	PB,HG,SR,LA,CU,O	
7911	PHC2350075	magnetic transition at 9.5K	(Tm,Ca)2CuO4	Tm1.83Ca0.17Cu1O4	Tm	1.83	Ca	0.17	Cu	1															O	4			1994																												T'																						30			30																																																																																																					New synthesis, structural features and superconductivity	1994		National Laboratory for Superconductivity, Institute of Physics Academia Sinica, Beijing 100 080, China	Physica.C235(1994)75-78	W.J. Zhu,Z.X. Zhao		
7912	PHC2350075	diamagnetism appears at 30K but not sharp transition	(Ba,K)PbO3	Ba0.9K0.1Pb1O3	Ba	0.9	K	0.1	Pb	1															O	3			1994																												ABO3				4.26		4.293																30			30																																																																																																Ba: K: Pb =1.5: 50: 1, mixture was melt at 250C in a Teflon crucible, crystal was grown by electro-crystalliqation					New synthesis, structural features and superconductivity	1994		National Laboratory for Superconductivity, Institute of Physics Academia Sinica, Beijing 100 080, China	Physica.C235(1994)75-78	W.J. Zhu,Z.X. Zhao		
7913	SSC1050037		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1998																												T																				36.5				5	36.5																																																																																															1	standard solid state reaction.					TWO REGIMES BEHAVIOR IN THE RESISTIVITY OF THE La1.85Sr0.15Cu1-xLixO4 SYSTEM: A SIGNATURE OF DIFFERENT ELECTRONIC STATES FOR HOLES			Laboratorio de Superconductivited, Facultad de Fisica-IMRE, Universidad de La Habana, San Lazaro y L, 10400, Ciudad Habana, Cuba	Solid State Commun.105(1998)37-40	B. Giordenengo,B.Giordanengo,E.M. Baggio-Saitovitch,E.M.Baggio-Saitovich,J.E. Musa,J.E.Musa,S. Garcia,S.Garcia		
7914	SSC1050037		(La,Sr)2(Cu,Li)O4	La1.85Sr0.15Cu0.98Li0.02O4	La	1.85	Sr	0.15	Cu	0.98	Li	0.02													O	4			1998																												T																				36.5				5	36.5																																																																																															1	standard solid state reaction.					TWO REGIMES BEHAVIOR IN THE RESISTIVITY OF THE La1.85Sr0.15Cu1-xLixO4 SYSTEM: A SIGNATURE OF DIFFERENT ELECTRONIC STATES FOR HOLES			Laboratorio de Superconductivited, Facultad de Fisica-IMRE, Universidad de La Habana, San Lazaro y L, 10400, Ciudad Habana, Cuba	Solid State Commun.105(1998)37-40	B. Giordenengo,B.Giordanengo,E.M. Baggio-Saitovitch,E.M.Baggio-Saitovich,J.E. Musa,J.E.Musa,S. Garcia,S.Garcia		
7915	SSC1050037		(La,Sr)2(Cu,Li)O4	La1.85Sr0.15Cu0.97Li0.03O4	La	1.85	Sr	0.15	Cu	0.97	Li	0.03													O	4			1998																												T																				33.5				7	33.5																																																																																															1	standard solid state reaction.					TWO REGIMES BEHAVIOR IN THE RESISTIVITY OF THE La1.85Sr0.15Cu1-xLixO4 SYSTEM: A SIGNATURE OF DIFFERENT ELECTRONIC STATES FOR HOLES			Laboratorio de Superconductivited, Facultad de Fisica-IMRE, Universidad de La Habana, San Lazaro y L, 10400, Ciudad Habana, Cuba	Solid State Commun.105(1998)37-40	B. Giordenengo,B.Giordanengo,E.M. Baggio-Saitovitch,E.M.Baggio-Saitovich,J.E. Musa,J.E.Musa,S. Garcia,S.Garcia		
7916	SSC1050037		(La,Sr)2(Cu,Li)O4	La1.85Sr0.15Cu0.95Li0.05O4	La	1.85	Sr	0.15	Cu	0.95	Li	0.05													O	4			1998																												T																				27.2				7	27.2																																																																																															1	standard solid state reaction.					TWO REGIMES BEHAVIOR IN THE RESISTIVITY OF THE La1.85Sr0.15Cu1-xLixO4 SYSTEM: A SIGNATURE OF DIFFERENT ELECTRONIC STATES FOR HOLES			Laboratorio de Superconductivited, Facultad de Fisica-IMRE, Universidad de La Habana, San Lazaro y L, 10400, Ciudad Habana, Cuba	Solid State Commun.105(1998)37-40	B. Giordenengo,B.Giordanengo,E.M. Baggio-Saitovitch,E.M.Baggio-Saitovich,J.E. Musa,J.E.Musa,S. Garcia,S.Garcia		
7917	PR0459951		Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4		1	1992																												T'																																																																																																																							Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7918	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.1O3.9	Nd	2	Cu	1	F	0.1															O	3.9		1	1992																												T'																																																																																																																							Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7919	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.12O3.88	Nd	2	Cu	1	F	0.12															O	3.88		1	1992																												T'																																																																																																																							Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7920	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.16O3.84	Nd	2	Cu	1	F	0.16															O	3.84		1	1992																												T'																																																																																																																							Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7921	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.18O3.82	Nd	2	Cu	1	F	0.18															O	3.82		1	1992																												T'																																																																																																																							Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7922	PR0459951		Nd2Cu(O,F)4	Nd2Cu1O4	Nd	2	Cu	1																	O	4		1	1992																												T'																					27				27																																																																																														Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7923	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.22O3.78	Nd	2	Cu	1	F	0.22															O	3.78		1	1992																												T'																			22		27				24.5																																																																																														Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7924	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.24O3.76	Nd	2	Cu	1	F	0.24															O	3.76		1	1992																												T'																					27				27																																																																																														Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7925	PR0459951		Nd2Cu(O,F)4	Nd2Cu1F0.3O3.7	Nd	2	Cu	1	F	0.3															O	3.7		1	1992																												T'																					27				27																																																																																														Nd2O3, CuO, NdF3		mixture-CAL(860C,10H in 20%O2-Ar gas flow)-press-pellet-SIN(1100C,14H in 1%O2-Ar gas flow)-ANN(910,14H in N2 flow)-cool to RT(5C/min)					Hall and thermoelectric-power coefficients of superconducting Nd2CuO4-xFx	199205		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,45(1992)9951	H. Yamauchi,Jun Sugiyama,Kiyotaka Matsuura,Michikazu Kosuge,Shoji Tanaka		
7926	PHC2680095	quench	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.05	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.05		1996																											2	Pb1201				3.774		8.691														37.6					37.6																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7927	PHC2680095	quench	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.06	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.06		1996																											2	Pb1201				3.776		8.687														37.8					37.8																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7928	PHC2680095	quench	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.09	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.09		1996																											2	Pb1201				3.776		8.688														36.7					36.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7929	PHC2680095	quench	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.12	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.12		1996																											2	Pb1201				3.777		8.665														35.9					35.9																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7930	PHC2680095	quench	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.15	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.15		1996																											2	Pb1201				3.784		8.668														32					32																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7931	PHC2680095	HIP	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.19	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.19		1996																											2	Pb1201				3.788		8.662														25.1					25.1																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7932	PHC2680095	HIP	(Pb,Cu)(Sr,La)CuOz	Pb0.6Cu0.4Sr1La1Cu1O5.21	Pb	0.6	Cu	0.4	Sr	1	La	1	Cu	1											O	z	5.21		1996																											2	Pb1201				3.795		8.637														25.1					25.1																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7933	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr1.1La0.9Cu1O5.07	Pb	0.6	Cu	0.4	Sr	1.1	La	0.9	Cu	1											O	z	5.07		1996																												Pb1201																				33.9					33.9																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7934	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr1.1La0.9Cu1O5.12	Pb	0.6	Cu	0.4	Sr	1.1	La	0.9	Cu	1											O	z	5.12		1996																												Pb1201																				31					31																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7935	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr1.1La0.9Cu1O5.18	Pb	0.6	Cu	0.4	Sr	1.1	La	0.9	Cu	1											O	z	5.18		1996																												Pb1201																				28					28																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7936	PHC2680095	HIP	(Pb,Cu)(sr,La)2CuOz	Pb0.6Cu0.4Sr1.1La0.9Cu1O5.19	Pb	0.6	Cu	0.4	Sr	1.1	La	0.9	Cu	1											O	z	5.19		1996																												Pb1201																				25					25																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7937	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.8La1.2Cu1O5.06	Pb	0.6	Cu	0.4	Sr	0.8	La	1.2	Cu	1											O	z	5.06		1996																												Pb1201																				28.7					28.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7938	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.8La1.2Cu1O5.11	Pb	0.6	Cu	0.4	Sr	0.8	La	1.2	Cu	1											O	z	5.11		1996																												Pb1201																				34.8					34.8																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7939	PHC2680095	HIP	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.8La1.2Cu1O5.29	Pb	0.6	Cu	0.4	Sr	0.8	La	1.2	Cu	1											O	z	5.29		1996																												Pb1201																				25.2					25.2																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7940	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.8La1.2Cu1O5.28	Pb	0.6	Cu	0.4	Sr	0.8	La	1.2	Cu	1											O	z	5.28		1996																												Pb1201																				28.1					28.1																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7941	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.9La1.1Cu1O5.06	Pb	0.6	Cu	0.4	Sr	0.9	La	1.1	Cu	1											O	z	5.06		1996																												Pb1201																				37.6					37.6																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7942	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.9La1.1Cu1O5.18	Pb	0.6	Cu	0.4	Sr	0.9	La	1.1	Cu	1											O	z	5.18		1996																												Pb1201																				31.6					31.6																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7943	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.6Cu0.4Sr0.9La1.1Cu1O5.24	Pb	0.6	Cu	0.4	Sr	0.9	La	1.1	Cu	1											O	z	5.24		1996																												Pb1201																				27.8					27.8																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7944	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr1La1Cu1O5.03	Pb	0.5	Cu	0.5	Sr	1	La	1	Cu	1											O	z	5.03		1996																												Pb1201				3.778		8.676														36.7					36.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7945	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr1La1Cu1O5.05	Pb	0.5	Cu	0.5	Sr	1	La	1	Cu	1											O	z	5.05		1996																												Pb1201				3.772		8.688														36.7					36.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7946	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr1La1Cu1O5.1	Pb	0.5	Cu	0.5	Sr	1	La	1	Cu	1											O	z	5.1		1996																												Pb1201				3.778		8.666														31.9					31.9																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7947	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr1La1Cu1O5.15	Pb	0.5	Cu	0.5	Sr	1	La	1	Cu	1											O	z	5.15		1996																												Pb1201				3.789		8.649														28					28																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7948	PHC2680095	HIP	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr1La1Cu1O5.19	Pb	0.5	Cu	0.5	Sr	1	La	1	Cu	1											O	z	5.19		1996																												Pb1201				3.791		8.627														24.1					24.1																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7949	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.8La1.2Cu1O5.01	Pb	0.5	Cu	0.5	Sr	0.8	La	1.2	Cu	1											O	z	5.01		1996																												Pb1201				3.772		8.684														38.7					38.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7950	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.8La1.2Cu1O5.1	Pb	0.5	Cu	0.5	Sr	0.8	La	1.2	Cu	1											O	z	5.1		1996																												Pb1201				3.783		8.673														34.9					34.9																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7951	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.8La1.2Cu1O5.16	Pb	0.5	Cu	0.5	Sr	0.8	La	1.2	Cu	1											O	z	5.16		1996																												Pb1201				3.791		8.651														28					28																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7952	PHC2680095	HIP	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.8La1.2Cu1O5.25	Pb	0.5	Cu	0.5	Sr	0.8	La	1.2	Cu	1											O	z	5.25		1996																												Pb1201				3.799		8.632														25.2					25.2																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7953	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.9La1.1Cu1O5.02	Pb	0.5	Cu	0.5	Sr	0.9	La	1.1	Cu	1											O	z	5.02		1996																												Pb1201				3.771		8.688														38.5					38.5																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7954	PHC2680095	quench	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.9La1.1Cu1O5.08	Pb	0.5	Cu	0.5	Sr	0.9	La	1.1	Cu	1											O	z	5.08		1996																												Pb1201				3.78		8.679														37.7					37.7																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7955	PHC2680095	as-sintered	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.9La1.1Cu1O5.16	Pb	0.5	Cu	0.5	Sr	0.9	La	1.1	Cu	1											O	z	5.16		1996																												Pb1201				3.79		8.652														28.1					28.1																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7956	PHC2680095	HIP	(Pb,Cu)(Sr,La)2CuOz	Pb0.5Cu0.5Sr0.9La1.1Cu1O5.22	Pb	0.5	Cu	0.5	Sr	0.9	La	1.1	Cu	1											O	z	5.22		1996																												Pb1201				3.79		8.609														24.9					24.9																																																																																														PbO, SrCO3, La2O2, CuO	1	mixture-CAL(800C,5H in air)-pellet-SIN(1010-1015C,1.7-2.0H in O2 flow)-FC, HIP or quench					Valence analysis of Pb and Cu and superconductivity of(Pb,Cu)(Sr,La)2CuOy			Institute for Materials Research,Tohoku University,Katahira,Apba-ku,Sendai   98-77, Japan	Physica.C,268(1996)95-99	Eriko Ohshima,Masae Kikuchi,Masayasu Nagoshi,Minako Shida,Yasuhiko Syono	Pb, Cu, Sr, La, Cu, O	
7957	PHC2530254		HgBa2Ca2Cu3(O,Fe)	Hg1Ba2Ca2Cu3Fe0.5Oz	Hg	1	Ba	2	Ca	2	Cu	3	Fe	0.5											O	z			1995																												Hg1223																						128.2			128.2																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7958	PHC2530254		HgBa2Ca2Cu3(O,Fe)	Hg1Ba2Ca2Cu3Fe0.6Oz	Hg	1	Ba	2	Ca	2	Cu	3	Fe	0.6											O	z			1995																												Hg1223																						130			130																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7959	PHC2530254		HgBa2Ca2Cu3(O,Fe)	Hg1Ba2Ca2Cu3Fe0.8Oz	Hg	1	Ba	2	Ca	2	Cu	3	Fe	0.8											O	z			1995																												Hg1223																						128.4			128.4																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7960	PHC2530254		HgBa2Ca2Cu3(O,Fe)	Hg1Ba2Ca2Cu3Fe1Oz	Hg	1	Ba	2	Ca	2	Cu	3	Fe	1											O	z			1995																												Hg1223																						125.2			125.2																																																																																																precursor(Ba-Ca-Cu-O)-CAL(900C,24H in O2 flow)-(mixed with HgO, CuF2)-sealed(quartz tube)-SIN(800C,10H)-FC					effect of F-doping in the H-Ba-Ca-Cu-O system	199511		Department of Physics, Hunan Narmal University, Changsha, Hunan 410006, P.R. China	Physica C,253(1995)254-258	Lin Yuan,Xiao-gang Wang,Zhiming Huang	Hg, Ba, Ca, Cu, O, F	
7961	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.96	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.96		1998																											3	Cu1212				3.789	3.867	11.59																82			82																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7962	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.8	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.8		1998																											3	Cu1212				3.795	3.872	11.6																81			81																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7963	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.75	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.75		1998																											3	Cu1212				3.803	3.864	11.63																60			60																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7964	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.64	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.64		1998																											3	Cu1212				3.806	3.858	11.64																47			47																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7965	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.53	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.53		1998																											3	Cu1212				3.817	3.851	11.67																34			34																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7966	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.48	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.48		1998																											2	Cu1212				3.833		11.68																10			10																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7967	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.42	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.42		1998																											2	Cu1212				3.836		11.7																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7968	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.26	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.26		1998																											2	Cu1212				3.835		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7969	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O6.15	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.15		1998																											2	Cu1212				3.834		11.74																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7970	PHC3000017		Cu(Ba,Sr)2YbCu2O6	Ba1.6Sr0.4Yb1Cu3O5.97	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	5.97		1998																											2	Cu1212				3.834		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7971	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.8	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.8		1998																											3	Cu1212				3.792	3.862	11.61																80			80																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7972	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.76	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.76		1998																											3	Cu1212				3.8	3.864	11.62																80			80																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7973	PHC3000017		Cu(Ba,Sr)2(YB,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.58	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.58		1998																											3	Cu1212				3.813	3.863	11.66																55			55																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7974	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.56	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.56		1998																											2	Cu1212				3.835		11.69																30			30																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7975	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.33	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.33		1998																											2	Cu1212				3.836		11.7																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7976	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.21	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.21		1998																											2	Cu1212				3.833		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7977	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6.07	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6.07		1998																											2	Cu1212				3.837		11.75																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7978	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.95Ca0.05Cu3O6	Ba	1.6	Sr	0.4	Yb	0.95	Ca	0.05	Cu	3											O	6+z	6		1998																											2	Cu1212				3.836		11.74																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7979	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.9Ca0.1Cu3O6.03	Ba	1.6	Sr	0.4	Yb	0.9	Ca	0.1	Cu	3											O	6+z	6.03		1998																											2	Cu1212				3.832		11.72																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7980	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15Cu3O6.83	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Cu	3											O	6+z	6.83		1998																											3	Cu1212				3.795	3.857	11.61																76			76																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7981	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15Cu3O6.6	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Cu	3											O	6+z	6.6		1998																											3	Cu1212				3.816	3.862	11.67																61			61																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7982	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15Cu3O6.36	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Cu	3											O	6+z	6.36		1998																											2	Cu1212				3.833		11.7																19			19																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7983	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15Cu3O6.17	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Cu	3											O	6+z	6.17		1998																											2	Cu1212				3.831		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7984	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15CaO6.22	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Ca												O	6+z	6.22		1998																											2	Cu1212				3.831		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7985	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.85Ca0.15Cu3O6.01	Ba	1.6	Sr	0.4	Yb	0.85	Ca	0.15	Cu	3											O	6+z	6.01		1998																											2	Cu1212				3.829		11.73																	5																																																																																																Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7986	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6.68	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6.68		1998																											3	Cu1212				3.801	3.857	11.6																74			74																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7987	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6.51	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6.51		1998																												Cu1212																						66			66																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7988	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6.3	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6.3		1998																											2	Cu1212				3.835		11.71																34			34																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7989	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6.19	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6.19		1998																											2	Cu1212				3.82		11.72																25			25																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7990	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6.19	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6.19		1998																											2	Cu1212				3.831		11.73																23			23																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7991	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.75Ca0.25Cu3O6	Ba	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6+z	6		1998																											2	Cu1212				3.833		11.72																22			22																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7992	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.63	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.63		1998																											3	Cu1212				3.806	3.855	11.62																77			77																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7993	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.53	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.53		1998																											3	Cu1212				3.816	3.857	11.65																78			78																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7994	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.52	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.52		1998																											3	Cu1212				3.827	3.848	11.66																79			79																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7995	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.45	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.45		1998																											2	Cu1212				3.835		11.68																73			73																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7996	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu2O6.4	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	2											O	6+z	6.4		1998																											2	Cu1212				3.838		11.69																61			61																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7997	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.28	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.28		1998																											2	Cu1212				3.837		11.72																51			51																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7998	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.8Ca0.2Cu3O6.04	Ba	1.6	Sr	0.4	Yb	0.8	Ca	0.2	Cu	3											O	6+z	6.04		1998																											2	Cu1212				3.83		11.72																13			13																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
7999	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.7Ca0.3Cu3O6	Ba	1.6	Sr	0.4	Yb	0.7	Ca	0.3	Cu	3											O	6+z	6		1998																											2	Cu1212				3.83		11.74																41			41																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8000	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Cu1Ba1.6Sr0.4Yb0.65Ca0.35Cu2O6.15	Cu	1	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	2									O	6+z	6.15		1998																											2	Cu1212				3.834		11.73																48			48																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8001	PHC3000017		Cu(Ba,Ca)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.15	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.15		1998																											2	Cu1212				3.835		11.73																49			49																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8002	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.65Ca0.35Cu3O6.04	Ba	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6+z	6.04		1998																											2	Cu1212				3.832		11.73																50			50																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8003	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.61	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.61		1998																											3	Cu1212				3.807	3.856	11.61																76			76																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8004	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.36	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.36		1998																											2	Cu1212				3.839		11.67																75			75																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8005	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.25	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.25		1998																											2	Cu1212				3.838		11.71																53			53																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8006	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.14	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.14		1998																											2	Cu1212				3.835		11.72																47			47																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8007	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.14	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.14		1998																											2	Cu1212				3.834		11.73																46			46																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8008	PHC3000017		Cu(Ba,Sr)2(Yb,Ca)Cu2O6	Ba1.6Sr0.4Yb0.6Ca0.4Cu3O6.04	Ba	1.6	Sr	0.4	Yb	0.6	Ca	0.4	Cu	3											O	6+z	6.04		1998																											2	Cu1212				3.835		11.72																47			47																																																																																														Yb2O3, CaCO3, BaCO3, SrCO3, CuO	1	mixture-CAL(in air)-SIN(900-940C, in air)-ANN(400C, 24H in O2 flow), or ANN(in Ar flow)					Investigation of different hole-doping routes in Cu(Ba,Sr)2(Yb1-xCax)Cu2O6+z	199805		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226, Japan	Physica.C,300(1998)17-25	H. Yamauchi,K. Fujinami,M. Karppinen		
8009	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.136	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.136		1998																												Hg1223																				132.9					132.9																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8010	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.044	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.044		1998																												Hg1201																				90.7					90.7																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8011	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.95K0.5O8+z	Bi	2	Sr	2	Ca	1	Cu	1.95	K	0.5											O	8+z		1	1998																												Bi2212				5.41	5.42	30.76														85					85																																										ESR meamrement, Brandt' model.	2670																																																					sol-gel method, ANN(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8012	PHC300033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.4K0.6O8+z	Bi	2	Sr	2	Ca	1	Cu	1.4	K	0.6											O	8+z			1998																												Bi2212				5.4	5.43	30.72														87					87																																										ESR meamrement, Brandt' model.	2209																																																					sol-gel method, ANN(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKxO8+delta: ESR study			School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica C300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8013	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.3K0.7O8+z	Bi	2	Sr	2	Ca	1	Cu	1.3	K	0.7											O	8+z		1	1998																												Bi2212				5.42	5.41	30.69														93					93																																										ESR meamrement, Brandt' model.	1906																																																					sol-gel method, ANN(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8014	PHC3000071	Ag-prepured	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		2	1998																											2	Hg1245				3.848		22.149																100			100																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8015	PHC3000071	N2-flow, 300C, 2OH	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		2	1998																											2	Hg1245				3.853		22.181																85			85																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8016	PHC3000071	O2-flow, 300C, 50H	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		2	1998																											2	Hg1245				3.852		22.161																106			106																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8017	PHC3000071	P(O2)=2000 bar, 300C, 10H	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		2	1998																											2	Hg1245				8.503		22.157																111			111																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8018	PHC3000071	As-prepared	HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z		2	1998																											2	Hg1234				3.845		19.001																116			116																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8019	PHC3000071	N2-flow, 300, 20H	HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z		2	1998																											2	Hg1234				3.8532		19.003																95			95																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8020	PHC3000071	O2-flow, 300C, 50H	HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z		2	1998																											2	Hg1234				3.852		19.009																116			116																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8021	PHC3000071	P(O2)=2000 bar, 300C, 10H	HgBa2Ca3Cu4Oz	Hg1Ba2Ca3Cu4Oz	Hg	1	Ba	2	Ca	3	Cu	4													O	z		2	1998																											2	Hg1234				3.851	19.011																	125			125																																																																																																High pressure synthesis, pressure, atmosphere, temperature, ratio of BaO/BaO2, are variables					Synthesis and characterization of overdoped Hg-1234 and Hg-1245 phases; the universal behavior of Tc variation in the HgBa2Can-1CunO2n+2+delta series	199805		Department of Chemistry, Moscow State University, 119899, Moscow, Russian Federation	Physica.C,300(1998)71-76	D.A. Pavlov,E.S. Itskevich,E.V. Antipov,I.G. Kuzemskaya,I.V. Morozov,K.A. Lokshin,L.F. Kulikova,M.L. Kovba,V.V. Davydov		
8022	PHC2130026	Sr2CuO2CO3 type.	(La,Ba)2CuO2(BO3)	La1Ba1Cu1B1O5	La	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.941		7.504																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8023	PHC2130026	Sr2CuO2CO3 type	(Pr,Ba)2CuO2(BO3)	Pr1Ba1Cu1B1O5	Pr	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.915		7.453																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8024	PHC2130026	Sr2CuO2CO3 type	(Nd,Ba)2CuO2(BO3)	Nd1Ba1Cu1B1O5	Nd	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.905		7.438																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8025	PHC2130026	Sr2CuO2CO3 type	(Sm,Ba)2CuO2(BO3)	Sm1Ba1Cu1B1O5	Sm	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.891		7.416																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8026	PHC2130026	Sr2CuO2CO3 type	(Eu,Ba)2CuO2(BO3)	Eu1Ba1Cu1B1O5	Eu	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.881		7.395																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8027	PHC2130026	Sr2CuO2CO3 type	(Gd,Ba)2CuO2(BO3)	Gd1Ba1Cu1B1O5	Gd	1	Ba	1	Cu	1	B	1													O	5			1993																											2					3.874		7.395																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8028	PHC2080193	Au thors say, Tc(onset)=45-60 for optimum composition	(Y,Sr,Ca)Sr2(Cu,SO4)3Oz	Y0.74Ca0.16Sr2.1Cu2.78S0.22O7	Y	0.74	Ca	0.16	Sr	2.1	Cu	2.78	S	0.22											O	7			1993																											3	Y123				3.825	3.843	11.26													25						25																																																																																															1	mixture-heat (1065C,14H in O2)-pellet-heat (1065C,14H in O2)-FC to RT					COPPER OXIDE SUPERCONDUCTORS CONTAINING SULPHATE AND PHOSPHATEGROUPS	199304			PHYSICA C,208(1993)193	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,SR,CU,S,O,BA	
8029	PHC2080116	unit cell-2a*b*2c	YCaBa4Cu5(NO3)0.3(CO3)0.7O11	Y1Ca1Ba4Cu5N0.3C0.7O14	Y	1	Ca	1	Ba	4	Cu	5	N	0.3	C	0.7									O	14			1993																											3	Y123				3.879	3.885	11.536																82			82										15																																																																																						mixture-bar-in an evacuated ampoule-heat(900C,24H)-FC to RT					"INTRODUCTION OF NITRATE GROUPS IN THE ""123""STRUCTURE"	199304			PHYSICA C,208(1993)116	A.MAIGNAN,B.RAVEAU,C.MICHEL,M.HERVIEU	Y,CA,BA,CU,N,C,O	
8030	PHC2080149	as-synthesized, Tl1201+Sr2CuO2CO3	(Tl,Bi)Sr4Cu2(CO3)O7	Tl0.5Bi0.5Sr4Cu2C1O10	Tl	0.5	Bi	0.5	Sr	4	Cu	2	C	1											O	10			1993																													P4/mmm			3.831		16.518																55			55																																																																																														Tl2O3, Bi2O3, SrCO3, Sr2CuO3, SrO2, CuO		mixture-bar-in alumina crucible-seal (evacuated quartz tube)-heat(860C,6H)-Q to RT					A 55 K SUPERCONDUCTING COPPER OXYCARBONATE: TL1-XBIXSR4CU2CO3O7	199304			PHYSICA C,208(1993)149	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,BI,SR,CU,C,O	
8031	PHC2080149	annealed in Ar/H2 at 290C for 15min	(Tl,Bi)Sr4Cu2(CO3)O7	Tl0.5Bi0.5Sr4Cu2C1O10	Tl	0.5	Bi	0.5	Sr	4	Cu	2	C	1											O	10			1993																																																		52			52																																																																																														Tl2O3, Bi2O3, SrCO3, Sr2CuO3, SrO2, CuO		mixture-bar-in alumina crucible-seal (evacuated quartz tube)-heat(860C,6H)-Q to RT					A 55 K SUPERCONDUCTING COPPER OXYCARBONATE: TL1-XBIXSR4CU2CO3O7	199304			PHYSICA C,208(1993)149	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,BI,SR,CU,C,O	
8032	PHC2080149	annealed in Ar/H2 at 290C for 75 min	(Tl,Bi)Sr4Cu2(CO3)O7	Tl0.7Bi0.3Sr4Cu2C1O10	Tl	0.7	Bi	0.3	Sr	4	Cu	2	C	1											O	10			1993																																																		50			50																																																																																														Tl2O3, Bi2O3, SrCO3, Sr2CuO3, SrO2, CuO		mixture-bar-in alumina crucible-seal (evacuated quartz tube)-heat(860C,6H)-Q to RT					A 55 K SUPERCONDUCTING COPPER OXYCARBONATE: TL1-XBIXSR4CU2CO3O7	199304			PHYSICA C,208(1993)149	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,BI,SR,CU,C,O	
8033	PHC2080149	as-synthesized, Tl1201+Sr2CuO2CO3	(Tl,Bi)Sr4Cu2(CO3)O7	Tl0.7Bi0.3Sr4Cu2C1O10	Tl	0.7	Bi	0.3	Sr	4	Cu	2	C	1											O	10			1993																																																		48			48																																																																																														Tl2O3, Bi2O3, SrCO3, Sr2CuO3, SrO2, CuO		mixture-bar-in alumina crucible-seal (evacuated quartz tube)-heat(860C,6H)-Q to RT					A 55 K SUPERCONDUCTING COPPER OXYCARBONATE: TL1-XBIXSR4CU2CO3O7	199304			PHYSICA C,208(1993)149	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,BI,SR,CU,C,O	
8034	PHC2080121	intergrowth (Bi2Sr2CuO6+Sr2CuO2CO3)	Bi2Sr4Cu2CO3O8	Bi2Sr4Cu2C1O11	Bi	2	Sr	4	Cu	2	C	1													O	11			1993																											3					5.466	5.46	39.5																30			30										5																																																																																					1	Bi2O3:SrCO3:CuO=1:4:2, mixture-heat(700C,48H+800C,2H in air)-Q to RT					THE BISMUTH OXYCARBONATE BI2SR4CU2CO3O8.	199304			PHYSICA C,208(1993)121	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,M.CALDES,M.HERVIEU	BI,SR,CU,C,O	
8035	PHC2070065		Y4Sr8Cu11CO3O25	Y4Sr8Cu11C1O28	Y	4	Sr	8	Cu	11	C	1													O	28			1993																											3		Bm2m			15.311	3.851	22.371																	4																																																																																																							"ORDERED SUBSTITUTION OF ""CO3""GROUPS FOR CUO4 SQUARE GROUPS IN THE ""123"" STRUCTURE"	199303			PHYSICA C,207(1993)65	B.DOMENGES,B.RAVEAU,M.HERVIEU	C,O,CU,Y,SR	
8036	PHC2050219	as-prepared		Tl0.5Pb0.5Sr4Cu2C7.75O23.25	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	7.75											O	23.25			1993																											2		P4/mmm			3.824		16.516																23			23										45																																																																																				Tl2O3, PbO2, SrO2, CuO, Sr2CuO3, C+SrCO3		mixture-press into bars-alumina crucible-seal in quartz ampoule-heat(900C,6H)-Q to RT					A 70 K SUPERCONDUCTOR	199302			PHYSICA C,205(1993)219	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,PB,SR,CU,C,O	
8037	PHC2050219	annealing in H2/Ar atmosphese(290C,15min)		Tl0.5Pb0.5Sr4Cu2C7.75O23.25	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	7.75											O	23.25			1993																																																		63			63										50																																																																																				Tl2O3, PbO2, SrO2, CuO, Sr2CuO3, C+SrCO3		mixture-press into bars-alumina crucible-seal in quartz ampoule-heat(900C,6H)-Q to RT					A 70 K SUPERCONDUCTOR	199302			PHYSICA C,205(1993)219	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,PB,SR,CU,C,O	
8038	PHC2050219	as-prepared		Tl0.5Pb0.5Sr4Cu2C7O21	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	7											O	21			1993																																																		60			60										70																																																																																				Tl2O3, PbO2, SrO2, CuO, Sr2CuO3, C+SrCO3		mixture-press into bars-alumina crucible-seal in quartz ampoule-heat(900C,6H)-Q to RT					A 70 K SUPERCONDUCTOR	199302			PHYSICA C,205(1993)219	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,PB,SR,CU,C,O	
8039	PHC2050219	annealing in H2/Ar atmosphese(290C, 15min)		Tl0.5Pb0.5Sr4Cu2C7O21	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	7											O	21			1993																																																		70			70										70																																																																																				Tl2O3, PbO2, SrO2, CuO, Sr2CuO3, C+SrCO3		mixture-press into bars-alumina crucible-seal in quartz ampoule-heat(900C,6H)-Q to RT					A 70 K SUPERCONDUCTOR	199302			PHYSICA C,205(1993)219	A.MAIGNAN,B.RAVEAU,C.MARTIN,C.MICHEL,M.HERVIEU,M.HUVE	TL,PB,SR,CU,C,O	
8040	NAT3570313	about 10% of C are replaced by Cu atoms.	(Ba,Sr)2CuO2(CO3)	Ba1.1Sr0.9Cu1.1C0.9O4.9+z	Ba	1.1	Sr	0.9	Cu	1.1	C	0.9													O	4.9+z			1992																											2					5.564		7.857													26		40	26			26										20																																																																																				BaCO3, SrCO3, CuO		mixture-CAL(800,20H +850C, 100H in air)-HIP(1000C, 50H in 20%O2+80%Ar, P=250 atm)					A NEW COPPER OXIDE SUPERCONDUCTOR CONTAINING CARBON	5			NATURE 357(1992)313	K.KINOSHITA,T.YAMADA		
8041	SSC0900435	IR spectrum shows BO3(3-)ion	YSr(Cu,(BO3))3O7	Y1Sr2Cu2.75B0.25Oz	Y	1	Sr	2	Cu	2.75	B	0.25													O	z			1994																											2	Y123				3.816		10.985																	10																																																																																																Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8042	SSC0900435	IR spectrum shows BO3(3-)ion.	Y(SrBa)2(Cu,(BO3))3O7	Y1Sr1.75Ba0.25Cu2.75B0.25Oz	Y	1	Sr	1.75	Ba	0.25	Cu	2.75	B	0.25											O	z			1994																											2	Y123				3.819		11.266																	10																																																																																																Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8043	SSC0900435	IR spectrum	Y(Sr,Ba)2(Cu,(BO3))3O7	Y1Sr1.5Ba5Cu2.75B0.25Oz	Y	1	Sr	1.5	Ba	5	Cu	2.75	B	0.25											O	z			1994																											2	Y123				3.826		11.33																	10																																																																																																Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8044	SSC0900435	IR spectrum shows BO(3-)ion	Y(Sr,Ba)2(Cu,(BO3))3O7	Y1Sr1.25Ba0.75Cu2.75B0.25Oz	Y	1	Sr	1.25	Ba	0.75	Cu	2.75	B	0.25											O	z			1994																											2	Y123				3.834		11.34																	10																																																																																																Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8045	SSC0900435	IR spectrum shows BO3(3-) ion.	Y(Sr,Ba)2(Cu,(BO3))3O7	Y1Sr1Ba1Cu2.75B0.25Oz	Y	1	Sr	1	Ba	1	Cu	2.75	B	0.25											O	z			1994																											2	Y123				3.836		11.354																35			35																																																																																														Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8046	SSC0900435		(Y,Ca)(Sr,Ba)2(Cu,BO3)3O7	Y0.5Ca0.5Sr1Ba1Cu2.75B0.25Oz	Y	0.5	Ca	0.5	Sr	1	Ba	1	Cu	2.75	B	0.25									O	z			1994																											2	Y123				3.836		11.305																50			50																																																																																														Y2O3, BaO2, SrCO3, CaCO3, CuO, H3BO3		miture-heat(1273K,16H in air)-SIN(1273K,16H in air)-FC to RT					SUPERCONDUCTING BORATE DERIVATIVES OF 123 CUPRATES	1994		Solid State and Structural chenistry Un 1t Bangalore-560-012, India	Solid State Commun.90(1994)435-437	C.N.R. Rao,R. Mahesh,R. Nagarajan		
8047	PHC2170027	Bi2Sr2CuOz+Sr2CuO2CO3 intergrowth	Bi2Sr4Cu2(CO3)O8	Bi2Sr4Cu2C1O11-z	Bi	2	Sr	4	Cu	2	C	1													O	11-z			1993																												Bi2201																						32			32																																																																																																mixture-pellet-sealed in quartz tube-heat(800C,6H)-Q to RT					LEAD SUBSTITUTION IN THE 30 K-SUPERCONDUCTOR BI2SR4-YCU2CO3O8-Z	199311			PHYSICA C,217(1993)27	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,M.HERVIEU,M.T.CALDES	BI,SR,CU,C,O	
8048	PHC2170027	S/C may be due to the trace of Bi2Sr4Cu2CO3O8	(Bi,Pb)2Sr3.5Cu2(CO3))8	Bi1.5Pb0.5Sr3.5Cu2C1O11-z	Bi	1.5	Pb	0.5	Sr	3.5	Cu	2	C	1											O	11-z			1993																											3					5.468	5.427	39.53																													1																																																																																						ANN(600C, 12H in P(O2)=20 bar)					LEAD SUBSTITUTION IN THE 30 K-SUPERCONDUCTOR BI2SR4-YCU2CO3O8-Z	199311			PHYSICA C,217(1993)27	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,M.HERVIEU,M.T.CALDES	BI,SR,CU,C,O	
8049	PHC2080351		(Y,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Y0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Y	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.863		11.457															79				79																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8050	PHC2080351	resistivity at 4.2K=about 0.7 mohm.cm	(Pr,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Pr0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Pr	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.885		11.529															30				30										1																																																																																					1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8051	PHC2080351		(Nd,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Nd0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Nd	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.885		11.553															74				74																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8052	PHC2080351		(Sm,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Sm0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Sm	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.876		11.516															77				77																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8053	PHC2080351		(Eu,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Eu1.5Pr0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Eu	1.5	Pr	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.874		11.493															78				78																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8054	PHC2080351		(Gd,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Gd0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Gd	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.872		11.492															78				78																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8055	PHC2080351		(Dy,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Dy0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Dy	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.867		11.469																78			78																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8056	PHC2080351		(Ho,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Ho0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Ho	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.865		11.45																79			79																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8057	PHC2080351		(Er,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Er0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Er	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.845		11.45																80			80										30																																																																																					1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8058	PHC2080351		(Tm,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Tm0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Tm	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.858		11.44																79			79																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8059	PHC2080351		(Yb,Ca)(Sr,Ba)2(Cu,CO3)3OZ	Yb0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Yb	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.853		11.447																78			78																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8060	PHC2080351		(Lu,Ca)(Sr,Ba)2(Cu,CO3)3Oz	Lu0.5Ca0.5Sr0.7Ba1.3Cu2.6C0.4O7-z	Lu	0.5	Ca	0.5	Sr	0.7	Ba	1.3	Cu	2.6	C	0.4									O	7-z		1	1993																											2	M1212				3.849		11.481																77			77																																																																																															1	mixture-pellet-fire(940-960C,3OH in almina crucible, in 99% O2+1% CO2 gas flow)-reground-pellet-fire in the same condition-ANN(800C,30H in O2)					SUPERCONDUCTOR WITH TC UP TO 80 K IN THE COMPOUND (LN,CA)(SR,BA)2(C,CU)CU2O7-Z	199304			PHYSICA C,208(1993)351	JUN AKIMITSU,TAMAKI KOBAYASHI,TOHRU DEN	R,CA,SR,BA,C,CU,O	
8061	PHC2130014	1065C	(Y,Ca,Sr)(Sr)2(Cu,SO4)3Oz	Y0.74Ca0.16Sr2.1Cu2.78S0.22O7	Y	0.74	Ca	0.16	Sr	2.1	Cu	2.78	S	0.22											O	7			1993																												Y123				3.825	3.844	11.244																34.9			34.9																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8062	PHC2130014	1050C	(Y,Ca,Sr)(Sr,Ba)2(Cu,SO4)3Oz	Y0.74Ca0.16Sr1.6Ba0.5Cu2.78S0.22O7	Y	0.74	Ca	0.16	Sr	1.6	Ba	0.5	Cu	2.78	S	0.22									O	7			1993																												Y123				3.827		11.439																54.9			54.9																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8063	PHC2130014	1000C	(Y,Ca,Sr)(Sr,Ba)2(Cu,SO4)3Oz	Y0.74Ca0.16Sr1.1Ba1Cu2.78S0.22O7	Y	0.74	Ca	0.16	Sr	1.1	Ba	1	Cu	2.78	S	0.22									O	7			1993																												Y123				3.833		11.534																75.1			75.1																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8064	PHC2130014	960C	(Y,Ca,Sr)(Sr,Ba)2(Cu,SO4)3Oz	Y0.74Ca0.16Sr0.6Ba1.5Cu2.78S0.22O7	Y	0.74	Ca	0.16	Sr	0.6	Ba	1.5	Cu	2.78	S	0.22									O	7			1993																												Y123				3.85		11.622																77.9			77.9																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8065	PHC2130014	1065C	(Y,Sr)Sr2(Cu,SO4)3Oz	Y0.84Sr2.16Cu2.78S0.22O7	Y	0.84	Sr	2.16	Cu	2.78	S	0.22													O	7			1993																												Y123																						45			45																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8066	PHC2130014	1000C	(Y,Sr)(Sr,Ba)2(Cu,SO4)3Oz	Y0.84Sr1.16Ba1Cu2.78S0.22O7	Y	0.84	Sr	1.16	Ba	1	Cu	2.78	S	0.22											O	7			1993																												Y123																						78.1			78.1																																																																																														Y2O3, Y2(SO4)3.8H2O, SrCO3, BaCO3, CuO	1	mixture-heat(930-1065C,14H in O2)-pellet-heat(930-1065C,14H in O2)-slow cool to RT					SUPERCONDUCTIVITY IN THE SYSTEM (Y,CA,SR)(BA,SR)2(CU3-Z(SO4)ZOX	199308			PHYSICA C,213(1993)14	C.GREAVES,C.M.MUIRHEAD,M.SLASKI,P.R.SLATER	Y,CA,SR,BA,CU,S,O	
8067	PHC2690001		HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3Oz	Hg	1	Ba	2	Ca	2	Cu	3													O	z			1996																												Hg1223																			120	135		132			135																																		HIR8067																																																														substrate=(100)Y0.15Zr0.85O1.93, gel-covered substrate were calcined at 900C to from the precursor B2Ca2Cu3Oz,-heat(870C,1.5H with Hg in quartz tube)					Giant mass anisotropy and high critical current in Hg-1223 superconducting films			Department of Materials and Interfaces,The Weizmann Institute of Science, Rehovot, Israel	Physica.C,269(1996)1-4	Shimon Reich,Yzhak Tsabba	Hg, Ba, Cu, O, Ca	
8068	PHC2290183	superlatlice=a*4a*2C. was found	(Ca,Sr)3Cu2COz	Ca0.9Sr2.1Cu2C0.75Oz	Ca	0.9	Sr	2.1	Cu	2	C	0.75													O	z			1994																											2					3.851		10.941													92			92			92										20																																																																								2														mixture+KclO3-seal in Au capsule-press(6GPa)-heat (1473K,30min)-Q to RT					High-ressure synthesis of an oxide carbonate superconductor with a Tc of 92K in the Ca-Sr-Cu-C-O system	1994		Institute for Chemical research, Kyoto University, Uji, Kyoto-fu 611, Japan	Physica.C,229(1994)183-187	K. Yamaura,M. Takano,Z. Hiroi		
8069	PHC2270245	(BO3)(Sr,Nd)2CuO2/(BO3)Sr2NdCu2O4, B-1201/B-1212, Cu valence=2.0, insulator	Nd2Sr3Cu3O6(BO3)2	Nd2Sr3Cu3B2O12	Nd	2	Sr	3	Cu	3	B	2													O	12			1994																											2		P4/nnc			7.767		35.828																	5																																																																																																H3BO3, CuO, Nd2O3, SrCO3		mixture-pellet-CAL(650C,12H in O2 flow)-pellet-heat(1030C, 12-24H in 1 atm O2)-Q to RT					Preparation and crystal structure of Nd2Sr3Cu3O6(BO3)2	199407			Physica C, 227(1994)245-253	Hisanori Yamane,Takeo Oku,Toshio Hirai,Yoshiki Amamoto,Yuzuru Miyazaki	Nd,Sr,Cu,O,B	
8070	PHC2270309	as-synthesized, not S/C	Y(Ba,Sr)2(Cu,BO3)3Oz	Y1Ba1Sr1Cu2.5B0.5Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.5											O	z		1	1994																											2	Y123				3.85		11.266																	5																																																																																																Y2CO3, SrCO3, BaCO3, CuO, H3BO3		mixture-heat(1000C,14H in O2)-pellet-heat(1000C 14H in O2)-slow cool to RT					Borate substitution in YSrBaCu3O7 studied by X-ray emission spectroscopy	199407			Physica C, 227(1994)309-312	C.Greaves,E.Z.Kurmaev,P.R.Slater,S.N.Shamin	Y,Sr,Ba,Cu,O,B	
8071	PHC2270309	nneal(425C, 24H in 250 bar O2)	Y(Ba,Sr)2(Cu,BO3)3Oz	Y1Ba1Sr1Cu2.5B0.5Oz	Y	1	Ba	1	Sr	1	Cu	2.5	B	0.5											O	z		1	1994																												Y123																						25			25																																																																																														Y2CO3, SrCO3, BaCO3, CuO, H3BO3		mixture-heat(1000C,14H in O2)-pellet-heat(1000C 14H in O2)-slow cool to RT					Borate substitution in YSrBaCu3O7 studied by X-ray emission spectroscopy	199407			Physica C, 227(1994)309-312	C.Greaves,E.Z.Kurmaev,P.R.Slater,S.N.Shamin	Y,Sr,Ba,Cu,O,B	
8072	PHC2200373	IR shows PO4(3-)	(Y,Ca)Sr(Cu,PO4)3Oz	Y0.7Ca0.3Sr2Cu2.8P0.2O0.8+z	Y	0.7	Ca	0.3	Sr	2	Cu	2.8	P	0.2											O	0.8+z			1994																											2	Y123				3.824		11.36																37			37																																																																																														Y2O3, CaCO3, BaCO3/SrCO3, CuO, NH4H2PO4		mixture-heart(1273-1338K, 16H in O2 flow)-heat(1273-1338K, 16H in O2 flow)-slow cool to RT					Oxyanion derivatives of cuprate superconductors: Superonducting 123 phosphates	199402			Physica C, 220(1994)373-376	C.N.R.Rao,R.Nagarajan,S.Ayyappan	Y,Ca,Ba,Sr,Cu,P,O	
8073	PHC2200373	IR shows PO4(3-)	Y(Ba,Sr)2(Cu,PO4)3Oz	Y1Ba1Sr1Cu2.8P0.2O4+z	Y	1	Ba	1	Sr	1	Cu	2.8	P	0.2											O	4+z			1994																											2	Y123				3.844		11.48																47			47																																																																																														Y2O3, CaCO3, BaCO3/SrCO3, CuO, NH4H2PO4		mixture-heart(1273-1338K, 16H in O2 flow)-heat(1273-1338K, 16H in O2 flow)-slow cool to RT					Oxyanion derivatives of cuprate superconductors: Superonducting 123 phosphates	199402			Physica C, 220(1994)373-376	C.N.R.Rao,R.Nagarajan,S.Ayyappan	Y,Ca,Ba,Sr,Cu,P,O	
8074	PHC2200373	IR shows PO4(3-)	(Y,Ca)(Ba,Sr)2(Cu,PO4)3Oz	Y0.7Ca0.3Ba1Sr1Cu2.8P0.2O0.8+z	Y	0.7	Ca	0.3	Ba	1	Sr	1	Cu	2.8	P	0.2									O	0.8+z			1994																											2	Y123				3.832		11.5															68				68																																																																																														Y2O3, CaCO3, BaCO3/SrCO3, CuO, NH4H2PO4		mixture-heart(1273-1338K, 16H in O2 flow)-heat(1273-1338K, 16H in O2 flow)-slow cool to RT					Oxyanion derivatives of cuprate superconductors: Superonducting 123 phosphates	199402			Physica C, 220(1994)373-376	C.N.R.Rao,R.Nagarajan,S.Ayyappan	Y,Ca,Ba,Sr,Cu,P,O	
8075	PHC2200373	IR shows PO4(3-)	YSr2(Cu,PO4)3Oz	Y1Sr2Cu2.8P0.2O0.8+z	Y	1	Sr	2	Cu	2.8	P	0.2													O	0.8+z			1994																											3	Y123				3.824	3.843	11.35																	23																																																																																																Y2O3, CaCO3, BaCO3/SrCO3, CuO, NH4H2PO4		mixture-heart(1273-1338K, 16H in O2 flow)-heat(1273-1338K, 16H in O2 flow)-slow cool to RT					Oxyanion derivatives of cuprate superconductors: Superonducting 123 phosphates	199402			Physica C, 220(1994)373-376	C.N.R.Rao,R.Nagarajan,S.Ayyappan	Y,Ca,Ba,Sr,Cu,P,O	
8076	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.15	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.15		1998																												Hg1223																				134.7					134.7																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8077	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.16	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.16		1998																												Hg1223																				134.2					134.2																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8078	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.187	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.187		1998																												Hg1223																				135.4					135.4																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8079	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.208	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.208		1998																												Hg1223																				135.8					135.8																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8080	PHC2980049		HgBa2Ca2Cu3Oz	Hg0.75Ba2.07Ca2.07Cu3.11O8.223	Hg	0.75	Ba	2.07	Ca	2.07	Cu	3.11													O	z	8.223		1998																												Hg1223																				133.4					133.4																																																																																																mixture((HgO+3CuO):(BaO+CuO)=1.00:2.00)-pellet-sealed in quartz tube-heat(625-660C,12-48H)					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8081	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.05	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.05		1998																												Hg1201																				93.8					93.8																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8082	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.058	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.058		1998																												Hg1201																				92.1					92.1																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8083	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.062	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.062		1998																												Hg1201																				96.5					96.5																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8084	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.063	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.063		1998																												Hg1201																				93.4					93.4																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8085	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.065	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.065		1998																												Hg1201																				91.6					91.6																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8086	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.079	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.079		1998																												Hg1201																				79.2					79.2																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8087	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.087	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.087		1998																												Hg1201																				70.3					70.3																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8088	PHC2980049		HgBa2CuOz	Hg0.92Ba2.05Cu1.03O4.103	Hg	0.92	Ba	2.05	Cu	1.03															O	z	4.103		1998																												Hg1201																				63.6					63.6																																																																																														HgO, CuO, BaO2		mixture(Hg:Ba:Cu=1.05:2.00:1.00)-pellet-seald in quartz tube-heat(800C,30-150min)-Q to RT					Chemical thermodynamics of Hg1201 and Hg1223 phases	199803		Department of Industrial Chemistry, Faculty of Science and Technology, Science University of Tokyo, 2641 Yamazaki, Noda-shi, chiba 278, Japan	Physica.C,298(1998)49-58	Kazuo Fueki,Tadashi Koyama,Tetsuo Tsuchida		
8089	PHC2130026	Sr2CuO2CO3 type	(Tb,Ba)2CuO2(BO3)	Tb1Ba1Cu1B1O5	Tb	1	Ba	1	Cu	1	B	1													O	5			1993																																3.869		7.387																	4.2																																																																																																							THE SYNTHESIS AND CHARACTERIZATION OF A NEW FAMILY OF SINGLE LAYER CUPRATES  LNBACUO2BO3 (LN=LA,PR,ND,SM,EU AND GD)	199308			PHYSICA C,213(1993)26	J.MAIER,LI RUKANG,R.K.KREMER	R,BA,CU,O,B	
8090	JSC1320163	not S/C	(Hg,Lu)2Ba2LuCu2Ox	Hg1.5Ba2.1Lu1.5Cu2OZ	Hg	1.5	Ba	2.1	Lu	1.5	Cu	2													O	Z			1997																											2	Hg2212				3.846		28.853																	4.5																																																																																																BaO2,R2O3,CuO		mixture-heart(835C,24H in O2)-precursor(Ba2RCu2Oz)+1.75HgO-wraped in Au+capsule-heat(18Kbar,920C,2H)					Synthesis, Structural, and Magnetic Characterization of New Hg2Ba2LnCu2O8-delta Phases with Ln=Nd-Gd, Dy-Lu			Laboratoire de Cristallographie, CNRS, BP 166, 38042 Grenoble Cedex 09, France	J.Solid State Chem.132,(1997)163-172	C. Chaillout,E. Gautier,E.V. Antipov,J.J. Capponi,J.L. Tholence,P. Toulemonde,S.M. Loureiro		
8091	JSC1320163	not S/C	(Hg,Yb)2Ba2YbCu2Ox	Hg1.6Ba1.96Yb1.4Cu2.08OZ	Hg	1.6	Ba	1.96	Yb	1.4	Cu	2.08													O	Z			1997																											2	Hg2212				3.849		28.79																	4.5																																																																																																BaO2,R2O3,CuO		mixture-heart(835C,24H in O2)-precursor(Ba2RCu2Oz)+1.75HgO-wraped in Au+capsule-heat(18Kbar,920C,2H)					Synthesis, Structural, and Magnetic Characterization of New Hg2Ba2LnCu2O8-delta Phases with Ln=Nd-Gd, Dy-Lu			Laboratoire de Cristallographie, CNRS, BP 166, 38042 Grenoble Cedex 09, France	J.Solid State Chem.132,(1997)163-172	C. Chaillout,E. Gautier,E.V. Antipov,J.J. Capponi,J.L. Tholence,P. Toulemonde,S.M. Loureiro		
8092	JSC1320163	not S/C	(Hg,Er)2Ba2ErCu2Ox	Hg1.54Ba1.98Er1.43Cu2.1OZ	Hg	1.54	Ba	1.98	Er	1.43	Cu	2.1													O	Z			1997																											2	Hg2212				3.8582		28.872																	4.5																																																																																																BaO2,R2O3,CuO		mixture-heart(835C,24H in O2)-precursor(Ba2RCu2Oz)+1.75HgO-wraped in Au+capsule-heat(18Kbar,920C,2H)					Synthesis, Structural, and Magnetic Characterization of New Hg2Ba2LnCu2O8-delta Phases with Ln=Nd-Gd, Dy-Lu			Laboratoire de Cristallographie, CNRS, BP 166, 38042 Grenoble Cedex 09, France	J.Solid State Chem.132,(1997)163-172	C. Chaillout,E. Gautier,E.V. Antipov,J.J. Capponi,J.L. Tholence,P. Toulemonde,S.M. Loureiro		
8093	JSC1320163	not S/C	(Hg,Gd)2Ba2GdCu2Oz	Hg1.7Ba2Gd1.3Cu2.05OZ	Hg	1.7	Ba	2	Gd	1.3	Cu	2.05													O	Z			1997																											2	Hg2212				3.8811		28.895																	4.5																																																																																																BaO2,R2O3,CuO		mixture-heart(835C,24H in O2)-precursor(Ba2RCu2Oz)+1.75HgO-wraped in Au+capsule-heat(18Kbar,920C,2H)					Synthesis, Structural, and Magnetic Characterization of New Hg2Ba2LnCu2O8-delta Phases with Ln=Nd-Gd, Dy-Lu			Laboratoire de Cristallographie, CNRS, BP 166, 38042 Grenoble Cedex 09, France	J.Solid State Chem.132,(1997)163-172	C. Chaillout,E. Gautier,E.V. Antipov,J.J. Capponi,J.L. Tholence,P. Toulemonde,S.M. Loureiro		
8094	JSC1320163	not S/C	(Hg,Nd)2Ba2NdCu2Oz	Hg1.9Ba1.8Nd1.3Cu2.6OZ	Hg	1.9	Ba	1.8	Nd	1.3	Cu	2.6													O	Z			1997																											2	Hg2212				3.9021		28.986																	4.5																																																																																																BaO2,R2O3,CuO		mixture-heart(835C,24H in O2)-precursor(Ba2RCu2Oz)+1.75HgO-wraped in Au+capsule-heat(18Kbar,920C,2H)					Synthesis, Structural, and Magnetic Characterization of New Hg2Ba2LnCu2O8-delta Phases with Ln=Nd-Gd, Dy-Lu			Laboratoire de Cristallographie, CNRS, BP 166, 38042 Grenoble Cedex 09, France	J.Solid State Chem.132,(1997)163-172	C. Chaillout,E. Gautier,E.V. Antipov,J.J. Capponi,J.L. Tholence,P. Toulemonde,S.M. Loureiro		
8095	PHC3000033			Bi2Sr2Ca1Cu1.5K0.5O8+z	Bi	2	Sr	2	Ca	1	Cu	1.5	K	0.5											O	8+z			1998																																5.41	5.42	30.76														85					85																																									A		2670			meV	36.5																																																						Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8096	PHC3000033			Bi2Sr2Ca1Cu1.4K0.6O8+z	Bi	2	Sr	2	Ca	1	Cu	1.4	K	0.6											O	8+z			1998																																5.4	5.43	30.72														87					87																																									A		2209			meV	38.2																																																						Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8097	PHC3000033			Bi2Sr2Ca1Cu1.3K0.7O8+z	Bi	2	Sr	2	Ca	1	Cu	1.3	K	0.7											O	8+z			1998																																5.42	5.41	30.69														93					93																																									A		1906			meV	40.4																																																						Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8098	PHC3000141		(Hg,Re)Ba2Ca2Cu3O8	Hg0.97Re0.03Ba2Ca2Cu3O8+z	Hg	0.97	Re	0.03	Ba	2	Ca	2	Cu	3											O	8+z			1998																											2	Hg1223				3.8531		15.6677																130		20	130																																																																																																(mix and CAL without Hg-,Re-oxde)-(mix with HgO,ReO2)-Al2O3 crucible in eacuated quartz anple-melt-growth					Flux growth of Hg1-xRexBa2Can-1CunO2n+2+delta single crystals by self-atmosphere	199805		Max-Planck-Institut fur festkorperforschung, Heisenbergstr. 1, D-70569, Stuttgart, Germany	Physica.C,300(1998)141-150	C.T. Lin,E. Schonherr,K. Peters,M. Cardona,Y. Yan		
8099	PHC3000141		(Hg,Re)Ba2CaCu2O6	Hg0.9Re0.1Ba2Ca1Cu2O6+z	Hg	0.9	Re	0.1	Ba	2	Ca	1	Cu	2											O	6+z			1998																											2	Hg1223				3.8634		12.7723																120		22	120																																																																																																(mix and CAL without Hg-,Re-oxde)-(mix with HgO,ReO2)-Al2O3 crucible in eacuated quartz anple-melt-growth					Flux growth of Hg1-xRexBa2Can-1CunO2n+2+delta single crystals by self-atmosphere	199805		Max-Planck-Institut fur festkorperforschung, Heisenbergstr. 1, D-70569, Stuttgart, Germany	Physica.C,300(1998)141-150	C.T. Lin,E. Schonherr,K. Peters,M. Cardona,Y. Yan		
8100	PHC3000217	sintering time=65H	Bi2(Sr,Hg)2CaCu2O8	Bi2Sr1.7Hg0.3Ca1Cu2Oz	Bi	2	Sr	1.7	Hg	0.3	Ca	1	Cu	2											O	z		1	1998																												Bi2212																			60		85				72.5																																																																																														Bi2O3,SrCO3,CuO,CaCO3,HgO	1	mixture-CAL-press-pellet-SIN(820C,65 or 89H in air					Effect of Hg addition on synthesis of Bi-based superconductors	199805		Superconductivity Research Laboratory, Department of Physics, Barkatullah University, Bhopal-462 026, India	Physica.C,300(1998)217-224	H.S. Tewari,N.K. Gaur,R.K. Singh,Vilas Shelke		
8101	PHC3000217	sintering time=89H	Bi2(Sr,Hg)2CaCu2O8	Bi2Sr1.7Hg0.3Ca1Cu2Oz	Bi	2	Sr	1.7	Hg	0.3	Ca	1	Cu	2											O	z		1	1998																												Bi2212																			72		90				81																																																																																														Bi2O3,SrCO3,CuO,CaCO3,HgO	1	mixture-CAL-press-pellet-SIN(820C,65 or 89H in air					Effect of Hg addition on synthesis of Bi-based superconductors	199805		Superconductivity Research Laboratory, Department of Physics, Barkatullah University, Bhopal-462 026, India	Physica.C,300(1998)217-224	H.S. Tewari,N.K. Gaur,R.K. Singh,Vilas Shelke		
8102	PHC3000217	sintering time=65H	Bi2(Sr,Hg)2Ca2Cu3O10	Bi2Sr1.7Hg0.3Ca2Cu3Oz	Bi	2	Sr	1.7	Hg	0.3	Ca	2	Cu	3											O	z		1	1998																												Bi2223																			64		85				74.5																																																																																														Bi2O3,SrCO3,CuO,CaCO3,HgO	1	mixture-CAL-press-pellet-SIN(820C,65 or 89H in air					Effect of Hg addition on synthesis of Bi-based superconductors	199805		Superconductivity Research Laboratory, Department of Physics, Barkatullah University, Bhopal-462 026, India	Physica.C,300(1998)217-224	H.S. Tewari,N.K. Gaur,R.K. Singh,Vilas Shelke		
8103	PHC3000217	sintering time=89H	Bi2(Sr,Hg)2Ca2Cu3O10	Bi2Sr1.7Hg0.3Ca2Cu3Oz	Bi	2	Sr	1.7	Hg	0.3	Ca	2	Cu	3											O	z		1	1998																												Bi2223																			92		130				111																																																																																														Bi2O3,SrCO3,CuO,CaCO3,HgO	1	mixture-CAL-press-pellet-SIN(820C,65 or 89H in air					Effect of Hg addition on synthesis of Bi-based superconductors	199805		Superconductivity Research Laboratory, Department of Physics, Barkatullah University, Bhopal-462 026, India	Physica.C,300(1998)217-224	H.S. Tewari,N.K. Gaur,R.K. Singh,Vilas Shelke		
8104	PHC3000281	notS/C	Ga(Sr,Ca)2(Yb,Ca)Cu2O7	Ga1Sr1.8Ca0.2Yb0.8Ca0.4Cu2O6.984	Ga	1	Sr	1.8	Ca	0.2	Yb	0.8	Ca	0.4	Cu	2									O	z	6.984		1998																												Ga1212				22.661	5.451	5.413																	5																																																																																																Ga2O3,SrCO3,CaCO3,Yb2O3,CuO	1	mixture-heat(935C,10H in air)-(985-990C,48-72H)-pellet-ANN(600C,10H in air)					Superconductivity, Ca content and oxygen deficiency of Ga(Sr,Ca)2(Yb,Ca)Cu2O7	199805		National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,300(1998)281-286	Akio Watanabe,Akira Ono		
8105	PHC3000281	HIPed sample notS/C	Ga(Sr,Ca)2(Yb,Ca)Cu2O7	Ga1Sr1.8Ca0.2Yb0.8Ca0.4Cu2O6.994	Ga	1	Sr	1.8	Ca	0.2	Yb	0.8	Ca	0.4	Cu	2									O	z	6.994		1998																												Ga1212				22.671	5.452	5.408																	5																																																																																																Ga2O3,SrCO3,CaCO3,Yb2O3,CuO	1	mixture-heat(935C,10H in air)-(985-990C,48-72H)-pellet-ANN(600C,10H in air)					Superconductivity, Ca content and oxygen deficiency of Ga(Sr,Ca)2(Yb,Ca)Cu2O7	199805		National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,300(1998)281-286	Akio Watanabe,Akira Ono		
8106	PHC3000281		Ga(Sr,Ca)2(Yb,Ca)Cu2O7	Ga1Sr1.8Ca0.2Yb0.78Ca0.42Cu2Oz	Ga	1	Sr	1.8	Ca	0.2	Yb	0.78	Ca	0.42	Cu	2									O	z			1998																												Ga1212				22.654	5.448	5.419																20			20																																																																																														Ga2O3,SrCO3,CaCO3,Yb2O3,CuO	1	mixture-heat(935C,10H in air)-(985-990C,48-72H)-pellet-ANN(600C,10H in air)					Superconductivity, Ca content and oxygen deficiency of Ga(Sr,Ca)2(Yb,Ca)Cu2O7	199805		National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,300(1998)281-286	Akio Watanabe,Akira Ono		
8107	PHC3000281	HIPed sample	Ga(Sr,Ca)2(Yb,Ca)Cu2O7	Ga1Sr1.8Ca0.2Yb0.75Ca0.45Cu2Oz	Ga	1	Sr	1.8	Ca	0.2	Yb	0.75	Ca	0.45	Cu	2									O	z			1998																												Ga1212				22.659	5.449	5.42																52			52																																																																																														Ga2O3,SrCO3,CaCO3,Yb2O3,CuO	1	mixture-heat(935C,10H in air)-(985-990C,48-72H)-pellet-ANN(600C,10H in air)					Superconductivity, Ca content and oxygen deficiency of Ga(Sr,Ca)2(Yb,Ca)Cu2O7	199805		National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,300(1998)281-286	Akio Watanabe,Akira Ono		
8156	PHC3010029		LaBa2Cu3O7	La1Ba2Cu3OZ	La	1	Ba	2	Cu	3															O	Z			1998																											3	Y123				3.9014	3.9294	11.789													70.3						70.3																																																																																														La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8157	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.97Fe0.03OZ	La	1	Ba	2	Cu	2.97	Fe	0.03													O	Z			1998																											3	Y123				3.917	3.9205	11.7828													55.2						55.2																																																																																														La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8158	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.94Fe0.06OZ	La	1	Ba	2	Cu	2.94	Fe	0.06													O	Z			1998																											2	Y123				3.9212		11.778													35.9						35.9																																																																																														La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8159	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.9Fe0.1OZ	La	1	Ba	2	Cu	2.9	Fe	0.1													O	Z			1998																											2	Y123				3.9236		11.772													10						10																																																																																														La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8160	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.85Fe0.15OZ	La	1	Ba	2	Cu	2.85	Fe	0.15													O	Z			1998																											2	Y123				3.9272		11.764																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8161	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.75Fe0.25OZ	La	1	Ba	2	Cu	2.75	Fe	0.25													O	Z			1998																											3	Y123				3.9173	3.9332	11.788																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8162	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.5Fe0.5OZ	La	1	Ba	2	Cu	2.5	Fe	0.5													O	Z			1998																											3	Y123				3.9166	3.9361	11.791																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8163	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2.4Fe0.6OZ	La	1	Ba	2	Cu	2.4	Fe	0.6													O	Z			1998																											3	Y123				3.9141	3.9373	11.803																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8164	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu2Fe1OZ	La	1	Ba	2	Cu	2	Fe	1													O	Z			1998																											3	Y123				3.924	3.9392	11.817																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8165	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu1.875Fe1.125OZ	La	1	Ba	2	Cu	1.875	Fe	1.125													O	Z			1998																											3	Y123				3.9314	3.9407	11.822																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8166	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu1.5Fe1.5OZ	La	1	Ba	2	Cu	1.5	Fe	1.5													O	Z			1998																											3					3.9454	3.9539	11.833																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8167	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu1.125Fe1.875OZ	La	1	Ba	2	Cu	1.125	Fe	1.875													O	Z			1998																											2					3.9519		11.832																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8168	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu1Fe2OZ	La	1	Ba	2	Cu	1	Fe	2													O	Z			1998																											2					3.9496		11.838																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8169	PHC3010029		LaBa2(Cu,Fe)3O7	La1Ba2Cu0.75Fe2.25OZ	La	1	Ba	2	Cu	0.75	Fe	2.25													O	Z			1998																											2					3.9538		11.849																	10																																																																																																La2O3, BaCO3, Fe2O3, CuO	1	mixture-Alumina crucible-heat(930C,1day in air)-pellet-heat(930C,1 day)-ANN(350C,1 day)-RT					Structural anomalies in LaBa2Cu3Ox cuprates with iron substitution	199805		National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, Nanjing 210093, China	Physica.C,301(1998)29-38	S.S. Jiang,W.J. Liu,W.M. Chen,X.H. Xiang,X.S. Wu,Y. Li		
8170	PHC3010315		YBa2Cu4O8	Y1Ba2Cu4O8+Z	Y	1	Ba	2	Cu	4															O	8+Z			1998																											3	Y124				3.8407	3.8701	27.231													77						77																																																																																														Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8171	PHC3010315		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.975Fe0.025O8+Z	Y	1	Ba	2	Cu	3.975	Fe	0.025													O	8+Z			1998																											3	Y124				3.8417	3.8727	27.21													66						66																																																																																														Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8172	PHC3010315		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.95Fe0.05O8+Z	Y	1	Ba	2	Cu	3.95	Fe	0.05													O	8+Z			1998																											3	Y124				3.8419	3.8734	27.208													51						51																																																																																														Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8173	PHC3010315		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.925Fe0.075O8+Z	Y	1	Ba	2	Cu	3.925	Fe	0.075													O	8+Z			1998																											3	Y124				3.8428	3.8736	27.2													35						35																																																																																														Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8174	PHC3010315		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.9Fe0.1O8+Z	Y	1	Ba	2	Cu	3.9	Fe	0.1													O	8+Z			1998																											3	Y124				3.8438	3.8743	27.192													10						10																																																																																														Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8175	PHC3010315		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.8Fe0.2O8+Z	Y	1	Ba	2	Cu	3.8	Fe	0.2													O	8+Z			1998																											3	Y124				3.8464	3.8705	29.159																																																																																																																	Y2O3,BaCO3,CuO,Fe2O3		mixture-diluted in 10ml of 96% nitric acid-dry-heat-(700C, in air)-CAL-mix with soduim nitvate-pellet-heat(800C,20H in O2flow-RT(0.5C/min))					Site occupancy and Tc degradation in iron substituted YBa2(Cu1-xFex)4O8+delta	199806		Instituto de Investigaciones en Materiales, UNAM, 04510 Me'xico D.F., Mexico	Physica.C,301(1998)315-325	M. Jimenez,M.L. Marquina,R. Escamilla,R. Gomez,R. Ridaura,S. Aburto,T. Akachi,V. Marquina		
8176	PHC3010155	Cu-valence=2.26	YBa4Cu7O15	Y2Ba4Cu7O15	Y	2	Ba	4	Cu	7															O	15		1	1998																											3	Y247				3.8364	3.8791	50.386																80			80																																																																																														CuO, YBa2Cu3O6		mixture-heat(950Cunder zokbar O2)					Effect of fluorination on the structure and superconducting properties of Y2Ba4CuO14+delta phases	199806		Department of chemistry, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,301(1998)155-164	A.M. Abakumov,E.M. Kopnin,E.V. Antipov,G.Van. Tendeloo,J. Karpinski,M.G. Rozova,M.L. Kovba,O.I. Lebedev,R.V. Shpanchenko,S.N. Putilin		
8177	PHC3010155	Cu-valence=2.02	YBa4Cu7O14	Y2Ba4Cu7O14	Y	2	Ba	4	Cu	7															O	14		1	1998																											3	Y247				3.849	3.8693	50.794																30			30																																																																																														CuO, YBa2Cu3O6		mixture-heat(950C,under 20 kbar O2)-ANN(625C,10H in Ar fiow P(O2)=10E-3 atm)					Effect of fluorination on the structure and superconducting properties of Y2Ba4CuO14+delta phases	199806		Department of chemistry, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,301(1998)155-164	A.M. Abakumov,E.M. Kopnin,E.V. Antipov,G.Van. Tendeloo,J. Karpinski,M.G. Rozova,M.L. Kovba,O.I. Lebedev,R.V. Shpanchenko,S.N. Putilin		
8178	PHC3010155	YBa4Cu7O14:XeF2=1:0.6 two phase	Y2Ba4Cu7(F,O)15	Y2Ba4Cu7F0.6OZ	Y	2	Ba	4	Cu	7	F	0.6													O	Z		2	1998																											3	Y247				3.8499	3.8769	50.664																40			40																																																																																																YBa4Cu7O14+XeF2-mixture-Ni crucible-sealed in Cu yubes-heat(300C,30H)					Effect of fluorination on the structure and superconducting properties of Y2Ba4CuO14+delta phases	199806		Department of chemistry, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,301(1998)155-164	A.M. Abakumov,E.M. Kopnin,E.V. Antipov,G.Van. Tendeloo,J. Karpinski,M.G. Rozova,M.L. Kovba,O.I. Lebedev,R.V. Shpanchenko,S.N. Putilin		
8179	PHC3010155	YBa4Cu7O14:XeF2=1:1.2,  Cu-valence=2.10	Y2Ba4Cu7(F,O)15	Y2Ba4Cu7F1.2OZ	Y	2	Ba	4	Cu	7	F	1.2													O	Z		1	1998																											3	Y247				3.8572	3.8777	51.775																56			56																																																																																																YBa4Cu7O14+XeF2-mixture-Ni crucible-sealed in Cu yubes-heat(300C,30H)					Effect of fluorination on the structure and superconducting properties of Y2Ba4CuO14+delta phases	199806		Department of chemistry, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,301(1998)155-164	A.M. Abakumov,E.M. Kopnin,E.V. Antipov,G.Van. Tendeloo,J. Karpinski,M.G. Rozova,M.L. Kovba,O.I. Lebedev,R.V. Shpanchenko,S.N. Putilin		
8180	PHC3010155	YBa4Cu7O14:XeF2=1:1.7, Cu-valence=2.11	Y2Ba4Cu7(F,O)15	Y2Ba4Cu7F1.7OZ	Y	2	Ba	4	Cu	7	F	1.7													O	Z		1	1998																											3	Y247				3.8576	3.878	51.962																62			62																																																																																																YBa4Cu7O14+XeF2-mixture-Ni crucible-sealed in Cu yubes-heat(300C,30H)					Effect of fluorination on the structure and superconducting properties of Y2Ba4CuO14+delta phases	199806		Department of chemistry, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,301(1998)155-164	A.M. Abakumov,E.M. Kopnin,E.V. Antipov,G.Van. Tendeloo,J. Karpinski,M.G. Rozova,M.L. Kovba,O.I. Lebedev,R.V. Shpanchenko,S.N. Putilin		
8181	PHC3010048		LaBaCaCu3O7	La1Ba1Ca1Cu3O7	La	1	Ba	1	Ca	1	Cu	3													O	7			1998																											2	1113				3.869		11.645																69			69																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8182	PHC3010048		(La,Nd)BaCaCu3O7	La0.75Nd0.25Ba1Ca1Cu3O7	La	0.75	Nd	0.25	Ba	1	Ca	1	Cu	3											O	7			1998																											2	1113				3.866		11.642																55			55																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8183	PHC3010048		NdBaCaCu3O7	Nd1Ba1Ca1Cu3O7	Nd	1	Ba	1	Ca	1	Cu	3													O	7			1998																											2	1113				3.862		11.623																33			33																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8184	PHC3010048		(La,Sm)BaCaCu3O7	La0.75Sm0.25Ba1Ca1Cu3O7	La	0.75	Sm	0.25	Ba	1	Ca	1	Cu	3											O	7			1998																											2	1113				3.865		11.632																71			71																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8185	PHC3010048		(La,Sm)BaCaCu3O7	La0.5Sm0.5Ba1Ca1Cu3O7	La	0.5	Sm	0.5	Ba	1	Ca	1	Cu	3											O	7			1998																											2	1113				3.866		11.621																66			66																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8186	PHC3010048		(La,Sm)BaCaCu3O7	La0.25Sm0.75Ba1Ca1Cu3O7	La	0.25	Sm	0.75	Ba	1	Ca	1	Cu	3											O	7			1998																											2	1113				3.862		11.601																65			65																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8187	PHC3010048		(La,Pr)BaCaCu3O7	La0.8Pr0.2Ba1Ca1Cu3O7	La	0.8	Pr	0.2	Ba	1	Ca	1	Cu	3											O	7		1	1998																											2	1113				3.867		11.639																52			52																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8188	PHC3010048		"""(La,Pr)BaCaCu3O7"""	La0.6Pr0.6Ba1Ca1Cu3O7	La	0.6	Pr	0.6	Ba	1	Ca	1	Cu	3											O	7		1	1998																											2	1113				3.866		11.63																28			28																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8189	PHC3010048		"""(La,Pr)BaCaCu3O7"""	La0.4Pr0.4Ba1Ca1Cu3O7	La	0.4	Pr	0.4	Ba	1	Ca	1	Cu	3											O	7		1	1998																											2	1113				3.87		11.624																14			14																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8190	SSC1080425		(La,Ca)2CaCu2O6	La1.82Ca1.18Cu2O6	La	1.82	Ca	1.18	Cu	2															O	6			1998																												2126																						55			55																																																																																																					IRREVERSIBILITY FIELDS AND CRITICAL CURRENTS FOR PURE AND Y-SUBSTITUTED La1.82Ca1.18Cu2O6 SUPERCONDUCTORS			Physics Department,Nortern Illinois University, Dekalb, IL 60115, U.S.A.	Solid State Commun.108(1998)425	B. Dabrowski,K. Rogacki,P.W. Klamut		
8191	PHC3010048		(La,Dy)BaCaCu3O7	La0.75Dy0.25Ba1Ca1Cu3O7	La	0.75	Dy	0.25	Ba	1	Ca	1	Cu	3											O	7		1	1998																																3.862		11.623																56			56																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8192	PHC3010048		(La,Dy)BaCaCu3O7	La0.5Dy0.5Ba1Ca1Cu3O7	La	0.5	Dy	0.5	Ba	1	Ca	1	Cu	3											O	7		1	1998																																3.86		11.606																55			55																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8193	PHC3010048		(La,Dy)BaCaCu3O7	La0.25Dy0.75Ba1Ca1Cu3O7	La	0.25	Dy	0.75	Ba	1	Ca	1	Cu	3											O	7		2	1998																																																		59			59																																																																																															1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8194	PHC3020010		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1998																											3	Y124				3.8441	3.8727	27.2381													75						75																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8195	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.9Pr0.1Ba2Cu4O8	Y	0.9	Pr	0.1	Ba	2	Cu	4													O	8		1	1998	emu/g	0.0000004			myu-B/Pr	2.45	8.5																				3	Y124				3.841	3.8727														66						66																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8196	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		1	1998	emu/g	0.0000005			myu-B/Pr	2.6	3.8																				3	Y124				3.8449	3.8766	27.2112													60						60																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8197	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.7Pr0.3Ba2Cu4O8	Y	0.7	Pr	0.3	Ba	2	Cu	4													O	8		1	1998	emu/g	0.000000618			myu-B/Pr	2.61	3.3																				3	Y124				3.8495	3.8774	27.205													61						61																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8198	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.6Pr0.4Ba2Cu4O8	Y	0.6	Pr	0.4	Ba	2	Cu	4													O	8		1	1998	emu/g	0.00000021			myu-B/Pr	2.5	2.58																				3	Y124				3.8557	3.8821	27.2181													54						54																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8199	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.5Pr0.5Ba2Cu4O8	Y	0.5	Pr	0.5	Ba	2	Cu	4													O	8		1	1998	emu/g	0.0000007			myu-B/Pr	2.65	2.83																				3	Y124				3.8588	3.8883	27.2404													50						50																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8200	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.4Pr0.6Ba2Cu4O8	Y	0.4	Pr	0.6	Ba	2	Cu	4													O	8		1	1998	emu/g	0.00000084			myu-B/Pr	2.63	7.9																				3	Y124				3.8635	3.889	27.2412													40						40																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by O2-HIP					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8201	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.3Pr0.7Ba2Cu4O8	Y	0.3	Pr	0.7	Ba	2	Cu	4													O	8			1998	emu/g	0.00000096			myu-B/Pr	2.72	10																				3	Y124				3.8673	3.8921	27.265													20						20																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by high pressure O2 technique					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8202	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.2Pr0.8Ba2Cu4O8	Y	0.2	Pr	0.8	Ba	2	Cu	4													O	8			1998	emu/g	0.00000096			myu-B/Pr	2.7	10.5																				3	Y124				3.8751	3.8968	27.2719																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by high pressure O2 technique					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8203	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Y0.1Pr0.9Ba2Cu4O8	Y	0.1	Pr	0.9	Ba	2	Cu	4													O	8			1998	emu/g	0.00000156			myu-B/Pr	2.66	11.8																				3	Y124				3.8797	3.9006	27.2927																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by high pressure O2 technique					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8204	PHC3020010		"""(Y,Pr)Ba2Cu4O8"""	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8			1998	emu/g	0.00000129			myu-B/Pr	2.67	7.3																				3	Y124				3.8851	3.9037	27.3173																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		mixture-pellet-CAL(850-900C in air)-pellet-SIN by high pressure O2 technique					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8205	PHC3020010		YBa4Cu7O15	Y2Ba4Cu7O15-Z	Y	2	Ba	4	Cu	7															O	15-Z			1998																											3	Y247				3.8426	3.8779	50.6168													84						84																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8206	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y1.8Pr0.2Ba4Cu7O15-Z	Y	1.8	Pr	0.2	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000047			myu-B/Pr	3.2	18.9																				3	Y247				3.839	3.8772	50.4991													70						70																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8207	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y1.6Pr0.4Ba4Cu7O15-Z	Y	1.6	Pr	0.4	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000036			myu-B/Pr	2.81	8.3																				3	Y247				3.8426	3.8829	50.58													74						74																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8208	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y1.4Pr0.6Ba4Cu7O15-Z	Y	1.4	Pr	0.6	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000043			myu-B/Pr	2.81	6.5																				3	Y247				3.8355	3.8844	50.5756													63						63																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8209	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y1.2Pr0.8Ba4Cu7O15-Z	Y	1.2	Pr	0.8	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000042			myu-B/Pr	2.9	7																				3	Y247				3.8541	3.8858	50.5726													57						57																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8210	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y1Pr1Ba4Cu7O15-Z	Y	1	Pr	1	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000055			myu-B/Pr	2.92	13																				3	Y247				3.8527	3.8829	50.5932													44						44																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8211	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y0.8Pr1.2Ba4Cu7O15-Z	Y	0.8	Pr	1.2	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000063			myu-B/Pr	2.97	9.3																				3	Y247				3.8613	3.8923	50.5947													33						33																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=9 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8212	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y0.6Pr1.4Ba4Cu7O15-Z	Y	0.6	Pr	1.4	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.000001			myu-B/Pr	2.78	11.7																				3	Y247				3.8721	3.9002	50.6271													10						10																																																																																														"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=6 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8213	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y0.4Pr1.6Ba4Cu7O15-Z	Y	0.4	Pr	1.6	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000123			myu-B/Pr	2.63	7.9																				3	Y247				3.8786	3.9009	50.655																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=6 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8214	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Y0.2Pr1.8Ba4Cu7O15-Z	Y	0.2	Pr	1.8	Ba	4	Cu	7													O	15-Z			1998	emu/g	0.00000132			myu-B/Pr	2.63	7.1																				3	Y247				3.8808	3.9002	50.6388																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=6 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8215	PHC3020010		"""(Y,Pr)2Ba4Cu7O15"""	Pr2Ba4Cu7O15-Z	Pr	2	Ba	4	Cu	7															O	15-Z			1998	emu/g	0.00000101			myu-B/Pr	2.92	15.4																				3	Y247				3.8815	3.9009	50.6403																	4.2																																																																																																"""Pr6O11, Y2O3, BaO2, CuO"""		"""high pressure oxyges technique SIN(980C, P(O2)=6 atm)"""					Synthesis and superonducting properties of (Y1-xPrx)Ba2Cu4O8 and (Y1-xPrx)2Ba4Cu7O15-y compounds	199806		Department of Crystalline Materials Science, Nagoya University, Nagoya 464-01, JApan	Physica.C,302(1998)10-22	A. Matsushita,H. Ikuta,I. Hirabayashi,N. Yamada,S. Horii,S. Katano,S. Morii,T. Matsumoto,U. Mizutani,Y. Funahashi,Y. Kodama,Y. Yamada		
8216	PHC3010017	Tc is defined as maximun ds/dT	YBa2Cu3Oz	Y1Ba2Cu3O6.765	Y	1	Ba	2	Cu	3															O	6.765		1	1998																												Y123																				75.8					75.8																																																																						TP8216																										"""Z=6.765 sample-ANN(175C,10H in H2 gas under 100 Torr"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8217	PHC3010017	Tc is defined as maximun ds/dT	YBa2Cu3HxOz	Y1Ba2Cu3H0.1O6.765	Y	1	Ba	2	Cu	3	H	0.1													O	6.765		1	1998																												Y123																				73					73																																																																						TP8217																										"""Z=6.765 sample-ANN(175C,10H in H2 gas under 100 Torr"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8218	PHC3010017	Tc is defined as maximun ds/dT	YBa2Cu3HxOz	Y1Ba2Cu3H0.24O6.765	Y	1	Ba	2	Cu	3	H	0.24													O	6.765		1	1998																												Y123																				68					68																																																																						TP8218																										"""Z=6.765 sample-ANN(175C,10H in H2 gas under 100 Torr"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8219	PHC3010017		YBa2Cu3Oz	Y1Ba2Cu3O6.795	Y	1	Ba	2	Cu	3															O	6.795		1	1998																												Y123																				82.5					82.5																																																																						TP8219																										"""Z=6.795 sample-predried(100C,30 min, in vac)-closed in capsule with H2 gas (<500 Torr)-ANN(200C,48H)-slow cool to RT"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8220	PHC3010017		YBa2Cu3HxOz	Y1Ba2Cu3H0.1O6.795	Y	1	Ba	2	Cu	3	H	0.1													O	6.795		1	1998																												Y123																				75					75																																																																						TP8220																										"""Z=6.795 sample-predried(100C,30 min, in vac)-closed in capsule with H2 gas (<500 Torr)-ANN(200C,48H)-slow cool to RT"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8221	PHC3010017		YBa2Cu3HxOz	Y1Ba2Cu3H0.2O6.795	Y	1	Ba	2	Cu	3	H	0.2													O	6.795		1	1998																												Y123																				72.5					72.5																																																																						TP8221																										"""Z=6.795 sample-predried(100C,30 min, in vac)-closed in capsule with H2 gas (<500 Torr)-ANN(200C,48H)-slow cool to RT"""					The change of Tc(onset) in YBa2Cu3O7-y due to hydrogenation	19805		W. Trzebiatowski Institute for Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 937,50-950 Wroclaw 2, Poland	Physica.C,301(1998)17-22	H. Drulis,J. Klamut,T. Cichorek,Z. Henkie		
8222	PHC3020137	"""HIP at 1080C, sub phase=CuTl1234"""	"""(Cu,Tl)Ba2Ca2Cu3O11"""	Cu0.25Tl0.75Ba2Ca2Cu3O11-Z	Cu	0.25	Tl	0.75	Ba	2	Ca	2	Cu	3											O	11-Z			1998																												Cu1223																				108					108																																																																																																"""precursor(Ba2CaCu2Oz,Ba2Ca2Cu3Oz,Ba2Ca3Cu4Oz)+Tl2O3-mixture-packing(Au capsule)-HIP"""					Synthesis of Cu1-xTlxBa2Ca2Cu3O11-y(x~0,7) superconductor by hot press	199806		Electrotechnical Laboratories, 1-1-4 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica.C,302(1998)137-142	H. Hirabayashi,H. Ihara,H. Yamamoto,K. Tanaka,K. Tokiwa,M. Tokumoto,Nawazish A. Khan		
8223	PHC3020137	"""HIP at 1000C, sub phase=CuTl1234"""	"""(Cu,Tl)Ba2Ca2Cu3O11"""	Cu0.25Tl0.75Ba2Ca2Cu3O11-Z	Cu	0.25	Tl	0.75	Ba	2	Ca	2	Cu	3											O	11-Z			1998																												Cu1223																				121					121																																																																																																"""precursor(Ba2CaCu2Oz,Ba2Ca2Cu3Oz,Ba2Ca3Cu4Oz)+Tl2O3-mixture-packing(Au capsule)-HIP"""					Synthesis of Cu1-xTlxBa2Ca2Cu3O11-y(x~0,7) superconductor by hot press	199806		Electrotechnical Laboratories, 1-1-4 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica.C,302(1998)137-142	H. Hirabayashi,H. Ihara,H. Yamamoto,K. Tanaka,K. Tokiwa,M. Tokumoto,Nawazish A. Khan		
8224	PHC3020137	"""HIP at 1030C, sub phase=CuTl1234"""	"""(Cu,Tl)Ba2Ca2Cu3O11"""	Cu0.25Tl0.75Ba2Ca2Cu3O11-Z	Cu	0.25	Tl	0.75	Ba	2	Ca	2	Cu	3											O	11-Z			1998																												Cu1223																				117					117																																																																																																"""precursor(Ba2CaCu2Oz,Ba2Ca2Cu3Oz,Ba2Ca3Cu4Oz)+Tl2O3-mixture-packing(Au capsule)-HIP"""					Synthesis of Cu1-xTlxBa2Ca2Cu3O11-y(x~0,7) superconductor by hot press	199806		Electrotechnical Laboratories, 1-1-4 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica.C,302(1998)137-142	H. Hirabayashi,H. Ihara,H. Yamamoto,K. Tanaka,K. Tokiwa,M. Tokumoto,Nawazish A. Khan		
8225	PHC3030001		"""(Cu,Ti)Sr2(Y,Ce)2Cu2Oz"""	Cu0.75Ti0.25Sr2Y1.3Ce0.7Cu2O8.71	Cu	0.75	Ti	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.71		1998																											2	Cu1222				3.8163		28.595																21			21																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8226	PHC3030001		"""(Cu,V)Sr2(Y,Ce)2Cu2Oz"""	Cu0.75V0.25Sr2Y1.3Ce0.7Cu2O8.77	Cu	0.75	V	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.77		1998																											2	Cu1222				3.826		28.2914																24.5			24.5																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8227	PHC3030001		"""(Cu,Cr)Sr2(Y,Ce)2Cu2Oz"""	Cu0.75Cr0.25Sr2Y1.3Ce0.7Cu2O8.87	Cu	0.75	Cr	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.87		1998																											2	Cu1222				3.8366		28.154																8			8																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8228	PHC3030001		"""(Cu,Fe)Sr2(Y,Ce)2Cu2Oz"""	Cu0.75Fe0.25Sr2Y1.3Ce0.7Cu2O8.49	Cu	0.75	Fe	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.49		1998																											2	Cu1222				3.8065		28.433																	4.2																																																																																																		"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8229	PHC3030001		"""(Cu,Co)Sr2(Y,Ce)2Cu2Oz"""	Cu0.75Co0.25Sr2Y1.3Ce0.7Cu2O8.43	Cu	0.75	Co	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.43		1998																											2	Cu1222				3.8077		28.468																24			24																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8230	PHC3030001		(Cu,Ga,)Sr2(Y,Ce)2Cu2Oz	Cu0.75Ga0.25Sr2Y1.3Ce0.7Cu2O8.6	Cu	0.75	Ga	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.6		1998																											2	Cu1222				3.8179		28.649																12			12																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8231	PHC3030001		(Cu,Ge)Sr2(Y,Ce)2Cu2Oz	Cu0.75Ge0.25Sr2Y1.3Ce0.7Cu2O8.59	Cu	0.75	Ge	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.59		1998																											2	Cu1222				3.8131		28.458																17.5			17.5																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8232	PHC3030001		(Cu,Mo)Sr2(Y,Ce)2Cu2Oz	Cu0.75Mo0.25Sr2Y1.3Ce0.7Cu2O8.76	Cu	0.75	Mo	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.76		1998																											2	Cu1222				3.8143		28.522																	4.2																																																																																																		"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8233	PHC3030001		(Cu,Ce)Sr2(Y,Ce)2Cu2Oz	Cu0.75Ce0.25Sr2Y1.3Ce0.7Cu2O8.91	Cu	0.75	Ce	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.91		1998																											2	Cu1222				3.8198		29.107																10			10																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8234	PHC3030001		(Cu,W)Sr2(Y,Ce)2Cu2Oz	Cu0.75W0.25Sr2Y1.3Ce0.7Cu2O8.81	Cu	0.75	W	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	8.81		1998																											2	Cu1222				3.8102		28.395																31.5			31.5																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8235	PHC3030001		(Cu,Re)Sr2(Y,Ce)2Cu2Oz	Cu0.75Re0.25Sr2Y1.3Ce0.7Cu2O9.06	Cu	0.75	Re	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z	9.06		1998																											2	Cu1222				3.8159		28.371																33.5			33.5																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8236	PHC3030001	"""ANN(1000C,20H under high pressure(100Kgf/cm2)O2)"""	(Cu,Mo)Sr2(Y,Ce)2Cu2Oz	Cu0.75Mo0.25Sr2Y1.3Ce0.7Cu2OZ	Cu	0.75	Mo	0.25	Sr	2	Y	1.3	Ce	0.7	Cu	2									O	Z			1998																											2	Cu1222																						40			40																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8237	PHC3030001		(Cu,Re)Sr2(Y,Ce)2Cu2Oz	Cu0.85Re0.15Sr2Y1.5Ce0.5Cu2OZ	Cu	0.85	Re	0.15	Sr	2	Y	1.5	Ce	0.5	Cu	2									O	Z			1998																												Cu1222																						43			43																																																																																																"""mixture-pellet-heat(1000C,20H in air)-SIN(1050C,10H in O2)-ANN(700C,20H under high pressure(100kgf/cm2)O2)"""					A new Superconductor with 1222 structure (Cu1-xMx)Sr2(Y1-yCey)2Cu2Odelta(M=Ti,V,Cr,Fe,Co,Ga,Ge,Mo,Ce,W and Re)	199807		Department of Physics, Aoyama-gakuin University, Setagaya-ku, Tokyo 157, Japan	Physica.C,303(1998)1-10	J.Akimitsu,M.Sato,M.Tamura,T.Den		
8238	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.6Pb0.4Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.6	Pb	0.4	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4532		17.9582														31.5					31.5																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8239	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.55Pb0.45Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.55	Pb	0.45	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4517		17.9701														33					33																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8240	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.5Pb0.5Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.5	Pb	0.5	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4469		17.982														33					33										22																																																																																				"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8241	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.45Pb0.55Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.45	Pb	0.55	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.446		17.978														34					34																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8242	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.4Pb0.6Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.4	Pb	0.6	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4408	5.4469	17.978														35					35																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8243	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.3Pb0.7Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.3	Pb	0.7	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4278	5.4521	17.9801														37					37																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8244	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.2Pb0.8Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.2	Pb	0.8	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.414	5.456	17.98														38.5					38.5																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8245	PHC3020325		(Bi,Pb)2Sr2(Eu,Ce)2Cu2Oz	Bi1.1Pb0.9Sr2Eu1.65Ce0.35Cu2OZ	Bi	1.1	Pb	0.9	Sr	2	Eu	1.65	Ce	0.35	Cu	2									O	Z		1	1998																											3	Bi2222				5.4132	5.4587	17.978														38					38																																																																																														"""Bi2O3, PbP, SrCO3, Eu2O3, CeO2, CuO"""		"""mixture-pellet-heat(900C,16H in air)-pellet-SIN(990C,16H in O2)-RT(0.3C/min)"""					Superconductivity and stuructural change in the (Bi2-yPby)Sr2(Eu2-xCex)Cu2Oz system	199807		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431-3192, Japan	Physica.C,302(1998)325-330	Hiroyuki Sasakura,Keisuke Kawabata,Ken-ichi Yoshida,Takashi Oka,Yoshikazu Hayashi		
8246	PHC3020244		(Cu,Cr)Sr2Ca5Cu6Oz	Cu6.5Sr2Ca5Cr0.5O15.17	Cu	6.5	Sr	2	Ca	5	Cr	0.5													O	Z	15.17	1	1998																											2	Cu1256				3.8651		24.192																32			32																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8247	PHC3020244		(Cu,Cr)Sr2Ca6Cu7Oz	Cu7.5Sr2Ca6Cr0.5O17.1	Cu	7.5	Sr	2	Ca	6	Cr	0.5													O	Z	17.1	2	1998																											2	Cu1267				3.8667		27.602																10			10																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8248	PHC3020244		(Cu,Cr)Sr2Ca7Cu8Oz	Cu8.5Sr2Ca7Cr0.5O19.05	Cu	8.5	Sr	2	Ca	7	Cr	0.5													O	Z	19.05	1	1998																											2	Cu1278				3.868		30.6																	4.2																																																																																																							New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8249	PHC3020244		(Cu,Cr)Sr2Ca8Cu9Oz	Cu9.5Sr2Ca8Cr0.5O21.05	Cu	9.5	Sr	2	Ca	8	Cr	0.5													O	Z	21.05	1	1998																											2	Cu1289				3.868		33.97																	4.2																																																																																																							New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8250	PHC3020244		(Cu,Cr)Sr2CuOz	Cu1.5Sr2Cr0.5O5.3	Cu	1.5	Sr	2	Cr	0.5															O	Z	5.3	1	1998																											2	Cu1201				3.9061		8.193																	4.2																																																																																																							New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8251	PHC3020244		(Cu,Cr)Sr2CaCu2Oz	Cu2.5Sr2Ca1Cr0.5O7.5	Cu	2.5	Sr	2	Ca	1	Cr	0.5													O	Z	7.5	1	1998																											2	Cu1212				3.8669		11.396																81			81																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8252	PHC3020244		(Cu,Cr)Sr2Ca2Cu3Oz	Cu3.5Sr2Ca2Cr0.5O9.55	Cu	3.5	Sr	2	Ca	2	Cr	0.5													O	Z	9.55	1	1998																											2	Cu1223				3.8577		14.575																103			103																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8253	PHC3020244		(Cu,Cr)Sr2Ca3Cu4Oz	Cu4.5Sr2Ca3Cr0.5O11.45	Cu	4.5	Sr	2	Ca	3	Cr	0.5													O	Z	11.45	1	1998																											2	Cu1234				3.8593		17.776																71			71																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8254	PHC3020244		(Cu,Cr)Sr2Ca4Cu5Oz	Cu5.5Sr2Ca4Cr0.5O13.35	Cu	5.5	Sr	2	Ca	4	Cr	0.5													O	Z	13.35	1	1998																											2	Cu1245				3.8614		20.975																65			65																																																																																																					New series of high-Tc Cr-based superconductors	199806		National Institute Research in Inorganic Materials, Namiki1-1, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,302(1998)244-256	E. Takayama-Muromachi,S.M. Loureiro,Y. Matsui		
8255	PHC3030041		"""Sr2Cu(O,Cl)4"""	Sr2Cu1Cl1.2O4.	Sr	2	Cu	1	Cl	1.2															O	4.0		1	1998																											2	0201				3.928		15.57																																																																																					uV/K	43			TP8255																															High pressure synthesis of SrCuO2+delta' compounds	199807		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome, 1-Chome Koto-ku, Tikyo 135-0062, Japan	Physica.c,303(1998)41-46	K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki		
8256	MRB0330825	not s/c	(La,Sr)2(Ca,Pr)Cu2O6	La1.6Sr0.4Ca0.5Pr0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Pr	0.5	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.839		19.54	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8257	MRB0330825	not s/c	(La,Sr)2(Ca,Eu)Cu2O6	La1.6Sr0.4Ca0.5Eu0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Eu	0.5	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.837		19.55	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8258	MRB0330825	not s/c	(La,Sr)2(Ca,Gd)Cu2O6	La1.6Sr0.4Ca0.5Gd0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Gd	0.5	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.827		19.5	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8259	MRB0330825	not s/c	(La,Sr)2(Ca,Tb)Cu2O6	La1.6Sr0.4Ca0.5Tb0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Tb	0.5	Cu	2											O	6-Z		1	1998																												2126	I4/mmm			3.829		19.53	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8260	MRB0330825	not s/c	(La,Sr)2(Ca,Y)Cu2O6	La1.6Sr0.4Ca0.5Yb0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Yb	0.5	Cu	2											O	6-Z		1	1998																												2126	I4/mmm			3.82		19.5	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8261	MRB0330825	not s/c	(La,Sr)2(Ca,Er)Cu2O6	La1.6Sr0.4Ca0.5Er0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Er	0.5	Cu	2											O	6-Z		1	1998																												2126	I4/mmm			3.831		19.54	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8262	MRB0330825	not s/c	(La,Sr)2(Ca,Tm)Cu2O6	La1.6Sr0.4Ca0.5Tm0.5Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.5	Tm	0.5	Cu	2											O	6-Z		1	1998																												2126	I4/mmm			3.825		19.53	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8263	MRB0330825	not s/c	(La,Sr)2(Ca,La)Cu2O6	La1.6Sr0.4Ca0.6La0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	La	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.839		19.65	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8264	MRB0330825	not s/c	(La,Sr)2(Ca,Nd)Cu2O6	La1.6Sr0.4Ca0.6Nd0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	Nd	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.836		19.56	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8265	MRB0330825	not s/c	(La,Sr)2(Ca,Sm)Cu2O6	La1.6Sr0.4Ca0.6Sm0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	Sm	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.835		19.55	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8266	MRB0330825	not s/c	(La,Sr)2(Ca,Dy)Cu2O6	La1.6Sr0.4Ca0.6Dy0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	Dy	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.828		19.51	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8267	MRB0330825	not s/c	(La,Sr)2(Ca,Ho)Cu2O6	La1.6Sr0.4Ca0.6Ho0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	Ho	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.833		19.56	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8268	MRB0330825	not s/c	(La,Sr)2(Ca,Yb)Cu2O6	La1.6Sr0.4Ca0.6Yb0.4Cu2O6-Z	La	1.6	Sr	0.4	Ca	0.6	Yb	0.4	Cu	2											O	6-Z		1	1998																											2	2126	I4/mmm			3.821		19.5	3																10																																																																																																La2O3, SrCO3, CaCO3, CuO		mixture-CAL(800-900C, 15-20H, in air)-pellet-SIN(980-1030C,40H)-slow cooling to RT					Rare-earth substituted 212-type compounds (La,Sr)2CaCu2O6.				Mat. Res. Bull., 33(1998)825	F. Wu,F.Tao,G.C. Che,G.D.Liu,X.L. Chen,Y.Z. Zhang,Z.X. Zhao		
8269	MRB0331241		La(Ba,Sr)2Cu3O7	La1Ba1.5Sr0.5Cu3O7-Z	La	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											2	Y123				3.8932		11.759	3												52.4					8.8	52.4																																																																							mOhm.cm							9.76																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8270	MRB0331241		Nd(Ba,Sr)2Cu3O7	Nd1Ba1.5Sr0.5Cu3O7-Z	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											2	Y123				3.8887		11.689	3												56.4					10.2	56.4																																																																							mOhm.cm							6.7																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8271	MRB0331241		Sm(Ba,Sr)2Cu3O7	Sm1Ba1.5Sr0.5Cu3O7-Z	Sm	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8424	3.8836	11.657	3												70.7					8.3	70.7																																																																							mOhm.cm							3.37																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8272	MRB0331241		Eu(Ba,Sr)2Cu3O7	Eu1Ba1.5Sr0.5Cu3O7-Z	Eu	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8361	3.883	11.655	3												76.8					6.4	76.8																																																																							mOhm.cm							4.03																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8273	MRB0331241		Gd(Ba,Sr)2Cu3O7	Gd1Ba1.5Sr0.5Cu3O7-Z	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8285	3.8782	11.654	3												85.6					1.7	85.6																																																																							mOhm.cm							2.92																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8274	MRB0331241		Dy(Ba,Sr)2Cu3O7	Dy1Ba1.5Sr0.5Cu3O7-Z	Dy	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8068	3.8743	11.632	3												86.5					1.1	86.5																																																																							mOhm.cm							2.25																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8275	MRB0331241		Ho(Ba,Sr)2Cu3O7	Ho1Ba1.5Sr0.5Cu3O7-Z	Ho	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8042	3.8739	11.61	3												86.8					1.5	86.8																																																																							mOhm.cm							1.43																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8276	MRB0331241		Y(Ba,Sr)2Cu3O7	Y1Ba1.5Sr0.5Cu3O7-Z	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.7976	3.8725	11.606	3												87.4					2.3	87.4																																																																							mOhm.cm							1.32																La2O3, SrCO3, BaCO3, CuO		mixture-CAL(950C, 14H, in air)-pellet-SIN(960C,12H,in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8277	SUP0110123	reduced sample,Tc=61K for as-sintered	TlSr2Ba2Cu2(CO3,NO3)O7	Tl1Sr2Ba2Cu2C2.7N0.3O7	Tl	1	Sr	2	Ba	2	Cu	2	C	2.7	N	0.3									O	7		1	1998																											3	Tl1222	Ammm			3.921	30.397	16.725	3															49			49																																																																																														Tl2O3, SrO2, Sr2CuO3, BaCuO2, SrCO3, CuO		mixture-plased in alumina tubes-sealed in evacuated quartz ampoules-fire(850C,48H)-Q in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8278	SUP0110123	reduced sample,Tc=61K for as-sintered	TlSr2Ba2Cu2(CO3,NO3)O7	Tl1Sr2Ba2Cu2C2.4N0.6O7	Tl	1	Sr	2	Ba	2	Cu	2	C	2.4	N	0.6									O	7			1998																											3	Tl1222	Ammm			3.921	30.937	16.725	3															49			49																																																																																														Tl2O3, SrO2, Sr2CuO3, BaCuO2, SrCO3, CuO		mixture-plased in alumina tubes-sealed in evacuated quartz ampoules-fire(850C,48H)-Q in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8279	SUP0110123	reduced sample,Tc=40K for as-sintered sample	(Tl,Pb)Sr4Cu2(CO3,NO3)O7	Tl0.5Pb0.5Sr4Cu2C0.9N0.1O7	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	0.9	N	0.1									O	7		1	1998																												Tl1222				3.821		16.503											inpurity phase=SrCO3, (Tl,Pb)Sr2CuO5					76			76																																																																																														Tl2O3, SrO2, Sr2CuO3, BaCuO2, SrCO3, CuO		mixture-plased in alumina tubes-sealed in evacuated quartz ampoules-fire(850C,48H)-Q in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8280	SUP0110123	reduced sample,Tc=28K for as-sintered sample	(Tl,Pb)Sr4Cu2(CO3,NO3)O7	Tl0.5Pb0.5Sr4Cu2C0.7N0.3O7	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	0.7	N	0.3									O	7		1	1998																												Tl1222				3.821		16.503											inpurity phase=SrCO3, (Tl,Pb)Sr2CuO5					70			70																																																																																														Tl2O3, SrO2, Sr2CuO3, BaCuO2, SrCO3, CuO		mixture-plased in alumina tubes-sealed in evacuated quartz ampoules-fire(850C,48H)-Q in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8281	SUP0110123	reduced sample,Tc=24K for as-sintered sample	(Tl,Pb)Sr4Cu2(CO3,NO3)O7	Tl0.5Pb0.5Sr4Cu2C0.5N0.5O7	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	0.5	N	0.5									O	7			1998																												Tl1222				3.821		16.503																70			70																																																																																														Tl2O3, SrO2, Sr2CuO3, BaCuO2, SrCO3, CuO		mixture-plased in alumina tubes-sealed in evacuated quartz ampoules-fire(850C,48H)-Q in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8282	SUP0110159	thickness=0.6 micron	(Tl,Bi)(Sr,Ba)2Ca2Cu3O9	Tl0.78Bi0.22Sr1.6Ba0.4Ca2Cu3O9-Z	Tl	0.78	Bi	0.22	Sr	1.6	Ba	0.4	Ca	2	Cu	3									O	9-Z		4	1998																												Tl1223																			106		110				108																																																			100000																																													two-step. Film by laser ablation, ANN(780-800C,40-60 min,in Ar flow	17	YSZ	Tl1.8Bi0.22Sr1.6Ba0.4Ca2.2Cu3.3O10.5		Epitaxial Film Growth of Tl0.78Bi0.22Sr1.6Ba0.4Ca2Cu3O9 on Rolling Assisted Biaxially Textured Nickel Substrates with YSZ and CeO2Buffer Layers	1998		Materials Synthesis Laboratory, Department of Chemistry and New York State Institute on Superconductivity, State University of NewYork, Buffalo, NY 14260-3000	J.Superconductivity,11(1998)159	A. Goyal,D.K. Christen,E.D. Specht,J.D. Budai,J.H. Wang,J.R. Thompson,J.Y. Lao.,L.P. Guo,M. Paranthaman,Z.F. Ren		
8283	SUP0110141	inpurity=Li2CuO2	(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1O4+Z	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	4+Z		2	1998																												Hg1201	P4/mmm		A	3.8439		8.6978	3															63			63		2								55																																																																																				Cr2O3, SrCO3, CuO, HgO		precursor(Cr-Sr-Cu-O)-mixed with HgO-wrap in Au foil-seal in quartz ampoule-heat(880C,8H)-Q to RT-ANN(in O2 flow)					Synthe sis and Structure of Hg1-xCrxSr2CuO4+delta Mercurocuprates	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2TT, UK	J.Superconductivity,11(1998)141	G.P. Peacock,I. Gameson,J.A. Hriljac,M. Slaski,M.O. Jones,Neil C. Hyatt,Peter P. Edwards		
8284	SUP0100231	inpurity=Li2CuO2	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.02O7	Y	1	Ba	2	Cu	3	Li	0.02													O	7		1	1997																												Y123																				91.18					91.18											Oe	deviation from linear region in M vs H					78.5		77																																																																											Y2O3, BaCO3, CuO,LiOH		Fire(890C,20H, in O2 flow)-press into bar-SIN(936C,16H)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
8285	SUP0100231	inpurity=Li2CuO2	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.08O7	Y	1	Ba	2	Cu	3	Li	0.08													O	7		1	1997																												Y123																				89.2					89.2																	33.7		77																																																																											Y2O3, BaCO3, CuO,LiOH		Fire(890C,20H, in O2 flow)-press into bar-SIN(936C,16H)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
8286	SUP0100231		YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.1O7	Y	1	Ba	2	Cu	3	Li	0.1													O	7		1	1997																																																88.91					88.91																	47.9		77																																																																											Y2O3, BaCO3, CuO,LiOH		Fire(890C,20H, in O2 flow)-press into bar-SIN(936C,16H)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
8287	SUP0100231	inpurity phases=Y2BaCuO5, CuO, Cu2O	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.3O7	Y	1	Ba	2	Cu	3	Li	0.3													O	7		1	1997																																																86					86																																																																																														Y2O3, BaCO3, CuO,LiOH		Fire(890C,20H, in O2 flow)-press into bar-SIN(936C,16H)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
8288	SUP0100231	inpurity phases=CuO, Li2CuO2	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.5O7	Y	1	Ba	2	Cu	3	Li	0.5													O	7		1	1997																																																83.79					83.79																																																																																														Y2O3, BaCO3, CuO,LiOH		Fire(890C,20H, in O2 flow)-press into bar-SIN(936C,16H)					The Effect of liOH Addition to the Superconducting Properties of YBa2Cu3O7-x			National Institute of Research and Development for Materials Physics, Bucharest-Magurele, P.O. Box MG7, Romania	J.Superconductivity,10(1997)231	Elena Cimpoiasu,J. Jaklovszky,Mihaela Carmen Bunescu,V. Sandu		
8289	SUP0110059		HgBa2CuO4+z	Hg1Ba2Cu1O4.08	Hg	1	Ba	2	Cu	1															O	4	4.08	1	1998																											2	Hg1201				3.8928		9.5528	2															96			96		2								75																																																																																				BaO, CuO, HgO		mixture(Hg:Ba:Cu=1.1:2:1)-press-(in alumina crucible)-seal in quartz ampoule(7Pa)-SIN(780C.10H)-oxygenation(350C,10H)					Nautron and Raman Scattering Studies of HgBa2CuO4+delta	199805		Department of Physics and Astronomy, University of Nebraska, Lincoln, NE 68588, USA	J.Superconductivity,11(1998)59	A.L. Vasiliev,E.P. Kvam,H.Luo,M. Chandrasekhar,M. Chen,Q. Cai,R. Li,S.H. Liou,W.B. Yelon		
8290	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.4K0.6O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.4	K	0.6											O	8+Z		1	1998																											3	Bi2212				5.41	5.42	30.76														85					85																																									A	x-band ESR	2670																																																					sol-gel method, final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8291	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.3K0.7O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.3	K	0.7											O	8+Z		1	1998																											3	Bi2212				5.4	5.43	30.72														87					87																																									A	x-band ESR	2209																																																					sol-gel method, final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8292	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.2K0.8O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.2	K	0.8											O	8+Z		1	1998																											3	Bi2212				5.42	5.41	30.69														93					93																																									A	x-band ESR	1906																																																					sol-gel method, final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8293	PHC3070265		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.218	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.218	3	1998																												Bi2212																				70					70																																									A	reversible M-H curve,Londoneq		3480																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8294	SSC1050155		YBa2Cu3O7	Y1Ba2Cu3O7+Z	Y	1	Ba	2	Cu	3															O	7+Z		4	1998																												Y123																							90																																											A	micro ware dielectric resonator		2700																																																				by laser ablation					THERMAL FLUCTUATION OF THE ORDER PARAMETER SYMMETRY IN HIGH Tc SUPERCONDUCTORS REVEALED FROM THE PENETRATION DEPTH MEASUREMENT			Department of Physics, National Tsing Hua University, Hsinchu Taiwan	Solid State Commun.105(1998)155-159	Juh Tzeng Lue,Li Jui Chen		
8295	SSC1060231	5wt% Ag-doped YBCO	Ag-YBa2Cu3O7	Y1Ba2Cu3O7+Z	Y	1	Ba	2	Cu	3															O	7+Z		4	1998																												Y123																			89.5					0.5	89.5																																									A	microweve velocity	1400																																																					pulse laser ablation using Ag-doped YBCO target, thickness-0.5mm					MICROWAVE PENETRATION DEPTH MEASUREMENTS OF Ag-YBa2Cu3O7-delta THIN FILMS			Tata Institute of Fundamental Research, Homi Bhabha Road, Munbai-400 005, India	Solid State Commun.106(1998)231-234	Davinder Kaur,H.W. Weber,R. Pinto		
8296	PRL0812140	Hg layer-Hg0.8Cu0.2 by EDX	(Hg,Cu)Ba2CuO4+z	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1998																												Hg1201																																																																		microm	direct measurement of vortex			8																																																			precursor(Ba-Cu-O)+HgO-Almina crucible-sealed in silica tube-heat(48H)					c-Axis Penetration Depth of Hg-1201 Single Crystals	9		IBM T.J. Watson Research Center, P.O. Box 278, Yorktown Heights, New York 10598	Phy.Rev.Lett81(1998)2140	A. Maignan,G. Villard,J.R. Kirtley,K.A. Moler		
8297	PHC2970103	anisotropy=75	HgBa2CuO4+z	Hg1Ba2Cu1O4.049	Hg	1	Ba	2	Cu	1															O	4+Z	4.049	3	1998																												Hg1201																						70			70																																				A			33		A			2160																																																				as-grown samples were annealed in Ar					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8298	PHC2970103	anisotropy=64	HgBa2CuO4	Hg1Ba2Cu1O4.055	Hg	1	Ba	2	Cu	1															O	4+Z	4.055	3	1998																												Hg1201																						78.2			78.2																																				A			34		A			1610																																																				as-grown samples were annealed in Ar					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8299	PHC2970103	anisotropy=46	HgBa2CuO4+z	Hg1Ba2Cu1O4.066	Hg	1	Ba	2	Cu	1															O	4+Z	4.066	3	1998																												Hg1201																						88.5			88.5																																				A			23		A			1530																																																				as-grown samples were annealed in Ar					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8300	PHC2970103	anisotropy=27	HgBa2CuO4+z	Hg1Ba2Cu1O4.096	Hg	1	Ba	2	Cu	1															O	4+Z	4.096	3	1998																												Hg1201																						95.6			95.6																																				A			20		A			1450																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8301	PHC2970103	anisotropy=26.6	HgBa2CuO4+z	Hg1Ba2Cu1O4.097	Hg	1	Ba	2	Cu	1															O	4+Z	4.097	3	1998																												Hg1201																						95.3			95.3																																				A			20		A			1650																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8302	PHC2970103	anisotropy=26.7	HgBa2CuO4+z	Hg1Ba2Cu1O4.1	Hg	1	Ba	2	Cu	1															O	4+Z	4.1	3	1998																												Hg1201																						94.1			94.1																																				A			22		A			1580																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8303	PHC2970103	anisotropy=25.5	HgBa2CuO4+z	Hg1Ba2Cu1O4.101	Hg	1	Ba	2	Cu	1															O	4+Z	4.101	3	1998																												Hg1201																						93.4			93.4																																	1.5			A			18		A			1560																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8304	PHC2970103	anisotropy=25.0	HgBa2CuO4	Hg1Ba2Cu1O4.103	Hg	1	Ba	2	Cu	1															O	4+Z	4.103	3	1998																												Hg1201																						92.5			92.5																																				A			20		A			1390																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8305	PHC2970103	anisotropy=25.1	HgBa2CuO4	Hg1Ba2Cu1O4.105	Hg	1	Ba	2	Cu	1															O	4+Z	4.105	3	1998																												Hg1201																						90.9			90.9																																				A			17		A			1560																																																				as grown sample					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8306	PHC2970103	anisotropy=22.6	HgBa2CuO4	Hg1Ba2Cu1O4.108	Hg	1	Ba	2	Cu	1															O	4+Z	4.108	3	1998																												Hg1201																						89.1			89.1																																				A			18		A			1770																																																				as-grown samples were annealed in O2					Doping dependence of superconducting parameters in HgBa2CuO4+delta single crystals	199803		Physik-Institut der Universitat Zurich, CH08057 Zurich, Swizerland	Physica.C,297(1998)103-110	C. Rossel,E.M. Kopnin,G.I. Meijer,H. Keller,H. Schwer,J. Hofer,J. Karpinski,M. Willemin,R. Molinski		
8307	MRB0331241		R(Ba,Sr)2CuO7	La1Ba1.5Sr0.5Cu3O7-Z	La	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											2	Y123				3.8982		11.759	3												52.4					8.8	52.4																																																																							mOhm,cm											9.76												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8308	MRB0331241		R(Ba,Sr)2CuO7	Nd1Ba1.5Sr0.5Cu3O7-Z	Nd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											2	Y123				3.8887		11.689	3												56.4					10.2	56.4																																																																							mOhm,cm											6.7												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8309	MRB0331241		R(Ba,Sr)2CuO7	Sm1Ba1.5Sr0.5Cu3O7-Z	Sm	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8424	3.8836	11.657	3												70.7					8.3	70.7																																																																							mOhm,cm											3.37												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8310	MRB0331241		R(Ba,Sr)2CuO7	Eu1Ba1.5Sr0.5Cu3O7-Z	Eu	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8361	3.883	11.655	3												76.8					6.4	76.8																																																																							mOhm,cm											4.03												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8311	MRB0331241		R(Ba,Sr)2CuO7	Gd1Ba1.5Sr0.5Cu3O7-Z	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8285	3.8782	11.654	3												85.6					1.7	85.6																																																																							mOhm,cm											2.92												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8312	MRB0331241		R(Ba,Sr)2CuO7	Dy1Ba1.5Sr0.5Cu3O7-Z	Dy	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8068	3.8743	11.632	3												86.5					1.1	86.5																																																																							mOhm,cm											2.25												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8313	MRB0331241		R(Ba,Sr)2CuO7	Ho1Ba1.5Sr0.5Cu3O7-Z	Ho	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.8042	3.8739	11.61	3												86.8					1.5	86.8																																																																							mOhm,cm											1.43												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8314	MRB0331241		R(Ba,Sr)2CuO7	Y1Ba1.5Sr0.5Cu3O7-Z	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z		1	1998																											3	Y123				3.7976	3.8725	11.606	3												87.4					2.3	87.4																																																																							mOhm,cm											1.32												R2O3,SrCO3,BaCO3,CuO	1	mixture-CAL(950C,14H in air)-pellet-SIN(960C,12H, in N2 flow)-slow cool to 400C(5C/min)-ANN(400C,12H in O2 flow)-cool to RT					Series of R(Ba,Sr)2Cu3Oz compounds with fixed Ba and Sr content and different rare-earth replacement R				Mat. Res. Bull., 33(1998)1241	C.M. Wang,H.-C.I. Kao,J.T. Huang,M.Y. Lin		
8315	PMB0710151	glass transion=426K	Bi4Sr3Ca3Cu4Oz	Bi4Sr3Ca3Cu4OZ	Bi	4	Sr	3	Ca	3	Cu	4													O	Z		6	1995									5.82																			4334																								70																																																												428	electrical conductivity																																		Bi2O3,SrCO3,CaCO3,CuO,PbO	9	melt(1100C,2H)-Q to RT, details see Phys.Rev,B48(1992)11075					Dielectric properties of semiconducting Bi4-nPbnSr3Ca3Cu3Cu4Ox (O<n<1) glasses: precursors for high-Tc superconductors			Slid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Philos.Magazine B, 71(1995)151	B.K. CHAUDHURI,S. CHATTERJEE,S. MOLLAH,S.CHAKRABORTY		
8316	PMB0710151	glass transion=415K	(Bi,Pb)4Sr3Ca3Cu4Oz	Bi4Pb0.1Sr3Ca3Cu4OZ	Bi	4	Pb	0.1	Sr	3	Ca	3	Cu	4											O	Z		6	1995									7																			4334																								72																																																												420	electrical conductivity																																		Bi2O3,SrCO3,CaCO3,CuO,PbO	9	melt(1100C,2H)-Q to RT, details see Phys.Rev,B48(1992)11075					Dielectric properties of semiconducting Bi4-nPbnSr3Ca3Cu3Cu4Ox (O<n<1) glasses: precursors for high-Tc superconductors			Slid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Philos.Magazine B, 71(1995)151	B.K. CHAUDHURI,S. CHATTERJEE,S. MOLLAH,S.CHAKRABORTY		
8317	PMB0710151	glass transion=408K	(Bi,Pb)4Sr3Ca3Cu4Oz	Bi4Pb0.5Sr3Ca3Cu4OZ	Bi	4	Pb	0.5	Sr	3	Ca	3	Cu	4											O	Z		6	1995									6.9																			4334																								73.5																																																												412	electrical conductivity																																		Bi2O3,SrCO3,CaCO3,CuO,PbO	9	melt(1100C,2H)-Q to RT, details see Phys.Rev,B48(1992)11075					Dielectric properties of semiconducting Bi4-nPbnSr3Ca3Cu3Cu4Ox (O<n<1) glasses: precursors for high-Tc superconductors			Slid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Philos.Magazine B, 71(1995)151	B.K. CHAUDHURI,S. CHATTERJEE,S. MOLLAH,S.CHAKRABORTY		
8318	PMB0710151	glass transion=402K	(Bi,Pb)4Sr3Ca3Cu4Oz	Bi4Pb1Sr3Ca3Cu4OZ	Bi	4	Pb	1	Sr	3	Ca	3	Cu	4											O	Z		6	1995									6.76																			4334																								78.5																																																												408	electrical conductivity																																		Bi2O3,SrCO3,CaCO3,CuO,PbO	9	melt(1100C,2H)-Q to RT, details see Phys.Rev,B48(1992)11075					Dielectric properties of semiconducting Bi4-nPbnSr3Ca3Cu3Cu4Ox (O<n<1) glasses: precursors for high-Tc superconductors			Slid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700 032, India	Philos.Magazine B, 71(1995)151	B.K. CHAUDHURI,S. CHATTERJEE,S. MOLLAH,S.CHAKRABORTY		
8319	SUP0110367	223+2212(a=5.380,C=30.69A).Tc-102K by TP	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Cu3Ca2O0.13	Bi	1.6	Pb	0.4	Sr	2	Cu	3	Ca	2											O	10+Z	0.13	2	1998																											2	Bi2223				5.411		37.03	3												102						102																																																																		microV/K	1.8			TP8319	mOhm,cm											8.73													1	see Cryogenics 35(1995)271, for deoxygenation see comment.					Thermoelectric Power of Deoxygenated Bi1.6Pb0.4Sr2Ca2Cu3O10+delta Sintered Superconducting Pellets			Coryogenic Engineering Centre, Indian Institute of Technology, Kharagpur-721 302, India	J.Superconductivity,11(1998)367	T.K. Dey		
8320	SUP0110367	De-oxygenation(700C,27H in vac 1.0E-2 Torr). 2223+2212(a=5.380,C=30,69A).Tc=87K by TP	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Cu3Ca2O10.11	Bi	1.6	Pb	0.4	Sr	2	Cu	3	Ca	2											O	10+Z	10.11	2	1998																											2	Bi2223				5.411		37.03	3												84						84																																																																		microV/K	4			TP8320	mOhm,cm											23.41													1	see Cryogenics 35(1995)271, for deoxygenation see comment.					Thermoelectric Power of Deoxygenated Bi1.6Pb0.4Sr2Ca2Cu3O10+delta Sintered Superconducting Pellets			Coryogenic Engineering Centre, Indian Institute of Technology, Kharagpur-721 302, India	J.Superconductivity,11(1998)367	T.K. Dey		
8321	SUP0110367	De-oxygenation(700C,27H in vac 1.0E-2 Torr). 2223+2212 Tc=64.5K by TP	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Cu3Ca2O10.08	Bi	1.6	Pb	0.4	Sr	2	Cu	3	Ca	2											O	10+Z	10.08	2	1998																											2	Bi2223				5.411		37.03	3												60						60																																																																		microV/K	7			TP8321	mOhm,cm											69.55													1	see Cryogenics 35(1995)271, for deoxygenation see comment.					Thermoelectric Power of Deoxygenated Bi1.6Pb0.4Sr2Ca2Cu3O10+delta Sintered Superconducting Pellets			Coryogenic Engineering Centre, Indian Institute of Technology, Kharagpur-721 302, India	J.Superconductivity,11(1998)367	T.K. Dey		
8322	SUP0110367	De-oxygenation(700C,50H in vac 1.0E-2 Torr).2223+2212. Tc=52K by TP	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Cu3Ca2O10.04	Bi	1.6	Pb	0.4	Sr	2	Cu	3	Ca	2											O	10+Z	10.04	2	1998																											2	Bi2223				5.411		37.03	3												45						45																																																																		microV/K	10			TP8322	mOhm,cm											93.65													1	see Cryogenics 35(1995)271, for deoxygenation see comment.					Thermoelectric Power of Deoxygenated Bi1.6Pb0.4Sr2Ca2Cu3O10+delta Sintered Superconducting Pellets			Coryogenic Engineering Centre, Indian Institute of Technology, Kharagpur-721 302, India	J.Superconductivity,11(1998)367	T.K. Dey		
8323	SUP0110327	no irradiation, Tc=84.3K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.02O7-Z	Y	1	Ba	2	Cu	3	Li	0.02													O	7-Z		1	1998																											3	Y123																				89.3				3	89.3																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8324	SUP0110327	neutron flvence=1.02E+21/m2, Tc=83.1K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.02O7-Z	Y	1	Ba	2	Cu	3	Li	0.02													O	7-Z		1	1998																											3	Y123																				89.1					89.1																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8325	SUP0110327	neutron flvence=4.98E+21/m2, Tc=85.7K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.02O7-Z	Y	1	Ba	2	Cu	3	Li	0.02													O	7-Z		1	1998																											3	Y123																				89.4				2.3	89.4																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8326	SUP0110327	neutron flvence=9.97E+21/m2, Tc=81.3K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.02O7-Z	Y	1	Ba	2	Cu	3	Li	0.02													O	7-Z		1	1998																											3	Y123																				88.3				4	88.3																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8327	SUP0110327	no irradiation, Tc=84.9K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.06O7-Z	Y	1	Ba	2	Cu	3	Li	0.06													O	7-Z		1	1998																											3	Y123																				87.1				4	87.1																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8328	SUP0110327	neutron flvence=1.02E+21/m2, Tc=83.1K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.06O7-Z	Y	1	Ba	2	Cu	3	Li	0.06													O	7-Z		1	1998																											3	Y123																				86.7				4	86.7																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8329	SUP0110327	neutron flvence=4.98E+21/m2, Tc=86.6K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.06O7-Z	Y	1	Ba	2	Cu	3	Li	0.06													O	7-Z		1	1998																											3	Y123																				88.8				1.2	88.8																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8330	SUP0110327	neutron flvence=9.97E+21/m2, Tc=78K by microwave absorption	YBa2Cu3(Li)O7	Y1Ba2Cu3Li0.06O7-Z	Y	1	Ba	2	Cu	3	Li	0.06													O	7-Z		1	1998																											3	Y123																				86.8				4	86.8																																																																																																fire(886C,20H, in O2 flow)-pellet-SIN(936C,20H in O2 flow)-Q(150C/min, in O2)-(irradiation condition, see comment)					Microwave Supectroscipy in YBCO Superconductors: Influence of Neutron Irradiation on the 123 Phase			National Institute of Materials physics, P.O. Box MG-6, Magurele, R-76900 Bucharest, Romania	J.Superconductivity , 11(1998)327	Alina Totovana,M. Velter-Stefanescu,V. Sandu		
8331	SUP0110279	main phase 2212+minor 2223, THC150=9.35mw/cm,K	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10.34	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z	10.34	2	1998																												Bi2212																			67.1						67.1																																																																							mOhm,cm											1.56													1	SIN(840C,5H in air)					Effect of Suttering Duration on the Thermal Conductivity of (Bi,Pb)-2223 Superconducting Pellets Between 10 and 150 K			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity , 11(1998)279	T.K. Dey		
8332	SUP0110279	main phase 2212+minor 2223, THC150=10.7mw/cm,K	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10.24	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z	10.24	2	1998																												Bi2212																			73.3						73.3																																																																							mOhm,cm											2.08													1	Sin(840C,20H in air)					Effect of Suttering Duration on the Thermal Conductivity of (Bi,Pb)-2223 Superconducting Pellets Between 10 and 150 K			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity , 11(1998)279	T.K. Dey		
8333	SUP0110279	main phase 2212+minor 2223, THC150=10.32mw/cm,K	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10.15	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z	10.15	2	1998																												Bi2212																			97						97																																																																							mOhm,cm											2.26													1	Sin(840C,40H in air)					Effect of Suttering Duration on the Thermal Conductivity of (Bi,Pb)-2223 Superconducting Pellets Between 10 and 150 K			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity , 11(1998)279	T.K. Dey		
8334	SUP0110279	main phase 2212+minor 2223, THC150=9.50mw/cm,K	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10.07	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z	10.07	2	1998																												Bi2212																			102.3						102.3																																																																							mOhm,cm											2.58													1	Sin(840C,70H in air)					Effect of Suttering Duration on the Thermal Conductivity of (Bi,Pb)-2223 Superconducting Pellets Between 10 and 150 K			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity , 11(1998)279	T.K. Dey		
8335	SUP0110279	main phase 2212+minor 2223, THC150=7.72mw/cm,K	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O9.91	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	Z	9.91	2	1998																												Bi2212																			104.4						104.4																																																																							mOhm,cm											2.86													1	Sin(840C,100H in air)					Effect of Suttering Duration on the Thermal Conductivity of (Bi,Pb)-2223 Superconducting Pellets Between 10 and 150 K			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, Indian Institute of Technology, Kharagpur 721302, India	J.Superconductivity , 11(1998)279	T.K. Dey		
8336	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			64	67	70			6	67																																																																		microV/K	-4.9				mOhm,cm											1.7													1	FC to RT					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8337	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			77	78	83			6	78																																																																		microV/K	-3.1				mOhm,cm											2.6													1	ANN(700C, in air)-Q					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8338	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			86.5	89	93			6.5	89																																																																		microV/K	-2				mOhm,cm											3													1	ANN(820C, in air)-Q					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8339	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			89	92	96			7	92																																																																		microV/K	-0.6				mOhm,cm											4.2													1	ANN(800C,4H, in N2)-Q					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8340	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			85	91	96			11	91																																																																		microV/K	1.7				mOhm,cm											7.1													1	ANN(550C,0.5H, in 1.0E-5 atm O2)					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8341	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			77	87	94			17	87																																																																		microV/K	2.6				mOhm,cm											15.3													1	ANN(550C,2.5H, in 1.0E-5 atm O2)					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8342	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			66	81	92			26	81																																																																		microV/K	5.5				mOhm,cm											34														ANN(550C,2.5H, in 1.0E-5 atm O2)+ANN(550C,10H,in 1.0E-8 atm O2					Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8343	SUP0110259		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8-Z	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8-Z		1	1998																												Bi2212																			47	70	83			36	70																																																																		microV/K	6				mOhm,cm											50																			Effect of Heat Treatment on the Superconductivity of Pb-Doped Bi-2212 System: Evidence for a Possible Phase Segregation			Sturucture Reseach Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, P.R. China	J.Superconductivity , 11(1998)259	Mao Zhiqiang,Xu Gaojie,Zhang Yuheng		
8344	SSC1080059	KOH=7wt%	(Ba,K)BiO3	Ba0.6K0.4Bi1O3+Z	Ba	0.6	K	0.4	Bi	1															O	3+Z		3	1998																												BKBO							3															31			31																																																																																														KOH,KNO3,Ba(OH)2*8H2O,Bi2O3		Electrodeposition method, Concentration of KOH (see comment) is controlling parameter					ELECTRODEPOSITION OF LARGE Ba1-xKxBiO3 CRAYSTALS FROM MOLTEN KOH/KNO3 SOLUTION			Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China	Solid State Commun., 108(1998)59	C.Y. Xu,J.B. Zhang,L.Z. Zhao,S.H. Liu		
8345	SSC1080059	KOH=17wt%	(Ba,K)BiO3	Ba0.6K0.4Bi1O3+Z	Ba	0.6	K	0.4	Bi	1															O	3+Z		3	1998																												BKBO							3															31			31																																																																																														KOH,KNO3,Ba(OH)2*8H2O,Bi2O3		Electrodeposition method, Concentration of KOH (see comment) is controlling parameter					ELECTRODEPOSITION OF LARGE Ba1-xKxBiO3 CRAYSTALS FROM MOLTEN KOH/KNO3 SOLUTION			Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China	Solid State Commun., 108(1998)59	C.Y. Xu,J.B. Zhang,L.Z. Zhao,S.H. Liu		
8346	SSC1080059	KOH=25wt%	(Ba,K)BiO3	Ba0.66K0.34Bi1O3+Z	Ba	0.66	K	0.34	Bi	1															O	3+Z		3	1998																												BKBO							3															30			30																																																																																														KOH,KNO3,Ba(OH)2*8H2O,Bi2O3		Electrodeposition method, Concentration of KOH (see comment) is controlling parameter					ELECTRODEPOSITION OF LARGE Ba1-xKxBiO3 CRAYSTALS FROM MOLTEN KOH/KNO3 SOLUTION			Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China	Solid State Commun., 108(1998)59	C.Y. Xu,J.B. Zhang,L.Z. Zhao,S.H. Liu		
8347	SSC1080059	KOH=38wt%	(Ba,K)BiO3	Ba0.76K0.24Bi1O3+Z	Ba	0.76	K	0.24	Bi	1															O	3+Z		3	1998																												BKBO							3															28			28																																																																																														KOH,KNO3,Ba(OH)2*8H2O,Bi2O3		Electrodeposition method, Concentration of KOH (see comment) is controlling parameter					ELECTRODEPOSITION OF LARGE Ba1-xKxBiO3 CRAYSTALS FROM MOLTEN KOH/KNO3 SOLUTION			Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China	Solid State Commun., 108(1998)59	C.Y. Xu,J.B. Zhang,L.Z. Zhao,S.H. Liu		
8348	SSC1080059	KOH=50wt%	(Ba,K)BiO3	Ba0.83K0.17Bi1O3+Z	Ba	0.83	K	0.17	Bi	1															O	3+Z		3	1998																												BKBO							3															20			20																																																																																														KOH,KNO3,Ba(OH)2*8H2O,Bi2O3		Electrodeposition method, Concentration of KOH (see comment) is controlling parameter					ELECTRODEPOSITION OF LARGE Ba1-xKxBiO3 CRAYSTALS FROM MOLTEN KOH/KNO3 SOLUTION			Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China	Solid State Commun., 108(1998)59	C.Y. Xu,J.B. Zhang,L.Z. Zhao,S.H. Liu		
8349	SUP0110215	main phase=87.54%, impurity phase=BaCuO2	LaBa2Cu3O7	La1Ba2Cu3OZ	La	1	Ba	2	Cu	3															O	Z		2	1998																											3	Y123	Pmmm			3.9014	3.9294	11.789	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8350	SUP0110215	main phase=91.1%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2.97Fe0.03OZ	La	1	Ba	2	Cu	2.97	Fe	0.03													O	Z		2	1998																											3	Y123	Pmmm			3.917	3.9205	11.7828	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8351	SUP0110215	main phase=88.9%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2.94Fe0.06OZ	La	1	Ba	2	Cu	2.94	Fe	0.06													O	Z		2	1998																											2	Y123	Pmmm			3.9212		11.778	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8352	SUP0110215	main phase=89.24%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2.9Fe0.1OZ	La	1	Ba	2	Cu	2.9	Fe	0.1													O	Z		2	1998																											2	Y123	Pmmm			3.9236		11.772	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8353	SUP0110215	main phase=84.91%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2.75Fe0.25OZ	La	1	Ba	2	Cu	2.75	Fe	0.25													O	Z		2	1998																											3	Y123	Pmmm			3.9173	3.9332	11.788	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8354	SUP0110215	main phase=86.68%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2.4Fe0.6OZ	La	1	Ba	2	Cu	2.4	Fe	0.6													O	Z		2	1998																											3	Y123	Pmmm			3.9141	3.9373	11.803	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8355	SUP0110215	main phase=92.05%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu2Fe1OZ	La	1	Ba	2	Cu	2	Fe	1													O	Z		2	1998																											3	Y123				3.924	3.9392	11.817	3																																																																																																																La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8356	SUP0110215	main phase=98.24%, impurity phase=BaCuO2	LaBa2(Cu,Fe)3O7	La1Ba2Cu1.5Fe1.5OZ	La	1	Ba	2	Cu	1.5	Fe	1.5													O	Z		2	1998																											3	Y123				3.9454	3.9539	11.833																																																																																																																	La2O3,BaCO3,CuO,Fe3O4		mixture-heat(930C,24H, in air)-pellet-heat(930C,24H)-(350C,24H in O2 flow)-FC to RT					X-ray Diffraction studies on LaBa2Cu3Ox Cuprates with Iron Substitution			National Laboratory of Solid State Microstructures, Institute of Solid State Physics, Nanjing University, and Center for Advanced Studies in Science and Technology of Microstructures, Nanjing University, Nanjing 210093, China	J.Superconductivity , 11(1998)215	S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8357	SUP0100507		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		1	1997																											3	Y123				3.8301	3.8988	11.6682	3												89			90			90																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8358	SUP0100507		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-Z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1997																											3	Y123				3.8358	3.894	11.6766	3												63			65			65																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8359	SUP0100507		(Y,Pr,Cd)Ba2Cu3O7	Y0.7Pr0.2Cd0.1Ba2Cu3O7-Z	Y	0.7	Pr	0.2	Cd	0.1	Ba	2	Cu	3											O	7-Z		1	1997																											3	Y123				3.8376	3.8953	11.6865													58			59			59																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8360	SUP0100507		(Y,Pr,Cd)Ba2Cu3O7	Y0.5Pr0.2Cd0.3Ba2Cu3O7-Z	Y	0.5	Pr	0.2	Cd	0.3	Ba	2	Cu	3											O	7-Z		1	1997																											3	Y123				3.8371	3.8957	11.6937													40			42			42																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8361	SUP0100507		(Y,Pr,Cd,Ca)Ba2Cu3O7	Y0.5Pr0.2Cd0.2Ca0.1Ba2Cu3O7-Z	Y	0.5	Pr	0.2	Cd	0.2	Ca	0.1	Ba	2	Cu	3									O	7-Z		1	1997																											3	Y123				3.8516	3.8809	11.6476													52			54			54																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8362	SUP0100507		(Y,Pr,Cd,Ca)Ba2Cu3O7	Y0.5Pr0.2Cd0.1Ca0.2Ba2Cu3O7-Z	Y	0.5	Pr	0.2	Cd	0.1	Ca	0.2	Ba	2	Cu	3									O	7-Z		1	1997																											3	Y123				3.8425	3.896	11.7801													67			68			68																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8363	SUP0100507		(Y,Pr,Ca)Ba2Cu3O7	Y0.5Pr0.2Ca0.3Ba2Cu3O7-Z	Y	0.5	Pr	0.2	Ca	0.3	Ba	2	Cu	3											O	7-Z		1	1997																											3	Y123				3.8442	3.907	11.7196													72			74			74																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8364	PSS0402145		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	Z	6.96	1	1998																											3	Y123				3.822	3.879	11.694	3												90.7	92.3				4.7	92.3																																																																		microV/K	-0.63																												1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8365	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.975Ca0.025Ba2Cu3O6.95	Y	0.975	Ca	0.025	Ba	2	Cu	3													O	Z	6.95	1	1998																											3	Y123				3.822	3.882	11.691	3												86.8	91.5				5.4	91.5																																																																		microV/K	-1.48																												1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8366	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.95Ca0.05Ba2Cu3O6.94	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	Z	6.94	1	1998																											3	Y123				3.822	3.879	11.689	3												83.3	88.2				6	88.2																																																																		microV/K	-1.18																												1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8367	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.925Ca0.075Ba2Cu3O6.93	Y	0.925	Ca	0.075	Ba	2	Cu	3													O	Z	6.93	1	1998																											3	Y123				3.824	3.878	11.69	3												80.7	86.3				9	86.3																																																																		microV/K	-1.2																												1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8368	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu3O6.93	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	Z	6.93	1	1998																											3	Y123				3.825	3.879	11.69	3												71.9	83.3				10	83.3																																																																		microV/K	-1.14																						0.0014						1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8369	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.85Ca0.15Ba2Cu3O6.9	Y	0.85	Ca	0.15	Ba	2	Cu	3													O	Z	6.9	1	1998																											3	Y123				3.828	3.871	11.693	3												71.5	79				10.3	79																																																																		microV/K	-1.29																						0.0023						1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8370	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.89	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	Z	6.89	1	1998																											3	Y123				3.832	3.875	11.697	3												66.6	78.2				10.9	78.2																																																																		microV/K	-1.24																						0.0032						1	SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8371	PSS0402145		YBa2Cu3O7	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	Z	6.73	1	1998																											3	Y123				3.822	3.879	11.694	3												61.1	63.7				5.3	63.7																																																																		microV/K	17.8			TP8371																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8372	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.975Ca0.025Ba2Cu3O6.72	Y	0.975	Ca	0.025	Ba	2	Cu	3													O	Z	6.72	1	1998																											3	Y123				3.822	3.882	11.691	3												67.9	70.8				7.5	70.8																																																																		microV/K	14			TP8372																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8373	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.95Ca0.05Ba2Cu3O6.7	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	Z	6.7	1	1998																											3	Y123				3.822	3.879	11.689	3												69.7	72				4	72																																																																		microV/K	12.4			TP8373																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8374	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.925Ca0.075Ba2Cu3O6.68	Y	0.925	Ca	0.075	Ba	2	Cu	3													O	Z	6.68	1	1998																											3	Y123				3.824	3.878	11.69	3												73.1	75.1				6	75.1																																																																		microV/K	13.3			TP8374																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8375	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu3O6.66	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	Z	6.66	1	1998																											3	Y123				3.825	3.879	11.69	3												77.3	80				5.6	80																																																																		microV/K	9.4			TP8375																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8376	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.85Ca0.15Ba2Cu3O6.58	Y	0.85	Ca	0.15	Ba	2	Cu	3													O	Z	6.58	1	1998																											3	Y123				3.828	3.871	11.693	3												74.2	80.6				8	80.6																																																																		microV/K	9.3			TP8376																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8377	PSS0402145		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.53	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	Z	6.53	1	1998																											3	Y123				3.832	3.875	11.697	3												76.6	80.9				7.6	80.9																																																																		microV/K	8			TP8377																										SIN(920-950C, in air)-slow cool to 450C-ANN(450C,2H, in O2 flow)-ANN(450C,2H , in air)-Q to RT					On possibility of introduction by calcium the additional states in conducting zone during doping YBa2Cu3Oy				Fizika tverdogo tela (Phys. Of the Solid State), 40(1998)2145			
8378	PR0409400		(Ba,K)BiO3	Ba0.65K0.35Bi1O3	Ba	0.65	K	0.35	Bi	1															O	3			1989																												BKBO																		K				30			30																				T	from M(H,T)	17.3							T/K		0.87					A	from Hc2(O)	36.8			A	from Hc1,Hc2	2200																																																					melt-cast polycrystalline sample.					MAGNETIC AND RESISTIVE MEASUREMENTS OF THE SUPERCONDUCTING CRITICAL FIELDS OF MELT-CAST BA0.65K0.35BIO3	198911	CRITICAL FIELDS     ,COHERENCE LENGTH    ,PENETRATION DEPTH   ,SPECIFIC-HEAT	MATERIALS SCIENCE DIVISION,ARGONNE NATIONAL LABORATORY,ARGONNE,ILLINOIS 60439	PHYS.REV.B,40(1989)9400	B. Dabrowski,B.DABROWSKI,D.G. Hinks,D.G.HINKS,G.W. Crabtree,G.W.CRABTREE,K.G. Vandervoort,K.G.VANDERVOORT,R. Hulschher,R.HULSCHER,U. Welp,U.WELP,W.K. Kwok,W.K.KWOK,Y. Zheng,Y.ZHENG	BA,K,BI,O	
8379	PR04903502	Tc=25Kphase(dHc2/dT=-1.1T/K) is included.	(Ba,K)BiO3	Ba0.55K0.45Bi1O3	Ba	0.55	K	0.45	Bi	1															O	3			1994																												BKBO																		K				30			30																				T	estimated from the data at 1.8K	32							T/K	from the dataatnear Tc	0.5					A	from Hc2zero	32																																																										electrochemical crystalliqation, see Solid State Commun.78(1991)967					Upper critical field of Ba1-xKxBiO3 single crystals			Laboratoire d'Etudes des Proprietes Electroniques des Solides,Grenoble,France	Phys.Rev.B, 49(1994)3502	A. Sulpice,A.G.M. Jansen,A.G.M.Jansen,A.Sulpice,C. Escribe-Filippini,C.Escribe-Filippini,H. Rakoto,H.Rakoto,J. Marcus,J.C. Ousset,J.C.Ousset,J.M. Broto,J.M.Broto,J.Marcus,M. Affronte,M.Affronte,S. Askenazy,S.Askenazy		
8380	PHC3070177		(Cu,C)Sr2CaCu2Oz	Cu0.5C0.5Sr2Ca1Cu2O7	Cu	0.5	C	0.5	Sr	2	Ca	1	Cu	2											O	Z	7	2	1998																											2	Cu1212				3.833		10.953												K				90			90																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8381	PHC3070177		(Cu,C)Sr2Ca4Cu5Oz	Cu0.5C0.5Sr2Ca1Cu5O10.8	Cu	0.5	C	0.5	Sr	2	Ca	1	Cu	5											O	Z	10.8	2	1998																											2	Cu1245				3.858		20.521												K				41			41																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8382	PHC3070177		(Cu,N,C)Sr2Ca2Cu3Oz	Cu0.5N0.25C0.25Sr2Ca2Cu3OZ	Cu	0.5	N	0.25	C	0.25	Sr	2	Ca	2	Cu	3									O	Z		2	1998																											2	M1223				3.835		14.26												K				90			90																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8383	PHC3070177		(Cu,N,C)Sr2Ca3Cu4Oz	Cu0.5N0.25C0.25Sr2Ca3Cu4OZ	Cu	0.5	N	0.25	C	0.25	Sr	2	Ca	3	Cu	4									O	Z		2	1998																											2	M1234				3.845		17.52												K				113			113																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8384	PHC3070177		(Cu,N,C)Sr2Ca4Cu5Oz	Cu0.5N0.25C0.25Sr2Ca4Cu5OZ	Cu	0.5	N	0.25	C	0.25	Sr	2	Ca	4	Cu	5									O	Z		2	1998																											2	M1245				3.864		20.7												K				65			65																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8385	PHC3070177		(Cu,N,C)Sr2Ca5Cu6Oz	Cu0.5N0.25C0.25Sr2Ca5Cu6OZ	Cu	0.5	N	0.25	C	0.25	Sr	2	Ca	5	Cu	6									O	Z		2	1998																											2	M1256				3.869		23.93												K				52			52																																																																																														CuO,Sr(NO3)2,SrCuO2,SrO2,Ca2CuO3,SrCO3,		mixture were sealed in Au capsules-react(5-6 G Pa, 1200-1375C, 1-6H)-Q to RT-pressure release					Homologous series of high-Tc superconductors (Cu,C)Sr2Can-1CunOy(n=2,5) and (Cu,N,C)Sr2Can-1CunOy (n=3-6)synthesized under high pressure	199810		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305-0044, Japan	Physica.C,307(1998)177-188	A.T. Matveev,E. Takayama-muromachi,N.D. Zhigadlo,Y. Anan,Y. Ishida,Y. Matsui		
8386	PHC3070189	A2BB'O6 type structure, complex cubic structure	HoBa2SbO6	Ho1Ba2Sb1O6	Ho	1	Ba	2	Sb	1															O	6			1998	emu/mol	-0.00982	emu,K/mol	14.44156			-5.46854																																							K					5																																																																																																	1						Structure, microstructure, magnetic properties and chemical stability of HoBa2SbO6 with Yba2Cu3O7-delta superconductor	199810		Department de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Physica.C,307(1998)189-196	C.C. de Souza Silva,D.A. Landinez Tellez,E. Chavira,J. Albino Aguiar,J. Guzman,J.M. Ferreira,Y.P. Yadava		
8387	PHC3070202	as-synthesized, overdoped		Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z			1998																												Hg1223				3.847		15.76												K				107			107																																		HIR8387																		JC8387																																												mixture(HgO,Ca2CuO3,BaCuO2+z)-packed into Au capsules-heat(950C,1H under 5 Gpa)-oxygen. Control(see comment)					Effect of overdoping on the irreversibility field and critical current density of the HgBa2Ca2Cu3O8+delta superconductor	199810		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,307(1998)202-208	H. Suematsu,H. Yamauchi,K. Fujinami,M. Karppinen		
8388	PHC3070202	ANN(300C,12H in flowing O2), optimally doped		Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z			1998																												Hg1223				3.85		15.78												K				132			132																																		HIR8388																		JC8388																																												mixture(HgO,Ca2CuO3,BaCuO2+z)-packed into Au capsules-heat(950C,1H under 5 Gpa)-oxygen. Control(see comment)					Effect of overdoping on the irreversibility field and critical current density of the HgBa2Ca2Cu3O8+delta superconductor	199810		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,307(1998)202-208	H. Suematsu,H. Yamauchi,K. Fujinami,M. Karppinen		
8389	PHC3070202	ANN(400C,24H, in Ar), under doped		Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z			1998																												Hg1223				3.853		15.78												K				118			118																																		HIR8389																		JC8389																																												mixture(HgO,Ca2CuO3,BaCuO2+z)-packed into Au capsules-heat(950C,1H under 5 Gpa)-oxygen. Control(see comment)					Effect of overdoping on the irreversibility field and critical current density of the HgBa2Ca2Cu3O8+delta superconductor	199810		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,307(1998)202-208	H. Suematsu,H. Yamauchi,K. Fujinami,M. Karppinen		
8390	PHC3070017	dtc/dp is the value at P=1.75GPa two step transition	(B,C)(Ba,Sr)2Ca2Cu3Oz	B0.7C0.3Ba1.5Sr0.5Ca2Cu3OZ	B	0.7	C	0.3	Ba	1.5	Sr	0.5	Ca	2	Cu	3									O	Z			1998																											2	M1223				3.861		14.21												K	117		118.3				117.65			K/GPa	2																																																																																												mixture-sealed in Au capsule-heat(1100C,2H,P=4.5GPa)					Pressure effect on Tc in (B1-xCx)(Ba1-ySry)2Ca2Cu3Oz(x=0.3,Y=0.25;x=0.35,y=0.3)and B0.8C0.2(Ba0.75Sr0.25)2Va3Cu4Oz	199810		Department of applied Electronics, Science University of Tokyo, 2641 Yamazaki, Noda, Chiba, 278-8510, Japan	Physica.C,307(1998)17-22	A. Iyo,C. Kunugi,H. Ihara,K. Tokiwa,S. Kuwata,T. Watanabe		
8391	PHC3070017	dtc/dp is the value at P=1.75GPa	(B,C)(Ba,Sr)2Ca2Cu3Oz	B0.65C0.35Ba1.4Sr0.6Ca2Cu3OZ	B	0.65	C	0.35	Ba	1.4	Sr	0.6	Ca	2	Cu	3									O	Z			1998																											2	M1223				3.862		14.2												K	118.8	119.6					119.6			K/GPa	2																																																																																												mixture-sealed in Au capsule-heat(1100C,2H,P=4.5GPa)					Pressure effect on Tc in (B1-xCx)(Ba1-ySry)2Ca2Cu3Oz(x=0.3,Y=0.25;x=0.35,y=0.3)and B0.8C0.2(Ba0.75Sr0.25)2Va3Cu4Oz	199810		Department of applied Electronics, Science University of Tokyo, 2641 Yamazaki, Noda, Chiba, 278-8510, Japan	Physica.C,307(1998)17-22	A. Iyo,C. Kunugi,H. Ihara,K. Tokiwa,S. Kuwata,T. Watanabe		
8392	PHC3070017	dtc/dp is the value at P=1.75GPa two step transition	(B,C)(Ba,Sr)2Ca3Cu4Oz	B0.8C0.2Ba1.5Sr0.5Ca3Cu4OZ	B	0.8	C	0.2	Ba	1.5	Sr	0.5	Ca	3	Cu	4									O	Z			1998																											2	M1234				3.854		17.41												K										K/GPa	1.9																																																																																												mixture-sealed in Au capsule-heat(1100C,2H,P=4.5GPa)					Pressure effect on Tc in (B1-xCx)(Ba1-ySry)2Ca2Cu3Oz(x=0.3,Y=0.25;x=0.35,y=0.3)and B0.8C0.2(Ba0.75Sr0.25)2Va3Cu4Oz	199810		Department of applied Electronics, Science University of Tokyo, 2641 Yamazaki, Noda, Chiba, 278-8510, Japan	Physica.C,307(1998)17-22	A. Iyo,C. Kunugi,H. Ihara,K. Tokiwa,S. Kuwata,T. Watanabe		
8393	PHC3070067			Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1998																											3	Bi2212				5.4079	5.4117	30.884												K				86.3			86.3																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8394	PHC3070067		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.65Pr0.35Cu2OZ	Bi	2	Sr	2	Ca	0.65	Pr	0.35	Cu	2											O	Z			1998																											3	Bi2212				5.4169	5.4324	30.661												K				69.4			69.4																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8395	PHC3070067		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.55Pr0.45Cu2OZ	Bi	2	Sr	2	Ca	0.55	Pr	0.45	Cu	2											O	Z			1998																											3	Bi2212				5.4603	5.4415	30.474												K				47.5			47.5																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8396	PHC3070067		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.46Pr0.54Cu2OZ	Bi	2	Sr	2	Ca	0.46	Pr	0.54	Cu	2											O	Z			1998																											3	Bi2212				5.4778	5.4584	30.435												K				31.4			31.4																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8397	PHC3070067		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2OZ	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	Z			1998																											3	Bi2212				5.4428	5.483	30.374												K				0.4			0.4																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8398	PR05812355	Hc(O)=0.21T,G-L parameter=85	(Ba,K)BiO3	Ba0.66K0.34Bi1O3	Ba	0.66	K	0.34	Bi	1															O	3		3	1998																												BKBO																		K				30			30													77									25									0.78							36.4					3089													my/md,K2	2.16	uning BCS relation deltaC/Tc=1.43GAMMA																																						electrodeposion					Scaling of magnetization and basic parameters of Ba1-xKxBiO3+y superconductors near Tc	11		Institute of Physics of Solid and Semiconductors, Academy of Science, Minsk 220072, Belarus	Phys.rev.B,58(1998)12355	D.Dew-Hughes,H. Szymczak,J.W. Lynn,M. Baran,R. Szymczak,S.M. Barilo,S.V. Shiryaev,V.I. Gatalskaya		
8399	PR05812355	Hc(O)=0.18T,G-L parameter=74	(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	1998																												BKBO																		K				29			29													74									19.3									0.65							41.5					3100													my/md,K2	1.8	uning BCS relation deltaC/Tc=1.43GAMMA																																						electrodeposion					Scaling of magnetization and basic parameters of Ba1-xKxBiO3+y superconductors near Tc	11		Institute of Physics of Solid and Semiconductors, Academy of Science, Minsk 220072, Belarus	Phys.rev.B,58(1998)12355	D.Dew-Hughes,H. Szymczak,J.W. Lynn,M. Baran,R. Szymczak,S.M. Barilo,S.V. Shiryaev,V.I. Gatalskaya		
8400	PR05812355	Hc(O)=0.187T,G-L parameter=80	(Ba,K)BiO3	Ba0.59K0.41Bi1O3	Ba	0.59	K	0.41	Bi	1															O	3		3	1998																												BKBO																		K				31			31													73									20.9									0.6							40					3200													my/md,K2	1.95	uning BCS relation deltaC/Tc=1.43GAMMA																																						seeded growth technique					Scaling of magnetization and basic parameters of Ba1-xKxBiO3+y superconductors near Tc	11		Institute of Physics of Solid and Semiconductors, Academy of Science, Minsk 220072, Belarus	Phys.rev.B,58(1998)12355	D.Dew-Hughes,H. Szymczak,J.W. Lynn,M. Baran,R. Szymczak,S.M. Barilo,S.V. Shiryaev,V.I. Gatalskaya		
8401	PHC1940194		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1992																																														K		31.4				2	31.4																													T/K		0.57																																																																	see Chem.Mater.3(1991)431					THE IRREVERSIBILITY LINE AND FLUX CREEP	199205			PHYSICA C,194(1992)194	C.W.CHU,H.H.FANG,H.Y.TANG,M.L.NORTON,P.H.HOR,W.C.CHAN,Y.Y.XUE,Z.J.HUANG	BA,K,BI,O,Y,CU	
8402	PHC2150350	G-L parameter=60,thermodynamic critical field=1900 Oe	(Ba,K)BiO3	Ba0.62K0.38Bi1O3.1	Ba	0.62	K	0.38	Bi	1															O	3.1	3.1		1993																												BKBO																				29.5		30.5		0.8	29.5											Oe		95								T	16							T/K		0.79					A		45			A		2700																												moOhm.cm	3025																								slectrochemical method, heat treatment(210C,45H in O2)					EFFECT OF GROWTH CONDITIONS ON THE SUPERCONDUCTIVITY OF BA1-XKXBIO3 CRYSTALS	199310			PHYSICA C,215(1993)350	M.D.LAN,N.SUZUKI,P.KLAVINS,R.N.SHELTON,S.NAKAMURA,T.UCHIDA,W.D.MOSLEY,Y.NAGATA	BA,K,BI,O	
8403	PHC2100133	0.35<x<0.40 in this paper, RT-27OK in this case, HIRFIG shows Hc2(T)	(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	1993																												BKBO																				32					32																									30						0.5					A		33																																												1.71														see Solid State Commun.85(1993)501					UPPER CRITICAL FIELD OF BA1-XKXBIO3 SINGLE CRYSTAL	199305			PHYSICA C,210(1993)133	C.ESCRIBE-FILIPPINI,H.RAKOTO,J.C.OUSSET,J.M.BROTO,J.MARCUS,M.AFFRONTE,S.ASKENAZY	BA,K,BI,O	
8404	PHC2290389	SIS tunneling, counter electrode=Au, K-content is not clear, estimated from Tc(by Asada)	(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3			1994																												BKBO																				15.5					15.5																																																3.5	1																																						-0.00000000136									electrochemical crystal growth, 210 in O2					Tunneling studies on Ba1-xKxBiO3 single crystals with Tc=15-30K	199408			Physica C, 229(1994)389-395	J.Akimitsu,M.Furuya,M.Kosugi,T.Ekino,T.Uchida,Y.Nagata	Ba,K,Bi,O	
8405	PR05106171		(Ba,K)BiO3	Ba0.54K0.46Bi1O3	Ba	0.54	K	0.46	Bi	1															O	3		3	1995																												BKBO																				18					18																																																																	THC8405																															Top-seeded electrochemical method.					Magnetothermal conductivity of Ba1-xKxBiO3 crystals	199503		Department of Physics,University of Michigan,Ann Arbor,Michigan 48109	Phys.Rev.B.,51(1995)6171	Baoxing Chen,C.Uher,D.A.Payne,F.Tsui,K.V.Rao,P.D.Han	Ba,K,Bi,O	
8406	PR05106171		(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	1995																												BKBO																				30					30																																																																	THC8406																															Top-seeded electrochemical method.					Magnetothermal conductivity of Ba1-xKxBiO3 crystals	199503		Department of Physics,University of Michigan,Ann Arbor,Michigan 48109	Phys.Rev.B.,51(1995)6171	Baoxing Chen,C.Uher,D.A.Payne,F.Tsui,K.V.Rao,P.D.Han	Ba,K,Bi,O	
8407	PR05004144	GAPENE=4.2+,-0.5, by FIM reflectivity	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	1994																												BKBO																						30.8		3	30.8																																									A		4550			cm(-1)	45	4.2	2																																															electrochemical method					Optical study of Ba0.6K0.4BiO3 single crystals:Noemal and superconducting properties	199408		Department of Physics and Astronomy, Unversity, Hamilton, Ontario, Canada L8S4M1	Phys.Rev.B,50(1994)4144	A.V. Puchkov,R.N. Shelton,T. Timusk,W.D. Mosley		
8408	APL0640244	Penet=3300+,-200A	(Ba,K)BiO3	Ba0.51K0.49Bi1O3	Ba	0.51	K	0.49	Bi	1															O	3		4	1994																												BKBO																						17.2			17.2																																									A	microwave surface resistance	3300				2.82	3.8	7																																															by molecular beam epitaxy, on (100)MgO, thickness=3600A		MgO(100)			Pnetration depth, microwave surface resistance, and gap ratio in NbN and Ba1-xKxBiO3 thin films	1		Center for Superconductivity resarch, Department of Physics, University of Maryland, College Park, Maryland 20742	Appl.Phys.Lett.64(1994)244	E.H. Hartford, Jr,E.S. Hellman,M. Bruns,M.S. Pambianchi,S.M. Anlage,S.Y. Lee		
8409	PR05406133	K-content estimatel from Tc-valve by Y.Asada, HIRFG shows Hc2(T)	(Ba,K)BiO3	Ba0.65K0.35Bi1O3	Ba	0.65	K	0.35	Bi	1															O	3		3	1996																												BKBO																						31.8		1.7	31.8																				T	defined as onset in real part of ac susseptibility				23.7			4.2																																																																				electrochemical method, melted mixtyre(K:Ba:Bi=72:1:2), bath temperature=300C					Positive curvature in the temperature dependence of Hc2 in KxBa1-xBiO3	199609		Institute of Solid State Physics RAS, 142432 Chernogolovka, Russia	Phys.Rev.B,54(1996)6133	A.K. Geim,G.E. Tsydynzhapov,L.A. Klinkova,N.V. Barkovskii,S. Wiegers,V.F. Gantmakher		
8410	SUP0100645		Eu(Ba,Sr)2Cu3O7	Eu1Ba1Sr1Cu3O6.95	Eu	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.95	1	1997																											3	Y123	Pmmm			3.803	3.845	11.582	3													84		82			84																																																																																														Eu2O3,Ba(NO3)2,Sr(NO3)2,CaCO3,CuO	1	mixture-CAL(1225C,24H)-Pellet-SIN(1250C,78H)-ANN(1100K,12H,in Ar flow)-FC to 725C					Effect of Ca Doping on the Structural and Superconducting Properties of EuBaSrCu3O7-delta	199706		Computer Division and Chemistry Division, Bahabha Atomic Research Centre, Mumbai 400 0085, India	J.Superconductivity,10(1997)645	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly,T.B Waji,T.B. Waje		
8411	SUP0100645		Eu(Ba,Sr,Ca)2Cu3O7	Eu1Ba1Sr0.9Ca0.1Cu3O6.95	Eu	1	Ba	1	Sr	0.9	Ca	0.1	Cu	3											O	7-Z	6.95	1	1997																											3	Y123	Pmmm			3.82	3.85	11.57	3													81		77			81																																																																																														Eu2O3,Ba(NO3)2,Sr(NO3)2,CaCO3,CuO	1	mixture-CAL(1225C,24H)-Pellet-SIN(1250C,78H)-ANN(1100K,12H,in Ar flow)-FC to 725C					Effect of Ca Doping on the Structural and Superconducting Properties of EuBaSrCu3O7-delta	199706		Computer Division and Chemistry Division, Bahabha Atomic Research Centre, Mumbai 400 0085, India	J.Superconductivity,10(1997)645	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly,T.B Waji,T.B. Waje		
8412	SUP0100645		Eu(Ba,Sr,Ca)2Cu3O7	Eu1Ba1Sr0.8Ca0.2Cu3O6.95	Eu	1	Ba	1	Sr	0.8	Ca	0.2	Cu	3											O	7-Z	6.95	1	1997																											2	Y123				3.84		11.575	3													75		72			75																																																																																														Eu2O3,Ba(NO3)2,Sr(NO3)2,CaCO3,CuO	1	mixture-CAL(1225C,24H)-Pellet-SIN(1250C,78H)-ANN(1100K,12H,in Ar flow)-FC to 725C					Effect of Ca Doping on the Structural and Superconducting Properties of EuBaSrCu3O7-delta	199706		Computer Division and Chemistry Division, Bahabha Atomic Research Centre, Mumbai 400 0085, India	J.Superconductivity,10(1997)645	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly,T.B Waji,T.B. Waje		
8413	SUP0100645		Eu(Ba,Sr,Ca)2Cu3O7	Eu1Ba1Sr0.7Ca0.3Cu3O6.95	Eu	1	Ba	1	Sr	0.7	Ca	0.3	Cu	3											O	7-Z	6.95	1	1997																											2	Y123				3.842		11.582	3													75		70			75																																																																																														Eu2O3,Ba(NO3)2,Sr(NO3)2,CaCO3,CuO	1	mixture-CAL(1225C,24H)-Pellet-SIN(1250C,78H)-ANN(1100K,12H,in Ar flow)-FC to 725C					Effect of Ca Doping on the Structural and Superconducting Properties of EuBaSrCu3O7-delta	199706		Computer Division and Chemistry Division, Bahabha Atomic Research Centre, Mumbai 400 0085, India	J.Superconductivity,10(1997)645	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly,T.B Waji,T.B. Waje		
8414	SUP0100645		Eu(Ba,Sr,Ca)2Cu3O7	Eu1Ba1Sr0.6Ca0.4Cu3O6.95	Eu	1	Ba	1	Sr	0.6	Ca	0.4	Cu	3											O	7-Z	6.95		1997																																																																																																																																																			Eu2O3,Ba(NO3)2,Sr(NO3)2,CaCO3,CuO	1	mixture-CAL(1225C,24H)-Pellet-SIN(1250C,78H)-ANN(1100K,12H,in Ar flow)-FC to 725C					Effect of Ca Doping on the Structural and Superconducting Properties of EuBaSrCu3O7-delta	199706		Computer Division and Chemistry Division, Bahabha Atomic Research Centre, Mumbai 400 0085, India	J.Superconductivity,10(1997)645	I.K. Gopalakrishnan,J.V. Yakhmi,R. Ganguly,T.B Waji,T.B. Waje		
8415	JSC1280310	unit cell volum=0.4083nm(-3), b/a=1.0053	GdBa2Cu4O8	Gd1Ba2Cu4O8-Z	Gd	1	Ba	2	Cu	4															O	8-Z		1	1997																											3	Y124																				77					77																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8416	JSC1280310	unit cell volum=0.4074nm(-3), b/a=1.0061	Gd(Ba,Sr)2Cu4O8	Gd1Ba1.9Sr0.1Cu4O8-Z	Gd	1	Ba	1.9	Sr	0.1	Cu	4													O	8-Z		1	1997																											3	Y124																				77					77																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8417	JSC1280310	unit cell volum=0.4066nm(-3), b/a=1.0068	Gd(Ba,Sr)2Cu4O8	Gd1Ba1.8Sr0.2Cu4O8-Z	Gd	1	Ba	1.8	Sr	0.2	Cu	4													O	8-Z		1	1997																											3	Y124																				77					77																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8418	JSC1280310	unit cell volum=0.4053nm(-3), b/a=1.0078		Ho1Ba2Cu4O8-Z	Ho	1	Ba	2	Cu	4															O	8-Z		1	1997																											3	Y124																				82					82																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8419	JSC1280310	unit cell volum=0.4032nm(-3), b/a=1.0091		Ho1Ba1.8Sr0.2Cu4O8-Z	Ho	1	Ba	1.8	Sr	0.2	Cu	4													O	8-Z		1	1997																											3	Y124																				82					82																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8420	JSC1280310	unit cell volum=0.4012nm(-3), b/a=1.0111		Ho1Ba1.6Sr0.4Cu4O8-Z	Ho	1	Ba	1.6	Sr	0.4	Cu	4													O	8-Z		1	1997																											3	Y124																				82					82																																																																																																See J.Am.Ceram.Soc.76(1993)1618, SIN(1073K, in O2 Flow)					Strontium Substitution in Superconducting RBa2Cu4O8  (R=Gd and Ho) Compound			Department of Industrial Chemistry, Faculty of Engineering, Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-03, Japan	J.Solid State Chem.128(1997)310-312	Kimihiro Tamashita,Kimihiro Yamashita,Motohide Matsuda,Takao Umegai,Takao Umegaki,Yasuhiko Aihara		
8421	SUP0100663	porosity=0.19	YBa2Cu3O7	Y1Ba2Cu3Co0.1OZ	Y	1	Ba	2	Cu	3	Co	0.1													O	Z		1	1997									5.18																		3	Y123				3.8207	3.8877	11.6871	3													91					91																																																																	THC8421																														1	pressing(aniaxial load 10-15tons in 18mm pellet) intp pellet					The Effects of Cobalt Substitution on the Thermal Diffusivity of YBa2Cu3O7-delta Superconductor	199706		Department of Applied Physics,Chalmers University of Technology, S-412 96 Gothenburg, Sweden	J.Superconductivity,10(1997)663	B.M. Suleiman,L. Borjesson		
8422	SUP0100663	porosity=0.27	YBa2(Cu,Co)3O7	Y1Ba2Cu2.9OZ	Y	1	Ba	2	Cu	2.9															O	Z		1	1997									4.62																		2	Y123				3.8624		11.7022	3													74					74																																																																	THC8422																														1	pressing(aniaxial load 10-15tons in 18mm pellet) intp pellet					The Effects of Cobalt Substitution on the Thermal Diffusivity of YBa2Cu3O7-delta Superconductor	199706		Department of Applied Physics,Chalmers University of Technology, S-412 96 Gothenburg, Sweden	J.Superconductivity,10(1997)663	B.M. Suleiman,L. Borjesson		
8423	SUP0110123		TlSr2Ba2Cu2O7(CO3,NO3)	Tl1Sr2Ba2Cu2C0.9N0.1O10	Tl	1	Sr	2	Ba	2	Cu	2	C	0.9	N	0.1									O	10		1	1998																											3	Tl1222				3.921	30.397	16.725														61					61																																																																																														Tl2O3,SrO2,Sr2CuO3	1	mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(48H,850C)-Q to RT in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8424	SUP0110123		TlSr2Ba2Cu2O7(CO3,NO3)	Tl1Sr2Ba2Cu2C0.9N0.1O10	Tl	1	Sr	2	Ba	2	Cu	2	C	0.9	N	0.1									O	10			1998																											3	Tl1222																				43					43																																																																																														BaCuO2,BaO,SrCO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(48H,850C)-Q to RT in air +ANN(290C,30min, in flowing 10%H2/Ar gas					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8425	SUP0110123		TlSr2Ba2Cu2O7(CO3,NO3)	Tl1Sr2Ba2Cu2C0.8N0.2O10	Tl	1	Sr	2	Ba	2	Cu	2	C	0.8	N	0.2									O	10			1998																											3	Tl1222				3.881	30.535	16.472														61					61																																																																																														Tl2O3,SrO2,Sr2CuO3	1	mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(48H,850C)-Q to RT in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8426	SUP0110123		TlSr2Ba2Cu2O7(CO3,NO3)	Tl1Sr2Ba2Cu2C0.8N0.2O10	Tl	1	Sr	2	Ba	2	Cu	2	C	0.8	N	0.2									O	10			1998																											3	Tl1222																				49					49																																																																																														BaCuO2,BaO,SrCO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(48H,850C)-Q to RT in air +ANN(290C,30min, in flowing 10%H2/Ar gas					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8427	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.9N0.1O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.9	N	0.1									O	10			1998																												Tl1222				3.821		16.503														40					40																																																																																														PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8428	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.9N0.1O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.9	N	0.1									O	10			1998																												Tl1222																				76					76																																																																																														PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air +ANN(290C,30min, in flowing 10%H2/Ar gas					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8429	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.7N0.3O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.7	N	0.3									O	10			1998																												Tl1222																				28					28																																																																																														PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8430	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.7N0.3O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.7	N	0.3									O	10			1998																												Tl1222																				70					70																																																																																														PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air +ANN(290C,30min, in flowing 10%H2/Ar gas					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8431	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.5N0.5O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.5	N	0.5									O	10			1998																												Tl1222																				24					24																																																																																														PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8432	SUP0110123	impurity=Pb0.5Tl0.5Sr2CuO5	(Tb,Tl)Sr4Cu2O7(CO3,NO3)	Pb0.5Tl0.5Sr4Cu2C0.5N0.5O10	Pb	0.5	Tl	0.5	Sr	4	Cu	2	C	0.5	N	0.5									O	10			1998																												Tl1222	I4/mmm																			70					70										35																																																																																				PbO,Tl2O3,SrO2,Sr2CuO3,TlNO3,CuO		mixture-alumina tube-quartz ampoules(10E-4 mbar)-heat(850C)-heat(850C,48H)-Q to RT in air +ANN(290C,30min, in flowing 10%H2/Ar gas					The Effect of Nitrates on Thallium based Oxycarbonate Superconductors	1998		School of Chemistry, University of Birmingham, Edgbaston, Birmingham, B15 2, UK	J.Superconductivity,11(1998)123	Bernard Raveau,I. Gameson,Martin O. Jones,P.P. Edwards		
8433	NAT3750301		(Sr,Ca)3Cu2(O4Cl2)	Sr2.3Ca0.7Cu2Cl1.3O4+Z	Sr	2.3	Ca	0.7	Cu	2	Cl	1.3													O	4+Z			1995																											2					3.8679		22.161															90	80			80																																																																							mOhm,cm											38														high-pressure synthesis,(5.0GPa,1000C,1H),10% exeess CuCO2 added.					Superconductivity at 80 K in (Sr,Ca)3Cu2O4+deltaCl2-y induced by apical oxygen doping	5		Superconductivity research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome, 1-Chome, Koto-ku, Tokyo 125, Japan	Nature,375(1995)301	C.Q. Jin,H. Yamauchi,N. Kushizuka,P. Laffez,S. Adachi,S. Tanaka,T. Tamura,T. Tatsuki,X.-J. Wu		
8434	SUP0090259	TCFIG shows Tc vs x in YBa2(Cu1-xAux)3Oz,x is determined by EDX	YBa2(Cu,Au)3O7	Y1Ba2Cu2.955Au0.045O7-Z	Y	1	Ba	2	Cu	2.955	Au	0.045													O	7-Z		3	1996																												Y123																						91.5			91.5	TC8434																																																																																														5	starting composition Y:Ba:Cu:Au=1:8:20:x or  1:8:(20-x):x, using yttria-stabiliqedzirconia					Effect of Gold Doping on the Superconducting Critical Temperature and Transition Width in Single-Crystal YBa2Cu3O7-z (YBCO)			Department of Physics and Materials Research Laboratory, University of Illinois at Urbana-Champaign, 1110 West Green Street, Urbana, Illinos 61801	J.Superconductivity,9(1996)259	D.M. Ginsberg,H. Ikuta		
8435	JSC1050609		(La,Ba)2CuO2(BO3)	La1Ba1Cu1B1O5	La	1	Ba	1	Cu	1	B	1													O	5			1993								240																			2	0201				3.943		7.508																	4.2																																																																																																		seact(870C,48H, in air)-SIN(950C,72H)-annealing in high O2 atmosphese					BaCuO2BO3:A New Single Layer Cuprate Containing BO3-,3 Anion oups as Connecting Elements	3		Max-Planck-Institut fur Festkorperforschung, Heisenbergstasse 1,7000 Sututtgart 80, Federal Republic of Germany	J.Solid State Chem.105(0993)609-612	J. MAIER,LI RUKANG,R.K. KREMER		
8436	PHC3010205		LaBaCaCu3O7	La1Ba1Ca1Cu3O7	La	1	Ba	1	Ca	1	Cu	3													O	7			1998																											2	1113				3.8689		11.6459															69	63			63																																																																																														La2O3,BaCO3,CaCO3,CuO,Co2O3,NiO,Ga2O3	1	mixture-heat (975C,12H in air)-FC to RT-ANN(575C,24H in flowing O2)-FC to RT					Effect of Cu-site Co, Ni and Ga substitution on the superconductivity of tetragonal LaBaCaCu3O7 system	199806		Centre for Superconducting and Electronic Materials, University of Wollongong, Wollonong, NSW 2522, Australia	Physica.C,301(1998)205-214	A.V. Narlikar,H.K. Liu,J. Horvat,M.P. Das,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8437	PHC2080286		(Ca,Sr)0.9CuOz	Ca0.27Sr0.63Cu1O2	Ca	0.27	Sr	0.63	Cu	1															O	2			1993																												IL																			50		110	110			110																																																																																																high -pressure synthesis(6GPa,1273K)					STRUCTURE AND SUPERCONDUCTIVITY OF THE INFINITE-LAYER COMPOUND(CA1-YSRY)1-XCUO2-Z	199304			PHYSICA C,208(1993)286	M.AZUMA,M.TAKANO,Y.TAKEDA,Z.HIROI	CA,SR,CU,O	
8438	PHC2080286		(Ca,Sr)0.95CuOz	Ca0.285Sr0.665Cu1O2-Z	Ca	0.285	Sr	0.665	Cu	1															O	2-Z			1993																												IL																						100			100																																																																																																high -pressure synthesis(6GPa,1273K)					STRUCTURE AND SUPERCONDUCTIVITY OF THE INFINITE-LAYER COMPOUND(CA1-YSRY)1-XCUO2-Z	199304			PHYSICA C,208(1993)286	M.AZUMA,M.TAKANO,Y.TAKEDA,Z.HIROI	CA,SR,CU,O	
8439	PHC2080286		(Ca,Sr)0.95CuOz	Ca0.285Sr0.665Cu1O2-Z	Ca	0.285	Sr	0.665	Cu	1															O	2-Z			1993																												IL																						40			40																																																																																																high -pressure synthesis(6GPa,1273K)					STRUCTURE AND SUPERCONDUCTIVITY OF THE INFINITE-LAYER COMPOUND(CA1-YSRY)1-XCUO2-Z	199304			PHYSICA C,208(1993)286	M.AZUMA,M.TAKANO,Y.TAKEDA,Z.HIROI	CA,SR,CU,O	
8440	PHC2080286		(Ca,Sr)0.95CuOz	Ca0.285Sr0.665Cu1O2-Z	Ca	0.285	Sr	0.665	Cu	1															O	2-Z			1993																												IL																							4.2																																																																																																		high -pressure synthesis(6GPa,1273K)					STRUCTURE AND SUPERCONDUCTIVITY OF THE INFINITE-LAYER COMPOUND(CA1-YSRY)1-XCUO2-Z	199304			PHYSICA C,208(1993)286	M.AZUMA,M.TAKANO,Y.TAKEDA,Z.HIROI	CA,SR,CU,O	
8441	PHC2100367	Tcsus is 44K, independent of x,solubility limit x=0.1	(Sr,Nd)CuO2	Sr0.9Nd0.1Cu1O2	Sr	0.9	Nd	0.1	Cu	1															O	2			1993																											2	IL				3.947		3.39																44			44																																																																																														R2O3,CuO,SrCuO2,SrCuO2		high-pressure synthesis(3GPa,1173K,1.5H)					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF THE INFINITE-LAYERCOMPOUNDS SR1-XLNXCUO2 (LN=LA,ND,SM,GD)	199306			PHYSICA C,210(1993)367	M.AZUMA,M.TAKANO,N.IKEDA,Y.BANDO,Y.TAKEDA,Z.HIROI	SR,CU,O,LA,ND,SM,GD	
8442	PHC2100367		(Sr,Gd)CuO2	Sr0.9Gd0.1Cu1O2	Sr	0.9	Gd	0.1	Cu	1															O	2			1993																												IL																			20			44			44																																																																																														R2O3,CuO,SrCuO2,SrCuO2		high-pressure synthesis(3GPa,1173K,1.5H)					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF THE INFINITE-LAYERCOMPOUNDS SR1-XLNXCUO2 (LN=LA,ND,SM,GD)	199306			PHYSICA C,210(1993)367	M.AZUMA,M.TAKANO,N.IKEDA,Y.BANDO,Y.TAKEDA,Z.HIROI	SR,CU,O,LA,ND,SM,GD	
8443	PHC2100367		(Sr,Sm)CuO2	Sr0.9Sm0.1Cu1O2	Sr	0.9	Sm	0.1	Cu	1															O	2			1993																												IL																			35			44			44																																																																																														R2O3,CuO,SrCuO2,SrCuO2		high-pressure synthesis(3GPa,1173K,1.5H)					SYNTHESIS AND SUPERCONDUCTING PROPERTIES OF THE INFINITE-LAYERCOMPOUNDS SR1-XLNXCUO2 (LN=LA,ND,SM,GD)	199306			PHYSICA C,210(1993)367	M.AZUMA,M.TAKANO,N.IKEDA,Y.BANDO,Y.TAKEDA,Z.HIROI	SR,CU,O,LA,ND,SM,GD	
8444	PHC2570313	RESRT=values at 180K	Sr2CaCu2(O,F)z	Sr2Ca1Cu2F2O4.6	Sr	2	Ca	1	Cu	2	F	2													O	4.6			1996																											2	0212				3.843		19.88															100	99			99																																																																							mOhm,cm											2.48														mixture-sealed in Au capsule-high pressure synthesis (5.5GPa,1250C,3H)-Q to RT					New oxyfluoride superconductors Sr2Can-1CunO2n+zF2+-y (N=2; Tc=99K,n=3; Tc=111K) prepared at high pressure			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C.257,(1996)313-320	E. Takayama-Muromachi,T. Kawashima,Y. Matsui		
8445	PHC2570313	RESRT=values at 180K	Sr2Ca2Cu3(O,F)z	Sr2Ca2Cu3F3.2O6.2	Sr	2	Ca	2	Cu	3	F	3.2													O	6.2			1996																											2	0223				3.84		26.17															110	111			111																																																																							mOhm,cm											7.3														mixture-sealed in Au capsule-high pressure synthesis (5.5GPa,1250C,3H)-Q to RT					New oxyfluoride superconductors Sr2Can-1CunO2n+zF2+-y (N=2; Tc=99K,n=3; Tc=111K) prepared at high pressure			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C.257,(1996)313-320	E. Takayama-Muromachi,T. Kawashima,Y. Matsui		
8446	PHC2670106	it contains 0212 phase(Sr2SrCuOz).S/C due to 0212 phase	Sr2CuOz	Sr2Cu1O3.1	Sr	2	Cu	1																	O	3.1			1996																											2	0201				3.788		12.434																70			70																																																																																																mixture-sealed in Au capsule-high pressure synthesis (5-6GPa,900-1300C,0.5-3H)-Q to RT, SrO2 as oxydiqing agent					Superconductivity in the series of compounds Sr2Can-1CunOy (n=1~4) prepared under high pressure			National Institute for Research in Inorganic Materials,1-1 Namiki,Tsukuba,Ibaraki 305, Japan	Physica.C,267(1996)106-112	E. Takayama-Muromachi,T. Kawashima	Sr, Ca, Cu, O	
8447	PHC2670106	not S/C	Sr2CuOz	Sr2Cu1O3.2	Sr	2	Cu	1																	O	3.2		1	1996																											2	0201				3.791		12.425																	5																																																																																																		mixture-sealed in Au capsule-high pressure synthesis (5-6GPa,900-1300C,0.5-3H)-Q to RT, SrO2 as oxydiqing agent					Superconductivity in the series of compounds Sr2Can-1CunOy (n=1~4) prepared under high pressure			National Institute for Research in Inorganic Materials,1-1 Namiki,Tsukuba,Ibaraki 305, Japan	Physica.C,267(1996)106-112	E. Takayama-Muromachi,T. Kawashima	Sr, Ca, Cu, O	
8448	PHC2670106	0212 phase is dominant,0201 and 0223 phases appers. Two step transition. Tc=109K maybe due to 0223 phase.	Sr2CaCu2Oz	Sr2Ca1Cu2O5.5	Sr	2	Ca	1	Cu	2															O	5.5			1996																											2	0212				3.821		20.74																77			77																																																																																																mixture-sealed in Au capsule-high pressure synthesis (5-6GPa,900-1300C,0.5-3H)-Q to RT, SrO2 as oxydiqing agent					Superconductivity in the series of compounds Sr2Can-1CunOy (n=1~4) prepared under high pressure			National Institute for Research in Inorganic Materials,1-1 Namiki,Tsukuba,Ibaraki 305, Japan	Physica.C,267(1996)106-112	E. Takayama-Muromachi,T. Kawashima	Sr, Ca, Cu, O	
8449	PHC2670106	0212,0201,0223,0234, phases were contained	Sr2Ca2Cu3Oz	Sr2Ca2Cu3O5.5	Sr	2	Ca	2	Cu	3															O	5.5			1996																											2	0223				3.863		27.22																109			109																																																																																																					Superconductivity in the series of compounds Sr2Can-1CunOy (n=1~4) prepared under high pressure			National Institute for Research in Inorganic Materials,1-1 Namiki,Tsukuba,Ibaraki 305, Japan	Physica.C,267(1996)106-112	E. Takayama-Muromachi,T. Kawashima	Sr, Ca, Cu, O	
8450	PHC2670106	0201,0212,0223,0234 phases weres contained. 0234 phase is dominant. Tc due to 0234 phase	Sr2(Sr,Ca)Cu3Oz	Sr2Ca1Cu2.8O7.5	Sr	2	Ca	1	Cu	2.8															O	7.5			1996																												0234				3.901		33.82																83			83																																																																																																					Superconductivity in the series of compounds Sr2Can-1CunOy (n=1~4) prepared under high pressure			National Institute for Research in Inorganic Materials,1-1 Namiki,Tsukuba,Ibaraki 305, Japan	Physica.C,267(1996)106-112	E. Takayama-Muromachi,T. Kawashima	Sr, Ca, Cu, O	
8451	APJ0354293	Jc=values at H=IT	Sr2CaCu2(O,F)z	Sr2Ca1Cu2F2O4.6	Sr	2	Ca	1	Cu	2	F	2													O	4.6			1996																											2	0212																						99			99																																		HIR8451																																																																			Dritical Current Densities and Irreversibility Fields of High Temperature Superconductor Sr2Ca2Cu3O7+z and Sr2Can-1CunO2n+zF2+y(n=2,3)			Department of Applied Physics,Tokyo Institute of Technology, Oh-okayama, Meguro,Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)4293	Eiji -TAKAYAMA-MUROMACHI,Shan Yu,Tetsuya KAWASHIMA,Yuichi OKUDA		
8452	APJ0354293	Jc=values at H=IT	Sr2Ca2Cu3(O,F)z	Sr2Ca2Cu3F3.2O6.2	Sr	2	Ca	2	Cu	3	F	3.2													O	6.2			1996																											2	0223																						111			111																																		HIR8452																																																																			Dritical Current Densities and Irreversibility Fields of High Temperature Superconductor Sr2Ca2Cu3O7+z and Sr2Can-1CunO2n+zF2+y(n=2,3)			Department of Applied Physics,Tokyo Institute of Technology, Oh-okayama, Meguro,Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)4293	Eiji -TAKAYAMA-MUROMACHI,Shan Yu,Tetsuya KAWASHIMA,Yuichi OKUDA		
8453	SUP0100507		(Y,Pr,Cd)Ba2Cu3O7	Y0.6Pr0.2Cd0.2Ba2Cu3O7-Z	Y	0.6	Pr	0.2	Cd	0.2	Ba	2	Cu	3											O	7-Z		1	1997																											3	Y123				3.8415	3.8956	11.6819													47			49			49																																																																																															1	mixture-CAL(930C,24H,in air)-pellet-SIN(950C,24H)-ANN(500C24H, in O2 flow)-slow cool to RT (1C/min)					Effect of Cd and Cd-Ca Substitution on the Superconductivity in Y1-xPrxBa2Cu3O7-delta Superconductor			Department of Physics, Saurashtra University, Rajkot 360 005, India	J.Superconductivity , 10(1997)507	Amish G. Joshi,C.M. Thakker,D.G. Kuberkar,M.V.S. Rao,Nikesh A. Shah,R.G. Kulkarni		
8454	PR0422551		(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3		1	1990									7.29																		1	BKBO				4.29															23		24				23.5																				T	defined as 0.9Rn,WHH theory	15.4							T/K			0.916				A		45.3			A	average particle size=2 micron,magnetization	803																																																			BaO,K2O,Bi2O3		mixture-ANN(700C,1H)-pellet-ANN					MAGNETIC PROPERTIES OF POLYCRYSTALLINE BA0.5K0.5BIO3	199008	MAGNETIZATION	DEPARTMENT OF PHYSICS, NATIONAL TAIWAN UNIVERSITY, TAIPEI, TAIWAN	PHY.REV.B,42(1990)2551	D.S. Lee,D.S.LEE,H.C. Yang,H.C.YANG,H.E. Horng,H.E.HORNG,M.H. Hsieh,M.H.HSIEH	BA,K,BI,O	
8455	PHC2290389	SIS tunneling, counter electrode=Au,K-content is not clear,estimated from Tc(by Asada)	(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3			1994																												BKBO																				28.6					28.6																																															4.3	3.5	1																																															electrochemical crystal growth, 210 in O2					Tunneling studies on Ba1-xKxBiO3 single crystals with Tc=15-30K	199408			Physica C, 229(1994)389-395	J.Akimitsu,M.Furuya,M.Kosugi,T.Ekino,T.Uchida,Y.Nagata	Ba,K,Bi,O	
8456	PHC3010205		LaBaCa(Cu,Co)3O7	La1Ba1Cu2.94Co0.06O7	La	1	Ba	1	Cu	2.94	Co	0.06													O	7			1998																											2	1113				3.8676		11.6433															60	57			57																																																																																														La2O3,BaCO3,CaCO3,CuO,Co2O3,NiO,Ga2O3	1	mixture-heat (975C,12H in air)-FC to RT-ANN(575C,24H in flowing O2)-FC to RT					Effect of Cu-site Co, Ni and Ga substitution on the superconductivity of tetragonal LaBaCaCu3O7 system	199806		Centre for Superconducting and Electronic Materials, University of Wollongong, Wollonong, NSW 2522, Australia	Physica.C,301(1998)205-214	A.V. Narlikar,H.K. Liu,J. Horvat,M.P. Das,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8457	PHC3010205		LaBaCa(Cu,Co)3O7	La1Ba1Cu2.88Co0.12O7	La	1	Ba	1	Cu	2.88	Co	0.12													O	7			1998																											2	1113				3.8671		11.6426															45	40			40																																																																																														La2O3,BaCO3,CaCO3,CuO,Co2O3,NiO,Ga2O3	1	mixture-heat (975C,12H in air)-FC to RT-ANN(575C,24H in flowing O2)-FC to RT					Effect of Cu-site Co, Ni and Ga substitution on the superconductivity of tetragonal LaBaCaCu3O7 system	199806		Centre for Superconducting and Electronic Materials, University of Wollongong, Wollonong, NSW 2522, Australia	Physica.C,301(1998)205-214	A.V. Narlikar,H.K. Liu,J. Horvat,M.P. Das,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8458	PHC3010205		LaBaCa(Cu,Co)3O7	La1Ba1Cu2.82Co0.18O7	La	1	Ba	1	Cu	2.82	Co	0.18													O	7			1998																											2	1113				3.8665		11.6403															20	14			14																																																																																														La2O3,BaCO3,CaCO3,CuO,Co2O3,NiO,Ga2O3	1	mixture-heat (975C,12H in air)-FC to RT-ANN(575C,24H in flowing O2)-FC to RT					Effect of Cu-site Co, Ni and Ga substitution on the superconductivity of tetragonal LaBaCaCu3O7 system	199806		Centre for Superconducting and Electronic Materials, University of Wollongong, Wollonong, NSW 2522, Australia	Physica.C,301(1998)205-214	A.V. Narlikar,H.K. Liu,J. Horvat,M.P. Das,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8459	PHC3010205		LaBaCa(Cu,Co)3O7	La1Ba1Cu2.76Co0.24O7	La	1	Ba	1	Cu	2.76	Co	0.24													O	7			1998																											2	1113				3.8649		11.6382																	4.2																																																																																																La2O3,BaCO3,CaCO3,CuO,Co2O3,NiO,Ga2O3	1	mixture-heat (975C,12H in air)-FC to RT-ANN(575C,24H in flowing O2)-FC to RT					Effect of Cu-site Co, Ni and Ga substitution on the superconductivity of tetragonal LaBaCaCu3O7 system	199806		Centre for Superconducting and Electronic Materials, University of Wollongong, Wollonong, NSW 2522, Australia	Physica.C,301(1998)205-214	A.V. Narlikar,H.K. Liu,J. Horvat,M.P. Das,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8460	PHC3070067			Bi2Sr2Ca0.89Pr0.11Cu2OZ	Bi	2	Sr	2	Ca	0.89	Pr	0.11	Cu	2											O	Z			1998																											3	Bi2212				5.411	5.4221	30.816																87.8			87.8																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8461	PHC3070067			Bi2Sr2Ca0.83Pr0.17Cu2OZ	Bi	2	Sr	2	Ca	0.83	Pr	0.17	Cu	2											O	Z			1998																											3	Bi2212				5.4	5.4318	30.761																84.3			84.3																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8462	PHC3070067			Bi2Sr2Ca0.72Pr0.28Cu2OZ	Bi	2	Sr	2	Ca	0.72	Pr	0.28	Cu	2											O	Z			1998																											3	Bi2212				5.4357	5.4396	30.697																73			73																																																																																																single crystals were grown by self-flux method					Pr-doping effect on the structure and superconductivity of Bi2Sr2Ca1-xPrxCu2Oy single crystals	199810		Department of Materials Science and Engineering, University of Science and Technology of China, Academia Sinica, Hefei 230026, China	Physica.C,307(1998)67-73	H.C. Ku,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun		
8463	APJ0354293	Jc=values at H=IT	Sr2Ca2Cu3Oz	Sr1Ca2Cu3OZ	Sr	1	Ca	2	Cu	3															O	Z			1996																											2	0223																						109			109																																		HIR8463																																																																			Dritical Current Densities and Irreversibility Fields of High Temperature Superconductor Sr2Ca2Cu3O7+z and Sr2Can-1CunO2n+zF2+y(n=2,3)			Department of Applied Physics,Tokyo Institute of Technology, Oh-okayama, Meguro,Tokyo 152, Japan	Jpn.J.Appl.Phys.35(1996)4293	Eiji -TAKAYAMA-MUROMACHI,Shan Yu,Tetsuya KAWASHIMA,Yuichi OKUDA		
8464	PHC3070265			Bi2Sr2Ca1Cu2O8.234	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.234	3	1998																												Bi2212																				84					84																																									A	reversible M-H curve, London eq.		2590																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8465	PHC3070265			Bi2Sr2Ca1Cu2O8.248	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.248	3	1998																												Bi2212																				86					86																																									A	reversible M-H curve, London eq.		2300																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8466	PHC3070265			Bi2Sr2Ca1Cu2O8.26	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.26	3	1998																												Bi2212																				91					91																																									A	reversible M-H curve, London eq.		2120																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8467	PHC3070265			Bi2Sr2Ca1Cu2O8.272	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.272	3	1998																												Bi2212																				92.2					92.2																																									A	reversible M-H curve, London eq.		2050																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8468	PHC3070265			Bi2Sr2Ca1Cu2O8.288	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.288	3	1998																												Bi2212																				90.2					90.2																																									A	reversible M-H curve, London eq.		2106																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8469	PHC3070265			Bi2Sr2Ca1Cu2O8.291	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.291	3	1998																												Bi2212																				89.1					89.1																																									A	reversible M-H curve, London eq.		2130																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8470	PHC3070265			Bi2Sr2Ca1Cu2O8.293	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.293	3	1998																												Bi2212																				87.5					87.5																																									A	reversible M-H curve, London eq.		2320																																																				cristals were grown from Bi-rich melts by a directional solidification method with Bi:Sr:Ca:Cu:-2.4:2:1:2					Correlation between Tc and ns/m* in Bi2Sr2CaCu2O8+delta single crystals	199810		ddepartment of Material Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Physica.C,307(1998)265-270	Shuquan Guo,Wenbin Wu,Xia Zhao,Xiao-Guang Li,Xiaojuan Fan,Xuefeng Sun,Xuefeng sun,Zhongxian Zhao		
8471	IOM0341255		TmBa2Cu3Oz	Tm1Ba2Cu3OZ	Tm	1	Ba	2	Cu	3															O	Z		3	1998																											3	Y123				3.829	3.877	11.699	3											K						0.2																																																																																0.068				0.24																						Neorganicheskie materialy(Inorganic Materials), 34(1998)1255			
8472	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6+Z	Y	1	Ba	2	Cu	3															O	6+Z		2	1996																												Y123																		K		22					22																																														meV	3.7	3.5	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8473	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O	6+Z	6.54	2	1996																												Y123																		K		40					40																																														meV	6.2	3.3	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8474	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6+Z	6.6	2	1996																												Y123																		K		42					42																																														meV	6.15	3.05	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8475	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	6+Z	6.72	2	1996																												Y123																		K		58					58																																														meV	7	2.9	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8476	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.74	Y	1	Ba	2	Cu	3															O	6+Z	6.74	2	1996																												Y123																		K		60					60																																														meV	7.5	2.8	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8477	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	6+Z	6.8	2	1996																												Y123																		K		77					77																																														meV	7.5	2.25	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8478	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	6+Z	6.85	2	1996																												Y123																		K		77					77																																														meV	9	2.7	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8479	SOV0020061		YBa2Cu3Oz	Y1Ba2Cu3O6.88	Y	1	Ba	2	Cu	3															O	6+Z	6.88	2	1996																												Y123																		K		82					82																																														meV	12	2.85	1																																														11	sol-gel method-press into bar-ANN(550C,5H)-cool to RT (10C/H)									Fizika tverdogo tela (Phys. Of the Solid State), 38(1996)1304			
8480	SSC1070509	semicoducting	(Pr,Ca)Ba2Cu3O7	Pr0.6Ca0.4Ba2Cu3O7-Z	Pr	0.6	Ca	0.4	Ba	2	Cu	3													O	7-Z		1	1998																											3	Y123																		K					5																																																																																																Pr6O11,CaCO3,BaCO3,CuO		precursor(Pr-Ca-Ba-Cu-O)+5wt% KclO4-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8481	SSC1070509	imprity phases=Ba O2, Ba Cu O2	(Pr,Ca)Ba2Cu3O7	Pr0.5Ca0.5Ba2Cu3O7-Z	Pr	0.5	Ca	0.5	Ba	2	Cu	3													O	7-Z		1	1998																											3	Y123				3.877	3.905	11.61												K			52	52			52										12																																																																																				Pr6O11,CaCO3,BaCO3,CuO		precursor(Pr-Ca-Ba-Cu-O)+5wt% KclO4-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8482	SSC1070509		(Pr,Ca)Ba2Cu3O7	Pr0.4Ca0.6Ba2Cu3O7-Z	Pr	0.4	Ca	0.6	Ba	2	Cu	3													O	7-Z			1998																											3	Y123																		K			33	33			33																																																																																														Pr6O11,CaCO3,BaCO3,CuO		precursor(Pr-Ca-Ba-Cu-O)+5wt% KclO4-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8483	SSC1070509	impurity phase=Ba Cu O2	(Pr,Ca)Ba2Cu3O7	Pr0.6Ca0.4Ba2Cu3O7-Z	Pr	0.6	Ca	0.4	Ba	2	Cu	3													O	7-Z			1998																											2	Y123																		K			39	39			39																																																																																																precursor(Pr-Ca-Ba-Cu-O)-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8484	SSC1070509	impurity phase=Ba Cu O2	(Pr,Ca)Ba2Cu3O7	Pr0.5Ca0.5Ba2Cu3O7-Z	Pr	0.5	Ca	0.5	Ba	2	Cu	3													O	7-Z			1998																											2	Y123				3.844		11.646												K			98	98			98																																																																																																precursor(Pr-Ca-Ba-Cu-O)-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8485	SSC1070509	impurity phase=Ba Cu O2	(Pr,Ca)Ba2Cu3O7	Pr0.4Ca0.6Ba2Cu3O7-Z	Pr	0.4	Ca	0.6	Ba	2	Cu	3													O	7-Z			1998																											2	Y123																		K			75	75			75																																																																																																precursor(Pr-Ca-Ba-Cu-O)-high pressure synthesis (1000C,5GPa)					OBSERVATION AND STUDIES OF 98 K SUPERCONDUCTIVITY IN OXYGEN-DEFICIENT TETRAGONAL Pr0.5Ca0.5Ba2Cu3O7-delta SYNTHESIZED UNDER HIGH-PRESSURE			Mational Laboratory for superconductivity, Center for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 10080, Peple's Republic of China	Solid State Commun.107(1998)509	D. Jin,D.Jin,F. Wu,F.Wu,L.F. Xu,L.F.Xu,Y.F. Xiong,Y.F.Xiong,Y.S. Yao,Y.S.Yao,Z.X. Zhao,Z.X.Zhao		
8486	SSC1080063	not S/C	Gd2Sr2Cu2TiOz	Gd2Sr2Cu2Ti1OZ	Gd	2	Sr	2	Cu	2	Ti	1													O	Z		1	1998																											2		I4/mmm																	K					13																																																																																																	1	mixture-CAL(1000C,48H)-pellet-SIN(1050C, in air)					SEARCH FOR SUPERCONDUCTIVITY IN Gd2-xCexCu2TiOy			Tata Institute of Fundamental Research, Homi Bhabha Road, Munbai-400005, India	Solid State Commun.108(1998)63	E. Sudhakar Reddy,E.V. Sampathkumaran,P.V. Patanjali,R. Pinto,R. Vijayaraghavan		
8487	SSC1080063	not S/C	(Gd,Ce)2Sr2Cu2TiOz	Gd1.95Ce0.05Sr2Cu2T11OZ	Gd	1.95	Ce	0.05	Sr	2	Cu	2	T1	1											O	Z		1	1998																											2																			K					13																																																																																																	1	mixture-CAL(1000C,48H)-pellet-SIN(1050C, in air)					SEARCH FOR SUPERCONDUCTIVITY IN Gd2-xCexCu2TiOy			Tata Institute of Fundamental Research, Homi Bhabha Road, Munbai-400005, India	Solid State Commun.108(1998)63	E. Sudhakar Reddy,E.V. Sampathkumaran,P.V. Patanjali,R. Pinto,R. Vijayaraghavan		
8488	SSC1080063	not S/C	(Gd,Ce)2Sr2Cu2TiOz	Gd0.5Ce0.5Sr2Cu2T11OZ	Gd	0.5	Ce	0.5	Sr	2	Cu	2	T1	1											O	Z		1	1998																											2																			K					13																																																																																																	1	mixture-CAL(1000C,48H)-pellet-SIN(1050C, in air)					SEARCH FOR SUPERCONDUCTIVITY IN Gd2-xCexCu2TiOy			Tata Institute of Fundamental Research, Homi Bhabha Road, Munbai-400005, India	Solid State Commun.108(1998)63	E. Sudhakar Reddy,E.V. Sampathkumaran,P.V. Patanjali,R. Pinto,R. Vijayaraghavan		
8489	SSC1080063	not S/C	(Gd,Ce)2Sr2Cu2TiOz	Gd1Ce1Sr2Cu2T11OZ	Gd	1	Ce	1	Sr	2	Cu	2	T1	1											O	Z		1	1998																											2																			K					13																																																																																																	1	mixture-CAL(1000C,48H)-pellet-SIN(1050C, in air)					SEARCH FOR SUPERCONDUCTIVITY IN Gd2-xCexCu2TiOy			Tata Institute of Fundamental Research, Homi Bhabha Road, Munbai-400005, India	Solid State Commun.108(1998)63	E. Sudhakar Reddy,E.V. Sampathkumaran,P.V. Patanjali,R. Pinto,R. Vijayaraghavan		
8490	PHC3010048		PrBaCaCu3O7	Pr1Ca1Cu3O7	Pr	1	Ca	1	Cu	3															O	7		1	1998																											2	1113				3.875		11.603												K					4.2																																																																																																	1	"""mixture-fire(975-995C)-ANN(575C,24H)"""					Synthesis, structural aspects and superconductivity of La1-xRExBaCaCu3O7 with RE=Nd,Dy,Sm and Pr	199805		National Physical Laboratory, Krishnan Marg, New Delhi 110012, India	Physica.C,301(1998)48-54	A.V. Narlikar,J. Horvat,Rajvir Singh,S.X. Dou,V.P.S. Awana		
8491	SSC1080425			La1.82Ca1.16Y0.02Cu2O6	La	1.82	Ca	1.16	Y	0.02	Cu	2													O	6			1998																												2126																		K				40			40																																																																																																					IRREVERSIBILITY FIELDS AND CRITICAL CURRENTS FOR PURE AND Y-SUBSTITUTED La1.82Ca1.18Cu2O6 SUPERCONDUCTORS			Physics Department,Nortern Illinois University, Dekalb, IL 60115, U.S.A.	Solid State Commun.108(1998)425	B. Dabrowski,K. Rogacki,P.W. Klamut		
8492	SSC1080613		(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.8Pb0.3Sr2Ca2Cu3Oz	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	3											O	z			1998																												Bi2223																			102.7		110				106.35																																																																																															1	mixture-CAL(800C,24H)-pellet-SIN(840C,144H)-Cool to RT (2C/min)					THE EFFECT OF VANADIUM DOPING ON SUPERCONDUCTING PROPERTIES OF (Bi,Pb)2Sr2Ca2(Cu1-xVx)3Oy CERAMICS			Department of Physics, Faculty of Science, Ege University, 35100 Bornova, Izmir-Turkey	Solid State Commun.108(1998)613	Dogan Abukay,Mustafa Tape		
8493	SSC1080613		(Bi,Pb)2Sr2Ca2(Cu,V)3Oz	Bi1.8Pb0.3Sr2Ca2Cu2.97V0.03Oz	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	2.97	V	0.03									O	z			1998																												Bi2223																			103.2		110				106.6																																																																																															1	mixture-CAL(800C,24H)-pellet-SIN(840C,144H)-Cool to RT (2C/min)					THE EFFECT OF VANADIUM DOPING ON SUPERCONDUCTING PROPERTIES OF (Bi,Pb)2Sr2Ca2(Cu1-xVx)3Oy CERAMICS			Department of Physics, Faculty of Science, Ege University, 35100 Bornova, Izmir-Turkey	Solid State Commun.108(1998)613	Dogan Abukay,Mustafa Tape		
8494	SSC1080613		(Bi,Pb)2Sr2Ca2(Cu,V)3Oz	Bi1.8Pb0.3Sr2Ca2Cu2.94V0.06Oz	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	2.94	V	0.06									O	z			1998																												Bi2223																			103.9		110				106.95																																																																																															1	mixture-CAL(800C,24H)-pellet-SIN(840C,144H)-Cool to RT (2C/min)					THE EFFECT OF VANADIUM DOPING ON SUPERCONDUCTING PROPERTIES OF (Bi,Pb)2Sr2Ca2(Cu1-xVx)3Oy CERAMICS			Department of Physics, Faculty of Science, Ege University, 35100 Bornova, Izmir-Turkey	Solid State Commun.108(1998)613	Dogan Abukay,Mustafa Tape		
8495	SSC1080613		(Bi,Pb)2Sr2Ca2(Cu,V)3Oz	Bi1.8Pb0.3Sr2Ca2Cu2.91V0.09Oz	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	2.91	V	0.09									O	z			1998																												Bi2223																			101.1		110				105.55																																																																																															1	mixture-CAL(800C,24H)-pellet-SIN(840C,144H)-Cool to RT (2C/min)					THE EFFECT OF VANADIUM DOPING ON SUPERCONDUCTING PROPERTIES OF (Bi,Pb)2Sr2Ca2(Cu1-xVx)3Oy CERAMICS			Department of Physics, Faculty of Science, Ege University, 35100 Bornova, Izmir-Turkey	Solid State Commun.108(1998)613	Dogan Abukay,Mustafa Tape		
8496	NAT3940157		(La,Nd,Ca)2CuO4	La1.798Nd0.052Ca0.15Cu1O4	La	1.798	Nd	0.052	Ca	0.15	Cu	1													O	4			1998																											2	T	I4/mmm																			31.6					31.6																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8497	NAT3940157		(La,Nd,Ca)2CuO4	La1.736Nd0.117Ca0.138Ba0.012Cu1O4	La	1.736	Nd	0.117	Ca	0.138	Ba	0.012	Cu	1											O	4			1998																											2	T	I4/mmm																			29.4					29.4																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8498	NAT3940157		(La,Nd,Ca,Ba,)2CuO4	La1.65Nd0.2Ca0.122Ba0.028Cu1O4	La	1.65	Nd	0.2	Ca	0.122	Ba	0.028	Cu	1											O	4			1998																											2	T	I4/mmm																			27.1					27.1																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8499	NAT3940157		(La,Nd,Ca,Ba,)2CuO4	La1.562Nd0.288Ca0.106Ba0.044Cu1O4	La	1.562	Nd	0.288	Ca	0.106	Ba	0.044	Cu	1											O	4			1998																											2	T	I4/mmm																			23					23																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8500	NAT3940157		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1998																											2	T	I4/mmm																			32.5					32.5																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8501	NAT3940157		(La,Sr,Ca,Ba)2CuO4	La1.85Sr0.12Ca0.016Ba0.014Cu1O4	La	1.85	Sr	0.12	Ca	0.016	Ba	0.014	Cu	1											O	4			1998																											2	T	I4/mmm																	K		30					30																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8502	NAT3940157		(La,Sr,Ca,Ba)2CuO4	La1.85Sr0.09Ca0.034Ba0.026Cu1O4	La	1.85	Sr	0.09	Ca	0.034	Ba	0.026	Cu	1											O	4			1998																											2	T	I4/mmm																	K		28.5					28.5																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8503	NAT3940157		(La,Sr,Ca,Ba)2CuO4	La1.85Sr0.06Ca0.05Ba0.04Cu1O4	La	1.85	Sr	0.06	Ca	0.05	Ba	0.04	Cu	1											O	4			1998																											2	T	I4/mmm																	K		27					27																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8504	NAT3940157		(La,Sr,Ca,Ba)2CuO4	La1.85Sr0.03Ca0.066Ba0.054Cu1O4	La	1.85	Sr	0.03	Ca	0.066	Ba	0.054	Cu	1											O	4			1998																											2	T	I4/mmm																	K		24					24																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8505	NAT3940157		(La,Sr,Ca,Ba)2CuO4	La1.85Sr0.016Ca0.074Ba0.06Cu1O4	La	1.85	Sr	0.016	Ca	0.074	Ba	0.06	Cu	1											O	4			1998																											2	T	I4/mmm																	K		23.5					23.5																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8506	NAT3940157		(La,Ca,Ba)2CuO4	La1.85Ca0.082Ba0.068Cu1O4	La	1.85	Ca	0.082	Ba	0.068	Cu	1													O	4			1998																											2	T	I4/mmm																	K		20					20																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8507	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.8Nd0.05Ca0.074Ba0.076Cu1O4	La	1.8	Nd	0.05	Ca	0.074	Ba	0.076	Cu	1											O	4			1998																											2	T	I4/mmm																	K		2.05					2.05																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8508	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.75Nd0.1Ca0.064Ba0.086Cu1O4	La	1.75	Nd	0.1	Ca	0.064	Ba	0.086	Cu	1											O	4			1998																											2	T	I4/mmm																	K		18					18																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8509	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.7Nd0.15Ca0.056Ba0.094Cu1O4	La	1.7	Nd	0.15	Ca	0.056	Ba	0.094	Cu	1											O	4			1998																											2	T	I4/mmm																	K		16					16																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8510	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.65Nd0.2Ca0.046Ba0.104Cu1O4	La	1.65	Nd	0.2	Ca	0.046	Ba	0.104	Cu	1											O	4			1998																											2	T	I4/mmm																	K					15																																																																																																		mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8511	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.6Nd0.25Ca0.038Ba0.112Cu1O4	La	1.6	Nd	0.25	Ca	0.038	Ba	0.112	Cu	1											O	4			1998																											2	T	I4/mmm																	K					15																																																																																																		mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8512	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.55Nd0.3Ca0.028Ba0.122Cu1O4	La	1.55	Nd	0.3	Ca	0.028	Ba	0.122	Cu	1											O	4			1998																											2	T	I4/mmm																	K					15																																																																																																		mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8513	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.5Nd0.35Ca0.018Ba0.132Cu1O4	La	1.5	Nd	0.35	Ca	0.018	Ba	0.132	Cu	1											O	4			1998																											2	T	I4/mmm																	K					15																																																																																																		mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8514	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.45Nd0.4Ca0.01Ba0.14Cu1O4	La	1.45	Nd	0.4	Ca	0.01	Ba	0.14	Cu	1											O	4			1998																											2	T	I4/mmm																	K					15																																																																																																		mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8515	NAT3940157		(La,Nd,Ca,Ba)2CuO4	La1.85Sr0.038Ba0.112Cu1O4	La	1.85	Sr	0.038	Ba	0.112	Cu	1													O	4			1998																											3	T	Abma																	K		32					32																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8516	NAT3940157		(La,Nd,Sr,Ba)CuO4	La1.842Nd0.008Sr0.036Ba0.114Cu1O4	La	1.842	Nd	0.008	Sr	0.036	Ba	0.114	Cu	1											O	4			1998																											3	T	Abma																	K		31.7					31.7																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8517	NAT3940157		(La,Nd,Sr,Ba)CuO4	La1.812Nd0.038Sr0.026Ba0.124Cu1O4	La	1.812	Nd	0.038	Sr	0.026	Ba	0.124	Cu	1											O	4			1998																											3	T	Abma																	K		31.1					31.1																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8518	NAT3940157		(La,Nd,Sr,Ba)CuO4	La1.776Nd0.074Sr0.014Ba0.136Cu1O4	La	1.776	Nd	0.074	Sr	0.014	Ba	0.136	Cu	1											O	4			1998																											3	T	Abma																	K		30					30																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8519	NAT3940157		(La,Nd,Ba)2CuO4	La1.736Nd0.116Ba0.15Cu1O4	La	1.736	Nd	0.116	Ba	0.15	Cu	1													O	4			1998																											3	T	Abma																	K		29					29																																																																																																mixture-SIN(1050C,200H in air)-Q to RT-ANN(400C,50H in flowing O2)					Cation effects in doped La2CuO4 superconductors	7		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE,UK	Nature.394(1998)157	A.L. Khalanov,J.A. McAllister,J.P. Attfield		
8520	APJ0374342		AlSr2(Ho,Ca)Cu2O7	Al1Sr2Ho0.65Ca0.35Cu2O7.01	Al	1	Sr	2	Ho	0.65	Ca	0.35	Cu	2											O	7	7.01		1998																												Al1212	Abma																	K																																																																																																							mixture-SIN(1050C, 200H, in air)-Q to RT-ANN(400C, 50H in flowing O2)					Preparation and Structure of Al(Sr,Ca)2HoCu2O7 and AlSr2(Ho,Ca)Cu2O7 Cuprates			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)4342	Akira ONO,Jianfu MAO,Shigeo HORIUCHI		
8521	APJ0374342	weak superconducting signal	AlSr2(Ho,Ca)Cu2O7	Al1Sr2Ho0.5Ca0.5Cu2O7.05	Al	1	Sr	2	Ho	0.5	Ca	0.5	Cu	2											O	7	7.05		1998																												Al1212																		K		18					18																																																																																																mixture-SIN(1050C, 200H, in air)-Q to RT-ANN(400C, 50H in flowing O2)					Preparation and Structure of Al(Sr,Ca)2HoCu2O7 and AlSr2(Ho,Ca)Cu2O7 Cuprates			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)4342	Akira ONO,Jianfu MAO,Shigeo HORIUCHI		
8522	APJ0374342		AlSr2(Ho,Ca)Cu2O7	Al1Sr2Ho0.4Ca0.6Cu2O7	Al	1	Sr	2	Ho	0.4	Ca	0.6	Cu	2											O	7			1998																											2	Al1212				7.64		22.5												K		24					24																																																																																																mixture-SIN(1050C, 200H, in air)-Q to RT-ANN(400C, 50H in flowing O2)					Preparation and Structure of Al(Sr,Ca)2HoCu2O7 and AlSr2(Ho,Ca)Cu2O7 Cuprates			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)4342	Akira ONO,Jianfu MAO,Shigeo HORIUCHI		
8523	APJ0375535		BSr2Ca2Cu3O9	B1Sr2Ca2Cu3O9	B	1	Sr	2	Ca	2	Cu	3													O	9			1998																												B1223																		K				75			75																																																																																																Samples were prepared by high pressure synthesis(6GPa,1250C), for grain alignment, powders were cured in H=5T, 12H					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8524	APJ0375535		BSr2Ca3Cu4O11	B1Sr2Ca3Cu4O11	B	1	Sr	2	Ca	3	Cu	4													O	11			1998																												B1234																		K				110			110																																																																																																Samples were prepared by high pressure synthesis(6GPa,1250C), for grain alignment, powders were cured in H=5T, 12H					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8525	APJ0375535		BSr2Ca4Cu513	B1Sr2Ca4Cu5O13	B	1	Sr	2	Ca	4	Cu	5													O	13			1998																												B1245																		K				85			85																																																																																																Samples were prepared by high pressure synthesis(6GPa,1250C), for grain alignment, powders were cured in H=5T, 12H					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8526	APJ0370100	Fig. Show P=1,2,3 for a,b,c axis thermopower	(Sr,Ca)14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41		3	1998																																														K					20																																																																																																SrCO3, CaCO3, CuO		mixture-heat(900C, 12H in air)-mix with Nacl-Al2O3crucible-heat(990C for x=0.1030C for x=6.8)					Growth by the Flux Method and Transport Properties of Sr14-xCaxCu24O41 Single Crystals			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-77, Japan	Jpn.J.Appl.Phys.37(1998)100	Katsumi KAKIMOTO,Takashi NoOJI,Yiji KOIKE		
8527	APJ0370100	Fig. Show P=1,2,3 for a,b,c axis thermopower	(Sr,Ca)14Cu24O41	Sr7.2Ca6.8Cu24O41	Sr	7.2	Ca	6.8	Cu	24															O	41		3	1998																																														K					20																																																																																																SrCO3, CaCO3, CuO		mixture-heat(900C, 12H in air)-mix with Nacl-Al2O3crucible-heat(990C for x=0.1030C for x=6.8)					Growth by the Flux Method and Transport Properties of Sr14-xCaxCu24O41 Single Crystals			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-77, Japan	Jpn.J.Appl.Phys.37(1998)100	Katsumi KAKIMOTO,Takashi NoOJI,Yiji KOIKE		
8528	JAP0845080	Tc, Hirr were determined by the out-of-plane resistivity	(Hg,Cu)Ba2CuO4	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z			1998																												Hg1201																		K	92	94					94																																																																							mOhm.cm											340														see Physica C 273(1997)205					c-axis resistivity of Hg-1201 single crystals	199811		Laboratoire CRISMAT, UMR 6508 associee au CNRS,ISMRA et Universite'de Caen, 6 Boulevard du Mare'chal Juin, 14050 Caen Cedex, France	J.Appl.Phys.84(1998)5080	A. Daignere,A. Maignan,A. Ruyter,G. Villard		
8529	JAP0830377	ANN(490C,1500H), optimum doping	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K				93		0.5	93																																																																																																single crystal grown by pulling technique-ANN(600C, 2H)-ANN(conditions writhn in comment)-Q					Magnetic properties of YBa2Cu3Oy crystal with various oxygen annealing conditions	199801		Superconductivity Research Laboratory 1-16-25 Shibaura, Minato-ku, Tokyo 105 Japan	J.Appl.Phys.83(1998)377	Masato Murakami,Masaya Watahiki,Setuko Tajima,Wen-Jye Jang		
8530	JAP0830377	ANN(540C,1400H), underdoped sample	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K				91		1.2	91																																																																																																single crystal grown by pulling technique-ANN(600C, 2H)-ANN(conditions writhn in comment)-Q					Magnetic properties of YBa2Cu3Oy crystal with various oxygen annealing conditions	199801		Superconductivity Research Laboratory 1-16-25 Shibaura, Minato-ku, Tokyo 105 Japan	J.Appl.Phys.83(1998)377	Masato Murakami,Masaya Watahiki,Setuko Tajima,Wen-Jye Jang		
8531	JAP0830377	ANN(410C,1500H), overdoped sample	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K				89		1.5	89																																																																																																single crystal grown by pulling technique-ANN(600C, 2H)-ANN(conditions writhn in comment)-Q					Magnetic properties of YBa2Cu3Oy crystal with various oxygen annealing conditions	199801		Superconductivity Research Laboratory 1-16-25 Shibaura, Minato-ku, Tokyo 105 Japan	J.Appl.Phys.83(1998)377	Masato Murakami,Masaya Watahiki,Setuko Tajima,Wen-Jye Jang		
8532	JAP0830377	ANN(600C,720H)	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K				83		1.6	83																																																																																																single crystal grown by pulling technique-ANN(600C, 2H)-ANN(conditions writhn in comment)-Q					Magnetic properties of YBa2Cu3Oy crystal with various oxygen annealing conditions	199801		Superconductivity Research Laboratory 1-16-25 Shibaura, Minato-ku, Tokyo 105 Japan	J.Appl.Phys.83(1998)377	Masato Murakami,Masaya Watahiki,Setuko Tajima,Wen-Jye Jang		
8533	PHC3080289		(Pb,V)Sr(Ca,Y)Cu2O2	Pb0.5V0.5Sr2Ca0.7Y0.3Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	Z			1998																												Pb1212																		K	61			61			61																																																																																														PbO, V2O3, SrCO3, CaCO3, Y2O3, Cu2O	1	mixture-SIN(996C 4H in flowing O2)-ANN(800C,20H in air)-Q to LN2					Synthesis and superconductivity of a type of Pb-1212 phase (Pb,V)Sr2(Ca,Y)Cu2Oz	199811		Department of Physics, Kangwon National University, Chunchon 200-701, South Korea	Physica.C,308(1998)289-293	H.K. Lee		
8534	PHC3080289		(Pb,V)Sr(Ca,Y)Cu2O2	Pb0.5V0.5Sr2Ca0.6Y0.4Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.6	Y	0.4	Cu	2									O	Z			1998																												Pb1212																		K																																																																																																					PbO, V2O3, SrCO3, CaCO3, Y2O3, Cu2O	1	mixture-SIN(996C 4H in flowing O2)-ANN(800C,20H in air)-Q to LN2					Synthesis and superconductivity of a type of Pb-1212 phase (Pb,V)Sr2(Ca,Y)Cu2Oz	199811		Department of Physics, Kangwon National University, Chunchon 200-701, South Korea	Physica.C,308(1998)289-293	H.K. Lee		
8535	PHC3080289		(Pb,V)Sr(Ca,Y)Cu2O2	Pb0.5V0.5Sr2Ca0.5Y0.5Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	Z			1998																												Pb1212																		K																																																																																																					PbO, V2O3, SrCO3, CaCO3, Y2O3, Cu2O	1	mixture-SIN(996C 4H in flowing O2)-ANN(800C,20H in air)-Q to LN2					Synthesis and superconductivity of a type of Pb-1212 phase (Pb,V)Sr2(Ca,Y)Cu2Oz	199811		Department of Physics, Kangwon National University, Chunchon 200-701, South Korea	Physica.C,308(1998)289-293	H.K. Lee		
8536	PHC3080289	R=not zero down to 5K	(Pb,V)Sr(Ca,Y)Cu2O2	Pb0.5V0.5Sr2Ca0.4Y0.6Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.4	Y	0.6	Cu	2									O	Z			1998																												Pb1212																		K																																																																																																					PbO, V2O3, SrCO3, CaCO3, Y2O3, Cu2O	1	mixture-SIN(996C 4H in flowing O2)-ANN(800C,20H in air)-Q to LN2					Synthesis and superconductivity of a type of Pb-1212 phase (Pb,V)Sr2(Ca,Y)Cu2Oz	199811		Department of Physics, Kangwon National University, Chunchon 200-701, South Korea	Physica.C,308(1998)289-293	H.K. Lee		
8537	PHC3080289	semiconductor	(Pb,V)Sr(Ca,Y)Cu2O2	Pb0.5V0.5Sr2Ca0.3Y0.7Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.3	Y	0.7	Cu	2									O	Z			1998																												Pb1212																		K																																																																																																					PbO, V2O3, SrCO3, CaCO3, Y2O3, Cu2O	1	mixture-SIN(996C 4H in flowing O2)-ANN(800C,20H in air)-Q to LN2					Synthesis and superconductivity of a type of Pb-1212 phase (Pb,V)Sr2(Ca,Y)Cu2Oz	199811		Department of Physics, Kangwon National University, Chunchon 200-701, South Korea	Physica.C,308(1998)289-293	H.K. Lee		
8538	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.5K0.5O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.5	K	0.5											O	8+Z		1	1998																											3	Bi2212				5.41	5.42	30.76												K		85					85																																									A	ESR study	2670																																																				1	sol-gel method. Final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8539	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.4K0.6O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.4	K	0.6											O	8+Z		1	1998																											3	Bi2212				5.4	5.43	30.72												K		87					87																																									A	ESR study	2209																																																				1	sol-gel method. Final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8540	PHC3000033		Bi2Sr2Ca(Cu,K)2O8	Bi2Sr2Ca1Cu1.3K0.7O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.3	K	0.7											O	8+Z		1	1998																											3	Bi2212				5.42	5.41	30.69												K		93					93																																									A	ESR study	1906																																																				1	sol-gel method. Final annealing(840C,12H)					Magnetic penetration depth in K-doped Bi-2212 Bi2Sr2CaCu2-xKO8+delta: ESR study	199805		School of Physics, University of Hyderabad, P.O. Central University, Hyderabad 500 046, India	Physica.C,300(1998)33-37	Ajay Mohan Suvarna,C.S. Sunandana		
8541	PRL0813765	Ru-microdomains are included in lamellar, broad transition	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												Sr2RuO4																		K		2.7					2.7																				T	defined by resistive transition (R=0.5Rn)		3.7	1.1										HC8541		A			180	50																																																								single crystal was grown by a floating zone method with RU self flux using RU rich feed rod					Enhancement of Superconductivity of Sr2RuO4 to 3 K by Embedded Metallic Microdomains			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett.81(1998)3765	E. Ohmichi,S. Ikeda,S. Nakatsuji,S. Nishizaki,T. Ando,Y. Maeno,Y. Mori		
8542	PRL0813765	single crystal with out Ru-microdomains, sharp transition	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												Sr2RuO4																		K		1.5					1.5																				T	resistive transition		1.5	0.1										HC8542		A			660	33																																																								single crystal was grown by a floating zone method with RU self flux using RU rich feed rod					Enhancement of Superconductivity of Sr2RuO4 to 3 K by Embedded Metallic Microdomains			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett.81(1998)3765	E. Ohmichi,S. Ikeda,S. Nakatsuji,S. Nishizaki,T. Ando,Y. Maeno,Y. Mori		
8543	EPL0410207	K-content estimated by Tc,(Asada), Hc2 by tunneling follows WHH theory	(B,K)BiO3	Ba1K1Bi1O4	Ba	1	K	1	Bi	1															O	4		3	1998																												BKBO																		K				23			23																				T	defined as R/R(n)=0.9	30																									3.9	3.9	1																						mohm.cm							0.1																		craystals were geown by electrochemical crystallization					Upper Critical Field in Ba1-xKxBiO3: Magnetotransport us. Magnetotunneling			Institute of Experimental Physics, Slovak Academy of Sciences, Sk-04353 Kosice, Slovakia	Europhys.Let.41(1998)207	A.G.M. JANSEN,C. ESCRIBE-FILIPPINI,J. MARCUS,P. SAMUELY,P. SZABO,P. WYDER,T. KLEIN		
8544	PRL0800157	underdoped, P=0.11 using Tallon's eq	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1998																												Bi2212																		K				83			83																																															45		1																																															crystals were grown uning a floating zone method, oxygen content controlled by annealing in various O2 pressure					Strong Dependence of the Superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCu2O8-delta			Materials Science Division and Science and Technology Center for superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCuO8-delta	Phys.Rev.Lett.80(1998)157	D.G. Hinks,J.F. Zasadzinski,K.E. Gray,N. Miyakawa,P. Guptasama		
8545	PRL0800157	optimally doped, P=0.16 using Tallon's eq	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1998																												Bi2212																		K				95			95																																															37.5		1																																															crystals were grown uning a floating zone method, oxygen content controlled by annealing in various O2 pressure					Strong Dependence of the Superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCu2O8-delta			Materials Science Division and Science and Technology Center for superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCuO8-delta	Phys.Rev.Lett.80(1998)157	D.G. Hinks,J.F. Zasadzinski,K.E. Gray,N. Miyakawa,P. Guptasama		
8546	PRL0800157	overdoped, P=0.22 using Tallon's eq	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1998																												Bi2212																		K				82			82																																															26		1																																															crystals were grown uning a floating zone method, oxygen content controlled by annealing in various O2 pressure					Strong Dependence of the Superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCu2O8-delta			Materials Science Division and Science and Technology Center for superconducting Gap on Oxygen Doping from Tunneling Measurements on Bi2Sr2CaCuO8-delta	Phys.Rev.Lett.80(1998)157	D.G. Hinks,J.F. Zasadzinski,K.E. Gray,N. Miyakawa,P. Guptasama		
8547	PRL0770727	as grown, for XY direction gapene=7.2	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1996																												Tl2201																		K				78			78																																																5.8	4																																															self-flux method					Superconducting Gap Anisotropy vs Doping Level in High-Tc Cuprates			Code 6650, Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.Lett.77(1996)727	C. Kendziora,M. Onellion,R.J. Kelley		
8548	PRL0770727	over doping sample (excess Oxygen). isotropic gap.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1996																												Tl2201																		K				37			37																																																3.9																																																self-flux method					Superconducting Gap Anisotropy vs Doping Level in High-Tc Cuprates			Code 6650, Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.Lett.77(1996)727	C. Kendziora,M. Onellion,R.J. Kelley		
8549	PRL0770727	nearly optimum sample. Raman scattering measurements. Gap shows anisotropy.for B<2g> peak gapene=7.5, for B<1g> gapene=8.5	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1996																												Bi2212																		K				90			90																																																6.2	4																																															self-flux method					Superconducting Gap Anisotropy vs Doping Level in High-Tc Cuprates			Code 6650, Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.Lett.77(1996)727	C. Kendziora,M. Onellion,R.J. Kelley		
8550	JIC0430662	mine phase=50.28%, Cu2O=2.95%, Nd2CuO4=6069%(Nd,Sr)3Cu2O6=1.38%, SrCu2O2=3.01%, SrCuO2=30.69%	(Sr,Nd)CuO2-z	Sr0.91Nd0.09Cu1O1.98	Sr	0.91	Nd	0.09	Cu	1															O	2-Z	1.98	2	1998																												CaCuO2	P4/mmm			3.9276		3.4252												K					4.2																																																																																																		mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8551	JIC0430662	mine phase=93%, Cu2O=1.34%, CuO=2.36%, SrCu2O4=3.3%	(Sr,Nd)CuO2-z	Sr0.86Nd0.14Cu1O2	Sr	0.86	Nd	0.14	Cu	1															O	2-Z	2	2	1998																												CaCuO2	P4/mmm			3.9388		3.3851												K			40				40																																																																																																mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8552	JIC0430662	mine phase=98.54%, Cu2O=1.46%	(Sr,Nd)CuO2-z	Sr0.83Nd0.17Cu1O2	Sr	0.83	Nd	0.17	Cu	1															O	2-Z	2	2	1998																												CaCuO2	P4/mmm			3.9425		3.3862												K			35				35																																																																																																mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8553	JIC0430662	mine phase=48.26%, Sr2Cu2O4=9.18%, SrCu2O2=34.56%	(Sr,Nd)CuO2-z	Sr0.81Nd0.19Cu1O2	Sr	0.81	Nd	0.19	Cu	1															O	2-Z	2	2	1998																												CaCuO2	P4/mmm			3.9387		3.3904												K			18				18																																																																																																mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8554	JIC0430662	mine phase=83.01%, Cu2O=8.73%, (Nd,Sr)3CuO6=1.38%, unknown phase.	(Sr,Nd)CuO2-z	Sr0.87Nd0.13Cu1O1.95	Sr	0.87	Nd	0.13	Cu	1															O	2-Z	1.95	2	1998																												CaCuO2	P4/mmm			3.9337		3.407												K					4.2																																																																																																		mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8555	JIC0430662	mine phase=94.43%, Cu2O=0.56%, Sr2Cu2O4=5.01%	(Sr,Nd)CuO2-z	Sr0.84Nd0.16Cu1O2.01	Sr	0.84	Nd	0.16	Cu	1															O	2-Z	2.01		1998																												CaCuO2	P4/mmm			3.9405		3.3911												K			40				40																																																																																																mixture of Nd, Cu, Ca, Sr-oxides, CaLL-SIN(860-900C, 8H in air)-pellet-SIN(780-1100C,5-7GPa, 5-30 min in chamber)									J.Inorg.Chem.43(1998)662			
8558	EPL0410207	Im the fig, P=1:Hc2 defined by magneto tunneling, P=2:Hc2defined R/Rn=0.9 in resistive trasition, P=3: Hirr	(Ba,K)BiO3	Ba0.54K0.46Bi1O3	Ba	0.54	K	0.46	Bi	1															O	3		3	1998																												BKBO																		K		23					23																															1.7																3.9	3.9	1																																															electrochemical caystallization					Upper Critical Field in Ba1-xKxBiO3: Magnetotransport us. Magnetotunneling			Institute of Experimental Physics, Slovak Academy of Sciences, Sk-04353 Kosice, Slovakia	Europhys.Let.41(1998)207	A.G.M. JANSEN,C. ESCRIBE-FILIPPINI,J. MARCUS,P. SAMUELY,P. SZABO,P. WYDER,T. KLEIN		
8559	LTP1051237	K-content estimated from Tc-x(Phys.Rev.B41(1990)4126)	(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3		3	1996																												BKBO																		K				20			20																					defied as tunneling conductance=zero	12.3																																																																										electrochemical caystallization					Upper Critical Field of Ba1-xKxBiO3 Measured by Magnetotunneling Spectroscopy			Institute of Experimental Physics, Slovak Academy of Sciences, Sk-04353 Kosice, Slovakia	J.Low Temp.Phys.105(1996)1237	A.G.M. Jansen,C. Escribe-Filippini,J. Marcus,L. Baril,P. Samuely,P. Szabo,P. Wyder		
8560	PHC3080009	as-synthesized	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																												Cu1223				3.861		14.76												K				67			67																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8561	PHC3080009	Ar-annealed at 300C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																												Cu1223				3.863		14.77																78			78																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8562	PHC3080009	Ar-annealed at 320C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																												Cu1223				3.867		14.78																82			82																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8563	PHC3080009	Ar-annealed at 340C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																												Cu1223				3.866		14.8																100			100																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8564	PHC3080009	Ar-annealed at 360C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																											2	Cu1223				3.867														K				110			110																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8565	PHC3080009	Ar-annealed at 400C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																											2	Cu1223				3.867														K				118			118																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8566	PHC3080009	Ar-annealed at 420C	CuBa2Ca2Cu3O8	Cu4Ba2Ca2O8+Z	Cu	4	Ba	2	Ca	2															O	8+Z			1998																											2	Cu1223				3.867														K				118			118																																																																																														BaCuO2, Ca2CuO3, CuO		precursor mixture-packed into Au capsule-high pressure synthesis(1000-1200C,30min, 5GPa)-Q to RT					Optimization of the synthesis and tuning the oxygen content of the CuBa2Ca2Cu3O8+delta(Cu-1223:P) superconductor	199811		Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)	H. Suematsu,H. Yamauchi,K. Isawa,M. Karppinen,T. Ito		
8567	LTP1051359		(Hg,Re)Ba2Ca2Cu3Oz	Hg0.75Re0.25Ba2Ca2Cu3OZ	Hg	0.75	Re	0.25	Ba	2	Ca	2	Cu	3											O	Z			1996																											2	Hg1223				3.8519		15.6843												K																																																																																																							precuresor(Re-Ba-Ca-Cu-O)+HgO-mixture-pellet-sealed(quartz ampule)-SIN(670-860C,5-55H)-Q to RT					Chemical Doping and Improved Flux Pinning in Hg-based Superconductors			Department of Superconductivity, University of Tokyo, Tokyo, 113, Japan	J.Low Temp.Phys.105(1996)1359	A. Yoshikawa,J. Shimoyama,J.D. Lorgensen,K. Kishio,K. Kitazawa,O. Chmaissem		
8568	LTP1051359	as-prepared, Hirr defined as Jc=1000A/cm2	(Hg,Re)Ba2Ca2Cu3Oz	Hg0.9Re0.1Ba2Ca2Cu3OZ	Hg	0.9	Re	0.1	Ba	2	Ca	2	Cu	3											O	Z			1996																											2	Hg1223																		K				135			135																																																																																																precuresor(Re-Ba-Ca-Cu-O)+HgO-mixture-pellet-sealed(quartz ampule)-SIN(670-860C,5-55H)-Q to RT					Chemical Doping and Improved Flux Pinning in Hg-based Superconductors			Department of Superconductivity, University of Tokyo, Tokyo, 113, Japan	J.Low Temp.Phys.105(1996)1359	A. Yoshikawa,J. Shimoyama,J.D. Lorgensen,K. Kishio,K. Kitazawa,O. Chmaissem		
8569	LTP1051359	O2-annealed, Hirr defined as Jc=1000A/Cm2	(Hg,Re)Ba2Ca2Cu3Oz	Hg0.9Re0.1Ba2Ca2Cu3OZ	Hg	0.9	Re	0.1	Ba	2	Ca	2	Cu	3											O	Z			1996																											2	Hg1223																		K				128			128																																																																																																precuresor(Re-Ba-Ca-Cu-O)+HgO-mixture-pellet-sealed(quartz ampule)-SIN(670-860C,5-55H)-Q to RT					Chemical Doping and Improved Flux Pinning in Hg-based Superconductors			Department of Superconductivity, University of Tokyo, Tokyo, 113, Japan	J.Low Temp.Phys.105(1996)1359	A. Yoshikawa,J. Shimoyama,J.D. Lorgensen,K. Kishio,K. Kitazawa,O. Chmaissem		
8570	LTP1051359	O2-annealed, Hirr defined as Jc=1000A/Cm2	(Hg,Re)Ba2Ca2Cu3Oz	Hg0.8Re0.2Ba2Ca2Cu3OZ	Hg	0.8	Re	0.2	Ba	2	Ca	2	Cu	3											O	Z			1996																											2	Hg1223																		K				133			133																																																																																																precuresor(Re-Ba-Ca-Cu-O)+HgO-mixture-pellet-sealed(quartz ampule)-SIN(670-860C,5-55H)-Q to RT					Chemical Doping and Improved Flux Pinning in Hg-based Superconductors			Department of Superconductivity, University of Tokyo, Tokyo, 113, Japan	J.Low Temp.Phys.105(1996)1359	A. Yoshikawa,J. Shimoyama,J.D. Lorgensen,K. Kishio,K. Kitazawa,O. Chmaissem		
8571	PHC3090161	optimally doped, H//c-axis	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z		3	1998																												Hg1223																		K				130			130																																																																																																					Influence of Re substitution on the flux pinning in (Hg,Re)Ba2Ca2Cu3O8+delta single crystals	199812		Institute of Physics , Polish Academy of Siences, Al. Lothkow 32/46, PL 02-668 Warsaw, Poland	Physica C,309(1998)161-169	A. Wisniewski,E.M. Kopnin,H. Schwer,J. Karpinski,M. Angst,R. Molinski,R. Puzniak,R. Szymczak		
8572	PHC3090161	underdoped, H//c-axis	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z		3	1998																												Hg1223																		K				120			120																																																																																																					Influence of Re substitution on the flux pinning in (Hg,Re)Ba2Ca2Cu3O8+delta single crystals	199812		Institute of Physics , Polish Academy of Siences, Al. Lothkow 32/46, PL 02-668 Warsaw, Poland	Physica C,309(1998)161-169	A. Wisniewski,E.M. Kopnin,H. Schwer,J. Karpinski,M. Angst,R. Molinski,R. Puzniak,R. Szymczak		
8573	PHC3090161	optimally doped, H//c-axis	HgBa2Ca2Cu3O8	Hg0.77Re0.23Ba2Ca2Cu3O8+Z	Hg	0.77	Re	0.23	Ba	2	Ca	2	Cu	3											O	8+Z		3	1998																												Hg1223																		K				130			130																																																																																																					Influence of Re substitution on the flux pinning in (Hg,Re)Ba2Ca2Cu3O8+delta single crystals	199812		Institute of Physics , Polish Academy of Siences, Al. Lothkow 32/46, PL 02-668 Warsaw, Poland	Physica C,309(1998)161-169	A. Wisniewski,E.M. Kopnin,H. Schwer,J. Karpinski,M. Angst,R. Molinski,R. Puzniak,R. Szymczak		
8574	PHC3090208		TlSr2CuO5	Tl1Sr2Cu1O5	Tl	1	Sr	2	Cu	1															O	5			1998																												Tl1201																		K					15																																																																																																		mixture-pellet-SIN(950C,10H)-cool to 650C-keep(650C,6H)					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8575	PHC3090208		Tl(Sr,Cr)2CuO5	Tl1Sr1.9Cr0.1Cu1O5	Tl	1	Sr	1.9	Cr	0.1	Cu	1													O	5			1998																												Tl1201																		K	30		45				37.5																																																																																																mixture-pellet-SIN(950C,10H)-cool to 650C-keep(650C,6H)					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8576	PHC3090208		Tl(Sr,Cr)2CuO5	Tl1Sr1.8Cr0.2Cu1O5	Tl	1	Sr	1.8	Cr	0.2	Cu	1													O	5			1998																												Tl1201																		K	43						43																																																																																																mixture-pellet-SIN(950C,10H)-cool to 650C-keep(650C,6H)					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8577	PHC3090208		Tl(Sr,Cr)2CuO5	Tl1Sr1.7Cr0.3Cu1O5	Tl	1	Sr	1.7	Cr	0.3	Cu	1													O	5			1998																												Tl1201																		K	47						47																																																																																																mixture-pellet-SIN(950C,10H)-cool to 650C-keep(650C,6H)					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8578	PHC3090208		Tl(Sr,Cr)2CuO5	Tl1Sr1.6Cr0.4Cu1O5	Tl	1	Sr	1.6	Cr	0.4	Cu	1													O	5			1998																												Tl1201																		K	48						48																																																																																																mixture-pellet-SIN(950C,10H)-cool to 650C-keep(650C,6H)					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8579	PHC3090208	nominal(Tl1201),XRD shows Tl2201 phase, posltion of Cr is not determined		Tl1Sr1.7Cr0.3Cu1O5	Tl	1	Sr	1.7	Cr	0.3	Cu	1													O	5			1998																												Tl2201				3.7598		23.4565												K				76			76																																																																																																sintered at 980C					New Tl 2201(Tl,Cr)2Sr2CuO6+ -delta phase material	199812		Midwest Superconductivity, 1315 Wakarusa Drive, Lawrence, KS 66049, USA	Physica C,309(1998)208-214	B.R. Xu,K.W. Wong,Y. Xin		
8580	PHC3090105	Jc is plotted, P=1 for H=5KOe and P=2 for H=40KOe	HxBi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1998																											3	Bi2212				5.37	5.4	30.75												K				87.5			87.5																																																																																																single crystal-ANN(700C,3days,in 90%Ar+10% O2)-hydrogenated electrohemically(KOH solution)					Superconducting properties of hydrogenated Bi2Sr2CaCu2O8+delta single crystals	199812		Institut fur Experimentalphysik IV, Ruhr-Universitat, 44780. Bochum, Germany	Physica C,309(1998)105-112	K. westerholt,N.M. Suleimanov,R. Noetzel,R.G. Mustafin,Th. Meier		
8581	PHC3090105	mayb phase separation(H-rich and H-poor), H:intersticial site. P=1 for H=5KOe and P=2 for H=40KOe	HxBi2Sr2CaCu2Oz	H1Bi2Sr2Ca1Cu2OZ	H	1	Bi	2	Sr	2	Ca	1	Cu	2											O	Z		3	1998																											3	Bi2212				5.4	5.46	30.75																87.5			87.5																																																																																																single crystal-ANN(700C,3days,in 90%Ar+10% O2)-hydrogenated electrohemically(KOH solution)					Superconducting properties of hydrogenated Bi2Sr2CaCu2O8+delta single crystals	199812		Institut fur Experimentalphysik IV, Ruhr-Universitat, 44780. Bochum, Germany	Physica C,309(1998)105-112	K. westerholt,N.M. Suleimanov,R. Noetzel,R.G. Mustafin,Th. Meier		
8582	PHC3090049	as-grown	(Tl,Pb)(Sr,Ba)2CaCu2Oz	Tl0.6Pb0.4Sr1.7Ba0.3Ca1Cu2OZ	Tl	0.6	Pb	0.4	Sr	1.7	Ba	0.3	Ca	1	Cu	2									O	Z		3	1998																												Tl1212						12.0824																89			89																																																																																																precursor+Tl2O3-heat(960C,0.5H in alumina crucible-cool to 720C(15C/H)-cool to RT (50C/H)					Magnetization studies of Tl0.6Pb0.4Sr1.7Ba0.3CaCu2Oy single crystals	199812		Department of Physics and Astronomy, University of Southampton, Southampton, SO17 IBJ, UK	Physica C,309(1998)49-55	M.T. Weller,P.A.J. de Groot,S. Kokkaliaris,S.N. Gordeev,X.M. yang		
8583	PHC3090049	after annealing(500bar N2,500C,2H), then cool to RT(60C/H)	(Tl,Pb)(Sr,Ba)2CaCu2Oz	Tl0.6Pb0.4Sr1.7Ba0.3Ca1Cu2OZ	Tl	0.6	Pb	0.4	Sr	1.7	Ba	0.3	Ca	1	Cu	2									O	Z		3	1998																												Tl1212						12.178																89			89																																																																																																precursor+Tl2O3-heat(960C,0.5H in alumina crucible-cool to 720C(15C/H)-cool to RT (50C/H)					Magnetization studies of Tl0.6Pb0.4Sr1.7Ba0.3CaCu2Oy single crystals	199812		Department of Physics and Astronomy, University of Southampton, Southampton, SO17 IBJ, UK	Physica C,309(1998)49-55	M.T. Weller,P.A.J. de Groot,S. Kokkaliaris,S.N. Gordeev,X.M. yang		
8584	PHC3090025		YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1998																											3	Y123				3.827	3.8876	11.677																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8585	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y0.95Ca0.05Ba2Cu3OZ	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.826	3.8853	11.679																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8586	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3OZ	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.8301	3.8843	11.674																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8587	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y0.85Ca0.15Ba2Cu3OZ	Y	0.85	Ca	0.15	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.8318	3.8766	11.684																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8588	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y1.8Ca0.2Ba2Cu3OZ	Y	1.8	Ca	0.2	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.8307	3.878	11.693																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8589	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y0.65Ca0.35Ba2Cu3OZ	Y	0.65	Ca	0.35	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.8358	3.8761	11.692																																																																																																																			standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8590	PHC3090025		(Y,Ca)Ba2Cu3Oz	Y0.5Ca0.5Ba2Cu3OZ	Y	0.5	Ca	0.5	Ba	2	Cu	3													O	Z		1	1998																											3	Y123				3.824	3.8782	11.704														77					77																																																																																																standard solid state reaction method					Microstrutural variations of YBa2Cu3Oy doped with Ca at high doping level	199812		National Laboratory of State Microstructures, Department of Pysics, Institute of Solid State Physics, and Center for Advanced studies in Science and Technology of Microstructures, University, Nanjing 210093, China	Physica C,309(1998)25-32	J. Lin,J.S. Liu,S.S. Jiang,W.M. Chen,X. Jin,X.S. Wu		
8591	PRL0824918		YBa2Cu3O7	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	7-Z	6.94		1999																												Y123																						93			93																																																																																																crystals were grown by the self-flux method in Y or Ca stabilized ZrO2 crucibles					Superconducting Gap deltac, the Pseudogap deltap, and Pair Fluctuations above Tc in Overdoped Y1-xCaxBa2Cu3O7-delta from Femtosecond time-Domain Spectroscopy			Jozef Stefan Institute, Jamova 39, 1001 Ljubljana, Slovenia	Phys.Rev.Lett.82(1999)4918	B. Podobnik,D. Mihailovic,D. Mihalovic,J. Demsar,Th.  Wolf,Th. Wolf,V.V. Kabanov,V.V. Kobanov		
8592	PRL0824918		(Y,Ca)Ba2Cu3O7	Y0.984Ca0.016Ba2Cu3O6.986	Y	0.984	Ca	0.016	Ba	2	Cu	3													O	7-Z	6.986		1999																												Y123																						89.5			89.5																																																																																																crystals were grown by the self-flux method in Y or Ca stabilized ZrO2 crucibles					Superconducting Gap deltac, the Pseudogap deltap, and Pair Fluctuations above Tc in Overdoped Y1-xCaxBa2Cu3O7-delta from Femtosecond time-Domain Spectroscopy			Jozef Stefan Institute, Jamova 39, 1001 Ljubljana, Slovenia	Phys.Rev.Lett.82(1999)4918	B. Podobnik,D. Mihailovic,D. Mihalovic,J. Demsar,Th.  Wolf,Th. Wolf,V.V. Kabanov,V.V. Kobanov		
8593	PRL0824918		(Y,Ca)Ba2Cu3O7	Y0.899Ca0.101Ba2Cu3O6.943	Y	0.899	Ca	0.101	Ba	2	Cu	3													O	7-Z	6.943		1999																												Y123																						83			83																																																																																																crystals were grown by the self-flux method in Y or Ca stabilized ZrO2 crucibles					Superconducting Gap deltac, the Pseudogap deltap, and Pair Fluctuations above Tc in Overdoped Y1-xCaxBa2Cu3O7-delta from Femtosecond time-Domain Spectroscopy			Jozef Stefan Institute, Jamova 39, 1001 Ljubljana, Slovenia	Phys.Rev.Lett.82(1999)4918	B. Podobnik,D. Mihailovic,D. Mihalovic,J. Demsar,Th.  Wolf,Th. Wolf,V.V. Kabanov,V.V. Kobanov		
8594	PRL0824918		(Y,Ca)Ba2Cu3O7	Y0.868Ca0.132Ba2Cu3O6.928	Y	0.868	Ca	0.132	Ba	2	Cu	3													O	7-Z	6.928		1999																												Y123																						75			75																																																																																																crystals were grown by the self-flux method in Y or Ca stabilized ZrO2 crucibles					Superconducting Gap deltac, the Pseudogap deltap, and Pair Fluctuations above Tc in Overdoped Y1-xCaxBa2Cu3O7-delta from Femtosecond time-Domain Spectroscopy			Jozef Stefan Institute, Jamova 39, 1001 Ljubljana, Slovenia	Phys.Rev.Lett.82(1999)4918	B. Podobnik,D. Mihailovic,D. Mihalovic,J. Demsar,Th.  Wolf,Th. Wolf,V.V. Kabanov,V.V. Kobanov		
8595	PRL0824930	electrochemical crystallizatio		Ba1K1Bi1O3	Ba	1	K	1	Bi	1															O	3			1999																												BKBO																						23.3			23.3																						16																45				reversible M-H region	3600																																																					K-content was estimated from Tc-x(by Asada)					Small Angle Neutron Scattering and Magnetization Measurements in the Cubic (K, Ba)BiO3 Superconductor			Laboratoire d'Etudes des Propriete's Electroniques des Solides, Centre National de la Recherche Scientifique, BP 166, 38042 Grenoble Cedex 9, France	Phys.Rev.Lett.82(1999)4930	I. Joumard,J. Marcus,R. Cubitt,T. Klein		
8596	SSC1060673	compositions of Cs,Sr are not described	(Cs,Sr)(Bi,Pb)O3	Cs1Sr1Bi0.25Pb0.75O3	Cs	1	Sr	1	Bi	0.25	Pb	0.75													O	3		2	1998																												ABO3																						7.5			7.5																																																																																																polycrystal prepared by decomposing stoichiometric mixture of 0.1 M aqueous constituent metal-EDTA solutions					OBSERVATION OF SUPERCONDUCTIVITY IN THE Cs-Sr-Bi-Pb-O SYSTEM			Metal Manufactures Ltd., High Temperature Superconductor Facility, Australian Technology Park, Eveleigh NSW 1430, Australia	Solid State Commun.106(1998)673	T.P. Beales		
8597	SCI2801589	I-intercalation, interlayer distance=15.7	I-Bi2(Sr,Ca)2CaCu2Oz	I1Bi2Sr1.5Ca1.5Cu2OZ	I	1	Bi	2	Sr	1.5	Ca	1.5	Cu	2											O	Z			1998																												Bi2212																						63.2			63.2																																																																																																intercalation technique					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8598	SCI2801589	HgI2-intercalation, interlayer distance=19.6	HgI2-Bi2(Sr,Ca)2CaCu2Oz	Hg1I2Bi2Sr1.5Ca1.5Cu2OZ	Hg	1	I	2	Bi	2	Sr	1.5	Ca	1.5	Cu	2									O	Z			1998																												Bi2212																						68			68																																																																																																intercalation technique					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8599	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 26.1A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C1H24Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	1	H	24	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						81			81																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8600	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 27.1A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C2H26Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	2	H	26	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						82			82																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8601	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 28.8A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C4H210Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	4	H	210	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						82			82																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8602	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 33.2A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C6H214Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	6	H	214	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						81.2			81.2																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8603	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 38.0A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C8H218Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	8	H	218	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						82			82																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8604	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 42.9A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C10H224Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	10	H	224	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						81.2			81.2																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8605	SCI2801589	intercalation-[(Py-CnH2n+1)2HgI4], bisalkylpyridinium tetraiodomercurate. Interlayer distance=A 48.1A	[(Py-CnH2n+1)2HgI4]Bi2(Sr,Ca)2CaCu2Oz	Py2C12H226Hg1I4Bi2Sr1.5Ca1.5Cu2OZ	Py	2	C	12	H	226	Hg	1	I	4	Bi	2	Sr	1.5	Ca	1.5	Cu	2			O	Z			1998																												Bi2212																						82.2			82.2																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8606	SCI2801589	intercalation-(Py-CnH2n+1)2HgI4, bisalkylpyridinium tetraiodomercurate. Interlayer distance= 23.08A	[(Py-CnH2n+1)2HgI4]0.35Bi2(Sr,La)2CuOz	Py2C2H24Hg1I4Bi2Sr1.6La0.4Cu1OZ	Py	2	C	2	H	24	Hg	1	I	4	Bi	2	Sr	1.6	La	0.4	Cu	1			O	Z			1998																												Bi2201																						28.1			28.1																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8607	SCI2801589	intercalation-(Py-CnH2n+1)2HgI4, bisalkylpyridinium tetraiodomercurate. Interlayer distance= 25.27 A	[(Py-CnH2n+1)2HgI4]0.35Bi2(Sr,La)2CuOz	Py2C8H210Hg1I4Bi2Sr1.6La0.4Cu1OZ	Py	2	C	8	H	210	Hg	1	I	4	Bi	2	Sr	1.6	La	0.4	Cu	1			O	Z			1998																												Bi2201																						27.6			27.6																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8608	SCI2801589	intercalation-(Py-CnH2n+1)2HgI4, bisalkylpyridinium tetraiodomercurate. Interlayer distance= 34.07A	[(Py-CnH2n+1)2HgI4]0.35Bi2(Sr,La)2CuOz	Py2C16H218Hg1I4Bi2Sr1.6La0.4Cu1OZ	Py	2	C	16	H	218	Hg	1	I	4	Bi	2	Sr	1.6	La	0.4	Cu	1			O	Z			1998																												Bi2201																						28.1			28.1																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8609	SCI2801589	intercalation-(Py-CnH2n+1)2HgI4, bisalkylpyridinium tetraiodomercurate. Interlayer distance= 43.08 A	[(Py-CnH2n+1)2HgI4]0.35Bi2(Sr,La)2CuOz	Py2C24H226Hg1I4Bi2Sr1.6La0.4Cu1OZ	Py	2	C	24	H	226	Hg	1	I	4	Bi	2	Sr	1.6	La	0.4	Cu	1			O	Z			1998																												Bi2201																						28			28																																																																																																HgI2-intercalated Bi-2212(m-1)-(solvent-mediated) reaction between HgI2 tntercalates and alkylpyridinium iodide					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8610	SCI2801589	I-intercalation. interlayer distance=15.8	IBi2(Sr,La)2CuOz	I1Bi2Sr1.6La0.4Cu1OZ	I	1	Bi	2	Sr	1.6	La	0.4	Cu	1											O	Z			1998																												Bi2201																						22.1			22.1																																																																																																intercalation technique					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8611	SCI2801589	HgI2-intercalation. interlayer distance=19.3	HgI2Bi2(Sr,La)2CuOz	Hg1I2Bi2Sr1.6La0.4Cu1OZ	Hg	1	I	2	Bi	2	Sr	1.6	La	0.4	Cu	1									O	Z			1998																												Bi2201																						22.1			22.1																																																																																																intercalation technique					High-Tc Superconductors in the Two-Dimensional Limit: [(Py-CnH2n+1)2Hgl4]-Bi2Sr2Cam-1CuOy(m=1 and 2)	199806		Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Science.280(1998)1589	Gyeong-Su Park,Jin-Ho Choy,Jin-Ho choy,Soon-Jae Kwon		
8612	PLA2400253		TlBa2Ca2Cu3Oz	Tl2Ba2Ca2Cu3OZ	Tl	2	Ba	2	Ca	2	Cu	3													O	Z		4	1998																												Tl2223																			118		127				122.5																																																																																																precursor film(Ba2Ca2CdxCu3Oz)on MgO-(film in Pt box and Tl2O3,precursor bulk)-sealed quartz-ANN(890C)					Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	199804		Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	Phys.Lett.A,240(1998)253	H.K. Singh,O.N. Srivastava		
8613	PLA2400253		TlBa2CdxCu3Oz	Tl2Ba2Ca2Cd0.1Cu3OZ	Tl	2	Ba	2	Ca	2	Cd	0.1	Cu	3											O	Z		4	1998																												Tl2223																			120		127				123.5																																																																																																precursor film(Ba2Ca2CdxCu3Oz)on MgO-(film in Pt box and Tl2O3,precursor bulk)-sealed quartz-ANN(890C)					Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	199804		Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	Phys.Lett.A,240(1998)253	H.K. Singh,O.N. Srivastava		
8614	PLA2400253		TlBa2CdxCu3Oz	Tl2Ba2Ca2Cd0.2Cu3OZ	Tl	2	Ba	2	Ca	2	Cd	0.2	Cu	3											O	Z		4	1998																												Tl2223						35.715													124		127				125.5																																																			112000																																													precursor film(Ba2Ca2CdxCu3Oz)on MgO-(film in Pt box and Tl2O3,precursor bulk)-sealed quartz-ANN(890C)					Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	199804		Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	Phys.Lett.A,240(1998)253	H.K. Singh,O.N. Srivastava		
8615	PLA2400253		TlBa2CdxCu3Oz	Tl2Ba2Ca2Cd0.3Cu3OZ	Tl	2	Ba	2	Ca	2	Cd	0.3	Cu	3											O	Z		4	1998																												Tl2223																			121		127				124																																																																																																precursor film(Ba2Ca2CdxCu3Oz)on MgO-(film in Pt box and Tl2O3,precursor bulk)-sealed quartz-ANN(890C)					Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	199804		Cadmium induced growth of 2223 phase and Tc enhancement in TBCCO high Tc thin films	Phys.Lett.A,240(1998)253	H.K. Singh,O.N. Srivastava		
8616	PLA2450158	S/C is shown in ESR. Granular superconductor structure model is shown	(Gd,Ce)2Sr2Cu2TiO10	Gd1.4Ce0.6Sr2Cu2Ti1O10	Gd	1.4	Ce	0.6	Sr	2	Cu	2	Ti	1											O	10		1	1998																																																11				3	11																																																																																																same as PhysicaC 176(1991)19. Details are not shown in the paper					Observation of predicted superconductivity in Gd1.4Ce0.6Sr2Cu2TiOx with x=10	199808		Department of Physics,University of Notre, Dame, Notre Dame, IN 46556, USA	Phys.Lett.A,245(1998)158	Dan Goldschmidt,David B. Pulling,Howard A Blackstead,John D. Dow		
8617	PHC3200009	gap=19-25 meV	Tl2Ba2CuO3	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	1999																											2	Tl2201																						86			86																																																	1																																															crystal was grown by flux method. Cleared surface is used for tunneling					Tunneling spectroscopy of Tl2Ba2CuO6	199907		Science and Technology Center for Superconductivity and Materials Science Division, Argonne National Laboratory, Argonne, IL 60439, USA	Physia C,320(1999)9-20	Dave G. Hinks,John F. Zasadzinski,K.E. Gray,Lutfi Ozyuzer,Ting-Wei Li,Zikri Yusof		
8618	PHC3200087		NaBa2Cu3Oz	Nd1Ba2Cu3O6.98	Nd	1	Ba	2	Cu	3															O	Z	6.98	1	1999																											3	Y123				3.8594	3.9163	11.7276													89	91	93	91			91																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8619	PHC3200087		Nd(Ba, La)2Cu3Oz	Nd1Ba1.9La0.1O6.86	Nd	1	Ba	1.9	La	0.1															O	Z	6.86	1	1999																											3	Y123				3.8663	3.9161	11.7414													79	83.5	88	84			83.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8620	PHC3200087		Nd(Ba, La)2Cu3Oz	Nd1Ba1.8La0.2O6.81	Nd	1	Ba	1.8	La	0.2															O	Z	6.81	1	1999																											3	Y123				3.8644	3.913	11.7422													72	78.5	85	79			78.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8621	PHC3200087		Nd(Ba, La)2Cu3Oz	Nd1Ba1.7La0.3O6.77	Nd	1	Ba	1.7	La	0.3															O	Z	6.77	1	1999																											3	Y123				3.8896	3.8943	11.7012													48	57.5	66	57			57.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8622	PHC3200087		Nd(Ba, La)2Cu3Oz	Nd1Ba1.65La0.35O6.69	Nd	1	Ba	1.65	La	0.35															O	Z	6.69	1	1999																											3	Y123				3.8868	3.8919	11.6958													24	36.5	49	36			36.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8623	PHC3200087		Nd(Ba, La)2Cu3Oz	Nd1Ba1.6La0.4O6.68	Nd	1	Ba	1.6	La	0.4															O	Z	6.68	1	1999																											3	Y123				3.8914	3.8941	11.6698															37				37																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8624	PHC3200087	not S/C	Nd(Ba, La)2Cu3Oz	Nd1Ba1.5La0.5O6.64	Nd	1	Ba	1.5	La	0.5															O	Z	6.64	1	1999																											3	Y123				3.8871	3.8908	11.6575																																																																																																																	Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8625	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.9Ca0.1Ba0.6La0.4Cu3O6.7	Nd	0.9	Ca	0.1	Ba	0.6	La	0.4	Cu	3											O	Z	6.7	1	1999																											3	Y123				3.8769	3.9222	11.6601													46	54.5	63	52			54.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8626	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.8Ca0.2Ba0.6La0.4Cu3O6.72	Nd	0.8	Ca	0.2	Ba	0.6	La	0.4	Cu	3											O	Z	6.72	1	1999																											3	Y123				3.8661	3.9131	11.6655													68	72	76	71			72																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8627	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.7Ca0.3Ba0.6La0.4Cu3O6.79	Nd	0.7	Ca	0.3	Ba	0.6	La	0.4	Cu	3											O	Z	6.79	1	1999																											3	Y123				3.8637	3.9116	11.7096													71	75	79	76			75																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8628	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.6Ca0.4Ba0.6La0.4Cu3O6.83	Nd	0.6	Ca	0.4	Ba	0.6	La	0.4	Cu	3											O	Z	6.83	1	1999																											3	Y123				3.8611	3.9226	11.6983													78	84	90	83			84																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8629	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.5Ca0.5Ba0.6La0.4Cu3O6.77	Nd	0.5	Ca	0.5	Ba	0.6	La	0.4	Cu	3											O	Z	6.77	1	1999																											3	Y123				3.8641	3.9207	11.6995													75	80.5	86	80			80.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8630	PHC3200087		Nd(Ba, Ca)(Ba,La)2Cu3Oz	Nd0.4Ca0.6Ba0.6La0.4Cu3O6.71	Nd	0.4	Ca	0.6	Ba	0.6	La	0.4	Cu	3											O	Z	6.71	1	1999																											3	Y123				3.8791	3.9307	11.6817													74	78.5	83	78			78.5																																																																																														Nd2O3, BaCO3, CuO, La2O3, 	1	SIN(930C, in air)-ANN(500C,24H in O2 flow)-RT(1C/min)					Influence of hole-filling by La and hole-doping by Ca on the superconductivity of NdBa2Cu3O7-delta	199907		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,320(1999)87-95	Amish G. Joshi,D.G. Kuberkar,R.G. Kulkarni		
8631	PHC3200173		HoBa2Cu3O7-z	Ho1Ba2Cu3O7-Z	Ho	1	Ba	2	Cu	3															O	7-Z			1999																												Y123																				90.7				1.5	90.7																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8632	PHC3200173		(Ho,Pr)Ba2Cu3Oz	Ho0.95Pr0.05Ba2Cu3O7-Z	Ho	0.95	Pr	0.05	Ba	2	Cu	3													O	7-Z			1999																												Y123																				60.5					60.5																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8633	PHC3200173		(Ho,Pr)Ba2Cu3Oz	Ho0.9Pr0.1Ba2Cu3O7-Z	Ho	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z			1999																												Y123																				86.7					86.7																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8634	PHC3200173		(Ho,Pr)Ba2Cu3Oz	Ho0.85Pr0.15Ba2Cu3O7-Z	Ho	0.85	Pr	0.15	Ba	2	Cu	3													O	7-Z			1999																												Y123																				81.2				2	81.2																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8635	PHC3200173		(Ho,Pr)Ba2Cu3Oz	Ho0.8Pr0.2Ba2Cu3O7-Z	Ho	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z			1999																												Y123																				75.6					75.6																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8636	PHC3200173		(Ho,Pr)Ba2Cu3Oz	Ho0.75Pr0.25Ba2Cu3O7-Z	Ho	0.75	Pr	0.25	Ba	2	Cu	3													O	7-Z			1999																												Y123																				67.5					67.5																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8637	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.7Pr0.3Ba2Cu3O7-Z	Ho	0.7	Pr	0.3	Ba	2	Cu	3													O	7-Z			1999																												Y123																				60				4.4	60																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8638	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.65Pr0.35Ba2Cu3O7-Z	Ho	0.65	Pr	0.35	Ba	2	Cu	3													O	7-Z			1999																												Y123																				53.4					53.4																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8639	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.6Pr0.4Ba2Cu3O7-Z	Ho	0.6	Pr	0.4	Ba	2	Cu	3													O	7-Z			1999																												Y123																				44					44																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8640	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.55Pr0.45Ba2Cu3O7-Z	Ho	0.55	Pr	0.45	Ba	2	Cu	3													O	7-Z			1999																												Y123																				39.8				5.6	39.8																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8641	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.5Pr0.5Ba2Cu3O7-Z	Ho	0.5	Pr	0.5	Ba	2	Cu	3													O	7-Z			1999																												Y123																				28.3					28.3																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8642	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.48Pr0.52Ba2Cu3O7-Z	Ho	0.48	Pr	0.52	Ba	2	Cu	3													O	7-Z			1999																												Y123																				25.8					25.8																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8643	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.45Pr0.55Ba2Cu3O7-Z	Ho	0.45	Pr	0.55	Ba	2	Cu	3													O	7-Z			1999																												Y123																				20.7			10.3		20.7																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8644	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.43Pr0.57Ba2Cu3O7-Z	Ho	0.43	Pr	0.57	Ba	2	Cu	3													O	7-Z			1999																												Y123																				9.51			13.5		9.51																																																																																															1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8645	PHC3200173		(Ho,Pr)Ba2Cu3O7	Ho0.4Pr0.6Ba2Cu3O7-Z	Ho	0.4	Pr	0.6	Ba	2	Cu	3													O	7-Z			1999																												Y123																																																																																																																								1	ANN(450C, in O2 flow)					Trapping mechanism of superconductivity suppression induced by Pr substitution in the Ho1-xPrxBa2Cu3O7-delta system	199907		Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C,320(1999)173-182	Z. Tomkowicz		
8646	PHC3200206		(Y,Ca)BaCu3Oz	Y0.8Ca0.2Ba2Cu3OZ	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	Z		1	1999																											3	Y123				3.879	3.8295	11.6819													75.1						75.1																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8647	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.95La0.05Cu3OZ	Y	0.8	Ca	0.2	Ba	0.95	La	0.05	Cu	3											O	Z		1	1999																											3	Y123				3.8776	3.8285	11.6846													77.5						77.5																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8648	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.9La0.1Cu3OZ	Y	0.8	Ca	0.2	Ba	0.9	La	0.1	Cu	3											O	Z		1	1999																											3	Y123				3.8769	3.8268	11.6782													80.7						80.7																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8650	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.85La0.15Cu3OZ	Y	0.8	Ca	0.2	Ba	0.85	La	0.15	Cu	3											O	Z		1	1999																											3	Y123				3.8754	3.8246	11.6708													81.4						81.4																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8651	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.8La0.2Cu3OZ	Y	0.8	Ca	0.2	Ba	0.8	La	0.2	Cu	3											O	Z		1	1999																											3	Y123				3.8731	3.8249	11.6602													82.1						82.1																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8652	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.75La0.25Cu3OZ	Y	0.8	Ca	0.2	Ba	0.75	La	0.25	Cu	3											O	Z		1	1999																											3	Y123				3.8679	3.8244	11.6447													75.1						75.1																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8653	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.7La0.3Cu3OZ	Y	0.8	Ca	0.2	Ba	0.7	La	0.3	Cu	3											O	Z		1	1999																											3	Y123				3.8649	3.8285	11.6355													74.1						74.1																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8654	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.6La0.4Cu3OZ	Y	0.8	Ca	0.2	Ba	0.6	La	0.4	Cu	3											O	Z		1	1999																											3	Y123				3.8533	3.8426	11.6091													62.3						62.3																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8655	PHC3200206		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba0.5La0.5Cu3OZ	Y	0.8	Ca	0.2	Ba	0.5	La	0.5	Cu	3											O	Z		1	1999																											3	Y123				3.8509	3.846	11.6587													59.8						59.8																																																																																														Y2O3, CaO, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,20H in air)-pellet-SIN(950C,20H in air)-ANN(350C,25H in O2 flow)-RT					Effect on sturucture and superconductivity for La and Ca codoping in YBa2Cu3Oy cuprates	199907		National Laboratory of Solid State Microstructures, Department of Physics, Institute of Solid State Physics, and Center for Advanced	Physica C,320(1999)206-212	F.Z. Wang,J. Gao,J.S. Liu,S.S. Jiang,X.S. Wu		
8656	PHC3200245		YBa2(Cu)3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1999																												Y123																						90.5			90.5																																																																																																					Suppression of antiferromagnetic spin fluctuation in Zn-substituted YBa2Cu3O7	199907		Department of Physics, Kpnkuk University, 93-1 Mo-Jin-Dong Kwang-Jin-Ku, Seoul 143-701, South Korea	Physica C,320(1999)245-252	B.J. Mean,D.H. Kim,H.B. Kim,H.S. Lee,Joung-Sook Cho,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
8657	PHC3200245		YBa2(Cu,Zn)3O7	Y1Cu2.99Zn0.01O7	Y	1	Cu	2.99	Zn	0.01															O	7		1	1999																												Y123																						86.6			86.6																																																																																																					Suppression of antiferromagnetic spin fluctuation in Zn-substituted YBa2Cu3O7	199907		Department of Physics, Kpnkuk University, 93-1 Mo-Jin-Dong Kwang-Jin-Ku, Seoul 143-701, South Korea	Physica C,320(1999)245-252	B.J. Mean,D.H. Kim,H.B. Kim,H.S. Lee,Joung-Sook Cho,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
8658	PHC3200245		YBa2(Cu,Zn)3O7	Y1Cu2.98Zn0.02O7	Y	1	Cu	2.98	Zn	0.02															O	7		1	1999																												Y123																						84.5			84.5																																																																																																					Suppression of antiferromagnetic spin fluctuation in Zn-substituted YBa2Cu3O7	199907		Department of Physics, Kpnkuk University, 93-1 Mo-Jin-Dong Kwang-Jin-Ku, Seoul 143-701, South Korea	Physica C,320(1999)245-252	B.J. Mean,D.H. Kim,H.B. Kim,H.S. Lee,Joung-Sook Cho,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
8659	PHC3200245		YBa2(Cu,Zn)3O7	Y1Cu2.97Zn0.03O7	Y	1	Cu	2.97	Zn	0.03															O	7		1	1999																												Y123																						81.5			81.5																																																																																																					Suppression of antiferromagnetic spin fluctuation in Zn-substituted YBa2Cu3O7	199907		Department of Physics, Kpnkuk University, 93-1 Mo-Jin-Dong Kwang-Jin-Ku, Seoul 143-701, South Korea	Physica C,320(1999)245-252	B.J. Mean,D.H. Kim,H.B. Kim,H.S. Lee,Joung-Sook Cho,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
8660	PHC3200277	as-synthesized	(Hg,Tl)2Ba2Ca2Cu3Oz	Hg1.2Tl0.8Ba2Ca2Cu3OZ	Hg	1.2	Tl	0.8	Ba	2	Ca	2	Cu	3											O	Z			1999																												Hg2223																						52			52																																		HIR8660																																				TP8660																										high pressure synthesis(6GPa, 1373K)					Thermoelectric power and irreversibility field of (Hg,Tl)2Ba2Can-1CunOy (n=2-5) superconductors	199907		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C,320(1999)277-284	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki		
8661	PHC3200277	as-synthesized	(Hg,Tl)2Ba2Ca3Cu4Oz	Hg1.2Tl0.8Ba2Ca3Cu4OZ	Hg	1.2	Tl	0.8	Ba	2	Ca	3	Cu	4											O	Z			1999																												Hg2234																						110			110																																																																						TP8661																										high pressure synthesis(6GPa, 1373K)					Thermoelectric power and irreversibility field of (Hg,Tl)2Ba2Can-1CunOy (n=2-5) superconductors	199907		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C,320(1999)277-284	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki		
8662	PHC3200277	as-synthesized	(Hg,Tl)2Ba2CaCu24Oz	Hg1Tl1Ba2Ca1Cu2OZ	Hg	1	Tl	1	Ba	2	Ca	1	Cu	2											O	Z			1999																												Hg2212																						35			35																																																																						TP8662																										high pressure synthesis(6GPa, 1273K)					Thermoelectric power and irreversibility field of (Hg,Tl)2Ba2Can-1CunOy (n=2-5) superconductors	199907		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C,320(1999)277-284	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki		
8663	PHC3200277	as-synthesized	(Hg,Tl)2Ba2Ca4Cu5Oz	Hg1Tl1Ba2Ca4Cu5OZ	Hg	1	Tl	1	Ba	2	Ca	4	Cu	5											O	Z			1999																												Hg2245																						90			90																																																																						TP8663																										high pressure synthesis(6GPa, 1273K)					Thermoelectric power and irreversibility field of (Hg,Tl)2Ba2Can-1CunOy (n=2-5) superconductors	199907		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C,320(1999)277-284	K. Tanabe,S. Adachi,T. Tamura,T. Tatsuki		
8664	PHC3190181		La3(La,Ba)Ba3Cu3Oz	La3.5Ba3.5Cu7O16.415	La	3.5	Ba	3.5	Cu	7															O	Z	16.415	1	1999																											2	3137				3.91		11.684																0			0																																																																																														La2O3, Y2O3, BaCO3, CuO, CaCO3	1	CAL(950C,24H)-pellet-SIN(940-960C,12H in N2+O2 gas)-ANN(500C,12H,in O2 flow)-RT(1C/min)					Structural studies of the superconducting La3.5-x-yYyCa2xBa3.5-xCu7Oz system	199906		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,319(1999)181-188	A. Sequeira,H. Rajagopal,M.V. Subbarao,R.G. Kulkarni		
8665	PHC3190181		La3(La,Y,Ca,Ba)ba3Cu7Oz	La3.1Y0.2Ca0.4Ba3.3Cu7O16.529	La	3.1	Y	0.2	Ca	0.4	Ba	3.3	Cu	7											O	Z	16.529	1	1999																											2	3137				3.894		11.659																55			55																																																																																														La2O3, Y2O3, BaCO3, CuO, CaCO3	1	CAL(950C,24H)-pellet-SIN(940-960C,12H in N2+O2 gas)-ANN(500C,12H,in O2 flow)-RT(1C/min)					Structural studies of the superconducting La3.5-x-yYyCa2xBa3.5-xCu7Oz system	199906		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,319(1999)181-188	A. Sequeira,H. Rajagopal,M.V. Subbarao,R.G. Kulkarni		
8666	PHC3190181		La3(La,Y,Ca,Ba)ba3Cu7Oz	La5.8Y0.4Ca0.8Ba3.1Cu7O16.548	La	5.8	Y	0.4	Ca	0.8	Ba	3.1	Cu	7											O	Z	16.548	1	1999																											2	3137				3.873		11.623																74			74																																																																																														La2O3, Y2O3, BaCO3, CuO, CaCO3	1	CAL(950C,24H)-pellet-SIN(940-960C,12H in N2+O2 gas)-ANN(500C,12H,in O2 flow)-RT(1C/min)					Structural studies of the superconducting La3.5-x-yYyCa2xBa3.5-xCu7Oz system	199906		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,319(1999)181-188	A. Sequeira,H. Rajagopal,M.V. Subbarao,R.G. Kulkarni		
8667	PHC3190181		La3(La,Y,Ca,Ba)ba3Cu7Oz	La2.5Y0.5Ca1Ba3Cu7O16.552	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	7											O	Z	16.552	1	1999																											2	3137				3.862		11.601																80			80																																																																																														La2O3, Y2O3, BaCO3, CuO, CaCO3	1	CAL(950C,24H)-pellet-SIN(940-960C,12H in N2+O2 gas)-ANN(500C,12H,in O2 flow)-RT(1C/min)					Structural studies of the superconducting La3.5-x-yYyCa2xBa3.5-xCu7Oz system	199906		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,319(1999)181-188	A. Sequeira,H. Rajagopal,M.V. Subbarao,R.G. Kulkarni		
8668	PHC3190181		La3(La,Y,Ca,Ba)ba3Cu7Oz	La2.1Y0.7Ca1.4Ba2.8Cu7O16.433	La	2.1	Y	0.7	Ca	1.4	Ba	2.8	Cu	7											O	Z	16.433	1	1999																											2	3137				3.839		11.493																79			79																																																																																														La2O3, Y2O3, BaCO3, CuO, CaCO3	1	CAL(950C,24H)-pellet-SIN(940-960C,12H in N2+O2 gas)-ANN(500C,12H,in O2 flow)-RT(1C/min)					Structural studies of the superconducting La3.5-x-yYyCa2xBa3.5-xCu7Oz system	199906		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physia C,319(1999)181-188	A. Sequeira,H. Rajagopal,M.V. Subbarao,R.G. Kulkarni		
8669	PHC3190209		(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.8Bi0.2Sr2Ca2Cu3O8.35	Hg	0.8	Bi	0.2	Sr	2	Ca	2	Cu	3											O	8.35	8.35	1	1999																											2	Hg1223				3.8067		15.2993																102			102										14																																																																																						precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8670	PHC3190209		(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.7Bi0.3Sr2Ca2Cu3O8.35	Hg	0.7	Bi	0.3	Sr	2	Ca	2	Cu	3											O	8.35	8.35	1	1999																											2	Hg1223				3.8185		15.2911																107			107										43																																																																																						precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8671	PHC3190209		(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.5Bi0.5Sr2Ca2Cu3O8.35	Hg	0.5	Bi	0.5	Sr	2	Ca	2	Cu	3											O	8.35	8.35	1	1999																											2	Hg1223				3.826		15.2534																107			107										33																																																																																						precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8672	PHC3190209		(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.7Bi0.3Sr2Ca2Cu3O8.15	Hg	0.7	Bi	0.3	Sr	2	Ca	2	Cu	3											O	Z	8.15		1999																												Hg1223																						108			108																																																																																																precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8673	PHC3190209		(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.7Bi0.3Sr2Ca2Cu3O8.65	Hg	0.7	Bi	0.3	Sr	2	Ca	2	Cu	3											O	Z	8.65		1999																												Hg1223																						104			104																																																																																																precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8674	PHC3190209	annealed at 400C in Ar	(Hg,Bi)Sr2Ca2Cu3Oz	Hg0.7Bi0.3Sr2Ca2Cu3O8.15	Hg	0.7	Bi	0.3	Sr	2	Ca	2	Cu	3											O	Z	8.15		1999																												Hg1223																						112			112																																																																																																precursor(SrCuO2, Ca2CuO3)-mixed with HgO, Bi2O3-Au capsule-high pressure synthesis(6GPa,1000C)					High-prssure synthesis and heat treatments of (Hg1-xBix)Sr2Ca2Cu3Oy	199906		Superconductivity Research Laboratory, ISTEC, 10-13, Shinpnpme 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physia C,319(1999)209-218	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8675	PHC3160113		NdBaCaCu3O7	Nd1Ba1Ca1Cu3O7	Nd	1	Ba	1	Ca	1	Cu	3													O	7		1	1999																											2	1113				3.866		11.6237																37			37																																																																																														Nd2O3, Pr6O11, BaCO3, CaCO3, CuO	1	CAL(975C,40H)-SIN(980C,24H in O2 flow)					Suppression of superconductivity with Pr substitution in Nd1-xPrxBaCaCuO7 system	199905		Instituto de Fisica 'Gleb Wataghin', UNICAMP, 13083-970, Campinas, SP, Brazil	Physica C,316(1999)113-118	A.V. Narlikar,Claudio A. Cardoso,O.F. de Lima,Rajvir Singh,S.K. Malik,V.P.S. Awana,W.B. Yelon		
8676	PHC3160113		(Nd,Pr)BaCaCu3O7	Nd0.9Pr0.1Ba1Ca1Cu3O7	Nd	0.9	Pr	0.1	Ba	1	Ca	1	Cu	3											O	7		1	1999																												1113																						35			35																																																																																														Nd2O3, Pr6O11, BaCO3, CaCO3, CuO	1	CAL(975C,40H)-SIN(980C,24H in O2 flow)					Suppression of superconductivity with Pr substitution in Nd1-xPrxBaCaCuO7 system	199905		Instituto de Fisica 'Gleb Wataghin', UNICAMP, 13083-970, Campinas, SP, Brazil	Physica C,316(1999)113-118	A.V. Narlikar,Claudio A. Cardoso,O.F. de Lima,Rajvir Singh,S.K. Malik,V.P.S. Awana,W.B. Yelon		
8677	PHC3160113		(Nd,Pr)BaCaCu3O7	Nd0.75Pr0.25Ba1Ca1Cu3O7	Nd	0.75	Pr	0.25	Ba	1	Ca	1	Cu	3											O	7		1	1999																												1113																						26			26																																																																																														Nd2O3, Pr6O11, BaCO3, CaCO3, CuO	1	CAL(975C,40H)-SIN(980C,24H in O2 flow)					Suppression of superconductivity with Pr substitution in Nd1-xPrxBaCaCuO7 system	199905		Instituto de Fisica 'Gleb Wataghin', UNICAMP, 13083-970, Campinas, SP, Brazil	Physica C,316(1999)113-118	A.V. Narlikar,Claudio A. Cardoso,O.F. de Lima,Rajvir Singh,S.K. Malik,V.P.S. Awana,W.B. Yelon		
8678	PHC3160113		(Nd,Pr)BaCaCu3O7	Nd0.65Pr0.35Ba1Ca1Cu3O7	Nd	0.65	Pr	0.35	Ba	1	Ca	1	Cu	3											O	7		1	1999																												1113																						10			10																																																																																														Nd2O3, Pr6O11, BaCO3, CaCO3, CuO	1	CAL(975C,40H)-SIN(980C,24H in O2 flow)					Suppression of superconductivity with Pr substitution in Nd1-xPrxBaCaCuO7 system	199905		Instituto de Fisica 'Gleb Wataghin', UNICAMP, 13083-970, Campinas, SP, Brazil	Physica C,316(1999)113-118	A.V. Narlikar,Claudio A. Cardoso,O.F. de Lima,Rajvir Singh,S.K. Malik,V.P.S. Awana,W.B. Yelon		
8679	PHC3160113		(Nd,Pr)BaCaCu3O7	Nd0.5Pr0.5Ba1Ca1Cu3O7	Nd	0.5	Pr	0.5	Ba	1	Ca	1	Cu	3											O	7		1	1999																												1113																							5																																																																																																Nd2O3, Pr6O11, BaCO3, CaCO3, CuO	1	CAL(975C,40H)-SIN(980C,24H in O2 flow)					Suppression of superconductivity with Pr substitution in Nd1-xPrxBaCaCuO7 system	199905		Instituto de Fisica 'Gleb Wataghin', UNICAMP, 13083-970, Campinas, SP, Brazil	Physica C,316(1999)113-118	A.V. Narlikar,Claudio A. Cardoso,O.F. de Lima,Rajvir Singh,S.K. Malik,V.P.S. Awana,W.B. Yelon		
8680	PHC3160021		YBa2Cu3Oz	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	Z	6.41	3	1999																												Y123																				10.1					10.1			6.2																																																																																																		Pressure dependence of Tc in strongly underdoped YBa2Cu3O6.41 as a function of pressure-temperature history	199905		Department of aPhysics, Washington University, C.B. 1105, One Brookings Drive, St. Louis, MO 63130 USA	Physica C,316(1999)21-26	Arvydas P. Paulikas,Boyd W. Veal,James S. Schilling,Vladimir G. Tissen,Yong Wang		
8681	PHC3120061		(La,K)2CuO4	La1.86K0.14Cu1O3.97	La	1.86	K	0.14	Cu	1															O	4-Z	3.97	1	1999																											2	T	14/mmm			3.7683		13.259																33			33																																																																																																La2O3:CuO=0.9:1, with excess KOH, heat(390-720C)					Correlation between synthesis, stoichiometry, structure and superconductivity of La2-xKxCuO4-delta	199901		Technische Universitat Berlin, Institut fur Anorganische und Analytische Chemie, Strasse des 17. Juni 135, D-10623 Berlin, Germany	Physica.C,312(1998)61-70	R. Schollhorn,W. Gunther,W. Paulus		
8682	PHC3120289		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1999																												Bi2212																				82					82																																																																			1.27			TP8682												1.56														mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8683	PHC3120289		Bi2Sr2(Ca,Tb)Cu2O8	Bi2Sr2Ca0.9Tb0.1Cu2OZ	Bi	2	Sr	2	Ca	0.9	Tb	0.1	Cu	2											O	Z		1	1999																												Bi2212																				92					92																																																																			1.55			TP8683												3.22														mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8684	PHC3120289		Bi2Sr2(Ca,Tb)Cu2O8	Bi2Sr2Ca0.8Tb0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Tb	0.2	Cu	2											O	z		1	1999																												Bi2212																				83					83																																																																			3.11			TP8684												9.27														mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8685	PHC3120289		Bi2Sr2(Ca,Tb)Cu2O8	Bi2Sr2Ca0.6Tb0.4Cu2Oz	Bi	2	Sr	2	Ca	0.6	Tb	0.4	Cu	2											O	z		1	1999																												Bi2212																				33					33																																																																			10.8			TP8685												11.25														mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8686	PHC3120289	semiconductor	Bi2Sr2(Ca,Tb)Cu2O8	Bi2Sr2Ca0.5Tb0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Tb	0.5	Cu	2											O	z		1	1999																												Bi2212																							5																																																																					33.7			TP8686																										mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8687	PHC3120289	semiconductor	Bi2Sr2(Ca,Tb)Cu2O8	Bi2Sr2Ca0.4Tb0.6Cu2Oz	Bi	2	Sr	2	Ca	0.4	Tb	0.6	Cu	2											O	z		1	1999																												Bi2212																																																																																												42.5			TP8687																										mixture-CAL(800C,24H)-Q to RT-pellet-heat(880C,20min)-Q to RT-heat(830C, 24H)-Q to RT					Thermoelectric power of the Bi2Sr2Ca1-xTbxCu2Oy system	199902		School of Physics, University of Hyderabad, Central University PO, Hyderabad-500 046, India	Physica.C,312(1998)289-298	D.R. Sita,R. Singh		
8688	PHC3150215		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																											3	Y123				3.8193	3.884	11.681													91	91.8				1.2	91.8																																																																																		16.2												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8689	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3OZ	Y	1	Ba	1.95	La	0.05	Cu	3													O	Z		1	1999																											3	Y123				3.8185	3.8837	11.6767													91	82.2				1.7	82.2																																																																																		8.64												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8690	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3OZ	Y	1	Ba	1.9	La	0.1	Cu	3													O	Z		1	1999																											3	Y123				3.8181	3.8858	11.6654													89.3	91				2.5	91																																																																																		2.64												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8691	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.85La0.15Cu3OZ	Y	1	Ba	1.85	La	0.15	Cu	3													O	Z		1	1999																											3	Y123				3.8189	3.8837	11.6612													89.2	89.7				1.3	89.7																																																																																		9.12												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8692	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3OZ	Y	1	Ba	1.8	La	0.2	Cu	3													O	Z		1	1999																											3	Y123				3.8221	3.8851	11.6426													86.8	89.2				5	89.2																																																																																		8												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8693	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.75La0.25Cu3OZ	Y	1	Ba	1.75	La	0.25	Cu	3													O	Z		1	1999																											3	Y123				3.8245	3.8807	11.6324													83.7	88.5				8.8	88.5																																																																																		5.52												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8694	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3OZ	Y	1	Ba	1.7	La	0.3	Cu	3													O	Z		1	1999																											3	Y123				3.8326	3.8746	11.6167													73	83.2				16.6	83.2																																																																																		6.16												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8695	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3OZ	Y	1	Ba	1.6	La	0.4	Cu	3													O	Z		1	1999																											3	Y123				3.85	3.8589	11.5958													41.5	55.2				27	55.2																																																																																		9.84												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8696	PHC3150215		Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3OZ	Y	1	Ba	1.5	La	0.5	Cu	3													O	Z		1	1999																											3	Y123				3.8554		11.568													22	36.8				33.2	36.8																																																																																		23.8												Y2O3, La2O3, BaCO3, CuO	1	mixture-CAL(950C,16H in air)-SIN(950C,16H in air)-ANN(450C,16H in flowing O2)					The influence of La substitution for Ba in YBa2Cu3Oy cuprates	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)215-222	J. Gao,X.S. Wu		
8697	PHC3150227		CaBa2Ca2Cu3O9-z	Ca2Ba2Cu3O9-Z	Ca	2	Ba	2	Cu	3															O	9-Z			1999																											2	Ca1223				3.85		16.5																107			107																																																																																																high-pressure synthesis. Steps were taker to minimiqe the possibility of C-contamination					Observation and identification of a 107 K superconducting family in the CaBa2Ca2Cu3O9-delta system	199904		Texas Center for Superconductivity at the University of Houston, TX 77204-5932, USA	Physica C,315(1999)227-234	B. Raveau,C.W. Chu,D.K. Ross,I. Rusakova,L. Gao,M. Hervieu,N.L. Wu,Y. Cao,Y.Y. Sun,Y.Y. Xue,Z.L. Du		
8698	PHC2540131	two step transition(110K,75K), 110K due to B1234 phase	BSr2Ca2Cu3O9	B1Sr2Ca2Cu3O9	B	1	Sr	2	Ca	2	Cu	3													O	9			1995																											2	B1223				3.821		13.854																75			75																																																																																														SrCuO2, SrO2, Ca2CuO3, B2O3, CuO		mixture-seal in Au capsule-high-P synthesis(1200-1300C, 1H, 6GPa)-Q to RT					New series of oxide superconductors, BSr2Can-1CunO2n+3 (n=3-5), prepared at high pressure	199511		National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tshukuba, Ibaraki, 305, Japan	Physica C,254(1995)131-136	E. Takayama-Muromachi,T. Kawashima,Y. Matsui	B, Sr, Ca, Cu, O	
8699	PHC2540131	two step transition(110K,85K), 110K due to B1234 phase 	BSr2Ca4Cu5O13	B1Sr2Ca4Cu5O13	B	1	Sr	2	Ca	4	Cu	5													O	13			1995																												B1245				3.837		20.22																85			85																																																																																														SrCuO2, SrO2, Ca2CuO3, B2O3, CuO		mixture-seal in Au capsule-high-P synthesis(1200-1300C, 1H, 6GPa)-Q to RT					New series of oxide superconductors, BSr2Can-1CunO2n+3 (n=3-5), prepared at high pressure	199511		National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tshukuba, Ibaraki, 305, Japan	Physica C,254(1995)131-136	E. Takayama-Muromachi,T. Kawashima,Y. Matsui	B, Sr, Ca, Cu, O	
8700	PHC2410137		BSr2Ca3CuO11	B1Sr2Ca3Cu4O11	B	1	Sr	2	Ca	3	Cu	4													O	11			1995																											2	B1234				3.8359		17.082																110			110																																																																																														SrCuO2, Ca2CuO3, SrO2, CuO, B2O3		mixture-seal in Au capsule-high pressure synthesis(1200, 1H, 6GPa)					New oxyborate superconductor,BSr2Ca3Cu4O11(Tc=110K) prepared at high pressure	199501		National Instiute for Research in Inorganic Materials(NIRIM),1-1 Namiki,Tsukuba,Ibaraki,305 Japan	Physica C.,241(1995)137-141	E.Takayama-Muromachi,K.Kosuda,Y.Matsui	B,Sr,Ca,Cu,O	
8701	PHC2240069		(Cu,C)Ba2Ca2Cu3O9	Cu0.5C0.5Ba2Ca2Cu3O9	Cu	0.5	C	0.5	Ba	2	Ca	2	Cu	3											O	9			1994																											2	CuC1223				3.859		14.766																67			67																																																																																																precursor(Ba2CaCu2O5)+CaCuO3+Ag2O-seal in Au capsule-high pressure synthesis(1200C, 1H 5GPa)					New oxycarbonate superconductors (Cu0.5C0.5)Ba2Can-1CunO2n+3 (n=3,4) prepared at high pressure				Physica C, 224(1994)69-74	E.Takayama-Muromachi,T.Kawashima,Y.Matsui	Cu,C,Ba,Ca,O	
8702	PHC2240069		(Cu,C)Ba2Ca3Cu4O11	Cu0.5C0.5Ba2Ca3Cu4O11	Cu	0.5	C	0.5	Ba	2	Ca	3	Cu	4											O	11			1994																											2	CuC1224				3.855		17.93																117			117																																																																																																precursor(Ba2CaCu2O5)+CaCuO3+Ag2O-seal in Au capsule-high pressure synthesis(1200C, 1H 5GPa)					New oxycarbonate superconductors (Cu0.5C0.5)Ba2Can-1CunO2n+3 (n=3,4) prepared at high pressure				Physica C, 224(1994)69-74	E.Takayama-Muromachi,T.Kawashima,Y.Matsui	Cu,C,Ba,Ca,O	
8703	PHC2880185		CCa2CaCu2O7	C1Ca3Cu2O7.1	C	1	Ca	3	Cu	2															O	7+Z	7.1		1997																												C1212				3.842		10.336													25		50	47			47																																																																																														CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8704	PHC2880185	not s/c	CCa2CaCu2O7	C1Ca3Cu2O7	C	1	Ca	3	Cu	2															O	7+Z	7		1997																																																			4.2																																																																																																CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8705	PHC2880185	not s/c	CCa2CaCu2O7	C1Ca3Cu2O7.2	C	1	Ca	3	Cu	2															O	7+Z	7.2		1997																																																			4.2																																																																																																CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8706	PHC2880185		(Cu,C)Ca2CaCu2Oz	Cu0.25C0.75Ca3Cu2O6.85	Cu	0.25	C	0.75	Ca	3	Cu	2													O	Z	6.85		1997																												C1212																						47			47																																																																																														CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8707	PHC2880185		(Cu,C)Ca2CaCu2Oz	Cu0.5C0.5Ca3Cu2O6.6	Cu	0.5	C	0.5	Ca	3	Cu	2													O	Z	6.6		1997																												C1212																						57			57																																																																																														CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8708	PHC2880185	not s/c volume faction=nearly zero	(Cu,C)Ca2CaCu2Oz	Cu0.75C0.25Ca3Cu2O6.5	Cu	0.75	C	0.25	Ca	3	Cu	2													O	Z	6.5		1997																												C1212																																																																																																																							CuO, CaCO3, Ca2CuO3, CaO2		mixture-seal in Au capsule-high pressure synthesis(1275, 1H, 6GPa)					High-pressure synthesis of a new oxycarbonate superconductor CCa3Cu2O7+Delta	199709		National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C,288(1997)185-189	A.T. Matveev,E. Takayama-Muromachi,S. Yamaoka,Y. Matsui		
8709	PHC2740048		(Ge,Cu)Sr2(Ca,Y)3Cu4O11	Ge0.3Cu0.7Sr2Ca2.9Y0.1Cu4O11.1	Ge	0.3	Cu	0.7	Sr	2	Ca	2.9	Y	0.1	Cu	4									O	11.1		2	1997																											2	M1234				3.8411		17.733																89			89																																																																																																high pressure synthesis					New high-Tc superconductors(GezCu1-z)Sr2Can-1-xYxCunOy (n=4,6) prepared at high pressure	199701		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki,Ibaraki 305, Japan	Physica.C,274(1997)48-54	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui		
8710	PHC2740048		(G,Cu)Sr2Ca5Cu6Oz	Ge0.3Cu0.7Sr2Ca3Cu4O11.05	Ge	0.3	Cu	0.7	Sr	2	Ca	3	Cu	4											O	11.05			1997																												M1256				3.8496		24.183																7			7																																																																																																high pressure synthesis					New high-Tc superconductors(GezCu1-z)Sr2Can-1-xYxCunOy (n=4,6) prepared at high pressure	199701		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki,Ibaraki 305, Japan	Physica.C,274(1997)48-54	A.T. Matveev,E. Takayama-Muromachi,J. Ramirez-Castellanos,Y. Matsui		
8711	PHC2730072	z=nominal, two step trasition(82K,112K),impurity=Cu1234		Cu0.5P0.5Sr2Ca2Cu3O9.25	Cu	0.5	P	0.5	Sr	2	Ca	2	Cu	3											O	Z	9.25		1996																												Cu1245																						82			82																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8712	PHC2730072	z=nominal		Cu0.5P0.5Sr2Ca1.9Y0.1Cu3O9.3	Cu	0.5	P	0.5	Sr	2	Ca	1.9	Y	0.1	Cu	3									O	Z	9.3		1996																												Cu1234																						84			84																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8713	PHC2730072	z=nominal		Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.35	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.35		1996																												Cu1234																						70			70																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8714	PHC2730072	z=nominal, two step trasition(50K,64K),impurity=Cu1223		Cu0.5P0.5Sr2Ca1.7Y0.3Cu3O9.4	Cu	0.5	P	0.5	Sr	2	Ca	1.7	Y	0.3	Cu	3									O	Z	9.4		1996																												Cu1212																						50			50																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8715	PHC2730072	z=nominal		Cu0.5P0.5Sr2Ca1.9Y0.1Cu3O9.4	Cu	0.5	P	0.5	Sr	2	Ca	1.9	Y	0.1	Cu	3									O	Z	9.4		1996																												Cu1234																						84			84																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8716	PHC2730072	z=nominal	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.25	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.25		1996																												Cu1223																						72			72																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8717	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.45	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.45		1996																												Cu1223																						74			74																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8718	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.55	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.55		1996																												Cu1223																						80			80																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca3(PO4)2					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8719	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.25	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.25		1996																												Cu1223																						68			68																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca2P2O7					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8720	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.35	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.35		1996																												Cu1223																						72			72																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca2P2O7					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8721	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.45	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.45		1996																												Cu1223																						76			76																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca2P2O7					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8722	PHC2730072	z=nominal value	(Cu,P)Sr2(Ca,Y)2Cu3Oz	Cu0.5P0.5Sr2Ca1.8Y0.2Cu3O9.55	Cu	0.5	P	0.5	Sr	2	Ca	1.8	Y	0.2	Cu	3									O	Z	9.55		1996																												Cu1223																						80			80																																																																																																high pressure synthesis(1250-1300C,1H,5-6 Gpa)P-source=Ca2P2O7					New series of oxyphosphate superconductors (Cu0.5P0.5)Sr2(Ca,Y)n-1CunOy [(Cu,P)-12(n-1)n,n=3-6] prepared under high pressure	199612		National Institute for Research in Inorganic Materials(NIRIM),1-1 Namiki, Tsukuba, Ibaraki, 305 Japan	Physica.C,273(1996)72-82	E. Takayama-Muromachi,M.Isobe,Y. Matsui		
8723	PHC1730009		La2CuO4	La2Cu1O4+Z	La	2	Cu	1																	O	4+Z		1	1991																												T																		K	33	35					35																																																																			116.1			TP8723																								La2O3, CuO		mixture-heat(950C,20H)-pellet-heat(1100C,26H)-ANN(550C,24H in O2)-slow cool					CHARACTERISTICS OF MIXED PHASE SUPERCONDUCTIVITY IN OXYGENATEDLA2CUO4+Z	199101		HLH.WILLS PHYSICS LABORATORY, UNIVERSITY OF BRISTOL BS8 1TL, UK	PHYSICA C,173(1991)9	D.L.YATES,J.A.WILSON,J.RYDER,L.AFALFIZ,P.A.MIDGLEY,R.EXLEY,R.J.BEYNON	LA,CU,O	
8724	APJ0375535	impurity phase=5-10%		B1Sr2Ca2Cu3O2N+3	B	1	Sr	2	Ca	2	Cu	3													O	2N+3			1998																												B1223																						75			75																																		HIR8724																		JC8724																																												high pressure synthesis(1250C,6GPa)					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8725	APJ0375535			B1Sr2Ca3Cu4O2N+3	B	1	Sr	2	Ca	3	Cu	4													O	2N+3		1	1998																												B1234																						110			110																																																				JC8725																																												high pressure synthesis(1250C,6GPa)					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8726	APJ0375535			B1Sr2Ca4Cu5O2N+3	B	1	Sr	2	Ca	4	Cu	5													O	2N+3		1	1998																												B1245																						85			85																																																				JC8726																																												high pressure synthesis(1250C,6GPa)					Anisotropy in Magnetic Hysteresis of BSr2Can-1CunO2n+3(n=3,4,5,) superconductors			National Institute for Research in Inorganic Materials(NIRIM), 1-1 Namiki, Tsukuba,Ibaraki 305-0044, Japan	Jpn.J.Appl.Phys.37(1998)5535	Eiji TAKAYAMA-MUROMACHI,Shan YU,Tetsuya Kawashima,Yoshishige UCHIDA		
8727	PR05400572	not s/c	La2CuO4	La2Cu1O4.02	La	2	Cu	1																	O	4+Z	4.02		1996								250																				T																																																																																																																									polycrystalline La2CuO4+z were prepared by electrochemically oxidizing.					Phase separasion and oxygen diffusion in electrochemically oxidized La2CuO4+: A static magnetic susceptibility study	199607		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B,54(1996)572	D.C. Johnston,F.C. Chou		
8728	PR05400572	phase separation,z=4.06 phase is superconducting at 34K	La2CuO4	La2Cu1O4.03	La	2	Cu	1																	O	4+Z	4.03		1996								250																				T																						34			34																																																																																																polycrystalline La2CuO4+z were prepared by electrochemically oxidizing.					Phase separasion and oxygen diffusion in electrochemically oxidized La2CuO4+: A static magnetic susceptibility study	199607		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B,54(1996)572	D.C. Johnston,F.C. Chou		
8729	PR05400572	phase separation,z=4.06 phase is superconducting at 34K	La2CuO4	La2Cu1O4.044	La	2	Cu	1																	O	4+Z	4.044		1996								240																				T																						34			34																																																																																																polycrystalline La2CuO4+z were prepared by electrochemically oxidizing.					Phase separasion and oxygen diffusion in electrochemically oxidized La2CuO4+: A static magnetic susceptibility study	199607		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B,54(1996)572	D.C. Johnston,F.C. Chou		
8730	PR05400572	nearly one phase(Tc=34K)	La2CuO4	La2Cu1O4.065	La	2	Cu	1																	O	4+Z	4.065		1996																												T																						34			34																																																																																																polycrystalline La2CuO4+z were prepared by electrochemically oxidizing.					Phase separasion and oxygen diffusion in electrochemically oxidized La2CuO4+: A static magnetic susceptibility study	199607		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B,54(1996)572	D.C. Johnston,F.C. Chou		
8731	PR05400572	high Tc phase	La2CuO4	La2Cu1O4.11	La	2	Cu	1																	O	4+Z	4.11		1996																												T																						42			42																																																																																																polycrystalline La2CuO4+z were prepared by electrochemically oxidizing.					Phase separasion and oxygen diffusion in electrochemically oxidized La2CuO4+: A static magnetic susceptibility study	199607		Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139	Phys.Rev.B,54(1996)572	D.C. Johnston,F.C. Chou		
8732	PR0414062	phase separation temperatre=280K	La2CuO4	La2Cu1O4.032	La	2	Cu	1																	O	4+Z	4.032		1990																												T																				30	35				30																																																																					56.1	TP8732																										crystal was grown from CuO rich La2O3-CuO melt in a Pt crucible. ANN(575C,12H in 3K bar O2)-cool(100C/h)					PHASE SEPARATION IN A HIGH-PRESSURE-OXYGENATED LA2CUO4+Z CRYSTAL: EVIDENCE FROM ANISOTROPIC ELECTRONIC TRANSPORT AND MAGNETIC SUSCEPTIBILITY	199003	SUSCEPTIBILITY      ,RESISTIVITY         ,THERMOELECTRIC POWER,SINGLE CRYSTAL      ,PHASE-SEPARATION	LOS ALAMOS NATIONAL LABORATORY, LOS ALAMOS, NEW MEXICO 87545	PHYS.REV.B,41(1990)4062	J.D.THOMPSON,J.E.SCHIRBER,M.F.HUNDLEY,S.-W.CHEONG,Z.FISK	LA,CU,O	
8733	JJP0380283	Tox=250C. Tox is the temperature where O3 gas suply is stopped during the post-growth cooling.	PbSr2CuO5+z	Pb1Sr2Cu1O5+Z	Pb	1	Sr	2	Cu	1															O	5+Z		4	1999																												Pb1201																							4.2																																																																																																		films were grown by MBE. Substrate=LaAlO3(001)					New Superconducting PbSr2CuO5+delta Prepared by a Novel Low-Temperature Synthetic Route Using Molecular Beam Epitaxy	199909		NTT Basic Research Laboratories, 3-1 Wakamiya, Morinosato, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys.Lett.38(1999)L283-L285	Michio NAITO,Shin-ichi KARIMOTO		
8734	JJP0380283	Tox=325C. Tox is the temperature where O3 gas suply is stopped during the post-growth cooling.	PbSr2CuO5+z	Pb1Sr2Cu1O5+Z	Pb	1	Sr	2	Cu	1															O	5+Z		4	1999																												Pb1201																			20						20																																																																																																films were grown by MBE. Substrate=LaAlO3(001)					New Superconducting PbSr2CuO5+delta Prepared by a Novel Low-Temperature Synthetic Route Using Molecular Beam Epitaxy	199909		NTT Basic Research Laboratories, 3-1 Wakamiya, Morinosato, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys.Lett.38(1999)L283-L285	Michio NAITO,Shin-ichi KARIMOTO		
8735	JJP0380283	Tox=480C. Tox is the temperature where O3 gas suply is stopped during the post-growth cooling.	PbSr2CuO5+z	Pb1Sr2Cu1O5+Z	Pb	1	Sr	2	Cu	1															O	5+Z		4	1999																												Pb1201																			40						40																																																																																																films were grown by MBE. Substrate=LaAlO3(001)					New Superconducting PbSr2CuO5+delta Prepared by a Novel Low-Temperature Synthetic Route Using Molecular Beam Epitaxy	199909		NTT Basic Research Laboratories, 3-1 Wakamiya, Morinosato, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys.Lett.38(1999)L283-L285	Michio NAITO,Shin-ichi KARIMOTO		
8736	JJP0380283	Tox=500C. Tox is the temperature where O3 gas suply is stopped during the post-growth cooling.	PbSr2CuO5+z	Pb1Sr2Cu1O5+Z	Pb	1	Sr	2	Cu	1															O	5+Z		4	1999																												Pb1201																			40						40																																																																																																films were grown by MBE. Substrate=LaAlO3(001)					New Superconducting PbSr2CuO5+delta Prepared by a Novel Low-Temperature Synthetic Route Using Molecular Beam Epitaxy	199909		NTT Basic Research Laboratories, 3-1 Wakamiya, Morinosato, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys.Lett.38(1999)L283-L285	Michio NAITO,Shin-ichi KARIMOTO		
8737	PHC3150059		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																																3.818	3.884	11.687													90.2						90.2																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8738	PHC3150059		Y(Ba,Pr)2Cu3O7	Y1Ba1.95Pr0.05Cu3OZ	Y	1	Ba	1.95	Pr	0.05	Cu	3													O	Z		1	1999																																															88.1						88.1																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8739	PHC3150059		Y(Ba,Pr)2Cu3O7	Y1Ba1.9Pr0.1Cu3OZ	Y	1	Ba	1.9	Pr	0.1	Cu	3													O	Z		1	1999																																															83.3						83.3																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8740	PHC3150059		Y(Ba,Pr)2Cu3O7	Y1Ba1.85Pr0.15Cu3OZ	Y	1	Ba	1.85	Pr	0.15	Cu	3													O	Z		1	1999																																3.823	3.888	11.677													76.1						76.1																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8741	PHC3150059		Y(Ba,Pr)2Cu3O7	Y1Ba1.8Pr0.2Cu3OZ	Y	1	Ba	1.8	Pr	0.2	Cu	3													O	Z		1	1999																																															67						67																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8742	PHC3150059		Y(Ba,Pr)2Cu3O7	Y1Ba1.75Pr0.25Cu3OZ	Y	1	Ba	1.75	Pr	0.25	Cu	3													O	Z		1	1999																																															51.9						51.9																																																																																															1	mixture-CAL(950C,24H in O2flow)-SIN(950C, 24H in O2flow)- RT(1C/min)					Comparison of Tc-depression of Pr at Y- and Ba-sites in YBa2Cu3Oy	199904		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,315(1999)59-65	J. Gao,W.H. Tang		
8743	PHC3130001	crystals were irradiated at RT. With 2.5 MeV/amu <84>Kr-ion. This irradiation did not influence the Tc value	(Y,Tm)Ba2Cu3O7	Y0.14Tm0.85Ba2Cu3O7	Y	0.14	Tm	0.85	Ba	2	Cu	3													O	7		1	1999																												Y123																						91			91																																		HIR8743																																																														self-flux method using ZrO2:Y crucible					Critical currents, pinning forces and irreversibility fields in (YxTm1-x)Ba2Cu3O7 single crystals with columnar defects in fields up to 50T	199902		Laboratorium voor Vaste-Stoffysica en Magnetisme, Katholieke Universiteit Leuven, Celestijnenlaan 200D, B-3001, Leuven, Belgium	Physica C,313(1999)1-10	A. Yu. Didyk,F. Herlach,I.N. Goncharov,J. Vanacken,K. Rosseel,L. Trappeniers,L. Weckhuysen,L.I. Leonyuk,V.V. Moshchalkov,W. Boon,Y. Bruynseraede		
8744	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu7Fe7O16.574	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	7	Fe	7									O	Z	16.574		1999																												3137				3.8628		11.6047													79	80	81	80			80																																																																																															1	mixture-heat (950,24H in air)-pellet-SIN(940-960C,12H in O2+Ar)-ANN(500C,12H in O2 flow-RT(1C/min)					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8745	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.86Fe0.14O16.578	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.86	Fe	0.14									O	Z	16.578		1999																												3137				3.8892		11.6047													73	77	80	75			77																																																																																															1	mixture-heat (950,24H in air)-pellet-SIN(940-960C,12H in O2+Ar)-ANN(500C,12H in O2 flow-RT(1C/min)					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8746	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.72Fe0.28O16.592	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.72	Fe	0.28									O	Z	16.592		1999																												3137				3.8815		11.6281													66	70	74	67.5			70																																																																																															1	mixture-heat (950,24H in air)-pellet-SIN(940-960C,12H in O2+Ar)-ANN(500C,12H in O2 flow-RT(1C/min)					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8747	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.58Fe0.42O16.599	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.58	Fe	0.42									O	Z	16.599		1999																												3137				3.8694		11.6047													62	68	73	63			68																																																																																															1	mixture-heat (950,24H in air)-pellet-SIN(940-960C,12H in O2+Ar)-ANN(500C,12H in O2 flow-RT(1C/min)					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8748	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.44Fe0.56O16.617	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.44	Fe	0.56									O	Z	16.617		1999																												3137				3.8727		11.6031													50	58	66	50			58																																																																																																					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8749	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.3Fe0.7O16.627	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.3	Fe	0.7									O	Z	16.627		1999																												3137				3.8694		11.6125													41	51	60	41			51																																																																																																					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8750	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.16Fe0.84O16.634	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	6.16	Fe	0.84									O	Z	16.634		1999																												3137																			31	41	50	31.5			41																																																																																																					Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8751	PHC3130041		(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu5.95Fe1.05O16.64	La	2.5	Y	0.5	Ca	1	Ba	3	Cu	5.95	Fe	1.05									O	Z	16.64		1999																												3137																							10																																																																																																							Superconducting properties of the Fe-substituted La2.5T0.5CaBa3(Cu1-xFex)7Oz perovskite	199902		Department of Physics, Saurashtra University Road, Rajkot 360 005, India	Physica C,313(1999)41-48	D.G. Kuberkar,M.V. Subbarao,R.G. Kulkarni		
8752	PHC3130049		Ca(Ba,Nd)2Cu3O7	Y1Ba1.8Nd0.2Cu3OZ	Y	1	Ba	1.8	Nd	0.2	Cu	3													O	Z			1999																											3	Y123				3.8873	3.8284	11.6748													89.9	90.8				1.4	90.8																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8753	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.95Ca0.05Ba1.8Nd0.2Cu3OZ	Y	0.95	Ca	0.05	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																											3	Y123				3.8842	3.8273	11.6716													84.2	87				2.8	87																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8754	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.9Ca0.1Ba1.8Nd0.2Cu3OZ	Y	0.9	Ca	0.1	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																											3	Y123				3.878	3.8314	11.6714													81.3	84.6				3.6	84.6																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8755	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.85Ca0.15Ba1.8Nd0.2Cu3OZ	Y	0.85	Ca	0.15	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																											3	Y123				3.878	3.8322	11.6715													80.6	84.5				4.6	84.5																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8756	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.8Nd0.2Cu3OZ	Y	0.8	Ca	0.2	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																											3	Y123				3.8817	3.8347	11.6668													81.3	85.8				6.4	85.8																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8757	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.75Ca0.25Ba1.8Nd0.2Cu3OZ	Y	0.75	Ca	0.25	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																												Y123				3.8775	3.8335	11.6791													80.4	81.5				2.8	81.5																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8758	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.7Ca0.3Ba1.8Nd0.2Cu3OZ	Y	0.7	Ca	0.3	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																												Y123				3.8786	3.836	11.6814													77.6	78.7				1	78.7																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8759	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.6Ca0.4Ba1.8Nd0.2Cu3OZ	Y	0.6	Ca	0.4	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																												Y123				3.8783	3.8349	11.6798													76.8	81.5				3.6	81.5																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8760	PHC3130049		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.5Ca0.5Ba1.8Nd0.2Cu3OZ	Y	0.5	Ca	0.5	Ba	1.8	Nd	0.2	Cu	3											O	Z			1999																												Y123				3.8698	3.8617	11.748													34						34																																																																																															1	ANN(450C,1000 min in O2 flow)					Structure and transport properties in calcium-doped YBa1.8Nd0.2Cu3Oy cuprates	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)49-57	J. Gao,X.S. Wu		
8761	PHC3130079		(Y,Ca)BaCu3O7	Y0.8Ca0.2Ba2Cu3OZ	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	Z			1999																											3	Y123				3.8801	3.8264	11.6874													74						74																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8762	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.95Nd0.05Cu3OZ	Y	0.8	Ca	0.2	Ba	1.95	Nd	0.05	Cu	3											O	Z			1999																											3	Y123				3.8826	3.8271	11.6822													76						76																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8763	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.9Nd0.1Cu3OZ	Y	0.8	Ca	0.2	Ba	1.9	Nd	0.1	Cu	3											O	Z			1999																											3	Y123				3.8818	3.8259	11.6804													79						79																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8764	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.85Nd0.15Cu3OZ	Y	0.8	Ca	0.2	Ba	1.85	Nd	0.15	Cu	3											O	Z			1999																											3	Y123				3.8829	3.8259	11.68													83						83																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8765	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba0.8Nd0.2Cu3OZ	Y	0.8	Ca	0.2	Ba	0.8	Nd	0.2	Cu	3											O	Z			1999																											3	Y123				3.8833	3.8253	11.6746													73						73																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8766	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.75Nd0.25Cu3OZ	Y	0.8	Ca	0.2	Ba	1.75	Nd	0.25	Cu	3											O	Z			1999																											3	Y123				3.8803	3.826	11.6611													69						69																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8767	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.7Nd0.3Cu3OZ	Y	0.8	Ca	0.2	Ba	1.7	Nd	0.3	Cu	3											O	Z			1999																											3	Y123				3.8789	3.8283	11.6591													63						63																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8768	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.6Nd0.4Cu3OZ	Y	0.8	Ca	0.2	Ba	1.6	Nd	0.4	Cu	3											O	Z			1999																											3	Y123				3.8668	3.8386	11.6381													58						58																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8769	PHC3130079		(Y,Ca)(Ba,Nd)2Cu3O7	Y0.8Ca0.2Ba1.5Nd0.5Cu3OZ	Y	0.8	Ca	0.2	Ba	1.5	Nd	0.5	Cu	3											O	Z			1999																											3	Y123				3.8753	3.8495	11.6156													32						32																																																																																															1	ANN(350C,25H in O2 flow)					Superconductivity and structural changes in Y0.8Ca0.2Ba2-xNdxCu3Oy cuprates with x=< 0.50	199902		Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China	Physica C,313(1999)79-86	J. Gao,X.S. Wu		
8770	PSS0411363		YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	Z	6.95	1	1999																											3	Y123				3.818	3.89	11.666	3													91					91																																																																		microV/P	0			TP8770																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8771	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.95Ca0.05Ba2Cu2.95Co0.05O6.96	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Co	0.05											O	Z	6.96	1	1999																											3	Y123				3.83	3.89	11.668	3													88					88																																																																		microV/P	2			TP8771																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8772	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.9Ca0.1Ba2Cu2.9Co0.1O6.95	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Co	0.1											O	Z	6.95	1	1999																											3	Y123				3.862	3.87	11.673	3													88					88																																																																		microV/P	4			TP8772																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8773	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.85Ca0.15Ba2Cu2.85Co0.15O6.97	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z	6.97	1	1999																											3	Y123				3.864	3.868	11.676	3													86					86																																																																		microV/P	5.5			TP8773																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8774	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.8Ca0.2Ba2Cu2.8Co0.2O6.98	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Co	0.2											O	Z	6.98	1	1999																											2	Y123				3.865		11.695	3													82.5					82.5																																																																		microV/P	5.5			TP8774																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8775	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.75Ca0.25Ba2Cu2.75Co0.25O7	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	Z	7	1	1999																											2	Y123				3.867		11.689	3													82.5					82.5																																																																		microV/P	5.5			TP8775																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8776	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.7Ca0.3Ba2Cu2.7Co0.3O7.02	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z	7.02	1	1999																											2	Y123				3.866		11.698	3													82					82																																																																		microV/P	5.5			TP8776																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8777	PSS0411363		YBa2Cu3Oz	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	Z	6.82	1	1999																											3	Y123				3.826	3.89	11.702	3													85					85																																																																		microV/P	6.5			TP8777																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8778	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.95Ca0.05Ba2Cu2.95Co0.05O6.84	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Co	0.05											O	Z	6.84	1	1999																											3	Y123				3.837	3.88	11.711	3													72.5					72.5																																																																		microV/P	14			TP8778																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8779	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.9Ca0.1Ba2Cu2.9Co0.1O6.84	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Co	0.1											O	Z	6.84	1	1999																											2	Y123				3.863		11.711	3													69.5					69.5																																																																		microV/P	16.5			TP8779																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8780	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.85Ca0.15Ba2Cu2.85Co0.15O6.83	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z	6.83	1	1999																											2	Y123				3.864		11.716	3													67.5					67.5																																																																		microV/P	19			TP8780																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8781	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.8Ca0.2Ba2Cu2.8Co0.2O6.83	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Co	0.2											O	Z	6.83	1	1999																											2	Y123				3.868		11.72	3													69					69																																																																		microV/P	21			TP8781																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8782	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.75Ca0.25Ba2Cu2.75Co0.25O6.82	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	Z	6.82	1	1999																											2	Y123				3.868		11.715	3													67.5					67.5																																																																		microV/P	19			TP8782																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8783	PSS0411363		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.7Ca0.3Ba2Cu2.7Co0.3O6.84	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z	6.84	1	1999																											2	Y123				3.868		11.714	3													70					70																																																																		microV/P	14.9			TP8783																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(Oxygen-deficient atmosphere, 450C, 2H)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8784	PSS0411363		YBa2Cu3O7	Y1Ba2Cu3O6.74	Y	1	Ba	2	Cu	3															O	Z	6.74	1	1999																											3	Y123				3.824	3.896	11.704	3													79.5					79.5																																																																		microV/P	9			TP8784																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8785	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.95Ca0.05Ba2Cu2.95Co0.05O6.75	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Co	0.05											O	Z	6.75	1	1999																											3	Y123				3.836	3.886	11.71	3													64					64																																																																		microV/P	22			TP8785																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8786	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.9Ca0.1Ba2Cu2.9Co0.1O6.76	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Co	0.1											O	Z	6.76	1	1999																											2	Y123				3.864		11.713	3													57.5					57.5																																																																		microV/P	24			TP8786																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8787	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.85Ca0.15Ba2Cu2.85Co0.15O6.78	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z	6.78	1	1999																											2	Y123				3.865		11.717	3													57.5					57.5																																																																		microV/P	25			TP8787																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8788	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.8Ca0.2Ba2Cu2.8Co0.2O6.78	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Co	0.2											O	Z	6.78	1	1999																											2	Y123				3.866		11.73	3													55.5					55.5																																																																		microV/P	21.5			TP8788																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8789	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.75Ca0.25Ba2Cu2.75Co0.25O6.8	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	Z	6.8	1	1999																											2	Y123				3.868		11.73	3													61					61																																																																		microV/P	15			TP8789																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8790	PSS0411363		(Y,Ca)Ba2(Cu,Co)3O7	Y0.7Ca0.3Ba2Cu2.7Co0.3O6.78	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z	6.78	1	1999																											2	Y123				3.87		11.725	3													59					59																																																																		microV/P	15			TP8790																									1	pellet-ANN(450C,6H+400C,10H in O2 flow)-ANN(475C,2H in Oxygen-deficient atmosphere, )									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1363	M.V.Elizarova,V.E.Gasumyantz		
8791	PSS0411165	Debye Temp=382K for low temperature analysis. gamma is for H=0 T. 	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-z	Pr	1.85	Ce	0.15	Cu	1															O	4-z		1	1999																											2	T'																						18			18										40																																											SP8791			mj/mole.K2	1.4		550																																			Pr2O3, CeO, CuO	3	mixture-CAL(950C,14H in air)-pellet-CAL(1100C,18H in air)-cool to RT(20C/min)-ANN(920C,7H in 0.0001 Torr)-cool to RT(10C/min)									Fizika tverdogo tera (Phys. Of the Solid State) 41(1999)1165	A.A.Shikov,G.Kh. Panova,M.N.Khlopkin,N.A.Chernoplekov		
8792	JSC1350017		SrCuO2F2-z	Sr2Cu1F2O2	Sr	2	Cu	1	F	2															O	2		3	1998																												T																						46			46																																																																																																precursor-fluorination(using F2 or MF2(M=Zn,Cu,Ag,Ni)					Superconducting Sr2-xAxCuO2F2+delta(A=Ca,Ba): Synthetic Pathways and Associated Structural Rearrangements			School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom; and  School of Physics and Space Research, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom	J.Solid State Chem.135(1998)17-27	C. Greaves,J.P. Hodges,M. Al-Mamouri,M. Al-Manouri,M. Slaski,M.G. Francesconi,P.P. Edwards,P.R. Slater		
8793	JSC1350017		(Sr,Ba)2CuO2F2-z	Sr1.4Ba0.6Cu1F2O2	Sr	1.4	Ba	0.6	Cu	1	F	2													O	2		3	1998																												T																						64			64																																																																																																precursor-fluorination(using F2 or MF2(M=Zn,Cu,Ag,Ni)					Superconducting Sr2-xAxCuO2F2+delta(A=Ca,Ba): Synthetic Pathways and Associated Structural Rearrangements			School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom; and  School of Physics and Space Research, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom	J.Solid State Chem.135(1998)17-27	C. Greaves,J.P. Hodges,M. Al-Mamouri,M. Al-Manouri,M. Slaski,M.G. Francesconi,P.P. Edwards,P.R. Slater		
8794	PRL0822792	untwinned crystal. anisotropy factor  < a>/< b> = 1.18.   < c>/< a> = 4.5	YBa2Cu3O7	Y1Ba2Cu3O4	Y	1	Ba	2	Cu	3															O	4		3	1999																												Y123																						92			92																																												1380																																																				ANN(490C in flowing O2)					Flux-Line Lattice Structures in Untwinned YBa2Cu3O7-delta	3		School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, United Kingdom	Phys.Rev.Lett.82(1989)2792	A. Rykov,C. Ager,C.M. Agerter,D.McK. Paul,E.M. Forgan,P.G. Kealey,R. Cubitt,S. Tajima,S.H. Lloyd,S.L. Lee,S.T. Johnson		
8800	PHC3130058		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		1	1999																											3	Bi2212																																																																																												-3.21			TP8800																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8801	PHC3130058		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.8La0.2Ca1Cu2OZ	Bi	2	Sr	1.8	La	0.2	Ca	1	Cu	2											O	Z		1	1999																											3	Bi2212																																																																																												4.57			TP8801																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8802	PHC3130058		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.6La0.4Ca1Cu2OZ	Bi	2	Sr	1.6	La	0.4	Ca	1	Cu	2											O	Z		1	1999																											3	Bi2212																																																																																												11.6			TP8802																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8803	PHC3130058		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.4La0.6Ca1Cu2OZ	Bi	2	Sr	1.4	La	0.6	Ca	1	Cu	2											O	Z		1	1999																											3	Bi2212																																																																																												20			TP8803																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8804	PHC3130058		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.3La0.7Ca1Cu2OZ	Bi	2	Sr	1.3	La	0.7	Ca	1	Cu	2											O	Z		1	1999																											3	Bi2212																																																																																												37.6			TP8804																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8805	PHC3130058		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.2La0.8Ca1Cu2OZ	Bi	2	Sr	1.2	La	0.8	Ca	1	Cu	2											O	Z		1	1999																											3	Bi2212																																																																																												51.1			TP8805																										SIN(860-920C). Sintering temperature increases as increasing x					The electronic structure and transport properties of BiSr2-xLaxCaCu2Oy(x=0.0-0.8)	199902		Structure Research Laboratory, USTC, Hefei, Anhui 230026, China	Physica C,313(1999)58-64	C.Y. Wang,G.G. Qian,K.Q. Ruan,L.Z. Cao,M.R. Ji,X.H. Chen		
8806	PHC3140125		(Tl,Pb)(Sr,Ba)2Ca2Cu3Oz	Tl0.5Pb0.5Sr1.6Ba0.4Ca2Cu3OZ	Tl	0.5	Pb	0.5	Sr	1.6	Ba	0.4	Ca	2	Cu	3									O	Z		2	1999																												Tl1223						15.478														120					120																																																																																														CuO,Sr(NO3)2,CaO,BaO2CuF2,PbO,TlO3		precursor was mixed writh xCuF2+0.5PbO+0.35Tl2O3. Heat(980C,10min)					Effect of fluorine on the phase formation and superconducting properties of Tl-1223 superconductors	199203		Physics Department, King Fahd University of Petroleum and Minerals, Dhahran, 31261, Saudi Arabia	Physica C,314(1999)125-132	A.S. Al-Harthi,Kh.A. Ziq,N.M. Hamdan		
8807	PHC3140125		(Tl,Pb)(Sr,Ba)2Ca2Cu3(F,O)z	Tl0.5Pb0.5Sr1.6Ba0.4Ca2Cu3F0.1OZ	Tl	0.5	Pb	0.5	Sr	1.6	Ba	0.4	Ca	2	Cu	3	F	0.1							O	Z		2	1999																												Tl1223						15.4631														120.5					120.5																																																																																														CuO,Sr(NO3)2,CaO,BaO2CuF2,PbO,TlO3		precursor was mixed writh xCuF2+0.5PbO+0.35Tl2O3. Heat(980C,10min)					Effect of fluorine on the phase formation and superconducting properties of Tl-1223 superconductors	199203		Physics Department, King Fahd University of Petroleum and Minerals, Dhahran, 31261, Saudi Arabia	Physica C,314(1999)125-132	A.S. Al-Harthi,Kh.A. Ziq,N.M. Hamdan		
8809	PHC3140125		(Tl,Pb)(Sr,Ba)2Ca2Cu3(F,O)z	Tl0.5Pb0.5Sr1.6Ba0.4Ca2Cu3F2.2OZ	Tl	0.5	Pb	0.5	Sr	1.6	Ba	0.4	Ca	2	Cu	3	F	2.2							O	Z		2	1999																												Tl1223						15.4704														121					121																																																																																														CuO,Sr(NO3)2,CaO,BaO2CuF2,PbO,TlO3		precursor was mixed writh xCuF2+0.5PbO+0.35Tl2O3. Heat(980C,10min)					Effect of fluorine on the phase formation and superconducting properties of Tl-1223 superconductors	199203		Physics Department, King Fahd University of Petroleum and Minerals, Dhahran, 31261, Saudi Arabia	Physica C,314(1999)125-132	A.S. Al-Harthi,Kh.A. Ziq,N.M. Hamdan		
8810	PHC3140125		(Tl,Pb)(Sr,Ba)2Ca2Cu3(F,O)z	Tl0.5Pb0.5Sr1.6Ba0.4Ca2Cu3F3OZ	Tl	0.5	Pb	0.5	Sr	1.6	Ba	0.4	Ca	2	Cu	3	F	3							O	Z		2	1999																												Tl1223						15.4611														123.5					123.5																																																																																														CuO,Sr(NO3)2,CaO,BaO2CuF2,PbO,TlO3		precursor was mixed writh xCuF2+0.5PbO+0.35Tl2O3. Heat(980C,10min)					Effect of fluorine on the phase formation and superconducting properties of Tl-1223 superconductors	199203		Physics Department, King Fahd University of Petroleum and Minerals, Dhahran, 31261, Saudi Arabia	Physica C,314(1999)125-132	A.S. Al-Harthi,Kh.A. Ziq,N.M. Hamdan		
8811	PHC3140196	as-grown,optimal O-content	(Hg,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																											2	Hg1201				3.8827		9.5274																97			97																						160									2.4			HIR8811		A			14.3		A	magnetization		1620																																																				O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8812	PHC3140196	400C,12H in O2	(Hg,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																											2	Hg1201				3.8884		9.5372																80			80																																																																																																O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8813	PHC3140196	500C,12H in O2	(Hg,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																											2	Hg1201				3.8896		9.5347																75			75																																		HIR8813							A	magnetization		2350																																																				O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8814	PHC3140196	500C,18H in O2	(Hg,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																												Hg1201																						55			55																																																																																																O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8815	PHC3140196		(HG,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																												Hg1201																						92			92																								114							1.8			HIR8815		A			17		A	Magnetization		1960																																																				O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8816	PHC3140196		(HG,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																												Hg1201																						85			85																								67							1.1					A			22		A	Magnetization		2130																																																				O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8817	PHC3140196		(HG,Cu)Ba2CuOz	Hg0.8Ba2Cu1.2O4+Z	Hg	0.8	Ba	2	Cu	1.2															O	4+Z		3	1999																												Hg1201																						62			62																																									A	Magnetization		2830																																																				O-content is controlled by post annealing under O2 mosphere					Effect of underdoping on the superconductivity of (Hg,Cu)Ba2CuO4+delta '1201' single crystals	199903		Laboratire CRISMAT, UMR 6508 associee au CNRS, ISMRA et Universite de Caen, 6, Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,314(1999)196-204	A. Daignere,A. Maignan,D. Pelloquin,G. Villard		
8818	PR05614275		La2CuO4	La2Cu1O4+Z	La	2	Cu	1																	O	4+Z		3	1997																												T																						33			33																																									micron.m	FIR			21																																																			TSFZ method. O-content,maybe,=4+0.06. oxdization 					Far-infrared reflectivity along the c axis in La2CuO4+delta, La1.89Ca1.11Cu2O4+delta, and Nd2CuO4-xFx single crystals	199702		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,56(1992)R14275	H. Shibata,T. Yamada		
8819	PR05614275		(La,Ca)2CaCu2O6	La1.89Ca1.1Cu2O6+Z	La	1.89	Ca	1.1	Cu	2															O	6+Z		3	1997																												2126																						47			47																																									micron.m	FIR measurement 			13																																																			CuO flux method. Oxdization by high O2 pressure					Far-infrared reflectivity along the c axis in La2CuO4+delta, La1.89Ca1.11Cu2O4+delta, and Nd2CuO4-xFx single crystals	199702		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,56(1992)R14275	H. Shibata,T. Yamada		
8820	PR05614275	F-content not measured. 	Nd2Cu(O,F)4	Nd2Cu1FO4-X	Nd	2	Cu	1	F																O	4-X		3	1997																												T'																						21			21																																									micron.m	FIR 			32																																																			CuO flux method. Oxdization by anealing in Ar					Far-infrared reflectivity along the c axis in La2CuO4+delta, La1.89Ca1.11Cu2O4+delta, and Nd2CuO4-xFx single crystals	199702		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,56(1992)R14275	H. Shibata,T. Yamada		
8821	PR05911672	ANN(0.2% O2,500C)	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212																						89			89																																									micron. M	Josephson plasma																																																						self-flux method in alumina crucible. Oxidized at 500C for 100 in O2-atmosplere					Josephson plasma frequencies in overdoped Bi2Sr2CaCu2O8+delta	199905		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,59(1999)R11672	A. Matsuda,H. Shibata		
8822	PR05911672	ANN(1 atm O2,500C)	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212																						85			85																																									micron. M	Josephson plasma			77																																																			self-flux method in alumina crucible. Oxidized at 500C for 100 in O2-atmosplere					Josephson plasma frequencies in overdoped Bi2Sr2CaCu2O8+delta	199905		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,59(1999)R11672	A. Matsuda,H. Shibata		
8823	PR05911672	ANN(9 atm O2,500C)	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212																						79			79																																									micron. M	Josephson plasma			48																																																			self-flux method in alumina crucible. Oxidized at 500C for 100 in O2-atmosplere					Josephson plasma frequencies in overdoped Bi2Sr2CaCu2O8+delta	199905		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,59(1999)R11672	A. Matsuda,H. Shibata		
8824	PR05911672	ANN(150 atm O2,500C)	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212																						71			71																																									micron. M	Josephson plasma			35																																																			self-flux method in alumina crucible. Oxidized at 500C for 100 in O2-atmosplere					Josephson plasma frequencies in overdoped Bi2Sr2CaCu2O8+delta	199905		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,59(1999)R11672	A. Matsuda,H. Shibata		
8825	PHC3210001	Hc2,Hirr were determined by specific heat. Ac-calorimetry	DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	7		3	1999																												Y123																				91.05					91.05																						144										2.3		HC8825																																																														self-flux method ussing YSZ, annealed at 450C, 72H in 100 bar O2.					Specific heat of a DyBa2Cu3O7-y single crystal in magnetic fields up to T	199908		Department of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, England, UK	Physica C,321(1999)1-11	G. Yang,M.A. Howson,N.J. Garfied,S.Abell		
8826	PRL0813519		Sm(La,Sr)CuOz	Sm1La0.8Sr0.2Cu1O3.95	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4-Z	3.95	1	1998																												T*																						28.8			28.8																																																																																																oxidization by HIP(900C, 50H in 100-400 atm O2)					Double Josephson Plasma Resonance in T* Phase SmLa1-xSrxCuO4-delta	10		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.81(1989)3519	H. Shibata,T. Yamada		
8827	PRL0813519		Sm(La,Sr)CuOz	Sm1La0.8Sr0.2Cu1O3.945	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4-Z	3.945	1	1998																												T*																						26			26																																																																																																oxidization by HIP(900C, 50H in 100-400 atm O2)					Double Josephson Plasma Resonance in T* Phase SmLa1-xSrxCuO4-delta	10		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.81(1989)3519	H. Shibata,T. Yamada		
8828	PRL0813519		Sm(La,Sr)CuOz	Sm1La0.8Sr0.2Cu1O3.94	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4-Z	3.94	1	1998																												T*																						24.6			24.6																																																																																																oxidization by HIP(900C, 50H in 100-400 atm O2)					Double Josephson Plasma Resonance in T* Phase SmLa1-xSrxCuO4-delta	10		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.81(1989)3519	H. Shibata,T. Yamada		
8829	PRL0813519		Sm(La,Sr)CuOz	Sm1La0.8Sr0.2Cu1O3.925	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4-Z	3.925	1	1998																												T*																						19.6			19.6																																																																																																oxidization by HIP(900C, 50H in 100-400 atm O2)					Double Josephson Plasma Resonance in T* Phase SmLa1-xSrxCuO4-delta	10		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.81(1989)3519	H. Shibata,T. Yamada		
8830	ETP1161723	c-axis oriented film. D=5500A,not s/c	(Nd,Ce)2CuO4	Nd1.88Ce0.12Cu1O4-Z	Nd	1.88	Ce	0.12	Cu	1															O	4-Z		5	1999																												T'																							5																							Hall coeflicient																																																		mOhm.cm												1.02													details,see Physica C180(1991)69									Zhurnal experimental'noi I teoreticheskoi fiziki (J.Exp. Th. Ph.) 116(1999)1723	A.I.Ponomarev,A.N.Ignatenkov,G.I.Harus,et al.		
8831	ETP1161723	c-axis oriented film. D=5500A,not s/c	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-Z	Nd	1.85	Ce	0.15	Cu	1															O	4-Z		5	1999																												T'																			20						20																					Hall coeflicient						5.5	1.4																																																							0.424													details,see Physica C180(1991)69									Zhurnal experimental'noi I teoreticheskoi fiziki (J.Exp. Th. Ph.) 116(1999)1723	A.I.Ponomarev,A.N.Ignatenkov,G.I.Harus,et al.		
8832	ETP1161723	c-axis oriented film. D=5000A,not s/c	(Nd,Ce)2CuO4	Nd1.83Ce0.17Cu1O4-Z	Nd	1.83	Ce	0.17	Cu	1															O	4-Z		5	1999																												T'																			12						12																																																																																			0.296													details,see Physica C180(1991)69									Zhurnal experimental'noi I teoreticheskoi fiziki (J.Exp. Th. Ph.) 116(1999)1723	A.I.Ponomarev,A.N.Ignatenkov,G.I.Harus,et al.		
8833	ETP1161723	c-axis oriented film. D=5700A,not s/c	(Nd,Ce)2CuO4	Nd1.82Ce0.18Cu1O4-Z	Nd	1.82	Ce	0.18	Cu	1															O	4-Z		5	1999																												T'																			6						6																					Hall coeflicient						4	1.4																																																							0.235													details,see Physica C180(1991)69									Zhurnal experimental'noi I teoreticheskoi fiziki (J.Exp. Th. Ph.) 116(1999)1723	A.I.Ponomarev,A.N.Ignatenkov,G.I.Harus,et al.		
8834	ETP1161723	c-axis oriented film. D=4000A,not s/c	(Nd,Ce)2CuO4	Nd1.8Ce0.2Cu1O4-Z	Nd	1.8	Ce	0.2	Cu	1															O	4-Z		5	1999																												T'																			1.3						1.3																					Hall coeflicient						2.2	1.4																																																							0.1													details,see Physica C180(1991)69									Zhurnal experimental'noi I teoreticheskoi fiziki (J.Exp. Th. Ph.) 116(1999)1723	A.I.Ponomarev,A.N.Ignatenkov,G.I.Harus,et al.		
8835	PSS0391520		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	Z	6.96	1	1997																											3	Y123				3.815	3.881	11.667													88						88																																																																																																standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8836	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.96	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.822	3.883	11.684													87.5						87.5																																																																						TP8836																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8837	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.96	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.823	3.89	11.67													83						83																																																																						TP8837																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8838	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.96	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.826	3.895	11.674													70						70																																																																						TP8838																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8839	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.96	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.831	3.897	11.666													57						57																																																																						TP8839																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8840	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.96	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.836	3.899	11.667													32						32																																																																						TP8840																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8841	PSS0391520		(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O6.96	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.838	3.908	11.675													12						12																																																																						TP8841																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8842	PSS0391520	not/sc.	(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O6.96	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	Z	6.96	1	1997																											3	Y123				3.846	3.911	11.686																	5																																																																								TP8842																										standard solid state sintering. ANN(450C,2H in O2 flow)-slow cool to RT					Thermopower measurements in (Y,Pr)Ba2Cu3Oz samples with Pr contents 0 - 0.6			Institute of Silicate Chemistry, Saint-Petrsburg, Russia	Fizika tverdogo tela(Phys. Of the Solid State) 39(1997)1520	E.V.VladimirskayaI.B.Patrina,V.E.Gasumyantz		
8843	BMS0210463	O-content by iodometry.	La(Ba,La)2Cu3O7	La1.5Ba1.5Cu3O6.55	La	1.5	Ba	1.5	Cu	3															O	Z	6.55	1	1998																											2	Y123				3.826		11.753	3																5																																																																																																		SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8844	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.4Ba1.5Ca0.1Cu3O6.59	La	1.4	Ba	1.5	Ca	0.1	Cu	3													O	Z	6.59	1	1998																											2	Y123				3.908		11.736	3																5																																																																																																		SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8845	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.35Ba1.5Ca0.15Cu3O6.67	La	1.35	Ba	1.5	Ca	0.15	Cu	3													O	Z	6.67	1	1998																											2	Y123				3.899		11.732	3												43						43																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8846	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.3Ba1.5Ca0.2Cu3O6.72	La	1.3	Ba	1.5	Ca	0.2	Cu	3													O	Z	6.72	1	1998																											2	Y123				3.891		11.726	3												48						48																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8847	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.25Ba1.5Ca0.25Cu3O6.74	La	1.25	Ba	1.5	Ca	0.25	Cu	3													O	Z	6.74	1	1998																											2	Y123				3.888		11.72	3												70						70																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8848	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.65Ba1.5Ca0.35Cu3O6.79	La	1.65	Ba	1.5	Ca	0.35	Cu	3													O	Z	6.79	1	1998																											2	Y123				3.885		11.703	3												72						72																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8849	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.1Ba1.5Ca0.4Cu3O6.82	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O	Z	6.82	1	1998																											2	Y123				3.884		11.693	3												70			72			72																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8850	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1.05Ba1.5Ca0.45Cu3O6.81	La	1.05	Ba	1.5	Ca	0.45	Cu	3													O	Z	6.81	1	1998																											2	Y123				3.881		11.686	3												71			74			74																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8851	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La1Ba1.5Ca0.5Cu3O6.85	La	1	Ba	1.5	Ca	0.5	Cu	3													O	Z	6.85	1	1998																											2	Y123				3.878		11.666	3												74			76			76																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8852	BMS0210463	O-content by iodometry.	La(Ba,La,Ca)2Cu3O7	La0.9Ba1.5Ca0.6Cu3O6.74	La	0.9	Ba	1.5	Ca	0.6	Cu	3													O	Z	6.74	1	1998																											2	Y123				3.899		11.701	3												70			73			73																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8853	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba1.4Ca0.6Cu3O6.9	La	1	Ba	1.4	Ca	0.6	Cu	3													O	Z	6.9	1	1998																											2	Y123				3.874		11.654	3												74				76		74																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8854	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba1.3Ca0.7Cu3O6.92	La	1	Ba	1.3	Ca	0.7	Cu	3													O	Z	6.92	1	1998																											2	Y123				3.867		11.64	3												73				76		73																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8855	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba1.2Ca0.8Cu3O6.95	La	1	Ba	1.2	Ca	0.8	Cu	3													O	Z	6.95	1	1998																											2	Y123				3.863		11.631	3												74				75		74																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8856	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba1.1Ca0.9Cu3O7.02	La	1	Ba	1.1	Ca	0.9	Cu	3													O	Z	7.02	1	1998																											2	Y123				3.858		11.613	3												75				77		75																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8857	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba1Ca1Cu3O6.99	La	1	Ba	1	Ca	1	Cu	3													O	Z	6.99	1	1998																											2	Y123				3.85		11.56	3												75				78		75																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8858	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba0.9Ca1.1Cu3O7.05	La	1	Ba	0.9	Ca	1.1	Cu	3													O	Z	7.05	1	1998																											2	Y123				3.824		11.483	3												71				72		71																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8859	BMS0210463		La(Ba,Ca)2Cu3O7	La1Ba0.8Ca1.2Cu3O7.11	La	1	Ba	0.8	Ca	1.2	Cu	3													O	Z	7.11	1	1998																											2	Y123				3.803		11.419	3												60				66		60																																																																																																SIN(950C,12H in O2)-slow cool to RT-ANN(500C,24H in O2 flow)-slow cool to RT(1C/min)								Saurashira Univ., India	Bul. Mat. Sci. (Indian Acad. Sci.) 21(1998)463	D.G.Kuberkar,N.A.Shah,et al.		
8860	PRL0804293	1*1*0.1mm3	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4+Z	Pr	1.85	Ce	0.15	Cu	1															O	4+Z		3	1998																												T'																				23.2					23.2																				T			10																56		A	calculated from coherence		850																											mOhm.cm							0.4																							General Features of Quantum Creep in High-Tc Superconductors	5		Institute COMPAS and Faculty of Physics and Astronomy, Vrije Universiteit, Amsterdam, The Netherlands	Phys.Rev.Lett.80(1989)4293	A. F. Th. Hoekstra,A. M. Testa,A.F.Th.Hoekstra,A.M. Testa,G. W. Crabtree,J. el Fattahi,K. Westerholt,M. Brinkmann,R. Griessen,W. K. Kwok		
8861	PRL0804293		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4+Z	Pr	1.85	Ce	0.15	Cu	1															O	4+Z			1998																												T'																				12.1					12.1																				T			6																73		A	calculated from coherence		900																											mOhm.cm							0.8																							General Features of Quantum Creep in High-Tc Superconductors	5		Institute COMPAS and Faculty of Physics and Astronomy, Vrije Universiteit, Amsterdam, The Netherlands	Phys.Rev.Lett.80(1989)4293	A. F. Th. Hoekstra,A. M. Testa,A.F.Th.Hoekstra,A.M. Testa,G. W. Crabtree,J. el Fattahi,K. Westerholt,M. Brinkmann,R. Griessen,W. K. Kwok		
8862	PR04510071	G-L=39	YBa2Cu3Oz	Y1Ba2Cu3O6.37	Y	1	Ba	2	Cu	3															O	Z	6.37	3	1992																												Y123																			13.5						13.5																								4												A			91		A			3550																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8863	PR04510071	G-L=36	YBa2Cu3Oz	Y1Ba2Cu3O6.38	Y	1	Ba	2	Cu	3															O	Z	6.38	3	1992																												Y123																			10.1						10.1																								3.9															92					3350																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8864	PR04510071	G-L=49	YBa2Cu3Oz	Y1Ba2Cu3O6.38	Y	1	Ba	2	Cu	3															O	Z	6.38	3	1992																												Y123																			11.3						11.3																								7															69					3360																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8865	PR04510071	G-L=65	YBa2Cu3Oz	Y1Ba2Cu3O6.38	Y	1	Ba	2	Cu	3															O	Z	6.38	3	1992																												Y123																			15.4						15.4																								14															49					3130																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8866	PR04510071	G-L=74	YBa2Cu3Oz	Y1Ba2Cu3O6.38	Y	1	Ba	2	Cu	3															O	Z	6.38	3	1992																												Y123																			17						17																								19															42					3100																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8867	PR04510071	G-L=62	YBa2Cu3Oz	Y1Ba2Cu3O6.43	Y	1	Ba	2	Cu	3															O	Z	6.43	3	1992																												Y123																			35						35																								25															36					2260																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8868	PR04510071	G-L=65	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45	3	1992																												Y123																				31.5					31.5																								40												A			34		A			2260																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8869	PR04510071	G-L=53	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45	3	1992																												Y123																				33.5					33.5																								26												A			36					1920																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8870	PR04510071	G-L=51	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45	3	1992																												Y123																				35.7					35.7																								26															36					1830																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8871	PR04510071	G-L=65	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45	3	1992																												Y123																				39.9					39.9																								28															29					1880																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8872	PR04510071	G-L=64	YBa2Cu3Oz	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	Z	6.52	3	1992																												Y123																				55					55																								39															29					1850																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8873	PR04510071	G-L=67	YBa2Cu3Oz	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	Z	6.52	3	1992																												Y123																				55					55																								40															29					1940																																																				no description 					High anisotropy ans a dimensionality crossover in the irreversibility behavior of oxygen-deficient YBa2Cu3O7-y	199205		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B,45(1992)10071	B.W. Veal,D.E. Farrell,D.H. Kim,G.T. Seidler,K.E. Gray,T.F. Rosenbaum		
8874	PRL0653441	thickness=	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1990																												Y123																				89.9					89.9																																									A	culculated from inductance L	2000																												mOhm.cm											0.33														films were grown epitaxally on LaAlO3 by coevaporation of Cu,Y,BaF2 in O2, ANN(850C in O2)					Metallic and Superconducting Surfaces of YBa2Cu3O7 Probed by Electrostatic Charge Modulation of Epitaxial Films	199012		AT&T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.65(1989)3441	A.F. Hebard,A.T. Fiory,M.L. O'Malley,P.M. Mankiewich,R.E. Howard,R.H. Eick		
8875	PRL0653441	thickness=	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1990																												Y123																				90.1					90.1																																										culculated from inductance L	1800																																							0.27														films were grown epitaxally on LaAlO3 by coevaporation of Cu,Y,BaF2 in O2, ANN(850C in O2)					Metallic and Superconducting Surfaces of YBa2Cu3O7 Probed by Electrostatic Charge Modulation of Epitaxial Films	199012		AT&T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.65(1989)3441	A.F. Hebard,A.T. Fiory,M.L. O'Malley,P.M. Mankiewich,R.E. Howard,R.H. Eick		
8876	PRL0653441	thickness=	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1990																												Y123																				91.4					91.4																																										culculated from inductance L	1800																																							0.194														films were grown epitaxally on LaAlO3 by coevaporation of Cu,Y,BaF2 in O2, ANN(850C in O2)					Metallic and Superconducting Surfaces of YBa2Cu3O7 Probed by Electrostatic Charge Modulation of Epitaxial Films	199012		AT&T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.65(1989)3441	A.F. Hebard,A.T. Fiory,M.L. O'Malley,P.M. Mankiewich,R.E. Howard,R.H. Eick		
8877	PRL0653441	thickness=	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1990																												Y123																				90.2					90.2																																										culculated from inductance L	1700																																							0.27														films were grown epitaxally on LaAlO3 by coevaporation of Cu,Y,BaF2 in O2, ANN(850C in O2)					Metallic and Superconducting Surfaces of YBa2Cu3O7 Probed by Electrostatic Charge Modulation of Epitaxial Films	199012		AT&T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.65(1989)3441	A.F. Hebard,A.T. Fiory,M.L. O'Malley,P.M. Mankiewich,R.E. Howard,R.H. Eick		
8878	PRL0653441	thickness=	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1990																												Y123																				90.2					90.2																																											2500																																							0.418														films were grown epitaxally on LaAlO3 by coevaporation of Cu,Y,BaF2 in O2, ANN(850C in O2)					Metallic and Superconducting Surfaces of YBa2Cu3O7 Probed by Electrostatic Charge Modulation of Epitaxial Films	199012		AT&T Bell Laboratories, Murray Hill, New Jersey 07974	Phys.Rev.Lett.65(1989)3441	A.F. Hebard,A.T. Fiory,M.L. O'Malley,P.M. Mankiewich,R.E. Howard,R.H. Eick		
8879	PRL0620217		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																												Y123																				89.7				0.2	89.7																																									A	suseptibility		1400																																																				See J. Cryst, Growth 85(1987)593					Direct Measurement of the Temperature-Dependent Magnetic Penetration Depth in Y-Ba-Cu-O Crystals	198901		IBM Tomas J. Watson Research center, Yorktown Heights, New York10598-0218	Phys.Rev.Lett.62(1989)217	A.P. Malozemoff,F. Holtzberg,L. Krusin-Elbaum,R.L. Greene,Y. Yeshurun		
8880	PRL0621908		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1989																												Y123																						92.5			92.5																					M(H,T)curve and WHH theory		674	122								10.5	1.9	HC8880					16.4	3																																																								crystals were grown by a partial melting method. J. Cryst. Growth 85(4987)593					Magnetic Measurements of the Upper Critical Field of YBa2Cu3O7-delta Single Crystals	198904		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.Lett.62(1989)1908	G.W. Crabtree,J.Z. Liu,K.G. Vandervoort,U. Welp,W.K. Kwok		
8881	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.9Er0.1Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.9	Er	0.1	Cu	2									O	Z		1	1999																												Pb1212																							5																																																																																																		SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8882	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.7Er0.3Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.7	Er	0.3	Cu	2									O	Z		1	1999																												Pb1212																			56.5						56.5																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8883	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.65Er0.35Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.65	Er	0.35	Cu	2									O	Z		1	1999																												Pb1212																			50.7						50.7																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8884	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.6Er0.6Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.6	Er	0.6	Cu	2									O	Z		1	1999																												Pb1212																			43.8						43.8																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8885	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.5Er0.5Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.5	Er	0.5	Cu	2									O	Z		1	1999																												Pb1212																			22.3						22.3																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8886	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.5V0.5Sr2Ca0.4Er0.6Cu2OZ	Pb	0.5	V	0.5	Sr	2	Ca	0.4	Er	0.6	Cu	2									O	Z		1	1999																												Pb1212																							5																																																																																																		SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8887	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.6V0.4Sr2Ca0.7Er0.3Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.7	Er	0.3	Cu	2									O	Z		1	1999																												Pb1212																			58.8						58.8																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8888	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.6V0.4Sr2Ca0.65Er0.35Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.65	Er	0.35	Cu	2									O	Z		1	1999																											2	Pb1212				3.8097		11.8381													64.1						64.1																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8889	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.6V0.4Sr2Ca0.6Er0.6Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.6	Er	0.6	Cu	2									O	Z		1	1999																											2	Pb1212				3.8079		11.8316													62						62																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8890	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.6V0.4Sr2Ca0.5Er0.5Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.5	Er	0.5	Cu	2									O	Z		1	1999																												Pb1212																			38.4						38.4																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8891	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.7V0.3Sr2Ca0.7Er0.3Cu2OZ	Pb	0.7	V	0.3	Sr	2	Ca	0.7	Er	0.3	Cu	2									O	Z		1	1999																												Pb1212																			58.8						58.8																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8892	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.7V0.3Sr2Ca0.65Er0.35Cu2OZ	Pb	0.7	V	0.3	Sr	2	Ca	0.65	Er	0.35	Cu	2									O	Z		1	1999																												Pb1212																			58.1						58.1																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8893	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.7V0.3Sr2Ca0.6Er0.4Cu2OZ	Pb	0.7	V	0.3	Sr	2	Ca	0.6	Er	0.4	Cu	2									O	Z		1	1999																												Pb1212																			58.8						58.8																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8894	PHC3210183		(Pb,V)Sr2(Ca,Er)Cu2Oz	Pb0.7V0.3Sr2Ca0.5Er0.5Cu2OZ	Pb	0.7	V	0.3	Sr	2	Ca	0.5	Er	0.5	Cu	2									O	Z		1	1999																												Pb1212																			16.6						16.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8895	PHC3210183		(Pb,V)Sr2(Ca,Lu)Cu2Oz	Pb0.6V0.4Sr2Ca0.65Lu0.35Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.65	Lu	0.35	Cu	2									O	Z		1	1999																											2	Pb1212				3.8035		11.8239													63.6						63.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8896	PHC3210183		(Pb,V)Sr2(Ca,Dy)Cu2Oz	Pb0.6V0.4Sr2Ca0.65Dy0.35Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.65	Dy	0.35	Cu	2									O	Z		1	1999																											2	Pb1212				3.8079		11.8406													56.6						56.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8897	PHC3210183		(Pb,V)Sr2(Ca,Gd)Cu2Oz	Pb0.6V0.4Sr2Ca0.65Gd0.35Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.65	Gd	0.35	Cu	2									O	Z		1	1999																											2	Pb1212				3.8267		11.8619													36.6						36.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8898	PHC3210183		(Pb,V)Sr2(Ca,Sm)Cu2Oz	Pb0.6V0.4Sr2Ca0.65Sm0.35Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.65	Sm	0.35	Cu	2									O	Z		1	1999																											2	Pb1212				3.8311		11.8768													25.5						25.5																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8899	PHC3210183		(Pb,V)Sr2(Ca,Lu)Cu2Oz	Pb0.6V0.4Sr2Ca0.6Lu0.4Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.6	Lu	0.4	Cu	2									O	Z		1	1999																											2	Pb1212				3.8009		11.8187													62.6						62.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8900	PHC3210183		(Pb,V)Sr2(Ca,Dy)Cu2Oz	Pb0.6V0.4Sr2Ca0.6Dy0.4Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.6	Dy	0.4	Cu	2									O	Z		1	1999																											2	Pb1212				3.8167		11.8484													53.6						53.6																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8901	PHC3210183		(Pb,V)Sr2(Ca,Gd)Cu2Oz	Pb0.6V0.4Sr2Ca0.6Gd0.4Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.6	Gd	0.4	Cu	2									O	Z		1	1999																											2	Pb1212				3.8299		11.8768													33.1						33.1																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8902	PHC3210183		(Pb,V)Sr2(Ca,Sm)Cu2Oz	Pb0.6V0.4Sr2Ca0.6Sm0.4Cu2OZ	Pb	0.6	V	0.4	Sr	2	Ca	0.6	Sm	0.4	Cu	2									O	Z		1	1999																											2	Pb1212				3.8311		11.8858													20.5						20.5																																																																																																SIN(995-997C,4H in flowing O2)-ANN(800C,12H in O2)-Q to LN2					Ion size effect on Tc in (Pb,V)Sr2(Ca,R)Cu2Oz(R=Sm, Gd, Dy, Er and Lu) systems	199908		Department of Physics, Kangwon National University Chunchon 200-701, South Korea	Physica C,321(1999)183-190	H.K. Lee,T.Y. Kim		
8903	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2Cu3O7	Ca0.1La0.9Ba1.65La0.35Cu3O7.15	Ca	0.1	La	0.9	Ba	1.65	La	0.35	Cu	3											O	Z	7.15		1999																												Y123																			57						57	TC8903																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8904	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2Cu3O7	Ca0.2La0.8Ba1.55La0.45Cu3O7.16	Ca	0.2	La	0.8	Ba	1.55	La	0.45	Cu	3											O	Z	7.16		1999																												Y123																			68						68	TC8904																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8905	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2Cu3O7	Ca0.3La0.7Ba1.45La0.55Cu3O7.16	Ca	0.3	La	0.7	Ba	1.45	La	0.55	Cu	3											O	Z	7.16		1999																												Y123																			76						76	TC8905																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8906	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2Cu3O7	Ca0.4La0.6Ba1.35La0.65Cu3O7.15	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	3											O	Z	7.15		1999																												Y123																			80						80	TC8906																																																																		5.91			TP8906																									1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8907	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2(Cu,Ni)3Oz	Ca0.4La0.6Ba1.35La0.65Cu2.955Ni0.045OZ	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	2.955	Ni	0.045									O	Z			1999																																															71.3						71.3	TC8907																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8908	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2(Cu,Ni)3Oz	Ca0.4La0.6Ba1.35La0.65Cu2.925Ni0.075OZ	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	2.925	Ni	0.075									O	Z			1999																																															63.8						63.8	TC8908																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8909	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2(Cu,Ni)3Oz	Ca0.4La0.6Ba1.35La0.65Cu2.85Ni0.15OZ	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	2.85	Ni	0.15									O	Z			1999																																															45.7						45.7	TC8909																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8910	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2(Cu,Ni)3Oz	Ca0.4La0.6Ba1.35La0.65Cu2.76Ni0.24OZ	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	2.76	Ni	0.24									O	Z			1999																																															23.6						23.6	TC8910																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8911	PHC3210199	Tc(z) is shown in TCFIG,T1 value is Tc(max)	(Ca,La)(Ba,La)2(Cu,Ni)3Oz	Ca0.4La0.6Ba1.35La0.65Cu2.7Ni0.3OZ	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	2.7	Ni	0.3									O	Z			1999																																															16.5						16.5	TC8911																																																																																														1	See Phys.Rev.B,48(1993)532					Transport measurements in the 1-2-3 system CLBLCO in both the oxygen-underdoped and-overdoped regions	199908		Department of Physics and Crown Center for Superconductivity, Technion, Israel Institute of Technology, 32000 Haifa, Israel	Physica C,321(1999)199-206	A. Knizhnik,C.G. Kuper,D. Goldschmidt,G.M. Reisner,Y. Direktovich,Y. Eckstein		
8912	PHC3220009		(Hg,Cr)Sr2Ca1Cu2Oz	Hg0.7Cr0.3Sr2Ca1Cu2OZ	Hg	0.7	Cr	0.3	Sr	2	Ca	1	Cu	2											O	Z			1999																												Hg1212				3.8451		11.9355																80			80																																																																																																high pressure synthesis (1000C,6GPa)					Synthesis of superconducting (Hg0.7Cr0.3)Sr2Can-1CunOy(n=2-5) using high-pressure technique	199909		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physica C,322(1999)9-18	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8913	PHC3220009		(Hg,Cr)Sr2Ca2Cu3Oz	Hg0.7Cr0.3Sr2Ca2Cu3OZ	Hg	0.7	Cr	0.3	Sr	2	Ca	2	Cu	3											O	Z			1999																												Hg1223				3.8494		15.1613																98			98																																																																																																high pressure synthesis (1000C,6GPa)					Synthesis of superconducting (Hg0.7Cr0.3)Sr2Can-1CunOy(n=2-5) using high-pressure technique	199909		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physica C,322(1999)9-18	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8914	PHC3220009		(Hg,Cr)Sr2Ca3Cu4Oz	Hg0.7Cr0.3Sr2Ca3Cu4OZ	Hg	0.7	Cr	0.3	Sr	2	Ca	3	Cu	4											O	Z			1999																												Hg1234				3.8583		18.2258																64			64																																																																																																high pressure synthesis (1000C,6GPa)					Synthesis of superconducting (Hg0.7Cr0.3)Sr2Can-1CunOy(n=2-5) using high-pressure technique	199909		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physica C,322(1999)9-18	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8915	PHC3220009		(Hg,Cr)Sr2Ca4Cu5Oz	Hg0.7Cr0.3Sr2Ca4Cu5OZ	Hg	0.7	Cr	0.3	Sr	2	Ca	4	Cu	5											O	Z			1999																												Hg1245				3.861		21.2903																45			45																																																																																																high pressure synthesis (1000C,6GPa)					Synthesis of superconducting (Hg0.7Cr0.3)Sr2Can-1CunOy(n=2-5) using high-pressure technique	199909		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Physica C,322(1999)9-18	E. Kandyel,S. Adachi,S. Tajima,X.-J. Wu		
8916	PHC3160069		(Cu,Cr)Sr2Ca1Cu2Oz	Cu2.5Cr0.5Sr2Ca1OZ	Cu	2.5	Cr	0.5	Sr	2	Ca	1													O	Z			1999																												Cu1212																																																											HIR8916																																																														See Physica C 302(1998)244					Critical current densities of high-Tc superconductors (Cu,Cr)Sr2Can-1CunO2n+3(n=2,3) prepared under high pressure	199905		National Institute for Research in Inorganic Materials, Namiki 1-1, Tsukuba, Ibaraki, 305-0044 Japan	Physica C,316(1999)69-76	E. Takayama-Muromachi,S. Yu,S.M. Loureiro		
8917	PHC3160069		(Cu,Cr)Sr2Ca2Cu3Oz	Cu3.5Cr0.5Sr2Ca2OZ	Cu	3.5	Cr	0.5	Sr	2	Ca	2													O	Z			1999																												Cu1223																																																											HIR8917																																																														See Physica C 302(1998)244					Critical current densities of high-Tc superconductors (Cu,Cr)Sr2Can-1CunO2n+3(n=2,3) prepared under high pressure	199905		National Institute for Research in Inorganic Materials, Namiki 1-1, Tsukuba, Ibaraki, 305-0044 Japan	Physica C,316(1999)69-76	E. Takayama-Muromachi,S. Yu,S.M. Loureiro		
8918	PHC3240015	O-content=nominel	TlSr2Ca2Cu3Oz	Tl1Sr2Ca2Cu3O9.4	Tl	1	Sr	2	Ca	2	Cu	3													O	Z	9.4	1	1999																											2	Tl1223				3.813		15.24																86			86																																		HIR8918																																	-0.56			TP8918																								Tl2O3, SrO2, CaO, CuO, Cu		high pressure synthesis (1100C,4H,6GPa) in Au capsule					Synthesis and characterization of asingle-phase TlSr2Ca2Cu3Oy	19910		Superconductivity Research Laboratory, ISTC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C,324(1999)15-20	K. Tanabe,S. Adachi,S. Fujihara,T. Kimura,T. Shibata,T. Tamura,T. Tatsuki		
8919	PHC3240133		YBa2Cu3O7	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123						11.6922														90.7					90.7																																																																																																using Au2O3 for Au    					Miscibility of Au and Cu in superconducting YBa2(Cu1-xAu)O7-delta for 0< x <0.15	199911		Physics Department , Purdue University, West Lafayette, IN 47907-1396, USA	Physica C,324(1999)133-136	B.M. Fetrow,C.L. Smiley,C.T. Bird,E. Dedrick,J.J. LaBelle,J.L. Calvin,J.M. Wegner,K.W. Holman,M.H. Davies,R.J. Hill,S.M. Durbin,S.M. Herman		
8920	PHC3240133		YBa2(Cu,Au)3O7	Y1Ba2Cu2.85Au0.15OZ	Y	1	Ba	2	Cu	2.85	Au	0.15													O	Z		1	1999																												Y123						11.7552														92.3					92.3																																																																																																using Au2O3 for Au    					Miscibility of Au and Cu in superconducting YBa2(Cu1-xAu)O7-delta for 0< x <0.15	199911		Physics Department , Purdue University, West Lafayette, IN 47907-1396, USA	Physica C,324(1999)133-136	B.M. Fetrow,C.L. Smiley,C.T. Bird,E. Dedrick,J.J. LaBelle,J.L. Calvin,J.M. Wegner,K.W. Holman,M.H. Davies,R.J. Hill,S.M. Durbin,S.M. Herman		
8921	PHC3240133		YBa2(Cu,Au)3O7	Y1Ba2Cu2.7Au0.3OZ	Y	1	Ba	2	Cu	2.7	Au	0.3													O	Z		1	1999																												Y123						11.7734													84.2	87.8	91				87.8																																																																																																using Au2O3 for Au    					Miscibility of Au and Cu in superconducting YBa2(Cu1-xAu)O7-delta for 0< x <0.15	199911		Physics Department , Purdue University, West Lafayette, IN 47907-1396, USA	Physica C,324(1999)133-136	B.M. Fetrow,C.L. Smiley,C.T. Bird,E. Dedrick,J.J. LaBelle,J.L. Calvin,J.M. Wegner,K.W. Holman,M.H. Davies,R.J. Hill,S.M. Durbin,S.M. Herman		
8922	PHC3240133		YBa2(Cu,Au)3O7	Y1Ba2Cu2.55Au0.45OZ	Y	1	Ba	2	Cu	2.55	Au	0.45													O	Z		1	1999																												Y123						11.8339													68.7	71.8	75				71.8																																																																																																using Au2O3 for Au    					Miscibility of Au and Cu in superconducting YBa2(Cu1-xAu)O7-delta for 0< x <0.15	199911		Physics Department , Purdue University, West Lafayette, IN 47907-1396, USA	Physica C,324(1999)133-136	B.M. Fetrow,C.L. Smiley,C.T. Bird,E. Dedrick,J.J. LaBelle,J.L. Calvin,J.M. Wegner,K.W. Holman,M.H. Davies,R.J. Hill,S.M. Durbin,S.M. Herman		
8923	PHC3240193	nominal 0 % Mn	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z			1999																												Bi2212						30.8258													83.7						83.7																																																																																																self-flux method					Growth of superconducting Bi2Sr2Ca(Cu1-xMn)2Oy single crystals	199911		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's republic of China	Physica C,324(1999)193-197	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
8924	PHC3240193	nominal 1 % Mn	Bi2Sr2Ca(Cu,Mn)2Oz	Bi2Sr2Ca1Cu1.54Au0.46OZ	Bi	2	Sr	2	Ca	1	Cu	1.54	Au	0.46											O	Z			1999																												Bi2212						30.7887													74.7						74.7																																																																																																self-flux method					Growth of superconducting Bi2Sr2Ca(Cu1-xMn)2Oy single crystals	199911		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's republic of China	Physica C,324(1999)193-197	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
8925	PHC3240193	nominal 2 % Mn	Bi2Sr2Ca(Cu,Mn)2Oz	Bi2Sr2Ca1Cu1.2Au0.8OZ	Bi	2	Sr	2	Ca	1	Cu	1.2	Au	0.8											O	Z			1999																												Bi2212						30.7793													73.2						73.2																																																																																																self-flux method					Growth of superconducting Bi2Sr2Ca(Cu1-xMn)2Oy single crystals	199911		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's republic of China	Physica C,324(1999)193-197	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
8926	PHC3240193	nominal 5 % Mn	Bi2Sr2Ca(Cu,Mn)2Oz	Bi2Sr2Ca1Cu0.2Au1.8OZ	Bi	2	Sr	2	Ca	1	Cu	0.2	Au	1.8											O	Z			1999																												Bi2212						30.7749													70.1						70.1																																																																																																self-flux method					Growth of superconducting Bi2Sr2Ca(Cu1-xMn)2Oy single crystals	199911		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's republic of China	Physica C,324(1999)193-197	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
8927	PHC3240193	nominal 8 % Mn	Bi2Sr2Ca(Cu,Mn)2Oz	Bi2Sr2Ca1Cu-1.7Au3.7OZ	Bi	2	Sr	2	Ca	1	Cu	-1.7	Au	3.7											O	Z			1999																												Bi2212						30.7716													63						63																																																																																																self-flux method					Growth of superconducting Bi2Sr2Ca(Cu1-xMn)2Oy single crystals	199911		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's republic of China	Physica C,324(1999)193-197	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
8928	PHC3250153		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212						3.0914																85.6			85.6																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8929	PHC3250153		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.975La0.025Cu2O8+Z	Bi	2	Sr	2	Ca	0.975	La	0.025	Cu	2											O	8+Z		3	1999																												Bi2212						3.0818																73.5			73.5																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8930	PHC3250153		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.95La0.05Cu2O8+Z	Bi	2	Sr	2	Ca	0.95	La	0.05	Cu	2											O	8+Z		3	1999																												Bi2212						3.686																64.4			64.4																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8931	PHC3250153		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.925La0.075Cu2O8+Z	Bi	2	Sr	2	Ca	0.925	La	0.075	Cu	2											O	8+Z		3	1999																												Bi2212						3.641																57.6			57.6																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8932	PHC3250153		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.8La0.2Cu2O8+Z	Bi	2	Sr	2	Ca	0.8	La	0.2	Cu	2											O	8+Z		3	1999																												Bi2212						3.0586																29.6			29.6																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8933	PHC3250153		Bi2Sr2(Ca,La)Cu2O8	Bi2Sr2Ca0.75La0.25Cu2O8+Z	Bi	2	Sr	2	Ca	0.75	La	0.25	Cu	2											O	8+Z		3	1999																												Bi2212						3.568																17.4			17.4																																																																																																self-flux method, Bi2Sr2(Ca,La)Cu2O8+z +20.2Bi2O3					Effect of La-doping on growth and superconductivity of Bi-2212 crystals	199911		Institut fur Angewandte Physik, Universitat Hamburg, Jungiustrasse 11, 20355 Humburg, Germany	Physica C,325(1999)153-158	H. Jin,J. Kotzler		
8934	PHC3250041	as-prepared sample. O-content by structural analysis.	(Hg,Mo)Ba2CuOz	Hg0.75Mo0.25Ba2Cu1O4.59	Hg	0.75	Mo	0.25	Ba	2	Cu	1													O	4+Z	4.59	1	1999																											2	Hg1201				3.883		9.3547												K				12			12																																																																																																precursor(Mo-Ba-Cu-O)+HgO					Synthesis, structure and superconductivity of Hg0.75Mo0.25Ba2CuO4+delta	199911		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, 43010 Fantanini, Parma, Italy	Physica C,325(1999)41-48	A. Santoro,C. Bougerol-Chaillout,F. Licci,M. Marezio,Q. Huang,R. Masini		
8935	PHC3250041	annealed sample. O-content by structural analysis.	(Hg,Mo)Ba2CuOz	Hg0.75Mo0.25Ba2Cu1O4.51	Hg	0.75	Mo	0.25	Ba	2	Cu	1													O	4+Z	4.51	1	1999																											2	Hg1201				3.8875		9.3592												K				40			40																																																																																																as-grown sample-ANN(350C, in Ar)					Synthesis, structure and superconductivity of Hg0.75Mo0.25Ba2CuO4+delta	199911		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, 43010 Fantanini, Parma, Italy	Physica C,325(1999)41-48	A. Santoro,C. Bougerol-Chaillout,F. Licci,M. Marezio,Q. Huang,R. Masini		
8936	EPL0450387	two-leg ladder. incommensulate structure. [A2Cu2O3]m[CuO2]n, (m,n) = (5,7)	(Sr,Ca,Bi,Y,Pb)10Cu17O29	Sr3.1Ca5.9Bi0.4Y0.3Pb0.3Cu16.7O29	Sr	3.1	Ca	5.9	Bi	0.4	Y	0.3	Pb	0.3	Cu	16.7									O	29		3	1999																												LAD				11.316	12.763	19.491															80	80		1	80																																				A				45	micron m				0.7																																																			self-flux method, heat(1100C)-cool to 900C(1C/h) needle-like samples were grown					Superconductivity in two-leg spin ladders[A2Cu2O3]5[CuO2]7 (A=Sr,Ca,Bi,Y,Pb)			Moscow State University-119899 Moscow, Russia	Europhys.Lett.45(1999)387-392	A. REZA,G.-J. BABONAS,H. SZYMCZAK,L. LEONYUK,L. SHAVANSKAYA,M. BARAN,R. SZYMCZAK,V. MALTSEV,V. RYBAKOV		
8937	EPL0460787	twinned crystal, Lindemann constant=0.16	NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z		3	1999																												Y123																				95.65					95.65																				T			287						T/K			3		HIR8937	resistance kink (1st order)																																																													melt-process, atmosphere=0.03% O2+Ar during growth 					Flux lattice melting in twinned NdBa2Cu3O7-y single crystals			Superconductivity Research Laboratory, ISTEC,10-13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Europhys.Lett.46(1999)787-793	A.K. PRADHAN,K. NAKAO,N. KOSHIZUKA,S. SHIBATA		
8938	PRL0722263	anisotropy factor=24.6 	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	1994																												T																				27.9					27.9																																									um	surface impedance 		0.75	17.4																																																			details of sample preparation are not described					Anisotropic Penetration Depth in La2-xSrxCuO4	199404		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ko,Tokyo 113,Japan	Phys.Rev.Lett.,72(1994)2263	A.Maeda,H.Kitano,K.Kishino,K.Uchinokura,T.Kimura,T.Shibauchi		
8939	PRL0722263	anisotropy factor=21. 	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		3	1994																												T																				32					32																																									um	surface impedance 		0.54	11																																																			details of sample preparation are not described					Anisotropic Penetration Depth in La2-xSrxCuO4	199404		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ko,Tokyo 113,Japan	Phys.Rev.Lett.,72(1994)2263	A.Maeda,H.Kitano,K.Kishino,K.Uchinokura,T.Kimura,T.Shibauchi		
8940	PRL0722263	anisotropy factor=14 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1994																												T																				35.1					35.1																																									um	surface impedance 		0.41	5.5																																																			details of sample preparation are not described					Anisotropic Penetration Depth in La2-xSrxCuO4	199404		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ko,Tokyo 113,Japan	Phys.Rev.Lett.,72(1994)2263	A.Maeda,H.Kitano,K.Kishino,K.Uchinokura,T.Kimura,T.Shibauchi		
8941	PRL0722263	anisotropy factor=12.1. 	(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4		3	1994																												T																				32.2					32.2																																									um	surface impedance 		0.17	2.03																																																			details of sample preparation are not described					Anisotropic Penetration Depth in La2-xSrxCuO4	199404		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ko,Tokyo 113,Japan	Phys.Rev.Lett.,72(1994)2263	A.Maeda,H.Kitano,K.Kishino,K.Uchinokura,T.Kimura,T.Shibauchi		
8942	PRL0722263	anisotropy factor=11.5. 	(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4		3	1994																												T																				29.1					29.1																																									um	surface impedance 		0.26	2.96																																																			details of sample preparation are not described					Anisotropic Penetration Depth in La2-xSrxCuO4	199404		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ko,Tokyo 113,Japan	Phys.Rev.Lett.,72(1994)2263	A.Maeda,H.Kitano,K.Kishino,K.Uchinokura,T.Kimura,T.Shibauchi		
8943	JSC1420205		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1999																												Bi2212																																																																																															TP8943																										conventional solid state reaction					Anomalous Thermoelectric Power Behaviors of lodine Intercalated (Bi,Pb)2Sr2Can-1CunO2n+4+delta Superconductors (n=2 and 3)			Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	J.Solid State Chem.142(1999)199-205	J.-H. Choy,S.-J. Hwang,W. Lee		
8944	JSC1420205	I-concentration unknown. Tc estimated from TPFIG	IBi2Sr2CaCu2O8	I1Bi2Sr2Ca1Cu2O8	I	1	Bi	2	Sr	2	Ca	1	Cu	2											O	8			1999																												Bi2212																																																																																															TP8944																										prestine and iodine were sealed and heat at 180C for 1h.					Anomalous Thermoelectric Power Behaviors of lodine Intercalated (Bi,Pb)2Sr2Can-1CunO2n+4+delta Superconductors (n=2 and 3)			Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	J.Solid State Chem.142(1999)199-205	J.-H. Choy,S.-J. Hwang,W. Lee		
8945	JSC1420205	Pb-concentration unknown. Tc estimated from TPFIG	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.7Pb0.3Sr2Ca2Cu3OZ	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	Z			1999																												Bi2223																																																																																															TP8945																										conventional solid state reaction					Anomalous Thermoelectric Power Behaviors of lodine Intercalated (Bi,Pb)2Sr2Can-1CunO2n+4+delta Superconductors (n=2 and 3)			Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	J.Solid State Chem.142(1999)199-205	J.-H. Choy,S.-J. Hwang,W. Lee		
8946	JSC1420205	Pb- and I-concentrations unknown. Tc estimated from TPFIG	I(Bi,Pb)2Sr2Ca2Cu3Oz	I1Bi1.7Pb0.3Sr2Ca2Cu3OZ	I	1	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3									O	Z			1999																												Bi2223																																																																																															TP8946																										prestine and iodine were sealed and heat at 150C for 10h.					Anomalous Thermoelectric Power Behaviors of lodine Intercalated (Bi,Pb)2Sr2Can-1CunO2n+4+delta Superconductors (n=2 and 3)			Department of Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	J.Solid State Chem.142(1999)199-205	J.-H. Choy,S.-J. Hwang,W. Lee		
8947	JAP0858299		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212				5.41		30.88																80			80											mT	Tochihara analysis		3.7	0.1																																																																																	self flux method.					Lower critical fields of Bi2Sr2CaCu2O8+d and YBa2Cu3O7-d single crystals	199906		Dpartment of Mathematics and Physics, National Defense Academy, Yokosuka 239-8686, Japan	J.Apple.Phys.85(1999)8299	H. Mazaki,H.Yasuoka,M. Kakihana,M. Osada,S. Tchihara		
8948	JAP0858299		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		3	1999																												Y123				3.81	3.88	11.67																89			89											mT	Tochihara analysis		18	2.7																																																																																	self flux method.					Lower critical fields of Bi2Sr2CaCu2O8+d and YBa2Cu3O7-d single crystals	199906		Dpartment of Mathematics and Physics, National Defense Academy, Yokosuka 239-8686, Japan	J.Apple.Phys.85(1999)8299	H. Mazaki,H.Yasuoka,M. Kakihana,M. Osada,S. Tchihara		
8949	JMR0140334	not s/c	GdBa4Cu3O8.5	Gd1Ba4Cu3O8.5+Z	Gd	1	Ba	4	Cu	3															O	8.5+Z		1	1999																												Y143				8.16528																			5																																																																																																		R:Ba:Cu=1:4:3, SIN(950C,24H in O2 flow)					Synthesis and crystal chemistry of the new compounds GdBa4Cu3O8.5+delta and DyBa4Cu3O8.5+delta	199902		Mail Stop K763, Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, new Mexico 87545	J.Mater.Les.14(1999)334	D.E. Peterson,E.J. Peterson,F.M. Muller,J.Y. Coulter,P.S. Baldonado,Y.T.  Zhu		
8950	JMR0140334	not s/c	DyBa4Cu3O8.5	Dy1Ba4Cu3O8.5+Z	Dy	1	Ba	4	Cu	3															O	8.5+Z		1	1999																												Y143				8.1081																			5																																																																																																		R:Ba:Cu=1:4:3, SIN(950C,24H in O2 flow)					Synthesis and crystal chemistry of the new compounds GdBa4Cu3O8.5+delta and DyBa4Cu3O8.5+delta	199902		Mail Stop K763, Materials Science and Technology Division, Los Alamos National Laboratory, Los Alamos, new Mexico 87545	J.Mater.Les.14(1999)334	D.E. Peterson,E.J. Peterson,F.M. Muller,J.Y. Coulter,P.S. Baldonado,Y.T.  Zhu		
8951	JSC1430277	size=0.25*0.18*0.02 mm3	(Hg,Re)Ba2Ca5Cu6Oz	Hg0.75Re0.22Ba2Ca5Cu6OZ	Hg	0.75	Re	0.22	Ba	2	Ca	5	Cu	6											O	Z		3	1999									5.721																			Hg1256				3.8542		25.162																100			100																																																																																																gas-phase high-pressure technique					Structure and Properties of 1256 and 1267 Type Hg1-xRexBa2Can-1CunO2n+2+4x+delta Single Crystals			Laboratorium fur Festkorperphysik, ETH Honggerberg, 8093 Zurich, Swizerland	J.Solid State Chem.143(1999)277-284	E.M. Kopnin,G.I. Meijer,H. Schwer,J. Karpinski,R. Molinski		
8952	JSC1430277	not twinned	(Hg,Re)Ba2Ca6Cu7Oz	Hg0.75Re0.22Ba2Ca6Cu7OZ	Hg	0.75	Re	0.22	Ba	2	Ca	6	Cu	7											O	Z		3	1999																												Hg1267				3.8514		28.388																84			84																																																																																																gas-phase high-pressure technique					Structure and Properties of 1256 and 1267 Type Hg1-xRexBa2Can-1CunO2n+2+4x+delta Single Crystals			Laboratorium fur Festkorperphysik, ETH Honggerberg, 8093 Zurich, Swizerland	J.Solid State Chem.143(1999)277-284	E.M. Kopnin,G.I. Meijer,H. Schwer,J. Karpinski,R. Molinski		
8953	JSC1440405		(Sr,K)2Bi2O7	Sr1.6K1.4Bi2O7	Sr	1.6	K	1.4	Bi	2															O	7			1999																											2		I4/mmm			4.1549		21.8273																	1.5																																																																																																		high O2-pressure technique. mixture of (Sr2Bi2O5,KO2,Bi2O3)-heat(300-450C, 20H, 40-80bar O2)					A New Layered Bismuthate (Sr,K)3Bi2O7: Synthesis and Crystal Structure			Department of Chemistry, Moscow State University, Moscow 119899, Russia	J.Solid State Chem.144(1999)405-408	C. Bougerol-Chaillout,E.V. Antipov,J.J. Capponi,J.S. Pshirkov,P. Bordet,S.M. Kazakov,S.N. Putilin		
8954	PHC2650171		(La,Ca)2CaCu2O6	La1.85Nd0Ca1.15Cu2O5.99	La	1.85	Nd	0	Ca	1.15	Cu	2													O	6-Z	5.99	1	1996																											2	2126				3.823		19.419												K	20	23	25				23																																																																																															1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8955	PHC2650171		(La,Nd,Ca)2CaCu2O6	La1.8Nd0.05Ca1.15Cu2O6-Z	La	1.8	Nd	0.05	Ca	1.15	Cu	2													O	6-Z		1	1996																											2	2126				3.822		19.405												K	15	19	23				19																																																																																															1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8956	PHC2650171		(La,Nd,Ca)2CaCu2O6	La1.75Nd0.1Ca1.15Cu2O6-Z	La	1.75	Nd	0.1	Ca	1.15	Cu	2													O	6-Z		1	1996																											2	2126				3.824		19.4												K	12	15	19				15																																																																																															1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8957	PHC2650171		(La,Nd,Ca)2CaCu2O6	La1.7Nd0.15Ca1.15Cu2O6-Z	La	1.7	Nd	0.15	Ca	1.15	Cu	2													O	6-Z		1	1996																											2	2126				3.822		19.396												K	8	11	14				11																																																																																															1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8958	PHC2650171		(La,Nd,Ca)2CaCu2O6	La1.65Nd0.2Ca1.15Cu2O5.99	La	1.65	Nd	0.2	Ca	1.15	Cu	2													O	6-Z	5.99	1	1996																											2	2126				3.824		19.382												K		5	9				5																																																																																															1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8959	PHC2650171		(La,Nd,Ca)2CaCu2O6	La1.45Nd0.4Ca1.15Cu2O5.98	La	1.45	Nd	0.4	Ca	1.15	Cu	2													O	6-Z	5.98	1	1996																											2	2126				3.823		19.347												K					4.2																																																																																																	1	SIN (1080C,12H in O2 flow)-ANN (1100C, 50H in 30 atm O2)					Temperature dependence of Hall angle in superconducting La1.85-xNdxCa1.15Cu2O6-z	07		Department o Inorganic Materials,Fculty of Engineering,Tokyo Institute of Technology,2-12-1 O-okayama,Meguro.Tokyo 152, Japan	Physica.C,265(1996)171-177	Junzo Tanaka,Minoru Takemoto,Naoki Ohashi,Osamu Fukunaga,Takaaki Tsurumi	La, Nd, Ca, Cu, O	
8960	JSC1350017	F-content is described as 2tz, but not measured.	Sr2Cu(O2F2)	Sr2Cu1F2O2	Sr	2	Cu	1	F	2															O	2		1	1998																												T																		K				46			46																																																																																																fluori nation (using metal difluoride)					Superconducting Sr2-xAxCuO2F2+delta(A=Ca,Ba): Synthetic Pathways and Associated Structural Rearrangements			School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom; and  School of Physics and Space Research, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom	J.Solid State Chem.135(1998)17-27	C. Greaves,J.P. Hodges,M. Al-Mamouri,M. Al-Manouri,M. Slaski,M.G. Francesconi,P.P. Edwards,P.R. Slater		
8961	JSC1350017	F-content is described as 2tz, but not measured.	(Sr,Ba)2Cu(O2,F2)	Sr1.4Ba0.6Cu1F2O2	Sr	1.4	Ba	0.6	Cu	1	F	2													O	2		1	1998																												T																						64			64																																																																																																fluori nation (using metal difluoride)					Superconducting Sr2-xAxCuO2F2+delta(A=Ca,Ba): Synthetic Pathways and Associated Structural Rearrangements			School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom; and  School of Physics and Space Research, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kingdom	J.Solid State Chem.135(1998)17-27	C. Greaves,J.P. Hodges,M. Al-Mamouri,M. Al-Manouri,M. Slaski,M.G. Francesconi,P.P. Edwards,P.R. Slater		
8962	PHC2170287	impuriy= (Ba,Sr)2CuO3	TlSr2(Sr,Ba)2Cu2(CO3)Oz	Tl1Sr3Ba1Cu2Co3OZ	Tl	1	Sr	3	Ba	1	Cu	2	Co	3											O	Z		1	1993																												Tl1223																			44	52.2					52.2																																																																																														Tl2O3, Sr2CuO2(CO3), BaO2, CuO		mixture-SIN( 930-950C, 0.5H in gas flow(99% O2+1% CO2) -Q to RT.					Incommensurate and commensurate superstructures in the oxycarbonate superconductor TlSr4-xBaxCu2(CO3)Oy (y=2)	199311		National Institute for Research in Inorganic Materials,Tsukuba,Japan	Physica C, 217(1993)287	H.Nakata,J.Akimitsu,M.Ogawa,M.Uehara,Y.Matsui	Tl,Sr,Ba,Cu,C,O	
8963	PHC2170287	impuriy= (Ba,Sr)2CuO3	TlSr2(Sr,Ba)2Cu2(CO3)Oz	Tl1Sr2.5Ba1.5Cu2Co3OZ	Tl	1	Sr	2.5	Ba	1.5	Cu	2	Co	3											O	Z		1	1993																												Tl1223																			59	64					64																																																																																														Tl2O3, Sr2CuO2(CO3), BaO2, CuO		mixture-SIN( 930-950C, 0.5H in gas flow(99% O2+1% CO2) -Q to RT.					Incommensurate and commensurate superstructures in the oxycarbonate superconductor TlSr4-xBaxCu2(CO3)Oy (y=2)	199311		National Institute for Research in Inorganic Materials,Tsukuba,Japan	Physica C, 217(1993)287	H.Nakata,J.Akimitsu,M.Ogawa,M.Uehara,Y.Matsui	Tl,Sr,Ba,Cu,C,O	
8964	PHC2170287	impuriy= (Ba,Sr)2CuO3	TlSr2(Sr,Ba)2Cu2(CO3)Oz	Tl1Sr2Ba2Cu2Co3OZ	Tl	1	Sr	2	Ba	2	Cu	2	Co	3											O	Z		1	1993																												Tl1223																			67.4	69	73				69																																																																																														Tl2O3, Sr2CuO2(CO3), BaO2, CuO		mixture-SIN( 930-950C, 0.5H in gas flow(99% O2+1% CO2) -Q to RT.					Incommensurate and commensurate superstructures in the oxycarbonate superconductor TlSr4-xBaxCu2(CO3)Oy (y=2)	199311		National Institute for Research in Inorganic Materials,Tsukuba,Japan	Physica C, 217(1993)287	H.Nakata,J.Akimitsu,M.Ogawa,M.Uehara,Y.Matsui	Tl,Sr,Ba,Cu,C,O	
8965	PHC2170287	impuriy= (Ba,Sr)2CuO3	TlSr2(Sr,Ba)2Cu2(CO3)Oz	Tl1Sr1.5Ba2.5Cu2Co3OZ	Tl	1	Sr	1.5	Ba	2.5	Cu	2	Co	3											O	Z		1	1993																												Tl1223																			59	64					64																																																																																														Tl2O3, Sr2CuO2(CO3), BaO2, CuO		mixture-SIN( 930-950C, 0.5H in gas flow(99% O2+1% CO2) -Q to RT.					Incommensurate and commensurate superstructures in the oxycarbonate superconductor TlSr4-xBaxCu2(CO3)Oy (y=2)	199311		National Institute for Research in Inorganic Materials,Tsukuba,Japan	Physica C, 217(1993)287	H.Nakata,J.Akimitsu,M.Ogawa,M.Uehara,Y.Matsui	Tl,Sr,Ba,Cu,C,O	
8966	PHC2070065	n=4 for(Y,Ca)nSr2nCu3n-1CO3O7n-3 series not s/c	Y4Sr8Cu11(CO3)O25	Y4Sr8Cu11C1O28	Y	4	Sr	8	Cu	11	C	1													O	28			1993																													Bm2m			15.311	3.851	22.371																	4																																																																																																	1	nominal composition=YSr2Cu3O7					"ORDERED SUBSTITUTION OF ""CO3""GROUPS FOR CUO4 SQUARE GROUPS IN THE ""123"" STRUCTURE"	199303			PHYSICA C,207(1993)65	B.DOMENGES,B.RAVEAU,M.HERVIEU	C,O,CU,Y,SR	
8967	PHC2080116	lattice parameters show subcell parameters	(Y,Ca)2Ba4Cu5(NO3,CO3)O11	Y1Ca1Ba4Cu5N0.3C0.7O14	Y	1	Ca	1	Ba	4	Cu	5	N	0.3	C 	0.7									O	14			1993																																3.879	3.885	11.536																82			82										15																																																																																					1	mixture-pellet-( evacuated ampoule) heat (900C,24H)-FC to RT					"INTRODUCTION OF NITRATE GROUPS IN THE ""123""STRUCTURE"	199304			PHYSICA C,208(1993)116	A.MAIGNAN,B.RAVEAU,C.MICHEL,M.HERVIEU	Y,CA,BA,CU,N,C,O	
8968	PHC2200310	impurity phase= BaCuO2, Tl-1223/Ag tape	TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9+Z	Tl	1	Ba	2	Ca	2	Cu	3													O	9+Z			1994																												Tl1223																						103			103																																		HIR8968																																																													1	nominal Tl:Ba:Ca:Cu= 2.12:2:2:3					Granularity, microstructure, and flux creep in TlBa2Ca2Cu3O9+z superconducting powder and silver-sheathed tapes	199402			Physica C, 220(1994)310-322	D.E.Peterson,M.E.McHenry,M.P.Maley,P.G.Wahlbeck,P.J.Kung	Tl,Ba,Ca,Cu,O	
8969	PHC2080226		(Sr,Ca)CuO2	Sr0.6Ca0.333Cu1O2.15	Sr	0.6	Ca	0.333	Cu	1															O	2+Z	2.15		1993																												IL																						82			82																																																																																																(Sr-Ca-Cu-O) samples were prepared using a high-pressure synthesis. oxidize using KClO3 or KClO4 For Z>=2.10, IL  phase decomposed to others.					HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING SR-CA-CU-O SAMPLES	199304			PHYSICA C,208(1993)226	H.YAMAUCHI,NOBUO MORI,SEIJI ADACHI,SHOJI TANAKA	SR,CA,CU,O	
8970	PHC2080226		(Sr,Ca)CuO2	Sr0.6Ca0.333Cu1O2.2	Sr	0.6	Ca	0.333	Cu	1															O	2+Z	2.2		1993																												IK																						98			98																																																																																																(Sr-Ca-Cu-O) samples were prepared using a high-pressure synthesis. oxidize using KClO3 or KClO4 For Z>=2.10, IL  phase decomposed to others.					HIGH-PRESSURE SYNTHESIS OF SUPERCONDUCTING SR-CA-CU-O SAMPLES	199304			PHYSICA C,208(1993)226	H.YAMAUCHI,NOBUO MORI,SEIJI ADACHI,SHOJI TANAKA	SR,CA,CU,O	
8971	PR04714654		(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			1993																											2	IL	P4/mmm			3.95		3.409																42			42																																																																																														SrCO3, La2O3, CuO		mixture-heat (950C,48H) -(boronitride capsule) -high pressure synthesis (950C,1H at 5 GPa) -ANN (500C,20H at 5 GPa)					STRUCTURE OF SUPERCONDUCTING SR0.9LA0.1CUO2 (TC=42K) FROM NEUTRON POWDER DIFFRACTION	199306			PHYS.REV.B,47(1993)14654	D.G.HINKS,F.KANAMARU,G.ER,J.D.JORGENSEN,J.L.WAGNER,P.G.RADAELLI,S.KIKKAWA		
8972	NAT3560775	impurity phase=CuO+unknown phase, second Tc=75K	(Sr,Ca)CuO2	Sr0.7Ca0.3Cu1O2	Sr	0.7	Ca	0.3	Cu	1															O	2			1992																											2	IL				3.902		3.35													35		110	110			110																																																																																																mixture-heat (1273K, 0.5H at 6GPa using anvil-tyre apparatus) -oxidize using KClO4					Superconductivity at 110 K in the infinite-layer compound(Sr1-xCax)1-yCuO2				Nature, 356(1992)775-776	M.Azuma,M.Takano,Y.Bando,Y.Takeda,Z.Hiroi		
8973	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						0.616			0.616	TC8973																			T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.0137										HC8973		A	esimated using Hc2(O) values.		1514																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8974	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						0.954			0.954	TC8973																			T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.0231										HC8974		A	esimated using Hc2(O) values.		1158																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8975	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						1.201			1.201	TC8973																			T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.0378										HC8975		A	esimated using Hc2(O) values.		920																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8976	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						1.242			1.242	TC8973																			T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.0465										HC8976		A	esimated using Hc2(O) values.		821																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8977	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						1.398			1.398																				T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.053										HC8977		A	esimated using Hc2(O) values.		752																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8978	PR06000610		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																						1.489			1.489																				T	using Hc2(O)=-0.68(dHc2/dT)*Tc.			0.0623										HC8978		A	esimated using Hc2(O) values.		683																																																									floating-zone image turnace, 15% excess Ru as flux, melted in 10% O2+ 90% Ar wuth total of 3 bar, Tc depends on the feed speed.					Suppression of superconductivity in Sr2RuO4 caused by defects	199907		Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 60(1999)610-615	Y.Maeno,Y.Mori,Z.Q.Mao		
8979	PR06000687	single phase is not s/c, semiconducting	(Bi,Cu)Sr2YCu2O7	Bi0.33Cu2.67Sr2Y1O6.88	Bi	0.33	Cu	2.67	Sr	2	Y	1													O	Z	6.88	1	1999																											2	M1212	P4/mmm			3.8135		11.705																	5																																																																																																	1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8980	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.264Mo0.066Cu2.67Sr2Y1O7.09	Bi	0.264	Mo	0.066	Cu	2.67	Sr	2	Y	1											O	Z	7.09	1	1999																												M1212				3.8123		11.6753																	5																																																																																																	1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8981	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.198Mo0.132Cu2.67Sr2Y1O7.18	Bi	0.198	Mo	0.132	Cu	2.67	Sr	2	Y	1											O	Z	7.18	1	1999																												M1212				3.8113		11.6235																	5																																																																																																	1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8982	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.165Mo0.165Cu2.67Sr2Y1O7.21	Bi	0.165	Mo	0.165	Cu	2.67	Sr	2	Y	1											O	Z	7.21	1	1999																												M1212				3.8123		11.6025																	5																																																																																																	1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8983	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.1485Mo0.1815Cu2.67Sr2Y1O7.21	Bi	0.1485	Mo	0.1815	Cu	2.67	Sr	2	Y	1											O	Z	7.21	1	1999																												M1212				3.8138		11.5938																20.6			20.6																																																																																															1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8984	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.132Mo0.198Cu2.67Sr2Y1O7.2	Bi	0.132	Mo	0.198	Cu	2.67	Sr	2	Y	1											O	Z	7.2	1	1999																												M1212				3.812		11.5852															29				29																																																																																															1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8985	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.1155Mo0.2145Cu2.67Sr2Y1O7.25	Bi	0.1155	Mo	0.2145	Cu	2.67	Sr	2	Y	1											O	Z	7.25	1	1999																												M1212				3.8155		11.5753																																																																																																																		1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8986	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.099Mo0.231Cu2.67Sr2Y1OZ	Bi	0.099	Mo	0.231	Cu	2.67	Sr	2	Y	1											O	Z		1	1999																												M1212																																																																																																																								1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8987	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0Mo0.33Cu2.67Sr2Y1O7.41	Bi	0	Mo	0.33	Cu	2.67	Sr	2	Y	1											O	Z	7.41	1	1999																												M1212				3.8132		11.5222															30	33			33																																																																																															1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8988	PR06000687		(Bi,Mo,Cu)Sr2YCu2Oz	Bi0.066Mo0.264Cu2.67Sr2Y1O7.32	Bi	0.066	Mo	0.264	Cu	2.67	Sr	2	Y	1											O	Z	7.32	1	1999																												M1212				3.8125		11.5469																31			31																																																																																															1	mixture-CAL(850-900C, 5-10H in air) -pellet - SIN(980C, 20-60H in air) -Q to RT-ANN(500C, 8H in O2 flow)					Superconductivity above 30 K in ((Bi-xMox)0.33Cu0.67)Sr2YCu2Oy:Appearance of superconductivity by transfer of holes from a block layer to a CuO2 layer	199907		Graduate School of Engineering, Yamagata University, 4-3-16, Jonan,  Yonezawa, Yamagata 992, Japan	Phys.Rev.B, 60(1999)687-697	Eiji Sato,Katsuro Okuyama,Rika Sekine,Shigetoshi Ohshima,Shiro Kambe,Takahiro Akao		
8989	SUP0110143	grain size=10*10*2 micron.	(Tl,Pb)Sr2Ca2Cu3Oz	Tl0.5Pb0.5Sr2Ca2Cu3OZ	Tl	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3											O	Z			1998									3.76																			Tl1223																						119			119																																		HIR8989																																																														precursor (Sr2Ca2Cu3Oz)+ Tl2O3, Pb3O4, LiO- pellet- SIN(940C, 5H in O2) - ANN(860C, 2H+ 800C, 24H in air)					Enhancement of microstructrual and magnetic properties by Li-doping in Tl, Pb-1223 superconductors	1998			J.Supercond, 11(1998)143-144	M.Ciszek,S.Wu,W.Y.Liang		
8990	SUP0110143	grain size=30*30*6 micron.	(Tl,Pb)Sr2Ca2Cu3LixOz	Tl0.5Pb0.5Sr2Ca2Cu3Li0.2OZ	Tl	0.5	Pb	0.5	Sr	2	Ca	2	Cu	3	Li	0.2									O	Z			1998									4.88																			Tl1223																						117			117																																		HIR8990																																																														precursor (Sr2Ca2Cu3Oz)+ Tl2O3, Pb3O4, LiO- pellet- SIN(940C, 5H in O2) - ANN(860C, 2H+ 800C, 24H in air)					Enhancement of microstructrual and magnetic properties by Li-doping in Tl, Pb-1223 superconductors	1998			J.Supercond, 11(1998)143-144	M.Ciszek,S.Wu,W.Y.Liang		
8991	PHB1651335	The low temperature linear term in specitic heat = 4.9mj/mole. K2	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1990																												Y124																				81.9					81.9																																																								mj/mol. K2	12		350	from specific heat at high temperature.																																				synthesized under 85 bar O2 at 1000C					SPECIFIC HEAT OF THE SUPERCONDUCTOR YBA2CU4O8 FROM 1.5 TO 300K	8		DEPARTEMENT DE PHYSIQUE DE LA MATIERE CONDENSEE, UNIVERSITE DEGENEVE CH-1211 GENEVE 4, SWITZERLAND	PHYSICA B,165(1990)1335	A.JUNOD,D.SANCHEZ,G.TRISCONE,J.MULLER,T.GRAF	Y,BA,CU,O	
8992	PR05407481	thin film	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		5	1996																												T						13.172														16.4					16.4																																									A	mutual inductance and fluctuation model.		8020																																																				The films were grown on SrTiO3 using sequential MBE					Variation of the in-plane penetration depth  ab a function of doping in La2-xSrxCuO4 z thin films on SrTiO3: Implications for the overdoped state	199609		"IBM reserch Division,Zurich reserch Laboratory, 8803 Ru""schlikon, Swizerland"	Phys.Rev.B,54(1996)7481	"A. Cretton,E. Ma""chler,E.J. Williams,F. Arrouy,J.-P. Locquet,O. Fischer,P. Martinoli,T. Schneider,Y. Jaccard"		
8993	PR05407481	thin film	(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4		5	1996																												T						13.182														22.6					22.6																																									A	mutual inductance and fluctuation model.		6580																																																				The films were grown on SrTiO3 using sequential MBE					Variation of the in-plane penetration depth  ab a function of doping in La2-xSrxCuO4 z thin films on SrTiO3: Implications for the overdoped state	199609		"IBM reserch Division,Zurich reserch Laboratory, 8803 Ru""schlikon, Swizerland"	Phys.Rev.B,54(1996)7481	"A. Cretton,E. Ma""chler,E.J. Williams,F. Arrouy,J.-P. Locquet,O. Fischer,P. Martinoli,T. Schneider,Y. Jaccard"		
8994	PR05407481	thin film	(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		5	1996																												T						13.198														21					21																																									A	mutual inductance and fluctuation model.		7060																																																				The films were grown on SrTiO3 using sequential MBE					Variation of the in-plane penetration depth  ab a function of doping in La2-xSrxCuO4 z thin films on SrTiO3: Implications for the overdoped state	199609		"IBM reserch Division,Zurich reserch Laboratory, 8803 Ru""schlikon, Swizerland"	Phys.Rev.B,54(1996)7481	"A. Cretton,E. Ma""chler,E.J. Williams,F. Arrouy,J.-P. Locquet,O. Fischer,P. Martinoli,T. Schneider,Y. Jaccard"		
8995	EPL0480073	substrate=LaAlO3, d=900A	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1999																												Y123																				91.3					91.3																																									A	sub milimeter wave transmission	2040																																																					magnetron sputtering					Universal relationship between the penetration depth and the mormal-state conductivity in YBaCuO	199910		Institut fur Physik, Universitat Augsburg-86135 Augsburg, Germany	Europhys Lett,48(1999)73-78	A.Loidl,A.Pimenov,A.V.Pronin,B.Schey,B.Stritzker,G.Jakob,H.Adrian,Yu.G.Goncharov		
8996	EPL0480073	substrate=NdGaO3, d=750A	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1999																												Y123																				89					89																																									A	sub milimeter wave transmission	2150																																																					magnetron sputtering					Universal relationship between the penetration depth and the mormal-state conductivity in YBaCuO	199910		Institut fur Physik, Universitat Augsburg-86135 Augsburg, Germany	Europhys Lett,48(1999)73-78	A.Loidl,A.Pimenov,A.V.Pronin,B.Schey,B.Stritzker,G.Jakob,H.Adrian,Yu.G.Goncharov		
8997	EPL0480073	substrate=NdGaO3, d=700A	YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		4	1999																												Y123																				91					91																																									A	sub milimeter wave transmission	2920																																																					laser ablation					Universal relationship between the penetration depth and the mormal-state conductivity in YBaCuO	199910		Institut fur Physik, Universitat Augsburg-86135 Augsburg, Germany	Europhys Lett,48(1999)73-78	A.Loidl,A.Pimenov,A.V.Pronin,B.Schey,B.Stritzker,G.Jakob,H.Adrian,Yu.G.Goncharov		
8998	EPL0490086	composition Bi2Sr1.9CaCu1.8O8+z by EDAX, tunneling by break-junction technique.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	2000																											3	Bi2212				5.41	5.55	30.81																88.5			88.5																																														meV	22.5	5.91	1																																															self-flux method.					The pseudogap in Bi2Sr2CaCu2O8+x single crystals from tunneling measurements: A possible evidence for the Cooper pairs above Tc	200001		Universite Libre de Bruxelles,Service de Physique des Solides CP233, Blvd.du Triomphe, B-1050 Brussels, Belgium	Europhys Lett,49(2000)86-91	A.Mourachkine		
8999	EPL0470715	penetration depth(ab)=8000-10000A estimated from microwave impedance measurement	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	1999																												T																						12			12																																									A	microwave impedance		8000																																																				traveling-solvent floating-zone method.					In-plane charge dynamics in La1.6-xNd0.4SrxCuO4: Absence of a charge gap in the spin/charge ordered state	199909		Superconductivity Research Laboratory,ISTEC-Tokyo 135-0062, Japan	Europhys Lett,47(1999)715-721	A.Maeda,H.Eisaki,H.Kitano,N.Ichikawa,N.L.Wang,S.Tajima,S.Uchida,T.Hanaguri		
9000	PR05802956	single cryotal 0.4*0.3*0.1 mm3, dTc/dp by resistivity measurement. d(TP300)/dp=0.2uV/K. kbar	YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8		3	1998																												Y124																						57			57			k/kbar	1.2																																																																																												high temperature-high pressure synthesis(600 bar Oz)					Anomalous transport properties in a YBa2Cu4O8 crystal	8		Anomalous transport properties in a YBa2Cu4O8 crystal	Phys.Rev.B,58(1998)R2956	B. Dabrowski,J.-S. Zhou,J.B. Goodenough		
9001	PR05911668	crystal(0.2*0.1*0.1 mm3), resistivity anisotropy=6	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1999																												Y124																				82				0.5	82																																																																																																flux method in Y2O3 crucibles, Ar/O2 mixture at 2000 bars with partial O2 pressure of 400 bars					Melting of the vortex lattice in YBa2Cu4O8 in parallel fields	199905		Institute for Solid State Physics, University of Tokyo, Roppongi 7-22-1, Tokyo 106-8666, Japan	Phys.Rev.B, 59(1999)R11668-R11671	H.Takagi,K.Tanabe,N.E.Hussey,N.Mori,N.Takeshita,S.Adachi,Y.Iye		
9002	PR05911563	crystal(1.16*0.54*0.36 mm3), G-L parameter=55, anisotropy factor=5.9, Lindeman const.=0.16	NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z		3	1999																												Y123																				95.56				0.3	95.56																							287									3	1																																																															self-flux method, 0.03%O2-Ar, ANN(320C, 300H)					First-order vortex lattice melting in twinned NdBa2Cu307-y single crystals	199905		Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome, 1-Chome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B, 59(1999)11563-11567	A.K.Pradhan,K.Nakao,N.Koshizuka,S.Shibata		
9003	PR05911679	84%O(18), isotope effect using T3 value	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	1999																												Ru1212																			35		46				40.5						0.12	O																																																																																								1	annealed(1060C, 7days in flowing O2)					Oxygen isotope effects on the critical and Curie temperatures and Raman modes in the ferromagnetic superconductor RuSr2GdCu2O8	199905		School of Chemical and Physical Sciences, Victoria University of Wellington, P.O. Box 600, Wellington, New Zealand	Phys.Rev.B, 59(1999)R11679-R11682	B.G.Walker,D.J.Pringle,H.J.Trodahl,J.L.Tallon		
9004	PHC2821407	nearly single phase., Beta(lattice term)=2.17mj/mol.K3	PrBa2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		1	1997								17																				Y124				3.879	3.902	27.28																	4.2																																																										mj/mol.K2	205	specitic heat		calculated by Asada using data.																																				nitric pyrolysis method at ambient oxygen pressure					Thermal properties of PrBa2Cu4O8 prepared at ambient oxygen pressure				Physica C, 282-287 (1997) 1407-1408	C.W.Lin,H.D.Yang,H.L.Tsay,J.-Y.Lin,J.C.Huang,M.K.Wu,S.R.Sheen,T.H.Meen		
9005	PHC2821413		Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1997																												Sr2RuO4																						1.2			1.2																																																						mj/mol.K	18.8	mj/mol.K2	40.9	specitic heat																																						by floating zone method					Pairing symmetry of superconducting Sr2RuO4 from specific heat measurements				Physica C, 282-287 (1997) 1413-1414	S.Farner,S.Ikeda,S.Nishizaki,T.Fujita,Y.Maeno		
9006	PHC2821423		(Tl,Pb)(Sr,Ba)2Ca2Cu3Oz	Tl0.58Pb0.4Sr1.6Ba0.4Ca2Cu3OZ	Tl	0.58	Pb	0.4	Sr	1.6	Ba	0.4	Ca	2	Cu	3									O	Z		1	1997																												Tl1223																				110					110																																																						mj/mol.K	30	mj/mol.K2	25	specitic heat																																						See Supercond. Sci. Technol, 8(1995)894					Specific heat and electron photoemission of Pb- and Bi- doped Tl-(Ba,Sr)-Ca-Cu-O (1223) high-temperature superconductors				Physica C, 282-287 (1997) 1423-1424	A.Kolodziejcyk,A.Kozlowski,G.Gritzner,M.Mair,R.Zalecki,W.Konig		
9007	PHC2821423		(Tl,Bi)(Sr,Ba)2Ca2Cu3Oz	Tl0.79Bi0.25Sr1.6Ba0.4Ca2Cu3OZ	Tl	0.79	Bi	0.25	Sr	1.6	Ba	0.4	Ca	2	Cu	3									O	Z		1	1997																												Tl1223																				115					115																																																						mj/mol.K	23	mj/mol.K2	27	specitic heat																																						See Supercond. Sci. Technol, 8(1995)894					Specific heat and electron photoemission of Pb- and Bi- doped Tl-(Ba,Sr)-Ca-Cu-O (1223) high-temperature superconductors				Physica C, 282-287 (1997) 1423-1424	A.Kolodziejcyk,A.Kozlowski,G.Gritzner,M.Mair,R.Zalecki,W.Konig		
9008	PHC2821423		(Tl,Bi)(Sr,Ba)2Ca2Cu3Oz	Tl0.74Bi0.3Sr1.8Ba0.2Ca2Cu3OZ	Tl	0.74	Bi	0.3	Sr	1.8	Ba	0.2	Ca	2	Cu	3									O	Z		1	1997																												Tl1223																				120					120																																																						mj/mol.K	28	mj/mol.K2	16	specitic heat																																						See Supercond. Sci. Technol, 8(1995)894					Specific heat and electron photoemission of Pb- and Bi- doped Tl-(Ba,Sr)-Ca-Cu-O (1223) high-temperature superconductors				Physica C, 282-287 (1997) 1423-1424	A.Kolodziejcyk,A.Kozlowski,G.Gritzner,M.Mair,R.Zalecki,W.Konig		
9009	PHC2821403	Gd(3+) ordering temperature by specitic heat measurement 	GdBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8		1	1997								2.2																				Y124																						74			74																																																																																																coprecipitation method, CAL(800C, 1atm O2 flow)-SIN(815C,10days in 1atm O2 flow), single pase by XRD					Magnetic field dependence of low temperature heat capacities of GdBa2Cu4O8				Physica C, 282-287 (1997) 1403-1404	J.C.Ho,J.C.Huang,M.K.Wu,S.R.Sheen,W.S.Huang,Y.D.Yao,Y.Y.Chen		
9010	PHC2821419	specitic heat by relaxation method	(Bi,Pb)2Sr2CuOz	Bi1.8Pb0.3Sr1.9Cu1OZ	Bi	1.8	Pb	0.3	Sr	1.9	Cu	1													O	Z		1	1997																												Bi2201																							1.5																																																										mj/mol.K2	8.75	specitic heat																																					1	solid state reaction					Anomalous electronic specific heat of Bi1.8Pb0.3Sr1.9CuOz				Physica C, 282-287 (1997)1419-1420	H.Mayama,K.Yamaya,Y.Okajima		
9011	PHC2821419	delte C=17.20 mj/mol.K, delta-C/gama.Tc=0.6	(Bi,Pb)2Sr2CuOz	Bi1.8Pb0.3Sr1.9Cu1OZ	Bi	1.8	Pb	0.3	Sr	1.9	Cu	1													O	Z		1	1997																												Bi2201																						4.7			4.7																																																								mj/mol.K2	6.1	specitic heat																																						solid state reaction-ANN in Ar					Anomalous electronic specific heat of Bi1.8Pb0.3Sr1.9CuOz				Physica C, 282-287 (1997)1419-1420	H.Mayama,K.Yamaya,Y.Okajima		
9012	PHC2821415		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8		1	1997																												Bi2212																				67					67																																																								uJ/K2.g	1.01	specitic heat	298	specitic heat																																			1	as-grown, furnace cool.					The relations of specific heat anomaly with variation of oxygen content in BiSrCaCuO(2212)				Physica C, 282-287 (1997)1415-1416	K.Q.Wang,L.Z.Cao,Y.Feng,Z.Q.Mao		
9013	PHC2821415		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8		1	1997																												Bi2212																				92					92																																																								uJ/K2.g	1.015	specitic heat	296.7	specitic heat																																				ANN (550C, 0.5H in E-5 atm O2)					The relations of specific heat anomaly with variation of oxygen content in BiSrCaCuO(2212)				Physica C, 282-287 (1997)1415-1416	K.Q.Wang,L.Z.Cao,Y.Feng,Z.Q.Mao		
9014	PHC2821415		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8		1	1997																												Bi2212																				80					80																																																								uJ/K2.g	0.978	specitic heat	295.6	specitic heat																																				ANN (550C, 2.5H in E-5 atm O2)-ANN(550C, 2.5H in E-8 atm O2)					The relations of specific heat anomaly with variation of oxygen content in BiSrCaCuO(2212)				Physica C, 282-287 (1997)1415-1416	K.Q.Wang,L.Z.Cao,Y.Feng,Z.Q.Mao		
9015	PHC2821415		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8		1	1997																												Bi2212																				81					81																																																								uJ/K2.g	1.087	specitic heat	303.5	specitic heat																																				ANN (550C, 5H in E-5 atm O2)-ANN (550C, 10H in E-8 atm O2)					The relations of specific heat anomaly with variation of oxygen content in BiSrCaCuO(2212)				Physica C, 282-287 (1997)1415-1416	K.Q.Wang,L.Z.Cao,Y.Feng,Z.Q.Mao		
9016	PRO5407462	untwinned single erystal		Lu1Ba2Cu3O7-Z	Lu	1	Ba	2	Cu	3															O	7-Z		3	1996																												Y123																			90.7		93				91.85																																																								mj/mol.K2	13.1	temperature range 0.6<T<10K																																						See Phys.Rev.Lett.72(1994)2632					Experimental investigation of the pairing state of high-temperature superconductors				Phys.Rev.B. 54 (1996) 7462	A.M.Goldman,Branko P.Stojkovic,C.C.Huang,C.R.Shih,H.D.Yang,J-Z. Liu,J.Buan,Nathan Israloff,Oriol T.Valls,Robert Shelton,S.Sridhar,T.Jacobs		
9017	PHC3240065		Ba2Ca2Cu3Oz	Ba2Ca2Cu3OZ	Ba	2	Ca	2	Cu	3															O	Z		1	1999																												0223				3.85		28.3																124			124																																		HIR9017																																																														high pressure synthesis(5GPa,770c),Ba:Ca:Cu = 2:2:4 for nominal					Magnetic irreversibility characteristics of highly unstable superconducting Ba2Ca2Cu3Oy and its derivative phase				Physca C, 324 (1999) 65-70	H.Suematsu,H.Yamauchi,M.Karppinen,T.Hosomi		
9018	PHC3240065	Ba-Ca-Cu-O,H-5223:I phase,derived from 12 6K phase	Ba2Ca2Cu3Oz	Ba2Ca2Cu3OZ	Ba	2	Ca	2	Cu	3															O	Z		1	1999																												0223				3.85		34																78			78																																		HIR9018																																																														high pressure synthesis(5GPa,770c),Ba:Ca:Cu = 2:2:4 for nominal					Magnetic irreversibility characteristics of highly unstable superconducting Ba2Ca2Cu3Oy and its derivative phase				Physca C, 324 (1999) 65-70	H.Suematsu,H.Yamauchi,M.Karppinen,T.Hosomi		
9019	JMC0091141	(CaxCuy)Ba2Ca2Cu3O8+z 	Ba2Ca2Cu3Oz	Ba2Ca2Cu3OZ	Ba	2	Ca	2	Cu	3															O	Z		1	1999																											2	0223				3.85		28.3																126			126																																																																																																high pressure synthesis,BaCuO2+z + Ca2CuO3+ Ba2Cu3O5+z + AgO - (5GPa,77OC,30min) - Q to RT					Identification of superconducting phases in the Ba-Ca-Cu-O system: an unstable phase with Tc = 126 K and its derivative with Tc=90 K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama, Japan	J.Mater.Chem., 9(1999)1141	H.Fjellvag,H.Suematsu,H.Yamauchi,M.Karppinen,T.Hosomi		
9020	JMC0091141	This phase is obtained by exposong 126k phase to air	Ba2Ca2Cu3Oz	Ba2Ca2Cu3OZ	Ba	2	Ca	2	Cu	3															O	Z		1	1999																											2	0223	I4/mmm			3.8486		33.979																90			90																																																																																																high pressure synthesis,BaCuO2+z + Ca2CuO3+ Ba2Cu3O5+z + AgO - (5GPa,77OC,30min) - Q to RT					Identification of superconducting phases in the Ba-Ca-Cu-O system: an unstable phase with Tc = 126 K and its derivative with Tc=90 K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama, Japan	J.Mater.Chem., 9(1999)1141	H.Fjellvag,H.Suematsu,H.Yamauchi,M.Karppinen,T.Hosomi		
9021	PHC3230001	underdopcng	(Y,Yb)Ba2Cu3Oz	Y0.975Yb0.025Ba2Cu3OZ	Y	0.975	Yb	0.025	Ba	2	Cu	3													O	Z		1	1999																												Y123																				65					65																																									nm	Mossbauer measurement,ppenet calculate from pemet.	204	166																																																				For Mossbawer mesurement,<170>Yb(3+)is doped oxygent control for different annealing condition					Local Fields in YBa2Cu3O7-delta measured on 170Yb3+ Mossbauer probes. I. Volume and surface penetration lengths	199910		DRECAM-SPEC, Centre d'Etudes de Saclay, 91191 Gift sur Yvette, France	Physica C,323(1999)1-11	C. Vaast-Paci,C.K. Ong,Catherine Chaillout,P. Bonville		
9022	PHC3230001	optimal doping	(Y,Yb)Ba2Cu3Oz	Y0.975Yb0.025Ba2Cu3OZ	Y	0.975	Yb	0.025	Ba	2	Cu	3													O	Z		1	1999																												Y123																				92					92																																									nm	Mossbauer measurement,ppenet calculate from pemet.	160	130																																																				For Mossbawer mesurement,<170>Yb(3+)is doped oxygent control for different annealing condition					Local Fields in YBa2Cu3O7-delta measured on 170Yb3+ Mossbauer probes. I. Volume and surface penetration lengths	199910		DRECAM-SPEC, Centre d'Etudes de Saclay, 91191 Gift sur Yvette, France	Physica C,323(1999)1-11	C. Vaast-Paci,C.K. Ong,Catherine Chaillout,P. Bonville		
9023	PHC3230001	overdoing	(Y,Yb)Ba2Cu3Oz	Y0.975Yb0.025Ba2Cu3OZ	Y	0.975	Yb	0.025	Ba	2	Cu	3													O	Z		1	1999																												Y123																				88					88																																									nm	Mossbauer measurement,ppenet calculate from pemet.	134	109																																																				For Mossbawer mesurement,<170>Yb(3+)is doped oxygent control for different annealing condition					Local Fields in YBa2Cu3O7-delta measured on 170Yb3+ Mossbauer probes. I. Volume and surface penetration lengths	199910		DRECAM-SPEC, Centre d'Etudes de Saclay, 91191 Gift sur Yvette, France	Physica C,323(1999)1-11	C. Vaast-Paci,C.K. Ong,Catherine Chaillout,P. Bonville		
9024	PHC3230001	Ca-doping	(Y,Yb,Ca)Ba2Cu3Oz	Y0.78Yb0.02Ca0.2Ba2Cu3OZ	Y	0.78	Yb	0.02	Ca	0.2	Ba	2	Cu	3											O	Z		1	1999																												Y123																																																																		nm	Mossbauer measurement,ppenet calculate from pemet.	118	96																																																				For Mossbawer mesurement,<170>Yb(3+)is doped oxygent control for different annealing condition					Local Fields in YBa2Cu3O7-delta measured on 170Yb3+ Mossbauer probes. I. Volume and surface penetration lengths	199910		DRECAM-SPEC, Centre d'Etudes de Saclay, 91191 Gift sur Yvette, France	Physica C,323(1999)1-11	C. Vaast-Paci,C.K. Ong,Catherine Chaillout,P. Bonville		
9025	PHC2351761	T2 defined as specific heat maximum point,susceptibity(200K)= -8.6 E-8 emu/g	Bi2Sr2CaCu2Oz	Bi2.12Sr1.71Ca1.22Cu1.95OZ	Bi	2.12	Sr	1.71	Ca	1.22	Cu	1.95													O	Z		3	1994																												Bi2212																				85.1		84.55			85.1																																																								mj/mol.K2	2.1	linear term at very low tempperatures	283																																					by the travelling solvent floating zone method					Anisotropic specific heat of a Bi2Sr2CaCu2O8 single crystal in magnetic fields up to 14 T				Physica C, 235-240 (1994) 1761-1762	A.Junod,B.Revaz,E.Walker,G.Triscone,J.Muller,K.-Q.Wang,T.Tsukamoto		
9026	PHC2821381	underdoped sample		Hg1Ba2Cu1O4.02	Hg	1	Ba	2	Cu	1															O	4+Z	4.02	1	1997																												Hg1201																						72			72																																																																																																See Physica C, 255(1995)173					Magnetic properties and NMR investigations of the Hg-based cuprate Hg-1201				Physica C, 282-287 (1997)1381-1382	A.A.Gippius,E.V.Antipov,K.Luders,M.Baenitz,M.Heinze,W.Hoffmann		
9027	PHC2821381	optimal doping		Hg1Ba2Cu1O4.08	Hg	1	Ba	2	Cu	1															O	4+Z	4.08	1	1997																												Hg1201																						96			96																																		HIR9027																																																														See Physica C, 255(1995)173					Magnetic properties and NMR investigations of the Hg-based cuprate Hg-1201				Physica C, 282-287 (1997)1381-1382	A.A.Gippius,E.V.Antipov,K.Luders,M.Baenitz,M.Heinze,W.Hoffmann		
9028	PHC3250109		(Hg,Sb)Ba2Ca2Cu3O8	Hg0.95Sb0.05Ba2Ca2Cu3O8+Z	Hg	0.95	Sb	0.05	Ba	2	Ca	2	Cu	3											O	8+Z		1	1999																												Hg1223																			132						132																																		HIR9028																		JC9028																																												precursor(Sb0.05Ba2Ca2Cu3Oz)+Hg2O,Hg vapour dittussion process					Oinprovement of critical current density in Sb-doped HgBa2Ca2Cu3O8+delta superconductor prepared Hg vapour diffusion process	199911		Department of Physics and Materials Science, City University of Hong Kong, Hong Kong people's republic of China	Physica C,325(1999)109-117	C.C. Lam,G.B. Peacock,J.Q. Li,J.S. Abell,L.J. Shen,P.P. Edwards		
9029	PRL0732484	untwinned sample,Temperatau dependence of peretratiou depth //a-and //b-axis were meamre I by susface impedance, //a- = 1600A, //b- = 1030A	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	3	1994																												Y123																				93.4				0.25	93.4																																																																																																Crystals were grown by a flux methed					Measurement of the ab Plane Anisotropy of Microwave Surface Impendance of Untwinned YBa2Cu3O6.95 Single Crystals	199410		Department of Physics,University of British Columbia,Vancouver,British Columbia Canada V6T 1Z1	Phys.Rev.Lett.,73(1994)2484	D.A.Bonn,D.Basov,D.J.Baar,Kuan Zhang,Ruixing Liang,S.Kamal,T.Timusk,W.N.Hardy	Y,Ba,Cu,O	
9030	PR04611019		Tl2Ba2CuO6	Tl2Ba2Cu1O6.164	Tl	2	Ba	2	Cu	1															O	6+Z	6.164	3	1992																											2	Tl2201	I4/mmm			3.864		23.165														0					0																																																																																																Crystals were grown by slow cooling method using KCl flux					TRANSPORT AND STRUCTURAL STUDY OF TL2BA2CUO6+Z SINGLE CRYSTALSPREPARED BY THE KCL FLUX METHOD	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYS.REV.B,46(1992)11019	Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	TL,BA,CU,O	
9031	PR04611019		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1992																												Tl2201																				10					10																																																																																											RH9031					Crystals were grown by slow cooling method using KCl flux					TRANSPORT AND STRUCTURAL STUDY OF TL2BA2CUO6+Z SINGLE CRYSTALSPREPARED BY THE KCL FLUX METHOD	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYS.REV.B,46(1992)11019	Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	TL,BA,CU,O	
9032	PR04611019		Tl2Ba2CuO6	Tl2Ba2Cu1O6.056	Tl	2	Ba	2	Cu	1															O	6+Z	6.056	3	1992																											2	Tl2201				3.867		23.21														40					40																																																																																																Crystals were grown by slow cooling method using KCl flux					TRANSPORT AND STRUCTURAL STUDY OF TL2BA2CUO6+Z SINGLE CRYSTALSPREPARED BY THE KCL FLUX METHOD	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYS.REV.B,46(1992)11019	Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	TL,BA,CU,O	
9033	PR04611019		Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1992																												Tl2201																				50					50																																																																																											RH9033					Crystals were grown by slow cooling method using KCl flux					TRANSPORT AND STRUCTURAL STUDY OF TL2BA2CUO6+Z SINGLE CRYSTALSPREPARED BY THE KCL FLUX METHOD	199211		FUNDAMENTAL RESEARCH LABORATORIES, NEC CORPORATION, TSUKUBA	PHYS.REV.B,46(1992)11019	Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	TL,BA,CU,O	
9034	PHC1900062	ANN(350C,in latw O2)	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1991																												Tl2201																							4.2																																																																																													RH9034					Crystals were grown by slow cooling method using KCl flux					SYNTHESIS AND PHYSICAL PROPERTIES OF TL2BA2CUO6+Z SINGLE CRYSTAL	199112			PHYSICA C,190(1991)62	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
9035	PHC1900062	ANN(300C,in air)	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1991																												Tl2201																			10						10																																																																																																Crystals were grown by slow cooling method using KCl flux					SYNTHESIS AND PHYSICAL PROPERTIES OF TL2BA2CUO6+Z SINGLE CRYSTAL	199112			PHYSICA C,190(1991)62	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
9036	PHC1900062	ANN(450C,in air)	Tl2Ba2CuO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		3	1991																												Tl2201																			75						75																																																																																																Crystals were grown by slow cooling method using KCl flux					SYNTHESIS AND PHYSICAL PROPERTIES OF TL2BA2CUO6+Z SINGLE CRYSTAL	199112			PHYSICA C,190(1991)62	H.IGARASHI,T.MANAKO,Y.KUBO,Y.SHIMAKAWA	TL,BA,CU,O	
9037	PHC2180024	pressure by diamond anvil upto 13 Gpa,maximum Tc= 133K at 4.2 Gpa	Tl2Ba2Ca2Cu3O10	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z		1	1993																												Tl2223																			125.1	128.5					128.5			K/Gpa	1.75																																																														mv/K	2																													The sample consists of a single grain. Composition=Tl1.6Ba2Ca2.4Cu3O10+z					Superconductivity at 133K in Tl2Ba2Ca2Cu3O10+x under high pressure	199312		Department of Physics and Astronomy,Free University,Amsterdam,The Netherland	Physica C, 218(1993)24	D.Tristan Jover,J.L.Tallon,R.Griessen,R.J.Wijngaarden,R.S.Liu	Tl,Ba,Ca,Cu,O	
9038	PHC2180001	maximum Tc = 150K at 12.Gpa , Presssure by cubic anvil	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z		1	1993																												Tl1223																						134			134			K/Gpa	2																																																																																										HgO,BaO,CaO,CuO	1	nominal (HgBa2CaCu3Oz)-heat(700C,1H)-ANN(300C,6H in flowing O2)					Large nhancement of Tc in the 134K superconductor HgBa2Ca2Cu3Oy under high pressure	199312	synthesis,high pressure	Institute for solid state Physics, University of Tokyo,Roppongi,Tokyo,Japan	Physica C, 218(1993)1	H.Takahashi,H.Yamauchi,N.Mori,S.Adachi,S.Tanaka,a,Tokiwa	Hg,Ba,Cu,Ca,O	
9039	PHC2351493	Tc is defined as T3. dTc/dP is estimated from the figure. Tc(max)=109.5K	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z			1994																												Hg1201																					92.5				92.5	TC9039		K/Gpa	1.2	23.1																																																																																											See Nature 362(1993)226					Universal enhancement of Tc under high pressure in HgBa2Cam-1CumO2m+2+z				Physica C, 235-240 (1994) 1493-1494	C.W.Chu,D.Rameriz,F.Chen,H.K.Mao,J.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue		
9040	PHC2351493	Tc is defined as T3. dTc/dP is estimated from the figure. Tc(max)=137.7K	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+Z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+Z			1994																												Hg1212																					116				116	TC9040		K/Gpa	1.75	29.3																																																																																											See Nature 362(1993)226					Universal enhancement of Tc under high pressure in HgBa2Cam-1CumO2m+2+z				Physica C, 235-240 (1994) 1493-1494	C.W.Chu,D.Rameriz,F.Chen,H.K.Mao,J.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue		
9041	PHC2351493	Tc is defined as T3. dTc/dP is estimated from the figure. Tc(max)=147K	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z			1994																												Hg1223																					123				123	TC9041		K/Gpa	3	31.2																																																																																											See Nature 362(1993)226					Universal enhancement of Tc under high pressure in HgBa2Cam-1CumO2m+2+z				Physica C, 235-240 (1994) 1493-1494	C.W.Chu,D.Rameriz,F.Chen,H.K.Mao,J.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue		
9042	PHC2351493	Tc is defined as T3. dTc/dP is estimated from the figure. Tc(max)=151.3K	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.9Pb0.1Ba2Ca2Cu3O8+Z	Hg	0.9	Pb	0.1	Ba	2	Ca	2	Cu	3											O	8+Z			1994																												Hg1223																					130				130	TC9042		K/Gpa	3.3	10.6																																																																																											See Nature 362(1993)226					Universal enhancement of Tc under high pressure in HgBa2Cam-1CumO2m+2+z				Physica C, 235-240 (1994) 1493-1494	C.W.Chu,D.Rameriz,F.Chen,H.K.Mao,J.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue		
9043	PHC2351493	Tc is defined as T3. dTc/dP is estimated from the figure. Tc(max)=145K	(Hg,Pb)Ba2Ca2Cu3O8	Hg0.8Pb0.2Ba2Ca2Cu3O8+Z	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	8+Z			1994																												Hg1223																					132				132	TC9043		K/Gpa	3	8																																																																																											See Nature 362(1993)226					Universal enhancement of Tc under high pressure in HgBa2Cam-1CumO2m+2+z				Physica C, 235-240 (1994) 1493-1494	C.W.Chu,D.Rameriz,F.Chen,H.K.Mao,J.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue		
9044	JAC2520076		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1997																											3	Y124				3.8452	3.8666	27.2417																77.5			77.5																																																																																																Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9045	JAC2520076		(Y,Tb)Ba2Cu4O8	Y0.9Tb0.1Ba2Cu4O8	Y	0.9	Tb	0.1	Ba	2	Cu	4													O	8		1	1997																											3	Y124			A	3.8459	3.8702	27.2521																78			78																																																																																																Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9046	JAC2520076		(Y,Ce)Ba2Cu4O8	Y0.9Ce0.1Ba2Cu4O8	Y	0.9	Ce	0.1	Ba	2	Cu	4													O	8		1	1997																											3	Y124			A	3.8456	3.8747	27.2191																38			38																																																																																																Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9047	JAC2520076		(Y,Pr)Ba2Cu4O8	Y0.9Pr0.1Ba2Cu4O8	Y	0.9	Pr	0.1	Ba	2	Cu	4													O	8		1	1997																											3	Y124			A	3.8446	3.8696	27.2321																75			75																																																																																																Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9048	JAC2520076		(Y,Lu)Ba2Cu4O8	Y0.76Lu0.24Ba2Cu4O8	Y	0.76	Lu	0.24	Ba	2	Cu	4													O	8		1	1997																											3	Y124			A	3.8409	3.864	27.2108																																																																																																																			Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9049	JAC2520076		Y(Ba,Sr)2Cu4O8	Y1Ba1.75Sr0.25Cu4O8	Y	1	Ba	1.75	Sr	0.25	Cu	4													O	8		1	1997																											3	Y124			A	3.8376	3.8643	27.1883																																																																																																																			Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9050	JAC2520076		(Y,Lu)(Ba,Sr)2Cu4O8	Y0.52Lu0.48Ba1.75Sr0.25Cu4O8	Y	0.52	Lu	0.48	Ba	1.75	Sr	0.25	Cu	4											O	8		1	1997																											3	Y124			A	3.824	3.8601	27.1662																																																																																																																			Polymerized complex method. See Physica C, 173(1991)377					Structure and superconductivity in Y1-xLnxBa2-ySryCu4O8 (Ln=Lu, Tb, Gd, Pr, Ce); the influence of ionic size and valency			Dept. of Inorganic Chemistry, Chalmers Univ. of Technology and Univ. of Goteborg, Goteborg, Sweden	J.Alloys and Compounds, 252(1997)76-82	L.-G.Johansson,P.Berastegui,S.-G.Eriksson	Y,Ba,Cu,O,Lu,Tb,Gd,Pr,Ce,Sr	
9051	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.7Cd0.3La1Cu3OZ	Ba	1	Ca	0.7	Cd	0.3	La	1	Cu	3											O	Z			1993																											2	1113			A			11.6243															55.4				55.4																																																																																																See PREPID=4509					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
9052	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.75Cd0.25La1Cu3OZ	Ba	1	Ca	0.75	Cd	0.25	La	1	Cu	3											O	Z			1993																											2	1113			A			11.62															60.6				60.6																																																																																																See PREPID=4509					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
9053	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.8Cd0.2La1Cu3OZ	Ba	1	Ca	0.8	Cd	0.2	La	1	Cu	3											O	Z			1993																											2	1113			A			11.6087															65.3				65.3																																																																																																See PREPID=4509					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
9054	PHC2160124		Ba(Ca,Cd)LaCu3Oz	Ba1Ca0.9Cd0.1La1Cu3OZ	Ba	1	Ca	0.9	Cd	0.1	La	1	Cu	3											O	Z			1993																											2	1113			A			11.6															74				74																																																																																																See PREPID=4509					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
9055	PHC2160124		BaCaLaCu3Oz	Ba1Ca1La1Cu3OZ	Ba	1	Ca	1	La	1	Cu	3													O	Z			1993																											2	1113			A			11.5887															80				80																																																																																																See PREPID=4509					REPLACING CA BY CD IN THE TETRAGONAL SUPERCONDUCTING SERIES BACAXCD1-XLACU3OY,0<-X<-1	199310			PHYSICA C,216(1993)124	STANLEY ENGELSBERG	BA,CA,CD,LA,CU,O	
9056	JAP0785212		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O7-Z	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8203	3.8542	11.7312													83.6						83.6																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9057	JAP0785212		(Tm,Pr)Ba2Cu3O7	Tm0.8Pr0.2Ba2Cu3O7-Z	Tm	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8254	3.8575	11.7349													80.9						80.9																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9058	JAP0785212		(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3O7-Z	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8269	3.8606	11.7393													78.5						78.5																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9059	JAP0785212		(Ho,Pr)Ba2Cu3O7	Ho0.8Pr0.2Ba2Cu3O7-Z	Ho	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8301	3.8651	11.741													74.1						74.1																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9060	JAP0785212		(Dy,Pr)Ba2Cu3O7	Dy0.8Pr0.2Ba2Cu3O7-Z	Dy	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8312	3.8704	11.7854													69.1						69.1																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9061	JAP0785212		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7-Z	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8484	3.8828	11.793													66.8						66.8																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9062	JAP0785212		(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O7-Z	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8493	3.8958	11.8003													64						64																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9063	JAP0785212		(Sm,Pr)Ba2Cu3O7	Sm0.8Pr0.2Ba2Cu3O7-Z	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8541	3.8991	11.8038													52.6						52.6																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9064	JAP0785212		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O7-Z	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		1	1995																											3	Y123			A	3.8637	3.8993	11.806													40.9						40.9																																																																																															1	standard solid state reaction method					Ion size effect on normal state resistivity in (R0.8Pr0.2)Ba2Cu3O7-z (R=Sm,Eu, Gd, Dy, Ho, Er, Tm, and Yb) systems	199510		Department of Physics, Chung Yuan Christian University, Chungli,Taiwan	J.Appl.Phys., 78(1995)5212	M.K.Wu,T.S.Lai,W.Y.Guan,Y.Chen		
9065	PHC2910025		GdBa2Cu3O7	Gd1Ba2Cu3O6.969	Gd	1	Ba	2	Cu	3															O	Z	6.969	1	1997																											3	Y123			A	3.8387	3.8968	11.6979														91					91																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9066	PHC2910025		(Gd,Mo)Ba2Cu3O7	Gd0.95Mo0.05Ba2Cu3O6.948	Gd	0.95	Mo	0.05	Ba	2	Cu	3													O	Z	6.948	1	1997																											3	Y123			A	3.8461	3.903	11.7015														82.4					82.4																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9067	PHC2910025		(Gd,Mo)Ba2Cu3O7	Gd0.9Mo0.1Ba2Cu3O6.907	Gd	0.9	Mo	0.1	Ba	2	Cu	3													O	Z	6.907	1	1997																											3	Y123			A	3.8844	3.8782	11.7126														65.9					65.9																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9068	PHC2910025		(Gd,Mo)Ba2Cu3O7	Gd0.85Mo0.15Ba2Cu3O6.855	Gd	0.85	Mo	0.15	Ba	2	Cu	3													O	Z	6.855	1	1997																											3	Y123			A	3.8795	3.8881	11.7312														59.2					59.2																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9069	PHC2910025		(Gd,Mo)Ba2Cu3O7	Gd0.8Mo0.2Ba2Cu3O6.807	Gd	0.8	Mo	0.2	Ba	2	Cu	3													O	Z	6.807	1	1997																											3	Y123			A	3.9376	3.9451	11.6571														52.5					52.5																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9070	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.8Ca0.05Mo0.15Ba2Cu3O6.651	Gd	0.8	Ca	0.05	Mo	0.15	Ba	2	Cu	3											O	Z	6.651	1	1997																											3	Y123			A	3.8504	3.897	11.6697														66.1					66.1																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9071	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.75Ca0.1Mo0.15Ba2Cu3O6.671	Gd	0.75	Ca	0.1	Mo	0.15	Ba	2	Cu	3											O	Z	6.671	1	1997																											3	Y123			A	3.8565	3.8929	11.7183														75.1					75.1																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9072	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.7Ca0.15Mo0.15Ba2Cu3O6.716	Gd	0.7	Ca	0.15	Mo	0.15	Ba	2	Cu	3											O	Z	6.716	1	1997																											3	Y123			A	3.8473	3.8939	11.7														86.3					86.3																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9073	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.65Ca0.2Mo0.15Ba2Cu3O6.818	Gd	0.65	Ca	0.2	Mo	0.15	Ba	2	Cu	3											O	Z	6.818	1	1997																											3	Y123			A	3.8494	3.897	11.694														84.1					84.1																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9074	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.6Ca0.25Mo0.15Ba2Cu3O6.761	Gd	0.6	Ca	0.25	Mo	0.15	Ba	2	Cu	3											O	Z	6.761	1	1997																											3	Y123			A	3.8392	3.9061	11.697														83.7					83.7																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9075	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.55Ca0.3Mo0.15Ba2Cu3O6.626	Gd	0.55	Ca	0.3	Mo	0.15	Ba	2	Cu	3											O	Z	6.626	1	1997																											3	Y123			A	3.8433	3.8949	11.7273														80.7					80.7																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9076	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.5Ca0.35Mo0.15Ba2Cu3O6.586	Gd	0.5	Ca	0.35	Mo	0.15	Ba	2	Cu	3											O	Z	6.586	1	1997																											3	Y123			A	3.8352	3.8959	11.703														77.7					77.7																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9077	PHC2910025		(Gd,Ca,Mo)Ba2Cu3O7	Gd0.45Ca0.4Mo0.15Ba2Cu3O6.537	Gd	0.45	Ca	0.4	Mo	0.15	Ba	2	Cu	3											O	Z	6.537	1	1997																											3	Y123			A	3.8392	3.898	11.697														73					73																																																																																														Gd2O3,BaCO3, CuO, MoO3,CaO	1	mixture - heat(950C, 24H in air in Pt crucible) - pellet - SIN(950C, 24H) - ANN(450C, 12H in O2 flow) - slow cool to RT (1 C/min)					Effect of Mo and Mo-Ca substitution on the superconductivity of GdBa2Cu3O7-delta	199711		Department of Physics, Saurashtra University, Rajkot 360 005, India	Physica.C,291(1997)25-33	Amish G. Joshi,D.G. Kuberkar,G.J. Baldha,R.G. Kulkami		
9078	PHC1950035		(Pb,Cu)Sr2(Ca,Y)Cu2O7	Pb0.7Sr2Ca0.5Y0.5Cu2.3O7-Z	Pb	0.7	Sr	2	Ca	0.5	Y	0.5	Cu	2.3											O	7-Z		1	1992																												Pb1212																			34	40	55	45			40										50																																																													mOhm.cm											27.8													1	mixture - alumina crucible in quartz -  heat(880C, 12H) - Q to RT - wrapped in Au foil - ANN(970C. 3H in O2) - cool to RT (2 C/min)					AN ENHANCEMENT OF TC,FROM 45 K TO 70 K,VIA CD SUBSTITUTION IN(PB,CU)SR2(CA,Y)CU2O7-Z	199205			PHYSICA C,195(1992)35	A.MAIGNAN,B.RAVEAU,C MICHEL,D.A.JEFFERSON,D.GROULT,M.HERVIEU,P.P.EDWARDS,R.S.LIU,S.F.HU	CD,PB,CU,SR,CA,Y,O	
9079	PHC1950035		(Pb,Cd)Sr2(Ca,Y)Cu2O7	Pb0.5Cd0.5Sr2Ca0.5Y0.5Cu2O7-Z	Pb	0.5	Cd	0.5	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	7-Z		1	1992																											2	Pb1212	p4/mmm		A	3.8195		11.9543													58	65	78	70			65										50																																																													mOhm.cm											14.6													1	mixture - alumina crucible in quartz -  heat(880C, 12H) - Q to RT - wrapped in Au foil - ANN(970C. 3H in O2) - cool to RT (2 C/min)					AN ENHANCEMENT OF TC,FROM 45 K TO 70 K,VIA CD SUBSTITUTION IN(PB,CU)SR2(CA,Y)CU2O7-Z	199205			PHYSICA C,195(1992)35	A.MAIGNAN,B.RAVEAU,C MICHEL,D.A.JEFFERSON,D.GROULT,M.HERVIEU,P.P.EDWARDS,R.S.LIU,S.F.HU	CD,PB,CU,SR,CA,Y,O	
9080	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator. O-T transition=913K.	ErBa2Cu3Oz	Er1Ba2Cu3O6.95	Er	1	Ba	2	Cu	3															O	z	6.95	1	2000																											3	Y123			A	3.819	3.887	11.677																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9081	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator. O-T transition=907 K	HoBa2Cu3Oz	Ho1Ba2Cu3O6.87	Ho	1	Ba	2	Cu	3															O	z	6.87	1	2000																											3	Y123			A	3.824	3.89	11.682																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9082	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator.O-T transition=913 K.	YBa2Cu3Oz	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	z	6.91	1	2000																											3	Y123			A	3.824	3.891	11.681																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9083	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator. O-T transition=900 K.	DyBa2Cu3Oz	Dy1Ba2Cu3O6.94	Dy	1	Ba	2	Cu	3															O	z	6.94	1	2000																											3	Y123			A	3.829	3.892	11.692																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9084	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator. O-T transition=871 K.	SmBa2Cu3Oz	Sm1Ba2Cu3O7.06	Sm	1	Ba	2	Cu	3															O	z	7.06	1	2000																											3	Y123			A	3.852	3.909	11.719																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9085	PHC3340295	Young's modulus using 200 kHz LiNbO3 piezoelectric oscilator. O-T transition=834 K.	NdBa2Cu3Oz	Nd1Ba2Cu3O6.87	Nd	1	Ba	2	Cu	3															O	z	6.87	1	2000																											3	Y123			A	3.869	3.921	11.746																																																																																																																		1	solid state reaction					Internal friction of RBa2Cu3Oy (R=Y, Er, Ho, Dy, Sm and Nd) at 200 kHz near orthorhombic-to-tetragonal phase transition	200006		Nagoya Institute of Technology, CRL, Tajimi, Gifu 507-0071, Japan	Physica C,334(2000)295-300	M. Inagaki,M. Ozawa,S. Suzuki,Y. Teshima		
9086	PHC3340237		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2000																												Bi2212																		K		90.4					90.4																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9087	PHC3340237		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.95Pr0.05Cu2Oz	Bi	2	Sr	2	Ca	0.95	Pr	0.05	Cu	2											O	z		3	2000																												Bi2212																		K		91.1					91.1																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9088	PHC3340237		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.87Pr0.13Cu2Oz	Bi	2	Sr	2	Ca	0.87	Pr	0.13	Cu	2											O	z		3	2000																												Bi2212																		K		88.9					88.9																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9089	PHC3340237		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.78Pr0.22Cu2Oz	Bi	2	Sr	2	Ca	0.78	Pr	0.22	Cu	2											O	z		3	2000																												Bi2212																		K		85.5					85.5																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9090	PHC3340237		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2Oz	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	z		3	2000																												Bi2212																		K		81.6					81.6																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9091	PHC3340237	not s/c	Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.5Pr0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Pr	0.5	Cu	2											O	z		3	2000																												Bi2212																							5																																																																																																		Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9092	PHC3340237		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.89Y0.11Cu2Oz	Bi	2	Sr	2	Ca	0.89	Y	0.11	Cu	2											O	z		3	2000																												Bi2212																		K		87.6					87.6																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9093	PHC3340237		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	z		3	2000																												Bi2212																		K		82					82																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9094	PHC3340237		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.69Y0.31Cu2Oz	Bi	2	Sr	2	Ca	0.69	Y	0.31	Cu	2											O	z		3	2000																												Bi2212																		K		70.8					70.8																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9095	PHC3340237		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.59Y0.41Cu2Oz	Bi	2	Sr	2	Ca	0.59	Y	0.41	Cu	2											O	z		3	2000																												Bi2212																		K		56.1					56.1																																																																																																Crystals were grown from Bi2O3-rich melt in Al2O3 crucible					The comparable effects on transport properties in Bi2Sr2Ca1-xPrxCu2Oy and Bi2Sr2Ca1-xYxCu2Oy single crystals	200006		Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C,334(2000)237-242	G.G. Qian,K.Q. Ruan,L.Z. Cao,Q. Cao,S.Y. Li,X.H. Chen		
9096	PHC3340141	as-prepared. Ferromag below curie temp.	(Eu,Ce)2RuSr2Cu2O10	Eu1.5Ce0.5Ru1Sr2Cu2O10	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2											O	10			2000							122																					Ru1222			A	3.846		28.72												K			32				32																																																																																														Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-heat(1000C,1 day in flowing O2)-pellet-SIN(1050C,72H in O2)-FC to RT					Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-z	200006		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Physica C,334(2000)141-151	I. Felner,O. Millo,U. Asaf,Y. Levi		
9097	PHC3340141	ANN(22 atm O2)	(Eu,Ce)2RuSr2Cu2O10	Eu1.5Ce0.5Ru1Sr2Cu2O10	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2											O	10			2000																												Ru1222																		K			38				38																																																																																														Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-heat(1000C,1 day in flowing O2)-pellet-SIN(1050C,72H in O2)-FC to RT					Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-z	200006		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Physica C,334(2000)141-151	I. Felner,O. Millo,U. Asaf,Y. Levi		
9098	PHC3340141	ANN at 75 atm O2. Ferromag below curie temp.	(Eu,Ce)2RuSr2Cu2O10	Eu1.5Ce0.5Ru1Sr2Cu2O10	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2											O	10			2000							168																					Ru1222																		K			46				46																																																																																														Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-heat(1000C,1 day in flowing O2)-pellet-SIN(1050C,72H in O2)-FC to RT					Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-z	200006		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Physica C,334(2000)141-151	I. Felner,O. Millo,U. Asaf,Y. Levi		
9099	PHC3340141	ANN at 150 atm O2. Ferromag below curie temp.	(Eu,Ce)2RuSr2Cu2O10	Eu1.5Ce0.5Ru1Sr2Cu2O10	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2											O	10			2000							225																					Ru1222																		K			49				49																																																																																														Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-heat(1000C,1 day in flowing O2)-pellet-SIN(1050C,72H in O2)-FC to RT					Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-z	200006		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Physica C,334(2000)141-151	I. Felner,O. Millo,U. Asaf,Y. Levi		
9100	PHC3340141	Hydrogen atoms  occupy  intersticial site. Ferromag below curie temp. Resistivity and SQUID show no s/c.	(Eu,Ce)2RuSr2Cu2O10H0.07	Eu1.5Ce0.5Ru1Sr2Cu2H0.07O10	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2	H	0.07									O	10			2000							225																					Ru1222																																																																																																																							Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-heat(1000C,1 day in flowing O2)-pellet-SIN(1050C,72H in O2)-FC to RT					Tuning of the superconducting and ferromagnetic behavior by oxygen and hydrogen in Eu1.5Ce0.5RuSr2Cu2O10-z	200006		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Physica C,334(2000)141-151	I. Felner,O. Millo,U. Asaf,Y. Levi		
9101	PHC3340025	growth axis is normal to c-axis	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2000																												T			A	3.773		13.233												K				39			39																																																																																																floating zone method under 8 atm O2 pressure					Angular dependence of the specific heat of La1.85Sr0.15CuO4 in superconducting mixed state	200006		"Russian Research Centre ""Kurchatov Institute"", Superconductivity and Solid State Physics Institute, Kurchatov Sq. 1, 123182 Moscow, Russia"	Physica C,334(2000)25-32	A.A. Shikov,D.A.Shulyatev,G.Kh. Panova,M.N. Khlopkin,N.A. Chernoplekov		
9102	PHC3340015	not s/c	(Nd,Sr,Ho)2CuO4	Nd1.2Sr0.4Ho0.4Cu1O4-z	Nd	1.2	Sr	0.4	Ho	0.4	Cu	1													O	4-z			2000																												T*			A	3.8321		12.4984												K					4																																																																																																		as-grown sample-ANN(500C,1day,20bar O2)-ANN(500C,1 day, 1400 bar O2)-ANN(800C, 18 H, 1800 bar O2)					T*-type substituted neodymium cuprates Nd1.2Sr0.8xY(Ho, Er, Yb)xCuO4-z: crystal chemistry and electrical conductivity	200006		Centre de Recherche sur la Matiere Divisee, UMR CNRS-Universite, 1B rue de la Ferollerie, 45071 Orleans Cedex 2, France	Physica C,334(2000)15-24	Francoise Archaimbault,Gabriel Caruntu,Jacques Choisnet,Michel Crespin,Paule Mouron		
9103	PHC3340015	not s/c	(Nd,Sr,Y)2CuO4	Nd1.2Sr0.35Y0.45Cu1O4-z	Nd	1.2	Sr	0.35	Y	0.45	Cu	1													O	4-z			2000																												T*																		K					4																																																																																																		as-grown sample-ANN(500C,1day,20bar O2)-ANN(500C,1 day, 1400 bar O2)-ANN(800C, 18 H, 1800 bar O2)					T*-type substituted neodymium cuprates Nd1.2Sr0.8xY(Ho, Er, Yb)xCuO4-z: crystal chemistry and electrical conductivity	200006		Centre de Recherche sur la Matiere Divisee, UMR CNRS-Universite, 1B rue de la Ferollerie, 45071 Orleans Cedex 2, France	Physica C,334(2000)15-24	Francoise Archaimbault,Gabriel Caruntu,Jacques Choisnet,Michel Crespin,Paule Mouron		
9104	PHC3340015	not s/c	(Nd,Sr,Ho)2CuO4	Nd1.2Sr0.37Ho0.43Cu1O4-z	Nd	1.2	Sr	0.37	Ho	0.43	Cu	1													O	4-z			2000																												T*																		K					4																																																																																																		as-grown sample-ANN(500C,1day,20bar O2)-ANN(500C,1 day, 1400 bar O2)-ANN(800C, 18 H, 1800 bar O2)					T*-type substituted neodymium cuprates Nd1.2Sr0.8xY(Ho, Er, Yb)xCuO4-z: crystal chemistry and electrical conductivity	200006		Centre de Recherche sur la Matiere Divisee, UMR CNRS-Universite, 1B rue de la Ferollerie, 45071 Orleans Cedex 2, France	Physica C,334(2000)15-24	Francoise Archaimbault,Gabriel Caruntu,Jacques Choisnet,Michel Crespin,Paule Mouron		
9105	PHC3340015	not s/c	(Nd,Sr,Er)2CuO4	Nd1.2Sr0.4Er0.4Cu1O4-z	Nd	1.2	Sr	0.4	Er	0.4	Cu	1													O	4-z			2000																												T*																		K					4																																																																																																		as-grown sample-ANN(500C,1day,20bar O2)-ANN(500C,1 day, 1400 bar O2)-ANN(800C, 18 H, 1800 bar O2)					T*-type substituted neodymium cuprates Nd1.2Sr0.8xY(Ho, Er, Yb)xCuO4-z: crystal chemistry and electrical conductivity	200006		Centre de Recherche sur la Matiere Divisee, UMR CNRS-Universite, 1B rue de la Ferollerie, 45071 Orleans Cedex 2, France	Physica C,334(2000)15-24	Francoise Archaimbault,Gabriel Caruntu,Jacques Choisnet,Michel Crespin,Paule Mouron		
9106	PHC3310045	not s/c	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		1	2000	emu/mol	0			myu-B/Pr	2.88	-3.6																					Y123																		K					4.2																																																																																																		solid state reaction					Insulator-metal transition by the substitution of Ho, Y or Ca for Pr in PrBa2Cu3O7-z	200004		Institute of Physics, Jagellonian University, Reymonta 4, 30-059 Cracow, Poland	Physica C.331(2000)45-56	A.J.Zaleski,A.W.Pacyna,G.Knebel,M.Balanda,P.Lunkenheimer,Z.Tomkowicz		
9107	PHC3310045	not s/c	PrBa2Cu3O6	Pr1Ba2Cu3O6	Pr	1	Ba	2	Cu	3															O	6		1	2000	emu/mol	0			myu-B/Pr	2.82	0.7																					Y123																		K					4.2																																																																																																		solid state reaction					Insulator-metal transition by the substitution of Ho, Y or Ca for Pr in PrBa2Cu3O7-z	200004		Institute of Physics, Jagellonian University, Reymonta 4, 30-059 Cracow, Poland	Physica C.331(2000)45-56	A.J.Zaleski,A.W.Pacyna,G.Knebel,M.Balanda,P.Lunkenheimer,Z.Tomkowicz		
9108	PHC3310045	not s/c	(Pr,Ca)Ba2Cu3O7	Pr0.7Ca0.3Ba2Cu3O7	Pr	0.7	Ca	0.3	Ba	2	Cu	3													O	7		1	2000	emu/mol	0.00061			myu-B/Pr	3.01	0.6																					Y123																		K					4.2																																																																																																		solid state reaction					Insulator-metal transition by the substitution of Ho, Y or Ca for Pr in PrBa2Cu3O7-z	200004		Institute of Physics, Jagellonian University, Reymonta 4, 30-059 Cracow, Poland	Physica C.331(2000)45-56	A.J.Zaleski,A.W.Pacyna,G.Knebel,M.Balanda,P.Lunkenheimer,Z.Tomkowicz		
9109	SSC1140533	P-induced SC. ladder plane is ac plane. Hc2(0)=3.2T if calculated from dHc2dT and using WHH theory. Measurement carried out at p=4.8 Gpa.	(Sr,Ca)14Cu24O41	Sr2.5Ca11.5Cu24O41	Sr	2.5	Ca	11.5	Cu	24															O	41		3	2000																												LAD																		K		5			0		5																																		HC9109																																																														Traveling solvent floating zone method under 10 atm O2.					Upper critical field of the spin ladder system Sr2.5Ca11.5Cu24O41	200005		Departement de Recherche Fondamentale sur la Matiere Condensee, SPSMS/LCP, CEA/Grenoble, 17 rue des Martyrs, 38054 Grenoble Cedex 9, France	Solid State Commun.,114(2000)533-536	D.Braithwaite,H.Fujino,I.Sheikin,J.Akimitsu,J.Flouquet,T.Nagata		
9110	PHC3360131		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2000																												Bi2212			A			30.849												K	84						84																																																																																																Single crystals were grown by a self-flux method. Cooling rate from melting point to end temperature is 1 C/h.					Growth and characterization of Bi2Sr2Ca1-xGdxCu2Oy single crystals by self-flux method	200007		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C,336(2000)131-136	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
9111	PHC3360131		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.91Gd0.09Cu2Oz	Bi	2	Sr	2	Ca	0.91	Gd	0.09	Cu	2											O	z		3	2000																												Bi2212			A			30.774												K	87						87																																																																																																Single crystals were grown by a self-flux method. Cooling rate from melting point to end temperature is 1 C/h.					Growth and characterization of Bi2Sr2Ca1-xGdxCu2Oy single crystals by self-flux method	200007		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C,336(2000)131-136	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
9112	PHC3360131		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.81Gd0.19Cu2Oz	Bi	2	Sr	2	Ca	0.81	Gd	0.19	Cu	2											O	z		3	2000																												Bi2212			A			30.657												K	83						83																																																																																																Single crystals were grown by a self-flux method. Cooling rate from melting point to end temperature is 1 C/h.					Growth and characterization of Bi2Sr2Ca1-xGdxCu2Oy single crystals by self-flux method	200007		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C,336(2000)131-136	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
9113	PHC3360131		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.68Gd0.32Cu2Oz	Bi	2	Sr	2	Ca	0.68	Gd	0.32	Cu	2											O	z		3	2000																												Bi2212			A			30.562												K	78						78																																																																																																Single crystals were grown by a self-flux method. Cooling rate from melting point to end temperature is 1 C/h.					Growth and characterization of Bi2Sr2Ca1-xGdxCu2Oy single crystals by self-flux method	200007		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C,336(2000)131-136	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
9114	PHC3360131		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.59Gd0.41Cu2Oz	Bi	2	Sr	2	Ca	0.59	Gd	0.41	Cu	2											O	z		3	2000																												Bi2212			A			30.496												K	63.1						63.1																																																																																																Single crystals were grown by a self-flux method. Cooling rate from melting point to end temperature is 1 C/h.					Growth and characterization of Bi2Sr2Ca1-xGdxCu2Oy single crystals by self-flux method	200007		Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C,336(2000)131-136	L. Wang,Q.F. Zhou,W.B. Wu,X. Zhao,X.-G. Li,X.F. Sun		
9115	JSC0920386	not s/c	(Ca,Sr)EuCuO3Cl	Ca0.8Sr0.2Eu1Cu1Cl1O3	Ca	0.8	Sr	0.2	Eu	1	Cu	1	Cl	1											O	3			1991																											2	T*			A	3.898		13.515												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9116	JSC0920386	not s/c	CaEuCuO3Cl	Ca1Eu1Cu1Cl1O3	Ca	1	Eu	1	Cu	1	Cl	1													O	3			1991																											2	T*			A	3.892		13.405												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9117	JSC0920386	not s/c	(Ca,Sr)GdCuO3Cl	Ca0.79Sr0.21Gd1Cu1Cl1O3	Ca	0.79	Sr	0.21	Gd	1	Cu	1	Cl	1											O	3			1991																											2	T*			A	3.893		13.517												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9118	JSC0920386	not s/c	CaGdCuO3Cl	Ca1Gd1Cu1Cl1O3	Ca	1	Gd	1	Cu	1	Cl	1													O	3			1991																											2	T*			A	3.888		13.389												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9119	JSC0920386	not s/c	SrNdCuO3Cl	Sr1Nd1Cu1Cl1O3	Sr	1	Nd	1	Cu	1	Cl	1													O	3			1991																											2	T*			A	3.956		13.88												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9120	JSC0920386	not s/c	(Ca,Sr)NdCuO3Cl	Ca0.72Sr0.28Nd1Cu1Cl1O3	Ca	0.72	Sr	0.28	Nd	1	Cu	1	Cl	1											O	3			1991							-10																				2	T*			A	3.926		13.665												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9121	JSC0920386	not s/c	(Ca,Sr)SmCuO3Cl	Ca0.78Sr0.22Sm1Cu1Cl1O3	Ca	0.78	Sr	0.22	Sm	1	Cu	1	Cl	1											O	3			1991																											2	T*			A	3.91		13.559												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9122	JSC0920386	not s/c	CaSmCuO3Cl	Ca1Sm1Cu1Cl1O3	Ca	1	Sm	1	Cu	1	Cl	1													O	3			1991							-5.3																				2	T*			A	3.901		13.43												K					4.2																																																																																																CuO,Ln2O3,SrO,CaO,SrCl2,CaCl2	1	pellet-SIN(820C,18H)					Synthesis,Structure, and Properties of a New T* Structure Copper-Oxychloride of MLnCuO3Cl (M=Ca,Sr and Ln=Nd,Sm,Eu,Gd)	199105		Rutgers,The State University of New Jersey, Piscataway, New Jersey 08855	J.Solid State Chem.,92(1991)386-400	Martha Greenblatt,Robert L.Fuller		
9123	PHC3360033	not s/c	(Li,Cu)Sr2YCu2Oz	Li0.33Sr2Y1Cu2.67Oz	Li	0.33	Sr	2	Y	1	Cu	2.67													O	z		2	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9124	PHC3360033	not s/c	(Co,Cu)Sr2YCu2Oz	Co0.33Sr2Y1Cu2.67Oz	Co	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9125	PHC3360033	not s/c	(Ni,Cu)Sr2YCu2Oz	Ni0.33Sr2Y1Cu2.67Oz	Ni	0.33	Sr	2	Y	1	Cu	2.67													O	z		2	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9126	PHC3360033	not s/c	(Zn,Cu)Sr2YCu2Oz	Zn0.33Sr2Y1Cu2.67Oz	Zn	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9127	PHC3360033	not s/c	(Pd,Cu)Sr2YCu2Oz	Pd0.33Sr2Y1Cu2.67Oz	Pd	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9128	PHC3360033	not s/c	(Al,Cu)Sr2YCu2Oz	Al0.33Sr2Y1Cu2.67Oz	Al	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9129	PHC3360033		(Fe,Cu)Sr2YCu2Oz	Fe0.33Sr2Y1Cu2.67Oz	Fe	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		30					30																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9130	PHC3360033		(Ga,Cu)Sr2YCu2Oz	Ga0.33Sr2Y1Cu2.67Oz	Ga	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		25					25																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9131	PHC3360033	not s/c	(Cr,Cu)Sr2YCu2Oz	Cr0.33Sr2Y1Cu2.67Oz	Cr	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9132	PHC3360033	not s/c	(In,Cu)Sr2YCu2Oz	In0.33Sr2Y1Cu2.67Oz	In	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9133	PHC3360033	not s/c	(Bi,Cu)Sr2YCu2Oz	Bi0.33Sr2Y1Cu2.67Oz	Bi	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9134	PHC3360033	not s/c	(Se,Cu)Sr2YCu2Oz	Se0.33Sr2Y1Cu2.67Oz	Se	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9135	PHC3360033	not s/c	(Ge,Cu)Sr2YCu2Oz	Ge0.33Sr2Y1Cu2.67Oz	Ge	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9136	PHC3360033		(Ti,Cu)Sr2YCu2Oz	Ti0.33Sr2Y1Cu2.67Oz	Ti	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		26					26																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9137	PHC3360033	not s/c	(Ru,Cu)Sr2YCu2Oz	Ru0.33Sr2Y1Cu2.67Oz	Ru	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9138	PHC3360033	not s/c	(Pt,Cu)Sr2YCu2Oz	Pt0.33Sr2Y1Cu2.67Oz	Pt	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9139	PHC3360033	not s/c	(Sn,Cu)Sr2YCu2Oz	Sn0.33Sr2Y1Cu2.67Oz	Sn	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9140	PHC3360033	not s/c	(Zr,Cu)Sr2YCu2Oz	Zr0.33Sr2Y1Cu2.67Oz	Zr	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9141	PHC3360033	not s/c	(V,Cu)Sr2YCu2Oz	V0.33Sr2Y1Cu2.67Oz	V	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9142	PHC3360033	not s/c	(Nb,Cu)Sr2YCu2Oz	Nb0.33Sr2Y1Cu2.67Oz	Nb	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9143	PHC3360033	not s/c	(Ta,Cu)Sr2YCu2Oz	Ta0.33Sr2Y1Cu2.67Oz	Ta	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9144	PHC3360033		(Mo,Cu)Sr2YCu2Oz	Mo0.33Sr2Y1Cu2.67Oz	Mo	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		35					35																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9145	PHC3360033		(W,Cu)Sr2YCu2Oz	W0.33Sr2Y1Cu2.67Oz	W	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		28					28																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9146	PHC3360033		(Re,Cu)Sr2YCu2Oz	Re0.33Sr2Y1Cu2.67Oz	Re	0.33	Sr	2	Y	1	Cu	2.67													O	z		1	2000																												M1212																		K		33					33																																																																																																pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9147	PHC3360033	not s/c	(Os,Cu)Sr2YCu2Oz	Os0.33Sr2Y1Cu2.67Oz	Os	0.33	Sr	2	Y	1	Cu	2.67													O	z			2000																												M1212																		K					20																																																																																																		pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9148	PHC3360033	Susceptibility anomalies at 56,96,108,160,197 K are found. Resistivity drop at about 60K, but not s/c	(As,Cu)Sr2YCu2Oz	As0.33Sr2Y1Cu2.67O6.88	As	0.33	Sr	2	Y	1	Cu	2.67													O	z	6.88		2000																											2	M1212	P4/mmm		A	3.829		11.47												K																																																																																																							pellet-SIN(850-1000C,10H, in air)-Q to RT					Synthesis of (M0.33Cu0.67)Sr2YCu2Oy: a novel layered cuprate with a block layer of (As0.33Cu0.67)O0.88	200007		Graduate School of Science and Engineering, Yamagata University, 4-3-16, Jonan, Yonezawa, Yamagata 992-8510, Japan	Physica C,336(2000)33-42	Eiji Sato,Kenji Hiraga,Osamu Ishii,Shiro Kambe,Takahiro Akao,Tetsu Ohsuna		
9150	SSC1130121	z-values by iodometric titration. Grain size about 6-9 micron. Specific heat by ac calorimeter. Tc=43 K. dC/Tc=7.35 mj/mol.K2	La2CuO4	La2Cu1O4.093	La	2	Cu	1																	O	4+z	4.093		1999																											3	T																		K		45					45																																																						mj/mol.K	320																																									solid state reaction-electro chemical oxidation (330K, 72H)					Observation of specific heat jump in La2CuO4.093 due to superconducting transition	199912		Faculty of Science, Himeji Institute of Technology, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan	Solid State Commun.,113(1999)121-124	M. Nakagawa,T. Hirayama,Y. Oda		
9151	PHC3340289	not s/c	La2CuOz	La2Cu1O3.998	La	2	Cu	1																	O	4+z	3.998	1	2000																											3	T																		K																																																																																																		RH9151					as-grown 					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9152	PHC3340289		La2CuOz	La2Cu1O4.068	La	2	Cu	1																	O	4+z	4.068	1	2000																												T																		K		36					36																																																																																											RH9152					electro-chemical oxidation(333K, 24H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9153	PHC3340289	second Tc=32 K	La2CuOz	La2Cu1O4.093	La	2	Cu	1																	O	4+z	4.093	1	2000																											3	T																		K		45					45																																																																																											RH9153					electro-chemical oxidation(333K, 72H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9154	PHC3340289		(La,Sr)2CuOz	La1.9Sr0.1Cu1O3.997	La	1.9	Sr	0.1	Cu	1															O	4+z	3.997	1	2000																											2	T																		K		32					32																																																																																																as-grown 					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9155	PHC3340289	second Tc=32 K	(La,Sr)2CuOz	La1.9Sr0.1Cu1O4.018	La	1.9	Sr	0.1	Cu	1															O	4+z	4.018	1	2000																												T																		K		40					40																																																																																																electro-chemical oxidation(333K, 24H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9156	PHC3340289	second Tc=32 K	(La,Sr)2CuOz	La1.9Sr0.1Cu1O4.023	La	1.9	Sr	0.1	Cu	1															O	4+z	4.023	1	2000																											2	T																		K		40					40																																																																																																electro-chemical oxidation(333K, 72H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9157	PHC3360143		Tl2Ba2CaCu2Oz	Tl2Ba2Ca1Cu2Oz	Tl	2	Ba	2	Ca	1	Cu	2													O	z		3	2000																												Tl2212			A	3.8509		29.372												K				105			105																																		HIR9157																																																														Single crystals were grown from stoichiometric mixture.					New Tl/Hg-2212 and -2223 superconducting crystals: growth, structures and superconductivity	200007		Laboratoire CRISMAT, UMR 6508, CNRS, ISMRA et Universite de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,336(2000)143-150	A. Maignan,C. Martin,D. Pelloquin,D. Thopart,J. Hejtmanek		
9158	PHC3360143	Compositions are Tl1.68Hg0.32Ba2Ca0.9Tl0.1Cu2Oz by EDS analysis.	(Tl,Hg)2Ba2CaCu2Oz	Tl1.7Hg0.3Ba2Ca1Cu2Oz	Tl	1.7	Hg	0.3	Ba	2	Ca	1	Cu	2											O	z		3	2000																												Tl2212			A															K				108			108																																		HIR9158																																																														Single crystals were grown from (Tl1.7Hg0.3)-2212.					New Tl/Hg-2212 and -2223 superconducting crystals: growth, structures and superconductivity	200007		Laboratoire CRISMAT, UMR 6508, CNRS, ISMRA et Universite de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,336(2000)143-150	A. Maignan,C. Martin,D. Pelloquin,D. Thopart,J. Hejtmanek		
9159	PHC3360143		Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3Oz	Tl	2	Ba	2	Ca	2	Cu	3													O	z		3	2000																												Tl2223			A	3.8472		35.836												K				123			123																																		HIR9159																																																														Single crystals were grown from stoichiometric mixture.					New Tl/Hg-2212 and -2223 superconducting crystals: growth, structures and superconductivity	200007		Laboratoire CRISMAT, UMR 6508, CNRS, ISMRA et Universite de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,336(2000)143-150	A. Maignan,C. Martin,D. Pelloquin,D. Thopart,J. Hejtmanek		
9160	PHC3360143	Compositions are Tl1.46Hg0.54Ba2Ca2Cu3Oz by EDS analysis.	(Tl,Hg)2Ba2Ca2Cu3Oz	Tl1.4Hg0.6Ba2Ca2Cu3Oz	Tl	1.4	Hg	0.6	Ba	2	Ca	2	Cu	3											O	z		3	2000																												Tl2223			A															K				118			118																																		HIR9160																																																														Single crystals were grown from (Tl1.4Hg0.6)-2223.					New Tl/Hg-2212 and -2223 superconducting crystals: growth, structures and superconductivity	200007		Laboratoire CRISMAT, UMR 6508, CNRS, ISMRA et Universite de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Physica C,336(2000)143-150	A. Maignan,C. Martin,D. Pelloquin,D. Thopart,J. Hejtmanek		
9161	PHC3340289		(La,Sr)2CuOz	La1.85Sr0.15Cu1O3.998	La	1.85	Sr	0.15	Cu	1															O	4+z	3.998	1	2000																											2	T																		K		37					37																																																																																											RH9161					as-grown 					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9162	PHC3340289		(La,Sr)2CuOz	La1.85Sr0.15Cu1O4.022	La	1.85	Sr	0.15	Cu	1															O	4+z	4.022	1	2000																												T																		K		40					40																																																																																																electro-chemical oxidation(333K, 24H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9163	PHC3340289		(La,Sr)2CuOz	La1.85Sr0.15Cu1O4.03	La	1.85	Sr	0.15	Cu	1															O	4+z	4.03	1	2000																											2	T																		K		40					40																																																																																																electro-chemical oxidation(333K, 72H)					Hall effect in electrochemically oxidized La2CuO4+z and (La1-xSrx)2CuO4+z	200006		Faculty of Science, Himeji Institute of Technology, 3-2-1, Kouto, Kamigori-cho, Ako-gun, Hyogo 678-1297, Japan 		Masahito Nakagawa,Toshikazu Hirayama,Yasukage Oda		
9165	APJ0393366		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		1	2000																											2	T'			A	3.953		12.129												K				17			17																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9166	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.8315Y0.0185Ce0.15Cu1O4	Pr	1.8315	Y	0.0185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.952		12.126												K				16			16																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9167	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.7945Y0.0555Ce0.15Cu1O4	Pr	1.7945	Y	0.0555	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.95		12.11												K				15			15																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9168	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.7575Y0.0925Ce0.15Cu1O4	Pr	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.948		12.105												K				14.5			14.5																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9169	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.665Y0.185Ce0.15Cu1O4	Pr	1.665	Y	0.185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.944		12.069												K				13			13																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9170	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.5725Y0.2775Ce0.15Cu1O4	Pr	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.94		12.046												K				11			11																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9171	APJ0393366		(Pr,Y,Ce)2CuO4	Pr1.48Y0.37Ce0.15Cu1O4	Pr	1.48	Y	0.37	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.936		12.022												K				9.5			9.5																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9172	APJ0393366	not s/c	(Pr,Y,Ce)2CuO4	Pr1.295Y0.555Ce0.15Cu1O4	Pr	1.295	Y	0.555	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.937		12.023												K					2																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9173	APJ0393366		(Nd,Ce)2CuO4	Nd1.85Y0.15Cu1O4	Nd	1.85	Y	0.15	Cu	1															O	4		1	2000																											2	T'			A	3.939		12.053												K				21			21																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9174	APJ0393366		(Nd,Y,Ce)2CuO4	Nd1.8315Y0.0185Ce0.15Cu1O4	Nd	1.8315	Y	0.0185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.938		12.04												K				20			20																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9175	APJ0393366		(Nd,Y,Ce)2CuO4	Nd1.7945Y0.0555Ce0.15Cu1O4	Nd	1.7945	Y	0.0555	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.935		12.025												K				19			19																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9176	APJ0393366		(Nd,Y,Ce)2CuO4	Nd1.7575Y0.0925Ce0.15Cu1O4	Nd	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.934		12.014												K				18			18																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9177	APJ0393366		(Nd,Y,Ce)2CuO4	Nd1.665Y0.185Ce0.15Cu1O4	Nd	1.665	Y	0.185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.929		11.999												K				16			16																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9178	APJ0393366		(Nd,Y,Ce)2CuO4	Nd1.5725Y0.2775Ce0.15Cu1O4	Nd	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.926		11.983												K				10.5			10.5																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9179	APJ0393366	not s/c	(Nd,Y,Ce)2CuO4	Nd1.48Y0.37Ce0.15Cu1O4	Nd	1.48	Y	0.37	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.922		11.953												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9180	APJ0393366	not s/c	(Nd,Y,Ce)2CuO4	Nd1.295Y0.555Ce0.15Cu1O4	Nd	1.295	Y	0.555	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.922		11.961												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9181	APJ0393366		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4		1	2000																											2	T'			A	3.912		11.874												K				17			17																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9182	APJ0393366		(Sm,Y,Ce)2CuO4	Sm1.80375Y0.04625Ce0.15Cu1O4	Sm	1.80375	Y	0.04625	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.91		11.868												K				15			15																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9183	APJ0393366		(Sm,Y,Ce)2CuO4	Sm1.7575Y0.0925Ce0.15Cu1O4	Sm	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.909		11.865												K				14			14																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9184	APJ0393366		(Sm,Y,Ce)2CuO4	Sm1.71125Y0.13875Ce0.15Cu1O4	Sm	1.71125	Y	0.13875	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.907		11.852												K				12			12																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9185	APJ0393366		(Sm,Y,Ce)2CuO4	Sm1.665Y0.185Ce0.15Cu1O4	Sm	1.665	Y	0.185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.906		11.845												K				10			10																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9186	APJ0393366	not s/c	(Sm,Y,Ce)2CuO4	Sm1.5725Y0.2775Ce0.15Cu1O4	Sm	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.905		11.838												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9187	APJ0393366		(Eu,Ce)2CuO4	Eu1.85Ce0.15Cu1O4	Eu	1.85	Ce	0.15	Cu	1															O	4		1	2000																											2	T'			A	3.901		11.826												K				7.5			7.5																																																																																														Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9188	APJ0393366		(Eu,Y,Ce)2CuO4	Eu1.80375Y0.04625Ce0.15Cu1O4	Eu	1.80375	Y	0.04625	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.9		11.816												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9189	APJ0393366		(Eu,Y,Ce)2CuO4	Eu1.7575Y0.0925Ce0.15Cu1O4	Eu	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.9		11.81												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9190	APJ0393366		(Eu,Y,Ce)2CuO4	Eu1.71125Y0.13875Ce0.15Cu1O4	Eu	1.71125	Y	0.13875	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.899		11.809												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9191	APJ0393366		(Eu,Y,Ce)2CuO4	Eu1.665Y0.185Ce0.15Cu1O4	Eu	1.665	Y	0.185	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.897		11.807												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9192	APJ0393366		(Eu,Y,Ce)2CuO4	Eu1.5725Y0.2775Ce0.15Cu1O4	Eu	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4		1	2000																											2	T'			A	3.896		11.806												K					5																																																																																																Pr6O11,Nd2O3,Sm2O3,Eu2O3,CeO2,CuO	1	mixture-heat(900C,24H in air)-pellet-heat(1000C, 48H, in air)-Q to RT-ANN(850C-950C,2H in air)					Structural and Magnetic Properties of (R1-xYx)1.85Ce0.15CuO4 (R=Pr, Nd, Sm and Eu)	6		Department of Electrical Engineering, Southern Taiwan University of Technology, Tainan 710, Taiwan, R.O.C.	Jpn J.Appl.Phys., 39(2000)3366-3370	Teen-Hang Meen		
9193	JPC0128231		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu1Oz	La	1.85	Sr	0.15	Cu	1															O	z			2000																												T																		K				38			38																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9194	JPC0128231		(La,Sr)2(Cu,Fe)O4	La1.845Sr0.155Cu0.995Fe0.005Oz	La	1.845	Sr	0.155	Cu	0.995	Fe	0.005													O	z			2000																												T																		K				30			30																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9195	JPC0128231		(La,Sr)2(Cu,Fe)O4	La1.84Sr0.16Cu0.99Fe0.01Oz	La	1.84	Sr	0.16	Cu	0.99	Fe	0.01													O	z			2000																												T																		K				20			20																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9196	JPC0128231		(La,Sr)2(Cu,Fe)O4	La1.837Sr0.163Cu0.987Fe0.013Oz	La	1.837	Sr	0.163	Cu	0.987	Fe	0.013													O	z			2000																												T																		K				12.8			12.8																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9197	JPC0128231		(La,Sr)2(Cu,Ga)O4	La1.845Sr0.155Cu0.995Ga0.005Oz	La	1.845	Sr	0.155	Cu	0.995	Ga	0.005													O	z			2000																												T																		K				32			32																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9198	JPC0128231		(La,Sr)2(Cu,Ga)O4	La1.84Sr0.16Cu0.99Ga0.01Oz	La	1.84	Sr	0.16	Cu	0.99	Ga	0.01													O	z			2000																												T																		K				26			26																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9199	JPC0128231		(La,Sr)2(Cu,Ga)O4	La1.83Sr0.17Cu0.98Ga0.02Oz	La	1.83	Sr	0.17	Cu	0.98	Ga	0.02													O	z			2000																												T																		K				13			13																																																																																															1	mixture-CAL(1000C)-pellet-SIN(1030-1100C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9200	JPC0128231		(Bi,Pb)2(Sr,La)2(Cu,Fe)Oz	Bi1.8Pb0.2Sr1.6La0.4Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.6	La	0.4	Cu	1											O	z		1	2000																												Bi2201																		K				31.2			31.2																																																																																															1	mixture-CAL(800-850C,40H, in air)-pellet-SIN(880C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9201	JPC0128231		(Bi,Pb)2(Sr,La)2(Cu,Fe)Oz	Bi1.8Pb0.2Sr1.62La0.38Cu0.98Fe0.02Oz	Bi	1.8	Pb	0.2	Sr	1.62	La	0.38	Cu	0.98	Fe	0.02									O	z		1	2000																												Bi2201																		K				21.1			21.1																																																																																															1	mixture-CAL(800-850C,40H, in air)-pellet-SIN(880C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9202	JPC0128231		(Bi,Pb)2(Sr,La)2(Cu,Fe)Oz	Bi1.8Pb0.2Sr1.63La0.37Cu0.97Fe0.03Oz	Bi	1.8	Pb	0.2	Sr	1.63	La	0.37	Cu	0.97	Fe	0.03									O	z		1	2000																												Bi2201																		K				13			13																																																																																															1	mixture-CAL(800-850C,40H, in air)-pellet-SIN(880C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9203	JPC0128231		(Bi,Pb)2(Sr,La)2(Cu,Ga)Oz	Bi1.8Pb0.2Sr1.61La0.39Cu0.99Ga0.01Oz	Bi	1.8	Pb	0.2	Sr	1.61	La	0.39	Cu	0.99	Ga	0.01									O	z		1	2000																												Bi2201																		K				21.8			21.8																																																																																															1	mixture-CAL(800-850C,40H, in air)-pellet-SIN(880C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9204	JPC0128231		(Bi,Pb)2(Sr,La)2(Cu,Ga)Oz	Bi1.8Pb0.2Sr1.62La0.38Cu0.98Ga0.02Oz	Bi	1.8	Pb	0.2	Sr	1.62	La	0.38	Cu	0.98	Ga	0.02									O	z		1	2000																												Bi2201																		K				12			12																																																																																															1	mixture-CAL(800-850C,40H, in air)-pellet-SIN(880C)-FC to RT					Different effects of Fe and Ga doping on Tc between the Bi2201 system and the La214 system			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys. C, 12(2000)8231-8238	Ding Zejun,Pu Qirong,Xu Gaojie,Zhang Yuheng		
9205	APL0763795	EDX gives Bi:Pb:Sr:Ca:Cu:Cr=1.65:0.79:2.1:1:1.96:0.01. For Hirr  H//c-axis.	(Bi,Pb)2Sr2Ca(Cu,Cr)2O8	Bi1.6Pb0.8Sr2Ca1Cu1.99Cr0.01Oz	Bi	1.6	Pb	0.8	Sr	2	Ca	1	Cu	1.99	Cr	0.01									O	z		3	2000																												Bi2212			A			30.794												K				68		2	68																																		HIR9205																																																														self-flux method. Annealed at 500C in air for 5 days					Improved flux pinning and anomalous magnetization peak in heavily overdoped Bi2-xPbxSr2CaCu2-yCryO8 +z  single crystals	6		Laboratory of Internal Friction and Defects in Solids, Institute of Solid State Physics, Chinese Academy of Science, Hefei 230031, China	Appl.Phys.Lett.,76(2000)3795-3797	B.Zhao,H.C.Ku,H.H.Wen,J.J.Du,W.H.Song,Y.P.Sun,Z.X.Zhao		
9206	APL0763795		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2000																												Bi2212																		K				88			88																																		HIR9206																																																														self-flux method. Annealed at 500C in air for 5 days					Improved flux pinning and anomalous magnetization peak in heavily overdoped Bi2-xPbxSr2CaCu2-yCryO8 +z  single crystals	6		Laboratory of Internal Friction and Defects in Solids, Institute of Solid State Physics, Chinese Academy of Science, Hefei 230031, China	Appl.Phys.Lett.,76(2000)3795-3797	B.Zhao,H.C.Ku,H.H.Wen,J.J.Du,W.H.Song,Y.P.Sun,Z.X.Zhao		
9207	PRL0844192	Tc was measured by torque magnetometer. Isotope effect on penetration depth was measured but values of xi were not given.	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		3	2000																												T																		K		19.6					19.6						0.47	O	97	1.13																																																																																							Floating zone method. Oxygen substitution by diffusion process in O<16> or O<18> atmosphere.					Oxygen-Isotope Effect on the In-Plane Penetration Depth in Underdoped La2-xSrxCuO4 Single Crystals	5		Physik-Institut der Universitut Z?rich, Winterthurerstrasse 190, CH-8057 Z?rich, Switzerland	Phys.Rev.Lett., 84(2000)4192-4195	Guo-meng Zhao,H.Keller,J.Hofer,K.Conder,K.Kishio,M.Willemin,T.Sasagawa		
9208	PRL0844192	Tc was measured by torque magnetometer. Isotope effect on penetration depth was measured but values of xi were not given.	(La,Sr)2CuO4	La1.914Sr0.086Cu1O4	La	1.914	Sr	0.086	Cu	1															O	4		3	2000																												T																		K		22.25					22.25						0.4	O	97	1.07																																																																																							Floating zone method. Oxygen substitution by diffusion process in O<16> or O<18> atmosphere.					Oxygen-Isotope Effect on the In-Plane Penetration Depth in Underdoped La2-xSrxCuO4 Single Crystals	5		Physik-Institut der Universitut Z?rich, Winterthurerstrasse 190, CH-8057 Z?rich, Switzerland	Phys.Rev.Lett., 84(2000)4192-4195	Guo-meng Zhao,H.Keller,J.Hofer,K.Conder,K.Kishio,M.Willemin,T.Sasagawa		
9209	PRL0800377	Isotope effect of Tc by M(T). Isotope effect of pseudo gap onset temp T* by Y<89> NMR. T* is no isotope  effect.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1998																												Y124																		K				81.8			81.8						0.076	O	90																																																																																								High-pressure synthesis (945C, 60 bar O2)-ANN(O<18> or O<16> atmosphere, 760C, 4H)					Absence of an Isotope Effect in the Pseudogap in YBa2Cu4O8 as Determined by Hugh-Resolution 89Y NMR	1		New Zealand Institute for Industrial Research, P.O. Box 31310, Lower Hutt, New zealand	Phys.Rev.Lett.,80(1998)377-380	G.V.M. Williams,H.J. Trodahl,J.L. Tallon,J.W. Quilty,N.E. Flower		
9210	PRL0815912	Isotope effect on Tc and pseudo gap onset temp. T* by Cu-NQR. Alpha for T* is 0.061.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1998																												Y124																		K				81			81						0.056	O	88	0.47																																																																																							Y-124 by solid state reaction - ANN(725C, 1.3 bar O2 in a sealed ampoule)					Isotope Dependence of the Spin Gap in YBa2Cu4O8 as Determined by Cu NQR Relaxation	199812		Physik-Institut, Universitut Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 81(1998)5912-5915	D.Brinkmann,F.Raffa,J.Roos,K.Conder,M.Eremin,M.Mali,T.Ohno		
9211	PRL0841990	Pseudogap onset temp. T* = 170 K for O<16> sample. T* = 220 K for O<18> sample.	HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8			2000																												Y124																		K				79			79						0.005	O	75	0.5																																																																																							O<16> sample was prepared by a high O2 pressure solid reaction process. O<18> substitution was performed by diffusion process.					Large Isotope Effect on the Pseudogap in the High-Temperature Superconductor HoBa2Cu4O8	2		Laboratory for Neutron Scattering, ETH Zurich and PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 84(2000)1990-1993	A.Furrer,D.Rubio Temprano,H.Mutka,J.Mesot,K.A.Muller,K.Konder,S.Janssen		
9212	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	7-z	6.98	1	1998																												Y123																		K		92					92																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9213	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba1.96Sr0.04Cu3O6.98	Y	1	Ba	1.96	Sr	0.04	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		91.8					91.8																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9214	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba1.8Sr0.2Cu3O6.98	Y	1	Ba	1.8	Sr	0.2	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		89					89																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9215	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba1.5Sr0.5Cu3O6.98	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		86					86																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9216	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba1.3Sr0.7Cu3O6.98	Y	1	Ba	1.3	Sr	0.7	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		84.5					84.5																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9217	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba1Sr1Cu3O6.98	Y	1	Ba	1	Sr	1	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		83.6					83.6																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9218	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba0.74Sr1.26Cu3O6.98	Y	1	Ba	0.74	Sr	1.26	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		80.5					80.5																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9219	PR05815208		Y(Ba,Sr)2Cu3O7	Y1Ba0.5Sr1.5Cu3O6.98	Y	1	Ba	0.5	Sr	1.5	Cu	3													O	7-z	6.98	1	1998																												Y123																		K		78					78																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9220	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.72	Y	1	Ba	2	Cu	3															O	7-z	6.72	1	1998																												Y123																		K		64.6					64.6																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9221	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	7-z	6.75	1	1998																												Y123																		K		76.6					76.6																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9222	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	1	1998																												Y123																		K		88.3					88.3																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9223	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	7-z	6.85	1	1998																												Y123																		K		89					89																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9224	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.89	Y	1	Ba	2	Cu	3															O	7-z	6.89	1	1998																												Y123																		K		92.1					92.1																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9225	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-z	6.93	1	1998																												Y123																		K		93.1					93.1																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9226	PR05815208		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-z	6.96	1	1998																												Y123																		K		91.4					91.4																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9227	PR05815208		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.75	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.75	1	1998																												Y123																		K		49.9					49.9																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9228	PR05815208		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.85	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.85	1	1998																												Y123																		K		72.9					72.9																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9229	PR05815208		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.9	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.9	1	1998																												Y123																		K		86.3					86.3																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9230	PR05815208		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.91	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.91	1	1998																												Y123																		K		86.3					86.3																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9231	PR05815208		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.95	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.95	1	1998																												Y123																		K		85.9					85.9																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9232	PR05815208		YBaSrCu3Oz	Y1Ba1Sr1Cu3O6.83	Y	1	Ba	1	Sr	1	Cu	3													O	7-z	6.83	1	1998																												Y123																		K		58.5					58.5																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9233	PR05815208		YBaSrCu3Oz	Y1Ba1Sr1Cu3O6.88	Y	1	Ba	1	Sr	1	Cu	3													O	7-z	6.88	1	1998																												Y123																		K		75.6					75.6																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9234	PR05815208		YBaSrCu3Oz	Y1Ba1Sr1Cu3O6.93	Y	1	Ba	1	Sr	1	Cu	3													O	7-z	6.93	1	1998																												Y123																		K		80.8					80.8																																																																																																See  PREPID=19254					Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
9235	PR05914099	Density is calculated from lattice parameters	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	1999							133		6.7																		2	Ru1212			A	3.84		11.57												K	16						16		1																																																																				TP9235																								RuO2,SrCO3,Gd2O3,CuO	1	mixture-SIN(1010C, flowing N2)-Sr2GdRuO6 add Cu2O-react(1050C,10H in O2 flow) on MgO single crystal					Coexistence of ferromagnetism and superconductivity in the hybrid ruthenate-cuprate compound RuSr2GdCu2O8 studied by muon spin rotation and dc magnetization	199906		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.B, 59(1999)14099-14107	A.Golnik,C.Bemhard,C.E.Stronach,Ch.Niedermayer,D.R.Noakes,E.Brocher,E.J.Ansaldo,J.L.Tallon,R.K.Kremer,Th.Blasius		
9236	PHC3380025	average grain size = 3.0+-0.5 micron meter	CuBa2YbCu2Oz	Ba2Yb1Cu3O6+z	Ba	2	Yb	1	Cu	3															O	6+z		1	2000																											3	Cu1212			A	3.795	3.879	11.61												K				90.1			90.1																																		HIR9236																																																													1	mixture-CAL(900-940C,60H)-ANN(300C,48H in O2)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9237	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.8Sr0.2Yb1Cu3O6+z	Ba	1.8	Sr	0.2	Yb	1	Cu	3													O	6+z		1	2000																											3	Cu1212			A	3.792	3.872	11.6												K				85.6			85.6																																		HIR9237																																																													1	mixture-CAL(900-940C,60H)-ANN(300C,48H in O2)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9238	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.6Sr0.4Yb1Cu3O6+z	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z		1	2000																											3	Cu1212			A	3.789	3.865	11.59												K				79.5			79.5																																		HIR9238																																																													1	mixture-CAL(900-940C,60H)-ANN(300C,48H in O2)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9239	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.4Sr0.6Yb1Cu3O6+z	Ba	1.4	Sr	0.6	Yb	1	Cu	3													O	6+z		1	2000																											3	Cu1212			A	3.785	3.859	11.56												K				77.9			77.9																																		HIR9239																																																													1	mixture-CAL(900-940C,60H)-ANN(300C,48H in O2)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9240	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.2Sr0.8Yb1Cu3O6+z	Ba	1.2	Sr	0.8	Yb	1	Cu	3													O	6+z		1	2000																											3	Cu1212			A	3.78	3.853	11.53												K				78.5			78.5																																		HIR9240																																																													1	mixture-CAL(900-940C,60H)-ANN(300C,48H in O2)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9241	PHC3380025		CuBa2YbCu2Oz	Ba2Yb1Cu3O6.66	Ba	2	Yb	1	Cu	3															O	6+z	6.66	1	2000																											3	Cu1212			A	3.814	3.873	11.7												K				65.3			65.3																																		HIR9241																																																													1	mixture-CAL(900-940C,60H, in O2)-ANN(400C, in Ar)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9242	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.8Sr0.2Yb1Cu3O6.61	Ba	1.8	Sr	0.2	Yb	1	Cu	3													O	6+z	6.61	1	2000																											3	Cu1212			A	3.81	3.868	11.67												K				56.7			56.7																																		HIR9242																																																													1	mixture-CAL(900-940C,60H, in O2)-ANN(400C, in Ar)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9243	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.6Sr0.4Yb1Cu3O6.69	Ba	1.6	Sr	0.4	Yb	1	Cu	3													O	6+z	6.69	1	2000																											3	Cu1212			A	3.806	3.861	11.65												K				48.9			48.9																																		HIR9243																																																													1	mixture-CAL(900-940C,60H, in O2)-ANN(400C, in Ar)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9244	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.4Sr0.6Yb1Cu3O6.66	Ba	1.4	Sr	0.6	Yb	1	Cu	3													O	6+z	6.66	1	2000																											3	Cu1212			A	3.802	3.852	11.62												K				43.1			43.1																																		HIR9244																																																													1	mixture-CAL(900-940C,60H, in O2)-ANN(400C, in Ar)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9245	PHC3380025		Cu(Ba,Sr)2YbCu2Oz	Ba1.2Sr0.8Yb1Cu3O6.61	Ba	1.2	Sr	0.8	Yb	1	Cu	3													O	6+z	6.61	1	2000																											3	Cu1212			A	3.801	3.851	11.59												K				36.7			36.7																																		HIR9245																																																													1	mixture-CAL(900-940C,60H, in O2)-ANN(400C, in Ar)					Effects of Sr substitution on the magnetic-field irreversibility in superconductive Cu(Ba1ySry)2YbCu2O6+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica C, 338(2000)25-28	E.S.Otabe,H.Yamauchi,M.Karppinen,T. Nakane,T.Matsushita,Y.Yasukawa		
9246	PHC2030240		(La,Ba)2CuO4	La1.934Ba0.066Cu1O4	La	1.934	Ba	0.066	Cu	1															O	4			1992																												T																		K				22.6			22.6																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9247	PHC2030240		(La,Ba)2CuO4	La1.93Ba0.07Cu1O4	La	1.93	Ba	0.07	Cu	1															O	4			1992																												T																		K				23.4			23.4																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9248	PHC2030240		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4			1992																												T																		K				26			26																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9249	PHC2030240		(La,Ba)2CuO4	La1.897Ba0.103Cu1O4	La	1.897	Ba	0.103	Cu	1															O	4			1992																												T																		K				14.5			14.5																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9250	PHC2030240		(La,Ba)2CuO4	La1.892Ba0.108Cu1O4	La	1.892	Ba	0.108	Cu	1															O	4			1992																												T																		K				10.7			10.7																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9251	PHC2030240		(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4			1992																												T																		K				5.4			5.4																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9252	PHC2030240		(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4			1992																												T																		K					4.2																																																																																																La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9253	PHC2030240		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4			1992																												T																		K				12.7			12.7																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9254	PHC2030240		(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4			1992																												T																		K				26.1			26.1																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9255	PHC2030240		(La,Ba)2CuO4	La1.82Ba0.18Cu1O4	La	1.82	Ba	0.18	Cu	1															O	4			1992																												T																		K				24.2			24.2																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9256	PHC2030240		(La,Ba)2CuO4	La1.78Ba0.22Cu1O4	La	1.78	Ba	0.22	Cu	1															O	4			1992																												T																		K				5.4			5.4																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9257	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4			1992																												T																		K				30.9			30.9																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9258	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.895Ba0.105Cu1O4	La	1.895	Ba	0.105	Cu	1															O	4			1992																												T																		K				33.1			33.1																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9259	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4			1992																												T																		K				32.3			32.3																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9260	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.884Ba0.116Cu1O4	La	1.884	Ba	0.116	Cu	1															O	4			1992																												T																		K				21.8			21.8																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9261	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.881Ba0.119Cu1O4	La	1.881	Ba	0.119	Cu	1															O	4			1992																												T																		K				9.3			9.3																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9262	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.877Ba0.123Cu1O4	La	1.877	Ba	0.123	Cu	1															O	4			1992																												T																		K				23.6			23.6																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9263	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4			1992																												T																		K				30.1			30.1																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9264	PHC2030240	Tc measured at p=20 kbar	(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4			1992																												T																		K				29.3			29.3																																																																																														La2O3,BaCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9265	PHC2030240		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4			1992																												T																		K				27.1			27.1																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9266	PHC2030240		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1992																												T																		K				31.8			31.8																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9267	PHC2030240		(La,Sr)2CuO4	La1.883Sr0.117Cu1O4	La	1.883	Sr	0.117	Cu	1															O	4			1992																												T																		K				31.6			31.6																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9268	PHC2030240		(La,Sr)2CuO4	La1.868Sr0.132Cu1O4	La	1.868	Sr	0.132	Cu	1															O	4			1992																												T																		K				34.4			34.4																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9269	PHC2030240		(La,Sr)2CuO4	La1.847Sr0.153Cu1O4	La	1.847	Sr	0.153	Cu	1															O	4			1992																												T																		K				37.6			37.6																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9270	PHC2030240		(La,Sr)2CuO4	La1.828Sr0.172Cu1O4	La	1.828	Sr	0.172	Cu	1															O	4			1992																												T																		K				37.5			37.5																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9271	PHC2030240		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1992																												T																		K				33			33																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9272	PHC2030240		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4			1992																												T																		K				21.3			21.3																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9273	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4			1992																												T																		K				29.6			29.6																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9274	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			1992																												T																		K				34.1			34.1																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9275	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.883Sr0.117Cu1O4	La	1.883	Sr	0.117	Cu	1															O	4			1992																												T																		K				34.4			34.4																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9276	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.868Sr0.132Cu1O4	La	1.868	Sr	0.132	Cu	1															O	4			1992																												T																		K				36.6			36.6																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9277	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.847Sr0.153Cu1O4	La	1.847	Sr	0.153	Cu	1															O	4			1992																												T																		K				40.9			40.9																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9278	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.828Sr0.172Cu1O4	La	1.828	Sr	0.172	Cu	1															O	4			1992																												T																		K				41.2			41.2																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9279	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			1992																												T																		K				33.3			33.3																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9280	PHC2030240	Tc measured at p=20 kbar	(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4			1992																												T																		K				22.1			22.1																																																																																														La2O3,SrCO3,CuO	1						PRESSURE EFFECTS ON SUPERCONDUCTIVITY AND STRUCTURAL PHASE TRANSITIONS IN LA2-XMXCUO4 (M=BA,SR)	199212			PHYSICA C,203(1992)240	M.IDO,N.YAMADA	LA,BA,SR,CU,O	
9281	PR05606288		(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4		1	1997																												T																		K		11.9					11.9			K/kbar	1																																																																																											1	SIN(1050C)-ANN(900C, 1 atm O2)					Electron-lattice coupling and stripe formation in La2-xBaxCuO4	199709		Center for Materials Science & Engineering, ETC 9.102, University of Texas at Austin, Austin, Texas 78712-1063	Phys.Rev.B, 56(1997)6288-6294	J. B. Goodenough,J.-S. Zhou		
9282	PR05606288		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4	La	1.88	Ba	0.12	Cu	1															O	4		1	1997																												T																		K					4.2																																																																																																	1	SIN(1050C)-ANN(900C, 1 atm O2)					Electron-lattice coupling and stripe formation in La2-xBaxCuO4	199709		Center for Materials Science & Engineering, ETC 9.102, University of Texas at Austin, Austin, Texas 78712-1063	Phys.Rev.B, 56(1997)6288-6294	J. B. Goodenough,J.-S. Zhou		
9283	PR05606288		(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		1	1997																												T																		K					4.2																																																																																																	1	SIN(1050C)-ANN(900C, 1 atm O2)					Electron-lattice coupling and stripe formation in La2-xBaxCuO4	199709		Center for Materials Science & Engineering, ETC 9.102, University of Texas at Austin, Austin, Texas 78712-1063	Phys.Rev.B, 56(1997)6288-6294	J. B. Goodenough,J.-S. Zhou		
9284	PR05606288		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4		1	1997																												T																		K					4.2																																																																																																	1	SIN(1050C)-ANN(900C, 1 atm O2)					Electron-lattice coupling and stripe formation in La2-xBaxCuO4	199709		Center for Materials Science & Engineering, ETC 9.102, University of Texas at Austin, Austin, Texas 78712-1063	Phys.Rev.B, 56(1997)6288-6294	J. B. Goodenough,J.-S. Zhou		
9285	PR05606288		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4		1	1997																												T																		K		7.4					7.4	TC9285		K/kbar	2.4																																																																																											1	SIN(1050C)-ANN(900C, 1 atm O2)					Electron-lattice coupling and stripe formation in La2-xBaxCuO4	199709		Center for Materials Science & Engineering, ETC 9.102, University of Texas at Austin, Austin, Texas 78712-1063	Phys.Rev.B, 56(1997)6288-6294	J. B. Goodenough,J.-S. Zhou		
9286	PR0465686		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z			1992																											3	Bi2212			A	5.41	5.38	30.68												K		76.1					76.1																																																																																														Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9287	PR0465686		Bi2Sr2(Ca,Ga)Cu2O8	Bi2Sr2Ca0.9Ga0.1Cu2Oz	Bi	2	Sr	2	Ca	0.9	Ga	0.1	Cu	2											O	z			1992																												Bi2212																		K		76.1					76.1																																																																																														Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9288	PR0465686		Bi2Sr2(Ca,Ga)Cu2O8	Bi2Sr2Ca0.8Ga0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Ga	0.2	Cu	2											O	z			1992																												Bi2212																		K		76.1					76.1																																																																																														Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9289	PR0465686		Bi2Sr2(Ca,Ga)Cu2O8	Bi2Sr2Ca0.7Ga0.3Cu2Oz	Bi	2	Sr	2	Ca	0.7	Ga	0.3	Cu	2											O	z			1992																												Bi2212																		K		76.1					76.1																																																																																														Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9290	PR0465686		Bi2Sr2(Ca,Ga)Cu2O8	Bi2Sr2Ca0.5Ga0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Ga	0.5	Cu	2											O	z			1992																												Bi2212																		K		76.1					76.1																																																																																														Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9291	PR0465686	R does not go to zero even at 5K	Bi2Sr2(Ca,Ga)Cu2O8	Bi2Sr2Ca0.4Ga0.6Cu2Oz	Bi	2	Sr	2	Ca	0.4	Ga	0.6	Cu	2											O	z			1992																												Bi2212																		K					5																																																																																																Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9292	PR0465686	semiconductive	Bi2Sr2GaCu2O8	Bi2Sr2Ga1Cu2Oz	Bi	2	Sr	2	Ga	1	Cu	2													O	z			1992																											3	Bi2212			A	5.43	5.39	24.48												K					5																																																																																																Bi2O3,SrCO3,CaCO3,Ga2O3,CuO	1	mixture-CAL(800C,12H)-FC-pellet-SIN(845C,72H)-FC					SUPERCONDUCTING AND SEMICONDUCTING PROPERTIES OF THE BI2SR2CA1-XGAXCU2OY SYSTEM	199209	X-RAY-DIFFRACTION   ,RESISTIVITY         ,SUSCEPTIBILITY	DEPARTMENT OF PHYSICS AND ASTRONOMY, MCMASTER UNIVERSITY, CANADA	PHYS.REV.B,46(1992)5686	R.K.NKUM,W.R.DATARS	BI,SR,CA,GA,CU,O	
9293	SSC0730341		(Nd,Sm,Ce)2CuO4	Nd1.75Sm0.1Ce0.15Cu1O3.972	Nd	1.75	Sm	0.1	Ce	0.15	Cu	1													O	z	3.972		1990																											2	T'			A	3.9454		12.079												K				22.2			22.2																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9294	SSC0730341		(Nd,Sm,Ce)2CuO4	Nd1.65Sm0.2Ce0.15Cu1O3.971	Nd	1.65	Sm	0.2	Ce	0.15	Cu	1													O	z	3.971		1990																											2	T'			A	3.9438		12.068												K				21.6			21.6																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9295	SSC0730341		(Nd,Sm,Ce)2CuO4	Nd1.55Sm0.3Ce0.15Cu1O3.972	Nd	1.55	Sm	0.3	Ce	0.15	Cu	1													O	z	3.972		1990																											2	T'			A	3.9411		12.055												K				21.8			21.8																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9296	SSC0730341		(Nd,La,Ce)2CuO4	Nd1.85Ce0.15Cu1O3.971	Nd	1.85	Ce	0.15	Cu	1															O	z	3.971		1990																											2	T'			A	3.9465		12.092												K				21.6			21.6																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9297	SSC0730341		(Nd,La,Ce)2CuO4	Nd1.55La0.3Ce0.15Cu1Oz	Nd	1.55	La	0.3	Ce	0.15	Cu	1													O	z			1990																											2	T'			A	3.9578		12.145												K				19.6			19.6																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9298	SSC0730341		(Nd,La,Ce)2CuO4	Nd1.05La0.8Ce0.15Cu1Oz	Nd	1.05	La	0.8	Ce	0.15	Cu	1													O	z			1990																											2	T'			A	3.9751		12.241												K				16.3			16.3																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9299	SSC0730341		(Nd,La,Ce)2CuO4	Nd0.85La1Ce0.15Cu1Oz	Nd	0.85	La	1	Ce	0.15	Cu	1													O	z			1990																											2	T'			A	3.9827		12.273												K				14.9			14.9																																																																																														CeO2,Nd2O3,La2O3,Sm2O3,CuO	1	mixture-pellet-heat(950C,12H in air)-FC-pellet-SIN(1080C,12H,in air)-FC-ANN(900C,12H in air)-Q to RT					RELATION BETWEEN TC AND CU-O BOND LENGTH WITHIN THE BASAL PLANE OF CE0.15ND1.85-XMXCUO4-Y (M=LA AND SM) AND CE0.15PR1.85CUO4-Y		OXYGEN CONTENT      ,SUSCEPTIBILITY      ,SUBSTITUTIONS       ,CU-O BOND	INSTITUTE FOR MATERIALS RESEARCH, TOHOKU UNIVERSITY, KATAHIRA,AOBA-KU, SENDAI 980, JAPAN	SOLID STATE COMMUN,73(1990)341	K.OH-ISHI,M.KIKUCHI,M.KOBAYASHI,Y.MUTO,Y.SYONO	CE,ND,CU,O,LA,SM,PR	
9300	PRL0851738	T(NQR)=130 K	(La,Nd,Sr)2CuO4	La1.52Nd0.4Sr0.08Cu1O4	La	1.52	Nd	0.4	Sr	0.08	Cu	1													O	4		3	2000								19.9																				T																		K	6.62						6.62																																																																																																traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9301	PRL0851738	charge order temp by X-ray=64.9K. T(NQR)=90 K	(La,Nd,Sr)2CuO4	La1.5Nd0.4Sr0.1Cu1O4	La	1.5	Nd	0.4	Sr	0.1	Cu	1													O	4		3	2000								45																				T																		K	6.62						6.62																																																																																																traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9302	PRL0851738	charge order temp by X-ray=68.9K. T(NQR)=69.5 K	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2000								55																				T																		K	2.65						2.65																																																																																																traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9303	PRL0851738	charge order temp by X-ray=59K. T(NQR)=59.6 K	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	2000								44.4																				T																		K	10.6						10.6																																																																																																traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9304	PRL0851738	 T(NQR)=38.4K	(La,Nd,Sr)2CuO4	La1.4Nd0.4Sr0.2Cu1O4	La	1.4	Nd	0.4	Sr	0.2	Cu	1													O	4		3	2000								16.6																				T																		K	13.9						13.9																																																																																																traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9305	PRL0851738	T(NQR)=39.1 K	(La,Nd,Sr)2CuO4	La1.35Nd0.4Sr0.25Cu1O4	La	1.35	Nd	0.4	Sr	0.25	Cu	1													O	4		3	2000								1.32																				T																		K																																																																																																							traveling solvent floating zone method					Local Magnetic Order vs Superconductivity in a Layered Cuprate	8		Department of Superconductivity, School of Engineering, University of Tokyo, 2-11-16 Yayoi, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 85(2000)1739-	J. M. Tranquada,J. R. Schneider,N. Ichikawa,P. M. Gehring,S. Uchida,S.-H. Lee,T. Niemoller		
9306	PHB2841085		(Cu,Tl)Ba2Ca2Cu3O10	Tl0.5Ba2Ca2Cu3.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3.5													O	10-z			2000																												Tl1223																		K				132			132																																																																																																samples were prepared at 850 C under 4 Gpa. ANN(400-600C,12H in flowing N2).  AgO was added as a oxidizer.					Selective reduction for hole-doping in Cu1-xTlx-1223 (Cu1-xTlxBa2Ca2Cu3O10-y) system with Tc>132K			Electrotechnical Laboratory, 1-1-4 Umezono,Tsukuba,Ibaraki, Japan	Physica B, 284-288(2000)1085-1086	A.Iyo,F.Tateai,H.Ihara,K.Ishida,K.Tanaka,M.Kawamura,M.Tokumoto,N.Terada,S.Miyashita,T.Watanabe,Y.Tanaka		
9307	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.95	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.95	1	2000																												Y123																		K	37						37	TC9307																																																																																													Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9308	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.85	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K	27.8						27.8	TC9308																																																																																										RH9308			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9309	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.61	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.61	1	2000																												Y123																		K	26						26	TC9309																																																																																													Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9310	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.66	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.66	1	2000																												Y123																		K	25.4						25.4	TC9310																																																																																													Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9311	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.76	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.76	1	2000																												Y123																		K	23.7						23.7	TC9311																																																																					TP9311																					RH9311			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9312	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.53	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.53	1	2000																												Y123																		K	15						15	TC9312																																																																																													Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9313	JPS0690170	not s/c	(Y,Pr)Ba2Cu3Oz	Y0.6Pr0.4Ba2Cu3O6.45	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	6+z	6.45	1	2000																												Y123																		K					4.2			TC9313																																																																																													Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9314	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	6+z	6.45	1	2000																												Y123																		K	33						33																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9315	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.53	Y	1	Ba	2	Cu	3															O	6+z	6.53	1	2000																												Y123																		K	50.3						50.3																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9316	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.61	Y	1	Ba	2	Cu	3															O	6+z	6.61	1	2000																												Y123																		K	55.5						55.5																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9317	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	6+z	6.66	1	2000																												Y123																		K	56.7						56.7																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9318	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.71	Y	1	Ba	2	Cu	3															O	6+z	6.71	1	2000																												Y123																		K	59						59																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9319	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.76	Y	1	Ba	2	Cu	3															O	6+z	6.76	1	2000																												Y123																		K	63						63																																																																						TP9319																					RH9319			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9320	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	6+z	6.85	1	2000																												Y123																		K	87.9						87.9																																																																						TP9320																					RH9320			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9321	JPS0690170		YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6+z	6.95	1	2000																												Y123																		K	90.2						90.2																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9322	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.45	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.45	1	2000																												Y123																		K					4.2																																																																																																Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9323	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.53	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.53	1	2000																												Y123																		K	5.2						5.2																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9324	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.61	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.61	1	2000																												Y123																		K	4.6						4.6																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9325	JPS0690170	not zero resistance	(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.66	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.66	1	2000																												Y123																		K			3.5				3.5																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9326	JPS0690170	not zero resistance	(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.71	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.71	1	2000																												Y123																		K			4				4																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9327	JPS0690170	not zero resistance	(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.76	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.76	1	2000																												Y123																		K			4				4																																																																						TP9327																					RH9327			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9328	JPS0690170	not zero resistance	(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.85	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K			4				4																																																																						TP9328																					RH9328			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9329	JPS0690170		(Y,Pr)Ba2Cu3Oz	Y0.5Pr0.5Ba2Cu3O6.95	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	6+z	6.95	1	2000																												Y123																		K	12.7						12.7																																																																																														Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9330	JPS0690170	not s/c	(Y,Pr)Ba2Cu3Oz	Y0.4Pr0.6Ba2Cu3O6.85	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K					4.2																																																																								TP9330																					RH9330			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9331	JPS0690170	not s/c	(Y,Pr)Ba2Cu3Oz	Y0.4Pr0.6Ba2Cu3O6.76	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	6+z	6.76	1	2000																												Y123																		K					4.2																																																																								TP9331																					RH9331			Y2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(880C,12H in air)-pellet-SIN(910C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9332	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.55	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.55	1	2000																												Y123																		K																																																																																																					Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9333	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.65	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.65	1	2000																												Y123																		K	21						21	TC9333																																																																																													Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9334	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.7	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.7	1	2000																												Y123																		K	25.6						25.6	TC9334																																																																																													Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9335	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.75	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.75	1	2000																												Y123																		K	23.4						23.4	TC9335																																																																																													Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9336	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.85	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K	26						26	TC9336																																																																																													Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9337	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.8Pr0.2Ba2Cu3O6.95	Sm	0.8	Pr	0.2	Ba	2	Cu	3													O	6+z	6.95	1	2000																												Y123																		K	41						41	TC9337																																																																																													Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9338	JPS0690170		SmBa2Cu3Oz	Sm1Ba2Cu3O6.55	Sm	1	Ba	2	Cu	3															O	6+z	6.55	1	2000																												Y123																		K	12.8						12.8																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9339	JPS0690170		SmBa2Cu3Oz	Sm1Ba2Cu3O6.65	Sm	1	Ba	2	Cu	3															O	6+z	6.65	1	2000																												Y123																		K	32.8						32.8																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9340	JPS0690170		SmBa2Cu3Oz	Sm1Ba2Cu3O6.75	Sm	1	Ba	2	Cu	3															O	6+z	6.75	1	2000																												Y123																		K	38.4						38.4																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9341	JPS0690170		SmBa2Cu3Oz	Sm1Ba2Cu3O6.85	Sm	1	Ba	2	Cu	3															O	6+z	6.85	1	2000																												Y123																		K	54.7						54.7																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9342	JPS0690170		SmBa2Cu3Oz	Sm1Ba2Cu3O6.95	Sm	1	Ba	2	Cu	3															O	6+z	6.95	1	2000																												Y123																		K	79.4						79.4																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9343	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.9Pr0.1Ba2Cu3O6.55	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	6+z	6.55	1	2000																												Y123																		K	12.2						12.2																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9344	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.9Pr0.1Ba2Cu3O6.65	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	6+z	6.65	1	2000																												Y123																		K	30.6						30.6																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9345	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.9Pr0.1Ba2Cu3O6.75	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	6+z	6.75	1	2000																												Y123																		K	36.3						36.3																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9346	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.9Pr0.1Ba2Cu3O6.85	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K	42.2						42.2																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9347	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.9Pr0.1Ba2Cu3O6.95	Sm	0.9	Pr	0.1	Ba	2	Cu	3													O	6+z	6.95	1	2000																												Y123																		K	57.5						57.5																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9348	JPS0690170	not s/c	(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.55	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.55	1	2000																												Y123																		K																																																																																																					Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9349	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.65	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.65	1	2000																												Y123																		K	10.6						10.6																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9350	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.75	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.75	1	2000																												Y123																		K	6.6						6.6																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9351	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.8	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.8	1	2000																												Y123																		K	5						5																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9352	JPS0690170	not zero-resistance	(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.85	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.85	1	2000																												Y123																		K			4.4				4.4																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9353	JPS0690170		(Sm,Pr)Ba2Cu3Oz	Sm0.7Pr0.3Ba2Cu3O6.95	Sm	0.7	Pr	0.3	Ba	2	Cu	3													O	6+z	6.95	1	2000																												Y123																		K	23.1						23.1																																																																																														Sm2O3,Pr6O11,BaCO3,CuO	1	mixture-heat(900C,12H in air)-pellet-SIN(925C,24H in air)-FC. O-control by annealing at proper temperature then quench.					On the Anomalous Oxygen-Number Dependence of the Superconducting Transition Temperature of R1-xPrxBa2Cu3O6+y (R=Y and Sm)			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc. Jpn, 69(2000)170-177	Jun Takeda,Makoto Ambai,Masatoshi Sato,Yoshiaki Kobayashi,Yukio Yasui		
9354	JMR0151076	compo.=nominal values	(Bi3Pb)Sr3Ca3Cu4Oz	Bi3Pb1Sr3Ca3Cu4Oz	Bi	3	Pb	1	Sr	3	Ca	3	Cu	4											O	z			2000																												Bi4334																		K	78		110				94																																																																		uV/K	0.28			TP9354	mOhm.cm											27.17												Bi2O3,PbO,CaCO3,SrO3,CuO,Cr2O3	1	precursor(Bi3PbSr3Ca3(Cu1-xCrx)4Oz)-melt(1100-1200C in Pt crucible)-Q to form glassy precursor-ANN(840C,24H in air)					Effect of Cr doping on the electrical conductivity and Seebeck coefficient in the superconductors obtained from the Bi-Pb-Sr-Ca-Cu-Cr-O-type glassy precursors by annealing	200005		olid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700032, India	J.Mater.Res., 15(2000)1076-1082	B.K. Chaudhuri,D. Kilian,H.K. Barik,S. Bhattacharya,S.K. Ghorai		
9355	JMR0151076	compo.=nominal values	(Bi3Pb)Sr3Ca3(Cu,Cr)4Oz	Bi3Pb1Sr3Ca3Cu3.8Cr0.2Oz	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.8	Cr	0.2									O	z			2000																												Bi4334																		K	46		69				57.5																																																																		uV/K	2.6			TP9355	mOhm.cm											30.08												Bi2O3,PbO,CaCO3,SrO3,CuO,Cr2O3	1	precursor(Bi3PbSr3Ca3(Cu1-xCrx)4Oz)-melt(1100-1200C in Pt crucible)-Q to form glassy precursor-ANN(840C,24H in air)					Effect of Cr doping on the electrical conductivity and Seebeck coefficient in the superconductors obtained from the Bi-Pb-Sr-Ca-Cu-Cr-O-type glassy precursors by annealing	200005		olid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700032, India	J.Mater.Res., 15(2000)1076-1082	B.K. Chaudhuri,D. Kilian,H.K. Barik,S. Bhattacharya,S.K. Ghorai		
9356	JMR0151076	compo.=nominal values	(Bi3Pb)Sr3Ca3(Cu,Cr)4Oz	Bi3Pb1Sr3Ca3Cu3.6Cr0.4Oz	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.6	Cr	0.4									O	z			2000																												Bi4334																		K	27		68				47.5																																																																		uV/K	6.61			TP9356	mOhm.cm											42.69												Bi2O3,PbO,CaCO3,SrO3,CuO,Cr2O3	1	precursor(Bi3PbSr3Ca3(Cu1-xCrx)4Oz)-melt(1100-1200C in Pt crucible)-Q to form glassy precursor-ANN(840C,24H in air)					Effect of Cr doping on the electrical conductivity and Seebeck coefficient in the superconductors obtained from the Bi-Pb-Sr-Ca-Cu-Cr-O-type glassy precursors by annealing	200005		olid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700032, India	J.Mater.Res., 15(2000)1076-1082	B.K. Chaudhuri,D. Kilian,H.K. Barik,S. Bhattacharya,S.K. Ghorai		
9357	JMR0151076	compo.=nominal values. R not to zero.	(Bi3Pb)Sr3Ca3(Cu,Cr)4Oz	Bi3Pb1Sr3Ca3Cu3.2Cr0.8Oz	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.2	Cr	0.8									O	z			2000																												Bi4334																		K			60				60																																																																		uV/K	6.92			TP9357	mOhm.cm											150.07												Bi2O3,PbO,CaCO3,SrO3,CuO,Cr2O3	1	precursor(Bi3PbSr3Ca3(Cu1-xCrx)4Oz)-melt(1100-1200C in Pt crucible)-Q to form glassy precursor-ANN(840C,24H in air)					Effect of Cr doping on the electrical conductivity and Seebeck coefficient in the superconductors obtained from the Bi-Pb-Sr-Ca-Cu-Cr-O-type glassy precursors by annealing	200005		olid State Physics Department, Indian Association for the Cultivation of Science, Calcutta-700032, India	J.Mater.Res., 15(2000)1076-1082	B.K. Chaudhuri,D. Kilian,H.K. Barik,S. Bhattacharya,S.K. Ghorai		
9358	JPS0632314		(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4			1994																												T																		K				25			25																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9359	JPS0632314		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4			1994																												T																		K				26			26																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9360	JPS0632314		(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4			1994																												T																		K				18.8			18.8																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9361	JPS0632314		(La,Ba)2CuO4	La1.885Ba0.115Cu1O4	La	1.885	Ba	0.115	Cu	1															O	4			1994																												T																		K				13.9			13.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9362	JPS0632314		(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4			1994																												T																		K				8.9			8.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9363	JPS0632314		(La,Ba)2CuO4	La1.865Ba0.135Cu1O4	La	1.865	Ba	0.135	Cu	1															O	4			1994																												T																		K				5.98			5.98																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9364	JPS0632314		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4	La	1.86	Ba	0.14	Cu	1															O	4			1994																												T																		K				9.96			9.96																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9365	JPS0632314		(La,Ba)2CuO4	La1.855Ba0.145Cu1O4	La	1.855	Ba	0.145	Cu	1															O	4			1994																												T																		K				13			13																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9366	JPS0632314		(La,Ba)2CuO4	La1.845Ba0.155Cu1O4	La	1.845	Ba	0.155	Cu	1															O	4			1994																												T																		K				26			26																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9367	JPS0632314		(La,Ba)2CuO4	La1.84Ba0.16Cu1O4	La	1.84	Ba	0.16	Cu	1															O	4			1994																												T																		K				27			27																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9368	JPS0632314		(La,Ba)2CuO4	La1.83Ba0.17Cu1O4	La	1.83	Ba	0.17	Cu	1															O	4			1994																												T																		K				26.9			26.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9369	JPS0632314		(La,Ba)2CuO4	La1.82Ba0.18Cu1O4	La	1.82	Ba	0.18	Cu	1															O	4			1994																												T																		K				22			22																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9370	JPS0632314		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4			1994																												T																		K				17.9			17.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9371	JPS0632314		(La,Nd,Ba)2CuO4	La1.83Nd0.1Ba0.07Cu1O4	La	1.83	Nd	0.1	Ba	0.07	Cu	1													O	4			1994																												T																		K				16			16																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9372	JPS0632314		(La,Nd,Ba)2CuO4	La1.8Nd0.1Ba0.1Cu1O4	La	1.8	Nd	0.1	Ba	0.1	Cu	1													O	4			1994																												T																		K				22			22																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9373	JPS0632314		(La,Nd,Ba)2CuO4	La1.79Nd0.1Ba0.11Cu1O4	La	1.79	Nd	0.1	Ba	0.11	Cu	1													O	4			1994																												T																		K				13			13																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9374	JPS0632314		(La,Nd,Ba)2CuO4	La1.75Nd0.1Ba0.15Cu1O4	La	1.75	Nd	0.1	Ba	0.15	Cu	1													O	4			1994																												T																		K				12			12																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9375	JPS0632314		(La,Nd,Ba)2CuO4	La1.74Nd0.1Ba0.16Cu1O4	La	1.74	Nd	0.1	Ba	0.16	Cu	1													O	4			1994																												T																		K				16.9			16.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9376	JPS0632314		(La,Nd,Ba)2CuO4	La1.72Nd0.1Ba0.18Cu1O4	La	1.72	Nd	0.1	Ba	0.18	Cu	1													O	4			1994																												T																		K				19.8			19.8																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9377	JPS0632314		(La,Nd,Ba)2CuO4	La1.72Nd0.2Ba0.08Cu1O4	La	1.72	Nd	0.2	Ba	0.08	Cu	1													O	4			1994																												T																		K				16.9			16.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9378	JPS0632314		(La,Nd,Ba)2CuO4	La1.7Nd0.2Ba0.1Cu1O4	La	1.7	Nd	0.2	Ba	0.1	Cu	1													O	4			1994																												T																		K				15			15																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9379	JPS0632314		(La,Nd,Ba)2CuO4	La1.69Nd0.2Ba0.11Cu1O4	La	1.69	Nd	0.2	Ba	0.11	Cu	1													O	4			1994																												T																		K				8.2			8.2																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9380	JPS0632314		(La,Nd,Ba)2CuO4	La1.64Nd0.2Ba0.16Cu1O4	La	1.64	Nd	0.2	Ba	0.16	Cu	1													O	4			1994																												T																		K				12			12																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9381	JPS0632314		(La,Nd,Ba)2CuO4	La1.62Nd0.2Ba0.18Cu1O4	La	1.62	Nd	0.2	Ba	0.18	Cu	1													O	4			1994																												T																		K				14.9			14.9																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9382	JPS0632314		(La,Nd,Ba)2CuO4	La1.6Nd0.2Ba0.2Cu1O4	La	1.6	Nd	0.2	Ba	0.2	Cu	1													O	4			1994																												T																		K				11			11																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9383	JPS0632314		(La,Nd,Ba)2CuO4	La1.52Nd0.4Ba0.08Cu1O4	La	1.52	Nd	0.4	Ba	0.08	Cu	1													O	4			1994																												T																		K				11			11																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9384	JPS0632314		(La,Nd,Ba)2CuO4	La1.5Nd0.4Ba0.1Cu1O4	La	1.5	Nd	0.4	Ba	0.1	Cu	1													O	4			1994																												T																		K				9.95			9.95																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9385	JPS0632314		(La,Nd,Ba)2CuO4	La1.475Nd0.4Ba0.125Cu1O4	La	1.475	Nd	0.4	Ba	0.125	Cu	1													O	4			1994																												T																		K	5		10				7.5																																																																																														La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9386	JPS0632314		(La,Nd,Sr)2CuO4	La1.475Nd0.4Sr0.125Cu1O4	La	1.475	Nd	0.4	Sr	0.125	Cu	1													O	4			1994																												T																																																																																											uV/K	35.18																											La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9387	JPS0632314		(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4			1994																												T																																																																																											uV/K	23.04																											La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9388	JPS0632314		(La,Nd,Sr)2CuO4	La1.44Nd0.4Sr0.16Cu1O4	La	1.44	Nd	0.4	Sr	0.16	Cu	1													O	4			1994																												T																																																																																											uV/K	15.36																											La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9389	JPS0632314		(La,Nd,Sr)2CuO4	La1.42Nd0.4Sr0.18Cu1O4	La	1.42	Nd	0.4	Sr	0.18	Cu	1													O	4			1994																												T																																																																																											uV/K	12.68																											La2O3,Nd2O3,BaCO3,SrCO3,CuO	1	mixture-heat(930C,20h)-pellet-SIN(1100C,20h)-FC					Relationship between the Structural Transitions and the Low Temperature Electronic State of (La,Nd)2-xMxCuO4 (M=Ba, Sr; x~1/8)	199406		Department of Physics, Faculty of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc. Jpn, 63(1994)2314-2223	Jun-ichi Yamada,Makoto Sakata,Masafumi Sera,Masaki-Takata,Masatoshi Sato,Takashi Takayama		
9500	PRL0850405	NMR studies were done for this sample.	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O6.8	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.8	3	2000																												Tl1212																		K				68			68																				T	calculated from WHH theory. Hc2 by susceptibility			43					T/K				0.89																																																															See Phys.Rev.B.,45(1992)5553					Superconducting Fluctuations and the Pseudogap in the Slightly Overdoped High-Tc Superconductor TlSr2CaCu2O6.8: High Magnetic Field NMR Studies	7		Department of Physical Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 85(2000)405-408	A.P.Reyes,Guo-qing Zheng,H.Ozaki,P.Kuhns,T.Kondo,W.G.Clark,W.G.Moulton,Y.Kitaoka,Y.Kubo,Y.Shimakawa		
9501	PRL0851116		NdBa2Cu3O7	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z		4	2000																												Y123			A			11.755												K	85						85																																									A	Microwave. By fitting using two fluid approx.	2400																																																					Film was deposited by dc magnetron sputtering from Nd1.09Ba1.91Cu3O7 target					Role of Nd/Ba Disorder on the Penetration Depth of Nd1 + xBa2-xCu3O7+z Thin Films	7		INFM and Dipartimento di Scienze Fisiche, Universit? di Napoli Federico II, I-80125 Napoli, Italy	Phys.Rev.Lett., 85(2000)1116-1119	A.Andreone,C.Cantoni,D.P.Norton,F.Fischer,F.Palomba,G.Pica,I.Maggio-Aprile,M.Salluzzo		
9502	PRL0851116		Nd(Nd,Ba)2Cu3O7	Nd1.04Ba1.96Cu3O7-Z	Nd	1.04	Ba	1.96	Cu	3															O	7-Z		4	2000																												Y123			A			11.74												K	86						86																																									A	Microwave. By fitting using two fluid approx.	2300																																																					Film was deposited by dc magnetron sputtering from Nd1.12Ba1.88Cu3O7 target					Role of Nd/Ba Disorder on the Penetration Depth of Nd1 + xBa2-xCu3O7+z Thin Films	7		INFM and Dipartimento di Scienze Fisiche, Universit? di Napoli Federico II, I-80125 Napoli, Italy	Phys.Rev.Lett., 85(2000)1116-1119	A.Andreone,C.Cantoni,D.P.Norton,F.Fischer,F.Palomba,G.Pica,I.Maggio-Aprile,M.Salluzzo		
9503	PRL0851116		Nd(Nd,Ba)2Cu3O7	Nd1.2Ba1.8Cu3O7-Z	Nd	1.2	Ba	1.8	Cu	3															O	7-Z		4	2000																												Y123			A			11.705												K	56						56																																									A	Microwave. By fitting using two fluid approx.	3800																																																					Film was deposited by pulsed lase deposition from Nd1Ba2Cu3O7 target on (100)LaAlO3.					Role of Nd/Ba Disorder on the Penetration Depth of Nd1 + xBa2-xCu3O7+z Thin Films	7		INFM and Dipartimento di Scienze Fisiche, Universit? di Napoli Federico II, I-80125 Napoli, Italy	Phys.Rev.Lett., 85(2000)1116-1119	A.Andreone,C.Cantoni,D.P.Norton,F.Fischer,F.Palomba,G.Pica,I.Maggio-Aprile,M.Salluzzo		
9504	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.77La0.23Cu1O6+Z	Bi	2	Sr	1.77	La	0.23	Cu	1													O	6+Z		3	2000																												Bi2201																		K	28						28	TC9504																																																																																															Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9505	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.61La0.39Cu1O6+Z	Bi	2	Sr	1.61	La	0.39	Cu	1													O	6+Z		3	2000																												Bi2201																		K	38.8						38.8																																																																																											RH9505					Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9506	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.34La0.66Cu1O6+Z	Bi	2	Sr	1.34	La	0.66	Cu	1													O	6+Z		3	2000																												Bi2201																		K	22						22																																																																																																Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9507	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.27La0.73Cu1O6+Z	Bi	2	Sr	1.27	La	0.73	Cu	1													O	6+Z		3	2000																												Bi2201																		K	14						14																																																																																											RH9507					Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9508	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.24La0.76Cu1O6+Z	Bi	2	Sr	1.24	La	0.76	Cu	1													O	6+Z		3	2000																												Bi2201																		K	12.1						12.1																																																																																																Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9509	PRL0850638		Bi2(Sr,La)2CuO6	Bi2Sr1.16La0.84Cu1O6+Z	Bi	2	Sr	1.16	La	0.84	Cu	1													O	6+Z		3	2000																												Bi2201																		K	1.82						1.82																																																																																											RH9509					Crystals were grown by floating zone method. Samples were annealed in flowing oxygen at 650C for 48hs.					Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
9510	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.8	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.8	1	1992																												Tl1212			A	3.7956		12.1252												K	68						68																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9511	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.82	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.82	1	1992																												Tl1212			A	3.793		12.1198												K																																																																																																					Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9512	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.825	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.825	1	1992																												Tl1212			A															K	40						40																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9513	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.837	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.837	1	1992																												Tl1212			A															K	31.5						31.5																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9514	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.85	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.85	1	1992																												Tl1212			A	3.7901		12.115												K	24						24																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9515	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.862	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.862	1	1992																												Tl1212			A															K	15.2						15.2																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9516	PR0455553		TlSr2CaCu2Oz	Tl1Sr2Ca1Cu2O6.88	Tl	1	Sr	2	Ca	1	Cu	2													O	7-Z	6.88	1	1992																												Tl1212			A	3.7848		12.113												K	0						0																																																																																														Tl2O3,SrO,CaO,CuO		mixture-pellet-sealed in Au crucible-SIN(900C, several days in O2)-ANN(350-550C, 5h, in Ar)					SUPERCONDUCTOR-TO-METAL TRANSITION CAUSED BY OXYGEN NONSTOICHIOMETRY IN TLSR2CACU2O7-Z HAVING A CU-O PYRAMIDAL LAYER	199203			PHYS.REV.B,45(1992)5553	H.IGARASHI,H.Igarashi,T.KONDO,T.Kondo,T.MANAKO,T.Manako,Y.KUBO,Y.Kubo,Y.SHIMAKAWA,Y.Shimakawa	TL,SR,CA,CU,O	
9517	JJP0301155		SrNb2Oz	Sr1Nb2Oz	Sr	1	Nb	2																	O	z			1991																															A															K				11.5			11.5										1.6																																																																																				La2O3,SrCO3,NbO2	1	mixture-sealed in silica tube with Zr plate-heat(1100C, 24h)-FC					A NEW NON-CU-OXIDE SUPERCONDUCTOR: (SR1-XLNX)NB2O6-Y (LN:LA,ND,PR AND CE)	199107		DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1 CHITOSEDAI,SETAGAYA,TOKYO 157	JJAP LETT.,30(1991)1155	HIROSHI SAWA,JIRO AMANO,JUN AKIMITSU,KAZUHIRO GYODA,MANAMI KOGAI,OSAMU NAGASE	SR,LA,ND,PR,CE,NB,O	
9518	JJP0301155		(Sr,Nd)Nb2Oz	Sr0.9Nd0.1Nb2Oz	Sr	0.9	Nd	0.1	Nb	2															O	z			1991																															A	11	7.683	5.585												K				11.5			11.5										14																																																																																				La2O3,SrCO3,NbO2	1	mixture-sealed in silica tube with Zr plate-heat(1100C, 24h)-FC					A NEW NON-CU-OXIDE SUPERCONDUCTOR: (SR1-XLNX)NB2O6-Y (LN:LA,ND,PR AND CE)	199107		DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1 CHITOSEDAI,SETAGAYA,TOKYO 157	JJAP LETT.,30(1991)1155	HIROSHI SAWA,JIRO AMANO,JUN AKIMITSU,KAZUHIRO GYODA,MANAMI KOGAI,OSAMU NAGASE	SR,LA,ND,PR,CE,NB,O	
9519	JJP0301155		CaNb2Oz	Ca1Nb2Oz	Ca	1	Nb	2																	O	z			1991																																														K				11			11																																																																																														La2O3,SrCO3,NbO2	1	mixture-sealed in silica tube with Zr plate-heat(1100C, 24h)-FC					A NEW NON-CU-OXIDE SUPERCONDUCTOR: (SR1-XLNX)NB2O6-Y (LN:LA,ND,PR AND CE)	199107		DEPARTMENT OF PHYSICS,AOYAMA-GAKUIN UNIVERSITY,6-16-1 CHITOSEDAI,SETAGAYA,TOKYO 157	JJAP LETT.,30(1991)1155	HIROSHI SAWA,JIRO AMANO,JUN AKIMITSU,KAZUHIRO GYODA,MANAMI KOGAI,OSAMU NAGASE	SR,LA,ND,PR,CE,NB,O	
9520	SUP0110437	Hc1(77K)=2.6 mT. Hc2(77K)=9T. Cohere(77K)=60A.	(Bi,Pb)2Sr2CaCu2Oz	Bi1.75Pb0.25Sr2Ca1Cu2.3Oz	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	2.3											O	z			1998																												Bi2212																		K	85						85																																				A		18			A		5400																																																										The Effects of Substitution of Sn for Cu in Bi1.75Pb0.25Sr2CaCu2.3-xSnxSnxOy	1998		Department of Physics and National Laboratory of Solid State Microstrutures, Nanjing University, Nanjing 210093, P.R. China	J.Superconductivity,11(1998)437	J.J. Jiang,K. Shen,L.Y. Li,S.X. Dou,Wu Ming Chen,X.H. Wang,X.N.Xu,Y.C. Guo,Z. Yu		
9521	SUP0110437	Hc1(77K)=2.0 mT. Hc2(77K)=9T. Cohere(77K)=100A.	(Bi,Pb)2Sr2Ca(Cu,Sn)2Oz	Bi1.75Pb0.25Sr2Ca1Cu2.25Sn0.05Oz	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	2.25	Sn	0.05									O	z			1998																												Bi2212																		K	86						86																																									A		6000																																																										The Effects of Substitution of Sn for Cu in Bi1.75Pb0.25Sr2CaCu2.3-xSnxSnxOy	1998		Department of Physics and National Laboratory of Solid State Microstrutures, Nanjing University, Nanjing 210093, P.R. China	J.Superconductivity,11(1998)437	J.J. Jiang,K. Shen,L.Y. Li,S.X. Dou,Wu Ming Chen,X.H. Wang,X.N.Xu,Y.C. Guo,Z. Yu		
9522	SUP0110437	Bi-2223 phase=15%	(Bi,Pb)2Sr2Ca(Cu,Sn)2Oz	Bi1.75Pb0.25Sr2Ca1Cu2.15Sn0.15Oz	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	2.15	Sn	0.15									O	z			1998																																														K	106.6						106.6																																																																																																					The Effects of Substitution of Sn for Cu in Bi1.75Pb0.25Sr2CaCu2.3-xSnxSnxOy	1998		Department of Physics and National Laboratory of Solid State Microstrutures, Nanjing University, Nanjing 210093, P.R. China	J.Superconductivity,11(1998)437	J.J. Jiang,K. Shen,L.Y. Li,S.X. Dou,Wu Ming Chen,X.H. Wang,X.N.Xu,Y.C. Guo,Z. Yu		
9523	SUP0110437	Bi-2223 phase=20%	(Bi,Pb)2Sr2Ca(Cu,Sn)2Oz	Bi1.75Pb0.25Sr2Ca1Cu2.1Sn0.2Oz	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	2.1	Sn	0.2									O	z			1998																																														K	105						105																																																																																																					The Effects of Substitution of Sn for Cu in Bi1.75Pb0.25Sr2CaCu2.3-xSnxSnxOy	1998		Department of Physics and National Laboratory of Solid State Microstrutures, Nanjing University, Nanjing 210093, P.R. China	J.Superconductivity,11(1998)437	J.J. Jiang,K. Shen,L.Y. Li,S.X. Dou,Wu Ming Chen,X.H. Wang,X.N.Xu,Y.C. Guo,Z. Yu		
9524	SUP0110437	Bi-2223 phase=45%	(Bi,Pb)2Sr2Ca(Cu,Sn)2Oz	Bi1.75Pb0.25Sr2Ca1Cu1.9Sn0.4Oz	Bi	1.75	Pb	0.25	Sr	2	Ca	1	Cu	1.9	Sn	0.4									O	z			1998																																														K	99						99																																																																																																					The Effects of Substitution of Sn for Cu in Bi1.75Pb0.25Sr2CaCu2.3-xSnxSnxOy	1998		Department of Physics and National Laboratory of Solid State Microstrutures, Nanjing University, Nanjing 210093, P.R. China	J.Superconductivity,11(1998)437	J.J. Jiang,K. Shen,L.Y. Li,S.X. Dou,Wu Ming Chen,X.H. Wang,X.N.Xu,Y.C. Guo,Z. Yu		
9525	SUP0110455		NdBa2Cu3O7	Nd1Ba2Cu3O6.82	Nd	1	Ba	2	Cu	3															O	7-z	6.82	1	1998																												Y123			A	3.855	3.913	11.741												K				95			95																																																																																										7					1	conventional solid state reaction					The Superconducting and Normal-State Transport Properties in Pure, Pr-Doped, and Ca-Doped NdBa2Cu3O7-y			Materials Science Center and Department of Physics, National Tsing Hua University Hsinchu, Taiwan, Republic of China.	J.Superconductivity,11(1998)455	J.C. Chen,S.H. Cheng,Weiyan Guan		
9526	SUP0110455		(Nd,Ca)Ba2Cu3O7	Nd0.9Ca0.1Ba2Cu3O6.63	Nd	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z	6.63	1	1998																												Y123			A	3.854	3.911	11.723												K				84.5			84.5																																																																																										7					1	conventional solid state reaction					The Superconducting and Normal-State Transport Properties in Pure, Pr-Doped, and Ca-Doped NdBa2Cu3O7-y			Materials Science Center and Department of Physics, National Tsing Hua University Hsinchu, Taiwan, Republic of China.	J.Superconductivity,11(1998)455	J.C. Chen,S.H. Cheng,Weiyan Guan		
9527	SUP0110455		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O6.81	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.81	1	1998																												Y123			A	3.855	3.92	11.748												K				50			50																																																																																										7					1	conventional solid state reaction					The Superconducting and Normal-State Transport Properties in Pure, Pr-Doped, and Ca-Doped NdBa2Cu3O7-y			Materials Science Center and Department of Physics, National Tsing Hua University Hsinchu, Taiwan, Republic of China.	J.Superconductivity,11(1998)455	J.C. Chen,S.H. Cheng,Weiyan Guan		
9528	SUP0110285		GdBa2Cu3O7	Gd1Ba2Cu3O6.94	Gd	1	Ba	2	Cu	3															O	7-z	6.94	1	1998																												Y123																		K		90.8					90.8																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9529	SUP0110285		(Gd,Hf)Ba2Cu3O7	Gd0.95Hf0.05Ba2Cu3O6.91	Gd	0.95	Hf	0.05	Ba	2	Cu	3													O	7-z	6.91	1	1998																												Y123																		K		86.9					86.9																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9530	SUP0110285		(Gd,Hf)Ba2Cu3O7	Gd0.9Hf0.1Ba2Cu3O6.88	Gd	0.9	Hf	0.1	Ba	2	Cu	3													O	7-z	6.88	1	1998																												Y123																		K		84.2					84.2																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9531	SUP0110285		(Gd,Hf)Ba2Cu3O7	Gd0.85Hf0.15Ba2Cu3O6.84	Gd	0.85	Hf	0.15	Ba	2	Cu	3													O	7-z	6.84	1	1998																												Y123																		K		81.8					81.8																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9532	SUP0110285		(Gd,Hf)Ba2Cu3O7	Gd0.8Hf0.2Ba2Cu3O6.79	Gd	0.8	Hf	0.2	Ba	2	Cu	3													O	7-z	6.79	1	1998																												Y123																		K		79.5					79.5																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9533	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.8Ca0.05Hf0.15Ba2Cu3O6.86	Gd	0.8	Ca	0.05	Hf	0.15	Ba	2	Cu	3											O	7-z	6.86	1	1998																												Y123																		K		80.6					80.6																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9534	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.75Ca0.1Hf0.15Ba2Cu3O6.89	Gd	0.75	Ca	0.1	Hf	0.15	Ba	2	Cu	3											O	7-z	6.89	1	1998																												Y123																		K		82.7					82.7																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9535	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.7Ca0.15Hf0.15Ba2Cu3O6.93	Gd	0.7	Ca	0.15	Hf	0.15	Ba	2	Cu	3											O	7-z	6.93	1	1998																												Y123																		K		83.8					83.8																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9536	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.65Ca0.2Hf0.15Ba2Cu3O6.96	Gd	0.65	Ca	0.2	Hf	0.15	Ba	2	Cu	3											O	7-z	6.96	1	1998																												Y123																		K		86.3					86.3																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9537	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.6Ca0.25Hf0.15Ba2Cu3O7	Gd	0.6	Ca	0.25	Hf	0.15	Ba	2	Cu	3											O	7-z	7	1	1998																												Y123																		K		81.3					81.3																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9538	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.55Ca0.35Hf0.15Ba2Cu3O7.06	Gd	0.55	Ca	0.35	Hf	0.15	Ba	2	Cu	3											O	7-z	7.06	1	1998																												Y123																		K		76					76																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9539	SUP0110285		(Gd,Ca,Hf)Ba2Cu3O7	Gd0.45Ca0.4Hf0.15Ba2Cu3O7.08	Gd	0.45	Ca	0.4	Hf	0.15	Ba	2	Cu	3											O	7-z	7.08	1	1998																												Y123																		K		71.9					71.9																																																																																															1	conventional solid state reaction. Oz determined by iodmetric method.					Effect of M and M-Ca Substitution on the Structure and Superconductivity of GdBa2Cu3O7-delta [M=Mo, Hf]	1998		Department of Physics, Saurashtra University, Rajkot-360 005, India	J.Superconductivity,11(1998)285	Amish G. Joshi,D.G. Kuberkar,M.V. Subbarao,Nikesh A. Shah,R.G. Kulkarni,Utpal S. Joshi		
9540	SSC0780967		(Ba,K)BiO3	Ba0.62K0.38Bi1O3	Ba	0.62	K	0.38	Bi	1															O	3		3	1991																												BKBO			A	4.2832														K		21.5					21.5																																																																																																single crystals were prepared by electrorytic oxidation. Mixture(KOH:Ba(OH).8H2O:Bi2O3=70:1:1). Bath temp=210C in air					ELECTROCHEMICAL SYNTHESIS AND CHARACTERIZATION OF SUPERCONDUCTING BA1-XKXBIO3 SINGLE CRYSTALS	199106		L.E.P.E.S.,CERS,ASSOCIE A L'UNIVERSITE J.FOURIER,BP 166,38042GRANOBLE CEDEX,FRANCE	SOLID STATE COMMUN.,78(1991)967	C.ESCRIBE-FILIPPINI,C.LCHAILLOUT,J.DURR,J.L.THOLENCE,J.MARCUS,S.K.AGARWAL,T.FOURNIER	BA,K,BI,O	
9541	SSC0780967		(Ba,K)BiO3	Ba0.57K0.43Bi1O3	Ba	0.57	K	0.43	Bi	1															O	3		3	1991																												BKBO			A	4.2788														K		21.2					21.2																																																																																																single crystals were prepared by electrorytic oxidation. Mixture(KOH:Ba(OH).8H2O:Bi2O3=70:1:1). Bath temp=210C in air					ELECTROCHEMICAL SYNTHESIS AND CHARACTERIZATION OF SUPERCONDUCTING BA1-XKXBIO3 SINGLE CRYSTALS	199106		L.E.P.E.S.,CERS,ASSOCIE A L'UNIVERSITE J.FOURIER,BP 166,38042GRANOBLE CEDEX,FRANCE	SOLID STATE COMMUN.,78(1991)967	C.ESCRIBE-FILIPPINI,C.LCHAILLOUT,J.DURR,J.L.THOLENCE,J.MARCUS,S.K.AGARWAL,T.FOURNIER	BA,K,BI,O	
9542	SSC0780967		(Ba,K)BiO3	Ba0.54K0.46Bi1O3	Ba	0.54	K	0.46	Bi	1															O	3		3	1991																												BKBO			A	4.2775														K		19					19																																																																																																single crystals were prepared by electrorytic oxidation. Mixture(KOH:Ba(OH).8H2O:Bi2O3=70:1:1). Bath temp=210C in air					ELECTROCHEMICAL SYNTHESIS AND CHARACTERIZATION OF SUPERCONDUCTING BA1-XKXBIO3 SINGLE CRYSTALS	199106		L.E.P.E.S.,CERS,ASSOCIE A L'UNIVERSITE J.FOURIER,BP 166,38042GRANOBLE CEDEX,FRANCE	SOLID STATE COMMUN.,78(1991)967	C.ESCRIBE-FILIPPINI,C.LCHAILLOUT,J.DURR,J.L.THOLENCE,J.MARCUS,S.K.AGARWAL,T.FOURNIER	BA,K,BI,O	
9543	SSC0780967		(Ba,K)BiO3	Ba0.52K0.48Bi1O3	Ba	0.52	K	0.48	Bi	1															O	3		3	1991																												BKBO			A	4.2772														K		18.7					18.7																																																																																																single crystals were prepared by electrorytic oxidation. Mixture(KOH:Ba(OH).8H2O:Bi2O3=70:1:1). Bath temp=210C in air					ELECTROCHEMICAL SYNTHESIS AND CHARACTERIZATION OF SUPERCONDUCTING BA1-XKXBIO3 SINGLE CRYSTALS	199106		L.E.P.E.S.,CERS,ASSOCIE A L'UNIVERSITE J.FOURIER,BP 166,38042GRANOBLE CEDEX,FRANCE	SOLID STATE COMMUN.,78(1991)967	C.ESCRIBE-FILIPPINI,C.LCHAILLOUT,J.DURR,J.L.THOLENCE,J.MARCUS,S.K.AGARWAL,T.FOURNIER	BA,K,BI,O	
9544	SSC0780967		(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3		3	1991																												BKBO			A	4.2661														K		16.5					16.5																																																																																																single crystals were prepared by electrorytic oxidation. Mixture(KOH:Ba(OH).8H2O:Bi2O3=70:1:1). Bath temp=210C in air					ELECTROCHEMICAL SYNTHESIS AND CHARACTERIZATION OF SUPERCONDUCTING BA1-XKXBIO3 SINGLE CRYSTALS	199106		L.E.P.E.S.,CERS,ASSOCIE A L'UNIVERSITE J.FOURIER,BP 166,38042GRANOBLE CEDEX,FRANCE	SOLID STATE COMMUN.,78(1991)967	C.ESCRIBE-FILIPPINI,C.LCHAILLOUT,J.DURR,J.L.THOLENCE,J.MARCUS,S.K.AGARWAL,T.FOURNIER	BA,K,BI,O	
9545	PHC2670270		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	1996																												BKBO																		K				31.2			31.2																				T		30																																																																										starting material (Ba:K:Bi=1:1.2:75). Flux method using KOH flux.					Short time study of the fishtail effect in Ba0.6K0.4BiO3 single crystals			"Laboratoire d""Etudes des Proprie'te's Electroniques des Solides-CNRS,B.P. 166,38042 Grenoble-Cedex, France"	Physica.C,267(1996)270-278	A. Sulpice,C. Escribe-Filippini,H. Rakoto,J. Marcus,J.M. Broto,R. Buder,T. Klein,W. Harneit,W. Schmidbauer	Ba, K, Bi, O	
9546	PHC2670270		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	1996																												BKBO																		K				29.1			29.1																				T		25																																																																										starting material (Ba:K:Bi=1:1.2:75). Flux method using KOH flux.					Short time study of the fishtail effect in Ba0.6K0.4BiO3 single crystals			"Laboratoire d""Etudes des Proprie'te's Electroniques des Solides-CNRS,B.P. 166,38042 Grenoble-Cedex, France"	Physica.C,267(1996)270-278	A. Sulpice,C. Escribe-Filippini,H. Rakoto,J. Marcus,J.M. Broto,R. Buder,T. Klein,W. Harneit,W. Schmidbauer	Ba, K, Bi, O	
9547	PR06114370		HgBa2CuO4	Hg1Ba2Cu1O4.01	Hg	1	Ba	2	Cu	1															O	4+z	4.01	1	2000																												Hg1201																		K				61			61																																																																																															1	mixture(Ba2CuO3+z  + HgO)					Magnetic flux dynamics and structural features in fluorinated HgBa2CuO4 as probed by <19>F NMR	200006		Department of Physics, Moscow State University, 119899 Moscow, Russia	Phys.Rev.B,61(2000)14370-14373	A. A. Gippius,A. M. Abakumov,E. N. Morozova,E. V. Antipov,G. Buntkowsky,K. Luders,M. G. Rozova,O. Klein,W. Hoffmann		
9548	PR06114370	F-content not given	HgBa2CuO4Fx	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	2000																												Hg1201			A	3.8828		9.523												K				97			97																																																																																																HgBa2CuO4-heat treatment(150C under 0.1 XeF2)					Magnetic flux dynamics and structural features in fluorinated HgBa2CuO4 as probed by <19>F NMR	200006		Department of Physics, Moscow State University, 119899 Moscow, Russia	Phys.Rev.B,61(2000)14370-14373	A. A. Gippius,A. M. Abakumov,E. N. Morozova,E. V. Antipov,G. Buntkowsky,K. Luders,M. G. Rozova,O. Klein,W. Hoffmann		
9549	PR06114370	F-content not given	HgBa2CuO4Fx	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	2000																												Hg1201			A	3.8825		9.51												K				96			96																																																																																																HgBa2CuO4-heat treatment(200C under 0.3 XeF2)					Magnetic flux dynamics and structural features in fluorinated HgBa2CuO4 as probed by <19>F NMR	200006		Department of Physics, Moscow State University, 119899 Moscow, Russia	Phys.Rev.B,61(2000)14370-14373	A. A. Gippius,A. M. Abakumov,E. N. Morozova,E. V. Antipov,G. Buntkowsky,K. Luders,M. G. Rozova,O. Klein,W. Hoffmann		
9550	PR06114815		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	2000																												BKBO																		K		29					29																																																																																																single crystals were grown using electrochemical synthesis.					Electronic transport in Ba1-xKxBiO3 single crystals	200006		Department of Physics and Condensed Matter Research Institute, Seoul National University, Seoul 151-742, Korea	Phys.Rev.B,61(2000)14815-14820	A. B. Kaiser,D. B. Zhu,G. C. McIntosh,J. H. Lee,K. Char,L. Z. Zhao,Y. W. Park		
9551	PR06114815		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	2000																												BKBO																		K		27					27																																																																																																single crystals were grown using electrochemical synthesis.					Electronic transport in Ba1-xKxBiO3 single crystals	200006		Department of Physics and Condensed Matter Research Institute, Seoul National University, Seoul 151-742, Korea	Phys.Rev.B,61(2000)14815-14820	A. B. Kaiser,D. B. Zhu,G. C. McIntosh,J. H. Lee,K. Char,L. Z. Zhao,Y. W. Park		
9552	PR06114804	G-L parameter=106	(Ba,Pb)BiO3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3		1	2000																												BPBO																		K				11.6			11.6											mT	estimated from Hc	0.97							T		5.2							T/K		0.65					A		66			A		7000																																																				1						Determination of irreversibility fields and superconducting parameters in BaPb0.75Bi0.25O3	200006		National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,61(2000)14804-14809	A. M. Campbell,D. N. Zheng,Z. X. Zhao		
9553	PR06114795	as-grown	YBa2Cu3O7	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	3	2000																												Y123																		K		83.1					83.1																																																																																																					Fishtail effect in the magnetization of superconducting RBa2Cu3O7-z (R = Y,Nd,Yb) and Y2Ba4Cu8O16 single crystals	200006		Atominstitut der Osterreichischen Universitaten, A-1020 Vienna, Austria	Phys.Rev.B,61(2000)	A. Wisniewski,F. M. Sauerzopf,H. W. Weber,M. Werner		
9554	PR06114795	neutron irradiation, fluence=1.0E+20 /m2	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2000																												Y123																		K		83.1					83.1																																																																																																					Fishtail effect in the magnetization of superconducting RBa2Cu3O7-z (R = Y,Nd,Yb) and Y2Ba4Cu8O16 single crystals	200006		Atominstitut der Osterreichischen Universitaten, A-1020 Vienna, Austria	Phys.Rev.B,61(2000)	A. Wisniewski,F. M. Sauerzopf,H. W. Weber,M. Werner		
9555	PR06114795	neutron irradiation, fluence=1.0E+21 /m2	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2000																												Y123																		K		82.6					82.6																																																																																																					Fishtail effect in the magnetization of superconducting RBa2Cu3O7-z (R = Y,Nd,Yb) and Y2Ba4Cu8O16 single crystals	200006		Atominstitut der Osterreichischen Universitaten, A-1020 Vienna, Austria	Phys.Rev.B,61(2000)	A. Wisniewski,F. M. Sauerzopf,H. W. Weber,M. Werner		
9556	PR06114795	neutron irradiation, fluence=5.0E+20 /m2	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2000																												Y123																		K		81.1					81.1																																																																																																					Fishtail effect in the magnetization of superconducting RBa2Cu3O7-z (R = Y,Nd,Yb) and Y2Ba4Cu8O16 single crystals	200006		Atominstitut der Osterreichischen Universitaten, A-1020 Vienna, Austria	Phys.Rev.B,61(2000)	A. Wisniewski,F. M. Sauerzopf,H. W. Weber,M. Werner		
9557	PRL0854787		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.22	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.22		2000																												Bi2212																		K		82					82																																														meV	19.75	5.6																																																no description					Discriminating the Superconducting Gap from the Pseudogap in Bi2Sr2CaCu2O8+z  by Interlayer Tunneling Spectroscopy	11		Department of Electronic Science and Engineering, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev.Lett.,85(2000)4787-4790	Minoru Suzuki,Takao Watanabe		
9558	PRL0854787		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.24	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.24		2000																												Bi2212																		K		88					88																																														meV	19.5	5.15																																																no description					Discriminating the Superconducting Gap from the Pseudogap in Bi2Sr2CaCu2O8+z  by Interlayer Tunneling Spectroscopy	11		Department of Electronic Science and Engineering, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev.Lett.,85(2000)4787-4790	Minoru Suzuki,Takao Watanabe		
9559	PRL0854787		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.25	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.25		2000																												Bi2212																		K		89					89																																														meV	19.25	5.03																																																no description					Discriminating the Superconducting Gap from the Pseudogap in Bi2Sr2CaCu2O8+z  by Interlayer Tunneling Spectroscopy	11		Department of Electronic Science and Engineering, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev.Lett.,85(2000)4787-4790	Minoru Suzuki,Takao Watanabe		
9560	PRL0854787		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.28		2000																												Bi2212																		K		81					81																																														meV	11.25	3.27																																																no description					Discriminating the Superconducting Gap from the Pseudogap in Bi2Sr2CaCu2O8+z  by Interlayer Tunneling Spectroscopy	11		Department of Electronic Science and Engineering, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev.Lett.,85(2000)4787-4790	Minoru Suzuki,Takao Watanabe		
9561	EPL0520584	Tc(max)=111.7K (at 10 kbar)	TlBa2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		3	2000																												Tl2212																		K	111						111			K/kbar	0.17	10																																																																																											no description					Crossovers in the out-of-plane resistivity of  superconducting Tl2Ba2CaCu2O8 single crystals			Departement de Physique, Ecole Polytechnique Federale de Lausanne CH-1015 Lausanne, Switzerland	Europhys. Lett., 52 (2000)584	A. Halbritter,D. Pavuna,G. Mihaly,H. Berger,J.-P. Salvetat		
9562	APL0774202		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2000																												Bi2212																		K		89.5					89.5																																									A			2690																																																				floating zone. See Physica C, 177(1991)79					Measurements of the absolute value of the penetration depth in high-Tc superconductors using a low-Tc superconductive coating			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, 1110 West Green Street, Urbana, Illinois 61801	Appl.Phys.Lett., 77(2000)4202	A. Carrington,A. R. Banks,D. G. Hinks,P. Fournier,P. Guptasarma,R. L. Greene,R. Prozorov,R. W. Giannetta		
9563	APL0774202		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2000																												T'																		K		22.5					22.5																																									A			2790																																																				directional solidification technique. See Phys.Rev.B, 50(1994)523					Measurements of the absolute value of the penetration depth in high-Tc superconductors using a low-Tc superconductive coating			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, 1110 West Green Street, Urbana, Illinois 61801	Appl.Phys.Lett., 77(2000)4202	A. Carrington,A. R. Banks,D. G. Hinks,P. Fournier,P. Guptasarma,R. L. Greene,R. Prozorov,R. W. Giannetta		
9564	APL0774202		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	2000																												Y123																		K		93					93																																									A			1390																																																									Measurements of the absolute value of the penetration depth in high-Tc superconductors using a low-Tc superconductive coating			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, 1110 West Green Street, Urbana, Illinois 61801	Appl.Phys.Lett., 77(2000)4202	A. Carrington,A. R. Banks,D. G. Hinks,P. Fournier,P. Guptasarma,R. L. Greene,R. Prozorov,R. W. Giannetta		
9565	NAT3900148	stability limit of K is about 60% in this method	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3			1997																												BKBO	I4/mcm		A	5.9419		8.4394												K				12			12										40																																																																																						mixture(Sr2Bi2O5, Bi2O3, KO2)-high pressure synthesis(2GPa, 700C, 1h, Pt crucible)					Discovery of a second family of bismuth-oxide-based superconductors			CNRS, Grenoble,France	Nature, 390(1997)148	A.Rysak,C.Chaillout,J.J.Capponi,J.L.Tholence,M.Nunez-Regueiro,P.Bordet,P.G.Radaelli,S.M.Kazakov,S.N.Putilin,V.Antipov		
9566	NAT3900148	preliminary study	(Sr,Rb)BiO3	Sr0.5Rb0.5Bi1O3	Sr	0.5	Rb	0.5	Bi	1															O	3			1997																												BKBO																		K				13			13										6																																																																																						mixture(Sr2Bi2O5, Bi2O3, Rb2O)-high pressure synthesis(2GPa, 700C, 1h, Pt crucible)					Discovery of a second family of bismuth-oxide-based superconductors			CNRS, Grenoble,France	Nature, 390(1997)148	A.Rysak,C.Chaillout,J.J.Capponi,J.L.Tholence,M.Nunez-Regueiro,P.Bordet,P.G.Radaelli,S.M.Kazakov,S.N.Putilin,V.Antipov		
9567	PR06211977	60% O<18>. Delta-Tc=-0.32 K	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3			2000																												BKBO			A	5.9418		8.4394												K				11.18			11.18						0.37	O	60																																																																																								Sr2Bi2O5-ground-mixture(Sr2Bi2O5, Bi2O3, KO2)-packed(Au capsules)-HIP(2GPa, 700C, 0.5h)					Large oxygen-isotope effect in Sr0.4K0.6BiO3: Evidence for phonon-mediated superconductivity	200010		Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B,62(2000)11977-11980	C. Bougerol,E. V. Antipov,Guo-meng Zhao,J. Karpinski,J. S. Pshirkov,K. Conder,M. Angst,M. Maciejewski,S. M. Kazakov		
9568	PR06211977	80% O<18>. Delta-Tc = -0.50 K	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3			2000																												BKBO																		K				11			11						0.42	O	80																																																																																								Sr2Bi2O5-ground-mixture(Sr2Bi2O5, Bi2O3, KO2)-packed(Au capsules)-HIP(2GPa, 700C, 0.5h)					Large oxygen-isotope effect in Sr0.4K0.6BiO3: Evidence for phonon-mediated superconductivity	200010		Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B,62(2000)11977-11980	C. Bougerol,E. V. Antipov,Guo-meng Zhao,J. Karpinski,J. S. Pshirkov,K. Conder,M. Angst,M. Maciejewski,S. M. Kazakov		
9569	PR06211977	100% O<16>	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3			2000																												BKBO																		K				11.5			11.5																																																																																																Sr2Bi2O5-ground-mixture(Sr2Bi2O5, Bi2O3, KO2)-packed(Au capsules)-HIP(2GPa, 700C, 0.5h)					Large oxygen-isotope effect in Sr0.4K0.6BiO3: Evidence for phonon-mediated superconductivity	200010		Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B,62(2000)11977-11980	C. Bougerol,E. V. Antipov,Guo-meng Zhao,J. Karpinski,J. S. Pshirkov,K. Conder,M. Angst,M. Maciejewski,S. M. Kazakov		
9570	JPS0682206	Anti-ferromagnet under ambient pressure	Sr2.5Ca11.5Cu24O41	Sr2.5Ca11.5Cu24O41	Sr	2.5	Ca	11.5	Cu	24															O	41		3	1999								2.2																				LAD																		K																																																																																																							traveling-solvent-floating zone method					Antiferromagnetic Ordering in the Spin Singlet State of  the Ladder/Chain Material: Sr2.5Ca11.5Cu24O41			Department of Physics, Aoyama-Gakuin University, Setagaya-ku, Tokyo 157-8572	J.Phys.Soc. Jpn 68(2000)2206	Hirokazu Fujino,Jun Akimitsu,Kazuhisa Kakurai,Masafumi Sera,Masahiko Hiroi,Masakazu Nishi,Norio Kobayashi,Susumu Katano,Takashi Nagata		
9571	JPS0691602	specific heat was measured by thermal relaxation calorimeter	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	2000																												T																		K				28.5			28.5																																																																																																crystals were grown by a traveling-solvent floating zone method					Quasiparticle Density of States of Clean and Dirty d-Wave Superconductors: Mixed-State Specific Heat of La 2-xSrxCuO 4 Single Crystals			Department of Advanced Materials Science, University of Tokyo, 7-3-1 Hongo, Tokyo 113-0033	J.Phys.Soc. Jpn 69(2000)1602	Fumiko Sakai,Hidenori Takagi,Hiroaki Suzuki1,Masanobu Isshiki,Minoru Nohara1,Nikorn Mangkorntong		
9572	JPS0691602	specific heat was measured by thermal relaxation calorimeter	(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4		3	2000																												T																		K				37			37																																																																																																crystals were grown by a traveling-solvent floating zone method					Quasiparticle Density of States of Clean and Dirty d-Wave Superconductors: Mixed-State Specific Heat of La 2-xSrxCuO 4 Single Crystals			Department of Advanced Materials Science, University of Tokyo, 7-3-1 Hongo, Tokyo 113-0033	J.Phys.Soc. Jpn 69(2000)1602	Fumiko Sakai,Hidenori Takagi,Hiroaki Suzuki1,Masanobu Isshiki,Minoru Nohara1,Nikorn Mangkorntong		
9573	JPS0691602	specific heat was measured by thermal relaxation calorimeter	(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4		3	2000																												T																		K				32			32																																																																																																crystals were grown by a traveling-solvent floating zone method					Quasiparticle Density of States of Clean and Dirty d-Wave Superconductors: Mixed-State Specific Heat of La 2-xSrxCuO 4 Single Crystals			Department of Advanced Materials Science, University of Tokyo, 7-3-1 Hongo, Tokyo 113-0033	J.Phys.Soc. Jpn 69(2000)1602	Fumiko Sakai,Hidenori Takagi,Hiroaki Suzuki1,Masanobu Isshiki,Minoru Nohara1,Nikorn Mangkorntong		
9574	PR06211989	carrier p=0.05. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	0						0																																																																																					E-3 cm3/C	4.61										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9575	PR06211989	carrier p=0.06.P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	4.8						4.8																																																																																					E-3 cm3/C	4.11										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9576	PR06211989	carrier p=0.07.P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	9.1						9.1																																																																																					E-3 cm3/C	3.75										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9577	PR06211989	carrier p=0.1.P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	19.4						19.4																																																																																					E-3 cm3/C	3.2										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9578	PR06211989	carrier p=0.12. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	23.9						23.9																																																																																					E-3 cm3/C	2.59										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9579	PR06211989	carrier p=0.14. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	26.7						26.7																																																																																					E-3 cm3/C	2.14										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9580	PR06211989	carrier p=0.16. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	27.6						27.6																																																																																					E-3 cm3/C	1.9										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9581	PR06211989	carrier p=0.19. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	25.5						25.5																																																																																					E-3 cm3/C	1.55										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9582	PR06211989	carrier p=0.20. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	24						24																																																																																					E-3 cm3/C	1.25										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9583	PR06211989	carrier p=0.24. P estimated from Tc using Tallon's eq.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		4	2000																												Bi2201																		K	13						13																																																																																					E-3 cm3/C	1.1										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9584	PR06211989	carrier p=0.05. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	0						0																																																																																					E-3 cm3/C	3.01										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9585	PR06211989	carrier p=0.06. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	14.6						14.6																																																																																					E-3 cm3/C	2.91										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9586	PR06211989	carrier p=0.07. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	27.8						27.8																																																																																					E-3 cm3/C	2.62										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9587	PR06211989	carrier p=0.09. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	50						50																																																																																					E-3 cm3/C	2.27										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9588	PR06211989	carrier p=0.12. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	72.9						72.9																																																																																					E-3 cm3/C	1.996										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9589	PR06211989	carrier p=0.16. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	84						84																																																																																					E-3 cm3/C	1.3										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9590	PR06211989	carrier p=0.23. P estimated from Tc using Tallon's eq.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	2000																												Bi2212																		K	50						50																																																																																					E-3 cm3/C	0.97										Thin films were grown by rf magnetron sputtering . Oxygen controled by annealing.					Temperature dependence of the Hall effect in single-layer and bilayer Bi2Sr2Can-1CunOy thin films at various oxygen contents	200010		Laboratoire de Physique des Solides, Ratiment 510, Universite Paris-Sud, 91405 Orsay Cedex, France	Phys.Rev.B,62(2000)11989-11992	H. Raffy,Z. KonstantinoviC,Z. Z. Li		
9591	P063014504	overdoped, ANN(300C). Anisotropy factor r=107	Bi2Sr2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8+z	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				71.5			71.5																																									A	fitting to decoupling theory		1640																																																				as-grown-ANN(380C,1 week, in O2)					Continuity and temperature dependence of the vortex-phase boundary of Bi2Sr2CaCu2O8 + z			Electrotechnical Laboratory, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B,63(2001)014504	A. Mumtaz,G. Rajaram,H. Bando,H. Obara,N. Shirakawa,T. Nakagawa,Y. Yamaguchi		
9592	P063014504	as-grown. Anisotropy factor r=178	Bi2Sr2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8+z	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				90.5			90.5																																									A	fitting to decoupling theory		1930																																																				TSFZ method, as-grown					Continuity and temperature dependence of the vortex-phase boundary of Bi2Sr2CaCu2O8 + z			Electrotechnical Laboratory, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B,63(2001)014504	A. Mumtaz,G. Rajaram,H. Bando,H. Obara,N. Shirakawa,T. Nakagawa,Y. Yamaguchi		
9593	P063014504	underdoped, ANN(730C), Anisotropy factor r=236	Bi2Sr2CaCu2O8	Bi2.2Sr1.8Ca1Cu2O8+z	Bi	2.2	Sr	1.8	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				80.5			80.5																																									A	fitting to decoupling theory		2520																																																				as-grown-ANN(730C,1 day in air)-Q to LN2					Continuity and temperature dependence of the vortex-phase boundary of Bi2Sr2CaCu2O8 + z			Electrotechnical Laboratory, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B,63(2001)014504	A. Mumtaz,G. Rajaram,H. Bando,H. Obara,N. Shirakawa,T. Nakagawa,Y. Yamaguchi		
9594	P063054501		Y(BaSr)Cu3O7	Y1Ba1Sr1Cu3O7+z	Y	1	Ba	1	Sr	1	Cu	3													O	7+z		1	2001																											3	Y123																		K		81					81																																		HIR9594																																																														mixture-fire(880-960C, several days)-ANN(high O2 pressure)					Increase of the superconducting Tc, irreversibility fields, and critical currents in tetragonal YBaSrCu3-xMoxO7 + d			Physics Department, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,63(2001)054501	B. Dabrowski,J. D. Jorgensen,K. Rogacki,O. Chmaissem		
9595	P063054501		Y(BaSr)(Cu,Mo)3O7	Y1Ba1Sr1Cu2.95Mo0.05O7.07	Y	1	Ba	1	Sr	1	Cu	2.95	Mo	0.05											O	7+z	7.07	1	2001																											3	Y123			A	3.8263	3.8126	11.5558												K		85					85																																		HIR9595																																																														mixture-fire(880-960C, several days)-ANN(high O2 pressure)					Increase of the superconducting Tc, irreversibility fields, and critical currents in tetragonal YBaSrCu3-xMoxO7 + d			Physics Department, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,63(2001)054501	B. Dabrowski,J. D. Jorgensen,K. Rogacki,O. Chmaissem		
9596	P063054501		Y(BaSr)(Cu,Mo)3O7	Y1Ba1Sr1Cu2.9Mo0.1O7.16	Y	1	Ba	1	Sr	1	Cu	2.9	Mo	0.1											O	7+z	7.16	1	2001																											2	Y123			A	3.8221		11.5754												K		86					86																																		HIR9596																																																														mixture-fire(880-960C, several days)-ANN(high O2 pressure)					Increase of the superconducting Tc, irreversibility fields, and critical currents in tetragonal YBaSrCu3-xMoxO7 + d			Physics Department, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,63(2001)054501	B. Dabrowski,J. D. Jorgensen,K. Rogacki,O. Chmaissem		
9597	P063054501		Y(BaSr)(Cu,Mo)3O7	Y1Ba1Sr1Cu2.8Mo0.2O7.3	Y	1	Ba	1	Sr	1	Cu	2.8	Mo	0.2											O	7+z	7.3	1	2001																											2	Y123			A	3.8307		11.5984												K		68					68																																																																																																mixture-fire(880-960C, several days)-ANN(high O2 pressure)					Increase of the superconducting Tc, irreversibility fields, and critical currents in tetragonal YBaSrCu3-xMoxO7 + d			Physics Department, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,63(2001)054501	B. Dabrowski,J. D. Jorgensen,K. Rogacki,O. Chmaissem		
9598	P063014508		HgBa2CuO4	Hg1Ba2Cu1O4.15	Hg	1	Ba	2	Cu	1															O	4+z	4.15		2001																											2	Hg1201			A	3.88		9.527												K				97.2			97.2																																																																																																mixture(Ba2CuO3,ReO3,HgO)-heat(300C, in O2)					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9599	P063014508		(Hg,Re)Ba2CuO4	Hg0.95Re0.05Ba2Cu1O4.37	Hg	0.95	Re	0.05	Ba	2	Cu	1													O	4+z	4.37		2001																											2	Hg1201			A	3.872		9.464												K				96			96																																																																																																mixture(Ba2CuO3,ReO3,HgO)-heat(300C, in O2)					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9600	P063014508		(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.42	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+z	4.42		2001																											2	Hg1201			A	3.872		9.42												K				95			95																																																																																																mixture(Ba2CuO3,ReO3,HgO)-heat(300C, in O2)					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9601	P063014508		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.58	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+z	4.58		2001																											2	Hg1201			A	3.876		9.39												K				35			35																																																																																																mixture(Ba2CuO3,ReO3,HgO)-heat(300C, in O2)					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9602	P063014508	optimum oxygen	HgBa2CuO4	Hg1Ba2Cu1O4.162	Hg	1	Ba	2	Cu	1															O	4+z	4.162		2001																												Hg1201																		K				97.4			97.4																																																																																																optimization in oxygen content					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9603	P063014508	optimum oxygen	(Hg,Re)Ba2CuO4	Hg0.95Re0.05Ba2Cu1O4.372	Hg	0.95	Re	0.05	Ba	2	Cu	1													O	4+z	4.372		2001																												Hg1201																		K				97			97																																																																																																optimization in oxygen content					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9604	P063014508	optimum oxygen	(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.425	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+z	4.425		2001																												Hg1201																		K				96.8			96.8																																																																																																optimization in oxygen content					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9605	P063014508	optimum oxygen	(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.525	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+z	4.525		2001																												Hg1201																		K				96.3			96.3																																																																																																optimization in oxygen content					Oxygen content, thermodynamic stability, and superconductivity of Hg1-xRexBa2CuO4 + z				Phys.Rev.B,63(2001)014508	A. Basset,A. Caneiro,A. Serquis,J. D. Jorgensen,J. P. Hodges,S. Short		
9606	JPS0680694	R=R0+A*T2 for T<30K. G-L =55 for H//a, =2.7 for H//c	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1999																												Sr2RuO4																		K		1.49					1.49											Oe			10	50					T			1.5	0.075												A			660	33	um			0.18	3.7																																																								Intrinsic Superconducting Parameters of Sr2RuO4			epartment of Physics, Kyoto University, Kyoto 606-8502	J.Phys.Soc. Jpn 68(2000)694	Shuji NishiZaki,Takashi Akima,Yoshiteru Maeno		
9607	LTP1050927	anisotropy factor=180. other Ni-content sample were described in Phys.Rev.Lett., 80(1998)1968	Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.988Ni0.012O8	Bi	2	Sr	2	Ca	1	Cu	1.988	Ni	0.012											O	8		3	1996																												Bi2212																		K	87.1		98				92.55																																																																																																traveling-solvent-floating zone method (TSFZ)					Ni-doping effect on the anisotropic resistivity in Bi2Sr2Ca(Cu1-xNix)2Oy single crystals			Institute of Applied Physics and Cryogenics Center, Univ. of Tsukuba, Japan	J.Low Temp.Phys., 105(1996)927	H.Ikeda,I.Tomitsuka,K.Ueno,R.Yoshizaki		
9608	PRL0862122	anisotropy factor(Rc/Rab at 100K)=600	Sm(La,Sr)CuO4	Sm1La0.85Sr0.15Cu1O3.98	Sm	1	La	0.85	Sr	0.15	Cu	1													O	4-z	3.98	3	2001																												T*																		K				30			30																																									um	far-infrared reflectivity spectra			25																																																								Transverse Josephson Plasma Mode in T* Phase SmLa1-xSrxCuO4-z Single Crystals			NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)2122	H. Shibata		
9609	PRL0862122	anisotropy factor(Rc/Rab at 100K)=1000	Sm(La,Sr)CuO4	Sm1La0.8Sr0.2Cu1O3.94	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4-z	3.94	3	2001																												T*																		K				25			25																																									um	far-infrared reflectivity spectra			35																																																								Transverse Josephson Plasma Mode in T* Phase SmLa1-xSrxCuO4-z Single Crystals			NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)2122	H. Shibata		
9610	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	7-z	6.2	3	2001																												Y123																		K					4.2																																																																																													RH9610					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9611	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.25	Y	1	Ba	2	Cu	3															O	7-z	6.25	3	2001																												Y123																		K					4.2																																																																																													RH9611					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9612	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.28	Y	1	Ba	2	Cu	3															O	7-z	6.28	3	2001																												Y123																		K					4.2																																																																																																		single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9613	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	7-z	6.4	3	2001																												Y123																		K		35.8					35.8																																																																																											RH9613					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9614	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	7-z	6.45	3	2001																												Y123																		K		47.3					47.3																																																																																											RH9614					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9615	PRL0860496	anisotropy factor(Rc/Rab at 100K)=1000	YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	7-z	6.5	3	2001																												Y123																		K		58.8					58.8																																																																																											RH9615					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9616	PRL0860496	anisotropy factor(Rc/Rab at 100K)=50	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-z	6.9	3	2001																												Y123																		K		92					92																																																																																											RH9616					single crystals were grown in a yttria crucible by self-flux method. Z controlled by ANN in O2.					Superconductor-to-Insulator Transition and Transport Properties of Underdoped YBa2Cu3Oy Crystals			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi Kanagawa 243-0198, Japan	Phys.Rev.Lett., 86(2001)496	Azusa Matsuda,Kouichi Semba		
9617	PRL0860500		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2001																												T																		K		35.6					35.6																																																																																																					c-Axis Optical Response in the Static Stripe Ordered Phase of the Cuprates			Superconductivity Research Laboratory, ISTEC, Tokyo 135-0062, Japan	Phys.Rev.Lett., 86(2001)500	H.Eisaki,S. Tajima,S.Uchida,T. Noda		
9618	PRL0860500		(La,Nd,Sr)2CuO4	La1.75Nd0.1Sr0.15Cu1O4	La	1.75	Nd	0.1	Sr	0.15	Cu	1													O	4		3	2001																												T																		K		31.7					31.7																																																																																																					c-Axis Optical Response in the Static Stripe Ordered Phase of the Cuprates			Superconductivity Research Laboratory, ISTEC, Tokyo 135-0062, Japan	Phys.Rev.Lett., 86(2001)500	H.Eisaki,S. Tajima,S.Uchida,T. Noda		
9619	PRL0860500	LTO-LTT phase transition at (20-0) K	(La,Nd,Sr)2CuO4	La1.73Nd0.12Sr0.15Cu1O4	La	1.73	Nd	0.12	Sr	0.15	Cu	1													O	4		3	2001																												T																		K		26.3					26.3																																																																																																					c-Axis Optical Response in the Static Stripe Ordered Phase of the Cuprates			Superconductivity Research Laboratory, ISTEC, Tokyo 135-0062, Japan	Phys.Rev.Lett., 86(2001)500	H.Eisaki,S. Tajima,S.Uchida,T. Noda		
9620	PRL0860500	LTO-LTT phase transition at 44 K	(La,Nd,Sr)2CuO4	La1.65Nd0.2Sr0.15Cu1O4	La	1.65	Nd	0.2	Sr	0.15	Cu	1													O	4		3	2001																												T																		K		20					20																																																																																																					c-Axis Optical Response in the Static Stripe Ordered Phase of the Cuprates			Superconductivity Research Laboratory, ISTEC, Tokyo 135-0062, Japan	Phys.Rev.Lett., 86(2001)500	H.Eisaki,S. Tajima,S.Uchida,T. Noda		
9621	PRL0860500	LTO-LTT phase transition at 74 K	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	2001																												T																		K		9.8					9.8																																																																																																					c-Axis Optical Response in the Static Stripe Ordered Phase of the Cuprates			Superconductivity Research Laboratory, ISTEC, Tokyo 135-0062, Japan	Phys.Rev.Lett., 86(2001)500	H.Eisaki,S. Tajima,S.Uchida,T. Noda		
9622	JPS0700437	THC by a steady-state method	Sr14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41		3	2001																												LAD																																																																																										THC9622																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9623	JPS0700437	THC by a steady-state method	(Sr,La)14Cu24O41	Sr13La1Cu24O41	Sr	13	La	1	Cu	24															O	41		3	2001																												LAD																																																																																										THC9623																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9624	JPS0700437	THC by a steady-state method	(Sr,La)14Cu24O41	Sr11La3Cu24O41	Sr	11	La	3	Cu	24															O	41		3	2001																												LAD																																																																																										THC9624																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9625	JPS0700437	THC by a steady-state method	(Sr,La)14Cu24O41	Sr9La5Cu24O41	Sr	9	La	5	Cu	24															O	41		3	2001																												LAD																																																																																										THC9625																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9628	JPS0700437	THC by a steady-state method	(Sr,Ca)14Cu24O41	Sr12.5Ca1.5Cu24O41	Sr	12.5	Ca	1.5	Cu	24															O	41		3	2001																												LAD																																																																																										THC9628																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9629	JPS0700437	THC by a steady-state method	(Sr,Ca)14Cu24O41	Sr11Ca3Cu24O41	Sr	11	Ca	3	Cu	24															O	41		3	2001																												LAD																																																																																										THC9629																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9630	JPS0700437	THC by a steady-state method	(Sr,Ca)14Cu24O41	Sr8Ca6Cu24O41	Sr	8	Ca	6	Cu	24															O	41		3	2001																												LAD																																																																																										THC9630																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9631	JPS0700437	THC by a steady-state method	(Sr,Ca)14Cu24O41	Sr5Ca9Cu24O41	Sr	5	Ca	9	Cu	24															O	41		3	2001																												LAD																																																																																										THC9631																															TSFZ method					Spin Gap and Hole Pairing in the Spin-Ladder Cuprate Sr14-xAxCu24O41 (A=Ca and La) Studied by the Thermal Conductivity			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579	J.Phys.Soc.jpn , 70(2001)437	Katsuhiko Maki,Kazutaka Kudo,Ken-ichi Kumagai,Satoru Ishikawa,Shigenori Tsuji,Tadashi Adachi,Takashi Noji,Yoji Koike		
9632	PHC3510078	dc susceptibility shows Tc=340K	PbCO3.2PbO+Ag2O	Pb2C1Ag2O6	Pb	2	C	1	Ag	2															O	6			2001																																														K	310	323	333	340			323																																																																																																(PbCO3.2PbO+Ag2O)  - press - heat(330C, 24h in 5 bar CO2)  - heat(24h in CO2+O2)					PbCO3.2PbO + Ag2O and PbCO3.PbO + Ag2O(PACO) systems: route for novel superconductors			A.Volta Applied Ceramics (AVAC), Zagrev,Croatia	Physica C, 351(2001)78-81	A.Tonejc,D.Djurek,M.Paljevic,Z.Medunic		
9633	JPS0700333	Meissner state not observed. Resistivity = zero at 23 K. M(T) and NED shows magnetic Curie-T = 149 K.	RuSr2YCu2O8	Ru1Sr2Y1Cu2O8	Ru	1	Sr	2	Y	1	Cu	2													O	8		1	2001					per Ru	0.96	149																					Ru1212			A	3.843		11.555												K	24		46				35																																																																																														SrCO3,Y2O3,CuO,Ru	1	precursor(Sr2YRuO6)+CuO. Mixture - sealed in Au - SIN(1300C, 0.5h under 5.5 Gpa) - ANN(600C, 40h in 200 kgf/cm2 (Ar:O2=80:20)					Coexistence of Superconductivity and (Anti-)Ferromagnetism in RuSr2YCu2O8			Department of Physics, Aoyama-Gakuin University, Setagaya-ku, Tokyo 157-8572	J.Phys.Soc.Jpn, 70(2001)333-336	Hazuki Kawano-Furukawa,Hideki Yoshizawa,Hiroyuki Takagiwa,Jun Akimitsu		
9634	PHC3510245	THC300=THC150, TP300=TP200	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K		78					78																																																													mW/cm.K	45.8				uV/K	5.35				mOhm.cm											2.59														high pressure O2-gas technique					Thermal transport of Pr substituted YBa2Cu4O8 compounds with CuO double chains			Faculty of Engineering, Iwate University, Ueda 4-3-5, Morioka 020 8551, Japan	Physica C, 351(2001)245	Hiromitsu Ogasawara,Michiaki Matsukawa,Ryuichi Sano,Sigeru Horii,Yuh Yamada		
9635	PHC3510245	THC300=THC150, TP300=TP200	(Y,Pr)Ba2Cu4O8	Y0.3Pr0.7Ba2Cu4O8	Y	0.3	Pr	0.7	Ba	2	Cu	4													O	8		1	2001																												Y124																		K		20					20																																																													mW/cm.K	47.3				uV/K	22.8				mOhm.cm											1														high pressure O2-gas technique					Thermal transport of Pr substituted YBa2Cu4O8 compounds with CuO double chains			Faculty of Engineering, Iwate University, Ueda 4-3-5, Morioka 020 8551, Japan	Physica C, 351(2001)245	Hiromitsu Ogasawara,Michiaki Matsukawa,Ryuichi Sano,Sigeru Horii,Yuh Yamada		
9636	PHC3510245	THC300=THC150, TP300=TP200	(Y,Pr)Ba2Cu4O8	Y0.2Pr0.8Ba2Cu4O8	Y	0.2	Pr	0.8	Ba	2	Cu	4													O	8		1	2001																												Y124																		K					5																																																															mW/cm.K	32.3				uV/K	28.1				mOhm.cm											3														high pressure O2-gas technique					Thermal transport of Pr substituted YBa2Cu4O8 compounds with CuO double chains			Faculty of Engineering, Iwate University, Ueda 4-3-5, Morioka 020 8551, Japan	Physica C, 351(2001)245	Hiromitsu Ogasawara,Michiaki Matsukawa,Ryuichi Sano,Sigeru Horii,Yuh Yamada		
9637	PHC3510245	THC300=THC150, TP300=TP200	(Y,Pr)Ba2Cu4O8	Y0.1Pr0.9Ba2Cu4O8	Y	0.1	Pr	0.9	Ba	2	Cu	4													O	8		1	2001																												Y124																		K					5																																																															mW/cm.K	37				uV/K	47.2				mOhm.cm											3.4														high pressure O2-gas technique					Thermal transport of Pr substituted YBa2Cu4O8 compounds with CuO double chains			Faculty of Engineering, Iwate University, Ueda 4-3-5, Morioka 020 8551, Japan	Physica C, 351(2001)245	Hiromitsu Ogasawara,Michiaki Matsukawa,Ryuichi Sano,Sigeru Horii,Yuh Yamada		
9638	PHC3510245	THC300=THC150, TP300=TP200	(Y,Pr)Ba2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K					5																																																															mW/cm.K	23.6				uV/K	64.6				mOhm.cm											0.6														high pressure O2-gas technique					Thermal transport of Pr substituted YBa2Cu4O8 compounds with CuO double chains			Faculty of Engineering, Iwate University, Ueda 4-3-5, Morioka 020 8551, Japan	Physica C, 351(2001)245	Hiromitsu Ogasawara,Michiaki Matsukawa,Ryuichi Sano,Sigeru Horii,Yuh Yamada		
9639	PHC1910211		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	1992																												Bi2212																		K				75.5			75.5						0.03	O	90	0.27																																																																																					Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9640	PHC1910211		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.937Y0.063Cu2O8+z	Bi	2	Sr	2	Ca	0.937	Y	0.063	Cu	2											O	8+z		1	1992																												Bi2212																		K				78			78						0.012	O	90	0.11																																																																																					Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9641	PHC1910211		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.875Y0.125Cu2O8+z	Bi	2	Sr	2	Ca	0.875	Y	0.125	Cu	2											O	8+z		1	1992																												Bi2212																		K				77.1			77.1							O	90																																																																																						Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9642	PHC1910211		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.75Y0.25Cu2O8+z	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	2											O	8+z		1	1992																												Bi2212																		K				71.3			71.3						0.065	O	90	0.54																																																																																					Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9643	PHC1910211		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.65Y0.35Cu2O8+z	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	2											O	8+z		1	1992																												Bi2212																		K				45.2			45.2						0.109	O	90	0.58																																																																																					Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9645	PHC1910211		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.55Y0.45Cu2O8+z	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	2											O	8+z		1	1992																												Bi2212																		K				22.1			22.1							O	90																																																																																						Bi2O3,SrCO3,CaO,Y2O3,CuO	1						DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9646	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.975Ca0.025Ba2Cu4O8	Y	0.975	Ca	0.025	Ba	2	Cu	4													O	8		1	1992																												Y124																		K				79.5			79.5						0.083	O	90	0.77																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9647	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.95Ca0.05Ba2Cu4O8	Y	0.95	Ca	0.05	Ba	2	Cu	4													O	8		1	1992																												Y124																		K				82.2			82.2						0.062	O	90	0.62																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9648	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.925Ca0.075Ba2Cu4O8	Y	0.925	Ca	0.075	Ba	2	Cu	4													O	8		1	1992																												Y124																		K				83.8			83.8						0.051	O	90	0.5																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9649	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8		1	1992																												Y124																		K				88.9			88.9						0.023	O	90	0.24																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9650	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.8Ca0.2Ba2Cu4O8	Y	0.8	Ca	0.2	Ba	2	Cu	4													O	8		1	1992																												Y124																		K				85.6			85.6						0.047	O	90	0.47																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9651	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.75Ca0.25Ba2Cu4O8	Y	0.75	Ca	0.25	Ba	2	Cu	4													O	8			1992																												Y124																		K				82.9			82.9							O	90																																																																																						Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9652	PHC1910211		(Y,Ca)Ba2Cu4O8	Y0.7Ca0.3Ba2Cu4O8	Y	0.7	Ca	0.3	Ba	2	Cu	4													O	8			1992																												Y124																		K				79.5			79.5						0.074	O	90	0.69																																																																																					Y2O3,BaO2,CaO,CuO	1	high O2 pressure synthesis. For x>0.1, (Ba,Ca)2Cu3+z phase increasing					DEPENDENCE OF THE OXYGEN ISOTOPE EFFECT UPON HOLE DENSITY IN BI2SR2CA1-XYXCU2O8+Z AND Y1-XCAXBA2CU4O8	199202			PHYSICA C,191(1992)211	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN,P.K.NARWANKAR	BI,SR,CA,Y,CU,O,BA	
9653	PRL0864100	NeelT by NED. Having large correlation length (100A)	YBa2Cu3O6.5	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	7-z	6.5	3	2001								310																				Y123																		K				55			55																																																																																																top seed melt texturing method					Antiferromagnetic Ordering in Superconducting YBa2Cu3O6.5				Phys.Rev.Lett., 86(2001)4100	B.Keimer,C.Bemhand,C.Niedemayer,C.Ulrich,L.P.Regnault,N.H.Andersen,P.Bourges,Y.Sidis		
9654	SST0131356	fully oxygenated, Hirr(77K)=13.1T	NdBa2Cu3Oz	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	2000																												Y123																		K				95.85			95.85																																									um			0.167	0.84						15000																																													slow cooling method					Effect of oxygen-induced disorder on magnetic flux dynamics and critical current in a NdBa2Cu3O7-d single crystal				Supercond. Sci. Technol.,13(2000)1356-1362	H. Kupfer,N. H. Kumar,Th. Wolf		
9655	SST0131356	oxygen deficient crystal, Hirr(77K)=7T	NdBa2Cu3Oz	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		3	2000																												Y123																		K				94.2			94.2																																									um			0.187	1.21						32000																																													slow cooling method					Effect of oxygen-induced disorder on magnetic flux dynamics and critical current in a NdBa2Cu3O7-d single crystal				Supercond. Sci. Technol.,13(2000)1356-1362	H. Kupfer,N. H. Kumar,Th. Wolf		
9656	SST0131302		(Tl,Pb)(Sr,Ba)Ca2Cu3Oz	Tl0.52Pb0.5Sr0.8Ba0.2Ca2Cu3Oz	Tl	0.52	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3									O	z			2000									4.2																			Tl1223																		K	115						115																																																			790																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9657	SST0131302		(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.54Pb0.5Sr0.8Ba0.2Ca2Cu3U0.005Oz	Tl	0.54	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.005							O	z			2000									4.34																			Tl1223																		K	114						114																																																			810																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9658	SST0131302		(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.54Pb0.5Sr0.8Ba0.2Ca2Cu3U0.01Oz	Tl	0.54	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.01							O	z			2000									4.44																			Tl1223																		K	113						113																																																			840																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9659	SST0131302		(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.51Pb0.5Sr0.8Ba0.2Ca2Cu3U0.02Oz	Tl	0.51	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.02							O	z			2000									4.89																			Tl1223																		K	114						114																																																			980																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9660	SST0131302		(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.5Pb0.5Sr0.8Ba0.2Ca2Cu3U0.04Oz	Tl	0.5	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.04							O	z			2000									4.48																			Tl1223																		K	114						114																																																			810																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9661	SST0131302	two step transition	(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.53Pb0.5Sr0.8Ba0.2Ca2Cu3U0.08Oz	Tl	0.53	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.08							O	z			2000									4.34																			Tl1223																		K	107						107																																																			365																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9662	SST0131302	two step transition	(Tl,Pb)(Sr,Ba)Ca2(Cu3,U)Oz	Tl0.5Pb0.5Sr0.8Ba0.2Ca2Cu3U0.2Oz	Tl	0.5	Pb	0.5	Sr	0.8	Ba	0.2	Ca	2	Cu	3	U	0.2							O	z			2000									4.37																			Tl1223																		K	103						103																																																			280																																												1	precursor + PbO + Tl2O3					Uranium-doped thallium-1223 superconductors				Supercond. Sci. Technol.,13( 2000)1302-1305	G. Gritzner,M.Eder		
9663	P063184504	anisotropy factor=100, parameters obtained by fitting of Koshelev theory(PRL 76(1996)1340)	(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.64Pb0.36Sr2Ca0.79Y0.21Cu2O8+z	Bi	1.64	Pb	0.36	Sr	2	Ca	0.79	Y	0.21	Cu	2									O	8+z		3	2001																												Bi2212																		K				86		2	86																																				A	Koshelev theory for resistivity		20		A	Koshelev theory for resistivity		2000																											mOhm.cm												0.3	250												self flux method					Experimental evidence of the decoupling line in (Bi1.64Pb0.36)Sr2(Ca0.79Y0.21)Cu2O8+z single crystals by resistivity measurements				Phys.Rev.B, 63(2001)184504	Ch. Goupil,Ch.Simon,D.Thopart		
9664	SSC1140107		La2CuOz	La2Cu1O4.0625	La	2	Cu	1																	O	4+z	4.0625		2000																												T 			A	5.3593	5.3786	13.2087												K				17			17																																																																		uV/K	48																													electrochemical oxydation					Superconducting phase with Tc of 17 K in La2CuO4+ z			National Laboratory for Superconductivity, Institute of Physics and Center for Condensed Matter Physics, Beijing 100080, People's Republic of China	Solid State Commun., 114(2000)107	C.Dong,F.Zhou,G.C.Che,Ling Chen,Y.Z.Huang,Z.X.Zhao		
9665	SSC1140107	two phases (32K phase , 17K phase)	La2CuOz	La2Cu1O4.08	La	2	Cu	1																	O	4+z	4.08		2000																												T			A	5.3338	5.4346	13.227												K				32			32																																																																																																electrochemical oxydation					Superconducting phase with Tc of 17 K in La2CuO4+ z			National Laboratory for Superconductivity, Institute of Physics and Center for Condensed Matter Physics, Beijing 100080, People's Republic of China	Solid State Commun., 114(2000)107	C.Dong,F.Zhou,G.C.Che,Ling Chen,Y.Z.Huang,Z.X.Zhao		
9667	IMP0141567	Tc = intragranular Tc.	(Bi,Pb)2(Sr,Ba)2(Ca,Er)2Cu3Oz	Bi1.6Pb0.4Sr1.8Ba0.2Ca1Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.8	Ba	0.2	Ca	1	Cu	3									O	z		1	2000																											2	Bi2223																		K		109.3					109.3																																																																																															1	solid state reaction.					Electrical andmagnetic properties of bulk (Bi1.6Pb0.4)(Sr1.8Ba0.2)(Ca1-xErx)2Cu3Oy superconducting system			Faculty of Physics, University of Babes-Bolyoi, Romania	Int'l.J.Mod.Phys., 14(2000)1567	A.V.Pop,GH.Ilonca,I.G.Deac,R.Deltour		
9668	IMP0141567	Tc = intragranular Tc. Bi2212 phase exist by XRD.	(Bi,Pb)2(Sr,Ba)2Ca2Cu3Oz	Bi1.6Pb0.4Sr1.8Ba0.2Ca1.99Er0.01Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.8	Ba	0.2	Ca	1.99	Er	0.01	Cu	3							O	z			2000																											2	Bi2223																		K		107.6					107.6																																																																																															1	solid state reaction.					Electrical andmagnetic properties of bulk (Bi1.6Pb0.4)(Sr1.8Ba0.2)(Ca1-xErx)2Cu3Oy superconducting system			Faculty of Physics, University of Babes-Bolyoi, Romania	Int'l.J.Mod.Phys., 14(2000)1567	A.V.Pop,GH.Ilonca,I.G.Deac,R.Deltour		
9669	IMP0141567	Tc = intragranular Tc. Bi2212 phase exist by XRD.	(Bi,Pb)2(Sr,Ba)2(Ca,Er)2Cu3Oz	Bi1.6Pb0.4Sr1.8Ba0.2Ca1.98Er0.02Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.8	Ba	0.2	Ca	1.98	Er	0.02	Cu	3							O	z			2000																											2	Bi2223																		K		107					107																																																																																															1	solid state reaction.					Electrical andmagnetic properties of bulk (Bi1.6Pb0.4)(Sr1.8Ba0.2)(Ca1-xErx)2Cu3Oy superconducting system			Faculty of Physics, University of Babes-Bolyoi, Romania	Int'l.J.Mod.Phys., 14(2000)1567	A.V.Pop,GH.Ilonca,I.G.Deac,R.Deltour		
9670	IMP0141567	Tc = intragranular Tc. Bi2212 phase exist by XRD.	(Bi,Pb)2(Sr,Ba)2(Ca,Er)2Cu3Oz	Bi1.6Pb0.4Sr1.8Ba0.2Ca1.97Er0.03Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.8	Ba	0.2	Ca	1.97	Er	0.03	Cu	3							O	z			2000																											2	Bi2223																		K		106					106																																																																																															1	solid state reaction.					Electrical andmagnetic properties of bulk (Bi1.6Pb0.4)(Sr1.8Ba0.2)(Ca1-xErx)2Cu3Oy superconducting system			Faculty of Physics, University of Babes-Bolyoi, Romania	Int'l.J.Mod.Phys., 14(2000)1567	A.V.Pop,GH.Ilonca,I.G.Deac,R.Deltour		
9671	IMP0141567	Tc = intragranular Tc. Bi2212 phase exist by XRD.	(Bi,Pb)2(Sr,Ba)2(Ca,Er)2Cu3Oz	Bi1.6Pb0.4Sr1.8Ba0.2Ca1.96Er0.04Cu3Oz	Bi	1.6	Pb	0.4	Sr	1.8	Ba	0.2	Ca	1.96	Er	0.04	Cu	3							O	z			2000																											2	Bi2223																		K		105.5					105.5																																																																																															1	solid state reaction.					Electrical andmagnetic properties of bulk (Bi1.6Pb0.4)(Sr1.8Ba0.2)(Ca1-xErx)2Cu3Oy superconducting system			Faculty of Physics, University of Babes-Bolyoi, Romania	Int'l.J.Mod.Phys., 14(2000)1567	A.V.Pop,GH.Ilonca,I.G.Deac,R.Deltour		
9672	JAC2250586		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1995																											3	Y124			A	3.8538	3.8745	27.267												K		78					78																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9673	JAC2250586		(Y,Eu)Ba2Cu4O8	Y0.75Eu0.25Ba2Cu4O8	Y	0.75	Eu	0.25	Ba	2	Cu	4													O	8		1	1995																											3	Y124			A	3.8648	3.8861	27.29												K		78					78																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9674	JAC2250586		(Y,Eu)Ba2Cu4O8	Y0.5Eu0.5Ba2Cu4O8	Y	0.5	Eu	0.5	Ba	2	Cu	4													O	8		1	1995																											3	Y124			A	3.8743	3.893	27.292												K		77					77																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9675	JAC2250586		(Y,Eu)Ba2Cu4O8	Y0.25Eu0.75Ba2Cu4O8	Y	0.25	Eu	0.75	Ba	2	Cu	4													O	8		1	1995																											3	Y124			A	3.8745	3.8921	27.292												K		75					75																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9676	JAC2250586		EuBa2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		1	1995																											3	Y124			A	3.882	3.8951	27.271												K		74					74																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9677	JAC2250586		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O	8		1	1995																											3	Y124			A	3.8623	3.8823	27.21												K		73					73																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9678	JAC2250586		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.92Fe0.08O8	Y	1	Ba	2	Cu	3.92	Fe	0.08													O	8		1	1995																											3	Y124			A	3.8792	3.9084	27.138												K		70					70																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9679	JAC2250586		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.88Fe0.12O8	Y	1	Ba	2	Cu	3.88	Fe	0.12													O	8		1	1995																											3	Y124			A	3.8718	3.9113	27.131												K		65					65																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9680	JAC2250586	Y124 + Y123	YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8	Y	1	Ba	2	Cu	3.84	Fe	0.16													O	8			1995																											3	Y124			A	3.8678	3.8865	27.981												K		61					61																																																																																																sol-gel method					Sol-gel synthesis and characterization of superconducting (Y1-xEux)Ba2(Cu1-y<57>Fey)4O8 samples			Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, Finland	J.Alloys Compd., 225(1995)586	Aivaras Kareiva,Johan Linden,Lauri Niinisto,Maarit Karppinen,Mikk Lippmaa		
9681	ZPB1020037	not s/c	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.97Cu0.03O6	Sr	2	Y	1	Ru	0.97	Cu	0.03													O	6			1997																											3	2116			A	5.7548	5.7852	8.1728																																																																																																																		1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9682	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.96Cu0.04O6	Sr	2	Y	1	Ru	0.96	Cu	0.04													O	6			1997																												2116																		K	5.1						5.1																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9683	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.95Cu0.05O6	Sr	2	Y	1	Ru	0.95	Cu	0.05													O	6			1997																											3	2116			A	5.7551	5.7841	8.1729												K	11.9						11.9																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9684	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.92Cu0.08O6	Sr	2	Y	1	Ru	0.92	Cu	0.08													O	6			1997																												2116																		K	17.6						17.6																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9685	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.9Cu0.1O6	Sr	2	Y	1	Ru	0.9	Cu	0.1													O	6			1997																											3	2116			A	5.7555	5.7868	8.1737												K	20.4						20.4																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9686	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.8Cu0.2O6	Sr	2	Y	1	Ru	0.8	Cu	0.2													O	6			1997																												2116																		K	23						23																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9687	ZPB1020037		Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.5Cu0.5O6	Sr	2	Y	1	Ru	0.5	Cu	0.5													O	6			1997																												2116																		K	61.5						61.5																																																																																															1	mixture-CAL(1000C, several days in air)-SIN(1390C, 12h in O2)-ANN(1330C-1400C)					Anomalous magnetic and superconducting properties in a Ru-based double perovskite			Materials Science Center and Department of Physics, Hsinchu, Taiwan, ROC	Z.Phys.B, 102(1997)37	C.Y.Tai,D.C.Ling,D.H.Chen,D.Y.Chen,F.C.Zhang,F.Z.Chien,G.Y.Tseng,M.K.Wu,S.R.Sheen		
9688	EPJ0150649	anomaly in magnetization appears at 23 K due to Ru-ordering.	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.5Cu0.5O6	Sr	2	Y	1	Ru	0.5	Cu	0.5													O	6			2000																												2116																		K			45	45		15	45																																																																																														SrCO3,Y2O3,CuO,RuO2	1	mixture-CAL(1000C in air)					Magnetism and superconductivity in Sr2YRu1-uCuuO6 and magnetism in Ba2GdRu1-uCuuO6			Physics Department, University of Notre Dame, Notre Dame, IN 46556, USA	Euro.Phys.J. B, 15(2000)649	A.J.Greer,B.Hitti,C.E.Stronach,D.B.Pulling,D.R.Harshman,D.Y.Chen,E.Koster,F.Z.Chien,H.A.Blackstead,J.D.Dow,M.Haka,M.J.DeMarco,M.K.Wu,S.Toorongian,W.J.Kossler		
9689	EPJ0150649	Two magnetic transitions at 48 K(Ru sublattice ordering) and 12.5 K(Gd sublattice ordering). Not s/c	Ba2Gd(Ru,Cu)O6	Ba2Gd1Ru0.9Cu0.1O6	Ba	2	Gd	1	Ru	0.9	Cu	0.1													O	6			2000																												2116																		K					4.2																																																																																																SrCO3,Y2O3,CuO,RuO2	1	mixture-CAL(1000C in air)					Magnetism and superconductivity in Sr2YRu1-uCuuO6 and magnetism in Ba2GdRu1-uCuuO6			Physics Department, University of Notre Dame, Notre Dame, IN 46556, USA	Euro.Phys.J. B, 15(2000)649	A.J.Greer,B.Hitti,C.E.Stronach,D.B.Pulling,D.R.Harshman,D.Y.Chen,E.Koster,F.Z.Chien,H.A.Blackstead,J.D.Dow,M.Haka,M.J.DeMarco,M.K.Wu,S.Toorongian,W.J.Kossler		
9690	P063144514	magnitude of isotope effect depends on Tc. Alpha derived from curve fitting using alpha(Tc)	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2001																												T																		K		1.5					1.5						0.18	O																																																																																									single crystals were grown by FZ method					Sign reversal of the oxygen isotope effect on Tc in Sr2RuO4			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 63(2001)144514	M.Udagawa,S.Nimori,S.Sakita,Y.Maeno,Y.Mori,Z.Q.Mao		
9691	P063144514	alpha is negative	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2001																												T																		K		1.35					1.35	ISO9691					-0.04	O																																																																																									single crystals were grown by FZ method					Sign reversal of the oxygen isotope effect on Tc in Sr2RuO4			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 63(2001)144514	M.Udagawa,S.Nimori,S.Sakita,Y.Maeno,Y.Mori,Z.Q.Mao		
9692	SST0080079		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1995	cm3.K/mol	0.000233	cm3.K/mol	0.03			15.4																				3	Y124			A	3.8538	3.8745	27.267												K		78					78																																																																																																sol-gel method					Iron substitution effects in YBa2Cu4O8 synthesized by the sol-gel technique				Supercond.Sci.Tecknol., 8(1995)79	A.Dareiva,J.Linden,J.Valo,K.Terryll,K.V.Rao,L.Ninisto,M.Karppinen,M.Leskela,V.Kozlov		
9693	SST0080079		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O	8			1995	cm3.K/mol	0.000275	cm3.K/mol	0.18			7.6																				3	Y124			A	3.8623	3.8823	27.21												K		73					73																																																																																																sol-gel method					Iron substitution effects in YBa2Cu4O8 synthesized by the sol-gel technique				Supercond.Sci.Tecknol., 8(1995)79	A.Dareiva,J.Linden,J.Valo,K.Terryll,K.V.Rao,L.Ninisto,M.Karppinen,M.Leskela,V.Kozlov		
9694	SST0080079		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.92Fe0.08O8	Y	1	Ba	2	Cu	3.92	Fe	0.08													O	8			1995	cm3.K/mol	0.000445	cm3.K/mol	0.34			-0.6																				3	Y124			A	3.8792	3.9084	27.138												K		70					70																																																																																																sol-gel method					Iron substitution effects in YBa2Cu4O8 synthesized by the sol-gel technique				Supercond.Sci.Tecknol., 8(1995)79	A.Dareiva,J.Linden,J.Valo,K.Terryll,K.V.Rao,L.Ninisto,M.Karppinen,M.Leskela,V.Kozlov		
9695	SST0080079		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.88Fe0.12O8	Y	1	Ba	2	Cu	3.88	Fe	0.12													O	8			1995	cm3.K/mol	0.000375	cm3.K/mol	0.43			-12.3																				3	Y124			A	3.8718	3.9113	27.131												K		65					65																																																																																																sol-gel method					Iron substitution effects in YBa2Cu4O8 synthesized by the sol-gel technique				Supercond.Sci.Tecknol., 8(1995)79	A.Dareiva,J.Linden,J.Valo,K.Terryll,K.V.Rao,L.Ninisto,M.Karppinen,M.Leskela,V.Kozlov		
9696	SST0080079		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8	Y	1	Ba	2	Cu	3.84	Fe	0.16													O	8			1995																											3	Y124			A	3.8678	3.8865	27.981												K		61					61																																																																																																sol-gel method					Iron substitution effects in YBa2Cu4O8 synthesized by the sol-gel technique				Supercond.Sci.Tecknol., 8(1995)79	A.Dareiva,J.Linden,J.Valo,K.Terryll,K.V.Rao,L.Ninisto,M.Karppinen,M.Leskela,V.Kozlov		
9697	P063132502	underdoped sample. Gap by ARPES.	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.38Sr2.01Cu1O6-z	Bi	1.8	Pb	0.38	Sr	2.01	Cu	1													O	6-z		3	2001																												Bi2201																		K				19			19																																														meV	14		9																																															TSFZ method. Oxygen content controlled by annealing (500 - 600C)					Fermi surface and superconducting gap in superstructure-free Bi1.80Pb0.38Sr2.01CuO6-z			Department of Physics, Tohoku University, 980-8578 Sendai, Japan	Phys.Rev.B, 63(2001)132502	I.Chong,M.Takano,T.Kamiyama,T.Sato,T.Takahashi,T.Terashima,Y.Naitoh		
9698	PRL0692276	Hc2 by torque method. Anisotropy factor > 150	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1992																												Bi2212																		K				84.7			84.7																				T	torque		22																		A			1100																																																				TSFZ method					Magnetic anisotropy of a Bi2Sr2CaCu2Ox single crystal			Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev.Lett., 69(1992)2276	A.A.Menovsky,A.Koshelev,B.Ivlev,D.G.de Groot, Z.Tamavski,J.C.Martinez,P.H.Kes,R.P.Griessen,S.H.Brongersma		
9699	PHC2820073	R(H) was measured, but not analyzed	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.9Cu1O6-z	Sr	2	Y	1	Ru	0.9	Cu	1													O	6-z			1997																												2116																		K	25	60	85				60																																																																																														SrCO3,RuO2,Y2O3,CuO	1	mixture-CAL(1000C)-SIN(1380C in 30%Ar + 70%O2)					Superconductivity in Ru-based double perovskite - The possible existence of a new superconducting pairing state				Physica C, 282(1997)73	D.C.Ling,D.Y.Chen,F.Z.Chien,J.L.Tseng,M.J.Wang,M.K.Wu,S.R.Sheen		
9700	PHC2820073	R(H) was measured, but not analyzed	Ba2Y(Ru,Cu)O6	Ba2Y1Ru0.9Cu0.1O6-z	Ba	2	Y	1	Ru	0.9	Cu	0.1													O	6-z			1997																												2116																		K	30		100				65																																																																																														BaCO3,RuO2,Y2O3,CuO	1	mixture-CAL(1000C)-SIN(1460C in 30%Ar + 70%O2)					Superconductivity in Ru-based double perovskite - The possible existence of a new superconducting pairing state				Physica C, 282(1997)73	D.C.Ling,D.Y.Chen,F.Z.Chien,J.L.Tseng,M.J.Wang,M.K.Wu,S.R.Sheen		
9701	PHC2920225		(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.95Ca0.05Cu3O8.1	Pb	2	Sr	2	Eu	0.95	Ca	0.05	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		59					59																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9702	PHC2920225		(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.9Ca0.1Cu3O8.1	Pb	2	Sr	2	Eu	0.9	Ca	0.1	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		69					69																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9703	PHC2920225		(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.85Ca0.15Cu3O8.1	Pb	2	Sr	2	Eu	0.85	Ca	0.15	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		71					71																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9704	PHC2920225		(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.8Ca0.2Cu3O8.1	Pb	2	Sr	2	Eu	0.8	Ca	0.2	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		73					73																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9705	PHC2920225		(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.75Ca0.25Cu3O8.1	Pb	2	Sr	2	Eu	0.75	Ca	0.25	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		74					74																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9706	PHC2920225	small amount of Sr2PbO4	(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.7Ca0.3Cu3O8.1	Pb	2	Sr	2	Eu	0.7	Ca	0.3	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		73					73																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9707	PHC2920225	small amount of Sr2PbO4	(Pb2Cu)Sr2(Eu,Ca)Cu2O8	Pb2Sr2Eu0.65Ca0.35Cu3O8.1	Pb	2	Sr	2	Eu	0.65	Ca	0.35	Cu	3											O	8	8.1	1	1997																												Pb3212																		K		71					71																																																																																															1	mixture-CAL(720C,50h in air). In this sample system oxygen content shows two values (8.1 or 9.8)					Annealing characteristics and calcium doping effects in the superconducting Pb2CuSr2[Eu1-xCax]Cu2O8+delta system	199712		Laboratory of Inorganic and Analytical Chemistry, Helsinki University of Technology, P.O. Box 6100, FIN-02015 Helsinki, Finland	Physica.C,292(1997)225-232	"J. Linden,J.Linden,L. Niinisto"",L.Niiniste,M. Karppinen,M. Lippmaa,M.Karppinen,M.Lippmaa,T. Karlemo,T.Karlemo"		
9708	P063212507	hole/Cu p=0.19	RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8			2001																												Ru1212																		K			35				35																																																																																																ANN(1060C, 7 days in O2)					Determination of Ru valence from x-ray absorption near-edge structure in RuSr2GdCu2O8-type superconductors			Department of Chemistry, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B, 63(2001)212507	H.-H.Hung,J.L.Tallon,L.-Y.Jang,R.S.Liu		
9709	P063212507	hole/Cu p=0.2	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2001																												Ru1212																		K			48				48																																																																																																ANN(1060C, 7 days in O2)					Determination of Ru valence from x-ray absorption near-edge structure in RuSr2GdCu2O8-type superconductors			Department of Chemistry, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B, 63(2001)212507	H.-H.Hung,J.L.Tallon,L.-Y.Jang,R.S.Liu		
9710	P063212507	hole/Cu p=0.23	RuSr2(Gd,Dy)Cu2O8	Ru1Sr2Gd0.6Dy0.4Cu2O8	Ru	1	Sr	2	Gd	0.6	Dy	0.4	Cu	2											O	8			2001																												Ru1212																		K			58				58																																																																																																ANN(1060C, 7 days in O2)					Determination of Ru valence from x-ray absorption near-edge structure in RuSr2GdCu2O8-type superconductors			Department of Chemistry, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B, 63(2001)212507	H.-H.Hung,J.L.Tallon,L.-Y.Jang,R.S.Liu		
9711	P063212507	hole/Cu p=0.14	Ru(Sr,Ba)2GdCu2O8	Ru1Sr1.6Ba0.4Gd1Cu2O8	Ru	1	Sr	1.6	Ba	0.4	Gd	1	Cu	2											O	8			2001																												Ru1212																		K	34		44				39																																																																																																ANN(1060C, 7 days in O2)					Determination of Ru valence from x-ray absorption near-edge structure in RuSr2GdCu2O8-type superconductors			Department of Chemistry, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B, 63(2001)212507	H.-H.Hung,J.L.Tallon,L.-Y.Jang,R.S.Liu		
9712	P063224512	impurity phase=SrRuO8	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8+z	Ru	1	Sr	2	Gd	1	Cu	2													O	8+z		1	2001																												Ru1212	4/mmm		A	3.8375		11.5623												K		45					45																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9713	P063224512	impurity phase=SrRuO8	(Ru,Cu)Sr2GdCu2O8	Ru0.9Sr2Gd1Cu2.1O8+z	Ru	0.9	Sr	2	Gd	1	Cu	2.1													O	8+z		1	2001																												Ru1212	4/mmm			3.8353		11.5362												K		65					65																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9714	P063224512	impurity phase=SrRuO8	(Ru,Cu)Sr2GdCu2O8	Ru0.8Sr2Gd1Cu2.2O8+z	Ru	0.8	Sr	2	Gd	1	Cu	2.2													O	8+z		1	2001																												Ru1212	4/mmm			3.8278		11.5263												K		70					70																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9715	P063224512	impurity phase=SrRuO8	(Ru,Cu)Sr2GdCu2O8	Ru0.7Sr2Gd1Cu2.3O8+z	Ru	0.7	Sr	2	Gd	1	Cu	2.3													O	8+z		1	2001																												Ru1212	4/mmm			3.827		11.512												K		72					72																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9716	P063224512	impurity phase=SrRuO8	(Ru,Cu)Sr2GdCu2O8	Ru0.6Sr2Gd1Cu2.4O8+z	Ru	0.6	Sr	2	Gd	1	Cu	2.4													O	8+z		1	2001																												Ru1212	4/mmm			3.8238		11.5066												K		72					72																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9717	P063224512	impurity phase=SrRuO8	(Ru,Cu)Sr2GdCu2O8	Ru0.25Sr2Gd1Cu2.75O8+z	Ru	0.25	Sr	2	Gd	1	Cu	2.75													O	8+z		1	2001																												Ru1212	4/mmm			3.8197		11.4581												K		62					62																																																																																														RuO2,SrCO3,Gd2O3,CuO	1	mixture-CAL(920C,in air)-pellet-ANN(970C, in O2 flow)-SIN(1060C, 10h, in 600bar O2)					Superconductivity in Ru1-xSr2GdCu2 + xO8-y compounds			Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B, 63(2001)224512	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut,S.Kolesnik		
9718	P063214504	gamma(in mj/mol-Sm.K2), debye-T estimated from specific heat(100-350C).	(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-z	Sm	1.85	Ce	0.15	Cu	1															O	4-z		3	2001					per mol	0.36	-6.4	4.7																				T'																		K				16.5			16.5																																																									103.2		219																																				1	flux method. As-grown crystals -ANN(880C,16h in an inert gas)-Q					Electronic and magnetic properties of the electron-doped superconductor Sm1.85Ce0.15CuO4-d							
9719	PHC3490289		RuSr2GdCu2Oz	Ru1Sr2Gd1Cu2Oz	Ru	1	Sr	2	Gd	1	Cu	2													O	z		1	2001																												Ru1212			A	3.838		11.559												K	22		45				33.5																																																																																															1	SIN(1050C, 72h in flowing O2)					Preparation, structure and superconductivity of Ru1222 and Ta-doped Ru1212			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 349(2001)289	S.Y.Li,X.H.Chen,Y.M.Xiong,Z.Sun		
9720	PHC3490289		(Ru,Ta)Sr2GdCu2Oz	Ru0.95Ta0.05Sr2Gd1Cu2Oz	Ru	0.95	Ta	0.05	Sr	2	Gd	1	Cu	2											O	z		1	2001																												Ru1212			A	3.839		11.565												K	10		35				22.5																																																																																															1	SIN(1050C, 72h in flowing O2)					Preparation, structure and superconductivity of Ru1222 and Ta-doped Ru1212			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 349(2001)289	S.Y.Li,X.H.Chen,Y.M.Xiong,Z.Sun		
9721	PHC3490289	not s/c	(Ru,Ta)Sr2GdCu2Oz	Ru0.85Ta0.15Sr2Gd1Cu2Oz	Ru	0.85	Ta	0.15	Sr	2	Gd	1	Cu	2											O	z		1	2001																												Ru1212			A	3.843		11.573												K					4																																																																																																	1	SIN(1050C, 24h in flowing O2)					Preparation, structure and superconductivity of Ru1222 and Ta-doped Ru1212			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 349(2001)289	S.Y.Li,X.H.Chen,Y.M.Xiong,Z.Sun		
9722	PHC3490289	higher oxygen content	RuSr2(Gd,Ce)Cu2Oz	Ru1Sr2Gd1.4Ce0.6Cu2Oz	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	z		1	2001																												Ru1222			A	3.844		28.615												K	35		45				40																																																																																															1	ANN(high O2 pressure)					Preparation, structure and superconductivity of Ru1222 and Ta-doped Ru1212			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 349(2001)289	S.Y.Li,X.H.Chen,Y.M.Xiong,Z.Sun		
9723	PHC3490317		Tl(Sr,Th)2CaCu2O7	Tl1Sr1.75Th0.25Ca1Cu2O7	Tl	1	Sr	1.75	Th	0.25	Ca	1	Cu	2											O	7		1	2001																												Tl1212	p4/mmm		A	3.801		12.099												K				51.6			51.6																																																																																																mixture-CAL(800-850C, 24h)-pellet-wrapped in Au foil-SIN(950C, 1 atm O2)					Preparation and magnetic relaxation of Th-doped TlSr2CaCu2O7 superconductors			Department of Physics, National Chung Cheng University, 160 San-Hsing, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 349(2001)317	J.F.Wang,L.R.Sung,W.H.Lee		
9724	PHC3490317		Tl(Sr,Th)2CaCu2O7	Tl1Sr1.65Th0.35Ca1Cu2O7	Tl	1	Sr	1.65	Th	0.35	Ca	1	Cu	2											O	7		1	2001																												Tl1212			A															K				55.3			55.3																																																																																																mixture-CAL(800-850C, 24h)-pellet-wrapped in Au foil-SIN(950C, 1 atm O2)					Preparation and magnetic relaxation of Th-doped TlSr2CaCu2O7 superconductors			Department of Physics, National Chung Cheng University, 160 San-Hsing, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 349(2001)317	J.F.Wang,L.R.Sung,W.H.Lee		
9725	PHC3490317		TlSr2(Ca,Th)Cu2O7	Tl1Sr2Ca0.75Th0.25Cu2O7	Tl	1	Sr	2	Ca	0.75	Th	0.25	Cu	2											O	7		1	2001																												Tl1212			A	3.8		12.094												K				52.5			52.5																																																																																																mixture-CAL(800-850C, 24h)-pellet-wrapped in Au foil-SIN(950C, 1 atm O2)					Preparation and magnetic relaxation of Th-doped TlSr2CaCu2O7 superconductors			Department of Physics, National Chung Cheng University, 160 San-Hsing, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 349(2001)317	J.F.Wang,L.R.Sung,W.H.Lee		
9726	PHC3490317		TlSr2(Ca,Th)Cu2O7	Tl1Sr2Ca0.65Th0.35Cu2O7	Tl	1	Sr	2	Ca	0.65	Th	0.35	Cu	2											O	7		1	2001																												Tl1212			A															K				55.3			55.3																																																																																																mixture-CAL(800-850C, 24h)-pellet-wrapped in Au foil-SIN(950C, 1 atm O2)					Preparation and magnetic relaxation of Th-doped TlSr2CaCu2O7 superconductors			Department of Physics, National Chung Cheng University, 160 San-Hsing, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 349(2001)317	J.F.Wang,L.R.Sung,W.H.Lee		
9727	PHC3110297		Tl(Sr,Gd)2CaCu2O7	Tl1Sr1.5Gd0.5Ca1Cu2O7	Tl	1	Sr	1.5	Gd	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.805		12.026												K	84			79			79																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9728	PHC3110297		Tl(Sr,Tb)2CaCu2O7	Tl1Sr1.5Tb0.5Ca1Cu2O7	Tl	1	Sr	1.5	Tb	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.796		12.014												K	83			80			80																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9729	PHC3110297		Tl(Sr,Dy)2CaCu2O7	Tl1Sr1.5Dy0.5Ca1Cu2O7	Tl	1	Sr	1.5	Dy	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.795		12.001												K	80			80			80																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9730	PHC3110297		Tl(Sr,Ho)2CaCu2O7	Tl1Sr1.5Ho0.5Ca1Cu2O7	Tl	1	Sr	1.5	Ho	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.794		11.996												K	82			80			80																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9731	PHC3110297		Tl(Sr,Er)2CaCu2O7	Tl1Sr1.5Er0.5Ca1Cu2O7	Tl	1	Sr	1.5	Er	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.787		11.997												K	73			78			78																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9732	PHC3110297		Tl(Sr,Tm)2CaCu2O7	Tl1Sr1.5Tm0.5Ca1Cu2O7	Tl	1	Sr	1.5	Tm	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.785		11.983												K	83			84			84																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9733	PHC3110297		Tl(Sr,Yb)2CaCu2O7	Tl1Sr1.5Yb0.5Ca1Cu2O7	Tl	1	Sr	1.5	Yb	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.783		11.981												K	81			84			84																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9734	PHC3110297		Tl(Sr,La)2CaCu2O7	Tl1Sr1.5La0.5Ca1Cu2O7	Tl	1	Sr	1.5	La	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.807		12.071												K	87			90			90																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9735	PHC3110297		Tl(Sr,Ce)2CaCu2O7	Tl1Sr1.5Ce0.5Ca1Cu2O7	Tl	1	Sr	1.5	Ce	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.808		12.027												K				5			5																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9736	PHC3110297		Tl(Sr,Pr)2CaCu2O7	Tl1Sr1.5Pr0.5Ca1Cu2O7	Tl	1	Sr	1.5	Pr	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.809		12.047												K	87			88			88																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9737	PHC3110297		Tl(Sr,Nd)2CaCu2O7	Tl1Sr1.5Nd0.5Ca1Cu2O7	Tl	1	Sr	1.5	Nd	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.809		12.046												K	87			88			88																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9738	PHC3110297		Tl(Sr,Sm)2CaCu2O7	Tl1Sr1.5Sm0.5Ca1Cu2O7	Tl	1	Sr	1.5	Sm	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.803		12.031												K	82			86			86																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9739	PHC3110297		Tl(Sr,Eu)2CaCu2O7	Tl1Sr1.5Eu0.5Ca1Cu2O7	Tl	1	Sr	1.5	Eu	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.801		12.024												K	86			88			88																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9740	PHC3110297		Tl(Sr,Lu)2CaCu2O7	Tl1Sr1.5Lu0.5Ca1Cu2O7	Tl	1	Sr	1.5	Lu	0.5	Ca	1	Cu	2											O	7		1	1999																												Tl1212			A	3.782		11.98												K	82			82			82																																																																																															1	mixture-CAL(800-850C, 24h)-pellet-sealed in quartz tube 1 atm O2 -SIN(950C, 2h)-Q to RT					Magnetic and superconducting properties of Tl(Sr1.5R0.5)CaCu2O7-delta compounds	199901		Department of Physics, National cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica.C,311(1998)297-302	L.R. Sung,L.R.Sung,M.R.Yeh,M.r. Yeh,W.H. Lee,W.H.Lee		
9741	PHC3110187	composition by EPMA. Bi,Pb,Y,Al entered from crucible and flux. Cu-site large deficiency. Semicon-like.	(Sr,Ca)10Cu17O29	Ca5.9Sr3.5Bi0.3Y0.1Pb0.1Al0.1Cu15.1O29	Ca	5.9	Sr	3.5	Bi	0.3	Y	0.1	Pb	0.1	Al	0.1	Cu	15.1							O	29		3	1999																												LAD			A	11.316	12.763	19.49												K	70		80				75																																									um	fitting		2.5	0.6																																																			self-flux method					Magnetic and superconducting properties of doped (Sr,Ca)10Cu17O29-type single crystals	199901		Institute Physics, Polish Academy of Sciences, AL. Lotniko'w 32/46, 02-668 Warsaw, Poland	Physica.C,311(1998)187-196	E. Mosiniewicz-Szablewska,E.Mosiniewicz-Szablewska,G.-J. Babonas,G.-J.Babonas,H. Szymczak,H.Szymczak,L. Leonyuk,L. Shvanskaya,L.Leonyuk,L.Shvanskaya,M. Baran,M.Baran,R. Szymczak,R.Szymczak,V. Maltsev,V.Maltsev		
9742	PHC3500105		(Ru,Ce)(Sr,Eu)2(Eu,Ce)2Cu2O10	Ru0.92Ce0.58Sr1.7Eu1.8Cu2O10	Ru	0.92	Ce	0.58	Sr	1.7	Eu	1.8	Cu	2											O	10			2001																												Ru1222			A	3.8424		28.559												K	12		40				26																																																																																															1	ANN(1040C, 48h, in O2)-ANN(1000C, 72h, in 1 Gpa O2)					Crystal structure of Ru(Sr,Gd)2(Gd,Sr)Cu2O8 and Ru(Sr,Eu)2(Eu,Ce)2Cu2O10 phases			Department of Solid State Physics and Chemistry, M.V. Lomonosov State Academy of Fine Chemical Technology, Moscow 117571, Russian Federation	Physica C, 350(2001)105	A.S.Andreeko,E.P.Khlybov,G.M.Kuz'micheva,I.E.Kostyleva,K.N.Gavrilov,V.V.Luparev		
9743	PHC3500024		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2001								132																				Ru1212			A	3.8375		11.563												K	35		46	35			35																																																																																															1	ANN(1010C, in Ar flow)-ANN(1030C-1060C in O2 flow)-slow cool to 500C-Q to RT-ANN(1065C, 600 atm O2-slow cool to RT					Effect of Ce doping on the superconducting and magnetic properties of RuSr2GdCu2O8			Department of Physics, Northern Illinois University, 218 Faraday Hall, DeKalb, IL 60115, USA	Physica C, 350(2001)24	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut		
9744	PHC3500024		RuSr2(Gd,Ce)Cu2O8	Ru1Sr2Gd0.98Ce0.02Cu2O8	Ru	1	Sr	2	Gd	0.98	Ce	0.02	Cu	2											O	8			2001								136																				Ru1212			A	3.8387		11.5621												K	13		36	13			13																																																																																															1	ANN(1010C, in Ar flow)-ANN(1030C-1060C in O2 flow)-slow cool to 500C-Q to RT-ANN(1065C, 600 atm O2-slow cool to RT					Effect of Ce doping on the superconducting and magnetic properties of RuSr2GdCu2O8			Department of Physics, Northern Illinois University, 218 Faraday Hall, DeKalb, IL 60115, USA	Physica C, 350(2001)24	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut		
9745	PHC3500024	not s/c	RuSr2(Gd,Ce)Cu2O8	Ru1Sr2Gd0.95Ce0.05Cu2O8	Ru	1	Sr	2	Gd	0.95	Ce	0.05	Cu	2											O	8			2001								145																				Ru1212			A	3.8406		11.5703												K					5																																																																																																	1	ANN(1010C, in Ar flow)-ANN(1030C-1060C in O2 flow)-slow cool to 500C-Q to RT-ANN(1065C, 600 atm O2-slow cool to RT					Effect of Ce doping on the superconducting and magnetic properties of RuSr2GdCu2O8			Department of Physics, Northern Illinois University, 218 Faraday Hall, DeKalb, IL 60115, USA	Physica C, 350(2001)24	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut		
9746	PHC3500024	SrRuO3 second phase detected	RuSr2(Gd,Ca)Cu2O8	Ru1Sr2Gd0.9Ca0.1Cu2O8	Ru	1	Sr	2	Gd	0.9	Ca	0.1	Cu	2											O	8			2001																												Ru1212			A															K			61				61																																																																																															1	ANN(1010C, in Ar flow)-ANN(1030C-1060C in O2 flow)-slow cool to 500C-Q to RT-ANN(1065C, 600 atm O2-slow cool to RT					Effect of Ce doping on the superconducting and magnetic properties of RuSr2GdCu2O8			Department of Physics, Northern Illinois University, 218 Faraday Hall, DeKalb, IL 60115, USA	Physica C, 350(2001)24	B.Dabrowski,J.Mais,M.Maxwell,P.W.Klamut		
9747	PHC3110246		EuBaSrCu3O7	Eu1Ba2Cu3O7	Eu	1	Ba	2	Cu	3															O	7			1999																												Y123			A	3.8021	3.8453	11.5821												K				84.4			84.4																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9748	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.9Pr0.1Ba2Cu3O7	Eu	0.9	Pr	0.1	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8305	3.8463	11.6157												K				68.3			68.3																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9749	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.8Pr0.2Ba2Cu3O7	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8551		11.6106												K				63			63																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9750	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.7Pr0.3Ba2Cu3O7	Eu	0.7	Pr	0.3	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8579		11.598												K				53.8			53.8																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9751	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.6Pr0.4Ba2Cu3O7	Eu	0.6	Pr	0.4	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8596		11.5989												K				37.8			37.8																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9752	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.5Pr0.5Ba2Cu3O7	Eu	0.5	Pr	0.5	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8586		11.5938												K				26.7			26.7																																																																																															1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9753	PHC3110246		(Eu,Pr)BaSrCu3O7	Eu0.4Pr0.6Ba2Cu3O7	Eu	0.4	Pr	0.6	Ba	2	Cu	3													O	7			1999																												Y123			A	3.8649		11.5959												K					4																																																																																																	1	mixture-CAL(1225K,24h)-pellet-SIN(1250C,78 h)-ANN(1100C,12h in flowing Ar)-ANN(725K,72h in O2)-cool to RT(1C/min)					Structural and superconducting properties of Ru1-xPrxBaSrCu3O7-delta	199901		Chemistry Division, Bhabha Atomic Research Center, Bombay 400 0085, India	Physica.C,311(1998)246-252	I.K. Gopalakrishnan,I.K.Gopalakrishnan,J.V. Yakhmi,J.V.Yakhmi,T.B. Waje,T.B.Waje		
9754	PHC3510329	carbonate-free samples. Optimally doped sample. Precise component=Hg0.970Ba2CuO4.059(CO3)0.0088 by NED.	HgBa2CuO4	Hg1Ba2Cu1O4.09	Hg	1	Ba	2	Cu	1															O	4+z	4.09	1	2001																												Hg1201			A	3.8817		9.5339												K	97			98			98	TC9754									80																																																																																				HgO,BaO,CuO	1	using carbon free materials					Superconducting and structural properties of nearly carbonate-free HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 351(2001)329	A.Yamamoto,F.Izumi,S.Tajima,Wei-Zhi Hu		
9755	PHC3510363	pseudogap temp. not shown numerically	HoNbO3	Ho1Nb1O3-z	Ho	1	Nb	1																	O	3-z			2001					per Ho	9																						ABO3																		K		15					15																																																																																																chemical reaction, then heat treatment.					On the superconducting and magnetic properties of HoNbO3-z and EuNbO3-z complex oxides			Institute of Solid State Physics, 142432, Chernogolovka, Moscow, Russia	Physica C, 351(2001)363	D.V.Shovkun,G.K.Strukova,I.E.Batov,S.A.Zver'kov,S.S.Khasanov,V.N.Zverev		
9756	PHC3510363	pseudogap temp. not shown numerically	EuNbO3	Eu1Nb1O3-z	Eu	1	Nb	1																	O	3-z			2001					per Eu	6.5	4.4																					ABO3																		K		6					6																																																																																																chemical reaction, then heat treatment.					On the superconducting and magnetic properties of HoNbO3-z and EuNbO3-z complex oxides			Institute of Solid State Physics, 142432, Chernogolovka, Moscow, Russia	Physica C, 351(2001)363	D.V.Shovkun,G.K.Strukova,I.E.Batov,S.A.Zver'kov,S.S.Khasanov,V.N.Zverev		
9757	PHC3510402	pseudogap temp. not shown numerically	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		90.38				3.2	90.38																																																																																																crystals were grown from a Bi2O3-rich melt in Al2O3 crucibles.					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9758	PHC3510402	pseudogap temp. not shown numerically	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.97Y0.03Cu2Oz	Bi	2	Sr	2	Ca	0.97	Y	0.03	Cu	2											O	z		3	2001																												Bi2212																		K		87.56				3.9	87.56																																																																																																crystals were grown from a Bi2O3-rich melt in Al2O3 crucibles.					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9759	PHC3510402	pseudogap temp. not shown numerically	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.95Y0.05Cu2Oz	Bi	2	Sr	2	Ca	0.95	Y	0.05	Cu	2											O	z		3	2001																												Bi2212																		K		82				6.2	82																																																																																																crystals were grown from a Bi2O3-rich melt in Al2O3 crucibles.					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9760	PHC3510402	pseudogap temp. not shown numerically	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.92Y0.08Cu2Oz	Bi	2	Sr	2	Ca	0.92	Y	0.08	Cu	2											O	z		3	2001																												Bi2212																		K		70.78				6.85	70.78																																																																																																crystals were grown from a Bi2O3-rich melt in Al2O3 crucibles.					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9761	PHC3510402	pseudogap temp. not shown numerically	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.89Y0.11Cu2Oz	Bi	2	Sr	2	Ca	0.89	Y	0.11	Cu	2											O	z		3	2001																												Bi2212																		K		56.1				5.5	56.1																																																																																																crystals were grown from a Bi2O3-rich melt in Al2O3 crucibles.					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9762	PHC3510402		Bi2(Sr,La)2CaCu2O8	Bi2Sr1.9La0.1Ca1Cu2Oz	Bi	2	Sr	1.9	La	0.1	Ca	1	Cu	2											O	z		1	2001																												Bi2212																		K		88.67				4.8	88.67																																																																		uV/K	2.11			TP9762																										not shown					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9763	PHC3510402	pseudogap temp.=160K	Bi2(Sr,La)2CaCu2O8	Bi2Sr1.8La0.2Ca1Cu2Oz	Bi	2	Sr	1.8	La	0.2	Ca	1	Cu	2											O	z		1	2001																												Bi2212																		K		85.3				7.3	85.3																																																																		uV/K	4.21			TP9763																										not shown					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9764	PHC3510402	pseudogap temp.=190K	Bi2(Sr,La)2CaCu2O8	Bi2Sr1.7La0.3Ca1Cu2Oz	Bi	2	Sr	1.7	La	0.3	Ca	1	Cu	2											O	z		1	2001																												Bi2212																		K		76.3				9.4	76.3																																																																		uV/K	6.84			TP9764																										not shown					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9765	PHC3510402	pseudogap temp.=220K	Bi2(Sr,La)2CaCu2O8	Bi2Sr1.6La0.4Ca1Cu2Oz	Bi	2	Sr	1.6	La	0.4	Ca	1	Cu	2											O	z		1	2001																												Bi2212																		K		60.73				10.7	60.73																																																																		uV/K	10.92			TP9765																										not shown					The detailed transport property of the underdoped Bi-2212 system in			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Physica C, 351(2001)402	C.Y.Wang,G.G.Qian,K.Q.Ruan,L.Z.Cao,Q.Cao,S.Y.Li,X.H.Chen		
9766	PHC3530060	optimally doped oxygen	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2001																												Tl2201																		K		88.9					88.9			K/Gpa	1.7																																																																																												See Physica C 199(1992)50. Not annealing					Influence of oxygen doping on the sign of the slope of Tc vs pressure curves in Tl2Ba2CuO6+x			Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka Moscow District, 142432 Russia	Physica C, 353(2001)60	N.N.Kolesnikov,O.M.Vyaselev,T.G.Togonidze		
9767	PHC3530060	overdoped but O-content not measured	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2001																												Tl2201																		K		40					40			K/Gpa	-4.3																																																																																												See Physica C 199(1992)50. Not annealing					Influence of oxygen doping on the sign of the slope of Tc vs pressure curves in Tl2Ba2CuO6+x			Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka Moscow District, 142432 Russia	Physica C, 353(2001)60	N.N.Kolesnikov,O.M.Vyaselev,T.G.Togonidze		
9768	PHC3530077		NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		1	2001																												Y123			A			11.7539												K		93.3				2.3	93.3																																																																						TP9768																									1	ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xPrxBa2Cu3O7- z			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 353(2001)77	M. Valldor,M.Andersson,O.Rapp,P.Lundqvist,S.R.Ghorbani		
9769	PHC3530077		(Nd,Pr)Ba2Cu3O7	Nd0.95Pr0.05Ba2Cu3O7-z	Nd	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A			11.7514												K		84.4				4	84.4																																																																						TP9769																									1	ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xPrxBa2Cu3O7- z			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 353(2001)77	M. Valldor,M.Andersson,O.Rapp,P.Lundqvist,S.R.Ghorbani		
9770	PHC3530077		(Nd,Pr)Ba2Cu3O7	Nd0.9Pr0.1Ba2Cu3O7-z	Nd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A			11.7437												K		73				5.3	73																																																																						TP9770																									1	ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xPrxBa2Cu3O7- z			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 353(2001)77	M. Valldor,M.Andersson,O.Rapp,P.Lundqvist,S.R.Ghorbani		
9771	PHC3530077		(Nd,Pr)Ba2Cu3O7	Nd0.85Pr0.15Ba2Cu3O7-z	Nd	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A			11.7435												K		59.7				4.4	59.7																																																																						TP9771																									1	ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xPrxBa2Cu3O7- z			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 353(2001)77	M. Valldor,M.Andersson,O.Rapp,P.Lundqvist,S.R.Ghorbani		
9772	PHC3390245		NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		1	2000																												Y123			A	3.8719	3.9215	11.7399												K		92.81					92.81																																																																		uV/K	8.93			TP9772																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9773	PHC3390245		(Nd,Ca)Ba2Cu3	Nd0.97Ca0.03Ba2Cu3O7-z	Nd	0.97	Ca	0.03	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.8674	3.917	11.7423												K		90.36					90.36																																																																		uV/K	4.96			TP9773																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9774	PHC3390245		(Nd,Ca)Ba2Cu3	Nd0.94Ca0.06Ba2Cu3O7-z	Nd	0.94	Ca	0.06	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.8652	3.9104	11.751												K		88					88																																																																		uV/K	4.86			TP9774																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9775	PHC3390245		(Nd,Ca)Ba2Cu3	Nd0.9Ca0.1Ba2Cu3O7-z	Nd	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.8607	3.9044	11.751												K		85.34					85.34																																																																		uV/K	4.22			TP9775																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9776	PHC3390245		(Nd,La)Ba2Cu3	Nd0.95La0.05Ba2Cu3O7-z	Nd	0.95	La	0.05	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.8686	3.9174	11.7441												K		91.78					91.78																																																																		uV/K	10.3			TP9776																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9777	PHC3390245		(Nd,La)Ba2Cu3	Nd0.9La0.1Ba2Cu3O7-z	Nd	0.9	La	0.1	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.868	3.9092	11.754												K		91.09					91.09																																																																		uV/K	10.98			TP9777																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9778	PHC3390245		(Nd,La)Ba2Cu3	Nd0.85La0.15Ba2Cu3O7-z	Nd	0.85	La	0.15	Ba	2	Cu	3													O	7-z		1	2000																												Y123			A	3.868	3.9086	11.7561												K		89.21					89.21																																																																		uV/K	11.02			TP9778																										ANN(460C, 3days in flowing O2)-cool to RT(12 C/h)					Thermoelectric power and resistivity of Nd1-xCaxBa2Cu3Oy and  Nd1-xLaxBa2Cu3Oy			Solid State Physics, Royal Institute of Technology, SE-100 44 Stockholm, Sweden	Physica C, 339(2000)245	M.Andersson,M.Valldor,O.Rapp,P.Lundqvist,S. R. Ghorbani		
9779	PHC3530200		TlSr2Ca2Cu3Oz	Tl1Sr2Ca2Cu3Oz	Tl	1	Sr	2	Ca	2	Cu	3													O	z		1	2001																												Tl1223			A	3.8121		15.2384												K				86			86																																		HIR9779																																	-0.4			TP9779																										high pressure synthesis(1100C, 1h, p=6GPa)-Q to RT					Doping states and irreversibility fields of high-pressure-synthesized  (Tl,Cu)Sr2Ca2Cu3Oy superconductors			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 353(2001)200	K.Tanabe,S.Adachi,S.Fujihara,T.Kimura,T.Shibata,T.Tatsuki		
9780	PHC3530200		(Tl,Cu)Sr2Ca2Cu3Oz	Tl0.8Sr2Ca2Cu3.2Oz	Tl	0.8	Sr	2	Ca	2	Cu	3.2													O	z		1	2001																												Tl1223			A	3.81		15.2679												K				92			92																																																																																																high pressure synthesis(1100C, 1h, p=6GPa)-Q to RT					Doping states and irreversibility fields of high-pressure-synthesized  (Tl,Cu)Sr2Ca2Cu3Oy superconductors			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 353(2001)200	K.Tanabe,S.Adachi,S.Fujihara,T.Kimura,T.Shibata,T.Tatsuki		
9781	PHC3530200		(Tl,Cu)Sr2Ca2Cu3Oz	Tl0.6Sr2Ca2Cu3.4Oz	Tl	0.6	Sr	2	Ca	2	Cu	3.4													O	z		1	2001																												Tl1223			A	3.8073		15.281												K				73			73																																		HIR9781																																	-3.52			TP9781																										high pressure synthesis(1100C, 1h, p=6GPa)-Q to RT					Doping states and irreversibility fields of high-pressure-synthesized  (Tl,Cu)Sr2Ca2Cu3Oy superconductors			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 353(2001)200	K.Tanabe,S.Adachi,S.Fujihara,T.Kimura,T.Shibata,T.Tatsuki		
9782	PHC3530200		(Tl,Cu)Sr2Ca2Cu3Oz	Tl0.4Sr2Ca2Cu3.6Oz	Tl	0.4	Sr	2	Ca	2	Cu	3.6													O	z		1	2001																												Tl1223			A	3.8073		15.3118												K				71			71																																																																																																high pressure synthesis(1100C, 1h, p=6GPa)-Q to RT					Doping states and irreversibility fields of high-pressure-synthesized  (Tl,Cu)Sr2Ca2Cu3Oy superconductors			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 353(2001)200	K.Tanabe,S.Adachi,S.Fujihara,T.Kimura,T.Shibata,T.Tatsuki		
9783	PHC3530200	ANN(350C, 20h, in Ar flow)	(Tl,Cu)Sr2Ca2Cu3Oz	Tl0.6Sr2Ca2Cu3.4Oz	Tl	0.6	Sr	2	Ca	2	Cu	3.4													O	z		1	2001																												Tl1223			A															K				94			94																																		HIR9783																																	-0.04			TP9783																										high pressure synthesis(1100C, 1h, p=6GPa)-Q to RT					Doping states and irreversibility fields of high-pressure-synthesized  (Tl,Cu)Sr2Ca2Cu3Oy superconductors			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 353(2001)200	K.Tanabe,S.Adachi,S.Fujihara,T.Kimura,T.Shibata,T.Tatsuki		
9784	PHC3530213	over-doped. two counterelectrode(Au) on ab-plane	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		87					87																																														meV	26	8.2																																																melt(1253K)-cool to 1078K(0.6K/h)					Superconducting energy gap of underdoped and overdoped Bi2Sr2CaCu2O8			Department of Applied Physics, Science University of Tokyo, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Physica C, 353(2001)213	D.Shimada,N.Tsuda,T.Oki		
9785	PHC3530213	two counterelectrode(Au) on ab-plane	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		92					92																																														meV	35	8.9																																																melt(1253K)-cool to 1078K(0.6K/h)					Superconducting energy gap of underdoped and overdoped Bi2Sr2CaCu2O8			Department of Applied Physics, Science University of Tokyo, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Physica C, 353(2001)213	D.Shimada,N.Tsuda,T.Oki		
9786	PHC3530213	two counterelectrode(Au) on ab-plane	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		87					87																																														meV	45	12																																																melt(1253K)-cool to 1078K(0.6K/h)					Superconducting energy gap of underdoped and overdoped Bi2Sr2CaCu2O8			Department of Applied Physics, Science University of Tokyo, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Physica C, 353(2001)213	D.Shimada,N.Tsuda,T.Oki		
9787	PHC3530213	two counterelectrode(Au) on ab-plane	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		84					84																																														meV	32	8.8																																																melt(1253K)-cool to 1078K(0.6K/h)					Superconducting energy gap of underdoped and overdoped Bi2Sr2CaCu2O8			Department of Applied Physics, Science University of Tokyo, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Physica C, 353(2001)213	D.Shimada,N.Tsuda,T.Oki		
9788	PHC3530213	two counterelectrode(Au) on ab-plane	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	2001																												Bi2212																		K		82					82																																														meV	33.5	9.4																																																melt(1253K)-cool to 1078K(0.6K/h)					Superconducting energy gap of underdoped and overdoped Bi2Sr2CaCu2O8			Department of Applied Physics, Science University of Tokyo, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Physica C, 353(2001)213	D.Shimada,N.Tsuda,T.Oki		
9789	SUP0130121		(La,Pb)2CuOz	La1.5Pb0.5Cu1Oz	La	1.5	Pb	0.5	Cu	1															O	z			2000																												T			A	5.348	5.3662	13.2193												K				15			15										8																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9790	SUP0130121		(La,Pb,Sr)2CuOz	La1.5Pb0.47Sr0.03Cu1Oz	La	1.5	Pb	0.47	Sr	0.03	Cu	1													O	z			2000																												T			A	3.7895		13.2064												K				22			22										5																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9791	SUP0130121		(La,Pb,Sr)2CuOz	La1.5Pb0.45Sr0.05Cu1Oz	La	1.5	Pb	0.45	Sr	0.05	Cu	1													O	z			2000																												T			A	3.7863		13.2086												K				27			27										19																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9792	SUP0130121		(La,Pb,Sr)2CuOz	La1.5Pb0.42Sr0.08Cu1Oz	La	1.5	Pb	0.42	Sr	0.08	Cu	1													O	z			2000																												T			A	3.784		13.2078												K				34			34										17																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9793	SUP0130121		(La,Pb,Sr)2CuOz	La1.5Pb0.4Sr0.1Cu1Oz	La	1.5	Pb	0.4	Sr	0.1	Cu	1													O	z			2000																												T			A	3.7818		13.2095												K				36			36										18																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9794	SUP0130121		(La,Pb,Sr)2CuOz	La1.5Pb0.35Sr0.15Cu1Oz	La	1.5	Pb	0.35	Sr	0.15	Cu	1													O	z			2000																												T			A	3.7802		13.212												K				38			38										38																																																																																						precursor(La1.5SrxCuOz)+PbO - sealed in quartz tube-heat(900C)-ANN(450C, 24h, 20 bar O2)-slow cool to RT					Synthesis, structure, and superconductivity of (La1.5Pb0.5-xSrx)CuOz			SRL, Shinonome,Koto-ku, Tokyo,Japan	J.Supercond., 13(2000)121	E.Kandyel,S.Adachi,S.Tajima		
9795	SUP0130137		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	2000																												Bi2212																		K		85.05					85.05																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9796	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.9Sn0.1O8+z	Bi	2	Sr	2	Ca	1	Cu	1.9	Sn	0.1											O	8+z		1	2000																												Bi2212																		K		84.82					84.82																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9797	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.8Sn0.2O8+z	Bi	2	Sr	2	Ca	1	Cu	1.8	Sn	0.2											O	8+z		1	2000																												Bi2212																		K		84.5					84.5																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9798	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.7Sn0.3O8+z	Bi	2	Sr	2	Ca	1	Cu	1.7	Sn	0.3											O	8+z		1	2000																												Bi2212																		K		83.76					83.76																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9799	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.6Sn0.4O8+z	Bi	2	Sr	2	Ca	1	Cu	1.6	Sn	0.4											O	8+z		1	2000																												Bi2212																		K		82.34					82.34																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9800	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.5Sn0.5O8+z	Bi	2	Sr	2	Ca	1	Cu	1.5	Sn	0.5											O	8+z		1	2000																												Bi2212																		K		80.31					80.31																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9801	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1.3Sn0.7O8+z	Bi	2	Sr	2	Ca	1	Cu	1.3	Sn	0.7											O	8+z		1	2000																												Bi2212																		K					77																																																																																																		SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9802	SUP0130137	XPS shows Sn enters with (2+) state	Bi2Sr2Ca(Cu,Sn)2O8	Bi2Sr2Ca1Cu1Sn1O8+z	Bi	2	Sr	2	Ca	1	Cu	1	Sn	1											O	8+z		1	2000																												Bi2212																		K					77																																																																																																		SIN(910-940C, 30-70h)					Substitution effect of Sn for Cu in the Bi2Sr2CaCu2-xSnxO8+z system			Technical Physics Department, Peking University, Beijing,China	J.Supercond., 13(2000)137	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9803	SUP0130569	conventional solid state reacted sample is not s/c.	(Cd,Bi,Pb)Sr2YCu2O7	Cd0.67Bi0.23Pb0.1Sr2Y1Cu2O7-z	Cd	0.67	Bi	0.23	Pb	0.1	Sr	2	Y	1	Cu	2									O	7-z			2000																												1212	P4/mmm		A	3.797		11.968												K	20		35				27.5																																																																																																ANN(1175K, under 5 Mpa O2)					Effect of high-pressure oxygen annealing in inducing superconductivity in calcium-free 1212-type cuprate (Cd0.67Bi0.23Pb0.10)YSr2Cu2O7-z			Novel Materials and Structural Chemistry Division, Bhabha Atomic Research Centre, Mumbai, India	J.Supercond., 13(2000)569	I.K.Gopalakrishnan,J.V.Yakhmi		
9804	SUP0130603		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	2000																												Bi2212																		K		84.7					84.7																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Pr for Ca in Bi2Sr2CaCu2O8+z system			Nanjing University, Nanjing, China	J.Supercond., 13(2000)603	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9805	SUP0130603		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8+z		1	2000																												Bi2212																		K		69.4					69.4																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Pr for Ca in Bi2Sr2CaCu2O8+z system			Nanjing University, Nanjing, China	J.Supercond., 13(2000)603	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9806	SUP0130603		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8+z		1	2000																												Bi2212																		K		43.5					43.5																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Pr for Ca in Bi2Sr2CaCu2O8+z system			Nanjing University, Nanjing, China	J.Supercond., 13(2000)603	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9807	SUP0130603		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2O8+z	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	8+z		1	2000																												Bi2212																		K		4.8					4.8																																																																																																SIN(910-940C, 30-70h)					Substitution effect of Pr for Ca in Bi2Sr2CaCu2O8+z system			Nanjing University, Nanjing, China	J.Supercond., 13(2000)603	C.G.Zhu,H.B.Pan,P.S.Xu,Q.Li,X.Y.Zhang		
9808	SUP0130653		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		1	2000																												Y123			A	3.8856	3.8211	11.6869												K	91.9						91.9																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9809	SUP0130653		Y(Ba,Na)2Cu3O7	Y1Ba1.95Na0.05Cu3Oz	Y	1	Ba	1.95	Na	0.05	Cu	3													O	z		1	2000																												Y123			A	3.8824	3.8182	11.6774												K	91.4						91.4																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9810	SUP0130653		Y(Ba,Na)2Cu3O7	Y1Ba1.9Na0.1Cu3Oz	Y	1	Ba	1.9	Na	0.1	Cu	3													O	z		1	2000																												Y123			A	3.8763	3.8155	11.6609												K	88.4						88.4																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9811	SUP0130653		Y(Ba,Na)2Cu3O7	Y1Ba1.85Na0.15Cu3Oz	Y	1	Ba	1.85	Na	0.15	Cu	3													O	z		1	2000																												Y123			A	3.8719	3.8101	11.6538												K	90.3						90.3																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9812	SUP0130653		Y(Ba,Na)2Cu3O7	Y1Ba1.8Na0.2Cu3Oz	Y	1	Ba	1.8	Na	0.2	Cu	3													O	z		1	2000																												Y123			A	3.8684	3.8073	11.6483												K	90.8						90.8																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9813	SUP0130653		Y(Ba,K)2Cu3O7	Y1Ba1.95K0.05Cu3Oz	Y	1	Ba	1.95	K	0.05	Cu	3													O	z		1	2000																												Y123			A	3.8802	3.8159	11.657												K	91.4						91.4																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9814	SUP0130653		Y(Ba,K)2Cu3O7	Y1Ba1.9K0.1Cu3Oz	Y	1	Ba	1.9	K	0.1	Cu	3													O	z		1	2000																												Y123			A	3.8744	3.8127	11.6534												K	77.3						77.3																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9815	SUP0130653		Y(Ba,K)2Cu3O7	Y1Ba1.85K0.15Cu3Oz	Y	1	Ba	1.85	K	0.15	Cu	3													O	z		1	2000																												Y123			A	3.8753	3.8129	11.6558												K	64.4						64.4																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9816	SUP0130653		Y(Ba,K)2Cu3O7	Y1Ba1.8K0.2Cu3Oz	Y	1	Ba	1.8	K	0.2	Cu	3													O	z		1	2000																												Y123			A	3.8761	3.8133	11.6598												K	71						71																																																																																																SIN(950C)-ANN(450C,12h, in flowing O2)					Comparison of superconductivity and structure for YBa2Cu3Oy with potassium and sodium doping			Nanjing University, Nanjing, China	J.Supercond., 13(2000)653	F.Z.Wang,Q.Li,S.Nie,S.S.Jiang,X.S.Wu		
9817	SUP0130037	not s/c	La2Ba2Cu4Oz	La2Ba2Cu4O9.348	La	2	Ba	2	Cu	4															O	z	9.348	1	2000																											2																								5																																																																																																		SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9818	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.9Er0.1Ba2Ca0.2Cu4.2O9.85	La	1.9	Er	0.1	Ba	2	Ca	0.2	Cu	4.2											O	z	9.85	1	2000																											2																				18						18																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9819	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.8Er0.2Ba2Ca0.4Cu4.4O10.371	La	1.8	Er	0.2	Ba	2	Ca	0.4	Cu	4.4											O	z	10.371	1	2000																											2																				40						40																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9820	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.75Er0.25Ba2Ca0.5Cu4.5O10.662	La	1.75	Er	0.25	Ba	2	Ca	0.5	Cu	4.5											O	z	10.662	1	2000																											2																				66						66																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9821	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.7Er0.3Ba2Ca0.6Cu4.6O10.92	La	1.7	Er	0.3	Ba	2	Ca	0.6	Cu	4.6											O	z	10.92	1	2000																											2																				70						70																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9822	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.65Er0.35Ba2Ca0.7Cu4.7O11.166	La	1.65	Er	0.35	Ba	2	Ca	0.7	Cu	4.7											O	z	11.166	1	2000																											2																				71						71																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9823	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.6Er0.4Ba2Ca0.8Cu4.8O11.424	La	1.6	Er	0.4	Ba	2	Ca	0.8	Cu	4.8											O	z	11.424	1	2000																											2																				76						76																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9824	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.55Er0.45Ba2Ca0.9Cu4.9O11.664	La	1.55	Er	0.45	Ba	2	Ca	0.9	Cu	4.9											O	z	11.664	1	2000																											2																				76						76																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9825	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1.5Er0.5Ba2Ca1Cu5O11.907	La	1.5	Er	0.5	Ba	2	Ca	1	Cu	5											O	z	11.907	1	2000																											2																				78						78																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9826	SUP0130037		(La,Er)2Ba2CaxCu4+xOz	La1Er1Ba2Ca2Cu6O14.122	La	1	Er	1	Ba	2	Ca	2	Cu	6											O	z	14.122	1	2000																											2																				79						79																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9827	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1.9Gd0.1Ba2Ca0.2Cu4.2O9.839	La	1.9	Gd	0.1	Ba	2	Ca	0.2	Cu	4.2											O	z	9.839	1	2000																											2																				15						15																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9828	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1.8Gd0.2Ba2Ca0.4Cu4.4O10.344	La	1.8	Gd	0.2	Ba	2	Ca	0.4	Cu	4.4											O	z	10.344	1	2000																											2																				39						39																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9829	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1.7Gd0.3Ba2Ca0.6Cu4.6O10.9	La	1.7	Gd	0.3	Ba	2	Ca	0.6	Cu	4.6											O	z	10.9	1	2000																											2																				64						64																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9830	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1.6Gd0.4Ba2Ca0.8Cu4.8O11.401	La	1.6	Gd	0.4	Ba	2	Ca	0.8	Cu	4.8											O	z	11.401	1	2000																											2																				76						76																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9831	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1.5Gd0.5Ba2Ca1Cu5O11.892	La	1.5	Gd	0.5	Ba	2	Ca	1	Cu	5											O	z	11.892	1	2000																											2																				79						79																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9832	SUP0130037		(La,Gd)2Ba2CaxCu4+xOz	La1Gd1Ba2Ca2Cu6O14.1	La	1	Gd	1	Ba	2	Ca	2	Cu	6											O	z	14.1	1	2000																											2																				79						79																																																																																																SIN(950C, 12h, in O2)-ANN(500C, 24h, in O2 flow)					Role of calcium in the evolution of superconductivity in a (La2-xRx)Ba2(CayCu4+y)Oz (R=Y, Er, Gd) system			Department of Physics,Saurashtra University, Rajkot, India	J.Supercond., 13(2000)37	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.Prasad		
9833	P063064505	high quarity sample. Thermal conductivity measured in the field for various orientations	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2001																												Sr2RuO4																		K				1.44			1.44																																																																	THC9833																																				Thermal conductivity of superconducting Sr2RuO4 in oriented magnetic fields			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 63(2001)064505	M.A.Tanatar,S.Nagai,T.Ishiguro,Y.Maeno,Z.Q.Mao		
9834	P064094515	Raman shift measured	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.6Ce0.4Cu2O10+z	Ru	1	Sr	2	Gd	1.6	Ce	0.4	Cu	2											O	10+z		1	2001																												Ru1222			A	3.84		28.58												K	18.5		43.3				30.9																																																																		uV/K	35.8			TP9834																									1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9835	P064094515	Raman shift measured	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.5Ce0.5Cu2O10+z	Ru	1	Sr	2	Gd	1.5	Ce	0.5	Cu	2											O	10+z		1	2001																												Ru1222			A	3.84		28.58												K	29.1		44.8				36.95																																																																		uV/K	32.6																												1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9836	P064094515	Raman shift measured	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.4Ce0.6Cu2O10+z	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	10+z		1	2001																												Ru1222			A	3.84		28.58												K	34.7		49.9				42.3																																																																		uV/K	24.2			TP9836																									1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9837	P064094515	Raman shift measured	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.3Ce0.7Cu2O10+z	Ru	1	Sr	2	Gd	1.3	Ce	0.7	Cu	2											O	10+z		1	2001																												Ru1222			A	3.84		28.58												K	32.1		47.9				40																																																																		uV/K	23.2																												1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9838	P064094515	Raman shift measured	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.2Ce0.8Cu2O10+z	Ru	1	Sr	2	Gd	1.2	Ce	0.8	Cu	2											O	10+z		1	2001																												Ru1222			A	3.84		28.58												K	21		45.3				33.15																																																																		uV/K	29.5			TP9838																									1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9839	P064094515	Raman shift measured	RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.4Ce0.6Cu2O10+z	Ru	1	Sr	2	Eu	1.4	Ce	0.6	Cu	2											O	10+z		1	2001																												Ru1222																		K	26		49				37.5																																																																		uV/K	30			TP9839																									1	final heat treatment (1060C, 7days in flowing O2) - cool to RT (4C/min)					Raman transport and magnetization study of the RuSr2R2-xCexCu2O10+z  (R = Gd, Eu) high-temperature superconducting cuprates			Industrial Research Limited, P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 64(2001)094515	G.V.M.Williams,M.Ryan		
9840	P064064508	coexistence of s/c and magnetic order. Ceramic sample	RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8		1	2001								132																				Ru1212																		K	12			32			32																																																																		uV/K	73																											RuO2,Eu2O3,CuO,SrCO3	1	SIN(1010C,10h, in flowing O2)-SIN(1050C,10h, in flowing O2)-SIN(1055C,10h, in flowing O2)					Transport and microwave study of superconducting and magnetic RuSr2EuCu2O8			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 64(2001)064508	A.Dulcic,D.Paar,G.V.M.Williams,M.Pozek,S.Kramer		
9841	P064064502	re-entrant s/c. R start to increase at 5 K. K-content = 0.45-0.6 by EDX.	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3		1	2001																												BKBO			A	5.94		8.43												K	10.1		12.5				11.3																																																																																																(Sr2Bi2O5+KO2+Bi2O3) - sealed in Au capsule - HIP(p=2 Gpa, 700C, 60 min)					Observation of anomalous reentrant superconductivity in Sr1-xKxBiO3			Department of Physics and Condensed Matter Research Institute, Seoul National University, Seoul 151-742, Korea	Phys.Rev.B, 64(2001)064502	A.N.Baranov,D.C.Kim,E.V.Antipov,G.T.Kim,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
9842	P064064502	re-entrant s/c. R start to increase at 8 K. K-content = 0.45-0.6 by EDX.	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3		1	2001																												BKBO																		K	10.5		12.6				11.55																																																																																																(Sr2Bi2O5+KO2+Bi2O3) - sealed in Au capsule - HIP(p=2 Gpa, 700C, 60 min)					Observation of anomalous reentrant superconductivity in Sr1-xKxBiO3			Department of Physics and Condensed Matter Research Institute, Seoul National University, Seoul 151-742, Korea	Phys.Rev.B, 64(2001)064502	A.N.Baranov,D.C.Kim,E.V.Antipov,G.T.Kim,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
9843	PHC3540363		Bi2Sr2CaCu2O8	Bi2.1Sr2.1Ca0.8Cu2Oz	Bi	2.1	Sr	2.1	Ca	0.8	Cu	2													O	z		1	2001																												Bi2212																		K				88			88																																																																																														Bi2O3,SrCO3,CaCO3,CuO,NiS	1	mixture-CAL(800C,40h)-SIN(850C,100h in air)- cool to 500C(1 C/min) - RT					Structural and magnetic properties of NiS doped Bi-2212 superconductors			Departamento de Fisica, Universidade Federal de Pernambuco, Av. Prof. Luis de Barros Freire s/n, 50670-901 Recife, PE, Brazil	Physica C, 354(2001)363	C.L.S.Lima,E.Montarroyos,J.Albino Aguiar,J.M.Ferreira,R.F.Jardim,Y.P.Yadava		
9844	PHC3540363	partial substitution of NiS for CuO	Bi1Sr2Ca(CuO,NiS)2O8	Bi2.1Sr2.1Ca0.8Cu1.98Ni0.02S0.02Oz	Bi	2.1	Sr	2.1	Ca	0.8	Cu	1.98	Ni	0.02	S	0.02									O	z		1	2001																												Bi2212																		K				80			80																																																																																														Bi2O3,SrCO3,CaCO3,CuO,NiS	1	mixture-CAL(800C,40h)-SIN(850C,100h in air)- cool to 500C(1 C/min) - RT					Structural and magnetic properties of NiS doped Bi-2212 superconductors			Departamento de Fisica, Universidade Federal de Pernambuco, Av. Prof. Luis de Barros Freire s/n, 50670-901 Recife, PE, Brazil	Physica C, 354(2001)363	C.L.S.Lima,E.Montarroyos,J.Albino Aguiar,J.M.Ferreira,R.F.Jardim,Y.P.Yadava		
9845	PHC3540363	partial substitution of NiS for CuO	Bi1Sr2Ca(CuO,NiS)2O8	Bi2.1Sr2.1Ca0.8Cu1.9Ni0.1S0.1Oz	Bi	2.1	Sr	2.1	Ca	0.8	Cu	1.9	Ni	0.1	S	0.1									O	z		1	2001																												Bi2212																		K				78			78																																																																																														Bi2O3,SrCO3,CaCO3,CuO,NiS	1	mixture-CAL(800C,40h)-SIN(850C,100h in air)- cool to 500C(1 C/min) - RT					Structural and magnetic properties of NiS doped Bi-2212 superconductors			Departamento de Fisica, Universidade Federal de Pernambuco, Av. Prof. Luis de Barros Freire s/n, 50670-901 Recife, PE, Brazil	Physica C, 354(2001)363	C.L.S.Lima,E.Montarroyos,J.Albino Aguiar,J.M.Ferreira,R.F.Jardim,Y.P.Yadava		
9846	PHC3540363	partial substitution of NiS for CuO	Bi1Sr2Ca(CuO,NiS)2O8	Bi2.1Sr2.1Ca0.8Cu1.8Ni0.2S0.2Oz	Bi	2.1	Sr	2.1	Ca	0.8	Cu	1.8	Ni	0.2	S	0.2									O	z		1	2001																												Bi2212																		K				78			78																																																																																														Bi2O3,SrCO3,CaCO3,CuO,NiS	1	mixture-CAL(800C,40h)-SIN(850C,100h in air)- cool to 500C(1 C/min) - RT					Structural and magnetic properties of NiS doped Bi-2212 superconductors			Departamento de Fisica, Universidade Federal de Pernambuco, Av. Prof. Luis de Barros Freire s/n, 50670-901 Recife, PE, Brazil	Physica C, 354(2001)363	C.L.S.Lima,E.Montarroyos,J.Albino Aguiar,J.M.Ferreira,R.F.Jardim,Y.P.Yadava		
9847	P064092510	compositions are nominal values. Gapene calculated from gap(77.3K)=32 meV using BCS dependency.	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.9Pb0.5Sr2Ca2Cu3O10+z	Bi	1.9	Pb	0.5	Sr	2	Ca	2	Cu	3											O	10+z			2001																												Bi2223																		K				110			110																																														meV	38.5	8.1	1																																														1	conventional solid state reaction					Tunneling spectroscopy of the normal-state gap in (Bi, Pb)2Sr2Ca2Cu3O10+z			Faculty of Integrated Arts and Sciences, and Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Phys.Rev.B, 64(2001)092510	H.Fujii,S.Hashimoto,T.Ekino,T.Takasaki		
9848	P064094518		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	2001																												Y124	Ammm		A	3.8402	3.8702	27.2283												K				77.7			77.7																																																																																																crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9849	P064094518	Tc not shown	Y(Ba,Sr)2Cu4O8	Y1Ba1.78Sr0.22Cu4O8	Y	1	Ba	1.78	Sr	0.22	Cu	4													O	8		3	2001																												Y124	Ammm		A	3.8299	3.8676	27.1707																																																																																																																			crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9850	P064094518	Tc not shown	Y(Ba,Sr)2Cu4O8	Y1Ba1.68Sr0.32Cu4O8	Y	1	Ba	1.68	Sr	0.32	Cu	4													O	8		3	2001																												Y124	Ammm		A	3.8232	3.8644	27.1387																																																																																																																			crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9851	P064094518	Tc not shown	Y(Ba,Sr)2Cu4O8	Y1Ba1.38Sr0.62Cu4O8	Y	1	Ba	1.38	Sr	0.62	Cu	4													O	8		3	2001																												Y124	Ammm		A	3.8086	3.8601	27.0588																																																																																																																			crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9852	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.76Sr0.24Cu4O8	Y	1	Ba	1.76	Sr	0.24	Cu	4													O	8		3	2001																												Y124																		K				76			76																																																																																																crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9853	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.46Sr0.54Cu4O8	Y	1	Ba	1.46	Sr	0.54	Cu	4													O	8		3	2001																												Y124																		K				79.5			79.5																																																																																																crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9854	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.4Sr0.6Cu4O8	Y	1	Ba	1.4	Sr	0.6	Cu	4													O	8		3	2001																												Y124																		K				80.5			80.5																																																																																																crystals were grown by flux method. Synthesis in high O2 pressure P(O2) = 900 bar					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9855	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K				80.5			80.5																																																																																																high pressure synthesis (P(O2)=450 bar, 100C, 40h)					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9856	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.8Sr0.2Cu4O8	Y	1	Ba	1.8	Sr	0.2	Cu	4													O	8		1	2001																												Y124																		K				79.8			79.8																																																																																																high pressure synthesis (P(O2)=450 bar, 100C, 40h)					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9857	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.6Sr0.4Cu4O8	Y	1	Ba	1.6	Sr	0.4	Cu	4													O	8		1	2001																												Y124																		K				80.5			80.5																																																																																																high pressure synthesis (P(O2)=450 bar, 100C, 40h)					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9858	P064094518	Tc defined as intersect of M=0 and line with thehighest dM/dT	Y(Ba,Sr)2Cu4O8	Y1Ba1.4Sr0.6Cu4O8	Y	1	Ba	1.4	Sr	0.6	Cu	4													O	8		1	2001																												Y124																		K				81.2			81.2																																																																																																high pressure synthesis (P(O2)=450 bar, 100C, 40h)					Influence of Sr substitution on the structure, charge distribution, and critical temperature of Y(Ba1-xSrx)2Cu4O8 single crystals			Solid State Physics Laboratory, ETH 8093 Zurich, Switzerland	Phys.Rev.B, 64(2001)094518	A.Mironov,J.Karpinski,J.Roos,M.Angst,M.Mali,S.M.Kazakov		
9859	P064134502	In figure Hp= the first peak, Hsp = the second peak in M-H curve, Hirr = irreversible field.	(Sm,La,Sr)2CuO4	Sm1La0.8Sr0.2Cu1O4	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4		3	2001																												T*																		K				24			24																																		HIR9859																																																														TSFZ method. As-grown - ANN(600C,7d in 200 bar O2)-ANN(300C, 3d)-cool to RT(25C/h)					Peak effects and the solid vortex phase of a T*-phase SmLa0.8Sr0.2CuO4-z single crystal			Van der Waals-Zeeman Instituut, Universiteit van Amsterdam, Valckenierstraat 65, 1018 XE, Amsterdam, The Netherlands	Phys.Rev.B, 64(2001)134502	A.A.Menovsky,A.A.Nugroho,I.M.Sutjahja,J.J.M.Franse,M.O.Tjia		
9860	MAT0107309	 Hc2(0) using WHH theory. Hall effect, specific heat were measured. Delta-C/gamma*Tc = 1.29	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2001																												pyrochlore			A	10.2244														K	1.15		1.47				1.31																				T	resistivity, using WHH theory	0.5							T/K	resistivity	0.62			HIR9860		A	from Hc2(0)	240															SP9860	mj/mol.K	37.9	mj/mol.K2	29.6	from SP	397	from SP																																				vapor transport method					Superconductivity in the correlated pyrochlore Cd2Re2O7			Solid State Devision, Oak Ridge National Lab, TN,USA	ccond-mat/0107309 (Phys.Rev.B,64(2001)180503)	C.S.Alexander,D.Mandrus,F.Drymiotis,J.He,R.Jin,S.MaCall		
9861	MAT0109050	The 1st order structural phase transition at 200 K. Thermal expansion coeff.  Alpha = 4.9 E-6 /K at RT	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2001																												pyrochlore			A	10.226														K		1					1																																																																																																heat in silica tube (900C, 72h)					Structural phase transition in the superconducting pyrochlore oxide Cd2Re2O7				ccond-mat/0109050	F.Sakai,J.Yamaura,M.Hanawa,Y.Muraoka,Z.Hiroi		
9862	MAT0106521	gamma from J.Chem.Phys., 71(1979)5287	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		1	2001																												pyrochlore			A	10.221														K		1.1					1.1																				T	resistivity, using WHH theory	0.8												HIR9862																						mj/mol.K2	26.6																																												Superconductivity in a pyrochlore oxide Cd2Re2O7				ccond-mat/0106521	H.Kato,H.Ohno,H.Sakai,K.Yoshimura,R.E.Walstedt,S.Kambe,T.Matsuda,Y.Haga,Y.Onuki		
9863	JJP0400262	magnetic relaxation studied.	(Tl,Pb)(sr,Nd)2CaCu2O7	Tl0.5Pb0.5Sr1.84Nd0.16Ca1Cu2O7	Tl	0.5	Pb	0.5	Sr	1.84	Nd	0.16	Ca	1	Cu	2									O	7		1	2001																												Tl1212			A	3.815		12.112												K		102		105		3	102																																																																																														Tl2O3,PbO2,Nd2O3,SrCO3,CaCO3,CuO	1	precursor(Sr1.84Nd0.16CaCu2Oz)+(Tl2O3+PbO2)-mix-wrap in Au foil-sealed qualtz tube-heat(950C,2h)-Q to RT					Magnetic-Relaxation Behavior of (Tl0.5Pb0.5)(Sr1.84Nd0.16)CaCu2O7 Superconducting Material			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, R.O.C.	Jpn. J. Appl. Phys. , 40 (2001) L262-L265	Li-Ru Sung,Shin-Hau Huang,Wun-Hsin Lee,Yeong-Der Yao		
9864	EPJ0200189	high quality twinned crystal	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2001																												Y123																		K		90.5				0.6	90.5																																																																	THC9864																										RH9864					flux method					Thermal conductivity and thermal Hall effect in Bi- and Y-based high-Tc superconductors				Eur. Phys. J. B, 20 (2001) 189-208	A.Freimuth,A.P.Kampf,B.Buchner,B.Zeini,G.Muller-Vogt,L.Winkler,M.Galffy,R.Gross		
9865	EPJ0200189	not optimal oxygen content	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2001																												Bi2212																		K		80					80																																																																	THC9865																										RH9865					flux method					Thermal conductivity and thermal Hall effect in Bi- and Y-based high-Tc superconductors				Eur. Phys. J. B, 20 (2001) 189-208	A.Freimuth,A.P.Kampf,B.Buchner,B.Zeini,G.Muller-Vogt,L.Winkler,M.Galffy,R.Gross		
9866	SST0140504	composition (Tl:Ba:Ca:Cu=1.11:2.02:1.84:3.03) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3Oz	Tl	1	Ba	2	Ca	2	Cu	3													O	z		1	2001																												Tl1223			A	3.85		15.881												K	130						130																																																																																																high pressure synthesis (850C, 3.5 Gpa) - ANN(700C,1h in N2)					Study on enhancement of Tc (>= 130 K) in TlBa2Ca2Cu3Oy superconductors				Supercond. Sci. Technol., 14 ( 2001 )504-510	A.Iyo,H.Ihara,K.Tokiwa,M.Tokumoto,T.Watanabe,Y.Ishiura,Y.Tanaka		
9867	JEL0600440	multiphase(Nb+fcc+Ba4Nb2O9). Average compositions=Ba0.6Nb0.8O1.1 by AES for x=0.33 sample in BaxNbO2-z.		Ba0.5Nb1O2-z	Ba	0.5	Nb	1																	O	2-z		2	1994																																														K	17.5		22				19.75																																																																																														Nb,BaO2		mixture-pellet-heat(500C, air, in quartz tube)					Superconductivity above 20K in barium-niobium-oxide compounds			Institute of Solid State Physics, Russian Academy of Science, Moscow, Russia	JETP Lett., 60(1994)440	G.K.Strukova,S.S.Khassanov,V.A.Gasparov		
9868	JEL0600440			Ba0.25Nb1O2-z	Ba	0.25	Nb	1																	O	2-z		2	1994																																														K	17.5		18.6				18.05																																																																																														Nb,BaO2		mixture-pellet-heat(500C, air, in quartz tube)					Superconductivity above 20K in barium-niobium-oxide compounds			Institute of Solid State Physics, Russian Academy of Science, Moscow, Russia	JETP Lett., 60(1994)440	G.K.Strukova,S.S.Khassanov,V.A.Gasparov		
9873	JAP0897657		(La,Nd)2CaBa2Cu5Oz	La1.7Nd0.3Ca0.6Ba2Cu4.6O11.892	La	1.7	Nd	0.3	Ca	0.6	Ba	2	Cu	4.6											O	10+z	11.892	1	2001																												2125	P4/mmm		A	3.8735		11.6686												K	78						78																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9874	JAP0897657		(La,Nd)2CaBa2Cu5Oz	La1.6Nd0.4Ca0.8Ba2Cu4.8O10+z	La	1.6	Nd	0.4	Ca	0.8	Ba	2	Cu	4.8											O	10+z		1	2001																												2125	P4/mmm																	K	70						70																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9875	JAP0897657		(La,Nd)2CaBa2Cu5Oz	La1.5Nd0.5Ca1Ba2Cu5O11.872	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	5											O	10+z	11.872	1	2001																												2125	P4/mmm		A	3.8742		11.6569												K	78						78																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9876	JAP0897657	T1 estimated by extraporating R(T) to low temperature	(La,Gd)2CaBa2Cu5Oz	La1.9Gd0.1Ca0.2Ba2Cu4.2O10+z	La	1.9	Gd	0.1	Ca	0.2	Ba	2	Cu	4.2											O	10+z		1	2001																												2125																		K	22						22																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9877	JAP0897657		(La,Gd)2CaBa2Cu5Oz	La1.7Gd0.3Ca0.6Ba2Cu4.6O10+z	La	1.7	Gd	0.3	Ca	0.6	Ba	2	Cu	4.6											O	10+z		1	2001																												2125																		K	64						64																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9878	JAP0897657		(La,Gd)2CaBa2Cu5Oz	La1.6Gd0.4Ca0.8Ba2Cu4.8O10+z	La	1.6	Gd	0.4	Ca	0.8	Ba	2	Cu	4.8											O	10+z		1	2001																												2125																		K	77						77																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9879	JAP0897657		(La,Gd)2CaBa2Cu5Oz	La1.5Gd0.5Ca1Ba2Cu5O10+z	La	1.5	Gd	0.5	Ca	1	Ba	2	Cu	5											O	10+z		1	2001																												2125																		K	80						80																																																																																															1	solid state reaction					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
9880	PHB2810924	not s/c	La2(La,Ba)Ba2Cu5Oz	La2.5Ba2.5Cu5O11.82	La	2.5	Ba	2.5	Cu	5															O	10+z	11.82	1	2000																												2125																		K					10																																																																																																	1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9881	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La2.3Yb0.1Ba2.3Ca0.2Cu5O11.805	La	2.3	Yb	0.1	Ba	2.3	Ca	0.2	Cu	5											O	10+z	11.805	1	2000																												2125																		K	25						25																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9882	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La2.1Yb0.2Ba2.1Ca0.4Cu5O11.802	La	2.1	Yb	0.2	Ba	2.1	Ca	0.4	Cu	5											O	10+z	11.802	1	2000																												2125																		K	47						47																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9883	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La1.9Yb0.3Ba1.9Ca0.6Cu5O11.797	La	1.9	Yb	0.3	Ba	1.9	Ca	0.6	Cu	5											O	10+z	11.797	1	2000																												2125																		K	60						60																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9884	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La1.7Yb0.4Ba1.7Ca0.8Cu5O11.795	La	1.7	Yb	0.4	Ba	1.7	Ca	0.8	Cu	5											O	10+z	11.795	1	2000																												2125																		K	76						76																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9885	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La1.5Yb0.5Ba1.5Ca1Cu5O11.785	La	1.5	Yb	0.5	Ba	1.5	Ca	1	Cu	5											O	10+z	11.785	1	2000																												2125																		K	76						76																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9886	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La1.3Yb0.6Ba1.3Ca1.2Cu5O11.74	La	1.3	Yb	0.6	Ba	1.3	Ca	1.2	Cu	5											O	10+z	11.74	1	2000																												2125																		K	73						73																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9887	PHB2810924		La2(La,Ba,Yb,Ca)Ba2Cu5Oz	La1.1Yb0.7Ba1.1Ca1.4Cu5O11.692	La	1.1	Yb	0.7	Ba	1.1	Ca	1.4	Cu	5											O	10+z	11.692	1	2000																												2125																		K	70						70																																																																																															1	solid state reaction					Dependence of superconductivity on hole concentration (Psh) in La-2125 perovskite system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 281(2000)924	D.G.Kuberkar,M.R.Gonal,N.A.Shah,R.G.Kulkarni,R.S.Thampi,Ram Prasad		
9888	PHB2590538		(La,Y)2CaBa2Cu5Oz	La1.9Y0.1Ba2Ca0.2Cu4.2Oz	La	1.9	Y	0.1	Ba	2	Ca	0.2	Cu	4.2											O	z		1	1999																												2125																		K	21						21																																																																																															1	solid state reaction					Correlation between hole concentration and Tc in (La2-xYx)Ba2(CayCu4+y)Oz superconductors			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 259(1999)538	Amish G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
9889	PHB2590538		(La,Y)2CaBa2Cu5Oz	La1.8Y0.2Ba2Ca0.4Cu4.4Oz	La	1.8	Y	0.2	Ba	2	Ca	0.4	Cu	4.4											O	z		1	1999																												2125																		K	42						42																																																																																															1	solid state reaction					Correlation between hole concentration and Tc in (La2-xYx)Ba2(CayCu4+y)Oz superconductors			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 259(1999)538	Amish G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
9890	PHB2590538		(La,Y)2CaBa2Cu5Oz	La1.7Y0.3Ba2Ca0.6Cu4.6Oz	La	1.7	Y	0.3	Ba	2	Ca	0.6	Cu	4.6											O	z		1	1999																												2125																		K	65						65																																																																																															1	solid state reaction					Correlation between hole concentration and Tc in (La2-xYx)Ba2(CayCu4+y)Oz superconductors			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 259(1999)538	Amish G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
9891	PHB2590538		(La,Y)2CaBa2Cu5Oz	La1.6Y0.4Ba2Ca0.8Cu4.8Oz	La	1.6	Y	0.4	Ba	2	Ca	0.8	Cu	4.8											O	z		1	1999																												2125																		K	78						78																																																																																															1	solid state reaction					Correlation between hole concentration and Tc in (La2-xYx)Ba2(CayCu4+y)Oz superconductors			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 259(1999)538	Amish G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
9892	PHB2590538		(La,Y)2CaBa2Cu5Oz	La1.5Y0.5Ba2Ca1Cu5Oz	La	1.5	Y	0.5	Ba	2	Ca	1	Cu	5											O	z		1	1999																												2125																		K	78						78																																																																																															1	solid state reaction					Correlation between hole concentration and Tc in (La2-xYx)Ba2(CayCu4+y)Oz superconductors			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	Physica B, 259(1999)538	Amish G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
9893	SUP0140341	re-entrant s/c. re-entrant at 5K. Resistive transition under magnetic fields shows sample dependency	(Sr,K)BiO3	Sr0.4K0.6Bi1O3	Sr	0.4	K	0.6	Bi	1															O	3		1	2001																												BKBO			A	5.94		8.43												K	10.1		12.5				11.3																																																																																														Sr2Bi2O5,KO2,Bi2O3		mixture-sealed in Au capsule-high pressure systhesis(2GPa, 20-60 min, 700C)					Anomalous reentrant resistance phenomena in superconducting  Sr1-xKxBiO3: Recovery of superconductivity with electric or magnetic field			Seoul National University,Seoul,Korea	J.Supercond., 14(2001)341	D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
9894	SUP0140397	O-content by iodometry	(La,Y)3CaBa3Cu7Oz	La2.5Y0.5Ca1Ba3Cu7O16.574	La	2.5	Y 	0.5	Ca	1	Ba	3	Cu	7											O	z	16.574	1	2001																												3137			A	3.8609		11.642												K	79	80	81	80			80																																																																																														La2O3,Y2O3,BaCO3,CuO,CaCO3,Fe2O3	1	mixture-heat(950C,24h in Pt crucible)-pellet-SIN(940C-960C,12h in O2 and N2)-ANN(500C,12h in O2 flow)-slow cool to RT(1C/min)					Structural studies of the superconducting La2.5Y0.5CaBa3(Cu1-xFex)7Oz (0<=x<=0.1) perovskite system by neutron diffraction			Saurashtra University,Rajkot,India	J.Supercond., 14(2001)397	D.C.Kundaliya,M.V.Subbarao,R.G.Kulkarni,S.K.Malik,W.B.Yelon		
9895	SUP0140397	O-content by iodometry	(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.86Fe0.14O16.578	La	2.5	Y 	0.5	Ca	1	Ba	3	Cu	6.86	Fe	0.14									O	z	16.578	1	2001																												3137			A	3.869		11.6697												K	73	77	80	75			77																																																																																														La2O3,Y2O3,BaCO3,CuO,CaCO3,Fe2O3	1	mixture-heat(950C,24h in Pt crucible)-pellet-SIN(940C-960C,12h in O2 and N2)-ANN(500C,12h in O2 flow)-slow cool to RT(1C/min)					Structural studies of the superconducting La2.5Y0.5CaBa3(Cu1-xFex)7Oz (0<=x<=0.1) perovskite system by neutron diffraction			Saurashtra University,Rajkot,India	J.Supercond., 14(2001)397	D.C.Kundaliya,M.V.Subbarao,R.G.Kulkarni,S.K.Malik,W.B.Yelon		
9896	SUP0140397	O-content by iodometry	(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.58Fe0.42O16.599	La	2.5	Y 	0.5	Ca	1	Ba	3	Cu	6.58	Fe	0.42									O	z	16.599	1	2001																												3137			A	3.8707		11.6225												K	62	68	73	63			68																																																																																														La2O3,Y2O3,BaCO3,CuO,CaCO3,Fe2O3	1	mixture-heat(950C,24h in Pt crucible)-pellet-SIN(940C-960C,12h in O2 and N2)-ANN(500C,12h in O2 flow)-slow cool to RT(1C/min)					Structural studies of the superconducting La2.5Y0.5CaBa3(Cu1-xFex)7Oz (0<=x<=0.1) perovskite system by neutron diffraction			Saurashtra University,Rajkot,India	J.Supercond., 14(2001)397	D.C.Kundaliya,M.V.Subbarao,R.G.Kulkarni,S.K.Malik,W.B.Yelon		
9897	SUP0140397	O-content by iodometry	(La,Y)3CaBa3(Cu,Fe)7Oz	La2.5Y0.5Ca1Ba3Cu6.3Fe0.7O16.627	La	2.5	Y 	0.5	Ca	1	Ba	3	Cu	6.3	Fe	0.7									O	z	16.627	1	2001																												3137			A	3.8772		11.6318												K	41	51	60	41			51																																																																																														La2O3,Y2O3,BaCO3,CuO,CaCO3,Fe2O3	1	mixture-heat(950C,24h in Pt crucible)-pellet-SIN(940C-960C,12h in O2 and N2)-ANN(500C,12h in O2 flow)-slow cool to RT(1C/min)					Structural studies of the superconducting La2.5Y0.5CaBa3(Cu1-xFex)7Oz (0<=x<=0.1) perovskite system by neutron diffraction			Saurashtra University,Rajkot,India	J.Supercond., 14(2001)397	D.C.Kundaliya,M.V.Subbarao,R.G.Kulkarni,S.K.Malik,W.B.Yelon		
9898	JAP0897663		LaBa2Cu3O7	La1Ba2Cu3O7	La	1	Ba	2	Cu	3															O	7		1	2001																												Y123																		K				89.6			89.6																																																																																																pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9899	JAP0897663		(La,Pr)Ba2Cu3O7	La0.9Pr0.1Ba2Cu3O7	La	0.9	Pr	0.1	Ba	2	Cu	3													O	7		1	2001																												Y123																		K				68.3			68.3																																																																																																pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9900	JAP0897663		(La,Pr)Ba2Cu3O7	La0.8Pr0.2Ba2Cu3O7	La	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	2001								5.8																				Y123																		K				59.8			59.8																																																																																																pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9901	JAP0897663		(La,Pr)Ba2Cu3O7	La0.7Pr0.3Ba2Cu3O7	La	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	2001								10.8																				Y123																		K				57.1			57.1																																																					SP9901																																											pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9902	JAP0897663		(La,Pr)Ba2Cu3O7	La0.6Pr0.4Ba2Cu3O7	La	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	2001								12.7																				Y123																		K				54.8			54.8																																																																																																pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9903	JAP0897663		(La,Pr)Ba2Cu3O7	La0.5Pr0.5Ba2Cu3O7	La	0.5	Pr	0.5	Ba	2	Cu	3													O	7		1	2001								13.5																				Y123																		K				51.7			51.7																																																																																																pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9904	JAP0897663		(La,Pr)Ba2Cu3O7	La0.4Pr0.6Ba2Cu3O7	La	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	2001								14.7																				Y123																																																																																																																									pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9905	JAP0897663		(La,Pr)Ba2Cu3O7	La0.3Pr0.7Ba2Cu3O7	La	0.3	Pr	0.7	Ba	2	Cu	3													O	7		1	2001								15.4																				Y123																																																																																																																									pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9906	JAP0897663		(La,Pr)Ba2Cu3O7	La0.2Pr0.8Ba2Cu3O7	La	0.2	Pr	0.8	Ba	2	Cu	3													O	7		1	2001								16.2																				Y123																																																																																																																									pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9907	JAP0897663		(La,Pr)Ba2Cu3O7	La0.1Pr0.9Ba2Cu3O7	La	0.1	Pr	0.9	Ba	2	Cu	3													O	7		1	2001								17.4																				Y123																																																																																																																									pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9908	JAP0897663		PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		1	2001								17.8																				Y123																																																																																																																									pellet-SIN(920-960C,1d in flowing Ar)-ANN(400C,2d in flowing O2)					Coexistence of superconductivity and antiferromagnetism in the La1-xPrxBa2Cu3O7 system			Department of Physics and National Laboratory of Solid State Microstructures, Nanjing University, Nanjing 210093, People's Republic of China	J.Appl.Phys., 89(2001)7663	H.M.Luo,S.Y.Ding,X.S.Wu		
9909	JPS0700644	NQR measurement	YBa2(Cu,Ni)4O8	Y1Ba2Cu3.964Ni0.036O8	Y	1	Ba	2	Cu	3.964	Ni	0.036													O	8		1	2001																												Y124																		K			63				63																																																																																															1	high-oxygen-pressure technique					Magnetic correlation near impurities in YBa2(Cu1-xMx)4O8 (M=Ni,Zn) via Cu nuclear spin-lattice relaxation			SRL-ISTEC, Shinonome,Koto-ku, Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)644	N.Koshizuka,N.Watanabe,T.Machi,Y.Itoh		
9910	JPS0700644	NQR measurement	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O	8		1	2001																												Y124																		K			68				68																																																																																															1	high-oxygen-pressure technique					Magnetic correlation near impurities in YBa2(Cu1-xMx)4O8 (M=Ni,Zn) via Cu nuclear spin-lattice relaxation			SRL-ISTEC, Shinonome,Koto-ku, Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)644	N.Koshizuka,N.Watanabe,T.Machi,Y.Itoh		
9911	JPS0700644	NQR measurement	YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O	8		1	2001																												Y124																		K			56				56																																																																																															1	high-oxygen-pressure technique					Magnetic correlation near impurities in YBa2(Cu1-xMx)4O8 (M=Ni,Zn) via Cu nuclear spin-lattice relaxation			SRL-ISTEC, Shinonome,Koto-ku, Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)644	N.Koshizuka,N.Watanabe,T.Machi,Y.Itoh		
9912	PHB2810909	Annealed at 300C in O2 flow	(Y,La)Ba2Cu3O7	Y0.625La0.375Ba2Cu3O7-z	Y	0.625	La	0.375	Ba	2	Cu	3													O	7-z		1	2000																												Y123																		K		85.2					85.2																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9913	PHB2810909	Annealed at 300C in O2 flow	(Y,La,Pr)Ba2Cu3O7	Y0.5625La0.3375Pr0.1Ba2Cu3O7-z	Y	0.5625	La	0.3375	Pr	0.1	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		63.7					63.7																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9914	PHB2810909	Annealed at 300C in O2 flow	(Y,La,Pr)Ba2Cu3O7	Y0.5La0.3Pr0.2Ba2Cu3O7-z	Y	0.5	La	0.3	Pr	0.2	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		44.8					44.8																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9915	PHB2810909	Annealed at 300C in O2 flow	(Y,La,Pr)Ba2Cu3O7	Y0.4375La0.2625Pr0.3Ba2Cu3O7-z	Y	0.4375	La	0.2625	Pr	0.3	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		28.9					28.9																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9916	PHB2810909	quenched from 500C	(Y,La)Ba2Cu3O7	Y0.625La0.375Ba2Cu3O7-z	Y	0.625	La	0.375	Ba	2	Cu	3													O	7-z		1	2000																												Y123																		K		50					50																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9917	PHB2810909	quenched from 500C	(Y,La,Pr)Ba2Cu3O7	Y0.5625La0.3375Pr0.1Ba2Cu3O7-z	Y	0.5625	La	0.3375	Pr	0.1	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		40					40																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9918	PHB2810909	quenched from 500C	(Y,La,Pr)Ba2Cu3O7	Y0.5La0.3Pr0.2Ba2Cu3O7-z	Y	0.5	La	0.3	Pr	0.2	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		21					21																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9919	PHB2810909	quenched from 500C	(Y,La,Pr)Ba2Cu3O7	Y0.4375La0.2625Pr0.3Ba2Cu3O7-z	Y	0.4375	La	0.2625	Pr	0.3	Ba	2	Cu	3											O	7-z		1	2000																												Y123																		K		0					0																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9920	PHB2810909		GdBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-z	6.95	1	2000																												Y123																		K		92.2					92.2																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9921	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.95	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.95	1	2000																												Y123																		K		78.5					78.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9922	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.95	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.95	1	2000																												Y123																		K		58.5					58.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9923	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.95	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.95	1	2000																												Y123																		K		39.3					39.3																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9924	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.65Pr0.35Ba2Cu3O6.95	Y	0.65	Pr	0.35	Ba	2	Cu	3													O	7-z	6.95	1	2000																												Y123																		K		33					33																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9925	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.95	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.95	1	2000																												Y123																		K		20.4					20.4																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9926	PHB2810909		GdBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	7-z	6.85	1	2000																												Y123																		K		84.4					84.4																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9927	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.85	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.85	1	2000																												Y123																		K		61.5					61.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9928	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.85	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.85	1	2000																												Y123																		K		45.2					45.2																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9929	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.85	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.85	1	2000																												Y123																		K		27.4					27.4																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9930	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.65Pr0.35Ba2Cu3O6.85	Y	0.65	Pr	0.35	Ba	2	Cu	3													O	7-z	6.85	1	2000																												Y123																		K		16.3					16.3																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9931	PHB2810909		GdBa2Cu3O7	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	7-z	6.75	1	2000																												Y123																		K		61.1					61.1																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9932	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.75	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.75	1	2000																												Y123																		K		52.2					52.2																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9933	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.75	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.75	1	2000																												Y123																		K		41.5					41.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9934	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.75	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.75	1	2000																												Y123																		K		25.2					25.2																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9935	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.65Pr0.35Ba2Cu3O6.75	Y	0.65	Pr	0.35	Ba	2	Cu	3													O	7-z	6.75	1	2000																												Y123																		K		6.3					6.3																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9936	PHB2810909		GdBa2Cu3O7	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	7-z	6.6	1	2000																												Y123																		K		49.6					49.6																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9937	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.6	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.6	1	2000																												Y123																		K		44.1					44.1																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9938	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.6	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.6	1	2000																												Y123																		K		37					37																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9939	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.6	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.6	1	2000																												Y123																		K		28.5					28.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9940	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.65Pr0.35Ba2Cu3O6.6	Y	0.65	Pr	0.35	Ba	2	Cu	3													O	7-z	6.6	1	2000																												Y123																		K		21.5					21.5																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9941	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.6	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.6	1	2000																												Y123																		K		0					0																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9942	PHB2810909		GdBa2Cu3O7	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	7-z	6.5	1	2000																												Y123																		K		31.1					31.1																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9943	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.5	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z	6.5	1	2000																												Y123																		K		21.1					21.1																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9944	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.5	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z	6.5	1	2000																												Y123																		K		11.1					11.1																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9945	PHB2810909		(Gd,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.5	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.5	1	2000																												Y123																		K		0					0																																																																																															1	solid state reaction-Q into L-N2 from high temperature. O-content by annealing in O2.					Rare-earth ionic radius dependence of superconductivity in Pe-substituted and oxygen deficient R1-xPrxBa2Cu3O7-z			Tokushima University,Tokushima,Japan	Physica B, 281(2000)909	K.Koyama,K.Mizuno,T.Saito,T.Tange		
9946	P064144524	x=0.11 determined by ICP-AES. Z=4.00 by iodometry. Phase transition = 256K(THT to OMT), = 53K(OMT to TLT)	(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4	4	3	2001																												T			A	5.4378	5.4756	15.7902												K		17.8		10.2			17.8																																																																						TP9946																					RH9946					TSFZ method					Crystal growth, transport properties, and crystal structure of the single-crystal La2-xBaxCuO4 (x = 0.11)			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Japan	Phys.Rev.B, 64(2001)144524	T.Adachi,T.Noji,Y.Koike		
9947	P064144521	not s/c	Pb2Sr2CmCu3O8	Pb2Sr2Cm1Cu3O8	Pb	2	Sr	2	Cm	1	Cu	3													O	8		1	2001						8.7		18																				Pb3212			A	5.4253	5.4605	15.8055												K					5																																																																																																	1	Cm<248> is a man-made radioactive isotope.					Electronic and magnetic properties of Cm in Pb2Sr2Cm1-xCaxCu3O8 (x = 0.0 and 0.5)			Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439 ,USA	Phys.Rev.B, 64(2001)144521	C.W.Williams,L.Soderholm,S.Skanthakumar		
9948	P064144521	not s/c. no indication of magnetic ordering of Cm.	Pb2Sr2(Cm,Ca)Cu3O8	Pb2Sr2Cm0.5Ca0.5Cu3O8	Pb	2	Sr	2	Cm	0.5	Ca	0.5	Cu	3											O	8		1	2001																												Pb3212																		K					5																																																																																																	1	Cm<248> is a man-made radioactive isotope.					Electronic and magnetic properties of Cm in Pb2Sr2Cm1-xCaxCu3O8 (x = 0.0 and 0.5)			Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439 ,USA	Phys.Rev.B, 64(2001)144521	C.W.Williams,L.Soderholm,S.Skanthakumar		
9949	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.98Zn0.02O4	La	1.875	Ba	0.125	Cu	0.98	Zn	0.02													O	4		1	2000																												T																																																																																	mj/mol.K2	5.95	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9950	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.96Zn0.04O4	La	1.875	Ba	0.125	Cu	0.96	Zn	0.04													O	4		1	2000																												T																																																																																	mj/mol.K2	8.57	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9951	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.94Zn0.06O4	La	1.875	Ba	0.125	Cu	0.94	Zn	0.06													O	4		1	2000																												T																																																																																	mj/mol.K2	11.61	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9952	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.92Zn0.08O4	La	1.875	Ba	0.125	Cu	0.92	Zn	0.08													O	4		1	2000																												T																																																																																	mj/mol.K2	12.02	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9953	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.9Zn0.1O4	La	1.875	Ba	0.125	Cu	0.9	Zn	0.1													O	4		1	2000																												T																																																																																	mj/mol.K2	11.96	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9954	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Zn)O4	La1.875Ba0.125Cu0.875Zn0.125O4	La	1.875	Ba	0.125	Cu	0.875	Zn	0.125													O	4		1	2000																												T																																																																																	mj/mol.K2	12.32	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9955	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Ni)O4	La1.875Ba0.125Cu0.99Ni0.01O4	La	1.875	Ba	0.125	Cu	0.99	Ni	0.01													O	4		1	2000																												T																																																																																	mj/mol.K2	5.3	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9956	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Ni)O4	La1.875Ba0.125Cu0.98Ni0.02O4	La	1.875	Ba	0.125	Cu	0.98	Ni	0.02													O	4		1	2000																												T																																																																																	mj/mol.K2	6.55	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9957	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Ni)O4	La1.875Ba0.125Cu0.96Ni0.04O4	La	1.875	Ba	0.125	Cu	0.96	Ni	0.04													O	4		1	2000																												T																																																																																	mj/mol.K2	6.19	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9958	PHB2810918	sp-heat measured for 1.5<T<7 K.	(La,Ba)2(Cu,Ni)O4	La1.875Ba0.125Cu0.94Ni0.06O4	La	1.875	Ba	0.125	Cu	0.94	Ni	0.06													O	4		1	2000																												T																																																																																	mj/mol.K2	6.61	low temp sp-heat																																											Effect of Zn- or Ni-substitution on specific heat in La1.875Ba0.125CuO4: role of spin interaction in stripe phase			Department of Applied Physics, Hokkaido University, Kita 13 Nishi 8, Kita-ku, Sapporo 060-8628, Japan	Physica B, 281-282(2000)918	K.Yamaya,O.Anegawa,S.Tanda,Y.Okajima		
9959	PHC3560192	resistivity is non-zero at 4.2K for as-grown sample.	(Hg,W)Sr2(Gd,Ce)2Cu2Oz	Hg0.75W0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2001																												Hg1222			A	3.838		29.115												K	4.2		27				15.6																																																																																																precursor(Sr2Gd1.5Ce0.5Cu2Oz)+HgO+MxOz, mix and press, sealed in quartz tube, SIN(950C,20h), ANN(450C,250 atm O2)					Synthesis and superconductivity study for (Hg,M)-1222 phase (M=W, Mo, V, Cr, Ti)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui , People's Republic of China	Physica C, 356(2001)192	L.Liu,R.Fan,S.Y.Li,X.H.Chen		
9960	PHC3560192	resistivity is non-zero at 4.2K for as-grown sample.	(Hg,Mo)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Mo0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Mo	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2001																												Hg1222			A	3.842		29.108												K			27				27																																																																																																precursor(Sr2Gd1.5Ce0.5Cu2Oz)+HgO+MxOz, mix and press, sealed in quartz tube, SIN(950C,20h), ANN(450C,250 atm O2)					Synthesis and superconductivity study for (Hg,M)-1222 phase (M=W, Mo, V, Cr, Ti)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui , People's Republic of China	Physica C, 356(2001)192	L.Liu,R.Fan,S.Y.Li,X.H.Chen		
9961	PHC3560192	not s/c. dominant phase = Hg-1222. Impurity phase = CeO2	(Hg,V)Sr2(Gd,Ce)2Cu2Oz	Hg0.75V0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	V	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z			2001																												Hg1222			A	3.86		28.858												K					4.2																																																																																																		precursor(Sr2Gd1.5Ce0.5Cu2Oz)+HgO+MxOz, mix and press, sealed in quartz tube, SIN(950C,20h), ANN(450C,250 atm O2)					Synthesis and superconductivity study for (Hg,M)-1222 phase (M=W, Mo, V, Cr, Ti)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui , People's Republic of China	Physica C, 356(2001)192	L.Liu,R.Fan,S.Y.Li,X.H.Chen		
9962	PHC3560192	not s/c. dominant phase = Hg-1222. Impurity phase = CeO2	(Hg,Cr)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Cr0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Cr	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z			2001																												Hg1222			A	3.864		28.676												K					4.2																																																																																																		precursor(Sr2Gd1.5Ce0.5Cu2Oz)+HgO+MxOz, mix and press, sealed in quartz tube, SIN(950C,20h), ANN(450C,250 atm O2)					Synthesis and superconductivity study for (Hg,M)-1222 phase (M=W, Mo, V, Cr, Ti)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui , People's Republic of China	Physica C, 356(2001)192	L.Liu,R.Fan,S.Y.Li,X.H.Chen		
9963	PHC2600117		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4			1996																												T'			A	3.953		12.129												K	16.4		20.4	17			17																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9964	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.8315Y0.0185Ce0.15Cu1O4	Pr	1.8315	Y	0.0185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.952		12.126												K	14.3		18.7	16			16																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9965	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.7945Y0.0555Ce0.15Cu1O4	Pr	1.7945	Y	0.0555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.95		12.11												K	13.3		18.5	15			15																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9966	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.7575Y0.0925Ce0.15Cu1O4	Pr	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.948		12.105												K	12.5		17.1	14.5			14.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9967	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.665Y0.185Ce0.15Cu1O4	Pr	1.665	Y	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.944		12.069												K	10.3		15.9	13			13																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9968	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.5725Y0.2775Ce0.15Cu1O4	Pr	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.94		12.046												K			13.5	11			11																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9969	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.48Y0.37Ce0.15Cu1O4	Pr	1.48	Y	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.936		12.022												K			12.1	9.5			9.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9970	PHC2600117		(Pr,Y,Ce)2CuO4	Pr1.295Y0.555Ce0.15Cu1O4	Pr	1.295	Y	0.555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.937		12.023												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9971	PHC2600117		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4			1996																												T'			A	3.939		12.053												K	18.9		23.3	21			21																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9972	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.8315Y0.0185Ce0.15Cu1O4	Nd	1.8315	Y	0.0185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.938		12.04												K	18		22.5	20			20																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9973	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.7945Y0.0555Ce0.15Cu1O4	Nd	1.7945	Y	0.0555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.935		12.025												K	17.3		21	19			19																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9974	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.7575Y0.0925Ce0.15Cu1O4	Nd	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.934		12.014												K	16.2		20.6	18			18																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9975	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.665Y0.185Ce0.15Cu1O4	Nd	1.665	Y	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.929		11.999												K	12.4		18.2	16			16																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9976	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.5725Y0.2775Ce0.15Cu1O4	Nd	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.926		11.983												K			13.9	10.5			10.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9977	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.48Y0.37Ce0.15Cu1O4	Nd	1.48	Y	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.922		11.953												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9978	PHC2600117		(Nd,Y,Ce)2CuO4	Nd1.295Y0.555Ce0.15Cu1O4	Nd	1.295	Y	0.555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.922		11.922												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9979	PHC2600117		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4			1996																												T'			A	3.912		11.874												K	16.2		20	17			17																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9980	PHC2600117		(Sm,Y,Ce)2CuO4	Sm1.80375Y0.04625Ce0.15Cu1O4	Sm	1.80375	Y	0.04625	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.91		11.868												K	14.4		18.1	15			15																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9981	PHC2600117		(Sm,Y,Ce)2CuO4	Sm1.7575Y0.0925Ce0.15Cu1O4	Sm	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.909		11.865												K	12		16.4	14			14																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9982	PHC2600117		(Sm,Y,Ce)2CuO4	Sm1.71125Y0.13875Ce0.15Cu1O4	Sm	1.71125	Y	0.13875	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.907		11.852												K			15	12			12																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9983	PHC2600117		(Sm,Y,Ce)2CuO4	Sm1.665Y0.185Ce0.15Cu1O4	Sm	1.665	Y	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.906		11.845												K			12.6	10			10																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9984	PHC2600117		(Sm,Y,Ce)2CuO4	Sm1.5725Y0.2775Ce0.15Cu1O4	Sm	1.5725	Y	0.2775	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.905		11.838												K			10.3				10.3																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9985	PHC2600117		(Eu,Ce)2CuO4	Eu1.85Ce0.15Cu1O4	Eu	1.85	Ce	0.15	Cu	1															O	4			1996																												T'			A	3.901		11.826												K			12.1	7.5			7.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9986	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.80375Y0.04625Ce0.15Cu1O4	Eu	1.80375	Y	0.04625	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.9		11.816												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9987	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.7575Y0.0925Ce0.15Cu1O4	Eu	1.7575	Y	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.9		11.81												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9988	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.71125Y0.13875Ce0.15Cu1O4	Eu	1.71125	Y	0.13875	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.899		11.809												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9989	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.665Y0.185Ce0.15Cu1O4	Eu	1.665	Y	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.897		11.807												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9990	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.61875Y0.23125Ce0.15Cu1O4	Eu	1.61875	Y	0.23125	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.896		11.806												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9991	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.84075Y0.00925Ce0.15Cu1O4	Eu	1.84075	Y	0.00925	Ce	0.15	Cu	1													O	4			1996																												T'			A															K			10.1	5.2			5.2																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9992	PHC2600117		(Eu,Y,Ce)2CuO4	Eu1.8315Y0.0185Ce0.15Cu1O4	Eu	1.8315	Y	0.0185	Ce	0.15	Cu	1													O	4			1996																												T'			A															K				4.3			4.3																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9993	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr1.665Gd0.185Ce0.15Cu1O4	Pr	1.665	Gd	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.944		12.075												K	14		18.2	15.5			15.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9994	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr1.48Gd0.37Ce0.15Cu1O4	Pr	1.48	Gd	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.94		12.045												K	12		17	14.5			14.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9995	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr1.295Gd0.555Ce0.15Cu1O4	Pr	1.295	Gd	0.555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.934		12.015												K	9.9		16	13.5			13.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9996	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr1.11Gd0.74Ce0.15Cu1O4	Pr	1.11	Gd	0.74	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.926		11.976												K			14.8	12.5			12.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9997	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr0.925Gd0.925Ce0.15Cu1O4	Pr	0.925	Gd	0.925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.924		11.947												K			13.9	9.5			9.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9998	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr0.74Gd1.11Ce0.15Cu1O4	Pr	0.74	Gd	1.11	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.918		11.913												K			11	7.5			7.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
9999	PHC2600117		(Pr,Gd,Ce)2CuO4	Pr0.555Gd1.295Ce0.15Cu1O4	Pr	0.555	Gd	1.295	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.919		11.921												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
10000	PR04901495	c-axis-oriented bulk compound	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10	Bi	2	Sr	2	Ca	2	Cu	3													O	10			1994																											3	Bi2223			A	5.51	5.19	37.28												K		109				3	109		1																																							A	Magnetization		1240																																																				see Physica C 200(1992)105					Flux-line-lattice melting in Bi2Sr2Ca2Cu3O10	1		Instituto de Fisica,Unicamp,Sao Paulo,Brazil	Phys.Rev.B, 49(1994)1495	J.H.S.Torres,S.Moehlecke,Y.Kopelevich	Bi,Sr,Ca,Cu,O	
10001	PR04901407	compound	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.23	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.23		1994																												Bi2212																		K				70			70		2																																																																																														see Physica C 165(1990)55					Electronic structure of Bi2Sr2Ca1-xYxCu2O8+z: Cu 2p x-ray-photoelectron spectra and occupied and unoccupied low-energy states	1		Laboratory of Applied and Solid State Physics, University of Groningen,Groningen,The Netherland	Phys.Rev.B, 49(1994)1407	G.A.Sawatzky,M.A.van Veenendaal,W.A.Groen	Bi,Sr,Ca,Y,Cu,O	
10002	PR04901407	compound	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8.23	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8	8.23		1994																												Bi2212																		K				85			85		2																																																																																														see Physica C 165(1990)55					Electronic structure of Bi2Sr2Ca1-xYxCu2O8+z: Cu 2p x-ray-photoelectron spectra and occupied and unoccupied low-energy states	1		Laboratory of Applied and Solid State Physics, University of Groningen,Groningen,The Netherland	Phys.Rev.B, 49(1994)1407	G.A.Sawatzky,M.A.van Veenendaal,W.A.Groen	Bi,Sr,Ca,Y,Cu,O	
10003	PR04901407	compound	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8.3	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8	8.3		1994																												Bi2212																		K				86			86		2																																																																																														see Physica C 165(1990)55					Electronic structure of Bi2Sr2Ca1-xYxCu2O8+z: Cu 2p x-ray-photoelectron spectra and occupied and unoccupied low-energy states	1		Laboratory of Applied and Solid State Physics, University of Groningen,Groningen,The Netherland	Phys.Rev.B, 49(1994)1407	G.A.Sawatzky,M.A.van Veenendaal,W.A.Groen	Bi,Sr,Ca,Y,Cu,O	
10004	PR04901407	compound	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8.29	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8	8.29		1994																												Bi2212																		K				64			64		2																																																																																														see Physica C 165(1990)55					Electronic structure of Bi2Sr2Ca1-xYxCu2O8+z: Cu 2p x-ray-photoelectron spectra and occupied and unoccupied low-energy states	1		Laboratory of Applied and Solid State Physics, University of Groningen,Groningen,The Netherland	Phys.Rev.B, 49(1994)1407	G.A.Sawatzky,M.A.van Veenendaal,W.A.Groen	Bi,Sr,Ca,Y,Cu,O	
10005	PR04901407	compound	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8.33	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8	8.33		1994																												Bi2212																		K				40			40		2																																																																																														see Physica C 165(1990)55					Electronic structure of Bi2Sr2Ca1-xYxCu2O8+z: Cu 2p x-ray-photoelectron spectra and occupied and unoccupied low-energy states	1		Laboratory of Applied and Solid State Physics, University of Groningen,Groningen,The Netherland	Phys.Rev.B, 49(1994)1407	G.A.Sawatzky,M.A.van Veenendaal,W.A.Groen	Bi,Sr,Ca,Y,Cu,O	
10006	PR04901499	compound	TlSr2GdCu2O7	Tl1Sr2Gd1Cu2O7-z	Tl	1	Sr	2	Gd	1	Cu	2													O	7-z			1994								2.4																			2	Tl1212			A	3.831		12.04																																																																																																																			see Phys.Rev.B 47(1993)178					Anisotropic Gd magnetism in TlSr2GdCu2O7-z,(Pb0.5Cu0.5)Sr2GdCu2O7-z, and Pb2Sr2GdCu3O8+z	1		Department of Physics,National Tsing Hua University,Hsinchu,Taiwan	Phys.Rev.B, 49(1994)1499	B.S.Chiou,C.C.Lai,H.C.Ku,J.C.Ho,J.H.Shieh	Tl,Sr,Gd,Cu,O,Pb,	
10007	PR04901499	compound	(Pb,Cu)Sr2GdCu2O7	Pb0.5Sr2Gd1Cu2.5O7-z	Pb	0.5	Sr	2	Gd	1	Cu	2.5													O	7-z			1994								2.3																			2	Pb1212			A	3.839		11.84																																																																																																																			see Phys.Rev.B 47(1993)178					Anisotropic Gd magnetism in TlSr2GdCu2O7-z,(Pb0.5Cu0.5)Sr2GdCu2O7-z, and Pb2Sr2GdCu3O8+z	1		Department of Physics,National Tsing Hua University,Hsinchu,Taiwan	Phys.Rev.B, 49(1994)1499	B.S.Chiou,C.C.Lai,H.C.Ku,J.C.Ho,J.H.Shieh	Tl,Sr,Gd,Cu,O,Pb,	
10008	PR04901499	compound	Pb2Sr2GdCu3O8	Pb2Sr2Gd1Cu3O8+y	Pb	2	Sr	2	Gd	1	Cu	3													O	8+y			1994								2.3																			3				A	5.411	5.448	15.74																																																																																																																			see Phys.Rev.B 47(1993)178					Anisotropic Gd magnetism in TlSr2GdCu2O7-z,(Pb0.5Cu0.5)Sr2GdCu2O7-z, and Pb2Sr2GdCu3O8+z	1		Department of Physics,National Tsing Hua University,Hsinchu,Taiwan	Phys.Rev.B, 49(1994)1499	B.S.Chiou,C.C.Lai,H.C.Ku,J.C.Ho,J.H.Shieh	Tl,Sr,Gd,Cu,O,Pb,	
10009	PR04901387		YBa2Cu3O7	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	6-z	6.98	3	1994																											3	Y123			A	3.82	3.886	11.696	2											K		89.8	90.4				89.8		1																																																																																												R2O3 (R=Y,Ho),BaCO3,CuO	5	Ho :  the flux was decanted before cooling beyond the BaO-CuO eutectic temperature(910 C)					Static and dynamic displacements in RBa2Cu3O7-z(R=Y,Ho;z=0.05,0.5): A neutron-diffraction study on single crystals	1		Institut fur Nukleare Festkorperphysik,Karlsruhe,Germany	Phys.Rev.B, 49(1994)1387	A.Erb,G.Collin,G.Heger,H.Claus,M.Braden,P.Schweiss,W.Reichardt	Y,Ba,Cu,O,Ho	
10010	PR04901387		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-z	6.96	3	1994																											3				A	3.819	3.885	11.68	2											K		90.75	90.95				90.75		1																																																																																												R2O3 (R=Y,Ho),BaCO3,CuO	5	Ho :  the flux was decanted before cooling beyond the BaO-CuO eutectic temperature(910 C)					Static and dynamic displacements in RBa2Cu3O7-z(R=Y,Ho;z=0.05,0.5): A neutron-diffraction study on single crystals	1		Institut fur Nukleare Festkorperphysik,Karlsruhe,Germany	Phys.Rev.B, 49(1994)1387	A.Erb,G.Collin,G.Heger,H.Claus,M.Braden,P.Schweiss,W.Reichardt	Y,Ba,Cu,O,Ho	
10011	PR04901387		YBa2Cu3O7	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	7-z	6.52	3	1994																											3	Y123			A	3.833	3.871	11.742	2											K		52.8	53.8				52.8		1																																																																																												R2O3 (R=Y,Ho),BaCO3,CuO	5	Ho :  the flux was decanted before cooling beyond the BaO-CuO eutectic temperature(910 C)					Static and dynamic displacements in RBa2Cu3O7-z(R=Y,Ho;z=0.05,0.5): A neutron-diffraction study on single crystals	1		Institut fur Nukleare Festkorperphysik,Karlsruhe,Germany	Phys.Rev.B, 49(1994)1387	A.Erb,G.Collin,G.Heger,H.Claus,M.Braden,P.Schweiss,W.Reichardt	Y,Ba,Cu,O,Ho	
10012	PR04901387		HoBa2Cu3O7	Ho1Ba2Cu2.94O6.94	Ho	1	Ba	2	Cu	2.94															O	7-z	6.94	3	1994																											3	Y123			A	3.841	3.875	11.682	2											K		77	85				77		1																																																																																												R2O3 (R=Y,Ho),BaCO3,CuO	5	Ho :  the flux was decanted before cooling beyond the BaO-CuO eutectic temperature(910 C)					Static and dynamic displacements in RBa2Cu3O7-z(R=Y,Ho;z=0.05,0.5): A neutron-diffraction study on single crystals	1		Institut fur Nukleare Festkorperphysik,Karlsruhe,Germany	Phys.Rev.B, 49(1994)1387	A.Erb,G.Collin,G.Heger,H.Claus,M.Braden,P.Schweiss,W.Reichardt	Y,Ba,Cu,O,Ho	
10013	PR04901387		HoBa2Cu3O7	Ho1Ba2Cu2.94O6.48	Ho	1	Ba	2	Cu	2.94															O	7-z	6.48	3	1994																											3	Y123			A	3.845	3.865	11.724	2											K		20	32				20		1																																																																																												R2O3 (R=Y,Ho),BaCO3,CuO	5	Ho :  the flux was decanted before cooling beyond the BaO-CuO eutectic temperature(910 C)					Static and dynamic displacements in RBa2Cu3O7-z(R=Y,Ho;z=0.05,0.5): A neutron-diffraction study on single crystals	1		Institut fur Nukleare Festkorperphysik,Karlsruhe,Germany	Phys.Rev.B, 49(1994)1387	A.Erb,G.Collin,G.Heger,H.Claus,M.Braden,P.Schweiss,W.Reichardt	Y,Ba,Cu,O,Ho	
10014	PR04900600	thin film	YBa2Cu3O7Hx	Y1Ba2Cu3H0.08O7	Y	1	Ba	2	Cu	3	H	0.08													O	7		4	1994																												Y123																		K			91	88			88		1																																																																																			m3/C		0.0000000027				RH10014						2		composite 1:2:3	thickness : 180nm-300nm	Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH,Bereich Schwerionenphysik,Berlin,Germany	Phys.Rev.B, 49(1994)600	A.Weidinger,B.Stritzker,G.Dortmann,H.Karl,J.Erxmeyer,J.Steiger,S.Blasser,T.Paatsch	Y,Ba,Cu,O	
10015	PR04900600	thin film	YBa2Cu3O7Hx	Y1Ba2Cu3H0.21O7	Y	1	Ba	2	Cu	3	H	0.21													O	7		4	1994																												Y123																		K			85	86			86		1																																																																																			m3/C		0.000000004										2		composite 1:2:3	thickness : 180nm-300nm	Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH,Bereich Schwerionenphysik,Berlin,Germany	Phys.Rev.B, 49(1994)600	A.Weidinger,B.Stritzker,G.Dortmann,H.Karl,J.Erxmeyer,J.Steiger,S.Blasser,T.Paatsch	Y,Ba,Cu,O	
10016	PR04900600	thin film	YBa2Cu3O7Hx	Y1Ba2Cu3H0.34O7	Y	1	Ba	2	Cu	3	H	0.34													O	7		4	1994																												Y123																		K			76	66			66		1																																																																																			m3/C		0.000000005										2		composite 1:2:3	thickness : 180nm-300nm	Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH,Bereich Schwerionenphysik,Berlin,Germany	Phys.Rev.B, 49(1994)600	A.Weidinger,B.Stritzker,G.Dortmann,H.Karl,J.Erxmeyer,J.Steiger,S.Blasser,T.Paatsch	Y,Ba,Cu,O	
10017	PR04900600	thin film	YBa2Cu3O7Hx	Y1Ba2Cu3H0.48O7	Y	1	Ba	2	Cu	3	H	0.48													O	7		4	1994																												Y123																		K			65	48			48		1																																																																																			m3/C		0.0000000059										2		composite 1:2:3	thickness : 180nm-300nm	Hydrogenation of thin Y-Ba-Cu-O films: Electrical transport and structure properties of YBa2Cu3O7 and YBa2Cu4O8	1		Hahn-Meitner-Institut Berlin GmbH,Bereich Schwerionenphysik,Berlin,Germany	Phys.Rev.B, 49(1994)600	A.Weidinger,B.Stritzker,G.Dortmann,H.Karl,J.Erxmeyer,J.Steiger,S.Blasser,T.Paatsch	Y,Ba,Cu,O	
10018	PR04901342	coherence length anisotropy ratio = 9.2	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	1994																												Y123																		K			92.5				92.5		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10019	PR04901342	coherence length anisotropy ratio = 10	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.985Fe0.015O7-z	Y	1	Ba	2	Cu	2.985	Fe	0.015													O	7-z		3	1994																												Y123																		K			91.5				91.5		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10020	PR04901342	coherence length anisotropy ratio = 11.5	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.96Fe0.04O7-z	Y	1	Ba	2	Cu	2.96	Fe	0.04													O	7-z		3	1994																												Y123																		K			90				90		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10021	PR04901342	coherence length anisotropy ratio = 19	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.87Fe0.13O7-z	Y	1	Ba	2	Cu	2.87	Fe	0.13													O	7-z		3	1994																												Y123																		K			78				78		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10022	PR04901342	coherence length anisotropy ratio = 23	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.83Fe0.17O7-z	Y	1	Ba	2	Cu	2.83	Fe	0.17													O	7-z		3	1994																												Y123																		K			72				72		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10023	PR04901342	coherence length anisotropy ratio = 29	YBa2(Cu,Fe)3O7	Y1Ba2Cu2.78Fe0.22O7-z	Y	1	Ba	2	Cu	2.78	Fe	0.22													O	7-z		3	1994																												Y123																		K			64				64		1																																																																																													5	ANN (420C,1 week in flowing oxygen)					Anisotropy of YBa2Cu3-xFexO7-z single crystals studied by torque magnetometry	1		Department of Physics and Astronomy,McMaster University ,Hamilton,Ontario,Canada	Phys.Rev.B, 49(1994)1342	J.Z.Liu,M.D.Lan,R.N.Shelton,T.R.Chien,W.R.Datars	Y,Ba,Cu,Fe,O	
10024	PR04901492		(Bi,Sr)2(Y,Ce)2Cu2O8	Bi0.5Sr1.5Y1.15Ce0.85Cu2O8-z	Bi	0.5	Sr	1.5	Y	1.15	Ce	0.85	Cu	2											O	8-z		1	1994																											2	T*			A	3.822		12.659												K	30	34	40	30		10	34		1																																																																																												Bi2O3,SrCO3,Y2O3,CeO2,CuO	1	CAL(950C,several overnight in Oxygen flow)-SIN(980C,36H in O2 flow)-Cool(0.25C/min to 500C)-HOLD(10H)-Cool(to room temperature)					T* phase (Bi0.5Sr1.5)(Y2-xCex)Cu2O8-z superconductors: The effect of ionic radius on structure	1		Department of Physics,University of Science & Technology of China,Hefei,People's Republic of China	Phys.Rev.B, 49(1994)1492	C.Y.Wong,G.E.Zhou,H.Chen,H.Zhang,L.Z.Cao,X.H.Chen,Y.H.Zhang,Z.J.Chen	Bi,Sr,Y,Ce,Cu,O	
10025	PR04901417	polycrystall	YBa2(Cu,Co)3O7	Y1Ba2Cu2.955Co0.045O7	Y	1	Ba	2	Cu	2.955	Co	0.045													O	7		4	1994																												Y123																		K																											T	from dHc2/dT			129					T/K	from Magnetization			2.01			A	from Hc2(0)			1.57																																																							5	see Physica C 214(1993)350					Magnetic susceptibilities, critical fields, and critical currents of Co- and Zn-doped YBa2Cu3O7	1		Interdiciplinary Research Center in Superconductivity,University of Cambridge, Cambridge,UK	Phys.Rev.B, 49(1994)1417	A.M.Campbell,A.Porch,D.N.Zheng,F.J.Blunt,J.D.Johnson,J.R.Cooper,P.A.Freeman	Y,Ba,Cu,Co,Zn,O	
10026	PR04901417	polycrystall	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1994																												Y123																		K				92			92																				T	from dHc2/dT			152					T/K	from Magnetization			2.32			A	from Hc2(0)			1.47																																																							5	see Physica C 214(1993)350					Magnetic susceptibilities, critical fields, and critical currents of Co- and Zn-doped YBa2Cu3O7	1		Interdiciplinary Research Center in Superconductivity,University of Cambridge, Cambridge,UK	Phys.Rev.B, 49(1994)1417	A.M.Campbell,A.Porch,D.N.Zheng,F.J.Blunt,J.D.Johnson,J.R.Cooper,P.A.Freeman	Y,Ba,Cu,Co,Zn,O	
10027	PR04901417	polycrystall	YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7	Y	1	Ba	2	Cu	2.88	Co	0.12													O	7		4	1994																												Y123																		K				81			81																																																																																															5	see Physica C 214(1993)350					Magnetic susceptibilities, critical fields, and critical currents of Co- and Zn-doped YBa2Cu3O7	1		Interdiciplinary Research Center in Superconductivity,University of Cambridge, Cambridge,UK	Phys.Rev.B, 49(1994)1417	A.M.Campbell,A.Porch,D.N.Zheng,F.J.Blunt,J.D.Johnson,J.R.Cooper,P.A.Freeman	Y,Ba,Cu,Co,Zn,O	
10028	PR04901417	polycrystall	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7		4	1994																												Y123																		K				42			42																				T	Hc2(0)=0.7*Tc*(dHc2/dT)|Tc			41					T/K	from Magnetization			1.45			A	from Hc2(0)			2.83																																																							5	see Physica C 214(1993)350					Magnetic susceptibilities, critical fields, and critical currents of Co- and Zn-doped YBa2Cu3O7	1		Interdiciplinary Research Center in Superconductivity,University of Cambridge, Cambridge,UK	Phys.Rev.B, 49(1994)1417	A.M.Campbell,A.Porch,D.N.Zheng,F.J.Blunt,J.D.Johnson,J.R.Cooper,P.A.Freeman	Y,Ba,Cu,Co,Zn,O	
10029	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K			86			0.5	86		1																																																																																												Bi2.4 : Sr2.0 : Ca1.0 : Cu2.0	5	see Physica C 213(1993)133ANN(in air,550C for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10030	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K			88			2.2	88		1																																																																																													5	see Physica C 213(1993)133ANN(in air,750C for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10031	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K			87				87		1																																																																																													5	see Physica C 213(1993)133ANN(in N2,at 550C for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10032	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K	87		92			5	89.5		1																																																																																													5	see Physica C 213(1993)133ANN(in N2,at 750 for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10033	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K	82		84.5			2.5	83.25		1																																																																																													5	see Physica C 213(1993)133ANN(in O2 at 550C for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10034	PR04901315		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1994																												Bi2212																		K	79		82			3	80.5		1																																																																																													5	see Physica C 213(1993)133ANN(in O2 at 750C for 20h)					Effect of annealing on the superconductivity of Bi2Sr2CaCu2Oz single crystals	1		Structure Research Labo,University of Science and Technology of China, Hefei,China	Phys.Rev.B, 49(1994)1315	Guien Zhou,Lei Shi,Liangbin Wang,Qiaonan Qin,Wenbin Wu,Xiao-Guang Li,Yitai Qian,Yuheng Zhang	Bi,Sr,Ca,Cu,O	
10035	PR05006929		Bi2Sr2(Ca)Cu2O8	Bi2.1Sr1.93Ca0.97Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.97	Cu	2													O	8+z			1994																											2	Bi2212			A	5.404		30.843												K		76.2					76.2																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10036	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.92Pr0.05Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.92	Pr	0.05	Cu	2											O	8+z			1994																											2	Bi2212			A	5.405		30.751												K		70.6					70.6																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10037	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.87Pr0.1Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.87	Pr	0.1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.41		30.726												K		70					70																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10038	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.77Pr0.2Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.77	Pr	0.2	Cu	2											O	8+z			1994																											2	Bi2212			A	5.42		30.677												K		57					57																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10039	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.72Pr0.25Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.72	Pr	0.25	Cu	2											O	8+z			1994																											2	Bi2212			A	5.426		30.65												K		47.4					47.4																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10040	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.67Pr0.3Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.67	Pr	0.3	Cu	2											O	8+z			1994																											2	Bi2212			A	5.432		30.646												K		30.3					30.3																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10041	PR05006929		Bi2Sr2(Ca,Pr)Cu2O8	Bi2.1Sr1.93Ca0.57Pr0.4Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.57	Pr	0.4	Cu	2											O	8+z			1994																											2	Bi2212			A	5.443		30.591												K		0.1					0.1																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10042	PR05006929		Bi2Sr2(Ca,Gd)Cu2O8	Bi2.1Sr1.93Ca0.92Gd0.05Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.92	Gd	0.05	Cu	2											O	8+z			1994																											2	Bi2212			A	5.4		30.707												K		78.6					78.6																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10043	PR05006929		Bi2Sr2(Ca,Gd)Cu2O8	Bi2.1Sr1.93Ca0.87Gd0.1Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.87	Gd	0.1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.417		30.744												K		63.3					63.3																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10044	PR05006929		Bi2Sr2(Ca,Gd)Cu2O8	Bi2.1Sr1.93Ca0.82Gd0.15Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.82	Gd	0.15	Cu	2											O	8+z			1994																											2	Bi2212			A	5.408		30.696												K		60.9					60.9																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10045	PR05006929		Bi2Sr2(Ca,Gd)Cu2O8	Bi2.1Sr1.93Ca0.77Gd0.2Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.77	Gd	0.2	Cu	2											O	8+z			1994																											2	Bi2212			A	5.418		30.62												K		49.6					49.6																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10046	PR05006929		Bi2Sr2(Ca,Gd)Cu2O8	Bi2.1Sr1.93Ca0.67Gd0.3Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.67	Gd	0.3	Cu	2											O	8+z			1994																											2	Bi2212			A	5.42		30.553												K		19.1					19.1																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10047	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.92Er0.05Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.92	Er	0.05	Cu	2											O	8+z			1994																											2	Bi2212			A	5.408		30.793												K		68.2					68.2																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10048	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.87Er0.1Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.87	Er	0.1	Cu	2											O	8+z			1994																											2	Bi2212			A	5.411		30.763												K		66.6					66.6																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10049	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.82Er0.15Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.82	Er	0.15	Cu	2											O	8+z			1994																											2	Bi2212			A	5.411		30.677												K		69.7					69.7																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10050	PR04904163	polycrystall	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4	4	4	1994																											3	T			A	5.357	5.401	13.155	4										at 295K.  There are lattice parameters at other temperature in this paper too.																																																																																																						La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10051	PR04904163	Polycrystall	(La,Sr)2CuO4	La1.925Sr0.075Cu1O4	La	1.925	Sr	0.075	Cu	1															O	4		4	1994																											3	T			A	5.351	5.366	13.208	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		18	22				18		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10052	PR04904163	polycrystall	(La,Sr)2CuO4	La1.913Sr0.087Cu1O4	La	1.913	Sr	0.087	Cu	1															O	4		4	1994																											3	T			A	5.349	5.359	13.208	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		25	28				25		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10053	PR04904163	Polycrystall	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		4	1994																											3	T			A	5.349	5.354	13.213	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		27	30				27		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10054	PR04904163	Polycrystall	(La,Sr)2CuO4	La1.888Sr0.112Cu1O4	La	1.888	Sr	0.112	Cu	1															O	4		4	1994																											2	T			A	5.347		13.22	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		27	29				27		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10055	PR04904163	polycrystall	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		4	1994																											2	T			A	5.347		13.226	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		27	31				27		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10056	PR04904163	polycrystall	(La,Sr)2CuO4	La1.862Sr0.138Cu1O4	La	1.862	Sr	0.138	Cu	1															O	4		4	1994																											2	T			A	5.345		13.228	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		33	39				33		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10057	PR04904163	polycrystall	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		4	1994																											2	T			A	5.342		14.232	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		36	40				36		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10058	PR04904163	polycrystall	(La,Sr)2CuO4	La1.837Sr0.162Cu1O4	La	1.837	Sr	0.162	Cu	1															O	4		4	1994																											2	T			A	5.34		13.236	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		36	39				36		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10059	PR04904163	polycrystall	(La,Sr)2CuO4	La1.825Sr0.175Cu1O4	La	1.825	Sr	0.175	Cu	1															O	4		4	1994																											2	T			A	5.338		13.242	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		35	38				35		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10060	PR04904163	polycrystall	(La,Sr)2CuO4	La1.812Sr0.188Cu1O4	La	1.812	Sr	0.188	Cu	1															O	4		4	1994																											2	T			A	5.337		13.246	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		33	36				33		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10061	PR04904163	polycrystall	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		4	1994																											2	T			A	5.335		13.247	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		28	32				28		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10062	PR04904163	polycrystall	(La,Sr)2CuO4	La1.788Sr0.213Cu1O4	La	1.788	Sr	0.213	Cu	1															O	4		4	1994																											2	T			A	5.333		13.242	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		23	26				23		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10063	PR04904163	polycrystall	(La,Sr)2CuO4	La1.775Sr0.225Cu1O4	La	1.775	Sr	0.225	Cu	1															O	4		4	1994																											2	T			A	5.332		13.254	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		20	25				20		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10064	PR04904163	polycrystall	(La,Sr)2CuO4	La1.763Sr0.237Cu1O4	La	1.763	Sr	0.237	Cu	1															O	4		4	1994																											2	T			A	5.33		14.257	4										at 295K.  There are lattice parameters at other temperature in this paper too.	K		13	17				13		2																																																																																												La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10065	PR04904163	polycrystall	(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		4	1994																											2	T			A	5.329		14.254	4										at 295K.  There are lattice parameters at other temperature in this paper too.																																																																																																						La2O3,SrCO3,CuO	1	CAL(700C for 24h under dynamic vacuum)introduce into a hot furnace in air.Q(room temperature)					Structural and superconducting properties of La2-xSrxCuO4 as a function of Sr content	2		Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)4163	A.W.Mitchell,B.A.Hunter,B.Dabrowski,D.G.Hinks,H.K.Viswanathan,J.D.Jorgensen,J.L.Wagner,K.G.Vandervoort,P.G.Radaelli	La,Sr,Cu,O	
10066	PR04903683	polycrystall	HgBa2CuO4	Hg1Ba2Cu1O4+d	Hg	1	Ba	2	Cu	1															O	4+d		1	1994																																														K			97				97		2																																												meV	14	3.6	1																																													HgO,Ba2CuO3		see Physica C 210,447 (1993) ANN(at 300C in Oxygen)					Point-contact tunneling study of HgBa2CuO4+z: BCS-like gap structure			Argonne National Lab,Argonne,Illinois,USA	Phys.Rev.B, 49(1994)3683	D.G.Hinks,J.F.Zasadzinski,J.L.Wagner,Jun Chen,K.E.Gray		
10067	PR04904189	polycrystall, figure=lattice part of thermal conductivity	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1994																												Y124																																																																																						W/K.M	7.6																																CuO,1:2:3 powder		by Hiping Methodsee J.Mater.Sci.Lett.9,770(1990)					Thermal conductivity of polycrystalline YBa2Cu4O8	2		Department of Experimental Physics,Umea University,Umea,Sweden	Phys.Rev.B, 49(1994)4189	Bengt Loberg,Bertil Sundqvist,Britt M.Andersson,John Niska	Y,Ba,Cu,O	
10068	PR04904182	Film	(Pr,Y)Ba2Cu3O7	Pr0.5Y0.5Ba2Cu3O7-d	Pr	0.5	Y	0.5	Ba	2	Cu	3													O	7-d		4	1994																												Y123																		K			22				22		1																																																																					m.ohm.cm											2.5													2	single-target pulsed-laser depositionsee Phys. Rev. Lett. 66,1537(1991)					Transport and structural properties of Pr1-xCaxBa2Cu3O7-z thin films grown by pulsed-laser deposition			Solid State Division,Oak Ridge National Lab,Oak Ridge,Tennessee,USA	Phys.Rev.B, 49(1994)4182	B.C.Chakoumakos,B.C.Sales,D.H.Lowndes,David P.Norton,E.C.Jones,J.D.Budai		
10069	PR04904182	Film	(Pr,Ca)Ba2Cu3O7	Pr0.7Ca0.3Ba2Cu3O7-x	Pr	0.7	Ca	0.3	Ba	2	Cu	3													O	7-x		4	1994																											3	Y123			A	3.847	3.908	11.736	3																																																																																																																			2		Pressed and fired PrCaBaCuO	see Mater.Res.Soc.Symp.Proc. 169(1990)431OxygenPressure 200mberCool(10C/min,O2 Pressure 400Torr) growth at 680C on (100) SrTiO3	Transport and structural properties of Pr1-xCaxBa2Cu3O7-z thin films grown by pulsed-laser deposition			Solid State Division,Oak Ridge National Lab,Oak Ridge,Tennessee,USA	Phys.Rev.B, 49(1994)4182	B.C.Chakoumakos,B.C.Sales,D.H.Lowndes,David P.Norton,E.C.Jones,J.D.Budai		
10070	PR04904182	Film	(Pr,Ca)Ba2Cu3O7	Pr0.6Ca0.4Ba2Cu3O7-d	Pr	0.6	Ca	0.4	Ba	2	Cu	3													O	7-d		4	1994																											3	Y123			A	3.84	3.904	11.739	3											K	10		25			15	17.5		1																																																																																															2		Pressed and fired PrCaBaCuO	see Mater.Res.Soc.Symp.Proc. 169(1990)431OxygenPressure 200mberCool(10C/min,O2 Pressure 400Torr) growth at 680C on (100) SrTiO3	Transport and structural properties of Pr1-xCaxBa2Cu3O7-z thin films grown by pulsed-laser deposition			Solid State Division,Oak Ridge National Lab,Oak Ridge,Tennessee,USA	Phys.Rev.B, 49(1994)4182	B.C.Chakoumakos,B.C.Sales,D.H.Lowndes,David P.Norton,E.C.Jones,J.D.Budai		
10071	PR04904182	film	(Pr,Ca)Ba2Cu3O7	Pr0.5Ca0.5Ba2Cu3O7-x	Pr	0.5	Ca	0.5	Ba	2	Cu	3													O	7-x		4	1994																											3	Y123			A	3.838	3.89	11.79	3											K	35		47			12	41		1																																																100000																					m.ohm.cm											1															2		Pressed and fired PrCaBaCuO	see Mater.Res.Soc.Symp.Proc. 169(1990)431OxygenPressure 200mberCool(10C/min,O2 Pressure 400Torr) growth at 680C on (100) SrTiO3	Transport and structural properties of Pr1-xCaxBa2Cu3O7-z thin films grown by pulsed-laser deposition			Solid State Division,Oak Ridge National Lab,Oak Ridge,Tennessee,USA	Phys.Rev.B, 49(1994)4182	B.C.Chakoumakos,B.C.Sales,D.H.Lowndes,David P.Norton,E.C.Jones,J.D.Budai		
10072	PR04904182	film	(Pr,Ca)Ba2Cu3O7	Pr0.4Ca0.6Ba2Cu3O7-x	Pr	0.4	Ca	0.6	Ba	2	Cu	3													O	7-x		4	1994																												Y123																																																																																																																										2		Pressed and fired PrCaBaCuO	see Mater.Res.Soc.Symp.Proc. 169(1990)431OxygenPressure 200mberCool(10C/min,O2 Pressure 400Torr) growth at 680C on (100) SrTiO3	Transport and structural properties of Pr1-xCaxBa2Cu3O7-z thin films grown by pulsed-laser deposition			Solid State Division,Oak Ridge National Lab,Oak Ridge,Tennessee,USA	Phys.Rev.B, 49(1994)4182	B.C.Chakoumakos,B.C.Sales,D.H.Lowndes,David P.Norton,E.C.Jones,J.D.Budai		
10073	PR04903502		(Ba,K)BiO3	Ba0.64K0.36Bi1O3	Ba	0.64	K	0.36	Bi	1															O	3		3	1994																											1				A	4.292			1										at Room Temperature.Relationship between potassium concentration and lattice parameter is given in P.R.B 41,4126(1990)	K	28.5						28.5		2																		T	direct measurement at 1.8K	25							T/K		0.55																																								mic.ohm.cm											200			m3/C	0.0000000006						/cm3				by Electrochemical CrystallizationThe detailed Procedure is reported in Solid State Commun. 78(1991)967					Upper critical field of Ba1-xKxBiO3 single crystals			Laboratoire d'Etudes des Proprietes Electroniques des Solides,Grenoble,France	Phys.Rev.B, 49(1994)3502	A. Sulpice,A.G.M. Jansen,A.G.M.Jansen,A.Sulpice,C. Escribe-Filippini,C.Escribe-Filippini,H. Rakoto,H.Rakoto,J. Marcus,J.C. Ousset,J.C.Ousset,J.M. Broto,J.M.Broto,J.Marcus,M. Affronte,M.Affronte,S. Askenazy,S.Askenazy		
10074	PR04903465	polycrystall	(Y,Ca)Ba2Fe3O8	Y0.95Ca0.05Ba2Fe3O8.08	Y	0.95	Ca	0.05	Ba	2	Fe	3													O	8+z	8.08	1	1994								638																			2		P4/mmm		A	3.917		11.809	3																																																																																																																Y2O3,BaCO3,CaCO3,high-purity Fe		prepared from liquid-mixed citrate precursors as descrived for YBa2Fe3O8 in J.Solid State Chem. 101,48 (1992)					Neutron-powder-diffraction study of the nuclear and magnetic structures of the substitution compound (Y1-xCax)Ba2Fe3O8+z(x=0.05,0.10,and 0.20)	2		Reactor Radiation Division,NIST,Gaithersburg,Maryland,USA	Phys.Rev.B, 49(1994)3465	A.D.Mighell,A.Kjekshus,A.Santoro,I.Natali Sora,J.W.Lynn,N.Rosov,P.Karen,Q.Huang,V.L.Karen	Y,Ca,Ba,Fe,O	
10075	PR04903465	polycrystall	(Y,Ca)Ba2Fe3O8	Y0.9Ca0.1Ba2Fe3O8.05	Y	0.9	Ca	0.1	Ba	2	Fe	3													O	8+z	8.05	1	1994								634																			2		P4/mmm		A	3.919		11.789	3																																																																																																																Y2O3,BaCO3,CaCO3,high-purity Fe		prepared from liquid-mixed citrate precursors as descrived for YBa2Fe3O8 in J.Solid State Chem. 101,48 (1992)					Neutron-powder-diffraction study of the nuclear and magnetic structures of the substitution compound (Y1-xCax)Ba2Fe3O8+z(x=0.05,0.10,and 0.20)	2		Reactor Radiation Division,NIST,Gaithersburg,Maryland,USA	Phys.Rev.B, 49(1994)3465	A.D.Mighell,A.Kjekshus,A.Santoro,I.Natali Sora,J.W.Lynn,N.Rosov,P.Karen,Q.Huang,V.L.Karen	Y,Ca,Ba,Fe,O	
10076	PR04903465	polycrystall	(Y,Ca)Ba2Fe3O8	Y0.8Ca0.2Ba2Fe3O8	Y	0.8	Ca	0.2	Ba	2	Fe	3													O	8+z	8	1	1994								624																			2		P4/mmm		A	3.911		11.766																																																																																																																	Y2O3,BaCO3,CaCO3,high-purity Fe		prepared from liquid-mixed citrate precursors as descrived for YBa2Fe3O8 in J.Solid State Chem. 101,48 (1992)					Neutron-powder-diffraction study of the nuclear and magnetic structures of the substitution compound (Y1-xCax)Ba2Fe3O8+z(x=0.05,0.10,and 0.20)	2		Reactor Radiation Division,NIST,Gaithersburg,Maryland,USA	Phys.Rev.B, 49(1994)3465	A.D.Mighell,A.Kjekshus,A.Santoro,I.Natali Sora,J.W.Lynn,N.Rosov,P.Karen,Q.Huang,V.L.Karen	Y,Ca,Ba,Fe,O	
10077	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.77Er0.2Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.77	Er	0.2	Cu	2											O	8+z			1994																											2	Bi2212			A	5.411		30.72												K		61.9					61.9																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10078	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.72Er0.25Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.72	Er	0.25	Cu	2											O	8+z			1994																											2	Bi2212			A	5.409		30.634												K		51.7					51.7																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10079	PR05006929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.67Er0.3Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.67	Er	0.3	Cu	2											O	8+z			1994																											2	Bi2212			A	5.409		30.585												K		36.4					36.4																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y   (R=Pr,Gd, and Er) systems	199409			Phys.Rev.B,50 (1994) 6929	G.V.Subba Rao,M.S. Ramachandra Rao,M.S.Ramachandra Rao,P. Sumana Prabhu,P.Sumana Prabhu,U.V. Varadaraju,U.V.Varadaraju	Bi,Sr,Ca,Cu,O,Pr,Gd.Er	
10080	PR0506929		Bi2Sr2(Ca,Er)Cu2O8	Bi2.1Sr1.93Ca0.57Er0.4Cu2O8+z	Bi	2.1	Sr	1.93	Ca	0.57	Er	0.4	Cu	2											O	8+z			1994																											2	Bi2212			A	5.425	5.409	30.542												K		0.1					0.1																																																																																																					Tc suppression and conduction mechanisms in Bi2.1Sr1.93Ca0.97-xRxCu2O8+y	199409		Materials Science Research Centre, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,50(1994)6929	M.S. Ramachandra Rao,P. Sumana Prabhu,U.V. Varadaraju		
10081	PR05013744		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-z			1994																												Y123																		K		42					42																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10082	PR05013744		YBa2(Cu,Fe,Zn)3O7	Y1Ba2Cu2.85Fe0.024Zn0.126O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.024	Zn	0.126											O	7-Z		1	1994																												Y123																		K		47.2					47.2																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10083	PR05013744		YBa2(Cu,Fe,Zn,)3O7	Y1Ba2Cu2.85Fe0.049Zn0.101O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.049	Zn	0.101											O	7-Z		1	1994																												Y123																		K		46.6					46.6																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10084	PR05013744		YBa2(Cu,Fe,Zn)3O7	Y1Ba2Cu2.85Fe0.075Zn0.075O7-z	Y	1	Ba	2	Cu	2.85	Fe	0.075	Zn	0.075											O	7-z		1	1994																												Y123																		K		50					50																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10085	PR05013744		YBa2(Cu,Fe,Zn)3O7	Y1Ba2Cu2.85Fe0.097Zn0.052O7-z	Y	1	Ba	2	Cu	2.85	Fe	0.097	Zn	0.052											O	7-z		1	1994																												Y123																		K		59					59																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10086	PR05013744		YBa2(Cu,Fe,Zn)3O7	Y1Ba2Cu2.85Fe0.126Zn0.024O7-Z	Y	1	Ba	2	Cu	2.85	Fe	0.126	Zn	0.024											O	7-Z		1	1994																												Y123																		K		67.9					67.9																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10087	PR05013744		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.85Fe0.15O7-z	Y	1	Ba	2	Cu	2.85	Fe	0.15													O	7-z		1	1994																												Y123																		K		73.1					73.1																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10088	PR05013744		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	7-z		1	1994																												Y123																		K		73.7					73.7																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10089	PR05013744		YBa2(Cu,Ga,Ni)3O7	Y1Ba2Cu2.85Ga0.025Ni0.124O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.025	Ni	0.124											O	7-z		1	1994																												Y123																		K		74.4					74.4																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10090	PR05013744		YBa2(Cu,Ga,Ni)3O7	Y1Ba2Cu2.85Ga0.049Ni0.101O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.049	Ni	0.101											O	7-z		1	1994																												Y123																		K		70.7					70.7																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10091	PR05013744		YBa2(Cu,Ga,Ni)3O7	Y1Ba2Cu2.85Ga0.075Ni0.075O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.075	Ni	0.075											O	7-z		1	1994																												Y123																		K		65					65																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10092	PR05013744		YBa2(Cu,Ga,Ni)307	Y1Ba2Cu2.85Ga0.097Ni0.052O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.097	Ni	0.052											O	7-z		1	1994																												Y123																		K		66.6					66.6																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10093	PR05013744		YBa2(Cu,Ga,Ni)3O7	Y1Ba2Cu2.85Ga0.126Ni0.024O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.126	Ni	0.024											O	7-z		1	1994																												Y123																		K		74.4					74.4																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10094	PR05013744		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-z		1	1994																												Y123																		K		76.4					76.4																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10095	PR05013744		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-z		1	1994																												Y123																		K		44.4					44.4																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10096	PR05013744		YBa2(Cu,Ga,Zn)3O7	Y1Ba2Cu2.85Ga0.025Zn0.124O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.025	Zn	0.124											O	7-z		1	1994																												Y123																		K		54.2					54.2																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10097	PR05013744		YBa2(Cu,Ga,Zn)307	Y1Ba2Cu2.85Ga0.049Zn0.101O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.049	Zn	0.101											O	7-z		1	1994																												Y123																		K		63					63																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10098	PR05013744		YBa2(Cu,Ga,Zn)3O7	Y1Ba2Cu2.85Ga0.075Zn0.075O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.075	Zn	0.075											O	7-z		1	1994																												Y123																		K		66.3					66.3																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10099	PR05013744		YBa2(Cu,Ga,Zn)3O7	Y1Ba2Cu2.85Ga0.101Zn0.049O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.101	Zn	0.049											O	7-z		1	1994																												Y123																		K		63.7					63.7																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10100	PR05013744		YBa2(Cu,Ga,Zn)3O7	Y1Ba2Cu2.85Ga0.126Zn0.024O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.126	Zn	0.024											O	7-z		1	1994																												Y123																		K		66.3					66.3																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10101	PR05013744		YBa2(Cu,Ga)3O7	Y1Ba2Cu2.85Ga0.15O7-z	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-z		1	1994																												Y123																		K		75.7					75.7																																																																																												/unit cell			1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10102	PR05013744		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-z	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-z		1	1994																												Y123																		K		41.6					41.6																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10103	PR05013744		YBa2(Cu,Ni,Zn)3O7	Y1Ba2Cu2.85Ni0.025Zn0.124O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.025	Zn	0.124											O	7-z		1	1994																												Y123																		K		47.9					47.9																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10104	PR05013744		YBa2(Cu,Ni,Zn)3O7	Y1Ba2Cu2.85Ni0.051Zn0.099O7-z	Y	1	Ba	2	Cu	2.85	Ni	0.051	Zn	0.099											O	7-z		1	1994																												Y123																		K		52.5					52.5																																																																																															1	(Ni,Zn),(Ga,Zn),(Ga,Ni),(Fe,Zn) as a dopant pairs, details are described in Physica C 208(1993)59, Oxygen content by TGA					Dopant interactions in superconducting YBa2Cu3O7	199411			Phys.rev.B.,50(1994) 13744	M.A.Castro,M.McElfresh,S.M.Durbin	Y,Ba,Cu,O	
10105	PR04909885	dTc/dP is for c-axis measurement, dTc/dP=-3.5 K/GPa for ab-plane measurement, dRH/dP=-0.39 E-9 m3/C.GPa	IBi2Sr2CaCu2O8	I1Bi2.2Sr1.8Ca1Cu2O8+y	I	1	Bi	2.2	Sr	1.8	Ca	1	Cu	2											O	8+y		3	1994																												Bi2212			A	5.13	5.13	37.1	3											K		73.6					73.6		1	K/GPa	-3.6																																																																																	cm3/C	0.00205						/formula u		Bi2O3, Sr(NO3), CaCO3, CuO, I	7	Bi:Sr:Ca:Cu=2.2:1.8:1:2 for the feed rod, and 2.4:1.5:1:1.8 for the solvent rod. Single Crystals of Bi-2.2:1.8:1:2 and elemental iodine were encapsulated in a pyrex tube under a vacuum of 10e-3 torr.I					Pressure dependence of the superconducting transition temperature and the Hall coefficient in IBi2.2Sr1.8CaCu2O8+z single crystals	4			Phys.Rev.B, 49(1994)9885	Jianding Yu,Mitsuru Itoh,Tetsuro Nakamura,Tongkai Huang,Yoshiyuki Inaguma	I,Bi,Sr,Ca,Cu,O	
10106	PR04909857		Bi2(Sr,Ba)2CuO6	Bi2Sr1.9Ba0.1Cu1Oy	Bi	2	Sr	1.9	Ba	0.1	Cu	1													O	y		1	1994																												Bi2201																																																																																											micro.V/K	-12																													See Physical Review B 47 (1993) 14467.					Relation of the incommensurate modulation structure and normal-state properties of the Ba-doped Bi2Sr2CuO6+z system	4			Phys.Rev.B, 49(1994)9857	Ji Mingrong,Mao Zhiqiang,Tian Mingliang,Wang Ruiping,Wang Yu,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Ba,Bi,Sr,Cu,O	
10107	PR04909857		Bi2(Sr,Ba)2CuO6	Bi2Sr1.8Ba0.2Cu1Oy	Bi	2	Sr	1.8	Ba	0.2	Cu	1													O	y		1	1994																												Bi2201																																																																																											micro.V/K	-4			TP10107																										See Physical Review B 47 (1993) 14467.					Relation of the incommensurate modulation structure and normal-state properties of the Ba-doped Bi2Sr2CuO6+z system	4			Phys.Rev.B, 49(1994)9857	Ji Mingrong,Mao Zhiqiang,Tian Mingliang,Wang Ruiping,Wang Yu,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Ba,Bi,Sr,Cu,O	
10108	PR04909857		Bi2(Sr,Ba)2CuO6	Bi2Sr1.6Ba0.4Cu1Oy	Bi	2	Sr	1.6	Ba	0.4	Cu	1													O	y		1	1994																												Bi2201																																																																																											micro.V/K	10			TP10108																										See Physical Review B 47 (1993) 14467.					Relation of the incommensurate modulation structure and normal-state properties of the Ba-doped Bi2Sr2CuO6+z system	4			Phys.Rev.B, 49(1994)9857	Ji Mingrong,Mao Zhiqiang,Tian Mingliang,Wang Ruiping,Wang Yu,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Ba,Bi,Sr,Cu,O	
10109	PR04909218		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1994																												Bi2212																		K		90.7		90.7			90.7		2								87										kOe		860							kOe/K	Estimated from fitting the experimental data to a full Lawrence-Doniach model calculation of the flu	-14					A	Estimated from fitting the experimental data to a full Lawrence-Doniach model calculation of the flu		21.4	0.4																																																													Temperature dependence of the magnetization of a Bi2Sr2CaCu2O8+z single crystal close to Tc	4			Phys.Rev.B, 49(1994)9218	A.Schilling,H.R.Ott,R.Jin	Bi,Sr,Ca,Cu,O	
10110	PR04909073		Bi2Sr2YCu2O8	Bi2Sr2Y1Cu2O8	Bi	2	Sr	2	Y	1	Cu	2													O	8		3	1994																																														K					4.2																																																															W/K.M	4			THC10110						mic.ohm.cm		100000000000			300000000							2000000													See Phys. Rev. B 45 (1992) 13025, J. of Appl. Phys. 68 (1990) 4876.					Thermal conductivity of insulating Bi2Sr2YCu2O8 and superconducting Bi2Sr2CaCu2O8: Failure of the phonon-gas picture	4		Department of Physics, State University of New York at Stony Brook, Stony Brook, New York 11794-3800	Phys.Rev.B,49(1994)9073	Laszlo Mihaly,Philip B. Allen,Xiaoqun Du		
10111	PR04909073		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1994																																														K		95	100				95		1																																																											W/K.M	5.8									mic.ohm.cm												300													See Phys. Rev. B 45 (1992) 13025, J. of Appl. Phys. 68 (1990) 4876.					Thermal conductivity of insulating Bi2Sr2YCu2O8 and superconducting Bi2Sr2CaCu2O8: Failure of the phonon-gas picture	4		Department of Physics, State University of New York at Stony Brook, Stony Brook, New York 11794-3800	Phys.Rev.B,49(1994)9073	Laszlo Mihaly,Philip B. Allen,Xiaoqun Du		
10112	PR04909084	dTc/dp=0.5 K/GPa for p>1GPa	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1994																											2	T																		K		36		33.6			36			K/GPa	1																																																																		TP10112																								Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10113	PR04909084	dTc/dp=0.5 K/GPa for p>1GPa	(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4		1	1994																											2	T																		K		34.6		33.2			34.6			K/GPa	0.95																																																																																										Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10114	PR04909084	dTc/dp=0.8 K/GPa for p>1GPa	(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4		1	1994																											2	T																		K		32.1		30.8			32.1			K/GPa	0.3																																																																		TP10114																								Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10115	PR04909084	dTc/dp=1.1K/GPa for p>1GPa	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1994																											2	T																		K		30.5		28			30.5			K/GPa	0.001																																																																																										Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10116	PR04909084	dTc/dp=0.4 K/GPa for p>1GPa	(La,Sr)2CuO4	La1.79Sr0.21Cu1O4	La	1.79	Sr	0.21	Cu	1															O	4		1	1994																											2	T																												K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10117	PR04909084	dTc/dp=0.5K/GPa for p>1GPa	(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		1	1994																											2	T																												K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10118	PR04909084	dTc/dp=0 for p>1GPa	(La,Sr)2CuO4	La1.77Sr0.23Cu1O4	La	1.77	Sr	0.23	Cu	1															O	4		1	1994																											3	T																		K		21.3		18			21.3			K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10119	PR04909084	dTc/dp=0 for p>1GPa	(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		1	1994																											3	T																		K		20		16			20			K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10120	PR04909084	dTc/dp=0 for p>1GPa	(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		1	1994																											3	T																												K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10121	PR04909084	dTc/dp is for p<1GPa	(La,Sr)2CuO4	La1.74Sr0.26Cu1O4	La	1.74	Sr	0.26	Cu	1															O	4		1	1994																											3	T																		K		9		7			9			K/GPa	0.1																																																																																										Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10122	PR04909084	dTc/dp is for p<1GPa	(La,Sr)2CuO4	La1.73Sr0.27Cu1O4	La	1.73	Sr	0.27	Cu	1															O	4		1	1994																											3	T																		K		12		7			12			K/GPa																																																																																											Oxides	1	SIN(at 1030-1100C for 1week with Intermittent Grinding.)SIN(at 1050C)ANN(900C for 1month) FC					Superconductor-to-metal transition in overdoped La2-xSrxCuO4	4			Phys.Rev.B, 49(1994)9084	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Sr,Cu,O	
10123	PR04909898	GL parameter=130	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1994																											3	Bi2212	Amma		A	5.375	5.395	30.65	3											K	82.5			84			84																													T/K		2.17					A			16.9		A		2200																												m.ohm.cm												0.5											Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10124	PR04909898	GL parameter=120	Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.994Fe0.006O8+d	Bi	2	Sr	2	Ca	1	Cu	1.994	Fe	0.006											O	8+d		3	1994																											3	Bi2212	Amma		A	5.375	5.39	30.64	3											K	82.5			81.5			81.5																													T/K		1.25					A			22		A		2640																												m.ohm.cm												0.71											Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10125	PR04909898		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.982Fe0.018O8+d	Bi	2	Sr	2	Ca	1	Cu	1.982	Fe	0.018											O	8+d		3	1994																											3	Bi2212																		K				71.5			71.5																																									A		2670																																																			Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10126	PR04909898		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.977Fe0.023O8+d	Bi	2	Sr	2	Ca	1	Cu	1.977	Fe	0.023											O	8+d		3	1994																											3	Bi2212																		K	66						66																																																																							m.ohm.cm												3.46											Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10127	PR04909898		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.954Fe0.046O8+d	Bi	2	Sr	2	Ca	1	Cu	1.954	Fe	0.046											O	8+d		3	1994																											3	Bi2212	Amma		A	5.4	5.425	30.68	3											K				69.5			69.5																																									A		3460																																																			Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10128	PR04909898		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.91Fe0.09O8+d	Bi	2	Sr	2	Ca	1	Cu	1.91	Fe	0.09											O	8+d		3	1994																											3	Bi2212																		K				69.5			69.5																																																																																														Bi2O3,SrCO3,CaCo3,CuO,Fe2O3	10	CAL(800C in air)SINANN (800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10129	PR04909898	GL parameter=218	Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.991Ni0.009O8+d	Bi	2	Sr	2	Ca	1	Cu	1.991	Ni	0.009											O	8+d		3	1994																											3	Bi2212	Amma		A	5.375	5.425	30.58	3											K	82.5			79.5			79.5																													T/K		3.57					A			12.1		A		2640																												m.ohm.cm												0.78											Bi2O3,SrCO3,CaCO3,CuO,NiO	10	CAL(800C in air)SINANN(800C in an atomosphere of 8% O2 and 92% Ar					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10130	PR04909898	GL parameter=219	Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.983Ni0.017O8+d	Bi	2	Sr	2	Ca	1	Cu	1.983	Ni	0.017											O	8+d		3	1994																											3	Bi2212	Amma		A	5.375	5.42	30.59	3											K	79			75.5			75.5																													T/K							A			11.8		A		2590																												m.ohm.cm												0.71											Bi2O3,SrCO3,CaCO3,CuO,NiO	10	CAL(800C in air)SINANN(800C in an atomosphere of 8% O2 and 92% Ar					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10131	PR04909898		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.982Ni0.018O8+d	Bi	2	Sr	2	Ca	1	Cu	1.982	Ni	0.018											O	8+d		3	1994																											3	Bi2212	Amma		A	5.365	5.445	30.555	3											K	72.5			74			74																																																																																														Bi2O3,SrCO3,CaCO3,CuO,NiO	10	CAL(800C in air)SINANN(800C in an atomosphere of 8% O2 and 92% Ar					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10132	PR04909898	GL parameter=211	Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.998Zn0.002O8+d	Bi	2	Sr	2	Ca	1	Cu	1.998	Zn	0.002											O	8+d		3	1994																											3	Bi2212	Amma		A	5.37	5.405	30.635	3											K	80.5			83			83																													T/K		4.54					A			12.9		A		2720																												m.ohm.cm												0.62											Bi2O3,SrCO3,CaCO3,CuO,ZnO	10	CAL(800C in aie)SINANN(800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10133	PR04909898		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.996Zn0.004O8+d	Bi	2	Sr	2	Ca	1	Cu	1.996	Zn	0.004											O	8+d		3	1994																											3	Bi2212	Amma		A	5.38	5.395	30.8	3											K				82.5			82.5																																																																																														Bi2O3,SrCO3,CaCO3,CuO,ZnO	10	CAL(800C in aie)SINANN(800C in an atmosphere of 8% O2 and 92% Ar)					Superconductivity in Bi2Sr2CaCu2O8+z single crystals doped with Fe,Ni, and Zn	4			Phys.Rev.B, 49(1994)9898	B.vom Hedt,H.Bach,K.Westerholt,W.Lisseck	Bi,Sr,Ca,Cu,O,Fe,Ni,Zn	
10134	PR04909150		DyBa2Cu4O8	Dy1Ba2Cu4O8	Dy	1	Ba	2	Cu	4															O	8		3	1994																																														K		73.6		73.6			73.6		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10135	PR04909150		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1994																																														K		80		80			80		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10136	PR04909150		GdBa2Cu4O8	Gd1Ba2Cu4O8	Gd	1	Ba	2	Cu	4															O	8		3	1994																																														K		74.7		74.7			74.7		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10137	PR04909150		HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		3	1994																																														K		79		79			79		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10138	PR04909150		ErBa2Cu4O8	Er1Ba2Cu4O8	Er	1	Ba	2	Cu	4															O	8		3	1994																																														K		80		80			80		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10139	PR04909150		TmBa2Cu4O8	Tm1Ba2Cu4O8	Tm	1	Ba	2	Cu	4															O	8		3	1994																																														K		79.9		79.9			79.9		3																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10140	PR04909150		YbBa2Cu4O8	Yb1Ba2Cu4O8	Yb	1	Ba	2	Cu	4															O	8		3	1994																																														K		78.8		78.8			78.8		2																																																																																														See Physica C 193 (1992) 64.					Magnetic anisotropy in single-crystal rare-earth-doped RBa2Cu4O8 (R=Y,Dy,Gd,Ho,Er,Tm,Yb)	4			Phys.Rev.B, 49(1994)9150	B.Dabrowski,D.H.Nichols,J.E.Crow,U.Welp	Ba,Cu,O,Y,Dy,Gd,Ho,Er,Tm,Yb	
10141	PR04909097		(La,Sr)2CuO4	La1.925Sr0.075Cu1O4+d	La	1.925	Sr	0.075	Cu	1															O	4+d		3	1994																																														K	23						23		1																																																																					m.ohm.cm					1.6							2.7																		Magnetoresistance in the normal state of La1.925Sr0.075CuO4+delta	4		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B,49(1994)9097	A. Lacerda,J.D. Thompson,J.P. Rodriguez,M.F. Hundley,P.C. Canfield,S.W. Cheong,Z. Fisk		
10142	PR04909248		(La,Sr,Pr)2CuO4	La1.07Pr0.85Sr0.08Cu1O4	La	1.07	Pr	0.85	Sr	0.08	Cu	1													O	4			1994																																														K		9		9			9																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10143	PR04909248		(La,Sr,Pr)2CuO4	La1.04Pr0.85Sr0.11Cu1O4	La	1.04	Pr	0.85	Sr	0.11	Cu	1													O	4			1994																																														K		17		17			17																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10144	PR04909248		(La,Sr,Pr)2CuO4	La1.03Pr0.85Sr0.12Cu1O4	La	1.03	Pr	0.85	Sr	0.12	Cu	1													O	4			1994																																														K		18		18			18																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10145	PR04909248		(La,Sr,Pr)2CuO4	La1.02Pr0.85Sr0.13Cu1O4	La	1.02	Pr	0.85	Sr	0.13	Cu	1													O	4			1994																																														K		22		22			22																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10146	PR04909248		(La,Sr,Pr)2CuO4	La1.01Pr0.85Sr0.14Cu1O4	La	1.01	Pr	0.85	Sr	0.14	Cu	1													O	4			1994																																														K		25		25			25																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10147	PR04909248		(La,Sr,Pr)2CuO4	La1Pr0.85Sr0.15Cu1O4	La	1	Pr	0.85	Sr	0.15	Cu	1													O	4			1994																																														K		28		28			28																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10148	PR04909248		(La,Sr,Pr)2CuO4	La0.97Pr0.85Sr0.18Cu1O4	La	0.97	Pr	0.85	Sr	0.18	Cu	1													O	4			1994																																														K		28		28			28																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10149	PR04909248		(La,Sr,Pr)2CuO4	La0.95Pr0.85Sr0.2Cu1O4	La	0.95	Pr	0.85	Sr	0.2	Cu	1													O	4			1994																																														K		27		27			27																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10150	PR04909248		(La,Sr,Pr)2CuO4	La0.92Pr0.85Sr0.23Cu1O4	La	0.92	Pr	0.85	Sr	0.23	Cu	1													O	4			1994																																														K		17		17			17																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10151	PR04909248		(La,Sr,Pr)2CuO4	La0.9Pr0.85Sr0.25Cu1O4	La	0.9	Pr	0.85	Sr	0.25	Cu	1													O	4			1994																																														K		10		10			10																																																																																																See Physica C 208 (1993) 217.					Disappearance of superconductivity in overdoped La1.15-xPr0.85SrxCuO4 and the orthorhombic-tetragonal phase boundary	4			Phys.Rev.B, 49(1994)9248	A.Freimuth,B.Buchner,B.Roden,G.Bauer,M.Breuer,N.Knauf,W.Schafer,W.Schlabitz	La,Pr,Sr,Cu,O	
10152	PR04909924		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																												Y123																		K		90				0.5	90		1																																		A	Microwave Self-Resonant Technique and Electron Paramagnetic Resonance Technique.		25	8	A	Microwave Self-Resonant Technique.		1800																											mic.ohm.cm											300															2		Stoichiometric YBCO (99.999% pure).	Target is (100)-oriented MgO.The thickness is about 500A.	Measurements of surface impedance, London penetration depth, and coherence length in Y-Ba-Cu-O films at microwave frequencies	4		Northeastern University, Boston, Massachusetts 02115	Phys.Rev.B,49(1994)9924	A. Widom,C. Vittoria,H. How,H. Jiang,T. Yuan		
10153	PR04910043		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																												Y123																		K			92.3				92.3																																				A			9	1														mJ/cm3.K	45																																									Y:Ba:Cu+Zn = 1:4:9-11. Well-decarbonated ceramic powder is heated to 1050C, then FC(3C/h, in air) below 900C, ANN(in flowing O2, at 500C, for100h) and FC (3C/h) to room temperature.					Normal and superconductive properties of Zn-substituted single-crystal YBa2(Cu1-xZnx)3O7-z	199404			Phys.Rev.B, 49(1994)10043	Azusa Matsuda,Kouichi Semba,Takao Ishii	Y,Ba,Cu,Zn,O	
10154	PR04910043		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.979Zn0.021O7-d	Y	1	Ba	2	Cu	2.979	Zn	0.021													O	7-d		3	1994																												Y123																		K			84				84																																				A			10	1.2														mJ/cm3.K	41																																									Y:Ba:Cu+Zn = 1:4:9-11. Well-decarbonated ceramic powder is heated to 1050C, then FC(3C/h, in air) below 900C, ANN(in flowing O2, at 500C, for100h) and FC (3C/h) to room temperature.					Normal and superconductive properties of Zn-substituted single-crystal YBa2(Cu1-xZnx)3O7-z	199404			Phys.Rev.B, 49(1994)10043	Azusa Matsuda,Kouichi Semba,Takao Ishii	Y,Ba,Cu,Zn,O	
10155	PR04910043		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.954Zn0.047O7-d	Y	1	Ba	2	Cu	2.954	Zn	0.047													O	7-d		3	1994																												Y123																		K			73.8				73.8																																				A			13	1.8														mJ/cm3.K	36																																									Y:Ba:Cu+Zn = 1:4:9-11. Well-decarbonated ceramic powder is heated to 1050C, then FC(3C/h, in air) below 900C, ANN(in flowing O2, at 500C, for100h) and FC (3C/h) to room temperature.					Normal and superconductive properties of Zn-substituted single-crystal YBa2(Cu1-xZnx)3O7-z	199404			Phys.Rev.B, 49(1994)10043	Azusa Matsuda,Kouichi Semba,Takao Ishii	Y,Ba,Cu,Zn,O	
10156	PR04910043		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7-d	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-d		3	1994																												Y123																		K			57.5				57.5																																				A			14.5	2.2														mJ/cm3.K	20.5																																									Y:Ba:Cu+Zn = 1:4:9-11. Well-decarbonated ceramic powder is heated to 1050C, then FC(3C/h, in air) below 900C, ANN(in flowing O2, at 500C, for100h) and FC (3C/h) to room temperature.					Normal and superconductive properties of Zn-substituted single-crystal YBa2(Cu1-xZnx)3O7-z	199404			Phys.Rev.B, 49(1994)10043	Azusa Matsuda,Kouichi Semba,Takao Ishii	Y,Ba,Cu,Zn,O	
10157	PR04909168		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1994									5.4																			Y123																		K	90.83		91.83			1	91.33		2								85																																																													m.ohm.cm											1.2														See PRB 48 (1992) 3423.					ac susceptibility near the superconducting transition in polycrystalline YBa2Cu3O7-delta	4		Laboratory for Low Temperature Physics, Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts 01003	Phys.Rev.B,49(1994)9168	R.B. Hallock,W.M. Tiernan		
10158	PR04909168		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1994									5.1																			Y123																		K	90.5		91.65			1	91.075		2								85																																																													m.ohm.cm											1														See PRB 48 (1992) 3423.					ac susceptibility near the superconducting transition in polycrystalline YBa2Cu3O7-delta	4		Laboratory for Low Temperature Physics, Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts 01003	Phys.Rev.B,49(1994)9168	R.B. Hallock,W.M. Tiernan		
10159	PR04909168		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1994									5.4																			Y123																		K			92.42			1	92.42		2								85																																																													m.ohm.cm											1.2														See PRB 48 (1992) 3423.					ac susceptibility near the superconducting transition in polycrystalline YBa2Cu3O7-delta	4		Laboratory for Low Temperature Physics, Department of Physics and Astronomy, University of Massachusetts, Amherst, Massachusetts 01003	Phys.Rev.B,49(1994)9168	R.B. Hallock,W.M. Tiernan		
10160	PR04912206		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1994																												Y123																		K	92.12					1	92.12																																																																							mic.ohm.m											14.33												Y2O3,BaCO3,CuO	1	SIN(930C,24h) - ANN(O2,900C to 600C at 1C/h, Dwell 12h, to 300C at 0.5C/h, to R.T.)					Excess conductivity and pair-breaking effects in YBa2Cu3O7 and Bi2Sr2Ca1-xYxCu2O8+z systems	199405			Phys.Rev.B, 49(1994)12206	C.P.Dhard,S.N.Bhatia	Y,Ba,Cu,O,Bi,Sr,Ca	
10161	PR04912206		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1994																												Y123																		K	86.4					1	86.4																																																																							mic.ohm.m											1.11															17			by Laser Ablation Method. Substrate is SrTiO3.	Excess conductivity and pair-breaking effects in YBa2Cu3O7 and Bi2Sr2Ca1-xYxCu2O8+z systems	199405			Phys.Rev.B, 49(1994)12206	C.P.Dhard,S.N.Bhatia	Y,Ba,Cu,O,Bi,Sr,Ca	
10162	PR04912206		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1994																												Bi2212																		K	85.7					4	85.7																																																																							mic.ohm.m											60.16												Bi2O3, Sr2CaCu2O8 precursor	1	matrix precursor method. Reacting Bi2O3 to Sr2CaCu2O8 in the Presence of O2 at 900~950C					Excess conductivity and pair-breaking effects in YBa2Cu3O7 and Bi2Sr2Ca1-xYxCu2O8+z systems	199405			Phys.Rev.B, 49(1994)12206	C.P.Dhard,S.N.Bhatia	Y,Ba,Cu,O,Bi,Sr,Ca	
10163	PR04912206		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1994																												Bi2212																		K	63.58					6	63.58																																																																							mic.ohm.m											22.2												Bi2O3, Sr2CaCu2O8 precursor	1	matrix precursor method. Reacting Bi2O3 to Sr2CaCu2O8 in the Presence of O2 at 900~950C					Excess conductivity and pair-breaking effects in YBa2Cu3O7 and Bi2Sr2Ca1-xYxCu2O8+z systems	199405			Phys.Rev.B, 49(1994)12206	C.P.Dhard,S.N.Bhatia	Y,Ba,Cu,O,Bi,Sr,Ca	
10164	PR04912206		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1994																												Bi2212																		K	50.33					9	50.33																																																																							mic.ohm.m											36.17												Bi2O3, Sr2CaCu2O8 precursor	1	matrix precursor method. Reacting Bi2O3 to Sr2CaCu2O8 in the Presence of O2 at 900~950C					Excess conductivity and pair-breaking effects in YBa2Cu3O7 and Bi2Sr2Ca1-xYxCu2O8+z systems	199405			Phys.Rev.B, 49(1994)12206	C.P.Dhard,S.N.Bhatia	Y,Ba,Cu,O,Bi,Sr,Ca	
10165	PR04912322		(Hg,Pb)Ba2Ca2Cu3O9	Hg0.66Pb0.33Ba2Ca2Cu3Oy	Hg	0.66	Pb	0.33	Ba	2	Ca	2	Cu	3											O	y		1	1994																											2	Hg1223			A	3.849		15.86	3											K	130		138	132		8	132										50																																																																																					1	Percursor SIN(oxygen,900C,16h) - MIX(Prec.:HgO:PbO2=1:0.8:0.2) - Wrapped( in Gold foil) - loaded(in a quartz-tube at 1e-1 torr O2) -  SIN(to 800C for 2~5h,hold at 800C for 2h,to 30C for 6H)					Superconductivity above 130K in the Hg-Pb-Ba-Ca-Cu-O system	199405			Phys.Rev.B, 49(1994)12322	A.G.Rinzler,A.Lungu,D.Kirven,D.Yang,F.J.Owens,F.Reidinger,J.C.Barry,T.Datta,Z.Iqbal	Hg,Ba,Pb,Ca,Cu,O	
10166	PR04913075		HgBa2CuO4	Hg1Ba2Cu1O4+d	Hg	1	Ba	2	Cu	1															O	4+d		1	1994																		GPa		104								Hg1201			A	3.874		9.503	3										Lattice const. was measured by Energy-Dispersive X-Ray DIffraction.	K	90		94			4	92			K/GPa	1.4						20																																																																																						In detail,see Nature 364 ,(1993) 129					Volume dependence of the superconducting transition temperature for the high-temperature superconductor HgBa2CuO4+z	199405			Phys.Rev.B, 49(1994)13075	Charles C.Kim,D.H.Liebenberg,E.F.Skelton,M.E.Reeves,M.S.Osofsky,S.B.Qadri,V.M.Browning	Hg,Ba,Cu,O	
10167	PR04913119		Bi2Sr2CuO6	Bi2.1Sr1.9Cu1Oy	Bi	2.1	Sr	1.9	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10168	PR04913119		Bi2Sr2CuO6	Bi2.15Sr1.85Cu1Oy	Bi	2.15	Sr	1.85	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10169	PR04913119		Bi2Sr2CuO6	Bi2.2Sr1.8Cu1Oy	Bi	2.2	Sr	1.8	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10170	PR04913119		Bi2Sr2CuO6	Bi2.25Sr1.75Cu1Oy	Bi	2.25	Sr	1.75	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10172	PR04913119		Bi2Sr2CuO6	Bi2.3Sr1.7Cu1Oy	Bi	2.3	Sr	1.7	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10173	PR04913119		Bi2Sr2CuO6	Bi2.35Sr1.65Cu1Oy	Bi	2.35	Sr	1.65	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10174	PR04913119		Bi2Sr2CuO6	Bi2.4Sr1.6Cu1Oy	Bi	2.4	Sr	1.6	Cu	1															O	y		1	1994																												Bi2201			A																																																																																																																				Bi2O3,SrCO3,CuO powder	1	SIN(800C,12h -> 820C,12h,in air) - SIN(850~870C,15h,in air)					Bi2+xSr2-xCuOy(0.10%$x%$0.40) studied by photoemission and inverse-photoemission spectroscopy	199405		Research Institute of Electronics, Shizuoka University, Hamamatsu 432, Japan	Phys.Rev.B,49(1994)13119	M. Nagoshi,M. Ogita,M. Shimomura,M. Tachiki,N. Sanada,Y. Fukuda,Y. Suzuki,Y. Syono		
10175	PR04913123		Tl(Ba,Sr)LaCuO5	Tl1Ba0.6Sr0.4La1Cu1O5	Tl	1	Ba	0.6	Sr	0.4	La	1	Cu	1											O		5	1	1994																											2	Tl1201	P4/mmm		A	3.821		8.901	3											K				20			20																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10176	PR04913123		Tl(Ba,Sr)LaCuO5	Tl1Ba0.3Sr0.7La1Cu1O5	Tl	1	Ba	0.3	Sr	0.7	La	1	Cu	1											O		5	1	1994																											2	Tl1201	P4/mmm		A	3.794		8.885	3											K				30			30																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10177	PR04913123		Tl(Sr,Ca)LaCuO5	Tl1Sr1La1Cu1O5	Tl	1	Sr	1	La	1	Cu	1													O		5	1	1994																											2	Tl1201	P4/mmm		A	3.779		8.864	3											K				32			32																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10178	PR04913123		Tl(Sr,Ca)LaCuO5	Tl1Sr0.7Ca0.3La1Cu1O5	Tl	1	Sr	0.7	Ca	0.3	La	1	Cu	1											O		5	1	1994																											2	Tl1201	P4/mmm		A	3.761		8.807	3											K				32			32																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10179	PR04913123		Tl(Sr,Ca)LaCuO5	Tl1Sr0.4Ca0.6La1Cu1O5	Tl	1	Sr	0.4	Ca	0.6	La	1	Cu	1											O		5	1	1994																											2	Tl1201	P4/mmm		A	3.753		8.737	3											K				26			26																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10180	PR04913123		Tl(Ba,Ca)LaCuO5	Tl1Ba0.8Ca0.2La1Cu1O5	Tl	1	Ba	0.8	Ca	0.2	La	1	Cu	1											O	5		1	1994																											2	Tl1201	P4/mmm		A	3.827		8.948	3											K																																																																																																							See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10181	PR04913123		Tl(Ba,Sr)LaCuO5	Tl1Ba1La1Cu1O5	Tl	1	Ba	1	La	1	Cu	1													O		5	1	1994																											2	Tl1201	P4/mmm		A	3.852		8.993	3											K																																																																																																							See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10182	PR04913123		Tl(Ba,Ca)LaCuO5	Tl1Ba0.6Ca0.4La1Cu1O5	Tl	1	Ba	0.6	Ca	0.4	La	1	Cu	1											O	5		1	1994																											2	Tl1201	P4/mmm		A	3.817		8.885	3											K				14			14																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10183	PR04913123		Tl(Ba,Ca)LaCuO5	Tl1Ba0.4Ca0.6La1Cu1O5	Tl	1	Ba	0.4	Ca	0.6	La	1	Cu	1											O	5		1	1994																											2	Tl1201	P4/mmm		A	3.79		8.815	3											K				16			16																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10184	PR04913123		Tl(Ba,Ca)LaCuO5	Tl1Ba0.2Ca0.8La1Cu1O5	Tl	1	Ba	0.2	Ca	0.8	La	1	Cu	1											O	5		1	1994																											2	Tl1201	P4/mmm		A	3.766		8.75	3											K				13			13																																																																																																See Phys.Rev.B 46 (1992) 6622					Possible overdoping in TlSrLaCuO5 and superconductivity in TlBaLaCuO5 by isovalent-cation substitution	199405			Phys.Rev.B, 49(1994)13123	A.S.Tamhane,A.Sundaresan,L.C.Gupta,M.Sharon,R.Nagarajan,R.Pinto,R.Vijayaraghavan	Tl,Sr,Ba,La,Cu,O	
10185	PR04913137	DTCDP is the value of c-axis stress dependence of Tc.For a-axis DTCDP=7.0 K/GPa . for b-axis DTCDP=5.9 K/GPa. DTCDP estimated from thermal expansion coefficient	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1994																												T																		K				28.5			28.5			K/GPa	-13.8																																																																																											7	by TSFZ method. In detail,See Phys.Rev.B 47 (1993) 8369					Uniaxial pressure dependence of Tc from high-resolution dilatometry of untwinned La2-xSrxCuO4 single crystals	199405			Phys.Rev.B, 49(1994)13137	Christoph Meingast,Frank Gugenberger,Georg Roth,Helmut Wuhl,Kai Grube,S.Uchida,Thomas Weber,Volker Breit,Y.Nakamura	La,Sr,Cu,O	
10186	PR04913137	DTCDP is the value of c-axis stress dependence of Tc.For a-axis DTCDP=2.5 K/GPa . for b-axis DTCDP=4.9 K/GPa. DTCDP estimated from thermal expansion coefficient.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1994																												T																		K				36			36			K/GPa	-6.8																																																																																											7	by TSFZ method. In detail,See Phys.Rev.B 47 (1993) 8369					Uniaxial pressure dependence of Tc from high-resolution dilatometry of untwinned La2-xSrxCuO4 single crystals	199405			Phys.Rev.B, 49(1994)13137	Christoph Meingast,Frank Gugenberger,Georg Roth,Helmut Wuhl,Kai Grube,S.Uchida,Thomas Weber,Volker Breit,Y.Nakamura	La,Sr,Cu,O	
10187	PR04913137	DTCDP is the value of c-axis stress dependence of Tc. For a-axis DTCDP=1.2 K/GPa . for b-axis DTCDP=8.1 K/GPa. DTCDP estimated  from thermal expansion coefficient	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	1994																												T																		K				29.5			29.5			K/GPa	-9.4																																																																																											7	by TSFZ method. In detail,See Phys.Rev.B 47 (1993) 8369					Uniaxial pressure dependence of Tc from high-resolution dilatometry of untwinned La2-xSrxCuO4 single crystals	199405			Phys.Rev.B, 49(1994)13137	Christoph Meingast,Frank Gugenberger,Georg Roth,Helmut Wuhl,Kai Grube,S.Uchida,Thomas Weber,Volker Breit,Y.Nakamura	La,Sr,Cu,O	
10188	PR04913184		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		4	1994																												Bi2212																		K	87						87																																																			400000																																														16			On SrTiO3 substrates. In detail , See Physica C 215 (1993) 123	Thermally activated flux movement and critical transort current density in epitaxial Bi2Sr2CaCu2O8+delta films	199405		"Technische Hochschule Darmstadt, Institut fur Festko""rperphysick, Hochschulstrasse 8,64289 Darmstadt, Germany"	Phys.Rev.B,49(1994)13184	F. Hillmer,H. Adrian,P. Wagner,U. Fray		
10189	PR04913184		Bi2Sr2CaCu2O8	Bi2.05Sr2Ca1Cu1.99Zn0.01O8+y	Bi	2.05	Sr	2	Ca	1	Cu	1.99	Zn	0.01											O	8+y		4	1994																												Bi2212																																																																												300000																																														16		Bi2.05Sr2.00Ca1.00(Cu0.995Zn0.005)2O8+y	On SrTiO3 substrates. In detail, See Physica C 215 (1993) 123	Thermally activated flux movement and critical transort current density in epitaxial Bi2Sr2CaCu2O8+delta films	199405		"Technische Hochschule Darmstadt, Institut fur Festko""rperphysick, Hochschulstrasse 8,64289 Darmstadt, Germany"	Phys.Rev.B,49(1994)13184	F. Hillmer,H. Adrian,P. Wagner,U. Fray		
10190	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.4La1.25Ba1.35Cu3O6.875	Ca	0.4	La	1.25	Ba	1.35	Cu	3													O	7	6.875	1	1994																											2	Y123			A	3.878		11.711	3											K																																																																														m.ohm.cm											3.8													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10191	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.4La1.25Ba1.35Cu3O6.99	Ca	0.4	La	1.25	Ba	1.35	Cu	3													O	7	6.99	1	1994																											2	Y123			A	3.876		11.679	3											K			45	38		6	38																																																																							m.ohm.cm											1.8													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10192	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.4La1.25Ba1.35Cu3O7.055	Ca	0.4	La	1.25	Ba	1.35	Cu	3													O	7	7.055	1	1994																											2	Y123			A	3.875		11.669	3											K			64	57		4.5	57	TC10192																																																																						m.ohm.cm											1.5													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10193	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.4La1.25Ba1.35Cu3O7.135	Ca	0.4	La	1.25	Ba	1.35	Cu	3													O	7	7.135	1	1994																											2	Y123			A	3.872		11.635	3											K			80	76		2	76																																																																							m.ohm.cm											1.1													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10194	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.1La1.25Ba1.65Cu3O6.88	Ca	0.1	La	1.25	Ba	1.65	Cu	3													O	7	6.88	1	1994																											2	Y123			A	3.909		11.761	3																																																																																									m.ohm.cm																								1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10195	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.1La1.25Ba1.65Cu3O6.985	Ca	0.1	La	1.25	Ba	1.65	Cu	3													O	7	6.985	1	1994																											2	Y123			A	3.905		11.739	3											K			16	5		6	5																																																																							m.ohm.cm											4.2													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10196	PR04915928		(Ca,La)(Ba,La)2Cu3O7	Ca0.1La1.25Ba1.65Cu3O7.06	Ca	0.1	La	1.25	Ba	1.65	Cu	3													O	7	7.06	1	1994																											2	Y123			A	3.903		11.72	3											K			47	38		4	38	TC10196																																																																						m.ohm.cm											3													1	MIX(in N2)-Fire(1 day,in air) 3times-SIN(in flowing O2 at 970C)In detail,see Physca C 217,217(1993)					Variation of Tc and resistivity in charge-compensated (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	199406		Department of Physics and Crown Center for Superconductivity, Technion Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B,49(1994)15928	A. Knizhnik,D. Goldschmidt,G.M. Reisner,Y. Direktovitch,Y. Eckstein		
10197	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.99Zn0.01O4	La	1.84	Sr	0.16	Cu	0.99	Zn	0.01													O		4	1	1994	emu/g		emu.K/g																																											K				28.8			28.8																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10198	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.98Zn0.02O4	La	1.84	Sr	0.16	Cu	0.98	Zn	0.02													O		4	1	1994	emu/g		emu.K/g																																											K				18.6			18.6																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10199	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.97Zn0.03O4	La	1.84	Sr	0.16	Cu	0.97	Zn	0.03													O		4	1	1994																																														K				7.85			7.85																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10200	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.96Zn0.04O4	La	1.84	Sr	0.16	Cu	0.96	Zn	0.04													O		4	1	1994	emu/g		emu.K/g																																											K					4.2																																																																																																La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10201	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.95Zn0.05O4	La	1.84	Sr	0.16	Cu	0.95	Zn	0.05													O		4	1	1994	emu/g		emu.K/g																																											K					4.2																																																																																																La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10202	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O		4	1	1994	emu/g		emu.K/g																																											K				39.3			39.3																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10203	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.99Zn0.01O4	La	1.78	Sr	0.22	Cu	0.99	Zn	0.01													O		4	1	1994	emu/g		emu.K/g																																											K				18.3			18.3																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10204	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.98Zn0.02O4	La	1.78	Sr	0.22	Cu	0.98	Zn	0.02													O		4	1	1994	emu/g																																													K				9.6			9.6																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10205	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.97Zn0.03O4	La	1.78	Sr	0.22	Cu	0.97	Zn	0.03													O		4	1	1994	emu/g		emu.K/g																																											K				3.3			3.3																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10206	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.96Zn0.04O4	La	1.78	Sr	0.22	Cu	0.96	Zn	0.04													O		4	1	1994	emu/g		emu.K/g																																											K					4.2																																																																																																La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10207	PR04916000		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O		4	1	1994	emu/g		emu.K/g																																											K				25.9			25.9																																																																																														La2O3,SrCO3,CuO,ZnO	1	SIN(in O2 for 24h at 1000-1075C)-refire-COOL(to 600C)-ANN(for24h)					Magnetic properties and electronic conduction of superconducting La2-xSrxCuO4	199406			Phys.Rev.B, 49(1994)1600	C.Manabe,M.Ido,M.Oda,N.Momono,T.Takano,Y.Miura	La,Sr,Cu,O	
10208	PR04915416		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1994																												Hg1223																		K	132			132			132																																														meV	48	8.5																																														Ba(NO3)3,Ca(*NO3)2,Ca(NO3)2,4H2O	1	precursor (pellet Ba-Ca-Cu-O) -MIX(in N2 ,HgO) - SIN(in quartz tubes,Hg vapor pressure 200atm)					Energy gap of the high-Tc superconductor HgBa2Ca2Cu3O8+z determined by point-contact spectroscopy	199406			Phys.Rev.B, 49(1994)15416	G.T.Jeong,J.I.Kye,S.H.Chun,S.I.Lee,Sergey Lee,Z.G.Khim	Hg,Ba,Ca,Cu,O	
10209	PR04916082		LaCuO2	La1Cu1O2.54	La	1	Cu	1																	O	z	2.54	1	1994																												IL																																																																																	mJ/mol.K2			281																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10210	PR04916082		LaCuO2	La1Cu1O2.64	La	1	Cu	1																	O	z	2.64	1	1994																												IL																																																																																	mJ/mol.K2	6.5		284																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10211	PR04916082		(Y,Ca)CuO2	Y0.99Ca0.01Cu1O2.58	Y	0.99	Ca	0.01	Cu	1															O	z	2.58	1	1994																												IL																																																																																				324																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10212	PR04916082		(Y,Ca)CuO2	Y0.99Ca0.01Cu1O2.65	Y	0.99	Ca	0.01	Cu	1															O	z	2.65	1	1994																												IL																																																																																	mJ/mol.K2	1.3		317																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10213	PR04916082		YCuO2	Y1Cu1O2.55	Y	1	Cu	1																	O	z	2.55	1	1994																												IL																																																																																				375																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10214	PR04916082		(Y,Ca)CuO2	Y0.99Ca0.01Cu1O2.5	Y	0.99	Ca	0.01	Cu	1															O	z	2.5	1	1994																												IL																																																																																				370																																				1	In details, see J.Solid State Chem. 104,437(1993)					Ground states of a triangular copper oxide system	199406		ATT Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,49(1994)16082	A.P. Ramirez,J.J. Krajewski,R.J. Cava,W.F. Peck, Jr		
10215	PR04915299		HgBa2CuO4	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1994																		GPa		65.4							2	Hg1201			A	3.878		9.516	3																																																																																																																	1	Vapor Solid Reaction TechniqueIn details,see Nature 365,323(1993)					Compressibility of the HgBa2Can-1CunO2n+2+z (n=1,2,3) high-temperature superconductors	199406			Phys.Rev.B, 49(1994)15299	C.W.Chu,H.K.Mao,J.H.Eggert,J.Z.Hu,L.Beauvais,R.L.Meng	Hg,Ba,Ca,Cu,O	
10216	PR04915299		HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6	Hg	1	Ba	2	Ca	1	Cu	2													O	6		1	1994																		GPa		91.6							2	Hg1212			A	3.855		12.609	3																																																																																																																	1	Vapor Solid Reaction TechniqueIn details,see Nature 365,323(1993)					Compressibility of the HgBa2Can-1CunO2n+2+z (n=1,2,3) high-temperature superconductors	199406			Phys.Rev.B, 49(1994)15299	C.W.Chu,H.K.Mao,J.H.Eggert,J.Z.Hu,L.Beauvais,R.L.Meng	Hg,Ba,Ca,Cu,O	
10217	PR04915299		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8	Hg	1	Ba	2	Ca	2	Cu	3													O	8		1	1994																		GPa		83.8							2	Hg1223			A	3.854		15.742	3																																																																																																																	1	Vapor Solid Reaction TechniqueIn details,see Nature 365,323(1993)					Compressibility of the HgBa2Can-1CunO2n+2+z (n=1,2,3) high-temperature superconductors	199406			Phys.Rev.B, 49(1994)15299	C.W.Chu,H.K.Mao,J.H.Eggert,J.Z.Hu,L.Beauvais,R.L.Meng	Hg,Ba,Ca,Cu,O	
10218	PR04915959	NdGaO3 substrate, thickness = 1 micron meter, Jc defined as voltage criterion 2 micro-V/mm	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		5	1994																												Bi2212																		K	82.4					3	82.4																																																			1800																																												8					substrate(NdGaO3), Film thickness 1 micrometer	Scaling in the angular dependence of the critical current and temperature-dependent anisotropy ratio in Bi2Sr2CaCu2O8	199406			Phys.Rev.B, 49(1994)15959	E.Milani,E.Silva,R.Fastampa,S.Sarti	Bi,Sr,Ca,Cu,O	
10219	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl0.97Sr2.04Lu0.94Cu2.05Oy	Tl	0.97	Sr	2.04	Lu	0.94	Cu	2.05													O	y		1	1994																											2		P4/mmm		A	3.796		11.975	3																																																																																																																CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10220	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl0.97Sr1.99Lu0.9Ca0.12Cu2.02Oy	Tl	0.97	Sr	1.99	Lu	0.9	Ca	0.12	Cu	2.02											O	y		1	1994																											2		P4/mmm		A	3.793		11.994	3											K				39			39																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10221	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1.04Sr1.98Lu0.78Ca0.22Cu1.98Oy	Tl	1.04	Sr	1.98	Lu	0.78	Ca	0.22	Cu	1.98											O	y		1	1994																											2		P4/mmm		A	3.792		12.01	3											K				72			72																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10222	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl0.98Sr2.05Lu0.68Ca0.26Cu2.03Oy	Tl	0.98	Sr	2.05	Lu	0.68	Ca	0.26	Cu	2.03											O	y		1	1994																											2		P4/mmm		A	3.79		12.02	3											K				69			69																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10223	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl0.99Sr2.03Lu0.57Ca0.36Cu2.05Oy	Tl	0.99	Sr	2.03	Lu	0.57	Ca	0.36	Cu	2.05											O	y		1	1994																											2		P4/mmm		A	3.788		12.02	3											K				64			64																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10224	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1.01Sr2.02Lu0.49Ca0.47Cu2.03Oy	Tl	1.01	Sr	2.02	Lu	0.49	Ca	0.47	Cu	2.03											O	y		1	1994																											2		P4/mmm		A	3.788		12.045	3											K				46			46																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10225	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1.05Sr2.02Lu0.42Ca0.53Cu1.98Oy	Tl	1.05	Sr	2.02	Lu	0.42	Ca	0.53	Cu	1.98											O	y		1	1994																											2		P4/mmm		A	3.785		12.059	3											K				30			30																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10226	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1.07Sr2.04Lu0.29Ca0.61Cu1.99Oy	Tl	1.07	Sr	2.04	Lu	0.29	Ca	0.61	Cu	1.99											O	y		1	1994																											2		P4/mmm		A	3.784		12.076	3											K				9			9																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10227	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1Sr2Lu0.2Ca0.8Cu2Oy	Tl	1	Sr	2	Lu	0.2	Ca	0.8	Cu	2											O	y		1	1994																											2		P4/mmm		A	3.782		12.092	3																																																																																																																CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10228	PR05001244		TlSr2(Lu,Ca)Cu2Oy	Tl1.25Sr1.99Ca0.77Cu1.99Oy	Tl	1.25	Sr	1.99	Ca	0.77	Cu	1.99													O	y		1	1994																											2		P4/mmm		A	3.783		12.116	3																																																																																																																CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10229	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl0.97Sr1.99Lu0.9Ca0.12Cu2.02Oy	Tl	0.97	Sr	1.99	Lu	0.9	Ca	0.12	Cu	2.02											O	y		1	1994																											2		P4/mmm		A	3.797		11.989	3											K				6			6																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10230	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl1.04Sr1.98Lu0.78Ca0.22Cu1.98Oy	Tl	1.04	Sr	1.98	Lu	0.78	Ca	0.22	Cu	1.98											O	y		1	1994																											2		P4/mmm		A	3.796		12.002	3											K				31			31																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10231	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl0.98Sr2.05Lu0.68Ca0.26Cu2.03Oy	Tl	0.98	Sr	2.05	Lu	0.68	Ca	0.26	Cu	2.03											O	y		1	1994																											2		P4/mmm		A	3.797		12.015	3											K				42			42																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10232	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl0.99Sr2.03Lu0.57Ca0.36Cu2.05Oy	Tl	0.99	Sr	2.03	Lu	0.57	Ca	0.36	Cu	2.05											O	y		1	1994																											2		P4/mmm		A	3.796		12.021	3											K				62			62																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10233	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl1.01Sr2Lu0.49Ca0.47Cu2.03Oy	Tl	1.01	Sr	2	Lu	0.49	Ca	0.47	Cu	2.03											O	y		1	1994																											2		P4/mmm		A	3.793		12.035	3											K				81			81																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10234	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl1.05Sr2.02Lu0.42Ca0.53Cu1.98Oy	Tl	1.05	Sr	2.02	Lu	0.42	Ca	0.53	Cu	1.98											O	y		1	1994																											2		P4/mmm		A	3.791		12.057	3											K				84			84																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10235	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl1.07Sr2.04Lu0.29Ca0.61Cu1.99Oy	Tl	1.07	Sr	2.04	Lu	0.29	Ca	0.61	Cu	1.99											O	y		1	1994																											2		P4/mmm		A	3.792		12.075	3											K				77			77																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10236	PR05001244	Ar Annealed (500C for 5h) Sample.	TlSr2(Lu,Ca)Cu2Oy	Tl1.25Sr1.99Ca0.77Cu1.99Oy	Tl	1.25	Sr	1.99	Ca	0.77	Cu	1.99													O	y		1	1994																											2		P4/mmm		A	3.793		12.122	3											K				70			70																																																																																														CaO, CuO, Tl2O3, Lu2O3, SrO	1	Dry (at 350C for 5h in flowing O2). Press. SIN (890-940C for 1-5h, 2-3times). ANN (350C for 10h in flowing O2).					Normal-state magnetic susceptibility in TlSr2(Lu1-xCax)Cu2Oz from the underdoped to the overdoped regime	199407			Phys.Rev.B, 50(1994)1244	Takashi Kondo,Takashi Manako,Yoshimi Kubo,Yuichi Shimakawa	Tl,Sr,Lu,Ca,Cu,O	
10237	PR05000517	The Sample is c-axis-aligned poly crystal.	HgBa2Ca2Cu3O8+d	Hg1Ba2CaCu3O8+d	Hg	1	Ba	2	Ca		Cu	3													O	8+d		1	1994									5.8																		2				A	3.852		15.792	3																																																																																																																Ba2Co3, CaCO3, CuO, HgO	1	Precursor material Ba2Ca3Cu3O7 and CuO: CAL (930C for 20h in O2).Mixing with HgO. SIN (850C for 1h under 5GPa). ANN (300C for 5h in O2).					Anisotropy of the magnetic properties of c-axis-aligned Hg Ba2Ca2Cu3O8+delta powders	199407		Electrotechnical Laboratory, 1-1-4  Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B,50(1994)517	H. Ihara,M. Hirabayashi,M. Tokumoto,Y.S. Song		
10238	PR05000594		(Y,Ca)Ba2Cu3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	z	6.65	1	1994																											3	Y123			A	3.834	3.87	11.694	3											K				57			57		3																																																																																												Y2O3, CuO, BaCO3, CaCO3	1	ANN (12h for 400C in Ar), FC					Role of Ca in enhancing the superconductivity of YBaCu3O7-y	199407		Tata Institute of Fundemental Research, Bombay 400005, India	Phys.Rev.B,50(1994)594	A.V. Narlikar,Ashwin Tulapurkar,S.K. Malik,V.P.S. Awana		
10239	PR05000594		(Y,Ca)Ba2Cu3Oz	Y0.95Ca0.05Ba2Cu3O6.7	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	z	6.7	1	1994																											3	Y123			A	3.839	3.869	11.733	3											K				70			70		3																																																																																												Y2O3, CuO, BaCO3, CaCO3	1	ANN (12h for 400C in Ar), FC					Role of Ca in enhancing the superconductivity of YBaCu3O7-y	199407		Tata Institute of Fundemental Research, Bombay 400005, India	Phys.Rev.B,50(1994)594	A.V. Narlikar,Ashwin Tulapurkar,S.K. Malik,V.P.S. Awana		
10240	PR05000594		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.7	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z	6.7	1	1994																											3	Y123			A	3.832	3.874	11.746	3											K				75			75		3																																																																																												Y2O3, CuO, BaCO3, CaCO3	1	ANN (12h for 400C in Ar), FC					Role of Ca in enhancing the superconductivity of YBaCu3O7-y	199407		Tata Institute of Fundemental Research, Bombay 400005, India	Phys.Rev.B,50(1994)594	A.V. Narlikar,Ashwin Tulapurkar,S.K. Malik,V.P.S. Awana		
10241	PR05000594		(Y,Ca)Ba2Cu3Oz	Y0.85Ca0.15Ba2Cu3O6.71	Y	0.85	Ca	0.15	Ba	2	Cu	3													O	z	6.71	1	1994																											3	Y123			A	3.837	3.867	11.756	3											K				78			78		3																																																																																												Y2O3, CuO, BaCO3, CaCO3	1	ANN (12h for 400C in Ar), FC					Role of Ca in enhancing the superconductivity of YBaCu3O7-y	199407		Tata Institute of Fundemental Research, Bombay 400005, India	Phys.Rev.B,50(1994)594	A.V. Narlikar,Ashwin Tulapurkar,S.K. Malik,V.P.S. Awana		
10242	PR05001171		YBa2Cu4O8	Y1Ba2Cu4O7.95	Y	1	Ba	2	Cu	4															O		7.95	1	1994																																														K			82				82																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10243	PR05001171		(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O7.95	Y	0.8	Pr	0.2	Ba	2	Cu	4													O		7.95	1	1994																																														K			74				74																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10244	PR05001171		(Y,Pr)Ba2Cu4O8	Y0.6Pr0.4Ba2Cu4O7.95	Y	0.6	Pr	0.4	Ba	2	Cu	4													O		7.95	1	1994																																														K			63				63																																																6.6																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10245	PR05001171		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.985Zn0.015O7.95	Y	1	Ba	2	Cu	3.985	Zn	0.015													O		7.95	1	1994																																														K			70				70																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10246	PR05001171		YBa2(Cu,Zn)4O8	Y1Ba2Cu0.95Zn0.05O7.95	Y	1	Ba	2	Cu	0.95	Zn	0.05													O		7.95	1	1994																																														K			46				46																																																8.2																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10247	PR05001171		YBa2(Cu,Zn)4O8	Y1Ba2Cu0.97Zn0.03O7.95	Y	1	Ba	2	Cu	0.97	Zn	0.03													O		7.95	1	1994																																														K			59				59																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10248	PR05001171		Y(Ba,Sr)2Cu4O8	Y1Ba1.8Sr0.2Cu4O7.95	Y	1	Ba	1.8	Sr	0.2	Cu	4													O		7.95	1	1994																																														K			82				82																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10249	PR05001171		Y(Ba,Sr)2Cu4O8	Y1Ba1.6Sr0.4Cu4O7.95	Y	1	Ba	1.6	Sr	0.4	Cu	4													O		7.95	1	1994																																														K			82				82																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10250	PR05001171		Y(Ba,Sr)2Cu4O8	Y1Ba1.4Sr0.6Cu4O7.95	Y	1	Ba	1.4	Sr	0.6	Cu	4													O		7.95	1	1994																																														K			82				82																																																																																															1	See Physica C 204, 147 (1993).					Infrared-active phonons and the superconducting gap of Tc-reduced double-chain YBa2Cu4O8 superconductors	199407			Phys.Rev.B, 50(1994)1171	A.P.Litvinchuk,C.Thomsen,L.-G.Johansson,L.Borjesson,M.Cardona,P.Berastegui	Y,Ba,Cu,O	
10251	PR05001178		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																												Y123																		K			90.4				90.4																																				A	Determined from Microwave Data.	20			A	Determined from Microwave Data.	1700							12000000																																													16	See J.Appl. Phys. 75, 393 (1994).					Frequency dependence of the surface impedance of YBa2Cu3O7-z thin films in a dc magnetic field: Investigation of vortex dynamics	199407			Phys.Rev.B, 50(1994)1178	D.E.Oates,D.Labbe-Lavigne,G.Dresselhaus,M.S.Dresselhaus,Sylvie Revenaz	Y,Ba,Cu,O	
10252	PR05001178		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																												Y123																		K			90.3				90.3																																				A	Determined from Microwave Data.	20			A	Determined from Microwave Data	1700							2700000																					mic.ohm.cm	4.22																							16	See J.Appl. Phys. 75, 393 (1994).					Frequency dependence of the surface impedance of YBa2Cu3O7-z thin films in a dc magnetic field: Investigation of vortex dynamics	199407			Phys.Rev.B, 50(1994)1178	D.E.Oates,D.Labbe-Lavigne,G.Dresselhaus,M.S.Dresselhaus,Sylvie Revenaz	Y,Ba,Cu,O	
10253	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu3O7-y	Yb	1	Ba	2	Cu	3															O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10254	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu2.95Ga0.05O7-y	Yb	1	Ba	2	Cu	2.95	Ga	0.05													O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10255	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu2.9Ga0.1O7-y	Yb	1	Ba	2	Cu	2.9	Ga	0.1													O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10256	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu2.85Ga0.15O7-y	Yb	1	Ba	2	Cu	2.85	Ga	0.15													O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10257	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu2.8Ga0.2O7-y	Yb	1	Ba	2	Cu	2.8	Ga	0.2													O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10258	PR05001223		YbBa2(Cu,Ga)O7-y	Yb1Ba2Cu2.7Ga0.3O7-y	Yb	1	Ba	2	Cu	2.7	Ga	0.3													O	7-y		1	1994																											3	Y123							3											K		90		90			90																																																																																														Yb2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10259	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu3O6.76	Nd	1	Ba	2	Cu	3															O		6.76	1	1994																											3	Y123							3											K		94		93			94																																																																																														Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10260	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu2.95Ga0.05O6.59	Nd	1	Ba	2	Cu	2.95	Ga	0.05													O		6.59	1	1994																											2	Y123							3											K		53		53			53																																																																																														Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10261	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu2.9Ga0.1O6.61	Nd	1	Ba	2	Cu	2.9	Ga	0.1													O		6.61	1	1994																											2	Y123							3											K		38		38			38																																																																																														Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10262	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu2.85Ga0.15O6.62	Nd	1	Ba	2	Cu	2.85	Ga	0.15													O		6.62	1	1994																											2	Y123							3											K				23			23																																																																																														Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10263	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu2.8Ga0.2O6.63	Nd	1	Ba	2	Cu	2.8	Ga	0.2													O		6.63	1	1994																											2	Y123							3																																																																																																																Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10264	PR05001223		NdBa2(Cu,Ga)O7-y	Nd1Ba2Cu2.7Ga0.3O6.68	Nd	1	Ba	2	Cu	2.7	Ga	0.3													O		6.68	1	1994																											2	Y123							3																																																																																																																Nd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10265	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu3O6.85	Er	1	Ba	2	Cu	3															O		6.85	1	1994																											3	Y123							3											K		93		91			93																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10266	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu2.95Ga0.05O6.75	Er	1	Ba	2	Cu	2.95	Ga	0.05													O		6.75	1	1994																											3	Y123							3											K		90		87			90																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10267	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu2.9Ga0.1O6.78	Er	1	Ba	2	Cu	2.9	Ga	0.1													O		6.78	1	1994																											3	Y123							3											K		86		82			86																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10268	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu2.85Ga0.15O6.69	Er	1	Ba	2	Cu	2.85	Ga	0.15													O		6.69	1	1994																											3	Y123							3											K				82			82																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10269	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu2.8Ga0.2O7-y	Er	1	Ba	2	Cu	2.8	Ga	0.2													O	7-y		1	1994																											2	Y123							3											K		81		82			81																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10270	PR05001223		ErBa2(Cu,Ga)O7-y	Er1Ba2Cu2.7Ga0.3O7-y	Er	1	Ba	2	Cu	2.7	Ga	0.3													O	7-y		1	1994																											2	Y123							3											K				80			80																																																																																														Er2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10271	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O		6.82	1	1994																											3	Y123							3											K		93		91			93																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10272	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu2.95Ga0.05O6.69	Y	1	Ba	2	Cu	2.95	Ga	0.05													O		6.69	1	1994																											3	Y123							3											K		88		89			88																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10273	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu2.9Ga0.1O6.8	Y	1	Ba	2	Cu	2.9	Ga	0.1													O		6.8	1	1994																											3	Y123							3											K		81		82			81																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10274	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu2.85Ga0.15O7-y	Y	1	Ba	2	Cu	2.85	Ga	0.15													O	7-y		1	1994																											2	Y123							3											K				78			78																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10275	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu2.8Ga0.2O7-y	Y	1	Ba	2	Cu	2.8	Ga	0.2													O	7-y		1	1994																											2	Y123							3											K		68		72			68																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10276	PR05001223		YBa2(Cu,Ga)O7-y	Y1Ba2Cu2.7Ga0.3O7-y	Y	1	Ba	2	Cu	2.7	Ga	0.3													O	7-y		1	1994																											2	Y123							3											K				70			70																																																																																														Y2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10277	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu3O6.75	Dy	1	Ba	2	Cu	3															O		6.75	1	1994																											3	Y123							3											K		94		92			94																																																																																														Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10278	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu2.95Ga0.05O6.69	Dy	1	Ba	2	Cu	2.95	Ga	0.05													O		6.69	1	1994																											3	Y123							3											K		83		81			83																																																																																														Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10279	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu2.9Ga0.1O6.7	Dy	1	Ba	2	Cu	2.9	Ga	0.1													O		6.7	1	1994																											2	Y123							3											K		68		68			68																																																																																														Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10280	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu2.85Ga0.15O6.74	Dy	1	Ba	2	Cu	2.85	Ga	0.15													O		6.74	1	1994																											2	Y123							3																																																																																																																Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10281	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu2.8Ga0.2O6.78	Dy	1	Ba	2	Cu	2.8	Ga	0.2													O		6.78	1	1994																											2	Y123							3											K		50		42			50																																																																																														Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10282	PR05001223		DyBa2(Cu,Ga)O7-y	Dy1Ba2Cu2.7Ga0.3O6.77	Dy	1	Ba	2	Cu	2.7	Ga	0.3													O		6.77	1	1994																											2	Y123							3											K				39			39																																																																																														Dy2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10283	PR05001223		GdBa2(Cu,Ga)O7-y	Gd1Ba2Cu3O7-y	Gd	1	Ba	2	Cu	3															O	7-y		1	1994																																														K		94		93			94																																																																																														Gd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10284	PR05001223		GdBa2(Cu,Ga)O7-y	Gd1Ba2Cu2.9Ga0.1O7-y	Gd	1	Ba	2	Cu	2.9	Ga	0.1													O	7-y		1	1994																																														K				62			62																																																																																														Gd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10285	PR05001223		GdBa2(Cu,Ga)O7-y	Gd1Ba2Cu2.7Ga0.3O7-y	Gd	1	Ba	2	Cu	2.7	Ga	0.3													O	7-y		1	1994																																														K				21			21																																																																																														Gd2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10286	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu3O6.82	Eu	1	Ba	2	Cu	3															O		6.82	1	1994																											3	Y123							3											K		94		93			94																																																																																														Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10287	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu2.95Ga0.05O6.78	Eu	1	Ba	2	Cu	2.95	Ga	0.05													O		6.78	1	1994																											2	Y123							3											K		79		75			79																																																																																														Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10288	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu2.9Ga0.1O6.74	Eu	1	Ba	2	Cu	2.9	Ga	0.1													O		6.74	1	1994																											2	Y123							3											K		52		55			52																																																																																														Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10289	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu2.85Ga0.15O6.76	Eu	1	Ba	2	Cu	2.85	Ga	0.15													O		6.76	1	1994																											2	Y123							3											K				43			43																																																																																														Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10290	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu2.8Ga0.2O6.63	Eu	1	Ba	2	Cu	2.8	Ga	0.2													O		6.63	1	1994																											2	Y123							3											K		14		22			14																																																																																														Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10291	PR05001223		EuBa2(Cu,Ga)O7-y	Eu1Ba2Cu2.7Ga0.3O6.69	Eu	1	Ba	2	Cu	2.7	Ga	0.3													O		6.69	1	1994																											2	Y123							3																																																																																																																Eu2O3, BaCO3, CuO, Ga2O3	1	CAL(in air at 910C for 24h), SIN (in flowing O2 at 930C for 50h),FC (to 680C in 5H and Maintain for 10h), FC(in 3h to 400C and Maintain for 10h), FC					Substitution of Ga for Cu in RBa2Cu3-x GaxO7-z systems (R=Yb,Er,Y,Dy,Gd,Eu, and Nd)	199407			Phys.Rev.B, 50(1994)1223	M.K.Wu,S.R.Sheen,Weiyan Guan,Y.F.Chen,Yunhui Xu	Yb,Er,Y,Gd,Dy,Eu,Nd,Ba,Ga,Cu,O	
10292	PR05001237		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.65Pb0.35Sr2Ca2Cu3O10	Bi	1.65	Pb	0.35	Sr	2	Ca	2	Cu	3											O		10	2	1994																											2				A	5.411		37.246												K	108.6						108.6																																																																																														Bi2O3, PbO, SrCO3, CaCO3, CuO	1	Raw Materials were dissolved in 1:1 HNO3, then drived at 120C. PRE (at 760C for 6h), ground,  CAL (at 810C for 12h), Cool, Press into pellets, SIN (at 850C for 360h), FCL					Properties and structure of the F-doped (Bi,Pb)-Sr-Ca-Cu-O superconductor	199407			Phys.Rev.B, 50(1994)1237	Guo-dong Zheng,Jie Li,Sai Gao,Shu-fen Jiang,Xiao-Gang Wang,Xiao-hui Gao	Bi,Pb,Sr,Ca,Cu,O,F	
10293	PR05001237		(Bi,Pb)2Sr2Ca2Cu3(O,F)y	Bi1.65Pb0.35Sr2Ca2Cu3FOz	Bi	1.65	Pb	0.35	Sr	2	Ca	2	Cu	3	F										O	z		2	1994																											2				A	5.357		36.951												K	116.4			117.2			117.2																																																																																														Bi2O3, PbO, SrCO3, CaCO3, CuF2	1	Heat (450C/h to 680C, 12C/h to 750C 750C for 12h), ground, press, SIN (790C for 10h, 835C for 160-180h), quench in air.					Properties and structure of the F-doped (Bi,Pb)-Sr-Ca-Cu-O superconductor	199407			Phys.Rev.B, 50(1994)1237	Guo-dong Zheng,Jie Li,Sai Gao,Shu-fen Jiang,Xiao-Gang Wang,Xiao-hui Gao	Bi,Pb,Sr,Ca,Cu,O,F	
10294	PR05000426		Y2Ba4Cu7O15	Y2Ba4Cu7O15.1	Y	2	Ba	4	Cu	7															O		15.1	1	1994																															A	3.834	3.879	50.61	3											K			92.8				92.8																																																																																															1	CAL (in O2 at 20bar pressure at 1020C for 12h) twice, ANN (in 100bar O2 at 300C for 3days).					Charge-carrier density and interplane coupling in Y2Ba4Cu7O15: A Cu NMR-NQR study	199407		"Physik-Institut, Universita""t Zu""rich, CH-8057 Zu""rich, Switzerland"	Phys.Rev.B,50(1994)426	D. Brinkmann,I. Mangelschots,J. Roos,M. Mali,R. Stern		
10295	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7		1994																																														K				91			91																																																																																																See Supercond. Sci. Technol. 2, 35 (1989).Fluorinated by Flowing Diluted NF3 Gas (3% in N2) at 300C.					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
10296	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.1O7	Y	1	Ba	2	Cu	3	F	0.1													O		7		1994																																														K				91			91																																																																																																See Supercond. Sci. Technol. 2, 35 (1989).Fluorinated by Flowing Diluted NF3 Gas (3% in N2) at 300C.					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
10297	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.2O7	Y	1	Ba	2	Cu	3	F	0.2													O		7		1994																																														K				91			91																																																																																																See Supercond. Sci. Technol. 2, 35 (1989).Fluorinated by Flowing Diluted NF3 Gas (3% in N2) at 300C.					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
10298	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O		6.7		1994																																														K				62.5			62.5																																																																																																See Supercond. Sci. Technol. 2, 35 (1989).Fluorinated by Flowing Diluted NF3 Gas (3% in N2) at 300C.					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
10299	PR05001290		YBa2Cu3OzFx	Y1Ba2Cu3F0.1O6.7	Y	1	Ba	2	Cu	3	F	0.1													O		6.7		1994																																														K				71			71																																																																																																See Supercond. Sci. Technol. 2, 35 (1989).Fluorinated by Flowing Diluted NF3 Gas (3% in N2) at 300C.					NMR study of the <89>Y resonance in fluorinated YBa2Cu3Oz	199407			Phys.Rev.B, 50(1994)1290	C.Korn,C.Perrin,H.M.Vieth,K.Luders,S.D.Goren,W.Hoffmann	Y,Ba,Cu,O,F	
10300	PR05004154	Powder.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		6	1994																											3	Y124			A	3.854	3.874	27.267	3											K				78			78																																																																																																By an acetatetartrate sol-gel method. MIX(Y2O3,Eu2O3 dissolved in Cu(CH3COO)2.H2O,Ba(CH3COO)2 ) ...In detail,see text.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10301	PR05004154	powder.	(Y,Eu)Ba2Cu4O8	Y0.75Eu0.25Ba2Cu4O8	Y	0.75	Eu	0.25	Ba	2	Cu	4													O	8		6	1994																											3	Y124			A	3.865	3.886	27.29	3											K				78			78																																																																																																By an acetatetartrate sol-gel method. MIX(Y2O3,Eu2O3 dissolved in Cu(CH3COO)2.H2O,Ba(CH3COO)2 ) ...In detail,see text.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10302	PR05004154	powder.	(Y,Eu)Ba2Cu4O8	Y0.5Eu0.5Ba2Cu4O8	Y	0.5	Eu	0.5	Ba	2	Cu	4													O	8		6	1994																											3	Y124			A	3.874	3.893	27.292	3											K				77			77																																																																																																By an acetatetartrate sol-gel method. MIX(Y2O3,Eu2O3 dissolved in Cu(CH3COO)2.H2O,Ba(CH3COO)2 ) ...In detail,see text.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10303	PR05004154	powder.	(Y,Eu)Ba2Cu4O8	Y0.25Eu0.75Ba2Cu4O8	Y	0.25	Eu	0.75	Ba	2	Cu	4													O	8		6	1994																											3	Y124			A	3.874	3.892	27.292	3											K				75			75																																																																																																By an acetatetartrate sol-gel method. MIX(Y2O3,Eu2O3 dissolved in Cu(CH3COO)2.H2O,Ba(CH3COO)2 ) ...In detail,see text.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10304	PR05004154	powder.	(Y,Eu)Ba2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		6	1994																											3	Y124			A	3.882	3.895	27.27	3											K				74			74																																																																																																By an acetatetartrate sol-gel method. MIX(Y2O3,Eu2O3 dissolved in Cu(CH3COO)2.H2O,Ba(CH3COO)2 ) ...In detail,see text.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10305	PR05004154	powder.	EuBa2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		6	1994																											3	Y124			A	3.88	3.892	27.25	3																																																																																																																	5	By LiF flux process.					Europium substitution effects in superconducting YBa2Cu4O8 synthesized under one atomosphere oxygen pressure	199408			Phys.Rev.B, 50(1994)4154	A.Kareiva,I.Tittonen,J.Linden,J.Miettinen,J.Valo,L.Niinisto,M.Karppinen,M.Leskela,M.Lippmaa,T.Katila	Y,Ba,Cu,O	
10306	PR05004168		La2CuO4	La2Cu1O4.017	La	2	Cu	1																	O	4	4.017	1	1994																												T																		K		34.7	39				34.7			K/kBar	0.07																																																															1.84			TP10306																									1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10307	PR05004168		La2CuO4	La2Cu1O4.034	La	2	Cu	1																	O	4	4.034	1	1994																												T																		K		30.7	36				30.7			K/kBar	0.29																																																																																											1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10308	PR05004168		La2CuO4	La2Cu1O4.047	La	2	Cu	1																	O	4	4.047	1	1994																												T																		K		29.7	37				29.7			K/kBar	0.18																																																																																											1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10309	PR05004168		La2CuO4	La2Cu1O4.054	La	2	Cu	1																	O	4	4.054	1	1994																												T																		K		29.1	35				29.1			K/kBar	0.13																																																																		TP10309																									1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10310	PR05004168		La2CuO4	La2Cu1O4.066	La	2	Cu	1																	O	4	4.066	1	1994																												T																		K		38	40				38			K/kBar	-0.26																																																																																											1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10311	PR05004168		La2CuO4	La2Cu1O4.07	La	2	Cu	1																	O	4	4.07	1	1994																												T																		K		40.4	43				40.4			K/kBar	0.06																																																															20.9			TP10311																									1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10312	PR05004168		La2CuO4	La2Cu1O4.095	La	2	Cu	1																	O	4	4.095	1	1994																												T																		K		37.8	41				37.8			K/kBar	0.06																																																																																											1	CAL(La2O3 powder,at 980C) - SIN(1030-1100C,1 week, in Air)then, electrochemical insertion of Oxygen in KOH.					Effect of pressure and quenching on superconductive La2CuO4+z (0<z<0.1)	199408			Phys.Rev.B, 50(1994)4168	H.Chen,J.-S.Zhou,J.B.Goodenough	La,Cu,O	
10313	PR05004260	Tc(max) = 116 K at 15 Gpa.	HgBa2CuO4	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1994																												Hg1201																		K			96				96	TC10313		K/GPa	1.94																																																																																												In detail,Physca C 212,266(1993) , ibid. 214,307(1993), ibid. 216,21(1993)					Superconductivity up to 164K in HgBa2Cam-1CumO2m+2+z (m=1,2, and 3) under quasihydrostatic pressures	199408			Phys.Rev.B, 50(1994)4262	C.W.Chu,D.Ramirez,F.Chen,H.K.Mao,J.H.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue	Hg,Ba,Ca,Cu,O	
10314	PR05004260	Tc(max) = 150 K at 29 Gpa.	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6	Hg	1	Ba	2	Ca	1	Cu	2													O	6		1	1994																												Hg1212																		K			125				125	TC10314		K/GPa	2.2																																																																																												In detail,Physca C 212,266(1993) , ibid. 214,307(1993), ibid. 216,21(1993)					Superconductivity up to 164K in HgBa2Cam-1CumO2m+2+z (m=1,2, and 3) under quasihydrostatic pressures	199408			Phys.Rev.B, 50(1994)4262	C.W.Chu,D.Ramirez,F.Chen,H.K.Mao,J.H.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue	Hg,Ba,Ca,Cu,O	
10315	PR05004260	Tc(max) = 164 K at 31 Gpa.	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8	Hg	1	Ba	2	Ca	2	Cu	3													O	8		1	1994																												Hg1223																		K			134				134	TC10315		K/GPa	3.8																																																																																												In detail,Physca C 212,266(1993) , ibid. 214,307(1993), ibid. 216,21(1993)					Superconductivity up to 164K in HgBa2Cam-1CumO2m+2+z (m=1,2, and 3) under quasihydrostatic pressures	199408			Phys.Rev.B, 50(1994)4262	C.W.Chu,D.Ramirez,F.Chen,H.K.Mao,J.H.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue	Hg,Ba,Ca,Cu,O	
10316	PR05004260		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.9Pb0.1Ba2Ca2Cu3O8	Hg	0.9	Pb	0.1	Ba	2	Ca	2	Cu	3											O	8		1	1994																												Hg1223																		K			130				130			K/GPa	4																																																																																												In detail,Physca C 212,266(1993) , ibid. 214,307(1993), ibid. 216,21(1993)					Superconductivity up to 164K in HgBa2Cam-1CumO2m+2+z (m=1,2, and 3) under quasihydrostatic pressures	199408			Phys.Rev.B, 50(1994)4262	C.W.Chu,D.Ramirez,F.Chen,H.K.Mao,J.H.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue	Hg,Ba,Ca,Cu,O	
10317	PR05004260		(Hg,Pb)Ba2Ca2Cu3O8	Hg0.8Pb0.2Ba2Ca2Cu3O8	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	8		1	1994																												Hg1223																		K			132				132			K/GPa	2.54																																																																																												In detail,Physca C 212,266(1993) , ibid. 214,307(1993), ibid. 216,21(1993)					Superconductivity up to 164K in HgBa2Cam-1CumO2m+2+z (m=1,2, and 3) under quasihydrostatic pressures	199408			Phys.Rev.B, 50(1994)4262	C.W.Chu,D.Ramirez,F.Chen,H.K.Mao,J.H.Eggert,L.Gao,Q.Xiong,R.L.Meng,Y.Y.Xue	Hg,Ba,Ca,Cu,O	
10318	PR05004212	anisotropic ratio = 5.6+-0.3.This is Measurement for  temperature dependence of under critical magnetic field.	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7	6.95	3	1994																												Y123																		K				93.05		0.3	93.05											Oe	from Magnetization vs magnetic field data.		200	1100																																																																																5	CuO-BaO flux method using Zirconia crucibles.in detail, see Physica C 195,51(1992)					Lower critical fields in an ellipsoid-shaped YBa2Cu3O6.95 single crystal	199408			Phys.Rev.B, 50(1994)4212	A.J.Berlinsky,D.A.Bonn,P.Dosanjh,Ruixing Liang,W.N.Hardy	Y,Ba,Cu,O	
10319	PR05004125		(Tl,Pb)Sr4Cu2(CO3)O7	Tl0.5Pb0.5Sr4Cu2C1O3O7	Tl	0.5	Pb	0.5	Sr	4	Cu	2	C	1	O	3									O	7		1	1994																																														K				71			71										65	Oe	from M-H curve.	24.4							T		57.6							T/K		1.2					A			23.9		A			1700																																																			1	In detail, see Physica C 205,219(1993)					Superconductivity of the oxycarbonate Tl0.5Pb0.5Sr4Cu2CO3O7: A magnetic study	199408		Laboratoire CRISMAT, Institut des Sciences de la Matiere et du Rayonnement, Universite' de Caen, Boulevard du Mare'chal Juin, 14050 Caen Cedex, france	Phys.Rev.B,50(1994)4125	A. Maignan,A. Wahl,Ch. Simon,S. Peluau		
10320	PR05003312		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																												Y123																		K				93			93																				T		150							T/K	direct observation.	2.4					A			14.5		A			1170							500000																			TP10320															m3/C					1	RH10320					sub=(100)SrTiO3,hollow cathode magnetron sputtering,T(sub)=780C in a 60Pa(Ar/O2=1.5:1.0)	16		stoichiometric YBCO	thickness=200 nm, RES(100K)=100 microOhm.cm, G-L parameter=75	Nernst, Seebeck, and Hall effects in the mixed state of YBa2Cu3O7-z and Bi2Sr2CaCu2O8+z thin films: A comparative study	199408			Phys.Rev.B, 50(1994)3312	A.Beck,F.Gollnik,H.-C.Ri,H.Adrian,P.Wagner,R.Gross,R.P.Huebener	Y,Ba,Cu,O,Bi,Sr,Ca	
10321	PR05003312		Bi2Sr2CaCu2O8+y	Bi2Sr2Ca1Cu2O8+x	Bi	2	Sr	2	Ca	1	Cu	2													O	8+x		5	1994																												Bi2212																		K				90.4			90.4																				T		158							T/K	direct observation.	2.5					A			14.2		A			2630							100000																			TP10321																				1	RH10321					dc sputtering in 3.0hPa O2, growth rate=30 A/min, T(sub)=830C, ANN(830C, 45min in O2)	16		Bi2212 composition	thickness=400 nm,RES(100K)=100 microOhm.cm, G-L parameter<185	Nernst, Seebeck, and Hall effects in the mixed state of YBa2Cu3O7-z and Bi2Sr2CaCu2O8+z thin films: A comparative study	199408			Phys.Rev.B, 50(1994)3312	A.Beck,F.Gollnik,H.-C.Ri,H.Adrian,P.Wagner,R.Gross,R.P.Huebener	Y,Ba,Cu,O,Bi,Sr,Ca	
10322	PR05004092		TlBa2PrCu2O7	Tl1Ba2Pr1Cu2O7	Tl	1	Ba	2	Pr	1	Cu	2													O	7		1	1994								8																				Tl1212																																																																														SP10322			J/mol.K2	0.57	linear term coefficient of molar specific heat.	280												ohm.cm											9600													1	see Physica C 202,104(1992)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10323	PR05004092		Tl(Ba,Sr)2PrCu2O7	Tl1Ba1.6Sr0.4Pr1Cu2O7-d	Tl	1	Ba	1.6	Sr	0.4	Pr	1	Cu	2											O	7-d		1	1994								6.5																				Tl1212																																																																																																ohm.cm																							SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10324	PR05004092		Tl(Ba,Sr)2PrCu2O7	Tl1Ba1.2Sr0.8Pr1Cu2O7-d	Tl	1	Ba	1.2	Sr	0.8	Pr	1	Cu	2											O	7-d		1	1994								5.7																				Tl1212																																																																																																																							SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10325	PR05004092		Tl(Ba,Sr)2PrCu2O7	Tl1Ba1Sr1Pr1Cu2O7-d	Tl	1	Ba	1	Sr	1	Pr	1	Cu	2											O	7-d		1	1994								5																				Tl1212																																																																														SP10325			J/mol.K2	0.34		290												ohm.cm											157												SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10326	PR05004092		Tl(Ba,Sr)2PrCu2O7	Tl1Ba0.8Sr1.2Pr1Cu2O7-d	Tl	1	Ba	0.8	Sr	1.2	Pr	1	Cu	2											O	7-d		1	1994								5																				Tl1212																																																																																																																							SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10327	PR05004092		Tl(Ba,Sr)2PrCu2O7	Tl1Ba0.4Sr1.6Pr1Cu2O7-d	Tl	1	Ba	0.4	Sr	1.6	Pr	1	Cu	2											O	7-d		1	1994								4.5																				Tl1212																																																																																																																							SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10328	PR05004092		TlSr2PrCu2O7	Tl1Sr2Pr1Cu2O7-d	Tl	1	Sr	2	Pr	1	Cu	2													O	7-d		1	1994								3.6																				Tl1212																																																																														SP10328			J/mol.K2	0.42		350												ohm.cm											0.189												SrCO3,BaCO3,Pr6O11,CuO	1	MIX-CAL(900C,12h)-SIN(add Tl2O3, gold foils)-ANN(flow O2,880-980C,5-10h)					Variation of antiferromagnetic Pr ordering in the Tl(Ba1-xSrx)2PrCu2O7-z system	199408			Phys.Rev.B, 50(1994)4092	C.C.Lai,H.C.Ku,H.K.Fun,J.C.Ho,T.J.Lee	Tl,Ba,Sr,Pr,Cu,O	
10329	PR05003431		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.197	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d	8.197	1	1994																											2	Bi2212			A	5.4		30.81	3											K		74					74																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10330	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.9Pr0.1Cu2O8.234	Bi	2	Sr	2	Ca	0.9	Pr	0.1	Cu	2											O	8+d	8.234	1	1994																											2	Bi2212			A	5.43		30.792	3											K		75.8					75.8																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10331	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8.282	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8+d	8.282	1	1994																											2	Bi2212			A	5.43		30.768	3											K		70					70																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10332	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.7Pr0.3Cu2O8.299	Bi	2	Sr	2	Ca	0.7	Pr	0.3	Cu	2											O	8+d	8.299	1	1994																											2	Bi2212			A	5.43		30.722	3											K		60.8					60.8																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10333	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8.316	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8+d	8.316	1	1994																											2	Bi2212			A	5.452		30.63	3											K		57					57																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10334	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.5Pr0.5Cu2O8.329	Bi	2	Sr	2	Ca	0.5	Pr	0.5	Cu	2											O	8+d	8.329	1	1994																											2	Bi2212			A	5.452		30.602	3											K		5.1					5.1																																																																																														Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10335	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2O8.373	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	8+d	8.373	1	1994																											2	Bi2212			A	5.463		30.514	3											K					4.2																																																																																																Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10336	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.3Pr0.7Cu2O8.411	Bi	2	Sr	2	Ca	0.3	Pr	0.7	Cu	2											O	8+d	8.411	1	1994																											2	Bi2212			A	5.478		30.426	3											K					4.2																																																																																																Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10337	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.2Pr0.8Cu2O8.458	Bi	2	Sr	2	Ca	0.2	Pr	0.8	Cu	2											O	8+d	8.458	1	1994																											2	Bi2212			A	5.478		30.393	3											K					4.2																																																																																																Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10338	PR05003431		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.1Pr0.9Cu2O8.53	Bi	2	Sr	2	Ca	0.1	Pr	0.9	Cu	2											O	8+d	8.53	1	1994																											2	Bi2212			A	5.478		30.38	3											K					4.2																																																																																																Pr6O11,Bi2O3,SrCO3,CaCO3,CuO	1	MIX-SIN(800C,12h,in air)-SIN(two or three times at 24h intervals)-CAL(840-950C,pellet)					Phase separaration and oxygen variation in Pr-doped Bi2Sr2CaCu2O8+delta	199408		Institute Physics, Chinese Academy of Sciences, Beijing 100080, Peple's Republic pf China	Phys.Rev.B,50(1994)3431	Guanghui Rao,Jianqi Li,Jingkui Liang,Jinrong Min,Xiaolong Chen		
10339	PR05003454	O(18) isotope	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-y	Pr	1.85	Ce	0.15	Cu	1															O	4-y		1	1994																												T'																		K				20.5			20.5						0.08	O																																																																																							Pr6O11,CeO2,CuO	1	MIX-SIN(1000C,48h,in air)-ANN(in air,900C,12h)-ANN(in N2,950C 12h -> 1000C 20h)-RT pellet was broken in half,and the halves were subjected to the 16Oxygen and 18Oxygen isotope diffusion.					Sizable oxygen isotope effects in the electron-doped Pr1.85Ce0.15CuO4-y	199408		Moris Research Inc., 1918 University Avenue, Berkeley, California 94704	Phys.Rev.B,50(1994)3454	Donald E. Morris,Guo-meng Zhao		
10340	PR05003209		(Bi,Pb)2Sr2Ca2Cu3(O,F)10	Bi1.7Pb0.3Sr2Ca2Cu3O10	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O		10	1	1994																												Bi2223																		K		106.5					106.5																																																																																														Bi2O3,PbO,SrCaO3,CaCO3,CuO,CuF2	1	MIXIn detail. Mod.Phys.Lett. B 6,943(1992)					Oxygen deficiencies in the F-doped Bi2-xPbxSr2Ca2Cu3O10 superconductors studied by positron annihilation	199408		Department of Physics, Wuhan University, Wuhan 430072, People's Republic of China	Phys.Rev.B,50(1994)3209	S.J. Wang,X.H. Gao,Z. Tang		
10341	PR05003209		(Bi,Pb)2Sr2Ca2Cu3(O,F)10	Bi1.7Pb0.3Sr2Ca2Cu3F0.2O9.8	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	F	0.2									O	z	9.8	1	1994																												Bi2223																		K		111					111																																																																																														Bi2O3,PbO,SrCaO3,CaCO3,CuO,CuF2	1	MIXIn detail. Mod.Phys.Lett. B 6,943(1992)					Oxygen deficiencies in the F-doped Bi2-xPbxSr2Ca2Cu3O10 superconductors studied by positron annihilation	199408		Department of Physics, Wuhan University, Wuhan 430072, People's Republic of China	Phys.Rev.B,50(1994)3209	S.J. Wang,X.H. Gao,Z. Tang		
10342	PR05003209		(Bi,Pb)2Sr2Ca2Cu3(O,F)10	Bi1.7Pb0.3Sr2Ca2Cu3F0.5O9.5	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	F	0.5									O	z	9.5	1	1994																												Bi2223																		K		113					113																																																																																														Bi2O3,PbO,SrCaO3,CaCO3,CuO,CuF2	1	MIXIn detail. Mod.Phys.Lett. B 6,943(1992)					Oxygen deficiencies in the F-doped Bi2-xPbxSr2Ca2Cu3O10 superconductors studied by positron annihilation	199408		Department of Physics, Wuhan University, Wuhan 430072, People's Republic of China	Phys.Rev.B,50(1994)3209	S.J. Wang,X.H. Gao,Z. Tang		
10343	PR05003209		(Bi,Pb)2Sr2Ca2Cu3(O,F)10	Bi1.7Pb0.3Sr2Ca2Cu3F0.8O9.2	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	F	0.8									O	z	9.2	1	1994																												Bi2223																		K		117.6					117.6																																																																																														Bi2O3,PbO,SrCaO3,CaCO3,CuO,CuF2	1	MIXIn detail. Mod.Phys.Lett. B 6,943(1992)					Oxygen deficiencies in the F-doped Bi2-xPbxSr2Ca2Cu3O10 superconductors studied by positron annihilation	199408		Department of Physics, Wuhan University, Wuhan 430072, People's Republic of China	Phys.Rev.B,50(1994)3209	S.J. Wang,X.H. Gao,Z. Tang		
10344	PR05003221	powder	La2CuO4	La2CuO4	La	2	Cu																		O	4		6	1994																		GPa		122							3	T			A	5.356	5.404	13.149	3																																																																																																																		In detail,Phys.Rev. B 49,4163(1994)x=0.10 sample ANN( 700C in flowing oxygen,-> slow cooling to RT)x=0.0 sample ANN( 700C in flowing N2,-> quench)					Structural effects of hydrostatic pressure in orthorhombic La2-xSrxCuO4	199408			Phys.Rev.B, 50(1994)3221	B.A.Hunter,D.G.Hinks,H.Shaked,H.Takahashi,J.D.Jorgensen,P.G.Radaelli,R.L.Hitterman	La,Sr,Cu,O	
10345	PR05003221	powder	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		6	1994																		GPa		147							3	T																																																																																																																									In detail,Phys.Rev. B 49,4163(1994)x=0.10 sample ANN( 700C in flowing oxygen,-> slow cooling to RT)x=0.0 sample ANN( 700C in flowing N2,-> quench)					Structural effects of hydrostatic pressure in orthorhombic La2-xSrxCuO4	199408			Phys.Rev.B, 50(1994)3221	B.A.Hunter,D.G.Hinks,H.Shaked,H.Takahashi,J.D.Jorgensen,P.G.Radaelli,R.L.Hitterman	La,Sr,Cu,O	
10346	PR05003246	This is Sample A. ANN(300C,14H in O2)	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+d	Hg	1	Ba	2	Ca	1	Cu	2													O	6+d		1	1994																												Hg1212																		K		124					124																																																																							m.ohm.cm											70									RH10346				1	See Physica C 216,21 (1993)Difference between Sample A and B is anneal condition.A:ANN(300C,14h,in O2)      B:ANN(300C,1.5h,in O2)					Hall-effect measurements of HgBa2CaCu2O6+z	199408			Phys.Rev.B, 50(1994)3246	C.W.Chu,H.Wu,J.M.Harris,N.P.Ong,R.L.Meng	Hg,Ba,Ca,Cu,O	
10347	PR05003246	This is Sample B. ANN(300C,1.5H in O2)	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+d	Hg	1	Ba	2	Ca	1	Cu	2													O	6+d		1	1994																												Hg1212																		K		124					124																																																																							m.ohm.cm											30									RH10347				1	See Physica C 216,21 (1993)Difference between Sample A and B is anneal condition.A:ANN(300C,14h,in O2)      B:ANN(300C,1.5h,in O2)					Hall-effect measurements of HgBa2CaCu2O6+z	199408			Phys.Rev.B, 50(1994)3246	C.W.Chu,H.Wu,J.M.Harris,N.P.Ong,R.L.Meng	Hg,Ba,Ca,Cu,O	
10348	PR05003288		Pb2Sr2PrCu3O8	Pb2Sr2Pr1Cu3O8	Pb	2	Sr	2	Pr	1	Cu	3													O	8	8	1	1994								6																			3	Pb3212	Cmmm		A	5.454	5.486	15.823	3																																																																							SP10348			mJ/mol.K2	200														m.ohm.cm											530												SrCO3,Pr2O3,CuO (Sr:Pr:Cu=2:1:3)	1	MIX-CAL(930C,in air)-MIX(Sr2PrCu3Ox + PbO)-SIN(750C,12h,in air)					Magnetic and Calorimetric studies of anomalous Pr antiferromagnetic ordering in orthorhombic Pb2Sr2PrCu3O8	199408			Phys.Rev.B, 50(1994)3288	H.C.Ku,J.C.Ho,J.H.Shieh	Pb,Sr,Pr,Cu,O	
10349	PR05003288		Pb2Sr2PrCu3O9	Pb2Sr2Pr1Cu3O9	Pb	2	Sr	2	Pr	1	Cu	3													O	9	9	1	1994																											3	Pb3212	Cmmm		A	5.507	5.51	15.881	3																																																																																																																SrCO3,Pr2O3,CuO (Sr:Pr:Cu=2:1:3)	1	MIX-CAL(930C,in air)-MIX(Sr2PrCu3Ox + PbO)-SIN(750C,12h,in air)					Magnetic and Calorimetric studies of anomalous Pr antiferromagnetic ordering in orthorhombic Pb2Sr2PrCu3O8	199408			Phys.Rev.B, 50(1994)3288	H.C.Ku,J.C.Ho,J.H.Shieh	Pb,Sr,Pr,Cu,O	
10350	PR05003337	Sample number is #1.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1994																												Y123			A															K				87.5			87.5																																									A	by mutual inductance of concentric solenoid  coil	1700																																																									on SrTiO3 substrates. by laser ablaion method.Preparation of #1-#3 samples is same .	Crossover in temperature dependence of penetration depth ramda(T) in superconducting YBa2Cu3O7-z films	199408			Phys.Rev.B, 50(1994)3337	Ju Young Lee,Kathleen M.Paget,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,O	
10351	PR05003337	Sample number is #2.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1994																												Y123																		K				88.3			88.3																																				A						by mutual inductance of concentric solenoid coil.	1710																																																									on SrTiO3 substrates. by laser ablaion method.Preparation of #1-#3 samples is same .	Crossover in temperature dependence of penetration depth ramda(T) in superconducting YBa2Cu3O7-z films	199408			Phys.Rev.B, 50(1994)3337	Ju Young Lee,Kathleen M.Paget,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,O	
10352	PR05003337	Sample number is #3.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1994																												Y123																		K				86.7			86.7																																									A	by mutual inductance of concentric solenoid coil.	1630																																																									on SrTiO3 substrates. by laser ablaion method.Preparation of #1-#3 samples is same .	Crossover in temperature dependence of penetration depth ramda(T) in superconducting YBa2Cu3O7-z films	199408			Phys.Rev.B, 50(1994)3337	Ju Young Lee,Kathleen M.Paget,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,O	
10353	PR05203071		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-d	Nd	1.85	Ce	0.15	Cu	1															O	4-d		5	1995																												T'			A			12.08												K		18.2	21.6				18.2																				T		6.3																																																	mic.ohm.cm				170							740																		1200A thick. c-axis oriented. The substrate is SrTiO3.	PR05203071	199508		"Institut fu""r Physik, Universita""t Augsburg, Memminger Strasse 6, D-86135 Augsburg, Germany"	Phys.Rev.B,52(1995)3071	K. Samwer,P. Seng, J. Diehl,R. Tidecks,S. Horn,S. Klimm		
10354	PR05204427		Tl(Ba,Sr)LaCuO5+d	Tl1Sr1La1Cu1O5.09	Tl	1	Sr	1	La	1	Cu	1													O	5+d	5.09	1	1995																											2	Tl1201	P4/mmm		A	3.76		8.804	4											K		30					30																																																																																																See Phys. Rev. B 46, 6622 (1992).					Rodox mechanism for the generation of holes in TlBa1-xSrxLaCuO5+z:A neutron-diffraction study	199508			Phys.Rev.B,52(1995)4427	A. Sequeira,A. Sundaresan,L. C. Gupta,M. Sharon,Rajini Sharma	Tl, Ba, Sr, La, Cu, O	
10355	PR05204427		Tl(Ba,Sr)LaCuO5+d	Tl1Ba0.3Sr0.7La1Cu1O5.11	Tl	1	Ba	0.3	Sr	0.7	La	1	Cu	1											O	5+d	5.11	1	1995																											2	Tl1201	P4/mmm		A	3.787		8.853	4											K		25					25																																																																																																See Phys. Rev. B 46, 6622 (1992).					Rodox mechanism for the generation of holes in TlBa1-xSrxLaCuO5+z:A neutron-diffraction study	199508			Phys.Rev.B,52(1995)4427	A. Sequeira,A. Sundaresan,L. C. Gupta,M. Sharon,Rajini Sharma	Tl, Ba, Sr, La, Cu, O	
10356	PR05204427		Tl(Ba,Sr)LaCuO5+d	Tl1Ba0.6Sr0.4La1Cu1O5.16	Tl	1	Ba	0.6	Sr	0.4	La	1	Cu	1											O	5+d	5.16	1	1995																											2	Tl1201	P4/mmm		A	3.805		8.915	4											K		22					22																																																																																																See Phys. Rev. B 46, 6622 (1992).					Rodox mechanism for the generation of holes in TlBa1-xSrxLaCuO5+z:A neutron-diffraction study	199508			Phys.Rev.B,52(1995)4427	A. Sequeira,A. Sundaresan,L. C. Gupta,M. Sharon,Rajini Sharma	Tl, Ba, Sr, La, Cu, O	
10357	PR05204427	Electrical resistance measurement shows that the sample is a semiconductor.	Tl(Ba,Sr)LaCuO5+d	Tl1Ba1La1Cu1O5.17	Tl	1	Ba	1	La	1	Cu	1													O	5+d	5.17	1	1995																											2	Tl1201	P4/mmm		A	3.845		8.993	4																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Rodox mechanism for the generation of holes in TlBa1-xSrxLaCuO5+z:A neutron-diffraction study	199508			Phys.Rev.B,52(1995)4427	A. Sequeira,A. Sundaresan,L. C. Gupta,M. Sharon,Rajini Sharma	Tl, Ba, Sr, La, Cu, O	
10358	PR05203756	The sample is c-axis aligned.anisotropy factor=4.4 	HgBa2Ca2Cu3Oy	Hg1Ba2Ca2Cu3Oy	Hg	1	Ba	2	Ca	2	Cu	3													O	y		1	1995																												Hg1223																		K				135			135											Oe	Calculate from magnetisation data.		100	339					T	Calculate from magnetisation data.		390	88												A	Calculate from magnetisation data.		19.3	4.4	A	Calculate from magnetisation data.		1540	6800																																																	HgO, BaO, CaO, CuO		SIN (at 665C for 100h)ANN (at 300C in flowing oxygen for 12h)					Superconducting-state thermodynamic parameters and anisotropy of HgBa2Can-1CunOy by reversible magnetization measurements	199508			Phys.Rev.B,52(1995)3756	H. Yamauchi,K. Isawa,R. Puz'niak,R. Usami	Hg, Ba, Ca, Cu, O	
10359	PR05203756	The sample is c-axis aligned. anisotropy factor=4.0 	HgBa2CaCu2Oy	Hg1Ba2Ca1Cu2Oy	Hg	1	Ba	2	Ca	1	Cu	2													O	y		1	1995																												Hg1212																		K				127			127											Oe	Calculate from magnetisation data.		65	208					T	Calculate from magnetisation data.		455	113												A	Calculate from magnetisation data.		16.6	4.1	A	Calculate from magnetisation data.		2050	8250																																																	HgO, BaO, CaO, CuO		SIN (at 625C for 24h)ANN (at 300C in flowing oxygen for 12h)					Superconducting-state thermodynamic parameters and anisotropy of HgBa2Can-1CunOy by reversible magnetization measurements	199508			Phys.Rev.B,52(1995)3756	H. Yamauchi,K. Isawa,R. Puz'niak,R. Usami	Hg, Ba, Ca, Cu, O	
10360	PR05203756	The sample is c-axis aligned. anisotropy factor=1.8 	HgBa2CuOy	Hg1Ba2Cu1Oy	Hg	1	Ba	2	Cu	1															O	y		1	1995																												Hg1201																		K				96			96											Oe	Calculate from magnetisation data.		82	129					T	Calculate from magnetisation data.		125	72												A	Calculate from magnetisation data.		21.1	12.1	A	Calculate from magnetisation data.		2600	4540																																																	HgO, BaO, CuO		SIN (at 650C for 1h)ANN (at 300C in flowing oxygen for 12h)					Superconducting-state thermodynamic parameters and anisotropy of HgBa2Can-1CunOy by reversible magnetization measurements	199508			Phys.Rev.B,52(1995)3756	H. Yamauchi,K. Isawa,R. Puz'niak,R. Usami	Hg, Ba, Ca, Cu, O	
10361	PR05203711		YBa2Cu3O7-d	Y1Ba2Cu3O6.3	Y	1	Ba	2	Cu	3															O		6.3	1	1995									5.56			GPa		95.2	GPa		37.3	GPa		70.8		0.276																																																																																																																													Y2O3, BaCO3, CuO	1	SIN (for 4h at 935C in dry,CO2-free air)ANN (for 16h at 648C in 0.1% oxygen/balance air)					Elastik and nonlinear acoustic properties of YBa2Cu3O7-x ceramics with different oxygen contents	199508			Phys.Rev.B52,(1995)3711	D.P. Almond,G.A. Saunders,K.C. Goretta,M. Cankurtaran,Q. wang	Y, Ba, Cu, O	
10362	PR05203711		YBa2Cu3O7-d	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O		6.6	1	1995									5.365			GPa		97.9	GPa		40.1	GPa		58.5		0.221																																																																																																																													Y2O3, BaCO3, CuO	1	SIN (for 4h at 935C in dry,CO2-free air)ANN(for 16h at 521C in 0.1% oxygen/balance air)					Elastik and nonlinear acoustic properties of YBa2Cu3O7-x ceramics with different oxygen contents	199508			Phys.Rev.B52,(1995)3711	D.P. Almond,G.A. Saunders,K.C. Goretta,M. Cankurtaran,Q. wang	Y, Ba, Cu, O	
10363	PR05203711		YBa2Cu3O7-d	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O		6.94	1	1995									5.47			GPa		65.3	GPa		26.4	GPa		41.4		0.237																																																																																																																														1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Elastik and nonlinear acoustic properties of YBa2Cu3O7-x ceramics with different oxygen contents	199508			Phys.Rev.B52,(1995)3711	D.P. Almond,G.A. Saunders,K.C. Goretta,M. Cankurtaran,Q. wang	Y, Ba, Cu, O	
10364	PR05203742		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O		4	1	1995																											2	T'							3											K				22.5			22.5																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10365	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.999Ni0.001O4	Nd	1.85	Ce	0.15	Cu	0.999	Ni	0.001													O		4	1	1995																											2	T'							3											K				20			20																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10366	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.997Ni0.003O4	Nd	1.85	Ce	0.15	Cu	0.997	Ni	0.003													O		4	1	1995																											2	T'							3											K				16			16																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10367	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.995Ni0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Ni	0.005													O		4	1	1995																											2	T'							3											K				12			12																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10368	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.993Ni0.007O4	Nd	1.85	Ce	0.15	Cu	0.993	Ni	0.007													O		4	1	1995																											2	T'							3											K				8			8																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10369	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.993Ni0.007O4	Nd	1.85	Ce	0.15	Cu	0.993	Ni	0.007													O		4	1	1995																											2	T'							3											K				5.5			5.5																																																																																															1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10370	PR05203742		(Nd,Ce)2(Cu,Ni)O4	Nd1.85Ce0.15Cu0.992Ni0.009O4	Nd	1.85	Ce	0.15	Cu	0.992	Ni	0.009													O		4	1	1995																											2	T'							3											K																																																																																																						1	CAL (in air for 24h at 1000C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10371	PR05203742		(Nd,Ce)2(Cu,Fe)O4	Nd1.85Ce0.15Cu0.998Fe0.002O4	Nd	1.85	Ce	0.15	Cu	0.998	Fe	0.002													O		4	1	1995																											2	T'							3											K				19.5			19.5																																																																																															1	CAL (in air for 24h at 900C)SIN (at 1100C for 18h)ANN (for 36h under flowing gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10372	PR05203742		(Nd,Ce)2(Cu,Fe)O4	Nd1.85Ce0.15Cu0.995Fe0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Fe	0.005													O		4	1	1995																											2	T'							3											K				16.5			16.5																																																																																															1	CAL (in air for 24h at 900C)SIN (at 1100C for 18h)ANN (for 36h under flowing gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10373	PR05203742		(Nd,Ce)2(Cu,Fe)O4	Nd1.85Ce0.15Cu0.99Fe0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Fe	0.01													O		4	1	1995																											2	T'							3											K				13			13																																																																																															1	CAL (in air for 24h at 900C)SIN (at 1100C for 18h)ANN (for 36h under flowing gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10374	PR05203742		(Nd,Ce)2(Cu,Fe)O4	Nd1.85Ce0.15Cu0.985Fe0.015O4	Nd	1.85	Ce	0.15	Cu	0.985	Fe	0.015													O		4	1	1995																											2	T'							3											K				6.5			6.5																																																																																															1	CAL (in air for 24h at 900C)SIN (at 1100C for 18h)ANN (for 36h under flowing gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10375	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.995Zn0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Zn	0.005													O		4	1	1995																											2	T'							3											K				18			18																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10376	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.99Zn0.01O4	Nd	1.85	Ce	0.15	Cu	0.99	Zn	0.01													O		4	1	1995																											2	T'							3											K				15.5			15.5																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10377	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.987Zn0.013O4	Nd	1.85	Ce	0.15	Cu	0.987	Zn	0.013													O		4	1	1995																											2	T'							3											K				14.5			14.5																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10378	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.985Zn0.015O4	Nd	1.85	Ce	0.15	Cu	0.985	Zn	0.015													O		4	1	1995																											2	T'							3											K				14			14																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10379	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.98Zn0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Zn	0.02													O		4	1	1995																											2	T'							3											K				13			13																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10380	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.975Zn0.025O4	Nd	1.85	Ce	0.15	Cu	0.975	Zn	0.025													O		4	1	1995																											2	T'							3											K				12			12																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10381	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.97Zn0.03O4	Nd	1.85	Ce	0.15	Cu	0.97	Zn	0.03													O		4	1	1995																											2	T'							3											K				11			11																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10382	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.96Zn0.04O4	Nd	1.85	Ce	0.15	Cu	0.96	Zn	0.04													O		4	1	1995																											2	T'							3											K				9.5			9.5																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10383	PR05203742		(Nd,Ce)2(Cu,Zn)O4	Nd1.85Ce0.15Cu0.95Zn0.05O4	Nd	1.85	Ce	0.15	Cu	0.95	Zn	0.05													O		4	1	1995																											2	T'							3											K				8			8																																																																																															1	CAL (in air for 24h at 1100C)SIN (at 1100C for 18h)ANN (for 36h under flowing nitrogen gas)					Magnetism of  Ni, and Zn in Nd1.85Ce0.15CuO4: Cmparison of experiment and theory	199508			Phys.Rev.B,52(1995)3742	B. Jayaram,H. Chen,J. Callaway	Fe, Ni, Zn, Nd, Ce, Cu, O	
10384	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu3O6.63	Y	1	Ba	2	Cu	3															O	7-y	6.63	3	1995																																														K	62						62																																																																							mic.ohm.cm					80	280000						540	50000	m3/C	0.0000000022								CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10385	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.97Zn0.03O6.63	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-y	6.63	3	1995																																														K	40						40																																																																							mic.ohm.cm					190							660		m3/C	0.0000000025					RH10385			CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10386	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.94Zn0.06O6.63	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y	6.63	3	1995																																														K	20						20																																																																							mic.ohm.cm					250	250000						800	60000	m3/C	0.0000000026					RH10386			CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10387	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.91Zn0.09O6.63	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-y	6.63	3	1995																																																																																																																												mic.ohm.cm		400			430							920											CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10388	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.91Zn0.09O6.63	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-y	6.63	3	1995																																																																																																																												mic.ohm.cm		520			470							970											CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10389	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.88Zn0.12O6.63	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-y	6.63	3	1995																																																																																																																												mic.ohm.cm		740			570							1110		m3/C	0.0000000028					RH10389			CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10390	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu3O6.03	Y	1	Ba	2	Cu	3															O	7-y	6.03	3	1995																																														K	92						92																																																																							mic.ohm.cm														m3/C	0.0000000006					RH10390			CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10391	PR05203884		YBa2(Cu,Zn)3O7-y	Y1Ba2Cu2.94Zn0.06O6.03	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y	6.03	3	1995																																																																																																																												mic.ohm.cm														m3/C	0.0000000008					RH10391			CuO, BaO							Effect of Zn doping on charge transport in YBa2Cu3O7-y	199508			Phys.Rev.B,52(1995)R3884	K. Mizuhashi,K. Tatenaka,S. uchida,Y. fukuzumi	Zn, Y, Ba, Cu, O	
10400	PR05007234		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																									by laser ablation method.BaF2 post-annealing process.	Sign reversals in the vortex-state Hall effect in Y-Ba-Cu-O: Correlations with the normal-state   Seebeck coefficient	199409			Phys.Rev.B,50 (1994) 7234-7237	Brian C.Sales,David Christen,Edwin C.Jones	Y,Ba,Cu,O	
10401	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1La1Cu1O5	Tl	1	Ba	1	La	1	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10402	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1.1La0.9Cu1O5	Tl	1	Ba	1.1	La	0.9	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10403	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5	Tl	1	Ba	1.2	La	0.8	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10404	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1.3La0.7Cu1O5	Tl	1	Ba	1.3	La	0.7	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10405	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1.4La0.6Cu1O5	Tl	1	Ba	1.4	La	0.6	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10406	PR05006402		Tl(Ba,La)2CuO5	Tl1Ba1.5La0.5Cu1O5	Tl	1	Ba	1.5	La	0.5	Cu	1													O		5	1	1994																																																																																																																																																			BaCO3,La2O3,CuO,Tl2O3	1	CAL(precursor,950-980,20-30h) - MIX(Tl2O3 + precursor, Tl:BaLaCuO=1.2 : 1)-SIN(890C-910C,10-15h)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10407	PR05006534		YBa2Cu3O7-d	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O		6.68	3	1994																																														K		63				3	63																																																																																															5	Y2O3 crucible, untwined crystal is obtained by picking up as-grown twin free cryatals or by applying uniaxial stress on the twinned cryatal. oxygen content -> ANN(600C,12h,quartz tube with 10g YBCO po					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10408	PR05006534		YBa2Cu3O7-d	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O		6.78	3	1994																																														K		82				2	82																																																																																															5	Y2O3 crucible, untwined crystal is obtained by picking up as-grown twin free cryatals or by applying uniaxial stress on the twinned cryatal. oxygen content -> ANN(600C,12h,quartz tube with 10g YBCO po					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10409	PR05006534		YBa2Cu3O7-d	Y1Ba2Cu3O6.88	Y	1	Ba	2	Cu	3															O		6.88	3	1994																																														K		92				1	92																																																																																															5	Y2O3 crucible, untwined crystal is obtained by picking up as-grown twin free cryatals or by applying uniaxial stress on the twinned cryatal. oxygen content -> ANN(600C,12h,quartz tube with 10g YBCO po					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10410	PR05006534		YBa2Cu3O7-d	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O		6.93	3	1994																																														K		92				1	92																																																																																															5	Y2O3 crucible, untwined crystal is obtained by picking up as-grown twin free cryatals or by applying uniaxial stress on the twinned cryatal. oxygen content -> ANN(600C,12h,quartz tube with 10g YBCO po					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10411	PR05007099	Temperature of substrate is 593C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10412	PR05007099	Temperature of substrate is 604C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10413	PR05007099	Temperature of substrate is 608C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10414	PR05007099	Temperature of substrate is 630C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10415	PR05007099	Temperature of substrate is 671C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10416	PR05007099	Temperature of substrate is 706C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10417	PR05007099	Temperature of substrate is 725C for this sample.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1994																																																																																																																																																				16				Y:Ba:Cu = 1.05:2.00:3.85	by rf magnetron sputtering only.  MgO substrate.Film thickness is 1500A.	Systematic study of the growth-temperature dependence pf structural disorder and superconductivity in YBa2Cu3O7-z thin films	199409			Phys.Rev.B,50 (1994) 7099	Jinhua Ye,Keikichi Nakanura	Y,Ba,Cu,O	
10418	PR05006534	abres = for parallel to a-axis	YBa2Cu3O7	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	z	6.68	3	1994																												Y123																		K		63				3	63																																																																							m.ohm.cm												0.7	50											5	Y2O3 crucible,untwinned crystal by picking up as-grown twin free crystal or applying uniaxial stress, oxygen content by ANN(600C,12H in quartz tube with 10g YBCO polycrystalline)					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10419	PR05006534	abres = for parallel to a-axis	YBa2Cu3O7	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O	z	6.78	3	1994																												Y123																		K		82				2	82																																																																							m.ohm.cm												0.48	22											5	Y2O3 crucible,untwinned crystal by picking up as-grown twin free crystal or applying uniaxial stress, oxygen content by ANN(600C,12H in quartz tube with 10g YBCO polycrystalline)					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10420	PR05006534	abres = for //a-axis	YBa2Cu3O7	Y1Ba2Cu3O6.88	Y	1	Ba	2	Cu	3															O	z	6.88	3	1994																												Y123																		K		92				1	92																																																																							m.ohm.cm												0.31	10											5	Y2O3 crucible,untwinned crystal by picking up as-grown twin free crystal or applying uniaxial stress, oxygen content by ANN(600C,12H in quartz tube with 10g YBCO polycrystalline)					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10421	PR05006534	abres = for //a-axis	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	z	6.93	3	1994																												Y123																		K		92				1	92																																																																							m.ohm.cm												0.22	5.2											5	Y2O3 crucible,untwinned crystal by picking up as-grown twin free crystal or applying uniaxial stress, oxygen content by ANN(600C,12H in quartz tube with 10g YBCO polycrystalline)					Interplace charge transport in YBa2Cu3O7-y: Spin-gap effect on in-place and out-of-plane resistivity	199409			Phys.Rev.B,50 (1994) 6534	H.Takagi,K.Mizuhashi,K.Takenaka,S.Uchida	Y,Ba,Cu,O	
10422	PR05006402	Tl:Ba:La:Cu=0.98:1.01:0.99:1.00 by EPMA	Tl(Ba,La)2CuO5	Tl1Ba1La1Cu1O5	Tl	1	Ba	1	La	1	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.85		9.025												K					4.2																																																																																							m3/C						RH10422				1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10423	PR05006402	Tl:Ba:La:Cu=1.00:1.13:0.87:1.03 by EPMA	Tl(Ba,La)2CuO5	Tl1Ba1.1La0.9Cu1O5	Tl	1	Ba	1.1	La	0.9	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.844		9.068												K	34.3	38.4	45.3			11	38.4																																																																																					m3/C						RH10423				1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10424	PR05006402	Tl:Ba:La:Cu=1.05:1.18:0.82:0.99	Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.84		9.114												K	40	45	49.1			9.1	45																																																																																					m3/C						RH10424				1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10425	PR05006402	Tl:Ba:La:Cu=1.07:1.27:0.73:0.93	Tl(Ba,La)2CuO5	Tl1Ba1.3La0.7Cu1O5	Tl	1	Ba	1.3	La	0.7	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.838		9.137												K	30.1	38.8	45.4			15.3	38.8																																																																																					m3/C						RH10425				1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10426	PR05006402	Tl:Ba:La:Cu=1.10:1.43:0.57:0.95	Tl(Ba,La)2CuO5	Tl1Ba1.4La0.6Cu1O5	Tl	1	Ba	1.4	La	0.6	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.838		9.162												K	20.2	24	28.5			8.3	24																																																																																					m3/C						RH10426				1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10427	PR05006402	Tl:Ba:La:Cu=1.07:1.51:0.49:0.92	Tl(Ba,La)2CuO5	Tl1Ba1.5La0.5Cu1O5	Tl	1	Ba	1.5	La	0.5	Cu	1													O	5		1	1994																											2	Tl1201	p4/mmm	123	A	3.845		9.285												K					4.2																																																																																							m3/C										1	precursor(BaCO3,La2O3,CuO)-CAL(950-980C,20-30H)-MIX(Tl2O3 and precursor, Tl:BaLaCuO=1.2:1)-SIN(890C-910C,10-15H)					Preparation and transport properties of single-phase TlBa1+xLa1-XCuO5(0<x<0.5)	199409			Phys.Rev.B.50 (1994) 6402	Takashi Manako,Yoshimi kubo	Tl,Ba,La,Cu,O	
10428	PR05006375		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7	7	1	1994									5.31																																																																																																													THC10428																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10429	PR05006375		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7	7	1	1994									4.85																																																																																																													THC10429																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10430	PR05006375		YBa2Cu3O6	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	z	6	1	1994																																																																																																																						THC10430																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10431	PR05006375		YBa2(Cu,Al)3O7	Y1Ba2Cu2.94Al0.06Oz	Y	1	Ba	2	Cu	2.94	Al	0.06													O	z		1	1994																																																																																																																						THC10431																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10432	PR05006375		YBa2(Cu,Al)3O7	Y1Ba2Cu2.7Al0.3Oz	Y	1	Ba	2	Cu	2.7	Al	0.3													O	z		1	1994																																																																																																																						THC10432																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10433	PR05006375		(Y,Gd)Ba2Cu3O7	Y0.3Gd0.7Ba2Cu3Oz	Y	0.3	Gd	0.7	Ba	2	Cu	3													O	z		1	1994																																																																																																																																																				1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10434	PR05006375	THCFIG  is normalized by THC(180K)	(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3Oz	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z		1	1994																																																																																																																						THC10434																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10435	PR05006375	THCFIG is normalized by THC(180K)	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3Oz	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z		1	1994																																																																																																																						THC10435																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10436	PR05006375	THCFIG is normalized by THC(180K)	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3Oz	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z		1	1994																																																																																																																						THC10436																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10437	PR05006375	THCFIG is normalized by THC(180K)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03Oz	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	z		1	1994																																																																																																																						THC10437																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10438	PR05006375	THCFIG is normalized by THC(180K)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06Oz	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	z		1	1994																																																																																																																						THC10438																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10439	PR05006375	THCFIG is normalized by THC(180K)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.82Zn0.18Oz	Y	1	Ba	2	Cu	2.82	Zn	0.18													O	z		1	1994																																																																																																																						THC10439																														1	standard solid state reaction, in details see Phys.Rev.B.,40(1989)4453 and J.Supercond. 1(1988)63					Thermal conductivity of impurity-doped high-Tc superconductors	199409			Phys.Rev.B,50 (1994) 6375	J.E.Crow,P.Pernambuco-Wise,S.T.Ting	Pr,Gd,Y,Ba,Cu,O,Zn,Al	
10500	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu1Ba2Cu4O8	Eu	1	Ba	2	Cu	4															O	8		2	1994																											3	Y124							3											K	70		71				70.5																																																																							m.ohm.cm					0.3							1.7											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10501	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu0.8Pr0.2Ba2Cu4O8	Eu	0.8	Pr	0.2	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	60		67				63.5																																																																							m.ohm.cm					1.2							3.1											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10502	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu0.6Pr0.4Ba2Cu4O8	Eu	0.6	Pr	0.4	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	36		44				40																																																																							m.ohm.cm					4.1							6.1											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10503	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu0.5Pr0.5Ba2Cu4O8	Eu	0.5	Pr	0.5	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	15		40				27.5																																																																							m.ohm.cm					11.6							10											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10504	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu0.4Pr0.6Ba2Cu4O8	Eu	0.4	Pr	0.6	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3																																																																																									m.ohm.cm		18.6			24							18											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10505	PR05010265		(Eu,Pr)Ba2Cu4O8	Eu0.3Pr0.7Ba2Cu4O8	Eu	0.3	Pr	0.7	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3																																																																																									m.ohm.cm					1700							800											Eu2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2)See Phys. Rev. B 46, 3573 (1992).					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10506	PR05010265		(Y,Pr)Ba2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		2	1994																											3	Y124			A	3.83	3.87	27.16	3											K	80		81				80.5																																																																							m.ohm.cm												2											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10507	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.9Pr0.1Ba2Cu4O8	Y	0.9	Pr	0.1	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	72		73				72.5																																																																							m.ohm.cm												2.6											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10508	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	69		72				70.5																																																																																														Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10509	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.7Pr0.3Ba2Cu4O8	Y	0.7	Pr	0.3	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	65		68				66.5																																																																							m.ohm.cm					2							3.8											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10510	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.6Pr0.4Ba2Cu4O8	Y	0.6	Pr	0.4	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	57		63				60																																																																							m.ohm.cm					2.9							5											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10511	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.5Pr0.5Ba2Cu4O8	Y	0.5	Pr	0.5	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	50		55				52.5																																																																							m.ohm.cm					3.4							6.2											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10512	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.4Pr0.6Ba2Cu4O8	Y	0.4	Pr	0.6	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	37		44				40.5																																																																							m.ohm.cm					4.8							8.4											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10513	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.3Pr0.7Ba2Cu4O8	Y	0.3	Pr	0.7	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3											K	18		40				29																																																																							m.ohm.cm					10.4							10.6											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10514	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.2Pr0.8Ba2Cu4O8	Y	0.2	Pr	0.8	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3																																																																																									m.ohm.cm					31.5							18.6											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10515	PR05010265		(Y,Pr)Ba2Cu4O8	Y0.1Pr0.9Ba2Cu4O8	Y	0.1	Pr	0.9	Ba	2	Cu	4													O	8		2	1994																											3	Y124							3																																																																																									m.ohm.cm		2400			800							1160											Y2O3, Ba(NO3)2, CuO, Pr6O11	1	SIN (at 900C, for 12h, in O2).SIN (at 820C, for 48h, in flowing O2).See Phys. Rev. B 46, 3573.					Superconductivity of the Pr-doped(Y,Eu) Ba2Cu4O8 system	199409			Phys.Rev.B,50 (1994) 10265	A.V.Narlikar,Ratan Lal,S.K.Agarwal,S.P.Pandey,V.P.S.Awana	Y,Eu,Ba,Cu,o,Pr	
10516	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.8La0.2Cu1O5	Tl	1	Ba	1.8	La	0.2	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.854		9.3	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10517	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.6La0.4Cu1O5	Tl	1	Ba	1.6	La	0.4	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.848		9.23	3											K			34				34																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10518	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.5La0.5Cu1O5	Tl	1	Ba	1.5	La	0.5	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.846		9.19	3											K			35				35																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10519	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.4La0.6Cu1O5	Tl	1	Ba	1.4	La	0.6	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.843		9.11	3											K			38				38																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10520	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.3La0.7Cu1O5	Tl	1	Ba	1.3	La	0.7	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.844		9.1	3											K			40				40																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10521	PR05010238		Tl(Ba,La)2CuO5	Tl1Ba1.2La0.8Cu1O5	Tl	1	Ba	1.2	La	0.8	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.84		9.06	3											K			30				30																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10522	PR05010238		Tl(Sr,La)2CuO5	Tl1Sr1.6La0.4Cu1O5	Tl	1	Sr	1.6	La	0.4	Cu	1													O	5		2	1994																											2	Tl1201	P4/mmm		A	3.748		8.913	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10523	PR05010238		Tl(Sr,La)2CuO5	Tl1Sr1.4La0.6Cu1O5	Tl	1	Sr	1.4	La	0.6	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.753		8.898	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10524	PR05010238		Tl(Sr,La)2CuO5	Tl1Sr1.2La0.8Cu1O5	Tl	1	Sr	1.2	La	0.8	Cu	1													O	5		1	1994																											2	Tl1201	P4/mmm		A	3.771		8.863	3											K			27				27																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10525	PR05010238		Tl(Sr,La)2CuO5	Tl1Sr1La1Cu1O8	Tl	1	Sr	1	La	1	Cu	1													O	8		1	1994																											2	Tl1201	P4/mmm		A	3.779		8.864	3											K			32				32																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10526	PR05010238		TlBa2(Ca,Gd)Cu2O7	Tl1Ba2Ca0.7Gd0.3Cu2O7	Tl	1	Ba	2	Ca	0.7	Gd	0.3	Cu	2											O	7		1	1994																											2	Tl1212	P4/mmm		A	3.867		12.601	3											K			78				78																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10527	PR05010238		TlBa2GdCu2O7	Tl1Ba2Gd1Cu2O7	Tl	1	Ba	2	Gd	1	Cu	2													O	7		1	1994																											2	Tl1212	P4/mmm		A	3.899		12.296	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10528	PR05010238		TlSr2(Ca,Gd)Cu2O7	Tl1Sr2Ca0.6Gd0.4Cu2O7	Tl	1	Sr	2	Ca	0.6	Gd	0.4	Cu	2											O	7		1	1994																											2	Tl1212	P4/mmm		A	3.808		12.081	3											K			65				65																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10529	PR05010238		TlSr2(Ca,Gd)Cu2O7	Tl1Sr2Ca0.4Gd0.6Cu2O7	Tl	1	Sr	2	Ca	0.4	Gd	0.6	Cu	2											O	7		1	1994																											2	Tl1212	P4/mmm		A	3.816		12.046	3											K			60				60																																																																																																See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10530	PR05010238		TlSr2(Ca,Gd)Cu2O7	Tl1Sr2Ca0.2Gd0.8Cu2O7	Tl	1	Sr	2	Ca	0.2	Gd	0.8	Cu	2											O	7		1	1994																											2	Tl1212	P4/mmm		A	3.828		12.047	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10531	PR05010238		TlSr2(Ca,Gd)Cu2O7	Tl1Sr2Gd1Cu2O7	Tl	1	Sr	2	Gd	1	Cu	2													O	7		1	1994																											2	Tl1212	P4/mmm		A	3.833		12.021	3																																																																																																																		See Phys. Rev. B 46, 6622 (1992).					Superconductivity and valence state of Tl in TlA2-XLaxCuO5 and TlA2Ca1-xGdxCu2O7(A=Ba,Sr)	199409			Phys.Rev.B,50 (1994) 10238	A.Sundaresan,C.S.Gopinath,L.C.Gupta,M.Sharon,R.Pinto,R.Vijayaraghavan,S.Subramaian	Tl,Ba,Sr,La,Cu,O	
10532	PR05010157	isomorphic to T* structure 	(Y,Ce)2Sr2CuFeO8	Y1.34Ce0.66Sr2Cu1Fe1O8	Y	1.34	Ce	0.66	Sr	2	Cu	1	Fe	1											O	8		1	1994					micro.B/Mo	3.6		187																			2	T*	P4mm	99	A	3.824		12.563	3																																																																																																																Y2O3, CeO2, SrCO3, CuO, Fe2O3	1	Ann (in air, at 1125C, for 24h) for ceveral times.Quench to room tempetature.					"Mo""ssbauer, crystal-structure, magnetic, and Raman studies of the (Y,Ce)2Sr2CuFeO8 compound ismorphic to superconductors with the T* structure"	199410		Institute of Materials Science National Research Center for Physical Sciences Demokritos, 153 10 Agia Paraskevi, Attiki, Greece	Phys.Rev.B,50(1994)10157	A. Kostikas,A. Simopoulos,C. Mitros,D. Niarchos,M. Pissas		
10533	PR05009672		(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1994																												Y123																		K			93			0.3	93																																									nm	The Penetration Length is evaluated from the conductivity, using a two fluid model.	170							60000000	1000000																				m.ohm.cm												0.35												16		2			The Substrates are NdGaO3.The Film Thicknesses are about 150nm.	Anomalous behavior of the complex conductivity of Y1-XPrxBa2Cu3O7 observed with THz spectroscopy	199409			Phys.Rev.B,50 (1994) 9672	H.-U.Habermeier,I.E.Trofimov,J.Kuhl,J.O.White,R.Buhleier,S.D.Brorson	Y,Pr,Ba,Cu,O	
10534	PR05009672		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7		5	1994																																														K			68				68																																									nm	The Penetration Length is evaluated from the conductivity, using a two fluid model.	350																												m.ohm.cm					0.17							0.45												16		2			The Substrates are NdGaO3.The Film Thicknesses are about 150nm.	Anomalous behavior of the complex conductivity of Y1-XPrxBa2Cu3O7 observed with THz spectroscopy	199409			Phys.Rev.B,50 (1994) 9672	H.-U.Habermeier,I.E.Trofimov,J.Kuhl,J.O.White,R.Buhleier,S.D.Brorson	Y,Pr,Ba,Cu,O	
10535	PR05009672		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7		5	1994																																														K			53				53																																									nm	The Penetration Length is evaluated from the conductivity, using a two fluid model.	375																												m.ohm.cm					0.2							0.5												16		2			The Substrates are NdGaO3.The Film Thicknesses are about 150nm.	Anomalous behavior of the complex conductivity of Y1-XPrxBa2Cu3O7 observed with THz spectroscopy	199409			Phys.Rev.B,50 (1994) 9672	H.-U.Habermeier,I.E.Trofimov,J.Kuhl,J.O.White,R.Buhleier,S.D.Brorson	Y,Pr,Ba,Cu,O	
10536	PR05009672		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7		5	1994																																														K			40			3	40																																									nm	The Penetration Length is evaluated from the conductivity, using a two fluid model.	375																												m.ohm.cm					0.32							0.62												16		2			The Substrates are NdGaO3.The Film Thicknesses are about 150nm.	Anomalous behavior of the complex conductivity of Y1-XPrxBa2Cu3O7 observed with THz spectroscopy	199409			Phys.Rev.B,50 (1994) 9672	H.-U.Habermeier,I.E.Trofimov,J.Kuhl,J.O.White,R.Buhleier,S.D.Brorson	Y,Pr,Ba,Cu,O	
10537	PR05009627	anisotropy factor r = 10 	Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.7Ca0.3Cu3O8+d	Pb	2	Sr	2	Y	0.7	Ca	0.3	Cu	3											O	8+d		3	1994																																														K				79		8	79																																									nm	The Penetration Length is evaluated from the conductivity, using a two fluid model.	590																																																				5	The samples were prepared by a PbO/NaCl flux method.ANN (in N2, at 500C, for 100h).					Anisotropy of superconducting Pb2Sr2(Y0.7Ca0.3)Cu3O8+z and Pb2Sr2Y1-yCu3O8+z	199409			Phys.Rev.B,50 (1994) 9627	J.E.Greedan,J.S.Xue,M.W.Fok,T.R.Chien,W.R.Datars	Pb,Sr,Y,Ca,Cu,O	
10538	PR05009627	Y-content nearly equal 0.1. anisotropy factor r = 11.3 	Pb2Sr2YCu3O8	Pb2Sr2Y0.1Cu3O8+d	Pb	2	Sr	2	Y	0.1	Cu	3													O	8+d		3	1994																																														K				70		7	70																																																																																															5	The samples were prepared by a PbO/NaCl flux method.ANN (in N2, at 500C, for 100h).					Anisotropy of superconducting Pb2Sr2(Y0.7Ca0.3)Cu3O8+z and Pb2Sr2Y1-yCu3O8+z	199409			Phys.Rev.B,50 (1994) 9627	J.E.Greedan,J.S.Xue,M.W.Fok,T.R.Chien,W.R.Datars	Pb,Sr,Y,Ca,Cu,O	
10539	PR05009627	anisotropy factor r = 13.  	Pb2Sr2(Sm,Eu)Cu3O8	Pb2Sr2Sm0.5Eu0.5Cu3O8+d	Pb	2	Sr	2	Sm	0.5	Eu	0.5	Cu	3											O	8+d		3	1994																																														K				45		25	45																																																																																															5	The samples were prepared by a PbO/NaCl flux method.ANN (in N2, at 500C, for 100h).					Anisotropy of superconducting Pb2Sr2(Y0.7Ca0.3)Cu3O8+z and Pb2Sr2Y1-yCu3O8+z	199409			Phys.Rev.B,50 (1994) 9627	J.E.Greedan,J.S.Xue,M.W.Fok,T.R.Chien,W.R.Datars	Pb,Sr,Y,Ca,Cu,O	
10540	PR05009619		Pb2Sr2TbCu3O8	Pb2Sr2Tb1Cu3O8+d	Pb	2	Sr	2	Tb	1	Cu	3													O	8+d			1994					micro.B/Mo	10.04		5.3																				Pb3212																																																																																																																									See Jpn.J.Appl.Phys. 32, L1225 (1993).					Calorimetric studies on the magnetic order of Pb2Sr2TbCu3O8+z	199409			Phys.Rev.B,50 (1994) 9619	C.R.Shih,H.D.Yang,T.H.Meen,Y.C.Chen	Pb,Sr,Tb,Cu,O	
10541	PR05009503		(Sr,Nd)CuO2	Sr0.875Nd0.125Cu1O2-d	Sr	0.875	Nd	0.125	Cu	1															O	2-d		5	1994																											2		P4/mmm	123	A	3.92		3.419	1											K			20				20																																																																							m.ohm.cm												0.6												16		2			The sample was prepared by Pulsed Laser Deposition method. The Substrate was SrTiO3(100).	Crystal sturucture of Sr0.875Nd0.125CuO2-z superconducting thin films	199409			Phys.Rev.B,50 (1994) 9503	H.Yamauchi,Mitsuru Izumi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10542	PR05009503		(Sr,Nd)CuO2	Sr0.875Nd0.125Cu1O2-d	Sr	0.875	Nd	0.125	Cu	1															O	2-d		5	1994																											2		P4/mmm	123	A	3.918		3.418	1											K			20				20																																																																							m.ohm.cm												0.6												16		2			The sample was prepared by Pulsed Laser Deposition method. The Substrate was SrTiO3(100).	Crystal sturucture of Sr0.875Nd0.125CuO2-z superconducting thin films	199409			Phys.Rev.B,50 (1994) 9503	H.Yamauchi,Mitsuru Izumi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10543	PR05009397	The Sample is directly deposited on Substrate.	(Sr,Nd)CuO2	Sr1Cu1O2-d	Sr	1	Cu	1																	O	2-d		5	1994																															A	3.903		3.448	1																																																																																									ohm.cm					2							0.13												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10544	PR05009397	The Sample is directly deposited on Substrate.	(Sr,Nd)CuO2	Sr0.955Nd0.045Cu1O2-d	Sr	0.955	Nd	0.045	Cu	1															O	2-d		5	1994																															A	3.907		3.442	1																																																																																									m.ohm.cm					2.5							3												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10545	PR05009397	The Sample is directly deposited on Substrate.	(Sr,Nd)CuO2	Sr0.925Nd0.075Cu1O2-d	Sr	0.925	Nd	0.075	Cu	1															O	2-d		5	1994																															A	3.91		3.429	1																																																																																									m.ohm.cm					2.3							0.9												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10546	PR05009397	The Sample is directly deposited on Substrate.	(Sr,Nd)CuO2	Sr0.9Nd0.1Cu1O2-d	Sr	0.9	Nd	0.1	Cu	1															O	2-d		5	1994																															A	3.912		3.425	1											K			10				10																																																																							m.ohm.cm					1.3							0.6												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10547	PR05009397	The Sample is directly deposited on Substrate.	(Sr,Nd)CuO2	Sr0.875Nd0.125Cu1O2-d	Sr	0.875	Nd	0.125	Cu	1															O	2-d		5	1994																															A	3.918		3.418	1											K			20				20																																																																							m.ohm.cm					1.2							0.6												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10548	PR05009397	The Sample was deposited with Pr2CuO4 underlayer.	(Sr,Nd)CuO2	Sr0.95Nd0.05Cu1O2-d	Sr	0.95	Nd	0.05	Cu	1															O	2-d		5	1994																															A	3.929		3.438	1																																																																																									m.ohm.cm					60							23												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10549	PR05009397	The Sample was deposited with Pr2CuO4 underlayer.	(Sr,Nd)CuO2	Sr0.875Nd0.125Cu1O2-d	Sr	0.875	Nd	0.125	Cu	1															O	2-d		5	1994																															A	3.946		3.408	1																																																																																									m.ohm.cm					0.3							0.3												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10550	PR05009397	The Sample was deposited with Nd2CuO4 underlayer.	(Sr,Nd)CuO2	Sr0.95Nd0.05Cu1O2-d	Sr	0.95	Nd	0.05	Cu	1															O	2-d		5	1994																															A	3.933		3.443	1																																																																																									m.ohm.cm					11							6												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10551	PR05009397	The Sample was deposited with Nd2CuO4 underlayer.	(Sr,Nd)CuO2	Sr0.875Nd0.125Cu1O2-d	Sr	0.875	Nd	0.125	Cu	1															O	2-d		5	1994																															A	3.931		3.418	1																																																																																									m.ohm.cm					2.2							1.5												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10552	PR05009397	The Sample was deposited with Sm2CuO4 underlayer.	(Sr,Nd)CuO2	Sr0.95Nd0.05Cu1O2-d	Sr	0.95	Nd	0.05	Cu	1															O	2-d		5	1994																															A	3.909		3.459	1																																																																																									m.ohm.cm					6000							60												16		2			The samples were prepared by Pulsd Laser Deposition Method. The Targets were Prepared by Solid-state reaction method.  The Substrate was SrTiO3(100). The film thicknesses are appximately 450A.	In-plane thermoelectic power of c-axis-oriented Sr1-xNdxCuO2-z thin films	199409			Phys.Rev.B,50 (1994) 9397	H.Yamauchi,Nobuyuki Sugii	Sr,Nd,Cu,O	
10553	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.03	Hg	1	Ba	2	Cu	1															O		4.03	1	1994																											2	Hg1201																		K			1				1																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10554	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.09	Hg	1	Ba	2	Cu	1															O		4.09	1	1994																											2	Hg1201																		K			50				50																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10555	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.17	Hg	1	Ba	2	Cu	1															O		4.17	1	1994																											2	Hg1201																		K			78				78																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10556	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.18	Hg	1	Ba	2	Cu	1															O		4.18	1	1994																											2	Hg1201																		K			97				97																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10557	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.28	Hg	1	Ba	2	Cu	1															O		4.28	1	1994																											2	Hg1201																		K			80				80																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10558	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.28	Hg	1	Ba	2	Cu	1															O		4.28	1	1994																											2	Hg1201																		K			87				87																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10559	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.36	Hg	1	Ba	2	Cu	1															O		4.36	1	1994																											2	Hg1201																		K			40				40																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10560	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.39	Hg	1	Ba	2	Cu	1															O		4.39	1	1994																											2	Hg1201																		K			22				22																																																																																														BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10561	PR05010346		HgBa2CuO4+d	Hg1Ba2Cu1O4.32	Hg	1	Ba	2	Cu	1															O		4.32	1	1994																											2	Hg1201																																																																																																																							BaO, CuO, Hg	1	The Sample was Synthesized by reacting precursor pellet of Ba2CuOx and a composite Hg source together. The precursor is obtained by repeatedly heating and pulverizing a mixture of BaO and CuO in flowi					Unusual hole dependence of Tc in HgBa2CuO4+delta	199410		Department of Physics and the Texas Center for Superconductivity at the University of Houston, Texas 77204-5932	Phys.Rev.B,50(1994)10346	A. Jacobson,C.W. Chu,F. Chen,J. Gibson,L.M. Liu,Q. Xiong,Y. Cao,Y.Y. Sun,Y.Y. Xue		
10562	PR05010080		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-y	Sm	1.85	Ce	0.15	Cu	1															O	4-y		1	1994																												T'							3											K			20.5				20.5																																																																																															11	See J. Alloys Compounds 199, 105 (1993).SIN (in flowing He at 950C for 20h).FNC (for 1h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10563	PR05010080		(Sm,Ce)2CuO4	Sm1.84Ce0.16Cu1O4-y	Sm	1.84	Ce	0.16	Cu	1															O	4-y		1	1994																												T'							3											K			21				21																																																																																															11	See J. Alloys Compounds 199, 105 (1993).SIN (in flowing He at 950C for 20h).FNC (for 1h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10564	PR05010080		(Sm,Ce)2CuO4	Sm1.83Ce0.17Cu1O4-y	Sm	1.83	Ce	0.17	Cu	1															O	4-y		1	1994																												T'							3											K			18.3				18.3																																																																																															11	See J. Alloys Compounds 199, 105 (1993).SIN (in flowing He at 950C for 20h).FNC (for 1h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10565	PR05010080		(Sm,Ce)2CuO4	Sm1.82Ce0.18Cu1O4-y	Sm	1.82	Ce	0.18	Cu	1															O	4-y		2	1994																												T'							3											K			16.8				16.8																																																																																															11	See J. Alloys Compounds 199, 105 (1993).SIN (in flowing He at 950C for 20h).FNC (for 1h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10566	PR05010080		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-y	Sm	1.85	Ce	0.15	Cu	1															O	4-y		1	1994																												T'							3											K			23.3				23.3																																																																																															11	See J. Alloys Compounds 199, 105 (1993).ANN (in flowing He, at 950C, for 20h).FNC (for 2h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10567	PR05010080		(Sm,Ce)2CuO4	Sm1.84Ce0.16Cu1O4-y	Sm	1.84	Ce	0.16	Cu	1															O	4-y		1	1994																												T'							3											K			22.9				22.9																																																																																															11	See J. Alloys Compounds 199, 105 (1993).ANN (in flowing He, at 950C, for 20h).FNC (for 2h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10568	PR05010080		(Sm,Ce)2CuO4	Sm1.83Ce0.17Cu1O4-y	Sm	1.83	Ce	0.17	Cu	1															O	4-y		1	1994																												T'							3											K			21.4				21.4																																																																																															11	See J. Alloys Compounds 199, 105 (1993).ANN (in flowing He, at 950C, for 20h).FNC (for 2h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10569	PR05010080		(Sm,Ce)2CuO4	Sm1.82Ce0.18Cu1O4-y	Sm	1.82	Ce	0.18	Cu	1															O	4-y		2	1994																												T'							3											K			18.8				18.8																																																																																															11	See J. Alloys Compounds 199, 105 (1993).ANN (in flowing He, at 950C, for 20h).FNC (for 2h).					Granular behavior in polycrystalline Sm2-xCexCuO4-y compounds	199409			Phys.Rev.B,50 (1994) 10080	D.Stroud,L.Ben-Dor,M.B.Maple,R.F.Jardim	Sm,Ce,Cu,O	
10620	PR05012752		(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	1994																		GPa		117							2	IL	P4/mmm		A	3.949		3.407	3											K				42			42																																																																																																see Phys. Rev. B 47,14654 (1993)					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10621	PR05012752		(Sr,Ca)CuO2	Sr0.7Ca0.3Cu1O2	Sr	0.7	Ca	0.3	Cu	1															O	2		1	1994																		GPa		118							2	IL	P4/mmm		A	3.903		3.345	3											K				99			99																																																																																														high purity (99.995%) SrCO3,CaCO3,CuO		MIX-CAL(950C,15h)-whole procedure repeated 5 times-SIN(at 5.7GPa,1050C,1h,sandwiched between two pellets of KClO4)-QUENCH(R.T.)					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10622	PR05012752	powder	(Sr,Ca)CuO2	Sr0.14Ca0.86Cu1O2	Sr	0.14	Ca	0.86	Cu	1															O	2		6	1994																		GPa		118.5							2	IL	P4/mmm		A	3.864		3.213	3																																																																																																																SrCO3,CaCO3,CuO (all 99.999%)		MIX(SrCO3,CaCO3,CuO=0.14 : 0.86 : 1)-CAL(in air,920-950C,48h)-SIN(for 1 week,950C)-COOL(R.T.)					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10623	PR05012752	preparation is unclear.	Sr4Cu6O10	Sr4Cu6O10	Sr	4	Cu	6																	O	10			1994																		GPa		102							3		C/mmm		A	3.914	19.354	3.406	3																																																																																																																							Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10624	PR05013778		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca1.73Pb0.17Cu2.86O8+d	Hg	1	Ba	2	Ca	1.73	Pb	0.17	Cu	2.86											O	8+d		1	1994																		GPa		143								Hg1223			A	3.85		15.849	3											K	130		133			3	131.5			K/GPa	1.5																																																																																												See ref.06 in text.This article is unpublished at this time.					Volume dependence of the superconducting transition temperature for the high-temperature superconductor HgBa2Ca2-xPbxCu3O8+z	199411			Phys.Rev.B.,50(1994) 13778	A.R.Drews,Charles C.Kim,D.H.Liebenberg,E.F.Skelton,M.E.Reeves,M.S.Osofsky,S.B.Qadri	Hg,Ba,Ca,Pb,Cu,O	
10625	PR05013684	Sample 1.  Anisotoropic ratio(Hc2 c-axis/Hc2 ab-plane) = 106    from surface resistance of micro wave .	Bi2Sr2CaCu2O8+y	Bi2Sr2Ca1Cu2O8+x	Bi	2	Sr	2	Ca	1	Cu	2													O	8+x		5	1994																																														K		81.8				4	81.8																																																																																															8	Substrate LaGaO3(sample 1),  NdGaO3(sample 2)  film thickness = 1 micron					Angular scaling of the microwave magnetodissipation in Bi2Sr2CaCu2O8+x	199411		"Dipartimento di Fisica ""E. Amaldi"" III Universita' di Roma, Via C.Segre 2,00146 Roma, Ltaly"	Phys.Rev.B,50(1994)13684	E. Silva,M. Giura,R. Fastampa,R. Marcon,S. Sarti		
10626	PR05013684	Sample 2.    Anisotoropic ratio(Hc2 c-axis/Hc2 ab-plane) = 26  from surface resistance of micro wave .	Bi2Sr2CaCu2O8+y	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		8	1994																																														K		84.9				7	84.9																																																																																															8	Substrate LaGaO3(sample 1),  NdGaO3(sample 2)  film thickness = 1 micron					Angular scaling of the microwave magnetodissipation in Bi2Sr2CaCu2O8+x	199411		"Dipartimento di Fisica ""E. Amaldi"" III Universita' di Roma, Via C.Segre 2,00146 Roma, Ltaly"	Phys.Rev.B,50(1994)13684	E. Silva,M. Giura,R. Fastampa,R. Marcon,S. Sarti		
10627	PR05013027	fiber. not irradiated.Jc value is not at a data at helium temperature ,but at 25K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		6	1994																												Bi2212																		K		83					83																																																		30000																																														Fiber were grown by laser-heated pedestal growth method.Fibers irradiated by neutrons up to a fluence of 2.2e15 cm2.					Magnetic irreversibility in Bi2Sr2CaCu2O8 fibers irradiated by neutrons	199411		Department of Physics, Bar-Ilan University, 52900 Ramat-Gan, Israel	Phys.Rev.B,50(1994)13027	D. Gazit,E.R. Yacoby,R.S. feigelson,Y. Yeshurun		
10628	PR05013027	Fiber, irradiated.(3.6e14 1/cm2)Jc value is not at a data at helium temperature ,but at 25K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		6	1994																												Bi2212																		K		83					83																																																		56000																																														Fiber were grown by laser-heated pedestal growth method.Fibers irradiated by neutrons up to a fluence of 2.2e15 cm2.					Magnetic irreversibility in Bi2Sr2CaCu2O8 fibers irradiated by neutrons	199411		Department of Physics, Bar-Ilan University, 52900 Ramat-Gan, Israel	Phys.Rev.B,50(1994)13027	D. Gazit,E.R. Yacoby,R.S. feigelson,Y. Yeshurun		
10629	PR05013027	Fiber, irradiated.(2.2e15 1/cm2)Jc value is not at a data at helium temperature ,but at 25K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		6	1994																												Bi2212																		K		83					83																																																		70000																																														Fiber were grown by laser-heated pedestal growth method.Fibers irradiated by neutrons up to a fluence of 2.2e15 cm2.					Magnetic irreversibility in Bi2Sr2CaCu2O8 fibers irradiated by neutrons	199411		Department of Physics, Bar-Ilan University, 52900 Ramat-Gan, Israel	Phys.Rev.B,50(1994)13027	D. Gazit,E.R. Yacoby,R.S. feigelson,Y. Yeshurun		
10630	PR05013778	bulk modulus=143 GPa,  dTc/dP=1.14+-0.03 K/GPa for line fit	HgBa2(Ca,Pb)2Cu3O8	Hg1Ba2Ca1.73Pb0.17Cu2.86O8+z	Hg	1	Ba	2	Ca	1.73	Pb	0.17	Cu	2.86											O	8+z			1994																		GPa		143							2	Hg1223			A	3.857		15.849												K	130	133				3	133			K/GPa	1.5																																																																																												in detail, ref.16 in this text, but this article is not published at this time					Volume dependence of the superconducting transition temperature for the high-temperature superconductor HgBa2Ca2-xPbxCu3O8+z	199411			Phys.Rev.B.,50(1994) 13778	A.R.Drews,Charles C.Kim,D.H.Liebenberg,E.F.Skelton,M.E.Reeves,M.S.Osofsky,S.B.Qadri	Hg,Ba,Ca,Pb,Cu,O	
10631	PR05012752		(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			1994																		GPa		117							2	IL	P4/mmm		A	3.949		3.407												K		42		42			42																																																																																																high-pressure(5GPa)-high-temp(950C) synthesis, for details see Phys.Rev.B.,47(1993)14654					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10632	PR05012752		(Sr,Ca)CuO2	Sr0.7Ca0.3Cu1O2	Sr	0.7	Ca	0.3	Cu	1															O	2			1994																		GPa		118							2	IL	P4/mmm		A	3.903		3.345												K		99		99			99																																																																																																high-pressure(5GPa)-high-temp(950C) synthesis, for details see Phys.Rev.B.,47(1993)14654					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10633	PR05012752		(Sr,Ca)CuO2	Sr0.14Ca0.86Cu1O2	Sr	0.14	Ca	0.86	Cu	1															O	2			1994																		GPa		118.5							2	IL	P4/mmm		A	3.864		3.213																																																																																																																			high-pressure(5GPa)-high-temp(950C) synthesis, for details see Phys.Rev.B.,47(1993)14654					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10634	PR05012752		Sr4Cu6O10	Sr4Cu6O10	Sr	4	Cu	6																	O	10			1994																		GPa		102							3		c/mmm		A	3.914	19.354	3.406																																																																																																																			high-pressure(5GPa)-high-temp(950C) synthesis, for details see Phys.Rev.B.,47(1993)14654					Structural effects of hydrostatic pressure in Sr1-xMxCuO2(M=La,Ca) and Sr4Cu6O10	199411			Phys.Rev.B.,50(1994) 12752	B.A.Hunter,B.Dabrowski,D.A.Payne,F.Kanamaru,G.Er,H.Shaked,J.D.Jorgensen,P.D.Han,P.G.Radaelli,R.L.Hitterman,S.Kikkawa,Y.Shimakawa	Sr,La,Ca,Cu,O	
10700	PR05015993		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O		4	3	1994																												T'																		K	15.75	15.9	16.15			0.5	15.9																																																																																															5	In detail, see Physica C 165,265 (1990)					Hall effect in the mixed state of superconducting L1.85Ce0.15CuO4(L=Nd,Sm)single crystals	199412			Phys.Rev.B.,50(1994)  !5993	J.Fontcuberta,J.L.Vicent,M.A.Crusellas,M.Cagigal,S.Pinol	Nd,Sm,Ce,Cu,O	
10701	PR05015993		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O		4	3	1994																												T'																		K	18.85	20	21.15			2.3	20																																																																																															5	In detail, see Physica C 165,265 (1990)					Hall effect in the mixed state of superconducting L1.85Ce0.15CuO4(L=Nd,Sm)single crystals	199412			Phys.Rev.B.,50(1994)  !5993	J.Fontcuberta,J.L.Vicent,M.A.Crusellas,M.Cagigal,S.Pinol	Nd,Sm,Ce,Cu,O	
10702	PR05015993		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O		4	3	1994																																														K	13.25	13.5	13.75			0.5	13.5																																																																																															5	In detail, see Physica C 165,265 (1990)					Hall effect in the mixed state of superconducting L1.85Ce0.15CuO4(L=Nd,Sm)single crystals	199412			Phys.Rev.B.,50(1994)  !5993	J.Fontcuberta,J.L.Vicent,M.A.Crusellas,M.Cagigal,S.Pinol	Nd,Sm,Ce,Cu,O	
10703	PR05015858		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O		8	1	1994																											3	Y124			A	3.833	3.873	27.28	3											K				59			59																																																																																														Y123,CuO	1	SIN(850 C,15h, Oxygen 150-200atm)ANN(200 C, H2 gas changed in gas pressure)In detail, see P.R.B 43,10368 (1991)					"Magnetic order induced by hydrogen in superconducting RBa2Cu4O8(R=Y,Gd) studied by Mo""ssbauer and NQR techniques"	199412		The Racah Insitute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B,50(1994)15858	C. Korn,E.R. Bauminger,H. Lutgemeier,H. Schone,I. Felner,I. Nowik,L. Frenkel-Ben Yakar,S. Schmenn,S.D. Goren,U. Asaf		
10704	PR05015858		GdBa2Cu4O8	Gd1Ba2Cu3.96Fe0.04O8	Gd	1	Ba	2	Cu	3.96	Fe	0.04													O		8	1	1994																											3	Y124			A	3.874	3.887	27.14	3																																																																																																																Gd123,CuO	1	preparation is same as PREPID 10703.					"Magnetic order induced by hydrogen in superconducting RBa2Cu4O8(R=Y,Gd) studied by Mo""ssbauer and NQR techniques"	199412		The Racah Insitute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B,50(1994)15858	C. Korn,E.R. Bauminger,H. Lutgemeier,H. Schone,I. Felner,I. Nowik,L. Frenkel-Ben Yakar,S. Schmenn,S.D. Goren,U. Asaf		
10705	PR05015858		GdBa2Cu4O8	Gd1Ba2Cu3.96Fe0.04H2O8	Gd	1	Ba	2	Cu	3.96	Fe	0.04	H	2											O		8	1	1994																											3	Y124			A	3.912	3.927	27.75	3																																																																																																																Gd123,CuO	1	preparation is same as PREPID 10703.					"Magnetic order induced by hydrogen in superconducting RBa2Cu4O8(R=Y,Gd) studied by Mo""ssbauer and NQR techniques"	199412		The Racah Insitute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B,50(1994)15858	C. Korn,E.R. Bauminger,H. Lutgemeier,H. Schone,I. Felner,I. Nowik,L. Frenkel-Ben Yakar,S. Schmenn,S.D. Goren,U. Asaf		
10706	PR05015875		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O		4	1	1994																																														K	36	36.7	37.4			1.4	36.7																																																																							m.ohm.cm				1.1																					In detail, see in Physics and Materials science of High Temperature Superconductors II (Kluwer,Dordecht,1992)					Resistivity,Hall effect,Nernst effect,and thermopower in the mixed state of La1.85Sr0.15CuO4	199412			Phys.Rev.B.,50(1994) 15875	A.Freimuth,C.Hohn,M.Galffy	La,Sr,Cu,O	
10707	PR05015967		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																																														K		90.8					90.8																																																																																																In detail, see J.Low Temp. Phys. 72,345 (1988)Samples are detwinned.This sample is unirradiated.					Testing models of the symmetry of the superconducting pairing state by low-temperature electron irradiation of an untwinned single crystal of YBa2Cu3O7-z	199412			Phys.Rev.B.,50(1994) 15967	D.M.Ginsberg,J.Giapintzakis,M.A.Kirk,S.Ockers	Y,Ba,Cu,O	
10708	PR05015967		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																																														K		89.1					89.1																																																																																																In detail, see J.Low Temp. Phys. 72,345 (1988)Samples are detwinned.This sample is irradiated at 0.98E+19 (e/cm2) by electron.					Testing models of the symmetry of the superconducting pairing state by low-temperature electron irradiation of an untwinned single crystal of YBa2Cu3O7-z	199412			Phys.Rev.B.,50(1994) 15967	D.M.Ginsberg,J.Giapintzakis,M.A.Kirk,S.Ockers	Y,Ba,Cu,O	
10709	PR05015967		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																																														K		87.5					87.5																																																																																																In detail, see J.Low Temp. Phys. 72,345 (1988)Samples are detwinned.This sample is irradiated at 1.96E+19 (e/cm2) by electron.					Testing models of the symmetry of the superconducting pairing state by low-temperature electron irradiation of an untwinned single crystal of YBa2Cu3O7-z	199412			Phys.Rev.B.,50(1994) 15967	D.M.Ginsberg,J.Giapintzakis,M.A.Kirk,S.Ockers	Y,Ba,Cu,O	
10710	PR05015967		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																																														K		88.6					88.6																																																																																																A sample of 'PREPID 10709' was annealed for 12hour at Room temp.					Testing models of the symmetry of the superconducting pairing state by low-temperature electron irradiation of an untwinned single crystal of YBa2Cu3O7-z	199412			Phys.Rev.B.,50(1994) 15967	D.M.Ginsberg,J.Giapintzakis,M.A.Kirk,S.Ockers	Y,Ba,Cu,O	
10711	PR05016033	powder	Tl2Ba2CuO6	Tl2Ba2Cu1O6+d	Tl	2	Ba	2	Cu	1															O	6+d		1	1994																											2	Tl2201			A	3.867		23.234	4											K		60					60																																																																																																For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)ANN(reduced in Ar, 500C)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10712	PR05016033	powder	Tl2Ba2CuO6	Tl2Ba2Cu1O6+d	Tl	2	Ba	2	Cu	1															O	6+d		1	1994																											2	Tl2201			A	3.866		23.159	4																																																																																																																		For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10713	PR05016033	powder	Tl2Ba2CuO6	Tl2Ba2Cu1O6+d	Tl	2	Ba	2	Cu	1															O	6+d		1	1994																											2	Tl2201			A	3.867		23.148	4																																																																																																																		For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)ANN(high pressure O2, 200-400atm, 300-350C, 5hour)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10714	PR05016033	powder	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-d	Tl	1	Sr	2	Ca	1	Cu	2													O	7-d		1	1994																															A	3.794		12.128	4											K		65					65																																																																																																For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)ANN(reduced in Ar, 500C)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10715	PR05016033	powder	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-d	Tl	1	Sr	2	Ca	1	Cu	2													O	7-d		1	1994																															A	3.784		12.119	4																																																																																																																		For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10716	PR05016033	powder	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7-d	Tl	1	Sr	2	Ca	1	Cu	2													O	7-d		1	1994																															A	3.783		12.12	4																																																																																																																		For as-grown sample,see P.R.B 45,5553 (1992), Physica C204,247 (1993).ANN(1 atm oxygen,350C, 10h)ANN(high pressure O2, 200-400atm, 300-350C, 5hour)					Overdoped metals in the Tl2Ba2CuO6+z and TlSr2CaCu2O7-z systems	199412			Phys.Rev.B.,50(1994) 16033	J.D.Jorgensen,T.Manako,Y.Kubo,Y.Simakawa	Tl,Ba,Cu,O,Sr,Ca	
10717	PR05016125	This data is as-made sample's.	YBa2Cu3O7	Y1Ba2Cu3Oy	Y	1	Ba	2	Cu	3															O	y		5	1994																																														K		91				2	91																																																																																																	17			By Laser ablation method. substrates sis SrTiO3. 750C, 1mbar oxygen.The films are c-axis oriented.Samples have been repeatedly annealed at reduced oxygen pressure. (1mbar<O2<1 bar).	Scaling of the Hall coefficient and resistivity in underdoped and overdoped RBa2Cu3Oy films	199412			Phys.Rev.B.,50(1994) 16125	D.van der Marel,J.E.Mooij,N.Y.Chen,V.C.Matijasevic	Ba,Cu,O,R	
10718	PR05016125		(Sm,Ca)Ba2Cu3O7	Sm0.9Ca0.1Ba2Cu3Oy	Sm	0.9	Ca	0.1	Ba	2	Cu	3													O	y		5	1994																																																																																																																																																						17			By MBE, in an Oxone beam, 750C.	Scaling of the Hall coefficient and resistivity in underdoped and overdoped RBa2Cu3Oy films	199412			Phys.Rev.B.,50(1994) 16125	D.van der Marel,J.E.Mooij,N.Y.Chen,V.C.Matijasevic	Ba,Cu,O,R	
10719	PR05016125		(Sm,Ca)Ba2Cu3O7	Sm0.8Ca0.2Ba2Cu3Oy	Sm	0.8	Ca	0.2	Ba	2	Cu	3													O	y		5	1994																																																																																																																																																						17			By MBE, in an Oxone beam, 750C.	Scaling of the Hall coefficient and resistivity in underdoped and overdoped RBa2Cu3Oy films	199412			Phys.Rev.B.,50(1994) 16125	D.van der Marel,J.E.Mooij,N.Y.Chen,V.C.Matijasevic	Ba,Cu,O,R	
10720	PR05016125		(Sm,Ca)Ba2Cu3O7	Sm0.6Ca0.4Ba2Cu3Oy	Sm	0.6	Ca	0.4	Ba	2	Cu	3													O	y		5	1994																																																																																																																																																						17			By MBE, in an Oxone beam, 750C.	Scaling of the Hall coefficient and resistivity in underdoped and overdoped RBa2Cu3Oy films	199412			Phys.Rev.B.,50(1994) 16125	D.van der Marel,J.E.Mooij,N.Y.Chen,V.C.Matijasevic	Ba,Cu,O,R	
10721	PR05016028		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1994																																																																																																																																																			Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10722	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.97Co0.03O7-d	Y	1	Ba	2	Cu	0.97	Co	0.03													O	7-d		3	1994																																														K				90.7			90.7																																																																																														Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10723	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.94Co0.06O7-d	Y	1	Ba	2	Cu	0.94	Co	0.06													O	7-d		3	1994																																														K				88.7			88.7																																																																																														Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10724	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.925Co0.075O7-d	Y	1	Ba	2	Cu	0.925	Co	0.075													O	7-d		3	1994																																														K				81.2			81.2																																																																																														Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10725	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.91Co0.09O7-d	Y	1	Ba	2	Cu	0.91	Co	0.09													O	7-d		3	1994																																														K				76.1			76.1																																																																																														Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10726	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.88Co0.12O7-d	Y	1	Ba	2	Cu	0.88	Co	0.12													O	7-d		3	1994																																														K				66.3			66.3																																																																																														Y2O3, BaCO3, CuO, CoO3	5	Y:Ba:Cu:Co = 1:8:20:10xHEAT(to 800C at 192C/h, to1000C at 50C/h)-Hold(1000C, 4h)-COOL(to 865C,4C/h)-ANN(O2, low pressure, 410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10727	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.94Co0.06O7-d	Y	1	Ba	2	Cu	0.94	Co	0.06													O	7-d		3	1994																																														K				89.7			89.7																																																																																														Y2O3,BaCO3,CuO,CoO3	5	Mostly, this preperation is same as 'PREPID 10721'.The difference is annealing process, i.e., ANN(O2,high pressure 51-53bar,410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10728	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.925Co0.075O7-d	Y	1	Ba	2	Cu	0.925	Co	0.075													O	7-d		3	1994																																														K				86.8			86.8																																																																																														Y2O3,BaCO3,CuO,CoO3	5	Mostly, this preperation is same as 'PREPID 10721'.The difference is annealing process, i.e., ANN(O2,high pressure 51-53bar,410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10729	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.91Co0.09O7-d	Y	1	Ba	2	Cu	0.91	Co	0.09													O	7-d		3	1994																																														K				86.4			86.4																																																																																														Y2O3,BaCO3,CuO,CoO3	5	Mostly, this preperation is same as 'PREPID 10721'.The difference is annealing process, i.e., ANN(O2,high pressure 51-53bar,410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10730	PR05016028		YBa2(Cu,Co)3O7	Y1Ba2Cu0.88Co0.12O7-d	Y	1	Ba	2	Cu	0.88	Co	0.12													O	7-d		3	1994																																														K				77.1			77.1																																																																																														Y2O3,BaCO3,CuO,CoO3	5	Mostly, this preperation is same as 'PREPID 10721'.The difference is annealing process, i.e., ANN(O2,high pressure 51-53bar,410C)					Transition temperature and irreversibility line of cobalt-doped single-crystal YBa2Cu3O7-z: The effect of high-pressure oxygen annealing	199412			Phys.Rev.B.,50(1994) 16028	D.M.Ginsberg,J.Giapintzakis,R.L.Neiman	Y,Ba,Cu,O	
10731	PR05016008		(Cu,C)Ba2Ca3Cu4Oz	Cu0.68C0.32Ba2Ca3Cu4O11+d	Cu	0.68	C	0.32	Ba	2	Ca	3	Cu	4											O	11+d		1	1994																											2	Cu1234	P4/mmm		A	3.862		17.951												K				117			117																																																																																														BaCuO2,CaCuO3,CuO,CaCO3		SIN(C0.5Ba2Ca3Cu4.5O11.1,in gold capsule, 5GPa,1200C,3h)-COOL(R.T.)In detail, see Phys.C 224,69 (1994)					Crystal structure of (Cu,C)Ba2Ca3Cu4O11+z(Tc=117K) by neutron-powder-diffraction analysis	199412			Phys.Rev.B.,50(1994) 16008	D.G.Hinks,D.Jorgensen,E-Takayama-Muromachi,F.Izumi,H.Shaked,R.L.Hitterman,T.Kamiyama,T.Kawashima,Y.Shimakawa	Cu,C,Ba,Ca,O	
10800	PR05101401		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																												Y123																		K		93					93																																									A			1400	9000																																																			See Jpn.J.Appl.Phys. 32,1091 (1993)					c-axis microwave conductivity of YBa2Cu3O7-z in the superconducting state	199501		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ku,Tokyo 113,Japan	Phys.Rev.B.,51(1995)1401	A.Maeda,H.Asaoka,H.Kitano,H.Takei,K.Uchinokura,T.Shibauchi	Y,Ba,O,Cu	
10801	PR05101401		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																												Y123			A			11.72	1											K		65					65																																				A					A			2800	120000																																																			See Jpn.J.Appl.Phys. 32,1091 (1993)					c-axis microwave conductivity of YBa2Cu3O7-z in the superconducting state	199501		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ku,Tokyo 113,Japan	Phys.Rev.B.,51(1995)1401	A.Maeda,H.Asaoka,H.Kitano,H.Takei,K.Uchinokura,T.Shibauchi	Y,Ba,O,Cu	
10802	PR05101401		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																												Y123			A			11.73	1											K		63					63																																									A				170000																																																			See Jpn.J.Appl.Phys. 32,1091 (1993)					c-axis microwave conductivity of YBa2Cu3O7-z in the superconducting state	199501		Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ku,Tokyo 113,Japan	Phys.Rev.B.,51(1995)1401	A.Maeda,H.Asaoka,H.Kitano,H.Takei,K.Uchinokura,T.Shibauchi	Y,Ba,O,Cu	
10803	PR05101397		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.4Sr2Ca2Cu3O10+d	Bi	1.8	Pb	0.4	Sr	2	Ca	2	Cu	3											O	10+d		1	1995																																														K		104				3	104																																														meV	29	6.5	9																																															In detail, see Appl.Superconduct. 1,81 (1993)SIN(powder of Bi1.8Pb0.4Sr2CaCu2Ox, Ca2CuO3 and CuO, packed into Ag tube)-Bi2223 tape					Superconducting enegy gap in Bi1.8Pb0.4Sr2Ca2Cu3O10+z studied by photoemission spectroscopy	199501		Materials Science Division,Argonne National Laboratory,Argonne,Illinois 60439	Phys.Rev.B.,51(1995)1397	A.J.Arko,A.P.Paulilkas,B.A.Andrews,C.Gu.B.W.Veal,D.Y.Kaufman,H.Ding,J.C.Campuzano,M.T.Lanagan,P.Kostic,P.Manuel,R.I.R.Blyth,R.Liu	Bi,Pb,Sr,Ca,Cu,O	
10804	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																			HgO,BaO,CaO,CuO	1	In detail, see physica C222,7 (1994)This sample is as sintered.					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10805	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,500C,24h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10806	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in 1 atm Oxygen,500C,24h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10807	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in 1 atm Oxygen,480C,48h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10808	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in 1 atm Oxygen,480C,96h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10809	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in 1 atm Oxygen,480C,124h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10810	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,500C,240h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10811	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10812	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,400C,24h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10813	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,400C,48h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10814	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,400C,72h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10815	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,400C,120h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10816	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,500C,24h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10817	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Oxygen,500C,48h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10818	PR05101330		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1995																																																																																																																																																					This sample is the annealed sample of 'PREPID 10804' by following.ANN(in Oxygen,300C,6h)ANN(in Nitrogen,400C,24h)					Thermoelectric power and resistivity measurements on oxygen-annealed HgBa2Ca2Cu3O8+z superconductors	199501		Physics Department,Victoria University of Wellington,P.O.Box 600,Wellington,New Zealand	Phys.Rev.B.,51(1995)1330	A.B.Kaiser,C.K.Subramaniam,M.Paranthaman	Hg,Ba,Ca,Cu,O	
10819	PR05101286		La2CuO4	La2Cu1O4.035	La	2	Cu	1																	O		4.035	3	1995																												T																		K	33.4	35	39			5.6	35			K/kBar	-0.5																																																																																										La2O3, CuO	7	By TSFZ. In detail, see Solid State Comm. 90,787(1994), Physica C 209,442(1993)MIX(Stoichiometric) - CAL(1123K) - SIN(1373K)TSFZ(1.0mm/h,solvent 78 mol%CuO, 0.2MPa Oxygen)					Pressure dependence of phase-transition temperatures in oxygenated single-crystalline La2CuO4.035	199501		Reseach Laboratory of Engineering Materials,Tokyo Institute of Tecnhology,4259 Nagatsuta,Midoriku,Yokohama 227,Japan	Phys.Rev.B.,51(1995)1286	Jian Ding Yu,Mitsuru Itoh,Tetsuro Nakamura,Tongkai Huang,Y.Inaguma	La,Cu,O	
10820	PR05101258		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-d	Pr	1.85	Ce	0.15	Cu	1															O	4-d		1	1995																															A	3.972			3											K				22.1			22.1																																																																																															1	SIN(900C and 1000C ,1 week total) - pelletized - SIN(1080C,2day) - SIN(in flowing Oxygen,950C) - COOL(R.T.) - ANN(in flowing He,  800-900C,16h)- COOL(R.T.)					X-ray-absorption studies of electron doping and band shifts in R2-xCexCuO4-z(R=Pr, Nd, Sm, Eu, and Gd)	199501			Peys.Rev.B,51(1995)1258	A. Sahiner,Beom-hoan O,D. Badresingh,G. Liang,J. Chen,J.T. Markert,M. Croft,W. Xu,Y. Guo,Yijie Tang	Pr, Nd, Sm, Eu, Gd, Cu, O	
10821	PR05101258		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-d	Nd	1.85	Ce	0.15	Cu	1															O	4-d		1	1995																												T'			A	3.952			3											K				24.2			24.2																																																																																															1	SIN(900C and 1000C ,1 week total) - pelletized - SIN(1080C,2day) - SIN(in flowing Oxygen,950C) - COOL(R.T.) - ANN(in flowing He,  800-900C,16h)- COOL(R.T.)					X-ray-absorption studies of electron doping and band shifts in R2-xCexCuO4-z(R=Pr, Nd, Sm, Eu, and Gd)	199501			Peys.Rev.B,51(1995)1258	A. Sahiner,Beom-hoan O,D. Badresingh,G. Liang,J. Chen,J.T. Markert,M. Croft,W. Xu,Y. Guo,Yijie Tang	Pr, Nd, Sm, Eu, Gd, Cu, O	
10822	PR05101258		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-d	Sm	1.85	Ce	0.15	Cu	1															O	4-d		1	1995																															A	3.927			3											K				18.3			18.3																																																																																															1	SIN(900C and 1000C ,1 week total) - pelletized - SIN(1080C,2day) - SIN(in flowing Oxygen,950C) - COOL(R.T.) - ANN(in flowing He,  800-900C,16h)- COOL(R.T.)					X-ray-absorption studies of electron doping and band shifts in R2-xCexCuO4-z(R=Pr, Nd, Sm, Eu, and Gd)	199501			Peys.Rev.B,51(1995)1258	A. Sahiner,Beom-hoan O,D. Badresingh,G. Liang,J. Chen,J.T. Markert,M. Croft,W. Xu,Y. Guo,Yijie Tang	Pr, Nd, Sm, Eu, Gd, Cu, O	
10823	PR05101258		(Eu,Ce)2CuO4	Eu1.85Ce0.15Cu1O4-d	Eu	1.85	Ce	0.15	Cu	1															O	4-d		1	1995																															A	3.918			3											K				10			10																																																																																															1	SIN(900C and 1000C ,1 week total) - pelletized - SIN(1080C,2day) - SIN(in flowing Oxygen,950C) - COOL(R.T.) - ANN(in flowing He,  800-900C,16h)- COOL(R.T.)					X-ray-absorption studies of electron doping and band shifts in R2-xCexCuO4-z(R=Pr, Nd, Sm, Eu, and Gd)	199501			Peys.Rev.B,51(1995)1258	A. Sahiner,Beom-hoan O,D. Badresingh,G. Liang,J. Chen,J.T. Markert,M. Croft,W. Xu,Y. Guo,Yijie Tang	Pr, Nd, Sm, Eu, Gd, Cu, O	
10824	PR05101258		(Gd,Ce)2CuO4	Gd1.85Ce0.15Cu1O4-d	Gd	1.85	Ce	0.15	Cu	1															O	4-d		1	1995																															A	3.914			3																																																																																																																	1	SIN(900C and 1000C ,1 week total) - pelletized - SIN(1080C,2day) - SIN(in flowing Oxygen,950C) - COOL(R.T.) - ANN(in flowing He,  800-900C,16h)- COOL(R.T.)					X-ray-absorption studies of electron doping and band shifts in R2-xCexCuO4-z(R=Pr, Nd, Sm, Eu, and Gd)	199501			Peys.Rev.B,51(1995)1258	A. Sahiner,Beom-hoan O,D. Badresingh,G. Liang,J. Chen,J.T. Markert,M. Croft,W. Xu,Y. Guo,Yijie Tang	Pr, Nd, Sm, Eu, Gd, Cu, O	
10825	PR05100547		YBa2Cu3O7	Y1Ba2Cu3O6.25	Y	1	Ba	2	Cu	3															O		6.25	1	1995																											2	Y123			A	3.862		11.788	4																																																																																																																Y2O3, BaCO3, CuO	1	e.g. see Physica C 167,571 (1990)SIN - ANN(510C, 160h, O2 0.01% in N2) - COOL(liq. N2 quench)					Local ordering and charge transfer during room-temperature annealing of quenched tetragonal YBa2Cu3O6.25	199501			Phys.Rev.B,51(1995)547	A.P. Paulikas,B.A. Hunter,B.W. Veal,H. Shaked,J.D. Jorgensen,R.L. Hitterman	Y, Ba, Cu, O	
10826	PR05101393		(Pb,Hg)Ba2Ca2Cu3Ox	Pb0.14Hg1.16Ba2Ca1.38Cu2.56Ox	Pb	0.14	Hg	1.16	Ba	2	Ca	1.38	Cu	2.56											O	x		1	1995																											2	Hg1223			A	3.85		15.847	3																																																																																																																	1	SIN(nitrates of Ba,Ca,Cu at 600C,20h) - MIX - SIN(600C,24h) - MIX(HgO, PbO, precursor) - SIN(855C,6h,in quartz tube)					Transport studies of bulk Pb0.2Hg0.8Ba2Ca1.75Cu3Ox	199501		Materials Science and Technology Division,Naval Research Laboratory,Washington,D.C.20375-5000	Phys.Rev.B.,51(1995)1393	A.R.Drews,E.F.Skelton,L.Toth,M.S.Osofsky,R.J.Soulen,Jr.,T.L.Francavilla,W.L.Lechter	Pb,Hg,Ba,Ca,Cu,O	
10827	PR05101393	Single Phase is 66%.	(Pb,Hg)Ba2Ca2Cu3Ox	Pb0.17Hg1.22Ba2Ca1.44Cu2.79Ox	Pb	0.17	Hg	1.22	Ba	2	Ca	1.44	Cu	2.79											O	x		2	1995																											1	Hg1223			A	3.853		15.851	3											K		133.6				2.5	133.6																																																																																																					Transport studies of bulk Pb0.2Hg0.8Ba2Ca1.75Cu3Ox	199501		Materials Science and Technology Division,Naval Research Laboratory,Washington,D.C.20375-5000	Phys.Rev.B.,51(1995)1393	A.R.Drews,E.F.Skelton,L.Toth,M.S.Osofsky,R.J.Soulen,Jr.,T.L.Francavilla,W.L.Lechter	Pb,Hg,Ba,Ca,Cu,O	
10828	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1995																															A	3.816	3.874	27	3											K				75			75																																																																																														Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10829	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.96Fe0.04O8	Y	1	Ba	2	Cu	3.96	Fe	0.04													O		8	1	1995																															A	3.828	3.867	26.95	3																																																																																																																Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10830	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.92Fe0.08O8	Y	1	Ba	2	Cu	3.92	Fe	0.08													O		8	1	1995																															A	3.842	3.866	26.86	3																																																																																																																Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10831	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.84Fe0.16O8	Y	1	Ba	2	Cu	3.84	Fe	0.16													O		8	1	1995																															A	3.844	3.852	26.87	3																																																																																																																Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10832	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.76Fe0.24O8	Y	1	Ba	2	Cu	3.76	Fe	0.24													O		8	1	1995																															A	3.854	3.854	26.87	3																																																																																																																Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10833	PR05100539		YBa2(Cu,Fe)4O8	Y1Ba2Cu3.6Fe0.4O8	Y	1	Ba	2	Cu	3.6	Fe	0.4													O		8	1	1995																															A	3.862	3.862	26.87	3																																																																																																																Y2O3, Ba(NO3)2, CuO, Fe2O3	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10834	PR05100539		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O		8	1	1995																															A	3.825	3.863	26.96	3																																																																																																																Y2O3, Ba(NO3)2, CuO, NiO	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10835	PR05100539		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.88Ni0.12O8	Y	1	Ba	2	Cu	3.88	Ni	0.12													O		8	1	1995																															A	3.824	3.869	26.94	3																																																																																																																Y2O3, Ba(NO3)2, CuO, NiO	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10836	PR05100539		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.8Ni0.2O8	Y	1	Ba	2	Cu	3.8	Ni	0.2													O		8	1	1995																															A	3.823	3.868	26.95	3																																																																																																																Y2O3, Ba(NO3)2, CuO, NiO	1	MIX - SIN(900C, 30minute) - Press - SIN(900C, 24h, in oxygen flow) - SIN(815C,48h)Control of oxygen content was performed by using Na2C2O4.					Tc degradation in cuprate superconductors from the resistivity of YBa2(Cu1-xMx)4O8 for M=Fe and Ni	199501			Phys.Rev.B.,51(1995) 539	A.V.Narlikar,Anjli Chhikara,Deepak Varandani,E.Gmelin,Ratan Lal,S.P.Pandey,V.P.S.Awana,V.S.Yadav	Y,Ba,Cu,O,Fe,Ni	
10900	PR05103104		(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.99	La	1.85	Sr	0.15	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	25			TP10900																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10901	PR05103104		(La,Sr)2CuO4	La1.82Sr0.18Cu1O3.99	La	1.82	Sr	0.18	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	11.5																											The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10902	PR05103104		(La,Sr)2CuO4	La1.8Sr0.2Cu1O3.99	La	1.8	Sr	0.2	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	6.5			TP10902																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10903	PR05103104		(La,Sr)2CuO4	La1.79Sr0.21Cu1O3.99	La	1.79	Sr	0.21	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	4.5			TP10903																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10904	PR05103104		(La,Sr)2CuO4	La1.77Sr0.23Cu1O3.99	La	1.77	Sr	0.23	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	2			TP10904																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10905	PR05103104		(La,Sr)2CuO4	La1.75Sr0.25Cu1O3.99	La	1.75	Sr	0.25	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	1			TP10905																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10906	PR05103104		(La,Sr)2CuO4	La1.74Sr0.26Cu1O3.99	La	1.74	Sr	0.26	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	-0.5			TP10906																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10907	PR05103104		(La,Sr)2CuO4	La1.73Sr0.27Cu1O3.99	La	1.73	Sr	0.27	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	-0.5			TP10907																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10908	PR05103104		(La,Sr)2CuO4	La1.72Sr0.28Cu1O3.99	La	1.72	Sr	0.28	Cu	1															O		3.99	1	1995																												T																																																																																											micro.V/K	-0.5			TP10908																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for a month)					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10909	PR05103104	The sample is nonsuperconductive.	(La,Sr)2CuO4	La1.65Sr0.35Cu1O3.9	La	1.65	Sr	0.35	Cu	1															O		3.9	1	1995																												T																																																																																											micro.V/K	22			TP10909																								The corresponding oxides & SrCO3	1	Quenched in air from 1210C					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10910	PR05103104		(La,Nd,Sr)2CuO4	La1.813Nd0.037Sr0.15Cu1O4-d	La	1.813	Nd	0.037	Sr	0.15	Cu	1													O	4-d		1	1995																												T																																																																																											micro.V/K	24			TP10910																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for 2-3days.					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10911	PR05103104		(La,Nd,Sr)2CuO4	La1.776Nd0.074Sr0.15Cu1O4-d	La	1.776	Nd	0.074	Sr	0.15	Cu	1													O	4-d		1	1995																												T																																																																																											micro.V/K	27			TP10911																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for 2-3days.					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10912	PR05103104		(La,Nd,Sr)2CuO4	La1.739Nd0.111Sr0.15Cu1O4-d	La	1.739	Nd	0.111	Sr	0.15	Cu	1													O	4-d		1	1995																												T																																																																																											micro.V/K	27			TP10912																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for 2-3days.					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10913	PR05103104		(La,Nd,Sr)2CuO4	La1.702Nd0.148Sr0.15Cu1O4-d	La	1.702	Nd	0.148	Sr	0.15	Cu	1													O	4-d		1	1995																												T																																																																																											micro.V/K	32			TP10913																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for 2-3days.					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10914	PR05103104		(La,Sr)2GaCuO5	La0.85Sr1.15Ga1Cu1O4.98	La	0.85	Sr	1.15	Ga	1	Cu	1													O		4.98	1	1995																																																																																																																							micro.V/K	43			TP10914																								The corresponding oxides & SrCO3	1	ANN (at 900C in Oxygen for 2-3days.					Thermoelectric power in single-layer copper oxides	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3104	J.-S.Zhou,J.B.Goodenough		
10915	PR05103116	in TPFIG , p=1 for thermopower along a-axis, p=2 for thermopower along b-axis	YBa2Cu3O7-d	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1995																												Y123																		K	86						86																																																																						TP10915																										See Physica C 195, 51 (1992) and Pys. Rev. Lett. 68, 2390 (1992).					Thermopower of an untwinned YBa2Cu3O7-z crustal	199502		Department of Physics,Victoria University of Wellington,Wellington,New Zealand	Phys.Rev.B.,51(1995)3116	A.B.Kaiser,B.J.Ruck,C.K.Subramaniam,H.J.Trodahl	Y,Ba,Cu,O	
10916	PR05103116	in TPFIG, p=1 for thermopower // a-axis, p=2 for thermopower// b-axis	YBa2Cu3O7-d	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O		6.7	3	1995																												Y123																		K	70						70																																																																						TP10916																										See Physica C 195, 51 (1992) and Pys. Rev. Lett. 68, 2390 (1992).					Thermopower of an untwinned YBa2Cu3O7-z crustal	199502		Department of Physics,Victoria University of Wellington,Wellington,New Zealand	Phys.Rev.B.,51(1995)3116	A.B.Kaiser,B.J.Ruck,C.K.Subramaniam,H.J.Trodahl	Y,Ba,Cu,O	
10917	PR05103250		YBa2Cu3O7-d	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O		6.96	1	1995																											3	Y123			A	3.821	3.891	11.673	3											K		90					90																																																																		micro.V/K	-1				m.ohm.cm											0.5												La, Y, Ca oxides & Ca, Ba carbonates.	1	SIN (at 920C in air) with several intermidiate grindings.ANN (at 400C in pure O2)					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10918	PR05103250		(Y,Ca)(Ba,La)2Cu3O7	Y0.9Ca0.1Ba1.9La0.1Cu3O6.96	Y	0.9	Ca	0.1	Ba	1.9	La	0.1	Cu	3											O		6.96	1	1995																											3	Y123			A	3.828	3.884	11.652	3											K		82					82																																																																		micro.V/K	-0.5				m.ohm.cm											0.7												La, Y, Ca oxides & Ca, Ba carbonates.	1	SIN (at 920C in air) with several intermidiate grindings.ANN (at 400C in pure O2)					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10919	PR05103250		(Y,Ca)(Ba,La)2Cu3O7	Y0.8Ca0.2Ba1.8La0.2Cu3O6.96	Y	0.8	Ca	0.2	Ba	1.8	La	0.2	Cu	3											O		6.96	1	1995																											3	Y123			A	3.836	3.87	11.68	3											K		78					78																																																																		micro.V/K	0.7				m.ohm.cm											0.8												La, Y, Ca oxides & Ca, Ba carbonates.	1	SIN (at 920C in air) with several intermidiate grindings.ANN (at 400C in pure O2)					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10920	PR05103250		(Y,Ca)(Ba,La)2Cu3O7	Y0.7Ca0.3Ba1.7La0.3Cu3O6.96	Y	0.7	Ca	0.3	Ba	1.7	La	0.3	Cu	3											O		6.96	1	1995																											3	Y123			A	3.838	3.862	11.663	3											K		78					78																																																																		micro.V/K	2				m.ohm.cm											0.8												La, Y, Ca oxides & Ca, Ba carbonates.	1	SIN (at 920C in air) with several intermidiate grindings.ANN (at 400C in pure O2)					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10921	PR05103250		(Y,Ca)(Ba,La)2Cu3O7	Y0.6Ca0.4Ba1.6La0.4Cu3O6.96	Y	0.6	Ca	0.4	Ba	1.6	La	0.4	Cu	3											O		6.96	1	1995																											2	Y123			A	3.855	3.855	11.671	3											K		78					78																																																																		micro.V/K	9				m.ohm.cm											1.2												La, Y, Ca oxides & Ca, Ba carbonates.	1	SIN (at 920C in air) with several intermidiate grindings.ANN (at 400C in pure O2)					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10922	PR05103250	The sample is quenched from 400C.	YBa2Cu3O7-d	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O		6.91		1995																											3	Y123																		K		90					90																																																																		micro.V/K	4				m.ohm.cm											0.8												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10923	PR05103250	The sample is quenched from 450C.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1995																											3	Y123																		K		85					85																																																																		micro.V/K	7				m.ohm.cm											0.9												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10924	PR05103250	The sample is quenched from 500C.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1995																											3	Y123																		K		78					78																																																																		micro.V/K	10				m.ohm.cm											0.9												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10925	PR05103250	The sample is quenched from 550C.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1995																											3	Y123																		K		60					60																																																																		micro.V/K	12				m.ohm.cm											1.3												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10926	PR05103250	The sample is quenched from 600C.	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1995																											3	Y123																		K		52					52																																																																		micro.V/K	22				m.ohm.cm											1.7												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10927	PR05103250	The sample is quenched from 650C.	YBa2Cu3O7-d	Y1Ba2Cu3O6.54	Y	1	Ba	2	Cu	3															O		6.54	1	1995																											3	Y123																		K		50					50																																																																		micro.V/K	31				m.ohm.cm											2.3												La,Cu oxides & Ba carbonate.	1	SIN (at 920C in air) with several intermidiate grindings.FNC to Tq, then quenched.					Chain contribution to the Seebeck coefficient in YBa2Cu3O7-z	199502		Center for Materials Science and Engineering,ETC 9.102,University of Texas at Austin,Austin,Texas 78712-1063	Phys.Rev.B.,51(1995)3250	J.-S.Zhou,J.B.Goodenough,J.P.Zhou,J.T.McDevitt	Y,Ba,Cu,O	
10928	PR05103261	The sample is c-axis-aligned. See Phys. Rev. B 36, 4025 (1987). G-L parameter=114 	Hg1Ba2Ca2Cu3O8-x	Hg1Ba2Ca2Cu3O8-x	Hg	1	Ba	2	Ca	2	Cu	3													O	8-x		1	1995																												Hg1223																		K				135.7			135.7																				T	From the analysis magnetization curve based on Hao and Clem's model, Hc and GL parameter were expect			108					T/K	From the analysis magnetization curve based on Hao and Clem's model, Hc and GL parameter were expect	-1.15					A	From the analysis magnetization curve based on Hao and Clem's model, Hc and GL parameter were expect		17.5		A	From the analysis magnetization curve based on Hao and Clem's model, Hc and GL parameter were expect		2059																																																		Precursor Ba2Ca2Cu3Ox, HgO	1	SIN (for %h at 900C), FNC (to room tempetature)ANN (for 20h at 300C in flowing Oxygen).See J. Mater. Chem. 4, 991 (1994).					Thermodynamic parameters of HgBa2Ca2Cu3O8-x from high-field magnetization	199502		Department of Physics,Pohang University of Science and Technology,P.O.Box 125,Pohang 790-784, South Korea	Phys.Rev.B.,51(1995)3261	Mun-Seog Kim,Myoung-Kwang Bae,Sung-Ik Lee,W.C.Lee	Hg,Ba,Ca,Cu,O	
10929	PR05103993		Bi4Sr4Ca1(Cu,Fe)3Ox	Bi3.9Sr3.3Ca1.3Cu2.883Fe0.117Ox	Bi	3.9	Sr	3.3	Ca	1.3	Cu	2.883	Fe	0.117											O	x		3	1995																													Pmm2		A			27.6	1											K		78.5		80			78.5																																																																							mic.ohm.cm					230																		BiO3, SrO, CaO, CuO, Fe2O3	10						Bi3.9Sr3.3Ca1.3(Cu0.961Fe0.039)3Ox:A high-Tc structure close to the two-dimensinal limit	199502		Lehrstuhl fur Experimentalphysik/Festkorperphysik,Ruhr-Universitat Bochum,D-44780 Bochum,Germany	Phys.Rev.B.,51(1995)3993	B.Freitag,B.vom Hedt,H.Bach,K.Westerholt,R.Noetzel,W.Li%!eck	Bi,Sr,Ca,Cu,Fe,O	
10930	PR05103993		Bi2Sr2CaCu2Ox	Bi2.03Sr2Ca0.9Cu2Ox	Bi	2.03	Sr	2	Ca	0.9	Cu	2													O	x		3	1995																													Amma		A			30.6	1											K		85.5					85.5																																																																																														BiO3, SrO, CaO, CuO, Fe2O3	10						Bi3.9Sr3.3Ca1.3(Cu0.961Fe0.039)3Ox:A high-Tc structure close to the two-dimensinal limit	199502		Lehrstuhl fur Experimentalphysik/Festkorperphysik,Ruhr-Universitat Bochum,D-44780 Bochum,Germany	Phys.Rev.B.,51(1995)3993	B.Freitag,B.vom Hedt,H.Bach,K.Westerholt,R.Noetzel,W.Li%!eck	Bi,Sr,Ca,Cu,Fe,O	
10931	PR05103893		TlSr2(Ca,Pr)Cu2O7	Tl1Sr2Ca0.8Pr0.2Cu2O7	Tl	1	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O		7	2	1995																											2	Tl1212	P4/mmm						3											K	58						58																																																																																																See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10932	PR05103893		TlSr2(Ca,Pr)Cu2O7	Tl1Sr2Ca0.6Pr0.4Cu2O7	Tl	1	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O		7	2	1995																											2	Tl1212	P4/mmm						3											K	70						70																																																																																																See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10933	PR05103893		TlSr2(Ca,Pr)Cu2O7	Tl1Sr2Ca0.4Pr0.6Cu2O7	Tl	1	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O		7	1	1995					micro.B/Mo	3.15	42	5																			2	Tl1212	P4/mmm		A	3.82		12.11	3											K	74						74																																																																																																See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10934	PR05103893		TlSr2(Ca,Pr)Cu2O7	Tl1Sr2Ca0.2Pr0.8Cu2O7	Tl	1	Sr	2	Ca	0.2	Pr	0.8	Cu	2											O		7	2	1995																											2	Tl1212	P4/mmm						3											K	38						38																																																																																																See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10935	PR05103893		TlSr2(Ca,Tb)Cu2O7	Tl1Sr2Ca0.4Tb0.6Cu2O7	Tl	1	Sr	2	Ca	0.4	Tb	0.6	Cu	2											O		7	2	1995					micro.B/Mo	9.53	21	6.2																			2	Tl1212	P4/mmm		A	3.81		12.04	3											K	62						62																																																																																																See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10936	PR05103893		TlSr2(Ca,Tb)Cu2O7	Tl1Sr2Tb1Cu2O7	Tl	1	Sr	2	Tb	1	Cu	2													O		7	2	1995					micro.B/Mo	9.68	24	7																			2	Tl1212	P4/mmm		A	3.82		12	3																																																																																																																		See Phys. Rev. B 49, 6388 (1994).					Superconducting and magnetic properties of TISr2Ca1-xRxCu2O7[R=Pr,Tb]	199502		Indian Institute of Technology,Bombay 400 076,India	Phys.Rev.B.,51(1995)3893	A.Sundaresan,Aravind D.Chinchure,K.Ghosh,L.C.Gupta,M.Sharon,S.Ramakrishnan,S.S.Shah,V.R.Marathe	Tl,Sr,Ca,Cu,O,Pr,Tb	
10937	PR05103120		(Pr,Ce)2Sr2GaCu2O9	Pr1.5Ce0.5Sr2Ga1Cu2O9	Pr	1.5	Ce	0.5	Sr	2	Ga	1	Cu	2											O		9	1	1995																											3		Fmmm	69	A	5.471	5.543	28.43	3																																																																										mJ/K2mol	721		278																																			Pr6O11, CeO2, SrCO3, Ga2O3, CuO	1	CAL (at 1000C for 2days if flowing oxygen), CAL (at 1050C for 2days in flowing oxygen), SIN (at 1050C for 2days in flowing oxygen), FNC, ANL (at 900C for 1day at 130atm).					Crossover from two-dimensional to three-dimensional magnetic structure in Pr1.5Ce0.5Sr2GaCu2O9	199502		Racah Institute of Physics,The Hebrew University,91904 Jerusalem,Israel	Phys.Rev.B.,51(1995)3120	D.Sprinzak,I.Felner,T.Kroner,U.Asaf	Pr,Ce,Sr,Ga,Cu,O	
10938	PR05103120		(Nd, Ce)2Sr2GaCu2O9	Nd1.5Ce0.5Sr2Ga1Cu2O9	Nd	1.5	Ce	0.5	Sr	2	Ga	1	Cu	2											O		9	1	1995	emu/mol		emu.K/mole	0.92	micro.B/Mo	2.2	1.5																				3		Fmmm	69	A	5.482	5.547	28.38	3																																																																																																																Nd2O3, CeO2, SrCO3, Ga2O3, CuO	1	CAL (at 1000C for 2days if flowing oxygen), CAL (at 1050C for 2days in flowing oxygen), SIN (at 1050C for 2days in flowing oxygen), FNC.					Crossover from two-dimensional to three-dimensional magnetic structure in Pr1.5Ce0.5Sr2GaCu2O9	199502		Racah Institute of Physics,The Hebrew University,91904 Jerusalem,Israel	Phys.Rev.B.,51(1995)3120	D.Sprinzak,I.Felner,T.Kroner,U.Asaf	Pr,Ce,Sr,Ga,Cu,O	
10939	PR05103316		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																												Y123																		K	92			92		0.25	92																																									A			1230	10500																																																		5	See Phys. Rev. B 60, 523 (1994).					Anisotropic surface impedance of YBa2Cu3O7-z single crystals	199502		Center for Superconductivity Research,Physics Department,University of Maryland,College Park,Maryland 20742	Phys.Rev.B.,51(1995)3316	D.H.Wu,J.L.Peng,Jain Mao,R.L.Greene,Steven  M.Anlage	Y,Ba,Cu,O	
10940	PR05103312		Tl2Ba2CuO6	Tl2Ba2Cu1O6+d	Tl	2	Ba	2	Cu	1															O	6+d		3	1995																											2	Tl2201							1																																																																																																														/cm3			5	See Phys. Rev. B 43, 12925.					ab-plane optical properties of Tl2Ba2CuO6+z	199502		Department of Physics and Astronomy,McMaster University,Hamilton,Ontario,Canada L8S 4M1	Phys.Rev.B.,51(1995)3312	A.M.Hermann,A.V.Puchkov,S.Doyle,T.Timusk	Tl,Ba,Cu,O	
10941	PR05103806	Containing a high density of dislocations.	Bi2Sr2CaCu2O8	Bi2Sr1.9Ca1Cu2O8+y	Bi	2	Sr	1.9	Ca	1	Cu	2													O	8+y		3	1995																																														K	84		93.5				88.75																																																																																															7	See J. Cryst. Growth 130, 325 (1993).					Fluctuation of vortices and the fluxon transition in Bi2Sr2CaCu2O8+y single crystals	199502		School of Materials Science and Engineering,University of New South Wales,P.O.Box 1,Kensington 2033 New South Wales,Australia	Phys.Rev.B.,51(1995)3806	G.D.Gu,G.J.Russell,J.G.Wen,J.W.Cochrane,N.Koshizuka,N.Nakamura,S.Tajima,Y,Zhao	Bi,Sr,Ca,Cu,O	
10942	PR05103806	Dislocation-free sample.	Bi2Sr2CaCu2O8	Bi2Sr1.9Ca1Cu2O8+y	Bi	2	Sr	1.9	Ca	1	Cu	2													O	8+y		3	1995																												Bi2212																		K	92		96				94																																																																																															7	See J. Cryst. Growth 130, 325 (1993).					Fluctuation of vortices and the fluxon transition in Bi2Sr2CaCu2O8+y single crystals	199502		School of Materials Science and Engineering,University of New South Wales,P.O.Box 1,Kensington 2033 New South Wales,Australia	Phys.Rev.B.,51(1995)3806	G.D.Gu,G.J.Russell,J.G.Wen,J.W.Cochrane,N.Koshizuka,N.Nakamura,S.Tajima,Y,Zhao	Bi,Sr,Ca,Cu,O	
11000	PR05115474	The Sample Preparation Method is not descrived.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7	3	1995																												Y123																		K	92					1	92																																																													W/K.M																																								Machanisms of heat conductivity in higr-Tc superconductors	199506			Phys.Rev.B.51(1995)15474	Miguel Angel Arranz,Raul Villar,Sebastia'n Vieira,Yury Pogorelov		
11001	PR05115474	The Sample Preparation Method is not descrived.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O		8	3	1995																												Bi2212																		K	80					1	80																																																													W/K.M																																								Machanisms of heat conductivity in higr-Tc superconductors	199506			Phys.Rev.B.51(1995)15474	Miguel Angel Arranz,Raul Villar,Sebastia'n Vieira,Yury Pogorelov		
11002	PR05115429		ErBa2Cu3O6+x	Er1Ba2Cu3O7	Er	1	Ba	2	Cu	3															O	6+x	7	3	1995					micro.B/Mo	4.9		0.62																				Y123																		K	92						92																																																																																															5	See Phys. Rev. Lett. 63, 2606 (1989).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11003	PR05115429		ErBa2Cu3O6+x	Er1Ba2Cu3O6.6	Er	1	Ba	2	Cu	3															O	6+x	6.6	3	1995								0.48																				Y123																		K	75						75																																																																																															5	See Appl. Phys. Lett. 51, 1050 (1987).ANN (at 600C for a week in N2, and at 900C for 2h in O2).FNC (to 500C, 50C/h and to room temperature, 0.6C/h).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11004	PR05115429		DyBa2Cu3O6+x	Dy1Ba2Cu3O6	Dy	1	Ba	2	Cu	3															O	6+x	6		1995					micro.B/Mo	7		0.93																				Y123																		K	90						90																																																																																																SSee J. Appl. Phys. 70, 5751 (1991).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11005	PR05115429		DyBa2Cu3O6+x	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	6+x	7	3	1995					micro.B/Mo	7		0.87																				Y123																		K	50						50																																																																																																SSee J. Appl. Phys. 70, 5751 (1991).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11006	PR05115429		DyBa2Cu3O6+x	Dy1Ba2Cu3O6	Dy	1	Ba	2	Cu	3															O	6+x	6	3	1995								0.55																				Y123																																																																																																																									SSee J. Appl. Phys. 70, 5751 (1991).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11007	PR05115429		NdBa2Cu3O6+x	Nd1Ba2Cu3O6.94	Nd	1	Ba	2	Cu	3															O	6+x	6.94	1	1995								0.53																				Y123																		K	90						90																																																																																																See Phys. Rev. B 40, 10963 (1989).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11008	PR05115429		NdBa2Cu3O6+x	Nd1Ba2Cu3O6.78	Nd	1	Ba	2	Cu	3															O	6+x	6.78	1	1995																												Y123																		K	63						63																																																																																																See Phys. Rev. B 40, 10963 (1989).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11009	PR05115429		NdBa2Cu3O6+x	Nd1Ba2Cu3O6.3	Nd	1	Ba	2	Cu	3															O	6+x	6.3	1	1995								1.5																				Y123																																																																																																																									See Phys. Rev. B 40, 10963 (1989).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11010	PR05115429		NdBa2Cu3O6+x	Nd1Ba2Cu3O6.13	Nd	1	Ba	2	Cu	3															O	6+x	6.13	1	1995					micro.B/Mo	0.85		1.75																				Y123																																																																																																																									See Phys. Rev. B 40, 10963 (1989).					Effects of oxygen on magnetic order of the rare-earth ions in RBa2Cu3O6+x (R=Dy, Er, Nd)	199506			Phys.Rev.B,51(1995)15429	B.W. Lee,J.W. Lynn,J.Z. Liu,M. Buchgeiser,M.B. Maple,R.N. Shelton,T.J. Goodwin,T.W. Clinton,Y.X. Jia	Dy, Er, Nd, Ba, Cu, O	
11011	PR05115420		YBa2Cu3O7-d	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O		6.9	5	1995																												Y123																		K	90.2		90.93				90.565																																				A				0.8																															mic.ohm.cm												275													See Physica C 182, 57 (1991).					Evidence for nonuniversal behavior of paraconductivity caused by predominant short-wavelength Gaussian fluctuations in YBaCu3O6.9	199506			Phys.Rev.B,51(1995)15420	Andrea Gauzzi,Davor Pavuna	Y, Ba, Cu, O	
11012	PR05115420		YBa2Cu3O7-d	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O		6.9	5	1995																												Y123																		K	90.5		91.13				90.815																																				A				1																															mic.ohm.cm												270													See Physica C 182, 57 (1991).					Evidence for nonuniversal behavior of paraconductivity caused by predominant short-wavelength Gaussian fluctuations in YBaCu3O6.9	199506			Phys.Rev.B,51(1995)15420	Andrea Gauzzi,Davor Pavuna	Y, Ba, Cu, O	
11013	PR05115420		YBA2Cu3O7-d	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O		6.9	5	1995																												Y123																		K	87.8		89.3				88.55																																				A				1.1																															mic.ohm.cm												325													See Physica C 182, 57 (1991).					Evidence for nonuniversal behavior of paraconductivity caused by predominant short-wavelength Gaussian fluctuations in YBaCu3O6.9	199506			Phys.Rev.B,51(1995)15420	Andrea Gauzzi,Davor Pavuna	Y, Ba, Cu, O	
11014	PR05115420		YBa2Cu3O7-d	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O		6.9	5	1995																												Y123																		K	89.3		90.57				89.935																																				A				1.1																															mic.ohm.cm												270													See Physica C 182, 57 (1991).					Evidence for nonuniversal behavior of paraconductivity caused by predominant short-wavelength Gaussian fluctuations in YBaCu3O6.9	199506			Phys.Rev.B,51(1995)15420	Andrea Gauzzi,Davor Pavuna	Y, Ba, Cu, O	
11015	PR05115407		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8.27	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d	8.27	2	1995																											2	Hg1223			A	3.848		15.778	4											K				135			135																																																																																														HgO, BaO, CaO, CuO	1						Structure and superconductivity of  HgBa2Ca2Cu3O8+z	199506			Phys.Rev.B,51(1995)15407	B.A. Hunter,D.G. Hinks,J.D. Jorgensen,J.L. Wagner	Hg, Ba, Ca, Cu, O	
11016	PR05115407		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8.22	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d	8.22	2	1995																											2	Hg1223			A	3.854		15.825	2											K				107			107																																																																																														HgO, BaO, CaO, CuO	1						Structure and superconductivity of  HgBa2Ca2Cu3O8+z	199506			Phys.Rev.B,51(1995)15407	B.A. Hunter,D.G. Hinks,J.D. Jorgensen,J.L. Wagner	Hg, Ba, Ca, Cu, O	
11017	PR05115407		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8.18	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d	8.18	2	1995																											2	Hg1223			A	3.855		15.825	2											K				94			94																																																																																														HgO, BaO, CaO, CuO	1						Structure and superconductivity of  HgBa2Ca2Cu3O8+z	199506			Phys.Rev.B,51(1995)15407	B.A. Hunter,D.G. Hinks,J.D. Jorgensen,J.L. Wagner	Hg, Ba, Ca, Cu, O	
11018	PR05115388		YBa2Cu3O7-d	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1995																												Y123																		K	92.8					0.3	92.8																																																																																																Single crystals were grown under cooling from 1200 to 910C.ANN (at 450C for 48h in flowing oxygen).					Transverse magnetoresistance of YBa2Cu3Ox single with different oxygen content	199506			Phys.Rev.B,51(1995)15388	A.G. Blinov,E.B. Amitin,G.I. Frolova,K.R. Zhdanov,L.A. Boyarsky,M.Yu. Kameneva,O.M. Kochergin,V.N. Naumov,V.Ya. Dikovsky	Y, Ba, Cu, O	
11019	PR05115388		YBa2Cu3O7-d	Y1Ba2Cu3O6.88	Y	1	Ba	2	Cu	3															O		6.88	3	1995																												Y123																		K	91.5					1.9	91.5																																																																																																Single crystals were grown under cooling from 1200 to 910C.ANN (at 450C for 48h in flowing oxygen).Ann (at 500C for 3h in gaseous helium)					Transverse magnetoresistance of YBa2Cu3Ox single with different oxygen content	199506			Phys.Rev.B,51(1995)15388	A.G. Blinov,E.B. Amitin,G.I. Frolova,K.R. Zhdanov,L.A. Boyarsky,M.Yu. Kameneva,O.M. Kochergin,V.N. Naumov,V.Ya. Dikovsky	Y, Ba, Cu, O	
11020	PR05115388		YBa2Cu3O7-d	Y1Ba2Cu3O6.62	Y	1	Ba	2	Cu	3															O		6.62	3	1995																												Y123																		K	34					22	34																																																																																																Single crystals were grown under cooling from 1200 to 910C.ANN (at 450C for 48h in flowing oxygen).Ann (at 500C for 10h in flow of gaseous helium)					Transverse magnetoresistance of YBa2Cu3Ox single with different oxygen content	199506			Phys.Rev.B,51(1995)15388	A.G. Blinov,E.B. Amitin,G.I. Frolova,K.R. Zhdanov,L.A. Boyarsky,M.Yu. Kameneva,O.M. Kochergin,V.N. Naumov,V.Ya. Dikovsky	Y, Ba, Cu, O	
11021	PR05115478		Y2Ba4Cu7O15-d	Y2Ba4Cu7O14.97	Y	2	Ba	4	Cu	7															O	15	14.97		1995																											3	Y247			A	3.831	3.881	50.679												K			93.1				93.1																																																																																														Ba metal		See Physica C 227, 68 (1994).					Supin pseudogap and interplane coupling in Y2Ba4Cu7O15:A63Cu nuclear spin-spin relaxation study	199506			Phys.Rev.B,51(1995)15478	D. Brinkmann,J. Roos,M. Mali,R.Stern	Y, Ba, Cu, O	
11022	PR05115653		YBa2Cu3O7-d	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	5	1995																												Y123																		K	92						92																																																																							m.ohm.cm											0.24															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11023	PR05115653		YBa2Cu3O7-d	Y1Ba2Cu3O6.77	Y	1	Ba	2	Cu	3															O		6.77	5	1995																												Y123																		K	80						80																																																																							m.ohm.cm											0.34															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11024	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.97Zn0.03O6.95	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		6.95	5	1995																												Y123																		K	81						81																																																																							m.ohm.cm											0.26															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11025	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.97Zn0.03O6.77	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		6.77	5	1995																												Y123																		K	67						67																																																																							m.ohm.cm				0.14							0.44															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11026	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.97Zn0.03O6.75	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		6.75	5	1995																												Y123																		K	58						58																																																																							m.ohm.cm				0.17							0.51															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11027	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.97Zn0.03O6.7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		6.7	5	1995																												Y123																		K	50						50																																																																							m.ohm.cm				0.19							0.55															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11028	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.97Zn0.03O6.68	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		6.68	5	1995																												Y123																		K	41						41																																																																							m.ohm.cm				0.23							0.7															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11029	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.95	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.95	5	1995																												Y123																		K	65						65																																																																							m.ohm.cm				0.1							0.3															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11030	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.77	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.77	5	1995																												Y123																		K	44						44																																																																							m.ohm.cm				0.23							0.55															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11031	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.75	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.75	5	1995																												Y123																		K	37						37																																																																							m.ohm.cm				0.24							0.58															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11032	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.7	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.7	5	1995																												Y123																		K	23						23																																																																							m.ohm.cm				0.3							0.65															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11033	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.68	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.68	5	1995																												Y123																		K	20						20																																																																							m.ohm.cm				0.35							0.74															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11034	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.53	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.53	5	1995																												Y123																																																																																																m.ohm.cm				0.47							1.26															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11035	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.48	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.48	5	1995																												Y123																																																																																																m.ohm.cm	0.04			0.7							1.6															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11036	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.42	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.42	5	1995																												Y123																																																																																																m.ohm.cm				0.8							1.9															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11037	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.38	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.38	5	1995																												Y123																																																																																																m.ohm.cm	1.24			0.95							1.98															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11038	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O6.33	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		6.33	5	1995																												Y123																																																																																																m.ohm.cm				2.4							1.05															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11039	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.95	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.95	5	1995																												Y123																		K	56						56																																																																							m.ohm.cm				0.13							0.37															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11040	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.77	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.77	5	1995																												Y123																		K	30						30																																																																							m.ohm.cm				0.27							0.63															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11041	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.75	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.75	5	1995																												Y123																		K	23						23																																																																							m.ohm.cm				0.32							0.68															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11042	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.7	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.7	5	1995																												Y123																		K	20						20																																																																							m.ohm.cm				0.35							0.77															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11043	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.68	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.68	5	1995																												Y123																		K	10						10																																																																							m.ohm.cm				0.43							0.87															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11044	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.65	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.65	5	1995																												Y123																		K	10						10																																																																							m.ohm.cm				0.37							0.9															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11045	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.6	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.6	5	1995																												Y123																		K	6						6																																																																							m.ohm.cm				0.42							1.03															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11046	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.56	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.56	5	1995																												Y123																																																																																																m.ohm.cm	0.67			0.65							1.37															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11047	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.5	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.5	5	1995																												Y123																																																																																																m.ohm.cm	0.97			0.83							1.69															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11048	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.48	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.48	5	1995																												Y123																																																																																																m.ohm.cm				0.83							1.78															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11049	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.91Zn0.09O6.44	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		6.44	5	1995																												Y123																																																																																																m.ohm.cm				0.96							1.85															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11050	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O6.95	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		6.95	5	1995																												Y123																		K	20						20																																																																							m.ohm.cm				0.23							0.58															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11051	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O6.81	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		6.81	5	1995																												Y123																																																																																																m.ohm.cm	0.27			0.4							0.7															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11052	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O6.76	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		6.76	5	1995																												Y123																																																																																																m.ohm.cm	0.68			0.68							1															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11053	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O6.74	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		6.74	5	1995																												Y123																																																																																																m.ohm.cm	0.75			0.71							1.09															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11054	PR05115653		YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O6.7	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		6.7	5	1995																												Y123																																																																																																m.ohm.cm	0.95			0.8							1.22															2			The substrate is SrTiO3.	Toransport properties of zinc-doped YBa2Cu3O7-z thin fillms	199506			Phys.Rev.B,51(1995)15653	A.P. Mackenzie,D.J.C. Walker,J.R. Cooper	Y, Ba, Cu, O, Zn	
11055	PR05116386		Bi2Sr2CuOx	Bi2Sr2Cu1Ox	Bi	2	Sr	2	Cu	1															O	x		3	1995																												Bi2201																		K			5			1	5																																																																							mic.ohm.cm				290																				5						Bloch-Gruneisen behavior for the in-plane resistivity of Bi2Sr2CuOx single crystals	6			Phys.Rev.B.,51(1995)16380			
11056	PR05116386		Bi2Sr2CuOx	Bi2Sr2Cu1Ox	Bi	2	Sr	2	Cu	1															O	x		3	1995																												Bi2201																		K			5			1	5																																																																							mic.ohm.cm				270																				5						Bloch-Gruneisen behavior for the in-plane resistivity of Bi2Sr2CuOx single crystals	6			Phys.Rev.B.,51(1995)16380			
11057	PR05116386		Bi2Sr2CuOx	Bi2Sr2Cu1Ox	Bi	2	Sr	2	Cu	1															O	x		3	1995																												Bi2201																		K			8			4	8																																																																							mic.ohm.cm				310																				5						Bloch-Gruneisen behavior for the in-plane resistivity of Bi2Sr2CuOx single crystals	6			Phys.Rev.B.,51(1995)16380			
11058	PR05116487	95% of oxygen is 18 O isotope.	YBa2Cu3O7-d	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O		6.94	1	1995																												Y123			A	3.821	3.884	11.687												K				92.6			92.6																																																																																														Y2O3, BaCO3, Cu	1	CAL (at 920C for 15h in flowing oxygen)SIN (at 920C for 15h in flowing oxygen)ANN (at 800C for 10h, and at 600C for 24h)					Observati of a possible oxygen isotope effect on the effective mass of carriers in YBa2Cu3O6.94	6			Phys.Rev.B,51(1995)16487	Donald E. Morris,Guo-meng Zhao	T, Ba, Cu, O	
11059	PR05116487		YBa2Cu3O7-d	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O		6.94	1	1995																												Y123			A	3.821	3.884	11.687												K				92.9			92.9																																																																																														Y2O3, BaCO3, Cu	1	CAL (at 920C for 15h in flowing oxygen)SIN (at 920C for 15h in flowing oxygen)ANN (at 800C for 10h, and at 600C for 24h)					Observati of a possible oxygen isotope effect on the effective mass of carriers in YBa2Cu3O6.94	6			Phys.Rev.B,51(1995)16487	Donald E. Morris,Guo-meng Zhao	T, Ba, Cu, O	
11060	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba2Cu3O6.88	Y	0.6	Pr	0.4	Ba	2	Cu	3													O		6.88	1	1995																											3	Y123			A	3.835	3.895	11.682	3											K		47				4	47																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11061	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba1.8Sr0.2Cu3O6.85	Y	0.6	Pr	0.4	Ba	1.8	Sr	0.2	Cu	3											O		6.85	1	1995																											3	Y123			A	3.84	3.885	11.653	3											K		47				4	47																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11062	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba1.6Sr0.4Cu3O6.87	Y	0.6	Pr	0.4	Ba	1.6	Sr	0.4	Cu	3											O		6.87	1	1995																											3	Y123			A	3.844	3.875	11.64	3											K		44				5	44																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11063	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba1.4Sr0.6Cu3O6.83	Y	0.6	Pr	0.4	Ba	1.4	Sr	0.6	Cu	3											O		6.83	1	1995																											3	Y123			A	3.843	3.863	11.615	3											K		45				5	45																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11064	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba1.2Sr0.8Cu3O6.89	Y	0.6	Pr	0.4	Ba	1.2	Sr	0.8	Cu	3											O		6.89	1	1995																											3	Y123			A	3.844	3.857	11.575	3											K		52				6	52																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11065	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba1Sr1Cu3O6.89	Y	0.6	Pr	0.4	Ba	1	Sr	1	Cu	3											O		6.89	1	1995																											2	Y123			A	3.84	3.84	11.56	3											K		53				11	53																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11066	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba0.8Sr1.2Cu3O6.89	Y	0.6	Pr	0.4	Ba	0.8	Sr	1.2	Cu	3											O		6.89	1	1995																											2	Y123			A	3.836	3.836	11.536	3											K		49				12	49																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11067	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba0.6Sr1.4Cu3O6.89	Y	0.6	Pr	0.4	Ba	0.6	Sr	1.4	Cu	3											O		6.89	2	1995																											2	Y123			A	3.834	3.834	11.53	3											K		49				8	49																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11068	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba0.4Sr1.6Cu3O7-d	Y	0.6	Pr	0.4	Ba	0.4	Sr	1.6	Cu	3											O	7-d		2	1995																												Y123																		K		50				9	50																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11069	PR05116444		(Y, Pr)(Ba,Sr)2Cu3O7-d	Y0.6Pr0.4Ba0.2Sr1.8Cu3O7-d	Y	0.6	Pr	0.4	Ba	0.2	Sr	1.8	Cu	3											O	7-d		2	1995																												Y123																		K		44					44																																																																																														Pr6O11, Y2O3, SrCO3, CuO	1	CAL (at 900C for 12h in air)CAL (at 900C for 24h) two or three timesCAL (at 930C-970C)					Superconductivity in Yo.6Pr0.4Ba2-xSrxCu3O7-z: The role of apical oxygen in hybridization	7		Institute of Physics,Chnese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B,51(1995)16444	Fei Wu,Guanghui Rao,Jingkui Liang,Xiaolong Chen,Yong Wang		
11070	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.976Zn0.024O8	Y	1	Ba	2	Cu	3.976	Zn	0.024													O		8	1	1995																												Y124																		K			63				63																																																																																														Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11071	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.95Zn0.05O8	Y	1	Ba	2	Cu	3.95	Zn	0.05													O		8	1	1995																												Y124																		K			47				47																																																																		micro.V/K	6.8																											Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11072	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.928Zn0.072O8	Y	1	Ba	2	Cu	3.928	Zn	0.072													O		8	1	1995																												Y124																		K			31				31																																																																		micro.V/K	7.1																											Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11073	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.9Zn0.1O8	Y	1	Ba	2	Cu	3.9	Zn	0.1													O		8	1	1995																												Y124																		K			12				12																																																																																														Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11074	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.85Zn0.15O8	Y	1	Ba	2	Cu	3.85	Zn	0.15													O		8	1	1995																												Y124																																																																																											micro.V/K	6.8																											Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11075	PR05116503		YBa2(Cu,Zn)4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1995																												Y124																		K			80				80																																																																		micro.V/K	70																											Y2O3, Ba(NO3)2, CuO, ZnO	1	CAL (at 700C in air)SIN (at 920C for 6h, at 930C for 24h, and at 930C for 24h in oxygen at 6MPa)					89 Y NMR study of the effect of Zn substitution on the spin dynamics of YBa2Cu4O8				Phys.Rev.B,51(1995)16503	A. J'anossy,G.V.M. Williams,J.L. Tallon,R. Meinhold		
11076	PR05116499	Electrochemical deintercalated or nitrogen annealed.	La2CuO4+d	La2Cu1O4	La	2	Cu	1																	O		4	1	1995								310																			3	T			A	5.355	5.405	13.143																																																																																																																	La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11077	PR05116499	as grown.	La2CuO4+d	La2Cu1O4.003	La	2	Cu	1																	O		4.003	1	1995																												T																																																																																																																							La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11078	PR05116499	Electrochemical intercalated with a constant current density, 50%*A/cm2.	La2CuO4+d	La2Cu1O4.06	La	2	Cu	1																	O		4.06	1	1995																												T																		K			45				45																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11079	PR05116499	Electrochemical intercalated with a constant current density, 50%*A/cm2.	La2CuO4+d	La2Cu1O4.065	La	2	Cu	1																	O		4.065	1	1995																												T																		K			45				45																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11080	PR05116499	Electrochemical intercalated with a constant current density, 50%*A/cm2.	La2CuO4+d	La2Cu1O4.075	La	2	Cu	1																	O		4.075	1	1995																												T																		K			45				45																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11081	PR05116499	Electrochemical intercalated with a constant current density, 50%*A/cm2.	La2CuO4+d	La2Cu1O4.08	La	2	Cu	1																	O		4.08	1	1995																												T																		K			45				45																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11082	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.03	La	2	Cu	1																	O		4.03	1	1995																												T																		K			32				32																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11083	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.04	La	2	Cu	1																	O		4.04	1	1995																												T																		K			32				32																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11084	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.05	La	2	Cu	1																	O		4.05	1	1995																												T																		K			32				32																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11085	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.06	La	2	Cu	1																	O		4.06	1	1995																												T																		K			42				42																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11086	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.08	La	2	Cu	1																	O		4.08	1	1995																												T																		K			42				42																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11087	PR05116499	Electrochemical intercalated with a potential technique.See Mater. Res Bull. 29, 735 (1994).	La2CuO4+d	La2Cu1O4.09	La	2	Cu	1																	O		4.09	1	1995																												T																		K			42				42																																																																																														La2O3, CuO	1	CAL (in air at 925C for 12h, at 1000C for 12h, at 1050C for 12h)SIN (at 1100C for 4h)					Superconducting phases of La2CuO4+x prepared by electrochemical oxdation at ambiant temperature	6			Phys.Rev.B,51(1995)16499	A.J. Jacobson,H.H. Feng,J.F. DiCarlo,P.H. Hor,S. Bhavaraju,Z.G. Li	La, Cu, O	
11100	PR05105994		Sr2CuO3	Sr2Cu1O3.02	Sr	2	Cu	1																	O		3.02	1	1995							-1.09	0.028																			3	Sr2CuO3	Immm		A	3.909	3.494	12.691	4																																																																																																																SrCO3, CuO	1	CAL(under flowing O2, for 24h), SIN(under flowing O2, for 24h), ANL(at 950C, in O2)					Magnetic susceptibility and low-temperature structure of the linear chain cuprate Sr2CuO3	199503		Du Pont,  Wilmington, Delaware 19880-0356	Phys.Rev.B,51(1995)5994	D.C. Johnston,M.K. Crawford,Q. Huang,R.L. Harlow,R.W. Erwin,T. Ami,Z.R. Wang		
11101	PR05105994		Sr2CuO3	Sr2Cu1O3.01	Sr	2	Cu	1																	O		3.01	1	1995							-0.83																				3	Sr2CuO3	Immm		A	3.909	3.494	12.691	4																																																																																																																SrCO3, CuO	1	CAL(under flowing O2, for 24h), SIN(under flowing O2, for 24h),ANL (at 600C, in N2)					Magnetic susceptibility and low-temperature structure of the linear chain cuprate Sr2CuO3	199503		Du Pont,  Wilmington, Delaware 19880-0356	Phys.Rev.B,51(1995)5994	D.C. Johnston,M.K. Crawford,Q. Huang,R.L. Harlow,R.W. Erwin,T. Ami,Z.R. Wang		
11102	PR05105994		Sr2CuO3	Sr2Cu1O2.99	Sr	2	Cu	1																	O		2.99	1	1995							-0.86																				3	Sr2CuO3	Immm		A	3.909	3.494	12.691	4																																																																																																																SrCO3, CuO	1	CAL(under flowing O2, for 24h), SIN(under flowing O2, for 24h),ANL(800C, in N2)					Magnetic susceptibility and low-temperature structure of the linear chain cuprate Sr2CuO3	199503		Du Pont,  Wilmington, Delaware 19880-0356	Phys.Rev.B,51(1995)5994	D.C. Johnston,M.K. Crawford,Q. Huang,R.L. Harlow,R.W. Erwin,T. Ami,Z.R. Wang		
11103	PR05105994		Sr2CuO3	Sr2Cu1O3	Sr	2	Cu	1																	O		3	1	1995							-7.81																				3	Sr2CuO3	Immm		A	3.909	3.494	12.691	4																																																																																																																SrCO3, CuO	1	CAL(under flowing O2, for 24h), SIN(under flowing O2, for 24h),ANL(327C, in 6Torr He)					Magnetic susceptibility and low-temperature structure of the linear chain cuprate Sr2CuO3	199503		Du Pont,  Wilmington, Delaware 19880-0356	Phys.Rev.B,51(1995)5994	D.C. Johnston,M.K. Crawford,Q. Huang,R.L. Harlow,R.W. Erwin,T. Ami,Z.R. Wang		
11104	PR05106035	The Sample is grain aligned.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1995																												Y124			A			27.21	3											K				81.4			81.4											Oe	By fitting the Hao-Clem variational model to the reversible magnetization data below Tc.	220							T	By fitting the Hao-Clem variational model to the reversible magnetization data below Tc.	58.1							T/K	By fitting the Hao-Clem variational model to the reversible magnetization data below Tc.	-1.02					A	By fitting the Hao-Clem variational model to the reversible magnetization data below Tc.	23.8			A	derived from coherence length.According to the BCS clean limit.	1880																																																			Oxide of Y and Cu, Barium carbonate	1	CAL(in air, at 900C), CAL(in 20% O2 and 80% Ar, for 12h, under 2kbar, at 1050C), FCL(1.5deg./min.)				The grain is aligned under 8.2T for 15h.	Reversible magnetization, critical, fields, and vortex structure in grain-aligned YBa2Cu4O8	199503		Ames Laboratory, U.S. Department of Enargy and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,51(1995)6035	B. Dabrowski,B.J. Suh,J. Gohng,Junghun Sok,L.A. Schwartzkopf,Ming Xu,Wei Chen		
11105	PR05106594		Y2Cu2O5	Y2Cu2O5	Y	2	Cu	2																	O		5	1	1995								13																																																																																																																																												1	See Physeca B 154, 189 (1989).					Magnetic behavior of R2Cu2O5 cuprates studied by neutron diffraction	199503		Institut de Ciencia de Materials de Barcelona,Consejo Superior de Investigaciones Cientificas,Campus Universitat Autonoma de Barcelona,ES-08193 Bellaterra,Spain	Phys.Rev.B.,51(1995)6594	J.L.Garcia-Munoz,J.Rodrigues-Carvajal,X.Obradors	Cu,O,Y,Er,Tm,Ho,Yb	
11106	PR05106594		Er2Cu2O5	Er2Cu2O5	Er	2	Cu	2																	O		5	1	1995								28																																																																																																																																												1	See Physeca B 154, 189 (1989).					Magnetic behavior of R2Cu2O5 cuprates studied by neutron diffraction	199503		Institut de Ciencia de Materials de Barcelona,Consejo Superior de Investigaciones Cientificas,Campus Universitat Autonoma de Barcelona,ES-08193 Bellaterra,Spain	Phys.Rev.B.,51(1995)6594	J.L.Garcia-Munoz,J.Rodrigues-Carvajal,X.Obradors	Cu,O,Y,Er,Tm,Ho,Yb	
11107	PR05106594		Tm2Cu2O5	Tm2Cu2O5	Tm	2	Cu	2																	O		5	1	1995								17																																																																																																																																												1	See Physeca B 154, 189 (1989).					Magnetic behavior of R2Cu2O5 cuprates studied by neutron diffraction	199503		Institut de Ciencia de Materials de Barcelona,Consejo Superior de Investigaciones Cientificas,Campus Universitat Autonoma de Barcelona,ES-08193 Bellaterra,Spain	Phys.Rev.B.,51(1995)6594	J.L.Garcia-Munoz,J.Rodrigues-Carvajal,X.Obradors	Cu,O,Y,Er,Tm,Ho,Yb	
11108	PR05106594		Ho2Cu2O5	Ho2Cu2O5	Ho	2	Cu	2																	O		5	1	1995								13																																																																																																																																												1	See Physeca B 154, 189 (1989).					Magnetic behavior of R2Cu2O5 cuprates studied by neutron diffraction	199503		Institut de Ciencia de Materials de Barcelona,Consejo Superior de Investigaciones Cientificas,Campus Universitat Autonoma de Barcelona,ES-08193 Bellaterra,Spain	Phys.Rev.B.,51(1995)6594	J.L.Garcia-Munoz,J.Rodrigues-Carvajal,X.Obradors	Cu,O,Y,Er,Tm,Ho,Yb	
11109	PR05106594		Yb2Cu2O5	Yb2Cu2O5	Yb	2	Cu	2																	O		5	1	1995								13																																																																																																																																												1	See Physeca B 154, 189 (1989).					Magnetic behavior of R2Cu2O5 cuprates studied by neutron diffraction	199503		Institut de Ciencia de Materials de Barcelona,Consejo Superior de Investigaciones Cientificas,Campus Universitat Autonoma de Barcelona,ES-08193 Bellaterra,Spain	Phys.Rev.B.,51(1995)6594	J.L.Garcia-Munoz,J.Rodrigues-Carvajal,X.Obradors	Cu,O,Y,Er,Tm,Ho,Yb	
11110	PR05106655	penet unit= micron meter	Bi2Sr2CaCu2O8+d	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1995																												Bi2212																		K				87		5	87																																									micron.m	 			493	meV	0.38			100																																														See Phys. Rev. B49, 1327 (1994).ANL(under 2e-5mbar,at 420C, for 25h)					Field and temperature dependence of the c-axis critical current in Bi2Sr2CaCu2O8+z single crystals at the melting and two-dimensional decomposition fields	199503		Superconducting Research Group,University of Birmingharm B15 2TT,United Kingdom	Phys.Rev.B.,51(1995)6655	C.E.Gough,Guang Yang,Sheng Luo	Bi,Sr,Ca,Cu,O	
11111	PR05106655	penet unit = micron meter	Bi2Sr2CaCu2O8+d	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1995																												Bi2212																		K				93		9	93																																									micron.m				162	meV	0.38			670																																														See Phys. Rev. B49, 1327 (1994).					Field and temperature dependence of the c-axis critical current in Bi2Sr2CaCu2O8+z single crystals at the melting and two-dimensional decomposition fields	199503		Superconducting Research Group,University of Birmingharm B15 2TT,United Kingdom	Phys.Rev.B.,51(1995)6655	C.E.Gough,Guang Yang,Sheng Luo	Bi,Sr,Ca,Cu,O	
11112	PR05106655	penet unit=micron meter	Bi2Sr2CaCu2O8+d	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1995																												Bi2212																		K				87.5		4	87.5																																									micron.m				117	meV	0.28			1275																																														See Phys. Rev. B49, 1327 (1994).ANL(at 520C, in O2, for 72h)					Field and temperature dependence of the c-axis critical current in Bi2Sr2CaCu2O8+z single crystals at the melting and two-dimensional decomposition fields	199503		Superconducting Research Group,University of Birmingharm B15 2TT,United Kingdom	Phys.Rev.B.,51(1995)6655	C.E.Gough,Guang Yang,Sheng Luo	Bi,Sr,Ca,Cu,O	
11200	PR05109261		(Pb,Cd)Sr2YCu2O7	Pb0.5Cd0.5Sr2Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	1	Cu	2											O	7-d		1	1995																												Pb1212			A	3.806		11.983	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11201	PR05109261		(Pb,Cd)Sr2(Y,Ca)Cu2O7	Pb0.5Cd0.5Sr2Y0.9Ca0.1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	0.9	Ca	0.1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.807		11.979	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11202	PR05109261		Pb,Cd)Sr2(Y,Ca)Cu2O7	Pb0.5Cd0.5Sr2Y0.8Ca0.2Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	0.8	Ca	0.2	Cu	2									O	7-d		1	1995																												Pb1212			A	3.806		11.967	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11203	PR05109261		Pb,Cd)Sr2(Y,Ca)Cu2O7	Pb0.5Cd0.5Sr2Y0.7Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.811		11.97	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11204	PR05109261		Pb,Cd)Sr2(Y,Ca)Cu2O7	Pb0.5Cd0.5Sr2Y0.6Ca0.4Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	0.6	Ca	0.4	Cu	2									O	7-d		1	1995																												Pb1212			A	3.813		11.966	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11205	PR05109261		Pb,Cd)Sr2(Y,Ca)Cu2O7	Pb0.5Cd0.5Sr2Y0.5Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.817		11.966	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11206	PR05109261		Pb,Cd)Sr2(Y,Sr)Cu2O7	Pb0.5Cd0.5Sr2.3Y0.7Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.3	Y	0.7	Cu	2											O	7-d		1	1995																												Pb1212			A	3.814		12.007	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11207	PR05109261		Pb,Cd)Sr2(Y,Sr)Cu2O7	Pb0.5Cd0.5Sr2.2Y0.8Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.2	Y	0.8	Cu	2											O	7-d		1	1995																												Pb1212			A	3.813		11.996	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11208	PR05109261		(Pb,Cd)Sr2(Y,Sr)Cu2O7	Pb0.5Cd0.5Sr2.1Y0.9Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.1	Y	0.9	Cu	2											O	7-d		1	1995																												Pb1212			A	3.812		11.988	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11209	PR05109261		(Pb,Cd)(Sr,Y)3Cu2O7	Pb0.5Cd0.5Sr1.9Y1.1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Y	1.1	Cu	2											O	7-d		1	1995																												Pb1212			A	3.811		11.945	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11210	PR05109261		(Pb,Cd)(Sr,Y)3Cu2O7	Pb0.5Cd0.5Sr1.8Y1.2Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.8	Y	1.2	Cu	2											O	7-d		1	1995																												Pb1212			A	3.811		11.906	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11211	PR05109261		(Pb,Cd)Sr2(Y,Sr,Ca)Cu2O7	Pb0.5Cd0.5Sr2.2Y0.5Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.2	Y	0.5	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.82		11.982	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11212	PR05109261		(Pb,Cd)Sr2(Y,Sr,Ca)Cu2O7	Pb0.5Cd0.5Sr2.1Y0.6Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.1	Y	0.6	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.814		11.976	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11213	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.9Y0.8Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Y	0.8	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.808		11.953	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11214	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.8Y0.9Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.8	Y	0.9	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.806		11.913	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11215	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.7Y1Ca0.3Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.7	Y	1	Ca	0.3	Cu	2									O	7-d		1	1995																												Pb1212			A	3.804		11.89	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11216	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr2.2Y0.3Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.2	Y	0.3	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.817		11.965	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11217	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr2.1Y0.4Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.1	Y	0.4	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.817		11.966	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11218	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.9Y0.6Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Y	0.6	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.817		11.942	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11219	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.8Y0.7Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.8	Y	0.7	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.814		11.906	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11220	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.7Y0.8Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.7	Y	0.8	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.811		11.88	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11221	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.6Y0.9Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.6	Y	0.9	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.808		11.855	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11222	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.5Y1Ca0.5Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.5	Y	1	Ca	0.5	Cu	2									O	7-d		1	1995																												Pb1212			A	3.805		11.828	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11223	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.9Ca0.1Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Ca	0.1	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.805		11.97	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11224	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.8Ca0.2Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.8	Ca	0.2	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.804		11.95	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11225	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.6Ca0.4Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.6	Ca	0.4	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.803		11.87	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11226	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.4Ca0.6Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.4	Ca	0.6	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.803		11.84																																																																																																																	PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11227	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.3Ca0.7Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.3	Ca	0.7	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.801		11.84	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11228	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.2Ca0.8Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.2	Ca	0.8	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.802		11.84	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11229	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.1Ca0.9Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.1	Ca	0.9	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.801		11.84	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11230	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1Ca1Y1Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1	Ca	1	Y	1	Cu	2									O	7-d		1	1995																												Pb1212			A	3.803		11.84	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11231	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.9Ca0.2Y0.9Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Ca	0.2	Y	0.9	Cu	2									O	7-d		1	1995																												Pb1212			A	3.806		11.947	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11232	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr2.2Ca0.1Y0.7Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.2	Ca	0.1	Y	0.7	Cu	2									O	7-d		1	1995																												Pb1212			A	3.811		12	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11233	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr2.1Ca0.2Y0.7Cu2O7-d	Pb	0.5	Cd	0.5	Sr	2.1	Ca	0.2	Y	0.7	Cu	2									O	7-d		1	1995																												Pb1212			A	3.81		11.992	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11234	PR05109261		(Pb,Cd)(Sr,Y,Ca)3Cu2O7	Pb0.5Cd0.5Sr1.9Ca0.4Y0.7Cu2O7-d	Pb	0.5	Cd	0.5	Sr	1.9	Ca	0.4	Y	0.7	Cu	2									O	7-d		1	1995																												Pb1212			A	3.807		11.939	3																																																																																																																PbO,CdO,SrCO3,Y2O3,CaCO3,CuO	1	CAL(850C,air,15h) - COOL(R.T.) - Pellet - SIN(950C,air,10h) - COOL(R.T.)This process was repeated several times.					Preferenttial occupancy and composition-driven c-axis variation in (Pb0.5Cd0.5)(Sr,Y,Ca)3Cu2O7-z	199504		Institute of Physics,Chinese Academy of Sciences,Beijing 100080,People's Republic of China	Phys.Rev.B.,51(1995)9261	Cheng Dong,Cong Wang,Fei Wu,Guanghui Rao,Jingkui Lian,Jinrong Min,Xiaolong Chen	Pb,Cd,Sr,Y,Ca,Cu,O	
11235	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu3O7-d	Nd	1	Ba	2	Cu	3															O	7-d		1	1995																												Y123			A	3.86	3.91	11.78	3											K		89.7	90				89.7										22																																														mJ/molK2	12.09		364																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11236	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu2.99Ga0.01O7-y	Nd	1	Ba	2	Cu	2.99	Ga	0.01													O	7-y		1	1995																												Y123			A	3.86	3.91	11.78	3											K		81.2	81.5				81.2										25																																														mJ/molK2	142.24		352																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11237	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.98Ga0.02O7-y	Nb	1	Ba	2	Cu	2.98	Ga	0.02													O	7-y		1	1995																												Nb123			A	3.87	3.91	11.78	3											K		80.2	82				80.2										27																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11238	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu2.97Ga0.03O7-y	Nd	1	Ba	2	Cu	2.97	Ga	0.03													O	7-y		1	1995																												Y123			A	3.88	3.92	11.77	3											K		70.5	72.5				70.5										23																																														mJ/molK2	18.62		351																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11239	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.96Ga0.04O7-y	Nb	1	Ba	2	Cu	2.96	Ga	0.04													O	7-y		1	1995																												Nb123			A	3.88	3.92	11.77	3											K		60.6	70				60.6										18																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11240	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.95Ga0.05O7-y	Nb	1	Ba	2	Cu	2.95	Ga	0.05													O	7-y		1	1995																												Nb123			A	3.88	3.91	11.76	3											K		60	63.5				60										27																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11241	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.94Ga0.06O7-y	Nb	1	Ba	2	Cu	2.94	Ga	0.06													O	7-y		1	1995																												Nb123			A	3.89	3.91	11.76	3											K		56.2	63.5				56.2										58																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11242	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.93Ga0.07O7-y	Nb	1	Ba	2	Cu	2.93	Ga	0.07													O	7-y		1	1995																												Nb123			A	3.89	3.9	11.76	3											K		52	63.5				52										60																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11243	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.92Ga0.08O7-y	Nb	1	Ba	2	Cu	2.92	Ga	0.08													O	7-y		1	1995																												Nb123			A	3.89	3.9	11.76	3											K		52.4	64.5				52.4										53																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11244	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu2.91Ga0.09O7-y	Nd	1	Ba	2	Cu	2.91	Ga	0.09													O	7-y		1	1995																												Y123			A	3.89	3.89	11.76	3											K		50.1	68.5				50.1										35																																														mJ/molK2	21.34		339																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11245	PR05108503		NdBa2(Cu,Ga)3O7	Nb1Ba2Cu2.9Ga0.1O7-y	Nb	1	Ba	2	Cu	2.9	Ga	0.1													O	7-y		1	1995																												Nb123			A	3.9	3.9	11.76	3											K		42.6	50.5				42.6										54																																																																																				Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11246	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu2.7Ga0.3O7-y	Nd	1	Ba	2	Cu	2.7	Ga	0.3													O	7-y		1	1995																												Y123			A	3.88	3.88	11.76	3											K																																																															mJ/molK2	32.86		314																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11247	PR05108503		NdBa2(Cu,Ga)3O7	Nd1Ba2Cu2.5Ga0.5O7-y	Nd	1	Ba	2	Cu	2.5	Ga	0.5													O	7-y		1	1995																												Y123			A	3.91	3.91	11.76	3																																																																										mJ/molK2	13.91		312																																			Nd2O3,BaO2,CuO,Ga2O3	1	SIN(920C,24h) - reground , This process is repeated 5 to 6 times.Pelletized - SIN(920C, 24h)ANN(900C,24h,O2) - ANN(600C,5days,O2) -COOL(R.T.)					Magnetic ordering of Nd3+ions in the high-temperature superconductor NdBa2Cu3-xGaxO7-y (0<x%$0.5 and 0.05<y<0.15)	199504		Max-Planck-Institut fur Festkorperforschung,D-70569 Stuttgart,,Germany	Phys.Rev.B.,51(1995)8503	A.M.Niraimathi,E.Gmelin,G.Rangarajan	Nb,Ba,Cu,Ga,O	
11248	PR05108551	Values of superconductivity section is estimated by flactuation analysis in clean limit only. About other estimation, see in the text.	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.3Sr2Ca2Cu3O10	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	3											O		10	1	1995																												Bi2223																		K				109			109																				T	See a comment of material secotion.	200							T/K		-2.55					A			12.8		A			1390																																																			1	The sample was sintered.neutron-unirradiated sample.					Influence of neutron irradiation damage on the equilibrium properties of the polycrystalline Bi1.8Pb0.3Sr2Ca2Cu3O10 superconductor	199504		Facultad de Recursos Naturales,Universidad de Talca,Talca,Chile	Phys.Rev.B.,51(1995)8551	B.C.Chakoumakos,D.K.Christen,J.G.Ossandon,J.R.Thompson,Y.C.Kim,Yang Ren Sun	Bi,Pb,Sr,Ca,Cu,O	
11249	PR05108551	Values of superconductivity section is estimated by flactuation analysis in clean limit only. About other estimation, see in the text.	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.3Sr2Ca2Cu3O10	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	3											O		10	1	1995																												Bi2223																		K				108			108																				T		250							T/K		-3.3					A			11.4		A			1520																																																			1	This sample was sintered.A neutron fluence = 0.8 E+17 n/cm2					Influence of neutron irradiation damage on the equilibrium properties of the polycrystalline Bi1.8Pb0.3Sr2Ca2Cu3O10 superconductor	199504		Facultad de Recursos Naturales,Universidad de Talca,Talca,Chile	Phys.Rev.B.,51(1995)8551	B.C.Chakoumakos,D.K.Christen,J.G.Ossandon,J.R.Thompson,Y.C.Kim,Yang Ren Sun	Bi,Pb,Sr,Ca,Cu,O	
11250	PR05108551	Values of superconductivity section is estimated by flactuation analysis in clean limit only. About other estimation, see in the text.	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.8Pb0.3Sr2Ca2Cu3O10	Bi	1.8	Pb	0.3	Sr	2	Ca	2	Cu	3											O		10	1	1995																												Bi2223																		K				107			107																				T		460							T/K		-6.2					A			8.5		A			2020																																																			1	This sample was sintered.An neutron fluence = 2.4 E+17 n/cm2					Influence of neutron irradiation damage on the equilibrium properties of the polycrystalline Bi1.8Pb0.3Sr2Ca2Cu3O10 superconductor	199504		Facultad de Recursos Naturales,Universidad de Talca,Talca,Chile	Phys.Rev.B.,51(1995)8551	B.C.Chakoumakos,D.K.Christen,J.G.Ossandon,J.R.Thompson,Y.C.Kim,Yang Ren Sun	Bi,Pb,Sr,Ca,Cu,O	
11251	PR05109193		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7	Y	1	Ba	2	Cu	2.94	Ni	0.06													O		7	4	1995																												Y123																		K				79			79																																									A	error +/- 300	2900																																																									codepositing Y,BaF2,Cu and dopant.postannealing at 900C in moist oxygen.	Magnetic penetration depth in Ni-and Zn-doped YBa2(Cu1-xMx)3O7 films	199504		Department of Physics,The Ohio State University,Columbus,Ohio 43210	Phys.Rev.B.,51(1995)9193	Eric R.Ulm,Jin-Tae Kim,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,Ni,Zn.O	
11252	PR05109193		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.12O7	Y	1	Ba	2	Cu	2.88	Ni	0.12													O		7	4	1995																												Y123																		K				70			70																																									A	error +/-60A	3920																																																									Laser ablation method.	Magnetic penetration depth in Ni-and Zn-doped YBa2(Cu1-xMx)3O7 films	199504		Department of Physics,The Ohio State University,Columbus,Ohio 43210	Phys.Rev.B.,51(1995)9193	Eric R.Ulm,Jin-Tae Kim,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,Ni,Zn.O	
11253	PR05109193		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.82Ni0.18O7	Y	1	Ba	2	Cu	2.82	Ni	0.18													O		7	4	1995																												Y123																		K				68			68																																				A					A	error +/- 60A	12440																																																									codepositing Y,BaF2,Cu and dopant.postannealing at 900C in moist oxygen.	Magnetic penetration depth in Ni-and Zn-doped YBa2(Cu1-xMx)3O7 films	199504		Department of Physics,The Ohio State University,Columbus,Ohio 43210	Phys.Rev.B.,51(1995)9193	Eric R.Ulm,Jin-Tae Kim,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,Ni,Zn.O	
11254	PR05109193		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.94Ni0.06O7	Y	1	Ba	2	Cu	2.94	Ni	0.06													O		7	4	1995																												Y123																		K				62			62																																									A	error is +/-40A	3900																																																									Laser ablation method.	Magnetic penetration depth in Ni-and Zn-doped YBa2(Cu1-xMx)3O7 films	199504		Department of Physics,The Ohio State University,Columbus,Ohio 43210	Phys.Rev.B.,51(1995)9193	Eric R.Ulm,Jin-Tae Kim,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,Ni,Zn.O	
11255	PR05109193		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.88Ni0.12O7	Y	1	Ba	2	Cu	2.88	Ni	0.12													O		7	4	1995																												Y123																		K				43			43																																									A	error is +/-800A	7800																																																									Laser ablation method.	Magnetic penetration depth in Ni-and Zn-doped YBa2(Cu1-xMx)3O7 films	199504		Department of Physics,The Ohio State University,Columbus,Ohio 43210	Phys.Rev.B.,51(1995)9193	Eric R.Ulm,Jin-Tae Kim,Steve R.Foltyn,Thomas R.Lemberger,Xindi Wu	Y,Ba,Cu,Ni,Zn.O	
11256	PR05109419		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																																														K	91					0.5	91																																																																							mic.ohm.cm												67	2000												See P.R.B 49, 12333 (1994)					Vortex liquid in single-crystal YBa2(Cu1-xFex)3O7-z of varying anisotropy	199504		Department of Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm,Sweden	Phys.Rev.B.,51(1995)9419	O.Rapp,Yu.Eltsev	Y,Ba,Cu,Fe,O	
11257	PR05109419		YBa2Cu3O7	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1995																																														K	91					0.5	91																																																																							mic.ohm.cm												69	2700												See P.R.B 49, 12333 (1994)					Vortex liquid in single-crystal YBa2(Cu1-xFex)3O7-z of varying anisotropy	199504		Department of Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm,Sweden	Phys.Rev.B.,51(1995)9419	O.Rapp,Yu.Eltsev	Y,Ba,Cu,Fe,O	
11258	PR05109419		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.895Fe0.105O7-d	Y	1	Ba	2	Cu	2.895	Fe	0.105													O	7-d		3	1995																																														K	70					2	70																																																																							mic.ohm.cm												56	42000												See P.R.B 49, 12333 (1994)					Vortex liquid in single-crystal YBa2(Cu1-xFex)3O7-z of varying anisotropy	199504		Department of Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm,Sweden	Phys.Rev.B.,51(1995)9419	O.Rapp,Yu.Eltsev	Y,Ba,Cu,Fe,O	
11259	PR05109419		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.805Fe0.195O7-d	Y	1	Ba	2	Cu	2.805	Fe	0.195													O	7-d		3	1995																																														K	51					2	51																																																																							mic.ohm.cm												79	235000												See P.R.B 49, 12333 (1994)					Vortex liquid in single-crystal YBa2(Cu1-xFex)3O7-z of varying anisotropy	199504		Department of Solid State Physics,The Royal Institute of Technology,S-100 44 Stockholm,Sweden	Phys.Rev.B.,51(1995)9419	O.Rapp,Yu.Eltsev	Y,Ba,Cu,Fe,O	
11260	PR05108641		(La,Sr)2CuO4	La1.89Sr0.11Cu0.995Fe0.005O4	La	1.89	Sr	0.11	Cu	0.995	Fe	0.005													O		4	1	1995																															A	3.766	3.766	13.2	3											K		14.7	16.5				14.7																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11261	PR05108641		(La,Sr)2CuO4	H0.1La1.89Sr0.11Cu0.995Fe0.005O4	H	0.1	La	1.89	Sr	0.11	Cu	0.995	Fe	0.005											O		4	1	1995																															A	3.766	3.766	13.19	3											K		14	16.5				14																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11262	PR05108641		(La,Sr)2CuO4	H0.27La1.89Sr0.11Cu0.995Fe0.005O4	H	0.27	La	1.89	Sr	0.11	Cu	0.995	Fe	0.005											O		4	1	1995																															A	3.767	3.767	13.18	3											K		13.8	16.5				13.8																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11263	PR05108641		(La,Sr)2CuO4	H0.4La1.89Sr0.11Cu0.995Fe0.005O4	H	0.4	La	1.89	Sr	0.11	Cu	0.995	Fe	0.005											O		4	1	1995																															A	3.768	3.82	13.17	3											K		13.5	16				13.5																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11264	PR05108641		(La,Sr)2CuO4	H0.55La0.89Sr0.11Cu0.995Fe0.005O4	H	0.55	La	0.89	Sr	0.11	Cu	0.995	Fe	0.005											O		4	1	1995																															A	3.79	3.82	13.15	3											K		13.2	16.5				13.2																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11265	PR05108641		(La,Sr)2CuO4	La1.8Sr0.2Cu0.995Fe0.005O4	La	1.8	Sr	0.2	Cu	0.995	Fe	0.005													O		4	1	1995																																														K		25.5	26.5				25.5																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11266	PR05108641		(La,Sr)2CuO4	H0.19La1.8Sr0.2Cu0.995Fe0.005O4	H	0.19	La	1.8	Sr	0.2	Cu	0.995	Fe	0.005											O		4	1	1995																																														K		27.2	28.7				27.2																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11267	PR05108641		(La,Sr)2CuO4	H0.55La1.8Sr0.2Cu0.995Fe0.005O4	H	0.55	La	1.8	Sr	0.2	Cu	0.995	Fe	0.005											O		4	1	1995																																														K		26	28				26																																																																																														La2O3,SrCO3,CuO and Fe2O3	1	SIN(Cu:Fe=0.995:0005).The hydrogenation was carried by means of volumetric method at 157C.					Phase separation of hydrogenated La2-xSrxCu(Fe)O4	199504		Institute for Low Temperature and Sturucture Research,Polish Academy of Sciences,P.O.Box 937,50-950 Wroclaw,Poland	Phys.Rev.B.,51(1995)8641	A.D.Shengelaya,A.J.Zaleski,J.Klamut,J.Olejniczak	La,Sr,Cu,Fe,O	
11268	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y1Sr2Cu2.7Mo0.3O7-d	Y	1	Sr	2	Cu	2.7	Mo	0.3													O	7-d		1	1995																															A	3.81		11.538	3											K		33.2					33.2																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11269	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.9Pr0.1Sr2Cu2.7Mo0.3O7-d	Y	0.9	Pr	0.1	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.814		11.534	3											K		33.1					33.1																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11270	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.8Pr0.2Sr2Cu2.7Mo0.3O7-d	Y	0.8	Pr	0.2	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.818		11.545	3											K		31.6					31.6																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11271	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.7Pr0.3Sr2Cu2.7Mo0.3O7-d	Y	0.7	Pr	0.3	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.826		11.547	3											K		29.7					29.7																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11272	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.6Pr0.4Sr2Cu2.7Mo0.3O7-d	Y	0.6	Pr	0.4	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.83		11.555	3											K		25.9					25.9																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11273	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.5Pr0.5Sr2Cu2.7Mo0.3O7-d	Y	0.5	Pr	0.5	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.835		11.575	3											K		22.2					22.2																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11274	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.4Pr0.6Sr2Cu2.7Mo0.3O7-d	Y	0.4	Pr	0.6	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.84		11.58	3											K		17.3					17.3																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11275	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.3Pr0.7Sr2Cu2.7Mo0.3O7-d	Y	0.3	Pr	0.7	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.844		11.591	3											K		12.2					12.2																																																																																														Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11276	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.2Pr0.8Sr2Cu2.7Mo0.3O7-d	Y	0.2	Pr	0.8	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.85		11.606	3																																																																																																																Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11277	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Y0.1Pr0.9Sr2Cu2.7Mo0.3O7-d	Y	0.1	Pr	0.9	Sr	2	Cu	2.7	Mo	0.3											O	7-d		1	1995																															A	3.853		11.613	3																																																																																																																Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11278	PR05108543		(Y,Pr)Sr2(Cu,Mo)3O7	Pr1Sr2Cu2.7Mo0.3O7-d	Pr	1	Sr	2	Cu	2.7	Mo	0.3													O	7-d		1	1995																															A	3.858		11.616	3																																																																																																																Y2O3,Pr6O11,SrCO3,CaCO3,CuO and MoO3	1	SIN(3h,1020C,Oxygen) - COOL(R.T.) This process is repeated twice.					Superconductivity and magnetism in Y1-xPrxSr2Cu2.7Mo0.3O7-z	199504		Departmment of Physics,National Sun Yat-Sen University,Kaohsing,Taiwan 804,Republic og China	Phys.Rev.B.,51(1995)8543	C.R.Shih,H.D.Yang,H.L.Tsay,Y.C.Chen	Y,Pr,Sr,Cu,Mo,O	
11279	PR05108582		(Y,Ca)Ba2Cu3O7	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O		6.98	4	1995																																														K	83.3						83.3																																																																							mic.ohm.cm											390													16					LaAlO3 substrates. Growth(790C, 120mTorr Ar and 80mTorr O2)ANN( 1 atm, O2, 480-500C, 2-4h)Further details can be found in Physica C 171,354 (1990)	Transport characterization of calcium-doped YBa2Cu3O7-z thin films	199504		Department of Materials Science and Engineering,Stabford University,Stanford,California 94305-2205	Phys.Rev.B.,51(1995)8582	J.C.Bravman,J.T.Kucera	Y,Ba,Cu,O	
11280	PR05108582		(Y,Ca)Ba2Cu3O7	Y0.9Ca0.1Ba2Cu3O6.96	Y	0.9	Ca	0.1	Ba	2	Cu	3													O		6.96	4	1995																																														K	81.5						81.5																																																																							mic.ohm.cm											330													16					LaAlO3 substrates. Growth(790C, 120mTorr Ar and 80mTorr O2)ANN( 1 atm, O2, 480-500C, 2-4h)Further details can be found in Physica C 171,354 (1990)	Transport characterization of calcium-doped YBa2Cu3O7-z thin films	199504		Department of Materials Science and Engineering,Stabford University,Stanford,California 94305-2205	Phys.Rev.B.,51(1995)8582	J.C.Bravman,J.T.Kucera	Y,Ba,Cu,O	
11281	PR05108582		(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.9	Y	0.8	Ca	0.2	Ba	2	Cu	3													O		6.9	4	1995																																														K	73.9						73.9																																																																							mic.ohm.cm											410													16					LaAlO3 substrates. Growth(790C, 120mTorr Ar and 80mTorr O2)ANN( 1 atm, O2, 480-500C, 2-4h)Further details can be found in Physica C 171,354 (1990)	Transport characterization of calcium-doped YBa2Cu3O7-z thin films	199504		Department of Materials Science and Engineering,Stabford University,Stanford,California 94305-2205	Phys.Rev.B.,51(1995)8582	J.C.Bravman,J.T.Kucera	Y,Ba,Cu,O	
11282	PR05108582		(Y,Ca)Ba2Cu3O7	Y0.7Ca0.3Ba2Cu3O6.87	Y	0.7	Ca	0.3	Ba	2	Cu	3													O		6.87	4	1995																																														K	88.7						88.7																																																																							mic.ohm.cm											450													16					LaAlO3 substrates. Growth(790C, 120mTorr Ar and 80mTorr O2)ANN( 1 atm, O2, 480-500C, 2-4h)Further details can be found in Physica C 171,354 (1990)	Transport characterization of calcium-doped YBa2Cu3O7-z thin films	199504		Department of Materials Science and Engineering,Stabford University,Stanford,California 94305-2205	Phys.Rev.B.,51(1995)8582	J.C.Bravman,J.T.Kucera	Y,Ba,Cu,O	
11283	PR05109123		(Tl,Pb)Sr2CaCu2Oz	Tl0.5Pb0.5Sr2Ca1Cu2Ox	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2											O	x		3	1995																												Tl1212																		K				77.7			77.7																				T	in order to derive these parameters, scaling theory for critical fluctuation in the magnetization by	90							T/K		1.7					A			19.3		A		2140																																																			Tl2O3,BaCuO2,CaO,PbO,SrCuO2,CuO	5	See Physica C 219,407 (1994)					Superconducting fluctuations in Tl-based single crystals: Evidence of universal features and derivation of basic parameters	199504		Laboratoire Crismat,CNRS URA 1318,Institut des Sciences de la Matiere et du Rayonnement,6 Boulevard du Marechal Juin,14050 Caen Cedex,France	Phys.Rev.B.,51(1995)9123	A.Maignan,A.Wahl,C.Martin,Ch.Simon,J.Provost,V.Hardy	Tl,Pb,Sr,Ca,Cu,O,Ba	
11284	PR05109123		TlBa2CaCu2Oz	Tl1Ba2Ca2Cu3Ox	Tl	1	Ba	2	Ca	2	Cu	3													O	x		3	1995																												Tl1223																		K				111.7			111.7																				T		160							T/K		2					A			14.5		A			1860																																																		Tl2O3,BaCuO2,CaO,PbO,SrCuO2,CuO	5	See Physica C 219,407 (1994)					Superconducting fluctuations in Tl-based single crystals: Evidence of universal features and derivation of basic parameters	199504		Laboratoire Crismat,CNRS URA 1318,Institut des Sciences de la Matiere et du Rayonnement,6 Boulevard du Marechal Juin,14050 Caen Cedex,France	Phys.Rev.B.,51(1995)9123	A.Maignan,A.Wahl,C.Martin,Ch.Simon,J.Provost,V.Hardy	Tl,Pb,Sr,Ca,Cu,O,Ba	
11285	PR05109123		Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3Ox	Tl	2	Ba	2	Ca	2	Cu	3													O	x		3	1995																												Tl2223																		K				123.6			123.6																				T		260							T/K		3					A			11.3		A			2070																																																		Tl2O3,BaCuO2,CaO,PbO,SrCuO2,CuO	5	See Physica C 219,407 (1994)					Superconducting fluctuations in Tl-based single crystals: Evidence of universal features and derivation of basic parameters	199504		Laboratoire Crismat,CNRS URA 1318,Institut des Sciences de la Matiere et du Rayonnement,6 Boulevard du Marechal Juin,14050 Caen Cedex,France	Phys.Rev.B.,51(1995)9123	A.Maignan,A.Wahl,C.Martin,Ch.Simon,J.Provost,V.Hardy	Tl,Pb,Sr,Ca,Cu,O,Ba	
11286	PR05109123		Tl2Ba2CaCu2Oz	Tl2Ba2Ca1Cu2Ox	Tl	2	Ba	2	Ca	1	Cu	2													O	x		3	1995																												Tl2212																		K				103.1			103.1																				T		180							T/K		2.6					A			13.4		A			2850																																																		Tl2O3,BaCuO2,CaO,PbO,SrCuO2,CuO	5	See Physica C 219,407 (1994)					Superconducting fluctuations in Tl-based single crystals: Evidence of universal features and derivation of basic parameters	199504		Laboratoire Crismat,CNRS URA 1318,Institut des Sciences de la Matiere et du Rayonnement,6 Boulevard du Marechal Juin,14050 Caen Cedex,France	Phys.Rev.B.,51(1995)9123	A.Maignan,A.Wahl,C.Martin,Ch.Simon,J.Provost,V.Hardy	Tl,Pb,Sr,Ca,Cu,O,Ba	
11287	PR05108434	The ratio of Ca:Na is unknown in this article.(Ca,Na)2CuO2Cl2.Meissner fraction is measured at 5K.	(Ca,Na)2CuCl2O2	Ca1.9Na0.1Cu1Cl2O2	Ca	1.9	Na	0.1	Cu	1	Cl	2													O		2	1	1995																																														K				26			26										43																																																																																					1	nominal composition Ca1.88Na0.12CuO2Cl2.SIN(6GPa,1173K,Na2O2,NaClO4 and Ca1.88Na0.12CuO2Cl2)					Structure and superconductivity without apical oxygens in(Ca,Na)2CuO2Cl2	199504		Science and Tecnology Center for Superconductivity and Materials Science Division,Argonne National Laboratory,Argonne,Illinios 60439	Phys.Rev.B.,51(1995)8434	D.N.Argyriou,J.D.Jorgensen,M.Takano,N.Kobayashi,R.L.Hitterman,Z.Hiroi	Ca,Na,Cu,O,Cl	
11300	PR05112900		YbBa2Cu3O7	Yb1Ba2Cu3O7	Yb	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.796	3.866	11.613	3											K		87.9	88.6			2	87.9			K/GPa	-0.51																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11301	PR05112900		TmBa2Cu3O7	Tm1Ba2Cu3O7	Tm	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.801	3.871	11.616	3											K		90.4				0.7	90.4			K/GPa	0.39																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11302	PR05112900		HoBa2Cu3O7	Ho1Ba2Cu3O7	Ho	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.818	3.883	11.633	3											K		91.5				0.7	91.5			K/GPa	0.62																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11303	PR05112900		DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.818	3.884	11.649	3											K		91.7				0.8	91.7			K/GPa	0.69																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11304	PR05112900		GdBa2Cu3O7	Gd1Ba2Cu3O7	Gd	1	Ba	2	Cu	3															O		7	1	1995																												Y123																		K		93.6				0.7	93.6			K/GPa	0.76																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11305	PR05112900		SmBa2Cu3O7	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.849	3.898	11.691	3											K		93.1				1.1	93.1			K/GPa	1.18																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11306	PR05112900		NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O		7	1	1995																											3	Y123			A	3.857	3.912	11.721	3											K		94.4				0.9	94.4			K/GPa	1.21																																																																																											1						Origin of the R-ion effect on Tc in RBa2Cu3O7	199505		Department Physics, National Taiwan University, Taipei, Taiwan, Republic of China	Phys.Rev.B,51(1995)12900	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.W. Cao,Y.Y. Xue		
11307	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.9Cu1Oy	Bi	2	Sr	1.9	Cu	1															O	y		2	1995																											3	Bi2201			A	5.372	5.367	24.573	3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11308	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.8Cu1Oy	Bi	2	Sr	1.8	Cu	1															O	y		1	1995																											3	Bi2201			A				3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11309	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.7Cu1Oy	Bi	2	Sr	1.7	Cu	1															O	y		1	1995																											3	Bi2201			A	5.382	5.379	24.528	3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11310	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.6Cu1Oy	Bi	2	Sr	1.6	Cu	1															O	y		1	1995																											3	Bi2201			A	5.386	5.384	24.536	3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11311	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.5Cu1Oy	Bi	2	Sr	1.5	Cu	1															O	y		1	1995																											3	Bi2201			A	5.401	5.43	24.349	3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11312	PR05112771		Bi2Sr2-xCuOy	Bi2Sr1.4Cu1Oy	Bi	2	Sr	1.4	Cu	1															O	y		1	1995																											3	Bi2201			A	5.414	5.435	24.338	3																																																																																																																Bi2O3, SrCO3, MgO	1	CAL(in air, at 830C), CAL(in air, at 830C, for 50h), SIN(in air, at 850C, for 50h)					Relation of local Cu2+spins,crystal microstructure,and chaege transport in the CuO2 plane in Bi2Sr2CuOy	199505		Structure Research Laboratory, of Science and technology of China, Hefei,230026, Peple's Republic of China	Phys.Rev.B,51(1995)12771	Mao Zhiqiang,Tian Mingliang,Xu Cunyi,Xu Yunhua,Yu Weijie	Bi, Sr, Cu, O	
11313	PR05112759		Tl2Ba2CuO6	Tl1.75Ba2Cu1.2O5.98	Tl	1.75	Ba	2	Cu	1.2															O		5.98	1	1995																												Tl2201							3											K	26						26																																																																							m.ohm.cm											0.9												(3n)Tl2O3, BaO, CaO, CuO	1	SIN(at 865-890C, in air or in flowing O2)					Determination of oxygen content and cation valences in superconducting Tl-based cuprates by wet chemical method	199505		Superconductivity Reserch Laboratory, ISTEC, 10-13 Shinonome 1-chome Koto-ku tokyo, Japan	Phys.Rev.B,51(1995)12759	A. Fukuoka,H. Yamauchi,K. Hamada,M. Itoh,M. Karppinen		
11314	PR05112759		Tl2Ba2CaCu2O8	Tl1.63Ba2Ca1.3Cu2O7.94	Tl	1.63	Ba	2	Ca	1.3	Cu	2													O		7.94	1	1995																												Tl2212							3											K	91						91																																																																							m.ohm.cm											2.1												(3n)Tl2O3, BaO, CaO, CuO	1	SIN(at 865-890C, in air or in flowing O2)					Determination of oxygen content and cation valences in superconducting Tl-based cuprates by wet chemical method	199505		Superconductivity Reserch Laboratory, ISTEC, 10-13 Shinonome 1-chome Koto-ku tokyo, Japan	Phys.Rev.B,51(1995)12759	A. Fukuoka,H. Yamauchi,K. Hamada,M. Itoh,M. Karppinen		
11315	PR05112759		Tl2Ba2Ca2Cu3O10	Tl1.62Ba2Ca2.3Cu3O9.92	Tl	1.62	Ba	2	Ca	2.3	Cu	3													O		9.92	1	1995																												Tl2223							3											K	113						113																																																																							m.ohm.cm											2												(3n)Tl2O3, BaO, CaO, CuO	1	SIN(at 865-890C, in air or in flowing O2)					Determination of oxygen content and cation valences in superconducting Tl-based cuprates by wet chemical method	199505		Superconductivity Reserch Laboratory, ISTEC, 10-13 Shinonome 1-chome Koto-ku tokyo, Japan	Phys.Rev.B,51(1995)12759	A. Fukuoka,H. Yamauchi,K. Hamada,M. Itoh,M. Karppinen		
11316	PR05112759		Tl2Ba2Ca3Cu4O12	Tl1.6Ba2Ca3.3Cu4O11.89	Tl	1.6	Ba	2	Ca	3.3	Cu	4													O		11.89	1	1995																												Tl2234							3											K	103						103																																																																							m.ohm.cm											2.7												(3n)Tl2O3, BaO, CaO, CuO	1	SIN(at 865-890C, in air or in flowing O2)					Determination of oxygen content and cation valences in superconducting Tl-based cuprates by wet chemical method	199505		Superconductivity Reserch Laboratory, ISTEC, 10-13 Shinonome 1-chome Koto-ku tokyo, Japan	Phys.Rev.B,51(1995)12759	A. Fukuoka,H. Yamauchi,K. Hamada,M. Itoh,M. Karppinen		
11317	PR05112747		Tl2Ba2CuO6	Tl1.89Ba2Cu1.11O6.18	Tl	1.89	Ba	2	Cu	1.11															O		6.18	1	1995																											2	Tl2201	I4/mmm		A	3.684		23.137	3											K	49						49																																																																																														Tl2O3(99.99%), BaO2(98%), CuO(99.999%)	1	SIN(at 800C, for 10h), SIN(at 820C, for 10h), SIN(at 865C, for 5h), SIN(at 865C, for 3h), ANL(at 480C for 5h), every process with FNC(to 25C, at 10C/min.). Then, quenched.					Cation distributions and possible phase separation in Tl2Ba2CuO6+zfrom synchrotron powder x-ray diffraction	199505		Interdisciplinary Raserch Centre in Superconductivity, Uuiversity of Cambridge,Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,51(1995)12747	A.P. Mackenzie,D.C. Sinclair,J.P. Attfleld,M.A.G. Aranda	Tl, Ba, Cu, O	
11318	PR05112747		Tl2Ba2CuO6	Tl1.97Ba2.02Cu1.01O6.16	Tl	1.97	Ba	2.02	Cu	1.01															O		6.16	1	1995																											3	Tl2201	Fmmm		A	5.448	5.497	23.178	3																																																																																																																Tl2O3(99.99%), BaO2(98%), CuO(99.999%)	1	SIN(at 800C, for 10h), SIN(at 820C, for 10h), SIN(at 820C for 10h),every process with FNC(to 25C, at 10C/min.)					Cation distributions and possible phase separation in Tl2Ba2CuO6+zfrom synchrotron powder x-ray diffraction	199505		Interdisciplinary Raserch Centre in Superconductivity, Uuiversity of Cambridge,Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,51(1995)12747	A.P. Mackenzie,D.C. Sinclair,J.P. Attfleld,M.A.G. Aranda	Tl, Ba, Cu, O	
11319	PR05112053	untwinned sample	YBa2Cu3O7-d	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O		6.93	3	1995																																														K		93.2				0.15	93.2																																																																																																See Phys. Rev. B50, 3458 (1994).					Additive quasiparticle and vortex Hall conductivities in La2-xSrxCuO4  and untwinned YBa2Cu3O6.93	199505		Joseph Henry Laboratoris of Prysics, Princeton University, Princeton, New Jersey 08544	Phys.Rev.B,51(1995)12053	J.M.Harris,K.Kitazawa,L.Taillefer,N.P.Ong,P.Matl,R.Gagnon,T.Kimura	La, Sr, Cu, O, Y, Ba	
11320	PR05112053	untwinned sample	YBa2Cu3O7-d	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O		6.93	3	1995																																														K		93.5		0.21			93.5																																																																																																See Phys. Rev. B50, 3458 (1994).					Additive quasiparticle and vortex Hall conductivities in La2-xSrxCuO4  and untwinned YBa2Cu3O6.93	199505		Joseph Henry Laboratoris of Prysics, Princeton University, Princeton, New Jersey 08544	Phys.Rev.B,51(1995)12053	J.M.Harris,K.Kitazawa,L.Taillefer,N.P.Ong,P.Matl,R.Gagnon,T.Kimura	La, Sr, Cu, O, Y, Ba	
11321	PR05112053		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O		4	3	1995																																														K		38.7				2	38.7																																																																							mic.ohm.cm											411													7						Additive quasiparticle and vortex Hall conductivities in La2-xSrxCuO4  and untwinned YBa2Cu3O6.93	199505		Joseph Henry Laboratoris of Prysics, Princeton University, Princeton, New Jersey 08544	Phys.Rev.B,51(1995)12053	J.M.Harris,K.Kitazawa,L.Taillefer,N.P.Ong,P.Matl,R.Gagnon,T.Kimura	La, Sr, Cu, O, Y, Ba	
11322	PR05111848	O(18)=84.6%	(Y,Pr)Ba2Cu3O7-d	Y0.8Pr0.2Ba2Cu3O7-d	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-d		1	1995																											3	Y123							3											K		75		74.9			75						0.11	O	84.6																																																																																								See Phys. Rev. B44, 5318 (1991), Physica B 169, 697(1991)					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11323	PR05111848	O(18)=79%	(Y,Pr)Ba2Cu3O7-d	Y0.7Pr0.3Ba2Cu3O7-d	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-d		1	1995																											3	Y123							3											K		60.5		59.5			60.5						0.19	O	79																																																																																								See Phys. Rev. B44, 5318 (1991), Physica B 169, 697(1991)					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11324	PR05111848	O(18)=85.5%	(Y,Pr)Ba2Cu3O7-d	Y0.6Pr0.4Ba2Cu3O7-d	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-d		1	1995																											3	Y123							3											K		47		45.8			47						0.31	O	85.5																																																																																								See Phys. Rev. B44, 5318 (1991), Physica B 169, 697(1991)					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11325	PR05111848	O(18)=85.9%	(Y,Pr)Ba2Cu3O7-d	Y0.5Pr0.5Ba2Cu3O7-d	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-d		1	1995																											3	Y123							3											K		32.7		27.7			32.7						0.51	O	85.9																																																																																								See Phys. Rev. B44, 5318 (1991), Physica B 169, 697(1991)					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11326	PR05111848	O(18)=85%	(Y,Pr,Ca)Ba2Cu3O7-d	Y0.8Pr0.2Ba2Cu3O7-d	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-d		1	1995																											3	Y123							3											K		67.7		67.5			67.7						0.14	O	85																																																															m.ohm.cm											0.2														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11327	PR05111848	O(18)+84%	(Y,Pr,Ca)Ba2Cu3O7-d	Y0.75Pr0.2Ca0.05Ba2Cu3O7-d	Y	0.75	Pr	0.2	Ca	0.05	Ba	2	Cu	3											O	7-d		1	1995																											3	Y123							3											K		60.2		63			60.2						0.08	O	84																																																															m.ohm.cm											0.11														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11328	PR05111848	O(18)=78%	(Y,Pr,Ca)Ba2Cu3O7-d	Y0.7Pr0.2Ca0.1Ba2Cu3O7-d	Y	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7-d		1	1995																											3	Y123							3											K		58		55.4			58						0.15	O	78																																																															m.ohm.cm											0.08														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11329	PR05111848	O(18)=77%	(Y,Pr,Ca)Ba2Cu3O7-d	Y0.65Pr0.2Ca0.15Ba2Cu3O7-d	Y	0.65	Pr	0.2	Ca	0.15	Ba	2	Cu	3											O	7-d		1	1995																											3	Y123							3											K		39.3		38.5			39.3						0.07	O	77																																																															m.ohm.cm											0.06														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11330	PR05111848	O(18)=76%	(Y,Pr,Ca)Ba2Cu3O7-d	Y0.6Pr0.2Ca0.2Ba2Cu3O7-d	Y	0.6	Pr	0.2	Ca	0.2	Ba	2	Cu	3											O	7-d		1	1995																											3	Y123							3											K		29.9		29.4			29.9						0.09	O	76																																																															m.ohm.cm											0.12														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11331	PR05111848	O(18)=75%	(Y,Pr,Ca)Ba2Cu3O7-d	Y1.55Pr0.2Ca0.25Ba2Cu3O7-d	Y	1.55	Pr	0.2	Ca	0.25	Ba	2	Cu	3											O	7-d		1	1995																											3	Y123							3											K		20.2		19.1			20.2						0.1	O	75																																																															m.ohm.cm											0.33														See Physeca C 185-189, 1379 (1991).					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11332	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.94Zn0.06O7-d	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-d		1	1995																											3	Y123							3											K		67.7		67.5			67.7						0.09	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11333	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.925Zn0.075O7-d	Y	1	Ba	2	Cu	2.925	Zn	0.075													O	7-d		1	1995																											3	Y123							3											K		60.2		63			60.2						0.06	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11334	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.88Zn0.12O7-d	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-d		1	1995																											3	Y123							3											K		58		55.4			58						0.06	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11335	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.85Zn0.15O7-d	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-d		1	1995																											3	Y123							3											K		39.3		38.5			39.3						0.04	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11336	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.82Zn0.06O7-d	Y	1	Ba	2	Cu	2.82	Zn	0.06													O	7-d		1	1995																											3	Y123							3											K		29.9		29.4			29.9						0.06	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11337	PR05111848	O(18)=86%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.79Zn0.21O7-d	Y	1	Ba	2	Cu	2.79	Zn	0.21													O	7-d		1	1995																											3	Y123							3											K		20.2		19.1			20.2						0.14	O	86																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11338	PR05111848	O(18)=88%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.775Zn0.225O7-d	Y	1	Ba	2	Cu	2.775	Zn	0.225													O	7-d		1	1995																											3	Y123							3											K		13.4		12.7			13.4						0.19	O	88																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11339	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.76Zn0.24O7-d	Y	1	Ba	2	Cu	2.76	Zn	0.24													O	7-d		1	1995																											3	Y123							3											K		9.6					9.6						0.7	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11340	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.745Zn0.255O7-d	Y	1	Ba	2	Cu	2.745	Zn	0.255													O	7-d		1	1995																											3	Y123							3											K		5.7					5.7						0.34	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11341	PR05111848	O(18)=92%	YBa2(Cu,Zn)3O7-d	Y1Ba2Cu2.737Zn0.262O7-d	Y	1	Ba	2	Cu	2.737	Zn	0.262													O	7-d		1	1995																											3	Y123							3											K		8					8						0.27	O	92																																																																																								"See ""Lattice effect in High-Tc Superconductors"",(World Scientific, Singapore, 1992) p148."					Evaliation of oxygen isotope experiments on Pr-,Ca-,and Zn-substituted YBa2Cu3O7	199505		Department of Physics,Simon Fraser University,Burnaby,British Columbia,Canada V5A 1S6	Phys,Rev.B.,51(1995)11848-11859	G.Soerensen,S.Gygax		
11342	PR05111826		(La,Sr)2CaCu2O6-d	La1.8Sr0.2Ca1Cu2O6-d	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6-d		1	1995																											2	2126			A	3.818		19.69	3											K			26.5				26.5																																																																			112			TP11342	m.ohm.cm				44			67				46												La2O3, SrCO3, CuO	1	SIN(at 900C, for 150h, in flowing O2)					Thermoelectric power and resistivity of La1.8Sr0.2CaCu2O6-z and the effects of O2 hot-isostatic-press annealing	199505			Phys.Rev.B,51(1995)11826	C.-J. Liu,H. Yamauchi	La, Sr, Ca, Cu, O	
11343	PR05111826		(La,Sr)2CaCu2O6-d	La1.8Sr0.2Ca1Cu2O6-d	La	1.8	Sr	0.2	Ca	1	Cu	2													O	6-d		1	1995																											2	2126			A	3.818		19.69	3											K	46		58			12	52																																																																			36.9			TP11343	m.ohm.cm				3			2.9				5.1												La2O3, SrCO3, CuO	1	SIN(at 900C, for 150h, in flowing O2), ANN(at 1090C, in mixture of 200atm O2 and 800atm Ar)					Thermoelectric power and resistivity of La1.8Sr0.2CaCu2O6-z and the effects of O2 hot-isostatic-press annealing	199505			Phys.Rev.B,51(1995)11826	C.-J. Liu,H. Yamauchi	La, Sr, Ca, Cu, O	
11344	PR05111767	The Sample is aligned, HC-figure is of Hc2(p=1 for H//ab and p=2 for H//c-axis). Anisotropy factor >8 	HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		2	1995																												Hg1223																		K				133.5			133.5											Oe			50	280					T			1150	149					T/K			12.1	1.6			A	Hao and Clem analysis using magnetization curve. 		15	1.9	A	Hao and Clem analysis using magnetization curve. 		1700	13000																																																	HgO, BaO, CaO, CuO	1	See Physica C 222, 7 (1994).The sample is aligned in a 5T field					Equilibrium superconducting properties of grain-aligned HgBa2Ca2Cu3O8+z	199505			Phys.Rev.B,51(1995)11767	D.K. Christen,J.G. Ossandon,J.R. Thompson,M. Paranthaman,Y.C. Kim	Hg, Ba, Ca, Cu, O	
11700	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.97	Y	1	Ba	2	Cu	3															O		6.97	1	1995																												Y123																		K				91.3		8	91.3																																									A	by muon-SR		1300																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11701	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.962	Y	1	Ba	2	Cu	3															O		6.962	1	1995																												Y123																		K				92.1		7	92.1																																									A	by muon-SR		1350																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11702	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.955	Y	1	Ba	2	Cu	3															O		6.955	1	1995																												Y123																		K				91.8		7	91.8																																				nm					A	by muon-SR		1400																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11703	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.906	Y	1	Ba	2	Cu	3															O		6.906	1	1995																												Y123																		K				92.4		11	92.4																																									A	by muon-SR		1600																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11704	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.828	Y	1	Ba	2	Cu	3															O		6.828	1	1995																												Y123																		K				88		9	88																																									A	by muon-SR		1800																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11705	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.773	Y	1	Ba	2	Cu	3															O		6.773	1	1995																												Y123																		K				71.2		16	71.2																																									A	by muon-SR		2100																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11706	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.702	Y	1	Ba	2	Cu	3															O		6.702	1	1995																												Y123																		K				69		13	69																																									A	by muon-SR		2100																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11707	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.666	Y	1	Ba	2	Cu	3															O		6.666	1	1995																												Y123																		K				60.5		17	60.5																																									A	by muon-SR		2250																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11708	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.602	Y	1	Ba	2	Cu	3															O		6.602	1	1995																												Y123																		K				59.4		17	59.4																																									A	by muon-SR		2200																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11709	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.556	Y	1	Ba	2	Cu	3															O		6.556	1	1995																												Y123																		K				58.5		8	58.5																																									A	by muon-SR		2250																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11710	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.546	Y	1	Ba	2	Cu	3															O		6.546	1	1995																												Y123																		K				59.4		12	59.4																																									A	by muon-SR		2550																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11711	PR05200541		YBa2Cu3O7	Y1Ba2Cu3O6.516	Y	1	Ba	2	Cu	3															O		6.516	1	1995																												Y123																		K				58.7		12	58.7																																									A	by muon-SR		2500																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11712	PR05200541		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1995																												Y124																		K				82		4	82																																									A	by muon-SR		1600																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11713	PR05200541		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		1	1995																												Bi2212																		K				83.5		18	83.5																																									A	by muon-SR		2050																																																			1	The samples used in this study were sintered disks of high quality with diameters between 10 and 25 mm.					Mnoun-spin rotation studies of the temperature dependence of the magnetic penetration depth in the YBa2Cu3Ox family and related compounds	199507			Phys.Rav.B,52(1995)541	"C. Kru""ger,D. Zech,E. Kaldis,E. M. Forgan,H. Keller,I. M. Savic',J. Karpinski,M. Warden,P. Zimmermann,R. Cubitt,S. L. Lee"	Y, Ba, Cu, O	
11714	PR05200727		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11715	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.99Co0.01O8+d	Bi	2	Sr	2	Ca	1	Cu	1.99	Co	0.01											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11716	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.98Co0.02O8+d	Bi	2	Sr	2	Ca	1	Cu	1.98	Co	0.02											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11717	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.96Co0.04O8+d	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11718	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.92Co0.08O8+d	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11719	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.88Co0.12O8+d	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11720	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.84Co0.16O8+d	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11721	PR05200727		Bi2Sr2Ca(Cu,Co)2O8	Bi2Sr2Ca1Cu1.8Co0.2O8+d	Bi	2	Sr	2	Ca	1	Cu	1.8	Co	0.2											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11722	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.98Fe0.02O8+d	Bi	2	Sr	2	Ca	1	Cu	1.98	Fe	0.02											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11723	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.96Fe0.04O8+d	Bi	2	Sr	2	Ca	1	Cu	1.96	Fe	0.04											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11724	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.92Fe0.08O8+d	Bi	2	Sr	2	Ca	1	Cu	1.92	Fe	0.08											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11725	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.88Fe0.12O8+d	Bi	2	Sr	2	Ca	1	Cu	1.88	Fe	0.12											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11726	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.84Fe0.16O8+d	Bi	2	Sr	2	Ca	1	Cu	1.84	Fe	0.16											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11727	PR05200727		Bi2Sr2Ca(Cu,Fe)2O8	Bi2Sr2Ca1Cu1.8Fe0.2O8+d	Bi	2	Sr	2	Ca	1	Cu	1.8	Fe	0.2											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11728	PR05200727		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.99Ni0.01O8+d	Bi	2	Sr	2	Ca	1	Cu	1.99	Ni	0.01											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11729	PR05200727		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.98Ni0.02O8+d	Bi	2	Sr	2	Ca	1	Cu	1.98	Ni	0.02											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11730	PR05200727		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.97Ni0.03O8+d	Bi	2	Sr	2	Ca	1	Cu	1.97	Ni	0.03											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11731	PR05200727		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.96Ni0.04O8+d	Bi	2	Sr	2	Ca	1	Cu	1.96	Ni	0.04											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11732	PR05200727		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr2Ca1Cu1.92Ni0.08O8+d	Bi	2	Sr	2	Ca	1	Cu	1.92	Ni	0.08											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11733	PR05200727		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.99Zn0.01O8+d	Bi	2	Sr	2	Ca	1	Cu	1.99	Zn	0.01											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11734	PR05200727		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	1	Cu	1.98	Zn	0.02											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11735	PR05200727		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.97Zn0.03O8+d	Bi	2	Sr	2	Ca	1	Cu	1.97	Zn	0.03											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11736	PR05200727		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	1	Cu	1.96	Zn	0.04											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11737	PR05200727		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.92Zn0.08O8+d	Bi	2	Sr	2	Ca	1	Cu	1.92	Zn	0.08											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11738	PR05200727		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11739	PR05200727		Bi2Sr2(Ca,Y)(Cu,Co)2O8	Bi2Sr2Ca0.7Y0.3Cu1.99Co0.01O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.99	Co	0.01									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11740	PR05200727		Bi2Sr2(Ca,Y)(Cu,Co)2O8	Bi2Sr2Ca0.7Y0.3Cu1.98Co0.02O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.98	Co	0.02									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11741	PR05200727		Bi2Sr2(Ca,Y)(Cu,Co)2O8	Bi2Sr2Ca0.7Y0.3Cu1.96Co0.04O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.96	Co	0.04									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11742	PR05200727		Bi2Sr2(Ca,Y)(Cu,Co)2O8	Bi2Sr2Ca0.7Y0.3Cu1.92Co0.08O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.92	Co	0.08									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11743	PR05200727		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.99Zn0.01O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.99	Zn	0.01									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11744	PR05200727		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.98	Zn	0.02									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11745	PR05200727		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.96	Zn	0.04									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11746	PR05200727		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.88Zn0.12O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.88	Zn	0.12									O	8+d		1	1995																												Bi2212																																																																																																																								1	Bi:Sr:[Ca,Y]:[Cu,Mo] = 2:2:1:2The value of d was changed by ANN(O2 or N2 gas,350-600C,24h)					Clear distinction between the underdoped and overdoped regime in the Tc suppression of Cu-site-substituted high-Tc cuprates	199507		Department of Applied Physics,Faculty of Engineering,Tohoku University,Aramaki Aova-ku,Sendai 980,Japan	Phys.Rev.B,52(1995)R727	A. Fujiwara,A.Fugiwara,M. Kato,M.Kato,T. Kluge,T. Noji,T.Kluge,T.Nogi,Y. Koike,Y. Saito,Y.Koike,Y.Saito		
11747	PR05201362		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.9Ce0.05Ca0.05Ba2Cu3O7-d	Lu	0.9	Ce	0.05	Ca	0.05	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	81						81																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11748	PR05201362		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.8Ce0.1Ca0.1Ba2Cu3O7-d	Lu	0.8	Ce	0.1	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	74						74																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11749	PR05201362		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.8Ce0.15Ca0.05Ba2Cu3O7-d	Lu	0.8	Ce	0.15	Ca	0.05	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	63						63																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11750	PR05201362		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.75Ce0.15Ca0.1Ba2Cu3O7-d	Lu	0.75	Ce	0.15	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	69						69																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11751	PR05201362		(Lu,Ce,Ca)Ba2Cu3O7	Lu0.7Ce0.15Ca0.15Ba2Cu3O7-d	Lu	0.7	Ce	0.15	Ca	0.15	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	58						58																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11752	PR05201362		LuBa2Cu3O7	Lu1Ba2Cu3O7-d	Lu	1	Ba	2	Cu	3															O	7-d		4	1995																												Y123																		K	88						88																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11753	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.93Pr0.07Ba2Cu3O7-d	Lu	0.93	Pr	0.07	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	85						85																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11754	PR05201362		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.9Pr0.05Ca0.05Ba2Cu3O7-d	Lu	0.9	Pr	0.05	Ca	0.05	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	82						82																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11755	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.9Pr0.1Ba2Cu3O7-d	Lu	0.9	Pr	0.1	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	83						83																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11756	PR05201362		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.8Pr0.1Ca0.1Ba2Cu3O7-d	Lu	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	78						78																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11757	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.8Pr0.2Ba2Cu3O7-d	Lu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	79						79																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11758	PR05201362		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.7Pr0.2Ca0.1Ba2Cu3O7-d	Lu	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	76						76																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11759	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.7Pr0.3Ba2Cu3O7-d	Lu	0.7	Pr	0.3	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	70						70																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11760	PR05201362		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.6Pr0.3Ca0.1Ba2Cu3O7-d	Lu	0.6	Pr	0.3	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	74						74																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11761	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.6Pr0.4Ba2Cu3O7	Lu	0.6	Pr	0.4	Ba	2	Cu	3													O	7		4	1995																												Y123																		K	54						54																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11762	PR05201362		(Lu,Pr,Ca)Ba2Cu3O7	Lu0.5Pr0.4Ca0.1Ba2Cu3O7-d	Lu	0.5	Pr	0.4	Ca	0.1	Ba	2	Cu	3											O	7-d		4	1995																												Y123																		K	57						57																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11763	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.5Pr0.5Ba2Cu3O7-d	Lu	0.5	Pr	0.5	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	37						37																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11764	PR05201362		(Lu,Pr)Ba2Cu3O7	Lu0.55Pr0.45Ba2Cu3O7-d	Lu	0.55	Pr	0.45	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K	24						24																																																																																																				pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11765	PR05201362		(Lu,Tb)Ba2Cu3O7	Lu0.9Tb0.1Ba2Cu3O7-d	Lu	0.9	Tb	0.1	Ba	2	Cu	3													O	7-d		4	1995																												Y123																		K																																																																																																											pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11766	PR05201362		(Lu,Tb)Ba2Cu3O7	Lu0.8Tb0.2Ba2Cu3O7-d	Lu	0.8	Tb	0.2	Ba	2	Cu	3													O	7-d		4	1995																												Y123																																																																																																																													pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11767	PR05201362		(Lu,Tb)Ba2Cu3O7	Lu0.7Tb0.3Ba2Cu3O7-d	Lu	0.7	Tb	0.3	Ba	2	Cu	3													O	7-d		4	1995																												Y123																																																																																																																													pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11768	PR05201362		(Lu,Tb)Ba2Cu3O7	Lu0.5Tb0.5Ba2Cu3O7-d	Lu	0.5	Tb	0.5	Ba	2	Cu	3													O	7-d		4	1995																												Y123																																																																												3000000																																																	pulsed laser ablation technique.In detail, see Phys. Rev. B 46 14242 (1992)	Structural stability of LuBa2Cu3O7-z and superconductivity in thin films of Lu1-xMxBa2Cu3O7-z(M=Pr, Tb, and Ce)	199507			Phys.Rev.B,52(1995)1362	A. S. Tamhane,L.C. Gupta,P.R. Apte,R. Pinto,S.P. Pai	Lu, Ba, Cu, O, Pr, Tb, Ce	
11769	PR05201389		Sr2PrNbCu2O8	Sr2Pr1Nb1Cu2O8-d	Sr	2	Pr	1	Nb	1	Cu	2													O	8-d		1	1995	emu/mol	0.00087			myu-B/mol	3.02	-12.8	2.3																				2112			nm	0.551		2.336	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11770	PR05201389		Sr2NdNbCu2O8	Sr2Nd1Nb1Cu2O8-d	Sr	2	Nd	1	Nb	1	Cu	2													O	8-d		1	1995	emu/mol	0.00202			myu-B/mol	3.1	-13																					2112			nm	0.55		2.336	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11771	PR05201389		Sr2SmNbCu2O8	Sr2Sm1Nb1Cu2O8-d	Sr	2	Sm	1	Nb	1	Cu	2													O	8-d		1	1995	emu/mol	0.00113			myu-B/mol	0.68	-5.8																					2112			nm	0.548		2.327	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11772	PR05201389		Sr2EuNbCu2O8	Sr2Eu1Nb1Cu2O8-d	Sr	2	Eu	1	Nb	1	Cu	2													O	8-d		1	1995	emu/mol	0.00099			myu-B/mol	0.44	-5.8																					2112			nm	0.547		2.326	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11773	PR05201389		Sr2GdNbCu2O8	Sr2Gd1Nb1Cu2O8-d	Sr	2	Gd	1	Nb	1	Cu	2													O	8-d		1	1995	emu/mol	0.0001			myu-B/mol	7.97	-3.6	2.18																				2112			nm	0.55		2.345	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11774	PR05201389		Sr2PrTaCu2O8	Sr2Pr1Ta1Cu2O8-d	Sr	2	Pr	1	Ta	1	Cu	2													O	8-d		1	1995	emu/mol	0.00091			myu-B/mol	2.89	-12	2.2																				2112			nm	0.549		2.342	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11775	PR05201389		Sr2NdTaCu2O8	Sr2Nd1Ta1Cu2O8-d	Sr	2	Nd	1	Ta	1	Cu	2													O	8-d		1	1995	emu/mol	0.00161			myu-B/mol	2.87	-14																					2112			nm	0.548		2.337	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11776	PR05201389		Sr2SmTaCu2O8	Sr2Sm1Ta1Cu2O8-d	Sr	2	Sm	1	Ta	1	Cu	2													O	8-d		1	1995	emu/mol	0.00122			myu-B/mol	0.66	-5																					2112			nm	0.547		2.333	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11777	PR05201389		Sr2EuTaCu2O8	Sr2Eu1Ta1Cu2O8-d	Sr	2	Eu	1	Ta	1	Cu	2													O	8-d		1	1995	emu/mol	0.00103			myu-B/mol	0.43	-7																					2112			nm	0.457		2.332	4																																																																																																																Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11778	PR05201389		Sr2GdTaCu2O8	Sr2Gd1Ta1Cu2O8-d	Sr	2	Gd	1	Ta	1	Cu	2													O	8-d		1	1995	emu/mol	0.0001			myu-B/mol	8.03	-2.8	2.18																				2112																																																																																																																							Nb2O5,Ta2O5,Pr6O11,Nd2O3,Sm2O3,Eu2O3		continuition from RAWMAT : Gd2O3,SrCO3,CuO.CAL(air,900) - pelletized - ANNANN(air,1000C,18h)					Synthesis and characterization of compounds Sr2RMCu2O8-z     (R=Pr, Nd, Sm, Eu, Gd; M =Nb, Ta)	199507			Phys.Rev.B,52(1995)1389	G. Hilscher,H. Michor,M. Divis,M. Vybornov,P. Fischer,P. Rogl,T. Holubar,W. Perthold	Sr, Pr, Nd, Sm, Em, Eu, GD, Nb, Ta, Cu, O	
11779	PR05200570	dTc/dP(ab) is writted in SUPERCONDUCTIVITY section.dTc/dP(c) is -6.6 K/GPa	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	1995																												T																		K					25.8					K/GPa	3.2																																																		mJ/mole.K	134																																									See Nature 337.21 (1989)					Unconventional lattice stiffening in superconducting La2-xSrxCuO4 single crystals	199507			Phys.Rev.B,52(1995)570	Minoru Nohara,Takashi Suzuki,Toshizo Fujita,Yoshiteru Maeno	La, Sr, Cu, O	
11780	PR05200570	dTc/dP(ab) is writted in SUPERCONDUCTIVITY section.dTc/dP(c) is -6.5 K/GPa	(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4		3	1995																												T																		K					35					K/GPa	3.8																																																		mJ/mole.K	336																																									See Nature 337.21 (1989)					Unconventional lattice stiffening in superconducting La2-xSrxCuO4 single crystals	199507			Phys.Rev.B,52(1995)570	Minoru Nohara,Takashi Suzuki,Toshizo Fujita,Yoshiteru Maeno	La, Sr, Cu, O	
11781	PR05200570	dTc/dP(ab) is writted in SUPERCONDUCTIVITY section.dTc/dP(c) is -5.4 K/GPa	(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4		3	1995																												T																		K					38.7					K/GPa	2.9																																																		mJ/mole.K	293																																									See Nature 337.21 (1989)					Unconventional lattice stiffening in superconducting La2-xSrxCuO4 single crystals	199507			Phys.Rev.B,52(1995)570	Minoru Nohara,Takashi Suzuki,Toshizo Fujita,Yoshiteru Maeno	La, Sr, Cu, O	
11782	PR05201347		(La,Ca)2NiO4	La1.67Ca0.33Ni1O4	La	1.67	Ca	0.33	Ni	1															O	4		1	1995																												T			A	3.818		12.58	3																																																																																																																	1	see P.R.B 49,7088 (1994)					Structural aspects of pressure-dependent hole ordering in La1.67M0.33Nio4     ( M=Ca, Sr, or, Ba)	199507			Phys.Rev.B,52(1995)1347	A. S. Cooper,J. D. Sullivan,M. B. Maple,M. Marezio,O. Chmaissem,S-W. Cheong,S. H. Han,Z. Fisk	La, Ca, Sr, Ba, Ni, O	
11783	PR05201347		(La,Sr)2NiO4	La1.67Sr0.33Ni1O4	La	1.67	Sr	0.33	Ni	1															O	4		1	1995																												T			A																																																																																																																					1	see P.R.B 49,7088 (1994)					Structural aspects of pressure-dependent hole ordering in La1.67M0.33Nio4     ( M=Ca, Sr, or, Ba)	199507			Phys.Rev.B,52(1995)1347	A. S. Cooper,J. D. Sullivan,M. B. Maple,M. Marezio,O. Chmaissem,S-W. Cheong,S. H. Han,Z. Fisk	La, Ca, Sr, Ba, Ni, O	
11784	PR05201347		(La,Ba)2NiO4	La1.67Ba0.33Ni1O4	La	1.67	Ba	0.33	Ni	1															O	4		1	1995																												T			A	3.847		12.81	3																																																																																																																	1	see P.R.B 49,7088 (1994)					Structural aspects of pressure-dependent hole ordering in La1.67M0.33Nio4     ( M=Ca, Sr, or, Ba)	199507			Phys.Rev.B,52(1995)1347	A. S. Cooper,J. D. Sullivan,M. B. Maple,M. Marezio,O. Chmaissem,S-W. Cheong,S. H. Han,Z. Fisk	La, Ca, Sr, Ba, Ni, O	
11785	PR05201320		ErBa2(Cu,Fe)3O7	Er1Ba2Cu2.985Fe0.015O7-d	Er	1	Ba	2	Cu	2.985	Fe	0.015													O	7-d		1	1995									5																			Y123																		K	88.5			88.7			88.7																																																																																															1	CAL(910C,24h) - SIN(935C,24h,flow O2) - SIN(600C,8h)- COOL(R.T.)					Low-field ac-susceptibility study of flux creep in metal-substituted ErBa2Cu3O7-z	199507			Peys.Rev.B,52(1995)1320	A. V. Narlikar,B. V. Kumaraswamy,Ratan Lal	Er, Ba, Cu, O	
11786	PR05201320		ErBa2(Cu,Co)3O7	Er1Ba2Cu2.985Co0.015O7-d	Er	1	Ba	2	Cu	2.985	Co	0.015													O	7-d		1	1995									4.6																			Y123																		K	89.1			89			89																																																																																															1	CAL(910C,24h) - SIN(935C,24h,flow O2) - SIN(600C,8h)- COOL(R.T.)					Low-field ac-susceptibility study of flux creep in metal-substituted ErBa2Cu3O7-z	199507			Peys.Rev.B,52(1995)1320	A. V. Narlikar,B. V. Kumaraswamy,Ratan Lal	Er, Ba, Cu, O	
11787	PR05201320		ErBa2(Cu,Ni)3O7	Er1Ba2Cu2.985Ni0.015O7-d	Er	1	Ba	2	Cu	2.985	Ni	0.015													O	7-d		1	1995									4.9																			Y123																		K	89.9			89.8			89.8																																																																																															1	CAL(910C,24h) - SIN(935C,24h,flow O2) - SIN(600C,8h)- COOL(R.T.)					Low-field ac-susceptibility study of flux creep in metal-substituted ErBa2Cu3O7-z	199507			Peys.Rev.B,52(1995)1320	A. V. Narlikar,B. V. Kumaraswamy,Ratan Lal	Er, Ba, Cu, O	
11788	PR05201320		ErBa2(Cu,Ga)3O7	Er1Ba2Cu2.985Ga0.015O7-d	Er	1	Ba	2	Cu	2.985	Ga	0.015													O	7-d		1	1995									5																			Y123																		K	89.8			89.5			89.5																																																																																															1	CAL(910C,24h) - SIN(935C,24h,flow O2) - SIN(600C,8h)- COOL(R.T.)					Low-field ac-susceptibility study of flux creep in metal-substituted ErBa2Cu3O7-z	199507			Peys.Rev.B,52(1995)1320	A. V. Narlikar,B. V. Kumaraswamy,Ratan Lal	Er, Ba, Cu, O	
11789	PR05201320		ErBa2Cu3O7	Er1Ba2Cu3O7-d	Er	1	Ba	2	Cu	3															O	7-d		1	1995									4.6																			Y123																		K	92.8			92.5			92.5																																																																																															1	CAL(910C,24h) - SIN(935C,24h,flow O2) - SIN(600C,8h)- COOL(R.T.)					Low-field ac-susceptibility study of flux creep in metal-substituted ErBa2Cu3O7-z	199507			Peys.Rev.B,52(1995)1320	A. V. Narlikar,B. V. Kumaraswamy,Ratan Lal	Er, Ba, Cu, O	
11790	PR05200071		(Y,Tb)Ba2Cu3O7	Y0.9Tb0.1Ba2Cu3O7	Y	0.9	Tb	0.1	Ba	2	Cu	3													O	7		3	1995																												Y123																		K			91			1.2	91																																																																																															5	In detail, see Ph.D Thesis, Department of Physics, Temple Univ., 1992Annealing process : ANN(450C, high-pressure O2)					Evidence of unusual hybridization: Electrical resistivity and specific heat of Y1-xTbxBa2Cu3O7 single crystals	199507		National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32306-4005	Phys.Rev.B,52(1995)71	F. Freibert,G. Cao,J.E. Crow,M. Shepard,P. Henning,S. McCall		
11791	PR05200071		(Y,Tb)Ba2Cu3O7	Y0.68Tb0.32Ba2Cu3O7	Y	0.68	Tb	0.32	Ba	2	Cu	3													O	7		3	1995																												Y123																		K			91			1.2	91																																																																																															5	In detail, see Ph.D Thesis, Department of Physics, Temple Univ., 1992Annealing process : ANN(450C, high-pressure O2)					Evidence of unusual hybridization: Electrical resistivity and specific heat of Y1-xTbxBa2Cu3O7 single crystals	199507		National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32306-4005	Phys.Rev.B,52(1995)71	F. Freibert,G. Cao,J.E. Crow,M. Shepard,P. Henning,S. McCall		
11792	PR05200462	As-prepared	HgBa2CuO4	Hg1Ba2Cu1O4.18	Hg	1	Ba	2	Cu	1															O		4.18	1	1995																												Hg1201			A	3.881		9.528	3											K				95			95																																																																																															1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11793	PR05200462	ANN(vacuum)	HgBa2CuO4	Hg1Ba2Cu1O4.08	Hg	1	Ba	2	Cu	1															O		4.08	1	1995																												Hg1201			A	3.893		9.528	3											K				53			53																																																																																															1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11794	PR05200462	Reannealing a previous material(No.11793) in Oxygen.	HgBa2CuO4	Hg1Ba2Cu1O4.18	Hg	1	Ba	2	Cu	1															O		4.18	1	1995																												Hg1201			A	3.881		9.528	3											K				94			94																																																																																															1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11795	PR05200462	Reannealing a previous material(No.11794) in vaccum.	HgBa2CuO4	Hg1Ba2Cu1O4.04	Hg	1	Ba	2	Cu	1															O		4.04	1	1995																												Hg1201			A	3.896		9.533	3											K																																																																																																						1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11796	PR05200462	Reannealing a previous material(No.11795) in high pressure Oxygen.	HgBa2CuO4	Hg1Ba2Cu1O4.23	Hg	1	Ba	2	Cu	1															O		4.23	1	1995																												Hg1201			A	3.876		9.517	3											K				30			30																																																																																															1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11797	PR05200462	As prepared in high pressure oxygen.	HgBa2CuO4	Hg1Ba2Cu1O4.21	Hg	1	Ba	2	Cu	1															O		4.21	1	1995																												Hg1201			A	3.877		9.522	3											K				80			80																																																																																															1	see Meng et al. Physica C 216,21 (1993)About annealing condition, see material comments.					Oxygen dependens  of the crystal structure of HgBa2CuO4+z and its relation tosuperconductivity	199507			Phys.Rev.B,52(1995)462	C. W. Chu,J. W. Lynn,Q. Huang,Q. Xiong	Hg, Ba, Cu, O	
11800	PR05207030		DyBa2Cu3O7	Dy1Ba2Cu3O7-d	Dy	1	Ba	2	Cu	3															O	7-d		1	1995																												Y123																		K		76.3					76.3																																																																	THC11800																														1	SIN(several times, air, 900C)-press-SIN(3 times, 12h,20% argon, total pressure 3kbar, 1050C)					Evidence for the shift of the transition temperature in RBa2Cu4O8 by thermal-coductivity measurements	199509			Phys.Rev.B,52(1995)R7030	A. Jezowski,B. Dobrowski,J. Klamut	Dy, Gd, Eu, Ba, Cu,O	
11801	PR05207030		GdBa2Cu3O7	Gd1Ba2Cu3O7-d	Gd	1	Ba	2	Cu	3															O	7-d		1	1995																												Y123																		K		73.1					73.1																																																																	THC11801																														1	SIN(several times, air, 900C)-press-SIN(3 times, 12h,20% argon, total pressure 3kbar, 1050C)					Evidence for the shift of the transition temperature in RBa2Cu4O8 by thermal-coductivity measurements	199509			Phys.Rev.B,52(1995)R7030	A. Jezowski,B. Dobrowski,J. Klamut	Dy, Gd, Eu, Ba, Cu,O	
11802	PR05207030		EuBa2Cu3O7	Eu1Ba2Cu3O7-d	Eu	1	Ba	2	Cu	3															O	7-d		1	1995																												Y123																		K		68					68																																																																	THC11802																														1	SIN(several times, air, 900C)-press-SIN(3 times, 12h,20% argon, total pressure 3kbar, 1050C)					Evidence for the shift of the transition temperature in RBa2Cu4O8 by thermal-coductivity measurements	199509			Phys.Rev.B,52(1995)R7030	A. Jezowski,B. Dobrowski,J. Klamut	Dy, Gd, Eu, Ba, Cu,O	
11803	PR05206840	86%O(18), deltaTc=1.5K	(La,Sr)2CuO4	La1.895Sr0.105Cu1O4	La	1.895	Sr	0.105	Cu	1															O	4		1	1995																												T																		K				26.3			26.3						0.5	O	86	1.5	15.5																																																																																				La2O3,SrCO3,CuO	1	MIX-Press(Pellet)-SIN(air,1000C,70h with 3 intermediate grindings)-ANN(air,900C,12h)Half pellets were subjected to 16O and 18O isotope diffusion.Diffusion(40h,900C,18O2 gas)					Oxygen isotope effect mass of caarriers from magnetik measurements on La2-xSrxCuO4	199509			Phys.Rev.B,52(1995)6840	A.P.B. Sinha,D.E. Morris,Guo-meng  Zhao,K.K. Singh	La, Sr, Cu, O	
11804	PR05206840	90%O(18), deltaTc=1.6K	(La,Sr)2CuO4	La1.89Sr0.11Cu1O4	La	1.89	Sr	0.11	Cu	1															O	4		1	1995																												T																		K				24.5			24.5						0.54	O	90	1.6	14																																																																																				La2O3,SrCO3,CuO	1	MIX-Press(Pellet)-SIN(air,1000C,70h with 3 intermediate grindings)-ANN(air,900C,12h)Half pellets were subjected to 16O and 18O isotope diffusion.Diffusion(40h,900C,18O2 gas)					Oxygen isotope effect mass of caarriers from magnetik measurements on La2-xSrxCuO4	199509			Phys.Rev.B,52(1995)6840	A.P.B. Sinha,D.E. Morris,Guo-meng  Zhao,K.K. Singh	La, Sr, Cu, O	
11805	PR05206840	85%O(18), deltaTc=2.6K	(La,Sr)2CuO4	La1.885Sr0.115Cu1O4	La	1.885	Sr	0.115	Cu	1															O	4		1	1995																												T																		K				24.7			24.7						0.9	O	85	2.6	12.1																																																																																				La2O3,SrCO3,CuO	1	MIX-Press(Pellet)-SIN(air,1000C,70h with 3 intermediate grindings)-ANN(air,900C,12h)Half pellets were subjected to 16O and 18O isotope diffusion.Diffusion(40h,900C,18O2 gas)					Oxygen isotope effect mass of caarriers from magnetik measurements on La2-xSrxCuO4	199509			Phys.Rev.B,52(1995)6840	A.P.B. Sinha,D.E. Morris,Guo-meng  Zhao,K.K. Singh	La, Sr, Cu, O	
11806	PR05207656		(Nd,Ce)2CuO4	Nd1.86Ce0.14Cu1O4-y	Nd	1.86	Ce	0.14	Cu	1															O	4-y		1	1995	emu/mol Nd	0.000479	emu.K/mol	1.49	myu-B/Nd	3.46	-41.2																					T'																																																																																																																								1	High temperature solid state reaction (see Physica C 167,53 (1990))ANN(as-prepared samples, 850C, 6h, 10e-5 mbar)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11807	PR05207656		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-y	Nd	1.85	Ce	0.15	Cu	1															O	4-y		1	1995	emu/mol Nd	0.000482	emu.K/mol	1.48	myu-B/Nd	3.44	-43																					T'																																																																																																																								1	High temperature solid state reaction (see Physica C 167,53 (1990))ANN(as-prepared samples, 850C, 6h, 10e-5 mbar)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11808	PR05207656		(Nd,Ce)2CuO4	Nd1.84Ce0.16Cu1O4-y	Nd	1.84	Ce	0.16	Cu	1															O	4-y		1	1995	emu/mol Nd	0.000432	emu.K/mol	1.29	myu-B/Nd	3.21	-38																					T'																																																																																																																								1	High temperature solid state reaction (see Physica C 167,53 (1990))ANN(as-prepared samples, 850C, 6h, 10e-5 mbar)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11809	PR05207656		(Nd,Ce)2CuO4	Nd1.82Ce0.18Cu1O4-y	Nd	1.82	Ce	0.18	Cu	1															O	4-y		1	1995	emu/mol Nd	0.001	emu.K/mol	1.32	myu-B/Nd	3.25	-48																					T'																																																																																																																								1	High temperature solid state reaction (see Physica C 167,53 (1990))ANN(as-prepared samples, 850C, 6h, 10e-5 mbar)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11810	PR05207656		NdBa2Cu3O7	Nd1Ba2Cu3O7-y	Nd	1	Ba	2	Cu	3															O	7-y		1	1995	emu/mol Nd	0.0013	emu.K/mol	1.22	myu-B/Nd	3.13	-29.2																					Y123																																																																																	mJ/molK2	8.1		351																																				1	See Phys. Rev. B 48, 16727 (1993)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11811	PR05207656		NeBa2(Cu,Zn)3O7	Nd1Ba2Cu2.98Zn0.02O7-d	Nd	1	Ba	2	Cu	2.98	Zn	0.02													O	7-d		1	1995	emu/mol Nd	0.0021	emu.K/mol	1.08	myu-B/Nd	2.94	-23																					Y123																																																																																																																								1	See Phys. Rev. B 48, 16727 (1993)					Magnetic susceptibility, specific heat, and crystal-field effects in neodymium cuprate superconductors	199509			Phys.Rev.B,52(1995)7656	G. Rangarajan,Nithya Ravindran,S. Uma,T. Sarkar,V. Sankaranarayanan		
11812	PR05207647		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		3	1995																												Bi2212			A	5.4	5.4	30.97	1											K	85	92	95			10	92																																																																						TP11812																								Bi2O3,CaCO3,SrCO3,CuO	7	MIX-SIN(860C,O2,24h, 2 times)-Press-SIN(865C,air,24h)FZ: pulling rate;first 80 mm/h, second 1 mm/h (2bars air)					Mixed-state thermoelectric and thermomagnetic effects of a Bi2Sr2CaCu2O8+z single crystal	199509			Phys.Rev.B,52(1995)7647	D. Hu,M. Ausloos,V. Brabers	Bi, Sr, Ca, Cu,O	
11813	PR05207046		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1995																												T'																		K				24			24																																																																																																c-axis oriented 20 micron single crystal (details, see Physica C 177, 79 (1991))					Anisotropy, pinning, and the mixed-state Hall effect	199509			Phys.Rev.B,52(1995)R7046	A.W. Smith,C.J. Lobb,J.L. Peng,Qi. Li,R.L. Greene,T.W. Clinton		
11814	PR05207046	c-axis oriented film (5000A).	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		4	1995																												Tl2212																		K				104			104																																																			10000000																																																	Laser ablation method.	Anisotropy, pinning, and the mixed-state Hall effect	199509			Phys.Rev.B,52(1995)R7046	A.W. Smith,C.J. Lobb,J.L. Peng,Qi. Li,R.L. Greene,T.W. Clinton		
11815	PR05207046		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1995																												Y123																		K				92			92																																																																																																				Laser ablation method.	Anisotropy, pinning, and the mixed-state Hall effect	199509			Phys.Rev.B,52(1995)R7046	A.W. Smith,C.J. Lobb,J.L. Peng,Qi. Li,R.L. Greene,T.W. Clinton		
11816	PR05207619		YBa2Cu3O7	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	6		1	1995																											2	Y123			A	3.847		11.795	3																																																																																																															297000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11817	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F0.17O6	Y	1	Ba	2	Cu	3	F	0.17													O	6		1	1995																											2	Y123			A	3.857		11.801	3																																																																																																															450000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11818	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F0.38O6	Y	1	Ba	2	Cu	3	F	0.38													O	6		1	1995																											2	Y123			A	3.86		11.772	3																																																																																																																Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11819	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F0.76O6	Y	1	Ba	2	Cu	3	F	0.76													O	6		1	1995																											2	Y123			A	3.863		11.745	3											K			35				35																																																																																													33600000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11820	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F1.11O6	Y	1	Ba	2	Cu	3	F	1.11													O	6		1	1995																											2	Y123			A	3.867		11.739	3											K			45				45																																																																																													97800000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11821	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F1.26O6	Y	1	Ba	2	Cu	3	F	1.26													O	6		1	1995																											2	Y123			A	3.868		11.715	3											K			55				55																																																																																													119000000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11822	PR05207619		YBa2Cu3O7Fx	Y1Ba2Cu3F1.46O6	Y	1	Ba	2	Cu	3	F	1.46													O	6		1	1995																											2	Y123			A	3.871		11.709	3											K			55				55																																																																																													205000000000000000000	Y2O3,BaCO3,CuO	1	CAL(2h,970C)-Quench(air)-Press(pellet)-SIN(2h,970C)-Quench(air)-Heat(vaccum)-Heat(NF3,320C)					Charge transfer in YBa2Cu3O6 doped with fluorine: Infrared reflectance and Raman scattering studies	199509		Laboratoire de Physique des Solides, CNRS URA 154, Universite' Pierre et Marie Curie, Tour 13, E2, 4 Place Jussieu, 75252 Paris, Case 79, Cedex 05, France	Phys.Rev.B,52(1995)7619	A. Sacuto,C. Julien,C. Perrin,M. Mokhtari,V.A. Shchukin		
11823	PR05207034		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1995																												Y124																						80			80																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11824	PR05207034		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.972Zn0.028O8	Y	1	Ba	2	Cu	3.972	Zn	0.028													O	8		1	1995																												Y124																						63			63																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11825	PR05207034		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.95Zn0.05O8	Y	1	Ba	2	Cu	3.95	Zn	0.05													O	8		1	1995																												Y124																						47.5			47.5																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11826	PR05207034		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.924Zn0.076O8	Y	1	Ba	2	Cu	3.924	Zn	0.076													O	8		1	1995																												Y124																						30.1			30.1																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11827	PR05207034		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.9Zn0.1O8	Y	1	Ba	2	Cu	3.9	Zn	0.1													O	8		1	1995																												Y124																						11.5			11.5																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11828	PR05207034		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.85Zn0.15O8	Y	1	Ba	2	Cu	3.85	Zn	0.15													O	8		1	1995																												Y124																							4.2																																																																																																Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11829	PR05207034		Y(Ba,La)2Cu4O8	Y1Ba1.9La0.1Cu3O8	Y	1	Ba	1.9	La	0.1	Cu	3													O	8		1	1995																												Y124																						64			64																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11830	PR05207034		Y(Ba,La)2(Cu,Zn)4O8	Y1Ba1.9La0.1Cu3.972Zn0.028O8	Y	1	Ba	1.9	La	0.1	Cu	3.972	Zn	0.028											O	8		1	1995																												Y124																						48.7			48.7																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11831	PR05207034		Y(Ba,La)2(Cu,Zn)4O8	Y1Ba1.9La0.1Cu3.95Zn0.05O8	Y	1	Ba	1.9	La	0.1	Cu	3.95	Zn	0.05											O	8		1	1995																												Y124																						33.3			33.3																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11832	PR05207034		Y(Ba,La)2(Cu,Zn)4O8	Y1Ba1.9La0.1Cu3.93Zn0.07O8	Y	1	Ba	1.9	La	0.1	Cu	3.93	Zn	0.07											O	8		1	1995																												Y124																						17.8			17.8																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11833	PR05207034		Y(Ba,La)2Cu4O8	Y1Ba1.8La0.2Cu4O8	Y	1	Ba	1.8	La	0.2	Cu	4													O	8		1	1995																												Y124																						44			44																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11834	PR05207034		Y(Ba,La)2(Cu,Zn)4O8	Y1Ba1.8La0.2Cu3.97Zn0.03O8	Y	1	Ba	1.8	La	0.2	Cu	3.97	Zn	0.03											O	8		1	1995																												Y124																						16.2			16.2																																																																																														Y2O3,La(NO3)3.6H2O,Ba(NO3)2,CuO,ZnO	1	SIN(6h,930C)-SIN(48h,940C)-SIN(48h,940C,O2,6MPa)					89 Y NMR study of Zn-induced local moments and pair breaking Y(Ba1-yLay)2(Cu1-xZnx)4O8	199509			Phys.Rev.B,52(1995)R7034	G.V.M. Wiliams,J.L. Tallon,R. Meinhold	Y, Ba, La, Cu, Zn, O	
11835	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.07	Hg	1	Ba	2	Cu	1															O		4.07	1	1995																												Hg1201																		K		45					45			K/GPa	1.9																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11836	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.12	Hg	1	Ba	2	Cu	1															O		4.12	1	1995																												Hg1201																		K		74					74			K/GPa	2.29																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11837	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.19	Hg	1	Ba	2	Cu	1															O		4.19	1	1995																												Hg1201																		K		95					95			K/GPa	1.94																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11838	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.22	Hg	1	Ba	2	Cu	1															O		4.22	1	1995																												Hg1201																		K		97					97			K/GPa	2.03																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11839	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.27	Hg	1	Ba	2	Cu	1															O		4.27	1	1995																												Hg1201																		K		91					91			K/GPa	1.45																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11840	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.3	Hg	1	Ba	2	Cu	1															O		4.3	1	1995																												Hg1201																		K		81					81			K/GPa	-0.101																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11841	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.31	Hg	1	Ba	2	Cu	1															O		4.31	1	1995																												Hg1201																		K		78					78			K/GPa	0.39																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11842	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.34	Hg	1	Ba	2	Cu	1															O		4.34	1	1995																												Hg1201																		K		59					59			K/GPa	1.06																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11843	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.36	Hg	1	Ba	2	Cu	1															O		4.36	1	1995																												Hg1201																		K		56					56			K/GPa	1.28																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11844	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.37	Hg	1	Ba	2	Cu	1															O		4.37	1	1995																												Hg1201																		K		40					40			K/GPa	0.994																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11845	PR05206854		HgBa2CuO4	Hg1Ba2Cu1O4.39	Hg	1	Ba	2	Cu	1															O		4.39	1	1995																												Hg1201																		K		26					26			K/GPa	0.612																																																																																												Controlled solid-vapor reaction.MIX(BaO,CuO)-SIN(930C,24h,Ar:O=4:1)-Precursor(Ba2CuOx)React(Ba2CuOx,Hg,in sealed quartz tube,810C,8h).About controlling oxygen contents d, see text.					Pressure effect on the  Tc of HgBa2CuO4+z with 0.07%$z%$0.39	199509			Phys.Rev.B,52(1995)6854	C.W. Chu,Q. Xiong,Y. Cao,Y.Y. Xue	Hg, Ba, Cu, O	
11846	PR05207006		(La,Ca)MnO3	La0.79Ca0.21Mn1O3	La	0.79	Ca	0.21	Mn	1															O	3		1	1995							203.3																																																																																																																																												La2O3,CaCO3,MnO2	1	SIN(1050C,20h)-reground-SIN(1300C,20h)-This step repeat 2 times.-SIN(1350C,air)					Substantial pressure effects on the electricai resistivity and ferromagnetic transition temperature	199509			Phys.Rev.B,52(1995)R7006	J.D. Thompson,J.J. Neumeier,M.F. Hundley,R.H. Heffner	La, Ca, Mn, O	
11847	PR05207006		(La,Ca)MnO3	La0.67Ca0.33Mn1O3	La	0.67	Ca	0.33	Mn	1															O	3		1	1995							267.2																																																																																																																																												La2O3,CaCO3,MnO2	1	SIN(1050C,20h)-reground-SIN(1300C,20h)-This step repeat 2 times.-SIN(1350C,air)					Substantial pressure effects on the electricai resistivity and ferromagnetic transition temperature	199509			Phys.Rev.B,52(1995)R7006	J.D. Thompson,J.J. Neumeier,M.F. Hundley,R.H. Heffner	La, Ca, Mn, O	
11848	PR05207006		(La,Ca)MnO3	La0.6Ca0.4Mn1O3	La	0.6	Ca	0.4	Mn	1															O	3		1	1995							271.3																																																																																																																																												La2O3,CaCO3,MnO2	1	SIN(1050C,20h)-reground-SIN(1300C,20h)-This step repeat 2 times.-SIN(1350C,air)					Substantial pressure effects on the electricai resistivity and ferromagnetic transition temperature	199509			Phys.Rev.B,52(1995)R7006	J.D. Thompson,J.J. Neumeier,M.F. Hundley,R.H. Heffner	La, Ca, Mn, O	
11900	PR05209736		Pb2Sr2TbCu3O8	Pb2Sr2Tb1Cu3O8	Pb	2	Sr	2	Tb	1	Cu	3													O	8		1	1995	emu/mol	0.0006			myu-B/mol	9.7	-21																					Pb3212																																																																																																																							PbO,Tb4O7,Y2O3,CuO,CaO,SrCO3	1	MIX-pelletizing-SIN(830C,20h)-COOL(R.T.)					Oxidation state and magnetic properties of Pb2Sr2Tb1-xYxCu3O8	199510		Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439-4831	Phys.Rev.B,52(1995)9736	L. Soderholm,Mark R. Antonio,S. Skanthakumar,U. Staub		
11901	PR05209736		Pb2Sr2(Tb,Y)Cu3O8	Pb2Sr2Tb0.1Y0.9Cu3O8	Pb	2	Sr	2	Tb	0.1	Y	0.9	Cu	3											O	8		1	1995	emu/mol	0.006			myu-B/mol	10.1	-1.9																					Pb3212																																																																																																																							PbO,Tb4O7,Y2O3,CuO,CaO,SrCO3	1	MIX-pelletizing-SIN(830C,20h)-COOL(R.T.)					Oxidation state and magnetic properties of Pb2Sr2Tb1-xYxCu3O8	199510		Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439-4831	Phys.Rev.B,52(1995)9736	L. Soderholm,Mark R. Antonio,S. Skanthakumar,U. Staub		
11902	PR05209736		Pb2Sr2(Tb,Y)Cu3O8	Pb2Sr2Tb0.05Y0.95Cu3O8	Pb	2	Sr	2	Tb	0.05	Y	0.95	Cu	3											O	8		1	1995	emu/mol	0.007			myu-B/mol	9.7	-1																					Pb3212																																																																																																																							PbO,Tb4O7,Y2O3,CuO,CaO,SrCO3	1	MIX-pelletizing-SIN(830C,20h)-COOL(R.T.)					Oxidation state and magnetic properties of Pb2Sr2Tb1-xYxCu3O8	199510		Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439-4831	Phys.Rev.B,52(1995)9736	L. Soderholm,Mark R. Antonio,S. Skanthakumar,U. Staub		
11903	PR05209736		Pb2Sr2(Tb,Y)Cu3O8	Pb2Sr2Tb0.02Y0.98Cu3O8	Pb	2	Sr	2	Tb	0.02	Y	0.98	Cu	3											O	8		1	1995	emu/mol	0.003			myu-B/mol	9.8	-0.9																					Pb3212																																																																																																																							PbO,Tb4O7,Y2O3,CuO,CaO,SrCO3	1	MIX-pelletizing-SIN(830C,20h)-COOL(R.T.)					Oxidation state and magnetic properties of Pb2Sr2Tb1-xYxCu3O8	199510		Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439-4831	Phys.Rev.B,52(1995)9736	L. Soderholm,Mark R. Antonio,S. Skanthakumar,U. Staub		
11904	PR05210569		YBa2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1995																												Y123																		K			93.5			0.25	93.5																				T	Calculated from the result of muon spin rotation measurement.The fitting function has the form, c(1	77														A	calculated from the result of muon spin rotation measurement.The fitting function has the form, c(1-		19			calculated from the result of muon spin rotation measurement.The fitting function has the form, c(1-		1500																																																			5	See Physica C 195, 51 (1992).					Ginzburg-Landau parameter in YBaCu3O6.95 below the irreversibility temperature as measured by %*+SR in high magnetic fields	199510		TRIUMF, Candian Institute for Advanced Reserch and Department of Physics, University of British Columbia, Vancouver, British Colombia, Canada V6T 1Z1	Phys.Rev.B,52(1995)10569	C. Niedermayer,J.H. Brewer,K.H. Chow,R. Liang,R.F. Kiefl,S.L. Lee,S.R. Kreitzman,T.M. Riseman,W.A. MacFarlane,W.N. Hardy		
11905	PR05210610		(Y,Ce)Sr2Cu2FeO8+d	Y1.5Ce0.5Sr2Cu2Fe1O8+d	Y	1.5	Ce	0.5	Sr	2	Cu	2	Fe	1											O	8+d		1	1995					micro.B/Mo	1.9	-7	25																					I4/mmm		A	3.819		28.075	3																																																																																																																Y2O3, CeO2, SrCO3, CuO, Fe2O3	1	CAL(at 1070C for 25h in air)SIN(at 1120C for 6days)QuenchANN (at 500C under flowing oxygen)FNC (under flowing oxygen)					"Structural, Mo""ssbauer and Raman studies of the (Y, Ce)2Sr2Cu2FeO8+y conpound"	199510			Phys.Rev.B,52(1995)10610	A. Simopoulos,D. Niarchos,E. Liarokapis,G. Kallias,M. Pissas,N. Poulakis	Y, Ce, Sr, Cu, Fe, O	
11906	PR05210610		(Y,Ce)2Sr2Cu2FeO8+d	Y1.5Ce0.5Sr2Cu2Fe1O8+d	Y	1.5	Ce	0.5	Sr	2	Cu	2	Fe	1											O	8+d		1	1995					micro.B/Mo	3.22	10	9																					I4/mmm		A	3.815		28.292	3																																																																																																																Y2O3, CeO2, SrCO3, CuO, Fe2O3	1	CAL (at 1070C for 24h in air)SIN (at 1120C for 6days)QuenchANN (at 500C under flowing oxygen)ANN (at 500C under flowing Ar for a day)FNC (under flowing Ar)					"Structural, Mo""ssbauer and Raman studies of the (Y, Ce)2Sr2Cu2FeO8+y conpound"	199510			Phys.Rev.B,52(1995)10610	A. Simopoulos,D. Niarchos,E. Liarokapis,G. Kallias,M. Pissas,N. Poulakis	Y, Ce, Sr, Cu, Fe, O	
11907	PR05210452		(Pb,Cu)2(Ba,Sr)2PrCu2O8	Pb1Cu3Ba1Sr1Pr1O8	Pb	1	Cu	3	Ba	1	Sr	1	Pr	1											O		8	1	1995					micro.B/Mo	8.06	-2.31	2.3																			2	Pb2212	I4/mmm		A	3.878		27.594	3																																																																							SP11907																		ohm.cm											746												BaCO3, SrCO3, R2O3(R=Pr,Gd,Y), CuO, PbO	1	BaCO3, SrCO3, R2O3 and CuO with the ratio Ba:Sr:R:Cu+1:1:1:3 were mixed.CAL(at 920CC in air with intermediate grinding)CAL (at 730C for  24h)SIN (at 825-830C in flowing Ar for 3days)Quench					Observation of Pr and Gd ordering in the 2212-type compounds (Pb0.5Cu0.5)2(Ba0.5Sr0.5)2RCu2O8(r=Pr, Gd)	199510			Phys.Rev.B,52(1995)10452	C.L. Yang,H.C. Ku,J.C. Ho,J.H. Shieh,Y.Y. Hsu	Pr, Gd, Pb, Cu, Ba, Sr, O	
11908	PR05210452		(Pb,Cu)2(Ba,Sr)2GdCu2O8	Pb1Cu3Ba1Sr1Gd1O8	Pb	1	Cu	3	Ba	1	Sr	1	Gd	1											O		8	1	1995																											2	Pb2212	I4/mmm		A	3.854		27.457	3																																																																							SP11908																																									BaCO3, SrCO3, R2O3(R=Pr,Gd,Y), CuO, PbO	1	BaCO3, SrCO3, R2O3 and CuO with the ratio Ba:Sr:R:Cu+1:1:1:3 were mixed.CAL(at 920CC in air with intermediate grinding)CAL (at 730C for  24h)SIN (at 825-830C in flowing Ar for 3days)Quench					Observation of Pr and Gd ordering in the 2212-type compounds (Pb0.5Cu0.5)2(Ba0.5Sr0.5)2RCu2O8(r=Pr, Gd)	199510			Phys.Rev.B,52(1995)10452	C.L. Yang,H.C. Ku,J.C. Ho,J.H. Shieh,Y.Y. Hsu	Pr, Gd, Pb, Cu, Ba, Sr, O	
11909	PR05210452		(Pb,Cu)2(Ba,Sr)2YCu2O8	Pb1Cu3Ba1Sr1Y1O8	Pb	1	Cu	3	Ba	1	Sr	1	Y	1											O		8	1	1995																											2	Pb1212	I4/mmm		A	3.83		27.45	3																																																																							SP11909																		ohm.cm											6.26												BaCO3, SrCO3, R2O3(R=Pr,Gd,Y), CuO, PbO	1	BaCO3, SrCO3, R2O3 and CuO with the ratio Ba:Sr:R:Cu+1:1:1:3 were mixed.CAL(at 920CC in air with intermediate grinding)CAL (at 730C for  24h)SIN (at 825-830C in flowing Ar for 3days)Quench					Observation of Pr and Gd ordering in the 2212-type compounds (Pb0.5Cu0.5)2(Ba0.5Sr0.5)2RCu2O8(r=Pr, Gd)	199510			Phys.Rev.B,52(1995)10452	C.L. Yang,H.C. Ku,J.C. Ho,J.H. Shieh,Y.Y. Hsu	Pr, Gd, Pb, Cu, Ba, Sr, O	
11910	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb1Ba1.7Sr0.3Cu3O6.9	Yb	1	Ba	1.7	Sr	0.3	Cu	3													O	7-d	6.9	1	1995																											3				A	3.794	3.87	11.6	3											K	81						81																																																																							m.ohm.cm											0.5													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11911	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.95Pr0.05Ba1.7Sr0.3Cu3O6.91	Yb	0.95	Pr	0.05	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.792	3.867	11.589												K	81						81																																																																							m.ohm.cm											0.66													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11912	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.9Pr0.1Ba1.7Sr0.3Cu3O6.9	Yb	0.9	Pr	0.1	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.9	1	1995																											3				A	3.794	3.863	11.593	3											K	81						81																																																																							m.ohm.cm											1.18													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11913	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.85Pr0.15Ba1.7Sr0.3Cu3O6.91	Yb	0.85	Pr	0.15	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.796	3.869	11.608	3											K	80						80																																																																							m.ohm.cm											1.51													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11914	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.8Pr0.2Ba1.7Sr0.3Cu3O6.92	Yb	0.8	Pr	0.2	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.92	1	1995																											3				A	3.797	3.869	11.617	3											K	76						76																																																																							m.ohm.cm											0.85													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11915	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.75Pr0.25Ba1.7Sr0.3Cu3O6.92	Yb	0.75	Pr	0.25	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.92	1	1995																											3				A	3.8	3.869	11.619	3											K	71						71																																																																							m.ohm.cm											0.95													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11916	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.7Pr0.3Ba1.7Sr0.3Cu3O6.93	Yb	0.7	Pr	0.3	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.803	3.869	11.628	3											K	63						63																																																																							m.ohm.cm				0.55							1.25													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11917	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.65Pr0.35Ba1.7Sr0.3Cu3O6.95	Yb	0.65	Pr	0.35	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.95	1	1995																											3				A	3.804	3.87	11.635	3											K	55						55																																																																							m.ohm.cm											1.3													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11918	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.6Pr0.4Ba1.7Sr0.3Cu3O6.93	Yb	0.6	Pr	0.4	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.815	3.874	11.652	3											K	46						46																																																																							m.ohm.cm				0.7							1.36													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11919	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.55Pr0.45Ba1.7Sr0.3Cu3O6.88	Yb	0.55	Pr	0.45	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.88	1	1995																											3				A	3.815	3.868	11.65	3											K	41						41																																																																							m.ohm.cm											1.6													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11920	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.5Pr0.5Ba1.7Sr0.3Cu3O6.93	Yb	0.5	Pr	0.5	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.815	3.873	11.655	3											K	30						30																																																																							m.ohm.cm				0.85							1.51													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11921	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.45Pr0.55Ba1.7Sr0.3Cu3O6.91	Yb	0.45	Pr	0.55	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.819	3.875	11.662	3											K	15						15																																																																							m.ohm.cm				1.1							1.49													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11922	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.4Pr0.6Ba1.7Sr0.3Cu3O6.87	Yb	0.4	Pr	0.6	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.87	1	1995																											3				A	3.826	3.873	11.674	3																																																																																									m.ohm.cm				2.15							2.31													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11923	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.3Pr0.7Ba1.7Sr0.3Cu3O6.91	Yb	0.3	Pr	0.7	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.83	3.882	11.67	3																																																																																									m.ohm.cm				4.5							3.51													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11924	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.2Pr0.8Ba1.7Sr0.3Cu3O6.92	Yb	0.2	Pr	0.8	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.92	1	1995																											3				A	3.837	3.881	11.716	3																																																																																									m.ohm.cm											4.41													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11925	PR05210504		(Yb,Pr)(Ba,Sr)2Cu3O7-d	Yb0.1Pr0.9Ba1.7Sr0.3Cu3O6.88	Yb	0.1	Pr	0.9	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.88	1	1995																											3				A	3.855	3.883	11.721	3																																																																																									m.ohm.cm											7.32													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11926	PR05210504		Pr(Ba,Sr)2Cu3O7	Pr1Ba1.7Sr0.3Cu3O6.87	Pr	1	Ba	1.7	Sr	0.3	Cu	3													O	7-d	6.87	1	1995																											3				A	3.861	3.89	11.722	3																																																																																									m.ohm.cm											13.6													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11927	PR05210504		Lu(Ba,Sr)2Cu3O7-d	Lu1Ba1.7Sr0.3Cu3O7-d	Lu	1	Ba	1.7	Sr	0.3	Cu	3													O	7-d		2	1995																											3				A	3.79	3.868	11.64	3											K	79						79																																																																							m.ohm.cm											1.02													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11928	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.9Pr0.1Ba1.7Sr0.3Cu3O6.95	Lu	0.9	Pr	0.1	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.95	1	1995																											3				A	3.794	3.869	11.609	3											K	79						79																																																																							m.ohm.cm											0.78													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11929	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.85Pr0.15Ba1.7Sr0.3Cu3O6.91	Lu	0.85	Pr	0.15	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.794	3.868	11.609	3											K	77						77																																																																							m.ohm.cm											0.88													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11930	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.8Pr0.2Ba1.7Sr0.3Cu3O6.93	Lu	0.8	Pr	0.2	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.795	3.87	11.611	3											K	75						75																																																																							m.ohm.cm											0.71													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11931	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.75Pr0.25Ba1.7Sr0.3Cu3O6.9	Lu	0.75	Pr	0.25	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.9	1	1995																											3				A	3.797	3.872	11.613	3											K	66						66																																																																							m.ohm.cm											0.82													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11932	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.7Pr0.3Ba1.7Sr0.3Cu3O6.89	Lu	0.7	Pr	0.3	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.89	1	1995																											3				A	3.799	3.871	11.618	3											K	61						61																																																																							m.ohm.cm											1.11													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11933	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.65Pr0.35Ba1.7Sr0.3Cu3O6.93	Lu	0.65	Pr	0.35	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.807	3.876	11.622	3											K	52						52																																																																							m.ohm.cm											1.25													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11934	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.6Pr0.4Ba1.7Sr0.3Cu3O6.91	Lu	0.6	Pr	0.4	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.812	3.877	11.625	3											K	47						47																																																																							m.ohm.cm											1.79													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11935	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.55Pr0.45Ba1.7Sr0.3Cu3O6.92	Lu	0.55	Pr	0.45	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.92	1	1995																											3				A	3.811	3.875	11.635	3											K	35						35																																																																							m.ohm.cm											1.49													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11936	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.5Pr0.5Ba1.7Sr0.3Cu3O6.92	Lu	0.5	Pr	0.5	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.92	1	1995																											3				A	3.813	3.874	11.643	3											K	20						20																																																																							m.ohm.cm											1.85													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11937	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.45Pr0.55Ba1.7Sr0.3Cu3O6.91	Lu	0.45	Pr	0.55	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.91	1	1995																											3				A	3.823	3.878	11.661	3																																																																																									m.ohm.cm											2.26													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11938	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.4Pr0.6Ba1.7Sr0.3Cu3O6.93	Lu	0.4	Pr	0.6	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.93	1	1995																											3				A	3.825	3.878	11.664	3																																																																																									m.ohm.cm											2.94													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11939	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.3Pr0.7Ba1.7Sr0.3Cu3O6.9	Lu	0.3	Pr	0.7	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.9	1	1995																											3				A	3.833	3.875	11.674	3																																																																																									m.ohm.cm											4.3													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11940	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.2Pr0.8Ba1.7Sr0.3Cu3O6.88	Lu	0.2	Pr	0.8	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.88	1	1995																											3				A	3.846	3.883	11.693	3																																																																																									m.ohm.cm											6.4													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11941	PR05210504		(Lu,Pr)(Ba,Sr)2Cu3O7-d	Lu0.1Pr0.9Ba1.7Sr0.3Cu3O6.89	Lu	0.1	Pr	0.9	Ba	1.7	Sr	0.3	Cu	3											O	7-d	6.89	1	1995																											3				A	3.856	3.887	11.705	3																																																																																									m.ohm.cm											13.6													1	CAL (at 900C for 24h)CAL (at 910-920C for 48h with intermittent grindings)SIN (at 930C for 24h)ANN (at 900C for 24h and at 600C for 48h in flowing oxygen)FNC					Suppression of superconductivity in the L-1-xPrxBa1.7Sr0.3Cu3O7(L=Yb and Lu) sistem: Obsrvation of the hole localization effect	199510			Phys.Rev.B,52(1995)10504	U.V. Varadaraju,V. Badri	Yb, Lu< Pr, Ba, Sr, Cu, O	
11942	PR05210474		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7	1	1995									4.746																		3				A	3.81	3.88	11.65	3											K		86				2	86																																																																							m.ohm.cm											0.79												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11943	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7	Y	1	Ba	2	Cu	2.94	Zn	0.06													O		7	1	1995									5.358																		3				A	3.81	3.88	11.64	3											K		64.9				3	64.9																																																																							m.ohm.cm				0.63							1.39												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11944	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7	Y	1	Ba	2	Cu	2.91	Zn	0.09													O		7	1	1995			emu.K/G.g	32			35.8		5.101																		3	Y123			A	3.82	3.88	11.65	3											K		56.9				3.4	56.9																																																																							m.ohm.cm				1.13							2.16												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11945	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7	Y	1	Ba	2	Cu	2.85	Zn	0.15													O		7	1	1995			emu.K/G.g	83			23.9		5.044																		3	Y123			A	3.81	3.88	11.64	3											K		43.2				3.8	43.2																																																																							m.ohm.cm				1.4							2.52												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11946	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.76Zn0.24O7	Y	1	Ba	2	Cu	2.76	Zn	0.24													O		7	1	1995			emu.K/G.g	140			6.6		5.266																		3	Y123			A	3.81	3.88	11.64	3											K		13				5.2	13																																																																							m.ohm.cm				4.74							6.48												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11947	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.7Zn0.3O7	Y	1	Ba	2	Cu	2.7	Zn	0.3													O		7	1	1995			emu.K/G.g	206			-1.7		5.68																		3	Y123			A	3.82	3.89	11.66	3																																																																																																																Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11948	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.979Zn0.021O7	Y	1	Ba	2	Cu	2.979	Zn	0.021													O		7	1	1995									4.971																		3	Y123			A	3.81	3.88	11.65	3											K		80.2				3.8	80.2																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11949	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		7	1	1995									5.407																		3	Y123			A	3.81	3.88	11.65	3											K		77				3	77																																																																							m.ohm.cm											1.1												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11950	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O7	Y	1	Ba	2	Cu	2.88	Zn	0.12													O		7	1	1995									5.69																		3	Y123			A	3.81	3.88	11.64	3											K		52				3.2	52																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 900C for 16h in air)SIN (at 950C for 24h in air)FNCANN (at 450C for 12h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11951	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7	1	1995			emu.K/G.g						4.608																		3	Y123			A	3.82	3.88	11.66	3											K		88				0.9	88																																																																							m.ohm.cm											1.44												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 920C for 15h in air)CAL (at 900C for 10h in air)SIN (at 950C for 20h in air)FNCANN (at 350C for 10h).					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11952	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.993Zn0.007O7	Y	1	Ba	2	Cu	2.993	Zn	0.007													O		7	1	1995			emu.K/G.g	1					4.513																		3	Y123			A	3.81	3.88	11.65	3											K		84				3.4	84																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 920C for 15h in air)CAL (at 900C for 10h in air)SIN (at 950C for 20h in air)FNCANN (at 350C for 10h).					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11953	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.985Zn0.015O7	Y	1	Ba	2	Cu	2.985	Zn	0.015													O		7	1	1995			emu.K/G.g	3					4.758																		3	Y123			A	3.822	3.89	11.66	3											K		80				1.9	80																																																																							m.ohm.cm											1.55												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 920C for 15h in air)CAL (at 900C for 10h in air)SIN (at 950C for 20h in air)FNCANN (at 350C for 10h).					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11954	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O		7	1	1995			emu.K/G.g	18			61		4.277																		3	Y123			A	3.81	3.88	11.65	3											K		76				2.2	76																																																																							m.ohm.cm											1.66												Y2O3, BaCO3, CuO, ZnO	1	CAL (at 920C for 15h in air)CAL (at 900C for 10h in air)SIN (at 950C for 20h in air)FNCANN (at 350C for 10h).					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11955	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.955Zn0.045O7	Y	1	Ba	2	Cu	2.955	Zn	0.045													O		7	1	1995			emu.K/G.g	52			42		4.457																		3	Y123			A	3.81	3.88	11.65	3											K		70.1				2.1	70.1																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 920C for 15h in air)CAL (at 900C for 10h in air)SIN (at 950C for 20h in air)FNCANN (at 350C for 10h).					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11956	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.82Zn0.18O7	Y	1	Ba	2	Cu	2.82	Zn	0.18													O		7	1	1995			emu.K/G.g	188			22		5.086																		3	Y123			A	3.81	3.89	11.64	3											K		38.4				5.7	38.4																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 910C for 12h in air) 2timesSIN (at 950C for 20h in air)FNCANN (at 400C for 20h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
11957	PR05210474		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.79Zn0.21O7	Y	1	Ba	2	Cu	2.79	Zn	0.21													O		7	1	1995			emu.K/G.g	223			12.8		4.821																		3	Y123			A	3.82	3.89	11.64	3											K		24.2				6.5	24.2																																																																																														Y2O3, BaCO3, CuO, ZnO	1	CAL (at 910C for 12h in air) 2timesSIN (at 950C for 20h in air)FNCANN (at 400C for 20h)					Magnetic and transport properties of Zn-doped YBa2Cu3O7 in the normal state	199510			Phys.Rev.B,52(1995)10474	J. Je'goudez,P. Monod,S. Zagoulaev	Y, Ba, Ca, O, Zn	
12000	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.38	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.38	1	1995																											2	Y123				3.904		11.822																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12001	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.42	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.42	1	1995																											2	Y123				3.905		11.816																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12002	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.5	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.5	1	1995																											2	Y123				3.907		11.813																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12003	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.63	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.63	1	1995																											2	Y123				3.911		11.792																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12004	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.71	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.71	1	1995																											2	Y123				3.911		11.78																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12005	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.8	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.8	1	1995																											2	Y123				3.912		11.768																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12006	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.89	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.89	1	1995																											2	Y123				3.908		11.76																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12007	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O6.98	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		6.98	1	1995																											2	Y123				3.905		11.737													8						8																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12008	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.1Ba1.65La1.25Cu3O7.06	Ca	0.1	Ba	1.65	La	1.25	Cu	3													O		7.06	1	1995																											2	Y123				3.903		11.72													41.9						41.9																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12009	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.43	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.43	1	1995																											2	Y123				3.887		11.762																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12010	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.5	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.5	1	1995																											2	Y123				3.884		11.76																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12011	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.61	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.61	1	1995																											2	Y123				3.883		11.744																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12012	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.69	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.69	1	1995																											2	Y123				3.88		11.723																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12013	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.78	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.78	1	1995																											2	Y123				3.878		11.718																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12014	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.87	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.87	1	1995																											2	Y123				3.878		11.709																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12015	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O6.98	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		6.98	1	1995																											2	Y123				3.876		11.679													40.1						40.1																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12016	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O7.05	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		7.05	1	1995																											2	Y123				3.875		11.669													60						60																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12017	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.35La1.25Cu3O7.14	Ca	0.4	Ba	1.35	La	1.25	Cu	3													O		7.14	1	1995																											2	Y123				3.873		11.637													78.8						78.8																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12018	PR05212982		(Ca,La)(Ba,Nd)2Cu3O7	Ca0.1Ba1.65Nd1.25Cu3O6.67	Ca	0.1	Ba	1.65	Nd	1.25	Cu	3													O		6.67	1	1995																											2	Y123				3.887		11.687																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12019	PR05212982		(Ca,La)(Ba,Nd)2Cu3O7	Ca0.1Ba1.65Nd1.25Cu3O6.84	Ca	0.1	Ba	1.65	Nd	1.25	Cu	3													O		6.84	1	1995																											2	Y123				3.885		11.663																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12020	PR05212982		(Ca,La)(Ba,Nd)2Cu3O7	Ca0.1Ba1.65Nd1.25Cu3O6.96	Ca	0.1	Ba	1.65	Nd	1.25	Cu	3													O		6.96	1	1995																											2	Y123				3.882	11.655																																																																																																																		La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12021	PR05212982		(Ca,La)(Ba,Nd)2Cu3O7	Ca0.1Ba1.65Nd1.25Cu3O7.03	Ca	0.1	Ba	1.65	Nd	1.25	Cu	3													O		7.03	1	1995																											2	Y123				3.882		11.652																																																																																																																	La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12022	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.15La1.45Cu3O7.02	Ca	0.4	Ba	1.15	La	1.45	Cu	3													O		7.02	1	1995																											2	Y123				3.874		11.637																	4.2																																																																																																La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12023	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.15La1.45Cu3O7.08	Ca	0.4	Ba	1.15	La	1.45	Cu	3													O		7.08	1	1995																											2	Y123				3.873		11.631																	4.2																																																																																																La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12024	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.15La1.45Cu3O7.12	Ca	0.4	Ba	1.15	La	1.45	Cu	3													O		7.12	1	1995																											2	Y123				3.874		11.629													7.6						7.6																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12025	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.15La1.45Cu3O7.21	Ca	0.4	Ba	1.15	La	1.45	Cu	3													O		7.21	1	1995																											2	Y123				3.871		11.617													43.9						43.9																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12026	PR05212982		(Ca,La)(Ba,La)2Cu3O7	Ca0.4Ba1.15La1.45Cu3O7.23	Ca	0.4	Ba	1.15	La	1.45	Cu	3													O		7.23	1	1995																											2	Y123				3.873															52.8						52.8																																																																																														La2O3,Nd2O3,CuO,BaCO3,CaCO3	1	MIX-SIN(16-20h,air,930-950C for La,Nd and Q=7.25, 950-980C for La and Q=7.35,7.45)-This step is repeated 3-4 times.-and more processes.In details, see text.					Relationship between superconductor and metal-insulator transitions in a large class of tetragonal 1:2:3 cuprates Ca-R-Ba-Cu-O (R=La, Nd)	011		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000,Israel	Phys.Rev.B,52(1995)12982	A. Knizhnik,D. Goldschmidt,G. M. Reisner,Y. Direktovitch,Y. Eckstein	Ca, La, Nd, Ba, Cu, O	
12027	PR05213006		PrBa2(Cu,Zn)3O7	Pr1Ba2Cu2.925Zn0.075O7-d	Pr	1	Ba	2	Cu	2.925	Zn	0.075													O	7-d		1	1995					Bohr magne	2.95		16																				Y123																																																																																																																							Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12028	PR05213006		PrBa2(Cu,Zn)3O7	Pr1Ba2Cu2.85Zn0.15O7-d	Pr	1	Ba	2	Cu	2.85	Zn	0.15													O	7-d		1	1995					Bohr magne	2.77		17																				Y123																																																																																																																							Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12029	PR05213006		PrBa2(Cu,Zn)3O7	Pr1Ba2Cu2.7Zn0.3O7-d	Pr	1	Ba	2	Cu	2.7	Zn	0.3													O	7-d		1	1995					Bohr magne	2.98		16																				Y123			A	3.882	3.917	11.702	4																																																																																																																Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12030	PR05213006		PrBa2Cu3O7	Pr1Ba2Cu3O7-d	Pr	1	Ba	2	Cu	3															O	7-d		1	1995					Bohr magne	2.85		17																				Y123	Pmmm		A	3.86	3.925	11.707	4																																																																																																																Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12031	PR05213006		PrBa2(Cu,Ga)3O7	Pr1Ba2Cu2.925Ga0.075O7-d	Pr	1	Ba	2	Cu	2.925	Ga	0.075													O	7-d		1	1995					Bohr magne	3.03		16																				Y123																																																																																																																							Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12032	PR05213006		PrBa2(Cu,Ga)3O7	Pr1Ba2Cu2.85Ga0.15O7-d	Pr	1	Ba	2	Cu	2.85	Ga	0.15													O	7-d		1	1995					Bohr magne	2.77		15																				Y123																																																																																																																							Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12033	PR05213006		PrBa2(Cu,Ga)3O7	Pr1Ba2Cu2.7Ga0.3O7-d	Pr	1	Ba	2	Cu	2.7	Ga	0.3													O	7-d		1	1995					Bohr magne	2.77		14																			2	Y123	P4/mmm		A	3.901		11.671	4																																																																																																																Pr6O11,BaCO3,CuO,ZnO,Ga2O3	1	MIX-SIN(930C, 24h)-this process was repeated at least 3 times.					Structural, magnetic, ahd heat-capacity studies on Zn- and Ga-substituted PrBa2Cu3O7-z	011		Tata Institute of Fundamental Research, Bombay 400005, India	Phys.Rev.B,52(1995)13006	H. Jhans,J. J. Rhyne,N. C. Soni,Ram Prasad,S. K. Dhar,S. K. Malik,V. P. S. Awana,W. B. Yelon	Pr, Ba, Cu, O, Zn, Ga	
12034	PR05213563		LaNiO3	La1Ni1O3	La	1	Ni	1																	O	3		1	1995																													Rbar3c		A	5.457	5.457	13.146	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12035	PR05213563		(La,Sr)NiO3	La0.9Sr0.1Ni1O3	La	0.9	Sr	0.1	Ni	1															O	3		1	1995																													Rbar3c		A	5.446	5.446	13.16	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12036	PR05213563		(La,Th)NiO3	La0.9Th0.1Ni1O3	La	0.9	Th	0.1	Ni	1															O	3		1	1995																													Rbar3c		A	5.456	5.456	13.155	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12037	PR05213563		NdNiO3	Nd1Ni1O3	Nd	1	Ni	1																	O	3		1	1995																													Pbnm		A	5.339	5.377	7.608	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12038	PR05213563		(Nd,Sr)NiO3	Nd0.99Sr0.01Ni1O3	Nd	0.99	Sr	0.01	Ni	1															O	3		1	1995																													Pbnm		A	5.393	5.375	7.607	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12039	PR05213563		(Nd,Sr)NiO3	Nd0.98Sr0.02Ni1O3	Nd	0.98	Sr	0.02	Ni	1															O	3		1	1995																													Pbnm		A	5.39	5.374	7.607	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12040	PR05213563		(Nd,Sr)NiO3	Nd0.97Sr0.03Ni1O3	Nd	0.97	Sr	0.03	Ni	1															O	3		1	1995																													Pbnm		A	5.397	5.366	7.601	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12041	PR05213563		(Nd,Sr)NiO3	Nd0.95Sr0.05Ni1O3	Nd	0.95	Sr	0.05	Ni	1															O	3		1	1995																													Pbnm		A	5.395	5.367	7.612	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12042	PR05213563		(Nd,Sr)NiO3	Nd0.9Sr0.1Ni1O3	Nd	0.9	Sr	0.1	Ni	1															O	3		1	1995																													Pbnm		A	5.401	5.364	7.617	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12043	PR05213563		(Nd,Ca)NiO3	Nd0.99Ca0.01Ni1O3	Nd	0.99	Ca	0.01	Ni	1															O	3		1	1995																													Pbnm		A	5.39	5.376	7.606	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12044	PR05213563		(Nd,Ca)NiO3	Nd0.98Ca0.02Ni1O3	Nd	0.98	Ca	0.02	Ni	1															O	3		1	1995																													Pbnm		A	5.39	5.373	7.604	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12045	PR05213563		(Nd,Ca)NiO3	Nd0.97Ca0.03Ni1O3	Nd	0.97	Ca	0.03	Ni	1															O	3		1	1995																													Pbnm		A	5.39	5.37	7.602	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12046	PR05213563		(Nd,Ca)NiO3	Nd0.95Ca0.05Ni1O3	Nd	0.95	Ca	0.05	Ni	1															O	3		1	1995																													Pbnm		A	5.393	5.37	7.605	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12047	PR05213563		(Nd,Ca)NiO3	Nd0.9Ca0.1Ni1O3	Nd	0.9	Ca	0.1	Ni	1															O	3		1	1995																													Pbnm		A	5.397	5.369	7.61	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12048	PR05213563		(Nd,Th)NiO3	Nd0.97Th0.03Ni1O3	Nd	0.97	Th	0.03	Ni	1															O	3		1	1995																													Pbnm		A	5.388	5.389	7.611	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12049	PR05213563		(Nd,Th)NiO3	Nd0.95Th0.05Ni1O3	Nd	0.95	Th	0.05	Ni	1															O	3		1	1995																													Pbnm		A	5.391	5.389	7.617	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12050	PR05213563		(Nd,Th)NiO3	Nd0.92Th0.08Ni1O3	Nd	0.92	Th	0.08	Ni	1															O	3		1	1995																													Pbnm		A	5.393	5.393	7.62	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12051	PR05213563		(Nd,Th)NiO3	Nd0.9Th0.1Ni1O3	Nd	0.9	Th	0.1	Ni	1															O	3		1	1995																													Pbnm		A	5.392	5.395	7.62	3																																																																																																																R2O3,Ni(NO3)2-6H2O,Ca(NO3)2,etc		liquid mix technique. Raw mat. were solved in acid.Decompose(600C)-SIN(800C,air,several hours)-SIN(1000C,200bar,O2,12h)-COOL(R.T.)					Influence of carrier injection on the metal-insulator transion in electron- and hole-doped R1-xAxNiO3 perovskites	011		Institute de Ciencia de Barcelona, Consejo Superior de Investigaciones Cienti'ficas, E-08193 Bellaterra, Spain	Phys.Rev.B,52(1995)13563	J. A. Alonso,J. L. Garci'a-Mun~oz,M. J. Mart'inez-Lope,M. Suaaidi	Sr, Ca, Th, Ce, Ni, O, R	
12052	PR05213134		YBa2Cu3O7	Y1Ba2Cu3O6.05	Y	1	Ba	2	Cu	3															O		6.05	3	1995																																																																																																																						THC12052						ohm.cm																								5	See Physica C 201,233 (1992)					Anomalous phonon damping and thermal coductivity in insulating cuprates	011		Physics Department, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,52(1995)R13134	C. K. Lowe-Ma,J. L. Cohn,T. A. Vanderah	Y, Ba, Cu, O, Pr	
12053	PR05213134		YBa2Cu3O7	Y1Ba2Cu3O6.07	Y	1	Ba	2	Cu	3															O		6.07	3	1995																																																																																																																												ohm.cm												4.5												5	See Physica C 201,233 (1992)					Anomalous phonon damping and thermal coductivity in insulating cuprates	011		Physics Department, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,52(1995)R13134	C. K. Lowe-Ma,J. L. Cohn,T. A. Vanderah	Y, Ba, Cu, O, Pr	
12054	PR05213134		YBa2Cu3O7	Y1Ba2Cu3O6.08	Y	1	Ba	2	Cu	3															O		6.08	3	1995																																																																																																																						THC12054						ohm.cm												0.3												5	See Physica C 201,233 (1992)					Anomalous phonon damping and thermal coductivity in insulating cuprates	011		Physics Department, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,52(1995)R13134	C. K. Lowe-Ma,J. L. Cohn,T. A. Vanderah	Y, Ba, Cu, O, Pr	
12055	PR05213134		YBa2Cu3O7	Y1Ba2Cu3O6.11	Y	1	Ba	2	Cu	3															O		6.11	3	1995																																																																																																																						THC12055						ohm.cm												0.03												5	See Physica C 201,233 (1992)					Anomalous phonon damping and thermal coductivity in insulating cuprates	011		Physics Department, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,52(1995)R13134	C. K. Lowe-Ma,J. L. Cohn,T. A. Vanderah	Y, Ba, Cu, O, Pr	
12056	PR05213134		YBa2Cu3O7	Pr1Ba2Cu3O6.05	Pr	1	Ba	2	Cu	3															O		6.05	3	1995																																																																																																																																																				5	See Physica C 201,233 (1992)					Anomalous phonon damping and thermal coductivity in insulating cuprates	011		Physics Department, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,52(1995)R13134	C. K. Lowe-Ma,J. L. Cohn,T. A. Vanderah	Y, Ba, Cu, O, Pr	
12057	PR05212883		(Tl,Pb)Sr2(Ca,Y)Cu2O7	Tl0.5Pb0.5Sr2Ca0.7Y0.3Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	0.7	Y	0.3	Cu	2									O	7		1	1995																												Tl1212	P4/mmm		A	3.81		12.066	3																																																																																																																CaCO3,Y2O3,SrCO3,CuO,Tl2O3,PbO	1	Precursor(fired,CaCO3 Y2O3 SrCO3 CuO,970C,12h,air)-MIX(Tl2O3 PbO precursor)-pelletizing-Wrap(gold foils)-SIN(950C,3h,flow O2)					Electron-spin-resonance studies of the hole-doping effect on (TL0.5Pb0.5) Sr2(Ca1-xYx)Cu2O7 high-T superconductors	011		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,52(1995)12883	Jun Tzeng Lue,Li Yeat Chen	Tl, Pb, Sr, Ca, Y, Cu, O	
12060	L094037007	Tc from In-NQR. Tc(max)=0.8 K at P=2.1 GPa. energy gap is independent pf P. dTc/dP estimated from Tc(P) figure.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2005																												HoCoGa5																	HoCoGa5	K		0.4					0.4			K/GPa	0.19																																												2.5	6																																															self flux method					Enhancing the Superconducting Transition Temperature of the Heavy Fermion Compound CeIrIn5 in the Absence of Spin Correlations			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	Phys.Rev.Lett., 94(2005)037007	Guo-qing Zheng,H.Shishido,Hiroki Kan,S.Kawasaki,Y.Kitaoka,Y.Onuki		
12061	L094047001		CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2005																												HoCoGa5																	HoCoGa5	K		2.3					2.3																				T	NQR			4.9										MMHC12061																																																														using In-flux.					Superconductivity in CeCoIn5-xSnx: Veil over an Ordered State or Novel Quantum Critical Point?			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 94(2005)047001	C.Capan,E.D.Bauer,F.Ronning,J.D.Thompson,J.L.Sarrao,R.Movshovich		
12062	L094047001		CeCo(In,Sn)5	Ce1Co1In4.97Sn0.03	Ce	1	Co	1	In	4.97	Sn	0.03																3	2005																												HoCoGa5																	HoCoGa5	K		1.86					1.86																				T	NQR	4.8																																																																										using In-flux.					Superconductivity in CeCoIn5-xSnx: Veil over an Ordered State or Novel Quantum Critical Point?			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 94(2005)047001	C.Capan,E.D.Bauer,F.Ronning,J.D.Thompson,J.L.Sarrao,R.Movshovich		
12063	L094047001		CeCo(In,Sn)5	Ce1Co1In4.94Sn0.06	Ce	1	Co	1	In	4.94	Sn	0.06																3	2005																												HoCoGa5																	HoCoGa5	K		1.57					1.57																				T	NQR	3.8																																																																										using In-flux.					Superconductivity in CeCoIn5-xSnx: Veil over an Ordered State or Novel Quantum Critical Point?			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 94(2005)047001	C.Capan,E.D.Bauer,F.Ronning,J.D.Thompson,J.L.Sarrao,R.Movshovich		
12064	L094047001		CeCo(In,Sn)5	Ce1Co1In4.88Sn0.12	Ce	1	Co	1	In	4.88	Sn	0.12																3	2005																												HoCoGa5																	HoCoGa5	K		0.93					0.93																				T	NQR	2.54																																																																										using In-flux.					Superconductivity in CeCoIn5-xSnx: Veil over an Ordered State or Novel Quantum Critical Point?			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 94(2005)047001	C.Capan,E.D.Bauer,F.Ronning,J.D.Thompson,J.L.Sarrao,R.Movshovich		
12065	L093156802	Anisotropic energy gap (2*gap/kTc) = 2.78 for I//c.  = 0.64  for I//a.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2004																												LuNi2B2C																	YNi2B2C	K				14.6			14.6																																																2.78	1																																															TSFZ method using image furnace.					Evidence of Gap Anisotropy in Superconducting YNi2B2C Using Directional Point-Contact Spectroscopy			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Phys.Rev.Lett., 93(2004)1568002	D. Jaiswal-Nagar,Goutam Sheet,H. Takeya,P. Raychaudhuri,S. Ramakrishnan		
12066	L093157004	hydrostatic pressure. PENET and GAPENE are almost pressure independent.	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6			2004																												pyrochlore																		K		6.3					6.3			K/GPa	0.9																																					A	susceptibility, muon-SR	2300					3.72	13																																																				Pressure Effects on the Transition Temperature and the Magnetic Field Penetration Depth in the Pyrochlore Superconductor RbOs2O6			Laboratory for Neutron Scattering, Eidgenossische Technische Hochschule, Zurich, Switzerland, and Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 93(2004)157004	A.Maisuradze,A.Shengelaya,C.Baines,D.Di.Castro,D.G.Eshchenko,D.Gavillet,F.La Mattina,H.Keller,J.Karpinski,N.D.Zhigadlo,R.Brutsch,R.Khasanov,S.M.Kazakov		
12067	L093247007	Co-valence determined using redox titration. The amount of H2O not given. Tc vs Co-valence were measured.	Nax(H3O)zCO2:yH2O	Na0.35Co1H2.6O3.3	Na	0.35	Co	1	H	2.6															O	3.3		1	2004																																														K				4.8			4.8																																																																																														Na2CO3,Co3O4,Na		Na-deintercalated materials were in H2O or D2O container					Revised Superconducting Phase Diagram of Hole-Doped Nax(H3O)zCoO2:yH2O			Hahn-Meitner-Institut, Glienicker Strasse 100, Berlin D-14109, Germany	Phys.Rev.Lett., 93(2004)247007	A.Chemseddine,C.J.Milne,D.Alber,D.N.Argyriou,J.Veira,N.Aliouane,S.Landsgesell		
12068	L094047006	pseudogap measured by NMR	Bi2Sr2CuO6.36	Bi2Sr2Cu1O6.36	Bi	2	Sr	2	Cu	1															O	6+z	6.36	3	2005																												Bi2201																		K				8			8																																																																																														Bi2O3,SrCO3,La2O3,CuO		TSFZ method					Critical Point and the Nature of the Pseudogap of Single-Layered Copper-Oxide Bi2Sr2-xLaxCuO6+z Superconductors			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 94(2005)047006	A.P.Reyes,B.Liang,C.T.Lin,Guo-qing Zheng,P. L. Kuhns		
12069	L094047006	pseudogap measured by NMR	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6		3	2005																												Bi2201																		K				32			32	MMTC12069																																																																																													Bi2O3,SrCO3,La2O3,CuO		TSFZ method					Critical Point and the Nature of the Pseudogap of Single-Layered Copper-Oxide Bi2Sr2-xLaxCuO6+z Superconductors			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 94(2005)047006	A.P.Reyes,B.Liang,C.T.Lin,Guo-qing Zheng,P. L. Kuhns		
12070	L094097002	structure = dhcp 	Am(I)	Am1	Am	1																							2005																												element																		K		0.62					0.62																																																																																																					Superconductivity in the Americium Metal as a Function of Pressure: Probing the Mott Transition			European Commission, Joint Research Centre, Institute for Transuranium, Elements Postfach 2340, 76125 Karlsruhe, Germany	Phys.Rev.Lett., 94(2005)097002	G.H.Lander,G.Kotliar,J.-C. Griveau,J.Rebizant		
12071	L094097002	structure=fcc. Tc(P) estimated from Fig.2 using V(P) in Phys.Rev.Lett., 85(2000)2961.	Am(II)	Am1	Am	1																							2005																												element																		K		2.2					2.2	MMTC12071																																	MMHC12071																																																																			Superconductivity in the Americium Metal as a Function of Pressure: Probing the Mott Transition			European Commission, Joint Research Centre, Institute for Transuranium, Elements Postfach 2340, 76125 Karlsruhe, Germany	Phys.Rev.Lett., 94(2005)097002	G.H.Lander,G.Kotliar,J.-C. Griveau,J.Rebizant		
12072	L094097002	structure=Pnma. 	Am(IV)	Am1	Am	1																							2005																												element																		K		1.5					1.5			K/GPa	-0.15																																																																																																	Superconductivity in the Americium Metal as a Function of Pressure: Probing the Mott Transition			European Commission, Joint Research Centre, Institute for Transuranium, Elements Postfach 2340, 76125 Karlsruhe, Germany	Phys.Rev.Lett., 94(2005)097002	G.H.Lander,G.Kotliar,J.-C. Griveau,J.Rebizant		
12073	SST0180041	epitaxial film, d=800 A. Figure shows substrate temperature dependence of Tc.	(Pr,Ca)Ba2Cu3O7	Pr0.5Ca0.5Ba2Cu3O7-z	Pr	0.5	Ca	0.5	Ba	2	Cu	3													O	7-z		5	2005																												Y123																		K			37			6	37	TC12073																			T	WHH theory, resistivity		47.1						T/K	resistivity		1.73																																																																Epitaxial films were grown on SrTiO3 using pulsed-laser ablation.					Growth and superconducting transition of Pr1-xCaxBa2Cu3O7-z (X=0.5) epitaxial thin films			National Laboratory for Superconductivity, Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, China	Supercond.Sci.Technol., 18(2005)41	D.N.Zheng,H.H.Wen,H.P.Yang,J.Li,J.Y.Xiang,P.Wang,R.L.Wang,Y.Z.Zhang,Z.X.Zhao,Z.Y.Liu		
12074	SST0180277	XRD, IR, resistivity, SUS were measured.	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4	4	1	2005																												T																		K		37					37																																																																																																conventional solid state reaction					Superconductivity, magnetic susceptibility and electrical resistivity of the double-doped La1.85-xSr0.15+xCu1-xCoxO4 (0=<x=<0.4)			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui, China	Supercond.Sci.Technol., 18(2005)277	Huan Wu,Letian Ding,Ling Lin,Weixian Wang,Yudong Sun,Yuheng Zhang		
12075	SST0180277	XRD, IR, resistivity, SUS were measured.	(La,Sr)2(Cu,Co)O4	La1.84Sr0.16Cu0.99Co0.01O4	La	1.84	Sr	0.16	Cu	0.99	Co	0.01													O	4	4	1	2005																												T																		K		29					29																																																																																																conventional solid state reaction					Superconductivity, magnetic susceptibility and electrical resistivity of the double-doped La1.85-xSr0.15+xCu1-xCoxO4 (0=<x=<0.4)			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui, China	Supercond.Sci.Technol., 18(2005)277	Huan Wu,Letian Ding,Ling Lin,Weixian Wang,Yudong Sun,Yuheng Zhang		
12076	SST0180277	XRD, IR, resistivity, SUS were measured.	(La,Sr)2(Cu,Co)O4	La1.83Sr0.17Cu0.98Co0.02O4	La	1.83	Sr	0.17	Cu	0.98	Co	0.02													O	4	4	1	2005																												T																		K		16					16																																																																																																conventional solid state reaction					Superconductivity, magnetic susceptibility and electrical resistivity of the double-doped La1.85-xSr0.15+xCu1-xCoxO4 (0=<x=<0.4)			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui, China	Supercond.Sci.Technol., 18(2005)277	Huan Wu,Letian Ding,Ling Lin,Weixian Wang,Yudong Sun,Yuheng Zhang		
12077	SST0180277	XRD, IR, resistivity, SUS were measured.	(La,Sr)2(Cu,Co)O4	La1.82Sr0.18Cu0.97Co0.03O4	La	1.82	Sr	0.18	Cu	0.97	Co	0.03													O	4	4	1	2005																												T																		K		3					3																																																																																																conventional solid state reaction					Superconductivity, magnetic susceptibility and electrical resistivity of the double-doped La1.85-xSr0.15+xCu1-xCoxO4 (0=<x=<0.4)			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui, China	Supercond.Sci.Technol., 18(2005)277	Huan Wu,Letian Ding,Ling Lin,Weixian Wang,Yudong Sun,Yuheng Zhang		
12078	SST0180277	XRD, IR, resistivity, SUS were measured. single phase for x=<0.4 in La1.85-xSr0.15+xCu1-xCoxO4.	(La,Sr)2(Cu,Co)O4	La1.8Sr0.2Cu0.95Co0.05O4	La	1.8	Sr	0.2	Cu	0.95	Co	0.05													O	4	4	1	2005																												T																		K					2																																																																																																		conventional solid state reaction					Superconductivity, magnetic susceptibility and electrical resistivity of the double-doped La1.85-xSr0.15+xCu1-xCoxO4 (0=<x=<0.4)			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui, China	Supercond.Sci.Technol., 18(2005)277	Huan Wu,Letian Ding,Ling Lin,Weixian Wang,Yudong Sun,Yuheng Zhang		
12079	P071100502	ANN(970C, 24h, in pure Ar)	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O4-z	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z		3	2005								0																				T'																		K				24			24																																																																																																TSFZ method. sample with different Tc were obtained by annealing in Ar.					Electronic inhomogeneity and competing phases in electron-doped superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 71(2005)100502	H.A.Mook,H.J.Kang,J.W.Lynn,Komiya,M.Matsuura,Pengcheng Dai,Seiki,Y.Kurita,Yoichi Ando		
12080	P071100502	ANN(940C, 24h, in pure Ar)	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O4-z	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z		3	2005								40																				T'																		K				21			21	TC12080																																																																																															TSFZ method. sample with different Tc were obtained by annealing in Ar.					Electronic inhomogeneity and competing phases in electron-doped superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 71(2005)100502	H.A.Mook,H.J.Kang,J.W.Lynn,Komiya,M.Matsuura,Pengcheng Dai,Seiki,Y.Kurita,Yoichi Ando		
12081	P071100502	ANN(915C, 1w, in pure Ar)	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O4-z	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z		3	2005								58																				T'																		K				16			16																																																																																																TSFZ method. sample with different Tc were obtained by annealing in Ar.					Electronic inhomogeneity and competing phases in electron-doped superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 71(2005)100502	H.A.Mook,H.J.Kang,J.W.Lynn,Komiya,M.Matsuura,Pengcheng Dai,Seiki,Y.Kurita,Yoichi Ando		
12082	P071104503		YBa2Cu3O7	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7+z	6.9	1	2005																											3	Y123			A	3.8154	3.8842	11.678											Cu-1212	K				92.5			92.5																																																																																																mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12083	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.94Fe0.06O6.929	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7+z	6.929	1	2005																											3	Y123			A	3.8331	3.8712	11.674											Cu-1212	K				85			85																																																																																																mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12084	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.9Fe0.1O6.929	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	7+z	6.929	1	2005																											2	Y123			A	3.8577		11.694											Cu-1212	K				71			71																																																																																																mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12085	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.84Fe0.16O6.959	Y	1	Ba	2	Cu	2.84	Fe	0.16													O	7+z	6.959	1	2005																											2	Y123			A	3.8631		11.687											Cu-1212	K				53			53																																																																																																mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12086	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.68Fe0.32O6.999	Y	1	Ba	2	Cu	2.68	Fe	0.32													O	7+z	6.999	1	2005																											2	Y123			A	3.87		11.682											Cu-1212	K				26			26																																																																																																mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12087	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.6Fe0.4O7.024	Y	1	Ba	2	Cu	2.6	Fe	0.4													O	7+z	7.024	1	2005																											2	Y123			A	3.8727		11.675											Cu-1212	K					4																																																																																																		mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12088	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.5Fe0.5O7.241	Y	1	Ba	2	Cu	2.5	Fe	0.5													O	7+z	7.241	1	2005																											2	Y123			A	3.8742		11.671											Cu-1212	K					4																																																																																																		mixture - heat(880-930C, 70h) - SIN(930C,40h, in air) - cool to RT(30C/h)					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12089	P071104503		YBa2Cu3O7	Y1Ba2Cu3O7.19	Y	1	Ba	2	Cu	3															O	7+z	7.19	1	2005																											2	Y123			A	3.8531		11.621											Cu-1212	K				89			89																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12090	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.94Fe0.06O7.254	Y	1	Ba	2	Cu	2.94	Fe	0.06													O	7+z	7.254	1	2005																											2	Y123			A	3.8565		11.619											Cu-1212	K				91			91																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12091	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.9Fe0.1O7.293	Y	1	Ba	2	Cu	2.9	Fe	0.1													O	7+z	7.293	1	2005																											2	Y123			A	3.8596		11.629											Cu-1212	K				87			87																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12092	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.84Fe0.16O7.303	Y	1	Ba	2	Cu	2.84	Fe	0.16													O	7+z	7.303	1	2005																											2	Y123			A	3.8619		11.626											Cu-1212	K				85			85																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12093	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.68Fe0.32O7.343	Y	1	Ba	2	Cu	2.68	Fe	0.32													O	7+z	7.343	1	2005																											2	Y123			A	3.8635		11.619											Cu-1212	K				82			82																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12094	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.6Fe0.4O7.401	Y	1	Ba	2	Cu	2.6	Fe	0.4													O	7+z	7.401	1	2005																											2	Y123			A	3.8665		11.609											Cu-1212	K				82			82																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12095	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.5Fe0.5O7.413	Y	1	Ba	2	Cu	2.5	Fe	0.5													O	7+z	7.413	1	2005																											2	Y123			A	3.8708		11.59											Cu-1212	K				80			80																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12096	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.4Fe0.6O7.453	Y	1	Ba	2	Cu	2.4	Fe	0.6													O	7+z	7.453	1	2005																											2	Y123			A	3.8727		11.584											Cu-1212	K				62			62																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12097	P071104503		(Cu,Fe)Ba2YCu2O7	Y1Ba2Cu2.3Fe0.7O7.484	Y	1	Ba	2	Cu	2.3	Fe	0.7													O	7+z	7.484	1	2005																											2	Y123			A	3.8738		11.579											Cu-1212	K				60			60																																																																																																mixed with 5 wt% KCl4, wrapped in Au-foil. heat(1000C,0.5h, P=6 GPa) - Q to RT.					Superconductivity and Mossbauer effect of FexCu1-xBa2YCu2O7+y superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)104503	G.C.Che,K.Q.Li,N.L.Di,Y.H.Liu,Z.H.Cheng,Z.Q.Kou,Z.X.Zhao		
12098	P071104513	hydrostatic pressure. lattice const. from polycrystalline's values. Tc(poly) = 4.3 K.	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2005																												T			A	5.3322	5.3624	13.152												K				3.5			3.5	TC12098		K/GPa	4.1																																																																																												TSFZ method					High-pressure study of structural phase transitions and superconductivity in La1.48Nd0.4Sr0.12CuO4			DuPont Company, Central Research and Development, Wilmington, Delaware 19880-0356, USA	Phys.Rev.B, 71(2005)104513	D.E.Cox,E.M.McCarron,J.S.Schilling,M.K.Crawford,N.Ichikawa,Q.Huang,R.L.Harlow,S.Deemyad,S.Uchida,S.W.Tozer,V.Tissen		
12099	P071104516	Td2(OMT to Pccn transition ) at 67 K.	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2005																												T																		K		10					10	TC12099																																																																																																				Magnetic-field effects on the in-plane electrical resistivity in single-crystal La2-xBaxCuO4 and La1.6-xNd0.4SrxCuO4 around x= 1/8 : Implication for the field-induced stripe order			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B, 71(2005)104516	K.Kudo,N.Kitajima,N.Kobayashi,T.Adachi,T.Manabe,T.Sasaki,Y.Koike		
12100	PR05216213		YBa2Cu3O7	Y1Ba2Cu3O6.26	Y	1	Ba	2	Cu	3															O	7-d	6.26	1	1995																												Y123	P4/mmm						3																																																																																								TP12100																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12101	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La0.2Ba1.8Cu3O6.31	Y	1	La	0.2	Ba	1.8	Cu	3													O	7-d	6.31	1	1995																												Y123	P4/mmm						3																																																																																								TP12101																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12102	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La0.3Ba1.7Cu3O7-d	Y	1	La	0.3	Ba	1.7	Cu	3													O	7-d		1	1995																												Y123	P4/mmm						3																																																																																								TP12102																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12103	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La0.4Ba1.6Cu3O6.65	Y	1	La	0.4	Ba	1.6	Cu	3													O	7-d	6.65	1	1995																												Y123	P4/mmm						3																																																																																								TP12103																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12104	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La0.6Ba1.4Cu3O6.8	Y	1	La	0.6	Ba	1.4	Cu	3													O	7-d	6.8	1	1995																												Y123	P4/mmm						3																																																																																								TP12104																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12105	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La0.8Ba1.2Cu3O6.83	Y	1	La	0.8	Ba	1.2	Cu	3													O	7-d	6.83	1	1995																												Y123	P4/mmm						3																																																																																								TP12105																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12106	PR05216213		Y(La,Ba)2Cu3O7-d	Y1La1Ba1Cu3O7.07	Y	1	La	1	Ba	1	Cu	3													O	7-d	7.07	1	1995																												Y123	P4/mmm						3																																																																																								TP12106																									1	ANL (in air for 5days at 620C and at 700C for 5h)					Observation of variable-range hopping up to 900 K the YLaxBa2-xCu3O7-delta system	199512		Materials Science Research Center, Indian Institute of Technology, Madras 600 036, India	Phys.Rev.B,52(1995)16231	U.V. Varadaraju,V. Ponnambalam		
12107	PR05216246		YBa2Cu3Oy	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	y	6.94	3	1995																																																																																																																							micro.V/K	-2				mic.ohm.cm												125	4250	m3/C		-0.00000000000035	0.0000000000004			RH12107					The Sample is prepared by a crystal-pulling technique.See PhysicaC 217, 222 (1993).					Normal-state transport properties of slightly overdoped YBa2Cu3Oy crystals prepared by a crystal-pulling technique	199512			Phys.Rev.B,52(1995)16246	I. Terasaki,S. Miyamoto,S. Tajima,S. Tanaka,Y. Sato		
12108	PR05215099		PrBa2Cu3O7	Pr1Ba2Cu3O6.9	Pr	1	Ba	2	Cu	3															O	7-d	6.9	1	1995						2.97		17																				Y123																																																																														SP12108			mj/mol.K2	118																																						1	See Phys. Rev. B 44, 5384 (1991).					Magnetic-field effect on the specific heat of PrBa2(Cu1-xCax)3O7-z	199512			Phys.Rev.B,52(1995)15099	C.R. Shih,H.D. Yang,H.L. Tsay,T.H. Meen,Y.C. Chen		
12109	PR05215099		PrBa2(Cu,Ga)3O7-d	Pr1Ba2Cu2.88Ga0.12O6.9	Pr	1	Ba	2	Cu	2.88	Ga	0.12													O	7-d	6.9	1	1995								14																				Y123																																																																														SP12109			mj/mol.K2	151	C=A/T2+BT+DT3, for 0.6<T<5K																																					1	See Phys. Rev. B 44, 5384 (1991).					Magnetic-field effect on the specific heat of PrBa2(Cu1-xCax)3O7-z	199512			Phys.Rev.B,52(1995)15099	C.R. Shih,H.D. Yang,H.L. Tsay,T.H. Meen,Y.C. Chen		
12110	PR05215099		PrBa2(Cu,Ga)3O7-d	Pr1Ba2Cu2.76Ga0.24O6.9	Pr	1	Ba	2	Cu	2.76	Ga	0.24													O	7-d	6.9	1	1995								10																				Y123																																																																														SP12110			mj/mol.K2	168	fitting eq. C=A/T2+BT+DT3 for 0.6<T<5K																																					1	See Phys. Rev. B 44, 5384 (1991).					Magnetic-field effect on the specific heat of PrBa2(Cu1-xCax)3O7-z	199512			Phys.Rev.B,52(1995)15099	C.R. Shih,H.D. Yang,H.L. Tsay,T.H. Meen,Y.C. Chen		
12111	PR05216101		SrCuO3+d	Sr1Cu1O2.99	Sr	1	Cu	1																	O	3+d	2.99	1	1995																											3				A	3.916	3.502	12.706	3																																																																																				micro.V/K	710			TP12111																								SrCO3, CuO	1	CAL (at 950C in air)SIN (at 1000C in air)quench from 500C					Transport properties of Cu-O chains in Sr2CuO3+z	199512			Phys.Rev.B,52(1995)16101	J.-S. Zhou,J.B. Goodenough,W.B. Archibald		
12112	PR05216101		SrCuO3+d	Sr1Cu1O2.97	Sr	1	Cu	1																	O	3+d	2.97	1	1995																											3				A	3.917	3.5	12.713	3																																																																																				micro.V/K	280			TP12112																								SrCO3, CuO	1	CAL (at 950C in air)SIN (at 1000C in air)quench from 500C					Transport properties of Cu-O chains in Sr2CuO3+z	199512			Phys.Rev.B,52(1995)16101	J.-S. Zhou,J.B. Goodenough,W.B. Archibald		
12113	PR05216101	oxygen content is 2.971-2.97.	SrCuO3	Sr1Cu1O3+d	Sr	1	Cu	1																	O	3+d		1	1995																											3				A	3.915	3.499	12.712	3																																																																																				micro.V/K	53			TP12113																								SrCO3, CuO	1	CAL (at 950C in air)SIN (at 1000C in air)quench from 500C					Transport properties of Cu-O chains in Sr2CuO3+z	199512			Phys.Rev.B,52(1995)16101	J.-S. Zhou,J.B. Goodenough,W.B. Archibald		
12114	PR05215727		YBa2Cu3O7-d	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	7-d	6.94	3	1995																												Y123																		K				91.4			91.4																																																					SP12114																																											See J. Cryst. Growth 132, 389 (1993).ANN (at 480C under 1bar oxygen)					Evidence chain superconductivity in near-stoichiometric YBa2Cu3Ox sinle crystals	199512			Phys.Rev.B,52(1995)R15727	"A. Erb,G. Mu""ller-Vogt,H. Claus,H. Rietschel,H. Wu""hl,P. Schweiss,R. Hauff,V. Breit"		
12115	PR05215727		YBa2Cu3O7-d	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	7-d	6.98	3	1995																												Y123																		K				89.4			89.4																																																					SP12115																																											See J. Cryst. Growth 132, 389 (1993).ANN (at 440C under 1bar oxygen)					Evidence chain superconductivity in near-stoichiometric YBa2Cu3Ox sinle crystals	199512			Phys.Rev.B,52(1995)R15727	"A. Erb,G. Mu""ller-Vogt,H. Claus,H. Rietschel,H. Wu""hl,P. Schweiss,R. Hauff,V. Breit"		
12116	PR05215727		YBa2Cu3O7-d	Y1Ba2Cu3O6.99	Y	1	Ba	2	Cu	3															O	7-d	6.99	3	1995																												Y123																		K				87.8			87.8																																																																																																See J. Cryst. Growth 132, 389 (1993).ANN (at 380C under 70bar oxygen)					Evidence chain superconductivity in near-stoichiometric YBa2Cu3Ox sinle crystals	199512			Phys.Rev.B,52(1995)R15727	"A. Erb,G. Mu""ller-Vogt,H. Claus,H. Rietschel,H. Wu""hl,P. Schweiss,R. Hauff,V. Breit"		
12117	PR05215727		YBa2Cu3O7-d	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7-d	7	3	1995																												Y123																		K				87.5			87.5																																																					SP12117																																											See J. Cryst. Growth 132, 389 (1993).ANN (at 380C under 200bar oxygen)					Evidence chain superconductivity in near-stoichiometric YBa2Cu3Ox sinle crystals	199512			Phys.Rev.B,52(1995)R15727	"A. Erb,G. Mu""ller-Vogt,H. Claus,H. Rietschel,H. Wu""hl,P. Schweiss,R. Hauff,V. Breit"		
12118	PR05215636		(Hg,Cr)Sr2CuO4+d	Hg0.73Cr0.38Sr2Cu1.04O4+d	Hg	0.73	Cr	0.38	Sr	2	Cu	1.04													O	4+d		2	1995																											2		P4/mmm		A	3.85		8.696	4											K				60			60																																																																																														HgO, Cr2O3, Sr(NO3)2, CuO	1	Cr0.3Sr2CuOz precursor was prepared by SIN (at 700C for 3h, at 900C for 18h in flowing oxygen). Then HgO was added and SIN (at 870C for 6h)					Chromium clustering and ordering in Hg1-xCrxSr2CuO4+z	199512		Materials Science Division and Science and Technology Center for Superconductivity, Argonne National Laboratory Argonne, Illinois 60439	Phys.Rev.B,52(1995)15636	B. Dabrowski,B.G. Storey,D.G. Hinks,D.N. Argyriou,H. Zhang,J.D. Jorgensen,L.D. Marks,O. Chmaissem,V.P. Dravid,Y.Y. Wang		
12119	PR05215598		Bi2Sr2CaCu2O8+d	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1995																																														K		86					86																																																																						TP12119	mic.ohm.cm												660	7000000												See J. Cryst. Growth 92, 687 (1988).					Changes of the dimensionality and Tc through the iodine intercalation and oxidation in Bi2Sr2CaCu2O8+z single crystals	199512		Department of Applied Physics, Faculty of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,52(1995)15598	Akihiko Fujiwara,Akio Yamanaka,Fujio Minami,Norio Kobayashi,Shunji Takekawa,Takashi Noji,Terukazu Nishizaki,Yoji Koike,Yoshitami Saito		
12120	PR05215598		Bi2Sr2CaCu2O8+dI	Bi2Sr2Ca1Cu2I1O8+d	Bi	2	Sr	2	Ca	1	Cu	2	I	1											O	8+d		3	1995																																														K		80.7					80.7																																																																						TP12120	mic.ohm.cm												410	6700000											7	See J. Cryst. Growth 92, 687 (1988).Stage-one iodine intercalation was archieved by sealing as-grown crystals with elemental iodine separately and ANN (at 180C for 330h).					Changes of the dimensionality and Tc through the iodine intercalation and oxidation in Bi2Sr2CaCu2O8+z single crystals	199512		Department of Applied Physics, Faculty of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,52(1995)15598	Akihiko Fujiwara,Akio Yamanaka,Fujio Minami,Norio Kobayashi,Shunji Takekawa,Takashi Noji,Terukazu Nishizaki,Yoji Koike,Yoshitami Saito		
12121	PR05215598		Bi2Sr2CaCu2O8-d	Bi2Sr2Ca1Cu2O8-d	Bi	2	Sr	2	Ca	1	Cu	2													O	8-d		3	1995																																														K		81.7					81.7																																																																						TP12121	mic.ohm.cm												130	3800000											7	ANN (under 10 atm of oxygen at 550C for 140h or under 600 atm of oxygen at 900C for 320h)					Changes of the dimensionality and Tc through the iodine intercalation and oxidation in Bi2Sr2CaCu2O8+z single crystals	199512		Department of Applied Physics, Faculty of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B,52(1995)15598	Akihiko Fujiwara,Akio Yamanaka,Fujio Minami,Norio Kobayashi,Shunji Takekawa,Takashi Noji,Terukazu Nishizaki,Yoji Koike,Yoshitami Saito		
12122	PR05215551		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		2	1995																												Hg1223			A	3.852		15.764	4						A/GPa	-0.011		-0.09		K				132			132																																																																																															1	See Physica C 217, 265 (1993).Precursor is Ba2Ca2Cu3Ox.CAL (under flowing oxygen at 925C for 72h)Then, yellow HgO was addedPress(1.8GPa for 20min)Heat (at 880C fpr 40min)					Crystal structure of HgBa2Ca2Cu3O8+z at high pressure(to 8.5 GPa) determined by powder neutron diffraction	199512		ISIS Facility,Rutherford Appleton Laboratory,Chilton,Didcot,Oxfordshire, OX11 0QX, United Kingdom	Phys.Rev.B,52(1995)15551	A.R. Armsorong,I. Gameson,J.J. Capponi,M. Maregio,P. Bordet,P.P. Edward,W.I.F. David		
12123	PR05216233		(La,Sr)2Cu(O, F)4+d	La0.7Sr1.3Cu1FO4+d	La	0.7	Sr	1.3	Cu	1	F														O	4+d		2	1995																											2	T			A	3.937		13.037	3																																																																																																																							Superconductivity at 55 K in La0.7Sr1.3 Cu(O,F)4+delta with reduced CuO2 sheets and apical anions	199512		Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,52(1995)16233	Cong Wang,Guanghui Rao,Jingkui Liang,Weihua Tang,Xiaolong Chen		
12126	P071134526	c-axis grain-aligned sample. anisotropy=8 from Hc2. Hirr(ab) = 45 T. (dC/gamma*Tc) = 2.2.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2005																												IL																		K				43			43																				T	SP-heat		150	12										HC12126																						mj/mol.K2	1.2	SP-heat																																						high-pressure synthesis					Dimensionality of superconductivity and vortex dynamics in the infinite-layer cuprate Sr0.9M0.1CuO2 (M=La,Gd)			Department of Physics, California Institute of Technology, Pasadena, California, USA	Phys.Rev.B, 71(2005)134526	A.D.Beyer,C.H.Mielke,C.R.Hughes,K.H.Kim,M.S.Park,N.-C.Yeh,N.Harrison,S.-I.Lee,V.S.Zapf		
12127	P071134526	cohere<c> given in discussion. (dC/gamma*Tc) = 2.9. Curie-Weiss behavior for Tc<T<RT. 	(Sr,Gd)CuO2	Sr0.9Gd0.1Cu1O2	Sr	0.9	Gd	0.1	Cu	1															O	2			2005					per Gd	8.2																						IL																		K				43			43																																				A				5.2													SP12127			mj/mol.K2	1.2	SP-heat																																						high-pressure synthesis					Dimensionality of superconductivity and vortex dynamics in the infinite-layer cuprate Sr0.9M0.1CuO2 (M=La,Gd)			Department of Physics, California Institute of Technology, Pasadena, California, USA	Phys.Rev.B, 71(2005)134526	A.D.Beyer,C.H.Mielke,C.R.Hughes,K.H.Kim,M.S.Park,N.-C.Yeh,N.Harrison,S.-I.Lee,V.S.Zapf		
12128	L094117001	H//c-axis	YBa2Cu3Oz	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	6+z	6.35	3	2005																												Y123																		K		8.9					8.9											Oe	M-H curve			13.3																			HC12128																																																														Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12129	L094117001	H//c-axis. O-content not given.	YBa2Cu3Oz	Y1Ba2Cu3O6+z	Y	1	Ba	2	Cu	3															O	6+z		3	2005																												Y123																		K		13.7					13.7											Oe	M-H curve			27.3																			HC12128																																																														Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12130	L094117001	H//c-axis. O-content not given.	YBa2Cu3Oz	Y1Ba2Cu3O6+z	Y	1	Ba	2	Cu	3															O	6+z		3	2005																												Y123																		K		15.3					15.3											Oe	M-H curve			32.4																			HC12128																																																														Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12131	L094117001	H//c-axis. O-content not given.	YBa2Cu3Oz	Y1Ba2Cu3O6+z	Y	1	Ba	2	Cu	3															O	6+z		3	2005																												Y123																		K		17.6					17.6											Oe	M-H curve			40.6																			HC12128																																																														Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12132	L094117001	H//c-axis. O-content not given.	YBa2Cu3Oz	Y1Ba2Cu3O6+z	Y	1	Ba	2	Cu	3															O	6+z		3	2005																												Y123																		K		22					22											Oe	M-H curve			57.3																			HC12128																																																														Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12133	L094117001	ORTHO-II phase. ppenet calculated from Hc1 using G-L parameter = 50.	YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	6+z	6.5	3	2005																												Y123																		K		56					56											Oe	M-H curve			238																										A	from Hc1 using G-L.		1750																																																				Q to ice-water from 570C. different Tc were obtained by annealing at RT under 3000 bar hydrostatic pressure					Lower Critical Field and Superfluid Density of Highly Underdoped YBa2Cu3O6+x Single Crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 94(2005)117001	D.A.Bonn,David Broun,Ruixing Liang,W.N.Hardy		
12134	P069184513	ORTHO-II. Gd-content - 1.05 - 1.35 at% for ESR measurement. penet(a)=202, penet(b)=140 nm.	YBa2Cu3Oz	Y1Ba2Cu3O6.52	Y	1	Ba	2	Cu	3															O	6+z	6.52	3	2004																												Y123																		K				56			56																																									nm	zero-field ESR		168	7500																																																			self-flux method using BaZrO3 crucible.					Absolute values of the London penetration depth in YBa2Cu3O6+y measured by zero field ESR spectroscopy on Gd doped single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada	Phys.Rev.B, 69(2004)184513	D.A.Bonn,G.K.Mullins,J.S.Bobowski,M.Raudsepp,P.J.Turner,R.Harris,Ruixing Liang,T.Pereg-Barnea,W.N.Hardy		
12135	P069184513	ORTHO-III. Gd-content - 1.05 - 1.35 at% for ESR measurement. penet(a)=135, penet(b)=116 nm.	YBa2Cu3Oz	Y1Ba2Cu3O6.77	Y	1	Ba	2	Cu	3															O	6+z	6.77	3	2004																												Y123																		K				75			75																																									nm	zero-field ESR		125	2068																																																			self-flux method using BaZrO3 crucible.					Absolute values of the London penetration depth in YBa2Cu3O6+y measured by zero field ESR spectroscopy on Gd doped single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada	Phys.Rev.B, 69(2004)184513	D.A.Bonn,G.K.Mullins,J.S.Bobowski,M.Raudsepp,P.J.Turner,R.Harris,Ruixing Liang,T.Pereg-Barnea,W.N.Hardy		
12136	P069184513	ORTHO-I. Gd-content - 1.05 - 1.35 at% for ESR measurement. penet(a)=103, penet(b)=80 nm.	YBa2Cu3Oz	Y1Ba2Cu3O6.995	Y	1	Ba	2	Cu	3															O	6+z	6.995	3	2004																												Y123																		K				89			89																																									nm	zero-field ESR		91	635																																																			self-flux method using BaZrO3 crucible.					Absolute values of the London penetration depth in YBa2Cu3O6+y measured by zero field ESR spectroscopy on Gd doped single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada	Phys.Rev.B, 69(2004)184513	D.A.Bonn,G.K.Mullins,J.S.Bobowski,M.Raudsepp,P.J.Turner,R.Harris,Ruixing Liang,T.Pereg-Barnea,W.N.Hardy		
12137	PRL0792875	twin boundary spacing = 1 micron. G-L =17.0.	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6+z	6.6	1	1997																												Y123																		K		59					59																																									A	muon-SR		1586																																																									Measurement of the Fundamental Length Scales in the Vortex State of YBa2Cu3O6.60			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 79(1997)2875	C.E.Stronach,D.A.Bonn,D.R.Noakes,J.E.Sonier,J.H.Brewer,M.F.White, Jr,R.F.Kiefl,R.I.Miller,Ruixing Liang,S.R.Dunsiger,T.M.Riseman,W.A.MacFarlane,W.N.Hardy		
12138	PRL0792875	detwinned sample. G-L = 17.0.	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6+z	6.6	1	1997																												Y123																		K		59					59																																									A	muon-SR		1699																																																									Measurement of the Fundamental Length Scales in the Vortex State of YBa2Cu3O6.60			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada 	Phys.Rev.Lett., 79(1997)2875	C.E.Stronach,D.A.Bonn,D.R.Noakes,J.E.Sonier,J.H.Brewer,M.F.White, Jr,R.F.Kiefl,R.I.Miller,Ruixing Liang,S.R.Dunsiger,T.M.Riseman,W.A.MacFarlane,W.N.Hardy		
12139	L094127001	Uemura relation is not valid.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2005																												IL																		K		43					43																																									A	muon-SR		1160																																																				high-pressure method using cubic multianvil press.					Muon-Spin-Rotation Measurements of the Penetration Depth of the Infinite-Layer Electron-Doped Sr0.9La0.1CuO2 Cuprate Superconductor			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 94(2005)127001	A.Shengelaya,D.Di Castro,D.G.Eshchenko,H.Keller,I.M.Savic,K.A.Muller,K.H.Kim,M.S.Park,R.Khasanov,Sung-IK Lee		
12140	JPS0723039	two step transition. For H=0.2T, single step behaviour. Gruneisen parameter of Tc, Hc2 are 96 and 243.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2003																												pyrochlore																		K		0.96					0.96	TC12140																			T	resistive transition	0.3																																																																															Superconductivity of Cd2Re2O7 under pressure			ISSP, University of Tokyo, Kashiwa,Chiba,Japan	J.Phys.Soc.Jpn, 72(2003)3039	M.Abliz,M.Hanawa,M.Hedo,T.Matsumoto,Y.Uwatoko,Z.Hiroi		
12141	PHC4200023	impurity phases=SrO2, unknown. Cl-content=nominal	Sr2CuO2Clz	Sr2Cu1Cl0.8O2+z	Sr	2	Cu	1	Cl	0.8															O	2+z		1	2005																												T			A	3.9231		15.6742												K		33					33																																																																																																precursor(Sr2CuO3,Sr2CuO2Cl2), mixed with SrO2 and CuO, then high pressure synthesis(1050C, 30min, P=6GPa)					"High pressure synthesis of a new superconductor Sr2CuO2+zCl2-y induced by ""apical oxygen doping"""			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 420(2005)23	C.Dong,C.Q.Jin,F.Y.Li,Q.Q.Liu,X.M.Qin,Y.Yu		
12142	PHC4200023	impurity phases=SrO2, unknown. Cl-content=nominal	Sr2CuO2Clz	Sr2Cu1Cl1O2+z	Sr	2	Cu	1	Cl	1															O	2+z		1	2005																												T			A	3.9329		15.654												K		20					20																																																																																																precursor(Sr2CuO3,Sr2CuO2Cl2), mixed with SrO2 and CuO, then high pressure synthesis(1050C, 30min, P=6GPa)					"High pressure synthesis of a new superconductor Sr2CuO2+zCl2-y induced by ""apical oxygen doping"""			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 420(2005)23	C.Dong,C.Q.Jin,F.Y.Li,Q.Q.Liu,X.M.Qin,Y.Yu		
12143	PHC4200023	impurity phases=SrO2, unknown. Cl-content=nominal	Sr2CuO2Clz	Sr2Cu1Cl1.2O2+z	Sr	2	Cu	1	Cl	1.2															O	2+z		1	2005																												T			A	3.9435		15.6426												K		30					30																																																																																																precursor(Sr2CuO3,Sr2CuO2Cl2), mixed with SrO2 and CuO, then high pressure synthesis(1050C, 30min, P=6GPa)					"High pressure synthesis of a new superconductor Sr2CuO2+zCl2-y induced by ""apical oxygen doping"""			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 420(2005)23	C.Dong,C.Q.Jin,F.Y.Li,Q.Q.Liu,X.M.Qin,Y.Yu		
12144	PHC4200023	impurity phases=SrO2, unknown. Cl-content=nominal	Sr2CuO2Clz	Sr2Cu1Cl1.4O2+z	Sr	2	Cu	1	Cl	1.4															O	2+z		1	2005																												T			A	3.961		15.6253												K		30					30																																																																																																precursor(Sr2CuO3,Sr2CuO2Cl2), mixed with SrO2 and CuO, then high pressure synthesis(1050C, 30min, P=6GPa)					"High pressure synthesis of a new superconductor Sr2CuO2+zCl2-y induced by ""apical oxygen doping"""			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 420(2005)23	C.Dong,C.Q.Jin,F.Y.Li,Q.Q.Liu,X.M.Qin,Y.Yu		
12145	PHC4190121		PrBa2Cu3Oz	Pr1Ba2Cu3Oz	Pr	1	Ba	2	Cu	3															O	z		1	2005								16.6																				Y123			A	3.8638	3.8916	11.7943												K					5																																																																																																Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12146	PHC4190121	RES77=RES(T=50 K)	Pr(Ba,Sr)2Cu3Oz	Pr1Ba1.9Sr0.1Cu3Oz	Pr	1	Ba	1.9	Sr	0.1	Cu	3													O	z		1	2005								17.3																				Y123			A	3.8672	3.8901	11.7857												K					5																																																																									Ohm.m				0.06																			Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12147	PHC4190121	RES77=RES(T=50 K)	Pr(Ba,Sr)2Cu3Oz	Pr1Ba1.8Sr0.2Cu3Oz	Pr	1	Ba	1.8	Sr	0.2	Cu	3													O	z		1	2005								17.7																				Y123			A	3.868	3.9034	11.7777												K					5																																																																									Ohm.m				0.09																			Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12148	PHC4190121	RES77=RES(T=50 K)	Pr(Ba,Sr)2Cu3Oz	Pr1Ba1.7Sr0.3Cu3Oz	Pr	1	Ba	1.7	Sr	0.3	Cu	3													O	z		1	2005								18																				Y123			A	3.8695	3.9015	11.7651												K					5																																																																									Ohm.m				0.58																			Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12149	PHC4190121	RES77=RES(T=50 K)	Pr(Ba,Sr)2Cu3Oz	Pr1Ba1.6Sr0.4Cu3Oz	Pr	1	Ba	1.6	Sr	0.4	Cu	3													O	z		1	2005								17.9																				Y123			A	3.8695		11.6969												K					5																																																																									Ohm.m				4.02																			Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12150	PHC4190121	RES77=RES(T=50 K)	Pr(Ba,Sr)2Cu3Oz	Pr1Ba1.5Sr0.5Cu3Oz	Pr	1	Ba	1.5	Sr	0.5	Cu	3													O	z		1	2005								17.8																				Y123			A	3.8882		11.6666												K					5																																																																									Ohm.m				2.91																			Pr6O11,BaCO3,SrCO3,CuO	1	mixture - CAL(930C,48h,in air) - SIN(940C,24h, in air) - ANN(450C,48h, in air)					Effects of Sr-doping on the phase transition and electrical properties in PrBa2-xSrxCu3Oy			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 419(2005)121	K.Yoshida,T.Sonobe		
12151	PCS0631027	2nd order phase transition at 200K. thermal expansion coeff. = 4.9 E-6 /K.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7			2002																												pyrochlore			A	10.226														K		1					1																																																					SP12151																																																Structural phase transition in the superconducting pyrochlore oxide Cd2Re2O7			Material Design and Characterization Laboratory, ISSP, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Chem.Solids, 63(2002)1027	F.Sakai,J.Yamaura,M.Hanawa,Y.Muraoka,Z.Hiroi		
12152	PCS0631027	M-I transition at 226K with no anomaly. not SC. thermal expansion coeff. = 4.3 E-6 /K.	Cd2Os2O7	Cd2Os2O7	Cd	2	Os	2																	O	7			2002																												pyrochlore																		K					1																																																																																																							Structural phase transition in the superconducting pyrochlore oxide Cd2Re2O7			Material Design and Characterization Laboratory, ISSP, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Chem.Solids, 63(2002)1027	F.Sakai,J.Yamaura,M.Hanawa,Y.Muraoka,Z.Hiroi		
12153	PHC4210056		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2005																												T			A	3.7733		13.2235												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12154	PHC4210056	SC volume decreases with increasing Mn content. Tc(end) not given.	(La,Sr)2(Cu,Mn)O4	La1.82Sr0.18Cu0.98Mn0.02O4	La	1.82	Sr	0.18	Cu	0.98	Mn	0.02													O	4		1	2005																												T			A	3.7761		13.2174												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12155	PHC4210056	SC volume decreases with increasing Mn content. Tc(end) not given.	(La,Sr)2(Cu,Mn)O4	La1.79Sr0.21Cu0.96Mn0.04O4	La	1.79	Sr	0.21	Cu	0.96	Mn	0.04													O	4		1	2005																												T			A	3.7808		13.1964												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12156	PHC4210056	SC volume decreases with increasing Mn content. Tc(end) not given.	(La,Sr)2(Cu,Mn)O4	La1.76Sr0.24Cu0.94Mn0.06O4	La	1.76	Sr	0.24	Cu	0.94	Mn	0.06													O	4		1	2005																												T			A	3.7818		13.1367												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12157	PHC4210056	SC volume decreases with increasing Mn content. Tc(end) not given.	(La,Sr)2(Cu,Mn)O4	La1.73Sr0.27Cu0.92Mn0.08O4	La	1.73	Sr	0.27	Cu	0.92	Mn	0.08													O	4		1	2005																												T			A	3.7822		13.1028												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12158	PHC4210056	SC volume decreases with increasing Mn content. Tc(end) not given.	(La,Sr)2(Cu,Mn)O4	La1.7Sr0.3Cu0.9Mn0.1O4	La	1.7	Sr	0.3	Cu	0.9	Mn	0.1													O	4		1	2005																												T			A	3.7837		13.0371												K			37				37																																																																																														La2O3,SrCO3,CuO,MnO2	1	mixture - heat(1150C,48h, in O2)					Effects of Mn doping on the superconductivity in La2-xSrxCuO4			Department of Telecommunication and Electric Engineering, Hefei University, Hefei 230027, Anhui, People's Republic of China	Physica C, 421(2005)56	Changjin Zhang,Hui Huang,Min Tan,Yuheng Zhang		
12159	PHC4210001	Cu(1) site substituted by CO3. CO2 concentration in sintering process = 400 ppm)	YBa2(Cu,CO3)3Oz	Y1Ba2Cu2.99C0.01Oz	Y	1	Ba	2	Cu	2.99	C	0.01													O	z		1	2005																												Y123			A	3.82	3.885	11.676												K		93					93																																																																																																mixture - CAL(860C,48h, in air) - CAL(in vac) - SIN(900C, in O2 + CO2)					Effects of carbon incorporation on doping state of YBa2Cu3Oy			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 421(2005)1	A.Yamamoto,K.Hirose,S.Tajima,T.Kakeshita,Y.Itoh		
12160	PHC4210001	Cu(1) site substituted by CO3. CO2 concentration in sintering process = 800 ppm)	YBa2(Cu,CO3)3Oz	Y1Ba2Cu2.98C0.02Oz	Y	1	Ba	2	Cu	2.98	C	0.02													O	z		1	2005																												Y123			A	3.823	3.888	11.67												K		92					92																																																																																																mixture - CAL(860C,48h, in air) - CAL(in vac) - SIN(900C, in O2 + CO2)					Effects of carbon incorporation on doping state of YBa2Cu3Oy			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 421(2005)1	A.Yamamoto,K.Hirose,S.Tajima,T.Kakeshita,Y.Itoh		
12161	PHC4210001	Cu(1) site substituted by CO3. CO2 concentration in sintering process = 2000 ppm)	YBa2(Cu,CO3)3Oz	Y1Ba2Cu2.96C0.04Oz	Y	1	Ba	2	Cu	2.96	C	0.04													O	z		1	2005																												Y123			A	3.827	3.887	11.663												K		80					80																																																																																																mixture - CAL(860C,48h, in air) - CAL(in vac) - SIN(900C, in O2 + CO2)					Effects of carbon incorporation on doping state of YBa2Cu3Oy			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 421(2005)1	A.Yamamoto,K.Hirose,S.Tajima,T.Kakeshita,Y.Itoh		
12162	PHC4210001	Cu(1) site substituted by CO3. CO2 concentration in sintering process = 4000 ppm)	YBa2(Cu,CO3)3Oz	Y1Ba2Cu2.92C0.08Oz	Y	1	Ba	2	Cu	2.92	C	0.08													O	z		1	2005																												Y123			A	3.828	3.889	11.64												K		65					65																																																																																																mixture - CAL(860C,48h, in air) - CAL(in vac) - SIN(900C, in O2 + CO2)					Effects of carbon incorporation on doping state of YBa2Cu3Oy			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 421(2005)1	A.Yamamoto,K.Hirose,S.Tajima,T.Kakeshita,Y.Itoh		
12163	PHC2820887	as-sintered. Cu-valence = 2.12	(Hg,Tl)2Ba2YCu2Oz	Hg1.4Tl0.6Ba2Y1Cu2O7.92	Hg	1.4	Tl	0.6	Ba	2	Y	1	Cu	2											O	z	7.92		1997																												Hg2212			A	3.867		28.88												K				11.7			11.7																																		HC12163																																																														high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12164	PHC2820887	as-sintered. Cu-valence = 2.13	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.9Ca0.1Cu2O7.88	Hg	1.4	Tl	0.6	Ba	2	Y	0.9	Ca	0.1	Cu	2									O	z	7.88		1997																												Hg2212			A	3.864		28.88												K				37			37																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12165	PHC2820887	as-sintered. Cu-valence = 2.14	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.8Ca0.2Cu2O7.83	Hg	1.4	Tl	0.6	Ba	2	Y	0.8	Ca	0.2	Cu	2									O	z	7.83		1997																												Hg2212			A	3.862		28.87												K				50			50																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12166	PHC2820887	as-sintered. Cu-valence = 2.16	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.7Ca0.3Cu2O7.81	Hg	1.4	Tl	0.6	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	z	7.81		1997																												Hg2212			A	3.859		28.95												K				74.5			74.5																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12167	PHC2820887	as-sintered. Cu-valence = 2.18	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.6Ca0.4Cu2O7.78	Hg	1.4	Tl	0.6	Ba	2	Y	0.6	Ca	0.4	Cu	2									O	z	7.78		1997																												Hg2212			A	3.857		28.99												K				84.6			84.6																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12168	PHC2820887	as-sintered. Cu-valence = 2.19	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.5Ca0.5Cu2O7.74	Hg	1.4	Tl	0.6	Ba	2	Y	0.5	Ca	0.5	Cu	2									O	z	7.74		1997																												Hg2212			A	3.854		29.02												K				84			84																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12169	PHC2820887	as-sintered. Cu-valence = 2.21	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.4Ca0.6Cu2O7.71	Hg	1.4	Tl	0.6	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	z	7.71		1997																												Hg2212			A	3.85		29.13												K				68.6			68.6																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12170	PHC2820887	as-sintered. Cu-valence = 2.24	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.3Ca0.7Cu2O7.68	Hg	1.4	Tl	0.6	Ba	2	Y	0.3	Ca	0.7	Cu	2									O	z	7.68		1997																												Hg2212			A	3.848		29.19												K				66.4			66.4																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12171	PHC2820887	as-sintered. Cu-valence = 2.26	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.2Ca0.8Cu2O7.66	Hg	1.4	Tl	0.6	Ba	2	Y	0.2	Ca	0.8	Cu	2									O	z	7.66		1997																												Hg2212			A	3.845		29.23												K				35.3			35.3																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12172	PHC2820887	as-sintered	(Hg,Tl)2Ba2CaCu2Oz	Hg1.4Tl0.6Ba2Ca1Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	1	Cu	2											O	z			1997																												Hg2212																		K					4.2																																																																																																		high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12173	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2YCu2Oz	Hg1.4Tl0.6Ba2Y1Cu2O7.92	Hg	1.4	Tl	0.6	Ba	2	Y	1	Cu	2											O	z	7.92		1997																												Hg2212																		K					4.2																																																																																																		high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12174	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.9Ca0.1Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.9	Ca	0.1	Cu	2									O	z			1997																												Hg2212																		K				20.3			20.3																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12175	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.8Ca0.2Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.8	Ca	0.2	Cu	2									O	z			1997																												Hg2212																		K				45.1			45.1																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12176	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.7Ca0.3Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	z			1997																												Hg2212																		K				60.1			60.1																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12177	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.6Ca0.4Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.6	Ca	0.4	Cu	2									O	z			1997																												Hg2212																		K				75.5			75.5																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12178	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.5Ca0.5Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.5	Ca	0.5	Cu	2									O	z			1997																												Hg2212																		K				81.4			81.4																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12179	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.4Ca0.6Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	z			1997																												Hg2212																		K				90.5			90.5																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12180	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.3Ca0.7Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.3	Ca	0.7	Cu	2									O	z			1997																												Hg2212																		K				65.4			65.4																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12181	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2(Y,Ca)Cu2Oz	Hg1.4Tl0.6Ba2Y0.2Ca0.8Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Y	0.2	Ca	0.8	Cu	2									O	z			1997																												Hg2212																		K				60.5			60.5																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12182	PHC2820887	ANN(290-450C,Ar-flow)	(Hg,Tl)2Ba2CaCu2Oz	Hg1.4Tl0.6Ba2Ca1Cu2Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	1	Cu	2											O	z			1997																												Hg2212																		K				34			34																																																																																																high-pressure-synthesis(1000-1050C, 1-8h, 5-6 GPa)					A new Hg-based homologous series of cuprate superconductors; (Hg,Tl)-22(n-1)n (n=1,5)			SRL-ISTEC, Shinonome,Tokyo,Japan	Physica C, 282-287(1997)887	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tatsuki,X.-J.Wu		
12183	PHC2730065		(Hg,Tl)2Ba2Ca2Cu3Oz	Hg1.4Tl0.6Ba2Ca2Cu3Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	2	Cu	3											O	z			1996																												Hg2223			A	3.8426		35.773												K				85.1			85.1																																																																																																Tl2O3,CaO,CuO added to precursor(Ba2Ca2Cu3Oz). mixture - heat(1000C,1-8h,P=5 GPa) - ANN(300C,12h, in flowing Ar)					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12184	PHC2730065		(Hg,Tl)2Ba2Ca2Cu3Oz	Hg1.2Tl0.8Ba2Ca2Cu3Oz	Hg	1.2	Tl	0.8	Ba	2	Ca	2	Cu	3											O	z			1996																												Hg2223			A	3.8454		35.749												K				88.1			88.1																																																																																																Tl2O3,CaO,CuO added to precursor(Ba2Ca2Cu3Oz). mixture - heat(1000C,1-8h,P=5 GPa) - ANN(300C,12h, in flowing Ar)					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12185	PHC2730065		(Hg,Tl)2Ba2Ca2Cu3Oz	Hg1Tl1Ba2Ca2Cu3Oz	Hg	1	Tl	1	Ba	2	Ca	2	Cu	3											O	z			1996																												Hg2223			A	3.844		35.687												K				88.6			88.6																																																																																																Tl2O3,CaO,CuO added to precursor(Ba2Ca2Cu3Oz). mixture - heat(1000C,1-8h,P=5 GPa) - ANN(300C,12h, in flowing Ar)					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12186	PHC2730065		(Hg,Tl)2Ba2Ca2Cu3Oz	Hg0.8Tl1.2Ba2Ca2Cu3Oz	Hg	0.8	Tl	1.2	Ba	2	Ca	2	Cu	3											O	z			1996																												Hg2223			A	3.8429		35.634												K				90.7			90.7																																																																																																Tl2O3,CaO,CuO added to precursor(Ba2Ca2Cu3Oz). mixture - heat(1000C,1-8h,P=5 GPa) - ANN(300C,12h, in flowing Ar)					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12187	PHC2730065		(Hg,Tl)2Ba2Ca3Cu4Oz	Hg1.4Tl0.6Ba2Ca3Cu4Oz	Hg	1.4	Tl	0.6	Ba	2	Ca	3	Cu	4											O	z			1996																												Hg2234			A	3.8488		42.139												K				116			116																																																																																																Hg:Tl:Ba:Ca:Cu=0.9:1.2:1.8:3.0:4.0) nominal. See num=12183.					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12188	PHC2730065		(Hg,Tl)2Ba2Ca3Cu4Oz	Hg1.2Tl0.8Ba2Ca3Cu4Oz	Hg	1.2	Tl	0.8	Ba	2	Ca	3	Cu	4											O	z			1996																												Hg2234			A	3.8469		42.131												K				114			114																																																																																																Hg:Tl:Ba:Ca:Cu=0.9:1.2:1.8:3.0:4.0) nominal. See num=12183.					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12189	PHC2730065		(Hg,Tl)2Ba2Ca3Cu4Oz	Hg1Tl1Ba2Ca3Cu4Oz	Hg	1	Tl	1	Ba	2	Ca	3	Cu	4											O	z			1996																												Hg2234			A	3.8429		42.029												K				112			112																																																																																																Hg:Tl:Ba:Ca:Cu=0.9:1.2:1.8:3.0:4.0) nominal. See num=12183.					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12190	PHC2730065		(Hg,Tl)2Ba2Ca3Cu4Oz	Hg0.8Tl1.2Ba2Ca3Cu4Oz	Hg	0.8	Tl	1.2	Ba	2	Ca	3	Cu	4											O	z			1996																												Hg2234			A	3.8432		41.927												K				107.6			107.6																																																																																																Hg:Tl:Ba:Ca:Cu=0.9:1.2:1.8:3.0:4.0) nominal. See num=12183.					Structural and superconducting properties of (Hg1-xTlx)2Ba2Can-1CuOy(n=3,4) superconductors prepared under high pressure	199612		SRL-ISTEC,1-10-13 Shinonome,Koto-ku, Tokyo 135 Japan	Physica.C,273(1996)65-71	A. Tokiwa-Yamamoto,A.Tokiwa-Yamamoto,K. Tanabe,K.Tanabe,S. Adachi,S.Adachi,T. Tamura,T. Tatsuki,T.Tamura,T.Tatsuki,X.-J. Wu,X.-J.Wu,Y. Moriwaki,Y.Moriwaki		
12191	ADS0090399		HgTlBa2CuO6	Hg1Tl1Ba2Cu1O6	Hg	1	Tl	1	Ba	2	Cu	1													O	6			1997																												Hg2201			A	3.836		23.24												K					4.2																																																																																																HgO,Tl2O3,BaO2,CaO,CuO,Cu		high pressure synthesis(1000C, 1-8h, 6 GPa). nominal composition = HgTlBa2Ca(n-1)Cu(n)O(2n+4).					Effect of oxygen partial pressure on the formation of (Hg,Tl)2Ba2Can-1CunOy(n=1 - 6) phases				Adv.Supercond. IX,ISS-96 in Sapporo	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tamura,T.Tatsuki,Xiao-Jing Wu,Y.Moriwaki		
12192	ADS0090399		HgTlBa2CaCu2O8	Hg1Tl1Ba2Ca1Cu2O8	Hg	1	Tl	1	Ba	2	Ca	1	Cu	2											O	8			1997																												Hg2212			A	3.845		29.22												K				35			35																																																																																														HgO,Tl2O3,BaO2,CaO,CuO,Cu		high pressure synthesis(1000C, 1-8h, 6 GPa). nominal composition = HgTlBa2Ca(n-1)Cu(n)O(2n+4).					Effect of oxygen partial pressure on the formation of (Hg,Tl)2Ba2Can-1CunOy(n=1 - 6) phases				Adv.Supercond. IX,ISS-96 in Sapporo	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tamura,T.Tatsuki,Xiao-Jing Wu,Y.Moriwaki		
12193	ADS0090399		HgTlBa2Ca2Cu3O10	Hg1Tl1Ba2Ca2Cu3O10	Hg	1	Tl	1	Ba	2	Ca	2	Cu	3											O	10			1997																												Hg2223			A	3.844		35.71												K				76			76																																																																																														HgO,Tl2O3,BaO2,CaO,CuO,Cu		high pressure synthesis(1000C, 1-8h, 6 GPa). nominal composition = HgTlBa2Ca(n-1)Cu(n)O(2n+4).					Effect of oxygen partial pressure on the formation of (Hg,Tl)2Ba2Can-1CunOy(n=1 - 6) phases				Adv.Supercond. IX,ISS-96 in Sapporo	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tamura,T.Tatsuki,Xiao-Jing Wu,Y.Moriwaki		
12194	ADS0090399		HgTlBa2Ca3Cu4O12	Hg1Tl1Ba2Ca3Cu4O12	Hg	1	Tl	1	Ba	2	Ca	3	Cu	4											O	12			1997																												Hg2234			A	3.848		42.11												K				110			110																																																																																														HgO,Tl2O3,BaO2,CaO,CuO,Cu		high pressure synthesis(1000C, 1-8h, 6 GPa). nominal composition = HgTlBa2Ca(n-1)Cu(n)O(2n+4).					Effect of oxygen partial pressure on the formation of (Hg,Tl)2Ba2Can-1CunOy(n=1 - 6) phases				Adv.Supercond. IX,ISS-96 in Sapporo	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tamura,T.Tatsuki,Xiao-Jing Wu,Y.Moriwaki		
12195	ADS0090399		HgTlBa2Ca4Cu5O14	Hg1Tl1Ba2Ca4Cu5O14	Hg	1	Tl	1	Ba	2	Ca	4	Cu	5											O	14			1997																												Hg2245			A	3.85		48.44												K				90			90																																																																																														HgO,Tl2O3,BaO2,CaO,CuO,Cu		high pressure synthesis(1000C, 1-8h, 6 GPa). nominal composition = HgTlBa2Ca(n-1)Cu(n)O(2n+4).					Effect of oxygen partial pressure on the formation of (Hg,Tl)2Ba2Can-1CunOy(n=1 - 6) phases				Adv.Supercond. IX,ISS-96 in Sapporo	A.Tokiwa-Yamamoto,K.Tanabe,S.Adachi,T.Tamura,T.Tatsuki,Xiao-Jing Wu,Y.Moriwaki		
12196	APL0561281	Fig.Tc shows Tc(off) for various ANN conditions	(Tl,Pb,Bi)Sr2Ca3Cu4Oz	Tl0.64Pb0.2Bi0.16Sr2Ca3Cu4Oz	Tl	0.64	Pb	0.2	Bi	0.16	Sr	2	Ca	3	Cu	4									O	z			1990																												Tl1234																		K	120		125				122.5	TC12196																																																																																													PbO,Bi2O3,SrCO3,CaCO3,CuO		precursor(Pb,Bi)Sr2Ca2Cu3Oz) + Tl2O3, heat(920C, in O2) - mix with (CaO+CuO) - SIN(920C,10h, in O2) - ANN(600,500,400C)					(Tl,Pb,Bi)Sr2Ca2Cu3Oz superconductors with zero resistance at 120 K			ISTEC,Tokyo,Japan	Appl.Phys.Lett., 56(1990)1281	H.Yamauchi,S.Tanaka,T.Kaneko,T.Wada		
12197	PHB3190310	d=1000A. resistive transition measured upto 110 T by pulsed field.	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		5	2002																												Y123																		K		84					84																				T	pulse field			120					T/K				2	HC12197																																																														films grown on MgO by laser ablation					High-magnetic-field study of high-Tc cuprates			 Institute for Solid States Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa-shi, 277-8581 Chiba, Japan	Physica B, 319(2002)310	H.Nakagawa,H.Sato,M.Naito,N.Miura,T.Sekitani,Y.Enomoto		
12200	PR05300086	To perform measurements of anistropic properties, we mechanically powdered the bulk sumple, mixed the powder with a resin and applied a magnetic field of 8 T at room temperature for 24 h.	HgBa2CuO4	Hg1Ba2Cu1O4+d	Hg	1	Ba	2	Cu	1															O	4+d		1	1996																												Hg1201																		K				96			96											Oe	NHC1=Phi_0/4*pi*lambda_ab^2 [ln(lanmbda_ab/xi_ab)+0.5]PHC1=Phi_0/4*pi*lambda_ab*lambda_c [ln(lanmbda		82	129					T	H_c2c(T)=H_c2c(0)[1-(T/Tc)^4]  Hc2ab=gamma*Hc2cgamma=lambda_c/lambda_ab		125	72												A	xi_ab=(Phi_0/2piH_c2c)^(1/2)xi_c=xi_ab/gammagamma=lambda_c/lambda_ab		21.1	12.1	A	get lambda(0) by the equation : lambda(T)=lambda(0)/[1-(T/Tc)^2.76]^0.6 :  lambda(T) is experimental		2600	4540																																																	HgO, BaO, CuO	1	MIX(HgO, BaO, CuO)-SIN(650C, 1h, in evacuated quartz tube)-ANN(300C, 6h, in flowing argon)				optimally doped	Overdoped regime of the high-Tc superconductor HgBa2CuO4+z and the relation between nirmal and superconducting carrier densities	01		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,53(1996)86	H. Yamauchi,R. Puz'niak,R. Usami	Hg, Ba, Cu, O	
12201	PR05300086	To perform measurements of anistropic properties, we mechanically powdered the bulk sumple, mixed the powder with a resin and applied a magnetic field of 8 T at room temperature for 24 h.	HgBa2CuO4	Hg1Ba2Cu1O4+d	Hg	1	Ba	2	Cu	1															O	4+d		1	1996																												Hg1201																		K				52			52											Oe	NHC1=Phi_0/4*pi*lambda_ab^2 [ln(lanmbda_ab/xi_ab)+0.5]PHC1=Phi_0/4*pi*lambda_ab*lambda_c [ln(lanmbda		71	89					T	H_c2c(T)=H_c2c(0)[1-(T/Tc)^4]  Hc2ab=gamma*Hc2cgamma=lambda_c/lambda_ab		25.7	19.4												A	xi_ab=(Phi_0/2piH_c2c)^(1/2)xi_c=xi_ab/gammagamma=lambda_c/lambda_ab		41.1	31	A	get lambda(0) by the equation : lambda(T)=lambda(0)/[1-(T/Tc)^2.76]^0.6 :  lambda(T) is experimental		2980	3950																																																	HgO, BaO, CuO	1	MIX(HgO, BaO, CuO)-SIN(650C, 1h, in evacuated quartz tube)-ANN(200C, 6h, in flowing oxygen)				over doped	Overdoped regime of the high-Tc superconductor HgBa2CuO4+z and the relation between nirmal and superconducting carrier densities	01		Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,53(1996)86	H. Yamauchi,R. Puz'niak,R. Usami	Hg, Ba, Cu, O	
12202	PR05300094		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	3	1996																												Y124																												K/GPa	5.6																																																																																											5	Single crystalline YBa2Cu4O8 was grown at 900 bars O2 and 1050C,using a BaO-CuO-rich flux.-ANN(500C,2h)					Anisotropic pressure dependence of the resistivity in YBa2Cu4O8	01		"Laboratorium fu""r Festkorperphysik, Eidgeno""ssische Technische Hodhschule Zu""rich, 8093 Zu""rich, Swizerland"	Phys.Rev.B,53(1996)94	B, Bucher,E. Kaldis,J. Karpinski,P. Wachter	Y, Ba, Cu, O	
12203	PR05300905		Bi2Sr2Ca1Cu2Oy	Bi2Sr2Ca1Cu2Oy	Bi	2	Sr	2	Ca	1	Cu	2													O	y		1	1996																												Bi2212																		K		76.6					76.6																																																																						TP12203	m.ohm.cm											1.2			m3/C	0.0000000019				1.5				Bi,Sr,CuO,SrCO3,CaCO3	1	MIX(Bi,Sr,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12204	PR05300905		Bi2Sr2(Ca,Nd)Cu2Oy	Bi2Sr2Ca0.9Nd0.1Cu2Oy	Bi	2	Sr	2	Ca	0.9	Nd	0.1	Cu	2											O	y		1	1996																												Bi2212																		K		83.9					83.9																																																																						TP12204	m.ohm.cm											2.7			m3/C	0.0000000029				1.5				Bi,Nd,CuO,SrCO3,CaCO3	1	MIX(Bi,Nd,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12205	PR05300905		Bi2Sr2(Ca,Nd)Cu2Oy	Bi2Sr2Ca0.8Nd0.2Cu2Oy	Bi	2	Sr	2	Ca	0.8	Nd	0.2	Cu	2											O	y		1	1996																												Bi2212																		K		82.6					82.6																																																																						TP12205	m.ohm.cm											3			m3/C	0.0000000042				1.5				Bi,Nd,CuO,SrCO3,CaCO3	1	MIX(Bi,Nd,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12206	PR05300905		Bi2Sr2(Ca,Nd)Cu2Oy	Bi2Sr2Ca0.7Nd0.3Cu2Oy	Bi	2	Sr	2	Ca	0.7	Nd	0.3	Cu	2											O	y		1	1996																												Bi2212																		K		75.9					75.9																																																																						TP12206	m.ohm.cm											3.5			m3/C	0.0000000068				1.5				Bi,Nd,CuO,SrCO3,CaCO3	1	MIX(Bi,Nd,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12207	PR05300905		Bi2Sr2(Ca,Nd)Cu2Oy	Bi2Sr2Ca0.6Nd0.4Cu2Oy	Bi	2	Sr	2	Ca	0.6	Nd	0.4	Cu	2											O	y		1	1996																												Bi2212																		K		56					56																																																																						TP12207	m.ohm.cm											3.8			m3/C	0.0000000096				1.5				Bi,Nd,CuO,SrCO3,CaCO3	1	MIX(Bi,Nd,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12208	PR05300905		Bi2Sr2(Ca,Nd)Cu2Oy	Bi2Sr2Ca0.5Nd0.5Cu2Oy	Bi	2	Sr	2	Ca	0.5	Nd	0.5	Cu	2											O	y		1	1996																												Bi2212																		K		36					36																																																																						TP12208	m.ohm.cm											11.1			m3/C	0.0000000125				1.5				Bi,Nd,CuO,SrCO3,CaCO3	1	MIX(Bi,Nd,CuO,SrCO3,CaCO3)-CAL(750C,15h)-SIN(850C,40h)-SIN(860C,40h)					Scaling of the thermoelectric power in a wide enperature range in Bi2Sr2Ca1-xNdxCu2Oy (x=0-0.5): Experiment and interpretation	01		Physique des solides,Code Postale 233, Universite' Libre de Bruxelles, B-1050 Bruxelles, Belgium	Phys.Rev.B,53(1996)905	A. V. Kazanskiy,E. V. Vladimirskaya,N. V. Ageev,V. E. Gasumyants,V. I. Kaydanov,V. I. Smirnov	Bi, Sr, Ca, Nd, Cu, O	
12209	PR05300920		Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8	Pb	2	Sr	2	Y	1	Cu	3													O		8	1	1996																											3	Pb3212	Cmmm		A	5.394	5.434	15.725	4																																																																																																																PbO,CuO,SrCO3,Y2O3	1	MIX(PbO,CuO,SrCO3,Y2O3)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12210	PR05300920		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O		8	1	1996																											3	Pb3212	Cmmm		A	5.379	5.418	15.745	4																																																																																																																PbO,CuO,CaCO3,SrCO3,Y2O3	1	MIX(PbO,CuO,SrCO3,Y2O3)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12211	PR05300920		Pb2Sr2Ce1Cu3O8	Pb2Sr2Ce1Cu3O8	Pb	2	Sr	2	Ce	1	Cu	3													O		8	1	1996																											3	Pb3212	Cmmm		A	5.431	5.474	15.824	4																																																																																																																PbO,CuO,SrCO3,Ce2(C2O4)3+9H2O	1	MIX(PbO,CuO,SrCO3,Ce2(C2O4)3+9H2O)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12212	PR05300920		Pb2Sr2(Ce,Ca)Cu3O8	Pb2Sr2Ce0.5Ca0.5Cu3O8	Pb	2	Sr	2	Ce	0.5	Ca	0.5	Cu	3											O		8	1	1996																											3	Pb3212	Cmmm		A	5.407	5.449	15.759	4																																																																																																																PbO,CuO,CaCO3,SrCO3,Ce2(C2O4)3+9H2O	1	MIX(PbO,CuO,CaCO3,SrCO3,Ce2(C2O4)3+9H2O)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12213	PR05300920		Pb2Sr2Pr1Cu3O8	Pb2Sr2Pr1Cu3O8	Pb	2	Sr	2	Pr	1	Cu	3													O		8	1	1996																											3	Pb3212	Cmmm		A	5.445	5.484	15.798	4																																																																																																																PbO,CuO,SrCO3,Pr6O11	1	MIX(PbO,CuO,SrCO3,Pr6O11)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12214	PR05300920		Pb2Sr2(Pr,Ca)Cu3O8	Pb2Sr2Pr0.5Ca0.5Cu3O8	Pb	2	Sr	2	Pr	0.5	Ca	0.5	Cu	3											O		8	1	1996																											3	Pb3212	Cmmm		A	5.402	5.446	15.8	4																																																																																																																PbO,CuO,CaCO3,SrCO3,Pr6O11	1	MIX(PbO,CuO,CaCO3,SrCO3,Pr6O11)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12215	PR05300920		Pb2Sr2Tb1Cu3O8	Pb2Sr2Yb1Cu3O8	Pb	2	Sr	2	Yb	1	Cu	3													O		8	1	1996																											3	Pb3212	Cmmm		A	5.403	5.443	15.732	4																																																																																																																PbO,CuO,SrCO3,Yb4O7		MIX(PbO,CuO,SrCO3,Yb4O7)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12216	PR05300920		Pb2Sr2(Tb,Ca)Cu3O8	Pb2Sr2Tb0.5Ca0.5Cu3O8	Pb	2	Sr	2	Tb	0.5	Ca	0.5	Cu	3											O		8	1	1996																											3	Pb3212	Cmmm		A	5.389	5.43	15.765	4																																																																																																																(PbO,CuO,CaCO3,SrCO3,Yb4O7		MIX(PbO,CuO,CaCO3,SrCO3,Yb4O7)-PREFIRE(750C,2days)-SIN(750C,2days,under a N2 atmosphere)					Oxdation state of Ce in Pb2Sr2Ce1-xCaxCu3O8	01		Chemistry Dvision and Institute Pulsed Neutron Source, Argonne National Laboratory, Argonne, Illinois 60439-4814	Phys.Rev.B,53(1996)920	L. Soderholm,S. Skanthakumar	Pb, Sr, Ce, Ca, Cu, O	
12220	P071184510	sintered sample. hole conc(p) determined by s(290K) for various O-content. Tc(max) at p=0.164. pseudogap temp(T*) also measured.	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O7-z	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z		1	2005																												Y123																		K				84.6			84.6	TC12220																																																																																															standard solid state reaction					Anomalous pseudogap and superconducting-state properties of heavily disordered Y1-xCaxBa2(Cu1-yZny)3O7-z			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 71(2005)184510	J.L.Tallon,J.R.Cooper,R.S.Islam,S.H.Naqib		
12221	P071184510	sintered sample. hole conc(p) determined by s(290K) for various O-content. Tc(max) at p=0.162. pseudogap temp(T*) also measured.	(Y,Ca)Ba2(Cu,Zn)3O7	Y0.8Ca0.2Ba2Cu2.955Zn0.045O7-z	Y	0.8	Ca	0.2	Ba	2	Cu	2.955	Zn	0.045											O	7-z		1	2005																												Y123																		K				64.2			64.2																																																																																																standard solid state reaction					Anomalous pseudogap and superconducting-state properties of heavily disordered Y1-xCaxBa2(Cu1-yZny)3O7-z			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 71(2005)184510	J.L.Tallon,J.R.Cooper,R.S.Islam,S.H.Naqib		
12222	P071184510	sintered sample. hole conc(p) determined by s(290K) for various O-content. Tc(max) at p=0.163. pseudogap temp(T*) also measured.	(Y,Ca)Ba2(Cu,Zn)3O7	Y0.8Ca0.2Ba2Cu2.91Zn0.09O7-z	Y	0.8	Ca	0.2	Ba	2	Cu	2.91	Zn	0.09											O	7-z		1	2005																												Y123																		K				51.4			51.4	TC12222																																																																																															standard solid state reaction					Anomalous pseudogap and superconducting-state properties of heavily disordered Y1-xCaxBa2(Cu1-yZny)3O7-z			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 71(2005)184510	J.L.Tallon,J.R.Cooper,R.S.Islam,S.H.Naqib		
12223	P071184510	sintered sample. hole conc(p) determined by s(290K) for various O-content. Tc(max) at p=0.171. pseudogap temp(T*) also measured.	(Y,Ca)Ba2(Cu,Zn)3O7	Y0.8Ca0.2Ba2Cu2.82Zn0.18O7-z	Y	0.8	Ca	0.2	Ba	2	Cu	2.82	Zn	0.18											O	7-z		1	2005																												Y123																		K				27.6			27.6																																																																																																standard solid state reaction					Anomalous pseudogap and superconducting-state properties of heavily disordered Y1-xCaxBa2(Cu1-yZny)3O7-z			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 71(2005)184510	J.L.Tallon,J.R.Cooper,R.S.Islam,S.H.Naqib		
12224	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	7-z	6.5	3	2005																												Y123																		K		53					53																																									micron-m	plasma frequency			7.8																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12225	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	7-z	6.6	3	2005																												Y123																		K		58					58																																									micron-m	plasma frequency			6.52																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12226	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	7-z	6.7	3	2005																												Y123																		K		63					63																																									micron-m	plasma frequency			5.05																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12227	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	3	2005																												Y123																		K		78					78																																									micron-m	plasma frequency			3.42																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12228	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	7-z	6.85	3	2005																												Y123																		K		89					89																																									micron-m	plasma frequency			2.01																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12229	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-z	6.9	3	2005																												Y123																		K		91.6					91.6																																									micron-m	plasma frequency			1.59																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12230	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-z	6.95	3	2005																												Y123																		K		93.2					93.2																																									micron-m	plasma frequency			1.01																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12231	P071184515	twinned single crystal. c-axis optical conductivity measured.	YBa2Cu3Oz	Y1Ba2Cu3O6.99	Y	1	Ba	2	Cu	3															O	7-z	6.99	3	2005																												Y123																		K		90					90																																									micron-m	plasma frequency			0.77																																																			crystals were grown by a flux method using YSZ.					Coherence, incoherence, and scaling along the c axis of YBa2Cu3O6+x			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 71(2005)184515	C.C.Homes,D.A.Bonn,Ruixing Liang,S.V.Dordevic,T.Timusk,W.N.Hardy		
12232	PHC2590036		(Hg,Tl)2Ba2YCu2O8	Hg1Tl1Ba2Y1Cu2O8-z	Hg	1	Tl	1	Ba	2	Y	1	Cu	2											O	8-z			1996																												Hg2212																		K					4.2																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12233	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1Tl1Ba2Y0.7Ca0.3Cu2O8-z	Hg	1	Tl	1	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	8-z			1996																												Hg2212																		K					4.2																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12234	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1Tl1Ba2Y0.4Ca0.6Cu2O8-z	Hg	1	Tl	1	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	8-z			1996																												Hg2212																		K					4.2																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12235	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1Tl1Ba2Ca1Cu2O8-z	Hg	1	Tl	1	Ba	2	Ca	1	Cu	2											O	8-z			1996																												Hg2212																		K				53			53																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12236	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg0.5Tl1.5Ba2Y0.4Ca0.6Cu2O8-z	Hg	0.5	Tl	1.5	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	8-z			1996																												Hg2212																		K					4.2																																																																																																	1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12237	PHC2590036		(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg0.5Tl1.5Ba2Ca1Cu2O8-z	Hg	0.5	Tl	1.5	Ba	2	Ca	1	Cu	2											O	8-z			1996																												Hg2212																		K				80			80																																																																																															1	materials were prepared by adding HgO,Tl2O3 to a precursor					Effect of Tl doping on the phase stability of Hg2Ba2(Y,Ca)1Cu2O8-z suoerconducters prepared by a high-pressure technique			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Physica C,259(1996)36-42	Ayako Tokiwa-Yamamoto,Keiichi Tanabe,Seiji Adachi,Tadashi Tatsuki,Xiao-Jing Wu		
12238	PHC4220088		(Fe,Cu)BaSrYbCu2O7	Fe0.5Ba1Sr1Yb1Cu2.5O7.432	Fe	0.5	Ba	1	Sr	1	Yb	1	Cu	2.5											O	7+z	7.432	1	2005																												Cu1212			A	3.8242		11.4721												K				29.7			29.7																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12239	PHC4220088		(Fe,Cu)BaSrTmCu2O7	Fe0.5Ba1Sr1Tm1Cu2.5O7.432	Fe	0.5	Ba	1	Sr	1	Tm	1	Cu	2.5											O	7+z	7.432	1	2005																												Cu1212			A	3.8298		11.4809												K				40			40																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12240	PHC4220088		(Fe,Cu)BaSrErCu2O7	Fe0.5Ba1Sr1Er1Cu2.5O7.439	Fe	0.5	Ba	1	Sr	1	Er	1	Cu	2.5											O	7+z	7.439	1	2005																												Cu1212			A	3.8322		11.4826												K				47.8			47.8																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12241	PHC4220088		(Fe,Cu)BaSrYCu2O7	Fe0.5Ba1Sr1Y1Cu2.5O7.424	Fe	0.5	Ba	1	Sr	1	Y	1	Cu	2.5											O	7+z	7.424	1	2005																												Cu1212			A	3.8325		11.4826												K				52.5			52.5																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12242	PHC4220088		(Fe,Cu)BaSrHoCu2O7	Fe0.5Ba1Sr1Ho1Cu2.5O7.462	Fe	0.5	Ba	1	Sr	1	Ho	1	Cu	2.5											O	7+z	7.462	1	2005																												Cu1212			A	3.8346		11.4932												K				45.2			45.2																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12243	PHC4220088		(Fe,Cu)BaSrDyCu2O7	Fe0.5Ba1Sr1Dy1Cu2.5O7.447	Fe	0.5	Ba	1	Sr	1	Dy	1	Cu	2.5											O	7+z	7.447	1	2005																												Cu1212			A	3.8411		11.4976												K				37.9			37.9																																																																																																(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12244	PHC4220088		(Fe,Cu)BaSrGdCu2O7	Fe0.5Ba1Sr1Gd1Cu2.5O7.432	Fe	0.5	Ba	1	Sr	1	Gd	1	Cu	2.5											O	7+z	7.432	1	2005																												Cu1212			A	3.8521		11.525												K					4.2																																																																																																		(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12245	PHC4220088		(Fe,Cu)BaSrEuCu2O7	Fe0.5Ba1Sr1Eu1Cu2.5O7.462	Fe	0.5	Ba	1	Sr	1	Eu	1	Cu	2.5											O	7+z	7.462	1	2005																												Cu1212			A	3.8536		11.5356												K					4.2																																																																																																		(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12246	PHC4220088		(Fe,Cu)BaSrSmCu2O7	Fe0.5Ba1Sr1Sm1Cu2.5O7.492	Fe	0.5	Ba	1	Sr	1	Sm	1	Cu	2.5											O	7+z	7.492	1	2005																												Cu1212			A	3.8596		11.5479												K					4.2																																																																																																		(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12247	PHC4220088		(Fe,Cu)BaSrNdCu2O7	Fe0.5Ba1Sr1Nd1Cu2.5O7.499	Fe	0.5	Ba	1	Sr	1	Nd	1	Cu	2.5											O	7+z	7.499	1	2005																												Cu1212																		K					4.2																																																																																																		(sintering sample) - mixed with 5wt% KClO4 - pellet - wrapped in Au-foil - high pressure synthesis(100C,0.5h, 6GPa) - q to RT					Synthesis and superconductivity of Fe0.5Cu0.5BaSrRCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, PR China	Physica C, 422(2005)88	G.C.Che,K.Q.Li,Y.H.Liu,Z.X.Zhao		
12248	PHC4220102	Cu-valence = 2.02	(Hg,Fe)Sr2YCu2O7	Hg0.5Fe0.5Sr2Y1Cu2O6.77	Hg	0.5	Fe	0.5	Sr	2	Y	1	Cu	2											O	7-z	6.77		2005																												Hg1212			A	3.8348		11.8133												K																																																																																																							precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12249	PHC4220102	Cu-valence = 2.05	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.9Ca0.1Cu2O6.75	Hg	0.5	Fe	0.5	Sr	2	Y	0.9	Ca	0.1	Cu	2									O	7-z	6.75		2005																												Hg1212			A	3.8326		11.8242												K																																																																																																							precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12250	PHC4220102	Cu-valence = 2.07	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.8Ca0.2Cu2O6.72	Hg	0.5	Fe	0.5	Sr	2	Y	0.8	Ca	0.2	Cu	2									O	7-z	6.72		2005																												Hg1212			A	3.8299		11.8327												K			30				30																																																																																																precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12251	PHC4220102	Cu-valence = 2.10	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.7Ca0.3Cu2O6.7	Hg	0.5	Fe	0.5	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7-z	6.7		2005																												Hg1212			A	3.8267		11.844												K	18		30				24										16																																																								uV/K	66.4			TP12251																										precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12252	PHC4220102	Cu-valence = 2.15	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.6Ca0.4Cu2O6.7	Hg	0.5	Fe	0.5	Sr	2	Y	0.6	Ca	0.4	Cu	2									O	7-z	6.7		2005																												Hg1212			A	3.8249		11.8538												K	37		55				46										24																																																								uV/K	42.2			TP12252																										precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12253	PHC4220102	Cu-valence = 2.18	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.5Ca0.5Cu2O6.68	Hg	0.5	Fe	0.5	Sr	2	Y	0.5	Ca	0.5	Cu	2									O	7-z	6.68		2005																												Hg1212			A	3.8222		11.8655												K	61		72				66.5										35																																																								uV/K	19.5			TP12253																										precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12254	PHC4220102	Cu-valence = 2.22	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.4Ca0.6Cu2O6.67	Hg	0.5	Fe	0.5	Sr	2	Y	0.4	Ca	0.6	Cu	2									O	7-z	6.67		2005																												Hg1212			A	3.8196		11.8772												K	73		82				77.5										38																																																								uV/K	2.8			TP12254																										precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12255	PHC4220102	Cu-valence = 2.25	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.3Ca0.7Cu2O6.65	Hg	0.5	Fe	0.5	Sr	2	Y	0.3	Ca	0.7	Cu	2									O	7-z	6.65		2005																												Hg1212			A	3.8174		11.8864												K	68		77				72.5										51																																																								uV/K	-5.9			TP12255																										precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12256	PHC4220102	Cu-valence = 2.26	(Hg,Fe)Sr2(Y,Ca)Cu2O7	Hg0.5Fe0.5Sr2Y0.2Ca0.8Cu2O6.63	Hg	0.5	Fe	0.5	Sr	2	Y	0.2	Ca	0.8	Cu	2									O	7-z	6.63		2005																												Hg1212			A	3.8174		11.8861												K	58		69				63.5										44																																																								uV/K	-6																													precursor(Sr-Y-Ca-Cu-O) using gel process. addition of (HgO+Fe2O3) - pellet - heat(900C,10h, in air) - FC to RT					Synthesis, structural and transport properties of (Hg,Fe)-1212 superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 422(2005)102	Elsayed Kandyel		
12257	P072024533	ANN(400C,72h,in 2atm O2). p = 0.43 /Cu, estimated from ARPES. overdoped.	(Bi,Pb)2Sr2CuO6	Bi1.74Pb0.38Sr1.88Cu1O6+z	Bi	1.74	Pb	0.38	Sr	1.88	Cu	1													O	6+z		3	2005																												Bi2201																		K					2																																																																				uV/K	-17.1			TP12257																										single crystals were grown by floating zone method					Contribution of electronic structure to thermoelectric power in (Bi,Pb)2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	Phys.Rev.B, 72(2005)024533	S.Shin,S.Tsuda,T.Kondo,T.Takeuchi,T.Yokoya,U.Mizutani		
12258	P072024533	ANN(750C, 24h, in 1atm air). p = 0.40] /Cu, estimated from ARPES. overdoped.	(Bi,Pb)2Sr2CuO6	Bi1.74Pb0.38Sr1.88Cu1O6+z	Bi	1.74	Pb	0.38	Sr	1.88	Cu	1													O	6+z		3	2005																												Bi2201																		K		7					7																																																																		uV/K	-15.3			TP12258																										single crystals were grown by floating zone method					Contribution of electronic structure to thermoelectric power in (Bi,Pb)2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	Phys.Rev.B, 72(2005)024533	S.Shin,S.Tsuda,T.Kondo,T.Takeuchi,T.Yokoya,U.Mizutani		
12259	P072024533	ANN(650C, 24h, in vac). p = 0.35 /Cu, estimated from ARPES. overdoped.	(Bi,Pb)2Sr2CuO6	Bi1.74Pb0.38Sr1.88Cu1O6+z	Bi	1.74	Pb	0.38	Sr	1.88	Cu	1													O	6+z		3	2005																												Bi2201																		K		21					21																																																																		uV/K	-10.5			TP12259																										single crystals were grown by floating zone method					Contribution of electronic structure to thermoelectric power in (Bi,Pb)2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	Phys.Rev.B, 72(2005)024533	S.Shin,S.Tsuda,T.Kondo,T.Takeuchi,T.Yokoya,U.Mizutani		
12260	P072024533	ANN(650C, 24h, in Ar flow). p = 0.28 /Cu, estimated from ARPES. optimal-doped.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.35Pb0.85Sr1.47La0.38Cu1O6+z	Bi	1.35	Pb	0.85	Sr	1.47	La	0.38	Cu	1											O	6+z		3	2005																												Bi2201																		K		35					35																																																																		uV/K	-0.84			TP12260																										single crystals were grown by floating zone method					Contribution of electronic structure to thermoelectric power in (Bi,Pb)2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	Phys.Rev.B, 72(2005)024533	S.Shin,S.Tsuda,T.Kondo,T.Takeuchi,T.Yokoya,U.Mizutani		
12261	P072024533	ANN(650C, 24h, in Ar flow). p = 0.25 /Cu, estimated from ARPES. underdoped.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.35Pb0.85Sr1.4La0.45Cu1O6+z	Bi	1.35	Pb	0.85	Sr	1.4	La	0.45	Cu	1											O	6+z		3	2005																												Bi2201																		K		27					27																																																																		uV/K	5.99			TP12261																										single crystals were grown by floating zone method					Contribution of electronic structure to thermoelectric power in (Bi,Pb)2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	Phys.Rev.B, 72(2005)024533	S.Shin,S.Tsuda,T.Kondo,T.Takeuchi,T.Yokoya,U.Mizutani		
12262	JJP0324517	Tc depends on the ratio(P) of sample/KCl3 during synthesizing. Tc(max)=50K obtained for P=10. 	(Cu,Mo)Sr2(Y,Ce)2Cu2Oz	Mo0.2Sr2Y1.2Ce0.8Cu2.8Oz	Mo	0.2	Sr	2	Y	1.2	Ce	0.8	Cu	2.8											O	z			1993																												Cu1222			A	3.814		28.34												K				50			50																																																																																														Y2O3,CeO2,MoO3,CuO,SrCO3	1	mixture - heat(850C, in air) - CAL(1010-1025C,6h) - ANN(1000C,6h, P=1.5-2.0 GPa with KClO3.					High-pressure synthesis of Mo-containing 1212 and 1222 compounds, (Cu,Mo)Sr2YCu2Oz and (Cu,Mo)Sr2(Y,Ce)2Cu2Oz			National Institute for Research in Inorganic Materials, Namiki, Tsukuba, Ibaraki, Japan	Jpn.J.Appl.Phys., 32(1993)4517	A.Ono		
12263	JJP0324517		(Cu,Mo)Sr2(Y,Ce)2Cu2Oz	Mo0.3Sr2Y1.2Ce0.8Cu2.7Oz	Mo	0.3	Sr	2	Y	1.2	Ce	0.8	Cu	2.7											O	z			1993																												Cu1222			A	3.82		28.344												K				45			45																																																																																														Y2O3,CeO2,MoO3,CuO,SrCO3	1	mixture - heat(850C, in air) - CAL(1010-1025C,6h) - ANN(1000C,6h, P=1.5-2.0 GPa with KClO3.					High-pressure synthesis of Mo-containing 1212 and 1222 compounds, (Cu,Mo)Sr2YCu2Oz and (Cu,Mo)Sr2(Y,Ce)2Cu2Oz			National Institute for Research in Inorganic Materials, Namiki, Tsukuba, Ibaraki, Japan	Jpn.J.Appl.Phys., 32(1993)4517	A.Ono		
12264	JJP0324517	Tc and lat-C depend on O-content	(Cu,Mo)Sr2YCu2Oz	Mo0.2Sr2Y1Cu2.8Oz	Mo	0.2	Sr	2	Y	1	Cu	2.8													O	z			1993																												Cu1212																		K				72			72	TC12264																																																																																													Y2O3,CeO2,MoO3,CuO,SrCO3	1	mixture - heat(850C, in air) - CAL(1010-1025C,6h) - ANN(1000C,6h, P=1.5-2.0 GPa with KClO3.					High-pressure synthesis of Mo-containing 1212 and 1222 compounds, (Cu,Mo)Sr2YCu2Oz and (Cu,Mo)Sr2(Y,Ce)2Cu2Oz			National Institute for Research in Inorganic Materials, Namiki, Tsukuba, Ibaraki, Japan	Jpn.J.Appl.Phys., 32(1993)4517	A.Ono		
12265	P072012501		(Cu,Mo)Sr2(Ce,Yb)3Cu2O11+z	Mo0.25Sr2Ce2.01Yb0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Yb	0.99	Cu	2.75											O	11+z			2005																												Cu1232	P4/mmm		A	3.8179		16.89												K				36.8			36.8																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12266	P072012501		(Cu,Mo)Sr2(Ce,Ho)3Cu2O11+z	Mo0.25Sr2Ce2.01Ho0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Ho	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8307		16.922												K				51.4			51.4																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12267	P072012501		(Cu,Mo)Sr2(Ce,Y)3Cu2O11+z	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8293		16.917												K				53			53																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12268	P072012501		(Cu,Mo)Sr2(Ce,Dy)3Cu2O11+z	Mo0.25Sr2Ce2.01Dy0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Dy	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8327		16.931												K				48.6			48.6																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12269	P072012501	not SC	(Cu,Mo)Sr2(Ce,Tb)3Cu2O11+z	Mo0.25Sr2Ce2.01Tb0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Tb	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8315		16.872												K																																																																																																					CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12270	P072012501		(Cu,Mo)Sr2(Ce,Gd)3Cu2O11+z	Mo0.25Sr2Ce2.01Gd0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Gd	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8428		16.946												K				47.3			47.3																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12271	P072012501		(Cu,Mo)Sr2(Ce,Eu)3Cu2O11+z	Mo0.25Sr2Ce2.01Eu0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Eu	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8436		16.949												K				37.1			37.1																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12272	P072012501		(Cu,Mo)Sr2(Ce,Nd)3Cu2O11+z	Mo0.25Sr2Ce2.01Nd0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Nd	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.857		16.993												K				31.7			31.7																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12273	P072012501	not SC	(Cu,Mo)Sr2(Ce,Pr)3Cu2O11+z	Mo0.25Sr2Ce2.01Pr0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Pr	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.855		16.914												K																																																																																																					CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12274	P072012501		(Cu,Mo)Sr2(Ce,La)3Cu2O11+z	Mo0.25Sr2Ce2.01La0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	La	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.8743		17.052												K				25.8			25.8																																																																																														CuO,MoO3,SrCO3,CeO2,RO3(Tb4O7,Pr6O11)	1	mixture - CAL(950,in air) - SIN(1020C, in air) - ANN(500C,30min, 5GPa-O2 using Ag2O2)					Chemical control of high-Tc superconductivity of the triple-fluorite-layer copper oxide (Cu,Mo)Sr2(Ce,R)3Cu2O11+z (R=Y,La-Yb)			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 72(2005)012501	H.Yamauchi,J.M.Chen,M.Karppinen,R.S.Liu,Y.Morita		
12275	JPS0741682	beta-pyrochlore. RRR > 100. gamma estimated from (dC/Tc) = 92.7 mJ/mol-Os.K2 assuming  (dTc/gamma*Tc)=1.43. unknown peak in SP-heat at 7.4 K.	KOsO6	K1Os2O6	K	1	Os	2																	O	6		3	2005																												pyrochlore																		K	9.53					0.1	9.53																													T/K	resistivity	4.3																									mJ/mol.K2	64.8	SP-heat																																						KOsO4 firstly prepared from K2O and Os. (KOsO4+Os+AgO) - heat(673K in sealed quartz tube.					Second Anomaly in the Specific Heat of beta-Pyrochlore Oxide Superconductor KOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 74(2005)1682	J.Yamaura,S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
12276	PHC4230119	94%Bi2223+6%Bi2212	(Bi,Sr)2Sr2Ca2Cu3Oz	Bi1.6Pb0.4Sr2Ca2Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	z		2	2005																												Bi2223			A	5.431		37.236												K	106.8						106.8																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12277	PHC4230119	92%Bi2223+8%Bi2212	(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.9995Sm0.0005Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.9995	Sm	0.0005	Cu	3									O	z		2	2005																												Bi2223			A	5.416		37.206												K	102						102																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12278	PHC4230119	83%Bi2223+17%Bi2212	(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.999Sm0.001Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.999	Sm	0.001	Cu	3									O	z		2	2005																												Bi2223			A	5.418		37.197												K	97.1						97.1																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12279	PHC4230119	79%Bi2223+21%Bi2212	(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.995Sm0.005Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.995	Sm	0.005	Cu	3									O	z		2	2005																												Bi2223			A	5.421		37.19												K	93.3						93.3																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12280	PHC4230119	74%Bi2223+26%Bi2212	(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.99Sm0.01Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.99	Sm	0.01	Cu	3									O	z		2	2005																												Bi2223			A	5.424		37.181												K	84.8						84.8																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12281	PHC4230119		(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.9Sm0.1Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.9	Sm	0.1	Cu	3									O	z		1	2005																												Bi2212			A	5.431		30.741												K	70						70																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12282	PHC4230119		(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1.5Sm0.5Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1.5	Sm	0.5	Cu	3									O	z		1	2005																												Bi2212			A	5.443		30.651												K	28						28																																																																																														Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12283	PHC4230119		(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1Sm1Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1	Sm	1	Cu	3									O	z		1	2005																												Bi2212			A	5.464		30.323												K					21																																																																																																Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12284	PHC4230119		(Bi,Sr)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca0.5Sm1.5Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	0.5	Sm	1.5	Cu	3									O	z		1	2005																												Bi2212			A	5.468		30.278												K					21																																																																																																Bi2O3,PbO,SrCO3,CaO,Sm2O3,CuO		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Structural and physical properties of Sm-doped Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			 Department of Physics, Faculty of Arts and Sciences, Abant Izzet Baysal University, 14280 Bolu, Turkey	Physica C, 423(2005)119	C.Terzioglu,E.Yanmaz,M.Yilmazlar,O.Ozturk		
12285	P072014504	hole conc = 0.22. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.95Sr1.92La0.1Cu1.03O6+z	Bi	1.95	Sr	1.92	La	0.1	Cu	1.03													O	6+z		1	2005																												Bi2201																		K				8.5			8.5																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12286	P072014504	hole conc = 0.20. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi2.02Sr1.82La0.15Cu1.02O6+z	Bi	2.02	Sr	1.82	La	0.15	Cu	1.02													O	6+z		1	2005																												Bi2201																		K				11			11																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12287	P072014504	hole conc = 0.19. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.93Sr1.85La0.23Cu0.99O6+z	Bi	1.93	Sr	1.85	La	0.23	Cu	0.99													O	6+z		1	2005																												Bi2201																		K				15			15																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12288	P072014504	hole conc = 0.17. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.96Sr1.66La0.31Cu1.01O6+z	Bi	1.96	Sr	1.66	La	0.31	Cu	1.01													O	6+z		1	2005																												Bi2201																		K				17			17																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12289	P072014504	hole conc = 0.17. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.99Sr1.66La0.33Cu1.01O6+z	Bi	1.99	Sr	1.66	La	0.33	Cu	1.01													O	6+z		1	2005																												Bi2201																		K				18.5			18.5																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12290	P072014504	hole conc = 0.19. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.91Sr1.69La0.4Cu0.98O6+z	Bi	1.91	Sr	1.69	La	0.4	Cu	0.98													O	6+z		1	2005																												Bi2201																		K				16			16																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12291	P072014504	hole conc = 0.15. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.97Sr1.56La0.45Cu1.02O6+z	Bi	1.97	Sr	1.56	La	0.45	Cu	1.02													O	6+z		1	2005																												Bi2201																		K				13			13																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12292	P072014504	hole conc = 0.12. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.97Sr1.44La0.56Cu1.04O6+z	Bi	1.97	Sr	1.44	La	0.56	Cu	1.04													O	6+z		1	2005																												Bi2201																		K				8			8																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12293	P072014504	hole conc = 0.07. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2(Sr,La)2CuO6	Bi1.98Sr1.21La0.78Cu1.03O6+z	Bi	1.98	Sr	1.21	La	0.78	Cu	1.03													O	6+z		1	2005																												Bi2201																		K					4																																																																																																Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12294	P072014504	hole conc = 0.19. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	Bi2Sr2CuO6	Bi2.03Sr1.72Cu1.25O6+z	Bi	2.03	Sr	1.72	Cu	1.25															O	6+z		1	2005																												Bi2201																		K				6			6																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12300	PR05315245		YbBa2Cu3O7	Yb1Ba2Cu3O7-y	Yb	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.877	3.801	11.646	3											K		91.3				1.5	91.3			K/GPa																																																																																											R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12301	PR05315245		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.99Zn0.01O7-y	Yb	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.869	3.801	11.656	3													87.8					87.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12302	PR05315245		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.98Zn0.02O7-y	Yb	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.875	3.803	11.651	3											K		83.3				2.6	83.3																																																																							m.ohm.cm											0.85												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12303	PR05315245		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.96Zn0.04O7-y	Yb	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.881	3.808	11.656	3													73.9				3.6	73.9																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12304	PR05315245		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.94Zn0.06O7-y	Yb	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.882	3.805	11.654	3													72.1				4.2	72.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12305	PR05315245		YbBa2(Cu,Zn)3O7	Yb1Ba2Cu2.92Zn0.08O7-y	Yb	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.879	3.809	11.66	3											K		70.6				3.5	70.6																																																																							m.ohm.cm											1.284												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12306	PR05315245		ErBa2Cu3O7	Er1Ba2Cu3O7-y	Er	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.878	3.809	11.655	3											K		93.1				0.4	93.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12307	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.99Zn0.01O7-y	Er	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.879	3.808	11.659	3											K		89.8					89.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12308	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.98Zn0.02O7-y	Er	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.876	3.805	11.647	3											K		84.8				1.5	84.8																																																																							m.ohm.cm											0.807												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12309	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.96Zn0.04O7-y	Er	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.876	3.808	11.652	3											K		76.3				2.4	76.3																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12310	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.94Zn0.06O7-y	Er	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.88	3.809	11.649	3											K		68.3				2.1	68.3																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12311	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.92Zn0.08O7-y	Er	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.876	3.807	11.65	3											K		62.7				2.2	62.7																																																																							m.ohm.cm											0.983												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12312	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.9Zn0.1O7-y	Er	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.877	3.808	11.65	3											K		60.4				3.7	60.4																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12313	PR05315245		ErBa2(Cu,Zn)3O7	Er1Ba2Cu2.85Zn0.15O7-y	Er	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.879	3.808	11.659	3											K		52.4				3.7	52.4																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12314	PR05315245		YBa2Cu3O7	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.886	3.818	11.669	3											K		93.4				0.4	93.4																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12315	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.99Zn0.01O7-y	Y	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.886	3.818	11.665	3											K		88.6					88.6																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12316	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.98Zn0.02O7-y	Y	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.888	3.82	11.665	3											K		84.8				1.7	84.8																																																																							m.ohm.cm											0.781												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12317	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.96Zn0.04O7-y	Y	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.886	3.817	11.664	3											K		75.1				2.6	75.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12318	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O7-y	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.886	3.817	11.063	3											K		69.2				2.7	69.2																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12319	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.92Zn0.08O7-y	Y	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.886	3.817	11.666	3											K		62.1				2.8	62.1																																																																							m.ohm.cm											1.06												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12320	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9Zn0.1O7-y	Y	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.886	3.818	11.667	3											K		60.1				3.9	60.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12321	PR05315245		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.85Zn0.15O7-y	Y	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.887	3.818	11.666	3											K		55.1				2.8	55.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12322	PR05315245		DyBa2Cu3O7	Dy1Ba2Cu3O7-y	Dy	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.894	3.836	11.684	3											K		95.1				2.4	95.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12323	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.99Zn0.01O7-y	Dy	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.889	3.826	11.673	3											K		89.5					89.5																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12324	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.98Zn0.02O7-y	Dy	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.895	3.829	11.672	3											K		84.8				3	84.8																																																																							m.ohm.cm											0.887												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12325	PR05315245		DyBa2(CuZ,n)3O7	Dy1Ba2Cu2.96Zn0.04O7-y	Dy	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.887	3.821	11.674	3											K		76.8				3.2	76.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12326	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.94Zn0.06O7-y	Dy	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.886	3.823	11.677	3											K		68.8				3.1	68.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12327	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.92Zn0.08O7-y	Dy	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.885	3.821	11.68	3											K		60.6				3.1	60.6																																																																							m.ohm.cm											1.108												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12328	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.9Zn0.1O7-y	Dy	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.887	3.822	11.676	3											K		56.3				4	56.3																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12329	PR05315245		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.85Zn0.15O7-y	Dy	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.887	3.829	11.699	3											K		51.5				4.5	51.5																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12330	PR05315245		GdBa2Cu3O7	Gd1Ba2Cu3O7-y	Gd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.898	3.838	11.703	3											K		94.8				1.5	94.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12331	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.99Zn0.01O7-y	Gd	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.906	3.842	11.703	3											K		89.8					89.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12332	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.98Zn0.02O7-y	Gd	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.908	3.847	11.716	3											K		86.3				3	86.3																																																																							m.ohm.cm											0.956												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12333	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.96Zn0.04O7-y	Gd	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.909	3.844	11.717	3											K		72.7				4.5	72.7																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12334	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.94Zn0.06O7-y	Gd	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.908	3.845	11.722	3											K		65.9				8	65.9																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12335	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.92Zn0.08O7-y	Gd	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.907	3.847	11.722	3											K		55.9				8.3	55.9																																																																							m.ohm.cm											1.224												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12336	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.9Zn0.1O7-y	Gd	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.909	3.844	11.722	3											K		49.2				8.9	49.2																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12337	PR05315245		GdBa2(Cu,Zn)3O7	Gd1Ba2Cu2.85Zn0.15O7-y	Gd	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.909	3.847	11.727	3											K		42.4				9.6	42.4																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12338	PR05315245		EuBa2Cu3O7	Eu1Ba2Cu3O7-y	Eu	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.897	3.84	11.709	3											K		94.5				3	94.5																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12339	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.99Zn0.01O7-y	Eu	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.892	3.834	11.714	3											K		91.3					91.3																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12340	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.98Zn0.02O7-y	Eu	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.898	3.839	11.718	3											K		86.3				4.3	86.3																																																																							m.ohm.cm											1.355												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12341	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.96Zn0.04O7-y	Eu	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.899	3.839	11.716	3											K		74.8				8	74.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12342	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.94Zn0.06O7-y	Eu	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.9	3.84	11.716	3											K		65.9				11.1	65.9																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12343	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.92Zn0.08O7-y	Eu	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.902	3.843	11.717	3											K		54.1				13.2	54.1																																																																							m.ohm.cm											1.602												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12344	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.9Zn0.1O7-y	Eu	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.896	3.839	11.717	3											K		47.4				14.2	47.4																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12345	PR05315245		EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.85Zn0.15O7-y	Eu	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.9	3.84	11.719	3											K		33.6				14.5	33.6																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12346	PR05315245		SmBa2Cu3O7	Sm1Ba2Cu3O7-y	Sm	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.903	3.849	11.732	3											K		95.1				2	95.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12347	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.99Zn0.01O7-y	Sm	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.905	3.849	11.737	3											K		91.3					91.3																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12348	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.98Zn0.02O7-y	Sm	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.906	3.848	11.736	3											K		86.3				5.9	86.3																																																																							m.ohm.cm											1.709												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12349	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.96Zn0.04O7-y	Sm	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.906	3.851	11.733	3											K		74.5				6.8	74.5																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12350	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.94Zn0.06O7-y	Sm	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.907	3.85	11.736	3											K		65.6				8.7	65.6																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12351	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.92Zn0.08O7-y	Sm	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.903	3.848	11.737	3											K		52.1				12	52.1																																																																							m.ohm.cm											1.86												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12352	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.9Zn0.1O7-y	Sm	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.909	3.853	11.737	3											K		43.6				17.4	43.6																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12353	PR05315245		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.85Zn0.15O7-y	Sm	1	Ba	2	Cu	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.913	3.856	11.735	3											K		31.8				18.6	31.8																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12354	PR05315245		NdBa2Cu3O7	Nd1Ba2Cu3O7-y	Nd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.918	3.861	11.773	3											K		95.1				2.4	95.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12355	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.99Zn0.01O7-y	Nd	1	Ba	2	Cu	2.99	Zn	0.01													O	7-y		1	1996																											3	Y123			A	3.913	3.863	11.774	3											K		94.5					94.5																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12356	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.98Zn0.02O7-y	Nd	1	Ba	2	Cu	2.98	Zn	0.02													O	7-y		1	1996																											3	Y123			A	3.915	3.86	11.774	3											K		86				10.3	86																																																																							m.ohm.cm											4.464												R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12357	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.96Zn0.04O7-y	Nd	1	Ba	2	Cu	2.96	Zn	0.04													O	7-y		1	1996																											3	Y123			A	3.917	3.862	11.779	3											K		72.7				10.8	72.7																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12358	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.94Zn0.06O7-y	Nd	1	Ba	2	Cu	2.94	Zn	0.06													O	7-y		1	1996																											3	Y123			A	3.91	3.86	11.77	3											K		64.1				17.6	64.1																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12359	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.92Zn0.08O7-y	Nd	1	Ba	2	Cu	2.92	Zn	0.08													O	7-y		1	1996																											3	Y123			A	3.915	3.857	11.788	3											K		36.6				24.7	36.6																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12360	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cu2.9Zn0.1O7-y	Nd	1	Ba	2	Cu	2.9	Zn	0.1													O	7-y		1	1996																											3	Y123			A	3.916	3.859	11.78	3											K		25				26.4	25																																																																																														R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12361	PR05315245		NdBa2(Cu,Zn)3O7	Nd1Ba2Cy2.85Zn0.15O7-y	Nd	1	Ba	2	Cy	2.85	Zn	0.15													O	7-y		1	1996																											3	Y123			A	3.917	3.859	11.773	3																																																																																																																R2O3,BaCO3,CuO,ZnO	1	R=Yb,Er,Y,Dy,Gd,Eu,Sm,NdMIX(R2O3,BaCO3,CuO,ZnO)-Calcine(915C,24h)-Reground-Press(4kbar,5*30*1mm^3)-SIN(925-930C(except R=Yb at 920C),72h in Oxygen flow)-ANN(680C,10h)-ANN(400C,10h)-Cool(10h in Oxygen					Rare-earth ion size effect on resistivity, susceptibility, and superconductivity of RBa2Cu3-xZnxO7-y (R=Yb, Er, Y, Dy, Gd, Eu, Sm, and Nd)	06		"Institut F""ur Schicht-und Ionentechnik, forschungszentrum Ju""lich Gesellschaft mit beschra""nkter Haftung,Postfach 1913,D-53425 Ju""lich Germay"	Phys.Rev.53,(1996)15245	"M.G. Berger,O. Glu""ck,S.S. Ata-Allah,Yunhui Xu"	R, Ba, Cu, Zn, O	
12362	PR05315272		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1996																												Bi2212							3											K				93			93																																				nm				0.8	nm			180																																																		Bi2O3,Sr(OH)2*8H2O,CaCO3,CuO	9	mix(Bi2O3,Sr(OH)2*8H2O,CaCO3,CuO)-sin(780C in alumina crucible)-sin(840C 12h)-transfered to a rotary conical gold crucible-heated to 980C-hold(2h)-cooled to 870C(0.67C/h)-cooled to 600C(25C/h)					Thermal fluctuation effects on the magnetization above and below the superconducting transition in Bi2Sr2CaCu2O8 in the weak magnetic field limit	199606		Laboratorio de Fisica de Materiales, Facultad de Fisica, Universidad de Compostela, 15706 Spain	Phys.Rev.B,53(1996)15272	C. Torro'n,E.G. Miramontes,Fe'lix Vidal,I. Rasines,J. Mosqueira,J.A. Campa		
12363	PR05315272		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1996																												Bi2212																		K				99			99																																				nm				1	nm			170																																																		Bi2O3,Sr(OH)2*8H2O,CaCO3,CuO	9	mix(Bi2O3,Sr(OH)2*8H2O,CaCO3,CuO)-sin(780C in alumina crucible)-sin(840C 12h)-transfered to a rotary conical gold crucible-heated to 980C-hold(2h)-cooled to 870C(0.67C/h)-cooled to 600C(25C/h)					Thermal fluctuation effects on the magnetization above and below the superconducting transition in Bi2Sr2CaCu2O8 in the weak magnetic field limit	199606		Laboratorio de Fisica de Materiales, Facultad de Fisica, Universidad de Compostela, 15706 Spain	Phys.Rev.B,53(1996)15272	C. Torro'n,E.G. Miramontes,Fe'lix Vidal,I. Rasines,J. Mosqueira,J.A. Campa		
12364	PR05314637		SmBa2Cu3O7+-Z	Sm1Ba2Cu3O6.92	Sm	1	Ba	2	Cu	3															O	7-Z	6.92	1	1996																											3					3.833	3.901	11.688	3											K		90		91			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12365	PR05314637		SmBa2(Cu,Fe)3Oz	Sm1Ba2Cu2.98Fe0.02O6.76	Sm	1	Ba	2	Cu	2.98	Fe	0.02													O	7-z	6.76	1	1996																											3					3.856	3.898	11.694	3											K		84		89			84																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12366	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.96Fe0.04O6.81	Sm	1	Ba	2	Cu	2.96	Fe	0.04													O	7-z	6.81	1	1996																											3					3.867	3.901	11.7	3											K		78		77			78																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12367	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.94Fe0.06O7-z	Sm	1	Ba	2	Cu	2.94	Fe	0.06													O	7-z		1	1996																											3					3.873	3.902	11.697	3											K		71		77			71																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12368	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.92Fe0.08O7-z	Sm	1	Ba	2	Cu	2.92	Fe	0.08													O	7-z		1	1996																											3					3.885	3.899	11.688	3											K		68		75			68																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12369	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.9Fe0.1O6.89	Sm	1	Ba	2	Cu	2.9	Fe	0.1													O	7-z	6.89	1	1996																											2					3.888		11.691	3											K		66		72			66																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12370	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.8Fe0.2O6.96	Sm	1	Ba	2	Cu	2.8	Fe	0.2													O	7-z	6.96	1	1996																											2	Y123				3.89		11.685	3											K		47		49			47																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12371	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.7Fe0.3O7-z	Sm	1	Ba	2	Cu	2.7	Fe	0.3													O	7-z		1	1996																											2					3.892		11.688	3											K				23			23																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12372	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.6Fe0.4O7-z	Sm	1	Ba	2	Cu	2.6	Fe	0.4													O	7-z		1	1996																											2					3.892		11.694	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12373	PR05314637		DyBa2Cu3O7	Dy1Ba2Cu3O6.84	Dy	1	Ba	2	Cu	3															O	7-z	6.84	1	1996																											3					3.816	3.881	11.664	3											K		90		92			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12374	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.98Fe0.02O6.88	Dy	1	Ba	2	Cu	2.98	Fe	0.02													O	77-z	6.88	1	1996																											3					3.82	3.882	11.672	3											K		88		90			88																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12375	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.96Fe0.04O6.89	Dy	1	Ba	2	Cu	2.96	Fe	0.04													O	7-z	6.89	1	1996																											3					3.824	3.877	11.664	3											K		82		88			82																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12376	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.94Fe0.06O6.88	Dy	1	Ba	2	Cu	2.94	Fe	0.06													O	7-z	6.88	1	1996																											3					3.841	3.865	11.664	3											K		78		86			78																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12377	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.92Fe0.08O7-z	Dy	1	Ba	2	Cu	2.92	Fe	0.08													O	7-z		1	1996																											2					3.856		11.668	3											K		74		78			74																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12378	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.9Fe0.1O6.84	Dy	1	Ba	2	Cu	2.9	Fe	0.1													O	7-z	6.84	1	1996																											2					3.857		11.668	3											K		70		73			70																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12379	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.8Fe0.2O6.93	Dy	1	Ba	2	Cu	2.8	Fe	0.2													O	7-z	6.93	1	1996																											2					3.863		11.657	3											K		58		59			58																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12380	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.7Fe0.3O6.96	Dy	1	Ba	2	Cu	2.7	Fe	0.3													O	7-z	6.96	1	1996																											2					3.867		11.657	3											K		10		45			10																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12381	PR05314637		DyBa2(Cu,Fe)3O7	Dy1Ba2Cu2.6Fe0.4O7.09	Dy	1	Ba	2	Cu	2.6	Fe	0.4													O	7-z	7.09	1	1996																											2					3.864		11.634	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12382	PR05314637		SmBa2Cu3O7	Sm1Ba2Cu3O6.89	Sm	1	Ba	2	Cu	3															O	7-z	6.89	1	1996																											3					3.831	3.904	11.702	3											K		90		91			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12383	PR05314637		SmBa2(Cu,Fe)3O7	Sm1Ba2Cu2.98Ni0.02O7-z	Sm	1	Ba	2	Cu	2.98	Ni	0.02													O	7-z		1	1996																											3					3.841	3.901	11.698	3											K		83		88			83																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12384	PR05314637		SmBa2Cu2.96Fe0.04O7+-Z	Sm1Ba2Cu2.96Ni0.04O6.88	Sm	1	Ba	2	Cu	2.96	Ni	0.04													O	7-z	6.88	1	1996																											3					3.84	3.899	11.702	3											K		83		88			83																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12385	PR05314637		SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.94Ni0.06O7-z	Sm	1	Ba	2	Cu	2.94	Ni	0.06													O	7-z		1	1996																											3					3.858	3.898	11.698	3											K		76		84			76																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12386	PR05314637	Tc not shown. 	SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.92Ni0.08O7-z	Sm	1	Ba	2	Cu	2.92	Ni	0.08													O	7-z		1	1996																											3								3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12387	PR05314637		SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.9Ni0.1O7-z	Sm	1	Ba	2	Cu	2.9	Ni	0.1													O	7-z		1	1996																											3								3											K		72		78			72																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12388	PR05314637		SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.8Ni0.2O7-z	Sm	1	Ba	2	Cu	2.8	Ni	0.2													O	7-z		1	1996																											3					3.871	3.9	11.685	3											K		50		53			50																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12389	PR05314637		SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.7Ni0.3O6.97	Sm	1	Ba	2	Cu	2.7	Ni	0.3													O	7-z	6.97	1	1996																											3					3.867	3.9	11.668	3											K		24		47			24																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12390	PR05314637		SmBa2(Cu,Ni)3O7	Sm1Ba2Cu2.6Ni0.4O7-z	Sm	1	Ba	2	Cu	2.6	Ni	0.4													O	7-z		1	1996																											3					3.873	3.895	11.675	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12391	PR05314637		DyBa2Cu3O7	Dy1Ba2Cu3O6.68	Dy	1	Ba	2	Cu	3															O	7-z	6.68	1	1996																											3					3.814	3.88	11.56	3											K		90		92			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12392	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.98Ni0.02O6.72	Dy	1	Ba	2	Cu	2.98	Ni	0.02													O	7-z	6.72	1	1996																											3					3.818	3.886	11.558	3											K		83		88			83																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12393	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.96Ni0.04O6.73	Dy	1	Ba	2	Cu	2.96	Ni	0.04													O	7-z	6.73	1	1996																											3					3.822	3.887	11.558	3											K		82		86			82																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12394	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.94Ni0.06O6.72	Dy	1	Ba	2	Cu	2.94	Ni	0.06													O	7-z	6.72	1	1996																											3					3.815	3.886	11.55	3											K		81		86			81																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12395	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.92Ni0.08O7-z	Dy	1	Ba	2	Cu	2.92	Ni	0.08													O	7-z		1	1996																											3					3.821	3.885	11.553	3											K		77		80			77																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12396	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.9Ni0.1O6.74	Dy	1	Ba	2	Cu	2.9	Ni	0.1													O	7-z	6.74	1	1996																											3					3.821	3.888	11.555	3											K		67		79			67																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12397	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.8Ni0.2O6.83	Dy	1	Ba	2	Cu	2.8	Ni	0.2													O	7-z	6.83	1	1996																											3					3.818	3.886	11.553	3											K		63		68			63																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12398	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.7Ni0.3O7-z	Dy	1	Ba	2	Cu	2.7	Ni	0.3													O	7-z		1	1996																											3					3.826	3.882	11.558	3											K		54		55			54																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12399	PR05314637		DyBa2(Cu,Ni)3O7	Dy1Ba2Cu2.6Ni0.4O6.83	Dy	1	Ba	2	Cu	2.6	Ni	0.4													O	7-z	6.83	1	1996																																			3											K		31		50			31																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12400	PR05314637		SmBa2Cu3O7	Sm1Ba2Cu3O6.82	Sm	1	Ba	2	Cu	3															O	7-z	6.82	1	1996																											3					3.833	3.905	11.686	3											K		90		91			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12401	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.98Zn0.02O6.82	Sm	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z	6.82	1	1996																											3					3.841	3.903	11.697	3											K		81		83			81																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12402	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.96Zn0.04O6.83	Sm	1	Ba	2	Cu	2.96	Zn	0.04													O	7-z	6.83	1	1996																											3					3.844	3.903	11.694	3											K		70		68			70																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12403	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.94Zn0.06O6.85	Sm	1	Ba	2	Cu	2.94	Zn	0.06													O	7-z	6.85	1	1996																											3					3.84	3.902	11.684	3											K		59		60			59																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12404	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.92Zn0.08O6.85	Sm	1	Ba	2	Cu	2.92	Zn	0.08													O	7-z	6.85	1	1996																											3					3.841	3.902	11.701	3											K		49		47			49																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12405	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.9Zn0.1O6.83	Sm	1	Ba	2	Cu	2.9	Zn	0.1													O	7-z	6.83	1	1996																											3					3.84	3.899	11.658	3											K		29		49			29																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12406	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.8Zn0.2O6.83	Sm	1	Ba	2	Cu	2.8	Zn	0.2													O	7-z	6.83	1	1996																											3					3.87	3.894	11.694	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12407	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.7Zn0.3O7-z	Sm	1	Ba	2	Cu	2.7	Zn	0.3													O	7-z		1	1996																											3					3.873	3.894	11.686	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12408	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.6Zn0.4O6.9	Sm	1	Ba	2	Cu	2.6	Zn	0.4													O	7-z	6.9	1	1996																											3					3.875	3.89	11.658	3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12409	PR05314637		DyBa2Cu3O7	Dy1Ba2Cu3O6.79	Dy	1	Ba	2	Cu	3															O	7-z	6.79	1	1996																											3					3.813	3.879		3											K		90		92			90																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12410	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.98Zn0.02O6.87	Dy	1	Ba	2	Cu	2.98	Zn	0.02													O	7-z	6.87	1	1996																											3					3.812	3.881		3											K		81		84			81																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12411	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.96Zn0.04O6.9	Dy	1	Ba	2	Cu	2.96	Zn	0.04													O	7-z	6.9	1	1996																											3					3.813	3.882		3											K		70		76			70																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12412	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.94Zn0.06O6.9	Dy	1	Ba	2	Cu	2.94	Zn	0.06													O	7-z	6.9	1	1996																											3					3.818	3.884		3											K		62		71			62																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12413	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.92Zn0.08O7-z	Dy	1	Ba	2	Cu	2.92	Zn	0.08													O	7-z		1	1996																											3								3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12414	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.9Zn0.1O6.96	Dy	1	Ba	2	Cu	2.9	Zn	0.1													O	7-z	6.96	1	1996																											3					3.833	3.886		3											K		44		56			44																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12415	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.8Zn0.2O6.95	Dy	1	Ba	2	Cu	2.8	Zn	0.2													O	7-z	6.95	1	1996																											3					3.825	3.886		3											K		13		25			13																																																																																														R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12416	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.7Zn0.3O6.99	Dy	1	Ba	2	Cu	2.7	Zn	0.3													O	7-z	6.99	1	1996																											3					3.834	3.89		3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12417	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.6Zn0.4O6.95	Dy	1	Ba	2	Cu	2.6	Zn	0.4													O	7-z	6.95	1	1996																											3					3.823	3.882		3											K																																																																																																					R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12419	PR05314637		SmBa2(Cu,Zn)3O7	Sm1Ba2Cu2.8Zn0.2O6.82	Sm	1	Ba	2	Cu	2.8	Zn	0.2													O	7-z	6.82	1	1996																																														K																																																																														m.ohm.cm											2.6												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12420	PR05314637		SmBa2(Cu,Zn)3O7	Sm0.9Ca0.1Ba2Cu2.8Zn0.2O6.85	Sm	0.9	Ca	0.1	Ba	2	Cu	2.8	Zn	0.2											O	7-z	6.85	1	1996																																														K	39		48	42		7	42																																																																							m.ohm.cm											1.8												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12421	PR05314637		SmBa2(Cu,Zn)3O7	Sm0.8Ca0.2Ba2Cu2.8Zn0.2O6.87	Sm	0.8	Ca	0.2	Ba	2	Cu	2.8	Zn	0.2											O	7-z	6.87	1	1996																																														K	36		41	45		4	45																																																																							m.ohm.cm											1.6												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12422	PR05314637		DyBa2(Cu,Zn)3O7	Dy1Ba2Cu2.7Zn0.3O6.9	Dy	1	Ba	2	Cu	2.7	Zn	0.3													O	7-z	6.9	1	1996																																																																																																																												m.ohm.cm											5.1												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12423	PR05314637		(Dy,Ca)Ba2(Cu,Zn)3O7	Dy0.9Ca0.1Ba2Cu2.7Zn0.3O6.72	Dy	0.9	Ca	0.1	Ba	2	Cu	2.7	Zn	0.3											O	7-z	6.72	1	1996																																														K	13		19	21		5	21																																																																							m.ohm.cm											3.3												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12424	PR05314637		(Dy,Ca)Ba2(Cu,Zn)3O7	Dy0.8Ca0.2Ba2Cu2.7Zn0.3O6.78	Dy	0.8	Ca	0.2	Ba	2	Cu	2.7	Zn	0.3											O	7-z	6.78	1	1996																																														K	30		22	28		7	28																																																																							m.ohm.cm											2.1												R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO	1	mix(R2O3(R=Sm,Dy),BaCO3,CuO,Fe2O3/NiO/ZnO)-sin(920C,24h-940C,24h)-press into pellet-sin(940C,24h)-O2 anenal(900C,24h-600C,24h)					Effect of 3d ion substitution in the RBa2Cu3-xMxO7(R=Sm,Dy; M=Fe,Ni and Zn) system: Implications of R ion dependence and disorder	06		Materials Science Research Centre,Institute of Technology, Madras 600 036, India	Phys.Rev.B,53(1996)14637	P.Sumana Prabhu,U.V. Varadaruju	Sm, Dy, Ba, Cu, Fe, Ni, Zn, O	
12425	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.4La0.6Ba1.35La0.65Cu3Oy	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	3											O	y			1996																											2	Y123																		K				79.1			79.1			K/GPa	2.1																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12426	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.4La0.6Ba1.35La0.65Cu3Oy	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	3											O	y			1996																											2	Y123																		K				74.4			74.4			K/GPa	3.7																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12427	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.1La0.9Ba1.65La0.35Cu3Oy	Ca	0.1	La	0.9	Ba	1.65	La	0.35	Cu	3											O	y			1996																											2	Y123																		K				45.4			45.4			K/GPa	4.7																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12428	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.2La0.8Ba1.55La0.45Cu3Oy	Ca	0.2	La	0.8	Ba	1.55	La	0.45	Cu	3											O	y			1996																											2	Y123																		K				54			54			K/GPa	4.7																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12429	PR05314631		((Ca,La)(Ba,La)2Cu3Oz	Ca0.2La0.8Ba1.55La0.45Cu3Oy	Ca	0.2	La	0.8	Ba	1.55	La	0.45	Cu	3											O	y			1996																											2	Y123																		K				28.1			28.1			K/GPa	4.6																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12430	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.2La0.8Ba1.55La0.45Cu3Oy	Ca	0.2	La	0.8	Ba	1.55	La	0.45	Cu	3											O	y			1996																											2	Y123																		K				15			15			K/GPa	5.6																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12431	PR05314631		(Ca,La)(Ba,La)2Cu3Oz	Ca0.4La0.6Ba1.35La0.65Cu3Oy	Ca	0.4	La	0.6	Ba	1.35	La	0.65	Cu	3											O	y			1996																											2	Y123																		K				79.4			79.4			K/GPa	1.37																																																																																												D.Goldschmidt,G.M.Reisner,Y.Direktovitch,A.Knizhnik,E.Gartstein,G.Kimmel,and Y.Eckstein,Phys.Rev.B 48,532(1993)D.Goldschmidt,A.Knizhnik,Y.Direktovitch,G.M.Reisner,and Y.Eckstein,ibid.49,15928(1994)					Pressure dependence of Tc in cuprate superconductors: Application to (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy	06		Department of Physics and Crown Center for Superconductivity, Technion, Haifa 32000, Israel	Phys.Rev.B,53(1996)14631	A.-K. Klehe,D. Goldschmidt,J.S. Schilling,Y. Eckstein	Ca, La, Ba, Cu, O	
12450	P072014504	hole conc = 0.22. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2Sr2CuO6	Bi1.83Pb0.19Sr1.92Cu1.06O6+z	Bi	1.83	Pb	0.19	Sr	1.92	Cu	1.06													O	6+z		1	2005																												Bi2201																		K				12			12																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12451	P072014504	hole conc = 0.19. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.69Pb0.3Sr1.92La0.16Cu1.08O6+z	Bi	1.69	Pb	0.3	Sr	1.92	La	0.16	Cu	1.08											O	6+z		1	2005																												Bi2201																		K				24			24																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12452	P072014504	hole conc = 0.16. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.61Pb0.3Sr1.65La0.36Cu1.08O6+z	Bi	1.61	Pb	0.3	Sr	1.65	La	0.36	Cu	1.08											O	6+z		1	2005																												Bi2201																		K				34			34																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12453	P072014504	hole conc = 0.12. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.66Pb0.34Sr1.52La0.4Cu1.1O6+z	Bi	1.66	Pb	0.34	Sr	1.52	La	0.4	Cu	1.1											O	6+z		1	2005																												Bi2201																		K				21			21																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12454	P072014504	hole conc = 0.15. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.63Pb0.34Sr1.53La0.41Cu1.01O6+z	Bi	1.63	Pb	0.34	Sr	1.53	La	0.41	Cu	1.01											O	6+z		1	2005																												Bi2201																		K				31			31																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12455	P072014504	hole conc = 0.12 chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.6Pb0.43Sr1.39La0.5Cu1.09O6+z	Bi	1.6	Pb	0.43	Sr	1.39	La	0.5	Cu	1.09											O	6+z		1	2005																												Bi2201																		K				5			5																																																																																														Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12456	P072014504	hole conc = 0.10. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.69Pb0.3Sr1.35La0.55Cu1.09O6+z	Bi	1.69	Pb	0.3	Sr	1.35	La	0.55	Cu	1.09											O	6+z		1	2005																												Bi2201																		K					4																																																																																																Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12457	P072014504	hole conc = 0.11. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.69Pb0.3Sr1.31La0.58Cu1.12O6+z	Bi	1.69	Pb	0.3	Sr	1.31	La	0.58	Cu	1.12											O	6+z		1	2005																												Bi2201																		K					4																																																																																																Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12458	P072014504	hole conc = 0.06. chemical compo. obtained by EDX. hole conc from L3-absorption edge.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.73Pb0.27Sr1.27La0.64Cu1.09O6+z	Bi	1.73	Pb	0.27	Sr	1.27	La	0.64	Cu	1.09											O	6+z		1	2005																												Bi2201																		K					4																																																																																																Bi2O3,La2O3,CuO,SrCO	1	standard sintering method. SIN(890C), SIN(800C for no La), in air. ANN(550C,5h in vac)					Evolution of the density of states at the Fermi level of Bi2-yPbySr2-xLaxCuO6+z  and Bi2Sr2-xLaxCuO6+z  cuprates with hole doping			Humboldt Universitat, Institut fur Physik, Newtonstrasse 15, 12489 Berlin, Germany	Phys.Rev.B, 72(2005)014504	A.Krapf,C.Janowitz,H.Dwelk,M.Schneider,R.-S.Unger,R.Manzke,R.Mitdank,R.Muller,S.Rogaschewski		
12500	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1996																											3	Bi2212			A	5.402	5.427	30.804	3											K				95			95																																																																																																					Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12501	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.9Ce0.1Cu2O8+y	Bi	2	Sr	2	Ca	0.9	Ce	0.1	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.406	5.427	30.715	3											K				52			52																																																																																																					Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12502	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.8Ce0.2Cu2O8+y	Bi	2	Sr	2	Ca	0.8	Ce	0.2	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.415	5.427	30.649	3											K				25			25																																																																																																					Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12503	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.75Ce0.25Cu2O8+y	Bi	2	Sr	2	Ca	0.75	Ce	0.25	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.422	5.421	30.524	3											K					5																																																																																																							Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12504	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.7Ce0.3Cu2O8+y	Bi	2	Sr	2	Ca	0.7	Ce	0.3	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.423	5.423	30.466	3											K					5																																																																																																							Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12505	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.6Ce0.4Cu2O8+y	Bi	2	Sr	2	Ca	0.6	Ce	0.4	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.429	5.432	30.404	3											K					5																																																																																																							Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12506	PR05302245		Bi2Sr2(Ca,Ce)Cu2O8	Bi2Sr2Ca0.5Ce0.5Cu2O8+y	Bi	2	Sr	2	Ca	0.5	Ce	0.5	Cu	2											O	8+y		1	1996																											3	Bi2212			A	5.432	5.433	30.375	3											K					5																																																																																																							Effect of substituting Ce at the Ca site on the high-temperature superconductor Bi2Sr2CaCu2O8+z	02		Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India	Phys.Rev.B,53(1996)2245	Latica Menon,S. K. Malik,V. P. S. Awana	Bi, Sr, Ca, Cu, O, Ce	
12507	PR05302781		SmBa2Cu3O7-y	Sm1Ba2Cu3O6.95	Sm	1	Ba	2	Cu	3															O		6.95	1	1996																											3	Y123			A	3.846	3.911	11.73	3											K				95			95																																																					SP12507													micro.V/K	6.1			TP12507	m.ohm.cm							2.5																BaCO3,Sm2O3,CuO	1	MIX(BaCO3,Sm2O3,CuO) - calcine(900C,overnight) - reground - press into pellets - SIN(930C,several days,with intermediate grindings) - HEAT(800C,5h,in flowing oxygen) - COOL(15C/h)					SmBa2Cu3O7-z ceramics processed under oxygen pressure of 250 bar: Enhancement of intragrain superconducting properties	02		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. box 937, 50-950 Wroctaw 2, Poland	Phys.Rev.B,53(1996)2781	A. J. Zaleski,C. Sulkowski,D. Wlosewicz,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
12508	PR05302781		SmBa2Cu3O7-y	Sm1Ba2Cu3O6.9	Sm	1	Ba	2	Cu	3															O		6.9	1	1996																											3	Y123			A	3.845	3.907	11.727	3																																																																							SP12508													micro.V/K	-0.8			TP12508	m.ohm.cm							14																BaCO3,Sm2O3,CuO	1	MIX(BaCO3,Sm2O3,CuO) - calcine(900C,overnight) - reground - press into pellets - SIN(930C,several days,with intermediate grindings) - HEAT(800C,5h,in flowing oxygen) - COOL(15C/h)- ANN(450C,250bar,in					SmBa2Cu3O7-z ceramics processed under oxygen pressure of 250 bar: Enhancement of intragrain superconducting properties	02		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. box 937, 50-950 Wroctaw 2, Poland	Phys.Rev.B,53(1996)2781	A. J. Zaleski,C. Sulkowski,D. Wlosewicz,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
12509	PR05302781		SmBa2Cu3O7-y	Sm1Ba2Cu3O7	Sm	1	Ba	2	Cu	3															O		7	1	1996																											3	Y123			A	3.845	3.91	11.721	3											K				96			96																																																					SP12509													micro.V/K	-1.5			TP12509	m.ohm.cm							15																BaCO3,Sm2O3,CuO	1	MIX(BaCO3,Sm2O3,CuO) - calcine(900C,overnight) - reground - press into pellets - SIN(930C,several days,with intermediate grindings) - HEAT(800C,5h,in flowing oxygen) - COOL(15C/h)- ANN(500C,250bar,in					SmBa2Cu3O7-z ceramics processed under oxygen pressure of 250 bar: Enhancement of intragrain superconducting properties	02		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. box 937, 50-950 Wroctaw 2, Poland	Phys.Rev.B,53(1996)2781	A. J. Zaleski,C. Sulkowski,D. Wlosewicz,T. Plackowski,Z. Bukowski	Sm, Ba, Cu, O	
12510	PR05302811		HgBa2CuO4+delta	Hg1Ba2Cu1O4.16	Hg	1	Ba	2	Cu	1															O		4.16	1	1996																												Hg1201																		K				88			88																																									A	1/lambda^2 vs T plot from reversible M at FIG.2.Then it was extrapolated by 1-(T/Tc)^2 fit.		1990																																																			1	The oxygen content delta of the samples was altered by heating the samples under different O2-partial pressures at about 300C.Ditails have been published elsewhere;Q. Xiong et al., Phys. Rev. B 50,103					variation of the temperature dependence of the penetration depth in HgBa2CuO4+z with oxidation	02		Department of Physics and the texas Center for Superconductivity, University of Houston, Houston, texas 77204-5932	Phys.Rev.B,53(1996)2811	C. W. Chu,Q. Xiong,Y. Cao,Y. Y. Xue	Hg, Ba, Cu, O	
12511	PR05302811		HgBa2CuO4+delta	Hg1Ba2Cu1O4.23	Hg	1	Ba	2	Cu	1															O		4.23	1	1996																												Hg1201																		K				97			97																																									A	1/lambda^2 vs T plot from reversible M at FIG.2.Then it was extrapolated by 1-(T/Tc)^2 fit.		1670																																																			1	The oxygen content delta of the samples was altered by heating the samples under different O2-partial pressures at about 300C.Ditails have been published elsewhere;Q. Xiong et al., Phys. Rev. B 50,103					variation of the temperature dependence of the penetration depth in HgBa2CuO4+z with oxidation	02		Department of Physics and the texas Center for Superconductivity, University of Houston, Houston, texas 77204-5932	Phys.Rev.B,53(1996)2811	C. W. Chu,Q. Xiong,Y. Cao,Y. Y. Xue	Hg, Ba, Cu, O	
12512	PR05302811		HgBa2CuO4+delta	Hg1Ba2Cu1O4.28	Hg	1	Ba	2	Cu	1															O		4.28	1	1996																												Hg1201																		K				88			88																																									A	1/lambda^2 vs T plot from London model or Bulaevskii model at FIG.2.Then it was extrapolated by 1-(T		1710																																																			1	The oxygen content delta of the samples was altered by heating the samples under different O2-partial pressures at about 300C.Ditails have been published elsewhere;Q. Xiong et al., Phys. Rev. B 50,103					variation of the temperature dependence of the penetration depth in HgBa2CuO4+z with oxidation	02		Department of Physics and the texas Center for Superconductivity, University of Houston, Houston, texas 77204-5932	Phys.Rev.B,53(1996)2811	C. W. Chu,Q. Xiong,Y. Cao,Y. Y. Xue	Hg, Ba, Cu, O	
12513	PR05302999	anisotropy factor = 30. 	HgBa2Ca2Cu3Oz	Hg1Ba2Ca2Cu3OZ	Hg	1	Ba	2	Ca	2	Cu	3													O	Z		1	1996																												Hg1223																		K				134.5			134.5																																									A	ac susceptibility 		2100	61000																																																	HgO,BaO,CaO,CuO	1	mix(HgO,BaO,CaO,CuO)-pelletize-fire(750C,10h)-heat(300C,flowing O2)-magnetically allign the the samples					Anisotropic magnetic penetration depth of grain-aligned HgBa2Ca2Cu3O8+delta	199602		Interdisciplinary research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B,53(1996)R2999	C. Panagopoulos,G.B. Peacock,I. Gameson,J.R. Cooper,J.W. Hodby,P.P. Edwards,W. Schmidbauer		
12514	PR05303003		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O		4	1	1996																												T'	I4/mmm		A	3.947		12.075	3											K				20			20																																																																																																The satndard solid-state reacttion					Increased Phase-breaking scattering rate in Zn-doped TBa2Cu3O7-z	02		Department of Solid State Physics, institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,53(1996)R3003	"J. Axna""s,O"". Rapp,W. Holm,Yu. Eltsev"	Zn, Y, Ba, Cu, O	
12515	PR05303003		(Nd,Tb,Ce)2CuO4	Nd1.665Tb0.185Ce0.15Cu1O4	Nd	1.665	Tb	0.185	Ce	0.15	Cu	1													O		4	1	1996																												T'	I4/mmm		A	3.942		12.05	3											K				13.5			13.5																																																																																																The satndard solid-state reacttion					Increased Phase-breaking scattering rate in Zn-doped TBa2Cu3O7-z	02		Department of Solid State Physics, institute of Technology, S-100 44 Stockholm, Sweden	Phys.Rev.B,53(1996)R3003	"J. Axna""s,O"". Rapp,W. Holm,Yu. Eltsev"	Zn, Y, Ba, Cu, O	
12516	PR05302975		(Nd,Tb,Ce)2CuO4	Nd1.48Tb0.38Ce0.15Cu1O4	Nd	1.48	Tb	0.38	Ce	0.15	Cu	1													O		4	1	1996																												T'	I4/mmm		A	3.935		12	3											K				8			8																																																																																																The satndard solid-state reacttion					Structural distortion and superconductivity in (Nd1-xTbx)1.85Ce0.15CuO4	02		"Forschungszentrum Karlsruhe, Institut fu""r Nukleare Festko""rpephysik, D-76021 Kalsruhe, Germany"	Phys.Rev.B,53(1996)R2975	M. Braden,P. Adelmann,R. Schweiss,T. Woisczyk	Nd, Tb, Ce, Cu, O	
12517	PR05302975		YBa2(Cu,Zn)3OZ	Y1Ba2Cu0.27Zn0.03OZ	Y	1	Ba	2	Cu	0.27	Zn	0.03													O	Z		3	1996																												Y123																		K		85.6				0.2	85.6																																				A			14	2																																																						Y2O3,CuO,BaCO3,ZnO	5	mix(Y2O3,CuO,BaCO3,ZnO)-crystal growing by a self-flux method-O2 anneal(450C,a few days)					Structural distortion and superconductivity in (Nd1-xTbx)1.85Ce0.15CuO4	02		"Forschungszentrum Karlsruhe, Institut fu""r Nukleare Festko""rpephysik, D-76021 Kalsruhe, Germany"	Phys.Rev.B,53(1996)R2975	M. Braden,P. Adelmann,R. Schweiss,T. Woisczyk	Nd, Tb, Ce, Cu, O	
12518	PR05302975		YBa2(Cu,Zn)3OZ	Y1Ba2Cu2.895Zn0.105OZ	Y	1	Ba	2	Cu	2.895	Zn	0.105													O	Z		3	1996																												Y123																		K		70				1.5	70																																				A			15	1.5																																																						Y2O3,CuO,BaCO3,ZnO	5	mix(Y2O3,CuO,BaCO3,ZnO)-crystal growing by a self-flux method-O2 anneal(450C,a few days)					Structural distortion and superconductivity in (Nd1-xTbx)1.85Ce0.15CuO4	02		"Forschungszentrum Karlsruhe, Institut fu""r Nukleare Festko""rpephysik, D-76021 Kalsruhe, Germany"	Phys.Rev.B,53(1996)R2975	M. Braden,P. Adelmann,R. Schweiss,T. Woisczyk	Nd, Tb, Ce, Cu, O	
12600	PR05306034	as-grown sample, THCFIG(p=1) for in-plane conductivity, p=2 for out-of-plane	YBa2Cu3O7-y	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		3	1996																												Y123																		K	60						60																																																													mW/K.cm																																			"prepared by a modified Czochralski method called the solute rich liquid crystal pulling methed, which are reported in""Y. Yamada and Y. Shiohara. Physica C 217, 182(1993)"					In-plane and out-of-plane thermal conductivity of a large single crystal of YBa2Cu3O7-x	03		Faculty of Engineering, Iwate University, 4-3-5 Ueda 020, Japan	Phys.Rev.B,53(1996)R6034	K. Noto,M. Matsukawa,T. Mizukoshi	Y, Ba, Cu, O	
12601	PR05306034	3 days annealed sample, THCFIG(p=1) for in-plane conductivity, p=2 for out-of-plane	YBa2Cu3O7-y	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		3	1996																												Y123																		K	92.7						92.7																																																													mW/K.cm																																			"prepared by a modified Czochralski method called the solute rich liquid crystal pulling methed, which are reported in""Y. Yamada and Y. Shiohara. Physica C 217, 182(1993)-ANN(in oxygen flow, 520C, for"					In-plane and out-of-plane thermal conductivity of a large single crystal of YBa2Cu3O7-x	03		Faculty of Engineering, Iwate University, 4-3-5 Ueda 020, Japan	Phys.Rev.B,53(1996)R6034	K. Noto,M. Matsukawa,T. Mizukoshi	Y, Ba, Cu, O	
12602	PR05306034	1 week annealed sample, THCFIG(p=1) for in-plane conductivity, p=2 for out-of-plane	YBa2Cu3O7-y	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		3	1996																												Y123																		K	92.7						92.7																																																													mW/K.cm																																			"prepared by a modified Czochralski method called the solute rich liquid crystal pulling methed, which are reported in""Y. Yamada and Y. Shiohara. Physica C 217, 182(1993)-ANN(in oxygen flow, 520C, for"					In-plane and out-of-plane thermal conductivity of a large single crystal of YBa2Cu3O7-x	03		Faculty of Engineering, Iwate University, 4-3-5 Ueda 020, Japan	Phys.Rev.B,53(1996)R6034	K. Noto,M. Matsukawa,T. Mizukoshi	Y, Ba, Cu, O	
12603	PR05306034	2 weeks annealed  sample, THCFIG(p=1) for in-plane conductivity, p=2 for out-of-plane	YBa2Cu3O7-y	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		3	1996																												Y123																		K	92.7						92.7																																																													mW/K.cm																																			"prepared by a modified Czochralski method called the solute rich liquid crystal pulling methed, which are reported in""Y. Yamada and Y. Shiohara. Physica C 217, 182(1993)-ANN(in oxygen flow, 520C, for"					In-plane and out-of-plane thermal conductivity of a large single crystal of YBa2Cu3O7-x	03		Faculty of Engineering, Iwate University, 4-3-5 Ueda 020, Japan	Phys.Rev.B,53(1996)R6034	K. Noto,M. Matsukawa,T. Mizukoshi	Y, Ba, Cu, O	
12604	PR05305170	nearly single phase. The possibility of the existence of minor phase of (Cu1-xCx)Ba2Ca3Cu4O11-y is not excluded. We, however, believe this situation would not affect our thermoelectric power result.	CuBa2Ca3Cu4O11-y	Ba2Ca3Cu5O11-y	Ba	2	Ca	3	Cu	5															O	11-y		1	1996																											2	Cu1234			A	3.859		18												K	115.9						115.9																																																																		micro.V/K	-3.4				m.ohm.cm											5.2												BaO2, CaO, CuO	1	MIX(BaO2,CaO,CuO with stoichiometric composition)-Synthesize(950C,5GPa,1h)detailed in C. -Q. Jin et al, Physica C 223, 238(1994)					Thermoelectric power of high-pressure synthesized CuBa2Ca3Cu4O11-z	03		Superconductivity research Laboratory, ISTEC, 10-13, Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,53(1996)5170	C.-J. Liu,C.-Q. Jun,H. Yamauchi	Cu, Ba, Ca, Cu, O	
12605	PR05305170	nearly single phase The possibility of the exitence of minor phase of (Cu1-xCx)Ba2Ca3Cu4O11-y is not excluded. We, however, believe this situation would not affect our thermoelectric power result.	CuBa2Ca3Cu4O11-y	Ba2Ca3Cu5O11-y	Ba	2	Ca	3	Cu	5															O	11-y		1	1996																												Cu1234																																																																																											micro.V/K	3.8				m.ohm.cm											16												BaO2, CaO, CuO	1	MIX(BaO2,CaO,CuO with stoichiometric composition)-Synthesize(950C,5GPa,1h)detailed in C. -Q. Jin et al, Physica C 223, 238(1994)					Thermoelectric power of high-pressure synthesized CuBa2Ca3Cu4O11-z	03		Superconductivity research Laboratory, ISTEC, 10-13, Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,53(1996)5170	C.-J. Liu,C.-Q. Jun,H. Yamauchi	Cu, Ba, Ca, Cu, O	
12606	PR05305848		Tl2Ba2CuO6	Tl2Ba2Cu1O6+y	Tl	2	Ba	2	Cu	1															O	6+y			1996																												Tl2201																		K	15						15																																																																																					m3/C	0.000000001										outlined in R. S. Liu, S. D. Hughes, R. J. Angel, T. P. Hackwell, A. P. Mackenzie, and P .P. Edwards, Physica C 198, 203(1992)Y. Shimakawa, Physica C 204,247(1993)M. A. G. Aranda, D. C. Sinclair, A. P					Normal-state magnetotransport in superconducting Tl2Ba2CuO6+z to millikelvin temperatures	03		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,53(1996)5848	A. P. Mackenzie,C. T. Lin,D. C. Sinclair,S. R. Julian	Tl, Ba, Cu, O	
12607	PR05305848		Tl2Ba2CuO6+y	Tl2Ba2Cu1O6+y	Tl	2	Ba	2	Cu	1															O	6+y			1996																																														K	11						11																																																																																																outlined in R. S. Liu, S. D. Hughes, R. J. Angel, T. P. Hackwell, A. P. Mackenzie, and P .P. Edwards, Physica C 198, 203(1992)Y. Shimakawa, Physica C 204,247(1993)M. A. G. Aranda, D. C. Sinclair, A. P					Normal-state magnetotransport in superconducting Tl2Ba2CuO6+z to millikelvin temperatures	03		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,53(1996)5848	A. P. Mackenzie,C. T. Lin,D. C. Sinclair,S. R. Julian	Tl, Ba, Cu, O	
12608	PR05305856		GdBa2Cu3O7	Gd1Ba2Cu3O7-y	Gd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.832	3.894	11.7	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12609	PR05305856		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.925Ni0.075O7-y	Gd	1	Ba	2	Cu	2.925	Ni	0.075													O	7-y		1	1996																											3	Y123			A	3.846	3.9	11.698	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12610	PR05305856		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.85Ni0.15O7-y	Gd	1	Ba	2	Cu	2.85	Ni	0.15													O	7-y		1	1996																											3	Y123			A	3.844	3.9	11.692	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12611	PR05305856		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.775Ni0.225O7-y	Gd	1	Ba	2	Cu	2.775	Ni	0.225													O	7-y		1	1996																											3	Y123			A	3.842	3.897	11.686	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12612	PR05305856		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.7Ni0.3O7-y	Gd	1	Ba	2	Cu	2.7	Ni	0.3													O	7-y		1	1996																											3	Y123			A	3.868	3.912	11.737	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12613	PR05305856		GdBa2(Cu,Ni)3O7	Gd1Ba2Cu2.55Ni0.45O7-y	Gd	1	Ba	2	Cu	2.55	Ni	0.45													O	7-y		1	1996																											3	Y123			A	3.889	3.911	11.734	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12614	PR05305856		GdBa2Cu3O7	Gd1Ba2Cu3O7-y	Gd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123			A	3.832	3.894	11.7	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12615	PR05305856		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.925Fe0.075O7-y	Gd	1	Ba	2	Cu	2.925	Fe	0.075													O	7-y		1	1996																											3	Y123			A	3.847	3.895	11.64	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12616	PR05305856		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.85Fe0.15O7-y	Gd	1	Ba	2	Cu	2.85	Fe	0.15													O	7-y		1	1996																											3	Y123			A	3.845	3.885	11.67	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12617	PR05305856		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.775Fe0.225O7-y	Gd	1	Ba	2	Cu	2.775	Fe	0.225													O	7-y		1	1996																											3	Y123			A	3.862	3.886	11.61	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12618	PR05305856		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.7Fe0.3O7-y	Gd	1	Ba	2	Cu	2.7	Fe	0.3													O	7-y		1	1996																											2	Y123			A	3.889	3.889	11.676	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12619	PR05305856		GdBa2(Cu,Fe)3O7	Gd1Ba2Cu2.55Fe0.45O7-z	Gd	1	Ba	2	Cu	2.55	Fe	0.45													O	7-z		1	1996																											3	Y123			A	3.892	3.892	11.676	3																																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12620	PR05305856		NdBa2Cu3O7	Nd1Ba2Cu3O7-y	Nd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12621	PR05305856		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.925Ni0.075O7-y	Nd	1	Ba	2	Cu	2.925	Ni	0.075													O	7-y		1	1996																											3	Y123																		K		80					80																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12622	PR05305856		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.85Ni0.15O7-y	Nd	1	Ba	2	Cu	2.85	Ni	0.15													O	7-y		1	1996																											3	Y123																		K		75					75																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12623	PR05305856		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.775Ni0.225O7-y	Nd	1	Ba	2	Cu	2.775	Ni	0.225													O	7-y		1	1996																											3	Y123																		K		72					72																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12624	PR05305856		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.7Ni0.3O7-y	Nd	1	Ba	2	Cu	2.7	Ni	0.3													O	7-y		1	1996																											3	Y123																		K		62					62																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12625	PR05305856		NdBa2(Cu,Ni)3O7	Nd1Ba2Cu2.55Ni0.45O7-y	Nd	1	Ba	2	Cu	2.55	Ni	0.45													O	7-y		1	1996																											3	Y123																		K		46					46																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12626	PR05305856		YBa2Cu3O7	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12627	PR05305856		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.925Ni0.075O7-y	Y	1	Ba	2	Cu	2.925	Ni	0.075													O	7-y		1	1996																											3	Y123																		K		80					80																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12628	PR05305856		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.85Ni0.15O7-y	Y	1	Ba	2	Cu	2.85	Ni	0.15													O	7-y		1	1996																											3	Y123																		K		73					73																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12629	PR05305856		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.775Ni0.225O7-y	Y	1	Ba	2	Cu	2.775	Ni	0.225													O	7-y		1	1996																											3	Y123																		K		68					68																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12630	PR05305856		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.7Ni0.3O7-y	Y	1	Ba	2	Cu	2.7	Ni	0.3													O	7-y		1	1996																											3	Y123																		K		60					60																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12631	PR05305856		YBa2(Cu,Ni)3O7	Y1Ba2Cu2.55Ni0.45O7-y	Y	1	Ba	2	Cu	2.55	Ni	0.45													O	7-y		1	1996																											3	Y123																		K		45					45																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12632	PR05305856		HoBa2Cu3O7	Ho1Ba2Cu3O7-y	Ho	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12633	PR05305856		HoBa2(Cu,Ni)3O7	Ho1Ba2Cu2.925Ni0.075O7-y	Ho	1	Ba	2	Cu	2.925	Ni	0.075													O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12634	PR05305856		HoBa2(Cu,Ni)3O7	Ho1Ba2Cu2.85No0.15O7-y	Ho	1	Ba	2	Cu	2.85	No	0.15													O	7-y		1	1996																											3	Y123																		K		85					85																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12635	PR05305856		HoBa2(Cu,Ni)3O7	Ho1Ba2Cu2.775Ni0.225O7-y	Ho	1	Ba	2	Cu	2.775	Ni	0.225													O	7-y		1	1996																											3	Y123																		K		84					84																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12636	PR05305856		HoBa2(Cu,Ni)3O7	Ho1Ba2Cu2.7Ni0.3O7-y	Ho	1	Ba	2	Cu	2.7	Ni	0.3													O	7-y		1	1996																											3	Y123																		K		78					78																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12637	PR05305856		HoBa2(Cu,Ni)3O7	Ho1Ba2Cu2.55Ni0.45O7-y	Ho	1	Ba	2	Cu	2.55	Ni	0.45													O	7-y		1	1996																											3	Y123																		K		75					75																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12638	PR05305856		TmBa2Cu3O7	Tm1Ba2Cu3O7-y	Tm	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12639	PR05305856		TmBa2(Cu,Ni)3O7	Tm1Ba2Cu2.925Ni0.075O7-y	Tm	1	Ba	2	Cu	2.925	Ni	0.075													O	7-y		1	1996																											3	Y123																		K		86					86																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12640	PR05305856		TmBa2(Cu,Ni)3O7	Tm1Ba2Cu2.85Ni0.15O7-y	Tm	1	Ba	2	Cu	2.85	Ni	0.15													O	7-y		1	1996																											3	Y123																		K		84					84																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12641	PR05305856		TmBa2(Cu,Ni)3O7	Tm1Ba2Cu2.775Ni0.225O7-y	Tm	1	Ba	2	Cu	2.775	Ni	0.225													O	7-y		1	1996																											3	Y123																		K		82					82																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12642	PR05305856		TmBa2(Cu,Ni)3O7	Tm1Ba2Cu2.7Ni0.3O7-y	Tm	1	Ba	2	Cu	2.7	Ni	0.3													O	7-y		1	1996																											3	Y123																		K		80					80																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12643	PR05305856		TmBa2(Cu,Ni)3O7	Tm1Ba2Cu2.55Ni0.45O7-y	Tm	1	Ba	2	Cu	2.55	Ni	0.45													O	7-y		1	1996																											3	Y123																		K		80					80																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12644	PR05305856		NdBa2Cu3O7	Nd1Ba2Cu3O7-y	Nd	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12645	PR05305856		NdBa2(Cu,Fe)3O7	Nd1Ba2Cu2.925Fe0.075O7-y	Nd	1	Ba	2	Cu	2.925	Fe	0.075													O	7-y		1	1996																											3	Y123																		K		66					66																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12646	PR05305856		NdBa2(Cu,Fe)3O7	Nd1Ba2Cu2.85Fe0.15O7-y	Nd	1	Ba	2	Cu	2.85	Fe	0.15													O	7-y		1	1996																											3	Y123																		K		57					57																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12647	PR05305856		NdBa2(Cu,Fe)3O7	Nd1Ba2Cu2.775Fe0.225O7-y	Nd	1	Ba	2	Cu	2.775	Fe	0.225													O	7-y		1	1996																											3	Y123																		K		46					46																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12648	PR05305856		NdBa2(Cu,Fe)3O7	Nd1Ba2Cu2.7Fe0.3O7-y	Nd	1	Ba	2	Cu	2.7	Fe	0.3													O	7-y		1	1996																											2	Y123																		K		24					24																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12649	PR05305856		NdBa2(Cu,Fe)3O7	Nd1Ba2Cu2.55Fe0.45O7-y	Nd	1	Ba	2	Cu	2.55	Fe	0.45													O	7-y		1	1996																											3	Y123																		K					4.2																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12650	PR05305856		YBa2Cu3O7	Y1Ba2Cu3O7-y	Y	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12651	PR05305856		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.925Fe0.075O7-y	Y	1	Ba	2	Cu	2.925	Fe	0.075													O	7-y		1	1996																											3	Y123																		K		88					88																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12652	PR05305856		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.775Fe0.225O7-y	Y	1	Ba	2	Cu	2.775	Fe	0.225													O	7-y		1	1996																											3	Y123																		K		63					63																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12653	PR05305856		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.7Fe0.3O7-y	Y	1	Ba	2	Cu	2.7	Fe	0.3													O	7-y		1	1996																											2	Y123																		K		35					35																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12654	PR05305856		YBa2(Cu,Fe)3O7	Y1Ba2Cu2.55Fe0.45O7-y	Y	1	Ba	2	Cu	2.55	Fe	0.45													O	7-y		1	1996																											3	Y123																		K					4.2																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12655	PR05305856		HoBa2Cu3O7	Ho1Ba2Cu3O7-y	Ho	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12656	PR05305856		HoBa2(Cu,Fe)3O7	Ho1Ba2Cu2.925Fe0.075O7-y	Ho	1	Ba	2	Cu	2.925	Fe	0.075													O	7-y		1	1996																											3	Y123																		K		88					88																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12657	PR05305856		HoBa2(Cu,Fe)3O7	Ho1Ba2Cu2.85Fe0.15O7-y	Ho	1	Ba	2	Cu	2.85	Fe	0.15													O	7-y		1	1996																											3	Y123																		K		85					85																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12658	PR05305856		HoBa2(Cu,Fe)3O7	Ho1Ba2Cu2.775Fe0.225O7-y	Ho	1	Ba	2	Cu	2.775	Fe	0.225													O	7-y		1	1996																											3	Y123																		K		64					64																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12659	PR05305856		HoBa2(Cu,Fe)3O7	Ho1Ba2Cu2.7Fe0.3O7-y	Ho	1	Ba	2	Cu	2.7	Fe	0.3													O	7-y		1	1996																											2	Y123																		K		41					41																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12660	PR05305856		HoBa2(Cu,Fe)3O7	Ho1Ba2Cu2.55Fe0.45O7-y	Ho	1	Ba	2	Cu	2.55	Fe	0.45													O	7-y		1	1996																											3	Y123																		K					4.2																																																																																																R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12661	PR05305856		TmBa2Cu3O7	Tm1Ba2Cu3O7-y	Tm	1	Ba	2	Cu	3															O	7-y		1	1996																											3	Y123																		K		90					90																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12662	PR05305856		TmBa2(Cu,Fe)3O7	Tm1Ba2Cu2.925Fe0.075O7-y	Tm	1	Ba	2	Cu	2.925	Fe	0.075													O	7-y		1	1996																											3	Y123																		K		89					89																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12663	PR05305856		TmBa2(Cu,Fe)3O7	Tm1Ba2Cu2.85Fe0.15O7-y	Tm	1	Ba	2	Cu	2.85	Fe	0.15													O	7-y		1	1996																											3	Y123																		K		86					86																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12664	PR05305856		TmBa2(Cu,Fe)3O7	Tm1Ba2Cu2.7Fe0.3O7-y	Tm	1	Ba	2	Cu	2.7	Fe	0.3													O	7-y		1	1996																											2	Y123																		K		77					77																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12665	PR05305856		TmBa2(Cu,Fe)3O7	Tm1Ba2Cu2.55Fe0.45O7-y	Tm	1	Ba	2	Cu	2.55	Fe	0.45													O	7-y		1	1996																											3	Y123																		K		55					55																																																																																														R2O3,BaCO3,CuO,NiO,Fe2O3	1	MIX(in stoichiometric ratios) - SYN(air,920C,2days,with intermediate grinding) - ANN(air,940C,with intermediate grinding) - ANN(450C,1-2 days,in oxygen flow) - Cool(slow)					Influence of rare-earth ionic radius on the properties of Ni- and Fe-substituted RBa2(Cu1-xMx)3O7-x systems (R=Y,Nd,Eu,Gd,Ho,Tm;M=Ni,Fe)	03		Institute for High Pressure Physics, Russian Academy of Sciences, Moscow regin,142092, Russia	Phys.Rev.B,53(1996)5856	V. N. Kochetkov,V. N. Narozhnyi	R, Ba, Cu, Ni, Fe, O	
12666	PR05305610		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O3.98	Pr	1.85	Ce	0.15	Cu	1															O		3.98	1	1996																												T'			nm	0.396	0.396	1.214	3											K				18			18											kA/m																																																																																			Pr6O11,CeO2,CuO	1	mix(Pr6O11,CeO2,CuO)-heat(900C,12h)-fire(1100C,7days with three intermediate grindings) and quench-reduce(950C,12h in Ar) and quench					Tunneling spectroscopy of the superconducting energy gap in RNi2B2C (R=Y and Lu)			faculty of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739, Japan	Phys.Rev.B,53(1996)5640	T.Ekino,H.Fujii,Jnn Akimitsu,Makoto Kosugi,Yuji Zenitani		
12667	PR05305839		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O7-y	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			84				84																																																																							m.ohm.cm											0.8			m3/C	0.0000000005								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12668	PR05305839		(Er,Pr)Ba2Cu3O7	Er0.8Pr0.2Ba2Cu3O7-y	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			78				78																																																																							m.ohm.cm											1			m3/C	0.0000000007								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12669	PR05305839		(Dy,Pr)Ba2Cu3O7	Dy0.8Pr0.2Ba2Cu3O7-y	Dy	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			72				72																																																																							m.ohm.cm											1.1			m3/C	0.0000000008								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12670	PR05305839		(Gd,Pr)Ba2Cu3O7	Gd0.8Pr0.2Ba2Cu3O7-y	Gd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			67				67																																																																							m.ohm.cm											1.3			m3/C	0.0000000008								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12671	PR05305839		(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O7-y	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			59				59																																																																							m.ohm.cm											1.4			m3/C	0.000000001								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12672	PR05305839		(Nd,Pr)Ba2Cu3O7	Nd0.8Pr0.2Ba2Cu3O7-y	Nd	0.8	Pr	0.2	Ba	2	Cu	3													O	7-y		1	1996																											3	Y123																		K			49				49																																																																							ohm.cm											1.7			m3/C	0.000000001								R2O3,Pr6O11,BaCO3,CuO	1	MIX(R2O3,Pr6O11,BaCO3,CuO,in stoichiometric) - ground - Calcine(915C,24h,in air, Al2O3 crucible) - Cool(slow) - press(3 tons/cm2, into pellets) - Heat(925-935C,3 days,in flowing oxygen) - ANN(680C, 10					Ion-size effect on normal-state transport properties in R0.8Pr0.2Ba2Cu3O7-y systems (R=Yb, Er, Dy, Gd, Eu, and Nd)	03		Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B,53(1996)5839	J. C. Chen,M. K. Wu,Weiyan Guan,Yunhui Xu	Yb, Er, Dy, Gd, Eu, Nd, Pr, Ba, Cu, O	
12700	PR05308604		EuSr2(Cu,Re)3Oz	Eu1Sr2Cu2.85Re0.25Oy	Eu	1	Sr	2	Cu	2.85	Re	0.25													O	y		1	1996																											2	Y123			A	3.836	3.836	11.51	3											K					12																																																																																																	1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12701	PR05308604		GdSr2(Cu,Re)3Oz	Gd1Sr2Cu2.85Re0.15Oy	Gd	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.83	3.833	11.511	3											K			25				25																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12702	PR05308604		TbSr2(Cu,Re)3Oz	Tb1Sr2Cu2.85Re0.15Oy	Tb	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.822	3.826	11.507	3											K	22		30				26																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12703	PR05308604		DySr2(Cu,Re)3Oz	Dy1Sr2Cu2.85Re0.15Oy	Dy	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.812	3.819	11.502	3											K	27		37				32																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12704	PR05308604		HoSr2(Cu,Re)3Oz	Ho1Sr2Cu2.85Re0.15Oy	Ho	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.807	3.822	11.501	3											K	42		51				46.5																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12705	PR05308604		ErSr2(Cu,Re)3Oz	Er1Sr2Cu2.85Re0.15OY	Er	1	Sr	2	Cu	2.85	Re	0.15													O	Y		1	1996																											3	Y123			A	3.806	3.822	11.5	3											K	43		51				47																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12706	PR05308604		TmSr2(Cu,Re)3Oz	Tm1Sr2Cu2.85Re0.15Oy	Tm	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.806	3.81	11.51	3											K	23		37				30																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12707	PR05308604		YSr2(Cu,Re)3Oz	Y1Sr2Cu2.85Re0.15Oy	Y	1	Sr	2	Cu	2.85	Re	0.15													O	y		1	1996																											3	Y123			A	3.803	3.819	11.516	3											K	41		47				44																																																																																															1	Prepare polycrystalline compounds of RSr2Cu2.85Re0.15Oy(R=lanthanides,Y)Calcine(1000C,12h)-Regrind-Pelletize-Sinter(flowing O2,1055C,(980C for Tm))-Cool(to 500C,1C/min)-anneal(10h)-Cool(to room temper					Strong rare-earth size dependence of Tc in RSr2Cu2.85Re0.15Oz	04		Department of Chemistry, Indian Institute of Technology,Powai, Bombay 400 076, India	Phys.Rev.B,53(1996)8604	L.C. Gupta,M. Murugesan,M. Sharon,M.S. Ramachandra Rao,R. Pinto,R. Vijayaraghavan	R, Sr, Cu, Re, O	
12708	PR05309460	This sample is grain-aligned.	HgBa2(Ca,Sr)Cu2O6	Hg1Ba2Ca0.86Sr0.14Cu2O6-Z	Hg	1	Ba	2	Ca	0.86	Sr	0.14	Cu	2											O	6-Z		1	1996																											2	Hg1212	P4/mmm		A	3.858	3.858	12.665	3											K				116			116											Oe	BCS clean limit								T	BCS clean limit			170.4					T/K				2.01			A	BCS clean limit		13.9	2	A	BCS clean limit			1913																																																	Ba2CuO3+x,Ca1-xSrxCuO2,HgO	1	Mix(Ba2CuO3+x,Ca1-xSrxCuO2,HgO)-Pelletize-Place inside an alumina tube and Seal  under vacuum-Heat(to 860C,8h)-Sinter(860C,10h)-Cool(to room temperature,8h					Three-dimensional superconducting behavior and thermodynamic parameters of HgBa2Ca0.86Sr0.14Cu2O6-z	04		Department of Physics, Pohang University of Science and Technology, pohang 790-784, South Korea	Phys.Rev.B,53(1996)9460	Mun-Seog  Kim,Nam H. Hur,Seong-Cho Yu,Sung-Ik Lee	Hg, Ba, Ca, Sr, Cu, O	
12709	PR05308902		Bi2Sr2CuO6	Bi2Sr2Cu1O6O6	Bi	2	Sr	2	Cu	1	O	6													O		6	3	1996																												Bi2201																		K					2																																																																									m.ohm.cm		6.4			10																		Bi2O3,SrCO3,CuO	5	Mix(Bi2O3,SrCO3,CuO)-React(950C,4h)-Cool(1C/h)					Transport properties of Bi2Sr2cuO6 single crystals: Possibility of interplane coupling in the weakly localized regime	04		Department of Applied Physics, Hokkaido University, Sapporo 060, Japan	Phys.Rev.B,53(1996)R8902	Katsuhiko Inagaki,Satoshi Tanda	Bi, Sr, Cu, O	
12800	PR05311976		YBa2Cu3O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O		6.96	1	1996																												Y123																		K	88.9						88.9			K/GPa	-0.27																																																														micro.V/K	0.1																												1						Pressure dependence of thermopower in YBa2Cu3O6.96 and YBa2Cu4O8	05		Center for Materials Science and Engineering, ETC 9.102,University of Texas at Austin, Texas 78712	Phys.Rev.B,53(1996)R11976	J.-S. Zhou,J.B. Goodenough	Y, Ba, Cu, O	
12801	PR05311976		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1996																												Y124																		K	62						62			K/GPa	6.6																																																														micro.V/K	7.1																												1						Pressure dependence of thermopower in YBa2Cu3O6.96 and YBa2Cu4O8	05		Center for Materials Science and Engineering, ETC 9.102,University of Texas at Austin, Texas 78712	Phys.Rev.B,53(1996)R11976	J.-S. Zhou,J.B. Goodenough	Y, Ba, Cu, O	
12802	PR05312416	This sample is grain-aligned.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		1	1996																												Bi2212			A			30.6	3											K				85			85																																				A	Hao-Clem model			9.5	A	Hao-Clem model		2438																																																			1						Effect of HgI2 intercalation on Bi2Sr2CaCu2Oy: Interlayer coupling effect	05		Department of physics, pohang University of Science and Technology,San 31 Hyojadong, Pohang, Kyugbuk, 790-784,Republic of Korea	Phys.Rev.B,53(1996)12416	Dong-Hoon Kim,Jin-Ho Choy,Mayoung-Kwang Bae,Mun-Seog Kim,Nam-Gyu Park,Seong-Ju Hwang,Sung-IK Lee	Bi, Sr, Ca, Cu, Hg, I	
12803	PR05312416		(HgI2)0.5Bi2Sr2CaCu2Oz	Hg0.5I1Bi2Sr2Ca1Cu2OZ	Hg	0.5	I	1	Bi	2	Sr	2	Ca	1	Cu	2									O	Z			1996																												Bi2212			A			44.9	3											K				82			82																																				A	Hao-Clem model			8.6	A	Hao-Clem model		3197																																																			1	The polycrystalline Bi2212 pellet and mercuric iodine (mole ratio of 1:5),together with free iodine (1.5 atm) were heated in an evacurated Pyrex tube.					Effect of HgI2 intercalation on Bi2Sr2CaCu2Oy: Interlayer coupling effect	05		Department of physics, pohang University of Science and Technology,San 31 Hyojadong, Pohang, Kyugbuk, 790-784,Republic of Korea	Phys.Rev.B,53(1996)12416	Dong-Hoon Kim,Jin-Ho Choy,Mayoung-Kwang Bae,Mun-Seog Kim,Nam-Gyu Park,Seong-Ju Hwang,Sung-IK Lee	Bi, Sr, Ca, Cu, Hg, I	
12804	PR05311855		YbBa2Cu3O9.97	Yb1Ba2Cu3O6.97	Yb	1	Ba	2	Cu	3															O		6.97	1	1996																												Y123																		K		88					88			K/GPa	-0.5																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12805	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.995Pr0.05Ba2Cu3O6.97	Yb	0.995	Pr	0.05	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		89.5					89.5			K/GPa	0.2																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12806	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.925Pr0.075Ba2Cu3O6.97	Yb	0.925	Pr	0.075	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		89					89			K/GPa	0.35																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12807	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.9Pr0.1Ba2Cu3O6.97	Yb	0.9	Pr	0.1	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		88.5					88.5			K/GPa	0.45																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12808	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.85Pr0.15Ba2Cu3O6.97	Yb	0.85	Pr	0.15	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		86.5					86.5			K/GPa																																																																																												1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12809	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O6.97	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		82					82			K/GPa	-0.55																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12810	PR05311855		(Yb,Pr)Ba2Cu3O7	Yb0.7Pr0.3Ba2Cu3O6.97	Yb	0.7	Pr	0.3	Ba	2	Cu	3													O		6.97	1	1996																												Y123																		K		73.5					73.5			K/GPa	-1.75																																																																																											1	Polycrystals were prepared by the standard solid-state reaction technique.All samples are annealed in flowing oxgen at 400 Cfor 8 hours.					Pressure effect on Tc for (Yb1-xPrx)Ba2Cu3O7	05		Department of Physics,National Taiwan University, Taipei, Taiwan,republic of China	Phys.Rev.B,53(1996)11855	C.W. Chu,C.Y. Huang,J.C. Ho,J.G. Lin,X.L. Cheng,Y.Y. Xue	Yb, Pr, Ba, Cu, O	
12811	PR05312410		Bi2(Sr,La)2CuOz	Bi2Sr1.8La0.2Cu1Oz	Bi	2	Sr	1.8	La	0.2	Cu	1													O	z		1	1996																												Bi2201			A	5.376	5.372	24.536	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12812	PR05312410		Bi2(Sr,La)2(Cu,Co)Oz	Bi2Sr1.8La0.2Cu0.8Co0.2Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.8	Co	0.2											O	z		1	1996																												Bi2201			A	5.395	5.378	24.196	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12813	PR05312410		Bi2(Sr,La)2(Cu,Co)Oz	Bi2Sr1.8La0.2Cu0.6Co0.4Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.6	Co	0.4											O	z		1	1996																												Bi2201			A	5.414	5.399	24.015	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12814	PR05312410		Bi2(Sr,La)2(Cu,Co)Oz	Bi2Sr1.8La0.2Cu0.4Co0.6Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.4	Co	0.6											O	z		1	1996																												Bi2201			A	5.416	5.403	23.695	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12815	PR05312410		Bi2(Sr,La)2(Cu,Co)Oz	Bi2Sr1.8La0.2Cu0.2Co0.8Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.2	Co	0.8											O	z		1	1996																												Bi2201			A	5.436	5.425	23.383	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12816	PR05312410		Bi2(Sr,La)2CoOz	Bi2Sr1.8La0.2Co1Oz	Bi	2	Sr	1.8	La	0.2	Co	1													O	z		1	1996																												Bi2201			A	5.458	5.435	23.306	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12817	PR05312410		Bi2(Sr,La)(Cu,Fe)Oz	Bi2Sr1.8La0.2Cu0.8Fe0.2Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.8	Fe	0.2											O	z		1	1996																												Bi2201			A	5.385	5.376	24.17	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12818	PR05312410		Bi2(Sr,La)2(Cu,Fe)Oz	Bi2Sr1.8La0.2Cu0.7Fe0.3Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.7	Fe	0.3											O	z		1	1996																												Bi2201			A	5.396	5.384	23.917	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12819	PR05312410		Bi2(Sr,La)2(Cu,Fe)Oz	Bi1Sr1.8La0.2Cu0.6Fe0.4Oz	Bi	1	Sr	1.8	La	0.2	Cu	0.6	Fe	0.4											O	z		1	1996																												Bi2201			A	5.416	5.396	23.828	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12820	PR05312410		Bi2(Sr,La)2(Cu,Fe)Oz	Bi2Sr1.8La0.2Cu0.5Fe0.5Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.5	Fe	0.5											O	z		1	1996																												Bi2201			A	5.432	5.413	23.704	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12821	PR05312410		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La0.2Cu0.98Ni0.02Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.98	Ni	0.02											O	z		1	1996																												Bi2201			A	5.379	5.373	24.53	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12822	PR05312410		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La0.2Cu0.96Ni0.04Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.96	Ni	0.04											O	z		1	1996																												Bi2201			A	5.382	5.375	24.522	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12823	PR05312410		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La0.2Cu0.94Ni0.06Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.94	Ni	0.06											O	z		1	1996																												Bi2201			A	5.384	5.378	24.485	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12824	PR05312410		Bi2(Sr,La)2(Cu,Ni)Oz	Bi2Sr1.8La0.2Cu0.92Ni0.08Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.92	Ni	0.08											O	z		1	1996																												Bi2201			A	5.387	5.38	24.403	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12825	PR05312410		Bi2(Sr,La)(Cu,Ni)Oz	Bi2Sr1.8La0.2Cu0.9Ni0.1Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.9	Ni	0.1											O	z		1	1996																												Bi2201			A	5.396	5.39	24.389	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12826	PR05312410		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.98Zn0.02Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.98	Zn	0.02											O	z		1	1996																												Bi2201			A	5.378	5.373	25.515	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12827	PR05312410		Bi2(Sr,La)(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.96Zn0.04Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.96	Zn	0.04											O	z		1	1996																												Bi2201			A	5.384	5.376	24.493	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12828	PR05312410		Bi2(Sr,La)(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.94Zn0.06Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.94	Zn	0.06											O	z		1	1996																												Bi2201			A	5.386	5.377	24.394	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12829	PR05312410		Bi2(Sr,La)(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.92Zn0.08Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.92	Zn	0.08											O	z		1	1996																												Bi2201			A	5.389	5.379	24.38	3																																																																																																																Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12830	PR05312410		Bi2(Sr,La)2(Cu,Zn)Oz	Bi2Sr1.8La0.2Cu0.9Zn0.1Oz	Bi	2	Sr	1.8	La	0.2	Cu	0.9	Zn	0.1											O	z		1	1996																												Bi2201																																																																																																																							Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO	1	Mix(Bi2O3,SrCO3,La2O3,Fe2O3,NiO,ZnO,CuO)-Heat(810-850C,36h)-Pelletize-Sin(885-930C,in flowing oxgen)					Modulation structure in Bi2Sr1.8La0.2Cu1-xMxOy (M=Fe, Co, Ni, and Zn)	05		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui,230026,People's Republic of China	Phys.Rev.B,53(1996)12410	Mao. Zhiqiang,Tian Mingliang,Wang Yu,Xu Cunyi,Xu Gaojie,Zhang Yuheng,Zhu Jingsheng,Zuo Jian	Bi, Sr, La, Cu, O, Fe, Co, Ni, Zn	
12831	PR05311340		(Pr,Ca)Sr2(Cu,Mo)3O7	Pr0.95Ca0.05Sr2Cu2.7Mo0.3O7-z	Pr	0.95	Ca	0.05	Sr	2	Cu	2.7	Mo	0.3											O	7-z		1	1996																											2	Y123	P4/mmm																	K	17						17																																																																																															1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12832	PR05311340		(Pr,Ca)Sr2(Cu,Mo)3O7	Pr0.9Ca0.1Sr2Cu2.7Mo0.3O7-z	Pr	0.9	Ca	0.1	Sr	2	Cu	2.7	Mo	0.3											O	7-z		1	1996					Bohr magne	3.52																					2	Y123	P4/mmm		A	3.857	3.857	11.624	3											K	8	17	24	20			17																																																								mJ/Pr mol	227																																						1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12833	PR05311340		(Pr,Ca)Sr2(Cu,Mo)3O7	Pr0.85Ca0.15Sr2Cu2.7Mo0.3O7-z	Pr	0.85	Ca	0.15	Sr	2	Cu	2.7	Mo	0.3											O	7-z		1	1996																											2	Y123	P4/mmm																	K	8	16	24				16																																																																																															1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12834	PR05311340		(Pr,Sr)Sr2(Cu,Mo))3O7	Pr0.95Sr2.05Cu2.7Mo0.3O7-z	Pr	0.95	Sr	2.05	Cu	2.7	Mo	0.3													O	7-z		1	1996																											2	Y123	P4/mmm																	K		13	20				13																																																																																															1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12835	PR05311340		(Pr,Sr)Sr2(Cu,Mo)3O7	Pr0.9Sr2.1Cu2.7Mo0.3O7-z	Pr	0.9	Sr	2.1	Cu	2.7	Mo	0.3													O	7-z		1	1996					Bohr magne	3.52																					2	Y123	P4/mmm		A	3.863	3.863	11.624	3											K	13	17	25				17																																																								mJ/Pr mol	221																																						1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12836	PR05311340		(Pr,Sr)Sr2(Cu,Mo)3O7	Pr0.85Sr2.15Cu2.7Mo0.3O7-z	Pr	0.85	Sr	2.15	Cu	2.7	Mo	0.3													O	7-z		1	1996																											2	Y123	P4/mmm																	K	15	17	25				17																																																																																															1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12837	PR05311340		(Pr,Sr)Sr2(Cu,Mo)3O7	Pr0.8Sr2.2Cu2.7Mo0.3O7-z	Pr	0.8	Sr	2.2	Cu	2.7	Mo	0.3													O	7-z		1	1996																											2	Y123	P4/mmm																	K	15	21	28				21																																																																																															1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12838	PR05311340		PrSr2(Cu,Mo)3O7	Pr1Sr2Cu2.7Mo0.3O7-z	Pr	1	Sr	2	Cu	2.7	Mo	0.3													O	7-z		1	1996					Bohr magne	3.05																					2	Y123	P4/mmm		A	3.858	3.858	11.616	3																																																																										mJ/Pr mol	212																																						1	All polycrystalline samples were prepared by the solid-state rreaction method.					Occurrence of superconductivity in Ca-and Sr-doped PrSr2Cu2.7Mo0.3O7-z	05		Department of Electrical Engineering, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, Republic of China	Phys.Rev.B,53(1996)11340	F.L. Juang,H.D. Yang,H.L. Tsay,W.M. Wang,Y.C. Chen	Ca, Pr, Sr, Cu, Mo, O	
12839	PR05311825			Pb0.26Bi1.74Sr1.85Ca0.9Cu1.95Oz	Pb	0.26	Bi	1.74	Sr	1.85	Ca	0.9	Cu	1.95											O	z		3	1996																												Bi2212																		K			68				68																																									A	Hao-Clem model		1900																																																			5	Grow by a self-flux method in almina crucibles-Anneal (in O2 300bar,440C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12840	PR05311825			Pb0.38Bi1.75Sr1.75Ca1.1Cu2Oz	Pb	0.38	Bi	1.75	Sr	1.75	Ca	1.1	Cu	2											O	z		3	1996																												Bi2212																		K			89				89																																									A	Hao-Clem model		2200																																																			5	Grow by a self-flux method in almina crucibles-Anneal(in Ar(sample no. 12841),in O2(sample no. 12842),550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12841	PR05311825			Pb0.38Bi1.75Sr1.75Ca1.1Cu2Oz	Pb	0.38	Bi	1.75	Sr	1.75	Ca	1.1	Cu	2											O	z		3	1996																												Bi2212																		K			87				87																																									A	Hao-Clem model		2300																																																			5	Grow by a self-flux method in almina crucibles-Anneal(in Ar(sample no. 12841),in O2(sample no. 12842),550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12842	PR05311825			Pb0.38Bi1.75Sr1.75Ca1.1Cu2Oz	Pb	0.38	Bi	1.75	Sr	1.75	Ca	1.1	Cu	2											O	z		3	1996																												Bi2212																		K			71.5				71.5																																									A	Hao-Clem model		2000																																																			5	Grow by a self-flux method in almina crucibles-Anneal(in Ar(sample no. 12841),in O2(sample no. 12842),550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12843	PR05311825			Bi2.1Sr1.9Ca0.74Cu2Oz	Bi	2.1	Sr	1.9	Ca	0.74	Cu	2													O	z		3	1996																												Bi2212																		K			88				88																																									A	Hao-Clem model		2700																																																			5	Grow by a self-flux method in gold crucibles-Anneal in O2(sample no. 12844),550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12844	PR05311825			Bi2.1Sr1.9Ca0.74Cu2Oz	Bi	2.1	Sr	1.9	Ca	0.74	Cu	2													O	z		3	1996																												Bi2212																		K			80				80																																									A	Hao-Clem model		2250																																																			5	Grow by a self-flux method in gold crucibles-Anneal in O2(sample no. 12844),550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12845	PR05311825			Bi2.1Sr1.7Ca1.1Cu2Oz	Bi	2.1	Sr	1.7	Ca	1.1	Cu	2													O	z		3	1996																												Bi2212																		K			94				94																																									A	Hao-Clem model		2050																																																			5	Grow by a self flux method in gold crucibles-Anneal(in Ar(sample no.12846),in O2(sample no.12847,550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12846	PR05311825			Bi2.1Sr1.7Ca1.1Cu2OZ	Bi	2.1	Sr	1.7	Ca	1.1	Cu	2													O	Z		3	1996																												Bi2212																		K			80				80																																									A	Hao-Clem model		2700																																																			5	Grow by a self flux method in gold crucibles-Anneal(in Ar(sample no.12846),in O2(sample no.12847,550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12847	PR05311825			Bi2.1Sr1.7Ca1.1Cu2OZ	Bi	2.1	Sr	1.7	Ca	1.1	Cu	2													O	Z		3	1996																												Bi2212																		K			85.5				85.5																																									A	Hao-Clem model		1950																																																			5	Grow by a self flux method in gold crucibles-Anneal(in Ar(sample no.12846),in O2(sample no.12847,550-650C,4-8days)					Temperature and doping dependence of the penetrasion depth in Bi2Sr2CaCu2O8+z	05		Walther-Mei%!ner-Institut,Walther-Mei%!ner-Strasse 8, D-85748 Garching, Germany	Phys.Rev.B,53(1996)11825	"F. Steinmeyer,F.X. Re'gi,H. Savary,J. Schneck,J.J. Neumeier,O. Waldmann,P. Mu""ller"	Bi, Sr, Ca, Cu, O	
12848	PR05311324		(La,Sr)2CuO4	La1.885Sr0.115Cu1O4	La	1.885	Sr	0.115	Cu	1															O	4		1	1996																												T																		K				29.5			29.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12849	PR05311324		(La,Nd,Sr)2CuO4	La1.845Nd0.04Sr0.115Cu1O4	La	1.845	Nd	0.04	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				28.5			28.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12850	PR05311324		(La,Nd,Sr)2CuO4	La1.805Nd0.08Sr0.115Cu1O4	La	1.805	Nd	0.08	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				27.5			27.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12851	PR05311324		(La,Nd,Sr)2CuO4	La1.785Nd0.1Sr0.115Cu1O4	La	1.785	Nd	0.1	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				27			27																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12852	PR05311324		(La,Nd,Sr)2CuO4	La1.76Nd0.125Sr0.115Cu1O4	La	1.76	Nd	0.125	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				25.5			25.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12853	PR05311324		(La,Nd,Sr)2CuO4	La1.745Nd0.14Sr0.115Cu1O4	La	1.745	Nd	0.14	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				17.5			17.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12854	PR05311324		(La,Nd,Sr)2CuO4	La1.735Nd0.15Sr0.115Cu1O4	La	1.735	Nd	0.15	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				16.5			16.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12855	PR05311324		(La,Nd,Sr)2CuO4	La1.685Nd0.2Sr0.115Cu1O4	La	1.685	Nd	0.2	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				11			11																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12856	PR05311324		(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		1	1996																												T																		K				32			32																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12857	PR05311324		(La,Nd,Sr)2CuO4	La1.835Nd0.04Sr0.125Cu1O4	La	1.835	Nd	0.04	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				32			32																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12858	PR05311324		(La,Nd,Sr)2CuO4	La1.795Nd0.08Sr0.125Cu1O4	La	1.795	Nd	0.08	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				29.5			29.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12859	PR05311324		(La,Nd,Sr)2CuO4	La1.775Nd0.1Sr0.125Cu1O4	La	1.775	Nd	0.1	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				27			27																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12860	PR05311324		(La,Nd,Sr)2CuO4	La1.75Nd0.125Sr0.125Cu1O4	La	1.75	Nd	0.125	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				17.5			17.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12861	PR05311324		(La,Nd,Sr)2CuO4	La1.735Nd0.14Sr0.125Cu1O4	La	1.735	Nd	0.14	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				15			15																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12862	PR05311324		(La,Nd,Sr)2CuO4	La1.725Nd0.15Sr0.125Cu1O4	La	1.725	Nd	0.15	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				12.5			12.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12863	PR05311324		(La,Nd,Sr)2CuO4	La1.675Nd0.2Sr0.125Cu1O4	La	1.675	Nd	0.2	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				10.5			10.5																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12864	PR05311324		(La,Nd,Sr)2CuO4	La1.575Nd0.3Sr0.125Cu1O4	La	1.575	Nd	0.3	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				9			9																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12865	PR05311324		(La,Nd,Sr)2CuO4	La1.775Nd0.125Sr0.1Cu1O4	La	1.775	Nd	0.125	Sr	0.1	Cu	1													O		4	1	1996																												T																		K				26			26																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12866	PR05311324		(La,Nd,Sr)2CuO4	La1.765Nd0.125Sr0.11Cu1O4	La	1.765	Nd	0.125	Sr	0.11	Cu	1													O		4	1	1996																												T																		K				26			26																																																													mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12867	PR05311324		(La,Nd,Sr)2CuO4	La1.76Nd0.125Sr0.115Cu1O4	La	1.76	Nd	0.125	Sr	0.115	Cu	1													O		4	1	1996																												T																		K				25.5			25.5																																																													mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12868	PR05311324		(La,Nd,Sr)2CuO4	La1.75Nd0.125Sr0.125Cu1O4	La	1.75	Nd	0.125	Sr	0.125	Cu	1													O		4	1	1996																												T																		K				17.5			17.5																																																													mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12869	PR05311324		(La,Nd,Sr)2CuO4	La1.74Nd0.125Sr0.135Cu1O4	La	1.74	Nd	0.125	Sr	0.135	Cu	1													O		4	1	1996																												T																		K				21			21																																																													mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12870	PR05311324		(La,Nd,Sr)2CuO4	La1.725Nd0.125Sr0.15Cu1O4	La	1.725	Nd	0.125	Sr	0.15	Cu	1													O		4	1	1996																												T																		K				33.5			33.5																																																													mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12871	PR05311324		(La,Nd,Sr)2CuO4	La1.715Nd0.125Sr0.16Cu1O4	La	1.715	Nd	0.125	Sr	0.16	Cu	1													O		4	1	1996																												T																		K				35			35																																																																																															1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12872	PR05311324		(La,Nd,Sr)2CuO4	La1.695Nd0.125Sr0.18Cu1O4	La	1.695	Nd	0.125	Sr	0.18	Cu	1													O		4	1	1996																												T																																																																																						mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
12873	PR05311324		(La,Nd,Sr)2CuO4	La1.675Nd0.125Sr0.2Cu1O4	La	1.675	Nd	0.125	Sr	0.2	Cu	1													O		4	1	1996																												T																																																																																						mW/K.cm																																		1					see Phys. Soc Jpn 63 (1994) 2314	Suppression of the superconcting transition temperature Tc around x-0.115 in La2-xSrxCuO4	05		Institute for Materials Research, Tohoku University, Sendai 980, Japan	Phys.Rev.B,53(1996)11324	M. Hiroi,M. Maki,M. Sera,N. Kobayashi	La, Sr, Cu, O	
13000	PR05503410		Bi2Sr2CaCu2O8	Bi2Sr1.9Ca1Cu1.8O8+y	Bi	2	Sr	1.9	Ca	1	Cu	1.8													O	8+y		3	1997																												Bi2212																		K			85				85																																														meV	26	7																																															5	self-flux (Al2O3 or ZrO2 crucibles)					Superconducting order parameter in partially substituted Bi2Sr2CaCu2O8+x single crystals as measured by the tunneling effect	199702		Universite' Libre de Bruxelles, Service de Physique des Solides, CP233, Boulevard du Triomphe, B-1050 Brussels, Belgium	Phys.Rev.B,55(1997)R3410	A.G.M. Jansen,D.N. Davydov,H. Hancotte,P. Wyder,R. Deltour		
13001	PR05503410		Bi2Sr2Ca(Cu,Ni)2O8	Bi2Sr1.95Ca0.95Cu2.01Ni0.04O8+y	Bi	2	Sr	1.95	Ca	0.95	Cu	2.01	Ni	0.04											O	8+y		3	1997																												Bi2212																		K			75				75																																														meV	38.5	11.9																																															5	self-flux (Al2O3 or ZrO2 crucibles)					Superconducting order parameter in partially substituted Bi2Sr2CaCu2O8+x single crystals as measured by the tunneling effect	199702		Universite' Libre de Bruxelles, Service de Physique des Solides, CP233, Boulevard du Triomphe, B-1050 Brussels, Belgium	Phys.Rev.B,55(1997)R3410	A.G.M. Jansen,D.N. Davydov,H. Hancotte,P. Wyder,R. Deltour		
13002	PR05503410		Bi2Sr2Ca(Cu,Zn)2O8	Bi2Sr2Ca1Cu1.98Zn0.02O8+y	Bi	2	Sr	2	Ca	1	Cu	1.98	Zn	0.02											O	8+y		3	1997																												Bi2212																		K			79				79																																														meV	25																																																5	self-flux (Al2O3 or ZrO2 crucibles)					Superconducting order parameter in partially substituted Bi2Sr2CaCu2O8+x single crystals as measured by the tunneling effect	199702		Universite' Libre de Bruxelles, Service de Physique des Solides, CP233, Boulevard du Triomphe, B-1050 Brussels, Belgium	Phys.Rev.B,55(1997)R3410	A.G.M. Jansen,D.N. Davydov,H. Hancotte,P. Wyder,R. Deltour		
13003	PR05503390		(Y,Pr)Ba2Cu3O7	Y0.87Pr0.13Ba2Cu3O7-d	Y	0.87	Pr	0.13	Ba	2	Cu	3													O	7-d		3	1997																												Y123																		K			85				85																																																																							m.ohm.cm								0.12	100																Ref. L. M. Paulius, B. W. Lee, M. B. Maple, and P. K. Tsai, Physica C 230,255(1994)					Nonmonotonic evolution of out-of-plane resistivity with Pr doping in Y1-xPrxBa2Cu3O7-delta single crystals	199702		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.B,55(1997)R3390	A.R. Baldwin,C.C. Almasan,C.N. Jiang,D.A. Gajewski,G.A. Levin,M.B. Maple,S.H. Han,T. Stein		
13004	PR05503390		(Y,Pr)Ba2Cu3O7	Y0.78Pr0.22Ba2Cu3O7-d	Y	0.78	Pr	0.22	Ba	2	Cu	3													O	7-d		3	1997																												Y123																		K			70				70																																																																							m.ohm.cm					0.12	50	0.26	65																	Ref. L. M. Paulius, B. W. Lee, M. B. Maple, and P. K. Tsai, Physica C 230,255(1994)					Nonmonotonic evolution of out-of-plane resistivity with Pr doping in Y1-xPrxBa2Cu3O7-delta single crystals	199702		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.B,55(1997)R3390	A.R. Baldwin,C.C. Almasan,C.N. Jiang,D.A. Gajewski,G.A. Levin,M.B. Maple,S.H. Han,T. Stein		
13005	PR05503390		(Y,Pr)Ba2Cu3O7	Y0.58Pr0.42Ba2Cu3O7-d	Y	0.58	Pr	0.42	Ba	2	Cu	3													O	7-d		3	1997																												Y123																		K			40				40																																																																							m.ohm.cm					0.23	185		0.51	100																Ref. L. M. Paulius, B. W. Lee, M. B. Maple, and P. K. Tsai, Physica C 230,255(1994)					Nonmonotonic evolution of out-of-plane resistivity with Pr doping in Y1-xPrxBa2Cu3O7-delta single crystals	199702		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.B,55(1997)R3390	A.R. Baldwin,C.C. Almasan,C.N. Jiang,D.A. Gajewski,G.A. Levin,M.B. Maple,S.H. Han,T. Stein		
13006	PR05503390		(Y,Pr)Ba2Cu3O7	Y0.47Pr0.53Ba2Cu3O7-d	Y	0.47	Pr	0.53	Ba	2	Cu	3													O	7-d		3	1997																																														K			8				8																																																																							m.ohm.cm					0.5	155		0.7	65																Ref. L. M. Paulius, B. W. Lee, M. B. Maple, and P. K. Tsai, Physica C 230,255(1994)					Nonmonotonic evolution of out-of-plane resistivity with Pr doping in Y1-xPrxBa2Cu3O7-delta single crystals	199702		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.B,55(1997)R3390	A.R. Baldwin,C.C. Almasan,C.N. Jiang,D.A. Gajewski,G.A. Levin,M.B. Maple,S.H. Han,T. Stein		
13007	PR05503390	non-superconductor	(Y,Pr)Ba2Cu3O7	Y0.45Pr0.55Ba2Cu3O7-d	Y	0.45	Pr	0.55	Ba	2	Cu	3													O	7-d		3	1997																												Y123																																																																																																m.ohm.cm		2.9	500		0.75	140		1.18	40																Ref. L. M. Paulius, B. W. Lee, M. B. Maple, and P. K. Tsai, Physica C 230,255(1994)					Nonmonotonic evolution of out-of-plane resistivity with Pr doping in Y1-xPrxBa2Cu3O7-delta single crystals	199702		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.B,55(1997)R3390	A.R. Baldwin,C.C. Almasan,C.N. Jiang,D.A. Gajewski,G.A. Levin,M.B. Maple,S.H. Han,T. Stein		
13008	PR05503374	magnetic superconductor	(Eu,Ce)2RuSr2Cu2O10	Eu1.4Ce0.6Ru1Sr2Cu2O10-d	Eu	1.4	Ce	0.6	Ru	1	Sr	2	Cu	2											O	10-d		1	1997								122.1																			2	Ru1222	I4/mmm		A	3.846		2.85	3											K				32			32																																														meV	9																																																1						Coexistence of magnetism and superconductivity in R1.4Ce0.6RuSr2Cu2O10-z (R=Eu and Gd)	199702		Racah Institute of Physics,The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B,55(1997)R3374	I. Felner,O. Millo,U. Asaf,Y. Levi		
13009	PR05503374	magnetic superconductor	(Gd,Ce)2RuSr2Cu2O10	Gd1.4Ce0.6Ru1Sr2Cu2O10-d	Gd	1.4	Ce	0.6	Ru	1	Sr	2	Cu	2											O	10-d		1	1997								180.5																			2	M2212	I4/mmm		A	3.844		28.621	3											K				42			42																																														meV	7.7																																																1						Coexistence of magnetism and superconductivity in R1.4Ce0.6RuSr2Cu2O10-z (R=Eu and Gd)	199702		Racah Institute of Physics,The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B,55(1997)R3374	I. Felner,O. Millo,U. Asaf,Y. Levi		
13010	PR05503929		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O		8	3	1997																												Tl2212																		K				103			103																													T/K			2.6																																																																A. Maignan et al. Physica 219,407(1994)M. Ledesert et al. Physica C232.387(1994)					Scaling behavior of conductivity and nagnetization in high-temperature superconductors	199702		Universite' de Tours, LEMA(Laboratoire d'Electrodynamique des Materiaux Avance's), UFR de Sciences, Parc Grandmont, 37200 Tours, France	Phys.Rev.B,55(1997)3929	A. Maignan,A. Wahl,Ch. Simon,F. Warmont,M.P. Delamare,V. Hardy		
13011	PR05503929		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O		7	3	1997																												Y123																		K				92			92																													T/K			1.9																																																																MTG techniqueM. P. Delamare et al. Physica C262,381(1996)					Scaling behavior of conductivity and nagnetization in high-temperature superconductors	199702		Universite' de Tours, LEMA(Laboratoire d'Electrodynamique des Materiaux Avance's), UFR de Sciences, Parc Grandmont, 37200 Tours, France	Phys.Rev.B,55(1997)3929	A. Maignan,A. Wahl,Ch. Simon,F. Warmont,M.P. Delamare,V. Hardy		
13012	PR05503929		(Tl,Bi)Si2CaCu2O7	Tl1Bi1Sr2Ca1Cu2O7	Tl	1	Bi	1	Sr	2	Ca	1	Cu	2											O		7	3	1997																												Tl1212																		K				86			86																													T/K			2.2																																																																A. Maignan et al. Physica 219,407(1994)M. Ledesert et al. Physica C232.387(1994)					Scaling behavior of conductivity and nagnetization in high-temperature superconductors	199702		Universite' de Tours, LEMA(Laboratoire d'Electrodynamique des Materiaux Avance's), UFR de Sciences, Parc Grandmont, 37200 Tours, France	Phys.Rev.B,55(1997)3929	A. Maignan,A. Wahl,Ch. Simon,F. Warmont,M.P. Delamare,V. Hardy		
13013	PR05503954	twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																		K				93.1		0.2	93.1																																																					SP13013			mJ/molK2	3.23																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13014	PR05503954	un-twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																																																																														SP13014			mJ/molK2	2.2																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13015	PR05503954	un-twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																																																																														SP13015			mJ/molK2	2																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13016	PR05503954	un-twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																																																																														SP13016			mJ/molK2	1.2																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13017	PR05503954	twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																																																																																	mJ/molK2	3																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13018	PR05503954	un-twin sample	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1997																												Y123																																																																														SP13018			mJ/molK2	2.4																																						5						Specific heat of YBa2Cu3O7-z	199702		Departments of Physics and Applied Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,55(1997)3954	Aharon Kapitulnik,David J. Baar,Devid L. Sisson,Jeffrey S. Urbach,Kathryn A. Moler,Malcolm R. Beasley,Ruixing Liang,Walter N. Hardy		
13019	PR05503297	non-superconductorsurpressed  by Pr's antferromagnetic order	(Pr,Ce)2Sr2NbCu2O10	Pr1.5Ce0.5Sr2Cu2Nb1O10-d	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-d		1	1997	emu/cc		emu.K/cc	0.011			16.94																				2	M2212	I4/mmm		A	3.887		28.762	3																																																																							SP13019																																										1						Pr and Cu magnetism in (Pr1.5Ce0.5)Sr2Cu2MO10-delta (M=Nb,Ta): Correlations with a suppression of superconductivity	199702		Department of Physics, University of California, Davis, California 95616	Phys.Rev.B,55(1997)3297	H.B. Radousky,J.W. Lynn,N. Rosov,R.N. Shelton,T.J. Goodwin		
13020	PR05503297	non-superconductorsurpressed  by Pr's antferromagnetic order	(Pr,Ce)2Sr2NbCu2O10	Pr1.5Ce0.5Sr2Cu2Nb1O10-d	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-d		1	1997	emu/cc		emu.K/cc	0.011			15.4																				2	M2212	I4/mmm		A	3.892		28.846	3																																																																																																																	1	deoxygenated Ar-gas (700C 2days)					Pr and Cu magnetism in (Pr1.5Ce0.5)Sr2Cu2MO10-delta (M=Nb,Ta): Correlations with a suppression of superconductivity	199702		Department of Physics, University of California, Davis, California 95616	Phys.Rev.B,55(1997)3297	H.B. Radousky,J.W. Lynn,N. Rosov,R.N. Shelton,T.J. Goodwin		
13021	PR05503297	non-superconductorsurpressed  by Pr's antferromagnetic order	(Pr,Ce)2Sr2TaCu2O10	Pr1.5Ce0.5Sr2Cu2Ta1O10-d	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Ta	1											O	10-d		1	1997	emu/cc		emu.K/cc	0.012			19.1																				2	M1222	I4/mmm		A	3.885		28.844	3																																																																																																																	1						Pr and Cu magnetism in (Pr1.5Ce0.5)Sr2Cu2MO10-delta (M=Nb,Ta): Correlations with a suppression of superconductivity	199702		Department of Physics, University of California, Davis, California 95616	Phys.Rev.B,55(1997)3297	H.B. Radousky,J.W. Lynn,N. Rosov,R.N. Shelton,T.J. Goodwin		
13022	PR05503297	non-superconductorsurpressed  by Pr's antferromagnetic order	(Pr,Ce)2Sr2TaCu2O10	Pr1.5Ce0.5Sr2Cu2Ta1O10-d	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Ta	1											O	10-d		1	1997	emu/cc		emu.K/cc	0.011			16.2																				2	M1222	I4/mmm		A	3.89		28.91	3																																																																																																																	1	deoxygenated Ar-gas (700C 2days)					Pr and Cu magnetism in (Pr1.5Ce0.5)Sr2Cu2MO10-delta (M=Nb,Ta): Correlations with a suppression of superconductivity	199702		Department of Physics, University of California, Davis, California 95616	Phys.Rev.B,55(1997)3297	H.B. Radousky,J.W. Lynn,N. Rosov,R.N. Shelton,T.J. Goodwin		
13023	PR05503297	non-superconductorsurpressed  by Pr's antferromagnetic order	(Eu,Ce)Sr2NbCu2O10	Eu1.5Ce0.5Sr2Cu2Nb1O10-d	Eu	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10-d		1	1997																											2	M2212	I4/mmm		A	3.866		28.756	3																																																																							SP13023			mJ/molK2	4.669		405.1																																				1						Pr and Cu magnetism in (Pr1.5Ce0.5)Sr2Cu2MO10-delta (M=Nb,Ta): Correlations with a suppression of superconductivity	199702		Department of Physics, University of California, Davis, California 95616	Phys.Rev.B,55(1997)3297	H.B. Radousky,J.W. Lynn,N. Rosov,R.N. Shelton,T.J. Goodwin		
13024	PR05503966		HgBa2CuO4+z	Hg1Ba2Cu1O4.06	Hg	1	Ba	2	Cu	1															O		4.06	1	1997																											2	Hg1201			A	3.886		9.532	4											K		71					71																																																																																														HgO,Ba2CuO3+x	1	Annealed 24 hours Ar flow 350C					Precision neutron-diffraction study of the high-Tc superconductor HgBa2CuO4+delta	199702		JINR, FLNP, 141980 Dubna, Russia	Phys.Rev.B,55(1997)3966	A.A. Gippius,A.M. Balagurov,D.A. Mikhailova,E.V. Antipov,S.N. Putilin,V.A. Alyoshin,V.G. Simkin,V.L. Aksenov,V.V. Sikolenko		
13025	PR05503966		HgBa2CuO4+z	Hg1Ba2Cu1O4.19	Hg	1	Ba	2	Cu	1															O		4.19	1	1997																											2	Hg1201			A	3.88		9.524	4											K		83					83																																																																																														HgO,Ba2CuO3+x	1	Annealed 24 hours high O2 pressure 250C					Precision neutron-diffraction study of the high-Tc superconductor HgBa2CuO4+delta	199702		JINR, FLNP, 141980 Dubna, Russia	Phys.Rev.B,55(1997)3966	A.A. Gippius,A.M. Balagurov,D.A. Mikhailova,E.V. Antipov,S.N. Putilin,V.A. Alyoshin,V.G. Simkin,V.L. Aksenov,V.V. Sikolenko		
13026	PR05503966		HgBa2CuO4+z	Hg1Ba2Cu1O4.12	Hg	1	Ba	2	Cu	1															O		4.12	1	1997																											2	Hg1201			A	3.885		9.526	4											K		98					98																																																																																														HgO,Ba2CuO3+x	1	Annealed 24 hours O2 flow 250C					Precision neutron-diffraction study of the high-Tc superconductor HgBa2CuO4+delta	199702		JINR, FLNP, 141980 Dubna, Russia	Phys.Rev.B,55(1997)3966	A.A. Gippius,A.M. Balagurov,D.A. Mikhailova,E.V. Antipov,S.N. Putilin,V.A. Alyoshin,V.G. Simkin,V.L. Aksenov,V.V. Sikolenko		
13027	PR05503966		HgBa2CuO4	Hg1Ba2Cu1O4+x	Hg	1	Ba	2	Cu	1															O	4+x		2	1997																											2	Hg1201			A	3.885		9.52	4											K		96					96																																																																																														HgO,Ba2CuO3+x	1	Annealed 24 hours O2 flow 250C					Precision neutron-diffraction study of the high-Tc superconductor HgBa2CuO4+delta	199702		JINR, FLNP, 141980 Dubna, Russia	Phys.Rev.B,55(1997)3966	A.A. Gippius,A.M. Balagurov,D.A. Mikhailova,E.V. Antipov,S.N. Putilin,V.A. Alyoshin,V.G. Simkin,V.L. Aksenov,V.V. Sikolenko		
13028	PR05503935		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-d	Nd	1.85	Ce	0.15	Cu	1															O	4-d		2	1997																											2	T'			A	3.955		12.124	3											K	17		26	24			24																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13029	PR05503935		(Nd,La,Ce)2CuO4	Nd1.65La0.2Ce0.15Cu1O4-d	Nd	1.65	La	0.2	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.963		12.157	3											K	12		26	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13030	PR05503935		(Nd,La,Ce)2CuO4	Nd1.35La0.5Ce0.15Cu1O4-d	Nd	1.35	La	0.5	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.97		12.209	3											K			26	18			18																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13031	PR05503935		(Nd,La,Ce)2CuO4	Nd1.15La0.7Ce0.15Cu1O4-d	Nd	1.15	La	0.7	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.979		12.249	3											K			26	18			18																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13032	PR05503935		(Nd,La,Ce)2CuO4	Nd0.9La0.95Ce0.15Cu1O4-d	Nd	0.9	La	0.95	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.979		12.267	3											K			26				26																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13033	PR05503935		(Nd,La,Ce)2CuO4	Nd0.85La1Ce0.15Cu1O4-d	Nd	0.85	La	1	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.983		12.3	3											K			26	15			15																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13034	PR05503935		(Nd,La,Ce)2CuO4	Nd0.75La1.1Ce0.15Cu1O4-d	Nd	0.75	La	1.1	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.983		12.303	3											K			26	10			10																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13035	PR05503935		(Nd,La,Ce)2CuO4	Nd0.8La1.1Ce0.1Cu1O4-d	Nd	0.8	La	1.1	Ce	0.1	Cu	1													O	4-d		2	1997																											2	T'			A	3.982		12.317	3											K	15		27	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13036	PR05503935		(Nd,La,Ce)2CuO4	Nd0.78La1.1Ce0.12Cu1O4-d	Nd	0.78	La	1.1	Ce	0.12	Cu	1													O	4-d		2	1997																											2	T'			A	3.987		12.299	3											K	10		26	17			17																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13037	PR05503935		(Nd,La,Ce)2CuO4	Nd0.65La1.1Ce0.25Cu1O4-d	Nd	0.65	La	1.1	Ce	0.25	Cu	1													O	4-d		2	1997																											2	T'			A	3.987		12.234	3											K																																																																																																						1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13038	PR05503935		(Nd,La,Ce)2CuO4	Nd0.65La1.2Ce0.15Cu1O4-d	Nd	0.65	La	1.2	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.988		12.283	3											K			26				26																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13039	PR05503935		(Nd,La,Ce)2CuO4	Nd0.55La1.3Ce0.15Cu1O4-d	Nd	0.55	La	1.3	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.995		12.307	3											K																																																																																																						1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13040	PR05503935		(Nd,La,Ce)2CuO4	Nd0.5La1.3Ce0.2Cu1O4-d	Nd	0.5	La	1.3	Ce	0.2	Cu	1													O	4-d		2	1997																											2	T'			A	3.994		12.289	3											K																																																																																																						1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13041	PR05503935		(Nd,La,Ce)2CuO4	Nd0.45La1.3Ce0.25Cu1O4-d	Nd	0.45	La	1.3	Ce	0.25	Cu	1													O	4-d		2	1997																											2	T'			A	3.995		12.271	3											K																																																																																																						1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13042	PR05503935		(Nd,La,Ce)2CuO4	Nd0.45La1.4Ce0.15Cu1O4-d	Nd	0.45	La	1.4	Ce	0.15	Cu	1													O	4-d		2	1997																											2	T'			A	3.994		12.286	3											K																																																																																																						1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13043	PR05503935		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-d	Nd	1.85	Ce	0.15	Cu	1															O	4-d		2	1997																											2	T'			A	3.955		12.124	3											K	17		26	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13044	PR05503935		(Nd,La,Ce)2CuO4	Nd1.66La0.2Ce0.14Cu1O4-d	Nd	1.66	La	0.2	Ce	0.14	Cu	1													O	4-d		2	1997																											2	T'			A	3.961		12.162	3											K	13		26	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13045	PR05503935		(Nd,La,Ce)2CuO4	Nd1.47La0.4Ce0.13Cu1O4-d	Nd	1.47	La	0.4	Ce	0.13	Cu	1													O	4-d		2	1997																											2	T'			A	3.965		12.179	3											K	13		26	22			22																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13046	PR05503935		(Nd,La,Ce)2CuO4	Nd1.22La0.6Ce0.12Cu1O4-d	Nd	1.22	La	0.6	Ce	0.12	Cu	1													O	4-d		2	1997																											2	T'			A	3.969		12.212	3											K	14		26	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13047	PR05503935		(Nd,La,Ce)2CuO4	Nd1.09La0.8Ce0.11Cu1O4-d	Nd	1.09	La	0.8	Ce	0.11	Cu	1													O	4-d		2	1997																											2	T'			A	3.974		12.268	3											K	13		26	24			24																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13048	PR05503935		(Nd,La,Ce)2CuO4	Nd0.9La1Ce0.1Cu1O4-d	Nd	0.9	La	1	Ce	0.1	Cu	1													O	4-d		2	1997																											2	T'			A	3.98		12.311	3											K	15		26	23			23																																																																																															1	Mixed - Sintered 1000C in Air - Pelletized - Sintered 1050C 24h in Air - Sintered 1050C 12h Flowing Dry N2					Relationship between the lattice parameter and superconductivity in the 2-1-4 series n-type cuprates	199702		National Laboratory for Superconductivity, Institute of Physics, and the Center of Condensed Matter Physics, chinese Academy of Sciences,Beijing, 100800,People's Republic of China	Phys.Rev.B,55(1996)3935	Cheng Dong,Cong Wang,Guangcan Che,Hong Chen,Zhiyu Qiao,Zhongxian Zhao		
13049	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.86	Y	1	Ba	2	Cu	3															O		6.86	1	1997																											3	Y123																																																																																						W/K.m	3.45				micro.V/K	3.65																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13050	PR05503155		YBa2Cu3Oz	Y1Ba2Cu2O6.92	Y	1	Ba	2	Cu	2															O		6.92	1	1997																											3	Y123																																																																																						W/K.m	3.9				micro.V/K	0.53																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13051	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.67	Y	1	Ba	2	Cu	3															O		6.67	1	1997																											3	Y123																																																																																						W/K.m	3.1				micro.V/K	11.5																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13052	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O		6.65	1	1997																											3	Y123																																																																																						W/K.m	3.2				micro.V/K	12.7			TP13052																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13053	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.58	Y	1	Ba	2	Cu	3															O		6.58	1	1997																											3	Y123																																																																																						W/K.m	2.9				micro.V/K	22.6																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13054	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.55	Y	1	Ba	2	Cu	3															O		6.55	1	1997																											3	Y123																																																																																						W/K.m	3				micro.V/K	29.8			TP13054																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13055	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.43	Y	1	Ba	2	Cu	3															O		6.43	1	1997																											3	Y123																																																																																						W/K.m	2.9				micro.V/K	49.1																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13056	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O		6.41	1	1997																											3	Y123																																																																																						W/K.m	3				micro.V/K	60.5			TP13056																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13057	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.28	Y	1	Ba	2	Cu	3															O		6.28	1	1997																											2	Y123																																																																																						W/K.m					micro.V/K	118																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13058	PR05503155		YBa2Cu3Oz	Y1Ba2Cu3O6.28	Y	1	Ba	2	Cu	3															O		6.28	1	1997																											2	Y123																																																																																						W/K.m	3.7			THC13058	micro.V/K	119			TP13058																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13059	PR05503155		YBa2Cu3O6.24	Y1Ba2Cu3O6.24	Y	1	Ba	2	Cu	3															O		6.24	1	1997																											2	Y123																																																																																						W/K.m	2.55			THC13059	micro.V/K	144																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13060	PR05503155		YBa2Cu3O6.20	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O		6.2	1	1997																											2	Y123																																																																																						W/K.m	3.1			THC13060	micro.V/K	186			TP13060																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13061	PR05503155		YBa2Cu3O6.20	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O		6.2	1	1997																											2	Y123																																																																																						W/K.m	2.85			THC13061	micro.V/K	188																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13062	PR05503155		YBa2Cu3O6.17	Y1Ba2Cu3O6.17	Y	1	Ba	2	Cu	3															O		6.17	1	1997																											2	Y123																																																																																						W/K.m	3.3			THC13062	micro.V/K	222			TP13062																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13063	PR05503155		YBa2Cu3O6.21	Y1Ba2Cu3O6.21	Y	1	Ba	2	Cu	3															O		6.21	1	1997																											2	Y123																																																																																						W/K.m	2.65			THC13063	micro.V/K	169																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13064	PR05503155		YBa2Cu3O6.18	Y1Ba2Cu3O6.18	Y	1	Ba	2	Cu	3															O		6.18	1	1997																											2	Y123																																																																																						W/K.m	3.3				micro.V/K	209			TP13064																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13065	PR05503155		YBa2Cu3O6.05	Y1Ba2Cu3O6.05	Y	1	Ba	2	Cu	3															O		6.05	1	1997																											2	Y123																																																																																						W/K.m	4.4			THC13065	micro.V/K	584																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13066	PR05503155		YBa2Cu3O6.07	Y1Ba2Cu3O6.07	Y	1	Ba	2	Cu	3															O		6.07	1	1997																											2	Y123																																																																																						W/K.m	4.8			THC13066	micro.V/K	534																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13067	PR05503155		YBa2Cu3O6.86	Y1Ba2Cu3O6.86	Y	1	Ba	2	Cu	3															O		6.86	1	1997																											3	Y123																																																																																						W/K.m	3.6			THC13067	micro.V/K	3.75																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13068	PR05503155		YBa2Cu3O6.85	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O		6.85	1	1997																											3	Y123																																																																																						W/K.m	4.5			THC13068	micro.V/K	4			TP13068																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13069	PR05503155		YBa2Cu3O6.81	Y1Ba2Cu3O6.81	Y	1	Ba	2	Cu	3															O		6.81	1	1997																											3	Y123																																																																																						W/K.m	3.3			THC13069	micro.V/K	6.9																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13070	PR05503155		YBa2Cu3O6.81	Y12Ba2Cu3O6.81	Y	12	Ba	2	Cu	3															O		6.81	1	1997																											3	Y123																																																																																						W/K.m	3.8			THC13070	micro.V/K	6.69			TP13070																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13071	PR05503155		YBa2Cu3O6.79	Y1Ba2Cu3O6.79	Y	1	Ba	2	Cu	3															O		6.79	1	1997																											3	Y123																																																																																						W/K.m	3.1			THC13071	micro.V/K	8.7																													R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
13072	PR05503155		YBa2Cu3O6.80	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O		6.8	1	1997																											3	Y123																																																																																						W/K.m	3.2			THC13072	micro.V/K	8.05			TP13072																										R. K. Siddique, Physica C 228, 365 (1994)J. D. Jorgensen et al., Phys. Rev. B 41, 1863 (1990)					Thermal transport in YBa2Cu3O6+x: Doping dependence across the phase diagram	199702		Department of Physics, University of Miami, Coral Gables, Florida 33124	Phys.Rev.B,55(1997)3155	C.P. Popoviciu,J.L. Cohn		
14000	PR05506612		HgBa2CaCu2O6.10	Hg1Ba2Ca1Cu2O6.1	Hg	1	Ba	2	Ca	1	Cu	2													O		6.1	1	1997																											2	Hg1212			A	3.864		12.712	3											K				93			93																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14001	PR05506612		HgBa2CaCu2O6.10	Hg1Ba2Ca1Cu2O6.1	Hg	1	Ba	2	Ca	1	Cu	2													O		6.1	1	1997																											2	Hg1212			A															K				92			92																																																																		mic.V/K	29.7				m.ohm.cm											270												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14002	PR05506612		HgBa2CaCu2O6.13	Hg1Ba2Ca1Cu2O6.13	Hg	1	Ba	2	Ca	1	Cu	2													O		6.13	1	1997																											2	Hg1212			A	3.862		12.698	3											K				102			102																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14003	PR05506612		HgBa2CaCu2O6.14	Hg1Ba2Ca1Cu2O6.14	Hg	1	Ba	2	Ca	1	Cu	2													O		6.14	1	1997																											2	Hg1212			A	3.86		12.69	3											K				105			105																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14004	PR05506612		HgBa2CaCu2O6.16	Hg1Ba2Ca1Cu2O6.16	Hg	1	Ba	2	Ca	1	Cu	2													O		6.16	1	1997																											2	Hg1212			A															K				121			121																																																																		mic.V/K	11.7				m.ohm.cm											105												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14005	PR05506612		HgBa2CaCu2O6.19	Hg1Ba2Ca1Cu2O6.19	Hg	1	Ba	2	Ca	1	Cu	2													O		6.19	1	1997																											2	Hg1212			A	3.86		12.703	3											K				122			122																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14006	PR05506612		HgBa2CaCu2O6.21	Hg1Ba2Ca1Cu2O6.21	Hg	1	Ba	2	Ca	1	Cu	2													O		6.21	1	1997																											2	Hg1212			A	3.86		12.693	3											K				127			127																																																																		mic.V/K	4.8				m.ohm.cm											90												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - As sintered					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14007	PR05506612		HgBa2CaCu2O6.24	Hg1Ba2Ca1Cu2O6.24	Hg	1	Ba	2	Ca	1	Cu	2													O		6.24	1	1997																											2	Hg1212			A															K				122			122																																																																		mic.V/K	-1.9				m.ohm.cm											45												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14008	PR05506612		HgBa2CaCu2O6.24	Hg1Ba2Ca1Cu2O6.24	Hg	1	Ba	2	Ca	1	Cu	2													O		6.24	1	1997																											2	Hg1212			A	3.855		12.684	3											K				121			121																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14009	PR05506612		HgBa2CaCu2O6.27	Hg1Ba2Ca1Cu2O6.27	Hg	1	Ba	2	Ca	1	Cu	2													O		6.27	1	1997																											2	Hg1212			A	3.854		12.681	3											K				110			110																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14010	PR05506612		HgBa2CaCu2O6.30	Hg1Ba2Ca1Cu2O6.3	Hg	1	Ba	2	Ca	1	Cu	2													O		6.3	1	1997																											2	Hg1212			A	3.853		12.675	3											K				100			100																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14011	PR05506612		HgBa2CaCu2O6.30	Hg1Ba2Ca1Cu2O6.3	Hg	1	Ba	2	Ca	1	Cu	2													O		6.3	1	1997																											2	Hg1212			A															K				100			100																																																																		mic.V/K	-4.4				m.ohm.cm											45												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14012	PR05506612		HgBa2CaCu2O6.31	Hg1Ba2Ca1Cu2O6.31	Hg	1	Ba	2	Ca	1	Cu	2													O		6.31	1	1997																											2	Hg1212			A	3.853		12.683	3											K				98			98																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665C 49-100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14013	PR05506612		HgBa2Ca2Cu3O8.17	Hg1Ba2Ca2Cu3O8.17	Hg	1	Ba	2	Ca	2	Cu	3													O		8.17	1	1997																											2	Hg1223			A															K				94			94																																																																		mic.V/K	41				m.ohm.cm											160												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14014	PR05506612		HgBa2Ca2Cu3O8.17	Hg1Ba2Ca2Cu3O8.17	Hg	1	Ba	2	Ca	2	Cu	3													O		8.17	1	1997																											2	Hg1223			A															K				98			98																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14015	PR05506612		HgBa2Ca2Cu3O8.16	Hg1Ba2Ca2Cu3O8.16	Hg	1	Ba	2	Ca	2	Cu	3													O		8.16	1	1997																											2	Hg1223			A	3.886		15.887	3											K				101			101																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14016	PR05506612		HgBa2Ca2Cu3O8.20	Hg1Ba2Ca2Cu3O8.2	Hg	1	Ba	2	Ca	2	Cu	3													O		8.2	1	1997																											2	Hg1223			A	3.858		15.873	3											K				105			105																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14017	PR05506612		HgBa2Ca2Cu3O8.20	Hg1Ba2Ca2Cu3O8.2	Hg	1	Ba	2	Ca	2	Cu	3													O		8.2	1	1997																											2	Hg1223			A															K				104			104																																																																		mic.V/K	33.8				m.ohm.cm											55												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed with Zr					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14018	PR05506612		HgBa2Ca2Cu3O8.25	Hg1Ba2Ca2Cu3O8.25	Hg	1	Ba	2	Ca	2	Cu	3													O		8.25	1	1997																											2	Hg1223			A	3.854		15.855	3											K				132			132																																																																		mic.V/K	11.4				m.ohm.cm											35												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - As sintered					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14019	PR05506612		HgBa2Ca2Cu3O8.29	Hg1Ba2Ca2Cu3O8.29	Hg	1	Ba	2	Ca	2	Cu	3													O		8.29	1	1997																											2	Hg1223			A	3.854		15.855	3											K				135			135																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14020	PR05506612		HgBa2Ca2Cu3O8.29	Hg1Ba2Ca2Cu3O8.29	Hg	1	Ba	2	Ca	2	Cu	3													O		8.29	1	1997																											2	Hg1223			A															K				135			135																																																																		mic.V/K	5.2				m.ohm.cm											20												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14021	PR05506612		HgBa2Ca2Cu3O8.30	Hg1Ba2Ca2Cu3O8.3	Hg	1	Ba	2	Ca	2	Cu	3													O		8.3	1	1997																											2	Hg1223			A	3.854		15.865	3											K				134			134																																																																							ohm.cm																							HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14022	PR05506612		HgBa2Ca2Cu3O8.30	Hg1Ba2Ca2Cu3O8.3	Hg	1	Ba	2	Ca	2	Cu	3													O		8.3	1	1997																											2	Hg1223			A															K				133			133																																																																		mic.V/K	1.9				m.ohm.cm											20												HgO,BaO,CaO,CuO	1	Mixed - Pelletized - Sintered 665-710C 100h - Annealed in O2					Dependence of Tc and transport properties on the Cu valence in HgBa2Can-1CunO2(n+1)+delta(n=2,3) superconductors	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6612	A. Fukuoka,A. Tokiwa-Yamamoto,K. Tanabe,M. Itoh,R. Usami,S. Adachi		
14023	PR055R6145		(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-z	Pr	1.85	Ce	0.15	Cu	1															O	4-z		5	1997																											2	T'	I4/mmm																	K		22.5	22			1.1	22.5																																																																							m.ohm.cm					0.77							0.0365												16	Pulsed Laser Deposition 200mTorr(N2O) Deposition Rate 0.3A/PulseSubstrate LaAlO3 Substrate Temperature 700 to 840 C]					Concentration range for superconductivity in high-quality Pr2-xCexCuO4-y thin films	199703		Center for SUperconductivity Research, department of Physics, University of maryland, College Park, Maryland 20742	Phys.Rev.B,55(1997)R6145	E. Maiser,G. Czjzek,J.L. Peng,R.L. Greene,T. Venkatesan		
14024	PR055R6145	not superconductor	(Pr,Ce)2CuO4	Pr1.9Ce0.1Cu1O4-y	Pr	1.9	Ce	0.1	Cu	1															O	4-y		5	1997																											2	T'	I4/mmm																																																																																															m.ohm.cm		0.77			0.552							1.24												16	Pulsed Laser Deposition 200mTorr(N2O) Deposition Rate 0.3A/PulseSubstrate LaAlO3 Substrate Temperature 700 to 840 C]					Concentration range for superconductivity in high-quality Pr2-xCexCuO4-y thin films	199703		Center for SUperconductivity Research, department of Physics, University of maryland, College Park, Maryland 20742	Phys.Rev.B,55(1997)R6145	E. Maiser,G. Czjzek,J.L. Peng,R.L. Greene,T. Venkatesan		
14025	PR05505674		(HgBr2)0.5Bi2Sr2CaCu2Oy	Hg0.5Br1Bi2Ca1Cu2OY	Hg	0.5	Br	1	Bi	2	Ca	1	Cu	2											O	Y		3	1997																													I4/mmm		A			43.2	1																																																																																																																	7	Traveling solvent floating zone methordand Intercalated HgBr2					Raman spectroscopic evidence on molecular mercuric bromide in the two-dimensional lattice of (HgBr2)0.5Bi2Sr2CaCu2Oy	199703		Department Chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Rev.B,55(1997)5674	Dong-Kuk Kim,Jin-Ho Choy,Seong-Ju Hwang		
14026	PR05506051		YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O		6.5	3	1997																												Y123																																																																																																m.ohm.cm									9.1														Ba2Cu5O8,Y2BaCuO5		CZ method  Y2O3crucible Ref. Y,Ymada et al,Phys. C 217,182 1993					Optical study of c-axis charge dynamics in YBa2Cu3Oy: Carrier self-confinement in the normal and the superconducting states	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, Shinonome 1-10-13, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6051	"I. Terasaki,J. Schu""tzmann,R. Hauff,S. Miyamoto,S. Tajima,Y. Sato"		
14027	PR05506051		YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O		6.6	3	1997																												Y123																								2																																																																								m.ohm.cm									7.2														Ba2Cu5O8,Y2BaCuO5		CZ method  Y2O3crucible Ref. Y,Ymada et al,Phys. C 217,182 1993					Optical study of c-axis charge dynamics in YBa2Cu3Oy: Carrier self-confinement in the normal and the superconducting states	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, Shinonome 1-10-13, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6051	"I. Terasaki,J. Schu""tzmann,R. Hauff,S. Miyamoto,S. Tajima,Y. Sato"		
14028	PR05506051		YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O		6.7	3	1997																												Y123																																																																																																m.ohm.cm									5														Ba2Cu5O8,Y2BaCuO5		CZ method  Y2O3crucible Ref. Y,Ymada et al,Phys. C 217,182 1993					Optical study of c-axis charge dynamics in YBa2Cu3Oy: Carrier self-confinement in the normal and the superconducting states	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, Shinonome 1-10-13, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6051	"I. Terasaki,J. Schu""tzmann,R. Hauff,S. Miyamoto,S. Tajima,Y. Sato"		
14029	PR05506051		YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O		6.8	3	1997																												Y123																		K		92					92																																																																							m.ohm.cm									3.5														Ba2Cu5O8,Y2BaCuO5		CZ method  Y2O3crucible Ref. Y,Ymada et al,Phys. C 217,182 1993					Optical study of c-axis charge dynamics in YBa2Cu3Oy: Carrier self-confinement in the normal and the superconducting states	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, Shinonome 1-10-13, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6051	"I. Terasaki,J. Schu""tzmann,R. Hauff,S. Miyamoto,S. Tajima,Y. Sato"		
14030	PR05506051		YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O		6.9	3	1997																												Y123																		K		88				0.5	88																																																																							m.ohm.cm									4														Ba2Cu5O8,Y2BaCuO5		CZ method  Y2O3crucible Ref. Y,Ymada et al,Phys. C 217,182 1993					Optical study of c-axis charge dynamics in YBa2Cu3Oy: Carrier self-confinement in the normal and the superconducting states	199703		Superconductivity Reserch Laboratory, International Superconductivity Technology Center, Shinonome 1-10-13, Koto-Ku, Tokyo 135, Japan	Phys.Rev.B,55(1997)6051	"I. Terasaki,J. Schu""tzmann,R. Hauff,S. Miyamoto,S. Tajima,Y. Sato"		
14031	PR05506584		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1997					Bohr magne	8.479		10.6																			2		I4/mmm		A	3.534		10.488	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14032	PR05506584		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1997					Bohr magne	8.62		8.5																			2		I4/mmm		A	3.518		10.528	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14033	PR05506584		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1997					Bohr magne	7.19		6.8																			2		I4/mmm		A	3.502		10.558	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14034	PR05506584		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	1997					Bohr magne	3.78		1.53																			2		I4/mmm		A	3.487		10.586	3	6																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14035	PR05506584	not Superconductor	YbNi2B2C	Yb1Ni2B2C1	Yb	1	Ni	2	B	2	C	1																1	1997																											2		I4/mmm		A	3.478		10.607	3	2																																																																																																																	Solid State Reaction (High Vapor Pressure)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14036	PR05506584		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1997																											2		I4/mmm							2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14037	PR05506584	not Superconductor	CeNi2B2C	Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	1997																											2		I4/mmm		A	3.638		10.227	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14038	PR05506584	not Superconductor	PrNi2B2C	Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																1	1997					Bohr magne	0.813		4																			2		I4/mmm		A	3.707		9.999	3	6																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14039	PR05506584		NdNi2B2C	Nd1Ni2B2C1	Nd	1	Ni	2	B	2	C	1																1	1997					Bohr magne	2.107		4.78																			2		I4/mmm		A	3.678		10.081	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
14040	PR05506584	not Superconductor	TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																1	1997					Bohr magne	7.78		15.4																			2		I4/mmm		A	3.554		10.435	3	2																																																																																																																	arc melting method (Ar atomosphere)					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
15000	PR05509125		Bi2Sr2Ca2Cu2O8+y	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		3	1997																												Bi2212			A	5.41	5.42	30.96	1		1/K								at Room Temperature	K	90						90																																																																																																Ref. J.Kobayashi et al.,Phys. Rev. B53 11784(1996)					Thermal expansion of superconducting Bi2Sr2CaCu2O8	199704		Kagami Memorial Laboratory for Materials Science and Technology, Waseda University, 2-8-26 Nishi-Waseda, Shinjuku-ku, Tokyo 169, Japan	Phys.Rev.B,55(1997)9125	H. Suzuki,H. Takano,J. Kobayashi,M. Nakamura,T. Asahi		
15001	PR05509160	detwin	(Pr,Y)Ba2Cu3O6.91	Pr0.8Y0.2Ba2Cu3O6.91	Pr	0.8	Y	0.2	Ba	2	Cu	3													O		6.91	3	1997																												Y123			A	3.868	3.926	11.708	2	1																																																																																																																	Ref. A.Erb et al., J.Cryst. Growth 132,389(1993)Ref. A.Erb et al., J.Cryst. Growth 137,487(1993)Ref. A.Erb et al., Physica C 245,245 (1995)					X-ray absorption spectroscopy of detwinned PrxY1-xBa2Cu3O7-y single crystals: Electronic structure and hole distribution	199704		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Germany	Phys.Rev.B,55(1997)9160	"A. Erb,C.T. Chen,E. Pellegrin,J. Fink,M. Kielwein,M. Knupfer,M. Merz,M.S. Golden,N. Nu""cker,P. Schweiss,S. Schuppler,V. Chakarian,Y.U. Idzerda"		
15002	PR05509160	detwin	YBa2Cu3O6.91	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O		6.91	3	1997																												Y123			A	3.819	3.884	11.681	2	1																																																																																																																	Ref. A.Erb et al., J.Cryst. Growth 132,389(1993)Ref. A.Erb et al., J.Cryst. Growth 137,487(1993)Ref. A.Erb et al., Physica C 245,245 (1995)					X-ray absorption spectroscopy of detwinned PrxY1-xBa2Cu3O7-y single crystals: Electronic structure and hole distribution	199704		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Germany	Phys.Rev.B,55(1997)9160	"A. Erb,C.T. Chen,E. Pellegrin,J. Fink,M. Kielwein,M. Knupfer,M. Merz,M.S. Golden,N. Nu""cker,P. Schweiss,S. Schuppler,V. Chakarian,Y.U. Idzerda"		
15003	PR05508529	textured	Bi2Sr2CaCu2O8+y	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		3	1997																												Bi2212																		K	82.9	89.9	108.2			25.3	89.9			K/GPa	2																																																																																												sinter forging methordtextured					Electrical resistance under pressure in textured Bi2Sr2CaCu2O8+y: Enhancement of the energy gap and thermodynamic fluctuations	199704		Schools of Physics and Materials Science, University of Bath, Claverton Down, Bath BA2 7AY, United Kingdom	Phys.Rev.B,55(1997)8529	D.P. Almond,G.A. Saunders,H.J. Liu,M.S. Acres,Q. Wang		
15004	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr1.8La0.1Cu1Oz	Bi	1.9	Pb	0.2	Sr	1.8	La	0.1	Cu	1											O	z		1	1997																											3	Bi2201			A	5.359	5.37	24.563	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15005	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr1.7La0.2Cu1Oz	Bi	1.9	Pb	0.2	Sr	1.7	La	0.2	Cu	1											O	z		1	1997																											3	Bi2201			A	5.368	5.38	24.494	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15006	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr1.55La0.35Cu1Oz	Bi	1.9	Pb	0.2	Sr	1.55	La	0.35	Cu	1											O	z		1	1997																											3	Bi2201			A	5.382	5.393	24.47	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15007	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr1.4La0.5Cu1Oz	Bi	1.9	Pb	0.2	Sr	1.4	La	0.5	Cu	1											O	z		1	1997																											3	Bi2201			A	5.388	5.398	24.326	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15008	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr1.2La0.7Cu1Oz	Bi	1.9	Pb	0.2	Sr	1.2	La	0.7	Cu	1											O	z		1	1997																											3	Bi2201			A	5.401	5.438	24.259	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15009	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.9Pb0.2Sr0.9La1Cu1Oz	Bi	1.9	Pb	0.2	Sr	0.9	La	1	Cu	1											O	z		1	1997																											3	Bi2201			A	5.427	5.458	23.914	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15010	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr1.8La0.1Cu1Oz	Bi	1.7	Pb	0.4	Sr	1.8	La	0.1	Cu	1											O	z		1	1997																											3	Bi2201			A	5.355	5.362	24.473	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15011	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr1.7La0.2Cu1Oz	Bi	1.7	Pb	0.4	Sr	1.7	La	0.2	Cu	1											O	z		1	1997																											3	Bi2201			A	5.358	5.368	24.444	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15012	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr1.55La0.35Cu1Oz	Bi	1.7	Pb	0.4	Sr	1.55	La	0.35	Cu	1											O	z		1	1997																											3	Bi2201			A	5.359	5.354	24.435	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15013	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr1.4La0.5Cu1Oz	Bi	1.7	Pb	0.4	Sr	1.4	La	0.5	Cu	1											O	z		1	1997																											3	Bi2201			A	5.363	5.366	24.314	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15014	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr1.2La0.7Cu1Oz	Bi	1.7	Pb	0.4	Sr	1.2	La	0.7	Cu	1											O	z		1	1997																											3	Bi2201			A	5.423	5.4	24.165	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15015	PR05509130		(Bi,Pb)2(Sr,La,Pb)2CuOz	Bi1.7Pb0.4Sr0.9La1Cu1Oz	Bi	1.7	Pb	0.4	Sr	0.9	La	1	Cu	1											O	z		1	1997																											3	Bi2201			A	5.44	5.447	24.129	3																																																																																																																Bi2O3,PbO,SrCO3,La2O3,CuO	1	mixed - preheated in air 820-830C 40h - pelletized - sintered in air 870-910C 60h - quenched in air					Relation of the superstructure modulation and extra-oxygen local-structural distortion in Bi2.1-yPbySr1.9-xLaxCuOz	199704		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, Peple's Republic of China	Phys.Rev.B,55(1997)9130	Fan Chenggao,Lu Bin,Mao Zhiqiang,Tan Shun,Tian Mingliang,Xu Cunyi,Xu. Gaojie,Zhang Shuyuan		
15016	PR05508674		HgBa2Ca2Cu3O8+y	Hg1Ba2Ca2Cu3O8+y	Hg	1	Ba	2	Ca	2	Cu	3													O	8+y		3	1997																											2	Hg1223																		K		110.4				1.2	110.4																																																						mJ/mole.K	1200																																									D. Colsoon et al., Physica C 233, 231 (1994)					Field dependence of the specific heat of single-crystal HgBa2Ca2Cu3O8+delta	199704		De'partement de Recherche Fondamentale sur la Matie're Condense'e, laboratoire de Cryophysique,Commissariat a' l'Energie Atomique-Grenoble,17 rue des Martyrs,38054 Grenoble Cedex 9, France	Phys.Rev.B,55(1997)R8674	A. Bertinotti,A. Carrington,C. Marcenat,D. Colson,F. Bouquet,J. Hammann,J.F. Marucco		
16000	PR05512005		Er2Ba4Cu7O14.92	Er2Ba4Cu7O14.92	Er	2	Ba	4	Cu	7															O		14.92	1	1997								0.54																			3	Y247	Ammm		A	3.826	3.866	50.368	3											K				89			89																																																																																															11	P. Berastegui et al., J. Appl. Phys. 73, 2424 (1993)					Long-range magnetic order of the Er ions in Er2Ba4Cu7O14.92	199705		Laboratory for Neutron Scattering, Eidgenossische Hochschule Zurich and Paul Scherrer Institut, CH-5232 Villigen PSI, Swizerland	Phys.Rev.B.,55(1997)R12005	A. Donni,F. Fauth,G. Bottger,H. Sato,P. Berastegui,P. Fischer,Y. Aoki		
16001	PR05512776		HgBa2CuO4+y	Hg1Ba2Cu1O4+y	Hg	1	Ba	2	Cu	1															O	4+y		1	1997	emu/g	-0.005																									2	Hg1201			A	3.871		9.493	3											K				91			91																																									A	microwave	15000																																																			HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16002	PR05512776		Hg0.95Ba2CuO4+y	Hg0.95Ba2Cu1O4+y	Hg	0.95	Ba	2	Cu	1															O	4+y		1	1997																											2	Hg1201			A	3.868		9.484	3											K				89.5			89.5																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16003	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.95Ba2Cu1.05O4+y	Hg	0.95	Ba	2	Cu	1.05															O	4+y		1	1997	emu/g	-0.01																									2	Hg1201			A	3.873		9.494	3											K				95.2			95.2																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16004	PR05512776		Hg0.90Ba2CuO4	Hg0.9Ba2Cu1O4+y	Hg	0.9	Ba	2	Cu	1															O	4+y		1	1997																											2	Hg1201			A	3.876		9.502	3											K				96			96																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16005	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.9Ba2Cu1.05O4+y	Hg	0.9	Ba	2	Cu	1.05															O	4+y		1	1997																											2	Hg1201			A	3.872		9.496	3											K				96			96																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16006	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.9Ba2Cu1.1O4+y	Hg	0.9	Ba	2	Cu	1.1															O	4+y		1	1997	emu/g	-0.014																									2	Hg1201			A	3.874		9.499	3											K				95.3			95.3																																									A	microwave	6000																																																			HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16007	PR05512776		Hg0.85Ba2CuO4	Hg0.85Ba2Cu1O4+y	Hg	0.85	Ba	2	Cu	1															O	4+y		1	1997																											2	Hg1201			A	3.87		9.492	3											K				93			93																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16008	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.85Ba2Cu1.05O4+y	Hg	0.85	Ba	2	Cu	1.05															O	4+y		1	1997																											2	Hg1201			A	3.872		9.497	3											K				95.5			95.5																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16009	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.85Ba2Cu1.1O4+y	Hg	0.85	Ba	2	Cu	1.1															O	4+y		1	1997																											2	Hg1201			A	3.874		9.497	3											K				94.5			94.5																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16010	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.85Ba2Cu1.15O4+y	Hg	0.85	Ba	2	Cu	1.15															O	4+y		1	1997	emu/g	-0.012																									2	Hg1201			A	3.872		9.495	3											K				95.5			95.5																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16011	PR05512776		Hg0.80Ba2CuO4	Hg0.8Ba2Cu1O4+y	Hg	0.8	Ba	2	Cu	1															O	4+y		1	1997																											2	Hg1201			A	3.873		9.499	3											K				94.5			94.5																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16012	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.8Ba2Cu1.05O4+y	Hg	0.8	Ba	2	Cu	1.05															O	4+y		1	1997																											2	Hg1201			A	3.87		9.492	3											K				95.8			95.8																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16013	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.8Ba2Cu1.1O4+y	Hg	0.8	Ba	2	Cu	1.1															O	4+y		1	1997																											2	Hg1201			A	3.872		9.494	3											K				94.3			94.3																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16014	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.8Ba2Cu1.15O4+y	Hg	0.8	Ba	2	Cu	1.15															O	4+y		1	1997																											2	Hg1201			A	3.875		9.502	3											K				93.2			93.2																																																																																														HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16015	PR05512776		(Hg,Cu)Ba2CuO4	Hg0.8Ba2Cu1.2O4+y	Hg	0.8	Ba	2	Cu	1.2															O	4+y		1	1997	emu/g	-0.009																									2	Hg1201			A	3.87		9.49	3											K				95.4			95.4																																									A	microwave	11000																																																			HgO,Ba2CuO3.3,CuO	1	Mixed - Pelletized - Heated 1 atm air in quartz tube to 800C 4h, at 800C 8h, to R.T. 8h					Synthesis, structure, and properties of the high-temperature superconductor HgBa2CuO4+delta	199705		School of Chemistry, The University of Birmingham, Edgbaston, Birmingham, B15 2TT, United Kindom	Phys.Rev.B,55(1997)12776	A. Porch,A.P. Kharel,I. Gameson,J.P. Hodges,P.P. Edwards		
16016	PR05511789	twin sampleValue at H=0 and T=0	Yba2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1997																												Y123																		K			93.2			0.25	93.2																																									A	mSR		1155																																																				Ref. J.E.Sonier et al.,Phys.Rev.Lett. 72,724(1994)ref.R.Liang et al.,Physica C 195,51(1992)					Magnetic field dependence of the London penetration depth in the vortex state of YBa2Cu3O6.95	199705		Department of Physics, Virginia State University, Petersburg, Virginia 23806	Phys.Rev.B,55(1997)11789	C.E. Stronach,D.A. Bonn,D.R. Noakes,J.E. Sonier,J.H. Brewer,R.F. Kiefl,Ruixing Liang,S.R. Dunsiger,T.M. Riseman,W.A. MacFarlane,W.N. Hardy		
16017	PR05511832		(Tl,Pb)Sr2CaCu2O7	Tl0.5Pb0.5Sr2Ca1Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2											O		7	1	1997																											2	Tl1212	P4/mmm						3	1										K		78.4					78.4			K/GPa	-0.4																																																																																										CaCO3,Y2O3,SrCO3,CuO,Tl2O3,PbO	1	Precursor:CaCO3,Y2O3,SrCO3,CuO calcined 970C 12hour in airPrecursor mixed with Tl2O3+PbO (950C 3hour)  in O2 flow					Pressure dependence of the superconducting critical temperature of the Tl0.5Pb0.5Sr2Ca1-xYxCu2O7 system	199705		Department of Physics and Astronomy, Free University, De Boelelaan 1081, 1081 HV Amsterdam, The Netherland	Phys.Rev.B.,55(1997)11832	D. Tristan Jover,H. Wilhelm,R.J. Wijingaarden,R.S. Liu		
16018	PR05511832		(Tl,Pb)Sr2(Ca,Y)Cu2O7	Tl0.5Pb0.5Sr2Ca0.9Y0.1Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	0.9	Y	0.1	Cu	2									O		7	1	1997																											2	Tl1212	P4/mmm						3	1										K		99.3					99.3			K/GPa	0.77																																																																																										CaCO3,Y2O3,SrCO3,CuO,Tl2O3,PbO	1	Precursor:CaCO3,Y2O3,SrCO3,CuO calcined 970C 12hour in airPrecursor mixed with Tl2O3+PbO (950C 3hour)  in O2 flow					Pressure dependence of the superconducting critical temperature of the Tl0.5Pb0.5Sr2Ca1-xYxCu2O7 system	199705		Department of Physics and Astronomy, Free University, De Boelelaan 1081, 1081 HV Amsterdam, The Netherland	Phys.Rev.B.,55(1997)11832	D. Tristan Jover,H. Wilhelm,R.J. Wijingaarden,R.S. Liu		
16019	PR05511832		(Tl,Pb)Sr2(Ca,Y)Cu2O7	Tl0.5Pb0.5Sr2Ca0.8Y0.2Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	0.8	Y	0.2	Cu	2									O		7	1	1997																											2	Tl1212	P4/mmm						3	1										K		105.2					105.2			K/GPa	1.5																																																																																										CaCO3,Y2O3,SrCO3,CuO,Tl2O3,PbO	1	Precursor:CaCO3,Y2O3,SrCO3,CuO calcined 970C 12hour in airPrecursor mixed with Tl2O3+PbO (950C 3hour)  in O2 flow					Pressure dependence of the superconducting critical temperature of the Tl0.5Pb0.5Sr2Ca1-xYxCu2O7 system	199705		Department of Physics and Astronomy, Free University, De Boelelaan 1081, 1081 HV Amsterdam, The Netherland	Phys.Rev.B.,55(1997)11832	D. Tristan Jover,H. Wilhelm,R.J. Wijingaarden,R.S. Liu		
16020	PR05511832		(Tl,Pb)Sr2(Ca,Y)Cu2O7	Tl0.5Pb0.5Sr2Ca0.65Y0.35Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	0.65	Y	0.35	Cu	2									O		7	1	1997																											2	Tl1212	P4/mmm						3	1										K		92					92			K/GPa	1.1																																																																																										CaCO3,Y2O3,SrCO3,CuO,Tl2O3,PbO	1	Precursor:CaCO3,Y2O3,SrCO3,CuO calcined 970C 12hour in airPrecursor mixed with Tl2O3+PbO (950C 3hour)  in O2 flow					Pressure dependence of the superconducting critical temperature of the Tl0.5Pb0.5Sr2Ca1-xYxCu2O7 system	199705		Department of Physics and Astronomy, Free University, De Boelelaan 1081, 1081 HV Amsterdam, The Netherland	Phys.Rev.B.,55(1997)11832	D. Tristan Jover,H. Wilhelm,R.J. Wijingaarden,R.S. Liu		
17000	PR05514152		Bi2Sr2CuO6	Bi2Sr2Cu1O6	Bi	2	Sr	2	Cu	1															O		6	3	1997																											2	Bi2201			A	5.36	5.37	24.64	1											K				7.5		2	7.5																																																																																																Precursor dissolved in liquied KCl,and in cavity(840-850C)Temperature Gradient(2-3K/cm)					In-plane optical response of Bi2sr2CuO6	199706		Material Science Center, Laboratory of Solid State Physics, University of Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands	Phys.Rev.B.,55(1997)14152	A.A. Tsvetkov,D. van der Marel,G.A. Kaljushnaia,J. Schutzmann,J.I. Gorina		
17001	PR05514761		(La,Nd,Sr)2CuO4	La1.55Nd0.3Sr0.15Cu1O4	La	1.55	Nd	0.3	Sr	0.15	Cu	1													O		4	1	1997								26																																																																																																																																												1						Magnetic order in La1.85-xNdxSr0.15CuO4 with 0.30%$x%$0.60	199706		Institut fur Metallphysik und Nukleare Festkorperphysik, Technische Universtat Braunschweig, Germany	Phys.Rev.B.,55(1997)R14761	B. Buchner,F.J. Litterst,H. Micklitz,H.-H. Klau%!A,M. Birke,M. Hillberg,M.A.C. de Melo,W. Wagener		
17002	PR05514761		(La,Nd,Sr)2CuO4	La1.4Nd0.45Sr0.15Cu1O4	La	1.4	Nd	0.45	Sr	0.15	Cu	1													O		4	1	1997								30																																																																																																																																												1						Magnetic order in La1.85-xNdxSr0.15CuO4 with 0.30%$x%$0.60	199706		Institut fur Metallphysik und Nukleare Festkorperphysik, Technische Universtat Braunschweig, Germany	Phys.Rev.B.,55(1997)R14761	B. Buchner,F.J. Litterst,H. Micklitz,H.-H. Klau%!A,M. Birke,M. Hillberg,M.A.C. de Melo,W. Wagener		
17003	PR05514761		(La,Nd,Sr)2CuO4	La1.35Nd0.5Sr0.15Cu1O4	La	1.35	Nd	0.5	Sr	0.15	Cu	1													O		4	1	1997								26																																																																																																																																												1						Magnetic order in La1.85-xNdxSr0.15CuO4 with 0.30%$x%$0.60	199706		Institut fur Metallphysik und Nukleare Festkorperphysik, Technische Universtat Braunschweig, Germany	Phys.Rev.B.,55(1997)R14761	B. Buchner,F.J. Litterst,H. Micklitz,H.-H. Klau%!A,M. Birke,M. Hillberg,M.A.C. de Melo,W. Wagener		
17004	PR05514761		(La,Nd,Sr)2CuO4	La1.25Nd0.6Sr0.15Cu1O4	La	1.25	Nd	0.6	Sr	0.15	Cu	1													O		4	1	1997								29																																																																																																																																												1						Magnetic order in La1.85-xNdxSr0.15CuO4 with 0.30%$x%$0.60	199706		Institut fur Metallphysik und Nukleare Festkorperphysik, Technische Universtat Braunschweig, Germany	Phys.Rev.B.,55(1997)R14761	B. Buchner,F.J. Litterst,H. Micklitz,H.-H. Klau%!A,M. Birke,M. Hillberg,M.A.C. de Melo,W. Wagener		
17005	PR05514581	cooled in furnace 	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.2Sr2Cu1O6+y	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	6+y		1	1997																											2	Bi2201																																																																																											micro.V/K	-11.2				m.ohm.cm				1.6							2.9													1	cooled in furnace					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17006	PR05514581	Annealed in N2, 700C, 2.5h 	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.2Sr2Cu1O6+y	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	6+y		1	1997																											2	Bi2201																																																																																											micro.V/K	-7				m.ohm.cm				2.5							4.3													1	annealed N2 700C 2.5h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17007	PR05514581	annealed in O2, 10E-5 atm, 550C, 2.5h 	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.2Sr2Cu1O6+y	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	6+y		1	1997																											2	Bi2201																		K			20				20																																																																		micro.V/K	-3.6				m.ohm.cm				4.8			4.6				5.7													1	annealed O2 10^{-5}atm 550C 2.5h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17008	PR05514581	annealed O2 10E-5 atm 630C 2.5h 	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.2Sr2Cu1O6+y	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	6+y		1	1997																											2	Bi2201																		K			20				20																																																																		micro.V/K	-2.2				m.ohm.cm				5.6			5.3				6.4													1	annealed O2 10^{-5}atm 630C 2.5h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17009	PR05514581	annealed O2 10E-5 atm, 630C, 2.5h + 650C 1.5h + 10E-8 atm 650C 2h 	(Bi,Pb)2Sr2CuO6	Bi1.8Pb0.2Sr2Cu1O6+y	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	6+y		1	1997																											2	Bi2201																		K			14				14																																																																		micro.V/K	-1.8				m.ohm.cm				39			51				32													1	annealed O2 10^{-5}atm 630C 2.5h + 650C 1.5h + 10^{-8}atm 650C 2h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17010	PR05514581		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+y	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+y		1	1997																											2	Bi2212																		K		67					67																																																																		micro.V/K	-5				m.ohm.cm				1			0.8				2.1													1	cooled in furnace					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17011	PR05514581		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+y	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+y		1	1997																											2	Bi2212																		K		78					78																																																																		micro.V/K	-2				m.ohm.cm							2.7				3.2													1	quenched in air					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17012	PR05514581		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+y	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+y		1	1997																											2	Bi2212																		K		92					92																																																																		micro.V/K	2				m.ohm.cm							6.7				5.3													1	annealed O2 10^{-5}atm 550C 0.5h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17013	PR05514581		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+y	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+y		1	1997																											2	Bi2212																		K		80					80																																																																		micro.V/K	5.5				m.ohm.cm							57				33													1	annealed O2 10^{-5}atm 550C 2.5h + 10^{-8}atm 550C 2.5h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17014	PR05514581		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2O8+y	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	8+y		1	1997																											2	Bi2212																		K		81					81																																																																		micro.V/K	6				m.ohm.cm							76				49													1	annealed O2 10^{-5}atm 550C 5h + 10^{-8}atm 550C 10h					Normal-state spin gap of Bi-based superconductors	199706		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,55(1997)14581	Mao Zhiqiang,Tian Mingliang,Wang Keqing,Wang Ruiping,Xu Gaojie		
17015	PR05514733	substrate = BaZrO3 	YBa2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1997																											3	Y123																		K				93.4			93.4																																									A	microwave, cavity	1000																																																				1	grown in BaZrO3 crucible					Microwave response of YBa2Cu3O6.95 crystals: Evidence for a multicomponent order parameter	199706		Department of Physics, Northeastern University, 360 Huntington Avenue. Boston, Massachsetts 02115	Phys.Rev.B.,55(1997)R14773	A. Erd,B.A. Willemsen,E. Walker,H. Srikanth,R. Flukiger,S. Sridhar,T. Jacobs		
17016	PR05514733	substrate = YSZ 	YBa2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1997																											3	Y123																																																																		A	microwave, cavity	1400																																																				1	grown in yttria-stabilized zirconia crucible					Microwave response of YBa2Cu3O6.95 crystals: Evidence for a multicomponent order parameter	199706		Department of Physics, Northeastern University, 360 Huntington Avenue. Boston, Massachsetts 02115	Phys.Rev.B.,55(1997)R14773	A. Erd,B.A. Willemsen,E. Walker,H. Srikanth,R. Flukiger,S. Sridhar,T. Jacobs		
17017	PR05514632		Bi2Sr2CaCu2O8+y	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1997																											3	Bi2212			A	5.39	5.397	30.768	4										In this paper, temperature dependence of lattice parameters is reported.But their temperature depandence is not linear.So da/aT etc. aren't listed.																																																																																																							7						Temperature-dependent changes in the sturucture of high-quality polycrystallin Bi2Sr2CaCu2O8+x material	199706		Advanced Electronic Materials Group, School of Physics, University of NSW, Sydney NSW 2052, Australia	Phys.Rev.B.,55(1997)14632	A.R. Anderson,G.D. Gu,G.J. Russell,N. Koshizuka,P.A. Miles,S.J. Kennedy		
17018	PR05515300		YBa2Cu3O6.92	Y1Ba2Cu3O6.92	Y	1	Ba	2	Cu	3															O		6.92	3	1997																											3	Y123																		K			90				90																																																																							m.ohm.cm								0.03						m3/C		0.0000000003	-0.0000000003								crystal-pulling techniqueannealed O2 flow 400C 10days					Anisotropic Hal mobility in slightly overdoped YBa2Cu3O6.92 from magnetoresistance and Hall-coefficient measurements	199706		Superconductivity Research Laboratory, International Superconductivity Technology, Center 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B.,55(1997)15300	I. Terasaki,S. Tajima,Y. Sato		
17019	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.79	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.79	1	1997																												336																		K				40			40																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17020	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.011	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.011	1	1997																												336																		K				78			78																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17021	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.079	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.079	1	1997																												336																		K				76			76																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17022	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.112	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.112	1	1997																												336																		K				72			72																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17023	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.16	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.16	1	1997																												336																		K				56			56																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17024	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O6.76	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		6.76	1	1997																												336																		K				34			34																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17025	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O6.97	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		6.97	1	1997																												336																		K				70			70																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17026	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.06	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.06	1	1997																												336																		K				79			79																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17027	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.06	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.06	1	1997																												336																		K				79			79																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17028	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.11	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.11	1	1997																												336																		K				77			77																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17029	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.123	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.123	1	1997																												336																		K				76			76																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17030	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.17	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.17	1	1997																												336																		K				70			70																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17031	PR05515228		(La,Ba,Ca)3Cu3O6	La1.1Ba1.5Ca0.4Cu3O7.25	La	1.1	Ba	1.5	Ca	0.4	Cu	3													O		7.25	1	1997																												336																		K				35			35																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17032	PR05515228		(La,Ba,Ca)3Cu3O6	La1.2Ba1.5Ca0.3Cu3O6.72	La	1.2	Ba	1.5	Ca	0.3	Cu	3													O		6.72	1	1997																												336																		K				27			27																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17033	PR05515228		(La,Ba,Ca)3Cu3O6	La1.2Ba1.5Ca0.3Cu3O6.93	La	1.2	Ba	1.5	Ca	0.3	Cu	3													O		6.93	1	1997																												336																		K				60			60																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17034	PR05515228		(La,Ba,Ca)3Cu3O6	La1.2Ba1.5Ca0.3Cu3O7.06	La	1.2	Ba	1.5	Ca	0.3	Cu	3													O		7.06	1	1997																												336																		K				75.2			75.2																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17035	PR05515228		(La,Ba,Ca)3Cu3O6	La1.3Ba1.5Ca0.2Cu3O6.7	La	1.3	Ba	1.5	Ca	0.2	Cu	3													O		6.7	1	1997																												336																		K				20			20																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17036	PR05515228		(La,Ba,Ca)3Cu3O6	La1.3Ba1.5Ca0.2Cu3O6.92	La	1.3	Ba	1.5	Ca	0.2	Cu	3													O		6.92	1	1997																												336																		K				45			45																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17037	PR05515228		(La,Ba,Ca)3Cu3O6	La1.3Ba1.5Ca0.2Cu3O6.94	La	1.3	Ba	1.5	Ca	0.2	Cu	3													O		6.94	1	1997																												336																		K				52			52																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17038	PR05515228		(La,Ba,Ca)3Cu3O6	La1.4Ba1.5Ca0.1Cu3O6.688	La	1.4	Ba	1.5	Ca	0.1	Cu	3													O		6.688	1	1997																												336																		K																																																																																																					La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17039	PR05515228		(La,Ba,Ca)3Cu3O6	La1.4Ba1.5Ca0.1Cu3O6.903	La	1.4	Ba	1.5	Ca	0.1	Cu	3													O		6.903	1	1997																												336																		K				25			25																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17040	PR05515228		(La,Ba,Ca)3Cu3O6	La1.4Ba1.5Ca0.1Cu3O6.943	La	1.4	Ba	1.5	Ca	0.1	Cu	3													O		6.943	1	1997																												336																		K				40			40																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17041	PR05515228		(La,Ba,Ca)3Cu3O6	La1.4Ba1.5Ca0.1Cu3O6.982	La	1.4	Ba	1.5	Ca	0.1	Cu	3													O		6.982	1	1997																												336																		K				51			51																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17042	PR05515228		(La,Ba)3Cu3O6	La1.5Ba1.5Cu3O6.657	La	1.5	Ba	1.5	Cu	3															O		6.657	1	1997																												336																																																																																																																							La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17043	PR05515228		(La,Ba)3Cu3O6	La1.5Ba1.5Cu3O6.884	La	1.5	Ba	1.5	Cu	3															O		6.884	1	1997																												336																																																																																																																							La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17044	PR05515228		(La,Ba)3Cu3O6	La1.5Ba1.5Cu3O7.021	La	1.5	Ba	1.5	Cu	3															O		7.021	1	1997																												336																																																																																																																							La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17045	PR05515228		(La,Ba)3Cu3O6	La1.5Ba1.5Cu3O7.078	La	1.5	Ba	1.5	Cu	3															O		7.078	1	1997																												336																																																																																																																							La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17046	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.4Ca0.1Cu3O6.912	La	1.5	Ba	1.4	Ca	0.1	Cu	3													O		6.912	1	1997																												336																		K				11			11																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17047	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.4Ca0.1Cu3O6.912	La	1.5	Ba	1.4	Ca	0.1	Cu	3													O		6.912	1	1997																												336																		K				16			16																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17048	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.4Ca0.1Cu3O6.932	La	1.5	Ba	1.4	Ca	0.1	Cu	3													O		6.932	1	1997																												336																		K				25			25																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17049	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.4Ca0.1Cu3O6.964	La	1.5	Ba	1.4	Ca	0.1	Cu	3													O		6.964	1	1997																												336																		K				35			35																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17050	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.3Ca0.2Cu3O6.897	La	1.5	Ba	1.3	Ca	0.2	Cu	3													O		6.897	1	1997																												336																		K				16			16																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17051	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.3Ca0.2Cu3O6.918	La	1.5	Ba	1.3	Ca	0.2	Cu	3													O		6.918	1	1997																												336																		K				25			25																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17052	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.3Ca0.2Cu3O6.957	La	1.5	Ba	1.3	Ca	0.2	Cu	3													O		6.957	1	1997																												336																		K				35			35																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17053	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.3Ca0.2Cu3O7.002	La	1.5	Ba	1.3	Ca	0.2	Cu	3													O		7.002	1	1997																												336																		K				16			16																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17054	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.1Ca0.4Cu3O6.764	La	1.5	Ba	1.1	Ca	0.4	Cu	3													O		6.764	1	1997																												336																		K				25			25																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17055	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.1Ca0.4Cu3O6.969	La	1.5	Ba	1.1	Ca	0.4	Cu	3													O		6.969	1	1997																												336																		K				40			40																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17056	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.1Ca0.4Cu3O7.05	La	1.5	Ba	1.1	Ca	0.4	Cu	3													O		7.05	1	1997																												336																		K				55			55																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17057	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1.1Ca0.4Cu3O7.082	La	1.5	Ba	1.1	Ca	0.4	Cu	3													O		7.082	1	1997																												336																		K				62			62																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17058	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1Ca0.5Cu3O6.801	La	1.5	Ba	1	Ca	0.5	Cu	3													O		6.801	1	1997																												336																		K				30			30																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17059	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1Ca0.5Cu3O6.981	La	1.5	Ba	1	Ca	0.5	Cu	3													O		6.981	1	1997																												336																		K				50			50																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17060	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1Ca0.5Cu3O7.126	La	1.5	Ba	1	Ca	0.5	Cu	3													O		7.126	1	1997																												336																		K				67			67																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17061	PR05515228		(La,Ba,Ca)3Cu3O6	La1.5Ba1Ca0.5Cu3O7.195	La	1.5	Ba	1	Ca	0.5	Cu	3													O		7.195	1	1997																												336																		K				74			74																																																																																														La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17062	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.1	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.1	1	1997																											2	336			A	3.881		11.71	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17063	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.12	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.12	1	1997																											2	336			A	3.88		11.704	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17064	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.14	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.14	1	1997																											2	336			A	3.88		11.763	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17065	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.16	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.16	1	1997																											2	336			A	3.879		11.703	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17066	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.18	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.18	1	1997																											2	336			A	3.879		11.698	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17067	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.02	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.02	1	1997																											2	336			A	3.885		11.74	4																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17068	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.14	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.14	1	1997																											2	336			A	3.881		11.71	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17069	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.12	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.12	1	1997																											2	336			A	3.883		11.717	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17070	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O7.08	La	1	Ba	1.5	Ca	0.5	Cu	3													O		7.08	1	1997																											2	336			A	3.885		11.728	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17071	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.86	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.86	1	1997																											2	336			A	3.897		11.786	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17072	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.8	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.8	1	1997																											2	336			A	3.9		11.805	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17073	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.76	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.76	1	1997																												336			A	3.903		11.814	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17074	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.68	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.68	1	1997																											2	336			A	3.907		11.838	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17075	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.6	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.6	1	1997																											2	336			A	3.91		11.864	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17076	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.52	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.52	1	1997																											2	336			A	3.915		11.886	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
17077	PR05515228		(La,Ba,Ca)3Cu3O6	La1Ba1.5Ca0.5Cu3O6.46	La	1	Ba	1.5	Ca	0.5	Cu	3													O		6.46	1	1997																											2	336			A	3.918		11.901	3																																																																																																																La2O3;CaCO3;BaCO3;CuO	1	La2O3 dried 1000C;CuO2(700C) CaCO3,BaCO3(200C)					High-pressure oxidation of the tetragonal La1.5-xBa1.5+x-yCayCu3Oz superconductors	199706		Department of Chemistry, University of Aberdeen, Meston Walk, Aberdeen AB24 3UE, Scotland, United Kingdom	Phys.Rev.B.,55(1997)15228	A.R. West,E.E. Lachowski,J.M.S. Skakle,R.I. Smith		
18100	PR05703650		HgBa2CuO4	Hg1Ba2Cu1O4+y	Hg	1	Ba	2	Cu	1															O	4+y		1	1998																												Hg1201																		K			97				97																																														meV	33	7.9	1																						m.ohm.cm											20														vapor/solid reaction technique					Quasiparticle tunneling spectra of the high-Tc mercury cuprates: Implications of the d-wave two-dimensional van Hove scenario	199802		Department of Applied Physics, Columbia University, New York, New York 10027	Phys.Rev.B,57(1998)3650-3662	C.C. Tsuei,C.W. Chu,J.Y.T. Wei,M.K. Wu,P.J.M. van Bentum,Q. Xiong		
18101	PR05703650		HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+y	Hg	1	Ba	2	Ca	1	Cu	2													O	6+y		5	1998																												Hg1212																		K	122		123	123			123																																														meV	50	9.5	1																						m.ohm.cm											0.4														laser-ablation (100) SrTiO3 substrate					Quasiparticle tunneling spectra of the high-Tc mercury cuprates: Implications of the d-wave two-dimensional van Hove scenario	199802		Department of Applied Physics, Columbia University, New York, New York 10027	Phys.Rev.B,57(1998)3650-3662	C.C. Tsuei,C.W. Chu,J.Y.T. Wei,M.K. Wu,P.J.M. van Bentum,Q. Xiong		
18102	PR05703650		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+y	Hg	1	Ba	2	Ca	2	Cu	3													O	8+y		1	1998																												Hg1223																		K			135				135																																														meV	75	13	1																						m.ohm.cm											20														vapor/solid reaction technique					Quasiparticle tunneling spectra of the high-Tc mercury cuprates: Implications of the d-wave two-dimensional van Hove scenario	199802		Department of Applied Physics, Columbia University, New York, New York 10027	Phys.Rev.B,57(1998)3650-3662	C.C. Tsuei,C.W. Chu,J.Y.T. Wei,M.K. Wu,P.J.M. van Bentum,Q. Xiong		
18103	PR05703683		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-y	Sm	1.85	Ce	0.15	Cu	1															O	4-y		1	1998																												T'																		K	14.5		27.5				21																													T/K		0.38																																																																11	Ref[2]:R. F. Jardim et al., Phys. Rev. B50 10080(1994)					Observation of granular superconductivity in polycrystalline Sm2-xCexCuO4-y	199802		Physics Department, University of Notre Dame, Indiana 46556	Phys.Rev.B,57(1998)3638	A.K. Helman,D.B. Pulling,H.A. Blackstead,P. Beeli,R.F. Jardim		
18104	PR05703683		(Sm,Ce)2CuO4	Sm1.84Ce0.16Cu1O4-y	Sm	1.84	Ce	0.16	Cu	1															O	4-y		1	1998																												T'																		K	18.2						18.2																																																																																															11	Ref[2]:R. F. Jardim et al., Phys. Rev. B50 10080(1994)					Observation of granular superconductivity in polycrystalline Sm2-xCexCuO4-y	199802		Physics Department, University of Notre Dame, Indiana 46556	Phys.Rev.B,57(1998)3638	A.K. Helman,D.B. Pulling,H.A. Blackstead,P. Beeli,R.F. Jardim		
18105	PR05703683		(Sm,Ce)2CuO4	Sm1.83Ce0.17Cu1O4-y	Sm	1.83	Ce	0.17	Cu	1															O	4-y		1	1998																												T'																		K	12						12																																																																																															11	Ref[2]:R. F. Jardim et al., Phys. Rev. B50 10080(1994)					Observation of granular superconductivity in polycrystalline Sm2-xCexCuO4-y	199802		Physics Department, University of Notre Dame, Indiana 46556	Phys.Rev.B,57(1998)3638	A.K. Helman,D.B. Pulling,H.A. Blackstead,P. Beeli,R.F. Jardim		
18106	PR05703683		(Sm,Ce)2CuO4	Sm1.82Ce0.18Cu1O4-y	Sm	1.82	Ce	0.18	Cu	1															O	4-y		1	1998																												T'																		K	8.8						8.8																																																																																															11	Ref[2]:R. F. Jardim et al., Phys. Rev. B50 10080(1994)					Observation of granular superconductivity in polycrystalline Sm2-xCexCuO4-y	199802		Physics Department, University of Notre Dame, Indiana 46556	Phys.Rev.B,57(1998)3638	A.K. Helman,D.B. Pulling,H.A. Blackstead,P. Beeli,R.F. Jardim		
18107	PR05703245		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	1998																												Tl2201																		K				91			91																																														meV	21																																																	Ref[16]:R. Mogilaevsky et al., Physica C 250 15 (1995)					Evidence of dx2-y2 symmetry in the tunneling conductance density of states of Tl2Ba2CuO6	199802		Illinois Institute of Technology, Chicago, Illinois 60616	Phys.Rev.B,57(1998)R3245	D.G. Hinks,J.F. Zasadzinski,K.E. Gray,L. Ozyuzer,R. Mogilevsky,Z. Tusof		
18200	PR05706121		HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O10+d	Hg	1	Ba	2	Ca	3	Cu	4													O	10+d		1	1998																											6	Hg1234	P4/mmm		A	3.852		18.988												K				125		6	125																				T	BCS Clean Limit		205						T/K	Hao-Clem model		2.2				A	BCS clean Limit			12.7	A	BCS clean Limit			157																																																			In High PressureRef[9]:T. I. Dyuzheva et al., J. Alloys, Compd. 223 74 (1995)					Enhanced anisotropic nature of HgBa2Ca3Cu4O10+delta	199803		Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Krea	Phys.Rev.B,57(1998)6121	Efim S. Itskevich,Irina Kuzemskaya,K.A. Lokshin,Mun-Seog Kim,Seong-Cho Yu,Sung-Ik Lee		
18201	PR05706121		HgBa2Ca3Cu4O10	Hg1Ba2Ca3Cu4O10+d	Hg	1	Ba	2	Ca	3	Cu	4													O	10+d		1	1998																											6	Hg1234	P4/mmm		A	3.852		18.988												K				125		6	125																				T	BCS dirty limit		195						T/K	2D scaling function		2.4				A	BCS dirty Limit			13	A	BCS dirty Limit			172																																																			In High PressureRef[9]:T. I. Dyuzheva et al., J. Alloys, Compd. 223 74 (1995)					Enhanced anisotropic nature of HgBa2Ca3Cu4O10+delta	199803		Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Krea	Phys.Rev.B,57(1998)6121	Efim S. Itskevich,Irina Kuzemskaya,K.A. Lokshin,Mun-Seog Kim,Seong-Cho Yu,Sung-Ik Lee		
18202	PR05705535		Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8+d	Pb	2	Sr	2	Y	1	Cu	3													O	8+d		1	1998																											3	Pb3212			A	5.394	5.434	15.725																																																																																																																	PbO,Y2O3,CuO,CaO,SrCO3	1	sintered 830C,20hour argon/oxygen=98%/2%					Structural disorder in the Pb2Sr2Y1-xCaxCu3O8+delta cuprates	199803		Swiss Light Source Project, Paul Scherrer Institute, CH-5232 Villigen PSI, Swizerland	Phys.Rev.B,57(1998)5535	K. Conder,L. Soderholm,P. Pattison,S. Skanthakumar,U. Staub		
18203	PR05705535		Pb2Sr2(Y,Ca)Cu3O8	Pb2Sr2Y0.5Ca0.5Cu3O8+d	Pb	2	Sr	2	Y	0.5	Ca	0.5	Cu	3											O	8+d		1	1998																											3	Pb3212			A	5.379	5.419	15.737												K				70			70																																																																																														PbO,Y2O3,CuO,CaO,SrCO3	1	sintered 830C,20hour argon/oxygen=98%/2%					Structural disorder in the Pb2Sr2Y1-xCaxCu3O8+delta cuprates	199803		Swiss Light Source Project, Paul Scherrer Institute, CH-5232 Villigen PSI, Swizerland	Phys.Rev.B,57(1998)5535	K. Conder,L. Soderholm,P. Pattison,S. Skanthakumar,U. Staub		
18204	PR05705630		(Hg,Au)Ba2Ca2Cu3O8	Hg0.7Au0.3Ba2Ca2Cu3O8+y	Hg	0.7	Au	0.3	Ba	2	Ca	2	Cu	3											O	8+y		6	1998																												Hg1223							35											K										K/GPa	0.8																																																																																											1	1.Ba(2)Ca(n-1)Cu(n)O(x)  ANN 900-925C 72h  2.mix with gold and mercury oxide 3,submit  1.8GPa  950C  1.6h					Overdoped Hg1-xAuxBa2Ca2Cu3O8+x and the origin of the intrinsic increase of Tc under pressure in mercury cuprates	199803		EPM-Matformag and Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble Cedex 9, France	Phys.Rev.B,57(1998)R5630	C. Acha,C. Chaillout,J.J. Capponi,M. Nunez-regueiro,P. Bordet,S.Le Floch		
18205	PR05705082		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1998																											2	Bi2212			A	5.406		30.84	3											K		78.6					78.6																																																																							m.ohm.cm							0.6				2												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18206	PR05705082		BI2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+y	Bi	2	Sr	2	Ca	1	Cu	2													O	8+y		1	1998																											2	Bi2212																		K		71.4					71.4																																																																							m.ohm.cm							0.3				1.2												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h - annealed in oxygen					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18207	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8+y	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8+y		1	1998																											2	Bi2212			A	5.418		30.76	3											K		83					83																																																																							m.ohm.cm							1.3				3												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18208	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.8Pr0.2Cu2O8+y	Bi	2	Sr	2	Ca	0.8	Pr	0.2	Cu	2											O	8+y		1	1998																											2	Bi2212																		K		87.1					87.1																																																																							m.ohm.cm							0.5				1.6												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h - annealed in oxygen					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18209	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8+y	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8+y		1	1998																											2	Bi2212			A	5.427		30.71	3											K		58					58																																																																							m.ohm.cm							1.7				3.7												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18210	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.6Pr0.4Cu2O8+y	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	8+y		1	1998																											2	Bi2212																		K		62.5					62.5																																																																							m.ohm.cm							1.5				3.5												Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h - annealed in oxygen					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18211	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.55Pr0.45Cu2O8+y	Bi	2	Sr	2	Ca	0.55	Pr	0.45	Cu	2											O	8+y		1	1998																											2	Bi2212			A	5.442		30.55	3											K		9.8					9.8																																																																																														Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18212	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.5Pr0.5Cu2O8+y	Bi	2	Sr	2	Ca	0.5	Pr	0.5	Cu	2											O	8+y		1	1998																											2	Bi2212			A	5.452		30.41	3											K		25.9					25.9																																																																																														Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18213	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2O8+y	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	8+y		1	1998																											3	Bi2212			A	5.458	5.449	30.37	3											K					15																																																																									m.ohm.cm				7.7			8.1																Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18214	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.4Pr0.6Cu2O8+y	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	8+y		1	1998																											3	Bi2212																		K					15																																																																									m.ohm.cm				13.8			13.8																Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h - annealed in oxygen					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18215	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.2Pr0.8Cu2O8+y	Bi	2	Sr	2	Ca	0.2	Pr	0.8	Cu	2											O	8+y		1	1998																											3	Bi2212			A	5.465	5.447	30.34	3																																																																																																																Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18216	PR05705082		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.2Pr0.8Cu2O8+y	Bi	2	Sr	2	Ca	0.2	Pr	0.8	Cu	2											O	8+y		1	1998																											3	Bi2212																																																																																																																							Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h - annealed in oxygen					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18217	PR05705082		Bi2Sr2PrCu2O8+y	Bi2Sr2Pr1Cu2O8+y	Bi	2	Sr	2	Pr	1	Cu	2													O	8+y		1	1998																											3	Bi2212			A	5.468	5.447	30.3	3																																																																																																																Bi2O3, SrCO3, CaCO3, Pr6O11, CuO	1	Bi2O3, SrCO3, CaCO3, Pr6O11, CuO ground - sintered in air 850C 12h 3times -  pelletized - calcined 850-930C 72h					Superconductivity and Raman scattering in Bi2Sr2Ca1-xPrxCu2Oy	199803		Structural Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B.,57(1998)5082	C.Y. Xu,G.G. Qian,J. Zou,L.Z. Cao,M. Yu,X.H. Chen,Z.S. Liu		
18218	PR05706165	Superconductivity doesn't appear.	La2CuO4	La2Cu1O4	La	2	Cu	1																	O		4	3	1998																												T																																																																																																																														Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18219	PR05706165	Superconductivity doesn't appear.	(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O		4	3	1998																												T			A			13.172	3																																																																																																																							Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18220	PR05706165		(La,Sr)2CuO4	La1.94Sr0.06Cu1O4	La	1.94	Sr	0.06	Cu	1															O	4		3	1998																												T			A			13.189	3											K				14			14																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18221	PR05706165		(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		3	1998																												T			A			13.2	3											K				24			24																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18222	PR05706165		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1998																												T																		K				29			29																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18223	PR05706165		(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		3	1998																												T			A			13.23	3											K				34			34																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18224	PR05706165		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1998																												T			A			13.24	3											K				38			38																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18225	PR05706165		(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4		3	1998																												T			A			13.249	3											K				37			37																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18226	PR05706165		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	1998																												T			A			13.248	3											K				32			32																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18227	PR05706165		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		3	1998																												T			A			13.26	3											K				16			16																																																																																															7	Heat treatment under 1bar O2 flow 900C, 100h					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18228	PR05706165		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1998																												T																		K				38			38																																																																																																					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18229	PR05706165		(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.993	La	1.85	Sr	0.15	Cu	1															O		3.993	3	1998																												T																		K				20			20																																																																																															7	Deoxygenated by anneal					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18230	PR05706165		(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.987	La	1.85	Sr	0.15	Cu	1															O		3.987	3	1998																												T																		K				12			12																																																																																															7	Deoxygenated by anneal					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18231	PR05706165	Superconductivity doesn't appear.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.98	La	1.85	Sr	0.15	Cu	1															O		3.98	3	1998																												T																																																																																																																								7	Deoxygenated by anneal					Doping dependence of the spatially modulated dynamical spin correlations and the superconducting-transition temperature in La2-xSrxCuO4	199803		Department of Physics, Tohoku University, Aramaki Aoba, Sendai 980-77, Japan	Phys.Rev.B,57(1998)6165	C.H. Lee,G. Shirane,H. Kimura,J. Wada,K. Kurahashi,K. Yamada,M. Greven,M.A. Kastner,R.J. Birgeneau,S. Hosoya,S. Ueki,S. Wakimoto,Y. Endoh,Y.J. Kim		
18299	PR05710923		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1998																												Y124																																																																																						W/K.M	6.3									m.ohm.cm							0.062				0.407														sinter cold-pressed(at high O2, 1000C). Details see J.Appl.Phys. 76(1994)3673					Thermal conductivity of polycrystalline YBa2Cu4O8 from 10 to 300K	199805		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennessee 37831-6116	Phys.Rev.B.,57(1998)10923	J.M. Schmitz,J.O. Scarbrough,J.R. Tompson,R.K. Williams		
18300	PR05707986	high quality single crystal. substrate = YSZ. 	YBa2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1998																												Y123																		K				92.4			92.4																																									A	surface impedance by 10GHz cavity using hot finger technique	1400																																																				5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Systematics of two-component superconductivity in YBa2Cu3O6.95 from microwave measurements of high-quality single crystals	199804		Department of Physics, Northeastern university, 360 Huntington Avenue, Boston, Massachusetts 02115	Phys.Rev.B.,57(1998)7986	H. Srikanth,S. Sridhar,Z. Zhai		
18301	PR05707986	high quality single crystal. substrate = BaZrO3  	YBa2Cu3O6.95	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O		6.95	3	1998																												Y123																		K				93.4			93.4																																									A	surface impedance by 10GHz cavity using hot finger technique	1000																																																				5	Crucible:BZO(BaZrO3)O2 anneal 100bar 20h 700C					Systematics of two-component superconductivity in YBa2Cu3O6.95 from microwave measurements of high-quality single crystals	199804		Department of Physics, Northeastern university, 360 Huntington Avenue, Boston, Massachusetts 02115	Phys.Rev.B.,57(1998)7986	H. Srikanth,S. Sridhar,Z. Zhai		
18302	PR05708667		(B,C)(Sr,Ba)2Ca2Cu3O9	B0.6C0.4Sr0.5Ba1.5Ca2Cu3O9	B	0.6	C	0.4	Sr	0.5	Ba	1.5	Ca	2	Cu	3									O		9	1	1998																												C1223	P4/mmm		A	3.862		14.135												K				119		7	119																				T	clean limit		136													A	clean limit		15.6		A	clean limit	2140																																																			Ba2Ca2Cu3O7,Sr2Ca2Cu3O7,B2O3,Ag2CO3	1	Ref[4]A. Iyo et al., Czech. J. Phys. 46,1481(1996)Precursor:calcined flow O2 1atmSample:calcined 1100C 3hour 4.5GPa					Interlayer coupling and superconducting properties of the triple-layer compound B0.6C0.4(Sr0.25Ba0.75)2Ca2Cu3O9	199804		Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B.,57(1998)8667	A. Iyo,H. Ihara,K. Tokiwa,M. Tokumoto,Mun-Seog Kim,Sung-Ik Lee		
18303	PR05708667		(B,C)(Sr,Ba)2Ca2Cu3O9	B0.6C0.4Sr0.5Ba1.5Ca2Cu3O9	B	0.6	C	0.4	Sr	0.5	Ba	1.5	Ca	2	Cu	3									O		9	1	1998																												C1223	P4/mmm		A	3.862		14.135												K				119		7	119																				T	dirty limit		130													A	dirty limit		16		A	dirty limit	2370																																																			Ba2Ca2Cu3O7,Sr2Ca2Cu3O7,B2O3,Ag2CO3	1	Ref[4]A. Iyo et al., Czech. J. Phys. 46,1481(1996)Precursor:calcined flow O2 1atmSample:calcined 1100C 3hour 4.5GPa					Interlayer coupling and superconducting properties of the triple-layer compound B0.6C0.4(Sr0.25Ba0.75)2Ca2Cu3O9	199804		Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B.,57(1998)8667	A. Iyo,H. Ihara,K. Tokiwa,M. Tokumoto,Mun-Seog Kim,Sung-Ik Lee		
18304	PR05708680		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		3	1998																												T																		K				17.5			17.5																																														meV	2.2		1																																														7	Ref[25]:K. Oka et al.,Jpn. J. Appl.Phys.,Part 1 28,937 (1989)Traveling-Solvent floating Zoneanneal O2 1E-4atm 1000C 4days					Tunneling spectroscopy of superconducting Nd1.85Ce0.15CuO4-delta	199804		Electrotechnical Laboratory, Umezono, tsukuba, Ibaraki 305, Japan	Phys.Rev.B.,57(1998)8680	H. Takashima,K. Kajimura,K. Oka,M. Koyanagi,S. Kashiwaya,S. Ueno,T. Ito,Y. Tanaka		
18305	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.45Y0.55Cu2O8+d	Bi	2	Sr	2	Ca	0.45	Y	0.55	Cu	2											O	8+d		1	1998																												Bi2212																		K		9.91					9.91																																																																			-2.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18306	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2O8+d	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	8+d		1	1998																												Bi2212																		K		34.9					34.9																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18307	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.55Y0.45Cu2O8+d	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	2											O	8+d		1	1998																												Bi2212																		K		50.4					50.4																																																																			5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18308	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8+d	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+d		1	1998																												Bi2212																		K		65.5					65.5																																																																			11				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18309	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.62Y0.38Cu2O8+d	Bi	2	Sr	2	Ca	0.62	Y	0.38	Cu	2											O	8+d		1	1998																												Bi2212																		K		72.4					72.4																																																																			16.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18310	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.65Y0.35Cu2O8+d	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	2											O	8+d		1	1998																												Bi2212																		K		80					80																																																																			25				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18311	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.68Y0.32Cu2O8+d	Bi	2	Sr	2	Ca	0.68	Y	0.32	Cu	2											O	8+d		1	1998																												Bi2212																		K		81.9					81.9																																																																			36.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18312	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+d		1	1998																												Bi2212																		K		87.5					87.5																																																																			2				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18313	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.75Y0.25Cu2O8+d	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	2											O	8+d		1	1998																												Bi2212																		K		87.9					87.9																																																																			5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18314	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8+d	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+d		1	1998																												Bi2212																		K		86.6					86.6																																																																			12				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18315	PR05707491		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.85Y0.15Cu2O8+d	Bi	2	Sr	2	Ca	0.85	Y	0.15	Cu	2											O	8+d		1	1998																												Bi2212																		K		84					84																																																																			15				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18316	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.5Y0.5Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		16.4					16.4																																																																			22.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18317	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.55Y0.45Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		34.5					34.5																																																																			35.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18318	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.6Y0.4Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		53					53																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18319	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.62Y0.38Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.62	Y	0.38	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		58.2					58.2																																																																			5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18320	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.65Y0.35Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		65.5					65.5																																																																			7.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18321	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.67Y0.33Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.67	Y	0.33	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		71.1					71.1																																																																			11				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18322	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		74.6					74.6																																																																			15.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18323	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.75Y0.25Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		78.5					78.5																																																																			28				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18324	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.8Y0.2Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		77.6					77.6																																																																			35				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18325	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.85Y0.15Cu1.98Zn0.02O8+d	Bi	2	Sr	2	Ca	0.85	Y	0.15	Cu	1.98	Zn	0.02									O	8+d		1	1998																												Bi2212																		K		77.2					77.2																																																																			11				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18326	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.5Y0.5Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K					4.2																																																																					16				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18327	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.55Y0.45Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		19					19																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18328	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.6Y0.4Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		33.6					33.6																																																																			22.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18329	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.65Y0.35Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		47.8					47.8																																																																			12.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18330	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.66Y0.34Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.66	Y	0.34	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		51.3					51.3																																																																			19				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18331	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.67Y0.33Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.67	Y	0.33	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		51.7					51.7																																																																			40.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18332	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.69Y0.31Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.69	Y	0.31	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		52.6					52.6																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18333	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		54.3					54.3																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18334	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.72Y0.28Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.72	Y	0.28	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		70.3					70.3																																																																			22.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18335	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.75Y0.25Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		75.4					75.4																																																																			25.5				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18336	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.8Y0.2Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		75					75																																																																			30				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18337	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.85Y0.15Cu1.96Zn0.04O8+d	Bi	2	Sr	2	Ca	0.85	Y	0.15	Cu	1.96	Zn	0.04									O	8+d		1	1998																												Bi2212																		K		71.6					71.6																																																																			16				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18338	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.5Y0.5Cu1.95Zn0.05O8+d	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.95	Zn	0.05									O	8+d		1	1998																												Bi2212																		K					4.2																																																																					19				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18339	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.55Y0.45Cu1.95Zn0.05O8+d	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	1.95	Zn	0.05									O	8+d		1	1998																												Bi2212																		K		19					19																																																																							m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18340	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.6Y0.4Cu1.95Zn0.05O8+d	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.95	Zn	0.05									O	8+d		1	1998																												Bi2212																		K		29.3					29.3																																																																			39				m.ohm.cm																							Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18341	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.65Y0.35Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		42.7					42.7																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18342	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.66Y0.34Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.66	Y	0.34	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		43.1					43.1																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18343	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.67Y0.33Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.67	Y	0.33	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		37.5					37.5																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18344	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.69Y0.31Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.69	Y	0.31	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		32.8					32.8																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18345	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		48.7					48.7																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18346	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.73Y0.27Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.73	Y	0.27	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		45.7					45.7																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18347	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.75Y0.25Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		49.1					49.1																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18348	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.8Y0.2Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		75					75																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18349	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.85Y0.15Cu1.95Zn0.05O8+z	Bi	2	Sr	2	Ca	0.85	Y	0.15	Cu	1.95	Zn	0.05									O	8+z		1	1998																												Bi2212																		K		65.1					65.1																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18350	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.55Y0.45Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.55	Y	0.45	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		11.6					11.6																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18351	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.6Y0.4Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		26.3					26.3																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18352	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.62Y0.38Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.62	Y	0.38	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		41.8					41.8																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18353	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.65Y0.35Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.65	Y	0.35	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		31					31																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18354	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.66Y0.34Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.66	Y	0.34	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		18.1					18.1																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18355	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.68Y0.32Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.68	Y	0.32	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		29.3					29.3																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18356	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.7Y0.3Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		29.3					29.3																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18357	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.73Y0.27Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.73	Y	0.27	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		40.1					40.1																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18358	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.75Y0.25Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		36.6					36.6																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18359	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.8Y0.2Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		70.2					70.2																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18360	PR05707491		Bi2Sr2(Ca,Y)(Cu,Zn)2O8	Bi2Sr2Ca0.85Y0.15Cu1.94Zn0.06O8+z	Bi	2	Sr	2	Ca	0.85	Y	0.15	Cu	1.94	Zn	0.06									O	8+z		1	1998																												Bi2212																		K		59.5					59.5																																																																																														Bi2O3,SrCO3,CaCO3,Y2O3,CuO,ZnO	1	prefire 800C 12h Airpress,sintered 860-880C 24hour					Anomalous suppression of superconductivity in Zn-substituted Bi2Sr2Ca1-xYx(Cu1-yZny)2O8+dlta	199804		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aramaki Aoba, Aoba-ku, Sendai 980-77, Japan	Phys.Rev.B.,57(1998)7491	Megumi Akoshima,Takashi Noji,Tasuhiro Ono,Yoji Koike		
18500	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	91						91																																																																							m.ohm.cm								0.13				0.49		mic. Ohm c		0.4		1.3	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18501	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	90.5						90.5																																																																							m.ohm.cm								0.23						mic. Ohm c		0.8		2.3	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18502	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	84						84																																																																							m.ohm.cm								0.31						mic. Ohm c				3.8	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18503	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	78						78																																																																							m.ohm.cm								0.26				0.93		mic. Ohm c		1.8		5	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18504	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	72						72																																																																							m.ohm.cm								0.58				1.06		mic. Ohm c		1.9		6.9	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18505	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	53						53																																																																							m.ohm.cm								0.68						mic. Ohm c				8.6	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18506	PR05713872		YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		3	1998																												Y123																		K	39						39																																																																							m.ohm.cm								1.13				1.3		mic. Ohm c		3.7		15.2	5.5						Ref. [23]; Th. Worf et al., J. Cryst. Growth 96, 1010 (1989)and annealed at 350C in Ar					Hall effect of YBa2Cu3O7-delta single crystals	199806				H.R. Ott,R. Jin		
18507	PR05714084	growth direction:c axis	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		5	1998																												Y123																		K		84					84																				T	T=1.6K					240		1.6																																																																			16	pulse laser abrationsubstrate:MgO(001)	5				Transport measurements of in-plane critical fields in YBa2Cu3O7-delta to 300 T 	199806		National pulsed Magnet Laboratory and Semiconductor Nanofabrication Facility, School of Physics, Yuniversity of New South Wales, Sydney 2052, Australia 	Phys.Rev.B,57(1998)R14084	A.I.Bykov,A.S.Dzurak,A.Skougarevsky,B.D.Bartram,B.E.Kane,C.M.Fowler,C.Mielke,D.Clark,D.G.Rickel,E.E.Mitchell,G.R.Facer,H.Nakagawa,J.C.King,J.D.Goettee,J.Herrmann,J.O.`Brien,K.-H.Muller,L.J.Campbell,N.E.Lumpkin,N.Miura,O.M.tatsenko,R.G.Clark,R.P.Starrett,V.V.Platonov,W.D.Zerwekh,Y.Enomoto		
18508	PR05713922		HgBa2CaCu2O6+d	Hg1Ba2Ca1Cu2O6+d	Hg	1	Ba	2	Ca	1	Cu	2													O	6+d		1	1998																												Hg1212			A	3.861		12.701	3	3																																																																																																																11	precursor Ba-Ca-Cu-Osolution:tartaric acid decompsed: Vac. 850C mixed HgOreact in silica tube 800C 30h and O2 Anneal 300C 6hour					Pressure effect in the Hg-based superconducyors: A structural study	199806		Department of Physics, Chalmers University of Technology, S-41296 Gothenburg, Sweden	Phys.Rev.B,57(1998)13922	A. Kareiba,I. Bryntse,I. Panas,J.S. Olsen,L. Gerward,L.G. Jhansson,R. Gatt		
18509	PR05713922		HgBa2Ca2Cu3O8+d	Hg1Ba2Ca2Cu3O8+d	Hg	1	Ba	2	Ca	2	Cu	3													O	8+d		1	1998																												Hg1223			A	3.857		15.857	3	3																																																																																																																11	precursor Ba-Ca-Cu-Osolution:tartaric acid decompsed: Vac. 850C mixed HgOreact in silica tube 800C 30h and O2 Anneal 300C 6hour					Pressure effect in the Hg-based superconducyors: A structural study	199806		Department of Physics, Chalmers University of Technology, S-41296 Gothenburg, Sweden	Phys.Rev.B,57(1998)13922	A. Kareiba,I. Bryntse,I. Panas,J.S. Olsen,L. Gerward,L.G. Jhansson,R. Gatt		
18510	PR05713422	d-wave BCS model	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1998																												Y123																		K				92			92																																									um	susceptibility		0.14	1.26	K	405																																															Y2O3, BaCO3, CuO	1	d=0.0 anneal O2 1atm 380C 24h   d=0.3 anneal O2 1atm  650C 12hd=0.43 anneal 0.2% O2/N2 1atm 550C 12h					Systematic behavior of the in-plane penetration depth in d-wave cuprates			Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambrige, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)13422	C. Panagopoulos,J.R. Cooper,T. Xiang		
18511	PR05713422	d-wave BCS model	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1998																												Y123																		K				66			66																																									um	susceptibility		0.21	4.53	K	280																																															Y2O3, BaCO3, CuO	1	d=0.0 anneal O2 1atm 380C 24h   d=0.3 anneal O2 1atm  650C 12hd=0.43 anneal 0.2% O2/N2 1atm 550C 12h					Systematic behavior of the in-plane penetration depth in d-wave cuprates			Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambrige, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)13422	C. Panagopoulos,J.R. Cooper,T. Xiang		
18512	PR05713422	d-wave BCS model	YBa2Cu3O7-d	Y1Ba2Cu3O7-d	Y	1	Ba	2	Cu	3															O	7-d		1	1998																												Y123																		K				57			57																																									um	susceptibility		0.28	7.17	K	220																																															Y2O3, BaCO3, CuO	1	d=0.0 anneal O2 1atm 380C 24h   d=0.3 anneal O2 1atm  650C 12hd=0.43 anneal 0.2% O2/N2 1atm 550C 12h					Systematic behavior of the in-plane penetration depth in d-wave cuprates			Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambrige, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)13422	C. Panagopoulos,J.R. Cooper,T. Xiang		
18513	PR05714470	Superconductor	Bi1.8Pb0.3Sr1.9CuOy	Bi1.8Pb0.3Sr1.9CuOy	Bi	1.8	Pb	0.3	Sr	1.9	Cu														O	y		1	1998																															A	5.382	5.326	24.627												K				4.7			4.7																																																						mJ/mole.K	17.2	mJ/molK2	6														m.ohm.cm				3.3							5.45												Bi2O3, PbO2, SrCO3, CuO	1	mixed 2h clacined 815C 8h sintered 840C 30h air					Specific-heat anomaly of overdoped Bi1.8Pb0.3Sr1.9CuOy	199806		Department of Applied Physics, Hokkaido University, Sapporo 060, Japan	Phys.Rev.B,57(1998)14470	H.Mayama,K.Yamaya,Y.Okajima		
18514	PR05714470	Normal	Bi1.8Pb0.3Sr1.9CuOy	Bi1.8Pb0.3Sr1.9CuOy	Bi	1.8	Pb	0.3	Sr	1.9	Cu														O	y		1	1998																															A	5.382	5.326	24.627												K																																																															mJ/molK2	8.7														m.ohm.cm				1.3							2.85												Bi2O3, PbO2, SrCO3, CuO	1	mixed 2h clacined 815C 8h sintered 840C 30h airannealed 450C 700h Ar					Specific-heat anomaly of overdoped Bi1.8Pb0.3Sr1.9CuOy	199806		Department of Applied Physics, Hokkaido University, Sapporo 060, Japan	Phys.Rev.B,57(1998)14470	H.Mayama,K.Yamaya,Y.Okajima		
18600	PR05800611		(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	1998																												T																		K			30				30																																																																							m.ohm.cm						520			870				300											7						Out-of-plane magnetoresistance of La2-xSrxCuO4: Evidence for intraplanar scatterrire in the c-axis transport	7		Interdisciplinary Research Centre for Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)R611	J.R.Cooper,N.E.Hussey,Y.Kodama,Y.Nishihara		
18601	PR05800611		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4		3	1998																												T																		K			40				40																																																																							m.ohm.cm						100			115				110											7						Out-of-plane magnetoresistance of La2-xSrxCuO4: Evidence for intraplanar scatterrire in the c-axis transport	7		Interdisciplinary Research Centre for Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)R611	J.R.Cooper,N.E.Hussey,Y.Kodama,Y.Nishihara		
18602	PR05800611		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1998																												T																		K			42				42																																																																							m.ohm.cm						65			70				78											7						Out-of-plane magnetoresistance of La2-xSrxCuO4: Evidence for intraplanar scatterrire in the c-axis transport	7		Interdisciplinary Research Centre for Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)R611	J.R.Cooper,N.E.Hussey,Y.Kodama,Y.Nishihara		
18603	PR05800611		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		3	1998																												T																		K			6				6																																																																							m.ohm.cm						10			5				35											7						Out-of-plane magnetoresistance of La2-xSrxCuO4: Evidence for intraplanar scatterrire in the c-axis transport	7		Interdisciplinary Research Centre for Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B,57(1998)R611	J.R.Cooper,N.E.Hussey,Y.Kodama,Y.Nishihara		
18604	PR05800619		PrBa2Cu3O6.6	Pr1Ba2Cu3O6.6	Pr	1	Ba	2	Cu	3															O		6.6	3	1998																											3	Y123			A	3.883	3.948	11.823	1											K	56.5		63.5				60			K/GPa	7.4																																																																			m.ohm.cm					0.6			0.62				0.4												7						Unusually large Tc enhancement in superconducting PrBa2Cu3Ox under pressure	7		National research Institute for Metals, 1-2-1 Sengen, Tsukuba 305, Japan	Phys.Rev.B,57(1998)R619	Akiyuki Matsushita,AkiyukiMatsushita,Jinhua Ye,JinhuaYe,Kunihiko Oka,KunihikoOka,Takehiko Matsumoto,TakehikoMatsumoto,Yoshikazu Nishihara,YoshikazuNishihara,Zhigang Zou,ZhigangZou		
18605	PR05800619		PrBa2Cu3O6.8	Pr1Ba2Cu3O6.8	Pr	1	Ba	2	Cu	3															O		6.8	3	1998																											3	Y123																		K	81					4	81			K/GPa	3.8																																																																																											7						Unusually large Tc enhancement in superconducting PrBa2Cu3Ox under pressure	7		National research Institute for Metals, 1-2-1 Sengen, Tsukuba 305, Japan	Phys.Rev.B,57(1998)R619	Akiyuki Matsushita,AkiyukiMatsushita,Jinhua Ye,JinhuaYe,Kunihiko Oka,KunihikoOka,Takehiko Matsumoto,TakehikoMatsumoto,Yoshikazu Nishihara,YoshikazuNishihara,Zhigang Zou,ZhigangZou		
18606	PR05801068	pure	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		5	1998																												Y123			A			11.71																																																																																										m.ohm.cm				8000							70														pulsed laser deposition. substrate:LaAlO3					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18607	PR05801068	amount of impurity : 4 %	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		5	1998																												Y123																																																																																																m.ohm.cm				400							15														pulsed laser deposition. substrate:LaAlO3					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18608	PR05801068	amount of impurity : 12 %	PrBa2Cu3O7	Pr1Ba2Cu3O7	Pr	1	Ba	2	Cu	3															O	7		5	1998																												Y123																																																																																																m.ohm.cm	9			6							2.5														pulsed laser deposition. substrate:LaAlO3					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18609	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.7Sr1.3Cu3O7	Pr	1	Ba	0.7	Sr	1.3	Cu	3													O	7		5	1998																												Y123			A			11.653																																																																																										m.ohm.cm				220							12														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 780 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18610	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.7Sr1.3Cu3O7	Pr	1	Ba	0.7	Sr	1.3	Cu	3													O	7		5	1998																												Y123																																																																																																m.ohm.cm				30							8														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 760 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18611	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.7Sr1.3Cu3O7	Pr	1	Ba	0.7	Sr	1.3	Cu	3													O	7		5	1998																												Y123			A			11.621																																																																																										m.ohm.cm	200			10							5														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 740 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18612	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.7Sr1.3Cu3O7	Pr	1	Ba	0.7	Sr	1.3	Cu	3													O	7		5	1998																												Y123																																																																																																m.ohm.cm	110			6							5														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 660 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18613	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.4Sr1.6Cu3O7	Pr	1	Ba	0.4	Sr	1.6	Cu	3													O	7		5	1998																												Y123			A			11.588																																																																																										m.ohm.cm	30			6.8							3.8														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 760 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18614	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.4Sr1.6Cu3O7	Pr	1	Ba	0.4	Sr	1.6	Cu	3													O	7		5	1998																												Y123			A			11.576																																																																																										m.ohm.cm	10			4.2							3.2														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 740 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18615	PR05801068		Pr(Ba,Sr)2Cu3O7	Pr1Ba0.4Sr1.6Cu3O7	Pr	1	Ba	0.4	Sr	1.6	Cu	3													O	7		5	1998																												Y123																																																																																																m.ohm.cm	5.5			3.3							2.8														pulsed laser deposition. substrate : LaAlO3.substrate temperature : 720 C					Electrical transport properties of highly doped PrBa2-xSrxCu3O7 thin films prepared by pulsed laser deposition	7		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.REv.B,58(1998)1068	M.Rajeswari,R.P.Sharma,T.Venkatesan,Y.G.Zhao,Z.W.Dong		
18616	PR05801000		Bi2Sr2Ca1Cu2O8	Bi2Sr2Ca1Cu2O8+d	Bi	2	Sr	2	Ca	1	Cu	2													O	8+d		3	1998																												Bi2212							1											K				86			86																																									A	Shown in fig6 .(ab-plain)  Deteminated HC1 and ref11.		1800																																																		Bi2O3,SrCO3,CaCO3,Pr6O11,CuO	5	The off-stoichiometric ratio were mixed,ground,and calcined in air for 1 day. The reacted powders with excess Bi2O3 included as a flux were thenused for crystal growth .And post post annealed 360 in a					Effect of Pr scattering on the penetration depth lambda ab in Bi2Sr2Ca1-xPrxCu2O8+delta single crystals	7		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan and Structure Research Laboratory, University of Science and Technology of China, Anhui 230026, China	Phys.Rev.B,58(1998)1000	H.C.Ku,X.-G.Li,X.F.Sun,Y.H.Toh,Y.Y.Hsu		
18617	PR05801000		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.89Pr0.11Cu2O8+d	Bi	2	Sr	2	Ca	0.89	Pr	0.11	Cu	2											O	8+d		3	1998																												Bi2212							1											K				88			88																																									A	Shown in fig6.(ab-plain)Determinated HC1 and ref11.		2200																																																		Bi2O3,SrCO3,CaCO3,Pr6O11,CuO	5	The off-stoichiometric ratio were mixed,ground,and calcined in air for 1 day. The reacted powders with excess Bi2O3 included as a flux were thenused for crystal growth .And post post annealed 360 in a					Effect of Pr scattering on the penetration depth lambda ab in Bi2Sr2Ca1-xPrxCu2O8+delta single crystals	7		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan and Structure Research Laboratory, University of Science and Technology of China, Anhui 230026, China	Phys.Rev.B,58(1998)1000	H.C.Ku,X.-G.Li,X.F.Sun,Y.H.Toh,Y.Y.Hsu		
18618	PR05801000		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.83Pr0.17Cu2O8+d	Bi	2	Sr	2	Ca	0.83	Pr	0.17	Cu	2											O	8+d		3	1998																												Bi2212							1											K				84			84																																									A	shown in fig6(ab-plain).Determinated HC1 and ref11.		2500																																																		Bi2O3,SrCO3,CaCO3,Pr6O11,CuO	5	The off-stoichiometric ratio were mixed,ground,and calcined in air for 1 day. The reacted powders with excess Bi2O3 included as a flux were thenused for crystal growth .And post post annealed 360 in a					Effect of Pr scattering on the penetration depth lambda ab in Bi2Sr2Ca1-xPrxCu2O8+delta single crystals	7		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan and Structure Research Laboratory, University of Science and Technology of China, Anhui 230026, China	Phys.Rev.B,58(1998)1000	H.C.Ku,X.-G.Li,X.F.Sun,Y.H.Toh,Y.Y.Hsu		
18619	PR05801000		Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.72Pr0.28Cu2O8+d	Bi	2	Sr	2	Ca	0.72	Pr	0.28	Cu	2											O	8+d		3	1998																												Bi2212			A	5.435	5.439	30.701	1											K				71			71																																									A	Shown in fig6.(ab-plain)Determinated HC1 and ref11		2900																																																		Bi2O3,SrCO3,CaCO3,Pr6O11,CuO	5	The off-stoichiometric ratio were mixed,ground,and calcined in air for 1 day. The reacted powders with excess Bi2O3 included as a flux were thenused for crystal growth .And post post annealed 360 in a					Effect of Pr scattering on the penetration depth lambda ab in Bi2Sr2Ca1-xPrxCu2O8+delta single crystals	7		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan and Structure Research Laboratory, University of Science and Technology of China, Anhui 230026, China	Phys.Rev.B,58(1998)1000	H.C.Ku,X.-G.Li,X.F.Sun,Y.H.Toh,Y.Y.Hsu		
18800	PR05805856		La2CuO4	La2Cu1O4.012	La	2	Cu	1																	O	4.012		1	1998																											3	T			A	5.3632	5.4162	13.179												K				32			32																																																																																															1	Solid state reaction anneal O2 100C 650bar					Superconducting properties in La2CuO4+delta with excess oxygen	9		Department of Material Science, Faculty of Science, Himeji Institute of Technology, 1475-2, Kanaji, Kamigori-cho, Ako-gun, Hyogo, 678-1297, Japan	Phys.Rev.B.,58(1998)5856	Akihiko Sumiyama,Masahito Nakagawa,Toshikazu Hirayama,Tosikazu Hirayama,Yasukage Oda		
18801	PR05805856		La2CuO4	La2Cu1O4.022	La	2	Cu	1																	O	4.022		1	1998																											3	T			A	5.3446	5.4334	13.252												K				42			42																																																																																															1	Solid state reaction anneal O2 100C 650bar electronical oxidation 333K 72h (in KOH)					Superconducting properties in La2CuO4+delta with excess oxygen	9		Department of Material Science, Faculty of Science, Himeji Institute of Technology, 1475-2, Kanaji, Kamigori-cho, Ako-gun, Hyogo, 678-1297, Japan	Phys.Rev.B.,58(1998)5856	Akihiko Sumiyama,Masahito Nakagawa,Toshikazu Hirayama,Tosikazu Hirayama,Yasukage Oda		
18802	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.4389	5.50414	23.1569	3																																																																																																																	1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 600atm 600C O2 anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18803	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.44746	5.50517	23.1556	3																																																																																																																	1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) As prepare					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18804	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.44663	5.50424	23.1517	3											K				24			24																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 200C Ar anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18805	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.45092	5.50119	23.1645	3											K				25			25																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 450C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18806	PR05805831		(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4	4	1	1998							560																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18807	PR05805831		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4	4	1	1998							450																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18808	PR05805831		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4	4	1	1998							300																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18809	PR05805831		(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4	4	1	1998							185																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18810	PR05805831		(La,Sr)2CuO4	La1.795Sr0.205Cu1O4	La	1.795	Sr	0.205	Cu	1															O	4	4	1	1998							130																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18811	PR05805831		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4	4	1	1998			emuK/g	0			500																					T							1											K			37				37																																																																																																La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18812	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.86Sr0.14Cu0.995Ni0.005O4	La	1.86	Sr	0.14	Cu	0.995	Ni	0.005													O	4	4	1	1998			emuK/g	0			507																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18813	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.86Sr0.14Cu0.99Ni0.01O4	La	1.86	Sr	0.14	Cu	0.99	Ni	0.01													O	4	4	1	1998			emuK/g	0			515																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18814	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.86Sr0.14Cu0.98Ni0.02O4	La	1.86	Sr	0.14	Cu	0.98	Ni	0.02													O	4	4	1	1998			emuK/g	0.0000022			514																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18815	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.86Sr0.14Cu0.97Ni0.03O4	La	1.86	Sr	0.14	Cu	0.97	Ni	0.03													O	4	4	1	1998			emuK/g	0.0000035			525																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18816	PR05805831		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4	4	1	1998			emuK/g	0			350																					T							1																																																																										mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18817	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.99Ni0.01O4	La	1.84	Sr	0.16	Cu	0.99	Ni	0.01													O	4	4	1	1998							395																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18818	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.985Ni0.015O4	La	1.84	Sr	0.16	Cu	0.985	Ni	0.015													O	4	4	1	1998							420																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18819	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.98Ni0.02O4	La	1.84	Sr	0.16	Cu	0.98	Ni	0.02													O	4	4	1	1998							420																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18820	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.97Ni0.03O4	La	1.84	Sr	0.16	Cu	0.97	Ni	0.03													O	4	4	1	1998							420																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18821	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.84Sr0.16Cu0.96Ni0.04O4	La	1.84	Sr	0.16	Cu	0.96	Ni	0.04													O	4	4	1	1998							425																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18822	PR05805831		(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4	4	1	1998			emuK/g	0			230																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18823	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.99Ni0.01O4	La	1.82	Sr	0.18	Cu	0.99	Ni	0.01													O	4	4	1	1998			emuK/g	0			265																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18824	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.98Ni0.02O4	La	1.82	Sr	0.18	Cu	0.98	Ni	0.02													O	4	4	1	1998			emuK/g	0			325																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18825	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.975Ni0.025O4	La	1.82	Sr	0.18	Cu	0.975	Ni	0.025													O	4	4	1	1998			emuK/g	0.0000012			330																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18826	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.97Ni0.03O4	La	1.82	Sr	0.18	Cu	0.97	Ni	0.03													O	4	4	1	1998			emuK/g	0.0000028			350																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18827	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.835Sr0.165Cu0.995Ni0.005O4	La	1.835	Sr	0.165	Cu	0.995	Ni	0.005													O	4	4	1	1998																												T							1											K			33				33																																																								mJ/K2mole	4.25																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18828	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.99Ni0.01O4	La	1.83	Sr	0.17	Cu	0.99	Ni	0.01													O	4	4	1	1998																												T							1											K			29				29																																																								mJ/K2mole	0.85																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18829	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.825Sr0.175Cu0.985Ni0.015O4	La	1.825	Sr	0.175	Cu	0.985	Ni	0.015													O	4	4	1	1998																												T							1											K			25				25																																																																																																La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18830	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.97Ni0.03O4	La	1.82	Sr	0.18	Cu	0.97	Ni	0.03													O	4	4	1	1998			emuK/g	0.0000042			355																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18831	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.96Ni0.04O4	La	1.82	Sr	0.18	Cu	0.96	Ni	0.04													O	4	4	1	1998							360																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18832	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.82Sr0.18Cu0.95Ni0.05O4	La	1.82	Sr	0.18	Cu	0.95	Ni	0.05													O	4	4	1	1998							360																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18833	PR05805831		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4	4	1	1998							130																					T							1											K			22				22																																																								mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18834	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.995Ni0.005O4	La	1.8	Sr	0.2	Cu	0.995	Ni	0.005													O	4	4	1	1998							165																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18835	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.99Ni0.01O4	La	1.8	Sr	0.2	Cu	0.99	Ni	0.01													O	4	4	1	1998							170																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18836	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.985Ni0.015O4	La	1.8	Sr	0.2	Cu	0.985	Ni	0.015													O	4	4	1	1998							210																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18837	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.98Ni0.02O4	La	1.8	Sr	0.2	Cu	0.98	Ni	0.02													O	4	4	1	1998							210																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18838	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.975Ni0.025O4	La	1.8	Sr	0.2	Cu	0.975	Ni	0.025													O	4	4	1	1998							250																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18839	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.97Ni0.03O4	La	1.8	Sr	0.2	Cu	0.97	Ni	0.03													O	4	4	1	1998							300																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18840	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.96Ni0.04O4	La	1.8	Sr	0.2	Cu	0.96	Ni	0.04													O	4	4	1	1998							310																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18841	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.95Ni0.05O4	La	1.8	Sr	0.2	Cu	0.95	Ni	0.05													O	4	4	1	1998							325																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18842	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.94Ni0.06O4	La	1.8	Sr	0.2	Cu	0.94	Ni	0.06													O	4	4	1	1998							345																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18843	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.93Ni0.07O4	La	1.8	Sr	0.2	Cu	0.93	Ni	0.07													O	4	4	1	1998							350																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18844	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.795Sr0.205Cu0.995Ni0.005O4	La	1.795	Sr	0.205	Cu	0.995	Ni	0.005													O	4	4	1	1998																												T							1																																																																										mJ/K2mole	0.88																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18845	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.79Sr0.21Cu0.99Ni0.01O4	La	1.79	Sr	0.21	Cu	0.99	Ni	0.01													O	4	4	1	1998																												T							1																																																																										mJ/K2mole	1.32																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18846	PR05805831		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4	4	1	1998							130																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18847	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.99Ni0.01O4	La	1.78	Sr	0.22	Cu	0.99	Ni	0.01													O	4	4	1	1998							140																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18848	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.985Ni0.015O4	La	1.78	Sr	0.22	Cu	0.985	Ni	0.015													O	4	4	1	1998							150																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18849	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.98Ni0.02O4	La	1.78	Sr	0.22	Cu	0.98	Ni	0.02													O	4	4	1	1998							170																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18850	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.97Ni0.03O4	La	1.78	Sr	0.22	Cu	0.97	Ni	0.03													O	4	4	1	1998							200																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18851	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.96Ni0.04O4	La	1.78	Sr	0.22	Cu	0.96	Ni	0.04													O	4	4	1	1998							245																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18852	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.955Ni0.045O4	La	1.78	Sr	0.22	Cu	0.955	Ni	0.045													O	4	4	1	1998							260																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18853	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.95Ni0.05O4	La	1.78	Sr	0.22	Cu	0.95	Ni	0.05													O	4	4	1	1998							270																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18854	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.94Ni0.06O4	La	1.78	Sr	0.22	Cu	0.94	Ni	0.06													O	4	4	1	1998							285																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18855	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.93Ni0.07O4	La	1.78	Sr	0.22	Cu	0.93	Ni	0.07													O	4	4	1	1998							300																					T							1																																																																																																																		La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18856	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.92Ni0.08O4	La	1.78	Sr	0.22	Cu	0.92	Ni	0.08													O	4	4	1	1998							300																					T							1											K			21				21																																																																																																La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18857	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.775Sr0.225Cu0.995Ni0.005O4	La	1.775	Sr	0.225	Cu	0.995	Ni	0.005													O	4	4	1	1998																												T							1											K			21				21																																																																																																La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18858	PR05805831		(La,Sr)2(Cu,Ni)O4	La1.77Sr0.23Cu0.99Ni0.01O4	La	1.77	Sr	0.23	Cu	0.99	Ni	0.01													O	4	4	1	1998																												T							1											K			18				18																																																																																																La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18859	PR05805831		(La,Sr)2CuO4	La1.99Sr0.01Cu1O4	La	1.99	Sr	0.01	Cu	1															O	4	4	1	1998																												T							1																																																						A			46																	mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18860	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.99Sr0.01Cu0.996Zn0.004O4	La	1.99	Sr	0.01	Cu	0.996	Zn	0.004													O	4	4	1	1998																												T							1																																																						A			46																	mJ/K2mole	1.8																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18861	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.99Sr0.01Cu0.992Zn0.008O4	La	1.99	Sr	0.01	Cu	0.992	Zn	0.008													O	4	4	1	1998																												T							1																																																						A			46																	mJ/K2mole	2.8																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18862	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.99Sr0.01Cu0.988Zn0.012O4	La	1.99	Sr	0.01	Cu	0.988	Zn	0.012													O	4	4	1	1998																												T							1																																																						A			46																	mJ/K2mole	3.5																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18863	PR05805831		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18864	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.86Sr0.14Cu0.9975Zn0.0025O4	La	1.86	Sr	0.14	Cu	0.9975	Zn	0.0025													O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	1.5																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18865	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.86Sr0.14Cu0.995Zn0.005O4	La	1.86	Sr	0.14	Cu	0.995	Zn	0.005													O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	2.25																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18866	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.86Sr0.14Cu0.994Zn0.006O4	La	1.86	Sr	0.14	Cu	0.994	Zn	0.006													O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	2.6																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18867	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.86Sr0.14Cu0.99Zn0.01O4	La	1.86	Sr	0.14	Cu	0.99	Zn	0.01													O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	3.8																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18868	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.86Sr0.14Cu0.985Zn0.015O4	La	1.86	Sr	0.14	Cu	0.985	Zn	0.015													O	4	4	1	1998																												T							1																																																						A			39																	mJ/K2mole	4.6																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18869	PR05805831		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18870	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.9975Zn0.0025O4	La	1.84	Sr	0.16	Cu	0.9975	Zn	0.0025													O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	1.65																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18871	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.995Zn0.005O4	La	1.84	Sr	0.16	Cu	0.995	Zn	0.005													O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	3.4																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18872	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.99Zn0.01O4	La	1.84	Sr	0.16	Cu	0.99	Zn	0.01													O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	5																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18873	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.985Zn0.015O4	La	1.84	Sr	0.16	Cu	0.985	Zn	0.015													O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	6.7																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18874	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.98Zn0.02O4	La	1.84	Sr	0.16	Cu	0.98	Zn	0.02													O	4	4	1	1998																												T							1																																																						A			36.5																	mJ/K2mole	8.25																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18875	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.975Zn0.025O4	La	1.84	Sr	0.16	Cu	0.975	Zn	0.025													O	4	4	1	1998																												T							1																																																						A			36.5																																																									La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18876	PR05805831		(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4	4	1	1998																												T							1																																																						A			34.5																	mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18877	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.995Zn0.005O4	La	1.82	Sr	0.18	Cu	0.995	Zn	0.005													O	4	4	1	1998																												T							1																																																						A			34.5																	mJ/K2mole	3.8																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18878	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.99Zn0.01O4	La	1.82	Sr	0.18	Cu	0.99	Zn	0.01													O	4	4	1	1998																												T							1																																																						A			34.5																	mJ/K2mole	5.6																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18879	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.985Zn0.015O4	La	1.82	Sr	0.18	Cu	0.985	Zn	0.015													O	4	4	1	1998																												T							1																																																						A			34.5																	mJ/K2mole	7.5																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18880	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.98Zn0.02O4	La	1.82	Sr	0.18	Cu	0.98	Zn	0.02													O	4	4	1	1998																												T							1																																																						A			34.5																	mJ/K2mole	8.1																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18881	PR05805831		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4	4	1	1998																												T							1											K			22				22																																																								mJ/K2mole	0																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18882	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.9975Zn0.0025O4	La	1.78	Sr	0.22	Cu	0.9975	Zn	0.0025													O	4	4	1	1998																												T							1											K			20				20																																																								mJ/K2mole	4.5																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18883	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.995Zn0.005O4	La	1.78	Sr	0.22	Cu	0.995	Zn	0.005													O	4	4	1	1998																												T							1											K			19				19																																																								mJ/K2mole	5.6																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18884	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.993Zn0.007O4	La	1.78	Sr	0.22	Cu	0.993	Zn	0.007													O	4	4	1	1998																												T							1											K			18				18																																																								mJ/K2mole	6.3																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18885	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.99Zn0.01O4	La	1.78	Sr	0.22	Cu	0.99	Zn	0.01													O	4	4	1	1998																												T							1											K			15				15																																																								mJ/K2mole	7.7																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18886	PR05805831		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.985Zn0.015O4	La	1.78	Sr	0.22	Cu	0.985	Zn	0.015													O	4	4	1	1998																												T							1											K			10				10																																																								mJ/K2mole	9.1																																							La2O3,SrCo3,CuO and (NiO or ZnO) powdersf high purity at 1050 C - 1150 C in an oxygen atomosphere followed by annealing in an oxygen atomosphereat 600 C for 24 h.					Contrasting Ni- and Zn-subsutitution effects on magnetic properties and superconductivity in La2-xSrxCuO4	9		Department of Physics, Hokkaido University, Sapporo 0600810, Japan	Phys.Rev.B.,58(1998)5831	M. Ido,M. Oda,N. Momono,T. Nagata,T. Nakano		
18887	PR05805960	underdope	Bi2Sr2CaCuO8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212																		K			79			3	79																																																																																																Annealing at 600 C under P(O2)= 4.67e-4 atm for one day at 400C					Pseudogap behavior in single-crystal Bi2Sr2CaCu2O8+delta probed by Cu NMR	9		Department of Physics Science, Graduate school of Engineering Science, Osaka University, Toyonaka, Osaka 560, Japan	Phys.Rev.B,58(1998)R5960	J. Shimoyama,K. Asayama,K. Ishida,K. Kishio,K. Yoshida,T. Mito,Y. Kitaoka,Y. Nakayama,Y. Tokunaga		
18888	PR05805960	overdope	Bi2Sr2CaCuO8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212																		K			77			3	77																																																																																																Annealing at 600 C under P(O2)= 2.1 atm for one day at 400C					Pseudogap behavior in single-crystal Bi2Sr2CaCu2O8+delta probed by Cu NMR	9		Department of Physics Science, Graduate school of Engineering Science, Osaka University, Toyonaka, Osaka 560, Japan	Phys.Rev.B,58(1998)R5960	J. Shimoyama,K. Asayama,K. Ishida,K. Kishio,K. Yoshida,T. Mito,Y. Kitaoka,Y. Nakayama,Y. Tokunaga		
18889	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201	F112/m		A	5.4559	5.49672	23.1901	3											K				38			38																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 500C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18890	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201	F112/m		A	5.45842	5.49889	23.2003	3											K				50			50																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 550C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18891	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201	F112/m		A	5.46289	5.49777	23.2127	3											K				68			68																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 600C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18892	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.46457	5.49509	23.2174	3											K				79			79																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 650C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18893	PR05805226		Tl2Ba2CUO6	Tl2Ba2Cu1O6+Z	Tl	2	Ba	2	Cu	1															O	6+Z		1	1998																											4	Tl2201			A	5.4663	5.49201	23.2231	3											K				90			90																																																																																															1	Ref[12]:A. C. Larson et al., Los Alamos National Laboratory report No. LA-UR-86-748 (1987) 700C Ar Anneal					Phase transitions in the TlBa2CuO6+delta superconductor	9		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madinley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.B.,58(1998)5226	D.R. Pederzolli,G.M. Wltschek,H. Fuess,J.P. Attfield		
18894	PR05806650		Tl2Ba2CaCu2Oz	Tl2Ba2Ca1Cu2OZ	Tl	2	Ba	2	Ca	1	Cu	2													O	Z		5	1998																												Tl2212																		K				100			100																																									microm	micro wave(hair pin resonator)	0.26																																																					Ref[12]M. M. Eddy et al., U. S. Patent 5,476,836 (1995); 5,508,255 (1996)		MgO		6000A Thick	Microwave loss and intermodulation in Tl2Ba2CaCu2Oy thin films	9		Superconductor Technologie, Inc., Santa Barbara, California 93111-2310	Phys.Rev.B,58(1998)6650	B. Gowe,Balam A. Willemsen,D.A. Bonn,D.J. Scalapino,K.E. Kihlstrom,T. Dahm,W.N. Hardy		
18900	PR05808937		YBaCu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O		8	1	1998																												Y124																		K				81			81																																																																																															1					"""atO260barRef[2]:G.V.M.Williamsetal.,Rhys.Rev.B52,7034(1995);54,9532(1996)"""	Muon-spin-rotation study of Zn-induced magnetic moments in cuprate high-Tc superconductors					C.Bernhard,C.Bucci,Ch.Niedermayer,G.V.M.Williams,J.L.Tallon,R.DeRenzi,T.Blasius		
18901	PR05808937		"""YBa2(Cu,Zn)4O8"""	Y1Ba2Cu3.925Zn0.075O8	Y	1	Ba	2	Cu	3.925	Zn	0.075													O		8	1	1998																												Y124																		K				25			25																																																																																															1					"""atO260barRef[2]:G.V.M.Williamsetal.,Rhys.Rev.B52,7034(1995);54,9532(1996)"""	Muon-spin-rotation study of Zn-induced magnetic moments in cuprate high-Tc superconductors					C.Bernhard,C.Bucci,Ch.Niedermayer,G.V.M.Williams,J.L.Tallon,R.DeRenzi,T.Blasius		
18902	PR05808901	overdoped	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1998																												Bi2212																		K				85			85																																																8.2																																																				"""inairRef[20]:D.M.Mitzietal.,Phys.RevB41,6564(1990)"""	ab-plane tunneling spectroscopy of underdoped Bi2Sr2CaCu2Oy					AnjanK.Gupta,K.-W.Ng		
18903	PR05808901	underdoped	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		3	1998																												Bi2212																		K				70			70																																																12.6																																																				"""inairRef[20]:D.M.Mitzietal.,Phys.RevB41,6564(1990)"""	ab-plane tunneling spectroscopy of underdoped Bi2Sr2CaCu2Oy					AnjanK.Gupta,K.-W.Ng		
18904	PR05809504		CuBa2(Ca,Mg)3Cu4O12-z	Ba2Ca2.85Mg0.15Cu5O12-z	Ba	2	Ca	2.85	Mg	0.15	Cu	5													O	12-z		1	1998																												Cu1234	P4/mmm		A	3.855		17.954	3											K				116.6			116.6																				T			127	86												A			19.2	13.2																															mOhmcm															7.61						/CuO2	0.5	"""BaCO3,CaCO3,CuO,MgO"""	1					precursormixedAgO(o.2molfrac.)mixedAgCO3(0.2molfrac.)at3.5GPaat1000CinAucapsule	Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
18905	PR05809504		CuBa2(Ca,Mg)3Cu4O12-z	Ba2Ca2.7Mg0.3Cu5O12-z	Ba	2	Ca	2.7	Mg	0.3	Cu	5													O	12-z		1	1998																												Cu1234	P4/mmm		A	3.848		17.907	3											K				116.4			116.4																				T			103	74												A			20	14.2																															mOhmcm															7.05						/CuO2	0.47	"""BaCO3,CaCO3,CuO,MgO"""	1					precursormixedAgO(o.2molfrac.)mixedAgCO3(0.2molfrac.)at3.5GPaat1000CinAucapsule	Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
18906	PR05809504		CuBa2(Ca,Mg)3Cu4O12-z	Ba2Ca2.4Mg0.6Cu5O12-z	Ba	2	Ca	2.4	Mg	0.6	Cu	5													O	12-z		1	1998																												Cu1234	P4/mmm		A	3.848		17.907	3											K				116.8			116.8																				T			115	80												A			20	14																															mOhmcm															7.86						/CuO2	0.53	"""BaCO3,CaCO3,CuO,MgO"""	1					precursormixedAgO(o.2molfrac.)mixedAgCO3(0.2molfrac.)at3.5GPaat1000CinAucapsule	Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
18907	PR05809504		CuBa2(Ca,Mg)3Cu4O12-z	Ba2Ca2.01Mg0.99Cu5O12-z	Ba	2	Ca	2.01	Mg	0.99	Cu	5													O	12-z		1	1998																												Cu1234	P4/mmm		A	3.847		17.917	3											K				116.6			116.6																				T			110	79												A			20	14.5																															mOhmcm															7.19						/CuO2	0.34	"""BaCO3,CaCO3,CuO,MgO"""	1					precursormixedAgO(o.2molfrac.)mixedAgCO3(0.2molfrac.)at3.5GPaat1000CinAucapsule	Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
18908	PR05809504		CuBa2Ca3Cu4O12-z	Ba2Ca3Cu5O12-z	Ba	2	Ca	3	Cu	5															O	12-z		1	1998																												Cu1234	P4/mmm		A	3.856		17.993	3											K				117.5			117.5																				T			195	121												A			16	10																															mOhmcm															5.4						/CuO2	0.36	"""BaCO3,CaCO3,CuO,MgO"""	1					precursormixedAgO(o.2molfrac.)mixedAgCO3(0.2molfrac.)at3.5GPaat1000CinAucapsule	Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
18909	PR05809536		HgBaCuO4+z	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		3	1998																												Hg1201	P4/mmm		A	3.888		9.538	1											K				95			95																													T/K	"""Calculated in fig.7,from 86K to 95K."""			-0.44																																																																			"""Thealuminacruciblewas1100Candplacedinatempuraturegradientofabout10K/cm,thebottombeingatthehighertempurature.Annialingfor3daysat400Cfollowedby2daysat350C."""	Irreversibility line in superconducting HgBa2CuO4+delta single crystals					A.Terzis,D.Niarchos,E.Moraitakis,G.Kallias,M.Charalambous,M.Pissas		
19100	PR05811153		DyBa2Cu3O7	Dy1Ba2Cu3O7	Dy	1	Ba	2	Cu	3															O	7.00	7	3	1998																												Y123																		K				91			91																																																								J/K2gat	0.0052	1gat=1/13mol=56.90g								mV/K	-2.6																												5	using BaZrO3 crusible. 100bar O2 anneal 330C 230h					Specific heat peaks observed up to 16 T on the melting line of vortex Matter in DyBa2Cu3O7			Departement de Physique de la Matiere Condensee, Universite de Geneve, CH-1211 Geneve 4, Swizerland	Phys.Rev.B,58(1999)11153	Alain Junod,Andreas Erb,Bernard Revaz		
19101	PR05811201	KClO3:YSCO=0.45	YSr2Cu3Oz	Y1Sr2Cu3O7.5	Y	1	Sr	2	Cu	3															O	7.5	7.5	2	1998																											2	Y123			A	3.795		11.38												K				62.5			62.5			K/GPa	3																																																																																										Y2O3,SrO,CuO	1	anneal 980C 60h flow O2 in Alumina crusible. KClO3 and YSr2Cu3O6.5 are pressed 3GPa 1000-1050C 2-8h					High-Temperature superconduting YSr2Cu3O7.5 under pressure			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,58(1999)11201	C.W. Chu,S.H. Xu,T.L. Hudson,Y. Cao,Y.S. Wang,Y.Y. Xue		
19102	PR05812427	Glassy sample	(Bi3Pb)Sr3Ca3Cu4Ox	Bi3Pb1Sr3Ca3Cu4OX	Bi	3	Pb	1	Sr	3	Ca	3	Cu	4											O	X		2	1998									6.76																			4334																		K	80						80																																																											408	Resistivity						microV/K	0.02			TP19102																									1	Ref21, Rapid quenching Tech., anneal 840C 40h air					depression of superconductivity and the phonon-drag effect in glass-ceramic superconductors obtained by annealing the Fe-doped(Bi,Pb)4Sr3Ca3Cu4-mFemOx glassy precursor			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700032, India	Phys.Rev.B,58(1999)12427	B.K. Chaudhuri,P.K. Pal,S. Bhattacharya,S. Chatterjee		
19103	PR05812427	Glassy sample	(Bi3Pb)Sr3Ca3(Cu,Fe)4Ox	Bi3Pb1Sr3Ca3Cu3.98Fe0.02OX	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.98	Fe	0.02									O	X		2	1998									6.59																			4334																		K	58		80				69																																																											416	Resistivity						microV/K	1			TP19103																									1	Ref21, Rapid quenching Tech., anneal 840C 40h air					depression of superconductivity and the phonon-drag effect in glass-ceramic superconductors obtained by annealing the Fe-doped(Bi,Pb)4Sr3Ca3Cu4-mFemOx glassy precursor			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700032, India	Phys.Rev.B,58(1999)12427	B.K. Chaudhuri,P.K. Pal,S. Bhattacharya,S. Chatterjee		
19104	PR05812427	Glassy sample	(Bi3Pb)Sr3Ca3(Cu,Fe)4Ox	Bi3Pb1Sr3Ca3Cu3.96Fe0.04OX	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.96	Fe	0.04									O	X		2	1998									6.08																			4334																		K	28		65				46.5																																																											470	Resistivity						microV/K	-2.65			TP19104																									1	Ref21, Rapid quenching Tech., anneal 840C 40h air					depression of superconductivity and the phonon-drag effect in glass-ceramic superconductors obtained by annealing the Fe-doped(Bi,Pb)4Sr3Ca3Cu4-mFemOx glassy precursor			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700032, India	Phys.Rev.B,58(1999)12427	B.K. Chaudhuri,P.K. Pal,S. Bhattacharya,S. Chatterjee		
19105	PR05812427	Glassy sample	(Bi3Pb)Sr3Ca3(Cu,Fe)4Ox	Bi3Pb1Sr3Ca3Cu3.95Fe0.05OX	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.95	Fe	0.05									O	X		2	1998									5.94																			4334																		K	20		55				37.5																																																											476	Resistivity						microV/K	-0.12			TP19105																									1	Ref21, Rapid quenching Tech., anneal 840C 40h air					depression of superconductivity and the phonon-drag effect in glass-ceramic superconductors obtained by annealing the Fe-doped(Bi,Pb)4Sr3Ca3Cu4-mFemOx glassy precursor			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700032, India	Phys.Rev.B,58(1999)12427	B.K. Chaudhuri,P.K. Pal,S. Bhattacharya,S. Chatterjee		
19106	PR05812427	Glassy sample	(Bi3Pb)Sr3Ca3(Cu,Fe)4Ox	Bi3Pb1Sr3Ca3Cu3.94Fe0.06OX	Bi	3	Pb	1	Sr	3	Ca	3	Cu	3.94	Fe	0.06									O	X		2	1998									5.8																			4334																		K																																																																		523	Resistivity																																			1	Ref21, Rapid quenching Tech., anneal 840C 40h air					depression of superconductivity and the phonon-drag effect in glass-ceramic superconductors obtained by annealing the Fe-doped(Bi,Pb)4Sr3Ca3Cu4-mFemOx glassy precursor			Department of Solid State Physics, Indian Association for the Cultivation of Science, Calcutta-700032, India	Phys.Rev.B,58(1999)12427	B.K. Chaudhuri,P.K. Pal,S. Bhattacharya,S. Chatterjee		
19201	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu1O4+Z	La	1.85	Sr	0.15	Cu	1															O	4+Z		6	1998																												T			A	3.771		13.21																																																																																																																	La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19202	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4+Z	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4+Z		6	1998																												T																					29				29		1																																																																					mohmcm				1.3			1.1				3												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19203	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4+Z	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4+Z		6	1998																												T																					31				31		1																																																																					mohmcm				2			1.5				4												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19204	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4+Z	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4+Z		6	1998																												T																					28				28		1																																																																					mohmcm				3.1			2.9				6.4												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19205	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.96Ni0.04O4+Z	La	1.85	Sr	0.15	Cu	0.96	Ni	0.04													O	4+Z		6	1998																												T																																																																																																mohmcm				4.2							7.3												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19206	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.95Ni0.05O4+Z	La	1.85	Sr	0.15	Cu	0.95	Ni	0.05													O	4+Z		6	1998																												T			A	3.773		13.19																																																																																																																	La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19207	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.9Ni0.1O4+Z	La	1.85	Sr	0.15	Cu	0.9	Ni	0.1													O	4+Z		6	1998																												T			A	3.777		13.16																																																																																										mohmcm				50							20												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19208	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.8Ni0.2O4+Z	La	1.85	Sr	0.15	Cu	0.8	Ni	0.2													O	4+Z		6	1998																												T			A	3.785		13.12																																																																																										mohmcm				6000							80												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19209	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.7Ni0.3O4+Z	La	1.85	Sr	0.15	Cu	0.7	Ni	0.3													O	4+Z		6	1998																												T			A	3.79		13.05																																																																																										mohmcm				20000							100												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19210	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.5Ni0.5O4+Z	La	1.85	Sr	0.15	Cu	0.5	Ni	0.5													O	4+Z		6	1998																												T			A	3.798		12.97																																																																																										mohmcm				900000							200												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19211	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.2Ni0.8O4+Z	La	1.85	Sr	0.15	Cu	0.2	Ni	0.8													O	4+Z		6	1998																												T			A	3.831		12.78																																																																																										mohmcm				1000000							500												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19212	PR05815116		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Ni1O4+Z	La	1.85	Sr	0.15	Ni	1															O	4+Z		6	1998																												T			A	3.849		12.74																																																																																										mohmcm				20000000							4000												La2O3,SrCO3,CuO,Ni2O3		standard ceramic tchniques. La2O3 was dried  at 900 C mixture powder was ground and preheated in air at 1020-1250 C for 20h with an intermediate grinding.And it was reground and pressed..				anneal:1050-1320 C for 24h then cooleddown to and kept 800 C in the furnance for a day.	Transport mechanism in La1.85Sr0.15Cu1-xNixO4+z (0=< x =< 1)	12		Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys.Rev.B,58(1998)15116	Mao Zhiqiang,Qiu Xueyin,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19213	PR05814219	anneal 500 C  O2 1000 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			30.58	1														78				78																																																																							mohmmm								2.1	2			3.2	3											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19214	PR05814219	anneal 500 C  O2 10 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			30.61	1														80				80																																																																							mohmmm								2.6	10			4	4											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19215	PR05814219	anneal 500 C  O2 1 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			30.72	1														85				85																																																																							mohmmm								3.2	23			5	5											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19216	PR05814219	anneal 500 C  O2 0.001 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			30.92	1														89				89																																																																							mohmmm								3.8	40			7.8	8											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19217	PR05814219	annial 500 C  O2 0.001 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			30.98	1														81				81																																																																							mohmmm								4.1	49			11.7	10											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19218	PR05814219	anneal 500 C  O2 0.001 atm	Bi2Sr2CaCu2O8+Z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1998																												Bi2212			A			31.09	1														76				76																																																																							mohmmm								4.5	72			12.2	10											5						Anisotropic resistivities of single-crystal Bi2Sr2CaCu2O8+delta with different oxygen content	12		Structural Research Laboratory and Department of Physics, University of Science and Technology China, Hofei 230026, People's Republic of China	Phys.Rev.B,58(1998)14219	G.C. Zhang,L.Z. Cao,M.Yu.K.Q. Ruan,S.Y. Li,X.H. Chen,Z. Gui		
19219	PR05814581	LaAlO3 substrate. anisotropy factor = 6.4 	YBa2Cu3O7z	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1998																												Y123							3														87				87		1																																		A	micro wave		14.4		A	micro wave		1300																																																				ref[27-29]					Anisotropic renormalized fluctuations in the microwave resistivity in YBa2Cu3O7-delta	12		Dipartiment di Fisica 'E. Amaldi', Unita INFM, and Diparitimento di Ingegneria Elettronica, Universita 'Roma Tre' Via della Vasca Navale 84, 00146 Pome, Italy	Phys.Rev.B,58(1998)14581	D. Neri,E. Silva,M. Giura,N. Sparvieri,R. Fastampa,R. Marcon,S. Sarti		
19220	PR05814581	LaAlO3 substrate. anisotropy factor = 5	YBa2Cu3O7z	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1998																												Y123							3														87				87		1																																		A	micro wave		17.5		A	micro wave		1300																																																				ref[27-29]					Anisotropic renormalized fluctuations in the microwave resistivity in YBa2Cu3O7-delta	12		Dipartiment di Fisica 'E. Amaldi', Unita INFM, and Diparitimento di Ingegneria Elettronica, Universita 'Roma Tre' Via della Vasca Navale 84, 00146 Pome, Italy	Phys.Rev.B,58(1998)14581	D. Neri,E. Silva,M. Giura,N. Sparvieri,R. Fastampa,R. Marcon,S. Sarti		
19221	PR05814581	LaAlO3 substrate?Banisotropy factor = 5.4 	YBa2Cu3O7z	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1998																												Y123							3														87				87		1																																		A	micro wave		16.5		A	micro wave		1500																																																				ref[27-29]					Anisotropic renormalized fluctuations in the microwave resistivity in YBa2Cu3O7-delta	12		Dipartiment di Fisica 'E. Amaldi', Unita INFM, and Diparitimento di Ingegneria Elettronica, Universita 'Roma Tre' Via della Vasca Navale 84, 00146 Pome, Italy	Phys.Rev.B,58(1998)14581	D. Neri,E. Silva,M. Giura,N. Sparvieri,R. Fastampa,R. Marcon,S. Sarti		
19222	PR05814581	LaAlO3 substrate?Banisotropy factor = 6.6 	YBa2Cu3O7z	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1998																												Y123																					84				84		1																																		A	micro wave		14.3		A	micro wave		1500																																																				ref[27-29]					Anisotropic renormalized fluctuations in the microwave resistivity in YBa2Cu3O7-delta	12		Dipartiment di Fisica 'E. Amaldi', Unita INFM, and Diparitimento di Ingegneria Elettronica, Universita 'Roma Tre' Via della Vasca Navale 84, 00146 Pome, Italy	Phys.Rev.B,58(1998)14581	D. Neri,E. Silva,M. Giura,N. Sparvieri,R. Fastampa,R. Marcon,S. Sarti		
19223	PR05814581	SrTiO3 substrate?Banisotropy factor = 6.3 	YBa2Cu3O7z	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1998																												Y123																					90				90		1																																		A	micro wave		15		A	micro wave		1100																																																				ref[27-29]					Anisotropic renormalized fluctuations in the microwave resistivity in YBa2Cu3O7-delta	12		Dipartiment di Fisica 'E. Amaldi', Unita INFM, and Diparitimento di Ingegneria Elettronica, Universita 'Roma Tre' Via della Vasca Navale 84, 00146 Pome, Italy	Phys.Rev.B,58(1998)14581	D. Neri,E. Silva,M. Giura,N. Sparvieri,R. Fastampa,R. Marcon,S. Sarti		
19224	PR05814753		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		6	1998																												T																					33			3	33		1																																																						mJ/molK2	5																																							ref[9][10]					Magnetic-field dependence of the low-temperature specific heat of La2-xSrxCuO4	12		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,58(1998)R14753	C.F. Chang,H.D. Yang,H.L. Tsay,J.-Y. Lin,S.J. Chen		
19225	PR05814753		(La,Sr)2CuO4	La1.84Sr0.16Cu1O4	La	1.84	Sr	0.16	Cu	1															O	4		6	1998																												T																					39			3	39		1																																																						mJ/molK2	10																																							ref[9][10]					Magnetic-field dependence of the low-temperature specific heat of La2-xSrxCuO4	12		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,58(1998)R14753	C.F. Chang,H.D. Yang,H.L. Tsay,J.-Y. Lin,S.J. Chen		
19226	PR05814753		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		6	1998																												T																					29			3	29		1																																																						mJ/molK2	12																																							ref[9][10]					Magnetic-field dependence of the low-temperature specific heat of La2-xSrxCuO4	12		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,58(1998)R14753	C.F. Chang,H.D. Yang,H.L. Tsay,J.-Y. Lin,S.J. Chen		
19227	PR05815231	asgrown	Bi2Sr2CaCu2O8+z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		6	1998																												Bi2212																					82			4	82		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2220																											ohmcm													6												ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19228	PR05815231	annealed	Bi2Sr2CaCu2O8+z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		6	1998																												Bi2212																					73				73		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2590																											ohmcm													0.9												ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19229	PR05815231	asgrown	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.79Y0.21Cu2O8+Z	Bi	2	Sr	2	Ca	0.79	Y	0.21	Cu	2											O	8+Z		6	1998																												Bi2212																					90			4	90		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		1900																											ohmcm													4												ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19230	PR05815231	annealed	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.79Y0.21Cu2O8+Z	Bi	2	Sr	2	Ca	0.79	Y	0.21	Cu	2											O	8+Z		6	1998																												Bi2212																					77				77		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2300																																																				ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19231	PR05815231	asgrown	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.72Y0.28Cu2O8+Z	Bi	2	Sr	2	Ca	0.72	Y	0.28	Cu	2											O	8+Z		6	1998																												Bi2212																					91			4	91		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2590																											ohmcm													3.2												ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19232	PR05815231	annealed	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.72Y0.28Cu2O8+Z	Bi	2	Sr	2	Ca	0.72	Y	0.28	Cu	2											O	8+Z		6	1998																												Bi2212																					81				81		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2280																																																				ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19233	PR05815231	asgrown	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.64Y0.36Cu2O8+Z	Bi	2	Sr	2	Ca	0.64	Y	0.36	Cu	2											O	8+Z		6	1998																												Bi2212																					88			4	88		1																																							A	frame work of London mode (ref[23])from mesured lisothermal magnetization vs Mt(H). Fit ref[24]		2980																											ohmcm													0.4												ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19234	PR05815231	annealed	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.64Y0.36Cu2O8+Z	Bi	2	Sr	2	Ca	0.64	Y	0.36	Cu	2											O	8+Z		6	1998																												Bi2212																					88				88		1																																																																																														ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19235	PR05815231	asgrown	Bi2Sr2(Ca,Y)Cu2O8+z	Bi2Sr2Ca0.57Y0.43Cu2O8+Z	Bi	2	Sr	2	Ca	0.57	Y	0.43	Cu	2											O	8+Z		6	1998																												Bi2212																					86			15	86		1																																																																																														ref[18]				anneal 100bar 540 C 12h	Doping dependence of the in-plane penetration depth and fishtail in Bi2Sr2Ca1-xYxCu2O8+delta single crystals	12		Laboratoire CRISMAT, CNRS UMR 6508, ISMRA et Universite de Unite Mixte de Recherche(UMR 6508) associee au CNRS, 6 Bd du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,58(1998)15231	A. Maignan,D. Pelloquin,G. Villard		
19236	PR05814617	Al-contamination(1-2%). grown in Al2O3 crusible	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1998																												Y124																					72				72																																																																	THC19236																															high pressure flux method ref[11]					Anisotropic in-plane thermal conductivity of single-crystal YBa2Cu4O8	12		Physics Department,  University, of Miami Coral Gables, Florida 33124	Phys.Rev.B,58(1998)14617	J. Karpinski,J.L. Cohn		
19237	PR05814617	Al-contamination(1-2%). grown in Al2O3 crusible	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1998																												Y124																					72				72																																																																	THC19237																															high pressure flux method ref[11]					Anisotropic in-plane thermal conductivity of single-crystal YBa2Cu4O8	12		Physics Department,  University, of Miami Coral Gables, Florida 33124	Phys.Rev.B,58(1998)14617	J. Karpinski,J.L. Cohn		
19238	PR05814617	grown in Y2O3 crusible	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1998																												Y124																					80				80																																																																	THC19238																															high pressure flux method ref[11]					Anisotropic in-plane thermal conductivity of single-crystal YBa2Cu4O8	12		Physics Department,  University, of Miami Coral Gables, Florida 33124	Phys.Rev.B,58(1998)14617	J. Karpinski,J.L. Cohn		
19239	PR05815238		(La,Lu)Ba2Cu3Oz	La0.5Lu0.5Ba2Cu3OZ	La	0.5	Lu	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.848	3.9047	11.729	3														87				87																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19240	PR05815238		(La,Yb)Ba2Cu3Oz	La0.5Yb0.5Ba2Cu3OZ	La	0.5	Yb	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8405	3.9012	11.712	3														81				81																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19241	PR05815238		(La,Tm)Ba2Cu3Oz	La0.5Tm0.5Ba2Cu3OZ	La	0.5	Tm	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.844	3.9039	11.726	3														84				84																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19242	PR05815238		(La,Er)Ba2Cu3Oz	La0.5Er0.5Ba2Cu3OZ	La	0.5	Er	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8477	3.9066	11.732	3														87				87																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19243	PR05815238		(La,Ho)Ba2Cu3Oz	La0.5Ho0.5Ba2Cu3OZ	La	0.5	Ho	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8522	3.9099	11.746	3														87				87																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19244	PR05815238		(La,Y)Ba2Cu3Oz	La0.5Y0.5Ba2Cu3OZ	La	0.5	Y	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8393	3.9057	11.719	3														84				84																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19245	PR05815238		(La,Dy)Ba2Cu3Oz	La0.5Dy0.5Ba2Cu3OZ	La	0.5	Dy	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.9618	3.9183	11.752	3														90				90																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19246	PR05815238		(La,Gd)Ba2Cu3Oz	La0.5Gd0.5Ba2Cu3OZ	La	0.5	Gd	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8545	3.9129	11.756	3														88				88																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19247	PR05815238		(La,Eu)Ba2Cu3Oz	La0.5Eu0.5Ba2Cu3OZ	La	0.5	Eu	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8664	3.9175	11.779	3														88				88																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19248	PR05815238		(La,Sm)Ba2Cu3Oz	La0.5Sm0.5Ba2Cu3OZ	La	0.5	Sm	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8685	3.9203	11.784	3														90				90																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19249	PR05815238		(La,Nd)Ba2Cu3Oz	La0.5Nd0.5Ba2Cu3OZ	La	0.5	Nd	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8759	3.9263	11.767	3														90				90																																																																																																Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19250	PR05815238		(La,Pr)Ba2Cu3Oz	La0.5Pr0.5Ba2Cu3OZ	La	0.5	Pr	0.5	Ba	2	Cu	3													O	Z		6	1998																												Y123			A	3.8763	3.9207	11.741	3														94			0.3	94		1																																		A				12.9																																																								Polycrystallic ceramic.Solid-state reaction tequnique. Mixed powder calcinenated at 920 C and regrond,repressed and further thermally treated (four times)at 940, 960,980,990 C in oxgen atomosphere.				anneal 950 C 44 h He atomosphere.The sumple furnance cooed to 500 C and annealed 24h.The process has been repeated until the amount of BaCuO2 was asymptotically reduced to constant varue.	Phaseseparation and onternal strains in the mixed La0.5R0.5Ba2Cu3Oy compounds (R=rare-earth element)	12		Solid State Physics Section, Department of Physics, University of Athens, GR-157 84 Athens, Greece	Phys.Rev.B,58(1998)15238	A. Gantis,A. Koufoudakis,D. Lampakis,D. Palles,E. Liarokapis,M. Calamiotou		
19251	PR05814548	O2 flow 500 C for 7 days	YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	3	1998																												Y123																					93			0.3	93		1																											T/K				2.1			A				13.2																															uohmcm								73																5						Phase diagram of optimally doped YBa2Cu3O7-delta: Effect of oxygen stoichiometry	12		Physics Department, Southampton University, Southampton, SO17 1BJ United Kingdom	Phys.Rev.B,58(1998)14548	A.G.M. Jansen,L. Taillefer,P.A.J. de Groot,R. Gagnon,R.M. Langan,S.N. Gordeev		
19252	PR05814548	O2 flow 525 C for 7 days	YBa2Cu3Oz	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	7-Z	6.91	3	1998																												Y123																					93			0.3	93		1																											T/K				2.04			A				12.5																															uohmcm								56																5						Phase diagram of optimally doped YBa2Cu3O7-delta: Effect of oxygen stoichiometry	12		Physics Department, Southampton University, Southampton, SO17 1BJ United Kingdom	Phys.Rev.B,58(1998)14548	A.G.M. Jansen,L. Taillefer,P.A.J. de Groot,R. Gagnon,R.M. Langan,S.N. Gordeev		
19253	PR05814548	O2 flow 475 C for 7 days	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95	3	1998																												Y123																																																						T/K				2.27																																						uohmcm								63																5						Phase diagram of optimally doped YBa2Cu3O7-delta: Effect of oxygen stoichiometry	12		Physics Department, Southampton University, Southampton, SO17 1BJ United Kingdom	Phys.Rev.B,58(1998)14548	A.G.M. Jansen,L. Taillefer,P.A.J. de Groot,R. Gagnon,R.M. Langan,S.N. Gordeev		
19254	PR05815208	A	YBa2Cu3Oz	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	7-Z	6.94	6	1998																												Y123																				90.5		92.5			90.5										100																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19255	PR05815208	G	YBa2Cu3Oz	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	7-Z	6.87	6	1998																												Y123																				93.5		93.5			93.5										100																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				SrO2 pellet: sealed in in a Pyrex ampoule together with zirconium foil .The ampoule were evacurated down to to 10-5 torr,heated to 440 C for 50-100h and cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19256	PR05815208	R	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	6	1998																												Y123																				92.6		92.4			92.6										100																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:Pressing powder sintered in air 950C overnight and cooled at rate of 100 C/h down to room temperature	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19257	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3O6.96	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-Z	6.96	6	1998																												Y123			A	3.799	3.87	11.621														89		87.2			89										98																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19258	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba1Sr1Cu3O6.98	Y	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.98	6	1998																												Y123			A	3.784	3.853	11.562														82		83			82										100																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19259	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba1Sr1Cu3O6.96	Y	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.96	6	1998																												Y123			A	3.785	3.853	11.562														83.5		83.5			83.5										100																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19260	PR05815208	R	Y(Ba,Sr)2Cu3Oz	Y1Ba1Sr1Cu3O6.8	Y	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.8	6	1998																												Y123			A	3.801	3.85	11.574														51.5		45.5			51.5										62																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:Pressing powder sintered in air 950C overnight and cooled at rate of 100 C/h down to room temperature	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19261	PR05815208	G	Y(Ba,Sr)2Cu3Oz	Y1Ba1Sr1Cu3O6.685	Y	1	Ba	1	Sr	1	Cu	3													O	7-Z	6.685	6	1998																												Y123			A	3.817	3.841	11.584														34		34.2			34										51																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				SrO2 pellet: sealed in in a Pyrex ampoule together with zirconium foil .The ampoule were evacurated down to to 10-5 torr,heated to 440 C for 50-100h and cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19262	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba0.75Sr1.25Cu3O6.91	Y	1	Ba	0.75	Sr	1.25	Cu	3													O	7-Z	6.91	6	1998																												Y123																				80		81			80										84																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19263	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba0.75Sr1.25Cu3O6.94	Y	1	Ba	0.75	Sr	1.25	Cu	3													O	7-Z	6.94	6	1998																												Y123			A	3.783	3.845	11.539														74		81.2			74										81.5																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19264	PR05815208	A	Y(Ba,Sr)2Cu3Oz	Y1Ba0.5Sr1.5Cu3OZ	Y	1	Ba	0.5	Sr	1.5	Cu	3													O	Z		6	1998																												Y123																				80		81			80										21																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19265	PR05815208	R	Y(Ba,Sr)2Cu3Oz	Y1Ba0.5Sr1.5Cu3OZ	Y	1	Ba	0.5	Sr	1.5	Cu	3													O	Z		6	1998																												Y123																				75		81			75										18																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:Pressing powder sintered in air 950C overnight and cooled at rate of 100 C/h down to room temperature	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19266	PR05815208	S	Y(Ba,Sr)2Cu3Oz	Y1Ba0.5Sr1.5Cu3OZ	Y	1	Ba	0.5	Sr	1.5	Cu	3													O	Z		6	1998																												Y123																				78		81			78										16																																																																																				Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				SrO2 pellet: sealed 10-5 torr and heat up to 600 C for 2h and cooled down to 500 C maintained at temperature for 10h and cooled down to room temperature 	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19267	PR05815208	ANN(480C, in flowing O2). not s/c. multi-phase sample. 	YSr2Cu3Oz	Y1Sr2Cu3OZ	Y	1	Sr	2	Cu	3															O	Z		6	1998																												Y123																																																																																																																							Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:in flowing oxygen at 880C for 2h,cooled at 30 C/h down to 480 C and maintained at this temperature for 50-100h before being cooled down to room temperature.	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19268	PR05815208	As-grown sample. multi-phase. not s/c. 	YSr2Cu3Oz	Y1Sr2Cu3OZ	Y	1	Sr	2	Cu	3															O	Z		6	1998																												Y123																																																																																																																							Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				anneal:Pressing powder sintered in air 950C overnight and cooled at rate of 100 C/h down to room temperature	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19269	PR05815208	ANN(480C, in flowing O2) + ANN(500C, in 20-30 atm O2). multi-phase sample. not s/c.  	YSr2Cu3Oz	Y1Sr2Cu3OZ	Y	1	Sr	2	Cu	3															O	Z		6	1998																												Y123																																																																																																																							Y2O3,CuO,BaCO3,SrCO3(SrO2 x=0.75,1)		solid-state reaction .sintered in air at 950 C for 80-100h with several inter mediate cooling and grindings.				SrO2 pellet: sealed 10-5 torr and heat up to 600 C for 2h and cooled down to 500 C maintained at temperature for 10h and cooled down to room temperature 	Structural and electronic effects of Sr substitution for Ba in Y(Ba1-xSrx)2Cu3Ow at verying w	12		Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche , Via Chiavari 18/A, 43100 Parma, Italy	Phys.Rev.B,58(1998)15208	A. Gauzzi,C. Chaillout-Bougerol,F. Licci,G.P. Radaelli,M. Marezio,R. Masini		
19300	PR05900641	film thickness=3600A 	(La,Sr)2CuO4	La1.865Sr0.135Cu1O4	La	1.865	Sr	0.135	Cu	1															O	4		5	1999																												T																		K			31				31																																									A	mutual inductance 	5900																												mOhmcm												1.6												5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19301	PR05900641	film thickness=2700 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			30.5				30.5																																									A	mutual inductance 	4500																												mOhmcm												1.1												5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19302	PR05900641	film thickness=5000 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			27.5				27.5																																									A	mutual inductance 	6000																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19303	PR05900641	film thickness=1200 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			27				27																																									A	mutual inductance 	6600																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19304	PR05900641	film thickness=1120 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			27				27																																									A	mutual inductance 	7400																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19305	PR05900641	film thickness=1200 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			23				23																																									A	mutual inductance 	7600																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19306	PR05900641	film thickness=900 A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			25				25																																									A	mutual inductance 	8400																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19307	PR05900641	film thickness=3400 A. 	(La,Sr)2CuO4	La1.825Sr0.175Cu1O4	La	1.825	Sr	0.175	Cu	1															O	4		5	1999																												T																		K			24				24																																									A	mutual inductance 	6000																												mOhmcm												0.8												5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19308	PR05900641	film thickness=5000 A. 	(La,Sr)2CuO4	La1.825Sr0.175Cu1O4	La	1.825	Sr	0.175	Cu	1															O	4		5	1999																												T																		K			27.5				27.5																																									A	mutual inductance 	7000																												mOhmcm																								5	Crucible:YSZ(yttria-stabilized zirconia)O2 anneal 100bar 20h 700C					Magnetic penetration depth in superconducting La2-xSrxCuO4 films	199901		Department of Physics, Ohio State University, Columbus, Ohio 43210-1106	Phys.Rev.B,59(1999)641	Igor E. Trofimov,Kathleen M. Paget,Marta Z. Cieplak,Sabyasachi Guha,Stefan J. Turneaure,Tohmas R. Lemberger		
19309	PR05901377	non-SC	BaY(Cu,Fe)O5+z	Ba1Y1Cu0.5Fe0.5O5+D	Ba	1	Y	1	Cu	0.5	Fe	0.5													O	5+D		1	1999																												0112			A	3.8796		7.66537	3																																																																																																																BaCO3,La2O3,Y2O3,CuO,Fe2O3	1					calcined 900C 12h grind sinter 1000C 24h 5GPa 1200C 30min	Layered (Cu,Fe) oxides of double perovskite structure. II. Extension of solid solubility of copper in (Ba,La)Y(Cu0.5+xFe0.5-x)2O5+delta vin high-pressure heat treatment	199901		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,59(1999)1377	H. Suematsu,H. Yamauchi,J. Linden,M. Karppinen,M. Nagase		
19310	PR05901377	non-SC	(Ba,La)Y(Cu,Fe)O5+z	Ba0.8La0.2Y1Cu0.6Fe0.4O5+D	Ba	0.8	La	0.2	Y	1	Cu	0.6	Fe	0.4											O	5+D		1	1999																												0112			A	3.8673		7.6497	3																																																																																																																BaCO3,La2O3,Y2O3,CuO,Fe2O3	1					calcined 900C 12h grind sinter 1000C 24h 5GPa 1200C 30min	Layered (Cu,Fe) oxides of double perovskite structure. II. Extension of solid solubility of copper in (Ba,La)Y(Cu0.5+xFe0.5-x)2O5+delta vin high-pressure heat treatment	199901		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,59(1999)1377	H. Suematsu,H. Yamauchi,J. Linden,M. Karppinen,M. Nagase		
19311	PR05901377	non-SC	(Ba,La)Y(Cu,Fe)O5+z	Ba0.6La0.4Y1Cu0.7Fe0.3O5+D	Ba	0.6	La	0.4	Y	1	Cu	0.7	Fe	0.3											O	5+D		1	1999																												0112			A	3.8981		7.624	3																																																																																																																BaCO3,La2O3,Y2O3,CuO,Fe2O3	1					calcined 900C 12h grind sinter 1000C 24h 5GPa 1200C 30min	Layered (Cu,Fe) oxides of double perovskite structure. II. Extension of solid solubility of copper in (Ba,La)Y(Cu0.5+xFe0.5-x)2O5+delta vin high-pressure heat treatment	199901		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,59(1999)1377	H. Suematsu,H. Yamauchi,J. Linden,M. Karppinen,M. Nagase		
19312	PR05900192	semi-conductive	La2CuO4	La2Cu1O4+Z	La	2	Cu	1																	O	4+Z		1	1999																												T																		K																																																																									microV/K	210			TP19312	mOhmcm				320							75													1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19313	PR05900192	semi-conductive	Nd2CuO4	Nd2Cu1O4-Y	Nd	2	Cu	1																	O	4-Y		1	1999																												T'																		K																																																																									microV/K	-360			TP19313	mOhmcm				1200							150													1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19314	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z		1	1999																												Bi2201																		K		8					8																																																																		microV/K	-16			TP19314																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19315	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.8La0.2Cu1O6+Z	Bi	2	Sr	1.8	La	0.2	Cu	1													O	6+Z		1	1999																												Bi2201																		K		12					12																																																																		microV/K	-14			TP19315																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19316	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.7La0.3Cu1O6+Z	Bi	2	Sr	1.7	La	0.3	Cu	1													O	6+Z		1	1999																												Bi2201																		K		19					19																																																																		microV/K	-13			TP19316																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19317	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+Z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+Z		1	1999																												Bi2201																		K		20					20																																																																		microV/K	-12			TP19317																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19318	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6+Z	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+Z		1	1999																												Bi2201																		K		21					21																																																																		microV/K	-6			TP19318																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19319	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.4La0.6Cu1O6+Z	Bi	2	Sr	1.4	La	0.6	Cu	1													O	6+Z		1	1999																												Bi2201																		K		11					11																																																																		microV/K																													1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19320	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.3La0.7Cu1O6+Z	Bi	2	Sr	1.3	La	0.7	Cu	1													O	6+Z		1	1999																												Bi2201																		K		10					10																																																																		microV/K	6			TP19320																									1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19321	PR05900192		Bi2(Sr,La)2CuO6	Bi2Sr1.2La0.8Cu1O6+Z	Bi	2	Sr	1.2	La	0.8	Cu	1													O	6+Z		1	1999																												Bi2201																																																																																											microV/K																													1					solid state reaction	Thermopower of high-Tc cuprates	199901			Phys.Rev.B, 59(1999)192	J.S.Kim,Mu-Yong Choi		
19322	PR05900203		TlBa2CaCu2O7-D	Tl1Ba2Ca1Cu2O7-D	Tl	1	Ba	2	Ca	1	Cu	2													O	7-D		5	1999																												Tl1212			A			12.66	1											K	93						93																																																		10000000	20000																																																	High quality c-oriented thin file Ref[13]:D. Lepez et al., Phys. Rev. Lett. 79,4258(1997) Ref[14]:D. Lepez et al., Phys. Rev Lett. 76,4034(1996)	Giant Tc shift in HgBa2CaCu2O6+delta and TlBa2CaCu2O7-delta superconductors due to Hg-Tl exchange	199901		Department of Physics and Astronomy, University of Kansas, Lawrence, Kansas 66045-2151	Phys.Rev.B,59(1999)203	A.A. Gapud,B.W. Kang,J.Z. Wu,M.P. Siegal,S.L. Yan,Y.Y. Xie		
19323	PR05900203		TlBa2CaCu2O7-D	Tl1Ba2Ca1Cu2O7-D	Tl	1	Ba	2	Ca	1	Cu	2													O	7-D		5	1999																												Tl1212			A			12.66	1											K	92						92																																																		10000000	20000																																																	High quality c-oriented thin file Ref[13]:D. Lepez et al., Phys. Rev. Lett. 79,4258(1997) Ref[14]:D. Lepez et al., Phys. Rev Lett. 76,4034(1996)	Giant Tc shift in HgBa2CaCu2O6+delta and TlBa2CaCu2O7-delta superconductors due to Hg-Tl exchange	199901		Department of Physics and Astronomy, University of Kansas, Lawrence, Kansas 66045-2151	Phys.Rev.B,59(1999)203	A.A. Gapud,B.W. Kang,J.Z. Wu,M.P. Siegal,S.L. Yan,Y.Y. Xie		
19324	PR05900203		HgBa2CaCu2O6+D	Hg1Ba2Ca1Cu2O6+D	Hg	1	Ba	2	Ca	1	Cu	2													O	6+D		5	1999																												Hg1212			A			12.67	1											K	122						122																																																		24000000	2500000																																																	High quality c-oriented thin file Ref[13]:D. Lepez et al., Phys. Rev. Lett. 79,4258(1997) Ref[14]:D. Lepez et al., Phys. Rev Lett. 76,4034(1996)	Giant Tc shift in HgBa2CaCu2O6+delta and TlBa2CaCu2O7-delta superconductors due to Hg-Tl exchange	199901		Department of Physics and Astronomy, University of Kansas, Lawrence, Kansas 66045-2151	Phys.Rev.B,59(1999)203	A.A. Gapud,B.W. Kang,J.Z. Wu,M.P. Siegal,S.L. Yan,Y.Y. Xie		
19325	PR05900203		HgBa2CaCu2O6+D	Hg1Ba2Ca1Cu2O6+D	Hg	1	Ba	2	Ca	1	Cu	2													O	6+D		5	1999																												Hg1212			A			12.67	1											K	120						120																																																		24000000	2500000																																																	High quality c-oriented thin file Ref[13]:D. Lepez et al., Phys. Rev. Lett. 79,4258(1997) Ref[14]:D. Lepez et al., Phys. Rev Lett. 76,4034(1996)	Giant Tc shift in HgBa2CaCu2O6+delta and TlBa2CaCu2O7-delta superconductors due to Hg-Tl exchange	199901		Department of Physics and Astronomy, University of Kansas, Lawrence, Kansas 66045-2151	Phys.Rev.B,59(1999)203	A.A. Gapud,B.W. Kang,J.Z. Wu,M.P. Siegal,S.L. Yan,Y.Y. Xie		
19326	PR05900203		HgBa2CaCu2O6+D	Hg1Ba2Ca1Cu2O6+D	Hg	1	Ba	2	Ca	1	Cu	2													O	6+D		5	1999																												Hg1212			A			12.67	1											K	123						123																																																		24000000	2500000																																																	High quality c-oriented thin file Ref[13]:D. Lepez et al., Phys. Rev. Lett. 79,4258(1997) Ref[14]:D. Lepez et al., Phys. Rev Lett. 76,4034(1996)	Giant Tc shift in HgBa2CaCu2O6+delta and TlBa2CaCu2O7-delta superconductors due to Hg-Tl exchange	199901		Department of Physics and Astronomy, University of Kansas, Lawrence, Kansas 66045-2151	Phys.Rev.B,59(1999)203	A.A. Gapud,B.W. Kang,J.Z. Wu,M.P. Siegal,S.L. Yan,Y.Y. Xie		
19327	PR05900725		(La,Sr)2CuO4	La1.983Sr0.017Cu1O4	La	1.983	Sr	0.017	Cu	1															O	4		1	1999								124																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19328	PR05900725		(La,Sr)2(Cu,Zn)O4	La1.983Sr0.017Cu0.95Zn0.05O4	La	1.983	Sr	0.017	Cu	0.95	Zn	0.05													O	4		1	1999								142																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19329	PR05900725		(La,Sr)2(Cu,Zn)O4	La1.983Sr0.017Cu0.9Zn0.1O4	La	1.983	Sr	0.017	Cu	0.9	Zn	0.1													O	4		1	1999								126																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19330	PR05900725		(La,Sr)2(Cu,Zn)O4	La1.983Sr0.017Cu0.85Zn0.15O4	La	1.983	Sr	0.017	Cu	0.85	Zn	0.15													O	4		1	1999								110																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19331	PR05900725		(La,Sr)2(Cu,Zn)O4	La1.983Sr0.017Cu0.8Zn0.2O4	La	1.983	Sr	0.017	Cu	0.8	Zn	0.2													O	4		1	1999								72																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19332	PR05900725		(La,Sr)2(Cu,Zn)O4	La1.983Sr0.017Cu0.75Zn0.25O4	La	1.983	Sr	0.017	Cu	0.75	Zn	0.25													O	4		1	1999								31																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19333	PR05900725		La2CuO4	La2Sr0Cu1Zn0O4	La	2	Sr	0	Cu	1	Zn	0													O	4		1	1999								280																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19334	PR05900725		La2(Cu,Zn)O4	La2Sr0Cu0.95Zn0.05O4	La	2	Sr	0	Cu	0.95	Zn	0.05													O	4		1	1999								231																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19335	PR05900725		La2(Cu,Zn)O4	La2Sr0Cu0.9Zn0.1O4	La	2	Sr	0	Cu	0.9	Zn	0.1													O	4		1	1999								180																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19336	PR05900725		La2(Cu,Zn)O4	La2Sr0Cu0.85Zn0.15O4	La	2	Sr	0	Cu	0.85	Zn	0.15													O	4		1	1999								152																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19337	PR05900725		La2(Cu,Zn)O4	La2Sr0Cu0.8Zn0.2O4	La	2	Sr	0	Cu	0.8	Zn	0.2													O	4		1	1999								112																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19338	PR05900725		La2(Cu,Zn)O4	La2Sr0Cu0.75Zn0.25O4	La	2	Sr	0	Cu	0.75	Zn	0.25													O	4		1	1999								75																				T																																																																																																																								1					Ref[9]:M. Breuer et al., Physica C208,217(1993) anneal 72h 625C(N2)	Mobility of holes and suppression of antiferromagnetic order in La2-xSrxCuO4	199901		II. Physikalisches Institut, Universitat zu Koln, D-50937 Koln, Germany	Phys.Rev.B,59(1999)R725	A. Hoshi,B. Buchner,C. Pflitsch,J. HarraB,J. Pommer,M. Hucker,R. Gross,V. Kataev		
19339	PR05901491		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1999																												T																		K		36					36																																																																		microV/K					mOhmcm				0.71							1.8												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19340	PR05901491		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1999																												T																		K		30		26			30																																																																		microV/K	7.8				mOhmcm				0.36							1.2												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19341	PR05901491		(La,Sr)2CuO4	La1.79Sr0.21Cu1O4	La	1.79	Sr	0.21	Cu	1															O	4		1	1999																												T																		K		27		25			27																																																																		microV/K	6.1				mOhmcm				0.31							1.02												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19342	PR05901491		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		1	1999																												T																		K		21		22			21																																																																		microV/K	5.9				mOhmcm				0.6							1												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19343	PR05901491		(La,Sr)2CuO4	La1.77Sr0.23Cu1O4	La	1.77	Sr	0.23	Cu	1															O	4		1	1999																												T																		K		21		20			21																																																																		microV/K	2.8				mOhmcm				0.52							0.88												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19344	PR05901491		(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		1	1999																												T																		K		16		15			16																																																																		microV/K	1.1				mOhmcm				0.3							0.74												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19345	PR05901491		(La,Sr)2CuO4	La1.74Sr0.26Cu1O4	La	1.74	Sr	0.26	Cu	1															O	4		1	1999																												T																		K		13		12			13																																																																		microV/K					mOhmcm				0.14							0.54												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19346	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.995Zn0.005O4	La	1.82	Sr	0.18	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		30		28			30																																																																		microV/K	9				mOhmcm				0.43							1.2												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19347	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.81Sr0.19Cu0.995Zn0.005O4	La	1.81	Sr	0.19	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		29		25			29																																																																		microV/K	7				mOhmcm				0.44							1.2												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19348	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.995Zn0.005O4	La	1.8	Sr	0.2	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		19.5		19.5			19.5																																																																		microV/K	5.7				mOhmcm				0.8							0.91												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19349	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.79Sr0.21Cu0.995Zn0.005O4	La	1.79	Sr	0.21	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		20		20			20																																																																		microV/K	5.7				mOhmcm				0.98							1.12												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19350	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.995Zn0.005O4	La	1.78	Sr	0.22	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		20		19.5			20																																																																		microV/K	2.1				mOhmcm				0.22							0.61												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19351	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.77Sr0.23Cu0.995Zn0.005O4	La	1.77	Sr	0.23	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		18		16			18																																																																		microV/K	1.5				mOhmcm				0.41							0.84												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19352	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.76Sr0.24Cu0.995Zn0.005O4	La	1.76	Sr	0.24	Cu	0.995	Zn	0.005													O	4		1	1999																												T																		K		13		12			13																																																																		microV/K	0.5				mOhmcm				0.26							0.68												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19353	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.83Sr0.17Cu0.99Zn0.01O4	La	1.83	Sr	0.17	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		25		24			25																																																																		microV/K	9.2				mOhmcm				0.73							1.7												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19354	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.99Zn0.01O4	La	1.82	Sr	0.18	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		25		24			25																																																																		microV/K	7.5				mOhmcm				0.52							1.51												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19355	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.815Sr0.185Cu0.99Zn0.01O4	La	1.815	Sr	0.185	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		24					24																																																																		microV/K					mOhmcm				0.52							0.99												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19356	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.81Sr0.19Cu0.99Zn0.01O4	La	1.81	Sr	0.19	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		19		19			19																																																																		microV/K	6.5				mOhmcm				1.03							1.15												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19357	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.805Sr0.195Cu0.99Zn0.01O4	La	1.805	Sr	0.195	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		20					20																																																																		microV/K					mOhmcm				0.95							1.4												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19358	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.99Zn0.01O4	La	1.8	Sr	0.2	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		21		20			21																																																																		microV/K	3.8				mOhmcm				0.6							1.44												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19359	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.79Sr0.21Cu0.99Zn0.01O4	La	1.79	Sr	0.21	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		20		19			20																																																																		microV/K	2.5				mOhmcm				0.96							1												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19360	PR05901491		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.99Zn0.01O4	La	1.78	Sr	0.22	Cu	0.99	Zn	0.01													O	4		1	1999																												T																		K		17		14			17																																																																		microV/K	0.5				mOhmcm				0.23							0.72												La2O3, SrCO3,CuO,ZnO	1					solid state reaction mixed prefire 900C air 12h sinter 750C 3h 1050C 24h 500C 72h O2flow	Anomalies of Tc, resistivity, and thermoelectric power in the overdoped region of La2-xSrxCu1-yZnyO4	199901		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Phys.Rev.B,59(1999)1491	N. Kakinuma,Y. Koike,Y. Ono		
19400	PR05904504	Polycrystalline sample	(Er,Pr)Ba2Cu3O7-z	Er0.8Pr0.2Ba2Cu3O7-Z	Er	0.8	Pr	0.2	Ba	2	Cu	3													O	7-Z		6	1999																												Y123			A	3.817	3.884	11.67	3											K			80				80																																																																							m-ohmcm							1.1																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19401	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.75Pr0.2Ca0.05Ba2Cu3O7-Z	Er	0.75	Pr	0.2	Ca	0.05	Ba	2	Cu	3											O	7-Z		1	1999																												Y123			A	3.82	3.883	11.672	3											K			80				80																																																																																														R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19402	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.7Pr0.2Ca0.1Ba2Cu3O7-Z	Er	0.7	Pr	0.2	Ca	0.1	Ba	2	Cu	3											O	7-Z		1	1999																												Y123			A	3.8205	3.882	11.67	3											K			78				78																																																																							m-ohmcm							0.78																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19403	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.6Pr0.2Ca0.2Ba2Cu3O7-Z	Er	0.6	Pr	0.2	Ca	0.2	Ba	2	Cu	3											O	7-Z		1	1999																												Y123			A	3.82	3.879	11.665	3											K			74				74																																																																							m-ohmcm							0.52																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19404	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.5Pr0.2Ca0.3Ba2Cu3O7-Z	Er	0.5	Pr	0.2	Ca	0.3	Ba	2	Cu	3											O	7-Z		1	1999																												Y123			A	3.824	3.876	11.688	3											K			71				71																																																																							m-ohmcm							0.37																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19405	PR05904504	Polycrystalline sample	(Er,Pr)Ba2Cu3O7-z	Er0.9Pr0.1Ba2Cu3O7-Z	Er	0.9	Pr	0.1	Ba	2	Cu	3													O	7-Z		1	1999																												Y123																		K			80				80																																																																							m-ohmcm							0.75																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19406	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.85Pr0.1Ca0.05Ba2Cu3O7-Z	Er	0.85	Pr	0.1	Ca	0.05	Ba	2	Cu	3											O	7-Z		1	1999																												Y123																		K			82				82																																																																							m-ohmcm							0.41																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19407	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.8Pr0.1Ca0.1Ba2Cu3O7-Z	Er	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	7-Z		1	1999																												Y123																		K			77				77																																																																							m-ohmcm							0.47																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19408	PR05904504	Polycrystalline sample	(Er,Pr,Ca)Ba2Cu3O7-z	Er0.7Pr0.1Ca0.2Ba2Cu3O7-Z	Er	0.7	Pr	0.1	Ca	0.2	Ba	2	Cu	3											O	7-Z		1	1999																												Y123																		K			73				73																																																																							m-ohmcm							0.58																R2O3,Pr6O11,CaCO3,BaCO3,CuO	1	thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h				thepowders were reground and pressed under 40kg/cm3 into pellets, which were sintered flowing oxgen at 930 C for 30h followed by slow cooling to 680 C for 8h and slowly cooled to 450 C for 30h	Ion-size effect on superconducting transition temperature Tc in R1-x-yPrxCayBa2Cu3O7-z systems (R=Er, Dy, Gd, Eu, Sm, and Nd)	199802		Department of Physics, National Tsing Hua University, Hsinchu, 300, Taiwan, Republic of China	Phys.Rev.B,59(1999)4504	J.C. Chen,Li-Chun Tung,M.K. Wu,Weiyan Guan		
19409	PR05903827		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	1999																												T																		K			43				43			K/Kbar	0.23																																																																			m-ohmcm					100			56				390																		Optimal superconductivity in La2-xSrCuO4	199802		Texas Materials Science, University of Texas at Austin, Texas 78712	Phys.Rev.B,59(1999)3827	H. Sato,J.-S. Zhou,J.B. Goodenough,M. Naito		
19410	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.919Zn0.081O6.7	Y	1	Ba	2	Cu	2.919	Zn	0.081													O	Z	6.7	3	1999																												Y123																		K			17				17																																																																							m-ohmcm					330			310				845												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19411	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.931Zn0.069O6.7	Y	1	Ba	2	Cu	2.931	Zn	0.069													O	Z	6.7	3	1999																												Y123																		K			28				28																																																																							m-ohmcm					250			255				790												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19412	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.961Zn0.039O6.7	Y	1	Ba	2	Cu	2.961	Zn	0.039													O	Z	6.7	3	1999																												Y123																		K			38				38																																																																							m-ohmcm					180			130				680												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19413	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.931Zn0.069O6.6	Y	1	Ba	2	Cu	2.931	Zn	0.069													O	Z	6.6	3	1999																												Y123																		K			20				20																																																																							m-ohmcm					320			290				1050												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19414	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.931Zn0.069O6.5	Y	1	Ba	2	Cu	2.931	Zn	0.069													O	Z	6.5	3	1999																												Y123																		K																																																																														m-ohmcm					670							1490												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19415	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.919Zn0.081O6.75	Y	1	Ba	2	Cu	2.919	Zn	0.081													O	Z	6.75	3	1999																												Y123																		K			20				20																																																																							m-ohmcm					250			245				590												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19416	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.919Zn0.081O6.8	Y	1	Ba	2	Cu	2.919	Zn	0.081													O	Z	6.8	3	1999																												Y123																		K			24				24																																																																							m-ohmcm					200			185				430												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19417	PR05903948		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.919Zn0.081O6.83	Y	1	Ba	2	Cu	2.919	Zn	0.081													O	Z	6.83	3	1999																												Y123																		K			28				28																																																																							m-ohmcm					180			150				395												5	anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)				anneal:500-600 C 1-2days together with sintered blocks  Zdetermined by ICP method and the waight of the sintered block. X determined by ICP method (error of less than +-0.1%)	Charge localization from local destruction of antiferromagnetic correlation in Zn-doped YBa2Cu3O7-delta	199802		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)R3948	Kouji Segawa,Yoichi Ando		
19418	PR05904390		YBa2Cu3O7-d	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z		5	1999																												Y123																		K				89.5		0.5	89.5																																									nm	micro wave	160					6.4																																																					Optimal conductivity in YBa2Cu3O7-delta thin films	199802		Institut fur Physik, Universitat Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B,59(1999)4390	A. Loidl,A. Pimenov,G. Jakob,H. Adrian		
19419	PR05903870		Nd(Ba,Nd)2Cu3O6+z	Nd1Ba2Cu3O6.09	Nd	1	Ba	2	Cu	3															O	Z	6.09	3	1999								376																				Y123			A	3.898		11.882	1											K				90.5		1.5	90.5																																																																																																slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h				slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h	Antiferromagnetic ordering states of oxygen-deficient NdBa2Cu3O6+delta and Nd1+yBa2-yCu3O6+x single crystals	199802		Forschungszentrum Kalsruhe, INFP and ITP, P.O. Box 3640, D-76021 Kaelsruhe, Germany	Phys.Rev.B,59(1999)3870	A.T. Boothroyd,E. Brecht,H. Lutgemeier,J.M. Reynolds,N.H. Andersen,P. Schweiss,Th. Wolf,W.W. Schmahl		
19420	PR05903870		Nd(Ba,Nd)2Cu3O6+z	Nd1Ba2Cu3O6.23	Nd	1	Ba	2	Cu	3															O	Z	6.23	3	1999								289																				Y123			A	3.9		11.79	1											K				60.5		1.5	60.5																																																																																																slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h				slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h	Antiferromagnetic ordering states of oxygen-deficient NdBa2Cu3O6+delta and Nd1+yBa2-yCu3O6+x single crystals	199802		Forschungszentrum Kalsruhe, INFP and ITP, P.O. Box 3640, D-76021 Kaelsruhe, Germany	Phys.Rev.B,59(1999)3870	A.T. Boothroyd,E. Brecht,H. Lutgemeier,J.M. Reynolds,N.H. Andersen,P. Schweiss,Th. Wolf,W.W. Schmahl		
19421	PR05903870		Nd(Ba,Nd)2Cu3O6+z	Nd1.08Ba1.92Cu3O6.17	Nd	1.08	Ba	1.92	Cu	3															O	Z	6.17	3	1999								385																				Y123			A	3.89		11.814	1											K				77.5		1.5	77.5																																																																																																slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h				slow-cooling method(ref33) The grouth was in air at pressure of 70 mbar. X=0(x=0.08) sample was started at 1283K(1313K) and cooling rate 0.8K/h(1K/h) .anneal in 1 bar O2 873-673K , 500-600h	Antiferromagnetic ordering states of oxygen-deficient NdBa2Cu3O6+delta and Nd1+yBa2-yCu3O6+x single crystals	199802		Forschungszentrum Kalsruhe, INFP and ITP, P.O. Box 3640, D-76021 Kaelsruhe, Germany	Phys.Rev.B,59(1999)3870	A.T. Boothroyd,E. Brecht,H. Lutgemeier,J.M. Reynolds,N.H. Andersen,P. Schweiss,Th. Wolf,W.W. Schmahl		
19422	PR05903385		PrBa2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		1	1999																												Y124																																																																																																m-ohmcm	0.33			0.65							0.7														Solid state reaction tecnique(ref2)				Solid state reaction tecnique(ref2)	Pressure effect on quasi-one-dimensional charge transport in PrBa2Cu4O8: Magnetotransport study	199802		Superconductivity Research Laboratory, International Superconductivity Technology Cenyer, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,59(1999)3385	C. Murayama,I. Terasaki,J. Kikuchi,K. Tanabe,N. Koshizuka,N. Mori,N. Seiji,S. Adachi,S. Tajima,T. Machi		
19501	PR05906635	grain aligned sample. anisotropy factor = 4.8 	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8	8	1	1999																												Y124							1															81.5			81.5																																									A	ac susceptibility 		1270	6150																																																			at 935 C in oxygen 6MPa pressure the nitrate being first decomposed by slow heating to 710 C in air and it was racted as die-pressed pellets for 96h with intermediate milling and plletizing every 16h					Effects of the Cu-O chains on the anisotropic penetration depth of YBa2Cu4O8			IRC in Superconductivity, University of Cambridge, Nadingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,59(1999)R6635	Christos Panagopoulos,Jeffery L. Tallon,Tao Xiang		
19502	PR05907209		HgBa2CuO4+Z	Hg1Ba2Cu1O4.06	Hg	1	Ba	2	Cu	1															O	4+Z	4.06		1999																												Hg1201			A	3.88723		9.5372			A/Ma	-12.27		-48									75				75																																																																																																				anneald in argon flow at 350 C	Structure of HgBa2CuO4+delta(0.06<delta<0.19) at ambient and high pressure			Joint Institute for Nuclear Research, 141980, Dubna, Moscow region, Russia	Phys.Rev.B,59(1999)7209	A.M. Balagurov,D.V. Sheptyakov,E.V. Antipov,M. Marezio,P.G. Radaelli,S.N. Putilin,V.L. Aksenov		
19503	PR05907209		HgBa2CuO4+Z	Hg1Ba2Cu1O4.13	Hg	1	Ba	2	Cu	1															O	4+Z	4.13		1999																												Hg1201			A	3.88367		9.5298															97				97																																																																																																				250 C ogen atomosphere	Structure of HgBa2CuO4+delta(0.06<delta<0.19) at ambient and high pressure			Joint Institute for Nuclear Research, 141980, Dubna, Moscow region, Russia	Phys.Rev.B,59(1999)7209	A.M. Balagurov,D.V. Sheptyakov,E.V. Antipov,M. Marezio,P.G. Radaelli,S.N. Putilin,V.L. Aksenov		
19504	PR05907209		HgBa2CuO4+Z	Hg1Ba2Cu1O4.19	Hg	1	Ba	2	Cu	1															O	4+Z	4.19		1999																												Hg1201			A	3.87923		9.5244			A/Ma	-14.18		-47.28									70				70																																																																																																				270 C under oygen Pressure of 90 bar	Structure of HgBa2CuO4+delta(0.06<delta<0.19) at ambient and high pressure			Joint Institute for Nuclear Research, 141980, Dubna, Moscow region, Russia	Phys.Rev.B,59(1999)7209	A.M. Balagurov,D.V. Sheptyakov,E.V. Antipov,M. Marezio,P.G. Radaelli,S.N. Putilin,V.L. Aksenov		
19505	PR05906550		Y1Ba2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123			A	3.822	3.886	11.677	3													92					92		1																																																																uV/K				TP19505																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19506	PR05906550		(Y,Ca)(Ba,La)2Cu3Oz	Y0.95Ca0.05Ba1.95La0.05Cu3OZ	Y	0.95	Ca	0.05	Ba	1.95	La	0.05	Cu	3											O	Z		1	1999																												Y123			A	3.82	3.883	3.882	3													89.5					89.5		1																																																																uV/K																													1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19507	PR05906550		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.9La0.1Cu3OZ	Y	0.9	Ca	0.1	Ba	1.9	La	0.1	Cu	3											O	Z		1	1999																												Y123			A	3.82	3.882	11.672	3													86					86		1																																																																uV/K				TP19507																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19508	PR05906550		(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.8La0.2Cu3OZ	Y	0.8	Ca	0.2	Ba	1.8	La	0.2	Cu	3											O	Z		1	1999																												Y123			A	3.819	3.873	11.658	3													85.5					85.5		1																																																																uV/K				TP19508																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19509	PR05906550		(Y,Ca)(Ba,La)2Cu3Oz	Y0.7Ca0.3Ba1.7La0.3Cu3OZ	Y	0.7	Ca	0.3	Ba	1.7	La	0.3	Cu	3											O	Z		1	1999																												Y123			A	3.83	3.871	11.641	3													84.5					84.5		1																																																																uV/K				TP19509																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19510	PR05906550		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.6La0.4Cu3OZ	Y	0.6	Ca	0.4	Ba	1.6	La	0.4	Cu	3											O	Z		1	1999																												Y123			A	3.85	3.853	11.628	3													83					83		1																																																																uV/K				TP19510																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19511	PR05906550		Y1Ba2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123			A	3.82	3.89	11.675	3													91.5					91.5		1																																																																uV/K				TP19511																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19512	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.95Ca0.05Ba2Cu2.95Co0.05OZ	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Co	0.05											O	Z		1	1999																												Y123			A	3.832	3.89	11.675	3													88					88		1																																																																uV/K				TP19512																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19513	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.9Ca0.1Ba2Cu2.9Co0.1OZ	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Co	0.1											O	Z		1	1999																												Y123			A	3.867	3.867	11.671	3													88.5					88.5		1																																																																uV/K				TP19513																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19514	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.85Ca0.15Ba2Cu2.85Co0.15OZ	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z		1	1999																												Y123			A	3.876	3.876	11.666	3													87					87		1																																																																uV/K				TP19514																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19515	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.8Ca0.2Ba2Cu2.8Co0.2OZ	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Co	0.2											O	Z		1	1999																												Y123			A	3.876	3.876	11.666	3													84					84		1																																																																uV/K				TP19515																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19516	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.75Ca0.25Ba2Cu2.75Co0.25OZ	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	Z		1	1999																												Y123			A	3.878	3.878	11.669	3													85					85		1																																																																uV/K				TP19516																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19517	PR05906550		(Y,Ca)Ba2(Cu,Co)3Oz	Y0.7Ca0.3Ba2Cu2.7Co0.3OZ	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z		1	1999																												Y123			A	3.879	3.879	11.671	3													83					83		1																																																																uV/K				TP19517																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19518	PR05906550	asgrown	Y1Ba2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123			A	3.822	3.886	11.677	3													86					86		1																																																																uV/K				TP19518																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19519	PR05906550	asgrown	(Y,Ca)(Ba,La)2Cu3Oz	Y0.95Ca0.05Ba1.95La0.05Cu3OZ	Y	0.95	Ca	0.05	Ba	1.95	La	0.05	Cu	3											O	Z		1	1999																												Y123			A	3.82	3.883	3.882	3													82					82		1																																																																uV/K				TP19519																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19520	PR05906550	asgrown	(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.9La0.1Cu3OZ	Y	0.9	Ca	0.1	Ba	1.9	La	0.1	Cu	3											O	Z		1	1999																												Y123			A	3.82	3.882	11.672	3													77.5					77.5		1																																																																uV/K				TP19520																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19521	PR05906550	asgrown	(Y,Ca)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.8La0.2Cu3OZ	Y	0.8	Ca	0.2	Ba	1.8	La	0.2	Cu	3											O	Z		1	1999																												Y123			A	3.819	3.873	11.658	3													76					76		1																																																																uV/K				TP19521																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19522	PR05906550	asgrown	(Y,Ca)(Ba,La)2Cu3Oz	Y0.7Ca0.3Ba1.7La0.3Cu3OZ	Y	0.7	Ca	0.3	Ba	1.7	La	0.3	Cu	3											O	Z		1	1999																												Y123			A	3.83	3.871	11.641	3													68					68		1																																																																uV/K				TP19522																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19523	PR05906550	asgrown	(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.6La0.4Cu3OZ	Y	0.6	Ca	0.4	Ba	1.6	La	0.4	Cu	3											O	Z		1	1999																												Y123			A	3.85	3.853	11.628	3													67.5					67.5		1																																																																uV/K				TP19523																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19524	PR05906550	asgrown	Y1Ba2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123			A	3.82	3.89	11.675	3													84.5					84.5		1																																																																uV/K				TP19524																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19525	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.95Ca0.05Ba2Cu2.95Co0.05OZ	Y	0.95	Ca	0.05	Ba	2	Cu	2.95	Co	0.05											O	Z		1	1999																												Y123			A	3.832	3.89	11.675	3													74.5					74.5		1																																																																uV/K				TP19525																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19526	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.9Ca0.1Ba2Cu2.9Co0.1OZ	Y	0.9	Ca	0.1	Ba	2	Cu	2.9	Co	0.1											O	Z		1	1999																												Y123			A	3.867	3.867	11.671	3													70					70		1																																																																uV/K				TP19526																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19527	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.85Ca0.15Ba2Cu2.85Co0.15OZ	Y	0.85	Ca	0.15	Ba	2	Cu	2.85	Co	0.15											O	Z		1	1999																												Y123			A	3.876	3.876	11.666	3													57					57		1																																																																uV/K				TP19527																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19528	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.8Ca0.2Ba2Cu2.8Co0.2OZ	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Co	0.2											O	Z		1	1999																												Y123			A	3.876	3.876	11.666	3													55					55		1																																																																uV/K				TP19528																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19529	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.75Ca0.25Ba2Cu2.75Co0.25OZ	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	Z		1	1999																												Y123			A	3.878	3.878	11.669	3													68					68		1																																																																uV/K				TP19529																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19530	PR05906550	asgrown	(Y,Ca)Ba2(Cu,Co)3Oz	Y0.7Ca0.3Ba2Cu2.7Co0.3OZ	Y	0.7	Ca	0.3	Ba	2	Cu	2.7	Co	0.3											O	Z		1	1999																												Y123			A	3.879	3.879	11.671	3													72					72		1																																																																uV/K				TP19530																									1	mixture were calcined in air at 940 C for 24h and sintered three times at 920-950 C for 24h.Finally pellets were heated in flowing oxygen at 450 C for 10h and furnance cool down.				Reduced oxygen sample annealed again at 450 C for 2h in vaccum atomosphere	Thermopower in Y1-xCaxBa2-xLaxCu3Oy and Y1-xCa2Cu3-xCoxOy			Department of Semiconductor Physics and Nanoelectronics. St. Petersburg State Technical University, 29 Politekhnicheskaya, St. Petersburg, 195251, Russia	Phys.Rev.B,59(1999)6550	I.B. Patrina,M.V. Elizarova,V.E. Gasumyants		
19531	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4	4		1999			ergK/Oe2g	0.0000025																								T							3														38				38		1																																																																					mohmcm				0.2			0.18				0.45														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19532	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La1.7575Pr0.0925Sr0.15Cu1O4	La	1.7575	Pr	0.0925	Sr	0.15	Cu	1													O	4	4		1999																												T							3														37				37		1																																																																					mohmcm				0.28			0.2				1														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19533	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La1.665Pr0.185Sr0.15Cu1O4	La	1.665	Pr	0.185	Sr	0.15	Cu	1													O	4	4		1999			ergK/Oe2g	0.000024																								T							3														35				35		1																																																																					mohmcm				0.7			0.5				2														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19534	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La1.48Pr0.37Sr0.15Cu1O4	La	1.48	Pr	0.37	Sr	0.15	Cu	1													O	4	4		1999			ergK/Oe2g	0.00008																								T							3														34				34		1																																																																					mohmcm				0.8			0.55				2.3														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19535	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La1.295Pr0.555Sr0.15Cu1O4	La	1.295	Pr	0.555	Sr	0.15	Cu	1													O	4	4		1999			ergK/Oe2g	0.0001																								T							3														33				33		1																																																																					mohmcm				1			0.75				2.95														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19536	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La1.13Pr0.72Sr0.15Cu1O4	La	1.13	Pr	0.72	Sr	0.15	Cu	1													O	4	4		1999			ergK/Oe2g	0.000113																								T							3														32				32		1																																																																					mohmcm				1.2			0.9				3.8														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19537	PR05906557	Curie constant unit is 10-5erg K/(Oe)2g and Fig 9	(La,Pr,Sr)2CuO4	La0.925Pr0.925Sr0.15Cu1O4	La	0.925	Pr	0.925	Sr	0.15	Cu	1													O	4	4		1999			ergK/Oe2g	0.000141																								T							3														32				32		1																																																																					mohmcm				1.25			0.95				4														Solid state reaction method.the mixed powder were sinered 1150 C in oxygen atomosohere for 24h with two mediate temperature at 980 C and 1000					Normal state transport propert and magnetic properties in the (La1-xPrx)1.85Sr0.15CuO4system and their correlation with Tc suppression: A signature of the effects of orthorhombic distortions			Laboratorio de Superconductividad, Facultad de Fisica, Universidad de La Habona, San Lazaro y L, La Habana 10400, Cuba	Phys.Rev.B,59(1999)6557	B. Giordanengo,C. Rettori,E.M. Baggio-Saitovitch,H. Salim de Amorim,J.E. Musa,M. Rothier de Amaral,Jr.,P.J.G. Pagliuso,S. Garcia,S.K. Malik,W.B. Yelon		
19538	PR05907216		Tl2Ba2Ca2Cu3O10+z	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z			1999																												Tl2223							3														119				119																																				A	magnetic resistivity			21																																																								See G.Villard et al(J.Appl.Phys. To be published)					c-axis magnetoconductivity of anisotropic  superconducting single crystals: The density-of-states fluctuation scenario			Laboratoire CRISMAT, UMR 6508, ISMRAet Universite de Caen-Cedex, France	Phys.Rev.B,59(1999)7216	A. Maignan,A. Ruyter,A. Wahl,D. Thopart,G. Villard,J.C. Soret,L. Ammor,V. Hardy		
19539	PR05907216		Tl2Ba2Ca2Cu3O10+z	Tl2Ba2Ca2Cu3O10+Z	Tl	2	Ba	2	Ca	2	Cu	3													O	10+Z			1999																												Tl2223							3														120				120																																				A	magnetic resistivity			21																																																								See G.Villard et al(J.Appl.Phys. To be published)					c-axis magnetoconductivity of anisotropic  superconducting single crystals: The density-of-states fluctuation scenario			Laboratoire CRISMAT, UMR 6508, ISMRAet Universite de Caen-Cedex, France	Phys.Rev.B,59(1999)7216	A. Maignan,A. Ruyter,A. Wahl,D. Thopart,G. Villard,J.C. Soret,L. Ammor,V. Hardy		
19540	PR05907216		HgBa2CuO4+Z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z			1999																												Hg1201							3																																																						A	magnetic resistivity			6																																																								See G.Villard et al(J.Appl.Phys. To be published)					c-axis magnetoconductivity of anisotropic  superconducting single crystals: The density-of-states fluctuation scenario			Laboratoire CRISMAT, UMR 6508, ISMRAet Universite de Caen-Cedex, France	Phys.Rev.B,59(1999)7216	A. Maignan,A. Ruyter,A. Wahl,D. Thopart,G. Villard,J.C. Soret,L. Ammor,V. Hardy		
19541	PR05907184		(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4	4	3	1999																												T							3														32				32																																																																																																TSFZ method . See Phys.Rev.Lett., 67(1991)1791.					Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19542	PR05907184		(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4	4	3	1999																												T							3														36				36																																																																							mohmcm					0.152			0.12				0.475													TSFZ method . See Phys.Rev.Lett., 67(1991)1791.					Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19543	PR05907184		YBa2Cu3O7	Y1Ba2Cu3O7-Z	Y	1	Ba	2	Cu	3															O	7-Z			1999																												Y123			A	3.82	3.88	11.67	3													91					91		1																																																																uV/K				TP19543	mohmcm							0.7				1													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19544	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.97Mn0.03O7-Z	Y	1	Ba	2	Cu	2.97	Mn	0.03													O	7-Z			1999																												Y123							3													91					91		1																																																																uV/K				TP19544	mohmcm							1.3				1.6													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19545	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.955Mn0.045O7-Z	Y	1	Ba	2	Cu	2.955	Mn	0.045													O	7-Z			1999																												Y123							3													91					91		1																																																																uV/K				TP19545	mohmcm							1.8				2.6													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19546	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.94Mn0.06O7-Z	Y	1	Ba	2	Cu	2.94	Mn	0.06													O	7-Z			1999																												Y123							3													91					91		1																																																																uV/K				TP19546	mohmcm							2.6				3.9													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19547	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.925Mn0.075O7-Z	Y	1	Ba	2	Cu	2.925	Mn	0.075													O	7-Z			1999																												Y123							3													85					85		1																																																																uV/K				TP19547	mohmcm							3.5				4.9													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19548	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.895Mn0.105O7-Z	Y	1	Ba	2	Cu	2.895	Mn	0.105													O	7-Z			1999																												Y123							3													83					83		1																																																																uV/K				TP19548	mohmcm							3.9				5.7													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19549	PR05907184		YBa2(Cu,Mn)3O7-z	Y1Ba2Cu2.85Mn0.15O7-Z	Y	1	Ba	2	Cu	2.85	Mn	0.15													O	7-Z			1999																												Y123							3													82					82		1																																																																uV/K				TP19549	mohmcm							4.6				5.7													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19550	PR05907184		YBa2(Cu,Fe)3O7-z	Y1Ba2Cu2.925Fe0.075O7-Z	Y	1	Ba	2	Cu	2.925	Fe	0.075													O	7-Z			1999																												Y123			A	3.83	3.87	11.65	3													80					80		1																																																																uV/K				TP19550	mohmcm							4				7.2													1	The mixture was 900 C 12h.The presintered powders were pressed into 1*1*0.5cm size atuniaxial pressure of 6T .These pellet were sintered at 930 C 36h and furnance cooled.				O2 annialed at 450 C 60h	Tenperature evolution of the pseudogap state in the infrared response of underdoped La2-xSrxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4MI	Phys.Rev.B,59(1999)7184	A.V. Puchkov,D.N. Basov,H.A. Mook,K. Kishio,M. Okuya,T. Kimura,T. Startseva,T. Timusk		
19601	PR05909642		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1999																												T							1														27				27		M																																												cm-1	100																																																	TSFZ method . See Physica C , 192(1992)247					Doping dependence of the pseudogap in La2-xSrxCuO4			Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A IS6	Phys.Rev.B,59(1999)9642	J.C. Irwin,J.G. Naeini,K. Kishio,M. Okuya,T. Kimura,X.K. Chen		
19602	PR05909642		(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4		3	1999																												T							1														35				35		2																																												cm-1	100																																																	TSFZ method . See Physica C , 192(1992)247					Doping dependence of the pseudogap in La2-xSrxCuO4			Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A IS6	Phys.Rev.B,59(1999)9642	J.C. Irwin,J.G. Naeini,K. Kishio,M. Okuya,T. Kimura,X.K. Chen		
19603	PR05909642		(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		3	1999																												T							1														37				37		2																																												cm-1	100																																																	TSFZ method . See Physica C , 192(1992)247					Doping dependence of the pseudogap in La2-xSrxCuO4			Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A IS6	Phys.Rev.B,59(1999)9642	J.C. Irwin,J.G. Naeini,K. Kishio,M. Okuya,T. Kimura,X.K. Chen		
19604	PR05909642		(La,Sr)2CuO4	La1.81Sr0.19Cu1O4	La	1.81	Sr	0.19	Cu	1															O	4		3	1999																												T							1														32				32		2																																												cm-1	100																																																	TSFZ method . See Physica C , 192(1992)247					Doping dependence of the pseudogap in La2-xSrxCuO4			Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A IS6	Phys.Rev.B,59(1999)9642	J.C. Irwin,J.G. Naeini,K. Kishio,M. Okuya,T. Kimura,X.K. Chen		
19605	PR05909642		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		3	1999																												T							1														30				30		2																																												cm-1	100																																																	TSFZ method . See Physica C , 192(1992)247					Doping dependence of the pseudogap in La2-xSrxCuO4			Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A IS6	Phys.Rev.B,59(1999)9642	J.C. Irwin,J.G. Naeini,K. Kishio,M. Okuya,T. Kimura,X.K. Chen		
19606	PR05908978	asgrown	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212			A			30.849	1															80.5			80.5		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19607	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.89Pr0.11Cu2OZ	Bi	2	Sr	2	Ca	0.89	Pr	0.11	Cu	2											O	Z		3	1999																												Bi2212						30.82	1															73			73		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19608	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.83Pr0.17Cu2OZ	Bi	2	Sr	2	Ca	0.83	Pr	0.17	Cu	2											O	Z		3	1999																												Bi2212						30.766	1															51.6			51.6		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19609	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.72Pr0.28Cu2OZ	Bi	2	Sr	2	Ca	0.72	Pr	0.28	Cu	2											O	Z		3	1999																												Bi2212						30.7	1															54.3			54.3		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19610	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.65Pr0.35Cu2OZ	Bi	2	Sr	2	Ca	0.65	Pr	0.35	Cu	2											O	Z		3	1999																												Bi2212						30.699	1															30			30		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19611	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.55Pr0.45Cu2OZ	Bi	2	Sr	2	Ca	0.55	Pr	0.45	Cu	2											O	Z		3	1999																												Bi2212						30.476	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19612	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.47Pr0.53Cu2OZ	Bi	2	Sr	2	Ca	0.47	Pr	0.53	Cu	2											O	Z		3	1999																												Bi2212						30.438	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19613	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.4Pr0.6Cu2OZ	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	Z		3	1999																												Bi2212						30.372	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19614	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.35Pr0.65Cu2OZ	Bi	2	Sr	2	Ca	0.35	Pr	0.65	Cu	2											O	Z		3	1999																												Bi2212						30.3	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19615	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.3Pr0.7Cu2OZ	Bi	2	Sr	2	Ca	0.3	Pr	0.7	Cu	2											O	Z		3	1999																												Bi2212						30.292	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19616	PR05908978	asgrown	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.22Pr0.78Cu2OZ	Bi	2	Sr	2	Ca	0.22	Pr	0.78	Cu	2											O	Z		3	1999																												Bi2212						30.232	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19617	PR05908978	annealed	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212						30.814	1															85.5			85.5		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19618	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.89Pr0.11Cu2OZ	Bi	2	Sr	2	Ca	0.89	Pr	0.11	Cu	2											O	Z		3	1999																												Bi2212						30.788	1															87.8			87.8		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19619	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.83Pr0.17Cu2OZ	Bi	2	Sr	2	Ca	0.83	Pr	0.17	Cu	2											O	Z		3	1999																												Bi2212						30.69	1															84.2			84.2		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19620	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.72Pr0.28Cu2OZ	Bi	2	Sr	2	Ca	0.72	Pr	0.28	Cu	2											O	Z		3	1999																												Bi2212						30.648	1															72.4			72.4		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19621	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.65Pr0.35Cu2OZ	Bi	2	Sr	2	Ca	0.65	Pr	0.35	Cu	2											O	Z		3	1999																												Bi2212						30.598	1															68.8			68.8		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19622	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.55Pr0.45Cu2OZ	Bi	2	Sr	2	Ca	0.55	Pr	0.45	Cu	2											O	Z		3	1999																												Bi2212						30.47	1															46.6			46.6		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19623	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.47Pr0.53Cu2OZ	Bi	2	Sr	2	Ca	0.47	Pr	0.53	Cu	2											O	Z		3	1999																												Bi2212						30.432	1															30.8			30.8		2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19624	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.4Pr0.6Cu2OZ	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	Z		3	1999																												Bi2212						30.369	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19625	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.35Pr0.65Cu2OZ	Bi	2	Sr	2	Ca	0.35	Pr	0.65	Cu	2											O	Z		3	1999																												Bi2212						30.295	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19626	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.3Pr0.7Cu2OZ	Bi	2	Sr	2	Ca	0.3	Pr	0.7	Cu	2											O	Z		3	1999																												Bi2212						30.248	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19627	PR05908978	annealed	Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.22Pr0.78Cu2OZ	Bi	2	Sr	2	Ca	0.22	Pr	0.78	Cu	2											O	Z		3	1999																												Bi2212						30.203	1																10				2																																																																																														irectional solidification method.  See Physica C, 305(1998)227					Hole filling and interlayer coupling in Bi2Sr2Ca1-xPrxCu2Oy single crystals			Department of Materials Science and Engineering, University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B,59(1999)8978	H.C. Ku,X. Zhao,X.-G. Li,X.F. Sun		
19628	PR05908962		(Bi,Pb)2Sr2CaCu2O8+z	I1Bi1.9Pb0.1Sr2Ca1Cu2O8+Z	I	1	Bi	1.9	Pb	0.1	Sr	2	Ca	1	Cu	2									O	8+Z		1	1999																												Bi2212																					80			4	80		2																																							A	optical spectra T=10K		1980																																																				Intercalation. See Nature 348(1990)145					ab-plane optical spectra of iodine-intercalated Bi1.9Pb0.1Sr2CaCu2O8+delta: Normal and superconducting properties			Department of Physics, University of Florida, Gainesville, Florida 32611	Phys.Rev.B,59(1999)8962	D.B. Tanner,G. Margaritondo,H. Berger,H.L. Liu		
19700	PR05911205		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1999																												Y124							3											K				77			77			K/kbar	0.63																																																																			mOHM				0.3																									ref[11],[12]. ,Anealed at 800C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19701	PR05911205		(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		1	1999																												Y124							3											K				66			66			K/kbar	0.65																																																																							0.55																									ref[11],[12]. ,Anealed at 800C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19702	PR05911205		(Y,Pr)Ba2Cu4O8	Y0.6Pr0.4Ba2Cu4O8	Y	0.6	Pr	0.4	Ba	2	Cu	4													O	8		1	1999																												Y124							3											K				49			49			K/kbar	0.25																																																																							0.74																									ref[11],[12]. ,Anealed at 800C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19703	PR05911205		(Y,Pr)Ba2Cu4O8	Y0.4Pr0.6Ba2Cu4O8	Y	0.4	Pr	0.6	Ba	2	Cu	4													O	8		1	1999																												Y124							3											K				32			32			K/kbar	-2.53																																																																							0.77																									ref[11],[12]. ,Anealed at 840C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19704	PR05911205		(Y,Pr)Ba2Cu4O8	Y0.3Pr0.7Ba2Cu4O8	Y	0.3	Pr	0.7	Ba	2	Cu	4													O	8		1	1999																												Y124							3																																																																																													0.98																									ref[11],[12]. ,Anealed at 840C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19705	PR05911205	impurity phase = BaCuO2(less than 5 %)	(Y,Pr)Ba2Cu4O8	Y0.1Pr0.9Ba2Cu4O8	Y	0.1	Pr	0.9	Ba	2	Cu	4													O	8		1	1999																												Y124							3																																																																																													1.1																									ref[11],[12]. ,Anealed at 840C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19706	PR05911205		PrBa2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		1	1999								17																				Y124							3																																																																																													1.32																									ref[11],[12]. ,Anealed at 840C.	Pressure effects on the superconductivity and magnetic order of Y1-xPrxBa2Cu4O8	199905		Department of Physics , National sun Yat-Sen University, Kaohsiung, Taiwan 804, Republic of China	Phys.Rev.B,59(1999)11205	C.F. Chang,H.D. Yang,H.L. Tsay,I.P. Hong,J.-Y. Lin,S. Chatterjee,S.S. Weng		
19707	PR05911217		YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		1	1999																												Y123																		K				90.5			90.5																																																																																														Y2O3,BaCo3,CuO,ZnO	1					solid-state reaction technique after mixing raw materials at stoichiometric ratio.	Relaxation mechanisms for 63,65Cu nuclear quadrupole resenance in Zn-doped YBa2Cu3O7	199905		Department of Physics, Konkuk University, Seoul 143-701, Korea	Phys.Rev.B,59(1999)11217	B.J. Mean,G.S. Go,H.B. Kim,H.S. Lee,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
19708	PR05911217		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.99Zn0.01O7	Y	1	Ba	2	Cu	2.99	Zn	0.01													O	7		1	1999																												Y123																		K				86.5			86.5																																																																																														Y2O3,BaCo3,CuO,ZnO	1					solid-state reaction technique after mixing raw materials at stoichiometric ratio.	Relaxation mechanisms for 63,65Cu nuclear quadrupole resenance in Zn-doped YBa2Cu3O7	199905		Department of Physics, Konkuk University, Seoul 143-701, Korea	Phys.Rev.B,59(1999)11217	B.J. Mean,G.S. Go,H.B. Kim,H.S. Lee,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
19709	PR05911217		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.98Zn0.02O7	Y	1	Ba	2	Cu	2.98	Zn	0.02													O	7		1	1999																												Y123																		K				85			85																																																																																														Y2O3,BaCo3,CuO,ZnO	1					solid-state reaction technique after mixing raw materials at stoichiometric ratio.	Relaxation mechanisms for 63,65Cu nuclear quadrupole resenance in Zn-doped YBa2Cu3O7	199905		Department of Physics, Konkuk University, Seoul 143-701, Korea	Phys.Rev.B,59(1999)11217	B.J. Mean,G.S. Go,H.B. Kim,H.S. Lee,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
19710	PR05911217		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O7	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7		1	1999																												Y123																		K				83.5			83.5																																																																																														Y2O3,BaCo3,CuO,ZnO	1					solid-state reaction technique after mixing raw materials at stoichiometric ratio.	Relaxation mechanisms for 63,65Cu nuclear quadrupole resenance in Zn-doped YBa2Cu3O7	199905		Department of Physics, Konkuk University, Seoul 143-701, Korea	Phys.Rev.B,59(1999)11217	B.J. Mean,G.S. Go,H.B. Kim,H.S. Lee,K.H. Lee,K.S. Han,Moohee Lee,S.W. Seo,T.K. Park,W.C. Lee		
19711	PR05911179		Bi2Sr2CaCu2O8+x	Bi2Sr2Ca1Cu2O8+X	Bi	2	Sr	2	Ca	1	Cu	2													O	8+X		3	1999																												Bi2212							3											K	78						78																																																																							mOHM								0.1	2950			0.195	2050											5					self-flux method.	Positive in-plane and negative out-of-plane magnetoresistance in the overdoped high-temperature superconductor Bi2Sr2CaCu2O8+x	199905		Institut fur Materialphysik der Universitat Wien and Ludwig Boltzmann Institut fur Festkorperphysik, Kopernikusgasse 15, A-1060 Wien, Austria	Phys.Rev.B,59(1999)11179	G. Heine,S.X.  Dou,W. Lang,X.L. Wang		
19712	PR05912048		Sr14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41		3	1999																												LAD			A	11.46	13.4	3.975			A/GPa	-0.01	-0.1	-0.01					Analytical methods are energy-dipersive spectroscopy(EDS) and x-ray diffraction(XRD).																																																																																																												Preparation method is not described.	High-pressure synchrotron-diffraction study of the superconducting spin-ladder compounds (Sr,M)14Cu24O41 (M=Ca, Ba, Nd)	199905		Laboratoire de Cristallographie CNRS, Boite Postale 166,38042 Grenoble Cedex 9, France	Phys.Rev.B,59(1999)12048	Catherine Chaillout,Celine Darie,Hidenori Takagi,Massimo Marezio,Michael Hanfland,Pierre Bordet,Robert J. Cava,Ste'phanie Pachot		
19713	PR05912048		(Sr,Ca)14Cu24O41	Sr8Ca6Cu24O41	Sr	8	Ca	6	Cu	24															O	41		3	1999																												LAD			A	11.38	13	3.917			A/GPa	-0.11	-0.1	-0.0069					Analytical methods are energy-dipersive spectroscopy(EDS) and x-ray diffraction(XRD).																																																																																																												Preparation method is not described.	High-pressure synchrotron-diffraction study of the superconducting spin-ladder compounds (Sr,M)14Cu24O41 (M=Ca, Ba, Nd)	199905		Laboratoire de Cristallographie CNRS, Boite Postale 166,38042 Grenoble Cedex 9, France	Phys.Rev.B,59(1999)12048	Catherine Chaillout,Celine Darie,Hidenori Takagi,Massimo Marezio,Michael Hanfland,Pierre Bordet,Robert J. Cava,Ste'phanie Pachot		
19714	PR05912048	Tc=12 K under 3-5 Gpa	(Sr,Ca)14Cu24O41	Sr0.4Ca13.6Cu24O41	Sr	0.4	Ca	13.6	Cu	24															O	41		3	1999																												LAD			A	11.25	12.43	3.906			A/GPa	-0.013	-0.087	-0.0075					Analytical methods are energy-dipersive spectroscopy(EDS) and x-ray diffraction(XRD)																																																																																																												Preparation method is not described.	High-pressure synchrotron-diffraction study of the superconducting spin-ladder compounds (Sr,M)14Cu24O41 (M=Ca, Ba, Nd)	199905		Laboratoire de Cristallographie CNRS, Boite Postale 166,38042 Grenoble Cedex 9, France	Phys.Rev.B,59(1999)12048	Catherine Chaillout,Celine Darie,Hidenori Takagi,Massimo Marezio,Michael Hanfland,Pierre Bordet,Robert J. Cava,Ste'phanie Pachot		
19715	PR05912048		(Sr,Ba)14Cu24O41	Sr10Ba4Cu24O41	Sr	10	Ba	4	Cu	24															O	41		3	1999																												LAD			A	11.52	13.8	3.96			A/GPa	-0.0113	-0.125	-0.00741					Analytical methods are energy-dipersive spectroscopy(EDS) and x-ray diffraction(XRD)																																																																																																												Preparation method is not described.	High-pressure synchrotron-diffraction study of the superconducting spin-ladder compounds (Sr,M)14Cu24O41 (M=Ca, Ba, Nd)	199905		Laboratoire de Cristallographie CNRS, Boite Postale 166,38042 Grenoble Cedex 9, France	Phys.Rev.B,59(1999)12048	Catherine Chaillout,Celine Darie,Hidenori Takagi,Massimo Marezio,Michael Hanfland,Pierre Bordet,Robert J. Cava,Ste'phanie Pachot		
19716	PR05912048		(Sr,Nd)14Cu24O41	Sr8Nd6Cu24O41	Sr	8	Nd	6	Cu	24															O	41		3	1999																												LAD			A	11.35	13	3.985			A/GPa	-0.01	-0.075	-0.0075					Analytical methods are energy-dipersive spectroscopy(EDS) and x-ray diffraction(XRD)																																																																																																												Preparation method is not described.	High-pressure synchrotron-diffraction study of the superconducting spin-ladder compounds (Sr,M)14Cu24O41 (M=Ca, Ba, Nd)	199905		Laboratoire de Cristallographie CNRS, Boite Postale 166,38042 Grenoble Cedex 9, France	Phys.Rev.B,59(1999)12048	Catherine Chaillout,Celine Darie,Hidenori Takagi,Massimo Marezio,Michael Hanfland,Pierre Bordet,Robert J. Cava,Ste'phanie Pachot		
19717	PR05912090		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1999																												T			A	3.772		13.21	3														38				38																																																																			23.1			TP19717	mOHM							0.8				1												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19718	PR05912090		(La,Sr)2(Cu,Co)O4	La1.84Sr0.16Cu0.99Co0.01O4	La	1.84	Sr	0.16	Cu	0.99	Co	0.01													O	4		1	1999																												T			A	3.773		13.21	3														30				30																																																																			22.2			TP19718	mOHM							2.6				2												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19719	PR05912090		(La,Sr)2(Cu,Co)O4	La1.83Sr0.17Cu0.98Co0.02O4	La	1.83	Sr	0.17	Cu	0.98	Co	0.02													O	4		1	1999																												T			A	3.775		13.19	3														18				18																																																																			21			TP19719	mOHM							4.5				2.8												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19720	PR05912090		(La,Sr)2(Cu,Co)O4	La1.8Sr0.2Cu0.95Co0.05O4	La	1.8	Sr	0.2	Cu	0.95	Co	0.05													O	4		1	1999																												T			A	3.776		13.15	3																																																																																					20			TP19720	mOHM											4												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19721	PR05912090		(La,Sr)2(Cu,Co)O4	La1.75Sr0.25Cu0.9Co0.1O4	La	1.75	Sr	0.25	Cu	0.9	Co	0.1													O	4		1	1999																												T			A	3.778		13.13	3																																																																																					19.3			TP19721	mOHM											7												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19722	PR05912090		(La,Sr)2(Cu,Co)O4	La1.7Sr0.3Cu0.85Co0.15O4	La	1.7	Sr	0.3	Cu	0.85	Co	0.15													O	4		1	1999																												T			A	3.78		13.1	3																																																																																					18.7			TP19722	mOHM											11												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19723	PR05912090		(La,Sr)2(Cu,Co)O4	La1.65Sr0.35Cu0.8Co0.2O4	La	1.65	Sr	0.35	Cu	0.8	Co	0.2													O	4		1	1999																												T			A	3.783		13.08	3																																																																																					25				mOHM											21												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19724	PR05912090		(La,Sr)2(Cu,Co)O4	La1.55Sr0.45Cu0.7Co0.3O4	La	1.55	Sr	0.45	Cu	0.7	Co	0.3													O	4		1	1999																												T			A	3.785		13	3																																																																																					34				mOHM											120												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19725	PR05912090		(La,Sr)2(Cu,Co)O4	La1.45Sr0.55Cu0.6Co0.4O4	La	1.45	Sr	0.55	Cu	0.6	Co	0.4													O	4		1	1999																												T			A	3.791		12.91	3																																																																																					60				mOHM											1000												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19726	PR05912090		(La,Sr)2(Cu,Co)O4	La1.25Sr0.75Cu0.4Co0.6O4	La	1.25	Sr	0.75	Cu	0.4	Co	0.6													O	4		1	1999																												T			A	3.815		12.74	3																																																																																					20.8				mOHM											60000												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19727	PR05912090		(La,Sr)2(Cu,Co)O4	La1.15Sr0.85Cu0.3Co0.7O4	La	1.15	Sr	0.85	Cu	0.3	Co	0.7													O	4		1	1999																												T			A	3.81		12.63	3																																																																																					21.3				mOHM											40000												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19728	PR05912090		(La,Sr)2(Cu,Co)O4	La1.05Sr0.95Cu0.2Co0.8O4	La	1.05	Sr	0.95	Cu	0.2	Co	0.8													O	4		1	1999																												T			A	3.806		12.58	3																																																																																					19.7				mOHM											38000												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19729	PR05912090		(La,Sr)2(Cu,Co)O4	La0.95Sr1.05Cu0.1Co0.9O4	La	0.95	Sr	1.05	Cu	0.1	Co	0.9													O	4		1	1999																												T			A	3.804		12.52	3																																																																																					18.3				mOHM											12000												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19730	PR05912090		(La,Sr)2CoO4	La0.85Sr1.15Co1O4	La	0.85	Sr	1.15	Co	1															O	4		1	1999																												T			A	3.797		12.5	3																																																																																					17.6				mOHM											5500												La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19731	PR05912090		(La,Sr)2CoO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1999																												T			A				3																																																																																					16.5																											La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19732	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.83Sr0.17Cu0.98Ga0.02O4	La	1.83	Sr	0.17	Cu	0.98	Ga	0.02													O	4		1	1999																												T			A				3																																																																																					10.5																											La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19733	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.81Sr0.19Cu0.96Ga0.04O4	La	1.81	Sr	0.19	Cu	0.96	Ga	0.04													O	4		1	1999																												T			A				3																																																																																					10																											La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19734	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.79Sr0.21Cu0.94Ga0.06O4	La	1.79	Sr	0.21	Cu	0.94	Ga	0.06													O	4		1	1999																												T			A				3																																																																																					16																											La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19735	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.75Sr0.25Cu0.9Ga0.1O4	La	1.75	Sr	0.25	Cu	0.9	Ga	0.1													O	4		1	1999																												T			A				3																																																																																																																La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19736	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.65Sr0.35Cu0.8Ga0.2O4	La	1.65	Sr	0.35	Cu	0.8	Ga	0.2													O	4		1	1999																												T			A				3																																																																																																																La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19737	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.55Sr0.45Cu0.7Ga0.3O4	La	1.55	Sr	0.45	Cu	0.7	Ga	0.3													O	4		1	1999																												T			A				3																																																																																																																La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19738	PR05912090		(La,Sr)2(Cu,Ga)O4	La1.45Sr0.55Cu0.6Ga0.4O4	La	1.45	Sr	0.55	Cu	0.6	Ga	0.4													O	4		1	1999																												T			A				3																																																																																																																La2O3,CuO,Co2O3,Ga2O3,SrCO3	1					solid-state reaction method.preheated in 1070-1030 C ,(reground and pressed into pelltes ,sintered in air at 1080-1320 C for 24h)*2,finally cooled down to 800 C and kept for 40h.	Transport properties of La1.85-xSr0.15+xCu1-xMxOy (M=Co, Ga)	199905		Structure Research Laboratory University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B,59(1999)12090	Jin Hao,Liu Dengpan,Mao Zhiqiang,Wang Bin,Xu Gaojie,Yan Hongjie,Zhang Yuheng		
19800	PR05913639	Polycrystalline sample	(Y,Yb)Ba2Cu3O7	Y0.5Yb0.5Ba2Sr0Cu3O7-Z	Y	0.5	Yb	0.5	Ba	2	Sr	0	Cu	3											O	7-Z		1	1999																												Y123							3											K	87.2						87.2		R																																																											Wm-1K-1	3.45			THC19800	uV/K-1	-0.2				uohmcm											883														Mixed powder sintered at 950 C					Thermal Conductivity of partially substituted YBa2Cu3O7-delta	199906		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennesee 37831-6116	Phys.Rev.B,59(1999)13639	J.O. Scarbrough,P.M. Martin,R.K. Williams		
19801	PR05913639	Polycrystalline sample	(Y,Yb)(Ba,Sr)2Cu3O7	Y0.5Yb0.5Ba1.4Sr0.6Cu3O7-Z	Y	0.5	Yb	0.5	Ba	1.4	Sr	0.6	Cu	3											O	7-Z		1	1999																												Y123							3																																																																															Wm-1K-1										uohmcm											1077														Mixed powder sintered at 950 C					Thermal Conductivity of partially substituted YBa2Cu3O7-delta	199906		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennesee 37831-6116	Phys.Rev.B,59(1999)13639	J.O. Scarbrough,P.M. Martin,R.K. Williams		
19802	PR05913639	Polycrystalline sample	(Y,Yb)(Ba,Sr)2Cu3O7	Y0.5Yb0.5Ba1.4Sr0.6Cu3O7-Z	Y	0.5	Yb	0.5	Ba	1.4	Sr	0.6	Cu	3											O	7-Z		1	1999																												Y123							3																																																																															Wm-1K-1										uohmcm											1101														Mixed powder sintered at 950 C					Thermal Conductivity of partially substituted YBa2Cu3O7-delta	199906		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennesee 37831-6116	Phys.Rev.B,59(1999)13639	J.O. Scarbrough,P.M. Martin,R.K. Williams		
19803	PR05913639	Polycrystalline sample	(Y,Dy)(Ba,Sr)2Cu3O7	Y0.2Dy0.8Ba1.4Sr0.6Cu3O7-Z	Y	0.2	Dy	0.8	Ba	1.4	Sr	0.6	Cu	3											O	7-Z		1	1999																												Y123							3																																																																															Wm-1K-1																																			Mixed powder sintered at 950 C					Thermal Conductivity of partially substituted YBa2Cu3O7-delta	199906		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennesee 37831-6116	Phys.Rev.B,59(1999)13639	J.O. Scarbrough,P.M. Martin,R.K. Williams		
19804	PR05913639	Polycrystalline sample	Dy(Ba,Sr)2Cu3O7	Dy1Ba1.4Sr0.6Cu3O7-Z	Dy	1	Ba	1.4	Sr	0.6	Cu	3													O	7-Z		1	1999																												Y123							3																																																																															Wm-1K-1																																			Mixed powder sintered at 950 C					Thermal Conductivity of partially substituted YBa2Cu3O7-delta	199906		Oak Ridge National Laboratory, P.O. Box 2008, Oak Ridge, Tennesee 37831-6116	Phys.Rev.B,59(1999)13639	J.O. Scarbrough,P.M. Martin,R.K. Williams		
19805	PR05914023		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1999																											3	T			A	3.7949	3.7949	13.214	3											K				38.9			38.9																																									A	ac susceptibility		2340	5470																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19806	PR05914023		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.995Ni0.005O4	La	1.85	Sr	0.15	Cu	0.995	Ni	0.005													O	4		1	1999																											3	T			A	3.7804	3.7804	13.227	3											K				36.1			36.1																																									A	ac susceptibility		2640	5210																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19807	PR05914023		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4		1	1999																											3	T			A	3.7816	3.7816	13.229	3											K				33.6			33.6																																									A	ac susceptibility		3510	4530																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19808	PR05914023		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.985Ni0.015O4	La	1.85	Sr	0.15	Cu	0.985	Ni	0.015													O	4		1	1999																											3	T			A	3.7758	3.7758	13.24	3											K				31.7			31.7																																									A	ac susceptibility		4310	4360																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19809	PR05914023		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4		1	1999																											3	T			A	3.7825	3.7925	13.218	3											K				26.8			26.8																																									A	ac susceptibility		3760	5080																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19810	PR05914023		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.965Ni0.035O4	La	1.85	Sr	0.15	Cu	0.965	Ni	0.035													O	4		1	1999																											3	T			A	3.7839	3.7839	13.213	3											K				23.8			23.8																																									A	ac susceptibility		2100	7520																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19811	PR05914023		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.995Zn0.005O4	La	1.85	Sr	0.15	Cu	0.995	Zn	0.005													O	4		1	1999																											3	T			A	3.7983	3.7983	13.223	3											K				31.9			31.9																																									A	ac susceptibility		6020	9320																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19812	PR05914023		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01O4	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	4		1	1999																											3	T			A	3.7951	3.7951	13.219	3											K				27.9			27.9																																									A	ac susceptibility		7390	9680																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19813	PR05914023		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.98Zn0.02O4	La	1.85	Sr	0.15	Cu	0.98	Zn	0.02													O	4		1	1999																											3	T			A	3.7879	3.7879	13.251	3											K				17.5			17.5																																									A	ac susceptibility		6640	9620																																																	La2O3,SrCO3CuO,ZnO,NiO	1	Mixed powder calcining at 920 ,945C and into pellets and fired at 1020C for 24h and 1050C for 24 h and 1100C for 48h				Annealed 920 C for 12h cooled to 445 C ,annealed at this temperature for 48h and slowly cooled to room temperature.	Influence of Ni and Zn susstitution on anisotropy of the penetration depth in La1.85Sr0.15CuO4	199906		Institute of Low Temperature and Structure Research , Polish Academy of Sciences, P.O. box 1410, 50950 Wrocloaw, Poland	Phys.Rev.B,59(1999)14023	A.J. Zaleski,J. Klamut		
19814	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi2.1Sr1.7Ca0.9Cu2OZ	Bi	2.1	Sr	1.7	Ca	0.9	Cu	2													O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		79.1					79.1																																																																							ohmcm								0.00029	3.5			0.000706	3.05											7	powder ratio Bi:Pb:Sr:Ca:Cu=2.1:0:1.8:1.0:2.0 and growth rate 0.2 mm/h post anneal : 100 % O2 2.1 atm 400 C					Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19815	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi1.9Sr1.7Ca0.9Cu2OZ	Bi	1.9	Sr	1.7	Ca	0.9	Cu	2													O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		73.3					73.3																																																																							ohmcm									2.7				2.6											7	powder ratio Bi:Pb:Sr:Ca:Cu=2.0:0.1:1.8:1.0:2.0 and growth rate 0.5 mm/h post anneal : 100 % O2 2.1 atm 400 C					Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19816	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi2Pb0.1Sr1.8Ca0.9Cu2OZ	Bi	2	Pb	0.1	Sr	1.8	Ca	0.9	Cu	2											O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		70					70																																																																							ohmcm									1.6				1.8											7	powder ratio Bi:Pb:Sr:Ca:Cu=1.9:0.2:1.8:1.0:2.0 and growth rate 0.5 mm/h post anneal : 100 % O2 2.1 atm 400 C					Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19817	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi1.8Pb0.2Sr1.8Ca0.9Cu2OZ	Bi	1.8	Pb	0.2	Sr	1.8	Ca	0.9	Cu	2											O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		67.2					67.2																																																																							ohmcm								0.000185	0.8			0.000584	2.53											7	powder ratio Bi:Pb:Sr:Ca:Cu=1.8:0.3:1.8:1.0:2.0 and growth rate 0.5 mm/h post anneal : 100 % O2 2.1 atm 400 C					Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19818	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi1.6Pb0.4Sr1.8Ca0.9Cu2OZ	Bi	1.6	Pb	0.4	Sr	1.8	Ca	0.9	Cu	2											O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		65.1					65.1																																																																							ohmcm								0.0001275	0.25			0.000458	1.64											7	powder ratio Bi:Pb:Sr:Ca:Cu=1.6:0.6:1.8:1.0:2.0 and growth rate 1.0 mm/h post anneal : 100 % O2 2.1 atm 400 C					Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19819	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi2.1Sr1.7Ca0.9Cu2OZ	Bi	2.1	Sr	1.7	Ca	0.9	Cu	2													O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		85					85																																																																							ohmcm									5.8				5.28											7	powder ratio Bi:Pb:Sr:Ca:Cu=2.1:0:1.8:1.0:2.0 and growth rate 0.5 mm/h post anneal : 100 % O2 2.1 atm 400 C				anneal: 450 C O2 0.02atm	Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19820	PR05914080	Pb doped. Concentrations are analyzed values.	Bi2Sr2Ca1Cu2Oz	Bi1.6Pb0.4Sr1.8Ca0.9Cu2OZ	Bi	1.6	Pb	0.4	Sr	1.8	Ca	0.9	Cu	2											O	Z		3	1999																												Bi2212																	Cation compositions were determined by ICP	K		85.5					85.5																																																																							ohmcm									1.5				1											7	powder ratio Bi:Pb:Sr:Ca:Cu=1.6:0.6:1.8:1.0:2.0 and growth rate 1.0 mm/h post anneal : 100 % O2 2.1 atm 400 C				anneal: 600 C O2 3.9*10-4 atm	Systematic decrese of resistivity anisotropy in Bi2Sr2CaCu2Oy by Pb doping	199906		Department of Superconductivity, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,59(1999)14080	J. Shimoyama,K. Kishio,K. Kitazawa,T. Fujita,T. Motohashi,Y. Nakayama		
19821	PR05914753		(La,Ba)2CuO4	La1.905Ba0.095Cu1O4	La	1.905	Ba	0.095	Cu	1															O	4		3	1999																												T																	Ba concentrations determined by ICP	K		31					31		R																																																																					10-4ohmcm					2.8	5400		2.5	7500			9.5	4000	10-3cm3/C	2.18					RH19821				7	ref [9]				annealed in flowing oxygen atompsphere at 650 C for 24h	Nomal-state magneto transport in La1.905Ba0.095CuO4single crystal	199906		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,59(1999)14753	H. Kojima,H.Tanabe,I. Tanaka,J. Takeya,T. Watauchi,Yasushi Abe,Yoichi Ando		
19900	PR06000114		YBa2Cu3Oz	Y1Ba2Cu3OY	Y	1	Ba	2	Cu	3															O	Y		3	1999																												Y123																	The compositions are analyzed by ICP	K	93						93																					M(T) at H															A	caluculated from Hc2(T) ,which is evaluated from Tc(H) measured bythe diamagnetic susceptibility.		2	12.9																																																												solute rich liquid crystal puling(SRLCP). Annealed in flowing O2 for 200h at 500C.	Impurity effects on the superconducting coherence length in Zn-or Ni-doped YBa2Cu3O6.9 single crystals	199907		Superconductivity Research Laboratory, International Superconductivity Technology Center, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)114	A.I. Rykov,I. Terasaki,K. Tomimoto,S. Tajima,T. Mimura		
19901	PR06000114		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.988Zn0.012OY	Y	1	Ba	2	Cu	2.988	Zn	0.012													O	Y		3	1999																												Y123																	The compositions are analyzed by ICP	K	85						85																					M(T) at H															A	caluculated from Hc2(T) ,which is evaluated from Tc(H) measured bythe diamagnetic susceptibility.		3.56	12.8																																																												solute rich liquid crystal puling(SRLCP). Annealed in flowing O2 for 200h at 500C.	Impurity effects on the superconducting coherence length in Zn-or Ni-doped YBa2Cu3O6.9 single crystals	199907		Superconductivity Research Laboratory, International Superconductivity Technology Center, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)114	A.I. Rykov,I. Terasaki,K. Tomimoto,S. Tajima,T. Mimura		
19902	PR06000114		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.982Zn0.018OY	Y	1	Ba	2	Cu	2.982	Zn	0.018													O	Y		3	1999																												Y123																	The compositions are analyzed by ICP	K	82						82																					M(T) at H															A	caluculated from Hc2(T) ,which is evaluated from Tc(H) measured bythe diamagnetic susceptibility.		4.1	14.3																																																												solute rich liquid crystal puling(SRLCP). Annealed in flowing O2 for 200h at 500C.	Impurity effects on the superconducting coherence length in Zn-or Ni-doped YBa2Cu3O6.9 single crystals	199907		Superconductivity Research Laboratory, International Superconductivity Technology Center, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)114	A.I. Rykov,I. Terasaki,K. Tomimoto,S. Tajima,T. Mimura		
19903	PR06000114		YBa2(Cu,Ni)3Oz	Y1Ba2Cu2.97Ni0.03OY	Y	1	Ba	2	Cu	2.97	Ni	0.03													O	Y		3	1999																												Y123																	The compositions are analyzed by ICP	K	87						87																					M(T) at H															A	caluculated from Hc2(T) ,which is evaluated from Tc(H) measured bythe diamagnetic susceptibility.		2.55	13.8																																																												solute rich liquid crystal puling(SRLCP). Annealed in flowing O2 for 200h at 500C.	Impurity effects on the superconducting coherence length in Zn-or Ni-doped YBa2Cu3O6.9 single crystals	199907		Superconductivity Research Laboratory, International Superconductivity Technology Center, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)114	A.I. Rykov,I. Terasaki,K. Tomimoto,S. Tajima,T. Mimura		
19904	PR06001377	GAP is measured using STM	Bi2(Sr,Bi)2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8.22	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+D	8.22	3	1999																												Bi2212																		K									RM																																												mV	42																																																					TSFZ	Temperature and doping dependence of the Bi2.1Sr1.9CaCu2O8+delta pseudogap and superconducting gap	199907		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,60(1999)1377	Azusa Matsuda,Satoshi Sugita,Takao Watanabe		
19905	PR06001377	GAP is measured using STM	Bi2(Sr,Bi)2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8.25	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+D	8.25	3	1999																												Bi2212																		K									RM																																												mV	55																																																					TSFZ	Temperature and doping dependence of the Bi2.1Sr1.9CaCu2O8+delta pseudogap and superconducting gap	199907		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,60(1999)1377	Azusa Matsuda,Satoshi Sugita,Takao Watanabe		
19906	PR06001377	GAP is measured using STM	Bi2(Sr,Bi)2CaCu2O8	Bi2.1Sr1.9Ca1Cu2O8.28	Bi	2.1	Sr	1.9	Ca	1	Cu	2													O	8+D	8.28	3	1999																												Bi2212																		K									RM																																												mV	41.8																																																					TSFZ	Temperature and doping dependence of the Bi2.1Sr1.9CaCu2O8+delta pseudogap and superconducting gap	199907		NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-01, Japan	Phys.Rev.B,60(1999)1377	Azusa Matsuda,Satoshi Sugita,Takao Watanabe		
20000	SOV0010001	thick film (50micron),microcrytallites oriented mainly along [DOI] with c-axis normal to substrate	Bi2Sr2Ca(Cu,Li)2O8	Bi2Sr2Ca1Cu1.2Li0.8Oz	Bi	2	Sr	2	Ca	1	Cu	1.2	Li	0.8											O	z		4	1995																												Bi2212																			89					10	89																																																																																																two stage process,melting (865C,10min)-ANN(820C,6min), substrate+MgO(100)									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20001	SOV0010001	multi-phase film(120micron),resistance=0.2 Ohm at RT	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	1995																												Bi2212																			82					20	82																																																																																														oxide, carbonate		two-stage process, melting(940c,10min)-ANN(840C,20min)  sustrate+MgO(100)									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20002	SOV0010001	multi-phase(Bi2212+Bi2201+others), 100micron thickness, resistance=1.64 Ohm at RT	Bi2Sr2Ca(Cu,Li)2O8	Bi2Sr2Ca1Cu1.2Li0.2Oz	Bi	2	Sr	2	Ca	1	Cu	1.2	Li	0.2											O	z		4	1995																												Bi2212																			50						50																																																																																																two stage process,melting (940C,10min)-ANN(840C,20min)  substrate+MgO(100)									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20003	SOV0010001	d=50micron,single phase, Resistance=1.17Ohm at RT	Bi2Sr2Ca(Cu,Li)2O8	Bi2Sr2Ca1Cu1.2Li0.8Oz	Bi	2	Sr	2	Ca	1	Cu	1.2	Li	0.8											O	z		4	1995																												Bi2212																			82						82																																																																																																two step process,melting(860C,10min)-ANN(820C,15min)  substate+poly-Mgo									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20004	SOV0010001	mult-phase,d=130micron, R=1.16 Ohm at RT		Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	1995																																															74						74																																																																																																melting(940C,10min)-ANN(840C,30min)  substrate+poiy-MgO									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20005	SOV0010001	d=150micron,single phase, R=0.5 Ohm at RT	Bi2Sr2Ca(Cu,Li)2O8	Bi2Sr2Ca1Cu1.2Li0.8Oz	Bi	2	Sr	2	Ca	1	Cu	1.2	Li	0.8											O	z		4	1995																												Bi2212																			80					10	80																																																																																																melting(860C,10min)-ANN(820C,15min)  (111)Ga-Gd garnet									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20006	SOV0010001	d=190micron, R=0.8 Ohm at RT	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		4	1995																												Bi2212																			40						40																																																																																																melting(950C,10min)-ANN(850C,60min)  (111)Ga-Gd garnet									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20007	SOV0010001	Bi2212+Bi2201+unknown phase d=50micron, R=0.23 Ohm at RT	Bi2Sr2Ca(Cu,Li)2O8	Bi2Sr2Ca1Cu1.2Li0.8Oz	Bi	2	Sr	2	Ca	1	Cu	1.2	Li	0.8											O	z		4	1995																												Bi2212																			74.2						74.2																																																																																																two step process,melting(860C,10min)-ANN(820C,15min)  substate+poly-Mgo									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20008	SOV0010001	d=120 micron, R=0.25 Ohm at RT	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		4	1995																																															76						76																																																																																																									Sverkhprovodimost':fizika,Khimiya,tekhnika, 8(1995)94	E.M.Gololovov,et.al	Bi,Sr,Ca,Cu,Li,O	Superconductivity:physics,chemistry,technique; 8(1995)94
20009	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1995																																															89					10	89																																																																																		1.3													9	mixture-melting (1330C,30min)-quench (850C, in Cu anvil)-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20010	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.24	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.24	1	1995																																															80					20	80																																																																																		0.7													9	mixture-melting (1330C,30min)-quench (850C, in Cu anvil)-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20011	SOV0010002		BiSr2CaCu2O8	Bi2Sr2Ca1Cu2O8.17	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.17	1	1995																																															85.5					15	85.5																																																																																		1													9	mixture-melting (1330C,30min)-quench (850C, in Cu anvil)-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20012	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.15	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.15	1	1995																																																			77																																																																																				1.2													9	mixture-melting (1330C,30min)-quench (850C, in Cu anvil)-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20013	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	1995																																															82.5					10.5	82.5																																																																																		1.4														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20014	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.14	Bi	2	Sr	2	Ca	1	Cu	2													O	8	8.14		1995																																															81					10	81																																																																																		0.8														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20015	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.16		1995																																															86					7	86																																																																																		0.7														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20016	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.16	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.16		1995																																															86					9	86																																																																																		0.5														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20017	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.15	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.15		1995																																																			77																																																																																				0.8														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20018	SOV0010002		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.15	Bi	2	Sr	2	Ca	1	Cu	2													O	z	8.15		1995																																																			77																																																																																				0.4														mixture-melt(1330,30min)-slow cooling-ANN(750-850C,90H in air)									Soverkhprovodimost':fizika,khimiya,tekhnika; 8(1995)100	I.B.Bobylev,et al	Bi,Sr,Ca,Cu,O	Superconductivity:phisics,chemistry,technique; 8(1995)100
20019	SOV0010007		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																			89					3.5	89																																																																															0.63																										Pis'ma v Zhurnal EXperimental'noy i Teoreticheskoy Fiziki:ZhETP Lett.,62(1995)934	L.P.Mezhov-Deglin,V.B.Yefimov	Bi,Sr,Ca,Cu,O	Pis'ma v Zhurnal Experimental'noy i Teoreticheskoy Fiziki, 62(1995)934-939
20020	SOV0010007		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																			86					1.5	86																																																																															0.22																										Pis'ma v Zhurnal EXperimental'noy i Teoreticheskoy Fiziki:ZhETP Lett.,62(1995)934	L.P.Mezhov-Deglin,V.B.Yefimov	Bi,Sr,Ca,Cu,O	Pis'ma v Zhurnal Experimental'noy i Teoreticheskoy Fiziki, 62(1995)934-939
20021	SOV0010007		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1995																												Bi2212																			82					4	82																																																																																																									Pis'ma v Zhurnal EXperimental'noy i Teoreticheskoy Fiziki:ZhETP Lett.,62(1995)934	L.P.Mezhov-Deglin,V.B.Yefimov	Bi,Sr,Ca,Cu,O	Pis'ma v Zhurnal Experimental'noy i Teoreticheskoy Fiziki, 62(1995)934-939
20022	SOV0010008	RRR=2.2	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		4	1995																												Y123						11.671													88.4						88.4																																																			2500000																																													laser evaporation,Excimer     laser, grouth rate=4A/10 pulses									Fizika tverdogo tela, 37(1995)880-893	Yu.A.Boikov,et al	Y,Ba,Cu,O	Fizika tverdogo tera(Solid State Phisics), 37(1995)880-893
20023	SOV0010008	RRR=2.6	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		4	1995																												Y123						11.677													89.5						89.5																																																			3500000																																													laser evaporation,Excimer     laser, grouth rate=4A/10 pulses									Fizika tverdogo tela, 37(1995)880-893	Yu.A.Boikov,et al	Y,Ba,Cu,O	Fizika tverdogo tera(Solid State Phisics), 37(1995)880-893
20024	SOV0010008	RRR=2.8	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		4	1995																												Y123						11.679													91						91																																																			5000000																																													laser evaporation,Excimer     laser, grouth rate=4A/10 pulses									Fizika tverdogo tela, 37(1995)880-893	Yu.A.Boikov,et al	Y,Ba,Cu,O	Fizika tverdogo tera(Solid State Phisics), 37(1995)880-893
20025	SOV0010009	inter grair Tc=67K	Bi4Sr3Ca3Cu4Oz	Bi4Sr3Ca3Cu4Oz	Bi	4	Sr	3	Ca	3	Cu	4													O	z			1995																											2	4334				5.412		30.624																80			80																																																																																														Bi2O3,CuO,SrCO3,CaCO3		mixture-pellet-heat(830C,65H in air),with multiple in termediately grinding-SIN(830C,60H in air)-cool to RT(100C/H)									Fizika nizkikh temperatur; 21(1995)265	S.V.Korostin,et al	Bi,Sr,Ca,Cu,Fe,O	Low Temperature Physics, Kharkov, Ukraine); 21(1995)265-269
20026	SOV0010009	distribation of Fe was determined by Mossbauer spectroscopy, intergrain Tc=58K	Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.96Fe0.4Oz	Bi	4	Sr	3	Ca	3	Cu	3.96	Fe	0.4											O	z			1995																											2	4334				5.403		30.614																72			72																																																																																														Bi2O3,CuO,SrCO3,CaCO3		mixture-pellet-heat(830C,65H in air),with multiple in termediately grinding-SIN(830C,60H in air)-cool to RT(100C/H)									Fizika nizkikh temperatur; 21(1995)265	S.V.Korostin,et al	Bi,Sr,Ca,Cu,Fe,O	Low Temperature Physics, Kharkov, Ukraine); 21(1995)265-269
20027	SOV0010009	inter grain Tc=44K	Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.88Fe0.12Oz	Bi	4	Sr	3	Ca	3	Cu	3.88	Fe	0.12											O	z			1995																											2					5.4		30.624																66			66																																																																																														Bi2O3,CuO,SrCO3,CaCO3		mixture-pellet-heat(830C,65H in air),with multiple in termediately grinding-SIN(830C,60H in air)-cool to RT(100C/H)									Fizika nizkikh temperatur; 21(1995)265	S.V.Korostin,et al	Bi,Sr,Ca,Cu,Fe,O	Low Temperature Physics, Kharkov, Ukraine); 21(1995)265-269
20028	SOV0010009	inter grain Tc=15K	Bi4Sr3Ca3(Cu,Fe)4Oz	Bi4Sr3Ca3Cu3.6Fe0.4Oz	Bi	4	Sr	3	Ca	3	Cu	3.6	Fe	0.4											O	z			1995																											2					5.406		30.59																70			70																																																																																														Bi2O3,CuO,SrCO3,CaCO3		mixture-pellet-heat(830C,65H in air),with multiple in termediately grinding-SIN(830C,60H in air)-cool to RT(100C/H)									Fizika nizkikh temperatur; 21(1995)265	S.V.Korostin,et al	Bi,Sr,Ca,Cu,Fe,O	Low Temperature Physics, Kharkov, Ukraine); 21(1995)265-269
20029	SOV0010010	crystal size=3*3*0.28 mm3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		3	1995																												Y123																			86.6					2	86.6																																																																																			0.78	4.6												crystal growth from melt solution									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)665-671	I.K.Kamilov,et al	Y,Ba,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)665-671
20030	SOV0010011	sul=(100)SrTiO3	LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.69																87		1	87																																																			1100000																																													Metal-organic CVD									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)113-122	S.V.Samoilenkov,et al.		
20031	SOV0010011	sul=(100)LaAl3	LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.69																87		2	87																																																			960000																																													Metal-organic CVD									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)113-122	S.V.Samoilenkov,et al.		
20032	SOV0010011	sul=(100)ZrO2	LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.67																87		1	87																																																			970000																																													Metal-organic CVD									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)113-122	S.V.Samoilenkov,et al.		
20033	SOV0010011	sul=(100)NdGaO3	LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.69																85		2	85																																																			80000																																													Metal-organic CVD									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)113-122	S.V.Samoilenkov,et al.		
20034	SOV0010011	sul=(100)CaGaAlO3	LuBa2Cu3O7	Lu1Ba2Cu3O7	Lu	1	Ba	2	Cu	3															O	7		4	1995																												Y123																						86		4	86																																																																																																Metal-organic CVD									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)113-122	S.V.Samoilenkov,et al.		
20035	SOV0010012	thickness=100nm, subst=AL2O3	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1995																												Y123																				86				4	86																								340																																																																								growth method not indicated									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)37-46	A.I.Bykov,et al	Y,Ba,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)37-46
20036	SOV0010014	polycrystaite film on MgO substrate	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1995																												Y123																			80					3	80																																														MeV	10	2.91	1																																																								Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)259-265	S.I.Tyutyunnikov,et al	Y,Ba,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)259-265
20037	SOV0010015	Tc=0K	(Nd, Ce)2CuO4	Nd1.88Ce0.12Cu1O4-z	Nd	1.88	Ce	0.12	Cu	1															O	4-z		5	1995																												T'																							4.2																																																																																					1.02													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20038	SOV0010015	RRR=3.6	(Nd,Ce)2CuO4	Nd1.86Ce0.14Cu1O4-z	Nd	1.86	Ce	0.14	Cu	1															O	4-z		5	1995																												T'																			22						22																																																																																			0.89													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20039	SOV0010015	RRR=4.8	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		5	1995																												T'																			23						23																																																																																			0.78													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20040	SOV0010015	RRR=3.8	(Nd,Ce)2CuO4	Nd1.83Ce0.17Cu1O4-z	Nd	1.83	Ce	0.17	Cu	1															O	4-z		5	1995																												T'																			14						14																																																																																			0.35													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20041	SOV0010015	RRR=3.8, ABRES=ro+A*T2 with ro=0.085,A=2.70E-6 mOhm,cm/K2	(Nd,Ce)2CuO4	Nd1.82Ce0.18Cu1O4-z	Nd	1.82	Ce	0.18	Cu	1															O	4-z		5	1995																												T'																			9						9																																																																																			0.32													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20042	SOV0010015	RRR=5.5 ABRES=ro+A*T2 with ro=0.047,A=2.70E-6 mOhm,cm/K2	(Nd,Ce)2CuO4	Nd1.8Ce0.2Cu1O4-z	Nd	1.8	Ce	0.2	Cu	1															O	4-z		5	1995																												T'																							4.2																																																																																					0.26													See Physica C, 180(1991)69,depositted by laser sputtering. in vac (780C,0.01 Torr, 40min)									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)193-201	N.A.Babushkina,et al	Nd,Ce,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)193-201
20043	SOV0010013	d=1000A gy laser sputlering in O2(1mbar,810C,constant O2flow 10cm3/min) on (110)NdGaO3	YBa2Cu3O4	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.675													89.4						89.4																																																																																																by laser sputlering in O2(1mbar,810C,constant O2flow 10cm3/min) on (110)NdGaO3									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)288-294	P.B.Mozhayev,et al	Y,Ba,Cu,O	Sverkhprovodimost': fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)288-294
20044	SOV0010013	d=1000A	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		4	1995																												Y123						11.68													92					1.5	92																																																			500000																																0.35													by laser sputlering in O2(1mbar,810C,constant O2flow 10cm3/min) on (110)NdGaO3									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)288-294	P.B.Mozhayev,et al	Y,Ba,Cu,O	Sverkhprovodimost': fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)288-294
20045	SOV0010017		La2CuO4	La2Cu1O4.03	La	2	Cu	1																	O	4+z	4.03		1995																												T	Bmab																			25.8	34				25.8																					HC2=(Fi/2*Pi*cohere^2)(T/Tc-1)											2.66	0.495						51	9																																																																	Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)523-530	A.A.Teplov,A.A.Zakharov	La,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)523-530
20046	SOV0010017	two phase,second phase was anti-ferromagnetic	La2CuO4	La2Cu1O4.04	La	2	Cu	1																	O	4+z	4.04	2	1995																												T	Fmmm																			28	36.1				28																					HC2=(Fi/2*Pi*cohere^2)(T/Tc-1)											6.1	0.8						39	5																																																								see									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)523-530	A.A.Teplov,A.A.Zakharov	La,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)523-530
20047	SOV0010018		EuBa2Cu3Oz	Eu1Ba2Cu3O6.5	Eu	1	Ba	2	Cu	3															O	7-z	6.5	1	1995																											3	Y123				3.851	3.904	11.662															92			3	92																																																																																																ANN(500C,5H)-cool to RT (100C/H) in O2 flow									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)734-737	N.I.Ignat'yeva	Eu,Ba,Cu,O	Sverkhprovodimost':fizika,khimiya,tekhnika(Superconductivity:physics,chemistry,technique); 8(1995)734-737
20048	SOV0010019		GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z		1	1996																											3	Y123				3.842	3.896	11.706													91.6		93.7			1.5	92.65																																																																														1.66																Ci-,Gd-oxide,Ba-nitrate	1	mixture-heat(800-850C,2H in air)-pellet-heat(950C,15H,in O2 flow)-FC-SIN(950C,18H in O2 flow)-stepwise cooling									Fizika tverdogo tela, 38(1996)145-154	V.P.D'yakonov,et al	Gd,Ba,Cu,O	Fizika tverdogo tera(Solid State Physics); 38(1996)145-154
20049	SOV0010019		Gd(Ba,Gd)2Cu3O7	Gd1.1Ba1.9Cu3O7-z	Gd	1.1	Ba	1.9	Cu	3															O	7-z		1	1996																											3	Y123				3.85	3.89	11.7													79.5		81.7			2.2	80.6																																																																														5.62																Ci-,Gd-oxide,Ba-nitrate	1	mixture-heat(800-850C,2H in air)-pellet-heat(950C,15H,in O2 flow)-FC-SIN(950C,18H in O2 flow)-stepwise cooling									Fizika tverdogo tela, 38(1996)145-154	V.P.D'yakonov,et al	Gd,Ba,Cu,O	Fizika tverdogo tera(Solid State Physics); 38(1996)145-154
20050	SOV0010019		Gd(Ba,Gd)2Cu3O7	Gd0.8Ba1.8Cu3O7-z	Gd	0.8	Ba	1.8	Cu	3															O	7-z		1	1996																											2	Y123				3.878		11.67													44.5		52.6			5	48.55																																																																														11.6																Ci-,Gd-oxide,Ba-nitrate	1	mixture-heat(800-850C,2H in air)-pellet-heat(950C,15H,in O2 flow)-FC-SIN(950C,18H in O2 flow)-stepwise cooling									Fizika tverdogo tela, 38(1996)145-154	V.P.D'yakonov,et al	Gd,Ba,Cu,O	Fizika tverdogo tera(Solid State Physics); 38(1996)145-154
20051	SOV0010019		Gd(Ba,Gd)2Cu3O7	Gd0.7Ba1.7Cu3O7-z	Gd	0.7	Ba	1.7	Cu	3															O	7-z		1	1996																											2	Y123				3.87		11.613													31.1		42			6.4	36.55																																																																														14.7																Ci-,Gd-oxide,Ba-nitrate	1	mixture-heat(800-850C,2H in air)-pellet-heat(950C,15H,in O2 flow)-FC-SIN(950C,18H in O2 flow)-stepwise cooling									Fizika tverdogo tela, 38(1996)145-154	V.P.D'yakonov,et al	Gd,Ba,Cu,O	Fizika tverdogo tera(Solid State Physics); 38(1996)145-154
20052	SOV0010019		Gd(Ba,Gd)2Cu3O7	Gd0.62Ba1.62Cu3O7-z	Gd	0.62	Ba	1.62	Cu	3															O	7-z		1	1996																											2	Y123				3.868		11.604													28.6		41			8	34.8																																																																														19																Ci-,Gd-oxide,Ba-nitrate	1	mixture-heat(800-850C,2H in air)-pellet-heat(950C,15H,in O2 flow)-FC-SIN(950C,18H in O2 flow)-stepwise cooling									Fizika tverdogo tela, 38(1996)145-154	V.P.D'yakonov,et al	Gd,Ba,Cu,O	Fizika tverdogo tera(Solid State Physics); 38(1996)145-154
20053	SOV0010020	two phase(La2CuO4+La2CuO4.08) ,calculated from b=12(Pi)^4*R*n/(5*Debeit^3),n=7	La2CuO4	La2Cu1O4.08	La	2	Cu	1																	O	4+z	4.08	2	1995																											3	T																			30						30																																																									2.51	C/T=g+B8T^2+a*T^4	394																																				1	mixture-heat(650C,15H2.5kbar in O2)-ANN									Fizika tverdogo tela, 37(1995)3661-3668	G.F.Syrykh,et al	La,Cu,O	Fizika tverdogo tera(Solid State Physics); 37(1995)3661-3668
20054	SOV0010020	two phase(La2CuO4+La2CuO4.08), calculated from b=12(Pi)^4*R*n/(5*Debeit^3),n=7	La2CuO4	La2Cu1O4+z	La	2	Cu	1																	O	4+z		1	1995																												T																							5																																																											0.64	C/T=g+b*T2+a*T^4	396																																					annealing of sample 20053 in vac									Fizika tverdogo tela, 37(1995)3661-3668	G.F.Syrykh,et al	La,Cu,O	Fizika tverdogo tera(Solid State Physics); 37(1995)3661-3668
20055	SOV0010021	Single phase ,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z		1	1996																											2	T			A				1											K				37.43			37.43						0.143																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20056	SOV0010021	Single phase, ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)04	La1.85Sr0.15Cu0.995Ni0.005O4+z	La	1.85	Sr	0.15	Cu	0.995	Ni	0.005													O	4+z		1	1996																											2	T			A				1											K				34.41			34.41						0.125																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20057	SOV0010021	Single phase ,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4+z	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4+z		1	1996																											2	T			A															K				30			30						0.147																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20058	SOV0010021	Single phase, ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.985Ni0.015O4+z	La	1.85	Sr	0.15	Cu	0.985	Ni	0.015													O	4+z		1	1996																											2	T			A				1											K				25.9			25.9						0.252																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20059	SOV0010021	Single phase, ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4+z	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4+z		1	1996																											2	T			A				1											K				21.96			21.96						0.266																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20060	SOV0010021	Single phase, ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4+z	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4+z		1	1996																											2	T			A				1											K				16.6			16.6						0.367																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20061	SOV0010021	Single phase, ISOTOPE=ln (1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4+z	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4+z		1	1996																											2	T			A				1											K				12.7			12.7						0.335																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20062	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z		1	1996																											2	T			A				1											K				37.5			37.5						0.148																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20063	SOV0010021	Single phase,ISOTOPE-ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.997Fe0.003O4+z	La	1.85	Sr	0.15	Cu	0.997	Fe	0.003													O	4+z		1	1996																											2	T			A				1											K				33.6			33.6						0.203																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20064	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.995Fe0.005O4+z	La	1.85	Sr	0.15	Cu	0.995	Fe	0.005													O	4+z		1	1996																											2	T			A				1											K				30.82			30.82						0.274																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20065	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)04	La1.85Sr0.15Cu0.993Fe0.007O4+z	La	1.85	Sr	0.15	Cu	0.993	Fe	0.007													O	4+z		1	1996																											2	T			A				1											K				26.25			26.25						0.69																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20066	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.992Fe0.008O4+z	La	1.85	Sr	0.15	Cu	0.992	Fe	0.008													O	4+z		1	1996																											2	T			A				1											K				24.73			24.73						0.805																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20067	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.991Fe0.009O4+z	La	1.85	Sr	0.15	Cu	0.991	Fe	0.009													O	4+z		1	1996																											2	T			A				1											K				19.85			19.85						0.966																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20068	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.989Fe0.011O4+z	La	1.85	Sr	0.15	Cu	0.989	Fe	0.011													O	4+z		1	1996																											2	T			A				1											K				17.7			17.7						1.29																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20069	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z		1	1996																											2	T			A				1											K				37.5			37.5						0.148																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20070	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.996Zn0.004O4+z	La	1.85	Sr	0.15	Cu	0.996	Zn	0.004													O	4+z		1	1996																											2	T			A				1											K				37.5			37.5						0.158																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20071	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.992Zn0.008O4+z	La	1.85	Sr	0.15	Cu	0.992	Zn	0.008													O	4+z		1	1996																											2	T			A				1											K				28.5			28.5						0.203																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20072	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.988Zn0.012O4+z	La	1.85	Sr	0.15	Cu	0.988	Zn	0.012													O	4+z		1	1996																											2	T			A				1											K				23.7			23.7						0.26																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20073	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.984Zn0.016O4+z	La	1.85	Sr	0.15	Cu	0.984	Zn	0.016													O	4+z		1	1996																											2	T			A				1											K				19			19						0.44																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20074	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.978Zn0.022O4+z	La	1.85	Sr	0.15	Cu	0.978	Zn	0.022													O	4+z		1	1996																											2	T			A				1											K				13.6			13.6						0.677																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20075	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z		1	1996																											2	T			A				1											K				37.57			37.57						0.146																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20076	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.998Co0.002O4+z	La	1.85	Sr	0.15	Cu	0.998	Co	0.002													O	4+z		1	1996																											2	T			A				1											K				34.61			34.61						0.157																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20077	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.995Co0.005O4+z	La	1.85	Sr	0.15	Cu	0.995	Co	0.005													O	4+z		1	1996																											2	T			A				1											K				32.17			32.17						0.168																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20078	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.993Co0.007O4+z	La	1.85	Sr	0.15	Cu	0.993	Co	0.007													O	4+z		1	1996																											2	T			A				1											K				29.57			29.57						0.236																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20079	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)(Cu,Co)O4	La1.85Sr0.15Cu0.99Co0.01O4+z	La	1.85	Sr	0.15	Cu	0.99	Co	0.01													O	4+z		1	1996																											2	T			A				1											K				24.86			24.86						0.388																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20080	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(CU,Co)O4	La1.85Sr0.15Cu0.988Co0.013O4+z	La	1.85	Sr	0.15	Cu	0.988	Co	0.013													O	4+z		1	1996																											2	T			A				1											K				23.21			23.21						0.455																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20081	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.985Co0.015O4+z	La	1.85	Sr	0.15	Cu	0.985	Co	0.015													O	4+z		1	1996																											2	T			A				1											K				13.82			13.82						1.29																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20082	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.983Co0.018O4+z	La	1.85	Sr	0.15	Cu	0.983	Co	0.018													O	4+z		1	1996																											2	T			A				1											K				13.05			13.05						1.075																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20083	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4+z	La	1.8	Sr	0.2	Cu	1															O	4+z		1	1996																											2	T			A				1											K				34.62			34.62						0.219																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20084	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.995Ni0.005O4+z	La	1.8	Sr	0.2	Cu	0.995	Ni	0.005													O	4+z		1	1996																											2	T			A				1											K				31.47			31.47						0.165																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20085	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.99Ni0.01O4+z	La	1.8	Sr	0.2	Cu	0.99	Ni	0.01													O	4+z		1	1996																											2	T			A				1											K				28.26			28.26						0.137																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20086	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.985Ni0.015O4+z	La	1.8	Sr	0.2	Cu	0.985	Ni	0.015													O	4+z		1	1996																											2	T			A				1											K				25.77			25.77						0.136																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20087	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La0.8Sr0.2Cu0.98Ni0.02O4+z	La	0.8	Sr	0.2	Cu	0.98	Ni	0.02													O	4+z		1	1996																											2	T			A				1											K				22.36			22.36						0.131																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20088	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.975Ni0.025O4+z	La	1.8	Sr	0.2	Cu	0.975	Ni	0.025													O	4+z		1	1996																											2	T			A				1											K				19.61			19.61						0.125																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20089	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.97Ni0.03O4+z	La	1.8	Sr	0.2	Cu	0.97	Ni	0.03													O	4+z		1	1996																											2	T			A				1											K				17.22			17.22						0.115																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20090	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Ni)O4	La1.8Sr0.2Cu0.965Ni0.035O4+z	La	1.8	Sr	0.2	Cu	0.965	Ni	0.035													O	4+z		1	1996																											2	T			A				1											K				14.03			14.03						0.155																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20091	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4+z	La	1.8	Sr	0.2	Cu	1															O	4+z		1	1996																											2	T			A				1											K				34.44			34.44						0.11																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20092	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.997Fe0.003O4+z	La	1.8	Sr	0.2	Cu	0.997	Fe	0.003													O	4+z		1	1996																											2	T			A				1											K				32.28			32.28						0.123																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20093	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.995Fe0.005O4+z	La	1.8	Sr	0.2	Cu	0.995	Fe	0.005													O	4+z		1	1996																											2	T			A				1											K				29.3			29.3						0.143																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20094	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.993Fe0.007O4+z	La	1.8	Sr	0.2	Cu	0.993	Fe	0.007													O	4+z		1	1996																											2	T			A				1											K				27.86			27.86						0.167																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20095	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.99Fe0.01O4+z	La	1.8	Sr	0.2	Cu	0.99	Fe	0.01													O	4+z		1	1996																											2	T			A				1											K				23.81			23.81						0.253																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20096	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.988Fe0.012O4+z	La	1.8	Sr	0.2	Cu	0.988	Fe	0.012													O	4+z		1	1996																											2	T			A				1											K				20.65			20.65						0.307																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20097	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18).,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.985Fe0.015O4+z	La	1.8	Sr	0.2	Cu	0.985	Fe	0.015													O	4+z		1	1996																											2	T			A				1											K				16.04			16.04						0.507																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20098	SOV0010021	Single phase,ISOTOPE=ln(1-dTc/Tc)/ln(M16/M18). ,ISOEL=O	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.983Fe0.017O4+z	La	1.8	Sr	0.2	Cu	0.983	Fe	0.017													O	4+z		1	1996																											2	T			A				1											K				13.02			13.02						0.564																																																																																								CuO,NiO,CaCO3	11	sol-gel method, mixture-heat(700C,10H+1100C,4H)-press to pellet-heat(1100C,2H)-ANN(1100C,3H)-ANN(600C,50H)-slow cool to RT					Anomalous isotope effect in high-temperature superconductor LSCO with 3d-impurities			Original paper:  Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)649-656	Physica C, 272(1996)257	N.A.Babushkina,A.P.Zhernov,A.V.Inyushkin,T.N.Kulagina,V.I.Ozhogin,L.V.Molchanova		
20099	SOV0010003	Two-phase sample:1)HgSr2(La,Ce)Cu2O(6+z) (phase1212)and2)HgSr2(La,Ce)2Cu3O(8+z)(phase 1223)with LATA=3.842(2),LATC=12.59(4).	HgSr2(La,Ce)Cu2O6	Hg1Sr2La0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	La	0.333	Ce	0.667	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.855		12.258	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides, Sr(CO3)2	1	precursor(R-Ce-Cu-O)-addition of HgO-pellet-heat(750C,3.5GPa,5min)in high pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20100	SOV0010003		HgSr2(La,Ce)Cu2O6	Hg1Sr2La0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	La	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.847		12.19	1											K					4.2																																																																																																La,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(La-Ce-Cu-O)-addition of HgO-pellet-heat(750C,4GPa,10min) in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20101	SOV0010003	Sihgle phase HgSr2(La,Ce)2Cu3O8(structure 1223)	HgSr2(La,Ce)Cu2O6	Hg1Sr2La0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	La	0.333	Ce	0.667	Cu	2											O	6+z		1	1995																											2	Hg1223			A	3.842		15.49	1											K					4.2																																																																																																La,Ce,Cu and Hg oxides,Sr(CO3)21	1	precursor(La-Ce,-Cu-O)-addition of HgO-pellet-heat(850C,3GPa,5min) in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20102	SOV0010003	Two-phase sample:1)HgSr2(La,Ce)Cu2O6(phase1212) and 1)HgSr2(La,Ce)2Cu3O8(phase 1223)with LATA=3.830(4), LATC=15.41(6)	HgSr2(La,Ce)Cu2O6	Hg1Sr2La0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	La	0.333	Ce	0.667	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.823		12.24	1											K			40				40																																																																																														La,Ce,Cu and Hg oxides, Sr(CO3)2	1	precursor (La-Ce-Cu-O)-addition of HgO-pellet-heat(850C,4GPa,15min) in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20103	SOV0010003	Two-phase sample:1)HgSr2(La,Ce)Cu2O6(phase1212) and 2)HgSr2(La,Ce)2Cu3O8(phase 1223)with LATA=3.843(6), LATC=15.60(2)	HgSr2(La,Ce)Cu2O6	Hg1Sr2La0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	La	0.333	Ce	0.667	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.873		12.22	1											K			40				40																																																																																														La,Ce,Cu and Hg oxides, Sr(CO3)2	1	precursor(La-Ce-Cu-O)-addition of HgO-pellet-heat(850C,7GPa,5min)in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20104	SOV0010003	Single phase HgSr2(La,Ca,Ce)Cu2O6(structure 1212**,in which Hg-O or(Hg,Cu)-O bond is along<hko>)	HgSr2(La,Ca,Ce)Cu2O6	Hg1Sr2La0.3Ca0.5Ce0.2Cu2O6+z	Hg	1	Sr	2	La	0.3	Ca	0.5	Ce	0.2	Cu	2									O	6+z		1	1995																											2	Hg1212			A	3.855		11.77	1											K			81				81																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20105	SOV0010003	Single phase HgSr2(La,Ca,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(La,Ca,Ce)Cu2O6	Hg1Sr2La0.3Ca0.4Ce0.3Cu2O6+z	Hg	1	Sr	2	La	0.3	Ca	0.4	Ce	0.3	Cu	2									O	6+z		1	1995																											2	Hg1212			A	3.826		12.08	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20106	SOV0010003	Two-phase sample:1)HgSr2(La,Ca)Cu2O6(phase1212) and 2)Hg(La,Sr)Cu2O4(phase 1201).	HgSr2(La,Ca)Cu2O6	Hg1Sr2La0.5Ca0.5Cu2O6+z	Hg	1	Sr	2	La	0.5	Ca	0.5	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.395		12.36	1											K			54				54																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20107	SOV0010003	Single phase HgSr2CaCu2O6(structure 1201)	HgSr2CaCu2O6	Hg1Sr2Ca1Cu2O6+z	Hg	1	Sr	2	Ca	1	Cu	2													O	6+z		1	1995																											2	Hg1201			A	3.867		8.64	1											K					4.2																																																																																																Cu and Hg oxides,Sr(CO3)2	1	precursor(Sr-Ca-Cu-O)-addition of HgO-pellet-heat(800C,SGPa,5min) in high-pressure chamber of the RtoriedR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20108	SOV0010003	Two-phase sample:1)(Hg,Cu)Sr2LaCu2O6(phase1212,)(Hg-Cu)-O bond along <100>)  and 2)HgSr2LaCu2O6 (phase 1212,Hg-O bond along<110>)with LATA=3.873(3) ATC=12.40(8)	HgSr2LaCu2O6	Hg1Sr2La1Cu2O6+z	Hg	1	Sr	2	La	1	Cu	2													O	6+z		2	1995																											2	Hg1212			A	3.834		11.56	1											K			28				28																																																																																														La,Cu and Hg oxides,Sr(CO3)2	1	precursor(La-Cu-Ca-O)-addition of HgO-pellet-heat (850C,4Gpa,5min) in high-pressure chamber of the RtoridR type									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20109	SOV0010003	Two-phase sample:1)HgSr2(La,Ca)Cu2O6(phase1212 withHg-O bond along<110>) and 2)HgSr2(La,Ca)Cu2O6(phase 1212 with Hg-O or(Hg,Cu)-O bond along<hko>)with LATA=3.845(5), LATC=11.73(4).	HgSr2(La,Ca)Cu2O6	Hg1Sr2La0.5Ca0.5Cu2O6+z	Hg	1	Sr	2	La	0.5	Ca	0.5	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.884		12.23	1											K			51				51																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20110	SOV0010003	Single phase HgSr2(La,Ca)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(La,Ca)Cu2O6	Hg1Sr2La0.5Ca0.5Cu2O6+z	Hg	1	Sr	2	La	0.5	Ca	0.5	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.857		12.17	1											K					4.2																																																																																																La,Cu and Hg Oxides,Sr(CO3)2	1	precursor(La-Cu-Sr-O)+ HgO-pellet heat treatment (750C,4Gpa,15min) in high-pressure chamber of the RtoroidR type									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20111	SOV0010003	Single phase HgSr2(Pr,Ce)Cu2O6(structure 1212,in wich Hg-O bond is along<110>)	HgSr2(Pr,Ce)Cu2O6	Hg1Sr2Pr0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	Pr	0.333	Ce	0.667	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.856		12.2	1											K					4.2																																																																																																Pr,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(Pr-Ce-Cu-Sr-O)+HgO-pellet heat treatment(750C, 3 GPa, 5min)in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20112	SOV0010003	Multiphase sample with Hg1212,Hg2212,CeO2,CuO	HgSr2(Pr,Ce)Cu2O6	Hg1Sr2Pr0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	Pr	0.333	Ce	0.667	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.857		12.23												K			40				40																																																																																														Pr,Ce,Cu and Hg oxides Sr(CO3)2	1	precursor (Pr-Ce-Cu-Sr-O)+ HgO-pellet heat treatment(800C,3.5 GPa, 5min)in high-pressure chamber of the RtoroidR type									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20113	SOV0010003	Single phase HgSr2(Nd,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	Hgsr2(Nd,Ce)Cu2O6	Hg1Sr2Nd0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	Nd	0.333	Ce	0.667	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.859		12.189	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20114	SOV0010003	Single phase HgSr2(Nd,Ce)Cu2O6(structure 1212,in wichi Hg-O bond is along<110>)	HgSr2(Nd,Ce)Cu2O6	Hg1Sr2Nd0.333Ce2Cu2O6+z	Hg	1	Sr	2	Nd	0.333	Ce	2	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.834		12.14	1											K					4.2																																																																																																La,Ce,Cu and Hg oxides,Sr(CO3)21	1	precursor(La-Ce,-Cu-O)-addition of HgO-pellet-heat(850C,3GPa,5min) in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20115	SOV0010003	Two-phase sample:1)HgSr2(Nd,Ca)Cu2O6(structure 1212,in which Hg-O bond is along <110>;2)Hg2Sr4(Nd,Ca)Cu2OZ(phase2212)or Hg2Sr4(Nd,Ca)3Cu5OZ(phase2435)withLATA=3.853(2),LATC=14.00(5)2=28.00(5).	HgSr2(Nd,Ca)Cu2O6	Hg1Sr2Nd0.925Ca0.075Cu2O6+z	Hg	1	Sr	2	Nd	0.925	Ca	0.075	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.855		12.07	1											K			56				56																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20116	SOV0010003	Single phase HgSr2(Nd,Ca,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Nd,Ca,Ce)Cu2O6	Hg1Sr2Nd0.3Ca0.5Ce0.2Cu2O6+z	Hg	1	Sr	2	Nd	0.3	Ca	0.5	Ce	0.2	Cu	2									O	6+z		1	1995																											2	Hg1212			A	3.831		12.08	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor (R-Ce-Cu-Sr-O)+HgO-pellet heat treatment(800C,3 GPa,5min)in high-pressure chamber of the RtoriedR type									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20117	SOV0010003	Two-phase sample:1)HgSr2(Sm,Ce)Cu2O6(Phase 1212 withHg-O bond along<110>)and 2)HgSr2(Sm,Ce)Cu2O6([hase1212**with Hg-O) or(Hg,Cu)-O bond along<hko>)withLATA=3.827(7),LATC=11.73(4)	HgSr2(Sm,Ce)Cu2O6	Hg1Sr2Sm0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	Sm	0.333	Ce	0.667	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.853		12.18	1											K			40				40																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20118	SOV0010003	Two-phase sample:1)HgSr2(Sm,Ce)Cu2O6(structure1212,in which hg-O bond is along<110>;2) Hg2Sr4(Sm,Ce)Cu2OZ (phase2212)or Hg2Sr4(Nd,Ca)3Cu5OZ(phase2435)withLATA=3.845(5), LATC=14.10(5) 2=28.20(5)	HgSr2(Sm,Ce)Cu2O6	Hg1Sr2Sm0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Sm	0.667	Ce	0.333	Cu	2											O	6+z		2	1995																											2	Hg1212			A	3.842		12.04	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20119	SOV0010003	Single phase HgSr2(Eu,Ca)Cu2O6(structure 1212,in wich Hg-O bond is along<110>)	HgSr2(Eu,Ca)Cu2O6	Hg1Sr2Eu0.5Ca0.5Cu2O6+z	Hg	1	Sr	2	Eu	0.5	Ca	0.5	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.835		12.03	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20120	SOV0010003	Single phase HgSr2(Gd,Ce)Cu2O6 (structure 1212,in which Hg-O bond is along<110>)	HgSr2(Gd,Ce)Cu2O6	Hg1Sr2Gd0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Gd	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.833		11.99	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20121	SOV0010003	Structure not indicated in the paper.	HgSr2(Tb,Ce)Cu2O6	Hg1Sr2Tp0.333Ce0.667Cu2O6+z	Hg	1	Sr	2	Tp	0.333	Ce	0.667	Cu	2											O	6+z		1	1995																															A	3.8		11.99	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20122	SOV0010003	Single phase HgSr2(Dy,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Dy,Ce)Cu2O6	Hg1Sr2Dy0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Dy	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.825		12.02	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20123	SOV0010003	Single phase Hg(Sr,Y)(Y,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	Hg(Sr,Y)(Y,Ce)Cu2O6	Hg1Sr0.85Y0.9Ce0.25Cu2O6+z	Hg	1	Sr	0.85	Y	0.9	Ce	0.25	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.815		12.04	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20124	SOV0010003	Single phase HgSr2(Ho,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Ho,Ce)Cu206	Hg1Sr2Ho0.333Ce0.667Cu2O6=z	Hg	1	Sr	2	Ho	0.333	Ce	0.667	Cu	2											O	6=z		1	1995																											2	Hg1212			A	3.833		11.93	1											K			72				72																																																																																														R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20125	SOV0010003	Single phase HgSr2(Ho,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Ho,Ce)Cu2O6	Hg1Sr2Ho0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Ho	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.834		12.08	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor (R-Ce-Cu-Sr-O)+HgO-pellet heat treatment(800C,3 GPa,5min)in high-pressure chamber of the RtoriedR type									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20126	SOV0010003	Single phase HgSr2(Ho,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Ho,Ce)Cu2O6	Hg1Sr2Ho0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Ho	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.81		12.04	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides, Sr(CO3)2	1	precursor(R-Ce-Cu-O)-addition of HgO-pellet-heat(750C,3.5GPa,5min)in high pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20127	SOV0010003	Single phase HgSr2(Ho,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Ho,Ce)Cu2O6	Hg1Sr2Ho0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Ho	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.816		12.02	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides Sr(CO3)2	1	precursor(R-Ce-Cu-Sr-O)+HgO-pellet-heat treatment(700C,4GPa,5min) in high-pressure chamber of the RtoroidR type.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20128	SOV0010003	Single phase HgSr2(Ho,Ce)Cu2O6(structure 1212,in which Hg-O bond is along<110>)	HgSr2(Ho,Ce)Cu2O6	Hg1Sr2Ho0.667Ce0.333Cu2O6+z	Hg	1	Sr	2	Ho	0.667	Ce	0.333	Cu	2											O	6+z		1	1995																											2	Hg1212			A	3.821		11.98	1											K					4.2																																																																																																R,Ce,Cu and Hg oxides,Sr(CO3)2	1	precursor(R-Ce-O)-addition of HgO-pellet-heat(750C,4GPa, 5min) in high-pressure chamber of the RtoroidRtype.									SC:PhChT(Sverkhprovodimost'fizika,khimiya,tekhnika), 8(1995)325-334	G.M.Kuz'mitcheva,et al.		
20129	SOV0010025		YBa2Cu3O7	Y0.19Ba1.99Cu2.85O7-z	Y	0.19	Ba	1.99	Cu	2.85															O	7-z		1	1995																												Y123			A			11.682	1										1-phase(123)sample	K	94.5				94.5		94.5		3																																																																																												CuO,Y2O3,BaCO3	1	mixture-CAL(900C,26H)-SIN(950C,45-70H)-slow cooling(10deg.min)-additional holding at 400C(10-20H).									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)702-708	K.I.Furaleva,et al.		
20130	SOV0010025	1-phase(123)sample with substitution by cations Sc,Sr and V, (1-x)YBa2Cu3O7-x(ScSr2V3O11),		Y1.27Ba1.89Cu2.82Sc0.01Sr0.13V0.07O7-z	Y	1.27	Ba	1.89	Cu	2.82	Sc	0.01	Sr	0.13	V	0.07									O	7-z		1	1995																												Y123			A			11.675	1											K					96				3																																																																																												BaCO3,SrCO3	1	(1-x)YBa2Cu3O7+x(ScSr2V3O11) and PREPID=20129									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)702-708	K.I.Furaleva,et al.		
20131	SOV0010025	1-phase(123)sample with substitution by cations Sc,Sr and V, (1-x)YBa2Cu3O7-x(ScSr2V3O11),		Y1.04Ba1.84Cu2.28Sc0.01Sr0.17V0.04O7-z	Y	1.04	Ba	1.84	Cu	2.28	Sc	0.01	Sr	0.17	V	0.04									O	7-z		1	1995																												Y123			A			11.672	1											K					108				3																																																																																												BaCO3,SrCO3	1	(1-x)YBa2Cu3O7+x(ScSr2V3O11) and PREPID=20129									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)702-708	K.I.Furaleva,et al.		
20132	SOV0010025	(1-x)YBa2Cu3O7-x(ScSr2V3O11), x=0.10		Y1.04Ba1.75Cu2.79Sc0.01Sr0.27V0.04O7-z	Y	1.04	Ba	1.75	Cu	2.79	Sc	0.01	Sr	0.27	V	0.04									O	7-z		1	1995																												Y123			A			11.667	1											K					91				3																																																																																												BaCO3,SrCO3	1	(1-x)YBa2Cu3O7+x(ScSr2V3O11) and PREPID=20129									Sverkhprovodimost':fizika,khimiya,tekhnika, 8(1995)702-708	K.I.Furaleva,et al.		
20133	JMC0050701		(Hg,Mn)Ba2CuO4	Hg0.8Mn0.2Ba2Cu1O4.2	Hg	0.8	Mn	0.2	Ba	2	Cu	1													O	4+z	4.2		1995																											2	Hg1201				3.89		9.343																91			91																																																																																														BaO,CaO,HgO,MnO2(Nd2O5,GeO2)		mixture-heat in silica tube(800C,12H),for details see PhysicaC,241(1995)1									J.Mater.Chem., 5(1995)701-703			
20134	JMC0050701		(Hg,Nb)Ba2CuO4	Hg0.8Nd0.2Ba2Cu1O4.3	Hg	0.8	Nd	0.2	Ba	2	Cu	1													O	4+z	4.3		1995																											2	Hg1201				3.885		9.461																77			77																																																																																														BaO,CaO,HgO,MnO2(Nd2O5,GeO2)		mixture-heat in silica tube(800C,12H),for details see PhysicaC,241(1995)1									J.Mater.Chem., 5(1995)701-703			
20135	JMC0050701		(Hg,Mn)Ba2CaCu2O6	Hg0.8Mn0.2Ba2Ca1Cu2O6.2	Hg	0.8	Mn	0.2	Ba	2	Ca	1	Cu	2											O	6+z	6.2		1995																											2	Hg1212				3.869		12.48																114			114																																																																																														BaO,CaO,HgO,MnO2(Nd2O5,GeO2)		mixture-heat in silica tube(800C,12H),for details see PhysicaC,241(1995)1									J.Mater.Chem., 5(1995)701-703			
20136	JMC0050701		(Hg,Ge)Ba2CaCu2O6	Hg0.8Ge0.2Ba2Ca1Cu2O6.2	Hg	0.8	Ge	0.2	Ba	2	Ca	1	Cu	2											O	6+z	6.2		1995																											2	Hg1212				3.857		12.599																124			124																																																																																														BaO,CaO,HgO,MnO2(Nd2O5,GeO2)		mixture-heat in silica tube(800C,12H),for details see PhysicaC,241(1995)1									J.Mater.Chem., 5(1995)701-703			
20137	JMC0050701		(Hg,Nd)Ba2Ca2Cu3O8	Hg0.8Nd0.2Ba2Ca2Cu3O8.3	Hg	0.8	Nd	0.2	Ba	2	Ca	2	Cu	3											O	8+z	8.3		1995																												Hg1223				3.852		15.794																128			128																																																																																														BaO,CaO,HgO,MnO2(Nd2O5,GeO2)		mixture-heat in silica tube(800C,12H),for details see PhysicaC,241(1995)1									J.Mater.Chem., 5(1995)701-703			
20138	IEE0430306	T(sub)=690C, single crystal thin film(350nm)	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		5	1995																																															88						88																																												170							2000000																																												17	slectron beam coevaporation,substrate=(100)MgO with butter layer(10-20nm) of MgO, then ANN(500C,1bar,0.5H,in O2 )									IEEE, 43(1995)306-314	A.Porch,et al.		Transactions on Microwave Theory and Technique,
20139	PSS1870067		YSr2(Cu,Al,Mo)3O7	Y1Sr2Cu2.8Al0.1Mo0.1O6+z	Y	1	Sr	2	Cu	2.8	Al	0.1	Mo	0.1											O	6+z		1	1995																											2	Y123				3.802		11.475																18			18																																																																																														Y2O3,SrCO3,Al(OH)3,CuO,MoO3(WO3)	1	mixture-CAL(950C,12-18H)-pellet-heat(980C,16-24H)-ANN(450C,60-72H in O2)					Strong Depression of Superconductivity in Al-Doped YSr2Cu2.8M0.2O6+z (M = Mo, W)				Physica Status Solidi(b), 187(1995) K67-K69	R.Suryanarayanan,et al.		
20140	PSS1870067		YSr2(Cu,Al,W)3O7	Y1Sr2Cu2.8Al0.1W0.1O6+z	Y	1	Sr	2	Cu	2.8	Al	0.1	W	0.1											O	6+z		1	1995																											2	Y123				3.802		11.475																17			17																																																																																														Y2O3,SrCO3,Al(OH)3,CuO,MoO3(WO3)	1	mixture-CAL(950C,12-18H)-pellet-heat(980C,16-24H)-ANN(450C,60-72H in O2)					Strong Depression of Superconductivity in Al-Doped YSr2Cu2.8M0.2O6+z (M = Mo, W)				Physica Status Solidi(b), 187(1995) K67-K69	R.Suryanarayanan,et al.		
20141	PSS1870067		YSr2(Cu,Mo,W)3O7	Y1Sr2Cu2.8Mo0.1W0.1O6+z	Y	1	Sr	2	Cu	2.8	Mo	0.1	W	0.1											O	6+z		1	1995																											2	Y123				3.805		11.52																32			32																																																																																														Y2O3,SrCO3,Al(OH)3,CuO,MoO3(WO3)	1	mixture-CAL(950C,12-18H)-pellet-heat(980C,16-24H)-ANN(450C,60-72H in O2)					Strong Depression of Superconductivity in Al-Doped YSr2Cu2.8M0.2O6+z (M = Mo, W)				Physica Status Solidi(b), 187(1995) K67-K69	R.Suryanarayanan,et al.		
20142	PSS1470119	substrate=(100)SrTiO3,thickness=100nm.	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1995																											3	Y123						11.675													90						90																																																			1000000																																												19	by laserabiation, for details see Physica.C,213(1993)145					Transport characteristics and structural analysis of YBa2Cu3O7-z thin films implanted with argon ions				Physica Status Solidi(a), 147(1995)119-128	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20143	PSS1470119	substrate=(100)SrTiO3, thickness=100nm. Arion fluence=5.0E=11/cm2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1995																											3	Y123						11.675													89						89																																																																																															19	by laserabiation, for details see Physica.C,213(1993)145					Transport characteristics and structural analysis of YBa2Cu3O7-z thin films implanted with argon ions				Physica Status Solidi(a), 147(1995)119-128	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20144	PSS1470119	substrate=(100)SrTiO3 thickness=100nm Arion fluence=5.0E+12/cm2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1995																											3	Y123						11.681													82						82																																																																																															19	bylaser ablation,Ar-ion(100keV) inplantation at RT					Transport characteristics and structural analysis of YBa2Cu3O7-z thin films implanted with argon ions				Physica Status Solidi(a), 147(1995)119-128	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20145	PSS1470119	substrate=(100)SrTiO3, thickness=100nm, Arionfluence=5.0E+13/cm2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1995																											3	Y123						11.75																																																																																																																		19	bylaser ablation,Ar-ion(100keV) inplantation at RT					Transport characteristics and structural analysis of YBa2Cu3O7-z thin films implanted with argon ions				Physica Status Solidi(a), 147(1995)119-128	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20146	PSS1470119	substrate=(100)SrTiO3, thickness=100nm, Arionfluence=1.0E+14/cm2	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7		5	1995																																		11.789																	4																																																																																																	19	by laserabiation, for details see Physica.C,213(1993)145					Transport characteristics and structural analysis of YBa2Cu3O7-z thin films implanted with argon ions				Physica Status Solidi(a), 147(1995)119-128	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20147	PSS1470221		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		2	1995																												Y123																				92				0.2	92																																																		2000000	3000																																												1	standard solid state sintering					Investigations on Flux Creep and Jc(T,B) Behavior in Y1-xEuxBa2Cu3O7-z				Physica Status Solidi(a), 147(1995)221-227	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20148	PSS1470221		(Y,Eu)Ba2Cu3O7	Y0.9Eu0.1Ba2Cu3O7-z	Y	0.9	Eu	0.1	Ba	2	Cu	3													O	7-z		2	1995																												Y123																				92				0.2	92																																																		5000000	1000																																												1	standard solid state sintering					Investigations on Flux Creep and Jc(T,B) Behavior in Y1-xEuxBa2Cu3O7-z				Physica Status Solidi(a), 147(1995)221-227	B.R.Zhao,M.Cai,M.H.Fang,Q.R.Zhang,X.J.Zhang,X.S.Rong,Z.K.Jiao,et al.		
20149	SOV0010022		HoBa2Cu3Oz	Ho1Ba2Cu3Oz	Ho	1	Ba	2	Cu	3															O	z		5	1996																												Y123																				92				3	92																																					calculated from normal resistivity			16		from normal resistivity			690																																		0.07																17	laser evaporation on SrTiO3 sulstrate, c-axis perpendiculer to substrate									Fizika tverdogo tela, 38(1996)1969-1985	N.P.Shabanova,et al.		
20150	SOV0010022		HoBa2Cu3Oz	Ho1Ba2Cu3Oz	Ho	1	Ba	2	Cu	3															O	z		5	1996																												Y123																				50					50																																								9					2600																																		1.1																17	laser evaporation on SrTiO3 sulstrate, c-axis perpendiculer to substrate									Fizika tverdogo tela, 38(1996)1969-1985	N.P.Shabanova,et al.		
20151	SOV0010027	AC resistivity impurity phase=Nd OF,Cu2O	Nd2Cu(O,F)4	Nd2Cu1F0.1O4	Nd	2	Cu	1	F	0.1															O	4		1	1996																											2	T'				3.917		12.09															6				6																																																																																														Nd2O3,CuO,NdOF	1	mixture-press into pellet-ANN(900C; 10-15H in air)-ANN(950-1000C,10-15H in to presence of Ni foil)									Zhurnal neorganicheskoy khimii, 41(1996)889-902	E.E.Fadeeva,et al.		
20152	SOV0010027	AC resistivity	Nd2Cu(O,F)4	Nd2Cu1F0.2O4	Nd	2	Cu	1	F	0.2															O	4		1	1996																											2	T'				3.917		12.09															13				13																																																																																														Nd2O3,CuO,NdOF	1	mixture-press into pellet-ANN(900C; 10-15H in air)-ANN(950-1000C,10-15H in to presence of Ni foil)									Zhurnal neorganicheskoy khimii, 41(1996)889-902	E.E.Fadeeva,et al.		
20153	SOV0010027	AC resistivity	Nd2Cu(O,F)4	Nd2Cu1F0.3O4	Nd	2	Cu	1	F	0.3															O	4		1	1996																											2	T'				3.917		12.09															19				19																																																																																														Nd2O3,CuO,NdOF	1	mixture-press into pellet-ANN(900C; 10-15H in air)-ANN(950-1000C,10-15H in to presence of Ni foil)									Zhurnal neorganicheskoy khimii, 41(1996)889-902	E.E.Fadeeva,et al.		
20154	SOV0010027	AC resistivity	Nd2Cu(O,F)4	Nd2Cu1F0.4O4	Nd	2	Cu	1	F	0.4															O	4		1	1996																											2	T'				3.917		12.09															23				23																																																																																														Nd2O3,CuO,NdOF	1	mixture-press into pellet-ANN(900C; 10-15H in air)-ANN(950-1000C,10-15H in to presence of Ni foil)									Zhurnal neorganicheskoy khimii, 41(1996)889-902	E.E.Fadeeva,et al.		
20155	SOV0010027	AC resistivity	Nd2Cu(O,F)4	Nd2Cu1F0.5O4	Nd	2	Cu	1	F	0.5															O	4		1	1996																											2	T'				3.917		12.09															18				18																																																																																														Nd2O3,CuO,NdOF	1	mixture-press into pellet-ANN(900C; 10-15H in air)-ANN(950-1000C,10-15H in to presence of Ni foil)									Zhurnal neorganicheskoy khimii, 41(1996)889-902	E.E.Fadeeva,et al.		
20156	SOV0010028	whisker	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2.3O8+z	Bi	2	Sr	2	Ca	1	Cu	2.3													O	8+z		6	1996																											3	Bi2212				5.39	5.34	30.62													60						60																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20157	SOV0010028	whisker	Bi2Sr2CaCu2O8	Bi2Sr2Ca1.2Cu3.22O8	Bi	2	Sr	2	Ca	1.2	Cu	3.22													O	8		6	1996																											3	Bi2212																			70						70																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20158	SOV0010028	whisker	Bi2Sr2CaCu2O8	Bi2.13Sr1.21Ca1.32Cu2.22O8+z	Bi	2.13	Sr	1.21	Ca	1.32	Cu	2.22													O	8+z		6	1996																											3	Bi2212																			90						90																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20159	SOV0010028	whisker		Bi2Sr1.37Ca1.31Cu2.22O8+z	Bi	2	Sr	1.37	Ca	1.31	Cu	2.22													O	8+z		6	1996																											3	Bi2212																			85		102				93.5																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20160	SOV0010028	whisker		Bi1.99Sr1.52Ca1.34Cu1.86Pb0.15O8+z	Bi	1.99	Sr	1.52	Ca	1.34	Cu	1.86	Pb	0.15											O	8+z		6	1996																											3	Bi2212																			60						60																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20161	SOV0010028	whisker		Bi2.1Sr1.45Ca1.21Cu2Pb0.09O8+z	Bi	2.1	Sr	1.45	Ca	1.21	Cu	2	Pb	0.09											O	8+z		6	1996																											3	Bi2212																			60						60																																																																																														Bi2O3,SrCO3,CaCO3,CuO		amorphous precursor was prepared by melt-quench method,whisker growth condition(820-860C,50-120H,O2 flow(0,05-0.5l/min))									Zhurnal neorganicheskoykhimii, 41(1996)921-926	T.E.Os'kina,Yu.D.Tret'yakov		
20162	SOV0010030		Bi2(Ba,In)2Cu6O6	Bi2Ba1.8In1.2Cu1O6+z	Bi	2	Ba	1.8	In	1.2	Cu	1													O	6+z		1	1996																											3	Bi2201				4.351	4.634	21.596																95		23	95																																																																																														Bi2O3,BaCO3,CuO,In2O3(PbO,RuO2)	1	mixture-SIN(650C,45H)-grinding-heat(730C,30H in almina crucible-ANN(730C,5H in O2 flow))-FC to RT in O2 flow									Neorganicheskie materialy, 32(1996)851-854	T.N.Kol'tzova,et al.		
20163	SOV0010030		Bi2(Ba,Pb)2CuO6	Bi2Ba1.8Pb0.2Cu1O6+z	Bi	2	Ba	1.8	Pb	0.2	Cu	1													O	6+z		1	1996																											3	Bi2201				4.344	4.616	21.417																95		13	95																																																																																														Bi2O3,BaCO3,CuO,In2O3(PbO,RuO2)	1	mixture-SIN(650C,45H)-grinding-heat(730C,30H in almina crucible-ANN(730C,5H in O2 flow))-FC to RT in O2 flow									Neorganicheskie materialy, 32(1996)851-854	T.N.Kol'tzova,et al.		
20164	SOV0010030		Bi2(Ba,Ru)2CuO6	Bi2Ba1.8Ru0.2Cu1O6+z	Bi	2	Ba	1.8	Ru	0.2	Cu	1													O	6+z		1	1996																																4.316	4.623	21.445																95		4	95																																																																																														Bi2O3,BaCO3,CuO,In2O3(PbO,RuO2)	1	mixture-SIN(650C,45H)-grinding-heat(730C,30H in almina crucible-ANN(730C,5H in O2 flow))-FC to RT in O2 flow									Neorganicheskie materialy, 32(1996)851-854	T.N.Kol'tzova,et al.		
20165	SOV0010030	not S/C	BiBa2CuO6	Bi2Ba2Cu1O6+z	Bi	2	Ba	2	Cu	1															O	6+z		1	1996																											3					4.322	4.642	21.38																																																																																																																	Bi2O3,BaCO3,CuO,In2O3(PbO,RuO2)	1	mixture-SIN(650C,45H)-grinding-heat(730C,30H in almina crucible-ANN(730C,5H in O2 flow))-FC to RT in O2 flow									Neorganicheskie materialy, 32(1996)851-854	T.N.Kol'tzova,et al.		
20166	SOV0010031	Hci(4.2K)=6.3Oe	Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3Oz	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z		1	1996																												Y123																						11			11			K/GPa	6.2									7.4																																																																																			mixture-heat(800C,2H in air)-grinding-heat(955C,5H+650C, 2H in O2 flow)-pellet-SIN(955C,17H in O2 flow)-step cooling (650C,4H+570C,1H+430C,4H+340C,15H)-ANN(400-810C in N2 flow)									Fizika tverdogo tela (Solid State Physics), 38(1996)1998-2011	M.Baran,et al		
20167	SOV0010031		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3Oz	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z		1	1996																												Y123																						42			42			K/GPa	5.4																																																																																												mixture-heat(800C,2H in air)-grinding-heat(955C,5H+650C, 2H in O2 flow)-pellet-SIN(955C,17H in O2 flow)-step cooling (650C,4H+570C,1H+430C,4H+340C,15H)-ANN(400-810C in N2 flow)									Fizika tverdogo tela (Solid State Physics), 38(1996)1998-2011	M.Baran,et al		
20168	SOV0010031		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3Oz	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z			1996																												Y123																						47			47			K/GPa	5.3									210																																																																																			mixture-heat(800C,2H in air)-grinding-heat(955C,5H+650C, 2H in O2 flow)-pellet-SIN(955C,17H in O2 flow)-step cooling (650C,4H+570C,1H+430C,4H+340C,15H)-ANN(400-810C in N2 flow)									Fizika tverdogo tela (Solid State Physics), 38(1996)1998-2011	M.Baran,et al		
20169	SOV0010031		Y(Ba,Sr)2Cu3Oz	Y1Ba1.5Sr0.5Cu3Oz	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	z			1996																												Y123																						90			90			K/GPa	2									560																																																																																			mixture-heat(800C,2H in air)-grinding-heat(955C,5H+650C, 2H in O2 flow)-pellet-SIN(955C,17H in O2 flow)-step cooling (650C,4H+570C,1H+430C,4H+340C,15H)-ANN(400-810C in N2 flow)									Fizika tverdogo tela (Solid State Physics), 38(1996)1998-2011	M.Baran,et al		
20170	SOV0010032	R is not zero at 4.2K	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.63	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.63	1	1996																												Y123																					18	18			18			K/GPa	6.6																																																																																										Gd2O3,CuO, Ba(NO3)2,Sr(NO3)2	1	mixture-heat(900-950C,in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(1K/min)-ANN(400-810C,in N2 flow for Oz control)									Fizika tverdogo tela, 38(1996)827-838	V.P.Diakonov,et al.		
20171	SOV0010032	Hci(4.2K)=250Oe	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.72	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.72	1	1996																												Y123																					32	32			32			K/GPa	5.8								deviation from linearity in M-H curve	254																																																																																	Gd2O3,CuO, Ba(NO3)2,Sr(NO3)2	1	mixture-heat(900-950C,in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(1K/min)-ANN(400-810C,in N2 flow for Oz control)									Fizika tverdogo tela, 38(1996)827-838	V.P.Diakonov,et al.		
20172	SOV0010032	Hci(4.2K)=500Oe	Gd(Ba,Sr)2Cu3Oz	Gd1Ba1.5Sr0.5Cu3O6.93	Gd	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.93	1	1996																												Y123																					82	82			82			K/GPa	2								deviation from linearity in M-H curve	501																																																																																	Gd2O3,CuO, Ba(NO3)2,Sr(NO3)2	1	mixture-heat(900-950C,in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(1K/min)-ANN(400-810C,in N2 flow for Oz control)									Fizika tverdogo tela, 38(1996)827-838	V.P.Diakonov,et al.		
20173	SOV0010032		Gd(Ba,Sr)2Cu3Oz	Gd1Ba1Sr1Cu3O6.77	Gd	1	Ba	1	Sr	1	Cu	3													O	7-z	6.77	1	1996																												Y123																					4	4			4																																																																																														Gd2O3,CuO, Ba(NO3)2,Sr(NO3)2	1	mixture-heat(900-950C,in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(1K/min)-ANN(400-810C,in N2 flow for Oz control)									Fizika tverdogo tela, 38(1996)827-838	V.P.Diakonov,et al.		
20174	SOV0010032		Gd(Ba,Sr)2Cu3Oz	Gd1Ba1Sr1Cu3O6.93	Gd	1	Ba	1	Sr	1	Cu	3													O	7-z	6.93	1	1996																												Y123																					83	83			83			K/GPa	5.8																																																																																										Gd2O3,CuO, Ba(NO3)2,Sr(NO3)2	1	mixture-heat(900-950C,in O2 flow)-pellet-SIN(955C,12H in O2 flow)-cool to RT(1K/min)-ANN(400-810C,in N2 flow for Oz control)									Fizika tverdogo tela, 38(1996)827-838	V.P.Diakonov,et al.		
20175	SOV0010034		Y(Ba,La)2Cu3Oz	Y1Ba1.5La0.5Cu3O7.22	Y	1	Ba	1.5	La	0.5	Cu	3													O	7+z	7.22	1	1995																												Y123																			32			36.6		17.2	36.6																																																																			40.5																												1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20176	SOV0010034		(Y,Ca)(Ba,La)2Cu3Oz	Y0.9Ca0.1Ba1.5La0.5Cu3O7.19	Y	0.9	Ca	0.1	Ba	1.5	La	0.5	Cu	3											O	7+z	7.19	1	1995																												Y123																			51.7			57.9		14.2	57.9																																																																			21			TP20176																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20177	SOV0010034		(Y,La)(Ba,La)2Cu3Oz	Y0.8Ca0.2Ba1.5La0.5Cu3O7.13	Y	0.8	Ca	0.2	Ba	1.5	La	0.5	Cu	3											O	7+z	7.13	1	1995																												Y123																			67.9			73		9.7	73																																																																			19.2			TP20177																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20178	SOV0010034		(Y,Ca)(Ba,La)2Cu3Oz	Y0.6Ca0.4Ba1.5La0.5Cu3O7.01	Y	0.6	Ca	0.4	Ba	1.5	La	0.5	Cu	3											O	7+z	7.01	1	1995																												Y123																			80.2			82.4		4.2	82.4																																																																			6.2			TP20178																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20179	SOV0010034		(Y,Ca)(Ba,La)2Cu3Oz	Y0.5Ca0.5Ba1.5La0.5Cu3O6.96	Y	0.5	Ca	0.5	Ba	1.5	La	0.5	Cu	3											O	7+z	6.96	1	1995																												Y123																			78.9			82.5		2.1	82.5																																																																			4.2			TP20179																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20180	SOV0010034		YBa2(Cu,Co)3O7	Y1Ba2Cu2.75Co0.25O7.06	Y	1	Ba	2	Cu	2.75	Co	0.25													O	7+z	7.06	1	1995																												Y123																			60.2			66.2		19.1	66.2																																																																			33			TP20180																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20181	SOV0010034		(Y,Ca)Ba2(Cu,Co)3O7	Y0.95Ca0.05Ba2Cu2.75Co0.25O7.06	Y	0.95	Ca	0.05	Ba	2	Cu	2.75	Co	0.25											O	7+z	7.06	1	1995																												Y123																			67.9			75.1		8.6	75.1																																																																			29			TP20181																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20182	SOV0010034		(Y,Ca)Ba2(Cu,Co)3O7	Y0.9Ca0.1Ba2Cu2.75Co0.25O7.03	Y	0.9	Ca	0.1	Ba	2	Cu	2.75	Co	0.25											O	7+z	7.03	1	1995																												Y123																			71.9			76.9		8	76.9																																																																			19.5			TP20182																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20183	SOV0010034		(Y,Ca)Ba2(Cu,Co)3O7	Y0.85Ca0.15Ba2Cu2.75Co0.25O7.01	Y	0.85	Ca	0.15	Ba	2	Cu	2.75	Co	0.25											O	7+z	7.01	1	1995																												Y123																			77.9			80.6		5.4	80.6																																																																			10.8			TP20183																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20184	SOV0010034		(Y,Ca)Ba2(Cu,Co)3O7	Y0.8Ca0.2Ba2Cu2.75Co0.25O7.01	Y	0.8	Ca	0.2	Ba	2	Cu	2.75	Co	0.25											O	7+z	7.01	1	1995																												Y123																			78.6			82.2		4	82.2																																																																			7.7			TP20184																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20185	SOV0010034		(Y,Ca)Ba2(Cu,Co)3O7	Y0.75Ca0.25Ba2Cu2.75Co0.25O6.98	Y	0.75	Ca	0.25	Ba	2	Cu	2.75	Co	0.25											O	7+z	6.98	1	1995																												Y123																			80.6			82.4		3.6	82.4																																																																			5.1			TP20185																									1	mixture-SIN(950C)-pellet-ANN(920-950C)-ANN(450C,in O2 flow)-slow cooling to RT									Fizika tverdogo tela, 37(1995)1990-2001	E.V.Vladimirskaya,et al.		
20186	SOV0010035		BiSr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1995																												Bi2212																			60			61		4	61																																																																			-3.8			TP20186												1.9														mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20187	SOV0010035		(Bi,Pb)2Sr2CaCu2O8	Bi1.34Pb0.66Sr2Ca1Cu2Oz	Bi	1.34	Pb	0.66	Sr	2	Ca	1	Cu	2											O	z		1	1995																												Bi2212																			71.2			72.2		3.5	72.2																																																																			-2.8			TP20187												2														mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20188	SOV0010035		(Bi,Pb)2Sr2CaCu2O8	Bi1.86Pb0.14Sr2Ca1Cu2Oz	Bi	1.86	Pb	0.14	Sr	2	Ca	1	Cu	2											O	z		1	1995																												Bi2212																			61			65		5.5	65																																																																			-5.3															0.83														mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20189	SOV0010035		(Bi,Pb)2Sr2CaCu2O8	Bi1.8Pb0.2Sr2Ca1Cu2Oz	Bi	1.8	Pb	0.2	Sr	2	Ca	1	Cu	2											O	z		1	1995																												Bi2212																			56.3			60.7		7.2	60.7																																																																			-5.5			TP20189												1.3														mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20190	SOV0010035		(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.34Pb0.66Sr2Ca2Cu3Oz	Bi	1.34	Pb	0.66	Sr	2	Ca	2	Cu	3											O	z		1	1995																												Bi2223																			99			108.9		7.6	108.9																																																																			1.9			TP20190												1.7														mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20191	SOV0010035		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2Oz	Bi	2	Sr	2	Ca	1	Cu	2													O	z		1	1995																												Bi2212																			74.2			84.2			84.2																																																																			-3.8															2.5				0.0000000016										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20192	SOV0010035		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.9Nd0.1Cu2Oz	Bi	2	Sr	2	Ca	0.9	Nd	0.1	Cu	2											O	z		1	1995																												Bi2212																			73.3			83.3			83.3																																																																			-2															2.6				0.0000000025										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20193	SOV0010035		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.8Nd0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Nd	0.2	Cu	2											O	z		1	1995																												Bi2212																			71.2			82			82																																																																			3.9															2.9				0.0000000039										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20194	SOV0010035		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.7Nd0.3Cu2Oz	Bi	2	Sr	2	Ca	0.7	Nd	0.3	Cu	2											O	z		1	1995																												Bi2212																			67			80.2			80.2																																																																			7.9															3.5				0.0000000065										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20195	SOV0010035		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.6Nd0.4Cu2Oz	Bi	2	Sr	2	Ca	0.6	Nd	0.4	Cu	2											O	z		1	1995																												Bi2212																			54.4			68.6			68.6																																																																			18.2															5.5				0.0000000088										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20196	SOV0010035		Bi2Sr2(Ca,Nd)Cu2O8	Bi2Sr2Ca0.5Nd0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Nd	0.5	Cu	2											O	z		1	1995																												Bi2212																			29			42.4			42.4																																																																			27.5															11.7				0.0000000112										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20197	SOV0010035		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2Oz	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	z		1	1995																												Bi2212																			66.9			78.9			78.9																																																																			-3.5			TP20197												3.1				0.0000000028										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20198	SOV0010035		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2Oz	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	z		1	1995																												Bi2212																			64.2			76.2			76.2																																																																			3.1			TP20198												3.8				0.0000000042										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20199	SOV0010035		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2Oz	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	z		1	1995																												Bi2212																			53.3			70.5			70.5																																																																			12.6			TP20199												5.3				0.0000000065										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20200	SOV0010035		Bi2Sr2(Ca,Y)Cu28	Bi2Sr2Ca0.6Y0.4Cu2Oz	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	z		1	1995																												Bi2212																			34.3			53.1			53.1																																																																			28			TP20200												7.7				0.0000000101										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20201	SOV0010035		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.5Y0.5Cu2Oz	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	2											O	z		1	1995																												Bi2212																			12.2			31.5			31.5																																																																			40.3			TP20201												12.5				0.0000000128										mixture-CAL-SIN(750C)-press into pellet-ANN(850-860C)									Fizika tverdogo tela, 37(1995)2152-2162	N.V.Ageyev,et al.		
20202	SOV0010036	super structure was detected	YBa2Cu3O7	Y1Ba1.8Cu3Oz	Y	1	Ba	1.8	Cu	3															O	z			1997																											3	Y123	Pmmm			3.822	3.894	11.674																94		3	94																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskiematerialy, 33(1997)728-731	T.N.Kol'tsova,et al.		
20203	SOV0010036	super structure was detected	YBa2Cu3O7	Y1Ba1.9Cu3Oz	Y	1	Ba	1.9	Cu	3															O	z			1997																											3	Y123	Pmmm			3.816	3.887	11.623																96		3	96																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskiematerialy, 33(1997)728-731	T.N.Kol'tsova,et al.		
20204	SOV0010036	super structure was detected	YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			1997																											3	Y123	Pmmm			3.817	3.889	11.667																97		7	97																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskiematerialy, 33(1997)728-731	T.N.Kol'tsova,et al.		
20205	SOV0010036	super structure was detected	YBa2Cu3O7	Y1Ba2.1Cu3Oz	Y	1	Ba	2.1	Cu	3															O	z			1997																											3	Y123	Pmmm			3.818	3.886	11.627																96		9	96																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskiematerialy, 33(1997)728-731	T.N.Kol'tsova,et al.		
20206	SOV0010036	super structure was detected	YBa2Cu3O7	Y1Ba2.2Cu3Oz	Y	1	Ba	2.2	Cu	3															O	z			1997																											3	Y123	Pmmm			3.83	3.891	11.682																96		11	96																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskiematerialy, 33(1997)728-731	T.N.Kol'tsova,et al.		
20207	SOV0010037	super structure was detected	YBa2Cu3O7	Y0.8Ba2Cu3O6.44	Y	0.8	Ba	2	Cu	3															O	z	6.44	1	1997																											3	Y123	Pmmm			3.818	3.883	11.629																96		5.5	96																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskie materialy, 33(1997)732-736	T.N.Kol'tsova,et al.		
20208	SOV0010037	super structure was detected	YBa2Cu2Cu3O7	Y0.9Ba2Cu3O6.58	Y	0.9	Ba	2	Cu	3															O	z	6.58	1	1997																											3	Y123	Pmmm			3.817	3.881	11.639																93.4		4.2	93.4																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskie materialy, 33(1997)732-736	T.N.Kol'tsova,et al.		
20209	SOV0010037	super structure was detected	YBa2Cu3O7	Y1Ba2Cu3O6.69	Y	1	Ba	2	Cu	3															O	z	6.69	1	1997																											3	Y123	Pmmm			3.817	3.889	11.667																97		2	97																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskie materialy, 33(1997)732-736	T.N.Kol'tsova,et al.		
20210	SOV0010037	super structure was detected	YBa2Cu3O7	Y1.1Ba2Cu3O6.87	Y	1.1	Ba	2	Cu	3															O	z	6.87	1	1997																											3	Y123	Pmmm			3.819	3.889	11.667																95.9		4.5	95.9																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskie materialy, 33(1997)732-736	T.N.Kol'tsova,et al.		
20211	SOV0010037	super structure was detected	YBa2Cu3O7	Y1.2Ba2Cu3O6.98	Y	1.2	Ba	2	Cu	3															O	z	6.98	1	1997																											3	Y123	Pmmm			3.827	3.894	11.756																93.4		2.4	93.4																																																																																															1	mixture-SIN(700C,7H)-grinding-(900C,45H)-slow-cool(from 900 to 50C,16H), all process in air									Neorganicheskie materialy, 33(1997)732-736	T.N.Kol'tsova,et al.		
20212	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2Oz	Pb0.63Cu0.27Sr2Y0.79Ca0.21Cu2Oz	Pb	0.63	Cu	0.27	Sr	2	Y	0.79	Ca	0.21	Cu	2									O	z		1	1997																												1212				3.821		11.841																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20213	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2Oz	Pb0.63Cu0.27Sr1.9Ca0.31Y0.79Cu2Oz	Pb	0.63	Cu	0.27	Sr	1.9	Ca	0.31	Y	0.79	Cu	2									O	z		1	1997																												1212				3.821		11.839																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20214	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2Oz	Pb0.63Cu0.27Sr1.8Ca0.41Y0.79Cu2Oz	Pb	0.63	Cu	0.27	Sr	1.8	Ca	0.41	Y	0.79	Cu	2									O	z		1	1997																												1212				3.82		11.835																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20215	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2O	Pb0.63Cu0.27Sr1.7Ca0.51Y0.79Cu2Oz	Pb	0.63	Cu	0.27	Sr	1.7	Ca	0.51	Y	0.79	Cu	2									O	z		1	1997																												1212				3.82		11.832																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20216	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2Oz	Pb0.63Cu0.27Sr1.6Ca0.61Y0.79Cu2Oz	Pb	0.63	Cu	0.27	Sr	1.6	Ca	0.61	Y	0.79	Cu	2									O	z		1	1997																												1212				3.819		11.83																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20217	SOV0010043	Superconductor	(Pb,Cu)(Sr,Ca)2(Y,Ca)CuOz	Pb0.63Cu0.27Sr1.5Ca0.71Y0.79Cu2Oz	Pb	0.63	Cu	0.27	Sr	1.5	Ca	0.71	Y	0.79	Cu	2									O	z		1	1997																												1212				3.819		11.828																																																																																																																	PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20218	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.9Cd0.1Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.9	Cd	0.1	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.819		11.871													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20219	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.8Cd0.2Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.8	Cd	0.2	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.817		11.904													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20220	SOV0010043	Superconductor	(Pb,cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.75Cd0.25Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.75	Cd	0.25	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.816		11.917													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20221	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.7Cd0.3Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.7	Cd	0.3	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.815		11.928													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20222	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr0.65Cd0.35Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	0.65	Cd	0.35	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.814		11.938													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20223	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.6Cd0.4Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.6	Cd	0.4	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.813		11.944													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20224	SOV0010043	Superconductor	(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.5Cd0.5Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.5	Cd	0.5	Y	0.79	Ca	0.21									O	z		1	1997																												1212				3.812		11.952													35		55				45																																																																																														PbO,SrCO3,CaCO3,Y2O3,CuO,(CdO)	1	precursor(without Pb)-qrinding under acetine-heat(760C,12H in air)-mix with Pb-fire(800C,10H+910C,40H)									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20225	SOV0010043	TK 4K	(Pb,Cu)Sr2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr2Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	2	Y	0.79	Ca	0.21											O	z		3	1997																												1212				3.82		11.84													4		65				34.5																																																																																																See J.Cryst.Growth 126(1993)471, melt in Pt crucible-heat(1000-1020C)-slow cool (0.5C/H) to 950C									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20226	SOV0010043	Tl<4K	(Pb,Cu)(Sr,Ca)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.79Ca0.21Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.79	Ca	0.21	Y	0.79	Ca	0.21									O	z		3	1997																											2	1212				3.819		11.834													4		65				34.5																																																																																																See J.Cryst.Growth 126(1993)471, melt in Pt crucible-heat(1000-1020C)-slow cool (0.5C/H) to 950C									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20227	SOV0010043		(Pb,Cu)(Sr,Cd)2(Y,Ca)Cu2Oz	Pb0.63Cu2.27Sr1.79Cd0.21Y0.79Ca0.21Oz	Pb	0.63	Cu	2.27	Sr	1.79	Cd	0.21	Y	0.79	Ca	0.21									O	z		3	1997																											2	1212				3.815		11.905													52		81				66.5																																																																																																See J.Cryst.Growth 126(1993)471, melt in Pt crucible-heat(1000-1020C)-slow cool (0.5C/H) to 950C									Zurnal neorganisheskoy khimii, 42(1997)181-183	A.L.Morz,S.A.Nedilko	Pb,Cu,Sr,Y,Ca,O	
20228	SOV0010042	dielectric	(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		1	1997																												T																																																																																	mJ/K2fu	4.3																																						1										Fizika tverdogo tela, 39(1997)1000-1004	K.A.Kvavadze,et al	La,Sr,Cu,O,Ba	
20229	SOV0010042		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1997																												T																																																																																	mJ/K2fu	2																																						1										Fizika tverdogo tela, 39(1997)1000-1004	K.A.Kvavadze,et al	La,Sr,Cu,O,Ba	
20230	SOV0010042		(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4		1	1997																												T																																																																																	mJ/K2fu	3.2																																						1										Fizika tverdogo tela, 39(1997)1000-1004	K.A.Kvavadze,et al	La,Sr,Cu,O,Ba	
20231	SOV0010042		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1997																												T																																																																																	mJ/K2fu	4.4																																						1										Fizika tverdogo tela, 39(1997)1000-1004	K.A.Kvavadze,et al	La,Sr,Cu,O,Ba	
20232	SOV0010039		HgBa2CuO4	Hg1Ba2Cu1O4.01	Hg	1	Ba	2	Cu	1															O	4	4.01	1	1997																												Hg1201	P4/mmm			3.892		9.529	3															61			61																																																																																																see Physica C,271(1996)197, heat(800C,12H)-cool to 650C(1.5C/min)-Q to mater-heat(330C,18H in 1.0E-2 torr)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20233	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																												Hg1201	P4/mmm			3.883	9.523		3															97			97																																																																																																fluorination F Hg1201 : XeF2=1 : 0.1-heat(150C,15H in N2-filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20234	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																												Hg1201	P4/mmm			3.881		9.511	3															97			97																																																																																																fluorination=Hg1201 : XeF2=1 :0.3-heat(200C,15H in N2-filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20235	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																												Hg1201	P4/mmm			3.876		9.494	3															96			96																																																																																																fluorination=Hg1201 : XeF2=1 : 0.5-heat(200C,15H in N2-filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20236	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																											2	Hg1201	P4/mmm			3.873		9.489	3															90			90																																																																																																fluorination=reduced Hg1201 : XeF2=1 : 0.4,-heat(200C,20H in N2 filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20237	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																											2	Hg1201	P4/mmm			3.872		9.482	3															88			88																																																																																																fluorination=reduced Hg1201 : XeF2=1 : 0.3-heat(200C, 30H in N2filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20238	SOV0010039		HgBa2CuO4Fx	Hg1Ba2Cu1FO4	Hg	1	Ba	2	Cu	1	F														O	4		1	1997																											2	Hg1201	P4/mmm			3.868		9.459	3															78			78																																																																																																fluorination=reduced Hg1201 : XeF2=1 : 1-heat(200C,50H in N2-filled tube)									preprint JINR E14-97-234(1997)	A.M.Abakumov,et al.		Joint Institute of Nuclear Research, Dubna, Moscow Region
20239	SOV0010041	Spheat(P=1 : H=O, H//c-axis, P=2 : H=8T, H//c-axis, P=3 : H=0,H//ab, P=4 : H=8T, H//ab), y=(C-Cb)/T, where Cb is normal state specific heat calculated by LSM. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1997																											2	T				3.773		13.233													39.2			39.2		0.5	39.2																				T	resistive transitin 50%,linear extraporation		120	40								4.37	1.45																																																		6	30											7	Zone melting by rediation heating.,See Physica C,256(1996)371									Zhurnal experimental'noy i teoreticheskoy fiziki, 112(1997)1386-1395	M.N.Chlopkin,et al.		
20240	SOV0010047		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95	1	1998																											3	Y123				3.822	3.885	11.67													87.3		89.7			3	88.5																																																																		micro.V/K	0.8											1.7				3.8													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20241	SOV0010047		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3O6.98	Y	1	Ba	1.95	La	0.05	Cu	3													O	z	6.98	1	1998																											3	Y123				3.82	3.894	11.655													88.8		89.8			1.1	89.3																																																																			1.3											1.5				3.5													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20242	SOV0010047		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O6.99	Y	1	Ba	1.9	La	0.1	Cu	3													O	z	6.99	1	1998																											3	Y123				3.823	3.895	11.65													89.5		91.2			3.2	90.35																																																																			6.3											0.7				1.6													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20243	SOV0010047		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O7.03	Y	1	Ba	1.8	La	0.2	Cu	3													O	z	7.03	1	1998																											3	Y123				3.819	3.89	11.65													86.9		90.5			5.8	88.7																																																																			9.3											1.4				2.9													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20244	SOV0010047		Y(ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3O7.1	Y	1	Ba	1.7	La	0.3	Cu	3													O	z	7.1	1	1998																											3	Y123				3.838	3.879	11.64													76.8		84.2			8.7	80.5																																																																			16.6											2.1				4.2													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20245	SOV0010047		Y(Ba,La)2Cu3)7	Y1Ba1.6La0.4Cu3O7.14	Y	1	Ba	1.6	La	0.4	Cu	3													O	z	7.14	1	1998																											2	Y123				3.857		11.6													62.8		73.5			10.9	68.15																																																																			18.5											1.5				2.9													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20246	SOV0010047		Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3O7.17	Y	1	Ba	1.5	La	0.5	Cu	3													O	z	7.17	1	1998																											2	Y123				3.853		11.58													50.9		57.3			11.6	54.1																																																																			39.7											2.8				4.8													1	ANN(450C,2H in O2 flow)-slow cooling to RT (2C/min)									Fizika tverdogo tela (Solid State Physics) 40(1998)17	V.E.Gasumiants,et al	Y,Ba,La,Cu,O	
20247	SOV0010048		YBa2Cu3O7	Y1Ba2Cu3O6.965	Y	1	Ba	2	Cu	3															O	z	6.965	1	1997																											3	Y123				3.815	3.881	11.667													88.5						88.5																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20248	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O6.965	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.822	3.883	11.684													88						88																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20249	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O6.965	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.823	3.89	11.67													85						85																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20250	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O6.965	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.826	3.895	11.674													70						70																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20251	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.965	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.831	3.897	11.666													55						55																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20252	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.965	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.836	3.899	11.667													35						35																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20253	SOV0010048		(Y,Pr)ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O6.965	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.838	3.908	11.675													10						10																																																																																														Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20254	SOV0010048		(Y,Pr)Ba2Cu3O7	Y0.4Pr0.6Ba2Cu3O6.965	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	z	6.965	1	1997																											3	Y123				3.846	3.911	11.686																	4.2																																																																																																Y2O3, CuO, Ba2CO3, Pr2O3	1	mixture-pellet (500MPa)-heat(900-950C, in air)-ANN(450C,2H in O2 flow)-slow cool to RT									Fizika tverdogo tela (Solid State Physics) 39(1997)1520-1525	V.E.Gasumiants,et al	Y,Pr,Ba,Cu,O	
20255	SOV0010049		YBa2Cu3O7	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		1	1997																											3	Y123				3.824	3.891	11.667														90					90		3																																																																																													11	Sol-gel method with ethylenglycol as gel, SIN(940C,2H in O2)-ANN(910C,20H)-slow cool to 20C(17H)									Zhurnal technicheskoy fiziki , 67(1997)31-34	T.V.Kratchino,et al		
20256	SOV0010049	unknown phases exist	YBa2Cu3O7	Y1Ba2Cu2.85Au0.15Oz	Y	1	Ba	2	Cu	2.85	Au	0.15													O	z		1	1997																											3	Y123				3.822	3.899	11.705														90					90		3																																																																																													11	Sol-gel method with ethylenglycol as gel, SIN(940C,2H in O2)-ANN(910C,20H)-slow cool to 20C(17H)									Zhurnal technicheskoy fiziki , 67(1997)31-34	T.V.Kratchino,et al		
20257	SOV0010049		YBa2Cu3O7	Y1Ba2Cu2.7Au0.3Oz	Y	1	Ba	2	Cu	2.7	Au	0.3													O	z		1	1997																											3	Y123				3.821	3.901	11.734														88					88		3																																																																																													11	Sol-gel method with ethylenglycol as gel, SIN(940C,2H in O2)-ANN(910C,20H)-slow cool to 20C(17H)									Zhurnal technicheskoy fiziki , 67(1997)31-34	T.V.Kratchino,et al		
20258	SOV0010050	main phase=Bi2212, minor=Bi2223, inprity=Bi2201, Ca2PbO4, LAT and Tc, for Bi2223, Jc77=16.7A		Bi1.7Pb0.3Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	z		2	1996																											2	Bi2223				5.391		36.826													105.1		112				108.55																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20259	SOV0010050	main=Bi2212, minor=Bi2223, LAT and Tc for Bi2223, Jc77=56.0A		Bi1.7Pb3Sr2Ca2Cu3Cs0.1Oz	Bi	1.7	Pb	3	Sr	2	Ca	2	Cu	3	Cs	0.1									O	z		2	1996																											2	Bi2223				5.405		36.938													106.1		112				109.05																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20260	SOV0010050	mixture of Bi2212 and Bi2223, LAT and Tc for Bi2223, Jc77=60.9A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.2Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.2									O	z		2	1996																											2	Bi2223				5.403		37.112													105.3		112				108.65																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20261	SOV0010050	mixture of Bi2212 and Bi2223, LAT and Tc for Bi2223, Jc77=60.9A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.3									O	z		2	1996																											2	Bi2223				5.398		37.062													106		112				109																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20262	SOV0010050	practically single phase, Jc77=48.0A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.4Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.4									O	z		1	1996																											2	Bi2223				5.385		37													102.6		112				107.3																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20263	SOV0010050	practically single phase, Jc77=36.0A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.5Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.5									O	z		1	1996																											2	Bi2223				5.387		37.042													105.1		112				108.55																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20264	SOV0010050	practically single phase, Jc77=48.0A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.6Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.6									O	z		1	1996																											2	Bi2223				5.387		37.018													104		112				108																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20265	SOV0010050	practically single phase, Jc77=128.0A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.7Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.7									O	z		1	1996																											2	Bi2223				5.393		37.062													105.9		112				108.95																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20266	SOV0010050	practically single phase, Jc77=41.7A		Bi1.7Pb0.3Sr2Ca2Cu3Cs0.8Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.8									O	z		1	1996																												Bi2223				5.382		36.959													105		112				108.5																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20267	SOV0010050	minor single phase, Jc77=36.0A		Bi0.7Pb0.3Sr2Ca2Cu3Cs0.9Oz	Bi	0.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	0.9									O	z		2	1996																												Bi2223				5.39		37													105.9		112				108.95																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20268	SOV0010050	minor phase=Bi2212, Jc77=26.9A		Bi1.7Pb0.3Sr2Ca2Cu3Cs1Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3	Cs	1									O	z		2	1996																												Bi2223				5.393		37.055													105		112				108.5																																																																																														Pb,Cu,Bi-oxide,Ca,Sr-cosbonate	1	CAL(770-860C, in air)-several step annealing									Pis'ma v Zhurnal Technicheskoy Fiziki, 22(1996)48-53	V.V.Petrashiko,V.V.Petrashko,et al,et al.	Bi,Sr,Ca,Cu,O,Pb,Cs	
20269	SOV0010117		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1995																											3	Y124	Ammm			3.839	3.869	27.343													80						80																																																																																														Y2O3, BaCu2O3	1	mixture-SIN(1085K, in O2 flow), see Physica C 182(1991)67									Philosoph. Mag. B, 71(1995)1137-1143	I.K.Gopalakrishnan,et al	Y,Ba,Cu,O,Ce	
20270	SOV0010117		(Y,Ce,Ca)Ba2Cu4O8	Y0.8Ce0.1Ca0.1Ba2Cu4O8	Y	0.8	Ce	0.1	Ca	0.1	Ba	2	Cu	4											O	8		1	1995																											3	Y124	Ammm			3.841	3.87	27.188													63						63																																																																																														Y2O3, BaCu2O3, CeO2, Ca(NO3)	1	mixture-SIN(1085K, in O2 flow), see Physica C 182(1991)67 4H2O									Philosoph. Mag. B, 71(1995)1137-1143	I.K.Gopalakrishnan,et al	Y,Ba,Cu,O,Ce	
20271	SOV0010125	semiconductor, not s/c	(Cd,Fe)Sr2YCu2O7	Cd0.5Fe0.5Sr2Y1Cu2O7-z	Cd	0.5	Fe	0.5	Sr	2	Y	1	Cu	2											O	7-z		1	1995																											2	1212	P4/mmm			3.809		11.423																																																																																																																	CdO, SrCO3, Y2O3, CuO, Fe2O3(Co2O3)		mixture-heat(840C,24H in air)-pellet-SIN(920C,40H in air)-FC									Physica Status Solidi(a), 152(1995)355-359	W.J.Yu,et al.		
20272	SOV0010125	semiconductor, not s/c	(Cd,Co)Sr2YCu2O7	Cd0.5Co0.5Sr2Y1Cu2O7-z	Cd	0.5	Co	0.5	Sr	2	Y	1	Cu	2											O	7-z		1	1995																											2	1212	P4/mmm			3.816		11.435																																																																																																																	CdO, SrCO3, Y2O3, CuO, Fe2O3(Co2O3)		mixture-heat(840C,24H in air)-pellet-SIN(920C,40H in air)-FC									Physica Status Solidi(a), 152(1995)355-359	W.J.Yu,et al.		
20273	SOV0010119	Hg1223>75% volume, inpurity phase=CaHgO2,Hg1234, Ba2Ca2Cu3Oz	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8.28	Hg	1	Ba	2	Ca	2	Cu	3													O	8	8.28	2	1995																											2	Hg1223	P4/mmm			3.852		15.842													118		119				118.5																																																																																														BaO, CaO, CuO, HgO		precursor(Ba2Ca2Cu3Oz)+HgO, ANN(750C,10H)-rapid cool to RT(5min)									Physica Status Solidi(a), 152(1995)477-483	X.S.Wu,et al.		
20274	SOV0010119	Hg1223>75% volume,inpurity phase=CaHgO2,Hg1234,Ba2Ca2Cu3Oz	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8.35	Hg	1	Ba	2	Ca	2	Cu	3													O	8	8.35	2	1995																											2	Hg1223	P4/mmm			3.852		15.842													133		135				134																																																																																														BaO, CaO, CuO, HgO		precursor(Ba2Ca2Cu3Oz)+ HgO, ANN(300C,8H in O2 flow)-vapid cool to RT									Physica Status Solidi(a), 152(1995)477-483	X.S.Wu,et al.		
20275	SOV0010120	TC by AC Susceptibility	(Nd,Pr)Ba2Cu3O7	Nd0.7Pr0.3Ba2Cu3O6.95	Nd	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.95	1	1995																											3	Y123				3.876	3.964	11.789	3																5																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20276	SOV0010120	TC by AC Susceptibility	(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.85Sr0.15Cu3Oz	Nd	0.7	Pr	0.3	Ba	1.85	Sr	0.15	Cu	3											O	z		1	1995																											3	Y123				3.874	3.961	11.782	3																5																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20277	SOV0010120	TC by AC Susceptibility	(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.75Sr0.25Cu3Oz	Nd	0.7	Pr	0.3	Ba	1.75	Sr	0.25	Cu	3											O	z		1	1995																											3	Y123				3.867	3.951	11.749	3															24			24																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20278	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.5Sr0.5Cu3Oz	Nd	0.7	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3											O	z		1	1995																											3	Y123				3.884	3.925	11.733	3															26			26																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20279	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.25Sr0.75Cu3Oz	Nd	0.7	Pr	0.3	Ba	1.25	Sr	0.75	Cu	3											O	z		1	1995																											2	Y123				3.903		11.731	3															27			27																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20280	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.15Sr0.85Cu3Oz	Nd	0.7	Pr	0.3	Ba	1.15	Sr	0.85	Cu	3											O	z		1	1995																											2	Y123				3.899		11.69	3															29			29																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20281	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1Sr1Cu3O6.87	Nd	0.7	Pr	0.3	Ba	1	Sr	1	Cu	3											O	z	6.87	1	1995																											2	Y123				3.901		11.674	3															34			34																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-ANN(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20282	SOV0010120		(Nd,Pr)BaCu3O7	Nd0.7Pr0.3Ba2Cu3O6.95	Nd	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.95	1	1995																											3	Y123				3.866	3.957	11.757	3																5																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20283	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.85Sr0.15Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1.85	Sr	0.15	Cu	3											O	7-z		1	1995																											3	Y123				3.865	3.954	11.755	3																5																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20284	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.75Sr0.25Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1.75	Sr	0.25	Cu	3											O	7-z		1	1995																											3	Y123				3.863	3.95	11.742	3																26																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20285	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.5Sr0.5Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3											O	7-z		1	1995																											3	Y123				3.88	3.929	11.73	3																29																																																																																																Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20286	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.25Sr0.75Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1.25	Sr	0.75	Cu	3											O	7-z		1	1995																											3	Y123				3.887	3.905	11.71	3															34			34																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20287	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1.15Sr0.85Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1.15	Sr	0.85	Cu	3											O	7-z		1	1995																											2	Y123				3.891		11.701	3															38			38																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20288	SOV0010120		(Nd,Pr)(Ba,Sr)2Cu3O7	Nd0.7Pr0.3Ba1Sr1Cu3O7-z	Nd	0.7	Pr	0.3	Ba	1	Sr	1	Cu	3											O	7-z		1	1995																											2	Y123				3.888		11.695	3															44			44																																																																																														Nd2O3, Pr2O3, BaCO3, CuO	1	mixture-CAL(950C,12-18H in air)-grind-pellet-heat(980C,16-24H in air)-heat(850C,24H in Ar)-FC to RT-heat(450C,72H in O2)-FC to RT									Mat.Res.Bull., 38(1995)1363-1370	A.Das,R.Suryanarayanan		
20289	SOV0010121	not superconducting	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	1995																											2	Hg1201				3.868		9.47																	4																																																																																																BaO2, CuO, HgO		precursor(Ba2CuOz)+HgO+CuO in Ar-filled dry box-SIN(920C, 0.6H, P=18 Kbar)									Mat.Res.Bull., 30(1995)1463-1470	S.M.Loureiro,et al.		
20290	SOV0010121	dominent phase=HgBa4Cu2CO3Cz  Tc due to Hg1201(minor phase)	(Hg,C)Ba2CuO4	Hg0.5C0.5Ba2Cu1O4+z	Hg	0.5	C	0.5	Ba	2	Cu	1													O	4+z		2	1995																											2	Hg1201				3.927		8.676																63			63																																																																																														BaO2, CuO, HgO, BaCO3		precursor(Ba2CuOz)+HgO+CuO in Ar-filled dry box-SIN(920C,0.6H, P=18Kbar)									Mat.Res.Bull., 30(1995)1463-1470	S.M.Loureiro,et al.		
20291	SOV0010121		CBa2CuO4	C1Ba2Cu1O4+z	C	1	Ba	2	Cu	1															O	4+z			1995																											2	Hg1201				4.004		7.909																	4																																																																																																BaO2, CuO, BaCO3		precursor(Ba2CuOz)+CuO+BaCO3 in Ar-filled dry box-SIN(920C, 2H, P=40Kbar)									Mat.Res.Bull., 30(1995)1463-1470	S.M.Loureiro,et al.		
20292	SOV0010130		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1995																												Y124																					80				80																																																																																																see Phys.Rev.B,41(1990)6616					Positron lifetime measurements in Ca-substituted Y-124 ceramics				Materials Lett., 25(1995)91-96	G.Cheng,et al.		
20293	SOV0010130		(Y,Ca)Ba2Cu4O8	Y0.95Ca0.05Ba2Cu4O8	Y	0.95	Ca	0.05	Ba	2	Cu	4													O	8		1	1995																												Y124																					87.2				87.2																																																																																																see Phys.Rev.B,41(1990)6616					Positron lifetime measurements in Ca-substituted Y-124 ceramics				Materials Lett., 25(1995)91-96	G.Cheng,et al.		
20294	SOV0010130		(Y,Ca)Ba2Cu4O8	Y0.9Ca0.1Ba2Cu4O8	Y	0.9	Ca	0.1	Ba	2	Cu	4													O	8		1	1995																												Y124																					89.5				89.5																																																																																																see Phys.Rev.B,41(1990)6616					Positron lifetime measurements in Ca-substituted Y-124 ceramics				Materials Lett., 25(1995)91-96	G.Cheng,et al.		
20295	SOV0010130		(Y,Ca)Ba2Cu4O8	Y0.88Ca0.12Ba2Cu4O8	Y	0.88	Ca	0.12	Ba	2	Cu	4													O	8		1	1995																												Y124																					88.5				88.5																																																																																																see Phys.Rev.B,41(1990)6616					Positron lifetime measurements in Ca-substituted Y-124 ceramics				Materials Lett., 25(1995)91-96	G.Cheng,et al.		
20296	SOV0010130		(Y,Ca)Ba2Cu4O8	Y0.85Ca0.15Ba2Cu4O8	Y	0.85	Ca	0.15	Ba	2	Cu	4													O	8		1	1995																												Y124																					87.8				87.8																																																																																																see Phys.Rev.B,41(1990)6616					Positron lifetime measurements in Ca-substituted Y-124 ceramics				Materials Lett., 25(1995)91-96	G.Cheng,et al.		
20297	SOV0010051		(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	z		2	1998																												Bi2223				5.411		37.115													109.8						109.8																																																																																														PbO,CuO,Bi2O3,CaCO3,SrCO3,PbF2,K2CO3	1	mixture-CAL(750C,16H)-pellet-ANN(820-827,69.5H)-pellet-SIN(838C,190H)slow cool to RT									Pis'ma v Zhurnal Technicheskoy Fiziki, 24(1998)8-15	V.V.Petrashko,et al.		
20298	SOV0010051		(Bi,Pb)2Sr2Ca2Cu3(F,O)10	Bi1.6Pb0.4Sr2Ca2Cu3F0.8Oz-0.8	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3	F	0.8									O	z-0.8		2	1998																												Bi2223				5.406		37.083													109.9						109.9																																																																																														PbO,CuO,Bi2O3,CaCO3,SrCO3,PbF2,K2CO3	1	mixture-CAL(750C,16H)-pellet-ANN(820-827,69.5H)-pellet-SIN(838C,190H)slow cool to RT									Pis'ma v Zhurnal Technicheskoy Fiziki, 24(1998)8-15	V.V.Petrashko,et al.		
20299	SOV0010051		(Bi,Pb)2(Sr,K)2Ca2Cu3(F,O)10	Bi1.6Pb0.4Sr1.98K0.02Ca2Cu3F0.8OZ-0.8	Bi	1.6	Pb	0.4	Sr	1.98	K	0.02	Ca	2	Cu	3	F	0.8							O	Z-0.8		2	1998																												Bi2223				5.399		37.019													106.6						106.6																																																																																														PbO,CuO,Bi2O3,CaCO3,SrCO3,PbF2,K2CO3	1	mixture-CAL(750C,16H)-pellet-ANN(820-827,69.5H)-pellet-SIN(838C,190H)slow cool to RT									Pis'ma v Zhurnal Technicheskoy Fiziki, 24(1998)8-15	V.V.Petrashko,et al.		
20300	SOV0010051		(Bi,Pb)2(Sr,K)2Ca2Cu3(F,O)10	Bi1.6Pb0.4Sr1.95K0.05Ca2Cu3F0.8Oz-0.8	Bi	1.6	Pb	0.4	Sr	1.95	K	0.05	Ca	2	Cu	3	F	0.8							O	z-0.8		2	1998																												Bi2223				5.398		36.972													105.6						105.6																																																																																														PbO,CuO,Bi2O3,CaCO3,SrCO3,PbF2,K2CO3	1	mixture-CAL(750C,16H)-pellet-ANN(820-827,69.5H)-pellet-SIN(838C,190H)slow cool to RT									Pis'ma v Zhurnal Technicheskoy Fiziki, 24(1998)8-15	V.V.Petrashko,et al.		
20301	SOV0010128	Tl1212(63 vol,%)+CuO(32%) and<5% impurity		Tl1.15Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	1.15	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4									O	z			1995																												Tl1212																						36			36																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20302	SOV0010128	Tl1212(73vol,%)+CuO(32%)and <5%impurity		Tl0.115Pb0.104Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.115	Pb	0.104	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																												Tl1212																						88			88																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20303	SOV0010128	Tl1212(67vol%)+Cuo(28%)and<5% impurity		Tl0.23Ca0.92Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.23	Ca	0.92	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																												Tl1223																						98			98																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20304	SOV0010128	Tl,Pb 1212(95vol, %)		Tl0.345Pb0.805Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.345	Pb	0.805	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																												Tl1223	P4/mmm			3.824		15.421																106			106																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20305	SOV0010128			Tl0.46Pb0.69Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.46	Pb	0.69	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z			1995																												Tl1223	P4/mmm			3.818		15.341																112			112																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20306	SOV0010128	Tl,Pb 1223(95vol %)		Tl0.575Pb0.575Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.575	Pb	0.575	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																												Tl1223	P4/mmm			3.82		15.348																116			116																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20307	SOV0010128	Tl,Pb 1212(45 vol%)+Tl,Pb1223(44%)+CaPbO4(6%)		Tl0.69Pb0.46Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.69	Pb	0.46	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																																																		119			119																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20308	SOV0010128	Tl,Pb 1212(80 vol %)+Ca2PbO4(15%)		Tl0.805Pb0.345Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.805	Pb	0.345	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z			1995																												Tl1212																						96			96																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20309	SOV0010128	Tl,Pb 1212(63vol %)+Ca2PbO4(32%)		Tl0.92Pb0.23Sr1.6Ba0.4Ca2Cu3Ag0.4Oz	Tl	0.92	Pb	0.23	Sr	1.6	Ba	0.4	Ca	2	Cu	3	Ag	0.4							O	z		2	1995																												Tl1212																						80			80																																																																																														SrCO3,BaCO3,CaCO3,CuO,AgNO3,Tl2O3		precursor(Sr-Ba-Ca-Cu-Ag-O)-mix with Tl2O3-press-wrapped in Au foil-heat(929C,2H in O2Flow)-cool to RT(4-5H)									Mater.Res.Bull., 30(1995)1243-1248	MParantharam,et al.		
20310	SOV0010126	glas temp. TG=426		Bi4Sr3Ca3Cu4OZ	Bi	4	Sr	3	Ca	3	Cu	4													O	Z		6	1995									5.82																																						70						70																																																											428	calculated from resistivity																																		Bi2O3, SrCo3, CaCO3, CuO, PbO		mixture-preheat(500C,5H)-regrinding-heat(1100C,2H)Q to RT, details see Phys.Rev.B,48(1992)11075					Investigation of dielectric properties of (Bi,Pb)4Sr3Ca3Cu4Oz for different content of Pb dopant			Indian Assoc. for Cultivation of Sci. Calcutta, India	Philos. Magazine  B, 71(1995)151-162	S.Mollah,et al.		
20311	SOV0010126	glas temp. TG=415		Bi3.9Pb0.1Sr3Ca3Cu4OZ	Bi	3.9	Pb	0.1	Sr	3	Ca	3	Cu	4											O	Z		6	1995									7																																						72						72																																																											420	calculated from resistivity																																		Bi2O3, SrCo3, CaCO3, CuO, PbO		mixture-preheat(500C,5H)-regrinding-heat(1100C,2H)Q to RT, details see Phys.Rev.B,48(1992)11075					Investigation of dielectric properties of (Bi,Pb)4Sr3Ca3Cu4Oz for different content of Pb dopant			Indian Assoc. for Cultivation of Sci. Calcutta, India	Philos. Magazine  B, 71(1995)151-162	S.Mollah,et al.		
20312	SOV0010126	glas temp. TG=408		Bi3.5Pb0.5Sr3Ca3Cu4OZ	Bi	3.5	Pb	0.5	Sr	3	Ca	3	Cu	4											O	Z		6	1995									6.9																																						73.5						73.5																																																											412	calculated from resistivity																																		Bi2O3, SrCo3, CaCO3, CuO, PbO		mixture-preheat(500C,5H)-regrinding-heat(1100C,2H)Q to RT, details see Phys.Rev.B,48(1992)11075					Investigation of dielectric properties of (Bi,Pb)4Sr3Ca3Cu4Oz for different content of Pb dopant			Indian Assoc. for Cultivation of Sci. Calcutta, India	Philos. Magazine  B, 71(1995)151-162	S.Mollah,et al.		
20313	SOV0010126	glas temp. TG=402		Bi1Pb1Sr3Ca3Cu4OZ	Bi	1	Pb	1	Sr	3	Ca	3	Cu	4											O	Z		6	1995									6.76																																						78.5						78.5																																																											408	calculated from resistivity																																		Bi2O3, SrCo3, CaCO3, CuO, PbO		mixture-preheat(500C,5H)-regrinding-heat(1100C,2H)Q to RT, details see Phys.Rev.B,48(1992)11075					Investigation of dielectric properties of (Bi,Pb)4Sr3Ca3Cu4Oz for different content of Pb dopant			Indian Assoc. for Cultivation of Sci. Calcutta, India	Philos. Magazine  B, 71(1995)151-162	S.Mollah,et al.		
20314	PSS0410389		YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95	1	1999																											3	Y123				3.822	3.885	11.67													88						88																																																																		microV/T																														standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20315	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3O6.98	Y	1	Ba	1.95	La	0.05	Cu	3													O	7-Z	6.98	1	1999																											3	Y123				3.82	3.894	11.655													90						90																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20316	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O6.99	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-Z	6.99	1	1999																											3	Y123				3.823	3.895	11.63													91						91																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20317	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.8La0.2Cu3O7.03	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-Z	7.03	1	1999																											3	Y123				3.819	3.89	11.65													89						89																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20318	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.7La0.3Cu3O7.1	Y	1	Ba	1.7	La	0.3	Cu	3													O	7-Z	7.1	1	1999																											3	Y123				3.828	3.879	11.64													80						80																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20319	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.6La0.4Cu3O7.14	Y	1	Ba	1.6	La	0.4	Cu	3													O	7-Z	7.14	1	1999																											2	Y123				3.857		11.6													70						70																																																																		microV/T																														standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20320	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.5La0.5Cu3O7.17	Y	1	Ba	1.5	La	0.5	Cu	3													O	7-Z	7.17	1	1999																											2	Y123				3.853		11.58													57						57																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20321	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba2Cu3O6.86	Y	1	Ba	2	Cu	3															O	7-Z	6.86	1	1999																											3	Y123				3.822	3.885	11.67													84						84																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20322	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.95La0.05Cu3O6.89	Y	1	Ba	1.95	La	0.05	Cu	3													O	7-Z	6.89		1999																											3	Y123				3.82	3.894	11.655													86						86																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20323	PSS0410389		Y(Ba,La)2Cu3O7	Y1Ba1.9La0.1Cu3O6.92	Y	1	Ba	1.9	La	0.1	Cu	3													O	7-Z	6.92		1999																											3	Y123				3.823	3.895	11.63													87						87																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20324	PSS0410389			Y1Ba1.8La0.2Cu3O6.96	Y	1	Ba	1.8	La	0.2	Cu	3													O	7-Z	6.96		1999																											3	Y123				3.819	3.89	11.65													78						78																																																																		microV/T																														standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20325	PSS0410389			Y1Ba1.7La0.3Cu3O7.02	Y	1	Ba	1.7	La	0.3	Cu	3													O	7-Z	7.02		1999																											3	Y123				3.828	3.879	11.64													77						77																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20326	PSS0410389			Y1Ba1.6La0.4Cu3O7.04	Y	1	Ba	1.6	La	0.4	Cu	3													O	7-Z	7.04		1999																											2	Y123				3.857		11.6													59						59																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20327	PSS0410389			Y1Ba1.5La0.5Cu3O7.06	Y	1	Ba	1.5	La	0.5	Cu	3													O	7-Z	7.06		1999																											2	Y123				3.853		11.58													22						22																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20328	PSS0410389		YBa2(Cu,Co)3O7	Y1Ba1.95Cu2.95Co0.05O7	Y	1	Ba	1.95	Cu	2.95	Co	0.05													O	7-Z	7	1	1999																											3	Y123				3.831	3.889	11.682													90						90																																																																		microV/T																														standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20329	PSS0410389		YBa2(Cu,Co)3O7	Y1Ba1.9Cu2.9Co0.1O7.02	Y	1	Ba	1.9	Cu	2.9	Co	0.1													O	7-Z	7.02	1	1999																											3	Y123				3.865	3.872	11.661													89						89																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20330	PSS0410389		YBa2(Cu,Co)3O7	Y1Ba1.85Cu2.85Co0.15O7.04	Y	1	Ba	1.85	Cu	2.85	Co	0.15													O	7-Z	7.04	1	1999																											2	Y123				3.869		11.676													79						79																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20331	PSS0410389		YBa2(Cu,Co)3O7	Y1Ba1.8Cu2.8Co0.2O7.05	Y	1	Ba	1.8	Cu	2.8	Co	0.2													O	7-Z	7.05	1	1999																											2	Y123				3.872		11.669													70						70																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20332	PSS0410389		YBa2(Cu,Co)3O7	Y1Ba1.75Cu2.75Co0.25O7.06	Y	1	Ba	1.75	Cu	2.75	Co	0.25													O	7-Z	7.06	1	1999																											2	Y123				3.874		11.666													63						63																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20333	PSS0410389			Y1Ba1.95Cu2.95Co0.05O6.9	Y	1	Ba	1.95	Cu	2.95	Co	0.05													O	7-Z	6.9		1999																											3	Y123				3.831	3.889	11.682													70						70																																																																		microV/T																														standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20334	PSS0410389			Y1Ba1.9Cu2.9Co0.1O6.92	Y	1	Ba	1.9	Cu	2.9	Co	0.1													O	7-Z	6.92		1999																											3	Y123				3.865	3.872	11.661													66						66																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20335	PSS0410389			Y1Ba1.85Cu2.85Co0.15O6.94	Y	1	Ba	1.85	Cu	2.85	Co	0.15													O	7-Z	6.94		1999																											2	Y123				3.869		11.676													55						55																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20336	PSS0410389			Y1Ba1.8Cu2.8Co0.2O6.95	Y	1	Ba	1.8	Cu	2.8	Co	0.2													O	7-Z	6.95		1999																											2	Y123				3.872		11.669													43						43																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
20337	PSS0410389			Y1Ba1.75Cu2.75Co0.25O6.95	Y	1	Ba	1.75	Cu	2.75	Co	0.25													O	7-Z	6.95		1999																											2	Y123				3.874		11.666													25						25																																																																																																standard solid state sintering, final processing (450C,10H, in O2 flow), ANN(450C,2H, in vacuum)								State Technical University and Inst. Silicate Chem., Saint-Petersburg	[Fizika tverdogo tela(Phys.of the Solid State)] 41(1999)389	E.V. Vladimirskaya,I.B. Patrina,M.V. Elizarova,V.E. Gasumyantz		
24000	PR05700632		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1998																												Y124																		K				80.5			80.5																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24001	PR05700632		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.996Ni0.004O8	Y	1	Ba	2	Cu	3.996	Ni	0.004													O	8		1	1998																												Y124																		K				78			78																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24002	PR05700632		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.98Ni0.02O8	Y	1	Ba	2	Cu	3.98	Ni	0.02													O	8		1	1998																												Y124																		K				63.1			63.1																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24003	PR05700632		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8		1	1998																												Y124																		K				44			44																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24004	PR05700632		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8		1	1998																												Y124																		K				14.7			14.7																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24005	PR05700632		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.992Zn0.008O8	Y	1	Ba	2	Cu	3.992	Zn	0.008													O		8	1	1998																												Y124																		K				66.1			66.1																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24006	PR05700632		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.98Zn0.02O8	Y	1	Ba	2	Cu	3.98	Zn	0.02													O		8	1	1998																												Y124																		K				47			47																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24007	PR05700632		YBa2(Cu,Zn)4O8	Y1Ba2Cu3.96Zn0.04O8	Y	1	Ba	2	Cu	3.96	Zn	0.04													O		8	1	1998																												Y124																		K				16			16																																																																																														Y2O3,BaCO3,NiO,ZnO,CuO	1	calcined (860C 12h) sintererd 880-920C 12hatm:Ar+20%O2 high-ozygen-pressure(at 1000C-1100C)Pressed					Temperature dependence of the phonon frequencies and linewidths of YBa2(Cu1-xMx)4O8 for M=Ni and Zn	199801		Superconductivity Research Laboratory, International Supercoductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Phys.Rev.B,57(1998)632	N. Koshizuka,N. Watanabe		
24008	PR05700550		(Eu,Ce)2NbSr2Cu2O10	Eu1.4Ce0.6Nb1Sr2Cu2O10-d	Eu	1.4	Ce	0.6	Nb	1	Sr	2	Cu	2											O	10-d		1	1998																											2	Nb1222	I4/mmm		A	3.866		28.72	3											K				21			21																																																																																														Eu2O3,SrCO3,Nb2O5,CuO	1	preheated at 1000C 1day flowing O2sintered  at 1120C 72hour					Reversible effect of hydrogen on superconductivity and weak ferromagnetism in Eu1.4Ce0.6MSr2Cu2O10-delta(M=Nb and Ru)	199801		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B,57(1998)550-555	C. Korn,I. Felner,S.D. Goren,U. Asaf		
24009	PR05700550		(Eu,Ce)2RuSr2Cu2O10	Eu1.4Ce0.6Ru1Sr2Cu2O10-d	Eu	1.4	Ce	0.6	Ru	1	Sr	2	Cu	2											O	10-d		1	1998								122																			2	Ru2122	I4/mmm		A	3.846		28.5	3											K				32			32																																																																																														Eu2O3,CeO2,SrCO3,Ru,CuO	1	preheated at 1000C 1day flowing O2sintered at 1050C 72h					Reversible effect of hydrogen on superconductivity and weak ferromagnetism in Eu1.4Ce0.6MSr2Cu2O10-delta(M=Nb and Ru)	199801		Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B,57(1998)550-555	C. Korn,I. Felner,S.D. Goren,U. Asaf		
24010	PR05701259		HgBa2CuO4	Hg1Ba2Cu1O4+d	Hg	1	Ba	2	Cu	1															O	4+d		1	1998																											2	Hg1201	P4/mmm		A	3.887		9.489	3	Fig2										K				92			92																																																																																														HgO,Tl2O3,BaCuO3+x,Ce0.86Sr0.14CuO2	1	refer to  N.H.Hur et al.,Mater. Res. Bull. 29,959(1994)or           N.H.Hur et al.,PhysicaC 241,1,(1995)					In situ temperature-dependent x-ray-absorption spectroscopic studies for the mercury-based superconductors	199801		Department of chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Reve,B57(1998)1259	Jin-Ho Choy,Nam Hwi Hur,Seong-Ju Hwang		
24011	PR05701259		HgBa2(Ca,Sr)Cu2O6	Hg1Ba2Ca0.86Sr0.14Cu2O6+d	Hg	1	Ba	2	Ca	0.86	Sr	0.14	Cu	2											O	6+d		1	1998																											2	Hg1212	P4/mmm		A	3.858		12.665	3	Fig2										K				120			120																																																																																														HgO,Tl2O3,BaCuO3+x,Ce0.86Sr0.14CuO2	1	refer to  N.H.Hur et al.,Mater. Res. Bull. 29,959(1994)or           N.H.Hur et al.,PhysicaC 241,1,(1995)					In situ temperature-dependent x-ray-absorption spectroscopic studies for the mercury-based superconductors	199801		Department of chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Reve,B57(1998)1259	Jin-Ho Choy,Nam Hwi Hur,Seong-Ju Hwang		
24012	PR05701259		(Hg,Tl)Ba2(Ca,Sr)Cu2O6	Hg0.5Tl0.5Ba2Ca0.86Sr0.14Cu2O6+d	Hg	0.5	Tl	0.5	Ba	2	Ca	0.86	Sr	0.14	Cu	2									O	6+d		1	1998																											2	Hg1212	P4/mmm		A	3.85		12.654	3	Fig2										K				122			122																																																																																														HgO,Tl2O3,BaCuO3+x,Ce0.86Sr0.14CuO2	1	refer to  N.H.Hur et al.,Mater. Res. Bull. 29,959(1994)or           N.H.Hur et al.,PhysicaC 241,1,(1995)					In situ temperature-dependent x-ray-absorption spectroscopic studies for the mercury-based superconductors	199801		Department of chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Reve,B57(1998)1259	Jin-Ho Choy,Nam Hwi Hur,Seong-Ju Hwang		
24013	PR05701259		HgBa2(Ca,Sr)2Cu3O8	Hg1Ba2Ca1.72Sr0.28Cu3O8+d	Hg	1	Ba	2	Ca	1.72	Sr	0.28	Cu	3											O	8+d		1	1998																											2	Hg1223	P4/mmm		A	3.865		16.032	3	Fig2										K				126			126																																																																																														HgO,Tl2O3,BaCuO3+x,Ce0.86Sr0.14CuO2	1	refer to  N.H.Hur et al.,Mater. Res. Bull. 29,959(1994)or           N.H.Hur et al.,PhysicaC 241,1,(1995)					In situ temperature-dependent x-ray-absorption spectroscopic studies for the mercury-based superconductors	199801		Department of chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Reve,B57(1998)1259	Jin-Ho Choy,Nam Hwi Hur,Seong-Ju Hwang		
24014	PR05701259		(Hg,Tl)Ba2(Ca,Sr)2Cu3O8	Hg0.5Tl0.5Ba2Ca1.72Sr0.28Cu3O8+d	Hg	0.5	Tl	0.5	Ba	2	Ca	1.72	Sr	0.28	Cu	3									O	8+d		1	1998																											2	Hg1223	P4/mmm		A	3.865		15.957	3	Fig2										K				128			128																																																																																														HgO,Tl2O3,BaCuO3+x,Ce0.86Sr0.14CuO2	1	refer to  N.H.Hur et al.,Mater. Res. Bull. 29,959(1994)or           N.H.Hur et al.,PhysicaC 241,1,(1995)					In situ temperature-dependent x-ray-absorption spectroscopic studies for the mercury-based superconductors	199801		Department of chemistry, Center for Molecular Catalysis, College of Natural Sciences, Seoul National University, Seoul 151-742, Korea	Phys.Reve,B57(1998)1259	Jin-Ho Choy,Nam Hwi Hur,Seong-Ju Hwang		
24015	PR05700613	P-induced SC. Pcrit =  3 GPa. Tc, s/c properties, resistivity measured  at 3GPa	(Sr,Ca)14Cu24O41	Sr0.4Ca13.6Cu24O41+z	Sr	0.4	Ca	13.6	Cu	24															O	41+z		1	1998																												LAD			A	11.26	12.426	27.38	3		A/K				%/GPa	0.08	0.73	0.22		K			10		0		10	TC24015																																																																						ohm.cm				0.033			0.033				0.026												SrCO3, CaCO3, CuO	1	mixed - calcined 950C, 4 days, in air - heated 1200C, 24h, in 20% O2 + 80% Ar gas, P=2000kgf/cm2					Structural and electrical properties under high pressure for the superconducting spin-ladder system Sr0.4Ca13.6Cu24O41+delta	199801		National Institute for research in Inorganic Materials (NIRIM), 1-1 Namiki, Tsukuba, Ibaraki 305 Japan	Phys.Rev.B,57(1998)613-621	E. Takayama-Muromachi,F. Izumi,H. Hayakawa,J.Q. Li,M. Isobe,M. Onoda,S. Nakano,T. Matsumoto,T. Ohta,Y. Matsui		
24100	SST0140504	composition (Tl:Ba:Ca:Cu = 1.01:2.01:1.90:3.09) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl0.75Ba2Ca2Cu3Oz	Tl	0.75	Ba	2	Ca	2	Cu	3													O	z			2001																												Tl1223			A	3.85		15.885												K				131			131																																																																																																high-pressure synthesis(850C,3.5 GPa) - ANN(700C,1h, in N2)					Study on enhancement of Tc (>= 130 K) in TlBa2Ca2Cu3Oy superconductors				Supercond. Sci. Technol., 14 ( 2001 )504-510	A.Iyo,H.Ihara,K.Tokiwa,M.Tokumoto,T.Watanabe,Y.Ishiura,Y.Tanaka		
24101	SST0140504	composition (Tl:Ba:Ca:Cu = 1.05:1.99:1.96:3.00) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl0.75Ba2Ca2Cu3Oz	Tl	0.75	Ba	2	Ca	2	Cu	3													O	z			2001																												Tl1223			A	3.851		15.889												K				133.5			133.5																																																																																																high-pressure synthesis(950C,3.5 GPa) - ANN(700C,1h, in N2)					Study on enhancement of Tc (>= 130 K) in TlBa2Ca2Cu3Oy superconductors				Supercond. Sci. Technol., 14 ( 2001 )504-510	A.Iyo,H.Ihara,K.Tokiwa,M.Tokumoto,T.Watanabe,Y.Ishiura,Y.Tanaka		
24102	SST0140504	composition (Tl:Ba:Ca:Cu = 1.12:1.93:1.91:3.05) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3Oz	Tl	1	Ba	2	Ca	2	Cu	3													O	z			2001																												Tl1223			A	3.852		15.841												K				122			122																																																																																																high-pressure synthesis(950C,3.5 GPa) - ANN(700C,1h, in N2)					Study on enhancement of Tc (>= 130 K) in TlBa2Ca2Cu3Oy superconductors				Supercond. Sci. Technol., 14 ( 2001 )504-510	A.Iyo,H.Ihara,K.Tokiwa,M.Tokumoto,T.Watanabe,Y.Ishiura,Y.Tanaka		
24103	SST0140504	composition (Tl:Ba:Ca:Cu = 1.03:1.93:1.73:3.31) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3C0.2Oz	Tl	1	Ba	2	Ca	2	Cu	3	C	0.2											O	z			2001																												Tl1223			A	3.856		15.865												K				123.5			123.5																																																																																																high-pressure synthesis(850C,3.5 GPa) - ANN(700C,1h, in N2)					Study on enhancement of Tc (>= 130 K) in TlBa2Ca2Cu3Oy superconductors				Supercond. Sci. Technol., 14 ( 2001 )504-510	A.Iyo,H.Ihara,K.Tokiwa,M.Tokumoto,T.Watanabe,Y.Ishiura,Y.Tanaka		
24104	PHC3570324	composition (Tl:Ba:Ca:Cu = 1.05:1.99:1.96:3.00) by SEM-EDX	TlBa2Ca2Cu3Oz	Tl0.75Ba2Ca2Cu3C0.02Oz	Tl	0.75	Ba	2	Ca	2	Cu	3	C	0.02											O	z			2001																												Tl1223			A	3.85		15.9																133.5			133.5																																																																																																mixture(precursor(Ba2Can-1CunC0.02Oz),Tl2O3,CuO,AgO) - high-pressure synthesis(950C, 3.5 GPa) - ANN(700C,1h inN2)					High-pressure synthesis of TlBa2Can-1CunOy (n=3 and 4) with Tc=133.5 K(n=3) and 127 K(n=4)			National Institute of AdvancedIndustrial Science and Technology(AIST) and CREST, Tsukuba central2, Umezono,Ibaraki,Japan	Physica C, 357(2001)324	A.Iyo,Y.Aizawa,Y.Tanaka,M.Tokumoto,K.Tokiwa,T.Watanabe,H.Ihara		
24105	PHC3570324	composition (Tl:Ba:Ca:Cu = 1.05:1.99:2.96:4.00) by SEM-EDX	TlBa2Ca3Cu4Oz	Tl0.75Ba2Ca2Cu3C0.02Oz	Tl	0.75	Ba	2	Ca	2	Cu	3	C	0.02											O	z			2001																												Tl1234			A	3.85		19.1																127			127																																																																																																mixture(precursor(Ba2Can-1CunC0.02Oz),Tl2O3,CuO,AgO) - high-pressure synthesis(950C, 3.5 GPa) - ANN(700C,1h inN2)					High-pressure synthesis of TlBa2Can-1CunOy (n=3 and 4) with Tc=133.5 K(n=3) and 127 K(n=4)			National Institute of AdvancedIndustrial Science and Technology(AIST) and CREST, Tsukuba central2, Umezono,Ibaraki,Japan	Physica C, 357(2001)324	A.Iyo,Y.Aizawa,Y.Tanaka,M.Tokumoto,K.Tokiwa,T.Watanabe,H.Ihara		
30000	PR06003680		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		1	1999																												Bi2212							3											K		78					78		R																																																																uV/K	-6.81			TP30000	mohmcm				0.33			0.4				0.9													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30001	PR06003680		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.96Co0.04OZ	Bi	2	Sr	2	Ca	1	Cu	1.96	Co	0.04											O	Z		1	1999																												Bi2212							3											K		69					69		R																																																																uV/K	-5.28			TP30001	mohmcm				0.62			0.65				1.1													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30002	PR06003680		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.92Co0.08OZ	Bi	2	Sr	2	Ca	1	Cu	1.92	Co	0.08											O	Z		1	1999																												Bi2212							3											K		62					62		R																																																																uV/K	-4.47			TP30002	mohmcm				0.8			0.77				1.85													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30003	PR06003680		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.88Co0.12OZ	Bi	2	Sr	2	Ca	1	Cu	1.88	Co	0.12											O	Z		1	1999																												Bi2212							3											K		58					58		R																																																																uV/K	-3.69			TP30003	mohmcm				1.1			1.05				1.65													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30004	PR06003680		Bi2Sr2Ca(Cu,Co)2Oz	Bi2Sr2Ca1Cu1.84Co0.16OZ	Bi	2	Sr	2	Ca	1	Cu	1.84	Co	0.16											O	Z		1	1999																												Bi2212							3											K		51					51		R																																																																uV/K	-2.37			TP30004	mohmcm				1.55			1.5				1.8													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30005	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.8Y0.2Cu2OZ	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	Z		1	1999																												Bi2212							3											K		89					89		R																																																																uV/K	2.23			TP30005	mohmcm							0.95				1.6													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30006	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.8Y0.2Cu1.96Co0.04OZ	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.96	Co	0.04									O	Z		1	1999																												Bi2212							3											K		78					78		R																																																																uV/K	4.2			TP30006	mohmcm				1.45			1.4				2.1													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30007	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.8Y0.2Cu1.92Co0.08OZ	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.92	Co	0.08									O	Z		1	1999																												Bi2212							3											K		66					66		R																																																																uV/K	7.48			TP30007	mohmcm				2.6			2.6				2.45													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30008	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.8Y0.2Cu1.88Co0.12OZ	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.88	Co	0.12									O	Z		1	1999																												Bi2212							3											K		48					48		R																																																																uV/K	10.1			TP30008	mohmcm				5.2			7.4				3.8													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30009	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.8Y0.2Cu1.84Co0.16OZ	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	1.84	Co	0.16									O	Z		1	1999																												Bi2212							3											K		35					35		R																																																																uV/K	12.8			TP30009																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30010	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.7Y0.3Cu2OZ	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	Z		1	1999																												Bi2212							3											K		92					92		R																																																																uV/K	6.28			TP30010																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30011	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.7Y0.3Cu1.96Co0.04OZ	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.96	Co	0.04									O	Z		1	1999																												Bi2212							3											K		79					79		R																																																																uV/K	8.16			TP30011																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30012	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.7Y0.3Cu1.92Co0.08OZ	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.92	Co	0.08									O	Z		1	1999																												Bi2212							3											K		41					41		R																																																																uV/K	11.3			TP30012																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30013	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.7Y0.3Cu1.88Co0.12OZ	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.88	Co	0.12									O	Z		1	1999																												Bi2212							3											K		12					12		R																																																																uV/K	16.1			TP30013																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30014	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.7Y0.3Cu1.84Co0.16OZ	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	1.84	Co	0.16									O	Z		1	1999																												Bi2212							3											K		0					0		R																																																																uV/K	20.4			TP30014																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30015	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.6Y0.4Cu2OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	Z		1	1999																												Bi2212							3											K		79					79		R																																																																uV/K	16.4			TP30015																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30016	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.6Y0.4Cu1.96Co0.04OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.96	Co	0.04									O	Z		1	1999																												Bi2212							3											K		38					38		R																																																																uV/K	19.9			TP30016																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30017	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.6Y0.4Cu1.92Co0.08OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.92	Co	0.08									O	Z		1	1999																												Bi2212							3											K		9					9		R																																																																uV/K	21.9			TP30017																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30018	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.6Y0.4Cu1.88Co0.12OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.88	Co	0.12									O	Z		1	1999																												Bi2212							3											K		0					0		R																																																																uV/K	25.7			TP30018																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30019	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.6Y0.4Cu1.84Co0.16OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	1.84	Co	0.16									O	Z		1	1999																												Bi2212							3											K		0					0		R																																																																uV/K	29			TP30019																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30020	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.6Y0.4Cu2OZ	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	Z		1	1999																												Bi2212							3																																																																																				uV/K	36.7			TP30020																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30021	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.5Y0.5Cu1.96Co0.04OZ	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.96	Co	0.04									O	Z		1	1999																												Bi2212							3																																																																																				uV/K	38.4			TP30021																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30022	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.5Y0.5Cu1.92Co0.08OZ	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.92	Co	0.08									O	Z		1	1999																												Bi2212							3																																																																																				uV/K	44.3			TP30022																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30023	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.5Y0.5Cu1.88Co0.12OZ	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.88	Co	0.12									O	Z		1	1999																												Bi2212							3																																																																																				uV/K	58.2			TP30023																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30024	PR06003680		Bi2Sr2(Ca,Y)(Cu,Co)2Oz	Bi2Sr2Ca0.5Y0.5Cu1.84Co0.16OZ	Bi	2	Sr	2	Ca	0.5	Y	0.5	Cu	1.84	Co	0.16									O	Z		1	1999																												Bi2212							3																																																																																				uV/K	61.6			TP30024																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30025	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.58Y0.42Cu2OZ	Bi	2	Sr	2	Ca	0.58	Y	0.42	Cu	2											O	Z		1	1999																												Bi2212							3																																																																																				uV/K	17.5			TP30025																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30026	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.56Y0.44Cu2OZ	Bi	2	Sr	2	Ca	0.56	Y	0.44	Cu	2											O	Z		1	1999																												Bi2212							3																																																																																				uV/K	22.3			TP30026																									1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30027	PR06003680		Bi2Sr2(Ca,Y)Cu2Oz	Bi2Sr2Ca0.54Y0.46Cu2OZ	Bi	2	Sr	2	Ca	0.54	Y	0.46	Cu	2											O	Z		1	1999																												Bi2212							3																																																																																				uV/K																													1	Stoichometric amount of oxides and carbonates were mixed throughly and then reacted in air for several days with intermediate grindings. The heat temperature was 860C-900C					Variation of Tc and transport properties of the Co-doped Bi2Sr2Ca1-xYxCu2O8 system	199908		Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B,60(1999)3680	B. Bandyopadhyay,B. Ghosh,P. Mandal		
30028	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.225	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.225	6.225	1	1999																												Cu1212	P4/mmm			3.8334		11.736	3										Oxigen concentrations determined by powder nutron	K					5																																																																																																Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 800 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30029	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.201	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.201	6.201	1	1999																												Cu1212	P4/mmm			3.8342		11.743	3										Oxigen concentrations determined by powder nutron	K					5																																																																																																Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 750 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30030	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.248	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.248	6.248	1	1999																												Cu1212	P4/mmm			3.8355		11.718	3										Oxigen concentrations determined by powder nutron	K					5																																																																																																Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 550 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30031	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.35	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.35	6.35	1	1999																												Cu1212	Pmmm			3.8172	3.8465	11.667	3										Oxigen concentrations determined by powder nutron	K		37					37																																																																																														Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 480 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30032	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.817	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.817	6.817	1	1999																												Cu1212	Pmmm			3.804	3.8583	11.637	3										Oxigen concentrations determined by powder nutron	K		55					55																																																																																														Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 380 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30033	PR06004378		Cu(Ba,Sr)2YbCu2Oz	Bi1.6Sr0.4Yb1Cu3O6.999	Bi	1.6	Sr	0.4	Yb	1	Cu	3													O	6.999	6.999	1	1999																												Cu1212	Pmmm			3.7934	3.8615	11.614	3										Oxigen concentrations determined by powder nutron	K		82					82																																																																																														Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				no aneeal	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30034	PR06004378		Cu(Ba,Sr)2(Yb,Ca)Cu2Oz	Bi1.6Sr0.4Yb0.9Ca0.1Cu3O6.104	Bi	1.6	Sr	0.4	Yb	0.9	Ca	0.1	Cu	3											O	6.104	6.104	1	1999																												Cu1212	P4/mmm			3.8314		11.745	3										Oxigen concentrations determined by powder nutron	K					5																																																																																																Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 800 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30035	PR06004378		Cu(Ba,Sr)2(Yb,Ca)Cu2Oz	Bi1.6Sr0.4Yb0.8Ca0.2Cu3O6.166	Bi	1.6	Sr	0.4	Yb	0.8	Ca	0.2	Cu	3											O	6.166	6.166	1	1999																												Cu1212	P4/mmm			3.8272		11.735	3										Oxigen concentrations determined by powder nutron	K					5																																																																																																Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 800 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30036	PR06004378		Cu(Ba,Sr)2(Yb,Ca)Cu2Oz	Bi1.6Sr0.4Yb0.75Ca0.25Cu3O6.072	Bi	1.6	Sr	0.4	Yb	0.75	Ca	0.25	Cu	3											O	6.072	6.072	1	1999																												Cu1212	P4/mmm			3.832		11.736	3										Oxigen concentrations determined by powder nutron	K		27					27																																																																																														Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 800 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30037	PR06004378		Cu(Ba,Sr)2(Yb,Ca)Cu2Oz	Bi1.6Sr0.4Yb0.65Ca0.35Cu3O6.075	Bi	1.6	Sr	0.4	Yb	0.65	Ca	0.35	Cu	3											O	6.075	6.075	1	1999																												Cu1212	P4/mmm			3.8334		11.734	3										Oxigen concentrations determined by powder nutron	K		43					43																																																																																														Yb2O3,BaCO3,SrCO3,CuO		ref[14]. Mixed powder sintered in air at 900-940 C and annealing in O2 at 350-400C for 48h				aneeal: in air atomosphere 800 C	Ca-substitution and O-doping effects in superconducting Cu(Ba0.8Sr0.2)2(Yb1-xCax)Cu2O6+z obtained from neutron diffraction refinements	199908		Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B,60(1999)4378	H. Rundlof,H. Yamauchi,K. Fujinami,K. Peitola,M. Karppinen,R. Tellgren,T. Nakane		
30100	PR06006991	in-plane Hall coeff.	Bi2(Sr,La)2CuO6	Bi2Sr1.76La0.24Cu1O6	Bi	2	Sr	1.76	La	0.24	Cu	1													O	6		3	1999																																													La concentrations determined by ICP	K			24				24		R																																																																					uohmcm					100			60				330		cm3/C	1.1					RH30100					Floating zone method. See Phys.Rev.Lett., 75(1995)4662					Nonuniversal power law of the Hall scattering rate in a single-layer cuprate Bi2Sr2-xLaxCuO6	199909		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R6991	T. Murayama,Yoichi Ando		
30101	PR06006991	in-plane Hall coeff.	Bi2(Sr,La)2CuO6	Bi2Sr1.7La0.3Cu1O6	Bi	2	Sr	1.7	La	0.3	Cu	1													O	6		3	1999																												Bi2201																	La concentrations determined by ICP	K			30				30		R																																																																					uohmcm					120			70				390		cm3/C	1.35					RH30101					Floating zone method. See Phys.Rev.Lett., 75(1995)4662					Nonuniversal power law of the Hall scattering rate in a single-layer cuprate Bi2Sr2-xLaxCuO6	199909		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R6991	T. Murayama,Yoichi Ando		
30102	PR06006991	in-plane Hall coeff.	Bi2(Sr,La)2CuO6	Bi2Sr1.56La0.44Cu1O6	Bi	2	Sr	1.56	La	0.44	Cu	1													O	6		3	1999																												Bi2201																	La concentrations determined by ICP	K			33				33		R																																																																					uohmcm					140			70				480		cm3/C	1.63					RH30102					Floating zone method. See Phys.Rev.Lett., 75(1995)4662					Nonuniversal power law of the Hall scattering rate in a single-layer cuprate Bi2Sr2-xLaxCuO6	199909		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R6991	T. Murayama,Yoichi Ando		
30103	PR06006991	in-plane Hall coeff.	Bi2(Sr,La)2CuO6	Bi2Sr1.43La0.57Cu1O6	Bi	2	Sr	1.43	La	0.57	Cu	1													O	6		3	1999																												Bi2201																	La concentrations determined by ICP	K			28.5				28.5		R																																																																					uohmcm					190			100				630		cm3/C	2.09					RH30103					Floating zone method. See Phys.Rev.Lett., 75(1995)4662					Nonuniversal power law of the Hall scattering rate in a single-layer cuprate Bi2Sr2-xLaxCuO6	199909		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R6991	T. Murayama,Yoichi Ando		
30104	PR06006991	in-plane Hall coeff.	Bi2(Sr,La)2CuO6	Bi2Sr1.34La0.66Cu1O6	Bi	2	Sr	1.34	La	0.66	Cu	1													O	6		3	1999																												Bi2201																	La concentrations determined by ICP	K			20				20		R																																																																					uohmcm					390			250				1000		cm3/C	2.99					RH30104					Floating zone method. See Phys.Rev.Lett., 75(1995)4662					Nonuniversal power law of the Hall scattering rate in a single-layer cuprate Bi2Sr2-xLaxCuO6	199909		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R6991	T. Murayama,Yoichi Ando		
30105	PR06007512	oxygen content=8.0 - 7.99. Ferromagnetic(Tm=134K) and s/c (Tc=20K for as-grown and Tc=37K for annealed) 	RuSr2GdCu2Oz	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	Z	8	1	1999							134																					M1212	P4/mmm						3		A/T	0.0000277		0.000831						K	37						37		R																																																																																												RuO2,SrCO3,Gd2O3,CuO		decomposed 960 C in air and flowing nitrogen at 1010 C for 10h followed by reaction in flowing oxygen at 1050 C and 1055 C for 10h and 1060 C in oxygen for 7 days.					Structure and microstructure of the ferromagnetic superconductor RuSr2GdCu2O8	199909		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambrige CB3 OHE United Kingdom	Phys.Rev.B,60(1999)7512	A.C. Mclaughlin,A.N. Fitch,J.L. Tallon,J.P. Affield,W. Zhou		
30200	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3Cu4Oz	Bi1.6Pb0.4Sr2Ca3Cu4OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	4											O	Z		1	1999																												Bi2234							3													108					108		R																																																																uV/K	1.06				mohmcm											0.053												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30201	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.996Ag0.004OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.996	Ag	0.004									O	Z		1	1999																												Bi2234							3													108.4					108.4		R																																																																uV/K	0.815				mohmcm											0.027												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30202	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.984Ag0.016OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.984	Ag	0.016									O	Z		1	1999																												Bi2234							3													108.4					108.4		R																																																																uV/K	0.84				mohmcm											0.021												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30203	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.98Ag0.02OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.98	Ag	0.02									O	Z		1	1999																												Bi2234							3													107.5					107.5		R																																																																uV/K	0.82				mohmcm											0.017												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30204	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.96Ag0.04OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.96	Ag	0.04									O	Z		1	1999																												Bi2234							3													107.5					107.5		R																																																																uV/K	0.804				mohmcm											0.011												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30205	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.92Ag0.08OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.92	Ag	0.08									O	Z		1	1999																												Bi2234							3													108.2					108.2		R																																																																uV/K	0.811				mohmcm											0.018												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30206	PR06009845	Poly crystall	(Bi,Pb)2Sr2Ca3(Cu,Ag)4Oz	Bi1.6Pb0.4Sr2Ca3Cu3.6Ag0.4OZ	Bi	1.6	Pb	0.4	Sr	2	Ca	3	Cu	3.6	Ag	0.4									O	Z		1	1999																												Bi2234							3													107.3					107.3		R																																																																uV/K	0.851				mohmcm											0.05												BiO2,PbO,SrO3,CaCO3,CuO,AgNO3	1	preheated 800 C for 20 h pressed 9 ton/cm2 after sintered at 850 C for 14 h in air pressed 0 ton/cm2					Thermodynamic fluctuations and the thermalectric coeffcient in (Bi1.6Pb0.4)Sr2Ca3(Cu1-xAg)4O12+delta superconductors	199910		Department of Physics, Universidad Nacional de Colombia, Bogota, Colombia	Phys.Rev.B,60(1999)9845	A. Marino,J.E. Rodriguez		
30207	PR06010489	1um particle size. As-grown	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123			A	3.82	3.85	11.68	3															92			92		M																																																																																																		as-grown	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30208	PR06010489	1um particle size, ANN(260 C, 0.5h in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123																						92			92		M																																																																																																		anneal: in Br2 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30209	PR06010489	1um particle size, ANN(450 C, 4h in He)	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1999																												Y123			A	3.83	3.86	11.74	3															60			60		M																																																																																																		anneal: in He 450 C 4h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30210	PR06010489	1um particle size, ANN(450C, 4H inHe)+ANN(260C, 0.5H in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1999																												Y123			A	3.82	3.88	11.6	3															92			92		M																																																																																																		anneal: in He 450 C 4h and in Br2 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30211	PR06010489	1um particle size, ANN(700 C, 4h in He)	YBa2Cu3Oz	Y1Ba2Cu3O6.1	Y	1	Ba	2	Cu	3															O	6.1	6.1	1	1999																												Y123			A	3.84	3.85	11.77	3															0			0		M																																																																																																		anneal: in He 700 C 4h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30212	PR06010489	1um particle size, ANN(700 C, 4h in He)+ANN(260 C, 0.25h in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.1	Y	1	Ba	2	Cu	3															O	6.1	6.1	1	1999																												Y123			A	3.82	3.87	11.7	3															92			92		M																																																																																																		anneal: in He 700 C 4h and in Br2 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30213	PR06010489	1um particle size, ANN(675 C, 8h in He)	YBa2Cu3Oz	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	6.2	6.2	1	1999																												Y123																											M																																																																																																		anneal: in He 675 C 8h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30214	PR06010489	1um particle size, ANN(675 C, 8h in He)+ANN(260 C, 0.5h in vac)	YBa2Cu3Oz	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	6.2	6.2	1	1999																												Y123																											M																																																																																																		anneal: in He 675 C 8h and vac 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30215	PR06010489	1um particle size, ANN(450 C, 8h in He)+ANN(560 C, 4h in O2)	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1999																												Y123																						92			92		M																																																																																																		anneal: in He 450 C 4h and in O2 560 C 4h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30216	PR06010489	20um particle size, as-grown	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123																						93			93		M																																																																																																			Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30217	PR06010489	20um particle size, ANN(450 C, 4h in He)	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1999																												Y123																						69			69		M																																																																																																		anneal: in He 450 C 4h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30218	PR06010489	20um particle size, ANN(450C, 4H inHe)+ANN(260C, 0.5H in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	6.6	6.6	1	1999																												Y123																						92			92		M																																																																																																		anneal: in He 450 C 4h and in Br2 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30219	PR06010489	20um particle size, ANN(750 C, 5h in He)	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123																											M																																																																																																		anneal: in He 750 C 5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30220	PR06010489	20um particle size, ANN(750 C, 5h in He)+ANN(260 C, 0.25h in Br2)	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		1	1999																												Y123																						93			93		M																																																																																																		anneal: in He 750 C 5h and in Br2 260 C 0.25h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30221	PR06010489	40um particle size, as-grown	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123																						93			93		M																																																																																																			Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30222	PR06010489	40um particle size, ANN(450 C, 4h in He)	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	6.7	6.7	1	1999																												Y123																						80			80		M																																																																																																		anneal: in He 450 C 4h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30223	PR06010489	40um particle size, ANN(450 C, 4h in He)+ANN(260 C, 0.5h in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	6.7	6.7	1	1999																												Y123																						93			93		M																																																																																																		anneal: in He 450 C 4h and in Br2 260 C 0.5h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30224	PR06010489	30um particle size, as-grown	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123																						92			92		M																																																																																																			Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30225	PR06010489	30um particle size, ANN(260 C, 24h in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	6.9	6.9	1	1999																												Y123																						92			92		M																																																																																																		anneal: in Br2 260 C 24h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30226	PR06010489	30um particle size, ANN(700 C, 4 h, in He)+ANN(260 C, 24 h, in Br2)	YBa2Cu3Oz	Y1Ba2Cu3O6.1	Y	1	Ba	2	Cu	3															O	6.1	6.1	1	1999																												Y123																						90			90		M																																																																																																		anneal: in He 700 C 4h and in Br2 260 C 24h	Role of bromine in restoring superconductivity in YBa2Cu3Oy	199910		Department of Physics and Institute of Materials Science, University of Connecticut, Storrs, Connecticut 06269	Phys.Rev.B,60(1999)10489	A.R. Moodenbaugh,D.B. Fenner,D.M. Potrepka,J.I. Budnick,M. Balasubramanian,W.A. Hines		
30300	PR06012475	They disscussed about NHC2 compared with magnetic Fields at which the resistivity equals 10, 50, 80, 90% of the normal state resistivity.	(La,Sr)2CuO4	La1.92Sr0.08Cu1O4	La	1.92	Sr	0.08	Cu	1															O	4		3	1999																												T																																													T	Magnetic Fields at which the resistivity equals 50% of the normal state resistivity.						19.3																																																																				7					Traveling-solvent floating-zone method. ref 15.	Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates	19911		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,60(1999)12475	A. Passner,G.S. Boebinger,J. Shimoyama,K. Kishio,K. Tamasaku,L.F. Schneemeyer,M. Okuya,N. Ichikawa,S. Uchida,S. Watauchi,T. Kimura,Yoichi Ando		
30301	PR06012475	They disscussed about NHC2 compared with magnetic Fields at which the resistivity equals 10, 50, 80, 90% of the normal state resistivity.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1999																												T																																													T	Magnetic Fields at which the resistivity equals 50% of the normal state resistivity.						48.3																																																																				7					Traveling-solvent floating-zone method. ref 15.	Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates	19911		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,60(1999)12475	A. Passner,G.S. Boebinger,J. Shimoyama,K. Kishio,K. Tamasaku,L.F. Schneemeyer,M. Okuya,N. Ichikawa,S. Uchida,S. Watauchi,T. Kimura,Yoichi Ando		
30302	PR06012475	They disscussed about NHC2 compared with magnetic Fields at which the resistivity equals 10, 50, 80, 90% of the normal state resistivity.	(La,Sr)2CuO4	La1.83Sr0.17Cu1O4	La	1.83	Sr	0.17	Cu	1															O	4		3	1999																												T																																													T	Magnetic Fields at which the resistivity equals 50% of the normal state resistivity.						51.5																																																																				7					Traveling-solvent floating-zone method. ref 15.	Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates	19911		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,60(1999)12475	A. Passner,G.S. Boebinger,J. Shimoyama,K. Kishio,K. Tamasaku,L.F. Schneemeyer,M. Okuya,N. Ichikawa,S. Uchida,S. Watauchi,T. Kimura,Yoichi Ando		
30303	PR06012475	They disscussed about NHC2 compared with magnetic Fields at which the resistivity equals 10, 50, 80, 90% of the normal state resistivity.	Bi2Sr2Ca1Cu2O8	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	1999																												Bi2212																																													T	Magnetic Fields at which the resistivity equals 50% of the normal state resistivity.						57.1																																																																				7					Floating method. Heat treated insealed quartz tubes to tune to the near-optimum doping.	Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates	19911		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,60(1999)12475	A. Passner,G.S. Boebinger,J. Shimoyama,K. Kishio,K. Tamasaku,L.F. Schneemeyer,M. Okuya,N. Ichikawa,S. Uchida,S. Watauchi,T. Kimura,Yoichi Ando		
30304	PR06012475	They disscussed about NHC2 compared with magnetic Fields at which the resistivity equals 10, 50, 80, 90% of the normal state resistivity.	YBa2Cu3O7	Y1Ba2Cu3O7-D	Y	1	Ba	2	Cu	3															O	7-D		3	1999																												Y123																																													T	Magnetic Fields at which the resistivity equals 50% of the normal state resistivity.						19																																																																				5	Flux method in zirconia crucibles and annealed in sealed quartz tubes to tune the oxyzen content to optimal doping.					Resistive upper critical fields and irreversibility lines of optimally doped high-Tc cuprates	19911		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.B,60(1999)12475	A. Passner,G.S. Boebinger,J. Shimoyama,K. Kishio,K. Tamasaku,L.F. Schneemeyer,M. Okuya,N. Ichikawa,S. Uchida,S. Watauchi,T. Kimura,Yoichi Ando		
30305	PR06012495		Bi2Sr2Ca1Cu2O8	Bi2Sr2Ca1Cu2O8+D	Bi	2	Sr	2	Ca	1	Cu	2													O	8+D		3	1999																												Bi2212																		K		82					82																																																																																															5	ref 25,29				Sample analysis method: EDS. Ref25.	Magnetotransport in Bi2Sr2Ca1-xYxCu2O8+delta single crystal: From the underdoped to the overdoped regime	19911		Laboratoire CRISMAT, UMR 6508, ISMRA et Universite' de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,60(1999)12495	A. Maignan,A. Wahl,Ch. Simon,D. Thopart,G. Villard		
30306	PR06012495		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8+D	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+D		3	1999																												Bi2212																		K		87.5					87.5																																																																																															5	ref 25,29				Sample analysis method: EDS. Ref25.	Magnetotransport in Bi2Sr2Ca1-xYxCu2O8+delta single crystal: From the underdoped to the overdoped regime	19911		Laboratoire CRISMAT, UMR 6508, ISMRA et Universite' de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,60(1999)12495	A. Maignan,A. Wahl,Ch. Simon,D. Thopart,G. Villard		
30307	PR06012495		Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.57Y0.43Cu2O8+D	Bi	2	Sr	2	Ca	0.57	Y	0.43	Cu	2											O	8+D		3	1999																												Bi2212																		K		84.8					84.8																																																																																															5	ref 25,29				Sample analysis method: EDS. Ref25.	Magnetotransport in Bi2Sr2Ca1-xYxCu2O8+delta single crystal: From the underdoped to the overdoped regime	19911		Laboratoire CRISMAT, UMR 6508, ISMRA et Universite' de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,60(1999)12495	A. Maignan,A. Wahl,Ch. Simon,D. Thopart,G. Villard		
30308	PR06012495		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.6Pb0.4Sr2Ca0.8Y0.2Cu2O8+D	Bi	1.6	Pb	0.4	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	8+D		3	1999																												Bi2212																		K		81.3					81.3																																																																																															5	ref 25,29				Sample analysis method: EDS. Ref25.	Magnetotransport in Bi2Sr2Ca1-xYxCu2O8+delta single crystal: From the underdoped to the overdoped regime	19911		Laboratoire CRISMAT, UMR 6508, ISMRA et Universite' de Caen, 6 Boulevard du Marechal Juin, 14050 Caen Cedex, France	Phys.Rev.B,60(1999)12495	A. Maignan,A. Wahl,Ch. Simon,D. Thopart,G. Villard		
30309	PR06013094	They measured MT and MH of each sample, then calculated thermodynamic parameters by using Hao-Clem model(ref 16).	(Hg,Pb)Ba2Ca2Cu3Oz	Hg0.7Pb0.3Ba2Ca2Cu3OY	Hg	0.7	Pb	0.3	Ba	2	Ca	2	Cu	3											O	Y		6	1999																												Hg1223			A			15.9	3															127			127																				T	Hao & Clem model	128							T/K	Hao & Clem model	1.4			HIR30309		A	Hao & Clem model			16	nm	Hao & Clem model			191																																																	BaCO3, SrCo3, CaCo3, CuO, HgO, PbO	1	ref 10				To aligne c-axis, the powder was ground down to around 20 micro meter amd mixed with epoxy, then cured in a magnetic field of 7 T for 10 h at room temperature.	Effects of subsutitution on dimensiinality and superconducting properties of  Hg0.7Pb0.3Ba2Ca2Cu3Oy	1999		National Creative Research Initiative Center for Superconductivity, Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B,60(1999)13094	Jae-Hyuk Choi,M.S. Kuznetsov,Mun-Seog Kim,N.P. Kiryakov,Sergey Lee,Su-Mi Oh,Sung-Ik Lee,Yi Zhuo		
30310	PR06013094	They measured MT and MH of each sample, then calculated thermodynamic parameters by using Hao-Clem model(ref 16).	(Hg,Pb)Sr2Ca2Cu3Oz	Hg0.7Pb0.3Sr2Ca2Cu3OY	Hg	0.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	Y		6	1999																												Hg1223			A			15.2	3															110			110																				T	Hao & Clem model	226							T/K	Hao & Clem model	2.8			HIR30310		A	Hao & Clem model			12	nm	Hao & Clem model			169																																																	BaCO3, SrCo3, CaCo3, CuO, HgO, PbO	1	ref 10				To aligne c-axis, the powder was ground down to around 20 micro meter amd mixed with epoxy, then cured in a magnetic field of 7 T for 10 h at room temperature.	Effects of subsutitution on dimensiinality and superconducting properties of  Hg0.7Pb0.3Ba2Ca2Cu3Oy	1999		National Creative Research Initiative Center for Superconductivity, Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B,60(1999)13094	Jae-Hyuk Choi,M.S. Kuznetsov,Mun-Seog Kim,N.P. Kiryakov,Sergey Lee,Su-Mi Oh,Sung-Ik Lee,Yi Zhuo		
30400	PR06014605		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		6	1999							138																				2	Ru1212			A	3.8387		11.562	3											K				36			36																																																																											6.9							4.3												RuO2, SnO2, SrCO3, Gd2O3, CuO	1	Ground and pelleted before pre-reaction in air at 1000 C for 3 days, then reground, repelleted, and heated at 1050 C in flowing oxygen for a further 3 days and, slow cooled to room temperature.					Tuning of the ferromagnetic and superconducting transitions by tin-doping in RuSr2GdCu2O8	199912		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,60(1999)14605	A.C. McLaughlin,J.P. Attfield		
30401	PR06014605		(Ru,Sn)Sr2GdCu2O8	Ru0.9Sn0.1Sr2Gd1Cu2O8	Ru	0.9	Sn	0.1	Sr	2	Gd	1	Cu	2											O	8		6	1999							112																				2	Ru1212			A	3.8359		11.5609	3											K				39			39																																																																							mOhm.cm				7.4							4.5												RuO2, SnO2, SrCO3, Gd2O3, CuO	1	Ground and pelleted before pre-reaction in air at 1000 C for 3 days, then reground, repelleted, and heated at 1050 C in flowing oxygen for a further 3 days and, slow cooled to room temperature.					Tuning of the ferromagnetic and superconducting transitions by tin-doping in RuSr2GdCu2O8	199912		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,60(1999)14605	A.C. McLaughlin,J.P. Attfield		
30402	PR06014605		(Ru,Sn)Sr2GdCu2O8	Ru0.8Sn0.2Sr2Gd1Cu2O8	Ru	0.8	Sn	0.2	Sr	2	Gd	1	Cu	2											O	8		6	1999							95																				2	Ru1212			A	3.8375		11.5575	3											K				48			48																																																																							mOhm.cm				2.8							2												RuO2, SnO2, SrCO3, Gd2O3, CuO	1	Ground and pelleted before pre-reaction in air at 1000 C for 3 days, then reground, repelleted, and heated at 1050 C in flowing oxygen for a further 3 days and, slow cooled to room temperature.					Tuning of the ferromagnetic and superconducting transitions by tin-doping in RuSr2GdCu2O8	199912		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,60(1999)14605	A.C. McLaughlin,J.P. Attfield		
30403	PR06014605		(Ru,Sn)Sr2GdCu2O8	Ru0.7Sn0.3Sr2Gd1Cu2O8	Ru	0.7	Sn	0.3	Sr	2	Gd	1	Cu	2											O	8		6	1999							87																				2	Ru1212			A	3.8379		11.5552	3											K				39			39																																																																							mOhm.cm				3.7							2.3												RuO2, SnO2, SrCO3, Gd2O3, CuO	1	Ground and pelleted before pre-reaction in air at 1000 C for 3 days, then reground, repelleted, and heated at 1050 C in flowing oxygen for a further 3 days and, slow cooled to room temperature.					Tuning of the ferromagnetic and superconducting transitions by tin-doping in RuSr2GdCu2O8	199912		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,60(1999)14605	A.C. McLaughlin,J.P. Attfield		
30404	PR06014605		(Ru,Sn)Sr2GdCu2O8	Ru0.6Sn0.4Sr2Gd1Cu2O8	Ru	0.6	Sn	0.4	Sr	2	Gd	1	Cu	2											O	8		6	1999							78																				2	Ru1212			A	3.8396		11.5525	3											K				31			31																																																																							mOhm.cm				6.6							3.4												RuO2, SnO2, SrCO3, Gd2O3, CuO	1	Ground and pelleted before pre-reaction in air at 1000 C for 3 days, then reground, repelleted, and heated at 1050 C in flowing oxygen for a further 3 days and, slow cooled to room temperature.					Tuning of the ferromagnetic and superconducting transitions by tin-doping in RuSr2GdCu2O8	199912		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B,60(1999)14605	A.C. McLaughlin,J.P. Attfield		
30405	PR06014872		(La,Sr)2CuO4	La1.975Sr0.025Cu1O4	La	1.975	Sr	0.025	Cu	1															O	4		6	1999																											3	T			A	5.35	5.39	13.16	3											K					4.2																																																																				uV/K	237																		E-9m3/C	14.9								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30406	PR06014872		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4	La	1.95	Sr	0.05	Cu	1															O	4		6	1999																											3	T			A	5.349	5.379	13.18	3											K					4.2																																																																				uV/K	158																		E-9m3/C	10.5								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30407	PR06014872		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		6	1999																											2	T			A	5.351		13.21	3											K			29				29																																																																		uV/K	68.3																		E-9m3/C	3.67								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30408	PR06014872		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		6	1999																											2	T			A	5.342		13.23	3											K			36				36																																																																		uV/K	29.5																		E-9m3/C	1.75								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30409	PR06014872		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		6	1999																											2	T			A	5.333		13.24	3											K			30				30																																																																		uV/K	10.1																		E-9m3/C	0.642								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30410	PR06014872		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		6	1999																											2	T			A	5.326		13.25	3											K			18				18																																																																		uV/K	1.54																		E-9m3/C	0.172								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30411	PR06014872		(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		6	1999																											2	T			A	5.325		13.25	3											K			10				10																																																																		uV/K	1.16																		E-9m3/C	0.106								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and refired at 1050 C for 72 h in air under pressure of 1 bar.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30412	PR06014872		(La,Sr)2CuO4	La1.65Sr0.35Cu1O4	La	1.65	Sr	0.35	Cu	1															O	4		6	1999																											2	T			A	5.317		13.26	3											K					4.2																																																																				uV/K	3.95																		E-9m3/C	-0.182								La2O3, SrCO3, CuO	1	Mixed and prefired in air at 950 C for 24 h, then remixed, pressed and sintered at 1000 C for 60 h, and regrounded, pelletized and sintered in oxygen under the pressure of 300 bar at 1000 C for 48 h.					Normal-state Ettingshausen, Seebeck, and Hall effects in La2-xSrxCuO4	199912		Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wrochaw, Poland	Phys.Rev.B,60(1999)14872	M. Matusiak,T. Plackowski		
30413	PR06015035	Optimally doped sample.	YBa2Cu3O7	Y1Ba2Cu3O7-D	Y	1	Ba	2	Cu	3															O	7-D		3	1999																												Y123																		K		93.1					93.1			K/GPa	0.8																																																																																												We grew high-quality large single crystals of Y-123 using a crystal pulling technique and detwinned them(ref.(9)), then cut and annealed in flowing O2 atmosphere for two weeks at 480 C.					Pressure effects on anisotropic resistivity in detwinned YBa2CuO7-delta:Unconventional carrier doping	199912		Superconductivity Reaearch Laboratory, Intrnational Superconductivity Technology Center, Shinonome 1-10-13, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)R15035	A.I. Rykov,I. Terasaki,K. Yoshida,S. Tajima		
30414	PR06015035	Over doped sample	YBa2Cu3O7	Y1Ba2Cu3O7-D	Y	1	Ba	2	Cu	3															O	7-D		3	1999																												Y123																		K		88.2					88.2			K/GPa	-0.3																																																																																												We grew high-quality large single crystals of Y-123 using a crystal pulling technique and detwinned them(ref.(9)), then cut and annealed in flowing O2 atmosphere for two weeks at 340 C.					Pressure effects on anisotropic resistivity in detwinned YBa2CuO7-delta:Unconventional carrier doping	199912		Superconductivity Reaearch Laboratory, Intrnational Superconductivity Technology Center, Shinonome 1-10-13, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,60(1999)R15035	A.I. Rykov,I. Terasaki,K. Yoshida,S. Tajima		
30415	PR06015055		YBa2Cu3O7	Y1Ba2Cu3O6.78	Y	1	Ba	2	Cu	3															O	Z	6.78	3	1999																												Y123																		K	69.2						69.2																																																																							uOhm.cm					61.4						321.8									RH30415				5	The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.				The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.	Hall effect in Zn-doped YBa2Cu3O7-delta revisited: Hall angle the pseudogap	199912		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R15055	Kouji Segawa,Yasushi Abe,Yoichi Ando		
30416	PR06015055		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.982Zn0.018O6.78	Y	1	Ba	2	Cu	2.982	Zn	0.018													O	Z	6.78	3	1999																												Y123																		K	56						56																																																																							uOhm.cm					85.2						340.9									RH30416				5	The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.				The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.	Hall effect in Zn-doped YBa2Cu3O7-delta revisited: Hall angle the pseudogap	199912		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R15055	Kouji Segawa,Yasushi Abe,Yoichi Ando		
30417	PR06015055		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.961Zn0.039O6.78	Y	1	Ba	2	Cu	2.961	Zn	0.039													O	Z	6.78	3	1999																												Y123																		K	42.9						42.9																																																																							uOhm.cm					130.9						371.6									RH30417				5	The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.				The final oxygen content is confirmed by iodometric titration. The actual Zn concentration in the crystals is measured with ICP spectrometry with an error in z of less than 0.001.	Hall effect in Zn-doped YBa2Cu3O7-delta revisited: Hall angle the pseudogap	199912		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,60(1999)R15055	Kouji Segawa,Yasushi Abe,Yoichi Ando		
30418	PR06015379		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1999																												T'																		K				21		1	21																																		HIR30418	M-H curve																																																												7	Grown by a flux method using pure Y 2 O 3 crucibles(ref.(19)). Annealing the crystals with pure YBCO powders in air at 575 C for 37 h, and subsequent quenching to room temperature.				Annealed in flowing N2 gas at 900 C for 30 h andsubsequently quenched to room temperature.	Vortex state in a Nd1.85Ce0.15CuO4-delta single crystal	199912		Van der Waals-Zeeman Institut, Universiteit van Amsterdam, Valckenierstraat 65 1018 XE. Amsterdom, The Netherlands	Phys.Rev.B,60(1999)15379	A.A. Menovsky,A.A. Nugroho,F.R. de Boer,I.M. Sutjahja,J.J. M. Franse,M.O. Tjia		
30500	PR06100627		YBa2Cu3O7-z	Y1Ba2Cu3O7-D	Y	1	Ba	2	Cu	3															O	7-D		3	2000																												Y123																																																																																																Ohmcm					0.00011	0.28						0.00054	0.06											5	ref[8]:Y. Fukuzumi et al., Phys. Rev. Lett. 76, 684(1996)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30501	PR06100627		YBa2(Cu,Zn)3O7-z	Y1Ba2Cu2.99Zn0.01O7-D	Y	1	Ba	2	Cu	2.99	Zn	0.01													O	7-D		3	2000																												Y123																																																																																																Ohmcm					0.00019	0.27						0.00066	0.06											5	ref[8]:Y. Fukuzumi et al., Phys. Rev. Lett. 76, 684(1996)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30502	PR06100627		YBa2(Cu,Zn)3O7-z	Y1Ba2Cu2.98Zn0.02O7-D	Y	1	Ba	2	Cu	2.98	Zn	0.02													O	7-D		3	2000																												Y123																																																																																																Ohmcm					0.00028	0.27						0.0008	0.06											5	ref[8]:Y. Fukuzumi et al., Phys. Rev. Lett. 76, 684(1996)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30503	PR06100627		YBa2(Cu,Zn)3O7-z	Y1Ba2Cu2.97Zn0.03O7-D	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-D		3	2000																												Y123																																																																																																Ohmcm					0.00042	0.25						0.00092	0.06											5	ref[8]:Y. Fukuzumi et al., Phys. Rev. Lett. 76, 684(1996)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30504	PR06100627		YBa2(Cu,Zn)3O7-z	Y1Ba2Cu2.96Zn0.04O7-D	Y	1	Ba	2	Cu	2.96	Zn	0.04													O	7-D		3	2000																												Y123																																																																																																Ohmcm					0.00059							0.00122												5	ref[8]:Y. Fukuzumi et al., Phys. Rev. Lett. 76, 684(1996)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30505	PR06100627		La1.8Sr0.2Cu1O4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	2000																												T																			31.4	32.9	33.9				32.9																																																																							Ohmcm					0.00006	0.017						0.00025	0.038											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30506	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.99Zn0.01O4	La	1.8	Sr	0.2	Cu	0.99	Zn	0.01													O	4		3	2000																												T																			25.7	26.4	27.1				26.4																																																																							Ohmcm					0.0007	0.019						0.000255	0.04											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30507	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.98Zn0.02O4	La	1.8	Sr	0.2	Cu	0.98	Zn	0.02													O	4		3	2000																												T																			16.8	17.5	20.7				17.5																																																																							Ohmcm					0.00085	0.019						0.00027	0.041											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30508	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.96Zn0.04O4	La	1.8	Sr	0.2	Cu	0.96	Zn	0.04													O	4		3	2000																												T																					4.6				4.6																																																																							Ohmcm					0.00135	0.022						0.00032	0.045											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30509	PR06100627		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2000																												T																			35.1	35.1	36.5				35.1																																																																							Ohmcm					0.00011	0.07						0.0004	0.085											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30510	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01O4	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	4		3	2000																												T																			29.1	29.4	31.6				29.4																																																																							Ohmcm					0.00023	0.075						0.00052	0.085											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30511	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.98Zn0.02O4	La	1.85	Sr	0.15	Cu	0.98	Zn	0.02													O	4		3	2000																												T																			12.4	13.8	16.3				13.8																																																																							Ohmcm					0.00031	0.08						0.00062	0.09											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30512	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.97Zn0.03O4	La	1.85	Sr	0.15	Cu	0.97	Zn	0.03													O	4		3	2000																												T																				2.1	3.2				2.1																																																																							Ohmcm					0.00039	0.09						0.00072	0.09											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30513	PR06100627		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.96Zn0.04O4	La	1.85	Sr	0.15	Cu	0.96	Zn	0.04													O	4		3	2000																												T																																																																																																Ohmcm					0.00045	0.12						0.000785	0.095											7	ref[15]:M. Mizuhashi et al., Phys. Rev. B52,R3884(1995)					Zn-doping effect on the c-axis charge dynamics of underdoped high-Tc cuprates	200001		Department of Superconductivity, University of Tokyo, Yayoi 2-11-16, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)627-633	K.Mizuhashi,S.Uchida,Y.Fukuzumi		
30514	PR06100741	dTc/dp = 2.0 K/GPa when pressure changed at T<200K 	YBa2Cu3Oz	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	6.41	6.41	3	2000																												Y123																		K				13.5			13.5			K/GPa	20.1																																																																																											5	Y:Ba:Cu=5:27:68 Au crusible cooling rate 0.3 to 1 C/h					Pressure dependence of Tc to 17 Gpa with and without relaxation effects in superconducting YBa2Cu3Ox	200001		Department of Phycics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130	Phys.Rev.B,61(2000)741-749	A.P.Paulikas,B.W.Veal,J.S.Schilling,S.Sadewasser		
30515	PR06100741	dTc/dp = 2.1 K/GPa when pressure changed at T<200K  	YBa2Cu3Oz	Y1Ba2Cu3O6.41	Y	1	Ba	2	Cu	3															O	6.41	6.41	3	2000																												Y123																		K				17.1			17.1	TC30515		K/GPa	20																																																																																											5	Y:Ba:Cu=5:27:68 Au crusible cooling rate 0.3 to 1 C/h					Pressure dependence of Tc to 17 Gpa with and without relaxation effects in superconducting YBa2Cu3Ox	200001		Department of Phycics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130	Phys.Rev.B,61(2000)741-749	A.P.Paulikas,B.W.Veal,J.S.Schilling,S.Sadewasser		
30516	PR06100741	dTc/dp = 2.3 K/GPa when pressure changed at T<200K 	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	6.45	6.45	3	2000																												Y123																		K				34.4			34.4			K/GPa	13																																																																																											5	Y:Ba:Cu=5:27:68 Au crusible cooling rate 0.3 to 1 C/h					Pressure dependence of Tc to 17 Gpa with and without relaxation effects in superconducting YBa2Cu3Ox	200001		Department of Phycics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130	Phys.Rev.B,61(2000)741-749	A.P.Paulikas,B.W.Veal,J.S.Schilling,S.Sadewasser		
30517	PR06100741	dTc/dp = 7.1 K/GPa when pressure changed at T<200K 	YBa2Cu3Oz	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	6.66	6.66	3	2000																												Y123																		K				64.2			64.2			K/GPa	9.3																																																																																											5	Y:Ba:Cu=5:27:68 Au crusible cooling rate 0.3 to 1 C/h					Pressure dependence of Tc to 17 Gpa with and without relaxation effects in superconducting YBa2Cu3Ox	200001		Department of Phycics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130	Phys.Rev.B,61(2000)741-749	A.P.Paulikas,B.W.Veal,J.S.Schilling,S.Sadewasser		
30518	PR06100741	 dTc/dp = 0.24 K/GPa when pressure changed at T<200K 	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	3	2000																												Y123																		K				92.5			92.5			K/GPa	0.24																																																																																											5	Y:Ba:Cu=5:27:68 Au crusible cooling rate 0.3 to 1 C/h					Pressure dependence of Tc to 17 Gpa with and without relaxation effects in superconducting YBa2Cu3Ox	200001		Department of Phycics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130	Phys.Rev.B,61(2000)741-749	A.P.Paulikas,B.W.Veal,J.S.Schilling,S.Sadewasser		
30519	PR06101500		Ca5.84Sr4.02Bi0.14Cu15.84O29	Ca5.84Sr4.02Bi0.14Cu15.84O29	Ca	5.84	Sr	4.02	Bi	0.14	Cu	15.84													O	29		3	2000																															A	11.346	12.809	19.52	1											K	72						72																																																6.5																																															5	Bi2CuO4, BaCuO2 flux at 960C					d-wave superconductivity of the hole-doped (SrCa)10Cu17O29 ladder compound	200001		Instytut Fizyki Polskiej Akademii Nauk, Al. Lotnikow 32, 02-668 Warszawa, Poland	Phys.Rev.B,61(2000)1500-1505	A.I.D'yachenko,A.V.Abal'oshev,I.S.Abal'osheva,L.Leonyuk,R.Szymczak,S.J.Lewandowski,V.Yu.Tarenkov		
30520	PR06101500		Bi2Sr2Ca1Cu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		1	2000																												Bi2212																																																																									7.5																																															1	30-40kbar anneal at 845C					d-wave superconductivity of the hole-doped (SrCa)10Cu17O29 ladder compound	200001		Instytut Fizyki Polskiej Akademii Nauk, Al. Lotnikow 32, 02-668 Warszawa, Poland	Phys.Rev.B,61(2000)1500-1505	A.I.D'yachenko,A.V.Abal'oshev,I.S.Abal'osheva,L.Leonyuk,R.Szymczak,S.J.Lewandowski,V.Yu.Tarenkov		
30521	PR06101473	Sample A	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2000																												T																																																																																	mJ/Kmol	1.8																																							in different laboratories					Evidence for line nodes in the energy gap for (La1.85Sr0.15)CuO4 from low-temperature specific-heat measurements	200001		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.B,61(2000)1473-1476	A.S.O'Connor,A.Schilling,B.Buffeteau,C.Marcenat,K.W.Dennis,N.E.Phillips,R.A.Fisher,R.Calemczuk,R.W.McCallum,T.E.Hargreaves		
30522	PR06101473	Sample B	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2000																												T																																																																																	mJ/Kmol	1.2																																							in different laboratories					Evidence for line nodes in the energy gap for (La1.85Sr0.15)CuO4 from low-temperature specific-heat measurements	200001		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.B,61(2000)1473-1476	A.S.O'Connor,A.Schilling,B.Buffeteau,C.Marcenat,K.W.Dennis,N.E.Phillips,R.A.Fisher,R.Calemczuk,R.W.McCallum,T.E.Hargreaves		
30523	PR06100689		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OY	Bi	2	Sr	2	Ca	1	Cu	2													O	Y		5	2000																												Bi2212																																																																							meV	20			1000000																																												Bi,Sr,Ca,Su	17	MBE method p=2.5E-3Pa 10% Ozonejet		MgO(100)			Nonequilibrium microwave emission due to tunnel injection of quasiparticles into a high-Tc Bi2Sr2CaCu2Oy superconductor	200001		Department of Applied Physics and CREST, Tokyo Institute of Technology, 2-12-1 Oh-okayama, Meguro-ku, Tokyo 152-8551, Japan	Phys.Rev.B,61(2000)689-693	E.Kume,I.Iguchi,K.Lee,K.Sato,T.Ishibashi		
30524	PR06101548		Pr(Pr,Ba)2Cu3O7-z	Pr1.05Ca0Ba1.95Cu3O7-D	Pr	1.05	Ca	0	Ba	1.95	Cu	3													O	7-D		1	2000																												Y123			A	3.863	3.918	11.65	3																																																																																																																Pr6O11,BaCO3CaCO3,CuO	1	calcined CO2-free air for 24-48h					Valence determination as a function of doping in PrBa2Cu3O7	200001		Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,61(2000)1548-1554	A.G.O.Conner,B.D.Patterson,L.Soderholm,M.J.Kramer,M.Knapp,M.Shi,S.R.Wasserman,U.Staub		
30525	PR06101548		Pr(Ca,Ba)2Cu3O7-z	Pr1Ca0.05Ba1.95Cu3O7-D	Pr	1	Ca	0.05	Ba	1.95	Cu	3													O	7-D		1	2000																												Y123			A	3.8413	3.9168	11.6547	3																																																																																																																Pr6O11,BaCO3CaCO3,CuO	1	calcined CO2-free air for 24-48h					Valence determination as a function of doping in PrBa2Cu3O7	200001		Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,61(2000)1548-1554	A.G.O.Conner,B.D.Patterson,L.Soderholm,M.J.Kramer,M.Knapp,M.Shi,S.R.Wasserman,U.Staub		
30526	PR06101548		(Pr,Ca)(Ca,Ba)2Cu3O7-z	Pr0.95Ca0.1Ba1.95Cu3O7-D	Pr	0.95	Ca	0.1	Ba	1.95	Cu	3													O	7-D		1	2000																												Y123			A	3.8358	3.9094	11.6449	3																																																																																																																Pr6O11,BaCO3CaCO3,CuO	1	calcined CO2-free air for 24-48h					Valence determination as a function of doping in PrBa2Cu3O7	200001		Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,61(2000)1548-1554	A.G.O.Conner,B.D.Patterson,L.Soderholm,M.J.Kramer,M.Knapp,M.Shi,S.R.Wasserman,U.Staub		
30527	PR06101548		(Pr,Ca)(Ca,Ba)2Cu3O7-z	Pr0.9Ca0.15Ba1.95Cu3O7-D	Pr	0.9	Ca	0.15	Ba	1.95	Cu	3													O	7-D		1	2000																												Y123			A	3.848	3.9	11.748	3																																																																																																																Pr6O11,BaCO3CaCO3,CuO	1	calcined CO2-free air for 24-48h					Valence determination as a function of doping in PrBa2Cu3O7	200001		Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,61(2000)1548-1554	A.G.O.Conner,B.D.Patterson,L.Soderholm,M.J.Kramer,M.Knapp,M.Shi,S.R.Wasserman,U.Staub		
30528	PR06101548		(Pr,Ca)(Ca,Ba)2Cu3O7-z	Pr0.85Ca0.2Ba1.95Cu3O7-D	Pr	0.85	Ca	0.2	Ba	1.95	Cu	3													O	7-D		1	2000																												Y123			A	3.848	3.896	11.733	3																																																																																																																Pr6O11,BaCO3CaCO3,CuO	1	calcined CO2-free air for 24-48h					Valence determination as a function of doping in PrBa2Cu3O7	200001		Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,61(2000)1548-1554	A.G.O.Conner,B.D.Patterson,L.Soderholm,M.J.Kramer,M.Knapp,M.Shi,S.R.Wasserman,U.Staub		
30529	PR06100107	plate	La2CuO4	La1Cu1O4	La	1	Cu	1																	O	4		3	2000																												T																		K	23						23	TC30529		K/GPa	3																																																																																											7	TSFZ					Role of two-dimensional electronic state in superconductivity in La2-xSrxCuO4	200001		Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526, Japan	Phys.Rev.B,61(2000)107-110	Fumihiko Nakamura,Junya Hori,Naoki Kikugawa,Tatsuo Goko,Toshizo Fujita,Yoshinori Uno		
30530	PR06100107	stick	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	2000																												T																		K	23						23	TC30530		K/GPa	-0.8																																																																																											7	TSFZ					Role of two-dimensional electronic state in superconductivity in La2-xSrxCuO4	200001		Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526, Japan	Phys.Rev.B,61(2000)107-110	Fumihiko Nakamura,Junya Hori,Naoki Kikugawa,Tatsuo Goko,Toshizo Fujita,Yoshinori Uno		
30531	PR06100107	plate	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2000																												T																		K	38						38	TC30531		K/GPa	5																																																																																											7	TSFZ					Role of two-dimensional electronic state in superconductivity in La2-xSrxCuO4	200001		Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526, Japan	Phys.Rev.B,61(2000)107-110	Fumihiko Nakamura,Junya Hori,Naoki Kikugawa,Tatsuo Goko,Toshizo Fujita,Yoshinori Uno		
30600	PR06103604	beta(lattice term of SP) = 0.392 mJ/mol.K4	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	3	2000																												Y123																		K		93					93																																																					SP30600			mJ/mol.K2	3	SP	403	SP																																			5	See Phys.Rev.B, 50(1994)4051				The Zn concentration was determined by Tc of the crystals to powder samples with knowm Zn concentration and annealed at the same conditions. Details is in ref.4.	Specific heat of Zn-doped YBa2Cu3O6.95: Possible evidence for Kondo screening in the superconducting state	200002		Department of Applied Physics and Department of Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,61(2000)3604-3609	A.Kapitulnik,D.A.Bonn,D.L.Sisson,R.Liang,S.G.Doettinger,W.N.Hardy		
30601	PR06103604	beta(lattice term of SP) = 0.308 mJ/mol.K4	YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.9955Zn0.0045O6.95	Y	1	Ba	2	Cu	2.9955	Zn	0.0045													O	6.95	6.95	3	2000																												Y123																		K		90					90																																																					SP30601			mJ/mol.K2	4.3	SP																																					5	See Phys.Rev.B, 50(1994)4051				The Zn concentration was determined by Tc of the crystals to powder samples with knowm Zn concentration and annealed at the same conditions. Details is in ref.4.	Specific heat of Zn-doped YBa2Cu3O6.95: Possible evidence for Kondo screening in the superconducting state	200002		Department of Applied Physics and Department of Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,61(2000)3604-3609	A.Kapitulnik,D.A.Bonn,D.L.Sisson,R.Liang,S.G.Doettinger,W.N.Hardy		
30602	PR06103604	beta(lattice term of SP) = 0.284 mJ/mol.K4	YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.9907Zn0.0093O6.95	Y	1	Ba	2	Cu	2.9907	Zn	0.0093													O	6.95	6.95	3	2000																												Y123																		K		88					88																																																					SP30602			mJ/mol.K2	5.8	SP																																					5	See Phys.Rev.B, 50(1994)4051				The Zn concentration was determined by Tc of the crystals to powder samples with knowm Zn concentration and annealed at the same conditions. Details is in ref.4.	Specific heat of Zn-doped YBa2Cu3O6.95: Possible evidence for Kondo screening in the superconducting state	200002		Department of Applied Physics and Department of Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,61(2000)3604-3609	A.Kapitulnik,D.A.Bonn,D.L.Sisson,R.Liang,S.G.Doettinger,W.N.Hardy		
30603	PR06103604	beta(lattice term of SP) = 0.274 mJ/mol.K4	YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.97Zn0.03O6.95	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	6.95	6.95	3	2000																												Y123																		K		81					81																																																					SP30603			mJ/mol.K2	11.7	SP	454	SP																																			5	See Phys.Rev.B, 50(1994)4051				The Zn concentration was determined by Tc of the crystals to powder samples with knowm Zn concentration and annealed at the same conditions. Details is in ref.4.	Specific heat of Zn-doped YBa2Cu3O6.95: Possible evidence for Kondo screening in the superconducting state	200002		Department of Applied Physics and Department of Physics, Stanford University, Stanford, California 94305	Phys.Rev.B,61(2000)3604-3609	A.Kapitulnik,D.A.Bonn,D.L.Sisson,R.Liang,S.G.Doettinger,W.N.Hardy		
30604	PR06103808	anisotropy factor=21.3. Tc derivation is described in ref.18. 	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	2000																												T																		K		30.3					30.3																																									um	The low field ac susceptibility technique. ref.13.		0.28	5.9																																																		1	ref.19					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30605	PR06103808	anisotropy factor=15. Tc derivation is described in ref.18. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2000																												T																		K		38.4					38.4																																									um	The low field ac susceptibility technique. ref.13.		0.26	3.8																																																		1	ref.19					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30606	PR06103808	anisotropy factor=12.9. Tc derivation is described in ref.18. 	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	2000																												T																		K		35.2					35.2																																									um	The low field ac susceptibility technique. ref.13.		0.197	2.45																																																		1	ref.19					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30607	PR06103808	anisotropy factor=12.1. Tc derivation is described in ref.18. 	(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		1	2000																												T																		K		28.1					28.1																																									um	The low field ac susceptibility technique. ref.13.		0.193	2.28																																																		1	ref.19					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30608	PR06103808	anisotropy factor=12.4. Tc derivation is described in ref.18. 	(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		1	2000																												T																		K		20					20																																									um	The low field ac susceptibility technique. ref.13.		0.194	2.37																																																		1	ref.19					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30609	PR06103808	Tc derivation is described in ref.19.	HgBa2CuO4+z	Hg1Ba2Cu1O4.1	Hg	1	Ba	2	Cu	1															O	4+Z	4.1	1	2000																												Hg1201																		K		60					60																																									um	The low field ac susceptibility technique. ref.13.			8.475																																																		1	ref.18					c-axis superfluid response and pseudogap in high-Tc superconductors	200002		Cavendish Laboratory and Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B,61(2000)R3808-R3810	C.Panagopoulos,C.W.Chu,J.R.Cooper,T.Xiang,Y.S.Wang		
30610	PR06104314		YBa2Cu3O7-z	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	1	2000																												Y123			A	3.819	3.888	11.693	3											K				90.5			90.5		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	The powder mixture was calcined at 860-920 C for 3 days.The calcined powders were pelletized and sinterd at 970 C for 2 days in flowing oxgen gas and then cooled at arate of 100 C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30611	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.98Ni0.02O6.95	Y	1	Ba	2	Cu	2.98	Ni	0.02													O	7-Z	6.95	1	2000																												Y123			A	3.819	3.887	11.69	3											K				87.5			87.5		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	The powder mixture was calcined at 860-920 C for 3 days.The calcined powders were pelletized and sinterd at 970 C for 2 days in flowing oxgen gas and then cooled at arate of 100 C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30612	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.95Ni0.05O6.94	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	7-Z	6.94	1	2000																												Y123			A	3.822	3.885	11.683	3											K				85			85		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	The powder mixture was calcined at 860-920 C for 3 days.The calcined powders were pelletized and sinterd at 970 C for 2 days in flowing oxgen gas and then cooled at arate of 100 C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30613	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.9Ni0.1O6.92	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z	6.92	1	2000																												Y123			A	3.821	3.885	11.68	3											K				80			80		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	The powder mixture was calcined at 860-920 C for 3 days.The calcined powders were pelletized and sinterd at 970 C for 2 days in flowing oxgen gas and then cooled at arate of 100 C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30614	PR06104314		YBa2Cu3O7-z	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	1	2000																												Y123			A	3.82	3.888	11.692	3											K				91			91		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 3 days in flowing N2 gas, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30615	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.98Ni0.02O6.94	Y	1	Ba	2	Cu	2.98	Ni	0.02													O	7-Z	6.94	1	2000																												Y123			A	3.819	3.887	11.689	3											K				86			86		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 3 days in flowing N2 gas, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30616	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.95Ni0.05O6.93	Y	1	Ba	2	Cu	2.95	Ni	0.05													O	7-Z	6.93	1	2000																												Y123			A	3.821	3.886	11.685	3											K				80			80		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 3 days in flowing N2 gas, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30617	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.9Ni0.1O6.93	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z	6.93	1	2000																												Y123			A	3.821	3.884	11.678	3											K				70			70		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 3 days in flowing N2 gas, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30618	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.9Ni0.1O6.95	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z	6.95	1	2000																												Y123			A	3.822	3.884	11.678	3											K				70			70		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 14 days in flowing N2 gas, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30619	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.9Ni0.1O6.93	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z	6.93	1	2000																												Y123			A	3.821	3.885	11.679	3											K				75			75		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 800 C for 3 days in air, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30620	PR06104314		YBa2(Cu,Ni)3O7-z	Y1Ba2Cu2.9Ni0.1O6.92	Y	1	Ba	2	Cu	2.9	Ni	0.1													O	7-Z	6.92	1	2000																												Y123			A	3.823	3.884	11.679	3											K				81			81		M																																																																																												Y2O3, BaCO3, CuO, NiO	1	Synthsized  as PREPNUM 30610.Then annealed at 1000 C for 3 days in a gas of p(O2)=400 atm, and quenched.Finally oxgenated  at 550 C for 18 days inflowing O2 gas and slowly cooled at a rate of 50C/h.					Control of Tc for Ni-substituted YBa2Cu3O7-z by annealing treatments	200002		Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,61(2000)4314-4318	E.Kandyel,N.Koshizuka,S.Adachi,S.Tajima,T.Machi,Y.Itoh		
30700	PR06106303		(Eu,Ce)Sr2CuTiO10	Eu1.5Ce0.5Sr2Cu1Ti1O10	Eu	1.5	Ce	0.5	Sr	2	Cu	1	Ti	1											O	10		6	2000																															A	3.863		28.5	1											K			22				22		M																																																																																	3.7											Eu2O3, CeO2, TiO2, SrCO3, CuO		The mixed powder into pellets and preheated at 1000 C for 24h in flowing O2 at 1atm. Sinterd at 1050 C for 72 h in a slightly pressurized and furnance cooled.					Observation of superconductivity in Eu1.5Ce0.5Sr2Cu2TiO10	200003		Department of Physics, University of Notre Dame, Notre Dame, Indiana 46556	Phys.Rev.B,61(2000)6303-6306	David B.Pulling,Howard A.Blackstead,Israel Felner,John D.Dow		
30701	PR06106327	Resistivity is the a-axis direction varue.	PrBa2Cu4O8	Pr1Ba2Cu4O8	Pr	1	Ba	2	Cu	4															O	8		3	2000																												Pr124			A	3.8811	3.9	27.42	1																																																																																									mohmcm		3.8			7.6																		PrOx, BaO, CuO	5	High Presure flix method with P(O2) 11atm in MgO crusible.Heat profile is FIG# at Ts = 1020 C					Growth and anisotropic resistivity of PrBa2Cu4O8 and Pr2Ba4Cu7O15-y single crystals: A direct probe of metallic Cu-O double chains	200003		Department of Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku Nagoya 464-8603, Japan	Phys.Rev.B,61(2000)6327-6333	A. Matsushita,A.Matsushita,H. Ikuta,H. Takagi,H.Ikuta,H.Takagi,I. Hirabayashi,I.Hirabayashi,J. H. Ye,J.H.Ye,N. E. Hussey,N.E.Hussey,S. Horii,S.Horii,U. Mizutani,U.Mizutani,Y. Yamada,Y.Yamada		
30702	PR06106327		Pr2Ba4Cu7O15-z	Pr2Ba4Cu7O15-Z	Pr	2	Ba	4	Cu	7															O	15-Z		3	2000																												Pr247			A	3.864	3.9	50.28	1																																																																																																																PrOx, BaO, CuO	5	High Presure flix method with P(O2) 11atm in Al2O3 crusible.Heat profile is FIG# at Ts = 1020 C The starting compositio is determined by ternary diagram in FIG 1.					Growth and anisotropic resistivity of PrBa2Cu4O8 and Pr2Ba4Cu7O15-y single crystals: A direct probe of metallic Cu-O double chains	200003		Department of Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku Nagoya 464-8603, Japan	Phys.Rev.B,61(2000)6327-6333	A. Matsushita,A.Matsushita,H. Ikuta,H. Takagi,H.Ikuta,H.Takagi,I. Hirabayashi,I.Hirabayashi,J. H. Ye,J.H.Ye,N. E. Hussey,N.E.Hussey,S. Horii,S.Horii,U. Mizutani,U.Mizutani,Y. Yamada,Y.Yamada		
30703	PR06106334		(Pb2Cu)Sr2(Dy,Ce)3Cu2O12	Pb2Sr2Dy0.84Ce0.5Cu3O12	Pb	2	Sr	2	Dy	0.84	Ce	0.5	Cu	3											O	12		5	2000																												Pb3232			A			21.39	1																																																																																				uV/K					ohmcm	0.3			0.11							0.077												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30704	PR06106334		(Pb2Cu)Sr2(Dy,Ce)3Cu2O12	Pb2Sr2Dy1Ce1.36Cu3O12	Pb	2	Sr	2	Dy	1	Ce	1.36	Cu	3											O	12		5	2000																												Pb3232			A			21.39	1																																																																																				uV/K				TP30704	ohmcm	1			0.97							0.06												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30705	PR06106334		(Pb2Cu)Sr2(Dy,Ce)3Cu2O12	Pb2Sr2Dy1.44Ce0.93Cu3O12	Pb	2	Sr	2	Dy	1.44	Ce	0.93	Cu	3											O	12		5	2000																												Pb3232			A			21.38	1																																																																																				uV/K				TP30705	ohmcm	1			0.96							0.05												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30706	PR06106334		(Pb2Cu)Sr2(Dy,Ce)5Cu2O16	Pb2Sr2Dy0.97Ce4.16Cu3O16	Pb	2	Sr	2	Dy	0.97	Ce	4.16	Cu	3											O	16		5	2000																												Pb3252			A			26.83	1																																																																																				uV/K				TP30706	ohmcm	0.26			0.12							0.074												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30707	PR06106334		(Pb2Cu)Sr2(Dy,Ce)5Cu2O16	Pb2Sr2Dy1.48Ce2.74Cu3O16	Pb	2	Sr	2	Dy	1.48	Ce	2.74	Cu	3											O	16		5	2000																												Pb3252			A			26.88	1																																																																																				uV/K					ohmcm	0.7			2.3							11												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30708	PR06106334		(Pb2Cu)Sr2(Dy,Ce)5Cu2O16	Pb2Sr2Dy186Ce2.79Cu3O16	Pb	2	Sr	2	Dy	186	Ce	2.79	Cu	3											O	16		5	2000																												Pb3252			A			26.88	1																																																																																				uV/K				TP30708	ohmcm	1.2			4.8							1.4												Pb, Sr, Ca, Dy or Eu, Ce, Cu metals	16	Metals were evaporated from the effsion cells onto a SrTiO3(001) surface.The growth temperature was 873-1073 K.				sample thickness is 39.5-80.7 nm	Transport properties of separated pairs of CuO2 planes in (Pb2Cu)Sr2DyxCen-x-zCu2O2n+6 (n=3,5) epitaxial films	200003		Advanced Materials & Devices Laboratory, Corporate Research & Development Center, Toshiba Corporation, 1, Komukai Toshiba-cho, Saiwai-ku, Kawasaki 212-8582, Japan	Phys.Rev.B,61(2000)6334-6342	Sumio Ikegawa,Yuichi Motoi		
30709	PR06106401		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		6	2000							133																				2	Ru1212	P4/mmm		A	3.83599		11.5628	4											K				35			35																																																																																														RuO2, SrCO3,160Gd2O3,CuO		The mixture was decomposed at 960 C in air and in a flowing N2 1atm at 1010 C.The material was reground and reacted in a flowing O2 for 10 h at 1050 C.finally it cooled slowly/					Crystal and magnetic structure of ferromagnetic superconducting RuSr2GdCu2O8	200003		Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,61(2000)6401-6407	H.Shaked,J.D.Jorgensen,J.L.Tallon,O.Chmaissem,P.Dollar		
30710	PR06106401		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		6	2000							133																				2	Ru1212	P4/mbm		A	5.42495		11.5626	4										O1:See Table1 caption.	K				35			35																																																																																														RuO2, SrCO3,160Gd2O3,CuO		The mixture was decomposed at 960 C in air and in a flowing N2 1atm at 1010 C.The material was reground and reacted in a flowing O2 for 10 h at 1050 C.finally it cooled slowly/					Crystal and magnetic structure of ferromagnetic superconducting RuSr2GdCu2O8	200003		Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,61(2000)6401-6407	H.Shaked,J.D.Jorgensen,J.L.Tallon,O.Chmaissem,P.Dollar		
30711	PR06106401		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		6	2000							133																				2	Ru1212	P4/mbm		A	5.42491		11.5628	4										O1,O1':See Table1 caption.	K				35			35																																																																																														RuO2, SrCO3,160Gd2O3,CuO		The mixture was decomposed at 960 C in air and in a flowing N2 1atm at 1010 C.The material was reground and reacted in a flowing O2 for 10 h at 1050 C.finally it cooled slowly/					Crystal and magnetic structure of ferromagnetic superconducting RuSr2GdCu2O8	200003		Department of Physics, Northern Illinois University, DeKalb, Illinois 60115	Phys.Rev.B,61(2000)6401-6407	H.Shaked,J.D.Jorgensen,J.L.Tallon,O.Chmaissem,P.Dollar		
30712	PR06106408		(Cu,C)Ba2Ca2Cu3Oz	C0.5Ba2Ca2Cu3.5OZ	C	0.5	Ba	2	Ca	2	Cu	3.5													O	Z		3	2000																												(Cu,C)1223			A	3.858		14.78	1											K			67.4	67			67		R	K/Gpa	-0.7																																																														uV/K				TP30712																								BaO, CaO,CuO Ba:Ca:Cu=2:1.5:3.5	1	The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				as-synthesized	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30713	PR06106408		(Cu,C)Ba2Ca2Cu3Oz	C0.5Ba2Ca2Cu3.5OZ	C	0.5	Ba	2	Ca	2	Cu	3.5													O	Z		3	2000																												(Cu,C)1223			A	3.858		14.78	1														88	88			88		R	K/Gpa	-0.3																																																														uV/K				TP30713																								BaO, CaO,CuO Ba:Ca:Cu=2:1.5:3.5		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				350C for 48 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30714	PR06106408		(Cu,C)Ba2Ca2Cu3Oz	C0.5Ba2Ca2Cu3.5OZ	C	0.5	Ba	2	Ca	2	Cu	3.5													O	Z		3	2000																												(Cu,C)1223			A	3.858		14.78	1														107	107			107		R	K/Gpa	0.9																																																														uV/K				TP30714																								BaO, CaO,CuO Ba:Ca:Cu=2:1.5:3.5		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				450 C for 48 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30715	PR06106408		(Cu,C)Ba2Ca2Cu3Oz	C0.5Ba2Ca2Cu3.5OZ	C	0.5	Ba	2	Ca	2	Cu	3.5													O	Z		3	2000																												(Cu,C)1223			A	3.858		14.78	1											K			115.7	118			118		R	K/Gpa	1.2																																																														uV/K																												BaO, CaO,CuO Ba:Ca:Cu=2:1.5:3.5		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				550 C for 48 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30716	PR06106408		(Cu,C)Ba2Ca3Cu4Oz	C0.5Ba2Ca3Cu4.5OZ	C	0.5	Ba	2	Ca	3	Cu	4.5													O	Z		3	2000																												(Cu,C)1234			A	3.857		17.89	1											K			115	112			112		R	K/Gpa	0.65																																																														uV/K				TP30716																								BaO, CaO,CuO		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				as-synthesized	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30717	PR06106408		(Cu,C)Ba2Ca3Cu4Oz	C0.5Ba2Ca3Cu4.5OZ	C	0.5	Ba	2	Ca	3	Cu	4.5													O	Z		3	2000																												(Cu,C)1234			A	3.857		17.89	1											K				111			111																																																																		uV/K				TP30717																								BaO, CaO,CuO		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				400 C for 48 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30718	PR06106408		(Cu,C)Ba2Ca3Cu4Oz	C0.5Ba2Ca3Cu4.5OZ	C	0.5	Ba	2	Ca	3	Cu	4.5													O	Z		3	2000																												(Cu,C)1234			A	3.857		17.89	1											K				108			108																																																																		uV/K				TP30718																								BaO, CaO,CuO		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				500C for 48 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30719	PR06106408		(Cu,C)Ba2Ca3Cu4Oz	C0.5Ba2Ca3Cu4.5OZ	C	0.5	Ba	2	Ca	3	Cu	4.5													O	Z		3	2000																												(Cu,C)1234			A	3.857		17.89	1											K			99	102			102		R	K/Gpa	0.75																																																														uV/K				TP30719																								BaO, CaO,CuO		The mixedpowder were calcined in Al2O3 crusible at 650-900 C for 40-48 h inflowing O2 with severalintermittent grindings.				600 C for 24 h in Argas	(Cu0.5C0.5)Ba2Cam-1CumOx for m=3 nd 4 under hydrostatic pressure	200003		Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B,61(2000)6408-6412	C.W.Chu,Y.Cao,Y.Y.Xue,Z.L.Du		
30720	PR06106471	grain size: 0.5-2 um	RuSr2GdCu2Oz	Ru1Sr2Gd1Cu2OZ	Ru	1	Sr	2	Gd	1	Cu	2													O	Z		6	2000							132																					Ru1212																		K	20		50				35		R																																																																					mohmcm				6.7			7.3				10.7												RuO2, SrCO3,160Gd2O3,CuO		The mixed powder warm up first in flowing N2 at 1010 K then successively in flowing O2 at 1050 C,1055 C and 1060 C. Samples were slow-cooled after each 10h reaction.					Heat capacity and transport studies of the ferromagnetic superconductor RuSr2GdCu2O8	200003		Industrial Research Ltd., P.O.Box 31310, Lower Hutt, New Zealand	Phys.Rev.B,61(2000)R6471-R6474	C.Bernhard,G.V.M.Williams,J.L.Tallon,J.W.Loram		
30721	PR06106471	grain size: 2-10 um	RuSr2GdCu2Oz	Ru1Sr2Gd1Cu2OZ	Ru	1	Sr	2	Gd	1	Cu	2													O	Z		6	2000							132																					Ru1212																		K	36	45.1	50				45.1		R																																																																uV/K	73			TP30721	mohmcm				2.5			2.3				4.9												RuO2, SrCO3,160Gd2O3,CuO		The mixed powder warm up first in flowing N2 at 1010 K then successively in flowing O2 at 1050 C,1055 C and 1060 C. Samples were slow-cooled after each 10h reaction.					Heat capacity and transport studies of the ferromagnetic superconductor RuSr2GdCu2O8	200003		Industrial Research Ltd., P.O.Box 31310, Lower Hutt, New Zealand	Phys.Rev.B,61(2000)R6471-R6474	C.Bernhard,G.V.M.Williams,J.L.Tallon,J.W.Loram		
30722	PR06106471	grain size: 2-10 um	RuSr2Gd(Cu,Zn)2Oz	Ru1Sr2Gd1Cu1.99Zn0.01OZ	Ru	1	Sr	2	Gd	1	Cu	1.99	Zn	0.01											O	Z		6	2000																												Ru1212																		K		37	46				37		R																																																																				TP30722	mohmcm				8.6			8.6				12.5												RuO2, SrCO3,160Gd2O3,CuO		The mixed powder warm up first in flowing N2 at 1010 K then successively in flowing O2 at 1050 C,1055 C and 1060 C. Samples were slow-cooled after each 10h reaction.					Heat capacity and transport studies of the ferromagnetic superconductor RuSr2GdCu2O8	200003		Industrial Research Ltd., P.O.Box 31310, Lower Hutt, New Zealand	Phys.Rev.B,61(2000)R6471-R6474	C.Bernhard,G.V.M.Williams,J.L.Tallon,J.W.Loram		
30723	PR06106471	grain size: 2-10 um	RuSr2Gd(Cu,Zn)2Oz	Ru1Sr2Gd1Cu1.98Zn0.02OZ	Ru	1	Sr	2	Gd	1	Cu	1.98	Zn	0.02											O	Z		6	2000																												Ru1212																		K		30	40				30		R																																																																					mohmcm				8			10.8				13												RuO2, SrCO3,160Gd2O3,CuO		The mixed powder warm up first in flowing N2 at 1010 K then successively in flowing O2 at 1050 C,1055 C and 1060 C. Samples were slow-cooled after each 10h reaction.					Heat capacity and transport studies of the ferromagnetic superconductor RuSr2GdCu2O8	200003		Industrial Research Ltd., P.O.Box 31310, Lower Hutt, New Zealand	Phys.Rev.B,61(2000)R6471-R6474	C.Bernhard,G.V.M.Williams,J.L.Tallon,J.W.Loram		
30724	PR06106471	grain size: 2-10 um	RuSr2Gd(Cu,Zn)2Oz	Ru1Sr2Gd1Cu1.96Zn0.04OZ	Ru	1	Sr	2	Gd	1	Cu	1.96	Zn	0.04											O	Z		6	2000																												Ru1212																		K		12.8	25				12.8		R																																																																					mohmcm				32			46				22												RuO2, SrCO3,160Gd2O3,CuO		The mixed powder warm up first in flowing N2 at 1010 K then successively in flowing O2 at 1050 C,1055 C and 1060 C. Samples were slow-cooled after each 10h reaction.					Heat capacity and transport studies of the ferromagnetic superconductor RuSr2GdCu2O8	200003		Industrial Research Ltd., P.O.Box 31310, Lower Hutt, New Zealand	Phys.Rev.B,61(2000)R6471-R6474	C.Bernhard,G.V.M.Williams,J.L.Tallon,J.W.Loram		
30800	PR06109707	In this system, superconducting gap in the outer CuO2 planes does not fully develop below Tc=117K but below Tc2=60K Which is messured by NMR in this paper.	(Cu,C)Ba2Ca3Cu4O12+x	Cu4.6C0.4Ba2Ca3O12+Z	Cu	4.6	C	0.4	Ba	2	Ca	3													O	12+Z		1	2000																												Cu1234							3											K				117			117		MT																																																																																													1	High-pressure synthesis technique. Ref.7.					Effect of carrier distribution on superconducting characteristics of the multilayered high-Tc cuprate (Cu0.6C0.4)Ba2Ca3Cu4O12+y : <63>Cu-NMR study	200004		Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B,61(2000)9707-9710	A.Iyo,H.Ihara,K.Asayama,K.Ishida,K.Tokiwa,Y.Kitaoka,Y.Tokunaga		
30801	PR06109269	In this paper PPNET is determined by eq.:lc=c/wps. wps is c-axis plasma frequency.	(Bi,Pb)2(Sr,Pb)2CaCu2Oz	Bi1.6Pb0.6Sr1.8Ca1Cu2OZ	Bi	1.6	Pb	0.6	Sr	1.8	Ca	1	Cu	2											O	Z		3	2000																												Bi2212																				65				5	65		MT																																							um				12.6																																																		7	ref 7,8. Annealed at 400C for 72h in asealed quartz tube with pure oxgen gas of the effective pressure P=2.1atm.				Bi:Pb:Sr:Ca:Cu=1.76:0.46:1.89:1.02:2.0 by ICP.	Observation of the Josephson plasma reflectivity edge in the infrared region in Bi-based superconducting cuprates	200004		Department of Applied Chemistry, University of Tokyo, Hongo 7-3-1, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B,61(2000)R9269-R9272	J. Shimoyama,J.Shimoyama,K. Kishio,K. Kitazawa,K. M. Kojima,K.Kishio,K.Kitazawa,K.M.Kojima,S. Tajima,S. Uchida,S.Tajima,S.Uchida,T. Motohashi,T.Motohashi		
30900	PR06111317		HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+Z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+Z		5	2000																												Hg1223																			131					2	131		R																											T/K				2	HIR30900																																					ohmcm									62															16	Sample were grown with re-doped Ba2Ca2Cu3Oz precursor powder by using plused-laser deposition followed by post annealing of Hg. The asgrown film on (100) SrTiO3.				340 C O2 annealing	Vortex phase diagram of HgBa2Ca2Cu3O8+z thin films from magnetoresistance measurements	200005		National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B,61(2000)11317-11320	Mun-Seog Kim,Sung-Ik Lee,W.N.Kang,Wan-Seon Kim		
30901	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z		1	2000																												Bi2201							3														20				20		R																																																																				TP30901	ohmcm	0.011			0.02			0.02				0.035													1	asgrown					Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30902	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.7La0.3Cu1O6+Z	Bi	2	Sr	1.7	La	0.3	Cu	1													O	6+Z		1	2000																												Bi2201							3														28				28		R																																																																				TP30902	ohmcm				0.021			0.02				0.042													1	asgrown					Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30903	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6+Z	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+Z		1	2000																												Bi2201							3														28				28		R																																																																				TP30903	ohmcm				0.037			0.032				0.065													1	asgrown					Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30904	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.3La0.7Cu1O6+Z	Bi	2	Sr	1.3	La	0.7	Cu	1													O	6+Z		1	2000																												Bi2201							3														20				20		R																																																																				TP30904	ohmcm	0.04			0.07			0.8				0.08													1	asgrown					Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30905	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.2La0.8Cu1O6+Z	Bi	2	Sr	1.2	La	0.8	Cu	1													O	6+Z		1	2000																												Bi2201							3																																																																																								TP30905	ohmcm	0.75			0.28							0.21													1	asgrown					Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30906	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z		1	2000																												Bi2201							3																																																																																									ohmcm	0.98			0.082							0.1													1					in vacuum for 6h at 400 C	Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30907	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z		1	2000																												Bi2201							3																																																																																									ohmcm	0.14			0.12							0.13													1					in vacuum for 6h at 500 C	Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30908	PR06111321		Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+Z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+Z		1	2000																												Bi2201							3																																																																																									ohmcm	0.47			0.29							0.23													1					in vacuum for 6h at 600 C	Unusual Tc variation with hole concentration in Bi2Sr2-xLaxCuO6+z	200005		Department of Physics and Institute of Basic Sciences, Sungkyunkwan University, Suwon 440-746, Korea	Phys.Rev.B,61(2000)11321-11323	J.S.Kim,Mu-Yong Choi		
30909	PR06111332	film composition:Bi1.79Pr0.2Ca2.64Cu1.59	Bi2(Pr,Ca)2(Ca,Pr)Cu2O8	Bi2Pr0.2Ca2.8Cu2O8+Z	Bi	2	Pr	0.2	Ca	2.8	Cu	2													O	8+Z		4	2000																												Bi2212						30.02	1												65	72.5	80				72.5		R																																																																					mohmcm				1.2			1.3				1.9														The laser ablation method..Pellets were heated at 820 C for 10 h in air and powder placed in a chamber at of 10E-7 Torr and ahated by a pulused KeE excima laser					Impact of Pr doping on superconductivity in Bi2PrxCa3-xCu2O8+z	200005		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431 3192, Japan	Phys.Rev.B,61(2000)11332-11335	H.Sasakura,K.Yoshida,R.Oshima,S.Tsukui,T.Santoh,Y.Mizokawa		
30910	PR06111332	film composition:Bi1.65Pr0.3Ca2.53Cu1.71	Bi2(Pr,Ca)2(Ca,Pr)Cu2O8	Bi2Pr0.3Ca2.7Cu2O8+Z	Bi	2	Pr	0.3	Ca	2.7	Cu	2													O	8+Z		4	2000																												Bi2212						29.97	1												57	67	77				67		R																																																																					mohmcm				1.4			1.4				2.1														The laser ablation method..Pellets were heated at 820 C for 10 h in air and powder placed in a chamber at of 10E-7 Torr and ahated by a pulused KeE excima laser					Impact of Pr doping on superconductivity in Bi2PrxCa3-xCu2O8+z	200005		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431 3192, Japan	Phys.Rev.B,61(2000)11332-11335	H.Sasakura,K.Yoshida,R.Oshima,S.Tsukui,T.Santoh,Y.Mizokawa		
30911	PR06111332	film composition:Bi1.79Pr0.4Ca2.82Cu1.77	Bi2(Pr,Ca)2(Ca,Pr)Cu2O8	Bi2Pr0.4Ca2.6Cu2O8+Z	Bi	2	Pr	0.4	Ca	2.6	Cu	2													O	8+Z		4	2000																												Bi2212						29.95	1												20	37.5	55				37.5		R																																																																					mohmcm				1.7			1.5				2.4														The laser ablation method..Pellets were heated at 820 C for 10 h in air and powder placed in a chamber at of 10E-7 Torr and ahated by a pulused KeE excima laser					Impact of Pr doping on superconductivity in Bi2PrxCa3-xCu2O8+z	200005		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431 3192, Japan	Phys.Rev.B,61(2000)11332-11335	H.Sasakura,K.Yoshida,R.Oshima,S.Tsukui,T.Santoh,Y.Mizokawa		
30912	PR06111332	film composition:Bi1.91Pr0.5Ca2.43Cu1.81	Bi2(Pr,Ca)2(Ca,Pr)Cu2O8	Bi2Pr0.5Ca2.5Cu2O8+Z	Bi	2	Pr	0.5	Ca	2.5	Cu	2													O	8+Z		4	2000																												Bi2212						29.92	1												15	30	45				30		R																																																																					mohmcm				4.3			4.8				4.6														The laser ablation method..Pellets were heated at 820 C for 10 h in air and powder placed in a chamber at of 10E-7 Torr and ahated by a pulused KeE excima laser					Impact of Pr doping on superconductivity in Bi2PrxCa3-xCu2O8+z	200005		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431 3192, Japan	Phys.Rev.B,61(2000)11332-11335	H.Sasakura,K.Yoshida,R.Oshima,S.Tsukui,T.Santoh,Y.Mizokawa		
30913	PR06111332	film composition:Bi1.57Pr0.6Ca2.09Cu1.56	Bi2(Pr,Ca)2(Ca,Pr)Cu2O8	Bi2Pr0.6Ca2.4Cu2O8+Z	Bi	2	Pr	0.6	Ca	2.4	Cu	2													O	8+Z		4	2000																												Bi2212						29.94	1																																																																																									mohmcm				7							6.1														The laser ablation method..Pellets were heated at 820 C for 10 h in air and powder placed in a chamber at of 10E-7 Torr and ahated by a pulused KeE excima laser					Impact of Pr doping on superconductivity in Bi2PrxCa3-xCu2O8+z	200005		Department of Physics, Hamamatsu University School of Medicine, Handa-cho, Hamamatsu, Shizuoka 431 3192, Japan	Phys.Rev.B,61(2000)11332-11335	H.Sasakura,K.Yoshida,R.Oshima,S.Tsukui,T.Santoh,Y.Mizokawa		
30914	PR06111752		ErBa2Cu3Oz	Er1Ba2Cu3O6.93	Er	1	Ba	2	Cu	3															O		6.93	6	2000																												Y123				3.816	3.886	11.683	3														91				91		R																																																																					mohmcm							0.5				0.9												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30915	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.97Zn0.03O6.93	Er	1	Ba	2	Cu	2.97	Zn	0.03													O	Z	6.93	6	2000																												Y123				3.814	3.882	11.684	3														81				81		R																																																																					mohmcm							0.75				1.25												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30916	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.94Zn0.06O6.92	Er	1	Ba	2	Cu	2.94	Zn	0.06													O	Z	6.92	6	2000																												Y123				3.813	3.887	11.683	3														69				69		R																																																																					mohmcm				0.95			0.85				1.5												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30917	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.88Zn0.12O6.92	Er	1	Ba	2	Cu	2.88	Zn	0.12													O	Z	6.92	6	2000																												Y123				3.819	3.881	11.689	3														52				52		R																																																																					mohmcm				1.3			1.15				2.1												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30918	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.82Zn0.18O6.91	Er	1	Ba	2	Cu	2.82	Zn	0.18													O	Z	6.91	6	2000																												Y123				3.818	3.884	11.689	3														50				50		R																																																																					mohmcm				1.45			1.4				2.8												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30919	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.76Zn0.24O6.89	Er	1	Ba	2	Cu	2.76	Zn	0.24													O	Z	6.89	6	2000																												Y123				3.821	3.88	11.69	3														36				36		R																																																																					mohmcm				2.3			2.2				3.3												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30920	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.7Zn0.3O6.86	Er	1	Ba	2	Cu	2.7	Zn	0.3													O	Z	6.86	6	2000																												Y123				3.829	3.876	11.699	3														32				32		R																																																																					mohmcm				2.85			2.75				3.9												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30921	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.64Zn0.03O6.82	Er	1	Ba	2	Cu	2.64	Zn	0.03													O	Z	6.82	6	2000																												Y123				3.834	3.854	11.701	3																																																																																									mohmcm				3.4							4												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30922	PR06111752		ErBa2(Cu,Zn)3Oz	Er1Ba2Cu2.55Zn0.45O6.8	Er	1	Ba	2	Cu	2.55	Zn	0.45													O	Z	6.8	6	2000																												Y123				3.838	3.848	11.705	3																																																																																									mohmcm				4.05							4.25												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30923	PR06111752		ErBa2(Cu,Fe)3Oz	Er1Ba2Cu2.97Fe0.03O6.94	Er	1	Ba	2	Cu	2.97	Fe	0.03													O	Z	6.94	6	2000																												Y123				3.836	3.867	11.683	3														88				88		R																																																																					mohmcm							0.8				1.7												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30924	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.94Zn0.03Fe0.03O6.94	Er	1	Ba	2	Cu	2.94	Zn	0.03	Fe	0.03											O	Z	6.94	6	2000																												Y123				3.838	3.86	11.682	3														76				76		R																																																																					mohmcm							1.4				2												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30925	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.91Zn0.06Fe0.03O6.93	Er	1	Ba	2	Cu	2.91	Zn	0.06	Fe	0.03											O	Z	6.93	6	2000																												Y123				3.834	3.865	11.683	3														63				63		R																																																																					mohmcm				2.2			2.1				3.1												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30926	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.85Zn0.12Fe0.03O6.94	Er	1	Ba	2	Cu	2.85	Zn	0.12	Fe	0.03											O	Z	6.94	6	2000																												Y123				3.839	3.863	11.683	3														50				50		R																																																																					mohmcm				2.8			2.6				3.8												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30927	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.78Zn0.18Fe0.03O6.93	Er	1	Ba	2	Cu	2.78	Zn	0.18	Fe	0.03											O	Z	6.93	6	2000																												Y123				3.84	3.859	11.686	3														46				46		R																																																																					mohmcm				3.05			3				4.5												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30928	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.73Zn0.24Fe0.03O6.92	Er	1	Ba	2	Cu	2.73	Zn	0.24	Fe	0.03											O	Z	6.92	6	2000																												Y123				3.836	3.858	11.688	3														43				43		R																																																																					mohmcm				3.3			3.2				5.4												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30929	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.67Zn0.3Fe0.03O6.88	Er	1	Ba	2	Cu	2.67	Zn	0.3	Fe	0.03											O	Z	6.88	6	2000																												Y123				3.842	3.856	11.689	3																																																																																									mohmcm				5.5							6												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30930	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.61Zn0.36Fe0.03O6.85	Er	1	Ba	2	Cu	2.61	Zn	0.36	Fe	0.03											O	Z	6.85	6	2000																												Y123				3.85	3.855	11.69	3																																																																																									mohmcm				6.8							7												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30931	PR06111752		ErBa2(Cu,Fe)3Oz	Er1Ba2Cu2.91Fe0.09O6.96	Er	1	Ba	2	Cu	2.91	Fe	0.09													O	Z	6.96	6	2000																												Y123				3.854	3.854	11.681	3														83				83		R																																																																					mohmcm							1.5				2.7												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30932	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.88Zn0.03Fe0.09O6.95	Er	1	Ba	2	Cu	2.88	Zn	0.03	Fe	0.09											O	Z	6.95	6	2000																												Y123				3.859	3.859	11.681	3														65				65		R																																																																					mohmcm					2.4		2.8				3.05												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30933	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.85Zn0.06Fe0.09O6.96	Er	1	Ba	2	Cu	2.85	Zn	0.06	Fe	0.09											O	Z	6.96	6	2000																												Y123				3.856	3.856	11.68	3														46				46		R																																																																					mohmcm					3.4		3.3				4.3												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30934	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.79Zn0.12Fe0.09O6.95	Er	1	Ba	2	Cu	2.79	Zn	0.12	Fe	0.09											O	Z	6.95	6	2000																												Y123				3.863	3.863	11.68	3														42				42		R																																																																					mohmcm					4		4				4.8												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30935	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.73Zn0.18Fe0.09O6.94	Er	1	Ba	2	Cu	2.73	Zn	0.18	Fe	0.09											O	Z	6.94	6	2000																												Y123				3.86	3.86	11.678	3														37				37		R																																																																					mohmcm					6.1		6.2				6.3												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30936	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.67Zn0.24Fe0.09O6.94	Er	1	Ba	2	Cu	2.67	Zn	0.24	Fe	0.09											O	Z	6.94	6	2000																												Y123				3.861	3.861	11.6775	3														32				32		R																																																																					mohmcm					7.2		7.4				8.2												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30937	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.61Zn0.3Fe0.09O6.9	Er	1	Ba	2	Cu	2.61	Zn	0.3	Fe	0.09											O	Z	6.9	6	2000																												Y123				3.857	3.857	11.67	3																																																																																									mohmcm					10.7						10.5												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30938	PR06111752		ErBa2(Cu,Fe)3Oz	Er1Ba2Cu2.82Fe0.18O6.97	Er	1	Ba	2	Cu	2.82	Fe	0.18													O	Z	6.97	6	2000																												Y123				3.853	3.853	11.68	3														72				72		R																																																																					mohmcm							3.4				3.5												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30939	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.79Zn0.03Fe0.18O6.97	Er	1	Ba	2	Cu	2.79	Zn	0.03	Fe	0.18											O	Z	6.97	6	2000																												Y123				3.853	3.853	11.683	3														44				44		R																																																																					mohmcm				5.5			5.8				5.8												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30940	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.76Zn0.06Fe0.18O6.97	Er	1	Ba	2	Cu	2.76	Zn	0.06	Fe	0.18											O	Z	6.97	6	2000																												Y123				3.856	3.856	11.684	3														25				25		R																																																																					mohmcm				7.6			7.8				7.8												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30941	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.7Zn0.12Fe0.18O6.95	Er	1	Ba	2	Cu	2.7	Zn	0.12	Fe	0.18											O	Z	6.95	6	2000																												Y123				3.856	3.856	11.683	3														23				23		R																																																																					mohmcm				8			9.5				8.5												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30942	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.64Zn0.18Fe0.18O6.95	Er	1	Ba	2	Cu	2.64	Zn	0.18	Fe	0.18											O	Z	6.95	6	2000																												Y123				3.851	3.851	11.684	3														21				21		R																																																																					mohmcm				12.5			14				12.3												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30943	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.58Zn0.24Fe0.18O6.94	Er	1	Ba	2	Cu	2.58	Zn	0.24	Fe	0.18											O	Z	6.94	6	2000																												Y123				3.854	3.854	11.686	3																																																																																									mohmcm				15							14.3												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30944	PR06111752		ErBa2(Cu,Zn,Fe)3Oz	Er1Ba2Cu2.52Zn0.3Fe0.18O6.91	Er	1	Ba	2	Cu	2.52	Zn	0.3	Fe	0.18											O	Z	6.91	6	2000																												Y123				3.851	3.851	11.689	3																																																																																									mohmcm				20							17.4												Er2O3,BaCO3,CuO,ZnO,FeO3	1	The mixed sample calcined at 920 C in air for period of 16-20 h.After four intermediate grindings and calcination in air the material was crushed, ground, pelletized and sintered in O2 for 36h at 960C				intervening for 24 h at 600 C	Correlation between superconducting critical temperature and normal-state resistivity parameters from the codoped ErBa2Cu3-x-yZnxFeyO7-z system	200005		National Physical Laboratory, K. S. Krishnan Marg, New Delhi 110012, India	Phys.Rev.B,61(2000)11752-11761	A.Sedky,A.V.Narlikar,Anurag Gupta,Ratan Lal,V.P.S.Awana		
30945	PR06111762		YBa2Cu3Oz	Y1Ba2Cu3O6.25	Y	1	Ba	2	Cu	3															O	Z	6.25	1	2000																												Y123				3.8711	3.8711	11.807	3																																																																																																																		The powder loaded in to steel die and uniaxially pressed at 1000 lb and placed into a tube furnance under 1 atm of flowing O2 at 800 C  and raise to 960 C for 72 h and quenched.The cycle was repeated.				annealing condition in ref 23	Possible charge inhomogeneities in the CuO2 planes of YBa2Cu3O6+x (x=0.25, 0.45, 0.65, 0.94) from pulsed neutron diffraction	200005		Department of Physics and Astronomy and Center for Fundamental Materials Research, Michigan State University, East Lansing, Michigan 48824-1116	Phys.Rev.B,61(2000)11762-11768	E.L.Brosha,G.H.Kwei,M.Gutmann,S.J.L.Billinge		
30946	PR06111762		YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	Z	6.45	1	2000																												Y123				3.8556	3.884	11.749	3																																																																																																																		The powder loaded in to steel die and uniaxially pressed at 1000 lb and placed into a tube furnance under 1 atm of flowing O2 at 800 C  and raise to 960 C for 72 h and quenched.The cycle was repeated.				annealing condition in ref 23	Possible charge inhomogeneities in the CuO2 planes of YBa2Cu3O6+x (x=0.25, 0.45, 0.65, 0.94) from pulsed neutron diffraction	200005		Department of Physics and Astronomy and Center for Fundamental Materials Research, Michigan State University, East Lansing, Michigan 48824-1116	Phys.Rev.B,61(2000)11762-11768	E.L.Brosha,G.H.Kwei,M.Gutmann,S.J.L.Billinge		
30947	PR06111762		YBa2Cu3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	Z	6.65	1	2000																												Y123				3.8364	3.8965	11.724	3																																																																																																																		The powder loaded in to steel die and uniaxially pressed at 1000 lb and placed into a tube furnance under 1 atm of flowing O2 at 800 C  and raise to 960 C for 72 h and quenched.The cycle was repeated.				annealing condition in ref 23	Possible charge inhomogeneities in the CuO2 planes of YBa2Cu3O6+x (x=0.25, 0.45, 0.65, 0.94) from pulsed neutron diffraction	200005		Department of Physics and Astronomy and Center for Fundamental Materials Research, Michigan State University, East Lansing, Michigan 48824-1116	Phys.Rev.B,61(2000)11762-11768	E.L.Brosha,G.H.Kwei,M.Gutmann,S.J.L.Billinge		
30948	PR06111762		YBa2Cu3Oz	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	Z	6.94	1	2000																												Y123				3.8256	3.8944	11.693	3																																																																																																																		The powder loaded in to steel die and uniaxially pressed at 1000 lb and placed into a tube furnance under 1 atm of flowing O2 at 800 C  and raise to 960 C for 72 h and quenched.The cycle was repeated.				annealing condition in ref 23	Possible charge inhomogeneities in the CuO2 planes of YBa2Cu3O6+x (x=0.25, 0.45, 0.65, 0.94) from pulsed neutron diffraction	200005		Department of Physics and Astronomy and Center for Fundamental Materials Research, Michigan State University, East Lansing, Michigan 48824-1116	Phys.Rev.B,61(2000)11762-11768	E.L.Brosha,G.H.Kwei,M.Gutmann,S.J.L.Billinge		
30950	PR06112420	optimal	YBa2Cu3O6+X	Y1Ba2Cu3O6+Z	Y	1	Ba	2	Cu	3															O	6+Z		1	2000																												Y123																		K	91.1						91.1																				T	MH curve		100	67					T/K	MH curve	1.2																																																																	oriented powder Ref[32]:P. Manca et al., Nuovo Cimento D 19, 1009 (1997)					Superconducting fluctuations and anomalous diamagnetism in underdoped YBa2Cu3O6+x from magnetization and <63>Cu NMR-NQR relaxation measurements	200005		"Department of Physics ""A.Volta,"" Unita INFM di Pavia-Via Bassi, 6 I-27100 Pavia, Italy"	Phys.Rev.B,61(2000)12420-12426	A.Lascialfari,A.Rigamonti,A.Rosso,A.Varlamov,P.Carretta		
30951	PR06112420	underdope disordered	YBa2Cu3O6+X	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Z	6.66	1	2000																												Y123																		K	63.32						63.32																				T	MH curve			70					T/K	MH curve	1.05																																																																	oriented powder Ref[32]:P. Manca et al., Nuovo Cimento D 19, 1009 (1997)					Superconducting fluctuations and anomalous diamagnetism in underdoped YBa2Cu3O6+x from magnetization and <63>Cu NMR-NQR relaxation measurements	200005		"Department of Physics ""A.Volta,"" Unita INFM di Pavia-Via Bassi, 6 I-27100 Pavia, Italy"	Phys.Rev.B,61(2000)12420-12426	A.Lascialfari,A.Rigamonti,A.Rosso,A.Varlamov,P.Carretta		
30952	PR06112420	underdope chain-ordered	YBa2Cu3O6+X	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Z	6.66	1	2000																												Y123																		K	64.5						64.5																				T	MH curve		65	45					T/K	MH curve	1.1																																																																	oriented powder Ref[32]:P. Manca et al., Nuovo Cimento D 19, 1009 (1997)					Superconducting fluctuations and anomalous diamagnetism in underdoped YBa2Cu3O6+x from magnetization and <63>Cu NMR-NQR relaxation measurements	200005		"Department of Physics ""A.Volta,"" Unita INFM di Pavia-Via Bassi, 6 I-27100 Pavia, Italy"	Phys.Rev.B,61(2000)12420-12426	A.Lascialfari,A.Rigamonti,A.Rosso,A.Varlamov,P.Carretta		
30953	PR06112420	underdope chain-ordered	YBa2Cu3O6+X	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	Z	6.66	1	2000																												Y123																		K	64.2						64.2																				T	MH curve								T/K	MH curve	1																																																																	oriented powder Ref[32]:P. Manca et al., Nuovo Cimento D 19, 1009 (1997)					Superconducting fluctuations and anomalous diamagnetism in underdoped YBa2Cu3O6+x from magnetization and <63>Cu NMR-NQR relaxation measurements	200005		"Department of Physics ""A.Volta,"" Unita INFM di Pavia-Via Bassi, 6 I-27100 Pavia, Italy"	Phys.Rev.B,61(2000)12420-12426	A.Lascialfari,A.Rigamonti,A.Rosso,A.Varlamov,P.Carretta		
30954	PR06111769	As prepared	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		1	2000																												Hg1201	P4/mmm		A	3.8785		9.4998		1																																																																																																																1	precursor at 18kbar 1193K precursor Ba2CuOy+HgO ; anneal 523K 1bar Ar 24h;					Local Oz probing in the high-Tc superconductor HgBa2CuO4+z	200005		CERN-EP/SC, CH-1211 Geneva 23, Switzerland	Phys.Rev.B,61(2000)11769-11775	B.Ctortecka,H.Haas,ISOLDE Collaboration,J.C.Soares,J.G.Correia,J.G.Marques,J.J.Capponi,J.P.Araujo,P.Bordet,P.Toulemonde,R.Gatt,S.Le Floch,S.M.Loureiro,T.Butz,W.Troger		
30955	PR06111769	1st Exp.	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		1	2000																												Hg1201	P4/mmm		A	3.8801		9.502		1										K					88																																																																																																	1	precursor at 18kbar 1193K precursor Ba2CuOy+HgO ; anneal 523K 1bar Ar 24h; 490K 220 min Ar					Local Oz probing in the high-Tc superconductor HgBa2CuO4+z	200005		CERN-EP/SC, CH-1211 Geneva 23, Switzerland	Phys.Rev.B,61(2000)11769-11775	B.Ctortecka,H.Haas,ISOLDE Collaboration,J.C.Soares,J.G.Correia,J.G.Marques,J.J.Capponi,J.P.Araujo,P.Bordet,P.Toulemonde,R.Gatt,S.Le Floch,S.M.Loureiro,T.Butz,W.Troger		
30956	PR06111769	3rd Exp.	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		1	2000																												Hg1201	P4/mmm		A	3.882		9.506		1																																																																																																																1	precursor at 18kbar 1193K precursor Ba2CuOy+HgO ; anneal 523K 1bar Ar 24h; 490K 180 min Ar					Local Oz probing in the high-Tc superconductor HgBa2CuO4+z	200005		CERN-EP/SC, CH-1211 Geneva 23, Switzerland	Phys.Rev.B,61(2000)11769-11775	B.Ctortecka,H.Haas,ISOLDE Collaboration,J.C.Soares,J.G.Correia,J.G.Marques,J.J.Capponi,J.P.Araujo,P.Bordet,P.Toulemonde,R.Gatt,S.Le Floch,S.M.Loureiro,T.Butz,W.Troger		
30957	PR06111769	2nd Exp.	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		1	2000																												Hg1201	P4/mmm		A	3.8768		9.4981		1																																																																																																																1	precursor at 18kbar 1193K precursor Ba2CuOy+HgO ; anneal 523K 1bar Ar 24h; 490K 200 min O2					Local Oz probing in the high-Tc superconductor HgBa2CuO4+z	200005		CERN-EP/SC, CH-1211 Geneva 23, Switzerland	Phys.Rev.B,61(2000)11769-11775	B.Ctortecka,H.Haas,ISOLDE Collaboration,J.C.Soares,J.G.Correia,J.G.Marques,J.J.Capponi,J.P.Araujo,P.Bordet,P.Toulemonde,R.Gatt,S.Le Floch,S.M.Loureiro,T.Butz,W.Troger		
30958	PR06111769	4th Exp.	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		1	2000																												Hg1201	P4/mmm		A	3.8758		9.495		1																																																																																																																1	precursor at 18kbar 1193K precursor Ba2CuOy+HgO ; anneal 523K 1bar Ar 24h; 490K 240 min O2					Local Oz probing in the high-Tc superconductor HgBa2CuO4+z	200005		CERN-EP/SC, CH-1211 Geneva 23, Switzerland	Phys.Rev.B,61(2000)11769-11775	B.Ctortecka,H.Haas,ISOLDE Collaboration,J.C.Soares,J.G.Correia,J.G.Marques,J.J.Capponi,J.P.Araujo,P.Bordet,P.Toulemonde,R.Gatt,S.Le Floch,S.M.Loureiro,T.Butz,W.Troger		
30959	PR06112404		SmBa2Cu3Oz	Sm1Ba-1Cu3O6.94	Sm	1	Ba	-1	Cu	3															O	Z	6.94	1	2000																												Y123			A	3.847	3.902	11.735	3													86.3					86.3																																																																		microV/K	5			TP30959																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
30960	PR06112404		Sm(Ba,Pr)2Cu3Oz	Sm1Ba1.9Pr0.1Cu3O6.99	Sm	1	Ba	1.9	Pr	0.1	Cu	3													O	Z	6.99	1	2000																												Y123			A	3.853	3.9	11.7	3													56.4					56.4																																																																		microV/K	20			TP30960																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
30961	PR06112404		Sm(Ba,Pr)2Cu3Oz	Sm1Ba1.85Pr0.15Cu3O7.02	Sm	1	Ba	1.85	Pr	0.15	Cu	3													O	Z	7.02	1	2000																												Y123			A	3.85	3.898	11.69	3													35					35																																																																		microV/K	28			TP30961																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
30962	PR06112404		Sm(Ba,Pr)2Cu3Oz	Sm1Ba1.8Pr0.2Cu3O7.04	Sm	1	Ba	1.8	Pr	0.2	Cu	3													O	Z	7.04	1	2000																												Y123			A	3.862	3.888	11.665	3													26.5					26.5																																																																		microV/K	36			TP30962																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
30963	PR06112404	not s/c 	Sm(Ba,Pr)2Cu3Oz	Sm1Ba1.7Pr0.3Cu3O7.07	Sm	1	Ba	1.7	Pr	0.3	Cu	3													O	Z	7.07	1	2000																												Y123			A	3.878	3.883	11.63	3																4.2																																																																				microV/K	90			TP30963																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
30964	PR06112404	not s/c 	Sm(Ba,Pr)2Cu3Oz	Sm1Ba1.65Pr0.35Cu3O7.1	Sm	1	Ba	1.65	Pr	0.35	Cu	3													O	Z	7.1	1	2000																												Y123			A	3.875	3.875	11.625	3																4.2																																																																				microV/K	120			TP30964																										950C 24h 2-3 times Anneal flow O2 450C 24h					Effect of praseodymium on the normal-state and superconducting properties of RBa2Cu3Oy: A comparative study of the role of the Pr ion on R and Ba sites	200005		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St. Petersburg 195 251, Russia	Phys.Rev.B,61(2000)12404-12411	M.V.Elizarova,R.Suryanarayanan,V.E.Gasumyants		
31000	PR06114956	nominal x=0.2. hole p=0.18 	Bi2(Sr,La)2CuO6	Bi2Sr1.77La0.23Cu1O6+Z	Bi	2	Sr	1.77	La	0.23	Cu	1													O	6+Z		3	2000																												Bi2201							5											K				31.5			31.5		1																																																																uV/K	-13.7																								RH31000				7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31001	PR06114956	nominal x=0.4. hole p=0.16 	Bi2(Sr,La)2CuO6	Bi2Sr1.61La0.39Cu1O6+D	Bi	2	Sr	1.61	La	0.39	Cu	1													O	6+D		3	2000																												Bi2201							5											K				36			36		1																																																																uV/K	-3.84																								RH31001				7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31002	PR06114956	nominal x=0.5. hole p=0.15 	Bi2(Sr,La)2CuO6	Bi2Sr1.51La0.49Cu1O6+D	Bi	2	Sr	1.51	La	0.49	Cu	1													O	6+D		3	2000																												Bi2201							5											K				33.5			33.5		1																																																																uV/K	2.74																												7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31003	PR06114956	hole p=0.14 	Bi2(Sr,La)2CuO6	Bi2Sr1.49La0.51Cu1O6+D	Bi	2	Sr	1.49	La	0.51	Cu	1													O	6+D		3	2000																												Bi2201							5											K				28.5			28.5		1																																																																uV/K	3.29																												7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31004	PR06114956	nominal x=0.6. hole p=0.13 	Bi2(Sr,La)2CuO6	Bi2Sr1.34La0.66Cu1O6+D	Bi	2	Sr	1.34	La	0.66	Cu	1													O	6+D		3	2000																												Bi2201							5											K				24			24		1																																																																uV/K	13.1																												7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31005	PR06114956	nominal x=0.7. hole p=0.12 from thermopower. 	Bi2(Sr,La)2CuO6	Bi2Sr1.27La0.73Cu1O6+D	Bi	2	Sr	1.27	La	0.73	Cu	1													O	6+D		3	2000																												Bi2201							5											K				17			17		1																																																																V/K	21.9																								RH31005				7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31006	PR06114956	nominal x=0.8. hole p=0.10 from thermopower. 	Bi2(Sr,La)2CuO6	Bi2Sr1.16La0.84Cu1O6+D	Bi	2	Sr	1.16	La	0.84	Cu	1													O	6+D		3	2000																												Bi2201							5											K																																																																									uV/K	43.3																								RH31006				7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31007	PR06114956	nominal x=1.0. hole p=0.03 from thermopower. 	Bi2(Sr,La)2CuO6	Bi2Sr0.98La1.02Cu1O6+D	Bi	2	Sr	0.98	La	1.02	Cu	1													O	6+D		3	2000																												Bi2201							5											K																																																																									uV/K	125.5																								RH31007				7	ref.6.All the crystals are annealed in flowing oxygen at 650 C for 48 h.				The actual La concentration are determined by ICP and EPMA	Carrier concentrations in Bi2Sr2-zLazCuO6 +z  single crystals and their relation to the Hall coefficient and thermopower	200006		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,61,(2000)R14956-R14959	Kouji Segawa,N. Miyamoto,S. Ono,Seiki Komiya,T. Murayama,Y. Hanaki,Yoichi Ando		
31008	PR06114960		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		6	2000							145																					Ru1212																		K				45			45		2																																																																																													1	ref.7.					Evidence for a bulk Meissner state in the ferromagnetic superconductor RuSr2GdCu2O8 from dc magnetization	200006		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.B,61,(2000)R14960-R14963	C. Bernhard,E. Brucher,J. L. Tallon,R. K. Kremer		
31009	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr2Cu1OY	Bi	1.8	Pb	0.2	Sr	2	Cu	1													O	Y		2	2000																												Bi2201							3											K		15.2				2.38	15.2		1																																																																																												Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31010	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.9La0.1Cu1OY	Bi	1.8	Pb	0.2	Sr	1.9	La	0.1	Cu	1											O	Y		2	2000																												Bi2201							3											K		20.2				2.697	20.2		1																																																																					mOHMcm				0.7			1.9																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31011	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.8La0.2Cu1OY	Bi	1.8	Pb	0.2	Sr	1.8	La	0.2	Cu	1											O	Y		2	2000																												Bi2201							3											K		21.2				2.807	21.2		1																																																																					mOHMcm				0.9			2.1																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31012	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.7La0.3Cu1OY	Bi	1.8	Pb	0.2	Sr	1.7	La	0.3	Cu	1											O	Y		2	2000																												Bi2201							3											K		27.4				3.108	27.4		1																																																																					mOHMcm				1.3			2.7																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31013	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.55La0.45Cu1OY	Bi	1.8	Pb	0.2	Sr	1.55	La	0.45	Cu	1											O	Y		2	2000																												Bi2201							3											K		28.3				2.957	28.3		1																																																																					mOHMcm				1.8			4																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31014	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.45La0.55Cu1OY	Bi	1.8	Pb	0.2	Sr	1.45	La	0.55	Cu	1											O	Y		2	2000																												Bi2201							3											K		28.6				3.086	28.6		1																																																																					mOHMcm				2.3			4.8																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31015	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.4La0.6Cu1OY	Bi	1.8	Pb	0.2	Sr	1.4	La	0.6	Cu	1											O	Y		2	2000																												Bi2201							3											K		28.3				3.128	28.3		1																																																																					mOHMcm				3			6.2																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31016	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.35La0.65Cu1OY	Bi	1.8	Pb	0.2	Sr	1.35	La	0.65	Cu	1											O	Y		2	2000																												Bi2201							3											K		27.8				3.198	27.8		1																																																																					mOHMcm				6.2			9.2																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31017	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.25La0.75Cu1OY	Bi	1.8	Pb	0.2	Sr	1.25	La	0.75	Cu	1											O	Y		2	2000																												Bi2201							3											K		26.9				3.173	26.9		1																																																																					mOHMcm				12.7			13.9																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31018	PR06115436		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.2La0.8Cu1OY	Bi	1.8	Pb	0.2	Sr	1.2	La	0.8	Cu	1											O	Y		2	2000																												Bi2201							3											K		24.9				3.119	24.9		1																																																																					mOHMcm				17.7			17.6																Bi2O3, PbO, SrCO3, La2O3, CuO.	1	(Grownd and calsined at 900 C for 12 h in air.)*2. Pressed into pellets and sinterd inair at925 C for 24 h. Then annealed at 600 C for 17 h and furnace cooled to room temperature.					Superconductivity and the valence state of the Sr site in defective Bi1.8Pb0.2Sr2CuOy	200006		Structure Research Laboratory, University of Science and Technology of China, Hefei, 230026 Anhui, People's Republic of China	Phys.Rev.B,61,(2000)15436-15441	Mao Zhiqiang,Yan Hongjie,Zhang Yuheng		
31019	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+D	Hg	1	Ba	2	Ca	2	Cu	3													O	8+D		2	2000																												Hg,Re-1223			A	3.8542		15.8359	3											K																																																																																																					Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31020	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.95Re0.05Ba2Ca2Cu3O8+D	Hg	0.95	Re	0.05	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85366		15.7424	3											K				132.52			132.52		2																																																																																												Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31021	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.9Re0.1Ba2Ca2Cu3O8+D	Hg	0.9	Re	0.1	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85132		15.6922	3											K				132.62			132.62		2																																																																																												Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31022	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.85Re0.15Ba2Ca2Cu3O8+D	Hg	0.85	Re	0.15	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85635		15.6973	3											K				132.92			132.92		2																																																																																												Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31023	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+D	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85196		15.6863	3											K				133.12		3	133.12		2	K/Gpa	6.82																																																																																										Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31024	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.8Re0.2Ba2Ca2Cu3O8+D	Hg	0.8	Re	0.2	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85343		15.6843	3											K				133.12			133.12		2																																																																																												Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31025	PR06115454		(Hg,Re)Ba2Ca2Cu3O8	Hg0.75Re0.25Ba2Ca2Cu3O8+D	Hg	0.75	Re	0.25	Ba	2	Ca	2	Cu	3											O	8+D		2	2000																												Hg,Re-1223			A	3.85488		15.7104	3											K				132.72			132.72		2																																																																																												Ba2Ca2Cu3O7+d,ReO2,HgO	1	Ba2Ca2Cu3O7+d and ReO2 heated at 930C for 10h,annealed in Ar(90%)-O2(10%) gas,then mixed with HgO,prepared by TBA(ref.14) with ff=0.7g/cm3,heated at 860C for 10h.					Effect of hydrostatic pressure on HgBa2Ca2Cu3O8 +z  superconductor doped with Re	200006		Centro Brasilero de Pesquisas Fisicas, Rio de Janeiro, RJ 22290-180, Brazil	Phys.Rev.B,61,(2000)15454-15461	A. Eichler,A. G. Cunha,A. Sin,Baggio-Saitovitch,E. V. L. de Mello,H. Belich,M. T. D. Orlando,T. Burghardt,X. Obradors		
31026	PR06114350		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		2	2000																												T							3											K		28.7					28.7		1																																																																																												La2O3,SrCO3,CuO.ref.5.	1						Impurity scattering effects on the low-temperature specific heat of d-wave superconductors	200006		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,61,(2000)14350-14353	C. F. Chang,H. D. Yang,J.-Y. Lin		
31027	PR06114350		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.99Ni0.01O4	La	1.78	Sr	0.22	Cu	0.99	Ni	0.01													O	4		2	2000																												T							3											K		21.2					21.2		1																																																																																												La2O3,SrCO3,CuO.ref.5.	1						Impurity scattering effects on the low-temperature specific heat of d-wave superconductors	200006		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,61,(2000)14350-14353	C. F. Chang,H. D. Yang,J.-Y. Lin		
31028	PR06114350		(La,Sr)2(Cu,Ni)O4	La1.78Sr0.22Cu0.98Ni0.02O4	La	1.78	Sr	0.22	Cu	0.98	Ni	0.02													O	4		2	2000																												T							3											K		17.4					17.4		1																																																																																												La2O3,SrCO3,CuO.ref.5.	1						Impurity scattering effects on the low-temperature specific heat of d-wave superconductors	200006		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B,61,(2000)14350-14353	C. F. Chang,H. D. Yang,J.-Y. Lin		
31029	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	PrBa2Cu3O7+z	Pr1Ba2Cu3O6.88	Pr	1	Ba	2	Cu	3															O	7-Z	6.88	2	2000								18																			3	Y123	Pmmm		A	3.827	3.927	11.709	3											K					2																																																																									mOHMcm							34																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31030	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.1Ba1.9Cu3O6.93	Pr	1.1	Ba	1.9	Cu	3															O	7-Z	6.93	2	2000								17																			3	Y123	Pmmm		A	3.876	3.918	11.688	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31031	PR06114825	Specific heat was measured. The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.2Ba1.8Cu3O7	Pr	1.2	Ba	1.8	Cu	3															O	7-Z	7	2	2000								15.5																			3	Y123	Pmmm		A	3.88793	3.90523	11.66619	3											K					2																																																																									mOHMcm							54																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31032	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.3Ba1.7Cu3O7.05	Pr	1.3	Ba	1.7	Cu	3															O	7-Z	7.05	2	2000								13.5																			3	Y123	Pmmm		A	3.892	3.898	11.643	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31033	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.4Ba1.6Cu3O7.11	Pr	1.4	Ba	1.6	Cu	3															O	7-Z	7.11	2	2000								12																			2	Y123	P/4mmm		A	3.894		11.634	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31034	PR06114825	Specific heat was measured. The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.5Ba1.5Cu3O7.19	Pr	1.5	Ba	1.5	Cu	3															O	7-Z	7.19	2	2000								10.5																			2	Y123	P/4mmm		A	3.89163		11.61779	3											K					2																																																																									mOHMcm							456																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31035	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.6Ba1.4Cu3O7.23	Pr	1.6	Ba	1.4	Cu	3															O	7-Z	7.23	2	2000								8																			2	Y123	P/4mmm		A	3.888		11.601	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31036	PR06114825	Specific heat was measured.The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.7Ba1.3Cu3O7.25	Pr	1.7	Ba	1.3	Cu	3															O	7-Z	7.25	2	2000								5.5																			3	Y123	Cmmm		A	5.48853	5.4903	11.57759	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31037	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.8Ba1.2Cu3O7.27	Pr	1.8	Ba	1.2	Cu	3															O	7-Z	7.27	2	2000								2.2																			3	Y123	Cmmm		A	5.477	5.484	11.547	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31038	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr1.9Ba1.1Cu3O7.29	Pr	1.9	Ba	1.1	Cu	3															O	7-Z	7.29	2	2000																											3	Y123	Cmmm		A	5.469	5.476	11.52	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31039	PR06114825	The oxygen content was determined from precision iodometric titration method(ref.29).	Pr(Ba,Pr)2Cu3O7+z	Pr2Ba1Cu3O7.31	Pr	2	Ba	1	Cu	3															O	7-Z	7.31	2	2000																											3	Y123	Cmmm		A	5.46	5.469	11.496	3											K					2																																																																																																Pr6O11,BaCO3,CuO.	1	Mixed and calcined between 850C and 910C in air for 2days, then pressed into pellets and sintered in flowing Ar gas at 900-940C for 1day,finally annealed in flowing O2 gas at 400C for 1day.					Variation of anomalous Pr ordering and crystal symmetry for the oxygenated Pr1 + xBa2-xCu3O7 + y system	200006		Department of Physics, National Tsing Hua University, Hsinchu 300, Taiwan	Phys.Rev.B,61,(2000)14825-14832	B. N. Lin,C. H. Chang,C. H. Lin,H. C. Chiang,H. C. Ku,H. M. Luo,H.-C. I. Kao,J. B. Shi,J. C. Ho,S. R. Hwang,T. I. Hsu,T. J. Lee,W.-H. Li,Y. H. Lin,Y. Y. Hsu		
31100	PR06200615	under-doped	HgBa2CuO4+z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		6	2000																												Hg1201																		K				72			72																																																																		uV/K	16																											HgO(99%), BaO, CuO(3N)	1	BaO was purified from BaCO3(99.997%) in vacaum at 1050C.				post annealed condition: for 1week in 1 atm of Ar at 350 C	Photoemission study of electronic states in HgBa2CuO4 +z  with various doping levels	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,62,(2000)615-621	A. Koma,A. Yamamoto,H. Uchiyama,K. Saiki,S. Tajima,W.-Z. Hu		
31101	PR06200615	under-doped	HgBa2CuO4+z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		6	2000																												Hg1201																		K				83			83																																																																		uV/K	11																											HgO(99%), BaO, CuO(3N)	1	BaO was purified from BaCO3(99.997%) in vacaum at 1050C.				post annealed condition: for 1week in 1 atm of Ar at 300 C	Photoemission study of electronic states in HgBa2CuO4 +z  with various doping levels	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,62,(2000)615-621	A. Koma,A. Yamamoto,H. Uchiyama,K. Saiki,S. Tajima,W.-Z. Hu		
31102	PR06200615	optimal-doped	HgBa2CuO4+z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		6	2000																												Hg1201																		K				97			97																																																																		uV/K	3																											HgO(99%), BaO, CuO(3N)	1	BaO was purified from BaCO3(99.997%) in vacaum at 1050C.				post annealed condition: for 1week in 1 atm of O2 at 300 C	Photoemission study of electronic states in HgBa2CuO4 +z  with various doping levels	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,62,(2000)615-621	A. Koma,A. Yamamoto,H. Uchiyama,K. Saiki,S. Tajima,W.-Z. Hu		
31103	PR06200615	over-doped	HgBa2CuO4+z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		6	2000																												Hg1201																		K				92			92																																																																		uV/K	0																											HgO(99%), BaO, CuO(3N)	1	BaO was purified from BaCO3(99.997%) in vacaum at 1050C.				post annealed condition: for 3week in 1 atm of O2 at 260 C	Photoemission study of electronic states in HgBa2CuO4 +z  with various doping levels	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,62,(2000)615-621	A. Koma,A. Yamamoto,H. Uchiyama,K. Saiki,S. Tajima,W.-Z. Hu		
31104	PR06200615	over-doped	HgBa2CuO4+z	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z		6	2000																												Hg1201																		K				86			86																																																																		uV/K	-2																											HgO(99%), BaO, CuO(3N)	1	BaO was purified from BaCO3(99.997%) in vacaum at 1050C.				post annealed condition: for 3week in 1 atm of O2 at 240 C	Photoemission study of electronic states in HgBa2CuO4 +z  with various doping levels	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Phys.Rev.B,62,(2000)615-621	A. Koma,A. Yamamoto,H. Uchiyama,K. Saiki,S. Tajima,W.-Z. Hu		
31105	PR06200626		Bi2Sr2CaCu2O8+z	Bi2Sr2Ca1Cu2O8+Z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z		3	2000																												Bi2212																		K	92.4						92.4		2																																																											W/km										uohmcm								65				225												7					Zn-doped crystals are turned to the optimumdoping by annealing at 750C for 48h. The contain of Zn was determined by ICP.	Temperature- and magnetic-field-dependent thermal conductivity of pure and Zn-doped Bi2Sr2CaCu2O8+z  single crystals	200007		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,62,(2000)626-630	A. Kapitulnik,J. Takeya,K. Nakamura,Yasushi Abe,Yoichi Ando		
31106	PR06200626		Bi2Sr2Ca(Cu,Zn)2O8+z	Bi2Sr2Ca1Cu1.988Zn0.012O8+Z	Bi	2	Sr	2	Ca	1	Cu	1.988	Zn	0.012											O	8+Z		3	2000																												Bi2212																		K	84.5					1.5	84.5		2																																																											W/km										uohmcm								80				315												7					Zn-doped crystals are turned to the optimumdoping by annealing at 750C for 48h. The contain of Zn was determined by ICP.	Temperature- and magnetic-field-dependent thermal conductivity of pure and Zn-doped Bi2Sr2CaCu2O8+z  single crystals	200007		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B,62,(2000)626-630	A. Kapitulnik,J. Takeya,K. Nakamura,Yasushi Abe,Yoichi Ando		
31107	PR06200622	Annealing at 350C. TP300= at 290K. 	Bi2(Sr,Bi)2CuO6+z	Bi2.1Sr1.9Cu1O6+Z	Bi	2.1	Sr	1.9	Cu	1															O	6+Z		3	2000																												Bi2201							3											K		0					0		1																																																																uV/K	-12.9																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31108	PR06200622	Annealing at 680C. TP300= at 290K. 	Bi2(Sr,Bi)2CuO6	Bi2.1Sr1.9Cu1O6+Z	Bi	2.1	Sr	1.9	Cu	1															O	6+Z		3	2000																												Bi2201							3											K		0					0		1																																																																uV/K	-9.6																																	annealing condition: under air at 680C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31109	PR06200622	Annealing at 350C. TP300= at 290K.  	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.74La0.16Cu1O6+Z	Bi	2.1	Sr	1.74	La	0.16	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		7.5					7.5		1																																																																uV/K	-9.21																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31110	PR06200622	Annealing at 450 - 480 C. TP300= at 290 K.  	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.74La0.16Cu1O6+Z	Bi	2.1	Sr	1.74	La	0.16	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		9.03					9.03		1																																																																uV/K	-7.09																																	annealing condition: under air at 450C-480C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31111	PR06200622	Annealing at 350C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.63La0.27Cu1O6+Z	Bi	2.1	Sr	1.63	La	0.27	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		15.1					15.1		1																																																																uV/K	-5.24																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31112	PR06200622	Annealing at 450-480 C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.63La0.27Cu1O6+Z	Bi	2.1	Sr	1.63	La	0.27	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		14.1					14.1		1																																																																uV/K	-3.79																																	annealing condition: under air at 450C-480C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31113	PR06200622	Annealing at 350C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.58La0.32Cu1O6+Z	Bi	2.1	Sr	1.58	La	0.32	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		15					15		1																																																																uV/K	-5.24																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31114	PR06200622	Annealing at 450-480C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.58La0.32Cu1O6+Z	Bi	2.1	Sr	1.58	La	0.32	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		13.5					13.5		1																																																																uV/K	-3.79																																	annealing condition: under air at 450C-480C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31115	PR06200622	Annealing at 550-580C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.55La0.32Cu1O6+Z	Bi	2.1	Sr	1.55	La	0.32	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		12.1					12.1		1																																																																uV/K	-1.67																																	annealing condition: under air at 550C-580C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31116	PR06200622	Annealing at 350C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.55La0.35Cu1O6+Z	Bi	2.1	Sr	1.55	La	0.35	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		12					12		1																																																																uV/K	1.63																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31117	PR06200622	Annealing at 550-580C. TP300= at 290K.  	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.55La0.35Cu1O6+Z	Bi	2.1	Sr	1.55	La	0.35	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		8					8		1																																																																uV/K	4.27																																	annealing condition: under air at 450C-480C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31118	PR06200622	Annealing at 680C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.55La0.35Cu1O6+Z	Bi	2.1	Sr	1.55	La	0.35	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		5.95					5.95		1																																																																uV/K	6																																	annealing condition: under air at 550C-580C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31119	PR06200622	Annealing at 350C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.37La0.53Cu1O6+Z	Bi	2.1	Sr	1.37	La	0.53	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		18.1					18.1		1																																																																uV/K	1.5																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31120	PR06200622	Annealing at 450-480C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.37La0.53Cu1O6+Z	Bi	2.1	Sr	1.37	La	0.53	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		17.1					17.1		1																																																																uV/K	4.41																																	annealing condition: under air at 450C-480C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31121	PR06200622	Annealing at 680C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.37La0.53Cu1O6+Z	Bi	2.1	Sr	1.37	La	0.53	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		12.3					12.3		1																																																																uV/K	12.5																																	annealing condition: under air at 680C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31122	PR06200622	Annealing at 350 C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.15La0.75Cu1O6+Z	Bi	2.1	Sr	1.15	La	0.75	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		15.1					15.1		1																																																																uV/K	16.7																																	annealing condition: under air at 350C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31123	PR06200622	Annealing at 680C. TP300= at 290K. 	Bi2(Sr,Bi,La)2CuO6	Bi2.1Sr1.15La0.75Cu1O6+Z	Bi	2.1	Sr	1.15	La	0.75	Cu	1													O	6+Z		3	2000																												Bi2201							3											K		0					0		1																																																																uV/K	25.3																																	annealing condition: under air at 680C	Dragging excitation characteristics from thermoelectric power in Bi2(Sr2-yLay)CuO6 +z  single crystals	200007		Departement de Physique, Universite de Versailles St. Quentin, 45 Avenue des Etats-Unis, 78035 Versailles, France	Phys.Rev.B,62,(2000)622-625	C. Ayache,G. Collin,Y. Dumont		
31124	PR06200799		(La,Ba)2CuO4	La1.95Ba0.05Cu1O4+Z	La	1.95	Ba	0.05	Cu	1															O	4+Z		5	2000																												T																		K																																																																														mohmcm					4.5							8													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31125	PR06200799		(La,Ba)2CuO4	La1.925Ba0.075Cu1O4+Z	La	1.925	Ba	0.075	Cu	1															O	4+Z		5	2000																												T																		K	34						34		1																																																																					mohmcm					0.35			0.3				1.2													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31126	PR06200799		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4+Z	La	1.9	Ba	0.1	Cu	1															O	4+Z		5	2000																												T																		K	38						38		1																																																																					mohmcm					0.23			0.2				0.8													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31127	PR06200799		(La,Ba)2CuO4	La1.89Ba0.11Cu1O4+Z	La	1.89	Ba	0.11	Cu	1															O	4+Z		5	2000																												T																		K	38						38		1																																																																					mohmcm					0.3			0.2				0.95													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31128	PR06200799		(La,Ba)2CuO4	La1.88Ba0.12Cu1O4+Z	La	1.88	Ba	0.12	Cu	1															O	4+Z		5	2000																												T																		K	39						39		1																																																																					mohmcm					0.2			0.12				0.7													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31129	PR06200799		(La,Ba)2CuO4	La1.875Ba0.125Cu1O4+Z	La	1.875	Ba	0.125	Cu	1															O	4+Z		5	2000																												T																		K	6						6		1																																																																					mohmcm					0.8			1				2													electron-beam coevaporation method				STO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31130	PR06200799		(La,Ba)2CuO4	La1.875Ba0.125Cu1O4+Z	La	1.875	Ba	0.125	Cu	1															O	4+Z		5	2000																												T																		K	40						40		1																																																																					mohmcm					0.2			0.15				0.6													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31131	PR06200799		(La,Ba)2CuO4	La1.87Ba0.13Cu1O4+Z	La	1.87	Ba	0.13	Cu	1															O	4+Z		5	2000																												T																		K	41						41		1																																																																					mohmcm					0.13			0.1				0.58													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31132	PR06200799		(La,Ba)2CuO4	La1.86Ba0.14Cu1O4+Z	La	1.86	Ba	0.14	Cu	1															O	4+Z		5	2000																												T																		K	42						42		1																																																																					mohmcm					0.12			0.1				0.52													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31133	PR06200799		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4+Z	La	1.85	Ba	0.15	Cu	1															O	4+Z		5	2000																												T																		K	8						8		1																																																																					mohmcm					0.38			0.42				1													electron-beam coevaporation method				STO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31134	PR06200799		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4+Z	La	1.85	Ba	0.15	Cu	1															O	4+Z		5	2000																												T																		K	43						43		1																																																																					mohmcm					0.1			0.05				0.45													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31135	PR06200799		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4+Z	La	1.8	Ba	0.2	Cu	1															O	4+Z		5	2000																												T																		K	38						38		1																																																																					mohmcm					0.08			0.05				0.35													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31136	PR06200799		(La,Ba)2CuO4	La1.75Ba0.25Cu1O4+Z	La	1.75	Ba	0.25	Cu	1															O	4+Z		5	2000																												T																		K	29						29		1																																																																					mohmcm					0.05			0.055				0.23													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31137	PR06200799		(La,Ba)2CuO4	La1.7Ba0.3Cu1O4+Z	La	1.7	Ba	0.3	Cu	1															O	4+Z		5	2000																												T																		K	16						16		1																																																																					mohmcm					0.07			0.03				0.23													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31138	PR06200799		(La,Ba)2CuO4	La1.65Ba0.35Cu1O4+Z	La	1.65	Ba	0.35	Cu	1															O	4+Z		5	2000																												T																		K																																																																														mohmcm		0.135			0.16							0.31													electron-beam coevaporation method				LSAO substrates	Absence of 1/8  anomaly in strained thin films of La2-xBaxCuO4 +z	200007		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B,62,(2000)R799-R802	A. Matsuda,A. Tsukada,H. Sato,M. Naito		
31139	PR06201244		(Pr,Ce)2Sr2Cu2NbO10	Pr1.5Ce0.5Sr2Cu2Nb1O10	Pr	1.5	Ce	0.5	Sr	2	Cu	2	Nb	1											O	10		6	2000																												Nb1222			A	3.97		28.75												K			28				28																																																																																																					Detection of the nearly invisible defect that disrupts bulk superconductivity in Pr1.5Ce0.5Sr2Cu2NbO10	200007		Department of Physics, University of Notre Dame, Notre Dame, Indiana 46556	Phys.Rev.B,62,(2000)1244-1251	David B. Pulling,H. Luo,Howard A. Blackstead,Israel Felner,John D. Dow,M. Chen,W. B. Yelon		
31140	PR06201350		NdBa2Cu3O7-z	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z		3	2000																												Y123																		K			93.8				93.8		2																																																																																														ref 28				sample were grown under the same oxgen partial pressure of 0.1 % and fully oxygenated at 300 C for 150 h	Flux pinning by Nd4Ba2Cu2O10 inclusions in NdBa2Cu3O7-z superconductors: A combined effect of point, interface, and  delta kappa    pinning at elevated temperatures	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-16-25, Shibaura, Minato-ku, Tokyo 105-0023, Japan	Phys.Rev.B,62,(2000)1350-1360	Masato Murakami,Noriko Chikumoto,Tadashi Mochida		
31141	PR06201350	Nd4Ba2Cu2O10 inclusions (10 mol%)	NdBa2Cu3O7-z	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			2000																												Y123																		K			94.5				94.5		2																																																																																														ref 29				sample were grown under the same oxgen partial pressure of 0.1 % and fully oxygenated at 300 C for 150 h	Flux pinning by Nd4Ba2Cu2O10 inclusions in NdBa2Cu3O7-z superconductors: A combined effect of point, interface, and  delta kappa    pinning at elevated temperatures	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-16-25, Shibaura, Minato-ku, Tokyo 105-0023, Japan	Phys.Rev.B,62,(2000)1350-1360	Masato Murakami,Noriko Chikumoto,Tadashi Mochida		
31142	PR06201350	Nd4Ba2Cu2O10  (10 mol%) + Pt (0.5 wtl%) + CeO2 (1.0 wt%) inclusions	NdBa2Cu3O7-z	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			2000																												Y123																		K			94.5				94.5		2																																																																																														ref 30				sample were grown under the same oxgen partial pressure of 0.1 % and fully oxygenated at 300 C for 150 h	Flux pinning by Nd4Ba2Cu2O10 inclusions in NdBa2Cu3O7-z superconductors: A combined effect of point, interface, and  delta kappa    pinning at elevated temperatures	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-16-25, Shibaura, Minato-ku, Tokyo 105-0023, Japan	Phys.Rev.B,62,(2000)1350-1360	Masato Murakami,Noriko Chikumoto,Tadashi Mochida		
31143	PR06201350	Nd4Ba2Cu2O10 inclusions (20 mol%)	NdBa2Cu3O7-z	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			2000																												Y123																		K			94.5				94.5		2																																																																																														ref 29				sample were grown under the same oxgen partial pressure of 0.1 % and fully oxygenated at 300 C for 150 h	Flux pinning by Nd4Ba2Cu2O10 inclusions in NdBa2Cu3O7-z superconductors: A combined effect of point, interface, and  delta kappa    pinning at elevated temperatures	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-16-25, Shibaura, Minato-ku, Tokyo 105-0023, Japan	Phys.Rev.B,62,(2000)1350-1360	Masato Murakami,Noriko Chikumoto,Tadashi Mochida		
31144	PR06201350	Nd4Ba2Cu2O10 inclusions (30 mol%)	NdBa2Cu3O7-z	Nd1Ba2Cu3O7-Z	Nd	1	Ba	2	Cu	3															O	7-Z			2000																												Y123																		K			95				95		2																																																																																														ref 29				sample were grown under the same oxgen partial pressure of 0.1 % and fully oxygenated at 300 C for 150 h	Flux pinning by Nd4Ba2Cu2O10 inclusions in NdBa2Cu3O7-z superconductors: A combined effect of point, interface, and  delta kappa    pinning at elevated temperatures	200007		Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-16-25, Shibaura, Minato-ku, Tokyo 105-0023, Japan	Phys.Rev.B,62,(2000)1350-1360	Masato Murakami,Noriko Chikumoto,Tadashi Mochida		
31145	PR06201387	PDHC2DT in fig5	Bi2(Sr,La)2CuO6+z	Bi2Sr1.75La0.25Cu1O6+Z	Bi	2	Sr	1.75	La	0.25	Cu	1													O	6+Z		3	2000																												Bi2201																		K			27.5				27.5		1																											T/K																																					uV/K	1.38																																	anneal condition: in flowing Ar gas at 680 C for 15h	Giant dissipation peak and current effect of in-plane resistance in Bi2Sr2-xLaxCuO6 + y single crystals under magnetic fields	200007		National Laboratory for Superconductivity, Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B,62,(2000)1387-1391	H. H. Wen,W. L. Yang,Z. X. Zhao		
31200	PR06204148		HgBa2CuO4	Hg1Ba2Cu1O4.05	Hg	1	Ba	2	Cu	1															O	4+Z	4.05	1	2000																												Hg1201																		K				73.5			73.5										84.4																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31201	PR06204148		HgBa2CuO4	Hg1Ba2Cu1O4.15	Hg	1	Ba	2	Cu	1															O	4+Z	4.15	1	2000																												Hg1201																		K				96.8			96.8										92.3																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31202	PR06204148		HgBa2CuO4	Hg1Ba2Cu1O4.18	Hg	1	Ba	2	Cu	1															O	4+Z	4.18	1	2000																												Hg1201																		K				96.6			96.6										64																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31203	PR06204148		HgBa2CuO4	Hg1Ba2Cu1O4.2	Hg	1	Ba	2	Cu	1															O	4+Z	4.2	1	2000																												Hg1201																		K				94.2			94.2										50																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31204	PR06204148		(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.33	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+Z	4.33	1	2000																												Hg1201																		K				87.2			87.2										45.4																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31205	PR06204148		(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.35	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+Z	4.35	1	2000																												Hg1201																		K				90.5			90.5										43.8																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31206	PR06204148		(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.41	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+Z	4.41	1	2000																												Hg1201																		K				94.5			94.5										52.5																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31207	PR06204148		(Hg,Re)Ba2CuO4	Hg0.9Re0.1Ba2Cu1O4.42	Hg	0.9	Re	0.1	Ba	2	Cu	1													O	4+Z	4.42	1	2000																												Hg1201																		K				93.8			93.8										39.5																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31208	PR06204148		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.49	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+Z	4.49	1	2000																												Hg1201																		K				93.7			93.7										45.6																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31209	PR06204148		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.52	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+Z	4.52	1	2000																												Hg1201																		K				94.8			94.8										39.8																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31211	PR06204148		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.55	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+Z	4.55	1	2000																												Hg1201																		K				93.7			93.7										59.4																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31212	PR06204148		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.58	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+Z	4.58	1	2000																												Hg1201																		K				34.7			34.7										56.8																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31220	PR06204148		(Hg,Re)Ba2CuO4	Hg0.85Re0.15Ba2Cu1O4.53	Hg	0.85	Re	0.15	Ba	2	Cu	1													O	4+Z	4.53	1	2000																												Hg1201																		K				96.3			96.3										52.3																																																																																					1	Synthesized by the sealed quartz tube technique(ref.21). The oxygen content was modified by different treatments under oxygen pressures within the range 180 and 1.7*10^-9 atm(ref.21).				The oxygen content was determined bu thermogravimetric and neutron diffraction analyses(ref.21).	Distinguishable effects of oxygen and rhenium in HgBa2CuO4 +z  superconductors	200008		Institut de Ci?ncia de Materials de Barcelona, Consejo Superior de Investigaciones Cient?ficas, Campus de la UAB, 08193 Bellaterra, Spain	Phys.Rev.B, 62(2000)4148-4153	A.Caneiro,A.Serquis,J.Fontcuberta,L.F?brega		
31300	PR06205989		La2CuO4	La2Cu1O4.03	La	2	Cu	1																	O	4+Z	4.03	6	2000																												T			A	5.396	5.356	13.144	3																																																																																																																La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31301	PR06205989		(La,Sr)2CuO4	La1.95Sr0.05Cu1O4.02	La	1.95	Sr	0.05	Cu	1															O	4+Z	4.02	6	2000																												T			A	5.371	5.369	13.219	3																																																																																				uV/K	95.6			TP31301																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31302	PR06205989		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4.01	La	1.9	Sr	0.1	Cu	1															O	4+Z	4.01	6	2000																												T			A	5.35	5.35	13.22	3											K			29				29		R																																																																uV/K	42			TP31302																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31303	PR06205989		(La,Sr)2CuO4	La1.85Sr0.15Cu1O3.99	La	1.85	Sr	0.15	Cu	1															O	4+Z	3.99	6	2000																												T			A	5.34	5.34	13.237	3											K			33				33		R																																																																uV/K	14.9			TP31303																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31304	PR06205989		(La,Sr)2CuO4	La1.8Sr0.2Cu1O3.95	La	1.8	Sr	0.2	Cu	1															O	4+Z	3.95	6	2000																												T			A	5.335	5.335	13.246	3											K			29				29		R																																																																uV/K	8.1			TP31304																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31305	PR06205989		(La,Sr)2CuO4	La1.75Sr0.25Cu1O3.93	La	1.75	Sr	0.25	Cu	1															O	4+Z	3.93	6	2000																												T			A	5.33	5.33	13.26	3											K			15				15		R																																																																uV/K	-0.5			TP31305																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31306	PR06205989		(La,Sr)2CuO4	La1.7Sr0.3Cu1O3.9	La	1.7	Sr	0.3	Cu	1															O	4+Z	3.9	6	2000																												T			A	5.331	5.331	13.261	3																																																																																				uV/K	0.98			TP31306																								La2O3, SrO, CuO	1	mixtures were calcined at 970 C for 20 h reground, then pressed into pellets and sintered at 90 C for 20 h. The pellets were heated in fllowing O2 at 450 C for 10 h and furnance cool.					Band spectrum transformation and Tc variation in the La2-xSrxCuOy system in the underdoped and overdoped regimes	200009		Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Technical University, 29 Polytekhnicheskaya, St.Petersburg, 195251, Russia	Phys.Rev.B,62(2000)5989-5996	M. V. Elizarova,V. E. Gasumyants		
31307	PR06206754		(La,Sr)3Mn2O7	La1.4Sr1.6Mn2O7	La	1.4	Sr	1.6	Mn	2															O	7		6	2000								60																				Sr3Ti2O7	1/4mmm		A	3.87		20.21																																																																																					uV/K	-2.57			TP31307	ohmcm	6.5			6.5																			CaO, SrCO3, MnO2, La2O3	1	The mixture were calcined at 1000 C and 1340 C in air. And it was pressed into plates which were sinterd at 1380 C for 20h.					Two-dimensional magnetic correlation and transport behavior of layered manganite La1.4Sr1.6Mn2-xCuxO7	200009		Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B,62(2000)6754-6760	Hong Zhu,Li Pi,XiaoJun Xu,YuHeng Zhang		
31308	PR06206754		(La,Sr)3(Mn,Cu)2O7	La1.4Sr1.6Mn1.95Cu0.05O7	La	1.4	Sr	1.6	Mn	1.95	Cu	0.05													O	7		6	2000																												Sr3Ti2O7																																																																																																ohmcm				140																			CaO, SrCO3, MnO2, La2O3	1	The mixture were calcined at 1000 C and 1340 C in air. And it was pressed into plates which were sinterd at 1380 C for 20h.					Two-dimensional magnetic correlation and transport behavior of layered manganite La1.4Sr1.6Mn2-xCuxO7	200009		Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B,62(2000)6754-6760	Hong Zhu,Li Pi,XiaoJun Xu,YuHeng Zhang		
31309	PR06206754		(La,Sr)3(Mn,Cu)2O7	La1.4Sr1.6Mn1.9Cu0.1O7	La	1.4	Sr	1.6	Mn	1.9	Cu	0.1													O	7		6	2000																												Sr3Ti2O7	1/4mmm																																																																																															ohmcm				200																			CaO, SrCO3, MnO2, La2O3	1	The mixture were calcined at 1000 C and 1340 C in air. And it was pressed into plates which were sinterd at 1380 C for 20h.					Two-dimensional magnetic correlation and transport behavior of layered manganite La1.4Sr1.6Mn2-xCuxO7	200009		Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B,62(2000)6754-6760	Hong Zhu,Li Pi,XiaoJun Xu,YuHeng Zhang		
31310	PR06206754		(La,Sr)3(Mn,Cu)2O7	La1.4Sr1.6Mn1.6Cu0.4O7	La	1.4	Sr	1.6	Mn	1.6	Cu	0.4													O	7		6	2000																												Sr3Ti2O7	1/4mmm																																																																																															ohmcm																							CaO, SrCO3, MnO2, La2O3	1	The mixture were calcined at 1000 C and 1340 C in air. And it was pressed into plates which were sinterd at 1380 C for 20h.					Two-dimensional magnetic correlation and transport behavior of layered manganite La1.4Sr1.6Mn2-xCuxO7	200009		Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B,62(2000)6754-6760	Hong Zhu,Li Pi,XiaoJun Xu,YuHeng Zhang		
31311	PR06206761		YBa2Cu3Oz	Y1Ba2Cu3O6.4	Y	1	Ba	2	Cu	3															O	7-Z	6.4	3	2000																												Y123																		K		35					35		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31312	PR06206761		YBa2Cu3-xZnxOz	Y1Ba2Cu3O6.56	Y	1	Ba	2	Cu	3															O	7-Z	6.56	3	2000																												Y123																		K		59					59		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31313	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	7-Z	6.65	3	2000																												Y123																		K		67					67		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31314	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	7-Z	6.73	3	2000																												Y123																		K		78					78		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31315	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.47	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.47	3	2000																												Y123																		K		18					18		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31316	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.52	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.52	3	2000																												Y123																		K		23					23		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31317	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.56	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.56	3	2000																												Y123																		K		24					24		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31318	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.62	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.62	3	2000																												Y123																		K		21					21		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31319	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.63	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.63	3	2000																												Y123																		K		25					25		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31320	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.69	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.69	3	2000																												Y123																		K		25					25		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31321	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.7	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.7	3	2000																												Y123																		K		25					25		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31322	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.72	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.72	3	2000																												Y123																		K		35					35		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31323	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.75	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.75	3	2000																												Y123																		K		48					48		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
31324	PR06206761		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.95Zn0.05O6.8	Y	1	Ba	2	Cu	2.95	Zn	0.05													O	7-Z	6.8	3	2000																												Y123																		K		60					60		R																																																																																												Y2O3, BaCO3, CuO, ZnO	1	The mixture were sintered at 900 C for 12 h in air and materials were mixed pelletized and sintered in air at 930 C 24 h.				Post annealing was in O2 at 500 C for 24h. The Oxygen content was determined by iodometric titration.	Anomalous muon-spin relaxation in the Zn-substituted YBa2Cu3-2yZn2yO7-z around the hole concentration of 1/8  per Cu	200009		Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai, Miyagi 980-8579, Japan	Phys.Rev.B,62(2000)6761-6765	Isao Watanabe,Kanetada Nagamine,Megumi Akoshima,Yoji Koike		
32000	PRL0760122		T2Ba2CuOz	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	7-Z	6	3	1996																												Tl2201																		K			25				25																																																																							mohmcm					0.03	40		0.02	30			0.18	220											5	self-flux method in almina crucibles seald with gold foil				anneal: in flowing O2 at 720 K for three days before in O2 for 10 min at 740 K	Angular Dependence of the c-axis Normal State Magnetoresistance in Single Crystal Tl2Ba2CuO6	199601		Interdisciplinary Research Centre in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.Lett.,76(1996)122	A.Carrington,A.P.Mackenzie,C.T.Lin,I.R.Fisher,J.M.Wheatley,J.R.Cooper,N.E.Hussey,O.Milat		
32001	PRL0760684		YBa2Cu3Oz	Y1Ba2Cu3O6.63	Y	1	Ba	2	Cu	3															O	7-Z	6.63	3	1996																												Y123																		K			76				76		R																																																																					mohmcm					0.1			0.1				0.55												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32002	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.97Zn0.03O6.63	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-Z	6.63	3	1996																												Y123																		K			45				45		R																																																																					mohmcm					0.2			0.15				0.68												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32003	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.63	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.63	3	1996																												Y123																		K			30				30		R																																																																					mohmcm					0.25			0.2				0.7												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32004	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.63	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.63	3	1996																												Y123																																																																																																mohmcm		0.4			0.42							0.82												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32005	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.63	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.63	3	1996																												Y123																		K																																																																														mohmcm		0.5			0.46							0.86												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32006	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.88Zn0.12O6.63	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-Z	6.63	3	1996																												Y123																		K																																																																														mohmcm		0.6			0.55							0.91												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32007	PRL0760684		YBa2Cu3Oz	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-Z	6.93	3	1996																												Y123																		K			90				90		R																																																																					mohmcm								0.04				0.18												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32008	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.97Zn0.03O6.93	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-Z	6.93	3	1996																												Y123																		K			82				82		R																																																																					mohmcm								0.06				0.21												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32009	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.93	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.93	3	1996																												Y123																		K			75				75		R																																																																					mohmcm					0.1			0.08				0.26												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32010	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.93	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.93	3	1996																												Y123																		K			55				55		R																																																																					mohmcm					0.15			0.12				0.33												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32011	PRL0760684		YBa2Cu3Oz	Y1Ba2Cu3O6.68	Y	1	Ba	2	Cu	3															O	7-Z	6.68	3	1996																												Y123																		K			15				15		R																																																																					mohmcm					0.08			0.08				0.42												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32012	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.68	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.68	3	1996																												Y123																		K			25				25		R																																																																					mohmcm					0.24			0.22				0.65												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32013	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.68	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.68	3	1996																												Y123																		K			60				60		R																																																																					mohmcm					0.36			0.32				0.85												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32014	PRL0760684		YBa2Cu3Oz	Y1Ba2Cu3O6.73	Y	1	Ba	2	Cu	3															O	7-Z	6.73	3	1996																												Y123																		K			62				62		R																																																																					mohmcm					0.08			0.08				0.35												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32015	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.73	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.73	3	1996																												Y123																		K			35				35		R																																																																					mohmcm					0.2			0.18				0.52												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32016	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.73	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.73	3	1996																												Y123																		K			25				25		R																																																																					mohmcm					0.3			0.25				0.65												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32017	PRL0760684		YBa2Cu3Oz	Y1Ba2Cu3O6.83	Y	1	Ba	2	Cu	3															O	7-Z	6.83	3	1996																												Y123																		K			90				90		R																																																																					mohmcm								0.06				0.27												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32018	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.83	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.83	3	1996																												Y123																		K			55				55		R																																																																					mohmcm					0.15			0.14				0.42												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32019	PRL0760684		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.83	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.83	3	1996																												Y123																		K			45				45		R																																																																					mohmcm					0.22			0.2				0.5												5	self-flux method ( CuO-BaO )				anneal: ref[9]	Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32020	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.9Sr0.1Cu0.98Zn0.02O4	La	1.9	Sr	0.1	Cu	0.98	Zn	0.02													O	4		3	1996																												T																																																																																																mohmcm		0.75			0.45							0.98												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32021	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.85Sr0.15Cu0.98Zn0.02O4	La	1.85	Sr	0.15	Cu	0.98	Zn	0.02													O	4		3	1996																												T																		K			20				20		R																																																																					mohmcm					0.25			0.23				0.62												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32022	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.7Sr0.3Cu0.98Zn0.02O4	La	1.7	Sr	0.3	Cu	0.98	Zn	0.02													O	4		3	1996																												T																																																																																																mohmcm		0.05			0.06							0.2												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32023	PRL0760684		(La,Sr)2CuOz	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1996																												T																		K			27				27		R																																																																					mohmcm					0.25			0.18				0.6												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32024	PRL0760684		(La,Sr)2CuOz	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	1996																												T																		K			37				37		R																																																																					mohmcm					0.1			0.04				0.4												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32025	PRL0760684		(La,Sr)2CuOz	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		3	1996																												T																																																																																																mohmcm					0.04							0.18												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32026	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.85Sr0.15Cu0.995Zn0.005O4	La	1.85	Sr	0.15	Cu	0.995	Zn	0.005													O	4		3	1996																												T																		K			30				30		R																																																																					mohmcm					0.15			0.1				0.48												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32027	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.85Sr0.15Cu0.99Zn0.01O4	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	4		3	1996																												T																		K			28				28		R																																																																					mohmcm					0.18			0.12				0.53												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32028	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.85Sr0.15Cu0.985Zn0.015O4	La	1.85	Sr	0.15	Cu	0.985	Zn	0.015													O	4		3	1996																												T																		K			22				22		R																																																																					mohmcm					0.2			0.15				0.53												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32029	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.85Sr0.15Cu0.96Zn0.04O4	La	1.85	Sr	0.15	Cu	0.96	Zn	0.04													O	4		3	1996																												T																																																																																																mohmcm		0.62										0.68												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32030	PRL0760684		(La,Sr)2CuOz	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		3	1996																												T																		K			32				32		R																																																																					mohmcm					0.06			0.04				0.25												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32031	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.8Sr0.2Cu0.99Zn0.01O4	La	1.8	Sr	0.2	Cu	0.99	Zn	0.01													O	4		3	1996																												T																		K			27				27		R																																																																					mohmcm					0.07			0.048				0.26												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32032	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.8Sr0.2Cu0.98Zn0.02O4	La	1.8	Sr	0.2	Cu	0.98	Zn	0.02													O	4		3	1996																												T																		K			22				22		R																																																																					mohmcm					0.09			0.052				0.275												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32033	PRL0760684		(La,Sr)2(Cu,Zn)Oz	La1.8Sr0.2Cu0.96Zn0.04O4	La	1.8	Sr	0.2	Cu	0.96	Zn	0.04													O	4		3	1996																												T																																																																																																mohmcm		0.07			0.13							0.32												7	TSFZ method ref[8]					Universal Superconductor-Insulator Transition and Tc Depression in Zn-Substituted High-Tc Cuprates in the Underdoped Regime	199601		Department of Superconductivity, University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,76(1996)1074	K.Mizuhashi,K.Takenaka,S.Uchida,Y.Fukuzumi		
32034	PRL0761348		(La,Ca,Nd)2CuOz	La1.75Ca0.15Nd0.1Cu1O4	La	1.75	Ca	0.15	Nd	0.1	Cu	1													O	4		1	1996																												T							4											K			30.5				30.5		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32035	PRL0761348		(La,Ca,Nd)2CuOz	La1.65Ca0.15Nd0.2Cu1O4	La	1.65	Ca	0.15	Nd	0.2	Cu	1													O	4		1	1996																												T							4											K			30				30		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32036	PRL0761348		(La,Ca,Nd)2CuOz	La1.55Ca0.15Nd0.3Cu1O4	La	1.55	Ca	0.15	Nd	0.3	Cu	1													O	4		1	1996																												T							4											K			28				28		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32037	PRL0761348		(La,Ca,Nd)2CuOz	La1.45Ca0.15Nd0.4Cu1O4	La	1.45	Ca	0.15	Nd	0.4	Cu	1													O	4		1	1996																												T							4											K			27.5				27.5		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32038	PRL0761348		(La,Ca,Nd)2CuOz	La1.35Ca0.15Nd0.5Cu1O4	La	1.35	Ca	0.15	Nd	0.5	Cu	1													O	4		1	1996																												T							4											K			26				26		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32039	PRL0761348		(La,Ca,Nd)2CuOz	La1.25Ca0.15Nd0.6Cu1O4	La	1.25	Ca	0.15	Nd	0.6	Cu	1													O	4		1	1996																												T							4											K			25				25		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32040	PRL0761348		(La,Ca,Nd)2CuOz	La1.05Ca0.15Nd0.8Cu1O4	La	1.05	Ca	0.15	Nd	0.8	Cu	1													O	4		1	1996																												T							4											K			24.5				24.5		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32041	PRL0761348		(La,Ca,Nd)2CuOz	La0.85Ca0.15Nd1Cu1O4	La	0.85	Ca	0.15	Nd	1	Cu	1													O	4		1	1996																												T							4											K			23				23		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32042	PRL0761348		(La,Ca)2CuOz	La1.92Ca0.08Cu1O4	La	1.92	Ca	0.08	Cu	1															O	4		1	1996																												T							4											K			16				16		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32043	PRL0761348		(La,Ca)2CuOz	La1.91Ca0.09Cu1O4	La	1.91	Ca	0.09	Cu	1															O	4		1	1996																												T							4											K			20				20		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32044	PRL0761348		(La,Ca)2CuOz	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4		1	1996																												T							4											K			22				22		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32045	PRL0761348		(La,Ca)2CuOz	La1.89Ca0.11Cu1O4	La	1.89	Ca	0.11	Cu	1															O	4		1	1996																												T							4											K			23				23		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32046	PRL0761348		(La,Ca)2CuOz	La1.885Ca0.115Cu1O4	La	1.885	Ca	0.115	Cu	1															O	4		1	1996																												T							4											K			23				23		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32047	PRL0761348		(La,Ca)2CuOz	La1.88Ca0.12Cu1O4	La	1.88	Ca	0.12	Cu	1															O	4		1	1996																												T							4											K			24				24		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32048	PRL0761348		(La,Ca)2CuOz	La1.875Ca0.125Cu1O4	La	1.875	Ca	0.125	Cu	1															O	4		1	1996																												T							4											K			26				26		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32049	PRL0761348		(La,Ca)2CuOz	La1.87Ca0.13Cu1O4	La	1.87	Ca	0.13	Cu	1															O	4		1	1996																												T							4											K			28				28		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32050	PRL0761348		(La,Ca)2CuOz	La1.86Ca0.14Cu1O4	La	1.86	Ca	0.14	Cu	1															O	4		1	1996																												T							4											K			32				32		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32051	PRL0761348		(La,Ca)2CuOz	La1.85Ca0.15Cu1O4	La	1.85	Ca	0.15	Cu	1															O	4		1	1996																												T							4											K			34				34		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32052	PRL0761348		(La,Ca)2CuOz	La1.84Ca0.16Cu1O4	La	1.84	Ca	0.16	Cu	1															O	4		1	1996																												T							4											K			34				34		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32053	PRL0761348		(La,Ca)2CuOz	La1.83Ca0.17Cu1O4	La	1.83	Ca	0.17	Cu	1															O	4		1	1996																												T							4											K			34				34		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32054	PRL0761348		(La,Ca)2CuOz	La1.82Ca0.18Cu1O4	La	1.82	Ca	0.18	Cu	1															O	4		1	1996																												T							4											K			33				33		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32055	PRL0761348		(La,Ca)2CuOz	La1.81Ca0.19Cu1O4	La	1.81	Ca	0.19	Cu	1															O	4		1	1996																												T							4											K			32				32		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32056	PRL0761348		(La,Ca)2CuOz	La1.8Ca0.2Cu1O4	La	1.8	Ca	0.2	Cu	1															O	4		1	1996																												T							4											K			30				30		R																																																																																														ref[8]					Dependence of Superconducting Transition Temperature on Doping and Structural Distortion of the CuO2 Planes in La2-xMxCuO4 (M=Nd,Ca,Sr)	199602		Physics Department ,Northern Illinois University, DeKalb,Illinois 60115	Phys.Rev.Lett.,76(1996)1348	B.A.Hunter,B.Dabrowski,D.G.Hinks,J.D.Jorgensen,J.L.Wagner,K.Rogacki,P.G.Radaelli,R.L.Hitterman,Z.Wang		
32057	PRL0770928		YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		5	1996																												Y123																		K	80						80																																																																							mohmcm									40				60												ref[8]					c-Axis Conductivity and Intrinsic Josephson Effects in YBa2Cu3O7-z	199607		Physik Department E10, Technische Universitat Munchen, 85747 Garching, Germany	Phys.Rev.Lett.,77(1996)928	A.Murk,M.Rapp,R.Semerad,W.Prusseit		
32058	PRL0770928		YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		5	1996																												Y123																		K	53						53																																																																							mohmcm									140				150												ref[8]					c-Axis Conductivity and Intrinsic Josephson Effects in YBa2Cu3O7-z	199607		Physik Department E10, Technische Universitat Munchen, 85747 Garching, Germany	Phys.Rev.Lett.,77(1996)928	A.Murk,M.Rapp,R.Semerad,W.Prusseit		
32059	PRL0770928		YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		5	1996																												Y123																		K	45						45																																																																							mohmcm						360			400				190												ref[8]					c-Axis Conductivity and Intrinsic Josephson Effects in YBa2Cu3O7-z	199607		Physik Department E10, Technische Universitat Munchen, 85747 Garching, Germany	Phys.Rev.Lett.,77(1996)928	A.Murk,M.Rapp,R.Semerad,W.Prusseit		
32060	PRL0770928		YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		5	1996																												Y123																		K	42						42																																																																							mohmcm						550			580				210												ref[8]					c-Axis Conductivity and Intrinsic Josephson Effects in YBa2Cu3O7-z	199607		Physik Department E10, Technische Universitat Munchen, 85747 Garching, Germany	Phys.Rev.Lett.,77(1996)928	A.Murk,M.Rapp,R.Semerad,W.Prusseit		
32061	PRL0771378		Sr14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41	41	6	1996																												LAD																																																																																																mohmcm											250												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32062	PRL0771378		(Sr,Ca)14Cu24O41	Sr12Ca2Cu24O41	Sr	12	Ca	2	Cu	24															O	41	41	6	1996																												LAD																																																																																																mohmcm				1000000000							100												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32063	PRL0771378		(Sr,Ca)14Cu24O41	Sr10Ca4Cu24O41	Sr	10	Ca	4	Cu	24															O	41	41	6	1996																												LAD																																																																																																mohmcm				6395000							32												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32064	PRL0771378		(Sr,Ca)14Cu24O41	Sr8Ca6Cu24O41	Sr	8	Ca	6	Cu	24															O	41	41	6	1996																												LAD																																																																																																mohmcm				15850							20												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32065	PRL0771378		(Sr,Ca)14Cu24O41	Sr6Ca8Cu24O41	Sr	6	Ca	8	Cu	24															O	41	41	6	1996																												LAD																																																																																																mohmcm				630							10												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32066	PRL0771378		(Sr,Ca)14Cu24O41	Sr4Ca10Cu24O41	Sr	4	Ca	10	Cu	24															O	41	41	6	1996																												LAD																																																																																																mohmcm	25118000			200							10												SrCO3, CaCO3, LaO3, CuO		ref[14]					Hole Doping of the CuO2 Chains in (La,Sr,Ca)14Cu24O41	199608		AT&T Bell Laboratoried, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)1378	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,T.M.Rice,W.F.Peck,Jr.		
32067	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.3Pr0.7Cu2OZ	Bi	2	Sr	2	Ca	0.3	Pr	0.7	Cu	2											O	Z		1	1996																												Bi2212																																																																																																mohmcm	300000			200							60														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32068	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.4Pr0.6Cu2OZ	Bi	2	Sr	2	Ca	0.4	Pr	0.6	Cu	2											O	Z		1	1996																												Bi2212																																																																																																mohmcm	300			30							18														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32069	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.5Pr0.5Cu2OZ	Bi	2	Sr	2	Ca	0.5	Pr	0.5	Cu	2											O	Z		1	1996																												Bi2212																																																																																																mohmcm	40			15							12														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32070	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.6Pr0.4Cu2OZ	Bi	2	Sr	2	Ca	0.6	Pr	0.4	Cu	2											O	Z		1	1996																												Bi2212																		K			25				25		R																																																																					mohmcm				8			4				9														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32071	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.7Pr0.3Cu2OZ	Bi	2	Sr	2	Ca	0.7	Pr	0.3	Cu	2											O	Z		1	1996																												Bi2212																		K			74				74		R																																																																					mohmcm							2.2				3														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32072	PRL0771837		Bi2Sr2(Ca,Pr)Cu2Oz	Bi2Sr2Ca0.9Pr0.1Cu2OZ	Bi	2	Sr	2	Ca	0.9	Pr	0.1	Cu	2											O	Z		1	1996																												Bi2212																		K			77				77		R																																																																					mohmcm							1.1				2														ref[9]					Coexistence of Superconductivity and Localization in Bi2Sr2(Caz,Pr1-z)Cu2O8+y	199608		II. Physikalisches Institut der Rheinisch-Westfalische Technische Hochschule Aachen, D-52056 Aachen,  Germany	Phys.Rev.Lett.,77(1996)1837	B.Beschoten,C.Quitmann,G.Guntherodt,S.Sadewasser		
32073	PRL0772065	A	Bi2Sr2-xLaxCuOz	Bi2Sr1.95La0.05Cu1OZ	Bi	2	Sr	1.95	La	0.05	Cu	1													O	Z		3	1996																												Bi2201																		K		13					13		R																																																																					mohmcm					2.6	3200		2.5	5200																ref[14]					Metallic In-Plane and Divergent Out-of-Plane Resistivity of a High-Tc Cuprate in the Zero-Temperature Limit	199609		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)2065	A.Passner,C.Geibel,F.Steglich,G.S.Boebinger,N.L.Wang,Y.Ando		
32074	PRL0772065	B	Bi2Sr2-xLaxCuOz	Bi2Sr1.95La0.05Cu1OZ	Bi	2	Sr	1.95	La	0.05	Cu	1													O	Z		3	1996																												Bi2201																		K		13					13		R																																																																					mohmcm					0.4	1200		0.3	2000																ref[14]					Metallic In-Plane and Divergent Out-of-Plane Resistivity of a High-Tc Cuprate in the Zero-Temperature Limit	199609		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)2065	A.Passner,C.Geibel,F.Steglich,G.S.Boebinger,N.L.Wang,Y.Ando		
32075	PRL0772065	C	Bi2Sr2-xLaxCuOz	Bi2Sr1.95La0.05Cu1OZ	Bi	2	Sr	1.95	La	0.05	Cu	1													O	Z		3	1996																												Bi2201																		K		14					14		R																																																																					mohmcm					0.09	1800		0.08	4000																ref[14]					Metallic In-Plane and Divergent Out-of-Plane Resistivity of a High-Tc Cuprate in the Zero-Temperature Limit	199609		Bell Laboratories, Lucent Technologies, 700 Mountain Avenue, Murray Hill, New Jersey 07974	Phys.Rev.Lett.,77(1996)2065	A.Passner,C.Geibel,F.Steglich,G.S.Boebinger,N.L.Wang,Y.Ando		
32076	PRL0774253	a-axis resistivity	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	1996																												Y124																		K				81			81			K/kbar	0.58																																																														uV/K				TP32076	uohmcm								250			1450														ref[6]					Transport Properties of a YBa2Cu4O8 Crystal under High Pressure	199611		Center for Material Science and Engineering, University of Texas at Austin, Austin, Texas 78712	Phys.Rev.Lett.,77(1996)4253	B.Dabrowski,J.-S.Zhou,J.B.Goodenough,K.Rogacki		
32100	PRL0781976	detwined	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	3	1997																												Y123																		K			93.8			0.2	93.8		R																																																											W/mK				THC32100																														5	self-decanting flux method[6]				anneal: for 240h at 500 C in O2 flow and quenched.	Anisotropy of Heat Conduction in YBa2Cu3O6.9 : A Probe of Chain Superconductivity	199705		Department of Physics, McGill University, 3600 University Street, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,78(1997)1976	B.Ellman,L.Taillefer,R.Gagnon,S.Pu		
32101	PRL0782624		YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	3	1997																												Y123																		K			93				93																																																													mW/Kcm				THC32101																														5	self-flux method[14]					Angular Position of Nodes in the Superconducting Gap of YBCO	199703		Laboratoire de Physique des Solides (associe au CNRS), Universite Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,78(1997)2624	H.Aubin,K.Behnia,L.Taillefer,M.Ribault,R.Gagnon		
32102	PRL0783757	asgrown	HgBa2CuOz	Hg1Ba2Cu1OZ	Hg	1	Ba	2	Cu	1															O	Z		6	1997																												Hg1201																		K				89			89																																																																																																single step gold amalgamation technique [9]				anneal: 300 C in O2 at 0.3 bar for one or two days	<17>O NMR Evidence for a Pseudogap in the Monolayer HgBa2CuO4+z	199705		LPS, URA2 CNRS, 91405 Orsay Cedex, France	Phys.Rev.Lett.,78(1997)3757	D.Colson,H.Alloul,J.-F.Marucco,J.Bobroff,P.Mendels,V.Viallet		
32103	PRL0783757	underdoped	HgBa2CuOz	Hg1Ba2Cu1OZ	Hg	1	Ba	2	Cu	1															O	Z		6	1997																												Hg1201																		K				75			75																																																																																																single step gold amalgamation technique [9]				anneal: 450 C in N2 at 1 atm	<17>O NMR Evidence for a Pseudogap in the Monolayer HgBa2CuO4+z	199705		LPS, URA2 CNRS, 91405 Orsay Cedex, France	Phys.Rev.Lett.,78(1997)3757	D.Colson,H.Alloul,J.-F.Marucco,J.Bobroff,P.Mendels,V.Viallet		
32104	PRL0784833	detwined	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1997																												Y123																		K			92				92																																																						mJ/molK2	55																																									ref[5, 6]					Anisotropic Latent Heat of Vortex-Lattice Melting in Untwinned YBa2Cu3O7-z	199706		Lawrence Berkeley National Laboratory and Department of Chemistry, University of California, Berkeley, California 94720	Phys.Rev.Lett.,78(1997)4833	A.Schilling,G.W.Crabtree,N.E.Phillips,R.A.Fisher,U.Welp,W.K.Kwok		
32105	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.2135	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.2135	3	1997																												Bi2212																		K			70				70		R																																																																					mohmcm								0.3	52000			0.91	8000											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32106	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.217	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.217	3	1997																												Bi2212																		K									R																																																																					mohmcm								0.26	39500			0.82	7000											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32107	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.22	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.22	3	1997																												Bi2212																		K									R																																																																					mohmcm								0.25	29500			0.64	6000											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32108	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.224	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.224	3	1997																												Bi2212																		K			89				89		R																																																																					mohmcm								0.2	19000			0.52	5000											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32109	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.245	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.245	3	1997																												Bi2212																		K			90				90		R																																																																					mohmcm								0.15				0.44												7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32110	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.255	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.255	3	1997																												Bi2212																		K									R																																																																					mohmcm								0.13				0.37												7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32111	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.26	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.26	3	1997																												Bi2212																		K									R																																																																					mohmcm								0.12	6000			0.33	3000											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32112	PRL0792113		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.27	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.27	3	1997																												Bi2212																		K			84				84		R																																																																					mohmcm								0.09	4000			0.25	2200											7	TSFZ method under a mixed gas O2(20%)+Ar(80%) flow				Z was obtained by a thermogravimetric measurements {P(O2) > 10e-4 atm}	Anistropic Resistivites of Precisely Oxygen Controlled Single-Crystal Bi2Sr2CaCu2O8+delta: Systematic Study on 	199709				A.Matsuda,T.Fujii,T.Watanabe		
32113	PRL0790483		YBa2Cu3Oz	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	Z	6	3	1997																												Y123																																																																																						mW/K2cm				THC32113																															ref[5, 6]   Zn:Cu = 1.5x:1-x     x = 0, 0.006, 0.02, 0.03				anneal : at 800 C in He gas for 64h	Universal Heat Conduction in YBa2Cu3O6.9	199707		Department of Physics, McGill University, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,79(1997)483	B.Lussier,H.Aubin,K.Behnia,L.Taillefer,R.Gagnon		
32114	PRL0790483		YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-Z	6.9	3	1997																												Y123																		K			93.6				93.6																																																													mW/K2cm				THC32114																															ref[5, 6]   Zn:Cu = 1.5x:1-x     x = 0, 0.006, 0.02, 0.03				anneal : at 800 C in He gas for 64h	Universal Heat Conduction in YBa2Cu3O6.9	199707		Department of Physics, McGill University, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,79(1997)483	B.Lussier,H.Aubin,K.Behnia,L.Taillefer,R.Gagnon		
32115	PRL0790483		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.982Zn0.018O6.9	Y	1	Ba	2	Cu	2.982	Zn	0.018													O	7-Z	6.9	3	1997																												Y123																		K			89.2				89.2																																																													mW/K2cm				THC32115																															ref[5, 6]   Zn:Cu = 1.5x:1-x     x = 0, 0.006, 0.02, 0.03				anneal : at 800 C in He gas for 64h	Universal Heat Conduction in YBa2Cu3O6.9	199707		Department of Physics, McGill University, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,79(1997)483	B.Lussier,H.Aubin,K.Behnia,L.Taillefer,R.Gagnon		
32116	PRL0790483		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.94Zn0.06O6.9	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-Z	6.9	3	1997																												Y123																		K			80				80																																																													mW/K2cm				THC32116																															ref[5, 6]   Zn:Cu = 1.5x:1-x     x = 0, 0.006, 0.02, 0.03				anneal : at 800 C in He gas for 64h	Universal Heat Conduction in YBa2Cu3O6.9	199707		Department of Physics, McGill University, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,79(1997)483	B.Lussier,H.Aubin,K.Behnia,L.Taillefer,R.Gagnon		
32117	PRL0790483		YBa2(Cu,Zn)3Oz	Y1Ba2Cu2.91Zn0.09O6.9	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-Z	6.9	3	1997																												Y123																		K			74.6				74.6																																																													mW/K2cm				THC32117																															ref[5, 6]   Zn:Cu = 1.5x:1-x     x = 0, 0.006, 0.02, 0.03				anneal : at 800 C in He gas for 64h	Universal Heat Conduction in YBa2Cu3O6.9	199707		Department of Physics, McGill University, Montreal, Quebec, Canada H3A 2T8	Phys.Rev.Lett.,79(1997)483	B.Lussier,H.Aubin,K.Behnia,L.Taillefer,R.Gagnon		
32205	PRL0800385	reduced	HgBa2CuOz	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8915		9.529												K				61			61																																																																																																Ba2CuO3+z +HgO synthesized [7].				reduced sample	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32206	PRL0800385	fluorination(150C,15h)	HgBa2CuOzF0.1	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8828		9.523												K				97			97																																																																																																Ba2CuO3+z +HgO synthesized [7].				M=0.1 anneal: 150C for 15h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32207	PRL0800385	fluorination(200C,15h)	HgBa2CuOzF0.3	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8825		9.51												K				97			97																																																																																																Ba2CuO3+z +HgO synthesized [7].				M=0.3 anneal: 200C for 15h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32208	PRL0800385	fluorination(200C,15h)	HgBa2CuOzF0.5	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8788		9.498												K				96			96																																																																																																Ba2CuO3+z +HgO synthesized [7].				M=0.5 anneal: 200C for 15h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32209	PRL0800385	fluorination(200C,20h)	HgBa2CuOzF0.4	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8742		9.493												K				80			80																																																																																																Ba2CuO3+z +HgO synthesized [7].				M=0.4 anneal: 200C for 20h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32210	PRL0800385	fluorination(200C,30h)	HgBa2CuOzF0.3	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8721		9.482												K				80			80																																																																																																Ba2CuO3+z +HgO synthesized [7].				M=0.3 anneal: 200C for 30h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32211	PRL0800385	fluorination(200C,50h)	HgBa2CuOzF1.0	Hg1Ba2Cu1O4	Hg	1	Ba	2	Cu	1															O	4		1	1998																												Hg1201			A	3.8679		9.459												K																																																																																																							Ba2CuO3+z +HgO synthesized [7].				M=1.0 anneal: 200C for 50h (M is the molar ratio of  XeF2 to Hg1201)	Effect of Fluorination on the Structure and Superconducting Properties of the Hg-1201 Phase	1		Department of Chemistry, Moscow State University, 119899 Moscow, Russia	Phys.Rev.Lett.,80(1998)385-388	A. M. Abakumov,A. M. Balagurov,A.M. Abakumov,A.M. Balagurov,D. A. Mikhailova,D.A. Mikhailova,E. V. Antipov,E.V. Antipov,M.G. Rozova,S. N. Putilin,S.N. Putilin,V. A. Alyoshin,V. L. Aksenov,V.A. Alyoshin,V.L. Aksenov		
32212	PRL0800841		PrBa2Cu3Oz	Pr1Ba2Cu3OZ	Pr	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																																																																																																mohmcm		666.67	50000		6.67	1428						1.25	8.33												ref[12]					Two-Dimentional Localization and Superconductor-Insulator Transition in Strongly Underdoped Single Craystals of Y1-xPrxBa2Cu3O7-delta	1		Department of Physics, Kent State University, Kent, Ohio 44242	Phys.Rev.Lett.,80(1998)841-844	C. C. Almasan,C.C. Almasan,D. A. Gajewski,D.A. Gajewki,G. A. Levin,G.A. Levin,M. B. Maple,M.B. Maple,S. H. Han,S.H. Han,T. Stein		
32213	PRL0801074		PrBa2Cu3Oz	Pr1Ba2Cu3OZ	Pr	1	Ba	2	Cu	3															O	Z		3	1998																											3	Y123	Pmmm		A	3.872	3.931	11.772	1											K	80						80		R	K/Gpa	3.9																																																																																										Pr5O11, BaCO3, CuO (4N)	7	Pr:Ba:Cu=1.05:1.95:2.96,  TSFZ method [13,14] in 0.1%O2+Ar flow gas				anneal: in a-Al2O3 crucible at 850 C for 24 h and then 550 C for 77h in O2 flow	Superconducting PrBa2Cu3Ox	1		Electrotechnical Laboratory, 1-1-4 Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.Lett.,80(1998)1074-1077	Jinhua Ye,Kunihiko Oka,Yoshikazu Nishihara,Zhigang Zou		
32214	PRL0801968	Anisotropy factor = 248	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1998																												Bi2212																		K			89				89																																																													W/K2m				THC32214																														7	TSFZ method [8]					Low-Temperature Anomaly in Thermal Conductivity of Bi2Sr2Ca(Cu1-xNix)2O8: Second Superconducting Phase?	1		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett.,80(1998)1968-1971	A. V. Balatsky,A.V. Balatsky,J. L. Sarrao,J.L. Sarrao,M. A. Hubbard,M. B. Salamon,M. Jaime,M.A. Hubbard,M.B. Salamon,R. Movshovich,R. Yoshizaki		
32215	PRL0801968	Ni-content estimated from earlier report (J.Low Temp.Phys., 105(1996)927). Anisotropy factor = 148.	Bi2Sr2Ca(Cu,Ni)2Oz	Bi2Sr2Ca1Cu1.98Ni0.02O8	Bi	2	Sr	2	Ca	1	Cu	1.98	Ni	0.02											O	8		3	1998																												Bi2212																		K			78				78																																																													W/K2m				THC32215																														7	TSFZ method [8]					Low-Temperature Anomaly in Thermal Conductivity of Bi2Sr2Ca(Cu1-xNix)2O8: Second Superconducting Phase?	1		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett.,80(1998)1968-1971	A. V. Balatsky,A.V. Balatsky,J. L. Sarrao,J.L. Sarrao,M. A. Hubbard,M. B. Salamon,M. Jaime,M.A. Hubbard,M.B. Salamon,R. Movshovich,R. Yoshizaki		
32216	PRL0801968	Ni-content estimated from earlier report (J.Low Temp.Phys., 105(1996)927). Anisotropy factor = 126.	Bi2Sr2Ca(Cu,Ni)2Oz	Bi2Sr2Ca1Cu1.97Ni0.03O8	Bi	2	Sr	2	Ca	1	Cu	1.97	Ni	0.03											O	8		3	1998																												Bi2212																		K			77				77																																																													W/K2m				THC32216																														7	TSFZ method [8]					Low-Temperature Anomaly in Thermal Conductivity of Bi2Sr2Ca(Cu1-xNix)2O8: Second Superconducting Phase?	1		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett.,80(1998)1968-1971	A. V. Balatsky,A.V. Balatsky,J. L. Sarrao,J.L. Sarrao,M. A. Hubbard,M. B. Salamon,M. Jaime,M.A. Hubbard,M.B. Salamon,R. Movshovich,R. Yoshizaki		
32217	PRL0801968	Ni-content estimated from earlier report (J.Low Temp.Phys., 105(1996)927). Anisotropy factor = 79.	Bi2Sr2Ca(Cu,Ni)2Oz	Bi2Sr2Ca1Cu1.952Ni0.048O8	Bi	2	Sr	2	Ca	1	Cu	1.952	Ni	0.048											O	8		3	1998																												Bi2212																		K			74				74																																																													W/K2m				THC32217																														7	TSFZ method [8]					Low-Temperature Anomaly in Thermal Conductivity of Bi2Sr2Ca(Cu1-xNix)2O8: Second Superconducting Phase?	1		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett.,80(1998)1968-1971	A. V. Balatsky,A.V. Balatsky,J. L. Sarrao,J.L. Sarrao,M. A. Hubbard,M. B. Salamon,M. Jaime,M.A. Hubbard,M.B. Salamon,R. Movshovich,R. Yoshizaki		
32223	PRL0805192		(Y,Ca)Ba2Cu3Oz	Y0.97Ca0.03Ba2Cu3O6	Y	0.97	Ca	0.03	Ba	2	Cu	3													O	7-Z	6	3	1998																												Y123																		K			0				0																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32224	PRL0805192		(Y,Ca)Ba2Cu3Oz	Y0.88Ca0.12Ba2Cu3O6	Y	0.88	Ca	0.12	Ba	2	Cu	3													O	7-Z	6	3	1998																												Y123																		K			0				0																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32225	PRL0805192		(Y,Ca)Ba2Cu3Oz	Y0.77Ca0.23Ba2Cu3O6	Y	0.77	Ca	0.23	Ba	2	Cu	3													O	7-Z	6	3	1998																												Y123																		K			0				0																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32226	PRL0805192		YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	7-Z	6.5	3	1998																												Y123																		K			55				55																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32227	PRL0805192		YBa2Cu3Oz	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	7-Z	6.91	3	1998																												Y123																		K			92				92																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32228	PRL0805192		(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3O6.91	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	7-Z	6.91	3	1998																												Y123																		K			78				78																																																																																																					Site-Specific X-Ray Absorption Spectroscopy of Y1-xCaxBa2Cu3O7-y : Overdoping and Role of Apical Oxygen for High Temperature Superconductivity	6		Forschungszentrum Karlsruhe, INFP, P.O. Box 3640, D-76021 Karlsruhe, Federal Republic of Germany	Phys.Rev.Lett.,80(1998)5192-5195	C. T. Chen,G.Muller-Vogt,J. Freeland,M. Klaser,M. Merz,N. Nucker,P. Schweiss,S. Schuppler,Th. Wolf,V. Chakarian,Y. U. Idzerda		
32229	PRL0811090	P-induced SC. Superconducting transition shows under high pressure. Tc=9K at 4.5 Gpa.	(Sr,Ca)14Cu24O41	Sr3.5Ca11.5Cu24O41	Sr	3.5	Ca	11.5	Cu	24															O	41	41	3	1998																												LAD																		K		9			0		9																																																																							mohmcm						0.33						7.5	0.9											7	TSFZ method under O2 gas at 10 atm.					Pressure-Induced Dimensional Crossover and Superconductivity in the Hole-Doped Two-Leg  LadderCompound Sr14-xCaxCu24O41	8		Department of Physics, Aoyama-Gakuin University, Chitosedai, Setagaya-ku, Tokyo 157, Japan	Phys.Rev.Lett.,81(1998)1090-1093	H. Eisaki,H. Takahashi,J. Akimitsu,J. Goto,M. Uehara,N. Motoyama,N.Mori,S. Uchida,T. Nagata,T. Nakanishi		
32231	PRL0812542	{110}STM	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K			90			1	90																																														meV	27	7																																																Crystal-pulling technique[18]				anneal: for 2week in O2 gas and reannealed in ultrapure O2 gas at 450C for 24h followed by slow cooling	Directional Tunneling and Andreev Reflection on YBa2Cu3O7-z Single Crystals : Predominance of d-Wave Pairing Symmetry Verified with the Generalized Blonder, Tinkham, and Klapwijk Theory	9		Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett.,81(1998)2542-2545	D. F. Garrigus,J. Y. T. Wei,M. Strasik,N.-C. Yeh		
32232	PRL0812542	{110}point contuct	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K			90			1	90																																														meV	27	7																																																Crystal-pulling technique[18]				anneal: for 2week in O2 gas and reannealed in ultrapure O2 gas at 450C for 24h followed by slow cooling	Directional Tunneling and Andreev Reflection on YBa2Cu3O7-z Single Crystals : Predominance of d-Wave Pairing Symmetry Verified with the Generalized Blonder, Tinkham, and Klapwijk Theory	9		Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett.,81(1998)2542-2545	D. F. Garrigus,J. Y. T. Wei,M. Strasik,N.-C. Yeh		
32233	PRL0812542	{100}STM	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K			90			1	90																																														meV	29	7.5																																																Crystal-pulling technique[18]				anneal: for 2week in O2 gas and reannealed in ultrapure O2 gas at 450C for 24h followed by slow cooling	Directional Tunneling and Andreev Reflection on YBa2Cu3O7-z Single Crystals : Predominance of d-Wave Pairing Symmetry Verified with the Generalized Blonder, Tinkham, and Klapwijk Theory	9		Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett.,81(1998)2542-2545	D. F. Garrigus,J. Y. T. Wei,M. Strasik,N.-C. Yeh		
32234	PRL0812542	{100}point contuct	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K			90			1	90																																														meV	28	7.2																																																Crystal-pulling technique[18]				anneal: for 2week in O2 gas and reannealed in ultrapure O2 gas at 450C for 24h followed by slow cooling	Directional Tunneling and Andreev Reflection on YBa2Cu3O7-z Single Crystals : Predominance of d-Wave Pairing Symmetry Verified with the Generalized Blonder, Tinkham, and Klapwijk Theory	9		Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett.,81(1998)2542-2545	D. F. Garrigus,J. Y. T. Wei,M. Strasik,N.-C. Yeh		
32235	PRL0812542	{001}STM	YBa2Cu3Oz	Y1Ba2Cu3OZ	Y	1	Ba	2	Cu	3															O	Z		3	1998																												Y123																		K			90			1	90																																														meV	19	4.9																																																Crystal-pulling technique[18]				anneal: for 2week in O2 gas and reannealed in ultrapure O2 gas at 450C for 24h followed by slow cooling	Directional Tunneling and Andreev Reflection on YBa2Cu3O7-z Single Crystals : Predominance of d-Wave Pairing Symmetry Verified with the Generalized Blonder, Tinkham, and Klapwijk Theory	9		Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett.,81(1998)2542-2545	D. F. Garrigus,J. Y. T. Wei,M. Strasik,N.-C. Yeh		
32236	PRL0814720		(Pr,Ce)2CuOz	Pr1.87Ce0.13Cu1OZ	Pr	1.87	Ce	0.13	Cu	1															O	Z		5	1998																												T'																		K			12				12																																																																							uohmcm					440			470																16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32237	PRL0814720		(Pr,Ce)2CuOz	Pr1.86Ce0.13Cu1OZ	Pr	1.86	Ce	0.13	Cu	1															O	Z		5	1998																												T'																		K			20				20																																																																							uohmcm					130			120																16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32238	PRL0814720		(Pr,Ce)2CuOz	Pr1.85Ce0.14Cu1OZ	Pr	1.85	Ce	0.14	Cu	1															O	Z		5	1998																												T'																		K			21				21																																																																							uohmcm								68																16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32239	PRL0814720		(Pr,Ce)2CuOz	Pr1.83Ce0.15Cu1OZ	Pr	1.83	Ce	0.15	Cu	1															O	Z		5	1998																												T'																		K			15				15																																																																							uohmcm								49																16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32240	PRL0814720		(Pr,Ce)2CuOz	Pr1.8Ce0.17Cu1OZ	Pr	1.8	Ce	0.17	Cu	1															O	Z		5	1998																												T'																		K			10				10																																																																							uohmcm								32																16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32241	PRL0814720		Pr2CuOz	Pr2Cu1OZ	Pr	2	Cu	1																	O	Z		5	1998																												T'																		K			0				0																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32242	PRL0814720		(Pr,Ce)2CuOz	Pr1.95Ce0.05Cu1OZ	Pr	1.95	Ce	0.05	Cu	1															O	Z		5	1998																												T'																		K			0				0																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32243	PRL0814720		(Pr,Ce)2CuOz	Pr1.9Ce0.1Cu1OZ	Pr	1.9	Ce	0.1	Cu	1															O	Z		5	1998																												T'																		K			0				0																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32244	PRL0814720		(Pr,Ce)2CuOz	Pr1.84Ce0.16Cu1OZ	Pr	1.84	Ce	0.16	Cu	1															O	Z		5	1998																												T'																		K			16				16																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32245	PRL0814720		(Pr,Ce)2CuOz	Pr1.82Ce0.18Cu1OZ	Pr	1.82	Ce	0.18	Cu	1															O	Z		5	1998																												T'																		K			13				13																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32246	PRL0814720		(Pr,Ce)2CuO4	Pr1.77Ce0.23Cu1OZ	Pr	1.77	Ce	0.23	Cu	1															O	Z		5	1998																												T'																		K			0				0																																																																																															16	ref[14, 15]					Insulator-Metal Crossover near Optimal Doping in Pr2-xCexCuO4: Anomalous Normal-State Low			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742	Phys.Rev.Lett.,81(1998)4720-4723	C. J. Lobb,E. Maiser,G. Czjzek,P. Fournier,P. Mohanty,R. A. Webb,R. L. Greene,S. Darzens,T. Venkatesan		
32247	PRL0815636	quench	TmBa2Cu3Oz	Tm1Ba2Cu3O6.37	Tm	1	Ba	2	Cu	3															O	7-Z	6.37		1998								35																				Y123																																																																																																mohmcm					0.6	1700						2	1350											5	ref[12]				anneal:ref[10]	Normal-State Resistivity Anisotropy in Underdoped RBa2Cu3O6+x Crystals	199812		Institute of Inorganic Chemistry, Siberian Branch of RAS, Lavrentyeva-3, 630090 Novosibirsk, Russia	Phys.Rev.Lett.,81(1998)5636-5639	A. N. Lavrov,L. P. Kozeeva,M. Yu. Kameneva		
32248	PRL0815636	not quench	TmBa2Cu3Oz	Tm1Ba2Cu3O6.37	Tm	1	Ba	2	Cu	3															O	7-Z	6.37		1998								60																				Y123																																																																																																mohmcm					0.4	1280						1.6	650											5	ref[12]				anneal:ref[10]	Normal-State Resistivity Anisotropy in Underdoped RBa2Cu3O6+x Crystals	199812		Institute of Inorganic Chemistry, Siberian Branch of RAS, Lavrentyeva-3, 630090 Novosibirsk, Russia	Phys.Rev.Lett.,81(1998)5636-5639	A. N. Lavrov,L. P. Kozeeva,M. Yu. Kameneva		
32249	PRL0815636		TmBa2Cu3Oz	Tm1Ba2Cu3O6.41	Tm	1	Ba	2	Cu	3															O	7-Z	6.41		1998																												Y123																		K			19				19																																																																							mohmcm						1350			1120				830											5	ref[12]				anneal:ref[10]	Normal-State Resistivity Anisotropy in Underdoped RBa2Cu3O6+x Crystals	199812		Institute of Inorganic Chemistry, Siberian Branch of RAS, Lavrentyeva-3, 630090 Novosibirsk, Russia	Phys.Rev.Lett.,81(1998)5636-5639	A. N. Lavrov,L. P. Kozeeva,M. Yu. Kameneva		
32250	PRL0815636		TmBa2Cu3Oz	Tm1Ba2Cu3O6.44	Tm	1	Ba	2	Cu	3															O	7-Z	6.44		1998																												Y123																		K			28				28																																																																							mohmcm						1030			100				420											5	ref[12]				anneal:ref[10]	Normal-State Resistivity Anisotropy in Underdoped RBa2Cu3O6+x Crystals	199812		Institute of Inorganic Chemistry, Siberian Branch of RAS, Lavrentyeva-3, 630090 Novosibirsk, Russia	Phys.Rev.Lett.,81(1998)5636-5639	A. N. Lavrov,L. P. Kozeeva,M. Yu. Kameneva		
32251	PRL0815636		TmBa2Cu3Oz	Tm1Ba2Cu3O6.49	Tm	1	Ba	2	Cu	3															O	7-Z	6.49		1998																												Y123																		K			50				50																																																																							mohmcm						700			750				250											5	ref[12]				anneal:ref[10]	Normal-State Resistivity Anisotropy in Underdoped RBa2Cu3O6+x Crystals	199812		Institute of Inorganic Chemistry, Siberian Branch of RAS, Lavrentyeva-3, 630090 Novosibirsk, Russia	Phys.Rev.Lett.,81(1998)5636-5639	A. N. Lavrov,L. P. Kozeeva,M. Yu. Kameneva		
32300	PRL0820410		Bi2(Sr,La)2CuOz	Bi2Sr1.75La0.25Cu1OZ	Bi	2	Sr	1.75	La	0.25	Cu	1													O	Z		3	1999																												Bi2201																		K			27				27																																	-1																																																														5	using CuO as flux					Josephson-Coupling Origin for the Upward Curvature of the Pseudo-Upper-Critical Field in Bi2Sr2-xLaxCuO6+z  Crystals	1		National Laboratory for Superconductivity, Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.Lett.,82(1999)410-413	H. H. Wen,W. L. Yang,Y. M. Ni,Z. X. Zhao		
32301	PRL0821313		(Sr,Ca)14Cu24O41	Sr6Ca8Cu24O41	Sr	6	Ca	8	Cu	24															O	41	41	3	1999																												LAD																																																																																																mohmcm						0.4						21	1.9												ref[9]					Pseudogap and Collective Mode in the Optical Conductivity Spectra of Hole-Doped Ladders in Sr14-xCaxCu24O41	2		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,82(1999)1313-1316	H. Eisaki,N. Motoyama,S. Tajima,S. Uchida,T. Osafune		
32302	PRL0821313		(Sr,Ca)14Cu24O41	Sr3Ca11Cu24O41	Sr	3	Ca	11	Cu	24															O	41	41	3	1999																												LAD																																																																																																mohmcm												12	0.9												ref[9]					Pseudogap and Collective Mode in the Optical Conductivity Spectra of Hole-Doped Ladders in Sr14-xCaxCu24O41	2		Department of Superconductivity, The University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett.,82(1999)1313-1316	H. Eisaki,N. Motoyama,S. Tajima,S. Uchida,T. Osafune		
32303	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7-Z	7	3	1999																												Y123																		K			87.8				87.8																																																						mJ/K.mol	5004	mJ/mol.K2	3.08	linear term below Tc	191																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32304	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	7-Z	6.98	3	1999																												Y123																		K			90.3				90.3																																																						mJ/K.mol	4966	mJ/mol.K2	2.97	linear term below Tc	175																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32305	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	7-Z	6.96	3	1999																												Y123																		K			91.8				91.8																																																						mJ/K.mol	4957	mJ/mol.K2	2.79	linear term below Tc	173																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32306	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.94	Y	1	Ba	2	Cu	3															O	7-Z	6.94	3	1999																												Y123																		K			93.5				93.5																																																						mJ/K.mol	4768	mJ/mol.K2	2.68	linear term below Tc	172																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32307	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	7-Z	6.91	3	1999																												Y123																		K			95.2				95.2																																																						mJ/K.mol	4284	mJ/mol.K2	2.71	linear term below Tc	173																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32308	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.87	Y	1	Ba	2	Cu	3															O	7-Z	6.87	3	1999																												Y123																		K			95.2				95.2																																																						mJ/K.mol	3522	mJ/mol.K2	3.32	linear term below Tc	176																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32309	PRL0821546		YBa2Cu3OZ	Y1Ba2Cu3O6.82	Y	1	Ba	2	Cu	3															O	7-Z	6.82	3	1999																												Y123																		K			89.9				89.9																																																						mJ/K.mol	1800	mJ/mol.K2	3.87	linear term below Tc	179																																										Specific Heat of YBa2Cu3O7-z , 0<=z<=0.2 : Concentrations of Paramagnetic Centers and Values of Other Parameters as Functions of z	2		Department of Chemistry, University of California and Lawrence Berkeley National Laboratory, Berkeley, California 94720	Phys.Rev.Lett.,82(1999)1546-1549	B. F. Woodfield,D. A. Wright,J. E. Gordon,J. P. Emerson,N. E. Phillips,R. A. Fisher		
32310	PRL0823148		Bi2Sr2CaCu2OZ	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212																		K			88.4				88.4			K/GPa	1.69																																																																																																	Interlayer Coupling and Superconducting Critical Temperature of Bi2Sr1.5La0.5CuO6+z and Bi2Sr2CaCu2O8+z : Incommensurate Effects of Pressure	4		Department of Microelectronics and Nanoscience, Chalmers University of Technology and Goteborg University, S-41296 Goteborg, Sweden	Phys.Rev.Lett.,82(1999)3148-3151	A. Yurgens,D. Winkler,T. Claeson,T. Murayama,Y. Ando		
32311	PRL0823148		Bi2(Sr,La)2CuOz	Bi2Sr1.5La0.5Cu1OZ	Bi	2	Sr	1.5	La	0.5	Cu	1													O	Z		3	1999																												Bi2201																		K			8.2				8.2			K/GPa	0.47																																																																																																	Interlayer Coupling and Superconducting Critical Temperature of Bi2Sr1.5La0.5CuO6+z and Bi2Sr2CaCu2O8+z : Incommensurate Effects of Pressure	4		Department of Microelectronics and Nanoscience, Chalmers University of Technology and Goteborg University, S-41296 Goteborg, Sweden	Phys.Rev.Lett.,82(1999)3148-3151	A. Yurgens,D. Winkler,T. Claeson,T. Murayama,Y. Ando		
32312	PRL0824300		(La,Sr)2CuO4	La1.93Sr0.07Cu1O4	La	1.93	Sr	0.07	Cu	1															O	4			1999																												T																		K			19				19																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32313	PRL0824300		(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4			1999																												T																		K			29				29																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32314	PRL0824300		(La,Sr)2CuO4	La1.885Sr0.115Cu1O4	La	1.885	Sr	0.115	Cu	1															O	4			1999																												T																		K			31				31																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32315	PRL0824300		(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4			1999																												T																		K			31				31																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32316	PRL0824300		(La,Sr)2CuO4	La1.865Sr0.135Cu1O4	La	1.865	Sr	0.135	Cu	1															O	4			1999																												T																		K			35				35																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32317	PRL0824300		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1999																												T																		K			38				38																																																																																																standard solid state reactions [17]					<63>Cu NQR Measurement of Stripe Order Parameter in La2-xSrxCuO4	5		Department of Physics and Center for Materials Science and Engineering, M.I.T., Cambridge, Massachusetts 02139	Phys.Rev.Lett.,82(1999)4300-4303	A. W. Hunt,K. R. Thurber,P. M. Singer,T. Imai		
32318	PRL0825120		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1OZ	Nd	1.85	Ce	0.15	Cu	1															O	Z		3	1999								150																				T'																																																																																																																								7	TSFZ method in O2 atmosphere of 4 atm				anneal: Ar gas for 100h at 1000 C and subsequently in O2 for 50 h at 500 C	Anomalous Pseudogap Formation in a Nonsuperconducting Crystal of Nd1.85Ce0.15CuO4+y : Implication of Charge Ordering	6		Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.Lett.,82(1999)5120-5123	K. Ishizaka,S. Shinomori,T. Ishikawa,Y. Onose,Y. Taguchi,Y. Tokura		
32319	PRL0825361	over doped: The superconducting gap is estimated by the interlayer tunneling spectroscopy experiments.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212																		K			87.1				87.1																																														meV	50																																																7	TSFZ method [6]				anneal : at 600 C for 100 h	Interlayer Tunneling Spectroscopy for Slightly Overdoped Bi2Sr2CaCu2O8+z	6		NTT Basic Research Laboratories, Nippon Telegraph and Telephone Corporation, 162 Tokai, Ibaraki 319-1193, Japan	Phys.Rev.Lett.,82(1999)5361-5364	Azusa Matsuda,Minoru Suzuki,Takao Watanabe		
32320	PRL0831018	optimal doped: The superconducting gap is estimated by SIS tunneling conductances.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212																		K			95				95																																														meV	35																																																7	a slightly modified FZ method [2]					Predominantly Superconducting Origin of Large Energy Gaps in Underdoped Bi2Sr2CaCu2O8+z from Tunneling Spectroscopy	8		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.Lett.,83(1999)1018-1021	C. Kendziora,D. G. Hinks,J. F. Zasadzinski,K. E. Gray,L. Ozyuzer,N. Miyakawa,P. Guptasarma		
32321	PRL0831018	over doped: The superconducting gap is estimated by SIS tunneling conductances.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212																		K			62				62																																														meV	17																																																7	a slightly modified FZ method [2]					Predominantly Superconducting Origin of Large Energy Gaps in Underdoped Bi2Sr2CaCu2O8+z from Tunneling Spectroscopy	8		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.Lett.,83(1999)1018-1021	C. Kendziora,D. G. Hinks,J. F. Zasadzinski,K. E. Gray,L. Ozyuzer,N. Miyakawa,P. Guptasarma		
32322	PRL0831018	under doped: The superconducting gap is estimated by SIS tunneling conductances.	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	1999																												Bi2212																		K			70				70																																														meV	50																																																7	a slightly modified FZ method [2]					Predominantly Superconducting Origin of Large Energy Gaps in Underdoped Bi2Sr2CaCu2O8+z from Tunneling Spectroscopy	8		Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.Lett.,83(1999)1018-1021	C. Kendziora,D. G. Hinks,J. F. Zasadzinski,K. E. Gray,L. Ozyuzer,N. Miyakawa,P. Guptasarma		
32323	PRL0831419		YBa2Cu3Oz	Y1Ba2Cu3O6.32	Y	1	Ba	2	Cu	3															O	7-Z	6.32	3	1999								205																				Y123																																																																																																mohmcm		3.5			1.3	4950						3.5	2600											5						Magnetoresistance in Heavily Underdoped YBa2Cu3O6+x : Antiferromagnetic Correlations and Normal-State Transport	8		Central Research Institute of Electric Power Industry, 2-11-1 Iwato-kita, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett.,83(1999)1419-1422	A. N. Lavrov,J. Takeya,Kouji Segawa,Yoichi Ando		
32324	PRL0831419		YBa2Cu3Oz	Y1Ba2Cu3O6.33	Y	1	Ba	2	Cu	3															O	7-Z	6.33	3	1999								160																				Y123																																																																																																mohmcm						3700							2000											5						Magnetoresistance in Heavily Underdoped YBa2Cu3O6+x : Antiferromagnetic Correlations and Normal-State Transport	8		Central Research Institute of Electric Power Industry, 2-11-1 Iwato-kita, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett.,83(1999)1419-1422	A. N. Lavrov,J. Takeya,Kouji Segawa,Yoichi Ando		
32325	PRL0831419		YBa2Cu3Oz	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	7-Z	6.35	3	1999								77																				Y123																																																																																																mohmcm			6100			2500							1400											5						Magnetoresistance in Heavily Underdoped YBa2Cu3O6+x : Antiferromagnetic Correlations and Normal-State Transport	8		Central Research Institute of Electric Power Industry, 2-11-1 Iwato-kita, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett.,83(1999)1419-1422	A. N. Lavrov,J. Takeya,Kouji Segawa,Yoichi Ando		
32326	PRL0832254	The superconducting gap is estimated by photoemission spectroscopy.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	Z	4	3	1999																												T																		K			38				38																																														meV	8																																																7	TSFZ method				anneal: under O2 flow at 900 C for 50 h	Pseudogap of Optimally Doped La1.85Sr0.15CuO4 Observed by Ultrahigh-Resolution Photoemission Spectroscopy	9		Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.Lett.,83(1999)2254-2257	K. Yamada,T. Sato,T. Takahashi,T. Yokoya,Y. Endoh,Y. Naitoh		
32327	PRL0832644		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1OZ	Nd	1.85	Ce	0.15	Cu	1															O	Z		5	1999			emuK/mol	0.2			2																					T'																		K			24				24																																														meV	3																																																						Anomalous Low Temperature Behavior of Superconducting Nd1.85Ce0.15CuO4-y	9		II. Physikalisches Institut, Universitat zu Koln, Zulpicher Strasse 77, D-50937 Koln, Germany	Phys.Rev.Lett.,83(1999)2644-2647	A. Marx,H. Sato,L. Alff,M. Naito,R. Gross,S. Kleefisch,S. Meyer,U. Schoop		
32328	PRL0833289		(La,Sr,Ba)2CuOz	La1.85Sr0.038Ba0.112Cu1O4	La	1.85	Sr	0.038	Ba	0.112	Cu	1													O	Z	4		1999																												T			A	3.78905		13.2979												K				32			32																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32329	PRL0833289		(La,Nd,Sr,Ba)2CuOz	La1.842Nd0.008Sr0.036Ba0.114Cu1O3.98	La	1.842	Nd	0.008	Sr	0.036	Ba	0.114	Cu	1											O	Z	3.98		1999																												T			A	3.78524		13.2829												K				31.7			31.7																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32330	PRL0833289		(La,Nd,Sr,Ba)2CuOz	La1.812Nd0.038Sr0.026Ba0.124Cu1O4	La	1.812	Nd	0.038	Sr	0.026	Ba	0.124	Cu	1											O	Z	4		1999																												T			A	3.78607		13.2868												K				31.1			31.1																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32331	PRL0833289		(La,Nd,Sr,Ba)2CuOz	La1.776Nd0.074Sr0.014Ba0.136Cu1O4.03	La	1.776	Nd	0.074	Sr	0.014	Ba	0.136	Cu	1											O	Z	4.03		1999																												T			A	3.78627		13.2817												K				30			30																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32332	PRL0833289		(La,Nd,Ba)2CuOz	La1.736Nd0.116Ba0.15Cu1O4.03	La	1.736	Nd	0.116	Ba	0.15	Cu	1													O	Z	4.03		1999																												T			A	3.78601		13.28												K				29			29																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32333	PRL0833289		(La,Sr)2CuOz	La1.85Sr0.15Cu1O4.01	La	1.85	Sr	0.15	Cu	1															O	Z	4.01		1999																												T			A	3.7773		13.2378												K			35.4	36			36		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32334	PRL0833289		(La,Sr,Ca,Ba)2CuOz	La1.85Sr0.12Ca0.016Ba0.014Cu1O3.99	La	1.85	Sr	0.12	Ca	0.016	Ba	0.014	Cu	1											O	Z	3.99		1999																												T			A	3.778		13.2357												K			31.5	34.1			34.1		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32335	PRL0833289		(La,Sr,Ca,Ba)2CuOz	La1.85Sr0.09Ca0.034Ba0.026Cu1O3.99	La	1.85	Sr	0.09	Ca	0.034	Ba	0.026	Cu	1											O	Z	3.99		1999																												T			A	3.7783		13.2302												K			31.3	32.2			32.2		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32336	PRL0833289		(La,Sr,Ca,Ba)2CuOz	La1.85Sr0.06Ca0.05Ba0.04Cu1O3.99	La	1.85	Sr	0.06	Ca	0.05	Ba	0.04	Cu	1											O	Z	3.99		1999																												T			A	3.7796		13.2272												K			26.2	30			30		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32337	PRL0833289		(La,Sr,Ca,Ba)2CuOz	La1.85Sr0.016Ca0.074Ba0.06Cu1O4.01	La	1.85	Sr	0.016	Ca	0.074	Ba	0.06	Cu	1											O	Z	4.01		1999																												T			A	3.7838		13.239												K			24.9	25.4			25.4		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32338	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.8Nd0.05Ca0.074Ba0.076Cu1O4.01	La	1.8	Nd	0.05	Ca	0.074	Ba	0.076	Cu	1											O	Z	4.01		1999																												T			A	13.2242		13.2242												K			17.3	23.7			23.7		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32339	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.75Nd0.1Ca0.064Ba0.086Cu1O4.03	La	1.75	Nd	0.1	Ca	0.064	Ba	0.086	Cu	1											O	Z	4.03		1999																												T			A	13.2158	5.344	13.2158												K			16	20.6			20.6		R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32340	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.7Nd0.15Ca0.056Ba0.094Cu1O4.02	La	1.7	Nd	0.15	Ca	0.056	Ba	0.094	Cu	1											O	Z	4.02		1999																												T			A	13.2141	5.344	13.2141												K									R																																																																																																		Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32341	PRL0833289		(La,Nd,Ca)2CuOz	La1.798Nd0.052Ca0.15Cu1O3.96	La	1.798	Nd	0.052	Ca	0.15	Cu	1													O	Z	3.96		1999																												T			A	5.34472	5.33694	13.1778												K				31.6			31.6																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32342	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.736Nd0.114Ca0.138Ba0.012Cu1O4.02	La	1.736	Nd	0.114	Ca	0.138	Ba	0.012	Cu	1											O	Z	4.02		1999																												T			A	5.3473	5.33619	13.1708												K				29.4			29.4																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32343	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.65Nd0.2Ca0.122Ba0.028Cu1O3.99	La	1.65	Nd	0.2	Ca	0.122	Ba	0.028	Cu	1											O	Z	3.99		1999																												T			A	5.35276	5.33529	13.1597												K				27.1			27.1																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32344	PRL0833289		(La,Nd,Ca,Ba)2CuOz	La1.562Nd0.288Ca0.106Ba0.044Cu1O3.98	La	1.562	Nd	0.288	Ca	0.106	Ba	0.044	Cu	1											O	Z	3.98		1999																												T			A	5.35706	5.33389	13.1492												K				23			23																																																																																																				Oxygen contents were determined by iodometric titration.	Systematic Cation Disorder Effects in L1.85M0.15CuO4 Superconductors	10		Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom and the Interdisciplinary Research Centre in Superconductivity, Madingley Road, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett.,83(1999)3289-3292	J. Paul Attfield,Judith A. McAllister		
32345	PRL0834156	detwinned	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	7-Z	6.95	3	1999																												Y123																		K			93.2				93.2																																				A	uSR			83																																																													Field Induced Reduction of the Low-Temperature Superfluid Density in YBa2Cu3O6.95	10		Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett.,83(1999)4156-4159	D. A. Bonn,G. D. Morris,J. Chakhalian,J. E. Sonier,J. H. Brewer,R. F. Kiefl,R. H. Heffner,R. I. Miller,R. Liang,W.N. Hardy		
32346	PRL0834381		YBa2(Cu,Li)3Oz	Y1Ba2Cu2.97Li0.03O7-Z	Y	1	Ba	2	Cu	2.97	Li	0.03													O	7-Z		3	1999																												Y123																		K			86				86																																																																																														Y2O3, BaO2, CuO, Li2CO3	1					Z=6.6 samples were performed at fixed temperature ranging from 340 C to 450 C under vacuum.	Spinless Impurities in High-Tc Cuprates: Kondo-Like Behavior	11		Laboratoire de Physique des Solides, UMR 8502, Universiti Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,83(1999)4381-4384	G. Collin,H. Alloul,J. Bobroff,J.-F. Marucco,N. Blanchard,P. Mendels,W. A. MacFarlane		
32347	PRL0834381		YBa2(Cu,Li)3Oz	Y1Ba2Cu2.94Li0.06O7-Z	Y	1	Ba	2	Cu	2.94	Li	0.06													O	7-Z		3	1999																												Y123																		K			78				78																																																																																														Y2O3, BaO2, CuO, Li2CO3	1					Z=6.6 samples were performed at fixed temperature ranging from 340 C to 450 C under vacuum.	Spinless Impurities in High-Tc Cuprates: Kondo-Like Behavior	11		Laboratoire de Physique des Solides, UMR 8502, Universiti Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,83(1999)4381-4384	G. Collin,H. Alloul,J. Bobroff,J.-F. Marucco,N. Blanchard,P. Mendels,W. A. MacFarlane		
32348	PRL0834381		YBa2(Cu,Li)3Oz	Y1Ba2Cu2.79Li0.21O7-Z	Y	1	Ba	2	Cu	2.79	Li	0.21													O	7-Z		3	1999																												Y123																		K			53				53																																																																																														Y2O3, BaO2, CuO, Li2CO3	1					Z=6.6 samples were performed at fixed temperature ranging from 340 C to 450 C under vacuum.	Spinless Impurities in High-Tc Cuprates: Kondo-Like Behavior	11		Laboratoire de Physique des Solides, UMR 8502, Universiti Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,83(1999)4381-4384	G. Collin,H. Alloul,J. Bobroff,J.-F. Marucco,N. Blanchard,P. Mendels,W. A. MacFarlane		
32349	PRL0834381		YBa2(Cu,Li)3Oz	Y1Ba2Cu2.97Li0.03O6.6	Y	1	Ba	2	Cu	2.97	Li	0.03													O	7-Z	6.6	3	1999																												Y123																		K			41				41																																																																																														Y2O3, BaO2, CuO, Li2CO3	1					Z=6.6 samples were performed at fixed temperature ranging from 340 C to 450 C under vacuum.	Spinless Impurities in High-Tc Cuprates: Kondo-Like Behavior	11		Laboratoire de Physique des Solides, UMR 8502, Universiti Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,83(1999)4381-4384	G. Collin,H. Alloul,J. Bobroff,J.-F. Marucco,N. Blanchard,P. Mendels,W. A. MacFarlane		
32350	PRL0834381		YBa2(Cu,Li)3Oz	Y1Ba2Cu2.94Li0.06O6.6	Y	1	Ba	2	Cu	2.94	Li	0.06													O	7-Z	6.6	3	1999																												Y123																		K			26				26																																																																																														Y2O3, BaO2, CuO, Li2CO3	1					Z=6.6 samples were performed at fixed temperature ranging from 340 C to 450 C under vacuum.	Spinless Impurities in High-Tc Cuprates: Kondo-Like Behavior	11		Laboratoire de Physique des Solides, UMR 8502, Universiti Paris-Sud, 91405 Orsay, France	Phys.Rev.Lett.,83(1999)4381-4384	G. Collin,H. Alloul,J. Bobroff,J.-F. Marucco,N. Blanchard,P. Mendels,W. A. MacFarlane		
32400	PRL0840155	c-axis oriented film.  thickness=5000 - 9000A. 	(La,Sr)2CuO4	La1.85Sr0.15Cu1OZ	La	1.85	Sr	0.15	Cu	1															O	Z		5	2000																												T																																																																		A			9800																																																			16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32401	PRL0840155	c-axis oriented film. thickness=5000 - 9000A. 	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01OZ	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	Z		5	2000																												T																																																																		A			10000																																																			16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32402	PRL0840155	c-axis oriented film. thickness=5000 - 9000A. 	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.975Zn0.025OZ	La	1.85	Sr	0.15	Cu	0.975	Zn	0.025													O	Z		5	2000																												T																																																																		A			16000																																																			16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32403	PRL0840155	c-axis oriented film. thickness=5000 - 9000A. 	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.97Zn0.03OZ	La	1.85	Sr	0.15	Cu	0.97	Zn	0.03													O	Z		5	2000																												T																																																																		A	Penetration depth is obtained by the mutal inductance of coil detailed (ref[6]).		19300																																																			16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32404	PRL0840155		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.945Zn0.055OZ	La	1.85	Sr	0.15	Cu	0.945	Zn	0.055													O	Z		5	2000																												T																																																																																																mohmcm		0.3			0.6			0.5				1.2												16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32405	PRL0840155		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.92Zn0.08OZ	La	1.85	Sr	0.15	Cu	0.92	Zn	0.08													O	Z		5	2000																												T																																																																																																mohmcm		0.6			0.6							1												16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32406	PRL0840155		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9Zn0.1OZ	La	1.85	Sr	0.15	Cu	0.9	Zn	0.1													O	Z		5	2000																												T																																																																																																mohmcm		0.8			0.75							1.3												16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32407	PRL0840155		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.88Zn0.12OZ	La	1.85	Sr	0.15	Cu	0.88	Zn	0.12													O	Z		5	2000																												T																		K			35.2				35.2																																																																							mohmcm		1.5			1.4							2.2												16	LaSrAlO4 substrates					Metallic Nonsuperconducting Phase and D-Wave Superconductivity in Zn-Substituted La1.85Sr0.15CuO4	1		Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland	Phys.Rev.Lett.,84(2000)155-158	A. Malinowski,B. Boyce,K. Karpinska,M. Berkowski,Marta Z. Cieplak,P. Lindenfeld,S. Guha,T. Skoskiewicz,Thomas R. Lemberger,W. Plesiewicz		
32408	PRL0841587	anisotropy factor = 530 for p = 0 GPa from Hirr using curve fitting.  = 130 for 2.5 GPa. 	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2OZ	Bi	2	Sr	2	Ca	1	Cu	2													O	Z		3	2000																												Bi2212																		K			86.3				86.3																																									A			2080																																																			5	self-flux method    Bi:Sr:Ca:Cu=2:2:1:2					Pressure Dependence of the Irreversibility Line in Bi2Sr2CaCu2O8+z : Role of Anisotropy in Flux-Line Formation	2		Catholic University of America, Washington, D.C. 20064	Phys.Rev.Lett.,84(2000)1587-1590	C. Kendziora,E. F. Skelton,M. E. Reeves,M. P. Raphael		
32409	PRL0845612		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	2000																												T							3											K	33					3	33																																																								mJ/molK2	1.54																																					La2O3, SrCO3, CuO(5N)		ref[7]					Depression of Quasiparticle Density of States at Zero Energy in La1.9Sr0.1Cu1-xZnxO4	6		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.Lett.,84(2000)5612-5615	C. F. Chang,H. D. Yang,J.-Y. Lin		
32410	PRL0845612		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.99Zn0.01O4	La	1.9	Sr	0.1	Cu	0.99	Zn	0.01													O	4		1	2000																												T							3											K	14					4	14																																																								mJ/molK2	5.5																																					La2O3, SrCO3, CuO(5N)		ref[7]					Depression of Quasiparticle Density of States at Zero Energy in La1.9Sr0.1Cu1-xZnxO4	6		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.Lett.,84(2000)5612-5615	C. F. Chang,H. D. Yang,J.-Y. Lin		
32411	PRL0845612		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.98Zn0.02O4	La	1.9	Sr	0.1	Cu	0.98	Zn	0.02													O	4		1	2000																												T							3											K	2						2																																																								mJ/molK2	6																																					La2O3, SrCO3, CuO(5N)		ref[7]					Depression of Quasiparticle Density of States at Zero Energy in La1.9Sr0.1Cu1-xZnxO4	6		Department of Physics, National Sun Yat-Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.Lett.,84(2000)5612-5615	C. F. Chang,H. D. Yang,J.-Y. Lin		
32412	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.77La0.23Cu1OZ	Bi	2	Sr	1.77	La	0.23	Cu	1													O	Z		3	2000																												Bi2201																		K	29.5						29.5		R																																																																					mohmcm					0.13			0.1				0.38												7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32413	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.61La0.39Cu1OZ	Bi	2	Sr	1.61	La	0.39	Cu	1													O	Z		3	2000																												Bi2201																		K	37						37		R																																																																					mohmcm					0.18			0.15				0.5								RH32413				7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32414	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.34La0.66Cu1OZ	Bi	2	Sr	1.34	La	0.66	Cu	1													O	Z		3	2000																												Bi2201																		K	23						23		R																																																																					mohmcm					0.31			0.24				0.95												7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32415	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.27La0.73Cu1OZ	Bi	2	Sr	1.27	La	0.73	Cu	1													O	Z		3	2000																												Bi2201																		K	14						14		R																																																																					mohmcm					0.5			0.32				1.2								RH32415				7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32416	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.24La0.76Cu1OZ	Bi	2	Sr	1.24	La	0.76	Cu	1													O	Z		3	2000																												Bi2201																		K	13						13		R																																																																					mohmcm					0.7			0.58				1.45												7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32417	PRL0850638		Bi2(Sr,La)2CuOz	Bi2Sr1.16La0.84Cu1OZ	Bi	2	Sr	1.16	La	0.84	Cu	1													O	Z		3	2000																												Bi2201																		K	3						3		R																																																																					mohmcm					0.91			0.94				1.55								RH32417				7					anneal: 650 C for 48h at O2 flow	Metal-to-Insulator Crossover in the Low-Temperature Normal State of Bi2Sr2-xLaxCuO6 +z	7		Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 85(2000)638-641	F. F. Balakirev,F.F.Balakirev,G. S. Boebinger,G.S.Boebinger,J. B. Betts,J.B.Betts,S. Ono,S.Ono,T. Murayama,T.Murayama,Yoichi Ando		
32418	PRL0845848	optimal	Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.25	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.25	3	2000																												Bi2212																		K			92				92		R																																																																					ohmcm									6.8				3.1											7					anneal: at 600 C for 20-30h slowly cooled to 300-400 C	Pseudogap in Bi2Sr2CaCu2O8+z  Studied by Measuring Anisotropic Susceptibilities and Out-of-Plane Transport	6		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-Shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.,84(2000)5848-5851	Azusa Matsuda,Takao Watanabe,Takenori Fujii		
32419	PRL0845848		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.26	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.26	3	2000																												Bi2212																		K			90				90		R																																																																					ohmcm									4.6				2.6											7					anneal: at 600 C for 20-30h slowly cooled to 300-400 C	Pseudogap in Bi2Sr2CaCu2O8+z  Studied by Measuring Anisotropic Susceptibilities and Out-of-Plane Transport	6		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-Shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.,84(2000)5848-5851	Azusa Matsuda,Takao Watanabe,Takenori Fujii		
32420	PRL0845848		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.27	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.27	3	2000																												Bi2212																		K			87				87		R																																																																					ohmcm									2.8				2											7					anneal: at 600 C for 20-30h slowly cooled to 300-400 C	Pseudogap in Bi2Sr2CaCu2O8+z  Studied by Measuring Anisotropic Susceptibilities and Out-of-Plane Transport	6		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-Shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.,84(2000)5848-5851	Azusa Matsuda,Takao Watanabe,Takenori Fujii		
32421	PRL0845848		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.28	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.28	3	2000																												Bi2212																		K			80				80		R																																																																					ohmcm									1.8				1.5											7					anneal: at 600 C for 20-30h slowly cooled to 300-400 C	Pseudogap in Bi2Sr2CaCu2O8+z  Studied by Measuring Anisotropic Susceptibilities and Out-of-Plane Transport	6		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-Shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.,84(2000)5848-5851	Azusa Matsuda,Takao Watanabe,Takenori Fujii		
32422	PRL0845848		Bi2Sr2CaCu2Oz	Bi2Sr2Ca1Cu2O8.3	Bi	2	Sr	2	Ca	1	Cu	2													O	8+Z	8.3	3	2000																												Bi2212																		K			70				70		R																																																																					ohmcm									0.6				0.9											7					anneal: 400 atm at 500 C for 50 h	Pseudogap in Bi2Sr2CaCu2O8+z  Studied by Measuring Anisotropic Susceptibilities and Out-of-Plane Transport	6		NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-Shi, Kanagawa 243-0198, Japan	Phys.Rev.Lett.,84(2000)5848-5851	Azusa Matsuda,Takao Watanabe,Takenori Fujii		
32423	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu)2CuO4	La1.8Eu0.2Cu1O4	La	1.8	Eu	0.2	Cu	1															O	4			2000								300																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32424	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.836Eu0.2Sr0.014Cu1O4	La	1.836	Eu	0.2	Sr	0.014	Cu	1													O	4			2000								190																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32425	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.835Eu0.2Sr0.015Cu1O4	La	1.835	Eu	0.2	Sr	0.015	Cu	1													O	4			2000								160																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32426	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.832Eu0.2Sr0.018Cu1O4	La	1.832	Eu	0.2	Sr	0.018	Cu	1													O	4			2000								130																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32427	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.83Eu0.2Sr0.02Cu1O4	La	1.83	Eu	0.2	Sr	0.02	Cu	1													O	4			2000								10																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32428	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.82Eu0.2Sr0.03Cu1O4	La	1.82	Eu	0.2	Sr	0.03	Cu	1													O	4			2000								9																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32429	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.81Eu0.2Sr0.04Cu1O4	La	1.81	Eu	0.2	Sr	0.04	Cu	1													O	4			2000								7																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32430	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.77Eu0.2Sr0.08Cu1O4	La	1.77	Eu	0.2	Sr	0.08	Cu	1													O	4			2000								6																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32431	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.76Eu0.2Sr0.09Cu1O4	La	1.76	Eu	0.2	Sr	0.09	Cu	1													O	4			2000								14																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32432	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.75Eu0.2Sr0.1Cu1O4	La	1.75	Eu	0.2	Sr	0.1	Cu	1													O	4			2000								15																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32433	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.73Eu0.2Sr0.12Cu1O4	La	1.73	Eu	0.2	Sr	0.12	Cu	1													O	4			2000								25																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32434	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.7Eu0.2Sr0.15Cu1O4	La	1.7	Eu	0.2	Sr	0.15	Cu	1													O	4			2000								24																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32435	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.67Eu0.2Sr0.18Cu1O4	La	1.67	Eu	0.2	Sr	0.18	Cu	1													O	4			2000								22																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32436	PRL0854590	Neel temperature was determined by uSR measurements.	(La,Eu,Sr)2CuO4	La1.65Eu0.2Sr0.2Cu1O4	La	1.65	Eu	0.2	Sr	0.2	Cu	1													O	4			2000								8																				T																																																																																																																									ref[9,11,12]					From Antiferromagnetic Order to Static Magnetic Stripes: The Phase Diagram of (La,Eu)2-xSrxCuO4	10		Institut for Metallphysik und Nukleare Festkorperphysik, TU Braunschweig, D-38106 Braunschweig, Germany	Phys.Rev.Lett.,85(2000)4590-4593	B. Buchner,F. J. Litterst,H. Walf,H.-H. Klauss,M. Hillberg,M. Hucker,W. Kopmann,W. Wagener		
32441	PRL0853696	Tc from surface resistance	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1OZ	Pr	1.85	Ce	0.15	Cu	1															O	Z		3	2000																												T'																		K		19				1.5	19																																									A			295				1.89																																															1						Microwave Electrodynamics of Electron-Doped Cuprate Superconductors	10		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742-4111	Phys.Rev.Lett.,85(2000)3696-3699	J. David Kokales,Lucia V. Mercaldo,Patrick Fournier,Richard L. Greene,Steven M. Anlage,Vladimir V. Talanov		
32442	PRL0853696	Tc from surface resistance	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1OZ	Pr	1.85	Ce	0.15	Cu	1															O	Z		3	2000																												T'																		K		19				1.7	19																																									A			390				1.37																																															1						Microwave Electrodynamics of Electron-Doped Cuprate Superconductors	10		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742-4111	Phys.Rev.Lett.,85(2000)3696-3699	J. David Kokales,Lucia V. Mercaldo,Patrick Fournier,Richard L. Greene,Steven M. Anlage,Vladimir V. Talanov		
32443	PRL0853696	Film. Tc from ac susceptibility 	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1OZ	Pr	1.85	Ce	0.15	Cu	1															O	Z		5	2000																												T'																		K				20		0.5	20																																									A			2660				1.62																																															1						Microwave Electrodynamics of Electron-Doped Cuprate Superconductors	10		Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 20742-4111	Phys.Rev.Lett.,85(2000)3696-3699	J. David Kokales,Lucia V. Mercaldo,Patrick Fournier,Richard L. Greene,Steven M. Anlage,Vladimir V. Talanov		
33000	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd1.665Gd0.185Ce0.15Cu1O4	Nd	1.665	Gd	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.938		12.045												K	15.8		21.6	19			19																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33001	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd1.48Gd0.37Ce0.15Cu1O4	Nd	1.48	Gd	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.93		11.995												K	14.9		20.4	18			18																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33002	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd1.295Gd0.555Ce0.15Cu1O4	Nd	1.295	Gd	0.555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.924		11.968												K	12.3		19.1	17			17																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33003	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd1.11Gd0.74Ce0.15Cu1O4	Nd	1.11	Gd	0.74	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.92		11.938												K	11.2		18.1	15			15																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33004	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd0.925Gd0.925Ce0.15Cu1O4	Nd	0.925	Gd	0.925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.915		11.911												K	9.5		16.7	13			13																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33005	PHC2600117		(Nd,Gd,Ce)2CuO4	Nd0.74Gd1.11Ce0.15Cu1O4	Nd	0.74	Gd	1.11	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.911		11.885												K			13.9	12			12																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33006	PHC2600117	not s/c	(Nd,Gd,Ce)2CuO4	Nd0.555Gd1.295Ce0.15Cu1O4	Nd	0.555	Gd	1.295	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.911		11.891												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33007	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm1.7575Gd0.0925Ce0.15Cu1O4	Sm	1.7575	Gd	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.911		11.868												K	14.8		18	15			15																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33008	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm1.665Gd0.185Ce0.15Cu1O4	Sm	1.665	Gd	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.907		11.858												K	12.3		17.3	13			13																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33009	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm1.48Gd0.37Ce0.15Cu1O4	Sm	1.48	Gd	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.906		11.849												K	10.8		15.3	10.5			10.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33010	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm1.295Gd0.555Ce0.15Cu1O4	Sm	1.295	Gd	0.555	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.905		11.843												K			11.9	8.5			8.5																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33011	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm1.11Gd0.74Ce0.15Cu1O4	Sm	1.11	Gd	0.74	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.904		11.837												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33012	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm0.925Gd0.925Ce0.15Cu1O4	Sm	0.925	Gd	0.925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.902		11.831												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33013	PHC2600117		(Sm,Gd,Ce)2CuO4	Sm0.74Gd1.11Ce0.15Cu1O4	Sm	0.74	Gd	1.11	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.903		11.833												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33014	PHC2600117		(Eu,Gd,Ce)2CuO4	Eu1.7575Gd0.0925Ce0.15Cu1O4	Eu	1.7575	Gd	0.0925	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.9		11.819												K			9.1	4.7			4.7																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33015	PHC2600117		(Eu,Gd,Ce)2CuO4	Eu1.665Gd0.185Ce0.15Cu1O4	Eu	1.665	Gd	0.185	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.899		11.811												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33016	PHC2600117		(Eu,Gd,Ce)2CuO4	Eu1.5725Gd0.2775Ce0.15Cu1O4	Eu	1.5725	Gd	0.2775	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.899		11.81												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33017	PHC2600117		(Eu,Gd,Ce)2CuO4	Eu1.48Gd0.37Ce0.15Cu1O4	Eu	1.48	Gd	0.37	Ce	0.15	Cu	1													O	4			1996																												T'			A	3.898		11.809												K																																																																																																							mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33018	PHC2600117		(Eu,Gd,Ce)2CuO4	Eu1.80375Gd0.04625Ce0.15Cu1O4	Eu	1.80375	Gd	0.04625	Ce	0.15	Cu	1													O	4			1996																												T'			A															K			10.2	5.7			5.7																																																																																																mixture-heat(1000C,48h, in air)-air quench to RT - oxygen reduction(850 - 950C, 2h in air)					Ionic-size effect on the structure and Tc of T'-(R1-xR'x)1.85Ce0.15CuO4 (R=Pr,Nd,Sm and Eu;R'=Gd and Y)			Department of Physics, National Sun Yat-Sen University, Kaohsiung 80424,Taiwan	Physica.C,260(1996)117-124	H.C.Ku,H.D.Yang,J.H.Shieh,T.H.Meen,W.H.Lee,W.J.Huang,Y.C.Chen		
33019	PHC3550023		EuBa2Cu3O7	Eu1Ba2Cu3O6.9	Eu	1	Ba	2	Cu	3															O	z	6.9	1	2001																												Y123			A	3.823	3.8922	11.627												K	92		93	94			94																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33020	PHC3550023		(Eu,Pr)Ba2Cu3O7	Eu0.9Pr0.1Ba2Cu3O6.78	Eu	0.9	Pr	0.1	Ba	2	Cu	3													O	z	6.78	1	2001																												Y123			A	3.8447	3.9089	11.5915												K	81		82	83			83																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33021	PHC3550023		(Eu,Pr)Ba2Cu3O7	Eu0.8Pr0.2Ba2Cu3O6.7	Eu	0.8	Pr	0.2	Ba	2	Cu	3													O	z	6.7	1	2001																												Y123			A	3.8702	3.9093	11.5361												K	65		67	65			65																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33022	PHC3550023		(Eu,Pr)Ba2Cu3O7	Eu0.7Pr0.3Ba2Cu3O6.66	Eu	0.7	Pr	0.3	Ba	2	Cu	3													O	z	6.66	1	2001																												Y123			A	3.8521	3.902	11.6118												K	40		60	41			41																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33023	PHC3550023	not s/c	(Eu,Pr)Ba2Cu3O7	Eu0.6Pr0.4Ba2Cu3O6.64	Eu	0.6	Pr	0.4	Ba	2	Cu	3													O	z	6.64	1	2001																												Y123			A	3.8562	3.9056	11.5313												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33024	PHC3550023		Eu(Ba,Pr)2Cu3O7	Eu1Ba1.9Pr0.1Cu3O6.75	Eu	1	Ba	1.9	Pr	0.1	Cu	3													O	z	6.75	1	2001																												Y123			A	3.7914	3.8757	11.6856												K	66		70	73			73																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33025	PHC3550023		Eu(Ba,Pr)2Cu3O7	Eu1Ba1.8Pr0.2Cu3O6.69	Eu	1	Ba	1.8	Pr	0.2	Cu	3													O	z	6.69	1	2001																												Y123			A	3.8165	3.8771	11.7386												K	31		44	46			46																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33026	PHC3550023	R not to zero at 20 K.	Eu(Ba,Pr)2Cu3O7	Eu1Ba1.7Pr0.3Cu3O6.59	Eu	1	Ba	1.7	Pr	0.3	Cu	3													O	z	6.59	1	2001																												Y123			A	3.8025	3.8989	11.8318												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33027	PHC3550023	not s/c	Eu(Ba,Pr)2Cu3O7	Eu1Ba1.6Pr0.4Cu3O6.51	Eu	1	Ba	1.6	Pr	0.4	Cu	3													O	z	6.51	1	2001																												Y123			A	3.8245	3.9082	11.7335												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33028	PHC3550023	not s/c	(Eu,Pr)(Ba,Sr)2Cu3Oz	Eu0.6Pr0.4Ba1.9Sr0.1Cu3O6.84	Eu	0.6	Pr	0.4	Ba	1.9	Sr	0.1	Cu	3											O	z	6.84	1	2001																												Y123			A	3.8174	3.8603	11.7962												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33029	PHC3550023	not s/c	(Eu,Pr)(Ba,Sr)2Cu3Oz	Eu0.6Pr0.4Ba1.8Sr0.2Cu3O6.88	Eu	0.6	Pr	0.4	Ba	1.8	Sr	0.2	Cu	3											O	z	6.88	1	2001																												Y123			A	3.8321	3.9	11.6943												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33030	PHC3550023		(Eu,Pr)(Ba,Sr)2Cu3Oz	Eu0.6Pr0.4Ba1.7Sr0.3Cu3O6.93	Eu	0.6	Pr	0.4	Ba	1.7	Sr	0.3	Cu	3											O	z	6.93	1	2001																												Y123			A	3.8303	3.898	11.6706												K	20		27	28			28																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33031	PHC3550023		(Eu,Pr)(Ba,Sr)2Cu3Oz	Eu0.6Pr0.4Ba1.6Sr0.4Cu3O7	Eu	0.6	Pr	0.4	Ba	1.6	Sr	0.4	Cu	3											O	z	7	1	2001																												Y123			A	3.8483	3.9026	11.6313												K	21		29	29			29																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33032	PHC3550023		(Eu,Pr)(Ba,Sr)2Cu3Oz	Eu0.6Pr0.4Ba1.5Sr0.5Cu3O6.89	Eu	0.6	Pr	0.4	Ba	1.5	Sr	0.5	Cu	3											O	z	6.89	1	2001																												Y123			A	3.8395	3.9084	11.6945												K	21		32	34			34																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33033	PHC3550023	not s/c	Eu(Ba,Pr,Sr)2Cu3O7	Eu1Ba1.6Pr0.3Sr0.1Cu3O6.71	Eu	1	Ba	1.6	Pr	0.3	Sr	0.1	Cu	3											O	z	6.71	1	2001																												Y123			A	3.8271	3.9186	11.7492												K					20																																																																																																	1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33034	PHC3550023		Eu(Ba,Pr,Sr)2Cu3O7	Eu1Ba1.5Pr0.3Sr0.2Cu3O6.81	Eu	1	Ba	1.5	Pr	0.3	Sr	0.2	Cu	3											O	z	6.81	1	2001																												Y123			A	3.8255	3.916	11.6113												K	20		27	28			28																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33035	PHC3550023		Eu(Ba,Pr,Sr)2Cu3O7	Eu1Ba1.4Pr0.3Sr0.3Cu3O6.92	Eu	1	Ba	1.4	Pr	0.3	Sr	0.3	Cu	3											O	z	6.92	1	2001																												Y123			A	3.8116	3.9031	11.707												K	21		30	29			29																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33036	PHC3550023		Eu(Ba,Pr,Sr)2Cu3O7	Eu1Ba1.3Pr0.3Sr0.4Cu3O7	Eu	1	Ba	1.3	Pr	0.3	Sr	0.4	Cu	3											O	z	7	1	2001																												Y123			A	3.8014	3.8981	11.6771												K	21		31	30			30																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33037	PHC3550023		Eu(Ba,Pr,Sr)2Cu3O7	Eu1Ba1.2Pr0.3Sr0.5Cu3O6.89	Eu	1	Ba	1.2	Pr	0.3	Sr	0.5	Cu	3											O	z	6.89	1	2001																												Y123			A	3.8165	3.9068	11.7431												K	21		33	32			32																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33038	PHC3550023	R not to zero at 20 K.	(Eu,Sr)(Ba,Pr)2Cu3O7	Eu0.9Sr0.1Ba1.6Pr0.1Cu3O6.58	Eu	0.9	Sr	0.1	Ba	1.6	Pr	0.1	Cu	3											O	z	6.58	1	2001																												Y123			A	3.8437	3.8828	11.642												K			30	32			32																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33039	PHC3550023		(Eu,Sr)(Ba,Pr)2Cu3O7	Eu0.8Sr0.2Ba1.6Pr0.1Cu3O6.78	Eu	0.8	Sr	0.2	Ba	1.6	Pr	0.1	Cu	3											O	z	6.78	1	2001																												Y123			A	3.8444	3.8753	11.6443												K	24		50	51			51																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33040	PHC3550023		(Eu,Sr)(Ba,Pr)2Cu3O7	Eu0.7Sr0.3Ba1.6Pr0.1Cu3O6.91	Eu	0.7	Sr	0.3	Ba	1.6	Pr	0.1	Cu	3											O	z	6.91	1	2001																												Y123			A	3.8374	3.8657	11.6919												K	28		52	54			54																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33041	PHC3550023		(Eu,Sr)(Ba,Pr)2Cu3O7	Eu0.6Sr0.4Ba1.6Pr0.1Cu3O7.06	Eu	0.6	Sr	0.4	Ba	1.6	Pr	0.1	Cu	3											O	z	7.06	1	2001																												Y123			A	3.8151	3.8919	11.8929												K	27		49	50			50																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33042	PHC3550023		(Eu,Sr)(Ba,Pr)2Cu3O7	Eu0.5Sr0.5Ba1.6Pr0.1Cu3O7.07	Eu	0.5	Sr	0.5	Ba	1.6	Pr	0.1	Cu	3											O	z	7.07	1	2001																												Y123			A	3.8085	3.8925	11.7019												K	20		40	42			42																																																																																															1	mixture-SIN(950C,12h inO2)-ANN(500C,24h in O2 flow)-slow cooling to RT(1C/min)					Effect of Sr-substitution on the restitution of superconductivity in Pr-substituted at rare earth and Ba-site in EuBa2Cu3Oz			Department of Physics, Saurashtra University, University Road, Rajkot 360 005, India	Physica C, 355(2001)23	D.G.Kuberkar,Krushna Mavani,M.R.Gonal,R.G.Kulkarni,R.Prasad,R.S.Thampi,S.Rayaprol		
33043	PHC3550267	Jc(5K,5T)=61500 A/cm2. Jc(50K,5T)=1200 A/cm2	CuBa2YCu2O7	Y1Ba2Cu3O6.91	Y	1	Ba	2	Cu	3															O	z	6.91		2001																												Y123																		K	93			93			93																																																																																																SIN(930C,80h)-cool to RT (100C/h) as-prepared.					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33044	PHC3550267	impurity phase=Y2BaCuO5,BaCuO2,CaO. Total impurity phase less than 2%. Tirr(1T)=77 K. Tirr(5T)=42 K.	(Cu,Re)Ba2YCu2O7	Y1Re0.05Ba2Cu2.95O6.94	Y	1	Re	0.05	Ba	2	Cu	2.95													O	z	6.94	1	2001																												Cu1212																		K	86			88			88																																																																																																SIN(930C,80h)-cool to RT (100C/h) as-prepared.					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33045	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.1Ba2Cu2.9O7	Y	1	Re	0.1	Ba	2	Cu	2.9													O	z	7		2001																												Cu1212																		K	70.5			91.5			91.5																																																																																																SIN(930C,80h)-cool to RT (100C/h) as-prepared.					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33046	PHC3550267	impurity phase = YBa2ReO6	(Cu,Re)Ba2YCu2O7	Y1Re0.15Ba2Cu2.85O7.07	Y	1	Re	0.15	Ba	2	Cu	2.85													O	z	7.07		2001																												Cu1212																		K	60			91.5			91.5																																																																																																SIN(930C,80h)-cool to RT (100C/h) as-prepared.					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33047	PHC3550267		CuBa2YCu2O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	z	6.96		2001																												Y123																		K	92.5			92			92																																																																																																(as-grown)-heat(880C,2h in flowing O2)-cool to 480C(30C/h)-ANN(480C,50-100h)-RT					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33048	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.05Ba2Cu2.95O7.02	Y	1	Re	0.05	Ba	2	Cu	2.95													O	z	7.02		2001																												Cu1212																		K	93			92			92																																																																																																(as-grown)-heat(880C,2h in flowing O2)-cool to 480C(30C/h)-ANN(480C,50-100h)-RT					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33049	PHC3550267	Jc(5K,5T)=23300 A/cm2. Jc(50K,5T)=68 A/cm2. Tirr(1T)=77 K. Tirr(5T)=41 K.	(Cu,Re)Ba2YCu2O7	Y1Re0.1Ba2Cu2.9O7.08	Y	1	Re	0.1	Ba	2	Cu	2.9													O	z	7.08		2001																												Cu1212			A	3.8419	3.8765	11.6913												K	89			90			90																																																																																																(as-grown)-heat(880C,2h in flowing O2)-cool to 480C(30C/h)-ANN(480C,50-100h)-RT					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33050	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.15Ba2Cu2.85O7.13	Y	1	Re	0.15	Ba	2	Cu	2.85													O	z	7.13		2001																												Cu1212																		K	85			90			90																																																																																																(as-grown)-heat(880C,2h in flowing O2)-cool to 480C(30C/h)-ANN(480C,50-100h)-RT					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33051	PHC3550267		CuBa2YCu2O7	Y1Ba2Cu3O6.96	Y	1	Ba	2	Cu	3															O	z	6.96		2001																												Y123																		K	91			92			92																																																																																																(as-grown sample+KClO3)-(sealed quartz tube)-heat(480C,12h)-cool to RT(100C/h)					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33052	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.05Ba2Cu2.95O7.04	Y	1	Re	0.05	Ba	2	Cu	2.95													O	z	7.04		2001																												Cu1212																		K	92.5			92			92																																																																																																(as-grown sample+KClO3)-(sealed quartz tube)-heat(480C,12h)-cool to RT(100C/h)					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33053	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.1Ba2Cu2.9O7.09	Y	1	Re	0.1	Ba	2	Cu	2.9													O	z	7.09		2001																												Cu1212																		K	91			91			91																																																																																																(as-grown sample+KClO3)-(sealed quartz tube)-heat(480C,12h)-cool to RT(100C/h)					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33054	PHC3550267		(Cu,Re)Ba2YCu2O7	Y1Re0.15Ba2Cu2.85O7.17	Y	1	Re	0.15	Ba	2	Cu	2.85													O	z	7.17		2001																												Cu1212																		K	85			91			91																																																																																																(as-grown sample+KClO3)-(sealed quartz tube)-heat(480C,12h)-cool to RT(100C/h)					Effects of Re substitution on the structure and superconductivity of Cu1-xRexBa2YCu2Ow			Istituto Materiali Speciali per Elettronica e Magnetismo del Consiglio Nazionale delle Ricerche, Parco Area delle Scienze 37A, Fontanini-Parma, Italy	Physica C, 355(2001)267	A.Gauzzi,A.Santoro,C.Bougerol-Chaillout,F.Licci,M.Marezio,P.Bordet,Q.Huang,R.Masini		
33055	PHC3560012		(K,La)BiO3	K0.9La0.1Bi1O3	K	0.9	La	0.1	Bi	1															O	3			2001																												BKBO			A	4.2121														K				5.74			5.74																																																																																														KO2,La2O3,Bi2O3,CaO,Ca6Bi6O15		mixture-Au capsule-press(5-6 Gpa)-heat(800-1100C,7min)-hold 1h-cool to RT					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33056	PHC3560012		(K,La)BiO3	K0.85La0.15Bi1O3	K	0.85	La	0.15	Bi	1															O	3			2001																												BKBO			A	4.2133														K				10.25			10.25																																																																																														KO2,La2O3,Bi2O3,CaO,Ca6Bi6O15		mixture-Au capsule-press(5-6 Gpa)-heat(800-1100C,7min)-hold 1h-cool to RT					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33057	PHC3560012		(K,La)BiO3	K0.8La0.2Bi1O3	K	0.8	La	0.2	Bi	1															O	3			2001																												BKBO			A	4.2155														K				12.2			12.2																																																																																														KO2,La2O3,Bi2O3,CaO,Ca6Bi6O15		mixture-Au capsule-press(5-6 Gpa)-heat(800-1100C,7min)-hold 1h-cool to RT					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33058	PHC3560012		(K,La)BiO3	K0.75La0.25Bi1O3	K	0.75	La	0.25	Bi	1															O	3			2001																												BKBO			A	4.2167														K				12.2			12.2																																																																																														KO2,La2O3,Bi2O3,CaO,Ca6Bi6O15		mixture-Au capsule-press(5-6 Gpa)-heat(800-1100C,7min)-hold 1h-cool to RT					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33059	PHC3560012		(K,Bi)BiO3	K0.95Bi1.05O3	K	0.95	Bi	1.05																	O	3			2001																												BKBO			A	4.2201														K				6			6																																																																																																synthesized at 900C, p=5GPa					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33060	PHC3560012		(K,Bi)BiO3	K0.9Bi1.1O3	K	0.9	Bi	1.1																	O	3			2001																												BKBO			A	4.2225														K				6.5			6.5	TC33060																																																																																															synthesized at 900C, p=5GPa					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33061	PHC3560012		(K,Bi)BiO3	K0.85Bi1.15O3	K	0.85	Bi	1.15																	O	3			2001																												BKBO			A	4.2245														K				7.4			7.4																																																																																																synthesized at 900C, p=5GPa					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33062	PHC3560012		(K,Bi)BiO3	K0.8Bi1.2O3	K	0.8	Bi	1.2																	O	3			2001																												BKBO			A	4.228														K				8.7			8.7																																																																																																synthesized at 900C, p=5GPa					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33063	PHC3560012	0.1<x<0.3 samples for  nominal values were prepared. Tc(onset) for all samples = 8.7 K	(K,Ca)BiO3	K0.75Ca0.25Bi1O3	K	0.75	Ca	0.25	Bi	1															O	3			2001																												BKBO			A	4.1893														K	7		8	8.7			8.7																																																																																																synthesized at 1000C, p=5GPa					Extended range of superconducting bismuthates K1-xAxBiO3 (A=La, Bi, and Ca)			SRL, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)12	A.Yamamoto,K.Yoshida,N.R.Khasanova,S.Tajima		
33064	PHC3050275	very small s/c volume fraction	RbBiOz	Rb1Bi1O3	Rb	1	Bi	1																	O	3			1998																												BKBO			A	4.2941														K				11			11										1																																																																																				Rb20, Bi2O3		high-pressure synthesis (5GPa,100C, 1h). oxydized using KCl4.					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33065	PHC3050275	very small s/c volume fraction	(Rb,Bi)BiO3	Rb0.9Bi1.1O3	Rb	0.9	Bi	1.1																	O	3			1998																												BKBO			A	4.2948														K				11			11										1.5																																																																																				Rb20, Bi2O3		high-pressure synthesis (5GPa,100C, 1h). oxydized using KCl4.					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33066	PHC3050275	very small s/c volume fraction	(Rb,Bi)BiO3	Rb0.7Bi1.3O3	Rb	0.7	Bi	1.3																	O	3			1998																												BKBO			A	4.2968														K				11			11										1																																																																																				Rb20, Bi2O3		high-pressure synthesis (5GPa,100C, 1h). oxydized using KCl4.					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33067	PHC3050275	very small s/c volume fraction	(Rb,Bi)BiO3	Rb0.6Bi1.4O3	Rb	0.6	Bi	1.4																	O	3			1998																												BKBO			A	4.2973														K				11			11										1																																																																																				Rb20, Bi2O3		high-pressure synthesis (5GPa,100C, 1h). oxydized using KCl4.					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33068	PHC3050275		KBiO3	K1Bi1O3	K	1	Bi	1																	O	3			1998																												BKBO			A	4.2287														K				10.2			10.2										40																																																																																				KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33069	PHC3050275		(K,Bi)BiO3	K0.95Bi1.05O3	K	0.95	Bi	1.05																	O	3			1998																												BKBO			A	4.2294														K				10.2			10.2										50																																																																																				KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33070	PHC3050275		(K,Bi)BiO3	K0.9Bi1.1O3	K	0.9	Bi	1.1																	O	3			1998																												BKBO			A	4.232														K				10.2			10.2										60																																																																																				KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33071	PHC3050275		(K,Bi)BiO3	K0.8Bi1.2O3	K	0.8	Bi	1.2																	O	3			1998																												BKBO			A	4.2332														K				10.2			10.2										4																																																																																				KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33072	PHC3050275		(K,Bi)BiO3	K0.7Bi1.3O3	K	0.7	Bi	1.3																	O	3			1998																												BKBO			A	4.2377														K																																																																																																					KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33073	PHC3050275		(K,Bi)BiO3	K1.1Bi1O3	K	1.1	Bi	1																	O	3			1998																												BKBO			A	4.2269														K				8.8			8.8										35																																																																																				KO2,Bi2O3		mixture-press-pellet-Au capsule-high pressure synthesis (5GPa,100C,1h)-RT					Superconductivity at 10.2 K in the K-Bi-O system			Superconductivity Research Laboratory, ISTEC, 10-13, Shinonome 1-Chome, Koto-ku, Tokyo 135-006, Japan	Physica C, 305(1998)275	A.Yamamoto,K.Tanabe,N.R.Khasanova,S.Tajima,X.-J.Wu		
33074	PHC3560115	Overdoped sample. Hirr defined as H where R=0.	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6			2001																												Tl2201			A															K			37			4	37																																		HIR33074																																																														contamination controlled flux method					Irreversibility line and lock-in transition in Tl2Ba2CuO6 single crystals			Cryogenics and Superconductivity Division, National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	Physica C, 356(2001)115	C.Terakura,D.G.Hinks,G.S.Okram,H.Aoki,M.Xu,S.Uji		
33075	PHC3560141		HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	2001																												Hg1201			A	3.879		9.532												K				98			98																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33076	PHC3560141	dTc/dx=-4 K/at%Mg	HgBa2(Cu,Mg)O4	Hg1Ba2Cu0.99Mg0.01O4+z	Hg	1	Ba	2	Cu	0.99	Mg	0.01													O	4+z		1	2001																												Hg1201			A	3.881		9.535												K				94			94																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33077	PHC3560141	dTc/dx=-4 K/at%Mg	HgBa2(Cu,Mg)O4	Hg1Ba2Cu0.98Mg0.02O4+z	Hg	1	Ba	2	Cu	0.98	Mg	0.02													O	4+z		1	2001																												Hg1201			A	3.883		9.534												K				89			89																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33078	PHC3560141	dTc/dx=-4 K/at%Mg	HgBa2(Cu,Mg)O4	Hg1Ba2Cu0.97Mg0.03O4+z	Hg	1	Ba	2	Cu	0.97	Mg	0.03													O	4+z		1	2001																												Hg1201			A	3.884		9.532												K				85			85																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33079	PHC3560141	dTc/dx=-7 K/at%Zn	HgBa2(Cu,Zn)O4	Hg1Ba2Cu0.99Zn0.01O4+z	Hg	1	Ba	2	Cu	0.99	Zn	0.01													O	4+z		1	2001																												Hg1201			A	3.882		9.532												K				89			89																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33080	PHC3560141	dTc/dx=-7 K/at%Zn	HgBa2(Cu,Zn)O4	Hg1Ba2Cu0.98Zn0.02O4+z	Hg	1	Ba	2	Cu	0.98	Zn	0.02													O	4+z		1	2001																												Hg1201			A	3.882		9.536												K				85			85																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33081	PHC3560141	dTc/dx=-7 K/at%Zn	HgBa2(Cu,Zn)O4	Hg1Ba2Cu0.97Zn0.03O4+z	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z		1	2001																												Hg1201			A	3.884		9.534												K				78			78																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33082	PHC3560141		HgBa2(Cu,Fe)O4	Hg1Ba2Cu0.99Fe0.01O4+z	Hg	1	Ba	2	Cu	0.99	Fe	0.01													O	4+z		1	2001																												Hg1201			A	3.879		9.519												K				96			96																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33083	PHC3560141		HgBa2(Cu,Fe)O4	Hg1Ba2Cu0.98Fe0.02O4+z	Hg	1	Ba	2	Cu	0.98	Fe	0.02													O	4+z		1	2001																												Hg1201			A	3.876		9.515												K				96			96																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33084	PHC3560141		HgBa2(Cu,Fe)O4	Hg1Ba2Cu0.97Fe0.03O4+z	Hg	1	Ba	2	Cu	0.97	Fe	0.03													O	4+z		1	2001																												Hg1201			A	3.875		9.504												K				95			95																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33085	PHC3560141		HgBa2(Cu,Co)O4	Hg1Ba2Cu0.99Co0.01O4+z	Hg	1	Ba	2	Cu	0.99	Co	0.01													O	4+z		1	2001																												Hg1201			A	3.88		9.526												K				96			96																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33086	PHC3560141		HgBa2(Cu,Co)O4	Hg1Ba2Cu0.98Co0.02O4+z	Hg	1	Ba	2	Cu	0.98	Co	0.02													O	4+z		1	2001																												Hg1201			A	3.879		9.521												K				96			96																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33087	PHC3560141		HgBa2(Cu,Co)O4	Hg1Ba2Cu0.97Co0.03O4+z	Hg	1	Ba	2	Cu	0.97	Co	0.03													O	4+z		1	2001																												Hg1201			A	3.877		9.508												K				94			94																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33088	PHC3560141		HgBa2(Cu,Ni)O4	Hg1Ba2Cu0.99Ni0.01O4+z	Hg	1	Ba	2	Cu	0.99	Ni	0.01													O	4+z			2001																												Hg1201			A	3.88		9.525												K				96			96																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33089	PHC3560141		HgBa2(Cu,Ni)O4	Hg1Ba2Cu0.98Ni0.02O4+z	Hg	1	Ba	2	Cu	0.98	Ni	0.02													O	4+z			2001																												Hg1201			A	3.88		9.524												K				94			94																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33090	PHC3560141	impurity phase = Ni3Ba3O8	HgBa2(Cu,Ni)O4	Hg1Ba2Cu0.97Ni0.03O4+z	Hg	1	Ba	2	Cu	0.97	Ni	0.03													O	4+z			2001																												Hg1201			A	3.879		9.526												K				95			95																																																																																														HgO,BaO,CuO,MgO(ZnO,Fe2O3,CoO,NiO)		mixture-pellet-sealed in an evacuated quartz tube-heat(750C,20h) - Q to water.  ANN(340C,72h, in O2)					Effects of metal substitution on superconductivity and crystal structure of HgBa2CuO4+z			Superconductivity Research Laboratory, International Superconductivity Technology Center (ISTEC), 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Physica C, 356(2001)141	A.Yamamoto,M.Izumi,S.Tajima,W.-Z.Hu		
33091	P064172514		Bi2(Sr,La)2CuO6	Bi2Sr1.5La0.5Cu1O6+z	Bi	2	Sr	1.5	La	0.5	Cu	1													O	6+z		3	2001																												Bi2201																		K		30.8					30.8																																																																																											RH33091					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33092	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.5La0.5Cu0.995Zn0.005O6+z	Bi	2	Sr	1.5	La	0.5	Cu	0.995	Zn	0.005											O	6+z		3	2001																												Bi2201																		K		22.6					22.6																																																																																											RH33092					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33093	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.5La0.5Cu0.991Zn0.009O6+z	Bi	2	Sr	1.5	La	0.5	Cu	0.991	Zn	0.009											O	6+z		3	2001																												Bi2201																		K		17.9					17.9																																																																																											RH33093					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33094	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.5La0.5Cu0.984Zn0.016O6+z	Bi	2	Sr	1.5	La	0.5	Cu	0.984	Zn	0.016											O	6+z		3	2001																												Bi2201																		K		10.4					10.4																																																																																											RH33094					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33095	P064172514		Bi2(Sr,La)2CuO6	Bi2Sr1.34La0.66Cu1O6+z	Bi	2	Sr	1.34	La	0.66	Cu	1													O	6+z		3	2001																												Bi2201																		K		20.3					20.3																																																																																											RH33095					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33096	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.34La0.66Cu0.995Zn0.005O6+z	Bi	2	Sr	1.34	La	0.66	Cu	0.995	Zn	0.005											O	6+z		3	2001																												Bi2201																		K		11.4					11.4																																																																																											RH33096					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33097	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.34La0.66Cu0.99Zn0.01O6+z	Bi	2	Sr	1.34	La	0.66	Cu	0.99	Zn	0.01											O	6+z		3	2001																												Bi2201																		K		8					8																																																																																											RH33097					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33098	P064172514		Bi2(Sr,La)2(Cu,Zn)O6	Bi2Sr1.34La0.66Cu0.978Zn0.022O6+z	Bi	2	Sr	1.34	La	0.66	Cu	0.978	Zn	0.022											O	6+z		3	2001																												Bi2201																		K					0.5																																																																																													RH33098					crystals grown by a floating zone method. ANN(650C,48h) - Q to RT					Zn-doping effect on the magnetotransport properties of Bi2Sr2-xLaxCuO6+z  single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 64(2001)172514	J.Takeya,S.Ono,Y.Ando,Y.Hanaki		
33099	PHC3630025		(Sm,La,Sr)2CuO4	Sm1La0.8Sr0.2Cu1O4	Sm	1	La	0.8	Sr	0.2	Cu	1													O	4		3	2001																											2	T*	P4/nmm		A	3.871		12.597												K				24			24																																																																																														Sm2O3,La2O3,SrCO3,Cu		TSFZ method using CuO-rich solvent. ANN(600C,7days and 300C,3days) - slow cool to RT(25C/h)					Single crystal growth of T*-phase SmLa0.8Sr0.2CuO4			Van der Waals-Zeeman Instituut, Universiteit van Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Physica C, 363(2001)25	A.A.Menovsky,A.A.Nugroho,H.Gelders,I.M.Sutjahja,J.J.M.Franse,M.Diantoro,M.O.Tjia		
33100	PHC3630243	highly twinned. Tc=86.5 K from thermopower.	YBa2Cu3O7	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	6.95	6.95	3	2001																												Y123																		K		92			0.5		92																																																																	THC33100					TP33100																										self-flux technique using TiO2 stabilized Y2O3 crucible. (1040C,24h) - cool to 960C(1C/h) - ANN(525C in O2) - cool to 250C(2C/h) - to RT(60C/h)					Thermal conductivity and thermoelectric power of high-quality YBa2Cu3O7-z crystals			Advanced Electronic Materials Group, School of Physics, University of New South Wales, Sydney, NSW 2052, Australia	Physica C, 363(2001)243	G.A.Shams,G.J.Russell,J.W.Cochrane		
33101	PHC3630080	not s/c	YBa2Cu3Oz	Y1Ba2Cu3O6.12	Y	1	Ba	2	Cu	3															O	6+z	6.12		2001																											2	Y123			A	3.8589		11.8199												K					4.2																																																																																																		oxygen controll, ANN(730C,24h, in Ar)					The effect of calcium substitution in deoxygenated R1xCaxBa2Cu3O6.1 systems (R=Y, Eu): appearance of superconductivity, insulator to metal transition			Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C, 363(2001)80	A.Szytula,J.Sokolowski,M.Balanda,P.Starowicz		
33102	PHC3630080	not s/c	(Y,Ca)Ba2Cu3Oz	Y0.8Ca0.2Ba2Cu3O6.12	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	6+z	6.12		2001																											2	Y123			A	3.856		11.8272												K					4.2																																																																																																		oxygen controll, ANN(730C,24h, in Ar)					The effect of calcium substitution in deoxygenated R1xCaxBa2Cu3O6.1 systems (R=Y, Eu): appearance of superconductivity, insulator to metal transition			Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C, 363(2001)80	A.Szytula,J.Sokolowski,M.Balanda,P.Starowicz		
33103	PHC3630080	s/c volume fraction is small.	(Y,Ca)Ba2Cu3Oz	Y0.7Ca0.3Ba2Cu3O6.12	Y	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.12		2001																											2	Y123			A	3.8541		11.8233												K				35			35																																																																																																oxygen controll, ANN(730C,24h, in Ar)					The effect of calcium substitution in deoxygenated R1xCaxBa2Cu3O6.1 systems (R=Y, Eu): appearance of superconductivity, insulator to metal transition			Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C, 363(2001)80	A.Szytula,J.Sokolowski,M.Balanda,P.Starowicz		
33104	PHC3630080	s/c volume fraction is small.	(Eu,Ca)Ba2Cu3Oz	Eu0.7Ca0.3Ba2Cu3O6.13	Eu	0.7	Ca	0.3	Ba	2	Cu	3													O	6+z	6.13		2001																											2	Y123			A	3.8751		11.8006												K				26			26																																																																																																oxygen controll, ANN(600C,10h, in flowing Ar)					The effect of calcium substitution in deoxygenated R1xCaxBa2Cu3O6.1 systems (R=Y, Eu): appearance of superconductivity, insulator to metal transition			Institute of Physics, Jagiellonian University, Reymonta 4, 30-059 Krakow, Poland	Physica C, 363(2001)80	A.Szytula,J.Sokolowski,M.Balanda,P.Starowicz		
33105	PHC3610040	as-grown. orthorhombicity=4.87 E-3. Tc=91.5 K from field cooling measurement.	LaBa2Cu3O7	La1Ba2Cu3O7-z	La	1	Ba	2	Cu	3															O	7-z		1	2001																											3	Y123			A	3.8922	3.9303	11.8104												K				93			93																																																																																																sol-gel method					Preparation by sol-gel, structure and superconductivity of pure and fluorinated LaBa2Cu3O7-d			Laboratoire de Physico-Chimie de l'Etat Solide, CNRS UMR 8648, B?t. 414, Universit? Paris-Sud, 91405 Orsay, France	Physica C, 361(2001)40	H.Selig,L.Ben-Dor,R.Nagarajan,R.Suryanarayanan		
33106	PHC3610040	fluorinated sample. F-content not shown. orthorhombicity=5.0 E-3. Tc=91.5 K from field cooling measurement.	LaBa2Cu3(O,F)7	La1Ba2Cu3O7-z	La	1	Ba	2	Cu	3															O	7-z		1	2001																											3	Y123			A	3.8892	3.9264	11.8051												K				93			93																																																																																																fluorination by using ClF3, (250 Torr, 220C,2h)					Preparation by sol-gel, structure and superconductivity of pure and fluorinated LaBa2Cu3O7-d			Laboratoire de Physico-Chimie de l'Etat Solide, CNRS UMR 8648, B?t. 414, Universit? Paris-Sud, 91405 Orsay, France	Physica C, 361(2001)40	H.Selig,L.Ben-Dor,R.Nagarajan,R.Suryanarayanan		
33107	PHC3630251	two step transition: intra-grain and inter-grain s/c transition. s/c properties depend on synthesis condition.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2001																												Ru1212																		K		30					30																																																																						TP33107																									1	CAL(960C,16h) - SIN(1060C,10h)					Synthesis, characterization and physical properties of the superconducting ferromagnet RuSr2GdCu2O8			Department of Physics, Texas Center for Superconductivity, University of Houston, Houston, TX 77204-5932, USA	Physica C, 363(2001)251	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.S.Wang,Y.Y.Xue		
33108	PHC2630286		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		1	1996																												Bi2212																		K		88.5					88.5																																																																																															1	CAL(800-820C in air)-SIN(865-880C, 15h)-FC-ANN(500C, in vac)					Electonic states and superconducting properties of Bi2Sr2(Ca,Gd)Cu2Oy studied by X-ray photoelectron and inverse-photoemission spectroscopy			Research Institute of Electronics, Shizuoka University, Hamamatsu, Japan	Physica C, 263(1996)286	M.Nagoshi,M.Shimomura,M.Tachiki,N.Sanada,T.Nakadaira,Y.Fukuda,Y.Suzuki,Y.Syono		
33109	PHC2630286		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.9Gd0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Gd	0.1	Cu	2											O	8+z		1	1996																												Bi2212																		K		90.9					90.9																																																																																															1	CAL(800-820C in air)-SIN(865-880C, 15h)-FC-ANN(500C, in vac)					Electonic states and superconducting properties of Bi2Sr2(Ca,Gd)Cu2Oy studied by X-ray photoelectron and inverse-photoemission spectroscopy			Research Institute of Electronics, Shizuoka University, Hamamatsu, Japan	Physica C, 263(1996)286	M.Nagoshi,M.Shimomura,M.Tachiki,N.Sanada,T.Nakadaira,Y.Fukuda,Y.Suzuki,Y.Syono		
33110	PHC2630286		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8+z		1	1996																												Bi2212																		K		86.1					86.1																																																																																															1	CAL(800-820C in air)-SIN(865-880C, 15h)-FC-ANN(500C, in vac)					Electonic states and superconducting properties of Bi2Sr2(Ca,Gd)Cu2Oy studied by X-ray photoelectron and inverse-photoemission spectroscopy			Research Institute of Electronics, Shizuoka University, Hamamatsu, Japan	Physica C, 263(1996)286	M.Nagoshi,M.Shimomura,M.Tachiki,N.Sanada,T.Nakadaira,Y.Fukuda,Y.Suzuki,Y.Syono		
33111	PR0435444		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			1991																												Bi2212																		K		81.1					81.1																																																																																															1	SIN(860-910C)-ANN(650C, in N2 gas)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33112	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.9Gd0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Gd	0.1	Cu	2											O	8+z			1991																												Bi2212																		K		61.5					61.5																																																																																															1	SIN(860-910C)-ANN(650C, in N2 gas)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33113	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8+z			1991																												Bi2212																		K		47					47																																																																																															1	SIN(860-910C)-ANN(650C, in N2 gas)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33114	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.7Gd0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Gd	0.3	Cu	2											O	8+z			1991																												Bi2212																		K		31.1					31.1																																																																																															1	SIN(860-910C)-ANN(650C, in N2 gas)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33115	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.6Gd0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	2											O	8+z			1991																												Bi2212																		K		13.3					13.3																																																																																															1	SIN(860-910C)-ANN(650C, in N2 gas)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33116	PR0435444		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			1991																												Bi2212																		K		72.6					72.6																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33117	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.9Gd0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Gd	0.1	Cu	2											O	8+z			1991																												Bi2212																		K		73.3					73.3																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33118	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.8Gd0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Gd	0.2	Cu	2											O	8+z			1991																												Bi2212																		K		73					73																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33119	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.7Gd0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Gd	0.3	Cu	2											O	8+z			1991																												Bi2212																		K		71.5					71.5																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33120	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.6Gd0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Gd	0.4	Cu	2											O	8+z			1991																												Bi2212																		K		61.1					61.1																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33121	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.55Gd0.45Cu2O8+z	Bi	2	Sr	2	Ca	0.55	Gd	0.45	Cu	2											O	8+z			1991																												Bi2212																		K		50.4					50.4																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33122	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.5Gd0.5Cu2O8+z	Bi	2	Sr	2	Ca	0.5	Gd	0.5	Cu	2											O	8+z			1991																												Bi2212																		K		34					34																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33123	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.45Gd0.55Cu2O8+z	Bi	2	Sr	2	Ca	0.45	Gd	0.55	Cu	2											O	8+z			1991																												Bi2212																		K		24					24																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33124	PR0435444		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.4Gd0.6Cu2O8+z	Bi	2	Sr	2	Ca	0.4	Gd	0.6	Cu	2											O	8+z			1991																												Bi2212																		K		4.8					4.8																																																																																																ANN(in air)					LOCALIZATION AND INTERACATION EFFECTS DURING SUPERCONDUCTOR-INSULATOR TRASITION OF BI2SR2CA1-XGDXCU2O8+D	199103		DEPARTMENT OF PHYSICS,UNIVERSITY OF NEBRASKA AT OMAHA,OMAHA,NEBRASKA 681820266	PHYS.REV.B,43(1991)5444	B.JAYARAM,M.T.WELLER,P.C.LANCHESTER	BI,SR,CA,GD,CU,O	
33125	APL0783097	Untwinned single crystal.H//c-axis. proton beam//c-axis. Jc(H) and Jc(T) are measured for various proton doses. 	YBa2Cu3Oz	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z		3	2001																												Y123																		K				92.87		0.4	92.87																																																				JC33125																																												self-flux method					Effects of successive proton irradiation on the peak effect in YBa2Cu3O7-d single crystals			Department of Physics, Western Michigan University, Kalamazoo, Michigan 49008	Appl.Phys.Lett., 78(2001)3097	A.M.Petrean,G.W.Crabtree,J.W.Snyder,L.M.Paulius,R.J.Olsson,S.Ferguson,V.Tobos,W.-K.Kwok		
33127	PHC3510301	P-induced SC. sample described as (Ca2Cu2O3)(CuO2)1.4276. s/c volume fraction is a few percent. Tc in figure defined as Tc(onset). The other phase c=2.7346A.	Ca14Cu24O41-z	Ca14Cu24O40.93	Ca	14	Cu	24																	O	41-z	40.93	2	2001																												LAD			A	11.238	12.379	3.904												K			8		0		8	TC33127																																																																																															heat(1170-1185C,20-40h, under p(O2)=500 bar)					CaO-CuO system at high oxygen pressure: bulk synthesis and transport properties of Ca14Cu24O41				Physica C, 351(2001)301	C.Bougerol-Chaillout,G.I.Meijer,J.Karpinski,M.Nunez-Regueiro,S.M.Kazakov		
33128	APL0782539	single domain with fine particles of (Sm,Eu)2BaCuO5(211-phase).	(Sm,Eu)Ba2Cu3O7	Sm0.5Eu0.5Ba2Cu3O7-z	Sm	0.5	Eu	0.5	Ba	2	Cu	3													O	7-z		1	2001																												Y123																		K				95			95																																																																																																melt-textured process. cooling rates of box and furnace = 1.4 C/h and 0.5 C/h. final annealing (300C, 200h, in flowing O2)					Growth of single-domain (Sm0.5Eu0.5)Ba2Cu3O7-d with high Tc and Jc by employing a thermal gradient			Superconductivity Research Laboratory, ISTEC, 1-16-25, Shibaura, Minato-ku, Tokyo 105 Japan	Appl.Phys.Lett., 78(2001)2539	A.Hu,M.Murakami,N.Sakai		
33129	SST0140429		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			2001																												Y123																		K				91.26			91.26																																																			41450																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33130	SST0140429		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.97Mn0.03O7-z	Y	1	Ba	2	Cu	2.97	Mn	0.03													O	7-z			2001																												Y123																		K				91.47			91.47																																																			26020																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33131	SST0140429		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.955Mn0.045O7-z	Y	1	Ba	2	Cu	2.955	Mn	0.045													O	7-z			2001																												Y123																		K				91.24			91.24																																																			26020																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33132	SST0140429		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.94Mn0.06O7-z	Y	1	Ba	2	Cu	2.94	Mn	0.06													O	7-z			2001																												Y123																		K				91.01			91.01																																																			27300																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33133	SST0140429		YBa2(Cu,Mn)3O7	Y1Ba2Cu2.925Mn0.075O7-z	Y	1	Ba	2	Cu	2.925	Mn	0.075													O	7-z			2001																												Y123																		K				90.75			90.75																																																			17800																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33134	SST0140429	impurity phases (BamMn2O8) less than 5 %.	YBa2(Cu,Mn)3O7	Y1Ba2Cu2.895Mn0.105O7-z	Y	1	Ba	2	Cu	2.895	Mn	0.105													O	7-z			2001																												Y123																		K				90.53			90.53																																																			20650																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33135	SST0140429	impurity phases (BamMn2O8) less than 5 %.	YBa2(Cu,Mn)3O7	Y1Ba2Cu2.85Mn0.15O7-z	Y	1	Ba	2	Cu	2.85	Mn	0.15													O	7-z			2001																												Y123																		K				89.37			89.37																																																			16250																																													pellet-SIN(930C, 36h)-FC-ANN(450C, 60h, in O2)					Dc magnetic properties of Mn doped YBa2Cu3O7-d superconductor				Supercond.Sci.Technol., 14(2001)429	E.I.Samuel,N.H.Kumar,S.K.Malik,V.S.Bai		
33136	SST0140398	15 K phase in La2CuO4.12. volume fraction = 36.9%	La2CuO4+z	La2Cu1O4+z	La	2	Cu	1																	O	4+z			2001																												T	Fmmm		A	5.3508	5.3864	13.2053												K				15			15																																																																																																solid state reaction. oxydation by using KMnO4.					Superconducting phases, charge ordering and possible correlation between them in La2CuO4.12				Supercond.Sci.Technol., 14(2001)398	C.Dong,F.Wu,G.C.Che,G.D.Liu,H.Chen,L.-M.Peng,L.Chen,M.Gao,Y.M.Ni,Z.X.Zhao		
33137	SST0140398	41 K phase in La2CuO4.12. volume fraction = 63.1%	La2CuO4+z	La2Cu1O4+z	La	2	Cu	1																	O	4+z			2001																												T	Fmmm		A	5.3324	5.426	13.2304												K				41			41																																																																																																solid state reaction. oxydation by using KMnO4.					Superconducting phases, charge ordering and possible correlation between them in La2CuO4.12				Supercond.Sci.Technol., 14(2001)398	C.Dong,F.Wu,G.C.Che,G.D.Liu,H.Chen,L.-M.Peng,L.Chen,M.Gao,Y.M.Ni,Z.X.Zhao		
33138	SUP0140437		(Hg,Mo)Sr2CuO4	Hg0.85Mo0.15Sr2Cu1O4	Hg	0.85	Mo	0.15	Sr	2	Cu	1													O	4		1	2001																												Hg1201			A	3.775		8.848												K				66			66																																																																																																solid state reaction. 					Susceptibility and X-ray absorption measurements on superconducting (Hg,Mo)Sr2CuO4+d system				J.Supercond., 14(2001) 437	B.D.Padalia,I.K.Gopalakrishnan,J.V.Yakhmi,O.Prakash,P.Selvam,S.Balamurugan,S.Gupta		
33139	SUP0140437		(Hg,Mo)Sr2CuO4	Hg0.75Mo0.25Sr2Cu1O4	Hg	0.75	Mo	0.25	Sr	2	Cu	1													O	4		1	2001																												Hg1201			A	3.791		8.818												K				50			50																																																																																																solid state reaction. 					Susceptibility and X-ray absorption measurements on superconducting (Hg,Mo)Sr2CuO4+d system				J.Supercond., 14(2001) 437	B.D.Padalia,I.K.Gopalakrishnan,J.V.Yakhmi,O.Prakash,P.Selvam,S.Balamurugan,S.Gupta		
33140	SUP0140437		(Hg,Mo)Sr2CuO4	Hg0.7Mo0.3Sr2Cu1O4	Hg	0.7	Mo	0.3	Sr	2	Cu	1													O	4		1	2001																												Hg1201			A	3.805		8.814												K				36			36																																																																																																solid state reaction. 					Susceptibility and X-ray absorption measurements on superconducting (Hg,Mo)Sr2CuO4+d system				J.Supercond., 14(2001) 437	B.D.Padalia,I.K.Gopalakrishnan,J.V.Yakhmi,O.Prakash,P.Selvam,S.Balamurugan,S.Gupta		
33141	SUP0140429	annealed in O2 + Ar gas.	(Hg,Cr)Sr2CuO4	Hg0.64Cr0.36Sr2Cu1O4+z	Hg	0.64	Cr	0.36	Sr	2	Cu	1													O	4+z		1	2001																												Hg1201			A	3.843		8.714												K	52		58				55																																																																																																nominal (Hg0.7Cr0.3Sr2CuO4+z). precursor(Sr2CuO3) + Cr2O3 - react(940C,24h, in O2).  Cr0.3Sr2CuOz + HgO - heat(880C).					Annealing effects in (Hg,Cr)Sr2CuO4+d: transport and X-ray absorption studies				J.Supercond., 14(2001) 429	B.D.Padalia,I.K.Gopalakrishnan,J.V.Yakhmi,O.Prakash,P.Selvam,S.Balamurugan,S.Gupta		
33142	MPL0150261	impurity phase = SrCuO2, Sr2CuO3, HgSrO2	(Hg,Re)Sr2CuO4	Hg0.9Re0.1Sr2Cu1O4+z	Hg	0.9	Re	0.1	Sr	2	Cu	1													O	4+z			2001																												Hg1201	P4/mmm		A	3.784		8.668												K				54			54																																																																																																precursor(Re0.1Sr2CuOz) + HgO - Au tube - sealed in quartz - heat(880C, 16h + 920C, 16h)					Superconductivity and CuK-XANES of (Hg,Re)Sr2CuO4+d				Mod.Phys.Lett. B, 15(2001)261	B.D.Padalia,I.K.Gopalakrishnan,J.V.Yakhmi,O.Prakash,P.Selvam,S.Balamurugan		
33143	MPL0150497	hole conc. = 0.063	(La,Sr)2CuO4	La1.985Sr0.015Cu1O4.024	La	1.985	Sr	0.015	Cu	1															O	4+z	4.024		2001																												T																		K				16			16																																																																																																electro-chemical oxidation					Wigner lattice order, collective mode, and supercondutivity in the La1.985Sr0.015CuO4+d system				Mod.Phys.Lett. B, 15(2001)497	P.Hemg Hor,Y.H.Kim		
33144	MPL0150497	hole conc. = 0.07	(La,Sr)2CuO4	La1.985Sr0.015Cu1O4.032	La	1.985	Sr	0.015	Cu	1															O	4+z	4.032		2001																												T																		K				26			26																																																																																																electro-chemical oxidation					Wigner lattice order, collective mode, and supercondutivity in the La1.985Sr0.015CuO4+d system				Mod.Phys.Lett. B, 15(2001)497	P.Hemg Hor,Y.H.Kim		
33145	JAP0897487	Magnetic Curie temp. confirmed by M-H hysteresis. coexistence of weak ferro and s/c.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2001							135																					Ru1212																		K	10		45				27.5																																																																																																mixture-heat(800C,12h + 1050C,24h, in air)-ANN(500C,24h, in O2)					Vortex dynamics and magnetic anisotropy in RuSr2GdCu2O8			Department of Physics, University of South Florida, Tampa, Florida 33620	J.Appl.Phys., 89(2001)7487	H.Srikanth,J.B.Wiley,J.Tallon,L.Spinu,T.Kodenkandath		
33146	JAP0897657		(La,Nd)2Ba2CaCu5O10	La1.8Nd0.2Ba2Ca0.4Cu4.4O7.183	La	1.8	Nd	0.2	Ba	2	Ca	0.4	Cu	4.4											O	10+z	7.183		2001																												2125	P4/mmm		A	3.8836		11.6754												K																																																																																																							mixture-CAL(950C,24h)-pellet-SIN(950C,12h,in flowing N2)-slow cool to 500C-ANN(500C,24h,inO2)-RT					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
33147	JAP0897657		(La,Nd)2Ba2CaCu5O10	La1.7Nd0.3Ba2Ca0.6Cu4.6O7.135	La	1.7	Nd	0.3	Ba	2	Ca	0.6	Cu	4.6											O	10+z	7.135		2001																												2125	P4/mmm		A	3.8735		11.6686												K	77						77																																																																																																mixture-CAL(950C,24h)-pellet-SIN(950C,12h,in flowing N2)-slow cool to 500C-ANN(500C,24h,inO2)-RT					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
33148	JAP0897657		(La,Nd)2Ba2CaCu5O10	La1.5Nd0.5Ba2Ca1Cu5O7.123	La	1.5	Nd	0.5	Ba	2	Ca	1	Cu	5											O	10+z	7.123		2001																												2125	P4/mmm		A	3.8742		11.6569												K	78						78																																																																																																mixture-CAL(950C,24h)-pellet-SIN(950C,12h,in flowing N2)-slow cool to 500C-ANN(500C,24h,inO2)-RT					Structural and superconducting properties of La2-xRxBa2CayCu4+yO10+z (R=Nd,Gd; y=2x) system			Department of Physics,Saurashtra University,Rajkot, Gujarat,India	J.Appl.Phys., 89(2001)7657	D.G.Kuberkar,K.Mavani,Krushna Mavani,N.A.Shah,R.G.Kulkami,R.G.Kulkarni,R.S.Thampi,S.K.Malik,S.Rayaprol,W.B.Yelon		
33149	JAP0897660	c-axis aligned poder. ramda(T)-ramda(0)=A*T2+C*T4.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O3.97	Pr	1.85	Ce	0.15	Cu	1															O	4-z	3.97		2001																												T'			A	3.961		12.147												K	17		23				20																																									nm	fitting susceptibility to Physica C 214(1993)350		132.8																																																				standard solid state reaction method. c-axis alignment was achieved by rotating under H=1 T.					Non- s-wave behavior of c-axis aligned Pr1.85 Ce0.15 CuO3.97 superconducting powder			Department of Physics, National Tsing Hua University, Hsinchu, Taiwan 300, Republic of China	J.Appl.Phys., 89(2001)7660	B.C.Chang,B.N.Lin,H.C.Chiang,H.C.Ku,T.I.Hsu,Y.Y.Hsu		
33150	SUP0140181	size=0.8*1.8*0.03 mm3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				84			84																																									micron.m	ac susceptibility for 100 kHz			70																																																								Triple approach to determination of the c-axis penetration depth in BSCCO crystals				J.Supercond., 14(2001) 181	A.A.Zhukov,A.Buzdin,D.V.Shovkun,H.Enriquez,M.Daumens,M.R.Trunin,N.Bontemps,T.Tamegai,Y.A.Nefyodov		
33151	SUP0140181	size=0.8*1.8*0.03 mm3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				84			84																																									micron.m	surface impedance			50																																																								Triple approach to determination of the c-axis penetration depth in BSCCO crystals				J.Supercond., 14(2001) 181	A.A.Zhukov,A.Buzdin,D.V.Shovkun,H.Enriquez,M.Daumens,M.R.Trunin,N.Bontemps,T.Tamegai,Y.A.Nefyodov		
33152	SUP0140181	size=0.8*1.8*0.03 mm3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				84			84																																									micron.m	microwave absorption			35																																																								Triple approach to determination of the c-axis penetration depth in BSCCO crystals				J.Supercond., 14(2001) 181	A.A.Zhukov,A.Buzdin,D.V.Shovkun,H.Enriquez,M.Daumens,M.R.Trunin,N.Bontemps,T.Tamegai,Y.A.Nefyodov		
33153	SUP0140181	size=1.5*1.5*0.1 mm3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				90			90																																									micron.m	ac susceptibility for 100 kHz			210																																																								Triple approach to determination of the c-axis penetration depth in BSCCO crystals				J.Supercond., 14(2001) 181	A.A.Zhukov,A.Buzdin,D.V.Shovkun,H.Enriquez,M.Daumens,M.R.Trunin,N.Bontemps,T.Tamegai,Y.A.Nefyodov		
33154	SUP0140181	size=1.5*1.5*0.1 mm3	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2001																												Bi2212																		K				90			90																																									micron.m	surface impedance			150																																																								Triple approach to determination of the c-axis penetration depth in BSCCO crystals				J.Supercond., 14(2001) 181	A.A.Zhukov,A.Buzdin,D.V.Shovkun,H.Enriquez,M.Daumens,M.R.Trunin,N.Bontemps,T.Tamegai,Y.A.Nefyodov		
33155	JCG2230175	size=4*2*0.1 mm3. compositions=Bi2.06Sr1.95Ca1.97Cu3.02O10+z by EPMA.	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca1Cu2O10+z	Bi	2	Sr	2	Ca	1	Cu	2													O	10+z		3	2001																												Bi2223			A			37.164												K				110			110																																																																							mOhm												0.014	7500												Bi2.1Sr1.9Ca2Cu3Oz - TSFZ method (growth rate=0.05 mm/h, in 20 %O2 + 80%Ar) - ANN(600C, in O2 flow)					Single-crystal growth of Bi2Sr2Ca2Cu3O10+d (Bi-2223) by TSFZ method			Department of Applied Physics, Faculty of Science, Science University of Tokyo, 1-3 Kagurazaka, Shinjyuku-ku, Tokyo , Japan	J.Cryst.Growth, 223(2001)175	A.Matsuda,T.Fujii,T.Watanabe		
33156	JCG2290396	maybe, overdoping state	Bi2(Sr,Nd)2CuO6	Bi1.8Sr1.1Nd0.7Cu1Oz	Bi	1.8	Sr	1.1	Nd	0.7	Cu	1													O	z		3	2001																												Bi2201																		K				20			20																																																																																																Crystals were grown from the Bi2Sr1.6Nd0.4CuOz melt.					Crystal growth of Bi2(Sr,Nd/Sm)2CuOy and their superconductivity			Institute for Materials Research,Tohoku University,2-1-1 Katahira,Aoba-ku,Sendai 980-8577,Japan	J.Cryst.Growth, 229(2001)396	H.Faqir,M.Itou,M.Kikuchi,T.Atou,Y.Murakami,Y.Syono		
33157	JCG2290391		(Gd,Ce)2Sr2NbCu2O10	Gd1.5Ce0.5Sr2Nb1Cu2O10+z	Gd	1.5	Ce	0.5	Sr	2	Nb	1	Cu	2											O	10+z		3	2001																												RSNCO			A	3.8588		28.6632												K				28			28																																																																																																Crystals grown by flux method using CuO flux.					Growth and characterization of superconducting (GdCe)2NbSr2Cu2O10-d single crystals			Crystal Growth Centre,Anna Uni v ersity,Chennai 600 025,India	J.Cryst.Growth, 229(2001)391	C.Subramanian,E.Srinivasan,P.Ramasamy,R.Jayavel,S.Uthayakumar		
33158	JAP0897669	peak effect is observed upto 70K.	(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.64Pb0.36Sr2Ca0.95Y0.05Cu2O8+z	Bi	1.64	Pb	0.36	Sr	2	Ca	0.95	Y	0.05	Cu	2									O	8+z		3	2001																												Bi2212																		K				76			76																																																																																																self-flux method. melt(Bi:Pb:Sr:Ca:Y:Cu=1.5:0.5:2:1-x:x:2). ANN(in air).					Superconductivity and flux pinning in Y and heavily Pb codoped Bi-2212 single crystals			Institute for Superconducting and Electronic Materials, University of Wollongong, NSW 2522, Australia	J.Appl.Phys., 89(2001)7669	D.Millikon,G.Heine,H.K.Liu,H.M.Luo,J.Horvat,S.X.Dou,S.Y.Ding,W.Lang,X.L.Wang		
33159	JAP0897669	resistivity drops steeply at 76 K.		Bi1.64Pb0.36Sr2Ca0.67Y0.33Cu2O8+z	Bi	1.64	Pb	0.36	Sr	2	Ca	0.67	Y	0.33	Cu	2									O	8+z		3	2001																												Bi2212																		K	25		76	25			25																																																																																																					Superconductivity and flux pinning in Y and heavily Pb codoped Bi-2212 single crystals			Institute for Superconducting and Electronic Materials, University of Wollongong, NSW 2522, Australia	J.Appl.Phys., 89(2001)7669	D.Millikon,G.Heine,H.K.Liu,H.M.Luo,J.Horvat,S.X.Dou,S.Y.Ding,W.Lang,X.L.Wang		
33160	IST990098	oxygen content represent starting composition	(CO3)Sr2CuO2	C1Sr2Cu1O5.35	C	1	Sr	2	Cu	1															O	5+z	5.35		2000																												M1201			A	3.898		7.4871												K																																																																																																					CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33161	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.9N0.1Sr2Cu1O5.35	C	0.9	N	0.1	Sr	2	Cu	1													O	5+z	5.35		2000																												M1201			A	3.899		7.4792												K				13			13																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33162	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.8N0.2Sr2Cu1O5.3	C	0.8	N	0.2	Sr	2	Cu	1													O	5+z	5.3		2000																												M1201			A	3.8974		7.4724												K				33			33																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33163	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.8N0.2Sr2Cu1O5.35	C	0.8	N	0.2	Sr	2	Cu	1													O	5+z	5.35		2000																												M1201			A	3.8983		7.4716												K				31			31																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33164	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.8N0.2Sr2Cu1O5.45	C	0.8	N	0.2	Sr	2	Cu	1													O	5+z	5.45		2000																												M1201			A	3.8984		7.4692												K				31			31																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33165	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.7N0.3Sr2Cu1O5.35	C	0.7	N	0.3	Sr	2	Cu	1													O	5+z	5.35		2000																												M1201			A	3.8984		7.4676												K				35			35																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33166	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.7N0.3Sr2Cu1O5.45	C	0.7	N	0.3	Sr	2	Cu	1													O	5+z	5.45		2000																												M1201			A	3.8976		7.4719												K				31			31																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33167	IST990098	oxygen content represent starting composition	(CO3,NO3)Sr2CuO2	C0.7N0.3Sr2Cu1O5.55	C	0.7	N	0.3	Sr	2	Cu	1													O	5+z	5.55		2000																												M1201			A	3.8978		7.4728												K				31			31																																																																																														CuO,Sr(NO3)2,Sr2CuO3,SrO2,SrCO3		mixture-sealed in Au capsule with Ag2O(oxidizing agent)-high pressure synthesis(5.5 GPa,1270C,1 h)-Q to RT					New oxycarbonitrate superconductors (C1-xNx)Sr2CuO5+y with a 1201-type structure			NIRIM , Tsukuba, Ibaraki, Japan	Advances in Superconductivity, 12(2000)98	E.Takayama-Muromachi,N.Zhigadlo,T.Asaka,Y.Anan,Y.Matsui		
33168	SST0140213		GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			2001																												Y123			A	3.8445	3.9094	11.68												K				91.4			91.4																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33169	SST0140213		(Gd,Ca)Ba2Cu3O7	Gd0.98Ca0.02Ba2Cu3O7-z	Gd	0.98	Ca	0.02	Ba	2	Cu	3													O	7-z			2001																												Y123																		K				85.4			85.4																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33170	SST0140213		(Gd,Ca)Ba2Cu3O7	Gd0.95Ca0.05Ba2Cu3O7-z	Gd	0.95	Ca	0.05	Ba	2	Cu	3													O	7-z			2001																												Y123			A	3.8545	3.9079	11.698												K				81.9			81.9																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33171	SST0140213		(Gd,Ca)Ba2Cu3O7	Gd0.9Ca0.1Ba2Cu3O7-z	Gd	0.9	Ca	0.1	Ba	2	Cu	3													O	7-z			2001																												Y123																		K				80.3			80.3																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33172	SST0140213		(Gd,Ca)Ba2Cu3O7	Gd0.85Ca0.15Ba2Cu3O7-z	Gd	0.85	Ca	0.15	Ba	2	Cu	3													O	7-z			2001																												Y123			A	3.8547	3.9139	11.676												K				79.5			79.5																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33173	SST0140213		(Gd,Ca)Ba2Cu3O7	Gd0.8Ca0.2Ba2Cu3O7-z	Gd	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z			2001																												Y123																		K				68.8			68.8																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33174	SST0140213		(Gd,Pr)Ba2Cu3O7	Gd0.9Pr0.1Ba2Cu3O7-z	Gd	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z			2001																												Y123																		K				67.1			67.1																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33175	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.85Pr0.1Ca0.05Ba2Cu3O7-z	Gd	0.85	Pr	0.1	Ca	0.05	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8571	3.9114	11.764												K				70.6			70.6																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33176	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.8Pr0.1Ca0.1Ba2Cu3O7-z	Gd	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8481	3.8824	11.684												K				77.4			77.4																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33177	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.75Pr0.1Ca0.15Ba2Cu3O7-z	Gd	0.75	Pr	0.1	Ca	0.15	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8579	3.8887	11.742												K				74.2			74.2																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33178	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.7Pr0.1Ca0.2Ba2Cu3O7-z	Gd	0.7	Pr	0.1	Ca	0.2	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8507	3.8846	11.724												K				69			69																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33179	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.65Pr0.1Ca0.25Ba2Cu3O7-z	Gd	0.65	Pr	0.1	Ca	0.25	Ba	2	Cu	3											O	7-z			2001																												Y123																		K				60.2			60.2																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33180	SST0140213		(Gd,Pr)Ba2Cu3O7	Gd0.85Pr0.15Ba2Cu3O7-z	Gd	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z			2001																												Y123																		K				55			55																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33181	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.8Pr0.15Ca0.05Ba2Cu3O7-z	Gd	0.8	Pr	0.15	Ca	0.05	Ba	2	Cu	3											O	7-z			2001																												Y123																		K				64.3			64.3																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33182	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.75Pr0.15Ca0.1Ba2Cu3O7-z	Gd	0.75	Pr	0.15	Ca	0.1	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8386	3.8877	11.64												K				71.5			71.5																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33183	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.7Pr0.15Ca0.15Ba2Cu3O7-z	Gd	0.7	Pr	0.15	Ca	0.15	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8362	3.8757	11.668												K				72.4			72.4																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33184	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.65Pr0.15Ca0.2Ba2Cu3O7-z	Gd	0.65	Pr	0.15	Ca	0.2	Ba	2	Cu	3											O	7-z			2001																												Y123			A	3.8439	3.8896	11.698												K				66.6			66.6																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33185	SST0140213		(Gd,Pr,Ca)Ba2Cu3O7	Gd0.6Pr0.15Ca0.25Ba2Cu3O7-z	Gd	0.6	Pr	0.15	Ca	0.25	Ba	2	Cu	3											O	7-z			2001																												Y123																		K				61.5			61.5																																																																																																mixture-CAL(850C,24h, in air in Al2O3)-ANN(930C,24h,in flowing O2)-slow cooling to RT					Investigation of structure and transport properties of Gd1-x-zPrxCazBa2Cu3O7-d system				Supercond.Sci.Technol., 14(2001)213	H.Shakeripour,M.Akhavan		
33186	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.7La0.3Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.7	La	0.3	Cu	1											O	z			2001																												Bi2201																		K	35		43				39																																																																																																solid state reaction, then annealing (3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33187	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.65La0.35Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.65	La	0.35	Cu	1											O	z			2001																												Bi2201																		K	37		45				41																																																																																																solid state reaction, then annealing (3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33188	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.6La0.4Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.6	La	0.4	Cu	1											O	z			2001																												Bi2201																		K	35		43				39																																																																																																solid state reaction, then annealing (3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33189	SST0140599		Bi2(sr,La)2CuOz	Bi2Sr1.65La0.35Cu1Oz	Bi	2	Sr	1.65	La	0.35	Cu	1													O	z			2001																												Bi2201																		K	27		38				32.5																																																																																																solid state reaction, then annealing (500C,3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33190	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.8Pb0.2Sr1.65La0.35Cu1Oz	Bi	1.8	Pb	0.2	Sr	1.65	La	0.35	Cu	1											O	z			2001																												Bi2201																		K			44				44																																																																																																solid state reaction, then annealing (500C,3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33191	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.6Pb0.4Sr1.65La0.35Cu1Oz	Bi	1.6	Pb	0.4	Sr	1.65	La	0.35	Cu	1											O	z			2001																												Bi2201																		K	39		47				43																																																																																																solid state reaction, then annealing (500C,3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33192	SST0140599		(Bi,Pb)2(Sr,La)2CuOz	Bi1.4Pb0.6Sr1.65La0.35Cu1Oz	Bi	1.4	Pb	0.6	Sr	1.65	La	0.35	Cu	1											O	z			2001																												Bi2201																		K	36		46				41																																																																																																solid state reaction, then annealing (500C,3h, in p(O2)=5 E-5 atm)					47 K superconductivity in Bi1.6Pb0.4Sr1.65La0.35CuOz				Supercond.Sci.Technol., 14(2001)599	T.Shun,X.Gaojie,Z.Changjin,Z.Jianwu,Z.Yuheng		
33193	P065014507	high pressure XRD	NbSr2EuCu2O8	Nb1Sr2Eu1Cu2O8	Nb	1	Sr	2	Eu	1	Cu	2													O	8		1	2001																		GPa		120								1212			A	3.8747		11.632							E-3 /GPa	2.4		3.5																																																																																																									solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33194	P065014507	high pressure XRD	GaSr2YCu2O7	Ga1Sr2Y1Cu2O7	Ga	1	Sr	2	Y	1	Cu	2													O	7		1	2001																		GPa		85								1212			A	22.808	5.484	5.406							E-3 /GPa	4.8	3.7	3.3																																																																																																									solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33195	P065014507	high pressure XRD	Pb2Sr2YCu3O8	Pb2Sr2Y1Cu3O8+z	Pb	2	Sr	2	Y	1	Cu	3													O	8+z		1	2001																		GPa		129								Pb3212			A	5.389	5.428	15.712							E-3 /GPa	1.3	1.6	4.8																																																																																																									solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33196	P065014507	high pressure XRD	HgBa2CuO4	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z		1	2001																		GPa		63								Hg1201			A	3.8851		9.526							E-3 /GPa	4.7		6.5																																																																																																							HgO, (Cr2O3), Ba2CuO3	1	solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33197	P065014507	high pressure XRD	(Hg,Cr)Ba2CuO4	Hg0.8Cr0.2Ba2Cu1O4+z	Hg	0.8	Cr	0.2	Ba	2	Cu	1													O	4+z		1	2001																		GPa		64								Hg1201			A	3.9063		9.333							E-3 /GPa	4.7		5.9																																																																																																							HgO, (Cr2O3), Ba2CuO3	1	solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33198	P065014507	high pressure XRD	Sr2Cu(O2,CO3)	Sr2Cu1C1O5	Sr	2	Cu	1	C	1															O	5		1	2001																		GPa		62								Sr2CuO3			A	7.808		14.997							E-3 /GPa	4.3		8.5																																																																																																							SrCO3,CuO	1	solid state reaction					Structure-compressibility relationships in layered cuprate materials			School of Chemistry, University of Birmingham, Edgbaston, Birmingham B15 2TT, United Kingdom	Phys.Rev.B, 65(2001)14507	A.P.Jephcoat,I.Gameson,J.A.Hriljac,Neil C.Hyatt,P.P.Edwards,Y.Miyazaki		
33199	P065024523	H//c-axis	(La,Sr)2CuO4	La1.94Sr0.06Cu1O4+z	La	1.94	Sr	0.06	Cu	1															O	4+z		3	2001																												T																		K		8.02					8.02																																																																																																					Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33200	P065024523	H//c-axis	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4+z	La	1.9	Sr	0.1	Cu	1															O	4+z		3	2001																												T																		K		26.9					26.9																																																3.76	13							mj/mol.K2	2.26	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33201	P065024523	H//c-axis	(La,Sr)2CuO4	La1.87Sr0.13Cu1O4+z	La	1.87	Sr	0.13	Cu	1															O	4+z		3	2001																												T																		K		34.4					34.4																																		HIR33201														4	13							mj/mol.K2	1.98	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33202	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.93Sr0.07Cu1O4+z	La	1.93	Sr	0.07	Cu	1															O	4+z			2001																												T																		K		14.7					14.7																																																3.96	13							mj/mol.K2	0.43	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33203	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.919Sr0.081Cu1O4+z	La	1.919	Sr	0.081	Cu	1															O	4+z			2001																												T																		K		20.6					20.6																																		HIR33203														4.08	13							mj/mol.K2	0.56	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33204	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4+z	La	1.91	Sr	0.09	Cu	1															O	4+z			2001																												T																		K		26.7					26.7																																		HIR33204														4.04	13							mj/mol.K2	1.19	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33205	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.889Sr0.111Cu1O4+z	La	1.889	Sr	0.111	Cu	1															O	4+z			2001																												T																		K		28.4					28.4																																		HIR33205														4.02	13							mj/mol.K2	1.83	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33206	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.883Sr0.117Cu1O4+z	La	1.883	Sr	0.117	Cu	1															O	4+z			2001																												T																		K		28.6					28.6																																		HIR33206														3.98	13							mj/mol.K2	1.56	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33207	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.857Sr0.143Cu1O4+z	La	1.857	Sr	0.143	Cu	1															O	4+z			2001																												T																		K		36.6					36.6																																																4.04	13							mj/mol.K2	2.79	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33208	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z			2001																												T																		K		37.4					37.4																																		HIR33208														4.04	13							mj/mol.K2	2.82	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33209	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.844Sr0.156Cu1O4+z	La	1.844	Sr	0.156	Cu	1															O	4+z			2001																												T																		K		36.8					36.8																																																4.24	13							mj/mol.K2	2.9	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33210	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.812Sr0.188Cu1O4+z	La	1.812	Sr	0.188	Cu	1															O	4+z			2001																												T																		K		31.7					31.7																																																4.2	13							mj/mol.K2	3.06	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33211	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.807Sr0.193Cu1O4+z	La	1.807	Sr	0.193	Cu	1															O	4+z			2001																												T																		K		29.8					29.8																																																4.14	13							mj/mol.K2	3.03	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33212	P065024523	magnetically aligned sample. optimum oxygen content. H//c-axis	(La,Sr)2CuO4	La1.766Sr0.234Cu1O4+z	La	1.766	Sr	0.234	Cu	1															O	4+z			2001																												T																		K		18.7					18.7																																																3.8	13							mj/mol.K2	2.81	parameter fitting from Hc measurement																																											Electronic density of states derived from thermodynamic critical field curves for underdoped La2-xSrxCuO4+d			Ames Laboratory, USDOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 65(2001)24523	D.K.Finnemore,Y.M.Huh		
33213	APA0740079	not s/c. as-grown. oxygen content 4+z (z less than 0.01)	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4+z	4		2002																												T			A	5.358	5.404	13.152												K					5																																																																																																	1	mixture-CAL(900C,36h, in air)-SIN(1000C, 100h, in air)-ANN(800C, 116h, in air)					Superconductivity at 45 K in La2CuO4+z oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, P.R. China	Appl.Phys. A, 74(2002)79	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Y.C.Lan,Z.X.Zhao		
33214	APA0740079	chemical oxidization using NaClO	La2CuO4	La2Cu1O4.11	La	2	Cu	1																	O	4+z	4.11		2002																												T			A	5.338	5.416	13.224												K				45			45										12.7																																																																																					1	mixture-CAL(900C,36h, in air)-SIN(1000C, 100h, in air)-ANN(800C, 116h, in air)					Superconductivity at 45 K in La2CuO4+z oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, P.R. China	Appl.Phys. A, 74(2002)79	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Y.C.Lan,Z.X.Zhao		
33215	PHC3660299	Hirr defined as delta-M=0.1 emu/cm3	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2002																												IL			A	3.95		3.41												K				43			43																																		HIR33215																																																														precursor(Sr0.9La0.1CuO2)-Au capsule-high pressure synthesis(4 GPa)					Synthesis and pinning properties of the infinite-layer superconductor Sr0.9La0.1CuO2			National Creative Research Initiative Center for Superconductivity and Department of Physics,Pohang University of Science		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Scog Kim,S.Y.Lee,Sung-Ik Lee,Yushu Yao		
33216	PHC3660238		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212																		K	86.2						86.2																																																																					-3.72	TP33216																										crystals were grown from Bi-rich melts by a directional soridification method. ANN(400C,2days,in air)					Gd substitution effect on the normal-state transport properties of Bi2Sr2Ca1-xGdxCu2O8+z single crystals			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 366(2002)238	Wenbin Wu,Xia Zhao,Xiaoguang Li,Xuefeng Sun,Yun Peng		
33217	PHC3660238		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.91Gd0.09Cu2O8+z	Bi	2	Sr	2	Ca	0.91	Gd	0.09	Cu	2											O	8+z		3	2002																												Bi2212																		K	87						87																																																																					-1.73	TP33217																										crystals were grown from Bi-rich melts by a directional soridification method. ANN(400C,2days,in air)					Gd substitution effect on the normal-state transport properties of Bi2Sr2Ca1-xGdxCu2O8+z single crystals			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 366(2002)238	Wenbin Wu,Xia Zhao,Xiaoguang Li,Xuefeng Sun,Yun Peng		
33218	PHC3660238		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.81Gd0.19Cu2O8+z	Bi	2	Sr	2	Ca	0.81	Gd	0.19	Cu	2											O	8+z		3	2002																												Bi2212																		K	84.1						84.1																																																																					3.19	TP33218																										crystals were grown from Bi-rich melts by a directional soridification method. ANN(400C,2days,in air)					Gd substitution effect on the normal-state transport properties of Bi2Sr2Ca1-xGdxCu2O8+z single crystals			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 366(2002)238	Wenbin Wu,Xia Zhao,Xiaoguang Li,Xuefeng Sun,Yun Peng		
33219	PHC3660238		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.68Gd0.32Cu2O8+z	Bi	2	Sr	2	Ca	0.68	Gd	0.32	Cu	2											O	8+z		3	2002																												Bi2212																		K	79						79																																																																					9.29	TP33219																										crystals were grown from Bi-rich melts by a directional soridification method. ANN(400C,2days,in air)					Gd substitution effect on the normal-state transport properties of Bi2Sr2Ca1-xGdxCu2O8+z single crystals			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 366(2002)238	Wenbin Wu,Xia Zhao,Xiaoguang Li,Xuefeng Sun,Yun Peng		
33220	PHC3660238		Bi2Sr2(Ca,Gd)Cu2O8	Bi2Sr2Ca0.59Gd0.41Cu2O8+z	Bi	2	Sr	2	Ca	0.59	Gd	0.41	Cu	2											O	8+z		3	2002																												Bi2212																		K	63.8						63.8																																																																					19.9	TP33220																										crystals were grown from Bi-rich melts by a directional soridification method. ANN(400C,2days,in air)					Gd substitution effect on the normal-state transport properties of Bi2Sr2Ca1-xGdxCu2O8+z single crystals			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 366(2002)238	Wenbin Wu,Xia Zhao,Xiaoguang Li,Xuefeng Sun,Yun Peng		
33221	PHC3660043	F-content shows nominal value. 0223 + 0234 phases	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F0.8O7.2+z	Ba	2	Ca	2	Cu	3	F	0.8													O	7.2+z		2	2001																												0223																		K				120			120																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33222	PHC3660043	F-content shows nominal value. 0223 + 0234 phases	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F1O7.0+z	Ba	2	Ca	2	Cu	3	F	1													O	7.0+z		2	2001																												0223																		K				116			116																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33223	PHC3660043	F-content shows nominal value.	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F1.2O6.8+z	Ba	2	Ca	2	Cu	3	F	1.2													O	6.8+z		1	2001																												0223																		K				113			113																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33224	PHC3660043	F-content shows nominal value.	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F1.3O6.7+z	Ba	2	Ca	2	Cu	3	F	1.3													O	6.7+z		1	2001																												0223			A	3.861		27.451												K				109			109																																		HIR33224																																																														precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33225	PHC3660043	F-content shows nominal value.	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F1.4O6.6+z	Ba	2	Ca	2	Cu	3	F	1.4													O	6.6+z		1	2001																												0223																		K	107			106			106																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33226	PHC3660043	F-content shows nominal value.	Bi2Ca2Cu3O6(O,F)2	Ba2Ca2Cu3F1.6O6.2+z	Ba	2	Ca	2	Cu	3	F	1.6													O	6.2+z		1	2001																												0223																		K	96			95.5			95.5																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33227	PHC3660043	F-content shows nominal value. oz=8.25+z	Bi2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1O8.2+z	Ba	2	Ca	3	Cu	4	F	1													O	8.2+z		1	2001																												0234			A	3.8558		33.8562												K				104			104																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33228	PHC3660043	F-content shows nominal value. oz=8.25+z	Bi2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.2O8.2+z	Ba	2	Ca	3	Cu	4	F	1.2													O	8.2+z		1	2001																												0234																		K	100.5			101			101																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33229	PHC3660043	F-content shows nominal value. oz=8.25+z	Bi2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.4O8.2+z	Ba	2	Ca	3	Cu	4	F	1.4													O	8.2+z		1	2001																												0234																		K	97						97																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33230	PHC3660043	F-content shows nominal value. oz=4.25+z	Bi2CaCu2O4(O,F)2	Ba2Ca1Cu2F1.3O4.2+z	Ba	2	Ca	1	Cu	2	F	1.3													O	4.2+z		1	2001																												0212			A	3.8791		21.1765												K				90			90																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33231	PHC3660043	F-content shows nominal value. oz=10.25+z	Bi2Ca4Cu5O10(O,F)2	Ba2Ca4Cu5F1O10+z	Ba	2	Ca	4	Cu	5	F	1													O	10+z		1	2001																												0245			A	3.8602		40.1307												K				90			90																																																																																																precursors(Ba2Can-1CunOz and BaCuO2) - mix - sealed in Au capsule -react(3.5-4.5GPa, 900-1050C, 2h)					Highpressure synthesis and properties of Ba2Can-1CunO2n(O,F)2 (n=2 - 5) superconductors			Electrotechnical Laboratory & CREST, Umezono, Tsukuba, Ibaraki, Japan	Physica C, 366(2001)43	A.Iyo,H.Ihara,M.Tokumoto,Y.Tanaka		
33232	SSC0200995		Li-Ti-O4	Li2.6Ti1.7O4	Li	2.6	Ti	1.7																	O	4		1	1976																												Li2TiO4																		K		11.4					11.4																				kOe		180			162			4.2	kOe/K		39			HC33232																																																																			Paramagnetic limiting in superconducting Li-Ti-0 ternary system			MIT,Cambridge, MA, USA	Solid State Commun., 20(1976)995	E.J.McNiff,Jr.,S.Forner		
33233	SSC0200995		Li-Ti-O4	Li2.6Ti1.9O4	Li	2.6	Ti	1.9																	O	4		1	1976																												Li2TiO4																		K		11.2					11.2																				kOe		148			124			4.2	kOe/K		20			HC33232																																																																			Paramagnetic limiting in superconducting Li-Ti-0 ternary system			MIT,Cambridge, MA, USA	Solid State Commun., 20(1976)995	E.J.McNiff,Jr.,S.Forner		
33234	SSC0200995		Li-Ti-O4	Li2.6Ti2.7O4	Li	2.6	Ti	2.7																	O	4		1	1976																												Li2TiO4																		K		10.9					10.9																				kOe		105			77			4.2	kOe/K		13			HC33232																																																																			Paramagnetic limiting in superconducting Li-Ti-0 ternary system			MIT,Cambridge, MA, USA	Solid State Commun., 20(1976)995	E.J.McNiff,Jr.,S.Forner		
33253	PCS2739	Tc,Hc2 were determined from R(H), C(H) measurement. RRR=28. G-L = 14. gamma in mj/K2.mol-Re.	Cd2Re2O7	Cd2Re2O7.1	Cd	2	Re	2																	O	7	7.1	3	2002																												pyrochlore			A	10.226														K	0.99		1.06	1		0.03	1											mT	specific heat	2							T	specific heat	0.29														A		340			A		4600					3.6	12					dC/r*Tc	1.15	mj/K2.m-Re	15.1	specific heat	458												mOhm.cm							0.0115				0.32														Chemical reaction(2CdO+5/3ReO3 + 1/3Re --Cd2Re2O7), 800 - 900C, 70h					Superconducting properties of the pyrochlore oxide Cd2Re2O7			Institute for Solid State Physics, University of Tokyo,Kashiwa, Chiba, Japan	J.Phys.Chem.Solids, 63(2002)1021	M.Hanawa,Z.Hiroi		
33254	PHC3660147	only structural data 	Hg2Ba2YCu2O8	Hg2Ba2Y1Cu2O8-z	Hg	2	Ba	2	Y	1	Cu	2													O	8-z		1	2002																												Hg2212			A	3.8606		28.915																																																																																																																			(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33255	PHC3660147	only structural data 	(Hg,Pb)2Ba2YCu2O8	Hg1.75Pb0.25Ba2Y1Cu2O8-z	Hg	1.75	Pb	0.25	Ba	2	Y	1	Cu	2											O	8-z		1	2002																												Hg2212			A	3.8749		28.9122																																																																																																																			(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33256	PHC3660147	only structural data 	Hg2Ba2(Y,Ca)Cu2O8	Hg2Ba2Y0.6Ca0.4Cu2O8-z	Hg	2	Ba	2	Y	0.6	Ca	0.4	Cu	2											O	8-z		1	2002																												Hg2212			A	3.8545		29.034																																																																																																																			(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33257	PHC3660147		Hg2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.5Ca0.5Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.5	Ca	0.5	Cu	2									O	8-z		1	2002																												Hg2212			A	3.8667		28.9804												K				84			84																																																																																																(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33258	PHC3660147		Hg2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.3Ca0.7Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.3	Ca	0.7	Cu	2									O	8-z		1	2002																												Hg2212																		K				80			80																																																																																																(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33259	PHC3660147		Hg2Ba2CaCu2O8	Hg1.5Pb0.5Ba2Ca1Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Ca	1	Cu	2											O	8-z		1	2002																												Hg2212																		K				60			60																																																																																																(Ba2(Y,Ca)Cu2Oz) - mixed with HgO/PbO2 - Au capsule - sealed then heat (4GPa, 100C, 2h)					Optimal and overdoped superconducting regimes in Hg-2212 system by Pb substitution			Grenoble Cedex, France	Physica C, 366(2002)147	J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde,R.Bruyere		
33260	JCG2290365		YbBa2Cu4O8	Yb1Ba2Cu4Oz	Yb	1	Ba	2	Cu	4															O	z		1	2001																												Y124																		K	78			79			79																																																																																																spin coated on SrTiO3(001), preheat(500C), heat(800C, 18h, in O2 flow, slow cooling					Tc enhancement by partial substitution of Ca in superconducting YbBa2Cu4O8 epitaxial films prepared by coating-pyrolysis process			National Institute of Advanced Industrial Science and Technology, Tsukuba,Ibaraki,Japan	J.Crys.Growth, 229(2001)365	I.Yamaguchi,S.Mizuta,T.Kumagai,T.Manabe,T.Shimizu,Y.Yajima		
33261	JCG2290365		(Yb,Ca)Ba2Cu4O8	Yb0.99Ca0.01Ba2Cu4Oz	Yb	0.99	Ca	0.01	Ba	2	Cu	4													O	z		1	2001																												Y124																		K	81			80			80																																																																																																spin coated on SrTiO3(001), preheat(500C), heat(800C, 18h, in O2 flow, slow cooling					Tc enhancement by partial substitution of Ca in superconducting YbBa2Cu4O8 epitaxial films prepared by coating-pyrolysis process			National Institute of Advanced Industrial Science and Technology, Tsukuba,Ibaraki,Japan	J.Crys.Growth, 229(2001)365	I.Yamaguchi,S.Mizuta,T.Kumagai,T.Manabe,T.Shimizu,Y.Yajima		
33262	JCG2290365	impurity phase=Y-123 phase	(Yb,Ca)Ba2Cu4O8	Yb0.95Ca0.05Ba2Cu4Oz	Yb	0.95	Ca	0.05	Ba	2	Cu	4													O	z		1	2001																												Y124																		K	83			81			81																																																																																																spin coated on SrTiO3(001), preheat(500C), heat(800C, 18h, in O2 flow, slow cooling					Tc enhancement by partial substitution of Ca in superconducting YbBa2Cu4O8 epitaxial films prepared by coating-pyrolysis process			National Institute of Advanced Industrial Science and Technology, Tsukuba,Ibaraki,Japan	J.Crys.Growth, 229(2001)365	I.Yamaguchi,S.Mizuta,T.Kumagai,T.Manabe,T.Shimizu,Y.Yajima		
33263	JCG2290365	impurity phase=Y-123 phase	(Yb,Ca)Ba2Cu4O8	Yb0.9Ca0.1Ba2Cu4Oz	Yb	0.9	Ca	0.1	Ba	2	Cu	4													O	z		1	2001																												Y124																		K	83			83			83																																																																																																spin coated on SrTiO3(001), preheat(500C), heat(800C, 18h, in O2 flow, slow cooling					Tc enhancement by partial substitution of Ca in superconducting YbBa2Cu4O8 epitaxial films prepared by coating-pyrolysis process			National Institute of Advanced Industrial Science and Technology, Tsukuba,Ibaraki,Japan	J.Crys.Growth, 229(2001)365	I.Yamaguchi,S.Mizuta,T.Kumagai,T.Manabe,T.Shimizu,Y.Yajima		
33264	JPS0702856		YBa2Cu3O7	Yb1Ba2Cu3O6.9	Yb	1	Ba	2	Cu	3															O	7-z	6.9	3	2001																												Y123																		K		92.8					92.8			K/GPa	1.3																																																																																												Crystal pulling method in air, then ANN(500C, in flowing O2)					Pressure-Induced Suppression of Pair Breaking in YBa2(Cu1-xZnx)3O7-z			SRL, ISTEC, Shinonome,Koto-ku,Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)2856	K.Yoshida,S.Tajima		
33265	JPS0702856		YBa2(Cu,Zn)3O7	Yb1Ba2Cu2.982Zn0.018O6.9	Yb	1	Ba	2	Cu	2.982	Zn	0.018													O	7-z	6.9	3	2001																												Y123																		K		85.1					85.1			K/GPa	1.7																																																																																												Crystal pulling method in air, then ANN(500C, in flowing O2)					Pressure-Induced Suppression of Pair Breaking in YBa2(Cu1-xZnx)3O7-z			SRL, ISTEC, Shinonome,Koto-ku,Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)2856	K.Yoshida,S.Tajima		
33266	JPS0702856		YBa2(Cu,Zn)3O7	Yb1Ba2Cu2.943Zn0.057O6.9	Yb	1	Ba	2	Cu	2.943	Zn	0.057													O	7-z	6.9	3	2001																												Y123																		K		64.3					64.3			K/GPa	2.8																																																																																												Crystal pulling method in air, then ANN(500C, in flowing O2)					Pressure-Induced Suppression of Pair Breaking in YBa2(Cu1-xZnx)3O7-z			SRL, ISTEC, Shinonome,Koto-ku,Tokyo,Japan	J.Phys.Soc.Jpn, 70(2001)2856	K.Yoshida,S.Tajima		
33267	PHC3410675		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4-z	Sm	1.85	Ce	0.15	Cu	1															O	4-z		1	2000																												T'																		K			20				20																																																																																																mixture-heat(900C,3d,in air)-final sintering(1200C)-reduction(970C, 18h, in flowing He)-cool to RT in 2h.					Superconductivity in polycrystalline Sm1.85(Ce1-xThx)0.15CuO4-y compouds			Universidade de Sao Paulo, Sao Paulo, Brazil	Physica C, 341(2000)675	E.A.Early,M.B.Maple,R.F.Jardim		
33268	PHC3410675		(Sm,Ce,Th)2CuO4	Sm1.85Ce0.1Th0.05Cu1O4-z	Sm	1.85	Ce	0.1	Th	0.05	Cu	1													O	4-z		1	2000																												T'																		K			19				19																																																																																																mixture-heat(900C,3d,in air)-final sintering(1200C)-reduction(970C, 18h, in flowing He)-cool to RT in 2h.					Superconductivity in polycrystalline Sm1.85(Ce1-xThx)0.15CuO4-y compouds			Universidade de Sao Paulo, Sao Paulo, Brazil	Physica C, 341(2000)675	E.A.Early,M.B.Maple,R.F.Jardim		
33269	PHC3410675		(Sm,Ce,Th)2CuO4	Sm1.85Ce0.07Th0.08Cu1O4-z	Sm	1.85	Ce	0.07	Th	0.08	Cu	1													O	4-z		1	2000																												T'																		K			18.5				18.5																																																																																																mixture-heat(900C,3d,in air)-final sintering(1200C)-reduction(970C, 18h, in flowing He)-cool to RT in 2h.					Superconductivity in polycrystalline Sm1.85(Ce1-xThx)0.15CuO4-y compouds			Universidade de Sao Paulo, Sao Paulo, Brazil	Physica C, 341(2000)675	E.A.Early,M.B.Maple,R.F.Jardim		
33270	PHC3410675		(Sm,Ce,Th)2CuO4	Sm1.85Ce0.03Th0.12Cu1O4-z	Sm	1.85	Ce	0.03	Th	0.12	Cu	1													O	4-z		1	2000																												T'																		K			16				16																																																																																																mixture-heat(900C,3d,in air)-final sintering(1200C)-reduction(970C, 18h, in flowing He)-cool to RT in 2h.					Superconductivity in polycrystalline Sm1.85(Ce1-xThx)0.15CuO4-y compouds			Universidade de Sao Paulo, Sao Paulo, Brazil	Physica C, 341(2000)675	E.A.Early,M.B.Maple,R.F.Jardim		
33271	PHC3410675		(Sm,Th)2CuO4	Sm1.85Th0.15Cu1O4-z	Sm	1.85	Th	0.15	Cu	1															O	4-z		1	2000																												T'																		K			13				13																																																																																																mixture-heat(900C,3d,in air)-final sintering(1200C)-reduction(970C, 18h, in flowing He)-cool to RT in 2h.					Superconductivity in polycrystalline Sm1.85(Ce1-xThx)0.15CuO4-y compouds			Universidade de Sao Paulo, Sao Paulo, Brazil	Physica C, 341(2000)675	E.A.Early,M.B.Maple,R.F.Jardim		
33272	PHC3410685	impurity =BaCuO2, major=Tl1223 phase, minor=Tl1212	(Tl,Ni)Ba2Ca2Cu3O9	Tl0.9Ni0.1Ba2Ca2Cu3O9-z	Tl	0.9	Ni	0.1	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.845		15.782												K		116.3					116.3																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33273	PHC3410685	impurity =BaCuO2, 	(Tl,Ni)Ba2Ca2Cu3O9	Tl0.8Ni0.2Ba2Ca2Cu3O9-z	Tl	0.8	Ni	0.2	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.842		15.762												K		113.4					113.4																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33274	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Ni)Ba2Ca2Cu3O9	Tl0.7Ni0.3Ba2Ca2Cu3O9-z	Tl	0.7	Ni	0.3	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.84		15.75												K		111.5					111.5																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33275	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Ni)Ba2Ca2Cu3O9	Tl0.6Ni0.4Ba2Ca2Cu3O9-z	Tl	0.6	Ni	0.4	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.843		15.755												K		109					109																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33276	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Ni)Ba2Ca2Cu3O9	Tl0.5Ni0.5Ba2Ca2Cu3O9-z	Tl	0.5	Ni	0.5	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.855		15.787												K		105					105																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33277	PHC3410685	impurity =BaCuO2, major=Tl1223 phase, minor=Tl1212	TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9-z	Tl	1	Ba	2	Ca	2	Cu	3													O	9-z			2000																												Tl1223			A	3.875		15.789												K		118					118																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33278	PHC3410685	impurity =BaCuO2, major=Tl1223 phase, minor=Tl1212	(Tl,Zn)Ba2Ca2Cu3O9	Tl0.9Zn0.1Ba2Ca2Cu3O9-z	Tl	0.9	Zn	0.1	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.863		15.778												K		119					119																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33279	PHC3410685	impurity =BaCuO2 	(Tl,Zn)Ba2Ca2Cu3O9	Tl0.8Zn0.2Ba2Ca2Cu3O9-z	Tl	0.8	Zn	0.2	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.841		15.772												K		124					124																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33280	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Zn)Ba2Ca2Cu3O9	Tl0.7Zn0.3Ba2Ca2Cu3O9-z	Tl	0.7	Zn	0.3	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.832		15.763												K		119					119																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33281	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Zn)Ba2Ca2Cu3O9	Tl0.6Zn0.4Ba2Ca2Cu3O9-z	Tl	0.6	Zn	0.4	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.831		15.761												K		117					117																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33282	PHC3410685	impurity =BaCuO2 + not defined phase	(Tl,Zn)Ba2Ca2Cu3O9	Tl0.4Zn0.6Ba2Ca2Cu3O9-z	Tl	0.4	Zn	0.6	Ba	2	Ca	2	Cu	3											O	9-z			2000																												Tl1223			A	3.834		15.781												K		113					113																																																																																																mixture-sealed quartz-heat(850C, 3.5h)-cool to RT(6C/min)					Replacement study of Thallium by Zn and Ni in Tl-1223 superconductor phase			Faculty of Science, Alexandria Unversity, Egypt	Physica C, 341(2000)685	A.I.Abou-Aly,A.L.Saad,L.H.Ibrahim,N.S.Aly,R.Awad		
33283	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.72Ca0.28Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.72	Ca	0.28	Cu	2									O	8-z			2000																												Hg2212																				74.5					74.5																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33284	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.72Ca0.28Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.72	Ca	0.28	Cu	2									O	8-z			2000																												Hg2212																				82.1					82.1																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33285	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.7Ca0.3Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	8-z			2000																												Hg2212																				84.3					84.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33286	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.29Ca0.71Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.29	Ca	0.71	Cu	2									O	8-z			2000																												Hg2212																				80.4					80.4																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33287	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.29Ca0.71Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.29	Ca	0.71	Cu	2									O	8-z			2000																												Hg2212																				60.4					60.4																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33288	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Ca1Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Ca	1	Cu	2											O	8-z			2000																												Hg2212																				55.3					55.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33289	PHC3410677	Ca-content by EDX	(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Ca1Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Ca	1	Cu	2											O	8-z			2000																												Hg2212																				43					43																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33290	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2YCu2O8	Hg1.4Tl0.6Ba2Y1Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	1	Cu	2											O	8-z			2000																												Hg2212																				14					14																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33291	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.9Ca0.1Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.9	Ca	0.1	Cu	2									O	8-z			2000																												Hg2212																				39.6					39.6																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33292	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.8Ca0.2Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.8	Ca	0.2	Cu	2									O	8-z			2000																												Hg2212																				52.3					52.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33293	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.7Ca0.3Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	8-z			2000																												Hg2212																				75.3					75.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33294	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.6Ca0.4Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.6	Ca	0.4	Cu	2									O	8-z			2000																												Hg2212																				84.3					84.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33295	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.5Ca0.5Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.5	Ca	0.5	Cu	2									O	8-z			2000																												Hg2212																				84.3					84.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33296	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.4Ca0.6Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.4	Ca	0.6	Cu	2									O	8-z			2000																												Hg2212																				69.4					69.4																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33297	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.3Ca0.7Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.3	Ca	0.7	Cu	2									O	8-z			2000																												Hg2212																				52.3					52.3																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33298	PHC3410677	Ca-content shows nominal value	(Hg,Tl)2Ba2(Y,Ca)Cu2O8	Hg1.4Tl0.6Ba2Y0.2Ca0.8Cu2O8-z	Hg	1.4	Tl	0.6	Ba	2	Y	0.2	Ca	0.8	Cu	2									O	8-z			2000																												Hg2212																				42.1					42.1																																																																																																HP-HT process. Ba2(Y,Ca)Cu2Oz was firstly prepared. Then, HgO, PbO2 added. Heat(100C, p=4GPa)					Enhancement of superconductivity in the double mercury layer compound Hg2Ba2(Y1-xCax)Cu2O8-z by Pb-doping			Grenoble Cedex, France	Physica C, 341(2000)677	A.Sin,J.L.Tholence,P.Bordet,P.Odier,P.Toulemonde		
33299	SSC1030215	Li-intercalated sample shows s/c. Li-content not known. Tc(max) for 2 month intercalating.	KCa2Nb3O10	K1Ca2Nb3O10	K	1	Ca	2	Nb	3															O	10			1997																																																1					1																																																																																														K2CO3,CaCO3,La2O3,Nb2O5		heat(1150C, in air)					Superconducting properties of layered perovskite KCa2Nb3O10 and KLaNb2O7			ISSP, University of Tokyo, Roppongi,Minato-ku, Japan	Solid State Commun., 103(1997)215	N.Mori,S.Ogawa,S.Takayanagi,T.Yamadaya,Y.Takano		
33300	SSC1030215	not s/c for 3 weeks intercalation of Li.  Li-content not known.	KLaNb2O7	K1La1Nb2O7	K	1	La	1	Nb	2															O	7			1997																																																			0.5																																																																																																K2CO3,CaCO3,La2O3,Nb2O5		heat(1150C, in air)					Superconducting properties of layered perovskite KCa2Nb3O10 and KLaNb2O7			ISSP, University of Tokyo, Roppongi,Minato-ku, Japan	Solid State Commun., 103(1997)215	N.Mori,S.Ogawa,S.Takayanagi,T.Yamadaya,Y.Takano		
33301	PRL0711899	Hirr = A*(Tc/T - 1) for near Tc. anisotropy factor = 370.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	1993																												Bi2212																		K				89.7			89.7										87																								HIR33301																																																														single crystals were grown from the melt in temperature gradient.					Irreversibility line of monocrystalline Bi2Sr2CaCu2O8: Experimental evidence for a dimensional crossover of the vorterx ensemble			Laboratorium fur Festkoperphysik, Eidgenosische Technische Hochschule Honggerberg, 8093 Zurich, Switzerland	Phys.Rev.Lett., 71(1993)1899	A.Schilling,H.R.Ott,J.D.Guo,R.Jin		
33302	PR06014617	penet<ab> derived from muon-SR of poly sample. carrier p=0.075(under-doped)	HgBa2CuO4+z	Hg1Ba2Cu1O4.1	Hg	1	Ba	2	Cu	1															O	4+Z	4.1	1	1999																												Hg1201																		K				60			60																																									um	muon-SR		0.194																																																				controlled solid-vapor reaction					Effects of carrier concentration on the superfluid density of high-Tc cuprates			IRC in Superconductivity, University of Cambridge, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 60(1999)14617	B.D.Rainford,C.Panagopoulos,C.W.Chu,J.Betouras,J.L.Tallon,J.R.Cooper,J.W.Loram,W.Lo,Y.S.Wang		
33303	PR06014617	penet<ab> derived from muon-SR of poly sample. carrier p=0.22 (over-doped)	HgBa2CuO4+z	Hg1Ba2Cu1O4.37	Hg	1	Ba	2	Cu	1															O	4+Z	4.37	1	1999																												Hg1201																		K				35			35																																									um	muon-SR		0.148																																																				controlled solid-vapor reaction					Effects of carrier concentration on the superfluid density of high-Tc cuprates			IRC in Superconductivity, University of Cambridge, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 60(1999)14617	B.D.Rainford,C.Panagopoulos,C.W.Chu,J.Betouras,J.L.Tallon,J.R.Cooper,J.W.Loram,W.Lo,Y.S.Wang		
33304	PRL0792320	>95% Hg1201. c-axis aligned grains(ave. size = 4 micron). anisotropy = 7.95.	HgBa2CuO4	Hg1Ba2Cu1O4+Z	Hg	1	Ba	2	Cu	1															O	4+Z			1997																												Hg1201																		K				93			93																																									um	ac-susceptibility		0.171	1.36																																																			single step technique					Probing the Order Parameter and the c-Axis Coupling of High-Tc Cuprates by Penetration Depth Measurements			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.Lett., 79(1997)2320	C.Panagopoulos,G.B.Peacock,I.Gameson,J.R.Cooper,P.P.Edwards,T.Xiang		
33305	PRL0792320	>90% Hg1223. c-axis aligned grains(ave. size = 10 micron). anisotropy = 34.5	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z			1997																												Hg1223																		K				134.5			134.5																																									um	ac-susceptibility		0.177	6.1																																																			single step technique					Probing the Order Parameter and the c-Axis Coupling of High-Tc Cuprates by Penetration Depth Measurements			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.Lett., 79(1997)2320	C.Panagopoulos,G.B.Peacock,I.Gameson,J.R.Cooper,P.P.Edwards,T.Xiang		
33306	PRL0792320		YBa2Cu3O7-z	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7-z	7		1997																												Y123																		K				92			92																																									um	ac-susceptibility			1.26																																																			fully oxygenated, ANN(380C, 24h, in O2) - slow cool to RT					Probing the Order Parameter and the c-Axis Coupling of High-Tc Cuprates by Penetration Depth Measurements			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.Lett., 79(1997)2320	C.Panagopoulos,G.B.Peacock,I.Gameson,J.R.Cooper,P.P.Edwards,T.Xiang		
33307	PRL0792320		YBa2Cu3O7-z	Y1Ba2Cu3O6.57	Y	1	Ba	2	Cu	3															O	7-z	6.57		1997																												Y123																		K				55			55																																									um	ac-susceptibility			7.17																																																			ANN(550C, 12h, in 0.2%O2/N2) - Q to LN2					Probing the Order Parameter and the c-Axis Coupling of High-Tc Cuprates by Penetration Depth Measurements			IRC in Superconductivity, University of Cambridge, Madingley Road, Cambridge, CB3 OHE, United Kingdom	Phys.Rev.Lett., 79(1997)2320	C.Panagopoulos,G.B.Peacock,I.Gameson,J.R.Cooper,P.P.Edwards,T.Xiang		
33308	PR04906392	thickness=3000A. gap in meV.	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		5	1994																												T'																		K		17.2					17.2																																									um	surface impedance		0.36			2.3	3.1	7																																															laser ablation in N2O atmosphere on (100)LaAlO3 substrate.					Temperature dependence of the penetration depth in Nd1.85Ce0.15CuO4-z superconducting thin films				Phys.Rev.B, 49(1994)6392	A.Andreone,A.Cassinese,A.Di Chiara,A.Gupta,E.Sarnelli,R.Vaglio		
33309	PR05000523	substrate=LaAlO3	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		5	1994																												T'																		K				21			21																																				A			72		A	surface impedance		1300				4	7																																															pulse laser deposition in N2O atmosphere on YSZ buffer layer (1000A).					Electrodynamics of Nd1.85Ce0.15CuO4: Comparison with Nb and YBa2Cu3O7-z			University of Maryland, USA	Phys.Rev.B, 50(1994)523	Dong-Ho Wu,J.L.Peng,J.Mao,R.L.Greene,S.M.Anlage,S.N.Mao,T.Venkatesan,X.X.Xi		
33310	PR05000523	substrate=Al2O3	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		5	1994																												T'																		K				21.5			21.5																																				A			80		A	surface impedance		760				4.06	7																																															pulse laser deposition in N2O atmosphere on YSZ buffer layer (1000A).					Electrodynamics of Nd1.85Ce0.15CuO4: Comparison with Nb and YBa2Cu3O7-z			University of Maryland, USA	Phys.Rev.B, 50(1994)523	Dong-Ho Wu,J.L.Peng,J.Mao,R.L.Greene,S.M.Anlage,S.N.Mao,T.Venkatesan,X.X.Xi		
33311	PR05000523		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	1994																												T'																		K				21.5			21.5																																				A			80		A	surface impedance		1250				3.9	7																																															directional solidification technique.					Electrodynamics of Nd1.85Ce0.15CuO4: Comparison with Nb and YBa2Cu3O7-z			University of Maryland, USA	Phys.Rev.B, 50(1994)523	Dong-Ho Wu,J.L.Peng,J.Mao,R.L.Greene,S.M.Anlage,S.N.Mao,T.Venkatesan,X.X.Xi		
33312	PLA2880105	ANN(650C, 6h, in O2). mechanical properties were calculated from ultrasonic velocity.	DyBaSrCu3O7	Dy1Ba1Sr1Cu3O7-z	Dy	1	Ba	1	Sr	1	Cu	3													O	7-z		1	2001									6.8			GPa		134	GPa		54	GPa		87							3	Y123			A	3.801	3.85	11.549												K	82						82																																																											448												mOhm.cm											0.29													1	solid state reaction					Elastic properties of superconducting and non-superconducting DyBaSrCu3O7-z			School of Applied Physics, Universiti Kebangsaan Malaysia, Bangi, Selangor, Malaysia	Physics Lett., A, 288(2001)105	Nor Azah Nik Jaafar,R.Abd-Shukor		
33313	PLA2880105	ANN(920C, 1h, in N2). mechanical properties were calculated from ultrasonic velocity.	DyBaSrCu3O7	Dy1Ba1Sr1Cu3O7-z	Dy	1	Ba	1	Sr	1	Cu	3													O	7-z		1	2001									6.58			GPa		110	GPa		43	GPa		78							2	Y123			A	3.836		11.614												K																																																																		402												kOhm.cm											3.37													1	solid state reaction					Elastic properties of superconducting and non-superconducting DyBaSrCu3O7-z			School of Applied Physics, Universiti Kebangsaan Malaysia, Bangi, Selangor, Malaysia	Physics Lett., A, 288(2001)105	Nor Azah Nik Jaafar,R.Abd-Shukor		
33314	P065094518	Hirr defined as Jc = 50 A/cm2.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		3	2002																												Y124																		K				78.1			78.1																																		HIR33314																																																														high pressure synthesis					Critical currents and order-disorder phase transition in the vortex states of YBa2Cu4O8 with chemically introduced disorder			Solid State Physics Laboratory ETH, CH 8093-Zurich, Switzerland	Phys.Rev.B, 65(2002)94518	A.Wisniewski,J.Karpinski,M.Angst,M.Baran,R.Puzniak,S.M.Kazakov		
33315	P065094518	Hirr defined as Jc = 50 A/cm2.	Y(Ba,Sr)2Cu4O8	Y1Ba1.8Sr0.2Cu4O8	Y	1	Ba	1.8	Sr	0.2	Cu	4													O	8		3	2002																												Y124																		K				76.5			76.5																																		HIR33315																																																														high pressure synthesis					Critical currents and order-disorder phase transition in the vortex states of YBa2Cu4O8 with chemically introduced disorder			Solid State Physics Laboratory ETH, CH 8093-Zurich, Switzerland	Phys.Rev.B, 65(2002)94518	A.Wisniewski,J.Karpinski,M.Angst,M.Baran,R.Puzniak,S.M.Kazakov		
33316	P065094518	Hirr defined as Jc = 50 A/cm2.	Y(Ba,Sr)2Cu4O8	Y1Ba1.65Sr0.35Cu4O8	Y	1	Ba	1.65	Sr	0.35	Cu	4													O	8		3	2002																												Y124																		K				80.8			80.8																																		HIR33316																																																														high pressure synthesis					Critical currents and order-disorder phase transition in the vortex states of YBa2Cu4O8 with chemically introduced disorder			Solid State Physics Laboratory ETH, CH 8093-Zurich, Switzerland	Phys.Rev.B, 65(2002)94518	A.Wisniewski,J.Karpinski,M.Angst,M.Baran,R.Puzniak,S.M.Kazakov		
33317	P065094518	Hirr defined as Jc = 50 A/cm2.	Y(Ba,Sr)2Cu4O8	Y1Ba1.6Sr0.4Cu4O8	Y	1	Ba	1.6	Sr	0.4	Cu	4													O	8		3	2002																												Y124																		K				81.4			81.4																																		HIR33317																																																														high pressure synthesis					Critical currents and order-disorder phase transition in the vortex states of YBa2Cu4O8 with chemically introduced disorder			Solid State Physics Laboratory ETH, CH 8093-Zurich, Switzerland	Phys.Rev.B, 65(2002)94518	A.Wisniewski,J.Karpinski,M.Angst,M.Baran,R.Puzniak,S.M.Kazakov		
33318	P065094518	Hirr defined as Jc = 50 A/cm2.	Y(Ba,Sr)2Cu4O8	Y1Ba1.36Sr0.64Cu4O8	Y	1	Ba	1.36	Sr	0.64	Cu	4													O	8		3	2002																												Y124																		K				81			81																																		HIR33318																																																														high pressure synthesis					Critical currents and order-disorder phase transition in the vortex states of YBa2Cu4O8 with chemically introduced disorder			Solid State Physics Laboratory ETH, CH 8093-Zurich, Switzerland	Phys.Rev.B, 65(2002)94518	A.Wisniewski,J.Karpinski,M.Angst,M.Baran,R.Puzniak,S.M.Kazakov		
33319	P065104506		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O3.97	Sm	1.85	Ce	0.15	Cu	1															O	4-z	3.97	3	2002								5																				T'	I4/mmm		A	3.9199		11.906												K				21.8			21.8																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33320	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.75Gd0.1Ce0.15Cu1O3.97	Sm	1.75	Gd	0.1	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								4.64																				T'	I4/mmm		A	3.9191		11.899												K				21.4			21.4																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33321	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.65Gd0.2Ce0.15Cu1O3.97	Sm	1.65	Gd	0.2	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								4.41																				T'	I4/mmm		A	3.9179		11.897												K				21			21																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33322	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.55Gd0.3Ce0.15Cu1O3.97	Sm	1.55	Gd	0.3	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								4.26																				T'	I4/mmm		A	3.9167		11.889												K				20.2			20.2																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33323	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.45Gd0.4Ce0.15Cu1O3.97	Sm	1.45	Gd	0.4	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								4.18																				T'	I4/mmm		A	3.9159		11.884												K				19.2			19.2																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33324	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.35Gd0.5Ce0.15Cu1O3.97	Sm	1.35	Gd	0.5	Ce	0.15	Cu	1													O	4-z	3.97	3	2002																												T'	I4/mmm		A	3.9143		11.878												K				18.8			18.8																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33325	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.25Gd0.6Ce0.15Cu1O3.97	Sm	1.25	Gd	0.6	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								3.5																				T'	I4/mmm		A	3.9131		11.875												K				16.8			16.8																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33326	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.15Gd0.7Ce0.15Cu1O3.97	Sm	1.15	Gd	0.7	Ce	0.15	Cu	1													O	4-z	3.97	3	2002																												T'	I4/mmm		A	3.9123		11.87												K				16.8			16.8																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33327	P065104506		(Sm,Gd,Ce)2CuO4	Sm1.05Gd0.8Ce0.15Cu1O3.97	Sm	1.05	Gd	0.8	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								2.97																				T'	I4/mmm		A	3.9107		11.863												K				15			15																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33328	P065104506		(Sm,Gd,Ce)2CuO4	Sm0.85Gd1Ce0.15Cu1O3.97	Sm	0.85	Gd	1	Ce	0.15	Cu	1													O	4-z	3.97	3	2002								2.66																				T'	I4/mmm		A	3.9087		11.854												K				11.3			11.3																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33329	P065104506		(Sm,Gd,Ce)2CuO4	Sm0.75Gd1.1Ce0.15Cu1O3.97	Sm	0.75	Gd	1.1	Ce	0.15	Cu	1													O	4-z	3.97	3	2002																												T'	I4/mmm		A	3.9067		11.852												K				9.6			9.6																																																																																														R2O3,CeO2,CuO	1	mixture in Pt crucible - heat(1200-1300C)-cool to (1000-1120), 1 C/h, then ANN(950C, in flowing Ar)					Superconductivity and magnetism of Sm1.85-xGdxCe0.15CuO4-d and Gd2-yCeyCuO4-d crystals			College of Science and Engineering, Aoyama Gakuin University Chitosedai, Setagaya, Tokyo, Japan	Phys.Rev.B, 65(2002)104506	H.Samata,L.Zhang,M.D.Lan,T.Shioga,T.Taniguchi,T.Uchida,Y.Nagata		
33330	P065104523	not s/c. Curie-T in DB is for H//ab. Curie-T for H//c is 2.5K. optical conductivity, specific heat were measured.	Sr2(Ru,Ti)O4	Sr2Ru0.9Ti0.1O4	Sr	2	Ru	0.9	Ti	0.1															O	4		3	2002							-100																								A	3.8744		12.7163												K					0.3																																																																																																		single crystals were grown by floating zone method					Transport, magnetic, thermodynamic, and optical properties in Ti-doped Sr2RuO4			Experimentalphysik V, Elektronische Korrelationen und Magnetismus, Institut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)104523	A.Loidl,A.Reller,E.-W.Scheidt,F.Mayr,J.Hemberger,K.Pucher,R.Horny,R.J.Cava,S.G.Ebbinghaus,S.Horn,S.Klimm,V.Fritsch		
33331	P065104523	not s/c. Curie-T in DB is for H//ab. Curie-T for H//c is 5.8K. optical conductivity, specific heat were measured.	Sr2(Ru,Ti)O4	Sr2Ru0.8Ti0.2O4	Sr	2	Ru	0.8	Ti	0.2															O	4		3	2002							-58																								A	3.8775		12.7008												K					0.3																																																																																																		single crystals were grown by floating zone method					Transport, magnetic, thermodynamic, and optical properties in Ti-doped Sr2RuO4			Experimentalphysik V, Elektronische Korrelationen und Magnetismus, Institut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)104523	A.Loidl,A.Reller,E.-W.Scheidt,F.Mayr,J.Hemberger,K.Pucher,R.Horny,R.J.Cava,S.G.Ebbinghaus,S.Horn,S.Klimm,V.Fritsch		
33332	PHC3570393	Li-intercalated layered niobium oxide	LixRbCa2Nb3O10	Li0.34Rb1Ca2Nb3O10	Li	0.34	Rb	1	Ca	2	Nb	3													O	10		1	2001																															A	7.7206														K				3.54			3.54																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33333	PHC3570393	Li-intercalated layered niobium oxide	LixRbCa2Nb3O10	Li0.46Rb1Ca2Nb3O10	Li	0.46	Rb	1	Ca	2	Nb	3													O	10		1	2001																																														K				3.54			3.54																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33334	PHC3570393	Li-intercalated layered niobium oxide	LixRbCa2Nb3O10	Li0.62Rb1Ca2Nb3O10	Li	0.62	Rb	1	Ca	2	Nb	3													O	10		1	2001																																														K				2.71			2.71																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33335	PHC3570393	Li-intercalated layered niobium oxide. not s/c	LixRbCa2Nb3O10	Li0.17Rb1Ca2Nb3O10	Li	0.17	Rb	1	Ca	2	Nb	3													O	10		1	2001																																														K					2																																																																																																		AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33336	PHC3570393	Li-intercalated layered niobium oxide	LixRbSr2Nb3O10	Li0.34Rb1Sr2Nb3O10	Li	0.34	Rb	1	Sr	2	Nb	3													O	10		1	2001																															A	7.794														K				6.03			6.03																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33337	PHC3570393	Li-intercalated layered niobium oxide	LixKCa2Nb3O10	Li0.34K1Ca2Nb3O10	Li	0.34	K	1	Ca	2	Nb	3													O	10		1	2001																															A	7.7343														K				5.39			5.39																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33338	PHC3570393	Li-intercalated layered niobium oxide. not s/c	LixCsCa2Nb3O10	Li0.17Cs1Ca2Nb3O10	Li	0.17	Cs	1	Ca	2	Nb	3													O	10		1	2001																																														K					2																																																																																																		AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33339	PHC3570393	Li-intercalated layered niobium oxide	LixCsCa2Nb3O10	Li0.34Cs1Ca2Nb3O10	Li	0.34	Cs	1	Ca	2	Nb	3													O	10		1	2001																																7.7469														K				5.4			5.4																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33340	PHC3570393	Li-intercalated layered niobium oxide	LixCsCa2Nb3O10	Li0.46Cs1Ca2Nb3O10	Li	0.46	Cs	1	Ca	2	Nb	3													O	10		1	2001																																														K				5.31			5.31																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33341	PHC3570393	Li-intercalated layered niobium oxide	LixCsCa2Nb3O10	Li0.62Cs1Ca2Nb3O10	Li	0.62	Cs	1	Ca	2	Nb	3													O	10		1	2001																																														K				4.71			4.71																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33342	PHC3570393	Li-intercalated layered niobium oxide	LixCsCa2Nb3O10	Li0.28Cs1Ca2Nb3O10	Li	0.28	Cs	1	Ca	2	Nb	3													O	10		1	2001																																														K				5.51			5.51																																																																																																AB2Nb3O10 (A=K,Rb,Cs), (B=Ca,Sr) were prepared by solid state reaction, then Li-intercalation by three electrode cell.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
33343	P065104505	ANN(400C,in vac). hole conc  p=0.052.	HgBa2CuOz	Hg1Ba2Cu1O4.032	Hg	1	Ba	2	Cu	1															O	4+z	4.032	1	2002																												Hg1201																		K				36			36																																																																		uV/K	84.9			TP33343																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33344	P065104505	ANN(350C,in vac). hole conc  p=0.062.	HgBa2CuOz	Hg1Ba2Cu1O4.033	Hg	1	Ba	2	Cu	1															O	4+z	4.033	1	2002																												Hg1201																		K				48			48																																																																		uV/K	66.3			TP33344																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33345	P065104505	ANN(450C,in Ar). hole conc  p=0.082.	HgBa2CuOz	Hg1Ba2Cu1O4.043	Hg	1	Ba	2	Cu	1															O	4+z	4.043	1	2002																												Hg1201																		K				72			72																																																																		uV/K	29.2			TP33345																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33346	P065104505	ANN(300C,in Ar). hole conc  p=0.103.	HgBa2CuOz	Hg1Ba2Cu1O4.052	Hg	1	Ba	2	Cu	1															O	4+z	4.052	1	2002																												Hg1201																		K				82			82																																																																		uV/K	13.3			TP33346																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33347	P065104505	ANN(300C,in 0.01 %O2). hole conc  p=0.123.	HgBa2CuOz	Hg1Ba2Cu1O4.058	Hg	1	Ba	2	Cu	1															O	4+z	4.058	1	2002																												Hg1201																		K				89			89																																																																		uV/K	7.2			TP33347																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33348	P065104505	ANN(00C,in 100 %O2). hole conc  p=0.132.	HgBa2CuOz	Hg1Ba2Cu1O4.047	Hg	1	Ba	2	Cu	1															O	4+z	4.047	1	2002																												Hg1201																		K				95			95																																																																		uV/K	4.3			TP33348																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33349	P065104505	ANN(300C,in 5 atm O2). hole conc  p=0.168.	HgBa2CuOz	Hg1Ba2Cu1O4.081	Hg	1	Ba	2	Cu	1															O	4+z	4.081	1	2002																												Hg1201																		K				98			98																																																																		uV/K	0.6			TP33349																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(930C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33350	P065104505	ANN(400C,in vac). hole conc  p=0.052.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.032	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.032	1	2002																												Hg1201																		K					2																																																																				uV/K	79.4			TP33350																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33351	P065104505	ANN(350C,in vac). hole conc  p=0.061.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.027	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.027	1	2002																												Hg1201																		K				28			28																																																																		uV/K	66.6			TP33351																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33352	P065104505	ANN(450C,in Ar). hole conc  p=0.086.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.043	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.043	1	2002																												Hg1201																		K				53			53																																																																		uV/K	25.9			TP33352																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33353	P065104505	ANN(300C,in Ar). hole conc  p=0.107.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.052	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.052	1	2002																												Hg1201																		K				69			69																																																																		uV/K	12.3			TP33353																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33354	P065104505	ANN(300C,in 0.01 %O2). hole conc  p=0.118.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.063	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.063	1	2002																												Hg1201																		K				75			75																																																																		uV/K	7.5			TP33354																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33355	P065104505	ANN(00C,in 100 %O2). hole conc  p=0.141.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.073	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.073	1	2002																												Hg1201																		K				82			82																																																																		uV/K	3.4			TP33355																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33356	P065104505	ANN(300C,in 5 atm O2). hole conc  p=0.153.	HgBa2(Cu,Zn)Oz	Hg1Ba2Cu0.97Zn0.03O4.081	Hg	1	Ba	2	Cu	0.97	Zn	0.03													O	4+z	4.081	1	2002																												Hg1201																		K				83			83																																																																		uV/K	2			TP33356																								HgO,BaO,CuO,ZnO	1	mixture - sealed in quartz - heat(850C, 20h) - Q to water - small pieces - ANN					Effects of Zn substitution on the superconductivity and pseudogap in HgBa2CuO4+d with various doping levels			Superconductivity Research Laboratory, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo , Japan	Phys.Rev.B, 65(2002)104505	A.Miyakita,A.Yamamoto,K.Minami,M.Izumi,S.Tajima,W.-Z.Hu		
33357	SSC1030215	4 weeks Li-intercalation. Li-content not known. 	LixKCa2Nb3O10	K1Ca2Nb3O10	K	1	Ca	2	Nb	3															O	10			1997																																														K				1			1																																																																																																Li-intercalation using the n-butyl Li n-hexane solution.					Superconducting properties of layered perovskite KCa2Nb3O10 and KLaNb2O7			ISSP, University of Tokyo, Roppongi,Minato-ku, Japan	Solid State Commun., 103(1997)215	N.Mori,S.Ogawa,S.Takayanagi,T.Yamadaya,Y.Takano		
33358	SSC1030215	5 weeks Li-intercalation sample shows no s/c. Li-content not known. 	LixKLaNb2O7	K1La1Nb2O7	K	1	La	1	Nb	2															O	7			1997																																														K					0.5																																																																																																		Li-intercalation using the n-butyl Li n-hexane solution.					Superconducting properties of layered perovskite KCa2Nb3O10 and KLaNb2O7			ISSP, University of Tokyo, Roppongi,Minato-ku, Japan	Solid State Commun., 103(1997)215	N.Mori,S.Ogawa,S.Takayanagi,T.Yamadaya,Y.Takano		
33359	PHC3570256	CDW,SDW measured by NED. LTO-to-LTT transition temperature=37.2 K.	(La,Ba,Sr)2CuO4	La1.875Ba0.075Sr0.05Cu1O4	La	1.875	Ba	0.075	Sr	0.05	Cu	1													O	4		3	2001																												T																		K		9.6					9.6																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33360	PHC3570256	CDW,SDW measured by NED. LTO-to-LTT transition temperature=35 K.	(La,Ba,Sr)2CuO4	La1.875Ba0.065Sr0.06Cu1O4	La	1.875	Ba	0.065	Sr	0.06	Cu	1													O	4		3	2001																												T			A	3.7842		13.2584												K		10.4					10.4																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33361	PHC3570256	CDW,SDW measured by NED. LTO-to-LTT transition temperature=31.5 K.	(La,Ba,Sr)2CuO4	La1.875Ba0.05Sr0.075Cu1O4	La	1.875	Ba	0.05	Sr	0.075	Cu	1													O	4		3	2001																												T			A	3.7847		13.2555												K		13.5					13.5																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33362	PHC3570256	CDW,SDW measured by NED. LTO-to-LTT transition temperature=30.2 K.	(La,Ba,Sr)2CuO4	La1.875Ba0.04Sr0.085Cu1O4	La	1.875	Ba	0.04	Sr	0.085	Cu	1													O	4		3	2001																												T			A	3.7834		13.2503												K		31.7					31.7																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33363	PHC3570256	CDW,SDW measured by NED. 	(La,Ba,Sr)2CuO4	La1.875Ba0.025Sr0.1Cu1O4	La	1.875	Ba	0.025	Sr	0.1	Cu	1													O	4		3	2001																												T			A	3.7823		13.2423												K		30.2					30.2																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33364	PHC3570256	CDW,SDW measured by NED. 	(La,Ba,Sr)2CuO4	La1.875Ba0.005Sr0.12Cu1O4	La	1.875	Ba	0.005	Sr	0.12	Cu	1													O	4		3	2001																												T																		K		31.1					31.1																																																																																																Traveling-solvent floating zone method					Effect of structural symmetry on the magnetic and superconducting properties in La1.875Ba0.125-xSrxCuO4			Institute for Chemical Research, Kyoto University, Gokasho, Uji, Japan	Physica C, 357-360(2001)256	H.Goka,K.Yamada,M.Fujita,Y.Ikeda		
33365	PHC3570039	Hirr for H//c.	YBa2Cu3O7-z	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2001																												Y123																		K		93					93																																		HIR33365																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33366	PHC3570039	Hirr for H//c.	YBa2Cu3O7-z	Y1Ba2Cu3O6.6	Y	1	Ba	2	Cu	3															O	7-z	6.6	3	2001																												Y123																		K		58.2					58.2																																		HIR33366																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33367	PHC3570039	Hirr for H//c.	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.97Ni0.03O7-z	Y	1	Ba	2	Cu	2.97	Ni	0.03													O	7-z		3	2001																												Y123																		K		87					87																																		HIR33367																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33368	PHC3570039	Hirr for H//c.	YBa2(Cu,Ni)3O7	Y1Ba2Cu2.91Ni0.09O7-z	Y	1	Ba	2	Cu	2.91	Ni	0.09													O	7-z		3	2001																												Y123																		K		76					76																																		HIR33368																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33369	PHC3570039	Hirr for H//c.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.988Zn0.012O7-z	Y	1	Ba	2	Cu	2.988	Zn	0.012													O	7-z		3	2001																												Y123																		K		85					85																																		HIR33369																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33370	PHC3570039	Hirr for H//c.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.982Zn0.018O7-z	Y	1	Ba	2	Cu	2.982	Zn	0.018													O	7-z		3	2001																												Y123																		K		82					82																																		HIR33370																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33371	PHC3570039	Hirr for H//c.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.91Zn0.09O7-z	Y	1	Ba	2	Cu	2.91	Zn	0.09													O	7-z		3	2001																												Y123																		K		55					55																																		HIR33371																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33372	PHC3570039	Hirr for H//c.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.988Zn0.012O6.75	Y	1	Ba	2	Cu	2.988	Zn	0.012													O	7-z	6.75	3	2001																												Y123																		K		62					62																																		HIR33372																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33373	PHC3570039	Hirr for H//c.	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.982Zn0.018O6.75	Y	1	Ba	2	Cu	2.982	Zn	0.018													O	7-z	6.75	3	2001																												Y123																		K		57.8					57.8																																		HIR33373																																																														Single crystals were grown by a pulling method. ANN in O2-flow. Q to L-N2. Impurity content by ICP.					Zn/Ni substitution effects on vortex states of underdoped YBa2Cu3Oy			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 357-360(2001)39	S.Tajima,T.Masui		
33374	PHC3570025		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			2001																												T																		K		38					38																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33375	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9975Zn0.0025O4	La	1.85	Sr	0.15	Cu	0.9975	Zn	0.0025													O	4			2001																												T																		K		34.8					34.8																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33376	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.995Zn0.005O4	La	1.85	Sr	0.15	Cu	0.995	Zn	0.005													O	4			2001																												T																		K		32.2					32.2																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33377	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9925Zn0.0075O4	La	1.85	Sr	0.15	Cu	0.9925	Zn	0.0075													O	4			2001																												T																		K		28.7					28.7																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33378	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.99Zn0.01O4	La	1.85	Sr	0.15	Cu	0.99	Zn	0.01													O	4			2001																												T																		K		26.4					26.4																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33379	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9875Zn0.0125O4	La	1.85	Sr	0.15	Cu	0.9875	Zn	0.0125													O	4			2001																												T																		K		22.3					22.3																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33380	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.985Zn0.015O4	La	1.85	Sr	0.15	Cu	0.985	Zn	0.015													O	4			2001																												T																		K		20					20																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33381	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9825Zn0.0175O4	La	1.85	Sr	0.15	Cu	0.9825	Zn	0.0175													O	4			2001																												T																		K		15					15																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33382	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.98Zn0.02O4	La	1.85	Sr	0.15	Cu	0.98	Zn	0.02													O	4			2001																												T																		K		13.7					13.7																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33383	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9775Zn0.0225O4	La	1.85	Sr	0.15	Cu	0.9775	Zn	0.0225													O	4			2001																												T																		K		8					8																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33384	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.975Zn0.025O4	La	1.85	Sr	0.15	Cu	0.975	Zn	0.025													O	4			2001																												T																		K		7.3					7.3																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33385	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.9725Zn0.0275O4	La	1.85	Sr	0.15	Cu	0.9725	Zn	0.0275													O	4			2001																												T																		K		1.2					1.2																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33386	PHC3570025		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4			2001																												T																		K		32					32																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33387	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9975Zn0.0025O4	La	1.8	Sr	0.2	Cu	0.9975	Zn	0.0025													O	4			2001																												T																		K		30.2					30.2																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33388	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9952Zn0.0048O4	La	1.8	Sr	0.2	Cu	0.9952	Zn	0.0048													O	4			2001																												T																		K		28.6					28.6																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33389	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9928Zn0.0072O4	La	1.8	Sr	0.2	Cu	0.9928	Zn	0.0072													O	4			2001																												T																		K		27					27																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33390	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.99Zn0.01O4	La	1.8	Sr	0.2	Cu	0.99	Zn	0.01													O	4			2001																												T																		K		25.6					25.6																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33391	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9883Zn0.0117O4	La	1.8	Sr	0.2	Cu	0.9883	Zn	0.0117													O	4			2001																												T																		K		23.6					23.6																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33392	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.983Zn0.017O4	La	1.8	Sr	0.2	Cu	0.983	Zn	0.017													O	4			2001																												T																		K		19.8					19.8																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33393	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.98Zn0.02O4	La	1.8	Sr	0.2	Cu	0.98	Zn	0.02													O	4			2001																												T																		K		17.7					17.7																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33394	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9777Zn0.0223O4	La	1.8	Sr	0.2	Cu	0.9777	Zn	0.0223													O	4			2001																												T																		K		15.7					15.7																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33395	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9753Zn0.0247O4	La	1.8	Sr	0.2	Cu	0.9753	Zn	0.0247													O	4			2001																												T																		K		13.7					13.7																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33396	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9727Zn0.0273O4	La	1.8	Sr	0.2	Cu	0.9727	Zn	0.0273													O	4			2001																												T																		K		11.1					11.1																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33397	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9703Zn0.0297O4	La	1.8	Sr	0.2	Cu	0.9703	Zn	0.0297													O	4			2001																												T																		K		9					9																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33398	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.9676Zn0.0324O4	La	1.8	Sr	0.2	Cu	0.9676	Zn	0.0324													O	4			2001																												T																		K		5.5					5.5																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33399	PHC3570025		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4			2001																												T																		K		26.9					26.9																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33400	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.9975Zn0.0025O4	La	1.9	Sr	0.1	Cu	0.9975	Zn	0.0025													O	4			2001																												T																		K		23.6					23.6																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33401	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.995Zn0.005O4	La	1.9	Sr	0.1	Cu	0.995	Zn	0.005													O	4			2001																												T																		K		19.1					19.1																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33402	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.9925Zn0.0075O4	La	1.9	Sr	0.1	Cu	0.9925	Zn	0.0075													O	4			2001																												T																		K		14.5					14.5																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33403	PHC3570025		(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.99Zn0.01O4	La	1.9	Sr	0.1	Cu	0.99	Zn	0.01													O	4			2001																												T																		K		8.8					8.8																																																																																																details are not shown					Zn-impurity effects on high-temperature superconductivity			School of Frontier Science, University of Tokyo, Bunkyo-ku,Tokyo,Japan	Physica C, 357-360(2001)25	S.Uchida		
33404	PHC3570230	ion radius(average) of R = 1.079. Hirr(77K)=1.25 T.	SmBa2Cu3O7	Sm1Ba2Cu3O7-z	Sm	1	Ba	2	Cu	3															O	7-z		1	2001																												Y123			A	3.85	3.9	11.71												K	92.9						92.9																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33405	PHC3570230	ion radius(average) of R = 1.066. Hirr(77K)=1.83 T.	EuBa2Cu3O7	Eu1Ba2Cu3O7-z	Eu	1	Ba	2	Cu	3															O	7-z		1	2001																												Y123			A	3.84	3.89	11.69												K	91.4						91.4																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33406	PHC3570230	ion radius(average) of R = 1.053. Hirr(77K)=4.15 T.	GdBa2Cu3O7	Gd1Ba2Cu3O6.98	Gd	1	Ba	2	Cu	3															O	7-z	6.98	1	2001																												Y123			A	3.84	3.9	11.71												K	94.2						94.2																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33407	PHC3570230	ion radius(average) of R = 1.019. Hirr(77K)=3.75 T.	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-z	6.93	1	2001																												Y123			A	3.82	3.89	11.66												K	91.4						91.4																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33408	PHC3570230	ion radius(average) of R = 0.999. Hirr(77K)=3.97 T.	(Y,Yb)Ba2Cu3O7	Y0.4Yb0.6Ba2Cu3O6.93	Y	0.4	Yb	0.6	Ba	2	Cu	3													O	7-z	6.93	1	2001																												Y123			A	3.8	3.87	11.65												K	91.1						91.1																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33409	PHC3570230	ion radius(average) of R = 0.992. Hirr(77K)=4.78 T.	(Y,Yb)Ba2Cu3O7	Y0.2Yb0.8Ba2Cu3O6.91	Y	0.2	Yb	0.8	Ba	2	Cu	3													O	7-z	6.91	1	2001																												Y123			A	3.81	3.87	11.66												K	91.4						91.4																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33410	PHC3570230	ion radius(average) of R = 0.985. Hirr(77K)=7.73 T.	YbBa2Cu3O7	Yb1Ba2Cu3O6.93	Yb	1	Ba	2	Cu	3															O	7-z	6.93	1	2001																												Y123			A	3.8	3.87	11.65												K	89.5						89.5																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33411	PHC3570230	ion radius(average) of R = 0.984. Hirr(77K)=6.83 T.	(Yb,Lu)Ba2Cu3O7	Yb0.9Lu0.1Ba2Cu3O7-z	Yb	0.9	Lu	0.1	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A	3.8	3.87	11.66												K	89.5						89.5																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33412	PHC3570230	ion radius(average) of R = 0.983. Hirr(77K)=5.45 T.	(Yb,Lu)Ba2Cu3O7	Yb0.8Lu0.2Ba2Cu3O6.94	Yb	0.8	Lu	0.2	Ba	2	Cu	3													O	7-z	6.94	1	2001																												Y123			A	3.8	3.87	11.66												K	89.9						89.9																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33413	PHC3570230	ion radius(average) of R = 0.983. Hirr(77K)=5.18 T.	(Yb,Lu)Ba2Cu3O7	Yb0.7Lu0.3Ba2Cu3O7-z	Yb	0.7	Lu	0.3	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A	3.8	3.87	11.66												K	89.7						89.7																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33414	PHC3570230	ion radius(average) of R = 0.982. Hirr(77K)=9.0 T.	(Yb,Lu)Ba2Cu3O7	Yb0.6Lu0.4Ba2Cu3O6.92	Yb	0.6	Lu	0.4	Ba	2	Cu	3													O	7-z	6.92	1	2001																												Y123			A	3.8	3.87	11.66												K	89.7						89.7																																																																																																heat(900-950C,12-120h) - ANN(350-400C,10-96h,in O2 gas)					Rare-earth-ion-size control on magnetic irreversibility field in CuBa2RECu2O7-z			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)230	H.Yamauchi,M.Karppinen,T.Nakane,Y.Yasukawa		
33415	PHC3570252		(Ba,K)BiO3	Ba0.6K0.4Bi1O3	Ba	0.6	K	0.4	Bi	1															O	3		3	2001																												BKBO			A	4.28														K				30.9			30.9																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33416	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.99Pr0.01O3	Ba	0.6	K	0.4	Bi	0.99	Pr	0.01													O	3		3	2001							2.53																					BKBO																		K				26.4			26.4																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33417	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.979Pr0.021O3	Ba	0.6	K	0.4	Bi	0.979	Pr	0.021													O	3		3	2001							2.26																					BKBO																		K				23.5			23.5																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33418	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.969Pr0.031O3	Ba	0.6	K	0.4	Bi	0.969	Pr	0.031													O	3		3	2001							0.36																					BKBO																		K				18.4			18.4																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33419	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.955Pr0.045O3	Ba	0.6	K	0.4	Bi	0.955	Pr	0.045													O	3		3	2001							-2.4																					BKBO																		K				14.4			14.4																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33420	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.933Pr0.067O3	Ba	0.6	K	0.4	Bi	0.933	Pr	0.067													O	3		3	2001							-2.6																					BKBO																		K				11.1			11.1																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33421	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.925Pr0.075O3	Ba	0.6	K	0.4	Bi	0.925	Pr	0.075													O	3		3	2001							-1.8																					BKBO																		K				4.5			4.5																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33422	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.6K0.4Bi0.918Pr0.082O3	Ba	0.6	K	0.4	Bi	0.918	Pr	0.082													O	3		3	2001							-6.1																					BKBO																		K					2																																																																																																Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33423	PHC3570252		(Ba,K)BiO3	Ba0.47K0.53Bi1O3	Ba	0.47	K	0.53	Bi	1															O	3		3	2001																												BKBO																		K				11			11																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33424	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.995Pr0.005O3	Ba	0.47	K	0.53	Bi	0.995	Pr	0.005													O	3		3	2001							1.01																					BKBO																		K				9			9																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33425	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.99Pr0.01O3	Ba	0.47	K	0.53	Bi	0.99	Pr	0.01													O	3		3	2001							1.99																					BKBO																		K				6.4			6.4																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33426	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.985Pr0.015O3	Ba	0.47	K	0.53	Bi	0.985	Pr	0.015													O	3		3	2001							1.01																					BKBO																		K				5.2			5.2																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33427	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.979Pr0.021O3	Ba	0.47	K	0.53	Bi	0.979	Pr	0.021													O	3		3	2001							-0.78																					BKBO																		K				4.5			4.5																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33428	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.972Pr0.028O3	Ba	0.47	K	0.53	Bi	0.972	Pr	0.028													O	3		3	2001							-1.1																					BKBO																		K				4			4																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33429	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.965Pr0.035O3	Ba	0.47	K	0.53	Bi	0.965	Pr	0.035													O	3		3	2001							-0.94																					BKBO																		K				2.97			2.97																																																																																														Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33430	PHC3570252		(Ba,K)(Bi,Pr)O3	Ba0.47K0.53Bi0.958Pr0.042O3	Ba	0.47	K	0.53	Bi	0.958	Pr	0.042													O	3		3	2001							-0.56																					BKBO																		K					2																																																																																																Bi2O3,Pr2O3,Ba(OH)2.8H2O, KOH		electrochemical method using Pt electrodes.					Two-step Tc suppression inPr-doped Ba1-xKxBiO3			Institute of Materials Science, University of Tsukuba, Tennoudai,Tsukuba,Ibaraki,Japan	Physica C, 357-360(2001)252	B.Prijamboedi,H.Uwe		
33431	MMM2260449	P-induced SC. s/c properties measured at p=3.5 GPa. c-axis//ladder. Hc2 defined as R(onset). Hc2//b-axis=0.7T, cohere//b = 10A.	Sr2Ca12Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2001																												LAD																		K			5		0		5																				T	R-onset		8	27										HC33431		A			120	400																																																								TSFZ method using infrared furnace under O2-gas					Anisotropy of the upper critical field of the spin-ladder Sr14-xCaxCu24O41			Institute for Solid State Physics, University of Tokyo, Kashiwa-shi, Chiba,Japan	J.Magn.Magn,Mater. 226-230(2001)449	H.Eisaki,H.Ishimoto,H.Mitamura,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Goto,T.Nakanishi		
33432	MRB0360971		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2001																												Y123			A	3.8171	3.8822	11.6734												K	85.49						85.49																																																																		uV/K	7.974			TP33432	mOhm.cm											9.24												Y2O3,BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,48h)-pellet-SIN(940C,42h)-FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33433	MRB0360971		(Y,Sm)Ba2Cu3O7	Y0.8Sm0.2Ba2Cu3O7-z	Y	0.8	Sm	0.2	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A	3.8171	3.884	11.6735												K	80						80																																																																		uV/K	7.765			TP33433	mOhm.cm											7.43												Y2O3,BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,48h)-pellet-SIN(940C,42h)-FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33434	MRB0360971		(Y,Sm)Ba2Cu3O7	Y0.6Sm0.4Ba2Cu3O7-z	Y	0.6	Sm	0.4	Ba	2	Cu	3													O	7-z		1	2001																												Y123			A	3.8171	3.8852	11.6735												K	78						78																																																																		uV/K	7.454			TP33434	mOhm.cm											5.79												Y2O3,BaCO3,Sm2O3,CuO	1	mixture-CAL(900C,48h)-pellet-SIN(940C,42h)-FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33435	PHC3070209	Y123 not detected by XRD.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			1998																												Y124																		K	64.3	68.8	74.5				68.8																																																																																																acetate-tartrate-sol-gel   method. precursor powder - CAL(800C,1h, in flowing O2) - SIN(835C) - ANN(835C, 40h, in flowing O2)					Enhancement of Tc by substituting strontium for barium in the YBa2Cu4O8 superconductor prepared by a sol-gel method	199810		Laboratory of Inorganic and Physical Chemistry, IMO, Limburgs Universitair Centrum, B-3590 Dipenbeek, Belgium	Physica.C,307(1998)209-220	A. Kareiva,A.Kareiva,C. Quaeyhaegens,C.Quaeyhaegens,D. Franco,D.Franco,G. Vanhoyland,G.Vanhoyland,J. D'Haen,J. Mullens,J. Yperman,J.D'Haen,J.Mullens,J.Yperman,L.C. Van Poucke,L.C.Van Poucke,M. D'Olieslaeger,M.D'Olieslaeger,M.K. Van Bael,M.K.Van Bael		
33436	PHC3070209	Y123 not detected by XRD.	Y(Ba,Sr)2Cu4O8	Y1Ba1.8Sr0.2Cu4O8	Y	1	Ba	1.8	Sr	0.2	Cu	4													O	8			1998																												Y124																		K	74.2	76.8	81.5				76.8																																																																																																acetate-tartrate-sol-gel   method. precursor powder - CAL(800C,1h, in flowing O2) - SIN(835C) - ANN(835C, 40h, in flowing O2)					Enhancement of Tc by substituting strontium for barium in the YBa2Cu4O8 superconductor prepared by a sol-gel method	199810		Laboratory of Inorganic and Physical Chemistry, IMO, Limburgs Universitair Centrum, B-3590 Dipenbeek, Belgium	Physica.C,307(1998)209-220	A. Kareiva,A.Kareiva,C. Quaeyhaegens,C.Quaeyhaegens,D. Franco,D.Franco,G. Vanhoyland,G.Vanhoyland,J. D'Haen,J. Mullens,J. Yperman,J.D'Haen,J.Mullens,J.Yperman,L.C. Van Poucke,L.C.Van Poucke,M. D'Olieslaeger,M.D'Olieslaeger,M.K. Van Bael,M.K.Van Bael		
33437	PHC3070209	Y123 not detected by XRD.	Y(Ba,Sr)2Cu4O8	Y1Ba1.6Sr0.4Cu4O8	Y	1	Ba	1.6	Sr	0.4	Cu	4													O	8			1998																												Y124																		K	73.4	76.6	81.8				76.6																																																																																																acetate-tartrate-sol-gel   method. precursor powder - CAL(800C,1h, in flowing O2) - SIN(835C) - ANN(835C, 40h, in flowing O2)					Enhancement of Tc by substituting strontium for barium in the YBa2Cu4O8 superconductor prepared by a sol-gel method	199810		Laboratory of Inorganic and Physical Chemistry, IMO, Limburgs Universitair Centrum, B-3590 Dipenbeek, Belgium	Physica.C,307(1998)209-220	A. Kareiva,A.Kareiva,C. Quaeyhaegens,C.Quaeyhaegens,D. Franco,D.Franco,G. Vanhoyland,G.Vanhoyland,J. D'Haen,J. Mullens,J. Yperman,J.D'Haen,J.Mullens,J.Yperman,L.C. Van Poucke,L.C.Van Poucke,M. D'Olieslaeger,M.D'Olieslaeger,M.K. Van Bael,M.K.Van Bael		
33438	PHC3070209	Y123 not detected by XRD.	Y(Ba,Sr)2Cu4O8	Y1Ba1.4Sr0.6Cu4O8	Y	1	Ba	1.4	Sr	0.6	Cu	4													O	8			1998																												Y124																		K	72.4	75.8	81				75.8																																																																																																acetate-tartrate-sol-gel   method. precursor powder - CAL(800C,1h, in flowing O2) - SIN(835C) - ANN(835C, 40h, in flowing O2)					Enhancement of Tc by substituting strontium for barium in the YBa2Cu4O8 superconductor prepared by a sol-gel method	199810		Laboratory of Inorganic and Physical Chemistry, IMO, Limburgs Universitair Centrum, B-3590 Dipenbeek, Belgium	Physica.C,307(1998)209-220	A. Kareiva,A.Kareiva,C. Quaeyhaegens,C.Quaeyhaegens,D. Franco,D.Franco,G. Vanhoyland,G.Vanhoyland,J. D'Haen,J. Mullens,J. Yperman,J.D'Haen,J.Mullens,J.Yperman,L.C. Van Poucke,L.C.Van Poucke,M. D'Olieslaeger,M.D'Olieslaeger,M.K. Van Bael,M.K.Van Bael		
33439	ECS0210399	impurity phase=Y123,Y211	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K			79				79																																																																																																aqueous sol-gel method in 1 atm O2, CAL820C,10h in flowing O2) - ANN(820C, 10h, in flowing O2)					Sol-Gel preparation and characterization of manganese-substituted superconducting YBa2(Cu1-xMnx)4O8 compounds			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-2006 Vilnius, Lithuania	J.Euro.Ceramics Soc., 21(2001)399	A.Baranauskas,A.Kareiva,D.Jasaitis,H.P.Beck,R.Haberkorn		
33440	ECS0210399	impurity phase=Y123,Y247, CuO	YBa2(Cu,Mn)4O8	Y1Ba2Cu3.96Mn0.04O8	Y	1	Ba	2	Cu	3.96	Mn	0.04													O	8		1	2001																												Y124																		K			62.8				62.8																																																																																																aqueous sol-gel method in 1 atm O2, CAL820C,10h in flowing O2) - ANN(820C, 10h, in flowing O2)					Sol-Gel preparation and characterization of manganese-substituted superconducting YBa2(Cu1-xMnx)4O8 compounds			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-2006 Vilnius, Lithuania	J.Euro.Ceramics Soc., 21(2001)399	A.Baranauskas,A.Kareiva,D.Jasaitis,H.P.Beck,R.Haberkorn		
33441	ECS0210399	impurity phase=Y123,Y247, BaCuO2,CuO	YBa2(Cu,Mn)4O8	Y1Ba2Cu3.92Mn0.08O8	Y	1	Ba	2	Cu	3.92	Mn	0.08													O	8		1	2001																												Y124																		K			41.6				41.6																																																																																																aqueous sol-gel method in 1 atm O2, CAL820C,10h in flowing O2) - ANN(820C, 10h, in flowing O2)					Sol-Gel preparation and characterization of manganese-substituted superconducting YBa2(Cu1-xMnx)4O8 compounds			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-2006 Vilnius, Lithuania	J.Euro.Ceramics Soc., 21(2001)399	A.Baranauskas,A.Kareiva,D.Jasaitis,H.P.Beck,R.Haberkorn		
33442	ECS0210399	not s/c, semicon-like. Y123+Y247. impurity phase=Y211, Y2Cu2O5,BaCuO2,CuO	YBa2(Cu,Mn)4O8	Y1Ba2Cu3.88Mn0.12O8	Y	1	Ba	2	Cu	3.88	Mn	0.12													O	8		2	2001																												Y123																		K																																																																																																							aqueous sol-gel method in 1 atm O2, CAL820C,10h in flowing O2) - ANN(820C, 10h, in flowing O2)					Sol-Gel preparation and characterization of manganese-substituted superconducting YBa2(Cu1-xMnx)4O8 compounds			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-2006 Vilnius, Lithuania	J.Euro.Ceramics Soc., 21(2001)399	A.Baranauskas,A.Kareiva,D.Jasaitis,H.P.Beck,R.Haberkorn		
33443	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.201	La(Ba,Sr)2Cu3O7	La1Ba1.5Sr0.5Cu3O6.902	La	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.902	1	2001																												Y123			A	3.9047		11.758												K		54					54																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33444	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.192	(La,Pr)(Ba,Sr)2Cu3O7	La0.9Pr0.1Ba1.5Sr0.5Cu3O6.904	La	0.9	Pr	0.1	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.904	1	2001																												Y123			A	3.9042		11.716												K		44					44																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33445	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.183	(La,Pr)(Ba,Sr)2Cu3O7	La0.8Pr0.2Ba1.5Sr0.5Cu3O6.906	La	0.8	Pr	0.2	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.906	1	2001																												Y123			A	3.9038		11.714												K		24					24																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33446	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.175	(La,Pr)(Ba,Sr)2Cu3O7	La0.7Pr0.3Ba1.5Sr0.5Cu3O6.909	La	0.7	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.909	1	2001																												Y123			A	3.9038		11.695												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33447	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.165	(La,Pr)(Ba,Sr)2Cu3O7	La0.6Pr0.4Ba1.5Sr0.5Cu3O6.91	La	0.6	Pr	0.4	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.91	1	2001																												Y123			A	3.899		11.7												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33448	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.158	(La,Pr)(Ba,Sr)2Cu3O7	La0.5Pr0.5Ba1.5Sr0.5Cu3O6.916	La	0.5	Pr	0.5	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.916	1	2001																												Y123			A	3.8979		11.673												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33449	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.161	(La,Pr)(Ba,Sr)2Cu3O7	La0.4Pr0.6Ba1.5Sr0.5Cu3O6.941	La	0.4	Pr	0.6	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.941	1	2001																												Y123			A	3.8888		11.666												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33450	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.153	(La,Pr)(Ba,Sr)2Cu3O7	La0.3Pr0.7Ba1.5Sr0.5Cu3O6.945	La	0.3	Pr	0.7	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.945	1	2001																												Y123			A	3.8869		11.67												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33451	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.157	(La,Pr)(Ba,Sr)2Cu3O7	La0.2Pr0.8Ba1.5Sr0.5Cu3O6.974	La	0.2	Pr	0.8	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.974	1	2001																												Y123			A	3.8857		11.65												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33452	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.150	(La,Pr)(Ba,Sr)2Cu3O7	La0.1Pr0.9Ba1.5Sr0.5Cu3O6.98	La	0.1	Pr	0.9	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.98	1	2001																												Y123			A	3.8841		11.649												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33453	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.141	Pr(Ba,Sr)2Cu3O7	Pr1Ba1.5Sr0.5Cu3O6.982	Pr	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z	6.982	1	2001																												Y123			A	3.8825		11.65												K					10																																																																																																	1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33454	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.214	(La,Ca)(Ba,Sr)2Cu3O7	La0.95Ca0.05Ba1.5Sr0.5Cu3O6.878	La	0.95	Ca	0.05	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.878	1	2001																												Y123			A	3.8987		11.763												K		66					66																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33455	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.224	(La,Ca)(Ba,Sr)2Cu3O7	La0.9Ca0.1Ba1.5Sr0.5Cu3O6.847	La	0.9	Ca	0.1	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.847	1	2001																												Y123			A	3.8979		11.742												K		68					68																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33456	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.235	(La,Ca)(Ba,Sr)2Cu3O7	La0.85Ca0.15Ba1.5Sr0.5Cu3O6.819	La	0.85	Ca	0.15	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.819	1	2001																												Y123			A	3.8969		11.729												K		71					71																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33457	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.247	(La,Ca)(Ba,Sr)2Cu3O7	La0.8Ca0.2Ba1.5Sr0.5Cu3O6.794	La	0.8	Ca	0.2	Ba	1.5	Sr	0.5	Cu	3											O	7-z	6.794	1	2001																												Y123			A	3.8966		11.686												K		73					73																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33458	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.198	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.85Ca0.05Pr0.1Ba1.5Sr0.5Cu3O6.865	La	0.85	Ca	0.05	Pr	0.1	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.865	1	2001																												Y123			A	3.8971		11.789												K		50					50																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33459	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.218	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.8Ca0.1Pr0.1Ba1.5Sr0.5Cu3O6.856	La	0.8	Ca	0.1	Pr	0.1	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.856	1	2001																												Y123			A	3.9054		11.723												K		56					56																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33460	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.238	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.75Ca0.15Pr0.1Ba1.5Sr0.5Cu3O6.845	La	0.75	Ca	0.15	Pr	0.1	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.845	1	2001																												Y123			A	3.9045		11.718												K		62					62																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33461	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.245	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.7Ca0.2Pr0.1Ba1.5Sr0.5Cu3O6.809	La	0.7	Ca	0.2	Pr	0.1	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.809	1	2001																												Y123			A	3.9036		11.708												K		63					63																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33462	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.198	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.75Ca0.05Pr0.2Ba1.5Sr0.5Cu3O6.886	La	0.75	Ca	0.05	Pr	0.2	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.886	1	2001																												Y123			A	3.8971		11.698												K		33					33																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33463	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.211	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.7Ca0.1Pr0.2Ba1.5Sr0.5Cu3O6.862	La	0.7	Ca	0.1	Pr	0.2	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.862	1	2001																												Y123			A	3.8962		11.688												K		40					40																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33464	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.225	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.65Ca0.15Pr0.2Ba1.5Sr0.5Cu3O6.84	La	0.65	Ca	0.15	Pr	0.2	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.84	1	2001																												Y123			A	3.8905		11.677												K		45					45																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33465	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.235	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.6Ca0.2Pr0.2Ba1.5Sr0.5Cu3O6.809	La	0.6	Ca	0.2	Pr	0.2	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.809	1	2001																												Y123			A	3.8885		11.665												K		47					47																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33466	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.193	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.65Ca0.05Pr0.3Ba1.5Sr0.5Cu3O6.896	La	0.65	Ca	0.05	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.896	1	2001																												Y123			A	3.8941		11.69												K		14					14																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33467	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.206	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.6Ca0.1Pr0.3Ba1.5Sr0.5Cu3O6.872	La	0.6	Ca	0.1	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.872	1	2001																												Y123			A	3.8927		11.679												K		26					26																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33468	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.221	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.55Ca0.15Pr0.3Ba1.5Sr0.5Cu3O6.851	La	0.55	Ca	0.15	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.851	1	2001																												Y123			A	3.8907		11.675												K		27					27																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33469	PHC3640575	Oxygen content by iodometry. hole conc p<sh>=0.235	(La,Ca,Pr)(Ba,Sr)2Cu3O7	La0.5Ca0.2Pr0.3Ba1.5Sr0.5Cu3O6.829	La	0.5	Ca	0.2	Pr	0.3	Ba	1.5	Sr	0.5	Cu	3									O	7-z	6.829	1	2001																												Y123			A	3.8838		11.66												K		34					34																																																																																															1	mixture - CAL(950C,18h) - pellet - SIN(950C, 16h) - cool to 400C(100C/h) in flowing N2 - ANN(400C, 12h, in flowing O2). For Ca sample, CAL(930C)					Correlation of Tc with compositions in the (La1-x-zCaxPrz)(Ba1.5Sr0.5)Cu3Oy superconducting series			Department of Chemistry, Tamkang University, Tamsui,Taiwan,ROC	Physica C, 364-365(2001)575	C.H.Lin,H.-C.I.Kao		
33470	PHC3690236	Josephson plasma resonance was measured. Heavili underdoped sample. Anisotropy=740	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212																		K		69.4					69.4																																									um	microwave absorption		0.31	229																																																			TSFZ method					Josephson plasma resonance in underdoped Bi2Sr2CaCu2O8+d crystals			Laboratoire des Solides Irradiees,,Ecole Polytechnique, Palaiseau,France	Physica C, 369(2002)236	C.J.van der Beek,M.B.Gaifullin,M.Konczykowski,Ming Li,P.Gierlowski,P.H.Kes,S.Colson,Y.Matsuda		
33471	PHC3660283	not s/c.	Pb3Sr2Cu3O8Cl	Pb3Sr2Cu3Cl1O8	Pb	3	Sr	2	Cu	3	Cl	1													O	8		1	2002																															A	5.44	5.492	19.49												K					4.2																																																																																																PbO,SrO2,CuO,PbBr2,PbCl2		mixture-heat(765C,12h in flowing N2/O2=99/1 gas)-slow cool(100C/h) to RT-heat(750C,12h)-ANN(400C,8h in flowing N2/O2=99/1 gas)					Synthesis, characterisation and crystal chemistry of Pb3Sr3Cu3O8Br: a new layered copper oxide-bromide			London &Scandinavian Metallurgical Co.Ltd,Fullerton Road,Rotherham,South Yorkshire S60 1DL,UK	Physica C, 366(2002)283	Joseph A.Hriljac,Neil C.Hyatt		
33472	PHC3660283	not s/c.	Pb3Sr2Cu3O8(Cl,Br)	Pb3Sr2Cu3Cl0.75Br0.25O8	Pb	3	Sr	2	Cu	3	Cl	0.75	Br	0.25											O	8		1	2002																															A	5.447	5.494	19.562												K					4.2																																																																																																PbO,SrO2,CuO,PbBr2,PbCl2		mixture-heat(765C,12h in flowing N2/O2=99/1 gas)-slow cool(100C/h) to RT-heat(750C,12h)-ANN(400C,8h in flowing N2/O2=99/1 gas)					Synthesis, characterisation and crystal chemistry of Pb3Sr3Cu3O8Br: a new layered copper oxide-bromide			London &Scandinavian Metallurgical Co.Ltd,Fullerton Road,Rotherham,South Yorkshire S60 1DL,UK	Physica C, 366(2002)283	Joseph A.Hriljac,Neil C.Hyatt		
33473	PHC3660283	not s/c.	Pb3Sr2Cu3O8(Cl,Br)	Pb3Sr2Cu3Cl0.5Br0.5O8	Pb	3	Sr	2	Cu	3	Cl	0.5	Br	0.5											O	8		1	2002																															A	5.452	5.495	19.624												K					4.2																																																																																																PbO,SrO2,CuO,PbBr2,PbCl2		mixture-heat(765C,12h in flowing N2/O2=99/1 gas)-slow cool(100C/h) to RT-heat(750C,12h)-ANN(400C,8h in flowing N2/O2=99/1 gas)					Synthesis, characterisation and crystal chemistry of Pb3Sr3Cu3O8Br: a new layered copper oxide-bromide			London &Scandinavian Metallurgical Co.Ltd,Fullerton Road,Rotherham,South Yorkshire S60 1DL,UK	Physica C, 366(2002)283	Joseph A.Hriljac,Neil C.Hyatt		
33474	PHC3660283	not s/c.	Pb3Sr2Cu3O8(Cl,Br)	Pb3Sr2Cu3Cl0.25Br0.75O8	Pb	3	Sr	2	Cu	3	Cl	0.25	Br	0.75											O	8		1	2002																															A	5.457	5.497	19.698												K					4.2																																																																																																PbO,SrO2,CuO,PbBr2,PbCl2		mixture-heat(765C,12h in flowing N2/O2=99/1 gas)-slow cool(100C/h) to RT-heat(750C,12h)-ANN(400C,8h in flowing N2/O2=99/1 gas)					Synthesis, characterisation and crystal chemistry of Pb3Sr3Cu3O8Br: a new layered copper oxide-bromide			London &Scandinavian Metallurgical Co.Ltd,Fullerton Road,Rotherham,South Yorkshire S60 1DL,UK	Physica C, 366(2002)283	Joseph A.Hriljac,Neil C.Hyatt		
33475	PHC3660283	not s/c.	Pb3Sr2Cu3O8Br	Pb3Sr2Cu3Br1O8	Pb	3	Sr	2	Cu	3	Br	1													O	8		1	2002																															A	5.464	5.501	19.766												K					4.2																																																																																																PbO,SrO2,CuO,PbBr2,PbCl2		mixture-heat(765C,12h in flowing N2/O2=99/1 gas)-slow cool(100C/h) to RT-heat(750C,12h)-ANN(400C,8h in flowing N2/O2=99/1 gas)					Synthesis, characterisation and crystal chemistry of Pb3Sr3Cu3O8Br: a new layered copper oxide-bromide			London &Scandinavian Metallurgical Co.Ltd,Fullerton Road,Rotherham,South Yorkshire S60 1DL,UK	Physica C, 366(2002)283	Joseph A.Hriljac,Neil C.Hyatt		
33476	PHB2840477	antiferro-order	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.9Cu0.1O6	Sr	2	Y	1	Ru	0.9	Cu	0.1													O	6		1	2000								28																				2116	P21/n		A	5.7602	5.7795	8.1506												K	30		45				37.5																																																																																																					Magnetism and superconductivity in Sr2A(Ru1-xCux)O6 (A=Y,Ho) system			Department of Physics, Material Science Centre, National Tsing Hua University, Hsinchu, Taiwan	Physica B, 284-288(2000)477	D.C.Ling,D.Y.Chen,F.Z.Chien,M.K.Wu		
33477	PHB2840477	ferromag-order	Sr2Ho(Ru,Cu)O6	Sr2Ho1Ru0.9Cu0.1O6	Sr	2	Ho	1	Ru	0.9	Cu	0.1													O	6		1	2000							15																					2116																		K	20		40				30																																																																																																					Magnetism and superconductivity in Sr2A(Ru1-xCux)O6 (A=Y,Ho) system			Department of Physics, Material Science Centre, National Tsing Hua University, Hsinchu, Taiwan	Physica B, 284-288(2000)477	D.C.Ling,D.Y.Chen,F.Z.Chien,M.K.Wu		
33478	PHC3640392	spin glass temp.=29K(Cu-ion). Antiferro-(Ru-ion). muon-SR measurements.	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.9Cu0.1O6	Sr	2	Y	1	Ru	0.9	Cu	0.1													O	6			2001								23																				2116																		K			45				45																																																																																																solid state reaction					Superconductivity and magnetism in Sr2Y(Ru1-uCuu)O6 and in Ba2Gd(Ru1-uCuu)O6			Department of Physics, Arizona State University, Tempe,AZ, USA	Physica C, 364-365(2001)392	A.J.Greer,C.E.Stronach,D.B.Pulling,D.R.Harshman,D.R.Noakes,E.Koster,F.Z.Chien,H.A.Blackstead,John D.Dow,M.K.Wu,W.J.Kossler		
33479	PHC3640392	Antiferro (Ru-ion)	Ba2Gd(Ru,Cu)O6	Ba2Gd1Ru0.9Cu0.1O6	Ba	2	Gd	1	Ru	0.9	Cu	0.1													O	6			2001								48																				2116																		K					4.2																																																																																																		solid state reaction					Superconductivity and magnetism in Sr2Y(Ru1-uCuu)O6 and in Ba2Gd(Ru1-uCuu)O6			Department of Physics, Arizona State University, Tempe,AZ, USA	Physica C, 364-365(2001)392	A.J.Greer,C.E.Stronach,D.B.Pulling,D.R.Harshman,D.R.Noakes,E.Koster,F.Z.Chien,H.A.Blackstead,John D.Dow,M.K.Wu,W.J.Kossler		
33480	PHC3700044	Bi:Sr:Ca:Cu:Co=1.94:1.87:0.95:1.99:0.01 by ICP	Bi2Sr2Ca(Cu,Co)2O8	Bi2.1Sr1.8Ca1Cu1.96Co0.04O8	Bi	2.1	Sr	1.8	Ca	1	Cu	1.96	Co	0.04											O	8		3	2002																												Bi2212																		K				73			73																																		HIR33480																																																														Floating zone method. ANN(500C,3d,in air)					Effects of impurities on magnetization in Bi2.12Sr1.8Ca(Cu1-xMx)2Oy (M=Co,Zn) single crystals			Department of Superconductivity,The University of Tokyo,Tokyo ,Japan	Physica C, 370(2002)44	K.Kitazawa,T.Hasegawa,X.R.Zhao		
33481	PHC3700044	Bi:Sr:Ca:Cu:Zn=1.95:1.82:1.00:1.998:0.002 by ICP	Bi2Sr2Ca(Cu,Zn)2O8	Bi2.1Sr1.8Ca1Cu1.982Zn0.018O8	Bi	2.1	Sr	1.8	Ca	1	Cu	1.982	Zn	0.018											O	8		3	2002																												Bi2212																		K				83			83																																		HIR33481																																																														Floating zone method. ANN(500C,3d,in air)					Effects of impurities on magnetization in Bi2.12Sr1.8Ca(Cu1-xMx)2Oy (M=Co,Zn) single crystals			Department of Superconductivity,The University of Tokyo,Tokyo ,Japan	Physica C, 370(2002)44	K.Kitazawa,T.Hasegawa,X.R.Zhao		
33482	PHC3700071	Gd moments order below 2.75. macroscopic s/c Tc=35 K. Mossbauer effect of Gd,Ru are measured.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2002								132																				Ru1212																		K		45					45																																																																																																solid state reaction. ANN(1060C, in flowing O2) - slow cool to 500C - Q to RT					Magnetic behavior of superconducting RuSr2GdCu2O8 studied by <155> Gd and <99> Ru Mossbauer spectroscopy and susceptibility measurements			Department of Physics,Northern Illinois University,218 Faraday Hall West,DeKalb,USA	Physica C, 370(2002)71	B.Dabrowski,C.W.Kimball,D.E.Brown,M.Maxwell,P.W.Klamut,R.Kmiec,R.Kruk		
33483	PHC3700163	M-I transition trasnsition temp.=74.4 K	(La,Sr)2(Cu,Fe)O4	La1.84Sr0.16Cu0.99Fe0.01O4	La	1.84	Sr	0.16	Cu	0.99	Fe	0.01													O	4		1	2002																												T																		K			30				30																																																																							mOhm.cm							5.5																	1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33484	PHC3700163	M-I transition trasnsition temp.=83.5 K. not s/c	(La,Sr)2(Cu,Fe)O4	La1.83Sr0.17Cu0.98Fe0.02O4	La	1.83	Sr	0.17	Cu	0.98	Fe	0.02													O	4		1	2002																												T																		K					10																																																																									mOhm.cm							8.71																	1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33485	PHC3700163	M-I transition trasnsition temp.=98.7 K. not s/c	(La,Sr)2(Cu,Fe)O4	La1.815Sr0.185Cu0.965Fe0.035O4	La	1.815	Sr	0.185	Cu	0.965	Fe	0.035													O	4		1	2002																												T																		K					10																																																																									mOhm.cm							32.34																	1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33486	PHC3700163	M-I transition trasnsition temp.=149.4 K. not s/c	(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.95Fe0.05O4	La	1.8	Sr	0.2	Cu	0.95	Fe	0.05													O	4		1	2002																												T																		K					10																																																																									mOhm.cm							426.58																	1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33487	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu1FeO4	La	1.85	Sr	0.15	Cu	1	Fe														O	4		1	2002																											2	T			A	3.7713		13.212												K			39.9				39.9																																																																							mOhm.cm							4.5				1.5													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33488	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.75Sr0.25Cu0.9Fe0.1O4	La	1.75	Sr	0.25	Cu	0.9	Fe	0.1													O	4		1	2002																											2	T			A	3.7826		13.167												K					10																																																																									mOhm.cm											6.2													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33489	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.65Sr0.35Cu0.8Fe0.2O4	La	1.65	Sr	0.35	Cu	0.8	Fe	0.2													O	4		1	2002																											2	T			A	3.7892		13.17												K					10																																																																									mOhm.cm											10.6													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33490	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.55Sr0.45Cu0.7Fe0.3O4	La	1.55	Sr	0.45	Cu	0.7	Fe	0.3													O	4		1	2002																											2	T			A	3.7974		13.105												K					10																																																																									mOhm.cm											31.9													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33491	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.45Sr0.55Cu0.6Fe0.4O4	La	1.45	Sr	0.55	Cu	0.6	Fe	0.4													O	4		1	2002																											2	T			A	3.8123		13.046												K					10																																																																									mOhm.cm											92.7													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33492	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.35Sr0.65Cu0.5Fe0.5O4	La	1.35	Sr	0.65	Cu	0.5	Fe	0.5													O	4		1	2002																											2	T			A	3.8282		13.01												K					10																																																																									mOhm.cm											170.4													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33493	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.25Sr0.75Cu0.4Fe0.6O4	La	1.25	Sr	0.75	Cu	0.4	Fe	0.6													O	4		1	2002																											2	T			A	3.8323		12.901												K					10																																																																									mOhm.cm											269													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33494	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La1.05Sr0.95Cu0.2Fe0.8O4	La	1.05	Sr	0.95	Cu	0.2	Fe	0.8													O	4		1	2002																											2	T			A	3.8533		12.844												K					10																																																																									Ohm.cm											1.187													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33495	PHC3700163	not s/c	(La,Sr)2(Cu,Fe)O4	La0.85Sr1.15Fe1O4	La	0.85	Sr	1.15	Fe	1															O	4		1	2002																											2	T			A	3.8595		12.753												K					10																																																																									Ohm.cm											14.08													1	mixture - pellet - SIN(1120 K, 24h, in air) - FC to RT					Phonon vibration and transport properties of La1.85-xSr0.15+xCu1-xFexOy			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)163	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33496	PHC3700253	magnetic order below 180 K is weak ferromagnetism	(Eu,Ce)2RuSr2Cu2O10	Eu1.5Ce0.5Ru1Sr2Cu2O10+z	Eu	1.5	Ce	0.5	Ru	1	Sr	2	Cu	2											O	10+z		1	2002							180																					Ru1222			A	3.846		28.72												K		45					45																																																																	THC33496					TP33496																								Eu2O3,CeO2,SrCO3,Ru,CuO	1	mixture-preheat(1275K, in flowing O2)-SIN(1325K,48h, in 1.1 atm O2)-FC  - reheat(1100K, 12h, in 54 atm O2)					Thermal transport in the oxygenated magnetic superconductor, Eu1.5Ce0.5RuSr2Cu2O10+z			Department of Physics,Texas A&M University,College Station,TX 77843-4242,USA	Physica C, 370(2002)253	B.D.Hennings,D.G.Naugle,I.Felner,K.D.D.Rathnayaka		
33497	PR05412014	Neel-T determined by sus(peak)	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		1	1996								295																			3	T			A	5.335	5.4148	13.1168												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33498	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.995Li0.005O4	La	2	Cu	0.995	Li	0.005															O	4		1	1996								258																				T																		K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33499	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.99Li0.01O4	La	2	Cu	0.99	Li	0.01															O	4		1	1996								221																			3	T			A	5.3331	5.4129	13.1097												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33500	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.985Li0.015O4	La	2	Cu	0.985	Li	0.015															O	4		1	1996								173																				T																		K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33501	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.98Li0.02O4	La	2	Cu	0.98	Li	0.02															O	4		1	1996								136																			3	T			A	5.3321	5.4082	13.1097												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33502	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.975Li0.025O4	La	2	Cu	0.975	Li	0.025															O	4		1	1996								91																				T																		K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33503	PR05412014	Neel-T determined by sus(peak)	La2(Cu,Li)O4	La2Cu0.97Li0.03O4	La	2	Cu	0.97	Li	0.03															O	4		1	1996								0																				T																		K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33504	PR05412014		La2(Cu,Li)O4	La2Cu0.95Li0.05O4	La	2	Cu	0.95	Li	0.05															O	4		1	1996																											3	T			A	5.3283	5.3987	13.1103												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33505	PR05412014		La2(Cu,Li)O4	La2Cu0.9Li0.1O4	La	2	Cu	0.9	Li	0.1															O	4		1	1996																											3	T			A	5.3245	5.3806	13.1123												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33506	PR05412014		La2(Cu,Li)O4	La2Cu0.8Li0.2O4	La	2	Cu	0.8	Li	0.2															O	4		1	1996																											3	T			A	5.3141	5.3388	13.1226												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33507	PR05412014		La2(Cu,Li)O4	La2Cu0.7Li0.3O4	La	2	Cu	0.7	Li	0.3															O	4		1	1996																											2	T			A	5.3093		13.1316												K					4.2																																																																																																La2O3,SrCO3,CuO,Li2CO3	1	mixture - heat(900C)					Structural, magnetic, and traansport properties of La2Cu1-xLiO4	199611		National High Magnetic Field Laboratory,Florida State University, Tallahassee, Florida 32306	Phys.Rev.B,54(1996)12014	B.C. Chakoumakos,B.C.Chakoumakos,D.P. Young,D.P.Young,E.C. Moshopoulou,E.G.Moshopoulou,J.D. Yhompson,J.D.Thompson,J.L. Sarrao,J.L.Sarrao,S.E. Nagler,S.E.Nagler,Z. Fisk,Z.Fisk		
33508	PHC3700269	not s/c. IR-shifts were measured.	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4			2002																												T			A	3.7587	3.8014	13.144												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33509	PHC3700269	not s/c. IR-shifts were measured.	La2(Cu,Li)O4	La2Cu0.9Li0.1O4	La	2	Cu	0.9	Li	0.1															O	4			2002																												T			A	3.7879	3.7905	13.163												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33511	PHC3700269	not s/c. IR-shifts were measured.	La2(Cu,Li)O4	La2Cu0.8Li0.2O4	La	2	Cu	0.8	Li	0.2															O	4			2002																												T			A	3.7824	3.7738	13.166												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33512	PHC3700269	not s/c. IR-shifts were measured.	La2(Cu,Li)O4	La2Cu0.7Li0.3O4	La	2	Cu	0.7	Li	0.3															O	4			2002																												T			A	3.7706	3.7691	13.18												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33513	PHC3700269	not s/c. IR-shifts were measured.	La2(Cu,Li)O4	La2Cu0.6Li0.4O4	La	2	Cu	0.6	Li	0.4															O	4			2002																												T			A	3.7313	3.7339	13.174												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33514	PHC3700269	not s/c. IR-shifts were measured.	La2(Cu,Li)O4	La2Cu0.5Li0.5O4	La	2	Cu	0.5	Li	0.5															O	4			2002																												T			A	3.7305		13.184												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33515	PHC3700269	IR-shifts were measured.	(La,Sr)2(Cu,Li)O4	La1.86Sr0.14Cu0.99Li0.01O4	La	1.86	Sr	0.14	Cu	0.99	Li	0.01													O	4			2002																												T			A	3.7725		13.227												K	33.7		42.8				38.25																																																																																															1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33516	PHC3700269	IR-shifts were measured.	(La,Sr)2(Cu,Li)O4	La1.87Sr0.13Cu0.98Li0.02O4	La	1.87	Sr	0.13	Cu	0.98	Li	0.02													O	4			2002																												T			A	3.774		13.217												K	25.9		39.8				32.85																																																																																															1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33517	PHC3700269	IR-shifts were measured.	(La,Sr)2(Cu,Li)O4	La1.885Sr0.115Cu0.965Li0.035O4	La	1.885	Sr	0.115	Cu	0.965	Li	0.035													O	4			2002																												T			A	3.7797		13.225												K		26.5	35.5				26.5																																																																																															1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33518	PHC3700269	IR-shifts were measured.	(La,Sr)2(Cu,Li)O4	La1.9Sr0.1Cu0.95Li0.05O4	La	1.9	Sr	0.1	Cu	0.95	Li	0.05													O	4			2002																												T			A	3.7796	3.7784	13.231												K		20	24.1				20																																																																																															1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33519	PHC3700269	not s/c. IR-shifts were measured.	(La,Sr)2(Cu,Li)O4	La1.95Sr0.05Cu0.9Li0.1O4	La	1.95	Sr	0.05	Cu	0.9	Li	0.1													O	4			2002																												T			A	3.777	3.7803	13.191												K					20																																																																																																	1	SIN(860C, in air)					Infrared spectra and transport properties of Li-doped La214 system			Structure Research Laboratory,University of Science and Technology f China,Hefei,Anhui 230026,China	Physica C, 370(2002)269	Gaojie Xu,Qirong Pu,Zejun Ding,Zengming Zhang		
33520	SSC1220189	Ruddlesden-Popper series n=2 structure (95% volume fraction. resistivity monotonically increase as lowering T	Ba2KBi2O7	Ba2K1Bi2O7	Ba	2	K	1	Bi	2															O	7			2002																															A	4.2516		21.89												K					4.2																																																																																																	1	400C in ampoule. 0.75 atm O2 atmosphere, then heated by hot furnace.					Synthesis, structure and properties of layered bismuthates: (Ba,K)3Bi2O7 and (Ba,K)2BiO4			Department of Chemistry,Moscow State University, Moscow,Russian Federation	Solid State Commun., 122(2002)189	E.V.Antipov,G.Van Tendeloo,M.L.Kovba,N.R.Khasanova,O.I.Lebedev,S.N.Putilin		
33521	SSC1190579	another two samples show no s/c. The peak at 150 K in susceptibility may due to AF.	(Fe,Cu)SrBaYCu2O7	Fe0.5Sr1Ba1Y1Cu2.5O7	Fe	0.5	Sr	1	Ba	1	Y	1	Cu	2.5											O	7		1	2001							150																					M1212	p4/mmm		A	3.844		11.53												K	40		77				58.5																																																																																														Y2O3,BaCO3,SrCO3Fe2O3,CuO	1	mixture-CAL(925C,60h,in air)-reduced (805C,40h in Ar)-oxygenate(1000C, 0.5h, 6GPa, 5 wt%KClO4)					Coexistence of magnetism and superconductivity in a new Fe-containing cuprate superconductor (Fe0.5Cu0.5)SrBaYCu2O7+z			Nastional Lab for Superconductivity, Institute of Physics, Beijing, China	Solid State Commun., 119(2001)579	C.Dong,D.N.Zheng,G.C.Che,H.Chen,H.Xiong,J.L.Shen,K.Q.Li,S.L.Jia,Y.M.Ni,Y.S.Yao,Z.A.Ren,Z.X.Zhao		
33522	P065144506	ferromagnetic order from Ru sublattice. AF order from Gd sublattice.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2002						2.7	142	2.7																				Ru1212	p4/mmm		A	3.8399		11.5766												K	31		50				40.5																																																																																															1	CAL(960C, in air)-pellet-heat(1010C, in N2)-powder-heat(1050C, in flowing O2)-SIN(1055C, 1060C)-ANN(1060C, in flowing O2)					Structural, transport, and magnetic properties of pure and La-doped RuSr2GdCu2O8			Insitut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)144506	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger,P.Mandal		
33523	P065144506	Gd-effective-M=7.94 Bohr-M and Curie-T(Gd)=-4 K were fixed.	Ru(Sr,La)2GdCu2O8	Ru1Sr1.98La0.02Gd1Cu2O8	Ru	1	Sr	1.98	La	0.02	Gd	1	Cu	2											O	8		1	2002						2.8	142																					Ru1212	p4/mmm		A	3.8397		11.5708												K	20		40				30																																																																																															1	CAL(960C, in air)-pellet-heat(1010C, in N2)-powder-heat(1050C, in flowing O2)-SIN(1055C, 1060C)-ANN(1060C, in flowing O2)					Structural, transport, and magnetic properties of pure and La-doped RuSr2GdCu2O8			Insitut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)144506	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger,P.Mandal		
33524	P065144506	Gd-effective-M=7.94 Bohr-M and Curie-T(Gd)=-4 K were fixed.	Ru(Sr,La)2GdCu2O8	Ru1Sr1.94La0.06Gd1Cu2O8	Ru	1	Sr	1.94	La	0.06	Gd	1	Cu	2											O	8		1	2002						2.8	154																					Ru1212	p4/mmm		A	3.8407		11.5662												K					4.2																																																																																																	1	CAL(960C, in air)-pellet-heat(1010C, in N2)-powder-heat(1050C, in flowing O2)-SIN(1055C, 1060C)-ANN(1060C, in flowing O2)					Structural, transport, and magnetic properties of pure and La-doped RuSr2GdCu2O8			Insitut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)144506	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger,P.Mandal		
33525	P065144506	Gd-effective-M=7.94 Bohr-M and Curie-T(Gd)=-4 K were fixed.	Ru(Sr,La)2GdCu2O8	Ru1Sr1.9La0.1Gd1Cu2O8	Ru	1	Sr	1.9	La	0.1	Gd	1	Cu	2											O	8		1	2002						2.4	180																					Ru1212	p4/mmm		A	3.8444		11.5583												K					4.2																																																																																																	1	CAL(960C, in air)-pellet-heat(1010C, in N2)-powder-heat(1050C, in flowing O2)-SIN(1055C, 1060C)-ANN(1060C, in flowing O2)					Structural, transport, and magnetic properties of pure and La-doped RuSr2GdCu2O8			Insitut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)144506	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger,P.Mandal		
33526	P065144506	Gd-effective-M=7.94 Bohr-M and Curie-T(Gd)=-4 K were fixed.	Ru(Sr,La)2GdCu2O8	Ru1Sr1.8La0.2Gd1Cu2O8	Ru	1	Sr	1.8	La	0.2	Gd	1	Cu	2											O	8		1	2002						2.4	185																					Ru1212	p4/mmm		A	3.8473		11.5657												K					4.2																																																																																																	1	CAL(960C, in air)-pellet-heat(1010C, in N2)-powder-heat(1050C, in flowing O2)-SIN(1055C, 1060C)-ANN(1060C, in flowing O2)					Structural, transport, and magnetic properties of pure and La-doped RuSr2GdCu2O8			Insitut fur Physik, Universitat Augsburg, Augsburg, Germany	Phys.Rev.B, 65(2002)144506	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger,P.Mandal		
33527	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.55Y0.45Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.55	Y	0.45	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		41.3					41.3																																																																		uV/K	19.9			TP33527																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33528	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.6Y0.4Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.6	Y	0.4	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		53.5					53.5																																																																		uV/K	12.5			TP33528																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33529	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.65Y0.35Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.65	Y	0.35	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		62.1					62.1																																																																		uV/K	7.05			TP33529																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33530	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.7Y0.3Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.7	Y	0.3	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		66.9					66.9																																																																		uV/K	5.18			TP33530																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33531	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.75Y0.25Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.75	Y	0.25	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		60.6					60.6																																																																		uV/K	5.21			TP33531																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33532	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)(Cu,Zn)2O8	Bi1.7Pb0.3Sr2Ca0.8Y0.2Cu1.94Zn0.06O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.8	Y	0.2	Cu	1.94	Zn	0.06							O	8			2001																												Bi2212																		K		54.4					54.4																																																																		uV/K	1.52			TP33532																									1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33533	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.5Y0.5Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.5	Y	0.5	Cu	2									O	8			2001																												Bi2212																		K		41.3					41.3																																																																		uV/K	25.5																												1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33534	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.6Y0.4Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.6	Y	0.4	Cu	2									O	8			2001																												Bi2212																		K		63.5					63.5																																																																		uV/K	12.5																												1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33535	PCS0620187		(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.7Pb0.3Sr2Ca0.8Y0.2Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	0.8	Y	0.2	Cu	2									O	8			2001																												Bi2212																		K		69.7					69.7																																																																		uV/K	-0.9																												1	CAL(750C, 12h, in air)-pellet-SIN(800C, 24h, in air)					Superconducting transition temperatures of R1-xPrxBa2Cu3O6+y (R=Y,Sm) and Bi1.7Pb0.3Sr2Ca1-x(Cu1-yZny)2O8+z			Department of Physics, Nasgoya University, Nagoya,Japan	J.Phys.Chem.Solids, 62(2001)187	J.Takeda,M.Ambai,M.Sato,Y.Yasui		
33536	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La2.5Gd0.5Ca1Ba3Cu7O16.539	La	2.5	Gd	0.5	Ca	1	Ba	3	Cu	7											O	z	16.539	1	2002																												3137			A	3.8708		11.6039												K	78	80	82				80																																																																							mOhm.cm											5.91											0.297	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33537	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La2.3Gd0.7Ca1Ba2.8Sr0.2Cu6.86In0.14O16.536	La	2.3	Gd	0.7	Ca	1	Ba	2.8	Sr	0.2	Cu	6.86	In	0.14							O	z	16.536	1	2002																												3137			A	3.8685		11.5867												K	69	72	76				72																																																																							mOhm.cm											6.06											0.276	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33538	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La2.1Gd0.9Ca1Ba2.6Sr0.4Cu6.72In0.28O16.54	La	2.1	Gd	0.9	Ca	1	Ba	2.6	Sr	0.4	Cu	6.72	In	0.28							O	z	16.54	1	2002																												3137			A	3.8641		11.5798												K	60	65	70				65																																																																							mOhm.cm											6.5											0.257	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33539	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La1.9Gd1.1Ca1Ba2.4Sr0.6Cu6.58In0.42O16.554	La	1.9	Gd	1.1	Ca	1	Ba	2.4	Sr	0.6	Cu	6.58	In	0.42							O	z	16.554	1	2002																												3137			A	3.8586		11.57												K	54	58	63				58																																																																							mOhm.cm											7.21											0.241	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33540	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La1.7Gd1.3Ca1Ba2.2Sr0.8Cu6.44In0.56O16.6	La	1.7	Gd	1.3	Ca	1	Ba	2.2	Sr	0.8	Cu	6.44	In	0.56							O	z	16.6	1	2002																												3137			A	3.8709		11.596												K	21	30	50				30																																																																							mOhm.cm											28.8											0.234	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33541	PHC3710315		(La,Gd)3Ca(Ba,Sr)3(Cu,In)7Oz	La1.5Gd1.5Ca1Ba2Sr1Cu6.3In0.7O16.62	La	1.5	Gd	1.5	Ca	1	Ba	2	Sr	1	Cu	6.3	In	0.7							O	z	16.62	1	2002																												3137			A	3.8861		11.6192												K					10																																																																									mOhm.cm											98.1											0.22	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33542	PHC3710315		(La,Gd)3Ca(Ba2Sr)(Cu,In)7Oz	La1.5Gd1.5Ca1Ba2Sr1Cu6.3In0.7Oz	La	1.5	Gd	1.5	Ca	1	Ba	2	Sr	1	Cu	6.3	In	0.7							O	z		1	2002																												3137			A	3.886		11.6189												K					10																																																																									mOhm.cm											98.1											0.22	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33543	PHC3710315		(La,Ca,Gd)3Ca(Ba2Sr)(Cu,In)7Oz	La1.3Gd1.5Ca1.2Ba2Sr1Cu6.3In0.7Oz	La	1.3	Gd	1.5	Ca	1.2	Ba	2	Sr	1	Cu	6.3	In	0.7							O	z		1	2002																												3137			A	3.872		11.5773												K	52	56	68.5				56																																																																							mOhm.cm											41											0.23	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33544	PHC3710315		(La,Ca,Gd)3Ca(Ba2Sr)(Cu,In)7Oz	La1.1Gd1.5Ca1.4Ba2Sr1Cu6.3In0.7Oz	La	1.1	Gd	1.5	Ca	1.4	Ba	2	Sr	1	Cu	6.3	In	0.7							O	z		1	2002																												3137			A	3.8701		11.5655												K	56.5	63	70.5				63																																																																							mOhm.cm											26.6											0.263	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33545	PHC3710315		(La,Ca,Gd)3Ca(Ba2Sr)(Cu,In)7Oz	La0.9Ga1.5Ca1.6Ba2Sr1Cu6.3In0.7Oz	La	0.9	Ga	1.5	Ca	1.6	Ba	2	Sr	1	Cu	6.3	In	0.7							O	z		1	2002																												3137			A	3.8698		11.5645												K	60.5	68	75.5				68																																																																							mOhm.cm											13.7											0.282	La2O3,Gd2O3,CaCO3,BaCO3,SrCO3,CuO,In2O3	1	SIN(940-960C,24h, in N2)-ANN(500C, 24h, in O2 flow)-slow cool to RT(1C/min)					Suppression of superconductivity in the (La2.5-xGd0.5+x)CaBa3-xSrx(Cu1-yIny)7Oz system due to hole filling by In and its revival by hole doping with Ca			Saurashtra University, Rajkot, India	Physica C, 371(2002)315	Amish G.Joshi,Darshan C.Kundaliya,Deelip G.Kuberkar,Ramchandra G.Kulkarni,Reeta Vij		
33546	P065172506	not s/c. 2nd phase=SrRuO3(19%), 3rd phase=CuO(8%). main phase(73%)	Pb2RuSr2Cu2O8Cl	Pb2Ru1Sr2Cu2Cl1O8	Pb	2	Ru	1	Sr	2	Cu	2	Cl	1											O	8		2	2002							117	10																				Ru1222	p4/mmm		A	3.8668		15.3699												K					10																																																																																																	1	solid state reaction					Structure and magnetism of the layered ruthenocuprate Pb2RuSr2Cu2O8Cl			Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom	Phys.Rev.B, 65(2002)172506	Abbie C.Mclaughlin,J.Paul Attfield,Judith A.McAllister,Lisa D.Stout		
33547	P065172501		(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2002																												IL																		K				43			43																																																																																														La2O3,SrCO3,CuO,ZnO(NiO)	1	CAL(920-945C, 36h)-high pressure sintering					Substitution for Cu in the electron-doped infinite-layer superconductor Sr0.9La0.1CuO2 : Ni reduces Tc much faster than Zn			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Seog Kim,S.Y.Lee,Sung-IK Lee		
33548	P065172501		(Sr,La)(Cu,Zn)O2	Sr0.9La0.1Cu0.99Zn0.01O2	Sr	0.9	La	0.1	Cu	0.99	Zn	0.01													O	2		1	2002																												IL																		K				42			42																																																																																														La2O3,SrCO3,CuO,ZnO(NiO)	1	CAL(920-945C, 36h)-high pressure sintering					Substitution for Cu in the electron-doped infinite-layer superconductor Sr0.9La0.1CuO2 : Ni reduces Tc much faster than Zn			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Seog Kim,S.Y.Lee,Sung-IK Lee		
33549	P065172501		(Sr,La)(Cu,Zn)O2	Sr0.9La0.1Cu0.97Zn0.03O2	Sr	0.9	La	0.1	Cu	0.97	Zn	0.03													O	2		1	2002																												IL			A	3.95		3.408												K				38			38																																																																																														La2O3,SrCO3,CuO,ZnO(NiO)	1	CAL(920-945C, 36h)-high pressure sintering					Substitution for Cu in the electron-doped infinite-layer superconductor Sr0.9La0.1CuO2 : Ni reduces Tc much faster than Zn			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Seog Kim,S.Y.Lee,Sung-IK Lee		
33560	P065172501		(Sr,La)(Cu,Ni)O2	Sr0.9La0.1Cu0.99Ni0.01O2	Sr	0.9	La	0.1	Cu	0.99	Ni	0.01													O	2		1	2002																												IL																		K				30			30																																																																																														La2O3,SrCO3,CuO,ZnO(NiO)	1	CAL(920-945C, 36h)-high pressure sintering					Substitution for Cu in the electron-doped infinite-layer superconductor Sr0.9La0.1CuO2 : Ni reduces Tc much faster than Zn			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Seog Kim,S.Y.Lee,Sung-IK Lee		
33561	P065172501		(Sr,La)(Cu,Ni)O2	Sr0.9La0.1Cu0.98Ni0.02O2	Sr	0.9	La	0.1	Cu	0.98	Ni	0.02													O	2		1	2002																												IL			A	3.943		3.417												K					5					K/GPa	19																																																																																										La2O3,SrCO3,CuO,ZnO(NiO)	1	CAL(920-945C, 36h)-high pressure sintering					Substitution for Cu in the electron-doped infinite-layer superconductor Sr0.9La0.1CuO2 : Ni reduces Tc much faster than Zn			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and		C.U.Jung,Heon-Jung Kim,J.Y.Kim,Min-Seok Park,Mun-Seog Kim,S.Y.Lee,Sung-IK Lee		
33562	L088247001	dTc/dp in DB at 0.2 GPa for hydrostatic. LTO-LTT transition (Td=68 K). Pressure dependence of Tc, Td shows different for uni-axial pressure.	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2002																												T																		K			8				8																																																																																											RH33562					traveling-solvent floating-zone method					Competition of Static Stripe and Superconducting Phases in La1.48Nd0.4Sr0.12CuO4 Controlled by Pressure			Department of Physics, Bharathidasan University, Tiruchirappalli -620 024, India	Phys.Rev.Lett., 88(2002)247001	H.Eisaki,H.Takashima,N.Mori,N.Takeshita,S.Arumugam,S.Uchida,T.Noda		
33563	MCP0750144	heat(850C,8h)	(Hg,Mo)Sr2CuO4+z	Hg0.85Mo0.15Sr2Cu1O4+z	Hg	0.85	Mo	0.15	Sr	2	Cu	1													O	4+z		1	2002																												Hg1201			A	3.781		8.868												K				56			56																																																																																																(precursor(Sr2CuO3) + MoO3,HgO) - (Au tube in sealed qualtz tube) - heat					Superconductivity in (Hg,Mo)Sr2CuO4+z system				Mat.Chem.Phys., 75(2002)144-146	I.K.Gopalakrishunan,J.V.Yakhmi,P.Selvam,S.Balamurugan		
33564	MCP0750144	heat(880C,8h)	(Hg,Mo)Sr2CuO4+z	Hg0.85Mo0.15Sr2Cu1O4+z	Hg	0.85	Mo	0.15	Sr	2	Cu	1													O	4+z		1	2002																												Hg1201			A	3.775		8.888												K				66			66																																																																																																(precursor(Sr2CuO3) + MoO3,HgO) - (Au tube in sealed qualtz tube) - heat					Superconductivity in (Hg,Mo)Sr2CuO4+z system				Mat.Chem.Phys., 75(2002)144-146	I.K.Gopalakrishunan,J.V.Yakhmi,P.Selvam,S.Balamurugan		
33565	MCP0750144	heat(880C,8h)	(Hg,Mo)Sr2CuO4+z	Hg0.75Mo0.25Sr2Cu1O4+z	Hg	0.75	Mo	0.25	Sr	2	Cu	1													O	4+z		1	2002																												Hg1201			A	3.791		8.818												K				50			50																																																																																																(precursor(Sr2CuO3) + MoO3,HgO) - (Au tube in sealed qualtz tube) - heat					Superconductivity in (Hg,Mo)Sr2CuO4+z system				Mat.Chem.Phys., 75(2002)144-146	I.K.Gopalakrishunan,J.V.Yakhmi,P.Selvam,S.Balamurugan		
33566	MCP0750144	heat(880C,8h)	(Hg,Mo)Sr2CuO4+z	Hg0.7Mo0.3Sr2Cu1O4+z	Hg	0.7	Mo	0.3	Sr	2	Cu	1													O	4+z		1	2002																												Hg1201			A	3.805		8.814												K				36			36																																																																																																(precursor(Sr2CuO3) + MoO3,HgO) - (Au tube in sealed qualtz tube) - heat					Superconductivity in (Hg,Mo)Sr2CuO4+z system				Mat.Chem.Phys., 75(2002)144-146	I.K.Gopalakrishunan,J.V.Yakhmi,P.Selvam,S.Balamurugan		
33567	MCP0750110	Curie T shows FM Curie T	GdSr2RuCu2O8	Gd1Sr2Ru1Cu2O8	Gd	1	Sr	2	Ru	1	Cu	2													O	8		1	2002							139.2																					Ru1212																		K	6.4		26.5				16.45																																																																																														Gd2O3,SrCO3,CuO,Ru	1	mixture-heat(600C,48h + 950C,24h,in air) - heat(100C,72h, in air) - ANN(1060C,96h, in O2)					Tuning of the superconducting and ferromagnetic transitions by Cu doping for Ru in GdSr2RuCu2O8				Mat.Chem.Phys., 75(2002)110-116	J.Janaki,M.C.Valsakumar,R.Nagarajan,T.A.Mary,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
33568	MCP0750110	Curie T shows FM Curie T	GdSr2(Ru,Cu)Cu2O8	Gd1Sr2Ru0.95Cu2.05O8	Gd	1	Sr	2	Ru	0.95	Cu	2.05													O	8		1	2002							135.8																					Ru1212																		K	12.6		39.5				26.05																																																																																														Gd2O3,SrCO3,CuO,Ru	1	mixture-heat(600C,48h + 950C,24h,in air) - heat(100C,72h, in air) - ANN(1060C,96h, in O2)					Tuning of the superconducting and ferromagnetic transitions by Cu doping for Ru in GdSr2RuCu2O8				Mat.Chem.Phys., 75(2002)110-116	J.Janaki,M.C.Valsakumar,R.Nagarajan,T.A.Mary,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
33569	MCP0750110	Curie T shows FM Curie T	GdSr2(Ru,Cu)Cu2O8	Gd1Sr2Ru0.9Cu2.1O8	Gd	1	Sr	2	Ru	0.9	Cu	2.1													O	8		1	2002							129.9																					Ru1212																		K	28.3		47.2				37.75																																																																																														Gd2O3,SrCO3,CuO,Ru	1	mixture-heat(600C,48h + 950C,24h,in air) - heat(100C,72h, in air) - ANN(1060C,96h, in O2)					Tuning of the superconducting and ferromagnetic transitions by Cu doping for Ru in GdSr2RuCu2O8				Mat.Chem.Phys., 75(2002)110-116	J.Janaki,M.C.Valsakumar,R.Nagarajan,T.A.Mary,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
33570	MCP0750110	Curie T shows FM Curie T	GdSr2(Ru,Cu)Cu2O8	Gd1Sr2Ru0.8Cu2.2O8	Gd	1	Sr	2	Ru	0.8	Cu	2.2													O	8		1	2002							123.2																					Ru1212																		K	16.8		40				28.4																																																																																														Gd2O3,SrCO3,CuO,Ru	1	mixture-heat(600C,48h + 950C,24h,in air) - heat(100C,72h, in air) - ANN(1060C,96h, in O2)					Tuning of the superconducting and ferromagnetic transitions by Cu doping for Ru in GdSr2RuCu2O8				Mat.Chem.Phys., 75(2002)110-116	J.Janaki,M.C.Valsakumar,R.Nagarajan,T.A.Mary,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
33571	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2002																												Y123																		K		91					91																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33572	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba1.96Sr0.04Cu3O7-z	Y	1	Ba	1.96	Sr	0.04	Cu	3													O	7-z		1	2002																												Y123																		K		90					90																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33573	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba1.9Sr0.1Cu3O7-z	Y	1	Ba	1.9	Sr	0.1	Cu	3													O	7-z		1	2002																												Y123																		K		88					88																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33574	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba1.8Sr0.2Cu3O7-z	Y	1	Ba	1.8	Sr	0.2	Cu	3													O	7-z		1	2002																												Y123																		K		85					85																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33575	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba1.6Sr0.4Cu3O7-z	Y	1	Ba	1.6	Sr	0.4	Cu	3													O	7-z		1	2002																												Y123																		K		83					83																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33576	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba1.2Sr0.8Cu3O7-z	Y	1	Ba	1.2	Sr	0.8	Cu	3													O	7-z		1	2002																												Y123																		K		80					80																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33577	P066012506	Cu NMR and buckling angle of CuO2 plane are measured.	Y(Ba,Sr)2Cu3O7	Y1Ba0.8Sr1.2Cu3O7-z	Y	1	Ba	0.8	Sr	1.2	Cu	3													O	7-z		1	2002																												Y123																		K		78					78																																																																																															1	standard solid state reaction method					Tc reduction in Sr-substituted Y(Ba1-xSrx)2Cu3O7-z investigated by <63>,<65> Cu nuclear quadrupole resonance			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing, China	Phys.Rev.B, 66(2002)12506	B.Q.Li,X.N.Ying,Y.H.Liu,Y.N.Huang,Y.N.Wang		
33578	P066020501	single crystal(1.4 cm3). Cu(2) site commensurate long range AF order(TN=330 K, M=0.14 Bohr-Mag) in Tc=93 K s/c.	YBa2(Cu,Co)3O7	Y1Ba2Cu2.961Co0.039O7-z	Y	1	Ba	2	Cu	2.961	Co	0.039													O	7-z		3	2002								330																				Y123																		K		93					93																																																																																																top-seed melt texturing method					Antiferromagnetic ordering in a 90 K copper oxide superconductor			DRECAM-SPEC, CE-Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20501	I.Mirebeau,J.A.Hodges,M.Hennion,P.Bourges,X.Chaud,Y.Sidis		
33579	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.09	Bi	2	Sr	2	Cu	1															O	6+z	6.09	1	2002																												Bi2201																		K		10					10																																																																		uV/K	-4.06			TP33579																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33580	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.13	Bi	2	Sr	2	Cu	1															O	6+z	6.13	1	2002																												Bi2201																		K		16					16																																																																		uV/K	-9.46			TP33580																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33581	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.14	Bi	2	Sr	2	Cu	1															O	6+z	6.14	1	2002																												Bi2201																		K		14					14																																																																		uV/K	-10.6			TP33581																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33582	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.16	Bi	2	Sr	2	Cu	1															O	6+z	6.16	1	2002																												Bi2201																		K		10					10																																																																		uV/K	-12.61			TP33582																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33583	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.175	Bi	2	Sr	2	Cu	1															O	6+z	6.175	1	2002																												Bi2201																		K		7					7																																																																		uV/K	-14.25			TP33583																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33584	P066020503		Bi2Sr2CuOz	Bi2Sr2Cu1O6.18	Bi	2	Sr	2	Cu	1															O	6+z	6.18	1	2002																												Bi2201																		K		3					3																																																																		uV/K	-16			TP33584																									1	solid state reaction O-content controlled by annealing (300 - 700C, 1<P(O2)<1 E-4 atm.					Thermopower in the strongly overdoped region of single-layer Bi2Sr2CuO6+z superconductor			SPEC, DSM/DRECAM, CEA Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20503	A.Forget,C.Ayache,D.Colson,F.Jean,G.Collin,G.Le Bras,M.Ocio,Z.Konstantinovic		
33585	P066024502	underdoped. ANN(700C, in N2 flow). M-crossing at T=64.4 K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212			A			30.9												K				65			65																													T/K		0.82					nm		2.5			nm		235																																																					TSFZ. P(O2)=25 mbar. Then annealing. products: Bi:Sr:Ca:Cu=2.23:1.9:0.96:2					Superconducting properties of strongly underdoped Bi2Sr2CaCu2O8+x single crystals			Kamerlingh Onnes Laboratory, Leiden University, P.O. Box 9504, 2300 RA Leiden, The Netherlands	Phys.Rev.B, 66(2002)24502	A.A.Menovsky,C.J.van der Beek,M.Konczykowski,M.Li,P.H.Kes		
33586	P066024502	optimally-doped. ANN(750C, in air). M-crossing at T=86.1 K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212			A			30.86												K				87.3			87.3																													T/K		2					nm		1.3			nm		163																																																					TSFZ. P(O2)=25 mbar. Then annealing. products: Bi:Sr:Ca:Cu=2.23:1.9:0.96:2					Superconducting properties of strongly underdoped Bi2Sr2CaCu2O8+x single crystals			Kamerlingh Onnes Laboratory, Leiden University, P.O. Box 9504, 2300 RA Leiden, The Netherlands	Phys.Rev.B, 66(2002)24502	A.A.Menovsky,C.J.van der Beek,M.Konczykowski,M.Li,P.H.Kes		
33587	P066024502	overdoped. ANN(400C, in O2 flow. M-crossing at T=78.6 K.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212			A			30.8												K				77			77																													T/K		1.2					nm		1.8			nm		136																																																					TSFZ. P(O2)=25 mbar. Then annealing. products: Bi:Sr:Ca:Cu=2.23:1.9:0.96:2					Superconducting properties of strongly underdoped Bi2Sr2CaCu2O8+x single crystals			Kamerlingh Onnes Laboratory, Leiden University, P.O. Box 9504, 2300 RA Leiden, The Netherlands	Phys.Rev.B, 66(2002)24502	A.A.Menovsky,C.J.van der Beek,M.Konczykowski,M.Li,P.H.Kes		
33588	P066024503	coexistence of s/c and weak FM. Tirr=75 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.6Ce0.4Sr2Ru1Cu2O10	Eu	1.6	Ce	0.4	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K				32			32																																																																																															1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33589	P066024503	coexistence of s/c and weak FM. Tirr=78 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.5Ce0.5Sr2Ru1Cu2O10	Eu	1.5	Ce	0.5	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K				34			34																																																																																															1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33590	P066024503	coexistence of s/c and weak FM. Tirr=88 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.4Ce0.6Sr2Ru1Cu2O10	Eu	1.4	Ce	0.6	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K				35			35																																																																																															1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33591	P066024503	coexistence of s/c and weak FM. Tirr=92 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.3Ce0.7Sr2Ru1Cu2O10	Eu	1.3	Ce	0.7	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K				33			33																																																																																															1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33592	P066024503	coexistence of s/c and weak FM. Tirr=99 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.2Ce0.8Sr2Ru1Cu2O10	Eu	1.2	Ce	0.8	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K				30			30																																																																																															1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33593	P066024503	not s/c. magnetic Tirr=109 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1.1Ce0.9Sr2Ru1Cu2O10	Eu	1.1	Ce	0.9	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K					5																																																																																																	1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33594	P066024503	not s/c. magnetic Tirr=120 K.	(Eu,Ce)2Sr2RuCu2O10	Eu1Ce1Sr2Ru1Cu2O10	Eu	1	Ce	1	Sr	2	Ru	1	Cu	2											O	10		1	2002																												Ru1222			A	3.864		28.72												K					5																																																																																																	1	solid state reaction. SIN(1050C, 50h, 1.1 atm-O2)					Magnetic-superconducting phase diagram of Eu2-xCexRuSr2Cu2O10-z			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 66(2002)24503	E.Galstyan,I.Felner,U.Asaf		
33595	PHC1910237	ANN(1125C, 60h, 25 atm-O2). Tc sensitive to O-contents.	(Nd,Ce)2Sr2NbCu2O10	Nd1.5Ce0.5Sr2Nb1Cu2O10	Nd	1.5	Ce	0.5	Sr	2	Nb	1	Cu	2											O	10		1	1992																												M1222			A	3.885		28.864												K				28			28																																																																																															1	solid state reaction. 					SUPERCONDUCTIVITY AT 28 K IN A CUPRATE WITH A NIOBIUM OXIDE INTERMEDIARY LAYER	199202			PHYSICA C,191(1992)237	B.HESSEN,B.Hessen,H.TAKAGI,H.Takagi,H.W.ZANDBERGEN,H.W.Zandbergen,J.J.KRAJEWSKI,J.J.Krajewski,R.B.VAN DOVER,R.B.Van Dover,R.J.CAVA,R.J.Cava,W.F.PECK JR.,W.F.Peck Jr.	SR,ND,CE,NB,CU,O	
33596	PHC1910237	ANN(1125C, 85h, 1 atm-O2). Tc sensitive to O-contents.	(Nd,Ce)2Sr2TaCu2O10	Nd1.5Ce0.5Sr2Ta1Cu2O10	Nd	1.5	Ce	0.5	Sr	2	Ta	1	Cu	2											O	10		1	1992																												M1222																		K				25			25																																																																																															1	solid state reaction. 					SUPERCONDUCTIVITY AT 28 K IN A CUPRATE WITH A NIOBIUM OXIDE INTERMEDIARY LAYER	199202			PHYSICA C,191(1992)237	B.HESSEN,B.Hessen,H.TAKAGI,H.Takagi,H.W.ZANDBERGEN,H.W.Zandbergen,J.J.KRAJEWSKI,J.J.Krajewski,R.B.VAN DOVER,R.B.Van Dover,R.J.CAVA,R.J.Cava,W.F.PECK JR.,W.F.Peck Jr.	SR,ND,CE,NB,CU,O	
33597	JPS0710574	spin gap temp=239.7 K	Y2Ba4Cu7O15	Y2Ba4Cu7O14	Y	2	Ba	4	Cu	7															O	15-z	14	1	2002																												Y247																		K					1.9																																																																																																		(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33598	JPS0710574	spin gap temp=237.8 K	Y2Ba4Cu7O15	Y2Ba4Cu7O14.03	Y	2	Ba	4	Cu	7															O	15-z	14.03	1	2002																												Y247			A	3.8596	3.8735	50.735												K				4.3			4.3																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33599	JPS0710574		Y2Ba4Cu7O15	Y2Ba4Cu7O14.19	Y	2	Ba	4	Cu	7															O	15-z	14.19	1	2002																												Y247			A	3.8614	3.8788	50.715												K				13.9			13.9																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33600	JPS0710574		Y2Ba4Cu7O15	Y2Ba4Cu7O14.33	Y	2	Ba	4	Cu	7															O	15-z	14.33	1	2002																												Y247																		K				22			22																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33601	JPS0710574	spin gap temp=209.6 K	Y2Ba4Cu7O15	Y2Ba4Cu7O14.46	Y	2	Ba	4	Cu	7															O	15-z	14.46	1	2002																												Y247																		K				32.1			32.1																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33602	JPS0710574		Y2Ba4Cu7O15	Y2Ba4Cu7O14.6	Y	2	Ba	4	Cu	7															O	15-z	14.6	1	2002																												Y247			A	3.854	3.8756	50.614												K				41.2			41.2																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33603	JPS0710574		Y2Ba4Cu7O15	Y2Ba4Cu7O14.81	Y	2	Ba	4	Cu	7															O	15-z	14.81	1	2002																												Y247			A	3.8476	3.8752	50.541												K				54.1			54.1																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33604	JPS0710574		Y2Ba4Cu7O15	Y2Ba4Cu7O14.95	Y	2	Ba	4	Cu	7															O	15-z	14.95	1	2002																												Y247			A	3.8494	3.8805	50.512												K				67			67																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33605	JPS0710574	spin gap temp=169.4 K	Y2Ba4Cu7O15	Y2Ba4Cu7O15	Y	2	Ba	4	Cu	7															O	15-z	15	1	2002																												Y247																		K				72.2			72.2																																																																																																(930-980C, P(o2)=3-8 bar, in sealed quartz)					Collapse of Superconductivity in the Y123/Y124 Superlattice System Y2Ba4Cu7O15-z			Department of Chemistry,Graduate School of Science,Kyoto University,Kyoto,Japan	J.Phys.Soc.Jpn, 71(2002)574	A.Irizawa,G.Hilscher,H.Michor,K.Kosuge,K.Yoshimura,M.Kato,T.Ohmura,T.Shibata,Y.Ito		
33606	JPS0710709	G-L = 21.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7			2002																												pyrochlore																		K				1			1																																				nm	from Hc2	34			nm	muon-SR. curve fitting analysis.	700																																																					see #33253					Quasiparticle Excitation in the superconducting pyrochlore Cd2Re2O7 probed by muon spin rotation			KFK, Tsukuba,Ibaraki,Japan	J.Phys.Soc.Jpn., 71(2002)709	A.Koda,M.Hanawa,R.Kadono,W.Higemoto,Y.Kawasaki,Z.Hiroi		
33607	CEM1560026	not s/c. (1520C, Ar+0.3%O2)	(Sr,Ca)2RuO4	Sr0.5Ca1.5Ru1O4	Sr	0.5	Ca	1.5	Ru	1															O	4		1	2001																												T			A	3.7752		12.563												K					4.2																																																																																																		mixture - pellet(2000kgf/cm2) - SIN(1100-1570C, P(O2)=0-0.01 bar (Ar +O2 gas)					Synthesis and single-crystal growth of Ca2-xSrxRuO4			Department of Physics, Kyoto University, Kyoto, Japan	J.Solid State Chem., 156(2001)26	S.Nakatsuji,Y.Maeno		
33608	CEM1560026	not s/c. (1503C, Ar+0.3 %O2)	(Sr,Ca)2RuO4	Sr1Ca1Ru1O4	Sr	1	Ca	1	Ru	1															O	4		1	2001																												T			A	3.8048		12.666												K					4.2																																																																																																		mixture - pellet(2000kgf/cm2) - SIN(1100-1570C, P(O2)=0-0.01 bar (Ar +O2 gas)					Synthesis and single-crystal growth of Ca2-xSrxRuO4			Department of Physics, Kyoto University, Kyoto, Japan	J.Solid State Chem., 156(2001)26	S.Nakatsuji,Y.Maeno		
33609	CEM1560026	not s/c. (1400C, Ar+0.1 %O2)	(Sr,Ca)2RuO4	Sr1.5Ca0.5Ru1O4	Sr	1.5	Ca	0.5	Ru	1															O	4		1	2001																												T			A	3.8371		12.729												K					4.2																																																																																																		mixture - pellet(2000kgf/cm2) - SIN(1100-1570C, P(O2)=0-0.01 bar (Ar +O2 gas)					Synthesis and single-crystal growth of Ca2-xSrxRuO4			Department of Physics, Kyoto University, Kyoto, Japan	J.Solid State Chem., 156(2001)26	S.Nakatsuji,Y.Maeno		
33610	PRL0774434	heavily overdoped. Raman spectroscopy	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	1996																												Tl2201																		K				25			25																																														cm-1	75	4.2	4																																															see Physica C, 242(1995)385.					Resonance Raman Study of the Superconducting Gap and Low Energy Excitations in Tl2Ba2CuO6+z Superconductors			Department of Physics, and Science and Technology Center for Superconductivity, University of Illinois, Urbana, Illinois ,USA	Phys.Rev.Lett., 77(1996)4434	G.Blumberg,M.V.Klein,Moonsoo Kang,N.N.Kolesnikov		
33611	PRL0774434	optimally-doped.  Raman spectroscopy	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	1996																												Tl2201																		K				85			85																																														cm-1	450	8	4																																															see Physica C, 242(1995)385.					Resonance Raman Study of the Superconducting Gap and Low Energy Excitations in Tl2Ba2CuO6+z Superconductors			Department of Physics, and Science and Technology Center for Superconductivity, University of Illinois, Urbana, Illinois ,USA	Phys.Rev.Lett., 77(1996)4434	G.Blumberg,M.V.Klein,Moonsoo Kang,N.N.Kolesnikov		
33612	PRL0764238	broad s/c transition(110-134 K). NMR(<63>Cu). spin gap temp=230 K defined as (1/T1T) has peak. 	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z		3	1996																												Hg1223																		K				115			115																																																																																																see Physica C, 233(1994)233					Spin Gap in HgBa2Ca2Cu3O8+z Single Crystals from <63>Cu NMR			Grenoble High Magnetic Field Laboratory, Grenoble Cedex, France	Phys.Rev.Lett., 76(1996)4238	A.Carrington,C.Berthier,D.Colson,M.-H.Julien,M.Horvatic,P.Carretta,P.Segransan,Y.Berthier		
33613	JPS0711553	R(300)=400, R(5K)=26 microOhm.cm. RRR=15. Tc(P=2.0 GPa)=3K. not known whether Tc increase continuously under pressure.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2002																												pyrochlore																		K		0.98					0.98	TC33613																																																																																															900 C in quartz ampoule.					High-Pressure Study on the Superconducting Pyrochlore Oxide Cd2Re2O7			Institute for Soli State Physics,University of Tokyo,Kashiwanoha,Kashiwa,Chiba , Japan	J.Phys.Soc.Jpn, 71(2002)1553	M.Abliz,M.Hanawa,M.Hedo,O.Shimomura,T.Yamada,T.Yamauchi,Y.Ohishi,Y.Uwatoko,Z.Hiroi		
33614	EPJ0260413	specific heat measurements.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												T																		K				0.43			0.43																																																								mJ/mol.K2	37																																							polycrystal - crystal growth by heating. ratio of SrCO3/RuO2 altered for each sample.					Low-temperature specific heat of Sr2RuO4			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	Eur.Phys. J.B, 26(2002)413	C.Langhammer,F.Steglich,M.Lang,T.Sasaki		
33615	EPJ0260413	specific heat measurements. RRR=42	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												T																		K				0.68			0.68																																																								mJ/mol.K2	28																																							polycrystal - crystal growth by heating. ratio of SrCO3/RuO2 altered for each sample.					Low-temperature specific heat of Sr2RuO4			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	Eur.Phys. J.B, 26(2002)413	C.Langhammer,F.Steglich,M.Lang,T.Sasaki		
33616	EPJ0260413	specific heat measurements. RRR=290	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												T																		K				1.1			1.1																																																								mJ/mol.K2	18.9																																							polycrystal - crystal growth by heating. ratio of SrCO3/RuO2 altered for each sample.					Low-temperature specific heat of Sr2RuO4			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	Eur.Phys. J.B, 26(2002)413	C.Langhammer,F.Steglich,M.Lang,T.Sasaki		
33617	EPJ0260413	specific heat measurements. RRR=290	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												T																		K				1.17			1.17																																																								mJ/mol.K2	17.8																																							polycrystal - crystal growth by heating. ratio of SrCO3/RuO2 altered for each sample.					Low-temperature specific heat of Sr2RuO4			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	Eur.Phys. J.B, 26(2002)413	C.Langhammer,F.Steglich,M.Lang,T.Sasaki		
33618	JPS0670560	residual gamma = 32.0 mJ/mol.K2. delta-C/gamma*Tc = 1.46	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												T																		K				0.79			0.79																																																								mJ/mol.K2	41.8																																							s/c properties depends on sample purity.					Evidence for unconventional superconductivity of Sr2RuO4 from specific-heat measurements			Department of Physics, Kyoto University, Kyoto, Japan	J.Phys.Soc.Jpn, 67(1998)560	S.Farner,S.Ikeda,S.Nishizaki,T.Fujita,Y.Maeno		
33619	JPS0670560	residual gamma = 26.5 mJ/mol.K2. delta-C/gamma*Tc = 1.02	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												T																		K				1.08			1.08																																																								mJ/mol.K2	38.9																																							s/c properties depends on sample purity.					Evidence for unconventional superconductivity of Sr2RuO4 from specific-heat measurements			Department of Physics, Kyoto University, Kyoto, Japan	J.Phys.Soc.Jpn, 67(1998)560	S.Farner,S.Ikeda,S.Nishizaki,T.Fujita,Y.Maeno		
33620	JPS0670560	residual gamma = 24.4 mJ/mol.K2. delta-C/gamma*Tc = 1.01	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												T																		K				1.14			1.14																																																								mJ/mol.K2	40.9																																							s/c properties depends on sample purity.					Evidence for unconventional superconductivity of Sr2RuO4 from specific-heat measurements			Department of Physics, Kyoto University, Kyoto, Japan	J.Phys.Soc.Jpn, 67(1998)560	S.Farner,S.Ikeda,S.Nishizaki,T.Fujita,Y.Maeno		
33621	EPL0580589	pseudogap not observed. gap by break junction.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2002																												Bi2212																		K				56			56																																														meV	14	5.8	1																																															self-flux method					Absence of pseudogap in heavily overdoped Bi2Sr2CaCu2O8+z  from tunneling spectroscopy of break junctions			Materials Science Division, Argonne National Laboratory, Argonne, IL, USA.	Europhys.Lett., 58(2002)589	C.Kendziora,J.F.Zasadzinski,K.E.Gray,L.Ozyuzer,N.Miyakawa		
33622	EPL0580758	not s/c upto 8 GPa.	Sr14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41		3	2002																												LAD																		K					2																																																																																																		crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33623	EPL0580758	not s/c upto 8 GPa.	(Sr,Ca)14Cu24O41	Sr11Ca3Cu24O41	Sr	11	Ca	3	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33624	EPL0580758	not s/c upto 8 GPa.	(Sr,Ca)14Cu24O41	Sr8Ca6Cu24O41	Sr	8	Ca	6	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33625	EPL0580758	not s/c upto 8 GPa.	(Sr,Ca)14Cu24O41	Sr6Ca8Cu24O41	Sr	6	Ca	8	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33626	EPL0580758	pressure-induced s/c. Tc(max)= 4K (P=5 GPa)	(Sr,Ca)14Cu24O41	Sr4Ca10Cu24O41	Sr	4	Ca	10	Cu	24															O	41		3	2002																												LAD																		K			4		0		4																																																																																																crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33627	EPL0580758	pressure-induced s/c. Tc(max)= 5.5K (P=3.5 GPa)	(Sr,Ca)14Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2002																												LAD																		K			5.5		0		5.5																																																																																																crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33628	EPL0580758	not s/c upto 8 GPa.	(Sr,Ca)14Cu24O41	Sr13Y1Cu24O41	Sr	13	Y	1	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		crystals by traveling-solvent-floating-zone(TSFZ) method					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33629	PHC3770146	not s/c	(Hg,Pb)2Ba2YCu2O8	Hg1.75Pb0.25Ba2Y1Cu2O8-z	Hg	1.75	Pb	0.25	Ba	2	Y	1	Cu	2											O	8-z		1	2002																												Hg2212			A	3.8672		28.8433												K					5																																																																																																HgO,PbO2,BaO2,Y2O3,CaO,CuO,Cu		mixture-pellet-Au capsule- HIP(3.5 GPa,100C,1h)					Crystal structure of (Hg1-yPby)2Ba2(Y1-xCax)Cu2O8-d superconducting compounds by neutron powder diffraction			Laboratoire de Cristallographie,25,avenue des martyrs,Grenoble Cedex,France	Physica C, 377(2002)146	C.Brachet,E.Suard,P.Bordet,P.Odier,P.Toulemonde		
33630	PHC3770146		(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.75Pb0.25Ba2Y0.7Ca0.3Cu2O8-z	Hg	1.75	Pb	0.25	Ba	2	Y	0.7	Ca	0.3	Cu	2									O	8-z		1	2002																												Hg2212			A	3.8574		28.8228												K			70				70																																																																																														HgO,PbO2,BaO2,Y2O3,CaO,CuO,Cu		mixture-pellet-Au capsule- HIP(3.5 GPa,100C,1h)					Crystal structure of (Hg1-yPby)2Ba2(Y1-xCax)Cu2O8-d superconducting compounds by neutron powder diffraction			Laboratoire de Cristallographie,25,avenue des martyrs,Grenoble Cedex,France	Physica C, 377(2002)146	C.Brachet,E.Suard,P.Bordet,P.Odier,P.Toulemonde		
33631	PHC3770146		(Hg,Pb)2Ba2(Y,Ca)Cu2O8	Hg1.5Pb0.5Ba2Y0.5Ca0.5Cu2O8-z	Hg	1.5	Pb	0.5	Ba	2	Y	0.5	Ca	0.5	Cu	2									O	8-z		1	2002																												Hg2212			A	3.8555		28.9314												K			84				84																																																																																														HgO,PbO2,BaO2,Y2O3,CaO,CuO,Cu		mixture-pellet-Au capsule- HIP(3.5 GPa,100C,1h)					Crystal structure of (Hg1-yPby)2Ba2(Y1-xCax)Cu2O8-d superconducting compounds by neutron powder diffraction			Laboratoire de Cristallographie,25,avenue des martyrs,Grenoble Cedex,France	Physica C, 377(2002)146	C.Brachet,E.Suard,P.Bordet,P.Odier,P.Toulemonde		
33632	JAP0917134	carrier = 1.69 E+27 /m3 from Hall coefficient.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8-z	Ru	1	Sr	2	Gd	1	Cu	2													O	8-z		1	2002																												Ru1212																		K			45				45			K/GPa	5.5																																																														uV/K	60																													High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33633	JAP0917134	carrier = 2.46 E+27 /m3 from Hall coefficient.	(Ru,Cu)Sr2GdCu2O8	Ru0.9Sr2Gd1Cu2.1O8-z	Ru	0.9	Sr	2	Gd	1	Cu	2.1													O	8-z		1	2002																												Ru1212																		K										K/GPa	5.5																																																														uV/K	17																													High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33634	JAP0917134	carrier = 3.06 E+27 /m3 from Hall coefficient.	(Ru,Cu)Sr2GdCu2O8	Ru0.8Sr2Gd1Cu2.2O8-z	Ru	0.8	Sr	2	Gd	1	Cu	2.2													O	8-z		1	2002																												Ru1212																		K										K/GPa	5.5																																																														uV/K	14.7																													High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33635	JAP0917134	carrier = 3.18 E+27 /m3 from Hall coefficient.	(Ru,Cu)Sr2GdCu2O8	Ru0.7Sr2Gd1Cu2.3O8-z	Ru	0.7	Sr	2	Gd	1	Cu	2.3													O	8-z		1	2002																												Ru1212																		K										K/GPa	5.5																																																														uV/K	12.7																													High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33636	JAP0917134	carrier = 3.18 E+27 /m3 from Hall coefficient.	(Ru,Cu)Sr2GdCu2O8	Ru0.6Sr2Gd1Cu2.4O8-z	Ru	0.6	Sr	2	Gd	1	Cu	2.4													O	8-z		1	2002																												Ru1212																		K			72				72			K/GPa	5.5																																																														uV/K	9.1																													High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33637	JAP0917134	magnetic order observed by muon-SR (FM or AF)	(Ru,Cu)Sr2GdCu2O8	Ru0.6Sr2Eu1Cu2.4O8-z	Ru	0.6	Sr	2	Eu	1	Cu	2.4													O	8-z		1	2002								5																				Ru1212																		K			70				70			K/GPa	5.5																																																																																												High pressure synthesis (600 bar O2, 1080C)					On the magnetic and superconducting properties of Ru1-xSr2RECu2+xO8-d ,RE=Gd, Eu, compounds			Northern Illinois University, DeKalb, Illinois	J.Appl.Phys., 91(2002)7134	A.Shengelaya,A.Wisniewski,B.Dabrowski,C.Sulkowski,H.Keller,I.Fita,I.Savic,M.Matusiak,M.Maxwell,P.W.Klamut,R.Khasanov,R.Puzniak,S.Kolesnik,S.M.Mini		
33638	JPM014L257	RRR=24. phase transition at T=200 K. s= -0.234 * T for T<20 K	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2002																												pyrochlore			A	10.223														K		1.4					1.4																																																																		uV/K	-2.2			TP33638	mOhm.cm							0.015				0.355													1	solid state reaction					Thermoelectric power of the superconducting pyrochlore Cd2Re2O7			Department of Physics, Toyama University, Toyama 930-8555, Japan	J. Phys.: Condens. Matter, 14 (2002) L257	A.Mitsuda,D.Huo,H.Ohno,H.Sakai,J.Sakurai,K.Yoshimura,M.Kato,R.E.Walstedt,S.Kambe,Y.Isikawa		
33639	PCS0631815		(Hg,Cr)Sr2CuO4	Hg0.7Cr0.3Sr2Cu1O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	1													O	4+z		1	2002																												Hg1201			A	3.8414		8.7017												K				68			68																																																																							mOhm.cm							0.318				3.43														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33640	PCS0631815		(Hg,Cr)Sr2(Cu,Zn)O4	Hg0.7Cr0.3Sr2Cu0.99Zn0.01O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.99	Zn	0.01											O	4+z		1	2002																												Hg1201			A	3.841		8.6829												K				63			63																																																																							mOhm.cm							0.532				3.51														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33641	PCS0631815		(Hg,Cr)Sr2(Cu,Zn)O4	Hg0.7Cr0.3Sr2Cu0.98Zn0.02O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.98	Zn	0.02											O	4+z		1	2002																												Hg1201			A	3.8414		8.6641												K				60			60																																																																							mOhm.cm							0.856				3.58														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33642	PCS0631815		(Hg,Cr)Sr2(Cu,Zn)O4	Hg0.7Cr0.3Sr2Cu0.97Zn0.03O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.97	Zn	0.03											O	4+z		1	2002																												Hg1201			A	3.842		8.6466												K				57			57																																																																							mOhm.cm							1.416				3.67														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33643	PCS0631815		(Hg,Cr)Sr2(Cu,Zn)O4	Hg0.7Cr0.3Sr2Cu0.96Zn0.04O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.96	Zn	0.04											O	4+z		1	2002																												Hg1201			A	3.8419		8.6281												K				54			54																																																																							mOhm.cm							2.053				3.83														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33644	PCS0631815		(Hg,Cr)Sr2(Cu,Zn)O4	Hg0.7Cr0.3Sr2Cu0.95Zn0.05O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.95	Zn	0.05											O	4+z		1	2002																												Hg1201			A	3.8424		8.6099												K				51			51																																																																							mOhm.cm							1.445				3.95														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33645	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.99Ni0.01O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.99	Ni	0.01											O	4+z		1	2002																												Hg1201			A	3.8415		8.6959												K				59			59																																																																							mOhm.cm							0.889				3.62														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33646	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.98Ni0.02O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.98	Ni	0.02											O	4+z		1	2002																												Hg1201			A	3.8418		8.69												K				53			53																																																																							mOhm.cm							1.522				3.88														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33647	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.97Ni0.03O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.97	Ni	0.03											O	4+z		1	2002																												Hg1201			A	3.842		8.6845												K				48			48																																																																							mOhm.cm							2.374				4.21														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33648	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.96Ni0.04O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.96	Ni	0.04											O	4+z		1	2002																												Hg1201			A	3.8424		8.6792												K				43			43																																																																							mOhm.cm							2.88				4.62														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33649	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.95Ni0.05O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.95	Ni	0.05											O	4+z		1	2002																												Hg1201			A	3.8426		8.6809												K				39			39																																																																							mOhm.cm							3.783				5.22														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33650	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.925Ni0.075O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.925	Ni	0.075											O	4+z		1	2002																												Hg1201			A	3.8429		8.6619												K				28			28																																																																							mOhm.cm							5.255				5.83														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33651	PCS0631815		(Hg,Cr)Sr2(Cu,Ni)O4	Hg0.7Cr0.3Sr2Cu0.9Ni0.1O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.9	Ni	0.1											O	4+z		1	2002																												Hg1201			A	3.8432		8.6477												K				18			18																																																																							mOhm.cm							7.073				6.96														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33652	PCS0631815		(Hg,Cr)Sr2(Cu,Co)O4	Hg0.7Cr0.3Sr2Cu0.99Co0.01O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.99	Co	0.01											O	4+z		1	2002																												Hg1201			A	3.8414		8.6961												K				58			58																																																																							mOhm.cm							1.22				3.7														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33653	PCS0631815		(Hg,Cr)Sr2(Cu,Co)O4	Hg0.7Cr0.3Sr2Cu0.98Co0.02O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.98	Co	0.02											O	4+z		1	2002																												Hg1201			A	3.8417		8.6902												K				52			52																																																																							mOhm.cm							2.007				4.24														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33654	PCS0631815		(Hg,Cr)Sr2(Cu,Co)O4	Hg0.7Cr0.3Sr2Cu0.97Co0.03O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.97	Co	0.03											O	4+z		1	2002																												Hg1201			A	3.8419		8.6833												K				46			46																																																																							mOhm.cm							3.411				4.82														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33655	PCS0631815		(Hg,Cr)Sr2(Cu,Co)O4	Hg0.7Cr0.3Sr2Cu0.96Co0.04O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.96	Co	0.04											O	4+z		1	2002																												Hg1201			A	3.8424		8.6777												K				42			42																																																																							mOhm.cm							4.395				5.25														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33656	PCS0631815		(Hg,Cr)Sr2(Cu,Co)O4	Hg0.7Cr0.3Sr2Cu0.95Co0.05O4+z	Hg	0.7	Cr	0.3	Sr	2	Cu	0.95	Co	0.05											O	4+z		1	2002																												Hg1201			A	3.8427		8.6729												K				35			35																																																																							mOhm.cm							5.452				5.81														precursor(Cr0.3Sr2(Cu,M)Oz) + HgO, pelletize, evacuated quartz tube, heat(870C, 8h), FC to RT.					Influence of Co, Ni, and Zn substitution for Cu on the structural and superconducting properties of (Hg0.7Cr0.3)Sr2CuO4+z			Department of Chemistry, Faculty of Science, Tanta University, Egypt	J.Phys.Chem.Solids, 63(2002)1815	E.Kandyel,M.A.Sekkina		
33657	SSC1230017	G-L = 25.3. anisotropy = 9.3.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2002																												IL																		K				42			42																				T	Hao & Clem model using M(H)	13.9							T/K		0.47					A	Hao & Clem model using M(H)		48.6	5.9	A	Hao & Clem model using M(H)	1470																																																					grains were aligned in epoxy under H=11 T.					Three-dimensional superconductivity in the infinite-layer compound Sr0.9La0.1CuO2 in entire region below Tc			Department of Physics, National Creative Research Initiative Center for Superconductivity, Pohang University of Science and Technology, Pohang, South Korea	Solid State Commun., 123(2002)17	C.U.Jung,J.Y.Kim,Jae-Hyuk Choi,Mun-Seog Kim,Sung-Ik Lee		
33658	L089057002	pressure-induced s/c. 7<s/c<9 GPa. Tc(max)=8 K, at p=8 GPa. p-T phase diagram. Metal-insulator T=135 K.	Beta-NaxV2O5	Na0.33V2O5	Na	0.33	V	2																	O	5			2002																												bronze																		K				8	0		8																																																																																																Czochralski method					Pressure-Induced Superconductivity in Beta-Na0.33V2O5 beyond Charge Ordering			Material Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	Phys.Rev.Lett., 89(2002)57002	N.Mori,T.Yamauchi,Y.Ueda		
33659	DEN1100436	Tl:Sr:Ca:Cu=0.94:1.90:1.02:2 by ICP	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7	Tl	1	Sr	2	Ca	1	Cu	2													O	7		1	1990																												Tl1212			A	3.7851		12.104												K					4.2																																																																																																SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33660	DEN1100436	Tl:Sr:Ca:Y:Cu=1.00:1.90:0.77:2 by ICP	TlSr2(Ca,Y)Cu2O7	Tl1Sr2Ca0.8Y0.2Cu2O7	Tl	1	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	7		1	1990																												Tl1212			A	3.7933		12.0801												K	28		77.5				52.75																																																																																														SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33661	DEN1100436	Tl:Sr:Ca:Y:Cu=0.98:1.92:0.58:0.4:2 by ICP	TlSr2(Ca,Y)Cu2O7	Tl1Sr2Ca0.6Y0.4Cu2O7	Tl	1	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	7		1	1990																												Tl1212			A	3.797		12.045												K	58		78				68																																																																																														SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33662	DEN1100436	Tl:Sr:Ca:Y:Cu=1.02:1.91:0.38:0.62:2 by ICP	TlSr2(Ca,Y)Cu2O7	Tl1Sr2Ca0.4Y0.6Cu2O7	Tl	1	Sr	2	Ca	0.4	Y	0.6	Cu	2											O	7		1	1990																												Tl1212			A	3.802		12.0105												K		35	77				35																																																																																														SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33663	DEN1100436	Tl:Sr:Ca:Y:Cu=1.02:1.96:0.18:0.85:2 by ICP	TlSr2(Ca,Y)Cu2O7	Tl1Sr2Ca0.2Y0.8Cu2O7	Tl	1	Sr	2	Ca	0.2	Y	0.8	Cu	2											O	7		1	1990																												Tl1212			A	3.8074		11.9805												K					4.2																																																																																																SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33664	DEN1100436	Tl:Sr:Y:Cu=0.92:1.96:1.05:2 by ICP	TlSr2YCu2O7	Tl1Sr2Y1Cu2O7	Tl	1	Sr	2	Y	1	Cu	2													O	7		1	1990																												Tl1212			A	3.8154		11.978												K					4.2																																																																																																SrO,Y2O3,CuO,Tl2O3		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in air)					Crystal structure and superconductivity in TlSr2Ca1-xYxCu2O7			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Trans.Inst.Elec.Eng. of Japan, 110(1990)436	A.Soeda,N.Maki,S.Takeuchi,T.Doi,T.Kamo		
33665	JJP029L057	Tl:Sr:Ca:Cu=0.95:2:1:2 by ICP. 14 % of Ca-site occupied by Tl.	TlSr2CaCu2O7	Tl1Sr2Ca1Cu2O7	Tl	1	Sr	2	Ca	1	Cu	2													O	7		1	1990																												Tl1212	P4/mmm		A	3.7859		12.104																																																																																																																	Tl2O3,SrO,CaO,CuO		precursor(Sr-Ca-Cu-O) + Tl2O3, mixture - pellet - heat(870C,30h, in alumina crucible) - FC to RT					Rietvelt Refinement of the structure of TlSr2CaCu2O7 by X-ray powder diffraction data			Hitachi Research Lab, Hitachi Ltd., Hitachi, Ibaraki, Japan	Jpn. J.Appl.Phys.Part 2, 29(1990)L57	K.Usami,T.Doi,T.Kamo		
33666	P066092504	optimally doped. spin gap temp T*=180 K, dT*/dp=7.5 K/GPa.	(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+z	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+z			2002																												Hg1223																		K		131.5					131.5			K/GPa	1.5																																																																																												See text					Pressure studies on the pseudogap and critical temperatures of a high-Tc superconductor			Universidade Federal Fluminense, Niteroi, Brazil	Phys.Rev.B, 66(2002)92504	E.Baggio-Saitovich,E.S.Gaixeiro,E.V.L.de Mello,J.L.Gonzalez,M.T.D.Orlando		
33667	P066092504	optimally doped. spin gap temp T*=160 K, dT*/dp=6.3 K/GPa.	(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+z	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+z			2002																												Hg1223																		K		132					132			K/GPa	2.6																																																																																												See text					Pressure studies on the pseudogap and critical temperatures of a high-Tc superconductor			Universidade Federal Fluminense, Niteroi, Brazil	Phys.Rev.B, 66(2002)92504	E.Baggio-Saitovich,E.S.Gaixeiro,E.V.L.de Mello,J.L.Gonzalez,M.T.D.Orlando		
33668	P066104519		NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		1	2002																												Y123																		K		91.5					91.5																																																																		uV/K	8.09			TP33668																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33669	P066104519	dTc/dx=-170 K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.95Ca0.025Pr0.025Ba2Cu3O7-z	Nd	0.95	Ca	0.025	Pr	0.025	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		86.1					86.1																																																																		uV/K	9.85			TP33669																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33670	P066104519	dTc/dx=-170 K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.9Ca0.05Pr0.05Ba2Cu3O7-z	Nd	0.9	Ca	0.05	Pr	0.05	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		81.4					81.4																																																																		uV/K	10.94			TP33670																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33671	P066104519	dTc/dx=-170 K	(Nd,Ca,Pr)Ba2Cu3O7	Nd0.8Ca0.1Pr0.1Ba2Cu3O7-z	Nd	0.8	Ca	0.1	Pr	0.1	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		70.8					70.8																																																																		uV/K	12.04			TP33671																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33672	P066104519	Tc from Phys.Rev.B, 56(1997)2848. Tc=93.6-232x	NdBa2Cu3O7	Nd1Ba2Cu3O7-z	Nd	1	Ba	2	Cu	3															O	7-z		1	2002																												Y123																		K		93.6					93.6																																																																		uV/K	5.54			TP33672																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33673	P066104519	Tc from Phys.Rev.B, 56(1997)2848. Tc=93.6-232x	(Nd,Ca,Th)Ba2Cu3O7	Nd0.97Ca0.015Th0.015Ba2Cu3O7-z	Nd	0.97	Ca	0.015	Th	0.015	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		90.4					90.4																																																																		uV/K	9.37			TP33673																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33674	P066104519	Tc from Phys.Rev.B, 56(1997)2848. Tc=93.6-232x	(Nd,Ca,Th)Ba2Cu3O7	Nd0.94Ca0.03Th0.03Ba2Cu3O7-z	Nd	0.94	Ca	0.03	Th	0.03	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		86.8					86.8																																																																		uV/K	13.42			TP33674																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33675	P066104519	Tc from Phys.Rev.B, 56(1997)2848. Tc=93.6-232x	(Nd,Ca,Th)Ba2Cu3O7	Nd0.9Ca0.05Th0.05Ba2Cu3O7-z	Nd	0.9	Ca	0.05	Th	0.05	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		81.8					81.8																																																																		uV/K	15.76			TP33675																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33676	P066104519	Tc from Phys.Rev.B, 56(1997)2848. Tc=93.6-232x	(Nd,Ca,Th)Ba2Cu3O7	Nd0.8Ca0.1Th0.1Ba2Cu3O7-z	Nd	0.8	Ca	0.1	Th	0.1	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K		73.4					73.4																																																																		uV/K	12.64			TP33676																										See text					Thermoelectric power of charge-neutral Nd1-2xCaxMxBa2Cu3O7-z (M=Th and Pr): Evidence for different types of localization			Department of Microelectronics and Information Technology, Stockholm-Kista, Sweden	Phys.Rev.B, 66(2002)104519	M.Andersson,O.Rapp,S.R.Ghorbani		
33677	P066104528	RH(100K)=0.0052 cm3/C	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		3	2002																												T																		K		27					27																																																																																					cm3/C					4	RH33677					single crystals grown by TSFZ method under O2					Hall coefficient of La1.88-yYySr0.12CuO4(y=0, 0.04) at low temperatures under high magnetic fields			Department of Physics, Sophia University, Tokyo,Japan	Phys.Rev.B, 66(2002)104528	K.Chiba,K.Yamada,M.Fujita,M.Minami,T.Fukase,T.Goto,T.Suzuki,Y.Oshima		
33678	P066104528	structural phase transition at 90 K(to OLT phase) and 65 K(to TLT phase). RH(100K)=0.0055 cm3/C.	(La,Y,Sr)2CuO4	La1.84Y0.04Sr0.12Cu1O4	La	1.84	Y	0.04	Sr	0.12	Cu	1													O	4		3	2002																												T																		K		17					17																																																																																					cm3/C					4	RH33678					single crystals grown by TSFZ method under O2					Hall coefficient of La1.88-yYySr0.12CuO4(y=0, 0.04) at low temperatures under high magnetic fields			Department of Physics, Sophia University, Tokyo,Japan	Phys.Rev.B, 66(2002)104528	K.Chiba,K.Yamada,M.Fujita,M.Minami,T.Fukase,T.Goto,T.Suzuki,Y.Oshima		
33679	PR06100778	Hirr(T) = Hirr(0)(1-t)**n	Sr2(Sr,Ca)Cu2(O,Cl)6	Sr2.3Ca0.7Cu2Cl1.3O4+z	Sr	2.3	Ca	0.7	Cu	2	Cl	1.3													O	4+z		1	2000																											2	0212	I4/mmm		A	3.8679		22.161												K	60		80	80			80																																		HIR33679																																																														precursor(SrCuO3,SrCuO2, Ca2CuO3,Sr2CuO2Cl2) - high temperature synthesis(1000C,30min, p=5.0 GPa)					High-pressure synthesis and superconducting properties of the oxychloride superconductor (Sr,Ca)3Cu2O4+zCl2-y	200001		Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,61(2000)778-783	C.-Q.Jin,H.Yamauchi,K.Tanabe,R.Puzniak,S.Adachi,S.Tanaka,T.Tamura,T.Tatsuski,X.-J.Wu,Z.-X.Zhao		
33680	EPJ0290369	spin gap = 20 K. spin gap temp T* = 20 K.	(La,Sr)2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		4	2002																												T																		K					1.5																																																																																																		DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33681	EPJ0290369	spin gap = 308 K. 	(La,Sr)2CuO4	La1.955Sr0.045Cu1O4	La	1.955	Sr	0.045	Cu	1															O	4		4	2002																												T																		K					1.5																																																																																																		DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33682	EPJ0290369	spin gap = 300 K. 	(La,Sr)2CuO4	La1.945Sr0.055Cu1O4	La	1.945	Sr	0.055	Cu	1															O	4		4	2002																												T																		K					1.5																																																																																																		DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33683	EPJ0290369	spin gap = 270 K. 	(La,Sr)2CuO4	La1.94Sr0.06Cu1O4	La	1.94	Sr	0.06	Cu	1															O	4		4	2002																												T																		K		2.8					2.8																																																																																																DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33684	EPJ0290369	spin gap = 229 K. spin gap temp T* = 343 K.	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		4	2002																												T																		K		18					18																																																																																																DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33685	EPJ0290369	spin gap = 130 K. spin gap temp T* = 221 K.	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		4	2002																												T																		K		22.3					22.3																																																																																																DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33686	EPJ0290369		(La,Sr)2CuO4	La1.75Sr0.25Cu1O4	La	1.75	Sr	0.25	Cu	1															O	4		4	2002																												T																		K		16.5					16.5																																																																																																DC sputtering from stoichiometric target on SrTiO3					High field transport properties of La2-xSrxCuO4 epitaxial thin films			Katholieke Universiteit Leuven, Celestijnenlaan, Belgium	Eur.Phys.J.B, 29(2002)369	J.Vanacken,L.Weckhuysen,P.Wagner,V.V.Moshchalkov		
33687	P066132510	high pressure synthesis. no modulation	YSr2Cu3Oz	Y1Sr2Cu3O7.2	Y	1	Sr	2	Cu	3															O	z	7.2	1	2002																												Y123			A	3.7903		11.3992												K		64					64																																																																																																high pressure synthesis					Superconductivity and microstructure of YSr2Cu3O6.875			EMAT,Unversity of Antwerp, Antwerp,Belgium	Phys.Rev.B, 66(2002)132510	A.Gauzzi,A.Prodi,E.Gilioli,F.Licci,G.Van Tendeloo,M.Marezio,O.I.Lebedev		
33688	P066132510	#33687 , then ANN(290C,10h, in 2 atm O2). c/a ratio = 2.95	YSr2Cu3Oz	Y1Sr2Cu3O6.92	Y	1	Sr	2	Cu	3															O	z	6.92	1	2002																												Y123																		K		68					68																																																																																																high pressure synthesis					Superconductivity and microstructure of YSr2Cu3O6.875			EMAT,Unversity of Antwerp, Antwerp,Belgium	Phys.Rev.B, 66(2002)132510	A.Gauzzi,A.Prodi,E.Gilioli,F.Licci,G.Van Tendeloo,M.Marezio,O.I.Lebedev		
33689	P066134508	interlayer distance=1.60 nm by Koshelev's model.  = 1.47 nm by XRD.	Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8	Tl	2	Ba	2	Ca	1	Cu	2													O	8		3	2002																												Tl2212			A			29.3												K				105			105																				T	WHH theory			161					T/K				2.11			A	in clean limit		14.3		A	by BLK model using M(H) data		2479																																																		Tl2O3, Ba2CaCu2Oz		(precursor(Ba2CaCu2Oz)+Tl2O3) - mixture - sealed in quartz(in Al2O3 crusible) - heat(950C,15 min) - cool to 900C(3C/h). ANN(400C,48h,in O2)					Equilibrium magnetization of Tl2Ba2CaCu2O8+z single crystal			Pohang University of Science and Technology, Pohang, Korea	Phys.Rev.B, 66(2002)134508	Heon-Jung Kim,In-Sun Jo,P.Chowdhury,Sung-Ik Lee		
33690	P066144503	As lowering Tc, metal-AFM(175K) - weak FM(100K) - S/C(42K) transitions. dHc2/dT=0.38 T/K near Tc.	Ru(Gd,Ce)2Sr2Cu2O10	Ru1Gd1.4Ce0.6Sr2Cu2O10+z	Ru	1	Gd	1.4	Ce	0.6	Sr	2	Cu	2											O	10+z		1	2002							100	175																				Ru1222			A	3.835		28.56												K		36	42				36																				T	WHH using Tc=39K, dHc2/dT=1.13 T/K	31							T/K		1.13					A		28																																																										sol-gel method. (100C,12h,in O2 flow) +  two times of heat(800C,24h,in 95 atm O2) 					Upper critical field of the magnetic superconductor RuGd1.4Ce0.6Sr2Cu2O10-z			Universidade de Sao Paulo, Sao Paulo, Brazil	Phys.Rev.B, 66(2002)144503	A.H.Lacerda,L.Ben-Dor,M.S.Torikachvili,M.T.Escote,R.F.Jardim,V.A.Meza		
33691	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	z	6.45	3	2002																												Y123																		K		20					20																				T	calculated from coherence length			24.7												A	Aslamazov-Larkin orbital fitting		37.3																											uV/K																			E-3 cm3/C	7.76										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33692	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	z	6.5	3	2002																												Y123																		K		35.5					35.5																				T	calculated from coherence length			31.6												A	Aslamazov-Larkin orbital fitting		32.6																											uV/K	71.4																		E-3 cm3/C	5.06										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33693	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.65	Y	1	Ba	2	Cu	3															O	z	6.65	3	2002																												Y123																		K		56.3					56.3																				T	calculated from coherence length			53.7												A	Aslamazov-Larkin orbital fitting		25.5																											uV/K	34.2			TP33693															E-3 cm3/C	2.7					RH33693					single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33694	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	z	6.7	3	2002																												Y123																		K		59.1					59.1																				T	calculated from coherence length			35.3												A	Aslamazov-Larkin orbital fitting		31																											uV/K	22.8			TP33694															E-3 cm3/C	1.7					RH33694					single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33695	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	z	6.75	3	2002																												Y123																		K		62.1					62.1																				T	calculated from coherence length			44.6												A	Aslamazov-Larkin orbital fitting		27.6																											uV/K	15.3																		E-3 cm3/C	1.43										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33696	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	3	2002																												Y123																		K		69.2					69.2																				T	calculated from coherence length			54.6												A	Aslamazov-Larkin orbital fitting		24.9																											uV/K	10.1																		E-3 cm3/C	1.2										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33697	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	z	6.85	3	2002																												Y123																		K		83.2					83.2																				T	calculated from coherence length			108												A	Aslamazov-Larkin orbital fitting		17.8																											uV/K	4.89																		E-3 cm3/C	1.12										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33698	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O6.95	Y	1	Ba	2	Cu	3															O	z	6.95	3	2002																												Y123																		K		93.4					93.4																				T	calculated from coherence length			280												A	Aslamazov-Larkin orbital fitting		11.3																											uV/K	-1.96																		E-3 cm3/C	0.66										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33699	L088167005	detwinned single crystal. TP300, RH300 from PRL0864907	YBa2Cu3Oz	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	z	7	3	2002																												Y123																		K		92					92																				T	calculated from coherence length			394												A	Aslamazov-Larkin orbital fitting		9.51																											uV/K	-7.17																		E-3 cm3/C	0.46										single crystals were grown in Y2O3 crucible by flux method, then detwinned.					Magnetoresistance of untwinned YBa2Cu3Oy single crystals in a wide range of doping: Anomalous hole-doping dependence of the coherence length			Central Research Institute of Electric Power Industry, Komae,Tokyo,Japan	Phys.Rev.Lett., 88(2002)167005	K.Segawa,Y.Ando		
33700	L088247001	For static P, Tc has no change upto 0.13 GPa. For uniaxial P, Tc increase beyond p=0.04 GPa(P//c). dTc/dP=24 K/GPa.	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2002																												T																		K		8					8			K/GPa	19																																																																																												crystals were grown by TSFZ method. Then ANN(900C, in flowing O2)					Competition of Static Stripe and Superconducting Phases in La1.48Nd0.4Sr0.12CuO4 Controlled by Pressure			Department of Physics, Bharathidasan University, Tiruchirappalli -620 024, India	Phys.Rev.Lett., 88(2002)247001	H.Eisaki,H.Takashima,N.Mori,N.Takeshita,S.Arumugam,S.Uchida,T.Noda		
33701	L089147002	muon-SR measured at 20 mK<T<4 K.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2002																												pyrochlore																		K		1					1																				T																A		260			A	muon-SR	7500																																																					single crystals were grown by vapor transport method					Temperature dependence of the magnetic penetration depth in the vortex state of the pyroclore superconductor, Cd2Re2O7			Solid State Division, Oak Ridge National Lab, Oak Ridge, Tennessee, USA	Phys.Rev.Lett., 89(2002)147002	D.Mandrus,J.E.Sonier,J.He,J.S.Cardner,M.D.Lumsden,R.F.Kiefl,R.I.Miller,R.Jin,S.R.Dunsiger,S.T.Bramwell		
33702	PHC3820395		RuSr2ErCu2O8	Ru1Sr2Er1Cu2O8	Ru	1	Sr	2	Er	1	Cu	2													O	8			2002																												Ru1212			A	3.8178		11.521																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33703	PHC3820395	susceptibility peak at 31K is due to Sr2RuHoO6	RuSr2HoCu2O8	Ru1Sr2Ho1Cu2O8	Ru	1	Sr	2	Ho	1	Cu	2													O	8			2002								148																				Ru1212			A	3.8266		11.5341																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33704	PHC3820395	susceptibility peak at 33K is due to Sr2RuYO6	RuSr2YCu2O8	Ru1Sr2Y1Cu2O8	Ru	1	Sr	2	Y	1	Cu	2													O	8			2002								141																				Ru1212			A	3.8268		11.5303																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33705	PHC3820395		RuSr2DyCu2O8	Ru1Sr2Dy1Cu2O8	Ru	1	Sr	2	Dy	1	Cu	2													O	8			2002																												Ru1212			A	3.8352		11.5354																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33706	PHC3820395		RuSr2TbCu2O8	Ru1Sr2Tb1Cu2O8	Ru	1	Sr	2	Tb	1	Cu	2													O	8			2002																												Ru1212			A	3.832		11.543																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33707	PHC3820395		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2002																												Ru1212			A	3.8341		11.5479																																																																																																																	RuO2,SrCuO2,R2O3		high pressure synthesis(20-80 kbar, 1073-1473 K) using belt-type apparatus					Lanthanide substitution by high pressure in the RuSr2GdCu2O8 magnetic superconductor			Universidad Complutense de Madrid, Madrid, Spain	Physica C, 382(2002)395-400	E.Moran,J.M.Gallardo-Amores,M.A.Alario-Franco,R.Ruiz-Bustos,R.Saez-Puche		
33708	PHC3830048	Jc from magnetization. Jc(70K,0T)=8.0 E+8 A/cm2. Jc(70K,1T)=6.8 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2002																												Y123			A	3.897	3.888	11.691												K	90.3	93					93																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33709	PHC3830048	Jc from magnetization. Jc(70K,0T)=7.8 E+8 A/cm2. Jc(70K,1T)=7.0 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.98Pr0.02Ba2Cu3O7-z	Y	0.98	Pr	0.02	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.898	3.888	11.693												K	90.6	92.2					92.2																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33710	PHC3830048	Jc from magnetization. Jc(70K,0T)=7.4 E+8 A/cm2. Jc(70K,1T)=7.9 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.96Pr0.04Ba2Cu3O7-z	Y	0.96	Pr	0.04	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.897	3.887	11.691												K	90.4	92					92																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33711	PHC3830048	Jc from magnetization. Jc(70K,0T)=7.3 E+8 A/cm2. Jc(70K,1T)=7.8 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.94Pr0.06Ba2Cu3O7-z	Y	0.94	Pr	0.06	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.897	3.889	11.691												K	89.6	91.5					91.5																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33712	PHC3830048	Jc from magnetization. Jc(70K,0T)=6.4 E+8 A/cm2. Jc(70K,1T)=7.9 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.92Pr0.08Ba2Cu3O7-z	Y	0.92	Pr	0.08	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.894	3.886	11.682												K	88.4	90.5					90.5																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33713	PHC3830048		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.895	3.888	11.686												K	86.6	89.2					89.2																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33714	PHC3830048	Jc from magnetization. Jc(70K,0T)=5.0 E+8 A/cm2. Jc(70K,1T)=5.0 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.85Pr0.15Ba2Cu3O7-z	Y	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.902	3.892	11.705												K	82	84.5					84.5																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33715	PHC3830048	Jc from magnetization. Jc(70K,0T)=3.0 E+8 A/cm2. Jc(70K,1T)=0.0 E+7 A/cm2	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.915	3.907	11.746												K	76.3	79.5					79.5																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33716	PHC3830048		(Y,Pr)Ba2Cu3O7	Y0.75Pr0.25Ba2Cu3O7-z	Y	0.75	Pr	0.25	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.915	3.907	11.746												K	68.5	72					72																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33717	PHC3830048		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z		1	2002																												Y123			A	3.894	3.887	11.684												K	60.3	64					64																																																																																															1	solid state reaction. final annealing (400C,24h, in flowing O2)					The effect of Pr-doping on the critical current density in YBa2Cu3O7-z			Department of Fundamental Energy Science, kyoto University,Gokasho, Uji, kyoto-fu, Japan	Physica C, 383(2002)48-54	K.Yoshida,T.Harada		
33718	PHC3830075	high quarity Pb-free Bi-2223 single crystal(98-99% Bi-2223 phase). RESN at 108K, 126K	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10+z	Bi	2	Sr	2	Ca	2	Cu	3													O	10+z		3	2002																												Bi2223			A	5.408	5.413	36.868												K		110					110	RES33718																																																																						mOhm.cm								0.67	33700	126		1.1	18400												TSFZ method. growth rate = 0.04 mm/h. ANN(850C, 500h in  O2 flow)					Single crystals of triple-layered cuprates Bi2Sr2Ca2Cu3O10+z; growth, annealing and characterization			Max-Planck-Institut fur Festkorperforschung,Stuttgart, Germany	Physica C, 383(2002)75-88	B.Liang,C.T.Lin,G.Yang,P.Shang		
33719	PHC3830122	textured crystal.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			2002																												Bi2212			A	5.41	5.4	30.81												K				84			84																																																																																																textured crystals were grown at 1mm/h rate. by floating zone method.					Substitutional effect of Mn on floating zone growth Bi-2212 bulk textured crystals			Crystal Growth Center, Anna University,Chennai, India	Physica C, 383(2002)122-126	E.Srinivasan,R.Jayavel,S.Subramanian,S.Uthayakumar		
33720	PHC3830122	textured crystal.	Bi2Sr2Ca(Cu,Mn)2O8	Bi2Sr2Ca1Cu1.9Mn0.1O8+z	Bi	2	Sr	2	Ca	1	Cu	1.9	Mn	0.1											O	8+z			2002																												Bi2212																		K				66			66																																																																																																textured crystals were grown at 1mm/h rate. by floating zone method.					Substitutional effect of Mn on floating zone growth Bi-2212 bulk textured crystals			Crystal Growth Center, Anna University,Chennai, India	Physica C, 383(2002)122-126	E.Srinivasan,R.Jayavel,S.Subramanian,S.Uthayakumar		
33721	PHC3830122	textured crystal.	Bi2Sr2Ca(Cu,Mn)2O8	Bi2Sr2Ca1Cu1.8Mn0.2O8+z	Bi	2	Sr	2	Ca	1	Cu	1.8	Mn	0.2											O	8+z			2002																												Bi2212																		K				53			53																																																																																																textured crystals were grown at 1mm/h rate. by floating zone method.					Substitutional effect of Mn on floating zone growth Bi-2212 bulk textured crystals			Crystal Growth Center, Anna University,Chennai, India	Physica C, 383(2002)122-126	E.Srinivasan,R.Jayavel,S.Subramanian,S.Uthayakumar		
33722	PHC3830122	textured crystal.	Bi2Sr2Ca(Cu,Mn)2O8	Bi2Sr2Ca1Cu1.7Mn0.3O8+z	Bi	2	Sr	2	Ca	1	Cu	1.7	Mn	0.3											O	8+z			2002																												Bi2212																		K				40			40																																																																																																textured crystals were grown at 1mm/h rate. by floating zone method.					Substitutional effect of Mn on floating zone growth Bi-2212 bulk textured crystals			Crystal Growth Center, Anna University,Chennai, India	Physica C, 383(2002)122-126	E.Srinivasan,R.Jayavel,S.Subramanian,S.Uthayakumar		
33723	PHC3830122	textured crystal. not s/c.	Bi2Sr2Ca(Cu,Mn)2O8	Bi2Sr2Ca1Cu1.6Mn0.4O8+z	Bi	2	Sr	2	Ca	1	Cu	1.6	Mn	0.4											O	8+z			2002																												Bi2212																		K					10																																																																																																		textured crystals were grown at 1mm/h rate. by floating zone method.					Substitutional effect of Mn on floating zone growth Bi-2212 bulk textured crystals			Crystal Growth Center, Anna University,Chennai, India	Physica C, 383(2002)122-126	E.Srinivasan,R.Jayavel,S.Subramanian,S.Uthayakumar		
33724	EPJ0190005	isotope effect of pseudogap temp T*. T*(Cu<65>) - T*(Cu<63>) = 185-160 = 25 K. alpha(T*) = -4.9	HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K				79			79							Cu																																																																																									high O2 pressure solid state reaction (1000C,450 bar O2,60h)					Large copper isotope effect on the pseudogap in the high-temperature superconductor HoBa2Cu4O8			ETH Zurich & PSI Villigen, Villigen PSI, Switzerland	Eur.Phys.J.B, 19(2001)5-8	A.Furrer,A.Sokolov,D.Rubio Temprano,J.Karpinski,J.Mesot,K.A.Muller,K.Conder,S.Janssen,S.M.Kazakov,V.Trounov		
33725	EPJ0190005	isotope effect of pseudogap temp T*. T*(O<18>) - T*(O<16>) = 220-170 = 50 K. alpha(T*) = -2.2	HoBa2Cu4O8	Ho1Ba2Cu4O8	Ho	1	Ba	2	Cu	4															O	8		1	2001																												Y124																		K				79			79							O																																																																																									high O2 pressure solid state reaction (1000C,450 bar O2,60h)					Large copper isotope effect on the pseudogap in the high-temperature superconductor HoBa2Cu4O8			ETH Zurich & PSI Villigen, Villigen PSI, Switzerland	Eur.Phys.J.B, 19(2001)5-8	A.Furrer,A.Sokolov,D.Rubio Temprano,J.Karpinski,J.Mesot,K.A.Muller,K.Conder,S.Janssen,S.M.Kazakov,V.Trounov		
33726	P066214509	c-axis aligned sample. anisotropy = 9.3. G-L//c-axis = 25.3	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2002																												IL			A	3.95		3.41												K				42.7			42.7											Oe	magnetization, Hao & Clem analysis			336					T	magnetization, Hao & Clem analysis			13.9												A	magnetization, Hao & Clem analysis		48.6	5.2	nm	magnetization, Hao & Clem analysis		147																																																				mixture - CAL(950C,36h) - high pressure synthesis(4 GPa)					Anisotropy and reversible magnetization of the infinite-layer superconductor Sr0.9La0.1CuO2			Department of Physics, Ohio State University,Columbus,Ohio,USA	Phys.Rev.B, 66(2002)214509	C.U.Jung,Heon-Jung Kim,J.Y.Kim,Jae-Hyuk Choi,Mun-Seog Kim,Sung-Ik Lee,T.R.Lemberger		
33727	P066184506	optimally O-doped. pseudogap-T, T* = 60 K. T*(O<18>) = 70 K(i.e. dT*=10 K). T* from neutron experiments.	(La,Ho,Sr)2CuO4	La1.81Ho0.04Sr0.15Cu1O4	La	1.81	Ho	0.04	Sr	0.15	Cu	1													O	4		1	2002																												T																		K				32			32						0.11	O	81																																																																																								solid state reaction .using O<18>, Cu<65> isotope.					Oxygen and copper isotope effects on the pseudogap in the high-temperature superconductor La1.81Ho0.04Sr0.15CuO4 studied by neutron crystal-field spectroscopy			ETH Zurich & PSI Villigen, Villigen PSI, Switzerland	Phys.Rev.B, 66(2002)184506	A.Furrer,D.Rubio Temprano,H.Mutka,K.A.Muller,K.Conder,V.Trounov		
33728	P066184506	optimally O-doped. pseudogap-T, T* = 60 K. T*(Cu<65>) = 60 K(i.e. dT*=0 K). T* from neutron experiments.	(La,Ho,Sr)2CuO4	La1.81Ho0.04Sr0.15Cu1O4	La	1.81	Ho	0.04	Sr	0.15	Cu	1													O	4		1	2002																												T																		K				32			32						0.29	Cu																																																																																									solid state reaction .using O<18>, Cu<65> isotope.					Oxygen and copper isotope effects on the pseudogap in the high-temperature superconductor La1.81Ho0.04Sr0.15CuO4 studied by neutron crystal-field spectroscopy			ETH Zurich & PSI Villigen, Villigen PSI, Switzerland	Phys.Rev.B, 66(2002)184506	A.Furrer,D.Rubio Temprano,H.Mutka,K.A.Muller,K.Conder,V.Trounov		
33729	PHC3830337	dTc/dp = 1.02 K/GPa(susceptibility). Ferromag Tm=123 K. dTm/dp = 6.7 K/GPa.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2003							123																					Ru1212																		K		42.4		43.8			42.4			K/GPa	1.06																																																																																										RuO2,Gd2O3,SrCO3,CuO	1	mixture-preheat(600-800C,12h)-CAL(960C,16h) - SIN(1015-1060C) - SIN(1065,10d, in O2)					Pressure effect on the superconducting and magnetic transitions of the superconducting ferromagnet RuSr2GdCu2O8			Texas Center for Superconductivity and Department of Physics , University of Houston, Houston, Texas,USA	Physica C, 383(2003)337	B.Lorenz,C.W.Chu,R.L.Meng,Y.Y.Xue		
33730	PHC3840343	starting= Ba0.6K0.45BiO3.1	(Ba,K)BiO3	Ba0.635K0.365Bi1O3	Ba	0.635	K	0.365	Bi	1															O	3		1	2003																												BKBO			A	4.2938														K				30.4			30.4																																																																																																high pressure synthesis (5GPa, 900C, 1h)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33731	PHC3840343	starting=Ba0.5K0.52BiO3.04	(Ba,K)BiO3	Ba0.557K0.443Bi1O3	Ba	0.557	K	0.443	Bi	1															O	3		1	2003																												BKBO			A	4.2734														K				25			25																																																																																																high pressure synthesis (5GPa, 900C, 1h)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33732	PHC3840343	starting=Ba0.4K0.63BiO3.16	(Ba,K)BiO3	Ba0.445K0.555Bi1O3	Ba	0.445	K	0.555	Bi	1															O	3		1	2003																												BKBO			A	4.248														K				14			14																																																																																																high pressure synthesis (5GPa, 900C, 1h)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33733	PHC3840343	starting=Ba0.3K0.74BiO3.28	(Ba,K)BiO3	Ba0.34K0.66Bi1O3	Ba	0.34	K	0.66	Bi	1															O	3		1	2003																												BKBO			A	4.2353														K				7			7																																																																																																high pressure synthesis (5GPa, 900C, 1h)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33734	PHC3840343	starting=Ba0.2K0.84BiO3.38	(Ba,K)BiO3	Ba0.257K0.743Bi1O3	Ba	0.257	K	0.743	Bi	1															O	3		1	2003																												BKBO			A	4.215														K					3																																																																																																		high pressure synthesis (5GPa, 900C, 1h)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33735	PHC3840343	starting=KBiO3.5	(K,Bi)BiO3	K0.92Bi1.08O3	K	0.92	Bi	1.08																	O	3		1	2003																												BKBO			A	4.2041														K				0			0																																																																																																high pressure synthesis (7 GPa, 1000C)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33736	PHC3840343	starting=K1.05BiO3.6	(K,Bi)BiO3	K0.915Bi1.085O3	K	0.915	Bi	1.085																	O	3		1	2003																												BKBO			A	4.2223														K				9			9																																																																																																high pressure synthesis (7 GPa, 1000C)					High pressure synthesis and superconductivity of Ba1-xKxBiO3 (0.35<x<1)			Seoul National University, Seoul, South Korea	Physica C, 383(2003)343	A.N.Baranov,B.J.Kim,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.C.Kim,Y.W.Park		
33737	JCG2110471		(Ba,K)BiO3	Ba0.33K0.67Bi1O3	Ba	0.33	K	0.67	Bi	1															O	3			2000																												BKBO	Pm3-m		A	4.238														K		0.77					0.77																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33738	JCG2110471		(Ba,K)BiO3	Ba0.35K0.65Bi1O3	Ba	0.35	K	0.65	Bi	1															O	3			2000																												BKBO	Pm3-m		A	4.241														K		1.88					1.88																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33739	JCG2110471		(Ba,K)BiO3	Ba0.4K0.6Bi1O3	Ba	0.4	K	0.6	Bi	1															O	3			2000																												BKBO	Pm3-m		A	4.25														K		7.2					7.2																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33740	JCG2110471		(Ba,K)BiO3	Ba0.45K0.55Bi1O3	Ba	0.45	K	0.55	Bi	1															O	3			2000																												BKBO	Pm3-m		A	4.259														K		12.7					12.7																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33741	JCG2110471		(Ba,K)BiO3	Ba0.5K0.5Bi1O3	Ba	0.5	K	0.5	Bi	1															O	3			2000																												BKBO	Pm3-m		A	4.267														K		18.6					18.6																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33742	JCG2110471		(Ba,K)BiO3	Ba0.644K0.356Bi1O3	Ba	0.644	K	0.356	Bi	1															O	3			2000																												BKBO																		K		29					29																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33743	JCG2110471		(Ba,K)BiO3	Ba0.613K0.387Bi1O3	Ba	0.613	K	0.387	Bi	1															O	3			2000																												BKBO																		K		30.7					30.7																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33744	JCG2110471		(Ba,K)BiO3	Ba0.584K0.416Bi1O3	Ba	0.584	K	0.416	Bi	1															O	3			2000																												BKBO																		K		28.8					28.8																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33745	JCG2110471		(Ba,K)BiO3	Ba0.553K0.447Bi1O3	Ba	0.553	K	0.447	Bi	1															O	3			2000																												BKBO																		K		25.5					25.5																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33746	JCG2110471		(Ba,K)BiO3	Ba0.542K0.458Bi1O3	Ba	0.542	K	0.458	Bi	1															O	3			2000																												BKBO																		K		23.1					23.1																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33747	JCG2110471		(Ba,K)BiO3	Ba0.595K0.405Bi1O3	Ba	0.595	K	0.405	Bi	1															O	3			2000																												BKBO																		K		31.2					31.2																																																																																																electrochemical growth using KOH flux					Electrochemical growth near the Ba1-xKxBiO3(x>0.5) - Ba1.7K1.3Bi2O7 boundary and the crystals properties			Institute of Solid State and Semiconductors Physics, Academy of Science, Minsk,Belarus	J.Crystal Growth, 211(2000)471-475	H.Szymczak,M.Baran,R.Szymczak,S.N.Barilo,S.N.Ustinovich,S.V.Shiryaev,V.I.Gatalskaya,V.V.Fedotova		
33748	PCS0601933		(Ba,K)BiO3	Ba0.665K0.335Bi1O2.985	Ba	0.665	K	0.335	Bi	1															O	3	2.985		1999																												BKBO																		K		27.3					27.3																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33749	PCS0601933		(Ba,K)BiO3	Ba0.66K0.34Bi1O3	Ba	0.66	K	0.34	Bi	1															O	3			1999																												BKBO																		K		26.2					26.2																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33750	PCS0601933		(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3			1999																												BKBO																		K		28.3					28.3																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33751	PCS0601933		(Ba,K)BiO3	Ba0.6K0.4Bi1O2.977	Ba	0.6	K	0.4	Bi	1															O	3	2.977		1999																												BKBO																		K		29					29																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33752	PCS0601933		(Ba,K)BiO3	Ba0.57K0.43Bi1O2.983	Ba	0.57	K	0.43	Bi	1															O	3	2.983		1999																												BKBO																		K		25.6					25.6																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33753	PCS0601933		(Ba,K)BiO3	Ba0.51K0.49Bi1O2.974	Ba	0.51	K	0.49	Bi	1															O	3	2.974		1999																												BKBO																		K		22.2					22.2																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33754	PCS0601933		(Ba,K)BiO3	Ba0.46K0.56Bi1O2.965	Ba	0.46	K	0.56	Bi	1															O	3	2.965		1999																												BKBO																		K		14.8					14.8																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33755	PCS0601933		(Ba,K)BiO3	Ba0.37K0.63Bi1O2.952	Ba	0.37	K	0.63	Bi	1															O	3	2.952		1999																												BKBO																		K		8.71					8.71																																																																																																electrochemical growth using KOH flux					Normal-state transport properties of Ba1-xKxBiO3 crystals			College of Science and Engineering, Aoyama Gakuin University,Setagaya, Tokyo,Japan	J.Phys.Chem.Solids, 60(1999)1933	A.Mishiro,H.Samata,M.Ohtsuka,T.Uchida,Y.Nagata		
33756	PHC3830315	as-prepared. Rietveld analysis shows Ru(Sr1.82Nd0.18)(Nd1.2Ce0.8)Cu2O10	RuSr2(Nd,Ce)2Cu2O10	Ru1Sr2Nd1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Nd	1.4	Ce	0.6	Cu	2											O	10-z			2003																												Ru1222			A	3.848		28.382												K					4.2																																																																																																RuO2,SrCO3,Nd2O3,CeO2,CuO	1	mixture-preheat(960C,8h,in air)-pellet-heat(1010C,8h,in O2)-heat(1050C,10h,in air)					Synthesis, crystal structure and properties of superconducting and non-superconducting RuSr2(Nd,Ce)2Cu2O10 phases			M.V.Lomonosov State Academy of Fine Chemical Technology,Moscow,Russia	Physica C, 383(2003)315	A.S.Andreenko,E.P.Khlybov,G.M.Kuz'micheva,I.E.Kostyleva,Yu.V.Esaulova		
33757	PHC3830315	ANN(400C,4h,in O2). Rietveld analysis shows (Ru0.67Cu0.33)(Sr1.66Nd0.34(Nd1.2Ce0.8)Cu2O9.74	RuSr2(Nd,Ce)2Cu2O10	Ru1Sr2Nd1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Nd	1.4	Ce	0.6	Cu	2											O	10-z			2003																												Ru1222			A	3.849		28.575												K		40					40																																																																																														RuO2,SrCO3,Nd2O3,CeO2,CuO	1	mixture-preheat(960C,8h,in air)-pellet-heat(1010C,8h,in O2)-heat(1050C,10h,in air)					Synthesis, crystal structure and properties of superconducting and non-superconducting RuSr2(Nd,Ce)2Cu2O10 phases			M.V.Lomonosov State Academy of Fine Chemical Technology,Moscow,Russia	Physica C, 383(2003)315	A.S.Andreenko,E.P.Khlybov,G.M.Kuz'micheva,I.E.Kostyleva,Yu.V.Esaulova		
33758	PHC3830315	ANN(700C,8h,in 350 atm O2). Rietveld analysis shows (Ru0.59Cu0.41)(Sr1.12Nd0.88)(Nd1.2Ce0.8)Cu2O10	RuSr2(Nd,Ce)2Cu2O10	Ru1Sr2Nd1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Nd	1.4	Ce	0.6	Cu	2											O	10-z			2003																												Ru1222			A	3.87		28.487												K					4.2																																																																																																RuO2,SrCO3,Nd2O3,CeO2,CuO	1	mixture-preheat(960C,8h,in air)-pellet-heat(1010C,8h,in O2)-heat(1050C,10h,in air)					Synthesis, crystal structure and properties of superconducting and non-superconducting RuSr2(Nd,Ce)2Cu2O10 phases			M.V.Lomonosov State Academy of Fine Chemical Technology,Moscow,Russia	Physica C, 383(2003)315	A.S.Andreenko,E.P.Khlybov,G.M.Kuz'micheva,I.E.Kostyleva,Yu.V.Esaulova		
33759	PHC3830315	2 times ANN(700C,8h,in 350 atm O2). Rietveld analysis shows (Ru0.62Cu0.38)(Sr1.41Nd0.59)(Nd1.2Ce0.8)Cu2O10	RuSr2(Nd,Ce)2Cu2O10	Ru1Sr2Nd1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Nd	1.4	Ce	0.6	Cu	2											O	10-z			2003																												Ru1222			A	3.861		28.502												K					4.2																																																																																																RuO2,SrCO3,Nd2O3,CeO2,CuO	1	mixture-preheat(960C,8h,in air)-pellet-heat(1010C,8h,in O2)-heat(1050C,10h,in air)					Synthesis, crystal structure and properties of superconducting and non-superconducting RuSr2(Nd,Ce)2Cu2O10 phases			M.V.Lomonosov State Academy of Fine Chemical Technology,Moscow,Russia	Physica C, 383(2003)315	A.S.Andreenko,E.P.Khlybov,G.M.Kuz'micheva,I.E.Kostyleva,Yu.V.Esaulova		
33760	PHC3830365		(Hg,Re)(Ba,Sr)2Ca2Cu3O8	Hg0.85Re0.15Ba2Ca2Cu3O8	Hg	0.85	Re	0.15	Ba	2	Ca	2	Cu	3											O	8			2003																												Hg1223			A			15.697												K	132.9						132.9																																		HIR33760																																																														precursor(Ba2Ca2Cu3Oz)+HgO - wrapped(Au foil) - sealed(quartz tube) - heat to 700C(300C/h) - heat to 835C (120C/h) - cool to RT(120C/h)					The resistive transition of (Hg0.85Re0.15)(Ba1-ySry)2Ca2Cu3O8+z superconducting polycrystals			Superconductivity Lab,IMRE-Physics Faculty, University of Havana, Havana,Cuba	Physica C, 383(2003)365	A.J.Batista-Leyva,E.Altshuler,L.Rivero,M.T.D.Orlando,R.Cobas		
33761	PHC3830365		(Hg,Re)(Ba,Sr)2Ca2Cu3O8	Hg0.85Re0.15Ba1.66Sr0.34Ca2Cu3O8	Hg	0.85	Re	0.15	Ba	1.66	Sr	0.34	Ca	2	Cu	3									O	8			2003																												Hg1223			A			15.632												K	131.3						131.3																																																																																																precursor(Ba2Ca2Cu3Oz)+HgO - wrapped(Au foil) - sealed(quartz tube) - heat to 700C(300C/h) - heat to 835C (120C/h) - cool to RT(120C/h)					The resistive transition of (Hg0.85Re0.15)(Ba1-ySry)2Ca2Cu3O8+z superconducting polycrystals			Superconductivity Lab,IMRE-Physics Faculty, University of Havana, Havana,Cuba	Physica C, 383(2003)365	A.J.Batista-Leyva,E.Altshuler,L.Rivero,M.T.D.Orlando,R.Cobas		
33762	PHC3830365		(Hg,Re)(Ba,Sr)2Ca2Cu3O8	Hg0.85Re0.15Ba1.6Sr0.4Ca2Cu3O8	Hg	0.85	Re	0.15	Ba	1.6	Sr	0.4	Ca	2	Cu	3									O	8			2003																												Hg1223			A			15.625												K	130.3						130.3																																																																																																precursor(Ba2Ca2Cu3Oz)+HgO - wrapped(Au foil) - sealed(quartz tube) - heat to 700C(300C/h) - heat to 835C (120C/h) - cool to RT(120C/h)					The resistive transition of (Hg0.85Re0.15)(Ba1-ySry)2Ca2Cu3O8+z superconducting polycrystals			Superconductivity Lab,IMRE-Physics Faculty, University of Havana, Havana,Cuba	Physica C, 383(2003)365	A.J.Batista-Leyva,E.Altshuler,L.Rivero,M.T.D.Orlando,R.Cobas		
33763	PHC3830365		(Hg,Re)(Ba,Sr)2Ca2Cu3O8	Hg0.85Re0.15Ba1.44Sr0.56Ca2Cu3O8	Hg	0.85	Re	0.15	Ba	1.44	Sr	0.56	Ca	2	Cu	3									O	8			2003																												Hg1223			A			15.6												K	128.7						128.7																																																																																																precursor(Ba2Ca2Cu3Oz)+HgO - wrapped(Au foil) - sealed(quartz tube) - heat to 700C(300C/h) - heat to 835C (120C/h) - cool to RT(120C/h)					The resistive transition of (Hg0.85Re0.15)(Ba1-ySry)2Ca2Cu3O8+z superconducting polycrystals			Superconductivity Lab,IMRE-Physics Faculty, University of Havana, Havana,Cuba	Physica C, 383(2003)365	A.J.Batista-Leyva,E.Altshuler,L.Rivero,M.T.D.Orlando,R.Cobas		
33764	PHC3830445	ANN(800C). Extremely underdoped sample. phase diagram shown .	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				60.5			60.5																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33765	PHC3830445	ANN(700C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				69.1			69.1																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33766	PHC3830445	ANN(600C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				78.2			78.2																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33767	PHC3830445	ANN(500C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212			A	5.422		30.73												K				83.1			83.1																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33768	PHC3830445	ANN(400C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				84.7			84.7																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33769	PHC3830445	ANN(300C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				84.1			84.1																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33770	PHC3830445	ANN(250C).	Bi2(Sr,Bi,La)2CaCu2Oz	Bi2.2Sr1.72La0.08Ca1Cu2O8	Bi	2.2	Sr	1.72	La	0.08	Ca	1	Cu	2											O	8		3	2003																												Bi2212																		K				82.5			82.5																																																																																																single crystals were grown by TSFZ method. Oxygen content z was controlled by ANN temperature.					Vortex phase diagram for extremely underdoped Bi2.2Sr1.72La0.08CaCu2O8+z			AIST,Tsukuba-shi,Ibaraki,Japan	Physica C, 383(2003)445	A.Mumtaz,H.Bando,K.Oka,Y.Yamaguchi		
33771	PHC3830450	g-value for Gd<3+> = 2.05024	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	10-z		1	2003																												Ru1222			A	3.8318		28.5325												K			42				42																																																																																														RuO2,Sb2O3,SrCO3,Gd2O3,CeO2,CuO	1	mixture-heat(1000C,36h, in air)-heat(1070C,60h, in flowing O2)-slow cool to RT					Transport and magnetic resonance properties of Ru1-xSbxSr2Gd1.4Ce0.6Cu2O10-z			Structure Research Laboratory, University of Science and Technology of China, Hefei, China	Physica C, 383(2003)450-456	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang		
33772	PHC3830450	g-value for Gd<3+> =2.02326	(Ru,Sb)Sr2(Gd,Ce)2Cu2O10	Ru0.99Sb0.01Sr2Gd1.4Ce0.6Cu2O10-z	Ru	0.99	Sb	0.01	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10-z		1	2003																												Ru1222			A	3.8328		28.5472												K			39.1				39.1																																																																																														RuO2,Sb2O3,SrCO3,Gd2O3,CeO2,CuO	1	mixture-heat(1000C,36h, in air)-heat(1070C,60h, in flowing O2)-slow cool to RT					Transport and magnetic resonance properties of Ru1-xSbxSr2Gd1.4Ce0.6Cu2O10-z			Structure Research Laboratory, University of Science and Technology of China, Hefei, China	Physica C, 383(2003)450-456	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang		
33773	PHC3830450	g-value for Gd<3+> =2.02979	(Ru,Sb)Sr2(Gd,Ce)2Cu2O10	Ru0.98Sb0.02Sr2Gd1.4Ce0.6Cu2O10-z	Ru	0.98	Sb	0.02	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10-z		1	2003																												Ru1222			A	3.834		28.5416												K			33				33																																																																																														RuO2,Sb2O3,SrCO3,Gd2O3,CeO2,CuO	1	mixture-heat(1000C,36h, in air)-heat(1070C,60h, in flowing O2)-slow cool to RT					Transport and magnetic resonance properties of Ru1-xSbxSr2Gd1.4Ce0.6Cu2O10-z			Structure Research Laboratory, University of Science and Technology of China, Hefei, China	Physica C, 383(2003)450-456	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang		
33774	PHC3830450	g-value for Gd<3+> =2.04358	(Ru,Sb)Sr2(Gd,Ce)2Cu2O10	Ru0.95Sb0.05Sr2Gd1.4Ce0.6Cu2O10-z	Ru	0.95	Sb	0.05	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10-z		1	2003																												Ru1222			A	3.8345		28.5282												K			29				29																																																																																														RuO2,Sb2O3,SrCO3,Gd2O3,CeO2,CuO	1	mixture-heat(1000C,36h, in air)-heat(1070C,60h, in flowing O2)-slow cool to RT					Transport and magnetic resonance properties of Ru1-xSbxSr2Gd1.4Ce0.6Cu2O10-z			Structure Research Laboratory, University of Science and Technology of China, Hefei, China	Physica C, 383(2003)450-456	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang		
33775	PHC3830450	g-value for Gd<3+> =2.01560	(Ru,Sb)Sr2(Gd,Ce)2Cu2O10	Ru0.93Sb0.07Sr2Gd1.4Ce0.6Cu2O10-z	Ru	0.93	Sb	0.07	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10-z		1	2003																												Ru1222			A	3.837		28.5108												K			17				17																																																																																														RuO2,Sb2O3,SrCO3,Gd2O3,CeO2,CuO	1	mixture-heat(1000C,36h, in air)-heat(1070C,60h, in flowing O2)-slow cool to RT					Transport and magnetic resonance properties of Ru1-xSbxSr2Gd1.4Ce0.6Cu2O10-z			Structure Research Laboratory, University of Science and Technology of China, Hefei, China	Physica C, 383(2003)450-456	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang		
33776	MSE0130215	ultrasonic, V<S>=2241 m/s, V<L>=3693 m/s.	(Bi,Pb)2AgxSr2Ca2Cu3Oz	Bi1.7Pb0.3Ag0.1Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Ag	0.1	Sr	2	Ca	2	Cu	3									O	z			1992									4.993		32.4	GPa		60.4	GPa		25.1	GPa		33.9		0.204	m/s		3693			Bi2223																		K		105					105																																																																																															1	precursor(Sr2Ca2Cu3O7)+(Bi2O3, PbO, Ag) - heat(810C, 24h, in air) - SIN(845C, 10d, in air)					Elastic and plastic behaviour of lead and silver doped Bi-Sr-Ca-Cu-O superconductors			Department of Physics, Osmania University, Hyderabad, India	Mater. Sci. Engneering, B13(1992)215-219	K.Nanda Kishore,M.Muralidhar,V.Hari Babu,Y.V.Ramana		
33777	MSE0130215	ultrasonic, V<S>=2239 m/s, V<L>=3633 m/s.	(Bi,Pb)2AgxSr2Ca2Cu3Oz	Bi1.7Pb0.3Ag0.2Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Ag	0.2	Sr	2	Ca	2	Cu	3									O	z			1992									4.995		31.33	GPa		59.7	GPa		25	GPa		32.5		0.194	m/s		3633			Bi2223																		K		97					97																																																																																															1	precursor(Sr2Ca2Cu3O7)+(Bi2O3, PbO, Ag) - heat(810C, 24h, in air) - SIN(845C, 10d, in air)					Elastic and plastic behaviour of lead and silver doped Bi-Sr-Ca-Cu-O superconductors			Department of Physics, Osmania University, Hyderabad, India	Mater. Sci. Engneering, B13(1992)215-219	K.Nanda Kishore,M.Muralidhar,V.Hari Babu,Y.V.Ramana		
33778	MSE0130215	ultrasonic, V<S>=2174 m/s, V<L>=3596 m/s.	(Bi,Pb)2AgxSr2Ca2Cu3Oz	Bi1.7Pb0.3Ag0.3Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Ag	0.3	Sr	2	Ca	2	Cu	3									O	z			1992									5.003		29	GPa		57.2	GPa		23.6	GPa		33.1		0.212	m/s		3596			Bi2223																		K		96					96																																																																																															1	precursor(Sr2Ca2Cu3O7)+(Bi2O3, PbO, Ag) - heat(810C, 24h, in air) - SIN(845C, 10d, in air)					Elastic and plastic behaviour of lead and silver doped Bi-Sr-Ca-Cu-O superconductors			Department of Physics, Osmania University, Hyderabad, India	Mater. Sci. Engneering, B13(1992)215-219	K.Nanda Kishore,M.Muralidhar,V.Hari Babu,Y.V.Ramana		
33779	MSE0130215		(Bi,Pb)2AgxSr2Ca2Cu3Oz	Bi1.7Pb0.3Ag0.4Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Ag	0.4	Sr	2	Ca	2	Cu	3									O	z			1992											27.05	GPa																Bi2223																		K		106					106																																																																																															1	precursor(Sr2Ca2Cu3O7)+(Bi2O3, PbO, Ag) - heat(810C, 24h, in air) - SIN(845C, 10d, in air)					Elastic and plastic behaviour of lead and silver doped Bi-Sr-Ca-Cu-O superconductors			Department of Physics, Osmania University, Hyderabad, India	Mater. Sci. Engneering, B13(1992)215-219	K.Nanda Kishore,M.Muralidhar,V.Hari Babu,Y.V.Ramana		
33780	MSE0130215	ultrasonic, V<S>=2328 m/s, V<L>=3726 m/s.	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.7Pb0.3Sr2Ca2Cu3Oz	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	z			1992									4.989		36.31	GPa		63.7	GPa		27	GPa		33.2		0.18	m/s		3726			Bi2223																		K																																																																																																						1	precursor(Sr2Ca2Cu3O7)+(Bi2O3, PbO, Ag) - heat(810C, 24h, in air) - SIN(845C, 10d, in air)					Elastic and plastic behaviour of lead and silver doped Bi-Sr-Ca-Cu-O superconductors			Department of Physics, Osmania University, Hyderabad, India	Mater. Sci. Engneering, B13(1992)215-219	K.Nanda Kishore,M.Muralidhar,V.Hari Babu,Y.V.Ramana		
33781	PHB1651283	ultrasonic wave velocity. Sr-content not described.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1990									6.22			GPa		124	GPa		50.1	GPa		78.5		0.24						T																		K		38					38																																																											410																																				1	standard solid state reaction technique.					Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
33782	PHB1651283	ultrasonic wave velocity	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1990									5.69			GPa		92.2	GPa		38.4	GPa		51.2		0.2						Y123																		K		90					90																																																											480																																				1	standard solid state reaction technique.					Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
33783	PHB1651283	ultrasonic wave velocity	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1990									5.35			GPa		38.8	GPa		16.1	GPa		21.9		0.2						Bi2212																		K		74					74																																																											250																																				1	standard solid state reaction technique.					Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
33784	PHB1651283	ultrasonic wave velocity. Pb-content not described.	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	8			1990									5.02			GPa		37.3	GPa		16	GPa		18.6		0.17						Bi2212																		K		80					80																																																											270																																				1	standard solid state reaction technique.					Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
33785	PHB1651283	ultrasonic wave velocity. Pb-content not described.	(Bi,Pb)2Sr2Ca2Cu3O8	Bi1.7Pb0.3Sr2Ca2Cu3O10	Bi	1.7	Pb	0.3	Sr	2	Ca	2	Cu	3											O	10			1990									4.35			GPa		33.7	GPa		14.2	GPa		17.4		0.18						Bi2223																		K		108					108																																																											280																																				1	standard solid state reaction technique.					Ultrasonic investigations of the layered perovskite ceramic superconducting systems			Tsinghua University, Beijing, P.R.China	Physica B, 165-166(1990)1283-1284	He Aisheng,He Yusheng,Jin Sheng,Xiang Jiong,Zhang Jincang		
33786	JPC0019067	Tc not described. C<11>=86.8 GPa. pressure dependence of C<11>, C<44> were measured. porocity=0.22.	GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			1989									5.549						GPa		29.5	GPa		47.5		0.242						Y123																																																																																																																									SIN(940C,48h, in O2-flow)-slow cool to RT(20C/h)					The effect of hydrostatic Pressure on the elastic behaviour of GdBa2Cu3O7-x			School of Physics and Materials Science,University of Bath,Claverton Down,Bath BA27AY,UK	J.Phys.Codens.Matter 1(1989)9067-9076	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper	Gd, Ba, Cu, O	
33787	JPC0016853	ultrasonic wave velocity was measured at 4.2K. porosity=0.22	GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			1989									5.549						GPa	64.5		GPa	84.6									Y123			A	3.925	3.863	11.755												K		92					92																																																											426																																					SIN(940C,48h, in O2-flow)-cool to RT					An ultrasonic study of superconducting and non-superconducting GdBa2Cu3O7-x			School of Physics and Materials Science, University of Bath, Claverton Down, Bath BA2 7AY, UK	J.Phys.C,1(1989)6853-6864	B.Chapman,D.P.Almond,E.F.Lambson,G.A.Saunders,J.Freestone,Qingxian Wang		
33788	PMB0590487	ultrasonic wave velocity	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1989									5.199			GPa		78	GPa		32.7	GPa		42.4		0.194						Y123			A	3.826	3.888	11.677																																																																														324																																					SIN(940C,48h, in O2-flow)-slow cool to RT(20C/h)					Elastic behaviour under pressure of high-Tc superconductors RBa2Cu3O7-z (R=Y, Gd and Eu)			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Phil.Mag. , 59(1989)487-497	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper		
33789	PMB0590487	ultrasonic wave velocity	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1989									5.985			GPa		116	GPa		50.1	GPa		56.4		0.157						Y123																																																																																				414																																					SIN(940C,48h, in O2-flow)-slow cool to RT(20C/h)					Elastic behaviour under pressure of high-Tc superconductors RBa2Cu3O7-z (R=Y, Gd and Eu)			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Phil.Mag. , 59(1989)487-497	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper		
33790	PMB0590487	ultrasonic wave velocity	EuBa2Cu3O7	Eu1Ba2Cu3O7-z	Eu	1	Ba	2	Cu	3															O	7-z			1989									4.793					52.6	GPa		21.7	GPa		30.4		0.212						Y123																																																																																				261																																					SIN(940C,48h, in O2-flow)-slow cool to RT(20C/h)					Elastic behaviour under pressure of high-Tc superconductors RBa2Cu3O7-z (R=Y, Gd and Eu)			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Phil.Mag. , 59(1989)487-497	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper		
33791	PMB0590487	ultrasonic wave velocity	GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z			1989									5.549			GPa		73.3	GPa		29.5	GPa		47.7		0.242						Y123																																																																																				297																																					SIN(940C,48h, in O2-flow)-slow cool to RT(20C/h)					Elastic behaviour under pressure of high-Tc superconductors RBa2Cu3O7-z (R=Y, Gd and Eu)			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Phil.Mag. , 59(1989)487-497	A.Al-Kheffaji,D.P.Almond,E.F.Lambson,G.A.Saunders,M.Cankurtaran,R.C.J.Draper		
33792	JMR0111645	tensile stress. compositions show nominal values. Tc not measured.	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.84Pb0.34Sr2.03Ca1.9Cu3.06Oz	Bi	1.84	Pb	0.34	Sr	2.03	Ca	1.9	Cu	3.06											O	z			1996												GPa		123.6								0.169						Bi2223																																																																																																																									MgO-whiskers were mixed by solid state reaction method.					Mechanical behavior of MgO-whisker reinforced (Bi,Pb)2Sr2Ca2Cu3Oy high-temperature superconducting composite			University of Houston, Houston,Texas, USA	J.Mater.Res., 11(1996)1645	M.S.Wong,S.S.Wang,Y.S.Yuan		
33793	JMR0111645	tensile stress. compositions show nominal values. 10% MgO-whisker. Tc not measured.	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.84Pb0.34Sr2.03Ca1.9Cu3.06Oz	Bi	1.84	Pb	0.34	Sr	2.03	Ca	1.9	Cu	3.06											O	z			1996												GPa		134.4								0.169						Bi2223																																																																																																																									MgO-whiskers were mixed by solid state reaction method.					Mechanical behavior of MgO-whisker reinforced (Bi,Pb)2Sr2Ca2Cu3Oy high-temperature superconducting composite			University of Houston, Houston,Texas, USA	J.Mater.Res., 11(1996)1645	M.S.Wong,S.S.Wang,Y.S.Yuan		
33794	JMR0111645	tensile stress. compositions show nominal values. 20% MgO-whisker. Tc not measured.	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.84Pb0.34Sr2.03Ca1.9Cu3.06Oz	Bi	1.84	Pb	0.34	Sr	2.03	Ca	1.9	Cu	3.06											O	z			1996												GPa		135.6								0.188						Bi2223																																																																																																																									MgO-whiskers were mixed by solid state reaction method.					Mechanical behavior of MgO-whisker reinforced (Bi,Pb)2Sr2Ca2Cu3Oy high-temperature superconducting composite			University of Houston, Houston,Texas, USA	J.Mater.Res., 11(1996)1645	M.S.Wong,S.S.Wang,Y.S.Yuan		
33795	SST0080101	porosity = p1. sound velocity V<L>=2990, V<S>=1850 m/s.	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	8			1995									4.65			GPa		41.57	GPa		15.91						m/s		2990			Bi2212			A	5.41	5.42	30.68												K				81			81																																																																																																mixture - CAL(800C,24h + 820C,50h) - press(various pressure) - SIN(840C,100h)					The relationship between the porosity and elastic moduli of the Bi-Pb-2212 high-Tc superconductor			Department of Physics,Osmania University,Hyderabad,India	Supercond.Sci.Technol., 8(1995)101-107	M.Muralidhar,P.V.Reddy,R.R.Reddy,V.H.Babu		
33796	SST0080101	porosity = p2. sound velocity V<L>=2800, V<S>=1780 m/s.	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	8			1995									4.5			GPa		35.28	GPa		13.78						m/s		2800			Bi2212																		K				80			80																																																																																																mixture - CAL(800C,24h + 820C,50h) - press(various pressure) - SIN(840C,100h)					The relationship between the porosity and elastic moduli of the Bi-Pb-2212 high-Tc superconductor			Department of Physics,Osmania University,Hyderabad,India	Supercond.Sci.Technol., 8(1995)101-107	M.Muralidhar,P.V.Reddy,R.R.Reddy,V.H.Babu		
33797	SST0080101	porosity = p3. sound velocity V<L>=2750, V<S>=1725 m/s.	(Bi,Pb)2Sr2CaCu2O8	Bi1.7Pb0.3Sr2Ca1Cu2O8	Bi	1.7	Pb	0.3	Sr	2	Ca	1	Cu	2											O	8			1995									4.46			GPa		33.72	GPa		13.27						m/s		2750			Bi2212																		K				81			81																																																																																																mixture - CAL(800C,24h + 820C,50h) - press(various pressure) - SIN(840C,100h)					The relationship between the porosity and elastic moduli of the Bi-Pb-2212 high-Tc superconductor			Department of Physics,Osmania University,Hyderabad,India	Supercond.Sci.Technol., 8(1995)101-107	M.Muralidhar,P.V.Reddy,R.R.Reddy,V.H.Babu		
33798	SST0060484	highly textured sample. ultrasound velocity. along c, G=19GPa elastic=44GPa. along ab, elastic modulus=118 GPa.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			1993									6.208						GPa		19											Bi2212																																																																																																																									Bi2212 powder samples were sinter forging in air at 840C					Anisotropic elastic and nonlinear acoustic properties of very dense textured Bi2Sr2CaCu2O8+y			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Supercond.Sci.Technol., 6(1993)484-489	B.Chapman,D.P.Almond,F.Chang,G.A.Saunders,K.C.Goretta,Li Jiaqiang,M.Cankurtaran,P.J.Ford,R.B.Poeppel		
33799	PHC3840075		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4+z	La	1.85	Sr	0.15	Cu	1															O	4+z			2003																												T			A	3.7743		13.227												K				37.9			37.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33800	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.995V0.005O4+z	La	1.85	Sr	0.15	Cu	0.995	V	0.005													O	4+z			2003																												T			A	3.7757		13.2244												K				36.9			36.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33801	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.9875V0.0125O4+z	La	1.85	Sr	0.15	Cu	0.9875	V	0.0125													O	4+z			2003																												T			A	3.7764		13.2188												K				35.9			35.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33802	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.9825V0.0175O4+z	La	1.85	Sr	0.15	Cu	0.9825	V	0.0175													O	4+z			2003																												T			A	3.7764		13.2163												K				35			35																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33803	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.98V0.02O4+z	La	1.85	Sr	0.15	Cu	0.98	V	0.02													O	4+z			2003																												T			A	3.7782		13.2142												K				30.9			30.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33804	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.975V0.025O4+z	La	1.85	Sr	0.15	Cu	0.975	V	0.025													O	4+z			2003																												T			A	3.7791		13.2125												K				29.9			29.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33805	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.95V0.05O4+z	La	1.85	Sr	0.15	Cu	0.95	V	0.05													O	4+z			2003																												T			A	3.7843		13.1981												K				28			28																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33806	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.925V0.075O4+z	La	1.85	Sr	0.15	Cu	0.925	V	0.075													O	4+z			2003																												T			A	3.7839		13.1943												K				23.9			23.9																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33807	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.9V0.1O4+z	La	1.85	Sr	0.15	Cu	0.9	V	0.1													O	4+z			2003																												T			A	3.7868		13.1887												K				15			15																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33808	PHC3840075		(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.875V0.125O4+z	La	1.85	Sr	0.15	Cu	0.875	V	0.125													O	4+z			2003																												T			A	3.7932		13.18												K				9.11			9.11																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33809	PHC3840075	Tc=0 K. This sample is s/c critical concentration in this system.	(La,Sr)2(Cu,V)O4	La1.85Sr0.15Cu0.85V0.15O4+z	La	1.85	Sr	0.15	Cu	0.85	V	0.15													O	4+z			2003																												T			A	3.793		13.1943												K				0			0																																																																																														La2O3,SrCO3,CuO,V2O5	1	mixture - CAL(900C,24h,in air) - pellet - heat(960C,72h) - cool to RT(30C/h)					The properties of V-substituted La1.85Sr0.15CuO4+z superconductor			National Lab for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing,China	Physica C, 384(2003)75-80	C.Dong,G.Che,G.Liu,H.Chen,L.Liu,S.Jia,Y.Ni,Z.Zhao		
33810	PHC3840102	average grain size = 1.44 micron-m. resistive transition under pressure.	(Tl,Pb)(Ba,Sr)2Ca2Cu3Oz	Tl0.5Pb0.5Ba1.6Sr0.4Ca2Cu3Oz	Tl	0.5	Pb	0.5	Ba	1.6	Sr	0.4	Ca	2	Cu	3									O	z		1	2003																												Tl1223																		K		120.2					120.2			K/kbar	0.22																																																																																												standard solid state reaction  .					Pressure effects on the intergrain coupling in (Tl0.5Pb0.5)(Ba0.8Sr0.2)2Ca2Cu3Oy ceramic superconductor			Universidade Fedral Fluminense,Niteroi,RJ,Brazil	Physica C, 384(2003)102-110	E.Baggio-Saitovitch,E.S.Yugue,E.V.L.de Mello,J.L.Gonzalez,M.T.D.Orlando		
33811	PHC3840237		(La,Sr)2CuO4	La1.7Sr0.3Cu1O3.997	La	1.7	Sr	0.3	Cu	1															O	4	3.997	1	2003																												T																				10.2					10.2																																																													W/m.K	7.48			THC33811	uV/K	1.18			TP33811	mOhm.cm							0.24				0.78			E-10 m3/C	0.98					RH33811					mixture - CAL(950C,24h,in air) - pellet - SIN(100C,60h) - SIN(1050C,72h,in air)					Thermomagnetic properties of the overdoped La1.7Sr0.3CuO4 superconductor			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, Wroclaw,Poland	Physica C, 384(2003)237-246	C.Sulkowski,H.Misiorek,M.Matusiak,T.Plackowski		
33812	MLT0160165	X-ray density=6.171. longitudinal modulus=56.2 GPa. elastic constant at 5 K.	YBa2Cu3Oz	Y1Ba2Cu3O6.2	Y	1	Ba	2	Cu	3															O	7-z	6.2	1	1993									4.433			GPa	51.2		GPa	21.51		GPa	27.5		0.19							Y123			A	3.8606	3.8664	11.7827																																																																														337	calculated from elastic constant																																			1	standard solid state reaction. oxygen content controlled by ANN.					Elastic constants and Debye temperature of Y1Ba2Cu3Ox: effect of oxygen content			NIST, Boulder, CO, USA	Materials Lett., 16(1993)165-168	Hassel Ledbetter,Ming Lei,Sihan Lin		
33813	MLT0160165	X-ray density=6.304. longitudinal modulus=62.8 GPa. elastic constant at 5 K.	YBa2Cu3Oz	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3															O	7-z	6.7	1	1993									4.523			GPa	56.6		GPa	23.59		GPa	31.3		0.199							Y123			A	3.8286	3.8868	11.6984																																																																														356	calculated from elastic constant																																			1	standard solid state reaction. oxygen content controlled by ANN.					Elastic constants and Debye temperature of Y1Ba2Cu3Ox: effect of oxygen content			NIST, Boulder, CO, USA	Materials Lett., 16(1993)165-168	Hassel Ledbetter,Ming Lei,Sihan Lin		
33814	MLT0160165	X-ray density=6.339. longitudinal modulus=63.8 GPa. elastic constant at 5 K.	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	1	1993									4.528			GPa	57.8		GPa	24.16		GPa	31.6		0.196							Y123			A	3.825	3.8957	11.6587																																																																														362	calculated from elastic constant																																			1	standard solid state reaction. oxygen content controlled by ANN.					Elastic constants and Debye temperature of Y1Ba2Cu3Ox: effect of oxygen content			NIST, Boulder, CO, USA	Materials Lett., 16(1993)165-168	Hassel Ledbetter,Ming Lei,Sihan Lin		
33815	MLT0160165	X-ray density=6.363. longitudinal modulus=62.7 GPa. elastic constant at 5 K.	YBa2Cu3Oz	Y1Ba2Cu3O6.9	Y	1	Ba	2	Cu	3															O	7-z	6.9	1	1993									4.553			GPa	57.4		GPa	24.23		GPa	30.4		0.185							Y123			A	3.8228	3.8926	11.6598																																																																														361	calculated from elastic constant																																			1	standard solid state reaction. oxygen content controlled by ANN.					Elastic constants and Debye temperature of Y1Ba2Cu3Ox: effect of oxygen content			NIST, Boulder, CO, USA	Materials Lett., 16(1993)165-168	Hassel Ledbetter,Ming Lei,Sihan Lin		
33816	MPL0071457	porosity=0.211. For zero porosity, E=143.2, G=58.6, B=89.8 GPa, p=0.224	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1993									5.15			GPa		85.5	GPa		34.2	GPa		57								Y123																		K		83					83																																																											331.9	calculated from elastic constant																																				sol-gel method. CAL(550C)-heat(920C,8h,in air)-SIN(945-950C,8h)-ANN(500-550C,20h,in O2)					Ultrasonic anomalies in Y-Ba-Cu-O high-Tc superconducting materials			Department of Physics,Osmania University,Hyderabad,India	Mod.Phys.Lett. B, 7(1993)1457-1465	K.B.Reddy,P.V.Reddy,R.R.Reddy,V.N.Mulay		
33817	MPL0071457	porosity=0.165. For zero porosity, E=134, G=57.14, B=70.28 GPa, p=0.172	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1993									5.45			GPa		92.2	GPa		38.13	GPa		50.9								Y123																		K		83					83																																																											345.7	calculated from elastic constant																																				sol-gel method. CAL(550C)-heat(920C,8h,in air)-SIN(945-950C,8h)-ANN(500-550C,20h,in O2)					Ultrasonic anomalies in Y-Ba-Cu-O high-Tc superconducting materials			Department of Physics,Osmania University,Hyderabad,India	Mod.Phys.Lett. B, 7(1993)1457-1465	K.B.Reddy,P.V.Reddy,R.R.Reddy,V.N.Mulay		
33818	SST0050529	ultrasound velocity were measured for various T and pressure. density=96% of d<x-ray>	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1992									6.07			GPa		108.9	GPa		46.1	GPa		47.4								Y123																		K	89		92	92			92																																																																																															1	standard solid state reaction. 					Correlation between anomalous elastic behaviour under pressure and with temperature near 220K in YBa2Cu3O7-x			School of Physics and Materials Science, University of Bath, Claverton Down, Bath, UK	Supercond.Sci.Technol., 5(1992)529-533	G.A.Saunders,M.Cankurtaran		
33819	MLT0210021	d<x>=6.632 g/cm3. porosity=38.17. For zero porosity, E=91.5, G=41.6, B=38.1 GPa, P=0.1	YBa2Cu3O7	Y1Ba2Cu3O6.957	Y	1	Ba	2	Cu	3															O	7-z	6.957	1	1994									4.1			GPa		31.15	GPa		8.62					0.3						Y123			A	3.823	3.885	11.676												K		91	102				91																																																											371	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33820	MLT0210021	d<x>=6.718 g/cm3. porosity=22.70. For zero porosity, E=91.79, G=35.28, B=76.8 GPa, P=0.3	SmBa2Cu3O7	Sm1Ba2Cu3O6.858	Sm	1	Ba	2	Cu	3															O	7-z	6.858	1	1994									5.19			GPa		52	GPa		20					0.3						Y123			A	3.856	3.899	11.69												K		90	98				90																																																											336	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33821	MLT0210021	d<x>=7.014 g/cm3. porosity=17.30. For zero porosity, E=102.3, G=39.89, B=78.2 GPa, P=0.28	GdBa2Cu3O7	Gd1Ba2Cu3O6.758	Gd	1	Ba	2	Cu	3															O	7-z	6.758	1	1994									5.8			GPa		68.2	GPa		26.6					0.28						Y123			A	3.832	3.887	11.704												K		92	103				92																																																											349	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33822	MLT0210021	d<x>=7.042 g/cm3. porosity=24.80. For zero porosity, E=106.44, G=41.61, B=80.3 GPa, P=0.27	TbBa2Cu3O7	Tb1Ba2Cu3O6.383	Tb	1	Ba	2	Cu	3															O	7-z	6.383	1	1994									5.29			GPa		56.1	GPa		21.7					0.29						Y123			A	3.816	3.87	11.757												K																																																																		317	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33823	MLT0210021	d<x>=7.019 g/cm3. porosity=25.90. For zero porosity, E=95.51, G=38.41, B=61.5, P=0.24	DyBa2Cu3O7	Dy1Ba2Cu3O6.879	Dy	1	Ba	2	Cu	3															O	7-z	6.879	1	1994									5.2			GPa		48.2	GPa		18.9					0.27						Y123			A	3.853	3.898	11.653												K		86	94				86																																																											345	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33824	MLT0210021	d<x>=7.069 g/cm3. porosity=18.70. For zero porosity, E=75.95, G=29.98, B=54.2, P=0.26	TmBa2Cu3O7	Tm1Ba2Cu3O6.71	Tm	1	Ba	2	Cu	3															O	7-z	6.71	1	1994									5.75			GPa		48.5	GPa		19.1					0.27						Y123			A	3.831	3.888	11.768												K		78	85				78																																																											301	calculated from elastic constant																																			1	standard solid state reaction. 					Elasticity studies of RE-Ba-Cu-O high-Tc superconductors			Department of Physics,Osmania University,Hyderabad,India	Materials Lett., 21(1994)21-29	K.Somaiah,P.V.Reddy,S.Shekar		
33825	PR04210098	Neel-T by susceptibility. Three magnetic phases(T=100K,50K,23K) were observed.	Nd2CuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4		3	1990								255																				T'			A	3.941		12.16												K					4																																																																																																		self-flux method					THREE-DEMENSIONAL MAGNETIC STRUCTURES AND RARE-EARTH MAGNETICORDERING IN ND2CUO4 AND PR2CUO4	199012	MAGNETISM           ,NEUTRON-SCATTERING  ,ANTIFERROMAGNETIC   ,PHASE TRANSITIONS	DEPARTMENT OF PHYSICS, TOHOKU UNIBERSITY, AOBA-KU, SENDAI 980,JAPAN	PHYS.REV.B,42(1990)10098	A.H.MOUDDEN,G.SHIRANE,H.KADOWAKI,K.KAKURAI,K.YAMADA,M.A.KASTNER,M.MATSUDA,P.M.GEHRING,R.J.BIRGENEAU,T.R.THURSTON,Y.ENDOH,Y.HIDAKA	PR,ND,CU,O	
33826	PR04210098	Neel-T by susceptibility. 	Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4		3	1990								255																				T'			A	3.962		12.21												K					4																																																																																																		self-flux method					THREE-DEMENSIONAL MAGNETIC STRUCTURES AND RARE-EARTH MAGNETICORDERING IN ND2CUO4 AND PR2CUO4	199012	MAGNETISM           ,NEUTRON-SCATTERING  ,ANTIFERROMAGNETIC   ,PHASE TRANSITIONS	DEPARTMENT OF PHYSICS, TOHOKU UNIBERSITY, AOBA-KU, SENDAI 980,JAPAN	PHYS.REV.B,42(1990)10098	A.H.MOUDDEN,G.SHIRANE,H.KADOWAKI,K.KAKURAI,K.YAMADA,M.A.KASTNER,M.MATSUDA,P.M.GEHRING,R.J.BIRGENEAU,T.R.THURSTON,Y.ENDOH,Y.HIDAKA	PR,ND,CU,O	
33827	PHC3780273	Neel-T(as-grown)=180 K.	(Nd,Ce)2CuO4	Nd1.9Ce0.1Cu1O4	Nd	1.9	Ce	0.1	Cu	1															O	4		3	2002								164.4																				T'																																																																																																																									single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33828	PHC3780273		(Nd,Ce)2CuO4	Nd1.88Ce0.12Cu1O4	Nd	1.88	Ce	0.12	Cu	1															O	4		3	2002								129.8																				T'																																																																																																																									single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33829	PHC3780273	dz=z(as-grown)-z(reduced) = 0.018	(Nd,Ce)2CuO4	Nd1.87Ce0.13Cu1O4	Nd	1.87	Ce	0.13	Cu	1															O	4		3	2002								99.5																				T'																																																																																																																									single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33830	PHC3780273		(Nd,Ce)2CuO4	Nd1.86Ce0.14Cu1O4	Nd	1.86	Ce	0.14	Cu	1															O	4		3	2002								90																				T'																		K				22.9			22.9																																																																																																single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33831	PHC3780273	dz=z(as-grown)-z(reduced) = 0.02. Neel-T(as-grown)=124.6 K.	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	2002								58.5																				T'																		K				24.3			24.3																																																																																																single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33832	PHC3780273	Neel-T(as-grown)=119.4 K.	(Nd,Ce)2CuO4	Nd1.84Ce0.16Cu1O4	Nd	1.84	Ce	0.16	Cu	1															O	4		3	2002								34.6																				T'																		K				22.6			22.6																																																																																																single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33833	PHC3780273	dz=z(as-grown)-z(reduced) = 0.0207. Neel-T(as-grown)=83.9 K.	(Nd,Ce)2CuO4	Nd1.83Ce0.17Cu1O4	Nd	1.83	Ce	0.17	Cu	1															O	4		3	2002																												T'																		K				15.7			15.7																																																																																																single crystals were grown by TSFZ method. reduced (920C, 12h, in Ar flow)					Electron-doping effect on magnetic order and superconductivity in Nd2-xCexCuO4 single crystals			Kyoto University, Uji,Kyoto,Japan	Physica C, 378-381(2002)273-277	K.Kurahashi,K.Yamada,M.Fujita,M.Matsuda,T.Uefuji		
33834	P067014514	Neel-T from muon-SR	(Pr,La,Ce)2CuO4	Pr0.91La1Ce0.09Cu1O4	Pr	0.91	La	1	Ce	0.09	Cu	1													O	4		3	2003								59.5																				T'																		K				25.2			25.2																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33835	P067014514	Neel-T from muon-SR	(Pr,La,Ce)2CuO4	Pr0.89La1Ce0.11Cu1O4	Pr	0.89	La	1	Ce	0.11	Cu	1													O	4		3	2003								39																				T'																		K				24.6			24.6																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33836	P067014514	oxygen reduction dz is about 0.03.	(Pr,La,Ce)2CuO4	Pr0.85La1Ce0.15Cu1O4	Pr	0.85	La	1	Ce	0.15	Cu	1													O	4		3	2003																												T'																		K				24			24																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33837	P067014514	oxygen reduction dz is about 0.03.	(Pr,La,Ce)2CuO4	Pr0.83La1Ce0.17Cu1O4	Pr	0.83	La	1	Ce	0.17	Cu	1													O	4		3	2003																												T'																		K				19.8			19.8																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33838	P067014514	oxygen reduction dz is about 0.03.	(Pr,La,Ce)2CuO4	Pr0.82La1Ce0.18Cu1O4	Pr	0.82	La	1	Ce	0.18	Cu	1													O	4		3	2003																												T'																		K				16.2			16.2																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33839	P067014514	oxygen reduction dz is about 0.03.	(Pr,La,Ce)2CuO4	Pr0.8La1Ce0.2Cu1O4	Pr	0.8	La	1	Ce	0.2	Cu	1													O	4		3	2003																												T'																		K				15.6			15.6																																																																																																See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33840	P067014514	Neel-T from muon-SR	(Pr,La,Ce)2CuO4	Pr0.96La1Ce0.04Cu1O4	Pr	0.96	La	1	Ce	0.04	Cu	1													O	4		1	2003								149																				T'																		K					2																																																																																																Pr6O11,La2O3,CeO2,CuO		mixture-heat(1040C,24h) - pellet - SIN(1200C,12h) - ANN(900-950C,10h,in Ar flow)					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33841	P067014514	Neel-T from muon-SR	(Pr,La,Ce)2CuO4	Pr0.94La1Ce0.06Cu1O4	Pr	0.94	La	1	Ce	0.06	Cu	1													O	4		1	2003								138.7																				T'																		K					2																																																																																																Pr6O11,La2O3,CeO2,CuO		mixture-heat(1040C,24h) - pellet - SIN(1200C,12h) - ANN(900-950C,10h,in Ar flow)					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33842	P067014514	Neel-T from muon-SR	(Pr,La,Ce)2CuO4	Pr0.92La1Ce0.08Cu1O4	Pr	0.92	La	1	Ce	0.08	Cu	1													O	4		3	2003								138.7																				T'																		K					2																																																																																																		See J.Phys.Soc.Jpn 71(2002)910.					Magnetic and superconducting phase diagram of electron-doped Pr1-xLaCexCuO4			Institute for Chemical Research,Kyoto University, Uji,Kyoto,Japan	Phys.Rev.B, 67(2003)014514	I.Watanabe,K.Kawashima,K.Nagamine,K.Yamada,M.Fujita,S.Kuroshima,T.Kubo,T.Uefuji		
33843	P067024505	Figure shows Tc(x). plasmon study by EELS.	(Ba,K)BiO3	Ba0.61K0.39Bi1O3	Ba	0.61	K	0.39	Bi	1															O	3		3	2003																												BKBO																		K		31.5					31.5	TC33843																																																																																															electrochemical growth method					Evidence of a small exciton in the Ba1-xKxBiO3 superconductor and its relationship with superconductivity			Northwestern University,Evanston,Illinois,USA	Phys.Rev.B, 67(2003)024505	P.D.Han,Y.Y.Wang		
33844	PHC3850373	Mossbauer of Fe measured	(Y,Pr)Ba2(Cu,Fe)4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8			2003																												Y124			A	3.8488	3.8771	27.2354												K		62					62																																																																																																precursor(Y0.8Pr0.2Ba2Cu4O8) + Fe2O3, then heat(790C,20h, in O2 flow) - slow cool to RT (0.5C/min).					Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4-xFexO8 system			Circuito Exterior,C.U.UNAM,Apdo,Mexico,Mexico	Physica C, 385(2003)373-382	M.L.Marquina,R.Escamilla,R.Gomez,R.Ridaura,T.Akachi,V.Marquina		
33845	PHC3850373	Mossbauer of Fe measured	(Y,Pr)Ba2(Cu,Fe)4O8	Y0.8Pr0.2Ba2Cu3.975Fe0.025O8	Y	0.8	Pr	0.2	Ba	2	Cu	3.975	Fe	0.025											O	8			2003																												Y124			A	3.8485	3.8788	27.2247												K		46					46																																																																																																precursor(Y0.8Pr0.2Ba2Cu4O8) + Fe2O3, then heat(790C,20h, in O2 flow) - slow cool to RT (0.5C/min).					Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4-xFexO8 system			Circuito Exterior,C.U.UNAM,Apdo,Mexico,Mexico	Physica C, 385(2003)373-382	M.L.Marquina,R.Escamilla,R.Gomez,R.Ridaura,T.Akachi,V.Marquina		
33846	PHC3850373	Mossbauer of Fe measured	(Y,Pr)Ba2(Cu,Fe)4O8	Y0.8Pr0.2Ba2Cu3.95Fe0.05O8	Y	0.8	Pr	0.2	Ba	2	Cu	3.95	Fe	0.05											O	8			2003																												Y124			A	3.8496	3.8799	27.2139												K		33					33																																																																																																precursor(Y0.8Pr0.2Ba2Cu4O8) + Fe2O3, then heat(790C,20h, in O2 flow) - slow cool to RT (0.5C/min).					Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4-xFexO8 system			Circuito Exterior,C.U.UNAM,Apdo,Mexico,Mexico	Physica C, 385(2003)373-382	M.L.Marquina,R.Escamilla,R.Gomez,R.Ridaura,T.Akachi,V.Marquina		
33847	PHC3850373	Mossbauer of Fe measured	(Y,Pr)Ba2(Cu,Fe)4O8	Y0.8Pr0.2Ba2Cu3.925Fe0.075O8	Y	0.8	Pr	0.2	Ba	2	Cu	3.925	Fe	0.075											O	8			2003																												Y124			A	3.8471	3.8782	27.204												K		10					10																																																																																																precursor(Y0.8Pr0.2Ba2Cu4O8) + Fe2O3, then heat(790C,20h, in O2 flow) - slow cool to RT (0.5C/min).					Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4-xFexO8 system			Circuito Exterior,C.U.UNAM,Apdo,Mexico,Mexico	Physica C, 385(2003)373-382	M.L.Marquina,R.Escamilla,R.Gomez,R.Ridaura,T.Akachi,V.Marquina		
33848	PHC3850373	Mossbauer of Fe measured	(Y,Pr)Ba2(Cu,Fe)4O8	Y0.8Pr0.2Ba2Cu3.9Fe0.1O8	Y	0.8	Pr	0.2	Ba	2	Cu	3.9	Fe	0.1											O	8			2003																												Y124			A	3.8493	3.8796	27.2081												K					4																																																																																																		precursor(Y0.8Pr0.2Ba2Cu4O8) + Fe2O3, then heat(790C,20h, in O2 flow) - slow cool to RT (0.5C/min).					Effect of Fe substitution in the structure and superconducting properties of the (Y0.8Pr0.2)Ba2Cu4-xFexO8 system			Circuito Exterior,C.U.UNAM,Apdo,Mexico,Mexico	Physica C, 385(2003)373-382	M.L.Marquina,R.Escamilla,R.Gomez,R.Ridaura,T.Akachi,V.Marquina		
33849	SSC1230017	s/c properties were obtained from Hao & Clem analysis. cohere//c estimated from anisotropy factor.G-L = 25.3. anisotropy=9.3. npenet estimated from anisotropy.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2002																												IL																		K				43			43																				T	Hao & Clem analysis from M	13.9							T/K	Hao & Clem analysis from M	0.47					A	Hao & Clem analysis from M		48.6	5.2	A	Hao & Clem analysis from M		1470																																																				pure phase synthesized by using cubic multi-anvil press.					Three-dimensional superconductivity in the infinite-layer compound Sr0.9La0.1CuO2 in entire region below Tc			Department of Physics, National Creative Research Initiative Center for Superconductivity, Pohang University of Science and Technology, Pohang, South Korea	Solid State Commun., 123(2002)17	C.U.Jung,J.Y.Kim,Jae-Hyuk Choi,Mun-Seog Kim,Sung-Ik Lee		
33850	MRB0361505	particle size = a few micron.m. new synthesis procedure. good homogeneity.	(Ba,K)BiO3	Ba0.6K0.4O3	Ba	0.6	K	0.4																	O	3			2001																												BKBO																		K				30.8			30.8																																																																																																(KOH pellet in Teflon crucible) - heat(200-260C) - added mixture(Ba(OH)2.8H2O + NaBiO3 + Bi2O3)					Synthesis of superconducting Ba1-xKxBiO3 by a modified molten salt process			Leiden University,Leiden, The Netherland	Mater.Res.Bull., 36(2001)1505	S.F.Liu,W.T.Fu		
33851	MRB0360971		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			2001																												Y123			A	3.8171	3.8822	11.6734												K	86.5						86.5																																																																		uV/K	7.974			TP33851	mOhm.cm											9.24													1	SIN(940C,42h,in air) - FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33852	MRB0360971		(Y,Sm)Ba2Cu3O7	Y0.8Sm0.2Ba2Cu3O7-z	Y	0.8	Sm	0.2	Ba	2	Cu	3													O	7-z			2001																												Y123			A	3.8171	3.884	11.6735												K	80						80																																																																		uV/K	7.765			TP33852	mOhm.cm											7.43													1	SIN(940C,42h,in air) - FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33853	MRB0360971		(Y,Sm)Ba2Cu3O7	Y0.6Sm0.4Ba2Cu3O7-z	Y	0.6	Sm	0.4	Ba	2	Cu	3													O	7-z			2001																												Y123			A	3.8171	3.8852	11.6735												K	78						78																																																																		uV/K	7.454			TP33853	mOhm.cm											5.79													1	SIN(940C,42h,in air) - FC to RT					Thermoelectric power of samarium substituted Y1-xSmxBa2Cu3O7-z superconducting pellets			High Temperature Superconductivity Laboratory, Cryogenic Engineering Centre, India	Mater.Res.Bull., 36(2001)971	A.K.Dhami,S.Basak,S.K.Ghatak,T.K.Dey		
33854	SST01600L1	T<sub>=510C. second phase= (Sr1-xCax)14Cu24O41-z	(Sr,Ca)CuO2	Sr0.6Ca0.2Cu1O2-z	Sr	0.6	Ca	0.2	Cu	1															O	2-z		4	2003																												IL			A	3.9154		3.3483												K					4.2																																																																									mOhm.cm											1.1														Films were grown by single target off-axis rf magnetron sputtering on SrTiO3(001) with total-p = 2.66 Pa. Then in-situ vacuum annealing.					Electron-doped superconductivity induced by oxygen vacancies in as-grown Sr0.6Ca0.4CuO2-z infinite-layer films			Nanoelectronics Research Institute of AIST,Tsukuba,Ibaraki,Japan	Supercond.Sci.Technol., 16(2003)L1-L3	A.Crisan,A.Iyo,A.Sundaresan,H.Ihara,H.Kito,J.C.Nie,M.Hirai,N.Terada,P.Badica,Y.Kodama,Y.Tanaka		
33855	SST01600L1	T<sub>=515C. n-type s/c. 	(Sr,Ca)CuO2	Sr0.6Ca0.2Cu1O2-z	Sr	0.6	Ca	0.2	Cu	1															O	2-z		4	2003																												IL			A	3.9293		3.3409												K	11		42				26.5																																																																							mOhm.cm											0.81														Films were grown by single target off-axis rf magnetron sputtering on SrTiO3(001) with total-p = 2.66 Pa. Then in-situ vacuum annealing.					Electron-doped superconductivity induced by oxygen vacancies in as-grown Sr0.6Ca0.4CuO2-z infinite-layer films			Nanoelectronics Research Institute of AIST,Tsukuba,Ibaraki,Japan	Supercond.Sci.Technol., 16(2003)L1-L3	A.Crisan,A.Iyo,A.Sundaresan,H.Ihara,H.Kito,J.C.Nie,M.Hirai,N.Terada,P.Badica,Y.Kodama,Y.Tanaka		
33856	SST01600L1	T<sub>=530C. excess O-vacancy.	(Sr,Ca)CuO2	Sr0.6Ca0.2Cu1O2-z	Sr	0.6	Ca	0.2	Cu	1															O	2-z		4	2003																												IL			A	3.934		3.3238												K					4.2																																																																									mOhm.cm											0.62														Films were grown by single target off-axis rf magnetron sputtering on SrTiO3(001) with total-p = 2.66 Pa. Then in-situ vacuum annealing.					Electron-doped superconductivity induced by oxygen vacancies in as-grown Sr0.6Ca0.4CuO2-z infinite-layer films			Nanoelectronics Research Institute of AIST,Tsukuba,Ibaraki,Japan	Supercond.Sci.Technol., 16(2003)L1-L3	A.Crisan,A.Iyo,A.Sundaresan,H.Ihara,H.Kito,J.C.Nie,M.Hirai,N.Terada,P.Badica,Y.Kodama,Y.Tanaka		
33857	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.937Sr0.063Cu1O4	La	1.937	Sr	0.063	Cu	1															O	4		3	2003																												T																		K				11.7			11.7																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33858	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.93Sr0.07Cu1O4	La	1.93	Sr	0.07	Cu	1															O	4		3	2003																												T																		K				15.4			15.4																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33859	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	2003																												T																		K				27.3			27.3																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33860	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	2003																												T																		K				29.2			29.2																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33861	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.889Sr0.111Cu1O4	La	1.889	Sr	0.111	Cu	1															O	4		3	2003																												T																		K				29.2			29.2																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33862	SST01600L7	large single crystal	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		3	2003																												T																		K				31			31																																																																																																TSFZ method					Under-doped La2-xSrxCuO4 with x=0.063-0.125: TSFZ growth of high-quality crystals and anomalous doping dependences of superconducting properties			Institute of Physics and Center for Condensed Matter Physics,Chinese Academy of Science,Beijing,China	Supercond.Sci.Technol., 16(2003)L7-L9	F.Zhou,J.W.Xiong,P.H.Hor,W.K.Chu,W.X.Ti,X.L.Dong,Z.H.Zhang,Z.X.Zhao		
33863	NAT4220053	CoO2/H2O/Na/H2O/CoO2 layers. R=0 is not attaied down to 2K.	Na0.35CoO2(H2O)1.3	Na0.35Co1H2.6O3.3	Na	0.35	Co	1	H	2.6															O	3.3			2003																													p6<3>/mmc																	K			3	5			5											Oe		100																																																																																			Na0.7CoO2 - oxidation					Superconductivity in two-dimensional CoO2 layers			Advanced Materials Lab,National Institute for Materials Science,Tsukuba,Ibaraki,Japan	Nature, 422(2003)53	E.Takayama-Muromachi,F.Izumi,H.Sakurai,K.Takada,R.A.Dllanlan,T.Sasaki		
33864	P066174510	optimal doped sample.sp-heat measured for T=2-7 K, H= 0-10 T range. gamma(H=0 T, s/c state)=1.4 mj/mol.K2.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2002																												T'																		K				22			22																																																					SP33864			mj/mol.K2	6.7	specific heat	362	specific heat																																				single crystal was grown by the directional solidification method.					Magnetic-field dependence of electronic specific heat in Pr1.85Ce0.15CuO4			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, Maryland 	Phys.Rev.B, 66(2002)174510	Amlan Biswas,Hamza Balci,P.Fournier,R.L.Greene,V.N.Smolyaninova		
33865	P067104503	thermal conductivity measured	La2CuO4	La2Cu1O4	La	2	Cu	1																	O	4		3	2003								306																				T																																																																																						W/m.K		2.69	13.74	THC33865																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33866	P067104503	thermal conductivity measured	(La,Sr)2CuO4	La1.99Sr0.01Cu1O4	La	1.99	Sr	0.01	Cu	1															O	4		3	2003								242																				T																																																																																						W/m.K		2.37	5.79	THC33866																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33867	P067104503	no magnetic order. thermal conductivity measured.	(La,Sr)2CuO4	La1.98Sr0.02Cu1O4	La	1.98	Sr	0.02	Cu	1															O	4		3	2003																												T																																																																																						W/m.K		2.37	4.32	THC33867																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33868	P067104503	no magnetic order. thermal conductivity measured.	(La,Sr)2CuO4	La1.96Sr0.04Cu1O4	La	1.96	Sr	0.04	Cu	1															O	4		3	2003																												T																																																																																						W/m.K		2.37	3.88	THC33868																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33869	P067104503	thermal conductivity measured	La2(Cu,Zn)O4	La2Cu0.99Zn0.01O4	La	2	Cu	0.99	Zn	0.01															O	4		3	2003																												T																																																																																						W/m.K		2.17	9.06	THC33869																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33870	P067104503	thermal conductivity measured	La2(Cu,Zn)O4	La2Cu0.98Zn0.02O4	La	2	Cu	0.98	Zn	0.02															O	4		3	2003																												T																																																																																						W/m.K		2.17	7.84	THC33870																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33871	P067104503	thermal conductivity measured	La2(Cu,Zn)O4	La2Cu0.96Zn0.04O4	La	2	Cu	0.96	Zn	0.04															O	4		3	2003																												T																																																																																						W/m.K		2.27	5.61	THC33871																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33872	P067104503	no magnetic order. thermal conductivity measured.	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		3	2003																												T																																																																																										THC33872																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33873	P067104503	no magnetic order. thermal conductivity measured.	(La,Nd,Sr)2CuO4	La1.28Nd0.6Sr0.12Cu1O4	La	1.28	Nd	0.6	Sr	0.12	Cu	1													O	4		3	2003																												T																																																																																										THC33873																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33874	P067104503	no magnetic order. thermal conductivity measured.	(La,Eu,Sr)2CuO4	La1.68Eu0.2Sr0.12Cu1O4	La	1.68	Eu	0.2	Sr	0.12	Cu	1													O	4		3	2003																												T																																																																																										THC33874																															TSFZ method					Thermal conductivity of lightly Sr- and Zn-doped La2CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B., 67(2003)104503	J.Takeya,S.Komiya,X.F.Sun,Y.Ando		
33875	P067104514		RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8		1	2003								132																				Ru1212																		K				11			11																																																																																														RuO2,SnO2,SrCO3,R2O3,CuO	1	CAL(960C,12h,in air)-pellet-SIN(1010C,10h,in N2 + 1050C,10h,inO2)					Effect of Sn, Nb, and La substitution on superconductivity and magnetic order in RuSr2RCu2O8 (R=Eu,Gd)			Unversitat Stuttgart, Stuttgart, Germany	Phys.Rev.B., 67(2003)104514	G.V.M.Williams,Ho Keun Lee,S.Kramer		
33876	P067104514		(Ru,Sn)Sr2EuCu2O8	Ru0.9Sn0.1Sr2Eu1Cu2O8	Ru	0.9	Sn	0.1	Sr	2	Eu	1	Cu	2											O	8		1	2003								84																				Ru1212																		K				16			16																																																																																														RuO2,SnO2,SrCO3,R2O3,CuO	1	CAL(960C,12h,in air)-pellet-SIN(1010C,10h,in N2 + 1050C,10h,inO2)					Effect of Sn, Nb, and La substitution on superconductivity and magnetic order in RuSr2RCu2O8 (R=Eu,Gd)			Unversitat Stuttgart, Stuttgart, Germany	Phys.Rev.B., 67(2003)104514	G.V.M.Williams,Ho Keun Lee,S.Kramer		
33877	P067104514		(Ru,Sn)Sr2EuCu2O8	Ru0.7Sn0.3Sr2Eu1Cu2O8	Ru	0.7	Sn	0.3	Sr	2	Eu	1	Cu	2											O	8		1	2003								36																				Ru1212																		K				20			20																																																																																														RuO2,SnO2,SrCO3,R2O3,CuO	1	CAL(960C,12h,in air)-pellet-SIN(1010C,10h,in N2 + 1050C,10h,inO2)					Effect of Sn, Nb, and La substitution on superconductivity and magnetic order in RuSr2RCu2O8 (R=Eu,Gd)			Unversitat Stuttgart, Stuttgart, Germany	Phys.Rev.B., 67(2003)104514	G.V.M.Williams,Ho Keun Lee,S.Kramer		
33878	P067104514	not s/c	(Ru,Nb)Sr2EuCu2O8	Ru0.6Nb0.4Sr2Eu1Cu2O8	Ru	0.6	Nb	0.4	Sr	2	Eu	1	Cu	2											O	8		1	2003								50																				Ru1212																		K																																																																																																					RuO2,SnO2,SrCO3,R2O3,CuO	1	CAL(960C,12h,in air)-pellet-SIN(1010C,10h,in N2 + 1050C,10h,inO2)					Effect of Sn, Nb, and La substitution on superconductivity and magnetic order in RuSr2RCu2O8 (R=Eu,Gd)			Unversitat Stuttgart, Stuttgart, Germany	Phys.Rev.B., 67(2003)104514	G.V.M.Williams,Ho Keun Lee,S.Kramer		
33879	P067092504	thickness=600A	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		5	2003																												Bi2212			A			30.966												K	88.4	93.1	97.4				93.1																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33880	P067092504	thickness=600A	Bi2Sr2(Ca,Sr)Cu2O8	Bi2Sr2.08Ca0.92Cu2O8	Bi	2	Sr	2.08	Ca	0.92	Cu	2													O	8		5	2003																												Bi2212			A			31.002												K	88.6	95.3	99.6				95.3																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33881	P067092504	thickness=600A	Bi2Sr2(Ca,Sr)Cu2O8	Bi2Sr2.2Ca0.8Cu2O8	Bi	2	Sr	2.2	Ca	0.8	Cu	2													O	8		5	2003																												Bi2212			A			31.056												K	84	89.9	94.2				89.9																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33882	P067092504	thickness=600A	Bi2Sr2(Ca,Sr)Cu2O8	Bi2Sr2.4Ca0.6Cu2O8	Bi	2	Sr	2.4	Ca	0.6	Cu	2													O	8		5	2003																												Bi2212			A			31.108												K	85.5	94.2	99.6				94.2																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33883	P067092504	thickness=600A	Bi2Sr2(Ca,Sr)Cu2O8	Bi2Sr2.65Ca0.35Cu2O8	Bi	2	Sr	2.65	Ca	0.35	Cu	2													O	8		5	2003																												Bi2212			A			31.206												K	80	93.6	101.2				93.6																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33884	P067092504	thickness=600A	Bi2Sr2SrCu2O8	Bi2Sr3Cu2O8	Bi	2	Sr	3	Cu	2															O	8		5	2003																												Bi2212			A			31.348												K	55.5	91.5	101.7				91.5																																																																																																MBE method. substrate=SrTiO3, oxidation using ozone beam at Ts=720-730 C.					Complete substitution of Sr for Ca in Bi2Sr2+xCa1-xCu2O8+z			Department of Physics,University of Illinois, Urbana,Illinois,USA	Phys.Rev.B., 67(2003)092504	J.N.Eckstein,L.Maritano,S.Oh,T.Di.Luccio,V.Lukic		
33885	JP01410693	R-ion radius vs Tc.	(La,Pr,Ca)Ba2Cu3O7	La0.2Pr0.3Ca0.5Ba2Cu3O7-z	La	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K				100			100																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33886	JP01410693	R-ion radius vs Tc.	(Pr,Ca)Ba2Cu3O7	Pr0.5Ca0.5Ba2Cu3O7-z	Pr	0.5	Ca	0.5	Ba	2	Cu	3													O	7-z		1	2002																												Y123																		K				105			105																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33887	JP01410693	R-ion radius vs Tc.	(Nd,Pr,Ca)Ba2Cu3O7	Nd0.2Pr0.3Ca0.5Ba2Cu3O7-z	Nd	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K				100			100																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33888	JP01410693	R-ion radius vs Tc.	(Sm,Pr,Ca)Ba2Cu3O7	Sm0.2Pr0.3Ca0.5Ba2Cu3O7-z	Sm	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K				98			98																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33889	JP01410693	R-ion radius vs Tc.	(Eu,Pr,Ca)Ba2Cu3O7	Eu0.2Pr0.3Ca0.5Ba2Cu3O7-z	Eu	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K				96			96																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33890	JP01410693	R-ion radius vs Tc.	(Gd,Pr,Ca)Ba2Cu3O7	Gd0.2Pr0.3Ca0.5Ba2Cu3O7-z	Gd	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K				96			96																																																																																														R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33891	JP01410693	R-ion radius vs Tc. hydrostatic-P (up to 1.05 GPa)	(Y,Pr,Ca)Ba2Cu3O7	Y0.2Pr0.3Ca0.5Ba2Cu3O7-z	Y	0.2	Pr	0.3	Ca	0.5	Ba	2	Cu	3											O	7-z		1	2002																												Y123																		K	60			105			105			K/GPa	5																																																																																										R2O3,CaCO3,BaCO3,CuO	1	high-pressure synthesis. precursor (R,Pr)0.5Ca0.5Ba2Cu3Oz - wrapped in Au foil - heat(900C,0.5h, p=6GPa)					The effect of Ca doping on the superconductivity of (R0.4Pr0.6)Ba2Cu3O7-z compounds prepared at high pressure (R=La,Pr,Nd,Sm,Eu,Gd and Y)			National Lab for Superconductivity, Chinese Academy of Science, Beijing, China	J.Phys.:Condens.Matter, 14(2002)10693	C.Dong,G.Che,H.Xiong,S.Jia,Y.Ni,Y.Yao,Z.Liu,Z.Zhao		
33892	JP01410747	Tc,Tm increase with P in the same way. Tc1, Tc2 in Fig. show T3, T1. magnetic ordering Tm defined as the peak of dR/dT. dTm/dP=5.7 K/GPa. B=173 GPa (P>6GPa)	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2002							130											GPa		136								Ru1212			A	3.836		11.527												K	35.5		46				40.75	TC33892		K/GPa	1.9																																																																																											1	solid state reaction					The effect of pressure on the superconductivity and magnetism of RuSr2GdCu2O8			Department of Physics, Faculty of Science, Kyushu University, Fukuoka, Japan	J.Phys.:Condens.Matter, 14(2002)10747	D.P.Hai,F.Honda,G.Oomi,K.Kadowaki,S.Kamizawa,T.Eto		
33893	PHC3860122	ANN sample. hole = 0.34	(Bi,Pb,S)Sr2(Ca,Nd)Cu2Oz	Bi0.8Pb0.1S0.1Sr2Ca0.7Nd0.3Cu2O6.95	Bi	0.8	Pb	0.1	S 	0.1	Sr	2	Ca	0.7	Nd	0.3	Cu	2							O	z	6.95		2003																												Bi1212			A	3.826	3.799	12.01												K				75			75																																																																																															1	SIN(850-860C,40h). some are ANN in flowing O2.					Structure and Superconductivity of (Bi,Pb,S)-1212 compound			University of New South Wales, Australia	Physica C, 386(2003)122	C.F.Yang,Y.Feng,Y.Zhao		
33894	PHC3860122	SIN sample. hole = 0.36	(Bi,Pb,S)Sr2(Ca,Nd)Cu2Oz	Bi0.6Pb0.2S0.2Sr2Ca0.7Nd0.3Cu2O6.95	Bi	0.6	Pb	0.2	S 	0.2	Sr	2	Ca	0.7	Nd	0.3	Cu	2							O	z	6.95		2003																												Bi1212			A	3.828	3.795	12.02												K				80			80																																																																																															1	SIN(850-860C,40h). some are ANN in flowing O2.					Structure and Superconductivity of (Bi,Pb,S)-1212 compound			University of New South Wales, Australia	Physica C, 386(2003)122	C.F.Yang,Y.Feng,Y.Zhao		
33895	PHC3860122	ANN sample. hole = 0.34	(Bi,Pb,S)Sr2(Ca,Nd)Cu2Oz	Bi0.5Pb0.25S0.25Sr2Ca0.7Nd0.3Cu2O6.97	Bi	0.5	Pb	0.25	S 	0.25	Sr	2	Ca	0.7	Nd	0.3	Cu	2							O	z	6.97		2003																												Bi1212			A	3.821	3.822	12.01												K				75			75																																																																																															1	SIN(850-860C,40h). some are ANN in flowing O2.					Structure and Superconductivity of (Bi,Pb,S)-1212 compound			University of New South Wales, Australia	Physica C, 386(2003)122	C.F.Yang,Y.Feng,Y.Zhao		
33896	PHC3860122	ANN sample. hole = 0.35	(Bi,Pb,S)Sr2(Ca,Nd)Cu2Oz	Bi0.2Pb0.4S0.4Sr2Ca0.7Nd0.3Cu2O6.99	Bi	0.2	Pb	0.4	S 	0.4	Sr	2	Ca	0.7	Nd	0.3	Cu	2							O	z	6.99		2003																												Bi1212			A	3.813	3.823	11.96												K				78			78																																																																																															1	SIN(850-860C,40h). some are ANN in flowing O2.					Structure and Superconductivity of (Bi,Pb,S)-1212 compound			University of New South Wales, Australia	Physica C, 386(2003)122	C.F.Yang,Y.Feng,Y.Zhao		
33897	JP01407383		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2002																												T			A	3.771		13.241												K			37.5				37.5																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33898	JP01407383		(La,Pr,Sr)2CuO4	La1.75Pr0.1Sr0.15Cu1O4	La	1.75	Pr	0.1	Sr	0.15	Cu	1													O	4		1	2002																												T			A	3.764		13.24												K			37.4				37.4																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33899	JP01407383		(La,Pr,Sr)2CuO4	La1.35Pr0.5Sr0.15Cu1O4	La	1.35	Pr	0.5	Sr	0.15	Cu	1													O	4		1	2002																												T			A	3.746		13.012												K			34.3				34.3																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33900	JP01407383		(La,Pr,Sr)2CuO4	La0.85Pr1Sr0.15Cu1O4	La	0.85	Pr	1	Sr	0.15	Cu	1													O	4		1	2002																												T			A	3.718		12.763												K			32.6				32.6																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33901	JP01407383	two phases, T' phase (a=3.925, c=12.292)	(La,Pr,Sr)2CuO4	La0.65Pr1.2Sr0.15Cu1O4	La	0.65	Pr	1.2	Sr	0.15	Cu	1													O	4			2002																												T			A	3.71		12.746												K			31.4				31.4																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33902	JP01407383	two phases, T  phase (a=3.706, c=12.741)	(La,Pr,Sr)2CuO4	La0.55Pr1.3Sr0.15Cu1O4	La	0.55	Pr	1.3	Sr	0.15	Cu	1													O	4			2002																												T'			A	3.925		12.286												K			29.6				29.6																																																																																															1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33903	JP01407383	not s/c	(La,Pr,Sr)2CuO4	La0.35Pr1.5Sr0.15Cu1O4	La	0.35	Pr	1.5	Sr	0.15	Cu	1													O	4			2002																												T'			A	3.925		12.286																																																																																																																		1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33904	JP01407383	not s/c	(Pr,Sr)2CuO4	Pr1.85Sr0.15Cu1O4	Pr	1.85	Sr	0.15	Cu	1															O	4			2002																												T'			A	3.925		12.282																																																																																																																		1	solid state reaction					Crystallographic evolution and superconductivity in the La1.85-xPrxSr0.15CuO4 system (0=<x=<1.85)			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)7383	Changjin Zhang,Yuheng Zhang		
33905	JP01409659		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			2002																												T			A	3.779		13.251												K			37				37																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33906	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.99Fe0.01O4	La	1.85	Sr	0.15	Cu	0.99	Fe	0.01													O	4			2002																												T			A	3.78		13.2457												K			33				33																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33907	JP01409659	Tc(onset) = nearly zero.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.98Fe0.02O4	La	1.85	Sr	0.15	Cu	0.98	Fe	0.02													O	4			2002																												T			A	3.7806		13.2421												K			0				0																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33908	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.84Sr0.16Cu0.99Fe0.01O4	La	1.84	Sr	0.16	Cu	0.99	Fe	0.01													O	4			2002																												T			A	3.78		13.246												K			35				35																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33910	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.83Sr0.17Cu0.98Fe0.02O4	La	1.83	Sr	0.17	Cu	0.98	Fe	0.02													O	4			2002																												T			A	3.7801		13.2448												K			31				31																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33911	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.82Sr0.18Cu0.97Fe0.03O4	La	1.82	Sr	0.18	Cu	0.97	Fe	0.03													O	4			2002																												T			A	3.7807		13.2405												K			29				29																																																																																															1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33912	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.8Sr0.2Cu0.95Fe0.05O4	La	1.8	Sr	0.2	Cu	0.95	Fe	0.05													O	4			2002																												T			A	3.7817		13.2382												K					4																																																																																																	1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33913	JP01409659		(La,Sr)2(Cu,Fe)O4	La1.75Sr0.25Cu0.9Fe0.1O4	La	1.75	Sr	0.25	Cu	0.9	Fe	0.1													O	4			2002																												T			A	3.7825		13.2263												K					4																																																																																																	1	solid state reaction					Effects of Fe doping of La1.85Sr0.15CuO4			Structure Research Lab, University of Science and Technology of China, Hefei,China	J.Phys.:Condens.Matter, 14(2002)9659	Changjin Zhang,Yuheng Zhang		
33914	EPL0580758	not s/c upto 8 GPa	Sr14Cu24O41	Sr14Cu24O41	Sr	14	Cu	24																	O	41		3	2002																												LAD																		K					2																																																																																																		single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33915	EPL0580758	not s/c upto 8 GPa	(Sr,Ca)14Cu24O41	Sr11Ca3Cu24O41	Sr	11	Ca	3	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33916	EPL0580758	not s/c upto 8 GPa	(Sr,Ca)14Cu24O41	Sr11Ca6Cu24O41	Sr	11	Ca	6	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33917	EPL0580758	not s/c upto 8 GPa	(Sr,Ca)14Cu24O41	Sr11Ca8Cu24O41	Sr	11	Ca	8	Cu	24															O	41		3	2002																												LAD																		K					2																																																																																																		single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33918	EPL0580758	pressure-induced s/c. critical-P = 5 GPa. Tc(max)=3 K at P=5 GPa.	(Sr,Ca)14Cu24O41	Sr11Ca10Cu24O41	Sr	11	Ca	10	Cu	24															O	41		3	2002																												LAD																		K		3			0		3																																																																																																single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33919	EPL0580758	pressure-induced s/c. critical-P = 3.5 GPa. Tc(max)=5 K at P=3.5 GPa.	(Sr,Ca)14Cu24O41	Sr11Ca12Cu24O41	Sr	11	Ca	12	Cu	24															O	41		3	2002																												LAD																		K		5			0		5																																																																																																single crystals were grown by TSFZ method.					Electronic phase diagram of a hole-doped two-leg ladder system, Sr14-xCaxCu24O41			Department of Superconductivity,The University of Tokyo,Bunkyo-ku,Tokyo,Japan	Europhys.Lett., 58(2002)758	H.Eisaki,H.Takahashi,N.Mori,N.Motoyama,N.Takeshita,S.Uchida,T.Nakanishi		
33920	L090137001	P-induced SC. s/c and NMR measurements at P=3.5 GPa. Tc(P=3.5 GPa) = 4.8 K. spin gap = 173 and 217 K from 1/T1 and K-shift.	(Sr,Ca)14Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2003																												LAD																		K				4.8	0		4.8																																		HC33920																																																														not shown					Superconductivity of the Sr2Ca12Cu24O41 spin-ladder system: Are the superconducting pairing and the spin-gap formation of the same origin?			ISSP, University of Tokyo, Kashiwa, Chiba, Japan	Phys.Rev.Lett., 90(2003)137001	N.Fujiwara,N.Mori,N.Motoyama,S.Uchida,T.Matsumoto,Y.Uwatoko		
33921	L090137002	heavily underdoped sample. anisotropy=600 (T=0.5Tc)	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2003																												Bi2212																		K				69.4			69.4																																									micron.m	Josephson plasma and magnetization		0.4	240																																																			TSFZ method(25 mbar-O2) + ANN(700C, 1 week, flowing N2)					Vortex fluctuations in underdoped Bi2Sr2CaCu2O8+z crystals			CNRS-UMR, Ecole Polytechnique, Palaiseau, France	Phys.Rev.Lett., 90(2003)137002	C.J.van der beek,M.Gaifullin,M.Konczykowski,M.Li,P.Gierlowski,P.H.Kes,S.Colson,Y.Matsuda		
33922	PRL0842945	slightly underdoped. anisotropy=550.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2000																												Bi2212																		K		82.5					82.5																																									micron.m	Josephson plasma and magnetization		0.2	110																																																			TFZ method					Abrupt change of Josephson plasma frequency at the phase boundary of the Bragg glass in Bi2Sr2CaCu2O8+z			ISSP, University of Tokyo, Kashiwa, Chiba, Japan	Phys.Rev.Lett., 84(2000)2945	J.Shimoyama,K.Kishio,M.B.Gaifullin,N.Chikumoto,Y.Matsuda		
33923	JP015L017	Tc(O<18>)=59.3 K. ppenet were measured by muon-SR but not shown numerically.	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.942	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.942	1	2003																												Y123																		K				60.6			60.6						0.22	O	98																																																																																							1	The exchange and back-exchange were carried out at 600C.					The oxygen-isotope effect on the in-plane penetration depth in underdoped Y1-xPrxBa2Cu3O7-z as revealed by muon-spin rotation			Physik-Institut der Universitat Zurich, Zurich, Switzerland	J.Phys.:Condens.Matter, 15(2003)L17	A.Shengelaya,E.Morenzoni,H.Keller,I.M.Savic,K.Conder,R.Khasanov		
33924	JP015L017	Tc(O<18>)=43.6 K. ppenet were measured by muon-SR but not shown numerically.	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.929	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.929	1	2003																												Y123																		K				45.3			45.3						0.37	O	78																																																																																							1	The exchange and back-exchange were carried out at 600C.					The oxygen-isotope effect on the in-plane penetration depth in underdoped Y1-xPrxBa2Cu3O7-z as revealed by muon-spin rotation			Physik-Institut der Universitat Zurich, Zurich, Switzerland	J.Phys.:Condens.Matter, 15(2003)L17	A.Shengelaya,E.Morenzoni,H.Keller,I.M.Savic,K.Conder,R.Khasanov		
33925	PHC3870411		YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2003																												Y123			A	3.811	3.875	11.651												K		93					93																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33926	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.9Pr0.05Ca0.05Ba2Cu3O7-z	Y	0.9	Pr	0.05	Ca	0.05	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.822	3.88	11.667												K		86.2					86.2																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33927	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.8Pr0.1Ca0.1Ba2Cu3O7-z	Y	0.8	Pr	0.1	Ca	0.1	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.822	3.883	11.667												K		83					83																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33928	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.7Pr0.15Ca0.15Ba2Cu3O7-z	Y	0.7	Pr	0.15	Ca	0.15	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.823	3.882	11.665												K		75.8					75.8																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33929	PHC3870411		(Y,Ca)Ba2Cu3O7	Y0.98Ca0.02Ba2Cu3O7-z	Y	0.98	Ca	0.02	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.822	3.884	11.674												K		90.5					90.5																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33930	PHC3870411		(Y,Ca)Ba2Cu3O7	Y0.95Ca0.05Ba2Cu3O7-z	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.817	3.879	11.665												K		88.6					88.6																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33931	PHC3870411		(Y,Ca)Ba2Cu3O7	Y0.92Ca0.08Ba2Cu3O7-z	Y	0.92	Ca	0.08	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.825	3.887	11.689												K		87					87																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33932	PHC3870411		(Y,Pr)Ba2Cu3O7	Y0.95Pr0.05Ba2Cu3O7-z	Y	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.817	3.88	11.67												K		91.8					91.8																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33933	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.93Pr0.05Ca0.02Ba2Cu3O7-z	Y	0.93	Pr	0.05	Ca	0.02	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.817	3.883	11.672												K		89.4					89.4																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33934	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.91Pr0.05Ca0.04Ba2Cu3O7-z	Y	0.91	Pr	0.05	Ca	0.04	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.822	3.884	11.679												K		87.3					87.3																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33935	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.89Pr0.05Ca0.06Ba2Cu3O7-z	Y	0.89	Pr	0.05	Ca	0.06	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.819	3.882	11.67												K		85.9					85.9																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33936	PHC3870411		(Y,Pr)Ba2Cu3O7	Y0.9Pr0.1Ba2Cu3O7-z	Y	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.823	3.879	11.66												K		88.8					88.8																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33937	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.88Pr0.1Ca0.02Ba2Cu3O7-z	Y	0.88	Pr	0.1	Ca	0.02	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.823	3.883	11.679												K		87					87																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33938	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.86Pr0.1Ca0.04Ba2Cu3O7-z	Y	0.86	Pr	0.1	Ca	0.04	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.823	3.888	11.684												K		85.5					85.5																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33939	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.84Pr0.1Ca0.06Ba2Cu3O7-z	Y	0.84	Pr	0.1	Ca	0.06	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.817	3.879	11.66												K		84.6					84.6																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33940	PHC3870411		(Y,Pr,Ca)Ba2Cu3O7	Y0.82Pr0.1Ca0.08Ba2Cu3O7-z	Y	0.82	Pr	0.1	Ca	0.08	Ba	2	Cu	3											O	7-z		1	2003																												Y123			A	3.823	3.88	11.665												K		83.4					83.4																																																																																														Y2O3,Pr6O11,CaCO3,BaCO3,CuO	1	ANN(400C, 24h) - slow cool to RT					Pr and Ca co-doping effects on the flux pinning properties in (Y1-x-yPrxCay)Ba2Cu3O7-z			Department of Fundamental Energy Science, Kyoto University, Gokasho, Uji, Kyoto-fu, Japan	Physica C, 387(2003)411	K.Yoshida,T.Harada		
33941	PHC3900075		(Bi,Pb)(Sr,La)CuOz	Bi1.6Pb0.4Sr1.6La0.4Cu1Oz	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	1											O	z		1	2003																												Bi2201																		K		34.8					34.8																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33942	PHC3900075		(Bi,Pb)(Sr,La)(Cu,Mn)Oz	Bi1.6Pb0.4Sr1.6La0.4Cu0.99Mn0.01Oz	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	0.99	Mn	0.01									O	z		1	2003																												Bi2201																		K		30.9					30.9																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33943	PHC3900075		(Bi,Pb)(Sr,La)(Cu,Mn)Oz	Bi1.6Pb0.4Sr1.6La0.4Cu0.98Mn0.02Oz	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	0.98	Mn	0.02									O	z		1	2003																												Bi2201																		K		26.1					26.1																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33944	PHC3900075		(Bi,Pb)(Sr,La)(Cu,Mn)Oz	Bi1.6Pb0.4Sr1.6La0.4Cu0.97Mn0.03Oz	Bi	1.6	Pb	0.4	Sr	1.6	La	0.4	Cu	0.97	Mn	0.03									O	z		1	2003																												Bi2201																		K		20.1					20.1																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33945	PHC3900075		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2003																												T																		K		38					38																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33946	PHC3900075		(La,Sr)2(Cu,Mn)O4	La1.84Sr0.16Cu0.99Mn0.01O4	La	1.84	Sr	0.16	Cu	0.99	Mn	0.01													O	4		1	2003																												T																		K		30.4					30.4																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33947	PHC3900075		(La,Sr)2(Cu,Mn)O4	La1.83Sr0.17Cu0.98Mn0.02O4	La	1.83	Sr	0.17	Cu	0.98	Mn	0.02													O	4		1	2003																												T 																		K		18.1					18.1																																																																																															1	Solid state reaction					Different Tc-suppression rates between Mn doped La214 and Bi2201 systems			University of Science and Technology of China, Hefei, Anhui,P R China	Physica C, 390(2003)75	B.Liu,C.Zhang,G.Xu,J.Zhang,Q.Pu,Y.Zhang,Z.Ding		
33948	PHC3900120		Tl2Ba2CaCu2O8	Tl2Ba2Ca1Cu2O8+z	Tl	2	Ba	2	Ca	1	Cu	2													O	8+z		1	2003																												Tl2212																		K		108					108																																																																		uV/K	1.48																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33949	PHC3900120		Tl2Ba2Ca(Cu,Co)2O8	Tl2Ba2Ca1Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	1	Cu	1.96	Co	0.04											O	8+z		1	2003																												Tl2212																		K		101.3					101.3																																																																		uV/K	3.55																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33950	PHC3900120		Tl2Ba2Ca(Cu,Co)2O8	Tl2Ba2Ca1Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	1	Cu	1.92	Co	0.08											O	8+z		1	2003																												Tl2212																		K		94.2					94.2																																																																		uV/K	4.73																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33951	PHC3900120		Tl2Ba2Ca(Cu,Co)2O8	Tl2Ba2Ca1Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	1	Cu	1.88	Co	0.12											O	8+z		1	2003																												Tl2212																		K		88.5					88.5																																																																		uV/K	7.09																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33952	PHC3900120	carrier p=0.183/Cu from Hall effect.	Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.95Y0.05Cu2O8+z	Tl	2	Ba	2	Ca	0.95	Y	0.05	Cu	2											O	8+z		1	2003																												Tl2212																		K		106.5					106.5																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33953	PHC3900120	carrier p=0.182/Cu from Hall effect.	Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.95Y0.05Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.95	Y	0.05	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		102.4					102.4																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33954	PHC3900120	carrier p=0.185/Cu from Hall effect.	Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.95Y0.05Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.95	Y	0.05	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K		92.6					92.6																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33959	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.95Y0.05Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	0.95	Y	0.05	Cu	1.88	Co	0.12									O	8+z		1	2003																												Tl2212																		K		85.5					85.5																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33960	PHC3900120		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.9Y0.1Cu2O8+z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	2											O	8+z		1	2003																												Tl2212																		K		105.8					105.8																																																																		uV/K	7.68																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33961	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.9Y0.1Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		97.9					97.9																																																																		uV/K	9.16																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33962	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.9Y0.1Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K		88.5					88.5																																																																		uV/K	13.3																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33963	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.9Y0.1Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	0.9	Y	0.1	Cu	1.88	Co	0.12									O	8+z		1	2003																												Tl2212																		K		78					78																																																																		uV/K	17.4																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33964	PHC3900120		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.85Y0.15Cu2O8+z	Tl	2	Ba	2	Ca	0.85	Y	0.15	Cu	2											O	8+z		1	2003																												Tl2212																		K		102.8					102.8																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33965	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.85Y0.15Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.85	Y	0.15	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		86.7					86.7																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33966	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.85Y0.15Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.85	Y	0.15	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K		76.2					76.2																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33967	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.85Y0.15Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	0.85	Y	0.15	Cu	1.88	Co	0.12									O	8+z		1	2003																												Tl2212																		K		61.6					61.6																																																																																															1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33968	PHC3900120		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.8Y0.2Cu2O8+z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	2											O	8+z		1	2003																												Tl2212																		K		77.7					77.7																																																																		uV/K	20.4																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33969	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.8Y0.2Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		66.8					66.8																																																																		uV/K	23.9																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33970	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.8Y0.2Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K		60.1					60.1																																																																		uV/K	26.3																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33971	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.8Y0.2Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	0.8	Y	0.2	Cu	1.88	Co	0.12									O	8+z		1	2003																												Tl2212																		K		45.1					45.1																																																																		uV/K	32.2																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33972	PHC3900120		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.75Y0.25Cu2O8+z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	2											O	8+z		1	2003																												Tl2212																		K		54.8					54.8																																																																		uV/K	37.8																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33973	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.75Y0.25Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		39.9					39.9																																																																		uV/K	43.7																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33974	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.75Y0.25Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K		29.7					29.7																																																																		uV/K	51.7																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33975	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.75Y0.25Cu1.88Co0.12O8+z	Tl	2	Ba	2	Ca	0.75	Y	0.25	Cu	1.88	Co	0.12									O	8+z		1	2003																												Tl2212																		K		19.3					19.3																																																																		uV/K	56.2																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33976	PHC3900120		Tl2Ba2(Ca,Y)Cu2O8	Tl2Ba2Ca0.7Y0.3Cu2O8+z	Tl	2	Ba	2	Ca	0.7	Y	0.3	Cu	2											O	8+z		1	2003																												Tl2212																		K		31.6					31.6																																																																		uV/K	52.3																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33977	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.7Y0.3Cu1.96Co0.04O8+z	Tl	2	Ba	2	Ca	0.7	Y	0.3	Cu	1.96	Co	0.04									O	8+z		1	2003																												Tl2212																		K		21.5					21.5																																																																		uV/K	55.9																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33978	PHC3900120		Tl2Ba2(Ca,Y)(Cu,Co)2O8	Tl2Ba2Ca0.7Y0.3Cu1.92Co0.08O8+z	Tl	2	Ba	2	Ca	0.7	Y	0.3	Cu	1.92	Co	0.08									O	8+z		1	2003																												Tl2212																		K																																																																									uV/K	60																												1	mixture - pellet - wrapped in Pt-foil sealed quartz tube. ANN(830C,6h) - cool to RT (40 C/h)					Effects of Co-substitution on superconductivity and transport in Tl2Ba2Ca1-xYx(Cu1-yCoy)2O8+z			Saha Institute of Nuclear Physics, Bidhannagar, Kolkata,India	Physica C, 390(2003)120	A.Poddar,B.Bandyopadhyay,B.Chattopadhyay		
33979	MAT0305503	Hc1(0) is  at 1.9K. G-L parameter = 140. delta-C/Tc = 107 mj/f.u.K2. delta-C/k*Tc = 0.67	NaxCoO2.yH2O	Na0.31Co1H2.6O3.3	Na	0.31	Co	1	H	2.6															O	3.3		1	2003																															A	2.82		19.65												K				4.3			4.3										10	Oe		13			13			1.9	T	estimated using WHH	10							kOe/K		34					A		57			A	calculated from Hc1	7900										SP33979			mj/f.u.K2	159		185	specific heat																																				Na in Na0.74CoO2 was deintercalated by excess Br in acetonitrile.					Layered cobalt oxyhydrate as a heavy-fermion compound with extreme type-II superconductivity			Department of Physics, Zhejiang University, Hangzhou  China	cond-mat/0305503	C.Feng,G.Cao,J.Shen,M.Fang,W.Lu,Yi Xu,Z.Xu		
33980	PHC3900254	niminal=Y:Ba:Cu=1:2:3, composition by ICP. Al-content from Al2O3 crucible.	YBa2(Cu,Al)3O7	Y1Ba2Cu2.75Al0.25O7-z	Y	1	Ba	2	Cu	2.75	Al	0.25													O	7-z		3	2003																												Y123																		K			80.8				80.8																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33981	PHC3900254	niminal=Y:Eu:Ba:Cu=0.9:0.1:2:3, composition by ICP. Al-content from Al2O3 crucible.	(Y,Eu)(Ba,Eu)2(Cu,Al)3O7	Y0.9Eu0.13Ba1.97Cu2.87Al0.29O7-z	Y	0.9	Eu	0.13	Ba	1.97	Cu	2.87	Al	0.29											O	7-z		3	2003																												Y123																		K			72.6				72.6																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33982	PHC3900254	niminal=Y:Eu:Ba:Cu=0.8:0.2:2:3, composition by ICP. Al-content from Al2O3 crucible.	(Y,Eu)(Ba,Eu)2(Cu,Al)3O7	Y0.88Eu0.17Ba1.95Cu2.82Al0.32O7-z	Y	0.88	Eu	0.17	Ba	1.95	Cu	2.82	Al	0.32											O	7-z		3	2003																												Y123																		K			67.5				67.5																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33983	PHC3900254	niminal=Y:Eu:Ba:Cu=0.7:0.3:2:3, composition by ICP. Al-content from Al2O3 crucible.	(Y,Eu)(Ba,Eu)2(Cu,Al)3O7	Y0.74Eu0.35Ba1.91Cu2.81Al0.3O7-z	Y	0.74	Eu	0.35	Ba	1.91	Cu	2.81	Al	0.3											O	7-z		3	2003																												Y123																		K			59.9				59.9																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33984	PHC3900254	niminal=Y:Eu:Ba:Cu=0.6:0.4:2:3, composition by ICP. Al-content from Al2O3 crucible.	(Y,Eu)(Ba,Eu)2(Cu,Al)3O7	Y0.68Eu0.39Ba1.93Cu2.73Al0.32O7-z	Y	0.68	Eu	0.39	Ba	1.93	Cu	2.73	Al	0.32											O	7-z		3	2003																												Y123																		K			47.5				47.5																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33985	PHC3900254	niminal=Y:Eu:Ba:Cu=0.5:0.5:2:3, composition by ICP. Al-content from Al2O3 crucible.	(Y,Eu)(Ba,Eu)2(Cu,Al)3O7	Y0.52Eu0.58Ba1.9Cu2.69Al0.42O7-z	Y	0.52	Eu	0.58	Ba	1.9	Cu	2.69	Al	0.42											O	7-z		3	2003																												Y123																		K			42.4				42.4																																																																																																self-flux method using Al2O3 crucible. heat(1015C,12h) - cool to 930 C(0.5 C/h)					Preparation and properties of (Y,Eu)-123 superconducting single crystals			Department of Materials Physics, University of Science and Technology Beijing, Beijing , China	Physica C, 390(2003)254	G.Cao,J.H.Ross Jr.,X.Xiong,Y.Li,Y.Liu,Z.Yin		
33986	JP01103169	Bi:Sr:Ca:Er:Cu=1.9:1.9:1.2:0:2 by ICP.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8		3	2003																												Bi2212			A			30.85												K		84					84																																																																																																self-flux method. using Al2O3 crucible. heat(900C,10h) - cool to 760C at 2 C/h.					Anisotropic resistivity of the antiferromagnetic insulator Bi2Sr2ErCu2O8			Department of Applied Physics, Waseda University, Tokyo, Japan	J.Phys.: Condens.Matter, 11(1999)3169	I.Terasaki,T.Kitajima,T.Takayanagi,T.Takemura		
33987	JP01103169	Bi:Sr:Ca:Er:Cu=1.6:1.8:1.2:0.1:2 by ICP.	Bi2Sr2(Ca,Er)Cu2O8	Bi2Sr2Ca0.9Er0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Er	0.1	Cu	2											O	8		3	2003																												Bi2212			A			30.9												K		87					87																																																																																																self-flux method. using Al2O3 crucible. heat(1020C,10h) - cool to 820C at 2 C/h.					Anisotropic resistivity of the antiferromagnetic insulator Bi2Sr2ErCu2O8			Department of Applied Physics, Waseda University, Tokyo, Japan	J.Phys.: Condens.Matter, 11(1999)3169	I.Terasaki,T.Kitajima,T.Takayanagi,T.Takemura		
33988	JP01103169	Bi:Sr:Ca:Er:Cu=1.6:1.9:1.0:0.5:2 by ICP. R<c>/R<ab> = maximum at 240 K.	Bi2Sr2(Ca,Er)Cu2O8	Bi2Sr2Ca0.5Er0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Er	0.5	Cu	2											O	8		3	2003																												Bi2212			A			30.32												K					4.2																																																																																																		self-flux method. using Al2O3 crucible. heat(1020C,10h) - cool to 820C at 2 C/h.					Anisotropic resistivity of the antiferromagnetic insulator Bi2Sr2ErCu2O8			Department of Applied Physics, Waseda University, Tokyo, Japan	J.Phys.: Condens.Matter, 11(1999)3169	I.Terasaki,T.Kitajima,T.Takayanagi,T.Takemura		
33989	JP01103169	Bi:Sr:Ca:Er:Cu=2.0:2.1:0:0.6:2 by ICP.  R<c>/R<ab> = maximum at 90 K.	Bi2Sr2ErCu2O8	Bi2Sr2Er1Cu2O8	Bi	2	Sr	2	Er	1	Cu	2													O	8		3	2003																												Bi2212			A			30.33												K					10																																																																																																		self-flux method. using Al2O3 crucible. heat(1020C,10h) - cool to 820C at 2 C/h.					Anisotropic resistivity of the antiferromagnetic insulator Bi2Sr2ErCu2O8			Department of Applied Physics, Waseda University, Tokyo, Japan	J.Phys.: Condens.Matter, 11(1999)3169	I.Terasaki,T.Kitajima,T.Takayanagi,T.Takemura		
33990	P067172501	hole/Cu = 0.17 	Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.9Pr0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Pr	0.1	Cu	2											O	8		3	2003																												Bi2212																		K		86					86																																																																																																self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33991	P067172501	hole/Cu = 0.135	Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.75Pr0.25Cu2O8	Bi	2	Sr	2	Ca	0.75	Pr	0.25	Cu	2											O	8		3	2003																												Bi2212																		K		88					88																																																																																																self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33992	P067172501	hole/Cu = 0.1 	Bi2Sr2(Ca,Pr)Cu2O8	Bi2Sr2Ca0.57Pr0.43Cu2O8	Bi	2	Sr	2	Ca	0.57	Pr	0.43	Cu	2											O	8		3	2003																												Bi2212																		K		48					48																																																																																																self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33993	P067172501	hole/Cu = 0.135 	Bi2Sr2(Ca,Er)Cu2O8	Bi2Sr2Ca0.9Er0.1Cu2O8	Bi	2	Sr	2	Ca	0.9	Er	0.1	Cu	2											O	8		3	2003																												Bi2212																		K		87					87																																																																																																self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33994	P067172501	AF. hole/Cu = 0.05	Bi2Sr2(Ca,Er)Cu2O8	Bi2Sr2Ca0.5Er0.5Cu2O8	Bi	2	Sr	2	Ca	0.5	Er	0.5	Cu	2											O	8		3	2003								50																				Bi2212																																																																																																																									self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33995	P067172501	AF. hole/Cu = 0.025	Bi2Sr2ErCu2O8	Bi2Sr2Er1Cu2O8	Bi	2	Sr	2	Er	1	Cu	2													O	8		3	2003								230																				Bi2212																																																																																																																									self-flux method. See J.Phys.:Condens.Matter, 11(1999)3169					Chemical potential shift in lightly doped to overdoped Bi2Sr2Ca1-xRxCu2O8+y  (R=Pr, Er)			Department of Physics and Department of Complexity Science and Engineering, University of Tokyo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172501	A.Fujimori,I.Terasaki,N.Harima,T.Sugaya		
33996	P067172502	small ferromagnetic component appears.	RuSr2YCu2O8	Ru0.9Sr2Y1Cu2.1O7.9	Ru	0.9	Sr	2	Y	1	Cu	2.1													O	8	7.9		2003								150																				Ru1212																		K		30					30																																																																																																high-T-high-P process.					Bulk superconductivity in Ru0.9Sr2YCu2.1O7.9			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki, Japan	Phys.Rev.B, 67(2003)172502	E.Takayama-Muromachi,T.Kawashima,V.P.S.Awana		
33997	P067184512		LaCuO4	La2Cu1O4	La	2	Cu	1																	O	4		3	2003																												T																																																																																										THC33997																															TSFZ method					Heat transport of La2-yEuyCuO4 and La1.88-yEuySr0.12CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B, 67(2003)184512	S.Komiya,X.F.Sun,Y.Ando		
33998	P067184512	ANN(flowing He)	(La,Eu)2CuO4	La1.98Eu0.02Cu1O4	La	1.98	Eu	0.02	Cu	1															O	4		3	2003																												T																																																																																										THC33998																															TSFZ method					Heat transport of La2-yEuyCuO4 and La1.88-yEuySr0.12CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B, 67(2003)184512	S.Komiya,X.F.Sun,Y.Ando		
33999	P067184512	ANN(flowing He)	(La,Eu)2CuO4	La1.8Eu0.2Cu1O4	La	1.8	Eu	0.2	Cu	1															O	4		3	2003																												T																																																																																										THC33999																															TSFZ method					Heat transport of La2-yEuyCuO4 and La1.88-yEuySr0.12CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B, 67(2003)184512	S.Komiya,X.F.Sun,Y.Ando		
34000	P067184512	ANN(850C,48h,in air)	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4		3	2003																												T																		K		32					32																																																																	THC34000																															TSFZ method					Heat transport of La2-yEuyCuO4 and La1.88-yEuySr0.12CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B, 67(2003)184512	S.Komiya,X.F.Sun,Y.Ando		
34001	P067184512	ANN(850C,48h,in air). filamentary S/C	(La,Eu,Sr)2CuO4	La0.68Eu0.2Sr0.12Cu1O4	La	0.68	Eu	0.2	Sr	0.12	Cu	1													O	4		3	2003																												T																		K		5					5																																																																	THC34001																															TSFZ method					Heat transport of La2-yEuyCuO4 and La1.88-yEuySr0.12CuO4 single crystals			Central Research Institute of Electric Power Industry, Komae, Tokyo, Japan	Phys.Rev.B, 67(2003)184512	S.Komiya,X.F.Sun,Y.Ando		
34002	PHC3910001	Jc measured by M.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2003																												Y123			A	3.816	3.882	11.673												K				93.1			93.1																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34003	PHC3910001	Jc measured by M.	Y(Ba,La)2Cu3O7	Y1Ba2.98La0.02Cu3O7-z	Y	1	Ba	2.98	La	0.02	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.879	11.664												K				94			94																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34004	PHC3910001	Jc measured by M.	Y(Ba,La)2Cu3O7	Y1Ba2.95La0.05Cu3O7-z	Y	1	Ba	2.95	La	0.05	Cu	3													O	7-z		1	2003																												Y123			A	3.814	3.876	11.649												K				94.5			94.5																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34005	PHC3910001	Jc measured by M.	Y(Ba,La)2Cu3O7	Y1Ba2.92La0.08Cu3O7-z	Y	1	Ba	2.92	La	0.08	Cu	3													O	7-z		1	2003																												Y123			A	3.816	3.873	11.646												K				94.2			94.2																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34006	PHC3910001	Jc measured by M.	Y(Ba,La)2Cu3O7	Y1Ba2.88La0.12Cu3O7-z	Y	1	Ba	2.88	La	0.12	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.876	11.655												K				93.3			93.3																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34007	PHC3910001	Jc measured by M.	Y(Ba,La)2Cu3O7	Y1Ba2.85La0.15Cu3O7-z	Y	1	Ba	2.85	La	0.15	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.876	11.652												K				89.9			89.9																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34008	PHC3910001		Y(Ba,Pr)2Cu3O7	Y1Ba2.98Pr0.02Cu3O7-z	Y	1	Ba	2.98	Pr	0.02	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.88	11.667												K				93.3			93.3																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34009	PHC3910001		Y(Ba,Pr)2Cu3O7	Y1Ba2.95Pr0.05Cu3O7-z	Y	1	Ba	2.95	Pr	0.05	Cu	3													O	7-z		1	2003																												Y123			A	3.81	3.874	11.649												K				92.7			92.7																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34010	PHC3910001		Y(Ba,Pr)2Cu3O7	Y1Ba2.92Pr0.08Cu3O7-z	Y	1	Ba	2.92	Pr	0.08	Cu	3													O	7-z		1	2003																												Y123			A	3.817	3.88	11.667												K				91.2			91.2																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34011	PHC3910001		Y(Ba,Pr)2Cu3O7	Y1Ba2.88Pr0.12Cu3O7-z	Y	1	Ba	2.88	Pr	0.12	Cu	3													O	7-z		1	2003																												Y123			A	3.817	3.877	11.661												K				88.2			88.2																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34012	PHC3910001		Y(Ba,Pr)2Cu3O7	Y1Ba2.85Pr0.15Cu3O7-z	Y	1	Ba	2.85	Pr	0.15	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.877	11.661												K				83.6			83.6																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34013	PHC3910001		Y(Ba,Nd)2Cu3O7	Y1Ba2.95Nd0.05Cu3O7-z	Y	1	Ba	2.95	Nd	0.05	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.884	11.673												K				93.7			93.7																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34014	PHC3910001		Y(Ba,Nd)2Cu3O7	Y1Ba2.92Nd0.08Cu3O7-z	Y	1	Ba	2.92	Nd	0.08	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.884	11.676												K				93.5			93.5																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34015	PHC3910001		Y(Ba,Nd)2Cu3O7	Y1Ba2.88Nd0.12Cu3O7-z	Y	1	Ba	2.88	Nd	0.12	Cu	3													O	7-z		1	2003																												Y123			A	3.82	3.884	11.673												K				93.2			93.2																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34016	PHC3910001		Y(Ba,Nd)2Cu3O7	Y1Ba2.85Nd0.15Cu3O7-z	Y	1	Ba	2.85	Nd	0.15	Cu	3													O	7-z		1	2003																												Y123			A	3.82	3.882	11.673												K				93.2			93.2																																																																																																mixture - pellet - CAL(940C,48h, in air) - SIN(920C,24h,in flowing O2) - slow cooling to 400C(1C/min) - ANN(400C, 24h) - FC to RT					The effect of rare-earth substitution at the Ba site on the flux pinning properties of Y(Ba2-xRx)Cu3O7-d (for R = La,Pr,and Nd)			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)1	K.Yoshida,T.Harada		
34017	PHC3910008	Jc-Fig shows Jc(H) at 70 K.	YbBa2Cu3O7	Yb1Ba2Cu3O7-z	Yb	1	Ba	2	Cu	3															O	7-z		1	2003																												Y123			A	3.804	3.874	11.654												K				91			91																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34018	PHC3910008	Jc-Fig shows Jc(H) at 70 K.	(Yb,Pr)Ba2Cu3O7	Yb0.98Pr0.02Ba2Cu3O7-z	Yb	0.98	Pr	0.02	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.806	3.877	11.667												K				91.3			91.3																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34019	PHC3910008	Jc-Fig shows Jc(H) at 70 K.	(Yb,Pr)Ba2Cu3O7	Yb0.96Pr0.04Ba2Cu3O7-z	Yb	0.96	Pr	0.04	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.808	3.877	11.667												K				91.6			91.6																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34020	PHC3910008	Jc-Fig shows Jc(H) at 70 K.	(Yb,Pr)Ba2Cu3O7	Yb0.94Pr0.06Ba2Cu3O7-z	Yb	0.94	Pr	0.06	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.807	3.875	11.656												K				91.5			91.5																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34021	PHC3910008	Jc-Fig shows Jc(H) at 70 K.	(Yb,Pr)Ba2Cu3O7	Yb0.92Pr0.08Ba2Cu3O7-z	Yb	0.92	Pr	0.08	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.81	3.877	11.663												K				91.2			91.2																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34022	PHC3910008		(Yb,Pr)Ba2Cu3O7	Yb0.9Pr0.1Ba2Cu3O7-z	Yb	0.9	Pr	0.1	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.809	3.874	11.653												K				89.9			89.9																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34023	PHC3910008		(Yb,Pr)Ba2Cu3O7	Yb0.85Pr0.15Ba2Cu3O7-z	Yb	0.85	Pr	0.15	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.811	3.876	11.659												K				87.5			87.5																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34024	PHC3910008		(Yb,Pr)Ba2Cu3O7	Yb0.8Pr0.2Ba2Cu3O7-z	Yb	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.814	3.874	11.654												K				82.9			82.9																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34025	PHC3910008		(Yb,Pr)Ba2Cu3O7	Yb0.75Pr0.25Ba2Cu3O7-z	Yb	0.75	Pr	0.25	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.819	3.88	11.666												K				76.1			76.1																																																																																															1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34026	PHC3910008		(Yb,Pr)Ba2Cu3O7	Yb0.7Pr0.3Ba2Cu3O7-z	Yb	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z		1	2003																												Y123			A	3.827	3.878	11.667												K				68			68																																																				JC34017																																											1	ANN(400C, 48h) - cool to RT(!c/min)					Effects of Pr-doping on the pinning properties in YbBa2Cu3O7-d			Department of Fundamental Energy Science, Graduate School of Energy Science, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan	Physica C, 391(2003)8	K.Yashida,T.Harada,T.Kawakami		
34027	PHC3570318	not s/c. nominal composition. two step FM. second Tm = 40 K, maybe Nd-ordering	(Nd,Ce)2CaCu2O6	Nd2.16Ce0.225Ca1Cu2O6.69	Nd	2.16	Ce	0.225	Ca	1	Cu	2													O	z	6.69		2001							150																					0212			A	3.845		19.349												K																																																																																																							high-pressure synthesis(1200 - 1300C, 6GPa)					High-pressure synthesis of 0212-, 1201- and 1212-type copper oxides			NIMS, Tsububa-shi, Ibaraki, Japan	Physica C, 357-360(2001)318	A.T.Matveev,E.Takayama-Muromachi,K.Kimoto,M.Isobe,N.D.Zhigadlo,T.Drezen,T.Kawashima,Y.Matsui		
34028	PHC3570121	not s/c. In M-H curves, FC-ZFC branching at 150K is due to Ru-moment. FM or AF not clear	RuSr2PrCu2O8	Ru1Sr2Pr1Cu2O8-z	Ru	1	Sr	2	Pr	1	Cu	2													O	8-z		1	2001							150																					Ru1212	P4/mmm		A	3.8922		11.6355												K					5																																																																																																		See Physica C, 341-348(2000)457					Synthesis and magnetism of Pr-based rutheno-cuprate compound RuSr2PrCu2O8-z			Materials and Structures Lab, Tokyo Institute of Technology, Nagatsuta, Midori-ku, Yokohama, Japan	Physica C, 357-360(2001)121	H.Yamauchi,J.Nakamura,M.Karppinen,S.K.Malik,V.P.S.Awana,W.B.Yelon		
34029	PHC3570393	Li-intercalated layered Nb-oxide.	LixRbCa2Nb3O10	Li0.17Rb1Ca2Nb3O10	Li	0.17	Rb	1	Ca	2	Nb	3													O	10			2001																																														K					2																																																																																																		Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34030	PHC3570393	Li-intercalated layered Nb-oxide.	LixRbCa2Nb3O10	Li0.34Rb1Ca2Nb3O10	Li	0.34	Rb	1	Ca	2	Nb	3													O	10			2001																															A	7.721														K				3.5			3.5																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34031	PHC3570393	Li-intercalated layered Nb-oxide.	LixRbCa2Nb3O10	Li0.46Rb1Ca2Nb3O10	Li	0.46	Rb	1	Ca	2	Nb	3													O	10			2001																																														K				3.51			3.51																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34032	PHC3570393	Li-intercalated layered Nb-oxide.	LixRbCa2Nb3O10	Li0.62Rb1Ca2Nb3O10	Li	0.62	Rb	1	Ca	2	Nb	3													O	10			2001																																														K				2.7			2.7																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34033	PHC3570393	Li-intercalated layered Nb-oxide.	LixCsCa2Nb3O10	Li0.17Cs1Ca2Nb3O10	Li	0.17	Cs	1	Ca	2	Nb	3													O	10			2001																																														K					2																																																																																																		Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34034	PHC3570393	Li-intercalated layered Nb-oxide.	LixCsCa2Nb3O10	Li0.28Cs1Ca2Nb3O10	Li	0.28	Cs	1	Ca	2	Nb	3													O	10			2001																																														K				5.51			5.51																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34035	PHC3570393	Li-intercalated layered Nb-oxide.	LixCsCa2Nb3O10	Li0.34Cs1Ca2Nb3O10	Li	0.34	Cs	1	Ca	2	Nb	3													O	10			2001																															A	7.7477														K				5.4			5.4																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34036	PHC3570393	Li-intercalated layered Nb-oxide.	LixCsCa2Nb3O10	Li0.46Cs1Ca2Nb3O10	Li	0.46	Cs	1	Ca	2	Nb	3													O	10			2001																																														K				5.29			5.29																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34037	PHC3570393	Li-intercalated layered Nb-oxide.	LixCsCa2Nb3O10	Li0.62Cs1Ca2Nb3O10	Li	0.62	Cs	1	Ca	2	Nb	3													O	10			2001																																														K				4.71			4.71																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34038	PHC3570393	Li-intercalated layered Nb-oxide.	LixRbSr2Nb3O10	Li0.34Rb1Sr2Nb3O10	Li	0.34	Rb	1	Sr	2	Nb	3													O	10			2001																															A	7.7938														K				6.01			6.01																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34039	PHC3570393	Li-intercalated layered Nb-oxide.	LixKCa2Nb3O10	Li0.34K1Ca2Nb3O10	Li	0.34	K	1	Ca	2	Nb	3													O	10			2001																															A	7.7345														K				5.42			5.42																																																																																																Li-intercalation by electrochemical method using electrode  AB2Nb3O10/1.0M-LiClO4/PC/Pt.					Electrochemical intercalation of lithium in layered niobates AB2Nb3O10 (A=K,Rb,Cs; B=Ca, Sr) and their superconductivity			Materials and Structures Lab, Tokyo Institute of Technology,Nagatsuda, Midori-ku, Yokohama, Japan	Physica C, 357(2001)393	I.Nagai,M.Kakihana,M.Kato,Y.Abe,Y.Koike		
34040	PHC3570406	FM Curie-T from M measurements	RuSr2SmCu2O8	Ru1Sr2Sm1Cu2O8	Ru	1	Sr	2	Sm	1	Cu	2													O	8		1	2001							146																					Ru1212			A	3.8402		11.5701												K	12						12																																																																																																precursor(RuSr2(Sm or Eu)O6 + 2CuO, then mixture - SIN(1040,1045, 1050, 1055C, in flowing O2)					Ferromagnetism and superconductivity in RuSr2RCu2O8 (R = Sm, Eu, Gd)			Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki, Japan	Physica C, 357-360(2001)406	D.P.Hai,I.Kakeya,K.Kadowaki,M.Furuyama,S.Kamisawa,T.Mochiku		
34041	PHC3570406	FM Curie-T from M measurements	RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8		1	2001							139																					Ru1212			A	3.8394		11.5697												K	17						17																																																																																																precursor(RuSr2(Sm or Eu)O6 + 2CuO, then mixture - SIN(1040,1045, 1050, 1055C, in flowing O2)					Ferromagnetism and superconductivity in RuSr2RCu2O8 (R = Sm, Eu, Gd)			Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki, Japan	Physica C, 357-360(2001)406	D.P.Hai,I.Kakeya,K.Kadowaki,M.Furuyama,S.Kamisawa,T.Mochiku		
34042	PHC3570406	FM Curie-T from M measurements	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2001							136																					Ru1212			A	3.8376		11.5694												K	36						36																																																																																																precursor(RuSr2(Sm or Eu)O6 + 2CuO, then mixture - SIN(1040,1045, 1050, 1055C, in flowing O2)					Ferromagnetism and superconductivity in RuSr2RCu2O8 (R = Sm, Eu, Gd)			Institute of Materials Science, University of Tsukuba, Tsukuba, Ibaraki, Japan	Physica C, 357-360(2001)406	D.P.Hai,I.Kakeya,K.Kadowaki,M.Furuyama,S.Kamisawa,T.Mochiku		
34043	PHC3570414	composition by EDX. starting compo. = 0.45KO2 + 0.5BaO + 0.1BaO2 + 0.5Bi2O3.	(Ba,K)BiO3	Ba0.635K0.365Bi1O3	Ba	0.635	K	0.365	Bi	1															O	3		1	2001																												BKBO			A	4.2938														K				30.4			30.4																																																																																																high-T-high-P synthesis (900C, 1h, under 5 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34044	PHC3570414	composition by EDX. starting compo. = 0.52KO2 + 0.5BaO + 0.5Bi2O3	(Ba,K)BiO3	Ba0.557K0.443Bi1O3	Ba	0.557	K	0.443	Bi	1															O	3		1	2001																												BKBO			A	4.2734														K				25			25																																																																																																high-T-high-P synthesis (900C, 1h, under 5 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34045	PHC3570414	composition by EDX. starting compo. = 0.63KO2 + 0.4BaO + 0.5Bi2O3	(Ba,K)BiO3	Ba0.445K0.555Bi1O3	Ba	0.445	K	0.555	Bi	1															O	3		1	2001																												BKBO			A	4.248														K				17			17																																																																																																high-T-high-P synthesis (900C, 1h, under 5 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34046	PHC3570414	composition by EDX. starting compo. = 0.74KO2 + 0.3BaO + 0.5Bi2O3	(Ba,K)BiO3	Ba0.34K0.66Bi1O3	Ba	0.34	K	0.66	Bi	1															O	3		1	2001																												BKBO			A	4.2338														K				7			7																																																																																																high-T-high-P synthesis (900C, 1h, under 5 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34047	PHC3570414	composition by EDX. starting compo. = 0.84KO2 + 0.2BaO + 0.5Bi2O3	(Ba,K)BiO3	Ba0.241K0.759Bi1O3	Ba	0.241	K	0.759	Bi	1															O	3		1	2001																												BKBO			A	4.2149														K					3																																																																																																		high-T-high-P synthesis (1000C, under 7 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34048	PHC3570414	composition by EDX. starting compo. = 0.8KO2 + 0.15K + 0.1BaO + 0.5Bi2O3	(Ba,K)BiO3	Ba0.19K0.81Bi1O3	Ba	0.19	K	0.81	Bi	1															O	3		1	2001																												BKBO			A	4.2164														K				8.4			8.4																																																																																																high-T-high-P synthesis (1000C, under 7 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34049	PHC3570414	composition by EDX. starting compo. = 1.05KO2 + 0.5Bi2O3	KBiO3	K1Bi1O3	K	1	Bi	1																	O	3		1	2001																												ABO3			A	4.2224														K				9			9																																																																																																high-T-high-P synthesis (1000C, under 7 GPa)					Superconductivity in the Ba1-xKxBiO3 system			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 357-360(2001)414	A.N.Baranov,D.C.Kim,E.V.Antipov,H.R.Kang,J.S.Kim,J.S.Pshirkov,Y.W.Park		
34050	PR04002690	G-L parameter=51. Hc(0)=1.64 kOe.	(Ba,Rb)BiO3	Ba0.6Rb0.4Bi1O3	Ba	0.6	Rb	0.4	Bi	1															O	3		1	1989																												BKBO			A	4.3														K		29					29											Oe	M-H curve	90							T	M(T) curve at H and WHH theory	11.8							T/K		0.59					A	from Hc2(0)	53			A	calculated from Hc(0)	2700													mj/mol.K2	2.4	calculated from Hc(0)																																				BaCO3,Rb2CO3,Bi2O3	1	mixture - CAL(750C, 12h, in flowing N2) - ANN(400C, 1h, in O2)					Superconducting properties of the Ba1-xRbxBiO3 system			Advanced Research Lab, Toshiba Research and Development Center, Saiwai-ku, Kawasaki, Japan	Phys.Rev.B, 40(1989)2690	I.Tomeno,K.Ando		
34051	PHC3910049		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2003																												Ru1212			A	3.838		11.579												K	31		45				38																																																																																															1	final annealing (1062C,1w, in flowing O2)					Synthesis and superconductive characterisation of RuSr2NdxGd1-xCu2O8 compounds (x = 0, 0.09, 0.18, 0.35)			INFM and Dipartimento di Chimica e Chimica Industriale, University of Genova, Via Dodecaneso 31, Genova, Italy	Physica C, 391(2003)49	A.Hu,C.Artini,G.A.Costa,M.Murakami,N.Chikumoto,P.Mele,R.Masini		
34052	PHC3910049		RuSr2(Gd,Nd)Cu2O8	Ru1Sr2Gd0.91Nd0.09Cu2O8	Ru	1	Sr	2	Gd	0.91	Nd	0.09	Cu	2											O	8			2003																												Ru1212			A	3.838		11.579												K	11		36				23.5																																																																																															1	final annealing (1062C,1w, in flowing O2)					Synthesis and superconductive characterisation of RuSr2NdxGd1-xCu2O8 compounds (x = 0, 0.09, 0.18, 0.35)			INFM and Dipartimento di Chimica e Chimica Industriale, University of Genova, Via Dodecaneso 31, Genova, Italy	Physica C, 391(2003)49	A.Hu,C.Artini,G.A.Costa,M.Murakami,N.Chikumoto,P.Mele,R.Masini		
34053	PHC3910049	T1<5 K	RuSr2(Gd,Nd)Cu2O8	Ru1Sr2Gd0.82Nd0.18Cu2O8	Ru	1	Sr	2	Gd	0.82	Nd	0.18	Cu	2											O	8			2003																												Ru1212			A	3.844		11.572												K			21				21																																																																																															1	final annealing (1062C,1w, in flowing O2)					Synthesis and superconductive characterisation of RuSr2NdxGd1-xCu2O8 compounds (x = 0, 0.09, 0.18, 0.35)			INFM and Dipartimento di Chimica e Chimica Industriale, University of Genova, Via Dodecaneso 31, Genova, Italy	Physica C, 391(2003)49	A.Hu,C.Artini,G.A.Costa,M.Murakami,N.Chikumoto,P.Mele,R.Masini		
34054	PHC3910049	not s/c. semicond.	RuSr2(Gd,Nd)Cu2O8	Ru1Sr2Gd0.65Nd0.35Cu2O8	Ru	1	Sr	2	Gd	0.65	Nd	0.35	Cu	2											O	8			2003																												Ru1212			A	3.845		11.565												K					5																																																																																																	1	final annealing (1062C,1w, in flowing O2)					Synthesis and superconductive characterisation of RuSr2NdxGd1-xCu2O8 compounds (x = 0, 0.09, 0.18, 0.35)			INFM and Dipartimento di Chimica e Chimica Industriale, University of Genova, Via Dodecaneso 31, Genova, Italy	Physica C, 391(2003)49	A.Hu,C.Artini,G.A.Costa,M.Murakami,N.Chikumoto,P.Mele,R.Masini		
34055	PHC1690133	secondary phases are 214 or 1212. samples with various Ce-, Eu-contents were investigated.	(Pb,Cu)(Eu,Ce)2(Sr,Eu)2Cu2Oz	Pb0.5Eu1.75Sr1.75Ce0.5Cu2.5Oz	Pb	0.5	Eu	1.75	Sr	1.75	Ce	0.5	Cu	2.5											O	z			1990																												Pb1222																		K	10		25				17.5										15																																																																																						mixture-CAL(850C,10h, in air)-heat(1080C,1h, in air)-ANN(800C, 10h, in O2)-stepwise cool to RT					NEW SUPERCONDUCTING CUPRATES(PB,CU)(EU,CE)2(SR,EU)2CU2OZ			SUPERCONDUCTIVITY RESEARCH LABORATORY, INTERNATIONAL SUPERCONDUCTIVITY  TECHNOLOGY CENTER, 10-13, SHINONOME 1-CHOME, KOTOKU,TOKYO 135, JAPAN	PHYSICA C,169(1990)133	ATARU ICHINOSE,H.YAMAUCHI,KAZUHIRO SAKUYUMA,SHIN-ICHI KORIYAMA,SHOJI TANAKA,TOSHIHIKO MAEDA	PB,CU,EU,CE,SU,O	
34056	JAP0702234	nearly single phase	(Tl,Pb)Sr2(Eu,Ce)2Cu2O9	Tl0.5Pb0.5Sr2Eu1.8Ce0.2Cu2O9	Tl	0.5	Pb	0.5	Sr	2	Eu	1.8	Ce	0.2	Cu	2									O	9			1991																												1222			A	3.91		29.98												K			40				40																																																																																															1	precursor(Sr2Eu1.8Ce0.2Cu2Oz) + add(PbO, 10 wt% excess -Tl2O3) - ANN(6bar-O2)					High-pressure oxygen-induced bulk superconductivity in 1222 structure Tl-Pb-Sr-Eu(Ce)-Cu-O				J.Appl.Phys., 70(1991)2234	A.P.B.Sinha,B.L.Ramakrishna,D.E.Morris,G.J.Auchterlonie,J.C.Barry,Z.Iqbal		
34057	PHC1930073		(Pb,Cu)(Sr,Nd)2(Eu,Ce)2Cu2O9	Pb0.5Sr1.75Nd0.25Eu1.5Ce0.5Cu2.5O9	Pb	0.5	Sr	1.75	Nd	0.25	Eu	1.5	Ce	0.5	Cu	2.5									O	9		1	1992																												Pb1222																		K		32					32																																																																																																					STRUCTURAL PROPERTIES OF (PB,CU)(SR,ND)2(HO,CE)2CU2O9-Z	199204			PHYSICA C,193(1992)73	FUJIO IZUMI,H.YAMAUCHI,HAJIME ASANO,NAOMICHI SAKAI,SHOJI TANAKA,TAKAHIRO WADA,TOSHIHIKO MAEDA	PB,CU,SR,ND,HO,CE,O	
34058	JP00705975	Tc is sensitive to SIN condition. SIN in O2.	(Pb,Cd)(Sr,Eu)2(Eu,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Eu1.6Ce0.6Cu2O9	Pb	0.5	Cd	0.5	Sr	1.8	Eu	1.6	Ce	0.6	Cu	2									O	9		1	1995																												Pb1222			A	3.8314		29.3902												K	35		43				39																																																																																																mixture-CAL(900C, overnight, in air)-pellet-SIN(1050C, 8h, in air or O2)					Crystal structure and superconductivity of new Pb-based 1222 cuprate (Pb0.5Cd0.5)(Sr0.9Eu0.1)2(Eu0.7Ce0.3)2Cu2O9+z				J.Phys.:Condens.Matter, 7(1995)5975	C.Dong,C.Wang,Fei Wu,G.Rao,H.Chen,J.Liang,J.Min		
34059	JP00705975	Tc is sensitive to SIN condition. SIN in air.	(Pb,Cd)(Sr,Eu)2(Eu,Ce)2Cu2O9	Pb0.5Cd0.5Sr1.8Eu1.6Ce0.6Cu2O9	Pb	0.5	Cd	0.5	Sr	1.8	Eu	1.6	Ce	0.6	Cu	2									O	9		1	1995																												Pb1222			A	3.8443		29.3937												K	12		19				15.5																																																																																																mixture-CAL(900C, overnight, in air)-pellet-SIN(1050C, 8h, in air or O2)					Crystal structure and superconductivity of new Pb-based 1222 cuprate (Pb0.5Cd0.5)(Sr0.9Eu0.1)2(Eu0.7Ce0.3)2Cu2O9+z				J.Phys.:Condens.Matter, 7(1995)5975	C.Dong,C.Wang,Fei Wu,G.Rao,H.Chen,J.Liang,J.Min		
34060	PHC3900277	X-ray analysis=Pr(Sr0.65Ba0.31Pr0.04)2(Cu0.94Al0.06)3Oz. Al from Al2O3 crucible. mag.prop. for H//c-axis. For H//ab, Curie-T=11.2 K, KAIZERO = 0.00045 emu/mol, Meff = 3.37 uB/f.u.	Pr(Sr,Ba,Pr)2Cu3O7	Pr1.3Sr1.3Ba0.6Cu3O6.98	Pr	1.3	Sr	1.3	Ba	0.6	Cu	3													O	7	6.98	3	2003	emu/mol	0.002	emu.K/mol	1.19	uB/f.u	3.08	21.7																					Y123			A	3.908		11.401												K					4.2																																																																																																		self-flux method using Al2O3 crucible. ANN(400C, 1w, in O2-flw)					Magnetic properties of Pr1.1Sr1.3Ba0.6Cu3O7 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, China	Physica C, 390(2003)277	G.Cao,M.Fang,Z.Jiao,Z.Xu,Zili Wen		
34061	JJP0310L25		(Pb,Cu)(Sr,La)2(Gd,La)2Cu2Oz	Pb0.5Sr1.45Gd1.95La0.6Cu2.5Oz	Pb	0.5	Sr	1.45	Gd	1.95	La	0.6	Cu	2.5											O	z		1	1992																												Pb1222			A	3.845		29.091												K				20			20																																																																																														Sr2CuO3,PbO,La2O3,Ln2O3,CuO	1	mixture-pellet-heat(780C, 1h, in air)-SIN(900C, 16h, in air)-ANN(500C, 100h, in 100atm O2)					New Pb-based cuprates with 1222 structure having no tetravalent ions, (Pb0.5Cu0.5)Sr2-xLn2-yLax+yCu2Oz (Ln:Gd,Dy,Ho and Er)			University of Osaka Prefecture,Osaka,Japan	Jpn.J.Appl.Phys., 31(1992)L25	H.Sasakura,H.Teraoka,K.Nakahigashi,K.Yoshiara,S.Minamigawa		
34062	JJP0310L25	semiconductor-like	(Pb,Cu)(Sr,La)2(Dy,La)2Cu2Oz	Pb0.5Sr1.55Dy1.8La0.65Cu2.5Oz	Pb	0.5	Sr	1.55	Dy	1.8	La	0.65	Cu	2.5											O	z		1	1992																												Pb1222			A	3.815		29.089												K					4.2																																																																																																Sr2CuO3,PbO,La2O3,Ln2O3,CuO	1	mixture-pellet-heat(780C, 1h, in air)-SIN(900C, 16h, in air)-ANN(500C, 100h, in 100atm O2)					New Pb-based cuprates with 1222 structure having no tetravalent ions, (Pb0.5Cu0.5)Sr2-xLn2-yLax+yCu2Oz (Ln:Gd,Dy,Ho and Er)			University of Osaka Prefecture,Osaka,Japan	Jpn.J.Appl.Phys., 31(1992)L25	H.Sasakura,H.Teraoka,K.Nakahigashi,K.Yoshiara,S.Minamigawa		
34063	JJP0310L25	semiconductor-like	(Pb,Cu)(Sr,La)2(Ho,La)2Cu2Oz	Pb0.5Sr1.6Ho1.75La0.65Cu2.5Oz	Pb	0.5	Sr	1.6	Ho	1.75	La	0.65	Cu	2.5											O	z		1	1992																												Pb1222			A	3.81		29.07												K					4.2																																																																																																Sr2CuO3,PbO,La2O3,Ln2O3,CuO	1	mixture-pellet-heat(780C, 1h, in air)-SIN(900C, 16h, in air)-ANN(500C, 100h, in 100atm O2)					New Pb-based cuprates with 1222 structure having no tetravalent ions, (Pb0.5Cu0.5)Sr2-xLn2-yLax+yCu2Oz (Ln:Gd,Dy,Ho and Er)			University of Osaka Prefecture,Osaka,Japan	Jpn.J.Appl.Phys., 31(1992)L25	H.Sasakura,H.Teraoka,K.Nakahigashi,K.Yoshiara,S.Minamigawa		
34064	JJP0310L25	semiconductor-like	(Pb,Cu)(Sr,La)2(Er,La)2Cu2Oz	Pb0.5Sr1.65Er1.75La0.6Cu2.5Oz	Pb	0.5	Sr	1.65	Er	1.75	La	0.6	Cu	2.5											O	z		1	1992																												Pb1222			A	3.804		29.013												K					4.2																																																																																																Sr2CuO3,PbO,La2O3,Ln2O3,CuO	1	mixture-pellet-heat(780C, 1h, in air)-SIN(900C, 16h, in air)-ANN(500C, 100h, in 100atm O2)					New Pb-based cuprates with 1222 structure having no tetravalent ions, (Pb0.5Cu0.5)Sr2-xLn2-yLax+yCu2Oz (Ln:Gd,Dy,Ho and Er)			University of Osaka Prefecture,Osaka,Japan	Jpn.J.Appl.Phys., 31(1992)L25	H.Sasakura,H.Teraoka,K.Nakahigashi,K.Yoshiara,S.Minamigawa		
34065	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.52Nd0.4Sr0.08Cu1O4	La	1.52	Nd	0.4	Sr	0.08	Cu	1													O	4			2000																												T																		K		9.34					9.34																																																																		uV/K	73.2			TP34065																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34066	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.5Nd0.4Sr0.1Cu1O4	La	1.5	Nd	0.4	Sr	0.1	Cu	1													O	4			2000																												T																		K		9.1					9.1																																																																		uV/K	49			TP34066																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34067	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4			2000																												T																		K		6.06					6.06																																																																		uV/K	32			TP34067																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34068	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4			2000																												T																		K		13.6					13.6																																																																		uV/K	24.2			TP34068																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34069	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.42Nd0.4Sr0.18Cu1O4	La	1.42	Nd	0.4	Sr	0.18	Cu	1													O	4			2000																												T																		K		17.2					17.2																																																																		uV/K	9.18			TP34069																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34070	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.4Nd0.4Sr0.2Cu1O4	La	1.4	Nd	0.4	Sr	0.2	Cu	1													O	4			2000																												T																		K		17.7					17.7																																																																		uV/K	4.88			TP34070																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34071	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd,Sr)2CuO4	La1.35Nd0.4Sr0.25Cu1O4	La	1.35	Nd	0.4	Sr	0.25	Cu	1													O	4			2000																												T																		K		8.33					8.33																																																																		uV/K	-1.37			TP34071																									1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34072	JPS0692917	sp-heat was measured. gamma not shown explicitly.	(La,Nd)2CuO4	La1.6Nd0.4Cu1O4	La	1.6	Nd	0.4	Cu	1															O	4			2000								250																				T																		K																																																																																																						1	mixture-pellet-SIN(1080C, 2d, in air)-FC to RT					Electronic specific heat of La2-x-zNdzSrxCu1-yZnyO4 up to room temperature			Department of Physics, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 69(2000)2917	J.Takeda,M.Sato,T.Inukai		
34073	PHC3910160	not s/c. 	(Hg,V)Sr2(Nd,Sr)Cu2O6+z	Hg0.65V0.35Sr2.3Nd0.7Cu2O6+z	Hg	0.65	V	0.35	Sr	2.3	Nd	0.7	Cu	2											O	6+z		1	2003																												Hg1212			A	3.8779		11.916												K					4.2																																																																																																HgO,V2O5,SrCuO2,Nd2O3,SrO2	1	pellet wrapped in Au-foil, sealed in quartz tube, heat(880C, 16h) - Q to RT					Synthesis, structure and superconducting properties of the (Hg0.65V0.35)Sr2(Nd1-ySry)Cu2O6+z system			Department of Engineering Materials, The University of She?eld,  She?eld, South Yorkshire, UK	Physica C, 391(2003)160	I.Gameson,K.L.Moran,N.C.Hyatt,R.Dupree		
34074	PHC3910160	detailed structure analysis using X-ray, NMR, NED.	(Hg,V)Sr2(Nd,Sr)Cu2O6+z	Hg0.65V0.35Sr2.4Nd0.6Cu2O6+z	Hg	0.65	V	0.35	Sr	2.4	Nd	0.6	Cu	2											O	6+z		1	2003																												Hg1212			A	3.877		11.924												K				67			67																																																																																														HgO,V2O5,SrCuO2,Nd2O3,SrO2	1	pellet wrapped in Au-foil, sealed in quartz tube, heat(880C, 16h) - Q to RT					Synthesis, structure and superconducting properties of the (Hg0.65V0.35)Sr2(Nd1-ySry)Cu2O6+z system			Department of Engineering Materials, The University of She?eld,  She?eld, South Yorkshire, UK	Physica C, 391(2003)160	I.Gameson,K.L.Moran,N.C.Hyatt,R.Dupree		
34075	PHC3910160		(Hg,V)Sr2(Nd,Sr)Cu2O6+z	Hg0.65V0.35Sr2.5Nd0.5Cu2O6+z	Hg	0.65	V	0.35	Sr	2.5	Nd	0.5	Cu	2											O	6+z		1	2003																												Hg1212			A	3.8764		11.93												K				82			82																																																																																														HgO,V2O5,SrCuO2,Nd2O3,SrO2	1	pellet wrapped in Au-foil, sealed in quartz tube, heat(880C, 16h) - Q to RT					Synthesis, structure and superconducting properties of the (Hg0.65V0.35)Sr2(Nd1-ySry)Cu2O6+z system			Department of Engineering Materials, The University of She?eld,  She?eld, South Yorkshire, UK	Physica C, 391(2003)160	I.Gameson,K.L.Moran,N.C.Hyatt,R.Dupree		
34076	PHC3910160	ANN(300C, 24h, in flowing O2)	(Hg,V)Sr2(Nd,Sr)Cu2O6+z	Hg0.6V0.4Sr2.47Nd0.53Cu2O6+z	Hg	0.6	V	0.4	Sr	2.47	Nd	0.53	Cu	2											O	6+z		1	2003																												Hg1212			A	3.8765		11.9232												K				67			67																																																																																														HgO,V2O5,SrCuO2,Nd2O3,SrO2	1	pellet wrapped in Au-foil, sealed in quartz tube, heat(880C, 16h) - Q to RT					Synthesis, structure and superconducting properties of the (Hg0.65V0.35)Sr2(Nd1-ySry)Cu2O6+z system			Department of Engineering Materials, The University of She?eld,  She?eld, South Yorkshire, UK	Physica C, 391(2003)160	I.Gameson,K.L.Moran,N.C.Hyatt,R.Dupree		
34077	PHC3910237	X-ray DENS=10.4119. hole=0.3. Jc(5K,0.6T)=1.2 E+6 A/cm2.	(La,Nd)2CaBa2Cu5Oz	La1.5Nd0.5Ca1Ba2Cu5O11.583	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	5											O	z	11.583		2003																												2125			A	3.8677		11.5998												K	78	79	80	77			79																																																																																															1	mixture-CAL(930C, 50h)-SIN(940-950C, 24h)-ANN(900C, 12h, in flowing N2)-ANN(900C, 12h, in flowing O2)-slow cool to 500C - ANN(500C, 24h, in O2)-slow cool to RT					Effect of Mo-substitution on superconductivity, flux pinning and critical currents of La1.5Nd0.5Ca1Ba2Cu5Oz			Department of Physics, Saurashtra University, Rajkot, India	Physica C, 391(2003)237	C.M.Thaker,D.C.Kundaliya,D.G.Kuberkar,D.S.Rana,K.Mavani,R.G.Kulkarni,S.K.Malik,S.Rayaprol		
34078	PHC3910237	X-ray DENS=10.4856. hole=0.205. Jc(5K,0.6T)=2.25 E+6 A/cm2.	(La,Nd)2CaBa2(Cu,Mo)5Oz	La1.5Nd0.5Ca1Ba2Cu4.95Mo0.05O11.345	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	4.95	Mo	0.05									O	z	11.345		2003																												2125			A	3.8727		11.5998												K	74	76	80	75			76																																																																																															1	mixture-CAL(930C, 50h)-SIN(940-950C, 24h)-ANN(900C, 12h, in flowing N2)-ANN(900C, 12h, in flowing O2)-slow cool to 500C - ANN(500C, 24h, in O2)-slow cool to RT					Effect of Mo-substitution on superconductivity, flux pinning and critical currents of La1.5Nd0.5Ca1Ba2Cu5Oz			Department of Physics, Saurashtra University, Rajkot, India	Physica C, 391(2003)237	C.M.Thaker,D.C.Kundaliya,D.G.Kuberkar,D.S.Rana,K.Mavani,R.G.Kulkarni,S.K.Malik,S.Rayaprol		
34079	PHC3910237	X-ray DENS=10.4798. hole=0.195. Jc(5K,0.6T)=1.5 E+6 A/cm2.	(La,Nd)2CaBa2(Cu,Mo)5Oz	La1.5Nd0.5Ca1Ba2Cu4.85Mo0.15O11.322	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	4.85	Mo	0.15									O	z	11.322		2003																												2125			A	3.8739		11.5992												K	66	70	78	68			70																																																																																															1	mixture-CAL(930C, 50h)-SIN(940-950C, 24h)-ANN(900C, 12h, in flowing N2)-ANN(900C, 12h, in flowing O2)-slow cool to 500C - ANN(500C, 24h, in O2)-slow cool to RT					Effect of Mo-substitution on superconductivity, flux pinning and critical currents of La1.5Nd0.5Ca1Ba2Cu5Oz			Department of Physics, Saurashtra University, Rajkot, India	Physica C, 391(2003)237	C.M.Thaker,D.C.Kundaliya,D.G.Kuberkar,D.S.Rana,K.Mavani,R.G.Kulkarni,S.K.Malik,S.Rayaprol		
34080	PHC3910237	X-ray DENS=10.6056. hole=0.124. Jc(5K,0.6T)=0.25 E+6 A/cm2.	(La,Nd)2CaBa2(Cu,Mo)5Oz	La1.5Nd0.5Ca1Ba2Cu4.75Mo0.25O11.143	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	4.75	Mo	0.25									O	z	11.143		2003																												2125			A	3.8664		11.5704												K	64	70	75	65			70																																																																																															1	mixture-CAL(930C, 50h)-SIN(940-950C, 24h)-ANN(900C, 12h, in flowing N2)-ANN(900C, 12h, in flowing O2)-slow cool to 500C - ANN(500C, 24h, in O2)-slow cool to RT					Effect of Mo-substitution on superconductivity, flux pinning and critical currents of La1.5Nd0.5Ca1Ba2Cu5Oz			Department of Physics, Saurashtra University, Rajkot, India	Physica C, 391(2003)237	C.M.Thaker,D.C.Kundaliya,D.G.Kuberkar,D.S.Rana,K.Mavani,R.G.Kulkarni,S.K.Malik,S.Rayaprol		
34081	PHC3910237	X-ray DENS=11.0157. hole=0.114. 	(La,Nd)2CaBa2(Cu,Mo)5Oz	La1.5Nd0.5Ca1Ba2Cu4.5Mo0.5O11.119	La	1.5	Nd	0.5	Ca	1	Ba	2	Cu	4.5	Mo	0.5									O	z	11.119		2003																												2125			A	3.8123		11.6142												K	39	50	60	48			50																																																																																															1	mixture-CAL(930C, 50h)-SIN(940-950C, 24h)-ANN(900C, 12h, in flowing N2)-ANN(900C, 12h, in flowing O2)-slow cool to 500C - ANN(500C, 24h, in O2)-slow cool to RT					Effect of Mo-substitution on superconductivity, flux pinning and critical currents of La1.5Nd0.5Ca1Ba2Cu5Oz			Department of Physics, Saurashtra University, Rajkot, India	Physica C, 391(2003)237	C.M.Thaker,D.C.Kundaliya,D.G.Kuberkar,D.S.Rana,K.Mavani,R.G.Kulkarni,S.K.Malik,S.Rayaprol		
34082	PHC3910298	Hg0.92Ba1.93Ca1.07Cu2.07Oz by SEM	HgBa2CaCu2O6	Hg1Ba2Ca1Cu2O6+z	Hg	1	Ba	2	Ca	1	Cu	2													O	6+z		1	2003																												Hg1212				3.8627		12.709												K				121			121											mT		7.7							T		100																																																																									1	ANN(880C, 10h, in sealed silica tube)					Irreversibility fields of the high-Tc superconductors Hg-1212 and (Hg,Tl)-1212			Department of Physics, Free University Berlin,  Berlin, Germany	Physica C, 391(2003)298	A.Abakumov,D.A.Pavlov,E.V.Antipov,I.Bryntse,K.Luders,M.Baenitz,P.Schilbe		
34083	PHC3910298	Hg0.74Tl0.20Ba1.95Ca1.04Cu2.05Oz by SEM	(Hg,Tl)Ba2CaCu2O6	Hg0.8Tl0.2Ba2Ca1Cu2O6+z	Hg	0.8	Tl	0.2	Ba	2	Ca	1	Cu	2											O	6+z		1	2003																												Hg1212				3.8592		12.67												K				124			124											mT		9.9							T		100																																																																									1	ANN(880C, 10h, in sealed silica tube)					Irreversibility fields of the high-Tc superconductors Hg-1212 and (Hg,Tl)-1212			Department of Physics, Free University Berlin,  Berlin, Germany	Physica C, 391(2003)298	A.Abakumov,D.A.Pavlov,E.V.Antipov,I.Bryntse,K.Luders,M.Baenitz,P.Schilbe		
34084	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.025	La	1.8	Nd	0.2	Cu	1															O	4+z	4.025	1	2003																												T																		K		15.9					15.9																																																																		uV/K	73.5			TP34084																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34085	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.04	La	1.8	Nd	0.2	Cu	1															O	4+z	4.04	1	2003																												T																		K		26.3					26.3																																																																		uV/K	53.8			TP34085																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34086	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.059	La	1.8	Nd	0.2	Cu	1															O	4+z	4.059	1	2003																												T																		K		26.7					26.7																																																																		uV/K	39.4			TP34086																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34087	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.07	La	1.8	Nd	0.2	Cu	1															O	4+z	4.07	1	2003																												T																		K		35.3					35.3																																																																		uV/K	32.5			TP34087																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34088	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.071	La	1.8	Nd	0.2	Cu	1															O	4+z	4.071	1	2003																												T																		K		34.8					34.8																																																																		uV/K	24.5			TP34088																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34089	LOW1210837	O-content by Faraday's law. TP300 at 290 K.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.086	La	1.8	Nd	0.2	Cu	1															O	4+z	4.086	1	2003																												T																		K		35.9					35.9																																																																		uV/K	18.1			TP34089																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34090	LOW1210837	O-content by Faraday's law. TP300 at 290 K. Tc not shown in Fig.	(La,Nd)2CuO4+z	La1.8Nd0.2Cu1O4.093	La	1.8	Nd	0.2	Cu	1															O	4+z	4.093	1	2003																												T																		K		25.6					25.6																																																																		uV/K	8.84			TP34090																									1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34091	LOW1210837		(La,Nd)2(Cu,Zn)O4	La1.8Nd0.2Cu0.99Zn0.01O4.086	La	1.8	Nd	0.2	Cu	0.99	Zn	0.01													O	4+z	4.086	1	2003																												T																		K		35.6					35.6	TC34091																																																																																														1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34092	LOW1210837		(La,Bi)2CuO4	La1.95Bi0.05Cu1O4.075	La	1.95	Bi	0.05	Cu	1															O	4+z	4.075	1	2003																												T																		K		25.7					25.7	TC34092																																																																																														1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34093	LOW1210837		(La,Bi)2(Cu,Zn)O4	La1.95Bi0.05Cu0.99Zn0.01O4.093	La	1.95	Bi	0.05	Cu	0.99	Zn	0.01													O	4+z	4.093	1	2003																												T																		K		22.7					22.7	TC34093																																																																																														1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34094	LOW1210837		(La,Pr)2CuO4	La1.8Pr0.2Cu1O4.11	La	1.8	Pr	0.2	Cu	1															O	4+z	4.11	1	2003																												T																		K								TC34094																																																																																														1	excess oxygen doping by electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34095	P065224520	TP300=282K value. <63>Cu NMR measured.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2002																												IL																		K		43					43																																																																		uV/K	-1.88			TP34095																										high pressure synthesis					Gap anisotropy, spin fluctuations, and normal-state properties of the electron-doped superconductor Sr0.9La0.1CuO2			Physikalisches Institut, Universitat Stuttgart, D-70550 Stuttgart, Germany	Phys.Rev.B, 65(2002)224520	A.Howes,C.U.Jung,G.V.M.Williams,H.J.Trodahl,Min-Seok Park,R.Dupree,S.Kramer,Sung-Ik Lee		
34096	P068054512		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2003																											2	T																		K			37				37																																																																																																See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34097	P068054512		(La,Sr)2(Cu,Mn)O4	La1.81Sr0.19Cu0.98Mn0.02O4	La	1.81	Sr	0.19	Cu	0.98	Mn	0.02													O	4		1	2003																											2	T																		K			37				37																																																																																																See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34098	P068054512		(La,Sr)2(Cu,Mn)O4	La1.77Sr0.23Cu0.96Mn0.04O4	La	1.77	Sr	0.23	Cu	0.96	Mn	0.04													O	4		1	2003																											2	T																		K			37				37																																																																																																See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34099	P068054512	R is not zero at 10 K.	(La,Sr)2(Cu,Mn)O4	La1.73Sr0.27Cu0.94Mn0.06O4	La	1.73	Sr	0.27	Cu	0.94	Mn	0.06													O	4		1	2003																											2	T																		K			37				37																																																																																																See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34100	P068054512	Neel-T defined as peak temperature in sus(T). not s/c	(La,Sr)2(Cu,Mn)O4	La1.65Sr0.35Cu0.9Mn0.1O4	La	1.65	Sr	0.35	Cu	0.9	Mn	0.1													O	4		1	2003								9.2																			2	T																		K					4.2																																																																																																		See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34101	P068054512	Neel-T defined as peak temperature in sus(T). not s/c	(La,Sr)2(Cu,Mn)O4	La1.45Sr0.55Cu0.8Mn0.2O4	La	1.45	Sr	0.55	Cu	0.8	Mn	0.2													O	4		1	2003								8.6																			2	T																		K					4.2																																																																																																		See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34102	P068054512	Neel-T defined as peak temperature in sus(T). not s/c	(La,Sr)2(Cu,Mn)O4	La1.25Sr0.75Cu0.7Mn0.3O4	La	1.25	Sr	0.75	Cu	0.7	Mn	0.3													O	4		1	2003								7.7																			2	T																		K					4.2																																																																																																		See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34103	P068054512	Neel-T defined as peak temperature in sus(T). not s/c	(La,Sr)2(Cu,Mn)O4	La1.21Sr0.79Cu0.68Mn0.32O4	La	1.21	Sr	0.79	Cu	0.68	Mn	0.32													O	4		1	2003								7.3																			2	T																		K					4.2																																																																																																		See Physica C, 340(2000)168					Magnetic states in La1.85-2xSr0.15+2xCu1-xMnxO4 (0=<x=<0.5)			Structure Research Laboratory, University of Science and Technology of China, National High Magnetic Field Laboratory, Hefei,  China	Phys.Rev.B, 68(2003)54512	C.Zhang,Y.Zhang		
34104	SST0160931	impurity phase=Tl-1212	(Tl,Pb)(Sr,Ba)2Ca2Cu3Oz	Tl0.54Pb0.5Sr1.7Ba0.3Ca2Cu3Oz	Tl	0.54	Pb	0.5	Sr	1.7	Ba	0.3	Ca	2	Cu	3									O	z			2003																												Tl1223																		K		120.6					120.6																																																																																																precursor(Ba-Sr-Ca-Cu-O) + (Tl2O3,PbO,TeO2) - mixture - press to disc - SIN(922C, 12m) - heat(910C,10h, in O2 flow) - ANN(790C,50h,in O2 flow)					Stabilizing the Tl-1223 phase by doping with tellurium			Institut fur Chemische Technologie Anorganischer Stoffe, Johannes Kepler Universitat, A4040 Linz, Austria	Supercond.Sci.Technol., 16(2003)931	Christian Deinhofer,Gerhard Gritzner		
34105	SST0160931		(Tl,Pb,Te)(Sr,Ba)2Ca2Cu3Oz	Tl0.54Pb0.49Te0.01Sr1.7Ba0.3Ca2Cu3Oz	Tl	0.54	Pb	0.49	Te	0.01	Sr	1.7	Ba	0.3	Ca	2	Cu	3							O	z		1	2003																												Tl1223																		K		120.6					120.6																																																																																																precursor(Ba-Sr-Ca-Cu-O) + (Tl2O3,PbO,TeO2) - mixture - press to disc - SIN(922C, 12m) - heat(910C,10h, in O2 flow) - ANN(790C,50h,in O2 flow)					Stabilizing the Tl-1223 phase by doping with tellurium			Institut fur Chemische Technologie Anorganischer Stoffe, Johannes Kepler Universitat, A4040 Linz, Austria	Supercond.Sci.Technol., 16(2003)931	Christian Deinhofer,Gerhard Gritzner		
34106	SST0160931		(Tl,Pb,Te)(Sr,Ba)2Ca2Cu3Oz	Tl0.54Pb0.45Te0.05Sr1.7Ba0.3Ca2Cu3Oz	Tl	0.54	Pb	0.45	Te	0.05	Sr	1.7	Ba	0.3	Ca	2	Cu	3							O	z		1	2003																												Tl1223																		K		120.2					120.2																																																																																																precursor(Ba-Sr-Ca-Cu-O) + (Tl2O3,PbO,TeO2) - mixture - press to disc - SIN(922C, 12m) - heat(910C,10h, in O2 flow) - ANN(790C,50h,in O2 flow)					Stabilizing the Tl-1223 phase by doping with tellurium			Institut fur Chemische Technologie Anorganischer Stoffe, Johannes Kepler Universitat, A4040 Linz, Austria	Supercond.Sci.Technol., 16(2003)931	Christian Deinhofer,Gerhard Gritzner		
34107	SST0160931	impurity phase=Ba2CuTeO6	(Tl,Pb,Te)(Sr,Ba)2Ca2Cu3Oz	Tl0.54Pb0.4Te0.1Sr1.7Ba0.3Ca2Cu3Oz	Tl	0.54	Pb	0.4	Te	0.1	Sr	1.7	Ba	0.3	Ca	2	Cu	3							O	z			2003																												Tl1223																		K		119					119																																																																																																precursor(Ba-Sr-Ca-Cu-O) + (Tl2O3,PbO,TeO2) - mixture - press to disc - SIN(922C, 12m) - heat(910C,10h, in O2 flow) - ANN(790C,50h,in O2 flow)					Stabilizing the Tl-1223 phase by doping with tellurium			Institut fur Chemische Technologie Anorganischer Stoffe, Johannes Kepler Universitat, A4040 Linz, Austria	Supercond.Sci.Technol., 16(2003)931	Christian Deinhofer,Gerhard Gritzner		
34108	PRL0770727	overdoped sample.  gap measured by Raman spectroscopy	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1996																												Bi2212																		K				57			57																																																5.2	4																																															self-flux method					Superconducting Gap Anisotropy vs Doping Level in High-Tc Cuprates			Code 6650, Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.Lett.77(1996)727	C. Kendziora,M. Onellion,R.J. Kelley		
34109	PRL0800149	overdoped. oxygen content not measured.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1998																												Bi2212																		K		56					56																																														meV	42	8.72	1																																															over- and under-doped samples were obtained by annealing in vac or high-pressure O2.					Pseudogap Precursor of the Superconducting Gap in Under-and Overdoped Bi2Sr2CaCu2O8+delta	1		DPMC, Universite' de Gene've, 24, Quai Ernest-Ansermet, 1211 Gene've 4, Swizerland	Phys.Rev.Lett.,80(1998)149-152	B. Revaz,B.Revaz,Ch. Renner,Ch.Renner,F.Fischer,J.-Y. Genoud,J.-Y.Genoud,K. Kadowaki,K.Kadowaki,O. Fischer		
34110	PRL0800149	overdoped. oxygen content not measured.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1998																												Bi2212																		K		74.3					74.3																																														meV	68	10.6	1																																															over- and under-doped samples were obtained by annealing in vac or high-pressure O2.					Pseudogap Precursor of the Superconducting Gap in Under-and Overdoped Bi2Sr2CaCu2O8+delta	1		DPMC, Universite' de Gene've, 24, Quai Ernest-Ansermet, 1211 Gene've 4, Swizerland	Phys.Rev.Lett.,80(1998)149-152	B. Revaz,B.Revaz,Ch. Renner,Ch.Renner,F.Fischer,J.-Y. Genoud,J.-Y.Genoud,K. Kadowaki,K.Kadowaki,O. Fischer		
34111	PRL0800149	optimal. oxygen content not measured.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1998																												Bi2212																		K		92.2					92.2																																														meV	83	10.5	1																																															over- and under-doped samples were obtained by annealing in vac or high-pressure O2.					Pseudogap Precursor of the Superconducting Gap in Under-and Overdoped Bi2Sr2CaCu2O8+delta	1		DPMC, Universite' de Gene've, 24, Quai Ernest-Ansermet, 1211 Gene've 4, Swizerland	Phys.Rev.Lett.,80(1998)149-152	B. Revaz,B.Revaz,Ch. Renner,Ch.Renner,F.Fischer,J.-Y. Genoud,J.-Y.Genoud,K. Kadowaki,K.Kadowaki,O. Fischer		
34112	PRL0800149	underdoped. oxygen content not measured.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1998																												Bi2212																		K		83					83																																														meV	88	12.3	1																																															over- and under-doped samples were obtained by annealing in vac or high-pressure O2.					Pseudogap Precursor of the Superconducting Gap in Under-and Overdoped Bi2Sr2CaCu2O8+delta	1		DPMC, Universite' de Gene've, 24, Quai Ernest-Ansermet, 1211 Gene've 4, Swizerland	Phys.Rev.Lett.,80(1998)149-152	B. Revaz,B.Revaz,Ch. Renner,Ch.Renner,F.Fischer,J.-Y. Genoud,J.-Y.Genoud,K. Kadowaki,K.Kadowaki,O. Fischer		
34113	P068064510		(Pr,Am)2CuO4	Pr1.85Am0.15Cu1O4	Pr	1.85	Am	0.15	Cu	1															O	4		1	2003					per f.u	4.7	81																					T'			A	3.9607		12.1676												K					5																																																																																																Am2(C2O4)3,Pr6O11,CuO	1	mixture-heat(900C, in air)-SIN(1100C, in air)-SIN(900c, 15h, in N2)					Incorporation of Am into the superconductor-related phase Pr2CuO4			Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 68(2003)64510	C.W.Williams,L.Soderholm,S.Skanthakumar		
34114	P068064510		Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4		1	2003																												T'			A	3.9602		12.2189												K					5																																																																																																Am2(C2O4)3,Pr6O11,CuO	1	mixture-heat(900C, in air)-SIN(1100C, in air)-SIN(900c, 15h, in N2)					Incorporation of Am into the superconductor-related phase Pr2CuO4			Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 68(2003)64510	C.W.Williams,L.Soderholm,S.Skanthakumar		
34115	PHC1790440		(Cm,Th)2CuO4	Cm1.85Th0.15Cu1O4	Cm	1.85	Th	0.15	Cu	1															O	4			1991																												T'			A	3.952		12.13												K																																																																																																												THE SUPERCONDUCTOR-RELATED OXIDES CM2CUO4 AND CM1.83TH0.17CUO4			ARGONNE NATIONAL LABORATORY,ARGONNE,IL 60439,USA	PHYSICA C,179(1991)440	C.W.WILLIAMS,L.SODERHOLM,U.WELP	CM,TH,CU,O	
34116	PR06004302	magnetic structure shown in figure.	Cm2CuO4	Cm2Cu1O4	Cm	2	Cu	1																	O	4			1999					per f.u	7.89		25																				T'			A	3.9305		12.112												K																																																																																																												Structure and magnetic properties of the high-Tc related phase Cm2CuO4			Chemistry Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 60(1999)4302	C.W.Williams,L.Soderholm,S.Skanthakumar		
34117	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.04 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.99La0.01Ba2Cu3O7.07	Y	0.99	La	0.01	Ba	2	Cu	3													O	z	7.07		2003																												Y123			A	3.8218	3.8875	11.677												K				91		30	91										81																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34118	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.092 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.9La0.1Ba2Cu3O6.97	Y	0.9	La	0.1	Ba	2	Cu	3													O	z	6.97		2003																												Y123			A	3.8239	3.8866	11.676												K				91		36	91										83																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34119	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.182 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.8La0.2Ba2Cu3O6.9	Y	0.8	La	0.2	Ba	2	Cu	3													O	z	6.9		2003																												Y123			A	3.8301	3.8874	11.685												K				84		44	84										71																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34120	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.282 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.7La0.3Ba2Cu3O6.92	Y	0.7	La	0.3	Ba	2	Cu	3													O	z	6.92		2003																												Y123			A	3.8385	3.8927	11.702												K				83		43	83										54																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34121	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.385 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.6La0.4Ba2Cu3O6.92	Y	0.6	La	0.4	Ba	2	Cu	3													O	z	6.92		2003																												Y123			A	3.8502	3.9034	11.732												K				85		52	85										49																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34122	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.472 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.5La0.5Ba2Cu3O7.01	Y	0.5	La	0.5	Ba	2	Cu	3													O	z	7.01		2003																												Y123			A	3.843	3.8992	11.717												K				86		45	86										56																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34123	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.617 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.4La0.6Ba2Cu3O6.99	Y	0.4	La	0.6	Ba	2	Cu	3													O	z	6.99		2003																												Y123			A	3.8561	3.9095	11.749												K				85		50	85										48																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34124	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.727 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.3La0.7Ba2Cu3O6.98	Y	0.3	La	0.7	Ba	2	Cu	3													O	z	6.98		2003																												Y123			A	3.8666	3.9165	11.778												K				82		50	82										49																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34125	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.827 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.2La0.8Ba2Cu3O7	Y	0.2	La	0.8	Ba	2	Cu	3													O	z	7		2003																												Y123			A	3.8694	3.9167	11.777												K				81		51	81										60																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34126	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.938 (in meas.)	(Y,La)Ba2Cu3Oz	Y0.1La0.9Ba2Cu3O7.05	Y	0.1	La	0.9	Ba	2	Cu	3													O	z	7.05		2003																												Y123			A	3.8822	3.9269	11.805												K				79		52	79										40																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34127	P068064502	impurity phase BaCuO2 < 8%. TCWIDTH(10-90% in sus). La-conc.=0.883 (in meas.)	LaBa2Cu3Oz	La1Ba2Cu3O6.95	La	1	Ba	2	Cu	3															O	z	6.95		2003																												Y123			A	3.8911	3.933	11.808												K				74		52	74										44																																																																																						mixture - CAL(920C,20h, in O2) - SIN(950C,30h, in He) - ANN(500C,15h, in O2 flow)					Phase formation and lattice strain in superconducting compound Y1-xLaxBa2Cu3Oy (0=<x=<1)			Solid State Physics Department, School of Physics, University of Athens, GR-15784 Athens, Greece	Phys.Rev.B, 68(2003)64502	A.Gantis,D.Lampakis,D.Palles,E.Liarokapis,M.Calamiotou		
34128	P068064507	paramag down to 5K. KAIZERO in emu/mol.Oe.	MoSr2(Pr,Ce)2Cu2O10	Mo1Sr2Pr1.5Ce1Cu2O10	Mo	1	Sr	2	Pr	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0011			per R-ion	2.85	-14.1																					Ru1222			A	3.861		28.38												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34129	P068064507	paramag down to 5K. KAIZERO in emu/mol.Oe.	MoSr2(Nd,Ce)2Cu2O10	Mo1Sr2Nd1.5Ce1Cu2O10	Mo	1	Sr	2	Nd	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0045			per R-ion	2.31	-2.1																					Ru1222			A	3.86		28.52												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34130	P068064507		MoSr2(Sm,Ce)2Cu2O10	Mo1Sr2Sm1.5Ce1Cu2O10	Mo	1	Sr	2	Sm	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0019			per R-ion	0.8	-12.4																					Ru1222			A	3.848		28.43												K				18			18																																																																																														R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34131	P068064507	sus(T) not Curie-Weis like. KAIZERO in emu/mol.Oe.	MoSr2(Eu,Ce)2Cu2O10	Mo1Sr2Eu1.5Ce1Cu2O10	Mo	1	Sr	2	Eu	1.5	Ce	1	Cu	2											O	10		1	2003																												Ru1222			A	3.838		28.41												K				23			23																																																																																														R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34132	P068064507	Two mag. transitions at 15 K and 184 K. KAIZERO in emu/mol.Oe.	MoSr2(Gd,Ce)2Cu2O10	Mo1Sr2Gd1.5Ce1Cu2O10	Mo	1	Sr	2	Gd	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.003			per R-ion	7.16	14.7																					Ru1222			A	3.833		28.43												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34133	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Tb,Ce)2Cu2O10	Mo1Sr2Tb1.5Ce1Cu2O10	Mo	1	Sr	2	Tb	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.003			per R-ion	8.7	-8.5																					Ru1222			A	3.818		28.33												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34134	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Dy,Ce)2Cu2O10	Mo1Sr2Dy1.5Ce1Cu2O10	Mo	1	Sr	2	Dy	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.011			per R-ion	10.1	-4.9																					Ru1222			A	3.815		28.37												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34135	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Ho,Ce)2Cu2O10	Mo1Sr2Ho1.5Ce1Cu2O10	Mo	1	Sr	2	Ho	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0047			per R-ion	10.6	-4.4																					Ru1222			A	3.812		28.4												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34136	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Er,Ce)2Cu2O10	Mo1Sr2Er1.5Ce1Cu2O10	Mo	1	Sr	2	Er	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0001			per R-ion	10.1	-11.3																					Ru1222			A	3.81		28.44												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34137	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Tm,Ce)2Cu2O10	Mo1Sr2Tm1.5Ce1Cu2O10	Mo	1	Sr	2	Tm	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.00184			per R-ion	7.56	-22																					Ru1222			A	3.797		28.3												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34138	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Yb,Ce)2Cu2O10	Mo1Sr2Yb1.5Ce1Cu2O10	Mo	1	Sr	2	Yb	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0022			per R-ion	3.58	-7.5																					Ru1222			A	3.807		28.41												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34139	P068064507	mag. transition not determined. KAIZERO in emu/mol.Oe.	MoSr2(Y,Ce)2Cu2O10	Mo1Sr2Y1.5Ce1Cu2O10	Mo	1	Sr	2	Y	1.5	Ce	1	Cu	2											O	10		1	2003	emu/m.Oe	0.0005			per R-ion	1.68	-1.4																					Ru1222			A	3.812		28.43												K					5																																																																																																R2O3,CeO2,SrCO3,MO,CuO2	1	mixture - heat(950C, 1d) - SIN(1050C, 2d, in O2)					Competition of superconductivity and magnetism in MoSr2R1.5Ce0.5Cu2O10-z (R=rare earth)			Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel	Phys.Rev.B, 68(2003)64507	E.Galstyan,I.Felner		
34140	P068064514		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2003																												Ru1212																		K	29.5		43.9				36.7																																																																		uV/K	76.8			TP34140															m3/C	0.00000000504					RH34140				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34141	P068064514		(Ru,Sn)Sr2GdCu2O8	Ru0.6Sn0.4Sr2Gd1Cu2O8	Ru	0.6	Sn	0.4	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K	6		30.1				18.05																																																																		uV/K	74.5			TP34141															m3/C	0.00000001006					RH34141				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34142	P068064514		(Ru,Sn)Sr2GdCu2O8	Ru0.8Sn0.2Sr2Gd1Cu2O8	Ru	0.8	Sn	0.2	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K	28.4		48				38.2																																																																		uV/K	73.1																		m3/C	0.00000000656					RH34142				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34143	P068064514		(Ru,Sn)Sr2GdCu2O8	Ru0.925Sn0.075Sr2Gd1Cu2O8	Ru	0.925	Sn	0.075	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K	30		45.6				37.8																																																																		uV/K	74.5																		m3/C	0.0000000058					RH34143				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34144	P068064514		(Ru,Sn)Sr2GdCu2O8	Ru0.975Sn0.025Sr2Gd1Cu2O8	Ru	0.975	Sn	0.025	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K	30		43.8				36.9																																																																		uV/K	74.5																		m3/C	0.0000000058					RH34144				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34145	P068064514	semiconductor like.	(Ru,Nb)Sr2GdCu2O8	Ru0.8Nb0.2Sr2Gd1Cu2O8	Ru	0.8	Nb	0.2	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K					2																																																																				uV/K	124.2			TP34145																					RH34145				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34146	P068064514		(Ru,Nb)Sr2GdCu2O8	Ru0.9Nb0.1Sr2Gd1Cu2O8	Ru	0.9	Nb	0.1	Sr	2	Gd	1	Cu	2											O	8			2003																												Ru1212																		K	4.1		19.2				11.65																																																																		uV/K	100.8			TP34146															m3/C	0.00000000778					RH34146				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34147	P068064514	semiconductor like.	RuSr2(Gd,Ce)Cu2O8	Ru1Sr2Gd0.9Ce0.1Cu2O8	Ru	1	Sr	2	Gd	0.9	Ce	0.1	Cu	2											O	8			2003																												Ru1212																		K					2																																																																				uV/K	107.2			TP34147															m3/C	0.00000000712					RH34147				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34148	P068064514	semiconductor like.	RuSr2(Gd,Ce)Cu2O8	Ru1Sr2Gd0.8Ce0.2Cu2O8	Ru	1	Sr	2	Gd	0.8	Ce	0.2	Cu	2											O	8			2003																												Ru1212																		K					2																																																																				uV/K	79.7			TP34148															m3/C	0.00000000902					RH34148				1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34149	P068064514		RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8			2003																												Ru1212																		K			30				30																																																																		uV/K	88.6																		m3/C	0.00000000925									1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34150	P068064514		RuSr2(Gd,Dy)Cu2O8	Ru1Sr2Gd0.6Dy0.4Cu2O8	Ru	1	Sr	2	Gd	0.6	Dy	0.4	Cu	2											O	8			2003																												Ru1212																		K	33.4		53.1				43.25																																																																		uV/K	73.2																		m3/C	0.00000000735									1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34151	P068064514		RuSr2(Gd,Y)Cu2O8	Ru1Sr2Gd0.9Y0.1Cu2O8	Ru	1	Sr	2	Gd	0.9	Y	0.1	Cu	2											O	8			2003																												Ru1212																		K	21.4		43				32.2																																																																		uV/K	70.2																		m3/C	0.00000000596									1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34152	P068064514		RuSr2Gd(Cu,Li)2O8	Ru1Sr2Gd1Cu1.9Li0.1O8	Ru	1	Sr	2	Gd	1	Cu	1.9	Li	0.1											O	8			2003																												Ru1212																		K	13		25				19																																																																		uV/K	79.4																		m3/C	0.00000000562									1	solid state reaction. ANN(1060C, in O2 flow)					Magnetotransport properties of doped RuSr2GdCu2O8			IRC in Superconductivity, Cambridge University, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 68(2003)64514	A.C.MacLaughlin,C.Bernhard,J.E.McCrone,J.L.Tallon,J.P.Attfield,J.R.Cooper		
34153	P068094507	c-axis oriented film. thickness=3000-6000A. 	(Pr,Ce)2CuO4	Pr1.87Ce0.13Cu1O4	Pr	1.87	Ce	0.13	Cu	1															O	4		5	2003																												T'																		K		10					10																				T	resistivity			6.5												A	Hc2		70																																																									Films made by PLD method on LaAlO3 substrate.					Doping dependence of the upper critical field of electron-doped Pr2-xCexCuO4 thin films			Canadian Institute of Advanced Research, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 68(2003)94507	P.Fournier,R.L.Greene		
34154	P068094507	c-axis oriented film. thickness=3000-6000A. Hc2 measured down to 38 mK.	(Pr,Ce)2CuO4	Pr1.86Ce0.14Cu1O4	Pr	1.86	Ce	0.14	Cu	1															O	4		5	2003																												T'																		K		21					21																				T	resistivity			10												A	Hc2		56																																																									Films made by PLD method on LaAlO3 substrate.					Doping dependence of the upper critical field of electron-doped Pr2-xCexCuO4 thin films			Canadian Institute of Advanced Research, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 68(2003)94507	P.Fournier,R.L.Greene		
34155	P068094507	c-axis oriented film. thickness=3000-6000A. Hc2 measured down to 38 mK.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2003																												T'																		K		23					23																				T	resistivity			9												A	Hc2		60																																																									Films made by PLD method on LaAlO3 substrate.					Doping dependence of the upper critical field of electron-doped Pr2-xCexCuO4 thin films			Canadian Institute of Advanced Research, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 68(2003)94507	P.Fournier,R.L.Greene		
34156	P068094507	c-axis oriented film. thickness=3000-6000A. Hc2 measured down to 38 mK.	(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O4	Pr	1.83	Ce	0.17	Cu	1															O	4		5	2003																												T'																		K		13					13																				T	resistivity			7												A	Hc2		67																																																									Films made by PLD method on LaAlO3 substrate.					Doping dependence of the upper critical field of electron-doped Pr2-xCexCuO4 thin films			Canadian Institute of Advanced Research, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 68(2003)94507	P.Fournier,R.L.Greene		
34157	P068094507	c-axis oriented film. thickness=3000-6000A. 	(Pr,Ce)2CuO4	Pr1.8Ce0.2Cu1O4	Pr	1.8	Ce	0.2	Cu	1															O	4		5	2003																												T'																		K		6					6																				T	resistivity			2.5												A	Hc2		113																																																									Films made by PLD method on LaAlO3 substrate.					Doping dependence of the upper critical field of electron-doped Pr2-xCexCuO4 thin films			Canadian Institute of Advanced Research, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 68(2003)94507	P.Fournier,R.L.Greene		
34158	P068094508	Two peaks (91K, 120K) in ac-sus are observed.	RuSr2(Dy,Ce)2Cu2O10	Ru1Sr2Dy1.5Ce0.5Cu2O10	Ru	1	Sr	2	Dy	1.5	Ce	0.5	Cu	2											O	10		1	2003																												Ru1222	I4/mmm		A	3.824		28.445												K					4.2																																																																																																		high pressure synthesis (6 GPa, 1200C)					Magnetization study of RuSr2Y1.5Ce0.5Cu2O10			Racah Institute of Physics, The Hebrew University, Jerusalem, Israel	Phys.Rev.B, 68(2003)94508	E.Takayama-Muromachi,I.Felner,V.P.S.Awana		
34159	P068094508	impurity phase < 0.3 %. AFM by Ru-sublattice. Two peaks (105K, 128K) in ac-sus are observed.	RuSr2(Y,Ce)2Cu2O10	Ru1Sr2Y1.5Ce0.5Cu2O10	Ru	1	Sr	2	Y	1.5	Ce	0.5	Cu	2											O	10			2003								152																				Ru1222	I4/mmm		A	3.819		28.439												K					4.2																																																																																																		high pressure synthesis (6 GPa, 1200C)					Magnetization study of RuSr2Y1.5Ce0.5Cu2O10			Racah Institute of Physics, The Hebrew University, Jerusalem, Israel	Phys.Rev.B, 68(2003)94508	E.Takayama-Muromachi,I.Felner,V.P.S.Awana		
34160	P068094508	Two peaks (107K, 130K) in ac-sus are observed.	RuSr2(Ho,Ce)2Cu2O10	Ru1Sr2Ho1.5Ce0.5Cu2O10	Ru	1	Sr	2	Ho	1.5	Ce	0.5	Cu	2											O	10		1	2003																												Ru1222	I4/mmm		A	3.813		28.419												K					4.2																																																																																																		high pressure synthesis (6 GPa, 1200C)					Magnetization study of RuSr2Y1.5Ce0.5Cu2O10			Racah Institute of Physics, The Hebrew University, Jerusalem, Israel	Phys.Rev.B, 68(2003)94508	E.Takayama-Muromachi,I.Felner,V.P.S.Awana		
34161	P068100502	sp-heat cntain T<-2> and T<5> terms. fitting range (0.6<T<10K).	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		3	2003																												T																		K					0.095																																																										mj/mol.K2	6.9		550	from sp-heat																																				ab- and c- axis single crystals were from large crystals. ANN(400 atm-O2, 900C, 2 weeks)					Electronic ground state of heavily overdoped nonsuperconducting La2-xSrxCuO4			LPQ (UPR5-CNRS), ESPCI, 10 Rue Vauquelin, F-75005 Paris, France	Phys.Rev.B, 68(2003)100502	H.Takagi,K.Behnia,M.Nohara,N.E.Hussey,N.Mangkorntong,S.J.C.Yates,S.Nakamae		
34162	P068104520	Thermal conductivity measured	(La,Nd,Sr)2CuO4	La1.48Nd0.4Sr0.12Cu1O4	La	1.48	Nd	0.4	Sr	0.12	Cu	1													O	4		3	2003																												T																		K				11			11																																																																	THC34162																															single crystals grown by TSFZ method. ANN(900C, 20h, in air)					Thermal conductivity in the stripe-ordered phase of cuprates and nickelates			Texas Materials Institute, University of Texas at Austin, Austin, Texas, USA	Phys.Rev.B, 68(2003)104520	J.-Q.Yan,J.-S.Zhou,J.B.Goodenough		
34163	P068104520	Thermal conductivity measured	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	2003																												T																		K				15			15																																																																	THC34163																															single crystals grown by TSFZ method. ANN(900C, 20h, in air)					Thermal conductivity in the stripe-ordered phase of cuprates and nickelates			Texas Materials Institute, University of Texas at Austin, Austin, Texas, USA	Phys.Rev.B, 68(2003)104520	J.-Q.Yan,J.-S.Zhou,J.B.Goodenough		
34164	P068104520	Thermal conductivity measured	(La,Nd,Sr)2CuO4	La1.4Nd0.4Sr0.2Cu1O4	La	1.4	Nd	0.4	Sr	0.2	Cu	1													O	4		3	2003																												T																		K					5																																																																			THC34164																															single crystals grown by TSFZ method. ANN(900C, 20h, in air)					Thermal conductivity in the stripe-ordered phase of cuprates and nickelates			Texas Materials Institute, University of Texas at Austin, Austin, Texas, USA	Phys.Rev.B, 68(2003)104520	J.-Q.Yan,J.-S.Zhou,J.B.Goodenough		
34165	P068104516		GdBa2Cu3Oz	Gd1Ba2Cu3O6.99	Gd	1	Ba	2	Cu	3															O	7-z	6.99	1	2003									5.47																		3	Y123			A	3.847	3.89	11.696												K		90.9				4.1	90.9																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34166	P068104516		Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.95Pr0.05Cu3O7.03	Gd	1	Ba	1.95	Pr	0.05	Cu	3													O	7-z	7.03	1	2003									4.32																		3	Y123			A	3.847	3.889	11.692												K		86.8				13.2	86.8																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34167	P068104516	hump in resistivity R(T) occurs at Tm=85.6 K.	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.9Pr0.1Cu3O7.03	Gd	1	Ba	1.9	Pr	0.1	Cu	3													O	7-z	7.03	1	2003									5.43																		3	Y123			A	3.855	3.886	11.671												K		63.3				16.3	63.3																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34168	P068104516	hump in resistivity R(T) occurs at Tm=90.9 K.	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.85Pr0.15Cu3O7.09	Gd	1	Ba	1.85	Pr	0.15	Cu	3													O	7-z	7.09	1	2003									4.26																		3	Y123			A	3.86	3.881	11.66												K		55.8				19.7	55.8																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34169	P068104516	hump in resistivity R(T) occurs at Tm=80.3 K.	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.8Pr0.2Cu3O7.01	Gd	1	Ba	1.8	Pr	0.2	Cu	3													O	7-z	7.01	1	2003									4.65																		2	Y123			A	3.87		11.645												K		44.5				25.1	44.5																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34170	P068104516	hump in resistivity R(T) occurs at Tm=82.8 K.	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.75Pr0.25Cu3O7.06	Gd	1	Ba	1.75	Pr	0.25	Cu	3													O	7-z	7.06	1	2003									4.62																		2	Y123			A	3.868		11.635												K		39.2				23.8	39.2																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34171	P068104516	hump in resistivity R(T) occurs at Tm=81.2 K.	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.7Pr0.3Cu3O7.06	Gd	1	Ba	1.7	Pr	0.3	Cu	3													O	7-z	7.06	1	2003									4.61																		2	Y123			A	3.869		11.608												K		22.9				35.7	22.9																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34172	P068104516		Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.65Pr0.35Cu3O6.97	Gd	1	Ba	1.65	Pr	0.35	Cu	3													O	7-z	6.97	1	2003									4.89																		2	Y123			A	3.869		11.585												K		10					10																																																																																																standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34173	P068104516	not s/c	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.6Pr0.4Cu3O6.99	Gd	1	Ba	1.6	Pr	0.4	Cu	3													O	7-z	6.99	1	2003									4.48																		2	Y123			A	3.868		11.58												K																																																																																																							standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34174	P068104516	not s/c	Gd(Ba,Pr)2Cu3Oz	Gd1Ba1.5Pr0.5Cu3O6.96	Gd	1	Ba	1.5	Pr	0.5	Cu	3													O	7-z	6.96	1	2003									4.29																		2	Y123			A	3.865		11.563												K																																																																																																							standard solid state reaction					Pr at Gd or Ba site in GdBa2Cu3O7 : Appearance of superconductivity			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, Tehran, Iran	Phys.Rev.B, 68(2003)104516	M.Akhavan,M.R.Mohammadizadeh		
34175	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.014	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.014	1	2003																												T'																		K		25					25																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34176	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.026	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.026	1	2003																												T'																		K		21.1					21.1																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34177	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.028	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.028	1	2003																												T'																		K		21.1					21.1																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34178	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.034	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.034	1	2003																												T'																		K		18.1					18.1																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34179	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.037	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.037	1	2003																												T'																		K		9.1					9.1																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34180	P068104524		(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.045	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.045	1	2003																												T'																		K		0					0																																																																																																solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34181	P068104524	spin glass temp (Nd-spin) = 1.82 K. not s/c.	(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.06	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.06	1	2003																												T'																		K					4.2																																																																																																		solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34182	P068104524	spin glass temp (Nd-spin) = 3.52 K. not s/c.	(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.062	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.062	1	2003																												T'																		K					4.2																																																																																																		solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34183	P068104524	spin glass temp (Cu-spin) = 5.00 K. not s/c.	(Nd,Ce)2CuOz	Nd1.85Ce0.15Cu1O4.064	Nd	1.85	Ce	0.15	Cu	1															O	4+z	4.064	1	2003																												T'																		K					4.2																																																																																																		solid state reaction (1070C, 200h, in air) - ANN(1173K, 50h, in various O2 pressure)					Magnetic phase diagram of Nd1.85Ce0.15CuO4+z from magnetization and muon spin relaxation measurements			"Department of Physics ""A. Volta"" and INFM, Pavia, Italy"	Phys.Rev.B, 68(2003)104524	A.Lascialfari,F.Tedoldi,P.Ghigna		
34184	LOW1310837	excess-O doping sample. Tc defined as R/Rn=0.5. hole conc. P=2z (z=excess-O)	(La,Nd)2CuOz	La1.8Nd0.2Cu1O4.0641	La	1.8	Nd	0.2	Cu	1															O	4+z	4.0641		2003																												T																		K		25.1					25.1	TC34184																																																																																															solid state reaction. excess oxygen doping was made by the electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34185	LOW1310837	excess-O doping sample. Tc defined as R/Rn=0.5. hole conc. P=2z (z=excess-O)	(La,Nd)2(Cu,Zn)Oz	La1.8Nd0.2Cu0.99Zn0.01O4.0631	La	1.8	Nd	0.2	Cu	0.99	Zn	0.01													O	4+z	4.0631		2003																												T																		K		4.87					4.87	TC34185																																																																																															solid state reaction. excess oxygen doping was made by the electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34186	LOW1310837	excess-O doping sample. Tc defined as R/Rn=0.5. hole conc. P=2z (z=excess-O)	(La,Bi)2CuOz	La1.95Bi0.05Cu1O4.0635	La	1.95	Bi	0.05	Cu	1															O	4+z	4.0635		2003																												T																		K		34.9					34.9	TC34186																																																																																															solid state reaction. excess oxygen doping was made by the electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34187	LOW1310837	excess-O doping sample. Tc defined as R/Rn=0.5. hole conc. P=2z (z=excess-O)	(La,Bi)2(Cu,Zn)Oz	La1.95Bi0.05Cu0.99Zn0.01O4.0628	La	1.95	Bi	0.05	Cu	0.99	Zn	0.01													O	4+z	4.0628		2003																												T																		K		24.2					24.2	TC34187																																																																																															solid state reaction. excess oxygen doping was made by the electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34188	LOW1310837	excess-O doping sample. Tc defined as R/Rn=0.5. hole conc. P=2z (z=excess-O)	(La,Pr)2CuOz	La1.8Pr0.2Cu1O4.0631	La	1.8	Pr	0.2	Cu	1															O	4+z	4.0631		2003																												T																		K		20.2					20.2	TC34188																																																																																															solid state reaction. excess oxygen doping was made by the electrochemical oxidation method.					1/8 anomaly in the excess-oxygen-doped La2-xAxCuO4+z (A = Nd, Bi, Pr)			Department of Applied Physics, Tohoku University, Sendai, Japan	J.Low Temp.Phys., 131(2003)837	H.Mikuni,I.Watanabe,K.Nagamine,S.Yairi,T.Adachi,Y.Koike		
34189	PHC3980085		(Ru,Cu)Sr2YCu2Oz	Ru0.8Sr2Y1Cu2.2O7.8	Ru	0.8	Sr	2	Y	1	Cu	2.2													O	8	7.8		2003							140																					Ru1212			A	3.815		11.504												K				43			43																																																																																																high-pressure synthesis (1200 - 1300C, 6 GPa)					High-pressure synthesis and physical properties of ruthenate-cuprates RuSr2LnCu2O8 (Ln=Y, Dy, Ho, Er)			Superconducting Materials Center, National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 398(2003)85	E.Takayama-Muromachi,T.Kawashima		
34190	PHC3980085	zero resistivity attains. additional ferromag-like transition at 27 K.	(Ru,Cu)Sr2YCu2Oz	Ru0.8Sr2Y1Cu2.2O8.1	Ru	0.8	Sr	2	Y	1	Cu	2.2													O	8	8.1		2003							121																					Ru1212			A	3.808		11.514												K	35			65			65																																																																																																high-pressure synthesis (1200 - 1300C, 6 GPa)					High-pressure synthesis and physical properties of ruthenate-cuprates RuSr2LnCu2O8 (Ln=Y, Dy, Ho, Er)			Superconducting Materials Center, National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 398(2003)85	E.Takayama-Muromachi,T.Kawashima		
34191	PHC3980085		RuSr2DyCu2Oz	Ru0.9Sr2Dy1Cu2O7.8	Ru	0.9	Sr	2	Dy	1	Cu	2													O	8	7.8	1	2003							170																					Ru1212			A	3.82		11.512												K					5																																																																																																		high-pressure synthesis (1200 - 1300C, 6 GPa)					High-pressure synthesis and physical properties of ruthenate-cuprates RuSr2LnCu2O8 (Ln=Y, Dy, Ho, Er)			Superconducting Materials Center, National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 398(2003)85	E.Takayama-Muromachi,T.Kawashima		
34192	PHC3980085		RuSr2HoCu2Oz	Ru0.9Sr2Ho1Cu2O7.8	Ru	0.9	Sr	2	Ho	1	Cu	2													O	8	7.8	1	2003							170																					Ru1212			A	3.813		11.499												K					5																																																																																																		high-pressure synthesis (1200 - 1300C, 6 GPa)					High-pressure synthesis and physical properties of ruthenate-cuprates RuSr2LnCu2O8 (Ln=Y, Dy, Ho, Er)			Superconducting Materials Center, National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 398(2003)85	E.Takayama-Muromachi,T.Kawashima		
34193	PHC3980085	not zero resistivity. FC-SQUID and resistivity start to decrease at 43 K and 23 K, respectively.	RuSr2ErCu2Oz	Ru0.9Sr2Er1Cu2O7.8	Ru	0.9	Sr	2	Er	1	Cu	2													O	8	7.8	1	2003							170																					Ru1212			A	3.81		11.505												K			23				23																																																																																																high-pressure synthesis (1200 - 1300C, 6 GPa)					High-pressure synthesis and physical properties of ruthenate-cuprates RuSr2LnCu2O8 (Ln=Y, Dy, Ho, Er)			Superconducting Materials Center, National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 398(2003)85	E.Takayama-Muromachi,T.Kawashima		
34194	JPS0661405	anisotropy R<c>/R<ab> exceeds 500 for T<80K. R=R0 + A*T2. A<ab>=7.3 nOhm.cm/K2. A<c>=4.0 uOhm.cm/K2	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1997																												T	I4/mmm		A	3.87		12.74												K		1					1																																																					SP34194			mj/mol.K2	35.7	from sp-heat																																						floating zone method					Two-Dimensional Fermi Liquid Behavior of the Superconductor Sr2RuO4			Department of Physics, Hiroshima University, Higashi-Hiroshima 739 , Japan	J.Phys.Soc.Jpn, 66(1997)1405	A.P.Mackenzie,F.Lichtenberg,H.Hashimoto,J.G.Bednorz,K.Yoshida,M.Nohara,N.E.Fussey,S.Ikeda,S.Nishizaki,T.Fujita,Y.Maeno		
34195	JPS0722453	y=1.3(tentative). NMR, spin-echo were measured. gap(delta)=8.1 K.	NaxCoO2/yH2O	Na0.75Co1H2.6O3.3	Na	0.75	Co	1	H	2.6															O	3.3			2003																																														K				4.5			4.5																																																3.6	6																																															See Nature 422(2003)53					<59>Co-NMR Knight Shift of Superconducting NaxCoO2-H2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602 ,Japan	J.Phys.Soc.Jpn, 72(2003)2453	M.Sato,M.Yokoi,Y.Kobayashi		
34196	P068134516	enriched <119>Sn (85 %) was used	(Ru,Sn)Sr2GdCu2O8	Ru0.95Sn0.05Sr2Gd1Cu2O8	Ru	0.95	Sn	0.05	Sr	2	Gd	1	Cu	2											O	8		1	2003							123																					Ru1212																		K			30				30																																																																																															1	solid state reaction. SIN(1050C, 4d, in O2 flow) - cool to RT(45C/h)					<119>Sn Mossbauer spectroscopy in the magnetic superconductor (Ru, Sn)Sr2GdCu2O8			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, Urca, CEP, Rio de Janeiro, Brazil	Phys.Rev.B, 68(2003)134516	Ada,E.Baggio-Saitovitch,I.Souza Azevedo,J.E.Musa,Lopez,S.Garcia Garcia		
34197	P068132507	G-L parameter = 244.	NaxCoO2/yH2O	Na0.35Co1H2.6O3.3	Na	0.35	Co	1	H	2.6															O	3.3			2003																																														K				4.6			4.6											Oe	deviation from M-H curve	28.1							T	using WHH theory	61							T/K		19.3			HC34197		A	from Hc2	23.2			A	From cohere and Hc1	5680																																																					See Nature 422(2003)53					Unconventional upper- and lower-critical fields and normal-state magnetic susceptibility of the superconducting compound Na0.35CoO2/1.3H2O			National Institute for Materials Science (SMC/NIMS), 1-1 Namiki, Tsukuba, Ibaraki, Japan	Phys.Rev.B, 68(2003)132507	E.Takayama-Muromochi,H.Sakurai,K.Kindo,K.Takada,S.Yoshii,T.Sasaki		
34198	P068132504	dTc/dP is estimated from Tc(P) by ASADA. Tc(P) = 4.68 - 0.0047*P - 0.183*P2.  y = 1.3 (tentative)	NaxCoO2/yH2O	Na0.35Co1H2.6O3.3	Na	0.35	Co	1	H	2.6															O	3.3		1	2003																													P6<3>/mmc		A	2.82		19.593												K				4.7			4.7	TC34198		K/GPa	-0.107																																																																																												See Nature 422(2003)53					Effect of hydrostatic pressure on the superconductivity in NaxCoO2/yH2O			Department of Physics and TCSAM, University of Houston, Houston, Texas, USA	Phys.Rev.B, 68(2003)132504	B.Lorenz,C.W.Chu,J.Cmaidalka,R.L.Meng		
34199	PHC3990069	as-prepared. Ru:Sr:Sm:Ce:Cu=0.95:2.04:1.37:0.54:2.08 by EDS. R(250K)=50.4 mOhm.cm. hysteresis observed at 5K.	RuSr2(Sm,Ce)2Cu2O10	Ru1Sr2Sm1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Sm	1.4	Ce	0.6	Cu	2											O	10-z		1	2003																												Ru1222			A	3.842		28.469												K	18		38				28																																																																																														RuO2,SrCO3,Sm2O3,CeO2,CuO	1	mixture - heat(1070C,60h, in flowing O2) - slow cool to RT					Structural, transport and magnetic properties of RuSr2Sm1.4Ce0.6Cu2O10-d			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 399(2003)69	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.J.Fan		
34200	PHC3990069	not s/c. as-prepared and ANN(1070C,24h, in air). Ru:Sr:Sm:Ce:Cu=0.95:1.98:1.39:0.61:2.07 by EDS. R(250K)=1346.9 mOhm.cm.	RuSr2(Sm,Ce)2Cu2O10	Ru1Sr2Sm1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Sm	1.4	Ce	0.6	Cu	2											O	10-z		1	2003																												Ru1222			A	3.844		28.477												K					5																																																																																																RuO2,SrCO3,Sm2O3,CeO2,CuO	1	mixture - heat(1070C,60h, in flowing O2) - slow cool to RT					Structural, transport and magnetic properties of RuSr2Sm1.4Ce0.6Cu2O10-d			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 399(2003)69	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.J.Fan		
34201	PHC3990069	as-prepared and ANN(1070C,24h,in O2-flow). Ru:Sr:Sm:Ce:Cu=0.93:2.01:1.39:0.60:2.07 by EDS. R(250K)=48.4 mOhm.cm.	RuSr2(Sm,Ce)2Cu2O10	Ru1Sr2Sm1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Sm	1.4	Ce	0.6	Cu	2											O	10-z		1	2003																												Ru1222			A	3.842		28.461												K	24		40				32																																																																																														RuO2,SrCO3,Sm2O3,CeO2,CuO	1	mixture - heat(1070C,60h, in flowing O2) - slow cool to RT					Structural, transport and magnetic properties of RuSr2Sm1.4Ce0.6Cu2O10-d			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 399(2003)69	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.J.Fan		
34202	PHC3990069	not s/c. as-prepared and ANN(1070C,24h,in Ar-flow). Ru:Sr:Sm:Ce:Cu=0.96:1.99:1.41:0.58:2.06 by EDS. R(250K)=1434.5 mOhm.cm.	RuSr2(Sm,Ce)2Cu2O10	Ru1Sr2Sm1.4Ce0.6Cu2O10-z	Ru	1	Sr	2	Sm	1.4	Ce	0.6	Cu	2											O	10-z		1	2003																												Ru1222			A	3.845		28.485												K					5																																																																																																RuO2,SrCO3,Sm2O3,CeO2,CuO	1	mixture - heat(1070C,60h, in flowing O2) - slow cool to RT					Structural, transport and magnetic properties of RuSr2Sm1.4Ce0.6Cu2O10-d			Structure Research Laboratory, Department of Materials Science and Engineering, University of Science and Technology of China, Hefei, China	Physica C, 399(2003)69	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.J.Fan		
34203	PHC3990061	HIP at 1000C. oz = 7.20 befor HIP sample.	YBa2Cu2(Cu,Fe)Oz	Y1Ba2Cu2.5Fe0.5O7.35	Y	1	Ba	2	Cu	2.5	Fe	0.5													O	7+z	7.35	1	2003																												1212			A	3.8659		11.5985												K			80	80			80	TC34203									50																																																																																						mixture - SIN(930C,40h,in air) - cool to RT(30C/h), mix with 5 wt% KClO4, then heat(750-1070C,0.5h, under 6GPa)					High-pressure synthesis of Fe0.5Cu0.5Ba2YCu2O7+d superconductors and influence of synthesis conditions on the lattice parameters and superconductivity			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, PR China	Physica C, 399(2003)61	G.Che,H.Chen,K.Li,S.Jia,W.Huang,Y.Liu,Z.Zhao		
34204	PHC3410563	Fe-1212 prepared without reducing ANN process is not s/c.	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.66	Fe	1	Sr	2	Y	1	Cu	2													O	7+z	7.66	1	2000																												1212																		K	25		62				43.5																																																																																																mixture - CAL(1173K,12h,in air) - SIN(1223K,24h,in air) - ANN(1073K,5h,in P(O2)=100 Pa) - cool to 573K - ANN(523K,24h,in P(O2)=3.5E+7 Pa)					Discovery of Superconductivity in Fe-Based Cuprates			Department of Superconductivity, University of Tokyo,Hongo, Bunkyo-ku, Tokyo, Japan	Physica C, 341(2000)563	J.Shimoyama,K.Kishio,K.Otzschi,T.Hinouchi		
34205	JPS0710790	sample without ANN(N2 flow) is not s/c. structure precisely investigated.	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.68	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.68	1	2002																											2	1212	P4/mmm		A	3.822		11.4024												K				50			50																																																																																																mixture - CAL(900C,24h,in air) - SIN(1000C,24h,in air) - ANN(800C,24h,in N2 flow) - ANN(300C,24h,in O2 flow) - ANN(350C,24hin 195 atm O2)					Crystal Structure of Magnetic Superconductor FeSr2YCu2O6+z				J.Phys.Soc.Jpn, 71(2002)790	H.Fujii,J.Suzuki,K.Hirata,K.Kadowaki,M.Furuyama,N.Metoki,S.Kamisawa,T.Mochiku,Y.Hata,Y.Mihara		
34206	PHC3980131		Y(Ba,Nd)2Cu3Oz	Y1Ba1.9Nd0.1Cu3Oz	Y	1	Ba	1.9	Nd	0.1	Cu	3													O	z		1	2003																												Y123			A	3.886	3.8215	11.687												K	90.6	91.6				2.3	91.6																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34207	PHC3980131	spin gap temp. = 116 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.95Ca0.05Ba1.9Nd0.1Cu3Oz	Y	0.95	Ca	0.05	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8827	3.8229	11.6815												K	86.2	87.2				2.4	87.2																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34208	PHC3980131	spin gap temp. = 122 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.9Ca0.1Ba1.9Nd0.1Cu3Oz	Y	0.9	Ca	0.1	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.881	3.8251	11.6839												K	82.5	83.7				2.6	83.7																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34209	PHC3980131	spin gap temp. = 128 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.85Ca0.15Ba1.9Nd0.1Cu3Oz	Y	0.85	Ca	0.15	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8802	3.827	11.6837												K	82.5	84.2				3.6	84.2																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34210	PHC3980131	spin gap temp. = 135.9 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.8Ca0.2Ba1.9Nd0.1Cu3Oz	Y	0.8	Ca	0.2	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8777	3.828	11.6809												K	81	82.7				3.5	82.7																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34211	PHC3980131	spin gap temp. = 158.1 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.75Ca0.25Ba1.9Nd0.1Cu3Oz	Y	0.75	Ca	0.25	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8776	3.8298	11.6832												K	77.1	80.1				4.8	80.1																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34212	PHC3980131	spin gap temp. = 165 K	(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.7Ca0.3Ba1.9Nd0.1Cu3Oz	Y	0.7	Ca	0.3	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8675	3.8488	11.7362												K	77.3	80.6				6.1	80.6																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34213	PHC3980131		(Y,Ca)(Ba,Nd)2Cu3Oz	Y0.6Ca0.4Ba1.9Nd0.1Cu3Oz	Y	0.6	Ca	0.4	Ba	1.9	Nd	0.1	Cu	3											O	z		1	2003																												Y123			A	3.8627	3.859	11.778												K	76.2	80.3				5.5	80.3																																																																																															1	mixture - CAL(950C,16h,in air) - SIN(950C,20h,in air) - ANN(400C,25h,in flowing O2) - FC to RT					Structure and spin-gap in the normal state of Y1-xCaxBa1.9Nd0.1Cu3Oy cuprates			Department of Physics, Nanjing University, Nanjing 210093, PR China	Physica C, 398(2003)131	A.Hu,E.M.Zhang,J.Du,J.Gao,S.S.Jiang,W.S.Tan,X.S.Wu,Y.M.Xu		
34214	PHC3980123	resistivity minimum at 87K. Ferromag-order	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2003							142																					Ru1212																		K	31	43	46	28			43																																																																						TP34214																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34215	PHC3980123	 Ferromag-order	Ru(Sr,La)2GdCu2O8	Ru1Sr1.98La0.02Gd1Cu2O8	Ru	1	Sr	1.98	La	0.02	Gd	1	Cu	2											O	8		1	2003							142																					Ru1212																		K	14	20.6	33	12			20.6																																		HC34215																																				TP34215																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34216	PHC3980123	 Ferromag-order	Ru(Sr,La)2GdCu2O8	Ru1Sr1.94La0.06Gd1Cu2O8	Ru	1	Sr	1.94	La	0.06	Gd	1	Cu	2											O	8		1	2003							154																					Ru1212																		K					1.5																																																																								TP34216																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34217	PHC3980123	 Ferromag-order	Ru(Sr,La)2GdCu2O8	Ru1Sr1.9La0.1Gd1Cu2O8	Ru	1	Sr	1.9	La	0.1	Gd	1	Cu	2											O	8		1	2003							180																					Ru1212																		K					1.5																																																																								TP34217																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34218	PHC3980123		RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8		1	2003																												Ru1212																		K	12		35				23.5																																																																						TP34218																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34219	PHC3980123		Ru(Sr,La)2EuCu2O8	Ru1Sr1.98La0.02Eu1Cu2O8	Ru	1	Sr	1.98	La	0.02	Eu	1	Cu	2											O	8		1	2003																												Ru1212																		K	5		23				14																																																																						TP34219																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34220	PHC3980123		Ru(Sr,La)2EuCu2O8	Ru1Sr1.94La0.06Eu1Cu2O8	Ru	1	Sr	1.94	La	0.06	Eu	1	Cu	2											O	8		1	2003																												Ru1212																		K	3		11				7																																																																						TP34220																									1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34221	PHC3980123		Ru(Sr,La)2EuCu2O8	Ru1Sr1.9La0.1Eu1Cu2O8	Ru	1	Sr	1.9	La	0.1	Eu	1	Cu	2											O	8		1	2003																												Ru1212																		K					1.5																																																																																																	1	ANN(1060C,6d,in flowing O2) - slow cool to RT					Transport and magnetic properties of Ru(Sr1-xLaxRCu2O8 (R=Gd, Eu) superconductor			Experimentalphysik V, EKM, Universitat Augsburg, Augsburg, Germany	Physica C, 398(2003)123	A.Hassen,A.Krimmel,A.Loidl,G.Ghosh,J.Hemberger,P.Choudhury,P.Mandal		
34222	P068134516	Tc not given. enriched <119>Sn (85 %) was used.	(Ru,Sn)Sr2GdCu2O8	Ru0.9Sn0.1Sr2Gd1Cu2O8	Ru	0.9	Sn	0.1	Sr	2	Gd	1	Cu	2											O	8		1	2003							109																					Ru1212																		K																																																																																																						1	solid state reaction. SIN(1050C, 4d, in O2 flow) - cool to RT(45C/h)					<119>Sn Mossbauer spectroscopy in the magnetic superconductor (Ru, Sn)Sr2GdCu2O8			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, Urca, CEP, Rio de Janeiro, Brazil	Phys.Rev.B, 68(2003)134516	Ada,E.Baggio-Saitovitch,I.Souza Azevedo,J.E.Musa,Lopez,S.Garcia Garcia		
34223	P068134516	Tc not given. impurity phase = SrSnO3. isomer shift (Mossbauer) measured.	(Ru,Sn)Sr2GdCu2O8	Ru0.8Sn0.2Sr2Gd1Cu2O8	Ru	0.8	Sn	0.2	Sr	2	Gd	1	Cu	2											O	8			2003							102																					Ru1212																		K																																																																																																						1	solid state reaction. SIN(1050C, 4d, in O2 flow) - cool to RT(45C/h)					<119>Sn Mossbauer spectroscopy in the magnetic superconductor (Ru, Sn)Sr2GdCu2O8			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, Urca, CEP, Rio de Janeiro, Brazil	Phys.Rev.B, 68(2003)134516	Ada,E.Baggio-Saitovitch,I.Souza Azevedo,J.E.Musa,Lopez,S.Garcia Garcia		
34224	P068134516	impurity phase = SrSnO3. isomer shift (Mossbauer) measured.	(Ru,Sn)Sr2GdCu2O8	Ru0.7Sn0.3Sr2Gd1Cu2O8	Ru	0.7	Sn	0.3	Sr	2	Gd	1	Cu	2											O	8			2003							106																					Ru1212																		K			11				11																																																																																															1	solid state reaction. SIN(1050C, 4d, in O2 flow) - cool to RT(45C/h)					<119>Sn Mossbauer spectroscopy in the magnetic superconductor (Ru, Sn)Sr2GdCu2O8			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, Urca, CEP, Rio de Janeiro, Brazil	Phys.Rev.B, 68(2003)134516	Ada,E.Baggio-Saitovitch,I.Souza Azevedo,J.E.Musa,Lopez,S.Garcia Garcia		
34225	MTL0573919	RESRT shows RES(250K). Curie-T shows ferromag-order of Ru, Tm, defined as FMR-onset-temperature.	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.4Ce0.6Cu2O10+z	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	10+z			2003							170																					Ru1222			A	3.8318		28.5325												K			45				45																																																																							mOhm.cm											11													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34226	MTL0573919	RESRT shows RES(250K). Curie-T shows ferromag-order of Ru, Tm, defined as FMR-onset-temperature.	(Ru,Pb)Sr2(Gd,Ce)2Cu2O10	Ru0.97Pb0.03Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.97	Pb	0.03	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z		1	2003							165																					Ru1222			A	3.8329		28.539												K			38				38																																																																							mOhm.cm											18													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34227	MTL0573919	RESRT shows RES(250K). Curie-T shows ferromag-order of Ru, Tm, defined as FMR-onset-temperature.	(Ru,Pb)Sr2(Gd,Ce)2Cu2O10	Ru0.8Pb0.2Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.8	Pb	0.2	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z		1	2003							160																					Ru1222			A	3.8405		28.5806												K			21				21																																																																							mOhm.cm											36													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34228	MTL0573919	RESRT shows RES(250K). Curie-T shows ferromag-order of Ru, Tm, defined as FMR-onset-temperature.	(Ru,Pb)Sr2(Gd,Ce)2Cu2O10	Ru0.6Pb0.4Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.6	Pb	0.4	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z		1	2003							150																					Ru1222			A	3.8416		28.5959												K			9.76				9.76																																																																							mOhm.cm											52													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34229	MTL0573919	RESRT shows RES(250K). Curie-T shows ferromag-order of Ru, Tm, defined as FMR-onset-temperature. Semiconductor-like.	(Ru,Pb)Sr2(Gd,Ce)2Cu2O10	Ru0.5Pb0.5Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.5	Pb	0.5	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z		1	2003							140																					Ru1222			A	3.8536		28.6314												K																																																																														mOhm.cm											56													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34230	PHC4000043	N2-ANN process is important for s/c. precise analysis of structure.	FeSr2YCu2O6	Fe1Sr2Y1Cu2O6+z	Fe	1	Sr	2	Y	1	Cu	2													O	6+z			2003																												Fe1212																		K				50			50																																																																																														Fe2O3,SrCO3,R2O3,CuO	1	mixture - CAL(900C,24h, in air) - SIN(1000C,24h, in air) - ANN(650C-850C,24h, in N2 flow + 300C,24h, in O2 flow) + 350C,24h, in 195 atm-O2)					Atomic ordering in FeSr2LnCu2O6+z  system (Ln = Nd, Y and Er)			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 400(2003)43-52	H.Fujii,I.Kakeya,J.Suzuki,K.Hirata,K.Kadowaki,K.Oikawa,T.Kamiyama,T.Mochiku,Y.Hata,Y.Nakano		
34231	PHC4000043	N2-ANN process is important for s/c. precise analysis of structure.	FeSr2NdCu2O6	Fe1Sr2Nd1Cu2O6+z	Fe	1	Sr	2	Nd	1	Cu	2													O	6+z			2003																												Fe1212																		K					4.2																																																																																																Fe2O3,SrCO3,R2O3,CuO	1	mixture - CAL(900C,24h, in air) - SIN(1000C,24h, in air) - ANN(650C-850C,24h, in N2 flow + 300C,24h, in O2 flow) + 350C,24h, in 195 atm-O2)					Atomic ordering in FeSr2LnCu2O6+z  system (Ln = Nd, Y and Er)			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 400(2003)43-52	H.Fujii,I.Kakeya,J.Suzuki,K.Hirata,K.Kadowaki,K.Oikawa,T.Kamiyama,T.Mochiku,Y.Hata,Y.Nakano		
34232	PHC4000043	N2-ANN process is important for s/c. precise analysis of structure.	FeSr2ErCu2O6	Fe1Sr2Er1Cu2O6+z	Fe	1	Sr	2	Er	1	Cu	2													O	6+z			2003																												Fe1212																		K				50			50																																																																																														Fe2O3,SrCO3,R2O3,CuO	1	mixture - CAL(900C,24h, in air) - SIN(1000C,24h, in air) - ANN(650C-850C,24h, in N2 flow + 300C,24h, in O2 flow) + 350C,24h, in 195 atm-O2)					Atomic ordering in FeSr2LnCu2O6+z  system (Ln = Nd, Y and Er)			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 400(2003)43-52	H.Fujii,I.Kakeya,J.Suzuki,K.Hirata,K.Kadowaki,K.Oikawa,T.Kamiyama,T.Mochiku,Y.Hata,Y.Nakano		
34233	PHC4000007	unknown phase  < 2%	(Ru,Mo)Sr2(Gd,Ce)2Cu2O10	Ru0.75Mo0.25Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.75	Mo	0.25	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z			2003																												Ru1222			A	3.8437		28.526												K	10		25				17.5																																																																																															1	solid state reaction					Synthesis, structure, superconducting and magnetic properties of (Ru<5+>1-xMo<6+>x)(Sr,Gd)2(Gd0.7Ce<4+>0.3)2Cu2O10-z (x=0.0, 0.25, 0.50, 0.75, 1.0)			Department of Solid State Physics and Chemistry, Lomonosov State Academy of Fine Chemical Technology, 86 Vernadsky Prosp., Moscow 119571, Russia	Physica C, 400(2003)7-18	A.S.Andreenko,A.Zalevski,G.M.Kuz'miicheva,I.E.Kostyleva,J.Warchulska		
34234	PHC4000007	impurity phases=15%-SrMoO4, 2%-CeO2, unknown phase < 2%.	(Ru,Mo)Sr2(Gd,Ce)2Cu2O10	Ru0.5Mo0.5Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.5	Mo	0.5	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z			2003																												Ru1222			A	3.8417		28.485												K	5		22				13.5																																																																																															1	solid state reaction					Synthesis, structure, superconducting and magnetic properties of (Ru<5+>1-xMo<6+>x)(Sr,Gd)2(Gd0.7Ce<4+>0.3)2Cu2O10-z (x=0.0, 0.25, 0.50, 0.75, 1.0)			Department of Solid State Physics and Chemistry, Lomonosov State Academy of Fine Chemical Technology, 86 Vernadsky Prosp., Moscow 119571, Russia	Physica C, 400(2003)7-18	A.S.Andreenko,A.Zalevski,G.M.Kuz'miicheva,I.E.Kostyleva,J.Warchulska		
34235	PHC4000007	2%-SrMoO4, unknown phase < 2%.	(Ru,Mo)Sr2(Gd,Ce)2Cu2O10	Ru0.25Mo0.75Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.25	Mo	0.75	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z			2003																												Ru1222			A	3.845		28.382												K					4.2																																																																																																	1	solid state reaction					Synthesis, structure, superconducting and magnetic properties of (Ru<5+>1-xMo<6+>x)(Sr,Gd)2(Gd0.7Ce<4+>0.3)2Cu2O10-z (x=0.0, 0.25, 0.50, 0.75, 1.0)			Department of Solid State Physics and Chemistry, Lomonosov State Academy of Fine Chemical Technology, 86 Vernadsky Prosp., Moscow 119571, Russia	Physica C, 400(2003)7-18	A.S.Andreenko,A.Zalevski,G.M.Kuz'miicheva,I.E.Kostyleva,J.Warchulska		
34236	PHC4000071		RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2003						2.89	133																					Ru1212				3.8399		11.5766												K		41					41																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34237	PHC4000071		(Ru,Ti)Sr2GdCu2O8	Ru0.99Ti0.01Sr2Gd1Cu2O8	Ru	0.99	Ti	0.01	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.08	131.6																					Ru1212				3.8378		11.5686												K		36.3					36.3																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34238	PHC4000071		(Ru,Ti)Sr2GdCu2O8	Ru0.97Ti0.03Sr2Gd1Cu2O8	Ru	0.97	Ti	0.03	Sr	2	Gd	1	Cu	2											O	8		1	2003						2.86	127.5																					Ru1212				3.8373		11.5683												K		40.3					40.3																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34239	PHC4000071		(Ru,Ti)Sr2GdCu2O8	Ru0.95Ti0.05Sr2Gd1Cu2O8	Ru	0.95	Ti	0.05	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.08	118																					Ru1212				3.8387		11.5649												K		32.2					32.2																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34240	PHC4000071		(Ru,Ti)Sr2GdCu2O8	Ru0.925Ti0.075Sr2Gd1Cu2O8	Ru	0.925	Ti	0.075	Sr	2	Gd	1	Cu	2											O	8		1	2003						2.75	114																					Ru1212				3.8386		11.5639												K		29.2					29.2																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34241	PHC4000071		(Ru,Rh)Sr2GdCu2O8	Ru0.95Rh0.05Sr2Gd1Cu2O8	Ru	0.95	Rh	0.05	Sr	2	Gd	1	Cu	2											O	8		1	2003						2.99	130																					Ru1212																				36.3					36.3																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34242	PHC4000071		(Ru,Rh)Sr2GdCu2O8	Ru0.925Rh0.075Sr2Gd1Cu2O8	Ru	0.925	Rh	0.075	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.03	125																					Ru1212																				29.8					29.8																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34243	PHC4000071		(Ru,Rh)Sr2GdCu2O8	Ru0.9Rh0.1Sr2Gd1Cu2O8	Ru	0.9	Rh	0.1	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.48	116																					Ru1212																				19.3					19.3																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34244	PHC4000071		(Ru,Rh)Sr2GdCu2O8	Ru0.8Rh0.2Sr2Gd1Cu2O8	Ru	0.8	Rh	0.2	Sr	2	Gd	1	Cu	2											O	8		1	2003						2.89	120																					Ru1212																				12.9					12.9																																																																																															1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34245	PHC4000071		(Ru,Rh)Sr2GdCu2O8	Ru0.85Rh0.15Sr2Gd1Cu2O8	Ru	0.85	Rh	0.15	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.14	112																					Ru1212																																																																																																																								1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34246	MTL0573919		(Ru,Pb)Sr2(Gd,Ce)2Cu2O10	Ru0.9Pb0.1Sr2Gd1.4Ce0.6Cu2O10+z	Ru	0.9	Pb	0.1	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	10+z		1	2003																												Ru1222																					29.1				29.1																																																																																		19													1	mixture - pellet - heat(1000C,36h, in air) - heat(1070C,60h, in flowing O2) - slow cool to RT					Effect of Pb doping on the superconducting and magnetic resonance properties of Ru-1222			Department of Materials Science and Engineering, Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, China	Materials Lett., 57(2003)3919	G.Li,L.Shi,S.J.Feng,X.-G.Li,X.D.Zhang,Y.Pu		
34247	PHC4000071		(Ru,Ti)Sr2GdCu2O8	Ru0.9Ti0.1Sr2Gd1Cu2O8	Ru	0.9	Ti	0.1	Sr	2	Gd	1	Cu	2											O	8		1	2003						3.31	127																					Ru1212																																																																																																																								1	mixture - CAL(930C, in air), heat(1020C,12h, in N2 or Ar) - pellet - heat(1040C,12h, in O2) - ANN(1060C,6d, in O2) - cool to RT(30C/h)					Structural, transport and magnetic properties of Ru1-xMxSr2GdCu2O8 (M=Ti and Rh for 0=< x =<0.2)			Experimentalphysik V, Elektronische Korrelation und Magnetismus, Universitat Augsburg, Universitae tsstrasse Augsburg, Germany	Physica C, 400(2003)71-80	A.Hassen,A.Krimmel,A.Loidl,J.Hemberger		
34250	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.98Na0.02Cu1O4	La	1.98	Na	0.02	Cu	1															O	4		1	2003																												T			A	5.3571	5.3969	13.1346												K					16																																																																																													RH34250					mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34251	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.95Na0.05Cu1O4	La	1.95	Na	0.05	Cu	1															O	4		1	2003																												T			A	5.3517	5.3989	13.1372												K					16																																																																																													RH34251					mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34252	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.9Na0.1Cu1O4	La	1.9	Na	0.1	Cu	1															O	4		1	2003								240																				T			A	5.3544	5.3982	13.1419												K					16																																																																																													RH34252					mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34253	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.85Na0.15Cu1O4	La	1.85	Na	0.15	Cu	1															O	4		1	2003																												T			A	5.3583	5.396	13.1473												K					16																																																																																													RH34253					mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34254	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.7Na0.3Cu1O4	La	1.7	Na	0.3	Cu	1															O	4		1	2003																												T			A	5.3522	5.3947	13.1423												K					16																																																																																																		mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34255	P068174505	insulator-like. hole not introduced into CuO2 plane.	(La,Na)2CuO4	La1.5Na0.5Cu1O4	La	1.5	Na	0.5	Cu	1															O	4		1	2003																												T			A	5.3548	5.3968	13.1397												K					16																																																																																																		mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34256	P068174505		(La,Sr,Na)2CuO4	La1.83Sr0.15Na0.02Cu1O4	La	1.83	Sr	0.15	Na	0.02	Cu	1													O	4		1	2003																												T			A	3.7899		13.1809												K				37			37																																																																						TP34256																										mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34257	P068174505		(La,Sr,Na)2CuO4	La1.8Sr0.15Na0.05Cu1O4	La	1.8	Sr	0.15	Na	0.05	Cu	1													O	4		1	2003																												T			A	3.7878		13.1995												K				37			37																																																																						TP34257																										mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34258	P068174505		(La,Sr,Na)2CuO4	La1.75Sr0.15Na0.1Cu1O4	La	1.75	Sr	0.15	Na	0.1	Cu	1													O	4		1	2003																												T			A	3.7776		13.1811												K				37			37																																																																																																mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34259	P068174505		(La,Sr,Na)2CuO4	La1.7Sr0.15Na0.15Cu1O4	La	1.7	Sr	0.15	Na	0.15	Cu	1													O	4		1	2003																												T			A	3.7751		13.1901												K				37			37																																																																																																mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34260	P068174505		(La,Sr,Na)2CuO4	La1.55Sr0.15Na0.3Cu1O4	La	1.55	Sr	0.15	Na	0.3	Cu	1													O	4		1	2003																												T			A	3.7655		13.2025												K				37			37																																																																																																mixture - pellet - heat(1100 - 1150C,48h,in O2)					Microstructure and the superconductivity in La2-x-ySrxNayCuO4 systems			1Structure Research Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 68(2003)174505	Changjin Zhang,Li Lu,Liwei Liu,Yuheng Zhang		
34261	P068180505	phase transformation (hexagonal to monoclinic) begins at about 0.15 GPa.	Na0.3CoO2:1.3H2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3			2003																		GPa		43																										K				4.8			4.8																																																																																																Na2S2O8 route method					Synthesis and high-pressure behavior of Na0.3CoO2: 1.3H2O and related phases			Physics Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 68(2003)180505	A.Moodenbaugh,S.Park,T.Vogt,Y.Lee		
34262	L091217001		Na0.3CoO2:1.4H2O	Na0.3Co1H2.8O3.4	Na	0.3	Co	1	H	2.8															O	3.4		1	2003																															A	2.823		19.696												K			4.5	4.5			4.5																																																					SP34262			mj/mol.K2	16.1																																					Na2CO3,Co3O4		See Nature 422(2003)53					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34263	L091217001		Na0.3CoO2:1.4D2O	Na0.3Co1D2.8O3.4	Na	0.3	Co	1	D	2.8															O	3.4		1	2003																															A	2.821		19.635												K			4.5	4.5			4.5																																																					SP34263			mj/mol.K2	16.4																																					Na2CO3,Co3O4		See Nature 422(2003)53					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34264	L091217001	not s/c.	Na0.6CoO2	Na0.6Co1O2	Na	0.6	Co	1																	O	2		1	2003																															A	2.837		10.878												K					5																																																																																																Na2CO3,Co3O4		See Nature 422(2003)53					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34265	L091217001	not s/c.	Na0.3CoO2:0.9H2O	Na0.3Co1H1.8O2.9	Na	0.3	Co	1	H	1.8															O	2.9		1	2003																															A	2.825		13.831												K					5																																																																																																Na2CO3,Co3O4		See Nature 422(2003)53					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34266	L091217001	not s/c.	Na0.3CoO2:1.8D2O	Na0.3Co1D3.6O3.8	Na	0.3	Co	1	D	3.6															O	3.8		1	2003																															A	2.823		19.66												K					5																																																																																																Na2CO3,Co3O4		See Nature 422(2003)53					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34267	L091217001	single crystal. resistivity minimum at T*=52K. large anisotropy, R<c>/R<ab>=1000.	Na0.3CoO2:1.3H2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3		3	2003																																														K			5				5																																																																																																floating zone and flux method					Observation of Bulk Superconductivity in NaxCoO2: yH2O and NaxCoO2: yD2O Powder and Single Crystals			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 91(2003)217001	B.C.Sales,D.Mandrus,P.Khalifah,R.Jin		
34268	JPS0723041	gap estimated by NQR fitting.	Na0.3CoO2:1.3H2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3		1	2003																																														K		4.7					4.7																																																3.5																																																					Unconventional Superconductivity and Nearly Ferromagnetic Spin Fluctuations in NaxCoO2: yH2O			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502	J.Phys.Soc.Jpn, 72(2003)3041	C.Michioka,E.Takayama-Muromachi,H.Sakurai,K.Ishida,K.Takada,K.Yoshimura,M.Kato,T.Sasaki,Y.Ihara,Y.Maeno		
34269	JPS0723254	ferromagnetism confirmed by ESR. 	RuSr2(Gd,Ce)2Cu2O10	Ru1Sr2Gd1.4Ce0.6Cu2O10	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	10		1	2003							180																					Ru1222			A	3.838		28.58												K		45					45																																																																																															1	2 wt % excess CuO was used.					Multiple Magnetic Transitions in RuSr2R1.4Ce0.6Cu2O10 (R = Gd, Eu) from Magnetization and ESR Spectroscopy			Department of Electronics and Computer Science, Tokyo University of Science, Yamaguchi, Daigaku-Dori 1-1-1, Onoda, Yamaguchi	J.Phys.Soc.Jpn, 72(2003)3254	H.Kojima,H.Shimizu,K.Yoshida		
34270	JPS0723254	ferromagnetism confirmed by ESR. paramag-Curie-T = 128 K from SUS.	RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.4Ce0.6Cu2O10	Ru	1	Sr	2	Eu	1.4	Ce	0.6	Cu	2											O	10		1	2003							180																					Ru1222			A	3.838		28.65												K		44					44																																																																																															1	2 wt % excess CuO was used.					Multiple Magnetic Transitions in RuSr2R1.4Ce0.6Cu2O10 (R = Gd, Eu) from Magnetization and ESR Spectroscopy			Department of Electronics and Computer Science, Tokyo University of Science, Yamaguchi, Daigaku-Dori 1-1-1, Onoda, Yamaguchi	J.Phys.Soc.Jpn, 72(2003)3254	H.Kojima,H.Shimizu,K.Yoshida		
34271	JPC0150L17	Tc(O<18>)=59.3K. penet not given. muon-SR. isotope effect for penet = 0.38.	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O6.942	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z	6.942	1	2003																												Y123																		K				60.6			60.6						0.22	O	78	-1.3																																																																																						1	standard solid state reaction. isotope exchange by heating in O2.					The oxygen-isotope effect on the in-plane penetration depth in underdoped Y1-xPrxBa2Cu3O7-z as revealed by muon-spin rotation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.:Condens.Matter 15(2003)L17-L23	A.Shengelaya,E.Morenzoni,H.Keller,I.M.Savie,K.Conder,R.Khasanov		
34272	JPC0150L17	Tc(O<18>)=43.6K. penet not given. muon-SR. isotope effect for penet = 0.71.	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.929	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.929	1	2003																												Y123																		K				45.3			45.3						0.37	O	78	-1.7																																																																																						1	standard solid state reaction. isotope exchange by heating in O2.					The oxygen-isotope effect on the in-plane penetration depth in underdoped Y1-xPrxBa2Cu3O7-z as revealed by muon-spin rotation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.:Condens.Matter 15(2003)L17-L23	A.Shengelaya,E.Morenzoni,H.Keller,I.M.Savie,K.Conder,R.Khasanov		
34273	JPC0150519	s/c properties are estimated from R(T), M-H curve. resistivity not zero at 1.8 K.	Na0.31CoO2:1.3H2O	Na0.31Co1H2.6O3.3	Na	0.31	Co	1	H	2.6															O	3.3		1	2003	emu/mole	0.0019					1.7																				7				A	2.824		19.68												K				4.3			4.3										9.2	Oe		13							kOe		100							kOe/K		34					A		57			A		7900			meV	0.5	2.71	14				SP34273			mj/mol.K2	15.9	specific heat	391	specific heat																																		Na2CO3,Co3O4		solid state reaction(1083K, in flowing O2). hydration by direct reaction with distilled water.					Superconductivity in a layered cobalt oxyhydrate Na0.31CoO2:1.3H2O			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter 15(2003)L519-L525	C.Feng,G.Cao,J.Shen,M.Fang,W.Lu,Yi Xu,Z.Xu		
34274	JPC0151693		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			2003																												T			A	3.775		13.22												K		35					35																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34275	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.85Sr0.15Cu0.99Ru0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ru	0.01													O	4			2003																												T			A	3.7803		13.2059												K		20.5					20.5																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34276	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.85Sr0.15Cu0.98Ru0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ru	0.02													O	4			2003																												T			A	3.7809		13.1935												K		10.8					10.8																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34277	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.85Sr0.15Cu0.97Ru0.03O4	La	1.85	Sr	0.15	Cu	0.97	Ru	0.03													O	4			2003																												T			A	3.7848		13.1891												K			10.8				10.8																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34279	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.83Sr0.17Cu0.99Ru0.01O4	La	1.83	Sr	0.17	Cu	0.99	Ru	0.01													O	4			2003																												T			A	3.775		13.2182												K		31.1					31.1																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34280	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.825Sr0.175Cu0.99Ru0.01O4	La	1.825	Sr	0.175	Cu	0.99	Ru	0.01													O	4			2003																												T																		K		29.6					29.6																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34281	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.82Sr0.18Cu0.99Ru0.01O4	La	1.82	Sr	0.18	Cu	0.99	Ru	0.01													O	4			2003																												T																		K		28.3					28.3																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34282	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.81Sr0.19Cu0.99Ru0.01O4	La	1.81	Sr	0.19	Cu	0.99	Ru	0.01													O	4			2003																												T																		K		26.5					26.5																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34283	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.79Sr0.21Cu0.99Ru0.01O4	La	1.79	Sr	0.21	Cu	0.99	Ru	0.01													O	4			2003																												T																		K		22.1					22.1																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34285	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.81Sr0.19Cu0.98Ru0.02O4	La	1.81	Sr	0.19	Cu	0.98	Ru	0.02													O	4			2003																												T																		K		13.5					13.5																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34286	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.805Sr0.195Cu0.98Ru0.02O4	La	1.805	Sr	0.195	Cu	0.98	Ru	0.02													O	4			2003																												T																		K		14.1					14.1																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34287	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.8Sr0.2Cu0.98Ru0.02O4	La	1.8	Sr	0.2	Cu	0.98	Ru	0.02													O	4			2003																												T																		K		15.6					15.6																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34288	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.795Sr0.205Cu0.98Ru0.02O4	La	1.795	Sr	0.205	Cu	0.98	Ru	0.02													O	4			2003																												T																		K		15.5					15.5																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34289	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.79Sr0.21Cu0.98Ru0.02O4	La	1.79	Sr	0.21	Cu	0.98	Ru	0.02													O	4			2003																												T																		K		11.2					11.2																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34291	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.79Sr0.21Cu0.97Ru0.03O4	La	1.79	Sr	0.21	Cu	0.97	Ru	0.03													O	4			2003																												T			A	3.7797		13.2138												K		14.8					14.8																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34292	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.78Sr0.22Cu0.97Ru0.03O4	La	1.78	Sr	0.22	Cu	0.97	Ru	0.03													O	4			2003																												T																		K		15.6					15.6																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34293	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.76Sr0.24Cu0.97Ru0.03O4	La	1.76	Sr	0.24	Cu	0.97	Ru	0.03													O	4			2003																												T																		K		16.1					16.1																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34294	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.75Sr0.25Cu0.97Ru0.03O4	La	1.75	Sr	0.25	Cu	0.97	Ru	0.03													O	4			2003																												T																		K		15.3					15.3																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34295	JPC0151693		(La,Sr)2(Cu,Ru)O4	La1.73Sr0.27Cu0.97Ru0.03O4	La	1.73	Sr	0.27	Cu	0.97	Ru	0.03													O	4			2003																												T																		K		14.1					14.1																																																																																															1	solid state reaction in Al2O3 (850C,24h), SIN(1150C, 48h)					Transport properties of Ru-doped La1.85Sr0.15CuO4 and the effect of carrier concentration compensation			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter 15(2003)1693	C.H.Wang,H.T.Zhang,L.Li,S.Y.Li,X.G.Luo,X.H.Chen,Y.M.Xiong		
34296	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.9Ca0.1Cu2O7+z	Co	1	Sr	2	Y	0.9	Ca	0.1	Cu	2											O	7+z		1	2003																												M1212			A	5.4027	5.4104	22.5269												K				15			15																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34297	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.8Ca0.2Cu2O7+z	Co	1	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	7+z		1	2003																												M1212			A	5.4031	5.4097	22.537												K				20			20																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34298	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.75Ca0.25Cu2O7+z	Co	1	Sr	2	Y	0.75	Ca	0.25	Cu	2											O	7+z		1	2003																												M1212																		K				30			30																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34299	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.7Ca0.3Cu2O7+z	Co	1	Sr	2	Y	0.7	Ca	0.3	Cu	2											O	7+z		1	2003																												M1212			A	5.3995	5.41	22.5319												K				40			40																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34300	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.65Ca0.35Cu2O7+z	Co	1	Sr	2	Y	0.65	Ca	0.35	Cu	2											O	7+z		1	2003																												M1212																		K				38			38																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34301	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.6Ca0.4Cu2O7+z	Co	1	Sr	2	Y	0.6	Ca	0.4	Cu	2											O	7+z		1	2003																												M1212			A	5.3973	5.4082	22.5689												K				34			34																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34302	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.55Ca0.45Cu2O7+z	Co	1	Sr	2	Y	0.55	Ca	0.45	Cu	2											O	7+z		1	2003																												M1212																		K				25			25																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34303	SSC1270493	as-prepared sample not s/c.	CoSr2(Y,Ca)Cu2O7	Co1Sr2Y0.5Ca0.5Cu2O7+z	Co	1	Sr	2	Y	0.5	Ca	0.5	Cu	2											O	7+z		1	2003																												M1212			A	5.3962	5.4068	22.6176												K				15			15																																																																																														Co3O4,SrCO3,Y2O3,CaCO3,CuO		mixture - CAL(975C,1000C). ANN(500C,30min, P=5GPa) using Ag2O as an oxygen source.					Superconductivity in CoSr2(Y1-xCax)Cu2O7+z			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 127(2003)493	H.Yamauchi,M.Karppinen,Y.Morita		
34304	SSC1280097	oxygen content by Rietveld analysis for 2125-structure. hole in sheet = 0.085.	(La,Pr)2CaBa2Cu5Oz	La1.9Pr0.1Ca0.2Ba2Cu4.2O9.8786	La	1.9	Pr	0.1	Ca	0.2	Ba	2	Cu	4.2											O	z	9.8786	1	2003																												2125	P4/mmm		A	3.8988		11.7235												K		25.5					25.5																																																																																														La2O3,BaCO3,CaCO3,CuO,Pr6O11		mixture - heat(930-940C,72h) - ANN(500C,24h, in O2) - slow cool to RT					Studies on La2-xPrxCayBa2Cu4+y (x = 0.1 - 0.5, y = 2x)  type mixed oxide superconductors			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun., 128(2003)97	C.M.Thaker,D.G.Kuberkar,D.S.Rana,K.R.Mavani,Manglesh Dixit,S.Bhattacharya,S.Rayaprol		
34305	SSC1280097	oxygen content by Rietveld analysis for 2125-structure. hole in sheet = 0.136.	(La,Pr)2CaBa2Cu5Oz	La1.8Pr0.2Ca0.4Ba2Cu4.4O10.7348	La	1.8	Pr	0.2	Ca	0.4	Ba	2	Cu	4.4											O	z	10.7348	1	2003																												2125	P4/mmm		A	3.8824		11.6698												K		35.4					35.4																																																																																														La2O3,BaCO3,CaCO3,CuO,Pr6O11		mixture - heat(930-940C,72h) - ANN(500C,24h, in O2) - slow cool to RT					Studies on La2-xPrxCayBa2Cu4+y (x = 0.1 - 0.5, y = 2x)  type mixed oxide superconductors			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun., 128(2003)97	C.M.Thaker,D.G.Kuberkar,D.S.Rana,K.R.Mavani,Manglesh Dixit,S.Bhattacharya,S.Rayaprol		
34306	SSC1280097	oxygen content by Rietveld analysis for 2125-structure. hole in sheet = 0.171.	(La,Pr)2CaBa2Cu5Oz	La1.7Pr0.3Ca0.6Ba2Cu4.6O10.8862	La	1.7	Pr	0.3	Ca	0.6	Ba	2	Cu	4.6											O	z	10.8862	1	2003																												2125	P4/mmm		A	3.8724		11.6417												K		47.6					47.6																																																																																														La2O3,BaCO3,CaCO3,CuO,Pr6O11		mixture - heat(930-940C,72h) - ANN(500C,24h, in O2) - slow cool to RT					Studies on La2-xPrxCayBa2Cu4+y (x = 0.1 - 0.5, y = 2x)  type mixed oxide superconductors			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun., 128(2003)97	C.M.Thaker,D.G.Kuberkar,D.S.Rana,K.R.Mavani,Manglesh Dixit,S.Bhattacharya,S.Rayaprol		
34307	SSC1280097	oxygen content by Rietveld analysis for 2125-structure. hole in sheet = 0.182.	(La,Pr)2CaBa2Cu5Oz	La1.6Pr0.4Ca0.8Ba2Cu4.8O11.1064	La	1.6	Pr	0.4	Ca	0.8	Ba	2	Cu	4.8											O	z	11.1064	1	2003																												2125	P4/mmm		A	3.865		11.6336												K		54					54																																																																																														La2O3,BaCO3,CaCO3,CuO,Pr6O11		mixture - heat(930-940C,72h) - ANN(500C,24h, in O2) - slow cool to RT					Studies on La2-xPrxCayBa2Cu4+y (x = 0.1 - 0.5, y = 2x)  type mixed oxide superconductors			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun., 128(2003)97	C.M.Thaker,D.G.Kuberkar,D.S.Rana,K.R.Mavani,Manglesh Dixit,S.Bhattacharya,S.Rayaprol		
34308	SSC1280097	oxygen content by Rietveld analysis for 2125-structure. hole in sheet = 0.185.	(La,Pr)2CaBa2Cu5Oz	La1.5Pr0.5Ca1Ba2Cu5O11.782	La	1.5	Pr	0.5	Ca	1	Ba	2	Cu	5											O	z	11.782	1	2003																												2125	P4/mmm		A	3.8712		11.6388												K		57.7					57.7																																																																																														La2O3,BaCO3,CaCO3,CuO,Pr6O11		mixture - heat(930-940C,72h) - ANN(500C,24h, in O2) - slow cool to RT					Studies on La2-xPrxCayBa2Cu4+y (x = 0.1 - 0.5, y = 2x)  type mixed oxide superconductors			Department of Physics, Saurashtra University, Rajkot 360 005, India	Solid State Commun., 128(2003)97	C.M.Thaker,D.G.Kuberkar,D.S.Rana,K.R.Mavani,Manglesh Dixit,S.Bhattacharya,S.Rayaprol		
34309	PRL0140305	carrier concentration determined from Hall effect. Tc by mutual inductance. Tc shows Tc(max)	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		3	1965																												ABO3																		K		0.58					0.58	TC34309																																																																																															reduction of single crystals					Dependence of the  superconducting transition temperature on carrier concentration in semiconducting SrTiO3			NBS	Phys.Rev.Lett., 14(1965)305	C.S.Koonce,E.Ambler,J.F.Schooley,J.H.Becker,M.L.Cohen,W.R.Hosler		
34310	EPJ0330025		SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		3	2003																												ABO3																		K		0.133					0.133																																		HC34310																																																														single crystal - polish. (111) surface. Mo pad by MBE. ANN(1150C,1h, P=1 E-8 mbar (vac))					Superconductivity of SrTiO3-z			Institute of Physics, Johannes Gutenberg University, 55099 Mainz, Germany	Eur.Phys.J.B, 33(2003)25	H.Adrian,M.Jourdan,N.Blumer		
34311	EPJ0330025		SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		3	2003																												ABO3																		K		0.214					0.214																																		HC34311																																																														single crystal - polish. (111) surface. Mo pad by MBE. ANN(1150C,1h, P=1 E-8 mbar (vac))					Superconductivity of SrTiO3-z			Institute of Physics, Johannes Gutenberg University, 55099 Mainz, Germany	Eur.Phys.J.B, 33(2003)25	H.Adrian,M.Jourdan,N.Blumer		
34312	P068214517	refined structure parameter by NED. Na, D2O content are precisely determined.	Na0.31CoO2:1.25D2O	Na0.31Co1D2.5O3.25	Na	0.31	Co	1	D	2.5															O	3.25			2003																															A	2.8216		19.7681												K		4.5					4.5																																																																																														Na0.61CoO2		using Br2 as oxidizer. then, deutoration.					Crystal structure of the sodium cobaltate deuterate superconductor NaxCoO2/4xD2O (x=1/3)			Materials Science Division, Argonne National Laboratory, Argonne Illinois 60439, USA	Phys.Rev.B, 68(2003)214517	D.G.Hinks,J.C.Burley,J.D.Jorgensen,M.Avdeev,S.Short		
34313	L089117001	RESN temp.= 3K.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												Sr2RuO4																		K	1.42						1.42																																																																							uOhm.cm							0.16																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34314	L089117001	Ti-content x=0.0005. RESN temp.= 3K.	Sr2(Ru,Ti)O4	Sr2Ru0.9995Ti0.0005O4	Sr	2	Ru	0.9995	Ti	0.0005															O	4		3	2002																												Sr2RuO4																		K	1.13						1.13																																																																							uOhm.cm							0.51																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34315	L089117001	RESN temp.= 3K.	Sr2(Ru,Ti)O4	Sr2Ru0.999Ti0.001O4	Sr	2	Ru	0.999	Ti	0.001															O	4		3	2002																												Sr2RuO4																		K	0.6						0.6																																																																							uOhm.cm							0.78																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34316	L089117001	Ti-content x=0.00125. RESN temp.= 3K.	Sr2(Ru,Ti)O4	Sr2Ru0.99875Ti0.00125O4	Sr	2	Ru	0.99875	Ti	0.00125															O	4		3	2002																												Sr2RuO4																		K	0.46						0.46																																																																							uOhm.cm							0.98																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34317	L089117001	RESN temp.= 3K.	Sr2(Ru,Ti)O4	Sr2Ru0.9975Ti0.0025O4	Sr	2	Ru	0.9975	Ti	0.0025															O	4		3	2002																												Sr2RuO4																		K					0.4																																																																									uOhm.cm							1.2																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34318	L089117001	RESN temp.= 3K.	Sr2(Ru,Ti)O4	Sr2Ru0.995Ti0.005O4	Sr	2	Ru	0.995	Ti	0.005															O	4		3	2002																												Sr2RuO4																		K					0.4																																																																									uOhm.cm							2.49																		floating zone.					Non-Fermi-Liquid Behavior in Sr2RuO4 with Nonmagnetic Impurities			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 89(2002)117001	N.Kikugawa,Y.Maeno		
34319	MTL0370068	not s/c.  hole conc. = 0.299. DENS is X-ray density.	La2Ba2Cu4Oz	La2Ba2Cu4O11.69	La	2	Ba	2	Cu	4															O	z	11.69	1	1998									5.546																			2125			A	3.897		11.748												K																																																																																																							adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34320	MTL0370068	tetragonal triple perovskite. hole conc. = 0.309. DENS is X-ray density.	(La,Y)2Ba2CaCu5Oz	La1.9Y0.1Ba2Ca0.2Cu4.2O11.72	La	1.9	Y	0.1	Ba	2	Ca	0.2	Cu	4.2											O	z	11.72	1	1998									5.696																			2125			A	3.88		11.73												K					21																																																																																																		adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34321	MTL0370068	tetragonal triple perovskite. hole conc. = 0.321. DENS is X-ray density.	(La,Y)2Ba2CaCu5Oz	La1.8Y0.2Ba2Ca0.4Cu4.4O11.77	La	1.8	Y	0.2	Ba	2	Ca	0.4	Cu	4.4											O	z	11.77	1	1998									5.862																			2125			A	3.864		11.681												K					43																																																																																																		adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34322	MTL0370068	tetragonal triple perovskite. hole conc. = 0.348. DENS is X-ray density.	(La,Y)2Ba2CaCu5Oz	La1.7Y0.3Ba2Ca0.6Cu4.6O11.85	La	1.7	Y	0.3	Ba	2	Ca	0.6	Cu	4.6											O	z	11.85	1	1998									5.995																			2125			A	3.857		11.654												K					67																																																																																																		adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34323	MTL0370068	tetragonal triple perovskite. hole conc. = 0.349. DENS is X-ray density.	(La,Y)2Ba2CaCu5Oz	La1.6Y0.4Ba2Ca0.8Cu4.8O11.86	La	1.6	Y	0.4	Ba	2	Ca	0.8	Cu	4.8											O	z	11.86	1	1998									6.107																			2125			A	3.852		11.64												K					78																																																																																																		adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34324	MTL0370068	tetragonal triple perovskite. hole conc. = 0.347. DENS is X-ray density.	(La,Y)2Ba2CaCu5Oz	La1.5Y0.5Ba2Ca1Cu5O11.86	La	1.5	Y	0.5	Ba	2	Ca	1	Cu	5											O	z	11.86	1	1998									6.269																			2125			A	3.834		11.619												K					78																																																																																																		adding CaO,CuO to La2Ba2Cu4. SIN(950C,12h, in O2) - ANN(500C,24h, in O2 flow)					Superconductivity in (La2-xYx)Ba2(CayCu4+y)Oz system			Department of Physics, Saurashtra University, Rajkot 360 005, India	Materials Lett., 37(1998)68	A.G.Joshi,D.G.Kuberkar,M.V.Subbarao,N.A.Shah,R.G.Kulkarni		
34325	PHC3910319	Hirr(0) = 46.9 T from fitting curve, Hirr(T)=Hirr(0)(1-t)^n. Jc(5K,4T) = 0.7 E+6 A/cm2. 	(Sr,Gd)CuO2	Sr0.9Gd0.1Cu1O2	Sr	0.9	Gd	0.1	Cu	1															O	2		1	2003																												IL			A	3.9348		3.3838												K				43			43										100																								HIR34325																																																														high pressure synthesis (6 GPa, 1000C, 2h) - Q to RT - ANN(500-600C, 3h)					Effect of the magnetic moments of Gd on the superconductivity in the infinite-layer superconductor Sr0.9Gd0.1CuO2			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, South Korea	Physica C, 391(2003)319	C.U.Jung,J.Y.Kim,Mun-Seog Kim,Sung-Ik Lee		
34326	L088227002	gap = 13.0 +- 1.0 meV at 4.2 K by STM	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2002																												IL	P4/mmm																	K				43			43										100																																				meV	13	7.03	11																																															See Physica C 366(2002)299					Strongly Correlated s-Wave Superconductivity in the N-Type Infinite-Layer Cuprate			Department of Physics, California Institute of Technology, Pasadena, California 91125	Phys.Rev.Lett., 88(2002)227002	C.-T.Chen,C.U.Jung,Heon-Jung Kim,J.Y.Kim,L.D.Bell,Min-Seok Park,N.-C.Yeh,P.Seneor,R.P.Vasquez,Sung-Ik Lee		
34327	P069014507	no-oxygenation	CuBaSrYCu2O7	Ba1Sr1Y1Cu3O7+z	Ba	1	Sr	1	Y	1	Cu	3													O	7+z		1	2004																											3	Y123			A	3.7864	3.8542	11.557												K	82.7						82.7																																																																																																no-oxygenation					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34328	P069014507	no-oxygenation	(Fe,Cu)BaSrYCu2O7	Fe0.1Ba1Sr1Y1Cu2.9O7+z	Fe	0.1	Ba	1	Sr	1	Y	1	Cu	2.9											O	7+z		1	2004																											3	Y123			A	3.8218	3.8448	11.5386												K	46.6						46.6																																																																																																no-oxygenation					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34329	P069014507	no-oxygenation	(Fe,Cu)BaSrYCu2O7	Fe0.2Ba1Sr1Y1Cu2.8O7+z	Fe	0.2	Ba	1	Sr	1	Y	1	Cu	2.8											O	7+z		1	2004																											2	Y123			A	3.8282		11.5467												K	36.1						36.1																																																																																																no-oxygenation					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34330	P069014507	no-oxygenation	(Fe,Cu)BaSrYCu2O7	Fe0.3Ba1Sr1Y1Cu2.7O7+z	Fe	0.3	Ba	1	Sr	1	Y	1	Cu	2.7											O	7+z		1	2004																											2	Y123			A	3.832		11.5254												K	7.8						7.8																																																																																																no-oxygenation					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34331	P069014507	no-oxygenation. not s/c.	(Fe,Cu)BaSrYCu2O7	Fe0.35Ba1Sr1Y1Cu2.65O7+z	Fe	0.35	Ba	1	Sr	1	Y	1	Cu	2.65											O	7+z		1	2004																											2	Y123			A	3.8355		11.5271												K					4.2																																																																																																		no-oxygenation					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34332	P069014507		(Fe0.5,Cu0.5)Ba2YCu2O7	Fe0.5Ba2Y1Cu2.5O7+z	Fe	0.5	Ba	2	Y	1	Cu	2.5													O	7+z		1	2004																											2	Y123			A	3.87		11.601												K	63		83				73																																																																																																mixture - CAL(925C,60h) - pettet - CAL(925C,60h) - cool to RT(30C/h) - oxygenate(1000C,0.5h, 5wt% KClO4, P=6GPa)					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34333	P069014507		(Fe0.5,Cu0.5)(Ba,Sr)2YCu2O7	Fe0.5Sr2Y1Cu2.5O7+z	Fe	0.5	Sr	2	Y	1	Cu	2.5													O	7+z		1	2004																											2	Y123			A	3.859		11.602												K			77				77																																																																																																mixture - CAL(925C,60h) - pettet - CAL(925C,60h) - cool to RT(30C/h) - oxygenate(1000C,0.5h, 5wt% KClO4, P=6GPa)					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34334	P069014507	As increasing annealing temperature (210-500C), s/c volume fraction decreases.	(Fe0.5,Cu0.5)(Ba,Sr)2YCu2O7	Fe0.5Ba1Sr1Y1Cu2.5O7.35	Fe	0.5	Ba	1	Sr	1	Y	1	Cu	2.5											O	7+z	7.35	1	2004																											2	Y123			A	3.838		11.5211												K				60			60										55																																																																																						mixture - CAL(925C,60h) - pettet - CAL(925C,60h) - cool to RT(30C/h) - oxygenate(1000C,0.5h, 5wt% KClO4, P=6GPa)					Fe0.5Cu0.5(Ba1-xSrx)2YCu2O7+z (x=0, 0.5, and 1)  superconductors prepared by high-pressure synthesis			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 69(2004)14507	C.Dong,G.C.Che,H.Chen,S.L.Jia,Y.M.Ni,Z.A.Ren,Z.X.Zhao		
34335	P069024512	ANN(1030C) sample. AF ordering due to Mo-sublattice. 	MoSr2YCu2Oz	Mo1Sr2Y1Cu2O7+z	Mo	1	Sr	2	Y	1	Cu	2													O	7+z			2004																												1212			A	3.811		11.52												K				18			18																																																6.8	11																																													Y2O3,SrCO3,Mo,CuO		mixture - heat(750C,1d) - SIN(conventional method)					Tuning the superconducting state in the magnetic MoSr2YCu2O8-z materials			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B, 69(2004)24512	E.Galstyan,I.Felner		
34336	P069024512	ANN(in 92 atm O2)	MoSr2YCu2Oz	Mo1Sr2Y1Cu2O7+z	Mo	1	Sr	2	Y	1	Cu	2													O	7+z			2004								16																				1212																		K				32			32																																																																																														Y2O3,SrCO3,Mo,CuO		mixture - heat(750C,1d) - SIN(conventional method)					Tuning the superconducting state in the magnetic MoSr2YCu2O8-z materials			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B, 69(2004)24512	E.Galstyan,I.Felner		
34337	P069024517	muon-SR shows 3 magnetic order points of 200K(AF order of Ru), 95K(unknown), 77.6K(weak ferro of Ru). s/c gives no effect tomagnetic order.	(Eu,Ce)2RuSr2Cu2O10	Eu1.4Ce0.6Ru1Sr2Cu2O10	Eu	1.4	Ce	0.6	Ru	1	Sr	2	Cu	2											O	10			2004							77.6	200																				Ru1222			A	3.846		28.72												K	22	40	43				40																																																																																															1	mixture - heat(1000C,1d,in flowing O2) - SIN(1050C,72h, in 1.1 atm O2) - FC.					Coexistence of magnetism and superconductivity in Eu1.4Ce0.6RuSr2Cu2O10 : A muon spin rotation and magnetization study			1Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B, 69(2004)24517	A.Shengelaya,D.G.Eshchenko,H.Kekker,I.Felner,I.M.Savic,K.A.Muller,R.Khasanov,U.Asaf		
34340	PHC4020317		(Sr,Pr)CuO2	Sr0.9Pr0.1Cu1O2	Sr	0.9	Pr	0.1	Cu	1															O	2		1	2004																												IL			A	3.9386		3.4044												K				41.5			41.5			K/GPa	-0.75																																																																																										SrCuO2,RCuO2		wrapped in Pt-foil, high pressure synthesis (9GPa, 1000C) - Q to RT					Superconducting magnetization and pressure effect on Tc in the infinite-layer high-Tc superconductors			Nuclear Reactor Research Department, Russian Academy of Sciences, Institute for Metal Physics, Ekaterinburg, Russia	Physica C, 402(2004)317	A.Mirmelstein,A.Podlesnyak,E.Khlybov,E.Mitberg,N.Mushnikov,V.Bobrovskii,V.Kazantsev		
34341	PHC4020317	c-axis aligned powder in epoxy.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2004																												IL			A	3.9423		3.4148												K				41.9			41.9																				T				18.2					T/K				0.62			A			42																																																							SrCuO2,RCuO2		wrapped in Pt-foil, high pressure synthesis (9GPa, 1000C) - Q to RT					Superconducting magnetization and pressure effect on Tc in the infinite-layer high-Tc superconductors			Nuclear Reactor Research Department, Russian Academy of Sciences, Institute for Metal Physics, Ekaterinburg, Russia	Physica C, 402(2004)317	A.Mirmelstein,A.Podlesnyak,E.Khlybov,E.Mitberg,N.Mushnikov,V.Bobrovskii,V.Kazantsev		
34342	PHC4020027	beta in SP = 3E-4 mj/mol.K4.  delta-C/gamma*Tc = 0.85	NaxCoO2/yH2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3			2004																																														K				4.2			4.2																																																								mj/mol.K2	12.2																																							deintercalate Na from Na0.7CoO2 by Br.					Specific heat study of the Na0.3CoO2:1.3H2O superconductor: influence of the complex chemistry			Department of Physics and Materials Research Institute, Pennsylvania State University, University Park, PA 16802, USA	Physica C, 402(2004)27	B.G.Ueland,M.L.Foo,P.Schiffer,R.E.Schaak,R.J.Cava,V.L.Miller		
34343	NAT4240527	during deintercalation process, Br-content = 0.5. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.45Co1H2.6O3.3	Na	0.45	Co	1	H	2.6															O	3.3			2003																															A															K				2			2																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34344	NAT4240527	during deintercalation process, Br-content = 1.0. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.4Co1H2.6O3.3	Na	0.4	Co	1	H	2.6															O	3.3			2003																															A	2.823		19.43												K				2			2																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34345	NAT4240527	during deintercalation process, Br-content = 10. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.32Co1H2.6O3.3	Na	0.32	Co	1	H	2.6															O	3.3			2003																															A	2.825		19.52												K				2.1			2.1																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34346	NAT4240527	during deintercalation process, Br-content = 20. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.33Co1H2.6O3.3	Na	0.33	Co	1	H	2.6															O	3.3			2003																															A	2.823		19.58												K				2.2			2.2																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34347	NAT4240527	during deintercalation process, Br-content = 30. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.32Co1H2.6O3.3	Na	0.32	Co	1	H	2.6															O	3.3			2003																															A	2.822		19.58												K				3			3																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34348	NAT4240527	during deintercalation process, Br-content = 40. Na-content by ICP-AES.	NaxCoO2/yH2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3			2003																															A	2.823		19.69												K				4.3			4.3																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34349	NAT4240527	during deintercalation process, Br-content = 100. Na-content by ICP-AES. two phases.	NaxCoO2/yH2O	Na0.29Co1H2.6O3.3	Na	0.29	Co	1	H	2.6															O	3.3			2003																															A	2.819		19.77												K				4			4																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34350	NAT4240527	during deintercalation process, Br-content = 50. Na-content by ICP-AES. two phases.	NaxCoO2/yH2O	Na0.26Co1H2.6O3.3	Na	0.26	Co	1	H	2.6															O	3.3			2003																															A	2.821		19.77												K				2.4			2.4																																																																																																					Superconductivity phase diagram of NaxCoO2-1.3H2O			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Nature, 424(2003)527	M.L.Foo,R.E.Schaak,R.J.Cava,T.Klimczuk		
34351	PHC4020152	impurity phase = HgO	Hg2Ba2YCu2O8	Hg2Ba2Y1Cu2O8-z	Hg	2	Ba	2	Y	1	Cu	2													O	8-z			2004																												Hg2212			A	3.8719		28.905												K				0			0																																																																																																high pressure synthesis (3.5 GPa, 1050C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34352	PHC4020152	impurity phase = (Hg,Sr)O, CuO	Hg2BaSrYCu2O8	Hg2Ba1Sr1Y1Cu2O8-z	Hg	2	Ba	1	Sr	1	Y	1	Cu	2											O	8-z			2004																												Hg2212			A	3.8327		28.422												K				32			32																																																																																																high pressure synthesis (3.5 GPa, 1050C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34353	PHC4020152	impurity phase = (Hg,Sr)O, CuO	Hg2Sr2YCu2O8	Hg2Sr2Y1Cu2O8-z	Hg	2	Sr	2	Y	1	Cu	2													O	8-z			2004																												Hg2212			A	3.8108		28.141												K				42			42																																																																																																high pressure synthesis (3.5 GPa, 1050C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34354	PHC4020152	impurity phase = HgO	Hg2Ba2(Y,Ca)Cu2O8	Hg2Ba2Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	2	Y	0.8	Ca	0.2	Cu	2											O	8-z			2004																												Hg2212			A	3.8589		28.918												K				21			21																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34355	PHC4020152		Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.9Sr0.1Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.9	Sr	0.1	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8546		28.873												K				27			27																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34356	PHC4020152		Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.8Sr0.2Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.8	Sr	0.2	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8514		28.846												K				32.5			32.5																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34357	PHC4020152		Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.7Sr0.3Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.7	Sr	0.3	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8477		28.806												K				39.5			39.5																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34358	PHC4020152		Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.6Sr0.4Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.6	Sr	0.4	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8454		28.763												K				38.5			38.5																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34359	PHC4020152		Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.5Sr0.5Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.5	Sr	0.5	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8425		28.733												K				41			41																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34360	PHC4020152	impurity phase = (Hg,Sr)O	Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba1.2Sr0.8Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	1.2	Sr	0.8	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8333		28.575												K				51			51																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34361	PHC4020152	impurity phase = (Hg,Sr)O	Hg2(Ba,Sr)2(Y,Ca)Cu2O8	Hg2Ba0.6Sr1.4Y0.8Ca0.2Cu2O8-z	Hg	2	Ba	0.6	Sr	1.4	Y	0.8	Ca	0.2	Cu	2									O	8-z			2004																												Hg2212			A	3.8134		28.302												K				60			60																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34362	PHC4020152	impurity phase = (Hg,Sr)O	Hg2Sr2(Y,Ca)Cu2O8	Hg2Sr2Y0.8Ca0.2Cu2O8-z	Hg	2	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	8-z			2004																												Hg2212			A	3.8039		28.107												K				58			58																																																																																																high pressure synthesis (3.5 GPa, 950C)					Enhancement of Tc by Sr substitution for Ba in Hg-2212 superconductor			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	Physica C, 402(2004)152	P.Odier,P.Toulemonde		
34363	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.94Ce0.06Cu1O4	Sm	1.94	Ce	0.06	Cu	1															O	4		1	2004																												T'																																																																																															TP34363																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34364	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.91Ce0.09Cu1O4	Sm	1.91	Ce	0.09	Cu	1															O	4		1	2004																												T'																																																																																															TP34364																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34365	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.89Ce0.11Cu1O4	Sm	1.89	Ce	0.11	Cu	1															O	4		1	2004																												T'																																																																																															TP34365																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34366	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.87Ce0.13Cu1O4	Sm	1.87	Ce	0.13	Cu	1															O	4		1	2004																												T'																																																																																															TP34366																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34367	PHC4030203		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4		3	2004																												T'																		K				18.6			18.6																																																																						TP34367																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34368	PHC4030203		(Sm,Ce)2CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4		1	2004																												T'																		K				15.7			15.7																																																																						TP34368																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34369	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.83Ce0.17Cu1O4	Sm	1.83	Ce	0.17	Cu	1															O	4		1	2004																												T'																																																																																															TP34369																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34370	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.81Ce0.19Cu1O4	Sm	1.81	Ce	0.19	Cu	1															O	4		1	2004																												T'																																																																																															TP34370																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34371	PHC4030203	Tc not given	(Sm,Ce)2CuO4	Sm1.79Ce0.21Cu1O4	Sm	1.79	Ce	0.21	Cu	1															O	4		1	2004																												T'																																																																																															TP34371																								Sm2O3,CeO2,CuO	1	standard solid state reaction					Anomalous thermopower of the electron-doped superconductor, Sm2-xCexCuO4			Structure Research Laboratory, Physics Department, University of Science and Technology of China, Hefei, Anhui, PR China	Physica C, 403(2004)203	H.S.Yang,J.Liu,L.Z.Cao,L.Zhang,M.D.Li,M.Yu,P.C.Li,Y.S.Chai		
34372	PHC4020303	impurity phase: Ca2PbO4. Tc1= 98 K and 93 K for nd-laser irradiation sample, 10 W/cm2 60 min, and 20 W/cm2 120 min, respectively.	(Bi,Nd,Tb,Pb)2Sr2Ca2Cu3O10	Bi0.8Nd0.1Tb0.1Pb1Sr2Ca2Cu3O10	Bi	0.8	Nd	0.1	Tb	0.1	Pb	1	Sr	2	Ca	2	Cu	3							O	10		1	2004																												Bi2223			A	3.6891		35.3162												K	108	115	117				115																																																																																															1	final ANN(500C, 20h, in O2 flow)					High energy Nd-laser irradiation effect on optimally co-doped terbium-neodymium BPSCCO bismuth cuprate superconductor			Department of Chemistry, HTc-Ceramic Superconductors Unit, Faculty of Science, Tanta University, Tanta, Egypt	Physica C, 402(2004)303	Khaled M.Elsabawy,Morsy M.A.Sekkina		
34373	PHC4030177	remanent = 0.15 m< B >. 	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2004							136																					Ru1212			A	3.8396		11.576												K	28		46				37																																																																																														SrCO3,Gd2O3,CuO,RuO2,Co2O3	1	mixture - CAL(900C,12h,in air) - heat(1010C,15h, in N2) - heat(1040C, 1050, 1060C, in flowing O2)					Effect of Co substitution on superconductivity and magnetic order in RuSr2GdCu2O8			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, PR China	Physica C, 403(2004)177	F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu		
34374	PHC4030177	remanent = 0.22 m< B >. 	(Ru,Co)Sr2GdCu2O8	Ru0.99Co0.01Sr2Gd1Cu2O8	Ru	0.99	Co	0.01	Sr	2	Gd	1	Cu	2											O	8		1	2004																												Ru1212			A	3.8393		11.5729												K	10		41				25.5																																																																																														SrCO3,Gd2O3,CuO,RuO2,Co2O3	1	mixture - CAL(900C,12h,in air) - heat(1010C,15h, in N2) - heat(1040C, 1050, 1060C, in flowing O2)					Effect of Co substitution on superconductivity and magnetic order in RuSr2GdCu2O8			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, PR China	Physica C, 403(2004)177	F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu		
34375	PHC4030177	R is not zero at 5K. remanent = 0.32 m< B >.	(Ru,Co)Sr2GdCu2O8	Ru0.97Co0.03Sr2Gd1CuO8	Ru	0.97	Co	0.03	Sr	2	Gd	1	Cu												O	8		1	2004																												Ru1212			A	3.8398		11.5709												K		13	34		5		13																																																																																														SrCO3,Gd2O3,CuO,RuO2,Co2O3	1	mixture - CAL(900C,12h,in air) - heat(1010C,15h, in N2) - heat(1040C, 1050, 1060C, in flowing O2)					Effect of Co substitution on superconductivity and magnetic order in RuSr2GdCu2O8			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, PR China	Physica C, 403(2004)177	F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu		
34376	PHC4030177	R is not zero at 5K. remanent = 0.44 m< B >.	(Ru,Co)Sr2GdCu2O8	Ru0.95Co0.05Sr2Gd1CuO8	Ru	0.95	Co	0.05	Sr	2	Gd	1	Cu												O	8		1	2004																												Ru1212			A	3.84		11.5675												K		5.5	21		5		5.5																																																																																														SrCO3,Gd2O3,CuO,RuO2,Co2O3	1	mixture - CAL(900C,12h,in air) - heat(1010C,15h, in N2) - heat(1040C, 1050, 1060C, in flowing O2)					Effect of Co substitution on superconductivity and magnetic order in RuSr2GdCu2O8			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, PR China	Physica C, 403(2004)177	F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu		
34377	PHC4030200	absolute value of PENET not given. PENET measured using LC resonator. gap obtained by s-wave fitting to PENET(T).	(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	2004																												BKBO																		K		31					31																																																3.53																																																electro-chemical method					Temperature dependence of magnetic penetration depth in B1-xKxBiO3 superconductor			Department of Physics and Astronomy and USC NanoCenter, University of South Carolina, Columbia, SC 29208, USA	Physica C, 403(2004)200	A.Snezhko,R.Prozorov		
34378	PHC3410729	Jc(5K,0 T) = 1.5 E+5 A/cm2. DENS is x-ray density.	(Ba,K)BiO3	Ba0.63K0.37Bi1O3	Ba	0.63	K	0.37	Bi	1															O	3		3	2000									8																			BKBO																		K				31			31											Oe		750			750			5																																																																													electro-chemical method					Observation of a linear temperature dependence of the critical current density in a Ba0.63K0.37Bi03 single crystal			Telecom. Basic Research Lab., ETHI, Taejon 305350, Korea	Physica C, 341(2000)729	Bong-Jun Kim,Hyun-Tak Kim,J.W.Hodby,Kang,Kwang-Yong,W.Schmidbauer,Y.C.Kim		
34379	P069094506		YBa2(Cu,Co)3O7	Y1Ba2Cu2.96Co0.04O7	Y	1	Ba	2	Cu	2.96	Co	0.04													O	z	7	1	2004																												Y123			A															K		91.5					91.5																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34380	P069094506		YBa2(Cu,Co)3O7	Y1Ba2Cu2.94Co0.06O7	Y	1	Ba	2	Cu	2.94	Co	0.06													O	z	7	1	2004																												Y123			A	3.8375	3.8815	11.7												K		78.3					78.3																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34381	P069094506		YBa2(Cu,Co)3O7	Y1Ba2Cu2.88Co0.12O7	Y	1	Ba	2	Cu	2.88	Co	0.12													O	z	7	1	2004																												Y123			A	3.8681		11.699												K		71					71																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34382	P069094506		YBa2(Cu,Co)3O7	Y1Ba2Cu2.76Co0.24O6.999	Y	1	Ba	2	Cu	2.76	Co	0.24													O	z	6.999	1	2004																												Y123			A	3.8724		11.697												K		50.7					50.7																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34383	P069094506		YBa2(Cu,Co)3O7	Y1Ba2Cu2.64Co0.36O7.03	Y	1	Ba	2	Cu	2.64	Co	0.36													O	z	7.03	1	2004																												Y123			A	3.8795		11.693												K		22					22																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34384	P069094506	no long range magnetic order down to 1.4 K.	YBa2(Cu,Co)3O7	Y1Ba2Cu2.58Co0.42O7.019	Y	1	Ba	2	Cu	2.58	Co	0.42													O	z	7.019	1	2004																												Y123																		K		0					0																																																																																															1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34385	P069094506	not s/c	YBa2(Cu,Co)3O7	Y1Ba2Cu2.52Co0.48O7.051	Y	1	Ba	2	Cu	2.52	Co	0.48													O	z	7.051	1	2004								102.9																				Y123																		K					4.2																																																																																																	1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34386	P069094506	not s/c	YBa2(Cu,Co)3O7	Y1Ba2Cu2.4Co0.6O7.07	Y	1	Ba	2	Cu	2.4	Co	0.6													O	z	7.07	1	2004								314.5																				Y123			A	3.8896		11.6889												K					4.2																																																																																																	1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34387	P069094506	not s/c	YBa2(Cu,Co)3O7	Y1Ba2Cu2.28Co0.72O7.1	Y	1	Ba	2	Cu	2.28	Co	0.72													O	z	7.1	1	2004								372.5																				Y123			A	3.8899		11.6799												K					4.2																																																																																																	1	standard solid state reaction method. ANN(350C, in O2)					Long- and short-range magnetic order, charge transfer, and superconductivity in YBa2Cu3-xCoxO7			Laboratoire des Solides Irradies, Ecole Polytechnique, 91128 Palaiseau, France	Phys.Rev.B, 69(2004)94506	A.Forget,F.Maury,I.Mirebeau,J.A.Hodges,P.Bourges,Y.Sidis		
34390	P066020501	Tc from neutron depolarization. commensurate AF observed by elastic neutron scattering.	YBa2(Cu,Co)3O7	Y1Ba2Cu2.961Co0.039O7+z	Y	1	Ba	2	Cu	2.961	Co	0.039													O	7+z			2002					myu-B/mol	0.14		330																				Y123																		K		93					93																																																																																																top-seeded melt texturing method					Antiferromagnetic ordering in a 90 K copper oxide superconductor			DRECAM-SPEC, CE-Saclay, 91191 Gif sur Yvette, France	Phys.Rev.B, 66(2002)20501	I.Mirebeau,J.A.Hodges,M.Hennion,P.Bourges,X.Chaud,Y.Sidis		
34391	P069104506		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4	4	1	2004																												T			A	3.7715		13.2132												K																																																																									uV/K	22.3																												1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34392	P069104506		(La,Sr)2(Cu,Fe)O4	La1.75Sr0.25Cu0.9Fe0.1O4	La	1.75	Sr	0.25	Cu	0.9	Fe	0.1													O	4	4	1	2004																												T			A	3.7831		13.1711												K					10																																																																				uV/K	18.1																												1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34393	P069104506	activation energy=5.85 (from RES), 2.06 meV (from TP).	(La,Sr)2(Cu,Fe)O4	La1.65Sr0.35Cu0.8Fe0.2O4	La	1.65	Sr	0.35	Cu	0.8	Fe	0.2													O	4	4	1	2004																												T			A	3.7894		13.1719												K					10																																																																				uV/K	18			TP34393																									1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34394	P069104506	activation energy=15.1 (from RES), 1.38 meV (from TP).	(La,Sr)2(Cu,Fe)O4	La1.55Sr0.45Cu0.7Fe0.3O4	La	1.55	Sr	0.45	Cu	0.7	Fe	0.3													O	4	4	1	2004																												T			A	3.7979		13.1094												K					10																																																																				uV/K	19.1																												1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34395	P069104506	activation energy=23.7 (from RES), 2.41 meV (from TP).	(La,Sr)2(Cu,Fe)O4	La1.45Sr0.55Cu0.6Fe0.4O4	La	1.45	Sr	0.55	Cu	0.6	Fe	0.4													O	4	4	1	2004																												T			A	3.8131		13.0532												K					10																																																																				uV/K	21.1																												1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34396	P069104506	TP300 represent TP(290K). activation energy=42.0. 	(La,Sr)2(Cu,Fe)O4	La1.35Sr0.65Cu0.6Fe0.5O4	La	1.35	Sr	0.65	Cu	0.6	Fe	0.5													O	4	4	1	2004																												T			A	3.8251		13.0191												K					10																																																																																																	1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34397	P069104506	TP300 represent TP(290K). activation energy=64.0 (from RES), 2.75 meV (from TP).	(La,Sr)2(Cu,Fe)O4	La1.25Sr0.75Cu0.6Fe0.6O4	La	1.25	Sr	0.75	Cu	0.6	Fe	0.6													O	4	4	1	2004																												T			A	3.8329		12.9465												K					10																																																																				uV/K	25.7																												1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34398	P069104506	TP300 represent TP(290K). activation energy=124.5 (from RES), 12.0 meV (from TP).	(La,Sr)2(Cu,Fe)O4	La1.05Sr0.95Cu0.6Fe0.8O4	La	1.05	Sr	0.95	Cu	0.6	Fe	0.8													O	4	4	1	2004																												T			A	3.8535		12.8461												K					10																																																																				uV/K	52.2			TP34398																									1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34399	P069104506		(La,Sr)2FeO4	La0.85Sr1.15Fe1O3.94	La	0.85	Sr	1.15	Fe	1															O	4	3.94		2004																												T			A	3.8596		12.75												K					10																																																																																																	1	standard solid state reaction method					Transport properties and spin correlations of La1.85-xSr0.15+xCu1-xFexO4			Structure Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, Anhui, China	Phys.Rev.B, 69(2004)104506	B.Liu,G.J.Xu,G.S.Wang,J.-C.Grivel,N.H.Andersen,Q.R.Pu,R.H.Tao,Z.J.Ding		
34400	L091087001	thickness=750A. Ce-content by ICP. second Tc = 20.7K.	(Pr,Ce)2CuO4	Pr1.885Ce0.115Cu1O4-z	Pr	1.885	Ce	0.115	Cu	1															O	4-z		5	2003																												T'																		K			13			3.9	13																																									A	mutual inductance	3890																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34401	L091087001	thickness=750A. Ce-content by ICP. second Tc = 20.7K.	(Pr,Ce)2CuO4	Pr1.876Ce0.124Cu1O4-z	Pr	1.876	Ce	0.124	Cu	1															O	4-z		5	2003																												T'																		K			21.3			1.3	21.3																																									A	mutual inductance	2290																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34402	L091087001	thickness=750A. Ce-content by ICP. 	(Pr,Ce)2CuO4	Pr1.873Ce0.127Cu1O4-z	Pr	1.873	Ce	0.127	Cu	1															O	4-z		5	2003																												T'																		K			23.1			0.8	23.1																																									A	mutual inductance	1970																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34403	L091087001	thickness=750A. Ce-content by ICP. gap obtained by fitting to PENET.	(Pr,Ce)2CuO4	Pr1.869Ce0.131Cu1O4-z	Pr	1.869	Ce	0.131	Cu	1															O	4-z		5	2003																												T'																		K			23.6			0.8	23.6																																									A	mutual inductance	1890					5.2																																																Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34404	L091087001	thickness=750A. Ce-content by ICP. 	(Pr,Ce)2CuO4	Pr1.867Ce0.133Cu1O4-z	Pr	1.867	Ce	0.133	Cu	1															O	4-z		5	2003																												T'																		K			23.3			0.5	23.3																																									A	mutual inductance	1600																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34405	L091087001	thickness=750A. Ce-content by ICP. second Tc = 22.9K.	(Pr,Ce)2CuO4	Pr1.863Ce0.137Cu1O4-z	Pr	1.863	Ce	0.137	Cu	1															O	4-z		5	2003																												T'																		K			23.2			0.7	23.2																																									A	mutual inductance	1560																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34406	L091087001	thickness=750A. Ce-content by ICP. second Tc = 20.2K.	(Pr,Ce)2CuO4	Pr1.856Ce0.144Cu1O4-z	Pr	1.856	Ce	0.144	Cu	1															O	4-z		5	2003																												T'																		K			21.2			0.9	21.2																																									A	mutual inductance	1610																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34407	L091087001	thickness=750A. Ce-content by ICP. second Tc = 16.6K.	(Pr,Ce)2CuO4	Pr1.848Ce0.152Cu1O4-z	Pr	1.848	Ce	0.152	Cu	1															O	4-z		5	2003																												T'																		K			19.8			2.4	19.8																																									A	mutual inductance	1690																																																					Films prepared by MBE on Pr2CuO4-buffer/SrTiO3					Magnetic Penetration Depth Measurements of Pr2-xCexCuO4-z Films on Buffered Substrates: Evidence for a Nodeless Gap			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 91(2003)087001	A.Tsukada,J.A.Skinta,M.Naito,Mun-Seog Kim,T.R.Lemberger		
34408	L091147002	Ce-content not given. underdoped sample.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2003																												T'																		K		15.9					15.9																																									A	muon-SR		3369																																																				directional solidification in Al2O3 crucible using CuO-based flux. O-reduction (900-1000C, in Ar-flow)					Superconductivity and Field-Induced Magnetism in Pr2-xCexCuO4 Single Crystals			Department of Physics, Simon Fraser University, Burnaby, British Columbia V5A 1S6, Canada	Phys.Rev.Lett., 91(2003)147002	C.R.Wiebe,G.M.Luke,J.E.Sonier,K.F.Poon,P.Fournier,P.Kyriakou,R.I.Miller,R.L.Greene,R.Liang		
34409	L088207005	Ce-content by ICP. underdoped. thickness=1250 A.	(La,Ce)2CuO4	La1.913Ce0.087Cu1O4-z	La	1.913	Ce	0.087	Cu	1															O	4-z		5	2002																												T'																		K		28.7				0.8	28.7																																									A	mutual inductance		3200																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34410	L088207005	Ce-content by ICP. optimal-doped. thickness=1250 A.	(La,Ce)2CuO4	La1.888Ce0.112Cu1O4-z	La	1.888	Ce	0.112	Cu	1															O	4-z		5	2002																												T'																		K		29.3				0.9	29.3																																									A	mutual inductance		2500																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34411	L088207005	Ce-content by ICP. overdoped. thickness=1250 A.	(La,Ce)2CuO4	La1.865Ce0.135Cu1O4-z	La	1.865	Ce	0.135	Cu	1															O	4-z		5	2002																												T'																		K		21.7				1	21.7																																									A	mutual inductance		2200																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34412	L088207005	Ce-content by ICP. underdoped. thickness=1000 A.	(La,Ce)2CuO4	La1.875Ce0.125Cu1O4-z	La	1.875	Ce	0.125	Cu	1															O	4-z		5	2002																												T'																		K		22.5				1.8	22.5																																									A	mutual inductance		3100																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34413	L088207005	Ce-content by ICP. optimal-doped. thickness=1000 A.	(La,Ce)2CuO4	La1.855Ce0.145Cu1O4-z	La	1.855	Ce	0.145	Cu	1															O	4-z		5	2002																												T'																		K		24.2				1	24.2																																									A	mutual inductance		1800																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34414	L088207005	Ce-content by ICP. overdoped. thickness=1000 A.	(La,Ce)2CuO4	La1.844Ce0.156Cu1O4-z	La	1.844	Ce	0.156	Cu	1															O	4-z		5	2002																												T'																		K		21.5				2.4	21.5																																									A	mutual inductance		2000																																																				Films by MBE on SrTiO3.					Evidence for a Transition in the Pairing Symmetry of the Electron-Doped Cuprates La2-xCexCuO4-y and Pr2-xCexCuO4-y			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207005	J.A.Skinta,M.Naito,Mun-Seog Kim,T.Greibe,T.R.Lemberger		
34415	PHC3411655	Ce-content not given. s-wave s/c model.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2000																												T'																		K		24					24																																									A	surface inpedance		390				1.37																																																directional solidification method					Microwave Electrodynamics of the Electron-Doped Cuprate Superconductors Pr2-xCexCuO4-y and Nd2-xCexCuO4-y			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, MD,USA	Physica C, 341-348(2000)1655	J.D.Kokales,L.V.Mercaldo,P.Fournier,R.L.Greene,S.M.Anlage,V.V.Talanov		
34416	PHC3411655	Ce-content not given. s-wave s/c model. GAPENE by fitting parameter of PENET(T).	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	2000																												T'																		K		19					19																																									A	surface inpedance		1150				1.61																																																directional solidification method					Microwave Electrodynamics of the Electron-Doped Cuprate Superconductors Pr2-xCexCuO4-y and Nd2-xCexCuO4-y			Center for Superconductivity Research, Department of Physics, University of Maryland, College Park, MD,USA	Physica C, 341-348(2000)1655	J.D.Kokales,L.V.Mercaldo,P.Fournier,R.L.Greene,S.M.Anlage,V.V.Talanov		
34417	L088207003	Ce-content by ICP.  thickness=750 A.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2002																												T'																		K		23.2				0.7	23.2																																									A	mutual inductance		2100																											uOhm.cm								21																	Films by MBE on SrTiO3.					Evidence for a Nodeless Gap from the Superfluid Density of Optimally Doped Pr1.855Ce0.145CuO4-y Films			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207003	J.A.Skinta,M.Naito,T.Greibe,T.R.Lemberger		
34418	L088207003	Ce-content by ICP.  thickness=1000 A.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2002																												T'																		K		24.2				1	24.2																																									A	mutual inductance		1800																											uOhm.cm								19																	Films by MBE on SrTiO3.					Evidence for a Nodeless Gap from the Superfluid Density of Optimally Doped Pr1.855Ce0.145CuO4-y Films			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207003	J.A.Skinta,M.Naito,T.Greibe,T.R.Lemberger		
34419	L088207003	Ce-content by ICP.  thickness=1250 A.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2002																												T'																		K		23.9				0.7	23.9																																									A	mutual inductance		1800																											uOhm.cm								18																	Films by MBE on SrTiO3.					Evidence for a Nodeless Gap from the Superfluid Density of Optimally Doped Pr1.855Ce0.145CuO4-y Films			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207003	J.A.Skinta,M.Naito,T.Greibe,T.R.Lemberger		
34420	L088207003	Ce-content by ICP.  thickness=750 A.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2002																												T'																		K		23.3				1.1	23.3																																									A	mutual inductance		2200																											uOhm.cm								23																	Films by MBE on SrTiO3.					Evidence for a Nodeless Gap from the Superfluid Density of Optimally Doped Pr1.855Ce0.145CuO4-y Films			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207003	J.A.Skinta,M.Naito,T.Greibe,T.R.Lemberger		
34421	L088207003	Ce-content by ICP.  thickness=750 A. insulating Pr2CuO4 buffer layer.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2002																												T'																		K		23.6				0.8	23.6																																									A	mutual inductance		1500																											uOhm.cm								26																	Films by MBE on SrTiO3.					Evidence for a Nodeless Gap from the Superfluid Density of Optimally Doped Pr1.855Ce0.145CuO4-y Films			Department of Physics, The Ohio State University, Columbus, Ohio, USA	Phys.Rev.Lett., 88(2002)207003	J.A.Skinta,M.Naito,T.Greibe,T.R.Lemberger		
34422	JJP033L168	Fig. shows Tc vs Ce-content.	(La,Ce)2CuO4	La1.87Ce0.13Cu1O4	La	1.87	Ce	0.13	Cu	1															O	4		1	1994																												T'			A	4.007		12.44												K	17		30				23.5	TC34422																																																																																													La2O3,CeO2,Cu2O	1	mixture - heat(1020C,48h, in Ar or N2) - pellet - oxidation(250-300C, in O2) - heat(600C,600h, in Ar or N2)					Synthesis of superconducting T'-(La1-xCex)2CuO4			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa, Japan	Jpn.J.Appl.Phys., 33(1994)L168	H.Shibata,K.Kinoshita,T.Yamada		
34423	PHC3721082	substrate = SrTiO3. Figure shows data for various substrates.	(La,Ce)2CuO4	La1.909Ce0.091Cu1O4	La	1.909	Ce	0.091	Cu	1															O	4		4	2002																												T'			A	4.0116		12.4524												K	30.3						30.3	TC34423																																																																																															Films by MBE on various substrates.					Role of substrates in molecular beam epitaxy growth of superconducting T'-La2-xCexCuO4 films			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa, Japan	Physica C, 372(2002)1082	M.Hepp,M.Naito,T.Greibe		
34424	PHC3570333	Figure shows Tc(x). thickness = 1000-2000 A.	(La,Ce)2CuO4	La1.89Ce0.11Cu1O4	La	1.89	Ce	0.11	Cu	1															O	4		4	2001																												T'			A	4.0156		12.4531												K	29.5		30				29.75	TC34424																																																																																															films grown by MBE on SrTiO3 at 685C. reduction(620C, P(O2)<E-8 Torr, 10 min)					Superconducting T'-La2-xCexCuO4 films grown by molecular beam epitaxy			NTT basic Research Laboratory, Atsugi-shi, Kanagawa,Japan	Physica C, 357(2001)333	M.Hepp,M.Naito		
34425	P066014531	not s/c. thickness=1000A.	(La,Ce)2CuO4	La1.94Ce0.06Cu1O4	La	1.94	Ce	0.06	Cu	1															O	4		4	2002																												T'			A			12.4809												K																																																																																																		RH34425					films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34426	P066014531	thickness=1000A.	(La,Ce)2CuO4	La1.92Ce0.08Cu1O4	La	1.92	Ce	0.08	Cu	1															O	4		4	2002																												T'			A			12.4708												K	15						15																																																																																																films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34427	P066014531	thickness=1000A.	(La,Ce)2CuO4	La1.91Ce0.09Cu1O4	La	1.91	Ce	0.09	Cu	1															O	4		4	2002																												T'			A			12.4563												K	18.2						18.2																																																																																																films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34428	P066014531	thickness=1000A.	(La,Ce)2CuO4	La1.89Ce0.11Cu1O4	La	1.89	Ce	0.11	Cu	1															O	4		4	2002																												T'			A			12.4504												K	25						25																																																																																											RH34428					films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34429	P066014531	thickness=1000A.	(La,Ce)2CuO4	La1.87Ce0.13Cu1O4	La	1.87	Ce	0.13	Cu	1															O	4		4	2002																												T'			A			12.4303												K	20						20																																																																																																films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34430	P066014531	thickness=1000A.	(La,Ce)2CuO4	La1.85Ce0.15Cu1O4	La	1.85	Ce	0.15	Cu	1															O	4		4	2002																												T'			A			12.4206												K	8.5						8.5																																																																																											RH34430					films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34431	P066014531	R not zero at 2.5 K. thickness=1000A.	(La,Ce)2CuO4	La1.84Ce0.16Cu1O4	La	1.84	Ce	0.16	Cu	1															O	4		4	2002																												T'			A			12.3998												K			3				3																																																																																											RH34431					films prepared by PLD method on SrTiO3 with buffer of BaTiO3(200A). Ts=700-780C, in P=300 mTorr.					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
34434	MPB0172609	orthorhombic distortion = 4.28 E-3	Gd(Sr,Ba)2Cu3Oz	Gd1Sr0.8Ba1.2Cu3Oz	Gd	1	Sr	0.8	Ba	1.2	Cu	3													O	z			2003																												Y123																		K		84					84																																																																																																ANN(800C,20h,in Ar) - ANN(450C,48h,in flowing O2					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34435	MPB0172609	orthorhombic distortion = 2.22 E-3	(Gd,Pr,Ca)(Sr,Ba)2CuOz	Gd0.8Pr0.1Ca0.1Sr0.8Ba1.2Cu3Oz	Gd	0.8	Pr	0.1	Ca	0.1	Sr	0.8	Ba	1.2	Cu	3									O	z			2003																												Y123																		K		69.8					69.8																																																																																																ANN(800C,20h,in Ar) - ANN(450C,48h,in flowing O2					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34436	MPB0172609	orthorhombic distortion = 2.51 E-3.	(Gd,Pr,Ca)(Sr,Ba)2CuOz	Gd0.6Pr0.2Ca0.2Sr0.8Ba1.2Cu3Oz	Gd	0.6	Pr	0.2	Ca	0.2	Sr	0.8	Ba	1.2	Cu	3									O	z			2003																												Y123																		K		44.9					44.9																																																																																																ANN(800C,20h,in Ar) - ANN(450C,48h,in flowing O2					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34437	MPB0172609	orthorhombic distortion = 6.26 E-3.	Er(Sr,Ba)2Cu3Oz	Er1Sr0.8Ba1.2Cu3Oz	Er	1	Sr	0.8	Ba	1.2	Cu	3													O	z			2003																												Y123																		K		83.9					83.9																																																																																																ANN(450C,48h,in O2-flow) - FC to RT					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34438	MPB0172609	orthorhombic distortion = 6.31 E-3.	(Er,Pr,Ca)(Sr,Ba)2CuOz	Er0.8Pr0.1Ca0.1Sr0.8Ba1.2Cu3Oz	Er	0.8	Pr	0.1	Ca	0.1	Sr	0.8	Ba	1.2	Cu	3									O	z			2003																												Y123																		K		78					78																																																																																																ANN(450C,48h,in O2-flow) - FC to RT					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34439	MPB0172609	orthorhombic distortion = 5.78 E-3.	(Er,Pr,Ca)(Sr,Ba)2CuOz	Er0.6Pr0.2Ca0.2Sr0.8Ba1.2Cu3Oz	Er	0.6	Pr	0.2	Ca	0.2	Sr	0.8	Ba	1.2	Cu	3									O	z			2003																												Y123																		K		72.5					72.5																																																																																																ANN(450C,48h,in O2-flow) - FC to RT					Structural and superconducting properties of RE1-2xPrxCaxSr0.8Ba1.2Cu3O7-z(RE=Er and Gd) high Tc superconductors			Mahidol University,Bangkok,Thailand	Int'l.J.Mod.Phys.B, 17(2003)2609	I.M.Tang,P.Winotai,R.Suryanarayanan,W.Charoenthai		
34440	MPB0170942	thickness=2500 A.	SmBa2Cu3O7	Sm1Ba2Cu3Oz	Sm	1	Ba	2	Cu	3															O	z		5	2003																												Y123			A			11.72												K		88					88																																									A	surface impedance	2550																																																					films were prepared by dc sputtering on LaAlO3 in 2.6 mbar O2.					Study of the electrodynamic response of SmBa2Cu3O7-z thin films in the microwave region			Universita' di Napoli, Napoli,Italy	Int'l.J.Mod.Phys.B, 17(2003)942	A.Andreone,A.M.Cucolo,E.Di Gennaro,G.Lamura,M.Boffa		
34441	SSC1290075		La2CuO4	La2Cu1O4.086	La	2	Cu	1																	O	4+z	4.086	1	2004	emu/Oe.g	0.0000002																										T			A	5.34	5.416	13.225												K		45.2					45.2																																																																																																samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34442	SSC1290075		La2(Cu,Zn)O4	La2Cu0.99Zn0.01O4.099	La	2	Cu	0.99	Zn	0.01															O	4+z	4.099	1	2004	emu/Oe.g	0.00000032	emu.K/Oe.g	0.00000421	m/Zn	1.17	6																					T			A	5.342	5.414	13.217												K		29.3					29.3																																																																																																samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34443	SSC1290075		La2(Cu,Zn)O4	La2Cu0.98Zn0.02O4.099	La	2	Cu	0.98	Zn	0.02															O	4+z	4.099	1	2004	emu/Oe.g	0.000000289	emu.K/Oe.g	0.00000856	m/Zn	1.18	-1.69																					T			A	5.341	5.416	13.217												K		19.2					19.2																																																																																																samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34444	SSC1290075		La2(Cu,Zn)O4	La2Cu0.97Zn0.03O4.1	La	2	Cu	0.97	Zn	0.03															O	4+z	4.1	1	2004	emu/Oe.g	0.000000216	emu.K/Oe.g	0.00001	m/Zn	1.04	-2.65																					T			A	5.4347	5.418	13.219												K		7.3					7.3																																																																																																samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34445	SSC1290075		La2(Cu,Zn)O4	La2Cu0.96Zn0.04O4.105	La	2	Cu	0.96	Zn	0.04															O	4+z	4.105	1	2004	emu/Oe.g	0.000000209	emu.K/Oe.g	0.00000943	m/Zn	0.88	-1.85																					T			A	5.343	5.418	13.212												K					4.2																																																																																																		samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34446	SSC1290075		La2(Cu,Zn)O4	La2Cu0.95Zn0.05O4.106	La	2	Cu	0.95	Zn	0.05															O	4+z	4.106	1	2004	emu/Oe.g	0.000000221	emu.K/Oe.g	0.00000798	m/Zn	0.72	-1.73																					T			A	5.343	5.419	13.206												K					4.2																																																																																																		samples prepared by solid state reaction. chemically oxidized using NaClO solution.					Superconductivity and magnetism of La2Cu1-xZnxO4+z chemically oxidized by NaClO			Institute of Physics and Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Solid State Commun., 129(2004)75	B.K.Ma,J.K.Liang,Q.Y.Tu,X.L.Chen,Z.X.Zhao		
34447	JPS0730819	beta-pyrochlore structure	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6			2004																												pyrochlore			A	10.114														K	6.1	6.3	8				6.3																				T		17												HC34447																			SP34447																																									Rb2O,Os		mixed powders - pellet - heat(773K,24h,in vac)					New Pyrochlore Oxide Superconductor RbOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 73(2004)819	S.Yonezawa,Y.Matsushita,Y.Muraoka,Z.Hiroi		
34448	JP01600L9	defect pyrochlore. O-content not determined.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2004																												pyrochlore			A	10.099														K	9	9.5	9.9	9.6			9.5										90																																																																																						(KO2+OsO2) - pellet - heat(873K,24h,in vac)					Superconductivity in a pyrochlore-related oxide KOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.:Condens.Matter, 16(2004)L9	S.Yonezawa,Y.Matsushita,Y.Muraoka,Z.Hiroi		
34449	L092157004	RRR=40.	NaxCoO2:yH2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3		3	2004																																														K	4.2						4.2																																		HC34449		A			100																	mj/mol.K2	16.6																																							Na0.75CoO2 was melted using optical floating zone. Na extraction by electrochemical method.					Thermodynamic and Transport Measurements of Superconducting Na0:3CoO2:1.3H2O Single Crystals Prepared by Electrochemical Deintercalation			Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts, USA	Phys.Rev.Lett., 92(2004)157004	E.T.Abel,F.C.Chou,J.H.Cho,K.Matan,P.A.Lee,Y.S.Lee		
34450	MPB0173622	not s/c	Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.5Ba0.5Cu2.9Mo0.1Oz	Nd	1	Sr	1.5	Ba	0.5	Cu	2.9	Mo	0.1											O	z			2003																												Y123																		K					25																																																																																																Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34451	MPB0173622		Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.5Ba0.5Cu2.85Mo0.15Oz	Nd	1	Sr	1.5	Ba	0.5	Cu	2.85	Mo	0.15											O	z			2003																												Y123																		K	26.5		42				34.25																																																																																														Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34452	MPB0173622		Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.5Ba0.5Cu2.7Mo0.3Oz	Nd	1	Sr	1.5	Ba	0.5	Cu	2.7	Mo	0.3											O	z			2003																												Y123																		K	15		30				22.5																																																																		uV/K	36.9																											Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34453	MPB0173622		NdSr2(Cu,Mo)3Oz	Nd1Sr2Cu2.8Mo0.2Oz	Nd	1	Sr	2	Cu	2.8	Mo	0.2													O	z			2003																												Y123																		K					25																																																																				uV/K	60.5																											Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34454	MPB0173622		Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.8Ba0.2Cu2.8Mo0.2Oz	Nd	1	Sr	1.8	Ba	0.2	Cu	2.8	Mo	0.2											O	z			2003																												Y123																		K					25																																																																				uV/K	41.1																											Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34455	MPB0173622		Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.65Ba0.35Cu2.8Mo0.2Oz	Nd	1	Sr	1.65	Ba	0.35	Cu	2.8	Mo	0.2											O	z			2003																												Y123																		K			26				26																																																																		uV/K	34.9																											Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34456	MPB0173622		Nd(Sr,Ba)2(Cu,Mo)3Oz	Nd1Sr1.5Ba0.5Cu2.8Mo0.2Oz	Nd	1	Sr	1.5	Ba	0.5	Cu	2.8	Mo	0.2											O	z			2003																												Y123																		K	27		35				31																																																																		uV/K	25.5																											Nd2O3,SrCO3,BaCO3,CuO,MoO3	1	mixture - CAL(1045C,5h,in O2) - pellet - SIN(1050C,5h,in flowing O2) - slow cool to RT.					Occurrence of superconductivity in Ba-doped NdSr2(Cu,Mo)3Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3622	H.K.Lee,K.D.Kim		
34457	MPB0173682	small amount of impurity phases	RuSr2(Eu,Ce)2Cu2Oz	Ru1Sr2Eu1.5Ce0.5Cu2Oz	Ru	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	z			2003																												Ru1222			A	3.837		28.49												K	26		46				36																																																																																															1	mixture - SIN(1010C,15h,in N2) - ANN(1060 - 1065C,134h,in flowing O2) - slow cool to RT.					Superconducting and magnetic properties of (Ru1-xNbx)Sr2(Eu1.5Ce0.5)Cu2Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3682	H.K.Lee,Y.C.Kim		
34458	MPB0173682	small amount of impurity phases	(Ru,Nb)Sr2(Eu,Ce)2Cu2Oz	Ru0.75Nb0.25Sr2Eu1.5Ce0.5Cu2Oz	Ru	0.75	Nb	0.25	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	z			2003																												Ru1222			A	3.848		28.54												K	25		42				33.5																																																																																															1	mixture - SIN(1010C,15h,in N2) - ANN(1060 - 1065C,134h,in flowing O2) - slow cool to RT.					Superconducting and magnetic properties of (Ru1-xNbx)Sr2(Eu1.5Ce0.5)Cu2Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3682	H.K.Lee,Y.C.Kim		
34459	MPB0173682		(Ru,Nb)Sr2(Eu,Ce)2Cu2Oz	Ru0.5Nb0.5Sr2Eu1.5Ce0.5Cu2Oz	Ru	0.5	Nb	0.5	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	z		1	2003																												Ru1222			A	3.853		28.69												K	25		39				32																																																																																															1	mixture - SIN(1010C,15h,in N2) - ANN(1060 - 1065C,134h,in flowing O2) - slow cool to RT.					Superconducting and magnetic properties of (Ru1-xNbx)Sr2(Eu1.5Ce0.5)Cu2Oz			Kangwon National University ,Chunchon, Korea	Int'l.J.Mod.Phys.B, 17(2003)3682	H.K.Lee,Y.C.Kim		
34460	JPS0731123	resistivity shows two anomalies, 340K(HTT to LTO) and 125K(LTO to LTT). dTc/dp value is for uniaxial pressure [110].	(La,Eu,Sr)2CuO4	La1.64Eu0.2Sr0.16Cu1O4	La	1.64	Eu	0.2	Sr	0.16	Cu	1													O	4		3	2004																												T																		K				10			10	TC34460		K/GPa	25																																																																																												crystals grown by TSFZ method					Gigantic Anisotropic Uniaxial Pressure Effect on Superconductivity within the CuO2 Plane of La1.64Eu0.2Sr0.16CuO4: Strain Control of Stripe Criticality			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki,Japan	J.Phys.Soc.Jpn, 73(2004)1123	H.Takagi,N.Takeshita,T.Sasagawa,T.Sugioka,Y.Tokura		
34461	JPS0731131	RRR=38. Hc2(T) defined as R/Rn = 0.9. Anisotropy factor = 9.2.	NaxCoO2:yH2O	Na0.35Co1H2.6O3.3	Na	0.35	Co	1	H	2.6															O	3.3		3	2004																																														K	3.9		4.5				4.2																				T	RES		15	1.7					T/K	RES		4.7	0.53	HC34461		A	from Hc2		120	13																																																								floating zone method					Superconducting Properties under Magnetic Field in Na0:35CoO2: 1.3H2O Single Crystal			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 73(2004)1131	K.Togano,K.Yamada,N.Kobayashi,N.Yoneyama,P.Badica,T.Sasaki		
34462	JPS0731297	Na-content is nominal value. y is not given.	NaxCoO2:yH2O	Na0.75Co1H2.6O3.3	Na	0.75	Co	1	H	2.6															O	3.3			2004																																														K				4.61			4.61																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34463	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 1 K/%Ir.	Nax(Co,Ir)O2:yH2O	Na0.75Co0.9995Ir0.0005H2.6O3.3	Na	0.75	Co	0.9995	Ir	0.0005	H	2.6													O	3.3			2004																																														K				4.59			4.59																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34464	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 1 K/%Ir.	Nax(Co,Ir)O2:yH2O	Na0.75Co0.995Ir0.005H2.6O3.3	Na	0.75	Co	0.995	Ir	0.005	H	2.6													O	3.3			2004																																														K				3.94			3.94																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34465	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 1 K/%Ir.	Nax(Co,Ir)O2:yH2O	Na0.75Co0.99Ir0.01H2.6O3.3	Na	0.75	Co	0.99	Ir	0.01	H	2.6													O	3.3			2004																																														K				3.54			3.54																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34466	JPS0731297	Na-content is nominal value. y is not given.	NaxCoO2:yH2O	Na0.75Co1H2.6O3.3	Na	0.75	Co	1	H	2.6															O	3.3			2004																																														K				4.49			4.49																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34467	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 2 K/%Ga.	Nax(Co,Ga)O2:yH2O	Na0.75Co0.9995Ga0.0005H2.6O3.3	Na	0.75	Co	0.9995	Ga	0.0005	H	2.6													O	3.3			2004																																														K				4.38			4.38																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34468	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 2 K/%Ga.	Nax(Co,Ga)O2:yH2O	Na0.75Co0.999Ga0.001H2.6O3.3	Na	0.75	Co	0.999	Ga	0.001	H	2.6													O	3.3			2004																																														K				4.19			4.19																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34469	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 2 K/%Ga.	Nax(Co,Ga)O2:yH2O	Na0.75Co0.9975Ga0.0025H2.6O3.3	Na	0.75	Co	0.9975	Ga	0.0025	H	2.6													O	3.3			2004																																														K				3.98			3.98																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34470	JPS0731297	Na-content is nominal value. y is not given. dTc/dx = 2 K/%Ga.	Nax(Co,Ga)O2:yH2O	Na0.75Co0.995Ga0.005H2.6O3.3	Na	0.75	Co	0.995	Ga	0.005	H	2.6													O	3.3			2004																																														K				2.99			2.99																																																																																																solid reaction(750-850C, 24-36 h). Na-deintercalate (in acetonitrite), then washed by distilled water.					Impurity Effects on the Superconducting Transition Temperature of NazCoO2: yH2O			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya, Japan	J.Phys.Soc.Jpn, 73(2004)1297	H.Watanabe,M.Sato,M.Yokoi,T.Moyoshi,Y.Kobayashi,Y.Mori		
34471	PHC4060058	structure analized using Amaa. FIR measured.	Bi2(Sr,Y,Ca)3Cu2O8	Bi2Sr2.1Y0.1Ca0.8Cu2O8.26	Bi	2	Sr	2.1	Y	0.1	Ca	0.8	Cu	2											O	8+z	8.26	1	2004																												Bi2212			A	5.405		30.76												K				96			96																																																																																															1	mixture - CAL - pellet - heat(850C,2d) + heat(860-890C, 21d)					The infrared properties of Bi2Y0.1Sr1.9CaCu2O8+z superconductor			Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47,Kosice, Slovakia	Physica C, 406(2004)58	J.Hejtmanek,K.Knizek,N.Hudakova		
34472	PHC4060058	structure analized using Amaa. FIR measured.	Bi2(Sr,Y,Ca)3Cu2O8	Bi2Sr1.9Y0.1Ca1Cu2O8.24	Bi	2	Sr	1.9	Y	0.1	Ca	1	Cu	2											O	8+z	8.24	1	2004																												Bi2212			A	5.4		30.74												K				94			94																																																																																															1	mixture - CAL - pellet - heat(850C,2d) + heat(860-890C, 21d)					The infrared properties of Bi2Y0.1Sr1.9CaCu2O8+z superconductor			Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47,Kosice, Slovakia	Physica C, 406(2004)58	J.Hejtmanek,K.Knizek,N.Hudakova		
34473	PHC4060058	structure analized using Amaa. FIR measured.	Bi2(Sr,Y,Ca)3Cu2O8	Bi2Sr1.8Y0.1Ca1.1Cu2O8.23	Bi	2	Sr	1.8	Y	0.1	Ca	1.1	Cu	2											O	8+z	8.23	1	2004																												Bi2212			A	5.4		30.73												K				93			93																																																																																															1	mixture - CAL - pellet - heat(850C,2d) + heat(860-890C, 21d)					The infrared properties of Bi2Y0.1Sr1.9CaCu2O8+z superconductor			Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47,Kosice, Slovakia	Physica C, 406(2004)58	J.Hejtmanek,K.Knizek,N.Hudakova		
34474	PHC4060058	structure analized using Amaa. FIR measured.	Bi2(Sr,Y,Ca)3Cu2O8	Bi2Sr1.6Y0.1Ca1.3Cu2O8.23	Bi	2	Sr	1.6	Y	0.1	Ca	1.3	Cu	2											O	8+z	8.23	1	2004																												Bi2212			A	5.401		30.65												K				89			89																																																																																															1	mixture - CAL - pellet - heat(850C,2d) + heat(860-890C, 21d)					The infrared properties of Bi2Y0.1Sr1.9CaCu2O8+z superconductor			Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47,Kosice, Slovakia	Physica C, 406(2004)58	J.Hejtmanek,K.Knizek,N.Hudakova		
34475	JPS0731651	structure=beta-pyrochlore. gamma estimated from BCS theory (delta-C/gamma*Tc = 1.43). GL = 90.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		1	2004																												pyrochlore			A	10.101														K	9.6		10				9.8										70	Oe		50							T		38.3												HC34475		A		30			A	muon-SR	2700										SP34475			mj/mol.K2	38																																							(KO2,OsO2) - heat(873K,24h, in O2)					Unprecedented Superconductivity in  beta-Pyrochlore Osmate KOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581,Japan	J.Phys.Soc.Jpn, 73(2004)1651	S.Yonezawa,Y.Muraoka,Z.Hiroi		
34476	JPS0731655	structure = beta-pyrochlore.	CsOs2O6	Cs1Os2O6	Cs	1	Os	2																	O	6		1	2004																												pyrochlore	Fd3(-)m		A	10.149														K	3.2	3.3	3.4				3.3										100																																																																																				Cs2CO3,Os		mixture - pellet - heat(673K,24h, in evacuated silica)					New beta-Pyrochlore Oxide Superconductor CsOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581,Japan	J.Phys.Soc.Jpn, 73(2004)1655	S.Yonezawa,Y.Muraoka,Z.Hiroi		
34477	SSC1310125	proton incorporation. water-vapor hydrated sample.	Na0.22H0.1CoO2/0.85H2O	Na0.22Co1H1.8O2.85	Na	0.22	Co	1	H	1.8															O	2.85	2.85		2004																															A	2.823		19.61												K				4.5			4.5																																																																																																Na0.7C0O2 - react with water vapor (or liquid) at RT for 1 week.					Proton incorporations and superconductivity in a cobalt oxyhydrate			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Solid State Commun., 131(2004)125	C.Feng,G.Cao,M.Zhong,X.Chen,X.Tang,Y.Xu,Z.Xu		
34478	SSC1310125	proton incorporation. water-liquid hydrated sample.	Na0.22H0.1CoO2/0.85H2O	Na0.22Co1H1.8O2.85	Na	0.22	Co	1	H	1.8															O	2.85	2.85		2004																															A	2.824		19.75												K				4.4			4.4																																																																																																Na0.7C0O2 - react with water vapor (or liquid) at RT for 1 week.					Proton incorporations and superconductivity in a cobalt oxyhydrate			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Solid State Commun., 131(2004)125	C.Feng,G.Cao,M.Zhong,X.Chen,X.Tang,Y.Xu,Z.Xu		
34479	SSC1290117	as-synthesized. not s/c.	TbSr2(Cu,Mo)3O7	Tb1Sr2Cu2.7Mo0.3O7.12	Tb	1	Sr	2	Cu	2.7	Mo	0.3													O	7+z	7.12	1	2004								7																				Y123			A	3.8371		11.5784												K					5																																																																																																Tb4O7,MoO3,SrO2,CuO	1	mixture - CAL(975, 990, 1000C, 24h) - ANN(1000C,24h, in air)					Superconductivity with transition temperature up to 80 K for TbSr2Cu2.7Mo0.3O7+z				Solid State Commun., 129(2004)117	A.Gupta,A.V.Nalikar,E.Takayama-Muromachi,H.Kishan,H.Yamauchi,M.Karppinen,S.K.Malik,T.Watanabe,V.Ganesan,V.P.S.Awana,W.B.Yelon		
34480	SSC1290117	O2-annealed sample.	TbSr2(Cu,Mo)3O7	Tb1Sr2Cu2.7Mo0.3O7.15	Tb	1	Sr	2	Cu	2.7	Mo	0.3													O	7+z	7.15	1	2004																												Y123																		K				37			37										20																																																																																				Tb4O7,MoO3,SrO2,CuO	1	mixture - CAL(975, 990, 1000C, 24h) - ANN(1000C,24h, in air) -  ANN(420C,12h + 360C,12h, in 120 atm O2 flow)					Superconductivity with transition temperature up to 80 K for TbSr2Cu2.7Mo0.3O7+z				Solid State Commun., 129(2004)117	A.Gupta,A.V.Nalikar,E.Takayama-Muromachi,H.Kishan,H.Yamauchi,M.Karppinen,S.K.Malik,T.Watanabe,V.Ganesan,V.P.S.Awana,W.B.Yelon		
34481	SSC1290117	mixed with AgO, then HIP(5GPa, 400C,30min). R not zero down to 5K.	TbSr2(Cu,Mo)3O7	Tb1Sr2Cu2.7Mo0.3O7+z	Tb	1	Sr	2	Cu	2.7	Mo	0.3													O	7+z		1	2004																												Y123																		K			80	80			80										14.5																																																																																				Tb4O7,MoO3,SrO2,CuO		mixture - CAL(975, 990, 1000C, 24h) - ANN(1000C,24h, in air) - mixed with 100 mol% of AgO - sealed in Au capsule - heat(5GPa,400C,30 min)					Superconductivity with transition temperature up to 80 K for TbSr2Cu2.7Mo0.3O7+z				Solid State Commun., 129(2004)117	A.Gupta,A.V.Nalikar,E.Takayama-Muromachi,H.Kishan,H.Yamauchi,M.Karppinen,S.K.Malik,T.Watanabe,V.Ganesan,V.P.S.Awana,W.B.Yelon		
34482	P069174506	single crystal 0.6*0.6*1.4 mm3.	La2CuO4.11	La2Cu1O4.11	La	2	Cu	1																	O	4	4.11	3	2004																												T																		K				45			45																																		HC34482																																																														TSFZ method. oxidized by electrochemical method.					Thermodynamic properties of excess-oxygen-doped La2CuO4.11 near a simultaneous transition to superconductivity and long-range magnetic order			National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 69(2004)174506	B.Khaykovich,B.L.Zink,C.D.Batista,F.Hellman,G.A.Jorge,L.Givale,M.A.Kastner,M.Jaime,R.J.Birgeneau,Y.S.Lee		
34483	PHC4050212	not s/c. spin glass temp. = 101.5 K	RuSr2(Y,Ce)2Cu2O10	Ru1Sr2Y1.5Ce0.5Cu2O10-z	Ru	1	Sr	2	Y	1.5	Ce	0.5	Cu	2											O	10-z			2004																												Ru1222			A	3.824		28.445												K																																																																																																							high-pressure synthesis					Magnetic properties of the RuSr2Ln1.5Ce0.5Cu2O10-d  (Ln=Y, Ho and Dy) and RuSr2YCu2O8-d rutheno-cuprate families: a comparative study			Grupo de Materiais e Dispositivos, CMDMC, Departamento de Fisica, UFSCar, Brazil	Physica C, 405(2004)212	C.A.Cardoso,E.Takayama-Muromachi,F.M.Araujo-Moreira,H.Kishan,O.F.de Lima,V.P.S.Awana		
34484	PHC4050212	not s/c. spin glass temp. = 103.3 K.	RuSr2(Ho,Ce)2Cu2O10	Ru1Sr2Ho1.5Ce0.5Cu2O10-z	Ru	1	Sr	2	Ho	1.5	Ce	0.5	Cu	2											O	10-z			2004																												Ru1222			A	3.819		28.439												K																																																																																																							high-pressure synthesis					Magnetic properties of the RuSr2Ln1.5Ce0.5Cu2O10-d  (Ln=Y, Ho and Dy) and RuSr2YCu2O8-d rutheno-cuprate families: a comparative study			Grupo de Materiais e Dispositivos, CMDMC, Departamento de Fisica, UFSCar, Brazil	Physica C, 405(2004)212	C.A.Cardoso,E.Takayama-Muromachi,F.M.Araujo-Moreira,H.Kishan,O.F.de Lima,V.P.S.Awana		
34485	PHC4050212	not s/c. spin glass temp. = 87.4 K.	RuSr2(Dy,Ce)2Cu2O10	Ru1Sr2Dy1.5Ce0.5Cu2O10-z	Ru	1	Sr	2	Dy	1.5	Ce	0.5	Cu	2											O	10-z			2004																												Ru1222			A	3.813		28.419												K																																																																																																							high-pressure synthesis					Magnetic properties of the RuSr2Ln1.5Ce0.5Cu2O10-d  (Ln=Y, Ho and Dy) and RuSr2YCu2O8-d rutheno-cuprate families: a comparative study			Grupo de Materiais e Dispositivos, CMDMC, Departamento de Fisica, UFSCar, Brazil	Physica C, 405(2004)212	C.A.Cardoso,E.Takayama-Muromachi,F.M.Araujo-Moreira,H.Kishan,O.F.de Lima,V.P.S.Awana		
34486	PHC4050212	not s/c. AF at 150 K.	RuSr2YCu2O8	Ru1Sr2Y1Cu2O8+z	Ru	1	Sr	2	Y	1	Cu	2													O	8+z			2004								150																				Ru1212			A	3.818		11.5222												K																																																																																																							high-pressure synthesis					Magnetic properties of the RuSr2Ln1.5Ce0.5Cu2O10-d  (Ln=Y, Ho and Dy) and RuSr2YCu2O8-d rutheno-cuprate families: a comparative study			Grupo de Materiais e Dispositivos, CMDMC, Departamento de Fisica, UFSCar, Brazil	Physica C, 405(2004)212	C.A.Cardoso,E.Takayama-Muromachi,F.M.Araujo-Moreira,H.Kishan,O.F.de Lima,V.P.S.Awana		
34487	P069184507	zero-field muon-SR measured.	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	2004																												T																		K				29.3			29.3																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34488	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.9975Zn0.0025O4	La	1.9	Sr	0.1	Cu	0.9975	Zn	0.0025													O	4		1	2004																												T																		K				23.71			23.71																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34489	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.995Zn0.005O4	La	1.9	Sr	0.1	Cu	0.995	Zn	0.005													O	4		1	2004																												T																		K				20.19			20.19																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34490	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.9925Zn0.0075O4	La	1.9	Sr	0.1	Cu	0.9925	Zn	0.0075													O	4		1	2004																												T																		K				15.23			15.23																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34491	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.99Zn0.01O4	La	1.9	Sr	0.1	Cu	0.99	Zn	0.01													O	4		1	2004																												T																		K				11.97			11.97																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34492	P069184507	not s/c. zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.98Zn0.02O4	La	1.9	Sr	0.1	Cu	0.98	Zn	0.02													O	4		1	2004																												T																		K					4.2																																																																																																La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34493	P069184507	zero-field muon-SR measured.	(La,Sr)2CuO4	La1.885Sr0.115Cu1O4	La	1.885	Sr	0.115	Cu	1															O	4		1	2004																												T																		K				27.57			27.57																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34494	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.885Sr0.115Cu0.9975Zn0.0025O4	La	1.885	Sr	0.115	Cu	0.9975	Zn	0.0025													O	4		1	2004																												T																		K				22.46			22.46																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34495	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.885Sr0.115Cu0.995Zn0.005O4	La	1.885	Sr	0.115	Cu	0.995	Zn	0.005													O	4		1	2004																												T																		K				17.64			17.64																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34496	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.885Sr0.115Cu0.9925Zn0.0075O4	La	1.885	Sr	0.115	Cu	0.9925	Zn	0.0075													O	4		1	2004																												T																		K				12.45			12.45																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34497	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.885Sr0.115Cu0.99Zn0.01O4	La	1.885	Sr	0.115	Cu	0.99	Zn	0.01													O	4		1	2004																												T																		K				8.56			8.56																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34498	P069184507	not s/c. zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.885Sr0.115Cu0.98Zn0.02O4	La	1.885	Sr	0.115	Cu	0.98	Zn	0.02													O	4		1	2004																												T																		K					4.2																																																																																																La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34499	P069184507	zero-field muon-SR measured.	(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4		1	2004																												T																		K				33.54			33.54																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34500	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.87Sr0.13Cu0.9975Zn0.0025O4	La	1.87	Sr	0.13	Cu	0.9975	Zn	0.0025													O	4		1	2004																												T																		K				28.92			28.92																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34501	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.87Sr0.13Cu0.995Zn0.005O4	La	1.87	Sr	0.13	Cu	0.995	Zn	0.005													O	4		1	2004																												T																		K				26.44			26.44																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34502	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.87Sr0.13Cu0.9925Zn0.0075O4	La	1.87	Sr	0.13	Cu	0.9925	Zn	0.0075													O	4		1	2004																												T																		K				21.02			21.02																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34503	P069184507	zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.87Sr0.13Cu0.99Zn0.01O4	La	1.87	Sr	0.13	Cu	0.99	Zn	0.01													O	4		1	2004																												T																		K				18.83			18.83																																																																																														La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34504	P069184507	not s/c. zero-field muon-SR measured.	(La,Sr)2(Cu,Zn)O4	La1.87Sr0.13Cu0.98Zn0.02O4	La	1.87	Sr	0.13	Cu	0.98	Zn	0.02													O	4		1	2004																												T																		K					2																																																																																																La2O3,SrCO3,CuO,ZnO	1	solid state reaction. ANN(500C,72h, in flowing O2)					Muon spin relaxation and magnetic susceptibility studies of the effects of nonmagnetic impurities on the Cu spin dynamics and superconductivity in La2-xSrxCu1-yZnyO4 around x=0.115			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Aoba-ku, Sendai, Japan	Phys.Rev.B, 69(2004)184507	I.Watanabe,K.Nagamine,K.Takahashi,S.Yairi,T.Adachi,Y.Koike		
34505	JMC0120646	not s/c	Hg2Os2O7	Hg2Os2O7	Hg	2	Os	2																	O	7			2002																												pyrochlore			A	10.245														K					4																																																																																																HgO,Os,OsO4		mixture - (silica ampoule) - heat(500C,1d) - FC to RT					The synthesis, structure and properties of Hg2Os2O7			Department of Chemistry, University of Southampton, Southampton, Hants, UK SO17 1BJ.	J.Mater.Chem., 12(2002)646	Jonathan Reading,Mark T. Weller,Sergey Gordeev		
34506	JP01604061	not s/c	Hg2Ba2YCu2O8	Hg2Ba2Y1Cu2O8-z	Hg	2	Ba	2	Y	1	Cu	2													O	8-z			2004																												Hg2212			A	3.8606		28.915												K				0			0																																																																																																high pressure synthesis(3.5 - 4.0 GPa, 15 - 20 min, 900 - 1050 C)					The effect of Sr substitution on superconductivity in Hg2(Ba1-ySry)2YCu2O8-z:  I.A neutron powder diffraction study			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	J.Phys.:Condens.Matter, 16(2004)4061	E.Suard,P.Bordet,P.Odier,P.Toulemonde,S.Le Floch		
34507	JP01604061		Hg(Ba,Sr)2YCu2O8	Hg2Ba1Sr1Y1Cu2O8-z	Hg	2	Ba	1	Sr	1	Y	1	Cu	2											O	8-z			2004																												Hg2212			A	3.8319		28.4176												K				32			32																																																																																																high pressure synthesis(3.5 - 4.0 GPa, 15 - 20 min, 900 - 1050 C)					The effect of Sr substitution on superconductivity in Hg2(Ba1-ySry)2YCu2O8-z:  I.A neutron powder diffraction study			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	J.Phys.:Condens.Matter, 16(2004)4061	E.Suard,P.Bordet,P.Odier,P.Toulemonde,S.Le Floch		
34508	JP01604061		Hg2Sr2YCu2O8	Hg2Sr2Y1Cu2O8-z	Hg	2	Sr	2	Y	1	Cu	2													O	8-z			2004																												Hg2212			A	3.8112		28.136												K				42			42																																																																																																high pressure synthesis(3.5 - 4.0 GPa, 15 - 20 min, 900 - 1050 C)					The effect of Sr substitution on superconductivity in Hg2(Ba1-ySry)2YCu2O8-z:  I.A neutron powder diffraction study			Laboratoire de Cristallographie, CNRS, 25 avenue des martyrs, BP166, F-38042 Grenoble cedex 09, France	J.Phys.:Condens.Matter, 16(2004)4061	E.Suard,P.Bordet,P.Odier,P.Toulemonde,S.Le Floch		
34509	L092227003	not s/c	(Pr,La,Ce)2CuO4	Pr1.29La0.7Ce0.01Cu1O4	Pr	1.29	La	0.7	Ce	0.01	Cu	1													O	4			2004								129																				T'	I4/mmm		A	3.964		12.28												K																																																																																																							single crystals grown by TSFZ method.					Spin-Flop Transition and the Anisotropic Magnetoresistance of Pr1.3-xLa0.7CexCuO4: Unexpectedly Strong Spin-Charge Coupling in the Electron-Doped Cuprates			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.Lett., 92(2004)227003	A.N.Lavrov,H.J.Kang,J.W.Lynn,P.Dai,S.-H.Lee,Seiki Komiya,T.Suzuki,Y.Ando,Y.Kurita		
34510	PR0515824	not s/c. Neel-T by NED.	Pr2CuO4	Pr2Cu1O4	Pr	2	Cu	1																	O	4		3	1995								284																				T'																		K																																																																																																							ANN(860C,in Ar)					Magnetic structure and spin dynamics of Pr and Cu in Pr2CuO4				Phys.Rev.B, 51(1995)5824	D.I.Zhigunov,I.W.Sumarlin,J.L.Peng,J.W.Lynn,S.N.Barilo,T.Chattopadhyay		
34511	P070020503	beta-pyrochlore. Debye-T = 240 K at 4 K. (delta-C/gamma*Tc) = 1.38	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6			2004																												pyrochlore			A	10.1137														K				6.4			6.4										77										T		6							T/K		1.2					A		74																		mJ/mol.K2	33.7	sp-heat	230	sp-heat																																		OsO2,Rb2O	1	mixture of (OsO2+Rb2O) - heat(600C,24h). resultant (RbOs2O6,RbOsO4) - removeed RbOsO4					Superconductivity in the geometrically frustrated pyrochlore RbOs2O6			Laboratory for Solid State Physics, ETH Zurich, 8093 Zurich, Switzerland	Phys.Rev.B, 70(2004)020203	B.Batlogg,J.Karpinski,M.Bruhwiler,N.D.Zhigadlo,S.M.Kazakov		
34512	SSC1310513		Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3Oz	Tl	2	Ba	2	Ca	2	Cu	3													O	z		1	2004																												Tl2223																		K								TC34512																																																																																														1	various O-content obtained by ANN(400C,various O2 pressure)					Effects of excess oxygen content on the hole-carrying CuO2-layers in Tl2(Ba1-xSrx)2Ca2Cu3Oy superconducting oxides			Department of Pure and Applied Chemistry, Faculty of Science and Technology, Tokyo University of Science,		.Chun-K.Loong,J.W.Richardson Jr,K.Takeuchi,M.Matsuzawa,N.Koura,Y.Idemoto		
34513	SSC1310513		Tl2(Ba,Sr)2Ca2Cu3Oz	Tl2Ba1.7Sr0.3Ca2Cu3Oz	Tl	2	Ba	1.7	Sr	0.3	Ca	2	Cu	3											O	z		1	2004																												Tl2223																		K								TC34512																																																																																														1	various O-content obtained by ANN(400C,various O2 pressure)					Effects of excess oxygen content on the hole-carrying CuO2-layers in Tl2(Ba1-xSrx)2Ca2Cu3Oy superconducting oxides			Department of Pure and Applied Chemistry, Faculty of Science and Technology, Tokyo University of Science,		.Chun-K.Loong,J.W.Richardson Jr,K.Takeuchi,M.Matsuzawa,N.Koura,Y.Idemoto		
34514	SSC1310513		Tl2(Ba,Sr)2Ca2Cu3Oz	Tl2Ba1.6Sr0.4Ca2Cu3Oz	Tl	2	Ba	1.6	Sr	0.4	Ca	2	Cu	3											O	z		1	2004																												Tl2223																		K								TC34512																																																																																														1	various O-content obtained by ANN(400C,various O2 pressure)					Effects of excess oxygen content on the hole-carrying CuO2-layers in Tl2(Ba1-xSrx)2Ca2Cu3Oy superconducting oxides			Department of Pure and Applied Chemistry, Faculty of Science and Technology, Tokyo University of Science,		.Chun-K.Loong,J.W.Richardson Jr,K.Takeuchi,M.Matsuzawa,N.Koura,Y.Idemoto		
34515	SSC1310513		Tl2(Ba,Sr)2Ca2Cu3Oz	Tl2Ba1.5Sr0.5Ca2Cu3Oz	Tl	2	Ba	1.5	Sr	0.5	Ca	2	Cu	3											O	z		1	2004																												Tl2223																		K								TC34512																																																																																														1	various O-content obtained by ANN(400C,various O2 pressure)					Effects of excess oxygen content on the hole-carrying CuO2-layers in Tl2(Ba1-xSrx)2Ca2Cu3Oy superconducting oxides			Department of Pure and Applied Chemistry, Faculty of Science and Technology, Tokyo University of Science,		.Chun-K.Loong,J.W.Richardson Jr,K.Takeuchi,M.Matsuzawa,N.Koura,Y.Idemoto		
34516	LES0620149	not s/c	TbxWO3	Tb0.1W1O3	Tb	0.1	W	1																	O	3			1978								1.54																				ABO3																		K																																																																																																							electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34517	LES0620149	Tc=2.47 K at P=20 kbar	NaxWO3	Na0.23W1O3	Na	0.23	W	1																	O	3			1978																												ABO3																		K		2.16					2.16			K/GPa	0.15																																																																																												electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34518	LES0620149	Tc=1.64 K at P=20 kbar	RbxWO3	Rb0.27W1O3	Rb	0.27	W	1																	O	3			1978																												ABO3																		K		1.9					1.9			K/GPa	-0.13																																																																																												electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34519	LES0620149	Tc=1.48 K at P=20 kbar	RbxWO3	Rb0.33W1O3	Rb	0.33	W	1																	O	3			1978																												ABO3																		K		1.76					1.76			K/GPa	-0.14																																																																																												electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34520	LES0620149	dTc/dP = +- 0 E-5 K/bar. Tc=2.89 K at P=20 kbar		Rb0.33W1O3	Rb	0.33	W	1																	O	3			1978																												ABO3																		K		2.89					2.89			K/GPa	0																																																																																												electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34521	LES0620149	Tc=2.26 K at P=20 kbar		Rb0.33W1O3	Rb	0.33	W	1																	O	3			1978																												ABO3																		K		2.45					2.45			K/GPa	-0.095																																																																																												electrolytic process					Superconductivity in the tungsten bronzes				J.Less-Common.Met., 62(1978)149	H.R.Shanks,J.E.Ostenson		
34522	SSC0150753		NaxWO3	Na0.2W1O3	Na	0.2	W	1																	O	3			1974																												ABO3																		K		3.05					3.05	TC34522																																																																																															solid state reaction					Enhancement of the superconducting transition temperature near a phase instability in NaxWO3			Ames Lab	Solid State Commun., 15(1974)753	H.R.Shanks		
34528	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.9Bi0.1O3	Ba	1	Pb	0.9	Bi	0.1															O	3			1980																												BPBO																				2.91					2.91																																																																																					e-3 cm3/C	-2.69						E+21 /cm3	2.15								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34529	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.85Bi0.15O3	Ba	1	Pb	0.85	Bi	0.15															O	3			1980																												BPBO																				8.7					8.7																																		HC34529																																																			e-3 cm3/C	-2.6						E+21 /cm3	2.23								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34530	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.8Bi0.2O3	Ba	1	Pb	0.8	Bi	0.2															O	3			1980																												BPBO																				10.25					10.25																																		HC34530																																																			e-3 cm3/C	-1.25						E+21 /cm3	4.36								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34531	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			1980																												BPBO																				11.7					11.7																																		HC34529																																																			e-3 cm3/C	-1.3						E+21 /cm3	4.33								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34532	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.7Bi0.3O3	Ba	1	Pb	0.7	Bi	0.3															O	3			1980																												BPBO																				11.23					11.23																																																																																					e-3 cm3/C	-1.63						E+21 /cm3	3.41								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34533	APP0220205		Ba(Pb,Bi)O3	Ba1Pb0.65Bi0.35O3	Ba	1	Pb	0.65	Bi	0.35															O	3			1980																												BPBO																				3.93					3.93																																																																																					e-3 cm3/C	-2.07						E+21 /cm3	2.82								Superconductivity in the BaPb1-xBixO3 system				Appl.Phys., 22(1980)205	A.Koma,S.Tanaka,T.D.Thanh		
34534	P070054519	sample with 0.1<x<0.15 in Li1+xTi2O4 was used. (delta-C/gamma*Tc) = 1.78. e-ph = 0.65. G-L = 29.	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		1	2004																												spinel																		K		11.4				0.3	11.4											mT		26.3							T		11							T/K		1.45			HC34534		A		55			A		1600			meV	1.97	4					SP34534			mJ/mol.K2	19.15	sp-heat	657	sp-heat																																		Li2CO3,TiO2		mixture - CAL(750C,20h,in O2) - (Li2Ti2O5+Ti2O3) - SIN(880C,24h,in vac), 15 % excess Li doped					Magnetic field dependence of low-temperature specific heat of the spinel oxide superconductor LiTi2O4			Department of Physics, National Sun Yat Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B, 70(2004)054519	C.P.Sun,F.C.Hsu,H.D.Yang,J.-Y.Lin,M.K.Wu,P.L.Ho,S.Mollah,Y.C.Liao		
34535	P070052502	Raman spectroscopy	NaxCoO2/1.3H2O	Na0.28Co1H2.6O3.3	Na	0.28	Co	1	H	2.6															O	3.3			2004																															A			19.683												K				4.21			4.21																																																																																																samples synthesized from ceramic NaxCO2 using chemical oxidation					Raman spectroscopy study of NaxCoO2 and superconducting NaxCoO2 /yH2O			Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 70(2004)052502	C.J.Nie,H.X.Yang,J.Q.Li,R.Jin,Y.G.Shi,Y.L.Liu		
34536	P070052502	Raman spectroscopy	NaxCoO2/1.3H2O	Na0.29Co1H2.6O3.3	Na	0.29	Co	1	H	2.6															O	3.3			2004																															A			19.804												K				3.91			3.91																																																																																																samples synthesized from ceramic NaxCO2 using chemical oxidation					Raman spectroscopy study of NaxCoO2 and superconducting NaxCoO2 /yH2O			Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 70(2004)052502	C.J.Nie,H.X.Yang,J.Q.Li,R.Jin,Y.G.Shi,Y.L.Liu		
34537	P070052502	Raman spectroscopy	NaxCoO2/1.3H2O	Na0.31Co1H2.6O3.3	Na	0.31	Co	1	H	2.6															O	3.3			2004																															A			19.618												K				4.81			4.81																																																																																																samples synthesized from ceramic NaxCO2 using chemical oxidation					Raman spectroscopy study of NaxCoO2 and superconducting NaxCoO2 /yH2O			Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 70(2004)052502	C.J.Nie,H.X.Yang,J.Q.Li,R.Jin,Y.G.Shi,Y.L.Liu		
34538	P070052502	Raman spectroscopy	NaxCoO2/1.3H2O	Na0.24Co1H2.6O3.3	Na	0.24	Co	1	H	2.6															O	3.3			2004																															A			19.807												K				3.51			3.51																																																																																																samples synthesized from ceramic NaxCO2 using chemical oxidation					Raman spectroscopy study of NaxCoO2 and superconducting NaxCoO2 /yH2O			Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 70(2004)052502	C.J.Nie,H.X.Yang,J.Q.Li,R.Jin,Y.G.Shi,Y.L.Liu		
34539	P070052502	Raman spectroscopy	NaxCoO2/1.3H2O	Na0.26Co1H2.6O3.3	Na	0.26	Co	1	H	2.6															O	3.3			2004																															A			19.832												K				2.71			2.71																																																																																																samples synthesized from ceramic NaxCO2 using chemical oxidation					Raman spectroscopy study of NaxCoO2 and superconducting NaxCoO2 /yH2O			Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 70(2004)052502	C.J.Nie,H.X.Yang,J.Q.Li,R.Jin,Y.G.Shi,Y.L.Liu		
34540	LTP0250177	nominal= LiTi2O3.95. (delta-C/gamma*Tc) = 1.59. Hc(0) = 1970 G. Sp-heat measured for 1<T<25 K.	Li1+xTi2-xO4	Li1Ti2O4	Li	1	Ti	2																	O	4			1976																												spinel			A	8.407														K		11.7					11.7																																																								mJ/mol.K2	21.4	sp-heat	685	sp-heat																																		TiO2,TiO1.5,Li2O3		SIN(750-800 C)					Superconducting and normal state properties of Li1+xTi2-xO4 spinel compounds. II.Low-temperature heat capacity				J.Low Temp.Phys., 25(1976)177	C.A.Luengo,D.C.Johnston,M.B.Maple,R.W.McCallum		
34541	LTP0250177	(delta-C/gamma*Tc) = 1.73. Hc(0) = 1970 G. Sp-heat measured for 1<T<25 K.	Li1+xTi2-xO4	Li1.05Ti1.95O4	Li	1.05	Ti	1.95																	O	4			1976																												spinel			A	8.4														K		12					12																																																								mJ/mol.K2	19.7	sp-heat	630	sp-heat																																		TiO2,TiO1.5,Li2O3		SIN(750-800 C)					Superconducting and normal state properties of Li1+xTi2-xO4 spinel compounds. II.Low-temperature heat capacity				J.Low Temp.Phys., 25(1976)177	C.A.Luengo,D.C.Johnston,M.B.Maple,R.W.McCallum		
34542	LTP0250177	nominal = Li1.1Ti1.9O3.95. (delta-C/gamma*Tc) = 1.4. Sp-heat measured for 1<T<25 K.	Li1+xTi2-xO4	Li1.1Ti1.9O4	Li	1.1	Ti	1.9																	O	4			1976																												spinel			A	8.384														K		9.6					9.6																																																								mJ/mol.K2	10.9	sp-heat	520	sp-heat																																		TiO2,TiO1.5,Li2O3		SIN(750-800 C)					Superconducting and normal state properties of Li1+xTi2-xO4 spinel compounds. II.Low-temperature heat capacity				J.Low Temp.Phys., 25(1976)177	C.A.Luengo,D.C.Johnston,M.B.Maple,R.W.McCallum		
34543	LTP0250177	not s/c. Sp-heat measured for 1<T<25 K.	Li1+xTi2-xO4	Li1.2Ti1.8O4	Li	1.2	Ti	1.8																	O	4			1976																												spinel			A	8.374														K					1																																																										mJ/mol.K2	3.6	sp-heat	650	sp-heat																																		TiO2,TiO1.5,Li2O3		SIN(750-800 C)					Superconducting and normal state properties of Li1+xTi2-xO4 spinel compounds. II.Low-temperature heat capacity				J.Low Temp.Phys., 25(1976)177	C.A.Luengo,D.C.Johnston,M.B.Maple,R.W.McCallum		
34544	LTP0250177	not s/c. gamma = 0 += 0.05 mJ/mol.K2. Sp-heat measured for 1<T<25 K.	Li1+xTi2-xO4	Li1.333Ti1.667O4	Li	1.333	Ti	1.667																	O	4			1976																												spinel			A	8.359														K					1																																																										mJ/mol.K2	0	sp-heat	610	sp-heat																																		TiO2,TiO1.5,Li2O3		SIN(750-800 C)					Superconducting and normal state properties of Li1+xTi2-xO4 spinel compounds. II.Low-temperature heat capacity				J.Low Temp.Phys., 25(1976)177	C.A.Luengo,D.C.Johnston,M.B.Maple,R.W.McCallum		
34545	PRL0783729	not s/c. heavy fermion behaviour. Wilson coefficient=1.7. Koringa ratio = 0.7	LiV2O4	Li1V2O4	Li	1	V	2																	O	4			1997																												spinel																		K					0.01																																																										mJ/mol.K2	420																																												LiV2O4: A Heavy Fermion Transition Metal Oxide				Phys.Rev.Lett., 78(1997)3729	A.L.Goldman,A.V.Mahajan,C.A.Swenson,D.A.Gajewski,D.C.Johnston,E.J.Freeman,F.Borsa,G.M.Luke,J.D.Jorgensen,J.Merrin,K.Kojima,L.L.Miller,M.B.Maple,N.R.Dillery,O.Chmaissem,R.P.Dickey,S.Kondo,T.Gu,Y.J.Uemura		
34546	PHC4080044	impurity phase = BaCuO2. PO4 enter to Cu1 site. broad transition	CaLaBa(Cu,(PO4))3Oz	Ca1La1Ba1Cu2.8P0.2O7	Ca	1	La	1	Ba	1	Cu	2.8	P	0.2											O	7			2004																												La1113			A	3.849	3.88	11.63												K				90			90																																																																																														La2O3,BaCO3,CaCO3,CuO,NH4H2(PO4)	1	mixture - CAL(950C,24h) - SIN(975C,12h,in air) - ANN(575C,24h,in O2) - FC					Preparation and characterization of the superconductor CaLaBaCu2.8(PO4)0.2O6.2 compound			Universidad Nacional Mayor de San Marcos, Lima, Peru	Physica C, 408(2004)44	D.A.Bustamante,G.J.C.Gonzalez,S.J.Flores,V.L.De Los Santos		
34547	PHC4080058	broad transition	(Y,Ca)SrBa(Cu,(BO3))3Oz	Y0.8Ca0.2Sr1Ba1Cu2.8B0.2O7	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.8	B	0.2									O	7			2004																												La1113			A	3.826	3.861	11.561												K				45			45																																																																																														Y2O3,CaCO3,SrCO3,BaO2,CuO,H3BO3	1	mixture - heat(1000C,16h,in air) - SIN ((1000C,16h,in air) - FC					Preparation and characterization of the superconductor [Y0.8Ca0.2]SrBaCu2.8(BO3)0.2O6.4 compound			Universidad Nacional Mayor de San Marcos, Lima, Peru	Physica C, 408(2004)58	B.L.Willems,D.A.Bustamante,G.J.C.Gonzalez,V.H.Barinotto C.,V.L.De Los Santos		
34548	CEM1771072	no Meissner effect below Tc. Tm is ferromag-temp.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8-z	Ru	1	Sr	2	Gd	1	Cu	2													O	8-z		1	2004							131																					Ru1212	P4/mmm		A	3.841		11.5731												K	16						16																																																																																															1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34549	CEM1771072	not s/c	RuSr2TbCu2O8	Ru1Sr2Tb1Cu2O8-z	Ru	1	Sr	2	Tb	1	Cu	2													O	8-z		1	2004																												Ru1212	P4/mmm		A	3.8368		11.5545												K					4.2																																																																																																	1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34550	CEM1771072	not s/c	RuSr2DyCu2O8	Ru1Sr2Dy1Cu2O8-z	Ru	1	Sr	2	Dy	1	Cu	2													O	8-z		1	2004																												Ru1212	P4/mmm		A	3.8309		11.5404												K					4.2																																																																																																	1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34551	CEM1771072	Tm is ferromag-temp. 	RuSr2YCu2O8	Ru1Sr2Y1Cu2O8-z	Ru	1	Sr	2	Y	1	Cu	2													O	8-z		1	2004							145																					Ru1212	P4/mmm		A	3.8275		11.5326												K	28	45					45																																																																																															1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34552	CEM1771072	Tm is ferromag-temp. M-I transition at 22 K.	RuSr2HoCu2O8	Ru1Sr2Ho1Cu2O8-z	Ru	1	Sr	2	Ho	1	Cu	2													O	8-z		1	2004							136																					Ru1212	P4/mmm		A	3.826		11.5299												K					4.2																																																																																																	1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34553	CEM1771072	Tm is ferromag-temp.   semiconductor-like down to 4.2 K.	RuSr2ErCu2O8	Ru1Sr2Er1Cu2O8-z	Ru	1	Sr	2	Er	1	Cu	2													O	8-z		1	2004							143																					Ru1212	P4/mmm		A	3.8209		11.5155												K					4.2																																																																																																	1	precursor(Sr2RRuO6) + CuO, mixture - seal(Au-cell) - SIN(1100-1200C,0.5h, P=5.5GPa)					A systematic study on the crystal structure and properties of RuSr2RCu2O8-z (R=Gd, Tb, Dy, Y, Ho, Er)			aInstitute of Physics and Center for Condensed Matter Physics, Laboratory of Optical Physics, Chinese Academy of Sciences, Beijing , PR China	J.Solid State Chem., 177(2004)1072	C.Q.Jin,F.S.Liu,G.B.Song,G.H.Rao,J.K.Liang,J.Luo,L.T.Yang,Q.L.Liu,X.M.Feng		
34554	P068100507		Gd(Ba,Gd)2Cu3O7	Gd1.05Ba1.95Cu3O6.94	Gd	1.05	Ba	1.95	Cu	3															O	7-z	6.94	1	2003								2.26																			3	Y123			A	3.8571	3.8977	11.7036												K		85					85										30																																																																																					1	CAL(900C,12h, in air) - SIN(940C,24h) - ANN(400C,24h, in O2)					Evidence for an interplay between superconductivity and antiferromagnetism of rare-earth ions in Gd1+xBa2-xCu3O7-z			Institute of Low Temperature and Structure Research, Polish Academy of Sciences,  Wroc?aw, Poland	Phys.Rev.B, 68(2003)10050	K.Rogacki		
34555	P068100507		Gd(Ba,Gd)2Cu3O7	Gd1.15Ba1.85Cu3O6.99	Gd	1.15	Ba	1.85	Cu	3															O	7-z	6.99	1	2003								2.36																			3	Y123			A	3.8662	3.8826	11.6733												K		48					48																																																																																															1	CAL(900C,12h, in air) - SIN(940C,24h) - ANN(400C,24h, in O2)					Evidence for an interplay between superconductivity and antiferromagnetism of rare-earth ions in Gd1+xBa2-xCu3O7-z			Institute of Low Temperature and Structure Research, Polish Academy of Sciences,  Wroc?aw, Poland	Phys.Rev.B, 68(2003)10050	K.Rogacki		
34556	P068100507		Gd(Ba,Gd)2Cu3O7	Gd1.2Ba1.8Cu3O7.03	Gd	1.2	Ba	1.8	Cu	3															O	7-z	7.03	1	2003								2.45																			2	Y123			A	3.8722		11.6553												K		42					42										45																																																																																					1	CAL(900C,12h, in air) - SIN(940C,24h) - ANN(400C,24h, in O2)					Evidence for an interplay between superconductivity and antiferromagnetism of rare-earth ions in Gd1+xBa2-xCu3O7-z			Institute of Low Temperature and Structure Research, Polish Academy of Sciences,  Wroc?aw, Poland	Phys.Rev.B, 68(2003)10050	K.Rogacki		
34557	P068100507		Gd(Ba,Gd)2Cu3O7	Gd1.25Ba1.75Cu3O6.98	Gd	1.25	Ba	1.75	Cu	3															O	7-z	6.98	1	2003								2.4																			2	Y123			A	3.8741		11.6346												K		28					28																																																																																															1	CAL(900C,12h, in air) - SIN(940C,24h) - ANN(400C,24h, in O2)					Evidence for an interplay between superconductivity and antiferromagnetism of rare-earth ions in Gd1+xBa2-xCu3O7-z			Institute of Low Temperature and Structure Research, Polish Academy of Sciences,  Wroc?aw, Poland	Phys.Rev.B, 68(2003)10050	K.Rogacki		
34558	ZPS0760303	inhomogeneous sample. (delta-C/gamma*Tc)= 1.4 . e-ph = 0.74 .	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4			1989																												spinel																		K		12.9					12.9																																																								mJ/mol.K2	2.6	sp-heat	490	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34559	ZPS0760303	(delta-C/gamma*Tc)= 1.57 . e-ph = 0.71 .	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		1	1989																												spinel																		K		12.4					12.4																																																								mJ/mol.K2	3.14	sp-heat	535	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34560	ZPS0760303	(delta-C/gamma*Tc)= 1.66 . e-ph = 0.70 .	Li(Ti,Li)2O4	Li1.04Ti1.96O4	Li	1.04	Ti	1.96																	O	4		1	1989																												spinel																		K		12.1					12.1																																																					SP34558			mJ/mol.K2	2.82	sp-heat	512	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34561	ZPS0760303	(delta-C/gamma*Tc)=1.77  . e-ph = 0.70 .	Li(Ti,Li)2O4	Li1.08Ti1.92O4	Li	1.08	Ti	1.92																	O	4		1	1989																												spinel																		K		11.8					11.8																																																								mJ/mol.K2	2.32	sp-heat	523	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34562	ZPS0760303	(delta-C/gamma*Tc)= 1.40 . e-ph = 0.70 .	Li(Ti,Li)2O4	Li1.12Ti1.88O4	Li	1.12	Ti	1.88																	O	4		1	1989																												spinel																		K		10.4					10.4																																																								mJ/mol.K2	1.94	sp-heat	470	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34563	ZPS0760303	(delta-C/gamma*Tc)= 0.60 . e-ph = 0.64 .	Li(Ti,Li)2O4	Li1.16Ti1.84O4	Li	1.16	Ti	1.84																	O	4		1	1989																												spinel																		K		8.3					8.3																																																								mJ/mol.K2	1.62	sp-heat	476	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34564	ZPS0760303		Li(Ti,Li)2O4	Li1.18Ti1.82O4	Li	1.18	Ti	1.82																	O	4		1	1989																												spinel																		K					1.5																																																										mJ/mol.K2	0.8	sp-heat	470	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34565	ZPS0760303		Li(Ti,Li)2O4	Li1.2Ti1.8O4	Li	1.2	Ti	1.8																	O	4		1	1989																												spinel																		K					1.5																																																										mJ/mol.K2	0.38	sp-heat	432	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34566	ZPS0760303		Li(Ti,Li)2O4	Li1.22Ti1.78O4	Li	1.22	Ti	1.78																	O	4		1	1989																												spinel																		K					1.5																																																										mJ/mol.K2	0.4	sp-heat	426	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34567	ZPS0760303		Li(Ti,Li)2O4	Li1.25Ti1.75O4	Li	1.25	Ti	1.75																	O	4		1	1989																												spinel																		K					1.5																																																										mJ/mol.K2	0.31	sp-heat	441	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34568	ZPS0760303	(delta-C/gamma*Tc)= 1.80 . e-ph = 0.69 .	(Li,Mg)Ti2O4	Li0.98Mg0.02Ti2O4	Li	0.98	Mg	0.02	Ti	2															O	4		1	1989																												spinel																		K		11.9					11.9																																																								mJ/mol.K2	2.72	sp-heat	495	sp-heat																																				solid state reaction					Superconductivity of LiTiO4 and related systems				Z.Phys.B, 76(1989)303	F.Gautier,J.M.Heintz,J.P.Kappler,M.Drillon,O.Durmeyer,R.Kuentzler,Y.Dossmann		
34569	SST0170023	O-content by TGA. R is not zero at 10 K. O-rich phase is responsible to SC.	La2(Cu,V)O4	La2Cu0.985V0.015O4.021	La	2	Cu	0.985	V	0.015															O	4	4.021		2004																												T			A	5.3972	5.3522	13.144												K			40				40																																																																																														La2O3,SrCO3,V2O5,CuO	1	CAL(900C,24h,in air) - SIN(960C,72h) - cool to RT(30C/h).					The doping effect of vanadium in La1.85Sr0.15CuO4+z and La2Cu1-xVxO4+z systems			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing, PR China	Supercond.Sci.Technol., 17(2004)23	C.Dong,G.C.Che,G.D.Liu,H.Chen,L.H.Liu,S.L.Jia,W.W.Huang,Z.X.Zhao		
34570	SST0170023	O-content by TGA. R is not zero at 10 K. O-rich phase is responsible to SC.	La2(Cu,V)O4	La2Cu0.975V0.025O4.032	La	2	Cu	0.975	V	0.025															O	4	4.032		2004																												T			A	5.3992	5.3522	13.144												K			40				40																																																																																														La2O3,SrCO3,V2O5,CuO	1	CAL(900C,24h,in air) - SIN(960C,72h) - cool to RT(30C/h).					The doping effect of vanadium in La1.85Sr0.15CuO4+z and La2Cu1-xVxO4+z systems			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing, PR China	Supercond.Sci.Technol., 17(2004)23	C.Dong,G.C.Che,G.D.Liu,H.Chen,L.H.Liu,S.L.Jia,W.W.Huang,Z.X.Zhao		
34571	SST0170023	O-content by TGA. R is not zero at 10 K. O-rich phase is responsible to SC.	La2(Cu,V)O4	La2Cu0.965V0.035O4.045	La	2	Cu	0.965	V	0.035															O	4	4.045		2004																												T			A	5.3979	5.3528	13.1472												K			40				40																																																																																														La2O3,SrCO3,V2O5,CuO	1	CAL(900C,24h,in air) - SIN(960C,72h) - cool to RT(30C/h).					The doping effect of vanadium in La1.85Sr0.15CuO4+z and La2Cu1-xVxO4+z systems			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing, PR China	Supercond.Sci.Technol., 17(2004)23	C.Dong,G.C.Che,G.D.Liu,H.Chen,L.H.Liu,S.L.Jia,W.W.Huang,Z.X.Zhao		
34572	SST0170023	O-content by TGA. R is not zero at 10 K. O-rich phase is responsible to SC.	La2(Cu,V)O4	La2Cu0.955V0.045O4.056	La	2	Cu	0.955	V	0.045															O	4	4.056		2004																												T			A	5.3979	5.3522	13.1425												K			40				40																																																																																														La2O3,SrCO3,V2O5,CuO	1	CAL(900C,24h,in air) - SIN(960C,72h) - cool to RT(30C/h).					The doping effect of vanadium in La1.85Sr0.15CuO4+z and La2Cu1-xVxO4+z systems			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Science, Beijing, PR China	Supercond.Sci.Technol., 17(2004)23	C.Dong,G.C.Che,G.D.Liu,H.Chen,L.H.Liu,S.L.Jia,W.W.Huang,Z.X.Zhao		
34573	SST0170143	ANN in O2. F substitute for apical-O. Ba:Ca:Cu=2.01:2.02:3.96.	Ba2Ca2Cu3O6F2	Ba2Ca2Cu3F2O6	Ba	2	Ca	2	Cu	3	F	2													O	6		3	2004																												0223																		K				90			90																																																																																																precursor(Ba2Ca2Cu3O7.5 + BaF2,CaF2,CuO,Cu2O) - heat(1150-1250C,0.5-1h,P=4.5GPa) - cool to 1050C(25-50 C/h)					Crystal growth of Ba2Can-1CunO2n(O,F)2 (n = 3 and 4) multi-layered superconductors under high pressure			National Institute of Advanced Industrial Science and Technology (AIST),Tsukuba, Ibaraki, Japan	Supercond.Sci.Technol., 17(2004)143	A.Iyo,K.Tokiwa,M.Hirai,T.Watanabe,Y.Tanaka		
34574	SST0170143	ANN in O2. F substitute for apical-O. Ba:Ca:Cu=2.02:2.99:3.99.	Ba2Ca3Cu4O8F2	Ba2Ca3Cu4F2O8	Ba	2	Ca	3	Cu	4	F	2													O	8		3	2004																												0234																		K				70			70																																																																																																precursor(Ba2Ca2Cu3O7.5 + BaF2,CaF2,CuO,Cu2O) - heat(1150-1250C,0.5-1h,P=4.5GPa) - cool to 1050C(25-50 C/h)					Crystal growth of Ba2Can-1CunO2n(O,F)2 (n = 3 and 4) multi-layered superconductors under high pressure			National Institute of Advanced Industrial Science and Technology (AIST),Tsukuba, Ibaraki, Japan	Supercond.Sci.Technol., 17(2004)143	A.Iyo,K.Tokiwa,M.Hirai,T.Watanabe,Y.Tanaka		
34575	SST0170093	minor phase=Bi-2212	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1Pb1Sr2Ca2Cu3O10	Bi	1	Pb	1	Sr	2	Ca	2	Cu	3											O	10		1	2004																												Bi2223			A	3.6732		35.6176												K	101		106				103.5																																																																																															1	SIN(780-840C,40h,in O2 flow) - slow cool to 500C(20C/h) - ANN(500C,20h,in O2 flow) - C to RT.					Terbium-neodymium co-doping in Bi sites on the BPSCCO bismuth cuprate superconductor			HTc-Ceramic Superconductors Unit, Chemistry Department, Faculty of Science, Tanta University, Tanta, Egypt	Supercond.Sci.Technol., 17(2004)93	Hosny A El-Daly,Khaled M Elsabawy,Morsy M A Sekkina		
34576	SST0170093	minor phase=Bi-2212	(Bi,Pb,Nd,Tb)2Sr2Ca2Cu3O10	Bi0.9Nd0.05Tb0.05Pb1Sr2Ca2Cu3O10	Bi	0.9	Nd	0.05	Tb	0.05	Pb	1	Sr	2	Ca	2	Cu	3							O	10		1	2004																												Bi2223			A	3.6923		35.4463												K	107		115				111																																																																																															1	SIN(780-840C,40h,in O2 flow) - slow cool to 500C(20C/h) - ANN(500C,20h,in O2 flow) - C to RT.					Terbium-neodymium co-doping in Bi sites on the BPSCCO bismuth cuprate superconductor			HTc-Ceramic Superconductors Unit, Chemistry Department, Faculty of Science, Tanta University, Tanta, Egypt	Supercond.Sci.Technol., 17(2004)93	Hosny A El-Daly,Khaled M Elsabawy,Morsy M A Sekkina		
34577	SST0170093	minor phase=Bi-2212	(Bi,Pb,Nd,Tb)2Sr2Ca2Cu3O10	Bi0.8Nd0.1Tb0.1Pb1Sr2Ca2Cu3O10	Bi	0.8	Nd	0.1	Tb	0.1	Pb	1	Sr	2	Ca	2	Cu	3							O	10		1	2004																												Bi2223			A	3.6891		35.3162												K	108		123				115.5																																																																																															1	SIN(780-840C,40h,in O2 flow) - slow cool to 500C(20C/h) - ANN(500C,20h,in O2 flow) - C to RT.					Terbium-neodymium co-doping in Bi sites on the BPSCCO bismuth cuprate superconductor			HTc-Ceramic Superconductors Unit, Chemistry Department, Faculty of Science, Tanta University, Tanta, Egypt	Supercond.Sci.Technol., 17(2004)93	Hosny A El-Daly,Khaled M Elsabawy,Morsy M A Sekkina		
34578	SST0170093	minor phase=Bi-2212	(Bi,Pb,Nd,Tb)2Sr2Ca2Cu3O10	Bi0.6Nd0.2Tb0.2Pb1Sr2Ca2Cu3O10	Bi	0.6	Nd	0.2	Tb	0.2	Pb	1	Sr	2	Ca	2	Cu	3							O	10		1	2004																												Bi2223			A	3.6687		35.1613												K	105		110				107.5																																																																																															1	SIN(780-840C,40h,in O2 flow) - slow cool to 500C(20C/h) - ANN(500C,20h,in O2 flow) - C to RT.					Terbium-neodymium co-doping in Bi sites on the BPSCCO bismuth cuprate superconductor			HTc-Ceramic Superconductors Unit, Chemistry Department, Faculty of Science, Tanta University, Tanta, Egypt	Supercond.Sci.Technol., 17(2004)93	Hosny A El-Daly,Khaled M Elsabawy,Morsy M A Sekkina		
34579	JP01601439	thermal expansion coefficient (temperature scale is wrong)	YBa2Cu3O7	Y1Ba2Cu3O6.93	Y	1	Ba	2	Cu	3															O	7-z	6.93		2004									5.34																			Y123			A	3.817	3.886	11.682												K		92					92																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34580	JP01601439		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9925Zn0.0075O6.92	Y	1	Ba	2	Cu	2.9925	Zn	0.0075													O	7-z	6.92		2004									5.32																			Y123			A	3.819	3.884	11.68												K		88					88																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34581	JP01601439	thermal expansion coefficient (temperature scale is wrong)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.985Zn0.015O6.95	Y	1	Ba	2	Cu	2.985	Zn	0.015													O	7-z	6.95		2004									5.28																			Y123			A	3.817	3.885	11.678												K		86					86																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34582	JP01601439		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.9775Zn0.0225O6.93	Y	1	Ba	2	Cu	2.9775	Zn	0.0225													O	7-z	6.93		2004									5.3																			Y123			A	3.821	3.884	11.673												K		83					83																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34583	JP01601439	thermal expansion coefficient (temperature scale is wrong)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.97Zn0.03O6.98	Y	1	Ba	2	Cu	2.97	Zn	0.03													O	7-z	6.98		2004									5.35																			Y123			A	3.82	3.884	11.67												K		80					80																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34584	JP01601439	thermal expansion coefficient (temperature scale is wrong)	YBa2(Cu,Zn)3O7	Y1Ba2Cu2.94Zn0.06O6.96	Y	1	Ba	2	Cu	2.94	Zn	0.06													O	7-z	6.96		2004									5.36																			Y123			A	3.822	3.886	11.672												K		71					71																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34585	JP01601439		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.88Zn0.12O6.95	Y	1	Ba	2	Cu	2.88	Zn	0.12													O	7-z	6.95		2004									5.32																			Y123			A	3.824	3.887	11.677												K		64					64																																																																																																					Influence of Zn doping on the thermal expansion of the high Tc superconductor Y1Ba2Cu3Oy			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim, India	J.Phys.:Condens.Matter, 16(2004)1439	Ashok Rao		
34586	P070092501	c-axis aligned. SC parameters were obtained by M using Hao & Clem model. Hc(0) = 1.02 T.	TlBa2Ca3Cu4Oz	Tl1Ba2Ca3Cu4Oz	Tl	1	Ba	2	Ca	3	Cu	4													O	z			2004																												Tl1234			A	3.849		19.005												K				128			128																				T		207							T/K		2.24					A			12.6		A			1560																																																									Enhanced two-dimensional properties of the four-layered cuprate high-Tc superconductor TlBa2Ca3Cu4Oy			Pohang University of Science and Technology, Pohang, Republic of Korea	Phys.Rev.B, 70(2004)092501	A.Iyo,H.J.Kim,K.H.Kim,K.Tokiwa,S.I.Lee,T.Watanabe,Y.Tanaka		
34587	PHC4120086	impurity phases=SrTiO3, CeO2	TiSr2(Sm,Ce)2Cu2O10	Ti1Sr2Sm1.6Ce0.4Cu2O10-z	Ti	1	Sr	2	Sm	1.6	Ce	0.4	Cu	2											O	10-z		1	2004																												1222	I4/mmm		A	3.8516		28.314												K			25				25																																																																																															1	mixture - CAL(960-1000C,in air) - heat(1050C,in O2)					Synthesis and structure refinements for (Ti,Cu)Sr2(RE0.8Ce0.2)2Cu2O10-z			Department of Materials Science and Engineering, Muroran Institute of Technology, Muroran, Japan	Physica C, 412-414(2004)86	H.Kito,J.Itoh,T.Ishigaki,Y.Ogasawara		
34588	PHC4120086	impurity phases=SrTiO3, CeO2	TiSr2(Eu,Ce)2Cu2O10	Ti1Sr2Eu1.6Ce0.4Cu2O10-z	Ti	1	Sr	2	Eu	1.6	Ce	0.4	Cu	2											O	10-z		1	2004																												1222	I4/mmm		A	3.8536		28.389												K			20				20																																																																																															1	mixture - CAL(960-1000C,in air) - heat(1050C,in O2)					Synthesis and structure refinements for (Ti,Cu)Sr2(RE0.8Ce0.2)2Cu2O10-z			Department of Materials Science and Engineering, Muroran Institute of Technology, Muroran, Japan	Physica C, 412-414(2004)86	H.Kito,J.Itoh,T.Ishigaki,Y.Ogasawara		
34589	PHC4120027		Ca2CuO2Cl2	Ca2Cu1Cl2.25O2	Ca	2	Cu	1	Cl	2.25															O	2			2004																												T			A	3.8549		15.1207												K				31			31																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34590	PHC4120027		Ca2CuO2Cl2+z	Ca2Cu1Cl2.3O2	Ca	2	Cu	1	Cl	2.3															O	2			2004																												T			A	3.8538		15.124												K				36			36																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34591	PHC4120027		Ca2CuO2Cl2+z	Ca2Cu1Cl2.4O2	Ca	2	Cu	1	Cl	2.4															O	2			2004																												T			A	3.8531		15.1261												K				38			38																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34592	PHC4120027		Ca2CuO2Cl2+z	Ca2Cu1Cl2.5O2	Ca	2	Cu	1	Cl	2.5															O	2			2004																												T			A	3.8531		15.1288												K				38			38																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34593	PHC4120027	not SC	Ca2CuO2Cl2	Ca2Cu1Cl2O2	Ca	2	Cu	1	Cl	2															O	2			2004																												T			A	3.8676		15.0493												K																																																																																																							precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34594	PHC4120027	not SC	Ca2CuO2Cl2+z	Ca2Cu1Cl2.1O2	Ca	2	Cu	1	Cl	2.1															O	2			2004																												T			A	3.8612		15.0925												K																																																																																																							precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34595	PHC4120027	not SC	Ca2CuO2Cl2+z	Ca2Cu1Cl2.15O2	Ca	2	Cu	1	Cl	2.15															O	2			2004																												T			A	3.8563		15.1054												K																																																																																																							precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34596	PHC4120027		Ca2CuO2Cl2+z	Ca2Cu1Cl2.18O2	Ca	2	Cu	1	Cl	2.18															O	2			2004																												T			A	3.8561		15.1086												K				24			24																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34597	PHC4120027		Ca2CuO2Cl2+z	Ca2Cu1Cl2.2O2	Ca	2	Cu	1	Cl	2.2															O	2			2004																												T			A	3.8559		15.1146												K				30			30																																																																																																precursor(Ca2CuO2Cl2, Ca2CuO3) + (CaCl2,CuO,Ca(ClO4)2), mixed - Au-capsule - high pressure(1000C,30min, 6GPa) - Q					Superconductivity at 38 K in the single layer oxychloride without cation substitution			Laboratory of Advanced Solid State Chemistry, Research Center for Elements Science, Institute for Chemical Research, Kyoto University, Uji, Kyoto-fu, Japan	Physica C, 412-414(2004)27	I.Yamada,M.Azuma,M.Takano		
34598	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2YCu2O7	Fe0.5Ba2Y1Cu2.5O7.41	Fe	0.5	Ba	2	Y	1	Cu	2.5													O	7+z	7.41	1	2004																												Cu1212			A	3.871		11.589												K		80					80																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34599	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2NdCu2O7	Fe0.5Ba2Nd1Cu2.5O7.54	Fe	0.5	Ba	2	Nd	1	Cu	2.5													O	7+z	7.54	1	2004																												Cu1212			A	3.918		11.686												K		0					0																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34600	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2SmCu2O7	Fe0.5Ba2Sm1Cu2.5O7.54	Fe	0.5	Ba	2	Sm	1	Cu	2.5													O	7+z	7.54	1	2004																												Cu1212			A	3.897		11.66												K		8					8																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34601	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2EuCu2O7	Fe0.5Ba2Eu1Cu2.5O7.51	Fe	0.5	Ba	2	Eu	1	Cu	2.5													O	7+z	7.51	1	2004																												Cu1212			A	3.893		11.654												K		60					60																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34602	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2GdCu2O7	Fe0.5Ba2Gd1Cu2.5O7.45	Fe	0.5	Ba	2	Gd	1	Cu	2.5													O	7+z	7.45	1	2004																												Cu1212			A	3.881		11.628												K		72					72																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34603	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2DyCu2O7	Fe0.5Ba2Dy1Cu2.5O7.52	Fe	0.5	Ba	2	Dy	1	Cu	2.5													O	7+z	7.52	1	2004																												Cu1212			A	3.875		11.621												K		75					75																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34604	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2HoCu2O7	Fe0.5Ba2Ho1Cu2.5O7.49	Fe	0.5	Ba	2	Ho	1	Cu	2.5													O	7+z	7.49	1	2004																												Cu1212			A	3.872		11.615												K		76					76																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34605	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2ErCu2O7	Fe0.5Ba2Er1Cu2.5O7.46	Fe	0.5	Ba	2	Er	1	Cu	2.5													O	7+z	7.46	1	2004																												Cu1212			A	3.866		11.587												K		72					72																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34606	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2TmCu2O7	Fe0.5Ba2Tm1Cu2.5O7.43	Fe	0.5	Ba	2	Tm	1	Cu	2.5													O	7+z	7.43	1	2004																												Cu1212			A	3.866		11.601												K		60					60																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34607	PHC4110047	O-content by iodometric method	(Fe,Cu)Ba2YbCu2O7	Fe0.5Ba2Yb1Cu2.5O7.45	Fe	0.5	Ba	2	Yb	1	Cu	2.5													O	7+z	7.45	1	2004																												Cu1212			A	3.86		11.585												K		72					72																																																																																																(ambient-P-sample + 5wt%KCl4) - (wrapped in Au-foil) - heat(1000C,0.5h,P=6GPa)					Structure, oxygen content and superconductivity of Fe0.5Cu0.5Ba2RCu2O7+z superconductors synthesized by high pressure			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Zhong Guan Cun, Beijing, PR China	Physica C, 411(2004)47	G.C.Che,H.Chen,K.Q.Li,W.W.Huang,Y.H.Liu,Z.X.Zhao		
34608	PHC4150001		(Ga,Cd)Sr2YCu2O7	Ga0.65Cd0.35Sr2Y1Cu2O7+z	Ga	0.65	Cd	0.35	Sr	2	Y	1	Cu	2											O	7+z			2004																											2	Ga1212			A	3.8438		11.4741												K																																																																																																					Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34609	PHC4150001		(Ga,Cd)Sr2YCu2O7	Ga0.65Cd0.4Sr2Y1Cu2O7+z	Ga	0.65	Cd	0.4	Sr	2	Y	1	Cu	2											O	7+z			2004																											2	Ga1212			A	3.841		11.4873												K			38				38																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34610	PHC4150001		(Ga,Cd)Sr2YCu2O7	Ga0.65Cd0.5Sr2Y1Cu2O7+z	Ga	0.65	Cd	0.5	Sr	2	Y	1	Cu	2											O	7+z			2004																											2	Ga1212			A	3.8374		11.4958												K			44				44																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34611	PHC4150001		(Ga,Cd)Sr2YCu2O7	Ga0.65Cd0.6Sr2Y1Cu2O7+z	Ga	0.65	Cd	0.6	Sr	2	Y	1	Cu	2											O	7+z			2004																											2	Ga1212			A	3.8353		11.5043												K			50				50																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34612	PHC4150001		GaSr2(Y,Ca)Cu2O7	Ga0.65Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.65	Sr	2	Y	0.7	Ca	0.3	Cu	2											O	7+z			2004																											3	Ga1212			A	22.8611	5.4741	5.3901												K	12		35				23.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34613	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.95Cd0.05Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.95	Cd	0.05	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.8707	5.4709	5.3922												K	15		40				27.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34614	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.9Cd0.1Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.9	Cd	0.1	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.8804	5.4655	5.3931												K	21		44				32.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34615	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.85Cd0.15Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.85	Cd	0.15	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.9019	5.464	5.3963												K	26		48				37																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34616	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.8Cd0.2Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.8	Cd	0.2	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.9203	5.4623	5.4031												K	33		50				41.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34617	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.75Cd0.25Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.75	Cd	0.25	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.9269	5.4584	5.3962												K	37		53				45																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34618	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.7Cd0.3Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.7	Cd	0.3	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											3	Ga1212			A	22.9393	5.4532	5.4146												K	40		55				47.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34619	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.65Cd0.35Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.65	Cd	0.35	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											2	Ga1212			A	3.8391		11.4792												K	45		57				51																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34620	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.6Cd0.4Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.6	Cd	0.4	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											2	Ga1212			A	3.8364		11.4924												K	46		59				52.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34621	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.5Cd0.5Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.5	Cd	0.5	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											2	Ga1212			A	3.8327		11.5008												K	54		63				58.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34622	PHC4150001		(Ga,Cd)Sr2(Y,Ca)Cu2O7	Ga0.4Cd0.6Sr2Y0.7Ca0.3Cu2O7+z	Ga	0.4	Cd	0.6	Sr	2	Y	0.7	Ca	0.3	Cu	2									O	7+z			2004																											2	Ga1212			A	3.8303		11.5063												K	58		65				61.5																																																																																														Ga2O3,CdO,SrCO3,Y2O3,CaCO3,CuO	1	pellet - SIN(1000C,12h, in Ar-20%O2 of 1800atm, using HIP)					Structural and superconducting properties of GaSr2YCu2O7 cuprate doped with cadmium			Faculty of Science, Department of Chemistry, Tanta University, Tanta, Egypt	Physica C, 415(2004)1	E.Kandyel		
34623	PHC4150172		RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.4Ce0.6Cu2O9.54	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	z	9.54		2004																											2	Ru1222			A	3.842		28.606												K	27		41				34																																																																		uV/K	16.2																													pellet - ANN(1010C,15h, in N2) - slow cool					Effect of Nb doping on superconducting and magnetic properties of RuSr2(Gd1.5-yEuyCe0.5)Cu2Oz			Department of Physics, Kangwon National University Chunchon, 200-701, Korea	Physica C, 415(2004)172	G.V.M.Williams,H.K.Lee		
34624	PHC4150172		(Ru,Nb)Sr2(Gd,Ce)2Cu2Oz	Ru0.875Nb0.125Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.875	Nb	0.125	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z			2004																											2	Ru1222			A	3.845		28.62												K	27		41				34																																																																																																pellet - ANN(1010C,15h, in N2) - slow cool					Effect of Nb doping on superconducting and magnetic properties of RuSr2(Gd1.5-yEuyCe0.5)Cu2Oz			Department of Physics, Kangwon National University Chunchon, 200-701, Korea	Physica C, 415(2004)172	G.V.M.Williams,H.K.Lee		
34625	PHC4150172		(Ru,Nb)Sr2(Gd,Ce)2Cu2Oz	Ru0.75Nb0.25Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.75	Nb	0.25	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z			2004																											2	Ru1222			A	3.8481		28.655												K	23		36				29.5																																																																		uV/K	21.9																													pellet - ANN(1010C,15h, in N2) - slow cool					Effect of Nb doping on superconducting and magnetic properties of RuSr2(Gd1.5-yEuyCe0.5)Cu2Oz			Department of Physics, Kangwon National University Chunchon, 200-701, Korea	Physica C, 415(2004)172	G.V.M.Williams,H.K.Lee		
34626	PHC4150172		(Ru,Nb)Sr2(Gd,Ce)2Cu2Oz	Ru0.625Nb0.375Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.625	Nb	0.375	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z			2004																											2	Ru1222			A	3.8511		28.679												K	23		36				29.5																																																																																																pellet - ANN(1010C,15h, in N2) - slow cool					Effect of Nb doping on superconducting and magnetic properties of RuSr2(Gd1.5-yEuyCe0.5)Cu2Oz			Department of Physics, Kangwon National University Chunchon, 200-701, Korea	Physica C, 415(2004)172	G.V.M.Williams,H.K.Lee		
34627	PHC4150172		(Ru,Nb)Sr2(Gd,Ce)2Cu2Oz	Ru0.5Nb0.5Sr2Gd1.4Ce0.6Cu2O9.64	Ru	0.5	Nb	0.5	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z	9.64		2004																											2	Ru1222			A	3.8531		28.698												K	24		36				30																																																																		uV/K	23.6																													pellet - ANN(1010C,15h, in N2) - slow cool					Effect of Nb doping on superconducting and magnetic properties of RuSr2(Gd1.5-yEuyCe0.5)Cu2Oz			Department of Physics, Kangwon National University Chunchon, 200-701, Korea	Physica C, 415(2004)172	G.V.M.Williams,H.K.Lee		
34628	PHC2710325	not SC	GaSr2(Tm,Ca)Cu2O7	Ga1Sr2Tm0.75Ca0.25Cu2O7	Ga	1	Sr	2	Tm	0.75	Ca	0.25	Cu	2											O	7		1	1996																											3	Ga1212			A	22.826	5.46	5.374												K				28			28																																		HC34628																																																														(solid state reaction) - packed in Au capsule with KCl3 - ANN(980-1010C, 3h, P=2 GPa)					Composition dependence of the critical temperature in superconducting Ga-1212 GaSr2Tm1-xCaxCu2O7			National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,271(1996)325-330	A. Ono,M. Tsutsumi		
34629	PHC2710325		GaSr2(Tm,Ca)Cu2O7	Ga1Sr2Tm0.7Ca0.3Cu2O7	Ga	1	Sr	2	Tm	0.7	Ca	0.3	Cu	2											O	7		1	1996																											3	Ga1212			A	22.822	5.462	5.373												K				40			40																																																																																																(solid state reaction) - packed in Au capsule with KCl3 - ANN(980-1010C, 3h, P=2 GPa)					Composition dependence of the critical temperature in superconducting Ga-1212 GaSr2Tm1-xCaxCu2O7			National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,271(1996)325-330	A. Ono,M. Tsutsumi		
34630	PHC2710325		GaSr2(Tm,Ca)Cu2O7	Ga1Sr2Tm0.65Ca0.35Cu2O7	Ga	1	Sr	2	Tm	0.65	Ca	0.35	Cu	2											O	7		1	1996																											3	Ga1212			A	22.813	5.459	5.374												K				47			47																																																																																																(solid state reaction) - packed in Au capsule with KCl3 - ANN(980-1010C, 3h, P=2 GPa)					Composition dependence of the critical temperature in superconducting Ga-1212 GaSr2Tm1-xCaxCu2O7			National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,271(1996)325-330	A. Ono,M. Tsutsumi		
34631	PHC2710325		GaSr2(Tm,Ca)Cu2O7	Ga1Sr2Tm0.6Ca0.4Cu2O7	Ga	1	Sr	2	Tm	0.6	Ca	0.4	Cu	2											O	7		1	1996																											3	Ga1212			A	22.787	5.458	5.369												K				51			51																																																																						TP34631																										(solid state reaction) - packed in Au capsule with KCl3 - ANN(980-1010C, 3h, P=2 GPa)					Composition dependence of the critical temperature in superconducting Ga-1212 GaSr2Tm1-xCaxCu2O7			National Institute for Reserch in Inorganic Materials, 1-1 Namiki, Tsukuba 305, Japan	Physica.C,271(1996)325-330	A. Ono,M. Tsutsumi		
34632	PHC2570086	not SC	GaSr2YCu2O7	Ga1Sr2Y1Cu2O7	Ga	1	Sr	2	Y	1	Cu	2													O	7			1996	cm3/mol	0.000058	K.cm3/mol	0.0053			-8.58	387																				Ga1212																		K					5																																																																								TP34632																								Y2O3,CaCO3,SrCO3,CuO,Ga2O3	1	pellet - CAL(900C,iw, in air) - ANN(600C, P=30MPa O2)					NMR and magnetic susceptibility in superconducting and antiferromagnetic Ga-based cuprates Y1-xCaxSr2Cu2GaO7  (0 %$ x %$ 0.3)	01		Institute for Solid State Physics, The University of Tokyo, Roppongi 7-22-1, Minato-ku, Tokyo 106, Japan	Physica.C.257,(1996)86-98	Alexandre I. Rykov,Atsushi Goto,Hiroshi Yasuoka,Tutaka Ueda		
34633	PHC2570086	not SC	GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.9Ca0.1Cu2O7	Ga	1	Sr	2	Y	0.9	Ca	0.1	Cu	2											O	7			1996	cm3/mol	0.000022	K.cm3/mol	0.013			-2.7																					Ga1212																		K					5																																																																								TP34633																								Y2O3,CaCO3,SrCO3,CuO,Ga2O3	1	pellet - CAL(900C,iw, in air) - ANN(600C, P=30MPa O2)					NMR and magnetic susceptibility in superconducting and antiferromagnetic Ga-based cuprates Y1-xCaxSr2Cu2GaO7  (0 %$ x %$ 0.3)	01		Institute for Solid State Physics, The University of Tokyo, Roppongi 7-22-1, Minato-ku, Tokyo 106, Japan	Physica.C.257,(1996)86-98	Alexandre I. Rykov,Atsushi Goto,Hiroshi Yasuoka,Tutaka Ueda		
34634	PHC2570086		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.8Ca0.2Cu2O7	Ga	1	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	7			1996	cm3/mol	0.000075	K.cm3/mol	0.0142			3.85																					Ga1212																		K			35				35																																																																						TP34634																								Y2O3,CaCO3,SrCO3,CuO,Ga2O3	1	pellet - CAL(900C,iw, in air) - ANN(600C, P=30MPa O2)					NMR and magnetic susceptibility in superconducting and antiferromagnetic Ga-based cuprates Y1-xCaxSr2Cu2GaO7  (0 %$ x %$ 0.3)	01		Institute for Solid State Physics, The University of Tokyo, Roppongi 7-22-1, Minato-ku, Tokyo 106, Japan	Physica.C.257,(1996)86-98	Alexandre I. Rykov,Atsushi Goto,Hiroshi Yasuoka,Tutaka Ueda		
34635	PHC2570086		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.7Ca0.3Cu2O7	Ga	1	Sr	2	Y	0.7	Ca	0.3	Cu	2											O	7			1996	cm3/mol	0.000154	K.cm3/mol	0.0107			1.8																					Ga1212																		K			35				35																																																																						TP34635																								Y2O3,CaCO3,SrCO3,CuO,Ga2O3	1	pellet - CAL(900C,iw, in air) - ANN(600C, P=30MPa O2)					NMR and magnetic susceptibility in superconducting and antiferromagnetic Ga-based cuprates Y1-xCaxSr2Cu2GaO7  (0 %$ x %$ 0.3)	01		Institute for Solid State Physics, The University of Tokyo, Roppongi 7-22-1, Minato-ku, Tokyo 106, Japan	Physica.C.257,(1996)86-98	Alexandre I. Rykov,Atsushi Goto,Hiroshi Yasuoka,Tutaka Ueda		
34636	PHC1910174	semicond.	GaSr2YCu2O7	Ga1Sr2Y1Cu2O7	Ga	1	Sr	2	Y	1	Cu	2													O	7			1992																											3	Ga1212			A	22.81	5.4821	5.39												K					10																																																																																																		SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34637	PHC1910174	semicond.	GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.9Ca0.1Cu2O7	Ga	1	Sr	2	Y	0.9	Ca	0.1	Cu	2											O	7			1992																											3	Ga1212			A	22.818	5.4791	5.388												K					10																																																																																																		SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34638	PHC1910174		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.8Ca0.2Cu2O7	Ga	1	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	7			1992																											3	Ga1212			A	22.854	5.4762	5.383												K					3.2																																																																																																		SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34639	PHC1910174		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.7Ca0.3Cu2O7	Ga	1	Sr	2	Y	0.7	Ca	0.3	Cu	2											O	7			1992																											3	Ga1212			A	22.867	5.473	5.378												K	23	25	36				25																																																																																																SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34640	PHC1910174		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.6Ca0.4Cu2O7	Ga	1	Sr	2	Y	0.6	Ca	0.4	Cu	2											O	7			1992																											3	Ga1212			A	22.862	5.4691	5.381												K	35	38					38																																																																																																SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34641	PHC1910174		GaSr2(Y,Ca)Cu2O7	Ga1Sr2Y0.5Ca0.5Cu2O7	Ga	1	Sr	2	Y	0.5	Ca	0.5	Cu	2											O	7			1992																											3	Ga1212			A	22.85	5.4691	5.381												K	35						35																																																																																																SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34642	PHC1910174		(Ga,Cu)Sr2(Y,Ca)Cu2O7	Ga0.9Sr2Y0.6Ca0.4Cu2.1O7	Ga	0.9	Sr	2	Y	0.6	Ca	0.4	Cu	2.1											O	7			1992																												Ga1212																		K	35	41	49				41																																																																																																SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34643	PHC1910174	two step transition	(Ga,Cu)Sr2(Y,Ca)Cu2O7	Ga0.8Sr2Y0.6Ca0.4Cu2.2O7	Ga	0.8	Sr	2	Y	0.6	Ca	0.4	Cu	2.2											O	7			1992																												Ga1212																		K	23	42	53				42																																																																																																SIN(1000C24h,1 atm-O2) - ANN(1000C,5h, in Ar-20%O2 of 1800 atm using HIP					"SUPERCONDUCTIVITY IN GA-BASED ""1212""CUPRATES"	199202			PHYSICA C,191(1992)174	H.YAMAUCHI,KOH-ICHI KUBO,SATOSHI TAKANO,SEIJI ADACHI	GA,CU,SR,Y,CA,O	
34645	PHC4170017	as-synthesized	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.36	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.36	1	2004																												M1212			A	3.826		11.386												K					2																																																																																																Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34646	PHC4170017	ANN(800C,24h,in N2)-ANN(300C,24h,in O2)	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.32	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.32	1	2004																												M1212			A	3.8228		11.383												K					2																																																																																																Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34647	PHC4170017	ANN(800C,24h,in N2)-ANN(300C,24h,in O2) -ANN(350C,24h,in 58 atm O2. Fe-site by Mossbauer.	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O6+z	Fe	1	Sr	2	Y	1	Cu	2													O	6+z		1	2004																												M1212			A	3.8128		11.335												K				42			42																																																																																														Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34648	PHC4170017	ANN(800C,24h,in N2)-ANN(300C,24h,in O2) -ANN(350C,24h,in 100 atm O2. Fe-site by Mossbauer.	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O6+z	Fe	1	Sr	2	Y	1	Cu	2													O	6+z		1	2004																												M1212			A	3.8112		11.33												K				48			48																																																																																														Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34649	PHC4170017	ANN(800C,24h,in N2)-ANN(300C,24h,in O2) -ANN(350C,24h,in 195 atm O2. Fe-site by Mossbauer.	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.68	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.68	1	2004	cm3/g	0.0000026			myuB/mol	3.3	-34																					M1212			A	3.8103		11.327												K				56			56																																																																																														Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34650	PHC4170017	ANN(350C,24h,in 195 atm O2)	FeSr2YCu2Oz	Fe1Sr2Y1Cu2O7.6	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.6	1	2004																												M1212			A	3.8115		11.337												K					2																																																																																																Y2O3,SrCO3,CuO,Fe2O3	1	mixture - CAL(900C,24h, in air) - pellet - SIN(1000C,24h, in air)					Redistribution of Fe ion and superconductivity of FeSr2YCu2O6+y system		OX34645	Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka , Japan	Physica C, 417(2004)17	H.Yasuoka,I.Kakeya,J.Suzuki,K.Kadowaki,T.Mochiku,Y.Hata,Y.Mihara,e.Kita		
34651	PHC4170033	semiconductor	(Y,Pr)BaCu3O7	Y0.4Pr0.6Ba2Cu3O7	Y	0.4	Pr	0.6	Ba	2	Cu	3													O	7		1	2004																												Y123	Pmmm		A	3.869	3.901	11.7063												K					3																																																																																																Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34652	PHC4170033	semiconductor	(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1.8Sr0.2Cu3O7	Y	0.4	Pr	0.6	Ba	1.8	Sr	0.2	Cu	3											O	7		1	2004																												Y123	Pmmm		A	3.845	3.898	11.6759												K					3																																																																				uV/K	103			TP34652																								Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34653	PHC4170033	semiconductor	(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1.6Sr0.4Cu3O7	Y	0.4	Pr	0.6	Ba	1.6	Sr	0.4	Cu	3											O	7		1	2004																												Y123	Pmmm		A	3.844	3.879	11.6356												K					3																																																																				uV/K	86			TP34653																								Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34654	PHC4170033	semiconductor	(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1.4Sr0.6Cu3O7	Y	0.4	Pr	0.6	Ba	1.4	Sr	0.6	Cu	3											O	7		1	2004																												Y123	Pmmm		A	3.86	3.868	11.5957												K					3																																																																				uV/K	51			TP34654																								Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34655	PHC4170033		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1.2Sr0.8Cu3O7	Y	0.4	Pr	0.6	Ba	1.2	Sr	0.8	Cu	3											O	7		1	2004																												Y123	P4/mmm		A	3.852		11.5659												K	5		26				15.5																																																																		uV/K	31			TP34655																								Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34656	PHC4170033		(Y,Pr)(Ba,Sr)2Cu3O7	Y0.4Pr0.6Ba1Sr1Cu3O7	Y	0.4	Pr	0.6	Ba	1	Sr	1	Cu	3											O	7		1	2004																												Y123	P4/mmm		A	3.849		11.5461												K	14		32				23																																																																		uV/K	23			TP34656																								Y2O3,Pr6O11,SrCO3,BaCO3,CuO	1	mixture - CAL(900,910,915,925C, 24h) - pellet - ANN(920C,40h,in O2 flow) - ANN(600C,24h,in O2)					Induction of superconductivity in Y0.4Pr0.6Ba2-xSrxCu3O7 system with increasing Sr substitution		OX34651	Superconductivity and Cryogenics Division, National Physical Laboratory, K.S. Krishnan Marg, New Delhi, India	Physica C, 417(2004)33	A.Gupta,A.V.Narlikar,D.Buddhikot,H.Kishan,M.A.Ansari,R.B.Saxena,R.Rawat,S.K.Malik,V.Ganesan,V.P.S.Awana		
34657	PHC4170063	spin gap temp. = 61.4 K	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	2004																												Y123			A	3.8797	3.8174	11.6667												K	40.5	44.7					44.7																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34658	PHC4170063	spin gap temp. =71.8  K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.99Gd0.01O7-z	Y	1	Ba	2	Cu	2.99	Gd	0.01													O	7-z		1	2004																												Y123			A	3.8781	3.8155	11.6629												K	42.9	44.4					44.4																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34659	PHC4170063	spin gap temp. = 57.5 K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.98Gd0.02O7-z	Y	1	Ba	2	Cu	2.98	Gd	0.02													O	7-z		1	2004																												Y123			A	3.8803	3.8174	11.6659												K	41.9	42.5					42.5																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34660	PHC4170063	spin gap temp. = 69.5 K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.97Gd0.03O7-z	Y	1	Ba	2	Cu	2.97	Gd	0.03													O	7-z		1	2004																												Y123			A	3.8819	3.8194	11.6704												K	38.6	40.4					40.4																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34661	PHC4170063	spin gap temp. = 70.4 K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.95Gd0.05O7-z	Y	1	Ba	2	Cu	2.95	Gd	0.05													O	7-z		1	2004																												Y123			A	3.8778	3.8161	11.6599												K	43.3	44.8					44.8																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34662	PHC4170063	spin gap temp. = 75.5 K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.9Gd0.1O7-z	Y	1	Ba	2	Cu	2.9	Gd	0.1													O	7-z		1	2004																												Y123			A	3.8777	3.8162	11.6539												K	33.1	33.7					33.7																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34663	PHC4170063	spin gap temp. = 79.1 K	YBa2(Cu,Gd)3O7	Y1Ba2Cu2.85Gd0.15O7-z	Y	1	Ba	2	Cu	2.85	Gd	0.15													O	7-z		1	2004																												Y123			A	3.8818	3.8212	11.6681												K	43.3	44.1					44.1																																																																																														Y2O3,BaCO3,CuO,Gd2O3	1	mixture - preheat(930C,24h) - slip form - SIN(930C,24h,in air) - cool to 350C(1C/min) in O2 flow - ANN(350C,24h)					Structure and spin gap in YBa2Cu3-xGdxO7-z superconductors		OX34657	Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	Physica C, 417(2004)63	G.Liu,J.Du,J.Gao,J.S.Liu,S.S.Jiang,S.Xu,X.S.Wu		
34664	PHC3410429		(Hg,Ti)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Ti0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Ti	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8426		29.229												K				38			38										20																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34665	PHC3410429		(Hg,V)Sr2(Gd,Ce)2Cu2Oz	Hg0.75V0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	V	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8566		29.126												K				47			47										11																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34666	PHC3410429		(Hg,Cr)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Cr0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Cr	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8573		29.122												K																																																																																																							two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34667	PHC3410429		(Hg,Mo)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Mo0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Mo	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.842		29.209												K				70			70										21																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34668	PHC3410429		(Hg,W)Sr2(Gd,Ce)2Cu2Oz	Hg0.75W0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8327		29.15												K	48		75	75			75										21																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34669	PHC3410429		(Hg,Re)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Re0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Re	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8455		29.14												K				50			50										15																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34670	PHC3410429		(Hg,W)Sr2(Sm,Ce)2Cu2Oz	Hg0.75W0.25Sr2Sm1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Sm	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8462		29.182												K				56			56										25																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34671	PHC3410429		(Hg,W)Sr2(Eu,Ce)2Cu2Oz	Hg0.75W0.25Sr2Eu1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8386		29.167												K				65			65										24																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34672	PHC3410429		(Hg,W)Sr2(Dy,Ce)2Cu2Oz	Hg0.75W0.25Sr2Dy1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Dy	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8161		29.087												K				71			71										22																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34673	PHC3410429		(Hg,W)Sr2(Ho,Ce)2Cu2Oz	Hg0.75W0.25Sr2Ho1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Ho	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8124		29.043												K				64			64										14																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34674	PHC3410429		(Hg,W)Sr2(Er,Ce)2Cu2Oz	Hg0.75W0.25Sr2Er1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Er	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222			A	3.8058		29.008												K				60			60										32																																																																																						two-step reaction. precursor(Sr2R1.5Ce0.5Cu2Oz). Then, mixed with HgO+M-oxides. packed in Au-capsule. then HIP(1100C,2 GPa, 2h) - Q					Superconductivity at 75 K in Hg-1222 cuprates: (Hg,M)Sr2(Ln,Ce)2Cu2Oz (M=Ti, V, Cr, Mo, W, Re; Ln=Sm-Er)		OX34664	SRL, ISTEC, Shinonome, Koto-ku, Tokyo, Japan	Physica C, 341-348(2000)429	A.Yamamoto,E.Kandyel,S.Tajima		
34675	P070174514	impurity phases = CeO2, Sr2CuWO6	(Hg,W)Sr2(Ce,Eu)3Cu2O11	Hg0.7W0.3Sr2Ce2.01Eu0.99Cu2O11+z	Hg	0.7	W	0.3	Sr	2	Ce	2.01	Eu	0.99	Cu	2									O	11+z			2004																												Hg1232																		K				26			26																																																																																																precursor(Sr:(Ce,Eu):Cu=2:3:2). mixed with HgO + WO3. packed in Au-capsule, then HIP(1100C, 30 min)					High-Tc superconductivity in three-fluorite-layer copper oxides. I. (Hg,W)Sr2(Ce,Eu)3Cu2O11+z		OX34675	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174514	H.Yamauchi,M.Karppinen,T.Motohashi,T.Nagai,T.Watanabe,Y.Matsui		
34676	P070174514	impurity phases = CeO2, Sr2CuWO6. R not zero at 4.2 K. three-fluorite layer S/C.	(Hg,W)Sr2(Ce,Eu)3Cu2O11	Hg0.7W0.3Sr2Ce1.74Eu1.26Cu2O11+z	Hg	0.7	W	0.3	Sr	2	Ce	1.74	Eu	1.26	Cu	2									O	11+z			2004																												Hg1232	P4/mmm		A	3.839		17.33												K			34	33			33										59																																																																																						precursor(Sr:(Ce,Eu):Cu=2:3:2). mixed with HgO + WO3. packed in Au-capsule, then HIP(1100C, 30 min)					High-Tc superconductivity in three-fluorite-layer copper oxides. I. (Hg,W)Sr2(Ce,Eu)3Cu2O11+z		OX34675	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174514	H.Yamauchi,M.Karppinen,T.Motohashi,T.Nagai,T.Watanabe,Y.Matsui		
34677	P070174514	main phase = (Hg,W)-1212	(Hg,W)Sr2(Ce,Eu)3Cu2O11	Hg0.7W0.3Sr2Ce1.5Eu1.5Cu2O11+z	Hg	0.7	W	0.3	Sr	2	Ce	1.5	Eu	1.5	Cu	2									O	11+z			2004																												Hg1222																		K				45			45																																																																																																precursor(Sr:(Ce,Eu):Cu=2:3:2). mixed with HgO + WO3. packed in Au-capsule, then HIP(1100C, 30 min)					High-Tc superconductivity in three-fluorite-layer copper oxides. I. (Hg,W)Sr2(Ce,Eu)3Cu2O11+z		OX34675	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174514	H.Yamauchi,M.Karppinen,T.Motohashi,T.Nagai,T.Watanabe,Y.Matsui		
34678	P070174515	impurity phase = CeO2	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.8338		16.98												K					4.2																																																																																																CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34679	P070174515	oxidize with 12.5 mol % Ag2O2. impurity phase = Ag, CeO2.	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.8311		16.95												K				12.1			12.1																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34680	P070174515	oxidize with 25 mol % Ag2O2. impurity phase = Ag, CeO2	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.8311		16.933												K				33.4			33.4																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34681	P070174515	oxidize with 50 mol % Ag2O2. impurity phase = CeO2	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.8305		16.926												K				50.9			50.9																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34682	P070174515	oxidize with 75 mol % Ag2O2. impurity phase = CeO2	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.828		16.918												K				51.7			51.7																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34683	P070174515	oxidize with 100 mol % Ag2O2. impurity phase = CeO2, unknown	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z			2004																												Cu1232			A	3.8292		16.917												K				52.9			52.9																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34684	P070174515		(Cu,Mo)Sr2YCu2O7	Mo0.25Sr2Y1Cu2.75O7+z	Mo	0.25	Sr	2	Y	1	Cu	2.75													O	7+z			2004																												Cu1212			A			11.4762												K				87.6			87.6																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34685	P070174515	as-synthesized. not SC.	(Cu,Mo)Sr2YCu2O7	Mo0.25Sr2Y1Cu2.75O7+z	Mo	0.25	Sr	2	Y	1	Cu	2.75													O	7+z			2004																												Cu1212			A			11.535												K					4.2																																																																																																CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34686	P070174515		(Cu,Mo)Sr2(Y,Ce)2Cu2O9	Mo0.25Sr2Y1.5Ce0.5Cu2.75O9+z	Mo	0.25	Sr	2	Y	1.5	Ce	0.5	Cu	2.75											O	9+z			2004																												Cu1222			A			14.2272												K				35.2			35.2																																																																																														CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air) - oxidize(5 GPa, 500C, 30 min with Ag2O2)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34687	P070174515	as-synthesized. not SC.	(Cu,Mo)Sr2(Y,Ce)2Cu2O9	Mo0.25Sr2Y1.5Ce0.5Cu2.75O9+z	Mo	0.25	Sr	2	Y	1.5	Ce	0.5	Cu	2.75											O	9+z			2004																												Cu1222			A			14.2835												K					4.2																																																																																																CuO,MoO3,SrCO3,CeO2,Y2O3		mixture - CAL(950C,in air) - SIN(1020C,in air)					High-Tc superconductivity in three-fluorite-layer copper oxides. II. (Cu,Mo)Sr2(Ce,Y)3Cu2O11+z		OX34678	Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 70(2004)174515	H.Yamauchi,M.Karppinen,T.Nagai,Y.Matsui,Y.Morita		
34688	P070184523	resistivities show T^2 dependence. Hc defined as the peak of AC-sus. anisotropy(from R) = 2. RRRc=35, RRR(ab)=93.	Ag5Pb2O6	Ag5Pb2O6	Ag	5	Pb	2																	O	6		3	2004																													P31m		A	5.9324		6.4105											Kagome layered structure	K				0.048			0.048																				Oe		3																															SP34688			mJ/mol.K2	3.42		186	sp-heat											uOhm.cm								1.5	9.7														AgNO3,Pb(NO3)2		mixture - put into AlO3 crucible - heat(80C,3h,in air) - heat(300C,8h) - heat(394C,5h) - keep(48h) - FC to RT.					Nonlinear temperature dependence of resistivity in single crystal Ag5Pb2O6		OX-34688	Department of Physics, Graduate School of Science, Kyoto University, Kyoto, Japan	Phys.Rev.B, 70(2004)184523	S.Yonezawa,Y.Maeno		
34689	PHC3990001	Hc1 from M-H curve. Anisotropy factor (from Hc1) = 165.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2003																												Bi2212																		K		87					87											Oe			1.7	280																			HIR34689																																																												BiO3,PbO,SrCO3,CaCO3,CuO		heat(1000C) - cool to 830C(2h/h). Pb evaporation is suppressed by (Sr,Ca)O layer formed on the cap surface.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
34690	PHC3990001	Hc1 from M-H curve. Anisotropy factor (from Hc1) = 24.5. no structural modulation.	(Bi,Pb)2Sr2CaCu2O8	Bi1.6Pb0.6Sr2Ca1Cu2O8+z	Bi	1.6	Pb	0.6	Sr	2	Ca	1	Cu	2											O	8+z		3	2003																												Bi2212																		K		91					91											Oe			4	98																																																																															BiO3,PbO,SrCO3,CaCO3,CuO		heat(1000C) - cool to 830C(2h/h). Pb evaporation is suppressed by (Sr,Ca)O layer formed on the cap surface.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
34691	PHC3990001	Hc1 from M-H curve. Anisotropy factor (from Hc1) = 25. no structural modulation.	(Bi,Pb)2Sr2CaCu2O8	Bi1.2Pb0.8Sr2Ca1Cu2O8+z	Bi	1.2	Pb	0.8	Sr	2	Ca	1	Cu	2											O	8+z		3	2003																												Bi2212																		K		93					93											Oe			8	200																																																																															BiO3,PbO,SrCO3,CaCO3,CuO		heat(1000C) - cool to 830C(2h/h). Pb evaporation is suppressed by (Sr,Ca)O layer formed on the cap surface.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
34692	JPS0732912	small amount of OsO2,Os	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		1	2004																												pyrochlore																		K		9.62					9.62	TC34692		K/GPa	0.67																																																																																																	High Pressure Effects on Superconductivity in the beta-Pyrochlore Oxides AOs2O6 (A = K, Rb, Cs)		OX-34692	Institute for Solid States Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 73(2004)2912	S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
34693	JPS0732912		RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		1	2004																												pyrochlore																		K		6.29					6.29			K/GPa	0.78																																																																																																	High Pressure Effects on Superconductivity in the beta-Pyrochlore Oxides AOs2O6 (A = K, Rb, Cs)		OX-34692	Institute for Solid States Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 73(2004)2912	S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
34694	JPS0732912		CsOs2O6	Cs1Os2O6	Cs	1	Os	2																	O	6		1	2004																												pyrochlore																		K		3.26					3.26			K/GPa	0.75																																																																																																	High Pressure Effects on Superconductivity in the beta-Pyrochlore Oxides AOs2O6 (A = K, Rb, Cs)		OX-34692	Institute for Solid States Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 73(2004)2912	S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
34695	MAT0404542	PENET estimated from Meissner volume. COHERE calculated from PENET.	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		1	2004																												pyrochlore																		K		6.3					6.3	TC34695		K/GPa	0.9																																A		74			A		5200																																																			OsO2,Rb2O		mixture - evacuated tube - heat(600C,24h) - remove RbOsO4 using HCl 10% solution.					Pressure effects on the transition temperature and the magnetic field penetration depth in the pyrochlore superconductor RbOs2O6		OX-34695	Laboratory for Neutron Scattering, ETH Zurich and Paul Scherrer Institut, Villigen PSI, Switzerland	cond-mat/0404542	D.G.Eshchenko,D.Gavillet,H.Keller,J.Karpinski,N.D.Zhigadlo,R.Brutsch,R.Khasanov,S.M.Kazakov		
34696	P070214502	under doped. O-content not measured. Tc(max)=  K(P=10.5GPa).	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2004																												Bi2212																		K		48					48	TC34696		K/GPa	1.5																																																																																												self-flux method in high thermal gradient using Bi:Sr:Ca:Cu=2:2:1:2.					High-pressure phase diagram of Bi2Sr2CaCu2O8+z single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 70(2004)214502	C.Kendziora,Ho-Kwang Mao,R.J.Hemley,V.V.Struzhkin,Xiao-Jia Chen		
34697	P070214502	under doped. O-content not measured. Tc(max)=  K(P=10.5GPa).	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2004																												Bi2212																		K		86					86			K/GPa	1.3																																																																																												self-flux method in high thermal gradient using Bi:Sr:Ca:Cu=2:2:1:2.					High-pressure phase diagram of Bi2Sr2CaCu2O8+z single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 70(2004)214502	C.Kendziora,Ho-Kwang Mao,R.J.Hemley,V.V.Struzhkin,Xiao-Jia Chen		
34698	P070214502	under doped. O-content not measured. Tc(max)=  K(P=10.5GPa).	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	2004																												Bi2212																		K		60					60			K/GPa																																																																																													self-flux method in high thermal gradient using Bi:Sr:Ca:Cu=2:2:1:2.					High-pressure phase diagram of Bi2Sr2CaCu2O8+z single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 70(2004)214502	C.Kendziora,Ho-Kwang Mao,R.J.Hemley,V.V.Struzhkin,Xiao-Jia Chen		
34699	PR04109551	R(ab) and Rc measured for P < 20 kbar.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z		3	1990																												Bi2212																		K	81.5	83					83			K/GPa	1.5																																																																																												flux method using CuO flux and Bi:Sr:Ca:Cu = 2:2:1:3					High-pressure study of Bi2Sr2CaCu2O8 single crystals		OX-34699	Institute of Physics of the University, Zagrev, Yugoslavia	Phys.Rev.B, 41(1990)9551	B.Keszei,L.Forro,V.Ilakovac		
34700	P070214505	C=a*T^2 term, a= 0.463 mj/mol.K3. lattice term, beta= 0.186 mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0).	(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		3	2004																												T																		K		27.4					27.4																																																								mJ/mol.K2	2.19																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34701	P070214505	C=a*T^2 term, a= 0.177 mj/mol.K3. lattice term, beta= 0.120 mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0).	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2004																												T																		K		36.1					36.1																																																								mJ/mol.K2	1.9																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34702	P070214505	C=a*T^2 term, a= 0.065 mj/mol.K3. lattice term, beta= 0.137 mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0). 1/8 problem.	(La,Sr)2CuO4	La1.89Sr0.11Cu1O4	La	1.89	Sr	0.11	Cu	1															O	4		3	2004																												T																		K		29.3					29.3																																																								mJ/mol.K2	1.7																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34703	P070214505	C=a*T^2 term, a= 0.158 mj/mol.K3. lattice term, beta= 0.145  mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0).	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4		3	2004																												T																		K		24.4					24.4																																																								mJ/mol.K2	2.64																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34704	P070214505	C=a*T^2 term, a= 0.131 mj/mol.K3. lattice term, beta= 0.177 mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0).	(La,Sr)2CuO4	La1.925Sr0.075Cu1O4	La	1.925	Sr	0.075	Cu	1															O	4		3	2004																												T																		K		15.6					15.6																																																								mJ/mol.K2	3.72																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34705	P070214505	C=a*T^2 term, a= -0.077 mj/mol.K3. lattice term, beta= 0.157 mj/mol.K4. Debye-T not given. gamma = T-linear term below Tc(H=0).	(La,Sr)2CuO4	La1.931Sr0.069Cu1O4	La	1.931	Sr	0.069	Cu	1															O	4		3	2004																												T																		K		12					12																																																								mJ/mol.K2	4.06																																							TSFZ method					Electronic specific heat and low-energy quasiparticle excitations in the superconducting state of La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 70(2004)214505	Fang Zhou,Hai-Hu Wen,Jiwu Xiong,S.Komiya,Tao Xiang,Wenxing Ti,Xuefeng Sun,Y.Ando,Zhi-Yong Liu		
34706	PHC4170077	solubility limit: x=0.1 for Gd1+xBa2-xCu3O7. ArPA process is effective for high-Tc and high Jc.	Gd(Ba,Gd)2Cu3O7	Gd1.1Ba1.9Cu3O7	Gd	1.1	Ba	1.9	Cu	3															O	7		1	2005									7.003																			Y123	Pmmm	47	A	3.8504	3.8918	11.655												K		93					93																																																																																																SIN - Q - post annealing in Ar flow(ArPA) - ANN(400C,in O2)					Solubility and superconductivity of Gd1+xBa2 xCu3O7-z compounds (x = -0.1, 0, 0.05, 0.1, 0.15 and 0.2)		OX34706	Tokyo University of Marine Science and Technology, 2-1-6, Etchu-jima, Koto-ku, Tokyo 135-8533, Japan	Physica C, 417(2005)77	A.Hu,C.Xu,I.Hirabayashi,M.Izumi,N.Sakai		
34707	PHC4180043	O-content by TGA.  el-density by P-annihilation = 1.028	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.84	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.84	1	2005																												Y123			A	3.8269	3.8881	11.6539												K		82					82																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34708	PHC4180043	O-content by TGA. O2-ANN at 400 C. el-density by P-annihilation = 1.029	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.78	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.78	1	2005																												Y123			A	3.8372	3.8828	11.6612												K		84.2					84.2																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34709	PHC4180043	O-content by TGA. O2-ANN at 450 C. el-density by P-annihilation = 1.014	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.59	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.59	1	2005																												Y123			A	3.855	3.8728	11.6701												K		67.3					67.3																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34710	PHC4180043	O-content by TGA. O2-ANN at 500 C. el-density by P-annihilation = 1.017	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.51	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.51	1	2005																												Y123			A	3.8439	3.8531	11.6729												K		62.6					62.6																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34711	PHC4180043	O-content by TGA. O2-ANN at 600 C. el-density by P-annihilation = 1.005	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.49	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.49	1	2005																												Y123			A	3.85		11.6773												K		61					61																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34712	PHC4180043	O-content by TGA. O2-ANN at 700 C. el-density by P-annihilation = 0.997	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.41	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.41	1	2005																												Y123			A	3.8481		11.6924												K		32.4					32.4																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34713	PHC4180043	O-content by TGA. O2-ANN at 800 C. el-density by P-annihilation = 1.000	(Y,Ca)Ba2Cu3O7	Y0.8Ca0.2Ba2Cu3O6.32	Y	0.8	Ca	0.2	Ba	2	Cu	3													O	7-z	6.32	1	2005																												Y123			A	3.8369		11.7453												K		25.8					25.8																																																																																														Y2O3,CaCO3,BaCO3,CuO	1	mixture - CAL(900C,48h,in air) - SIN(920C,24h,in flowing O2) - ANN(400-600C,24h,in O2) - FC to RT, different ANN for different O-content.					Local electronic structure, O-T phase transition and oxygen content in Y0.8Ca0.2Ba2Cu3Oy (y = 6.84 - 6.32) high-Tc superconductors		OX-34707	Department of Physics, Shanghai University, Shanghai 200436, PR China	Physica C, 418(2005)43	C.Chi,C.Jing,F.Liu,J.Zhang,L.Li,S.Cao,W.Li		
34715	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.875Na0.125Cu1Br2O2	Ca	1.875	Na	0.125	Cu	1	Br	2													O	2		1	2005																												T																		K					5																																																																																																		Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34716	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.85Na0.15Cu1Br2O2	Ca	1.85	Na	0.15	Cu	1	Br	2													O	2		1	2005																												T			A	3.8617		17.0218												K		10					10																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34717	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.825Na0.175Cu1Br2O2	Ca	1.825	Na	0.175	Cu	1	Br	2													O	2		1	2005																												T																		K		10.5					10.5																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34718	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.8Na0.2Cu1Br2O2	Ca	1.8	Na	0.2	Cu	1	Br	2													O	2		1	2005																												T																		K		11					11																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34719	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.75Na0.25Cu1Br2O2	Ca	1.75	Na	0.25	Cu	1	Br	2													O	2		1	2005																												T																		K		18					18																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34720	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.7Na0.3Cu1Br2O2	Ca	1.7	Na	0.3	Cu	1	Br	2													O	2		1	2005																												T																		K		16.5					16.5																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34721	PHC4190032	apical site = Br	(Ca,Na)2CuO2Br2	Ca1.65Na0.35Cu1Br2O2	Ca	1.65	Na	0.35	Cu	1	Br	2													O	2		1	2005																												T																		K		18					18																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34722	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.9Na0.1Cu1Br1Cl1O2	Ca	1.9	Na	0.1	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K					5																																																																																																		Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34723	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.875Na0.125Cu1Br1Cl1O2	Ca	1.875	Na	0.125	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		15					15																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34724	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.85Na0.15Cu1Br1Cl1O2	Ca	1.85	Na	0.15	Cu	1	Br	1	Cl	1											O	2		1	2005																												T			A	3.8563		16.1376												K		19					19																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34725	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.825Na0.175Cu1Br1Cl1O2	Ca	1.825	Na	0.175	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		23					23																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34726	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.8Na0.2Cu1Br1Cl1O2	Ca	1.8	Na	0.2	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		19					19																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34727	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.75Na0.25Cu1Br1Cl1O2	Ca	1.75	Na	0.25	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		19					19																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34728	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.7Na0.3Cu1Br1Cl1O2	Ca	1.7	Na	0.3	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		23.5					23.5																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34729	PHC4190032	apical site = BrCl.	(Ca,Na)2CuO2BrCl	Ca1.65Na0.35Cu1Br1Cl1O2	Ca	1.65	Na	0.35	Cu	1	Br	1	Cl	1											O	2		1	2005																												T																		K		24					24																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34730	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.94Na0.06Cu1Cl2O2	Ca	1.94	Na	0.06	Cu	1	Cl	2													O	2		1	2005																												T																		K					5																																																																																																		Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34731	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.9Na0.1Cu1Cl2O2	Ca	1.9	Na	0.1	Cu	1	Cl	2													O	2		1	2005																												T																		K		13					13																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34732	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.875Na0.125Cu1Cl2O2	Ca	1.875	Na	0.125	Cu	1	Cl	2													O	2		1	2005																												T																		K		25					25																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34733	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.85Na0.15Cu1Cl2O2	Ca	1.85	Na	0.15	Cu	1	Cl	2													O	2		1	2005																												T			A	3.8508		15.0895												K		25					25																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34734	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.825Na0.175Cu1Cl2O2	Ca	1.825	Na	0.175	Cu	1	Cl	2													O	2		1	2005																												T																		K		26					26																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34735	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.8Na0.2Cu1Cl2O2	Ca	1.8	Na	0.2	Cu	1	Cl	2													O	2		1	2005																												T																		K		27.5					27.5																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34736	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.75Na0.25Cu1Cl2O2	Ca	1.75	Na	0.25	Cu	1	Cl	2													O	2		1	2005																												T																		K		26.5					26.5																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34737	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.7Na0.3Cu1Cl2O2	Ca	1.7	Na	0.3	Cu	1	Cl	2													O	2		1	2005																												T																		K		27.7					27.7																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34738	PHC4190032	apical site = Cl.	(Ca,Na)2CuO2Cl2	Ca1.65Na0.35Cu1Cl2O2	Ca	1.65	Na	0.35	Cu	1	Cl	2													O	2		1	2005																												T																		K		28					28																																																																																																Ca2CuO2Cl2/Ca2CuO2Br2 were prepared by solid reaction. ADD(NaCl,NaBr,NaClO3), high-pressure synthesis(1000-1200C,5.5 GPa,10-30 min)					Superconducting phase diagram in Ca2-xNaxCuO2Cl2-yBry			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 419(2005)32	H.Kawashima,J.Akimitsu,T.Suzuki,Y.Zenitani		
34739	JPS0732940	gap from Knight shift of Cd<111> NMR. Hc2(0.1K) = 0.4 T	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2004																												pyrochlore																		K		1					1																				T					0.4			0.1																				2.3	6																																															chemical transport reaction					Decrease in <111>Cd Knight shift in superconducting Cd2Re2O7: Evidence for spin-singlet pairing			Advanced Science Research Center, JERI, Tokai,Ibaraki, Japan	J.Phys.Soc.Jpn, 73(2004)2940	H.Murakawa,H.Ohno,H.Sakai,K.Ishida,K.Kitagawa,K.Yoshimura,M.Kato,R.E.Walstedt,S.Kambe,Y.Tokunaga		
34740	L087187001	O-content not determined. Tc determined by SP-heat.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7		3	2001																												pyrochlore			A	10.226														K		0.97					0.97																																																								mj/mol.K2	15.1	SP-heat	458	SP-heat																																				mixture - pellet - heat(800-900C,70h, in quartz ampoule)					Superconductivity at 1 K in Cd2Re2O7			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 87(2001)187001	J.Yamaura,M.Hanawa,T.Sakakibara,T.Tayama,Y.Muraoka,Z.Hiroi		
34741	PHC3990001	modulation = 4.88b. anisotropy(30K) = 165.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			2003																												Bi2212																		K				87			87											Oe	M-H curve				30	1.7	280																HIR34741																																																												BiO3,PbO,SrCO3,CaCO3,CuO,		vertical 3-zone furnace. cooling rate = 2C/h from 1000C to 830C. T-gradient = 3 C/cm.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
34742	PHC3990001	effective Pb-content x = 0.33 by EDX. modulation = 8.44b. anisotropy(30K) = 24.5.	(Bi,Pb)2Sr2CaCu2O8	Bi1.4Pb0.6Sr2Ca1Cu2O8	Bi	1.4	Pb	0.6	Sr	2	Ca	1	Cu	2											O	8			2003																												Bi2212																		K				91			91											Oe	M-H curve				30	4	98																																																																												BiO3,PbO,SrCO3,CaCO3,CuO,		vertical 3-zone furnace. cooling rate = 2C/h from 1000C to 830C. T-gradient = 3 C/cm.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
34743	PHC3990001	effective Pb-content x = 0.39 by EDX. no-modulation. anisotropy(30K) = 25.	(Bi,Pb)2Sr2CaCu2O8	Bi1.2Pb0.8Sr2Ca1Cu2O8	Bi	1.2	Pb	0.8	Sr	2	Ca	1	Cu	2											O	8			2003																												Bi2212																		K				93			93											Oe	M-H curve				30	8	200																																																																												BiO3,PbO,SrCO3,CaCO3,CuO,		vertical 3-zone furnace. cooling rate = 2C/h from 1000C to 830C. T-gradient = 3 C/cm.					Modulation-free phase in heavily Pb-doped (Bi,Pb)2212 crystals		OX-34689	University of Geneva (DPMC), 24 quai E. Ansermet, Geneva CH-1211, Switzerland	Physica C, 399(2003)1	E.Walker,G.van Tendeloo,N.Clayton,N.Musolino,R.Flukiger,S.Bals		
40000	PR0950333	isotope In(112)-99.5% pure	Sn(112)	Sn1	Sn	1																							1954																																														K		3.809					3.809																				Oe		312.3							Oe/K		144.3																																																																						Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40001	PR0950333	isotope In(118)-99.19% pure	Sn(118)	Sn1	Sn	1																							1954																																														K		3.7452					3.7452																				Oe		303.3							Oe/K		139.8																																																																						Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40002	PR0950333	isotope In(124)-99.91% pure	Sn(124)	Sn1	Sn	1																							1954																																														K		3.6657					3.6657																				Oe		298.4							Oe/K		141																																																																						Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40003	PR0950333	natural Tl	Tl	Tl1	Tl	1																							1954																																														K		2.3917					2.3917																				Oe		172.8							Oe/K		125.8			HC40003																																																																			Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40004	PR0950333	isotope Tl(205)-99.73% pure. M=205.02. isotope effect  apha = 0.49 +- 10%(standard deviation)	Tl(205)	Tl1	Tl	1																							1954																																														K		2.3861					2.3861						0.49	Tl	99.73												Oe		171.4							Oe/K		129.2			HC40004																																																																			Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40005	PR0950333	isotope Tl(203)-99.74% pure. M=203.33	Tl(203)	Tl1	Tl	1																							1954																																														K		2.3956					2.3956																				Oe		170							Oe/K		130.5			HC40005																																																																			Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40006	PR0950333	natural In.	In	In1	In	1																							1954																																														K		3.4178					3.4178																				Oe		275							Oe/K		142.2			HC40006																																																																			Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40007	PR0950333	99.999 Hg in Pyrex capillary.	Hg	Hg1	Hg	1																							1954																																														K		4.1596					4.1596																				Oe		404.5							Oe/K		196.2			HC40007																																																																			Threshold field properties of some superconductors				Phys.Rev., 95(1954)333	E.Maxwell,O.S.Lutes		
40008	PR1040549	commercial high purity Pb(M=207.27). isotope shift measured for six samples with different M. alpha = 0.52+-0.04	Pb	Pb1	Pb	1																							1956																																														K		7.22					7.22						0.52	Pb																																																																																									purity= 99.999%					Isotope effect in superconducting lead				Phys.Rev., 104(1956)549	R.R.Hake,D.E.Mapother,D.L.Decker		
40009	PR0860235	M<av>=113.58. Tc by mutual inductance.	Sn	Sn1	Sn	1																							1952																																														K		3.8082					3.8082																				Oe		312.4							Oe/K		147																																																																						Superconductivity of the isotope of tin				Phys.Rev., 86(1952)235	E.Maxwell		
40010	PR0860235	M<av>=118.70.Tc by mutual inductance. isotope shift measured for 113.58<M<123.01	Sn	Sn1	Sn	1																							1952																																														K		3.7419					3.7419						0.505	Sn																																																																																														Superconductivity of the isotope of tin				Phys.Rev., 86(1952)235	E.Maxwell		
40011	PR0860235	M<av>=118.05. Tc by mutual inductance.	Sn	Sn1	Sn	1																							1952																																														K		3.7444					3.7444																				Oe		307.7																																																																															Superconductivity of the isotope of tin				Phys.Rev., 86(1952)235	E.Maxwell		
40012	PR0840691	M<av>=200.7	Hg	Hg1	Hg	1																							1951																																														K		4.173					4.173	TC40012					0.504	Hg													Oe		419																																																																															The isotope effect in superconductivity. I. Mercury				Phys.Rev., 84(1951)691	C.A.Reynolds,B.Serin,L.B.Nesbitt		
40013	PLA0240340		Be22Mo	Be22Mo1	Be	22	Mo	1																					1967																																														K		2.51					2.51						0.23	Mo																																																																																									arc-melting					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40014	PLA0240340		Be22W	Be22W1	Be	22	W	1																					1967																																														K		4.12					4.12																																																																																																arc-melting					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40015	PLA0240340		Be22Tc	Be22Tc1	Be	22	Tc	1																					1967																																														K		5.21					5.21																																																																																																arc-melting					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40016	PLA0240340		Be22Re	Be22Re1	Be	22	Re	1																					1967																																														K		9.65					9.65						0.23	Mo																																																																																									arc-melting					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40017	PLA0240340		Mo	Mo1	Mo	1																							1967																																														K		0.902				0.001	0.902						0.37	Mo																																																																																									Mo isotope purified by boiling out in UHV by EBM.					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40018	PLA0240340		Tc	Tc1	Tc	1																							1967																																														K		7.79					7.79																																																																																																					Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
40019	PR1550364	as-received. RRR=33.	Tc	Tc1	Tc	1																							1967																																														K	7.82		8.25				8.035																																																																							uOhm.cm							0.65			9	22																			Superconducting properties of technetium				Phys.Rev., 155(1967)364	S.T.Sekura,R.H.Kernohan,G.R.Love		
40020	PR1550364	ANN(1800C,1h). RRR=97. G-L = 0.92. Debye-T from J.Less-Common Metals, 12(1967)29.	Tc	Tc1	Tc	1																							1967																																														K				7.77			7.77																				kOe		2.62							kOe/K		3.25			HC40020																									411																																										Superconducting properties of technetium				Phys.Rev., 155(1967)364	S.T.Sekura,R.H.Kernohan,G.R.Love		
40021	PR1550364	ANN(1000C, in H2). RRR=120. sharp transition.	Tc	Tc1	Tc	1																							1967																																														K		7.71		7.73			7.71																																																																														0.15			9	18.4																			Superconducting properties of technetium				Phys.Rev., 155(1967)364	S.T.Sekura,R.H.Kernohan,G.R.Love		
40022	PR0104572	beta-Ga is metastable. alpha-Ga is not SC at 2K. (gapene) is estimated from Hc.	beta-Ga	Ga1	Ga	1																							1974																																														K		6.07					6.07						0.43	Ga		0.073											Oe		540							Oe/K		155																	3.49								erg/cm3.K2	1340	estimated from Hc																																						See Phys.Rev.B, 7(1973)166					Isotope effect in superconducting beta-phase gallium				Phys.Rev.B, 10(1974)4572	Hugo Parr		
40023	PR0103818	H-content determined by (p-v-t) method. inverse isotope effect i.e.  Tc(PdH) < Tc(PdD).	PdHx	H0.965Pd1	H	0.965	Pd	1																					1974																																														K		6.45					6.45	TC40023																																																																																															hydriding (5N-Pd + H2 or D2, T=RT, p=<5kbar) - Q to Liq.N2.					Concentration dependence of the superconducting transition temperature in PdHx and PdDx				Phys.Rev.B, 10(1974)3818	J.E.Schirber,C.J.M.Northrup,Jr		
40024	PR0103818		PdDx	D0.967Pd1	D	0.967	Pd	1																					1974																																														K		8.14					8.14	TC40023																																																																																															hydriding (5N-Pd + H2 or D2, T=RT, p=<5kbar) - Q to Liq.N2.					Concentration dependence of the superconducting transition temperature in PdHx and PdDx				Phys.Rev.B, 10(1974)3818	J.E.Schirber,C.J.M.Northrup,Jr		
40025	PR0074290		U1-xMox	Mo0.18U0.82	Mo	0.18	U	0.82																					1973																																													gamma-phase	K		2.115					2.115						0.4	U																																																																																									arc-melting					Isotope effect in superconducting gamma-uranium alloys				Phys.Rev.B, 7(1973)4290	J.D.Lindsay,R.W.White,M.C.Tinkle,S.W.Hayter,R.D.Fowler		
40026	PR0024442		natural-Cd	Cd1	Cd	1																							1970																																														K		0.5173					0.5173						0.385	Cd																						Oe/K		91			HC40026																																																																			Isotope effect insuperconducting cadmium				Phys.Rev.B, 2(1970)4442	R.E.Fassnacht,J.R.Dillinger		
40027	PR0024442		Cd(100)	Cd1	Cd	1																							1970																																														K		0.5218					0.5218																													Oe/K		91.9			HC40026																																																																			Isotope effect insuperconducting cadmium				Phys.Rev.B, 2(1970)4442	R.E.Fassnacht,J.R.Dillinger		
40028	PR0024442		Cd(114)	Cd1	Cd	1																							1970																																														K		0.5148					0.5148																													Oe/K		93.3			HC40028																																																																			Isotope effect insuperconducting cadmium				Phys.Rev.B, 2(1970)4442	R.E.Fassnacht,J.R.Dillinger		
40029	PR0024442		Cd(116)	Cd1	Cd	1																							1970																																														K		0.5115					0.5115																													Oe/K		91.3			HC40028																																																																			Isotope effect insuperconducting cadmium				Phys.Rev.B, 2(1970)4442	R.E.Fassnacht,J.R.Dillinger		
40030	P072064520	impurity phase = LaC2 < 15%. TCFIG shows cell-volume(T). (dC/gamma*Tc) = 2.2.	La2C3	C3La2	C	3	La	2																					2005																		GPa		89								Pu2C3			A	8.815													Pu2C3, cI40	K		13.5		13.5		0.1	13.5	LAT40030																																																																																													La(4N),graphite(4N)		arc-melting, ANN(650C,3d) - cool to RT(10C/h)					Structural properties of the sesquicarbide superconductor La2C3 at high pressure			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.B, 72(2005)064520	X.Wang,I.Loa,K.Syassen,R.K.Kremer,A.Simon,M.Hanfland,K.Ahn		
40031	P072064520	SC is not investigated. Sample obtained as impurity phase of La2C3. TCFIG shows cell-volume(T).	LaC2	C2La1	C	2	La	1																					2005																		GPa		76.3								Pu2C3	I4/mmm	139	A	3.9323		6.574																				LAT40031																																																																																													La(4N),graphite(4N)		arc-melting, ANN(650C,3d) - cool to RT(10C/h)					Structural properties of the sesquicarbide superconductor La2C3 at high pressure			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.B, 72(2005)064520	X.Wang,I.Loa,K.Syassen,R.K.Kremer,A.Simon,M.Hanfland,K.Ahn		
40032	APL0842859		Y2C3	C3Y2	C	3	Y	2																					2004																												Pu2C3																		K			17.9	17.3			17.3																				T	linear approx.	43.5							T/K		2.52			HC40032																																																												Y,graphite		mixture(Y:C=2:3.01) - heat(1400C,30 min, P=3.5 GPa) in BN crucible					Superconducting properties of the 18 K phase in yttrium sesquicarbide system			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Appl.Phys.Lett., 84(2004)2859	T.Nakane,T.Mochiku,H.Kito,J.Itoh,M.Nagao,H.Kumakura,Y.Takano		
40033	APL0842859		Y2(C,B)3	Y2C2.9B0.1	Y	2	C	2.9	B	0.1																			2004																												Pu2C3																		K				16.4			16.4																																																																																														Y,graphite,B		mixture - heat(1400C,30 min, P=3.5 GPa) in BN crucible					Superconducting properties of the 18 K phase in yttrium sesquicarbide system			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Appl.Phys.Lett., 84(2004)2859	T.Nakane,T.Mochiku,H.Kito,J.Itoh,M.Nagao,H.Kumakura,Y.Takano		
40034	PR0140128	unstable in air. SC-properties measured without air. Tc, Hc2 measured by ac-sus.	La2C3	C3La2	C	3	La	2																					1976																												Pu2C3																		K				11.1			11.1											Oe	ac-susceptibility	30			22			4.2	T	WHH theory	13.1			9.5			4.2	T/K		1.8			HC40034																						mj/mol.K2	6.1	estimated from dHc2/dT																																						arc-melting in air					Critical-magnetic-field curve of lanthanum sesquicarbide			U. S. Naval Research Laboratory, Washington, D. C. 20375	Phys.Rev.B, 14(1976)128	T. L. Francavilla,F. L. Carter		
40035	P072064521	Incommensurability = 0.133 reciprocal lattice unit	(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	2005	emu/g	0.00000015																										T																		K				29			29																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40036	P072064521		(La,Sr)2CuO4	La1.78Sr0.22Cu1O4	La	1.78	Sr	0.22	Cu	1															O	4		1	2005	emu/g	0.00000023																										T																		K				22			22																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40037	P072064521		(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		1	2005			emu.K/g	0.00000131																								T																		K				14.2			14.2																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40038	P072064521		(La,Sr)2CuO4	La1.74Sr0.26Cu1O4	La	1.74	Sr	0.26	Cu	1															O	4		1	2005			emu.K/g	0.00000353																								T																		K				9.95			9.95																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40039	P072064521		(La,Sr)2CuO4	La1.72Sr0.28Cu1O4	La	1.72	Sr	0.28	Cu	1															O	4		1	2005			emu.K/g	0.00000311																								T																		K				4.98			4.98																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40040	P072064521	Incommensurability = 0.111 reciprocal lattice unit	(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.995Zn0.005O4	La	1.8	Sr	0.2	Cu	0.995	Zn	0.005													O	4		1	2005			emu.K/g	0.00000127																								T																		K				26.1			26.1																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40041	P072064521		(La,Sr)2(Cu,Zn)O4	La1.8Sr0.2Cu0.99Zn0.01O4	La	1.8	Sr	0.2	Cu	0.99	Zn	0.01													O	4		1	2005			emu.K/g	0.00000459																								T																		K				11			11																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40042	P072064521		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.9975Zn0.0025O4	La	1.78	Sr	0.22	Cu	0.9975	Zn	0.0025													O	4		1	2005			emu.K/g	0.00000184																								T																		K				18.5			18.5																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40043	P072064521		(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.995Zn0.005O4	La	1.78	Sr	0.22	Cu	0.995	Zn	0.005													O	4		1	2005			emu.K/g	0.00000259																								T																		K				9.88			9.88																																																																																														La2O3,SrCO3,CuO,ZnO	1	mixture - heat(900C,12h,in air) - pellet - SIN(900C,10h,in air+1150C,10h,in air) - ANN(850C,12h,in flowing O2)					Magnetic properties of the overdoped superconductor La2-xSrxCuO4 with and without Zn impurities			Department of Physics, University of Toronto, Toronto, Ontario, Canada M5S 1A7	Phys.Rev.B, 72(2005)064521	S.Wakimoto,R.J.Birgeneau,A.Kagedan,Hyunkyung Kim,I.Swainson,K.Yamada,H.Zhang		
40044	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8+z	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z			2005																												Bi2212																		K				72			72																				T	WHH theory, dHc2/dT	33.9																			A	from M using Kogan's model and lat-c	2831																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40045	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.9Y0.1Cu2O8+z	Bi	2	Sr	2	Ca	0.9	Y	0.1	Cu	2											O	8+z			2005																												Bi2212																		K				84			84																				T	WHH theory, dHc2/dT	44.4																			A	from M using Kogan's model and lat-c	2861																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40046	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.8Y0.2Cu2O8+z	Bi	2	Sr	2	Ca	0.8	Y	0.2	Cu	2											O	8+z			2005																												Bi2212																		K				91.7			91.7																				T	WHH theory, dHc2/dT	50.4																			A	from M using Kogan's model and lat-c	2880																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40047	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.75Y0.25Cu2O8+z	Bi	2	Sr	2	Ca	0.75	Y	0.25	Cu	2											O	8+z			2005																												Bi2212																		K				92.8			92.8																				T	WHH theory, dHc2/dT	39.9																			A	from M using Kogan's model and lat-c	3107																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40048	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.7Y0.3Cu2O8+z	Bi	2	Sr	2	Ca	0.7	Y	0.3	Cu	2											O	8+z			2005																												Bi2212																		K				89			89																				T	WHH theory, dHc2/dT	29.4																			A	from M using Kogan's model and lat-c	3295																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40049	P072064525	hole conc = 0.213 estimated from Tc using Tallon's eq. PENET is at T/Tc = 0.6.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.6Y0.4Cu2O8+z	Bi	2	Sr	2	Ca	0.6	Y	0.4	Cu	2											O	8+z			2005																												Bi2212																		K				67.8			67.8																				T	WHH theory, dHc2/dT	17.2																			A	from M using Kogan's model and lat-c	3611																																																			Bi2O3,SrCO3,CaCO3,CuO,Y2O3	1	sintering temperature linearly increases from 850C for x=0 to 900C for x=0.5.					Hole concentration dependence of penetration depth and upper critical field in Bi2Sr2(Ca,Y)Cu2O8+z extracted from reversible magnetization			Department of Physics, Pusan National University, Busan 609-735, Korea	Phys.Rev.B, 72(2005)064525	G.C.Kim,M.Cheon,H.Kim,Y.C.Kim,D.Y.Jeong		
40050	P072064527	two gaps, the higher(sigma-band) is in table. the lower(pai-band) is (gap=2.12 meV, GAPENE=1.29)	MgB2	B2Mg1	B	2	Mg	1																				1	2005																												AlB2																		K				38			38																																														meV	6.81	4.16	9																																															high-P and high-T synthesis.					Carbon-substitution dependent multiple superconducting gap of MgB2: A sub-meV resolution photoemission study			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 72(2005)064527	S.Tsuda,T.Yokoya,T.Kiss,T.Shimojima,S.Shin,T.Togashi,S.Watanabe,C.Zhang,C.T.Chen,S.Lee,H.Uchiyama,S.Tajima,N.Nakai,K.Machida		
40051	P072064527	two gaps, the higher(sigma-band) is in table. the lower(pai-band) is (gap=2.03 meV, GAPENE=1.33)	Mg(B,C)2	Mg1B0.96C0.04	Mg	1	B	0.96	C	0.04																		1	2005																												AlB2																		K				35.5			35.5																																														meV	6.1	3.99	9																																															high-P and high-T synthesis.					Carbon-substitution dependent multiple superconducting gap of MgB2: A sub-meV resolution photoemission study			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 72(2005)064527	S.Tsuda,T.Yokoya,T.Kiss,T.Shimojima,S.Shin,T.Togashi,S.Watanabe,C.Zhang,C.T.Chen,S.Lee,H.Uchiyama,S.Tajima,N.Nakai,K.Machida		
40052	P072064527	two gaps, the higher(sigma-band) is in table. the lower(pai-band) is (gap=2.02 meV, GAPENE=1.56)	Mg(B,C)2	Mg1B0.9C0.1	Mg	1	B	0.9	C	0.1																		1	2005																												AlB2																		K				30			30																																														meV	4.82	3.73	9																																															high-P and high-T synthesis.					Carbon-substitution dependent multiple superconducting gap of MgB2: A sub-meV resolution photoemission study			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 72(2005)064527	S.Tsuda,T.Yokoya,T.Kiss,T.Shimojima,S.Shin,T.Togashi,S.Watanabe,C.Zhang,C.T.Chen,S.Lee,H.Uchiyama,S.Tajima,N.Nakai,K.Machida		
40053	P072064527	two gaps, the higher(sigma-band) is in table. the lower(pai-band) is (gap=1.72 meV, GAPENE=1.66)	Mg(B,C)2	Mg1B0.85C0.15	Mg	1	B	0.85	C	0.15																		1	2005																												AlB2																		K				24			24																																														meV	4.22	4.08	9																																															high-P and high-T synthesis.					Carbon-substitution dependent multiple superconducting gap of MgB2: A sub-meV resolution photoemission study			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 72(2005)064527	S.Tsuda,T.Yokoya,T.Kiss,T.Shimojima,S.Shin,T.Togashi,S.Watanabe,C.Zhang,C.T.Chen,S.Lee,H.Uchiyama,S.Tajima,N.Nakai,K.Machida		
40054	P072094504	The hier gap is in table, the lower is 2.3meV. At P=1.13GPa, PENET = 1033 A, (2*gap/kTc) = 1.43 and 4.28 for two gaps. PENET-shift (P=0 to 1.13GPa) = 3.1%.	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K				38.73			38.73				-1.24																																					A	from M using Schonberg eq	1048			meV	7.2	4.31																																																heat(600C,1h+800C,1h+900C,1h, in BN crucible with Ar)					Pressure effect on the magnetic penetration depth in MgB2			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 72(2005)094504	D.Di Castro,R.Khasanov,C.Grimaldi,J.Karpinski,S.M.Kazakov,R.Brutsch,H.Keller		
40055	P072104504	PENET(= 2500 ~ 3000 A, almost independent of H) obtained by muon-SR measurements. Hc2(0)=7.25 T using power law fitting(n=1.15). GAPENE from fitting parameter of PENET(T).	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		1	2005																												pyrochlore			A	10.1137														K				6.32			6.32																				T	WHH theory, dHc2/dT	6							T/K	muon-SR	1.37			HC40055							A	muon-SR	2500					3.47																																														OsO2,RbO2		mixture - pellet - quartz tube - heat(600C,24h). remove impurity phase(RbOsO4) by etching 2h in 10%HCl.					Magnetic penetration depth in RbOs2O6 studied by muon spin rotation			Laboratory for Neutron Scattering, ETH Zurich and Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 72(2005)104504	R. Khasanov,D. G. Eshchenko,D.Di Castro,A.Shengelya,F.La Mattina,A.Maisuradze,C.Baines,H.Luetkens,J.Karpinski,S.M.Kazakov,H.Keller		
40056	P072104506	B<11> enriched sample. LAT-A by NED(T=3K). (dC/gamma*Tc) = 2.0. SP-heat fitting (2 < T < 5 K). GAPENE by SP-heat.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2005																													P4<3>32		A	6.7485														K		7.5					7.5																																																3.94								mj/mol.K2	9	SP-heat	221	SP-heat. beta=1.08 mj/mol.K4																																				two stage arc-melting					Low-temperature specific-heat and neutron-diffraction studies on Li2Pd3B and Li2Pt3B superconductors			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 72(2005)104506	H.Takeya,K.Hirata,K.Yamaura,K.Togano,M.EI Massalami,R.Rapp,F.A.Chaves,B.Ouladdiaf		
40057	P072104506	B<11> enriched sample. LAT-A by NED(T=2K). (dC/gamma*Tc) = 2.0. SP-heat fitting (Tc < T < 5 K). GAPENE by SP-heat.	Li2Pt3B	Li2Pt3B1	Li	2	Pt	3	B	1																		1	2005																													P4<3>32		A	6.7345														K		2.17					2.17																																																3.53								mj/mol.K2	7	SP-heat	228	SP-heat. beta=0.98 mj/mol.K4																																				two stage arc-melting					Low-temperature specific-heat and neutron-diffraction studies on Li2Pd3B and Li2Pt3B superconductors			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 72(2005)104506	H.Takeya,K.Hirata,K.Yamaura,K.Togano,M.EI Massalami,R.Rapp,F.A.Chaves,B.Ouladdiaf		
40058	P072104508		(Pu,U)CoGa5	Pu0.9U0.1Co1Ga5	Pu	0.9	U	0.1	Co	1	Ga	5																	2005							-17																					HoCoGa5			A	4.228		6.778												K				8.4			8.4										100										T	WHH theory, dHc2/dT	8.7																																																																										arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40059	P072104508	30% Ho2CoGa8 type phase	(U,Np)CoGa5	U0.9Np0.1Co1Ga5	U	0.9	Np	0.1	Co	1	Ga	5																	2005							-25																					HoCoGa5			A	4.229		6.776												K				7.2			7.2										5										T	WHH theory, dHc2/dT	3.4																																		mj/mol.K2	120	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40060	P072104508		Pu(Co,Rh)Ga5	Pu1Co0.5Rh0.5Ga5	Pu	1	Co	0.5	Rh	0.5	Ga	5																	2005																												HoCoGa5			A	4.261		6.818												K				15.5			15.5										100										T	WHH theory, dHc2/dT	70																																		mj/mol.K2	190	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40061	P072104508		Pu(Co,Rh)Ga5	Pu1Co0.1Rh0.9Ga5	Pu	1	Co	0.1	Rh	0.9	Ga	5																	2005																												HoCoGa5			A	4.293		6.849												K				10.2			10.2										100										T	WHH theory, dHc2/dT	28																																		mj/mol.K2	120	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40062	P072104508		PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																			2005							-36																					HoCoGa5			A	4.301		6.857												K				8.9			8.9																				T	WHH theory, dHc2/dT	22																																		mj/mol.K2	150	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40063	P072104508		Pu(Co,Fe)Ga5	Pu1Co0.9Fe0.1Ga5	Pu	1	Co	0.9	Fe	0.1	Ga	5																	2005							-53																					HoCoGa5			A	4.23		6.78												K				13.5			13.5																				T	WHH theory, dHc2/dT	64																																		mj/mol.K2	80	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40064	P072104508		Pu(Co,Fe)Ga5	Pu1Co0.8Fe0.2Ga5	Pu	1	Co	0.8	Fe	0.2	Ga	5																	2005																												HoCoGa5			A	4.232		6.78												K				10			10																				T	WHH theory, dHc2/dT	40																																		mj/mol.K2	130	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40065	P072104508	not SC	PuFeGa5	Pu1Fe1Ga5	Pu	1	Fe	1	Ga	5																			2005																												HoCoGa5			A	4.263		6.768												K					2																																																																																																		arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40066	P072104508		Pu(Co,Ni)Ga5	Pu1Co0.9Ni0.1Ga5	Pu	1	Co	0.9	Ni	0.1	Ga	5																	2005							-24																					HoCoGa5			A	4.229		6.779												K				16.6			16.6																				T	WHH theory, dHc2/dT	69																																		mj/mol.K2	142	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40067	P072104508	not SC	PuNiGa5	Pu1Ni1Ga5	Pu	1	Ni	1	Ga	5																			2005							-44																					HoCoGa5			A	4.245		6.796												K					2																																																										mj/mol.K2	195	SP-heat																																						arc-melting - wrapped in Ti-foil - ANN(850C,1w, in vac)					Tuning of the electronic properties in PuCoGa5 by actinide (U, Np) and transition-metal (Fe, Rh, Ni) substitutions			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)104508	P.Boulet,E.Colineau,F.Wastin,J.Rebizant,P.Javorsky,G.H.Lander,J.D.Thompson		
40068	P072144504	Tc increases with increasing P. Tc(P=1.5GPa) = 3.2 K. contaminants(Ba6Si46, BaSi2)	Ba24Si100	Ba24Si100	Ba	24	Si	100																					2005																												clathrate			A	14.07														K		1.4					1.4																				T	SP measurement	0.24														A	from Hc2	372								meV	0.212	3.52					SP40068			mj/mol.K2	182	SP-heat	411	SP-heat											mOhm.cm											50														high-pressure synthesis					Superconductivity and physical properties of Ba24Si100 determined from electric transport, specific-heat capacity, and magnetic susceptibility measurements			1Department of Physics, Graduate School of Science, Tohoku University and CREST-JST, 6-3 Aoba Aramaki Aoba-ku, Sendai, Miyagi, Japan	Phys.Rev.B, 72(2005)144504	T.Rachi,H.Yashino,R.Kumashiro,M.Kitajima,K.Kobayashi,K.Yokogawa,K.Murata,N.Kimura,H.Aoki,H.Fukuoka,S.Yamanaka,H.Shimotani,T.Takenobu,Y.Iwasa,T.Sasaki,N.Kobayashi,Y.Miyazaki,K.Saito,F.Guo,K.Kobayashi		
40069	JPC0172453	grain size by SEM. effective PENET = 1.31*PPENET = 2044A. PPENET(P=1.02GPa) = 1305 A(P-dependence)	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	2005																												Y124																		K		80.05					80.05			K/GPa	5																																					A	Schoenberg model		1560																																																		Y2O3,BaCO3,CuO		solid state reaction					Pressure effect on the in-plane magnetic penetration depth in YBa2Cu4O8							
40070	P063224522	98.46% B<11>. T-dependence of lattice parameter measured by NED.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2	P6/mmm	191	A	3.0849		3.5211			(dl/dT)/l	0.0000054		0.0000114						K		39				0.4	39																																																																																														B<11>,Mg		mixture(B<11> + Mg-chunk) - react(800C,1.5h, BN crucible under Ar)					Lattice properties of MgB2 versus temperature and pressure			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B, 63(2001)224522	D.G.Hinks,J.D.Jorgensen,S.Short		
40071	SSC0641445	high-pressure phase(35 kbar). Intercalation. unstable	NaC2	C2Na1	C	2	Na	1																					1987																																														K		5					5																				Oe						1150	490	2.9																																																																		pyrolytic graphite, Na		high pressure synthesis (450-700C, P=45 kbar)					On the superconductivity of graphite intercalation compounds with sodium				SOLID STATE COMMUN.,64(1987)1445	A.D.BRONNIKOV,A.V.PALNICHENKO,I.T.BELASH,O.V.ZHARIKOV		
40072	SSC0641445	high-pressure phase(37 kbar). Intercalation. unstable. Tc = 3.8~2.3	NaC3	C3Na1	C	3	Na	1																					1987																																														K		2.3					2.3																																																																																														pyrolytic graphite, Na		high pressure synthesis (450-700C, P=45 kbar)					On the superconductivity of graphite intercalation compounds with sodium				SOLID STATE COMMUN.,64(1987)1445	A.D.BRONNIKOV,A.V.PALNICHENKO,I.T.BELASH,O.V.ZHARIKOV		
40073	P072174508	anisotropy = 7. weak ferro (Tm=131 K). G-L parameter = 1040.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2005							131																					Ru1212	P4/mbm		A	5.428		11.589												K	39		56				47.5											Oe	RES	12							T	resistance, linear fitting	133												HC40073		A	from Hc2	5																																	mOhm.cm											9.2												RuO2,SrCO3,Gd2O3,CuO	1	mixture - CAL(960C,16h,in air) - pellet - SIN(1015C,10h,in flowing N2) - heat(1060C,10h,in flowing O2) - ANN(1065C,5d,in O2) - FC to RT(15C/h)					Critical fields and the spontaneous vortex state in the weakly ferromagnetic superconductor RuSr2GdCu2O8			Department of Physics, National Tsing Hua University, Hsinchu, Taiwan 300, Republic of China	Phys.Rev.B, 72(2005)174508	C.Y.Yang,B.C.Chang,H.C.Ku,Y.Y.Hsu		
40074	P072180504	type-I SC. Hc2 in TBL shows Hc. G-L parameter = 0.26.	Ag5Pb2O6	Ag5Pb2O6	Ag	5	Pb	2																	O	6		3	2005																																														K				0.0524			0.0524																				Oe		2.19												HC40074		micron	clean limit	11			A	London-PENET	830																																																					crystals grown by self-flux method from (5mmol AgNO3 + 1mmol Pb(NO3)2).					Type-I superconductivity of the layered silver oxide Ag5Pb2O6			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 72(2005)180504	S.Yonezawa,Y.Maeno		
40075	PRL0170917	cubic-to-tetra at 10 K (c/a = 0.9603). Thermodynamic Hc(0) = 57 Oe.	Ag7O8(NO3)	Ag7N1O11	Ag	7	N	1																	O	11		3	1966																															A	9.893														K		1.04					1.04																																																																																																electrolytic oxidation of aqueous solutions of the silver salts AgX.					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
40076	PRL0170917		Ag7O8F	Ag7F1O8	Ag	7	F	1																	O	8		3	1966																															A	9.833														K		0.3					0.3																																																																																																electrolytic oxidation of aqueous solutions of the silver salts AgX.					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
40077	PRL0170917		Ag7O8(BF)4	Ag7B4F4O8	Ag	7	B	4	F	4															O	8		3	1966																															A	9.942														K		0.15					0.15																																																																																																electrolytic oxidation of aqueous solutions of the silver salts AgX.					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
40078	JPS0560419	impurity phase (20%Sb)	YbSb2	Sb2Yb1	Sb	2	Yb	1																					1987	emu/g	-0.00000017	emu.K/g	0.000016			10																								A	4.56	16.7	4.26												K		1.3					1.3																																																																																														Yb(3N),Sb(6N)		heat(1100C,0.5d, in evacuated qualtz ampule) - recrystalize(Bridgeman method)					Superconductivity of YbSb2			Electrotechnical Laboratory, Japan	J.Phys.Soc.Jpn, 56(1987)419	Y.Yamaguchi,S.Waki,K.Mitsugi		
40079	JPS0503245	K-intercalated graphite. Tc (= 152 mK) independent of x for 8.0 < x < 14.7 in CxK. Hc measured for H//c and H//ab.	CxK	C8.1K1	C	8.1	K	1																					1981																																														K				0.152			0.152	TC40079																																																																																															K-intercalated samples using highly oriented pyrolitic graphite.					Potassium concentration dependence of the superconductivity in the potassium graphite intercalation compounds			Department of Chemistry, Kyoto University,Japan	J.Phys.Soc.Jpn, 50(1981)3245	M.Kobayashi,I.Tsujikawa		
40080	PR0454803	RRR > 400. type-I SC. G-L parameter = 0.025. Tc = 353mK by SP-heat). SC-properties show those of type-I SC. (dC/gamma*Tc) = 1.40.	TaSi2	Si2Ta1	Si	2	Ta	1																				3	1992																													P6<2>22																C40,	K		0.345					0.345																				mT	by SP-heat	2.98														micron		2.5			A		630													mj/mol.K2	3.2	SP-heat	465	SP-heat																																				Czochralski method					Superconductivity in TaSi2 single crystal				Phys.Rev.B, 45(1992)4803	U.Gottlieb,J.C.Lasjaunias,J.L.Tholence,O.Laborde,O.Thomas,R.Madar		
40081	P072184503	6.7%RuSb2, 0.6%Sb are included. PENET and COHERE at 0.05 K using modified London eq.(muonSR measurement)	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																		1	2005																													Im-3		A	9.2766													by NED	K		0.97					0.97																																				A	FF-muonSR	345			A	FF-muonSR	3650																																																					flux growth method					Probing the vortex state of PrRu4Sb12 through muon spin rotation and relaxation			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, Oxfordshire, OX11 0QX, United Kingdom	Phys.Rev.B, 72(2005)184503	D.T.Adroja,A.D.Hillier,J.-G.Park,E.A.Coremychkin,K.A.McEwen,N.Takeda,R.Osborn,B.D.Rainford,R.M.Ibberson		
40082	P072184508	P-dependence of lattice const measured. (dB0/dP) = 3.6 (bulk modulus)	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2005																		GPa		76.1								HoCoGa5			A	4.6129		7.5513																																																																																																																			self-flux method					High-pressure structural parameters of the superconductors CeMIn5 and PuMGa5 (M=Co,Rh)			European Commission, JRC, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)184508	P.S.Normile,S.Heathman,M.Idiri,P.Boulet,J.Rebizant,F.Wastin,G.H.Lander,T.Le Bihan,A.Lindbaum		
40083	P072184508	P-dependence of lattice const measured. (dB0/dP) = 4.1 (bulk modulus)	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2005																		GPa		85.4								HoCoGa5			A	4.652		7.542																																																																																																																			self-flux method					High-pressure structural parameters of the superconductors CeMIn5 and PuMGa5 (M=Co,Rh)			European Commission, JRC, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)184508	P.S.Normile,S.Heathman,M.Idiri,P.Boulet,J.Rebizant,F.Wastin,G.H.Lander,T.Le Bihan,A.Lindbaum		
40084	P072184508	P-dependence of lattice const measured. (dB0/dP) = 5.0  (bulk modulus)	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2005																		GPa		89								HoCoGa5			A	4.2354		6.7939																																																																																																																			self-flux method					High-pressure structural parameters of the superconductors CeMIn5 and PuMGa5 (M=Co,Rh)			European Commission, JRC, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)184508	P.S.Normile,S.Heathman,M.Idiri,P.Boulet,J.Rebizant,F.Wastin,G.H.Lander,T.Le Bihan,A.Lindbaum		
40085	P072184508	P-dependence of lattice const measured. (dB0/dP) = 5.0  (bulk modulus)	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2005																		GPa		104								HoCoGa5			A	4.3012		6.8569																																																																																																																			self-flux method					High-pressure structural parameters of the superconductors CeMIn5 and PuMGa5 (M=Co,Rh)			European Commission, JRC, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 72(2005)184508	P.S.Normile,S.Heathman,M.Idiri,P.Boulet,J.Rebizant,F.Wastin,G.H.Lander,T.Le Bihan,A.Lindbaum		
40086	L095117006	nearly hydrostatic pressure. CDW temp = 32 K (at P=0)	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	2005																												2H-NbSe2																		K		7.1					7.1	TC40086		K/GPa	0.25																														HC40086																																																																			Pressure Induced Effects on the Fermi Surface of Superconducting 2H-NbSe2			Instituto de Ciencia de Materiales Nicolas Cabrera, Universidad Autonoma de Madrid, 28049 Madrid, Spain	Phys.Rev.Lett., 95(2005)117006	H.Suderow,V.G.Tissen,J.P.Brison,J.L.Martinez,S.Vieira		
40087	L095167004	small amount of Os. Tc goes to zero at Pc=12+-1 GPa.	CsOs2O6	Cs1Os2O6	Cs	1	Os	2																	O	6			2005																												pyrochlore																	beta-pyrochlore	K		3.3					3.3	TC40087																																																																																															See J.Phys.Soc.Jpn, 73(2004)819					Anomalous Pressure Dependence of the Superconducting Transition Temperature of beta-Pyrochlore AOs2O6 Oxides			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 95(2005)167004	T.Muramatsu,N.Takeshita,C.Terakura,H.Takagi,Y.Tokura,S.Yonezawa,Y.Muraoka,Z.Hiroi		
40088	L095167004	small amount of Os. Tc goes to zero at Pc=7+-0.5 GPa	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6			2005																												pyrochlore																	beta-pyrochlore	K		6.3					6.3	TC40088																																																																																															See J.Phys.Soc.Jpn, 73(2004)819					Anomalous Pressure Dependence of the Superconducting Transition Temperature of beta-Pyrochlore AOs2O6 Oxides			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 95(2005)167004	T.Muramatsu,N.Takeshita,C.Terakura,H.Takagi,Y.Tokura,S.Yonezawa,Y.Muraoka,Z.Hiroi		
40089	L095167004	10 mol%Cd2Os2O7. Tc goes to zero at Pc = 6+-1 GPa.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2005																												pyrochlore																	beta-pyrochlore	K		9.6					9.6	TC40089																																																																																															See J.Phys.Soc.Jpn, 73(2004)819					Anomalous Pressure Dependence of the Superconducting Transition Temperature of beta-Pyrochlore AOs2O6 Oxides			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 95(2005)167004	T.Muramatsu,N.Takeshita,C.Terakura,H.Takagi,Y.Tokura,S.Yonezawa,Y.Muraoka,Z.Hiroi		
40090	L095247004	heavy-fermion. P-induced SC (Pc=12 kbar). SC properties are for P = 16.2 kbar. current(resistivity) //[100].	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2005								1.6																				BaNiSn3	I4mm	107																K		0.9			0		0.9	PH40090																			T	SUS	7							T/K	SUS	12																									mj/mol.K2	120	from JPS0673601													mOhm.cm											420												Ce(4N),Rh(3N),Si(5N)		tetra-arc furnace in Ar. ANN(900C,1w in vac)					Pressure-Induced Superconductivity in Noncentrosymmetric Heavy-Fermion CeRhSi3			Center for Low Temperature Science, Tohoku University, Sendai, Miyagi 980-8578, Japan	Phys.Rev.Lett., 95(2005)247004	N.Kimura,K.Ito,K.Saitoh,Y.Umeda,H.Aoki,T.Terashima		
40091	L089157004	Resistivity rho(T) = rho(0) + A*T^n	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5																		K		2.27					2.27	TC40091																																																																																															self flux method					Superconductivity and Quantum Criticality in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett., 89(2002)157004	V.A.Sidorov,M.Nicklas,P.G.Pagliuso,J.L.Sarrao,Y.Bang,A.V.Balatsky,J.D.Thompson		
40092	L093147005		PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2004																												HoCoGa5			A	4.3012		6.8569												K		8.5					8.5	TC40092																																																																																															flux method					Structural Tuning of Unconventional Superconductivity in PuMGa5 (M=Co,Rh)			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 93(2004)147005	E.D.Bauer,J.D.Thompson,J.L.Sarrao,L.A.Morales,F.Wastin,J.Rebizant,J.C.Griveau,P.Javorsky,P.Boulet,E.Colineau,G.H.Lander,G.R.Stewart		
40093	MMM2720154	Resistivity follows T^1.3 law for Tc < T < 60K	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2004																												HoCoGa5			A	4.2356		6.7939												K		18.5					18.5	TC40093																																																																																																				Pressure dependence of the superconductivity in PuCoGa5			European Commission Joint Research Centre, Institute for Transuranium Elements, Karlsruhe Establishment Postfach 2340, D-76125 Karlsruhe, Germany	J.Magn.Magn.Mater., 272-276(2004)154	J.-C.Griveau,C.Pfleiderer,P.Boulet,J.Rebizant,F.Wastin		
40094	JP017L0121	Two SC peaks appear in SP-heat(Tc1=0.8K, Tc2=0.54K). Fig shows H(T) for two phases. For Tc2, (dHc2/dT)=-2.5 T/K.. (dC/T) = 0.35 J/mol.K2.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		1	2005								2.25																				CePt3B																		K		0.8					0.8																													T/K	SP-heat	9			HC40094																			SP40094			mj/mol.K2	420																																							See Phys.Rev.Lett., 92(2004)27003. ANN(920C) - Q to cold water.					Double specific heat anomaly of the superconducting state of CePt3Si			Chemische Physik und Materialwissenschaften, Universitat Augsburg, 86159 Augsburg, Germany	J.Phys.: Condens.Matter, 17(2005)L121	E.-W.Scheidt,F.Mayr,G.Eickerling,P.Rogl,E.Bauer		
40095	JP017L0311	impurity phase: 7%Si, 6%BaSi2. G-L parameter = 21.	Ba24Si100	Ba24Si100	Ba	24	Si	100																					2005																												clathrate			A	14.063														K		1.55		1.55			1.55										90	Oe	dc magnetization	12			9			0.4	T	ac-SUS	0.35							T/K	ac-SUS	0.27			HC40095		A	GL theory using Hc1, Hc2	310			A	GL theory using Hc1, Hc2	6500																																																			BaSi2,Si		mixture - pellet - (h-BN crucible) - (HP-HT synthesis, 650C,1h, P=1.1 GPa)					Superconductivity in the Ba24Si100 cubic clathrate with sp2 and sp3 silicon bondings			Laboratoire de Physique de la Matiere Condensee et Nanostructures, Batiment Leon Brillouin, Universite Claude Bernard Lyon I and CNRS, F-69622 Villeurbanne cedex, France	J.Phys.: Condens.Matter, 17(2005)L311	R.Vlennois,P.Toulemonde,C.Paulsen,A.San-Miguel		
40096	JP017S0889	P-induced SC. Pcrit = 1.53 GPa. Tc(max) = 2.2 K at P=2.5 GPa. In<115> NQR measured for various P and T.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2005																												HoCoGa5																		K		2.2			0		2.2	PH40096																																																																																															self-flux method					The phase diagram of antiferromagnetism and superconductivity in CeRhIn5: a study of <115>In NQR under pressure			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.: Condens.Matter, 17(2005)S889	S.Kawasaki,M.Yashima,T.Mito,Y.Kawasaki,G.-q Zheng,Y.Kitaoka,D.Aoki,Y.Haga,Y.Onuki		
40097	JP01704539	Two Neel-T(5.2K, 4.5K). P-induced SC. SC properties for P=3.6 GPa. Tc defined as T3. Neel-T goes to zero at P=3.9 GPa.	Ce2Ni3Ge5	Ce2Ni3Ge5	Ce	2	Ni	3	Ge	5																		1	2005								5.2																				U2Co3Si5	Ibam		A	9.815	11.843	5.962												K	0.18		0.26		0		0.22																				T		0.7												HC40097		A		210																																																										arc-melting. ANN(800C,1w, wrapped in Ta-foil, evacuated quartz tube)					A change of electronic state tuned by pressure: pressure-induced superconductivity of the antiferromagnet Ce2Ni3Ge5			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.: Condens.Matter, 17(2005)4539	M.Nakashima,H.Kohara,A.Thamizhavel,T.D.Matsuda,Y.Haga,M.Hedo,Y.Uwatoko,R.Settai,Y.Onuki		
40098	JAP0925494	encapsulated in C-nanocages, average size = 42.6 nm. Hc(T) from Physica C, 425(2005)62	YC2	C2Y1	C	2	Y	1																				1	2002																															A	3.6771		6.1882												K				3.838			3.838											Oe					22			3.5															HC40098																																uV/K	-47																													anode(30wt%Y2O3) - standard direct current arc(20V-110A) under 1.3E+4 Pa H2 pressure					Surface superconductivity and structural analysis of YC2 single crystals encapsulated in carbon nanocages			Department of Environmental Science and Materials Science, College of Science and Engineering, Iwaki Meisei University, Iwaki Fukushima 970-8551, Japan	J.Appl.Phys., 92(2002)5494	Y.Yosida		
40099	JP01707353	partially filled skutterudite. small amount of LaP, RhP2.	LaxRh4P12	La0.6Rh4P12	La	0.6	Rh	4	P	12																			2005																												skutterudite			A	8.0581														K		17					17																																																																																																high-T and high-P synthesis(1100C, 1.5h, P=4GPa)					Superconductivity of the new skutterudite compound LaxRh4P12 prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.: Condens.Matter 17(2005)7353	I.Shirotani,S.Sato,C.Sekine,K.Takeda,I.Inagawa,T.Yagi		
40100	JP01410767	Tc defined as Tc(on) for (dTc/dP). Tc(CDW) = 60 K. (dTc(CDW)/dP) = 42 K/GPa.	ZrTe3	Te3Zr1	Te	3	Zr	1																				3	2002																																														K	1.9		4				2.95			K/GPa	-5.6																																																																																												chemical transport method using iodine as a transport agent					The effect of pressure on the charge-density wave and superconductivity in ZrTe3			Department of Applied Physics, Hokkaido University, Sapporo 060-8623, Japan	J.Phys.: Condens.Matter 14(2002)10767	K.Yamaya,M.Yoneda,S.Yasuzuka,Y.Okajima,S.Tanda		
40101	P068024522	nominal composition=(Ce:Cu:Si = 20.25:40:39.75 ). high-Tc phase. (dTc/dP) with positive sign. Hc(T) was measured. (dC/gamma*Tc) = 0.89	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		1	2003																												ThCr2Si2			A	4.0934		9.9158												K		0.73					0.73																																																																																																levitation melting					Pairing symmetry in two distinct superconducting states of CeCu2Si2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha 5-1-5, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 68(2003)024522	M.Ishikawa,N.Takeda,M.Koeda,M.Hedo,Y.Uwatoko		
40102	P068024522	nominal composition=(Ce:Cu:Si = 20.25:40.25:39.5 ). low-Tc phase. (dTc/dP) with negative sign. Hc(T) was measured. (dC/gamma*Tc) = 1.27	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		1	2003																												ThCr2Si2			A	4.0973		9.9053												K		0.61					0.61																																																																																																levitation melting					Pairing symmetry in two distinct superconducting states of CeCu2Si2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha 5-1-5, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 68(2003)024522	M.Ishikawa,N.Takeda,M.Koeda,M.Hedo,Y.Uwatoko		
40103	JP01704383	Ferromagnetic (FM-Curie temp)	HoFe4P12	Ho1Fe4P12	Ho	1	Fe	4	P	12																		1	2005					uB/Ho	10.43	5																					skutterudite			A	7.7854														K					1.8																																																																																																		high-T and high-P synthesis(1000-1200C, P=4GPa)					Electrical and magnetic properties of new filled skutterudites LnFe4P12 (Ln = Ho, Er, Tm and Yb) and YRu4P12 with heavy lanthanide (including Y) prepared at high pressure				J.Phys.: Condens.Matter 17(2005)4383	I.Shirotani,N.Araseki,Y.Shimaya,R.Nakata,K.Kihou,C.Sekine,T.Yagi		
40104	JP01704383	not SC	ErFe4P12	Er1Fe4P12	Er	1	Fe	4	P	12																		1	2005					uB/Er	9.59																						skutterudite			A	7.7832														K					1.8																																																																																																		high-T and high-P synthesis(1000-1200C, P=4GPa)					Electrical and magnetic properties of new filled skutterudites LnFe4P12 (Ln = Ho, Er, Tm and Yb) and YRu4P12 with heavy lanthanide (including Y) prepared at high pressure				J.Phys.: Condens.Matter 17(2005)4383	I.Shirotani,N.Araseki,Y.Shimaya,R.Nakata,K.Kihou,C.Sekine,T.Yagi		
40105	JP01704383	not SC	TmFe4P12	Tm1Fe4P12	Tm	1	Fe	4	P	12																		1	2005					uB/Tm	6.58																						skutterudite			A	7.7802														K					1.8																																																																																																		high-T and high-P synthesis(1000-1200C, P=4GPa)					Electrical and magnetic properties of new filled skutterudites LnFe4P12 (Ln = Ho, Er, Tm and Yb) and YRu4P12 with heavy lanthanide (including Y) prepared at high pressure				J.Phys.: Condens.Matter 17(2005)4383	I.Shirotani,N.Araseki,Y.Shimaya,R.Nakata,K.Kihou,C.Sekine,T.Yagi		
40106	JP01704383	not SC	YbFe4P12	Yb1Fe4P12	Yb	1	Fe	4	P	12																		1	2005																												skutterudite			A	7.7877														K					1.8																																																																																																		high-T and high-P synthesis(1000-1200C, P=4GPa)					Electrical and magnetic properties of new filled skutterudites LnFe4P12 (Ln = Ho, Er, Tm and Yb) and YRu4P12 with heavy lanthanide (including Y) prepared at high pressure				J.Phys.: Condens.Matter 17(2005)4383	I.Shirotani,N.Araseki,Y.Shimaya,R.Nakata,K.Kihou,C.Sekine,T.Yagi		
40107	JP01704383		YRu4P12	Y1Ru4P12	Y	1	Ru	4	P	12																		1	2005																												skutterudite			A	8.0298														K		8.5					8.5																																																																																																high-T and high-P synthesis(1000-1200C, P=4GPa)					Electrical and magnetic properties of new filled skutterudites LnFe4P12 (Ln = Ho, Er, Tm and Yb) and YRu4P12 with heavy lanthanide (including Y) prepared at high pressure				J.Phys.: Condens.Matter 17(2005)4383	I.Shirotani,N.Araseki,Y.Shimaya,R.Nakata,K.Kihou,C.Sekine,T.Yagi		
40108	PHC2160264		(Hg,Pr)Sr2(Ca,Sr,Pr)Cu2O6	Hg0.4Pr0.8Sr2.4Ca0.4Cu2O6+z	Hg	0.4	Pr	0.8	Sr	2.4	Ca	0.4	Cu	2											O	6+z			1993																												1212																		K				74			74										18																																																																																				HgO,Pr6O11,SrO2,SrCuO2,CaO	1	SIN(800C, in silica tube)					NEW 1212-TYPE SUPERCONDUCTORS WITH A TC UP TO 85 K IN THE SYSTEM HG-PR-SR-CA-CU-O	199311			PHYSICA C,216(1993)264	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU	HG,PR,SR,CA,CU,O	
40109	PHC2160264	oz = nominal value.	(Hg,Pr)Sr2(Ca,Pr)Cu2O6	Hg0.4Pr1.1Sr2Ca0.5Cu2O7.9	Hg	0.4	Pr	1.1	Sr	2	Ca	0.5	Cu	2											O	6+z	7.9		1993																												1212			A	3.8463	3.8018	12.154												K				76			76										35																																																																																				HgO,Pr6O11,SrO2,SrCuO2,CaO	1	SIN(800C, in silica tube)					NEW 1212-TYPE SUPERCONDUCTORS WITH A TC UP TO 85 K IN THE SYSTEM HG-PR-SR-CA-CU-O	199311			PHYSICA C,216(1993)264	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU	HG,PR,SR,CA,CU,O	
40110	PHC2160264	oz = nominal value.	(Hg,Pr)Sr2(Ca,Pr)Cu2O6	Hg0.4Pr1.1Sr2Ca0.5Cu2O6.9	Hg	0.4	Pr	1.1	Sr	2	Ca	0.5	Cu	2											O	6+z	6.9		1993																												1212			A	3.8538	3.8181	12.17												K				60			60										5																																																																																				HgO,Pr6O11,SrO2,SrCuO2,CaO	1	SIN(800C, in silica tube)					NEW 1212-TYPE SUPERCONDUCTORS WITH A TC UP TO 85 K IN THE SYSTEM HG-PR-SR-CA-CU-O	199311			PHYSICA C,216(1993)264	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU	HG,PR,SR,CA,CU,O	
40111	PHC2160257	(Hg,Bi)-1212 phase. homogeneity range is 0.35 < x < 1 in (Ca1-xNdx)-1212	(Hg,Bi)Sr2(Ca,Nd)Cu2Oz	Hg0.5Bi0.5Sr2Ca0.65Nd0.35Cu2Oz	Hg	0.5	Bi	0.5	Sr	2	Ca	0.65	Nd	0.35	Cu	2									O	z			1993																												1212			A	3.8093		12.0654												K				94			94																																																																																														HgO,Bi2O3,SrO2,CaO,CuO,R2O3	1	mixture - press to bars - heat to 900C in quartz tube - slow cool to RT					"A 94 K HG-BASED SUPERCONDUCTOR WITH A ""1212"" STRUCTURE"	199311			PHYSICA C,216(1993)257	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,CA,CU,O,ND,Y,PR	
40112	PHC2160257	(Hg,Bi)-1212 phase	(Hg,Bi)Sr2(Ca,Y)Cu2Oz	Hg0.5Bi0.5Sr2Ca0.65Y0.35Cu2Oz	Hg	0.5	Bi	0.5	Sr	2	Ca	0.65	Y	0.35	Cu	2									O	z			1993																												1212			A	3.7951		12.036												K				93			93																																																																																														HgO,Bi2O3,SrO2,CaO,CuO,R2O3	1	mixture - press to bars - heat to 900C in quartz tube - slow cool to RT					"A 94 K HG-BASED SUPERCONDUCTOR WITH A ""1212"" STRUCTURE"	199311			PHYSICA C,216(1993)257	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,CA,CU,O,ND,Y,PR	
40113	PHC2160257	(Hg,Bi)-1212 phase	(Hg,Bi)Sr2(Ca,Pr)Cu2Oz	Hg0.5Bi0.5Sr2Ca0.65Pr0.35Cu2Oz	Hg	0.5	Bi	0.5	Sr	2	Ca	0.65	Pr	0.35	Cu	2									O	z			1993																												1212			A	3.8051		12.054												K				95			95																																																																																														HgO,Bi2O3,SrO2,CaO,CuO,R2O3	1	mixture - press to bars - heat to 900C in quartz tube - slow cool to RT					"A 94 K HG-BASED SUPERCONDUCTOR WITH A ""1212"" STRUCTURE"	199311			PHYSICA C,216(1993)257	A.MAIGNAN,B.RAVEAU,C.MICHEL,D.PELLOQUIN,G.VAN TENDELOO,M.HERVIEU	HG,BI,SR,CA,CU,O,ND,Y,PR	
40114	PHC2910097	impurity phases: HgSr2CaCu2Oz, HgSr2(Ca,Y)Cu2Oz, (Hg,Ti)Sr2CaCu2Oz. Majority phase = Hg1212, O2-annealed sample.	(Hg,Ti)Sr2(Ca,Y)Cu2Oz	Hg0.75Ti0.25Sr2Ca0.65Y0.35Cu2Oz	Hg	0.75	Ti	0.25	Sr	2	Ca	0.65	Y	0.35	Cu	2									O	z			1997																												1212																		K	50		100				75																																																																																																two step process. precursor + (precursor + HgO) sealed in silica with Hg-vapor, then heat to 850C.					Synthesis, structure and superconductivity of (Hg1-yTiy)Sr2(Ca1-xYx)Cu2Oz	199711		Institute of Materials Science, University of Tsukuba, Ibaraki 305, Japan	Physica.C,291(1997)97-103	E. Kandyel,H. Asano,M. Abou-Sekkina,T. Kamiyama		
40115	PHC2160264		(Hg,Pr)Sr2(Sr,Pr)Cu2Oz	Hg0.4Pr0.6Sr2.7Pr0.3Cu2O6+z	Hg	0.4	Pr	0.6	Sr	2.7	Pr	0.3	Cu	2											O	6+z			1993																												1212																		K				85			85										100																																																																																				HgO,Pr6O11,SrO2,SrCuO2,CaO	1	SIN(800C, in silica tube)					NEW 1212-TYPE SUPERCONDUCTORS WITH A TC UP TO 85 K IN THE SYSTEM HG-PR-SR-CA-CU-O	199311			PHYSICA C,216(1993)264	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU	HG,PR,SR,CA,CU,O	
40116	PHC2160264		(Hg,Pr)Sr2(Sr,Pr)Cu2Oz	Hg0.4Pr0.6Sr2.5Pr0.5Cu2O6+z	Hg	0.4	Pr	0.6	Sr	2.5	Pr	0.5	Cu	2											O	6+z			1993																												1212																		K				74			74										35																																																																																				HgO,Pr6O11,SrO2,SrCuO2,CaO	1	SIN(800C, in silica tube)					NEW 1212-TYPE SUPERCONDUCTORS WITH A TC UP TO 85 K IN THE SYSTEM HG-PR-SR-CA-CU-O	199311			PHYSICA C,216(1993)264	A.MAIGNAN,B.RAVEAU,C.MICHEL,F.GOUTENOIRE,G.VAN TENDELOO,M.HERVIEU	HG,PR,SR,CA,CU,O	
40117	JP01411249	Two step structural transformation, Ts1,Ts2. P-dependence shown in TCFIG. at 2.8 GPa(Ts1,Ts2 =0), Tc goes to max(Tc=3.85 K). (dC/gamma*Tc) = 1.47	Ba6Ge25	Ba6Ge25	Ba	6	Ge	25																				1	2002																												clathrate																		K		0.24					0.24	TC40117																			T	resistivity	0.6							T/K	resistivity	2.9					A		280																																																										rf-melting in Ar					High-pressure studies on a new superconducting clathrate: Ba6Ge25			Max Planck Institute for the Chemical Physics of Solids, Nothnitzer Str. 40, 01187 Dresden, Germany	J.Phys.: Condens.Matter 14(2002)11249	H.Q.Yuan,F.M.Grosche,W.Carrillo-Cabrera,S.Paschen,G.Sparn,M.Baenitz,Yu Grin,F.Steglich		
40118	P072214520	impurity phase = LaPd2Ge2. RRR=24.5	La3Pd4Ge4	La3Pd4Ge4	La	3	Pd	4	Ge	4																			2005																											3	U3Ni4Si4	Immm		A	4.22	4.385	25.003												K				2.75			2.75											Oe	M-H curve	54							T	WHH, resistivity	0.3							T/K		0.16			HC40118		A		330			A		2480																																																			La,Pd,Ge		arc-melting - wrapped in Mo-foil - ANN(1173K,1w, in silica tube)					Superconductivity in the ternary germanide La3Pd4Ge4			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 72(2005)214520	H.Fujii,T.Mochiku,H.Takeya,A.Sato		
40119	P072214523	RRR=105. spark-cut sample. not SC after surface etching. SC maybe induced by spark erosion.	ZrZn2	Zn2Zr1	Zn	2	Zr	1																				3	2005																																														K			0.6				0.6																																																																							uOhm.cm							0.53				55.6												Zr(4N),Zn(6N)		load into Y2O3 crucible - sealed in Ta bomb - heat(1210C) - cool to MP(2C/h) -ANN(500C,72h)					Superconductivity induced by spark erosion in ZrZn2			H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, Bristol BS8 1TL, United Kingdom	Phys.Rev.B, 72(2005)214523	E.A.Yelland,S.M.Hayden,S.J.C.Yates,C.Pfleiderer,M.Uhlarz,R.Vollmer,H.v.Lohneysen,N.R.Bernhoeft,R.P.Smith,S.S.Saxena,N.Kimura		
40120	P072220505	Thermal expansion coeff. changes from + to - at Tc on cooling.	MgB2	B2Mg1	B	2	Mg	1																				1	2005									2.56																			AlB2																		K	38.7			38.7			38.7			K/GPa	-1.07																																																																																												pellet with B < 11 > - heat(800C,30min, P=3GPa)					Negative thermal expansion of MgB2 in the superconducting state and anomalous behavior of the bulk Gruneisen function			Department of Physics, P.O. Box 173840, Montana State University, Bozeman, Montana 59717-3840, USA	Phys.Rev.B, 72(2005)220505	J.J.Neumeier,T.Tomita,M.Debessai,J.S.Schilling,P.W.Barnes,D.G.Hinks,J.D.Jorgensen		
40121	P072224509	gap estimated from PENET. P-dependence of (PENET)^(-2) = 0.60 %/kbar.	ZrB12	B12Zr1	B	12	Zr	1																				3	2005																																														K				6			6	TC40121		K/GPa	-0.225																																					A	powder susceptibility	1400			meV	1.251	4.79																																																single crystal - ground to be powder for PENET measurements. etching in nitric acid.					Anomalous electron-phonon coupling probed on the surface of superconductor ZrB12			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057, Zurich, Switzerland	Phys.Rev.B, 72(2005)224509	R.Khasanov,D.Di Castro,M.Belogolovskii,Yu.Paderno,V.Filippov,R.Brutsch,H.Keller		
40122	P072224510	reversible M measured  for H//c. Physical properties analyzed using Hao & Clem model. G-L = 89.0. Thermodynamic Hc(0) = 1202 Oe.	(Ca,Na)CuO2Cl2	Ca1.82Na0.18Cu1Cl2O2	Ca	1.82	Na	0.18	Cu	1	Cl	2													O	2		3	2005																												T																		K				27			27																				T				16.9					T/K				0.8			A			44.1		A			4380																																																		CaCuO2Cl2,NaClO4,NaCl		mixture - Pt crucible - high pressure synthesis(1150-1200C,30 min,P=5.2 GPa)					Effect of apical oxygen replacement by chlorine on the thermodynamic properties of Ca1.82Na0.18CuO2Cl2 single crystals			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B, 72(2005)224510	Kyung-Hee Kim,Heon-Jung Kim,Jung-Dae Kim,H.-G.Lee,Sung-Ik Lee		
40123	JP016L0255	P-induced SC. Pcr = 4 GPa. SC properties at P = 6.5 GPa. Tc defined as Tc(on). RRR=220.	CeNiGe3	Ce1Ni1Ge3	Ce	1	Ni	1	Ge	3																			2004							-12	5.5																				SmNiGe3	Cmmm	65	A	21.808	4.135	4.168												K			0.48		0		0.48	TC40123																			T		2												HC40123		A		130																		mJ/mol.K2	34														uOhm.cm							1.5				220												Ce(3N),Ni(4N),Ge(5N)		arc-melting. ANN(800C,4d,Ta-foil in vac)					High-pressure effect on the electronic state in CeNiGe3: pressure-induced superconductivity			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.:Condens.Matter, 16(2004)L255	M.Nakashima,K.Tabata,A.Thamizhavel,T.C.Kobayashi,M.Hedo,Y.Uwatoko,K.Shimizu,R.Settai,Y.Onuki		
40124	PHC4250090		(Cu,Tl)Ba2Ca2Cu3O10	Cu0.5Tl0.5Ba2Ca2Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	2	Cu	3											O	10-z			2005																												M1223	P4/mmm		A	3.857		14.718												K	108						108																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40125	PHC4250090		(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Cu0.5Tl0.5Ba2Ca1.6Mg0.4Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	1.6	Mg	0.4	Cu	3									O	10-z			2005																												M1223	P4/mmm																	K	115						115																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40126	PHC4250090		(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Cu0.5Tl0.5Ba2Ca1.2Mg0.8Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	1.2	Mg	0.8	Cu	3									O	10-z			2005																												M1223	P4/mmm																	K	117						117																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40127	PHC4250090		(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Cu0.5Tl0.5Ba2Ca0.8Mg1.2Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	0.8	Mg	1.2	Cu	3									O	10-z			2005																												M1223	P4/mmm																	K	130						130																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40128	PHC4250090	R is const at T = 120 K.	(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Cu0.5Tl0.5Ba2Ca0.5Mg1.5Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	0.5	Mg	1.5	Cu	3									O	10-z			2005																												M1223	P4/mmm		A	3.83		14.2												K					77																																																																																																Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40129	PHC4250090		(Cu,Tl)Ba2(Ca,Pr)2Cu3O10	Cu0.5Tl0.5Ba2Ca1.9Pr0.1Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	1.9	Pr	0.1	Cu	3									O	10-z			2005																												M1223	P4/mmm																	K	96		125				110.5																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40130	PHC4250090		(Cu,Tl)Ba2(Ca,Pr)2Cu3O10	Cu0.5Tl0.5Ba2Ca1.8Pr0.2Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	1.8	Pr	0.2	Cu	3									O	10-z			2005																												M1223	P4/mmm																	K		100	116				100																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40131	PHC4250090		(Cu,Tl)Ba2(Ca,Pr)2Cu3O10	Cu0.5Tl0.5Ba2Ca1.6Pr0.4Cu3O10-z	Cu	0.5	Tl	0.5	Ba	2	Ca	1.6	Pr	0.4	Cu	3									O	10-z			2005																												M1223	P4/mmm		A	3.926		14.717												K		80	108				80																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO or Pr2O3	1	mixture - heat(810C,24h,in air). mixture(precursor + Tl2O3) - wrapped in Al-foil - SIN(810C,10 min) - FC to RT.					The study of inter-plane coupling in Cu0.5Tl0.5Ba2Ca2Cu3O10-d superconductor by Mg and Pr substitution at Ca site			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 425(2005)90	Nawazish A.Khan,Asim Javaid,A.A.Khurram,Naghma Haider		
40132	PHC4250144	sharp transition.	(Mg,Cu)B2	Mg1.9Cu0.1B12	Mg	1.9	Cu	0.1	B	12																			2005																												AlB2																		K		37.3				0.2	37.3																																																																																														Mg,Cu,B		mixture - cylindrical sample(100MPa) - Fe crucible - heat(archeating, 250-350C, in vac)					Synthesis and properties of Mg(1-x)CuxB2 bulk obtained by self-propagating high-temperature synthesis (SHS) method at low temperature			School of Science, Lanzhou University of Technology, Gansu Lanzhou 730050, China	Physica C, 425(2005)144	W.J.Feng,T.D.Xia,T.Z.Liu,W.J.Zhao,Z.Q.Wei		
40133	PHC4250144	solubility limit is about x=0.1. maybe (x=0.1 and MgCu2 with small grain sizes). Jc(10K,0.5T)= 6.7E+5 A/cm2	(Mg,Cu)B2	Mg1.8Cu0.2B12	Mg	1.8	Cu	0.2	B	12																			2005																												AlB2																		K		36.5					36.5																																																			670000																																											Mg,Cu,B		mixture - cylindrical sample(100MPa) - Fe crucible - heat(archeating, 250-350C, in vac)					Synthesis and properties of Mg(1-x)CuxB2 bulk obtained by self-propagating high-temperature synthesis (SHS) method at low temperature			School of Science, Lanzhou University of Technology, Gansu Lanzhou 730050, China	Physica C, 425(2005)144	W.J.Feng,T.D.Xia,T.Z.Liu,W.J.Zhao,Z.Q.Wei		
40134	P072224503	not SC.	CaCuO2Cl2	Ca1Cu1Cl2O2	Ca	1	Cu	1	Cl	2															O	2			2005																												T			A	3.8674		15.0412												K					4.2																																																																																																Ca2CuO2Cl2,CaCl2,CuO,Ca(ClO4)2		mixture - Au capsule - high pressure synthesis(1273K,30min,P=6 GPa) - Q to RT.					Single-layer oxychloride superconductor Ca2-xCuO2Cl2 with A-site cation deficiency			Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan	Phys.Rev.B, 72(2005)224503	I.Yamada,A.A.Belik,M.Azuma,S.Harjo,T.Kamiyama,Y.Shimakawa,M.Takano		
40135	P072224503	nominal composition. Ca-deficiency = 0.048 by NED.	Ca2-xCuO2Cl2	Ca1.9Cu1Cl2O2	Ca	1.9	Cu	1	Cl	2															O	2			2005																												T			A	3.8564		15.0984												K				15			15																																																																																														Ca2CuO2Cl2,CaCl2,CuO,Ca(ClO4)2		mixture - Au capsule - high pressure synthesis(1273K,30min,P=6 GPa) - Q to RT.					Single-layer oxychloride superconductor Ca2-xCuO2Cl2 with A-site cation deficiency			Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan	Phys.Rev.B, 72(2005)224503	I.Yamada,A.A.Belik,M.Azuma,S.Harjo,T.Kamiyama,Y.Shimakawa,M.Takano		
40136	P072224503	nominal composition. Ca-deficiency = 0.074 by NED.	Ca2-xCuO2Cl2	Ca1.85Cu1Cl2O2	Ca	1.85	Cu	1	Cl	2															O	2			2005																												T			A	3.8549		15.1132												K				30			30																																																																																														Ca2CuO2Cl2,CaCl2,CuO,Ca(ClO4)2		mixture - Au capsule - high pressure synthesis(1273K,30min,P=6 GPa) - Q to RT.					Single-layer oxychloride superconductor Ca2-xCuO2Cl2 with A-site cation deficiency			Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan	Phys.Rev.B, 72(2005)224503	I.Yamada,A.A.Belik,M.Azuma,S.Harjo,T.Kamiyama,Y.Shimakawa,M.Takano		
40137	P072224503	nominal composition. Ca-deficiency = 0.092 by NED.	Ca2-xCuO2Cl2	Ca1.8Cu1Cl2O2	Ca	1.8	Cu	1	Cl	2															O	2			2005																												T			A	3.8521		15.1224												K				39			39																																																																																														Ca2CuO2Cl2,CaCl2,CuO,Ca(ClO4)2		mixture - Au capsule - high pressure synthesis(1273K,30min,P=6 GPa) - Q to RT.					Single-layer oxychloride superconductor Ca2-xCuO2Cl2 with A-site cation deficiency			Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan	Phys.Rev.B, 72(2005)224503	I.Yamada,A.A.Belik,M.Azuma,S.Harjo,T.Kamiyama,Y.Shimakawa,M.Takano		
40138	P072224503	nominal composition. ANN(773K,12h,in vac)	Ca2-xCuO2Cl2	Ca1.8Cu1Cl2O2	Ca	1.8	Cu	1	Cl	2															O	2			2005																												T																		K				43			43																																																																																														Ca2CuO2Cl2,CaCl2,CuO,Ca(ClO4)2		mixture - Au capsule - high pressure synthesis(1273K,30min,P=6 GPa) - Q to RT.					Single-layer oxychloride superconductor Ca2-xCuO2Cl2 with A-site cation deficiency			Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan	Phys.Rev.B, 72(2005)224503	I.Yamada,A.A.Belik,M.Azuma,S.Harjo,T.Kamiyama,Y.Shimakawa,M.Takano		
40139	PHC4320053	linear thermal expansion coeff. = 7.97 E-5/K. Hc2(0) = 8.9 T defined as mid point in R-T.	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		1	2005																												spinel			A	8.4					K^(-1)	0.0000797								K		12.1				0.3	12.1																				T	onset in M-T	9.3												HC40139		A		298			A		2250																																																			TiO,Li2Ti3O7		mixture - pellet - CAL(805C,50h,in vac) - slow cool to RT					Investigations on preparation, upper critical field and low temperature thermal expansion of LiTi2O4 superconductor			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, China	Physica C, 432(2005)53	H.X.Geng,A.F.Dong,G.C.Che,W.W.Huang,S.L.Jia,Z.X.Zhao		
40140	PHC4320065	B-content not given. hole concentration = 5.57E+20/cc. Tc defined as mid point. G-L parameter = 7.6	B-doped diamond	C1	C	1																						1	2005																												diamond																		K		0.38					0.38																				T	R(mid)	0.37												HC40140		A		116			A		1540																																																					B-doped polycrystals were prepared by microwave plasma assisted chemical vapor deposition on Si-substrates.					Electronic properties of boron-doped diamond on the border between the normal and the superconducting state			I. Physikalisches Institut, Universitat Gottingen, D-37077 Gottingen, Germany	Physica C, 432(2005)65	K.Winzer,D.Bogdanov,Ch.Wild		
40141	PHC4320065	B-content not given. hole concentration = 1.34E+21/cc. Tc defined as mid point. G-L parameter = 13.3	B-doped diamond	C1	C	1																						1	2005																												diamond																		K		2.5					2.5																				T	R(mid)	2.44												HC40140		A		122			A		1450																																																					B-doped polycrystals were prepared by microwave plasma assisted chemical vapor deposition on Si-substrates.					Electronic properties of boron-doped diamond on the border between the normal and the superconducting state			I. Physikalisches Institut, Universitat Gottingen, D-37077 Gottingen, Germany	Physica C, 432(2005)65	K.Winzer,D.Bogdanov,Ch.Wild		
40142	PHC4320065	B-content not given. hole concentration = 1.19E+21/cc. Tc defined as mid point. G-L parameter = 11.9	B-doped diamond	C1	C	1																						1	2005																												diamond																		K		2.62					2.62																				T	R(mid)	2.23												HC40142																																																														B-doped polycrystals were prepared by microwave plasma assisted chemical vapor deposition on Si-substrates.					Electronic properties of boron-doped diamond on the border between the normal and the superconducting state			I. Physikalisches Institut, Universitat Gottingen, D-37077 Gottingen, Germany	Physica C, 432(2005)65	K.Winzer,D.Bogdanov,Ch.Wild		
40143	PHC4320065	B-content not given. hole concentration = 3.37E+20/cc.  not SC.	B-doped diamond	C1	C	1																						1	2005																												diamond																		K					0.05																																																																																																		B-doped polycrystals were prepared by microwave plasma assisted chemical vapor deposition on Si-substrates.					Electronic properties of boron-doped diamond on the border between the normal and the superconducting state			I. Physikalisches Institut, Universitat Gottingen, D-37077 Gottingen, Germany	Physica C, 432(2005)65	K.Winzer,D.Bogdanov,Ch.Wild		
40144	PHC4320193	C-content = 0.068 by XRD.	Mg(B,C)2	Mg1B1.95C0.05	Mg	1	B	1.95	C	0.05																		1	2005																												AlB2																		K				34			34																				T		30.4												HC40144																																																												Mg,B,B4C		two step process. mixture - react(1200C,48h) - ground - pellet - SIN(1200C,48h)					Synthesis of Mg(B1-xCx)2 powders			Ames Laboratory US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 432(2005)193	R.H.T.Wilke,S.L.Bud'ko,P.C.Canfield,D.K.Finnemore,S.T.Hannahs		
40145	PHC4320193	C-content = 0.138 by XRD.	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		1	2005																												AlB2																		K				27.5			27.5																				T		32.8																																																																								Mg,B,B4C		two step process. mixture - react(1200C,48h) - ground - pellet - SIN(1200C,48h)					Synthesis of Mg(B1-xCx)2 powders			Ames Laboratory US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 432(2005)193	R.H.T.Wilke,S.L.Bud'ko,P.C.Canfield,D.K.Finnemore,S.T.Hannahs		
40146	PHC4320257	Jc(H) shows a decay of power law. Hirr defined as Jc(H) = 100 A/cm2	CNT-doped MgB2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																			2005									2.3																			AlB2			A	3.067		3.522												K			34.2				34.2																				T	R(on)	24.1												HC40146																																																												Mg,amorphous-B,CNT		mixture - pellet - heat(1700C,0.5h,under P=5GPa) - FC to RT					Comparison of physical properties for carbon nanotube doped MgB2 superconductors synthesized with different process			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Physica C, 432(2005)257	Guoqiu,Yuan,Xiaonong Xu,Zhihe Wang,Dingwei Lu,Xin Jin		
40147	PHC4320257	Jc(H) shows a decay of expornential law. Hirr defined as Jc(H) = 100 A/cm2	CNT-doped MgB2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																			2005									1.8																			AlB2			A	3.074		3.522												K			35.4				35.4																				T	R(on)	24.3												HC40147																																																												Mg,amorphous-B,CNT		mixture - pellet - heat(700C,2h, under ambient P of Ar) - FC to RT					Comparison of physical properties for carbon nanotube doped MgB2 superconductors synthesized with different process			National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Physica C, 432(2005)257	Guoqiu,Yuan,Xiaonong Xu,Zhihe Wang,Dingwei Lu,Xin Jin		
40148	PHC4320281	not SC	(Ga,Co)Sr2(Tm,Ca)Cu2Oz	Ga0.5Co0.5Sr2Tm0.7Ca0.3Cu2Oz	Ga	0.5	Co	0.5	Sr	2	Tm	0.7	Ca	0.3	Cu	2									O	z			2005																												M1212			A	22.8109	5.4443	5.3807												K					18																																																																				uV/K	20.8																											Ga2O3,Co3O4,SrCO3,Tm2O3,CaCO3,CuO	1	mixture - CAL(900C,12h,in air) - pellet - SIN(1010C,24h,in following O2) - slow cool to RT - ANN(400C,2h + 350C,5h)					Superconductivity in the (Ga1-yCoy)Sr2(Tm1-xCax)Cu2Oz compounds synthesized under ambient pressure			Department of Physics, Kangwon National University, Hoyza-2-Dong 192-1, Chunchon 200-701, Republic of Korea	Physica C, 432(2005)281	H.K.Lee,Y.H.Kim		
40149	PHC4320281		(Ga,Co)Sr2(Tm,Ca)Cu2Oz	Ga0.5Co0.5Sr2Tm0.6Ca0.4Cu2Oz	Ga	0.5	Co	0.5	Sr	2	Tm	0.6	Ca	0.4	Cu	2									O	z			2005																												M1212			A	22.8301	5.4413	5.378												K	20		41	35			35										26																																																								uV/K	8.9																											Ga2O3,Co3O4,SrCO3,Tm2O3,CaCO3,CuO	1	mixture - CAL(900C,12h,in air) - pellet - SIN(1010C,24h,in following O2) - slow cool to RT - ANN(400C,2h + 350C,5h)					Superconductivity in the (Ga1-yCoy)Sr2(Tm1-xCax)Cu2Oz compounds synthesized under ambient pressure			Department of Physics, Kangwon National University, Hoyza-2-Dong 192-1, Chunchon 200-701, Republic of Korea	Physica C, 432(2005)281	H.K.Lee,Y.H.Kim		
40150	PHC4320281		(Ga,Co)Sr2(Tm,Ca)Cu2Oz	Ga0.5Co0.5Sr2Tm0.5Ca0.5Cu2Oz	Ga	0.5	Co	0.5	Sr	2	Tm	0.5	Ca	0.5	Cu	2									O	z			2005																												M1212			A	22.8245	5.4473	5.3786												K	25		43				34																																																																		uV/K	4.8																											Ga2O3,Co3O4,SrCO3,Tm2O3,CaCO3,CuO	1	mixture - CAL(900C,12h,in air) - pellet - SIN(1010C,24h,in following O2) - slow cool to RT - ANN(400C,2h + 350C,5h)					Superconductivity in the (Ga1-yCoy)Sr2(Tm1-xCax)Cu2Oz compounds synthesized under ambient pressure			Department of Physics, Kangwon National University, Hoyza-2-Dong 192-1, Chunchon 200-701, Republic of Korea	Physica C, 432(2005)281	H.K.Lee,Y.H.Kim		
40151	PHC4320281		(Ga,Co)Sr2(Tm,Ca)Cu2Oz	Ga0.4Co0.6Sr2Tm0.6Ca0.4Cu2Oz	Ga	0.4	Co	0.6	Sr	2	Tm	0.6	Ca	0.4	Cu	2									O	z			2005																												M1212			A	22.8285	5.4401	5.3802												K	20		40				30																																																																		uV/K	9.28																											Ga2O3,Co3O4,SrCO3,Tm2O3,CaCO3,CuO	1	mixture - CAL(900C,12h,in air) - pellet - SIN(1010C,24h,in following O2) - slow cool to RT - ANN(400C,2h + 350C,5h)					Superconductivity in the (Ga1-yCoy)Sr2(Tm1-xCax)Cu2Oz compounds synthesized under ambient pressure			Department of Physics, Kangwon National University, Hoyza-2-Dong 192-1, Chunchon 200-701, Republic of Korea	Physica C, 432(2005)281	H.K.Lee,Y.H.Kim		
40152	PHC4320281	not SC	(Ga,Co)Sr2(Tm,Ca)Cu2Oz	Ga0.2Co0.8Sr2Tm0.6Ca0.4Cu2Oz	Ga	0.2	Co	0.8	Sr	2	Tm	0.6	Ca	0.4	Cu	2									O	z			2005																												M1212			A	22.8048	5.4333	5.3852												K					18																																																																				uV/K	15.5																											Ga2O3,Co3O4,SrCO3,Tm2O3,CaCO3,CuO	1	mixture - CAL(900C,12h,in air) - pellet - SIN(1010C,24h,in following O2) - slow cool to RT - ANN(400C,2h + 350C,5h)					Superconductivity in the (Ga1-yCoy)Sr2(Tm1-xCax)Cu2Oz compounds synthesized under ambient pressure			Department of Physics, Kangwon National University, Hoyza-2-Dong 192-1, Chunchon 200-701, Republic of Korea	Physica C, 432(2005)281	H.K.Lee,Y.H.Kim		
40153	PHC4330009		LuNiBxCy	Lu1Ni1B1C1	Lu	1	Ni	1	B	1	C	1																	2005																													P4/mmm		A	3.492		7.55												K				2.5			2.5																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40154	PHC4330009	The best phase purity with no 1221 phase	LuNiBxCy	Lu1Ni1B0.9C1	Lu	1	Ni	1	B	0.9	C	1																	2005																													P4/mmm		A	3.492		7.552												K				2.6			2.6											Oe					40			1.6	Oe					1200			1.6																												mJ/mol.K2	2.85	SP-heat	440	SP-heat																																				arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40155	PHC4330009		LuNiBxCy	Lu1Ni1B0.8C1	Lu	1	Ni	1	B	0.8	C	1																	2005																													P4/mmm		A	3.489		7.546												K				2.6			2.6																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40156	PHC4330009		LuNiBxCy	Lu1Ni1B0.9C1.1	Lu	1	Ni	1	B	0.9	C	1.1																	2005																													P4/mmm		A	3.492		7.553												K				2.9			2.9																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40157	PHC4330009	10% 1221 phase. Tc increases as increasing C/B ratio	LuNiBxCy	Lu1Ni1B0.8C1.2	Lu	1	Ni	1	B	0.8	C	1.2																	2005																													P4/mmm		A	3.488		7.545												K				3.2			3.2																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40158	PHC4330009	no 1221 phase	LuNiBxCy	Lu1Ni1B1.1C0.9	Lu	1	Ni	1	B	1.1	C	0.9																	2005																													P4/mmm		A	3.495		7.557												K				2.4			2.4																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40159	PHC4330009	no 1221 phase	LuNiBxCy	Lu1Ni1B1C0.85	Lu	1	Ni	1	B	1	C	0.85																	2005																													P4/mmm		A	3.495		7.562												K				2.4			2.4																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40160	PHC4330009	no 1221 phase	LuNiBxCy	Lu1Ni1B0.95C0.95	Lu	1	Ni	1	B	0.95	C	0.95																	2005																													P4/mmm		A	3.494		7.557												K				2.5			2.5																																																																																																arc-melting - wrapped in Ta foil - ANN(950C,1w, in evacuated quartz tube)					Effect of boron, carbon stoichiometry on the superconducting properties of LuNiBxCy system			a Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India	Physica C, 433(2005)9	G.V.M.Kiruthika,P.L.Paulose,Sujata Patil,L.C.Gupta		
40161	PHC4330139	d(lnTc)/dP = 0.064 /GPa.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																			2005																													P4<2>32		A	6.7639														K		8.2		8			8.2			K/GPa	0.41																																																																																												(Pd,Ni)3B by two step arc-melting. Li + (Pd,Ni)3B - react(600-700C,48h,in 20-25 bar Ar)					Study of the effect of Ni substitution and external pressure in Li2Pd3B superconductor			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603 102, Tamil Nadu, India	Physica C, 433(2005)139	Awadhesh Mani,T.Geetha Kumary,A.Bharathi,S.Kalavathi,V.Sankara Sastry,Y.Hariharan		
40162	PHC4330139		Li2(Pd,Ni)3B	Li2Pd2.94Ni0.06B1	Li	2	Pd	2.94	Ni	0.06	B	1																	2005																													P4<2>32		A	6.7619														K				7.7			7.7																																																																																																(Pd,Ni)3B by two step arc-melting. Li + (Pd,Ni)3B - react(600-700C,48h,in 20-25 bar Ar)					Study of the effect of Ni substitution and external pressure in Li2Pd3B superconductor			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603 102, Tamil Nadu, India	Physica C, 433(2005)139	Awadhesh Mani,T.Geetha Kumary,A.Bharathi,S.Kalavathi,V.Sankara Sastry,Y.Hariharan		
40163	PHC4330139		Li2(Pd,Ni)3B	Li2Pd2.85Ni0.15B1	Li	2	Pd	2.85	Ni	0.15	B	1																	2005																													P4<2>32		A	6.7596														K				7.5			7.5																																																																																																(Pd,Ni)3B by two step arc-melting. Li + (Pd,Ni)3B - react(600-700C,48h,in 20-25 bar Ar)					Study of the effect of Ni substitution and external pressure in Li2Pd3B superconductor			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603 102, Tamil Nadu, India	Physica C, 433(2005)139	Awadhesh Mani,T.Geetha Kumary,A.Bharathi,S.Kalavathi,V.Sankara Sastry,Y.Hariharan		
40164	PHC4330139		Li2(Pd,Ni)3B	Li2Pd2.7Ni0.3B1	Li	2	Pd	2.7	Ni	0.3	B	1																	2005																													P4<2>32		A	6.7535														K				7.3			7.3																																																																																																(Pd,Ni)3B by two step arc-melting. Li + (Pd,Ni)3B - react(600-700C,48h,in 20-25 bar Ar)					Study of the effect of Ni substitution and external pressure in Li2Pd3B superconductor			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603 102, Tamil Nadu, India	Physica C, 433(2005)139	Awadhesh Mani,T.Geetha Kumary,A.Bharathi,S.Kalavathi,V.Sankara Sastry,Y.Hariharan		
40165	PHC4330139		Li2(Pd,Ni)3B	Li2Pd2.4Ni0.6B1	Li	2	Pd	2.4	Ni	0.6	B	1																	2005																													P4<2>32		A	6.7374														K				7.69			7.69																																																																																																(Pd,Ni)3B by two step arc-melting. Li + (Pd,Ni)3B - react(600-700C,48h,in 20-25 bar Ar)					Study of the effect of Ni substitution and external pressure in Li2Pd3B superconductor			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603 102, Tamil Nadu, India	Physica C, 433(2005)139	Awadhesh Mani,T.Geetha Kumary,A.Bharathi,S.Kalavathi,V.Sankara Sastry,Y.Hariharan		
40166	CEM0540136		Li1+xTi2-xO4	Li1Ti2O4	Li	1	Ti	2																	O	4			1984			cm3/mol	0.00227			-0.9																					spinel			A	8.407														K		11				3	11																																																																																																mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40167	CEM0540136		Li1+xTi2-xO4	Li1.05Ti1.95O4	Li	1.05	Ti	1.95																	O	4			1984			cm3/mol	0.00705			0.1																					spinel			A	8.4008														K		10.5				3.2	10.5																																																																																																mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40168	CEM0540136		Li1+xTi2-xO4	Li1.07Ti1.93O4	Li	1.07	Ti	1.93																	O	4			1984			cm3/mol	0.00757			0.5																					spinel			A	8.3972														K		10.4				3.2	10.4																																																																																																mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40169	CEM0540136		Li1+xTi2-xO4	Li1.1Ti1.9O4	Li	1.1	Ti	1.9																	O	4			1984			cm3/mol	0.00377			1.6																					spinel			A	8.392														K		10.3				3.9	10.3																																																																																																mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40170	CEM0540136		Li1+xTi2-xO4	Li1.12Ti1.88O4	Li	1.12	Ti	1.88																	O	4			1984			cm3/mol	0.0033			2.5																					spinel			A	8.3901														K		9.4				3	9.4																																																																																																mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40171	CEM0540136		Li1+xTi2-xO4	Li1.15Ti1.85O4	Li	1.15	Ti	1.85																	O	4			1984			cm3/mol	0.00317			2.5																					spinel			A	8.3841														K																																																																																																							mixture of (Li2TiO3,TiO2) - heat(800C,8h,in O2) using Au-foil, alumina boat					Localized moments in the superconducting Li1+xTi2-x spinel system				J.Solid State Chem., 54(1984)136	M.R.Harrison,P.P.Edwards,J.B.Goodenough		
40172	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.34Co1H2.6O3.3	Na	0.34	Co	1	H	2.6															O	3.3			2006																															A	2.822		19.5												K				2.65			2.65																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40173	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.32Co1H2.6O3.3	Na	0.32	Co	1	H	2.6															O	3.3			2006																															A	2.822		19.62												K				3.6			3.6																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40174	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.31Co1H2.6O3.3	Na	0.31	Co	1	H	2.6															O	3.3			2006																															A	2.819		19.59												K				3.7			3.7																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40175	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.28Co1H2.6O3.3	Na	0.28	Co	1	H	2.6															O	3.3			2006																															A	2.817		19.73												K				4.75			4.75																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40176	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.25Co1H2.6O3.3	Na	0.25	Co	1	H	2.6															O	3.3			2006																															A	2.817		19.8												K				4.7			4.7																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40177	JP018L0063	Na-content by ICP. NQR measured.	NaxCoO2/1.3H2O	Na0.26Co1H2.6O3.3	Na	0.26	Co	1	H	2.6															O	3.3			2006																															A	2.815		19.79												K				4.6			4.6																																																																																																precursor(Na0.75CoO2) was immersed in the Br2/CH3CN solution with various Br-contents.					Na content dependence of superconductivity and the spin correlations in NaxCoO2:1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40178	PLA0150303	Tc by ac-SUS. Tc was investigated for mass(ave) of Zr = 91.22, 94, 92, 90.	Zr	Zr1	Zr	1																							1965																																														K		0.49					0.49						0.05	Zr																																																	mj/mol.K2	2.75		280																																										Superconductivity of zirconium isotopes				Phys.Lett., 15(1965)303	E.Bucher,J.Muller,J.L.Olsen,C.Palmy		
40179	PR1660457	Tc by ac-SUS. Debye-T from Phys.Rev.Lett., 2(1959)260.	Re	Re1	Re	1																							1968																																														K		1.703					1.703						0.356	Re																																																				417																																										Isotope effect in superconducting rhenium				Phys.Rev., 166(1968)457	E.Maxwell,Myron Strongin,T.B.Reed		
40180	PR1640565	Tc was measured for M=63.96, 65.91, 67.94. RRR=10. Hc2 shows Hc(type-I).	Zn	Zn1	Zn	1																							1967																																														K		0.855					0.855						0.375	Zn													Oe		53.94							Oe/K		104.9																									mj/mol.K2	0.654																																												Superconducting transitions of isotopes of zinc				Phys.Rev., 164(1967)565	R.E.Fassnacht,J.R.Dillinger		
40181	PR1630356	gamma-U alloy. Tc = 2.132 K for U(235)	U1-xMox	Mo0.16U0.84	Mo	0.16	U	0.84																					1967																																														K		2.121					2.121																																																																																																arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40182	PR1630356	gamma-U alloy. Tc = 2.130 K for U(235)	U1-xMox	Mo0.18U0.82	Mo	0.18	U	0.82																					1967																																														K		2.118					2.118						0.53	U																																																																																									arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40183	PR1630356	gamma-U alloy. Tc = 2.124 K for U(235)	U1-xMox	Mo0.2U0.8	Mo	0.2	U	0.8																					1967																																														K		2.113					2.113																																																																																																arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40184	PR1630356	gamma-U alloy. Tc = 2.023 K for U(235)	U1-xNbx	Nb0.18U0.82	Nb	0.18	U	0.82																					1967																																														K		2.011					2.011																																																																																																arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40185	PR1630356	gamma-U alloy. Tc = 2.023 K for U(235)	U1-xNbx	Nb0.2U0.8	Nb	0.2	U	0.8																					1967																																														K		2.009					2.009						0.54	U																																																																																									arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40186	PR1630356	gamma-U alloy. Tc = 2.024 K for U(235)	U1-xNbx	Nb0.22U0.78	Nb	0.22	U	0.78																					1967																																														K		2.01					2.01																																																																																																arc-melting					Isotope effect in superconducting gamma-Uranium alloys				Phys.Rev., 163(1967)356	H.H.Hill,R.W.White,J.D.G.Lindsay,R.D.Fowler,B.T.Matthias		
40187	PR1410407	Tc by SUS. Tc shows no isotopic mass dependence. Hc2 shows Hc(type-I). M=99.2, 101.1(natural), 103.9 are measured.	Ru	Ru1	Ru	1																							1966																																														K		0.509					0.509						0	Ru													Oe		70																																		mj/mol.K2	2.8	calculated from Hc																																											Critical magnetic fields of superconducting ruthenium isotopes and search for isotope effect				Phys.Rev., 141(1966)407	J.W.Gibson,R.A.Hein		
40188	PR1311105	mean mass = 187.4, 188.3, 190.2(natural), 192.0 were measured. Hc2 shows Hc(type-I). gamma = 4.77E-4 cal/mol.K2 calculated from Hc.	Os	Os1	Os	1																							1963																																														K		0.671					0.671						0.21	Os													Oe		80.4																																																																															Isotope effect in superconducting osmium				Phys.Rev., 131(1963)1105	R.A.Hein,J.W.Gibson		
40189	PR1121888	M(ave) = 207.271. Hc2 shows Hc(type-I).	Pb	Pb1	Pb	1																							1958																																														K		7.172					7.172																				Oe		802												HC40189																																																																			Critical field measurements on superconducting lead isotopes				Phys.Rev., 112(1958)1888	D.L.Decker,D.E.Mapother,R.W.Shaw		
40190	PR1121522	Isotope effect derived from Hc(M). Tc measured for M=207.811, 207.460, 207.271, 206.884, 206.543, 206.193.	Pb	Pb1	Pb	1																							1958																																														K		7.175					7.175						0.501	Pb																																																																																														Isotope effect on the superconducting transition in lead				Phys.Rev., 112(1958)1522	R.R.Hake,D.E.Mapother,D.L.Decker		
40191	CEM1540488		(Hg,W)Sr2(Sm,Ce)2Cu2Oz	Hg0.75W0.25Sr2Sm1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Sm	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8462		29.182												K	35		56				45.5																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40192	CEM1540488		(Hg,W)Sr2(Eu,Ce)2Cu2Oz	Hg0.75W0.25Sr2Eu1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8386		29.167												K	39		65				52																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40193	CEM1540488		(Hg,W)Sr2(Gd,Ce)2Cu2Oz	Hg0.75W0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8327		29.15												K	48		75				61.5																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40194	CEM1540488		(Hg,W)Sr2(Dy,Ce)2Cu2Oz	Hg0.75W0.25Sr2Dy1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Dy	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8161		29.087												K	49		71				60																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40195	CEM1540488		(Hg,W)Sr2(Ho,Ce)2Cu2Oz	Hg0.75W0.25Sr2Ho1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Ho	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8124		29.043												K	42		64				53																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40196	CEM1540488		(Hg,W)Sr2(Er,Ce)2Cu2Oz	Hg0.75W0.25Sr2Er1.5Ce0.5Cu2Oz	Hg	0.75	W	0.25	Sr	2	Er	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8058		29.008												K	36		60				48																																																																																																precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40197	CEM1540488		(Hg,Ti)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Ti0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Ti	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8426		29.229												K			38				38										20																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40198	CEM1540488		(Hg,V)Sr2(Gd,Ce)2Cu2Oz	Hg0.75V0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	V	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8566		29.126												K			47				47										11																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40199	CEM1540488	not SC.	(Hg,Cr)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Cr0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Cr	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8573		29.122												K					4.2																																																																																																		precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40200	CEM1540488		(Hg,Mo)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Mo0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Mo	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.842		29.209												K			70				70										21																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40201	CEM1540488	using ReO2 as Re source.	(Hg,Re)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Re0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Re	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8466		29.158												K			39				39										14																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40202	CEM1540488	using ReO3 as Re source.	(Hg,Re)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Re0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Re	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8455		29.14												K			50				50										15																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40203	CEM1540488	using ReO3 and 10%LiClO4 as Re source.	(Hg,Re)Sr2(Gd,Ce)2Cu2Oz	Hg0.75Re0.25Sr2Gd1.5Ce0.5Cu2Oz	Hg	0.75	Re	0.25	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	z		1	2000																												Hg1222	I4/mmm		A	3.8437		29.131												K			70				70										22																																																																																						precursors(Sr2Gd2-xCex)Cu2Oz,Sr2(R1.5Ce0.5)Cu2Oz) - CAL -pelley - mixed with HgO, M-oxide - sealed in Au - high pressure synthesis(1100C,2h,2GPa)					Synthesis and Study of Hg-Based 1222-Type Superconducting Cuprates (Hg,M)Sr2(Ln, Ce)2Cu2Oz			Superconductivity Research Laboratory, ISTEC, 10}13 Shinonome 1-Chome, Koto-ku, Tokyo 135-0062, Japan	J.Solid State Chem., 154(2000)488	E.Kandyl,A.Yamamoto,J.G.Wen,S.Tajima		
40204	CEM1710367		Y2C2I2	Y2C2I2	Y	2	C	2	I	2																		1	2003																		GPa		37																										K				10			10			K/GPa	1.3																																																																																										Y,YI3,C		mixture with a slight excess C (5%). See J.Phys.Chem.B, 103(1999)5446					Pressure dependence of TC of the layered superconductor Y2C2I2: lattice versus electronic effects			Max-Planck-Institut fur Festkorperforschung, D-70569 Stuttgart, Germany	J.Solid State Chem., 171(2003)367	K.Ahn,A.Grzechnik,R.K.Kremer,A.Simon,W.G.Marshall		
40205	PHC3410719		Y2C2Br2	Y2C2Br2	Y	2	C	2	Br	2																			2000																													C2/m																	K				5.03			5.03			K/GPa	-0.13																																																																																												sensitive to moisture. all handling in dry Ar.					Pressure dependence of the transition temperature of the layered superconductors Y2C2Br2-xIx			Max-Planck-Institut fur Festkorperforschung, Stuttgart,Germany	Physica C, 341-348(2000)719	R.W.Henn,K.Ahn,H.-A.Krug von Nidda,R.K.Kremer,A.Simon		
40206	PHC3410719		Y2C2(Br,I)2	Y2C2Br1I1	Y	2	C	2	Br	1	I	1																	2000																													C2/m																	K				5.08			5.08			K/GPa	-0.79																																																																																												sensitive to moisture. all handling in dry Ar.					Pressure dependence of the transition temperature of the layered superconductors Y2C2Br2-xIx			Max-Planck-Institut fur Festkorperforschung, Stuttgart,Germany	Physica C, 341-348(2000)719	R.W.Henn,K.Ahn,H.-A.Krug von Nidda,R.K.Kremer,A.Simon		
40207	PHC3410719		Y2C2(Br,I)2	Y2C2Br0.5I1.5	Y	2	C	2	Br	0.5	I	1.5																	2000																													C2/m																	K				11.6			11.6			K/GPa	-0.54																																																																																												sensitive to moisture. all handling in dry Ar.					Pressure dependence of the transition temperature of the layered superconductors Y2C2Br2-xIx			Max-Planck-Institut fur Festkorperforschung, Stuttgart,Germany	Physica C, 341-348(2000)719	R.W.Henn,K.Ahn,H.-A.Krug von Nidda,R.K.Kremer,A.Simon		
40208	PHC3410719		Y2C2I2	Y2C2I2	Y	2	C	2	I	2																			2000																													C2/m																	K				9.97			9.97			K/GPa	1.05																																																																																												sensitive to moisture. all handling in dry Ar.					Pressure dependence of the transition temperature of the layered superconductors Y2C2Br2-xIx			Max-Planck-Institut fur Festkorperforschung, Stuttgart,Germany	Physica C, 341-348(2000)719	R.W.Henn,K.Ahn,H.-A.Krug von Nidda,R.K.Kremer,A.Simon		
40209	PHC3410719		La2C2Br2	La2C2Br2	La	2	C	2	Br	2																			2000																													C2/m																	K				7.03			7.03			K/GPa	1.26																																																																																												sensitive to moisture. all handling in dry Ar.					Pressure dependence of the transition temperature of the layered superconductors Y2C2Br2-xIx			Max-Planck-Institut fur Festkorperforschung, Stuttgart,Germany	Physica C, 341-348(2000)719	R.W.Henn,K.Ahn,H.-A.Krug von Nidda,R.K.Kremer,A.Simon		
40210	CEM1781705	Cu-valence = 2.10 from XAS.	Cu(Ba,Eu)2(Ce,Eu)2Cu2O9	Ba1.34Eu2Ce0.66Cu3O8.96	Ba	1.34	Eu	2	Ce	0.66	Cu	3													O	9-z	8.96	1	2006																												Cu1222			A	3.86		28.49												K			15				15										12																																																																																				CuO,BaCO3,Eu2O3,CeO2		nominal(Eu:Ba:Ce:Cu=6:4:2:9). SIN(1020C,15h,in flowing O2) - ANN(300C,24h,in flowing N2) - cool to RT (20C/min).					Oxygen nonstoichiometry and valence of copper in the Cu-1222 superconductor			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)1705	M.Karppinen,M.Arai,J.M.Lee,T.S.Chan,Y.Morita,J.M.Chen,R.S.Liu,H.Yamauchi		
40211	CEM1781705	as-prepared sample. Cu-valence = 2.11 from XAS.	Cu(Ba,Eu)2(Ce,Eu)2Cu2O9	Ba1.34Eu2Ce0.66Cu3O9.02	Ba	1.34	Eu	2	Ce	0.66	Cu	3													O	9-z	9.02	1	2006																												Cu1222			A	3.86		28.48												K			25				25										29																																																																																				CuO,BaCO3,Eu2O3,CeO2		nominal(Eu:Ba:Ce:Cu=6:4:2:9). SIN(1020C,15h,in flowing O2).					Oxygen nonstoichiometry and valence of copper in the Cu-1222 superconductor			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)1705	M.Karppinen,M.Arai,J.M.Lee,T.S.Chan,Y.Morita,J.M.Chen,R.S.Liu,H.Yamauchi		
40212	CEM1781705	Cu-valence = 2.24 from XAS.	Cu(Ba,Eu)2(Ce,Eu)2Cu2O9	Ba1.34Eu2Ce0.66Cu3O9-z	Ba	1.34	Eu	2	Ce	0.66	Cu	3													O	9-z		1	2006																												Cu1222			A	3.86		28.48												K			62				62	TC40212									59																																																																																				CuO,BaCO3,Eu2O3,CeO2		nominal(Eu:Ba:Ce:Cu=6:4:2:9). SIN(1020C,15h,in flowing O2)  - mixed with 100 mol% Ag2O2 - high pressure synthesis(500C,30min,5 GPa).					Oxygen nonstoichiometry and valence of copper in the Cu-1222 superconductor			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)1705	M.Karppinen,M.Arai,J.M.Lee,T.S.Chan,Y.Morita,J.M.Chen,R.S.Liu,H.Yamauchi		
40213	PHC3350259	compositions show nominal values.	(Cu,V)Sr2(Ca,Sr)2Cu3Oz	V0.5Sr2.25Ca1.75Cu3.5O9.7	V	0.5	Sr	2.25	Ca	1.75	Cu	3.5													O	9.7			2000																												Cu1223			A	3.8418		14.691												K		98					98																																		HIR40213																																																														high pressure synthesis (1300C, P = 6 GPa)					High-pressure synthesis and Jc-related properties of Cr- and V-based high Tc superconductors			National Institute for Research in Inorganic Materials, Tsukuba,Japan	Physica C, 335(2000)259	S.Yu,N.D.Zhigadlo,E.Takayama-Muromachi		
40214	PHC3350259	compositions show nominal values.	(Cu,V)Sr2(Ca,Sr)3Cu3Oz	V0.5Sr2.7Ca2.3Cu4.5O11.6	V	0.5	Sr	2.7	Ca	2.3	Cu	4.5													O	11.6			2000																												Cu1234			A	3.8497		17.9												K		107					107																																		HIR40214																																																														high pressure synthesis (1300C, P = 6 GPa)					High-pressure synthesis and Jc-related properties of Cr- and V-based high Tc superconductors			National Institute for Research in Inorganic Materials, Tsukuba,Japan	Physica C, 335(2000)259	S.Yu,N.D.Zhigadlo,E.Takayama-Muromachi		
40215	PHC3350259	compositions show nominal values.	(Cu,V)Sr2(Ca,Sr)4Cu3Oz	V0.5Sr2.4Ca3.6Cu5.5O13.55	V	0.5	Sr	2.4	Ca	3.6	Cu	5.5													O	13.55			2000																												Cu1245			A	3.8498		21.036												K		75					75																																		HIR40213																																																														high pressure synthesis (1300C, P = 6 GPa)					High-pressure synthesis and Jc-related properties of Cr- and V-based high Tc superconductors			National Institute for Research in Inorganic Materials, Tsukuba,Japan	Physica C, 335(2000)259	S.Yu,N.D.Zhigadlo,E.Takayama-Muromachi		
40216	PHC3350259	compositions show nominal values.	(Cu,V)Sr2(Ca,Sr)5Cu3Oz	V0.5Sr2.3Ca4.7Cu6.5O15.5	V	0.5	Sr	2.3	Ca	4.7	Cu	6.5													O	15.5			2000																												Cu1256			A	3.8532		24.226												K		75					75																																		HIR40214																																																														high pressure synthesis (1300C, P = 6 GPa)					High-pressure synthesis and Jc-related properties of Cr- and V-based high Tc superconductors			National Institute for Research in Inorganic Materials, Tsukuba,Japan	Physica C, 335(2000)259	S.Yu,N.D.Zhigadlo,E.Takayama-Muromachi		
40217	PHC3350259	compositions show nominal values.	(Cu,V)Sr2(Ca,Sr)6Cu3Oz	V0.5Sr2.6Ca5.4Cu7.5O17.3	V	0.5	Sr	2.6	Ca	5.4	Cu	7.5													O	17.3			2000																												Cu1267			A	3.8572		27.434												K		73					73																																		HIR40213																																																														high pressure synthesis (1300C, P = 6 GPa)					High-pressure synthesis and Jc-related properties of Cr- and V-based high Tc superconductors			National Institute for Research in Inorganic Materials, Tsukuba,Japan	Physica C, 335(2000)259	S.Yu,N.D.Zhigadlo,E.Takayama-Muromachi		
40218	CEM1782274	not SC	CoSr2(Y,Ce)2Cu2O9	Co1Sr2Y1.5Ce0.5Cu2O9	Co	1	Sr	2	Y	1.5	Ce	0.5	Cu	2											O	9			2005	emu/mol	0.0002			M/mol	5.12	-311	43																				Co1222	Cmcm		A	28.1548	5.4255	5.4013												K					10																																																																																																Y2O3,CeO2,SrCO3,Co3O4,CuO	1	mixture - pellet - heat(1000C,10h) - pellet - SIN(1100C,30h,flowing O2) - FC to RT					Doping studies of the magnetic cobaltocuprate CoSr2Y2-xCexCu2O9+-z			Chemistry Department, University of Aberdeen, Meston Walk, Aberdeen, AB24 3UE, UK	J.Solid State Chem., 178(2006)2274	A.C.Mclaughlin,D.Morrice,F.Sher		
40219	CEM1782274	not SC	CoSr2(Y,Ce)2Cu2O9	Co1Sr2Y1.4Ce0.6Cu2O9	Co	1	Sr	2	Y	1.4	Ce	0.6	Cu	2											O	9			2005	emu/mol	0.0007			M/mol	5.23	-344	48																				Co1222	Cmcm		A	28.1548	5.4281	5.4035												K					10																																																																																																Y2O3,CeO2,SrCO3,Co3O4,CuO	1	mixture - pellet - heat(1000C,10h) - pellet - SIN(1100C,30h,flowing O2) - FC to RT					Doping studies of the magnetic cobaltocuprate CoSr2Y2-xCexCu2O9+-z			Chemistry Department, University of Aberdeen, Meston Walk, Aberdeen, AB24 3UE, UK	J.Solid State Chem., 178(2006)2274	A.C.Mclaughlin,D.Morrice,F.Sher		
40220	CEM1782274	not SC	CoSr2(Y,Ce)2Cu2O9	Co1Sr2Y1.3Ce0.7Cu2O9	Co	1	Sr	2	Y	1.3	Ce	0.7	Cu	2											O	9			2005	emu/mol	0.0005			M/mol	5.29	-360	67																				Co1222	Cmcm		A	28.1444	5.4337	5.4054												K					10																																																																																																Y2O3,CeO2,SrCO3,Co3O4,CuO	1	mixture - pellet - heat(1000C,10h) - pellet - SIN(1100C,30h,flowing O2) - FC to RT					Doping studies of the magnetic cobaltocuprate CoSr2Y2-xCexCu2O9+-z			Chemistry Department, University of Aberdeen, Meston Walk, Aberdeen, AB24 3UE, UK	J.Solid State Chem., 178(2006)2274	A.C.Mclaughlin,D.Morrice,F.Sher		
40221	CEM1782274	not SC	CoSr2(Y,Ce)2Cu2O9	Co1Sr2Y1.2Ce0.8Cu2O9	Co	1	Sr	2	Y	1.2	Ce	0.8	Cu	2											O	9			2005	emu/mol	0.0007			M/mol	5.46	-370	90																				Co1222	Cmcm		A	28.1457	5.4375	5.4079												K					10																																																																																																Y2O3,CeO2,SrCO3,Co3O4,CuO	1	mixture - pellet - heat(1000C,10h) - pellet - SIN(1100C,30h,flowing O2) - FC to RT					Doping studies of the magnetic cobaltocuprate CoSr2Y2-xCexCu2O9+-z			Chemistry Department, University of Aberdeen, Meston Walk, Aberdeen, AB24 3UE, UK	J.Solid State Chem., 178(2006)2274	A.C.Mclaughlin,D.Morrice,F.Sher		
40222	CEM1783464	OZ shows 'largest possible' O-content calculated from Cu-valence (=2.45)	(Cu,Mo)Sr2YCu2O7	Mo0.25Sr2Y1Cu2.75O7+z	Mo	0.25	Sr	2	Y	1	Cu	2.75													O	7+z		1	2005																												Cu1212	P4/mmm		A	3.815		11.47												K				88			88																																																																																																mixture - CAL(950C,in air) - SIN(1020C,in air) - high pressure oxygenated(500C,30min, P=5 GPa, with 75mol% Ag2O2)					Hole doping and superconductivity characteristics of the s = 1, 2 and 3 members of the (Cu,Mo)-12s2 homologous series of layered copper oxides			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)3464	M. Karppinen,Y.Morita,T.Kobayashi,I.Grigoraviciute,J.M.Chen,R.S.Liu,H.Yamauchi		
40223	CEM1783464	OZ shows 'largest possible' O-content calculated from Cu-valence (=2.26)	(Cu,Mo)Sr2(Ce,Y)2Cu2O7	Mo0.25Sr2Ce0.9Y1.1Cu2.75O9+z	Mo	0.25	Sr	2	Ce	0.9	Y	1.1	Cu	2.75											O	9+z		1	2005																												Cu1222	I4/mmm		A	3.822		14.2												K				61			61																																																																																																mixture - CAL(950C,in air) - SIN(1020C,in air) - high pressure oxygenated(500C,30min, P=5 GPa, with 75mol% Ag2O2)					Hole doping and superconductivity characteristics of the s = 1, 2 and 3 members of the (Cu,Mo)-12s2 homologous series of layered copper oxides			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)3464	M. Karppinen,Y.Morita,T.Kobayashi,I.Grigoraviciute,J.M.Chen,R.S.Liu,H.Yamauchi		
40224	CEM1783464	OZ shows 'largest possible' O-content calculated from Cu-valence (=2.28)	(Cu,Mo)Sr2(Ce,Y)3Cu2O7	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2005																												Cu1232	P4/mmm		A	3.828		16.92												K				53			53																																																																																																mixture - CAL(950C,in air) - SIN(1020C,in air) - high pressure oxygenated(500C,30min, P=5 GPa, with 75mol% Ag2O2)					Hole doping and superconductivity characteristics of the s = 1, 2 and 3 members of the (Cu,Mo)-12s2 homologous series of layered copper oxides			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Solid State Chem., 178(2006)3464	M. Karppinen,Y.Morita,T.Kobayashi,I.Grigoraviciute,J.M.Chen,R.S.Liu,H.Yamauchi		
40225	PRL0710283	Tc for (Cu65,O16), (Cu65,O18), (Cu63,O16), (Cu63,O18) were measured. Tc shows for (Cu63,O16)	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		1	1993																												T																		K		27.84					27.84						0.91	O	86	2.51																																																																																					La2O3,SrCO3,Cu<65>O or Cu<63>O	1	annealing in <16>O2 or <18>O2 for oxygen isotope effect					Copper and Oxygen isotope effects in La2-xSrxCuO4			Department of Physics, University of Alberta, Edmonton, Alberta, Canada	Phys.Rev.Lett., 71(1993)283	J.P.Franck,S.Harker,J.H.Brewer		
40226	PRL0710283	Tc for (Cu65,O16), (Cu65,O18), (Cu63,O16), (Cu63,O18) were measured. Tc shows for (Cu63,O16)	(La,Sr)2CuO4	La1.875Sr0.125Cu1O4	La	1.875	Sr	0.125	Cu	1															O	4		1	1993																												T																		K		27.84					27.84						0.93	Cu	100	0.84																																																																																					La2O3,SrCO3,Cu<65>O or Cu<63>O	1	annealing in <16>O2 or <18>O2 for oxygen isotope effect					Copper and Oxygen isotope effects in La2-xSrxCuO4			Department of Physics, University of Alberta, Edmonton, Alberta, Canada	Phys.Rev.Lett., 71(1993)283	J.P.Franck,S.Harker,J.H.Brewer		
40227	PRL0710283	Tc for (Cu65,O16), (Cu65,O18), (Cu63,O16), (Cu63,O18) were measured. Tc shows for (Cu63,O16)	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1993																												T																		K		37.94					37.94						0.11	O	92	0.41																																																																																					La2O3,SrCO3,Cu<65>O or Cu<63>O	1	annealing in <16>O2 or <18>O2 for oxygen isotope effect					Copper and Oxygen isotope effects in La2-xSrxCuO4			Department of Physics, University of Alberta, Edmonton, Alberta, Canada	Phys.Rev.Lett., 71(1993)283	J.P.Franck,S.Harker,J.H.Brewer		
40228	PRL0710283	Tc for (Cu65,O16), (Cu65,O18), (Cu63,O16), (Cu63,O18) were measured. Tc shows for (Cu63,O16)	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1993																												T																		K		37.94					37.94						0.15	Cu	100	0.14																																																																																					La2O3,SrCO3,Cu<65>O or Cu<63>O	1	annealing in <16>O2 or <18>O2 for oxygen isotope effect					Copper and Oxygen isotope effects in La2-xSrxCuO4			Department of Physics, University of Alberta, Edmonton, Alberta, Canada	Phys.Rev.Lett., 71(1993)283	J.P.Franck,S.Harker,J.H.Brewer		
40229	PR06109257	no Cu isotope effect in Cu(2) mode Raman at RT. Tc by magnetization	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	2000																												Y124																		K				81.6			81.6						0.098	Cu		0.25																																																																																						1	standard solid state reaction. heat(945C, P=60 bar O2)					Contrasting oxygen and copper isotope effects in YBa2Cu4O8 superconducting and normal states	200004		2. Physikalisches Institut, Universitat Stuttgart, Pfafffenwaldring 57, D-70569 Stuttgart, Germany	Phys.Rev.B,61(2000)R9257-R9260	D.J.Pringle,G.V.M.Williams,J.L.Tallon		
40230	L092057602	PPENET(O<18>) = 155.82 nm. d(PPENET)/PPENET = 2.8 %. Isotope effect mainly from in-plane oxygen.	YBa2Cu3O7	Y1Ba2Cu3O6.85	Y	1	Ba	2	Cu	3															O	7-z	6.85		2004																												Y123																		K				89.3			89.3						0.015	O	95	0.2																																A	muon-SR		1518.5																																																				films of 600 nm thickness. ANN(600C,25h, in O2) - slow cool (20C/h)					Direct Observation of the Oxygen Isotope Effect on the In-Plane Magnetic Field Penetration Depth in Optimally Doped YBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057, Switzerland	Phys.Rev.Lett., 92(2004)057602	R.Khasanov,D.G.Eshchenko,H.Luetkens,E.Morenzoni,T.Prokscha,A.Suter,N.Garifianov,M.Mali,J.Roos,K.Conder,H.Keller		
40231	PHC2980203		(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7		1	1998																												Y123																		K				73.2			73.2						0.09	Cu		0.2																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40232	PHC2980203		(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7		1	1998																												Y123																		K				59.7			59.7						0.16	Cu		0.3																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40233	PHC2980203		(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7		1	1998																												Y123																		K				45.3			45.3						0.22	Cu		0.3																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40234	PHC2980203		(Y,Pr)Ba2Cu4O8	Y0.8Pr0.2Ba2Cu4O8	Y	0.8	Pr	0.2	Ba	2	Cu	4													O	8		1	1998																												Y124																		K				70.2			70.2						0.09	Cu		0.2																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40235	PHC2980203		(Y,Pr)Ba2Cu4O8	Y0.7Pr0.3Ba2Cu4O8	Y	0.7	Pr	0.3	Ba	2	Cu	4													O	8		1	1998																												Y124																		K				63.5			63.5						0.1	Cu		0.2																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40236	PHC2980203		Y(La,Ba)2Cu3O7	Y1La0.3Ba1.7Cu3O7	Y	1	La	0.3	Ba	1.7	Cu	3													O	7		1	1998																												Y123																		K				57.45			57.45						0.2	Cu		0.35																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40237	PHC2980203		Y(La,Ba)2Cu4O8	Y1La0.3Ba1.7Cu4O8	Y	1	La	0.3	Ba	1.7	Cu	4													O	8		1	1998																												Y124																		K				52.6			52.6						0.36	Cu		0.6																																																																																							mixture - pellet - CAL(950C,15h,in flowing O2) - pellet - SIN(950C,15h,in flowing O2) - slow cool to 400C - ANN(500C,10h,in O2)					Copper isotope shifts in Pr and La substituted 123 and 124 cuprate superconductors; comparison with oxygen isotope shifts	199804		Morris research, Inc, 44 Marguerita Road, Berkeley, CA 96707, USA	Physica.C,298(1998)203-208	A.P.B. Shinha,A.V. Inyushkin,D.E. Morris,V. Kirtikar		
40238	P068220506	ISOTOPE = 0.297 for in-plane oxygen. Table value of ISOTOPE is for all site O-exchange. For penetration depth, ISOTOPE = 0.56.	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O7-z	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z			2003																												Y123																		K				44.62			44.62						0.331	O		1.66																																																																																							To prepare oxygen site selective sample, two-step exchange process was applied.					Site-selective oxygen isotope effect on the magnetic-field penetration depth in underdoped Y0.6Pr0.4Ba2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057, Switzerland	Phys.Rev.B, 68(2003)220506	R.Khasanov,A.Shengelava,E.Morenzoni,M.Angst,K.Conder,I.M.Savic,D.Lampakis,E.Liarokapis,A.Tatsi,H.Keller		
40239	PHC4340053	93% (Hg,Re)-1223,impurity phase= HgCaO2,BaCO3,CaCuO2,BaCuO2. underdoped sample(P=0.152)	(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+z	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+z			2006																												Hg1223			A	3.8545		15.6874												K				132.6			132.6			K/GPa	8																																																														uV/K	3			TP40239																										precursor(Re-Ba-Ca-Cu-O) prepared in (5%o2+95%Ar), then mixed with HgO. heat(865C,72h) in quartz tube.					Distortion of ReO6 octahedron in the Hg0.82Re0.18Ba2Ca2Cu3O8+z superconductor			Preslab?High Pressure Laboratory, UFES, Vitoria, ES 29075-910, Brazil	Physica C, 434(2006)53	M.T.D.Orlando,C.A.C.Passos,J.L.Passamai Jr.,E.F.Medeiros,C.G.P.Orlando,R.V.Sampaio,H.S.P.Correa,F.C.L.de Melo,L.G.Martinez,J.L.Rossi		
40240	PHC4340053	93% (Hg,Re)-1223,impurity phase= HgCaO2,BaCO3,CaCuO2,BaCuO2. optimum sample(P=0.16)	(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+z	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+z			2006																												Hg1223			A	3.8541		15.6881												K				133.2			133.2			K/GPa	1.9																																																														uV/K	1.8			TP40240																										precursor(Re-Ba-Ca-Cu-O) prepared in (10%o2+90%Ar), then mixed with HgO. heat(865C,72h) in quartz tube.					Distortion of ReO6 octahedron in the Hg0.82Re0.18Ba2Ca2Cu3O8+z superconductor			Preslab?High Pressure Laboratory, UFES, Vitoria, ES 29075-910, Brazil	Physica C, 434(2006)53	M.T.D.Orlando,C.A.C.Passos,J.L.Passamai Jr.,E.F.Medeiros,C.G.P.Orlando,R.V.Sampaio,H.S.P.Correa,F.C.L.de Melo,L.G.Martinez,J.L.Rossi		
40241	PHC4340053	93% (Hg,Re)-1223,impurity phase= HgCaO2,BaCO3,CaCuO2,BaCuO2. overdoped sample(P=0.167)	(Hg,Re)Ba2Ca2Cu3O8	Hg0.82Re0.18Ba2Ca2Cu3O8+z	Hg	0.82	Re	0.18	Ba	2	Ca	2	Cu	3											O	8+z			2006																												Hg1223			A	3.8544		15.6891												K				132.7			132.7			K/GPa	-1.6																																																														uV/K	0.5			TP40241																										precursor(Re-Ba-Ca-Cu-O) prepared in (15%o+85%Ar), then mixed with HgO. heat(865C,72h) in quartz tube.					Distortion of ReO6 octahedron in the Hg0.82Re0.18Ba2Ca2Cu3O8+z superconductor			Preslab?High Pressure Laboratory, UFES, Vitoria, ES 29075-910, Brazil	Physica C, 434(2006)53	M.T.D.Orlando,C.A.C.Passos,J.L.Passamai Jr.,E.F.Medeiros,C.G.P.Orlando,R.V.Sampaio,H.S.P.Correa,F.C.L.de Melo,L.G.Martinez,J.L.Rossi		
40242	PHC4340121	ANN(1000C,3d). AlB2phase + Si	CaCuxSiy	Ca1Cu0.25Si1.7	Ca	1	Cu	0.25	Si	1.7																			2006																												AlB2			A	3.9937		4.3634												K	3.2			3.2			3.2											Oe					40			2	kOe					9.5			2																																																																				arc-melting - ANN(800-100C, in quartz tube) - water quench to RT					Superconductivity in the copper-poor region of the Ca(Cu,Si)2-x system			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62102, Taiwan, ROC	Physica C, 434(2006)121	W.J.Hor,H.H.Sung,W.H.Lee		
40243	PHC4340121	ANN(1000C,3d). AlB2phase + Si	CaCuxSiy	Ca1Cu0.25Si1.75	Ca	1	Cu	0.25	Si	1.75																			2006																												AlB2			A	3.9971		4.3463												K	3.1			3.1			3.1																																																																																																arc-melting - ANN(800-100C, in quartz tube) - water quench to RT					Superconductivity in the copper-poor region of the Ca(Cu,Si)2-x system			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62102, Taiwan, ROC	Physica C, 434(2006)121	W.J.Hor,H.H.Sung,W.H.Lee		
40244	PHC4340121	ANN(1000C,3d). AlB2phase + Si	CaCuxSiy	Ca1Cu0.33Si1.67	Ca	1	Cu	0.33	Si	1.67																			2006																												AlB2			A	4.0159		4.3532												K	2.3			2.3			2.3																																																																																																arc-melting - ANN(800-100C, in quartz tube) - water quench to RT					Superconductivity in the copper-poor region of the Ca(Cu,Si)2-x system			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62102, Taiwan, ROC	Physica C, 434(2006)121	W.J.Hor,H.H.Sung,W.H.Lee		
40245	PHC4340121	ANN(1000C,3d). AlB2phase	CaCuxSiy	Ca1Cu0.25Si1.55	Ca	1	Cu	0.25	Si	1.55																			2006																												AlB2			A	3.9862		4.3343												K	2.9			2.9			2.9																																																																																																arc-melting - ANN(800-100C, in quartz tube) - water quench to RT					Superconductivity in the copper-poor region of the Ca(Cu,Si)2-x system			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62102, Taiwan, ROC	Physica C, 434(2006)121	W.J.Hor,H.H.Sung,W.H.Lee		
40246	PHC4340121	ANN(1000C,3d). AlB2phase	CaCuxSiy	Ca1Cu0.25Si1.6	Ca	1	Cu	0.25	Si	1.6																			2006																												AlB2			A	3.9937		4.3423												K	3			3			3																																																																																																arc-melting - ANN(800-100C, in quartz tube) - water quench to RT					Superconductivity in the copper-poor region of the Ca(Cu,Si)2-x system			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62102, Taiwan, ROC	Physica C, 434(2006)121	W.J.Hor,H.H.Sung,W.H.Lee		
40247	P073014515	Tc by SP-heat. lower-Tc = 1.724 K. (dC/Tc) = 788 mJ/mol.K2.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2006																												skutterudite																		K		1.81					1.81																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40248	P073014515	Tc by SP-heat. lower-Tc = 1.714 K. (dC/Tc) = 624 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.98La0.02Os4Sb12	Pr	0.98	La	0.02	Os	4	Sb	12																3	2006																												skutterudite																		K		1.8					1.8																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40249	P073014515	Tc by SP-heat. lower-Tc = 1.697 K. (dC/Tc) = 560 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.95La0.05Os4Sb12	Pr	0.95	La	0.05	Os	4	Sb	12																3	2006																												skutterudite																		K		1.79					1.79																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40250	P073014515	Tc by SP-heat.  (dC/Tc) = 417 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.9La0.1Os4Sb12	Pr	0.9	La	0.1	Os	4	Sb	12																3	2006																												skutterudite																		K		1.7					1.7																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40251	P073014515	Tc by SP-heat.  (dC/Tc) = 226 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.8La0.2Os4Sb12	Pr	0.8	La	0.2	Os	4	Sb	12																3	2006																												skutterudite																		K		1.645					1.645																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40252	P073014515	Tc by SP-heat.  (dC/Tc) = 110 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.7La0.3Os4Sb12	Pr	0.7	La	0.3	Os	4	Sb	12																3	2006																												skutterudite																		K		1.528					1.528																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40253	P073014515	Tc by SP-heat.  (dC/Tc) = 110 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.6La0.4Os4Sb12	Pr	0.6	La	0.4	Os	4	Sb	12																3	2006																												skutterudite																		K		1.414					1.414																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40254	P073014515	Tc by SP-heat.  (dC/Tc) = 73.8 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.4La0.6Os4Sb12	Pr	0.4	La	0.6	Os	4	Sb	12																3	2006																												skutterudite																		K		1.172					1.172																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40255	P073014515	Tc by SP-heat.  (dC/Tc) = 88.1 mJ/mol.K2.	(Pr,La)Os4Sb12	Pr0.2La0.8Os4Sb12	Pr	0.2	La	0.8	Os	4	Sb	12																3	2006																												skutterudite																		K		0.903					0.903																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40256	P073014515	Tc by SP-heat.  (dC/Tc) = 85.7 mJ/mol.K2.	LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2006																												skutterudite																		K		0.741					0.741																																																																																																Sb-flux method					Collective heavy-fermion state and superconductivity in Pr1-xLaxOs4Sb12: A specific heat study			Department of Physics, University of Florida, P.O. Box 118440, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 73(2006)014515	C.R.Rotundu,P.Kumar,B.Andraka		
40257	P073014517		RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.5Ce0.5Cu2O10-z	Ru	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10-z		1	2006								140																				Ru1222	I4/mmm		A	3.835		28.493												K		33					33																																																																																														RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40258	P073014517		(Ru,Mo)Sr2(Eu,Ce)2Cu2O10	Ru0.8Mo0.2Sr2Eu1.5Ce0.5Cu2O10-z	Ru	0.8	Mo	0.2	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10-z		1	2006								135																				Ru1222	I4/mmm																	K		37.5					37.5																																																																																														RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40259	P073014517		(Ru,Mo)Sr2(Eu,Ce)2Cu2O10	Ru0.8Mo0.4Sr2Eu1.5Ce0.5Cu2O10-z	Ru	0.8	Mo	0.4	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10-z		1	2006								120																				Ru1222	I4/mmm																	K		40					40																																																																																														RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40260	P073014517		(Ru,Mo)Sr2(Eu,Ce)2Cu2O10	Ru0.8Mo0.6Sr2Eu1.5Ce0.5Cu2O10-z	Ru	0.8	Mo	0.6	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10-z		1	2006								100																				Ru1222	I4/mmm																	K		23					23																																																																																														RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40261	P073014517	not SC	(Ru,Mo)Sr2(Eu,Ce)2Cu2O10	Ru0.8Mo0.8Sr2Eu1.5Ce0.5Cu2O10-z	Ru	0.8	Mo	0.8	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10-z		1	2006																												Ru1222	I4/mmm																	K					1.2																																																																																																RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40262	P073014517	not SC	MoSr2(Eu,Ce)2Cu2O10	Mo1Sr2Eu1.5Ce0.5Cu2O10-z	Mo	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10-z		1	2006																												Ru1222	I4/mmm		A	3.843		28.4653												K					1.2																																																																																																RuO2,SrO2,Eu2O3,CeO2,CuO,Mo2O3	1	mixture - CAL(1000,1020,1040C, 24h) - pellet - ANN(1075C,40h,in flowing O2) - slow cooling to RT - ANN(400C,24h, in O2 flow) - slow cooling to RT					Experimental study of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z  : Effect of Mo doping on magnetic behavior and Tc variation			National Physical Laboratory, Dr. K.S. Kirishnan Marg, New Delhi-110012, India	Phys.Rev.B, 73(2006)014517	V.P.S.Awana,R.Lal,H.Kishan,A.V.Narlikar,M.Peurla,R.Laiho		
40263	P073024512	Tc = 6.25-4.3*x   for YB6+x. RRR=3.87. (dC/gamma*Tc) = 2.02. G-L(Tc) = 3.0. surface SC, Hc3 = 640 mT from resistivity.	YB6	B6Y1	B	6	Y	1																					2006																															A	4.1002														K		7.15					7.15			K/GPa	-0.53							mT		20							mT		295							mT/K		59			HC40263														4.1					SP40263			mJ/gat.K2	0.58	SP-heat	706																																										Superconductivity mediated by a soft phonon mode: Specific heat, resistivity, thermal expansion, and magnetization of YB6			Department of Condensed Matter Physics, University of Geneva, CH-1211 Geneva 4, Switzerland	Phys.Rev.B, 73(2006)024512	R.Lortz,Y.Wang,U.Tutsch,S.Abe,C.Meingast,P.Popovich,W.Knafo,N.Shitsevalova,Yu.B.Paderno,A.Junod		
40264	PRL0431892	Tc = 0.49 K for specific heat measurement.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		1	1979																												ThCr2Si2																		K		0.63					0.63																																																					SP40264																																											induction heating in Ar					Superconductivity in presence of strong Pauli paramagnetism: CeCu2Si2				Phys.Rev.Lett., 43(1979)1892	F.Steglich,J.Aarts,C.D.Bredl,W.Lieke,D.Meschede,W.Franz,H.Schafer		
40265	PRL0431892		LaCu2Si2	La1Cu2Si2	La	1	Cu	2	Si	2																		1	1979																												ThCr2Si2																		K					0.05																																																																																																		induction heating in Ar					Superconductivity in presence of strong Pauli paramagnetism: CeCu2Si2				Phys.Rev.Lett., 43(1979)1892	F.Steglich,J.Aarts,C.D.Bredl,W.Lieke,D.Meschede,W.Franz,H.Schafer		
40266	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	UBe13	Be13U1	Be	13	U	1																				1	1986																																														K		0.95					0.95	TC40266		K/GPa	0.16																																																																																												arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40267	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.9911Th0.0089Be13	U	0.9911	Th	0.0089	Be	13																		1	1986																																														K		0.66					0.66	TC40266		K/GPa	0.16																																																																																												arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40268	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.9981Th0.019Be13	U	0.9981	Th	0.019	Be	13																		1	1986																																														K		0.573					0.573	TC40268		K/GPa	0.5																																																																																												arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40269	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.974Th0.026Be13	U	0.974	Th	0.026	Be	13																		1	1986																																														K		0.58					0.58	TC40268		K/GPa	0.5																																																																																												arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40270	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.97Th0.03Be13	U	0.97	Th	0.03	Be	13																		1	1986																																														K		0.623					0.623	TC40270		K/GPa																																																																																													arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40271	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.9622Th0.0378Be13	U	0.9622	Th	0.0378	Be	13																		1	1986																																														K		0.557					0.557	TC40270		K/GPa																																																																																													arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40272	PRL0571619	nearly hydrostatic P. Tc defined as 10% change.	(U,Th)Be13	U0.9397Th0.0603Be13	U	0.9397	Th	0.0603	Be	13																		1	1986																																														K		0.344					0.344	TC40270		K/GPa	0.13																																																																																												arc-melting					Superconductivity under pressure in (U1-xThx)Be13: Evidence for two superconducting states				Phys.Rev.Lett., 57(1986)1619	S.E.Lambert,Y.Dalichaouch,M.B.Maple,J.L.Smith,Z.Fisk		
40273	PR04602958	residual resistivity from best fitting of R(T)	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1992																											2	Sc5Co4Si10			A	12.3158		4.076												K		8.5					8.5																																																											391.59	curve fitting of R(T)											uOhm.cm							12.8																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40274	PR04602958	residual resistivity from best fitting of R(T)	(Sc,Dy)5Ir4Si10	Sc4.5Dy0.5Ir4Si10	Sc	4.5	Dy	0.5	Ir	4	Si	10																	1992																											2	Sc5Co4Si10			A	12.3391		4.0917												K		6.95					6.95																																																											363.3	curve fitting of R(T)											uOhm.cm							20.22																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40275	PR04602958	residual resistivity from best fitting of R(T)	(Sc,Dy)5Ir4Si10	Sc4Dy1Ir4Si10	Sc	4	Dy	1	Ir	4	Si	10																	1992																											2	Sc5Co4Si10			A	12.3632		4.1066												K		5.95					5.95																																																											356.9	curve fitting of R(T)											uOhm.cm							40.95																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40276	PR04602958		(Sc,Dy)5Ir4Si10	Sc3.5Dy1.5Ir4Si10	Sc	3.5	Dy	1.5	Ir	4	Si	10																	1992								3.22																			2	Sc5Co4Si10			A	12.3881		4.1215												K		3.93					3.93																																																																																																arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40277	PR04602958		(Sc,Dy)5Ir4Si10	Sc3Dy2Ir4Si10	Sc	3	Dy	2	Ir	4	Si	10																	1992							11	3.5																			2	Sc5Co4Si10			A	12.4139		4.1364												K					2																																																																																																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40278	PR04602958		(Sc,Dy)5Ir4Si10	Sc2Dy3Ir4Si10	Sc	2	Dy	3	Ir	4	Si	10																	1992							13	4																			2	Sc5Co4Si10			A	12.4645		4.1661												K					2																																																																																																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40279	PR04602958	residual resistivity from best fitting of R(T)	(Sc,Dy)5Ir4Si10	Sc1Dy4Ir4Si10	Sc	1	Dy	4	Ir	4	Si	10																	1992							15.8	4.5																			2	Sc5Co4Si10			A	12.5186		4.1967												K					2																																																													309.3	curve fitting of R(T)											uOhm.cm							521.4																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40280	PR04602958	residual resistivity from best fitting of R(T)	(Sc,Dy)5Ir4Si10	Sc0.5Dy4.5Ir4Si10	Sc	0.5	Dy	4.5	Ir	4	Si	10																	1992								4.75																			2	Sc5Co4Si10			A	12.5435		4.2124												K					2																																																													315.3	curve fitting of R(T)											uOhm.cm							555																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40281	PR04602958	residual resistivity from best fitting of R(T)	Dy5Ir4Si10	Dy5Ir4Si10	Dy	5	Ir	4	Si	10																			1992							18.1	5																			2	Sc5Co4Si10			A	12.5693		4.2264												K					2																																																													406.2	curve fitting of R(T)											uOhm.cm							397																		arc-melting					Magnetism and superconductivity in Sc5-xDyxIr4Si10 alloys			Tata Institute of Fundamental Research, Bombay,India	Phys.Rev.B, 46(1992)2958	S.Ramakrishnan,K.Ghosh,Girsh Chandra		
40282	PR04810440	not SC	Dy5Os4Ge10	Dy5Os4Ge10	Dy	5	Os	4	Ge	10																			1993			emu/mol.K	72.09			-9.2	6																			2	Sc5Co4Si10	Pm3n		A	13.034		4.295																																																																														200.5	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40283	PR04810440	not SC	(Y,Dy)5Os4Ge10	Y1Dy4Os4Ge10	Y	1	Dy	4	Os	4	Ge	10																	1993			emu/mol.K	58.96			-8.1	4.8																			2	Sc5Co4Si10	Pm3n		A	13.0294		4.2946																																																																																																																	Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40284	PR04810440	not SC	(Y,Dy)5Os4Ge10	Y1.25Dy3.75Os4Ge10	Y	1.25	Dy	3.75	Os	4	Ge	10																	1993			emu/mol.K	54.88			-7.46	4.75																			2	Sc5Co4Si10	Pm3n		A	13.028		4.2945																																																																														222	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40285	PR04810440	not SC	(Y,Dy)5Os4Ge10	Y1.5Dy3.5Os4Ge10	Y	1.5	Dy	3.5	Os	4	Ge	10																	1993			emu/mol.K	50.55			-7.24	4.1																			2	Sc5Co4Si10	Pm3n		A	13.0272		4.2944																																																																														224	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40286	PR04810440		(Y,Dy)5Os4Ge10	Y2Dy3Os4Ge10	Y	2	Dy	3	Os	4	Ge	10																	1993			emu/mol.K	43.72			-2.1	3.1																			2	Sc5Co4Si10	Pm3n		A	13.0251		4.2941												K		2.86					2.86																				kOe	resistive transition	3.1												HC40286																									231	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40287	PR04810440		(Y,Dy)5Os4Ge10	Y2.5Dy2.5Os4Ge10	Y	2.5	Dy	2.5	Os	4	Ge	10																	1993			emu/mol.K	35.31			-1.28																				2	Sc5Co4Si10	Pm3n		A	13.0227		4.2938												K		3.8					3.8																																																																																														Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40288	PR04810440		(Y,Dy)5Os4Ge10	Y3Dy2Os4Ge10	Y	3	Dy	2	Os	4	Ge	10																	1993			emu/mol.K	29.53			-1.1																				2	Sc5Co4Si10	Pm3n		A	13.0205		4.2936												K		4.8					4.8																																																											249.4	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40289	PR04810440		(Y,Dy)5Os4Ge10	Y3.25Dy1.75Os4Ge10	Y	3.25	Dy	1.75	Os	4	Ge	10																	1993			emu/mol.K	25.42			-0.6																				2	Sc5Co4Si10	Pm3n		A	13.0191		4.2935												K		5.2					5.2																				kOe	resistive transition	6.9												HC40289																																																												Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40290	PR04810440		(Y,Dy)5Os4Ge10	Y4Dy1Os4Ge10	Y	4	Dy	1	Os	4	Ge	10																	1993			emu/mol.K	14.68			-0.14																				2	Sc5Co4Si10	Pm3n		A	13.0163		4.2931												K		6.9					6.9																				kOe	resistive transition	30																																					241	curve fitting of R(T)																																		Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40291	PR04810440		Y5Os4Ge10	Y5Os4Ge10	Y	5	Os	4	Ge	10																			1993																											2	Sc5Co4Si10	Pm3n		A	13.0121		4.2927												K		9.1					9.1																				kOe	resistive transition	61																																					234	curve fitting of R(T)											uOhm.cm											150												Dy(3N),Y(3N),Os(3N),Ge(5N)		arc-melting					MAGNETISM AND SUPERCONDUCTIVITY IN THE Y5-XDYXOS4GE10 SYSTEM	199310			PHYS.REV.B,48(1993)10440	GIRISH CHANDRA,K.GHOSH,S.RAMAKRISHNAN		
40292	PR08700799		KBi	Bi1K1	Bi	1	K	1																					1952																																														K		3.6					3.6																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40293	PR08700799		CaBi3	Bi3Ca1	Bi	3	Ca	1																					1952																																														K		1.7					1.7																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40294	PR08700799		BaBi3	Ba1Bi3	Ba	1	Bi	3																					1952																																														K		5.69					5.69																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40295	PR08700799		RhBi2	Bi2Rh1	Bi	2	Rh	1																					1952																																														K		2.2					2.2																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40296	PR08700799		RhBi4	Bi4Rh1	Bi	4	Rh	1																					1952																																														K		2.75					2.75																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40297	PR08700799		NiBi3	Bi3Ni1	Bi	3	Ni	1																					1952																																														K		3.6					3.6																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40298	PR08700799		ZrN	N1Zr1	N	1	Zr	1																					1952																																														K		9.05					9.05																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40299	PR08700799		VN	N1V1	N	1	V	1																					1952																																														K		7.5					7.5																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40300	PR08700799		Mo2C	C1Mo2	C	1	Mo	2																					1952																																														K		2.78					2.78																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40301	PR08700799		W2C	C1W2	C	1	W	2																					1952																																														K		2.74					2.74																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40302	PR08700799		Mo2B	B1Mo2	B	1	Mo	2																					1952																																														K		4.74					4.74																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40303	PR08700799		gamma-Mo2N	Mo2N1	Mo	2	N	1																					1952																																														K		5					5																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40304	PR08700799		delta-MoN	Mo1N1	Mo	1	N	1																					1952																											3																			K		12					12																																																																																																arc-melting					A Search for New Superconducting Compounds			Institute for Study of Metals, University of Chicago, Chikago, Illinois	Phys.Rev.B,87(1952)799	B.T. MATTHIAS,J.K. HULM		
40305	CHM0175935	T(sub)=973 K, dep. rate = 54 nm/h, thickness = 108 nm,	beta-Mo2N	Mo2N1	Mo	2	N	1																				5	2005																											2																			K		5.2					5.2																																																																																																pulsed laser deposition (P0=1.0 E-8 Torr). substrate = alpha-Al2O3 (001). radiation of N-radical					Synthesis and characterization of superconducting beta-Mo2N crystalline phase on a Si substrate: An application of pulsed laser deposition to nitride chemistry			Department of Applied Chemistry, Hiroshima University, Higashi-Hiroshima, Japan	Chem.Mater., 17(2005)5935	K.Inumaru,K.Baba,S.Yamanaka		
40306	P073052504	T(sub)=973 K, dep. rate = 8.2 nm/h, thickness = 49 nm, x = 0.86 in MoNx. distortion angle(alpha) = 89.41	MoN	Mo1N1	Mo	1	N	1																				5	2006																												NaCl			A	4.184													NaCl, B1,	K		4.2					4.2																																																																																																pulsed laser deposition (P0=1.0 E-8 Torr). substrate = alpha-Al2O3 (001). radiation of N-radical					Structural distortion and suppression of superconductivity in stoichiometric B1-MoN epitaxial thin films			Department of Applied Chemistry, Hiroshima University, Higashi-Hiroshima, Japan	Phys.Rev.B, 73(2006)052504	K.Inumaru,K.Baba,S.Yamanaka		
40307	JSC0090323	100 % (NH3) intercalation	Sr0.2(NH3)yTaS2	Sr0.2Ta1S2	Sr	0.2	Ta	1	S	2																			1974																												2H-MoS2																	2H-MoS2, C7,hP6	K		2.8					2.8																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40308	JSC0090323	40 % (NH3) intercalation	Sr0.2(NH3)yMoS2	Sr0.2Mo1S2	Sr	0.2	Mo	1	S	2																			1974																												2H-MoS2																	2H-MoS2, C7,hP6	K		5.1					5.1																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40309	JSC0090323	40 % (NH3) intercalation	Sr0.2(NH3)yWS2	Sr0.2W1S2	Sr	0.2	W	1	S	2																			1974																												2H-MoS2																	2H-MoS2, C7,hP6	K		3.5					3.5																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40310	JSC0090323	70 % (NH3) intercalation	Ca0.2(NH3)yMoS2	Ca0.2Mo1S2	Ca	0.2	Mo	1	S	2																			1974																												3R-MoS2																	3R-MoS2,  , hR9	K		3.6					3.6																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40311	JSC0090323	15 % (NH3) intercalation	Ba0.2(NH3)yMoS2	Ba0.2Mo1S2	Ba	0.2	Mo	1	S	2																			1974																												3R-MoS2																	3R-MoS2,  , hR9	K		5.7					5.7																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40312	JSC0090323	30 % (NH3) intercalation	Yb0.2(NH3)yMoS2	Yb0.2Mo1S2	Yb	0.2	Mo	1	S	2																			1974																												3R-MoS2																	3R-MoS2,  , hR9	K		2.4					2.4																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40313	JSC0090323	60 % (NH3) intercalation	Sr0.2(NH3)yMoSe2	Sr0.2Mo1Se2	Sr	0.2	Mo	1	Se	2																			1974																												2H-MoS2																	2H-MoS2, C7,hP6	K		5					5																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40314	JSC0090323	40 % (NH3) intercalation. SC transition is not clear.	Sr0.2(NH3)yWSe2	Sr0.2W1Se2	Sr	0.2	W	1	Se	2																			1974																												2H-MoS2																	2H-MoS2, C7,hP6	K		1.4					1.4																																																																																																alkaline earth metal and Y were intercalated to layered transition metal dichalcogenides in liquid ammonia.					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,M.W.Shafer,S.Kawarazaki		
40315	JPS0740851	not SC.  reaction(720C,2d)	(SnS)1+z(Ta,S2)2	Sn1.16Ta2S5.16	Sn	1.16	Ta	2	S	5.16																			2005																															A			17.75												K					2																																																																																																		stoichiometric(M,Ta,S) - mixed and press with delta= 0.14(Pb), 0.08(Bi), 0.16(Sn,Sb)  - reaction (720 or 800C,2d, in quartz ampoule)					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40316	JPS0740851	orthorhombic. reaction(720C,2d).	(PbS)1+z(Ta,S2)2	Pb1.14Ta2S5.14	Pb	1.14	Ta	2	S	5.14																			2005																											3				A			17.97												K				3.3			3.3																																																																																																stoichiometric(M,Ta,S) - mixed and press with delta= 0.14(Pb), 0.08(Bi), 0.16(Sn,Sb)  - reaction (720 or 800C,2d, in quartz ampoule)					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40317	JPS0740851	reaction(800C,2d)	(SbS)1+z(Ta,S2)2	Sb1.16Ta2S5.16	Sb	1.16	Ta	2	S	5.16																			2005																															A			17.51												K				3			3																																																																																																stoichiometric(M,Ta,S) - mixed and press with delta= 0.14(Pb), 0.08(Bi), 0.16(Sn,Sb)  - reaction (720 or 800C,2d, in quartz ampoule)					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40318	JPS0740851	monoclinic. reaction(720C,2d)	(BiS)1+z(Ta,S2)2	Bi1.08Ta2S5.08	Bi	1.08	Ta	2	S	5.08																			2005																															A			17.48												K				2.7			2.7																																																																																																stoichiometric(M,Ta,S) - mixed and press with delta= 0.14(Pb), 0.08(Bi), 0.16(Sn,Sb)  - reaction (720 or 800C,2d, in quartz ampoule)					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40319	JPS0740851	Na-content = 0.6 - 0.7. (HO)-content y = nearly 2.	Nax(H2O)y(SnS)1+z(TaS2)2	Na0.6Sn1Ta2S5	Na	0.6	Sn	1	Ta	2	S	5																	2005																															A			23.78												K				4			4																																																																																																hydration by topotactic reaction. samples were plaxed in 0.2 - 0.4M Na2S2O4 aqueous solution for several minutes at RT.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40320	JPS0740851	Na-content = 0.3 -0.5. (HO)-content y = nearly 2.	Nax(H2O)y(PbS)1+z(TaS2)2	Na0.3Pb1Ta2S5	Na	0.3	Pb	1	Ta	2	S	5																	2005																															A			23.91												K				3.7			3.7																																																																																																hydration by topotactic reaction. samples were plaxed in 0.2 - 0.4M Na2S2O4 aqueous solution for several minutes at RT.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40321	JPS0740851	Na-content = 0.3 -0.5. (HO)-content y = nearly 2.	Nax(H2O)y(SbS)1+z(TaS2)2	Na0.3Sb1Ta2S5	Na	0.3	Sb	1	Ta	2	S	5																	2005																															A			23.26												K				3.5			3.5																																																																																																hydration by topotactic reaction. samples were plaxed in 0.2 - 0.4M Na2S2O4 aqueous solution for several minutes at RT.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40322	JPS0740851	not SC.  Na-content = nearly 0.4. (HO)-content y = nearly 2.	Nax(H2O)y(BiS)1+z(TaS2)2	Na0.4Bi1Ta2S5	Na	0.4	Bi	1	Ta	2	S	5																	2005																															A			23.34												K					2																																																																																																		hydration by topotactic reaction. samples were plaxed in 0.2 - 0.4M Na2S2O4 aqueous solution for several minutes at RT.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
40323	JPS0732073	Tc, gap from NQR measurements. Fig. shows Tc(P) and gap(P).	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2004																												HoCoGa5			A	4.62		7.56												K		2.3					2.3	MTC40323																																															8.86	6																																															In-flux method					Magnetic Criticality and Unconventional Superconductivity in CeCoIn5: Study of 115In-Nuclear Quadrupole Resonance under Pressure			Department of Materials Science and Technology, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 73(2004)2073	M.Yashima,S.Kawasaki,Y.Kawasaki,G.-q.Zheng,Y.Kitaoka,H.Shishido,R.Settai,Y.Haga,Y.Onuki		
40324	ZPS1950215	P-induced SC. Tc at 115 kbar.	Ge	Ge1	Ge	1																							1966																																														K		5.35			0		5.35			GPa	-0.21																																																							275																																										Zur Supraleitung von Germanium und Silizium unter hohem Druck				Z.Physik, 195(1966)215	J.Wittig		
40325	ZPS1950215	P-induced SC. Tc at 120 kbar. (dTc/dP) has negative value.	Si	Si1	Si	1																							1966																																														K		6.7			0		6.7																																																											376																																										Zur Supraleitung von Germanium und Silizium unter hohem Druck				Z.Physik, 195(1966)215	J.Wittig		
40326	PHB2590001	p-induced SC. Pc =  GPa. Tc = Tc(max) at 16 GPa.	CeCu2Ge2	Ce1Cu2Ge2	Ce	1	Cu	2	Ge	2																			1999								4.1																				ThCr2Si2																		K		2			0		2	MTC40326																																																																																																				Magnetism and superconductivity in heavy fermion compounds at high pressure			University of Geneva, DPMC, 24 Quai E.- Ansermet, 1211 Gene% ve 4, Switzerland	Physica B, 259(1999)1	D.Jaccard,E.Vargoz,H.Wilhelm,K.Alami-Yadri		
40327	PR0301182	Tc(max) = 2.0 K at P = 40 kbar. For P>100 kbar, no sign of SC down to 1.2 K.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		1	1984																												ThCr2Si2																		K		0.7		0.67		0.05	0.7	MTC40327																																																																																															arc-melting					High-pressure valence instability and Tc maximum in superconducting CeCu2Si2				Phys.Rev.B, 30(1984)1182	B.Bellarbi,A.Benoit,D.Jaccard,J.M.Mignot,H.F.Braun		
40328	L096057001	entire Au-end-MWNT(multi-walled carbon nano-tube). (dV/dI) of junctions was measured.	C-nanotube	C1	C	1																							2006																																														K			12				12																																																																																																					Superconductivity in Entirely End-Bonded Multiwalled Carbon Nanotubes			Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.Lett., 96(2006)057001	I.Takesue,J.Haruyama,N.Kobayashi,S.Chiashi,S.Maruyama,T.Sugai,H.Shinohara		
40329	PCS0670751	anomaly in SUS not due to SC.	YbFe4Al8	Yb1Fe4Al8	Yb	1	Fe	4	Al	8																			2006								150																							A	8.712		5.044												K					1																																																																																																		induction melting					Magnetic and electronic properties of the antiferromagnetic YbFe4Al8 compound			Institute of Molecular Physics, Polish Academy of Sciences,Smoluchowskiego,Poznan.Poland	J.Phys.Chem.Solids, 67(2006)751	T.Tolinski,B.Andrzejewski,A.Kowalczyk,G.Chelkowska,A.Szlaferek,J.Frackowiak		
40330	JPS0742408		(Ca,Na)CuO2Cl2	Ca1.9Na0.1Cu1Cl2O2	Ca	1.9	Na	0.1	Cu	1	Cl	2													O	2		1	2005																												T																		K				8			8	TC40330									1																																																																																						high pressure synthesis					Magnetic Phase Diagram of Hole-Doped Ca2-xNaxCuO2Cl2 Cuprate Superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2408	K.Ohishi,I.Yamada,A.Koda,W.Higemoto,S.R.Saha,R.Kadono,K.M.Kojima,M.Azuma,M.Takano		
40331	JPS0742408		(Ca,Na)CuO2Cl2	Ca1.88Na0.12Cu1Cl2O2	Ca	1.88	Na	0.12	Cu	1	Cl	2													O	2		1	2005																												T																		K				16.8			16.8										16																																																																																						high pressure synthesis					Magnetic Phase Diagram of Hole-Doped Ca2-xNaxCuO2Cl2 Cuprate Superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2408	K.Ohishi,I.Yamada,A.Koda,W.Higemoto,S.R.Saha,R.Kadono,K.M.Kojima,M.Azuma,M.Takano		
40332	JPS0742408		(Ca,Na)CuO2Cl2	Ca1.85Na0.15Cu1Cl2O2	Ca	1.85	Na	0.15	Cu	1	Cl	2													O	2		1	2005																												T																		K				25			25										60																																																																																						high pressure synthesis					Magnetic Phase Diagram of Hole-Doped Ca2-xNaxCuO2Cl2 Cuprate Superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2408	K.Ohishi,I.Yamada,A.Koda,W.Higemoto,S.R.Saha,R.Kadono,K.M.Kojima,M.Azuma,M.Takano		
40333	JPS0742408		(Ca,Na)CuO2Cl2	Ca1.8Na0.2Cu1Cl2O2	Ca	1.8	Na	0.2	Cu	1	Cl	2													O	2		1	2005																												T																		K				26.4			26.4										48																																																																																						high pressure synthesis					Magnetic Phase Diagram of Hole-Doped Ca2-xNaxCuO2Cl2 Cuprate Superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2408	K.Ohishi,I.Yamada,A.Koda,W.Higemoto,S.R.Saha,R.Kadono,K.M.Kojima,M.Azuma,M.Takano		
40334	JPS0742408	not SC.	(Ca,Na)CuO2Cl2	Ca1.998Na0.002Cu1Cl2O2	Ca	1.998	Na	0.002	Cu	1	Cl	2													O	2		1	2005								240																				T																		K					5																																																																																																		high pressure synthesis					Magnetic Phase Diagram of Hole-Doped Ca2-xNaxCuO2Cl2 Cuprate Superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2408	K.Ohishi,I.Yamada,A.Koda,W.Higemoto,S.R.Saha,R.Kadono,K.M.Kojima,M.Azuma,M.Takano		
40335	JPS0742586	Two gap SC. DB shows higher value. GAPENE(1) = 2.7 - 3.8. GAP(1) = 1.6 - 2.3 meV. GAPENE(2) = 6.6 - 8.4, GAP(2) = 4.0 - 5.1 meV. by break junction tunneling.	ZrNCl0.7	Zr1N1Cl0.7	Zr	1	N	1	Cl	0.7																			2005																																														K		14					14																																														meV	4	6.6	1																																															mix(beta-ZrNCl + NaN3) - press to pellet - c-axis oriented sample. All process in pure Ar box.					Tunneling Spectroscopy of Deintercalated Layered Nitride Superconductor ZrNCl0.7			Graduate school of Advanced Sciences of Matter, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8530	J.Phys.Soc.Jpn, 74(2005)2586	T.Takasaki,T.Ekino,H.Fujii,S.Yamanaka		
40336	JPS0742667	Heavy Fermion SC. Tc defined by SUS.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																			2005																												ThCr2Si2																		K				1.1			1.1	MTC40336																																																																																																				Correlation among Long-Range Ordered States Revealed by Pressure versus Temperature Phase Diagram in URu2Si2			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602	J.Phys.Soc.Jpn, 74(2005)2667	S.Uemura,G.Motoyama,Y.Oda,T.Nishioka,N.Sato		
40337	JPS0742806		La(Pr,Ce)CuO4	Pr0.89La1Ce0.11Cu1O3.98	Pr	0.89	La	1	Ce	0.11	Cu	1													O	4-z	3.98		2005																												T'																		K		26					26																																																																																																					Field-Induced Uniform Antiferromagnetic Order Associated with Superconductivity in Pr1-xLaCexCuO4-z			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2806	R.Kadono,K.Ohishi,A.Koda,S.R.Saha,W.Higemoto,M.Fujita,K.Yamada		
40338	JPS0742806		La(Pr,Ce)CuO4	Pr0.85La1Ce0.15Cu1O3.95	Pr	0.85	La	1	Ce	0.15	Cu	1													O	4-z	3.95		2005																												T'																		K		19					19																																																																																																					Field-Induced Uniform Antiferromagnetic Order Associated with Superconductivity in Pr1-xLaCexCuO4-z			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 74(2005)2806	R.Kadono,K.Ohishi,A.Koda,S.R.Saha,W.Higemoto,M.Fujita,K.Yamada		
40339	JPS0743370	La<139>, P<31> NMR measurement shows the sample is s-wave SC. penetration depth estimated from Knight shift.	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																			2005																												skutterudite																		K		4.1					4.1																																									A		2200					3.8	6																																																				Evidence for s-Wave Superconductivity with Antiferromagnetic Fluctuations in Filled Skutterudite LaFe4P12: <139>La and <31>P-NMR Studies			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502	J.Phys.Soc.Jpn, 74(2005)3370	Y.Nakai,K.Ishida,D.Kikuchi,H.Sugawara,H.Sato		
40340	SSC1320379		MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2004																												ABO3			A	3.8091														K				7.1			7.1																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40341	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.995Ru0.005	Mg	1	C	1	Ni	2.995	Ru	0.005																	2004																												ABO3			A	3.8104														K				6.93			6.93																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40342	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.99Ru0.01	Mg	1	C	1	Ni	2.99	Ru	0.01																	2004																												ABO3			A	3.8105														K				6.71			6.71																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40343	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.98Ru0.02	Mg	1	C	1	Ni	2.98	Ru	0.02																	2004																												ABO3			A	3.8108														K				6.52			6.52	MTC40343																																																																																																				The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40344	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.967Ru0.033	Mg	1	C	1	Ni	2.967	Ru	0.033																	2004																												ABO3			A	3.8117														K				6.1			6.1																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40345	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.934Ru0.066	Mg	1	C	1	Ni	2.934	Ru	0.066																	2004																												ABO3			A	3.8135														K				5.6			5.6																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40346	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.9Ru0.1	Mg	1	C	1	Ni	2.9	Ru	0.1																	2004																												ABO3			A	3.817														K				4.72			4.72																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40347	SSC1320379		MgC(Ni,Ru)3	Mg1C1Ni2.8Ru0.2	Mg	1	C	1	Ni	2.8	Ru	0.2																	2004																												ABO3			A															K				3.47			3.47																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40348	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.999Fe0.001	Mg	1	C	1	Ni	2.999	Fe	0.001																	2004																												ABO3			A	3.8099														K				6.93			6.93																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40349	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.995Fe0.005	Mg	1	C	1	Ni	2.995	Fe	0.005																	2004																												ABO3			A	3.8102														K				6.44			6.44																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40350	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.99Fe0.01	Mg	1	C	1	Ni	2.99	Fe	0.01																	2004																												ABO3			A	3.8101														K				6.25			6.25																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40351	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.985Fe0.015	Mg	1	C	1	Ni	2.985	Fe	0.015																	2004																												ABO3			A	3.81														K				5.96			5.96	MTC40351																																																																																																				The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40352	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.98Fe0.02	Mg	1	C	1	Ni	2.98	Fe	0.02																	2004																												ABO3			A	3.8106														K				5.46			5.46																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40353	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.975Fe0.025	Mg	1	C	1	Ni	2.975	Fe	0.025																	2004																												ABO3			A	3.811														K				5.17			5.17																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40354	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.967Fe0.033	Mg	1	C	1	Ni	2.967	Fe	0.033																	2004																												ABO3			A	3.8107														K				4.9			4.9																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40355	SSC1320379		MgC(Ni,Fe)3	Mg1C1Ni2.95Fe0.05	Mg	1	C	1	Ni	2.95	Fe	0.05																	2004																												ABO3			A	3.8114														K				3.72			3.72																																																																																																					The effect of Fe and Ru substitution on the superconductivity in MgCNi3			Frick Laboratory, Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	Solid State Commun., 132(2004)379	T.Klimczuk,R.J.Cava		
40356	SSC1330321		MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2			A	3.0827		3.532												K	36.6						36.6																																																																																																					Structure and superconductivity of Mg1-xPbxB2			Departement de Physique, Faculte des Sciences de Bizerte, Laboratoire de Physique des Materiaux, Zarzouna 7021, Tunisia	Solid State Commun., 133(2005)321	A.Mchirgui,F.Ben Azzouz,M.Annabi,M.Zouaoui,M.Ben Salem		
40357	SSC1330321		(Mg,Pb)B2	Mg0.99Pb0.01B2	Mg	0.99	Pb	0.01	B	2																			2005																												AlB2			A	3.0801		3.53												K	35.9						35.9																																																																																																					Structure and superconductivity of Mg1-xPbxB2			Departement de Physique, Faculte des Sciences de Bizerte, Laboratoire de Physique des Materiaux, Zarzouna 7021, Tunisia	Solid State Commun., 133(2005)321	A.Mchirgui,F.Ben Azzouz,M.Annabi,M.Zouaoui,M.Ben Salem		
40358	SSC1330321		(Mg,Pb)B2	Mg0.98Pb0.02B2	Mg	0.98	Pb	0.02	B	2																			2005																												AlB2			A	3.0769		3.5283												K	35.5						35.5																																																																																																					Structure and superconductivity of Mg1-xPbxB2			Departement de Physique, Faculte des Sciences de Bizerte, Laboratoire de Physique des Materiaux, Zarzouna 7021, Tunisia	Solid State Commun., 133(2005)321	A.Mchirgui,F.Ben Azzouz,M.Annabi,M.Zouaoui,M.Ben Salem		
40360	SSC1330321		(Mg,Pb)B2	Mg0.94Pb0.06B2	Mg	0.94	Pb	0.06	B	2																			2005																												AlB2			A	3.0745		3.5277												K	35						35																																																																																																					Structure and superconductivity of Mg1-xPbxB2			Departement de Physique, Faculte des Sciences de Bizerte, Laboratoire de Physique des Materiaux, Zarzouna 7021, Tunisia	Solid State Commun., 133(2005)321	A.Mchirgui,F.Ben Azzouz,M.Annabi,M.Zouaoui,M.Ben Salem		
40361	SSC1330321		(Mg,Pb)B2	Mg0.9Pb0.1B2	Mg	0.9	Pb	0.1	B	2																			2005																												AlB2			A	3.0723		3.527												K	34						34																																																																																																					Structure and superconductivity of Mg1-xPbxB2			Departement de Physique, Faculte des Sciences de Bizerte, Laboratoire de Physique des Materiaux, Zarzouna 7021, Tunisia	Solid State Commun., 133(2005)321	A.Mchirgui,F.Ben Azzouz,M.Annabi,M.Zouaoui,M.Ben Salem		
40362	SSC1340725	Coexistence of SC and FM observed. But, FR temperature not given explicitely.	(La,Sr)2(Cu,Mn)O4	La1.77Sr0.23Cu0.94Mn0.06O4	La	1.77	Sr	0.23	Cu	0.94	Mn	0.06													O	4		1	2005																												T			A	3.7519		13.1423											K2NiF4	K			34				34																																																																																																solid state reaction					Superconductivity coexisting with ferromagnetism in mixed-valence Mn doped La1.85-(4/3)xSr0.15+(4/3)xCu1-xMnxO4			Structure Research Laboratory, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Solid State Commun., 134(2005)725	Huan Wu,Shun Tan,Yuheng Zhang		
40363	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2CaCu2O7	Tl0.5Pb0.5Sr2Ca1Cu2O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2											O	7		1	2005																												Tl1212			A	3.8028		12.1148												K	78		85	85			85																																																																							mOhm.cm							2.47				3.99												Tl2O3,PbO,SrCO3,CaCO3,CuO,Co2O3	1	precursor(Sr2Ca(Cu,Co)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40364	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Co)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.98Co0.02O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.98	Co	0.02									O	7		1	2005																												Tl1212			A	3.8031		11.1201												K	58		72				65																																																																							mOhm.cm							4.55				11.24												Tl2O3,PbO,SrCO3,CaCO3,CuO,Co2O3	1	precursor(Sr2Ca(Cu,Co)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40365	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Co)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.95Co0.05O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.95	Co	0.05									O	7		1	2005																												Tl1212			A	3.8039		12.1426												K	49		53	53			53																																																																							mOhm.cm							7.04				16.97												Tl2O3,PbO,SrCO3,CaCO3,CuO,Co2O3	1	precursor(Sr2Ca(Cu,Co)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40366	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Ni)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.98Ni0.02O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.98	Ni	0.02									O	7		1	2005																												Tl1212			A	3.8031		12.1025												K	58		69				63.5																																																																							mOhm.cm							6.07				12.89												Tl2O3,PbO,SrCO3,CaCO3,CuO,NiO	1	precursor(Sr2Ca(Cu,Ni)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40367	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Ni)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.95Ni0.05O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.95	Ni	0.05									O	7		1	2005																												Tl1212			A	3.8037		12.0748												K	44		50	50			50																																																																							mOhm.cm							10.14				22.64												Tl2O3,PbO,SrCO3,CaCO3,CuO,NiO	1	precursor(Sr2Ca(Cu,Ni)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40368	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Zn)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.98Zn0.02O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.98	Zn	0.02									O	7		1	2005																												Tl1212			A	3.8032		12.1264												K	65		77				71																																																																							mOhm.cm							3.53				10.46												Tl2O3,PbO,SrCO3,CaCO3,CuO,ZnO	1	precursor(Sr2Ca(Cu,Zn)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40369	SSC1350214	RESN shows resistivity at 0 K (extrapolated value)	(Tl,Pb)Sr2Ca(Cu,Zn)2O7	Tl0.5Pb0.5Sr2Ca1Cu2.95Zn0.05O7	Tl	0.5	Pb	0.5	Sr	2	Ca	1	Cu	2.95	Zn	0.05									O	7		1	2005																												Tl1212			A	3.804		12.1558												K	58		73	73			73																																																																							mOhm.cm							4.55				15.82												Tl2O3,PbO,SrCO3,CaCO3,CuO,ZnO	1	precursor(Sr2Ca(Cu,Zn)2Oz), mixed with Tl2O3, PbO. mixture - pellet - wrapped in Au foil - heat(850C,10min, in flowing O2) - FC to RT.					Effect of 3d metal ion doping on the structure and superconductivity of (Tl0.5Pb0.5)Sr2CaCu2O7			Chemistry Department, Faculty of Science, Tanta University, Tanta 31527, Egypt	Solid State Commun., 135(2005)214	E.Kandyel,M.A.Sekkina,M.A.T.Dawoud,M.Y.Bohnam		
40370	MMM2580067	RRR>1000. R measured for J//<100> and H//<011>. G-L = 10.	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																		3	2003																												skutterudite																		K		4.2					4.2																				T		1.72												MHC40370		A		140			A		1400																																										m3/C	0.00000000015										Sn-flux method					Anomalous transport properties in the filled skutterudites			Department of Physics, Tokyo Metropolitan University, Hachioji-shi, Tokyo,Japan	J.Mag.Mag.Mater., 258-259(2003)67	H.Sato,Y.Abe,T.D.Matsuda,K.Abe,N.Namiki,H.Sugawara,Y.Aoki		
40371	SSC0750047	layer compound (MS)nTS2. 3D-BCS superconductor. SP-lattice term(beta) = 1.40  mJ/mol.K4. (dC/gamma*Tc) = 1.3. Tc(SP) = 2.78 K.	(SnS)1.17NbS2	Sn1.17Nb1S3.17	Sn	1.17	Nb	1	S	3.17																		3	1990																												MS2																		K				2.75			2.75																																																								mJ/mol.K2	7.4																																							single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40372	SSC0750047	layer compound (MS)nTS2. 3D-BCS superconductor. SP-lattice term(beta) = 1.36  mJ/mol.K4. (dC/gamma*Tc) = 1.2. Tc(SP) = 2.73 K.	(PbS)1.14NbS2	Pb1.14Nb1S3.14	Pb	1.14	Nb	1	S	3.14																		3	1990																												MS2																		K				2.72			2.72																																																								mJ/mol.K2	6.9																																							single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40373	SSC0750047	layer compound (MS)nTS2. 3D-BCS superconductor.	(SnS)1.15TaS2	Sn1.15Ta1S3.15	Sn	1.15	Ta	1	S	3.15																		3	1990																												MS2																		K				2.85			2.85																																																																																																single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40374	SSC0750047	layer compound (MS)nTS2. 3D-BCS superconductor.	(PbS)1.13TaS2	Pb1.13Ta1S3.13	Pb	1.13	Ta	1	S	3.13																		3	1990																												MS2																		K				3.08			3.08																																																																																																single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40375	SSC0750047	layer compound (MS)nTS2. SP-lattice term(beta) = 1.78  mJ/mol.K4. (dC/gamma*Tc) = 0.6. Tc(SP) = 0.75 K.	(BiS)1.08TaS2	Bi1.08Ta1S3.08	Bi	1.08	Ta	1	S	3.08																		3	1990																												MS2																		K				0.76			0.76																																																								mJ/mol.K2	10.1																																							single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40376	SSC0750047	layer compound (MS)nTS2.	(SmS)1.15NbS2	Sm1.15Nb1S3.15	Sm	1.15	Nb	1	S	3.15																		3	1990																												MS2																		K					0.07																																																																																																		single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40377	SSC0750047	layer compound (MS)nTS2. 2D superconductor. SP-lattice term(beta) = 0.77  mJ/mol.K4.	(LaS)1.14NbS2	La1.14Nb1S3.14	La	1.14	Nb	1	S	3.14																		3	1990																												MS2																		K					0.07																																																										mJ/mol.K2	23																																							single crystals prepared by vapour transport method. (NH4)2PbCl6 was added. Cl is transport gas.					SUPERCONDUCTIVITY IN MISFIT LAYER COMPOUNDS (MS)NTS2			KAMERLINGH ONNES LABORATORY, LEIDEN UNIVERSITY, P.O. BOX 9506,2300 RA LEIDEN, THE NETHERLANDS.	SOLID STATE COMMUN.,75(1990)47	D.REEFMAN,H.B.BROM,J.BAAK	BI,PB,SN,LA,SM,NB,TA,S	
40378	PCS0670605	Tc defined as maximum (dM/dT). impurity phase : BaCuO2, CuO	LaBaCa(Cu,(PO4))3O7	La1Ba1Ca1Cu2.9P0.1O7.4-z	La	1	Ba	1	Ca	1	Cu	2.9	P	0.1											O	7.4-z			2006																												La1113			A	3.8374	3.8152	11.5039												K				20			20																																																																																														La2O3,BaCO3,CaCO3,CuO,NH4H2(PO4)		mixture - pellet - CAL(950C,24h) - SIN(975C,12h,in air) - ANN(575C,24h,in O2) - FC to RT					Superconductivity in the system CaLaBaCu3-x(PO4)xO7-z with x = 0.1, 0.3, 0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)605	V.L.De Los Santos,D.A.Bustamante,G.J.Gonzalez,S.J.Flores,X.Obradors		
40379	PCS0670605	Tc defined as maximum (dM/dT). impurity phase : BaCuO2, CuO	LaBaCa(Cu,(PO4))3O7	La1Ba1Ca1Cu2.7P0.3O8.2-z	La	1	Ba	1	Ca	1	Cu	2.7	P	0.3											O	8.2-z			2006																												La1113			A	3.8373	3.8061	11.502												K				14			14																																																																																														La2O3,BaCO3,CaCO3,CuO,NH4H2(PO4)		mixture - pellet - CAL(950C,24h) - SIN(975C,12h,in air) - ANN(575C,24h,in O2) - FC to RT					Superconductivity in the system CaLaBaCu3-x(PO4)xO7-z with x = 0.1, 0.3, 0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)605	V.L.De Los Santos,D.A.Bustamante,G.J.Gonzalez,S.J.Flores,X.Obradors		
40380	PCS0670605	Tc defined as maximum (dM/dT). impurity phase : BaCuO2, CuO	LaBaCa(Cu,(PO4))3O7	La1Ba1Ca1Cu2.5P0.5O9-z	La	1	Ba	1	Ca	1	Cu	2.5	P	0.5											O	9-z			2006																												La1113			A	3.8179	3.7655	11.4181												K				20			20																																																																																														La2O3,BaCO3,CaCO3,CuO,NH4H2(PO4)		mixture - pellet - CAL(950C,24h) - SIN(975C,12h,in air) - ANN(575C,24h,in O2) - FC to RT					Superconductivity in the system CaLaBaCu3-x(PO4)xO7-z with x = 0.1, 0.3, 0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)605	V.L.De Los Santos,D.A.Bustamante,G.J.Gonzalez,S.J.Flores,X.Obradors		
40381	PCS0670594		(Y,Ca)SrBa(Cu,(BO3))3O7	Y0.8Ca0.2Sr1Ba1Cu2.9B0.1O7.3-z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.9	B	0.1									O	7.3-z			2006																												Y123			A	3.8276	3.821	11.4187												K				35			35																																																																																														Y2O3,BaO2,SrCO3,CaCO3,CuO,H3BO3		mixture - heat(1273K,16h,in O2) - SIN(1273K,16h,inO2) FC(50C/h) to RT					Superconductivity in the system [Y0.8Ca0.2](SrBa)Cu3-x(BO3)xO7-z with 0.1=< x =<0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)594	D.A.Bustamante,V.L.De Los Santos,B.Willems,V.H.Barinotto C.,J.C.Gonzalez,X.Obradors		
40382	PCS0670594		(Y,Ca)SrBa(Cu,(BO3))3O7	Y0.8Ca0.2Sr1Ba1Cu2.8B0.2O7.6-z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.8	B	0.2									O	7.6-z			2006																												Y123			A	3.8309	3.8268	11.3901												K				37			37																																																																																														Y2O3,BaO2,SrCO3,CaCO3,CuO,H3BO3		mixture - heat(1273K,16h,in O2) - SIN(1273K,16h,inO2) FC(50C/h) to RT					Superconductivity in the system [Y0.8Ca0.2](SrBa)Cu3-x(BO3)xO7-z with 0.1=< x =<0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)594	D.A.Bustamante,V.L.De Los Santos,B.Willems,V.H.Barinotto C.,J.C.Gonzalez,X.Obradors		
40383	PCS0670594		(Y,Ca)SrBa(Cu,(BO3))3O7	Y0.8Ca0.2Sr1Ba1Cu2.7B0.3O7.9-z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.7	B	0.3									O	7.9-z			2006																												Y123			A	3.8272	3.8238	11.3615												K				38			38																																																																																														Y2O3,BaO2,SrCO3,CaCO3,CuO,H3BO3		mixture - heat(1273K,16h,in O2) - SIN(1273K,16h,inO2) FC(50C/h) to RT					Superconductivity in the system [Y0.8Ca0.2](SrBa)Cu3-x(BO3)xO7-z with 0.1=< x =<0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)594	D.A.Bustamante,V.L.De Los Santos,B.Willems,V.H.Barinotto C.,J.C.Gonzalez,X.Obradors		
40384	PCS0670594		(Y,Ca)SrBa(Cu,(BO3))3O7	Y0.8Ca0.2Sr1Ba1Cu2.6B0.4O8.2-z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.6	B	0.4									O	8.2-z			2006																												Y123			A	3.8762	3.816	11.622												K				31			31																																																																																														Y2O3,BaO2,SrCO3,CaCO3,CuO,H3BO3		mixture - heat(1273K,16h,in O2) - SIN(1273K,16h,inO2) FC(50C/h) to RT					Superconductivity in the system [Y0.8Ca0.2](SrBa)Cu3-x(BO3)xO7-z with 0.1=< x =<0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)594	D.A.Bustamante,V.L.De Los Santos,B.Willems,V.H.Barinotto C.,J.C.Gonzalez,X.Obradors		
40385	PCS0670594		(Y,Ca)SrBa(Cu,(BO3))3O7	Y0.8Ca0.2Sr1Ba1Cu2.5B0.5O8.5-z	Y	0.8	Ca	0.2	Sr	1	Ba	1	Cu	2.5	B	0.5									O	8.5-z			2006																												Y123			A	3.8303	3.8282	11.2754												K				28			28																																																																																														Y2O3,BaO2,SrCO3,CaCO3,CuO,H3BO3		mixture - heat(1273K,16h,in O2) - SIN(1273K,16h,inO2) FC(50C/h) to RT					Superconductivity in the system [Y0.8Ca0.2](SrBa)Cu3-x(BO3)xO7-z with 0.1=< x =<0.5			Lab. Superconductividad, Facultad de Ciencias Fisicas, Universidad Nacional Mayor de San Marcos, Ap. Postal 14-0149, Lima 14, Peru	J.Phys.Chem.Solids, 67(2006)594	D.A.Bustamante,V.L.De Los Santos,B.Willems,V.H.Barinotto C.,J.C.Gonzalez,X.Obradors		
40386	PCS0670431	small SC volume fraction but bulk SC.  crystal size = 5*7*36 mm3. x = 0.05 - 0.06 in (La1-xCax)2CaCu2O6+z were prepared.	(La,Ca)2CaCu2O6	La1.85Ca1.15Cu2O6+z	La	1.85	Ca	1.15	Cu	2															O	6+z		3	2006																												2126																		K				28			28										2																																																																																						floating zone method in a flow of pure O2(P=11 bar)					Crystal growth and superconductivity of (La1-xCax)2CaCu2O6+z			Brookhaven National Laboratory, Physics Department, Upton, NY 11973-5000, USA	J.Phys.Chem.Solids, 67(2006)431	G.D.Gu,M.Hucker,Y.-J.Kim,J.M.Tranquada,H.Dabkowska,G.M.Luke,T.Timusk,B.D.Gaulin,Q.Li,A.R.Moodenbaugh		
40387	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 2.84 meV.	Mg(B,C)2	Mg1B1.89C0.11	Mg	1	B	1.89	C	0.11																		3	2006																												AlB2																		K				34.7			34.7																																														meV	6.01		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40388	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 2.99 meV.	Mg(B,C)2	Mg1B1.834C0.166	Mg	1	B	1.834	C	0.166																		3	2006																												AlB2																		K				32			32	MTC40388																																													meV	5.46		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40389	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 2.76 meV.	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		3	2006																												AlB2																		K				28.8			28.8	GAP40389																																													meV	4.83		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40390	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 3.13 meV.	Mg(B,C)2	Mg1B1.736C0.264	Mg	1	B	1.736	C	0.264																		3	2006																												AlB2																		K				17.6			17.6																																														meV	3.13		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40391	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 2.84 meV.	MgB2	B2Mg1	B	2	Mg	1																				3	2006																												AlB2																		K				38.7			38.7																																														meV	7.12		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40392	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 2.84 meV.	(Mg,Al)B2	Mg0.98Al0.02B2	Mg	0.98	Al	0.02	B	2																		3	2006																												AlB2																		K				35.9			35.9	GAP40392																																													meV	6.89		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40393	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 3.17 meV.	(Mg,Al)B2	Mg0.92Al0.08B2	Mg	0.92	Al	0.08	B	2																		3	2006																												AlB2																		K				31.6			31.6																																														meV	6.12		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40394	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 0.77 meV.	(Mg,Al)B2	Mg0.82Al0.18B2	Mg	0.82	Al	0.18	B	2																		3	2006																												AlB2																		K				25.7			25.7	MTC40394																																													meV	4.02		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40395	PCS0670360	gap by point contact tunneling. Lower gap(pai) = 0.41 meV.	(Mg,Al)B2	Mg0.79Al0.21B2	Mg	0.79	Al	0.21	B	2																		3	2006																												AlB2																		K				27.1			27.1																																														meV	3.87		1																																															crystals grown by using high pressure method in a cubic anvil.					A point-contact study of the superconducting gaps in Al-substituted and C-substituted MgB2 single crystals			Dipartimento di Fisica and INFM, Politecnico di Torino, 10129 Torino, Italy	J.Phys.Chem.Solids, 67(2006)360	R.S.Gonnelli,D.Daghero,G.A.Ummarino,A.Calzolari,V.Dellarocca,V.A.Stepanov,S.M.Kazakov,J.Jun,J.Karpinski		
40396	PHB2300286	RRR=260.	YbSn3	Sn3Yb1	Sn	3	Yb	1																				3	1997																																														K		3.6					3.6										95										T		0.04																																					165	Bloch-Gruneisen relation of R																																		Yb(4N),Sn(5N)		Bridgeman method. nominal (Yb:Sn = 1.2:3). sample moving (3mm/h. T(max) = 850 C.					De Haas-van Alphen effect and magnetoresistance in YbSn3			Nagoya Institute of Technology, Nagoya,Japan	Physica B, 230-232(1997)286	I.Sakamoto,S.Ohara,I.Oguro,S.Maruno		
40397	PHB2300364	Heavy-fermion SC.	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																		3	1997								5																			3	PrNi2Al3	P6/mmm																	K		1.1					1.1																																																								mJ/mol.K2	130	SP-heat																																						floating zone method in a mirror furnace.					Superconducting and magnetic properties of UNi2Al3 single crystal				Physica B, 230-232(1997)364	M.Mihalik,F.E.Kayzel,T.Yoshida,K.Kuwahara,H.Amitsuka,T.Sakakibara,A.A.Menovsky,J.A.Mydosh,J.J.M.Franse		
40398	PHB2300380	dC = 28.95 mJ/mol.K. (dC/gamma*Tc) = 1.25	LaRhBi	La1Rh1Bi1	La	1	Rh	1	Bi	1																		1	1997																											3	TiNiSi			A	7.588	4.772	8.087											epsiron-TiNiSi type	K	2.35	2.36	2.6				2.36																																																								mJ/mol.K2	9.8	SP-heat	196	SP-heat																																				arc-melting					Kondo effect in CeRhBi and superconductivity in LaRhBi			Department of Physics, Faculty of Science,Tohoku University,Sendai,Japan	Physica B, 230-232(1997)380	S.Yoshii,D.Tazawa,M.Kasaya		
40399	PHB2300394	G-L = 41. Hc1, Hc2  measured  for H//[001].	U6Fe	Fe1U6	Fe	1	U	6																				3	1997																												U6Mn																		K		3.95					3.95											Oe	M-H	144							T	resistive	13.1												MHC40399		A	from Hc2	50			A	from Hc1	2060																																																			U6.1Fe		Czochoralski method in tetra-arc furnace. pulling speed = 10-15 mm/h. ANN(630C,1w)					Superconducting property of single crystal U6Fe			Japan Atomic Energy Research Institute, Tokai, Ibaraki,Japan	Physica B, 230-232(1997)394	E.Yamamoto,Y.Haga,A.Nakamura,N.Kimura,Y.Inada,H.Sugawara,H.Sato,Y.Onuki		
40400	SSC1370601	not SC	CuSr2(Ce,Y)3Cu2O11	Sr2Ce2.01Y0.99Cu3O11+z	Sr	2	Ce	2.01	Y	0.99	Cu	3													O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.823		17.23												K					4																																																																																																		mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40401	SSC1370601		(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.05Sr2Ce2.01Y0.99Cu2.95O11+z	Mo	0.05	Sr	2	Ce	2.01	Y	0.99	Cu	2.95											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.822		17.203												K				34			34																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40402	SSC1370601		(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.1Sr2Ce2.01Y0.99Cu2.9O11+z	Mo	0.1	Sr	2	Ce	2.01	Y	0.99	Cu	2.9											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.828		17.098												K				34			34																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40403	SSC1370601		(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.15Sr2Ce2.01Y0.99Cu2.85O11+z	Mo	0.15	Sr	2	Ce	2.01	Y	0.99	Cu	2.85											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.829		17.047												K				41			41																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40404	SSC1370601		(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.2Sr2Ce2.01Y0.99Cu2.8O11+z	Mo	0.2	Sr	2	Ce	2.01	Y	0.99	Cu	2.8											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.825		16.975												K				47			47																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40405	SSC1370601	impurity phase = CeO2	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.828		16.917												K				53			53																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40406	SSC1370601	impurity phase = CeO2	(Cu,W)Sr2(Ce,Y)3Cu2O11	W0.25Sr2Ce2.01Y0.99Cu2.75O11+z	W	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.82		16.988												K				53			53																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40407	SSC1370601	impurity phase = CeO2	(Cu,Re)Sr2(Ce,Y)3Cu2O11	Re0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Re	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.824		16.938												K				56			56																																																																																																mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40408	SSC1370601	impurity phase = CeO2	(Cu,Pb)Sr2(Ce,Y)3Cu2O11	Pb0.25Sr2Ce2.01Y0.99Cu2.75O11+z	Pb	0.25	Sr	2	Ce	2.01	Y	0.99	Cu	2.75											O	11+z		1	2006																											2	Cu1232	P4/mmm		A	3.83		17.23												K					4																																																																																																		mixture - CAL(950C,24h) - SIN(1020-1030C,24h) - mixed (sample+Ag2O2: mole ratio = 4:3) - ANN(500C,30min,5 GPa)					Superconductivity in the 'triple-fluorite-layer' copper oxides (Cu,M)-1232 (M = Mo, W, Re, Pb)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 137(2006)601	I.Grigoraviciute,M.Arai,H.Yamauchi,M.Karppinen		
40409	L090197005		(Pr,La,Ce)2CuO4	Pr0.91La1Ce0.09Cu1O4	Pr	0.91	La	1	Ce	0.09	Cu	1													O	4		3	2003																												T'																		K				24			24																				T	SUS			7.5										HC40409																																																														traveling solvent floating zone method					Fermi-Liquid Ground State in the n-Type Pr0.91LaCe0.09CuO4-y Copper-Oxide Superconductor			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 90(2003)197005	Guo-qing Zheng,T.Sato,Y.Kitaoka,M.Fujita,K.Yamada		
40410	PHC4360025	Jc obtained from dM(magnetization)	EuBa2Cu3O7	Eu1Ba2Cu3Oz	Eu	1	Ba	2	Cu	3															O	z		1	2006																												Y123			A	3.8533	3.906	11.7181												K				93			93																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40411	PHC4360025	Jc obtained from dM(magnetization)	(Eu,Ca)Ba2Cu3O7	Eu0.8Ca0.2Ba2Cu3Oz	Eu	0.8	Ca	0.2	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8485	3.8927	11.7099												K				80.1			80.1																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40412	PHC4360025	Jc obtained from dM(magnetization)	(Eu,Ca)Ba2Cu3O7	Eu0.75Ca0.25Ba2Cu3Oz	Eu	0.75	Ca	0.25	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8549	3.8934	11.7205												K				79.7			79.7																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40413	PHC4360025	Jc obtained from dM(magnetization)	(Eu,Ca)Ba2Cu3O7	Eu0.7Ca0.3Ba2Cu3Oz	Eu	0.7	Ca	0.3	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8549	3.8802	11.7199												K				79.7			79.7																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40414	PHC4360025	Jc obtained from dM(magnetization)	GdBa2Cu3O7	Gd1Ba2Cu3Oz	Gd	1	Ba	2	Cu	3															O	z		1	2006																												Y123			A	3.8432	3.906	11.7181												K				91.7			91.7																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40415	PHC4360025	Jc obtained from dM(magnetization)	(Gd,Ca)Ba2Cu3O7	Gd0.8Ca0.2Ba2Cu3Oz	Gd	0.8	Ca	0.2	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8475	3.8996	11.7221												K				81			81																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40416	PHC4360025	Jc obtained from dM(magnetization)	(Gd,Ca)Ba2Cu3O7	Gd0.75Ca0.25Ba2Cu3Oz	Gd	0.75	Ca	0.25	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8488	3.8954	11.7418												K				80			80																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40417	PHC4360025	Jc obtained from dM(magnetization)	(Gd,Ca)Ba2Cu3O7	Gd0.7Ca0.3Ba2Cu3Oz	Gd	0.7	Ca	0.3	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8428	3.8933	11.7497												K				79			79																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40418	PHC4360025	Jc obtained from dM(magnetization)	ErBa2Cu3O7	Er1Ba2Cu3Oz	Er	1	Ba	2	Cu	3															O	z		1	2006																												Y123			A	3.8164	3.8868	11.6605												K				90.9			90.9																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40419	PHC4360025	Jc obtained from dM(magnetization)	(Er,Ca)Ba2Cu3O7	Er0.8Ca0.2Ba2Cu3Oz	Er	0.8	Ca	0.2	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8216	3.8817	11.6985												K				78.5			78.5																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40420	PHC4360025	Jc obtained from dM(magnetization)	(Er,Ca)Ba2Cu3O7	Er0.75Ca0.25Ba2Cu3Oz	Er	0.75	Ca	0.25	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.8225	3.8762	11.6989												K				71.6			71.6																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40421	PHC4360025	Jc obtained from dM(magnetization)	(Er,Ca)Ba2Cu3O7	Er0.7Ca0.3Ba2Cu3Oz	Er	0.7	Ca	0.3	Ba	2	Cu	3													O	z		1	2006																												Y123			A	3.823	3.8752	11.6924												K				75.7			75.7																																																																																																mixture - heat(900C,21h,in flowing O2) - heat(930C,21h,in flowing O2) - ANN(450C,23h)					Effects of calcium substitution on the superconducting properties of R1-xCaxBa2Cu3Oz (R = Eu, Gd, Er; 0 =< x =< 0.3) polycrystalline samples			Institute of Solid State Physics, Bulgarian Academy of Sciences, 72, Tzarigradsko Chaussee Blvd., 1784 Sofia, Bulgaria	Physica C, 436(2006)25	E.K.Nazarova,K.Nenkov,G.Fuchs,K.-H.Muller		
40422	PHC4360051		(Cu,Tl)Ba2Ca2Cu3Oz	Tl0.5Ba2Ca2Cu3.5Oz	Tl	0.5	Ba	2	Ca	2	Cu	3.5													O	z			2006																												Tl1223			A	3.913		15.08												K																																																																																																					Ba(NO3)2,Ca(NO3)2,Cu(CN)2,BeO,Tl2O3		precursor(Cu-Ba-Ca-Be-Cu-O) was mixed with Tl2O3.  Then, wrapped in Al-foil  - SIN(880C,7min) - Q to RT					Superconductivity in Be substituted by Ca in Cu0.5Tl0.5Ba2Can-1-yBeyCunO2n+4-d (n = 3,4 and y = 0.7, 1.5, 1.7, 2.0)			Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 436(2006)51	Nawazish A.Khan,G.Husnain		
40423	PHC4360051	O-content measuring method not given.	(Cu,Tl)Ba2(Ca,Be)2Cu3Oz	Tl0.5Ba2Ca1.3Be0.7Cu3.5O7.886	Tl	0.5	Ba	2	Ca	1.3	Be	0.7	Cu	3.5											O	z	7.886		2006																												Tl1223			A	3.905		15.058												K	92		115	95			95																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,BeO,Tl2O3		precursor(Cu-Ba-Ca-Be-Cu-O) was mixed with Tl2O3.  Then, wrapped in Al-foil  - SIN(880C,7min) - Q to RT					Superconductivity in Be substituted by Ca in Cu0.5Tl0.5Ba2Can-1-yBeyCunO2n+4-d (n = 3,4 and y = 0.7, 1.5, 1.7, 2.0)			Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 436(2006)51	Nawazish A.Khan,G.Husnain		
40424	PHC4360051	O-content measuring method not given.	(Cu,Tl)Ba2(Ca,Be)2Cu3Oz	Tl0.5Ba2Ca0.3Be1.7Cu3.5O7.685	Tl	0.5	Ba	2	Ca	0.3	Be	1.7	Cu	3.5											O	z	7.685		2006																												Tl1223			A	3.909		15.065												K				115			115																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,BeO,Tl2O3		precursor(Cu-Ba-Ca-Be-Cu-O) was mixed with Tl2O3.  Then, wrapped in Al-foil  - SIN(880C,7min) - Q to RT					Superconductivity in Be substituted by Ca in Cu0.5Tl0.5Ba2Can-1-yBeyCunO2n+4-d (n = 3,4 and y = 0.7, 1.5, 1.7, 2.0)			Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 436(2006)51	Nawazish A.Khan,G.Husnain		
40425	PHC4360051	post ANN(600C). O-content measuring method not given.	(Cu,Tl)Ba2(Ca,Be)3Cu4Oz	Tl0.5Ba2Ca1.5Be1.5Cu4.5O9.887	Tl	0.5	Ba	2	Ca	1.5	Be	1.5	Cu	4.5											O	z	9.887		2006																												Tl1234																		K	96		110	115			115																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,BeO,Tl2O3		precursor(Cu-Ba-Ca-Be-Cu-O) was mixed with Tl2O3.  Then, wrapped in Al-foil  - SIN(880C,7min) - Q to RT					Superconductivity in Be substituted by Ca in Cu0.5Tl0.5Ba2Can-1-yBeyCunO2n+4-d (n = 3,4 and y = 0.7, 1.5, 1.7, 2.0)			Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 436(2006)51	Nawazish A.Khan,G.Husnain		
40426	PHC4360051	post ANN(600C). O-content measuring method not given.	(Cu,Tl)Ba2(Ca,Be)3Cu4Oz	Tl0.5Ba2Ca1Be2Cu4.5O9.948	Tl	0.5	Ba	2	Ca	1	Be	2	Cu	4.5											O	z	9.948		2006																												Tl1234																		K	96			110			110																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,BeO,Tl2O3		precursor(Cu-Ba-Ca-Be-Cu-O) was mixed with Tl2O3.  Then, wrapped in Al-foil  - SIN(880C,7min) - Q to RT					Superconductivity in Be substituted by Ca in Cu0.5Tl0.5Ba2Can-1-yBeyCunO2n+4-d (n = 3,4 and y = 0.7, 1.5, 1.7, 2.0)			Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 436(2006)51	Nawazish A.Khan,G.Husnain		
40427	PHC4360081	O-content = 3.99 - 3.97. Hall coeff. RH(T) measured.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O3.98	Pr	1.85	Ce	0.15	Cu	1															O	4-z	3.98	1	2006																												T'			A	3.968		12.121												K		21.2					21.2																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40428	PHC4360081	O-content = 3.99 - 3.97. Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.99V0.01O3.98	Pr	1.85	Ce	0.15	Cu	0.99	V	0.01													O	4-z	3.98	1	2006																												T'			A	3.964		12.158												K		22					22																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40429	PHC4360081	O-content = 3.99 - 3.97. Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.98V0.02O3.98	Pr	1.85	Ce	0.15	Cu	0.98	V	0.02													O	4-z	3.98	1	2006																												T'			A	3.965		12.153												K		22.3					22.3																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40430	PHC4360081	O-content = 3.99 - 3.97. Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.97V0.03O3.98	Pr	1.85	Ce	0.15	Cu	0.97	V	0.03													O	4-z	3.98	1	2006																												T'			A	3.964		12.15												K		21.2					21.2																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40431	PHC4360081	O-content = 3.99 - 3.97. Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.96V0.04O3.98	Pr	1.85	Ce	0.15	Cu	0.96	V	0.04													O	4-z	3.98	1	2006																												T'			A	3.961		12.157												K		22.4	25.6				22.4																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40432	PHC4360081	Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.94V0.06O4-z	Pr	1.85	Ce	0.15	Cu	0.94	V	0.06													O	4-z		1	2006																												T'			A	3.957		12.199												K		15.4					15.4																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40433	PHC4360081	Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.92V0.08O4-z	Pr	1.85	Ce	0.15	Cu	0.92	V	0.08													O	4-z		1	2006																												T'			A	3.954		12.236												K					4.2																																																																																																Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40434	PHC4360081	Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,V)O4	Pr1.85Ce0.15Cu0.9V0.1O4-z	Pr	1.85	Ce	0.15	Cu	0.9	V	0.1													O	4-z		1	2006																												T'			A	3.95		12.255												K					4.2																																																																																																Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40435	PHC4360081	Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.995Ni0.005O4-z	Pr	1.85	Ce	0.15	Cu	0.995	Ni	0.005													O	4-z		1	2006																												T'			A	3.961		12.189												K		17.5					17.5																																																																																														Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40436	PHC4360081	Hall coeff. RH(T) measured.	(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.99Ni0.01O4-z	Pr	1.85	Ce	0.15	Cu	0.99	Ni	0.01													O	4-z		1	2006																												T'			A	3.96		12.198												K					4.2																																																																																																Pr6O11,CeO2,CuO,V2O5(or Ni2O3)		mixture - CAL(920 and 960C,24h, in air) - SIN(1000C,24h) - ANN(900-960C,12h, in flowing N2)					Effect on superconductivity of high valence ions V4+ and Ni3+ substitution for Cu site in Pr1.85Ce0.15CuO4-d system			Department of Physics, Shanghai University, Shangda Road, 99, Shanghai 200444, China	Physica C, 436(2006)81	Fen Liu,Shixun,Cao,Jincang Zhang,Lingwei Li,Changyun Chi		
40437	PCS0670529		CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2006																																														K		0.73					0.73	MTC40437																																																																																															excess Cu flux. (40 mol %Cu + 60 mol %CeCu2(Si,Ge)2)					Superconducting phases and quantum criticality in CeCu2Si2			MPI for Chemical Physics of Solids, High Pressure Science Section, Dresden 01187 Germany	J.Phys.Chem.Solids, 67(2006)529	G.Sparn,O.Stockert,F.M.Grosche,H.Q.Yuan,E.Faulhaber,C.Geibel,M.Deppe,H.S.Jeevan,M.Loewenhaupt,G.Zwicknagl,F.Steglich		
40438	PCS0670529	Two SC regions. Tc(max) = 0.96K (P=5.4 GPa) for region-1 and Tc(max) = 0.39 K (P=1 GPa) for region-2.	CeCu2(Si,Ge)2	Ce1Cu2Si1.8Ge0.2	Ce	1	Cu	2	Si	1.8	Ge	0.2																3	2006								1.3																																						K		0.12					0.12	MTC40438																																																																																															excess Cu flux. (40 mol %Cu + 60 mol %CeCu2(Si,Ge)2)					Superconducting phases and quantum criticality in CeCu2Si2			MPI for Chemical Physics of Solids, High Pressure Science Section, Dresden 01187 Germany	J.Phys.Chem.Solids, 67(2006)529	G.Sparn,O.Stockert,F.M.Grosche,H.Q.Yuan,E.Faulhaber,C.Geibel,M.Deppe,H.S.Jeevan,M.Loewenhaupt,G.Zwicknagl,F.Steglich		
40439	PCS0670529	not SC	CeCu2(Si,Ge)2	Ce1Cu2Si1.5Ge0.5	Ce	1	Cu	2	Si	1.5	Ge	0.5																3	2006								1.9																																						K					0.2			MTC40439																																																																																															excess Cu flux. (40 mol %Cu + 60 mol %CeCu2(Si,Ge)2)					Superconducting phases and quantum criticality in CeCu2Si2			MPI for Chemical Physics of Solids, High Pressure Science Section, Dresden 01187 Germany	J.Phys.Chem.Solids, 67(2006)529	G.Sparn,O.Stockert,F.M.Grosche,H.Q.Yuan,E.Faulhaber,C.Geibel,M.Deppe,H.S.Jeevan,M.Loewenhaupt,G.Zwicknagl,F.Steglich		
40440	PHC4340141		La3CaBa3Cu7Oz	La3Ca1Ba3Cu7O16.678	La	3	Ca	1	Ba	3	Cu	7													O	z	16.678	1	2006																												3137			A	3.866		11.6218												K	80		81				80.5																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40441	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.9Cd0.1Ba3Cu7O16.611	La	3	Ca	0.9	Cd	0.1	Ba	3	Cu	7											O	z	16.611	1	2006																												3137			A	3.8662		11.6287												K	77		78				77.5																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40442	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.8Cd0.2Ba3Cu7O16.536	La	3	Ca	0.8	Cd	0.2	Ba	3	Cu	7											O	z	16.536	1	2006																												3137			A	3.8668		11.6324												K	75		77				76																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40443	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.7Cd0.3Ba3Cu7O16.459	La	3	Ca	0.7	Cd	0.3	Ba	3	Cu	7											O	z	16.459	1	2006																												3137			A	3.8676		11.6369												K	70		73				71.5																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40444	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.6Cd0.4Ba3Cu7O16.41	La	3	Ca	0.6	Cd	0.4	Ba	3	Cu	7											O	z	16.41	1	2006																												3137			A	3.8685		11.6492												K	65		70				67.5																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40445	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.5Cd0.5Ba3Cu7O16.375	La	3	Ca	0.5	Cd	0.5	Ba	3	Cu	7											O	z	16.375	1	2006																												3137			A	3.8692		11.6586												K	56		62				59																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40446	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.4Cd0.6Ba3Cu7O16.336	La	3	Ca	0.4	Cd	0.6	Ba	3	Cu	7											O	z	16.336	1	2006																												3137			A	3.8701		11.6695												K	45		52				48.5																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40447	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.3Cd0.7Ba3Cu7O16.303	La	3	Ca	0.3	Cd	0.7	Ba	3	Cu	7											O	z	16.303	1	2006																												3137			A	3.871		11.6826												K	32		40				36																																																																																														La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40448	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.2Cd0.8Ba3Cu7O16.261	La	3	Ca	0.2	Cd	0.8	Ba	3	Cu	7											O	z	16.261	1	2006																												3137			A	3.8717		11.6949												K			26																																																																																																		La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40449	PHC4340141		La3(Ca,Cd)Ba3Cu7Oz	La3Ca0.1Cd0.9Ba3Cu7O16.217	La	3	Ca	0.1	Cd	0.9	Ba	3	Cu	7											O	z	16.217	1	2006																												3137			A	3.8726		11.7073												K					5																																																																																																La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40450	PHC4340141		La3CdBa3Cu7Oz	La3Cd1Ba3Cu7O16.188	La	3	Cd	1	Ba	3	Cu	7													O	z	16.188	1	2006																												3137			A	3.8738		11.7168												K					5																																																																																																La2O3,CdO,CaCO3,BaCO3,CuO		To obtain fully oxygenated samples, ANN(773K, 12h, in O2-flow), then slow cool to RT (1K/min)					On the effect of Cd doping for Ca in La3CaBa3Cu7Oy superconducting cuprate			Faculty of Science, Department of Chemistry, Tanta University, Tanta 31527, Egypt	Physica C, 434(2006)141	Elsayed Kandyel,Khaled M.Elsabawy		
40451	PHC4340178		NdBa2Cu3O7	Nd1Ba2Cu3O7	Nd	1	Ba	2	Cu	3															O	6+z	7	1	2006																												Y123			A	3.8649	3.9163	11.767												K		95.1					95.1																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40452	PHC4340178	Sr partially occupied Nd site. Nd partially on Ba site	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.8Sr0.2Cu3O6.96	Nd	1	Ba	1.8	Sr	0.2	Cu	3													O	6+z	6.96	1	2006																												Y123			A	3.8646	3.9043	11.741												K		91.1					91.1																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40453	PHC4340178	Sr partially occupied Nd site. Nd partially on Ba site	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.6Sr0.4Cu3O6.94	Nd	1	Ba	1.6	Sr	0.4	Cu	3													O	6+z	6.94	1	2006																												Y123			A	3.8656	3.8954	11.719												K		86					86																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40454	PHC4340178	Sr partially occupied Nd site. Nd partially on Ba site	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.4Sr0.6Cu3O6.94	Nd	1	Ba	1.4	Sr	0.6	Cu	3													O	6+z	6.94	1	2006																												Y123			A	3.8702	3.8856	11.699												K		75					75																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40455	PHC4340178	Sr partially occupied Nd site. Nd partially on Ba site	Nd(Ba,Sr)2Cu3O7	Nd1Ba1.2Sr0.8Cu3O6.97	Nd	1	Ba	1.2	Sr	0.8	Cu	3													O	6+z	6.97	1	2006																												Y123			A	3.869	3.8757	11.673												K		66.9					66.9																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40456	PHC4340178	Sr partially occupied Nd site. Nd partially on Ba site	Nd(Ba,Sr)2Cu3O7	Nd1Ba1Sr1Cu3O7.02	Nd	1	Ba	1	Sr	1	Cu	3													O	6+z	7.02	1	2006																												Y123			A	3.8667	3.8691	11.637												K		49.9					49.9																																																																																														Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40457	PHC4340178	not SC	PrBa2Cu3O7	Pr1Ba2Cu3O6.98	Pr	1	Ba	2	Cu	3															O	6+z	6.98	1	2006								16.8																				Y123			A	3.8565	3.9238	11.699												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40458	PHC4340178	not SC	Pr(Ba,Sr)2Cu3O7	Pr1Ba1.8Sr0.2Cu3O6.97	Pr	1	Ba	1.8	Sr	0.2	Cu	3													O	6+z	6.97	1	2006								18.8																				Y123			A	3.8542	3.9197	11.688												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40459	PHC4340178	not SC	Pr(Ba,Sr)2Cu3O7	Pr1Ba1.6Sr0.4Cu3O6.99	Pr	1	Ba	1.6	Sr	0.4	Cu	3													O	6+z	6.99	1	2006								19.8																				Y123			A	3.856	3.9069	11.663												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40460	PHC4340178	not SC	Pr(Ba,Sr)2Cu3O7	Pr1Ba1.4Sr0.6Cu3O6.97	Pr	1	Ba	1.4	Sr	0.6	Cu	3													O	6+z	6.97	1	2006								20.6																				Y123			A	3.872	3.8852	11.643												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40461	PHC4340178	not SC	Pr(Ba,Sr)2Cu3O7	Pr1Ba1.2Sr0.8Cu3O6.96	Pr	1	Ba	1.2	Sr	0.8	Cu	3													O	6+z	6.96	1	2006								18.8																				Y123			A	3.8648		11.638												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40462	PHC4340178	not SC	Pr(Ba,Sr)2Cu3O7	Pr1Ba1Sr1Cu3O6.98	Pr	1	Ba	1	Sr	1	Cu	3													O	6+z	6.98	1	2006								16.2																				Y123			A	3.8626		11.624												K					4																																																																																																Nd2O3(or Pr6O11),BaCO3,SrCO3,CuO		mixture - SIN(950-980C) - heat(950(Nd), 900(Pr), 10h, in flowing gas(Ar:O2=100:1)) - slow cool to 400C ANN(400C,60h, in flowing O2) - FC to RT					Comparison of the Sr substitution effect on Nd(Ba1 xSrx)2Cu3O6+d and Pr(Ba1-xSrx)2Cu3O6+d prepared under reducing atmosphere			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), 1-1 Oho, Tsukuba, Ibaraki 305-0801, Japan	Physica C, 434(2006)178	T.Wuernisha,F.Sano,Y.Takahashi,T.Kamiyama,Y.Takano,K.Sekizawa		
40463	P066014531	not SC. thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.94Ce0.06Cu1O4	La	1.94	Ce	0.06	Cu	1															O	4		4	2002																												T'			A			12.4811												K					4																																																																																							m3/C	-0.00000000054					RH40463					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40464	P066014531	thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.92Ce0.08Cu1O4	La	1.92	Ce	0.08	Cu	1															O	4		4	2002																												T'			A			12.4707												K	13.9						13.9																																																																																					m3/C	-0.00000000031					RH40464					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40465	P066014531	thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.89Ce0.11Cu1O4	La	1.89	Ce	0.11	Cu	1															O	4		4	2002																												T'			A			12.4507												K	24.9						24.9																																																																																					m3/C	-0.00000000044					RH40465					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40466	P066014531	thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.87Ce0.13Cu1O4	La	1.87	Ce	0.13	Cu	1															O	4		4	2002																												T'			A			12.4307												K	22						22																																																																																					m3/C	-0.00000000003					RH40466					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40467	P066014531	thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.85Ce0.15Cu1O4	La	1.85	Ce	0.15	Cu	1															O	4		4	2002																												T'			A			12.4211												K	10						10																																																																																					m3/C	0.00000000018					RH40467					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40468	P066014531	R is not zero at 4 K. thickness = 1000A. ANN(650C, 5.0E-7 Torr < P(O2) < 1.0E-6 Torr)	(La,Ce)2CuO4	La1.84Ce0.16Cu1O4	La	1.84	Ce	0.16	Cu	1															O	4		4	2002																												T'			A			12.4011												K			6																																																																																									m3/C	0.0000000004					RH40468					films deposited on (100)SrTiO3 substrates by a pulsed laser deposition. buffer layer = BTO					Electron-doped superconductor La2-xCexCuO4: Preparation of thin films and modified doping range for superconductivity			Correlated Electron Research Center (CERC), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki, Japan	Phys.Rev.B, 66(2002)14531	A.Sawa,H.Takagi,M.Kawasaki,Y.Tokura		
40469	PRL0744927	Hall coeffic. measured	(Pr,Ce)2CuO4	Pr1.96Ce0.04Cu1O4	Pr	1.96	Ce	0.04	Cu	1															O	4		3	1995																												T'																		K		23.6					23.6	TC40469																																																																																															new reduction process: single crystals sandwiched with the same composition crystals, then heat(1080C,80h)					Extended superconducting concentration range observed in Pr2-xCexCuO4-z			Ruhr-Universitat Bochum, Bochum,Germany	Phys.Rev.Lett., 74(1995)4927	M.Brinkmann,T.Rex,H.Bach,K.Westerholt		
40470	PRL0744927	Hall coeffic. measured	(Pr,Ce)2CuO4	Pr1.91Ce0.09Cu1O4	Pr	1.91	Ce	0.09	Cu	1															O	4		3	1995																												T'																		K		21.5					21.5																																																																																																new reduction process: single crystals sandwiched with the same composition crystals, then heat(1080C,80h)					Extended superconducting concentration range observed in Pr2-xCexCuO4-z			Ruhr-Universitat Bochum, Bochum,Germany	Phys.Rev.Lett., 74(1995)4927	M.Brinkmann,T.Rex,H.Bach,K.Westerholt		
40471	PRL0744927	Hall coeffic. measured	(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O4	Pr	1.83	Ce	0.17	Cu	1															O	4		3	1995																												T'																		K		20.3					20.3																																																																																																new reduction process: single crystals sandwiched with the same composition crystals, then heat(1080C,80h)					Extended superconducting concentration range observed in Pr2-xCexCuO4-z			Ruhr-Universitat Bochum, Bochum,Germany	Phys.Rev.Lett., 74(1995)4927	M.Brinkmann,T.Rex,H.Bach,K.Westerholt		
40472	PR0510404	(dC/gamma*Tc) = 1.49	UBe13	Be13U1	Be	13	U	1																				1	1995																																														K		2.06					2.06																																																								J/mol.K2	1.31																																							arc-melting					Effects of boron substitution on the superconducting state of UBe13			Los Alamos National Laboratory,	Phys.Rev.B, 51(1995)404	W.P.Beyermann,R.H.Heffner,J.L.Smith,M.F.Hundley,P.C.Canfield,J.D.Thompson		
40473	PR0510404	(dC/gamma*Tc) = 2.12	U(Be,B)13	U1Be12.9896B0.0104	U	1	Be	12.9896	B	0.0104																		1	1995																																														K		1.89					1.89																																																								J/mol.K2	1.28																																							arc-melting					Effects of boron substitution on the superconducting state of UBe13			Los Alamos National Laboratory,	Phys.Rev.B, 51(1995)404	W.P.Beyermann,R.H.Heffner,J.L.Smith,M.F.Hundley,P.C.Canfield,J.D.Thompson		
40474	PR0510404	(dC/gamma*Tc) = 3.78	U(Be,B)13	U1Be12.9701B0.0299	U	1	Be	12.9701	B	0.0299																		1	1995																																														K		1.66					1.66																																																								J/mol.K2	1.34																																							arc-melting					Effects of boron substitution on the superconducting state of UBe13			Los Alamos National Laboratory,	Phys.Rev.B, 51(1995)404	W.P.Beyermann,R.H.Heffner,J.L.Smith,M.F.Hundley,P.C.Canfield,J.D.Thompson		
40475	PR0510404	(dC/gamma*Tc) = 2.63	U(Be,B)13	U1Be12.9558B0.0442	U	1	Be	12.9558	B	0.0442																		1	1995																																														K		0.988					0.988																																																								J/mol.K2	1.98																																							arc-melting					Effects of boron substitution on the superconducting state of UBe13			Los Alamos National Laboratory,	Phys.Rev.B, 51(1995)404	W.P.Beyermann,R.H.Heffner,J.L.Smith,M.F.Hundley,P.C.Canfield,J.D.Thompson		
40476	J075013706	as-cast. non-stoichiometric effect.	CePt3Si	Ce1Pt3.03Si0.97	Ce	1	Pt	3.03	Si	0.97																			2006																												CePt3B																		K				0.37			0.37																																																																																																arc-melting					Magnetism and Superconductivity of CePt3Si and Ce1+xPt3+ySi1+z			Graduate School of Material Science, University of Hyogo, Kamigori-cho, Ako-gun, Hyogo 678-1297	J.Phys.Soc.Jpn, 75(2006)013706	G.Motoyama,S.Yamamoto,H.Takezoe,Y.Oda,K.Ueda,T.Kohara		
40477	J075013706	as-annealed(950C,1w). non-stoichiometric effect.	CePt3Si	Ce1Pt2.97Si1	Ce	1	Pt	2.97	Si	1																			2006																												CePt3B																		K				0.72			0.72																																																																																																arc-melting					Magnetism and Superconductivity of CePt3Si and Ce1+xPt3+ySi1+z			Graduate School of Material Science, University of Hyogo, Kamigori-cho, Ako-gun, Hyogo 678-1297	J.Phys.Soc.Jpn, 75(2006)013706	G.Motoyama,S.Yamamoto,H.Takezoe,Y.Oda,K.Ueda,T.Kohara		
40478	J075013706	as-annealed(950C,1w). non-stoichiometric effect.	CePt3Si	Ce1.01Pt3Si1	Ce	1.01	Pt	3	Si	1																			2006																												CePt3B																		K				0.75			0.75																																																																																																arc-melting					Magnetism and Superconductivity of CePt3Si and Ce1+xPt3+ySi1+z			Graduate School of Material Science, University of Hyogo, Kamigori-cho, Ako-gun, Hyogo 678-1297	J.Phys.Soc.Jpn, 75(2006)013706	G.Motoyama,S.Yamamoto,H.Takezoe,Y.Oda,K.Ueda,T.Kohara		
40479	MMM2580067	G-L = 10.	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																		3	2003																												skutterudite																		K		4.1					4.1																				T														MHC40479		A		140			A		1400																																										m3/C	0.00000000015										Sn-flux method					Anomalous transport properties in the filled skutterudites			Department of Physics, Tokyo Metropolitan University, Hachioji-shi, Tokyo,Japan	J.Mag.Mag.Mater., 258-259(2003)67	H.Sato,Y.Abe,T.D.Matsuda,K.Abe,N.Namiki,H.Sugawara,Y.Aoki		
40480	JP01201339	P-induced SC. some R-drop observed at P=0. Tc and Hc2 data for P=23 kbar.	CeNi2Ge2	Ce1Ni2Ge2	Ce	1	Ni	2	Ge	2																		3	2000																																														K		0.23	0.32		0		0.23	MTC40480																												T/K		5			MHC40480																																																														Czochralski method					Superconductivity, upper critical field and normal state resistivity in CeNi2Ge2 under pressure				J.Phys.:Condens.Matter, 12(2000)1339	D.Braithwaite,T.Fukuhara,A.Demuer,I.Sheikin,S.Kambe,J.-P.Brison,K.Maezawa,T.Naka,J.Flouqet		
40481	JP012L0533	P-induced SC. Tc(max) = 0.39 K at P = 2.72 GPa.	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																			2000																																														K		0.39			0.12		0.39	MTC40481																																																																																																				Anomalous low temperature states in CeNi2Ge2 and CePd2Si2			Cavendish Laboratory, Cambridge,UK	J.Phys.:Condens.Matter, 12(2000)L533	F.M.Grosche,P.Agarwal,S.R.Julian,N.J.Wilson,R.K.W.Haselwimmer,S.J.S.Lister,N.D.Mathur,F.V.Carter,S.S.Saxena,C.G.Lonzarich		
40482	JP012L0533	Tc(max) = 0.34K at P=1.95GPa.	CeNi2Ge2	Ce1Ni2Ge2	Ce	1	Ni	2	Ge	2																			2000																																														K		0.2					0.2	MTC40482																																																																																																				Anomalous low temperature states in CeNi2Ge2 and CePd2Si2			Cavendish Laboratory, Cambridge,UK	J.Phys.:Condens.Matter, 12(2000)L533	F.M.Grosche,P.Agarwal,S.R.Julian,N.J.Wilson,R.K.W.Haselwimmer,S.J.S.Lister,N.D.Mathur,F.V.Carter,S.S.Saxena,C.G.Lonzarich		
40483	J075043703	no inversion symmetry. P-induced SC. Pcrit = 1.8 GPa. Curie-T = -109K for H//[100] and =-186K for H//[001] (TBL value). SC properties are for P=2.5 GPa. RRR=98.	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2006							-186	5																			2	BaNiSn3	I4mm		A	4.252		9.715												K		1.6			0		1.6	MTC40483																			T		11.1							T/K		11.4			MHC40483		A	Hc2(0)	54																		mJ/mol.K2	120														uOhm.cm							1.4																		crystals grown using tetra-arc furnace, wrapped in Ta-foil, ANN(950C,5d, in sealed quartz tube.					Pressure-Induced Heavy-Fermion Superconductivity in Antiferromagnet CeIrSi3 without Inversion Symmetry			1Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 75(2006)043703	I.Sugitani,Y.Okuda,H.Shishido,T.Yamada,A.Thamizhavel,E.Yamamoto,T.D.Matsuda,Y.Haga,T.Takeuchi,R.Settai,Y.Onuki		
40484	J075043713	5-fold structure. compositions, Ca:Al:Si=100:97:98	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2006																											2	AlB2	P3		A	4.2169		22.0643												K			8.2																																																																																																				floating zone method					Two Types of Multistack Structures in MgB2-Type Superconductor CaAlSi			Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 75(2006)043713	H.Sagayama,Y.Wakabayashi,H.Sawa,T.Kamiyama,A.Hoshikawa,S.Harjo,K.Uozato,A.Ghosh,M.Tokunaga,T.Tamegai		
40485	J075043713	6-fold structure. compositions, Ca:Al:Si=100:100:96	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2006																											2	AlB2	P6<3>		A	4.1842		26.3898												K			6																																																																																																				floating zone method					Two Types of Multistack Structures in MgB2-Type Superconductor CaAlSi			Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 75(2006)043713	H.Sagayama,Y.Wakabayashi,H.Sawa,T.Kamiyama,A.Hoshikawa,S.Harjo,K.Uozato,A.Ghosh,M.Tokunaga,T.Tamegai		
40486	J075044713	P-induced SC. SC properties are at P=6.8 GPa. Hc2(0) is estimated using WHH from [dHc2/dT]. measuring Hc2(0)= 1.55 T. Tc defined as Tc(mid). Pc(AF)=7GPa. Pc(SC)=1.7 GPa. Kondo-T = 4.5K. RRR=50	CeNiGe3	Ce1Ni1Ge3	Ce	1	Ni	1	Ge	3																		1	2006								5.5																				SmNiGe3			A	21.808	4.135	4.168												K		0.43			0		0.43	MTC40486																			T	from dHc2/dT	3.2							T/K		10.8			MHC40486		A	from Hc2(0)	106																																																										See J.Phys:Condens.Matter,16(2004)L255					Pressure-Induced Superconductivity Emerging from Antiferromagnetic Phase in CeNiGe3			Graduate School of Natural Science and Technology, Okayama University, Tsushimanaka, Okayama 700-8530	J.Phys.Soc.Jpn, 75(2006)044713	H.Kotegawa,K.Takeda,T.Miyoshi,S.Fukushima,H.Hidaka,T.C.Kobayashi,T.Akazawa,Y.Ohishi,M.Nakashima,A.Thamizhavel,R.Settai,Y.Onuki		
40487	J075045002	beta pyrochlore. SC properties affect by water(moisture). Hc2 by rf-impedance. Anomalous phase transition at 7.5K. G-L = 80.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		3	2006																												pyrochlore	Fd[-]3m																	K	9.6						9.6																				T	rf-impedance	30.6												HC40487		A	from Hc2(0)	33			A	muon-SR	2700																												uOhm.cm							5																		See J.Phys:Condens.Matter,16(2004)L9					Upper Critical Field of beta-Pyrochlore KOs2O6 Single Crystals			Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 75(2006)045002	E.Ohmichi,T.Osada,S.Yonezawa,Y.Muraoka,Z.Hiroi		
40488	P073094509	not SC	Yb2.75C60	C60Yb2.75	C	60	Yb	2.75																					2006																												fullerene																		K					2																																																																																																C60,Yb(Sm)	1	mixture - pelletize - heat(923K,24-72h)					Superconducting phase sequence in RxC60 fullerides (R=Sm and Yb)			Department of Physics, Graduate School of Science, Tohoku University and CREST-JST, 6-3 Aoba Aramaki Aoba-ku, Sendai, Miyagi 980-8578, Japan	Phys.Rev.B, 73(2006)094509	M.Akada,T.Hirai,J.Takeuchi,T.Yamamoto,R.Kumashiro,K.Tanigaki		
40489	P073094509	sample with x=3.5 in YbxC60 has maximum SC fraction.	Yb3.5C60	C60Yb3.5	C	60	Yb	3.5																					2006																												fullerene																		K				6			6																																																																																														C60,Yb(Sm)	1	mixture - pelletize - heat(923K,24-72h)					Superconducting phase sequence in RxC60 fullerides (R=Sm and Yb)			Department of Physics, Graduate School of Science, Tohoku University and CREST-JST, 6-3 Aoba Aramaki Aoba-ku, Sendai, Miyagi 980-8578, Japan	Phys.Rev.B, 73(2006)094509	M.Akada,T.Hirai,J.Takeuchi,T.Yamamoto,R.Kumashiro,K.Tanigaki		
40490	P073094509	SmxC60 is not SC for 1=<x=<6.	Sm3C60	C60Sm3	C	60	Sm	3																					2006																												fullerene																		K					2																																																																																																C60,Yb(Sm)	1	mixture - pelletize - heat(923K,24-72h)					Superconducting phase sequence in RxC60 fullerides (R=Sm and Yb)			Department of Physics, Graduate School of Science, Tohoku University and CREST-JST, 6-3 Aoba Aramaki Aoba-ku, Sendai, Miyagi 980-8578, Japan	Phys.Rev.B, 73(2006)094509	M.Akada,T.Hirai,J.Takeuchi,T.Yamamoto,R.Kumashiro,K.Tanigaki		
40491	P073094510	special care kaken for getting ZrB2-needle free sample from ZrB12 single crystals.	ZrB12	B12Zr1	B	12	Zr	1																				3	2006																												UB12	Fm3m		A	7.4072														K	6						6											A	LC measurement	41							T	resistive and linear extraporation	0.162														A	from Hc2(0)	450			A	calculation from Hc1	2800																																																					floating zone method					Two-gap superconductivity in ZrB12: Temperature dependence of critical magnetic fields in single crystals			Institute of Solid State Physics RAS, 142432 Chernogolovka, Moscow District, Russia	Phys.Rev.B, 73(2006)094510	V.A.Gasparov,N.S.Sidorov,I.I.Zver'kova		
40492	JTL0800330	Debye-T from SP-heat is 800-1200 K(Junod et al)	ZrB12	B12Zr1	B	12	Zr	1																				3	2004									3.6																			UB12			A	7.4072														K	5.97					0.04	5.97																																																											300	from R(T)																																				(ZrB2+B) - zone induction melting					On electron transport in ZrB12, ZrB2, and MgB2 in norml state				JETP.Lett., 80(2004)330	V.A.Gasparov,M.P.Kulalov,N.S.Sidorov,I.J.Zrer'kova,V.B.Filipov,A.B.Lyashenko,Yu.B.Paderno		
40493	P073094518	beta-pyrochlore. G-L = 66.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		3	2006																												pyrochlore			A	10.0968														K		9.5					9.5											Oe		116							T		24							T/K		3.6					A		37			A		2430					4.57								mJ/mol.K2	76																																					Os,K(Rb)O2		mixed in Ar filled dry box - pellet - quartz tube - ADD(ag2O) - heat(600C,1h) - cool to 400C(5C/h) - cool to RT(150C/h)					Mass enhancement, correlations, and strong-coupling superconductivity in the beta-pyrochlore KOs2O6			Laboratory for Solid State Physics, ETH Zurich, 8093 Zurich, Switzerland	Phys.Rev.B, 73(2006)094518	M.Bruhwiler,S.M.Kazakov,J.Karpinski,B.Batlogg		
40494	P073094518	beta-pyrochlore. G-L = 34.	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		3	2006																												pyrochlore																		K		6.4					6.4											Oe		92							T		6							T/K		1.2					A		74			A		2520					3.87								mJ/mol.K2	44																																					Os,K(Rb)O2		mixed in Ar filled dry box - pellet - quartz tube - ADD(ag2O) - heat(600C,1h) - cool to 400C(5C/h) - cool to RT(150C/h)					Mass enhancement, correlations, and strong-coupling superconductivity in the beta-pyrochlore KOs2O6			Laboratory for Solid State Physics, ETH Zurich, 8093 Zurich, Switzerland	Phys.Rev.B, 73(2006)094518	M.Bruhwiler,S.M.Kazakov,J.Karpinski,B.Batlogg		
40495	P073094522	P-induced SC. hydrostatic pressure using DAC. Tc increases with P upto 90 GPa (Tc=17K).	Y	Y1	Y	1																							2006																																														K		17			0		17	MTC40495																																																																																																				Superconductivity at 17 K in yttrium metal under nearly hydrostatic pressures up to 89 GPa			Department of Physics, Washington University, CB 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.B, 73(2006)094522	J.J.Hamlin,V.G.Tissen,J.S.Schilling		
40496	PRL0190892	alpha-U. isotope effect measured at P = 11 kbar (Tc=2.17K)	alpha-U	U1	U	1																							1967																																														K		0.2					0.2						2.2	U																																																																																									arc-melting. ANN(640C,100h, P=2E-9 Torr)					Positive isotope effect on the superconducting transition temperature of alpha-uranium			University of California,Los Alamos,USA	Phys.Rev.Lett., 19(1967)892	R.D.Fowler,J.D.G.Lindsay,R.W.White,H.H.Hill,B.T.Matthias		
40497	PRL0401104	Mo6Se8 leads to MoSe2 contamination. Tc defined as midpoint of mutual inductance.	Mo6Se8	Mo6Se7.6	Mo	6	Se	7.6																					1978																												Chevrel			A	9.56		11.17												K		6.28					6.28						0.27	Mo																																																																																									heat from 400 to 1200(2.4C/min), the react (1200C,13h), Q to RT.					Isotope effect of the superconducting transition temperature in binary Chevrel-phase Mo6Se8				Phys.Rev.Lett., 40(1978)1104	F.J.Culetto,F.Pobell		
40498	PRL0401104	Mo6Se8 leads to MoSe2 contamination. Tc defined as midpoint of mutual inductance.	Mo6Se8	Mo6Se7.6	Mo	6	Se	7.6																					1978																												Chevrel			A	9.56		11.17												K		6.28					6.28						0.27	Se																																																																																									heat from 400 to 1200(2.4C/min), the react (1200C,13h), Q to RT.					Isotope effect of the superconducting transition temperature in binary Chevrel-phase Mo6Se8				Phys.Rev.Lett., 40(1978)1104	F.J.Culetto,F.Pobell		
40499	PRL0371410		HfV2	Hf1V2	Hf	1	V	2																					1976																												MgCu2(Laves)			A	7.3702													MgCu2(Laves), C15	K		9.67					9.67																													T/K		4.3			MHC40499																																																														induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40600	PRL0371410		HfV2H0.5	Hf1V2H0.5	Hf	1	V	2	H	0.5																			1976																												MgCu2(Laves)			A	7.4132													MgCu2(Laves), C15	K		7.33					7.33						0.5	H																											MHC40499																																																														induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40601	PRL0371410		HfV2D0.5	Hf1V2D0.5	Hf	1	V	2	D	0.5																			1976																												MgCu2(Laves)			A	7.4265													MgCu2(Laves), C15	K		5.93					5.93																																		MHC40499																																																														induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40602	PRL0371410		HfV2Hx	Hf1V2H0.4	Hf	1	V	2	H	0.4																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		8.42					8.42																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40603	PRL0371410		HfV2Hx	Hf1V2H1	Hf	1	V	2	H	1																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		4.87					4.87																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40604	PRL0371410		HfV2Hx	Hf1V2H1.6	Hf	1	V	2	H	1.6																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		2.2					2.2																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40605	PRL0371410		HfV2Dx	Hf1V2D0.25	Hf	1	V	2	D	0.25																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		8.24					8.24																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40606	PRL0371410		HfV2Dx	Hf1V2D0.75	Hf	1	V	2	D	0.75																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		4.29					4.29																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40607	PRL0371410		HfV2Dx	Hf1V2D1	Hf	1	V	2	D	1																			1976																												MgCu2(Laves)																	MgCu2(Laves), C15	K		3.41					3.41																																																																																																induction melting , ANN(800C,100h). H(D) introduced at RT, 500psi.					Pronounced isotope effect in the superconductivity of HfV2			University of Pittsburgh,USA	Phys.Rev.Lett., 37(1976)1410	P.Duffer,D.M.Gualtieri,V.U.S.Rao		
40608	PRL0340144	inverse isotope effect. Tc(PdH) < Tc(PdD).	PdH0.9	H0.9Pd1	H	0.9	Pd	1																					1975																																														K		4.11					4.11	MTC40608																																																																																															samples made by electrolytic charging method at T = -78C.					Electronic model for the reverse isotope effect in superconducting Pd-H(D)			University of Illinois,USA	Phys.Rev.Lett., 34(1975)144	R.J.Miller,C.B.Satterthwaite		
40609	PRL0340144	inverse isotope effect. Tc(PdH) < Tc(PdD).	PdD0.9	D0.9Pd1	D	0.9	Pd	1																					1975																																														K		6					6	MTC40608																																																																																															samples made by electrolytic charging method at T = -78C.					Electronic model for the reverse isotope effect in superconducting Pd-H(D)			University of Illinois,USA	Phys.Rev.Lett., 34(1975)144	R.J.Miller,C.B.Satterthwaite		
40610	PSS0310655		ZrV2	V2Zr1	V	2	Zr	1																					1975																												MgCu2(Laves)			A	7.439													MgCu2(Laves), C15	K		8.85					8.85																																																																																														Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40611	PSS0310655		Zr(V,Fe)2	Zr1V1.85Fe0.15	Zr	1	V	1.85	Fe	0.15																			1975																												MgCu2(Laves)			A	7.395													MgCu2(Laves), C15	K		6.41					6.41																																																																																														Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40612	PSS0310655	Hc2by resistive transition	Zr(V,Fe)2	Zr1V1.7Fe0.3	Zr	1	V	1.7	Fe	0.3																			1975																												MgCu2(Laves)			A	7.362													MgCu2(Laves), C15	K		4.49					4.49																																		MHC40612																																																												Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40613	PSS0310655	not SC	Zr(V,Fe)2	Zr1V0.8Fe1.2	Zr	1	V	0.8	Fe	1.2																			1975							62																					MgZn2(Laves)			A	5.075		8.289											MgZn2(Laves), C14	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40614	PSS0310655	not SC	Zr(V,Fe)2	Zr1V0.4Fe1.6	Zr	1	V	0.4	Fe	1.6																			1975							359																					MgZn2(Laves)			A	5.022		8.248											MgZn2(Laves), C14	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40615	PSS0310655	not SC	ZrFe2	Fe2Zr1	Fe	2	Zr	1																					1975							659																					MgCu2(Laves)			A	7.056													MgCu2(Laves), C15	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40616	PSS0310655		HfV2	Hf1V2	Hf	1	V	2																					1975																												MgCu2(Laves)			A	7.4													MgCu2(Laves), C15	K		9.34					9.34																																																																																														Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40617	PSS0310655		Hf(V,Fe)2	Hf1V1.85Fe0.15	Hf	1	V	1.85	Fe	0.15																			1975																												MgZn2(Laves)			A	5.208		8.484											MgZn2(Laves), C14	K		7.04					7.04																																																																																														Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40618	PSS0310655	Hc2by resistive transition	Hf(V,Fe)2	Hf1V1.7Fe0.3	Hf	1	V	1.7	Fe	0.3																			1975																												MgZn2(Laves)			A	5.178		8.434											MgZn2(Laves), C14	K		5					5																																		MHC40618																																																												Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40619	PSS0310655	not SC	Hf(V,Fe)2	Hf1V0.8Fe1.2	Hf	1	V	0.8	Fe	1.2																			1975							112																					MgZn2(Laves)			A	5.057		8.256											MgZn2(Laves), C14	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40620	PSS0310655	not SC	Hf(V,Fe)2	Hf1V0.4Fe1.6	Hf	1	V	0.4	Fe	1.6																			1975							336																					MgZn2(Laves)			A	5.018		8.191											MgZn2(Laves), C14	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40621	PSS0310655	not SC	HfFe2	Fe2Hf1	Fe	2	Hf	1																					1975							567																					MgCu2(Laves)			A	7.025													MgCu2(Laves), C15	K					4.2																																																																																																Zr(Hf),V,Fe		levitation melting. ANN(900C,3d)					Superconducting and magnetic properties of ZrN2-xFex and HfV2-xFex alloys			University of Pittsburgh,USA	phys.stat.sol.(a), 31(1975)655	P.Duffer,S.G.Sankar,V.U.S.Rao,R.L.Bergner,R.Obermyer		
40622	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	ZrV2	V2Zr1	V	2	Zr	1																					1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		8.54					8.54																				T	resistive	13.6			10.3			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40623	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	(Zr,Hf)V2	Zr0.87Hf0.13V2	Zr	0.87	Hf	0.13	V	2																			1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		9.45					9.45																				T	resistive	19.4			15.6			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40624	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	(Zr,Hf)V2	Zr0.7Hf0.3V2	Zr	0.7	Hf	0.3	V	2																			1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		9.9					9.9																				T	resistive	25.1			20.6			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40625	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	(Zr,Hf)V2	Zr0.5Hf0.5V2	Zr	0.5	Hf	0.5	V	2																			1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		10.1					10.1																				T	resistive	26.6			22			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40626	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	(Zr,Hf)V2	Zr0.3Hf0.7V2	Zr	0.3	Hf	0.7	V	2																			1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		9.96					9.96																				T	resistive	26.8			22			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40627	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	(Zr,Hf)V2	Zr0.13Hf0.87V2	Zr	0.13	Hf	0.87	V	2																			1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		9.76					9.76																				T	resistive	25.6			20.9			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40628	APL0180235	Hc2(0) estimated from Hc2(4.2) using parabolic T-dependence of Hc2(T)	HfV2	Hf1V2	Hf	1	V	2																					1971																												MgCu2(Laves)																	MgCu2(Laves), C15	K		9.26					9.26																				T	resistive	24.8			19.7			4.2																																																																				arc melted HfxZr1-x were put into V-tube. cold-rolled, heat(900-1200C), then Laves phase obtained.					A new high-field superconductor, V2HfxZr1-x			National Research Institute for Metals, Japan	Appl.Phys.Lett., 18(1971)235	K.Inoue,K.Tachikawa,Y.Iwasa		
40629	ZPB2680261	H-implantation layer thickness = 1500A. Tc shows optimal value for this system)	(Pd,Cu)Hx	Pd0.55Cu0.45H0.7	Pd	0.55	Cu	0.45	H	0.7																			1974																																														K		16.6					16.6																																																																																																Pd-noble metal(Cu,Ag,Au) alloys were made by arc-melting. H-implantation (130kV, at 4.2K)					High superconducting transition temperatures in the palladium-noble metal-hydrogen system				Z.Phys., 268(1974)261	B.Stritzker		
40630	ZPB2680261	H-implantation layer thickness = 1500A. Tc shows optimal value for this system)	(Pd,Ag)Hx	Pd0.7Ag0.3H0.8	Pd	0.7	Ag	0.3	H	0.8																			1974																																														K		15.6					15.6																																																																																																Pd-noble metal(Cu,Ag,Au) alloys were made by arc-melting. H-implantation (130kV, at 4.2K)					High superconducting transition temperatures in the palladium-noble metal-hydrogen system				Z.Phys., 268(1974)261	B.Stritzker		
40631	ZPB2680261	H-implantation layer thickness = 1500A. Tc shows optimal value for this system)	(Pd,Au)Hx	Pd0.84Au0.16H0.9	Pd	0.84	Au	0.16	H	0.9																			1974																																														K		13.6					13.6																																																																																																Pd-noble metal(Cu,Ag,Au) alloys were made by arc-melting. H-implantation (130kV, at 4.2K)					High superconducting transition temperatures in the palladium-noble metal-hydrogen system				Z.Phys., 268(1974)261	B.Stritzker		
40632	L096107008	highly oriented graphite. intercalated sample. gap by analyzing of PENET.	CaC6	C6Ca1	C	6	Ca	1																					2006																																														K		11.46				0.4	11.46																																				A	mutual inductance		350		A	magnetization		720		meV	1.79	3.6																																																react (pyrolytic graphite platelet, molten Li-Ca alloy, at 350C under Ar)					Experimental Evidence of s-Wave Superconductivity in Bulk CaC6			"CNR-INFM Coherentia and Department of Physics, University of Naples ""Federico II"" I-80125, Napoli, Italy"	Phys.Rev.Lett., 96(2006)107008	G.Lamura,M.Aurino,G.Cifariello,E.Di Gennaro,A.Andreone,N.Emery,C.Herold,J.-F.Mareche,P.Lagrange		
40633	L096147001	In<115> NQR measured. gap & Curie-T were obtained from NQR measurements.	Ce(Rh,Ir)In5	Ce1Rh0.4Ir0.6In5	Ce	1	Rh	0.4	Ir	0.6	In	5																3	2006																												HoCoGa5																		K		0.91					0.91																																																4.69																																																self-flux method					Enhancing the Superconducting Transition Temperature of CeRh1-xIrxIn5 due to the Strong-Coupling Effects of Antiferromagnetic Spin Fluctuations: An <115>In Nuclear Quadrupole Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)147001	S.Kawasaki,M.Yashima,Y.Mugino,H.Mukuda,Y.Kitaoka,H.Shishido,Y.Onuki		
40634	L096147001	In<115> NQR measured. gap & Curie-T were obtained from NQR measurements.	Ce(Rh,Ir)In5	Ce1Rh0.3Ir0.7In5	Ce	1	Rh	0.3	Ir	0.7	In	5																3	2006							0.2																					HoCoGa5																		K		1.2					1.2																																																8.28																																																self-flux method					Enhancing the Superconducting Transition Temperature of CeRh1-xIrxIn5 due to the Strong-Coupling Effects of Antiferromagnetic Spin Fluctuations: An <115>In Nuclear Quadrupole Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)147001	S.Kawasaki,M.Yashima,Y.Mugino,H.Mukuda,Y.Kitaoka,H.Shishido,Y.Onuki		
40635	L096147001	In<115> NQR measured. gap & Curie-T were obtained from NQR measurements.	Ce(Rh,Ir)In5	Ce1Rh0.2Ir0.8In5	Ce	1	Rh	0.2	Ir	0.8	In	5																3	2006							2.47																					HoCoGa5																		K		0.67					0.67																																																7.54																																																self-flux method					Enhancing the Superconducting Transition Temperature of CeRh1-xIrxIn5 due to the Strong-Coupling Effects of Antiferromagnetic Spin Fluctuations: An <115>In Nuclear Quadrupole Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)147001	S.Kawasaki,M.Yashima,Y.Mugino,H.Mukuda,Y.Kitaoka,H.Shishido,Y.Onuki		
40636	L096147001	In<115> NQR measured. gap & Curie-T were obtained from NQR measurements.	Ce(Rh,Ir)In5	Ce1Rh0.1Ir0.9In5	Ce	1	Rh	0.1	Ir	0.9	In	5																3	2006							4.59																					HoCoGa5																		K		0.35					0.35																																																4.69																																																self-flux method					Enhancing the Superconducting Transition Temperature of CeRh1-xIrxIn5 due to the Strong-Coupling Effects of Antiferromagnetic Spin Fluctuations: An <115>In Nuclear Quadrupole Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)147001	S.Kawasaki,M.Yashima,Y.Mugino,H.Mukuda,Y.Kitaoka,H.Shishido,Y.Onuki		
40637	L096147001	In<115> NQR measured. gap & Curie-T were obtained from NQR measurements.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2006							7.56																																							K		0.41					0.41																																																5.23																																																self-flux method					Enhancing the Superconducting Transition Temperature of CeRh1-xIrxIn5 due to the Strong-Coupling Effects of Antiferromagnetic Spin Fluctuations: An <115>In Nuclear Quadrupole Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)147001	S.Kawasaki,M.Yashima,Y.Mugino,H.Mukuda,Y.Kitaoka,H.Shishido,Y.Onuki		
40638	PHB2810005	non-stoichiometric SC	CeNi2Ge2	Ce1.005Ni2.02Ge1.98	Ce	1.005	Ni	2.02	Ge	1.98																		1	2000																																														K			0.03				0.03																																																																																																arc-melting. ANN(800C,120h)					Incipient superconductivity and NFL behavior in off-stoichiometric Ce1+xNi2+yGe2+z polycrystals			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Str. 48, D-01187 Dresden, Germany	Physica B, 281&282(2000)5	P.Gegenwart,P.Hinze,C.Geibel,M.Lang,F.Steglich		
40639	PHB2810005	non-stoichiometric SC	CeNi2Ge2	Ce1.005Ni2.025Ge1.975	Ce	1.005	Ni	2.025	Ge	1.975																		1	2000																																														K	0.01		0.06				0.035	LAT40639																																																																																															arc-melting. ANN(800C,120h)					Incipient superconductivity and NFL behavior in off-stoichiometric Ce1+xNi2+yGe2+z polycrystals			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Str. 48, D-01187 Dresden, Germany	Physica B, 281&282(2000)5	P.Gegenwart,P.Hinze,C.Geibel,M.Lang,F.Steglich		
40640	L096157001	weak static AF order(Cu-moment). spin excitations were studied by inelastic ND.	(Pr,Ce,La)2CuO4	Pr0.88Ce0.12La1Cu1O4-z	Pr	0.88	Ce	0.12	La	1	Cu	1													O	4-z		3	2006								40																				T'																		K				21			21																																																																																																mirrow image furnace. ANN(765C,4h, P < 1.0E-6 mbar)					High-Energy Spin Excitations in the Electron-Doped Superconductor Pr0.88LaCe0.12CuO4-z with Tc = 21 K			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.Lett., 96(2006)157001	S.D.Wilson,S.Li,H.Woo,P.Dai,H.A.Mook,C.D.Frost,S.Komiya,Y.Ando		
40641	P068054507	anisotropy (Rc/Rab) = 3.1 at RT. anisotropy factor(from Hc2) increases with increasing T: 2.0 (t=0.5) to 3.0 (t=0.9).	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2003																												AlB2																		K				6		0.2	6																				T	WHH approx.		1.68	0.86					T/K	magnetization		0.405	0.208	MHC40641		A	from Hc2		196	100																																																													Angular dependence of the upper critical field in CaAlSi single crystal: Deviation from the Ginzburg-Landau anisotropic mass model			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 68(2003)054507	A.K.Ghosh,M.Tokunaga,T.Tamegai		
40642	PHC4390043	anisotropy = 4 from coherence length. specific data has no(or bad) unit. structure data (rhombohedral, a=5.17 A, alpha=49.55) from J.Solid State Chem, 178(2005)2847.	CaC6	C6Ca1	C	6	Ca	1																					2006																															A	5.17														K				11.3		1	11.3																													T/K			0.1	0.025	MHC40642		A			360	90																																																								intercalation process. See Nature Phys. 1(2005)39					Anisotropic superconducting phase diagram of C6Ca			Materials Science Division, Argonne National Laboratory, Argonne, IL 60439, United States	Physica C, 439(2006)43	R.Xie,D.Rosenmann,A.Rydh,H.Claus,G.Karapetrov,W.K.Kwok,U.Welp		
40643	PHC4400006		MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2006																															A	3.8159														K				6.5			6.5																																																																																														Mg,Zn,C,Ni-powder		nominal (Mg1-x)1.5ZnxCNi3. pellet - SIN(900C)					Chemical pressure effect on the superconductor MgCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan	Physica C, 440(2006)6	M.Uehara,T.Amano,S.Takano,T.Kori,T.Yamazaki,Y.Kimishima		
40644	PHC4400006		(Mg,Zn)CNi3	Mg0.9Zn0.1C1Ni3	Mg	0.9	Zn	0.1	C	1	Ni	3																	2006																															A	3.8035														K				4.5			4.5																																																																																														Mg,Zn,C,Ni-powder		nominal (Mg1-x)1.5ZnxCNi3. pellet - SIN(900C)					Chemical pressure effect on the superconductor MgCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan	Physica C, 440(2006)6	M.Uehara,T.Amano,S.Takano,T.Kori,T.Yamazaki,Y.Kimishima		
40645	PHC4400006		(Mg,Zn)CNi3	Mg0.8Zn0.2C1Ni3	Mg	0.8	Zn	0.2	C	1	Ni	3																	2006																															A	3.7959														K				2.82			2.82																																																																																														Mg,Zn,C,Ni-powder		nominal (Mg1-x)1.5ZnxCNi3. pellet - SIN(900C)					Chemical pressure effect on the superconductor MgCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan	Physica C, 440(2006)6	M.Uehara,T.Amano,S.Takano,T.Kori,T.Yamazaki,Y.Kimishima		
40646	PHC4400006		(Mg,Zn)CNi3	Mg0.7Zn0.3C1Ni3	Mg	0.7	Zn	0.3	C	1	Ni	3																	2006																															A	3.7718														K				2.5			2.5																																																																																														Mg,Zn,C,Ni-powder		nominal (Mg1-x)1.5ZnxCNi3. pellet - SIN(900C)					Chemical pressure effect on the superconductor MgCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan	Physica C, 440(2006)6	M.Uehara,T.Amano,S.Takano,T.Kori,T.Yamazaki,Y.Kimishima		
40647	PHC4400006	Mg1-xCdxCNi3 were prepared at 900C, P=3.5 GPa. single phase not obtained.	CdCNi3	Cd1C1Ni3	Cd	1	C	1	Ni	3																			2006																															A	3.8425														K				3.4			3.4																																																																																																synthesized (900C,P=3.5 GPa)					Chemical pressure effect on the superconductor MgCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, 79-5 Tokiwadai, Hodogaya-ku, Yokohama 240-8501, Japan	Physica C, 440(2006)6	M.Uehara,T.Amano,S.Takano,T.Kori,T.Yamazaki,Y.Kimishima		
40648	P073144509	Tc and Tn measured by muon-SR. Clear evidence for coexistence of AC and AF.	YBa2Cu3Oz	Y1Ba2Cu3O6.375	Y	1	Ba	2	Cu	3															O	7-z	6.375	3	2006								9.45																				Y123																		K				19			19	TC40648																																																																																																				Coexistence of magnetism and superconductivity in ultraclean underdoped YBa2Cu3O6.37			Department of Physics & Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia, Canada	Phys.Rev.B, 73(2006)144509	R.I.Miller,R.F.Kiefl,J.H.Brewer,F.D.Callaghan,J.E.Sonier,R.Liang,D.A.Bonn,W.Hardy		
40649	P073144510	c-axis resistivity and its angle dependence were measured. Anisotropy = 2.6	(Y,Pr)Ba2Cu3Oz	Y0.54Pr0.46Ba2Cu3O7-z	Y	0.54	Pr	0.46	Ba	2	Cu	3													O	7-z		3	2006																												Y123																		K	38						38																																																																																																					High temperature mixed state c-axis dissipation in low carrier density Y0.54Pr0.46Ba2Cu3O7-z			Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 73(2006)144510	T.Katuwal,V.Sandu,C.C.Almasan,B,J,Taylor,M.B.Maple		
40650	P073144518		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2006																												T			A	3.7743		13.2242												K			37.4				37.4																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40651	P073144518		(La,Sr)2(Cu,Ti)O4	La1.85Sr0.15Cu0.98Ti0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ti	0.02													O	4		1	2006																												T			A	3.781		13.2077												K			32.3				32.3																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40652	P073144518		(La,Sr)2(Cu,Ti)O4	La1.85Sr0.15Cu0.96Ti0.04O4	La	1.85	Sr	0.15	Cu	0.96	Ti	0.04													O	4		1	2006																												T			A	3.7873		13.1849												K			26.1				26.1																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40653	P073144518	not SC	(La,Sr)2(Cu,Ti)O4	La1.85Sr0.15Cu0.94Ti0.06O4	La	1.85	Sr	0.15	Cu	0.94	Ti	0.06													O	4		1	2006																												T			A	3.7956		13.1648												K					5																																																																																																La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40654	P073144518		(La,Sr)2(Cu,Ti)O4	La1.81Sr0.19Cu0.98Ti0.02O4	La	1.81	Sr	0.19	Cu	0.98	Ti	0.02													O	4		1	2006																												T			A	3.7743		13.218												K			33				33																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40655	P073144518		(La,Sr)2(Cu,Ti)O4	La1.77Sr0.23Cu0.96Ti0.04O4	La	1.77	Sr	0.23	Cu	0.96	Ti	0.04													O	4		1	2006																												T			A	3.7765		13.2135												K			32.8				32.8																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40656	P073144518		(La,Sr)2(Cu,Ti)O4	La1.73Sr0.27Cu0.94Ti0.06O4	La	1.73	Sr	0.27	Cu	0.94	Ti	0.06													O	4		1	2006																												T			A	3.7785		13.2096												K			30				30																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40657	P073144518		(La,Sr)2(Cu,Ti)O4	La1.69Sr0.31Cu0.92Ti0.08O4	La	1.69	Sr	0.31	Cu	0.92	Ti	0.08													O	4		1	2006																												T			A	3.7805		13.2006												K			30				30																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40658	P073144518		(La,Sr)2(Cu,Ti)O4	La1.65Sr0.35Cu0.9Ti0.1O4	La	1.65	Sr	0.35	Cu	0.9	Ti	0.1													O	4		1	2006																												T			A	3.7834		13.1983												K			29.9				29.9																																																																																														La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40659	P073144518	not SC.	(La,Sr)2(Cu,Ti)O4	La1.63Sr0.37Cu0.89Ti0.11O4	La	1.63	Sr	0.37	Cu	0.89	Ti	0.11													O	4		1	2006																												T			A															K					5																																																																																																La2O3,SrCO3,TiO2,CuO		SIN(1120-1230C, 24h, in air)					Suppression of superconductivity by the localization of hole carriers in Ti-doped La1.85Sr0.15CuO4			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)144518	Caixia Wang,Yuping Sun,Zhe Qu,Yuheng Zhang		
40660	P073174515		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	2006																												T			A	3.7721		13.2004												K				37			37																																																																																														La2O3,SrCO3,RuO2,CuO		mixture - heat(900C,24h,in Al2O3) - pellet - heat(1000C,24h) - SIN(1100C,24h,in air)					Superconductivity and anomalous magnetic properties of the double-doping La1.85-2xSr0.15+2xCu1-xRuxO4 (0=<x=<0.3) compounds			Hefei High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 73(2006)174515	Jing Xie,Jiyu Fan,Shun Tan,Yuheng Zhang		
40661	P073174515		(La,Sr)2(Cu,Ru)O4	La1.83Sr0.17Cu0.99Ru0.01O4	La	1.83	Sr	0.17	Cu	0.99	Ru	0.01													O	4		1	2006																												T			A	3.7715		13.2017												K				30			30																																																																																														La2O3,SrCO3,RuO2,CuO		mixture - heat(900C,24h,in Al2O3) - pellet - heat(1000C,24h) - SIN(1100C,24h,in air)					Superconductivity and anomalous magnetic properties of the double-doping La1.85-2xSr0.15+2xCu1-xRuxO4 (0=<x=<0.3) compounds			Hefei High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 73(2006)174515	Jing Xie,Jiyu Fan,Shun Tan,Yuheng Zhang		
40662	P073174515	no resistance drop at Tc.	(La,Sr)2(Cu,Ru)O4	La1.81Sr0.19Cu0.98Ru0.02O4	La	1.81	Sr	0.19	Cu	0.98	Ru	0.02													O	4		1	2006																												T			A															K				30			30																																																																																														La2O3,SrCO3,RuO2,CuO		mixture - heat(900C,24h,in Al2O3) - pellet - heat(1000C,24h) - SIN(1100C,24h,in air)					Superconductivity and anomalous magnetic properties of the double-doping La1.85-2xSr0.15+2xCu1-xRuxO4 (0=<x=<0.3) compounds			Hefei High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 73(2006)174515	Jing Xie,Jiyu Fan,Shun Tan,Yuheng Zhang		
40663	P073174515	no resistance drop at Tc. R is semiconductor-like	(La,Sr)2(Cu,Ru)O4	La1.79Sr0.21Cu0.97Ru0.03O4	La	1.79	Sr	0.21	Cu	0.97	Ru	0.03													O	4		1	2006																												T			A	3.7751		13.1945												K				24			24																																																																																														La2O3,SrCO3,RuO2,CuO		mixture - heat(900C,24h,in Al2O3) - pellet - heat(1000C,24h) - SIN(1100C,24h,in air)					Superconductivity and anomalous magnetic properties of the double-doping La1.85-2xSr0.15+2xCu1-xRuxO4 (0=<x=<0.3) compounds			Hefei High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 73(2006)174515	Jing Xie,Jiyu Fan,Shun Tan,Yuheng Zhang		
40664	P073174515	no resistance drop at Tc. R is semiconductor-like. spin glass temp.= 24.0K	(La,Sr)2(Cu,Ru)O4	La1.77Sr0.23Cu0.96Ru0.04O4	La	1.77	Sr	0.23	Cu	0.96	Ru	0.04													O	4		1	2006																												T			A	3.7759		13.1859												K					5																																																																																																La2O3,SrCO3,RuO2,CuO		mixture - heat(900C,24h,in Al2O3) - pellet - heat(1000C,24h) - SIN(1100C,24h,in air)					Superconductivity and anomalous magnetic properties of the double-doping La1.85-2xSr0.15+2xCu1-xRuxO4 (0=<x=<0.3) compounds			Hefei High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 73(2006)174515	Jing Xie,Jiyu Fan,Shun Tan,Yuheng Zhang		
40665	P073184509	carrier estimated from s(290K). in-plane resistivity, MR, Hall effect were measured.	(Y,Ca)Ba2Cu3Oz	Y0.95Ca0.05Ba2Cu3Oz	Y	0.95	Ca	0.05	Ba	2	Cu	3													O	z		5	2006																												Y123																		K		84.8				0.5	84.8																																																																		uV/K	5.6																								RH40665	hole/Cu	0.136			Films were grown on SrTiO3(100) substrates using pulsed laser deposition.					Effect of Zn substitution on the normal-state magnetoresistivity of epitaxial Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy and Y0.9Ca0.1Ba2Cu3Oy films			IRC in Superconductivity and Department of Physics, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B, 73(2006)184509	I.Kokanovic,J.R.Cooper,S.H.Naqib,R.S.Islam,R.A.Chakalov		
40666	P073184509	carrier estimated from s(290K). in-plane resistivity, MR, Hall effect were measured.	(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.95Ca0.05Ba2Cu2.94Zn0.06Oz	Y	0.95	Ca	0.05	Ba	2	Cu	2.94	Zn	0.06											O	z		5	2006																												Y123																		K		66				1.5	66																																																																		uV/K	2.4																								RH40666	hole/Cu	0.157			Films were grown on SrTiO3(100) substrates using pulsed laser deposition.					Effect of Zn substitution on the normal-state magnetoresistivity of epitaxial Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy and Y0.9Ca0.1Ba2Cu3Oy films			IRC in Superconductivity and Department of Physics, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B, 73(2006)184509	I.Kokanovic,J.R.Cooper,S.H.Naqib,R.S.Islam,R.A.Chakalov		
40667	P073184509	carrier estimated from s(290K). in-plane resistivity, MR, Hall effect were measured.	(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.95Ca0.05Ba2Cu2.88Zn0.12Oz	Y	0.95	Ca	0.05	Ba	2	Cu	2.88	Zn	0.12											O	z		5	2006																												Y123																		K		33.9				1.1	33.9																																																																		uV/K	5.4																								RH40667	hole/Cu	0.137			Films were grown on SrTiO3(100) substrates using pulsed laser deposition.					Effect of Zn substitution on the normal-state magnetoresistivity of epitaxial Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy and Y0.9Ca0.1Ba2Cu3Oy films			IRC in Superconductivity and Department of Physics, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B, 73(2006)184509	I.Kokanovic,J.R.Cooper,S.H.Naqib,R.S.Islam,R.A.Chakalov		
40668	P073184509	carrier estimated from s(290K). in-plane resistivity, MR, Hall effect were measured.	(Y,Ca)Ba2Cu3Oz	Y0.9Ca0.1Ba2Cu3Oz	Y	0.9	Ca	0.1	Ba	2	Cu	3													O	z		5	2006																												Y123																		K		79.5				0.7	79.5																																																																		uV/K	-5.3																								RH40668	hole/Cu	0.212			Films were grown on SrTiO3(100) substrates using pulsed laser deposition.					Effect of Zn substitution on the normal-state magnetoresistivity of epitaxial Y0.95Ca0.05Ba2(Cu1-xZnx)3Oy and Y0.9Ca0.1Ba2Cu3Oy films			IRC in Superconductivity and Department of Physics, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.B, 73(2006)184509	I.Kokanovic,J.R.Cooper,S.H.Naqib,R.S.Islam,R.A.Chakalov		
40669	P073184521	energy gap from Andreev reflection of PtIr/LiTi2O4 point contact. aged sample may have some off-stoichiometric phases.	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		1	2006																												spinel			A	8.4														K		12.3	12.5			0.3	12.3																				T		11.6												HC40669												meV	1.9	4																																														Li2Ti3O7,TiO		mixture - CAL(805C,50h, in evacuated quartz tube) - react(2Li2Ti3O7 + 2TiO = 4LiTi2O4) - slow cool					Electrical resistivity and Andreev reflection spectroscopy of the superconducting oxide spinel LiTi2O4			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 73(2006)184521	L.Tang,P.Y.Zou,L.Shan,A.F.Dong,G.C.Che,H.H.Wen		
40670	P073184523	5-fold structure. PENET from frequency shift analysis of LC-tunnel diode for H//ab and H//c fields. GAPENE(c-plane) = 4.21.	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2006																												AlB2																		K		6.2					6.2																																				A			3100	6500								3.54																							mOhm.cm							0.045																		floating zone method					Anisotropic s-wave superconductivity in CaAlSi single crystals from penetration depth measurements			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 73(2006)184523	R.Prozorov,T.A.Olheiser,R.W.Giannetta,K.Uozato,T.Tamegai		
40671	P073184523	6-fold structure. PENET from frequency shift analysis of LC-tunnel diode for H//ab and H//c fields. GAPENE(c-plane) = 4.03.	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2006																												AlB2																		K		7.3					7.3																																				A			3100	6500								3.54																							mOhm.cm							0.033																		floating zone method					Anisotropic s-wave superconductivity in CaAlSi single crystals from penetration depth measurements			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 73(2006)184523	R.Prozorov,T.A.Olheiser,R.W.Giannetta,K.Uozato,T.Tamegai		
40672	JPS0732631	RRR=2.85	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2004																												AlB2																		K				7.7			7.7											Oe	magnetization	138							T		2.6												MHC40672		A		159			A	from Hc1(0)	2186																												mOhm.cm							0.1139																		arc-melting					Unconventional behavior of field-induced quasiparticle excitation in Ca(Al0.5Si0.5)2			Department of Physics,Aoyama Gakuin University, Sagamihara, Kanagawa, Japan	J.Phys.Soc.Jpn, 73(2004)2631	S.Kuroiwa,H.Takagiwa,M.Yamazawa,J.Akimitsu,K.Ohishi,A.Koda,W.Higemoto,R.Kadono		
40673	PCS0671334		Ba24Si100	Ba24Si100	Ba	24	Si	100																					2006	emu/mol-Si	-0.00154																										clathrate			A	14.07													type-III clathrate	K		1.4					1.4																				T	estimation from C(T,H)	0.24														A	from Hc2	372								meV	0.212									mJ/mol.K2	182														mOhm.cm											50														synthesized under high pressure					Specific heat capacity and magnetic susceptibility of superconducting Ba24Si100			Department of Physics, Graduate School of Science, Tohoku University and CREST-JST, 6-3 Aoba Aramaki Aoba-ku, Sendai, Miyagi 980-8578, Japan	J.Phys.Chem.Solids, 67(2006)1334	T.Rachi,K.Tanigaki,R.Kumashiro,K.Kobayashi,H.Yashino,K.Murata,H.Fukuoka,S.Yamanaka,H.Shimotani,T.Takenobu,Y.Iwasa,T.Sasaki,N.Kobayashi,Y.Miyazaki,K.Saito		
40674	PCS0671117	impurity phase = Si	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2006																												clathrate			A	10.3177														K		8					8																																																																																																high pressure-high-temperature synthesis (3GPa,800C,1h)					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40675	PCS0671117	impurity phase = Si	(Ba6Sr2)Si46	Ba6Sr2Si46	Ba	6	Sr	2	Si	46																			2006																												clathrate			A	10.3086														K		7.2					7.2																																																																																																high pressure-high-temperature synthesis (3GPa,800C,1h)					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40676	PCS0671117	impurity phase = Si	(Ba4Sr4)Si46	Ba4Sr4Si46	Ba	4	Sr	4	Si	46																			2006																												clathrate			A	10.2882														K		5.3					5.3																																																																																																high pressure-high-temperature synthesis (3GPa,800C,1h)					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40677	PCS0671117	impurity phase = Si	(Ba2Sr6)Si46	Ba2Sr6Si46	Ba	2	Sr	6	Si	46																			2006																												clathrate			A	10.2801														K		4.1					4.1																																																																																																high pressure-high-temperature synthesis (3GPa,800C,1h)					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40678	PCS0671117	impurity phase = Si	(Ba7Ca1)Si46	Ba7Ca1Si46	Ba	7	Ca	1	Si	46																			2006																												clathrate			A	10.3167														K		7.65					7.65																																																																																																high pressure-high-temperature synthesis (3GPa,800C,1h)					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40679	PCS0671117	synthesis(5GPa,900C,1h). impurity phase = Si	(Ba6Ca2)Si46	Ba6Ca2Si46	Ba	6	Ca	2	Si	46																			2006																												clathrate			A	10.2878														K		5.2					5.2																																																																																																high pressure-high-temperature synthesis					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40680	PCS0671117	synthesis(5GPa,900C,1h). impurity phase = Si, CaSi2	(Ba4Ca4)Si46	Ba4Ca4Si46	Ba	4	Ca	4	Si	46																			2006																												clathrate			A	10.2775														K		3.7					3.7																																																																																																high pressure-high-temperature synthesis					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40681	PCS0671117	synthesis(1.1GPa,650C,1h). impurity phase = Si	Ba24Si100	Ba24Si100	Ba	24	Si	100																					2006																												clathrate			A	14.063														K		1.55					1.55																																																																																																high pressure-high-temperature synthesis					High pressure synthesis and properties of intercalated silicon clathrates			LPMCN, Universite Lyon-I and CNRS, Batiment Leon Brillouin, 43 Boulevard du 11 Novembre 1918, F-69622 Villeurbanne cedex, France	J.Phys.Chem.Solids, 67(2006)1117	P.Toulemonde,A.San Miguel,A.Merlen,R.Viennois,S.Le Floch,Ch.Adessi,X.Blase,J.L.Tholence		
40682	PCS0670751	not SC. SUS shows negative value at low temperature for ZFC, but no resistivity drop.	YbFe4Al8	Yb1Fe4Al8	Yb	1	Fe	4	Al	8																			2006																											2				A	8.712		5.044												K					2																																																																																																		induction melting					Magnetic and electronic properties of the antiferromagnetic YbFe4Al8 compound			Institute of Molecular Physics, Polish Academy of Sciences,Smoluchowskiego,Poznan.Poland	J.Phys.Chem.Solids, 67(2006)751	T.Tolinski,B.Andrzejewski,A.Kowalczyk,G.Chelkowska,A.Szlaferek,J.Frackowiak		
40683	J075064711	sub-meV resolution PES(Photoemission spectroscopy)	LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																		3	2006																												skutterudite																		K		7.2					7.2																																														meV	1.3	4.2	9																																															Sn-flux method					Superconducting Gap of Filled Skutterudite Superconductor LaRu4P12 Studied by Sub-meV Resolution Photoemission Spectroscopy			The Institute for Solid State Physics, The University of Tokyo, 5-1-5 Kashiwa-no-ha, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 75(2006)064711	S.Tsuda,T.Yokoya,T.Kiss,T.Shimojima,S.Shin,T.Togashi,S.Watanabe,C.Q.Zhang,C.T.Chen,H.Sugawara,H.Sato,H.Harima		
40684	P073214505	B<11> NMR measured	MgB2	B2Mg1	B	2	Mg	1																				1	2006																												AlB2			A	3.0847		3.5256												K		38.5					38.5																																																																																														Mg,B(amorphous),Fe2O3(powder)		mixture - pellet - wrapped in Ta-foil - ANN(900C,15min)					Effects of Fe substitution on Tc suppression of MgB2: A <11>B NMR study			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 73(2006)214505	C.S.Lue,T.H.Su,B.X.Xie,S.K.Chen,J.L.MacManus-Driscoll,Y.K.Kuo,H.D.Yang		
40685	P073214505	B<11> NMR measured	(Mg,Fe)B2	Mg0.997Fe0.003B2	Mg	0.997	Fe	0.003	B	2																		1	2006																												AlB2			A	3.0841		3.5247												K		37.7					37.7																																																																																														Mg,B(amorphous),Fe2O3(powder)		mixture - pellet - wrapped in Ta-foil - ANN(900C,15min)					Effects of Fe substitution on Tc suppression of MgB2: A <11>B NMR study			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 73(2006)214505	C.S.Lue,T.H.Su,B.X.Xie,S.K.Chen,J.L.MacManus-Driscoll,Y.K.Kuo,H.D.Yang		
40686	P073214505	B<11> NMR measured	(Mg,Fe)B2	Mg0.994Fe0.006B2	Mg	0.994	Fe	0.006	B	2																		1	2006																												AlB2			A	3.0827		3.5241												K		34.2					34.2																																																																																														Mg,B(amorphous),Fe2O3(powder)		mixture - pellet - wrapped in Ta-foil - ANN(900C,15min)					Effects of Fe substitution on Tc suppression of MgB2: A <11>B NMR study			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 73(2006)214505	C.S.Lue,T.H.Su,B.X.Xie,S.K.Chen,J.L.MacManus-Driscoll,Y.K.Kuo,H.D.Yang		
40687	P073214505	B<11> NMR measured	(Mg,Fe)B2	Mg0.988Fe0.012B2	Mg	0.988	Fe	0.012	B	2																		1	2006																												AlB2			A	3.082		3.5232												K		32					32																																																																																														Mg,B(amorphous),Fe2O3(powder)		mixture - pellet - wrapped in Ta-foil - ANN(900C,15min)					Effects of Fe substitution on Tc suppression of MgB2: A <11>B NMR study			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 73(2006)214505	C.S.Lue,T.H.Su,B.X.Xie,S.K.Chen,J.L.MacManus-Driscoll,Y.K.Kuo,H.D.Yang		
40688	P073214505	B<11> NMR measured	(Mg,Fe)B2	Mg0.97Fe0.03B2	Mg	0.97	Fe	0.03	B	2																		1	2006																												AlB2			A	3.0804		3.5217												K		30					30																																																																																														Mg,B(amorphous),Fe2O3(powder)		mixture - pellet - wrapped in Ta-foil - ANN(900C,15min)					Effects of Fe substitution on Tc suppression of MgB2: A <11>B NMR study			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 73(2006)214505	C.S.Lue,T.H.Su,B.X.Xie,S.K.Chen,J.L.MacManus-Driscoll,Y.K.Kuo,H.D.Yang		
40689	P073214508	RRR=7.2.  Tc(SP-heat) = 38.0 K	MgB2	B2Mg1	B	2	Mg	1																				1	2006																												AlB2			A	3.085		3.525												K		38.8		38.5		0.4	38.8																																																								mJ/mol.K2	3		670												uOhm.cm							2.5																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40690	P073214508	RRR=3.3.	Mg1-x(AlLi)xB2	Mg0.95Al0.025Li0.025B2	Mg	0.95	Al	0.025	Li	0.025	B	2																1	2006																												AlB2			A	3.083		3.512												K		37		36.2		0.7	37																																																																							uOhm.cm							6.5																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40691	P073214508	RRR=2.6.  Tc(SP-heat) = 31.0 K	Mg1-x(AlLi)xB2	Mg0.9Al0.05Li0.05B2	Mg	0.9	Al	0.05	Li	0.05	B	2																1	2006																												AlB2			A	3.082		3.497												K		36.4		34.1		1.5	36.4																																																								mJ/mol.K2	2.9		640												uOhm.cm							8.2																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40692	P073214508	RRR=2.0.  Tc(SP-heat) = 28.0 K	Mg1-x(AlLi)xB2	Mg0.8Al0.1Li0.1B2	Mg	0.8	Al	0.1	Li	0.1	B	2																1	2006																												AlB2			A	3.08		3.474												K		32.9		29		3	32.9																																																								mJ/mol.K2	2.7		615												uOhm.cm							14																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40693	P073214508	RRR=1.8.  Tc(SP-heat) = 24.0 K	Mg1-x(AlLi)xB2	Mg0.7Al0.15Li0.15B2	Mg	0.7	Al	0.15	Li	0.15	B	2																1	2006																												AlB2			A	3.074		3.454												K		32		26.9		4	32																																																								mJ/mol.K2	2.4		580												uOhm.cm							32																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40694	P073214508	RRR=1.8	Mg1-x(AlLi)xB2	Mg0.65Al0.175Li0.175B2	Mg	0.65	Al	0.175	Li	0.175	B	2																1	2006																												AlB2			A	3.075		3.453												K		30.7		25.1		5	30.7																																																																							uOhm.cm							28																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40695	P073214508	RRR=1.5	Mg1-x(AlLi)xB2	Mg0.6Al0.2Li0.2B2	Mg	0.6	Al	0.2	Li	0.2	B	2																1	2006																												AlB2			A	3.069		3.435												K		26.1		20.4		4.4	26.1																																																																							uOhm.cm							33																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40696	P073214508	RRR=1.5	Mg1-x(AlLi)xB2	Mg0.55Al0.225Li0.225B2	Mg	0.55	Al	0.225	Li	0.225	B	2																1	2006																												AlB2			A	3.07		3.432												K		25.6		18.1		4.1	25.6																																																																							uOhm.cm							40																		mixture(Mg+(AlLi)) - pellet, then put in Ta-tube with crystalline B, heat(850-900C,1h, in quartz tube) - heat(100C,100h)					Role of charge doping and lattice distortions in codoped Mg1-x(AlLi)xB2 compounds			CNR-INFM-LAMIA and Dipartimento di Fisica, Universita di Genova, Via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 73(2006)214508	M.Monni,C.Ferdeghini,M.Putti,P.Manfrinetti,A.Palenzona,M.Affronte,P.Postorino,M.Lavagnini,A.Sacchetti,D.Di Castro,F.Sacchetti,C.Petrillo,A.Orecchini		
40697	P073214528	Hc2(T) in Fig. obtained by ac-SUS (Hc2(0)=3.58 T). GL parameter = 27.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2006																																														K				7.6			7.6											mT	muon-SR	9.5							T	muon-SR	3.66												MHC40697		A	from Hc2	95			A	muon-SR	2520			meV	1.31	4																																																two-step arc-melting. first, Pd3B(arc-melt), then addition of Li(arc-melt)					Muon-spin-rotation measurements of the penetration depth in Li2Pd3B			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 73(2006)214528	R.Khasanov,I.L.Landau,C.Baines,F.La Mattina,A.Maisuradze,K.Togano,H.Keller		
40698	P073224519	NPENET measured directly using scanning SQUID spectroscopy	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		5	2006																												Y123																		K				83			83																																									um				19.5																																																			Pulsed Laser Deposition on SrTiO3(110)					Images of interlayer vortices and c-axis penetration depth of high-Tc YBa2Cu3O7-y superconductor			Nanomaterials Laboratory, National Institute for Materials Science, Sengen 1-2-1, Tsukuba 305-0047, Japan	Phys.Rev.B, 73(2006)224519	I.Iguchi,T.Takeda,T.Uchiyama,A.Sugimoto,T.Hatano		
40699	P073224516		NbB2	B2Nb1	B	2	Nb	1																					2006																												AlB2			A	3.1088		3.2724												K		2.73					2.73																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40700	P073224516		Nb1-xB2	B2Nb0.9	B	2	Nb	0.9																					2006																												AlB2			A	3.1079		3.269												K		3.64					3.64																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40701	P073224516		Nb1-xB2	B2Nb0.8	B	2	Nb	0.8																					2006																												AlB2			A	3.1089		3.2693												K		4.55					4.55																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40702	P073224516		Nb1-xB2	B2Nb0.7	B	2	Nb	0.7																					2006																												AlB2			A	3.0978		3.3193												K		7.96					7.96																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40703	P073224516		Nb1-xB2	B2Nb0.6	B	2	Nb	0.6																					2006																												AlB2			A	3.0973		3.319												K		8.04					8.04																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40704	P073224516		Nb1-xB2	B2Nb0.5	B	2	Nb	0.5																					2006																												AlB2			A	3.0952		3.3172												K		7.56					7.56																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40705	P073224516		Nb1-xB2	B2Nb0.4	B	2	Nb	0.4																					2006																												AlB2			A	3.0967		3.3183												K		6.57					6.57																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40706	P073224516		Nb1-xB2	B2Nb0.3	B	2	Nb	0.3																					2006																												AlB2			A	3.0961		3.3172												K		6.1					6.1																																																																																														Nb(powder),B(amorphous)		high-pressure synthesis. mixture - put in BN tube - heat(1200C,10min) - SIN(1200C,0.5h,P=6 GPa) - Q to RT					Correlations among superconductivity, structural instability, and band filling in Nb1-xB2 at the critical point x = 0.2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100080, People's Republic of China	Phys.Rev.B, 73(2006)224516	R.J.Xiao,K.Q.Li,H.X.Yang,G.C.Che,H.R.Zhang,C.Ma,Z.X.Zhao,J.Q.Li		
40707	L093107003	c-axis penetration depth measured by microwave method for various Tc samples ( See HIRFIG). crystal size=1.803*0.203*0.391 mm3.	YBa2Cu3Oz	Y1Ba2Cu3O6.35	Y	1	Ba	2	Cu	3															O	6+z	6.35	3	2004																												Y123																		K		20					20																																		PENET40707							um	microwave			28																																																								Survival of the d-Wave Superconducting State near the Edge of Antiferromagnetism in the Cuprate Phase Diagram			Department of Physics and Astronomy, University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z1	Phys.Rev.Lett., 93(2004)107003	A.Hosseini,D.M.Broun,D.E.Sheehy,T.P.Davis,M.Franz,W.N.Hardy,Ruixing Liang,D.A.Bonn		
40708	L096247004		KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2006																												pyrochlore																		K		9.6					9.6																																																																	THC40708																																				Thermal Conductivity of the Pyrochlore Superconductor KOs2O6: Strong Electron Correlations and Fully Gapped Superconductivity			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.Lett., 96(2006)247004	Y.Kasahara,Y.Shimono,T.Shibauchi,Y.Matsuda,S.Yonezawa,Y.Muraoka,Z.Hiroi		
40709	PHC4420091		TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3Oz	Tl	1	Ba	2	Ca	2	Cu	3													O	z		1	2006																												Tl1223																		K		128				2.2	128																																																																		uV/K	2.24			TP40709																					RH40709	E+21/cc	3.669			precursor(Ba2Ca2Cu3O7.45) mixed with 0.5Tl2O3  -  heat(900C,3h, P=4.5 GPa) - ANN(600C,40h, in N2)					Transport properties of TlBa2Ca2Cu3Oy in an over-doped state			Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-3510, Japan	Physica C, 442(2006)91	S.Mikusu,N.Urita,Y.Hashinaka,K.Tokiwa,A.Iyo,Y.Tanaka,T.Watanabe		
40710	PHC4420091		TlBa2Ca2Cu3Oz	Tl1Ba2Ca2Cu3Oz	Tl	1	Ba	2	Ca	2	Cu	3													O	z		1	2006																												Tl1223			A	3.864		15.912												K		130				1.2	130																																																																																												E+21/cc	3.139			precursor(Ba2Ca2Cu3O7.45) mixed with 0.5Tl2O3  -  heat(1080C,3h, P=4.5 GPa) - ANN(200C,75h, in Ar)					Transport properties of TlBa2Ca2Cu3Oy in an over-doped state			Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-3510, Japan	Physica C, 442(2006)91	S.Mikusu,N.Urita,Y.Hashinaka,K.Tokiwa,A.Iyo,Y.Tanaka,T.Watanabe		
40711	PHC4420101	Bi2223-phase=94%. Bi2212+unknown phase = 6 %. Thermal expansion coeff. = 7.90 E-7 /K.	(Bi,Pb)2Sr2Ca2Cu3Oz	Bi1.6Pb0.4Sr2Ca2Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	z		1	2006										GPa	0.254																	Bi2223			A	5.413		37.236												K	107		116				111.5																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40712	PHC4420101	Bi2223-phase=92%. Bi2212+unknown phase = 8 %. Thermal expansion coeff. = 7.70 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.9995Sm0.0005Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.9995	Sm	0.0005	Cu	3									O	z		1	2006										GPa	0.272																	Bi2223			A	5.416		37.206												K	102		116				109																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40713	PHC4420101	Bi2223-phase=83%. Bi2212+unknown phase = 17 %. Thermal expansion coeff. = 7.50 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.999Sm0.001Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.999	Sm	0.001	Cu	3									O	z		2	2006										GPa	0.294																	Bi2223			A	5.418		37.197												K	97		112				104.5																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40714	PHC4420101	Bi2223-phase=79%. Bi2212+unknown phase = 21 %. Thermal expansion coeff. = 6.95 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.995Sm0.005Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.995	Sm	0.005	Cu	3									O	z		2	2006										GPa	0.348																	Bi2223			A	5.421		37.19												K	93		107				100																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40715	PHC4420101	Bi2223-phase=74%. Bi2212+unknown phase = 26 %. Thermal expansion coeff. = 6.50 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.99Sm0.01Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.99	Sm	0.01	Cu	3									O	z		2	2006										GPa	0.398																	Bi2223			A	5.424		37.181												K	85		102				93.5																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40716	PHC4420101	Bi2212-phase = 100%.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.9Sm0.1Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.9	Sm	0.1	Cu	3									O	z		1	2006										GPa	0.442																	Bi2212			A	5.431		30.741												K	70		88				79																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40717	PHC4420101	Bi2212-phase = 100%.  Thermal expansion coeff. = 5.92 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca2.5Sm0.5Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	2.5	Sm	0.5	Cu	3									O	z		1	2006										GPa	0.525																	Bi2212			A	5.443		30.651												K	28		78				53																																																																																																mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40718	PHC4420101	not SC.. Bi2212-phase = 100%.  Thermal expansion coeff. = 5.80 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca1Sm1Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	1	Sm	1	Cu	3									O	z		1	2006										GPa	0.552																	Bi2212			A	5.464		30.323												K					21																																																																																																		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40719	PHC4420101	not SC. Bi2212-phase = 100%.  Thermal expansion coeff. = 5.70 E-7 /K.	(Bi,Pb)2Sr2(Ca,Sm)2Cu3Oz	Bi1.6Pb0.4Sr2Ca0.5Sm1.5Cu3Oz	Bi	1.6	Pb	0.4	Sr	2	Ca	0.5	Sm	1.5	Cu	3									O	z		1	2006										GPa	0.623																	Bi2212			A	5.468		30.278												K					21																																																																																																		mixture - CAL(800-850C,24h) - pellet SIN(860-950C,200h) - cool to RT(3C/min or 5C/min)					Thermal expansion and Vickers hardness measurements on Bi1.6Pb0.4Sr2Ca2-xSmxCu3Oy superconductors			Department of Physics, Faculty of Science and Arts, Kirikkale University, 71451 Yahsihan, Kirikkale, Turkey	Physica C, 442(2006)101	M.Yilmazlar,H.A.Cetinkara,M.Nursoy,O.Ozturk,C.Terzioglu		
40720	SSC1390057		Nb2SnC	Nb2Sn1C1	Nb	2	Sn	1	C	1																		1	2006																													P6<3>/mmc		A	3.22		13.707												K	3.3		7.8	4		4	4																																																																																														graphite,Nb,Sn		mixture - sealed in quartz ampoule - heat(1200C,24h) - SIN(1200C,48h)					Superconductivity in the Nb2SnC compound			Grupo de Supercondutividade, Departamento de Engenharia de Materiais, Faenquil-Polo Urbo Industrial Gleba AI 6 s/n, 12600-970 Lorena, SP, Brazil	Solid State Commun., 139(2006)57	A.D. Bortolozo,O.H.Sant'Anna,M.S.da Luz,C.A.M.dos Santos,A.S.Pereira,K.S.Trentin,A.J.S.Machado		
40721	SSC1390057		Nb2SnC	Nb2Sn1C1	Nb	2	Sn	1	C	1																		1	2006																																														K			7.8	7.8		0.6	7.8										32										T	resistive	7.8														A	from Hc2	65																																																								graphite,Nb,Sn		mixture with binder of paraffin wax(2 wt%) - heat(270C,4h) - heat(P=2.5 GPa, 523C, 30 min)					Superconductivity in the Nb2SnC compound			Grupo de Supercondutividade, Departamento de Engenharia de Materiais, Faenquil-Polo Urbo Industrial Gleba AI 6 s/n, 12600-970 Lorena, SP, Brazil	Solid State Commun., 139(2006)57	A.D. Bortolozo,O.H.Sant'Anna,M.S.da Luz,C.A.M.dos Santos,A.S.Pereira,K.S.Trentin,A.J.S.Machado		
40722	PHC4340173		TaC	C1Ta1	C	1	Ta	1																				1	2006																																														K		10.16					10.16																																		MHC40722																																																																			Effect of nanocrystal/carbon nanotube interface on surface superconductivity of TaC encapsulated in the multiwall carbon nanotubes			Department of Life and Envirounmental Science,College of Science and Engineering, Iwaki Meisei University,Fukushima,Japan	Physica C, 434(2006)173	Y.Yosida,I.Ishiguro		
40723	PHC4340173	nano-crystals encapsulated in MWCNT(multiwall carbon nanotube). Hc3/Hc2 = 1.24 for t < 0.9.	TaC	C1Ta1	C	1	Ta	1																				1	2006																															A	4.4526														K		10.16					10.16																																																																																																synthesis of single crystals TaC encapsulated in MWCNT using dc-arc evaporation of composite anode containing the mixture.					Effect of nanocrystal/carbon nanotube interface on surface superconductivity of TaC encapsulated in the multiwall carbon nanotubes			Department of Life and Envirounmental Science,College of Science and Engineering, Iwaki Meisei University,Fukushima,Japan	Physica C, 434(2006)173	Y.Yosida,I.Ishiguro		
40724	PR138A1170	G-L = 13. Hc(4.2K) = 0.80 kG. Clogston-Hp = 130 kG.	NbC	C1Nb1	C	1	Nb	1																					1965																																														K		9					9											Oe					120			4.2	T	resistive	1.69			1.69			4.2																												erg/cm3.K2	0.0023	estimated from RESN													mOhm.cm							0.0351																							High-field superconductivity of carbides				Phys.Rev., 38A(1965)1170	H.J.Fink,A.C.Thorsen,E.Parker,V.F.Zackav,L.Toth		
40725	PR138A1170	G-L = 8.1. Hc(1.2K) = 0.99 kG. Clogston-Hp = 214 kG.	(Nb,Ta)C	Nb0.4Ta0.6C1	Nb	0.4	Ta	0.6	C	1																			1965																																														K		11.8					11.8											Oe					190			1.2	T	resistive	1.41			1.41			1.2																												erg/cm3.K2	0.0012	estimated from RESN													mOhm.cm							0.0307																							High-field superconductivity of carbides				Phys.Rev., 38A(1965)1170	H.J.Fink,A.C.Thorsen,E.Parker,V.F.Zackav,L.Toth		
40726	PR138A1170	G-L = 3.2. Hc(1.2K) = 0.81 kG. Clogston-Hp = 185 kG.	TaC	C1Ta1	C	1	Ta	1																					1965																																														K		10.2					10.2											Oe					220			1.2	T	resistive	0.46			0.46			1.2																												erg/cm3.K2	0.0011	estimated from RESN													mOhm.cm							0.0127																							High-field superconductivity of carbides				Phys.Rev., 38A(1965)1170	H.J.Fink,A.C.Thorsen,E.Parker,V.F.Zackav,L.Toth		
40727	PR138A1170	G-L = 42. Hc(1.2K) = 1.3 kG. Clogston-Hp = 238 kG.	Mo1-xCx	C0.44Mo0.56	C	0.44	Mo	0.56																					1965																																														K		13					13											Oe					87			1.2	T	resistive	9.85			9.85			1.2																												erg/cm3.K2	0.0019	estimated from RESN													mOhm.cm							0.128																							High-field superconductivity of carbides				Phys.Rev., 38A(1965)1170	H.J.Fink,A.C.Thorsen,E.Parker,V.F.Zackav,L.Toth		
40728	PR138A1170	G-L = 53. Hc(1.2K) = 1.7 kG. Clogston-Hp = 181 kG.	Mo3Al2C	Mo3Al2C1	Mo	3	Al	2	C	1																			1965																																														K		10					10											Oe					91			1.2	T	resistive	15.6			15.6			1.2																												erg/cm3.K2	0.005	estimated from RESN													mOhm.cm							0.0987																							High-field superconductivity of carbides				Phys.Rev., 38A(1965)1170	H.J.Fink,A.C.Thorsen,E.Parker,V.F.Zackav,L.Toth		
40729	AC12810012	layered structure (La-O/Fe-P). carrier is electron(negative thermopower).	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1			2006																											2				A	3.964		8.512												K	3.2		5				4.1										18																																																																																				LaP,FeP,Fe2P,La,LaF3,La2O3		powder mixture - in silica tube(Ar-gas) - heat(1200C,40h)					Iron-based layered superconductor: LaOFeP			ERATO-SORST,JST, Frontier Collaborative Research Center, Tokyo Institute of Technology,Nagatsuta, Yokohama,Japan	J.Am.Chem.Soc., 128(2006)10012	Y.Kamihira,H.Hiramatsu,M.Hirano,R.Kawamura,H.Yanagi,T.Kamiya,H.Hosono		
40730	AC12810012	layered structure (La-O/Fe-P). F-content  = nominal value. carrier is electron(negative thermopower).	La(O,F)FeP	La1Fe1P1F0.06O0.94	La	1	Fe	1	P	1	F	0.06													O	0.94			2006																												oxypnictide																		K	6		9				7.5										91																																																																																				LaP,FeP,Fe2P,La,LaF3,La2O3		powder mixture - in silica tube(Ar-gas) - heat(1200C,40h)					Iron-based layered superconductor: LaOFeP			ERATO-SORST,JST, Frontier Collaborative Research Center, Tokyo Institute of Technology,Nagatsuta, Yokohama,Japan	J.Am.Chem.Soc., 128(2006)10012	Y.Kamihira,H.Hiramatsu,M.Hirano,R.Kawamura,H.Yanagi,T.Kamiya,H.Hosono		
40731	JAC4080054	not SC. XRD pattern shows significant splitting. SP-heat shows magnetic ordering.	CePt3Al	Ce1Pt3Al1	Ce	1	Pt	3	Al	1																			2006																																														K					0.4																																																																																																Ce(3N),Pt(4N),Al(5N),Ge(6N)		arc-melting - ANN(850C,8d, in vac(wrapped in Ta)					Transport and thermodynamic properties of CePt3X intermetallics			Charles University, Department of Electronic Structures, Ke Karlovu 5, 121 16 Praha 2, The Czech Republic	J.Alloys & Compd., 408-412(2006)54	J.Vejpravova,J.Prokleska,V.Sechovsky		
40732	JAC4080054	not SC. XRD pattern shows significant splitting. SP-heat shows magnetic ordering.	CePt3Ge	Ce1Pt3Ge1	Ce	1	Pt	3	Ge	1																			2006																																														K					0.4																																																																																																Ce(3N),Pt(4N),Al(5N),Ge(6N)		arc-melting - ANN(850C,8d, in vac(wrapped in Ta)					Transport and thermodynamic properties of CePt3X intermetallics			Charles University, Department of Electronic Structures, Ke Karlovu 5, 121 16 Praha 2, The Czech Republic	J.Alloys & Compd., 408-412(2006)54	J.Vejpravova,J.Prokleska,V.Sechovsky		
40733	JAC4080054	not SC. XRD pattern shows significant splitting. SP-heat shows magnetic ordering.	CePt3B	Ce1Pt3B1	Ce	1	Pt	3	B	1																			2006																																														K					0.4																																																																																																Ce(3N),Pt(4N),Al(5N),Ge(6N)		arc-melting - ANN(850C,8d, in vac(wrapped in Ta)					Transport and thermodynamic properties of CePt3X intermetallics			Charles University, Department of Electronic Structures, Ke Karlovu 5, 121 16 Praha 2, The Czech Republic	J.Alloys & Compd., 408-412(2006)54	J.Vejpravova,J.Prokleska,V.Sechovsky		
40734	JP01800L68	Na-content by ICP. NQR of Co<59> measured.	NaxCoO2:(H2O)1.3	Na0.34Co1H2.6O3.3	Na	0.34	Co	1	H	2.6															O	3.3			2006																															A	2.822		19.5												K				2.65			2.65																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40735	JP01800L68	Na-content by ICP. NQR of Co<59> measured.	NaxCoO2:(H2O)1.3	Na0.32Co1H2.6O3.3	Na	0.32	Co	1	H	2.6															O	3.3			2006																															A	2.822		19.62												K				2.6			2.6																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40736	JP01800L68	Na-content by ICP. NQR of Co<59> measured.	NaxCoO2:(H2O)1.3	Na0.31Co1H2.6O3.3	Na	0.31	Co	1	H	2.6															O	3.3		1	2006																															A	2.819		19.59												K				3.7			3.7																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40737	JP01800L68	Na-content by ICP. NQR of Co<59> measured.	NaxCoO2:(H2O)1.3	Na0.28Co1H2.6O3.3	Na	0.28	Co	1	H	2.6															O	3.3		1	2006																															A	2.817		19.73												K				4.75			4.75																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40738	JP01800L68	Na-content by ICP. NQR of Co<59> measured.	NaxCoO2:(H2O)1.3	Na0.25Co1H2.6O3.3	Na	0.25	Co	1	H	2.6															O	3.3		1	2006																															A	2.817		19.8												K				4.7			4.7																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40739	JP01800L68	Na-content by ICP. NQR of Co<59> measured. (1/T1) shows T^3 variation down to Tc/6.	NaxCoO2:(H2O)1.3	Na0.26Co1H2.6O3.3	Na	0.26	Co	1	H	2.6															O	3.3		1	2006																															A	2.815		19.79												K				4.6			4.6																																																																																																precursor(Na0.75CoO2) immersed in Br/CH3CN solution. For several Na-content, different Br-content solution used					Na content dependence of superconductivity and the spin correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama, Japan	J.Phys.Condens.Matter, 18(2006)L63	Guo-qing Zheng,K.Matano,R.L.Meng,J.Cmaidalka,C.W.Chu		
40740	SCI2922462	SWCNT(Single-walled carbon nanotube)  4 A in diameter.	C(CNT)	C1	C	1																							2001																																														K		15					15																																																																																														RuO2,SrO2,Eu2O3,CeO2,CuO	1	mixture - CAL(1020, 1040, 1060C for 24h) - pellet - ANN(1075C, 40h, in O2-flow) - slow cool to RT.					Superconductivity in 4 angstrom single-walled carbon nanotubes				Science 292(2001)2462	C.T.Chan,G.D.Li,G.H.Wen,J.N.Wang,L.Zhang,N.Wang,P.Sheng,X.X.Zhang,Z.K.Tang		
40741	JP01802563	magnetic transition at 140 K.	RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.5Ce0.5Cu2O9.6	Ru	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10-z	9.6		2006																												Ru1222	I4/mmm		A	3.8378		28.4849												K	25	33	43	25			33																				T	resistivity, extrapolation	32												HC40741		A	from Hc2	32																												uV/K				TP40741																										mixture - pellet - sealed in evacuated quartz tube(c-coated) - heat(1200C,6h) Q to RT					Magnetism, upper critical field and thermoelectric power of the magnetosuperconductor RuSr2Eu1.5Ce0.5Cu2O10-z			National Physical Laboratory, Dr K S Krishnan Marg, New Delhi-110012, India	J.Phys.Condens.Matter, 18(2006)2563	R.Lal,V.P.S.Awana,M.Peurla,Rajeev Rawat,V.Ganesan,H.Kishan,A.V.Marlikar,R.Laiho		
40742	JP01804417	parkerite structure. PENET,Hc1(0), GL-parameter calculated from Hc(0) using GLAG theory. Hc(0)=6.68 mT, GL = 10.1.  Tc(SP) = 0.72 K. (dC/gamma*Tc) = 1.35.	Bi2Ni3S2	Bi2Ni3S2	Bi	2	Ni	3	S	2																			2006																													C2/m																	K	0.75	0.79	0.85				0.79											mT	estimation from Hc	1.08							mT	resistivity, WHH	95							mT/K		180			MHC40742		A	from Hc2	590			A	estimation from Hc(0), GLAG	5919										MSP40742			mJ/mol.K2	11.4	SP-heat	189	SP-heat																																				mixture - pellet - sealed in evacuated quartz tube(c-coated) - heat(1200C,6h) Q to RT					Superconductivity in ternary chalcogenides Bi2Ni3X2 (X = S, Se)			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	J.Phys.Condens.Matter, 18(2006)4417	T.Sakamoto,M.Wakeshima,Y.Hinatsu		
40743	JP01804417	parkerite structure. PENET,Hc1(0), GL-parameter calculated from Hc(0) using GLAG theory. Hc(0)=6.39 mT, GL = 8.31.  Tc(SP) = 0.70 K. (dC/gamma*Tc) = 1.16.	Bi2Ni3Se2	Bi2Ni3Se2	Bi	2	Ni	3	Se	2																			2006																													C2/m																	K	0.66	0.73	0.86				0.73											mT	estimation from Hc	1.15							mT	resistivity, WHH	75							mT/K		148			MHC40743		A	from Hc2	660			A	estimation from Hc(0), GLAG	5497										MSP40743			mJ/mol.K2	12.2	SP-heat	173	SP-heat																																				mixture - pellet - sealed in evacuated quartz tube(c-coated) - heat(1200C,6h) Q to RT					Superconductivity in ternary chalcogenides Bi2Ni3X2 (X = S, Se)			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	J.Phys.Condens.Matter, 18(2006)4417	T.Sakamoto,M.Wakeshima,Y.Hinatsu		
40744	PHC4430029		Tl2Ba2Ca(Cu,Fe)2O8	Tl2Ba2Ca1Cu1.98Fe0.02O8	Tl	2	Ba	2	Ca	1	Cu	1.98	Fe	0.02											O	8			2006																												Tl2212																		K		106		107			106																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40745	PHC4430029	NMR measured. measurement of F-content was not shown.	Tl2Ba2Ca(Cu,Fe)2(F,O)8	Tl2Ba2Ca1Cu1.98Fe0.02F0.1O7.95	Tl	2	Ba	2	Ca	1	Cu	1.98	Fe	0.02	F	0.1									O	7.95			2006																												Tl2212																		K		110		111			110																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40746	PHC4430029	impurity phase=negligible CuO, BaCO3. NMR measured. measurement of F-content was not shown.	Tl2Ba2Ca(Cu,Fe)2(F,O)8	Tl2Ba2Ca1Cu1.98Fe0.02F0.2O7.9	Tl	2	Ba	2	Ca	1	Cu	1.98	Fe	0.02	F	0.2									O	7.9			2006																												Tl2212																		K		109		111			109																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40747	PHC4430029	impurity phase=CuO,BaCO3,BaCuO2,BaF2. measurement of F-content was not shown.	Tl2Ba2Ca(Cu,Fe)2(F,O)8	Tl2Ba2Ca1Cu1.98Fe0.02F0.3O7.85	Tl	2	Ba	2	Ca	1	Cu	1.98	Fe	0.02	F	0.3									O	7.85			2006																												Tl2212																		K		101		106			101																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40748	PHC4430029		Tl2Ba2(Ca,Ce)(Cu,Fe)2O8	Tl2Ba2Ca0.9Ce0.1Cu1.98Fe0.02O8	Tl	2	Ba	2	Ca	0.9	Ce	0.1	Cu	1.98	Fe	0.02									O	8			2006																												Tl2212																		K		99		103			99																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40749	PHC4430029	NMR measured. NMR measured. measurement of Ce- and F-content was not shown.	Tl2Ba2(Ca,Ce)(Cu,Fe)2(F,O)8	Tl2Ba2Ca0.9Ce0.1Cu1.98Fe0.02F0.2O7.9	Tl	2	Ba	2	Ca	0.9	Ce	0.1	Cu	1.98	Fe	0.02	F	0.2							O	7.9			2006																												Tl2212																		K		103		106			103																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40750	PHC4430029	impurity phase=BaCO3	Tl2Ba2(Ca,Ce)Cu2O8	Tl2Ba2Ca0.9Ce0.1Cu2O8	Tl	2	Ba	2	Ca	0.9	Ce	0.1	Cu	2											O	8			2006																												Tl2212																		K		100		102			100																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40751	PHC4430029	impurity phase=BaCO3	Tl2Ba2(Ca,Ce)Cu2O8	Tl2Ba2Ca0.8Ce0.2Cu2O8	Tl	2	Ba	2	Ca	0.8	Ce	0.2	Cu	2											O	8			2006																												Tl2212																		K		103		103			103																																																																																																See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40752	PHC4430029	not SC. impurity phase=BaCO3, BaCuO2	Tl2Ba2(Ca,Ce)Cu2O8	Tl2Ba2Ca0.7Ce0.3Cu2O8	Tl	2	Ba	2	Ca	0.7	Ce	0.3	Cu	2											O	8			2006																												Tl2212																		K																																																																																																							See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40753	PHC4430029	not SC. impurity phase=BaCO3, BaCuO2	Tl2Ba2(Ca,Ce)Cu2O8	Tl2Ba2Ca0.6Ce0.4Cu2O8	Tl	2	Ba	2	Ca	0.6	Ce	0.4	Cu	2											O	8			2006																												Tl2212																		K																																																																																																							See Inorganic Mater., 42-3(2006)1					Effect of fluorine and cerium substitutions on the properties of the Tl2Ba2CaCu1.98Fe0.02O8 superconductor			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus P, Brovki 19, Minsk 220072, Belarus	Physica C, 443(2006)29	A.I. Akimov,V. Ksenofontov,S.A. Lebedev,T.M. Tkachenka		
40754	P074020505	as-grown. p = 0.143 (determined using Tallon's eq.. with Tc(max)=93.6 K)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				91.5			91.5																				T	using dHc2/dT & WHH	221							T/K		3.45					A	from Hc2	12.2																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40756	P074020505	ANN(520C, 110h). p = 0.126 (determined using Tallon's eq.. with Tc(max)=93.6 K)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				84.4			84.4																				T	using dHc2/dT & WHH	191.5							T/K		3.23					A	from Hc2	13.1																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40757	P074020505	ANN(540C, 120h). p = 0.116 (determined using Tallon's eq.. with Tc(max)=93.6 K)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				78.6			78.6																				T	using dHc2/dT & WHH	167							T/K		3.03					A	from Hc2	14																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40758	P074020505	ANN(580C, 110h). p = 0.102 (determined using Tallon's eq.. with Tc(max)=93.6 K)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				68			68																				T	using dHc2/dT & WHH	97							T/K		2					A	from Hc2	18.5																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40759	P074020505	ANN(680C, 130h). p = 0.093 (determined using Tallon's eq.. with Tc(max)=93.6 K)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				58.4			58.4																				T	using dHc2/dT & WHH	78.5							T/K		1.82					A	from Hc2	20.4																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40760	P074020505	ANN(520C,90h, in flowing N2). p = 0.070 (determined using Tallon's eq.. with Tc(max)=93.6 K). Tc = 0 for p = 0.058(=p<cr>)	YBa2Cu3Oz	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		3	2006																												Y123																		K				30.3			30.3																				T	using dHc2/dT & WHH	36.9							T/K		1.43					A	from Hc2	30.2																																																										Crystals were grown by top-seeded solution growth using Ba3Cu5O solvent. ANN(400C,180h in flowing O2)					Reversible magnetization and critical fluctuations in systematically doped YBa2Cu3O7-z single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)020505R	Hong Gao,Cong Ren,Lei Shan,Yue Wang,Yingzi Zhang,Shiping Zhao,Xin Yao,Hai-Hu Wen		
40761	P070020505	P-induced SC. Tc shows at P = 1.75 GPa. Figure shows Tc(x) at P=1.75 GPa.	Ce(Rh,Ir)In5	Ce1Rh0.9Ir0.1In5	Ce	1	Rh	0.9	Ir	0.1	In	5																	2004																												HoCoGa5																		K		2.04			0		2.04	MTC40761																																																																																																				Two superconducting phases in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 70(2004)020505	M.Nicklas,V.A.Sidorov,H.A.Borges,P.G.Pagliuso,J.L.Sarrao,J.D.Thompson		
40762	P070020505	P-induced SC. Tc shows at P = 1.0 GPa. Figure shows Tc(x) at P=1.0 GPa.	Ce(Rh,Ir)In5	Ce1Rh0.75Ir0.25In5	Ce	1	Rh	0.75	Ir	0.25	In	5																	2004								2.86																				HoCoGa5																		K		1.84			0		1.84	MTC40762																																																																																																				Two superconducting phases in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 70(2004)020505	M.Nicklas,V.A.Sidorov,H.A.Borges,P.G.Pagliuso,J.L.Sarrao,J.D.Thompson		
40763	P070020505	Figure shows Tc(x) at P=0 GPa.	Ce(Rh,Ir)In5	Ce1Rh0.5Ir0.5In5	Ce	1	Rh	0.5	Ir	0.5	In	5																	2004								3.65																				HoCoGa5																		K		0.79					0.79	MTC40763																																																																																																				Two superconducting phases in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 70(2004)020505	M.Nicklas,V.A.Sidorov,H.A.Borges,P.G.Pagliuso,J.L.Sarrao,J.D.Thompson		
40764	P074012504	Li-content by ICP. Hc2(T) defined as R/Rn = 0.9.	Li0.68NbO2	Li0.68Nb1O2	Li	0.68	Nb	1																	O	2		1	2006																												MoS2																		K	4.8		5.5			0.7	5.15																																		MHC40764	resistive											meV	0.8		14							mj/mol.K2	3.588	SP-heat	462																																					LiNbO2 synthesized by heating (1050C,60h) of (Li3NbO+NbO), Chemical reaction (Li0.93NbO2 + bromine as oxidative agent, at RT)					Evidence of s-wave pairing symmetry in the layered superconductor Li0.68NbO2 from specific heat measurements			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)012504	G.T.Liu,J.L.Luo,Z.Li,Y.Q.Guo,N.L.Wang,D.Jin,T.Xiang		
40765	P074020501	P-induced SC. Pc*(AF) = 1.95 K. P(Tcmax) = 2.4 GPa. Coexistence phase(AF+SC) appears below Pc* under magnetic field. SP-heat measured. SC data for P=2.41 GPa.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																			2006																												HoCoIn5																		K		2.24			0		2.24																													T/K		35			MHC40765																																																																			Coexistence of antiferromagnetism and superconductivity in CeRhIn5 under high pressure and magnetic field				Phys.Rev.B, 74(2006)020501R	G. Knebel,D. Aoki,D. Braithwaite,B. Salce,J. Flouquet		
40766	P074024505	Figure of Tc(P) contains the data of two samples(RRR=10 and 25). no difference between R//ab and R//c measurements.	C6Yb	C6Yb1	C	6	Yb	1																				3	2006																																														K		6.5					6.5	MTC40766		K/GPa	0.37																																																																																																	Pressure dependence of the superconducting transition temperature in C6Yb and C6Ca			Cavendish Laboratory, University of Cambridge, J. J. Thompson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 74(2006)020501R	R.P.Smith,A.Kusmartseva,Y.C.Ko,S.S.Sexena,A.Akrap,L.Forro,M.Laad,T.E.Weller,M.Ellerby,N.T.Skipper		
40767	P074024505	Tc by M(50Oe)	C6Ca	C6Ca1	C	6	Ca	1																				3	2006																																														K		11.1					11.1	MTC40767		K/GPa	0.5																																																																																																	Pressure dependence of the superconducting transition temperature in C6Yb and C6Ca			Cavendish Laboratory, University of Cambridge, J. J. Thompson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 74(2006)020501R	R.P.Smith,A.Kusmartseva,Y.C.Ko,S.S.Sexena,A.Akrap,L.Forro,M.Laad,T.E.Weller,M.Ellerby,N.T.Skipper		
40768	GIC1981288		KTl1.5C4	K1Tl1.5C4	K	1	Tl	1.5	C	4																			1981																												GIC																		K		2.7					2.7																																																																																																					Physics of Intercalation Compounds'' ed, L.Pietronero and E.Tosatti				Springer, 1981, p=288	F.L.Vogel,R.Wachnick,L.A.Pendrys		
40769	GIC1981288		KTl1.5C8	K1Tl1.5C8	K	1	Tl	1.5	C	8																			1981																												GIC																		K		2.45					2.45																																																																																																					Physics of Intercalation Compounds'' ed, L.Pietronero and E.Tosatti				Springer, 1981, p=288	F.L.Vogel,R.Wachnick,L.A.Pendrys		
40770	SYN0050257	anisotropy factor = 4.7	KC8	C8K1	C	8	K	1																				3	1983																												GIC																		K		0.134					0.134																													Oe/K			160	40.3			A			7800	2000																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40771	SYN0050257	anisotropy factor = 6.2	KC8	C8K1	C	8	K	1																				3	1983																												GIC																		K		0.145					0.145																													Oe/K			160	42.8			A			9400	1500																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40772	SYN0050257	anisotropy factor = 10.4	KHgC4	K1Hg1C4	K	1	Hg	1	C	4																		3	1983																												GIC																		K		0.86					0.86																													Oe/K			760	57.2			A			2600	200																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40773	SYN0050257	anisotropy factor = 11.0	KHgC4	K1Hg1C4	K	1	Hg	1	C	4																		3	1983																												GIC																		K		0.73					0.73																													Oe/K			788	80.5	MHC40773		A			2400	240																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40774	SYN0050257	anisotropy factor = 10.2	RbHgC4	Rb1Hg1C4	Rb	1	Hg	1	C	4																		3	1983																												GIC																		K		0.99					0.99																													Oe/K			363	40.7	MHC40774		A			2900	320																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40775	SYN0050257	anisotropy factor = 15.5	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																		3	1983																												GIC																		K		1.9					1.9																													Oe/K			621	42.7			A			2000	140																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40776	SYN0050257	anisotropy factor = 21.7	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																		3	1983																												GIC																		K		1.94					1.94																													Oe/K			1060	47.5	MHC40776		A			1900	85																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40777	SYN0050257	anisotropy factor = 41.3	RbHgC8	Rb1Hg1C8	Rb	1	Hg	1	C	8																		3	1983																												GIC																		K		1.4					1.4																													Oe/K			2100	62.9	MHC40777		A			1900	58																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40778	SYN0050257	anisotropy factor = 47	RbHgC8	Rb1Hg1C8	Rb	1	Hg	1	C	8																		3	1983																												GIC																		K		1.4					1.4																													Oe/K			2090	44.3	MHC40778		A			2300	49																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40779	SYN0050257	anisotropy factor = 10	KTl1.5C4	K1Tl1.5C4	K	1	Tl	1.5	C	4																		3	1983																												GIC																		K		2.56					2.56																													Oe/K			16800	1690	MHC40779		A			276	27.8																																																								C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40780	SYN0050257	not SC	KTl1.5	K1Tl1.5	K	1	Tl	1.5																					1983																																														K					0.4																																																																																																		C8M prepared by usual two temperature method. C8M react with Hg vapor at 100C.					Superconductivity of graphite intercalation compounds-stage and pressure dependence of anisotropy				Synth.Met., 5(1983)257	Y.Iye,S.Tanuma		
40781	JPS0501964	pseudo single crystal. anisotropy factor = 31	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																		3	1981																												GIC																		K				1.9			1.9																													Oe/K			2300	69	MHC40781		A			1600	48																																																								KHg prepared in pyrex tube(400C,1d, in vac) - HOPG(graphite)+KHg2(300C,1w, in vac)					Anisotropic superconductivity in the graphite potassium-amalgam intercalation compound C8KHg				J.Phys.Soc.Jpn, 50(1981)1964	Y.Koike,S.Tanuma		
40782	JPS0501964	pseudo single crystal. anisotropy factor = 30	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																		3	1981																												GIC																		K				1.7			1.7																													Oe/K			2300	74	MHC40781		A			1600	52																																																								KHg prepared in pyrex tube(400C,1d, in vac) - HOPG(graphite)+KHg2(300C,1w, in vac)					Anisotropic superconductivity in the graphite potassium-amalgam intercalation compound C8KHg				J.Phys.Soc.Jpn, 50(1981)1964	Y.Koike,S.Tanuma		
40783	PR02606315	dTc/dT is for P-region of P>0.08 kbar.	KHgC4	K1Hg1C4	K	1	Hg	1	C	4																			1982																												GIC																		K	0.85		1.42				1.135			K/GPa	-0.49																																																																																																	Observation of anomalies in the pressure dependence of the superconducting transition temperature of potassium-based graphite intercalation compounds				Phys.Rev.B, 26(1982)6315	L.E.DeLong,V.Yeh,V.Tondiglia,P.C.Eklund,S.E.Lambert,M.B.Maple		
40784	PR02606315	not SC (P<10.1 kbar)	KC24	C24K1	C	24	K	1																					1982																												GIC																		K					0.07																																																																																																							Observation of anomalies in the pressure dependence of the superconducting transition temperature of potassium-based graphite intercalation compounds				Phys.Rev.B, 26(1982)6315	L.E.DeLong,V.Yeh,V.Tondiglia,P.C.Eklund,S.E.Lambert,M.B.Maple		
40785	SSC0380103	thermodynamic Hc(0) = 73 Oe	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																			1981																												GIC			A			13.51												K		1.93					1.93																																																								mj/mol.K2	0.2	SP-heat	260																																										Superconductivity of the graphite intercalation compounds KHgC8 and RbHgC8: Evidence from specific heat				Solid State Commun., 38(1981)103	M.G.Alexander,D.P.Goshorn,P.Lagrange,M.E.Makrini,D.G.Onn		
40786	SSC0380103	(dC/gamma*Tc) = 2.3	RbHgC8	Rb1Hg1C8	Rb	1	Hg	1	C	8																			1981																												GIC			A			14.21												K		1.46					1.46																																																								mj/mol.K2	0.15	SP-heat	235																																										Superconductivity of the graphite intercalation compounds KHgC8 and RbHgC8: Evidence from specific heat				Solid State Commun., 38(1981)103	M.G.Alexander,D.P.Goshorn,P.Lagrange,M.E.Makrini,D.G.Onn		
40787	PR02204535		RbC8	Rb1C8	Rb	1	C	8																					1980																												GIC																																																																																	mj/mol.K2	1.15	SP-heat	439																																										Low-temperature specific heat of the graphite intercalation compounds KC8, CsC8, RbC8, and their parent highly oriented pyrolytic graphite			Department of Physics, University of Delaware, Newark, Delaware 19711	Phys.Rev.B, 22(1980)4535	M.G.Alexander,D.P.Goshorn,D.G.Onn		
40788	PR02204535		CsC8	Cs1C8	Cs	1	C	8																					1980																												GIC																																																																																	mj/mol.K2	0.45	SP-heat	397																																										Low-temperature specific heat of the graphite intercalation compounds KC8, CsC8, RbC8, and their parent highly oriented pyrolytic graphite			Department of Physics, University of Delaware, Newark, Delaware 19711	Phys.Rev.B, 22(1980)4535	M.G.Alexander,D.P.Goshorn,D.G.Onn		
40789	PR02204535		KC8	K1C8	K	1	C	8																					1980																												GIC																																																																																	mj/mol.K2	0.75	SP-heat	374																																										Low-temperature specific heat of the graphite intercalation compounds KC8, CsC8, RbC8, and their parent highly oriented pyrolytic graphite			Department of Physics, University of Delaware, Newark, Delaware 19711	Phys.Rev.B, 22(1980)4535	M.G.Alexander,D.P.Goshorn,D.G.Onn		
40790	JPC005L230	Tc(P=0) = 7.149 - 7.191. (dTc/dP) = 0.028 K/GPa for P > 35 kbar.	NbSe2	Nb1Se2	Nb	1	Se	2																				3	1972																												TX2			A	3.45	12.56													K		7.15					7.15	MTC40790		K/GPa	0.495																																																																																																	Superconductivity of Nbse2 to 140 kbar				J.Phys.C, 5(1972)L230	T.F.Smith,L.E.Delong,A.R.Moodenbaugh,T.H.Geballe,R.E.Schwall		
40791	PHF0051713		TaS2	S2Ta1	S	2	Ta	1																					1975																												TX2			A	3.32		12.08											2H-type	K		0.65				0.19	0.65			K/GPa	0.975																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40792	PHF0051713		Ta(S,Se)2	Ta1S1.8Se0.2	Ta	1	S	1.8	Se	0.2																			1975																												TX2			A	3.33		12.18											4H-type	K		2.75				0.04	2.75			K/GPa	0.23																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40793	PHF0051713		Ta(S,Se)2	Ta1S1.6Se0.4	Ta	1	S	1.6	Se	0.4																			1975																												TX2			A	3.34		12.24											2H-type	K		3.84				0.24	3.84			K/GPa	0.575																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40794	PHF0051713		Ta(S,Se)2	Ta1S1.2Se0.8	Ta	1	S	1.2	Se	0.8																			1975																												TX2			A	3.36		24.84											4H-type	K		3.7				0.1	3.7			K/GPa	0.55																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40795	PHF0051713		Ta(S,Se)2	Ta1S1Se1	Ta	1	S	1	Se	1																			1975																												TX2			A	3.367		12.5											2H-type	K		3.36				0.12	3.36			K/GPa	0.55																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40796	PHF0051713		Ta(S,Se)2	Ta1S0.4Se1.6	Ta	1	S	0.4	Se	1.6																			1975																												TX2			A	3.41		25.28											4H-type	K		3.04				0.11	3.04			K/GPa	0.405																																																																																												(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40797	PHF0051713		TaSe2	Se2Ta1	Se	2	Ta	1																					1975																												TX2			A	3.43		12.7											2H-type	K		0.14				0.02	0.14																																																																																																(Ta-wire+Se-chunks+S-powder) - (evacuated quartz tube) - react(900-1000C, 5d)					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40798	PHF0051713	collidine-intercalated TaS2. M=collidine	TaS2(collidine)0.167	Ta1S2M0.167	Ta	1	S	2	M	0.167																			1975																												TX2			A	3.32		19.44											2H-type	K		2.84					2.84																																																																																																					Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40799	PHF0051713	pyridine-intercalated TaS2. M=pyridine	TaS2(pyridine)0.5	Ta1S2M0.5	Ta	1	S	2	M	0.5																			1975																												TX2			A	3.33		24.04											2H-type	K		3.24				0.3	3.24			K/GPa	-0.05																																																																																																	Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40800	PHF0051713	picoline-intercalated TaS2. M=picoline	TaS2(pikoline)0.333	Ta1S2M0.333	Ta	1	S	2	M	0.333																			1975																												TX2			A	3.31		23.5											2H-type	K		2.74				0.15	2.74			K/GPa	0.205																																																																																																	Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40801	PHF0051713	aniline-intercalated TaS2. M=aniline. (dTc/dP) < 0.13 K/GPa	TaS2(aniline)0.75	Ta1S2M0.75	Ta	1	S	2	M	0.75																			1975																												TX2			A	3.32		36.4											2H-type	K		2.49				1.66	2.49			K/GPa	0																																																																																																	Superconductivity of TaS2-xSex layer compounds at high pressure				J.Phys.F, 5(1975)1713	T.F.Smith,R.N.Shelton,R.E.Schwall		
40802	SSC0441145	Tc by ac-sus.	KHgC8	K1Hg1C8	K	1	Hg	1	C	8																		3	1982																												GIC			A			13.51												K		1.85					1.85			K/GPa	-0.65																																																																																										HOPG,Hg,K		KC8 firstly prepared. Then react with excess-Hg at 200C. Quench to Liq.N2					Pressure dependence of the superconducting transition temperature of the stage-2 potassium mercurographitide intercalation compound				Solid State Commun., 44(1982)1150	L.E.De Long,V.Yeh,P.C.Eklund		
40803	SSC0441145	not SC upto 22 kbar. Tc by ac-sus.	KHgC4	K1Hg1C4	K	1	Hg	1	C	4																			1982																												GIC																		K					1.3																																																																																																HOPG,Hg,K		KC8 firstly prepared. Then react with excess-Hg at 200C. Quench to Liq.N2					Pressure dependence of the superconducting transition temperature of the stage-2 potassium mercurographitide intercalation compound				Solid State Commun., 44(1982)1150	L.E.De Long,V.Yeh,P.C.Eklund		
40804	SSC0430005	Hc2 estimated from linear extrapolation to T=0 K. anisotropy factor = 4.5.	KTl1.5C4	K1Tl1.5C4	K	1	Tl	1.5	C	4																			1982																												GIC																		K		2.7					2.7																				kOe			20	4												A			290	60																																																								heat(graphite,KTl,Tl) in evacuated tube(200C)					Superconductivity of graphite intercalated with thallium alloys				Solid State Commun., 43(1982)5	R.A.Wachnik,L.A.Pendrys,F.L.Vogel,P.Lagrange		
40805	SSC0430005		KTl1.5C8	K1Tl1.5C8	K	1	Tl	1.5	C	8																			1982																												GIC																		K		2.45					2.45																				kOe																																																																												heat(graphite,KTl,Tl) in evacuated tube(200C)					Superconductivity of graphite intercalated with thallium alloys				Solid State Commun., 43(1982)5	R.A.Wachnik,L.A.Pendrys,F.L.Vogel,P.Lagrange		
40806	PRL0340577	N:S = 30.41:69.59. crystal polymer, quasi-1D material. e-ph coupling = 0.31.	(SN)x	N0.3S0.7	N	0.3	S	0.7																					1975																																														K		0.26					0.26																																																								mJ/g.K2	0.018	SP-heat	170																																										Superconductivity in polysulfur nitride (SN)x			IBM,San Jose	Phys.Rev.Lett., 34(1975)577	R.L.Greene,G.B.Street,L.J.Suter		
40807	PR05210315	Hc2(T) measured for H//[100] and H//[110]. no anisotyopy.	UBe13	Be13U1	Be	13	U	1																				3	1995																												NaZn13																	NaZn13, cF112	K				0.9035			0.9035																													T/K	SUS	32.8																																																																	Al-flux removed with NaOh. ANN(1000C, 6 months)					Inductive measurements and study of the upper critical field in UBe13 single crystals as a function of field orientation	199510			Phys.Rev.B,52(1995)10315	B. Andraka,G.R. Stewart,M.W. Meisel,P.J.C. Signore	V, Be	
40808	PR05210315	Hc2(T) measured for H//[100] and H//[110]. no anisotyopy.	UBe13	Be13U1	Be	13	U	1																				3	1995																												NaZn13																	NaZn13, cF112	K				0.9015			0.9015																													T/K	SUS	25.5																																																																	Al-flux removed with NaOh. ANN(1000C, 6 months)					Inductive measurements and study of the upper critical field in UBe13 single crystals as a function of field orientation	199510			Phys.Rev.B,52(1995)10315	B. Andraka,G.R. Stewart,M.W. Meisel,P.J.C. Signore	V, Be	
40809	PR05210315	Hc2(T) measured for H//[100] and H//[110]. no anisotyopy.	UBe13	Be13U1	Be	13	U	1																				3	1995																												NaZn13																	NaZn13, cF112	K				0.8493			0.8493																													T/K	SUS	34.5																																																																	Al-flux removed with NaOh. ANN(1000C, 6 months)					Inductive measurements and study of the upper critical field in UBe13 single crystals as a function of field orientation	199510			Phys.Rev.B,52(1995)10315	B. Andraka,G.R. Stewart,M.W. Meisel,P.J.C. Signore	V, Be	
40810	PR05215517	Jc measured using Bean model	K3C60	C60K3	C	60	K	3																				3	1995																												fullerene																		K				19.3			19.3											Oe	deviation in M-H curve	42																					MHC40810																																																														doping temperature = 165C for K and = 200K for Rb.					Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
40811	PR05215517	Jc measured using Bean model	Rb3C60	C60Rb3	C	60	Rb	3																				3	1995																												fullerene																		K				30			30											Oe	deviation in M-H curve	32																					MHC40810																																																														doping temperature = 165C for K and = 200K for Rb.					Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
40812	PR05209847	Hc2(0) estimated from Hc2(2.2K)  using linear approximation.	CeRu2	Ce1Ru2	Ce	1	Ru	2																					1995																												Laves																	Laves, C15	K				6.1			6.1																				T		8.4			2.2			4.5																																																																									Magnetic anomaly and the peak effect in superconduting CeRu2	199510			Phys.Rev.B,52(1995)9847	A.K. Pradhan,P. Chaddah,S.B. Roy	Ce, Ru	
40813	PR05207689	Tc not shown. G-L parameter = 70.	Nb0.35Ti0.65	Nb0.35Ti0.65	Nb	0.35	Ti	0.65																					1995																																														K																											T					10.4			4.2						MHC40813																																																																			Conparison of pinning parameters between low-Tc superconductors and YBa2Cu3O7-z	199509			Phys.Rev.B,52(1995)7689	"A.A. Zhukov,H. Ku""pfer,K. Kimura,K.Slama,R. Kresse,R. meier-Hirmer,T. Mathushita,T. Wolf,W. Jahn"	Y, Ba, Cu, O	
40814	PR05207689	Tc not shown. G-L parameter = 29.6. irradiated with fast neutrons , fluences = 2*E+22 /m2.	V3Si	V3Si1	V	3	Si	1																				3	1995																												Cr3Si(A15)																		K																											T					11.6			11.3						MHC40813																																																														ANN(1800C, 3w)					Conparison of pinning parameters between low-Tc superconductors and YBa2Cu3O7-z	199509			Phys.Rev.B,52(1995)7689	"A.A. Zhukov,H. Ku""pfer,K. Kimura,K.Slama,R. Kresse,R. meier-Hirmer,T. Mathushita,T. Wolf,W. Jahn"	Y, Ba, Cu, O	
40815	PR05207689	Tc not shown. G-L parameter = 17.3 irradiated with fast neutrons , fluences = 2*E+29 /m2.	V3Si	V3Si1	V	3	Si	1																				3	1995																												Cr3Si(A15)																		K																											T					5.6			13.5						MHC40813																																																														ANN(1800C, 3w)					Conparison of pinning parameters between low-Tc superconductors and YBa2Cu3O7-z	199509			Phys.Rev.B,52(1995)7689	"A.A. Zhukov,H. Ku""pfer,K. Kimura,K.Slama,R. Kresse,R. meier-Hirmer,T. Mathushita,T. Wolf,W. Jahn"	Y, Ba, Cu, O	
40817	PR05207689	Tc not shown. G-L parameter = 100	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1995																												Chevrel																		K																											T					11.6			10						MHC40813																																																																			Conparison of pinning parameters between low-Tc superconductors and YBa2Cu3O7-z	199509			Phys.Rev.B,52(1995)7689	"A.A. Zhukov,H. Ku""pfer,K. Kimura,K.Slama,R. Kresse,R. meier-Hirmer,T. Mathushita,T. Wolf,W. Jahn"	Y, Ba, Cu, O	
40818	JPS0522301	non-annealed sample. Hc1(0) shows Hc1(0.5K).	Cr74Re26	Cr0.74Re0.26	Cr	0.74	Re	0.26																					1983																															A	2.9516														K		3.12					3.12	MTC40818										Oe		100			100			0.5																																																																													arc-melting					Coexistence of antiferromagnetism and superconductivity in CrRe alloys				J.Phys.Soc.Jpn, 52(1983)2301	Y.Nishihara,Y.Yamaguchi,S.Waki,T.Kohara		
40819	PHF010L333	sample from Viennese.  Tc confirmed by SUS and RES.	Y4Co3	Co3Y4	Co	3	Y	4																					1980							6																																							K		2.1					2.1																																																																							mOhm.cm	0.0151																													Magnetism and superconductivity in a transition metal compounds: Y4Co3				J.Phys.F, 10(1980)L333	A.Kolodziejczyk,R.V.B.Sarkissian,B.R.Coles		
40820	PHF010L333	Sample from Imperial College.  Tc confirmed by SUS and RES.	Y4Co3	Co3Y4	Co	3	Y	4																					1980																																														K		1.5					1.5																																																																							mOhm.cm	0.0143																													Magnetism and superconductivity in a transition metal compounds: Y4Co3				J.Phys.F, 10(1980)L333	A.Kolodziejczyk,R.V.B.Sarkissian,B.R.Coles		
40821	JPS0542359	1st stage graphite. G-L parameter estimated tobe 0.33(Hc3=110 mOe) for H//c-axis.	C8Rb	C8Rb1	C	8	Rb	1																				3	1985																												GIC																		K				0.0252			0.0252																																																																																																react(230C,5d)					Superconductivity in the first stage rubidium graphite intercalation compound C8Rb				J.Phys.Soc.Jpn, 54(1985)2359	M.Kobayashi,T.Enoki,H.Inokuchi,M.Sano,A.Sumiyama,Y.Oda,H.Nagano		
40822	JPS0501275	MP=85.5 C. RRR=30. Hc3(0) = 4.038 kOe. thermodynamic Hc(0) = 0.520 kOe. e-ph coupling = 0.90. Rn = 2.8 uOhm.cm	In5Bi3	Bi3In5	Bi	3	In	5																					1981																												In5Bi3																	In5Bi3, tI32	K		4.14					4.14																				kOe		1.911							kOe/K		0.63			MHC40822																																																														melt in pyrex glass in vac.					Superconductivity and electrical resistivity saturation in intermetallic compound In5Bi3				J.Phys.Soc.Jpn, 50(1981)1275	K.Mori,N.Tamura,Y.Saito		
40823	JPS0450050	RRR=30. COHERE// = 610 A, COHERE/n = 77 A at 5.54 K. (Hc2//)/(Hc2/n) = 7.5 - 5.8 for 5.2 < T < 5.8K.	2H-NbS2	Nb1S2	Nb	1	S	2																				3	1978																												TX2																	2H-type	K		5.84					5.84																				kOe				21		6.99	0.88	5.54	kOe/K			22.6	4.5																																						uOhm.cm							1.7																		Chemical vapor transport method					Anisotropy of upper critical field in superconducting 2H-NbS2				J.Phys.Soc.Jpn, 50(1981)50	K.Onabe,M.Naito,S.Tanaka		
40824	SSC0920181	(dC/gamma*Tc) = 0.25	LaCu	Cu1La1	Cu	1	La	1																					1994																												FeB																		K		6.15				0.2	6.15																				kOe		12.6							kOe/K		2.97			MHC40824		A		162																					148	SP-heat																																				arc-melting					Upper critical magnetic field and specific heat studies on LaCu				Solid State Commun., 92(1994)181	J.W.Chen,Y.Y.Chen		
40825	SSC0860643	G-L parameter = 53.	K3C60	C60K3	C	60	K	3																				3	1993																												fullerene																		K		19.7				0.25	19.7																				T		17.5							T/K		1.34			MHC40825		A		45			A		2400																																																					sublimation growth and intercalation					Determination of superconducting and normal state parameters of single crystal K3C60				Solid State Commun., 86(1993)643	J.G.Hou,Vincent H.Crespi,X.-D.Xiang,W.A.Vareka,G.Briceno,A.Zittl,Marvin L.Cohen		
40826	SSC0690921	quench to 100K. high pressure phase(pressure quench). LAT-c = 3.69 A at 100K.	C2Li	C2Li1	C	2	Li	1																					1989																												GIC																		K			1.9				1.9																																																																																																react(350C, P=30-40 kbar, in stainless tube)					Superconductivity of graphite intercalation compound with C2Li				Solid State Commun., 69(1989)921	I.T.Belash,A.D.Bronnikov,O.V.Zharikov,A.V.Pal'nichenko		
40827	SSC0560589	tape. deposition temp. = 900C.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1985																												Cr3Si(A15)																	Cr3Si, A15	K		19.09					19.09																				T		25.14							T/K		1.9			MHC40827																																																														CVD method. Nb-Ge layers(thickness = 1-6 micron-m) on stainless tape) then, react thermally					Properties of Nb3Ge tapes for high field magnets				Solid State Commun., 56(1985)589	O.Demolliens,F.Weiss,R.Madar,J.P.Senateur,J.C.Vallier		
40828	SSC0560589	tape. deposition temp. = 1000C.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1985																												Cr3Si(A15)																	Cr3Si, A15	K		20.46					20.46																				T		31.19							T/K		2.2			MHC40827																																																														CVD method. Nb-Ge layers(thickness = 1-6 micron-m) on stainless tape) then, react thermally					Properties of Nb3Ge tapes for high field magnets				Solid State Commun., 56(1985)589	O.Demolliens,F.Weiss,R.Madar,J.P.Senateur,J.C.Vallier		
40829	SSC0520641	annealed at 680 K. GAMMA from Junod et al.	Ti3Sb	Sb1Ti3	Sb	1	Ti	3																					1984																												Cr3Si(A15)																	Cr3Si, A15	K		5.5					5.5																				kOe	using WHH.	54.1				15.1		4.4	T/K		1.4			MHC40829																						mj/cm3.K2	0.73																																							arc-melting					Superconductivity and upper critical field studies on A-15 superconducting Ti3Sb compound				Solid State Commun., 52(1984)641	S.Ramkrishnan,A.K.Nigam,Girish Chandra		
40830	SSC0520641	annealed at 850 K. GAMMA from Junod et al.	Ti3Sb	Sb1Ti3	Sb	1	Ti	3																					1984																												Cr3Si(A15)			A	5.2218													Cr3Si, A15	K		6.5					6.5																				kOe	using WHH.	52				19.2		4.4	T/K		1.16			MHC40829																						mj/cm3.K2	0.8																																							arc-melting					Superconductivity and upper critical field studies on A-15 superconducting Ti3Sb compound				Solid State Commun., 52(1984)641	S.Ramkrishnan,A.K.Nigam,Girish Chandra		
40831	SSC0390773	spin-orbit parameter = 0.1 from fitting Hc2(T).	V1-xGax	Ga0.205V0.795	Ga	0.205	V	0.795																				1	1981																												Cr3Si(A15)			A	4.814													Cr3Si, A15	K		9.7				0.22	9.7																				T		13							T/K		4.3			MHC40831																																																														arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40832	SSC0390773	spin-orbit parameter = 0.2 from fitting Hc2(T).	V1-xGax	Ga0.222V0.778	Ga	0.222	V	0.778																				1	1981																												Cr3Si(A15)			A	4.815													Cr3Si, A15	K		12.3				0.45	12.3																				T		17.8							T/K		4.3			MHC40831																																																														arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40833	SSC0390773	spin-orbit parameter = 0.3 from fitting Hc2(T).	V1-xGax	Ga0.236V0.764	Ga	0.236	V	0.764																				1	1981																												Cr3Si(A15)			A	4.816													Cr3Si, A15	K		14.6				0.48	14.6																				T		22.3							T/K		4.3			MHC40831																																																														arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40834	SSC0390773	spin-orbit parameter = 0.25 from fitting Hc2(T).	V1-xGax	Ga0.248V0.752	Ga	0.248	V	0.752																				1	1981																												Cr3Si(A15)																	Cr3Si, A15	K		15.1				0.23	15.1																				T		22.5							T/K		4.3																																																																	arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40835	SSC0390773	spin-orbit parameter = 0.3 from fitting Hc2(T).	V1-xGax	Ga0.253V0.747	Ga	0.253	V	0.747																				1	1981																												Cr3Si(A15)			A	4.819													Cr3Si, A15	K		14.9				1.3	14.9																				T		22.8							T/K		4.3																																																																	arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40836	SSC0390773	spin-orbit parameter = 0.25 from fitting Hc2(T).	V1-xGax	Ga0.265V0.735	Ga	0.265	V	0.735																				1	1981																												Cr3Si(A15)			A	4.82													Cr3Si, A15	K		13.6				0.9	13.6																				T		21.8							T/K		5.5			MHC40836																																																														arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40837	SSC0390773	spin-orbit parameter = 0.3 from fitting Hc2(T).	V1-xGax	Ga0.281V0.719	Ga	0.281	V	0.719																				1	1981																												Cr3Si(A15)			A	4.823													Cr3Si, A15	K		12.2				2.46	12.2																				T		20.3							T/K		5.5																																																																	arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40838	SSC0390773	spin-orbit parameter = 0.25 from fitting Hc2(T).	V1-xGax	Ga0.296V0.704	Ga	0.296	V	0.704																				1	1981																												Cr3Si(A15)			A	4.825													Cr3Si, A15	K		12.1				1.55	12.1																				T		19.4							T/K		5.5																																																																	arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40839	SSC0390773	ordered sample. spin-orbit parameter = 0.3 from fitting Hc2(T).	V1-xGax	Ga0.25V0.75	Ga	0.25	V	0.75																				1	1981																												Cr3Si(A15)																	Cr3Si, A15	K		15.3					15.3																				T		23.4							T/K		4.3			MHC40839																																																														arc-melting. ANN(1400C,6h) - ANN(1100-1200C,24h) - ANN(650C,1w)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
40840	SSC0390959	cubic. sample produced by RCA.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				3	1981																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																				T		29			26			4.2	T/K		2.4			MHC40840																																																																			Upper critical fields of cubic and tetragonal single crystal and polycrystalline Nb3Sn in dc fields to 30 tesra				Solid State Commun., 39(1981)959	S.Foner,E.J.McNiff,Jr		
40841	SSC0390959	tetragonal. RRR = 8. sample produced by RCA	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				3	1981																												Cr3Si(A15)																	Cr3Si, A15	K		17.4					17.4																				T		24			22			4.2	T/K		2			MHC40841																																																																			Upper critical fields of cubic and tetragonal single crystal and polycrystalline Nb3Sn in dc fields to 30 tesra				Solid State Commun., 39(1981)959	S.Foner,E.J.McNiff,Jr		
40842	SSC0390959	tetragonal. RRR = 50. sample used for dHvA effect measurements.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				3	1981																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																				T		20			18			4.2	T/K		1.6			MHC40842																																																																			Upper critical fields of cubic and tetragonal single crystal and polycrystalline Nb3Sn in dc fields to 30 tesra				Solid State Commun., 39(1981)959	S.Foner,E.J.McNiff,Jr		
40843	SSC0390959	tetragonal. polycrystal. sample produced by RCA	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				1	1981																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																				T		25			23			4.2	T/K		2.1			MHC40843																																																																			Upper critical fields of cubic and tetragonal single crystal and polycrystalline Nb3Sn in dc fields to 30 tesra				Solid State Commun., 39(1981)959	S.Foner,E.J.McNiff,Jr		
40844	SSC0390959	cubic. polycrystal. sample produced by NML.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				1	1981																												Cr3Si(A15)																	Cr3Si, A15	K		17.4					17.4																				T		29			26			4.2	T/K		2.4			MHC40844																																																																			Upper critical fields of cubic and tetragonal single crystal and polycrystalline Nb3Sn in dc fields to 30 tesra				Solid State Commun., 39(1981)959	S.Foner,E.J.McNiff,Jr		
40845	SSC0300723	ANN(1800C,10h). GAMMA from Junod et al.	Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1979																												Cr3Si(A15)																	Cr3Si, A15	K		8.7					8.7																				T		12.5			8			4.2	T/K		1.95			MHC40845																						mJ/gat.K2	5.6																																												Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
40846	SSC0300723	ANN(950C, 1 month)	Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1979																												Cr3Si(A15)																	Cr3Si, A15	K		10.9					10.9																																		MHC40845																																																																			Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
40847	SSC0300723	ANN(1500C, 48h). GAMMA from Junod et al.	Nb3Au	Au1Nb3	Au	1	Nb	3																					1979																												Cr3Si(A15)																	Cr3Si, A15	K		10.7					10.7																				T		23.5			18			4.2	T/K		3.2			MHC40847																						mJ/gat.K2	9.3																																												Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
40848	SSC0300723	ANN(1500C,48h + 750C, 10d). GAMMA from Junod et al.	Nb3(Au,Pt)	Nb3Au0.7Pt0.3	Nb	3	Au	0.7	Pt	0.3																			1979																												Cr3Si(A15)																	Cr3Si, A15	K		13					13																				T		29.5			24.6			4.2	T/K		3.3			MHC40848																						mJ/gat.K2	8.5																																												Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
40849	SSC0300723	Heat(1250C) then quenched into water.	Nb3(Au,Pt)	Nb3Au0.7Pt0.3	Nb	3	Au	0.7	Pt	0.3																			1979																												Cr3Si(A15)																	Cr3Si, A15	K		10					10																																		MHC40849																						mJ/g.K2	0.018																																												Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
40850	SSC0190197	polymer. RRR = 70. SP lattice term coeff. = 8.8 E-6 J/g.K4.  compositions and SP-heat data by Phys.Rev.Lett., 34(1975)89.	(SN)x	N0.3S0.7	N	0.3	S	0.7																					1976																																														K		0.29					0.29																				kOe			8.1	0.87										MHC40850		A			3000	135																																																													The upper critical field of superconducting polysulfur nitride, (SN)x				Solid State Commun., 19(1976)197	L.J.Azevedo,W.G.Clark,G.Deutscher,R.L.Greene,G.B.Street,L.J.Suter		
40851	SSC0160341	Hc2 measured by ESR of Gd(dopant). (dC/gamma*Tc) = 3.4. thermodynamic Hc(0) = 1.7 kG. 519.3 g/mol.	LaOs2	La1Os2	La	1	Os	2																					1975																												Laves																	Laves, C15	K		8.9				0.13	8.9																				T		3																										6.1	14							mJ/gat.K2	5.3		163																																					arc-melting in Ar, ANN(1100C)					Superconducting properties of LaOs2				Solid State Commun., 16(1975)341	H.E.Hoenig,K.Baberschke,W.Schrittenlacher		
40852	SSC0360721	Debye-temp. is a function of T. data shows DEBYE-T(0 K). SP of high-Tc materials should be analyze using new model.	V3Si	Si1V3	Si	1	V	3																					1980																												Cr3Si(A15)																	Cr3Si, A15	K		17					17																																																3.77	14							mJ/gat.K2	13.2		297																																										Comment on specific heat of a transforming V3Si crystal				Solid State Commun., 36(1980)721	A.Junod,J.Muller		
40853	SSC0330581	RRR=26. transformation temp. = 20.2K. cubic(T>20.2K), tetragonal(T<20.2 K). For tetragonal, GAMMA=67.6 mJ/mol.K2 and DEBYE-T = 425 K.	V3Si	Si1V3	Si	1	V	3																					1980																												Cr3Si(A15)			A	4.724													Cr3Si, A15	K		16.8				0.07	16.8																																																3.46	14							mJ/mol.K2	5934		465																																					electron beam floating zone refining					Specific heat of a transforming V3Si crystal				Solid State Commun., 33(1980)581	C.C.Huang,A.M.Goldman,L.E.Toth		
40854	PRL0531829	95% single phase	U2PtC2	U2Pt1C2	U	2	Pt	1	C	2																			1984																											2				A	3.52		12.54												K		1.47					1.47																													T/K		9																									mJ/mol.K2	37.7		273																																					arc-melting, then ANN(1300C,3h, in vac)					U2PtC2 and systematics of heavyfermions				Phys.Rev.Lett., 53(1984)1829	G.P.Meisner,A.L.Giorgi,A.C.Lawson,G.R.Stewart,J.O.Willis,M.S.Wire,J.L.Smith		
40855	PR140A1620	sample from Argonne(ANL). Tc = 2.0K at P=10 kbar (from SP-heat)	alpha-U	U1	U	1																							1965																																														K		1					1	MTC40855		K/GPa	1.05																																																							200																																										Pressure dependence of the superconducting transition temperature of uranium				Phys.Rev. A140(1965)1620	T.F.Smith,W.E.Gardner		
40856	L097077003	tunneling //c-axis using STM.	CaC6	C6Ca1	C	6	Ca	1																				3	2006																																														K		10					10																																				A			330							meV	1.6	3.66	11																																															10 days immersion of highly oriented graphite in molten Li-Ca alloy (350C).					Scanning Tunneling Spectroscopy on the Novel Superconductor CaC6			Institut des Nanosciences de Paris, Universites Paris 6 et 7, UMR 7588 au CNRS, 140 rue de Lourmel, 75015 Paris, France	Phys.Rev.Lett., 97(2006)077003	N.Bergeal,V.Dubost,Y.Noat,W.Sacks,D.Roditchev,N.Emery,C.Herold,J-F.Mareche,P.Lagrange,G.Loupias		
40857	L097107001	SC for x > 0.05 in LixZrNCl.	LixZrNCl	Li0.06Zr1N1Cl1	Li	0.06	Zr	1	N	1	Cl	1																	2006																																														K		15.2					15.2	MTC40857																																																																																																				Increase in Tc upon Reduction of Doping in LixZrNCl Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 97(2006)107001	Y.Taguchi,A.Kitora,Y.Iwasa		
40858	L097107001		LixZrNCl	Li0.1Zr1N1Cl1	Li	0.1	Zr	1	N	1	Cl	1																	2006																																														K																																																																																																												Increase in Tc upon Reduction of Doping in LixZrNCl Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 97(2006)107001	Y.Taguchi,A.Kitora,Y.Iwasa		
40859	SSC1390334	not SC. Solubility limit of Mn = 0.3 in (Ru1-xMnx). hole conc. = 0.0824 from thermopower.	(Gd,Ce)2Sr2(Ru,Mn)Cu2O10	Gd1.4Ce0.6Sr2Ru0.99Mn0.01Cu2O10	Gd	1.4	Ce	0.6	Sr	2	Ru	0.99	Mn	0.01	Cu	2									O	10		1	2006																												Ru1222			A			28.551												K					4.2																																																																									mOhm.cm											121.3												Gd2O3,CeO2,SrCO3,CuO,MnO2	1	mixture - heat (1000C,24h,in air) - ANN(1050C,48h, in O2)					Effect of Mn substitution on the delicate balance between structure and properties of Gd1.4Ce0.6Sr2RuCu2O10			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 139(2006)334	S.Kalavathi,J.Janaki,T.N.Sairam,Awadhesh Mani,R.Rawat,V.Sankara Sasty		
40860	PHC4430057	0.4=< x =<0.7 in (TlxPb0.5) were investigated.	(Tl,Pb)(Ba,Sr)2(Ca,Gd)Cu2Oz	Tl0.5Pb0.5Ba0.1Sr1.9Ca0.8Gd0.2Cu2Oz	Tl	0.5	Pb	0.5	Ba	0.1	Sr	1.9	Ca	0.8	Gd	0.2	Cu	2							O	z		1	2006																												Tl1212			A	3.809		12.117												K	98						98																																																																																																wet malic acid gel technique.					Under- and over-doped bulk (TlaPb0.5)(Sr0.95Ba0.05)2(Ca0.8Gd0.2)Cu2Oz 1212 superconductors prepared via solution gel synthesis			Institute for Chemical Technology of Inorganic Materials, Johannes Kepler University, A 4040 Linz, Austria	Physica C, 443(2006)57	H.Sudra,G.Gritzner		
40861	PHC4490053	Jc(B) was measured at various temperature.	MgB2	B2Mg1	B	2	Mg	1																				1	2006																												AlB2			A	3.0859		3.5263											AlB2, C32	K				38.5			38.5																																																																																														Mg,Al,B		solid state reaction using 100nm Al powder. 3 wt% extra Mg was added to compensate for its loss.					Investigation on MgB2 superconductor doped by nano-Al powder			School of Material Science and Engineering, Zhengzhou University, No. 97, Wenhua Road, Zhengzhou, Henan 450002, People's Republic of China	Physica C, 449(2006)53	H.L.Xu,Y.Feng,Y.Zhao,G.Yan,M.H.Pu,H.X.Lu,R.Zhang,Z.Xu		
40862	PHC4490053	Jc(B) was measured at various temperature.	(Mg,Al)B2	Mg0.99Al0.01B2	Mg	0.99	Al	0.01	B	2																		1	2006																												AlB2			A	3.0856		3.5237											AlB2, C32	K				38			38																																																																																														Mg,Al,B		solid state reaction using 100nm Al powder. 3 wt% extra Mg was added to compensate for its loss.					Investigation on MgB2 superconductor doped by nano-Al powder			School of Material Science and Engineering, Zhengzhou University, No. 97, Wenhua Road, Zhengzhou, Henan 450002, People's Republic of China	Physica C, 449(2006)53	H.L.Xu,Y.Feng,Y.Zhao,G.Yan,M.H.Pu,H.X.Lu,R.Zhang,Z.Xu		
40863	PHC4490053	Jc(B) was measured at various temperature.	(Mg,Al)B2	Mg0.98Al0.02B2	Mg	0.98	Al	0.02	B	2																		1	2006																												AlB2			A	3.0859		3.5236											AlB2, C32	K				37.5			37.5																																																																																														Mg,Al,B		solid state reaction using 100nm Al powder. 3 wt% extra Mg was added to compensate for its loss.					Investigation on MgB2 superconductor doped by nano-Al powder			School of Material Science and Engineering, Zhengzhou University, No. 97, Wenhua Road, Zhengzhou, Henan 450002, People's Republic of China	Physica C, 449(2006)53	H.L.Xu,Y.Feng,Y.Zhao,G.Yan,M.H.Pu,H.X.Lu,R.Zhang,Z.Xu		
40864	PHC4490053	Jc(B) was measured at various temperature.	(Mg,Al)B2	Mg0.95Al0.05B2	Mg	0.95	Al	0.05	B	2																		1	2006																												AlB2			A	3.0833		3.5179											AlB2, C32	K				36.5			36.5																																																																																														Mg,Al,B		solid state reaction using 100nm Al powder. 3 wt% extra Mg was added to compensate for its loss.					Investigation on MgB2 superconductor doped by nano-Al powder			School of Material Science and Engineering, Zhengzhou University, No. 97, Wenhua Road, Zhengzhou, Henan 450002, People's Republic of China	Physica C, 449(2006)53	H.L.Xu,Y.Feng,Y.Zhao,G.Yan,M.H.Pu,H.X.Lu,R.Zhang,Z.Xu		
40865	PHC4490053	Jc(B) was measured at various temperature.	(Mg,Al)B2	Mg0.92Al0.08B2	Mg	0.92	Al	0.08	B	2																		1	2006																												AlB2			A	3.083		3.5112											AlB2, C32	K				35.5			35.5																																																																																														Mg,Al,B		solid state reaction using 100nm Al powder. 3 wt% extra Mg was added to compensate for its loss.					Investigation on MgB2 superconductor doped by nano-Al powder			School of Material Science and Engineering, Zhengzhou University, No. 97, Wenhua Road, Zhengzhou, Henan 450002, People's Republic of China	Physica C, 449(2006)53	H.L.Xu,Y.Feng,Y.Zhao,G.Yan,M.H.Pu,H.X.Lu,R.Zhang,Z.Xu		
40866	P074092502	Co-valence = 3.48. Hc2 is lower than Pauli limit.	NaxCoO2/yH2O	Na0.346Co1H2.6O3.3	Na	0.346	Co	1	H	2.6															O	3.3			2006																															A			19.692												K				4.81			4.81	TC40866																																																																																															final process (NaOH aqueous solution)					Valence and Na content dependences of superconductivity in NaxCoO2:yH2O			National Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 74(2006)092502	H.Sakurai,N.Tsujii,O.Suzuki,H.Kitazawa,G.Kido,K.Takada,T.Sasaki,E.Takayama-Muromachi		
40867	P074092502	Co-valence = 3.48. Hc2 is higher than Pauli limit.	NaxCoO2/yH2O	Na0.38Co1H2.6O3.3	Na	0.38	Co	1	H	2.6															O	3.3			2006																															A			19.588												K				2.8			2.8	TC40866																																																																																															final process (NaOH aqueous solution)					Valence and Na content dependences of superconductivity in NaxCoO2:yH2O			National Institute for Materials Science, Namiki 1-1, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 74(2006)092502	H.Sakurai,N.Tsujii,O.Suzuki,H.Kitazawa,G.Kido,K.Takada,T.Sasaki,E.Takayama-Muromachi		
40868	P070144516	Hc2(0) = 5.2 T estimated from lower field region.	NaxCoO2/yH2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3		1	2004																																														K				4.345			4.345																				T	WHH	28												HC40868																																																														Na0.7CoO2 - Na removed by Br - washed with acetonitrile - water air dry					Possible singlet-to-triplet pairing transition in NaxCoO2:yH2O			Department of Theoretical Physics, Institute of Physics, 40-007 Katowice, Poland	Phys.Rev.B, 70(2004)144516	M.M.Maska,M.Mierzejewski,B.Andrzejewski,M.L.Foo,R.J.Cava,T.Klimczuk		
40869	P072060512	not SC. Schottky term(alpha) = 258.1 mJ.K2/mol.	NaxCoO2	Na0.74Co1O2	Na	0.74	Co	1																	O	2	2	3	2005																																														K					0.4																																																										mJ/mol.K2	34.05	SP-heat	328.2																																					single crystal(using flux method). Na-content obtained by controlling deintercalated time.					Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40870	P072060512	not SC. Schottky term(alpha) = 19.44 mJ.K2/mol.	NaxCoO2	Na0.72Co1O2	Na	0.72	Co	1																	O	2	2	3	2005																																														K					0.4																																																										mJ/mol.K2	32.91	SP-heat	453.6																																					single crystal(using flux method). Na-content obtained by controlling deintercalated time.					Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40871	P072060512	not SC. Schottky term(alpha) = 11.59 mJ.K2/mol.	NaxCoO2	Na0.48Co1O2	Na	0.48	Co	1																	O	2	2	3	2005																																														K					0.4																																																										mJ/mol.K2	8.231	SP-heat	257.4																																					single crystal(using flux method). Na-content obtained by controlling deintercalated time.					Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40872	P072060512	not SC. Schottky term(alpha) = 3.410 mJ.K2/mol.	NaxCoO2	Na0.35Co1O2	Na	0.35	Co	1																	O	2	2	3	2005																																														K					0.4																																																										mJ/mol.K2	12.11	SP-heat	319																																					single crystal(using flux method). Na-content obtained by controlling deintercalated time.					Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40873	P072060512	not SC. Schottky term(alpha) = 0.5174 mJ.K2/mol.	NaxCoO2	Co1O2	Co	1																			O	2	2	3	2005																																														K					0.4																																																										mJ/mol.K2	13.33	SP-heat	559.1																																					single crystal(using flux method). Na-content obtained by controlling deintercalated time.					Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40874	P072060512	Tc defined as midpoint in SP-jump. (dC) = 45.5 mJ/mol.K. (dC/gamma*Tc) = 0.71	NaxCoO2/yH2O	Na0.35Co1H1.4O2	Na	0.35	Co	1	H	1.4															O	2	2	3	2005																																														K		4.7					4.7																				T		17.1							T/K		5.3			HC40874		A		44																		mJ/mol.K2	13.7	SP-heat																																											Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40875	P072060512	Tc defined as midpoint in SP-jump.	NaxCoO2/yD2O	Na0.35Co1D1.4O2	Na	0.35	Co	1	D	1.4															O	2	2	3	2005																																														K		4.7					4.7																				T		17.1							T/K		5.3			HC40874		A		44																		mJ/mol.K2	13.3	SP-heat																																											Dependence of the specific heat of NaxCoO2:yH2O/D2O on sodium and water concentrations			Condensed Matter Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 72(2005)060512	R.Jin,B.C.Sales,S.Li,D.Mandrus		
40876	PCS0670590	anisotropy factor = 4.3 (Hc2 anisotropy)	NaxCoO2/yH2O	Na0.35Co1H1.3O3.3	Na	0.35	Co	1	H	1.3															O	3.3		3	2006																															A			19.613												K		3.7					3.7											A	ellipsoidal fitting			19.1					T	WHH		15.6	3.6					T/K			6.12	1.41																																																															Na0.7CoO2 single crystal by traveling zone method - Br2/CH3CN solution for 28.5h - H2O for 135h					Anisotropy of Na0.35CoO2/1.3H2O superconductor			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai 980-8577, Japan	J.Phys.Chem.Solids, 67(2006)590	P.Badica,T.Kondo,K.Togano,K.Yamada		
40877	P074100506	as-prepared	Sr2CuO3+z	Sr2Cu1O3.4	Sr	2	Cu	1																	O	3+z	3.4	1	2006																											2	T	I4/mmm		A	3.795		12.507												K				75			75																																																																																														SrO2,CuO		high pressure synthesis(6GPa,1100C,1h) using SrO2 as an oxidizer.					Enhancement of the superconducting critical temperature of Sr2CuO3+z up to 95 K by ordering dopant atoms			Institute of Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)100506R	Q.Q.Liu,H.Yang,X.M.Qin,Y.Yu,L.X.Yang,F.Y.Li,R.C.Yu,C.Q.Jin,S.Uchida		
40878	P074100506	ANN(250C). Apical O is ordered.	Sr2CuO3+z	Sr2Cu1O3.4	Sr	2	Cu	1																	O	3+z	3.4	1	2006																											2	T																		K				95			95																																																																																														SrO2,CuO		high pressure synthesis(6GPa,1100C,1h) using SrO2 as an oxidizer.					Enhancement of the superconducting critical temperature of Sr2CuO3+z up to 95 K by ordering dopant atoms			Institute of Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 74(2006)100506R	Q.Q.Liu,H.Yang,X.M.Qin,Y.Yu,L.X.Yang,F.Y.Li,R.C.Yu,C.Q.Jin,S.Uchida		
40879	P074100508	TP300<ab> is at 280K.	(Y,La)(Ba,La)2Cu3Oz	Y0.38Ba1.74La0.88Cu3O6.95	Y	0.38	Ba	1.74	La	0.88	Cu	3													O	z	6.95	3	2006																											2	Y123			A	3.901		11.763												K	25						25																																																																		uV/K			38	TP40879																										flux method using Y2O3 crucible. then ANN(485C,1 atm O2,7d)					Doping n-type carriers by La substitution for Ba in the YBa2Cu3Oy system			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 74(2006)100508R	K.Segawa,Y.Ando		
40880	P074100508	TP300<ab> is at 280K.	(Y,La)(Ba,La)2Cu3Oz	Y0.38Ba1.74La0.88Cu3O6.21	Y	0.38	Ba	1.74	La	0.88	Cu	3													O	z	6.21	3	2006																												Y123																		K					4.2																																																																				uV/K			-70.6	TP40880															cm3/C			-0.0275			RH40880					flux method using Y2O3 crucible. then ANN(890C,6h, in 2E-5 atm O2)					Doping n-type carriers by La substitution for Ba in the YBa2Cu3Oy system			Central Research Institute of Electric Power Industry, Komae, Tokyo 201-8511, Japan	Phys.Rev.B, 74(2006)100508R	K.Segawa,Y.Ando		
40881	NAT3890164		Sr3Cu2O5Cl	Sr3Cu2Cl1O5	Sr	3	Cu	2	Cl	1															O	5			1997																															A	3.907		22.53												K				70			70																																																																																																(Sr2CuO3 +KCl3) in Au-capsule, high-pressure synthesis (60 kbar, 950C,3h)					Application of scanning SQUID petrology to high-pressure materials science			Colombia University,USA	Nature, 389(1997)164	B.A.Scott,J.R.Kirtley,D.Walker,B-H.Chen,Y.Wang		
40882	PHC2600249	O-content by TGA. oz=3.14 by iodometric titration. O-vacancy located in CuO2 layer.	(Sr,Ba)2CuO4	Sr0.8Ba1.2Cu1O3.35	Sr	0.8	Ba	1.2	Cu	1															O	3+z	3.35		1996																												T			A	3.8988		12.815												K				50			50										2																																																																																						Sr2CuO2(CO3) + Ba2CuO2(CO3),  ANN(240C,15h, in N2)					Observation of superconductivity(Tc=50 K)in a new tetragonal alkaline-earth cuprate Sr0.8Ba1.2CuO3+z,synthesised at ambient preesure			School of Chemistry, University of Birmingham, Birmingham B15 2TT, UK	Physica.C,260(1996)249-256	C. Greaves,G. Van tendeloo,J.P. Hodges,M. Slaski,P.P. Edwards,P.R. Slater		
40883	PR0212717	collidine-intercalated TaS2. M = collidine.	TaS2(collidine)(1/6)	S2Ta1	S	2	Ta	1																				3	1980																												TX2																	2H-type	K		3.2				0.2	3.2																													T/K			10	0.33			A			180	6																																																								mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40884	PR0212717	Pyridine-intercalated TaS2. M = pyridine.	TaS2(pyridine)(1/2)	Ta1S2M0.167	Ta	1	S	2	M	0.167																		3	1980																												TX2																	2H-type	K		3.47				0.2	3.47																													T/K			7	0.28	MHC40884		A			183	7.3																mJ/mol.K2	9.1	calculated from (dHc2/dT)																																						mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40885	PR0212717	Aniline-intercalated TaS2. M = Aniline.	TaS2(aniline)(3/4)	Ta1S2M0.5	Ta	1	S	2	M	0.5																		3	1980																												TX2																	2H-type	K		2.9				0.2	2.9																													T/K			9.6	0.26	MHC40885		A			209	5.6																																																								mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40886	PR0212717		Ta(S,Se)2	Ta1S1.6Se0.4	Ta	1	S	1.6	Se	0.4																		3	1980																												TX2																	4H-type	K		4.1				0.07	4.1																													T/K			4.4	0.8			A			100	18.2																mJ/mol.K2	11.2	calculated from (dHc2/dT)																																						mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40887	PR0212717	collidine-intercalated TaS1.6Se0.4. M = collidine.	Ta(S,Se)2(collidine)(1/6)	Ta1S1.6Se0.4M0.167	Ta	1	S	1.6	Se	0.4	M	0.167																3	1980																												TX2																	4H-type	K		2.6				0.19	2.6																													T/K			24	0.34	MHC40887		A			193	2.8																																																								mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40888	PR0212717	Pyridine-intercalated TaS1.6Se0.4. M = pyridine.	Ta(S,Se)2(pyridine)(1/2)	Ta1S1.6Se0.4M0.5	Ta	1	S	1.6	Se	0.4	M	0.5																3	1980																												TX2																	4H-type	K		2.1				0.13	2.1																													T/K			22.5	0.3			A			228	3																mJ/mol.K2	9.3	calculated from (dHc2/dT)																																						mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40889	PR0212717		NbSe2	Nb1Se2	Nb	1	Se	2																				3	1980																												TX2																	2H-type	K		7.1				0.07	7.1																													T/K			2.3	0.8			A			76	26																mJ/mol.K2	16.5	calculated from (dHc2/dT)																																						mother crystals grown at 700-1000C. intercalation by reacting at 150-200 C for 1-4 weeks in sealed quartz tube.					Upper critical fields and reduced dimensionality of the superconducting layered compounds			Yale University, USA	Phys. Rev.B, 21(1980)2717	D.E.Prober,R.E.Schwall,M.R.Beasley		
40890	P074134506	magnetic moment measured	RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.2Ce0.8Cu2O10+z	Ru	1	Sr	2	Eu	1.2	Ce	0.8	Cu	2											O	10+z		1	2006																												Ru1222																		K			38			27	38																																																																																																					Superconducting and magnetic properties of Ru1-yMySr2Eu2-xCexCu2O10+z (M=Nb, Sn)			The MacDiarmid Institute for Advanced Materials and Nanotechnology, Industrial Research, Lower Hutt, New Zealand	Phys.Rev.B, 74(2006)134506	S.K.Goh,G.V.M.Williams,E.K.Hemery,H.K.Lee		
40891	P074134506	magnetic moment measured	(Ru,Sn)Sr2(Eu,Ce)2Cu2O10	Ru0.9Sn0.1Sr2Eu1.2Ce0.8Cu2O10+z	Ru	0.9	Sn	0.1	Sr	2	Eu	1.2	Ce	0.8	Cu	2									O	10+z		1	2006																												Ru1222																		K			34.6			24	34.6																																																																																																					Superconducting and magnetic properties of Ru1-yMySr2Eu2-xCexCu2O10+z (M=Nb, Sn)			The MacDiarmid Institute for Advanced Materials and Nanotechnology, Industrial Research, Lower Hutt, New Zealand	Phys.Rev.B, 74(2006)134506	S.K.Goh,G.V.M.Williams,E.K.Hemery,H.K.Lee		
40892	P074134506	magnetic moment measured	(Ru,Sn)Sr2(Eu,Ce)2Cu2O10	Ru0.8Sn0.2Sr2Eu1.2Ce0.8Cu2O10+z	Ru	0.8	Sn	0.2	Sr	2	Eu	1.2	Ce	0.8	Cu	2									O	10+z		1	2006																												Ru1222																		K			37			5	37																																																																																																					Superconducting and magnetic properties of Ru1-yMySr2Eu2-xCexCu2O10+z (M=Nb, Sn)			The MacDiarmid Institute for Advanced Materials and Nanotechnology, Industrial Research, Lower Hutt, New Zealand	Phys.Rev.B, 74(2006)134506	S.K.Goh,G.V.M.Williams,E.K.Hemery,H.K.Lee		
40893	PHC4450084	Tc, thermopower measured for 0.2 =< x =< 0.8 in Bi2Sr2-xLaxCuOz. La-content not given. Tc vs S(290K) shown in figure.	Bi2(Sr,La)2CuOz	Bi2Sr1.6La0.4Cu1Oz	Bi	2	Sr	1.6	La	0.4	Cu	1													O	z		3	2006																												Bi2201																		K		33					33	TC40893																																																																	uV/K	17																													single crystals grown by FZ method					R dependence of superconductivity and thermopower in the Bi2Sr2-xRxCuOy (R = La, Sm and Eu) system			Department of Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan	Physica C, 445-448(2006)84	Y.Okada,H.Ikuta		
40894	PHC4450084	Tc, thermopower measured for 0.2 =< x =< 0.8 in Bi2Sr2-xSmxCuOz. Sm-content not given. Tc vs S(290K) shown in figure.	Bi2(Sr,LSm2CuOz	Bi2Sr1.6Sm0.4Cu1Oz	Bi	2	Sr	1.6	Sm	0.4	Cu	1													O	z		3	2006																												Bi2201																		K		23					23	TC40894																																																																																															single crystals grown by FZ method					R dependence of superconductivity and thermopower in the Bi2Sr2-xRxCuOy (R = La, Sm and Eu) system			Department of Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan	Physica C, 445-448(2006)84	Y.Okada,H.Ikuta		
40895	PHC4450084	Tc, thermopower measured for 0.2 =< x =< 0.8 in Bi2Sr2-xEuxCuOz. Eu-content not given. Tc vs S(290K) shown in figure.	Bi2(Sr,Eu)2CuOz	Bi2Sr1.6Eu0.4Cu1Oz	Bi	2	Sr	1.6	Eu	0.4	Cu	1													O	z		3	2006																												Bi2201																		K		15.5					15.5	TC40895																																																																																															single crystals grown by FZ method					R dependence of superconductivity and thermopower in the Bi2Sr2-xRxCuOy (R = La, Sm and Eu) system			Department of Crystalline Materials Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8603, Japan	Physica C, 445-448(2006)84	Y.Okada,H.Ikuta		
40896	PCS0672144	cubic anvil high-P (7.5 GPa). Neel-T = 50 K at P = 0.5 GPa. dTc increases with increasing P.	CeRu2	Ce1Ru2	Ce	1	Ru	2																				1	2006																												MgCu2(Laves)			A	7.544													MgCu2,C15	K				6.3		0.2	6.3	MTC40896		K/GPa	0.1																																																																																												arc-melting, degass(800C, in vac), ANN(1100C,12d)					Signature of pressure-induced phase separation in Ce1-xLaxRu2 system			Department of Physics, Okayama University, 3-1-1 Tsushima-Naka, Okayama 700-8530, Japan	J.Phys.Chem.Solids, 67(2006)2144	F.Ono,N.Q.Sun,Y.Matsushima,N.L.Saini		
40897	PCS0672144	cubic anvil high-P (7.5 GPa). Neel-T = 80 K at P = 0.5 GPa. dTc increases with increasing P.	(Ce,La)Ru2	Ce0.91La0.09Ru2	Ce	0.91	La	0.09	Ru	2																		1	2006																												MgCu2(Laves)			A	7.555													MgCu2,C15	K				5.25		0.7	5.25	MTC40897		K/GPa	0.033																																																																																												arc-melting, degass(800C, in vac), ANN(1100C,12d)					Signature of pressure-induced phase separation in Ce1-xLaxRu2 system			Department of Physics, Okayama University, 3-1-1 Tsushima-Naka, Okayama 700-8530, Japan	J.Phys.Chem.Solids, 67(2006)2144	F.Ono,N.Q.Sun,Y.Matsushima,N.L.Saini		
40898	P070094509	EXAFS measured	CeRu2	Ce1Ru2	Ce	1	Ru	2																				1	2004																												MgCu2(Laves)			A	7.544													MgCu2,C15	K		6.17					6.17																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40899	P070094509		(Ce,La)Ru2	Ce0.97La0.03Ru2	Ce	0.97	La	0.03	Ru	2																		1	2004																												MgCu2(Laves)			A	7.547													MgCu2,C15	K		6.45					6.45																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40900	P070094509		(Ce,La)Ru2	Ce0.94La0.06Ru2	Ce	0.94	La	0.06	Ru	2																		1	2004																												MgCu2(Laves)			A	7.551													MgCu2,C15	K		6.55					6.55	MTC40900																																																																																															arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40901	P070094509	EXAFS measured	(Ce,La)Ru2	Ce0.91La0.09Ru2	Ce	0.91	La	0.09	Ru	2																		1	2004																												MgCu2(Laves)			A	7.555													MgCu2,C15	K		6.57					6.57																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40902	P070094509		(Ce,La)Ru2	Ce0.88La0.12Ru2	Ce	0.88	La	0.12	Ru	2																		1	2004																												MgCu2(Laves)			A	7.561													MgCu2,C15	K		6.14					6.14																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40903	P070094509	EXAFS measured	(Ce,La)Ru2	Ce0.85La0.15Ru2	Ce	0.85	La	0.15	Ru	2																		1	2004																												MgCu2(Laves)			A	7.565													MgCu2,C15	K		5.35					5.35																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40904	P070094509	EXAFS measured	(Ce,La)Ru2	Ce0.8La0.2Ru2	Ce	0.8	La	0.2	Ru	2																		1	2004																												MgCu2(Laves)			A	7.573													MgCu2,C15	K		4.77					4.77																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40905	P070094509	EXAFS measured	(Ce,La)Ru2	Ce0.25La0.75Ru2	Ce	0.25	La	0.75	Ru	2																		1	2004																												MgCu2(Laves)			A	7.671													MgCu2,C15	K		1.42					1.42																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
40906	JPS0641471	H-T phase diagram from ac-SUS.	CeRu2	Ce1Ru2	Ce	1	Ru	2																				1	1995																												MgCu2(Laves)																	MgCu2,C15	K				6.2			6.2																																		MHC40906																																				TP40906																								Ce(4N),Ru(3N)		arc-melting, ANN(1000C,1w)					Evidence of multiple superconducting phases in CeRu2			University of Ryukyus,Okinawa,Japan	J.Phys.Soc.Jpn, 64(2995)1471	T.Nakama,M.Hedo,T.Maekawa,M.Higa,R.Resel,H.Sugawara,R.Settai,Y.Onuki,K.Yagasaki		
40907	MMM1770425	Tc by ac-SUS. (dTc/dP) = +0.33 K/GPa for 0.5 < P =< 1 GPa. large softening of transverse stiffness (C11-C12)/2.	CeRu2	Ce1Ru2	Ce	1	Ru	2																					1998																												MgCu2(Laves)																	MgCu2,C15	K		6.28					6.28	MTC40907		K/GPa	-0.47																																																																																												arc-melting					Pressure effect on superconducting transition temperature of Cel-xLaxRu2			College of Science, University of the Ryukyus, Nishihara, Okinawa 903-01, Japan	J.Mag.Mag.Mat., 177-181(1998)425	T.Nakama,Y.Uwatoko,T.Kohama,A.T.Burkov,Y.Yamaguchi,H.Yoshida,S.Abe,T.Kaneko,N.Mori,K.Yagasaki		
40908	MMM1770425		(Ce,La)Ru2	Ce0.97La0.03Ru2	Ce	0.97	La	0.03	Ru	2																			1998																												MgCu2(Laves)																	MgCu2,C15	K		5.89					5.89			K/GPa	-0.31																																																																																												arc-melting					Pressure effect on superconducting transition temperature of Cel-xLaxRu2			College of Science, University of the Ryukyus, Nishihara, Okinawa 903-01, Japan	J.Mag.Mag.Mat., 177-181(1998)425	T.Nakama,Y.Uwatoko,T.Kohama,A.T.Burkov,Y.Yamaguchi,H.Yoshida,S.Abe,T.Kaneko,N.Mori,K.Yagasaki		
40909	PHB2810088	Ta in Figure shows temperature of an abrupt decrease in R(T), new phase appears.	CeRu2	Ce1Ru2	Ce	1	Ru	2																					2000																												MgCu2(Laves)																	MgCu2,C15	K		6.23					6.23	MTC40909		K/GPa	0.23																																																																																												arc-melting					Pressure-induced structural-phase transition of CeRu2			Department of Physics, University of the Ryukyus, Senbaru, Nishihara-cho, Okinawa 903-0213, Japan	Physica B, 281-282(2000)88	M.Hedo,T.Nakama,A.T.Burkov,K.Yagasaki,Y.Uwatoko,H.Takahashi,T.Nakanishi,N.Mori		
40910	P074134512	Hall number = 0.921E+20/cm3. G-L = 48. thermodynamical Hc = 57 Oe.  For PbTe, Debye-T = 168 K.	(Pb,Tl)Te	Pb0.989Tl0.011Te1	Pb	0.989	Tl	0.011	Te	1																		3	2006																												NaCl																		K		1.16					1.16											Oe	from Hc, GL	3							T	WHH approx.	0.39												MHC40910		A	from Hc2	290			um	from PENET(London)	1.4													mJ/mol.K2	0.511																																							grown by an unseeded physical vapor transport method					Type II superconducting parameters of Tl-doped PbTe determined from heat capacity and electronic transport measurements			Department of Materials Science and Engineering and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 74(2006)134512	Y.Matsushita,P.A.Wianecki,A.T.Sommer,T.H.Geballe,I.R.Fisher		
40911	P074134512	Hall number = 1.067 E+20/cm3. G-L = 79. thermodynamical Hc = 54 Oe. (dC/gamma*Tc) = 1.55.	(Pb,Tl)Te	Pb0.986Tl0.014Te1	Pb	0.986	Tl	0.014	Te	1																		3	2006																												NaCl																		K		1.38					1.38											Oe	from Hc, GL	2							T	WHH approx.	0.6												MHC40910		A	from Hc2	240			um	from PENET(London)	1.9														0.782																																							grown by an unseeded physical vapor transport method					Type II superconducting parameters of Tl-doped PbTe determined from heat capacity and electronic transport measurements			Department of Materials Science and Engineering and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 74(2006)134512	Y.Matsushita,P.A.Wianecki,A.T.Sommer,T.H.Geballe,I.R.Fisher		
40912	P074134513	not SC. RRR = 10.5.	PrNi2B2C	Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																3	2006																												LuNi2B2C			A	3.6996		9.9885												K					2																																																																									uOhm.cm								3.6																	rf-induction furnace.					Isomorphous PrT2B2C (T=Co,Ni,Pt)  single crystals: Structural, transport, and magnetic properties			Centro de Ciencias de la Materia Condensada, Universidad Nacional Autonoma de Mexico, AP 2681, Ensenada 22800, B. C., Mexico	Phys.Rev.B, 74(2006)134513	A.Duran,S.Bernes,R.Falconi,R.Escudero,O.Laborde,M.Guillot		
40913	P074134513	not SC. RRR = 32	PrCo2B2C	Pr1Co2B2C1	Pr	1	Co	2	B	2	C	1																3	2006																												LuNi2B2C			A	3.6156		10.3507												K					2																																																																									uOhm.cm								1.7																	rf-induction furnace.					Isomorphous PrT2B2C (T=Co,Ni,Pt)  single crystals: Structural, transport, and magnetic properties			Centro de Ciencias de la Materia Condensada, Universidad Nacional Autonoma de Mexico, AP 2681, Ensenada 22800, B. C., Mexico	Phys.Rev.B, 74(2006)134513	A.Duran,S.Bernes,R.Falconi,R.Escudero,O.Laborde,M.Guillot		
40914	P074134513	RRR = 5.5.	PrPt2B2C	Pr1Pt2B2C1	Pr	1	Pt	2	B	2	C	1																3	2006																												LuNi2B2C			A	3.8373		10.761												K		6					6																				kOe			12.003	10.845					kOe/K			2.986	2.698	MHC40914		A			165	175	A			2722	2871																										uOhm.cm								2.4																	rf-induction furnace.					Isomorphous PrT2B2C (T=Co,Ni,Pt)  single crystals: Structural, transport, and magnetic properties			Centro de Ciencias de la Materia Condensada, Universidad Nacional Autonoma de Mexico, AP 2681, Ensenada 22800, B. C., Mexico	Phys.Rev.B, 74(2006)134513	A.Duran,S.Bernes,R.Falconi,R.Escudero,O.Laborde,M.Guillot		
40915	PHB3830076	not SC. Chemical analysis, Si-content x = 0.19 by EPMA.	La(Al,Si)2	La1Al1.85Si0.15	La	1	Al	1.85	Si	0.15																			2006																												AlB2			A	4.9254		4.3864											AlB2, C32,	K					2																																																																																																		arc-melting					Lattice constants and electrical resistivity of C32-type LaAl2-xSix (0.27 =< x =< 0.56)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 383(2006)76	M.Imai,H.Abe,T.Aoyagi,T.Kimura		
40916	PHB3830076	not SC. Chemical analysis, Si-content x = 0.27 by EPMA.	La(Al,Si)2	La1Al1.75Si0.25	La	1	Al	1.75	Si	0.25																			2006																												AlB2			A	4.4042		4.3958											AlB2, C32,	K					2																																																																																																		arc-melting					Lattice constants and electrical resistivity of C32-type LaAl2-xSix (0.27 =< x =< 0.56)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 383(2006)76	M.Imai,H.Abe,T.Aoyagi,T.Kimura		
40917	PHB3830076	not SC. Chemical analysis, Si-content x = 0.42 by EPMA.	La(Al,Si)2	La1Al1.64Si0.36	La	1	Al	1.64	Si	0.36																			2006																												AlB2			A	4.372		4.4093											AlB2, C32,	K					2																																																																																																		arc-melting					Lattice constants and electrical resistivity of C32-type LaAl2-xSix (0.27 =< x =< 0.56)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 383(2006)76	M.Imai,H.Abe,T.Aoyagi,T.Kimura		
40918	PHB3830076	not SC. Chemical analysis, Si-content x = 0.49 by EPMA.	La(Al,Si)2	La1Al1.55Si0.45	La	1	Al	1.55	Si	0.45																			2006																												AlB2			A	4.35		4.4119											AlB2, C32,	K					2																																																																																																		arc-melting					Lattice constants and electrical resistivity of C32-type LaAl2-xSix (0.27 =< x =< 0.56)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 383(2006)76	M.Imai,H.Abe,T.Aoyagi,T.Kimura		
40919	PHB3830076	not SC. Chemical analysis, Si-content x = 0.56 by EPMA.	La(Al,Si)2	La1Al1.45Si0.55	La	1	Al	1.45	Si	0.55																			2006																												AlB2			A	4.3297		4.4136											AlB2, C32,	K					2																																																																																																		arc-melting					Lattice constants and electrical resistivity of C32-type LaAl2-xSix (0.27 =< x =< 0.56)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 383(2006)76	M.Imai,H.Abe,T.Aoyagi,T.Kimura		
40920	P074144511	Two band analysis. PENET and Hc1(0) show for sigma band. Hc2(0)//ab = Hc2(MgB2) + 21.4 T, Hc2(0)//c = Hc2(MgB2) + 5.76 T.	Mg(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																		3	2006																												AlB2																		K				35.4		2.4	35.4											mT			11	32.6						curve fitting, Hc2(T) by ac-SUS.													MHC40920		A	from Hc2		60	15	A			1327	682																																																			high-pressure synthesis using cubic anvil.					Anisotropic reversible mixed-state properties of superconducting carbon-doped Mg(B1-xCx)2 single crystals			Atomic Institute of the Austrian Universities, 1020 Vienna, Austria	Phys.Rev.B, 74(2006)144511	C.Krutzler,M.Zehetmayer,M.Eisterer,H.W.Weber,N.D.Zhigadlo,J.Karpinski,A.Wisniewski		
40921	P074144511	Two band analysis. PENET and Hc1(0) show for sigma band. Hc2(0)//ab = Hc2(MgB2) + 16.9 T, Hc2(0)//c = Hc2(MgB2) + 6.91 T.	Mg(B,C)2	Mg1B1.868C0.132	Mg	1	B	1.868	C	0.132																		3	2006																												AlB2																		K				33.15		4	33.15											mT			7.45	19.5						curve fitting, Hc2(T) by ac-SUS.															A	from Hc2		58.4	17.9	A			1752	798																																																			high-pressure synthesis using cubic anvil.					Anisotropic reversible mixed-state properties of superconducting carbon-doped Mg(B1-xCx)2 single crystals			Atomic Institute of the Austrian Universities, 1020 Vienna, Austria	Phys.Rev.B, 74(2006)144511	C.Krutzler,M.Zehetmayer,M.Eisterer,H.W.Weber,N.D.Zhigadlo,J.Karpinski,A.Wisniewski		
40922	P074144511	Two band analysis. PENET and Hc1(0) show for sigma band. Hc2(0)//ab = Hc2(MgB2) + 11.0 T, Hc2(0)//c = Hc2(MgB2) + 8.22 T.	Mg(B,C)2	Mg1B1.81C0.19	Mg	1	B	1.81	C	0.19																		3	2006																												AlB2																		K				30.57		7	30.57											mT			6.03	11.4						curve fitting, Hc2(T) by ac-SUS.															A	from Hc2		53.9	22.9	A			2094	947																																																			high-pressure synthesis using cubic anvil.					Anisotropic reversible mixed-state properties of superconducting carbon-doped Mg(B1-xCx)2 single crystals			Atomic Institute of the Austrian Universities, 1020 Vienna, Austria	Phys.Rev.B, 74(2006)144511	C.Krutzler,M.Zehetmayer,M.Eisterer,H.W.Weber,N.D.Zhigadlo,J.Karpinski,A.Wisniewski		
40923	P074144520	Ce-content by DXPA. pseudogap temp. = 47.9 K , obtained from measurement of MR.	(Sm,Ce)CuO4	Sm1.86Ce0.14Cu1O4	Sm	1.86	Ce	0.14	Cu	1															O	4		3	2006																												T'																		K		22.7					22.7																																																																																																self-flux method. ANN(945C,15h, in flowing Ar)					Pseudogap in electron-doped superconducting Sm2-xCexCuO4-z by interlayer magnetotransport			Department of Electronic Science and Engineering, Kyoto University, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto 615-8510, Japan	Phys.Rev.B, 74(2006)144520	T.Kawakami,T.Shibauchi,Y.Terao,M.Suzuki		
40924	P074144520	Ce-content by DXPA. pseudogap temp. = 45.0 K , obtained from measurement of MR.	(Sm,Ce)CuO4	Sm1.857Ce0.143Cu1O4	Sm	1.857	Ce	0.143	Cu	1															O	4		3	2006																												T'																		K		22.3					22.3																																																																																																self-flux method. ANN(945C,15h, in flowing Ar)					Pseudogap in electron-doped superconducting Sm2-xCexCuO4-z by interlayer magnetotransport			Department of Electronic Science and Engineering, Kyoto University, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto 615-8510, Japan	Phys.Rev.B, 74(2006)144520	T.Kawakami,T.Shibauchi,Y.Terao,M.Suzuki		
40925	P074144520	Ce-content by DXPA. pseudogap temp. = 40.0 K , obtained from measurement of MR.	(Sm,Ce)CuO4	Sm1.85Ce0.15Cu1O4	Sm	1.85	Ce	0.15	Cu	1															O	4		3	2006																												T'																		K		19.7					19.7																																																																																																self-flux method. ANN(945C,15h, in flowing Ar)					Pseudogap in electron-doped superconducting Sm2-xCexCuO4-z by interlayer magnetotransport			Department of Electronic Science and Engineering, Kyoto University, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto 615-8510, Japan	Phys.Rev.B, 74(2006)144520	T.Kawakami,T.Shibauchi,Y.Terao,M.Suzuki		
40926	P074144520	Ce-content by DXPA. pseudogap temp. = 35.0 K , obtained from measurement of MR.	(Sm,Ce)CuO4	Sm1.844Ce0.156Cu1O4	Sm	1.844	Ce	0.156	Cu	1															O	4		3	2006																												T'																		K		16.4					16.4																																																																																																self-flux method. ANN(945C,15h, in flowing Ar)					Pseudogap in electron-doped superconducting Sm2-xCexCuO4-z by interlayer magnetotransport			Department of Electronic Science and Engineering, Kyoto University, Kyotodaigaku-Katsura, Nishikyo-ku, Kyoto 615-8510, Japan	Phys.Rev.B, 74(2006)144520	T.Kawakami,T.Shibauchi,Y.Terao,M.Suzuki		
40927	J075103801	not SC. spin glass for T < 23 K.	Ca2Ru2O7	Ca2Ru2O7	Ca	2	Ru	2																	O	7		3	2006	emu.K/Ru	0.000595	emu.K/Ru	0.0165	uB/Ru	0.36	-4.3																					pyrochlore			A	10.197														K					5.5																																																																									mOhm.cm											2												RuO2,CaO		mixture encapsulated with 30%H2O2, then heat (600C,3d, P=150 MPa)					A Novel Pyrochlore Ruthenate: Ca2Ru2O7			Department of Physics, Chuo University, 1-13-27 Kasuga, Bunkyo-ku, Tokyo 112-8551	J.Phys.Soc.Jpn, 75(2006)103801	T.Munenaka,H.Sato		
40928	JP01808533	re-entrant SC. no minimum in Hc2(T) at Neel-T.	(Ho,Y)Ni2B2C	Ho0.75Y0.25Ni2B2C1	Ho	0.75	Y	0.25	Ni	2	B	2	C	1														3	2006								3.9																				LuNi2B2C																		K	7.6					0.5	7.6																																		MHC40928																																																														floating zone method					Reentrant behaviour in Y-doped Ho0.75Y0.25Ni2B2C single crystal			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 18(2006)8533	S.R.Zhao,Z.A.Xu,H.Takeya,K.Hirata,J.L.Luo		
40929	JP01808037	not SC	La3Ni4Si4	La3Ni4Si4	La	3	Ni	4	Si	4																		1	2006																												U3Ni4Si4	I4/mmm		A	4.1308	4.176	23.578												K					1.8																																																																																																		arc-melting. ANN(1173-1373 K, 1w, in Mo-foil(silica tube))					Structure and superconductivity of the ternary intermetallics of La3Ni4Si4, La3Ni4Ge4, and La3Pd4Si4			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.:Condens.Matter, 18(2006)8037	H.Fujii		
40930	JP01808037	not SC	La3Ni4Ge4	La3Ni4Ge4	La	3	Ni	4	Ge	4																		1	2006																												U3Ni4Si4	I4/mmm		A	4.2017	4.2167	24.031												K					1.8																																																																																																		arc-melting. ANN(1173-1373 K, 1w, in Mo-foil(silica tube))					Structure and superconductivity of the ternary intermetallics of La3Ni4Si4, La3Ni4Ge4, and La3Pd4Si4			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.:Condens.Matter, 18(2006)8037	H.Fujii		
40931	JP01808037	RRR = 7.5. G-L = 9.9	La3Pd4Si4	La3Pd4Si4	La	3	Pd	4	Si	4																		1	2006																												U3Ni4Si4	I4/mmm		A	4.2254	4.2871	24.551												K	2.1		2.2	2.15			2.15											Oe	M-H curve	28							T	WHH theory	0.22							T/K		0.15					A	from Hc2	380			A	calculated from Hc1	3760																												uOhm.cm							8				60														arc-melting. ANN(1173-1373 K, 1w, in Mo-foil(silica tube))					Structure and superconductivity of the ternary intermetallics of La3Ni4Si4, La3Ni4Ge4, and La3Pd4Si4			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.:Condens.Matter, 18(2006)8037	H.Fujii		
40932	PHC3880571	sample has x > 1 in PdHx. x is not given. dR at Tc is very small. R is not to zero down to 4.2 K.. No sus-measurements.	PdHx	H1Pd1	H	1	Pd	1																					2003																																														K			51.6				51.6																																																																																																H loaded into Pd wire(50 micron-m) using as cathode in electrochemical cell.					Possibility of high temperature superconducting phases in PdH				Physica C, 388-389(2003)571	P.Tripodi,D.Di Gioacchino,R.Borelli,J.D.Vinko		
40933	PR0324426		Pd2YSn	Pd2Y1Sn1	Pd	2	Y	1	Sn	1																			1985																												Heusler			A	6.716													Cu2MnAl, L2<1>	K		4.55					4.55																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40934	PR0324426	dTc/dx = -44 K/atm-Gd in Pd2Y1-xGdxSn	Pd2(Y,Gd)Sn	Pd2Y0.98Gd0.02Sn1	Pd	2	Y	0.98	Gd	0.02	Sn	1																	1985																												Heusler			A	6.716													L2<1>, Heusler	K		3.24					3.24																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40935	PR0324426		Pd2(Y,Gd)Sn	Pd2Y0.95Gd0.05Sn1	Pd	2	Y	0.95	Gd	0.05	Sn	1																	1985																												Heusler			A	6.717													L2<1>, Heusler	K		2.41					2.41																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40936	PR0324426		Pd2(Y,Gd)Sn	Pd2Y0.9Gd0.1Sn1	Pd	2	Y	0.9	Gd	0.1	Sn	1																	1985																												Heusler			A	6.722													L2<1>, Heusler	K					1.2																																																																																																		arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40937	PR0324426		Pd2(Y,Dy)Sn	Pd2Y0.9Dy0.1Sn1	Pd	2	Y	0.9	Dy	0.1	Sn	1																	1985																												Heusler			A	6.716													L2<1>, Heusler	K		3.46					3.46																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40938	PR0324426		Pd2(Y,Dy)Sn	Pd2Y0.85Dy0.15Sn1	Pd	2	Y	0.85	Dy	0.15	Sn	1																	1985																												Heusler			A	6.718													L2<1>, Heusler	K		2.8					2.8																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40939	PR0324426		Pd2(Y,Dy)Sn	Pd2Y0.8Dy0.2Sn1	Pd	2	Y	0.8	Dy	0.2	Sn	1																	1985																												Heusler			A	6.718													L2<1>, Heusler	K		1.4					1.4																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40940	PR0324426		Pd2(Y,Dy)Sn	Pd2Y0.7Dy0.3Sn1	Pd	2	Y	0.7	Dy	0.3	Sn	1																	1985																												Heusler			A	6.722													L2<1>, Heusler	K					1.2																																																																																																		arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40941	PR0324426		Pd2(Y,Ho)Sn	Pd2Y0.9Ho0.1Sn1	Pd	2	Y	0.9	Ho	0.1	Sn	1																	1985																												Heusler			A	6.715													L2<1>, Heusler	K		4.06					4.06																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40942	PR0324426		Pd2(Y,Er)Sn	Pd2Y0.9Er0.1Sn1	Pd	2	Y	0.9	Er	0.1	Sn	1																	1985																												Heusler			A	6.715													L2<1>, Heusler	K		3.87					3.87																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40943	PR0324426		Pd2(Y,Er)Sn	Pd2Y0.8Er0.2Sn1	Pd	2	Y	0.8	Er	0.2	Sn	1																	1985																												Heusler			A	6.714													L2<1>, Heusler	K		3.73					3.73																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40944	PR0324426		Pd2(Y,Er)Sn	Pd2Y0.7Er0.3Sn1	Pd	2	Y	0.7	Er	0.3	Sn	1																	1985																												Heusler			A	6.714													L2<1>, Heusler	K		3.8					3.8																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40945	PR0324426		Pd2(Y,Er)Sn	Pd2Y0.6Er0.4Sn1	Pd	2	Y	0.6	Er	0.4	Sn	1																	1985																												Heusler			A	6.711													L2<1>, Heusler	K		2.77					2.77																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40946	PR0324426		Pd2(Y,Tm)Sn	Pd2Y0.95Tm0.05Sn1	Pd	2	Y	0.95	Tm	0.05	Sn	1																	1985																												Heusler			A	6.716													L2<1>, Heusler	K		4.12					4.12																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40947	PR0324426		Pd2(Y,Tm)Sn	Pd2Y0.9Tm0.1Sn1	Pd	2	Y	0.9	Tm	0.1	Sn	1																	1985																												Heusler			A	6.71													L2<1>, Heusler	K		4.12					4.12																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40948	PR0324426		Pd2(Y,Tm)Sn	Pd2Y0.75Tm0.25Sn1	Pd	2	Y	0.75	Tm	0.25	Sn	1																	1985																												Heusler			A	6.703													L2<1>, Heusler	K		3.73					3.73																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40949	PR0324426		Pd2(Y,Tm)Sn	Pd2Y0.5Tm0.5Sn1	Pd	2	Y	0.5	Tm	0.5	Sn	1																	1985																												Heusler			A	6.69													L2<1>, Heusler	K		3.65					3.65																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40950	PR0324426		Pd2(Y,Tm)Sn	Pd2Y0.25Tm0.75Sn1	Pd	2	Y	0.25	Tm	0.75	Sn	1																	1985																												Heusler			A	6.681													L2<1>, Heusler	K		3.06					3.06																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40951	PR0324426		Pd2TmSn	Pd2Tm1Sn1	Pd	2	Tm	1	Sn	1																			1985																												Heusler			A	6.67													L2<1>, Heusler	K		2.82					2.82																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40952	PR0324426		Pd2(Y,Yb)Sn	Pd2Y0.9Yb0.1Sn1	Pd	2	Y	0.9	Yb	0.1	Sn	1																	1985																												Heusler			A	6.713													L2<1>, Heusler	K		4.37					4.37																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40953	PR0324426		Pd2(Y,Yb)Sn	Pd2Y0.7Yb0.3Sn1	Pd	2	Y	0.7	Yb	0.3	Sn	1																	1985																												Heusler			A	6.704													L2<1>, Heusler	K		4.03					4.03																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40954	PR0324426		Pd2YbSn	Pd2Yb1Sn1	Pd	2	Yb	1	Sn	1																			1985																												Heusler			A	6.658													L2<1>, Heusler	K		2.42					2.42																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40955	PR0324426		Pd2ScSn	Pd2Sc1Sn1	Pd	2	Sc	1	Sn	1																			1985																												Heusler			A	6.503													L2<1>, Heusler	K		2.05					2.05																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40956	PR0324426		Pd2LuSn	Pd2Lu1Sn1	Pd	2	Lu	1	Sn	1																			1985																												Heusler			A	6.644													L2<1>, Heusler	K		3.05					3.05																																																																																																arc-melting . ANN(800C,7d, in vac)					Depression of the superconducting transition temperature of the Heusler alloy Pd2YSn with the addition of magnetic rare-earth metals			Materials Science and Technology Division, Argonne National Laboratory, Argonne,Illinois,USA	Phys.Rev.B, 32(1985)4426	S.K.Malik,A.M.Umarji,G.K.Shenoy		
40957	PR0532651		Pd2ScPb	Pd2Sc1Pb1	Pd	2	Sc	1	Pb	1																		3	1996					uB/mol	0																						Heusler			A	6.63													L2<1>, Heusler	K				2.4			2.4																																																																																																flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40958	PR0532651		Pd2YPb	Pd2Y1Pb1	Pd	2	Y	1	Pb	1																		3	1996					uB/mol	0																						Heusler			A	6.74													L2<1>, Heusler	K				2.3			2.3																																																																																																flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40959	PR0532651		Pd2GdPb	Pd2Gd1Pb1	Pd	2	Gd	1	Pb	1																		3	1996					uB/mol	8.51	-17.3	4.5																				Heusler			A	6.81													L2<1>, Heusler	K					1.8																																																																																																		flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40960	PR0532651		Pd2TbPb	Pd2Tb1Pb1	Pd	2	Tb	1	Pb	1																		3	1996					uB/mol	10.17	-16.9	2.8																				Heusler			A	6.79													L2<1>, Heusler	K					1.8																																																																																																		flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40961	PR0532651		Pd2DyPb	Pd2Dy1Pb1	Pd	2	Dy	1	Pb	1																		3	1996					uB/mol	11.13	-9.8	2.4																				Heusler			A	6.76													L2<1>, Heusler	K					1.8																																																																																																		flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40962	PR0532651		Pd2HoPb	Pd2Ho1Pb1	Pd	2	Ho	1	Pb	1																		3	1996					uB/mol	11.1	-6.5	0.8																				Heusler			A	6.75													L2<1>, Heusler	K					1.8																																																																																																		flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40963	PR0532651		Pd2ErPb	Pd2Er1Pb1	Pd	2	Er	1	Pb	1																		3	1996					uB/mol	9.77	-5.2	0.6																				Heusler			A	6.76													L2<1>, Heusler	K					1.8																																																																																																		flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40964	PR0532651		Pd2TmPb	Pd2Tm1Pb1	Pd	2	Tm	1	Pb	1																		3	1996					uB/mol	7.85	-2.7																					Heusler			A	6.72													L2<1>, Heusler	K				2.1			2.1																																																																																																flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40965	PR0532651		Pd2YbPb	Pd2Yb1Pb1	Pd	2	Yb	1	Pb	1																		1	1996					uB/mol	4.15	-3.6																					Heusler			A	6.73													L2<1>, Heusler	K				2.8			2.8																																																																																																sealed in Ta-tube. heat(1300C,1h) - Q to water					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40966	PR0532651		Pd2LuPb	Pd2Lu1Pb1	Pd	2	Lu	1	Pb	1																		3	1996																												Heusler			A	6.73													L2<1>, Heusler	K				2.4			2.4																																																																																																flux method. heat to 1200C, then slowly cooled (10C/h)					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40967	PR0532651		Pd2ThPb	Pd2Th1Pb1	Pd	2	Th	1	Pb	1																		1	1996																												Heusler			A	6.88													L2<1>, Heusler	K					1.8																																																																																																		sealed in Ta-tube. heat(1300C,1h) - Q to water					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40968	PR0532651	GAMMA is T-dependent. lattice term in SP (beta) = 3.8 mJ/mol.K4	Pd2UPb	Pd2U1Pb1	Pd	2	U	1	Pb	1																		1	1996					uB/mol	2.8	-51	35																				Heusler			A	6.85													L2<1>, Heusler	K					1.8																																																										mJ/mol.K2	98																																							sealed in Ta-tube. heat(1300C,1h) - Q to water					Superconductivity and magnetism in the Heusler alloys MPd2Pb  (M=rare earth, Th, and U)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 53(1996)2651	C.L.Seaman,N.R.Dilley,M.C.de Andrade,J.Herrmann,M.B.Maple,Z.Fisk		
40969	P074184510	nominal: Mo3C1.8. Thermodynamic Hc(0) = 0.15 T.  (dC/gamma*Tc) = 1.48	eta-Mo3C2	C2Mo3	C	2	Mo	3																					2006																													P6<3>/mmc		A	3.0105		14.6112												K				7.4			7.4											Oe	M vs H curve	140							T	SP-heat	5.7												MHC40696		A		76			A		1970													mJ/mol.K2	11.8																																							mixture - Ta crucible with h-BN coating.  High pressure synthesis(1700C,1h,6GPa) - Quench.					Superconductivity in the hexagonal-layered molybdenum carbide eta-Mo3C2			Advanced Nano Materials Laboratory, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 74(2006)184510	K.Yamaura,Q.Huang,M.Akashi,E.Takayama-Muromachi		
40970	P074184520	Isotope <16>O sample. Pseudogap Temp. = 82.2 K	(La,Sr,Ho)2CuO4	La1.85Sr0.11Ho0.04Cu1O4	La	1.85	Sr	0.11	Ho	0.04	Cu	1													O	4			2006																												T																		K				13.9			13.9																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40971	P074184520	Isotope <16>O sample. Pseudogap Temp. = 61.0 K	(La,Sr,Ho)2CuO4	La1.81Sr0.15Ho0.04Cu1O4	La	1.81	Sr	0.15	Ho	0.04	Cu	1													O	4			2006																												T																		K				32.5			32.5																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40972	P074184520	Isotope <16>O sample. Pseudogap Temp. = 49.2 K	(La,Sr,Ho)2CuO4	La1.76Sr0.2Ho0.04Cu1O4	La	1.76	Sr	0.2	Ho	0.04	Cu	1													O	4			2006																												T																		K				28.4			28.4																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40973	P074184520	Isotope <16>O sample. Pseudogap Temp. = 46.5 K.	(La,Sr,Ho)2CuO4	La1.71Sr0.25Ho0.04Cu1O4	La	1.71	Sr	0.25	Ho	0.04	Cu	1													O	4			2006																												T																		K				10.1			10.1																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40974	P074184520	Isotope effect, 78% exchange of <18>O . Pseudogap Temp. = 103.5 K	(La,Sr,Ho)2CuO4	La1.85Sr0.11Ho0.04Cu1O4	La	1.85	Sr	0.11	Ho	0.04	Cu	1													O	4			2006																																														K				11.7			11.7																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40975	P074184520	Isotope effect, 78% exchange of <18>O . Pseudogap Temp. = 70.0 K	(La,Sr,Ho)2CuO4	La1.81Sr0.15Ho0.04Cu1O4	La	1.81	Sr	0.15	Ho	0.04	Cu	1													O	4			2006																												T																		K				30.8			30.8																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40976	P074184520	Isotope effect, 78% exchange of <18>O . Pseudogap Temp. = 53.7 K	(La,Sr,Ho)2CuO4	La1.76Sr0.2Ho0.04Cu1O4	La	1.76	Sr	0.2	Ho	0.04	Cu	1													O	4			2006																												T																		K				27.3			27.3																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40977	P074184520	Isotope effect, 78% exchange of <18>O . Pseudogap Temp. = 48.4 K	(La,Sr,Ho)2CuO4	La1.71Sr0.25Ho0.04Cu1O4	La	1.71	Sr	0.25	Ho	0.04	Cu	1													O	4			2006																												T																		K				9.8			9.8																																																																																																Solid state reaction. <18>O by diffusion process (see Mat.Sci.Eng., R, R32(2001)41)					Pseudogap of the high-temperature superconductor La1.96-xSrxHo0.04CuO4 as observed by neutron crystal-field spectroscopy			Laboratory for Neutron Scattering, ETH Zurich & PSI Villigen, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 74(2006)184520	P.S.Hafliger,A.Podlesnyak,K.Conder,E.Pomjakushina,A.Furrer		
40978	P074184523	RES(40K)//ab = 2.36 uOhm.cm. THC(77K)//ab = 96.24 W/m.K. anisotropy factor from Hc2 = 3.77 at T/Tc = 0.6.	(Mg,Al)B2	Mg0.983Al0.017B1	Mg	0.983	Al	0.017	B	1																		3	2006																												AlB2																		K				35.9			35.9																																		MHC40978																											W/m.K				MTHC40978						uOhm.cm												9.204													high-pressure synthesis					Thermal conductivity of Al-doped MgB2: Impurity scattering and the validity of the Wiedemann-Franz law			Laboratorium fur Festkorperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B, 74(2006)184523	A.V.Sologubenko,N.D.Zhigadlo,J.Karpinski,H.R.Ott		
40979	P074184523	RES(40K)//ab = 4.13 uOhm.cm. THC(77K)//ab = 51.18 W/m.K. anisotropy factor from Hc2 = 3.27 at T/Tc = 0.6.	(Mg,Al)B2	Mg0.927Al0.073B1	Mg	0.927	Al	0.073	B	1																		3	2006																												AlB2																		K				33			33																																		MHC40979																											W/m.K				MTHC40979						uOhm.cm												11.151													high-pressure synthesis					Thermal conductivity of Al-doped MgB2: Impurity scattering and the validity of the Wiedemann-Franz law			Laboratorium fur Festkorperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B, 74(2006)184523	A.V.Sologubenko,N.D.Zhigadlo,J.Karpinski,H.R.Ott		
40980	P074172506		(Ca,La)(Ba,La)2Cu3O7	Ca0.2Ba1.55La1.25Cu3O7.159	Ca	0.2	Ba	1.55	La	1.25	Cu	3													O	z	7.159	1	2006																																														K		68.7					68.7	TC40980																																																																																															See Phys.Rev.B, 49(1994)15928					Evidence for two fluids in cuprate superconductors from a nuclear resonance study of (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oz			Technion?Israel Institue of Technology, 32000 Haifa, Israel	Phys.Rev.B, 74(2006)172506	Amit Keren,Amit Kanigel,Galina Bazalitsky		
40981	P074172506		(Ca,La)(Ba,La)2Cu3O7	Ca0.3Ba1.45La1.25Cu3O7.172	Ca	0.3	Ba	1.45	La	1.25	Cu	3													O	z	7.172	1	2006																																														K		76.9					76.9	TC40981																																																																																															See Phys.Rev.B, 49(1994)15928					Evidence for two fluids in cuprate superconductors from a nuclear resonance study of (CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oz			Technion?Israel Institue of Technology, 32000 Haifa, Israel	Phys.Rev.B, 74(2006)172506	Amit Keren,Amit Kanigel,Galina Bazalitsky		
40982	P074174515	stoichiometric (z=4.0) sample/ Phase = T + T'. Substrate = LaAlO3(a = 3.793 A). thickness = 450 A. not SC	(La,Ce)2CuO4	La1.94Ce0.06Cu1O4	La	1.94	Ce	0.06	Cu	1															O	4	4	5	2006																												T'			A			12.5104												K		0					0																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40983	P074174515	stoichiometric (z=4.0) sample/ Phase = T + T'. Substrate = LaAlO3(a = 3.793 A). thickness = 450 A.	(La,Ce)2CuO4	La1.925Ce0.075Cu1O4	La	1.925	Ce	0.075	Cu	1															O	4	4	5	2006																												T'			A			12.4781												K		3.92					3.92																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40984	P074174515	stoichiometric (z=4.0) sample/ Phase = T + T'. Substrate = LaAlO3(a = 3.793 A). thickness = 450 A.	(La,Ce)2CuO4	La1.91Ce0.09Cu1O4	La	1.91	Ce	0.09	Cu	1															O	4	4	5	2006																												T'			A			12.4593												K		22.5					22.5																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40985	P074174515	substrate = LaAlO3(a = 3.793 A). thickness = 450 A. stoichiometric (z=4.0) sample	(La,Ce)2CuO4	La1.895Ce0.105Cu1O4	La	1.895	Ce	0.105	Cu	1															O	4	4	4	2006																												T'			A			12.4485												K		24.3					24.3																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40986	P074174515	substrate = LaAlO3(a = 3.793 A). thickness = 450 A. stoichiometric (z=4.0) sample	(La,Ce)2CuO4	La1.88Ce0.12Cu1O4	La	1.88	Ce	0.12	Cu	1															O	4	4	4	2006																												T'			A			12.4377												K		24.3					24.3																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40987	P074174515	oxidized (z>4.0) sample, but z is not given. Substrate = LaAlO3 (a=3.793 A). thickness = 450 A.	La2CuO4	La2Cu1O4+z	La	2	Cu	1																	O	4+z		4	2006																												T			A			13.1758												K		37.8					37.8																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40988	P074174515	oxidized (z>4.0) sample, but z is not given. Substrate = LaAlO3 (a=3.793 A). thickness = 450 A.	(La,Ce)2CuO4	La1.97Ce0.03Cu1O4+z	La	1.97	Ce	0.03	Cu	1															O	4+z		4	2006																												T			A			13.1569												K		31.1					31.1																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40989	P074174515	Phae = T + T'.  oxidized (z>4.0) sample., but z is not given. Substrate = LaAlO3 (a=3.793 A). thickness = 450 A.	(La,Ce)2CuO4	La1.94Ce0.06Cu1O4+z	La	1.94	Ce	0.06	Cu	1															O	4+z		5	2006																												T			A			13.103												K		7.97					7.97																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40990	P074174515	Phae = T + T'.  not SC.  oxidized (z>4.0) sample., but z is not given. Substrate = LaAlO3 (a=3.793 A). thickness = 450 A.	(La,Ce)2CuO4	La1.91Ce0.09Cu1O4+z	La	1.91	Ce	0.09	Cu	1															O	4+z		5	2006																												T			A			13.0249												K		0					0																																																																																																MBE method (multiple electron-gun). Substrate = LaAlO3. substrate temp = 630C					Doping of Ce in T-La2CuO4: Rigorous test for electron-hole symmetry for high-Tc superconductivity			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Naka-cho, Koganei, Tokyo 184-8588, Japan	Phys.Rev.B, 74(2006)174515	A.Tsukada,H.Yamamoto,M.Naito		
40991	JJP039L485	R not zero at 4.2 K.	(La,Ce)2CuO4	La1.936Ce0.064Cu1O4	La	1.936	Ce	0.064	Cu	1															O	4		4	2000																												T'			A			12.5153												K			13.8				13.8																																																																																																MBE method. Substrate = SrTiO3. growth rate = 15 nm/min. substrate temp = 660 C.					Superconducting T' -La2-xCexCuO4 films grown by molecular beam epitaxy			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys., 39(2000)L485	M.Naito,M.Hepp		
40992	JJP039L485		(La,Ce)2CuO4	La1.891Ce0.109Cu1O4	La	1.891	Ce	0.109	Cu	1															O	4		4	2000																												T'			A			12.458												K	27.8		29.2				28.5	TC40992																																																																																															MBE method. Substrate = SrTiO3. growth rate = 15 nm/min. substrate temp = 660 C.					Superconducting T' -La2-xCexCuO4 films grown by molecular beam epitaxy			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys., 39(2000)L485	M.Naito,M.Hepp		
40993	JJP039L485		(La,Ce)2CuO4	La1.821Ce0.179Cu1O4	La	1.821	Ce	0.179	Cu	1															O	4		4	2000																												T'			A			12.4031												K	4.45		10				7.225																																																																																																MBE method. Substrate = SrTiO3. growth rate = 15 nm/min. substrate temp = 660 C.					Superconducting T' -La2-xCexCuO4 films grown by molecular beam epitaxy			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Jpn.J.Appl.Phys., 39(2000)L485	M.Naito,M.Hepp		
40994	JJP033L168	Fig. shows Tc(on), Tc(end) vs Ce-content.	(La,Ce)2CuO4	La1.87Ce0.13Cu1Oz	La	1.87	Ce	0.13	Cu	1															O	z		1	1994																												T'			A	4.007		12.44												K	17		30				23.5	TC40994																																																																																													La2O3,CeO2,Cu2O	1	solid state reaction. oxidized in O2, 250<T<300 C. finally annealed in Ar or N2 (600C, 600h).					Synthesis of superconducting T'-(La1-xCex)2CuO4			NTT Basic Research Laboratories 3-1, Morinosato-Wakamiya, Atsugi-shi, Kanagawa, Japan	Jpn.J.Appl.Phys., 33(1994)L168	H.Shibata,K.Kinoshita,T.Yamada		
40995	DRM0151898	W-containing diamond-like film (thickness=500nm)	W-O-C	W0.474O0.106C0.42	W	0.474	O	0.106	C	0.42																		4	2006																																														K	3.75	3.85					3.85																																		MHC40995																																																														plasma-enhanced CVD + co-sputtering of W on Si-oxide substrate					Superconductivity in W-containing diamond-like nanocomposite films			Institute of Fluid Science, Tohoku University, Sendai, Japan	Diamond Relat.Mater., 15(2006)1898	H.Miki,T.Takeno,T.Takagi,A.Bozhko,M.Shupegin,H.Onodera,T.Komiyama,T.Aoyama		
40996	CHM0112185	not SC. nominal composition = (Cu0.5V0.5)Sr2CaCu2O7.3. susceptibility(5 K) =	(Cu,V)Sr2CaCu2Oz	Cu2.5V0.5Sr2Ca1Oz	Cu	2.5	V	0.5	Sr	2	Ca	1													O	z			1999																																														K					4.2																																																																																																V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
40997	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2CaCu2O7.5. susceptibility(5 K) = -5.64 emu/g.	(Cu,V)Sr2Ca2Cu3Oz	Cu3.5V0.5Sr2Ca1Oz	Cu	3.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1223																		K		98					98																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
40998	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2CaCu2O7.15. susceptibility(5 K) = -9.07 emu/g.	(Cu,V)Sr2Ca3Cu4Oz	Cu4.5V0.5Sr2Ca1Oz	Cu	4.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1234																		K		98					98																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
40999	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2Ca2Cu3O9.6. susceptibility(5 K) = -7.17 emu/g.	(Cu,V)Sr2Ca3Cu4Oz	Cu4.5V0.5Sr2Ca1Oz	Cu	4.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1234			A	3.8497		17.9												K		107					107																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42000	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2Ca2Cu3O9.4. susceptibility(5 K) = -7.64 emu/g.	(Cu,V)Sr2Ca4Cu5Oz	Cu5.5V0.5Sr2Ca1Oz	Cu	5.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1245																		K		75					75																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42001	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2Ca2Cu3O9.0. susceptibility(5 K) = -1.58 emu/g.	(Cu,V)Sr2Ca5Cu6Oz	Cu6.5V0.5Sr2Ca1Oz	Cu	6.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1256																		K		73					73																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42002	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2Ca3Cu4O11.15. susceptibility(5 K) = -5.85 emu/g.	(Cu,V)Sr2C63Cu7Oz	Cu7.5V0.5Sr2Ca1Oz	Cu	7.5	V	0.5	Sr	2	Ca	1													O	z			1999																												M1267																		K		73					73																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42003	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2(Ca3.6Sr0.4)Cu5O13.55. susceptibility(5 K) = -8.91 emu/g.	(Cu,V)Sr2(Ca,Sr)4Cu5Oz	Cu5.5V0.5Sr2.4Ca3.6Oz	Cu	5.5	V	0.5	Sr	2.4	Ca	3.6													O	z			1999																												M1245			A	3.8498		21.036												K		75	101				75																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42004	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2(Ca3.6Sr0.4)Cu5O13.5. susceptibility(5 K) = -7.52 emu/g.	(Cu,V)Sr2(Ca,Sr)5Cu6Oz	Cu6.5V0.5Sr3.75Ca3.25Oz	Cu	6.5	V	0.5	Sr	3.75	Ca	3.25													O	z			1999																												M1256			A	3.8532		24.226												K		75					75																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42005	CHM0112185	nominal composition = (Cu0.5V0.5)Sr2(Ca4.7Sr0.3)Cu5O15.3. susceptibility(5 K) = -4.86 emu/g.	(Cu,V)Sr2(Ca,Sr)6Cu7Oz	Cu7.5V0.5Sr3.94Ca4.06Oz	Cu	7.5	V	0.5	Sr	3.94	Ca	4.06													O	z			1999																												M1267			A	3.8572		27.434												K		75					75																																																																																														V2O5,SrCuO2,SrO2,Ca2CuO3,CuO		high pressure synthesis (6GPa,1300C,1h) - Q to RT					High-pressure synthesis and characterization of a new series of V-based superconductors (Cu0.5V0.5)Sr2Can-1CunOy			National Institute for Research in Inorganic Materials, Tsukuba, Ibaraki, Japan	Chem.Mater., 11(1999)2185	N.D.Zhigadlo,Y.Anan,T.Asaka,Y.Ishida,Y.Matsui,E.Takayama-Muromachi		
42006	JTL0820081	NMR of Pb<207> measured at 20 K.	Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			2005																												BPBO																	delta-phase	K		12.5					12.5	TC42006																																																																																																				Knight shift in superconducting oxides BaPb1-xBixO3 (x<0.35)				JETP Lett., 82(2005)81	V.V.Ogloblichev,A.V.Pogudin,Yu.V.Piskunov,S.V.Verkhovskii,A.Yu.Yakubovsky,A.Trokiner		
42007	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-MoByCx	Mo1B0.01C0.82	Mo	1	B	0.01	C	0.82																			1997																												NaCl																	delta-phase	K		12.2					12.2	MTC42007																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42008	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-MoByCx	Mo1B0.03C0.82	Mo	1	B	0.03	C	0.82																			1997																												NaCl																	delta-phase	K		11.8					11.8	MTC42007																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42009	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-MoByCx	Mo1B0.05C0.82	Mo	1	B	0.05	C	0.82																			1997																												NaCl																	delta-phase	K		11.5					11.5	MTC42007																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42010	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-(Mo,Hf)Cx	Mo0.95Hf0.05C0.65	Mo	0.95	Hf	0.05	C	0.65																			1997																												NaCl																	delta-phase	K		8.81					8.81	MTC42010																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42011	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-(Mo,Hf)Cx	Mo0.95Hf0.05C0.68	Mo	0.95	Hf	0.05	C	0.68																			1997																												NaCl																	delta-phase	K		9.87					9.87	MTC42010																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42012	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-(Mo,Hf)Cx	Mo0.95Hf0.05C0.7	Mo	0.95	Hf	0.05	C	0.7																			1997																												NaCl																	delta-phase	K		10.9					10.9	MTC42012																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42013	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-(Mo,Hf)Cx	Mo0.95Hf0.05C0.73	Mo	0.95	Hf	0.05	C	0.73																			1997																												NaCl																	delta-phase	K		12					12	MTC42012																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42014	MPL0110939	delta-phase Mo-C stabilized by addition of 3rd element.	delta-(Mo,Hf)Cx	Mo0.95Hf0.05C0.74	Mo	0.95	Hf	0.05	C	0.74																			1997																												NaCl																	delta-phase	K		12.4					12.4	MTC42012																																																																																															arc-melting					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42015	MPL0110939	phase area: 0.35<C/Mo ratio<0.52 and 1463< T(K) <2795.	beta-Mo2C	C1Mo2	C	1	Mo	2																					1997																															A	3.012	4.745												beta-phase, hexagonal	K		2.8					2.8																																																																																																					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42016	MPL0110939	phase area: 0.48<C/Mo ratio<0.50 and  T(K) <1763.	alpha-Mo2C	C1Mo2	C	1	Mo	2																					1997																															A	4.733	6.035	5.206											alpha-phase, ortho.	K		4.1					4.1																																																																																																					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42017	MPL0110939	phase area: 0.59<C/Mo ratio<0.64 and 1928< T(K) <2823.	alpha-MoCx	C0.64Mo1	C	0.64	Mo	1																					1997																															A	3.016	14.659												alpha-phase, hex.	K		8.9					8.9																																																																																																					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42018	MPL0110939	phase area: 0.66<C/Mo ratio<0.76 and 2233< T(K) <2853.	delta-MoCx	C0.75Mo1	C	0.75	Mo	1																					1997																															A	4.2904													delta-phase, cubic	K		14.7					14.7																																																																																																splat cooling					Structural instability and superconductivity of the defect cubic structure delta-MoC1-x			University of Patros, Greece	Mod.Phys.Lett. B, 11(1997)939	N.S.Athanasiou		
42019	P074214513	Tc by ac-SUS.	CaC6	C6Ca1	C	6	Ca	1																					2006																												GIC																		K				11.4		0.15	11.4	MTC42019		K/GPa	0.48																																																																																												See Phys.Rev.Lett., 96(2006)107008					Effect of pressure on superconducting Ca-intercalated graphite CaC6			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany	Phys.Rev.B, 74(2006)214513	J.S.Kim,L.Boeri,R.K.Kremer,F.S.Razavi		
42020	P074214515	gap shows maximum value. reflectance measured for 18 - 34000 cm(-1).	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2006																												T'																		K				20			20																																									A		2000			meV	4.3	5	15																																															Crystals were grown from a CuO-based flux using a directional solidification method.					Optical determination of the superconducting energy gap in electron-doped Pr1.85Ce0.15CuO4			Condensed Matter Physics & Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 74(2006)214515	C.C.Homes,R.P.S.M.Lobo,P.Fournier,A.Zimmers,R.L.Greene		
42021	P070132502	d = 3780 A. reflectance measured for 60 - 21000 cm(-1).	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		3	2004																												T'																		K	21						21																																									A			3300				4.7	15																																															Films were epitaxially grown by pulsed-laser deposition on SrTiO3.					Infrared signature of the superconducting state in Pr2-xCexCuO4			Laboratoire de Physique du Solide (UPR 5 CNRS) ESPCI, 10 Rue Vauquelin 75231 Paris, France	Phys.Rev.B, 70(2004)132502	A.Zimmers,R.P.S.M.Lobo,N.Bontemps,C.C.Homes,M.C.Barr,Y.Dagan,R.L.Greene		
42022	P070132502	d = 3750 A. reflectance measured for 60 - 21000 cm(-1).	(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O4	Pr	1.83	Ce	0.17	Cu	1															O	4		3	2004																												T'																		K	15						15																																									A			2000				4.7	15																																															Films were epitaxially grown by pulsed-laser deposition on SrTiO3.					Infrared signature of the superconducting state in Pr2-xCexCuO4			Laboratoire de Physique du Solide (UPR 5 CNRS) ESPCI, 10 Rue Vauquelin 75231 Paris, France	Phys.Rev.B, 70(2004)132502	A.Zimmers,R.P.S.M.Lobo,N.Bontemps,C.C.Homes,M.C.Barr,Y.Dagan,R.L.Greene		
42023	L088107002	gap value for maximum. gap(max) located closer to the nodes. Gap-Fig shows for B2g channel. lower gap: (2d/kTc) = 3.3 at Brillouin zone.	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		3	2002																												T'																		K				22		2	22	GAP42023																																															4.4	4																																															See Physica C, 177(1991)79					Nonmonotonic dx2-y2 Superconducting Order Parameter in Nd2-xCexCuO4			Bell Laboratories, Lucent Technologies, Murray Hill, New Jersey 07974	Phys.Rev.Lett., 88(2002)107002	G.Blumberg,A.Koitzsch,A.Gozar,B.S.Dennis,C.A.Kendziora,P.Fournier,R.L.Greene		
42024	P074220502	G-L parameter = 800.	Mg10Ir19B16	Mg10Ir19B16	Mg	10	Ir	19	B	16																			2006																													I-43m		A	10.568														K		4.4	5			0.4	4.4											Oe	M-H curve	35			35			2	T		3			2			2.4																																																																		Mg,Ir,a-B	1	mixture - wrapped in Ta-foil - heat(600C,30min + 900C,1h,in 95Ar-5H2 atmosphere) - addition of 20%Mg - heat(900C,1h)					Superconductivity in noncentrosymmetric Mg10Ir19B16			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 74(2006)220502R	T.Klimczuk,Q.Xu,E.Morosan,J.D.Thompson,H.W.Zandbergen,R.J.Cava		
42025	P074220506	Hc2 increases linearly with lowering T down to 0.5 K. High field by pulse field. The sample is block coprised of single crystal pieces.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2006																												pyrochlore																		K			9.73				9.73																				T	resistive	33												HC42025		A		32																																																															Uncommonly high upper critical field of the pyrochlore superconductor KOs2O6 below the enhanced paramagnetic limit			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.B, 74(2006)220506R	T.Shibauchi,L.Krusin-Elbaum,Y.Kasahara,Y.Shimono,Y.Matsuda,R.D.McDonald,C.H.Mielke,S.Yonezawa,Z.Hiroi,M.Arai,T.Kita,G.Blatter,M.Sigrist		
42026	PHC4510001	Jc defined as 1 uV/cn. Jc-unit = A/cm2.	(Hg,Sb)Ba2Ca2Cu3	Hg0.8Sb0.2Ba2Ca2Cu3O8+z	Hg	0.8	Sb	0.2	Ba	2	Ca	2	Cu	3											O	8+z		1	2007																												Hg1223			A	3.846		15.846												K	126						126																																																			730																																											Ba(NO3)2,CaO,CuO,HgO,Sb2O3,PbO	1	(Ba:Ca:Cu=2:2.2:3.2)mixture - heat(925C,48h,in flowing O2) - mixed with (HgO,Sb2O3,PbO) - Pt-box in quartz tube - heat(840C,12h).					Influence of simultaneous doping of Sb and Pb on phase formation, superconducting and microstructural characteristics of HgBa2Ca2Cu3O8+d			Department of Physics, Banaras Hindu University, Varanasi, India	Physica C, 451(2007)1	Rajiv Giri,R.S.Tiwari,O.N.Srivastava		
42027	PHC4510001	Jc defined as 1 uV/cn. Jc-unit = A/cm2.	(Hg,Sb,Pb)Ba2Ca2Cu3	Hg0.8Sb0.15Pb0.05Ba2Ca2Cu3O8+z	Hg	0.8	Sb	0.15	Pb	0.05	Ba	2	Ca	2	Cu	3									O	8+z		1	2007																												Hg1223			A	3.845		15.854												K	127						127																																																			865																																											Ba(NO3)2,CaO,CuO,HgO,Sb2O3,PbO	1	(Ba:Ca:Cu=2:2.2:3.2)mixture - heat(925C,48h,in flowing O2) - mixed with (HgO,Sb2O3,PbO) - Pt-box in quartz tube - heat(840C,12h).					Influence of simultaneous doping of Sb and Pb on phase formation, superconducting and microstructural characteristics of HgBa2Ca2Cu3O8+d			Department of Physics, Banaras Hindu University, Varanasi, India	Physica C, 451(2007)1	Rajiv Giri,R.S.Tiwari,O.N.Srivastava		
42028	PHC4510001	Jc defined as 1 uV/cn. Jc-unit = A/cm2.	(Hg,Sb,Pb)Ba2Ca2Cu3	Hg0.8Sb0.1Pb0.1Ba2Ca2Cu3O8+z	Hg	0.8	Sb	0.1	Pb	0.1	Ba	2	Ca	2	Cu	3									O	8+z		1	2007																												Hg1223			A	3.847		15.866												K	129						129																																																			1075																																											Ba(NO3)2,CaO,CuO,HgO,Sb2O3,PbO	1	(Ba:Ca:Cu=2:2.2:3.2)mixture - heat(925C,48h,in flowing O2) - mixed with (HgO,Sb2O3,PbO) - Pt-box in quartz tube - heat(840C,12h).					Influence of simultaneous doping of Sb and Pb on phase formation, superconducting and microstructural characteristics of HgBa2Ca2Cu3O8+d			Department of Physics, Banaras Hindu University, Varanasi, India	Physica C, 451(2007)1	Rajiv Giri,R.S.Tiwari,O.N.Srivastava		
42029	PHC4510001	Jc defined as 1 uV/cn. Jc-unit = A/cm2.	(Hg,Sb,Pb)Ba2Ca2Cu3	Hg0.8Sb0.05Pb0.15Ba2Ca2Cu3O8+z	Hg	0.8	Sb	0.05	Pb	0.15	Ba	2	Ca	2	Cu	3									O	8+z		1	2007																												Hg1223			A	3.843		15.871												K	133						133																																																			1850																																											Ba(NO3)2,CaO,CuO,HgO,Sb2O3,PbO	1	(Ba:Ca:Cu=2:2.2:3.2)mixture - heat(925C,48h,in flowing O2) - mixed with (HgO,Sb2O3,PbO) - Pt-box in quartz tube - heat(840C,12h).					Influence of simultaneous doping of Sb and Pb on phase formation, superconducting and microstructural characteristics of HgBa2Ca2Cu3O8+d			Department of Physics, Banaras Hindu University, Varanasi, India	Physica C, 451(2007)1	Rajiv Giri,R.S.Tiwari,O.N.Srivastava		
42030	PHC4510001	Jc defined as 1 uV/cn. Jc-unit = A/cm2.	(Hg,Pb)Ba2Ca2Cu3	Hg0.8Pb0.2Ba2Ca2Cu3O8+z	Hg	0.8	Pb	0.2	Ba	2	Ca	2	Cu	3											O	8+z		1	2007																												Hg1223			A	3.842		15.878												K	130						130																																																			1420																																											Ba(NO3)2,CaO,CuO,HgO,Sb2O3,PbO	1	(Ba:Ca:Cu=2:2.2:3.2)mixture - heat(925C,48h,in flowing O2) - mixed with (HgO,Sb2O3,PbO) - Pt-box in quartz tube - heat(840C,12h).					Influence of simultaneous doping of Sb and Pb on phase formation, superconducting and microstructural characteristics of HgBa2Ca2Cu3O8+d			Department of Physics, Banaras Hindu University, Varanasi, India	Physica C, 451(2007)1	Rajiv Giri,R.S.Tiwari,O.N.Srivastava		
42031	PHC4510019	compositions by ICP.	BaAlSi	Ba1Al1Si1	Ba	1	Al	1	Si	1																			2007																												AlB2			A	4.2845		5.136												K					2																																																																																																		melt in h-BN cell using RF furnace.					Missing superconductivity in BaAlSi with the AlB2 type structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Physica C, 451(2007)19	S.Yamanaka,T.Otsuki,T.Ide,H.Fukuoka,R.Kumashiro,T.Rachi,K.Tanigaki,F.Guo,K.Kobayashi		
42032	PHC4510019	compositions by ICP. Tc = 2.8 - 3.0 for 0.05 =< x =<0.5 in BaAl1-xSi1+x.	BaAlSi	Ba1Al0.95Si1.05	Ba	1	Al	0.95	Si	1.05																			2007																												AlB2			A	4.2549		5.1372												K				2.8			2.8																																																																																																melt in h-BN cell using RF furnace.					Missing superconductivity in BaAlSi with the AlB2 type structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Physica C, 451(2007)19	S.Yamanaka,T.Otsuki,T.Ide,H.Fukuoka,R.Kumashiro,T.Rachi,K.Tanigaki,F.Guo,K.Kobayashi		
42033	SSC1410519		(Y,Th)NiC2	Y0.9Th0.1Ni1C2	Y	0.9	Th	0.1	Ni	1	C	2																1	2007																												CeNiC2			A	3.574	4.503	6.03												K	5.13		6.88				6.005																																																																																																arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42034	SSC1410519		(Y,Th)NiC2	Y0.8Th0.2Ni1C2	Y	0.8	Th	0.2	Ni	1	C	2																1	2007																												CeNiC2			A	3.602	4.496	6.039												K	5.7		7.37				6.535																																																																																																arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42035	SSC1410519		(Y,Th)NiC2	Y0.7Th0.3Ni1C2	Y	0.7	Th	0.3	Ni	1	C	2																1	2007																												CeNiC2			A	3.621	4.497	6.049												K	6.84		8.05				7.445																																																																																																arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42036	SSC1410519		(Y,Th)NiC2	Y0.6Th0.4Ni1C2	Y	0.6	Th	0.4	Ni	1	C	2																	2007																												CeNiC2			A	3.637	4.495	6.051												K	7.51		8.19				7.85																																																																																																arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42037	SSC1410519	lattice term coeffic in SP = 0.25 mj/mol.K4. (dC/gamma*Tc) = 1.25	(Y,Th)NiC2	Y0.5Th0.5Ni1C2	Y	0.5	Th	0.5	Ni	1	C	2																	2007																												CeNiC2			A	3.671	4.492	6.086												K	8.2	8.3	8.4				8.3																																																						mj/mol.K	115	mj/mol.K2	11.04	SP-heat																																						arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42038	SSC1410519		YNiC2	Y1Ni1C2	Y	1	Ni	1	C	2																		1	2007																												CeNiC2			A	3.568	4.5	6.02												K					0.4																																																																																																		arc-melting in Ar					Superconductivity in the Th-doped YNiC2 compounds			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 141(2007)515	K.J.Syu,H.H.Sung,W.H.Lee		
42039	JAC4290064	needle-like Pb precipitates at boundaries of Pd49.2Yb27.4Pb23.4 grains.	Pd2YbPb	Pd2Yb1Pb1	Pd	2	Yb	1	Pb	1																		1	2007					uB	4.1	-5																					Heusler			A	6.739													L2<1>, Heusler phase	K	2.85			2.5			2.5										100																								MHC42039																																																														arc-melting in Ar, ANN(800 C,60 d)					Superconductivity in the Heusler alloy Pd2YbPb			Department of Physics, Faculty of Sciences and Letters, Istanbul Technical University, 34469 Maslak, Istanbul, Turkey	J.Alloys Compd., 429(2007)64	Y.Oner,O.Kamer,E.Alveroglu,M.Acet,T.Krenke		
42040	SSC1010323		LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	1997																												CeNiC2	Amm2		A	3.961	4.561	6.197												K	3			2.9			2.9																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42041	SSC1010323		(La,Th)NiC2	La0.9Th0.1Ni1C2	La	0.9	Th	0.1	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.95	4.565	6.196												K	4.5			4.45			4.45																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42042	SSC1010323		(La,Th)NiC2	La0.8Th0.2Ni1C2	La	0.8	Th	0.2	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.942	4.551	6.19												K	5.4			5.4			5.4																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42043	SSC1010323		(La,Th)NiC2	La0.7Th0.3Ni1C2	La	0.7	Th	0.3	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.936	4.542	6.18												K	7.3			7.2			7.2																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42044	SSC1010323		(La,Th)NiC2	La0.6Th0.4Ni1C2	La	0.6	Th	0.4	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.926	4.531	6.183												K	7.8			7.7			7.7																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42045	SSC1010323		(La,Th)NiC2	La0.5Th0.5Ni1C2	La	0.5	Th	0.5	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.918	4.517	6.175												K	7.9			7.9			7.9	MTC42045																																																																																													La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42046	SSC1010323		(La,Th)NiC2	La0.4Th0.6Ni1C2	La	0.4	Th	0.6	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.914	4.512	6.179												K	7.7			7.6			7.6																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42047	SSC1010323		(La,Th)NiC2	La0.3Th0.7Ni1C2	La	0.3	Th	0.7	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.91	4.496	6.185												K	6.8			6.3			6.3																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42048	SSC1010323		(La,Th)NiC2	La0.2Th0.8Ni1C2	La	0.2	Th	0.8	Ni	1	C	2																1	1997																												CeNiC2	Amm2		A	3.897	4.488	6.195												K	4.9			4.2			4.2																																																																																														La(3N),Ni(4N),C(5N),Th		arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Superconductivity in the series (La1-xThx)NiC2 (0=<x=<0.8)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 101(1997)323	W.H.Lee,H.K.Zeng		
42049	SSC1020433	gamma = 5.0 mJ/mol.K2 by extraporation in C/T vs T2 plot. (dC/gamma*Tc) = 1.30	(La,Th)NiC2	La0.5Th0.5Ni1C2	La	0.5	Th	0.5	Ni	1	C	2																1	1997																												CeNiC2																		K				7.9			7.9																																																								mj/mol.K2	7.5	entropy analysis in SP																																						arc-melting in Ar, ANN(1200C,3d, wrapped in Ta-foil in quartz tube)					Calorimetric studies of superconducting (La1-xThx)NiC2 (x = 0.1 - 0.9)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 102(1997)433	W.H.Lee,H.K.Zeng,Y.Y.Chen,Y.D.Yao,J.C.Ho		
42050	J075124702	energy gap obtained from T1(NMR) of Sb(1)-site	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2006																												skutterudite																		K		1.85					1.85																																																6.9	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42051	J075124702	energy gap obtained from T1(NMR) of Sb(1)-site	(Pr,La)Os4Sb12	Pr0.95La0.05Os4Sb12	Pr	0.95	La	0.05	Os	4	Sb	12																3	2006																												skutterudite																		K		1.84					1.84																																																5.9	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42052	J075124702	energy gap obtained from T1(NMR) of Sb(1)-site	(Pr,La)Os4Sb12	Pr0.8La0.2Os4Sb12	Pr	0.8	La	0.2	Os	4	Sb	12																3	2006																												skutterudite																		K		1.8					1.8																																																5.2	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42053	J075124702	energy gap obtained from T1(NMR) of Sb(1)-site	(Pr,La)Os4Sb12	Pr0.6La0.4Os4Sb12	Pr	0.6	La	0.4	Os	4	Sb	12																3	2006																												skutterudite																		K		1.67					1.67																																																4.2	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42054	J075124702	energy gap obtained from T1(NMR) of Sb(2)-site	(Pr,La)Os4Sb12	Pr0.2La0.8Os4Sb12	Pr	0.2	La	0.8	Os	4	Sb	12																3	2006																												skutterudite																		K		1.07					1.07																																																3.4	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42055	J075124702	energy gap obtained from T1(NMR) of Sb(2)-site	LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2006																												skutterudite																		K		0.74					0.74																																																3.45	6																																															Sb-flux method					Multiband Superconductivity in Filled-Skutterudite Compounds (Pr1-xLax)Os4Sb12: An Sb Nuclear-Quadrupole-Resonance Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)124702	M.Yogi,T.Nagai,Y.Imamura,H.Mukuda,Y.Kitaoka,D.Kikuchi,H.Sugawara,Y.Aoki,H.Sato,H.Harima		
42056	J076023704	enriched sample(C<12>:C<13> = 9:1). two gaps: table value is for larger gap(main), lower value of  (2d/kTc) = 2 , measured by NMR.	Y2C3	C3Y2	C	3	Y	2																				1	2007																												Pu2C3	I4[-]3d																	K				15.7			15.7																																																5	6																																															arc-melting , high pressure.					Multigap Superconductivity in Y2C3: A <13>C-NMR Study			Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 76(2007)023704	A.Harada,S.Akutagawa,Y.Miyamichi,H.Mukuda,Y.Kitaoka,J.Akimitsu		
42057	JPS0730649	resistivity for J//[100] shows Tc=0.6 K at P=0. bulk SC appears above 1.2 GPa. Tc(P) shows for bulk SC. RR for J//[100] = 20 uOhm.cm. dHvA effect also measured.	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																		3	2004					uB/Ce	0.55		2.8																				Ho2CoGa8																		K		0.6					0.6	MTC42057																																																							mj/mol.K2	800	SP-heat																																						self-flux method					Electronic, Magnetic and Superconducting Properties of Quasi-two Dimensional Compounds Ce2RhIn8 and La2RhIn8			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 73(2004)649	T.Ueda,H.Shishido,S.Hashimoto,T.Okubo,M.Yamada,Y.Inada,R.Settai,H.Harima,A.Galatanu,E.Yamamoto,N.Nakamura,K.Sugiyama,T.Takeuchi,K.Kindo,T.Namiki,Y.Aoki,H.Sato,Y.Onuki		
42058	JAC4280094	not SC	MgNi3B2	Mg1Ni3B2	Mg	1	Ni	3	B	2																			2007																											7		P6<4>22	181	A	4.88		8.787											hex, hP18	K					1.8																																																										mJ/mol.K2	4.9	from SP	609	from SP																																				mixture - Ta-crucible - sealed in Ar - heat(900C or 950 C, 1w)					Structure, transport and magnetic properties of MgNi3B2			CNR-INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	J.Alloy Compd, 428(2007)94	P.Manfrinetti,M.Pani,S.K.Dhar,R.Kulkarni		
42059	PHC2130190		Ca5C60	C60Ca5	C	60	Ca	5																					1993																												fullerene																		K		8.4					8.4	MTC42059		K/GPa	1.1																																																																																										Ca,C60		mixture in W-cell in evacuated quartz tube. Heat(550C,20h)					PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION OF CALCIUM FULLERENE CA5C60	199308			PHYSICA C,213(1993)190	A.R.KORTAN,J.E.SCHIRBER,N.KOPYLOV,W.R.BAYLESS	CA,C	
42060	PRL0832258	N(0) = 6.0 states/eV.mol-C60 from kai(P) = 5.5 E-4 emu/mol. lattice const(295 K) analyzed from three phase model(Ba6-, Ba4-, Ba3-C60)	Ba4C60	Ba4C60	Ba	4	C	60																					1999																												fullerene			A	11.61	11.2349	10.883												K				6.7			6.7																																																																																																react(C60 +Ba or Sr) in Ta-cell.  ANN(550-650C, 12d)					Structural and Electronic Properties of the Noncubic Superconducting Fullerides A'4C60  (A' = Ba, Sr )			School of Chemistry, Physics and Environmental Science, University of Sussex, Brighton, BN1 9QJ, United Kingdom	Phys.Rev.Lett., 83(1999)2258	G.M.Brown,S.Taga,B.Gogia,K.Kordatos,S.Margadonna,K.Prassides,Y.Iwasa,K.Tanigaki,A.N.Fitch,P.Pattison		
42061	PRL0832258	N(0) = 2.5 states/eV.mol-C60 from kai(P) = 2.2 E-4 emu/mol.	Sr4C60	C60Sr4	C	60	Sr	4																					1999																												fullerene																		K				4.4			4.4																																																																																																react(C60 +Ba or Sr) in Ta-cell.  ANN(550-650C, 12d)					Structural and Electronic Properties of the Noncubic Superconducting Fullerides A'4C60  (A' = Ba, Sr )			School of Chemistry, Physics and Environmental Science, University of Sussex, Brighton, BN1 9QJ, United Kingdom	Phys.Rev.Lett., 83(1999)2258	G.M.Brown,S.Taga,B.Gogia,K.Kordatos,S.Margadonna,K.Prassides,Y.Iwasa,K.Tanigaki,A.N.Fitch,P.Pattison		
42062	NAT3550529	x = 1.5, 3, 4, 4.5, 5, 6, 8 in CaxC60 were prepared and investigated.	Ca5C60	C60Ca5	C	60	Ca	5																					1992																												fullerene			A	14.01														K				8.4			8.4																																																																																														Ca,C60		mixture in Ta-cell in quartz tube. heat(550C, 20h)					Superconductivity at 8.4K in calcium-doped C60			AT&T Bell Lab, New Jersey,USA	Nature, 355(1992)529	A.R.Kortan,N.Kopylov,S.Glarum,E.M.Gyorgy,A.P.Ramirez,R.M.Fleming,F.A.Thiel,R.C.Haddon		
42063	NAT3600566	Tc(on) measured by microwave absorption.	Ba6C60	Ba6C60	Ba	6	C	60																					1992																											1	fullerene			A	11.171														K				7			7										12																																																																																											Superconductivity in barium fulleride			AT&T Bell Lab, New Jersey,USA	Nature, 360(1992)566	A.R.Kortan,N.Kopylov,S.Glarum,E.M.Gyorgy,A.P.Ramirez,R.M.Fleming,O.Zhou,F.A.Thiel,P.L.Trevor,R.C.Haddon		
42064	JAC2750480	RRR = 13.3. (dTn/dP) = 0.08 K/kbar. Tn by resistivity measurement.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	1998								17.5																																						K		1.1				0.2	1.1																																																																																																Czochralski method					Anisotropy of Cr-like anomaly in U1-xCexRu2Si2			Institute of Experimental Physics, SAS, Watsonova 47, 043 53 Kosice, Slovakia	J.Alloy Compd, 275-277(1998)480	S.Matas,M.Mihalik,Z.Amold,J.Kamarad,V.Pavlik,K.Flachbart,A.Menovsky		
42065	JAC2750480	not SC. RRR = 1.6. (dTn/dP) = 0.13 K/kbar. Tn by resistivity measurement.	(U,Ce)Ru2Si2	U0.975Ce0.025Ru2Si2	U	0.975	Ce	0.025	Ru	2	Si	2																3	1998								15.6																																						K					0.35																																																																																																		Czochralski method					Anisotropy of Cr-like anomaly in U1-xCexRu2Si2			Institute of Experimental Physics, SAS, Watsonova 47, 043 53 Kosice, Slovakia	J.Alloy Compd, 275-277(1998)480	S.Matas,M.Mihalik,Z.Amold,J.Kamarad,V.Pavlik,K.Flachbart,A.Menovsky		
42067	MTL0583847		HgPbx	Hg1Pb1.8	Hg	1	Pb	1.8																					2004																												AuCu			A	4.9818		4.55												K	5.5		5.7	5.7			5.7																																																																																																Amalgams(1.8=<x=<2.3 in HgPbx) - sealed in quartz - heat(80C or 120C, 10h) - pellet - ANN(80 or 120 C, 3h)					Superconductivity in the HgPb2 with type AuCu structure			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 58(2004)3847	A.D.Bortolozo,B.Ferreira,C.A.M.dos Santos,M.S.da Luz,R.Ricardo da Silva,A.J.S.Machado		
42068	MTL0583847		HgPbx	Hg1Pb2	Hg	1	Pb	2																					2004																												AuCu			A	4.9861		4.5405												K			5.8				5.8																																																																																																Amalgams(1.8=<x=<2.3 in HgPbx) - sealed in quartz - heat(80C or 120C, 10h) - pellet - ANN(80 or 120 C, 3h)					Superconductivity in the HgPb2 with type AuCu structure			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 58(2004)3847	A.D.Bortolozo,B.Ferreira,C.A.M.dos Santos,M.S.da Luz,R.Ricardo da Silva,A.J.S.Machado		
42069	MTL0583847		HgPbx	Hg1Pb2.1	Hg	1	Pb	2.1																					2004																												AuCu			A	4.9893		4.5476												K			5.85				5.85																																																																																																Amalgams(1.8=<x=<2.3 in HgPbx) - sealed in quartz - heat(80C or 120C, 10h) - pellet - ANN(80 or 120 C, 3h)					Superconductivity in the HgPb2 with type AuCu structure			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 58(2004)3847	A.D.Bortolozo,B.Ferreira,C.A.M.dos Santos,M.S.da Luz,R.Ricardo da Silva,A.J.S.Machado		
42070	MTL0583847	Pb phase(Tc=7.2 K) appears.	HgPbx	Hg1Pb2.3	Hg	1	Pb	2.3																					2004																												AuCu			A	4.9957		4.5512												K			6				6																																																																																																Amalgams(1.8=<x=<2.3 in HgPbx) - sealed in quartz - heat(80C or 120C, 10h) - pellet - ANN(80 or 120 C, 3h)					Superconductivity in the HgPb2 with type AuCu structure			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 58(2004)3847	A.D.Bortolozo,B.Ferreira,C.A.M.dos Santos,M.S.da Luz,R.Ricardo da Silva,A.J.S.Machado		
42071	P075014509	Tc shows Tc(natural-Ca). dTc(natural-Ca - Ca<44>) = 0.57 K. Tc measured by magnetization.	CaC6	C6Ca1	C	6	Ca	1																					2007																												GIC																		K			11.62				11.62						0.55	Ca																																																																																									vapor transport method					Large Ca isotope effect in the CaC6 superconductor			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 75(2007)014509	D.G.Hinks,D.Rosenmann,H.Claus,M.S.Bailey,J.D.Jorgensen		
42072	P075014509	Tc shows Tc(Ca<40>). dTc(Ca<40> - Ca<44>) = 0.53 K. Tc measured by magnetization.	CaC6	C6Ca1	C	6	Ca	1																					2007																												GIC																		K			11.57				11.57						0.5	Ca																																																																																									vapor transport method					Large Ca isotope effect in the CaC6 superconductor			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 75(2007)014509	D.G.Hinks,D.Rosenmann,H.Claus,M.S.Bailey,J.D.Jorgensen		
42073	MTL0610263	Sm occupy Hg vacancies og HgPb2(tetragonal)	HgSm0.5Pb2	Hg1Sm0.5Pb2	Hg	1	Sm	0.5	Pb	2																			2007																												AuCu																		K			5.7	5.7			5.7																																																																																																Amalgams(HgSm0.5Pb2,HgSmPb2,HgSm0.5In0.5Pb2) - in quartz tube - heat (80C,10h) - pellet - ANN(3h)					Superconductivity in a new quaternary phase with HgSm0.5In0.5Pb2 composition			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 61(2007)263	R.Corsini,A.D.Bortolozo,M.S.da Luz,R.Ricardo da Silva,C.A.M.dos Santos,A.J.S.Machado		
42074	MTL0610263	Sm occupy Hg vacancies og HgPb2(tetragonal)	HgSmPb2	Hg1Sm1Pb2	Hg	1	Sm	1	Pb	2																			2007																												AuCu																		K			5.9	5.9			5.9																																																																																																Amalgams(HgSm0.5Pb2,HgSmPb2,HgSm0.5In0.5Pb2) - in quartz tube - heat (80C,10h) - pellet - ANN(3h)					Superconductivity in a new quaternary phase with HgSm0.5In0.5Pb2 composition			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 61(2007)263	R.Corsini,A.D.Bortolozo,M.S.da Luz,R.Ricardo da Silva,C.A.M.dos Santos,A.J.S.Machado		
42075	MTL0610263	Sm and In  occupy Hg vacancies og HgPb2(tetragonal)	Hg(Sm,In)Pb2	Hg1Sm0.5In0.5Pb2	Hg	1	Sm	0.5	In	0.5	Pb	2																	2007																												AuCu			A	4.883		4.8716												K				6.9			6.9	MTC42075																																																																																															Amalgams(HgSm0.5Pb2,HgSmPb2,HgSm0.5In0.5Pb2) - in quartz tube - heat (80C,10h) - pellet - ANN(3h)					Superconductivity in a new quaternary phase with HgSm0.5In0.5Pb2 composition			Departamento de Engenharia de Materiais, Faenquil, C.P. 116, 12600-970, Lorena SP, Brazil	Mater.Lett., 61(2007)263	R.Corsini,A.D.Bortolozo,M.S.da Luz,R.Ricardo da Silva,C.A.M.dos Santos,A.J.S.Machado		
42076	PHC4510082	P-induced SC. Using diamond anvil upto 115 GPa. Tc shows maximum value obtained by this work (P=115 GPa).	Y	Y1	Y	1																							2007																																														K				19.5	0		19.5	MTC42076		K/GPa	0.35																																																																																												Y is cut from an ingot(Aldrich Chemical 99.9%)					Superconductivity at 20 K in yttrium metal at pressures exceeding 1 Mbar			Department of Physics, Washington University, CB 1105, One Brookings Dr, St. Louis, MO 63130, United States	Physica C, 451(2007)82	J.J.Hamlon,V.G.Tissen,J.S.Schilling		
42077	J075083703	P-induced SC. Tc by resistivity. Ca transforms from Ca-IV to Ca-V at 139 GPa. Tc(max) = 25 K at P=161 GPa. Hc2(0) = 12-15 T(P=161 GPa)  estimated .	Ca	Ca1	Ca	1																							2006																																														K				25	0		25	MTC42077																																																																																															99.99 % Ca(Sigma-Aldrich)					Superconductivity of Ca Exceeding 25K at Megabar Pressures			KYOKUGEN, Center for Quantum Science and Technology under Extreme Conditions, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 75(2006)083703	T.Yabuuchi,T.Matsuoka,Y.Nakamoto,K.Shimizu		
42078	MMM3100E31	not bulk SC (no specific heat anomaly). SC sample has superstructure in XRD pattern.	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																		3	2007								2.8																				Ho2CoGa8																		K	0.5		0.8				0.65																																																																																																In-flux method					Relation between superconductivity and superstructure in Ce2RhIn8			aInstitute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Mag.Mag.Mater., 310(2007)e31	M.Koeda,T.Fujiwara,M.Hedo,Y.Uwatoko,H.Sagayama,Y.Wakabayashi,H.Sawa		
42079	MMM3100563	not SC for P < 8 GPa, T > 0.08 K. TCFIG shows Tn(P).	CeIrGe3	Ce1Ir1Ge3	Ce	1	Ir	1	Ge	3																			2007								8.7																				BaNiSn3			A	4.409		10.032												K					0.08			MTC42079																																																																																															Using tetra arc furnace.					Magnetic and superconducting properties of CeIrSi3 and CeIrGe3 without inversion symmetry			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Mag.Mag.Mater., 310(2007)563	Y.Okuda,I.Sugitani,H.Shishido,T.Yamada,A.Thamizhavel,E.Yamamoto,T.D.Matsuda,Y.Haga,T.Takeuchi,R.Settai,Y.Onuki		
42080	MMM3100416	amorphous Ce-Ru alloys prepared by dc sputtering. They are superconducting for x<0.39 in CexRu1-x. SPHEAT shows gamma(x) measured by SP-heat.	a-Ce0.15Ru0.85	Ce0.15Ru0.85	Ce	0.15	Ru	0.85																					2007																												AMOR																		K		3.9					3.9																																																					MSP42080			mJ/mol.K2.	8.26																																					Ce(3N),Ru(3N)		Ce-Ru ingot(arc melting) - dc sputtering					Specific heat of amorphous CexRu100-x alloys			Materials Science of Engineering, Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J.Mag.Mag.Mater., 310(2007)416	Y.Amakai,S.Murayama,H.Takano,M.Mizutani,K.Asano,Y.Obi,K.Takanashi		
42081	PR05907266	CDW-temp = 83 K. SP-jump = 360J/mol.K at 83 K.	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																		3	1999																												Sc5Co4Si10			A	12.4936		4.1852											at 295 K.	K		3.9					3.9																																																																							uOhm.cm												195	60												single crystals were grown in tri-furnace using Czochralski method					Strongly coupled charge-density wave transition in single-crystal Lu5Ir4Si10			Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev.B, 59(1999)7266	B.Becker,N.G.Patil,S.Ramakrishnan,A.A.Menovsky,G.J.Nieuwenhuys,J.A.Mydosh,M.Kohgi,K.Iwasa		
42082	PR04307688	not SC. Tn < 0.052 K.	Yb5Ir4Si10	Yb5Ir4Si10	Yb	5	Ir	4	Si	10																			1991							-58.8																					Sc5Co4Si10			A	12.503		4.182												K					0.052																																																																																																		arc melting - ANN(1250C,1d in quartz ampule,160Torr Ar) - ANN(1050C,3d)					Low temperature physical properties of R5Ir4Si10 (R=Dy,Ho,Er,Tm, and Yb) compounds				Phys.Rev.B, 43(1991)7688	H.D.Yang,P.Klavins,R.N.Shelton		
42083	PR04307688	not SC. another magnetic transition at 0.86 K (SP-heat anomaly).	Tm5Ir4Si10	Tm5Ir4Si10	Tm	5	Ir	4	Si	10																			1991							-27.1	1.9																				Sc5Co4Si10			A	12.513		4.197												K					0.052																																																																																																		arc melting - ANN(1250C,1d in quartz ampule,160Torr Ar) - ANN(1050C,3d)					Low temperature physical properties of R5Ir4Si10 (R=Dy,Ho,Er,Tm, and Yb) compounds				Phys.Rev.B, 43(1991)7688	H.D.Yang,P.Klavins,R.N.Shelton		
42084	PR04307688	not SC.	Er5Ir4Si10	Er5Ir4Si10	Er	5	Ir	4	Si	10																			1991							0.6	3																				Sc5Co4Si10			A	12.54		4.208												K					0.052																																																																																																		arc melting - ANN(1250C,1d in quartz ampule,160Torr Ar) - ANN(1050C,3d)					Low temperature physical properties of R5Ir4Si10 (R=Dy,Ho,Er,Tm, and Yb) compounds				Phys.Rev.B, 43(1991)7688	H.D.Yang,P.Klavins,R.N.Shelton		
42085	PR04307688	not SC.	Ho5Ir4Si10	Ho5Ir4Si10	Ho	5	Ir	4	Si	10																			1991							-13.2	2																				Sc5Co4Si10			A	12.558		4.218												K					0.052																																																																																																		arc melting - ANN(1250C,1d in quartz ampule,160Torr Ar) - ANN(1050C,3d)					Low temperature physical properties of R5Ir4Si10 (R=Dy,Ho,Er,Tm, and Yb) compounds				Phys.Rev.B, 43(1991)7688	H.D.Yang,P.Klavins,R.N.Shelton		
42086	PR04307688	not SC.	Dy5Ir4Si10	Dy5Ir4Si10	Dy	5	Ir	4	Si	10																			1991							-5.9	5																				Sc5Co4Si10			A	12.577		4.237												K					0.052																																																																																																		arc melting - ANN(1250C,1d in quartz ampule,160Torr Ar) - ANN(1050C,3d)					Low temperature physical properties of R5Ir4Si10 (R=Dy,Ho,Er,Tm, and Yb) compounds				Phys.Rev.B, 43(1991)7688	H.D.Yang,P.Klavins,R.N.Shelton		
42087	L089057002	beta-V bronze. P-induced SC. P<crit) = 7.0 GPa.  7 < SC < 9 GPa. M-I transition at 135 K. R measured for I//b-axis. Tc at P=8 GPa. Tc(off) = 6.0 K at P=7.0 GPa.	beta-Na0.33V2O5	Na0.33V2O5	Na	0.33	V	2																	O	5		3	2002								25																																					beta-Vanadium bronze	K			8	6	0		6	PH42087																																																																																															rf-heating Czochralski method.					Pressure-Induced Superconductivity in Beta-Na0.33V2O5 beyond Charge Ordering			Material Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	Phys.Rev.Lett., 89(2002)57002	N.Mori,T.Yamauchi,Y.Ueda		
42088	MMM3100844	P-induced SC. P<crit> = 4.3 GPa. Tc shows at 5.5 GPa.	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																			2007								21																				BaNiSn3																		K			0.7		0		0.7																																																																																																arc melting - wrapped in Ta-foil - sealed in vac - ANN(850C,1w)					Pressure-induced superconductivity in CeCoGe3 without inversion symmetry			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Mag.Mag.Mater., 310(2007)844	R.Settai,I.Sugitani,Y.Okuda,A.Thamizhavel,M.Nakashima,Y.Onuki,H.Harima		
42089	MMM3100207	T<CDW> = 83 K. C<CDW> = 8.5 mj/mol.K. e-ph coupling = 0.43.	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			2007																												Sc5Co4Si10																		K		3.9		3.75			3.9																																																																																																					Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42090	MMM3100207	T<CDW> = 75 K.  C<CDW> = 6.8 mj/mol.K.	Lu5Ir4(Si,Ge)10	Lu5Ir4Si9.95Ge0.05	Lu	5	Ir	4	Si	9.95	Ge	0.05																	2007																												Sc5Co4Si10																		K		4.1		4.03			4.1																																																																																																					Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42091	MMM3100207	T<CDW> = 64 K. C<CDW> = 3.9 mj/mol.K.	Lu5Ir4(Si,Ge)10	Lu5Ir4Si9.9Ge0.1	Lu	5	Ir	4	Si	9.9	Ge	0.1																	2007																												Sc5Co4Si10																		K		4.7		4.82			4.7																																																																																																					Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42092	MMM3100207	T<CDW> = 51 K. C<CDW> = 1.5 mj/mol.K.	Lu5Ir4(Si,Ge)10	Lu5Ir4Si9.8Ge0.2	Lu	5	Ir	4	Si	9.8	Ge	0.2																	2007																												Sc5Co4Si10																		K		5.8		5.78			5.8																																																																																																					Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42093	MMM3100207	T<CDW> = 47 K. C<CDW> = 0.75 mj/mol.K.	Lu5Ir4(Si,Ge)10	Lu5Ir4Si9.5Ge0.5	Lu	5	Ir	4	Si	9.5	Ge	0.5																	2007																												Sc5Co4Si10																		K		6		6.08			6																																																																																																					Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42094	MMM3100207	no CDW.	Lu5Ir4(Si,Ge)10	Lu5Ir4Si9Ge1	Lu	5	Ir	4	Si	9	Ge	1																	2007																												Sc5Co4Si10																		K				6.38			6.38	MTC42094																																																																																																				Multiple phase transitions in rare earth R5T4M10 (T = Rh, Ir and M=Si, Sn)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai-400005, India	J.Mag.Mag.Mater., 310(2007)207	S.Ramakrishnan,J.A.Mydosh		
42095	P063024504	ANN(500C,6d in vac). Tc<2K. TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8986														K					2																																																																				uV/K	144																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42096	P063024504	ANN(450C,10d in vac). Tc<2K. TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8948														K					2																																																																				uV/K	109																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42097	P063024504	ANN(400C,10d in vac). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.894														K				26			26																																																																		uV/K	80																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42098	P063024504	ANN(350C,6d in vac). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.892														K				46			46																																																																		uV/K	60																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42099	P063024504	ANN(300C,10d in vac). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8895														K				62			62																																																																		uV/K	48																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42100	P063024504	ANN(400C,10d in Ar). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8869														K				72			72																																																																		uV/K	25																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42101	P063024504	ANN(350C,10d in Ar). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8853														K				77			77																																																																		uV/K	17																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42102	P063024504	ANN(300C,8d in Ar). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8843														K				83			83																																																																		uV/K	9																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42103	P063024504	ANN(300C,7d in O20.01%-Ar). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8825														K				91			91																																																																		uV/K	7																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42104	P063024504	ANN(300C,7d in O20.1%-Ar). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.881														K				95			95																																																																		uV/K	6																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42105	P063024504	ANN(300C,7d in O2). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8789														K				98			98																																																																		uV/K	3.2																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42106	P063024504	ANN(240C,21d in O2). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.8759														K				92			92																																																																		uV/K	-0.1																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42107	P063024504	ANN(320C,8d in 6atm-O2). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.875														K				86			86																																																																		uV/K	-3																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42108	P063024504	ANN(270C,8d in 6atm-O2). TP300 = TP(290K). P determined from TP(290K) using TP(290K)-p relation.	HgBa2CuOz	Hg1Ba2Cu1O4+z	Hg	1	Ba	2	Cu	1															O	4+z			2001																												Hg1201			A	3.743														K				80			80																																																																		uV/K	-4.5																											HgO,BaO,CuO	1	solid state reaction. To minimize C-impurity, HgO and BaO made using special process.					Thermoelectric power and resistivity of HgBa2CuO4+z  over a wide doping range			Superconductivity Research Laboratory, International Superconductivity Technology Center, 1-10-13 Shinonome, Koto-ku Tokyo 135-0062, Japan	Phys.Rev.B, 63(2001)024504	A.Yamamoto,Wei-Zhi Hu,S.Tajima		
42109	PHY0550663	GAMMA calculated from Hc. Gruneizen const. = 2.6.	Al	Al1	Al	1																							1971																																														K		1.159					1.159																																		MHC42109																						mJ/mol.K2	1.67																																												Critical magnetic fields of aluminum, gallium and thorium under pressure and the isotope effect of cadmium				Physica, 55(1971)663	C.Palmy,R.Flach,P.de Trey		
42110	PHY0550663	GAMMA calculated from Hc. Gruneizen const. = -0.4.	Ga	Ga1	Ga	1																							1971																																														K		1.061					1.061	MTC42110		K/GPa	-0.138																														MHC42110																						mJ/mol.K2	0.53																																												Critical magnetic fields of aluminum, gallium and thorium under pressure and the isotope effect of cadmium				Physica, 55(1971)663	C.Palmy,R.Flach,P.de Trey		
42111	PHY0550663	GAMMA calculated from Hc. Gruneizen const. = 0.57.	Th	Th1	Th	1																							1971																																														K		1.38					1.38	MTC42111		K/GPa	-0.13																														MHC42111																						mJ/mol.K2	4.33																																												Critical magnetic fields of aluminum, gallium and thorium under pressure and the isotope effect of cadmium				Physica, 55(1971)663	C.Palmy,R.Flach,P.de Trey		
42112	PHY0550663		Cd	Cd1	Cd	1																							1971																																														K		0.541					0.541						0.32	Cd																																																																																														Critical magnetic fields of aluminum, gallium and thorium under pressure and the isotope effect of cadmium				Physica, 55(1971)663	C.Palmy,R.Flach,P.de Trey		
42114	P075054513	G-L parameter = 20.	Ba8Si40Ga6	Ba8Si40Ga6	Ba	8	Si	40	Ga	6																			2007																												clathrate	Pm3[-]n	223	A	10.4261														K		3.3					3.3										96	Oe		35							kOe		8.5														A	from Hc2	200			A	calculated using G-L theory	3700																																																			Ba,Si,Ga		multistep melting in Ar, then solid state reaction					Superconductivity in gallium-substituted Ba8Si46 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Phys.Rev.B, 75(2007)054513	Y.Li,R.Zhang,Y.Liu,N.Chen,Z.P.Luo,X.Ma,G.Cao,Z.S.Feng,Chia-Ren Hu,J.H.Ross,Jr.		
42115	P075054513	not SC at 1.8 K.	Ba8Si36Ga10	Ba8Si36Ga10	Ba	8	Si	36	Ga	10																			2007																												clathrate	Pm3[-]n	223	A	10.4896														K					1.8																																																																																																Ba,Si,Ga		multistep melting in Ar, then solid state reaction					Superconductivity in gallium-substituted Ba8Si46 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Phys.Rev.B, 75(2007)054513	Y.Li,R.Zhang,Y.Liu,N.Chen,Z.P.Luo,X.Ma,G.Cao,Z.S.Feng,Chia-Ren Hu,J.H.Ross,Jr.		
42116	P075060503	T<CDW> = 250 K. e-ph = 0.45. (dC/gamma*Tc) = 1.35. G-L parameter = 151.	Bi2Rh3Se2	Bi2Rh3Se2	Bi	2	Rh	3	Se	2																			2007																															A	11.414	8.3709	11.989											parkerite-type structure. beta = 89.153 deg.	K	0.76	0.84	0.9				0.84											Oe	from Hc(0) using G-L theory	1.2							T	resistive transition	1.13							T/K		1.95			MHC42116		A	from Hc2	171			um	from Hc(0), Hc1 using G-L theory	2.57													mJ/mol.K2	9.5	SP	194	SP																																				mixture - heat(1320K,6h in silica tube) - Q					Charge-density-wave superconductor Bi2Rh3Se2			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	Phys.Rev.B, 75(2007)060503R	T.Sakamoto,M.Wakeshima,Y.Hinatsu,K.Matsuhira		
42117	P075064517	Tc=2.0 K from SP-heat. quasi-1D superconductor. residual resistivity at 4.0 K. // means //Nb-chain. e-ph = 1.05.  Hc2(0) by linear approx.	Nb2Se3	Nb2Se3	Nb	2	Se	3																					2007																													P<21/m>		A	5.505	3.4349	9.2369											monoclinic, beta=130.160 deg.	K	2.2		2.4				2.3																				T	resistive transition		1.4	0.75										MHC42117		A	from Hc2		203	153																mJ/mol.K2	9.96	SP	223	SP											uOhm.cm								26	105																single crystals were grown using a molten metallic flux method.					Anisotropy of electrical transport and superconductivity in metal chains of Nb2Se3			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 75(2007)064517	R.Hu,K.Lauritch-Kullas,J.O'Brian,V.F.Mitrovic,C.Petrovic		
42118	PHB3780857	Amorphous superconductig region, x=15 =< SC < 47 at%.	a-CexRu1-x	Ce0.147Ru0.853	Ce	0.147	Ru	0.853																					2006																												AMOR																		K		3.6					3.6																																																																																																Amorphous samples fabricated by a DC high-rate sputtering method.					Heavy fermion like behavior and superconductivity in amorphous CexRu100-x alloy			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Physica B, 378-380(2006)857	Y.Obi,S.Murayama,Y.Amakai,Y.Okada,K.Asano		
42119	PHB3780857	not SC.	a-CexRu1-x	Ce0.805Ru0.195	Ce	0.805	Ru	0.195																					2006																																														K					1.8																																																																																																		Amorphous samples fabricated by a DC high-rate sputtering method.					Heavy fermion like behavior and superconductivity in amorphous CexRu100-x alloy			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Physica B, 378-380(2006)857	Y.Obi,S.Murayama,Y.Amakai,Y.Okada,K.Asano		
42120	PHC4500071		(Ca,La)(Ba,La)2Cu3Oz	Ca0.1La1.15Ba1.75Cu3O7.148	Ca	0.1	La	1.15	Ba	1.75	Cu	3													O	7+z	7.148	1	2006																												Y123																		K		57.1					57.1	MTC42120																																																																																																				Quantum critical point, scaling and universality in high Tc (CaxLa1-x)(Ba2-c-xLac+x)Cu3Oy			Department of Physics, Technion, Haifa 32000, Israel	Physica C, 450(2006)71	B.Watkins,H.Chashka,Y.Direktovich,A.Knizhnik,Y.Eckstein		
42121	P072045106		Lu5Ir4(Si,Ge)10	Lu5Ir4Si8Ge2	Lu	5	Ir	4	Si	8	Ge	2																	2005																												Sc5Co4Si10			A	12.4837		4.1781												K				6.6			6.6	MTC42121																																																																																															arc melting					Competition between superconductivity and charge-density-wave ordering in the Lu5Ir4(Si1-xGex)10 alloy system			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 72(2005)045106	Y.Singh,R.Nirmala,S.Ramakrishnan,S.K.Malik		
42122	P072045106		Lu5Ir4(Si,Ge)10	Lu5Ir4Si6Ge4	Lu	5	Ir	4	Si	6	Ge	4																	2005																												Sc5Co4Si10			A	12.6082		4.2008												K				5.1			5.1																																																																																																arc melting					Competition between superconductivity and charge-density-wave ordering in the Lu5Ir4(Si1-xGex)10 alloy system			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 72(2005)045106	Y.Singh,R.Nirmala,S.Ramakrishnan,S.K.Malik		
42123	P072045106		Lu5Ir4Ge10	Lu5Ir4Ge10	Lu	5	Ir	4	Ge	10																			2005																												Sc5Co4Si10			A	12.8281		4.2415												K				2.5			2.5																																																																																																arc melting					Competition between superconductivity and charge-density-wave ordering in the Lu5Ir4(Si1-xGex)10 alloy system			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 72(2005)045106	Y.Singh,R.Nirmala,S.Ramakrishnan,S.K.Malik		
42124	PLA3450398		Ba8Si42Cu4	Ba8Si42Cu4	Ba	8	Si	42	Cu	4																		1	2005																												clathrate	Pm3[-]n	223	A	10.3257														K				2.9			2.9											Oe	M-H curve	30																												A	calculated from Hc1	1480																																																					multistep melting in Ar, then solid state reaction					Vacancy and copper-doping effect on superconductivity for clathrate materials			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Phys.Lett.A, 345(2005)398	Y.Li,Y.Liu,N.Chen,G.Cao,Z.Feng,J.H.Ross Jr.		
42125	PHC4530012	not SC. dTc/dp value for 40 < P < 60 GPa. P<crit> = 9.4 GPa (linear extraporation to Tc=0 K).	omega-Ti	Ti1	Ti	1																							2007																																													hexagonal	K					0.06			MTC42125		K/GPa	0.07																																																																																												electron-arc melting in vac.					Superconducting temperature of the x-phase in Ti, Zr and Hf metals at high pressures			Institute of Solid State Physics, Russian Academy of Sciences, 142432 Chernogolovka, Moscow District, Russia	Physica C, 453(2007)12	I.O.Bashkin,V.G.Tissen,M.V.Nefedova,E.G.Ponyatovsky		
42126	PHC4500124	impuriti phases = MgCu2,MgO	(Mg,Cu)B2	Mg0.95Cu0.05B2	Mg	0.95	Cu	0.05	B	2																			2006																												AlB2			A	3.087		3.524												K	36.9		38.6			1.7	37.75																																																																																																mixture - pellet - wrapped in Ta foil - heat(850C, in Ar flow)					Effect of Cu doping in MgB2 superconductor at various processing temperatures			Superconductivity Research Laboratory, Department of Physics, Barkatullah University, Bhopal 462026, India	Physica C, 450(2006)124	K.Singh,R.Mohan,N.Kaur,N.K.Gaur,M.Dixit,V.Shelke,R.K.Singh		
42127	L091247001	Tc defined as maximum of (dR/dT) in  (dR/dT) vs T plot. (dTc/da) = 17.1 K/A for pressure effect.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2003																												clathrate																		K		8.4					8.4	MTC42127																																																																																															mixed(BaSi2 + Si powder) - SIN(1000K,5GPa,in h-BN cell) - Q					Superconductivity in Doped sp3 Semiconductors: The Case of the Clathrates			LPMCN, Universite Claude Bernard Lyon I and CNRS, UMR 5586, Batiment Brillouin, 43 Bd du 11 Novembre 1918, 69622 Villeurbanne Cedex, France	Phys.Rev.Lett., 91(2003)247001	D.Connetable,V.Timoshevskii,B.Masenelli,J.Beille,J.Marcus,B.Barbara,A.M.Saitta,G.-M.Rignanese,P.Melinon,S.Yamanaka,X.Blase		
42128	PHB2890385	G-L = 56. H//c-axis for muon-SR.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2000																												clathrate																		K		8					8																				T	magnetization	6.5												MHC42128		A	from Hc2	72			A	muon-SR	4000																																																					"See ""fullerene Sci.Tech., 3(1998)7686"""					Muon spin relaxation measurements of magnetic-field penetration depth in Ba8Si46			Department of Physics, Columbia University, 538 West 120th St., New York, NY 10027, USA	Physica B, 289-290(2000)385	I.M.Gat,Y.Fudamoto,A.Kinkhabwala,M.I.Larkin,G.M.Luke,J.Merrin,B.Nachumi,Y.J.Uemura,K.M.Kojima,E.Eiji,S.Yamanaka		
42129	PHC4080869	2nd transition at Tc = 4K. XRD peaks of Ba-Ge compounds except for clathrate not seen.	Ba8Ge46	Ba8Ge46	Ba	8	Ge	46																					2004																												clathrate																		K				10			10																																																																																																high temperature reaction					Study of superconducting Ba-Ge-Co compounds			aDepartment of Physics, Texas A&M University, College Station, TX 77843-4242, USA	Physica C, 408(2004)869	Yang Li,J.H.Ross Jr.,J.A.Larrea,Elisa Baggio-Saitovitch		
42130	PHC4080869	Tc=10K phase(maybe Co-free clathrate) observed.	Ba8(Ge,Co)46	Ba8Ge42Co4	Ba	8	Ge	42	Co	4																			2004																												clathrate																		K				7			7																																																																																																high temperature reaction					Study of superconducting Ba-Ge-Co compounds			aDepartment of Physics, Texas A&M University, College Station, TX 77843-4242, USA	Physica C, 408(2004)869	Yang Li,J.H.Ross Jr.,J.A.Larrea,Elisa Baggio-Saitovitch		
42131	P075104505	Cu-content determined from lat-c. anisotropy(Hc2(sb)/Hc2c) = 1.7 at 0.35 K. almost T-independent. G-L = 25(H//ab), = 13.4(H//c). gammma in mJ/mol-Ti.K2.	Cu0.07TiSe2	Cu0.07Ti1Se2	Cu	0.07	Ti	1	Se	2																		3	2007																																													hexagonal	K		3.9				0.1	3.9											Oe			32	53			13	1.8	T	resistive		1.238	0.729												A	from Hc2		213	125	A			2850	5840											mJ/mol.K2	4.3														uOhm.cm							80																		single crystals were grown by Cl-vapor transport.					Anisotropic properties of the layered superconductor Cu0.07TiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	Phys.Rev.B, 75(2007)104505	E.Morosan,Lu Li,N.P.Ong,R.J.Cava		
42132	P075104518	hole concentration p = 0.188, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		84					84																																														meV	40	11.2	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42133	P075104518	hole concentration p = 0.203, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		76					76																																														meV	22	6.8	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42134	P075104518	hole concentration p = 0.209, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		72					72																																														meV	23	7.6	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42135	P075104518	hole concentration p = 0.214, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		68					68																																														meV	28	9.6	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42136	P075104518	hole concentration p = 0.252, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		27					27																																														meV	9.5	8.2	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42137	P075104518	hole concentration p = 0.253, estimated using Tallon's eq. energy gap from thermal conductivity using d-wave SC theory.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2007																												Tl2201																		K		26					26																																														meV	6.7	6	3																																															flux method. optimal sample (500C,in vac). overdoped samples (400-480C, in 50-60 mbar-O2)					Doping dependence of the superconducting gap in Tl2Ba2CuO6+z from heat transport			Department of Physics, University of Toronto, Toronto, Canada M5S 1A7	Phys.Rev.B, 75(2007)104518	D.G.Hawthom,S.Y.Li,M.Sutherland,Etienne Boaknin,R.W.Hill,C.Proust,F.Ronning,M.A.Tanatar,D.Peets,R.Liang,D.A.Bonn,W.N.Hardy,N.N.Kolesnikov		
42138	NAP0020544	RRR = 0.5. T<CDW> = 217 K.	TiSe2	Se2Ti1	Se	2	Ti	1																					2006																															A	3.5388		6.0098												K					0.8																																																																				uV/K	23.3																																		Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42139	NAP0020544	RRR = 3.2. T<CDW> = 180 K. gamma in mJ/mol(Ti).K2	CuxTiSe2	Cu0.02Ti1Se2	Cu	0.02	Ti	1	Se	2																			2006																															A	3.5404		6.0156												K					0.8			MTC42142																																																							mJ/mol.K2	1.6									uV/K	-80																																		Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42140	NAP0020544		CuxTiSe2	Cu0.045Ti1Se2	Cu	0.045	Ti	1	Se	2																			2006																																														K		0.95					0.95																																																																																																					Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42141	NAP0020544	T<CDW> = 94.6 K.	CuxTiSe2	Cu0.05Ti1Se2	Cu	0.05	Ti	1	Se	2																			2006																																														K		1.4					1.4																																																																																																					Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42142	NAP0020544	RRR = 3.3T<CDW> = 60.5 K.	CuxTiSe2	Cu0.06Ti1Se2	Cu	0.06	Ti	1	Se	2																			2006																															A	3.5436		6.0273												K		2.39					2.39	LAT42142																																																																	uV/K	-66.5																																		Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42143	NAP0020544	RRR = 5.39. gamma in mJ/mol(Ti).K2	CuxTiSe2	Cu0.08Ti1Se2	Cu	0.08	Ti	1	Se	2																			2006																															A	3.5447		6.0354												K		4.15					4.15	MTC42142																																	MHC42143																			MSP42143			mJ/mol.K2	4.34									uV/K	-49.3																																		Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42144	NAP0020544	RRR = 5.39	CuxTiSe2	Cu0.1Ti1Se2	Cu	0.1	Ti	1	Se	2																			2006																															A	3.546		6.0436												K		2.68					2.68																																																																		uV/K	-49.9																																		Superconductivity in CuxTiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	NaturePhys., 2(2006)544	E.Morosan,H.W.Zandbergen,B.S.Dennis,J.W.G.Bos,Y.Onose,T.Klimczuk,A.P.Ramirez,N.P.Ong,R.J.Cava		
42145	PHC4540030	Tm defined as peak of M-T curve. Hc2(0) estimated by fitting : Hc2 = Hc2(0)*(1-t^2)^a.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2007								130																				Ru1212	P4/mmm		A	3.8389		11.5652												K		39					39																				T	resistive	52														A	from Hc2	25																																	mOhm.cm											15												Ru,Ir,SrCO3,Gd2O3,CuO		precursor(Sr2GdRu1-xIrxO6) was prepared by heating(1250C,12h,in air). Then added CuO - SIN(1060C,72h,in flowing O2)					Effect of Ir substitution in the ferromagnetic superconductor RuSr2GdCu2O8			aInstituto de Fisica, Universidade de Sao Paulo, CP 66318, 05315-970 Sao Paulo, SP, Brazil	Physica C, 454(2007)30	A.R.Jurelo,S.Andrade,R.F.Jardim,F.C.Fonseca,M.S.Torikachvili,A.H.Lacerda,L.Ben-Dor		
42146	PHC4540030	Tm defined as peak of M-T curve. Hc2(0) estimated by fitting : Hc2 = Hc2(0)*(1-t^2)^a.	(Ru,Ir)Sr2GdCu2O8	Ru0.98Ir0.02Sr2Gd1Cu2O8	Ru	0.98	Ir	0.02	Sr	2	Gd	1	Cu	2											O	8		1	2007								126																				Ru1212	P4/mmm																	K		38					38																				T	resistive	53														A	from Hc2	24																																																								Ru,Ir,SrCO3,Gd2O3,CuO		precursor(Sr2GdRu1-xIrxO6) was prepared by heating(1250C,12h,in air). Then added CuO - SIN(1060C,72h,in flowing O2)					Effect of Ir substitution in the ferromagnetic superconductor RuSr2GdCu2O8			aInstituto de Fisica, Universidade de Sao Paulo, CP 66318, 05315-970 Sao Paulo, SP, Brazil	Physica C, 454(2007)30	A.R.Jurelo,S.Andrade,R.F.Jardim,F.C.Fonseca,M.S.Torikachvili,A.H.Lacerda,L.Ben-Dor		
42147	PHC4540030	Tm defined as peak of M-T curve. Hc2(0) estimated by fitting : Hc2 = Hc2(0)*(1-t^2)^a.	(Ru,Ir)Sr2GdCu2O8	Ru0.95Ir0.05Sr2Gd1Cu2O8	Ru	0.95	Ir	0.05	Sr	2	Gd	1	Cu	2											O	8		1	2007								120																				Ru1212	P4/mmm																	K		32.5					32.5																				T	resistive	53														A	from Hc2	24																																																								Ru,Ir,SrCO3,Gd2O3,CuO		precursor(Sr2GdRu1-xIrxO6) was prepared by heating(1250C,12h,in air). Then added CuO - SIN(1060C,72h,in flowing O2)					Effect of Ir substitution in the ferromagnetic superconductor RuSr2GdCu2O8			aInstituto de Fisica, Universidade de Sao Paulo, CP 66318, 05315-970 Sao Paulo, SP, Brazil	Physica C, 454(2007)30	A.R.Jurelo,S.Andrade,R.F.Jardim,F.C.Fonseca,M.S.Torikachvili,A.H.Lacerda,L.Ben-Dor		
42148	PHC4540030	Tm defined as peak of M-T curve. Hc2(0) estimated by fitting : Hc2 = Hc2(0)*(1-t^2)^a.	(Ru,Ir)Sr2GdCu2O8	Ru0.9Ir0.1Sr2Gd1Cu2O8	Ru	0.9	Ir	0.1	Sr	2	Gd	1	Cu	2											O	8		1	2007								112																				Ru1212	P4/mmm		A	3.8399		11.5644												K		22					22																				T	resistive	54														A	from Hc2	24																																	mOhm.cm											21												Ru,Ir,SrCO3,Gd2O3,CuO		precursor(Sr2GdRu1-xIrxO6) was prepared by heating(1250C,12h,in air). Then added CuO - SIN(1060C,72h,in flowing O2)					Effect of Ir substitution in the ferromagnetic superconductor RuSr2GdCu2O8			aInstituto de Fisica, Universidade de Sao Paulo, CP 66318, 05315-970 Sao Paulo, SP, Brazil	Physica C, 454(2007)30	A.R.Jurelo,S.Andrade,R.F.Jardim,F.C.Fonseca,M.S.Torikachvili,A.H.Lacerda,L.Ben-Dor		
42149	PHC4510134	Hc2 measured and defined by new analysis of M(H).	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2007																																														K				6.87			6.87																				T	fitting of M(H)	3.48														A	from Hc2	97			A	from cohere and G-L parameter	3000																																																										Temperature dependences of the upper critical field and Ginzburg-Landau parameter of Li2Pd3B from magnetization measurements			Physik-Institut der Universitat Zurich, Zurich,Switzerland	Physica C, 451(2007)134	I.L.Landau,R.Khasanov,K.Togano,H.Keller		
42150	J076034714	Tc decreases with increasing a. SP-heat measured for sample c(a = 3.846 A, Tc-2.5 K). G-L parameter = 23.	CdCNi3	Cd1C1Ni3	Cd	1	C	1	Ni	3																			2007																												CaTiO3			A	3.844														K		3.2		3.2			3.2											mT	M-H curve, t2-fitting	8.6							T	resistive, WHH fitting	2.2														A	from Hc2	122			A	G-L theory using Hc1	2767													mJ/mol.K2	18	SP-heat	352	SP-heat																																				powder mixture(Cd:C:Ni=1.1:1:3) - BN cell - high pressure synthesis(900C,3.5 GPa, 1h) - SIN(900-1100C, 3.5 GPa, 0.5-1.0 h)					Superconducting Properties of CdCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Hodogaya-ku, Yokohama 240-8501	J.Phys.Soc.Jpn, 76(2007)034714	M.Uehara,T.Yamazaki,T.Kori,T.Kashida,Y.Kimishima,I.Hase		
42151	J076034714	Tc decreases with increasing a. SP-heat measured for sample c(a = 3.846 A, Tc-2.5 K). G-L parameter = 32.	CdCNi3	Cd1C1Ni3	Cd	1	C	1	Ni	3																			2007																												CaTiO3			A	3.845														K		2.8		2.8			2.8											mT	M-H curve, t2-fitting	3.6							T	resistive, WHH fitting	1.8														A	from Hc2	135			A	G-L theory using Hc1	4276													mJ/mol.K2	18	SP-heat	352	SP-heat																																				powder mixture(Cd:C:Ni=1.1:1:3) - BN cell - high pressure synthesis(900C,3.5 GPa, 1h) - SIN(900-1100C, 3.5 GPa, 0.5-1.0 h)					Superconducting Properties of CdCNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Hodogaya-ku, Yokohama 240-8501	J.Phys.Soc.Jpn, 76(2007)034714	M.Uehara,T.Yamazaki,T.Kori,T.Kashida,Y.Kimishima,I.Hase		
42152	P073245106	not SC	GaCNi3	Ga1C1Ni3	Ga	1	C	1	Ni	3																			2006	emu/mol	0.0039	emh.K/mol	0.21			-19.1																					CaTiO3			A	3.604														K					2																																																										mJ/mol.K2	25.3	SP-heat	448	SP-heat																																									Strong electron-electron correlation in the antiperovskite compound GaCNi3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 73(2006)245106	P.Tong,Y.P.Sun,X.B.Zhu,W.H.Song		
42153	J076044708	RRR=100, Rn=0.40 uOhm.cm for J//[110]. RRR=110, Rn=0.48 uOhm.cm for J//[001]. (dC/gamma*Tc) = 0.8	LaIrSi3	La1Ir1Si3	La	1	Ir	1	Si	3																		3	2007																												BaNiSn3																		K		0.77					0.77																																																								mJ/mol.K2	4.5	SP-heat	225	SP-heat																																									Magnetic and Superconducting Properties of LaIrSi3 and CeIrSi3 with the Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)044708	Y.Okuda,Y.Miyauchi,Y.Ida,Y.Takeda,C.Tonohiro,Y.Oduchi,T.Yamada,N.duc Dong,T.D.Matsuda,Y.Haga,T.Takeuchi,M.Hagiwara,K.Kindo,H.Harima,K.Sugiyama,R.Settai,Y.Onuki		
42154	J076044708	P-induced SC. SC properties measured at 2.65 GPa. RRR=200, Rn=0.71 uOhm.cm,  for J//[110]. RRR=130, Rn=1.03 uOhm.cm, Tc = 1.62 K, Hc=9.5 T, (-(dHc2/dT) = 13.0 T/K  for J//[001].	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2007								5																				BaNiSn3																		K		1.59			0		1.59																				T		30							T/K		20			MHC42154																																																																			Magnetic and Superconducting Properties of LaIrSi3 and CeIrSi3 with the Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)044708	Y.Okuda,Y.Miyauchi,Y.Ida,Y.Takeda,C.Tonohiro,Y.Oduchi,T.Yamada,N.duc Dong,T.D.Matsuda,Y.Haga,T.Takeuchi,M.Hagiwara,K.Kindo,H.Harima,K.Sugiyama,R.Settai,Y.Onuki		
42155	J076044708		Ce(Ir,Co)Si3	Ce1Ir0.8Co0.2Si3	Ce	1	Ir	0.8	Co	0.2	Si	3																	2007								4																				BaNiSn3																		K		0.62					0.62																				T		4.2												MHC42155																																																														arc-melting, then ANN(900C)					Magnetic and Superconducting Properties of LaIrSi3 and CeIrSi3 with the Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)044708	Y.Okuda,Y.Miyauchi,Y.Ida,Y.Takeda,C.Tonohiro,Y.Oduchi,T.Yamada,N.duc Dong,T.D.Matsuda,Y.Haga,T.Takeuchi,M.Hagiwara,K.Kindo,H.Harima,K.Sugiyama,R.Settai,Y.Onuki		
42156	J076044708	not single phase. lattice parameter shows x=0.2 from Vegard's law.	Ce(Ir,Co)Si3	Ce1Ir0.65Co0.35Si3	Ce	1	Ir	0.65	Co	0.35	Si	3																	2007								0																				BaNiSn3			A	4.221		9.766												K		0.75					0.75																				T		5.2							T/K		15			MHC42155																																																														arc-melting, then ANN(900C)					Magnetic and Superconducting Properties of LaIrSi3 and CeIrSi3 with the Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)044708	Y.Okuda,Y.Miyauchi,Y.Ida,Y.Takeda,C.Tonohiro,Y.Oduchi,T.Yamada,N.duc Dong,T.D.Matsuda,Y.Haga,T.Takeuchi,M.Hagiwara,K.Kindo,H.Harima,K.Sugiyama,R.Settai,Y.Onuki		
42157	SNM0200249	tetermination of O-content not given. Tc shows Tc(max).	RbxWO3	Rb0.19W1O3.001	Rb	0.19	W	1																	O	3	3.001		2007																												bronze	P63/mcm																hexagonal	K		5.02					5.02																																																																																														Rb2WO4,WO3,W		mixture - pellet - sealed in vac - heat(650C,5h) - heat(850C,15h)					Effect of Oxygen Concentration on Superconducting Properties of Rubidium Tungsten Bronzes RbxWOy			Department of Physics, Tamkang University, Tamsui 251, Taiwan, ROC.	J.Supercond.Nov. Magn., 2(2007)249	L.C.Ting,H.H.Hsieh,H.H.Kang,D.C.Ling,H.L.Liu,W.F.Pong,F.Z.Chien,P.H.Hor		
42158	SNM0200249	tetermination of O-content not given. Tc shows Tc(max).	RbxWO3	Rb0.23W1O3.05	Rb	0.23	W	1																	O	3	3.05		2007																												bronze	P63/mcm																hexagonal	K		5.01					5.01																																																																																														Rb2WO4,WO3,W		mixture - pellet - sealed in vac - heat(650C,5h) - heat(850C,15h)					Effect of Oxygen Concentration on Superconducting Properties of Rubidium Tungsten Bronzes RbxWOy			Department of Physics, Tamkang University, Tamsui 251, Taiwan, ROC.	J.Supercond.Nov. Magn., 2(2007)249	L.C.Ting,H.H.Hsieh,H.H.Kang,D.C.Ling,H.L.Liu,W.F.Pong,F.Z.Chien,P.H.Hor		
42159	SNM0200249	tetermination of O-content not given. Tc shows Tc(max).	RbxWO3	Rb0.27W1O2.93	Rb	0.27	W	1																	O	3	2.93		2007																												bronze	P63/mcm																hexagonal	K		3					3																																																																																														Rb2WO4,WO3,W		mixture - pellet - sealed in vac - heat(650C,5h) - heat(850C,15h)					Effect of Oxygen Concentration on Superconducting Properties of Rubidium Tungsten Bronzes RbxWOy			Department of Physics, Tamkang University, Tamsui 251, Taiwan, ROC.	J.Supercond.Nov. Magn., 2(2007)249	L.C.Ting,H.H.Hsieh,H.H.Kang,D.C.Ling,H.L.Liu,W.F.Pong,F.Z.Chien,P.H.Hor		
42160	C019016218	Tc(SP) = 3.61K. Hc(0) = 16.9 mT calculated from SP-heat data. (dC/gamma*Tc) = 1.46. G-L parameter = 34.1	La6ZnSb15	La6Zn1Sb15	La	6	Zn	1	Sb	15																		1	2007																												La6MnSb15	Imm2		A	15.37	19.42	4.361												K	3.65	3.74	3.85				3.74										19.2	Oe	calculate using Hc(0)	12.3							T	resistive	0.81												MHC42160		A	calculate using Hc(0)	201			A	calculate using Hc(0)	6850					3.09	14																																													powder of La,Zn,Sb		mixture - pellet - sealed in quartz tube(vac) - heat(600C,3h) - heat(600-900C,100h), several times.					Superconductivity in the ternary antimonide La6ZnSb15			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	J. Phys.: Condens. Matter 19 (2007) 016218	M.Wakeshima,C.Sakai,Y.Hinatsu		
42161	C019176230	Thermal expansion coefficient measured.	CuxTiSe2	Cu0.06Ti2Se2	Cu	0.06	Ti	2	Se	2																		1	2007																																														K				2			2	MTC42161		K/GPa	0.54																																																																																												two step solid state reaction					Thermal expansion and effect of pressure on superconductivity in CuxTiSe2			Ames Laboratory US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J. Phys.: Condens. Matter, 19(2007)176230	B.L.Bud'ko,P.C.Canfield,E.Morosan,R.J.Cava,G.M.Schmiedeshoff		
42162	C019176230	Thermal expansion coefficient measured.	CuxTiSe2	Cu0.08Ti2Se2	Cu	0.08	Ti	2	Se	2																		1	2007																																														K				3.95			3.95	MTC42161																																																																																															two step solid state reaction					Thermal expansion and effect of pressure on superconductivity in CuxTiSe2			Ames Laboratory US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J. Phys.: Condens. Matter, 19(2007)176230	B.L.Bud'ko,P.C.Canfield,E.Morosan,R.J.Cava,G.M.Schmiedeshoff		
42163	C019176230	Thermal expansion coefficient measured.	CuxTiSe2	Cu0.1Ti2Se2	Cu	0.1	Ti	2	Se	2																		1	2007																																														K				2.95			2.95	MTC42161		K/GPa	-0.18																																																																																												two step solid state reaction					Thermal expansion and effect of pressure on superconductivity in CuxTiSe2			Ames Laboratory US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J. Phys.: Condens. Matter, 19(2007)176230	B.L.Bud'ko,P.C.Canfield,E.Morosan,R.J.Cava,G.M.Schmiedeshoff		
42164	C019186225	magnetic hysteresis loops were measured.	RuSr2(Gd,Ce)2Cu2O10-z	Ru1Sr2Gd1.5Ce0.5Cu2O10-z	Ru	1	Sr	2	Gd	1.5	Ce	0.5	Cu	2											O	10-z		1	2007																												Ru1222			A	3.835		28.573												K	25						25																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42165	C019186225	magnetic hysteresis loops were measured.	(Ru,Nb)Sr2(Gd,Ce)2Cu2O10-z	Ru0.9Nb0.1Sr2Gd1.5Ce0.5Cu2O10-z	Ru	0.9	Nb	0.1	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	10-z		1	2007																												Ru1222																		K	28.1			26.8			26.8																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42166	C019186225	magnetic hysteresis loops were measured.	(Ru,Nb)Sr2(Gd,Ce)2Cu2O10-z	Ru0.8Nb0.2Sr2Gd1.5Ce0.5Cu2O10-z	Ru	0.8	Nb	0.2	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	10-z		1	2007																												Ru1222																		K	28.9			28			28																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42167	C019186225	magnetic hysteresis loops were measured.	(Ru,Nb)Sr2(Gd,Ce)2Cu2O10-z	Ru0.7Nb0.3Sr2Gd1.5Ce0.5Cu2O10-z	Ru	0.7	Nb	0.3	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	10-z		1	2007																												Ru1222																		K	28.4			27.4			27.4																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42168	C019186225	magnetic hysteresis loops were measured.	(Ru,Nb)Sr2(Gd,Ce)2Cu2O10-z	Ru0.6Nb0.4Sr2Gd1.5Ce0.5Cu2O10-z	Ru	0.6	Nb	0.4	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	10-z		1	2007																												Ru1222																		K	27.8			27			27																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42169	C019186225	magnetic hysteresis loops were measured.	(Ru,Nb)Sr2(Gd,Ce)2Cu2O10-z	Ru0.5Nb0.5Sr2Gd1.5Ce0.5Cu2O10-z	Ru	0.5	Nb	0.5	Sr	2	Gd	1.5	Ce	0.5	Cu	2									O	10-z		1	2007																												Ru1222			A	3.851		28.715												K	26			25.7			25.7																																																																																																mixture - pellet - CAL(1000, 1020, 1040 C for 24h) - ANN(1075C,40h, in O2-flow) - (slow cool to RT) - ANN(400C,24h, in O2-flow)					Superconducting and magnetic behaviour of niobium doped RuSr2Gd1.5Ce0.5Cu2O10-z			Departamento de F?sica, UFSCar, Sao Carlos?SP, 13565-905, Brazil	J. Phys.: Condens. Matter, 19(2007)186225	C.A.Cardoso,F.M.Araujo-Moreira,V.P.S.Awana,H.Kishan,O.F.de Lima		
42170	J076054701	O-content by thermogravimetry	(Cu,C)Ba2Ca4Cu5Oz	C0.3Ba2Ca4Cu5.7O12.8	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	12.8	1	2007																												(Cu,C)1245																		K				99			99	TC42170																																																																																															ANN(RT-600C, N2-flow(200cm3/min)					Unconventional Variation of Tc in the Multilayered Cuprate Superconductor (Cu,C)Ba2Ca4Cu5Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510	J.Phys.Soc.Jpn, 76(2007)054701	M.Hirai,Y.Kodama,H.Kito,Y.Tanaka,K.Tokiwa,T.Watanabe,A.Iyo		
42171	J076054701	O-content by thermogravimetry	(Cu,C)Ba2Ca4Cu5Oz	C0.3Ba2Ca4Cu5.7O12.965	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	12.965	1	2007																												(Cu,C)1245																		K				93.3			93.3	TC42170																																																																																															ANN(RT-600C, N2-flow(200cm3/min)					Unconventional Variation of Tc in the Multilayered Cuprate Superconductor (Cu,C)Ba2Ca4Cu5Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510	J.Phys.Soc.Jpn, 76(2007)054701	M.Hirai,Y.Kodama,H.Kito,Y.Tanaka,K.Tokiwa,T.Watanabe,A.Iyo		
43000	SCI1740493	M =ammonia. reaction(80C,3d ).	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2					2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43001	SCI1740493	M = pyridine. reaction(200C,30d ).	(M)0.5NbS2	M0.5Nb1S2	M	0.5	Nb	1	S	2																			1971																										layered		TX2				3.34													hexagonal, 2H-TaS2	K		4					4																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43002	SCI1740493	M = s-collidine. reaction(200C,23d ).	(M)0.167NbS2	M0.167Nb1S2	M	0.167	Nb	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.5					3.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43003	SCI1740493	M = aniline. reaction(170C,23d ).	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		4					4																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43004	SCI1740493	M =tributylphosphine . reaction(200C,30d ).	(M)0.125	M0.125Nb1S2	M	0.125	Nb	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.5					3.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43005	SCI1740493	M = ammonia. reaction(25C,3d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.328													hexagonal, 2H-TaS2	K		42					42																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43006	SCI1740493	M = ammonium acetate. reaction(150C,1h ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.33													hexagonal, 2H-TaS2	K		2					2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43007	SCI1740493	M = amylamine . reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																		K		2.2					2.2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43008	SCI1740493	M = aniline. reaction(150C,16d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43009	SCI1740493	M = aniline. reaction(150C,16d ).	(M)0.75TaS2	M0.75Ta1S2	M	0.75	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2.5					2.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43010	SCI1740493	M = butyramine . reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43011	SCI1740493	M =butyramide . reaction(150C,21d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43012	SCI1740493	M = s-collidine. reaction(160C13d ).	(M)0.167TaS2	M0.167Nb1S2	M	0.167	Nb	1	S	2																			1971																										layered		TX2				3.319													hexagonal, 2H-TaS2	K		2					2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43013	SCI1740493	M = 4,4'-dipyridyl. reaction(160C,21d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.316													hexagonal, 2H-TaS2	K		2.5					2.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43014	SCI1740493	M = ethylamine. reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.334													hexagonal, 2H-TaS2	K		3.3					3.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43015	SCI1740493	M = hexanamide. reaction(150C,21d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43016	SCI1740493	M =hydrazine . reaction(10C,10min ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.334													hexagonal, 2H-TaS2	K		4.7					4.7																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43017	SCI1740493	M = isoquinoline. reaction(160C,28d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2.5					2.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43018	SCI1740493	M =LiOH . reaction(25C,30min ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.33													hexagonal, 2H-TaS2	K		4.5					4.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43019	SCI1740493	M = NH4OH . reaction(25C,30min ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.326													hexagonal, 2H-TaS2	K		3.3					3.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43020	SCI1740493	M = methylamine. reaction(25C30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.329													hexagonal, 2H-TaS2	K		4.2					4.2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43021	SCI1740493	M = octadecylamine. reaction( 40C,30d).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3					3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43022	SCI1740493	M =pentadecylamine . reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.328													hexagonal, 2H-TaS2	K		2.8					2.8																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43023	SCI1740493	M = p-phenylenediamine. reaction(140C,4h ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.318													hexagonal, 2H-TaS2	K		3.3					3.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43024	SCI1740493	M = p-phenylenediamine. reaction(140C,4h ).	(M)0.25TaS2	M0.25Ta1S2	M	0.25	Ta	1	S	2																			1971																										layered		TX2				3.318													hexagonal, 2H-TaS2	K		2.9					2.9																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43025	SCI1740493	M = potassium formate. reaction(200C,1h ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.334													hexagonal, 2H-TaS2	K		4.7					4.7																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43026	SCI1740493	M = propylamine. reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.33													hexagonal, 2H-TaS2	K		3					3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43027	SCI1740493	M = pyridine-N-oxide. reaction(100C,8h ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.335													hexagonal, 2H-TaS2	K		2.5					2.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43028	SCI1740493	M = pyridine chloride. reaction(170C4d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.329													hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43029	SCI1740493	M = quinoline. reaction(160C,16d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2.8					2.8																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43030	SCI1740493	M = RbOH. reaction( 25C,30min).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.325													hexagonal, 2H-TaS2	K		4.3					4.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43031	SCI1740493	M = septadecylamine. reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2.7					2.7																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43032	SCI1740493	M = NaOH. reaction(25C,30min ).	(NaOH)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.326													hexagonal, 2H-TaS2	K		4.8					4.8																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43033	SCI1740493	M =stearamide . reaction(150C10d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.1					3.1																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43034	SCI1740493	M = tetradecylamine. reaction( 25C,30min).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.325													hexagonal, 2H-TaS2	K		2.4					2.4																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43035	SCI1740493	M = N,N,N',N'-Tetramethyl-p-phenylenediamine. reaction(20013d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.335													hexagonal, 2H-TaS2	K		2.9					2.9																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43036	SCI1740493	M = thiobenzamide. reaction(160C,8d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3.3					3.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43037	SCI1740493	M = tributylamine. reaction(200C,7d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		3					3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43038	SCI1740493	M = tributylphosphine . reaction(200C,115d ).	(M)0.125TaS2	M0.125Ta1S2	M	0.125	Ta	1	S	2																			1971																										layered		TX2				3.318													hexagonal, 2H-TaS2	K		2					2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43039	SCI1740493	M = tridecylamine . reaction(25C,30d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.322													hexagonal, 2H-TaS2	K		2.5					2.5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43040	SCI1740493	M =triton B . reaction( 25C,30min).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.331													hexagonal, 2H-TaS2	K		5					5																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43041	SCI1740493	M =valeramide . reaction(150C,21d ).	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2.9					2.9																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43042	SCI1740493	M = s-collidine.	(M)0.17(Ta,W)S2	M0.17Ta0.8W0.2S2	M	0.17	Ta	0.8	W	0.2	S	2																	1971																										layered		TX2																	hexagonal, 2H-TaS2	K		2					2																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43043	SCI1740493	M = s-collidine.	(M)0.17(Ta,W)S2	M0.17Ta0.3W0.7S2	M	0.17	Ta	0.3	W	0.7	S	2																	1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.4																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43044	SCI1740493	M = ammonia.	(M)TiS2	M1Ti1S2	M	1	Ti	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.3																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43045	SCI1740493	M = aniline.	(M)TiS2	M1Ti1S2	M	1	Ti	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.3																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43046	SCI1740493	M = s-collidine.	(M)0.17TiS2	M0.17Ti1S2	M	0.17	Ti	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.3																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43047	SCI1740493	M = pyridine.	(M)0.5TiS2	M0.5Ti1S2	M	0.5	Ti	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.3																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43048	SCI1740493	M = tributylphosphine.	(M)0.125TiS2	M0.125Ti1S2	M	0.125	Ti	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K					0.3																																																																																																							Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43049	SCI1740493	M = N,N-dimethylaniline.  reaction(170C,3d)	(M)TiS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2																	hexagonal, 2H-TaS2	K		4.3					4.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43050	SCI1740493	M = KOH. reaction( 25C,30min).	(M)TiS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.328													hexagonal, 2H-TaS2	K		5.3					5.3																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43051	SCI1740493	M = CsOH. reaction( 25C,30min).	(M)TiS2	M1Ta1S2	M	1	Ta	1	S	2																			1971																										layered		TX2				3.33													hexagonal, 2H-TaS2	K		3.8					3.8																																																																																																					Intercalation complexes of Lewis bases and layered sulfides: A large class of new superconductors				Science, 174(1971)493	F.R.Gamble,J.H.Osiecki,M.Cais,R.Pisharody		
43060	JCP0553525	M = pyridine . reaction (200C,1d ).	(M)0.5TaS2	M0.5Ta1S2	M	0.5	Ta	1	S	2																			1971									4.1																	layered		TX2			A	3.326		23.7											hexagonal, 2H-TaS2	K		3.55					3.55																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43061	JCP0553525	M = 2-aminopyridine . reaction (200C,11d ).	(M)0.53TaS2	M0.53Ta1S2	M	0.53	Ta	1	S	2																			1971									4.06																	layered		TX2			A	3.325		24.18											hexagonal, 2H-TaS2	K		3.25					3.25																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43062	JCP0553525	M = 4-aminopyridine . reaction (200C,11d ).	(M)0.51TaS2	M0.51Ta1S2	M	0.51	Ta	1	S	2																			1971									3.96																	layered		TX2			A	3.328		23.94											hexagonal, 2H-TaS2	K		3.4					3.4																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43063	JCP0553525	M = 2,6-diaminopyridine . reaction (160C,9d ).	(M)0.53TaS2	M0.53Ta1S2	M	0.53	Ta	1	S	2																			1971									3.72																	layered		TX2			A			28											hexagonal, 2H-TaS2	K		3.5					3.5																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43064	JCP0553525	M = 2-dimethylaminopyridine . reaction (160C,14d ).	(M)0.32TaS2	M0.32Ta1S2	M	0.32	Ta	1	S	2																			1971									4.04																	layered		TX2			A	3.323		23.88											hexagonal, 2H-TaS2	K		3.15					3.15																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43065	JCP0553525	M = 4-dimethylaminopyridine . reaction (160C,28d ).	(M)0.34TaS2	M0.34Ta1S2	M	0.34	Ta	1	S	2																			1971									3.99																	layered		TX2			A	3.323		24.5											hexagonal, 2H-TaS2	K		2.3					2.3																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43066	JCP0553525	M = 2-ethylpyridine . reaction ( 160C,10d).	(M)0.29TaS2	M0.29Ta1S2	M	0.29	Ta	1	S	2																			1971									4.47																	layered		TX2			A	3.328		19.28											hexagonal, 2H-TaS2	K		3					3																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43067	JCP0553525	M = 3-ethylpyridine . reaction ( 160C,10d).	(M)0.29TaS2	M0.29Ta1S2	M	0.29	Ta	1	S	2																			1971									4.15																	layered		TX2			A	3.315		22.68											hexagonal, 2H-TaS2	K		4.5					4.5																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43068	JCP0553525	M = 4-ethylpyridine . reaction ( 200C,11d).	(M)0.33TaS2	M0.33Ta1S2	M	0.33	Ta	1	S	2																			1971									4.02																	layered		TX2			A	3.326		23.96											hexagonal, 2H-TaS2	K		2.95					2.95																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43069	JCP0553525	M = 2-isopropylpyridine . reaction (160C,10d ).	(M)0.25TaS2	M0.25Ta1S2	M	0.25	Ta	1	S	2																			1971									4.13																	layered		TX2			A	3.323		22.9											hexagonal, 2H-TaS2	K		3.8					3.8																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43070	JCP0553525	M = 4-isopropylpyridine . reaction (160C,10d ).	(M)0.28TaS2	M0.28Ta1S2	M	0.28	Ta	1	S	2																			1971									3.98																	layered		TX2			A	3.314		23.96											hexagonal, 2H-TaS2	K		2.82					2.82																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43071	JCP0553525	M =  2-methylpyridine. reaction (200C,7d ).	(M)0.34TaS2	M0.34Ta1S2	M	0.34	Ta	1	S	2																			1971									4.07																	layered		TX2			A	3.326		23.58											hexagonal, 2H-TaS2	K		2.95					2.95																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43072	JCP0553525	M =  3-methylpyridine. reaction (160C,25d ).	(M)0.33TaS2	M0.33Ta1S2	M	0.33	Ta	1	S	2																			1971																										layered		TX2			A	3.33		23.66											hexagonal, 2H-TaS2	K		2.95					2.95																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43073	JCP0553525	M =  4-methylpyridine. reaction (200C,7d ).	(M)0.33TaS2	M0.33Ta1S2	M	0.33	Ta	1	S	2																			1971									4.13																	layered		TX2			A	3.328		23.52											hexagonal, 2H-TaS2	K		2.7					2.7																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43074	JCP0553525	M = 2,6-dimethylpyridine . reaction ( 160C, 10d).	(M)0.2TaS2	M0.2Ta1S2	M	0.2	Ta	1	S	2																			1971									4.75																	layered		TX2			A	3.32		19.18											hexagonal, 2H-TaS2	K		2.15					2.15																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43075	JCP0553525	M = 2,4,6-trimethylpyridine . reaction ( 160C, 6d).	(M)0.165TaS2	M0.165Ta1S2	M	0.165	Ta	1	S	2																			1971									4.7																	layered		TX2			A	3.319		19.34											hexagonal, 2H-TaS2	K		1.95					1.95																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43076	JCP0553525	M = 2-phenylpyridine . reaction (160C,14d ).	(M)0.255TaS2	M0.255Ta1S2	M	0.255	Ta	1	S	2																			1971									4.11																	layered		TX2			A	3.328		23.84											hexagonal, 2H-TaS2	K		3.15					3.15																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43077	JCP0553525	M = 4-phenylpyridine . reaction (200C,35d ).	(M)0.26TaS2	M0.26Ta1S2	M	0.26	Ta	1	S	2																			1971									4.04																	layered		TX2			A	3.323		24.62											hexagonal, 2H-TaS2	K		1.6					1.6																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43078	JCP0553525	M = 2-propylpyridine . reaction (200C,5d ).	(M)0.245TaS2	M0.245Ta1S2	M	0.245	Ta	1	S	2																			1971									4.04																	layered		TX2			A	3.324		22.92											hexagonal, 2H-TaS2	K		2.85					2.85																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43079	JCP0553525	M = 4-propylpyridine . reaction (200C,5d ).	(M)0.25TaS2	M0.25Ta1S2	M	0.25	Ta	1	S	2																			1971									4.04																	layered		TX2			A	3.329		23.7											hexagonal, 2H-TaS2	K		2.75					2.75																																																																																																2H-TaS2 was prepared by heating (950C,several days). Intercalation was done by heating 2H-TaS2 with organic compound under the conditions described in [comment]					Some superconducting intercalation complexes of TaS2 and substituted pyridines			Syva Research Institute,California	J.Chem.Phys., 55(1971)3525	F.R.Gamble,J.H.Osicki,F.J.DiSalvo		
43080	1262	M = pyridine. Hc2 measured at 1.1 K (t= (T/Tc) = 0.73)	(M)Ta(S,Se)2	M1Ta1S1Se1	M	1	Ta	1	S	1	Se	1																	1973																										layered		TX2																	hexagonal, 2H-TaS2	K		1.5					1.5																				kOe	resistive, linear					19.1	2.6	1.1																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
43081	1262	M = pyridine. Hc2 measured at 1.4 K (t= (T/Tc) = 0.43). Hc2//ab > 150 kOe at 1.4 K.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1973																										layered		TX2																	hexagonal, 2H-TaS2	K		3.25					3.25																				kOe	resistive, linear						4.9	1.4																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
43083	1918	intercalated material = Srx(NH3)y.  M=NH3	Sr0.05(M)0.01MoS2	Sr0.05M0.01Mo1S2	Sr	0.05	M	0.01	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5.1					5.1																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43084	1918	intercalated material = Srx(NH3)y.  M=NH3	Sr0.17(M)0.4MoS2	Sr0.17M0.4Mo1S2	Sr	0.17	M	0.4	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		4.9					4.9																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43085	1918	intercalated material = Srx(NH3)y.  M=NH3	Sr0.14(M)0.42MoS2	Sr0.14M0.42Mo1S2	Sr	0.14	M	0.42	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5.1					5.1																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43086	1918	intercalated material = Srx(NH3)y.  M=NH3	Sr0.19(M)0.54MoS2	Sr0.19M0.54Mo1S2	Sr	0.19	M	0.54	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5.2					5.2																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43087	1918	intercalated material = Srx(NH3)y.  M=NH3. using 117micron powder MoS2.	Sr0.73(M)0.99MoS2	Sr0.73M0.99Mo1S2	Sr	0.73	M	0.99	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5					5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43088	1918	intercalated material = Srx(NH3)y.  M=NH3. using 53 micron powder MoS2.	Sr0.68(M)1.27MoS2	Sr0.68M1.27Mo1S2	Sr	0.68	M	1.27	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5					5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43090	1918	intercalated material = Ybx(NH3)y.  M=NH3	Yb0.1(M)0.16MoS2	Yb0.1M0.16Mo1S2	Yb	0.1	M	0.16	Mo	1	S	2																	1974																										layered		TX2																	hexagonal, 2H-TaS2	K		2.4					2.4																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43091	1918	intercalated material = 0.2Ca(NH3)x. M = 0.2Ca(NH3)x	(M)MoS2	M1Mo1S2	M	1	Mo	1	S	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		3.6					3.6																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43092	1918	intercalated material = 0.2Ba(NH3)x. M = 0.2Ba(NH3)x	(M)MoS2	M1Mo1S2	M	1	Mo	1	S	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5.7					5.7																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43093	1918	intercalated material = 0.2Sr(NH3)x. M = 0.2Sr(NH3)x	(M)MoSe2	M1Mo1Se2	M	1	Mo	1	Se	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		5					5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43094	1918	intercalated material = 0.2Sr(NH3)x. M = 0.2Sr(NH3)x	(M)WS2	M1W1S2	M	1	W	1	S	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		3.5					3.5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43095	1918	intercalated material = 0.4Yb(NH3)x. M = 0.4Yb(NH3)x	(M)WS2	M1W1S2	M	1	W	1	S	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		2.2					2.2																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43096	1918	intercalated material = 0.2Sr(NH3)x. M = 0.2Sr(NH3)x	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2																	hexagonal, 2H-TaS2	K		2.8					2.8																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
43097	CEM0090176	M=pyridine. 4H-phase. (Roberts REF#=1910)	(M)Ta(S,Se)2	M0.48Ta1S1.6Se0.4	M	0.48	Ta	1	S	1.6	Se	0.4																	1974																										layered		TX2			A			24.06											hexagonal, 2H-TaS2	K		2.8					2.8																																																																																																					Studies of the system TaS2-xSex			Stanford University, California	J.Solid State Chem., 9(1974)176	J.F.Revelli,W.A.Phillips		
43098	MRB0140797	Li-intercalated . interlayer distance d = 642 pm.	Li0.33TaS2	Li0.33Ta1S2	Li	0.33	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K					0.5																																																																																																							Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43099	MRB0140797	Na-intercalated . interlayer distance d = 735 pm.	Na0.33TaS2	Na0.33Ta1S2	Na	0.33	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		4.7					4.7																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43100	MRB0140797	K-intercalated . interlayer distance d = 820 pm.	K0.33TaS2	K0.33Ta1S2	K	0.33	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		3.8					3.8																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43101	MRB0140797	Rb-intercalated . interlayer distance d = 860 pm.	Rb0.33TaS2	Rb0.33Ta1S2	Rb	0.33	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		3					3																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43102	MRB0140797	Cs-intercalated . interlayer distance d = 900 pm.	Cs0.33TaS2	Cs0.33Ta1S2	Cs	0.33	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		3.8					3.8																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43103	MRB0140797	M-intercalated . M = Li0.33(H2O)0.67.  interlayer distance d = 897 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.6					5.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43104	MRB0140797	M-intercalated . M = Na0.33(H2O)0.67.  interlayer distance d = 898 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.5					5.5																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43105	MRB0140797	M-intercalated . M = K0.33(H2O)0.67.  interlayer distance d = 897 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.6					5.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43106	MRB0140797	M-intercalated . M = Rb0.33(H2O)0.67.  interlayer distance d = 899 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.5					5.5																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43107	MRB0140797	M-intercalated . M = Cs0.33(H2O)0.67.  interlayer distance d = 920 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		2.8					2.8																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43108	MRB0140797	M-intercalated . M = Li0.33(H2O)1.7.  interlayer distance d = 1165 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.3					5.3																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43109	MRB0140797	M-intercalated . M = Na0.33(H2O)1.7.  interlayer distance d = 1182 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		5.2					5.2																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43110	MRB0140797	M-intercalated . M = Na0.33(NMF)y.  NMF = N-methylformamide. NMF content (y) not given. interlayer distance d = 1890 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		4.6					4.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43111	MRB0140797	M-intercalated . M = K0.33(NMF)y.  NMF = N-methylformamide. NMF content (y) not given. interlayer distance d = 1730 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		4.6					4.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43112	MRB0140797	M-intercalated . M = Rb0.33(NMF)y.  NMF = N-methylformamide. NMF content (y) not given. interlayer distance d = 1740 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		4.6					4.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43113	MRB0140797	M-intercalated . M = Cs0.33(NMF)y.  NMF = N-methylformamide. NMF content (y) not given. interlayer distance d = 1750 pm.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		4.6					4.6																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43114	MRB0140797	Li-intercalated . interlayer distance d = 643 pm.	(Li)NbS2	Li0.5Nb1S2	Li	0.5	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K					0.5																																																																																																							Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43115	MRB0140797	Na-intercalated . interlayer distance d = 736 pm.	(Na)NbS2	Na0.5Nb1S2	Na	0.5	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		1.3					1.3																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43116	MRB0140797	K-intercalated . interlayer distance d = 820 pm.	(K)NbS2	K0.5Nb1S2	K	0.5	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		1.7					1.7																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43117	MRB0140797	Rb-intercalated . interlayer distance d = 850 pm.	(Rb)NbS2	Rb0.5Nb1S2	Rb	0.5	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		1.8					1.8																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43118	MRB0140797	Cs-intercalated . interlayer distance d = 890 pm.	(Cs)NbS2	Cs0.5Nb1S2	Cs	0.5	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		2.8					2.8																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43119	MRB0140797	M-intercalated . M = Li0.5(H2O)y.  H2O content y not given.  interlayer distance d = 897 pm.	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		2.9					2.9																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43120	MRB0140797	M-intercalated . M = Na0.5(H2O)y.  H2O content y not given.  interlayer distance d = 897 pm.	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		3.1					3.1																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43121	MRB0140797	M-intercalated . M = K0.5(H2O)y.  H2O content y not given.  interlayer distance d = 891 pm.	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		3					3																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43122	MRB0140797	M-intercalated . M = Rb0.5(H2O)y.  H2O content y not given.  interlayer distance d = 900 pm.	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		2.9					2.9																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43123	MRB0140797	M-intercalated . M = Cs0.5(H2O)y.  H2O content y not given.  interlayer distance d = 922 pm.	(M)NbS2	M1Nb1S2	M	1	Nb	1	S	2																			1979																										layered		TX2																	2H-TaS2	K		2.5					2.5																																																																																																					Superconductivity in layered ternary chalcogenides AxTaS2 and AxNbS2 and influence of topotactic solvation				Mat.Res.Bull. , 14(1979)797	A.Lerf,F.Sernetz,W.Biberacher,R.Schollhorn		
43124	1871	H-intercalated. lattice term coeff. of SP: (beta) = 0.54 mJ/mol.K4. (dC/gamma*Tc) = 2.2.	HxTaS2	H0.1Ta1S2	H	0.1	Ta	1	S	2																			1975																										layered		TX2																	2H-TaS2	K		3.9					3.9																																																								mJ/mol.K2	8.9	SP-heat																																						electrolysis using Pt anode					Properties of HxTaS2: Correlation between the superconducting Tc and an electronic instability in layer compounds				J.CHEM.PHYS.,62(1975)967	D.W.MURPHY,F.J.DISALVO,G.R.STEWART,G.W.HULLJR.,J.V.ACRIVOS,J.V.WASZCZAK,S.EARLY,S.F.MAYER,T.H.GEBALL		
43125	SCI1680568	M-intercalated. M = pyridine. Tc = 0.7 K for H//c-axis.	(M)0.5TaS2	M0.5Ta1S2	M	0.5	Ta	1	S	2																			1970																										layered		TX2																		K		3.5					3.5																																																																																																heat(Ta,S) in evacuated quartz tube at 900C,several days					Superconductivity in layered structure organometallic crystals				Science, 168(1970)568	F.R.Gamble,F.J.DiSalvo,R.A.Klemm,T.H.Geballe		
43126	1262	M-intercalated. M = pyridine. anisotropy (Hc2) = 7	(M)TaSSe	M1Ta1S1Se1	M	1	Ta	1	S	1	Se	1																	1973																										layered		TX2																		K		1.5					1.5																				kOe						19.1	2.6	1.1																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
43127	1262	M-intercalated. M = pyridine. Hc2//a > 66 kOe at 2.0 K.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1973																										layered		TX2																		K		3.25					3.25																											1.4	2																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
43128	JPS0630658	M-intercalated. M = (LaS). TP300 shows TP at 280 K. R not zero at 1.2 K for stage-I.	(M)NbS2	M1.2Nb1S2	M	1.2	Nb	1	S	2																			1994	emu/mol-La	0.000016					-0.67																			layered		TX2			A	5.857														K			4.3	2.2			2.2																																																																		uV/K	46																																		Electrical transport properties of incommensurate layer compounds (RES)xNbS2 (RE=rare-earth metals; x = 1.2, 0.6)			Department of Chemistry, Faculty of Science, Kyoto University,Japan	J.Phys.Soc.Jpn, 63(1994)658	T.Terashima,N.Kojima		
43129	JPS0630658	M-intercalated. M = (CeS).  stage-I structure. TP300 shows TP at 280 K. RES(a) = 330 uOhm.cm at 294 K. RES(b) = 323 uOhm.cm at 285 K.	(M)NbS2	M1.2Nb1S2	M	1.2	Nb	1	S	2																			1994																										layered		TX2			A	5.777														K			2.5				2.5																																																																		uV/K	39																																		Electrical transport properties of incommensurate layer compounds (RES)xNbS2 (RE=rare-earth metals; x = 1.2, 0.6)			Department of Chemistry, Faculty of Science, Kyoto University,Japan	J.Phys.Soc.Jpn, 63(1994)658	T.Terashima,N.Kojima		
43130	MRB0091597	M-intercalated. M = Li0.3(H2O)y. H2O content y not given. thermodynamical critical field Hc(0) = 170 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.33		23.42												K		3.83					3.83																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43131	MRB0091597	M-intercalated. M = Na0.3(H2O)y. H2O content y not given. thermodynamical critical field Hc(0) = 250 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.33		23.63												K		5.41					5.41																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43132	MRB0091597	M-intercalated. M = K0.3(H2O)y. H2O content y not given. thermodynamical critical field Hc(0) = 230 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.35		18.18												K		5.25					5.25																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43133	MRB0091597	M-intercalated. M = Rb0.3(H2O)y. H2O content y not given. thermodynamical critical field Hc(0) = 210 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.33		18.18												K		4.4					4.4																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43134	MRB0091597	M-intercalated. M = Cs0.3(H2O)y. H2O content y not given. thermodynamical critical field Hc(0) = 110 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.34		19.01												K		2.75					2.75																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43135	MRB0091597	M-intercalated. M = Ca0.3(H2)y. H2O content y not given. thermodynamical critical field Hc(0) = 130 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.33		23.76												K		3.47					3.47																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43136	MRB0091597	M-intercalated. M = Sr0.3(H2)y. H2O content y not given. thermodynamical critical field Hc(0) = 190 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.32		23.75												K		4.03					4.03																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43137	MRB0091597	M-intercalated. M = Ba0.3(H2)y. H2O content y not given. thermodynamical critical field Hc(0) = 150 Oe determined from magnetization.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																			1974																										layered		TX2			A	3.32		23.98												K		3.74					3.74																																																																																																hydration of AxTaS2 with water.					Superconductivity in hydrated ternary tantalum sulfided				Mat.Res.Bull. , 9(1974)1597	F.Sernetz,A.Lerf,R.Schollhorn		
43138	JCP0621068	Ca-intercalated.  Ca-content not known (0.05=< x =<0.07).	(Ca)xMoS2	Ca0.6Mo1S2	Ca	0.6	Mo	1	S	2																			1975																											3	TX2			A	8.894	9.869	18.64											2H-MoS2	K			4				4																				kOe			50	7																																																																								intercalation was done by placing MoS2 into a solution of alkaline earth metal in liquid ammonia at -70C for 3days.					The alkaline earth intercalates of molybdenum disulfide				J.Chem.Phys., 62(1975)1068	R.B.Somoano,V.Hadek,A.Rembaum,S.Samson,J.A.Woollam		
43139	JCP0621068	Sr-intercalated. Sr-content not known (0.06=< x =<0.1).	(Sr)xMoS2	Sr0.8Mo1S2	Sr	0.8	Mo	1	S	2																			1975																											2	TX2			A	10.396		18.62											2H-MoS2	K			5.6				5.6																				kOe			35	12																																																																								intercalation was done by placing MoS2 into a solution of alkaline earth metal in liquid ammonia at -70C for 3days.					The alkaline earth intercalates of molybdenum disulfide				J.Chem.Phys., 62(1975)1068	R.B.Somoano,V.Hadek,A.Rembaum,S.Samson,J.A.Woollam		
50000	PR0163925	glass temperature = 598 K. e-ph coupling = 1.5 .	Zr1-xBex	Be30Zr70	Be	30	Zr	70																					1977									5.72																			AMOR																		K		2.8				0.01	2.8																													T/K		2.38			MHC50000		A		71																																	uOhm.cm	294																								liquid quenching (10E+5 K/s), 30 um thick ribbon.					Superconducting properties of Be-Zr glassy alloys obtained by liquid quenching			Material Research Centere, Allied Chemical Corporation, Morristown, New Jersey	Phys.Rev.B, 16(1977)3925	R.Hasegawa,L.E.Tanner		
50001	PR0163925	glass temperature = 613 K. e-ph coupling = 1.2 .	Zr1-xBex	Be35Zr65	Be	35	Zr	65																					1977									5.65																			AMOR																		K		2.6				0.08	2.6																													T/K		1.7			MHC50000																																					uOhm.cm	231.9																								liquid quenching (10E+5 K/s), 30 um thick ribbon.					Superconducting properties of Be-Zr glassy alloys obtained by liquid quenching			Material Research Centere, Allied Chemical Corporation, Morristown, New Jersey	Phys.Rev.B, 16(1977)3925	R.Hasegawa,L.E.Tanner		
50002	PR0163925	glass temperature = 623 K. e-ph coupling = 1.2 .	Zr1-xBex	Be40Zr60	Be	40	Zr	60																					1977									5.55																			AMOR																		K		2.1				0.01	2.1																													T/K		2			MHC50000																																					uOhm.cm	282.1																								liquid quenching (10E+5 K/s), 30 um thick ribbon.					Superconducting properties of Be-Zr glassy alloys obtained by liquid quenching			Material Research Centere, Allied Chemical Corporation, Morristown, New Jersey	Phys.Rev.B, 16(1977)3925	R.Hasegawa,L.E.Tanner		
50003	PR0163925	glass temperature = 648 K.	Zr1-xBex	Be45Zr55	Be	45	Zr	55																					1977									5.35																			AMOR																		K					1																																																																									uOhm.cm	281.2																								liquid quenching (10E+5 K/s), 30 um thick ribbon.					Superconducting properties of Be-Zr glassy alloys obtained by liquid quenching			Material Research Centere, Allied Chemical Corporation, Morristown, New Jersey	Phys.Rev.B, 16(1977)3925	R.Hasegawa,L.E.Tanner		
50004	PR0180206		(Mo,Ru)0.8P0.2	Mo64Ru16P20	Mo	64	Ru	16	P	20																			1978																												AMOR																		K		7.31					7.31																													T/K		2.45			MHC50004																																					uOhm.cm											300														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50005	PR0180206		(Mo,Ru)0.8P0.2	Mo48Ru32P20	Mo	48	Ru	32	P	20																			1978																												AMOR																		K		6.18					6.18																													T/K		2.55			MHC50004																																					uOhm.cm											300														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50006	PR0180206		(Mo,Ru)0.8P0.2	Mo32Ru48P20	Mo	32	Ru	48	P	20																			1978																												AMOR																		K		4.68					4.68																													T/K		2.68			MHC50006																																					uOhm.cm											330														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50007	PR0180206		(Mo,Ru)0.8P0.2	Mo16Ru64P20	Mo	16	Ru	64	P	20																			1978																												AMOR																		K		3.43					3.43																													T/K		2.76			MHC50006																																					uOhm.cm											320														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50008	PR0180206		Mo8PB	Mo80P10B10	Mo	80	P	10	B	10																			1978																												AMOR																		K		9					9																													T/K		1.76			MHC50008																																																														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50009	PR0180206		(Mo,Ru)8PB	Mo64Re16P10B10	Mo	64	Re	16	P	10	B	10																	1978																												AMOR																		K		8.71					8.71																													T/K		2.42			MHC50008																																																														melt(1100C) - rapid quench. foil thickness = 60 um.					Superconductivity, magnetic susceptibility, and electronic properties of amorphous (Mo1-xRux)80P20 alloys obtained liquid quenching			W.M.Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California	Phys.Rev.B, 18(1978)206	W.L.Johnson,S.J.Poon,J.Durand,P.Duwez		
50010	PR0190193		La1-xAlx	Al0.2La0.8	Al	0.2	La	0.8																					1979																												AMOR																		K		4.43					4.43																													T/K		2.54			MHC50010		A	calculated from (dHc2/dT)	54.1																																	uOhm.cm							163																		alloys prepared by induction melting. amorphous by splat cooling.					Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50011	PR0190193		La1-xAlx	Al0.22La0.78	Al	0.22	La	0.78																					1979																												AMOR																		K		4.3					4.3																													T/K		2.67			MHC50010		A	calculated from (dHc2/dT)	53.6																																	uOhm.cm							172																		alloys prepared by induction melting. amorphous by splat cooling.					Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50012	PR0190193		La1-xAlx	Al0.25La0.75	Al	0.25	La	0.75																					1979																												AMOR																		K		3.98					3.98																													T/K		2.5			MHC50010		A	calculated from (dHc2/dT)	57.4																																	uOhm.cm							181																		alloys prepared by induction melting. amorphous by splat cooling.					Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50013	PR0190193		La1-xAlx	Al0.27La0.73	Al	0.27	La	0.73																					1979																												AMOR																		K		3.82					3.82																													T/K		2.39			MHC50013		A	calculated from (dHc2/dT)	60.1																																	uOhm.cm							185																		alloys prepared by induction melting. amorphous by splat cooling.					Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50014	PR0190193		La1-xAlx	Al0.32La0.68	Al	0.32	La	0.68																					1979																												AMOR																		K		3.23					3.23																													T/K		2.62			MHC50013		A	calculated from (dHc2/dT)	62.4																																	uOhm.cm							194																		alloys prepared by induction melting. amorphous by splat cooling.					Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50015	PR0190193		La1-xAlx	Al0.18La0.82	Al	0.18	La	0.82																					1979																												AMOR																		K		4.65					4.65	MTC50015																																																																																																				Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50016	PR0190193		La1-xAux	Au0.2La0.8	Au	0.2	La	0.8																					1979																												AMOR																		K		4.23					4.23	MTC50015																																																																																																				Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50017	PR0190193		La1-xGex	Ge0.2La0.8	Ge	0.2	La	0.8																					1979																												AMOR																		K		5.1					5.1	MTC50015																																																																																																				Alloying effect on superconductivity in amorphous lanthanum-based alloys			IBM Thomas J.Watson Research Center, Yorktown Heights, New York	Phys.Rev.B, 19(1979)193	K.Agyeman,R.Muller,C.C.Tsuei		
50018	PRL0391480	gamma = (0.4 - 6) E-3 mJ/g.K2.	Zr1-xPdx	Pd0.3Zr0.7	Pd	0.3	Zr	0.7																					1977																												AMOR																		K		2.53				0.01	2.53																																																2.94											180	SP-heat																																				melt-quench					Low-temperature properties of a superconducting disordered metal			Bell Laboratories, Murray Hill, New Jersey	Phys.Rev.Lett., 39(1977)1480	J.E.Graebner,B.Golding,R.J.Schutz,F.S.L.Hsu,H.S.Chen		
50019	PRL0391580	Tc(R) = 3.6 K. (dC) = 36.4 mJ/mol.K2. (dC/gamma*Tc) = 1.4 . e-ph coupling = 0.88.	La1-xAux	Au0.2La0.8	Au	0.2	La	0.8																					1977																												AMOR																		K		3.71				0.12	3.71																																																											96	SP-heat																																				splat cooling					"Specific heats of superconducting splat-cooled ""amorphous"" La1-xAux alloys"			Texas A & M University, College Station, Texas	Phys.Rev.Lett., 39(1977)1580	W.H.Shull,D.G.Naugle		
50020	PRL0391580	Tc(R) = 3.3 K. (dC) = 35.8 mJ/mol.K2. (dC/gamma*Tc) = 1.7 . e-ph coupling = 0.82.	La1-xAux	Au0.24La0.76	Au	0.24	La	0.76																					1977																												AMOR																		K		3.28				0.2	3.28																																																											99	SP-heat																																				splat cooling					"Specific heats of superconducting splat-cooled ""amorphous"" La1-xAux alloys"			Texas A & M University, College Station, Texas	Phys.Rev.Lett., 39(1977)1580	W.H.Shull,D.G.Naugle		
50021	PHC2750333		Zr-Ti-Cu-Ni-Be	Zr41.2Ti13.8Cu12.5Ni10Be22.5	Zr	41.2	Ti	13.8	Cu	12.5	Ni	10	Be	22.5															1997																												AMOR																		K		1.1					1.1																													T/K		2.04			MHC50021																																					uOhm.cm											195														melt-quench					Superconductivity in the metallic amorphous alloy Zr41.2Ti13.8Cu12.5Ni10Be22.5	199702		School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Tel Aviv University,Ramat Aviv,69978 Tel Aviv, Israel	Physica.C,275(1997)333-336	A. Gerber,A. Milner,A. Rubstein,A. Voronel,M.P. Macht,Yu. Rosenberg		
50022	PHC2750333	metal. ANN(550C) of #50021 sample.	Zr-Ti-Cu-Ni-Be	Zr41.2Ti13.8Cu12.5Ni10Be22.5	Zr	41.2	Ti	13.8	Cu	12.5	Ni	10	Be	22.5															1997																																														K		0.9					0.9																													T/K		1			MHC50021																																					uOhm.cm											75														melt-quench					Superconductivity in the metallic amorphous alloy Zr41.2Ti13.8Cu12.5Ni10Be22.5	199702		School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Tel Aviv University,Ramat Aviv,69978 Tel Aviv, Israel	Physica.C,275(1997)333-336	A. Gerber,A. Milner,A. Rubstein,A. Voronel,M.P. Macht,Yu. Rosenberg		
50023	PHB2630296	Tc(crystalized sample) =  3.84 K..	Sn	Sn1	Sn	1																							1999																												AMOR																		K		4.46					4.46																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50024	PHB2630296	crystalizing temp. = 174 K. Tc(crystalized sample) =  3.27 K..	CuxSn1-x	Cu20Sn80	Cu	20	Sn	80																					1999																												AMOR																		K		5.71					5.71																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50025	PHB2630296	crystalizing temp. = 194 K. Tc(crystalized sample) = 2.57  K..	CuxSn1-x	Cu30Sn70	Cu	30	Sn	70																					1999																												AMOR																		K		4.91					4.91																																																																	MTHC50025																															Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50026	PHB2630296	crystalizing temp. = 212 K. Tc(crystalized sample) =  2.04 K..	CuxSn1-x	Cu40Sn60	Cu	40	Sn	60																					1999																												AMOR																		K		4.19					4.19																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50027	PHB2630296	crystalizing temp. = 228 K.	CuxSn1-x	Cu50Sn50	Cu	50	Sn	50																					1999																												AMOR																		K		3.26					3.26																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50028	PHB2630296	crystalizing temp. = 261 K.	CuxSn1-x	Cu60Sn40	Cu	60	Sn	40																					1999																												AMOR																		K		2.26					2.26																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50029	PHB2630296	crystalizing temp. = 322 K.	CuxSn1-x	Cu70Sn30	Cu	70	Sn	30																					1999																												AMOR																		K		1.2					1.2																																																																																																Deposited at 5 K on microchip substrates.					Thermal conductivity of CuxSn100-x films at low temperatures			TU Chemnitz, Institut fur Physik, Professur Physik dnner Schichten, 09107 Chemnitz, Germany	Physica B, 263-264(1999)296	R.Schmidt,Th.Franke,P.Haussler		
50030	PHC3920336	thickness d = 290 nm film. Hc2 defined as 0.9Rn and 0.1Rn.	MgxB1-x	B0.69Mg0.31	B	0.69	Mg	0.31																					2003																												AMOR																		K	5.7						5.7	MTC50030																																	MHC50030																																																														Coevaporation of Mg and B by EB-gun on glass substrates(RT).					Superconductivity and vortex states in thick amorphous MgxB1-x films			Research Center for Low Temperature Physics, Tokyo Institute of Technology, 2-12-1, Ohokayama, Meguro-ku, Tokyo 152-8551, Japan	Physica C, 392-396(2003)336	S.Okuma,S.Togo,K.Amemori		
50031	JAP0515475	ribbon(thickness=0.04 mm). vickers = 560 DPN, Tensile fracture = 2060 MPa, crystallization temp. = 718 K.	TixNbySiz	Ti70Nb15Si15	Ti	70	Nb	15	Si	15																			1980																												AMOR																		K	4.6					0.45	4.6																																																																							uOhm.cm											170														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50032	JAP0515475	ribbon(thickness=0.04 mm). vickers = 58 DPN, Tensile fracture = 2010 MPa, crystallization temp. = 770 K. Hc2(0) = 27 E+5 A/m.	TixNbySiz	Ti55Nb30Si15	Ti	55	Nb	30	Si	15																			1980																												AMOR																		K	4.9					0.55	4.9																				kOe		34							kOe/K		75.3																																								uOhm.cm											170														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50033	JAP0515475		TixNbySiz	Ti60Nb25Si15	Ti	60	Nb	25	Si	15																			1980																												AMOR																		K		4.8				0.5	4.8																																																																							uOhm.cm											180														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50034	JAP0515475		TixNbySiz	Ti50Nb35Si15	Ti	50	Nb	35	Si	15																			1980																												AMOR																		K		5				0.55	5																																																																							uOhm.cm											160														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50035	JAP0515475		TixNbySiz	Ti45Nb40Si15	Ti	45	Nb	40	Si	15																			1980																												AMOR																		K		5.1				0.55	5.1																																																																							uOhm.cm											150														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50036	JAP0515475		TixNbySiz	Ti56Nb30Si14	Ti	56	Nb	30	Si	14																			1980																												AMOR																		K		5				0.4	5																																																																							uOhm.cm											170														arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50037	JAP0515475		TixNbySiz	Ti55Nb30Si15	Ti	55	Nb	30	Si	15																			1980																												AMOR																		K		4.9					4.9																																																																																																arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50038	JAP0515475		TixNbySiz	Ti54Nb30Si16	Ti	54	Nb	30	Si	16																			1980																												AMOR																		K		4.8					4.8																																																																																																arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50039	JAP0515475		TixNbySiz	Ti52Nb30Si18	Ti	52	Nb	30	Si	18																			1980																												AMOR																		K		4.7					4.7																																																																																																arc-melting, cold roll quenching.					Superconductivity of ductile Ti-Nb-Si amorphous alloys			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 51(1980)5475	A.Inoue,H.M.Kimura,T.Masumoto,C.Suryanarayana,A.Hoshi		
50040	PR0134827	thickness = 50 um	LaxAuy	Au22La78	Au	22	La	78																					1976																												AMOR																		K		3.934				0.018	3.934																																																																							uOhm.cm							280																		liquid quenching					Effect of thermodynamic fluctuations on the shape and width of the resistive transition in three-dimensional amorphous superconducting alloys			IBM Thomas J.Watson Research Center, Yorktown Hights, New York	Phys.Rev.B, 13(1976)4827	W.L.Johnson,C.C.Tsuei		
50041	PR0134827	thickness = 50 um	LaxAuyCuz	La75Au15Cu10	La	75	Au	15	Cu	10																			1976																												AMOR																		K		3.795				0.022	3.795																																																																							uOhm.cm							320																		liquid quenching					Effect of thermodynamic fluctuations on the shape and width of the resistive transition in three-dimensional amorphous superconducting alloys			IBM Thomas J.Watson Research Center, Yorktown Hights, New York	Phys.Rev.B, 13(1976)4827	W.L.Johnson,C.C.Tsuei		
50042	PR0134827	thickness = 0.1 - 1 um	MoxRey	Mo30Re70	Mo	30	Re	70																					1976																												AMOR																		K		7.62				0.021	7.62																																																																																																rf sputtering					Effect of thermodynamic fluctuations on the shape and width of the resistive transition in three-dimensional amorphous superconducting alloys			IBM Thomas J.Watson Research Center, Yorktown Hights, New York	Phys.Rev.B, 13(1976)4827	W.L.Johnson,C.C.Tsuei		
50043	PR0134827	thickness = 0.1 - 1 um	NbxGey	Ge1Nb3	Ge	1	Nb	3																					1976																												AMOR																		K		3.342				0.014	3.342																																																																																																rf sputtering					Effect of thermodynamic fluctuations on the shape and width of the resistive transition in three-dimensional amorphous superconducting alloys			IBM Thomas J.Watson Research Center, Yorktown Hights, New York	Phys.Rev.B, 13(1976)4827	W.L.Johnson,C.C.Tsuei		
50044	PR04812866	neutron dose = 0	ZrxCuy	Cu40Zr60	Cu	40	Zr	60																					1993																												AMOR																		K		1.6					1.6																				T		2.88							T/K		2.75			MHC50044																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50045	PR04812866	neutron dose = 0.75 E+18 n/cm3	ZrxCuy	Cu40Zr60	Cu	40	Zr	60																					1993																												AMOR																		K		1.14					1.14																				T		1.98							T/K		2.62			MHC50044																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50046	PR04812866	neutron dose = 2.2 E+18 n/cm3	ZrxCuy	Cu40Zr60	Cu	40	Zr	60																					1993																												AMOR																		K		0.78					0.78																				T		1.4							T/K		2.42			MHC50044																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50047	PR04812866	neutron dose = 0	ZrxCuy	Cu50Zr50	Cu	50	Zr	50																					1993																												AMOR																		K		0.74					0.74																				T		1.24							T/K		2.94			MHC50047																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50048	PR04812866	neutron dose = 0.75 E+18 n/cm3	ZrxCuy	Cu50Zr50	Cu	50	Zr	50																					1993																												AMOR																		K		0.54					0.54																				T		0.91							T/K		2.73			MHC50047																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50049	PR04812866	neutron dose = 2.2 E+18 n/cm3	ZrxCuy	Cu50Zr50	Cu	50	Zr	50																					1993																												AMOR																		K		0.35					0.35																				T		0.59							T/K		2.56			MHC50047																																																														arc melting followed by melt spinning.					Variation of disorder in superconducting glassy metals			Department of Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 48(1993)12866	A.Nordstrom,U.Dahlborg,O.Rapp		
50050	JAP0524711	Vickers = 580 DPN. crystallization temp. = 798 K.	TixNbySiz	Ti55Nb30Si15	Ti	55	Nb	30	Si	15																			1981																												AMOR																		K		4.9				0.5	4.9																				kOe		18.8																																																																										rapid quenching from melt.					Superconductivity in amorphous + crystalline Ti-(Nb or V)-Si-B ductile alloys obtained by rapid quenching from the melt			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 52(1981)4711	A.Inoue,Y.Takahashi,A.Hoshi,C.Suryanarayana,T.Masumoto		
50051	JAP0524711	Vickers = 665 DPN. crystallization temp. = 852 K.	TixNbySiz	Ti45Nb40Si15	Ti	45	Nb	40	Si	15																			1981																												AMOR																		K		5.1				0.5	5.1																				kOe		20.1																																																																										rapid quenching from melt.					Superconductivity in amorphous + crystalline Ti-(Nb or V)-Si-B ductile alloys obtained by rapid quenching from the melt			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 52(1981)4711	A.Inoue,Y.Takahashi,A.Hoshi,C.Suryanarayana,T.Masumoto		
50052	JAP0524711	Vickers = 570 DPN. crystallization temp. = 741 K.	TixNbySizB3	Ti55Nb30Si12B3	Ti	55	Nb	30	Si	12	B	3																	1981																												AMOR																		K		5				0.5	5																				kOe		18.8																																																																										rapid quenching from melt.					Superconductivity in amorphous + crystalline Ti-(Nb or V)-Si-B ductile alloys obtained by rapid quenching from the melt			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 52(1981)4711	A.Inoue,Y.Takahashi,A.Hoshi,C.Suryanarayana,T.Masumoto		
50053	JAP0524711	Vickers = 630 DPN. crystallization temp. = 796 K.	TixNbySizB3	Ti45Nb40Si12B3	Ti	45	Nb	40	Si	12	B	3																	1981																												AMOR																		K		5.4				0.7	5.4																				kOe		22.6																																																																										rapid quenching from melt.					Superconductivity in amorphous + crystalline Ti-(Nb or V)-Si-B ductile alloys obtained by rapid quenching from the melt			The Research Institute for Iron, Steel, and Other Metals, Tohoku University, Sendai, Japan	J.Appl.Phys., 52(1981)4711	A.Inoue,Y.Takahashi,A.Hoshi,C.Suryanarayana,T.Masumoto		
50054	PR0225213	crystallized at 951 K.	Nb1-xRhx	Nb55Rh45	Nb	55	Rh	45																					1980																												AMOR																		K	4.52	5.13	5.13				5.13																																																								mJ/mol.K2	3.92	calculated from (dHc2/dT) using GLAG theory	273	calculated from Young's modulus.																																				rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50055	PR0225213	crystallized at 1168 K.	Nb1-xIrx	Ir45Nb55	Ir	45	Nb	55																					1980																												AMOR																		K		4.88					4.88																													T/K		2.5			MHC50055																						mJ/mol.K2	3.16	calculated from (dHc2/dT) using GLAG theory	253	calculated from Young's modulus.																																				rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50056	PR0225213	crystallized at 1151 K.	Ta1-xRhx	Rh45Ta55	Rh	45	Ta	55																					1980																												AMOR																		K	3.17	3.37	3.37				3.37																													T/K		2.5			MHC50056																						mJ/mol.K2	2.67	calculated from (dHc2/dT) using GLAG theory	247	calculated from Young's modulus.																																				rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50057	PR0225213	crystallized at 1338 K.	Ta1-xIrx	Ir45Ta55	Ir	45	Ta	55																					1980																												AMOR																		K	2.92	3.39	3.41				3.39																																																								mJ/mol.K2	2.34	calculated from (dHc2/dT) using GLAG theory	232	calculated from Young's modulus.																																				rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50058	PR0225213		NbxTayRhz	Nb41.25Ta13.75Rh45	Nb	41.25	Ta	13.75	Rh	45																			1980																												AMOR																		K	4.32		4.91				4.615																																																								mJ/mol.K2	3.78	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50059	PR0225213		NbxTayRhz	Nb27.5Ta27.5Rh45	Nb	27.5	Ta	27.5	Rh	45																			1980																												AMOR																		K	3.9		4.03				3.965																																																								mJ/mol.K2	3.73	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50060	PR0225213		NbxTayRhz	Nb13.75Ta41.25Rh45	Nb	13.75	Ta	41.25	Rh	45																			1980																												AMOR																		K	3.49		3.63				3.56																																																								mJ/mol.K2	3.33	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50061	PR0225213		NbxTayIrz	Nb41.25Ta13.75Ir45	Nb	41.25	Ta	13.75	Ir	45																			1980																												AMOR																		K	4.23		4.47				4.35																																																								mJ/mol.K2	3.11	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50062	PR0225213		NbxTayIrz	Nb27.5Ta27.5Ir45	Nb	27.5	Ta	27.5	Ir	45																			1980																												AMOR																		K	3.89		3.98				3.935																																																								mJ/mol.K2	2.86	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50063	PR0225213		NbxTayIrz	Nb13.75Ta41.25Ir45	Nb	13.75	Ta	41.25	Ir	45																			1980																												AMOR																		K	3.03		3.6				3.315																																																								mJ/mol.K2	2.72	calculated from (dHc2/dT) using GLAG theory																																						rapid quench.					Superconductivity in amorphous T5T9 transition-metal alloys (T5=Nb, Ta; T9=Rh, Ir)			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee	Phys.Rev.B, 22(1980)5213	C.C.Koch,D.M.Kroeger,J.O.Scarbrough,B.C.Giessen		
50064	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.43.	ZrxRhy	Rh43Zr57	Rh	43	Zr	57																					1983																												AMOR																		K		2.18					2.18																													kG/K		26			MHC50064																																					uOhm.cm							214				205														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50065	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.48.	ZrxRhy	Rh41Zr59	Rh	41	Zr	59																					1983																												AMOR																		K		2.44					2.44																													kG/K		27			MHC50064																																					uOhm.cm							200				187														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50066	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.51.	ZrxRhy	Rh37Zr63	Rh	37	Zr	63																					1983																												AMOR																		K		2.86					2.86																													kG/K		28			MHC50066																																					uOhm.cm							194				182														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50067	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.61.	ZrxRhy	Rh27Zr73	Rh	27	Zr	73																					1983																												AMOR																		K		3.57					3.57																													kG/K		31																																								uOhm.cm							177				166														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50068	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.61.	ZrxRhy	Rh24Zr76	Rh	24	Zr	76																					1983																												AMOR																		K		3.67					3.67																													kG/K		32			MHC50066																																					uOhm.cm							185				180														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50069	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.64.	ZrxRhy	Rh23Zr77	Rh	23	Zr	77																					1983																												AMOR																		K		3.66					3.66																													kG/K		32																																								uOhm.cm							175				165														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50070	PR0271596	amorphous film. RESN shows resistivity at 25 K. e-ph coupling = 0.61.	ZrxRhy	Rh20Zr80	Rh	20	Zr	80																					1983																												AMOR																		K		3.72					3.72																													kG/K		31																																								uOhm.cm							184				171														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50071	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru28Zr72	Ru	28	Zr	72																					1983																												AMOR																		K		3.76					3.76																													kG/K		27																																								uOhm.cm							194																		rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50072	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru27Zr73	Ru	27	Zr	73																					1983																												AMOR																		K		3.11					3.11																													kG/K		27																																								uOhm.cm							213				203														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50073	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru22Zr78	Ru	22	Zr	78																					1983																												AMOR																		K		3.73					3.73																													kG/K		23																																								uOhm.cm							193				184														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50074	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru18Zr82	Ru	18	Zr	82																					1983																												AMOR																		K		3.78					3.78																													kG/K		28																																								uOhm.cm							205				196														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50075	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru18Zr82	Ru	18	Zr	82																					1983																												AMOR																		K		3.33					3.33																													kG/K		27																																								uOhm.cm							185																		rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50076	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru13Zr87	Ru	13	Zr	87																					1983																												AMOR																		K		3.57					3.57																													kG/K		20																																								uOhm.cm							193				188														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50077	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru11Zr89	Ru	11	Zr	89																					1983																												AMOR																		K		3.84					3.84																													kG/K		21																																								uOhm.cm							198																		rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50078	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru11Zr89	Ru	11	Zr	89																					1983																												AMOR																		K		3.9					3.9																													kG/K		24																																								uOhm.cm							204				196														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50079	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRuy	Ru8Zr92	Ru	8	Zr	92																					1983																												AMOR																		K		3.79					3.79																													kG/K		20																																								uOhm.cm							200				196														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50080	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRey	Re30Zr70	Re	30	Zr	70																					1983																												AMOR																		K		2.69					2.69																													kG/K		24																																								uOhm.cm							199				190														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50081	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRey	Re16Zr84	Re	16	Zr	84																					1983																												AMOR																		K		3.32					3.32																													kG/K		25																																								uOhm.cm							179				171														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50082	PR0271596	amorphous film. RESN shows resistivity at 25 K.	ZrxRey	Re10Zr90	Re	10	Zr	90																					1983																												AMOR																		K		4.12					4.12																													kG/K		23																																								uOhm.cm							147				143														rf diode cosputtering on glass substrates at RT.					Electronic density of states in amorphous zirconium alloys			Energy Conversion Devices, Inc., Troy, Michigan	Phys.Rev.B, 27(1983)1596	F.P.Missell,S.Frota-Pessoa,J.Wood,J.Tyler,J.E.Keem		
50083	PR0275519	as-quenched sample.	Zr2Co	Co1Zr2	Co	1	Zr	2																					1983																												AMOR																		K		3					3																													kG/K		32.7																																								uOhm.cm							180																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50084	PR0275519	as-quenched sample.	Zr2Ni	Ni1Zr2	Ni	1	Zr	2																					1983																												AMOR																		K		2.77					2.77																													kG/K		28.6																																								uOhm.cm							170																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50085	PR0275519	as-quenched sample.	Zr2Pd	Pd1Zr2	Pd	1	Zr	2																					1983																												AMOR																		K		2.36					2.36																													kG/K		28.5																																								uOhm.cm							175																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50086	PR0275519	as-quenched sample.	Zr3Ni	Ni1Zr3	Ni	1	Zr	3																					1983																												AMOR																		K		3.35					3.35																													kG/K		33.4																																								uOhm.cm							170																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50087	PR0275519	as-quenched sample.	Zr3Pd	Pd1Zr3	Pd	1	Zr	3																					1983																												AMOR																		K		2.96					2.96																													kG/K		30.2																																								uOhm.cm							180																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50088	PR0275519	as-quenched sample.	Zr3Rh	Rh1Zr3	Rh	1	Zr	3																					1983																												AMOR																		K		4.3					4.3																													kG/K		31.8																																								uOhm.cm							230																		melt-quench					Thermal-relaxation studies of the stability of amorphous structures in zirconium-based superconducting alloya			Department of Physics, University of Virginia, Charlottesville, Virginia	Phys.Rev.B, 27(1983)5519	S.J.Poon		
50089	PR0281396	RESN shows resistivity at 4.2 K.	ZrxCoy	Co21Zr79	Co	21	Zr	79																					1983																												AMOR																		K		3.78					3.78																													kG/K		34.1			MHC50089																						mJ/mol.K2	5.75	calculated from Rn, (dHc2/dT)													uOhm.cm							170																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50090	PR0281396	RESN shows resistivity at 4.2 K.	ZrxCoy	Co25Zr75	Co	25	Zr	75																					1983																												AMOR																		K		3.47					3.47																													kG/K		33.9			MHC50089																						mJ/mol.K2	5.21	calculated from Rn, (dHc2/dT)													uOhm.cm							179																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50091	PR0281396	RESN shows resistivity at 4.2 K.	ZrxCoy	Co28Zr72	Co	28	Zr	72																					1983																												AMOR																		K		3.12					3.12																													kG/K		33.8			MHC50091																						mJ/mol.K2	5.06	calculated from Rn, (dHc2/dT)													uOhm.cm							181																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50092	PR0281396	RESN shows resistivity at 4.2 K.	ZrxCoy	Co35Zr65	Co	35	Zr	65																					1983																												AMOR																		K		2.48					2.48																													kG/K		34.8			MHC50091																						mJ/mol.K2	4.96	calculated from Rn, (dHc2/dT)													uOhm.cm							180																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50093	PR0281396	RESN shows resistivity at 4.2 K.	ZrxNiy	Ni22Zr78	Ni	22	Zr	78																					1983																												AMOR																		K		3.47					3.47																													kG/K		31.9			MHC50093																						mJ/mol.K2	5.33	calculated from Rn, (dHc2/dT)													uOhm.cm							168																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50094	PR0281396	RESN shows resistivity at 4.2 K.	ZrxNiy	Ni24Zr76	Ni	24	Zr	76																					1983																												AMOR																		K		3.29					3.29																													kG/K		31.5			MHC50093																						mJ/mol.K2	4.87	calculated from Rn, (dHc2/dT)													uOhm.cm							178																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50095	PR0281396	RESN shows resistivity at 4.2 K.	ZrxNiy	Ni27Zr73	Ni	27	Zr	73																					1983																												AMOR																		K		3.1					3.1																													kG/K		31.9			MHC50093																						mJ/mol.K2	4.87	calculated from Rn, (dHc2/dT)													uOhm.cm							178																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50096	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Ti)xNiy	Zr70.2Ti7.8Ni22	Zr	70.2	Ti	7.8	Ni	22																			1983																												AMOR																		K		3.32					3.32																													kG/K		32.9			MHC50096																						mJ/mol.K2	5.03	calculated from Rn, (dHc2/dT)													uOhm.cm							180																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50097	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Ti)xNiy	Zr62.4Ti15.6Ni22	Zr	62.4	Ti	15.6	Ni	22																			1983																												AMOR																		K		3.09					3.09																													kG/K		35.2			MHC50096																						mJ/mol.K2	5.48	calculated from Rn, (dHc2/dT)													uOhm.cm							172																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50098	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Ti)xNiy	Zr54.6Ti23.4Ni22	Zr	54.6	Ti	23.4	Ni	22																			1983																												AMOR																		K		2.78					2.78																													kG/K		36.3			MHC50096																						mJ/mol.K2	5.21	calculated from Rn, (dHc2/dT)													uOhm.cm							182																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50099	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Nb)xNiy	Zr74.1Ti3.9Ni22	Zr	74.1	Ti	3.9	Ni	22																			1983																												AMOR																		K		3.65					3.65																													kG/K		31.5			MHC50099																						mJ/mol.K2	5.14	calculated from Rn, (dHc2/dT)													uOhm.cm							171																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50100	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Nb)xNiy	Zr66.3Ti11.7Ni22	Zr	66.3	Ti	11.7	Ni	22																			1983																												AMOR																		K		3.56					3.56																													kG/K		29.5			MHC50099																						mJ/mol.K2	5.04	calculated from Rn, (dHc2/dT)													uOhm.cm							159																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50101	PR0281396	RESN shows resistivity at 4.2 K.	(Zr,Nb)xNiy	Zr62.4Ti15.6Ni22	Zr	62.4	Ti	15.6	Ni	22																			1983																												AMOR																		K		3.34					3.34																													kG/K		28.2			MHC50099																						mJ/mol.K2	4.71	calculated from Rn, (dHc2/dT)													uOhm.cm							162																		melt spinning					Upper critical fields and superconducting transition temperatures of some zirconium-base amorphous transition-metal alloys			Department of Physics, Indiana University , Bloomington, Indiana	Phys.Rev.B, 28(1983)1396	M.G.Karkut,R.R.Hake		
50110	PR0302898		(Ni20Zr80)1-xMnx	Ni19.75Zr79Mn1.25	Ni	19.75	Zr	79	Mn	1.25																			1984																												AMOR																		K		1.92		2.43			1.92																																																																																																All films deposited by dc sputtering from arc-melted buttans at temperature range of 77 - 508 K.					Local Mn moment in amorphous Mn-Zr alloys			AT&T Bell Laboratory¿Murray Hill, New Jersey	Phys.Rev.B, 30(1984)2898	J.J.Hauser,J.V.Waszczak		
50111	PR0302898		(Ni20Zr80)1-xMnx	Ni19.5Zr78Mn2.5	Ni	19.5	Zr	78	Mn	2.5																			1984																												AMOR																		K		1.41					1.41																																																																																																All films deposited by dc sputtering from arc-melted buttans at temperature range of 77 - 508 K.					Local Mn moment in amorphous Mn-Zr alloys			AT&T Bell Laboratory¿Murray Hill, New Jersey	Phys.Rev.B, 30(1984)2898	J.J.Hauser,J.V.Waszczak		
50112	PR0302898		(Cu20Zr80)1-xMnx	Cu19.8Zr79.2Mn1	Cu	19.8	Zr	79.2	Mn	1																			1984																												AMOR																		K		2.11					2.11																																																																																																All films deposited by dc sputtering from arc-melted buttans at temperature range of 77 - 508 K.					Local Mn moment in amorphous Mn-Zr alloys			AT&T Bell Laboratory¿Murray Hill, New Jersey	Phys.Rev.B, 30(1984)2898	J.J.Hauser,J.V.Waszczak		
50113	PR0302898		(Cu20Zr80)1-xMnx	Cu19.6Zr78.4Mn2	Cu	19.6	Zr	78.4	Mn	2																			1984																												AMOR																		K		1.14					1.14																																																																																																All films deposited by dc sputtering from arc-melted buttans at temperature range of 77 - 508 K.					Local Mn moment in amorphous Mn-Zr alloys			AT&T Bell Laboratory¿Murray Hill, New Jersey	Phys.Rev.B, 30(1984)2898	J.J.Hauser,J.V.Waszczak		
50114	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.07 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd35Zr65	Pd	35	Zr	65																					1984																												AMOR																		K		1.98					1.98																													kG/K		30.7																																								uOhm.cm							165																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50115	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.06 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd34Zr66	Pd	34	Zr	66																					1984																												AMOR																		K		2.1					2.1																													kG/K		27.5																																								uOhm.cm							151																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50116	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.19 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd32Zr68	Pd	32	Zr	68																					1984																												AMOR																		K		2.24					2.24																													kG/K		28																																								uOhm.cm							137																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50117	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 0.92 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd31Zr69	Pd	31	Zr	69																					1984																												AMOR																		K		2.34					2.34																													kG/K		28.2																																								uOhm.cm							179																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50118	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 0.86 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd29Zr71	Pd	29	Zr	71																					1984																												AMOR																		K		2.49					2.49																													kG/K		26.3																																								uOhm.cm							180																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50119	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 0.99 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd27Zr73	Pd	27	Zr	73																					1984																												AMOR																		K		2.6					2.6																													kG/K		28.6																																								uOhm.cm							172																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50120	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.08 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd23Zr77	Pd	23	Zr	77																					1984																												AMOR																		K		2.84					2.84	MTC50120																												kG/K		30.1																																								uOhm.cm							168																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50121	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.08 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd22Zr78	Pd	22	Zr	78																					1984																												AMOR																		K		2.88					2.88																													kG/K		30.1																																								uOhm.cm							170																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50122	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.09 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xPdx	Pd20Zr80	Pd	20	Zr	80																					1984																												AMOR																		K		2.91					2.91																													kG/K		29.8																																								uOhm.cm							168																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50123	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.91 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni31Zr69	Ni	31	Zr	69																					1984																												AMOR																		K		2.44					2.44																													kG/K		41.2																																								uOhm.cm							118																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50124	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.50 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni30Zr70	Ni	30	Zr	70																					1984																												AMOR																		K		2.58					2.58																													kG/K		38.2																																								uOhm.cm							140																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50125	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.41 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni29Zr71	Ni	29	Zr	71																					1984																												AMOR																		K		2.64					2.64																													kG/K		41.3																																								uOhm.cm							163																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50126	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.14 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni24Zr76	Ni	24	Zr	76																					1984																												AMOR																		K		2.94					2.94																													kG/K		38.4																																								uOhm.cm							193																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50127	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.19 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni21Zr79	Ni	21	Zr	79																					1984																												AMOR																		K		3.06					3.06																													kG/K		36.6																																								uOhm.cm							180																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50128	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.12 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni20Zr80	Ni	20	Zr	80																					1984																												AMOR																		K		3.17					3.17																													kG/K		33.3																																								uOhm.cm							175																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50129	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.09 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni18Zr82	Ni	18	Zr	82																					1984																												AMOR																		K		2.98					2.98																													kG/K		30.4																																								uOhm.cm							166																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50130	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.06 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni17Zr83	Ni	17	Zr	83																					1984																												AMOR																		K		3					3																													kG/K		29.7																																								uOhm.cm							168																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50131	PR0295207	composition by EDS. RESN shows RES at 25 K. dressed DOS(N*) = 1.10 states/eV.atom.spin calculated from RESN and (dHc2/dT).	Zr1-xNix	Ni16Zr84	Ni	16	Zr	84																					1984																												AMOR																		K		3.06					3.06																													kG/K		28.1																																								uOhm.cm							154																		rf-diode cosputtering					Electronic density of states in amorphous Zr-Pd and Zr-Ni alloys			Energy Conversion Devices, Incorporated, West Maple Road¿Troy, Michigan	Phys.Rev.B, 29(1984)5207	F.P.Missell,J.E.Keem		
50132	PR0305135	ribbon. Thickness = 20 micron.m. minimum in SUS at 20 K.	Zr1-xCox	Co35.38Zr64.62	Co	35.38	Zr	64.62																					1984																												AMOR																		K		2.67				0.013	2.67																																																																																																arc-melting. Ribonns by melt-spinning(induction furnace).					Normal-state magnetic susceptibility as a structural probe in an amorphous superconducting Zr-Co alloy			Department of Solid State Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 30(1984)5135	O.Rapp,L.Hedman		
50133	PR0313100	DOS = 6.9 state/eV.atom calculated from Rn and (dHc2/T).	U1-xCox	Co14.3U85.7	Co	14.3	U	85.7																					1985																												AMOR																		K		0.78					0.78																													kOe/K		44			MHC50133																																					uOhm.cm							73.4																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50134	PR0313100		U1-xCox	Co28U72	Co	28	U	72																					1985																												AMOR																		K		0.6					0.6																																																																							uOhm.cm							87.3																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50135	PR0313100	DOS = 5.8 state/eV.atom calculated from Rn and (dHc2/T).	U1-xFex	Fe14.3U85.7	Fe	14.3	U	85.7																					1985																												AMOR																		K		1					1																													kOe/K		40.5																																								uOhm.cm							85.6																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50136	PR0313100	DOS = 5.2 state/eV.atom calculated from Rn and (dHc2/T).	U1-xFex	Fe22U78	Fe	22	U	78																					1985																												AMOR																		K		0.98					0.98																													kOe/K		43			MHC50133																																					uOhm.cm							88.7																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50137	PR0313100		U1-xNix	Ni14.3U85.7	Ni	14.3	U	85.7																					1985																												AMOR																		K		0.53					0.53																																																																							uOhm.cm							73.5																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50138	PR0313100		U1-xNix	Ni28U72	Ni	28	U	72																					1985																												AMOR																		K					0.5																																																																									uOhm.cm							90																		arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50139	PR0313100	DOS = 2.6 state/eV.atom calculated from Rn and (dHc2/T).	Th1-xNix	Ni25Th75	Ni	25	Th	75																					1985																												AMOR																		K		3.7					3.7																													kOe/K		17.3			MHC50133																																																														arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50140	PR0313100	DOS = 2.8 state/eV.atom calculated from Rn and (dHc2/T).	Th1-xCox	Co20Th80	Co	20	Th	80																					1985																												AMOR																		K		3.8					3.8																													kOe/K		17.3																																																																	arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50141	PR0313100	DOS = 2.6 state/eV.atom calculated from Rn and (dHc2/T).	Zr1-xCox	Co25Zr75	Co	25	Zr	75																					1985																												AMOR																		K		3.18					3.18																													kOe/K		3.4																																																																	arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50142	PR0313100		Zr1-xFex	Fe30Zr70	Fe	30	Zr	70																					1985																												AMOR																		K		0.5					0.5																																																																																																arc-melting. Ribonns by melt-spinning.					Superconductivity in amorphous actinide alloys			Ames Laboratory, Iowa State University, Ames, Iowa	Phys.Rev.B, 31(1985)3100	S.J.Poon,A.J.Drehman,K.M.Wong,A.W.Clegg		
50143	PR0337820	starting sample is crystal. beta-Sn phase (Tc=3.9 K, dTc/dP = 15 mK/GPa). Tc shows Tc(crit)= Tc(15 GPa). Tc(max) = 5.2 K(P = 17 GPa).	a-Si	Si1	Si	1																							1986																												AMOR																		K		5			0		5	MTC50143		K/GPa	-0.044																																																																																												p-type semiconductor single crystal powder with acceptor= 1 E+13/cm3, prepared by crushing between two carbide pistons.					Pressure-induced superconductivity in high-pressure phases of Si				Phys.Rev.B, 33(1986)7820	C.N.J.Wagner,F.P.Bundy,K.J.Dunn,T.H.Lin,W.Y.Dong		
50144	PR0337820	starting sample is amorphous film. beta-Sn phase (Tc=6.8 K, dTc/dP = 5.2 mK/GPa). Tc shows Tc(crit)= Tc (15 GPa). Tc(max) = 8.4 K(P = 21 GPa).	a-Si	Si1	Si	1																							1986																												AMOR																		K		6.8			0		6.8	MTC50144		K/GPa	-0.053																																																																																												amorphous film(d=1 um) prepared by sputtering on 10 um-thick mica sheet.					Pressure-induced superconductivity in high-pressure phases of Si				Phys.Rev.B, 33(1986)7820	C.N.J.Wagner,F.P.Bundy,K.J.Dunn,T.H.Lin,W.Y.Dong		
50145	PR0344558	Tc(x) = 0.225(x-49.7) - 0.00306(x-49.7)^2 in Co<100-x>Zr<x>.	Co1-xZrx	Co40Zr60	Co	40	Zr	60																					1986																												AMOR																		K								MTC50145																																																																																													Zr(99.8%),Co(99.998%)		Ar-arc melting. melt-spun onto a roller at liq.N2 temp.					Superconductivity, normal-state resistivity, and magnetic susceptivility of amorphous Zr-Co alloys			Department of Solid State Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 34(1986)4558	M.Flodin,L.Hedman,O.Rapp		
50146	PR0344558	Tc(x) = 0.225(x-49.7) - 0.00306(x-49.7)^2 in Co<100-x>Zr<x>.	Co1-xZrx	Co20Zr80	Co	20	Zr	80																					1986																												AMOR																		K																																																																																																					Zr(99.8%),Co(99.998%)		Ar-arc melting. melt-spun onto a roller at liq.N2 temp.					Superconductivity, normal-state resistivity, and magnetic susceptivility of amorphous Zr-Co alloys			Department of Solid State Physics, The Royal Institute of Technology, Stockholm, Sweden	Phys.Rev.B, 34(1986)4558	M.Flodin,L.Hedman,O.Rapp		
50147	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P). two-step transition. maybe, existence of omega-phase Zr.	Ni1-xZrx	Ni20Zr80	Ni	20	Zr	80																					1989																												AMOR																		K		3.77					3.77			K/GPa	0.148																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50148	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P).	Ni1-xZrx	Ni29Zr71	Ni	29	Zr	71																					1989																												AMOR																		K		2.92					2.92			K/GPa	0.107																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50149	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P).	Ni1-xZrx	Ni33Zr67	Ni	33	Zr	67																					1989																												AMOR																		K		2.6					2.6			K/GPa	0.081																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50150	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P).	Ni1-xZrx	Ni36.5Zr63.5	Ni	36.5	Zr	63.5																					1989																												AMOR																		K		2.44					2.44			K/GPa	0.047																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50151	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P).	Ni1-xZrx	Ni40Zr60	Ni	40	Zr	60																					1989																												AMOR																		K		2.31					2.31			K/GPa	0.0245																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50152	PR0394677	quasihydrostatic pressure upto 8 GPa. Tc shows extraporated (P=0) value from Tc(P).	Ni1-xZrx	Ni45Zr55	Ni	45	Zr	55																					1989																												AMOR																		K		2					2			K/GPa	-0.075																																																																																												amorphous ribbon prepared by melt spinning onto Cu-wheel.					Pressure dependence of superconductivity in amorphous ZrxNi100-x alloys			Brock University, St.Catharines, Ontario, Canada	Phys.Rev.B, 34(1989)4677	F.Mahini,F.S.Razavi,Z.Altounian		
50153	JIM0210115		Nb1-xSix	Nb82Si18	Nb	82	Si	18																					1980																												AMOR																		K			4.4				4.4																																																																																																mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50154	JIM0210115		Nb1-xSix	Nb81Si19	Nb	81	Si	19																					1980																												AMOR																		K			4.35				4.35	MTC50154																																																																																															mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50155	JIM0210115		Nb1-xSix	Nb80Si20	Nb	80	Si	20																					1980																												AMOR																		K			4.23				4.23																																																																																																mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50156	JIM0210115	Hc2(0) shows Hc2(4.2K)	(Nb,Mo)0.8Si0.2	Nb70Mo10Si20	Nb	70	Mo	10	Si	20																			1980																												AMOR																		K			4.8				4.8																				T	RES	1.16				1.16		4.2	T/K	RES	2.89																																																																	mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50157	JIM0210115	Jc(4.2K) in A/cm2.	(Nb,Mo)0.8Si0.2	Nb60Mo20Si20	Nb	60	Mo	20	Si	20																			1980																												AMOR																		K			5				5																																																		4600																																														mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50158	JIM0210115	Hc2(0) shows Hc2(4.2K). Jc(4.2K) in A/cm2.	(Nb,Mo)0.8Si0.2	Nb55Mo25Si20	Nb	55	Mo	25	Si	20																			1980																												AMOR																		K			5.3				5.3																				T	RES	2.89				2.89		4.2	T/K	RES	2.89																			11000																																														mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50159	JIM0210115		(Nb,Si)0.96C0.04	Nb80Si16C4	Nb	80	Si	16	C	4																			1980																												AMOR																		K		4.5					4.5																																																																																																mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50160	JIM0210115	Hc2(0) shows Hc2(4.2K)	(Nb,Si)0.96Ge0.04	Nb80Si16Ge4	Nb	80	Si	16	Ge	4																			1980																												AMOR																		K		4.7					4.7																				T	RES	0.54				0.54		4.2	T/K	RES	2.76																																																																	mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
50161	JIM0210115	Hc2(0) shows Hc2(4.2K). Jc(4.2K) in A/cm2.	(Nb,Si)0.96B0.04	Nb80Si16B4	Nb	80	Si	16	B	4																			1980																												AMOR																		K		4.7					4.7																				T	RES	0.8				0.8		4.2	T/K	RES	2.39																			4400																																														mother compound melted in arc-furnace. rapid quench using Cu-roll.					Superconductivity of ductile Nb-based amorphous alloys			Tohoku University, Japan	Trans.JIM, 21(1980)115	T.Masumoto,A.Inoue,S.Sakai,H.Kimura,A.Hoshi		
90000	L093247004	RRR=6.5. structure: cubic, composed of distorted Pd6B octahedrons. Hc2(0)=6.2 T from linear extraporation. (delta-C/Tc) = 20.78 mj/mol.K2.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																			2004																															A	6.7523														K			8.2	8			8																				T		4.8							T/K		0.84																																																																	arc-melting					Superconductivity in the Metal Rich Li-Pd-B Ternary Boride			Institute for Materials Research, Tohoku University, 2-1-1, Katahira, Aoba-ku, Sendai, Japan	Phys.Rev.Lett., 93(2004)247004	H.Takeya,K.Hirata,K.Togano,P.Badica,S.Orimo,Y.Nakamori		
90001	L094107002	Two step s/c transition at Tc1=1.86 K, Tc2=1.72 K.. Two Hc1(0), 31 Oe and 44 Oe. Maybe 3rd s/c phase (Tc3=0.6 K)	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2005																												skutterudite																	skutterudite	K		1.86					1.86											Oe		44																					MHC90001																																																														Sb-flux method					Pronounced Enhancement of the Lower Critical Field and Critical Current Deep in the Superconducting State of PrOs4Sb12			Max Planck Institute for Chemical Physics of Solids, Dresden, Germany	Phys.Rev.Lett., 94(2005)107002	A.C.Mota,F.Steglich,M.B.Maple,N.A.Frederick,T.Cichorek,W.M.Yuhasz		
90002	L094107005	point contact tunneling (150 mK to 2.5 K). Two gaps (d1(0) = 0.95 meV and d2(0) = 2.4 meV) are observed. [gapene] shows higher value.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																			2005																																														K		2.3					2.3	MTC13320																																													meV	2.4	24	1																																															self-flux method					Spectroscopic Evidence for Multiple Order Parameter Components in the Heavy Fermion Superconductor CeCoIn5			Department of Physics, University of Toronto, Toronto, Ontario, M5S 1A7 Canada	Phys.Rev.Lett., 94(2005)107005	C.Petrovic,C.S.Turel,J.Berdeklis,J.Y.T.Wei,M.A.Tanatar,P.M.C.Rourke		
90003	ANG0351685		La9Br5(CBC)3	La9Br5B3C6	La	9	Br	5	B	3	C	6																	1996																																														K		6					6																																																																																																					La9Br5(CBC)3: A new superconductor				Angew.Chem.Int.ed.Engl., 35(1996)1685	A.Simon,C.Felser,H.Mattausch,R.Dronskowski		
90004	L094107001	RRR=5. R=A*T^2. Resistive Hc2 is different from diamagnetic Hc2.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		1	2005																																														K		0.68					0.68																																																																																																arc-melting - ANN(900C,5-10 d)					Low-Temperature Susceptibility of the Noncentrosymmetric Superconductor CePt3Si			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana, 70803, USA	Phys.Rev.Lett., 94(2005)107001	D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams,X.S.Wu		
90005	L094107001		(Ce,La)Pt3Si	Ce0.99La0.01Pt3Si1	Ce	0.99	La	0.01	Pt	3	Si	1																1	2005																																														K		0.57					0.57																																																																																																arc-melting - ANN(900C,5-10 d)					Low-Temperature Susceptibility of the Noncentrosymmetric Superconductor CePt3Si			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana, 70803, USA	Phys.Rev.Lett., 94(2005)107001	D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams,X.S.Wu		
90006	L094107001		(Ce,La)Pt3Si	Ce0.985La0.015Pt3Si1	Ce	0.985	La	0.015	Pt	3	Si	1																1	2005																																														K		0.15					0.15																																																																																																arc-melting - ANN(900C,5-10 d)					Low-Temperature Susceptibility of the Noncentrosymmetric Superconductor CePt3Si			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana, 70803, USA	Phys.Rev.Lett., 94(2005)107001	D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams,X.S.Wu		
90007	L094107001		(Ce,La)Pt3Si	Ce0.98La0.02Pt3Si1	Ce	0.98	La	0.02	Pt	3	Si	1																1	2005																																														K		0.03					0.03																																																																																																arc-melting - ANN(900C,5-10 d)					Low-Temperature Susceptibility of the Noncentrosymmetric Superconductor CePt3Si			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana, 70803, USA	Phys.Rev.Lett., 94(2005)107001	D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams,X.S.Wu		
90008	L094107001	not s/c.	(Ce,La)Pt3Si	Ce0.97La0.03Pt3Si1	Ce	0.97	La	0.03	Pt	3	Si	1																1	2005																																														K																																																																																																							arc-melting - ANN(900C,5-10 d)					Low-Temperature Susceptibility of the Noncentrosymmetric Superconductor CePt3Si			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana, 70803, USA	Phys.Rev.Lett., 94(2005)107001	D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams,X.S.Wu		
90009	P071060502	B-doped diamond. B-content = 2.5 E+21 B/cm3. carrier = 1.8 /cm3 from Hall effect. (dC/gamma*Tc) = 0.5	diamond	C1	C	1																							2005																												diamond																	diamond	K	3.4		4.5				3.95																				T	Tc(on), WHH theory	14							T/K	Tc(on)	4.7			MHC90009		A	Hc2	48																		mj/mol.K2	0.113		1440																																					starting (4 wt% B - diamond)					Superconducting and normal-state properties of heavily hole-doped diamond			Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow Region, Russia	Phys.Rev.B, 71(2005)060502	E.A.Ekimov,E.D.Bauer,J.D.Tompson,S.M.Stishov,V.A.Sidorov		
90010	P071064505		(Cu,K)1.5Co1.5S4	Cu1.3K0.2Co1.5S4	Cu	1.3	K	0.2	Co	1.5	S	4																1	2005																												spinel																	spinel	K	4.37		4.54	4.4			4.4																				T		1.89																																																																								CuS,Co,K2CO3,S		Chemical reaction. SIN(1073K, 48h) in evacuated quartz tube.					Superconductivity in thiospinel Cu1.3K0.2Co1.5S4			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People's Republic of China	Phys.Rev.B, 71(2005)064505	H.Chen,H.H.Wen,L.Fang,L.Shan,P.Y.Zou,X.F.Lu,Z.Xu		
90011	SST017S250	RR=2.15 microOhmcm. e-ph = 0.67. Hc2 defined as disapperance of Andreev reflection.	ZrB12	B12Zr1	B	12	Zr	1																				3	2004																												UB12			A	7.4072													UB12	K				6.2			6.2																				T	Andreev reflection	0.112												MHC90011												meV	1.22	4.8											283	Broch-Gruneisen eq. R																																				floating zone method					Andreev-reflection spectroscopy in ZrB12 single crystals			INFM?Dipartimento di Fisica, Politecnico di Torino, 10129 Torino, Italy	Supercond.Sci.Technol., 17(2004)S250	A.Calzolari,D.Daghero,G.A.Ummarino,R.S.Gonnelli,V.A.Stepanov,V.B.Filippov,Valeria Dellarocca,Y.B.Paderno		
90012	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2005																												skutterudite																	skutterudite	K		1.77					1.77																																																								mj/mol.K2	421	SP-heat	186	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90013	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os3.8Ru0.2Sb12	Pr	1	Os	3.8	Ru	0.2	Sb	12																	2005																												skutterudite																	skutterudite	K		1.63					1.63																																																								mj/mol.K2	617	SP-heat	199	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90014	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os3.6Ru0.4Sb12	Pr	1	Os	3.6	Ru	0.4	Sb	12																	2005																												skutterudite																	skutterudite	K		1.62					1.62																																																								mj/mol.K2	565	SP-heat	200	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90015	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os3.2Ru0.8Sb12	Pr	1	Os	3.2	Ru	0.8	Sb	12																	2005																												skutterudite																	skutterudite	K		1.54					1.54																																																								mj/mol.K2	393	SP-heat	152	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90016	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os2.4Ru1.6Sb12	Pr	1	Os	2.4	Ru	1.6	Sb	12																	2005																												skutterudite																	skutterudite	K		1.21					1.21																																																								mj/mol.K2	138	SP-heat	138	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90017	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os1.6Ru2.4Sb12	Pr	1	Os	1.6	Ru	2.4	Sb	12																	2005																												skutterudite																	skutterudite	K		0.75					0.75																																																								mj/mol.K2	35.8	SP-heat	181	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90018	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	Pr(Os,Ru)4Sb12	Pr1Os0.6Ru3.4Sb12	Pr	1	Os	0.6	Ru	3.4	Sb	12																	2005																												skutterudite																	skutterudite	K		0.94					0.94																																																								mj/mol.K2	49.3	SP-heat	218	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90019	P071064508	SP-heat. gamma and debye-T by fitting for Gamma<3> ground state.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																			2005																												skutterudite																	skutterudite	K		1.11					1.11																																																								mj/mol.K2	59.1	SP-heat	232	SP-heat																																									Evolution of crystalline electric field effects, superconductivity, and heavy-fermion behavior in the specific heat of Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 71(2005)064508	M.B.Maple,N.A.Frederick,T.A.Sayles		
90020	PHC2710311	lattice constant by NED. s/c properties not measured.	HoNiBC	Ho1Ni1B1C1	Ho	1	Ni	1	B	1	C	1																	1996								9.82																				Er4Rh6Sn19			A	3.5631		7.5486												K																																																																																																							arc-melting					Neutoron powder diffraction study of the nuclear and magnetic structures of HoNi1.985Co0.015B2C and HoNiBC			Reactor Radiation Division,National Institute of Standards and Technology, Gaithersburg, MD 20899, USA	Physica.C,271(1996)311-318	A. Santoro,B.C. Chakoumakos,J.J. Krajewski,J.W. Lynn,Q. Huang,R.J. Cava,W.F. Peck, Jr.		
90021	MRB0170963		Er4Ru6Sn19	Er4Ru6Sn19	Er	4	Ru	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.73		27.354											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90022	MRB0170963		Lu4Ru6Sn19	Lu4Ru6Sn19	Lu	4	Ru	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.692		27.263											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90023	MRB0170963		Er4Co6Sn19	Er4Co6Sn19	Er	4	Co	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.529		26.932											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90024	MRB0170963		Lu4Co6Sn19	Lu4Co6Sn19	Lu	4	Co	6	Sn	19																			1982																												Er4Rh6Sn19																	Er4Rh6Sn19 type, Pearson=tI232	K		1.5					1.5																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90025	MRB0170963		Sc4Rh6Sn19	Sc4Rh6Sn19	Sc	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.565		27.034											Er4Rh6Sn19 type, Pearson=tI232	K		4.5					4.5																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90026	MRB0170963		Y4Rh6Sn19	Y4Rh6Sn19	Y	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.772		27.456											Er4Rh6Sn19 type, Pearson=tI232	K		3.2					3.2																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90027	MRB0170963		Ho4Rh6Sn19	Ho4Rh6Sn19	Ho	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.747		27.388											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90028	MRB0170963		Er4Rh6Sn19	Er4Rh6Sn19	Er	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.725		27.365											Er4Rh6Sn19 type, Pearson=tI232	K		1.2					1.2																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90029	MRB0170963		Tm4Rh6Sn19	Tm4Rh6Sn19	Tm	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.706		27.32											Er4Rh6Sn19 type, Pearson=tI232	K		2.3					2.3																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90030	MRB0170963		Lu4Rh6Sn19	Lu4Rh6Sn19	Lu	4	Rh	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.693		27.289											Er4Rh6Sn19 type, Pearson=tI232	K		4					4																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90031	MRB0170963		Sc4Ir6Sn19	Sc4Ir6Sn19	Sc	4	Ir	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.574		27.057											Er4Rh6Sn19 type, Pearson=tI232	K		1.1					1.1																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90032	MRB0170963		Er4Ir6Sn19	Er4Ir6Sn19	Er	4	Ir	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.756		27.402											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90033	MRB0170963		Tm4Ir6Sn19	Tm4Ir6Sn19	Tm	4	Ir	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.727		27.371											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90034	MRB0170963		Yb4Ir6Sn19	Yb4Ir6Sn19	Yb	4	Ir	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.757		27.444											Er4Rh6Sn19 type, Pearson=tI232	K					1.1																																																																																																							Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90035	MRB0170963		Lu4Ir6Sn19	Lu4Ir6Sn19	Lu	4	Ir	6	Sn	19																			1982																												Er4Rh6Sn19			A	13.708		27.325											Er4Rh6Sn19 type, Pearson=tI232	K		3.2					3.2																																																																																																					Isotherms of the superconducting/magnetic ternary stannides				Mat.Res.Bull., 17(1982)963	A.S.Cooper,G.P.Espinosa,H.Barz		
90036	LES0710135		InMo3Se3	In1Mo3Se3	In	1	Mo	3	Se	3																			1980																												Tl2Fe6Te6	P6<3>/m		A	8.835		4.492											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																											J.Less-Common Met., 71(1980)135	A.Lipka,H.G.vonSchnering,K.Yvon,W.Honle		
90037	LES0710135		InMo3Te3	In1Mo3Te3	In	1	Mo	3	Te	3																			1980																												Tl2Fe6Te6	P6<3>/m		A	9.326		4.59											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																											J.Less-Common Met., 71(1980)135	A.Lipka,H.G.vonSchnering,K.Yvon,W.Honle		
90038	LES0710135		TlMo3Se3	Tl1Mo3Se3	Tl	1	Mo	3	Se	3																			1980																												Tl2Fe6Te6	P6<3>/m		A	8.918		4.482											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																											J.Less-Common Met., 71(1980)135	A.Lipka,H.G.vonSchnering,K.Yvon,W.Honle		
90039	LES0710135		TlMo3Te3	Tl1Mo3Te3	Tl	1	Mo	3	Te	3																			1980																												Tl2Fe6Te6	P6<3>/m		A	9.428		4.583											Tl2Fe6Te6 type,  Pearson=tI232	K		5.84					5.84																																																																																																									J.Less-Common Met., 71(1980)135	A.Lipka,H.G.vonSchnering,K.Yvon,W.Honle		
90040	LES0710135		TlFe3Te3	Tl1Fe3Te3	Tl	1	Fe	3	Te	3																			1980																												Tl2Fe6Te6	P6<3>/m		A	9.35		4.223											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																											J.Less-Common Met., 71(1980)135	A.Lipka,H.G.vonSchnering,K.Yvon,W.Honle		
90041	MRB0190915		Li2Mo6Se6	Li2Mo6Se6	Li	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	8.513		4.48											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90042	MRB0190915		Na2Mo6Se6	Na2Mo6Se6	Na	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	8.629		4.479											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90043	MRB0190915		K2Mo6Se6	K2Mo6Se6	K	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	9.022		4.481											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90044	MRB0190915		Rb2Mo6Se6	Rb2Mo6Se6	Rb	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	9.243		4.483											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90045	MRB0190915		Cs2Mo6Se6	Cs2Mo6Se6	Cs	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	9.533		4.484											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90046	MRB0190915		In2Mo6Se6	In2Mo6Se6	In	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	8.851		4.497											Tl2Fe6Te6 type,  Pearson=tI232	K					1																																																																																																							A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90047	MRB0190915		Te2Mo6Se6	Te2Mo6Se6	Te	2	Mo	6	Se	6																			1984																												Tl2Fe6Te6			A	8.933		4.478											Tl2Fe6Te6 type,  Pearson=tI232	K		3					3																																																																																																					A facile synthesis of pseudo one-monodimensional ternary molybdenum chalcogenides M2Mo6X6 (X = Se,Te; M = Li,Na..Cs)				Mater.Res.Bull., 19(1984)915	F.J.Disalvo,G.W.Hull,J.M.Tarascon		
90048	A097073903	RRR=2.5. (dC/Tc)=27 mj/mol.K2. (dC/gamma*Tc) = 2.7. PENET = 2001 A at 1.8K.. G-L = 17.3.	La3Ir2Ge2	La3Ir2Ge2	La	3	Ir	2	Ge	2																		1	2005																												La3Ni2Ga2	Pbcm		A	5.819	8.217	13.644												K	4.7			4.7			4.7											Oe					117			1.8	T	WHH	2.69			2.46			1.8	T/K		0.83					A		111																mj/mol.K	126.9	mj/mol.K2	10														uOhm.cm							71.4																		arc-melting in Ar, ANN(800C), then Quench.					Short-range magnetic correlation with Kondo-lattice behavior in Ce3Ir2Ge2 and superconductivity in La3Ir2Ge2	3		Institute for Materials Research, Tohoku University, Oarai, Ibaraki, 311-1313 Japan	J.Appl.Phys., 97(2005)073903	A.Tobe,D.X.Li,H.Onodera,S.Nimori,Y.Haga,Y.Homma,Y.Onuki,Y.Shiokawa		
90049	A097073903		Ce3Ir2Ge2	Ce3Ir2Ge2	Ce	3	Ir	2	Ge	2																		1	2005					uB/Ce	1.92	-29.1	7.5																				La3Ni2Ga2	Pbcm			5.729	8.124	13.507												K					2																																																																																																		arc-melting in Ar, ANN(800C), then Quench.					Short-range magnetic correlation with Kondo-lattice behavior in Ce3Ir2Ge2 and superconductivity in La3Ir2Ge2	3		Institute for Materials Research, Tohoku University, Oarai, Ibaraki, 311-1313 Japan	J.Appl.Phys., 97(2005)073903	A.Tobe,D.X.Li,H.Onodera,S.Nimori,Y.Haga,Y.Homma,Y.Onuki,Y.Shiokawa		
90050	JPS0733389	La<139>-NMR. e-ph = 1.0 estimated from Debye-T.	La3Ir2Ge2	La3Ir2Ge2	La	3	Ir	2	Ge	2																		1	2004																												La3Ni2Ga2																		K	4.7						4.7																																																3.52	6																																															arc-melting in Ar, ANN(800C), then Quench.					<139>La NQR Relaxation in a Superconductor La3Ir2Ge2			Department of Physics, Faculty of Engineering, University of Tokushima, Tokushima, Japan	J.Phys.Soc.Jpn, 73(2004)3389	D.X.Li,T.Ohno,Y.Homma,Y.Kawasaki,Y.Kishimoto,Y.Shiokawa		
90051	SST0180183		MgB2	B2Mg1	B	2	Mg	1																				1	2005																												AlB2																		K			38.6				38.6																				T	WHH	14.2												MHC90051																																																														mixture(Mg,B,Al) wrapped in Ta-foil,  then heat(950C,2h, 3.5 GPa)					The upper critical field and two-gap nature in Mg1-xAlxB2			Pohang University of Science and Technology, Pohang, Korea	Supercond.Sci.Technol., 18(2005)183	Byeongwon Kang,Heon-Jung Kim,Min-Seok Park,Sung-Ik Lee		
90052	SST0180183		(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																		1	2005																												AlB2																		K			37.5				37.5																				T	WHH	10.8																																																																										mixture(Mg,B,Al) wrapped in Ta-foil,  then heat(950C,2h, 3.5 GPa)					The upper critical field and two-gap nature in Mg1-xAlxB2			Pohang University of Science and Technology, Pohang, Korea	Supercond.Sci.Technol., 18(2005)183	Byeongwon Kang,Heon-Jung Kim,Min-Seok Park,Sung-Ik Lee		
90053	SST0180183		(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																		1	2005																												AlB2																		K			33.4				33.4																				T	WHH	9.1																																																																										mixture(Mg,B,Al) wrapped in Ta-foil,  then heat(950C,2h, 3.5 GPa)					The upper critical field and two-gap nature in Mg1-xAlxB2			Pohang University of Science and Technology, Pohang, Korea	Supercond.Sci.Technol., 18(2005)183	Byeongwon Kang,Heon-Jung Kim,Min-Seok Park,Sung-Ik Lee		
90054	SST0180183		(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																		1	2005																												AlB2																		K			26.7				26.7																				T	WHH	5.2																																																																										mixture(Mg,B,Al) wrapped in Ta-foil,  then heat(950C,2h, 3.5 GPa)					The upper critical field and two-gap nature in Mg1-xAlxB2			Pohang University of Science and Technology, Pohang, Korea	Supercond.Sci.Technol., 18(2005)183	Byeongwon Kang,Heon-Jung Kim,Min-Seok Park,Sung-Ik Lee		
90095	PRL0391161	Pcrit = 34 kbar. Tc monotonically increases upto 48 kbar. Tc(max) = 0.5 K at P=48 kbar.	Ba	Ba1	Ba	1																							1977																												bcc																		K		0.5			0		0.5	MTC90095																																																																																																				Superconductivity of bcc Barium under Pressure				Phys.Rev.Lett., 39(1977)1161	C.Probst,J.Wittig		
90096	PRB0250194	Tc decreases from 4.8 K(P=251 kbar) to 4.2 K(P=383 kbar).	Ba	Ba1	Ba	1																							1982																																														K		4.8			0		4.8	MTC90096																																																																																																				Pressure-induced superconductivity in strontium and barium				Phys.Rev.B, 42(1982)194	F.P.Bundy,K.J.Dunn		
90097	PRB0250194	Pcrit = 300 kbar.	Sr	Sr1	Sr	1																							1982																																														K		3.55			0		3.55	MTC90097																																																																																																				Pressure-induced superconductivity in strontium and barium				Phys.Rev.B, 42(1982)194	F.P.Bundy,K.J.Dunn		
90098	PRL0231375	beta-La	La	La1	La	1																							1969																												fcc																		K		5.9					5.9	MTC90098		K/GPa	1.31																																																																																																	Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90099	PRL0231375	alpha-La	La	La1	La	1																							1969																												dhcp																		K		4.86					4.86	MTC90099		K/GPa	1.4																																																																																																	Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90100	PRL0231375		La1-xCex	Ce0.0007La0.9993	Ce	0.0007	La	0.9993																					1969																												fcc																		K		4.65					4.65	MTC90098																																																																																																				Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90101	PRL0231375		La1-xCex	Ce0.013La0.987	Ce	0.013	La	0.987																					1969																												fcc																		K		3.7					3.7	MTC90098																																																																																																				Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90102	PRL0231375		La1-xCex	Ce0.013La0.987	Ce	0.013	La	0.987																					1969																												dhcp																		K		3.1					3.1	MTC90099																																																																																																				Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90103	PRL0231375		La1-xCex	Ce0.02La0.98	Ce	0.02	La	0.98																					1969																												fcc																		K		2.56					2.56	MTC90098																																																																																																				Pressure-Induced Magnetic-Nonmagnetic Transition of Ce Impurities in La				Phys.Rev.Lett., 23(1969)1375	J.Wittig,K.S.Kim,M.B.Maple		
90104	PRL0420469	Pcrit = 180 kbar. Tc(max) = 0.34 K (P=215 kbar).	Sc	Sc1	Sc	1																							1979																												hcp																		K		0.34			0		0.34	MTC90104																																																																																																				Superconductivity in a New High-Pressure Phase of Scandium				Phys.Rev.Lett., 42(1979)469	C.Probst,F.A.Schmidt,J.Wittig,K.A.Gschneider,Jr.		
90105	JPS0593843	99.8% purity. Phase transitions at P=7 and 31 GPa (hcp - hexagonal - bcc). dTc/dP = 0.12 K/GPa (hex), = -0.14 K/GPa (bcc).	Zr	Zr1	Zr	1																							1990																																														K		0.52					0.52	MTC90105																																																																																																				SUPERCONDUCTIVITY AND PHASE TRANSITION OF ZIRCONIUM UNDER HIGHPRESSURE UP TO 50 GPA	199011			J.PHYS.SOC.JAPAN,59(1990)3843	HARUKI KAWAMURA,MOTOTADA KOBAYASHI,YUICHI AKAHAMA	ZR	
90106	PRL0794262	Tc depends on the pressure medium used and on the compression process.	Nb	Nb1	Nb	1																							1997																																														K		9.2					9.2	MTC90106																																																																																																				Superconducting Tc and electron-phonon coupling in Nb to 132 GPa: Magnetic susceptibility at megabar pressures				Phys.Rev.Lett., 79(1997)4262	Ho-kwang Mao,R.J.Hemley,V.V.Struzhkin,Y.A.Timofeev		
90107	PRL0794262		Ta	Ta1	Ta	1																							1997																																														K		4.4					4.4	MTC90107																																																																																																				Superconducting Tc and electron-phonon coupling in Nb to 132 GPa: Magnetic susceptibility at megabar pressures				Phys.Rev.Lett., 79(1997)4262	Ho-kwang Mao,R.J.Hemley,V.V.Struzhkin,Y.A.Timofeev		
90108	PR1120031		Sn	Sn1	Sn	1																							1958																																														K		3.732					3.732	MTC90108		K/GPa	-0.49																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90109	PR1120031		In	In1	In	1																							1958																																														K		3.403					3.403	MTC90109		K/GPa	-0.43																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90110	PR1120031		Ta	Ta1	Ta	1																							1958																																														K		4.301					4.301	MTC90110		K/GPa	-0.026																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90111	PR1120031		Tl	Tl1	Tl	1																							1958																																														K		2.38					2.38	MTC90111		K/GPa	0.237																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90112	PR1120031		alpha-Hg	Hg1	Hg	1																							1958																																														K		4.156					4.156	MTC90112		K/GPa	-0.336																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90113	PR1120031		beta-Hg	Hg1	Hg	1																							1958																																														K		4.017					4.017	MTC90112		K/GPa	-0.43																																																																																																	Effects of pressure on the superconducting transition temperatures of Sn, In, Ta, Tl, and Hg				Phys.Rev., 112(1958)31	C.A.Swenson,L.D.Jennings		
90114	PRL0350104		Al	Al1	Al	1																							1975																																														K		1.18					1.18	MTC90114																																																																																																				High-pressure effects on the superconducting transition temperature of aluminum				Phys.Rev.Lett., 35(1975)104	A.W.Webb,D.U.Gubser		
90115	PRL0441623	The lower and upper pressure phases (metallic) with different Tc exist. The lower Tc(max)=4.67 K, the upper Tc(max)=6.30 K.	Te	Te1	Te	1																							1980																																														K		6.3			0		6.3	MTC90115																																																																																																				Pressure dependence of superconducting transition temperature of high-pressure metallic Te				Phys.Rev.Lett., 44(1980)1623	F.P.Bundy,K.J.Dunn		
90116	PR05016274	black-P(simple cubic). Pcrit = 11 GPa. P is continuously increased at 4.2 K.	P	P1	P	1																							1994																												cubic																		K		10.7			0		10.7	MTC90116																																																																																																				Phase transitions and superconductivity of black phosphorus and phosphorus-arsenic alloys at low temperatures and high pressures				Phys.Rev.B, 50(1994)16274	H.Kawamura,I.Shirotani,J.Mikami,K.Tsuji,O.Shimomura,T.Adachi,T.Nakajima,Y.Katayama		
90117	PR05016274	simple cubic. Pcrit = 16 GPa. P is continuously increased at 4.2 K.	P1-xAsx	As0.1P0.9	As	0.1	P	0.9																					1994																												cubic																		K		9.9			0		9.9	MTC90116																																																																																																				Phase transitions and superconductivity of black phosphorus and phosphorus-arsenic alloys at low temperatures and high pressures				Phys.Rev.B, 50(1994)16274	H.Kawamura,I.Shirotani,J.Mikami,K.Tsuji,O.Shimomura,T.Adachi,T.Nakajima,Y.Katayama		
90118	PR0465523	Pcrit = 27 GPa. Tc(max) = 2.4 K(P=32 GPa).	As	As1	As	1																							1992																																														K		2.4			0		2.4	MTC90118																																																																																																				SUPERCONDUCTIVITY IN ARSENIC AT HIGH PRESSURES	199209	PRESSURE            ,TC                  ,PHASE TRANSITION	DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA, BARKELEY	PHYS.REV.B,46(1992)5523	A.L.Chen,ANTHONY L.CHEN,M.L.Cohen,MARVIN L.COHEN,P.Y.Yu,PETER Y.YU,S.P.Lewis,STEVEN P.LEWIS,ZHENPENG SU,Zh.Su	AS	
90119	PR0337820	amorphous. Pcrit = 15 GPa(Tc=7.6 K). Tc(max) = 8.4 K(P = 21 GPa). Tc decreases monotonically from Tc(max).	Si	Si1	Si	1																							1986																																														K		8.4			0		8.4	MTC90119		K/GPa	-0.053																																																																																																	Pressure-induced superconductivity in high-pressure phases of Si				Phys.Rev.B, 33(1986)7820	C.N.J.Wagner,F.P.Bundy,K.J.Dunn,T.H.Lin,W.Y.Dong		
90120	PR0337820	crystalline. Pcrit = 13 GPa(Tc=7.6 K). Tc(max) = 5.2 K(P =171 GPa). Tc decreases monotonically from Tc(max).	Si	Si1	Si	1																							1986																																														K		5.2			0		5.2	MTC90119		K/GPa	-0.044																																																																																																	Pressure-induced superconductivity in high-pressure phases of Si				Phys.Rev.B, 33(1986)7820	C.N.J.Wagner,F.P.Bundy,K.J.Dunn,T.H.Lin,W.Y.Dong		
90121	FTT0142527	Fig.1 in Phys.Rev.Lett., 44(1980)1623.	Te	Te1	Te	1																							1973																																														K		4.3			0		4.3	MTC90121																																																																																																								Sov.Phys.Solid State, 14(1973)2192	I.V.Berman,P.Kurkin,Zh.I.Binzarov		
90122	P071132508	T(CDW) and Tc measured upto P=11 GPa.	ZrTe3	Te3Zr1	Te	3	Zr	1																				3	2005																																														K		2.1					2.1	MTC90122																																																																																															iodine transport method					Pressure effect on competition between charge density wave and superconductivity in ZrTe3: Appearance of pressure-induced reentrant superconductivity			Department of Applied Physics, Graduate School of Engineering, Hokkaido University, Sapporo, Japan	Phys.Rev.B, 71(2005)132508	K.Yamaya,M.Abliz,M.Hedo,R.Yomo,Y.Uwatoko		
90123	P071144505	RRR=7.2. DB shows values for sigma-band. For pai-band, gap=2.85 meV, gapene = 1.70.	MgB2	B2Mg1	B	2	Mg	1																				1	2005																												AlB2																		K		39					39																																		MHC90123													7.5	4.4	1																																																				Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90124	P071144505	RRR=4.7	(Mg,Al)B2	Mg0.95Al0.05B2	Mg	0.95	Al	0.05	B	2																		1	2005																												AlB2																		K		36.6					36.6																																		MHC90124																																																																			Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90125	P071144505	RRR=2.7	(Mg,Al)B2	Mg0.93Al0.07B2	Mg	0.93	Al	0.07	B	2																		1	2005																												AlB2																		K		35.8					35.8																																		MHC90123																																																																			Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90126	P071144505	RRR=2.2. DB shows values for sigma-band. For pai-band, gap=2.5 meV, gapene = 1.75.	(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																		1	2005																												AlB2																		K		33.4					33.4																																		MHC90124													5.4	3.9	1																																																				Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90127	P071144505	RRR=1.9	(Mg,Al)B2	Mg0.85Al0.15B2	Mg	0.85	Al	0.15	B	2																		1	2005																												AlB2																		K		31.5					31.5																																		MHC90123																																																																			Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90128	P071144505	RRR=2.1. DB shows values for sigma-band. For pai-band, gap=1.7 meV, gapene = 1.4.	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																		1	2005																												AlB2																		K		29.1					29.1																																		MHC90124													3.8	3	1																																																				Critical field of Al-doped MgB2 samples: Correlation with the suppression of the sigma-band gap			INFM-LAMIA, Dipartimento di Fisica, Universita di Genova, via Dodecaneso 33, 16146 Genoa, Italy	Phys.Rev.B, 71(2005)144505	A.Palenzona,C.Ferdeghini,C.Tarantini,D.Daghero,I.Pallecchi,M.Monni,M.Putti,P.Manfriinetti,R.S.Gonnelli,V.A.Stepanov		
90129	P071144512	anisotropy(T=0 K) = 6.39	MgB2	B2Mg1	B	2	Mg	1																				1	2005																												AlB2																		K				38.8			38.8																				T			16.2	2.54																																																																								two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90130	P071144512	anisotropy(T=0 K) = 4.32	(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																		1	2005																												AlB2																		K				32.1			32.1																							12.7	2.92										MHC90130																																																														two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90131	P071144512	anisotropy(T=0 K) = 2.26	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																		1	2005																												AlB2																		K				25.6			25.6																							5.54	2.39																																																																								two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90132	P071144512		(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																		1	2005																												AlB2																		K				7.9			7.9																																																																																																two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90133	P071144512	anisotropy(T=0 K) = 5.40	Mg(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																		1	2005																												AlB2																		K				36			36																							32.1	5.91																																																																								two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90134	P071144512	anisotropy(T=0 K) = 2.71	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		1	2005																												AlB2																		K				21			21																							24.6	9.13																																																																								two step synthesis. heat(1000 - 1200C,10d) - press to pellet - heat(1200C,10d)					Difference between Al and C doping in anisotropic upper critical field development in MgB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 71(2005)144512	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90135	P070174503	nearly single phase. RRR=1.85. e-ph coupling = 1.45. G-L =43.3. Specific heat measurements. (dC/gamma*Tc) = 2.09	MgCNi3	Mg1C1.6Ni3	Mg	1	C	1.6	Ni	3																		1	2004																												ABO3			A	3.8107														K		6.9	7	7			6.9											mT		11.3							T		11														A		54.7			A		2370													mj/mol.K2	27	SP-heat	292	SP-heat																																				mixture - pellet - wrapped in Ta foil - quartz tube(Ar atmosphere) - SIN(600C,0.5h + 900C,1h)					Evidence for strong electron-phonon coupling in MgCNi3			Institut fur Festkorper- und Werkstoffforschung Dresden, Postfach 270116, D-01171 Dresden, Germany	Phys.Rev.B, 70(2004)174503	A.Handstein,A.Walte,G.Fuchs,H.Rosner,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.Shulga,V.N.Narozhnyi		
90136	P067052501	(dC/gamma*Tc) = 1.97	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2003																												ABO3																		K		6.4					6.4																				T		10.6														A		56			A		1280					4	14							mj/mol.K2	33.6	SP-heat	287	SP-heat																																				wrapped in Ta foil - SIN(600C + 900C)					BCS-like superconductivity in MgCNi3			Institute of Physics, National Chiao Tung University, Hsinchu 300, Taiwan, Republic of China	Phys.Rev.B, 67(2003)052501	C.-Q.Jin,H.D.Yang,H.L.Huang,J.-Y.Lin,P.H.Lin,P.L.Ho,R.-C.Yu,Y.-L.Zhang		
90137	L094157002		(Pb,Tl)Te	Pb0.996Tl0.004Te1	Pb	0.996	Tl	0.004	Te	1																		3	2005																																														K		0.061					0.061																																																																																																single crystals were grown by an unseeded vapor transport method.					Evidence for Charge Kondo Effect in Superconducting Tl-Doped PbTe			Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305-4045, USA	Phys.Rev.Lett., 94(2005)157002	H.Bluhm,I.R.Fisher,T.H.Geballe,Y.Matsushita		
90138	L094157002		(Pb,Tl)Te	Pb0.9922Tl0.0078Te1	Pb	0.9922	Tl	0.0078	Te	1																		3	2005																																														K		0.51					0.51																																																																																																single crystals were grown by an unseeded vapor transport method.					Evidence for Charge Kondo Effect in Superconducting Tl-Doped PbTe			Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305-4045, USA	Phys.Rev.Lett., 94(2005)157002	H.Bluhm,I.R.Fisher,T.H.Geballe,Y.Matsushita		
90139	L094157002		(Pb,Tl)Te	Pb0.987Tl0.013Te1	Pb	0.987	Tl	0.013	Te	1																		3	2005																																														K		1.32					1.32	MTC90139																																																																																															single crystals were grown by an unseeded vapor transport method.					Evidence for Charge Kondo Effect in Superconducting Tl-Doped PbTe			Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305-4045, USA	Phys.Rev.Lett., 94(2005)157002	H.Bluhm,I.R.Fisher,T.H.Geballe,Y.Matsushita		
90140	1246		(Sn,Ag)Te	Sn0.87Ag0.1Te1	Sn	0.87	Ag	0.1	Te	1																			1973																																														K		1.88					1.88																																																																																																					Superconductivity as a function of carrier density and magnetic spin concentration in the Sn-Te-MnTe system				J.PHYS.CHEM.SOLIDS,34(1973)183	C.K.JONES,D.W.DEIS,M.D.MATHUR,W.J.CARR JR.		
90141	1246		SnTe	Sn0.97Te1	Sn	0.97	Te	1																					1973																																														K		0.189					0.189																																																																																												n/cm3	1320000000000000000000								Superconductivity as a function of carrier density and magnetic spin concentration in the Sn-Te-MnTe system				J.PHYS.CHEM.SOLIDS,34(1973)183	C.K.JONES,D.W.DEIS,M.D.MATHUR,W.J.CARR JR.		
90142	1246	Mn = 10 ppm	SnTe	Sn0.97Te1	Sn	0.97	Te	1																					1973																																														K		0.087					0.087																																																																																												n/cm3	1130000000000000000000								Superconductivity as a function of carrier density and magnetic spin concentration in the Sn-Te-MnTe system				J.PHYS.CHEM.SOLIDS,34(1973)183	C.K.JONES,D.W.DEIS,M.D.MATHUR,W.J.CARR JR.		
90143	930	Sn4P2.65 by analysis. Hall coefficient at 77K.	Sn4P3	P3Sn4	P	3	Sn	4																					1969																																														K		1.24					1.24																																																																																					E-4 cm3/C				-2.1			E+22/cm3	3								On the superconductivity, carrier concentration and the ionic model of Sn4P3 and Sn4As3				PHYS.LETT.A,29(1969)293	M.H.VAN MARREN		
90144	930	Sn3.80As3 by analysis. Hall coefficient at 77K.	Sn4As3	As3Sn4	As	3	Sn	4																					1969																																														K		1.23					1.23																																																																																					E-4 cm3/C				-2.8			E+22/cm3	2.2								On the superconductivity, carrier concentration and the ionic model of Sn4P3 and Sn4As3				PHYS.LETT.A,29(1969)293	M.H.VAN MARREN		
90145	848	gamma-phase. Hall mobility = 2.0 cm3/V.sec	Tl5Te3	Te3Tl5	Te	3	Tl	5																					1968																												bct			A	8.92		12.63												K	2.19		2.23				2.21																																		MHC90145																																																			E-4 cm3/C	4.2						E+22/cm3	1.5								Electrical conductivity and superconductivity in the gamma-phase of the Tl-Te system				J.APPL.PHYS.,39(1968)3003	A.JUODAKIS,C.R.KANNEWURF		
90146	622	N- and O-concentrations not determined. substrate temp. = 30 C	NbNxOy	Nb1N1Oy	Nb	1	N	1																	O	y		4	1975																																														K		9.6				1.4	9.6																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90147	622	substrate temp. = 350 C	NbNxOy	Nb1N1.34O0.27	Nb	1	N	1.34																	O	y	0.27	4	1975																																														K		11.3				1.4	11.3																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90148	622	substrate temp. = 700 C	NbNxOy	Nb1N1.25O0.25	Nb	1	N	1.25																	O	y	0.25	4	1975																																														K		11.9				1.8	11.9																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90149	622	substrate temp. = 500 C	NbNxOy	Nb1N1.22O0.18	Nb	1	N	1.22																	O	y	0.18	4	1975																																														K		12.3				0.8	12.3																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90150	622	substrate temp. = 350 C.	NbNxOy	Nb1N1.08O0.27	Nb	1	N	1.08																	O	y	0.27	4	1975																																														K		12.8				0.7	12.8																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90151	622	substrate temp. = 650 C.	NbNxOy	Nb1N0.9O0.02	Nb	1	N	0.9																	O	y	0.02	4	1975																																														K		14.7				1.5	14.7																																																																																																RF-sputtering. various substrate tempeature. substrate= silica slides.					The effect of composition on the superconducting transition temperature in NbNxOy				MAT.RES.BULL.,10(1975)379	D.ROGOWSKI,P.F.CARCIA,R.MESSIER,R.ROY		
90152	515		In1-xTe	In0.95Te1	In	0.95	Te	1																					1965																												NaCl			A	6.14														K		2.7					2.7																																																																																												E+22 /cm3	1.47			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90153	515		In1-xTe	In0.91Te1	In	0.91	Te	1																					1965																												NaCl			A	6.11														K		2.04					2.04																																																																																												E+22 /cm3	1.28			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90154	515		In1-xTe	In0.87Te1	In	0.87	Te	1																					1965																												NaCl			A	6.081														K		1.55					1.55	MTC90154																																																																																											E+22 /cm3	1.09			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90155	515		In1-xTe	In0.83Te1	In	0.83	Te	1																					1965																												NaCl			A	6.055														K		1.15					1.15																																																																																												E+22 /cm3	0.88			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90156	515		In1-xTe	In0.82Te1	In	0.82	Te	1																					1965																												NaCl			A	6.052														K		1.06					1.06																																																																																												E+22 /cm3	0.83			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90157	515		In1+xTe	In1.15Te1	In	1.15	Te	1																					1965																												NaCl			A	6.179														K		2.6					2.6																																																																																												E+22 /cm3	1.34			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90158	515		In1+xTe	In1.1Te1	In	1.1	Te	1																					1965																												NaCl			A	6.182														K		2.8					2.8																																																																																												E+22 /cm3	1.45			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90159	515		In1+xTe	In1.05Te1	In	1.05	Te	1																					1965																												NaCl			A	6.181														K		3.41					3.41																																																																																												E+22 /cm3	1.58			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90160	515		In1+xTe	In1.015Te1	In	1.015	Te	1																					1965																												NaCl			A	6.178														K		3.51					3.51																																																																																												E+22 /cm3	1.67			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90161	515		In1+xTe	In1Te1	In	1	Te	1																					1965																												NaCl			A	6.177														K		3.45					3.45																																																																																												E+22 /cm3	1.71			NaCl type compounds were obtained by using 30 kbar, 400-500 C for less than 4 hr.					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
90162	988	gamma estimated from the data.	(Sr,Ba)TiO3	Sr0.925Ba0.075Ti1O3	Sr	0.925	Ba	0.075	Ti	1															O	3			1967																												ABO3																		K		0.5					0.5																																																					MSP90162			mj/mol.K2	2.4	SP-heat																																		E+19 /cm3	9.6								The heat capacity of a mixed titanate superconductor				PHYS.LETT.A,25(1967)623	J.H.COLWELL		
90163	1555	Pcrit = 120 kbar	Si	Si1	Si	1																							1973																																														K		6.7			0		6.7																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90164	1555	Pcrit = 115 kbar	Ge	Ge1	Ge	1																							1973																																														K		5.35			0		5.35																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90165	1555	Pcrit = 250 kbar	GaAs	As1Ga1	As	1	Ga	1																					1973																																														K		4.8			0		4.8																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90166	1555	Pcrit = 125 kbar	AlSb	Al1Sb1	Al	1	Sb	1																					1973																																														K		2.8			0		2.8																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90167	1555	Pcrit = 70 kbar	GaSb	Ga1Sb1	Ga	1	Sb	1																					1973																																														K		4.2			0		4.2																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90168	1555	Pcrit = 27 kbar	InTe	In1Te1	In	1	Te	1																					1973																																														K		2.18			0		2.18																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90169	1555	Pcrit = 25 kbar	BiSn	Bi1Sn1	Bi	1	Sn	1																					1973																																														K		7.88			0		7.88																																																																																																					Conditions for the appearance and the nature of surface superconductivity of indium antimonide				Sov.Phys.Semicond., 7(1973)593	G.A.VIKHILL,N.A.VITOVSKII,S.M.RYVKIN,T.V.MASHOVETS		
90170	1280	P-induced SC. Pcrit = 60 kbar. dTc/dP = 1.27 E-4 K/kbar at Pcrit. There are four phases. P(I-II) = 67.5 kbar. P(II-IV) = 81.4 kbar.	Bi2Te3	Bi2Te3	Bi	2	Te	3																					1972																																														K		2.8			0		2.8	MTC90170		K/GPa	1.27																																																																																																	Superconductivity of bismuth telluride				Sov.Phys.Solid State, 13(1972)2098	E.S.ITSKEVICH,M.A.IL'INA		
90171	594	Nb-doped SrTiO3. carrier doping by Nb-doping. mobility = 600 cm2/V.s. G-L = 8.4	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		3	1966																												ABO3																		K		0.43					0.43																																		MHC90171																						mj/mol.K2	1.6	SP-heat																																		E+20 /cm3	1.7								Magnetization and critical fields of superconducting SrTiO3				PHYS.REV.,148(1966)280	E.AMBLER,J.F.SCHOOLEY,J.H.COLWELL,W.R.HOSLER		
90172	594	carrier doping by reducing. mobility = 225 cm2/V.s at 4.2 K. G-L = 13.2	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		3	1966																												ABO3																		K		0.33					0.33																																		MHC90172																																																										E+20 /cm3	1								Magnetization and critical fields of superconducting SrTiO3				PHYS.REV.,148(1966)280	E.AMBLER,J.F.SCHOOLEY,J.H.COLWELL,W.R.HOSLER		
90173	1005		SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3			1967																												ABO3																		K		0.3					0.3											Oe	M-H curve	2.8																																																																															E+19 /cm3	5.8	SrTiO3,BaTiO3,CaTiO3		available powder mixture - press(15000 psi) - SIN(1600 C, 1h)					Superconductive properties of ceramic mixed titanates				PHYS.REV.,159(1967)301	E.R.PFEIFFER,H.P.R.FREDELIKSE,J.F.SCHOOLEY,W.R.HOSLER		
90174	1005		(Sr,Ba)TiO3	Sr0.95Ba0.05Ti1O3	Sr	0.95	Ba	0.05	Ti	1															O	3			1967																												ABO3																		K		0.5					0.5											Oe	M-H curve	3.9																																																																															E+19 /cm3	6.7	SrTiO3,BaTiO3,CaTiO3		available powder mixture - press(15000 psi) - SIN(1600 C, 1h)					Superconductive properties of ceramic mixed titanates				PHYS.REV.,159(1967)301	E.R.PFEIFFER,H.P.R.FREDELIKSE,J.F.SCHOOLEY,W.R.HOSLER		
90175	1005		(Sr,Ca)TiO3	Sr0.7Ca0.3Ti1O3	Sr	0.7	Ca	0.3	Ti	1															O	3			1967																												ABO3																		K		0.5					0.5											Oe	M-H curve	1.9																																																																															E+19 /cm3	6.7	SrTiO3,BaTiO3,CaTiO3		available powder mixture - press(15000 psi) - SIN(1600 C, 1h)					Superconductive properties of ceramic mixed titanates				PHYS.REV.,159(1967)301	E.R.PFEIFFER,H.P.R.FREDELIKSE,J.F.SCHOOLEY,W.R.HOSLER		
90177	JAP0400409	P-T phase diagram shown in text.	InSb-II	In1Sb1	In	1	Sb	1																					1969									7.3																			Tetra			A	5.862		3.105												K		2					2																																																																																																samples were annealed at various T and P, then quenched to 80 K priori-to P-release.					The P-T phase diagram of InSb at high temperatures and pressures				J.Appl.Phys., 40(1969)409	Mario D.Banus,Mary C.Lavine		
90178	JAP0400409	P-T phase diagram shown in text.	InSb-III	In1Sb1	In	1	Sb	1																					1969									8.5																			Hexa			A	6.099		5.708												K		4.1					4.1																																																																																																samples were annealed at various T and P, then quenched to 80 K priori-to P-release.					The P-T phase diagram of InSb at high temperatures and pressures				J.Appl.Phys., 40(1969)409	Mario D.Banus,Mary C.Lavine		
90179	JAP0400409	P-T phase diagram shown in text.	InSb-IV	In1Sb1	In	1	Sb	1																					1969									7.9																			Ortho			A	2.921	5.532	3.093												K		3.6					3.6																																																																																																samples were annealed at various T and P, then quenched to 80 K priori-to P-release.					The P-T phase diagram of InSb at high temperatures and pressures				J.Appl.Phys., 40(1969)409	Mario D.Banus,Mary C.Lavine		
90180	JPS0740700	RRR=1. G-L = 54. (dC/gamma*Tc) = 1.90	W7Re13B	W7Re13B1	W	7	Re	13	B	1																			2005																												beta-Mn	P4<1>32		A	6.819														K			7.1	7.1			7.1											mT		7.7							T	WHH theory	11.4							T/K		2.22			MHC90180		A		54			A	calculated from Hc1	2925					4.28	14							mj/mol.K2	65.16	SP-heat	257	SP-heat																																				mixture(W,Re,B,C) - arc-melting in Ar					Superconductivity in Intermetallic W7Re13X (X = B and C) Compounds			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa ,Japan	J.Phys.Soc.Jpn, 74(2005)700	A.Kawano,J.Akimitsu,K.Kawashima,T.Muranaka		
90181	JPS0740700	RRR=1. G-L = 80. (dC/gamma*Tc) = 1.93	W7Re13C	W7Re13C1	W	7	Re	13	C	1																			2005																												beta-Mn	P4<1>32		A	6.801														K			7.5	7.3			7.3											mT		4							T	WHH theory	12.6							T/K		2.23			MHC90180		A		51			A	calculated from Hc1	4060					4.02	14				MSP90181			mj/mol.K2	64.19	SP-heat	259	SP-heat																																				mixture(W,Re,B,C) - arc-melting in Ar					Superconductivity in Intermetallic W7Re13X (X = B and C) Compounds			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa ,Japan	J.Phys.Soc.Jpn, 74(2005)700	A.Kawano,J.Akimitsu,K.Kawashima,T.Muranaka		
90182	JPS0740851	Na and H2O contents measured by EPMA.	Nax(H2O)y(SnS)(TaS2)2	Na0.65H5Sn1.16S5.16Ta2O2.5	Na	0.65	H	5	Sn	1.16	S	5.16	Ta	2											O		2.5		2005																															A			23.78												K				4			4																																																																																																anhydrate samples were prepared by solid state reaction. hydration by topotactic reaction.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90183	JPS0740851	Na and H2O contents measured by EPMA.	Nax(H2O)y(PbS)(TaS2)2	Na0.4H3.6Pb1.14S5.14Ta2O1.8	Na	0.4	H	3.6	Pb	1.14	S	5.14	Ta	2											O		1.8		2005																															A			23.91												K				3.7			3.7																																																																																																anhydrate samples were prepared by solid state reaction. hydration by topotactic reaction.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90184	JPS0740851	Na and H2O contents measured by EPMA.	Nax(H2O)y(SbS)(TaS2)2	Na0.4H3.6Sb1.16S5.16Ta2O1.8	Na	0.4	H	3.6	Sb	1.16	S	5.16	Ta	2											O		1.8		2005																															A			23.26												K				3.5			3.5																																																																																																anhydrate samples were prepared by solid state reaction. hydration by topotactic reaction.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90185	JPS0740851	Na and H2O contents measured by EPMA.	Nax(H2O)y(BiS)(TaS2)2	Na0.4H5Bi1.08S5.08Ta2O2.5	Na	0.4	H	5	Bi	1.08	S	5.08	Ta	2											O		2.5		2005																															A			23.34												K					2																																																																																																		anhydrate samples were prepared by solid state reaction. hydration by topotactic reaction.					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90186	JPS0740851		(SnS)x(TaS2)2	Sn1.16S5.16Ta2	Sn	1.16	S	5.16	Ta	2																			2005																															A			17.75												K					2																																																																																																		solid state reaction					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90187	JPS0740851		(PbS)x(TaS2)2	Pb1.14S5.14Ta2	Pb	1.14	S	5.14	Ta	2																			2005																															A			17.97												K				3.3			3.3																																																																																																solid state reaction					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90188	JPS0740851		(SbS)x(TaS2)2	Sb1.16S5.16Ta2	Sb	1.16	S	5.16	Ta	2																			2005																															A			17.51												K				3			3																																																																																																solid state reaction					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90189	JPS0740851		(BiS)x(TaS2)2	Bi1.08S5.08Ta2	Bi	1.08	S	5.08	Ta	2																			2005																															A			17.48												K				2.7			2.7																																																																																																solid state reaction					Enhanced Superconducting Transition Temperature in the Water-intercalated Sulfides			Department of Advanced Materials Science, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 74(2005)851	F.Sakai,H.Takagi,M.Nohara,N.Katayama		
90190	JPS0740855	SC range for 9 < P < 16 GPa. Tc(max) = 0.62 K at P=12 GPa. Two Tc phases appear around P=12 GPA.	UGe2	Ge2U1	Ge	2	U	1																				3	2005																															A															K				0.62	0		0.62	MTC90190																																																																																															See Phys.Rev.B, 65(2002)020510.					Correlation between Superconductivity and Ferromagnetism in UGe2			Department of Physics, Graduate School of Science, Nagoya University, Nagoya, Japan	J.Phys.Soc.Jpn, 74(2005)855	G.Motoyama,H.Nakane,N.K.Sato,T.Nishioka		
90191	JPS0741014	Hc2(0) = 3.42 T from WHH theory.	Li2BPd3	Li2B1Pd3	Li	2	B	1	Pd	3																			2005																															A	6.7635														K				7.61			7.61											Oe		138.1							T	linear approx.	5.09														nm	from Hc2	9.89			nm	calculated from Hc1	190																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90192	JPS0741014	Hc2(0) = 2.91 T from WHH theory.	Li2B(Pd,Pt)3	Li2B1Pd2.7Pt0.3	Li	2	B	1	Pd	2.7	Pt	0.3																	2005																															A															K				6.59			6.59											Oe		120.6							T	linear approx.	4.56														nm	from Hc2	10.9			nm	calculated from Hc1	202.9																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90193	JPS0741014	Hc2(0) = 2.35 T from WHH theory.	Li2B(Pd,Pt)3	Li2B1Pd2.4Pt0.6	Li	2	B	1	Pd	2.4	Pt	0.6																	2005																															A	6.7544														K				4.9			4.9											Oe		104.1							T	linear approx.	4.08														nm	from Hc2	12.2			nm	calculated from Hc1	215.9																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90194	JPS0741014	Hc2(0) = 1.87 T from WHH theory.	Li2B(Pd,Pt)3	Li2B1Pd1.5Pt1.5	Li	2	B	1	Pd	1.5	Pt	1.5																	2005																															A	6.75														K				3.72			3.72											Oe		89.7							T	linear approx.	3.42														nm	from Hc2	13.6			nm	calculated from Hc1	230.4																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90195	JPS0741014	Hc2(0) = 1.34 T from WHH theory.	Li2B(Pd,Pt)3	Li2B1Pd0.9Pt2.1	Li	2	B	1	Pd	0.9	Pt	2.1																	2005																															A	6.7333														K				2.31			2.31											Oe		67.8							T	linear approx.	2.48														nm	from Hc2	16.1			nm	calculated from Hc1	246.4																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90196	JPS0741014	Hc2(0) = 1.06 T from WHH theory.	Li2BPt3	Li2B1Pt3	Li	2	B	1	Pt	3																			2005																															A	6.7294														K				1.86			1.86											Oe		38.4							T	linear approx.	1.82														nm	from Hc2	18			nm	calculated from Hc1	365.2																																																					Two step arc-melting method. second step = B(Pd1-xPtx)3 + Li					Superconductivity in a New Pseudo-Binary Li2B(Pd1-xPtx)3 (x = 0 - 1) Boride System			Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Japan	J.Phys.Soc.Jpn, 74(2005)1014	K.Togano,P.Badica,T.Kondo		
90197	JPS0741030	impurity phases = FeP2, FeP4 < 2%	SmFe4P12	Sm1Fe4P12	Sm	1	Fe	4	P	12																		1	2005								1.6																				skutterudite																		K					1.8																																																																																																		samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90198	JPS0741030		LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																		1	2005																												skutterudite																		K		4					4																																																								mj/mol.K2	52.4	SP-heat	671	SP-heat																																				samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90199	JPS0741030	impurity phases = RuP2, RuP4 < 2%. M-I transition at 16.5 K.	SmRu4P12	Sm1Ru4P12	Sm	1	Ru	4	P	12																		1	2005																												skutterudite																		K					1.8																																																																																																		samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90200	JPS0741030		LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																		1	2005																												skutterudite																		K		7					7																																																								mj/mol.K2	28.8	SP-heat	603	SP-heat																																				samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90201	JPS0741030	impurity phases = OsP2, OsP4 < 2%	SmOs4P12	Sm1Os4P12	Sm	1	Os	4	P	12																		1	2005								4.5																				skutterudite																		K					1.8																																																																																																		samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90202	JPS0741030		LaOs4P12	La1Os4P12	La	1	Os	4	P	12																		1	2005																												skutterudite																		K		1.8					1.8																																																								mj/mol.K2	20.3	SP-heat	482	SP-heat																																				samples were prepared at high-T and high-P.					Specific Heat Study on Sm-based Filled Skutterudite Phosphides SmT4P12 (T = Fe, Ru and Os)			Faculty of Engineering, Kyushu Institute of Technology, Kitakyushu, Japan	J.Phys.Soc.Jpn, 74(2005)1030	C.Sekine,H.Amitsuka,I.Shirotani,K.Matsuhira,M.Wakeshima,Ram Giri,Y.Doi,Y.Hinatsu,Y.Shimaya		
90203	JPS0741115	From 2nd to 1st phase transition change occurs at 0.7 K.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2005																																														K				2.25			2.25	MTC90203																			T			11.6	4.95										MHC90203																																																														using excess In flux.					Pressure Dependence of the First-Order Superconducting Phase Transition in CeCoIn5			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 74(2005)1115	H.Shishido,M.Hedo,R.Settai,T.Sakakibara,T.Tayama,Y.Namai,Y.Onuki,Y.Uwatoko		
90204	JPS0741255	impurity phase=Os(18.4%). lattice term const = 8.7 micro-J/mol.K6. Debye-T not given.	CsOs2O6	Cs1Os1O6	Cs	1	Os	1																	O	6		1	2005																												pyrochlore			A	10.1477														K		3.3					3.3																																																								mj/mol.K2	19.5	SP-heat																																						(Cs2O or Rb2O) + OsO2, solid state reaction(773-873 K, 24h)					Specific Heat of the beta-Pyrochlore Oxide Superconductors CsOs2O6 and RbOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 74(2005)1255	J.Yamaura,S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
90205	JPS0741255	impurity phase=Os(11.5%). lattice term const = 17.5 micro-J/mol.K6. Debye-T not given.	RbOs2O6	Rb1Os1O6	Rb	1	Os	1																	O	6		1	2005																												pyrochlore																		K		6.3					6.3																																																								mj/mol.K2	21.7	SP-heat																																						(Cs2O or Rb2O) + OsO2, solid state reaction(773-873 K, 24h)					Specific Heat of the beta-Pyrochlore Oxide Superconductors CsOs2O6 and RbOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba, Japan	J.Phys.Soc.Jpn, 74(2005)1255	J.Yamaura,S.Yonezawa,T.Muramatsu,Y.Muraoka,Z.Hiroi		
90206	JPS0741386		NbB2+x	B2Nb1	B	2	Nb	1																				1	2005																												AlB2																		K				4.44			4.44										44										kOe	resistive transition	6.4																																																																										powder(Nb,B), pellet sealed in qurtz tube, heat(1000C,30h)					Correlation between Superconducting Carrier Density and Transition Temperature in NbB2+x			Department of Physics, Aoyama Gakuin University, Sagamihara, Kanagawa, Japan	J.Phys.Soc.Jpn, 74(2005)1386	A.Koda,H.Takagiwa,J.Akimitsu,K.Ohishi,M.Yamazawa,R.Kadono,S.Kuroiwa,W.Higemoto		
90207	JPS0741386		NbB2+x	B2.03Nb1	B	2.03	Nb	1																				1	2005																												AlB2																		K				5.26			5.26										34										kOe	resistive transition	7.6																																																																										powder(Nb,B), pellet sealed in qurtz tube, heat(1000C,30h)					Correlation between Superconducting Carrier Density and Transition Temperature in NbB2+x			Department of Physics, Aoyama Gakuin University, Sagamihara, Kanagawa, Japan	J.Phys.Soc.Jpn, 74(2005)1386	A.Koda,H.Takagiwa,J.Akimitsu,K.Ohishi,M.Yamazawa,R.Kadono,S.Kuroiwa,W.Higemoto		
90208	JPS0741386	Penet value at 2 K.	NbB2+x	B2.1Nb1	B	2.1	Nb	1																				1	2005																												AlB2																		K				5.8			5.8										29										kOe	resistive transition	10.5																			A	muon-SR	2330																																																					powder(Nb,B), pellet sealed in qurtz tube, heat(1000C,30h)					Correlation between Superconducting Carrier Density and Transition Temperature in NbB2+x			Department of Physics, Aoyama Gakuin University, Sagamihara, Kanagawa, Japan	J.Phys.Soc.Jpn, 74(2005)1386	A.Koda,H.Takagiwa,J.Akimitsu,K.Ohishi,M.Yamazawa,R.Kadono,S.Kuroiwa,W.Higemoto		
90209	PR1220459	(dH0/dP) = -5.36E-4 G/psi, where H0=Hc at 0 K.	Pb	Pb1	Pb	1																							1961																																														K		7.175					7.175			K/GPa	-0.379																																																																																												99.999% purity. melt in graphite-coated glass tube. cool to RT(20C/h)					Pressure effect on superconducting lead			Department of Physics, University of Illinois,Urbana, Illinois,USA	Phys.Rev., 122(1961)459	D.E.Mapother,M.Garfinkel		
90210	PR1590353	Debye-T used in data-analysis.	Pb	Pb1	Pb	1																							1967																																														K		7.193					7.193			K/GPa	-0.386																																																							102																																										Will pressure destroy superconductivity			University of California, San Diego, California,USA	Phys.Rev., 159(1967)353	C.W.Chu,T.F.Smith		
90211	JPC0130L17	SC properties are at P=1.26 GPa, where Tc=0.7 K(max). gammma(P=1.13GPa) = 97 mj/mol.K2	UGe2	Ge2U1	Ge	2	U	1																					2001							52																								A	4.0089	15.0889	4.095												K		0.7			0		0.7																				T		1.9														A		130																			30																																												Pressure-induced superconductivity in a ferromagnet UGe2			Research Center for Materials Science at Extreme Conditions, Osaka University, Toyonaka, Osaka, Japan	J.Phys: Condens.Matter, 13(2001)L17	K.Amaya,K.Hanazono,N.Tateiwa,R.Settai,T.C.Kobayashi,Y.Haga,Y.Onuki		
90212	1022	carrier n=20.0 E+20/cc.carrier by Hall effect. G-L parameter = 6.1	SnTe	Sn1Te1	Sn	1	Te	1																				1	1969																												NaCl																		K		0.214					0.214											Oe		1.9							Oe		90							Oe/K		850			MHC90212																						erg/cc.K2	386	calculated from( dHc2/dT)																																		n/cm3	2000000000000000000000			Czochralski method.					Critical magnetic fields of superconducting SnTe				PHYS.REV.,179(1969)497	P.H.E.MEIJER,R.A.HEIN		
90213	1022	carrier n=16.9 E+20/cc. carrier by Hall effect. G-L parameter = 5.6	SnTe	Sn1Te1	Sn	1	Te	1																				1	1969																												NaCl																		K		0.174					0.174											Oe		1.2							Oe		60							Oe/K		800			MHC90213																						erg/cc.K2	406	calculated from( dHc2/dT)																																		n/cm3	1690000000000000000000			Czochralski method.					Critical magnetic fields of superconducting SnTe				PHYS.REV.,179(1969)497	P.H.E.MEIJER,R.A.HEIN		
90214	1022	carrier n=12.8 E+20/cc.  carrier by Hall effect. G-L parameter = 3.9	SnTe	Sn1Te1	Sn	1	Te	1																				1	1969																												NaCl																		K		0.104					0.104											Oe		0.7							Oe		22							Oe/K		405			MHC90214																						erg/cc.K2	214	calculated from( dHc2/dT)																																		n/cm3	1280000000000000000000			Czochralski method.					Critical magnetic fields of superconducting SnTe				PHYS.REV.,179(1969)497	P.H.E.MEIJER,R.A.HEIN		
90215	1022	carrier n=10.5 E+20/cc.  carrier by Hall effect. G-L parameter = 4.4	SnTe	Sn1Te1	Sn	1	Te	1																				1	1969																												NaCl																		K		0.068					0.068											Oe		0.5							Oe		13							Oe/K		420			MHC90215																						erg/cc.K2	181	calculated from( dHc2/dT)																																		n/cm3	1050000000000000000000			Czochralski method.					Critical magnetic fields of superconducting SnTe				PHYS.REV.,179(1969)497	P.H.E.MEIJER,R.A.HEIN		
90216	1022	carrier n=7.5 E+20/cc.  carrier by Hall effect. Single phase for 0< x =< 0.04 in Sn1-xTex	SnTe	Sn1Te1	Sn	1	Te	1																				1	1969																												NaCl																		K		0.034					0.034																						5																																																																						n/cm3	750000000000000000000			Czochralski method.					Critical magnetic fields of superconducting SnTe				PHYS.REV.,179(1969)497	P.H.E.MEIJER,R.A.HEIN		
90217	1292	(1/3) of La-sites are vacant	La3Se4	La3Se4	La	3	Se	4																				1	1968																												Th3P4	I4<->3d		A	9.049														K		10					10	MTC90217																																																																																													3N-La, 5N-Se,		direct reaction (powder) at 50C below the melting temp.					Superconductivity in the lanthanum selenide system				PHYS.REV.,168(1968)408	F.HOLTZBERG,P.E.SEIDEN,S.VON MOLNER		
90218	470	carrier n=1.71 E+22/cc	InTe	In1Te1	In	1	Te	1																					1964																												NaCl			A	6.18														K		3.2					3.2																																																																																																					Superconductivity of intermetallic compounds with NaCl-type and related structures				PHYS.REV.LETT.,13(1964)127	G.W.HULL,S.GELLER		
90219	470	carrier n=0.56 E+22/cc	Sn4As3	As3Sn4	As	3	Sn	4																					1964																																														K		1.16					1.16																																																																																																					Superconductivity of intermetallic compounds with NaCl-type and related structures				PHYS.REV.LETT.,13(1964)127	G.W.HULL,S.GELLER		
90220	470	carrier n=0.47 E+22/cc	In3Te4	In3Te4	In	3	Te	4																					1964																																														K		1.15					1.15																																																																																																					Superconductivity of intermetallic compounds with NaCl-type and related structures				PHYS.REV.LETT.,13(1964)127	G.W.HULL,S.GELLER		
90221	470	carrier n=1.06 E+22/cc	Ge3Te4	Ge3Te4	Ge	3	Te	4																					1964																																														K		1.55					1.55																																																																																																					Superconductivity of intermetallic compounds with NaCl-type and related structures				PHYS.REV.LETT.,13(1964)127	G.W.HULL,S.GELLER		
90222	611	carrier from Hall coefficient	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		1	1966																																														K		0.3					0.3											Oe		2.75																																																																															E+19/cc	6.4			press and sintering(1650C)					Superconductivity in ceramic, mixed titanates 				PHYS.REV.LETT.,16(1966)579	E.PREIFFER,H.P.R.FREDERIKSE,J.F.SCHOOLEY,W.E.THURBER,W.R.HOSLER		
90223	611	carrier from Hall coefficient	(Sr,Ba)TiO3	Sr0.95Ba0.05Ti1O3	Sr	0.95	Ba	0.05	Ti	1															O	3		1	1966																																														K		0.55					0.55											Oe		3.9																																																																															E+19/cc	6.7			press and sintering(1650C)					Superconductivity in ceramic, mixed titanates 				PHYS.REV.LETT.,16(1966)579	E.PREIFFER,H.P.R.FREDERIKSE,J.F.SCHOOLEY,W.E.THURBER,W.R.HOSLER		
90224	611	carrier from Hall coefficient	(Sr,Ca)TiO3	Sr0.925Ca0.075Ti1O3	Sr	0.925	Ca	0.075	Ti	1															O	3		1	1966																																														K		0.5					0.5											Oe		3.8																																																																															E+19/cc	8.7			press and sintering(1650C)					Superconductivity in ceramic, mixed titanates 				PHYS.REV.LETT.,16(1966)579	E.PREIFFER,H.P.R.FREDERIKSE,J.F.SCHOOLEY,W.E.THURBER,W.R.HOSLER		
90225	611	carrier from Hall coefficient	(Sr,Ca)TiO3	Sr0.7Ca0.3Ti1O3	Sr	0.7	Ca	0.3	Ti	1															O	3		1	1966																																														K		0.55					0.55											Oe		2.15																																																																															E+19/cc	6.7			press and sintering(1650C)					Superconductivity in ceramic, mixed titanates 				PHYS.REV.LETT.,16(1966)579	E.PREIFFER,H.P.R.FREDERIKSE,J.F.SCHOOLEY,W.E.THURBER,W.R.HOSLER		
90226	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.03Sn0.97Te1.01	In	0.03	Sn	0.97	Te	1.01																			1974																																														K		1.07					1.07																																																																																												E+21/cc	3.47			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90227	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.04Sn0.96Te1.01	In	0.04	Sn	0.96	Te	1.01																			1974																																														K		1.14					1.14																																																																																												E+21/cc	6.1			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90228	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.045Sn0.955Te1.01	In	0.045	Sn	0.955	Te	1.01																			1974																																														K		1.2					1.2																																																																																												E+21/cc	7.33			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90229	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.05Sn0.95Te1.01	In	0.05	Sn	0.95	Te	1.01																			1974																																														K		1.43					1.43																																																																																												E+21/cc	9.28			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90230	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.06Sn0.94Te1.01	In	0.06	Sn	0.94	Te	1.01																			1974																																														K		1.36					1.36																																																																																												E+21/cc	10.9			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90231	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.08Sn0.92Te1.01	In	0.08	Sn	0.92	Te	1.01																			1974																																														K		1.45					1.45																																																																																												E+21/cc	17			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90232	1857	carrier from Hall coefficient	(In,Sn)Te1.01	In0.1Sn0.9Te1.01	In	0.1	Sn	0.9	Te	1.01																			1974																																														K		1.75					1.75																																																																																												E+21/cc	30			ANN(580C,1w)					Carrier density dependences of the superconducting transitions in n-type InxSn1-xTe1+y				J.PHYS.SOC.JAPAN,36(1974)1705	E.KANDA,H.MIYAUCHI,T.NAKAJIMA		
90233	PHC4200083	(dlnTc/P) = -0.030 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		38.7					38.7	MTC90233		K/GPa	-1.17																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90234	PHC4200083	(dlnTc/P) = -0.027 /GPa	Mg(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																			2005																												AlB2																		K		35.5					35.5	MTC90234		K/GPa	-0.966																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90235	PHC4200083	(dlnTc/P) = -0.036 /GPa	Mg(B,C)2	Mg1B1.85C0.15	Mg	1	B	1.85	C	0.15																			2005																												AlB2																		K		27.2					27.2	MTC90235		K/GPa	-0.974																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90236	PHC4200083	(dlnTc/P) = -0.031 /GPa	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2005																												AlB2																		K		21.5					21.5	MTC90235		K/GPa	-0.664																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90237	PHC4200083	(dlnTc/P) = -0.051 /GPa	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2005																												AlB2																		K		22.9					22.9	MTC90237		K/GPa	-1.18																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90238	PHC4200083	neutron irradiated sample(fluence=1 E+19 n/cm2), then ANN(400C,24h). (dlnTc/dP) = -0.038 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		30.4					30.4	MTC90238		K/GPa	-1.15																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90239	PHC4200083	neutron irradiated sample(fluence=1 E+19 n/cm2), then ANN(300C,24h). (dlnTc/dP) = -0.044 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		22.8					22.8	MTC90238		K/GPa	-1.01																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90240	PHC4200083	neutron irradiated sample(fluence=1 E+19 n/cm2), then ANN(250C,24h). (dlnTc/dP) = -0.045 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		17.1					17.1	MTC90240		K/GPa	-0.759																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90241	PHC4200083	neutron irradiated sample(fluence=1 E+19 n/cm2), then ANN(200C,24h). (dlnTc/dP) = -0.039 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		13.6					13.6	MTC90240		K/GPa	-0.526																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90242	PHC4200083	neutron irradiated sample(fluence=1 E+19 n/cm2), then ANN(150C,24h). (dlnTc/dP) = -0.043 /GPa	MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2																		K		8.13					8.13	MTC90240		K/GPa	-0.345																																																																																																	Effect of pressure on the superconducting transition temperature of doped and neutron-damaged MgB2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Physica C, 420(2005)83	M.Angst,P.C.Canfield,R.H.T.Wilke,S.L.Bud'ko		
90243	P071174506	Al-content by EDX.	(Mg,Al)B2	Mg0.978Al0.022B2	Mg	0.978	Al	0.022	B	2																		3	2005									2.65																			AlB2	P6/mmm		A	3.0819		3.499												K				34.7			34.7																																																																																																melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90244	P071174506	Al-content by EDX.	(Mg,Al)B2	Mg0.956Al0.044B2	Mg	0.956	Al	0.044	B	2																		3	2005									2.654																			AlB2	P6/mmm		A	3.082		3.494												K				34			34																																																																																																melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90245	P071174506	Al-content by EDX.	(Mg,Al)B2	Mg0.915Al0.085B2	Mg	0.915	Al	0.085	B	2																		3	2005									2.664																			AlB2	P6/mmm		A	3.079		3.488												K				32.4			32.4	MTC90245																																																																																															melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90246	P071174506	Al-content by EDX. Two phases: phase-I (a=3.082, c=3.459), phase-II(a=3.047, c=6.724)	(Mg,Al)B2	Mg0.815Al0.185B2	Mg	0.815	Al	0.185	B	2																		3	2005									2.746																			AlB2	P6/mmm		A	3.062		3.42												K				25.3			25.3																																																																																																melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90247	P071174506	gap by point contact tunneling. two gaps(delta = 7.1 and 2.80 meV). DB-value shows higher ones.	MgB2	B2Mg1	B	2	Mg	1																				3	2005																												AlB2																		K				38.2			38.2																																		MHC90247												meV	7.1	4.32	1																																															melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90248	P071174506	gap by point contact tunneling. two gaps(delta = 4.30 and 2.30 meV). DB-value shows higher ones.	(Mg,Al)B2	Mg0.815Al0.09B2	Mg	0.815	Al	0.09	B	2																		3	2005																												AlB2																		K				32.7			32.7																																														meV	4.3	3.05	1																																															melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90249	P071174506	gap by point contact tunneling. two gaps(delta = 4.0 and 0.75 meV). DB-value shows higher ones.	(Mg,Al)B2	Mg0.815Al0.18B2	Mg	0.815	Al	0.18	B	2																		3	2005																												AlB2																		K				25.7			25.7																																														meV	4	3.62	1																																															melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90250	P071174506		(Mg,Al)B2	Mg0.815Al0.024B2	Mg	0.815	Al	0.024	B	2																		3	2005																												AlB2																		K				35			35																																		MHC90250																																																														melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90251	P071174506		(Mg,Al)B2	Mg0.815Al0.092B2	Mg	0.815	Al	0.092	B	2																		3	2005																												AlB2																		K				32			32																																		MHC90251																																																														melt(Mg+B,Al) above 20 kbar, crystal growth (1800C, or 1960C) high pressure synthesis					Al substitution in MgB2 crystals: Influence on superconducting and structural properties			Laboratory for Solid State Physics, ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)174506	B.Batlogg,D.Daghero,E.Muller,G.A.Ummarino,G.Schuck,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,P.Wagli,R.Gonnelli,R.Puzniak,S.M.Kazakov,V.A.Stepanov		
90252	P071220505	Tc(H=1.46 K) = 5.7 K. B[11] NMR measured.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2005																																														K				7.1			7.1																																																2.2	6																																													Li(3N),Pd(3N),B(2N)		two step arc-melting. nominal: Li:Pd:B = 2.1:3:1					Superconductivity of the ternary boride Li2Pd3B probed by [11]B NMR			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 71(2005)220505	Guo-qing Zheng,M.Nishiyama,Y.Inada		
90253	L094247006	RRR=21. Hc2(0)//a=2.03T, Hc2//b = 1.28T, Hc2//c = 0.55T. Tc=0.257K for RRR=34 and Tc=0.274K for RRR=152 sample.	URhGe	U1Rh1Ge1	U	1	Rh	1	Ge	1																		3	2005																												TiNiSi																		K	0.205	0.222	0.238				0.222																				T			2.03	0.55										MHC90253																																																														Czochralski method. ANN(1300C,24h) - etching - ANN(880C,18d)					p-Wave Superconductivity in the Ferromagnetic Superconductor URhGe			DRFMC/SPSMS, CEA-Grenoble, Grenoble 38054, France	Phys.Rev.Lett., 94(2005)247006	A.D.Huxley,F.Hardy		
90254	PHC4220065	FM transition at 300K. Soft and weak FM. not SC. Structure type=CaTiO3(perovskite)	AlCNi3	Al1C1Ni3	Al	1	C	1	Ni	3																			2005							300																					ABO3	Pm-3m		A	3.587														K					4																																																																																																Al,C,Ni powder		mixture - pellet - wrapped in Ta-foil - sealed quartz tube - heat(700C,30h + 980C,40h) - cool to RT(150C/h)					Synthesis and physical properties of AlCNi3			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Physica C, 422(2005)65	A.F.Dong,G.C.Che,H.Chen,S.L.Jia,W.W.Huang,Z.X.Zhao		
90255	P071174511	Hc1 criterion: dM=7.0E-4 emu. cylinderical sample. 	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2005																												ABO3																		K				6.9			6.9											Oe	M-H curve	145.1							T	SP-heat	11.8														A	from Hc2(0)	53			A	calculated from Hc1 and G-L	2001																																																					powder metallurgy method					Evidence for s-wave pairing from measurement of the lower critical field in MgCNi3			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing , China	Phys.Rev.B, 71(2005)174511	G.C.Che,H.Gao,H.H.Wen,L.Shan,X.F.Lu,Z.A.Ren,Z.Wang		
90256	P071184512	nominal compo: x=0 in MgC1.5-xBxNi3.	MgCNi3	Mg1C0.925Ni3	Mg	1	C	0.925	Ni	3																			2005																												ABO3			A	3.811														K				7.09			7.09																																																																																																using 99.5 at%[11]B-isotope. wrapped in Zr-foil, fired(600C,0.5h + 900C,1h) under (95Ar-5H2)-gas.					Effect of [11]B substitution on the superconductivity of MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 71(2005)184512	J.D.Jorgensen,M.Avdeev,R.J.Cava,T.Klimczuk		
90257	P071184512	nominal compo: x=0.05 in MgC1.5-xBxNi3.	Mg(C,B)Ni3	Mg1C0.885B0.04Ni3	Mg	1	C	0.885	B	0.04	Ni	3																	2005																												ABO3			A	3.8124														K				6.97			6.97																																																																																																using 99.5 at%[11]B-isotope. wrapped in Zr-foil, fired(600C,0.5h + 900C,1h) under (95Ar-5H2)-gas.					Effect of [11]B substitution on the superconductivity of MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 71(2005)184512	J.D.Jorgensen,M.Avdeev,R.J.Cava,T.Klimczuk		
90258	P071184512	nominal compo: x=0.10 in MgC1.5-xBxNi3.	Mg(C,B)Ni3	Mg1C0.853B0.072Ni3	Mg	1	C	0.853	B	0.072	Ni	3																	2005																												ABO3			A	3.8146														K				6.76			6.76																																																																																																using 99.5 at%[11]B-isotope. wrapped in Zr-foil, fired(600C,0.5h + 900C,1h) under (95Ar-5H2)-gas.					Effect of [11]B substitution on the superconductivity of MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 71(2005)184512	J.D.Jorgensen,M.Avdeev,R.J.Cava,T.Klimczuk		
90259	P071184512	nominal compo: x=0.151 in MgC1.5-xBxNi3.	Mg(C,B)Ni3	Mg1C0.814B0.111Ni3	Mg	1	C	0.814	B	0.111	Ni	3																	2005																												ABO3			A	3.8168														K				6.88			6.88																																																																																																using 99.5 at%[11]B-isotope. wrapped in Zr-foil, fired(600C,0.5h + 900C,1h) under (95Ar-5H2)-gas.					Effect of [11]B substitution on the superconductivity of MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 71(2005)184512	J.D.Jorgensen,M.Avdeev,R.J.Cava,T.Klimczuk		
90260	P071184512	nominal compo: x=0.2 in MgC1.5-xBxNi3. solubility limit:x=0.16 measured by NPD.	Mg(C,B)Ni3	Mg1C0.771B0.154Ni3	Mg	1	C	0.771	B	0.154	Ni	3																	2005																												ABO3			A	3.8197														K				6.44			6.44																																																																																																using 99.5 at%[11]B-isotope. wrapped in Zr-foil, fired(600C,0.5h + 900C,1h) under (95Ar-5H2)-gas.					Effect of [11]B substitution on the superconductivity of MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 71(2005)184512	J.D.Jorgensen,M.Avdeev,R.J.Cava,T.Klimczuk		
90261	PHB3590035	resistivity(max) at T=46 K. Sp-heat measured for 0.3 < T= < 4 K.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2005																																														K		2.26					2.26																																																																																																In-flux method					Rapid suppression of superconductivity in CeCoIn5-xSnx			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Physica B, 359-361(2005)35	D.J.Mixson,E.D.Bauer,J.D.Thompson,J.L.Sarrao,M.F.Hundley,N.O.Moreno,P.G.Pagliuso,R.Movshovich		
90262	PHB3590035	dTc/dx = -0.6 K/at%Sn. resistivity(max) at T=47.5 K. Sp-heat measured for 0.3 < T= < 4 K.	CeCo(In,Sn)5	Ce1Co1In4.94Sn0.06	Ce	1	Co	1	In	4.94	Sn	0.06																3	2005																																														K		1.56					1.56	MTC90262																																																																																															In-flux method					Rapid suppression of superconductivity in CeCoIn5-xSnx			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Physica B, 359-361(2005)35	D.J.Mixson,E.D.Bauer,J.D.Thompson,J.L.Sarrao,M.F.Hundley,N.O.Moreno,P.G.Pagliuso,R.Movshovich		
90263	P072014534	2H-TaS2. anisotropy = 6.4.	NaxTaS2	Na0.1Ta1S2	Na	0.1	Ta	1	S	2																		3	2005																												2H-TaS2	P6[-]m2		A			12.082												K	4.3		4.83	4.4		0.5	4.4																				T			16	2.5					T/K	resistivity		4.5	0.7163	MHC90263																																																												NaCl,Ta,S		mixture - pellet - quartz tube - heat(920C,48C) - cool to 700C(1-2 C/h) - FC to RT					Fabrication and superconductivity of NaxTaS2 crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China	Phys.Rev.B, 72(2005)014534	C.Dong,H.Chen,H.H.Wen,L.Fang,L.Shan,L.Tang,P.Y.Zou,Y.Wang,Z.Xu		
90264	P072014534	2H-TaS2. anisotropy(resistivity)= 63.6 at 10K, and = 5.3 at 300 K.	NaxTaS2	Na0.05Ta1S2	Na	0.05	Ta	1	S	2																		3	2005																												2H-TaS2	P6[-]m2																	K				4			4																																																																																														NaCl,Ta,S		mixture - pellet - quartz tube - heat(920C,48C) - cool to 700C(1-2 C/h) - FC to RT					Fabrication and superconductivity of NaxTaS2 crystals			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China	Phys.Rev.B, 72(2005)014534	C.Dong,H.Chen,H.H.Wen,L.Fang,L.Shan,L.Tang,P.Y.Zou,Y.Wang,Z.Xu		
90265	P072024521	single crystal. H-direction not described	Rb3C60	C60Rb3	C	60	Rb	3																				3	2005																												fullerene																		K				30.9			30.9											mT	trapped magnetization	0.91							T	WHH theory and dHc2/dT	93							T/K		4.4					nm		1.9			nm	calculated from Hc1	1100																																																					vapor phase doping method					Mixed state parameters of single crystalline Rb3C60 fullerene superconductors			Atominstitut der Osterreichischen Universitaten, Stadionallee 2, 1020 Vienna, Austria	Phys.Rev.B, 72(2005)024521	F.M.Sauerzopf,H.Kuzmany,H.W.Weber,M.Halushka,V.Buntar		
90266	P072020501	Hc2 defined as 0.8Rn. Hc2(0)//ab = 18.4 T from (dHc2/dT) and WHH theory. anisotropy = 4.5 by Hc2.	ZrNClx	Zr1N1Cl0.7	Zr	1	N	1	Cl	0.7																		3	2005																																														K			12.8				12.8																				T			27						T/K			2.21	0.49	MHC90266		A			71	16																																																								powder sample - pressed into pellet to orient ZrN plane under 150 MPa in Ar.					Upper critical field in the electron-doped layered superconductor ZrNCl0.7: Magnetoresistance studies			Department of Quantum Matter, AdSM, Hiroshima University, Higashi-Hiroshima, 739-8530, Japan	Phys.Rev.B, 72(2005)020501	H.Tou,L.Zhu,M.Sera,S.Yamanaka,T.Sasaki,Y.Iwasa,Y.J.Tanaka,Y.Taguchi		
90267	P072024547	RRR=9.33. gamma=0.34mJ/gat.K2. (dC/gamma*Tc) = 1.66. Hc(0) = 41.5 mT.	ZrB12	B12Zr1	B	12	Zr	1																				3	2005									3.63																			UB12																		K		5.97		6		0.025	5.97																																																3.7	14				MSP90267	mJ/mol.K	44.02	mJ/mol.K2	4.42	SP-heat	970	SP-heat											uOhm.cm							1.925				17.95														zone melting					Specific heat, magnetic susceptibility, resistivity and thermal expansion of the superconductor ZrB12			Department of Condensed Matter Physics, University of Geneva, CH-1211 Geneva 4 (Switzerland)	Phys.Rev.B, 72(2005)024547	A.Junod,C.Meingast,R.Lortz,S.Abe,V.Filippov,Y.Wang,Yu.B.Paderno		
90268	P072024551		Ce(Rh,Co)In5	Ce1Rh0.9Co0.1In5	Ce	1	Rh	0.9	Co	0.1	In	5																3	2005																												HoCoGa5																		K								MTC90268																																																																																															molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90269	P072024551		Ce(Rh,Co)In5	Ce1Rh0.8Co0.2In5	Ce	1	Rh	0.8	Co	0.2	In	5																3	2005								3.7																				HoCoGa5																		K								MTC90269																																																							mJ/mol.K2	340	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90270	P072024551	(dC/gamma*Tc) = 0.7	Ce(Rh,Co)In5	Ce1Rh0.6Co0.4In5	Ce	1	Rh	0.6	Co	0.4	In	5																3	2005								3.6																				HoCoGa5																		K		1.5					1.5	MTC90270																																																					mJ/mol.K	340	mJ/mol.K2	320	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90271	P072024551	(dC/gamma*Tc) = 1.8	Ce(Rh,Co)In5	Ce1Rh0.4Co0.6In5	Ce	1	Rh	0.4	Co	0.6	In	5																3	2005								2.9																				HoCoGa5																		K		1.43					1.43	MTC90271																																																					mJ/mol.K	1560	mJ/mol.K2	620	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90272	P072024551	(dC/gamma*Tc) = 0.9	Ce(Rh,Co)In5	Ce1Rh0.35Co0.65In5	Ce	1	Rh	0.35	Co	0.65	In	5																3	2005								2.4																				HoCoGa5																		K		1.38					1.38																																																						mJ/mol.K	930	mJ/mol.K2	730	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90273	P072024551	(dC/gamma*Tc) = 0.4	Ce(Rh,Co)In5	Ce1Rh0.29Co0.71In5	Ce	1	Rh	0.29	Co	0.71	In	5																3	2005								2.1																				HoCoGa5																		K		1.56					1.56																																																						mJ/mol.K	820	mJ/mol.K2	830	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90274	P072024551	(dC/gamma*Tc) = 0.8	Ce(Rh,Co)In5	Ce1Rh0.23Co0.77In5	Ce	1	Rh	0.23	Co	0.77	In	5																3	2005																												HoCoGa5																		K		1.38					1.38																																																						mJ/mol.K	1210	mJ/mol.K2	780	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90275	P072024551	(dC/gamma*Tc) = 0.5	Ce(Rh,Co)In5	Ce1Rh0.13Co0.87In5	Ce	1	Rh	0.13	Co	0.87	In	5																3	2005																												HoCoGa5																		K		1.73					1.73																																																						mJ/mol.K	1030	mJ/mol.K2	620	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90276	P072024551	(dC/gamma*Tc) = 0.5	Ce(Rh,Co)In5	Ce1Rh0.07Co0.93In5	Ce	1	Rh	0.07	Co	0.93	In	5																3	2005																												HoCoGa5																		K		1.89					1.89																																																						mJ/mol.K	1090	mJ/mol.K2	560	SP-heat																																						molten In-flux method in alumina crucible.					Superconductivity and non-Fermi liquid behavior near antiferromagnetic quantum critical points in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California?San Diego, La Jolla, California, USA	Phys.Rev.B, 72(2005)024551	E.D.Bauer,H.Kimura,J.R.Jeffries,K.-D.Hof,M.B.Maple,N.A.Frederick,T.A.Sayles,V.S.Zapf		
90277	JPS0741698	anisotropy=3.9 from Hc2. Maki-parameter k2=50 for H//[100]. thermodynamic Hc(0)=4.7 kOe. kaizero = 4.5E-4 emu/mol for H//[001]. p-direction=H//[100]	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2005	emu/mol	0.00043			uB/Pu	0.85																						HoCoGa5			A			6.84												K				8.6			8.6																				T			27	15					T/K			3.5	2																																																															Ga-flux method. 94% enriched Pu[239]:Rh:Ga = 1:1:20, heat(1100C,2h,in alumina crucible) - slow cool to RT.					Single Crystal Growth and Anisotropic Superconducting Property of PuRhGa5			Advanced Science Research Center, Japan Atomic Energy Research Institute, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 74(2005)1698	A.Nakamura,D.Aoki,E.Yamamoto,K.Nakajima,T.Matsuda,Y.Arai,Y.Haga,Y.Homma,Y.Onuki,Y.Shiokawa		
90278	JPS0741782	P-induced SC. Pcrit = 0.8 GPa(lower SC) and 1.8 GPa(upper SC). CDW-temp = 58 K(chain I) and 142 K(chain III). (dTc/dP) for 4 < P < 5.7 GPa	NbSe3	Nb1Se3	Nb	1	Se	3																				3	2005																																														K		5			0		5	MTC90278		K/GPa	-0.45																																																																																												vapor transport. (Nb wire and Se) in sealed quartz tube at 1030 K(with t-gradient of 1 K/cm)					Coexistence of the Upper Charge-Density-Wave and the Superconductivity in NbSe3			Department of Molecular Materials Science, Graduate School of Science, Osaka City University, Sumiyoshi-ku, Osaka, Japan	J.Phys.Soc.Jpn, 74(2005)1782	K.Murata,K.Yamaya,M.Shimotori,S.Yasuzuka,T.Fujimoto		
90279	JPS0591341	P-induced SC. Pcrit = 7.5 kbar. (dTc/dP) at Pcrit is estimated from Tc(P). CDW-temp = 58 K(chain I) and 142 K(chain III).	NbSe3	Nb1Se3	Nb	1	Se	3																				3	1990																																														K		3.71			0		3.71	MTC90279		K/GPa	-1.77																																																																																												not described					Pressure effect on the charge-density waves and the superconductivity in NbSe3			Department of Physics,Facalty of Science, Hokkaido University, Sapporo, Japan	J.Phys.Soc.Jpn, 59(1990)1341	M.Ido,T.Ijiri,Y.Okajima,Y.Okayama		
90280	PCS0650333	slow cool to 973 K.	BaxSi46	Ba7.76Si46	Ba	7.76	Si	46																				1	2004																												clathrate			A	10.314														K				9			9																																																																																														Si,BaSi2		nominal BaSi2:Si=8:30. high pressure synthesis(1573K, P=3GPa)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
90281	PCS0650333	slow cool to 1073 K.	BaxSi46	Ba7.61Si46	Ba	7.61	Si	46																				1	2004																												clathrate			A	10.331														K				8.2			8.2																																																																																														Si,BaSi2		nominal BaSi2:Si=8:30. high pressure synthesis(1573K, P=3GPa)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
90282	PCS0650333	slow cool to 973 K. then ANN(800K,24h)	BaxSi46	Ba6.63Si46	Ba	6.63	Si	46																				1	2004																												clathrate			A	10.262														K				6			6																																																																																														Si,BaSi2		nominal BaSi2:Si=8:30. high pressure synthesis(1573K, P=3GPa)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
90283	PCS0650333	ANN(800K,24h)	BaxSi46	Ba6.62Si46	Ba	6.62	Si	46																				1	2004																												clathrate			A	10.288														K				5			5																																																																																														Si,BaSi2		nominal BaSi2:Si=8:30. high pressure synthesis(1273K, P=3GPa) - slow cool to 973 K.					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
90284	IOC0422933	TCFIG shows Tc vs x for NaxBa6Si46 and BaxBa6Si46.	BaxSi46	Ba7.76Si46	Ba	7.76	Si	46																				1	2003																												clathrate		223	A	10.3141																		9			9	MTC90284																																																																																													Si,BaSi2		nominal BaSi2:Si=8:30. high pressure synthesis(1573K, P=3GPa)					Superconductivity of Metal Deficient Silicon Clathrate Compounds, Ba8-xSi46 (0 <x =< 1.4)			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima 739-8527, Japan	Inorg. Chem., 42(2003)2933	H.Fukuoka,J.Kiyoto,S.Yamanaka		
90285	JPS0410026		CeRu2	Ce1Ru2	Ce	1	Ru	2																				1	1976																												Laves																	Laves, C15	K		6.2					6.2																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
90286	JPS0410026		(Ce,Pr)Ru2	Ce0.9Pr0.1Ru2	Ce	0.9	Pr	0.1	Ru	2																		1	1976																												Laves																	Laves, C15	K		6.55					6.55																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
90287	JPS0410026		(Ce,Pr)Ru2	Ce0.8Pr0.2Ru2	Ce	0.8	Pr	0.2	Ru	2																		1	1976																												Laves																	Laves, C15	K		5.82					5.82																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
90288	JPS0410026		(Ce,Pr)Ru2	Ce0.7Pr0.3Ru2	Ce	0.7	Pr	0.3	Ru	2																		1	1976																												Laves																	Laves, C15	K		5.11					5.11	MPH90288																																																																																																				Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
90289	JPS0410026		(Ce,Pr)Ru2	Ce0.65Pr0.35Ru2	Ce	0.65	Pr	0.35	Ru	2																		1	1976																												Laves																	Laves, C15	K		1.25	3.55				1.25																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
90290	JPS0271463	ANN(900C,10d in sealed quartz). dC=10.97mj/K. (dC/gamma*Tc) = 0.71.	LaGex	Ge2La1	Ge	2	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		2.24					2.24																																																					MSP90290																																																The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90291	JPS0271463	dC=9.73mj/K. (dC/gamma*Tc) = 0.76.	LaGex	Ge1.9La1	Ge	1.9	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		2.17					2.17																																																																																																					The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90292	JPS0271463	two step transition, lower Tc = 1.91 K. dC=8.95mj/K. (dC/gamma*Tc) = 0.66.	LaGex	Ge1.85La1	Ge	1.85	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		2.17					2.17																																																																																																					The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90293	JPS0271463	two step transition, lower Tc = 1.87 K.	LaGex	Ge1.83La1	Ge	1.83	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		2.17					2.17																																																																																																					The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90294	JPS0271463	two step transition, lower Tc = 1.83 K.	LaGex	Ge1.81La1	Ge	1.81	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		2.17					2.17																																																					MSP90294																																																The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90295	JPS0271463	two step transition, lower Tc = 1.70 K.	LaGex	Ge1.8La1	Ge	1.8	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		1.87					1.87																																																																																																					The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90296	JPS0271463	dC=7.03mj/K. (dC/gamma*Tc) = 1.28.	LaGex	Ge1.78La1	Ge	1.78	La	1																				1	1969																												alpha-ThSi2																	alpha-ThSi2, C[c]	K		1.57					1.57																																																					MSP90296																																																The specific heat and superconductivity of La-Ge system				J.Phys.Soc.Jpn, 27(1969)1463	T.Satoh,Y.Asada		
90297	PHC4240025	RRR=2.6	YGe3	Ge3Y1	Ge	3	Y	1																				1	2005																												DyGe3	Cmcm		A	4.0497	20.801	3.9147											DyGe3,	K	2.2	2.35	2.7	2.1			2.35											Oe					10			1.9	T					0.025			1.9																																																																									Superconductivity in YGe3			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 424(2005)25	M.S.Wei,H.H.Sung,W.H.Lee		
90298	PHC4240079		MgB2	B2Mg1	B	2	Mg	1																					2005																												AlB2			A	3.0849		3.5241											AlB2, C32	K		38.2					38.2																																																																																														Mg,B,Cr		solid state reaction. mixture - pellet - wrapped in Ta-foil - quartz tube(Ar) - heat(950C,10h) - cool to RT					The charge transfer induced by Cr doping in MgB2			Structure Research Laboratory and Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui, China	Physica C, 424(2005)79	H.Zhang,J.Zhao,L.Shi		
90299	PHC4240079	impurity phase: MgO	(Mg,Cr)B2	Mg0.99Cr0.01B2	Mg	0.99	Cr	0.01	B	2																			2005																												AlB2			A	3.0841		3.5236											AlB2, C32	K		36.7					36.7																																																																																														Mg,B,Cr		solid state reaction. mixture - pellet - wrapped in Ta-foil - quartz tube(Ar) - heat(950C,10h) - cool to RT					The charge transfer induced by Cr doping in MgB2			Structure Research Laboratory and Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui, China	Physica C, 424(2005)79	H.Zhang,J.Zhao,L.Shi		
90300	PHC4240079	impurity phase: MgO	(Mg,Cr)B2	Mg0.98Cr0.02B2	Mg	0.98	Cr	0.02	B	2																			2005																												AlB2			A	3.0867		3.5234											AlB2, C32	K		35.3					35.3																																																																																														Mg,B,Cr		solid state reaction. mixture - pellet - wrapped in Ta-foil - quartz tube(Ar) - heat(950C,10h) - cool to RT					The charge transfer induced by Cr doping in MgB2			Structure Research Laboratory and Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui, China	Physica C, 424(2005)79	H.Zhang,J.Zhao,L.Shi		
90301	PHC4240079	impurity phase: MgO	(Mg,Cr)B2	Mg0.97Cr0.03B2	Mg	0.97	Cr	0.03	B	2																			2005																												AlB2			A	3.0854		3.5221											AlB2, C32	K		35.1					35.1																																																																																														Mg,B,Cr		solid state reaction. mixture - pellet - wrapped in Ta-foil - quartz tube(Ar) - heat(950C,10h) - cool to RT					The charge transfer induced by Cr doping in MgB2			Structure Research Laboratory and Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui, China	Physica C, 424(2005)79	H.Zhang,J.Zhao,L.Shi		
90302	PHC4240079	impurity phase: MgO, CrB, CrB2	(Mg,Cr)B2	Mg0.95Cr0.05B2	Mg	0.95	Cr	0.05	B	2																			2005																												AlB2			A	3.0848		3.52											AlB2, C32																																																																																																						Mg,B,Cr		solid state reaction. mixture - pellet - wrapped in Ta-foil - quartz tube(Ar) - heat(950C,10h) - cool to RT					The charge transfer induced by Cr doping in MgB2			Structure Research Laboratory and Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui, China	Physica C, 424(2005)79	H.Zhang,J.Zhao,L.Shi		
90303	P072054516	(dTc/dx) = -12 K. Tc = 6.24 - 12x in Dy1-xTbxNi2B2C	(Dy,Tb)Ni2B2C	Dy0.95Tb0.05Ni2B2C1	Dy	0.95	Tb	0.05	Ni	2	B	2	C	1														3	2005								10																				LuNi2B2C																		K				5.61			5.61																																																																																																flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90304	P072054516		(Dy,Tb)Ni2B2C	Dy0.9Tb0.1Ni2B2C1	Dy	0.9	Tb	0.1	Ni	2	B	2	C	1														3	2005								10																				LuNi2B2C																		K				4.7			4.7																																																																																																flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90305	P072054516		(Dy,Tb)Ni2B2C	Dy0.75Tb0.25Ni2B2C1	Dy	0.75	Tb	0.25	Ni	2	B	2	C	1														3	2005								9.83																				LuNi2B2C																		K				3.24			3.24																																																																																																flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90306	P072054516		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	2005								10.3																				LuNi2B2C																		K				6.24			6.24																																																																																																flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90307	P072054516		(Dy,Tb)Ni2B2C	Dy0.6Tb0.4Ni2B2C1	Dy	0.6	Tb	0.4	Ni	2	B	2	C	1														3	2005								9.87																				LuNi2B2C																		K					2																																																																																																		flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90308	P072054516		(Dy,Tb)Ni2B2C	Dy0.4Tb0.6Ni2B2C1	Dy	0.4	Tb	0.6	Ni	2	B	2	C	1														3	2005								9.4																				LuNi2B2C																		K					2																																																																																																		flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90309	P072054516		(Dy,Tb)Ni2B2C	Dy0.2Tb0.8Ni2B2C1	Dy	0.2	Tb	0.8	Ni	2	B	2	C	1														3	2005								12.5																				LuNi2B2C																		K					2																																																																																																		flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90310	P072054516		(Dy,Tb)Ni2B2C	Dy0.1Tb0.9Ni2B2C1	Dy	0.1	Tb	0.9	Ni	2	B	2	C	1														3	2005								13.5																				LuNi2B2C																		K					2																																																																																																		flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90311	P072054516		(Dy,Tb)Ni2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																3	2005								15																				LuNi2B2C																		K					2																																																																																																		flux method. Ni2B flux					Effect of Tb substitution for Dy on superconductivity and magnetism in Dy1-xTbxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang , Korea	Phys.Rev.B, 72(2005)054516	J.-H,Choi,H.J.Kim,H.B.Kim,H.J.Doh,S.I.Lee,B.K.Cho		
90312	PHC4110101	as-sintered. R is maximum at T=150 K.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O15	Pr	2	Ba	4	Cu	7															O	15-z	15		2004								16																				Y247			A	3.888	3.9037	50.66																																																																																																																	Pr6O11,BaO2,CuO		mixture - pellet - CAL(850-900C, in air) - SIN(975C,18h, P(O2) = 5 atm)					Superconductivity in Pr2Ba4Cu7O15-z with metallic double chains			Department of Materials Science and Technology, Iwate University, Ueda 4-3-5, Morioka 020-8551, Japan	Physica C, 411(2004)101	M.Matsukawa,Y.Yamada,M.Chiba,H.Ogasawara,T.Shibata,A.Matsushita,Y.Takano		
90313	PHC4110101	ANN(650C,4d in air). O-content determined by TGA.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.5	Pr	2	Ba	4	Cu	7															O	15-z	14.5		2004																												Y247			A	3.8923	3.902	50.814												K			10				10																																																																																														Pr6O11,BaO2,CuO		mixture - pellet - CAL(850-900C, in air) - SIN(975C,18h, P(O2) = 5 atm)					Superconductivity in Pr2Ba4Cu7O15-z with metallic double chains			Department of Materials Science and Technology, Iwate University, Ueda 4-3-5, Morioka 020-8551, Japan	Physica C, 411(2004)101	M.Matsukawa,Y.Yamada,M.Chiba,H.Ogasawara,T.Shibata,A.Matsushita,Y.Takano		
90314	PHC4110101	ANN(400C,24h, in vac). O-content not measured.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O15-z	Pr	2	Ba	4	Cu	7															O	15-z			2004																												Y247																		K	12		18				15																																																																																														Pr6O11,BaO2,CuO		mixture - pellet - CAL(850-900C, in air) - SIN(975C,18h, P(O2) = 5 atm)					Superconductivity in Pr2Ba4Cu7O15-z with metallic double chains			Department of Materials Science and Technology, Iwate University, Ueda 4-3-5, Morioka 020-8551, Japan	Physica C, 411(2004)101	M.Matsukawa,Y.Yamada,M.Chiba,H.Ogasawara,T.Shibata,A.Matsushita,Y.Takano		
90315	P072014519	RRR=100. H//[100]. magnetoresistance measured. G-L parameter = 4.8 using PENET=4700A.	LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2005																												skutterudite																		K		0.74					0.74																				T		0.035							T/K		0.068				MHC90315	A		970																																MTP90315																					MRH90315					Sb self-flux method					Transport properties of the heavy-fermion superconductor PrOs4Sb12			Graduate School of Science, Tokyo Metropolitan University, Minami-Ohsawa, Hachioji, Tokyo 192-0397, Japan	Phys.Rev.B, 72(2005)014519	H. Sugawara,M.Kobayashi,S.Osaki,S.R.Saha,T.Namiki,Y.Aoki,H.Sato		
90316	P072014519	RRR=50	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2005																												skutterudite																		K		1.85					1.85																																																																						MTP90316																					MRH90316					Sb self-flux method					Transport properties of the heavy-fermion superconductor PrOs4Sb12			Graduate School of Science, Tokyo Metropolitan University, Minami-Ohsawa, Hachioji, Tokyo 192-0397, Japan	Phys.Rev.B, 72(2005)014519	H. Sugawara,M.Kobayashi,S.Osaki,S.R.Saha,T.Namiki,Y.Aoki,H.Sato		
90317	P072054520	P-induced SC. Pcrit = 3.5 GPa. Hc2(P) also measured.	Sr2Ca12Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2005																												LAD																		K		5.18			0		5.18	TC90317																																		HC90317																																				mOhm.cm											3														TSFZ method using infrared furnace in O2					Magnetic field effect on the pressure-induced superconducting state in the hole-doped two-leg ladder compound Sr2Ca12Cu24O41			Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa-shi, Chiba 277-8581, Japan	Phys.Rev.B, 72(2005)054520	T.Nakanishi,N.Motoyama,H.Mitamura,N.Takeshita,H.Takahashi,H.Eisaki,S.Uchida,M.Mori		
90318	PHB3590895		LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2005																												skutterudite																		K		0.74					0.74											Oe		12							T		0.04														A		910			A		4700																																																			La,Os,Sb		Sb self-flux method					mSR studies on LaOs4Sb12 in comparison with the time-reversal-symmetry-broken superconductor PrOs4Sb12			Department of Physics, Tokyo Metropolitan University, Minami-Ohsawa 1-1, Hachioji-Shi, Tokyo 192-0397, Japan	Physica B, 359-361(2005)895	Y.Aoki,W.Higemoto,S.Sanada,K.Ohishi,S.R.Saha,A.Koda,K.Nishiyama,R.Kadono,H.Sugawara,H.Sato		
90319	JPC0152071		LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2003																												skutterudite																		K		1					1																				T		0.65																																																																										Sb-flux method					Superconductivity and the high-field ordered phase in the heavy-fermion compound PrOs4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, CA 92093, USA	J.Phys.:Condens.Matter, 15(2003)S2071	M.B.Maple,P.-C.Ho,N.A.Frederick,V.S.Zapf,W.M.Yuhasz,E.D.Bauer,A.D.Christianson,A.H.Lacerda		
90320	EPL0690263	high density granular sample. SP-heat: relaxation method. gamma(H) = 1.04 + 0.17 H^(0.85)	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2005																												IL																		K				43			43																																																								mj/mol.K2	1.04	SP-heat																																											Bulk evidence for s-wave pairing symmetry in electron-doped infinite-layer cuprate Sr0.9La0.1CuO2			National Laboratory for Superconductivity, Institute of Physics Chinese Academy of Sciences, Beijing 100080, PRC	Europhys.Lett., 69(2005)263	Z.Y.Liu,H.H.Wen,L.Shan,H.P.Yang,X.F.Lu,H.Gao,M.S.Park,C.U.Jung,S.I.Lee		
90321	PRL0520679	Sp-heat jump is broad. (dC/gamma*Tc) = 0.48	UPt3	Pt3U1	Pt	3	U	1																					1984																																														K	0.54			0.5		0.03	0.5																																																								mj/mol.K2	450	SP-heat																																											Possibility of coexistence of bulk superconductivity and spin fluctuations in UPt3				Phys.Rev.Lett., 52(1984)679	G.R.Stewart,Z.Fisk,J.O.Willis,J.L.Smith		
90322	PR0390151	lattice const. from J.Phys.Chem.Solids, 36(1985)123	U6Mn	Mn1U6	Mn	1	U	6																					1989																												U6Mn			A	10.312		5.255												K		2.21					2.21																																																								mj/mol.K2	98.81	Sp-heat for 3 < T < 5.75	195.6																																					arc-melting. wrapped in Ta-foil, then annealed below peritectic temperature.					Low-temperature heat-capacity study of the U6X(X=Mn, Fe, Co, Ni) compounds				Phys.Rev.B, 39(1989)151	K.N.Yang,M.B.Maple,L.E.DeLong,J.G.Huber,A.Junod		
90323	PR0390151	lattice const. from J.Phys.Chem.Solids, 36(1985)123	U6Fe	Fe1U6	Fe	1	U	6																					1989																												U6Mn			A	10.303		5.235												K		3.7					3.7																																																								mj/mol.K2	151.7	4.2<T<10.2	114.3																																					arc-melting. wrapped in Ta-foil, then annealed below peritectic temperature.					Low-temperature heat-capacity study of the U6X(X=Mn, Fe, Co, Ni) compounds				Phys.Rev.B, 39(1989)151	K.N.Yang,M.B.Maple,L.E.DeLong,J.G.Huber,A.Junod		
90324	PR0390151	lattice const. from J.Phys.Chem.Solids, 36(1985)123	U6Co	Co1U6	Co	1	U	6																					1989																												U6Mn			A	10.323		5.191												K		2.29					2.29																																																								mj/mol.K2	129.7	2.6<T<5.5 K	111.5																																					arc-melting. wrapped in Ta-foil, then annealed below peritectic temperature.					Low-temperature heat-capacity study of the U6X(X=Mn, Fe, Co, Ni) compounds				Phys.Rev.B, 39(1989)151	K.N.Yang,M.B.Maple,L.E.DeLong,J.G.Huber,A.Junod		
90325	PR0390151	lattice const. from J.Phys.Chem.Solids, 36(1985)123	U6Ni	Ni1U6	Ni	1	U	6																					1989																												U6Mn			A	10.39		5.156												K		0.35					0.35																																																								mj/mol.K2	91.36	0.85<T<5.0 K	178.9																																					arc-melting. wrapped in Ta-foil, then annealed below peritectic temperature.					Low-temperature heat-capacity study of the U6X(X=Mn, Fe, Co, Ni) compounds				Phys.Rev.B, 39(1989)151	K.N.Yang,M.B.Maple,L.E.DeLong,J.G.Huber,A.Junod		
90326	PRL0491448	Hc1 calculated from Hc1(0)=1.8 mT using demagnetization factor D=0.20.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		1	1982																																														K		0.64					0.64											Oe	M vs H curve	23							T		1.7							T/K		5.8																																																																						"Critical fields of the ""heavy-fermion"" superconductor CeCu2Si2"				Phys.Rev.Lett., 49(1982)1448	U.Rauchschwalbe,W.Lieke,C.D.Bredl,F.Steglich,J.Aarts,K.M.Martini,A.C.Mota		
90327	PRL0520469	single crystals obtained using excess Cu, are superconducting. (gap/gamma*Tc) = 1.27	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	1984																																														K		0.64					0.64																				T			2.44	2.04					T/K			23	23	MHC90327																						mj/mol.K2	730																																							Bridgeman method using Al2O3 crucible. Ce:Cu:Si = 1:2(1+x):2, x=0.3 is best.					Superconductivity in CeCu2Si2 single crystals				Phys.Rev.Lett., 52(1984)469	W.Assmus,M.Herrmann,U.Rauchschwalbe,S.Riegel,W.Lieke,H.Spille,S.Horn,G.Weber,F.Steglich,G.Cordier		
90328	P072024543	growth axis [110]. martensitic transformation not completely(T=117.6K). lattice-const at 20K. H//[110]. Hc(0)=0.279T. G-L parameter=90. (dC/RTc)=2.05. e-ph coupling = 1.67.	HfV2	Hf1V2	Hf	1	V	2																				3	2005																												MgCu2(Laves)			A	5.173	5.216	7.4051											MgCu2(Laves), C15	K			8.6				8.6											Oe		100							T		35.4														A		31			A		2740													mj/mol.K2	45.9		170																																					arc-melting , then floating zone method					Specific heat of single-crystal HfV2: Strong-coupling conventional superconductivity and the effect of the martensitic transition			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 72(2005)024543	F.R.Drymiotis,J.C.Lashley,T.Kimura,G.Lawes,J.L.Smith,D.J.Thoma,R.A.Fisher,N.E.Phillips,Ya.Mudryk,V.K.Pecharsky,X.Moya,A.Planes		
90329	P072024543	poly crystal. martensitic transformation at T=96.3K.  (dC/RTc)=1.95. e-ph coupling = 2.25.	HfV2	Hf1V2	Hf	1	V	2																				1	2005																												MgCu2(Laves)																	MgCu2(Laves), C15	K			7.6				7.6																																																								mj/mol.K2	55.8		162																																					arc-melting					Specific heat of single-crystal HfV2: Strong-coupling conventional superconductivity and the effect of the martensitic transition			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 72(2005)024543	F.R.Drymiotis,J.C.Lashley,T.Kimura,G.Lawes,J.L.Smith,D.J.Thoma,R.A.Fisher,N.E.Phillips,Ya.Mudryk,V.K.Pecharsky,X.Moya,A.Planes		
90330	L095087003	intercalated sample	CaC6	C6Ca1	C	6	Ca	1																					2005																													R3[-]m																rhombohedral lat-a=5.17 A, alpha=49.55 degree	K				11.5			11.5																																		MHC90330		nm			35	13																																																								reaction(350C,10d, under Ar atmosphere) (pyrolytic graphite + molten Li-Ca)					Superconductivity of Bulk CaC6			Laboratoire de Chimie du Solide Mineral?UMR 7555, Universite Henri Poincare Nancy I, B.P. 239, Cedex, France	Phys.Rev.Lett., 95(2005)087003	N.Emery,C.Herold,M.d'Astuto,V.Garcia,Ch.Bellin,J.F.Mareche,P.Lagrange,G.Loupias		
90331	MAT0503570	intercalated sample. anisotropy factor = 2.	YbC6	C6Yb1	C	6	Yb	1																					2005																																														K				6.5			6.5										90																								MHC90331																																																														highly oriented pyrolytic graphite. deposit and intercalate by vapor transport method					Superconductivity in the Intercalated Graphite Compounds C6Yb and C6Ca			Department of Physics and Astronomy, University College of London, Gower Street, London, UK	cond-mat/0503570	T.E.Weller,M.Ellerby,S.S.Saxenal,R.P.Smith,N.T.Skipper		
90332	MAT0503570	intercalated sample	CaC6	C6Ca1	C	6	Ca	1																					2005																																														K				11.5			11.5																																																																																																highly oriented pyrolytic graphite. deposit and intercalate by vapor transport method					Superconductivity in the Intercalated Graphite Compounds C6Yb and C6Ca			Department of Physics and Astronomy, University College of London, Gower Street, London, UK	cond-mat/0503570	T.E.Weller,M.Ellerby,S.S.Saxenal,R.P.Smith,N.T.Skipper		
90333	SSC0430005	stage-I compound	KTl1.5C4	K1Tl1.5C4	K	1	Tl	1.5	C	4																			1982																															A			12.08												K				2.7			2.7																																		MHC90333																																																														heat(highly oriented pyrolytic graphite in KTl + Tl atmosphere)					Superconductivity of graphite intercalated with thallium alloys				Solid State Commun., 43(1982)5	R.A.Wachnik,L.A.Pendrys,F.L.Vogel,P.Lagrange		
90334	SSC0430005	stage-II compound	KTl1.5C8	K1Tl1.5C8	K	1	Tl	1.5	C	8																			1982																															A			15.48												K				2.45			2.45																																																																																																stoichiometric(graphite powder+Ktl+Tl) - heat(in sealed tube)					Superconductivity of graphite intercalated with thallium alloys				Solid State Commun., 43(1982)5	R.A.Wachnik,L.A.Pendrys,F.L.Vogel,P.Lagrange		
90335	SSC0690921	Unstable. XRD at 100K. Tc depends on time. After 10 days, Tc = 1.7 K.	LiC2	C2Li1	C	2	Li	1																					1989																															A			3.69												K		1.9					1.9																																																																																																(graphite+Li) - heat(350C,6h, P=30-40 kbar) - quench to (80-100 K)					Superconductivity of graphite intercalation compound with C2Li				Solid State Commun., 69(1989)921	I.T.Belash,A.D.Bronnikov,O.V.Zharikov,A.V.Pal'nichenko		
90336	L095097006	disorder effect (La,Nd) of Tc was measured.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2005																												T																		K				35.3			35.3																																																																																					cm3/C	0.0011					RH90336										Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90337	L095097006	disorder effect (La,Nd) of Tc was measured.	(La,Nd,Sr)2CuO4	La1.75Nd0.1Sr0.15Cu1O4	La	1.75	Nd	0.1	Sr	0.15	Cu	1													O	4		3	2005																												T																		K				31.8			31.8																																																																																																					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90338	L095097006	disorder effect (La,Nd) of Tc was measured.	(La,Nd,Sr)2CuO4	La1.65Nd0.2Sr0.15Cu1O4	La	1.65	Nd	0.2	Sr	0.15	Cu	1													O	4		3	2005																												T																		K				29			29																																																																																																					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90339	L095097006	disorder effect (La,Nd) of Tc was measured.	(La,Nd,Sr)2CuO4	La1.55Nd0.3Sr0.15Cu1O4	La	1.55	Nd	0.3	Sr	0.15	Cu	1													O	4		3	2005																												T																		K				19.2			19.2																																																																																																					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90340	L095097006	disorder effect (La,Nd) of Tc was measured.	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	2005																												T																		K				9			9																																																																																					cm3/C	0.00108					RH90340										Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90341	L095097006		Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2005																												Bi2201			A			24.44												K				34			34																																																																																					cm3/C	0.0013					RH90341					ANN(650C,48h, in flowing O2) - Q to RT					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90342	L095097006		Bi2(Sr,Nd)2CuO6	Bi2Sr1.6Nd0.4Cu1O6+z	Bi	2	Sr	1.6	Nd	0.4	Cu	1													O	6+z		3	2005																												Bi2201																		K				29.5			29.5																																																																																																ANN(650C,48h, in flowing O2) - Q to RT					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90343	L095097006		Bi2(Sr,Eu)2CuO6	Bi2Sr1.6Eu0.4Cu1O6+z	Bi	2	Sr	1.6	Eu	0.4	Cu	1													O	6+z		3	2005																												Bi2201																		K				16			16																																																																																																ANN(650C,48h, in flowing O2) - Q to RT					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90344	L095097006		Bi2(Sr,Gd)2CuO6	Bi2Sr1.6Gd0.4Cu1O6+z	Bi	2	Sr	1.6	Gd	0.4	Cu	1													O	6+z		3	2005																												Bi2201			A			24.35												K				12.9			12.9																																																																																					cm3/C	0.0013					RH90344					ANN(650C,48h, in flowing O2) - Q to RT					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90345	L095097006		Bi2(Sr,La,Gd)2CuO6	Bi2Sr1.6La0.2Gd0.2Cu1O6+z	Bi	2	Sr	1.6	La	0.2	Gd	0.2	Cu	1											O	6+z		3	2005																												Bi2201																		K				27			27																																																																																																ANN(650C,48h, in flowing O2) - Q to RT					Effect of Disorder Outside the CuO2 Planes on Tc of Copper Oxide Superconductors			Department of Advanced Materials Science, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.Lett., 95(2005)097006	K.Fujita,T.Noda,K.M.Kojima,H.Eisaki,S.Uchida		
90346	PR1440300		In1-xCdx	Cd0.01In0.99	Cd	0.01	In	0.99																				1	1966																																														K	3.34		3.349				3.3445																																																																																																melt in pyrex tube at 200 C) - ANN(130C).					Electronic structure and superconductivity of indium-cadmium alloys				Phys.Rev., 144(1966)300	M.F.Merriam		
90347	PR1440300		In1-xCdx	Cd0.02In0.98	Cd	0.02	In	0.98																				1	1966																																														K	3.286		3.303				3.2945	MTC90347																																																																																															melt in pyrex tube at 200 C) - ANN(130C).					Electronic structure and superconductivity of indium-cadmium alloys				Phys.Rev., 144(1966)300	M.F.Merriam		
90348	PR1440300		In1-xCdx	Cd0.03In0.97	Cd	0.03	In	0.97																				1	1966																																														K	3.267		3.284				3.2755																																																																																																melt in pyrex tube at 200 C) - ANN(130C).					Electronic structure and superconductivity of indium-cadmium alloys				Phys.Rev., 144(1966)300	M.F.Merriam		
90349	PR1440300		In1-xCdx	Cd0.04In0.96	Cd	0.04	In	0.96																				1	1966																																														K	3.252		3.267				3.2595																																																																																																melt in pyrex tube at 200 C) - ANN(130C).					Electronic structure and superconductivity of indium-cadmium alloys				Phys.Rev., 144(1966)300	M.F.Merriam		
90350	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	La3In	In1La3	In	1	La	3																					1969																																														K		9.46					9.46			K/GPa	0.36																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90351	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	(La,Ce)3In	La2.9579Ce0.0421In1	La	2.9579	Ce	0.0421	In	1																			1969																																														K		7.11					7.11			K/GPa	-0.34																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90352	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	(La,Ce)3In	La2.9394Ce0.0606In1	La	2.9394	Ce	0.0606	In	1																			1969																																														K		5.72					5.72			K/GPa	-0.82																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90353	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	(La,Ce)3In	La2.9251Ce0.0749In1	La	2.9251	Ce	0.0749	In	1																			1969																																														K		4.42					4.42			K/GPa	-1.47																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90354	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	(La,Ce)3In	La2.9234Ce0.0766In1	La	2.9234	Ce	0.0766	In	1																			1969																																														K		4.02					4.02			K/GPa	-1.74																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90355	PRL0230118	Tc by mutual inductance. (dTc/dP) estimated from Tc(P) figure.	(La,Gd)3In	La2.9602Gd0.0398In1	La	2.9602	Gd	0.0398	In	1																			1969																																														K		6.04					6.04			K/GPa	0.53																																																																																												arc-melting in Ar.					Pressure-dependent pair breaking in superconducting La3-xCexIn alloys				Phys.Rev.Lett., 23(1969)118	M.B.Maple,Kang-Soo Kim		
90356	PLA0370251	Tc for Zr isotope(90, 91, 92, 94) were measured.	ZrB12	B12Zr1	B	12	Zr	1																					1971																																														K		5.94				0.04	5.94	MTC90356					0.32	Zr																																																																																									arc-melting					Superconducting isotope effect in ZrB12				Phys.Lett.A, 37(1971)251	Z.Fisk,A.C.Lawsom,B.T.Mattias,E.Corenzwit		
90357	PR1790452	Tc by ac-impedance bridge. Tc measured for various Mo isotopes.	Mo2B	B1Mo2	B	1	Mo	2																					1969																												CuAl2			A	5.543		4.735												K		5.86					5.86						0.42	Mo																																																																																														Superconducting isotope effect in molybdenum boride and tungsten boride				Phys.Rev., 179(1969)452	J.J.Englhardt		
90358	PR1790452	Tc by ac-impedance bridge. Tc measured for various B isotopes.	Mo2B	B1Mo2	B	1	Mo	2																					1969																												CuAl2																		K		5.86					5.86						0.004	B																																																																																														Superconducting isotope effect in molybdenum boride and tungsten boride				Phys.Rev., 179(1969)452	J.J.Englhardt		
90359	PR1790452	Tc by ac-impedance bridge. Tc measured for various W isotopes.	W2B	B1W2	B	1	W	2																					1969																												CuAl2			A	5.564		4.74												K		3.18					3.18						0.52	W																																																																																														Superconducting isotope effect in molybdenum boride and tungsten boride				Phys.Rev., 179(1969)452	J.J.Englhardt		
90360	PR1790452	Tc by ac-impedance bridge. Tc measured for various B isotopes.	W2B	B1W2	B	1	W	2																					1969																												CuAl2																		K		3.18					3.18						0.09	B																																																																																														Superconducting isotope effect in molybdenum boride and tungsten boride				Phys.Rev., 179(1969)452	J.J.Englhardt		
90361	PR1201964	Using Sn(116), Sn(124)	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1960																												Cr3Si(A15)																	A15	K		17.9					17.9						0.025	Sn																																																																																														Isotope effect in Nb3Sn				Phys.Rev., 120(1960)1964	G.E.Devlin,E.Corenzwit		
90362	PR1201964	Using Sn(116), Sn(124)	Sn	Sn1	Sn	1																							1960																																														K		3.72					3.72						0.46	Sn																																																																																														Isotope effect in Nb3Sn				Phys.Rev., 120(1960)1964	G.E.Devlin,E.Corenzwit		
90363	PR1291025		Mo3Ir	Ir1Mo3	Ir	1	Mo	3																					1963																												Cr3Si(A15)																	A15	K		8.35					8.35						0.22	Mo																																																																																														Intermediate isotope effect of molybdenum and Mo3Ir				Phys.Rev., 129(1963)1025	B.T.Mattias,T.H.Geballe,E.Corenzwit,G.W.Hull,Jr		
90364	PR1291025		Mo	Mo1	Mo	1																							1963																																														K		0.916					0.916						0.33	Mo																																																																																														Intermediate isotope effect of molybdenum and Mo3Ir				Phys.Rev., 129(1963)1025	B.T.Mattias,T.H.Geballe,E.Corenzwit,G.W.Hull,Jr		
90365	PLA0240340		Be22Mo	Be22Mo1	Be	22	Mo	1																					1967																																														K		2.51					2.51						0.23	Mo																																																																																														Superconductivity and isotope effect in Be22X compounds and molybdenum				Phys. Lett., 24A(1967)340	E.Bucher,C.Palmy		
93309	PHC4070031	C-content, x = 0.06864 (estimated from LATA)	MgB2	B2Mg1	B	2	Mg	1																				1	2004																												AlB2			A	3.0841		3.5281												K		38.81					38.81																																																																																																solid-vapour reaction (900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
100001	1867	deposited at 4K.	Ag0.15Bi0.85	Ag0.15Bi0.85	Ag	0.15	Bi	0.85																					1974																																														K		5.3					5.3																																																																																																									J.DE PHYS.(PARIS),35(1974)261	D.KORN,G.ZIBOLD,W.MURER		
100002	606		Ag1Bi2	Ag1Bi2	Ag	1	Bi	2																					1966																																														K		3					3																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100003	11		Ag1Bi1	Ag1Bi1	Ag	1	Bi	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100004	11		Ag2Bi1	Ag2Bi1	Ag	2	Bi	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100005	84		Ag1Bi1	Ag1Bi1	Ag	1	Bi	1																					1933																																														K					1.32																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100006	1769		Ag1Be2	Ag1Be2	Ag	1	Be	2																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100007	11		Ag2Be1	Ag2Be1	Ag	2	Be	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100008	486		Ag5Ba1	Ag5Ba1	Ag	5	Ba	1																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100009	605	clathrate 	Ag7O8(BF4) 	Ag7F4O8B1	Ag	7	F	4	O	8	B	1																	1966																																													cubic	K		0.15					0.15																																																																																																					METALIC CONDUCTTIVITY AND SUPERCONDUCTIVITY IN SOME SILVER CLATHRATE SALTS				PHYS.REV.LETT.,17(1966)917	D.B.MCWHAN,K.ANDRES,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
100010	84		Ag0.91As0.09	Ag0.91As0.09	Ag	0.91	As	0.09																					1933																																														K					1.32																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100011	1895		Ag0.002Al0.998	Ag0.002Al0.998	Ag	0.002	Al	0.998																					1974																																														K		1.128					1.128																																																																																																									PHYS.REV.B,10(1974)2756	F.BEHROOZI,F.H.ROGAN,G.A.WILKINSON,M.P.GARFUNCLE		
100012	1413		Ag0.167Al0.833	Ag0.167Al0.833	Ag	0.167	Al	0.833																					1973																																														K		0.88					0.88																																																																																																									PHIL.MAG.,28(1973)867	A.NEMOZ		
100013	605		Ag7F1O8	Ag7F1O8	Ag	7	F	1	O	8																			1966																																													cubic	K		0.3					0.3																																																																																																					METALIC CONDUCTTIVITY AND SUPERCONDUCTIVITY IN SOME SILVER CLATHRATE SALTS				PHYS.REV.LETT.,17(1966)917	D.B.MCWHAN,K.ANDRES,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
100014	1146		Ag7F0.25N0.75O10.25	Ag7F0.25N0.75O10.25	Ag	7	F	0.25	N	0.75	O	10.25																	1967																																														K		1.04					1.04																																																																																																					Nuclear magnetic resonance and superconductivity in the clathrate salts [Ag7O8]HF2				J.AMER.CHEM.SOC.,89(1967)7121	A.C.GOSSARD,D.K.HINDERMANN,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
100015	1146		Ag7F2H1O8	Ag7F2H1O8	Ag	7	F	2	H	1	O	8																	1967																																														K		1.5					1.5																																																																																																					Nuclear magnetic resonance and superconductivity in the clathrate salts [Ag7O8]HF2				J.AMER.CHEM.SOC.,89(1967)7121	A.C.GOSSARD,D.K.HINDERMANN,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
100016	651		Ag2I1	Ag2I1	Ag	2	I	1																					1966																																														K		0.066					0.066																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1747	K.ANDRES,M.B.ROBIN,N.A.KUEBLER		
100017	1901		Ag0.16D00.47Pd0.84	Ag0.16D0.47Pd0.84	Ag	0.16	D	0.47	Pd	0.84																			1974																																														K		15.3					15.3																																																																																																									Z.PHYS.,268(1974)261	B.STRITZKER		
100018	1864		Ag0.56Cu0.22Sn0.5Zn0	Ag0.56Cu0.22Sn0.5Zn0.17	Ag	0.56	Cu	0.22	Sn	0.5	Zn	0.17																	1972																																														K					0.033																																																																																																											REV.SCI.INSTRUM.,43(1972)1540	J.LANDAU,R.ROSENBAUM		
100019	84		Ag4Cu9	Ag4Cu9	Ag	4	Cu	9																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100020	99		Ag1Cl2	Ag1Cl2	Ag	1	Cl	2																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100021	1917		Ag0.035Cd0.01Sn0.95 	Ag0.035Cd0.01Sn0.955	Ag	0.035	Cd	0.01	Sn	0.955																			1969																																														K		3.65					3.65																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100022	1917		Ag0.04Cd0.784Cu0.01Z	Ag0.04Cd0.784Cu0.01Zn0.166	Ag	0.04	Cd	0.784	Cu	0.01	Zn	0.166																	1969																																														K					1.3																																																																																																											REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100023	1617		Ag0.6Cd0.4	Ag0.6Cd0.4	Ag	0.6	Cd	0.4																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
100024	84		Ag5Cd8	Ag5Cd8	Ag	5	Cd	8																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100025	697	P=9.5 kbar.  	Ag1La1	Ag1La1	Ag	1	La	1																					1966																												CsCl																	CsCl, B2	K		1.2					1.2																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1555	C.C.CHAO,H.L.LUO,T.F.SMITH		
100026	697		Ag1La1	Ag1La1	Ag	1	La	1																					1966																																														K		0.96					0.96																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1555	C.C.CHAO,H.L.LUO,T.F.SMITH		
100027	1899	1000-240A	Ag0.12In0.88	Ag0.12In0.88	Ag	0.12	In	0.88																					1975																																														K		4.69					4.69																																																																																																									SOLID STATE COMMUN.,16(1975)581	C.G.GRANQVIST		
100028	1317		Ag2In1	Ag2In1	Ag	2	In	1																					1971																												CuAl2																	CuAl2, C16	K		2.11					2.11																																																																																																									SOLID STATE COMMUN.,9(1971)1881	B.P.CLAYMAN,R.F.FRINDT		
100029	533		Ag3In1	Ag3In1	Ag	3	In	1																					1965																																														K					1.4																																																																																																											ZH.EKSP.TEOR.FIZ.,49(1965)159	N.E.ALEKSEEVSKII		
100030	1617		Ag0.85In0.15	Ag0.85In0.15	Ag	0.85	In	0.15																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
100031	258		Ag0.55Hg0.45	Ag0.55Hg0.45	Ag	0.55	Hg	0.45																																																																		hexagonal	K					1.08																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
100032	259		Ag0.7Hg0.3	Ag0.7Hg0.3	Ag	0.7	Hg	0.3																																																																		cubic	K					0.33																																																																																																							From Roberts' Table, unpublished results				Unpublished results	C.Raub,T.H.Geballe		
100033	489		Ag0.438Hg0.562	Ag0.438Hg0.562	Ag	0.438	Hg	0.562																					1964																												Cu5Zn8																	Cu5Zn8, D8[2]	K		0.64					0.64																																																																																																									BULL.AM.PHYS.SOC.,9(1964)268	A.R.SWEEDLER,D.C.HAMILTON,M.F.MERRIAM		
100034	1729		Ag0.5Ge0.5	Ag0.5Ge0.5	Ag	0.5	Ge	0.5																					1971																																														K					1.5																																																																																																											ZH.ETF PIS.RED.,13(1971)412	N.E.ALEKSEEVSKII,V.I.TSEBRO,V.M.ZAKOSARENKO		
100035	1082	200-600A  deposit  at 4K.	Ag0.45Ge0.55	Ag0.45Ge0.55	Ag	0.45	Ge	0.55																					1971																																														K		1.5					1.5																																																																																																					Zur Supraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,243(1971)361	B.STRITZKER,H.WUHL		
100036	487		Ag4Ge1	Ag4Ge1	Ag	4	Ge	1																					1964																																													hexagonal	K		0.85					0.85																																																																																																									SCIENCE,145(1964)581	D.C.HAMILTON,H.L.LUO,M.F.MERRIAM		
100037	11		Ag2S1	Ag2S1	Ag	2	S	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100038	1060		Ag0.05Rh0.04Ti0.91	Ag0.05Rh0.04Ti0.91	Ag	0.05	Rh	0.04	Ti	0.91																			1964																																														K		1.95					1.95																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
100039	1221		Ag2Pb3S1	Ag2Pb3S1	Ag	2	Pb	3	S	1																			1973																												beta-Mn																	beta-Mn, A13	K		1.13					1.13																																																																																																									J.LESS-COMMON METALS,30(1973)167	A.C.LAWSON,CH.J.RAUB,H.R.KHAN,H.TRUNK,W.A.FERTIG		
100040	1917		Ag0.15Pb0.975Sn0.01	Ag0.15Pb0.975Sn0.01	Ag	0.15	Pb	0.975	Sn	0.01																			1969																																														K		7.25					7.25																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100041	11		Ag2O1	Ag2O1	Ag	2	O	1																					1952																																														K					0.128																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100042	181		Ag1Nb3	Ag1Nb3	Ag	1	Nb	3																																																																			K		8.28					8.28																																																																																																					From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
100043	605	Thermodynamic Hc(0) = 57 Oe, G-L parameter = 100.	Ag7O8(NO3)	Ag7N1O11	Ag	7	N	1																	O	11			1966																																													cubic	K		1.04					1.04																																																																																																					METALIC CONDUCTTIVITY AND SUPERCONDUCTIVITY IN SOME SILVER CLATHRATE SALTS				PHYS.REV.LETT.,17(1966)917	D.B.MCWHAN,K.ANDRES,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
100044	1163		Ag1.2Mo4.8S6	Ag1.2Mo4.8S6	Ag	1.2	Mo	4.8	S	6																			1972																																													rhombohedral	K		8.9					8.9																																																																																																									SCI.,175(1972)1465	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO		
100045	614	0-19 kbar	Ag1Mo4S5	Ag1Mo4S5	Ag	1	Mo	4	S	5																			1975																																														K		7.7					7.7																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
100046	1193		Ag1Mo4S5	Ag1Mo4S5	Ag	1	Mo	4	S	5																			1972																																														K		8.3					8.3																																																																																																									SCI.,177(1972)267	A.C.LAWSON,R.VISWANATHAN		
100047	RMP0350001		Ag1Mg1	Ag1Mg1	Ag	1	Mg	1																					1963																												CsCl																	CsCl, B2	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100048	658		Ag1Lu1	Ag1Lu1	Ag	1	Lu	1																					1967																												CsCl																	CsCl, B2	K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100049	1377		Ag1Th2	Ag1Th2	Ag	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K		2.19					2.19																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100050	487		Ag1Te3	Ag1Te3	Ag	1	Te	3																					1964																																													cubic	K		2.6					2.6																																																																																																									SCIENCE,145(1964)581	D.C.HAMILTON,H.L.LUO,M.F.MERRIAM		
100051	11		Ag1Te3	Ag1Te1	Ag	1	Te	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100052	486		Ag5Sr1	Ag5Sr1	Ag	5	Sr	1																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100053	486		Ag5Sn1	Ag5Sn1	Ag	5	Sn	1																					1965																												Mg																	Mg, A3	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100054	85		Ag3Sn1	Ag3Sn1	Ag	3	Sn	1																					1932																																														K					1.36																																																																																																							From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100055	84		Ag0.92Sn0.8	Ag0.92Sn0.8	Ag	0.92	Sn	0.8																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100056	533		Ag1Si2	Ag1Si2	Ag	1	Si	2																					1965																																														K					1.4																																																																																																											ZH.EKSP.TEOR.FIZ.,49(1965)159	N.E.ALEKSEEVSKII		
100057	11		Ag2Se1	Ag2Se1	Ag	2	Se	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100058	99		Ag1Sb1	Ag1Sb1	Ag	1	Sb	1																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100059	84		Ag0.865Sb0.135	Ag0.865Sb0.135	Ag	0.865	Sb	0.135																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100060	84		Ag3Sb1	Ag3Sb1	Ag	3	Sb	1																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100061	486		Al1Au4	Al1Au4	Al	1	Au	4																					1965																												beta-Mn																	beta-Mn, A13	K		0.7					0.7																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100062	1011		Al2Au1	Al2Au1	Al	2	Au	1																					1969																												CaF2																	CaF2, C1	K		0.095					0.095																																																																																																									BULL.AMER.PHYS.SOC.,14(1969)382	A.MENTH,G.HULL,J.H.WERNICK,J.P.MAITA,T.H.GEBALLE		
100063	939		Al0.9As0.05Ga0.05Nb3	Al0.9As0.05Ga0.05Nb3	Al	0.9	As	0.05	Ga	0.05	Nb	3																	1969																																														K		19.2					19.2																																																																																																									PHYS.LETT.A,28(1969)707	P.R.SAHM,T.V.PRUSS		
100064	762		Al1	Al1	Al	1																							1965																																														K		1.175					1.175																																																																																																									PHYS.REV.,138(1965)A1428	G.CHANIN,S.CAPLAN		
100065	1506		Ag0.005Zn0.995	Ag0.005Zn0.995	Ag	0.005	Zn	0.995																					1973																																														K		0.763					0.763																																																																																																									J.LOW TEMP.PHYS.,11(1973)687	E.DUCLA-SOARES,J.D.N.CHEEKE		
100066	1009		Ag1Zn1	Ag1Zn1	Ag	1	Zn	1																																																																		gamma	K					1.3																																																																																																							From Roberts' Table, unpublished results				Personal communication	D.R.O'Boyle		
100067	84		Ag1Zn3	Ag1Zn3	Ag	1	Zn	3																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100068	84		Ag5Zn8	Ag5Zn8	Ag	5	Zn	8																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100069	658		Ag1Y1	Ag1Y1	Ag	1	Y	1																					1967																												CsCl																	CsCl, B2	K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100070	1900		Ag0.1Tl0.9	Ag0.1Tl0.9	Ag	0.1	Tl	0.9																					1974																																														K		3.57					3.57																																																																																																									Z.PHYS.,269(1974)23	C.G.GRANQVIST,T.CLAAESON		
100071	85	 eutectic	Ag1Tl1	Ag1Tl1	Ag	1	Tl	1																					1932																																														K		2.67					2.67																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100072	84		Ag0.94Tl0.06	Ag0.94Tl0.06	Ag	0.94	Tl	0.06																					1933																																														K		2.32					2.32																																																																																																					From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100073	496		Al2C1Mo3	Al2C1Mo3	Al	2	C	1	Mo	3																			1964																												beta-Mn																	beta-Mn, A13	K		10					10																																																																																																									SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100074	1564		Al1C1La3	Al1C1La3	Al	1	C	1	La	3																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100075	632		Al1C1Cr2	Al1C1Cr2	Al	1	C	1	Cr	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100076	496		Al2C1Cr3	Al2C1Cr3	Al	2	C	1	Cr	3																			1964																																													hexagonal	K					4.2																																																																																																											SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100077	558		Al4C3	Al4C3	Al	4	C	3																																																																			K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100078	1360		Al0.95Be0.05Nb3	Al0.95Be0.05Nb3	Al	0.95	Be	0.05	Nb	3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		19.6					19.6																																																																																																									J.PHYS.SOC.JAPAN,35(1973)108	M.KUDO,S.FUKASE,U.KAWABE		
100079	1769		Al1Be13	Al1Be13	Al	1	Be	13																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100080	674		Al0.1Be0.9	Al0.1Be0.9	Al	0.1	Be	0.9																					1975																																														K		7.2					7.2																																																																																																									Z.PHYS.B,20(1975)241	C.G.GRANQVIST,T.CLAESON		
100081	674		Al0.3Be0.7	Al0.3Be0.7	Al	0.3	Be	0.7																					1975																																														K		6.5					6.5																																																																																																									Z.PHYS.B,20(1975)241	C.G.GRANQVIST,T.CLAESON		
100082	1360		Al0.95B0.05Nb3	Al0.95B0.05Nb3	Al	0.95	B	0.05	Nb	3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		19.1					19.1																																																																																																									J.PHYS.SOC.JAPAN,35(1973)108	M.KUDO,S.FUKASE,U.KAWABE		
100083	767		Al0.2B5Mo1.8	Al0.2B5Mo1.8	Al	0.2	B	5	Mo	1.8																			1970																												AlB2																	AlB2, C32	K		5.7					5.7																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100084	1617		Al0.15Au0.85	Al0.15Au0.85	Al	0.15	Au	0.85																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
100085	1507		Al0.996Co0.004	Al0.996Co0.004	Al	0.996	Co	0.004																					1972																																														K																																																																																																																J.LOW TEMP.PHYS.,8(1972)219	C.RIZZUO,E.BABIC,E.SALAMONI,P.J.FORD		
100086	655		Al2Ce1	Al2Ce1	Al	2	Ce	1																					1967																												MgCu2(Laves)																	MgCu2, C15	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100087	427		Al2Ca1Si1	Al2Ca1Si1	Al	2	Ca	1	Si	1																			1962																																														K		5.8					5.8																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100088	RMP0350001		Al4Ca1	Al4Ca1	Al	4	Ca	1																					1963																												Al4Ba																	Al4Ba, D1[3]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100089	RMP0350001		Al2Ca1	Al2Ca1	Al	2	Ca	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100090	711		Al1C1Y3	Al1C1Y3	Al	1	C	1	Y	3																																																																	K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100091	632		Al1C1V2	Al1C1V2	Al	1	C	1	V	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100092	496		Al2C1V3	Al2C1V3	Al	2	C	1	V	3																			1964																																													hexagonal	K					4.2																																																																																																											SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100093	711		Al1C1Ti3	Al1C1Ti3	Al	1	C	1	Ti	3																																																																	K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100094	496		Al2C1Ti3	Al2C1Ti3	Al	2	C	1	Ti	3																			1964																																													hexagonal	K					4.2																																																																																																											SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100095	496		Al2C1Ta3	Al2C1Ta3	Al	2	C	1	Ta	3																			1964																																													hexagonal	K					4.2																																																																																																											SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100096	496		Al2CaNb3	Al2C1Nb3	Al	2	C	1	Nb	3																			1964																																													hexagonal	K					4.2																																																																																																											SOL.STATE COMMUN.,2(1964)123	E.PARKER,J.JOHNSTON,L.KENNEDY,TOTH		
100097	1073		Al0.5Ga0.5V3	Al0.5Ga0.5V3	Al	0.5	Ga	0.5	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.9					12.9																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100098	1339		Al0.5Ga0.5Nb3	Al0.5Ga0.5Nb3	Al	0.5	Ga	0.5	Nb	3																			1972																																														K		19					19																																																																																																									PHYS.LETT.A,38(1972)323	A.WICKLUND,E.J.MCNIFF JR.,G.W.WEBB,L.J.VIELAND,R.E.MILLER,S.FONER		
100099	1976		Al0.9Ga0.1Nb3	Al0.9Ga0.1Nb3	Al	0.9	Ga	0.1	Nb	3																			1971																																														K		17.7					17.7																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
100100	976		Al0.999Fe0.001	Al0.999Fe0.001	Al	0.999	Fe	0.001																					1963																																														K		1.5					1.5																																																																																																									PHYS.LETT.,7(1963)108	F.J.DUCHATENINER,S.H.GOEDMOED		
100101	1507		Al0.998Fe0.002	Al0.998Fe0.002	Al	0.998	Fe	0.002																					1972																																														K																																																																																																																J.LOW TEMP.PHYS.,8(1972)219	C.RIZZUO,E.BABIC,E.SALAMONI,P.J.FORD		
100102	1651	deposited at Liq.N2 temperature. d=260A	Al0.997Er0.003	Al0.997Er0.003	Al	0.997	Er	0.003																					1974																																														K		1.658					1.658																																																																																																									PHYS.LETT.A,47(1974)193	P.MONCEAU		
100103	RMP0350001		Al1Cu1Zr1	Al1Cu1Zr1	Al	1	Cu	1	Zr	1																			1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100104	1134	d = 750A	Al1Cu1	Al1Cu1	Al	1	Cu	1																					1968																																														K		3.45					3.45																																																																																																									PHYS.REV.LETT.,21(1968)1320	D.H.DOUGRASS JR.,F,J.E.CROW,KAMMERER,M.A.JENSEN,M.STRONGIN,O,R.D.PARKS		
100105	1640	rapid quench 	Al0.992Cu0.008	Al0.992Cu0.008	Al	0.992	Cu	0.008																					1970																																														K					1.48																																																																																																											PHYS.REV.B,2(1970)3580	B.LEONTIC,E.BABIC,I.ZORIC,R.KRSNIK		
100106	84		Al4Cu9	Al4Cu9	Al	4	Cu	9																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100107	1377		Al2.06Cu1	Al2.06Cu1	Al	2.06	Cu	1																					1972																												CuAl2																	CuAl2, C16	K		0.65					0.65																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100108	1976		Al1Cr0.3Nb2.7	Al1Cr0.3Nb2.7	Al	1	Cr	0.3	Nb	2.7																			1971																																														K		14.1					14.1																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
100109	823		Al0.8Ge0.2Nb3	Al0.8Ge0.2Nb3	Al	0.8	Ge	0.2	Nb	3																			1967																												Cr3Si(A15)																	Cr3Si, A15	K		20.05					20.05																																																																																																									ZH.ETF PIS.RED.,6(1967)901	N.E.ALEKSEEVSKII,N.N.MIKHAILOV,N.V.AGEEV,V.F.SHAMRAI		
100110	1976		Al0.9Ge0.1Nb3	Al0.9Ge0.1Nb3	Al	0.9	Ge	0.1	Nb	3																			1971																																														K		18.9					18.9																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
100111	1660	irradiated	Al1Ge1Nb3	Al1Ge1Nb3	Al	1	Ge	1	Nb	3																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		19.5					19.5																																																																																																									PHYS.REV.LETT.,33(1974)169	A.R.SWEEDLER,D.G.SCHWEITZER,G.W.WEBB		
100112	1819	long annealing 	Al0.77Ge0.23Nb3	Al0.77Ge0.23Nb3	Al	0.77	Ge	0.23	Nb	3																			1970																												Cr3Si(A15)																	Cr3Si, A15	K		20.75					20.75																																																																																																									Z.PHYS.,237(1970)432	J.RUZICKA		
100113	1120	deposited at 77K	Al1Ge1	Al1Ge1	Al	1	Ge	1																					1971																																														K		5.5					5.5																																																																																																									PHYS.LETT.A,35(1971)265	F.MEUNIER,G.DEUTSCHER,J.P.FARGES,P.NEDELLEC		
100114	1528		Al0.9Ge0.1	Al0.9Ge0.1	Al	0.9	Ge	0.1																					1969																																														K		6.45					6.45																																																																																																									J.VAC.SCI.TECH.,6(1969)677	E.GUYON,F.NEUNIER		
100115	1622	deposited at 77K	Al0.964Ge0.036	Al0.964Ge0.036	Al	0.964	Ge	0.036																					1971																																														K		2.74					2.74																																																																																																									PHYS.REV.B,3(1971)1611	J.J.HAUSER		
100116	746		Al1Ge0.026	Al1Ge0.026	Al	1	Ge	0.026																					1965																																														K																																																																																																																PHYS.REV.,137(1965)A112	W.C.JOINER		
100117	427		Al0.33Ge0.67	Al0.33Ge0.67	Al	0.33	Ge	0.67																					1962																																														K		1.75					1.75																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100118	1924	P = 0-18 kbar	Al2Gd0.002La0.998	Al2Gd0.002La0.998	Al	2	Gd	0.002	La	0.998																			1974																																														K		2.45					2.45																																																																																																									Z.PHYSIK,271(1974)305	E.UMLAUF,J.KELLER,M.DIETRICH,P.HOLZER,R.MEIER,W.GEY		
100119	1073		Al0.1Ga0.9V3	Al0.1Ga0.9V3	Al	0.1	Ga	0.9	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		13.9					13.9																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100120	1073		Al0.3Ga0.7V3	Al0.3Ga0.7V3	Al	0.3	Ga	0.7	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		13.9					13.9																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100121	943		Al1La3	Al1La3	Al	1	La	3																					1968																												Ni3Sn																	Ni3Sn, D0[19]	K		6.16					6.16																																																																																																									PHYS.LETT.A,28(1968)12	K.SEKIZAWA,K.YASUKOCHI,Y.KUWASAWA		
100122	658		Al1La1	Al1La1	Al	1	La	1																					1967																																														K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100123	1422		Al2La1	Al2La1	Al	2	La	1																					1972																												MgCu2(Laves)																	MgCu2, C15	K																																																																																																																SOLID STATE COMMUN.,11(1972)175	G.RIBLET,K.WINZER		
100124	1924	P =  18, 20 kbar	Al2La1	Al2La1	Al	2	La	1																					1974																												MgCu2(Laves)																	MgCu2, C15	K		0.3					0.3																																																																																																									Z.PHYSIK,271(1974)305	E.UMLAUF,J.KELLER,M.DIETRICH,P.HOLZER,R.MEIER,W.GEY		
100125	1425		Al2La1	Al2La1	Al	2	La	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		2.237					2.237																																																																																																									SOLID STATE COMMUN.,12(1973)757	C.A.LUENGO,M.B.MAPLE		
100126	711		Al4La1	Al4La1	Al	4	La	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100127	1631		Al11La3	Al11La3	Al	11	La	3																					1970																																													orthorhombic	K					1.3																																																																																																											PHYS.LETT.A,31(1970)103	H.J.VAN DAAL,K.H.J.BUSCHOW		
100128	1201		Al0.046In0.1151Sn0.8	Al0.046In0.151Sn0.803	Al	0.046	In	0.151	Sn	0.803																			1965																																														K		4.38					4.38																																																																																																					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
100129	1966		Al0.75Ge0.25Nb3.8	Al0.75Ge0.25Nb3.8	Al	0.75	Ge	0.25	Nb	3.8																			1974																																														K		20.34					20.34																																																																																																									METAL SCIENCE,8(1974)28	J.A.CAVE,T.J.DAVIS		
100130	876		Al0.75Ge0.25Nb0.003	Al0.75Ge0.25Nb0.003	Al	0.75	Ge	0.25	Nb	0.003																			1969																																														K		20.7					20.7																																																																																																									J.APPL.PHYS.,40(1969)2010	B.T.MATTHIAS,E.CORENZWIT,E.J.MCNIFF JR.,S.FONER		
100131	1446		Al0.66Ge0.22Nb3.1	Al0.66Ge0.22Nb3.1	Al	0.66	Ge	0.22	Nb	3.1																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		20.29					20.29																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
100132	885		Al0.75Ge0.25Nb3	Al0.75Ge0.25Nb3	Al	0.75	Ge	0.25	Nb	3																			1970																												Cr3Si(A15)																	Cr3Si, A15	K		20.2					20.2																																																																																																									J.LOW TEMP.PHYS.,3(1970)393	F.J.CADIEU		
100133	412		Al5Mo1	Al5Mo1	Al	5	Mo	1																																																																		hexagonal	K					1.15																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
100134	RMP0350001		Al12Mo1	Al12Mo1	Al	12	Mo	1																					1963																																													cubic	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100135	1604		Al0.339Mg0.61	Al0.39Mg0.61	Al	0.39	Mg	0.61																					1974																																														K		1.5					1.5																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
100136	1764	deposited at  0.4K	Al0.6Mg0.4	Al0.6Mg0.4	Al	0.6	Mg	0.4																					1973																																														K		1.7					1.7																																																																																																									PHYS.STAT.SOL.,60(1973)157	C.G.GRANQVIST,J.IVARSSON,T.CLAESON		
100137	1340		Al0.11Mg0.89	Al0.11Mg0.89	Al	0.11	Mg	0.89																					1972																																														K					0.013																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100138	1604		Al0.61Mg0.39	Al0.61Mg0.39	Al	0.61	Mg	0.39																					1974																																													hexagonal	K		0.85					0.85																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
100139	1604		Al0.28Mg0.18	Al0.28Mg0.18	Al	0.28	Mg	0.18																					1974																												Cu																	Cu, A1	K		1.63					1.63																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
100140	RMP0350001		Al2Mg3	Al2Mg3	Al	2	Mg	3																					1963																												alpha-Mn																	alpha-Mn, A12	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100141	RMP0350001		Al3Mg2	Al3Mg2	Al	3	Mg	2																					1963																																													cubic	K		0.84					0.84																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100142	658		Al2Lu1	Al2Lu1	Al	2	Lu	1																					1967																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100143	659		Al1Lu3	Al1Lu3	Al	1	Lu	3																																																																			K					1.1																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
100144	RMP0350001		Al1Lu2	Al1Lu2	Al	1	Lu	2																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100145	1075		Al1Nb3	Al1Nb3	Al	1	Nb	3																					1969																																														K		18.1					18.1																																																																																																									Z.PHYS.,219(1969)397	G.MEYER		
100146	939		Al1Nb3	Al1Nb3	Al	1	Nb	3																					1969																																														K		18.52					18.52																																																																																																									PHYS.LETT.A,28(1969)707	P.R.SAHM,T.V.PRUSS		
100147	1215		Al1Nb3	Al1Nb3	Al	1	Nb	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		18.8					18.8																																																																																																									SOLID STATE COMMUN.,7(1969)837	A.C.GOSSARD,A.MENTH,G.W.HULL JR.,J.P.MAITA,R.H.WILLENS,R.R.SODEN,T.H.GEBALLE		
100148	1795	splat cooling 	Al1Nb3	Al1Nb3	Al	1	Nb	3																					1966																												W																	W, A2	K		3.1					3.1																																																																																																									TRANS.MET.SOC.AIME,236(1966)171	E.BUEHLER,R.H.WILLENS		
100149	557		Al0.33Nb0.67	Al0.33Nb0.67	Al	0.33	Nb	0.67																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K		13.5					13.5																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
100150	412		Al3Nb1	Al3Nb1	Al	3	Nb	1																																																	Al3Ti																	Al3Ti, D0[22]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
100151	632		Al2N1Nb3	Al2N1Nb3	Al	2	N	1	Nb	3																			1966																												beta-Mn																	beta-Mn, A13	K		1.3					1.3																																																																																																									J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100152	558		Al1N1	Al1N1	Al	1	N	1																																																	ZnS(wurtzite)																	ZnS(wurtzite), B4	K		1.55					1.55																																																																																																									INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100153	1759		Al0.2Mo5S6Sn1	Al0.2Mo5S6Sn1	Al	0.2	Mo	5	S	6	Sn	1																	1974																																														K																																																																																																																J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
100154	1597		Al0.5Mo5S6Sn1	Al0.5Mo5S6Sn1	Al	0.5	Mo	5	S	6	Sn	1																	1974																																														K		14.2					14.2																																																																																																									PHYS.LETT.A,49(1974)269	E.J.ALEXANDER,E.J.MCNIFF JR.,S.FONER		
100155	427		Al1Mo6Pd1	Al1Mo6Pd1	Al	1	Mo	6	Pd	1																			1962																																														K		2.1					2.1																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100156	125		Al1Mo3	Al1Mo3	Al	1	Mo	3																					1959																												Cr3Si(A15)																	Cr3Si, A15	K		0.58					0.58																																																																																																									J.PHYS.AND CHEM.SOLIDS,9(1959)93	E.CORENZWIT		
100157	1073		Al1Nb2.1V0.9	Al1Nb2.1V0.9	Al	1	Nb	2.1	V	0.9																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100158	1115		Al1Nb1Sn1	Al1Nb1Sn1	Al	1	Nb	1	Sn	1																			1971																												Cr3Si(A15)																	Cr3Si, A15	K		17.45					17.45																																																																																																									PHYS.LETT.A,34(1971)43	A.W.WICKLUND,L.J.VIELAND		
100159	1404		Al0.5Nb3Sn0.5	Al0.5Nb3Sn0.5	Al	0.5	Nb	3	Sn	0.5																			1969																																														K		15.8					15.8																																																																																																									J.APPL.PHYS.,40(1969)2000	A.J.PATTERSON,N.PESSAL,R.D.BLAUGHER		
100160	1821		Al0.22Nb0.75Si0.3	Al0.22Nb0.75Si0.3	Al	0.22	Nb	0.75	Si	0.3																			1971																																														K		19.2					19.2																																																																																																									Z.NATURFORSCH.A,26(1971)1035	A.MULLER		
100161	801		Al0.91Nb3Sb0.1	Al0.9Nb3Sb0.1	Al	0.9	Nb	3	Sb	0.1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		18.06					18.06																																																																																																									PHYS.REV.,152(1966)341	C.C.DICKSON,E.PARTHE,F.ROTHWARF,H.BOLLER,J.A.SCHMITZ,R.C.THIEL		
100162	801		Al0.95Nb3Sb0.5	Al0.95Nb3Sb0.5	Al	0.95	Nb	3	Sb	0.5																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		17.81					17.81																																																																																																									PHYS.REV.,152(1966)341	C.C.DICKSON,E.PARTHE,F.ROTHWARF,H.BOLLER,J.A.SCHMITZ,R.C.THIEL		
100163	1667		Al0.01Nb0.97O0.02	Al0.01Nb0.97O0.02	Al	0.01	Nb	0.97	O	0.02																			1973																																														K		8.3					8.3																																																																																																									FIZ.METAL.METALLOVED.,35(1973)1174	A.F.ORLOV,A.K.MILAY,K.A.OSIPOV,L.S.SOBIYEVA,T.L.BOROVICH		
100164	1667		Al0.04Nb0.895O0.06	Al0.04Nb0.895O0.06	Al	0.04	Nb	0.895	O	0.06																			1973																																														K		7.1					7.1																																																																																																									FIZ.METAL.METALLOVED.,35(1973)1174	A.F.ORLOV,A.K.MILAY,K.A.OSIPOV,L.S.SOBIYEVA,T.L.BOROVICH		
100165	1888		Al1Nb2Ni1	Al1Nb2Ni1	Al	1	Nb	2	Ni	1																			1965																																														K		4.2					4.2																																																																																																									IZV.AKAD.NAUK SSSR METALLY.,(1965)132-136	I.I.KORNILOV,L.N.GUSEVA,R.S.MINTS,YU.S.MALKOV		
100166	1410		Al1Nb3	Al1Nb3	Al	1	Nb	3																					1970																																														K		17.4					17.4																																																																																																									J.SPPL.PHYS.,41(1970)4958	J.I.GITTLEMAN,J.J.HANAK,J.P.PELLICANE,S.BOZOWSKI		
100167	1660		Al1Nb3	Al1Nb3	Al	1	Nb	3																					1974																																														K		18.6					18.6																																																																																																									PHYS.REV.LETT.,33(1974)169	A.R.SWEEDLER,D.G.SCHWEITZER,G.W.WEBB		
100168	859		Al0.215Nb0.785	Al0.215Nb0.785	Al	0.215	Nb	0.785																					1968																																													sigma-phase	K		17.97					17.97																																																																																																									APPL.PHYS.LETT.,13(1968)68	E.R.PARKER,L.D.HARTSOUGH,V.F.ZACKAY		
100169	712		Al12Re1	Al12Re1	Al	12	Re	1																																																																		cubic	K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100170	486		Al1Pt1	Al1Pt1	Al	1	Pt	1																					1965																																													cubic	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100171	486		Al2Pt1	Al2Pt1	Al	2	Pt	1																					1965																												CaF2																	CaF2, C1	K		0.55					0.55																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100172	RMP0350001		Al3Pd4Si1	Al3Pd4Si1	Al	3	Pd	4	Si	1																			1963																												FeSi																	FeSi, B20	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100173	RMP0350001		Al1Os1	Al1Os1	Al	1	Os	1																					1963																												CsCl																	CsCl, B2	K		0.39					0.39																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100174	173		Al3Os1	Al3Os1	Al	3	Os	1																					1961																																														K		5.9					5.9																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
100175	1431		Al3Os2	Al3Os2	Al	3	Os	2																					1968																																														K					1.1																																																																																																							Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
100176	1431		Al2Os1	Al2Os1	Al	2	Os	1																					1968																																														K					1.1																																																																																																							Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
100177	1431		Al13Os4	Al13Os4	Al	13	Os	4																					1968																																														K		5.5					5.5																																																																																																					Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
100178	1980		Al0.175Nb0.775Zr0.05	Al0.175Nb0.775Zr0.05	Al	0.175	Nb	0.775	Zr	0.05																			1974																																														K		10					10																																																																																																									METALLOFIZIKA,50(1974)83	A.I.SUDOVTSOV,V.I.LATYSHEVA,V.M.PAN		
100179	1980		Al0.23Nb0.75Zr0.013	Al0.23Nb0.75Zr0.013	Al	0.23	Nb	0.75	Zr	0.013																			1974																																														K		18.3					18.3																																																																																																									METALLOFIZIKA,50(1974)83	A.I.SUDOVTSOV,V.I.LATYSHEVA,V.M.PAN		
100180	1073		Al1Nb2.7V0.3	Al1Nb2.7V0.3	Al	1	Nb	2.7	V	0.3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100181	1795	splat-cooling	Al1Ta3	Al1Ta3	Al	1	Ta	3																					1966																												W																	W, A2	K		1.59					1.59																																																																																																									TRANS.MET.SOC.AIME,236(1966)171	E.BUEHLER,R.H.WILLENS		
100182	RMP0350001		Al1Ta3	Al1Ta3	Al	1	Ta	3																					1963																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100183	412		Al3Ta1	Al3Ta1	Al	3	Ta	1																																																	Al3Ti																	Al3Ti, D0[22]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
100184	1201		Al0.152Sn0.848	Al0.152Sn0.848	Al	0.152	Sn	0.848																					1965																																														K		3.69					3.69																																																																																																					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
100185	1073		Al0.2Si0.8V3	Al0.2Si0.8V3	Al	0.2	Si	0.8	V	3																			1969																																														K		15.7					15.7																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100186	1073		Al0.1Si0.9V3	Al0.1Si0.9V3	Al	0.1	Si	0.9	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
100187	659		Al1Sc3	Al1Sc3	Al	1	Sc	3																																																																			K					1.1																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
100188	RMP0350001		Al2Sc1	Al2Sc1	Al	2	Sc	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100189	1431		Al13Ru4	Al13Ru4	Al	13	Ru	4																					1968																																													monoclinic	K					1.1																																																																																																							Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
100190	412		Al5Re24	Al5Re24	Al	5	Re	24																																																	alpha-Mn																	alpha-Mn, A12	K		3.35					3.35																																																																																																					From Roberts' Table, Private communication				Private communication	J.Muller		
100191	712		Al1Re1	Al1Re1	Al	1	Re	1																																																	CsCl																	CsCl, B2	K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100192	711		Al6Re1	Al6Re1	Al	6	Re	1																																																																			K		1.85					1.85																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100193	1363	deposited at T =  350-450C	Al1V3	Al1V3	Al	1	V	3																					1971																																														K		10.3					10.3																																																																																																									SOLID STATE COMMUN.,9(1971)855	J.D.HARTSOUGH,R.H.HAMMOND		
100194	514		Al0.108V0.892	Al0.108V0.892	Al	0.108	V	0.892																					1964																																													cubic	K		1.82					1.82																																																								mj/mol.K2	7.25		487																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
100195	824	Si-additions	Al1V3	Al1V3	Al	1	V	3																					1967																												Cr3Si(A15)																	Cr3Si, A15	K		10.3					10.3																																																																																																									ZH.ETF PIS.RED.,6(1967)584	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100196	1369		Al1V3	Al1V3	Al	1	V	3																					1972																												W																	W, A2	K					3																																																																																																											METALL.,26(1972)29	CH.J.RAUB,E.ROSCHEL		
100197	412		Al3V1	Al3V1	Al	3	V	1																																																	Al3Ti																	Al3Ti, D0[22]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
100198	715		Al3U1	Al3U1	Al	3	U	1																					1970																												AuCu3																	AuCu3, L1[2]	K					0.07																																																																																																											J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100199	1803		Al0.03Ti0.81V0.16	Al0.03Ti0.81V0.16	Al	0.03	Ti	0.81	V	0.16																			1964																																														K		5.1					5.1																																																																																																									Z.METALLKDE.,55(1964)711	C.J.RAUB,U.ZWICKER		
100200	RMP0350001		Al3Ti1	Al3Ti1	Al	3	Ti	1																					1963																												Al3Ti																	Al3Ti, D0[22]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100201	927		Al2Th3	Al2Th3	Al	2	Th	3																					1969																																													tetragonal	K		2.6					2.6																																																																																																									PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100202	1377		Al1Th2	Al1Th2	Al	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K		0.09					0.09																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100203	RMP0350001		Al2Th1	Al2Th1	Al	2	Th	1																					1963																												AlB2																	AlB2, C32	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100204	1373		Al3Th1	Al3Th1	Al	3	Th	1																					1971																												Ni3Sn																	Ni3Sn, D0[19]	K		0.75					0.75																																																																																																					Low-temperature specific heat of CeAl3 and related compounds				SOLID STATE COMMUN.,9(1971)1981	H.J.VAN DAAL,K.H.J.BUSCHOW,M.H.VAN MAAREN		
100205	RMP0350001		Al3Zr1	Al3Zr1	Al	3	Zr	1																					1963																												Al3Zr																	Al3Zr, D0[23]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100206	1372		Al2Zn2Zr1	Al2Zn2Zr1	Al	2	Zn	2	Zr	1																			1972																												AuCu3																	AuCu3, L1[2]	K					0.08																																																																																																											J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
100207	1793		Al0.85An0.15	Al0.85Zn0.15	Al	0.85	Zn	0.15																					1967																																														K																																																																																																																TRANS.MET.SOC.AIME,239(1967)891	G.A.BESKE,J.WULFF,P.HILSCH		
100208	435		Al0.9922Zn0.008	Al0.992Zn0.008	Al	0.992	Zn	0.008																					1963																																														K		1.132					1.132																																																																																																									PHYS.LETT.,5(1963)30	B.B.GOODMAN,R.GEISER		
100209	1372		Al2Yb1	Al2Yb1	Al	2	Yb	1																					1972																												MgCu2(Laves)																	MgCu2, C15	K					0.06																																																																																																											J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
100210	715		Al3Yb1	Al3Yb1	Al	3	Yb	1																					1970																												AuCu3																	AuCu3, L1[2]	K		0.94					0.94																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100211	659		Al1 y3	Al1Y3	Al	1	Y	3																																																																			K					1.1																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
100212	711		Al1Y2	Al1Y2	Al	1	Y	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100213	711		Al1Y1	Al1Y1	Al	1	Y	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100214	711		Al2Y3	Al2Y3	Al	2	Y	3																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100215	127		Al2Y1	Al2Y1	Al	2	Y	1																					1959																												MgCu2(Laves)																	MgCu2, C15	K					0.34																																																																																																											ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
100216	427		Al5Y2	Al5Y2	Al	5	Y	2																					1962																																														K					1.55																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100217	2		As2Cu1	As2Cu1	As	2	Cu	1																					1948																																														K					1.57																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
100218	262		As1Co1	As1Co1	As	1	Co	1																																																	MnP																	MnP, B31	K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
100219	262		As2Co1	As2Co1	As	2	Co	1																																																	FeS2(marcasite)																	FeS2, C18	K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
100220	865	prepared under  60 kbar	As2Cd1Sn1	As2Cd1Sn1	As	2	Cd	1	Sn	1																			1969																												NaCl																	NaCl, B1	K		2.29					2.29																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)1609	H.KATZMAN,H.L.LUO,J.G.HUBER,T.DONOHUE,W.F.LIBBY		
100221	867	P of 60-70 kbar	As2Cd1Ge1	As2Cd1Ge1	As	2	Cd	1	Ge	1																			1969																																													tetragonal	K		3.02					3.02																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)2794	H.KATZMAN,H.L.LUO,T.DONOHUE,W.F.LIBBY		
100222	111		As1Bi1Pb1Sb1	As1Bi1Pb1Sb1	As	1	Bi	1	Pb	1	Sb	1																	1930																																														K		9					9																																																																																																									ROY.SOC.CAN.TRANS.,24(1930)53	J.C.MCLENNAN,J.O.WILHELM,L.F.ALLEN		
100223	111		As1Bi1Pb1	As1Bi1Pb1	As	1	Bi	1	Pb	1																			1930																																														K		9					9																																																																																																									ROY.SOC.CAN.TRANS.,24(1930)53	J.C.MCLENNAN,J.O.WILHELM,L.F.ALLEN		
100224	1982		As0.15Bi0.15Nb3Sn0.7	As0.15Bi0.15Nb3Sn0.7	As	0.15	Bi	0.15	Nb	3	Sn	0.7																	1964																																														K		18.07					18.07																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100225	99	eutectic 	As1Au1	As1Au1	As	1	Au	1																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100226	1504		Am0.01Si2Th1	Am0.01Si2Th1	Am	0.01	Si	2	Th	1																			1973																																														K		2.66					2.66																																																																																																									PHYS.LETT.A,43(1973)205	C.E.OLSEN		
100227	RMP0350001		Al1Zr3	Al1Zr3	Al	1	Zr	3																					1963																												AuCu3																	AuCu3, L1[2]	K		0.73					0.73																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100228	RMP0350001		Al2Zr1	Al2Zr1	Al	2	Zr	1																					1963																												MgZn2(Laves)																	MgZn2, C14	K		0.35					0.35																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100229	1583		As1Hf1	As1Hf1	As	1	Hf	1																					1968																												TiAs																	TiAs, B[i]	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100230	1583		As2Hf1	As2Hf1	As	2	Hf	1																					1968																												Co2Si																	Co2Si, C23	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100231	1508		As1Ge1W1	As1Ge1W1	As	1	Ge	1	W	1																			1972																																													monoclinic	K					0.035																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100232	1508		As1Ge1Re1	As1Ge1Re1	As	1	Ge	1	Re	1																			1972																																													monoclinic	K					0.33																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100233	1508		As1Ge1Mo1	As1Ge1Mo1	As	1	Ge	1	Mo	1																			1972																																													monoclinic	K					0.035																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100234	891	prepared at high-P and high-T	As1Ge1	As1Ge1	As	1	Ge	1																					1970																																														K		3.5					3.5																																																																																																									SOLID STATE CHEM.,1(1970)143	H.S.YOUNG,P.C.DONOHUE		
100235	1982		As0.15Ga0.15Nb3Sn0.7	As0.15Ga0.15Nb3Sn0.7	As	0.15	Ga	0.15	Nb	3	Sn	0.7																	1964																																														K		18.01					18.01																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100236	1730	P-induced SC.  P<cr> = 260 kbar.	As1Ga1	As1Ga1	As	1	Ga	1																					1971																																														K		4.8			0		4.8																																																																																																									ZH.ETF PIS.RED.,14(1971)18	I.V.BERMAN,N.B.BRANDT,V.I.SIDOROV		
100237	84		As0.4Fe0.6	As0.4Fe0.6	As	0.4	Fe	0.6																					1933																																														K					1.3																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100238	RMP0350001		As4Cu18Sb3	As4Cu18Sb3	As	4	Cu	18	Sb	3																			1963																																													cubic	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100239	11		As1Cu3	As1Cu3	As	1	Cu	3																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100240	99	eutectic	As1Cu1	As1Cu1	As	1	Cu	1																					1930																																														K					2.2																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100241	85	eutectic	As1Pb1	As1Pb1	As	1	Pb	1																					1932																																														K		8.4					8.4																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100242	1582		As1Os1	As1Os1	As	1	Os	1																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
100243	11		As1Ni1	As1Ni1	As	1	Ni	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100244	1982		As0.15Nb3Sn0.7Tl0.15	As0.15Nb3Sn0.7Tl0.15	As	0.15	Nb	3	Sn	0.7	Tl	0.15																	1964																																														K		17.98					17.98																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100245	1982	sintered	As0.15Nb3Sn0.85	As0.15Nb3Sn0.85	As	0.15	Nb	3	Sn	0.85																			1964																																														K		17.98					17.98																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100246	1982		As0.15Nb3Pb0.15Sn0.7	As0.15Nb3Pb0.15Sn0.7	As	0.15	Nb	3	Pb	0.15	Sn	0.7																	1964																																														K		18.05					18.05																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100247	1508		As2Nb1	As2Nb1	As	2	Nb	1																					1972																																													monoclinic	K					0.012																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100248	1583		As3Mo1	As3Mo1	As	3	Mo	1																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100249	1508		As2Mo1	As2Mo1	As	2	Mo	1																					1972																																													monoclinic	K		0.41					0.41																																																																																																									J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100250	491		As1Ir2	As1Ir2	As	1	Ir	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100251	491		As1Ir1	As1Ir1	As	1	Ir	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100252	1982		As0.15In0.15Nb3Sn0.7	As0.15In0.15Nb3Sn0.7	As	0.15	In	0.15	Nb	3	Sn	0.7																	1964																																														K		17.99					17.99																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100253	491		As3Pt2	As3Pt2	As	3	Pt	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100254	491		As2Pt1	As2Pt1	As	2	Pt	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100255	413		As1Pd1Se1	As1Pd1Se1	As	1	Pd	1	Se	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.2																																																																																																											PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
100256	530		As1Pd7	As1Pd7	As	1	Pd	7																					1963																																														K					1.1																																																																																																											J.LESS-COMMON METALS,5(1963)271	CH.J.RAUB,G.W.WEBB		
100257	262		As3Pd5	As3Pd5	As	3	Pd	5																																																																			K					1.9																																																																																																							From Roberts' Table				Unpublished	C.Raub		
100258	427		As2Pd3	As2Pd3	As	2	Pd	3																					1962																																														K					1.4																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100259	530		As2Pd1	As2Pd1	As	2	Pd	1																					1963																																														K					1.1																																																																																																											J.LESS-COMMON METALS,5(1963)271	CH.J.RAUB,G.W.WEBB		
100260	491		As2Pd5	As2Pd5	As	2	Pd	5																					1963																																														K		0.46					0.46																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100261	530		As1Pd3	As1Pd3	As	1	Pd	3																					1963																												Ni3P																	Ni3P, D0[e]	K					0.3																																																																																																											J.LESS-COMMON METALS,5(1963)271	CH.J.RAUB,G.W.WEBB		
100262	491		As1Pd2	As1Pd2	As	1	Pd	2																					1963																															A	9.79		6.62											hexagonal	K		0.6					0.6																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100263	491		As1Pd2	As1Pd2	As	1	Pd	2																					1963																												Fe2P			A	6.65		3.58											Fe2P, C22	K		1.7					1.7																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100264	35		As1Pd1	As1Pd1	As	1	Pd	1																					1954																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.02																																																																																																							Superconducting compounds				Phys.Rev., 93(1954)1415	B.T.Matthias,E.Corenzwit,C.F.Miller		
100265	1583		As2Th1	As2Th1	As	2	Th	1																					1968																												Co2Si																	Co2Si, C23	K					1.2																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100266	1584		As7Tc3	As7Tc3	As	7	Tc	3																					1968																												Ge7Ir3																	Ge7Ir3, D8[f]	K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
100267	1508		As2Ta1	As2Ta1	As	2	Ta	1																					1972																																													monoclinic	K					0.035																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100268	85	eutectic	As1Sn1	As1Sn1	As	1	Sn	1																					1932																																														K		4.1					4.1																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100269	1219		As0.25Se0.75Y1	As0.25Se0.75Y1	As	0.25	Se	0.75	Y	1																			1970																												NaCl																	NaCl, B1	K		0.78					0.78																																																																																																									SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
100270	84		As0.26Sb0.74	As0.26Sb0.74	As	0.26	Sb	0.74																					1933																																														K					1.32																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100271	491		As1Ru2	As1Ru2	As	1	Ru	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100272	491		As1Ru1	As1Ru1	As	1	Ru	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100273	1583		As1Rh2	As1Rh2	As	1	Rh	2																					1968																												CaF2																	CaF2, C1	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100274	262		As3Rh5	As3Rh5	As	3	Rh	5																																																																			K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
100275	491		As1Rh1	As1Rh1	As	1	Rh	1																					1963																												MnP			A	5.62	3.58	6											MnP, B31	K		0.58					0.58																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100276	1584		As7Re3	As7Re3	As	7	Re	3																					1968																												Ge7Ir3																	Ge7Ir3, D8[f]	K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
100277	1830		Au1	Au1	Au	1																							1974																												Cu																	Cu, A1	K					0.002																																																																																																											J.LOW TEMP.PHYS.,16(1974)409	R.A.BUHRMAN,W.P.HALPERIN		
100278	1583		As1Zr1	As1Zr1	As	1	Zr	1																					1968																												TiAs																	TiAs, B[i]	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100279	1583		As2Zr1	As2Zr1	As	2	Zr	1																					1968																												Co2Si																	Co2Si, C23	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100280	427		As1Zn1	As1Zn1	As	1	Zn	1																					1962																																														K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100281	1584		As1Y1	As1Y1	As	1	Y	1																					1968																												TiAs																	TiAs, B[i]	K					0.31																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
100282	427		As1W1	As1W1	As	1	W	1																					1962																																														K					1.4																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100283	1583		As3W2	As3W2	As	3	W	2																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100284	1508		As2W1	As2W1	As	2	W	1																					1972																																													monoclinic	K		0.9					0.9																																																																																																									J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100285	1508		As2V1	As2V1	As	2	V	1																					1972																																													monoclinic	K					0.33																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
100286	1578		As1V3	As1V3	As	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K					1																																																																																																											FIZ.TVERDOGO TELA.,15(1973)1312	V.N.BOGOMOLOV		
100287	1584		As1Ti1	As1Ti1	As	1	Ti	1																					1968																												TiAs																	TiAs, B[i]	K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
100288	1583		As2Ti1	As2Ti1	As	2	Ti	1																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
100289	486		Au1Ga1	Au1Ga1	Au	1	Ga	1																					1965																												MnP																	MnP, B31	K		1.2					1.2																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100290	76		Au0.5Cu0.5	Au0.5Cu0.5	Au	0.5	Cu	0.5																					1930																																														K					1.11																																																																																																											Z.Phys., 64(1930)581	W.Meissner		
100291	76		Au0.25Cu0.75	Au0.25Cu0.75	Au	0.25	Cu	0.75																					1930																																														K					1.11																																																																																																											Z.Phys., 64(1930)581	W.Meissner		
100292	84		Au5Cd8	Au5Cd8	Au	5	Cd	8																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100293	486		Au5Ca1	Au5Ca1	Au	5	Ca	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		0.34					0.34																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100294	870		Au0.1C1.3Y0.9	Au0.1C1.3Y0.9	Au	0.1	C	1.3	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		10.1					10.1																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100295	281		Au2Bi1	Au2Bi1	Au	2	Bi	1																					1932																												MgCu2(Laves)																	MgCu2, C15	K		1.84					1.84																																																																																																									PROC.ACAD.SCI.AMSTERDAM,35(1932)748	T.JURREAANSE,W.J.DEHAAS		
100296	1057		Au1Be1	Au1Be1	Au	1	Be	1																					1967																																														K		0.91					0.91																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100297	RMP0350001		Au1Be5	Au1Be5	Au	1	Be	5																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100298	138		Au1Be1	Au1Be1	Au	1	Be	1																					1959																												FeSi																	FeSi, B20	K		2.64					2.64																																																																																																									J.PHYS.AND CHEM.OF SOLIDS,10(1959)342	B.T.MATTHIAS		
100299	486		Au5Ba1	Au5Ba1	Au	5	Ba	1																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K		0.4					0.4																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100300	767		Au0.285Mo1.8	Au0.2B5Mo1.8	Au	0.2	B	5	Mo	1.8																			1970																												AlB2																	AlB2, C32	K		4.5					4.5																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100301	394		Au5K1	Au5K1	Au	5	K	1																					1964																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.32																																																																																																											Z.ANORG.ALLG.CHEM.,332(1964)5	CH.J.RAUB,V.B.COMPTON		
100302	866		Au0.9In2Pd0.1	Au0.9In2Pd0.1	Au	0.9	In	2	Pd	0.1																			1969																																														K					0.36																																																																																																											J.PHYS.CHEM.SOLIDS,30(1969)1949	A.MENTH,G.HULL,J.H.WERNICK,J.P.MAITA,T.H.GEBALLE		
100303	486		Au1In1	Au1In1	Au	1	In	1																					1965																																														K		0.6					0.6																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100304	1863		Au1In2	Au1In2	Au	1	In	2																					1973																												CaF2																	CaF2, C1	K		0.22					0.22																																																																																																									REV.SCI.INSTRUM.,44(1973)1186	J.H.WERNICK,K.ANDRES		
100305	1617		Au0.88In0.12	Au0.88In0.12	Au	0.88	In	0.12																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
100306	84		Au0.75Hg0.25	Au0.75Hg0.25	Au	0.75	Hg	0.25																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100307	1867	deposited at 4K	Au0.41Ge0.59	Au0.41Ge0.59	Au	0.41	Ge	0.59																					1974																																														K		2.2					2.2																																																																																																									J.DE PHYS.(PARIS),35(1974)261	D.KORN,G.ZIBOLD,W.MURER		
100308	1179	deposited at 4K	Au0.5Ge0.5	Au0.5Ge0.5	Au	0.5	Ge	0.5																					1971																																														K		3.6					3.6																																																																																																									LT-12, Tokyo (1971) 339	B.Stritzker,H.Wuhl		
100309	908	laser pulse preparation	Au1Ge1	Au1Ge1	Au	1	Ge	1																					1970																																														K		2.7					2.7																																																																																																									ZH.ETF PIS.RED., 12(1970)228	N.E.ALEKSEEVSKII,V.I.TSEBEO,V.M.ZAKOSARENKO		
100310	908		Au1Ge1	Au1Ge1	Au	1	Ge	1																					1970																																														K					1.4																																																																																																											ZH.ETF PIS.RED., 12(1970)228	N.E.ALEKSEEVSKII,V.I.TSEBEO,V.M.ZAKOSARENKO		
100311	1534	P=6 kbar	Au1Ga2	Au1Ga2	Au	1	Ga	2																					1972																																														K		1.9					1.9																																																																																																									PHYS.REV.LETT.,28(1972)1127	J.E.SCHIRBER		
100312	866		Au1Ga2	Au1Ga2	Au	1	Ga	2																					1969																												CaF2																	CaF2, C1	K		1.12			0.34		1.12																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)1949	A.MENTH,G.HULL,J.H.WERNICK,J.P.MAITA,T.H.GEBALLE		
100313	1438	sputtered film, d=10,000A	Au0.25Nb0.75	Au0.25Nb0.75	Au	0.25	Nb	0.75																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		11.2					11.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
100314	568		Au1Nb3	Au1Nb3	Au	1	Nb	3																					1964																												W																	W, A2	K		1.2					1.2																																																																																																									PHYS.LETT.,8(1964)27	E.BUCHER,F.LAVES,H.VON PHILIPSBORN,J.MULLER		
100315	492		Au1Nb3	Au1Nb3	Au	1	Nb	3																					1965																												Cr3Si(A15)																	Cr3Si, A15	K		11.5					11.5																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
100316	1466		Au1Nb3	Au1Nb3	Au	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		11.22					11.22																																																																																																									J.JAPAN INST.METALS,37(1973)558	K.TACHIKAWA,Y.YOSHIDA		
100317	1377		Au1Na2	Au1Na2	Au	1	Na	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100318	RMP0350001		Au2Na1	Au2Na1	Au	2	Na	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.34																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100319	RMP0350001		Au1Mg1	Au1Mg1	Au	1	Mg	1																					1963																												CsCl																	CsCl, B2	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100320	658		Au1Lu1	Au1Lu1	Au	1	Lu	1																					1967																												CsCl																	CsCl, B2	K					0.35																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100321	1908	rapid quench	Au0.22La0.78	Au0.22La0.78	Au	0.22	La	0.78																					1975																																														K		3.4					3.4																																																																																																									PHYS.REV.B,11(1975)150	P.DUWEZ,S.J.POON,W.L.JOHNSON		
100322	1908	rapid quench	Au0.24La0.76	Au0.24La0.76	Au	0.24	La	0.76																					1975																																														K		4					4																																																																																																									PHYS.REV.B,11(1975)150	P.DUWEZ,S.J.POON,W.L.JOHNSON		
100323	1908		Au0.33La0.67	Au0.33La0.67	Au	0.33	La	0.67																					1975																																														K		3.2					3.2																																																																																																									PHYS.REV.B,11(1975)150	P.DUWEZ,S.J.POON,W.L.JOHNSON		
100324	658		Au1La1	Au1La1	Au	1	La	1																					1967																																														K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100325	229		Au0.2Sn0.8	Au0.2Sn0.8	Au	0.2	Sn	0.8																					1962																																													orthorhombic	K		2.38					2.38																																																																																																									J.PHYS.CHEM.SOLIDS,23(1962)405	M.F.GENDRON,R.E.JONES		
100326	486		Au1Sn1	Au1Sn1	Au	1	Sn	1																					1965																												NiAs																	NiAs, B8[1]	K		1.25					1.25																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100327	486		Au5Sn1	Au5Sn1	Au	5	Sn	1																					1965																												Mg																	Mg, A3	K		1.1					1.1																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100328	RMP0350001		Au1Sb2	Au1Sb2	Au	1	Sb	2																					1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		0.58					0.58																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100329	1060		Au0.5Rh0.4Ti0.91	Au0.5Rh0.4Ti0.91	Au	0.5	Rh	0.4	Ti	0.91																			1964																																														K		3					3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
100330	1116	rapid quench	Au0.167Pd0.166Te0.66	Au0.167Pd0.166Te0.667	Au	0.167	Pd	0.166	Te	0.667																			1971																																													cubic	K		4.6					4.6																																																																																																									PHYS.LETT.A,34(1971)80	C.C.TSUEI,H.YEN,P.DUWEZ		
100331	1116	rapid quench	Au0.3Pd0.033Te0.666	Au0.3Pd0.033Te0.666	Au	0.3	Pd	0.033	Te	0.666																			1971																																													cubic	K		2.6					2.6																																																																																																									PHYS.LETT.A,34(1971)80	C.C.TSUEI,H.YEN,P.DUWEZ		
100332	866		Au0.95Pd0.5Ga2	Au0.95Pd0.5Ga2	Au	0.95	Pd	0.5	Ga	2																			1969																												CaF2																	CaF2, C1	K		1.75					1.75																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)1949	A.MENTH,G.HULL,J.H.WERNICK,J.P.MAITA,T.H.GEBALLE		
100333	521		Au1Pb3	Au1Pb3	Au	1	Pb	3																					1964																																														K		4.4					4.4																																																																																																									PHYS.LETT.,10(1964)44	H.L.CASWELL		
100334	1377		Au1Pb2	Au1Pb2	Au	1	Pb	2																					1972																												CuAl2																	CuAl2, C16	K		3.1					3.1																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100335	486		Au2Pb1	Au2Pb1	Au	2	Pb	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		1.18					1.18																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100336	922		Au0.7Nb3Pt0.3	Au0.7Nb3Pt0.3	Au	0.7	Nb	3	Pt	0.3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5																																																																																																									PHYS.LETT.A,30(1969)170	F.HEINIGER,J.MULLER,P.SPITZLI,R.FLUKIGER		
100337	RMP0350001		Au1Zr3	Au1Zr3	Au	1	Zr	3																					1963																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100338	RMP0350001		Au1Zr3	Au1Zr3	Au	1	Zr	3																					1963																												Cr3Si(A15)																	Cr3Si, A15	K		0.92					0.92																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100339	84		Au5Zn8	Au5Zn8	Au	5	Zn	8																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100340	RMP0350001		Au1Zn3	Au1Zn3	Au	1	Zn	3																					1963																																														K		1.21					1.21																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100341	1617		Au0.85Zn0.15	Au0.85Zn0.15	Au	0.85	Zn	0.15																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
100342	707	levitation method	Au0.23V0.77	Au0.23V0.77	Au	0.23	V	0.77																					1969																																														K		0.66					0.66																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
100343	85	eutectec 	Au1Tl1	Au1Tl1	Au	1	Tl	1																					1932																																														K		1.92					1.92																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100344	70		Au0.27Tl0.73	Au0.27Tl0.73	Au	0.27	Tl	0.73																					1929																																														K		2.04					2.04																																																																																																									Proc.Acad.Sci.Amsterdam, 32(1929)715	W.J.DeHaas,E. Van Aubel,J.Voogd		
100345	1959		Au1Tl2	Au1Tl2	Au	1	Tl	2																					1974																												CuAl2																	CuAl2, C16	K		4.25					4.25																																																																																																					From Roberts' Table. Private communication				Unpublished. personal commun.	H.L.Luo		
100346	1377		Au1Th2	Au1Th2	Au	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K		3.65					3.65																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100347	487		Au3Te5	Au3Te5	Au	3	Te	5																					1964																																														K		1.62					1.62																																																																																																									SCIENCE,145(1964)581	D.C.HAMILTON,H.L.LUO,M.F.MERRIAM		
100348	1015		Au1Ta4.3	Au1Ta4.3	Au	1	Ta	4.3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		0.51					0.51																																																																																																									Z.PHYS.,230(1970)443	E.CORENZWIT,E.VIELHABER,H.L.LUO		
100349	1014		B6Dy0.01Y0.99	B6Dy0.01Y0.99	B	6	Dy	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100350	705		B6Dy1	B6Dy1	B	6	Dy	1																					1968																																														K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100351	10		Cr2B1	B1Cr2	B	1	Cr	2																					1954																												CuAl2																	CuAl2, C16	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100352	11		B1Cr1	B1Cr1	B	1	Cr	1																					1952																												CrB																	CrB, B[f]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100353	11		B2Cr1	B2Cr1	B	2	Cr	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100354	1377		B1Co2	B1Co2	B	1	Co	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100355	1014		B6Ce0.01Y0.99	B6Ce0.01Y0.99	B	6	Ce	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100356	705		B6Ce1	B6Ce1	B	6	Ce	1																					1968																												CaB6																	CaB6, D2[1]	K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100357	558		B6Ca1	B6Ca1	B	6	Ca	1																																																	CaB6																	CaB6, D2[1]	K					1.28																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100358	966		B1C1Mo2	B1C1Mo2	B	1	C	1	Mo	2																			1968																																													orthorhombic	K		7.1					7.1																																																																																																									ACTA MET.,16(1968)1177	J.ZBASNIK,L.E.TOTH		
100359	11		B4C1	B4C1	B	4	C	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100360	11		B0.86Ba0.14	B0.86Ba0.14	B	0.86	Ba	0.14																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100361	1014		B6Ho0.01Y0.99	B6Ho0.01Y0.99	B	6	Ho	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100362	705		B12Ho1	B12Ho1	B	12	Ho	1																					1968																																														K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100363	705		B6Ho1	B6Ho1	B	6	Ho	1																					1968																																														K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100364	767		B5Hf0.2Nb1.8	B5Hf0.2Nb1.8	B	5	Hf	0.2	Nb	1.8																			1970																												AlB2																	AlB2, C32	K		3.6					3.6																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100365	767		B5Hf0.2Mo1.8	B5Hf0.2Mo1.8	B	5	Hf	0.2	Mo	1.8																			1970																												AlB2																	AlB2, C32	K		8.4					8.4																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100366	1815		B1Hf1	B1Hf1	B	1	Hf	1																					1967																												NaCl																	NaCl, B1	K		3.1					3.1																																																																																																									ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100367	705		B6Gd1	B6Gd1	B	6	Gd	1																					1968																												CaB6																	CaB6, D2[1]	K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100368	1377		B1Fe2	B1Fe2	B	1	Fe	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100369	1014		B6Eu0.01Y0.99	B6Eu0.01Y0.99	B	6	Eu	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100370	705		B6Eu1	B6Eu1	B	6	Eu	1																					1968																												CaB6																	CaB6, D2[1]	K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100371	1014		B6Er0.01Y0.09	B6Er0.01Y0.99	B	6	Er	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100372	705		B12Er1	B12Er1	B	12	Er	1																					1968																																														K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100373	767		B5Mo1.7Nb0.3	B5Mo1.7Nb0.3	B	5	Mo	1.7	Nb	0.3																			1970																												AlB2																	AlB2, C32	K		8.3					8.3																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100374	767		B5Mo0.2Nb1.8	B5Mo0.2Nb1.8	B	5	Mo	0.2	Nb	1.8																			1970																												AlB2																	AlB2, C32	K		4.3					4.3																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100375	1105		B1Mo2	B1Mo2	B	1	Mo	2																					1967																												CuAl2																	CuAl2, C16	K		5.85					5.85																																																																																																									SCI.,155(1967)191	B.T.MATTHIAS,G.W.WEBB,J.J.ENGLEHARDT		
100376	11		B1Mo1	B1Mo1	B	1	Mo	1																					1952																												MoB																	MoB, B[g]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100377	11		B1Mo1	B1Mo1	B	1	Mo	1																					1952																												CrB																	CrB, B[f]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100378	767		B2Mo1	B2Mo1	B	2	Mo	1																					1970																												AlB2																	AlB2, C32	K					1																																																																																																											PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100379	11		B0.72Mo0.28	B0.72Mo0.28	B	0.72	Mo	0.28																					1952																												Mo2B5																	Mo2B5, D8[i]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100380	767		B2.5Mo1	B2.5Mo1	B	2.5	Mo	1																					1970																												AlB2																	AlB2, C32	K		7.45					7.45																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100381	1377		B1Mn2	B1Mn2	B	1	Mn	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100382	705		B12Lu1	B12Lu1	B	12	Lu	1																					1968																																														K		0.48					0.48																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100383	1815		B6La1	B6La1	B	6	La	1																					1967																												CaB6																	CaB6, D2[1]	K					1.3																																																																																																											ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100384	11		B1Ir1	B1Ir1	B	1	Ir	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100385	767		B2.5Nb1	B2.5Nb1	B	2.5	Nb	1																					1970																												AlB2																	AlB2, C32	K		6.4					6.4																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100386	11		B1N1	B1N1	B	1	N	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100387	767		B5Mo1.69Zr0.31	B5Mo1.69Zr0.31	B	5	Mo	1.69	Zr	0.31																			1970																												AlB2																	AlB2, C32	K		11.2					11.2																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100388	767		B5Mo1.9Zr0.1	B5Mo1.9Zr0.1	B	5	Mo	1.9	Zr	0.1																			1970																												AlB2																	AlB2, C32	K		8.9					8.9																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100389	767		B5Mo1.9Y0.1	B5Mo1.9Y0.1	B	5	Mo	1.9	Y	0.1																			1970																												AlB2																	AlB2, C32	K		8					8																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100390	767		B5Mo1.7V0.3	B5Mo1.7V0.3	B	5	Mo	1.7	V	0.3																			1970																												AlB2																	AlB2, C32	K		5.5					5.5																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100391	767		B5Mo1.7Ti0.3	B5Mo1.7Ti0.3	B	5	Mo	1.7	Ti	0.3																			1970																												AlB2																	AlB2, C32	K		7.1					7.1																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100392	767		B5Mo1.7Ta0.3	B5Mo1.7Ta0.3	B	5	Mo	1.7	Ta	0.3																			1970																												AlB2																	AlB2, C32	K		7					7																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100393	1377		B1Mo1.75Ta0.25	B1Mo1.75Ta0.25	B	1	Mo	1.75	Ta	0.25																			1972																												CuAl2																	CuAl2, C16	K		3.05					3.05																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100394	1377		B1Mo1.5Ta0.5	B1Mo1.5Ta0.5	B	1	Mo	1.5	Ta	0.5																			1972																												CuAl2																	CuAl2, C16	K		1.81					1.81																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100395	767		B5Mo1.8Sc0.2	B5Mo1.8Sc0.2	B	5	Mo	1.8	Sc	0.2																			1970																												AlB2																	AlB2, C32	K		8.8					8.8																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100396	1309		B3Mo6S8Sn1	B3Mo6S8Sn1	B	3	Mo	6	S	8	Sn	1																	1973																																														K		15					15																																																																																																									MAT.RES.BULL.,8(1973)657	B.T.MATTHIAS,E.CORENZWIT,J.P.REMEIKA,M.MAREZIO,P.D.DERNIER		
100397	767		B5Nb1.8Zr0.2	B5Nb1.8Zr0.2	B	5	Nb	1.8	Zr	0.2																			1970																												AlB2																	AlB2, C32	K		5.9					5.9																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100398	767		B5Nb1.9Y0.1	B5Nb1.9Y0.1	B	5	Nb	1.9	Y	0.1																			1970																												AlB2																	AlB2, C32	K		9.3					9.3																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100399	767		B5nb1.8V0.2	B5Nb1.8V0.2	B	5	Nb	1.8	V	0.2																			1970																												AlB2																	AlB2, C32	K		2.5					2.5																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100400	767		B5Nb1.9Ti0.1	B5Nb1.9Ti0.1	B	5	Nb	1.9	Ti	0.1																			1970																												AlB2																	AlB2, C32	K		4					4																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100401	767		B5Nb1.8Th0.2	B5Nb1.8Th0.2	B	5	Nb	1.8	Th	0.2																			1970																												AlB2																	AlB2, C32	K		7					7																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100402	767		B5Nb1.9Sc0.1	B5Nb1.9Sc0.1	B	5	Nb	1.9	Sc	0.1																			1970																												AlB2																	AlB2, C32	K		6.6					6.6																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100403	767		B5Nb1.8Ru0.2	B5Nb1.8Ru0.2	B	5	Nb	1.8	Ru	0.2																			1970																												AlB2																	AlB2, C32	K		6					6																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100404	1951		B2Nb1	B2Nb1	B	2	Nb	1																					1967																																														K																																																																																																																TOHOKU UNIVN.RES.INST.SCI.REPTS.SER.A,18(1967)413	E.KANDA,K.UKEI		
100405	927		B2Nb3	B2Nb3	B	2	Nb	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100406	11		B0.57Nb0.43	B0.57Nb0.43	B	0.57	Nb	0.43																					1952																												Ta3B4																	Ta3B4, D7[b]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100407	11		B1Nb1	B1Nb1	B	1	Nb	1																					1952																												CrB																	CrB, B[f]	K		8.25					8.25																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100408	767		B2Nb1	B2Nb1	B	2	Nb	1																					1970																												AlB2																	AlB2, C32	K					1																																																																																																											PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100409	173		B3Ru7	B3Ru7	B	3	Ru	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		2.58					2.58																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
100410	RMP0350001		B3Rh7	B3Rh7	B	3	Rh	7																					1963																												Fe3Th7																	Fe3Th7, D10[2]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100411	141		B1Rh2	B1Rh2	B	1	Rh	2																					1955																																													orthorhombic	K					1																																																																																																											ACTA CRYST.,8(1955)15	S.GELLER		
100412	11		B1Rh1	B1Rh1	B	1	Rh	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100413	465		B1Re2	B1Re2	B	1	Re	2																					1963																																														K		4.6					4.6																																																																																																					SPECIFIC HEATS TRANSITION METAL SUPERCONDUCTORS				PHYS.REV.,129(1963)1115	F.J.MOORIN,J.P.MAITA		
100414	11		B1Pt1	B1Pt1	B	1	Pt	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100415	1014		B6Pr0.01Y0.99	B6Pr0.01Y0.99	B	6	Pr	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100416	705		B6Pr1	B6Pr1	B	6	Pr	1																					1968																												CaB6																	CaB6, D2[1]	K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100417	RMP0350001		B2Os1	B2Os1	B	2	Os	1																					1963																												AlB2																	AlB2, C32	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100418	1377		B1Ni2	B1Ni2	B	1	Ni	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100419	1014		B0.006Nd0.01Y0.99	B0.006Nd0.01Y0.99	B	0.006	Nd	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100420	705		B6nd1	B6Nd1	B	6	Nd	1																					1968																												CaB6																	CaB6, D2[1]	K		3			0.35		3																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100421	1377		B1Ta1.25W0.75	B1Ta1.25W0.75	B	1	Ta	1.25	W	0.75																			1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100422	927		B2Ta3	B2Ta3	B	2	Ta	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100423	1377		B1Ta2	B1Ta2	B	1	Ta	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100424	1815		B1Ta1	B1Ta1	B	1	Ta	1																					1967																												CrB																	CrB, B[f]	K		4					4																																																																																																									ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100425	11		B4Ta3	B4Ta3	B	4	Ta	3																					1952																												Ta3B4																	Ta3B4, D7[b]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100426	11		B2Ta1	B2Ta1	B	2	Ta	1																					1952																												AlB2																	AlB2, C32	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100427	1014		B6Sm0.01Y0.99	B6Sm0.01Y0.99	B	6	Sm	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100428	1815		B6Sm1	B6Sm1	B	6	Sm	1																					1967																												CaB6																	CaB6, D2[1]	K					1.28																																																																																																											ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100429	1815		B2Sc1	B2Sc1	B	2	Sc	1																					1967																												AlB2																	AlB2, C32	K					1.3																																																																																																											ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100430	1815		B4Sc1	B4Sc1	B	4	Sc	1																					1967																																													hexagonal	K					1.34																																																																																																											ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100431	705		B12Sc1	B12Sc1	B	12	Sc	1																					1968																																														K		0.39					0.39																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100432	10		B1Ru2	B1Ru2	B	1	Ru	2																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100433	10		B1V2	B1V2	B	1	V	2																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100434	10		B1V1	B1V1	B	1	V	1																					1954																												CrB																	CrB, B[f]	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100435	1014		B6Tm0.01Y0.99	B6Tm0.01Y0.99	B	6	Tm	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100436	705		B12Tm1	B12Tm1	B	12	Tm	1																					1968																																														K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100437	10		B1Ti1	B1Ti1	B	1	Ti	1																					1954																												FeB																	FeB, B27	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100438	11		B2Ti1	B2Ti1	B	2	Ti	1																					1952																												AlB2																	AlB2, C32	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100439	10		B1Th1	B1Th1	B	1	Th	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100440	40		B2Th1	B2Th1	B	2	Th	1																					1953																																														K					1.77																																																																																																							Studies of compounds for superconductivity				Phys.Rev., 90(1953)115	W.T.Ziegler,R.A.Young		
100441	705		B6Th1	B6Th1	B	6	Th	1																					1968																																														K		0.74					0.74																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100442	1014		B6Tb0.01Y0.99	B6Tb0.01Y0.99	B	6	Tb	0.01	Y	0.99																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100443	705		B6Tb1	B6Tb1	B	6	Tb	1																					1968																												CaB6																	CaB6, D2[1]	K					0.35																																																																																																											SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100444	1377		B1Ta1.5W0.5	B1Ta1.5W0.5	B	1	Ta	1.5	W	0.5																			1972																												CuAl2																	CuAl2, C16	K		0.25					0.25																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100445	1815		B1Zr1	B1Zr1	B	1	Zr	1																					1967																												NaCl																	NaCl, B1	K		3.4					3.4																																																																																																									ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
100446	40		B2Zr1	B2Zr1	B	2	Zr	1																					1953																												AlB2																	AlB2, C32	K					1.8																																																																																																							Studies of compounds for superconductivity				Phys.Rev., 90(1953)115	W.T.Ziegler,R.A.Young		
100447	782		B12Zr1	B12Zr1	B	12	Zr	1																					1969																																													cubic	K		6					6																																																																																																									SCIENCE,165(1969)279	B.T.MATTHIAS,Z.FISK		
100448	1014		B12Yb0.01Zr0.99	B12Yb0.01Zr0.99	B	12	Yb	0.01	Zr	0.99																			1969																																														K		4.4					4.4																																																																																																									PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100449	558		B6Yb1	B6Yb1	B	6	Yb	1																																																	CaB6																	CaB6, D2[1]	K					1.28																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100450	1014		B6Y0.99Yb0.01	B6Y0.99Yb0.01	B	6	Y	0.99	Yb	0.01																			1969																																														K																																																																																																																PROC.NAT.ACAD.SCI.,64(1969)1151	B.T.MATTHIAS,E.CORENZWIT,Z.FISK		
100451	705		B6Y1	B6Y1	B	6	Y	1																					1968																												CaB6																	CaB6, D2[1]	K		6.5			1.28		6.5																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100452	705		B12Y1	B12Y1	B	12	Y	1																					1968																																														K		4.7					4.7																																																																																																									SCIENCE,159(1968)530	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,K.ANDRES,T.H.GEBALLE		
100453	1377		B1W2	B1W2	B	1	W	2																					1972																												CuAl2																	CuAl2, C16	K		3.22					3.22																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100454	11		B1W1	B1W1	B	1	W	1																					1952																												MoB																	MoB, B[g]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100455	11		B5W2	B5W2	B	5	W	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100456	927		B2V3	B2V3	B	2	V	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100457	28		Ba1Pd2	Ba1Pd2	Ba	1	Pd	2																					1957																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
100458	1372		Ba0.1Pb3Sr0.9	Ba0.1Pb3Sr0.9	Ba	0.1	Pb	3	Sr	0.9																			1972																																													tetragonal	K		1.75					1.75																																																																																																									J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
100459	644		Ba0.14O3W1	Ba0.14O3W1	Ba	0.14	O	3	W	1																			1966																																													hexagonal	K		2.2					2.2																																																																																																									SOLID STATE COMMUN.,4(1966)25	F.J.DARNELL,P.E.BIERSTEDT,T.A.BITHER		
100460	575		Ba0.13O3W1	Ba0.13O3W1	Ba	0.13	O	3	W	1																			1965																																													tetragonal	K		1.9					1.9																																																																																																									PHYS.LETT.,19(1965)82	A.R.SWEEDLER,B.T.MATTHIAS,J.K.HULM,T.H.GEBALLE		
100461	1232		Ba1Hg1	Ba1Hg1	Ba	1	Hg	1																					1966																												CsCl																	CsCl, B2	K		2.32					2.32																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
100462	715		Ba1Bi3	Ba1Bi3	Ba	1	Bi	3																					1970																																													tetragonal	K		5.8					5.8																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100463	710	quenched film 	Ba1	Ba1	Ba	1																							1975																																														K		3					3																																																																																																									PHYS.LETT.A,51(1975)353	C.REALE		
100464	1702	pressure-induced s/c. Tc=4.5 K at P=148 kbar. dTc/dP = 1.3 E-5 K/bar.	Ba1	Ba1	Ba	1																							1971																																														K		4.5			0		4.5			K/GPa	0.13																																																																																																	Superconductivity of Bismuth, Barium, and Lead at pressures exceeding 100 kbar				ZH.EKSP.TEOR.FIZ.,61(1971)2357, Soviet Physics JETP, 34(1972)1263	E.M.DIZHUR,E.S.ITSKEVICH,M.A.IL'INA		
100465	1702	pressure-induced s/c. Tc=4.7 K at P=168 kbar.	Ba1	Ba1	Ba	1																							1971																																														K		4.7			0		4.7																																																																																																					Superconductivity of Bismuth, Barium, and Lead at pressures exceeding 100 kbar				ZH.EKSP.TEOR.FIZ.,61(1971)2357, Soviet Physics JETP, 34(1972)1263	E.M.DIZHUR,E.S.ITSKEVICH,M.A.IL'INA		
100466	1702	Pressure-induced s/c. Tc=4.9 K at P=175 kbar.	Ba1	Ba1	Ba	1																							1971																																														K		4.9			0		4.9																																																																																																					Superconductivity of Bismuth, Barium, and Lead at pressures exceeding 100 kbar				ZH.EKSP.TEOR.FIZ.,61(1971)2357, Soviet Physics JETP, 34(1972)1263	E.M.DIZHUR,E.S.ITSKEVICH,M.A.IL'INA		
100467	1702	pressure-induced s/c. Tc=5.1 K at P=192 kbar.	Ba1	Ba1	Ba	1																							1971																																														K		5.1			0		5.1																																																																																																					Superconductivity of Bismuth, Barium, and Lead at pressures exceeding 100 kbar				ZH.EKSP.TEOR.FIZ.,61(1971)2357, Soviet Physics JETP, 34(1972)1263	E.M.DIZHUR,E.S.ITSKEVICH,M.A.IL'INA		
100468	1233		Ba1	Ba1	Ba	1																																																			W																	W, A2	K					0.014																																																																																																											QUOTED IN REF.,1232	K.ANDERSON		
100469	1057		Be0.92Cu0.08	Be0.92Cu0.08	Be	0.92	Cu	0.08																					1967																												W																	W, A2	K		0.84					0.84																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100470	427		Be1Cr2	Be1Cr2	Be	1	Cr	2																					1962																												MgZn2(Laves)																	MgZn2, C14	K					1.75																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100471	1769		Be2Cr1	Be2Cr1	Be	2	Cr	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100472	1769		Be12Cr1	Be12Cr1	Be	12	Cr	1																					1973																																													tetragonal	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100473	712		Be5Co1	Be5Co1	Be	5	Co	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100474	1769		Be12Co1	Be12Co1	Be	12	Co	1																					1973																																													tetragonal	K					1.15																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100475	1057		Be21Co5	Be21Co5	Be	21	Co	5																					1967																												Cu5Zn8																	Cu5Zn8, D8[2]	K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100476	1057		Be0.944Co0.056	Be0.944Co0.056	Be	0.944	Co	0.056																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100477	1769		Be13Ce1	Be13Ce1	Be	13	Ce	1																					1973																												NaZn13																	NaZn13, D2[3]	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100478	1769		Be13Ca1	Be13Ca1	Be	13	Ca	1																					1973																												NaZn13																	NaZn13, D2[3]	K					1.38																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100479	28		Ba1Rh2	Ba1Rh2	Ba	1	Rh	2																					1957																												MgCu2(Laves)																	MgCu2, C15	K		6					6																																																																																																					Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
100480	28		Ba1Pt2	Ba1Pt2	Ba	1	Pt	2																					1957																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
100481	1769		Be5Ga1	Be5Ga1	Be	5	Ga	1																					1973																																														K		5.8					5.8																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100482	1769		Be6Ga1	Be6Ga1	Be	6	Ga	1																					1973																																														K		6					6																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100483	1769		Be8Ga1	Be8Ga1	Be	8	Ga	1																					1973																																														K		5.7					5.7																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100484	1769		Be13Ga1	Be13Ga1	Be	13	Ga	1																					1973																																														K		5.6					5.6																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100485	1769		Be22Ga1	Be22Ga1	Be	22	Ga	1																					1973																																														K		5.7					5.7																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100486	1769		Be2Fe1	Be2Fe1	Be	2	Fe	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100487	712		Be11Fe1	Be11Fe1	Be	11	Fe	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100488	1057		Be0.95Fe0.05	Be0.95Fe0.05	Be	0.95	Fe	0.05																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100489	1057		Be0.977Fe0.023	Be0.977Fe0.023	Be	0.977	Fe	0.023																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100490	1769		Be3Cu1	Be3Cu1	Be	3	Cu	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100491	1057		Be0.858Cu0.142	Be0.858Cu0.142	Be	0.858	Cu	0.142																					1967																												W																	W, A2	K		0.56					0.56																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100492	1057		Be0.89Cu0.11	Be0.89Cu0.11	Be	0.89	Cu	0.11																					1967																												W																	W, A2	K		1.11					1.11																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100493	1769		Be12Mg1Re1	Be12Mg1Re1	Be	12	Mg	1	Re	1																			1973																																														K		10.1					10.1																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100494	1769		Be13Mg1	Be13Mg1	Be	13	Mg	1																					1973																												NaZn13																	NaZn13, D2[3]	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100495	1964		Be13Lu1	Be13Lu1	Be	13	Lu	1																					1975																																													cubic	K					0.45																																																																																																											PHYS.REV.,11(1975)40	A.S.COOPER,E.BUCHER,G.W.HULL,J.P.MAITA,R.C.FULTON		
100496	1964		Be13La1	Be13La1	Be	13	La	1																					1975																																													cubic	K					0.45																																																																																																											PHYS.REV.,11(1975)40	A.S.COOPER,E.BUCHER,G.W.HULL,J.P.MAITA,R.C.FULTON		
100497	1769		Be5Ir1	Be5Ir1	Be	5	Ir	1																					1973																																														K		1.5					1.5																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100498	1769		Be13Ir1	Be13Ir1	Be	13	Ir	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100499	1057		Be0.95Ir0.05	Be0.95Ir0.05	Be	0.95	Ir	0.05																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100500	712		Be13Hf1	Be13Hf1	Be	13	Hf	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100501	712		Be17Hf2	Be17Hf2	Be	17	Hf	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100502	1769		Be13Ge1	Be13Ge1	Be	13	Ge	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100503	1769		Be2Ga1	Be2Ga1	Be	2	Ga	1																					1973																																														K		6.3					6.3																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100504	1769		Be3Ga1	Be3Ga1	Be	3	Ga	1																					1973																																														K		6.7					6.7																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100505	1822		Be22Mo0.6Re0.4	Be22Mo0.6Re0.4	Be	22	Mo	0.6	Re	0.4																			1973																																													cubic	K		8.3					8.3																																																																																																									Z.PHYS.,259(1973)307	A.MULLER,W.KLOSE		
100506	1822		Be22Mo0.3Re0.7	Be22Mo0.3Re0.7	Be	22	Mo	0.3	Re	0.7																			1973																																													cubic	K		8.6					8.6																																																																																																									Z.PHYS.,259(1973)307	A.MULLER,W.KLOSE		
100507	1822		Be22Mo0.4Re0.6	Be22Mo0.4Re0.6	Be	22	Mo	0.4	Re	0.6																			1973																																													cubic	K		8.6					8.6																																																																																																									Z.PHYS.,259(1973)307	A.MULLER,W.KLOSE		
100508	712		Be1Mo3	Be1Mo3	Be	1	Mo	3																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100509	1769		Be2Mo1	Be2Mo1	Be	2	Mo	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100510	1909		Be12Mo1	Be12Mo1	Be	12	Mo	1																					1968																																													tetragonal	K					1.38																																																																																																											PHYS.REV.,171(1968)591	N.M.WOLCOTT,R.L.FALGE JR.		
100511	427		Be13Mo1	Be13Mo1	Be	13	Mo	1																					1962																																													tetragonal	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100512	1922		Be22Mo1	Be22Mo1	Be	22	Mo	1																					1973																																													cubic	K		2.545					2.545																																																																																																									UKR.FIZ.ZH.,18(1973)672	A.A.MATSAKOVA,N.M.MATYUSHENKO,N.S.PUSACHEV		
100513	1769		Be2Mn1	Be2Mn1	Be	2	Mn	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100514	1769		Be8Mn1	Be8Mn1	Be	8	Mn	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100515	712		Be12Mn1	Be12Mn1	Be	12	Mn	1																																																																		tetragonal	K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100516	1769		Be13Mn1	Be13Mn1	Be	13	Mn	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100517	1057	arc melted	Be0.96Ni0.04	Be0.96Ni0.04	Be	0.96	Ni	0.04																					1967																																														K		0.76					0.76																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100518	1057	arc melted, slow cool	Be0.934Ni0.066	Be0.934Ni0.066	Be	0.934	Ni	0.066																					1967																																														K		0.88					0.88																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100519	1057	slow cool	Be0.9Ni0.1	Be0.9Ni0.1	Be	0.9	Ni	0.1																					1967																																														K		0.58					0.58																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100520	1057	arc melted	Be0.9Ni0.1	Be0.9Ni0.1	Be	0.9	Ni	0.1																					1967																												W																	W, A2	K		2.38					2.38																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100521	1057	arc melted. slow cool. 	Be21Ni5	Be21Ni5	Be	21	Ni	5																					1967																												Cu5Zn8																	Cu5Zn8, D8[2]	K		0.72					0.72																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100522	427		Be8Nb5Zr2	Be8Nb5Zr2	Be	8	Nb	5	Zr	2																			1962																																														K		5.2					5.2																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100523	927		Be2Nb1.5Ta1.5	Be2Nb1.5Ta1.5	Be	2	Nb	1.5	Ta	1.5																			1969																												Si2U3																		K		1.7					1.7																																																																																																									PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100524	927		Be2Nb3	Be2Nb3	Be	2	Nb	3																					1969																												Si2U3																	tetragonal	K		2.3					2.3																																																																																																									PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100525	712		Be2Nb1	Be2Nb1	Be	2	Nb	1																																																																			K		2.15					2.15																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100526	712		Be3Nb1	Be3Nb1	Be	3	Nb	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100527	1909		Be12Nb1	Be12Nb1	Be	12	Nb	1																					1968																																													tetragonal	K					1.38																																																																																																											PHYS.REV.,171(1968)591	N.M.WOLCOTT,R.L.FALGE JR.		
100528	712		Be17Nb2	Be17Nb2	Be	17	Nb	2																																																																			K		1.47			1.38		1.47																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100529	1769		Be12Pd1	Be12Pd1	Be	12	Pd	1																					1973																																													tetragonal	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100530	1769		Be13Pd1	Be13Pd1	Be	13	Pd	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100531	1057		Be22Pd1	Be22Pd1	Be	22	Pd	1																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100532	1903		Be0.86Pb0.14	Be0.86Pb0.14	Be	0.86	Pb	0.14																					1975																																														K		9.7					9.7																																																																																																									Z.PHYS.B,20(1975)13	C.G.GRANQVIST,T.CLAESON		
100533	1769		Be22Os0.005Re1	Be22Os0.005Re1	Be	22	Os	0.005	Re	1																			1973																																														K		9.8					9.8																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100534	1769		Be0.8Os0.2	Be0.8Os0.2	Be	0.8	Os	0.2																					1973																																														K		8.6					8.6																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100535	1769		Be0.9Os0.1	Be0.9Os0.1	Be	0.9	Os	0.1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100536	1057		Be0.95Os0.05	Be0.95Os0.05	Be	0.95	Os	0.05																					1967																																														K		0.57					0.57																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100537	712		Be2Os1	Be2Os1	Be	2	Os	1																																																																			K		3.07					3.07																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100538	1769		Be5Os1	Be5Os1	Be	5	Os	1																					1973																																														K		9.2					9.2																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100539	1769		Be13Os1	Be13Os1	Be	13	Os	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100540	1769		Be22Os1	Be22Os1	Be	22	Os	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100541	1769		Be22Rh1	Be22Rh1	Be	22	Rh	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100542	1769		Be49Rh1	Be49Rh1	Be	49	Rh	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100543	1390		Be22Re0.95W0.05	Be22Re0.95W0.05	Be	22	Re	0.95	W	0.05																			1967																																														K		9.45					9.45																																																																																																									HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
100544	1390		Be22Re0.95Os0.05	Be22Re0.95Os0.05	Be	22	Re	0.95	Os	0.05																			1967																																														K		9.2					9.2																																																																																																									HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
100545	1390		Be0.96Re0.04	Be0.96Re0.04	Be	0.96	Re	0.04																					1967																																														K		9.5					9.5																																																																																																									HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
100546	567		Be0.957Re0.043	Be0.957Re0.043	Be	0.957	Re	0.043																					1965																																														K		9.67					9.67																																																																																																									PHYS.LETT.,19(1965)263	E.BUCHER,F.HEINIGER,J.MULLER,P.SPTZLI		
100547	567		Be0.98Re0.02	Be0.98Re0.02	Be	0.98	Re	0.02																					1965																																													cubic	K		9.75					9.75																																																																																																									PHYS.LETT.,19(1965)263	E.BUCHER,F.HEINIGER,J.MULLER,P.SPTZLI		
100548	1769		Be2Re1	Be2Re1	Be	2	Re	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100549	1390		Be22Re1	Be22Re1	Be	22	Re	1																					1967																																													cubic	K		9.33					9.33																																																																																																									HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
100550	1769		Be5Pt1	Be5Pt1	Be	5	Pt	1																					1973																																														K		2.3					2.3																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100551	1057		Be0.95Pt0.005	Be0.95Pt0.005	Be	0.95	Pt	0.005																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100552	RMP0350001		Be5Pd1	Be5Pd1	Be	5	Pd	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100553	712		Be2Ru1	Be2Ru1	Be	2	Ru	1																																																																			K		1.35					1.35																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100554	1769		Be5Ru1	Be5Ru1	Be	5	Ru	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100555	712		Be17Ru3	Be17Ru3	Be	17	Ru	3																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100556	1769		Be13Ru1	Be13Ru1	Be	13	Ru	1																					1973																																														K		1.3					1.3																																																																																																									DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100557	1769		Be22Ru1	Be22Ru1	Be	22	Ru	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100558	1769		Be1Rh1	Be1Rh1	Be	1	Rh	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100559	712		Be2Rh1	Be2Rh1	Be	2	Rh	1																																																																			K		1.37					1.37																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100560	1769		Be4.4Rh1	Be4.4Rh1	Be	4.4	Rh	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100561	1769		Be5Rh1	Be5Rh1	Be	5	Rh	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100562	1769		Be8.5Rh1	Be8.5Rh1	Be	8.5	Rh	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100563	1769		Be13Rh1	Be13Rh1	Be	13	Rh	1																					1973																																														K					1																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100564	1057		Be0.95Rh0.05	Be0.95Rh0.05	Be	0.95	Rh	0.05																					1967																																														K					0.45																																																																																																											Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100565	1922		Be12W1	Be12W1	Be	12	W	1																					1973																																													tetragonal	K					1.7																																																																																																											UKR.FIZ.ZH.,18(1973)672	A.A.MATSAKOVA,N.M.MATYUSHENKO,N.S.PUSACHEV		
100566	1922		Be22W1	Be22W1	Be	22	W	1																					1973																																													cubic	K		4.12					4.12																																																																																																									UKR.FIZ.ZH.,18(1973)672	A.A.MATSAKOVA,N.M.MATYUSHENKO,N.S.PUSACHEV		
100567	1769		Be13U1	Be13U1	Be	13	U	1																					1973																												NaZn13																	NaZn13, D2[3]	K					0.04																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100568	RMP0350001		Be2Ti1	Be2Ti1	Be	2	Ti	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100569	1769		Be13Th1	Be13Th1	Be	13	Th	1																					1973																												NaZn13																	NaZn13, D2[3]	K					0.04																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100571	1377		Be1Ta2	Be1Ta2	Be	1	Ta	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
100572	927		Be2Ta3	Be2Ta3	Be	2	Ta	3																					1969																												Si2U3																	tetragonal	K		1					1																																																																																																									PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
100573	1909		Be17Ta2	Be17Ta2	Be	17	Ta	2																					1968																																														K					1.38																																																																																																											PHYS.REV.,171(1968)591	N.M.WOLCOTT,R.L.FALGE JR.		
100574	1909		Be12Ta1	Be12Ta1	Be	12	Ta	1																					1968																																													tetragonal	K					1.38																																																																																																											PHYS.REV.,171(1968)591	N.M.WOLCOTT,R.L.FALGE JR.		
100575	1784	rapid quench. broad transition	Be0.62Si0.38	Be0.62Si0.38	Be	0.62	Si	0.38																					1974																																														K		9					9																																																																																																									PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
100576	1057		Be0.95Ru0.05	Be0.95Ru0.05	Be	0.95	Ru	0.05																					1967																																														K		1.47					1.47																																																																																																									Z.PHYS.,200(1967)7	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL		
100577	8		Bi2Ca3	Bi2Ca3	Bi	2	Ca	3																					1952																																														K					1.38																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100578	153		Bi3Ca1	Bi3Ca1	Bi	3	Ca	1																					1959																																														K		2					2																																																																																																									FIZ.IKHIM,14(1959) 113&117	G.S.ZHDANOV,N.E.ALEKSEEVSKII,N.N.ZHRAVLEV		
100579	870		Bi0.1C1.45Y0.9	Bi0.1C1.45Y0.9	Bi	0.1	C	1.45	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		9.35					9.35																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100580	870		Bi0.3C1.45Y0.7	Bi0.3C1.45Y0.7	Bi	0.3	C	1.45	Y	0.7																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100581	606		Bi1C1	Bi1C1	Bi	1	C	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100582	1769		Be2Zr1	Be2Zr1	Be	2	Zr	1																					1973																												AlB2																	AlB2, C32	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100583	712		Be17Zr2	Be17Zr2	Be	17	Zr	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100584	1909		Be13Zr1	Be13Zr1	Be	13	Zr	1																					1968																												NaZn13																	NaZn13, D2[3]	K					1.15																																																																																																											PHYS.REV.,171(1968)591	N.M.WOLCOTT,R.L.FALGE JR.		
100585	712		Be16Zr1	Be16Zr1	Be	16	Zr	1																																																	NaZn13																	NaZn13, D2[3]	K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100586	1769		Be13Y1	Be13Y1	Be	13	Y	1																					1973																																														K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100587	1769		Be2W1	Be2W1	Be	2	W	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K					1.4																																																																																																											DOK.AKAD.NAUK SSSR,208(1973)303	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
100588	712		Be21W5	Be21W5	Be	21	W	5																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100589	2		Bi2Cr1	Bi2Cr1	Bi	2	Cr	1																					1948																																														K					1.57																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
100590	262		Bi1Co0.1Sc0.9	Bi1Co0.1Sc0.9	Bi	1	Co	0.1	Sc	0.9																																																																	K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
100591	606		Bi1Co1	Bi1Co1	Bi	1	Co	1																					1966																																														K		0.49					0.49																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100592	11		Bi1Ce1	Bi1Ce1	Bi	1	Ce	1																					1952																												NaCl																	NaCl, B1	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100593	11		Bi2Ce1	Bi2Ce1	Bi	2	Ce	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100594	1917	weight fraction 	Bi0.54Cd0.25Sn0.26	Bi0.54Cd0.2Sn0.26	Bi	0.54	Cd	0.2	Sn	0.26																			1969																																														K		3.69					3.69																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100595	1917	weight fraction 	Bi0.396Cd0.594Sn0.01	Bi0.396Cd0.594Sn0.01	Bi	0.396	Cd	0.594	Sn	0.01																			1969																																														K					1.3																																																																																																											REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100596	402		Bi0.5Dc0.1Pb0.27Sn0.	Bi0.5Dc0.1Pb0.27Sn0.13	Bi	0.5	Dc	0.1	Pb	0.27	Sn	0.13																	1930																																														K																																																																																																																COMM.KAMERLINGH ONNES LAB.,19(1930)208B	J.VOOGD,W.J.DEHAAS		
100597	109	weight fraction 	Bi0.5Cd0.125Pb0.25Sn	Bi0.5Cd0.125Pb0.25Sn0.125	Bi	0.5	Cd	0.125	Pb	0.25	Sn	0.125																	1930																																														K		8.2					8.2																																																																																																									ROY.SOC.CANADA TRANS.,24(1930)25	J.C.MCLENNAN,J.F.ALLEN,J.O.WILHELM		
100598	1917	weight fraction 	Bi0.28Dc0.19In0.53	Bi0.28Dc0.19In0.53	Bi	0.28	Dc	0.19	In	0.53																			1969																																														K		5.85					5.85																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100599	99	eutectec	Bi1Cd1	Bi1Cd1	Bi	1	Cd	1																					1930																																														K					1.88																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100600	1204	weight fraction 	Bi0.6Cd0.4	Bi0.6Cd0.4	Bi	0.6	Cd	0.4																					1967																																														K		0.53					0.53																																																																																																									J.APPL.PHYS.,38(1967)3667	J.R.DILLINGER,R.E.FASSNACHT		
100601	1982		Bi0.15Ge0.15Nb3Sn0.7	Bi0.15Ge0.15Nb3Sn0.7	Bi	0.15	Ge	0.15	Nb	3	Sn	0.7																	1964																																														K		17.75					17.75																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100602	11		Bi2Ge1	Bi2Ge1	Bi	2	Ge	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100603	1982		bi0.15Ga0.15Nb3Sn0.7	Bi0.15Ga0.15Nb3Sn0.7	Bi	0.15	Ga	0.15	Nb	3	Sn	0.7																	1964																																														K		18.04					18.04																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100604	606		Bi1Fe1	Bi1Fe1	Bi	1	Fe	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100605	11		Bi1Cu1Mg1	Bi1Cu1Mg1	Bi	1	Cu	1	Mg	1																			1952																												MgAgAs																	MgAgAs, C1[b]	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100606	95		BI1Cu3	Bi1Cu3	Bi	1	Cu	3																					1955																																														K					1.5																																																																																																							From Roberts' Table				Naturwiss, 42(1955)451	W.Buckel		
100607	606		Bi1Cu1	Bi1Cu1	Bi	1	Cu	1																					1966																																														K		1.4					1.4																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100608	154		Bi1Cu1	Bi1Cu1	Bi	1	Cu	1																					1960																																														K		2.2					2.2																																																																																																									ZH.EKSP.TEOR.FIZ.,38(1960)294	N.E.ALEKSEEVSKI,V.V.BONDAR,YU.M.POLUKAROV		
100609	52		Bi1Cs2	Bi1Cs2	Bi	1	Cs	2																					1957																																														K					1.5																																																																																																											Zh.Eksp.Teor.Fiz, 34(1957)827	N.N.Zhuravlev		
100610	52		Bi1Cs3	Bi1Cs3	Bi	1	Cs	3																					1957																																													cubic	K					1.5																																																																																																											Zh.Eksp.Teor.Fiz, 34(1957)827	N.N.Zhuravlev		
100611	52		Bi2Cs1	Bi2Cs1	Bi	2	Cs	1																					1957																												MgCu2(Laves)																	MgCu2, C15	K		4.75					4.75																																																																																																									Zh.Eksp.Teor.Fiz, 34(1957)827	N.N.Zhuravlev		
100612	606		Bi1Cr1	Bi1Cr1	Bi	1	Cr	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100613	1732	co-evaporated 	Bi1In1	Bi1In1	Bi	1	In	1																					1971																																														K		7.95					7.95																																																																																																									ZH.ETF PIS.RED.,14(1971)496	A.F.ORLOV		
100614	842		Bi0.015In0.985	Bi0.015In0.985	Bi	0.015	In	0.985																					1968																																														K		3.725					3.725																																																																																																									PHYS.LETT.A,27(1968)13	I.F.SILVERA,J.A.CAPE		
100615	722		Bi0.0119In0.981	Bi0.019In0.981	Bi	0.019	In	0.981																					1965																																														K		3.86					3.86																																																																																																									PHYS.REV.,140(1965)A1169	B.SERIN,T.MCCONVILLE		
100616	1121		Bi0.02In0.98	Bi0.02In0.98	Bi	0.02	In	0.98																					1964																																														K		3.845					3.845																																																																																																									PHYS.REV.LETT.,12(1964)101	B.ROSENBLUM,G.FISCHER,M.CARDNA		
100617	1247	P = 0-18 kbar	Bi0.025In0.975	Bi0.025In0.975	Bi	0.025	In	0.975																					1972																																														K		4.07					4.07																																																																																																									J.PHYS.F:METAL PHYS.,2(1972)306	E.PAPP		
100618	634		Bi0.05In0.95	Bi0.05In0.95	Bi	0.05	In	0.95																					1966																																														K		4.65					4.65																																																																																																									J.LESS-COMMON METALS,11(1966)296	J.S.HEROLD,J.V.HUTCHERSON,R.L.GUAY		
100619	634		Bi0.1In0.9	Bi0.1In0.9	Bi	0.1	In	0.9																					1966																																														K		5.05					5.05																																																																																																									J.LESS-COMMON METALS,11(1966)296	J.S.HEROLD,J.V.HUTCHERSON,R.L.GUAY		
100620	843	P = 30 kbar	Bi0.343In0.657	Bi0.343In0.657	Bi	0.343	In	0.657																					1968																																														K		5.55					5.55																																																																																																									PHYS.LETT.A,27(1968)116	B.C.DEATON,D.E.GORDON		
100621	1112		Bi3In5	Bi3In5	Bi	3	In	5																					1970																																														K		4.2					4.2																																																																																																									PHYS.LETT.A,32(1970)295	E.CRUCEANU,E.HERING,H.SCHWARZ		
100622	634		Bi1In1	Bi1In1	Bi	1	In	1																					1966																												PbO																	PbO, B10	K					0.5																																																																																																											J.LESS-COMMON METALS,11(1966)296	J.S.HEROLD,J.V.HUTCHERSON,R.L.GUAY		
100623	1978		Bi1In2	Bi1In2	Bi	1	In	2																					1972																																														K		5.87					5.87																																																																																																									REV.ROUM.PHYS.,17(1972)547	E.CRUCEANU,H.ULLMAIER		
100624	1198		Bi1In2	Bi1In2	Bi	1	In	2																					1964																																													hexagonal	K		5.6					5.6																																																																																																									J.APPL.PHYS.,35(1964)3322	A.W.LAWSON,G.A.SAUNDERS		
100625	8		Bi2Mg3	Bi2Mg3	Bi	2	Mg	3																					1952																												La2O3																	La2O3, D5[2]	K					1.5																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100626	8		Bi1Li3	Bi1Li3	Bi	1	Li	3																					1952																												BiF3																	BiF3, D0[3]	K					1.43																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100627	1351		Bi1Li1	Bi1Li1	Bi	1	Li	1																					1971																												AuCu																	AuCu, L1[0]	K		2.455					2.455																																																																																																									J.PHYS.SOC.JAPAN,30(1971)294	T.SAMBONGI		
100628	8		Bi1K3	Bi1K3	Bi	1	K	3																					1952																												Na3As																	Na3As, D0[18]	K					1.4																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100629	8		Bi2K3	Bi2K3	Bi	2	K	3																					1952																																														K					3.6																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100630	95		Bi1K1	Bi1K1	Bi	1	K	1																					1955																																														K		3.6					3.6																																																																																																					From Roberts' Table				Naturwiss, 42(1955)451	W.Buckel		
100631	897	P = 0-10 kbar	Bi2K1	Bi2K1	Bi	2	K	1																					1969																																														K		3.57					3.57																																																																																																									ZH.ETF PIS.RED.,9(1969)571	N.E.ALEKSEEVSKII		
100632	153		Bi2K1	Bi2K1	Bi	2	K	1																					1959																												MgCu2(Laves)																	MgCu2, C15	K		3.58					3.58																																																																																																									FIZ.IKHIM,14(1959) 113&117	G.S.ZHDANOV,N.E.ALEKSEEVSKII,N.N.ZHRAVLEV		
100633	606		Bi2Ir1	Bi2Ir1	Bi	2	Ir	1																					1966																																														K		3.96					3.96																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100634	491		BI1Ir2	Bi1Ir2	Bi	1	Ir	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100635	491		Bi1Ir1	Bi1Ir1	Bi	1	Ir	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100636	1982		Bi0.15In0.15NB3Sn0.7	Bi0.15In0.15Nb3Sn0.7	Bi	0.15	In	0.15	Nb	3	Sn	0.7																	1964																																														K		18.01					18.01																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100637	606		Bi1Os1	Bi1Os1	Bi	1	Os	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100638	8		Bi1Ni1	Bi1Ni1	Bi	1	Ni	1																					1952																												NiAs																	NiAs, B8[1]	K		4.25					4.25																																																																																																									Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100639	8		Bi3Ni1	Bi3Ni1	Bi	3	Ni	1																					1952																																													orthorhombic	K		4.06					4.06																																																																																																									Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100640	1982		Bi0.15Nb3Sn0.7Tl0.15	Bi0.15Nb3Sn0.7Tl0.15	Bi	0.15	Nb	3	Sn	0.7	Tl	0.15																	1964																																														K		18.12					18.12																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100641	1982	sintered	Bi0.15Nb3Sn0.85	Bi0.15Nb3Sn0.85	Bi	0.15	Nb	3	Sn	0.85																			1964																																														K		18.23					18.23																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
100642	508		Bi1Nb3	Bi1Nb3	Bi	1	Nb	3																					1964																																													cubic	K					2.25																																																																																																											PHYS.CHEM.SOLIDS,25(1964)1213	D.H.KILLPATRICK		
100643	508		Bi1Nb3	Bi1Nb3	Bi	1	Nb	3																					1964																												Cr3Si(A15)																	Cr3Si, A15	K		4.5					4.5																																																																																																									PHYS.CHEM.SOLIDS,25(1964)1213	D.H.KILLPATRICK		
100644	4		Bi1Na1	Bi1Na1	Bi	1	Na	1																					1949																												AuCu																	AuCu, L1[0]	K		2.25					2.25																																																																																																									Zh.Eksp.Teor.Fiz, 19(1949)671	N.E.Alekseevskii		
100645	8		Bi1Na3	Bi1Na3	Bi	1	Na	3																					1952																												Na3As																	Na3As, D0[18]	K					1.4																																																																																																											Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100646	606		Bi3Mo1	Bi3Mo1	Bi	3	Mo	1																					1966																																														K		3.7					3.7																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100647	11		Bi1Mo1	Bi1Mo1	Bi	1	Mo	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100648	606		Bi1Mn1	Bi1Mn1	Bi	1	Mn	1																					1966																												NiAs																	NiAs, B8[1]	K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100649	1457	P=12-18 kbar	Bi0.575Pb0.425	Bi0.575Pb0.425	Bi	0.575	Pb	0.425																					1973																																													hexagonal	K		8.03					8.03																																																																																																									J.LOW TEMP.PHYS.,10(1973)543	D.K.FINNEMORE,R.E.JONES JR.		
100650	843		Bi0.625Pb0.375	Bi0.625Pb0.375	Bi	0.625	Pb	0.375																					1968																																														K		8.05					8.05																																																																																																									PHYS.LETT.A,27(1968)116	B.C.DEATON,D.E.GORDON		
100651	402		Bi0.07Pb0.93	Bi0.07Pb0.93	Bi	0.07	Pb	0.93																					1930																																														K		7.7					7.7																																																																																																									COMM.KAMERLINGH ONNES LAB.,19(1930)208B	J.VOOGD,W.J.DEHAAS		
100652	402		Bi0.1Pb0.9	Bi0.1Pb0.9	Bi	0.1	Pb	0.9																					1930																																														K		7.95					7.95																																																																																																									COMM.KAMERLINGH ONNES LAB.,19(1930)208B	J.VOOGD,W.J.DEHAAS		
100653	402		Bi0.2Pb0.8	Bi0.2Pb0.8	Bi	0.2	Pb	0.8																					1930																																														K		8.15					8.15																																																																																																									COMM.KAMERLINGH ONNES LAB.,19(1930)208B	J.VOOGD,W.J.DEHAAS		
100654	851		Bi0.23Pb0.77	Bi0.23Pb0.77	Bi	0.23	Pb	0.77																					1968																																														K		7.8					7.8																																																																																																									Z.PHYS.,213)1968)79	J.HASSE,J.SEIBERTH		
100655	851		Bi0.26Pb0.74	Bi0.26Pb0.74	Bi	0.26	Pb	0.74																					1968																																														K		8.3					8.3																																																																																																									Z.PHYS.,213)1968)79	J.HASSE,J.SEIBERTH		
100656	1318		Bi0.3Pb0.7	Bi0.3Pb0.7	Bi	0.3	Pb	0.7																					1971																																														K		8.63					8.63																																																																																																									SOLID STATE COMMUN.,9(1971)1961	J.G.ADLER,T.T.CHEN		
100657	403		Bi0.35Pb0.65	Bi0.35Pb0.65	Bi	0.35	Pb	0.65																					1931																																														K		8.7					8.7																																																																																																									COMM.KAMERLINGH ONNES LAB.,19(1931)214B	J.VOOGD,W.J.DEHAAS		
100658	1485		Bi0.45Pb0.55	Bi0.45Pb0.55	Bi	0.45	Pb	0.55																					1971																																														K		8.4					8.4																																																																																																									PHYS.LETT.A,37(1971)457	J.HASSE,V.REICHERT,W.BUCKEL		
100659	310		Bi0.5Pb0.5	Bi0.5Pb0.5	Bi	0.5	Pb	0.5																					1960																																														K		8.4					8.4																																																																																																									PHYS.REV.LETT.,5(1960)149	J.H.WERNICK		
100660	85	weight fraction , eutectec 	Bi0.65Pb0.35	Bi0.65Pb0.35	Bi	0.65	Pb	0.35																					1932																																														K		8.8					8.8																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
100661	413		Bi1Pd1Se1	Bi1Pd1Se1	Bi	1	Pd	1	Se	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1					1																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
100662	198		Bi0.4Pd0.6	Bi0.4Pd0.6	Bi	0.4	Pd	0.6																					1960																												NiAs																	NiAs, B8[1]	K		4					4																																																																																																									KRISTALLOGRAFIA,5(1960) 553	G.S.ZHDANOV,N.N.ZHURAVLEV,R.N.KUSHMIN		
100663	145		Bi0.25Pd0.75	Bi0.25Pd0.75	Bi	0.25	Pd	0.75																					1956																																														K																																																																																																																IZVEST.AKAD.NAUK.SSSR SER.FIZ.,20(1956)708	G.S.ZHDANOV,N.N.ZHURAVLEV		
100664	38		Bi1Pd1	Bi1Pd1	Bi	1	Pd	1																																																																		orthorhombic	K		3.74					3.74																																																																																																												
100665	8		Bi2Pd1	Bi2Pd1	Bi	2	Pd	1																					1952																																													monoclinic	K		1.73					1.73																																																																																																									Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100666	6		Bi2Pd1	Bi2Pd1	Bi	2	Pd	1																					1954																																													tetragonal	K		4.25					4.25																																																																																																									Zh.Eksp.Teor.Fiz., 27(1954)125	N.E.Alekseevskii		
100667	109		Bi0.5Pb0.25Sn0.25	Bi0.5Pb0.25Sn0.25	Bi	0.5	Pb	0.25	Sn	0.25																			1930																																														K		8.5					8.5																																																																																																									ROY.SOC.CANADA TRANS.,24(1930)25	J.C.MCLENNAN,J.F.ALLEN,J.O.WILHELM		
100668	1917	weight fraction	Bi0.525pb0.32Sn0.155	Bi0.525Pb0.32Sn0.155	Bi	0.525	Pb	0.32	Sn	0.155																			1969																																														K		8.68					8.68																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100669	111		Bi1Pb1Sb1	Bi1Pb1Sb1	Bi	1	Pb	1	Sb	1																			1930																																														K		8.9					8.9																																																																																																									ROY.SOC.CAN.TRANS.,24(1930)53	J.C.MCLENNAN,J.O.WILHELM,L.F.ALLEN		
100670	484		Bi0.95Pb0.05	Bi0.95Pb0.05	Bi	0.95	Pb	0.05																					1965																																														K					1.03																																																																																																											NG.S.C.CAN.J.PHYS.,43(1965)594	J.G.ADLER		
100671	1774	deposited at 4.2 K	Bi0.25Pb0.75	Bi0.25Pb0.75	Bi	0.25	Pb	0.75																					1973																																														K		6.9					6.9																																																																																																									PHYS.REV.B,7(1973)4850	G.BERGMANN		
100672	1485		Bi0.45Pb0.55	Bi0.45Pb0.55	Bi	0.45	Pb	0.55																					1971																																													amorphous	K		7					7																																																																																																									PHYS.LETT.A,37(1971)457	J.HASSE,V.REICHERT,W.BUCKEL		
100673	59	beta phase 	Bi2Rh1	Bi2Rh1	Bi	2	Rh	1																					1955																																													monoclinic	K					1.3																																																																																																											Zh.Eksp.Teor.Fiz, 28(1955)237	N.E.Alekseevskii,G.S.Zhdanov,N.N.Zhuravlev		
100674	59		BI2Rh1	Bi2Rh1	Bi	2	Rh	1																					1955																																													monoclinic	K					1.34																																																																																																											Zh.Eksp.Teor.Fiz, 28(1955)237	N.E.Alekseevskii,G.S.Zhdanov,N.N.Zhuravlev		
100675	606		Bi1Re2	Bi1Re2	Bi	1	Re	2																					1966																																														K		2.2					2.2																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100676	53		Bi2Rb1	Bi2Rb1	Bi	2	Rb	1																					1958																												MgCu2(Laves)																	MgCu2, C15	K		4.25					4.25																																																																																																									Zh.Eksp.Teor.Fiz, 34(1958)820	N.N.Zhuravlev,G.S.Zhdanov		
100677	413		Bi1Pt1Te1	Bi1Pt1Te1	Bi	1	Pt	1	Te	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.15					1.15																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
100678	413		Bi1Pt1Se1	Bi1Pt1Se1	Bi	1	Pt	1	Se	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.45					1.45																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
100679	002		Bi3Pt1	Bi3Pt1	Bi	3	Pt	1																					1948																																														K					1.8																																																																																																											ZH.EKSP.TEOR.FIZ.,18(1948)101	N.E.ALEKSEEVSKII		
100681	002	low temp. alpha phase	Bi2Pt1	Bi2Pt1	Bi	2	Pt	1																					1948																																														K					1.8																																																																																																											ZH.EKSP.TEOR.FIZ.,18(1948)101	N.E.ALEKSEEVSKII		
100682	060		BI2Pt1	Bi2Pt1	Bi	2	Pt	1																					1953																															A	6.44		6.25											hexagonal	K		0.155					0.155																																																																																																									EKSP.TEOR.FIZ.,25(1953)383	N.E.ALKSEEVSKII,YU.P.GAIDKOV		
100683	158		Bi1Pr1	Bi1Pr1	Bi	1	Pr	1																					1959																												NaCl																	NaCl, B1	K																																																																																																																SER.MAT.MEKH ASTRON.FIZ.I KHIM.,14(1959)117	G.S.ZHDANOV,N.E.ALEKSEEVSKII,N.N.ZHURAVLEV		
100684	413		Bi1Pd1Te1	Bi1Pd1Te1	Bi	1	Pd	1	Te	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.2					1.2																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
100685	11		Bi1Sb1	Bi1Sb1	Bi	1	Sb	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100686	60		Bi2S3	Bi2S3	Bi	2	S	3																					1953																												Sb2S3																	Sb2S3, D5[8]	K					0.1																																																																																																											Eksp.Teor.Fiz, 25(1953)383	"N.E.Alekseevskii
,Yu.P.Gaidkov"		
100687	8		Bi1S3	Bi1S3	Bi	1	S	3																					1952																																														K																																																																																																																Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
100688	606		Bi1S1	Bi1S1	Bi	1	S	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100689	119		Bi2S1	Bi2S1	Bi	2	S	1																					1948																																														K					1.9																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
100690	606		Bi1Ru1	Bi1Ru1	Bi	1	Ru	1																					1966																																														K		5.7					5.7																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100691	491		Bi1Ru2	Bi1Ru2	Bi	1	Ru	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100692	491		Bi1Ru1	Bi1Ru1	Bi	1	Ru	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
100693	2	alpha phase	Bi4Rh1	Bi4Rh1	Bi	4	Rh	1																					1948																																													cubic	K					0.1																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
100694	155	gamma-type	Bi0.8Rh0.2	Bi0.8Rh0.2	Bi	0.8	Rh	0.2																					1958																																													hexagonal	K		2.7					2.7																																																																																																									KRISTALLOGRAPHIA,3(1958)373	A.I.SOKLAKOV,G.S.ZHDANOV,N.N.ZHURAVLEV,R.N.KUSMIN		
100695	59	beta-type	Bi3Rh1	Bi3Rh1	Bi	3	Rh	1																					1955																															A	9.027	4.24	11.522											orthorhombic	K		3.2					3.2																																																																																																									Zh.Eksp.Teor.Fiz, 28(1955)237	N.E.Alekseevskii,G.S.Zhdanov,N.N.Zhuravlev		
100696	1588		Bi1Rh1	Bi1Rh1	Bi	1	Rh	1																					1960																												NiAs																	NiAs, B8[1]	K		2.06					2.06																																																																																																									KRISTALLOGRAPHIYA,5(1960)553	G.S.ZHDANOV,N.N.ZHURAVLEV,R.N.KUZ'MIN		
100697	606		Bi3Te1	Bi3Te1	Bi	3	Te	1																					1966																																														K		1					1																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100698	11		Bi3Sr1	Bi3Sr1	Bi	3	Sr	1																					1952																												AuCu3																	AuCu3, L1[2]	K		5.7					5.7																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100699	1091	P = 25 kbar, T = 77K	Bi0.4Sn0.6	Bi0.4Sn0.6	Bi	0.4	Sn	0.6																					1968																																														K		7.34					7.34																																																																																																									FIZ.METAL.METALLOVED.,26(1968)921	A.E.ZAKHAROV,A.G.RABIN'KIN		
100700	70	eutectec	Bi1Sn1	Bi1Sn1	Bi	1	Sn	1																					1929																																														K		3.8					3.8																																																																																																									Proc.Acad.Sci.Amsterdam, 32(1929)715	W.J.DeHaas,E. Van Aubel,J.Voogd		
100701	843	P = 30 kbar	Bi1Sn1	Bi1Sn1	Bi	1	Sn	1																					1968																																														K		4.2					4.2																																																																																																									PHYS.LETT.A,27(1968)116	B.C.DEATON,D.E.GORDON		
100702	843		Bi1Sn1	Bi1Sn1	Bi	1	Sn	1																					1968																																														K		3.72					3.72																																																																																																									PHYS.LETT.A,27(1968)116	B.C.DEATON,D.E.GORDON		
100703	1091	P = 25 kbar, T = 77K	Bi0.5Sn0.5	Bi0.5Sn0.5	Bi	0.5	Sn	0.5																					1968																																													monoclinic	K		0.788					0.788																																																																																																									FIZ.METAL.METALLOVED.,26(1968)921	A.E.ZAKHAROV,A.G.RABIN'KIN		
100704	1091	P = 25 kbar, T = 77K	Bi0.6Sn0.4	Bi0.6Sn0.4	Bi	0.6	Sn	0.4																					1968																																														K		7					7																																																																																																									FIZ.METAL.METALLOVED.,26(1968)921	A.E.ZAKHAROV,A.G.RABIN'KIN		
100705	1917	weight fraction	Bi0.57Sn0.43	Bi0.57Sn0.43	Bi	0.57	Sn	0.43																					1969																																														K		2.25					2.25																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100706	606		Bi3Sn1	Bi3Sn1	Bi	3	Sn	1																					1966																																														K		3.77					3.77																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100707	84		Bi2Se3	Bi2Se3	Bi	2	Se	3																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100708	606		Bi1Sc1	Bi1Sc1	Bi	1	Sc	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100709	411		Bi1Y1	Bi1Y1	Bi	1	Y	1																					1962																												NaCl																	NaCl, B1	K																																																																																																																KRISTALLOGRAPHIYA,7(1962)787	E.M.SMIRNOVA,N.N.ZHURAVLEV		
100710	173		Bi2Y3	Bi2Y3	Bi	2	Y	3																					1961																																														K		2.25					2.25																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
100711	606		Bi1W1	Bi1W1	Bi	1	W	1																					1966																																														K					0.3																																																																																																							MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100712	825		Bi1V3	Bi1V3	Bi	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K					4.2																																																																																																											DOKL.AN SSR,171(1966)331	E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
100713	1774		Bi0.85Tl0.15	Bi0.85Tl0.15	Bi	0.85	Tl	0.15																					1973																																														K		6.23					6.23																																																																																																									PHYS.REV.B,7(1973)4850	G.BERGMANN		
100714	265		Bi0.26Tl0.74	Bi0.26Tl0.74	Bi	0.26	Tl	0.74																					1962																																														K		4.4					4.4																																																																																																									IBM J.RES.DEV.,6(1962)68	B.R.COLES		
100715	90		Bi5Tl3	Bi5Tl3	Bi	5	Tl	3																					1929																																														K		6.4					6.4																																																																																																					From Roberts' Table.				J.Commun.Kamerlingh-Onnes Lab, 18(1929)199c	W.J.DeHaas,J.Voogd		
100716	843	after 30 kbar 	Bi0.86Tl0.14	Bi0.86Tl0.14	Bi	0.86	Tl	0.14																					1968																																														K		6.5					6.5																																																																																																									PHYS.LETT.A,27(1968)116	B.C.DEATON,D.E.GORDON		
100717	712		Bi1Ti3	Bi1Ti3	Bi	1	Ti	3																																																																		tetragonal	K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100718	1582		Bi5Th3	Bi5Th3	Bi	5	Th	3																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
100720	84		Bi2Te3	Bi2Te3	Bi	2	Te	3																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
100721	10		C0.2Cr0.8	C0.2Cr0.8	C	0.2	Cr	0.8																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100722	10		C0.3Cr0.71	C0.3Cr0.71	C	0.3	Cr	0.71																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100723	11		C2Cr3	C2Cr3	C	2	Cr	3																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100724	1222		C3Ce0.2Th1.8	C3Ce0.2Th1.8	C	3	Ce	0.2	Th	1.8																			1973																												Pu2C3																	Pu2C3, D5[c]	K					4																																																																																																											J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100725	11		C2Ce1	C2Ce1	C	2	Ce	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100726	632		C1Cd1Ti2	C1Cd1Ti2	C	1	Cd	1	Ti	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100727	870		C1.35Ca0.1Y0.9	C1.35Ca0.1Y0.9	C	1.35	Ca	0.1	Y	0.9																			1969																																														K		10.5					10.5																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100728	11		Br2Cu1	Br2Cu1	Br	2	Cu	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100729	1582		Bi2Zr1	Bi2Zr1	Bi	2	Zr	1																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
100730	RMP0350001		Bi0.3Zr0.7	Bi0.3Zr0.7	Bi	0.3	Zr	0.7																					1963																																														K		1.51					1.51																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100731	606		Bi1Zr3	Bi1Zr3	Bi	1	Zr	3																					1966																																														K		2.84					2.84																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100732	606		BI3Zn1	Bi3Zn1	Bi	3	Zn	1																					1966																																														K		0.87					0.87																																																																																																					MANY MORE SUPERCONDUCTING BISMUTH PHASES				PHYS.REV.LETT.,17(1966)640	A.JAYARAMAN,B..T.MATTHIAS,E.CORENZWIT,K.ANDRES,T.H.GEBALLE		
100733	1222		C3Er0.2Th1.8	C3Er0.2Th1.8	C	3	Er	0.2	Th	1.8																			1973																												Pu2C3																	Pu2C3, D5[c]	K		8.2					8.2																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100734	1222		C3Er0.1Th1.9	C3Er0.1Th1.9	C	3	Er	0.1	Th	1.9																			1973																												Pu2C3																	Pu2C3, D5[c]	K		6.8					6.8																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100735	1222		C3Er1Th1	C3Er1Th1	C	3	Er	1	Th	1																			1973																												Pu2C3																	Pu2C3, D5[c]	K		4.6					4.6																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100736	1222		C3Er0.8Th1.2	C3Er0.8Th1.2	C	3	Er	0.8	Th	1.2																			1973																												Pu2C3																	Pu2C3, D5[c]	K		7					7																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100737	1222		C3Er0.6Th1.4	C3Er0.6Th1.4	C	3	Er	0.6	Th	1.4																			1973																												Pu2C3																	Pu2C3, D5[c]	K		8.1					8.1																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100738	1222		C3Er0.4Th1.6	C3Er0.4Th1.6	C	3	Er	0.4	Th	1.6																			1973																												Pu2C3																	Pu2C3, D5[c]	K		8.2					8.2																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100739	784		C2Er1	C2Er1	C	2	Er	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100740	784		C2Dy1	C2Dy1	C	2	Dy	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100741	494		C0.016Cs1	C0.016Cs1	C	0.016	Cs	1																					1965																																														K					0.011																																																																																																							SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100742	494		C8Cs1	C8Cs1	C	8	Cs	1																					1965																																													hexagonal	K		0.135					0.135																																																																																																					SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100743	870		C1.45Cr0.1Y0.9	C1.45Cr0.1Y0.9	C	1.45	Cr	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		12.4					12.4																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100744	632		C1Cr2Ga1	C1Cr2Ga1	C	1	Cr	2	Ga	1																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100745	1813		C1Hf0.15Mo0.85	C1Hf0.15Mo0.85	C	1	Hf	0.15	Mo	0.85																			1966																												NaCl																	NaCl, B1	K		9					9																																																																																																									ISZ.AKAD.NAUK SSSR.NEORGAN.MATER.,2(1966)2145	I.A.SHCHERBAK,O.I.SHYLISHOVA		
100746	650		C0.75Hf0.05Mo0.95	C0.75Hf0.05Mo0.95	C	0.75	Hf	0.05	Mo	0.95																			1966																												NaCl																	NaCl, B1	K		14.2					14.2																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)235	H.C.GATOS,V.SADAGOPAN		
100747	632		C1Hf2In1	C1Hf2In1	C	1	Hf	2	In	1																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100748	559		C0.985Hf1	C0.985Hf1	C	0.985	Hf	1																					1966																																														K					1.28																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100749	20		C1Hf1	C1Hf1	C	1	Hf	1																					1932																												NaCl																	NaCl, B1	K					1.23																																																																																																											Z.Phys.,  75(1932)521	W.Meissner,H.Franz,H.Westerhoff		
100750	870		C1.35Ge0.1Y0.9	C1.35Ge0.1Y0.9	C	1.35	Ge	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		10.6					10.6																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100751	RMP0350001		C0.05Ge3V5	C0.05Ge3V5	C	0.05	Ge	3	V	5																			1963																												Mn5Si3																	Mn5Si3, D8[8]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100752	767		C1.5Ge3La5	C1.5Ge3La5	C	1.5	Ge	3	La	5																			1970																																													cubic	K		3.3					3.3																																																																																																									PROC.NAT.ACAD.SCI.,67(1970)313	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI,W.H.ZACHARIASEN		
100753	784		C2Gd1	C2Gd1	C	2	Gd	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100754	635		C1Ga1Mo2	C1Ga1Mo2	C	1	Ga	1	Mo	2																			1967																																													hexagonal	K		4.1					4.1																																																																																																									J.LESS-COMMON METALS,13(1967)129	L.E.TOTH		
100755	1564		C1Ga1La3	C1Ga1La3	C	1	Ga	1	La	3																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100756	119		C1Fe3	C1Fe3	C	1	Fe	3																					1948																																														K					1.3																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
100757	793		C1Ir1Mo3	C1Ir1Mo3	C	1	Ir	1	Mo	3																			1971																																													cubic	K		3.2					3.2																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100758	793		C1Ir2Mo3	C1Ir2Mo3	C	1	Ir	2	Mo	3																			1971																																													cubic	K		1.8					1.8																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100759	632		C1In1Zr2	C1In1Zr2	C	1	In	1	Zr	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100760	870		C1.35In0.15Y0.85	C1.35In0.15Y0.85	C	1.35	In	0.15	Y	0.85																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100761	632		C1In1Nb2	C1In1Nb2	C	1	In	1	Nb	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100762	1564		C1In1La3	C1In1La3	C	1	In	1	La	3																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100763	1222		C3Ho0.2Th1.8	C3Ho0.2Th1.8	C	3	Ho	0.2	Th	1.8																			1973																												Pu2C3																	Pu2C3, D5[c]	K		5.4					5.4																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100764	1222		C3Ho0.4Th1.6	C3Ho0.4Th1.6	C	3	Ho	0.4	Th	1.6																			1973																												Pu2C3																	Pu2C3, D5[c]	K		5.5					5.5																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100765	1222		C3Ho0.6Th1.4	C3Ho0.6Th1.4	C	3	Ho	0.6	Th	1.4																			1973																												Pu2C3																	Pu2C3, D5[c]	K		5.2					5.2																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100766	784		C2Ho1	C2Ho1	C	2	Ho	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100767	558		C1Hf0.6Zr0.4	C1Hf0.6Zr0.4	C	1	Hf	0.6	Zr	0.4																																															NaCl																	NaCl, B1	K					1.28																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100768	559		C1Hf0.9Nb0.1	C1Hf0.9Nb0.1	C	1	Hf	0.9	Nb	0.1																			1966																												NaCl																	NaCl, B1	K					4.2																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100769	1148	prepared at high pressure	C1.45La0.5Th0.5	C1.45La0.5Th0.5	C	1.45	La	0.5	Th	0.5																			1970																																													cubic	K		14.2					14.2																																																																																																									J.LESS-COMMON METALS,22(1970)131	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100770	1564		C1La3Sn1	C1La3Sn1	C	1	La	3	Sn	1																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100771	1564		C1La3Pb1	C1La3Pb1	C	1	La	3	Pb	1																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100772	1148	prepared at high pressure	C13La1	C13La1	C	13	La	1																					1970																																													cubic	K		4.8					4.8																																																																																																									J.LESS-COMMON METALS,22(1970)131	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100773	1148	arc melted	C1.3La1	C1.3La1	C	1.3	La	1																					1970																																													cubic	K		8.3					8.3																																																																																																									J.LESS-COMMON METALS,22(1970)131	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100774	1971		C3La2	C3La2	C	3	La	2																					1972																												Pu2C3																	Pu2C3, D5[c]	K		11					11																																																																																																					"""Superconductivity in d- and f-band metals, ed. D.H.Douglas"" 1972"				Sup. in d- & f-band metals, p=147	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
100775	1148		C1.58La1	C1.58La1	C	1.58	La	1																					1970																																													cubic	K		9.6					9.6																																																																																																									J.LESS-COMMON METALS,22(1970)131	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100776	784		C2La1	C2La1	C	2	La	1																					1968																												CaC2																	CaC2, C11[a]	K		1.44					1.44																																																																																																									J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100777	494		C16K1	C16K1	C	16	K	1																					1965																																													hexagonal	K					0.011																																																																																																							SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100778	494		C8K1	C8K1	C	8	K	1																					1965																																													hexagonal	K		0.55					0.55																																																																																																					SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100779	793		C1Ir2W3	C1Ir2W3	C	1	Ir	2	W	3																			1971																																													cubic	K		2.1					2.1																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100780	1018		C2Ir1U2	C2Ir1U2	C	2	Ir	1	U	2																			1969																																													tetragonal	K					0.3																																																																																																											PROC.NAT.ACAD.SCI.,64(1969)459	B.T.MATTHIAS,C.W.CHU,D.WOHLLENBEN,E.CORENZWIT		
100781	966		C0.64Mo1	C0.64Mo1	C	0.64	Mo	1																					1968																																													hexagonal	K		8					8																																																																																																									ACTA MET.,16(1968)1177	J.ZBASNIK,L.E.TOTH		
100782	966		C0.69Mo1	C0.69Mo1	C	0.69	Mo	1																					1968																												NaCl																	NaCl, B1	K		12.1					12.1																																																																																																									ACTA MET.,16(1968)1177	J.ZBASNIK,L.E.TOTH		
100783	1824		C0.44Mo0.56	C0.44Mo0.56	C	0.44	Mo	0.56																					1965																																														K		13					13																																																																																																									ACTA MET.,13(1965)379	E.R.PARKER,J.OLSEN,L.E.TOTH,M.WELLS,V.F.ZACKAY		
100784	1132		C1Mo2	C1Mo2	C	1	Mo	2																					1971																																													L3	K		3.45					3.45																																																																																																									J.LESS-COMMON METALS,25(1971)97	B.W.JAMES,D.G.POMFRET,G.H.WOSTENHOLM,J.L.DYKINS,M.R.DAVIS,N.MORTON		
100785	966		C1Mo2	C1Mo2	C	1	Mo	2																					1968																																													orthorhombic	K		10.8					10.8																																																																																																									ACTA MET.,16(1968)1177	J.ZBASNIK,L.E.TOTH		
100786	11		C1Mo1	C1Mo1	C	1	Mo	1																					1952																																													hexagonal	K		9.26					9.26																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100787	1006		C1Mo1	C1Mo1	C	1	Mo	1																					1967																												NaCl																	NaCl, B1	K		14.3					14.3																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
100788	1795	splat cool	C1Mn0.02Mo0.98	C1Mn0.02Mo0.98	C	1	Mn	0.02	Mo	0.98																			1966																																													cubic	K					1.7																																																																																																											TRANS.MET.SOC.AIME,236(1966)171	E.BUEHLER,R.H.WILLENS		
100789	1795		C1Mn1	C1Mn1	C	1	Mn	1																					1966																																													hexagonal	K					1.7																																																																																																											TRANS.MET.SOC.AIME,236(1966)171	E.BUEHLER,R.H.WILLENS		
100790	863		C2Lu1	C2Lu1	C	2	Lu	1																					1969																																													tetragonal	K		3.33					3.33																																																																																																									J.APPL.PHYS.,40(1969)3161	E.O.THORLAND,J.GRAOT,R.W.GREEN,S.LEGVOLD		
100791	1564		C1La3Tl1	C1La3Tl1	C	1	La	3	Tl	1																			1973																																													cubic	K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100792	1971		C1.5La0.9Th0.1	C1.5La0.9Th0.1	C	1.5	La	0.9	Th	0.1																			1972																																													cubic	K		12.9					12.9																																																																																																					"""Superconductivity in d- and f-band metals, ed. D.H.Douglas"" 1972"				Sup. in d- & f-band metals, p=147	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
100793	128		C0.5Mo0.17Zr0.42	C0.5Mo0.17Zr0.42	C	0.5	Mo	0.17	Zr	0.42																			1956																																														K		9.5					9.5																																																																																																									J.PHYS.CHEM.SOLIDS.,1(1956)188	B.T.MATTIAS,E.A.WOOD,E.CORENZWIT,V.B.BALA		
100794	870		C1.45Mo0.1Y0.9	C1.45Mo0.1Y0.9	C	1.45	Mo	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		13.8					13.8																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100795	522		C1Mo0.83Ti0.17	C1Mo0.83Ti0.17	C	1	Mo	0.83	Ti	0.17																			1963																												NaCl																	NaCl, B1	K		10.2					10.2																																																																																																									Z.METALLKDE DTSCH.,54(1963)477	U.ZWICKER		
100796	1813		C1Mo0.85Ta0.15	C1Mo0.85Ta0.15	C	1	Mo	0.85	Ta	0.15																			1966																												NaCl																	NaCl, B1	K		8.9					8.9																																																																																																									ISZ.AKAD.NAUK SSSR.NEORGAN.MATER.,2(1966)2145	I.A.SHCHERBAK,O.I.SHYLISHOVA		
100797	650		C0.6Mo4.8Si0.3	C0.6Mo4.8Si0.3	C	0.6	Mo	4.8	Si	0.3																			1966																												Mn5Si3			A	7.286		5.046											Mn5Si3, D8[8]	K		7.6					7.6																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)235	H.C.GATOS,V.SADAGOPAN		
100798	1006		C1Mo0.9Ru0.1	C1Mo0.9Ru0.1	C	1	Mo	0.9	Ru	0.1																			1967																												NaCl																	NaCl, B1	K		13.6					13.6																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
100799	793		C1Mo3Re2	C1Mo3Re2	C	1	Mo	3	Re	2																			1971																																													hexagonal	K					1																																																																																																											J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100800	1006		C1Mo0.9Re0.1	C1Mo0.9Re0.1	C	1	Mo	0.9	Re	0.1																			1967																												NaCl																	NaCl, B1	K		13.8					13.8																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
100801	793		C2Mo1Re1	C2Mo1Re1	C	2	Mo	1	Re	1																			1971																																													cubic	K		3.8					3.8																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100802	793		C1Mo3Pt2	C1Mo3Pt2	C	1	Mo	3	Pt	2																			1971																																													cubic	K		1.1					1.1																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100803	571	plus  2% VC	C0.4Mo0.6	C0.4Mo0.6	C	0.4	Mo	0.6																					1965																																														K		11.2					11.2																																																																																																					HIGH-FIELD SUPERCONDUCTIVITY OF CARBIDES				PHYS.REV.,138(1965)A1170	A.C.THORSEN,H.J.FINK		
100804	966		C0.42Mo1	C0.42Mo1	C	0.42	Mo	1																					1968																																													L'3	K		2.8					2.8																																																																																																									ACTA MET.,16(1968)1177	J.ZBASNIK,L.E.TOTH		
100805	RMP0350001		C0.05Nb5Si3	C0.05Nb5Si3	C	0.05	Nb	5	Si	3																			1963																												Mn5Si3																	Mn5Si3, D8[8]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100806	474		C1Nb2	C1Nb2	C	1	Nb	2																					1953																																													hexagonal	K		9.1			1.98		9.1																																																																																																									THIRD INTERNAT CONF.ON LOW TEMP.PHYS.,(1953)	G.HARDY,J.K.HULM		
100807	1542		C1Nb1	C1Nb1	C	1	Nb	1																					1971																												NaCl																	NaCl, B1	K		11.1					11.1																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
100808	1703		C0.98Nb1	C0.98Nb1	C	0.98	Nb	1																					1972																																														K		11.56					11.56																																																																																																									ZH.EKSP.TEOR.FIZ.,62(1972)300	A.G.RABIN'KIN,L.B.DUBROVSKSYA,P.V.GEL'D		
100809	271		C1Nb1	C1Nb1	C	1	Nb	1																					1962																																														K		12					12																																																																																																					EFFECT OF COMPOSITION ON THE SUPERCONDUCTING TRANSITION TEMPERATURE OF TANTALUM CARBIDE AND NIOBIUM CARBIDE				PHYS.REV.,125(1962)837	A.L.GIORGI,ALLEN L.BOWMAN,B.T.MATTHIAS,E.G.SZKLARZ,E.K.STORMS		
100810	1971		C0.78N0.22Th1	C0.78N0.22Th1	C	0.78	N	0.22	Th	1																			1972																												NaCl																	NaCl, B1	K		5.6					5.6																																																																																																					"""Superconductivity in d- and f-band metals, ed. D.H.Douglas"" 1972"				Sup. in d- & f-band metals, p=147	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
100811	1511		C0.2N0.8Nb0.8V0.2	C0.2N0.8Nb0.8V0.2	C	0.2	N	0.8	Nb	0.8	V	0.2																	1966																																														K		5.5					5.5																																																																																																									PHYS.,2(1966)311	J.K.HULM,N.PESSALL		
100812	1511		C0.25N0.75Nb0.85Ti0.	C0.25N0.75Nb0.85Ti0.15	C	0.25	N	0.75	Nb	0.85	Ti	0.15																	1966																																														K		17.8					17.8																																																																																																									PHYS.,2(1966)311	J.K.HULM,N.PESSALL		
100813	1038		C1N1Nb1	C1N1Nb1	C	1	N	1	Nb	1																			1965																																														K																																																																																																												Critical supercurrents in niobium carbonitrides				APPL.PHYS.LETT.,7(1965)38	C.K.LONES,H.A.JOHANSEN,J.K..HULM,N.PESSALL		
100814	1234		C0.026N0.974Nb1	C0.026N0.974Nb1	C	0.026	N	0.974	Nb	1																			1967																																														K		17.2					17.2																																																																																																									J.PHYS.CHEM.SOLIDS,28(1967)333	K.M.RALLS,M.R.PICKUS,M.W.WILLAMS		
100815	1383		C1N1Nb1	C1N1Nb1	C	1	N	1	Nb	1																			1971																																														K		17.3					17.3																																																																																																									APPL.PHYS.LETT.,19(1971)305	C.K.JONES,J.R.GAVALER,M.A.JANOCKO		
100816	559		C0.35N0.65Nb1	C0.35N0.65Nb1	C	0.35	N	0.65	Nb	1																			1966																												NaCl																	NaCl, B1	K		17.8					17.8																																																																																																									KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100817	1018		C2Pt1U2	C2Pt1U2	C	2	Pt	1	U	2																			1969																																													tetragonal	K		1.47					1.47																																																																																																									PROC.NAT.ACAD.SCI.,64(1969)459	B.T.MATTHIAS,C.W.CHU,D.WOHLLENBEN,E.CORENZWIT		
100818	784		C2Pr1	C2Pr1	C	2	Pr	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100819	164	ion implantation	C0.6Pd1	C0.6Pd1	C	0.6	Pd	1																					1975																																														K		1.3					1.3																																																																																																									PHYS.LETT.A,51(1975)147	B.STRIZKER,J.BECKER		
100820	632		C1Pb1Ti2	C1Pb1Ti2	C	1	Pb	1	Ti	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100821	793		C1Os2W3	C1Os2W3	C	1	Os	2	W	3																			1971																																													cubic	K		2.9					2.9																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100822	1018		C2Os1U2	C2Os1U2	C	2	Os	1	U	2																			1969																																													tetragonal	K					0.3																																																																																																											PROC.NAT.ACAD.SCI.,64(1969)459	B.T.MATTHIAS,C.W.CHU,D.WOHLLENBEN,E.CORENZWIT		
100823	1222		C3Nd0.2Th1.8	C3Nd0.2Th1.8	C	3	Nd	0.2	Th	1.8																			1973																																													D5[d]	K					4																																																																																																											J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100824	784		C2Nd1	C2Nd1	C	2	Nd	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100825	870		C1.35Nb0.1Y0.9	C1.35Nb0.1Y0.9	C	1.35	Nb	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		10.8					10.8																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100826	559		C1Nb0.1Ti0.9	C1Nb0.1Ti0.9	C	1	Nb	0.1	Ti	0.9																			1966																												NaCl																	NaCl, B1	K					4.2																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100827	990		C1Nb0.4Ta0.6	C1Nb0.4Ta0.6	C	1	Nb	0.4	Ta	0.6																			1967																																													cubic	K		10					10																																																																																																									PHYS.LETT.A,25(1967)542	R.E.GLOVER		
100828	632		C1Nb2Sn1	C1Nb2Sn1	C	1	Nb	2	Sn	1																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
100829	1018		C2Ru1U2	C2Ru1U2	C	2	Ru	1	U	2																			1969																																													tetragonal	K					0.3																																																																																																											PROC.NAT.ACAD.SCI.,64(1969)459	B.T.MATTHIAS,C.W.CHU,D.WOHLLENBEN,E.CORENZWIT		
100830	112		C1Ru1	C1Ru1	C	1	Ru	1																					1931																																														K		2.04			1.9		2.04																																																																																																									ROY.SOC.CAN.TRANS.,25(1931)13	J.C.MCLENNAN,J.F.ALLEN,J.O.WILHELM		
100831	1018		C2Rh1U2	C2Rh1U2	C	2	Rh	1	U	2																			1969																																													tetragonal	K					0.3																																																																																																											PROC.NAT.ACAD.SCI.,64(1969)459	B.T.MATTHIAS,C.W.CHU,D.WOHLLENBEN,E.CORENZWIT		
100832	1735	prepared at P=160-180 kbar, T=1000C. 	C1Rh1	C1Rh1	C	1	Rh	1																					1972																												NaCl																	NaCl, B1	K		3.4					3.4																																																																																																									ZH.ETF PIS.RED.,16(1972)609	L.G.KHVOSTANTSEV,L.N.FOMICHEVA,S.V.POPOVA		
100833	1735		C1Rh1	C1Rh1	C	1	Rh	1																					1972																												TiAs																	TiAs, B[i]	K		1.6					1.6																																																																																																									ZH.ETF PIS.RED.,16(1972)609	L.G.KHVOSTANTSEV,L.N.FOMICHEVA,S.V.POPOVA		
100834	870		C1.35Re0.3Y0.7	C1.35Re0.3Y0.7	C	1.35	Re	0.3	Y	0.7																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100835	793		C1Re2W3	C1Re2W3	C	1	Re	2	W	3																			1971																												beta-Mn																	beta-Mn, A13	K					1																																																																																																											J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100836	793		C2Re1W1	C2Re1W1	C	2	Re	1	W	1																			1971																																													cubic	K		3.8					3.8																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100837	712		C0.04Re0.96	C0.04Re0.96	C	0.04	Re	0.96																																																																			K		1.98					1.98																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
100838	494		C16Rb1	C16Rb1	C	16	Rb	1																					1965																																														K					0.011																																																																																																							SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100839	494		C8Rb1	C8Rb1	C	8	Rb	1																					1965																																														K		0.023					0.023																																																																																																					SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
100840	793		C1Pt2W3	C1Pt2W3	C	1	Pt	2	W	3																			1971																																													cubic	K		1.2					1.2																																																																																																									J.LESS-COMMON METALS,23(1971)103	A.C.LAWSON		
100841	1961		C0.754Ta1	C0.754Ta1	C	0.754	Ta	1																					1968																												NaCl																	NaCl, B1	K					1.05																																																																																																											PROC.BRITISH CERAMIC SOC.,10(1968)183-193	A.L.GIORGI,E.G.SZKLARZ,T.C.WALLACE		
100842	1542		C1Ta1	C1Ta1	C	1	Ta	1																					1971																												NaCl																	NaCl, B1	K		10.35					10.35																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
100843	870		C1.35Sn0.1Y0.9	C1.35Sn0.1Y0.9	C	1.35	Sn	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		10.2					10.2																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100844	784		C2Sm1	C2Sm1	C	2	Sm	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100845	870		C1.35Si0.1Y0.9	C1.35Si0.1Y0.9	C	1.35	Si	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		11.3					11.3																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100846	RMP0350001		C0.05Si3V5	C0.05Si3V5	C	0.05	Si	3	V	5																			1963																												Mn5Si3																	Mn5Si3, D8[8]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100847	11		C1Si1	C1Si1	C	1	Si	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100848	1222		C3Sc1.4Th0.6	C3Sc1.4Th0.6	C	3	Sc	1.4	Th	0.6																			1973																																														K		5.4					5.4																																																																																																									J.LESS-COMMON METALS,30(1973)217	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA		
100849	871		C3Sc4	C3Sc4	C	3	Sc	4																					1969																																													cubic	K					1																																																																																																											J.LESS-COMMON METLS,19(1969)253	A.L.GIORGI,B.T.MATTHIAS,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100850	558		C0.96Sc1	C0.96Sc1	C	0.96	Sc	1																																																	NaCl																	NaCl, B1	K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100851	870		C1.35Ru0.3Y0.7	C1.35Ru0.3Y0.7	C	1.35	Ru	0.3	Y	0.7																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100852	870		C1.35Ru0.1Y0.9	C1.35Ru0.1Y0.9	C	1.35	Ru	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		11.2					11.2																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100853	870		C1.55Th0.3Y0.7	C1.55Th0.3Y0.7	C	1.55	Th	0.3	Y	0.7																			1969																												Pu2C3																	Pu2C3, D5[c]	K		17					17																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100854	1148		C1.45Th1	C1.45Th1	C	1.45	Th	1																					1970																																													cubic	K		4.1			3.9		4.1																																																																																																									J.LESS-COMMON METALS,22(1970)131	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100855	1971		C1Th1	C1Th1	C	1	Th	1																					1972																												NaCl																	NaCl, B1	K					1.2																																																																																																							"""Superconductivity in d- and f-band metals, ed. D.H.Douglas"" 1972"				Sup. in d- & f-band metals, p=147	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
100856	633		C1Tc1	C1Tc1	C	1	Tc	1																					1966																																													cubic	K		3.85					3.85																																																																																																									J.Less-Common Metals, 11(1966)455	A.L.Giorgi,E.G.Szklarz		
100857	784		C2Tb1	C2Tb1	C	2	Tb	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100858	559		C1Ta0.2Zr0.8	C1Ta0.2Zr0.8	C	1	Ta	0.2	Zr	0.8																			1966																												NaCl																	NaCl, B1	K					4.2																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100859	694		C1Ta0.5W0.5	C1Ta0.5W0.5	C	1	Ta	0.5	W	0.5																			1966																																														K		10.1					10.1																																																																																																									ACTA MET.,14(1966)1403	C.M.YEN,C.P.WANG,L.E.TOTH		
100860	128		C1Ta0.45W0.55	C1Ta0.45W0.55	C	1	Ta	0.45	W	0.55																			1956																																														K		10.5					10.5																																																																																																									J.PHYS.CHEM.SOLIDS.,1(1956)188	B.T.MATTIAS,E.A.WOOD,E.CORENZWIT,V.B.BALA		
100861	558		C1Ta0.4Ti0.6	C1Ta0.4Ti0.6	C	1	Ta	0.4	Ti	0.6																																															NaCl																	NaCl, B1	K		4.8					4.8																																																																																																									INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100862	505	sputtered film, d=947 A.	C1Ta1	C1Ta1	C	1	Ta	1																					1964																												NaCl																	NaCl, B1	K		5.09					5.09																																																																																																									J.ELECTROCHEM.SOC.,111(1964)936	D.GERSTENBERG,P.M.HALL		
100863	10		C1Ta2	C1Ta2	C	1	Ta	2																					1954																																													L'3	K		3.26					3.26																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100864	967		C0.47Ta1	C0.47Ta1	C	0.47	Ta	1																					1968																												CdI2																	CdI2, C6	K					1.6																																																																																																											ACTA MET.,16(1968)1183	L.E.TOTH,M.ISHIKAWA,Y.A.CHANG		
100865	870		C1.45U0.15Y0.85	C1.45U0.15Y0.85	C	1.45	U	0.15	Y	0.85																			1969																												Pu2C3																	Pu2C3, D5[c]	K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100866	10		C1U1	C1U1	C	1	U	1																					1954																												NaCl																	NaCl, B1	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100867	784		C2Tm1	C2Tm1	C	2	Tm	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100868	558		C0.8Zr0.2	C0.8Zr0.2	C	0.8	Zr	0.2																																																	NaCl																	NaCl, B1	K					1.28																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100869	558		C0.6Zr0.4	C0.6Zr0.4	C	0.6	Zr	0.4																																																	NaCl																	NaCl, B1	K					1.28																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100870	870		C1.35Ti0.1Y0.9	C1.35Ti0.1Y0.9	C	1.35	Ti	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		10.7					10.7																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100871	870		C1.5Ti0.3Y0.7	C1.5Ti0.3Y0.7	C	1.5	Ti	0.3	Y	0.7																			1969																												Pu2C3																	Pu2C3, D5[c]	K		12.9					12.9																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100872	558		C1Ti0.8W0.2	C1Ti0.8W0.2	C	1	Ti	0.8	W	0.2																																															NaCl																	NaCl, B1	K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100873	10		C1Ti1	C1Ti1	C	1	Ti	1																					1954																												NaCl																	NaCl, B1	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100874	870		C1.65Th0.4Y0.6	C1.65Th0.4Y0.6	C	1.65	Th	0.4	Y	0.6																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100875	870		C1.55Th0.7Y0.3	C1.55Th0.7Y0.3	C	1.55	Th	0.7	Y	0.3																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100876	870		C1.35Th0.9Y0.1	C1.35Th0.9Y0.1	C	1.35	Th	0.9	Y	0.1																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100877	2.64	broad transition	C1W2	C1W2	C	1	W	2																																																																		cubic	K		5.2					5.2																																																																																																												
100878	1223		C1W2	C1W2	C	1	W	2																					1972																																													orthorhombic	K		4.05					4.05																																																																																																									J.LESS-COMMON METALS,29(1972)423	B.W.JAMES,D.C.B.HEPBURN,G.H.WOSTERHOLM,N.MORTON		
100879	1132		C1W2	C1W2	C	1	W	2																					1971																																													hexagonal	K		3.35					3.35																																																																																																									J.LESS-COMMON METALS,25(1971)97	B.W.JAMES,D.G.POMFRET,G.H.WOSTENHOLM,J.L.DYKINS,M.R.DAVIS,N.MORTON		
100880	11		C1W2	C1W2	C	1	W	2																					1952																																													L'3	K		2.74					2.74																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100881	1037		C1W1	C1W1	C	1	W	1																					1965																																														K					0.3																																																																																																							Geballe & Hull quoted in this Paper (From Roberts' Table. )				Appl.Phys.Lett., 7(1965)25	R.H.Willens,E.Buehler		
100882	1036		C0.46W0.54	C0.46W0.54	C	0.46	W	0.54																					1965																												Cu																	Cu, A1	K		9					9																																																																																																									APPL.PHYS.LETT.,7(1965)25	E.BUEHLER,R.H.WILLENS		
100883	1036		C0.55W0.45	C0.55W0.45	C	0.55	W	0.45																					1965																												Cu																	Cu, A1	K		8.1					8.1																																																																																																									APPL.PHYS.LETT.,7(1965)25	E.BUEHLER,R.H.WILLENS		
100884	1036		C0.5W0.5	C0.5W0.5	C	0.5	W	0.5																					1965																												Cu																	Cu, A1	K		10					10																																																																																																									APPL.PHYS.LETT.,7(1965)25	E.BUEHLER,R.H.WILLENS		
100885	558		C1V0.4Zr0.6	C1V0.4Zr0.6	C	1	V	0.4	Zr	0.6																																															NaCl																	NaCl, B1	K					4.2																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100886	870		C1.45V0.1Y0.9	C1.45V0.1Y0.9	C	1.45	V	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		11.5					11.5																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100887	559		C0.922V1	C0.922V1	C	0.922	V	1																					1966																																														K					1.28																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
100888	10		C1V2	C1V2	C	1	V	2																					1954																																													hexagonal	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100889	RMP0350001		Ca1Ga2	Ca1Ga2	Ca	1	Ga	2																					1963																												AlB2																	AlB2, C32	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100890	486		Ca1Cu5	Ca1Cu5	Ca	1	Cu	5																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100891	10		C1Zr1	C1Zr1	C	1	Zr	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
100892	784		C2Yb1	C2Yb1	C	2	Yb	1																					1968																																														K					2																																																																																																											J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100893	870		C1.35Y0.8Zn0.2	C1.35Y0.8Zn0.2	C	1.35	Y	0.8	Zn	0.2																			1969																																														K					4																																																																																																											J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100894	870		C1.45y0.9Zn0.1	C1.45Y0.9Zn0.1	C	1.45	Y	0.9	Zn	0.1																			1969																												Pu2C3																	Pu2C3, D5[c]	K		13					13																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100895	870		C1.45Y1	C1.45Y1	C	1.45	Y	1																					1969																												Pu2C3																	Pu2C3, D5[c]	K		11.5					11.5																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100896	558		C0.92Y1	C0.92Y1	C	0.92	Y	1																																																	NaCl																	NaCl, B1	K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100897	711		C1Y3	C1Y3	C	1	Y	3																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
100898	868	P=15-25 kbar, broad transition.	C3Y2	C3Y2	C	3	Y	2																					1969																												Pu2C3																	Pu2C3, D5[c]	K		11.5					11.5																																																																																																									J.LESS-COMMON METALS,17(1969)91	A.L.GIORGI,M.C.KRUPKA,M.H.KRIKORIANE.G.SZKLARZ		
100899	784		C2Y1	C2Y1	C	2	Y	1																					1968																												CaC2																	CaC2, C11[a]	K		3.75					3.75																																																																																																									J.LESS-COMMON METALS,14(1968)247	A.L.GIORGI,E.G.SZKLARZ,M.C.KRUPKA,N.H.KRIKORIAN,T.C.WALLACE		
100900	870		C1.55w0.1Y0.9	C1.55W0.1Y0.9	C	1.55	W	0.1	Y	0.9																			1969																												Pu2C3																	Pu2C3, D5[c]	K		14.5					14.5																																																																																																									J.LESS-COMMON METALS, 19(1969)113	A.L.GIORGI,E.G.SZKLLARZ,M.C.KRUPKA,N.H.KRIKORIAN		
100901	1607		Cd1	Cd1	Cd	1																							1970																												Mg																	Mg, A3	K		0.517					0.517																																																																																																									PHYS.REV.B,2(1970)442	J.R.DILLINGER,R.E.FASSNACHT		
100902	486		Ca1Zn5	Ca1Zn5	Ca	1	Zn	5																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
100903	715		Ca1Tl3	Ca1Tl3	Ca	1	Tl	3																					1970																												AuCu3																	AuCu3, L1[2]	K		2.04					2.04																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100904	961		Ca1Si2	Ca1Si2	Ca	1	Si	2																					1967																												ThSi2																	ThSi2, C[c]	K		1.58					1.58																																																																																																									J.LESS-COMMON METALS,12(1967)75	D.B.MCWHAN,J.R.SOULEN,M.S.SILVERMAN,V.B.COMPTON		
100905	961		Ca1Si2	Ca1Si2	Ca	1	Si	2																					1967																												CaSi2																	CaSi2, C12	K					0.32																																																																																																											J.LESS-COMMON METALS,12(1967)75	D.B.MCWHAN,J.R.SOULEN,M.S.SILVERMAN,V.B.COMPTON		
100906	427		Ca1Si1	Ca1Si1	Ca	1	Si	1																					1962																																													orthorhombic	K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100907	427		Ca2Si1	Ca2Si1	Ca	2	Si	1																					1962																																													cubic	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100908	2		Ca1Se1	Ca1Se1	Ca	1	Se	1																					1948																																														K					1.7																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
100909	1232		Ca1Hg5	Ca1Hg5	Ca	1	Hg	5																					1966																																														K		1.7					1.7																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
100910	1232		Ca1Hg3	Ca1Hg3	Ca	1	Hg	3																					1966																																														K		1.6					1.6																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
100911	1232		Ca1Hg1	Ca1Hg1	Ca	1	Hg	1																					1966																												CsCl																	CsCl, B2	K		1.6					1.6																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
100912	427		Ca1Ge3	Ca1Ge3	Ca	1	Ge	3																					1962																																														K					0.15																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
100913	1340		Cd0.86Mg0.14	Cd0.86Mg0.14	Cd	0.86	Mg	0.14																					1972																																													hexagonal	K		0.145					0.145																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100914	1340		Cd0.9Mg0.1	Cd0.9Mg0.1	Cd	0.9	Mg	0.1																					1972																																														K		0.138					0.138																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100915	1340		Cd0.96Mg0.04	Cd0.96Mg0.04	Cd	0.96	Mg	0.04																					1972																																														K		0.24					0.24																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100916	RMP0350001		Cd11La1	Cd11La1	Cd	11	La	1																					1963																																													cubic	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100917	1564		Cd0.1In0.9La3	Cd0.1In0.9La3	Cd	0.1	In	0.9	La	3																			1973																												AuCu3																	AuCu3, L1[2]	K		9.55					9.55																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
100918	1506		Cd0.97Hg0.03	Cd0.97Hg0.03	Cd	0.97	Hg	0.03																					1973																																														K		0.53					0.53																																																																																																									J.LOW TEMP.PHYS.,11(1973)687	E.DUCLA-SOARES,J.D.N.CHEEKE		
100919	RMP0350001		Cd1Hg1	Cd1Hg1	Cd	1	Hg	1																					1963																																														K		2.15					2.15																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100920	1467	deposited at 1 K. 	Cd0.9Ge0.1	Cd0.9Ge0.1	Cd	0.9	Ge	0.1																					1973																																														K		1.7					1.7																																																																																																									J.LOW TEMP.PHYS.,10(1973)735	C.G.GRANQVIST,T.CLAESON		
100921	1665		Cd0.06Cu0.94Se2	Cd0.06Cu0.94Se2	Cd	0.06	Cu	0.94	Se	2																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.3					1.3																																																																																																									J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
100922	1665		Cd0.04Cu0.96S2	Cd0.04Cu0.96S2	Cd	0.04	Cu	0.96	S	2																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.3					1.3																																																																																																									J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
100923	1009		Cd1Cu1	Cd1Cu1	Cd	1	Cu	1																																																																			K					1.3																																																																																																							From Roberts' Table, unpublished results				Personal communication	D.R.O'Boyle		
100924	1609		Cd1	Cd1	Cd	1																							1960																												Mg																	Mg, A3	K		0.53					0.53																																																																																																									ZH.EKSP.TEOR.FIZ.,39(1960)1193	N.V.ZAVARITSKII		
100925	1491	quench condensed at 0.4 K.	Cd0.1Pd0.9	Cd0.1Pd0.9	Cd	0.1	Pd	0.9																					1973																																														K		6.92					6.92																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
100926	119		Cd1O1	Cd1O1	Cd	1	O	1																					1948																																														K					1.3																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
100927	258		Cd2Na1	Cd2Na1	Cd	2	Na	1																																																																			K					1.06																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
100928	258		Cd6Na1	Cd6Na1	Cd	6	Na	1																																																																			K					1.08																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
100929	614	P=0-22 kbar	Cd1Mo5S6	Cd1Mo5S6	Cd	1	Mo	5	S	6																			1975																																														K		3.7					3.7																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
100930	1163		Cd1Mo5S6	Cd1Mo5S6	Cd	1	Mo	5	S	6																			1972																																													rhombohedral	K		2.4					2.4																																																																																																									SCI.,175(1972)1465	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO		
100931	1340		Cd0.2Mg0.08	Cd0.2Mg0.08	Cd	0.2	Mg	0.08																					1972																																													hexagonal	K					0.015																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100932	1340		Cd0.5Mg0.5	Cd0.5Mg0.5	Cd	0.5	Mg	0.5																					1972																																													orthorhombic	K					0.015																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100933	1340		Cd0.6Mg0.4	Cd0.6Mg0.4	Cd	0.6	Mg	0.4																					1972																																													orthorhombic	K		0.016					0.016																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100934	1340		Cd0.7Mg0.3	Cd0.7Mg0.3	Cd	0.7	Mg	0.3																					1972																																														K		0.105					0.105																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100935	1340		cd0.75Mg0.25	Cd0.75Mg0.25	Cd	0.75	Mg	0.25																					1972																																													hexagonal	K		0.16					0.16																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100936	1340		Cd0.8Mg0.2	Cd0.8Mg0.2	Cd	0.8	Mg	0.2																					1972																																													hexagonal	K		0.185					0.185																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
100937	656		Ce1	Ce1	Ce	1																																																			Cu																	Cu, A1	K					0.4																																																																																																							quoted in J.Phys.Chem.Solids 28(1967)1846				Unpublished	J.C.Ho,N.E.Phillips,T.F.Smith		
100938	23		Ce1	Ce1	Ce	1																							1951																												Cu																	Cu, A1	K					0.25																																																																																																											Nature, 167(1951)111	B.B.Goodman		
100939	1917	weight fraction 	Cd0.825Zn0.175	Cd0.825Zn0.175	Cd	0.825	Zn	0.175																					1969																																														K					1.3																																																																																																											REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100940	1052		Cd0.2Zn0.8	Cd0.2Zn0.8	Cd	0.2	Zn	0.8																					1969																																														K		0.628					0.628																																																																																																									CRYOGENICS,9(1969)63	C.C.ACKERMAN,L.D.ALLEN,W.C.OVERTON		
100941	1052		Cd0.002Zn0.998	Cd0.002Zn0.998	Cd	0.002	Zn	0.998																					1969																																														K		0.78					0.78																																																																																																									CRYOGENICS,9(1969)63	C.C.ACKERMAN,L.D.ALLEN,W.C.OVERTON		
100942	1052		Cd0.02Zn0.98	Cd0.02Zn0.98	Cd	0.02	Zn	0.98																					1969																																														K		0.675					0.675																																																																																																									CRYOGENICS,9(1969)63	C.C.ACKERMAN,L.D.ALLEN,W.C.OVERTON		
100943	825		Cd1V3	Cd1V3	Cd	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K					4.2																																																																																																											DOKL.AN SSR,171(1966)331	E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
100944	1900	deposited at 0.3 K. 	Cd0.1Tl0.9	Cd0.1Tl0.9	Cd	0.1	Tl	0.9																					1974																																														K		3.5					3.5																																																																																																									Z.PHYS.,269(1974)23	C.G.GRANQVIST,T.CLAAESON		
100945	70		Cd0.17Tl0.83	Cd0.17Tl0.83	Cd	0.17	Tl	0.83																					1929																																														K		2.3					2.3																																																																																																									Proc.Acad.Sci.Amsterdam, 32(1929)715	W.J.DeHaas,E. Van Aubel,J.Voogd		
100946	70		Cd0.18Sn0.72	Cd0.18Sn0.72	Cd	0.18	Sn	0.72																					1929																																														K		3.65					3.65																																																																																																									Proc.Acad.Sci.Amsterdam, 32(1929)715	W.J.DeHaas,E. Van Aubel,J.Voogd		
100947	99		Cd0.4Sb0.6	Cd0.4Sb0.6	Cd	0.4	Sb	0.6																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100948	1917	weight fraction 	Cd0.18Pb0.32Sn0.5	Cd0.18Pb0.32Sn0.5	Cd	0.18	Pb	0.32	Sn	0.5																			1969																																														K		7.5					7.5																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
100949	469		Ce1Ir3	Ce1Ir3	Ce	1	Ir	3																					1965																																														K		3.34					3.34																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100950	469		Ce1Ir2	Ce1Ir2	Ce	1	Ir	2																					1965																												MgCu2(Laves)																	MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100951	715		Ce1In3	Ce1In3	Ce	1	In	3																					1970																												AuCu3																	AuCu3, L1[2]	K					0.07																																																																																																											J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100952	68		Ce0.975Fe0.025	Ce0.975Fe0.025	Ce	0.975	Fe	0.025																					1948																																														K					2																																																																																																											J.Chem.Phys., 16(1948)838	W.T.Ziegler		
100954	113		Ce0.35Eu0.02Gd0.06La	Ce0.35Eu0.02Gd0.06La0.2	Ce	0.35	Eu	0.02	Gd	0.06	La	0.2																	1929																																														K					2.3																																																																																																											ROY.SOC.CAN.TRANS.,23(1929)287	J.C.MCLENNAN,J.O.WILHELM,L.E.HOWLETT		
100955	655		Ce1Co1.33Rh0.67	Ce1Co1.33Rh0.67	Ce	1	Co	1.33	Rh	0.67																			1967																												MgCu2(Laves)																	MgCu2, C15	K					0.33																																																																																																											J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100956	655		Ce1Co1.67Rh0.33	Ce1Co1.67Rh0.33	Ce	1	Co	1.67	Rh	0.33																			1967																												MgCu2(Laves)																	MgCu2, C15	K		0.47					0.47																																																																																																									J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100957	655		Ce1Co1.33Ni0.67	Ce1Co1.33Ni0.67	Ce	1	Co	1.33	Ni	0.67																			1967																												MgCu2(Laves)																	MgCu2, C15	K					0.33																																																																																																											J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100958	655		Ce1Co1.67Ni0.33	Ce1Co1.67Ni0.33	Ce	1	Co	1.67	Ni	0.33																			1967																												MgCu2(Laves)																	MgCu2, C15	K		0.46					0.46																																																																																																									J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100959	655		Ce1Co2	Ce1Co2	Ce	1	Co	2																					1967																												MgCu2(Laves)																	MgCu2, C15	K		1.5					1.5																																																																																																									J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100960	618	P-induced s/c. P<crit>=50kbar. for high pressure phase. 	Ce1	Ce1	Ce	1																							1968																																														K		1.7			0		1.7																																																																																																					SUPERCONDUCTIVITY OF CERIUM UNDER PRESSURE				PHYS.REV.LETT.,21(1968)1250	JORG WITTING		
100961	1783		Ce1Pt0.1Ru1.9	Ce1Pt0.1Ru1.9	Ce	1	Pt	0.1	Ru	1.9																			1972																												MgCu2(Laves)																	MgCu2, C15	K		4.08					4.08																																																																																																									PHYS.REV.B,6(1972)3286	D.C.KOSHIMAKI,K.A.GSCHNEIDNER,R.R.JOSEPH		
100962	469		Ce1Pt5	Ce1Pt5	Ce	1	Pt	5																					1965																												CeCo3B2			A	5.369		4.385											CeCo3B2, CaCu5, D2[d]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100963	469		Ce1Pt3	Ce1Pt3	Ce	1	Pt	3																					1965																												MgCu2(Laves)																	MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100964	469		Ce1Pt2	Ce1Pt2	Ce	1	Pt	2																					1965																												MgCu2(Laves)			A	7.73													MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100965	99		Ce1Pb1	Ce1Pb1	Ce	1	Pb	1																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
100966	RMP0350001		Ce1Os2	Ce1Os2	Ce	1	Os	2																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.62																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100967	655		Ce1Ni2	Ce1Ni2	Ce	1	Ni	2																					1967																												MgCu2(Laves)																	MgCu2, C15	K					0.015																																																																																																											J.PHYS.CHEM.SOLIDS,28(1967)1846	G.F.SMITH,I.R.HARRIS		
100968	40		Ce1N0.87	Ce1N0.87	Ce	1	N	0.87																					1953																																														K					1.8																																																																																																							Studies of compounds for superconductivity				Phys.Rev., 90(1953)115	W.T.Ziegler,R.A.Young		
100969	1016	P-0-10-24 kbar	Ce0.02La-.98	Ce0.02La0.98	Ce	0.02	La	0.98																					1969																																														K		2.6					2.6																																																																																																									PHYS.REV.LETT.,23(1969)1375	J.WITTIG,K.S.KIM,M.B.MAPLE		
100970	1016	P=22-110 kbar	Ce0.16La0.84	Ce0.16La0.84	Ce	0.16	La	0.84																					1969																																														K		8.7					8.7																																																																																																									PHYS.REV.LETT.,23(1969)1375	J.WITTIG,K.S.KIM,M.B.MAPLE		
100971	1468		Ce0.04La0.96	Ce0.04La0.96	Ce	0.04	La	0.96																					1971																																														K					0.05																																																																																																											J.LOW TEMP.PHYS.,5(1971)191	E.UMLAUF,H.KREUZER,J.SCHNEIDER,R.MEIER		
100972	469		Ce1Ir5	Ce1Ir5	Ce	1	Ir	5																					1965																																														K		1.82					1.82																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100973	12		Co1	Co1	Co	1																							1935																												Mg																	Mg, A3	K					1.36																																																																																																											Proc.Roy.Soc.(London),151(1935)A610	N.Kurti,F.Simon		
100974	1477	not SC(resistivity)	(Y,Ce)	Ce0.0178Y1	Ce	0.0178	Y	1																					1971																																														K					1.5																																																																																																											J.LOW TEMP.PHYS.,4(1971)657	S.YOSHIDA,T.SUGAWARA		
100975	1811		Ce0.8Tb0.2Ru2	Ce0.8Tb0.2Ru2	Ce	0.8	Tb	0.2	Ru	2																			1974																																														K		2.6					2.6																																																																																																									W.J.APPL.CRYST.,7(1974)230	K.IBEL,S.ROTH,W.JUST		
100976	715		Ce1Sn3	Ce1Sn3	Ce	1	Sn	3																					1970																												AuCu3																	AuCu3, L1[2]	K					0.07																																																																																																											J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
100977	1913		Ce0.12Si1V2.88	Ce0.12Si1V2.88	Ce	0.12	Si	1	V	2.88																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		15.32					15.32																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
100978	25		Ce1Si2	Ce1Si2	Ce	1	Si	2																					1958																												ThSi2																	ThSi2, C[c]	K					1																																																																																																							Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
100979	11		Ce0.25Sb3	Ce0.25Sb3	Ce	0.25	Sb	3																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
100980	558		Ce2S3	Ce2S3	Ce	2	S	3																																																																		cubic	K																																																																																																																INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
100981	258		Ce1S1	Ce1S1	Ce	1	S	1																																																	NaCl																	NaCl, B1	K					1.06																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
100982	1820		Ce1Ru2Sc1	Ce1Ru2Sc1	Ce	1	Ru	2	Sc	1																			1971																												MgCu2(Laves)																	MgCu2, C15	K		6.2					6.2																																																																																																									Z.NATURFORSCH.A,26(1971)141	B.Z.HILLENBRAND,M.WILHELM		
100983	1783		Ce1Ru2	Ce1Ru2	Ce	1	Ru	2																					1972																																														K		6.18					6.18																																																																																																									PHYS.REV.B,6(1972)3286	D.C.KOSHIMAKI,K.A.GSCHNEIDNER,R.R.JOSEPH		
100984	1783		Ce1Pt0.2Ru1.8	Ce1Pt0.2Ru1.8	Ce	1	Pt	0.2	Ru	1.8																			1972																												MgCu2(Laves)																	MgCu2, C15	K		3.4					3.4																																																																																																									PHYS.REV.B,6(1972)3286	D.C.KOSHIMAKI,K.A.GSCHNEIDNER,R.R.JOSEPH		
100985	469		Co2Lu1	Co2Lu1	Co	2	Lu	1																					1965																												MgCu2(Laves)			A	7.123													MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
100986	658		Co1La3	Co1La3	Co	1	La	3																					1967																												Al3Ni																	Al3Ni, D0[11]	K		4.28					4.28			K/GPa	0.085																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
100987	1624		Co0.004Ir0.996	Co0.004Ir0.996	Co	0.004	Ir	0.996																					1971																																														K		0.046					0.046																																																																																																									PHYS.REV.B,3(1971)91	G.RIBLET.		
100988	351	deposited at 6 K. 	Co0.03In0.97	Co0.03In0.97	Co	0.03	In	0.97																					1955																																														K		3.95					3.95																																																																																																									Z.PHYS.,141(1955)263	W.OPITZ		
100989	RMP0350001		Co1Hf2	Co1Hf2	Co	1	Hf	2																					1963																												Fe3W3C																	Fe3W3C, E9[3]	K		0.56					0.56																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100990	770		Co1Ge2	Co1Ge2	Co	1	Ge	2																					1970																																														K					0.051																																																																																																											PROG.IN LOW TEMP.PHYS.,6(1970)205	C.K.JONES,D.W.DEIS,J.K.HULM,M.ASHKIN		
100991	RMP0350001		Co1Ge3	Co1Ge3	Co	1	Ge	3																					1963																																													orthorhombic	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
100992	1181		Co0.98Fe0.02U1	Co0.98Fe0.02U1	Co	0.98	Fe	0.02	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
100993	1866		Co0.5Fe0.5U6	Co0.5Fe0.5U6	Co	0.5	Fe	0.5	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		3					3																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
100994	1392		Co0.5Fe0.5Ti1	Co0.5Fe0.5Ti1	Co	0.5	Fe	0.5	Ti	1																			1967																																														K		3.3					3.3																																																																																																									J.APPL.PHYS.,38(1967)1337	B.F.DESAVAGE,J.F.GOFF		
100995	984		Co0.02Cu0.98Rh2Si4	Co0.02Cu0.98Rh2Si4	Co	0.02	Cu	0.98	Rh	2	Si	4																	1967																												Al2MgO4																	Al2MgO4, H1[1]	K		3.8					3.8																																																																																																					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
100996	1181		Co0.98Cr0.02U1	Co0.98Cr0.02U1	Co	0.98	Cr	0.02	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
100997	914		Co0.5Ni0.5Zr2	Co0.5Ni0.5Zr2	Co	0.5	Ni	0.5	Zr	2																			1969																												CuAl2																	CuAl2, C16	K		3.1					3.1																																																																																																									J.PHYS.SOC.JAPAN,26(1969)866	K.YAMAYA,T.MITSUI,T.SAMBONGI		
100998	1001		Co0.3Ni0.7V3	Co0.3Ni0.7V3	Co	0.3	Ni	0.7	V	3																			1963																												Cr3Si(A15)																	Cr3Si, A15	K					2																																																																																																											TRANS.AIME,227(1963)1407	J.W.DOWNEY,S.T.ZEGLER		
100999	1001		Co0.5Ni0.5V3	Co0.5Ni0.5V3	Co	0.5	Ni	0.5	V	3																			1963																												Cr3Si(A15)																	Cr3Si, A15	K					2																																																																																																											TRANS.AIME,227(1963)1407	J.W.DOWNEY,S.T.ZEGLER		
101000	1181		Co0.98Ni0.02U1	Co0.98Ni0.02U1	Co	0.98	Ni	0.02	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101001	RMP0350001		Co1Nb1V1	Co1Nb1V1	Co	1	Nb	1	V	1																			1963																												MgZn2(Laves)																	MgZn2, C14	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101002	1181		Co0.975Mo0.025U1	Co0.975Mo0.025U1	Co	0.975	Mo	0.025	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101003	1181		Co0.96Mo0.04U6	Co0.96Mo0.04U6	Co	0.96	Mo	0.04	U	6																			1970																																														K		1.5					1.5																																																																																																					LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101004	881		Co0.002Mo0.815Re0.18	Co0.002Mo0.815Re0.185	Co	0.002	Mo	0.815	Re	0.185																			1969																																														K		5.8					5.8																																																																																																									J.LOW TEMP.PHYS.,1(1969)355	H.E.HOENING,N.BARTH		
101005	920		Co0.5Mn0.5U6	Co0.5Mn0.5U6	Co	0.5	Mn	0.5	U	6																			1968																												U6Mn																	MnU6, D2[c]	K		2.55					2.55																																																																																																									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
101006	1181		Co0.92Mn0.08U6	Co0.92Mn0.08U6	Co	0.92	Mn	0.08	U	6																			1970																																														K		2.2					2.2																																																																																																					LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101007	1181		Co0.98Mn0.02U1	Co0.98Mn0.02U1	Co	0.98	Mn	0.02	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101008	469		Co1Lu3	Co1Lu3	Co	1	Lu	3																					1965																																														K																																																																																																												SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101009	260		Co1Sc1	Co1Sc1	Co	1	Sc	1																																																																			K					1.03																																																																																																											UNPUBLISHED	C.RAUB,M.F.MERRIAM		
101010	2		Co1Sb1	Co1Sb1	Co	1	Sb	1																					1948																																														K					1.8																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
101011	1476		Co0.6Rh0.4Zr2	Co0.6Rh0.4Zr2	Co	0.6	Rh	0.4	Zr	2																			1971																												CuAl2																	CuAl2, C16	K		8					8																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101012	1001		Co0.5Rh0.5V3	Co0.5Rh0.5V3	Co	0.5	Rh	0.5	V	3																			1963																												Cr3Si(A15)																	Cr3Si, A15	K					2																																																																																																											TRANS.AIME,227(1963)1407	J.W.DOWNEY,S.T.ZEGLER		
101013	1001		Co0.9Rh0.1V3	Co0.9Rh0.1V3	Co	0.9	Rh	0.1	V	3																			1963																												Cr3Si(A15)																	Cr3Si, A15	K					2																																																																																																											TRANS.AIME,227(1963)1407	J.W.DOWNEY,S.T.ZEGLER		
101014	1181		Co0.97Rh0.03U1	Co0.97Rh0.03U1	Co	0.97	Rh	0.03	U	1																			1970																																														K																																																																																																												LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101015	1181		Co0.94RH0.06U6	Co0.94Rh0.06U6	Co	0.94	Rh	0.06	U	6																			1970																																														K		2					2																																																																																																					LT-12				LT-12(1970, Kyoto) P 345	B.R.COLES		
101016	1060		Co0.05Rh0.04Ti0.91	Co0.05Rh0.04Ti0.91	Co	0.05	Rh	0.04	Ti	0.91																			1964																																														K		4					4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101017	95		Co0.5Rh0.5Si2	Co0.5Rh0.5Si2	Co	0.5	Rh	0.5	Si	2																			1955																																														K		2					2																																																																																																					From Roberts' Table				Naturwiss, 42(1955)451	W.Buckel		
101018	601		Co2P1	Co2P1	Co	2	P	1																					1965																												Co2Si																	Co2Si, C23	K					0.97																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101019	11		Co1O1	Co1O1	Co	1	O	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101020	1355		Co0.85Ni0.15Zr2	Co0.85Ni0.15Zr2	Co	0.85	Ni	0.15	Zr	2																			1970																												CuAl2																	CuAl2, C16	K		6					6																																																																																																									J.PHYS.SOC.JAPAN,29(1970)879	K.YAMAYA,T.MITSUI,T.SAMGONGI		
101021	RMP0350001		Co1Ti1	Co1Ti1	Co	1	Ti	1																					1963																												W																	W, A2	K		0.71					0.71																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101022	173		Co3Th7	Co3Th7	Co	3	Th	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		1.83					1.83																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101023	1377		Co1Ta1.75Zr0.25	Co1Ta1.75Zr0.25	Co	1	Ta	1.75	Zr	0.25																			1972																												CuAl2																	CuAl2, C16	K		0.9					0.9																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101024	1377		Co1Ta2	Co1Ta2	Co	1	Ta	2																					1972																												CuAl2																	CuAl2, C16	K		0.82					0.82																																																																		uV/K	3																																		Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101025	1362		Co0.02Sn0.98Ta3	Co0.02Sn0.98Ta3	Co	0.02	Sn	0.98	Ta	3																			1973																																														K		4					4																																																																																																									J.PHYS.SOC.JAPAN,34(1973)1168	K.ASAYAMA,S.WADA		
101026	1377		Co1Sn2	Co1Sn2	Co	1	Sn	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101027	RMP0350001		Co5.2Si2V2.8	Co5.2Si2V2.8	Co	5.2	Si	2	V	2.8																			1963																												alpha-Mn																	alpha-Mn, A12	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101028	43		Co1Si2	Co1Si2	Co	1	Si	2																					1953																												CaF2																	CaF2, C1	K		1.22					1.22																																																																																																					Superconducting properties of cobalt disilicide				Phys.Rev., 89(1953)439	B.T.Matthias,J.K.Hulm		
101029	95		Co1Si1	Co1Si1	Co	1	Si	1																					1955																																														K																																																																																																												From Roberts' Table				Naturwiss, 42(1955)451	W.Buckel		
101030	1372		Co1Sc0.12Zr1.875	Co1Sc0.125Zr1.875	Co	1	Sc	0.125	Zr	1.875																			1972																												CuAl2																	CuAl2, C16	K		2.89					2.89																																																																																																									J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
101031	469		Co1Sc3	Co1Sc3	Co	1	Sc	3																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101032	1377		Co1Sc2	Co1Sc2	Co	1	Sc	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101033	1476		Co1Zr2	Co1Zr2	Co	1	Zr	2																					1971																												CuAl2																	CuAl2, C16	K		5					5																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101034	1476		Co1Zr1	Co1Zr1	Co	1	Zr	1																					1971																												CsCl																	CsCl, B2	K					1.2																																																																																																											J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101035	RMP0350001		Co2Zr1	Co2Zr1	Co	2	Zr	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101036	469		Co0.28Y0.72	Co0.28Y0.72	Co	0.28	Y	0.72																					1965																																														K		0.34					0.34																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101037	469		Co1Y3	Co1Y3	Co	1	Y	3																					1965																																														K		0.34					0.34																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101038	469		Cu1Y2	Cu1Y2	Cu	1	Y	2																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101039	RMP0350001		Co3V1Zr2	Co3V1Zr2	Co	3	V	1	Zr	2																			1963																												MgZn2(Laves)																	MgZn2, C14	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101040	948		Co1V3	Co1V3	Co	1	V	3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											J.PHYS.CHEM.SOLIDS, 31(1970)1531	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FLUKIGER		
101041	21		Co1U6	Co1U6	Co	1	U	6																					1958																												U6Mn																	MnU6, D2[c]	K		2.3					2.3																																																																																																									J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101042	21		Co1U1	Co1U1	Co	1	U	1																					1958																												CsCl																	CsCl, B2	K		1.7					1.7																																																																																																									J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101043	759		Co0.01Ti0.99	Co0.01Ti0.99	Co	0.01	Ti	0.99																					1964																																														K					1.5																																																																																																											PHYS.REV.,135(1964)A1151	J.A.CAPE,R.R.HAKE		
101044	173		Co1Ti2	Co1Ti2	Co	1	Ti	2																					1961																												Fe3W3C																	Fe3W3C, E9[3]	K		3.44					3.44																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101045	945		Cr3Ge1	Cr3Ge1	Cr	3	Ge	1																					1971																												Cr3Si(A15)																	Cr3Si, A15	K					1.2																																																																																																											J.PHYS.CHEM.SOLIDS,32(1971)459	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FULKIGER		
101046	10		Cr1Ge1	Cr1Ge1	Cr	1	Ge	1																					1954																												FeSi																	FeSi, B20	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101047	10		Cr0.6Ge0.4	Cr0.6Ge0.4	Cr	0.6	Ge	0.4																					1954																																													tetragonal	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101048	RMP0350001		Cr1Ga4	Cr1Ga4	Cr	1	Ga	4																					1963																																													cubic	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101049	RMP0350001		Cr3Ga1	Cr3Ga1	Cr	3	Ga	1																					1963																												Cr3Si(A15)																	Cr3Si, A15	K					0.3																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101050	1866		Cr0.2Fe0.8U6	Cr0.2Fe0.8U6	Cr	0.2	Fe	0.8	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		3.3					3.3																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101051	984		Cr0.008Cu1Rh1.992S4	Cr0.008Cu1Rh1.992S4	Cr	0.008	Cu	1	Rh	1.992	S	4																	1967																												Al2MgO4																	Al2MgO4, H1[1]	K		3.9					3.9																																																																																																					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
101052	1526		Cr1	Cr1	Cr	1																							1973																												W																	W, A2	K		3.1					3.1																																																																																																									J.VAC.SCI.TECH.,10(1973)611	P.H.SCHMIDT		
101053	788		Cr1	Cr1	Cr	1																							1969																												W																	W, A2	K					0.015																																																																																																											PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
101054	32		Co0.1Zr0.9	Co0.1Zr0.9	Co	0.1	Zr	0.9																					1955																																													hexagonal	K		3.9					3.9																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
101055	1476		Co1Zr3	Co1Zr3	Co	1	Zr	3																					1971																																														K		3.9					3.9																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101056	1476	splat cooled. 	Co1Zr2	Co1Zr2	Co	1	Zr	2																					1971																																													amorphous	K		7					7																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101057	707		Cr0.72Os0.28	Cr0.72Os0.28	Cr	0.72	Os	0.28																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		3.95					3.95																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101058	707		Cr0.67Os0.33	Cr0.67Os0.33	Cr	0.67	Os	0.33																					1969																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.03					1.03																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101059	557		Cr0.6Os0.4	Cr0.6Os0.4	Cr	0.6	Os	0.4																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.4																																																																																																											PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101060	556		Cr0.8Os0.2	Cr0.8Os0.2	Cr	0.8	Os	0.2																					1966																																													cubic	K		2.5					2.5																																																																																																									PHYS.KONDENS.MATERIE,5(1966)285	F.HEINIGER		
101061	181		Cr3O1	Cr3O1	Cr	3	O	1																																																	Cr3Si(A15)																	Cr3Si, A15	K					1.02																																																																																																							From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
101062	1979		Cr0.071Nb0.929	Cr0.071Nb0.929	Cr	0.071	Nb	0.929																					1973																																														K		6.95					6.95																																																																																																									DOK.AKAD.NAUK.BELORUSS,17(1973)497	A.K.FEDOTOV,N.N.SIROTA		
101063	1510		Cr0.03N1Nb0.97	Cr0.03N1Nb0.97	Cr	0.03	N	1	Nb	0.97																			1966																												NaCl																	NaCl, B1	K					0.32																																																																																																											PHYS.,2(1966)293	B.T.MATTHIAS,H.J.WILLIAMS,J.P.MAITA,J.P.REMEIKAA.M.CLOGSTON,T.H.GEBALLE,V.B.COMPTON		
101064	11		Cr1N1	Cr1N1	Cr	1	N	1																					1952																												NaCl																	NaCl, B1	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101065	224		Cr0.78Ir0.22	Cr0.78Ir0.22	Cr	0.78	Ir	0.22																					1962																																														K					0.3																																																																																																							SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101066	945		Cr0.835Ir0.165	Cr0.835Ir0.165	Cr	0.835	Ir	0.165																					1971																												Cr3Si(A15)																	Cr3Si, A15	K		0.77					0.77																																																																																																									J.PHYS.CHEM.SOLIDS,32(1971)459	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FULKIGER		
101067	1692		Cr0.82Ir0.18	Cr0.82Ir0.18	Cr	0.82	Ir	0.18																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		0.75					0.75																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101068	707		Cr3Ir1	Cr3Ir1	Cr	3	Ir	1																					1969																																														K		0.168					0.168																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101069	1446		Cr0.72Ru0.28	Cr0.72Ru0.28	Cr	0.72	Ru	0.28																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.468					3.468																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101070	1060		Cr0.05Rh0.04Ti0.91	Cr0.05Rh0.04Ti0.91	Cr	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.75					3.75																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101071	224		Cr0.5Rh0.5	Cr0.5Rh0.5	Cr	0.5	Rh	0.5																					1962																																														K					0.3																																																																																																							SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101072	224		Cr0.9Rh0.1	Cr0.9Rh0.1	Cr	0.9	Rh	0.1																					1962																																														K					0.3																																																																																																							SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101073	707		Cr0.75Rh0.25	Cr0.75Rh0.25	Cr	0.75	Rh	0.25																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		0.072					0.072																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101074	1096		Cr0.38Re0.62	Cr0.38Re0.62	Cr	0.38	Re	0.62																					1964																																														K		4.1					4.1																																																																																																									PHYS.KONDENS MATERIE,2(1964)377	J.MUHEIM,J.MULLER		
101075	RMP0350001		Cr1Re1	Cr1Re1	Cr	1	Re	1																					1963																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101076	224		Cr3Pt1	Cr3Pt1	Cr	3	Pt	1																					1962																												Cr3Si(A15)																	Cr3Si, A15	K					0.3																																																																																																							SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101077	707		Cr0.79Pt0.21	Cr0.79Pt0.21	Cr	0.79	Pt	0.21																					1969																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101078	945		Cr0.915Pt0.185	Cr0.915Pt0.185	Cr	0.915	Pt	0.185																					1971																												Cr3Si(A15)																	Cr3Si, A15	K					1.2																																																																																																											J.PHYS.CHEM.SOLIDS,32(1971)459	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FULKIGER		
101079	601		Cr3P1	Cr3P1	Cr	3	P	1																					1965																												Ni3P																	Ni3P, D0[e]	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101080	601		Cr1P1	Cr1P1	Cr	1	P	1																					1965																												MnP																	MnP, B31	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101081	477		Cr0.025Ti0.975	Cr0.025Ti0.975	Cr	0.025	Ti	0.975																					1965																																														K		3.5					3.5																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
101082	93		Cr1Ti3	Cr1Ti3	Cr	1	Ti	3																					1959																																														K		3.7					3.7																																																																																																					Ferromagnetic solutes in superconductors				Phys.Rev., 115(1959)1597	B.Matthias,V.B.Compton,H.Suhl,E.Corenzwit		
101083	1586	two phases	Cr2Ti1	Cr2Ti1	Cr	2	Ti	1																					1974																												MgCu2(Laves)																	MgCu2, C15	K					0.025																																																																																																											PHYS.LETT.A,50(1974)159	J.INVARSSON,O.RAPP,T.CLAESON		
101084	1913		Cr0.21Si1V2.79	Cr0.21Si1V2.79	Cr	0.21	Si	1	V	2.79																			1965																												Cr3Si(A15)																	Cr3Si, A15	K					14																																																																																																											AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101085	10		Cr1Si2	Cr1Si2	Cr	1	Si	2																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101086	10		Cr0.6Si0.4	Cr0.6Si0.4	Cr	0.6	Si	0.4																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101087	945		Cr1Si1	Cr1Si1	Cr	1	Si	1																					1971																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											J.PHYS.CHEM.SOLIDS,32(1971)459	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FULKIGER		
101088	707		Cr3Si1	Cr3Si1	Cr	3	Si	1																					1969																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101089	1987	broad transition	Cr0.03Sc0.97	Cr0.03Sc0.97	Cr	0.03	Sc	0.97																					1963																																														K		3.1					3.1																																																																																																									BULL.AMER.PHYS.SOC.II,8(1963)294	B.T.MATTHIAS,O.ARRHENIUS,TT.H.GEBALLE		
101090	11		Cr1Sb2	Cr1Sb2	Cr	1	Sb	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101091	37		Cr1Sb1	Cr1Sb1	Cr	1	Sb	1																					1953																												Fe3Zn10																	Fe3Zn10, D8[1]	K					1																																																																																																							Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
101092	224		Cr0.9Ru0.1	Cr0.9Ru0.1	Cr	0.9	Ru	0.1																					1962																																													cubic	K					0.3																																																																																																							SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101093	1532		Cs0.3Mo1S2	Cs0.3Mo1S2	Cs	0.3	Mo	1	S	2																			1974																																													hexagonal	K		6.8					6.8																																																																																																									PHYS.REV.LETT.,32(1974)712	J.A.WOOLLAM,P.O'CONNOR,R.B.SOMOANO		
101094	781	P=125 kbar	Cs1	Cs1	Cs	1																							1970																																														K																																																																																																																PHYS.REV.LETT.,24(1970)812	J.WITTIG		
101095	494		Cs1	Cs1	Cs	1																							1965																												W																	W, A2	K					0.011																																																																																																							SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
101096	RMP0350001		Cr2Zr1	Cr2Zr1	Cr	2	Zr	1																					1963																												MgZn2(Laves)																	MgZn2, C14	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101097	1586		Cr2Zr1	Cr2Zr1	Cr	2	Zr	1																					1974																												MgCu2(Laves)																	MgCu2, C15	K					0.025																																																																																																											PHYS.LETT.A,50(1974)159	J.INVARSSON,O.RAPP,T.CLAESON		
101098	1979		Cr0.099V0.901	Cr0.099V0.901	Cr	0.099	V	0.901																					1973																																														K		3.3					3.3																																																																																																									DOK.AKAD.NAUK.BELORUSS,17(1973)497	A.K.FEDOTOV,N.N.SIROTA		
101099	788		Cr0.1V0.9	Cr0.1V0.9	Cr	0.1	V	0.9																					1969																																														K		3.21					3.21																																																																																																									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
101100	700		Cr0.017U0.983	Cr0.017U0.983	Cr	0.017	U	0.983																					1966																																														K		0.75					0.75																																																																																																									SCIENCE,151(1966)985	B.T.MATTHIAS,D.K.WOHLLEBEN,E.CORENZWIT,G.W.HULL JR.,J.C.HO,K.ANDRES,N.E.PHILLIPS,T.H.GEBALLE		
101101	21		Cr0.3U0.7	Cr0.3U0.7	Cr	0.3	U	0.7																					1958																																														K					1.08																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101102	21		Cr0.6U0.4	Cr0.6U0.4	Cr	0.6	U	0.4																					1958																																														K					1.08																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101103	584		Cr0.1Ti0.3V6	Cr0.1Ti0.3V0.6	Cr	0.1	Ti	0.3	V	0.6																			1967																																														K		5.6					5.6																																																																																																					PARAMAGNETIC SUPERCONDUCTIVITY IN EXTREME TYPE-II SUPERCONDUCTORS				PHYS.REV.,158(1967)356	R.R.HAKE		
101104	477		Cr0.011Ti0.967V0.022	Cr0.011Ti0.967V0.022	Cr	0.011	Ti	0.967	V	0.022																			1965																																														K		3.6					3.6																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
101105	1604		Cu1.64Mg1Zn0.36	Cu1.64Mg1Zn0.36	Cu	1.64	Mg	1	Zn	0.36																			1974																																														K					0.03																																																																																																											PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101106	1604		Cu0.4Mg0.3Si0.3	Cu0.4Mg0.3Si0.3	Cu	0.4	Mg	0.3	Si	0.3																			1974																																														K					0.03																																																																																																											PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101107	11		Cu1Mg1Sb1	Cu1Mg1Sb1	Cu	1	Mg	1	Sb	1																			1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101108	37		Cu2Mg1	Cu2Mg1	Cu	2	Mg	1																					1953																												MgZn2(Laves)																	MgZn2, C14	K					1																																																																																																							Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
101109	1908	liquid quench	Cu0.3La0.7	Cu0.3La0.7	Cu	0.3	La	0.7																					1975																																														K		3.5					3.5																																																																																																									PHYS.REV.B,11(1975)150	P.DUWEZ,S.J.POON,W.L.JOHNSON		
101110	658		Cu1La1	Cu1La1	Cu	1	La	1																					1967																																														K		5.85					5.85			K/GPa	1.1																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101111	1374		Cu4K1S3	Cu4K1S3	Cu	4	K	1	S	3																			1952																																													tetragonal	K		1.4					1.4																																																																																																									Z.ANORG.ALLG.CHEM.,269(1952)141	M.H.VAN MAAREN		
101112	1179	deposited at 4 K.	Cu0.5Ge0.5	Cu0.5Ge0.5	Cu	0.5	Ge	0.5																					1971																																														K		3.3					3.3																																																																																																									LT-12, Tokyo (1971) 339	B.Stritzker,H.Wuhl		
101113	533		Cu3Ga1	Cu3Ga1	Cu	3	Ga	1																					1965																																														K					1.4																																																																																																											ZH.EKSP.TEOR.FIZ.,49(1965)159	N.E.ALEKSEEVSKII		
101114	RMP0350001		Cu1Ga2	Cu1Ga2	Cu	1	Ga	2																					1963																																													tetragonal	K					1.27																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101115	1526		Cu1	Cu1	Cu	1																							1973																												Cu																	Cu, A1	K					0.02																																																																																																											J.VAC.SCI.TECH.,10(1973)611	P.H.SCHMIDT		
101116	500		Cs0.32O3W1	Cs0.32O3W1	Cs	0.32	O	3	W	1																			1965																															A	7.4		7.6											hexagonal	K		1.12					1.12																																																																																																					Superconductivity of the alkali tungsten bronzes				PHYS.LETT.,15(1965)108	A.R.SWEEDLER,B.T.MATTHIAS,CH.J.RAUB		
101117	1218	deposited at 2 K.	Cu0.1Pb0.9	Cu0.1Pb0.9	Cu	0.1	Pb	0.9																					1970																																														K		6.5					6.5																																																																																																									SOLID STATE COMMUN.,8(1970)1085	K.KNORR,N.BARTH		
101118	111	eutectec	Cu1Pb1	Cu1Pb1	Cu	1	Pb	1																					1930																																														K					2.25																																																																																																											ROY.SOC.CAN.TRANS.,24(1930)53	J.C.MCLENNAN,J.O.WILHELM,L.F.ALLEN		
101119	11		Cu1P1	Cu1P1	Cu	1	P	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101120	RMP0350001		Cu0.287O0.14Ti0.573	Cu0.287O0.14Ti0.573	Cu	0.287	O	0.14	Ti	0.573																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101121	11		Cu2O1	Cu2O1	Cu	2	O	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101122	11		Cu1O1	Cu1O1	Cu	1	O	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101123	1374		Cu3Na2S3	Cu3Na2S3	Cu	3	Na	2	S	3																			1952																																														K		0.3					0.3																																																																																																									Z.ANORG.ALLG.CHEM.,269(1952)141	M.H.VAN MAAREN		
101124	558		Cu3N1	Cu3N1	Cu	3	N	1																																																																			K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
101125	1831		Cu1Mo4S5	Cu1Mo4S5	Cu	1	Mo	4	S	5																			1974																																														K		11					11																																																																																																									J.LESS-COMMON METALS,34(1974)125	C.F.WOODHEAD,J.G.BOOTH,N.MORTON		
101126	614	P=0-18 kbar 	Cu1Mo3S4	Cu1Mo3S4	Cu	1	Mo	3	S	4																			1975																																														K		11.8					11.8																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
101127	1725		Cu1Mo3S4	Cu1Mo3S4	Cu	1	Mo	3	S	4																			1974																																														K		10.8					10.8																																																																																																									ZH.ETF PIS.RED,20(1974)59	N.E.ALEKSEEVSKII,N.M.DOVROVOL'SKII,V.I.TSEBRO		
101128	1664		Cu1.5Mo45S6	Cu1.5Mo4.5S6	Cu	1.5	Mo	4.5	S	6																			1974																																													rhombohedral	K		10.9					10.9																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)L13	G.BONGI,H.JONES,O.FISCHER,R.ODERMATT		
101129	1665		Cu0.2S2Zn0.8	Cu0.2S2Zn0.8	Cu	0.2	S	2	Zn	0.8																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.3																																																																																																											J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
101130	1665		Cu0.6S2Zn0.4	Cu0.6S2Zn0.4	Cu	0.6	S	2	Zn	0.4																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.3																																																																																																											J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
101131	984		Cu1S4V2	Cu1S4V2	Cu	1	S	4	V	2																			1967																												Al2MgO4																	Al2MgO4, H1[1]	K		4.45					4.45																																																																																																					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
101132	984		Cu1S4Ti2	Cu1S4Ti2	Cu	1	S	4	Ti	2																			1967																												Al2MgO4																	Al2MgO4, H1[1]	K					0.05																																																																																																							Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
101133	643		Cu1S1Se1	Cu1S1Se1	Cu	1	S	1	Se	1																			1966																												FeS2(marcasite)																	FeS2, C18	K		1.5					1.5																																																																																																									SOLID STATE COMMUN.,4(1966)533	C.T.PREWITT,H.S.YOUNG,J.L.GILLSON,P.E.BIERSTEDT,R.B.FLIPPEN,T.A.BITHER		
101134	77		Cu1.8S1	Cu1.8S1	Cu	1.8	S	1																					1950																																														K					1.3																																																																																																											Z.Phys., 128(1950)324	W.Buckel,R.Hilsch		
101135	1354	P=0-10 kbar	Cu1S1	Cu1S1	Cu	1	S	1																					1970																												CuS																	CuS, B18	K		1.65					1.65																																																																																																									J.PHYS.SOC.JAPAN,28(1970)369	E.KANDA,M.ISHINO,T.NAKAJIMA		
101136	1130		Cu1S2	Cu1S2	Cu	1	S	2																					1967																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.56					1.56																																																																																																									J.CHEM.PHYS.,47(1967)1769	J.S.KOUVEL,R.A.MUNSON,W.DESORBO		
101137	1060		Cu0.05Rh0.04Ti0.91	Cu0.05Rh0.04Ti0.91	Cu	0.05	Rh	0.04	Ti	0.91																			1964																																														K		2.5					2.5																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101138	1760		Cu1Rh1.95Se4Sn0.05	Cu1Rh1.95Se4Sn0.05	Cu	1	Rh	1.95	Se	4	Sn	0.05																	1974																												Al2MgO4																	Al2MgO4, H1[1]	K		2.7					2.7																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1387	D.A.O'CONNOR,N.W.GRIMES,P.P.DAWES		
101139	1760		Cu1Rh2Se4	Cu1Rh2Se4	Cu	1	Rh	2	Se	4																			1974																												Al2MgO4																	Al2MgO4, H1[1]	K		3.5					3.5																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1387	D.A.O'CONNOR,N.W.GRIMES,P.P.DAWES		
101140	1898		Cu1Rh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			1975																												Al2MgO4																	Al2MgO4, H1[1]	K		4.8					4.8																																																																																																									SOLID STATE COMMUN.,16(1975)139	N.W.GRIMS,P.P.DAWES		
101141	1665		Cu0.95Se2Zn0.05	Cu0.95Se2Zn0.05	Cu	0.95	Se	2	Zn	0.05																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K		2.45					2.45																																																																																																									J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
101142	643		Cu1Se1Te1	Cu1Se1Te1	Cu	1	Se	1	Te	1																			1966																												FeS2(marcasite)																	FeS2, C18	K		2					2																																																																																																									SOLID STATE COMMUN.,4(1966)533	C.T.PREWITT,H.S.YOUNG,J.L.GILLSON,P.E.BIERSTEDT,R.B.FLIPPEN,T.A.BITHER		
101143	1584		Cu1Se2	Cu1Se2	Cu	1	Se	2																					1968																												FeS2(marcasite)																	FeS2, C18	K		2.43					2.43																																																																																																									STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
101144	11		Cu1Se1	Cu1Se1	Cu	1	Se	1																					1952																												CuS																	CuS, B18	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101145	2		Cu1Sb1	Cu1Sb1	Cu	1	Sb	1																					1948																																														K					1.8																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
101146	769		Cu0.81Sb0.19	Cu0.81Sb0.19	Cu	0.81	Sb	0.19																					1968																																													hexagonal	K		0.07					0.07																																																																																																									PHYS.LETT.A,28(1968)67	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDERSON		
101147	769		Cu0.786Sb0.214	Cu0.786Sb0.214	Cu	0.786	Sb	0.214																					1968																																													hexagonal	K		0.047					0.047																																																																																																									PHYS.LETT.A,28(1968)67	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDERSON		
101148	769		Cu0.844Sb0.156	Cu0.844Sb0.156	Cu	0.844	Sb	0.156																					1968																												Mg																	Mg, A3	K		0.067					0.067																																																																																																									PHYS.LETT.A,28(1968)67	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDERSON		
101149	1617		Cu0.845Sb0.155	Cu0.845Sb0.155	Cu	0.845	Sb	0.155																					1970																												BiF3																	BiF3, D0[3]	K		0.184					0.184																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
101150	1589		Cu2Sb1	Cu2Sb1	Cu	2	Sb	1																					1968																												Cu2Sb																	Cu2Sb, C38	K		0.085					0.085																																																																																																									STRUCTUER AND BONDING,4(1968)83-229	E.BUCHER,K.ANDRESS		
101151	1589		Cu3Sb1	Cu3Sb1	Cu	3	Sb	1																					1968																																													orthorhombic	K		0.041					0.041																																																																																																									STRUCTUER AND BONDING,4(1968)83-229	E.BUCHER,K.ANDRESS		
101152	1589		Cu3Sb1	Cu3Sb1	Cu	3	Sb	1																					1968																																													cubic	K		1.8					1.8																																																																																																									STRUCTUER AND BONDING,4(1968)83-229	E.BUCHER,K.ANDRESS		
101153	1744	deposited at 4.2 K.	Cu0.14Sn0.86	Cu0.14Sn0.86	Cu	0.14	Sn	0.86																					1969																																														K		6.62					6.62																																																																																																									FIZ.METAL.METALLOVED,28(1969)1111	A.I.MOYSEYEV,T.A.UGOL'NIKOVA		
101154	1218		Cu0.1Sn0.9	Cu0.1Sn0.9	Cu	0.1	Sn	0.9																					1970																																														K		6.8					6.8																																																																																																									SOLID STATE COMMUN.,8(1970)1085	K.KNORR,N.BARTH		
101155	85		Cu3Sn1	Cu3Sn1	Cu	3	Sn	1																					1932																																														K					1.31																																																																																																							From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
101156	71		Cu0.8Sn0.2	Cu0.8Sn0.2	Cu	0.8	Sn	0.2																					1930																																														K					1.5																																																																																																											Proc.Acad.Sci.Amsterdam, 33(1930)258	W.J.DeHaas,E.Van Aubel		
101157	84		Cu0.94Sn0.06	Cu0.94Sn0.06	Cu	0.94	Sn	0.06																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101158	11		Cu1Si1	Cu1Si1	Cu	1	Si	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101159	95		Cu0.25Si0.75	Cu0.25Si0.75	Cu	0.25	Si	0.75																					1955																																														K					1.28																																																																																																							From Roberts' Table				Naturwiss, 42(1955)451	W.Buckel		
101160	84		Cu3Si1	Cu3Si1	Cu	3	Si	1																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101161	84		Cu0.91Si0.09	Cu0.91Si0.09	Cu	0.91	Si	0.09																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101162	1617		Cu0.86Si0.14	Cu0.86Si0.14	Cu	0.86	Si	0.14																					1970																																													hexagonal	K		0.058					0.058																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
101163	1665		Cu0.1Se2Zn0.9	Cu0.1Se2Zn0.9	Cu	0.1	Se	2	Zn	0.9																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.3																																																																																																											J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
101164	1665		Cu0.6Se2Zn0.4	Cu0.6Se2Zn0.4	Cu	0.6	Se	2	Zn	0.4																			1970																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.3																																																																																																											J.SOLID STATE CHEM.,1(1970)526	H.S.YOUNG,P.C.DONOHUE,P.E.BIERSTEDT,T.A.BITHER,W.H.CLOUD		
101165	110		D0.11Nb1D0.13Nb1	D0.11Nb1D0.13Nb1	D	0.11	Nb	1	D	0.13	Nb	1																	1957																																														K		9.12					9.12																																																																																																									Z.NATURFORSCH A,12(1957)247	E.Z.SCHRODER		
101166	190	Hc2(8.2K)=0.0835T. Hc2(0) is estimated using two fluid model by Y.Asada 	D0.018Nb0.982	D0.018Nb0.982	D	0.018	Nb	0.982																					1963																																														K		9.23					9.23																				T		0.396																																																																															EFFECT OF DISSOLVED GASES ON SOME SUPERCONDUCTING PROPERTIES OF NIOBIUM				PHYS.REV.,132(1963)107	WARREN DESORBO		
101167	84		Cu1Zn3	Cu1Zn3	Cu	1	Zn	3																					1933																																														K					1.28																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101168	1009		Cu1Zn1	Cu1Zn1	Cu	1	Zn	1																																																																			K					1.3																																																																																																							From Roberts' Table, unpublished results				Personal communication	D.R.O'Boyle		
101169	1617		Cu0.67Zn0.33	Cu0.67Zn0.33	Cu	0.67	Zn	0.33																					1970																												Cu																	Cu, A1	K					0.014																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
101170	658		Cu1Y1	Cu1Y1	Cu	1	Y	1																					1967																												CsCl																	CsCl, B2	K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101171	RMP0350001		Cu5U1	Cu5U1	Cu	5	U	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101172	RMP0350001		Cu1Ti1	Cu1Ti1	Cu	1	Ti	1																					1963																												gamma-CuTi																	gamma-CuTi, B11	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101173	1377		Cu1Th2	Cu1Th2	Cu	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K		3.44					3.44																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101174	1584	high temperature phase.	Cu1Te1	Cu1Te1	Cu	1	Te	1																					1968																																														K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
101175	643		Cu1Te2	Cu1Te2	Cu	1	Te	2																					1966																												FeS2(marcasite)																	FeS2, C18	K		1.3					1.3																																																																																																									SOLID STATE COMMUN.,4(1966)533	C.T.PREWITT,H.S.YOUNG,J.L.GILLSON,P.E.BIERSTEDT,R.B.FLIPPEN,T.A.BITHER		
101176	1584		Cu4Te3	Cu4Te3	Cu	4	Te	3																					1968																																														K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
101177	68		Fe0.008La0.992	Fe0.008La0.992	Fe	0.008	La	0.992																					1948																																														K		4.85					4.85																																																																																																									J.Chem.Phys., 16(1948)838	W.T.Ziegler		
101178	1624	Fe = 330 ppm	Ir1	Ir1	Ir	1																							1971																																														K		0.051					0.051																																																																																																									PHYS.REV.B,3(1971)91	G.RIBLET.		
101179	RMP0350001		Fe1Hf2	Fe1Hf2	Fe	1	Hf	2																					1963																												Fe3W3C																	Fe3W3C, E9[3]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101180	1377		Fe1Ge2	Fe1Ge2	Fe	1	Ge	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101181	272		Fe1	Fe1	Fe	1																							1933																												W																	W, A2	K					0.75																																																																																																											COMMUN.KAMERLINGH ONNES LAB.,21(1933)230A	W.H.KEESOM		
101182	1324	Tm=0.66 K	Eu0.012La0.988	Eu0.012La0.988	Eu	0.012	La	0.988																					1973																																														K		2.15					2.15																																																																																																									PHYS.REV.LETT.,30(1973)1132	D.DUMPRECHT,P.STEINER,S.HUFNER		
101183	339	Eu-wire. R(min) at 145 K and R(peak) at 90K, maybe magnetic ordering.	Eu1	Eu1	Eu	1																							1960																												W																	W, A2	K					1.3																																																																																																							ELECTRICAL RESISTIVITY OF EUROPIUM AND YTTERBIUM				PHYS.REV.,1171960)953	F.H.SPEDDING,M.A.CURRY,S.LEGVOLD		
101184	1389		Er0.1Th0.9	Er0.1Th0.9	Er	0.1	Th	0.9																					1969																																														K					0.015																																																																																																											HELV.PHYS.ACTA,42(1969)590	E.BUCHER,K.ANDRESS		
101185	115		Er0.01La0.99	Er0.01La0.99	Er	0.01	La	0.99																					1958																																														K		5.3					5.3																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101186	245		Er1	Er1	Er	1																							1946																												Mg																	Mg, A3	K					0.8																																																																																																											NEUE PHYS.BLATTER,8(1946)207	E.JUSTI		
101187	115		Dy0.01La0.99	Dy0.01La0.99	Dy	0.01	La	0.99																					1958																																														K		3.8					3.8																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101188	1187		D3.61Th1	D3.61Th1	D	3.61	Th	1																					1966																																														K		8.35					8.35																																																																																																									Physica 32(1966)1253	J.F.DaSilva,N.W.J.Van Duykeren,Z.Dokoupil		
101189	601		Fe2P1	Fe2P1	Fe	2	P	1																					1965																												Fe2P																	Fe2P, C22	K					0.97																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101190	920		Fe1Np6	Fe1Np6	Fe	1	Np	6																					1968																																														K					0.5																																																																																																											PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
101191	32		Fe0.05Ni0.05Zr0.9	Fe0.05Ni0.05Zr0.9	Fe	0.05	Ni	0.05	Zr	0.9																			1955																																														K		3.9					3.9																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
101192	920		Fe0.75Ni0.25U6	Fe0.75Ni0.25U6	Fe	0.75	Ni	0.25	U	6																			1968																																														K		1.4					1.4																																																																																																									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
101193	920		Fe0.25Ni0.75U6	Fe0.25Ni0.75U6	Fe	0.25	Ni	0.75	U	6																			1968																																														K		3					3																																																																																																									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
101194	1866		Fe0.5Ni0.5U6	Fe0.5Ni0.5U6	Fe	0.5	Ni	0.5	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		2.1					2.1																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101195	1800		Fe0.03Nb0.25Ti0.72	Fe0.03Nb0.25Ti0.72	Fe	0.03	Nb	0.25	Ti	0.72																			1968																																														K		8.5					8.5																																																																																																									Z.METALLKDE.,59(1968)69	T.NISHIMURA,U.ZWICKER		
101196	1800		Fe0.04Nb0.1Ti0.86	Fe0.04Nb0.1Ti0.86	Fe	0.04	Nb	0.1	Ti	0.86																			1968																																														K		7.4					7.4																																																																																																									Z.METALLKDE.,59(1968)69	T.NISHIMURA,U.ZWICKER		
101197	1800		Fe0.08Nb0.05Ti0.87	Fe0.08Nb0.05Ti0.87	Fe	0.08	Nb	0.05	Ti	0.87																			1968																																														K		4.7					4.7																																																																																																									Z.METALLKDE.,59(1968)69	T.NISHIMURA,U.ZWICKER		
101198	1866		Fe0.5Mn0.5U6	Fe0.5Mn0.5U6	Fe	0.5	Mn	0.5	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		2.8					2.8																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101199	563		Fe0.01La0.001Rh0.99	Fe0.01La0.001Rh0.99	Fe	0.01	La	0.001	Rh	0.99																			1964																																														K		0.75					0.75																																																																																																									J.APPL.PHYS.,35(1964)3487	B.A.HOLM,B.T.MATTHIAS,D.C.HAMILTON,E.CORENZWIT,G.ARRHENIUS,G.W.HULL JR.,R.FITZGERALD,T.H.GEBALLE		
101200	563		Fe0.01La0.01Rh0.98	Fe0.01La0.01Rh0.98	Fe	0.01	La	0.01	Rh	0.98																			1964																																														K		0.75					0.75																																																																																																									J.APPL.PHYS.,35(1964)3487	B.A.HOLM,B.T.MATTHIAS,D.C.HAMILTON,E.CORENZWIT,G.ARRHENIUS,G.W.HULL JR.,R.FITZGERALD,T.H.GEBALLE		
101201	1377		Fe1Sn2	Fe1Sn2	Fe	1	Sn	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101202	84		Fe0.95Sn0.05	Fe0.95Sn0.05	Fe	0.95	Sn	0.05																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101203	RMP0350001		Fe5Si2V3	Fe5Si2V3	Fe	5	Si	2	V	3																			1963																												alpha-Mn																	alpha-Mn, A12	K					0.37																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101204	11		Fe1Si1	Fe1Si1	Fe	1	Si	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101205	744		Fe0.02Sc0.05Zr0.93	Fe0.02Sc0.05Zr0.93	Fe	0.02	Sc	0.05	Zr	0.93																			1966																																														K		0.35					0.35																																																																																																					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
101206	2		Fe1Sb3	Fe1Sb3	Fe	1	Sb	3																					1948																																														K					1.45																																																																																																											Zh.Eksp.Teor.Fiz., 18(1948)101	N.E.Alekseevskii		
101207	427		Fe1Sb2	Fe1Sb2	Fe	1	Sb	2																					1962																																													orthorhombic	K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101208	22		Fe1Sb1	Fe1Sb1	Fe	1	Sb	1																					1958																																														K					1.8																																																																																																							Superconductivity of Lanthanum and Some Lanthanum Alloys				Phys.Rev., 109(1958)243	G.S.Anderson,S.Legvold,F.H.Spedding		
101209	99		Fe1S1	Fe1S1	Fe	1	S	1																					1930																																														K					1.9																																																																																																											Phil.Mag., 10(1930)500	J.C.McLennam,J.F.Allen,J.O.Wilhelm		
101210	1060		Fe0.05Rh0.04Ti0.91	Fe0.05Rh0.04Ti0.91	Fe	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.9					3.9																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101211	712		Fe0.02Re0.98	Fe0.02Re0.98	Fe	0.02	Re	0.98																																																																			K		1.6					1.6																																																																																																					From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
101212	601		Fe1P1	Fe1P1	Fe	1	P	1																					1965																												MnP																	MnP, B31	K					0.97																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101213	1533	amorphous films. gap by tunneling using Al-I-Ga films. Annealing at 15 K produced beta-Ga, which shows Tc = 6.2 K and (2d/kTc) = 3.9.	Ga1	Ga1	Ga	1																						4	1968																																													amorphous, beta phase	K		8.45					8.45																																														meV	1.65	4.5	1																																															deposited on substrate at 4 K.									PHYS.REV.LETT.,20(1968)1496	C.V.BRISCOE,H.WUHL,J.E.JACKSON		
101214	1048	delta-phase	Ga1	Ga1	Ga	1																							1969																																														K		7.85					7.85																																																																																																									C.R.ACAD.SCI.B,268(1969)1314	I.EPELBOIN,L.BOSIO,R.DEFRAIN		
101215	1047	gamma phase	Ga1	Ga1	Ga	1																							1967																																														K		7.6					7.6																																																																																																									C.R.ACAD.SCI.B,(1967)264,1592	A.DEFRAIN,I.EPELBOIN,L.BOSIO,R.CORTES		
101216	1595	beta phase	Ga1	Ga1	Ga	1																							1974																																														K		3.07					3.07																																																																																																									PHYS.REV.B,10(1974)4572	H.PARR		
101217	803	TBL values of Hc2 and (dHc2/dT) are Hc (type-I SC).	Ga1	Ga1	Ga	1																							1966																																														K		1.083					1.083																				Oe		59.2							Oe/K		93.8			MHC101217																																																																			Superconducting transition and critical field of pure gallium single crystals			MIT	Phys.Rev., 150(1966)315	W.D.Gregory,T.P.Sheahen,J.F.Cochran		
101218	32		Fe0.1Zr0.9	Fe0.1Zr0.9	Fe	0.1	Zr	0.9																					1955																																														K		1					1																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
101219	1377		Fe1Zr2	Fe1Zr2	Fe	1	Zr	2																					1972																												CuAl2																	CuAl2, C16	K		0.17					0.17																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101220	21		Fe1U6	Fe1U6	Fe	1	U	6																					1958																												U6Mn																	MnU6, D2[c]	K		3.9					3.9																																																																																																									J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101221	21		Fe2U1	Fe2U1	Fe	2	U	1																					1958																												MgCu2(Laves)																	MgCu2, C15	K					1.06																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101222	RMP0350001		Fe1Ti1	Fe1Ti1	Fe	1	Ti	1																					1963																												W																	W, A2	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101223	173		Fe3Th7	Fe3Th7	Fe	3	Th	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		1.86					1.86																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101224	1626		Fe2Te3	Fe2Te3	Fe	2	Te	3																					1974																																														K					1.8																																																																																																											CAN.J.PHYS.,52(1974)1800	E.HERMON,J.QUARONI,R.C.SWEET,W.B.MUIR		
101225	1340		Ga0.03Mg0.97	Ga0.03Mg0.97	Ga	0.03	Mg	0.97																					1972																																														K					0.013																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
101226	659		Ga1Lu3	Ga1Lu3	Ga	1	Lu	3																																																																			K					1.1																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
101227	715		Ga3Lu1	Ga3Lu1	Ga	3	Lu	1																					1970																												AuCu3																	AuCu3, L1[2]	K		2.3					2.3																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101228	658		Ga1La3	Ga1La3	Ga	1	La	3																					1967																																														K		5.84					5.84			K/GPa	1.12																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101229	711		Ga1La1	Ga1La1	Ga	1	La	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101230	863		Ga2La1	Ga2La1	Ga	2	La	1																					1969																																														K					1.4																																																																																																											J.APPL.PHYS.,40(1969)3161	E.O.THORLAND,J.GRAOT,R.W.GREEN,S.LEGVOLD		
101231	1073		Ga0.8In0.2V3	Ga0.8In0.2V3	Ga	0.8	In	0.2	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.7					12.7																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
101232	1564		Ga0.3In0.7La3	Ga0.3In0.7La3	Ga	0.3	In	0.7	La	3																			1973																												AuCu3																	AuCu3, L1[2]	K		9.25					9.25																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
101233	1377		Ga1Hf2	Ga1Hf2	Ga	1	Hf	2																					1972																												CuAl2																	CuAl2, C16	K		0.21					0.21																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101234	1073		Ga0.8Ge0.2V3	Ga0.8Ge0.2V3	Ga	0.8	Ge	0.2	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		13.6					13.6																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
101235	1784	rapid quench 	Ga0.1Ge0.9	Ga0.1Ge0.9	Ga	0.1	Ge	0.9																					1974																																														K		5.3					5.3																																																																																																									PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
101236	1545	deposited at  4-5K  d =  150-3000 A	Ga1	Ga1	Ga	1																							1971																																														K		8.5					8.5																																																																																																									PHYSICA,55(1971)250	D.G.NAUGLE,R.E.ALOVER,W.MOORMAN		
101237	1599	vapor deposition	Ga0.4Nb0.6	Ga0.4Nb0.6	Ga	0.4	Nb	0.6																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		20.3					20.3																																																																																																									PHYS.LETT.A,49(1974)407	A.W.WIKLUND,L.J.VIELAND		
101238	1190		Ga0.37Nb0.63	Ga0.37Nb0.63	Ga	0.37	Nb	0.63																					1971																																													tetragonal	K					6																																																																																																											SOLID STATE COMMUN.,9(1971)1769	A.WICKLUND,G.W.WEBB,L.J.VIELAND,R.E.MILLER		
101239	1446		Ga1Nb3	Ga1Nb3	Ga	1	Nb	3																					1972																																														K		14.5					14.5																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101240	1970		Ga1Nb3	Ga1Nb3	Ga	1	Nb	3																					1975																												Cr3Si(A15)																	Cr3Si, A15	K		20.3					20.3																																																																																																									J.LOW TEMP.PHYS.,18(1975)147	P.P.M.MEINCKE,V.NOVOTNY		
101241	927		Ga3Nb5	Ga3Nb5	Ga	3	Nb	5																					1969																																														K		1.35					1.35																																																																																																									PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
101242	433	brown 	Ga1N1	Ga1N1	Ga	1	N	1																					1963																																														K					1.38																																																																																																											ZH.EKSP.TEOR.FIZ.,44(1963)1413	G.V.SAMSONOV,N.E.ALEKSEEVSKII,O.I.SHULITSOVA		
101243	433	gray - black 	Ga1N1	Ga1N1	Ga	1	N	1																					1963																												ZnS(wurtzite)																	ZnS(wurtzite), B4	K		5.85					5.85																																																																																																									ZH.EKSP.TEOR.FIZ.,44(1963)1413	G.V.SAMSONOV,N.E.ALEKSEEVSKII,O.I.SHULITSOVA		
101244	1725		Ga0.5Mo5S6Sn1	Ga0.5Mo5S6Sn1	Ga	0.5	Mo	5	S	6	Sn	1																	1974																																														K		13.3					13.3																																																																																																									ZH.ETF PIS.RED,20(1974)59	N.E.ALEKSEEVSKII,N.M.DOVROVOL'SKII,V.I.TSEBRO		
101245	RMP0350001		Ga1Mo3	Ga1Mo3	Ga	1	Mo	3																					1963																												Cr3Si(A15)																	Cr3Si, A15	K		0.76					0.76																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101246	117		Ga2Mo1	Ga2Mo1	Ga	2	Mo	1																					1957																																														K		9.5					9.5																																																																																																									PROG.IN LOW TEMP.PHY.,11(1957)138	B.T.MATTHIAS		
101247	1295		Ga4Mo1	Ga4Mo1	Ga	4	Mo	1																					1972																																														K		9.8					9.8																																																																																																									HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
101248	1977		Ga5Mn1.85	Ga5Mn1.85	Ga	5	Mn	1.85																					1973																																													tetragonal	K					1.2																																																																																																											J.APPL.CRYST.,6(1973)240	P.L.NORMAN,W.J.KICHINGMAN		
101249	1955		Ga0.5Si0.5V3	Ga0.5Si0.5V3	Ga	0.5	Si	0.5	V	3																			1974																																														K		18.2					18.2																																																																																																					From Roberts' Table.				LT-13,  P=475	B.C.Deaton,D.E.Cordon		
101250	1955		Ga0.25Si0.75V3	Ga0.25Si0.75V3	Ga	0.25	Si	0.75	V	3																			1974																																														K		18.6					18.6																																																																																																					From Roberts' Table.				LT-13,  P=475	B.C.Deaton,D.E.Cordon		
101251	659		Ga1Sc3	Ga1Sc3	Ga	1	Sc	3																																																																			K					3.3																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
101252	695		Ga1Sb1	Ga1Sb1	Ga	1	Sb	1																					1965																																														K		5.9					5.9																																																																																																									SCIENCE,147(1965)1441	D.B.MCWHAN,E.GREGORY,G.W.HULL JR.,T.R.R.MCDONALD		
101253	427		Ga1Pt1	Ga1Pt1	Ga	1	Pt	1																					1962																												FeSi																	FeSi, B20	K		1.74			0.34		1.74																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101254	486		Ga2Pt1	Ga2Pt1	Ga	2	Pt	1																					1965																																														K		1.9					1.9																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
101255	427		Ga7Pt3	Ga7Pt3	Ga	7	Pt	3																					1962																												CaF2																	CaF2, C1	K		2.9			1.1		2.9																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101256	1491	quench. condensed at 4 K	Ga0.1Pb0.9	Ga0.1Pb0.9	Ga	0.1	Pb	0.9																					1973																																														K		6.33					6.33																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
101257	1073		Ga1Nb2.4V0.6	Ga1Nb2.4V0.6	Ga	1	Nb	2.4	V	0.6																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
101258	1982		Ga0.15Nb3Sn0.7Tl0.15	Ga0.15Nb3Sn0.7Tl0.15	Ga	0.15	Nb	3	Sn	0.7	Tl	0.15																	1964																																														K		18.14					18.14																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101259	1982		Ga0.15Nb3Sb0.15Sn0.7	Ga0.15Nb3Sb0.15Sn0.7	Ga	0.15	Nb	3	Sb	0.15	Sn	0.7																	1964																																														K		16.89					16.89																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101260	1982		Ga0.15Nb3Pb0.15Sn0.7	Ga0.15Nb3Pb0.15Sn0.7	Ga	0.15	Nb	3	Pb	0.15	Sn	0.7																	1964																																														K		18.11					18.11																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101261	958		Ga0.45V0.55	Ga0.45V0.55	Ga	0.45	V	0.55																					1965																																													hexagonal	K					2.1																																																																																																											J.LESS-COMMON METALS,9(1965)416	.H.B.PROBST,J.J.FISCHER		
101262	1675		Ga0.71V0.29	Ga0.71V0.29	Ga	0.71	V	0.29																					1974																																														K		4.2					4.2																																																																																																									SOLID STATE COMMUN.,15(1974)1047	C.PAPASTAIKOUDIS,E.CRUCEANU,G.ANTESBERGER		
101263	416		Ga5V2	Ga5V2	Ga	5	V	2																																																																		tetragonal	K		3.55			2.1		3.55																																																																																																					From Roberts' Table.				to be published.	J.Muller,R.Reinmann		
101264	1407		Ga1V3	Ga1V3	Ga	1	V	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		14.19					14.19																																																																																																									J.APPL.PHYS.,40(1969)2817	D.L.DECKER,H.L.LAQUER		
101265	1343		Ga1V3	Ga1V3	Ga	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																																																																																																									J.PHYS.CHEM.SOLIDS,34(1973)1445	C.C.KOCH		
101266	578		Ga1V3	Ga1V3	Ga	1	V	3																					1960																												Cr3Si(A15)																	Cr3Si, A15	K		16.8					16.8																																																																																																					CORRELATIONS BETWEEN SUPERCONDUCTIVITY AND NUCLEAR MAGNETIC RESONANCE PROPERTIES				PHYS.REV.LETT.,5(1960)149	B.T.MATTHIAS,J.EISINGER,V.JACCARINO,W.E.BLUMBERG		
101267	412		Ga3U1	Ga3U1	Ga	3	U	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
101268	RMP0350001		Ga3Ti1	Ga3Ti1	Ga	3	Ti	1																					1963																												Al3Ti																	Al3Ti, D0[22]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101269	RMP0350001		Ga1Ti3	Ga1Ti3	Ga	1	Ti	3																					1963																												Ni3Sn																	Ni3Sn, D0[19]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101270	1377		Ga1Th2 	Ga1Th2	Ga	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101271	927		Ga2Ta3	Ga2Ta3	Ga	2	Ta	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
101272	1955		Ga1Si1V3	Ga1Si1V3	Ga	1	Si	1	V	3																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		18.6					18.6																																																																																																					From Roberts' Table.				LT-13,  P=475	B.C.Deaton,D.E.Cordon		
101273	187		Gd0.09La0.91Os2	Gd0.09Ls0.91Os2	Gd	0.09	Ls	0.91	Os	2																			1960																																														K		6					6																																																																																																					PROPERTIES OF SOME MAGNETIC SUPERCONDUCTORS				PHYS.REV.,119(1960)1570	A.L.WILLIAMS,D.D.DAVIS,R.M.BOZORTH		
101274	328		Gd0.005La0.995	Gd0.005La0.995	Gd	0.005	La	0.995																					1960																																														K		3.7					3.7																																																																																																									HELV.PHYS.ACTA,33(1960)459	J.MULLER,M.RISI		
101275	115		Gd0.01La0.99	Gd0.01La0.99	Gd	0.01	La	0.99																					1958																																														K		0.6					0.6																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101276	711		Ga3Zr5	Ga3Zr5	Ga	3	Zr	5																																																				A	8.02		5.678												K		3.85					3.85																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101277	1377		Ga1Zr2	Ga1Zr2	Ga	1	Zr	2																					1972																												CuAl2																	CuAl2, C16	K		0.38					0.38																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101278	927		Ga2Zr3	Ga2Zr3	Ga	2	Zr	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
101279	RMP0350001		Ga3Zr1	Ga3Zr1	Ga	3	Zr	1																					1963																												Al3Ti																	Al3Ti, D0[22]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101280	863		Ga2Y1	Ga2Y1	Ga	2	Y	1																					1969																																													tetragonal	K		1.68					1.68																																																																																																									J.APPL.PHYS.,40(1969)3161	E.O.THORLAND,J.GRAOT,R.W.GREEN,S.LEGVOLD		
101281	711		Ga1Y1	Ga1Y1	Ga	1	Y	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101282	659		Ga1Y3	Ga1Y3	Ga	1	Y	3																																																																			K					1.1																																																																																																							From Roberts' Table, Private communication, quoted in J.Phys.Chem.Solids 28(1967)569				Private communication	B.T.Matthias		
101283	460		Ga1V1	Ga1V1	Ga	1	V	1																					1963																																														K		16.45					16.45																																																																																																									PHYS.LETT.,4(1963)292	D.KOCH,E.SAUR,G.OTTO		
101284	310		Ga1V3	Ga1V3	Ga	1	V	3																					1960																																														K		14.5					14.5																																																																																																									PHYS.REV.LETT.,5(1960)149	J.H.WERNICK		
101285	037		Ge1Ir1	Ge1Ir1	Ge	1	Ir	1																					1953																												MnP																	MnP, B31	K		4.7					4.7																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
101286	491		Ge7Ir3	Ge7Ir3	Ge	7	Ir	3																					1963																																														K		0.87					0.87																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101287	1528		Ge0.1In0.9	Ge0.1In0.9	Ge	0.1	In	0.9																					1969																																														K		6.2					6.2																																																																																																									J.VAC.SCI.TECH.,6(1969)677	E.GUYON,F.NEUNIER		
101288	1784	rapid quench	Ge0.3In0.7	Ge0.3In0.7	Ge	0.3	In	0.7																					1974																																														K																																																																																																																PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
101289	1377		Ge1Hf2	Ge1Hf2	Ge	1	Hf	2																					1972																												CuAl2																	CuAl2, C16	K					0.05																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101290	311		Ge0.22H0.16Nb1	Ge0.22H0.16Nb1	Ge	0.22	H	0.16	Nb	1																			1963																												Cr3Si(A15)																	Cr3Si, A15	K					4.2																																																																																																											METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101291	303	tetragonal  Ge(II)	Ge1	Ge1	Ge	1																																																																				tetragonal	K					0.33																																																																																																							From Roberts' Table.				Unpublished	H.R.Hart,Jr.,B.W.Roberts		
101292	1068	P = 115 kbar	Ge1	Ge1	Ge	1																							1966																																														K		5.35					5.35																																																																																																									Z.PHYS.,195(1966)215	J.WITTIG		
101293	12		Ge1	Ge1	Ge	1																							1935																												diamond																	diamond, A4	K					0.05																																																																																																											Proc.Roy.Soc.(London),151(1935)A610	N.Kurti,F.Simon		
101294	1123		Gd0.002Th0.998	Gd0.002Th0.998	Gd	0.002	Th	0.998																					1967																																														K		0.714					0.714																																																																																																									PHYS.REV.LETT.,18(1967)899	D.K.FINNEMORE,D.T.PETERSON,W.R.DECKER		
101295	1561		Gd0.001Th0.999	Gd0.001Th0.999	Gd	0.001	Th	0.999																					1969																																														K		1.11					1.11																																																																																																									PHYS.REV.,188(1969)723	D.K.FINNEMORE,R.L.CAPPELLETTI		
101296	1759		Gd0.2Mo6Pb1S8	Gd0.2Mo6Pb1S8	Gd	0.2	Mo	6	Pb	1	S	8																	1974																																														K		14.3					14.3																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101297	RMP0350001		Ge3Nb5	Ge3Nb5	Ge	3	Nb	5																					1963																																													tetragonal	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101298	10	plus free metal.	Ge1Nb2	Ge1Nb2	Ge	1	Nb	2																					1954																																														K		1.9					1.9																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101299	10		Ge2Nb3	Ge2Nb3	Ge	2	Nb	3																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101300	1446		Ge1Nb3	Ge1Nb3	Ge	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.28					6.28																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101301	558		Ge3N4	Ge3N4	Ge	3	N	4																																																																			K					1.38																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
101302	42		Ge0.41Mo0.59	Ge0.41Mo0.59	Ge	0.41	Mo	0.59																					1953																																														K					1.2																																																																																																							Superconducting silicides and Germanides				Phys.Rev., 89(1953)884	G.F.Hardy,J.K.Hulm		
101303	10		Ge2Mo1	Ge2Mo1	Ge	2	Mo	1																					1954																												MoSi2																	MoSi2, C11[b]	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101304	1692		Ge0.23Mo0.77	Ge0.23Mo0.77	Ge	0.23	Mo	0.77																					1974																																														K		2.16					2.16																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101305	1446		Ge1Mo3	Ge1Mo3	Ge	1	Mo	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		1.6					1.6																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101306	916		Ge1.78La1	Ge1.78La1	Ge	1.78	La	1																					1969																												ThSi2																	ThSi2, C[c]	K		1.57					1.57																																																																																																									J.PHYS.SOC.JAPAN,27(1969)1463	T.SATOH,Y.ASADA		
101307	25		Ge2La1	Ge2La1	Ge	2	La	1																					1958																																													orthorhombic	K		1.49					1.49																																																																																																					Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
101308	916		Ge2La1	Ge2La1	Ge	2	La	1																					1969																												ThSi2																	ThSi2, C[c]	K		2.24					2.24																																																																																																									J.PHYS.SOC.JAPAN,27(1969)1463	T.SATOH,Y.ASADA		
101309	491		Ge2Pd5	Ge2Pd5	Ge	2	Pd	5																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101311	491		Ge1Pd2	Ge1Pd2	Ge	1	Pd	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101312	RMP0350001		Ge0Pd1	Ge1Pd1	Ge	1	Pd	1																					1963																												MnP																	MnP, B31	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101313	427		Ge2Pd1	Ge2Pd1	Ge	2	Pd	1																					1962																																														K					1.47																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101314	1982		Ge0.15Nb3Sn0.85	Ge0.15Nb3Sn0.85	Ge	0.15	Nb	3	Sn	0.85																			1964																																														K		17.8					17.8																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101315	1982		Ge0.15Nb3Pb0.15Sn0.7	Ge0.15Nb3Pb0.15Sn0.7	Ge	0.15	Nb	3	Pb	0.15	Sn	0.7																	1964																																														K		17.82					17.82																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101316	498		Ge1Nb3	Ge1Nb3	Ge	1	Nb	3																					1965																												Cr3Si(A15)																	Cr3Si, A15	K		17					17																																																																																																					SUPERCONDUCTIVITY OF NB3GE				PHYS.REV.,139(1965)A1501	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,R.H.WILLENS,T.H.GEBALLE		
101317	1726		Ge1Nb3	Ge1Nb3	Ge	1	Nb	3																					1974																																														K		22.1					22.1																																																																																																									ZH.ETF PIS.RED.,19(1974)510	E.V.MEL'NIKOV,I.V.VORONOVA,M.N.SMIRNOVA,N.N.MIKHAILOV,O.ALAVROVA		
101318	311		Ge0.72Nb3.28	Ge0.72Nb3.28	Ge	0.72	Nb	3.28																					1963																																														K		5.5					5.5																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101319	311		Ge0.55Nb3.45	Ge0.55Nb3.45	Ge	0.55	Nb	3.45																					1963																																														K		4.9					4.9																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101320	311		Ge0.22Nb1	Ge0.22Nb1	Ge	0.22	Nb	1																					1963																												Cr3Si(A15)																	Cr3Si, A15	K		5.3					5.3																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101321	10		Ge2Ta1	Ge2Ta1	Ge	2	Ta	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101322	1784		Ge0.3Sn0.7	Ge0.3Sn0.7	Ge	0.3	Sn	0.7																					1974																																														K																																																																																																																PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
101323	1073		Ge0.15Si0.9V3	Ge0.1Si0.9V3	Ge	0.1	Si	0.9	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		14.4					14.4																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
101324	25		Ge2Sc1	Ge2Sc1	Ge	2	Sc	1																					1958																																														K		1.3					1.3																																																																																																					Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
101325	1829	rapid quench	GE0.3Sb0.7	Ge0.3Sb0.7	Ge	0.3	Sb	0.7																					1974																																													cubic	K		3.3					3.3																																																																																																									J.SPPL.PHYS.,45(1974)3683	S.J.POON,W.L.JOHNSON		
101326	1683		Ge0.5Ru0.5	Ge0.5Ru0.5	Ge	0.5	Ru	0.5																					1973																																														K					1.1																																																																																																											ZH.ETF PIS'MA RED.,18(1973)94	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
101327	1683		Ge0.5Rh0.5	Ge0.5Rh0.5	Ge	0.5	Rh	0.5																					1973																																														K					1.1																																																																																																											ZH.ETF PIS'MA RED.,18(1973)94	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
101328	141		Ge3Rh5	Ge3Rh5	Ge	3	Rh	5																					1955																															A	5.42	10.32	3.96											orthorhombic	K		2.12					2.12																																																																																																									ACTA CRYST.,8(1955)15	S.GELLER		
101329	RMP0350001		Ge1Rh1	Ge1Rh1	Ge	1	Rh	1																					1963																												MnP			A	5.7	6.48	3.25											MnP, B31	K		0.96					0.96																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101330	1683	deposited at 4.2 K.	Ge0.5Pt0.5	Ge0.5Pt0.5	Ge	0.5	Pt	0.5																					1973																																														K		1.4			1		1.4																																																																																																									ZH.ETF PIS'MA RED.,18(1973)94	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
101331	RMP0350001		Ge1Pt1	Ge1Pt1	Ge	1	Pt	1																					1963																												MnP			A	6.088	5.733	3.701											MnP, B31	K		0.4					0.4																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101332	1683	deposited at 4.2 K.	Ge0.6Pd0.4	Ge0.6Pd0.4	Ge	0.6	Pd	0.4																					1973																																														K		3.1					3.1																																																																																																									ZH.ETF PIS'MA RED.,18(1973)94	N.E.ALEKSEEVSKII,V.M.ZAKOSARENKO		
101333	719		Ge1V3	Ge1V3	Ge	1	V	3																					1964																																														K		6.7					6.7																																																																																																									PHYS.REV.,134(1964)A198	H.C.THEUERER,J.J.HAUSER		
101334	1164		Ge1V3	Ge1V3	Ge	1	V	3																					1971																												Cr3Si(A15)																	Cr3Si, A15	K		6.9					6.9																																																																																																									PROC.NAT.ACAD.SCI.,68(1971)56	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI		
101335	1446		Ge1V3	Ge1V3	Ge	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.1					6.1																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101336	RMP0350001		Ge3U1	Ge3U1	Ge	3	U	1																					1963																												AuCu3																	AuCu3, L1[2]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101337	989	superimposed films	Ge1Tl1	Ge1Tl1	Ge	1	Tl	1																					1967																																														K																																																																																																																PHYS.LETT.A,25(1967)688	D.G.NAUGLE		
101338	1784	rapid quench	Ge0.3Tl0.7	Ge0.3Tl0.7	Ge	0.3	Tl	0.7																					1974																																														K																																																																																																																PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
101339	522		Ge3Ti5	Ge3Ti5	Ge	3	Ti	5																					1963																												Mn5Si3																	Mn5Si3, D8[8]	K					1.2																																																																																																											Z.METALLKDE DTSCH.,54(1963)477	U.ZWICKER		
101340	10		Ge2Ti1	Ge2Ti1	Ge	2	Ti	1																					1954																												TiSi2																	TiSi2, C54	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101341	1377		Ge1Th2	Ge1Th2	Ge	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101342	927		Ge2Th3	Ge2Th3	Ge	2	Th	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
101343	1410	4000A	Ge1Ta3	Ge1Ta3	Ge	1	Ta	3																					1970																																														K		8					8																																																																																																									J.SPPL.PHYS.,41(1970)4958	J.I.GITTLEMAN,J.J.HANAK,J.P.PELLICANE,S.BOZOWSKI		
101345	410		H0.7Nb0.3	H0.7Nb0.3	H	0.7	Nb	0.3																																																																			K					0.47																																																																																																							From Roberts' Table.				Unpublished	A.C.Rose-Innes		
101346	49		H0.33Nb0.67	H0.33Nb0.67	H	0.33	Nb	0.67																					1942																																													cubic	K		7.28					7.28																																																																																																									Phys.Rev., 61(1942)738	F.H.Horn,W.F.Bruckzch,Jr.,W.T.Ziegler,D.H.Andrews,Jr.		
101347	1379		H1.33N0.33O3W1	H1.33N0.33O3W1	H	1.33	N	0.33	O	3	W	1																	1968																																													hexagonal	K		3.2					3.2																																																																																																									INORGANIC CHEM.,7(1968)1646	A.W.SLEIGHT,D.C.PEASE,T.A.BITHER,T.E.GIER		
101348	488		H1.96La1	H1.96La1	H	1.96	La	1																					1963																																														K					0.33																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1375	D.S.SCHREIBER,M.F.MERRIAM		
101349	40		H2.45La1	H2.45La1	H	2.45	La	1																					1953																																													cubic	K					1.8																																																																																																							Studies of compounds for superconductivity				Phys.Rev., 90(1953)115	W.T.Ziegler,R.A.Young		
101350	10		Ge1Zr1	Ge1Zr1	Ge	1	Zr	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101351	RMP0350001		Ge2Zr1	Ge2Zr1	Ge	2	Zr	1																					1963																												ZrSi2																	ZrSi2, C49	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101352	RMP0350001		Ge3Zr5	Ge3Zr5	Ge	3	Zr	5																					1963																												Mn5Si3																	Mn5Si3, D8[8]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101353	1784	rapid quench	Ge0.3Zn0.7	Ge0.3Zn0.7	Ge	0.3	Zn	0.7																					1974																																														K																																																																																																																PHYS.REV.B,9(1974)4742	C.C.TSUEI,W.L.JOHNSON		
101354	676	(dC/gamma*Tc) = 0.80. SUS(RT) = 3.9 E-5 emu/mol.	Ge1.62Y1	Ge1.62Y1	Ge	1.62	Y	1																					1966																												ThSi2																	alpha-ThSi2, C[c]	K		2.4					2.4																																																								mJ/mol.K2	4																																							arc-melting					Anomalous specific heat of superconducting lanthanum and yttrium compounds				Phys.Lett., 20(1966)565	T.Satoh,T.Ohtsuka		
101355	711		Ge1Y1	Ge1Y1	Ge	1	Y	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101356	25		Ge2Y1	Ge2Y1	Ge	2	Y	1																					1958																												ThSi2																	ThSi2, C[c]	K		3.8					3.8																																																																																																					Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
101357	1299		Hf2Ir1	Hf2Ir1	Hf	2	Ir	1																					1966																												Fe3W3C																	Fe3W3C, E9[3]	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101358	632		Hf2In1N1	Hf2In1N1	Hf	2	In	1	N	1																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
101359	942		Hf1	Hf1	Hf	1																							1968																												Mg																	Mg, A3	K					0.015																																																																																																											PHYS.LETT.A,28(1968)326	J.E.COX		
101360	RMP0350001		H2Zr1	H2Zr1	H	2	Zr	1																					1963																																													L2[b]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101361	1144		H0.32V0.68	H0.32V0.68	H	0.32	V	0.68																					1970																																														K					4.2																																																																																																											PHYS.REV.LETT.,25(1970)1618	D.G.WESTLAKE,S.T.OCKERS		
101362	1617		H0.5V1	H0.5V1	H	0.5	V	1																					1970																																														K					1.7																																																																																																											PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
101363	RMP0350001		H2Ti1	H2Ti1	H	2	Ti	1																					1963																																													cubic	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101364	1871		H0.11S2Ta1	H0.11S2Ta1	H	0.11	S	2	Ta	1																			1975																										layered		TX2																	2H-TaS2 phase	K		4.2					4.2																																																																																																electrolysis using Pt anode					Properties of HxTaS2: Correlation between the superconducting Tc and an electronic instability in layer compounds				J.CHEM.PHYS.,62(1975)967	D.W.MURPHY,F.J.DISALVO,G.R.STEWART,G.W.HULLJR.,J.V.ACRIVOS,J.V.WASZCZAK,S.EARLY,S.F.MAYER,T.H.GEBALL		
101365	1311		H0.73Pd1	H0.73Pd1	H	0.73	Pd	1																					1972																																														K					1.25																																																																																																											PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
101366	1311		H0.81Pd1	H0.81Pd1	H	0.81	Pd	1																					1972																																														K		2.5					2.5																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
101367	1311		H0.87Pd1	H0.87Pd1	H	0.87	Pd	1																					1972																																														K		4.3					4.3																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
101368	1763		H0.94Pd1	H0.94Pd1	H	0.94	Pd	1																					1973																																														K		6.6					6.6																																																																																																									PHYS.STAT.SOL.B,59(1973)329	T.SKOSKIEWICZ		
101369	1391		Hf0.04NB0.42Ta0.04Ti	Hf0.04Nb0.42Ta0.04Ti0.5	Hf	0.04	Nb	0.42	Ta	0.04	Ti	0.5																	1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101370	1438		Hf0.5Nb0.5	Hf0.5Nb0.5	Hf	0.5	Nb	0.5																					1974																																														K		9.5					9.5																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101371	1438	high temperature substrate	Hf0.33Nb0.67	Hf0.33Nb0.67	Hf	0.33	Nb	0.67																					1974																																														K		17					17																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101372	885		Hf0.15Nb0.85	Hf0.15Nb0.85	Hf	0.15	Nb	0.85																					1970																																														K		9.85					9.85																																																																																																									J.LOW TEMP.PHYS.,3(1970)393	F.J.CADIEU		
101373	1961	Zr=500 ppm	Hf1N1.118	Hf1N1.118	Hf	1	N	1.118																					1968																												NaCl																	NaCl, B1	K					2																																																																																																											PROC.BRITISH CERAMIC SOC.,10(1968)183-193	A.L.GIORGI,E.G.SZKLARZ,T.C.WALLACE		
101374	1542		Hf1N1	Hf1N1	Hf	1	N	1																					1971																												NaCl																	NaCl, B1	K		8.83					8.83																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
101375	266		Hf0.15Mo0.85	Hf0.15Mo0.85	Hf	0.15	Mo	0.85																					1962																																													cubic	K					1.02																																																																																																											IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101376	956		Hf1Mo2	Hf1Mo2	Hf	1	Mo	2																					1970																																													cubic	K		1					1																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
101377	1586		Hf1Mo2	Hf1Mo2	Hf	1	Mo	2																					1974																												MgCu2(Laves)																	MgCu2, C15	K		0.076					0.076																																																																																																									PHYS.LETT.A,50(1974)159	J.INVARSSON,O.RAPP,T.CLAESON		
101378	1586		Hf1Mo2	Hf1Mo2	Hf	1	Mo	2																					1974																												MgNi2(Laves)																	MgNi2(Laves), C36	K		0.065					0.065																																																																																																									PHYS.LETT.A,50(1974)159	J.INVARSSON,O.RAPP,T.CLAESON		
101379	266		Hf0.9Mo0.1	Hf0.9Mo0.1	Hf	0.9	Mo	0.1																					1962																																														K		2.5					2.5																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101380	1673	P=0-28 kbar	H15Th4	H15Th4	H	15	Th	4																					1974																																														K		8.45					8.45																																																																																																									SOLID STATE COMMUN.,15(1974)941	C.B.SATTERTHWAITE,H.RIETSCHEL,M.DIETRICH,W.GEY		
101381	266		Hf0.875Re0.125	Hf0.875Re0.125	Hf	0.875	Re	0.125																					1962																																													cubic	K		1.7					1.7																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101382	127		Hf1Os2	Hf1Os2	Hf	1	Os	2																					1959																												MgZn2(Laves)																	MgZn2, C14	K		2.69					2.69																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
101383	RMP0350001		Hf0.67Ni0.233Ru0.1	Hf0.67Ni0.233Ru0.1	Hf	0.67	Ni	0.233	Ru	0.1																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101384	RMP0350001		Hf0.63Ni0.25Re0.12	Hf0.63Ni0.25Re0.12	Hf	0.63	Ni	0.25	Re	0.12																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101385	1377		Hf2Ni1	Hf2Ni1	Hf	2	Ni	1																					1972																												CuAl2																	CuAl2, C16	K		0.87					0.87																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101386	1391		Hf0.13Nb0.47Zr0.13	Hf0.13Nb0.74Zr0.13	Hf	0.13	Nb	0.74	Zr	0.13																			1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101387	1391		Hf0.3Nb0.4Zr0.3	Hf0.3Nb0.4Zr0.3	Hf	0.3	Nb	0.4	Zr	0.3																			1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101388	1334		Hf0.36Nb0.62Zr0.02	Hf0.36Nb0.62Zr0.02	Hf	0.36	Nb	0.62	Zr	0.02																			1972																																														K		7.75					7.75																																																																																																									PHIL.MAG.,25(1972)303	C.C.KOCH,R.W.CARPENTER		
101389	1438		Hf0.33Nb0.17V0.7	Hf0.33Nb0.17V0.7	Hf	0.33	Nb	0.17	V	0.7																			1974																																														K					4.2																																																																																																											J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101390	1438		Hf0.33Nb0.33V0.33	Hf0.33Nb0.33V0.33	Hf	0.33	Nb	0.33	V	0.33																			1974																																														K		6.6					6.6																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101391	1391		Hf0.04Nb0.4Ti0.52V0.	Hf0.04Nb0.4Ti0.52V0.04	Hf	0.04	Nb	0.4	Ti	0.52	V	0.04																	1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101392	1391		Hf0.04Nb0.32Ti0.64	Hf0.04Nb0.32Ti0.64	Hf	0.04	Nb	0.32	Ti	0.64																			1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101393	181		Hf1Si2	Hf1Si2	Hf	1	Si	2																																																																			K					1.02																																																																																																							From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
101394	927		Hf3Si2	Hf3Si2	Hf	3	Si	2																					1969																																														K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
101395	1377		Hf2Si1	Hf2Si1	Hf	2	Si	1																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101396	1583		Hf1Sb2	Hf1Sb2	Hf	1	Sb	2																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
101397	RMP0350001		Hf1Ru1	Hf1Ru1	Hf	1	Ru	1																					1963																												CsCl																	CsCl, B2	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101398	1060		Hf0.05Rh0.04Ti0.91	Hf0.05Rh0.04Ti0.91	Hf	0.05	Rh	0.04	Ti	0.91																			1964																																														K		1.7					1.7																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101399	1058		Hf2Rh1	Hf2Rh1	Hf	2	Rh	1																					1966																												Fe3W3C																	Fe3W3C, E9[3]	K		2.02					2.02																																																																																																									Z.PHYS.,197(1966)276	H.WUHL		
101400	1058		Hf1Rh1	Hf1Rh1	Hf	1	Rh	1																					1966																																														K		1.73					1.73																																																																																																									Z.PHYS.,197(1966)276	H.WUHL		
101401	266		Hf0.025Re0.975	Hf0.025Re0.975	Hf	0.025	Re	0.975																					1962																																													hexagonal	K		7.3					7.3																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101402	266		Hf0.14Re0.86	Hf0.14Re0.86	Hf	0.14	Re	0.86																					1962																												alpha-Mn																	alpha-Mn, A12	K		5.86					5.86																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101403	266		Hf1Re2	Hf1Re2	Hf	1	Re	2																					1962																												MgZn2(Laves)																	MgZn2, C14	K		5.61					5.61																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101404	266		Hf0.5Re0.5	Hf0.5Re0.5	Hf	0.5	Re	0.5																					1962																												alpha-Mn																	alpha-Mn, A12	K					1.02																																																																																																											IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101405	258		Hg8K1	Hg8K1	Hg	8	K	1																																																																			K		3.42					3.42																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101406	256		Hg1In1	Hg1In1	Hg	1	In	1																					1963																																														K		3.81					3.81																																																																																																									J.LESS-COMMONMETALS,5(1963)41	B.R.COLES,M.F.MERRIAM,Z.FISK		
101407	579		Hg1	Hg1	Hg	1																							1965																												alpha-Hg																	alpha-Hg, A10	K		4.154					4.154																																																																																																									PHYS.REV. A,140(1965)507	D.E.MAPOTHER,D.K.FINNEMORE		
101408	47		Hf1Zr0.05	Hf1Zr0.05	Hf	1	Zr	0.05																					1952																																														K					0.22																																																																																																											Phys.Rev., 86(1952)628	L.D.Roberts,J.W.T.Dabbs		
101409	1		Hf0.99Zr0.01	Hf0.99Zr0.01	Hf	0.99	Zr	0.01																					1954																																													hexagonal	K		0.37					0.37																																																																																																									Rev.Mod.Phys., 26(1954)277	J.Eisenstein		
101410	1586		Hf1W2	Hf1W2	Hf	1	W	2																					1974																												MgCu2(Laves)																	MgCu2, C15	K					0.033																																																																																																											PHYS.LETT.A,50(1974)159	J.INVARSSON,O.RAPP,T.CLAESON		
101411	1189		Hf0.5V2Zr0.5	Hf0.5V2Zr0.5	Hf	0.5	V	2	Zr	0.5																			1970																												MgCu2(Laves)																	MgCu2, C15	K		10.1					10.1																																																																																																					LT-12				LT-12 (1970, Kyoto) p 483	K. INQUE,K.TACHIKAWA		
101412	1722		Hf0.6V2Zr0.4	Hf0.6V2Zr0.4	Hf	0.6	V	2	Zr	0.4																			1973																																														K		9.9					9.9																																																																																																					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
101413	1189		Hf1V2.3	Hf1V2.3	Hf	1	V	2.3																					1970																												MgCu2(Laves)																	MgCu2, C15	K		9.2					9.2																																																																																																					LT-12				LT-12 (1970, Kyoto) p 483	K. INQUE,K.TACHIKAWA		
101414	1323		Hf1V2	Hf1V2	Hf	1	V	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		9.2					9.2																																																																																																									JAPAN J.APPL.PHYS.,12(1973)161	K.INOUE,K.TACHIKAWA		
101415	1149	chemical analysis: Hf0.335Tc0.665	Hf1Tc2	Hf1Tc2	Hf	1	Tc	2																					1970																												MgZn2(Laves)			A	5.2001		8.6175											MgZn2, C14	K		5.6					5.6																																																																																																									J.LESS-COMMON METALS,22(1970)246	A.L.GIORGI,E.G.SZKLARZ		
101416	1816		Hf0.2Ta0.8	Hf0.2Ta0.8	Hf	0.2	Ta	0.8																					1972																																													cubic	K		6.9					6.9																																																																																																					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
101417	1232		Hg2Mg5	Hg2Mg5	Hg	2	Mg	5																					1966																																														K					0.3																																																																																																							Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101418	1232		Hg3Mg1	Hg3Mg1	Hg	3	Mg	1																					1966																												Mn5Si3																	Mn5Si3, D8[8]	K		0.48					0.48																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101419	1232		Hg1Mg1	Hg1Mg1	Hg	1	Mg	1																					1966																																														K		0.48					0.48																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101420	1232		Hg1Mg1	Hg1Mg1	Hg	1	Mg	1																					1966																												CsCl																	CsCl, B2	K		1.39					1.39																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101421	1232		Hg2Mg1	Hg2Mg1	Hg	2	Mg	1																					1966																												MoSi2																	MoSi2, C11[b]	K		4					4																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101422	258		Hg3Li1	Hg3Li1	Hg	3	Li	1																																																																		hexagonal	K		1.7					1.7																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101423	258		Hg1Li3	Hg1Li3	Hg	1	Li	3																																																																		cubic	K					1.08																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101424	258		Hg7K5	Hg7K5	Hg	7	K	5																																																																			K					1.14																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101425	258		Hg1K1	Hg1K1	Hg	1	K	1																																																																			K					1.14																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101426	258		Hg2K1	Hg2K1	Hg	2	K	1																																																																			K		1.2					1.2																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101427	258		Hg3K1	Hg3K1	Hg	3	K	1																																																																			K		3.18					3.18																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101428	258		Hf4K1	Hf4K1	Hf	4	K	1																																																																			K		3.27					3.27																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101429	91		Hg1Sn1	Hg1Sn1	Hg	1	Sn	1																					1913																																														K		4.2					4.2																																																																																																									Commun. Kamerlingh-Onnes Lab, 13(1913)133d	K.Onnes		
101430	84		Hg1S1	Hg1S1	Hg	1	S	1																					1933																																														K					1.3																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101431	258		Hg5Pt2	Hg5Pt2	Hg	5	Pt	2																																																																			K					1.06																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101432	258		Hg3Pt1	Hg3Pt1	Hg	3	Pt	1																																																																			K					1.06																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101433	489		Hg4Pt1	Hg4Pt1	Hg	4	Pt	1																					1964																																														K					0.32																																																																																																											BULL.AM.PHYS.SOC.,9(1964)268	A.R.SWEEDLER,D.C.HAMILTON,M.F.MERRIAM		
101434	258		Hg2Pt1	Hg2Pt1	Hg	2	Pt	1																																																																			K					1.1																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101435	258		Hg2Na3	Hg2Na3	Hg	2	Na	3																																																																		tetragonal	K					1.08																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101436	258		Hg1Na1	Hg1Na1	Hg	1	Na	1																																																																		orthorhombic	K					1.08																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101437	258		Hg2Na1	Hg2Na1	Hg	2	Na	1																																																																		hexagonal	K		1.62					1.62																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101438	258		Hg4Na1	Hg4Na1	Hg	4	Na	1																																																																			K		3.05					3.05																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101439	661		Hg5Mn2	Hg5Mn2	Hg	5	Mn	2																					1964																																														K					2.1																																																																																																											PHYS.LETT.,7(1964)297	H.A.C.M.BRUNING,H.C.DONKERSLOOT,J.H.N.VAN VUCHT		
101440	1232		Hg1Mg3	Hg1Mg3	Hg	1	Mg	3																					1966																												Na3As																	Na3As, D0[18]	K		0.16					0.16																																																																																																					Superconducting transition temperatures of mercury-alkaline earth metal compounds				J.PHYS.CHEM.SOLIDS,27(1966)1081	T.Claeson,H.L.Luo		
101441	1564		In0.5La3Tl0.5	In0.5La3Tl0.5	In	0.5	La	3	Tl	0.5																			1973																												AuCu3																	AuCu3, L1[2]	K		8.9					8.9																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
101442	1564		In0.8La3Sn0.2	In0.8La3Sn0.2	In	0.8	La	3	Sn	0.2																			1973																												AuCu3																	AuCu3, L1[2]	K		7.8					7.8																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
101443	658	P = 0-35 kbar	La3In	In1La3	In	1	La	3																					1967																																														K		9.83					9.83			K/GPa	0.47																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101444	1564		In1La3	In1La3	In	1	La	3																					1973																												AuCu3																	AuCu3, L1[2]	K		9.54					9.54																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
101445	715		In3La1	In3La1	In	3	La	1																					1970																												AuCu3																	AuCu3, L1[2]	K		0.7					0.7																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101446	1620		In1	In1	In	1																							1970																												In																	In, A6	K		3.409					3.409																																																																																																									PHYS.REV.B,2(1970)2547	D.E.MAPOTHER,D.L.CONNELLY,D.U.GUSER		
101447	291		Ho1	Ho1	Ho	1																							1962																												Mg																	Mg, A3	K					0.38																																																																																																							From Roberts' Table.				LT-8 (London, 1962), paper 5.3	O.V.Lounasmaa		
101448	980		Hg1Zr3	Hg1Zr3	Hg	1	Zr	3																					1967																												Cr3Si(A15)																	Cr3Si, A15	K					0.35																																																																																																											SOLID STATE COMMUN.,5(1967)221	E.VIELHABER,H.L.LUO		
101449	715		Hg3Zr1	Hg3Zr1	Hg	3	Zr	1																					1970																												AuCu3																	AuCu3, L1[2]	K		3.28					3.28																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101450	258		Hg0.698Tl0.302	Hg0.698Tl0.302	Hg	0.698	Tl	0.302																																																																			K		3.888					3.888																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101451	258		Hg0.714Tl0.286	Hg0.714Tl0.286	Hg	0.714	Tl	0.286																																																																			K		3.875					3.875																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101452	258		Hg0.97Tl0.03	Hg0.97Tl0.03	Hg	0.97	Tl	0.03																																																																			K		4.109					4.109																																																																																																					From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
101453	644		In0.11O3W1	In0.11O3W1	In	0.11	O	3	W	1																			1966																																													hexagonal	K		2.8					2.8																																																																																																									SOLID STATE COMMUN.,4(1966)25	F.J.DARNELL,P.E.BIERSTEDT,T.A.BITHER		
101454	427		In0.5Nb3Zr0.5	In0.5Nb3Zr0.5	In	0.5	Nb	3	Zr	0.5																			1962																																														K		6.4					6.4																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101455	1982		In0.15NB3Sb0.15Sn0.7	In0.15Nb3Sb0.15Sn0.7	In	0.15	Nb	3	Sb	0.15	Sn	0.7																	1964																																														K		16.09					16.09																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101456	1982		In0.15Nb3Sn0.85	In0.15Nb3Sn0.85	In	0.15	Nb	3	Sn	0.85																			1964																																														K		18.26					18.26																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101457	508		In1Nb3	In1Nb3	In	1	Nb	3																					1964																																													cubic	K					2.25																																																																																																											PHYS.CHEM.SOLIDS,25(1964)1213	D.H.KILLPATRICK		
101458	8	high pressure and high temperature 	In1Nb3	In1Nb3	In	1	Nb	3																					1952																												Cr3Si(A15)																	Cr3Si, A15	K		8					8																																																																																																									Izv.Akad.Nauk.SSSR Ser.Fiz., 16(1952)233	N.E.Alekseevskii,N.B.Brandt,T.I.Kostina		
101459	1825	sputtered film	In1Nb3	In1Nb3	In	1	Nb	3																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		7.6					7.6																																																																																																									J.APPL.PHYS.,45(1974)4590	H.L.LUO,L.KAMMERDINER		
101460	1866		In0.488Na0.025Pb0.48	In0.488Na0.025Pb0.488	In	0.488	Na	0.025	Pb	0.488																			1975																																														K		6					6																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101461	632		In1N1Ti2	In1N1Ti2	In	1	N	1	Ti	2																			1966																												Cr2AlC																	hexagonal, H-phase	K					1.1																																																																																																											J.LESS-COMMON METALS,10(1966)29	C.M.YEN,L.E.TOTH,W.JEITSCHKO		
101462	558		In1N1	In1N1	In	1	N	1																																																	ZnS(wurtzite)																	ZnS(wurtzite), B4	K		3.38					3.38																																																																																																									INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
101463	1340		In0.18Mg0.82	In0.18Mg0.82	In	0.18	Mg	0.82																					1972																																													hexagonal	K					0.013																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
101464	715		In3Lu1	In3Lu1	In	3	Lu	1																					1970																												AuCu3																	AuCu3, L1[2]	K		0.24					0.24																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101465	489		In1Rh1	In1Rh1	In	1	Rh	1																					1964																												CsCl																	CsCl, B2	K					0.32																																																																																																											BULL.AM.PHYS.SOC.,9(1964)268	A.R.SWEEDLER,D.C.HAMILTON,M.F.MERRIAM		
101466	RMP0350001		In3Rh1	In3Rh1	In	3	Rh	1																					1963																																													tetragonal	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101467	351	deposited at 6 K	In0.97Pd0.03	In0.97Pd0.03	In	0.97	Pd	0.03																					1955																																														K		4.45					4.45																																																																																																									Z.PHYS.,141(1955)263	W.OPITZ		
101468	489		In1Pd1	In1Pd1	In	1	Pd	1																					1964																												CsCl																	CsCl, B2	K		0.7					0.7																																																																																																									BULL.AM.PHYS.SOC.,9(1964)268	A.R.SWEEDLER,D.C.HAMILTON,M.F.MERRIAM		
101469	1041		In0.22Pb0.57Sn0.21	In0.22Pb0.57Sn0.21	In	0.22	Pb	0.57	Sn	0.21																			1966																																														K																																																																																																																APPL.PHYS.LETT.,8(1966)319	J.D.LIVINGSTON		
101470	1491	quench condensation	In0.1Pb0.9	In0.1Pb0.9	In	0.1	Pb	0.9																					1973																																														K		6.8					6.8																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
101471	1269		In0.087Pb0.913	In0.087Pb0.913	In	0.087	Pb	0.913																					1970																																														K		7.035					7.035																																																																																																									PHYS.REV.B,2(1970)105	J.H.FEARDY,R.L.CAPPELLETTI,R.W.ROLLINS		
101472	919		In0.35Pb0.965	In0.35Pb0.965	In	0.35	Pb	0.965																					1969																																														K																																																																																																																J.PHYS.SOC.JAPAN,27(1969)615	M.TAKATA		
101473	809		In0.6Pb0.4	In0.6Pb0.4	In	0.6	Pb	0.4																					1966																																														K		6.36					6.36																																																																																																					From Roberts' Table.				Ann.Acad.Sci.Finnicae A VI No.210(1966)78	F.A.Otter,Jr.,G.B.Yntema		
101474	665		In0.913Pn0.087	In0.913Pb0.087	In	0.913	Pb	0.087																					1964																																														K		4.2					4.2																																																																																																									PHYS.LETT.,13(1964)195	W.F.DRUYYESTEYN		
101475	1025		In0.961Pb0.039	In0.961Pb0.039	In	0.961	Pb	0.039																					1968																																														K		3.64					3.64																																																																																																									SCI.REP.RITU A,20(1968)129	K.NOTO		
101476	1140		In0.955Pb0.045	In0.955Pb0.045	In	0.955	Pb	0.045																					1966																																														K		3.69					3.69																																																																																																									J.PHYS.SOC.JAPAN,21(1966)2122	K.NOTO,T.FUKUROI,Y.MUTO		
101477	1164		In0.88Sn0.12	In0.88Sn0.12	In	0.88	Sn	0.12																					1971																																														K		5.03					5.03																																																																																																									PROC.NAT.ACAD.SCI.,68(1971)56	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,L.D.LONGINOTTI		
101478	204		In0.75Sn0.3	In0.7Sn0.3	In	0.7	Sn	0.3																					1961																																														K		7.3					7.3																																																																																																									J.CHEM.PHYS.,34(1961)2194	B.T.MATTHIAS,J.H.WERNIC		
101479	204		In0.55Sn0.5	In0.5Sn0.5	In	0.5	Sn	0.5																					1961																																														K		6.9					6.9																																																																																																									J.CHEM.PHYS.,34(1961)2194	B.T.MATTHIAS,J.H.WERNIC		
101480	26		In0.75Sn0.25	In0.75Sn0.25	In	0.75	Sn	0.25																					1958																																													tetragonal	K		5.95					5.95																																																																																																					Measurements on superconducting contacts				Phys.Rev.,109(1958)686	H.Meissner		
101481	1073		In0.2Si0.8V3	In0.2Si0.8V3	In	0.2	Si	0.8	V	3																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.2					16.2																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
101482	212		In1Sc3	In1Sc3	In	1	Sc	3																					1962																												Ni3Sn																	Ni3Sn, D0[19]	K																																																																																																																ACTA CRYST.,15(1962)94	B.T.MATTHIAS,V.B.COMPTON		
101483	853		In1Sc2	In1Sc2	In	1	Sc	2																					1971																												Ni2In																	Ni2In, B8[2]	K					4.2																																																																																																											J.PHYS.F:METAL PHYS.,1(1971)93	I.R.HARRIS,W.A.HINES		
101484	1911		In2Sb1Te2	In2Sb1Te2	In	2	Sb	1	Te	2																			1964																												NaCl																	NaCl, B1	K		1.06					1.06																																																																																																									ANGEW.CHEM.INTERNAT.EDIT.,3(1964)588	A.REBENAU,K.DENEKE,M.M.VAN DER MEIJ		
101485	761		In1Sb1Sn1	In1Sb1Sn1	In	1	Sb	1	Sn	1																			1964																												beta-Sn																	beta-Sn, A5	K		2.5					2.5																																																																																																									PHYS.REV.,135(1964)A1460,A145	A.J.DARNELL,B.R.TITTMAN,H.E.BOMMEL,W.R.LIBBY		
101486	1116	rapid quench 	In0.25Sb0.75	In0.25Sb0.75	In	0.25	Sb	0.75																					1971																																													cubic	K		4.1					4.1																																																																																																									PHYS.LETT.A,34(1971)80	C.C.TSUEI,H.YEN,P.DUWEZ		
101487	471		In1Sb1	In1Sb1	In	1	Sb	1																					1963																																														K		2.1					2.1																																																																																																									SCIENCE,140(1963)62-63	D.B.MCWHAN,G.W.HULL JR.,S.GELLER		
101488	711		In3Ru1	In3Ru1	In	3	Ru	1																																																																			K		2.68					2.68																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101489	209		In0.005Tl0.995	In0.005Tl0.995	In	0.005	Tl	0.995																					1961																																														K		2.418					2.418																																																																																																					STUDY OF THE SUPERCONDUCTING TRANSITION TEMPERATURE IN DILUTE THALLIUM SOILD SOLUTIONS				PHYS.REV.,123(1961)466	D.J.QUINN,J.I.BUDNICK		
101490	1377		In1Th2	In1Th2	In	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101491	715		In3Th1	In3Th1	In	3	Th	1																					1970																												AuCu3																	AuCu3, L1[2]	K					0.05																																																																																																											J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101492	515		In3Te4	In3Te4	In	3	Te	4																					1965																																														K		1.25					1.25																																																																																																					Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
101493	515		In2Te3	In2Te3	In	2	Te	3																					1965																																														K					1																																																																																																							Crystal chemistry and superconductivity of pressure-induced phases in the In-Te system				J.PHYS.CHEM.SOLIDS, 26(1965)353	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
101494	506		In1Te1	In1Te1	In	1	Te	1																					1964																												NaCl																	NaCl, B1	K		3.45					3.45																																																																																																									APPL.PHYS.LETT.,4(1964)35	A.JAYARAMAN,G.W.HULL JR.,S.GELLER		
101495	696		In1Te1	In1Te1	In	1	Te	1																					1965																																													tetragonal	K					1.37																																																																																																											SCIENCE,147(1965)1569	C.B.SCLAR,C.C.CARRISON,C.M.SCHWARTZ		
101496	761		In1Te1	In1Te1	In	1	Te	1																					1964																												NaCl																	NaCl, B1	K		2.2					2.2																																																																																																									PHYS.REV.,135(1964)A1460,A145	A.J.DARNELL,B.R.TITTMAN,H.E.BOMMEL,W.R.LIBBY		
101497	229		In2Te1	In2Te1	In	2	Te	1																					1962																																														K					1.37																																																																																																											J.PHYS.CHEM.SOLIDS,23(1962)405	M.F.GENDRON,R.E.JONES		
101498	1724		In0.012Sn0.988	In0.012Sn0.988	In	0.012	Sn	0.988																					1964																																														K		3.69					3.69																																																																																																									J.PHYS.(PARIS),25(1964)374	G.CHOL		
101499	1612		In0.05Sn0.95	In0.05Sn0.95	In	0.05	Sn	0.95																					1969																																														K		3.625					3.625																																																																																																									PHYS.REV.,187(1969)766	F.DELACRUZ,M.CARDONA,M.D.MALONEY		
101500	1917		IN0.5Sn0.5	In0.5Sn0.5	In	0.5	Sn	0.5																					1969																																														K		7.45					7.45																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
101501	469		Ir2Lu1	Ir2Lu1	Ir	2	Lu	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		2.47					2.47																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101502	469		Ir3Lu1	Ir3Lu1	Ir	3	Lu	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		2.89					2.89																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101503	469		Ir3La7	Ir3La7	Ir	3	La	7																					1965																												Fe3Th7																	Fe3Th7, D10[2]	K		2.24					2.24																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101504	469		Ir2La1	Ir2La1	Ir	2	La	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		0.48					0.48																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101505	658		Ir3La7	Ir3La7	Ir	3	La	7																					1967																												Fe3Th7																	Fe3Th7, D10[2]	K		2.32					2.32																																																																																																					Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101506	469		Ir5La1	Ir5La1	Ir	5	La	1																					1965																																														K		2.13					2.13																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101507	1492	RRR > 2000 	Ir1	Ir1	Ir	1																							1973																												Cu																	Cu, A1	K		0.113					0.113																																																																																																									J.LOW TEMP.PHYS.,13(1973)211	D.U.GUBSER,R.J.SOULEN JR.		
101508	RMP0350001		In1Zr3	In1Zr3	In	1	Zr	3																					1963																												AuCu3																	AuCu3, L1[2]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101509	715		In3Yb1	In3Yb1	In	3	Yb	1																					1970																												AuCu3																	AuCu3, L1[2]	K					0.05																																																																																																											J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101510	715		In3Y1	In3Y1	In	3	Y	1																					1970																												AuCu3																	AuCu3, L1[2]	K		0.78					0.78																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101511	824		In1V3	In1V3	In	1	V	3																					1967																												Cr3Si(A15)																		K		13.9					13.9																																																																																																diffusion annealing method (V-wire with In vapor, 1000-1200C, 20h)									ZH.ETF PIS.RED.,6(1967)584	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101512	1900	deposited at 0.3 K 	In0.1Tl0.9	In0.1Tl0.9	In	0.1	Tl	0.9																					1974																																														K		3.27					3.27																																																																																																									Z.PHYS.,269(1974)23	C.G.GRANQVIST,T.CLAAESON		
101513	1580		Ir0.25Mo0.75Nb2.25Pt	Ir0.25Mo0.75Nb2.25Pt0.75	Ir	0.25	Mo	0.75	Nb	2.25	Pt	0.75																																													Cr3Si(A15)																	Cr3Si, A15	K		6.5					6.5																																																																																																					From Roberts' Table.				personal communication	B.R.Coles		
101514	707		Ir1Mo3Nb1Pt1	Ir1Mo3Nb1Pt1	Ir	1	Mo	3	Nb	1	Pt	1																	1969																																														K		5.82					5.82																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101515	707		Ir1Mo3Nb3Pt1	Ir1Mo3Nb3Pt1	Ir	1	Mo	3	Nb	3	Pt	1																	1969																																														K		6.13					6.13																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101516	1438		Ir0.29Mo0.41Nb0.3	Ir0.29Mo0.41Nb0.3	Ir	0.29	Mo	0.41	Nb	0.3																			1974																																														K		8.7					8.7																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101517	33		Ir1Mo1	Ir1Mo1	Ir	1	Mo	1																					1955																																													hexagonal	K		1.85			1		1.85																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
101518	1039		Ir1Mo1	Ir1Mo1	Ir	1	Mo	1																					1965																												AuCd																	AuCd, B19	K		8.8					8.8																																																																																																									APPL.PHYS.LETT.,7(1965)72	E.R.GIESSEN,E.R.SADAGOPAN,H.C.GATOS		
101519	276		Ir0.26Mo0.74	Ir0.26Mo0.74	Ir	0.26	Mo	0.74																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6.7					6.7																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101520	1446		Ir1Mo3	Ir1Mo3	Ir	1	Mo	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		8.8					8.8																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101521	469		Ir1Lu3	Ir1Lu3	Ir	1	Lu	3																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101522	469		Ir3Lu7	Ir3Lu7	Ir	3	Lu	7																					1965																																														K		0.78					0.78																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101523	469		Ir1Lu2	Ir1Lu2	Ir	1	Lu	2																					1965																																														K		0.84					0.84																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101524	469		Ir1Lu1	Ir1Lu1	Ir	1	Lu	1																					1965																												CsCl			A	3.33													CsCl, B2	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101525	492		Ir0.05Nb3Rh0.95	Ir0.05Nb3Rh0.95	Ir	0.05	Nb	3	Rh	0.95																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		2.38					2.38																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
101526	492		Ir0.02Nb3Rh0.98	Ir0.02Nb3Rh0.98	Ir	0.02	Nb	3	Rh	0.98																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		2.43					2.43																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
101527	1299		Ir0.45Nb1Pt2.55	Ir0.45Nb1Pt2.55	Ir	0.45	Nb	1	Pt	2.55																			1966																												Ni3Sn																	Ni3Sn, D0[19]	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101528	1299		Ir2.55Nb1Pt0.45	Ir2.55Nb1Pt0.45	Ir	2.55	Nb	1	Pt	0.45																			1966																																													hexagonal	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101529	1299		Ir2.67Nb1Pt0.24	Ir2.67Nb1Pt0.24	Ir	2.67	Nb	1	Pt	0.24																			1966																												AuCu3																	AuCu3, L1[2]	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101530	592		Ir0.1Nb0.9	Ir0.1Nb0.9	Ir	0.1	Nb	0.9																					1965																																														K		2.3					2.3																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101531	1625		Ir0.34Nb0.66	Ir0.34Nb0.66	Ir	0.34	Nb	0.66																					1971																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.25					2.25																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
101532	1466		Ir1Nb3	Ir1Nb3	Ir	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.07					2.07																																																																																																									J.JAPAN INST.METALS,37(1973)558	K.TACHIKAWA,Y.YOSHIDA		
101533	1299		Ir1.05Nb0.95	Ir1.05Nb0.95	Ir	1.05	Nb	0.95																					1966																												AuCu																	AuCu, L1[0]	K		4.75					4.75																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101534	1299		Ir1.15Nb	Ir1.15Nb0.85	Ir	1.15	Nb	0.85																					1966																																													orthorhombic	K		4.6					4.6																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101535	4.2		Ir3Nb1	Ir3Nb1	Ir	3	Nb	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																														
101536	1438		Ir0.3Mo0.4Re0.3	Ir0.3Mo0.4Re0.3	Ir	0.3	Mo	0.4	Re	0.3																			1974																																														K		9.5					9.5																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101537	201		Ir1.5O0.5Y1	Ir1.5O0.5Y1	Ir	1.5	O	0.5	Y	1																			1959																																														K		2.4					2.4																																																																																																									J.PHYS.CHEM.SOLIDS,11(1959)346	B.T.MATTHIAS,E.CORENZWIT,H.SUHL		
101538	171		Ir1Os1Y1	Ir1Os1Y1	Ir	1	Os	1	Y	1																			1960																																														K		2.6					2.6																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
101539	963		Ir0.825Os0.1Ru0.075	Ir0.825Ru0.1Os0.075	Ir	0.825	Ru	0.1	Os	0.075																			1968																																														K		0.16					0.16																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101540	963		Ir0.73Os0.17Ru0.1	Ir0.73Os0.17Ru0.1	Ir	0.73	Os	0.17	Ru	0.1																			1968																																														K		0.34					0.34																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101541	963		Ir0.76Os0.09Rh0.15	Ir0.76Os0.09Rh0.15	Ir	0.76	Os	0.09	Rh	0.15																			1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101542	963		Ir0.75Os0.05Rh0.2	Ir0.75Os0.05Rh0.2	Ir	0.75	Os	0.05	Rh	0.2																			1968																																														K		0.055					0.055																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101543	963		Ir0.18Os0.47Rh0.35	Ir0.18Os0.47Rh0.35	Ir	0.18	Os	0.47	Rh	0.35																			1968																																														K		0.55					0.55																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101544	963		Ir0.75Os0.25	Ir0.75Os0.25	Ir	0.75	Os	0.25																					1968																																														K		0.4					0.4																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101545	239		Ir0.5Os0.5	Ir0.5Os0.5	Ir	0.5	Os	0.5																					1963																																													cubic	K		0.98					0.98																																																																																																					SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
101546	RMP0350001		Ir0.265O0.085Zr0.65	Ir0.265O0.085Zr0.65	Ir	0.265	O	0.085	Zr	0.65																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		2.3					2.3																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101547	RMP0350001		Ir0.287O0.14Ti0.573	Ir0.287O0.14Ti0.573	Ir	0.287	O	0.14	Ti	0.573																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		5.5					5.5																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101548	1624		Ir0.984Ni0.016	Ir0.984Ni0.016	Ir	0.984	Ni	0.016																					1971																																														K		0.052					0.052																																																																																																									PHYS.REV.B,3(1971)91	G.RIBLET.		
101549	1438		Ir0.2Ru0.05Zr0.75	Ir0.2Ru0.05Zr0.75	Ir	0.2	Ru	0.05	Zr	0.75																			1974																																														K		6.8					6.8																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101550	1438		Ir0.125Rh0.125Zr0.75	Ir0.125Rh0.125Zr0.75	Ir	0.125	Rh	0.125	Zr	0.75																			1974																																														K		10.2					10.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101551	1060		Ir0.05Rh0.04Ti0.91	Ir0.05Rh0.04Ti0.91	Ir	0.05	Rh	0.04	Ti	0.91																			1964																																														K		4					4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101552	963		Ir0.3Rh0.5Ru0.2	Ir0.3Rh0.5Ru0.2	Ir	0.3	Rh	0.5	Ru	0.2																			1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101553	963		Ir0.98Re0.02	Ir0.98Re0.02	Ir	0.98	Re	0.02																					1968																																														K		1.7					1.7																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101554	963		Ir0.775Pt0.175Rh0.5	Ir0.775Pt0.175Rh0.05	Ir	0.775	Pt	0.175	Rh	0.05																			1968																																														K		0.032					0.032																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101555	963		Ir0.72Pt0.08Rh0.02	Ir0.72Pt0.08Rh0.2	Ir	0.72	Pt	0.08	Rh	0.2																			1968																																														K		0.03					0.03																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101556	963		Ir0.8Pt0.2	Ir0.8Pt0.2	Ir	0.8	Pt	0.2																					1968																																														K		0.046					0.046																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101557	963		Ir0.9Pt0.1	Ir0.9Pt0.1	Ir	0.9	Pt	0.1																					1968																																														K		0.066					0.066																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101558	963		Ir0.83Pd0.04Pt0.125	Ir0.83Pd0.045Pt0.125	Ir	0.83	Pd	0.045	Pt	0.125																			1968																																														K		0.037					0.037																																																																																																					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101559	491		Ir1P1	Ir1P1	Ir	1	P	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101560	491		Ir2P1	Ir2P1	Ir	2	P	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101561	RMP0350001		Ir1Si1	Ir1Si1	Ir	1	Si	1																					1963																												MnP																	MnP, B31	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101562	552		Ir1Se2.9	Ir1Se2.9	Ir	1	Se	2.9																					1965																																														K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101563	552		Ir1Se2	Ir1Se2	Ir	1	Se	2																					1965																															A	20.94	5.93	3.74											orthorhombic	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101564	127		Ir2.5Sc1	Ir2.5Sc1	Ir	2.5	Sc	1																					1959																												MgCu2(Laves)																	MgCu2, C15	K		2.46					2.46																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
101565	469		Ir0.32Sc0.68	Ir0.32Sc0.68	Ir	0.32	Sc	0.68																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101566	469		Ir1Sc1	Ir1Sc1	Ir	1	Sc	1																					1965																												CsCl			A	3.205													CsCl, B2	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101567	469		Ir3Sc1	Ir3Sc1	Ir	3	Sc	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101568	469		Ir1Sc3	Ir1Sc3	Ir	1	Sc	3																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101569	491		Ir2Sb1	Ir2Sb1	Ir	2	Sb	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
101570	481		Ir1Sb1	Ir1Sb1	Ir	1	Sb	1																																																	NiAs																	NiAs, B8[1]	K					0.35																																																																																																											LT-9(1965)600	R.C.Miller,R.A.Hein,J.W.Gibson,J.K.Hulm,C.K.Jones,R.Mazelsky		
101571	552		Ir1S2.6	Ir1S2.6	Ir	1	S	2.6																					1965																																														K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101572	552		Ir1S1	Ir1S1	Ir	1	S	1																					1965																																														K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101573	173		Ir2Th1	Ir2Th1	Ir	2	Th	1																					1961																												MgCu2(Laves)			A	7.664													MgCu2, C15	K		6.5					6.5																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101574	469		Ir3Th1	Ir3Th1	Ir	3	Th	1																					1965																																														K		4.71					4.71																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101575	469		Ir5Th1	Ir5Th1	Ir	5	Th	1																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K		3.93					3.93																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101576	552		Ir0.5Te0.5	Ir0.5Te0.5	Ir	0.5	Te	0.5																					1965																												NiAs																	NiAs, B8[1]	K		3					3																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101577	552		Ir1Te2	Ir1Te2	Ir	1	Te	2																					1965																												CdI2			A	3.93		5.393											CdI2, C6	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101578	552		Ir1Te3	Ir1Te3	Ir	1	Te	3																					1965																												FeS2(pyrite)			A	6.413													FeS2(pyrite), C2	K		1.18					1.18																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
101579	963		Ir0.85Ta0.15	Ir0.85Ta0.15	Ir	0.85	Ta	0.15																					1968																																														K					0.024																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
101580	276		Ir0.35Ta0.65	Ir0.35Ta0.65	Ir	0.35	Ta	0.65																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.2																																																																																																											HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101581	28		Ir2Sr1	Ir2Sr1	Ir	2	Sr	1																					1957																												MgCu2(Laves)																	MgCu2, C15	K		5.7					5.7																																																																																																					Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
101582	486		Ir1Sn2	Ir1Sn2	Ir	1	Sn	2																					1965																												CaF2																	CaF2, C1	K		0.78					0.78																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
101583	1438		Ir0.2Si0.05Zr0.75	Ir0.2Si0.05Zr0.75	Ir	0.2	Si	0.05	Zr	0.75																			1974																																														K		6.2					6.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101584	RMP0350001		Ir1Si3	Ir1Si3	Ir	1	Si	3																					1963																												Na3As																	Na3As, D0[18]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101585	498		Ir0.33V2.67	Ir0.33V2.67	Ir	0.33	V	2.67																					1965																																														K		1.39					1.39																																																																																																					SUPERCONDUCTIVITY OF NB3GE				PHYS.REV.,139(1965)A1501	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,R.H.WILLENS,T.H.GEBALLE		
101586	948		Ir1V3	Ir1V3	Ir	1	V	3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											J.PHYS.CHEM.SOLIDS, 31(1970)1531	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FLUKIGER		
101587	1299		Ir1V1	Ir1V1	Ir	1	V	1																					1966																																													orthorhombic	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101588	1299		Ir1V1	Ir1V1	Ir	1	V	1																					1966																												AuCu																	AuCu, L1[0]	K					1.36																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101589	1299		Ir2U1	Ir2U1	Ir	2	U	1																					1966																												AuCu3																	AuCu3, L1[2]	K					4.2																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101590	RMP0350001		Ir3V1	Ir3V1	Ir	3	V	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101591	412		Ir3U3	Ir3U1	Ir	3	U	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
101592	717		Ir0.04Ti0.96	Ir0.04Ti0.96	Ir	0.04	Ti	0.96																					1964																																													cubic	K		1.6					1.6																																																																																																					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
101593	717		Ir0.1Ti0.9	Ir0.1Ti0.9	Ir	0.1	Ti	0.9																					1964																																													cubic	K		4.3					4.3																																																																																																					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
101594	1446		Ir1Ti3	Ir1Ti3	Ir	1	Ti	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		4.97					4.97																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101595	173		Ir3Th7	Ir3Th7	Ir	3	Th	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		1.52					1.52																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101596	469		Ir1Th1	Ir1Th1	Ir	1	Th	1																					1965																																														K		0.37					0.37																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101597	1476		Ir1Zr3	Ir1Zr3	Ir	1	Zr	3																					1971																																													tetragonal	K		2.13					2.13																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101598	1476		Ir3Zr5	Ir3Zr5	Ir	3	Zr	5																					1971																												Mn5Si3																	Mn5Si3, D8[8]	K					1.2																																																																																																											J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101599	1476		Ir1Zr2	Ir1Zr2	Ir	1	Zr	2																					1971																												CuAl2																	CuAl2, C16	K		7.23					7.23																																																																																																									J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
101600	173		Ir2Zr1	Ir2Zr1	Ir	2	Zr	1																					1961																												MgCu2(Laves)																	MgCu2, C15	K		4.1					4.1																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101601	247		Ir2Yb1	Ir2Yb1	Ir	2	Yb	1																					1959																																														K					1.3																																																																																																							MAGNETIZATION OF COMPOUNDS OF RARE EARTHS WITH PLATINUM METALS				PHYS.REV.,115(1959)1595	B.T.MATTHIAS,D.D.DAVIS,E.CORENZWIT,H.SHUL,R.M.BOZORTH		
101602	469		Ir0.7Y0.3	Ir0.7Y0.3	Ir	0.7	Y	0.3																					1965																												MgCu2(Laves)																	MgCu2, C15	K		2.16					2.16																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101603	469		Ir1Y4	Ir1Y4	Ir	1	Y	4																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101604	469		Ir2Y3	Ir2Y3	Ir	2	Y	3																					1965																																														K		1.61					1.61																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101605	127		Ir2Y1	Ir2Y1	Ir	2	Y	1																					1959																												MgCu2(Laves)																	MgCu2, C15	K		2.18					2.18																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
101606	469		Ir3Y1	Ir3Y1	Ir	3	Y	1																					1965																																														K		3.5					3.5																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101607	33		Ir0.25W0.75	Ir0.25W0.75	Ir	0.25	W	0.75																					1955																																														K		3.82					3.82																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
101608	295		Ir0.28W0.72	Ir0.28W0.72	Ir	0.28	W	0.72																					1962																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.46					4.46																																																																																																					FROM Roberts' Table.				LT-8(1962, London ) paper 4.8	E.Bucher,F.Heiniger,J.Muller		
101609	1271		La0.98Lu0.02	La0.98Lu0.02	La	0.98	Lu	0.02																					1970																																														K		4.643					4.643																																																																																																					Coexistence of superconductivity and short-range magnetic order				PHYS.REV.B,2(1970)1287	D.K.FINNEMORE,L.J.WILLIAMS,W.R.DECKER		
101610	115		La0.99Lu0.01	La0.99Lu0.01	La	0.99	Lu	0.01																					1958																																													hexagonal	K		5.6					5.6																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101611	11		K1Sb1	K1Sb1	K	1	Sb	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101612	1212		K0.3O3Re1	K0.3O3Re1	K	0.3	O	3	Re	1																			1969																																													hexagonal	K		3.6					3.6																																																																																																									SOLID STATE COMMUN.,7(1969)299	A.W.SLEIGHT,P.E.BIERSTEDT,T.A.BITHER		
101613	1974		K0.28Mo1S2	K0.28Mo1S2	K	0.28	Mo	1	S	2																			1971																																														K		6.2					6.2																																																																																																									JPL QUARTERLY TECH.REV.,1(1971)33	A.REMBAUM,R.B.SOMOANO		
101614	1920		K0.4Mo1S2	K0.4Mo1S2	K	0.4	Mo	1	S	2																			1973																												3R-MoS2			A	3.2072		24.7915											hexagonal	K		5.5					5.5																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
101615	1920		K0.4Mo1S2	K0.4Mo1S2	K	0.4	Mo	1	S	2																			1973																												2H-MoS2			A	3.2036		16.5804											hexagonal	K		6.1					6.1																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
101616	1212		K0.9Mo1O3	K0.9Mo1O3	K	0.9	Mo	1	O	3																			1969																																														K					1.3																																																																																																											SOLID STATE COMMUN.,7(1969)299	A.W.SLEIGHT,P.E.BIERSTEDT,T.A.BITHER		
101617	1212		K0.5Mo1O3	K0.5Mo1O3	K	0.5	Mo	1	O	3																			1969																																													tetragonal	K		4.2					4.2																																																																																																									SOLID STATE COMMUN.,7(1969)299	A.W.SLEIGHT,P.E.BIERSTEDT,T.A.BITHER		
101618	23		K1	K1	K	1																							1951																												W																	W, A2	K					0.08																																																																																																											Nature, 167(1951)111	B.B.Goodman		
101619	1438		Ir0.25Zr0.75	Ir0.25Zr0.75	Ir	0.25	Zr	0.75																					1974																																														K		8					8																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101620	32		Ir0.1Zr0.9	Ir0.1Zr0.9	Ir	0.1	Zr	0.9																					1955																																													hexagonal	K		5.5					5.5																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
101621	469		La1Pt2	La1Pt2	La	1	Pt	2																					1965																												MgCu2(Laves)																	MgCu2, C15	K		0.46					0.46																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101622	1490		La0.98Pr0.02Ru2	La0.98Pr0.02Ru2	La	0.98	Pr	0.02	Ru	2																			1972																												MgCu2(Laves)																	MgCu2, C15	K		1.92					1.92																																																																																																					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
101623	115		La0.99Pr0.01	La0.99Pr0.01	La	0.99	Pr	0.01																					1958																																														K		5.3					5.3																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101624	768		La1Pb3	La1Pb3	La	1	Pb	3																					1968																												AuCu3																	AuCu3, L1[2]	K		4.07					4.07																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
101625	1375		La1Os2	La1Os2	La	1	Os	2																					1973																												MgZn2(Laves)																	MgZn2, C14	K		6.5					6.5																																																																																																									J.LESS-COMMON METALS,32(1973)173	A.C.LAWSON		
101626	1897		La1Os2	La1Os2	La	1	Os	2																					1975																												MgCu2(Laves)																	MgCu2, C15	K		8.9					8.9																																																																																																									SOLID STATE COMMUN.,16(1975)341	H.E.HOENING		
101627	1565		La1	La1	La	1																							1971																																														K		3.3					3.3																																																																																																									PHYSICA,55(1971)555	J.I.GITTLEMAN,J.J.HANAK		
101628	668		La1N1	La1N1	La	1	N	1																					1965																																														K		1.35					1.35																																																																																																									PHYS.LETT.,14(1965)261	A.NEMOZ,D.BROCHIER,J.BLANC,J.J.VEYSSIE		
101629	1759		La0.2Mo6.35Pb0.8S8	La0.2Mo6.35Pb0.8S8	La	0.2	Mo	6.35	Pb	0.8	S	8																	1974																																														K		13.2					13.2																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101630	658		La1Mg2	La1Mg2	La	1	Mg	2																					1967																												MgCu2(Laves)																	MgCu2, C15	K		1.05					1.05																																																																																																					Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101631	22		La0.55Lu0.45	La0.55Lu0.45	La	0.55	Lu	0.45																					1958																																													hexagonal	K		2.2					2.2																																																																																																					Superconductivity of Lanthanum and Some Lanthanum Alloys				Phys.Rev., 109(1958)243	G.S.Anderson,S.Legvold,F.H.Spedding		
101632	22		La0.8Lu0.2	La0.8Lu0.2	La	0.8	Lu	0.2																					1958																																													hexagonal	K		3.4					3.4																																																																																																					Superconductivity of Lanthanum and Some Lanthanum Alloys				Phys.Rev., 109(1958)243	G.S.Anderson,S.Legvold,F.H.Spedding		
101633	808		La1Si2	La1Si2	La	1	Si	2																					1966																												ThSi2																	ThSi2, C[c]	K		2.3					2.3																																																																																																					FROM Roberts' Table.				Ann.Acad.Sci.Finnicae A, VI No.210(1966)p=92	T.Ohtsuka,T.Satoh		
101634	288		La5Si3	La5Si3	La	5	Si	3																					1962																																														K		1.6					1.6																																																																																																									BULL.AMER.PHYS.SOC.,7(1962)474,621	C.BETZ,H.MUIR,W.E.HENRY		
101635	1965		La2.4Se4Y0.6	La2.4Se4Y0.6	La	2.4	Se	4	Y	0.6																			1975																												Th3P4			A	9.004													Th3P4, D7[3]	K		3.92					3.92																																																								mj/mol.K2	4.5		221																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101636	1965		La3Se4	La3Se4	La	3	Se	4																					1975																												Th3P4			A	9.06													Th3P4, D7[3]	K		7.8					7.8																																																								mj/mol.K2	6.3		195																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101637	1965		La1Se1	La1Se1	La	1	Se	1																					1975																												NaCl			A	6.06													NaCl, B1	K		1.02					1.02																																																								mj/mol.K2	3.77		231																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101638	1965		La2.4S4Y0.6	La2.4S4Y0.6	La	2.4	S	4	Y	0.6																			1975																												Th3P4			A	8.67													Th3P4, D7[3]	K		4.77					4.77																																																								mj/mol.K2	6.2		252																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101639	1965		La3S4	La3S4	La	3	S	4																					1975																												Th3P4			A	8.73													Th3P4, D7[3]	K		8.06					8.06																																																								mj/mol.K2	7.2		230																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101640	1965		La1S1	La1S1	La	1	S	1																					1975																												NaCl			A	5.856													NaCl, B1	K		0.84					0.84																																																								mj/mol.K2	3.28		276																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
101641	1026		La1Ru2	La1Ru2	La	1	Ru	2																					1970																												MgCu2(Laves)																	MgCu2, C15	K		4.1					4.1																																																																																																									PHYS.LETT.A,33(1970)61	B.HILLENBRAND,M.WILLHELM		
101642	469		La7Rh3	La7Rh3	La	7	Rh	3																					1965																												Fe3Th7																	Fe3Th7, D10[2]	K		2.58					2.58																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101643	469		La1Rh5	La1Rh5	La	1	Rh	5																					1965																																														K		1.62					1.62																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101644	469		La1Rh3	La1Rh3	La	1	Rh	3																					1965																																														K		2.6					2.6																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101645	1856		La0.7Y0.3	La0.7Y0.3	La	0.7	Y	0.3																					1974																																													hexagonal	K		1.85					1.85																																																																																																									J.PHYS.SOC.JAPAN,36(1974)1485	J.TAKEUCHI,T.AOI,Y.MASUDA		
101646	808		La0.75Y0.25	La0.75Y0.25	La	0.75	Y	0.25																					1966																																														K		2.5					2.5																																																																																																					FROM Roberts' Table.				Ann.Acad.Sci.Finnicae A, VI No.210(1966)p=92	T.Ohtsuka,T.Satoh		
101647	856		La0.85Y0.15	La0.85Y0.15	La	0.85	Y	0.15																					1968																																													hexagonal	K		3.06					3.06																																																																																																									PHYS.LETT.A,27(1968)264	E.DUCLA-SOARES,J.D.N.CHEEWE		
101648	22		La0.95Y0.05	La0.95Y0.05	La	0.95	Y	0.05																					1958																																														K		5.4					5.4																																																																																																					Superconductivity of Lanthanum and Some Lanthanum Alloys				Phys.Rev., 109(1958)243	G.S.Anderson,S.Legvold,F.H.Spedding		
101649	1240		La1Tl3	La1Tl3	La	1	Tl	3																					1968																												AuCu3																	AuCu3, L1[2]	K		1.57					1.57																																																																																																									J.PHYS.CHEM.SOLIDS,29(1968)295	A.M.TOXMAN,N.R.STEMPLE,R.J.GAMBINO		
101650	1564		La3Tl1	La3Tl1	La	3	Tl	1																					1973																												AuCu3																	AuCu3, L1[2]	K		8.86					8.86																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
101651	1370		La3Te4	La3Te4	La	3	Te	4																					1973																												Th3P4																	Th3P4, D7[3]	K		5.3					5.3																																																																																																					FROM Roberts' Table.				personal commun.	E.Bucher,K.Andres,F.J.Disalvo		
101652	1370		La1Te1	La1Te1	La	1	Te	1																					1973																												NaCl																	NaCl, B1	K		1.48					1.48																																																																																																					FROM Roberts' Table.				personal commun.	E.Bucher,K.Andres,F.J.Disalvo		
101653	1329		La0.84Sn3Tm0.16	La0.84Sn3Tm0.16	La	0.84	Sn	3	Tm	0.16																			1973																																														K		3.3					3.3																																																																																																									SOLID STATE COMMUN.,13(1973)25	A.R.SWEEDLER,J.E.CROW,R.P.GUERTIN,S.FONER		
101654	1240		La1Sn3	La1Sn3	La	1	Sn	3																					1968																												AuCu3																	AuCu3, L1[2]	K		6.5					6.5																																																																																																									J.PHYS.CHEM.SOLIDS,29(1968)295	A.M.TOXMAN,N.R.STEMPLE,R.J.GAMBINO		
101655	1913		La0.06Si1V2.94	La0.06Si1V2.94	La	0.06	Si	1	V	2.94																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		15.92					15.92																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101656	1913		La0.006Si1V2.994	La0.006Si1V2.994	La	0.006	Si	1	V	2.994																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		16.48					16.48																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101657	469		Lu0.275Rh0.725	Lu0.275Rh0.725	Lu	0.275	Rh	0.725																					1965																												MgCu2(Laves)																	MgCu2, C15	K		1.27					1.27																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101658	469		Lu1Rh5	Lu1Rh5	Lu	1	Rh	5																					1965																																														K		0.49					0.49																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
101659	127		Lu1Os2	Lu1Os2	Lu	1	Os	2																					1959																												MgZn2(Laves)																	MgZn2, C14	K		3.49					3.49																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
101660	85		Li1Pb1	Li1Pb1	Li	1	Pb	1																					1932																																														K		7.2					7.2																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
101661	1379		Li0.3O3W1	Li0.3O3W1	Li	0.3	O	3	W	1																			1968																																													hexagonal	K		2.2					2.2																																																																																																									INORGANIC CHEM.,7(1968)1646	A.W.SLEIGHT,D.C.PEASE,T.A.BITHER,T.E.GIER		
101662	1920	Li-content x is not described ( 0.4=<x=<1.0). hexagonal.	LixMo1S2	Li0.4Mo1S2	Li	0.4	Mo	1	S	2																			1973																												2H-MoS2			A			19.039											hexagonal	K		3.7					3.7																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
101663	658		La1Zn1	La1Zn1	La	1	Zn	1																					1967																												CsCl																	CsCl, B2	K		1.04					1.04			K/GPa	0.085																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
101664	115		La0.99Y0.01	La0.99Y0.01	La	0.99	Y	0.01																					1958																																														K		5.5					5.5																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
101665	808		La0.15Y0.85	La0.15Y0.85	La	0.15	Y	0.85																					1966																																													hexagonal	K		0.1			0.1		0.1																																																																																																					FROM Roberts' Table.				Ann.Acad.Sci.Finnicae A, VI No.210(1966)p=92	T.Ohtsuka,T.Satoh		
101666	1350		La0.35Y0.65	La0.35Y0.65	La	0.35	Y	0.65																					1967																																													hexagonal	K		0.4					0.4																																																																																																									J.PHYS.SOC.JAPAN,23(1967)9	T.OHTSUKA,T.SATOH		
101667	808		La0.48Y0.52	La0.48Y0.52	La	0.48	Y	0.52																					1966																																													rhombohedral	K		1					1																																																																																																					FROM Roberts' Table.				Ann.Acad.Sci.Finnicae A, VI No.210(1966)p=92	T.Ohtsuka,T.Satoh		
101668	1856		La0.6Y0.4	La0.6Y0.4	La	0.6	Y	0.4																					1974																																														K		1.29					1.29																																																																																																									J.PHYS.SOC.JAPAN,36(1974)1485	J.TAKEUCHI,T.AOI,Y.MASUDA		
101669	1604		Mg2Zn11	Mg2Zn11	Mg	2	Zn	11																					1974																																													cubic	K		0.88					0.88																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101670	1604		Mg1Zn1	Mg1Zn1	Mg	1	Zn	1																					1974																												MgZn2(Laves)																	MgZn2, C14	K		0.93					0.93																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101671	1604		Mg2Zn3	Mg2Zn3	Mg	2	Zn	3																					1974																																														K		0.76					0.76																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101672	1604		Mg1Zn1	Mg1Zn1	Mg	1	Zn	1																					1974																																														K		0.92					0.92																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101673	1604		Mg7Zn3	Mg7Zn3	Mg	7	Zn	3																					1974																																														K		0.28					0.28																																																																																																									PHYSICA SCRIPTA,9(1974)353	T.ALAESON		
101674	13		Mg0.47Tl0.53	Mg0.47Tl0.53	Mg	0.47	Tl	0.53																					1951																												CsCl																	CsCl, B2	K		2.75					2.75																																																																																																									Proc.of Low Temp.Conf.NBS, 65(1951)	L.Guttman,J.W.Stout		
101675	1491		Mg0.1Pb0.9	Mg0.1Pb0.9	Mg	0.1	Pb	0.9																					1973																																														K		6.61					6.61																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
101676	427		Mg2Pb1	Mg2Pb1	Mg	2	Pb	1																					1962																																														K		5.6					5.6																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101677	1163		Mg0.9Mo5.1S6	Mg0.9Mo5.1S6	Mg	0.9	Mo	5.1	S	6																			1972																																													rhombohedral	K		2.5					2.5																																																																																																									SCI.,175(1972)1465	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO		
101678	1219		Lu1Se1	Lu1Se1	Lu	1	Se	1																					1970																												NaCl																	NaCl, B1	K		0.56					0.56																																																																																																									SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
101679	1210		Lu1S1	Lu1S1	Lu	1	S	1																					1966																												NaCl																	NaCl, B1	K		1.1					1.1																																																																																																									J.APPL.PHYS.,37(1966)4880	R.E.ENSTROM		
101680	RMP0350001		Lu1Ru2	Lu1Ru2	Lu	1	Ru	2																					1963																												MgZn2(Laves)																	MgZn2, C14	K		0.86					0.86																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101681	11		Mo1N1	Mo1N1	Mo	1	N	1																					1952																																													hexagonal	K		12					12																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101682	11		Mo2N1	Mo2N1	Mo	2	N	1																					1952																																													cubic	K		5					5																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
101683	1031		Mo1	Mo1	Mo	1																							1965																												W																	W, A2	K		0.916					0.916																																																																																																									ZH.EKSP.TEOR.FIZ.,49(1965)1091	A.D.SHVETS,I.G.D'YAKOV		
101684	21		Mn1U6	Mn1U6	Mn	1	U	6																					1958																												U6Mn																	MnU6, D2[c]	K		2.32					2.32																																																																																																									J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
101685	490		Mn0.01Ti0.99	Mn0.01Ti0.99	Mn	0.01	Ti	0.99																					1963																																														K		1.2					1.2																																																																																																					SUPERCONDUCTIVITY OF TITANIUM				PHYS.REV.LETT.,11(1963)248	JR.,R.L.FALGE		
101686	477		Mn0.02Ti0.98	Mn0.02Ti0.98	Mn	0.02	Ti	0.98																					1965																																														K		1.9					1.9																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
101687	759		Mn0.14Ti0.86	Mn0.14Ti0.86	Mn	0.14	Ti	0.86																					1964																																														K		2.55					2.55																																																																																																									PHYS.REV.,135(1964)A1151	J.A.CAPE,R.R.HAKE		
101688	1913		Mn0.21Si1V2.79	Mn0.21Si1V2.79	Mn	0.21	Si	1	V	2.79																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		15.5					15.5																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101689	1913		Mn0.03si1V2.97	Mn0.03Si1V2.97	Mn	0.03	Si	1	V	2.97																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		16.25					16.25																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101690	1060		Mn0.05Rh0.04Ti0.91	Mn0.05Rh0.04Ti0.91	Mn	0.05	Rh	0.04	Ti	0.91																			1964																																														K		2.4					2.4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101691	1866		Mn0.33Ni0.67U6	Mn0.33Ni0.67U6	Mn	0.33	Ni	0.67	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		1.6					1.6																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101692	1866		Mn0.67Ni0.33U6	Mn0.67Ni0.33U6	Mn	0.67	Ni	0.33	U	6																			1975																												U6Mn																	MnU6, D2[c]	K		2.7					2.7																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101693	1438		Mo0.3Nb0.1Re0.6	Mo0.3Nb0.1Re0.6	Mo	0.3	Nb	0.1	Re	0.6																			1974																																														K		10.1					10.1																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101694	881		Mo0.725Nb0.061Re0.18	Mo0.725Nb0.061Re0.187	Mo	0.725	Nb	0.061	Re	0.187																			1969																																														K		5					5																																																																																																									J.LOW TEMP.PHYS.,1(1969)355	H.E.HOENING,N.BARTH		
101695	1513		Mo0.02Nb0.98	Mo0.02Nb0.98	Mo	0.02	Nb	0.98																					1969																																														K		8.58					8.58																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
101696	1157		Mo0.05Nb0.95	Mo0.05Nb0.95	Mo	0.05	Nb	0.95																					1967																																														K		8					8																																																																																																									PHYS.REV.,158(1967)340	D.M.GINSBERG,J.K.HULM,R.L.CAPPELLETTI		
101697	1298		Mo0.1Nb0.9	Mo0.1Nb0.9	Mo	0.1	Nb	0.9																					1968																																														K		6.38					6.38																																																																																																									PHYS.REV.,173(1968)504	J.LOWELL,R.A.FRENH		
101698	1103		Mo0.15Nb0.85	Mo0.15Nb0.85	Mo	0.15	Nb	0.85																					1967																																														K		5.3					5.3																																																																																																									CRYOGENICS,7(1967)83	J.LOWELL,K.MENDELSSOHN,R.A.FRENCH		
101699	1103		Mo0.2Nb0.8	Mo0.2Nb0.8	Mo	0.2	Nb	0.8																					1967																																														K		4.23					4.23																																																																																																									CRYOGENICS,7(1967)83	J.LOWELL,K.MENDELSSOHN,R.A.FRENCH		
101700	1696		Mo0.25Nb0.75	Mo0.25Nb0.75	Mo	0.25	Nb	0.75																					1966																																														K		3.47					3.47																																																																																																									ZH.EKSP.TEOR.FIZ.,51(1966)59	N.B.BRANDT,N.I.GINZBURG		
101701	300		Mo0.4Nb0.6	Mo0.4Nb0.6	Mo	0.4	Nb	0.6																					1962																																														K		0.6					0.6																																																																																																					FROM Roberts' Table.				LT-8(1962, London ) paper 4.5	R.D.Blaugher,J.K.Hulm,J.A.. Rayne,B.W.Veal,R.A.Hein		
101702	432		Mo0.7Nb0.3	Mo0.7Nb0.3	Mo	0.7	Nb	0.3																					1963																																														K		0.016					0.016																																																																																																					SUPERCONDUCTIVITY BELOW 20 MILLIDEGREES				PHYS.REV.LETT.,11(1963)6	J.W.GIBSON,R.A.HEIN,R.D.BLAUGHER		
101703	1920	Na-content not  x  described (0.3=<x=<0.6). hexagonal	Mo1NaxS2	Mo1Na0.3S2	Mo	1	Na	0.3	S	2																			1973																												2H-MoS2			A			14.998											hexagonal	K		4.1					4.1																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
101704	1841		Mo1N1	Mo1N1	Mo	1	N	1																					1974																																													hexagonal	K		14.8					14.8																																																																																																									MAT.RES.BULL.,9(1974)1085	B.T.MATTHIAS,J.M.VANDENBERG		
101705	1759		Mo6.35Pb1S8	Mo6.35Pb1S8	Mo	6.35	Pb	1	S	8																			1974																																														K		12.6					12.6																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101706	1309		Mo6Pb0.92S7.5	Mo6Pb0.92S7.5	Mo	6	Pb	0.92	S	7.5																			1973																																													rhombohedral	K		15.2					15.2																																																																																																									MAT.RES.BULL.,8(1973)657	B.T.MATTHIAS,E.CORENZWIT,J.P.REMEIKA,M.MAREZIO,P.D.DERNIER		
101707	1725		Mo5Pb1S7	Mo5Pb1S7	Mo	5	Pb	1	S	7																			1974																																														K		12.5					12.5																																																																																																									ZH.ETF PIS.RED,20(1974)59	N.E.ALEKSEEVSKII,N.M.DOVROVOL'SKII,V.I.TSEBRO		
101708	1597		Mo5.1Pb1S6	Mo5.1Pb1S6	Mo	5.1	Pb	1	S	6																			1974																																														K		14.4					14.4																																																																																																									PHYS.LETT.A,49(1974)269	E.J.ALEXANDER,E.J.MCNIFF JR.,S.FONER		
101709	1597		Mo5.1Pb0.9S6	Mo5.1Pb0.9S6	Mo	5.1	Pb	0.9	S	6																			1974																																														K		13.2					13.2																																																																																																									PHYS.LETT.A,49(1974)269	E.J.ALEXANDER,E.J.MCNIFF JR.,S.FONER		
101710	1936		Mo0.15Pa0.85	Mo0.15Pa0.85	Mo	0.15	Pa	0.85																					1974																																														K		3.08					3.08																																																																																																					FROM Roberts' Table.				LT-13(1974)vol.3 p=377	R.D.Fowler,L.B.Asprey,J.D.G.Lindsay,R.W.White		
101711	1995		Mo4P3	Mo4P3	Mo	4	P	3																																																																		orthorhombic	K		2.5					2.5																																																																																																					FROM Roberts' Table.				unpublished	Z.Fisk		
101712	601		Mo3P1	Mo3P1	Mo	3	P	1																					1965																												Ni3P																	Ni3P, D0[e]	K		5.31					5.31																																																																																																					Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
101713	1692		Mo3Os1	Mo3Os1	Mo	3	Os	1																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101714	276		Mo0.62Os0.38	Mo0.62Os0.38	Mo	0.62	Os	0.38																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		5.65					5.65																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101715	182		Mo1Os2	Mo1Os2	Mo	1	Os	2																					1961																																														K		5.2					5.2																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
101716	1438		Mo0.2Nb0.2Re0.6	Mo0.2Nb0.2Re0.6	Mo	0.2	Nb	0.2	Re	0.6																			1974																																														K		7.6					7.6																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101717	1692		Mo0.55Pt0.05Re0.425	Mo0.55Pt0.05Re0.425	Mo	0.55	Pt	0.05	Re	0.425																			1974																																														K		11.25					11.25																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101718	1692		Mo0.5Pt0.05Re0.45	Mo0.5Pt0.05Re0.45	Mo	0.5	Pt	0.05	Re	0.45																			1974																												sigma-CrFe																	sigma-CrFe, D8[b]	K		5.32					5.32																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101719	845		Mo0.72Pt0.28	Mo0.72Pt0.28	Mo	0.72	Pt	0.28																					1968																																														K		5.6					5.6																																																																																																									J.LESS-COMMON METALS,15(1968)193	H.OCKEN,J.H.N.VAN VUCHT		
101720	707		Mo0.8Pt0.2	Mo0.8Pt0.2	Mo	0.8	Pt	0.2																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		4.56					4.56																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101721	1692		Mo0.815Pt0.185	Mo0.815Pt0.185	Mo	0.815	Pt	0.185																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		4.62					4.62																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101722	707		Mo0.815Pt0.15	Mo0.85Pt0.15	Mo	0.85	Pt	0.15																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		8.8					8.8																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101723	1420		Mo0.93Pt0.17	Mo0.93Pt0.17	Mo	0.93	Pt	0.17																					1972																												W																	W, A2	K		2.8					2.8																																																																																																									SOLID STATE COMMUN.,11(1972)61	A.PAOLI,J.MULLER,K.YVON,R.FLUKIGER,R.ROGGEN		
101724	RMP0350001		Mo0.5Pd0.5	Mo0.5Pd0.5	Mo	0.5	Pd	0.5																					1963																																													hexagonal	K		3.52					3.52																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101725	1759		Mo6.35Pb0.7S8Sn0.36	Mo6.35Pb0.7S8Sn0.36	Mo	6.35	Pb	0.7	S	8	Sn	0.36																	1974																																														K		10					10																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101726	1759		Mo6.35Pb0.9S8Sn0.12	Mo6.35Pb0.9S8Sn0.12	Mo	6.35	Pb	0.9	S	8	Sn	0.12																	1974																																														K		11					11																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101727	1759		Mo6.3Pb1S6Se2	Mo6.3Pb1S6Se2	Mo	6.3	Pb	1	S	6	Se	2																	1974																																														K		5.4					5.4																																																																																																									J.PHYS.C:SOLID STATE PHYS.,7(1974)1450	G.BONGI,H.JONES,M.SERGENT,O.FISCHER,R.CHEVREL		
101728	1831		Mo6Pb1S7	Mo6Pb1S7	Mo	6	Pb	1	S	7																			1974																																														K		14					14																																																																																																									J.LESS-COMMON METALS,34(1974)125	C.F.WOODHEAD,J.G.BOOTH,N.MORTON		
101729	557		Mo0.42Re0.58	Mo0.42Re0.58	Mo	0.42	Re	0.58																					1964																																														K		8.4					8.4																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101730	327	Hc(T) parabolic T dependence.	Mo3Re1	Mo3Re1	Mo	3	Re	1																				3	1962																																														K		9.8					9.8																				Oe		530							Oe/K		114																																																																						SUPERCONDUCTING CRITICAL FIELD OF SINGLE-CRYSTAL MO2RE				PHYS.REV.,125(1962)474	J.K.HULM,R.D.BLAUGHER		
101731	1692		Mo0.5Re0.5	Mo0.5Re0.5	Mo	0.5	Re	0.5																					1974																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6.5					6.5																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101732	276		Mo0.5Re0.5	Mo0.5Re0.5	Mo	0.5	Re	0.5																					1961																																														K		11.6					11.6																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101733	555		Mo0.52Re0.48	Mo0.52Re0.48	Mo	0.52	Re	0.48																					1966																																														K		11.1					11.1																																																																																																					THERMAL AND ELECTRICAL CONDUCTIVITIES OF MO-RE ALLOYS IN THE SUPERCONDUCTING AND NORMAL STATE				PHYS.REV.,142(1966)251	E.LERNER,J.G.DAUNT		
101734	592		Mo0.57Re0.43	Mo0.57Re0.43	Mo	0.57	Re	0.43																					1965																																														K		14					14																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101735	555		Mo0.6Re0.4	Mo0.6Re0.4	Mo	0.6	Re	0.4																					1966																																														K		10.6					10.6																																																																																																					THERMAL AND ELECTRICAL CONDUCTIVITIES OF MO-RE ALLOYS IN THE SUPERCONDUCTING AND NORMAL STATE				PHYS.REV.,142(1966)251	E.LERNER,J.G.DAUNT		
101736	1331		Mo0.66Re0.34	Mo0.66Re0.34	Mo	0.66	Re	0.34																					1968																																														K		11.8					11.8																																																																																																									PHIL.MAG.,18(1968)1089	A.ECHARRI,A.V.NARLIKAR.,D.DEW-HUGHES,M.J.WITCOMB		
101737	881		Mo0.815Re0.185	Mo0.815Re0.185	Mo	0.815	Re	0.185																					1969																																														K		8.27					8.27																																																																																																									J.LOW TEMP.PHYS.,1(1969)355	H.E.HOENING,N.BARTH		
101738	881		Mo0.865Re0.135	Mo0.865Re0.135	Mo	0.865	Re	0.135																					1969																																														K		6.1					6.1																																																																																																									J.LOW TEMP.PHYS.,1(1969)355	H.E.HOENING,N.BARTH		
101739	1696		Mo0.9Re0.1	Mo0.9Re0.1	Mo	0.9	Re	0.1																					1966																																														K		2.97					2.97																																																																																																									ZH.EKSP.TEOR.FIZ.,51(1966)59	N.B.BRANDT,N.I.GINZBURG		
101740	1920		Mo1Rb0.3S2	Mo1Rb0.3S2	Mo	1	Rb	0.3	S	2																			1973																												2H-MoS2			A	3.2039		17.1937											hexagonal	K		6.25					6.25																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
101741	182		Mo0.39Ru0.61	Mo0.39Ru0.61	Mo	0.39	Ru	0.61																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6.9					6.9																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
101742	33		Mo1Ru1	Mo1Ru1	Mo	1	Ru	1																					1955																																													hexagonal	K		10.5					10.5																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
101743	276		Mo0.6Ru0.4	Mo0.6Ru0.4	Mo	0.6	Ru	0.4																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		7					7																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101744	1033		Mo0.6Ru0.4	Mo0.6Ru0.4	Mo	0.6	Ru	0.4																					1964																																													hexagonal	K		8.7					8.7																																																																																																					Metastable phases and superconductors produced by plasma-jet spraying				Appl.Phys.Lett.,5(1964)120	M.Moss,D.L.Smith,R.A.Lefever		
101745	557		Mo0.61Ru0.39	Mo0.61Ru0.39	Mo	0.61	Ru	0.39																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K		7.18					7.18																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101746	1060		Mo0.05Rh0.04Ti0.91	Mo0.05Rh0.04Ti0.91	Mo	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.3					3.3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101747	1438		Mo0.75Rh0.25	Mo0.75Rh0.25	Mo	0.75	Rh	0.25																					1974																																														K		6.6					6.6																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101748	33		Mo1Rh1	Mo1Rh1	Mo	1	Rh	1																					1955																																													hexagonal	K		1.97					1.97																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
101749	1384		Mo0.7Re0.3	Mo0.7Re0.3	Mo	0.7	Re	0.3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		15					15																																																																																																									APPL.PHYS.LETT.,21(1972)179	C.K.JONES,J.R.GAVALER,M.A.JANOCKO		
101750	557		Mo0.23Re0.77	Mo0.23Re0.77	Mo	0.23	Re	0.77																					1964																												alpha-Mn																	alpha-Mn, A12	K		9.25					9.25																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101751	266		Mo0.28Re0.72	Mo0.28Re0.72	Mo	0.28	Re	0.72																					1962																																														K		6.5					6.5																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
101752	182		Mo1Re3	Mo1Re3	Mo	1	Re	3																					1961																												alpha-Mn																	alpha-Mn, A12	K		9.89					9.89																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
101753	1584		Mo3Se4	Mo3Se4	Mo	3	Se	4																					1968																																													monoclinic	K		5.8					5.8																																																																																																									STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
101754	1309		Mo3Se4	Mo3Se4	Mo	3	Se	4																					1973																																													rhombohedral	K		6.3					6.3																																																																																																									MAT.RES.BULL.,8(1973)657	B.T.MATTHIAS,E.CORENZWIT,J.P.REMEIKA,M.MAREZIO,P.D.DERNIER		
101755	117		Mo3Sb4	Mo3Sb4	Mo	3	Sb	4																					1957																																														K		2.1					2.1																																																																																																									PROG.IN LOW TEMP.PHY.,11(1957)138	B.T.MATTHIAS		
101756	1583		Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																					1968																																														K		2.31					2.31																																																																																																									STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
101757	1163		Mo5S6Zn1	Mo5S6Zn1	Mo	5	S	6	Zn	1																			1972																																													rhombohedral	K		3					3																																																																																																									SCI.,175(1972)1465	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO		
101758	1728		Mo1S2Sr0.2	Mo1S2Sr0.2	Mo	1	S	2	Sr	0.2																			1974																																														K		5.6					5.6																																																																																																									ZH.ETF PIS.RED.,19(1974)742	A.A.GUSEINOV,L.N.BULAEVSKII		
101759	614		Mo3S4Sn0.6	Mo3S4Sn0.6	Mo	3	S	4	Sn	0.6																			1975																																														K		14.2					14.2																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
101760	1163		M05S6Sn1	Mo5S6Sn1	Mo	5	S	6	Sn	1																			1972																																													rhombohedral	K		13.4					13.4																																																																																																									SCI.,175(1972)1465	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO		
101761	1831		Mo6S7Sn1	Mo6S7Sn1	Mo	6	S	7	Sn	1																			1974																																														K		13					13																																																																																																									J.LESS-COMMON METALS,34(1974)125	C.F.WOODHEAD,J.G.BOOTH,N.MORTON		
101762	1309		Mo3S2Se2	Mo3S2Se2	Mo	3	S	2	Se	2																			1973																																													rhombohedral	K		3.3					3.3																																																																																																									MAT.RES.BULL.,8(1973)657	B.T.MATTHIAS,E.CORENZWIT,J.P.REMEIKA,M.MAREZIO,P.D.DERNIER		
101763	1309		Mo3S1Se3	Mo3S1Se3	Mo	3	S	1	Se	3																			1973																																													rhombohedral	K		3.4					3.4																																																																																																									MAT.RES.BULL.,8(1973)657	B.T.MATTHIAS,E.CORENZWIT,J.P.REMEIKA,M.MAREZIO,P.D.DERNIER		
101764	224		Mo0.25Ru0.975	Mo0.25Ru0.75	Mo	0.25	Ru	0.75																					1962																																													hexagonal	K		2.6					2.6	MTC1764																																																																																																				SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
101765	600		Mo0.91Ti0.09	Mo0.91Ti0.09	Mo	0.91	Ti	0.09																					1965																																														K		2.95					2.95																																																																																																									PHYS.LETT.,14(1965)181	R.D.BLAUGHER		
101766	1584		Mo1Te2	Mo1Te2	Mo	1	Te	2																					1968																																														K		0.3					0.3																																																																																																									STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
101767	202		Mo0.05Tc0.95	Mo0.05Tc0.95	Mo	0.05	Tc	0.95																					1961																																														K		10.8					10.8																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101768	202		Mo0.1Tc0.9	Mo0.1Tc0.9	Mo	0.1	Tc	0.9																					1961																																														K		13.4					13.4																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101769	202		Mo0.25Tc0.75	Mo0.25Tc0.75	Mo	0.25	Tc	0.75																					1961																																														K		15.8					15.8																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101770	202		Mo0.3Tc0.7	Mo0.3Tc0.7	Mo	0.3	Tc	0.7																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		12					12																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101771	1656		Mo0.4Tc0.6	Mo0.4Tc0.6	Mo	0.4	Tc	0.6																					1972																																														K		14.7					14.7																																																																																																									PHYS.LETT.A,41(1972)307	C.C.KOCH,J.A.C.MARPLES		
101772	202		Mo0.45Tc0.55	Mo0.45Tc0.55	Mo	0.45	Tc	0.55																					1961																																														K		14					14																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101773	202		Mo0.5Tc0.5	Mo0.5Tc0.5	Mo	0.5	Tc	0.5																					1961																																														K		14					14																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
101774	42		Mo0.59Si0.41	Mo0.59Si0.41	Mo	0.59	Si	0.41																					1953																																														K		1.34					1.34																																																																																																					Superconducting silicides and Germanides				Phys.Rev., 89(1953)884	G.F.Hardy,J.K.Hulm		
101775	1692		Mo0.77Si0.23	Mo0.77Si0.23	Mo	0.77	Si	0.23																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		1.7					1.7																																																																																																					Electronically 'atypical' a 15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	R.Flukiger,A.Paoli,J.Muller		
101776	10		Mo3Si1	Mo3Si1	Mo	3	Si	1																					1954																												Cr3Si(A15)																	Cr3Si, A15	K		1.402					1.402																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
101777	1988		Mo2Zr1	Mo2Zr1	Mo	2	Zr	1																					1966																												MgCu2(Laves)																	MgCu2, C15	K		0.125			0.025		0.125																																																																																																									PROC.10TH INTER.CONF.ON LOW TEMP.PHYS.,2(1966)86	C.K.JONES,J.K.HULM,R.C.MILLER,T.Y.TIEN		
101778	788		Mo0.15V0.85	Mo0.15V0.85	Mo	0.15	V	0.85																					1969																																														K		2.28					2.28																																																																																																									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
101779	788		Mo0.3V0.7	Mo0.3V0.7	Mo	0.3	V	0.7																					1969																																														K		0.76					0.76																																																																																																									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
101780	788		Mo0.5V0.5	Mo0.5V0.5	Mo	0.5	V	0.5																					1969																																														K		0.11					0.11																																																																																																									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
101781	879		Mo0.006U0.944	Mo0.006U0.944	Mo	0.006	U	0.944																					1968																																														K		1.2					1.2																																																																																																									PHYS.REV.,176(1968)556	C.W.CHU,J.E.GORDON,M.B.MAPLE,T.F.SMITH,W.E.GARDNER		
101782	349		Mo0.12U0.88	Mo0.12U0.88	Mo	0.12	U	0.88																					1959																												W																	W, A2	K		1.85					1.85																																																																																																									J.PHYS.CHEM.SOLIDS,11(1959)12	T.G.BERLINCOURT		
101783	177		Mo0.14U0.86	Mo0.14U0.86	Mo	0.14	U	0.86																					1961																																														K		2.02					2.02																																																																																																					FROM Roberts' Table.				LT-7 (Univ.Toronto,1961)350	B.B.Goodman,J.Hillairet,J.J.Veyssie,L.Weil		
101784	177		Mo0.18U0.82	Mo0.18U0.82	Mo	0.18	U	0.82																					1961																												W																	W, A2	K		2.113					2.113																																																																																																					FROM Roberts' Table.				LT-7 (Univ.Toronto,1961)350	B.B.Goodman,J.Hillairet,J.J.Veyssie,L.Weil		
101785	349		Mo0.22U0.78	Mo0.22U0.78	Mo	0.22	U	0.78																					1959																												W																	W, A2	K		2.06					2.06																																																																																																									J.PHYS.CHEM.SOLIDS,11(1959)12	T.G.BERLINCOURT		
101786	177		Mo0.3U0.7	Mo0.3U0.7	Mo	0.3	U	0.7																					1961																												W																	W, A2	K		1.97					1.97																																																																																																					FROM Roberts' Table.				LT-7 (Univ.Toronto,1961)350	B.B.Goodman,J.Hillairet,J.J.Veyssie,L.Weil		
101787	274		Mo0.1Ti0.9	Mo0.1Ti0.9	Mo	0.1	Ti	0.9																					1961																												Mg																	Mg, A3	K		3.25					3.25																																																																																																									HELV.PHYS.ACTA,34(1961)410	E.BUCHER,J.MULLER		
101788	805		Mo0.16Ti0.84	Mo0.16Ti0.84	Mo	0.16	Ti	0.84																					1966																																														K		4.246					4.246																																																																																																									ANN.ACAD.SCI.FINNICAE A VI,210(1966)78	L.J.BARNES,R.R.HAKE		
101789	1461		N1Nb1	N1Nb1	N	1	Nb	1																					1971																																														K		15.2					15.2																																																																																																									J.APPL.PHYS.,42(1971)54	A.PATTERSON,C.K.JONES,J.R.GAVALER,M.A.JANOCKO		
101790	1406		N1Nb1	N1Nb1	N	1	Nb	1																					1969																																														K		15.23					15.23																																																																																																									J.APPL.PHYS.,40(1969)2153	C.K.JONES,D.W.DEIS,J.K.HULM,J.R.GAVALER		
101791	582		N1Nb1	N1Nb1	N	1	Nb	1																					1965																																														K		14.5					14.5																																																																																																					SUPERCONDUCTIVITY OF NBC/NBN WHISKERS				PHYS.REV.,140(1965)A1581	F.J.DARNELL,JR.,P.E.BIERSTEDT,R.K.WARING,W.O.FORSHEY		
101792	248		N0.003Nb0.997	N0.003Nb0.997	N	0.003	Nb	0.997																																																																			K		9.12					9.12																																																																																																					FROM Roberts' Table.				unpublished	W.DeSorbo,G.E.Nichols		
101793	1527		N1Nb2	N1Nb2	N	1	Nb	2																					1969																																													hexagonal	K		8.6					8.6																																																																																																									J.VAC.SCI.TECH.,6(1969)177	J.K.HULM,J.R.GAVALER,M.A.JANOCKOC.K.JONES		
101794	96		N0.48Nb1	N0.48Nb1	N	0.48	Nb	1																					1956																																													hexagonal	K		5.5					5.5																																																																																																					FROM Roberts' Table.				Z.Naturforsch., 11a(1956)517	G.Lautz,E.Z.Schroder		
101795	96		N0.8Nb1	N0.8Nb1	N	0.8	Nb	1																					1956																																													tetragonal	K		8.9					8.9																																																																																																					FROM Roberts' Table.				Z.Naturforsch., 11a(1956)517	G.Lautz,E.Z.Schroder		
101796	1510		N0.84Nb1	N0.84Nb1	N	0.84	Nb	1																					1966																												NaCl																	NaCl, B1	K		13.5					13.5																																																																																																									PHYS.,2(1966)293	B.T.MATTHIAS,H.J.WILLIAMS,J.P.MAITA,J.P.REMEIKAA.M.CLOGSTON,T.H.GEBALLE,V.B.COMPTON		
101797	1070		N0.92Nb1	N0.92Nb1	N	0.92	Nb	1																					1968																												NaCl																	NaCl, B1	K		16.5					16.5																																																																																																									Z.PHYS.,210(1968)70	E.SAUR,G.HORN		
101798	96		N1Nb1	N1Nb1	N	1	Nb	1																					1956																												TiAs																	TiAs, B[i]	K		5.1			1.94		5.1																																																																																																					FROM Roberts' Table.				Z.Naturforsch., 11a(1956)517	G.Lautz,E.Z.Schroder		
101799	1473		N1Nb1	N1Nb1	N	1	Nb	1																					1972																												NaCl																	NaCl, B1	K		16					16																																																																																																									J.APPL.PHYS.,43(1972)3158	D.W.DEIS,J.R.GAVALER,M.D.MATHUR		
101800	956		Mo2Zr1	Mo2Zr1	Mo	2	Zr	1																					1970																																														K		4.75					4.75																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
101801	694		N0.84Ti1	N0.84Ti1	N	0.84	Ti	1																					1966																																														K					1.17																																																																																																											ACTA MET.,14(1966)1403	C.M.YEN,C.P.WANG,L.E.TOTH		
101802	694		N0.99Ti1	N0.99Ti1	N	0.99	Ti	1																					1966																												NaCl																	NaCl, B1	K		4.35					4.35																																																																																																									ACTA MET.,14(1966)1403	C.M.YEN,C.P.WANG,L.E.TOTH		
101803	1542		N1Ti1	N1Ti1	N	1	Ti	1																					1971																												NaCl																	NaCl, B1	K		5.49					5.49																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
101804	1971		N1Th1	N1Th1	N	1	Th	1																					1972																												NaCl																	NaCl, B1	K		3.3					3.3																																																																																																					"""Superconductivity in d- and f-band metals, ed. D.H.Douglas"" 1972"				Sup. in d- & f-band metals, p=147	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
101805	1986	polymer polysulfur nitride	N1S1	N1S1	N	1	S	1																					1975																																														K		0.26					0.26																																																																																																									PHYS.REV.LETT.,34(1975)577	G.B.STREET,L.J.SUTER,R.L.GREENE		
101806	1511		N1Nb0.9V0.1	N1Nb0.9V0.1	N	1	Nb	0.9	V	0.1																			1966																																														K		6.6					6.6																																																																																																									PHYS.,2(1966)311	J.K.HULM,N.PESSALL		
101807	880		N0.85Nb0.66Ti0.34	N0.85Nb0.66Ti0.34	N	0.85	Nb	0.66	Ti	0.34																			1969																																														K		17.61					17.61																																																																																																									J.LOW TEMP.PHYS.,1(1969)29	E.SAUR,G.HORN,G.OTTO,K.HECHLER		
101808	880		N0.88Nb0.256Ti0.744	N0.88Nb0.256Ti0.744	N	0.88	Nb	0.256	Ti	0.744																			1969																												NaCl																	NaCl, B1	K		14.72					14.72																																																																																																									J.LOW TEMP.PHYS.,1(1969)29	E.SAUR,G.HORN,G.OTTO,K.HECHLER		
101809	880		N0.9Nb0.114Ti0.886	N0.9Nb0.114Ti0.886	N	0.9	Nb	0.114	Ti	0.886																			1969																												NaCl																	NaCl, B1	K		10.1					10.1																																																																																																									J.LOW TEMP.PHYS.,1(1969)29	E.SAUR,G.HORN,G.OTTO,K.HECHLER		
101810	1234		N0.988Nb1O0.002	N0.998Nb1O0.002	N	0.998	Nb	1	O	0.002																			1967																																														K		17.3					17.3																																																																																																									J.PHYS.CHEM.SOLIDS,28(1967)333	K.M.RALLS,M.R.PICKUS,M.W.WILLAMS		
101811	1439		N5Nb4	N5Nb4	N	5	Nb	4																					1974																																													tetragonal	K		8.5					8.5																																																																																																									J.APPL.PHYS.,45(1974)1389	G.OYA,Y.ONODERA		
101812	1175		N1Nb1	N1Nb1	N	1	Nb	1																					1971																																														K		17.3					17.3																																																																																																					FROM Roberts' Table.				LT-12( 1971)329	Y.Saito,T.Anayama,Y.Onodera,T.Yamashita,K.Konenou,Y.Muto		
101813	1995		Nb3P1	Nb3P1	Nb	3	P	1																																																																		tetragonal	K		2					2																																																																																																					FROM Roberts' Table.				unpublished	Z.Fisk		
101814	173		Nb0.6Os0.4	Nb0.6Os0.4	Nb	0.6	Os	0.4																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.85					1.85																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101815	276		Nb0.5Os0.5	Nb0.5Os0.5	Nb	0.5	Os	0.5																					1961																												alpha-Mn																	alpha-Mn, A12	K		2.86					2.86																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101816	173		NbOs2	Nb1Os2	Nb	1	Os	2																					1961																												alpha-Mn																	alpha-Mn, A12	K		2.52					2.52																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101817	707		Nb3Os1	Nb3Os1	Nb	3	Os	1																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		1.05					1.05																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101818	1993		Nb1O1	Nb1O1	Nb	1	O	1																					1974																												NaCl																	NaCl, B1	K		1.5					1.5																																																																																																					FROM Roberts' Table.				LT-13( )648	E.Bucher,E.Ehrenfreund,A.C.Gossard,K.Andres,J.H.Wernick,J.P.Maita,A.S.Cooper,L.D.Longinotti		
101819	1491	quench condensation	Na0.1Pb0.9	Na0.1Pb0.9	Na	0.1	Pb	0.9																					1973																																														K		5.93					5.93																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
101820	715		Na1Pb3	Na1Pb3	Na	1	Pb	3																					1970																												AuCu3																	AuCu3, L1[2]	K		5.62					5.62																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
101821	500	tetragonal phase	Na0.2O3W1	Na0.2O3W1	Na	0.2	O	3	W	1																			1965																															A	12.1		3.7											tetragonal	K		0.55					0.55																																																																																																					Superconductivity of the alkali tungsten bronzes				PHYS.LETT.,15(1965)108	A.R.SWEEDLER,B.T.MATTHIAS,CH.J.RAUB		
101822	278		N1Zr1	N1Zr1	N	1	Zr	1																					1962																												NaCl																	NaCl, B1	K		10.7					10.7																																																																																																									BULL.AMER.PHYS.SOC.,7(1962)176	A.L.GIORGI,E.G.SZKLARZ		
101823	1592		N0.75V1	N0.75V1	N	0.75	V	1																					1975																												NaCl																	NaCl, B1	K		2.3					2.3																																																																																																									J.PHYS.CHEM.SOLIDS,36(1975)7	F.I.AJAMI,R.K.MACCRONE		
101824	1542		N1V1	N1V1	N	1	V	1																					1971																												NaCl																	NaCl, B1	K		8.5					8.5																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
101825	276		Nb0.5Re0.5	Nb0.5Re0.5	Nb	0.5	Re	0.5																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		3.8					3.8																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101826	592		Nb0.9Re0.1	Nb0.9Re0.1	Nb	0.9	Re	0.1																					1965																																														K		4.5					4.5																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101827	592		Nb0.9Re0.1	Nb0.9Re0.1	Nb	0.9	Re	0.1																					1965																																														K		4.5					4.5																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101828	557		N0.62Pt0.38	N0.62Pt0.38	N	0.62	Pt	0.38																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.21					4.21																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101829	592		Nb0.9Pt.1	Nb0.9Pt0.1	Nb	0.9	Pt	0.1																					1965																																														K		2.5					2.5																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101830	1446		Nb3Pt1	Nb3Pt1	Nb	3	Pt	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		10.9					10.9																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101831	557		Nb0.6Pd0.4	Nb0.6Pd0.4	Nb	0.6	Pd	0.4																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.6					1.6																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101832	276		Nb0.6Pd0.4	Nb0.6Pd0.4	Nb	0.6	Pd	0.4																					1961																												alpha-Mn																	alpha-Mn, A12	K		2.47					2.47																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101833	592		Nb0.9Pd0.1	Nb0.9Pd0.1	Nb	0.9	Pd	0.1																					1965																																														K		3.5					3.5																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101834	1982		Nb3Pb0.15Sn0.85	Nb3Pb0.15Sn0.85	Nb	3	Pb	0.15	Sn	0.85																			1964																																														K		18.16					18.16																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101835	795		Nb0.67Pb1S3Ta0.33	Nb0.67Pb1S3Ta0.33	Nb	0.67	Pb	1	S	3	Ta	0.33																	1970																																													tetragonal	K		2.01					2.01																																																																																																									SOLID STATE COMMUN.,8(1970)1513	J.P.MAITA,L.SCHMIDT,S.L.MCCARTHY		
101836	778		Nb1Pb1S3	Nb1Pb1S3	Nb	1	Pb	1	S	3																			1970																																													tetragonal	K		2.66					2.66																																																																																																									PHYS.LETT.A,31(1970)551	L.SCHMIDT		
101837	1299		Nb0.45Rh0.55	Nb0.45Rh0.55	Nb	0.45	Rh	0.55																					1966																																													orthorhombic	K		3.07					3.07																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101838	1299		Nb0.48Rh0.52	Nb0.48Rh0.52	Nb	0.48	Rh	0.52																					1966																												AuCu																	AuCu, L1[0]	K		3.76					3.76																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101839	557		Nb0.6Rh0.4	Nb0.6Rh0.4	Nb	0.6	Rh	0.4																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.21					4.21																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101840	1446		Nb3Rh1	Nb3Rh1	Nb	3	Rh	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.79					2.79																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
101841	1299		Nb0.85Rh0.15	Nb0.85Rh0.15	Nb	0.85	Rh	0.15																					1966																												AuCd																	AuCd, B19	K		3					3																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101842	592		Nb0.9Rh0.1	Nb0.9Rh0.1	Nb	0.9	Rh	0.1																					1965																																														K		2.8					2.8																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101843	1990		Nb0.11Re0.78Ta0.11	Nb0.11Re0.78Ta0.11	Nb	0.11	Re	0.78	Ta	0.11																			1973																												alpha-Mn																	alpha-Mn, A12	K		8.8					8.8																																																																																																									IZV.AKAD.NAUK SSSR METAL,4(1973)225	E,M.A.TYLKINA,M.SAVITSKIY,V.E.ALYUSHIN		
101844	1990		Nb0.05Re0.75Ta0.2	Nb0.05Re0.75Ta0.2	Nb	0.05	Re	0.75	Ta	0.2																			1973																												alpha-Mn																	alpha-Mn, A12	K		9.8					9.8																																																																																																									IZV.AKAD.NAUK SSSR METAL,4(1973)225	E,M.A.TYLKINA,M.SAVITSKIY,V.E.ALYUSHIN		
101845	557		Nb0.29Re0.71	Nb0.29Re0.71	Nb	0.29	Re	0.71																					1964																												alpha-Mn																	alpha-Mn, A12	K		5.6					5.6																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101846	557		Nb0.38Re0.62	Nb0.38Re0.62	Nb	0.38	Re	0.62																					1964																												alpha-Mn																	alpha-Mn, A12	K		2.45					2.45																																																																																																									PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
101847	276		Nb0.4Re0.6	Nb0.4Re0.6	Nb	0.4	Re	0.6																					1961																												alpha-Mn																	alpha-Mn, A12	K		2.36					2.36																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101848	2.76		Nb0.4Re0.6	Nb0.4Re0.6	Nb	0.4	Re	0.6																																																	sigma-CrFe																	sigma-CrFe, D8[b]	K		2.5					2.5																																																																																																												
101849	1150		Nb1S3Sn1	Nb1S3Sn1	Nb	1	S	3	Sn	1																			1972																																													tetragonal	K		2.85					2.85																																																																																																									PHYS.LETT.A,40(1972)353	M.H.VAN MAAREN		
101850	675		Nb1S2	Nb1S2	Nb	1	S	2																					1966																																													hexagonal	K		5.5					5.5																																																																																																									PHYS.LETT.,20(1966)131	G.M.SCHAEFFER,M.H.VAN MAAREN		
101851	1853		Nb1S2	Nb1S2	Nb	1	S	2																					1974																																													hexagonal	K		6.2					6.2																																																																																																									PHIL.MAG.,30(1974)1091	A.J.GRANT,D.JEROME,P.MOLINIE		
101852	667		Nb1Ru3	Nb1Ru3	Nb	1	Ru	3																					1974																																													hexagonal	K		12					12																																																																																																									ZH.ETF PIS.RED.,20(1974)648	L.N.FOMICHEVA,N.I.PALNIKOV,S.V.POPOVA		
101853	276		Nb0.4Ru0.6	Nb0.4Ru0.6	Nb	0.4	Ru	0.6																					1961																																														K		2.5					2.5																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
101854	417		Nb0.6Ru0.4	Nb0.6Ru0.4	Nb	0.6	Ru	0.4																					1963																																													tetragonal	K		1.2					1.2																																																																																																									PHYS.KONDENS.MATERIE,1(1963)225	D.BENDER,E.BUCHER,J.MULLER		
101855	417		Nb0.8Ru0.2	Nb0.8Ru0.2	Nb	0.8	Ru	0.2																					1963																												W																	W, A2	K		4.8			1		4.8																																																																																																									PHYS.KONDENS.MATERIE,1(1963)225	D.BENDER,E.BUCHER,J.MULLER		
101856	417		Nb0.9Ru0.1	Nb0.9Ru0.1	Nb	0.9	Ru	0.1																					1963																												W																	W, A2	K		2.8					2.8																																																																																																									PHYS.KONDENS.MATERIE,1(1963)225	D.BENDER,E.BUCHER,J.MULLER		
101857	293		Nb0.925Ru0.075	Nb0.925Ru0.075	Nb	0.925	Ru	0.075																					1962																																														K		4.2					4.2																																																																																																					FROM Roberts' Table.				LT-8(1962, London ) paper 4.7	E.Bucher,J.Muheim,J.Muller		
101858	1060		Nb0.05Rh0.04Ti0.91	Nb0.05Rh0.04Ti0.91	Nb	0.05	Rh	0.04	Ti	0.91																			1964																																														K		2.4					2.4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101859	1438		Nb0.45Re0.55	Nb0.45Re0.55	Nb	0.45	Re	0.55																					1974																																														K		6.2					6.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101860	1299		Nb0.375Rh0.625	Nb0.375Rh0.625	Nb	0.375	Rh	0.625																					1966																																													monoclinic	K		2.7					2.7																																																																																																									PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
101861	409		Nb3Si1	Nb3Si1	Nb	3	Si	1																					1963																												AuCu3																	AuCu3, L1[2]	K		1.5					1.5																																																																																																									ACTA CRYST.,16(1963)228	F.GALASSO,J.PYLE		
101862	1150		Nb1Se3Sn1	Nb1Se3Sn1	Nb	1	Se	3	Sn	1																			1972																																													tetragonal	K		3.09					3.09																																																																																																									PHYS.LETT.A,40(1972)353	M.H.VAN MAAREN		
101863	1809		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1974																												2H-NbSe2																		K		7					7																																																																																																									CAN.J.PHYS.,52(1974)861	D.J.HUNTLEY,R.F.FRINDT		
101864	1505		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1973																												2H-NbSe2																		K		7.38					7.38																																																																																																									J.LOW TEMP.PHYS.,11(1973)421	J.P.JAN,P.DETREY,S.GYGAX		
101865	1695		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1974																												2H-NbSe2																	hexagonal	K		6.95					6.95																																																																																																									SOLID STATE COMMUN.,14(1974)1259	G.N.SCHRAUZER,H.PRAKASH		
101866	1500		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1973																												2H-NbSe2																	hexagonal	K		7.3					7.3																																																																																																									PHYS.LETT.A,45(1973)99	A.HOSHI,K.NOTO,N.TOYOTA,Y.MUTO		
101867	1582		Nb3Se4	Nb3Se4	Nb	3	Se	4																					1968																																														K		1.61					1.61																																																																																																									STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
101868	1002		Nb0.25Sb0.25Ti0.5	Nb0.25Sb0.25Ti0.5	Nb	0.25	Sb	0.25	Ti	0.5																			1970																												Cr3Si(A15)																	Cr3Si, A15	K		2.05					2.05																																																																																																					Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
101869	1002		Nb0.5Sb0.25Ti0.25	Nb0.5Sb0.25Ti0.25	Nb	0.5	Sb	0.25	Ti	0.25																			1970																																														K		3.05					3.05																																																																																																					Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
101870	1982		Nb3Sb0.15Sn0.7Tl0.15	Nb3Sb0.15Sn0.7Tl0.15	Nb	3	Sb	0.15	Sn	0.7	Tl	0.15																	1964																																														K		16.04					16.04																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101871	1582		Nb5Sb4	Nb5Sb4	Nb	5	Sb	4																					1968																																														K		8.6					8.6																																																																																																									STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
101872	1002	e-ph coupling = 0.49 	Nb0.83Sb0.17	Nb0.83Sb0.17	Nb	0.83	Sb	0.17																					1970																												Cr3Si(A15)			A	5.265													Cr3Si, A15	K		1.95					1.95																																																								mj/mol.K2	2.95		345																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
101873	311		Nb0.84S0.16	Nb0.84S0.16	Nb	0.84	S	0.16																					1963																												Cr3Si(A15)																	Cr3Si, A15	K		5.6					5.6																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101874	RMP0350001		Nb0.92Sn0.08	Nb0.92Sn0.08	Nb	0.92	Sn	0.08																					1963																																													cubic	K		5.6					5.6																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101875	1742		Nb3Sn1	Nb3Sn1	Nb	3	Sn	1																					1967																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																									FIZ.METAL.METALLOVED.,24(1967)1050	K.V.KISELEVA,S.A.MEDVEDEV,V.A.LYKHIIN		
101876	185		Nb3Sn1	Nb3Sn1	Nb	3	Sn	1																					1960																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3																																																																																																					LT7 (Toronto), 1960 p382				REF.,176 382	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101877	149		Nb3Sn1	Nb3Sn1	Nb	3	Sn	1																					1958																												Cr3Si(A15)																	Cr3Si, A15	K		18.07					18.07																																																																																																									Z.PHYS.,151(1958)307	W.WIEDEMANN		
101878	1913		Nb0.03Si1V2.97	Nb0.03Si1V2.97	Nb	0.03	Si	1	V	2.97																			1965																												Cr3Si(A15)																	Cr3Si, A15	K		15.8					15.8																																																																																																									AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
101879	255		Nb3Si1Sn1V3	Nb3Si1Sn1V3	Nb	3	Si	1	Sn	1	V	3																																													Cr3Si(A15)																	Cr3Si, A15	K		4					4																																																																																																					FROM Roberts' Table.				unpublished	G.O.S.Arrhnius,M.F.Merriam		
101880	419		Nb3Si0.06Sn0.94	Nb3Si0.06Sn0.94	Nb	3	Si	0.06	Sn	0.94																			1963																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																									NATURE,198(1963)984	B.BAYLES,F.GLASSO,S.SOEHLE		
101881	419		Nb3Si0.25Sn0.75	Nb3Si0.25Sn0.75	Nb	3	Si	0.25	Sn	0.75																			1963																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																									NATURE,198(1963)984	B.BAYLES,F.GLASSO,S.SOEHLE		
101882	419		Nb3Si0.27Sn0.73	Nb3Si0.27Sn0.73	Nb	3	Si	0.27	Sn	0.73																			1963																												Cr3Si(A15)																	Cr3Si, A15	K		13.9					13.9																																																																																																									NATURE,198(1963)984	B.BAYLES,F.GLASSO,S.SOEHLE		
101883	419		Nb3Si0.5Sn0.5	Nb3Si0.5Sn0.5	Nb	3	Si	0.5	Sn	0.5																			1963																												Cr3Si(A15)																	Cr3Si, A15	K		8.3					8.3																																																																																																									NATURE,198(1963)984	B.BAYLES,F.GLASSO,S.SOEHLE		
101884	255		Nb3Si0.6Sn0.4	Nb3Si0.6Sn0.4	Nb	3	Si	0.6	Sn	0.4																																															Cr3Si(A15)																	Cr3Si, A15	K		6.5					6.5																																																																																																					FROM Roberts' Table.				unpublished	G.O.S.Arrhnius,M.F.Merriam		
101885	473		Nb0.69Sn0.25Ta0.06	Nb0.69Sn0.25Ta0.06	Nb	0.69	Sn	0.25	Ta	0.06																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101886	359		Nb3Sn1	Nb3Sn1	Nb	3	Sn	1																					1962																																														K		18					18																																																																																																									Z.PHYS,170(1962)154	C.MULLER,E.SAUR		
101887	1522		Nb1Sn2	Nb1Sn2	Nb	1	Sn	2																					1965																																													orthorhombic	K		2.68					2.68																																																																																																									PHILIPS RES.REPTS.,20(1965)136	D.J.VAN OOIJEN,H.A.C.BRUNING,J.H.N.VAN VUCHT		
101888	1591		Nb0.5Sn0.5	Nb0.5Sn0.5	Nb	0.5	Sn	0.5																					1972																																														K		17.5					17.5																																																																																																									FIZIKA GORENIYA I VZRYVA,8(1972)578	A.I.MATYTSIN,I.M.BARSKII,V.YA.DIKOVSKII		
101889	139		Nb0.5Sn0.5	Nb0.5Sn0.5	Nb	0.5	Sn	0.5																					1960																																														K		17.91					17.91																																																																																																					LT7 (Toronto) 1960, p379-382				REF.,176 379-382	E.J.SAUR,H.G.JANSEN		
101890	964		Nb6Sn5	Nb6Sn5	Nb	6	Sn	5																					1966																																													orthorhombic	K		2.07					2.07																																																																																																									PHYS.LETT.,21(1966)501	J.P.CHARLESWORTH		
101891	355		Nb3Sn2	Nb3Sn2	Nb	3	Sn	2																					1962																																													tetragonal	K		17.2					17.2																																																																																																									J.APPL.PHYS.,33(1962)2657	H.C.GATOS,T.B.REED		
101892	311		Nb0.72Sn0.28	Nb0.72Sn0.28	Nb	0.72	Sn	0.28																					1963																																														K		18.2					18.2																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101893	311		Nb0.76Sn0.74	Nb0.76Sn0.74	Nb	0.76	Sn	0.74																					1963																																														K		18.1					18.1																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101894	1591		Nb0.8Sn0.2	Nb0.8Sn0.2	Nb	0.8	Sn	0.2																					1972																																														K		17.3					17.3																																																																																																									FIZIKA GORENIYA I VZRYVA,8(1972)578	A.I.MATYTSIN,I.M.BARSKII,V.YA.DIKOVSKII		
101895	311		Nb0.8Sn0.2	Nb0.8Sn0.2	Nb	0.8	Sn	0.2																					1963																																														K		18.5					18.5																																																																																																									METALLURGY OF ADVANCED ELECTRONICS MATE,71(1963)	H.C.GATOS,J.T.ROBBY,T.B.REED,W.J.LAFLEUR		
101896	893		Nb0.8Sn0.2	Nb0.8Sn0.2	Nb	0.8	Sn	0.2																					1971																																														K		7.5					7.5																																																																																																									PHYS.STAT.SOL.A,4(1971)387	C.C.TSUEI,L.R.NEWKIRK		
101897	864		Nb0.991Ta0.009	Nb0.991Ta0.009	Nb	0.991	Ta	0.009																					1969																																														K		8.87					8.87																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)873	A.IKUSIMA,T.MIZUSAKI		
101898	427		Nb0.75Sn0.125Zr0.125	Nb0.75Sn0.125Zr0.125	Nb	0.75	Sn	0.125	Zr	0.125																			1962																												Cr3Si(A15)																	Cr3Si, A15	K		16.7					16.7																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
101899	185		Nb0.25Sn0.25V0.5	Nb0.25Sn0.25V0.5	Nb	0.25	Sn	0.25	V	0.5																			1960																												Cr3Si(A15)																	Cr3Si, A15	K		5.5					5.5																																																																																																					LT7 (Toronto), 1960 p382				REF.,176 382	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101900	255		Nb0.375Sn0.25V0.375	Nb0.375Sn0.25V0.375	Nb	0.375	Sn	0.25	V	0.375																																															Cr3Si(A15)																	Cr3Si, A15	K		7.4					7.4																																																																																																					FROM Roberts' Table.				unpublished	G.O.S.Arrhnius,M.F.Merriam		
101901	473		Nb0.55Sn0.25V0.25	Nb0.5Sn0.25V0.25	Nb	0.5	Sn	0.25	V	0.25																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		9.8					9.8																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101902	473		Nb0.625Sn0.25V0.125	Nb0.625Sn0.25V0.125	Nb	0.625	Sn	0.25	V	0.125																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		14.2					14.2																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101903	1982		Nb3Sn0.85Tl0.15	Nb3Sn0.85Tl0.15	Nb	3	Sn	0.85	Tl	0.15																			1964																																														K		18.2					18.2																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
101904	185		Nb0.25Sn0.25Ta0.25V0	Nb0.25Sn0.25Ta0.25V0.25	Nb	0.25	Sn	0.25	Ta	0.25	V	0.25																	1960																												Cr3Si(A15)																	Cr3Si, A15	K		6.2					6.2																																																																																																					LT7 (Toronto), 1960 p382				REF.,176 382	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101905	185		Nb0.5Sn0.25Ta0.125V0	Nb0.5Sn0.25Ta0.125V0.125	Nb	0.5	Sn	0.25	Ta	0.125	V	0.125																	1960																												Cr3Si(A15)																	Cr3Si, A15	K		12.2					12.2																																																																																																					LT7 (Toronto), 1960 p382				REF.,176 382	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101906	473		Nb0.25Sn0.25Ta0.5	Nb0.25Sn0.25Ta0.5	Nb	0.25	Sn	0.25	Ta	0.5																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		10.8					10.8																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101907	473		Nb0.5Sn0.25Ta0.25	Nb0.5Sn0.25Ta0.25	Nb	0.5	Sn	0.25	Ta	0.25																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101908	473		NB0.625Sn0.25Ta0.125	Nb0.625Sn0.25Ta0.125	Nb	0.625	Sn	0.25	Ta	0.125																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
101909	911		Nb0.17Ta0.83	Nb0.17Ta0.83	Nb	0.17	Ta	0.83																					1968																																														K		4.65					4.65																																																																																																									J.PHYS.SOC.JAPAN,25(1968)1307	K.YASUKOCHI,T.OGASAWARA,Y.KUBOTA		
101910	1103		Nb0.2Ta0.8	Nb0.2Ta0.8	Nb	0.2	Ta	0.8																					1967																																														K		4.64					4.64																																																																																																									CRYOGENICS,7(1967)83	J.LOWELL,K.MENDELSSOHN,R.A.FRENCH		
101911	911		Nb0.92Ta0.71	Nb0.92Ta0.71	Nb	0.92	Ta	0.71																					1968																												CsCl																	CsCl, B2	K		4.94					4.94																																																																																																									J.PHYS.SOC.JAPAN,25(1968)1307	K.YASUKOCHI,T.OGASAWARA,Y.KUBOTA		
101912	911		Nb0.37Ta0.63	Nb0.37Ta0.63	Nb	0.37	Ta	0.63																					1968																												CsCl																	CsCl, B2	K		5.31					5.31																																																																																																									J.PHYS.SOC.JAPAN,25(1968)1307	K.YASUKOCHI,T.OGASAWARA,Y.KUBOTA		
101913	244		Nb0.47Ta0.53	Nb0.47Ta0.53	Nb	0.47	Ta	0.53																					1960																																														K		6.2					6.2																																																																																																									PROC.ROY.SOC.(LONDON)A,255(1960)267	A.C.ROSE-INNES,A.CALVERLY		
101914	722		Nb0.5Ta0.5	Nb0.5Ta0.5	Nb	0.5	Ta	0.5																					1965																																														K		6.25					6.25																																																																																																									PHYS.REV.,140(1965)A1169	B.SERIN,T.MCCONVILLE		
101915	244		Nb0.64Ta0.36	Nb0.64Ta0.36	Nb	0.64	Ta	0.36																					1960																																														K		6.8					6.8																																																																																																									PROC.ROY.SOC.(LONDON)A,255(1960)267	A.C.ROSE-INNES,A.CALVERLY		
101916	864		Nb0.803Ta0.197	Nb0.803Ta0.197	Nb	0.803	Ta	0.197																					1969																																														K		7.85					7.85																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)873	A.IKUSIMA,T.MIZUSAKI		
101917	911		Nb0.87Ta0.13	Nb0.87Ta0.13	Nb	0.87	Ta	0.13																					1968																												CsCl																	CsCl, B2	K		8.15					8.15																																																																																																									J.PHYS.SOC.JAPAN,25(1968)1307	K.YASUKOCHI,T.OGASAWARA,Y.KUBOTA		
101918	864		Nb0.938Ta0.062	Nb0.938Ta0.062	Nb	0.938	Ta	0.062																					1969																																														K		8.42					8.42																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)873	A.IKUSIMA,T.MIZUSAKI		
101919	964		Nb0.957Ta0.043	Nb0.957Ta0.043	Nb	0.957	Ta	0.043																					1966																												CsCl																	CsCl, B2	K		8.55					8.55																																																																																																									PHYS.LETT.,21(1966)501	J.P.CHARLESWORTH		
101920	864		Nb0.984Ta0.016	Nb0.984Ta0.016	Nb	0.984	Ta	0.016																					1969																																														K		8.76					8.76																																																																																																									J.PHYS.CHEM.SOLIDS,30(1969)873	A.IKUSIMA,T.MIZUSAKI		
101921	1241		Nb0.95Ti0.05	Nb0.95Ti0.05	Nb	0.95	Ti	0.05																					1971																																														K		9.41					9.41																																																																																																									J.PHYS.CHEM.SOLIDS, 32(1971)1531	M.S.LUBELL,R.H.KERNOHAN		
101922	796		Nb1Te2	Nb1Te2	Nb	1	Te	2																					1969																																													hexagonal	K		0.66					0.66																																																																																																									PHYS.LETT.A,29(1969)571	H.B.HARLAND,M.H.VAN MAAREN		
101923	711		Nb3Te4	Nb3Te4	Nb	3	Te	4																																																																			K		1.49					1.49																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
101924	1147		Nb0.03Tc0.97	Nb0.03Tc0.97	Nb	0.03	Tc	0.97																					1970																												Mg																	Mg, A3	K		12.8					12.8																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101925	1147		Nb0.06Tc0.94	Nb0.06Tc0.94	Nb	0.06	Tc	0.94																					1970																												Mg																	Mg, A3	K		12.8					12.8																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101926	1147		Nb0.24Tc0.76	Nb0.24Tc0.76	Nb	0.24	Tc	0.76																					1970																												alpha-Mn																	alpha-Mn, A12	K		12.9					12.9																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101927	1147		Nb0.42Tc0.58	Nb0.42Tc0.58	Nb	0.42	Tc	0.58																					1970																												alpha-Mn																	alpha-Mn, A12	K		10.9					10.9																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101928	1147		Nb0.69Tc0.31	Nb0.69Tc0.31	Nb	0.69	Tc	0.31																					1970																												W																	W, A2	K					2																																																																																																											J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101929	1147		Nb0.93Tc0.07	Nb0.93Tc0.07	Nb	0.93	Tc	0.07																					1970																												W																	W, A2	K		7					7																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101930	1147		Nb0.97Tc0.03	Nb0.97Tc0.03	Nb	0.97	Tc	0.03																					1970																												W																	W, A2	K		7.6					7.6																																																																																																									J.LESS-COMMON METALS,20(1970)173	A.L.GIORGI,E.G.SZKLARZ		
101931	1398		Nb0.31Ta0.06Ti0.62	Nb0.31Ta0.06Ti0.62	Nb	0.31	Ta	0.06	Ti	0.62																			1969																																														K		9					9																																																																																																					Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
101932	1356		Nb0.025Ta0.975	Nb0.025Ta0.975	Nb	0.025	Ta	0.975																					1970																																														K		4.465					4.465																																																																																																					Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
101933	1792		Nb0.5Ti0.3V0.2	Nb0.5Ti0.3V0.2	Nb	0.5	Ti	0.3	V	0.2																			1969																																														K		7.8					7.8																																																																																																					FROM Roberts' Table.				Trans.Met.Soc. AIME 245(1969)2350	J.T.A.Pollack,V.Sadagopan,H.C.Gatos		
101934	499		Nb0.025Ti0.975	Nb0.025Ti0.975	Nb	0.025	Ti	0.975																					1965																																													hexagonal	K		1.5					1.5																																																																																																					SUPERCONDUCTIVITY OF ALPH-TITANIUM SOLID SOLUTIONS WITH VANADIUM,NIOBIUM,AND TANTALUM				PHYS.REV.,137(1965)A142	CH.J.RAUB,U.ZWICKER		
101935	965		Nb0.22Ti0.8	Nb0.22Ti0.8	Nb	0.22	Ti	0.8																					1968																																														K		7.8					7.8																																																																																																									J.LESS-COMMON METALS,14(1968)253	E.ROSCHEL,T.MEIER,U.ZWICKER		
101936	1800		Nb0.25Ti0.75	Nb0.25Ti0.75	Nb	0.25	Ti	0.75																					1968																																														K		7.4					7.4																																																																																																									Z.METALLKDE.,59(1968)69	T.NISHIMURA,U.ZWICKER		
101937	1803		Nb0.33Ti0.67	Nb0.33Ti0.67	Nb	0.33	Ti	0.67																					1964																																														K		9.3					9.3																																																																																																									Z.METALLKDE.,55(1964)711	C.J.RAUB,U.ZWICKER		
101938	874		Nb0.44Ti0.56	Nb0.44Ti0.56	Nb	0.44	Ti	0.56																					1966																																														K		8.99					8.99																																																																																																									PHYS.REV.LETT.,17(1966)81	L.J.NEURINGER,Y.SHAPIRA		
101939	841		Nb0.5Ti0.5	Nb0.5Ti0.5	Nb	0.5	Ti	0.5																					1967																																														K		10.3					10.3																																																																																																									FIZ.METAL.METALLOVED,23(1967)511	A.A.SHUBIN,G.P.MOTULEVICH,I.Y.E.LEKSIMA,L.N.FEDOTOV		
101940	830		Nb0.55Ti0.45	Nb0.55Ti0.45	Nb	0.55	Ti	0.45																					1968																																														K		9.4					9.4																																																																																																									ZH.EKSP.TEOR.FIZ.,54(1968)1031	A.A.MATSAKOVA,B.G.LAZAREV,O.N.OVCHARENKO,V.G.VOLOTAKAYA		
101941	592		Nb0.6Ti0.4	Nb0.6Ti0.4	Nb	0.6	Ti	0.4																					1965																																														K		9.8					9.8																																																																																																					SOLUTE SIZE AND VALENCE EFFECT IN SOME SUPERCONDUCTING ALLOYS OF TRANSITION ELEMENTS				PHYS.REV.,140(1965)A914	WARREN DESORBO		
101942	1398		Nb0.7Ti0.3	Nb0.7Ti0.3	Nb	0.7	Ti	0.3																					1969																																														K		10.1					10.1																																																																																																					Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
101943	885		Nb0.75Ti0.25	Nb0.75Ti0.25	Nb	0.75	Ti	0.25																					1970																																														K		10.02					10.02																																																																																																									J.LOW TEMP.PHYS.,3(1970)393	F.J.CADIEU		
101944	1241		Nb0.9Ti0.1	Nb0.9Ti0.1	Nb	0.9	Ti	0.1																					1971																																														K		9.61					9.61																																																																																																									J.PHYS.CHEM.SOLIDS, 32(1971)1531	M.S.LUBELL,R.H.KERNOHAN		
101945	177		Nb0.26U0.74	Nb0.26U0.74	Nb	0.26	U	0.74																					1961																																														K		1.85					1.85																																																																																																					FROM Roberts' Table.				LT-7 (Univ.Toronto,1961)350	B.B.Goodman,J.Hillairet,J.J.Veyssie,L.Weil		
101946	349		Nb0.222U0.778	Nb0.222U0.778	Nb	0.222	U	0.778																					1959																												W																	W, A2	K		1.98					1.98																																																																																																									J.PHYS.CHEM.SOLIDS,11(1959)12	T.G.BERLINCOURT		
101947	965		Nb0.19Ti0.74Zr0.07	Nb0.19Ti0.74Zr0.07	Nb	0.19	Ti	0.74	Zr	0.07																			1968																																														K		9.1					9.1																																																																																																									J.LESS-COMMON METALS,14(1968)253	E.ROSCHEL,T.MEIER,U.ZWICKER		
101948	965		Nb0.21Ti0.61zr0.18	Nb0.21Ti0.61Zr0.18	Nb	0.21	Ti	0.61	Zr	0.18																			1968																																														K		7.21					7.21																																																																																																									J.LESS-COMMON METALS,14(1968)253	E.ROSCHEL,T.MEIER,U.ZWICKER		
101949	1391		Nb0.35Ti0.45Zr0.2	Nb0.35Ti0.45Zr0.2	Nb	0.35	Ti	0.45	Zr	0.2																			1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
101950	1789		Nb0.35Ti0.6Zr0.05	Nb0.35Ti0.6Zr0.05	Nb	0.35	Ti	0.6	Zr	0.05																			1968																																														K		8.6					8.6																																																																																																									TRANS.MET.SOC.AIME,242(1968)1793	F.ISHIDA,M.KITADA,T.DOI,U.KAWABE		
101951	830		Nb0.35Ti0.15Zr0.5	Nb0.35Ti0.15Zr0.5	Nb	0.35	Ti	0.15	Zr	0.5																			1968																																														K		9.3					9.3																																																																																																									ZH.EKSP.TEOR.FIZ.,54(1968)1031	A.A.MATSAKOVA,B.G.LAZAREV,O.N.OVCHARENKO,V.G.VOLOTAKAYA		
101952	1789		Nb0.5Ti0.1Zr0.4	Nb0.5Ti0.1Zr0.4	Nb	0.5	Ti	0.1	Zr	0.4																			1968																																														K		10.3					10.3																																																																																																									TRANS.MET.SOC.AIME,242(1968)1793	F.ISHIDA,M.KITADA,T.DOI,U.KAWABE		
101953	830		Nb0.75Ti0.15Zr0.1	Nb0.75Ti0.15Zr0.1	Nb	0.75	Ti	0.15	Zr	0.1																			1968																																														K		9.7					9.7																																																																																																									ZH.EKSP.TEOR.FIZ.,54(1968)1031	A.A.MATSAKOVA,B.G.LAZAREV,O.N.OVCHARENKO,V.G.VOLOTAKAYA		
101954	1792		Nb0.1Ti0.4V0.5	Nb0.1Ti0.4V0.5	Nb	0.1	Ti	0.4	V	0.5																			1969																																														K		5.3					5.3																																																																																																					FROM Roberts' Table.				Trans.Met.Soc. AIME 245(1969)2350	J.T.A.Pollack,V.Sadagopan,H.C.Gatos		
101955	1792		Nb0.4Ti0.4V0.2	Nb0.4Ti0.4V0.2	Nb	0.4	Ti	0.4	V	0.2																			1969																																														K		7.6					7.6																																																																																																					FROM Roberts' Table.				Trans.Met.Soc. AIME 245(1969)2350	J.T.A.Pollack,V.Sadagopan,H.C.Gatos		
101956	1792		Nb0.5Ti0.2V0.3	Nb0.5Ti0.2V0.3	Nb	0.5	Ti	0.2	V	0.3																			1969																																														K		8.5					8.5																																																																																																					FROM Roberts' Table.				Trans.Met.Soc. AIME 245(1969)2350	J.T.A.Pollack,V.Sadagopan,H.C.Gatos		
101957	1806		Nb0.1Zr0.9	Nb0.1Zr0.9	Nb	0.1	Zr	0.9																					1966																																														K		7.6					7.6																																																																																																									TRANS.MET.SOC.AIME,236(1966)1594	R.F.HEHEMANN,S.T.ZEGLER		
101958	1579		Nb0.13Zr0.87	Nb0.13Zr0.87	Nb	0.13	Zr	0.87																					1972																																														K		6.42					6.42																																																																																																					The superconducting transition behavior of Zr-Nb binary alloys				J.NUCLEAR MATERIALS,43(1972)258	F.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
101959	1806		NB0.15Zr0.85	Nb0.15Zr0.85	Nb	0.15	Zr	0.85																					1966																																														K		6.2					6.2																																																																																																									TRANS.MET.SOC.AIME,236(1966)1594	R.F.HEHEMANN,S.T.ZEGLER		
101960	1579		Nb0.2Zr0.8	Nb0.2Zr0.8	Nb	0.2	Zr	0.8																					1972																																														K		8					8																																																																																																					The superconducting transition behavior of Zr-Nb binary alloys				J.NUCLEAR MATERIALS,43(1972)258	F.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
101961	971		Nb0.25Zr0.75	Nb0.25Zr0.75	Nb	0.25	Zr	0.75																					1965																																														K		10.45					10.45																																																																																																									ZH.EKSP.TEOR.FIZ.,48(1965)818	I.N.GONCHAROV,I.S.KHUKHAREVA,YU.F.BYCHKOV		
101962	1157		NB0.38Zr0.62	Nb0.38Zr0.62	Nb	0.38	Zr	0.62																					1967																																														K		8.7					8.7																																																																																																									PHYS.REV.,158(1967)340	D.M.GINSBERG,J.K.HULM,R.L.CAPPELLETTI		
101963	1301		Nb0.5Zr0.5	Nb0.5Zr0.5	Nb	0.5	Zr	0.5																					1968																																														K		10.75					10.75																																																																																																									ZH.EKSP.TEOR.FIZ.,55(1968)2160	E.PAPP,N.B.BRANDT		
101964	1333		Nb0.6Zr0.4	Nb0.6Zr0.4	Nb	0.6	Zr	0.4																					1972																																														K		10.75					10.75																																																																																																									PHIL.MAG.,25(1972)1291	I.MILNE,T.R.FINLAYSON		
101965	1313		Nb0.68Zr0.32	Nb0.68Zr0.32	Nb	0.68	Zr	0.32																					1971																																														K		10.05					10.05																																																																																																									SOLID STATE COMMUN.,9(1971)1339	I.MILNE,T.R.FINLAYSON		
101966	1157		Nb0.75Zr0.25	Nb0.75Zr0.25	Nb	0.75	Zr	0.25																					1967																												W																	W, A2	K		11					11																																																																																																									PHYS.REV.,158(1967)340	D.M.GINSBERG,J.K.HULM,R.L.CAPPELLETTI		
101967	1352	NMR (Nb< 93 >) measurements 	Nb0.85Zr0.15	Nb0.85Zr0.15	Nb	0.85	Zr	0.15																					1967																																														K		10.8					10.8																																																								mj/mol.K2	10.5		234																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
101968	1707		Nb0.5V1.5Zr1	Nb0.5V1.5Zr1	Nb	0.5	V	1.5	Zr	1																			1968																												MgZn2(Laves)																	MgZn2, C14	K		4.3					4.3																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
101969	32		Ni0.1Zr0.9	Ni0.1Zr0.9	Ni	0.1	Zr	0.9																					1955																																													hexagonal	K		1.5					1.5																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
101970	1355		Ni1Zr2	Ni1Zr2	Ni	1	Zr	2																					1970																												CuAl2																	CuAl2, C16	K		1.6					1.6																																																																																																									J.PHYS.SOC.JAPAN,29(1970)879	K.YAMAYA,T.MITSUI,T.SAMGONGI		
101971	RMP0350001		Ni0.5V0.16Zr0.34	Ni0.5V0.16Zr0.34	Ni	0.5	V	0.16	Zr	0.34																			1963																												MgCu2(Laves)																	MgCu2, C15	K		0.43					0.43																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101972	707		Ni0.22V0.78	Ni0.22V0.78	Ni	0.22	V	0.78																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		0.35					0.35																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
101973	1866		Ni1U6	Ni1U6	Ni	1	U	6																					1975																												U6Mn																	MnU6, D2[c]	K		0.86					0.86																																																																																																					Lattice parameters and superconductivity of the compounds U6Mn, U6Fe, U6Co and U6Ni and alloys between them				J.Phys.Chem.Solids, 36(1975)123	J.J.ENGLEHARDT		
101974	173		Ni3Th7	Ni3Th7	Ni	3	Th	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		1.98					1.98																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101975	1377		Ni1Ta2	Ni1Ta2	Ni	1	Ta	2																					1972																												CuAl2																	CuAl2, C16	K		0.9					0.9																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
101976	1060		Ni0.05Rh0.04Ti0.91	Ni0.05Rh0.04Ti0.91	Ni	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.5					3.5																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101977	301		Ni0.1Pd0.9Te2	Ni0.1Pd0.9Te2	Ni	0.1	Pd	0.9	Te	2																			1961																												CdI2																	CdI2, C6	K		1.3					1.3																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
101978	301		Ni0.05Pd0.95Te2	Ni0.05Pd0.95Te2	Ni	0.05	Pd	0.95	Te	2																			1961																												CdI2																	CdI2, C6	K		1.4					1.4																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
101979	1438		Nb0.2Zr0.8	Nb0.2Zr0.8	Nb	0.2	Zr	0.8																					1974																																														K		9.2					9.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
101980	1740		Nb0.04Zr0.96	Nb0.04Zr0.96	Nb	0.04	Zr	0.96																					1967																																														K		4.9					4.9																																																																																																									FIZ.METAL.METALLOVED.,23(1967)871	N.N.BUYNOV,S.V.SUDAREVA,YE.P.ROMANOV		
101981	644		O3Tl0.03W1	O3Tl0.03W1	O	3	Tl	0.03	W	1																			1966																																													hexagonal	K		2.14					2.14																																																																																																									SOLID STATE COMMUN.,4(1966)25	F.J.DARNELL,P.E.BIERSTEDT,T.A.BITHER		
101982	1450		O1.07Ti1	O1.07Ti1	O	1.07	Ti	1																					1972																												NaCl																	NaCl, B1	K		1					1																																																																																																					Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
101983	1472		O1Ti1	O1Ti1	O	1	Ti	1																					1972																																													monoclinic	K		1.06					1.06																																																																																																					"Superconductivity in cubic and monoclinic ""TiO"""				J.APPL.PHYS.,43(1972)2478	M.D.BANUS,M.SJOSTRAND,P.H.DEESOM,T.B.REED		
101984	1542		O1Ti1	O1Ti1	O	1	Ti	1																					1971																												NaCl																	NaCl, B1	K		0.6					0.6																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
101985	644		O3Sr0.08W1	O3Sr0.08W1	O	3	Sr	0.08	W	1																			1966																																													hexagonal	K		4					4																																																																																																									SOLID STATE COMMUN.,4(1966)25	F.J.DARNELL,P.E.BIERSTEDT,T.A.BITHER		
101986	84		O1Sn1	O1Sn1	O	1	Sn	1																					1933																																														K		3.81					3.81																																																																																																					From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
101987	RMP0350001		O0.105Rh0.285Zr0.61	O0.105Rh0.285Zr0.61	O	0.105	Rh	0.285	Zr	0.61																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		11.8					11.8																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101988	RMP0350001		O0.14Rh0.287Ti0.573	O0.14Rh0.287Ti0.573	O	0.14	Rh	0.287	Ti	0.573																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		3.37					3.37																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101989	181		O1Re1Ti1	O1Re1Ti1	O	1	Re	1	Ti	1																																																																	K		5.74					5.74																																																																																																					From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
101990	1883		O3Rb0.33W1	O3Rb0.33W1	O	3	Rb	0.33	W	1																			1975																																														K		7.7					7.7																																																																																																					Ph.D thesis , Stanford Univ.(1969) quoted in this paper				J.Solid State Chem., 12(1975)362	A.R.Sweedler		
101991	RMP0350001		O0.105Pd0.285Zr0.61	O0.105Pd0.285Zr0.61	O	0.105	Pd	0.285	Zr	0.61																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		2.09					2.09																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101992	1542		O1b1	Nb1O1	Nb	1	O	1																					1971																												NaCl																	NaCl, B1	K		1.39					1.39																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
101993	RMP0350001		Os1Ti1	Os1Ti1	Os	1	Ti	1																					1963																												CsCl																	CsCl, B2	K		0.46					0.46																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
101994	173		Os3Th7	Os3Th7	Os	3	Th	7																					1961																												Fe3Th7																	Fe3Th7, D10[2]	K		1.51					1.51																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101995	173		Os1Ta1	Os1Ta1	Os	1	Ta	1																					1961																												alpha-Mn																	alpha-Mn, A12	K		1.95					1.95																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
101996	127		Os2Sc1	Os2Sc1	Os	2	Sc	1																					1959																												MgZn2(Laves)																	MgZn2, C14	K		4.6					4.6																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
101997	1060		Os0.05Rh0.04Ti0.91	Os0.05Rh0.04Ti0.91	Os	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.5					3.5																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
101998	1368		Os0.97Rh0.03	Os0.97Rh0.03	Os	0.97	Rh	0.03																					1972																																													hexagonal	K		0.09					0.09																																																																																																					data quoted in this paper				J.Less-Common Metals, 26(1972)319	A.C.Mota		
101999	171		Os1Re1Y1	Os1Re1Y1	Os	1	Re	1	Y	1																			1960																																														K		2					2																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
102000	1646		Os0.058Re0.942	Os0.058Re0.942	Os	0.058	Re	0.942																					1971																																													hexagonal	K		1.93					1.93																																																																																																									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
102001	569		Os1	Os1	Os	1																							1965																												Mg																	Mg, A3	K		0.66					0.66																																																																																																									CROGENICS,5(1965)283	C.PALMY,E.BUCHER,J.L.OLSEN,J.MULLER		
102002	503	films by vacuum evaporation	O1W3	O1W3	O	1	W	3																					1965																												Cr3Si(A15)																	Cr3Si, A15	K		3.35					3.35																																																																																																					SUPERCONDUCTIVITY IN FILMS OF BETA TUNGSTEN AND OTHER TRANSITION METALS				PHYS.REV.LETT.,15(1965)260	A.S.COOPER,B.T.MATTHIAS,G.W.HULL,K.ANDRES,T.H.GEBALLE,W.L.BOND		
102003	RMP0350001		O1V3Zr3	O1V3Zr3	O	1	V	3	Zr	3																			1963																												Fe3W3C																	Fe3W3C, E9[3]	K		7.5					7.5																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102004	248		O0.03V0.97	O0.03V0.97	O	0.03	V	0.97																																																																		cubic	K		2.4					2.4																																																																																																					FROM Roberts' Table.				unpublished	W.DeSorbo,G.E.Nichols		
102005	85		P1Pb1	P1Pb1	P	1	Pb	1																					1932																																														K		7.8					7.8																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
102006	32		Os0.06Zr0.94	Os0.06Zr0.94	Os	0.06	Zr	0.94																					1955																																													hexagonal	K		5.6					5.6																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102007	173		Os2Zr1	Os2Zr1	Os	2	Zr	1																					1961																												MgZn2(Laves)																	MgZn2, C14	K		3					3																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102008	1478		Os2Y1	Os2Y1	Os	2	Y	1																					1971																												MgZn2(Laves)																	MgZn2, C14	K		4.7					4.7																																																																																																									J.LOW TEMP.PHYS.,4(1971)669	S.L.MCCARTHY		
102009	266		Os0.075W0.925	Os0.075W0.925	Os	0.075	W	0.925																					1962																																													cubic	K		0.9					0.9																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102010	266		Os0.1W0.9	Os0.1W0.9	Os	0.1	W	0.9																					1962																																														K		1.5					1.5																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102011	266		Os0.15W0.85	Os0.15W0.85	Os	0.15	W	0.85																					1962																																														K		2.2					2.2																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102012	33		Os0.25W0.75	Os0.25W0.75	Os	0.25	W	0.75																					1955																																														K		3.02					3.02																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
102013	276		Os0.34W0.66	Os0.34W0.66	Os	0.34	W	0.66																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		3.81					3.81																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102014	182		Os0.74W0.26	Os0.74W0.26	Os	0.74	W	0.26																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.4					4.4																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102015	948		Os0.5V0.5	Os0.5V0.5	Os	0.5	V	0.5																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		5.15					5.15																																																																																																									J.PHYS.CHEM.SOLIDS, 31(1970)1531	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FLUKIGER		
102016	707		Os0.55V0.45	Os0.55V0.45	Os	0.55	V	0.45																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		5.04					5.04																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102017	756		Pb1Pt1	Pb1Pt1	Pb	1	Pt	1																					1964																																														K		7.2					7.2																																																																																																									PHYS.REV.,136(1964)A637	H.C.THEURERER,J.J.HAUSER,N.R.WERTHAMER		
102018	229		Pb0.8Pt0.2	Pb0.8Pt0.2	Pb	0.8	Pt	0.2																					1962																																														K		2.8					2.8																																																																																																									J.PHYS.CHEM.SOLIDS,23(1962)405	M.F.GENDRON,R.E.JONES		
102019	1377		Pb2Pd1	Pb2Pd1	Pb	2	Pd	1																					1972																												CuAl2																	CuAl2, C16	K		3.01					3.01																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102020	1193		Pb1Mo6S7	Pb1Mo6S7	Pb	1	Mo	6	S	7																			1972																																														K		11.1					11.1																																																																																																									SCI.,177(1972)267	A.C.LAWSON,R.VISWANATHAN		
102021	1709		Pb1	Pb1	Pb	1																							1972																												Cu																	Cu, A1	K		7.195					7.195																																																																																																									PHYS.REV.B,5(1972)4357	G.CHANIN,J.P.TORRE		
102022	1936		Pa0.75Zr0.25	Pa0.75Zr0.25	Pa	0.75	Zr	0.25																					1974																																														K		1.54					1.54																																																																																																					FROM Roberts' Table.				LT-13(1974)vol.3 p=377	R.D.Fowler,L.B.Asprey,J.D.G.Lindsay,R.W.White		
102023	504		Pa1	Pa1	Pa	1																							1965																																													tetragonal	K		1.4					1.4																																																																																																					SUPERCONDUCTIVITY OF PROTACTINIUM				PHYS.REV.LETT.,15(1965)860	B.T.MATTHIAS,C.E.OLSEN,H.H.HILL,J.D.G.LINDSEY,L.B.ASPREY,R.D.FOWLER,W.WHITE		
102024	601		P1W3	P1W3	P	1	W	3																					1965																												Ni3P																	Ni3P, D0[e]	K		2.76					2.76																																																																																																					Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
102025	1382		P1Sn1	P1Sn1	P	1	Sn	1																					1970																												NaCl																	NaCl, B1	K		4					4																																																																																																									INORGANIC CHEM.,9(1970)335	P.C.DONOHUE		
102026	1976		P0.3si0.7V3	P0.3Si0.7V3	P	0.3	Si	0.7	V	3																			1971																												Cr3Si(A15)																	Cr3Si, A15	K		14.75					14.75																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
102027	1976		P0.2Si0.8V3	P0.2Si0.8V3	P	0.2	Si	0.8	V	3																			1971																												Cr3Si(A15)																	Cr3Si, A15	K		16.6					16.6																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
102028	491		P1Rh2	P1Rh2	P	1	Rh	2																					1963																												CaF2																	CaF2, C1	K					1.03																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102029	715		Pb3Th1	Pb3Th1	Pb	3	Th	1																					1970																												AuCu3																	AuCu3, L1[2]	K		5.55					5.55																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102030	715		Pb3Sr1	Pb3Sr1	Pb	3	Sr	1																					1970																																													tetragonal	K		1.85					1.85																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102031	1491	quench condensed at 0.4 K 	Pb0.9Sn0.1	Pb0.9Sn0.1	Pb	0.9	Sn	0.1																					1973																																														K		7.17					7.17																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
102032	1153		Pb0.01Sn0.99	Pb0.01Sn0.99	Pb	0.01	Sn	0.99																					1967																																														K		3.752					3.752																																																																																																									PHYS.REV.,154(1967)329	C.A.REYNOLDS,C.W.LBRICH,G.J.PERSON,J.E.GUETHS,M.A.MITCHELL		
102033	1917		Pb0.28Sn0.72	Pb0.28Sn0.72	Pb	0.28	Sn	0.72																					1969																																														K		7.05					7.05																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
102034	1917		Pb0.36Sn0.64	Pb0.36Sn0.64	Pb	0.36	Sn	0.64																					1969																																														K		7.75					7.75																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
102035	1917		Pb0.57Sn0.43	Pb0.57Sn0.43	Pb	0.57	Sn	0.43																					1969																																														K		7.45					7.45																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
102036	1491	quench condensed at 0.4 K 	Pb0.9Sb0.1	Pb0.9Sb0.1	Pb	0.9	Sb	0.1																					1973																																														K		6.28					6.28																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
102037	109	eutectec	Pb1Sb1	Pb1Sb1	Pb	1	Sb	1																					1930																																														K		6.6					6.6																																																																																																									ROY.SOC.CANADA TRANS.,24(1930)25	J.C.MCLENNAN,J.F.ALLEN,J.O.WILHELM		
102038	778		Pb1S3Ta1	Pb1S3Ta1	Pb	1	S	3	Ta	1																			1970																																													tetragonal	K		3.11					3.11																																																																																																									PHYS.LETT.A,31(1970)551	L.SCHMIDT		
102039	1377		Pb1.9Rh1	Pb1.9Rh1	Pb	1.9	Rh	1																					1972																												CuAl2																	CuAl2, C16	K		1.32					1.32																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102040	229		Pb2Rh1	Pb2Rh1	Pb	2	Rh	1																					1962																												CuAl2																	CuAl2, C16	K		2.66					2.66																																																																																																									J.PHYS.CHEM.SOLIDS,23(1962)405	M.F.GENDRON,R.E.JONES		
102041	1491	quench condensed at 0.4 K 	Pb0.9Zn0.1	Pb0.9Zn0.1	Pb	0.9	Zn	0.1																					1973																																														K		7.12					7.12																																																																																																									J.LOW TEMP.PHYS.,13(1973)1	C.G.GRANQUIST,T.CLAESON		
102042	715		Pb3Yb1	Pb3Yb1	Pb	3	Yb	1																					1970																												AuCu3																	AuCu3, L1[2]	K		0.23					0.23																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102043	715		Pb3Y1	Pb3Y1	Pb	3	Y	1																					1970																												AuCu3																	AuCu3, L1[2]	K		4.72					4.72																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102044	82		Pb1Tl2	Pb1Tl2	Pb	1	Tl	2																					1935																																														K		4.1					4.1																																																																																																					FROM Roberts' Table.				Phys.Z.Sowjetunion, 7(1935)122	J.N.Rjabinin,L.W.Schubnikow		
102045	74		Pb0.35Tl0.65	Pb0.35Tl0.65	Pb	0.35	Tl	0.65																					1935																																														K		3.8					3.8																																																																																																					FROM Roberts' Table.				Proc.Kon.Akad.Amsterdam, 38(1935)2	W.J.DeHaas,J.M.Casimir-Jonker		
102046	403		Pb0.6Tl0.4	Pb0.6Tl0.4	Pb	0.6	Tl	0.4																					1931																																														K		5.8					5.8																																																																																																									COMM.KAMERLINGH ONNES LAB.,19(1931)214B	J.VOOGD,W.J.DEHAAS		
102047	1200		Pb0.73Tl0.27	Pb0.73Tl0.27	Pb	0.73	Tl	0.27																					1965																																														K		6.43					6.43																																																																																																									J.APPL.PHYS.,36(1965)2895	R.H.KERNOHAN,S.T.SEKULA		
102048	653		Pb0.79Tl0.21	Pb0.79Tl0.21	Pb	0.79	Tl	0.21																					1966																																														K		6.43					6.43																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102049	653		Pb0.85Tl0.15	Pb0.85Tl0.15	Pb	0.85	Tl	0.15																					1966																																														K		6.73					6.73																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102050	653		Pb0.89Tl0.11	Pb0.89Tl0.11	Pb	0.89	Tl	0.11																					1966																																														K		6.88					6.88																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102051	653		Pb0.93Tl0.075	Pb0.93Tl0.075	Pb	0.93	Tl	0.075																					1966																																														K		6.98					6.98																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102052	653		Pb0.96Tl0.04	Pb0.96Tl0.04	Pb	0.96	Tl	0.04																					1966																																														K		7.06					7.06																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102053	RMP0350001		Pd1Sb2	Pd1Sb2	Pd	1	Sb	2																					1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.25					1.25																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102054	1296		Pd1Sb1	Pd1Sb1	Pd	1	Sb	1																					1968																												NiAs																	NiAs, B8[1]	K		1.66					1.66																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
102055	491	rapid quench	Pd2.2S1	Pd2.2S1	Pd	2.2	S	1																					1963																															A	8.93													cubic	K		1.63					1.63																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102056	32		Pd0.05Ru0.05Zr0.9	Pd0.05Ru0.05Zr0.9	Pd	0.05	Ru	0.05	Zr	0.9																			1955																																														K		9					9																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102057	1372		Pd0.02Rh0.31Zr0.67	Pd0.02Rh0.31Zr0.67	Pd	0.02	Rh	0.31	Zr	0.67																			1972																												CuAl2																	CuAl2, C16	K		9.85					9.85																																																																																																									J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
102058	1372		Pd0.4Rh0.29Zr0.67	Pd0.04Rh0.29Zr0.67	Pd	0.04	Rh	0.29	Zr	0.67																			1972																												CuAl2																	CuAl2, C16	K		8.56					8.56																																																																																																									J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
102059	1060		Pd0.05Rh0.04Ti0.91	Pd0.05Rh0.04Ti0.91	Pd	0.05	Rh	0.04	Ti	0.91																			1964																																														K		3.7					3.7																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102060	301		Pd0.95Rh0.05Te2	Pd0.95Rh0.05Te2	Pd	0.95	Rh	0.05	Te	2																			1961																												CdI2																	CdI2, C6	K		1.65					1.65																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102061	301		Pd0.95Pt0.05Te2	Pd0.95Pt0.05Te2	Pd	0.95	Pt	0.05	Te	2																			1961																												CdI2																	CdI2, C6	K		1.71					1.71																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102062	301		Pd0.9Pt0.1Te2	Pd0.9Pt0.1Te2	Pd	0.9	Pt	0.1	Te	2																			1961																												CdI2																	CdI2, C6	K		1.65					1.65																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102063	RMP0350001		Pb1Zr3	Pb1Zr3	Pb	1	Zr	3																					1963																												Cr3Si(A15)																	Cr3Si, A15	K		0.76					0.76																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102064	RMP0350001		Pb3Zr5	Pb3Zr5	Pb	3	Zr	5																					1963																												Mn5Si3																	Mn5Si3, D8[8]	K		4.6					4.6																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102065	491		Pd1Sn1	Pd1Sn1	Pd	1	Sn	1																					1963																												MnP			A	3.87	6.13	6.32											MnP, B31	K		0.41					0.41																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102066	491		Pd3Sn2	Pd3Sn2	Pd	3	Sn	2																					1963																												Ni2In																	Ni2In, B8[2]	K		0.64					0.64																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102067	491		Pd2Sn1	Pd2Sn1	Pd	2	Sn	1																					1963																												Co2Si			A	8.12	5.65	4.31											Co2Si, C37	K		0.41					0.41																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102068	RMP0350001		Pd1Si1	Pd1Si1	Pd	1	Si	1																					1963																												MnP			A	6.133	5.599	3.381											MnP, B31	K		0.93					0.93																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102069	140		Pd0.67Se0.33	Pd0.67Se0.33	Pd	0.67	Se	0.33																					1958																																														K		2.2					2.2																																																																																																									J.PHYS.CHEM.SOLIDS,4(1958)318	B.T.MATTHIAS,S.GELLER		
102070	140		Pd5Se2	Pd5Se2	Pd	5	Se	2																					1958																																														K		2.3					2.3																																																																																																									J.PHYS.CHEM.SOLIDS,4(1958)318	B.T.MATTHIAS,S.GELLER		
102071	552		Pd4Se1	Pd4Se1	Pd	4	Se	1																					1965																															A	5.2324		5.647											tetragonal	K		0.42					0.42																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102072	552	PdxSe x= 6 - 7.  	Pd6.7Se1	Pd6.7Se1	Pd	6.7	Se	1																					1965																																														K		0.66					0.66																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102073	413		Pd1Sb1Te1	Pd1Sb1Te1	Pd	1	Sb	1	Te	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.2					1.2																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
102074	413		Pd1Sb1Se1	Pd1Sb1Se1	Pd	1	Sb	1	Se	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1					1																																																																																																									PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
102075	950		Pd0.51Sb0.49	Pd0.51Sb0.49	Pd	0.51	Sb	0.49																					1968																																														K		1.67					1.67																																																																																																									PHYS.REV.,169(1968)457	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
102076	1116	rapid quench 	Pd0.165Sb0.835	Pd0.165Sb0.835	Pd	0.165	Sb	0.835																					1971																																													cubic	K		4.9					4.9																																																																																																									PHYS.LETT.A,34(1971)80	C.C.TSUEI,H.YEN,P.DUWEZ		
102077	1377		Pd1Tl2	Pd1Tl2	Pd	1	Tl	2																					1972																												CuAl2																	CuAl2, C16	K		1.32					1.32																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102078	1377		Pd1Th2	Pd1Th2	Pd	1	Th	2																					1972																												CuAl2																	CuAl2, C16	K		0.75					0.75																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102079	552		Pd0.87Te2	Pd0.87Te2	Pd	0.87	Te	2																					1965																												CdI2			A	4.037		5.127											CdI2, C6	K		1.85					1.85																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102080	552		Pd0.95Te2	Pd0.95Te2	Pd	0.95	Te	2																					1965																												CdI2			A	4.037		5.128											CdI2, C6	K		1.89					1.89																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102081	301		Pd1.05Te2	Pd1.05Te2	Pd	1.05	Te	2																					1961																												CdI2																	CdI2, C6	K		1.77					1.77																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102082	1027		Pd1Te2	Pd1Te2	Pd	1	Te	2																					1970																												CdI2																	CdI2, C6	K		1.69					1.69																																																																																																					Superconductivity in layered structure organo-metallic crystals				Science, 168(1970)568	F.R.Gamble,F.J.DeSalvo,R.A.Klemm,T.H.Geballe		
102083	301		Pd1.25Te2	Pd1.25Te2	Pd	1.25	Te	2																					1961																												CdI2																	CdI2, C6	K		2.2					2.2																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102084	301		Pd1.5Te2	Pd1.5Te2	Pd	1.5	Te	2																					1961																												CdI2																	CdI2, C6	K		2.21					2.21																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102085	301		Pd1.75Te2	Pd1.75Te2	Pd	1.75	Te	2																					1961																												CdI2																	CdI2, C6	K		2.25					2.25																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102086	552		Pd1Te1	Pd1Te1	Pd	1	Te	1																					1965																												NiAs			A	4.152													NiAs, B8[1]	K		3.85					3.85																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102087	552		Pd3Te1	Pd3Te1	Pd	3	Te	1																					1965																																														K		0.76					0.76																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102088	426		Pd1Sn2	Pd1Sn2	Pd	1	Sn	2																																																																			K		3.34					3.34																																																																																																					FROM Roberts' Table.				unpublished	K.Yasukochi		
102089	469		Pt1Th1	Pt1Th1	Pt	1	Th	1																					1965																																														K		0.44					0.44																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102090	469		Pt5Th1	Pt5Th1	Pt	5	Th	1																					1965																																														K		3.13					3.13																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102091	552		Pt1Te1	Pt1Te1	Pt	1	Te	1																					1965																															A	6.6144	5.636	11.865											orthorhombic	K		0.59					0.59																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102092	707		Pt0.15Ta0.85	Pt0.15Ta0.85	Pt	0.15	Ta	0.85																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		0.4					0.4																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102093	276		Pt0.3Ta0.7	Pt0.3Ta0.7	Pt	0.3	Ta	0.7																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.45					1.45																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102094	182		Pt1Ta1	Pt1Ta1	Pt	1	Ta	1																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1					1																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102095	486		Pt1Sn1	Pt1Sn1	Pt	1	Sn	1																					1965																												NiAs																	NiAs, B8[1]	K		0.37					0.37																																																																																																									J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
102096	RMP0350001		Pt1Si1	Pt1Si1	Pt	1	Si	1																					1963																												MnP			A	5.932	5.595	3.603											MnP, B31	K		0.88					0.88																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102097	037		Pt1Sb1	Pt1Sb1	Pt	1	Sb	1																					1953																												NiAs																	NiAs, B8[1]	K		2.1					2.1																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
102098	1060		Pt0.05Rh0.04Ti0.91	Pt0.05Rh0.04Ti0.91	Pt	0.05	Rh	0.04	Ti	0.91																			1964																																														K		4.3					4.3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102099	32		Pd0.1Zr0.9	Pd0.1Zr0.9	Pd	0.1	Zr	0.9																					1955																																													hexagonal	K		7.5					7.5																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102100	707		Pd1V3	Pd1V3	Pd	1	V	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		0.082					0.082																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102101	127		Pt2Y1	Pt2Y1	Pt	2	Y	1																					1959																												MgCu2(Laves)																	MgCu2, C15	K		1.57					1.57																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
102102	469		Pt2.2Y1	Pt2.2Y1	Pt	2.2	Y	1																					1965																												MgCu2(Laves)																	MgCu2, C15	K		1.7					1.7																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102103	239		Pt0.5W0.5	Pt0.5W0.5	Pt	0.5	W	0.5																					1963																																														K		1.45					1.45																																																																																																					SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
102104	707		Pt0.22V0.78	Pt0.22V0.78	Pt	0.22	V	0.78																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		1.76					1.76																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102105	1177		Pt1V3	Pt1V3	Pt	1	V	3																					1971																												Cr3Si(A15)																	Cr3Si, A15	K		3.62					3.62																																																																																																					FROM Roberts' Table.				LT-12(1971)333	J.E.Cox,R.A.Hein,R.M.Waterstrat		
102106	948		Pt1V3	Pt1V3	Pt	1	V	3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		3.2					3.2																																																																																																									J.PHYS.CHEM.SOLIDS, 31(1970)1531	A.JUNOD,F.HEINIGER,J.L.STAUDENMANN,J.MULLER,P.SPITZLI,R.FLUKIGER		
102107	707		Pt1V3	Pt1V3	Pt	1	V	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		3.62					3.62																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102108	700		Pt0.017U0.983	Pt0.017U0.983	Pt	0.017	U	0.983																					1966																																														K		0.85					0.85																																																																																																									SCIENCE,151(1966)985	B.T.MATTHIAS,D.K.WOHLLEBEN,E.CORENZWIT,G.W.HULL JR.,J.C.HO,K.ANDRES,N.E.PHILLIPS,T.H.GEBALLE		
102109	698		Pt0.02U0.98	Pt0.02U0.98	Pt	0.02	U	0.98																					1966																																														K		0.87			1.2		0.87																																																																																																									SCIENCE,152(1966)755	B.T.MATTHIAS,E.S.FISHER,K.ANDRESS,T.F.SMITH,T.H.GEBALLE,W.H.ZACHARIASEN		
102110	1377		Pt1Tl2	Pt1Tl2	Pt	1	Tl	2																					1972																												CuAl2																	CuAl2, C16	K		1.58					1.58																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102111	707		Pt1Ti3	Pt1Ti3	Pt	1	Ti	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		0.58					0.58																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102112	469		Pt3Th7	Pt3Th7	Pt	3	Th	7																					1965																												Fe3Th7																	Fe3Th7, D10[2]	K		0.98					0.98																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102113	182		Re1Ta1	Re1Ta1	Re	1	Ta	1																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.3					1.3																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102114	276		Re0.65Ta0.35	Re0.65Ta0.35	Re	0.65	Ta	0.35																					1961																												alpha-Mn																	alpha-Mn, A12	K		1.58					1.58																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102115	182		Re0.75Ta0.25	Re0.75Ta0.25	Re	0.75	Ta	0.25																					1961																												alpha-Mn																	alpha-Mn, A12	K		6.78					6.78																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102116	1646		Re0.83Ru0.17	Re0.83Ru0.17	Re	0.83	Ru	0.17																					1971																																													hexagonal	K		2.23					2.23																																																																																																									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
102117	1060		Re0.05Th0.04Ti0.91	Re0.05Rh0.04Ti0.91	Re	0.05	Rh	0.04	Ti	0.91																			1964																																														K		2.3					2.3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102118	1646		Re0.94Os0.06	Os0.06Re0.94	Os	0.06	Re	0.94																					1971																																														K		1.93					1.93																																																																																																									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
102119	503		Re1	Re1	Re	1																							1965																																														K		7					7																																																																																																					SUPERCONDUCTIVITY IN FILMS OF BETA TUNGSTEN AND OTHER TRANSITION METALS				PHYS.REV.LETT.,15(1965)260	A.S.COOPER,B.T.MATTHIAS,G.W.HULL,K.ANDRES,T.H.GEBALLE,W.L.BOND		
102120	1636		Re1	Re1	Re	1																							1971																																														K		1.696					1.696																																																																																																									PHYS.REV.B,4(1971)2988	M.L.A.MACVICAR,R.M.ROSE,S.I.OCHIAI		
102121	32		Pt1Zr1	Pt1Zr1	Pt	1	Zr	1																					1955																												Mg																	Mg, A3	K		3					3																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102122	469		Pt0.42Y0.58	Pt0.42Y0.58	Pt	0.42	Y	0.58																					1965																																														K		0.76					0.76																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102123	469		Pt3Y7	Pt3Y7	Pt	3	Y	7																					1965																												Fe3Th7																	Fe3Th7, D10[2]	K		0.82					0.82																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102124	469		Pt2Y3	Pt2Y3	Pt	2	Y	3																					1965																																														K		0.9					0.9																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102125	266		Re0.15W0.85	Re0.15W0.85	Re	0.15	W	0.85																					1962																																													cubic	K		2.4					2.4																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102126	266		Re0.25W0.75	Re0.25W0.75	Re	0.25	W	0.75																					1962																																													cubic	K		4.6					4.6																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102127	266		Re0.6W0.4	Re0.6W0.4	Re	0.6	W	0.4																					1962																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6					6																																																																																																									IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102128	182		Re3W1	Re3W1	Re	3	W	1																					1961																												alpha-Mn																	alpha-Mn, A12	K		9					9																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102129	412		Re0.6V0.4	Re0.6V0.4	Re	0.6	V	0.4																																																	W																	W, A2	K		2.2					2.2																																																																																																					From Roberts' Table, Private communication				Private communication	J.Muller		
102130	412		Re0.76V0.24	Re0.76V0.24	Re	0.76	V	0.24																																																	sigma-CrFe																	sigma-CrFe, D8[b]	K		4.52					4.52																																																																																																					From Roberts' Table, Private communication				Private communication	J.Muller		
102131	RMP0350001		Re0.9V0.1	Re0.9V0.1	Re	0.9	V	0.1																					1963																																														K		9.4					9.4																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102132	572		Re0.92V0.08	Re0.92V0.08	Re	0.92	V	0.08																					1966																												Mg																	Mg, A3	K		6.8					6.8																																																																																																									PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102133	1438		Re0.83Ti0.17	Re0.83Ti0.17	Re	0.83	Ti	0.17																					1974																																														K		9					9																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102134	173		Re24Ti5	Re24Ti5	Re	24	Ti	5																					1961																												alpha-Mn																	alpha-Mn, A12	K		6.6					6.6																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102135	711		Re2Th1	Re2Th1	Re	2	Th	1																																																	MgZn2(Laves)																	MgZn2, C14	K		5.05					5.05																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102136	1438		Re0.75Ta0.25	Re0.75Ta0.25	Re	0.75	Ta	0.25																					1974																																														K		4.7					4.7																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102137	33		Rh0.53Se0.47	Rh0.53Se0.47	Rh	0.53	Se	0.47																					1955																												FeS2(pyrite)																	FeS2(pyrite), C2	K		6					6																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
102138	1060		Rh0.04Sc0.05Ti0.91	Rh0.04Sc0.05Ti0.91	Rh	0.04	Sc	0.05	Ti	0.91																			1964																																														K		1.3					1.3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102139	469		Rh0.24Sc0.76	Rh0.24Sc0.76	Rh	0.24	Sc	0.76																					1965																																														K		0.92					0.92																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102140	35		Rh17S15	Rh17S15	Rh	17	S	15																					1954																															A	9.911													cubic	K		5.8					5.8																																																																																																					Superconducting compounds				Phys.Rev., 93(1954)1415	B.T.Matthias,E.Corenzwit,C.F.Miller		
102141	1060		Rh0.04Ru0.05Ti0.91	Rh0.04Ru0.05Ti0.91	Rh	0.04	Ru	0.05	Ti	0.91																			1964																																														K		3.5					3.5																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102142	427		Re24Zr5	Re24Zr5	Re	24	Zr	5																					1962																																														K		3					3																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102143	173		Re6Zr	Re6Zr1	Re	6	Zr	1																					1961																												alpha-Mn																	alpha-Mn, A12	K		7.4					7.4																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102144	133		Re0.67Zr0.33	Re0.67Zr0.33	Re	0.67	Zr	0.33																					1957																												MgZn2(Laves)																	MgZn2, C14	K		6.8					6.8																																																																																																									CAN.J.PHYS.,35(1957)892	G.K.WHITE,S.B.WOODS		
102145	127		Re0.67Y0.33	Re0.67Y0.33	Re	0.67	Y	0.33																					1959																												MgCu2(Laves)																	MgCu2, C15	K		1.83					1.83																																																																																																									ACTA CRYST.,12(1959)651	B.T.MATTHIAS,V.B.COMPTON		
102146	1438		Re0.5W0.5	Re0.5W0.5	Re	0.5	W	0.5																					1974																																														K		8.1					8.1																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102147	1438		Re0.6W0.4	Re0.6W0.4	Re	0.6	W	0.4																					1974																																														K		9.7					9.7																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102148	1438		Re0.73W0.27	Re0.73W0.27	Re	0.73	W	0.27																					1974																																														K		8.3					8.3																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102149	RMP0350001		Rh3Th7	Rh3Th7	Rh	3	Th	7																					1963																												Fe3Th7																	Fe3Th7, D10[2]	K		2.15					2.15																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102150	469		Rh1Th1	Rh1Th1	Rh	1	Th	1																					1965																																														K		0.36					0.36																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102151	469		Rh5Th1	Rh5Th1	Rh	5	Th	1																					1965																																														K		1.07					1.07																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102152	552		Rh0.67Te0.33	Rh0.67Te0.33	Rh	0.67	Te	0.33																					1965																																														K		0.49					0.49																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102153	033	alpha-type	Rh1Te2	Rh1Te2	Rh	1	Te	2																					1955																												FeS2(pyrite)			A	6.441													FeS2(pyrite), C2	K		1.51					1.51																																																																																																					EMPIRICAL RELATION BETWEEN SUPERCONDUCTIVITY AND THE NUMBER OF VALANCE ELECTRONS PER ATOM				PHYS.REV.,97(1955)74	B.T.MATTHIAS		
102154	1060		Rh0.04Ta0.05Ti0.91	Rh0.04Ta0.05Ti0.91	Rh	0.04	Ta	0.05	Ti	0.91																			1964																																														K		2.3					2.3																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102155	1438		Rh0.33Ta0.66	Rh0.33Ta0.66	Rh	0.33	Ta	0.66																					1974																																														K		7					7																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102156	276		Rh0.4Ta0.6	Rh0.4Ta0.6	Rh	0.4	Ta	0.6																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.35					2.35																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102157	182		Rh1Ta1	Rh1Ta1	Rh	1	Ta	1																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2					2																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102158	28		Rh2Sr1	Rh2Sr1	Rh	2	Sr	1																					1957																												MgCu2(Laves)																	MgCu2, C15	K		6.2					6.2																																																																																																					Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
102159	1377		Rh1Sn2	Rh1Sn2	Rh	1	Sn	2																					1972																												CuAl2																	CuAl2, C16	K		0.6					0.6																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102160	35		Rh0.36Se0.64	Rh0.36Se0.64	Rh	0.36	Se	0.64																					1954																												FeS2(pyrite)																	FeS2(pyrite), C2	K		6					6																																																																																																					Superconducting compounds				Phys.Rev., 93(1954)1415	B.T.Matthias,E.Corenzwit,C.F.Miller		
102161	698		Rh0.02U0.98	Rh0.02U0.98	Rh	0.02	U	0.98																					1966																																														K		0.96					0.96																																																																																																									SCIENCE,152(1966)755	B.T.MATTHIAS,E.S.FISHER,K.ANDRESS,T.F.SMITH,T.H.GEBALLE,W.H.ZACHARIASEN		
102162	1060		Rh0.91Ti0.04Zr0.05	Rh0.91Ti0.04Zr0.05	Rh	0.91	Ti	0.04	Zr	0.05																			1964																																														K		1.8					1.8																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102163	1060		Rh0.91Ti0.04Y0.05	Rh0.91Ti0.04Y0.05	Rh	0.91	Ti	0.04	Y	0.05																			1964																																														K		1.4					1.4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102164	1060		Rh0.91Ti0.4w0.05	Rh0.91Ti0.4W0.05	Rh	0.91	Ti	0.4	W	0.05																			1964																																														K		3.4					3.4																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102165	1060		Rh0.91Ti0.4V0.05	Rh0.91Ti0.4V0.05	Rh	0.91	Ti	0.4	V	0.05																			1964																																														K		2.9					2.9																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102166	1060		Rh0.04Ti0.96	Rh0.04Ti0.96	Rh	0.04	Ti	0.96																					1964																																													cubic	K		2					2																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102167	1071		Rh0.06Ri0.94	Rh0.06Ti0.94	Rh	0.06	Ti	0.94																					1968																																													cubic	K		2.6					2.6																																																																																																									Z.PHYS.,208(1968)238	E.OFTEDAL,G.DUMMER		
102168	1071		Rh0.08Ti0.92	Rh0.08Ti0.92	Rh	0.08	Ti	0.92																					1968																																													cubic	K		3.5					3.5																																																																																																									Z.PHYS.,208(1968)238	E.OFTEDAL,G.DUMMER		
102169	717		Rh0.1Ti0.9	Rh0.1Ti0.9	Rh	0.1	Ti	0.9																					1964																																													cubic	K		4					4																																																																																																					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
102170	717		Rh0.12Ti0.88	Rh0.12Ti0.88	Rh	0.12	Ti	0.88																					1964																																													cubic	K		4					4																																																																																																					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
102171	766		Rh0.88Ti0.12	Rh0.88Ti0.12	Rh	0.88	Ti	0.12																					1963																																													cubic	K		4					4																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
102172	1060		Rh0.91Ti0.09	Rh0.91Ti0.09	Rh	0.91	Ti	0.09																					1964																																														K		2					2																																																																																																									Z.PHYS.,178(1964)216	CH.J.RAUB		
102173	766		Rh1Zr3	Rh1Zr3	Rh	1	Zr	3																					1963																												Fe3W3C																	Fe3W3C, E9[3]	K		11					11																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
102174	1858		Rh0.33Zr0.67	Rh0.33Zr0.67	Rh	0.33	Zr	0.67																					1973																																														K		11.25					11.25																																																																																																									J.LESS-COMMON METALS,33(1973)275	K.TACHIKAWA,K.TOGANO		
102175	1476		Rh1Zr2	Rh1Zr2	Rh	1	Zr	2																					1971																												CuAl2																	CuAl2, C16	K		11.36					11.36	MTC2175																																																																																																								J.LOW TEMP.PHYS.,4(1971)489	S.L.MCCARTHY		
102176	033		Rh0.4Zr0.6	Rh0.4Zr0.6	Rh	0.4	Zr	0.6																					1955																																														K		7					7																																																																																																					EMPIRICAL RELATION BETWEEN SUPERCONDUCTIVITY AND THE NUMBER OF VALANCE ELECTRONS PER ATOM				PHYS.REV.,97(1955)74	B.T.MATTHIAS		
102177	648		Rh1Zr1	Rh1Zr1	Rh	1	Zr	1																					1965																																														K		2.7			1.7		2.7																																																																																																					Superconductivity in zirconium-rhodium alloys				J.PHYS.CHEM.SOLIDS,26(1965)1347	S.T.ZEGLER		
102178	469		Rh1Y3	Rh1Y3	Rh	1	Y	3																					1965																																														K		0.65					0.65																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102179	469		Rh2Y3	Rh2Y3	Rh	2	Y	3																					1965																																														K		1.48					1.48																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102180	469		Rh3Y1	Rh3Y1	Rh	3	Y	1																					1965																												MgCu2(Laves)			A	7.424													MgCu2, C15	K		1.07					1.07																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102181	469		Rh5Y1	Rh5Y1	Rh	5	Y	1																					1965																																														K		0.56					0.56																																																																																																					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102182	1438		Rh0.3W0.7	Rh0.3W0.7	Rh	0.3	W	0.7																					1974																																														K		7.3					7.3																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102183	33		Rh1W1	Rh1W1	Rh	1	W	1																					1955																																													hexagonal	K		3.37					3.37																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
102184	1496		Rh0.35V0.65	Rh0.35V0.65	Rh	0.35	V	0.65																					1973																																														K		1.075					1.075																																																																																																									J.LOW TEMP.PHYS.A,46(1973)21	J.E.COX,R.M.WATERSTRAT		
102185	1930		Ru0.46V0.54	Ru0.46V0.54	Ru	0.46	V	0.54																					1971																												CsCl																	CsCl, B2	K		5					5																																																																																																									PHYS.REV.B,4(1971)320	A.S.COOPER,C.W.CHU,E.BUCHER,J.P.MAITA		
102186	RMP0350001		Ru1Ti1	Ru1Ti1	Ru	1	Ti	1																					1963																												CsCl																	CsCl, B2	K		1.07					1.07																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102187	173		Ru2Th1	Ru2Th1	Ru	2	Th	1																					1961																												MgCu2(Laves)																	MgCu2, C15	K		3.56					3.56																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102188	1026		Ru2Sc1	Ru2Sc1	Ru	2	Sc	1																					1970																												MgZn2(Laves)																	MgZn2, C14	K		2.24					2.24																																																																																																									PHYS.LETT.A,33(1970)61	B.HILLENBRAND,M.WILLHELM		
102189	816		Ru1	Ru1	Ru	1																							1962																												Mg																	Mg, A3	K		0.493					0.493																																																																																																									ZH.EKSP.TEOR.FIZ.,43(1962)2309	A.A.MATSAKOVA,B.G.LAZAREV,L.S.LAZAREVA,O.N.OVCHARENKO		
102190	1438		Rh0.25Zr0.75	Rh0.25Zr0.75	Rh	0.25	Zr	0.75																					1974																																														K		11.4					11.4																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102191	1438		Rh0.33zr0.66	Rh0.33Zr0.66	Rh	0.33	Zr	0.66																					1974																																														K		11.2					11.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102192	1061	as-cast sample	Rh0.03Zr0.97	Rh0.03Zr0.97	Rh	0.03	Zr	0.97																					1965																																														K		10.4					10.4																																																																																																					Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
102193	766		Rh0.12Zr0.88	Rh0.12Zr0.88	Rh	0.12	Zr	0.88																					1963																															A	3.54													cubic	K		11					11																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
102194	1858		Rh0.14Zr0.86	Rh0.14Zr0.86	Rh	0.14	Zr	0.86																					1973																																														K		11.1					11.1																																																																																																									J.LESS-COMMON METALS,33(1973)275	K.TACHIKAWA,K.TOGANO		
102195	033		Rh0.14Zr0.86	Rh0.14Zr0.86	Rh	0.14	Zr	0.86																					1955																																													hexagonal	K		9.5					9.5																																																																																																					EMPIRICAL RELATION BETWEEN SUPERCONDUCTIVITY AND THE NUMBER OF VALANCE ELECTRONS PER ATOM				PHYS.REV.,97(1955)74	B.T.MATTHIAS		
102196	033		Rh0.17Zr0.83	Rh0.17Zr0.83	Rh	0.17	Zr	0.83																					1955																																														K		9.6					9.6																																																																																																					EMPIRICAL RELATION BETWEEN SUPERCONDUCTIVITY AND THE NUMBER OF VALANCE ELECTRONS PER ATOM				PHYS.REV.,97(1955)74	B.T.MATTHIAS		
102197	1262	Hc2 for H//layer at 2.34 K. For H normal to layer, Hc2(2.34K) = 12.8 kOe.	S1.2Se0.8Ta1	S1.2Se0.8Ta1	S	1.2	Se	0.8	Ta	1																			1973																																														K		3.9					3.9																				kOe	resistive, linear					92.1	12.8	2.34																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
102198	32		Ru0.1Zr0.9	Ru0.1Zr0.9	Ru	0.1	Zr	0.9																					1955																																													hexagonal	K		5.7					5.7																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102199	1478		Ru2Zr1	Ru2Zr1	Ru	2	Zr	1																					1971																												MgZn2(Laves)																	MgZn2, C14	K		2.4					2.4																																																																																																									J.LOW TEMP.PHYS.,4(1971)669	S.L.MCCARTHY		
102200	1026		Ru2Y1	Ru2Y1	Ru	2	Y	1																					1970																												MgZn2(Laves)																	MgZn2, C14	K		2.42					2.42																																																																																																									PHYS.LETT.A,33(1970)61	B.HILLENBRAND,M.WILLHELM		
102201	1438		Ru0.4W0.6	Ru0.4W0.6	Ru	0.4	W	0.6																					1974																																														K		5					5																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102202	1438		Ru0.5W0.5	Ru0.5W0.5	Ru	0.5	W	0.5																					1974																																														K		5.7					5.7																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102203	276		Ru0.4W0.6	Ru0.4W0.6	Ru	0.4	W	0.6																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.67					4.67																																																																																																									HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102204	33		Ru1W1	Ru1W1	Ru	1	W	1																					1955																																														K		7.5					7.5																																																																																																					Empirical Relation between Superconductivity and the Number of Valence Electrons per Atom				Phys.Rev.,97(1955)74	B.T.Matthias		
102205	182		Ru0.58W0.42	Ru0.58W0.42	Ru	0.58	W	0.42																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K		5.2					5.2																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)134	J.K.HULM,R.D.BLAUGHER		
102206	119		Ru0.4V0.6	Ru0.4V0.6	Ru	0.4	V	0.6																					1948																																														K		1					1																																																																																																					From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102207	572		Ru0.45V0.55	Ru0.45V0.55	Ru	0.45	V	0.55																					1966																												CsCl																	CsCl, B2	K		4					4																																																																																																									PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102208	1119		Ru0.452V0.548	Ru0.452V0.548	Ru	0.452	V	0.548																					1971																																														K		4.2					4.2																																																																																																									PHYS.LETT.A,35(1971)117	L.R.TESTARDI		
102209	1917	weight fraction 	Sb0.05Sn0.95	Sb0.05Sn0.95	Sb	0.05	Sn	0.95																					1969																																														K		3.75					3.75																																																																																																									REV.SCI.INSTRUMENTS,40(1969)180	W.G.BADER,W.H.WARREN JR.		
102210	85		Sb0.4Sn0.6	Sb0.4Sn0.6	Sb	0.4	Sn	0.6																					1932																																														K		3.8					3.8																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
102211	1542		Sb1Sn1	Sb1Sn1	Sb	1	Sn	1																					1971																												NaCl																	NaCl, B1	K		1.56					1.56																																																																																																									PHYSICA,55(1971)60	J.K.HULM,M.S.WALKER,N.PESSALL		
102212	1829	rapid quench 	Sb0.7Sn0.3	Sb0.7Sn0.3	Sb	0.7	Sn	0.3																					1974																																													cubic	K		2.85					2.85																																																																																																									J.SPPL.PHYS.,45(1974)3683	S.J.POON,W.L.JOHNSON		
102213	1659		S1.1Zr1	S1.1Zr1	S	1.1	Zr	1																					1972																												NaCl																	NaCl, B1	K		4.5					4.5																																																																																																									PHYS.LETT.A,41(1972)447	A.MOODENBAUGH,D.C.JOHNSTON		
102214	1219		S1Y1	S1Y1	S	1	Y	1																					1970																												NaCl																	NaCl, B1	K		1.9					1.9																																																																																																									SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102215	797		S2Ta1	S2Ta1	S	2	Ta	1																					1967																																														K		0.8					0.8																																																																																																									PHYS.LETT.A,24(1967)645	G.M.SCHSRFFER,M.H.VAN MAAREN		
102216	796		S2Ta1	S2Ta1	S	2	Ta	1																					1969																																													hexagonal	K		1.6					1.6																																																																																																									PHYS.LETT.A,29(1969)571	H.B.HARLAND,M.H.VAN MAAREN		
102217	1918		S2Ta1	S2Ta1	S	2	Ta	1																					1974																																													hexagonal	K		0.8					0.8																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
102218	1150		S3Sn1Ta1	S3Sn1Ta1	S	3	Sn	1	Ta	1																			1972																																													tetragonal	K		2.96					2.96																																																																																																									PHYS.LETT.A,40(1972)353	M.H.VAN MAAREN		
102219	1262	Hc2 for H//layer at 2.9 K. For H normal to layer, Hc2(2.9K) = 6.7 kOe.	S0.8Se1.2Ta1	S0.8Se1.2Ta1	S	0.8	Se	1.2	Ta	1																			1973																												TX2																	2H-TaS2 phase	K		3.9					3.9																				kOe	resistive, linear approx.					45	6.7	2.9																																																																									Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
102220	1262	Hc2 for H//layer at 2.2 K. For H normal to layer, Hc2(2.2K)=11.0 kOe.	S1Se1Ta1	S1Se1Ta1	S	1	Se	1	Ta	1																			1973																												TX2																	2H-TaS2 phase	K		3.7					3.7																				kOe	resistive, linear approx.					73.8	11	2.2						MHC102220																																																																			Anisotropic superconductivity in layer compounds				PHYS.REV.B,7(1973)991	R.C.MORRIS,R.V.COLEMAN		
102221	744		Sc0.01Zr0.99	Sc0.01Zr0.99	Sc	0.01	Zr	0.99																					1966																																														K		0.32					0.32																																																																																																					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102222	744		Sc0.05Zr0.95	Sc0.05Zr0.95	Sc	0.05	Zr	0.95																					1966																																														K		0.11					0.11																																																								mj/mol.K2	2.5		311																																					arc-melting 					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102223	744		Sc0.07Zr0.93	Sc0.07Zr0.93	Sc	0.07	Zr	0.93																					1966																																														K		0.08					0.08																																																																																																					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102224	RMP0350001		Sb2Zr3	Sb2Zr3	Sb	2	Zr	3																					1963																																														K		1.74					1.74																																																																																																					Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102225	514		Sb0.03V0.97	Sb0.03V0.97	Sb	0.03	V	0.97																					1964																												W																	W, A2	K		2.63					2.63																																																								mj/mol.K2	7.96		346																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
102226	578		Sb1V3	Sb1V3	Sb	1	V	3																					1960																												Cr3Si(A15)																	Cr3Si, A15	K		0.8					0.8																																																																																																					CORRELATIONS BETWEEN SUPERCONDUCTIVITY AND NUCLEAR MAGNETIC RESONANCE PROPERTIES				PHYS.REV.LETT.,5(1960)149	B.T.MATTHIAS,J.EISINGER,V.JACCARINO,W.E.BLUMBERG		
102227	111		Sb0.28Tl0.72	Sb0.28Tl0.72	Sb	0.28	Tl	0.72																					1930																																														K		5.2					5.2																																																																																																									ROY.SOC.CAN.TRANS.,24(1930)53	J.C.MCLENNAN,J.O.WILHELM,L.F.ALLEN		
102228	85		Sb0.66Tl0.33	Sb0.66Tl0.33	Sb	0.66	Tl	0.33																					1932																																														K		5.2					5.2																																																																																																					From Roberts' Table				Z.Elektrochem., 38(1932)312	K.Clusius		
102229	1438		Sb0.25Ti0.75	Sb0.25Ti0.75	Sb	0.25	Ti	0.75																					1974																																														K		7.2					7.2																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102230	1002		Sb1Ti3	Sb1Ti3	Sb	1	Ti	3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		5.47					5.47																																																																																																					Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
102231	1015		Sb1Ta3	Sb1Ta3	Sb	1	Ta	3																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		0.72					0.72																																																																																																									Z.PHYS.,230(1970)443	E.CORENZWIT,E.VIELHABER,H.L.LUO		
102232	1724		Sb0.011Sn0.989	Sb0.011Sn0.989	Sb	0.011	Sn	0.989																					1964																																														K		3.642					3.642																																																																																																									J.PHYS.(PARIS),25(1964)374	G.CHOL		
102233	880		Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.86					16.86																																																																																																									J.LOW TEMP.PHYS.,1(1969)29	E.SAUR,G.HORN,G.OTTO,K.HECHLER		
102234	1073		Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.95					16.95																																																																																																									Z.PHYS.,218(1969)52	G.OTTO		
102235	707		Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		17					17																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102236	10		Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																					1954																												Cr3Si(A15)																	Cr3Si, A15	K		17.1					17.1																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102237	32		Si0.263V0.737	Si0.263V0.737	Si	0.263	V	0.737																					1955																												Cr3Si(A15)																	Cr3Si, A15	K		15.8					15.8																																																																																																					Superconductivity of zirconium alloys				Phys.Rev., 100(1955)626	B.T.Matthias,E.Corenzwit		
102238	707		Si0.3V0.7	Si0.3V0.7	Si	0.3	V	0.7																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.95					16.95																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102239	1976		Si1Ti0.15V2.85	Si1Ti0.15V2.85	Si	1	Ti	0.15	V	2.85																			1971																																														K		14.55					14.55																																																																																																									ANN.CHEM.,6(1971)309	J.HALLAIS		
102240	10		Si2Th1	Si2Th1	Si	2	Th	1																					1954																												AlB2																	AlB2, C32	K		2.41					2.41																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102241	10		Si2Th1	Si2Th1	Si	2	Th	1																					1954																												ThSi2																	ThSi2, C[c]	K		3.16					3.16																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102242	961		Si3Sr2	Si3Sr2	Si	3	Sr	2																					1967																												ThSi2																	ThSi2, C[c]	K		0.55					0.55																																																																																																									J.LESS-COMMON METALS,12(1967)75	D.B.MCWHAN,J.R.SOULEN,M.S.SILVERMAN,V.B.COMPTON		
102243	1219		Se1Y1	Se1Y1	Se	1	Y	1																					1970																												NaCl																	NaCl, B1	K		2.5					2.5																																																																																																									SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102244	711		Se4Nb3	Nb3Se4	Nb	3	Se	4																																																																			K		1.61					1.61																																																																																																					From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102245	1829	rapid quench 	Sn0.35Ye0.65	Sn0.35Te0.65	Sn	0.35	Te	0.65																					1974																																													cubic	K		1.9					1.9																																																																																																									J.SPPL.PHYS.,45(1974)3683	S.J.POON,W.L.JOHNSON		
102246	473		Sn0.25Ta0.5V0.25	Sn0.25Ta0.5V0.25	Sn	0.25	Ta	0.5	V	0.25																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		3.7					3.7																																																																																																									RCA REV.,25(1964)338-341	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
102247	185		Sn0.25Ta0.25V0.5	Sn0.25Ta0.25V0.5	Sn	0.25	Ta	0.25	V	0.5																			1960																												Cr3Si(A15)																	Cr3Si, A15	K		2.8					2.8																																																																																																					LT7 (Toronto), 1960 p382				REF.,176 382	F.D.ROSI,G.D.CODY,G.T.MCCONVILLE,J.J.HANAK		
102248	1446		Sn1Ta3	Sn1Ta3	Sn	1	Ta	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.4					6.4																																																																																																									J.LOW TEMP.PHYS.,6(1972)171	T.F.SMITH		
102249	581	low ordered state	Sn1Ta3	Sn1Ta3	Sn	1	Ta	3																					1965																												Cr3Si(A15)			A	5.2772													Cr3Si, A15	K		6.2					6.2																				kG		15.5																																																																										sintering (1450C, 1h) 					Effect of processing on the superconducting properties and long-range order of Ta3Sn				J.APPL.PHYS.,36(1965)3256	G.W.PEARSALL,J.WULFF,T.H.COURTNEY		
102250	581		Sn1Ta3	Sn1Ta3	Sn	1	Ta	3																					1965																												Cr3Si(A15)			A	5.2801													Cr3Si, A15	K		8.35					8.35																				kG		72.5																																																																										sintering (900C, 4h) 					Effect of processing on the superconducting properties and long-range order of Ta3Sn				J.APPL.PHYS.,36(1965)3256	G.W.PEARSALL,J.WULFF,T.H.COURTNEY		
102251	10		Si0.4W0.6	Si0.4W0.6	Si	0.4	W	0.6																					1954																																														K		2.84					2.84																																																																																																					The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102252	144		Si0.22V0.78	Si0.22V0.78	Si	0.22	V	0.78																					1959																												Cr3Si(A15)																	Cr3Si, A15	K		14.38					14.38																																																																																																									ZH.EKSP.TEOR.FIZ.,37(1959)1461	A.I.SUDOVTSOV,B.G.LAZAREV,E.E.SEMENENKO		
102253	707		Si0.2V0.8	Si0.2V0.8	Si	0.2	V	0.8																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		7.51					7.51																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102254	323		Si0.206V0.794	Si0.206V0.794	Si	0.206	V	0.794																					1962																												Cr3Si(A15)																	Cr3Si, A15	K		14.5					14.5																																																																																																									DOK.AKAD.NAUK(CCCP),145(1962)82	E.M.SAVISKY,N.E.ALEKSEEVSKII,V.V.BARON,YU.V.EFIMOV		
102255	1933	dTc/dP = 3.7 E-5 K/bar.	Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																				3	1974																												Cr3Si(A15)																	Cr3Si, A15	K		16.6					16.6			K/GPa	0.37																																																																																																	Effect of lattice transformation on the pressure dependence of Tc of V3Si single crystals				PHYS.REV.B,10(1974)4030	C.W.CHU,S.HUANG		
102256	707		Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		16.65					16.65																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102257	1652		Ta0.05V2Zr0.95	Ta0.05V2Zr0.95	Ta	0.05	V	2	Zr	0.95																			1974																																														K		8.9					8.9																																																																																																									PHYS.LETT.A,47(1974)209	H.HAYASHI,T.TAKASHIMA		
102258	572		Ta0.25V0.75	Ta0.25V0.75	Ta	0.25	V	0.75																					1966																												W																	W, A2	K		2.8					2.8																																																																																																									PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102259	572		Ta0.5V0.5	Ta0.5V0.5	Ta	0.5	V	0.5																					1966																												W																	W, A2	K		2.35					2.35																																																																																																									PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102260	572		Ta0.75V0.25	Ta0.75V0.25	Ta	0.75	V	0.25																					1966																												W																	W, A2	K		2.65					2.65																																																																																																									PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102261	874		Ta0.52Ti0.48	Ta0.52Ti0.48	Ta	0.52	Ti	0.48																					1966																																														K		7.86					7.86																																																																																																									PHYS.REV.LETT.,17(1966)81	L.J.NEURINGER,Y.SHAPIRA		
102262	713		Ta1	Ta1	Ta	1																							1970																												W																	W, A2	K		4.463					4.463																																																																																																					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
102263	1015		Sn1Zr4	Sn1Zr4	Sn	1	Zr	4																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		0.92					0.92																																																																																																									Z.PHYS.,230(1970)443	E.CORENZWIT,E.VIELHABER,H.L.LUO		
102264	726	laminar period study 	Sn0.91Zn0.09	Sn0.91Zn0.09	Sn	0.91	Zn	0.09																					1966																																														K		3.722					3.722																																																																																																									PHYS.REV.,145(1966)218	D.A.CLAYTON,O.S.LUTES		
102265	128		Sn1V3	Sn1V3	Sn	1	V	3																					1956																												Cr3Si(A15)																	Cr3Si, A15	K		7					7																																																																																																									J.PHYS.CHEM.SOLIDS.,1(1956)188	B.T.MATTIAS,E.A.WOOD,E.CORENZWIT,V.B.BALA		
102266	1369		Sn1V3	Sn1V3	Sn	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.8					3.8																																																																																																									METALL.,26(1972)29	CH.J.RAUB,E.ROSCHEL		
102267	715		Sn3Th1	Sn3Th1	Sn	3	Th	1																					1970																												AuCu3																	AuCu3, L1[2]	K		3.33					3.33																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102268	1829	rapid quench 	Sn0.25Te0.75	Sn0.25Te0.75	Sn	0.25	Te	0.75																					1974																																													cubic	K		1.7					1.7																																																																																																									J.SPPL.PHYS.,45(1974)3683	S.J.POON,W.L.JOHNSON		
102269	1138		Tc0.1V0.9	Tc0.1V0.9	Tc	0.1	V	0.9																					1967																																														K		1.5					1.5																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102270	1138		Tc0.6V0.4	Tc0.6V0.4	Tc	0.6	V	0.4																					1967																																														K		4.17					4.17																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102271	1138		Tc0.65V0.35	Tc0.65V0.35	Tc	0.65	V	0.35																					1967																																														K		4.49					4.49																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102272	1138	quick cool	Tc0.7V0.3	Tc0.7V0.3	Tc	0.7	V	0.3																					1967																																														K		6.41					6.41																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102273	1791		Tc0.7V0.3	Tc0.7V0.3	Tc	0.7	V	0.3																					1969																																														K		8.3					8.3																																																																																																									TRANS.MET.SOC.AIME,245(1969)1957	C.C.KOCH,G.R.LOVE		
102274	1138		Tc0.75V0.25	Tc0.75V0.25	Tc	0.75	V	0.25																					1967																																														K		11.07					11.07																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102275	1138		Tc0.8V0.2	Tc0.8V0.2	Tc	0.8	V	0.2																					1967																																														K		11.24					11.24																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102276	1138		Tc0.9V0.1	Tc0.9V0.1	Tc	0.9	V	0.1																					1967																																														K		11.32					11.32																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102277	1138		Tc0.95V0.05	Tc0.95V0.05	Tc	0.95	V	0.05																					1967																																														K		10.99					10.99																																																																																																					Superconductivity in the Technetium-Vanadium Alloy System				J.APPL.PHYS.,38(1967)4359	C.C.KOCH,R.H.KERNOHAN,S.T.SEKULA		
102278	1149		Tc0.44Th0.56	Tc0.44Th0.56	Tc	0.44	Th	0.56																					1970																												MgZn2(Laves)			A	5.393		9.223											MgZn2, C14	K		5.3					5.3																																																																																																									J.LESS-COMMON METALS,22(1970)246	A.L.GIORGI,E.G.SZKLARZ		
102279	1180		Tc1	Tc1	Tc	1																							1971																																														K		7.46					7.46																																																																																																					From Roberts' Table.				LT-12(1971)341	G.Kostorz,S.Mihailovich		
102280	1790		Ta0.96Zr0.04	Ta0.96Zr0.04	Ta	0.96	Zr	0.04																					1969																																														K		5.7					5.7																																																																																																									TRANS.MET.SOC.AIME,245(1969)1953	H.C.GATOS,J.T.A.POLLACK		
102281	499		Ti0.975V0.025	Ti0.975V0.025	Ti	0.975	V	0.025																					1965																																													hexagonal	K		1.4					1.4																																																																																																					SUPERCONDUCTIVITY OF ALPH-TITANIUM SOLID SOLUTIONS WITH VANADIUM,NIOBIUM,AND TANTALUM				PHYS.REV.,137(1965)A142	CH.J.RAUB,U.ZWICKER		
102282	253		Ti1	Ti1	Ti	1																							1961																												Mg																	Mg, A3	K		0.4					0.4																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102283	1377		Th2Zn1	Th2Zn1	Th	2	Zn	1																					1972																												CuAl2																	CuAl2, C16	K		0.67					0.67																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102284	234		Th0.5Y0.5	Th0.5Y0.5	Th	0.5	Y	0.5																					1961																																														K		1.25					1.25																																																																																																									RARE EARTH RESEARCH E.V.KLEBER ED.,(1961)158	B.T.MATTHIAS,K.A.GSCHNEIDER JR.		
102285	1227		Th1U0.001	Th1U0.001	Th	1	U	0.001																					1972																																														K		0.785					0.785																																																																																																									SOLID STATE COMMUN.,10(1972)459	C.A.LUENGO,J.G.SERENI,J.M.COTIGNOLA		
102286	715		Th1Tl3	Th1Tl3	Th	1	Tl	3																					1970																												AuCu3																	AuCu3, L1[2]	K		0.87					0.87																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102287	1123		Th1	Th1	Th	1																							1967																												Cu																	Cu, A1	K		1.39					1.39																																																																																																									PHYS.REV.LETT.,18(1967)899	D.K.FINNEMORE,D.T.PETERSON,W.R.DECKER		
102288	1219		Te1Y1	Te1Y1	Te	1	Y	1																					1970																												NaCl			A	6.093													NaCl, B1	K		2.05					2.05																																																																																																									SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102289	848		Te3Tl5	Te3Tl5	Te	3	Tl	5																					1968																																														K		2.078					2.078																																																																																																					Electrical conductivity and superconductivity in the gamma-phase of the Tl-Te system				J.APPL.PHYS.,39(1968)3003	A.JUODAKIS,C.R.KANNEWURF		
102290	1149	chemical analysis: Zr0.332Tc0.668	Tc2Zr1	Tc2Zr1	Tc	2	Zr	1																					1970																												MgZn2(Laves)			A	5.2185		8.6527											MgZn2, C14	K		7.6					7.6																																																																																																									J.LESS-COMMON METALS,22(1970)246	A.L.GIORGI,E.G.SZKLARZ		
102291	202		Tc6Zr1	Tc6Zr1	Tc	6	Zr	1																					1961																												alpha-Mn																	alpha-Mn, A12	K		9.7					9.7																																																																																																					SUPERCONDUCTIVITY OF TECHNETIUM ALLOYS AND COMPOUNDS				PHYS.REV.,123(1961)1567	B.T.MATTHIAS,E.CORENZWIT,F.J.MORIN,J.P.MAITA,V.B.COMPTON		
102292	1337		Tc0.9W0.1	Tc0.9W0.1	Tc	0.9	W	0.1																					1966																																														K		10.4					10.4																																																																																																									BULL.L'ACAD.POLONAISE DES SCI.,14(1966)565	E.TROJNAR,J.NIEMIEC		
102293	1956		Ti0.013V0.987	Ti0.013V0.987	Ti	0.013	V	0.987																					1974																																														K		12.8					12.8																																																																																																					From Roberts' Table.				LT-13(1974)485	H.J.Spitzer		
102294	874		Ti0.42V0.58	Ti0.42V0.58	Ti	0.42	V	0.58																					1966																																														K		7.52					7.52																																																																																																									PHYS.REV.LETT.,17(1966)81	L.J.NEURINGER,Y.SHAPIRA		
102295	466		Ti1V1	Ti1V1	Ti	1	V	1																					1963																																														K		6.09					6.09																																																																																																					SUPERCONDUCTIVITY AT HIGH MAGNETIC FIELDS				PHYS.REV.,131(1963)140	R.R.HAKE,T.G.BERLINCOURT		
102296	600		Ti0.516V0.484	Ti0.516V0.484	Ti	0.516	V	0.484																					1965																																														K		7.2					7.2																																																								mj/mol.K2	9.2		386																																														PHYS.LETT.,14(1965)181	R.D.BLAUGHER		
102297	878		Ti0.6V0.4	Ti0.6V0.4	Ti	0.6	V	0.4																					1967																																														K		7					7																																																																																																									PHYS.LETT.A,24(1967)663	E.MAXWELL,W.H.HACKETT JR.,Y.B.KIM		
102298	600		Ti0.615V0.385	Ti0.615V0.385	Ti	0.615	V	0.385																					1965																																														K		7.07					7.07																																																																																																									PHYS.LETT.,14(1965)181	R.D.BLAUGHER		
102299	514		Ti0.7V0.3	Ti0.7V0.3	Ti	0.7	V	0.3																					1964																																														K		6.14					6.14																																																								mj/mol.K2	10.1		244																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
102300	584		Ti0.75V0.25	Ti0.75V0.25	Ti	0.75	V	0.25																					1967																																														K		5.3					5.3																																																																																																					PARAMAGNETIC SUPERCONDUCTIVITY IN EXTREME TYPE-II SUPERCONDUCTORS				PHYS.REV.,158(1967)356	R.R.HAKE		
102301	1861		Ti0.76V0.24	Ti0.76V0.24	Ti	0.76	V	0.24																					1971																																														K		4.382					4.382																																																																																																									SCRIPTA METALLURGICA,5(1971)81	D.H.POLONIS,R.TAGGART,T.S.LUHMAN		
102302	584		Ti0.775V0.225	Ti0.775V0.225	Ti	0.775	V	0.225																					1967																																														K		4.7					4.7																																																																																																					PARAMAGNETIC SUPERCONDUCTIVITY IN EXTREME TYPE-II SUPERCONDUCTORS				PHYS.REV.,158(1967)356	R.R.HAKE		
102303	253		Ti0.9V0.1	Ti0.9V0.1	Ti	0.9	V	0.1																					1961																																														K		6.3					6.3																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102304	477		Ti0.96V0.04	Ti0.96V0.04	Ti	0.96	V	0.04																					1965																																														K		2.7					2.7																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
102305	641	1900,25-48 KBAR	Tl	Tl1	Tl	1																							1966																																														K		1.38					1.38																																																																																																					Influence of lattice structure on superconductivity in thallium				SOLID STATE COMMUN.,4(1966)403	W.GEY		
102306	641	high pressure phase (P>35 kbar). Tc is at 35 kbar.	fcc-Tl	Tl1	Tl	1																							1966																												Cu																	Cu, A1	K		1.45					1.45			K/GPa	-0.085																																																							88																																										Influence of lattice structure on superconductivity in thallium				SOLID STATE COMMUN.,4(1966)403	W.GEY		
102307	641	hcp-Tl (0 < P < 35 KBAR). Tc(P=35kbar) = 1.95 K.	hcp-Tl	Tl1	Tl	1																							1966																												Mg																	Mg, A3	K		2.4					2.4			K/GPa	-0.15																																																							99																																										Influence of lattice structure on superconductivity in thallium				SOLID STATE COMMUN.,4(1966)403	W.GEY		
102308	1378		Tl1	Tl1	Tl	1																							1964																												W																	W, A2	K		2.332					2.332																																																																																																					From Roberts' Table. Master's thesis , Univ. of Illinois				unpublished	W.O.Gentry		
102309	527		Tl1	Tl1	Tl	1																							1964																												Mg																	Mg, A3	K		2.38					2.38																																																																																																					SPECIFIC HEAT OF MERCURY AND THALLIUM BETWEEN 0.35 AND 4.2K				PHYS.REV.,135(1964)A631	B.J.C.VAN DER HOEVEN,JR.,P.H.KEESOM		
102310	253		Ti0.81Zr0.82	Ti0.81Zr0.82	Ti	0.81	Zr	0.82																					1961																																													hexagonal	K		1.03					1.03																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102311	253		Ti0.33Zr0.66	Ti0.33Zr0.66	Ti	0.33	Zr	0.66																					1961																																													hexagonal	K		1.35					1.35																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102312	1061		Ti0.5Zr0.5	Ti0.5Zr0.5	Ti	0.5	Zr	0.5																					1965																																														K		1.65					1.65																																																																																																					Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
102313	477		Ti0.5Zr0.5	Ti0.5Zr0.5	Ti	0.5	Zr	0.5																					1965																																														K		1.23					1.23																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
102314	253		Ti0.66Zr0.33	Ti0.66Zr0.33	Ti	0.66	Zr	0.33																					1961																																													hexagonal	K		1.36					1.36																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102315	1438		Ti0.17V0.5Zr0.33	Ti0.17V0.5Zr0.33	Ti	0.17	V	0.5	Zr	0.33																			1974																																														K		7.6					7.6																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102316	1438		Ti0.33V0.33Zr0.33	Ti0.33V0.33Zr0.33	Ti	0.33	V	0.33	Zr	0.33																			1974																																														K		6.6					6.6																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102317	584		Ti0.75V0.25	Ti0.75V0.25	Ti	0.75	V	0.25																					1967																																														K		5.3					5.3																																																																																																					PARAMAGNETIC SUPERCONDUCTIVITY IN EXTREME TYPE-II SUPERCONDUCTORS				PHYS.REV.,158(1967)356	R.R.HAKE		
102318	1861		Ti0.76V0.24	Ti0.76V0.24	Ti	0.76	V	0.24																					1971																																														K		4.382					4.382																																																																																																									SCRIPTA METALLURGICA,5(1971)81	D.H.POLONIS,R.TAGGART,T.S.LUHMAN		
102319	584		Ti0.775V0.225	Ti0.775V0.225	Ti	0.775	V	0.225																					1967																																														K		4.7					4.7																																																																																																					PARAMAGNETIC SUPERCONDUCTIVITY IN EXTREME TYPE-II SUPERCONDUCTORS				PHYS.REV.,158(1967)356	R.R.HAKE		
102320	253		Ti0.9V0.1	Ti0.9V0.1	Ti	0.9	V	0.1																					1961																																														K		6.3					6.3																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102321	477		Ti0.96V0.04	Ti0.96V0.04	Ti	0.96	V	0.04																					1965																																														K		2.7					2.7																																																																																																									LT-9(1965) 482-486	E.Bucher,F.Heininger,J.Muller		
102322	499		Ti0.975V0.025	Ti0.975V0.025	Ti	0.975	V	0.025																					1965																																													hexagonal	K		1.4					1.4																																																																																																					SUPERCONDUCTIVITY OF ALPH-TITANIUM SOLID SOLUTIONS WITH VANADIUM,NIOBIUM,AND TANTALUM				PHYS.REV.,137(1965)A142	CH.J.RAUB,U.ZWICKER		
102323	21		Ti1U2	Ti1U2	Ti	1	U	2																					1958																												AlB2																	AlB2, C32	K					1.06																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
102324	980		Ti4Tl1	Ti4Tl1	Ti	4	Tl	1																					1967																												Cr3Si(A15)																	Cr3Si, A15	K					0.35																																																																																																											SOLID STATE COMMUN.,5(1967)221	E.VIELHABER,H.L.LUO		
102325	253		Ti1	Ti1	Ti	1																							1961																												Mg																	Mg, A3	K		0.4					0.4																																																																																																					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102326	1377		Th2Zn1	Th2Zn1	Th	2	Zn	1																					1972																												CuAl2																	CuAl2, C16	K		0.67					0.67																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102327	234		Th0.5Y0.5	Th0.5Y0.5	Th	0.5	Y	0.5																					1961																																														K		1.25					1.25																																																																																																									RARE EARTH RESEARCH E.V.KLEBER ED.,(1961)158	B.T.MATTHIAS,K.A.GSCHNEIDER JR.		
102328	1227		Th1U0.001	Th1U0.001	Th	1	U	0.001																					1972																																														K		0.785					0.785																																																																																																									SOLID STATE COMMUN.,10(1972)459	C.A.LUENGO,J.G.SERENI,J.M.COTIGNOLA		
102329	889		V0.4Zr0.6	V0.4Zr0.6	V	0.4	Zr	0.6																					1968																																														K		7.8					7.8	MTC102329																																	MHC102329																																																														arc-melting					Upper critical field of Zr-V alloys			Nihon University	Jpn J.Appl.Phys., 7(1968)1128	K.Yasohama,N.Usui		
102330	889		V0.6Zr0.4	V0.6Zr0.4	V	0.6	Zr	0.4																					1968																																														K		8.3					8.3																																																																																																arc-melting					Upper critical field of Zr-V alloys			Nihon University	Jpn J.Appl.Phys., 7(1968)1128	K.Yasohama,N.Usui		
102331	173		V2Zr1	V2Zr1	V	2	Zr	1																					1961																												MgCu2(Laves)																	MgCu2, C15	K		9					9																																																																																																									J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102332	1323		V2Zr1	V2Zr1	V	2	Zr	1																					1973																																													orthorhombic	K		8.5					8.5																																																																																																									JAPAN J.APPL.PHYS.,12(1973)161	K.INOUE,K.TACHIKAWA		
102333	1189		V0.7Zr0.3	V0.7Zr0.3	V	0.7	Zr	0.3																					1970																												MgCu2(Laves)																	MgCu2, C15	K		8.6					8.6																																																																																																					LT-12				LT-12 (1970, Kyoto) p 483	K. INQUE,K.TACHIKAWA		
102334	RMP0350001		V1Zr3	V1Zr3	V	1	Zr	3																					1963																												AuCu3																	AuCu3, L1[2]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102335	RMP0350001		Tm1	Tm1	Tm	1																							1963																												Mg																	Mg, A3	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102336	980		Tl1Zr4	Tl1Zr4	Tl	1	Zr	4																					1967																												Cr3Si(A15)																	Cr3Si, A15	K					0.35																																																																																																											SOLID STATE COMMUN.,5(1967)221	E.VIELHABER,H.L.LUO		
102337	715		Tl3Y1	Tl3Y1	Tl	3	Y	1																					1970																												AuCu3																	AuCu3, L1[2]	K		1.52					1.52																																																																																																									J.PHYS.CHEM.SOLIDS,31(1970)2653	E.E.HAVINGA,H.DAMSMA,M.H.VAN MAAREN		
102338	825		Tl1V3	Tl1V3	Tl	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K					4.2																																																																																																											DOKL.AN SSR,171(1966)331	E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
102339	600		Ti0.615V0.385	Ti0.615V0.385	Ti	0.615	V	0.385																					1965																																														K		7.07					7.07																																																								mj/mol.K2	7.1		395																																														PHYS.LETT.,14(1965)181	R.D.BLAUGHER		
102340	514		Ti0.7V0.3	Ti0.7V0.3	Ti	0.7	V	0.3																					1964																																														K		6.14					6.14																																																																																																					Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
102341	258		K1Na2	K1Na2	K	1	Na	2																																																																			K					1.05																																																																																																							From Roberts' Table, unpublished results				Unpublished results	M.F.Merriam		
102342	1920		Cs0.3Mo1S2	Cs0.3Mo1S2	Cs	0.3	Mo	1	S	2																			1973																												2H-MoS2			A			19.606											hexagonal	K		6.3					6.3																																																																																																					Alkali metal intercalates of molybdenum disulfide				J.CHEM.PHYS.,58(1973)697	A.REMBAUM,R.B.SOMOANO,V.HADEK		
102343	741	Ta impurity	Zn2Zr1	Zn2Zr1	Zn	2	Zr	1																					1966																												MgCu2(Laves)																	MgCu2, C15	K					0.1																																																																																																											PHYS.REV.,148(1966)940	R.A.HEIN,R.L.FALGE JR.		
102344	1475		Zn1	Zn1	Zn	1																							1971																												Mg																	Mg, A3	K		0.857					0.857																																																																																																									J.LOW TEMP.PHYS.,5(1971)683	F.W.SMITH		
102345	1338	RRR=100	Yb1	Yb1	Yb	1																							1970																												Mg																	Mg, A3	K					0.015																																																																																																											PHYS.REV.B,2(1970)3911	A.JAYARAMAN,E.BUCHER,J.P.MAITA,K.ANDRES,K.NASSAU,P.D.DERNIER,P.H.SCHMIDT		
102346	RMP0350001		Yb1	Yb1	Yb	1																							1963																												Cu																	Cu, A1	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102347	658		Y1Zn1	Y1Zn1	Y	1	Zn	1																					1967																												CsCl																	CsCl, B2	K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
102348	472	P = 0-110 kbar	Y1	Y1	Y	1																							1974																																														K					0.1																																																																																																							New superconducting modifications of yttrium				JETP Lett., 20(1974)8 	I.V.BERMAN,N.B.BRANDT,YU.P.KURKIN		
102349	472	P = 110-125-160 kbar,  RRR = 8	Y	Y1	Y	1																							1974																																														K		2.5					2.5																																																																																																					New superconducting modifications of yttrium				JETP Lett., 20(1974)8 	I.V.BERMAN,N.B.BRANDT,YU.P.KURKIN		
102350	1526		Y	Y1	Y	1																							1973																												Mg																	Mg, A3	K					1.1																																																																																																											J.VAC.SCI.TECH.,10(1973)611	P.H.SCHMIDT		
102351	1367		Y	Y1	Y	1																																																			Mg																	Mg, A3	K					0.005																																																																																																							From Roberts' Table.				private commun.	W.C.Black,A.C.Mota		
102352	1988		W2Zr1	W2Zr1	W	2	Zr	1																					1966																												MgCu2(Laves)																	MgCu2, C15	K					0.033																																																																																																											PROC.10TH INTER.CONF.ON LOW TEMP.PHYS.,2(1966)86	C.K.JONES,J.K.HULM,R.C.MILLER,T.Y.TIEN		
102353	534		La2S3	La2S3	La	2	S	3																					1965																																													cubic	K					1.25																																																																																																							SUPERCONDUCTING LANTHANUM CHALCOGENIDES				PHYS.REV.LETT.,14(1965)952	F.HOLTZBERG,R.M.BOZORTH,S.METHFESSEL		
102354	469		La1Rh2	La1Rh2	La	1	Rh	2																					1965																												MgCu2(Laves)																	MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102355	469		La1Pt5	La1Pt5	La	1	Pt	5																					1965																												CeCo3B2																	CeCo3B2, CaCu5, D2[d]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102356	469		La1Pd3	La1Pd3	La	1	Pd	3																					1965																												AuCu3			A	4.233													AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102357	768		La1Pb3	La1Pb3	La	1	Pb	3																					1968																												AuCu3																	AuCu3, L1[2]	K		4.07					4.07																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
102358	558		La1P1	La1P1	La	1	P	1																																																	NaCl																	NaCl, B1	K					1.68																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
102359	181		La1Ni1O3	La1Ni1O3	La	1	Ni	1	O	3																																																																	K					1.02																																																																																																							From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
102360	559		La1N0.98	La1N0.98	La	1	N	0.98																					1966																												NaCl																	NaCl, B1	K					1.38																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
102361	559		La1N0.98	La1N0.98	La	1	N	0.98																					1966																												NaCl																	NaCl, B1	K					1.38																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
102362	658		La1Mg1	La1Mg1	La	1	Mg	1																					1967																																														K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
102363	427		K2Te3	K2Te3	K	2	Te	3																					1962																																														K					1.46																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102364	1212		K0.9O3Re1	K0.9O3Re1	K	0.9	O	3	Re	1																			1969																																														K					1.3																																																																																																											SOLID STATE COMMUN.,7(1969)299	A.W.SLEIGHT,P.E.BIERSTEDT,T.A.BITHER		
102365	1219		Lu1Te1	Lu1Te1	Lu	1	Te	1																					1970																												NaCl																	NaCl, B1	K					0.35																																																																																																											SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102366	469		Lu1Rh2	Lu1Rh2	Lu	1	Rh	2																					1965																												MgCu2(Laves)			A	7.404													MgCu2, C15	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102367	469		Lu1Rh1	Lu1Rh1	Lu	1	Rh	1																					1965																												NaCl			A	3.334													NaCl, B1	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102368	469		Lu2Rh1	Lu2Rh1	Lu	2	Rh	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102369	469		Lu3Rh1	Lu3Rh1	Lu	3	Rh	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102370	2.58		Li1Zn1	Li1Zn1	Li	1	Zn	1																																																	NaTl																	NaTl, B32	K					1.14																																																																																																														
102371	1191		Li1Ti1	Li1Ti1	Li	1	Ti	1																					1972																																														K					1																																																																																																											SCI.,175(1972)884	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO,P.H.SCHMIDT		
102372	1965		La2.4Te4Y0.6	La2.4Te4Y0.6	La	2.4	Te	4	Y	0.6																			1975																												Th3P4			A	9.586													Th3P4, D7[3]	K					1.7																																																										mj/mol.K2	2.1		208																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
102373	863		La5Sn3	La5Sn3	La	5	Sn	3																					1969																																														K					1.4																																																																																																											J.APPL.PHYS.,40(1969)3161	E.O.THORLAND,J.GRAOT,R.W.GREEN,S.LEGVOLD		
102374	1353	as grown	La1Si1.82	La1Si1.82	La	1	Si	1.82																					1970																												ThSi2			A	4.27		13.93											alpha-ThSi2, C[c]	K					1.2																																																																																																							Superconductivity of LaSi2				J.Phys.Soc.Jpn,28(1970)263	T.Satoh,Y.Asada		
102375	534		La2Se3	La2Se3	La	2	Se	3																					1965																																														K					1.25																																																																																																							SUPERCONDUCTING LANTHANUM CHALCOGENIDES				PHYS.REV.LETT.,14(1965)952	F.HOLTZBERG,R.M.BOZORTH,S.METHFESSEL		
102376	RMP0350001		La1Sb1	La1Sb1	La	1	Sb	1																					1963																												NaCl																	NaCl, B1	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102377	76		Mn0.24Ni0.76	Mn0.24Ni0.76	Mn	0.24	Ni	0.76																					1930																																														K					1.3																																																																																																											Z.Phys., 64(1930)581	W.Meissner		
102378	557		Mn0.73Mo0.27	Mn0.73Mo0.27	Mn	0.73	Mo	0.27																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.3																																																																																																											PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
102379	557		Mn0.63Mo0.37	Mn0.63Mo0.37	Mn	0.63	Mo	0.37																					1964																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.3																																																																																																											PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
102380	1340		Mg0.97Zn0.03	Mg0.97Zn0.03	Mg	0.97	Zn	0.03																					1972																																														K					0.013																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
102381	658		Mg1Y1	Mg1Y1	Mg	1	Y	1																					1967																												CsCl																	CsCl, B2	K					0.33																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
102382	557		Mg24Y5	Mg24Y5	Mg	24	Y	5																					1964																												alpha-Mn																	alpha-Mn, A12	K					1.3																																																																																																											PHYS.KOND.MATERIE,2(1964)210	E.BUCHER,F.HEINIGER,J.MULLER		
102383	1340		Mg0.85Tl0.15	Mg0.85Tl0.15	Mg	0.85	Tl	0.15																					1972																																														K					0.013																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
102384	84		Mg0.94Tl0.06	Mg0.94Tl0.06	Mg	0.94	Tl	0.06																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102385	1340		Mg0.97Sn0.03	Mg0.97Sn0.03	Mg	0.97	Sn	0.03																					1972																												CsCl																	CsCl, B2	K					2.02																																																																																																											PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
102387	1340		Mg0.93Pb0.07	Mg0.93Pb0.07	Mg	0.93	Pb	0.07																					1972																																														K		0.013					0.013																																																																																																									PHYS.REV.B,6(1972)103	A.S.COOPER,E.BUCHER,J.P.MAITA,K.ANDRES,V.HEINE		
102389	84		Mo1O2	Mo1O2	Mo	1	O	2																					1933																																														K					1.3																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102390	69		Mo0.28O0.72	Mo0.28O0.72	Mo	0.28	O	0.72																					1930																																														K					1.28																																																																																																							From Roberts' Table.				Z.Physik, 65(1930)30	W.Meissner,H.Z.Franz		
102391	84		Mo0.85Ni0.15	Mo0.85Ni0.15	Mo	0.85	Ni	0.15																					1933																																														K					4.2																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102392	300		Mo0.6Nb0.4	Mo0.6Nb0.4	Mo	0.6	Nb	0.4																					1962																																														K					0.05																																																																																																							FROM Roberts' Table.				LT-8(1962, London ) paper 4.5	R.D.Blaugher,J.K.Hulm,J.A.. Rayne,B.W.Veal,R.A.Hein		
102393	759		Mn0.002Ti0.499Zr0.49	Mn0.002Ti0.499Zr0.499	Mn	0.002	Ti	0.499	Zr	0.499																			1964																																														K					1.24																																																																																																											PHYS.REV.,135(1964)A1151	J.A.CAPE,R.R.HAKE		
102394	1377		Mn1Sn2	Mn1Sn2	Mn	1	Sn	2																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102395	37		Mn1Sb1	Mn1Sb1	Mn	1	Sb	1																					1953																												NiAs																	NiAs, B8[1]	K					1																																																																																																							Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
102396	788		Mn0.2Ru0.8	Mn0.2Ru0.8	Mn	0.2	Ru	0.8																					1969																																														K																																																																																																																PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
102397	RMP0350001		Mn1Re1	Mn1Re1	Mn	1	Re	1																					1963																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102398	601		Mn1P1	Mn1P1	Mn	1	P	1																					1965																												MnP																	MnP, B31	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
102399	11		Mn2O3	Mn2O3	Mn	2	O	3																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102400	RMP0350001		Mn1Ni1Zr1	Mn1Ni1Zr1	Mn	1	Ni	1	Zr	1																			1963																												MgCu2(Laves)																	MgCu2, C15	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102401	1913		Mo0.99Si1V2.01	Mo0.99Si1V2.01	Mo	0.99	Si	1	V	2.01																			1965																																														K					1.9																																																																																																											AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
102402	10		Mo1Si2	Mo1Si2	Mo	1	Si	2																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102403	1918		Mo1Se2	Mo1Se2	Mo	1	Se	2																					1974																																													hexagonal	K					1.25																																																																																																							Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
102404	614	P=0-7-21 kbar	Mo5S6Zn1	Mo5S6Zn1	Mo	5	S	6	Zn	1																			1975																																														K		3.2					3.2																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
102405	614	P=0-22 kbar	Mo3S4Sn0.6	Mo3S4Sn0.6	Mo	3	S	4	Sn	0.6																			1975																																														K		14.2					14.2																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
102406	1584		Mo2S3	Mo2S3	Mo	2	S	3																					1968																												TRI																		K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102407	918		Mo1S2	Mo1S2	Mo	1	S	2																					1969																																													hexagonal	K					1.25																																																																																																											J.PHYS.SOC.JAPAN,27(1969)590	K.SEKIZAWA,K.YASUKOCHI,N.USEI,Y.KUWASAWA		
102408	845		Mo1Pt2	Mo1Pt2	Mo	1	Pt	2																					1968																																													orthorhombic	K					1																																																																																																											J.LESS-COMMON METALS,15(1968)193	H.OCKEN,J.H.N.VAN VUCHT		
102409	1721		Mo0.69Pt0.31	Mo0.69Pt0.31	Mo	0.69	Pt	0.31																					1973																												Mg																	Mg, A3	K					1.2																																																																																																											J.LESS-COMMON METAL,32(1973)207	A.PAOLI,CH.SUSZ,J.MULLER,K.YVON,R.FULKIGER,R.ROGGEN		
102410	614	P=0-5-21 kbar	Mo6Pb0.92S7.5	Mo6Pb0.92S7.5	Mo	6	Pb	0.92	S	7.5																			1975																																														K		14					14																																																																																																									MAT.RES.BULL.,10(1975)297	A.C.LAWSON,D.C.JOHNSTON,R.N.SHELTON		
102411	1583		Mo1P2	Mo1P2	Mo	1	P	2																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102412	35		Mo1P1	Mo1P1	Mo	1	P	1																					1954																												WC																	WC, B[h]	K					1.03																																																																																																							Superconducting compounds				Phys.Rev., 93(1954)1415	B.T.Matthias,E.Corenzwit,C.F.Miller		
102415	119		N1Se1	N1Se1	N	1	Se	1																					1948																																														K					1.3																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102416	69		N0.97Sc1	N0.97Sc1	N	0.97	Sc	1																					1930																												NaCl																	NaCl, B1	K					1.38																																																																																																							From Roberts' Table.				Z.Physik, 65(1930)30	W.Meissner,H.Z.Franz		
102417	146	particle size = 20-26 A	N0.34Re1	N0.34Re1	N	0.34	Re	1																					1958																																														K		5					5																																																																																																									J.PHYS.AND CHEM.OF SOLIDS,7(1958)98	B.T.MATTHIAS,W.H.ZACHARIASEN		
102418	559		N0.98Pr1	N0.98Pr1	N	0.98	Pr	1																					1966																												NaCl																	NaCl, B1	K					1.38																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
102419	1439		N6Nb5	N6Nb5	N	6	Nb	5																					1974																																													hexagonal	K					1.77																																																																																																											J.APPL.PHYS.,45(1974)1389	G.OYA,Y.ONODERA		
102420	10		Mo3Zr1	Mo3Zr1	Mo	3	Zr	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102421	84		Mo0.75W0.75	Mo0.75W0.75	Mo	0.75	W	0.75																					1933																																														K					4.2																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102422	1584		Mo3Te4	Mo3Te4	Mo	3	Te	4																					1968																																														K					0.31																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102423	509		Mo3Sn1	Mo3Sn1	Mo	3	Sn	1																					1964																																													cubic	K					1																																																																																																											PHYS.CHEM.SOLIDS,25(1964)1499	D.H.KILLPATRICK		
102424	509		Mo3Sn1	Mo3Sn1	Mo	3	Sn	1																					1964																												Cr3Si(A15)																	Cr3Si, A15	K					0.35																																																																																																											PHYS.CHEM.SOLIDS,25(1964)1499	D.H.KILLPATRICK		
102425	500	tetragonal-II phase. not s/c.	Na0.1O3W1	Na0.1O3W1	Na	0.1	O	3	W	1																			1965																															A	5.2		3.9											tetragonal	K					0.04																																																																																																							Superconductivity of the alkali tungsten bronzes				PHYS.LETT.,15(1965)108	A.R.SWEEDLER,B.T.MATTHIAS,CH.J.RAUB		
102426	559		N0.906Zr1	N0.906Zr1	N	0.906	Zr	1																					1966																												NaCl																	NaCl, B1	K					1.38																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
102427	604		N1Y1	N1Y1	N	1	Y	1																					1966																												NaCl																	NaCl, B1	K					1.4																																																																																																							SUPERHEATING AND SUPERCOOLING IN THE SUPERCOMMDUCTING TRANSITION OF SMALL INDIUM SPHERES				PHYS.REV.LETT.,17(1966)87	F.ROTHWARF,J.FEDER,S.R.KISER		
102428	11		N1W2	N1W2	N	1	W	2																					1952																																													cubic	K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102429	559		N0.97W1	N0.97W1	N	0.97	W	1																					1966																												NaCl																	NaCl, B1	K					1.38																																																																																																											KHIMICHESKAYA AVYAZB V.POLUPROVODNIKAKHI,(1966)299-316	O.I.SHULISHOVA		
102430	10		N2V5	N2V5	N	2	V	5																					1954																																													hexagonal	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102431	10		N1U1	N1U1	N	1	U	1																					1954																												NaCl																	NaCl, B1	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102432	505	1200A	N1Ta2	N1Ta2	N	1	Ta	2																					1964																																														K					1.2																																																																																																											J.ELECTROCHEM.SOC.,111(1964)936	D.GERSTENBERG,P.M.HALL		
102433	505	1200A	N1Ta1	N1Ta1	N	1	Ta	1																					1964																												NaCl																	NaCl, B1	K		4.84					4.84																																																																																																									J.ELECTROCHEM.SOC.,111(1964)936	D.GERSTENBERG,P.M.HALL		
102434	10		N4Th3	N4Th3	N	4	Th	3																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102435	1815		N6Tb1	N6Tb1	N	6	Tb	1																					1967																																														K					1.28																																																																																																											ISZ.AKAD.NAUK.SSSR.NEORGAN.MATER.,3(1967)1495	I.A.SHCHERBACK,O.I.SHULISHOVA		
102436	906		N1Ta1	N1Ta1	N	1	Ta	1																					1970																																														K					4.2																																																																																																											ZH.ETF PIS.RED.,12(1970)101	L.G.BOIKO,S.V.POPOVA		
102437	1299		Nb0.45Pt3Zrr2.55	Nb0.45Pt3Zr2.55	Nb	0.45	Pt	3	Zr	2.55																			1966																																													hexagonal	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102438	1299		Nb1Pt2.58Ru0.42	Nb1Pt2.58Ru0.42	Nb	1	Pt	2.58	Ru	0.42																			1966																												Ni3Sn																	Ni3Sn, D0[19]	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102439	1299		Nb1Pt1.8Ru1.2	Nb1Pt1.8Ru1.2	Nb	1	Pt	1.8	Ru	1.2																			1966																																													hexagonal	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102440	1410	rf-sputtered film, d = 10,000 A.	Nb3Pt1	Nb3Pt1	Nb	3	Pt	1																					1970																												Cr3Si(A15)																	Cr3Si, A15	K		11					11																																																																																																									J.SPPL.PHYS.,41(1970)4958	J.I.GITTLEMAN,J.J.HANAK,J.P.PELLICANE,S.BOZOWSKI		
102441	1299		Nb1Pt1	Nb1Pt1	Nb	1	Pt	1																					1966																																													orthorhombic	K					1.46																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102442	1825		Nb3Pb1	Nb3Pb1	Nb	3	Pb	1																					1974																												Cr3Si(A15)																	Cr3Si, A15	K					9																																																																																																											J.APPL.PHYS.,45(1974)4590	H.L.LUO,L.KAMMERDINER		
102443	892		Nb1P1Se1	Nb1P1Se1	Nb	1	P	1	Se	1																			1969																																														K					1.25																																																																																																											INORG.CHEM.,8(1969)2690	P.C.DONOHUE,P.E.BIERSTEDT		
102444	892		Nb1P1S1	Nb1P1S1	Nb	1	P	1	S	1																			1969																																													orthorhombic	K		12.5					12.5																																																																																																									INORG.CHEM.,8(1969)2690	P.C.DONOHUE,P.E.BIERSTEDT		
102445	1229		NB1Os0.42Pt2.58	Nb1Os0.42Pt2.58	Nb	1	Os	0.42	Pt	2.58																			1972																												Ni3Sn																	Ni3Sn, D0[19]	K					1.6																																																																																																											III SOLID STATE COMMUN.,10(1972)1033	R.E.GLOVER,W.FELSCH		
102446	1450		Nb1O2	Nb1O2	Nb	1	O	2																					1972																																														K																																																																																																												Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
102447	427		Na1Te1	Na1Te1	Na	1	Te	1																					1962																																														K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102448	427		Na3Sb1	Na3Sb1	Na	3	Sb	1																					1962																																													hexagonal	K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102449	1283		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1972																												2H-NbSe2																	hexagonal	K		8.8					8.8																																																																																																									FIZ.TVERDOGO TELA,14(1972)515	E.S.ITSKEVICH,G.A.KALYUZHNAYA,M.A.IL'INA		
102450	1891	P=0-6.5-0 KBAR	Nb1Se2	Nb1Se2	Nb	1	Se	2																					1974																												2H-NbSe2																	hexagonal	K		7.77					7.77																																																																																																									J.PHYS.SOC.JAPAN,37(1974)36	K.YAMAYA		
102451	399		Nb1Sc1	Nb1Sc1	Nb	1	Sc	1																					1962																																														K																																																																																																																SUPERCONDUCTORS ED.BY M.TANENBAUM & W.V.,(1962)53-58	D.H.LESLIE,R.R.HAKE,T.G.BERLINCOURT		
102452	1584		Nb1Sb2	Nb1Sb2	Nb	1	Sb	2																					1968																																													monoclinic	K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102453	1825	films, sputter or evaporate 	Nb3Sb1	Nb3Sb1	Nb	3	Sb	1																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		2.2					2.2																																																																																																									J.APPL.PHYS.,45(1974)4590	H.L.LUO,L.KAMMERDINER		
102454	801		Nb3Sb1	Nb3Sb1	Nb	3	Sb	1																					1966																												Cr3Si(A15)																	Cr3Si, A15	K					0.4																																																																																																											PHYS.REV.,152(1966)341	C.C.DICKSON,E.PARTHE,F.ROTHWARF,H.BOLLER,J.A.SCHMITZ,R.C.THIEL		
102455	1853	P=0,7,13 kbar	Nb1S2	Nb1S2	Nb	1	S	2																					1974																																														K		6.26					6.26																																																																																																									PHIL.MAG.,30(1974)1091	A.J.GRANT,D.JEROME,P.MOLINIE		
102456	10		Nb1S1	Nb1S1	Nb	1	S	1																					1954																																														K					1.28																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102457	667	P=100 kbar, T = 1200-1300 C	Nb1Ru3	Nb1Ru3	Nb	1	Ru	3																					1974																												AuCu3																	AuCu3, L1[2]	K		15					15																																																																																																									ZH.ETF PIS.RED.,20(1974)648	L.N.FOMICHEVA,N.I.PALNIKOV,S.V.POPOVA		
102458	417		Nb0.7Ru0.3	Nb0.7Ru0.3	Nb	0.7	Ru	0.3																					1963																																														K					1																																																																																																											PHYS.KONDENS.MATERIE,1(1963)225	D.BENDER,E.BUCHER,J.MULLER		
102459	1299		Nb1Rh3	Nb1Rh3	Nb	1	Rh	3																					1966																												AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102461	1849	vapor deposition	Nb0.71Sn0.29	Nb0.71Sn0.29	Nb	0.71	Sn	0.29																					1964																																														K		18.3					18.3																																																																																																									RCA REVIEW,256(1964)405	J.L.COOPER		
102462	262		Nb2.5Si3Zr2.5	Nb2.5Si3Zr2.5	Nb	2.5	Si	3	Zr	2.5																																															Mn5Si3																	Mn5Si3, D8[8]	K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
102463	1913		Nb0.39Si1V2.61	Nb0.39Si1V2.61	Nb	0.39	Si	1	V	2.61																			1965																																														K					14																																																																																																											AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
102464	1953		Nb0.75Si0.25	Nb0.75Si0.25	Nb	0.75	Si	0.25																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		9					9																																																																																																					From Roberts' Table.				LT-13(1974)465	R.H.Hammond,S.Hazra		
102465	1438		Nb0.79Si0.21	Nb0.79Si0.21	Nb	0.79	Si	0.21																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		9.3					9.3																																																																																																									J.APPL.PHYS.,45(1974)447	A.R.STORM,D.D.BACON,J.H.WERNICK,L.R.TESTARDI,W.A.ROYER		
102466	10		Nb1Si2	Nb1Si2	Nb	1	Si	2																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102467	10		Nb3Si12	Nb3Si12	Nb	3	Si	12																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102468	42		Nb0.63Si0.37	Nb0.63Si0.37	Nb	0.63	Si	0.37																					1953																																														K					1.2																																																																																																							Superconducting silicides and Germanides				Phys.Rev., 89(1953)884	G.F.Hardy,J.K.Hulm		
102469	RMP0350001		Nb5Si3	Nb5Si3	Nb	5	Si	3																					1963																																													tetragonal	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102470	10		Nb0.67Si0.33	Nb0.67Si0.33	Nb	0.67	Si	0.33																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102471	1535	d = 12-30A	Nb1Se2	Nb1Se2	Nb	1	Se	2																					1972																												2H-NbSe2																		K		4.7					4.7																																																																																																					Superconductivity in Ultrathin NbSe2 Layers				Phys.Rev.Lett., 28(1972)299	R.F.Frindt		
102472	1283		Nb1Se2	Nb1Se2	Nb	1	Se	2																					1972																												2H-NbSe2																		K		8.9					8.9																																																																																																									FIZ.TVERDOGO TELA,14(1972)515	E.S.ITSKEVICH,G.A.KALYUZHNAYA,M.A.IL'INA		
102473	427		Ni1P1	Ni1P1	Ni	1	P	1																					1962																																														K					1.57																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102474	601		Ni2P1	Ni2P1	Ni	2	P	1																					1965																												Fe2P																	Fe2P, C22	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
102475	217		Ni3P1	Ni3P1	Ni	3	P	1																																																	Ni3P																	Ni3P, D0[e]	K					1.01																																																																																																											UNPUBLISHED RESULTS,	J.K.HULM,R.D.BLAUGHER		
102476	11		Ni1O1	Ni1O1	Ni	1	O	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102477	25		Nd1Si2	Nd1Si2	Nd	1	Si	2																					1958																												ThSi2																	ThSi2, C[c]	K					1																																																																																																							Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
102478	558		Nd2S3	Nd2S3	Nd	2	S	3																																																																		cubic	K					1.68																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
102479	RMP0350001		Nb1Zn3	Nb1Zn3	Nb	1	Zn	3																					1963																												AuCu3																	AuCu3, L1[2]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102480	1584		Nb1Te4	Nb1Te4	Nb	1	Te	4																					1968																																														K					0.025																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102481	1583		Nb5Te4	Nb5Te4	Nb	5	Te	4																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102482	1585	P > 59 kbar	Nb3Te1	Nb3Te1	Nb	3	Te	1																					1974																												Cr3Si(A15)																	Cr3Si, A15	K					2.5																																																																																																											J.PHYS.CHEM.SOLIDS,35(1974)1181	A.C.LAWSON,D.L.REBERTSON,H.T.HALL,J.F.CANNON		
102483	1603		Nb3Sn1	Nb3Sn1	Nb	3	Sn	1																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		17.77					17.77																																																																																																									PHYS.REV.LETT.,33(1974)1283	C.W.CHU		
102484	355		Nb2Sn3	Nb2Sn3	Nb	2	Sn	3																					1962																																													tetragonal	K					5																																																																																																											J.APPL.PHYS.,33(1962)2657	H.C.GATOS,T.B.REED		
102485	119		O2Mo5	Mo5O2	Mo	5	O	2																					1948																																														K					1.28																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102486	11		O2Mo1	Mo1O2	Mo	1	O	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102487	21		Ni1U1	Ni1U1	Ni	1	U	1																					1958																																														K					1.12																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
102488	RMP0350001		Ni1Ti1	Ni1Ti1	Ni	1	Ti	1																					1963																												W																	W, A2	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102489	301		Ni1Te2	Ni1Te2	Ni	1	Te	2																					1961																												CdI2																	CdI2, C6	K					1.2																																																																																																							PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102490	37		Ni1Te1	Ni1Te1	Ni	1	Te	1																					1953																												NiAs																	NiAs, B8[1]	K					1																																																																																																							Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
102491	84		Ni0.93Sn0.07	Ni0.93Sn0.07	Ni	0.93	Sn	0.07																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102492	119		Ni1Si1	Ni1Si1	Ni	1	Si	1																					1948																																														K					1.9																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102493	37		Ni1Si2	Ni1Si2	Ni	1	Si	2																					1953																												CaF2																	CaF2, C1	K					1																																																																																																							Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
102494	427		Ni1Sb3	Ni1Sb3	Ni	1	Sb	3																					1962																																														K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
102495	RMP0350001		Ni1Sb1	Ni1Sb1	Ni	1	Sb	1																					1963																												NiAs																	NiAs, B8[1]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102496	11		Ni1S1	Ni1S1	Ni	1	S	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102497	575		O2W1	O2W1	O	2	W	1																					1965																																														K					0.3																																																																																																											PHYS.LETT.,19(1965)82	A.R.SWEEDLER,B.T.MATTHIAS,J.K.HULM,T.H.GEBALLE		
102498	575		O3W1	O3W1	O	3	W	1																					1965																																														K					0.3																																																																																																											PHYS.LETT.,19(1965)82	A.R.SWEEDLER,B.T.MATTHIAS,J.K.HULM,T.H.GEBALLE		
102499	11		O3V2	O3V2	O	3	V	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102500	11		O2U1	O2U1	O	2	U	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102501	11		O3Tl2	O3Tl2	O	3	Tl	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102502	119		O3Ti2	O3Ti2	O	3	Ti	2																					1948																																														K					1.3																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102503	1379		O3Sn0.19W1	O3Sn0.19W1	O	3	Sn	0.19	W	1																			1968																																													tetragonal	K					1.3																																																																																																											INORGANIC CHEM.,7(1968)1646	A.W.SLEIGHT,D.C.PEASE,T.A.BITHER,T.E.GIER		
102504	1379		O3Sn0.21W1	O3Sn0.21W1	O	3	Sn	0.21	W	1																			1968																																													hexagonal	K					1.3																																																																																																											INORGANIC CHEM.,7(1968)1646	A.W.SLEIGHT,D.C.PEASE,T.A.BITHER,T.E.GIER		
102505	119		O3Sn2	O3Sn2	O	3	Sn	2																					1948																																														K					1.3																																																																																																							From Roberts' Table.				Gottingen Report, (1948)187	E.Justi		
102506	11		O3Rh2	O3Rh2	O	3	Rh	2																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102507	1212		O2Re1	O2Re1	O	2	Re	1																					1969																																														K					1.3																																																																																																											SOLID STATE COMMUN.,7(1969)299	A.W.SLEIGHT,P.E.BIERSTEDT,T.A.BITHER		
102508	181		O2Pb1	O2Pb1	O	2	Pb	1																																																																			K					1.02																																																																																																							From Roberts' Table, unpublished results				Unpublished results	R.D.Blaugher		
102509	786	P=170 kbar	P	P1	P	1																							1968																																														K		5.8					5.8																																																																																																					Superconductivity of phosphorus at high pressure				JETP Lett., 7(1968)323	I.V.BERMAN,N.B.BRANDT		
102510	955		Os4Zr11	Os4Zr11	Os	4	Zr	11																					1971									9.71																						A	13.428													cubic	K					1.2																																																																																																											J.LESS-COMMON METALS,23(1971)241	L.SCHMIDT,S.L.MCCARTHY		
102511	266		Os0.8W0.2	Os0.8W0.2	Os	0.8	W	0.2																					1962																																													hexagonal	K					1																																																																																																											IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102512	266		Os0.9W0.1	Os0.9W0.1	Os	0.9	W	0.1																					1962																																													hexagonal	K					1																																																																																																											IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102513	RMP0350001		Os0.29V0.71	Os0.29V0.71	Os	0.29	V	0.71																					1963																												CsCl																	CsCl, B2	K					0.37																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102514	RMP0350001		Os2U1	Os2U1	Os	2	U	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.37																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102515	RMP0350001		Os2Th1	Os2Th1	Os	2	Th	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102516	276		Os0.3Ta0.7	Os0.3Ta0.7	Os	0.3	Ta	0.7																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1																																																																																																											HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102517	RMP0350001		Os1Si1	Os1Si1	Os	1	Si	1																					1963																												FeSi																	FeSi, B20	K					0.6																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102518	963		Os0.2Rh0.8	Os0.2Rh0.8	Os	0.2	Rh	0.8																					1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
102519	1583		Os1P1	Os1P1	Os	1	P	1																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102520	503	films by vacuum evaporation	O1W3	O1W3	O	1	W	3																					1965																												Cr3Si(A15)																	beta-W	K					0.012																																																																																																							SUPERCONDUCTIVITY IN FILMS OF BETA TUNGSTEN AND OTHER TRANSITION METALS				PHYS.REV.LETT.,15(1965)260	A.S.COOPER,B.T.MATTHIAS,G.W.HULL,K.ANDRES,T.H.GEBALLE,W.L.BOND		
102521	1219		P0.4S0.6Y1	P0.4S0.6Y1	P	0.4	S	0.6	Y	1																			1970																												NaCl																	NaCl, B1	K					0.36																																																																																																											SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102522	892	prepared at P=65 kbar	P1S1Ta1	P1S1Ta1	P	1	S	1	Ta	1																			1969																																													orthorhombic	K					1.25																																																																																																											INORG.CHEM.,8(1969)2690	P.C.DONOHUE,P.E.BIERSTEDT		
102523	491		P1Ru2	P1Ru2	P	1	Ru	2																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102525	1582		P1Re2	P1Re2	P	1	Re	2																					1968																												Co2Si																	Co2Si, C23	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102526	1583		P4Re3	P4Re3	P	4	Re	3																					1968																																													monoclinic	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102527	491		P0.26Pt0.74	P0.26Pt0.74	P	0.26	Pt	0.74																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102528	491	low temperature phase	P3Pd7	P3Pd7	P	3	Pd	7																					1963																																														K		0.7					0.7																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102529	491	high temperature phase	P3Pd7	P3Pd7	P	3	Pd	7																					1963																																													rhombohedral	K		1					1																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102530	262		P2Pd5	P2Pd5	P	2	Pd	5																																																																			K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
102531	262		P3Pd5	P3Pd5	P	3	Pd	5																																																																			K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
102532	786	P = 220 kbar	P	P1	P	1																							1968																																														K		5.6					5.6																																																																																																					Superconductivity of phosphorus at high pressure				JETP Lett., 7(1968)323	I.V.BERMAN,N.B.BRANDT		
102533	1936		Pa1	Pa1	Pa	1																							1974																												Cu																	Cu, A1	K					0.4																																																																																																							FROM Roberts' Table.				LT-13(1974)vol.3 p=377	R.D.Fowler,L.B.Asprey,J.D.G.Lindsay,R.W.White		
102534	1915		P0.95Zr1	P0.95Zr1	P	0.95	Zr	1																					1974																												NaCl																	NaCl, B1	K		4.6					4.6																																																																																																									MAT.RES.BULL.,9(1974)1671	A.R.MOODENBAUGH,D.C.JOHNSTON,R.VISWANATHAN		
102535	1995		P1Zr3	P1Zr3	P	1	Zr	3																																																																		tetragonal	K		4.5					4.5																																																																																																					FROM Roberts' Table.				unpublished	Z.Fisk		
102536	1583		P2Zr1	P2Zr1	P	2	Zr	1																					1968																												Co2Si																	Co2Si, C23	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102537	601		P1W1	P1W1	P	1	W	1																					1965																												MnP																	MnP, B31	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
102538	1508		P2W1	P2W1	P	2	W	1																					1972																																													monoclinic	K					0.33																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
102539	128		P1V3	P1V3	P	1	V	3																					1956																																														K					1																																																																																																											J.PHYS.CHEM.SOLIDS.,1(1956)188	B.T.MATTIAS,E.A.WOOD,E.CORENZWIT,V.B.BALA		
102540	1508		P2V1	P2V1	P	2	V	1																					1972																																													monoclinic	K					0.035																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
102541	601		P1V1	P1V1	P	1	V	1																					1965																												NiAs																	NiAs, B8[1]	K					1.01																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
102542	1583		P2Ti1	P2Ti1	P	2	Ti	1																					1968																												Co2Si																	Co2Si, C23	K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102543	1582		P1Ti1	P1Ti1	P	1	Ti	1																					1968																												TiAs																	TiAs, B[i]	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102544	1382		P1Sn1	P1Sn1	P	1	Sn	1																					1970																																													tetragonal	K					1.25																																																																																																											INORGANIC CHEM.,9(1970)335	P.C.DONOHUE		
102545	552		Pd4S1	Pd4S1	Pd	4	S	1																					1965																															A	5.1147													tetragonal	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102546	963		Pd0.5Rh0.5	Pd0.5Rh0.5	Pd	0.5	Rh	0.5																					1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
102547	963		Pd0.25Pt0.25Rh0.5	Pd0.25Pt0.25Rh0.5	Pd	0.25	Pt	0.25	Rh	0.5																			1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
102548	963		Pd0.4Pt0.1Rh0.5	Pd0.4Pt0.1Rh0.5	Pd	0.4	Pt	0.1	Rh	0.5																			1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
102549	23		Pd1	Pd1	Pd	1																							1951																												Cu																	Cu, A1	K					0.1																																																																																																											Nature, 167(1951)111	B.B.Goodman		
102550	825		Pb1V3	Pb1V3	Pb	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K					4.2																																																																																																											DOKL.AN SSR,171(1966)331	E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
102551	653		Pb0.96Tl0.04	Pb0.96Tl0.04	Pb	0.96	Tl	0.04																					1966																																														K		7.06					7.06																																																																																																									J.PHYS.CHEM.SOLIDS,27(1966)1863	R.H.KERNAHAN,S.T.SEKURA		
102552	84		Pb1Se1	Pb1Se1	Pb	1	Se	1																					1933																																														K					1.26																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102553	778		Pb1S3Ti1	Pb1S3Ti1	Pb	1	S	3	Ti	1																			1970																																													tetragonal	K					0.05																																																																																																											PHYS.LETT.A,31(1970)551	L.SCHMIDT		
102554	64		Pb1S1	Pb1S1	Pb	1	S	1																					1950																																														K					1																																																																																																											Proc.Phys.Soc.(London),  A63(1950)1181	J.Darby,J.Hatton,B.V.Rollin		
102555	489		Pb1Rh2	Pb1Rh2	Pb	1	Rh	2																					1964																																														K					0.32																																																																																																											BULL.AM.PHYS.SOC.,9(1964)268	A.R.SWEEDLER,D.C.HAMILTON,M.F.MERRIAM		
102556	1372		Pb1Pd3	Pb1Pd3	Pb	1	Pd	3																					1972																												AuCu3																	AuCu3, L1[2]	K					0.1																																																																																																											J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
102557	552		Pd4Te1	Pd4Te1	Pd	4	Te	1																					1965																															A	12.674													cubic	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102558	28		Pd2Sr1	Pd2Sr1	Pd	2	Sr	1																					1957																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
102559	229,222		Pd1Sn4	Pd1Sn4	Pd	1	Sn	4																																																																		orthorhombic	K					1.35																																																																																																														
102560	301		Pd1Se1Te1	Pd1Se1Te1	Pd	1	Se	1	Te	1																			1961																												CdI2																	CdI2, C6	K					1.2																																																																																																							PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102561	140		Pd1Se2	Pd1Se2	Pd	1	Se	2																					1958																																														K					1.5																																																																																																											J.PHYS.CHEM.SOLIDS,4(1958)318	B.T.MATTHIAS,S.GELLER		
102562	552		Pd1Se1	Pd1Se1	Pd	1	Se	1																					1965																												PdS			A	6.727		6.912											PdS, B34	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102563	140		Pd1Se1	Pd1Se1	Pd	1	Se	1																					1958																																													cubic	K					1																																																																																																											J.PHYS.CHEM.SOLIDS,4(1958)318	B.T.MATTHIAS,S.GELLER		
102564	552		Pd17Se15	Pd17Se15	Pd	17	Se	15																					1965																															A	10.606													cubic	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102565	469		Pd1Sc2	Pd1Sc2	Pd	1	Sc	2																					1965																												Fe3W3C			A	12.442													Fe3W3C, E9[3]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102567	491		Pd1S1	Pd1S1	Pd	1	S	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102568	491		Pd2.8S1	Pd2.8S1	Pd	2.8	S	1																					1963																																													cubic	K		1.63					1.63																																																																																																									J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102569	413		Pt1Sb1Se1	Pt1Sb1Se1	Pt	1	Sb	1	Se	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.2																																																																																																											PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
102570	963		Pt0.2Rh0.8	Pt0.2Rh0.8	Pt	0.2	Rh	0.8																					1968																																														K					0.015																																																																																																							Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
102571	23		Pt1	Pt1	Pt	1																							1951																												Cu																	Cu, A1	K					0.1																																																																																																											Nature, 167(1951)111	B.B.Goodman		
102572	558		Pr2S3	Pr2S3	Pr	2	S	3																																																																		cubic	K					1.68																																																																																																											INSTITUTE METALLOFIZIKI AN U.S.S.R.KIEV,(1966-YEAR                     1966	O.I.SHULISHOVA		
102573	23		Pr1	Pr1	Pr	1																							1951																																													hexagonal	K					0.25																																																																																																											Nature, 167(1951)111	B.B.Goodman		
102574	208		Po1	Po1	Po	1																							1961																																														K					1.6																																																																																																											BULL.AMER.PHYS.SOC.,6(1961)92	E.W.WIEDERHOLD,J.W.SNIDER,R.J.SPRY		
102575	469		Pd3Y1	Pd3Y1	Pd	3	Y	1																					1965																												AuCu3			A	4.076													AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102576	711		Pd1Th1	Pd1Th1	Pd	1	Th	1																																																																			K					1.5																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102577	456		Pd5Th3	Pd5Th3	Pd	5	Th	3																																																																			K					1.3																																																																																																							From Roberts' Table.				unpublished	J.Thomson,B.R.Coles		
102578	456		Pd3Th1	Pd3Th1	Pd	3	Th	1																																																																			K					1.3																																																																																																							From Roberts' Table.				unpublished	J.Thomson,B.R.Coles		
102579	1372		Pd4Th1	Pd4Th1	Pd	4	Th	1																					1972																												AuCu3																	AuCu3, L1[2]	K					0.1																																																																																																											J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
102580	469		Pd5Th1	Pd5Th1	Pd	5	Th	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102581	469		Pt4Th1	Pt4Th1	Pt	4	Th	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102582	301		Pt1Te2	Pt1Te2	Pt	1	Te	2																					1961																												CdI2																	CdI2, C6	K					1.2																																																																																																							PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
102583	276		Pt0.2Ta0.8	Pt0.2Ta0.8	Pt	0.2	Ta	0.8																					1961																												sigma-CrFe																	sigma-CrFe, D8[b]	K					1.2																																																																																																											HELV.PHYS.ACTA,343(1961)843	E.BUCHER,F.HEINIGER,J.MULLER		
102584	1299		Pt2Ta1	Pt2Ta1	Pt	2	Ta	1																					1966																																													orthorhombic	K					1.6																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102585	28		Pt2Sr1	Pt2Sr1	Pt	2	Sr	1																					1957																												MgCu2(Laves)																	MgCu2, C15	K					1.02																																																																																																							Superconducting alkaline earth compounds				Phys.Rev., 107(1957)1558	B.T.Matthias,E.Corenzwit		
102586	229		Pt1Sn4	Pt1Sn4	Pt	1	Sn	4																					1962																																													orthorhombic	K					1.3																																																																																																											J.PHYS.CHEM.SOLIDS,23(1962)405	M.F.GENDRON,R.E.JONES		
102587	486		Pt1Sn2	Pt1Sn2	Pt	1	Sn	2																					1965																												CaF2																	CaF2, C1	K					0.34																																																																																																											J.PHYS.CHEM.SOLIDS,26(1965)665	B.T.MATTHIAS,C.J.RAUB,D.C.HAMILTON,E.CORENZWIT,G.W.HULL JR.		
102588	412		Pt3Sn1	Pt3Sn1	Pt	3	Sn	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
102589	469		Pt1Sc4	Pt1Sc4	Pt	1	Sc	4																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102590	469		Pt1Sc1	Pt1Sc1	Pt	1	Sc	1																					1965																												CsCl			A	3.268													CsCl, B2	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102591	469		Pt3Sc1	Pt3Sc1	Pt	3	Sc	1																					1965																												AuCu3																	AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102592	413		Pt1Sb1Te1	Pt1Sb1Te1	Pt	1	Sb	1	Te	1																			1963																												FeS2(pyrite)																	FeS2(pyrite), C2	K					1.2																																																																																																											PHYS.LETT.,5(1963)226	F.HULLIGER,J.MULLER		
102593	494		Rb1	Rb1	Rb	1																							1965																												W																	W, A2	K					0.011																																																																																																							SUPERCONDUCTIVITY GRAPHITIC COMPOUNDS				PHYS.REV.LETT.,14(1965)225	B.T.MATTHIAS,D.MACNAIR,K.ANDRES,N.B.HANNAY,P.SCHMIDT,T.H.GEBALLE		
102594	1581		Pu1	Pu1	Pu	1																							1964																																													monoclinic	K					0.4																																																																																																											REV.MOD.PHYS.,36(1964)144	K.MENDELSSOHN		
102595	469		Pt1Y1	Pt1Y1	Pt	1	Y	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102596	469		Pt3Y1	Pt3Y1	Pt	3	Y	1																					1965																												AuCu3																	AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102597	469		Pt5Y1	Pt5Y1	Pt	5	Y	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102598	707		Pt1V3	Pt1V3	Pt	1	V	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		2.53					2.53																																																																																																									LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102599	173		Pt0.33V0.67	Pt0.33V0.67	Pt	0.33	V	0.67																					1961																																														K					1.02																																																																																																											J.PHYS.CHEM.SOLIDS,19(1961)130	B.T.MATTHIAS,E.CORENZWIT,V.B.COMPTON		
102600	1372		Pt3V1	Pt3V1	Pt	3	V	1																					1972																												AuCu3																	AuCu3, L1[2]	K					0.07																																																																																																											J.LESS-COMMON METALS,27(1972)169	E.E.HAVINGA		
102601	711		Pt8Ti1	Pt8Ti1	Pt	8	Ti	1																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102602	456		Pt5Th3	Pt5Th3	Pt	5	Th	3																																																																			K					1.3																																																																																																							From Roberts' Table.				unpublished	J.Thomson,B.R.Coles		
102603	456		Pt2Th1	Pt2Th1	Pt	2	Th	1																																																																			K					1.3																																																																																																							From Roberts' Table.				unpublished	J.Thomson,B.R.Coles		
102604	469		Pt3Th1	Pt3Th1	Pt	3	Th	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102605	469		Rh1Sc4	Rh1Sc4	Rh	1	Sc	4																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102606	469		Rh0.32Sc0.68	Rh0.32Sc0.68	Rh	0.32	Sc	0.68																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102608	469		Rh3Sc1	Rh3Sc1	Rh	3	Sc	1																					1965																												AuCu3			A	3.898													AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102609	RMP0350001		Rh1Sb1	Rh1Sb1	Rh	1	Sb	1																					1963																												MnP																	MnP, B31	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102610	103		Rh1	Rh1	Rh	1																							1947																												Cu																	Cu, A1	K					0.086																																																																																																											J.PHYS.(U.S.S.R.),11(1947)95	L.MIGNOV,N.E.ALEKSEEVSKII		
102611	266		Re0.1W0.9	Re0.1W0.9	Re	0.1	W	0.9																					1962																																													cubic	K					1.02																																																																																																											IBM J.RES.DEV.,6(1962)116	A.TAYLOR,J.K.HULM,R.D.BLAUGHER		
102612	RMP0350001		Re2U1	Re2U1	Re	2	U	1																					1963																																													orthorhombic	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102613	1913		Re0.18Si1V2.82	Re0.18Si1V2.82	Re	0.18	Si	1	V	2.82																			1965																												Cr3Si(A15)																	Cr3Si, A15	K					14																																																																																																											AZV.AKAD.NAUK SSSR,1(1965)354	E.I.GLADYSHEVSKII,E.M.SAVITSKII,V.V.BARON,YU.V.EFIMOV		
102614	712		Re1Si2	Re1Si2	Re	1	Si	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished work, Univ. of Geneva				Unpublished results	E.Bucher,A.Zambelli		
102615	711		Re1Se2	Re1Se2	Re	1	Se	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102616	781		Rb1	Rb1	Rb	1																							1970																																														K					1.2																																																																																																											PHYS.REV.LETT.,24(1970)812	J.WITTIG		
102617	412		Rh3V1	Rh3V1	Rh	3	V	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
102618	707		Rh1V3	Rh1V3	Rh	1	V	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K					0.015																																																																																																											LOW TEMP.PHYS.,1(1969)539	J.E.COX,R.D.BLAUGHER,R.E.HEIN,R.M.J.WATERSTRAT		
102619	412		Rh3U1	Rh3U1	Rh	3	U	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
102620	1071		Rh1Ti2	Rh1Ti2	Rh	1	Ti	2																					1968																																														K					1.2																																																																																																											Z.PHYS.,208(1968)238	E.OFTEDAL,G.DUMMER		
102621	412		Rh3Ti1	Rh3Ti1	Rh	3	Ti	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
102622	469		Rh2Th1	Rh2Th1	Rh	2	Th	1																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102623	469		Rh3Th1	Rh3Th1	Rh	3	Th	1																					1965																												AuCu3																	AuCu3, L1[2]	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102624	280		Rh1Te1	Rh1Te1	Rh	1	Te	1																																																	NiAs																	NiAs, B8[1]	K					1.06																																																																																																							From Roberts' Table.				private commun.	B.T.Matthias		
102625	088	high temperature form	Rh1Te2	Rh1Te2	Rh	1	Te	2																					1933																												CdI2																	CdI2, C6	K					1.06																																																																																																											PHIL.MAG.,16(1933)1005	J.F.ALLEN		
102626	1299		Rh2Ta1	Rh2Ta1	Rh	2	Ta	1																					1966																												Co2Si																	Co2Si, C37	K					1.39																																																																																																											PHYS.STAT.SOL.,13(1966)423	H.C.GATOS,V.SADAGOPAN		
102627	RMP0350001		Rh1Si1	Rh1Si1	Rh	1	Si	1																					1963																												FeSi																	FeSi, B20	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102628	35		Rh0.29Se0.71	Rh0.29Se0.71	Rh	0.29	Se	0.71																					1954																																														K					1.04																																																																																																							Superconducting compounds				Phys.Rev., 93(1954)1415	B.T.Matthias,E.Corenzwit,C.F.Miller		
102629	1757	P = 0-24 kbar	Ru0.465V0.535	Ru0.465V0.535	Ru	0.465	V	0.535																					1974																																														K		5.8					5.8																																																																																																					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
102630	1930		Ru0.5V0.5	Ru0.5V0.5	Ru	0.5	V	0.5																					1971																																														K					0.4																																																																																																											PHYS.REV.B,4(1971)320	A.S.COOPER,C.W.CHU,E.BUCHER,J.P.MAITA		
102631	412		Ru3U1	Ru3U1	Ru	3	U	1																																																	AuCu3																	AuCu3, L1[2]	K					1.2																																																																																																							From Roberts' Table, Private communication				Private communication	J.Muller		
102632	552		Ru1Te2	Ru1Te2	Ru	1	Te	2																					1965																												FeS2(pyrite)			A	6.391													FeS2(pyrite), C2	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102633	552		Ru1Se2	Ru1Se2	Ru	1	Se	2																					1965																												FeS2(pyrite)			A	5.934													FeS2(pyrite), C2	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102634	491		Ru2Sb1	Ru2Sb1	Ru	2	Sb	1																					1963																																														K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102635	491		Ru1Sb1	Ru1Sb1	Ru	1	Sb	1																					1963																												MnP																	MnP, B31	K					0.35																																																																																																											J.PHYS.CHEM.SOLIDS,24(1963)1093	B.T.MATTHIAS,CH.J.RAUB,T.H.GEBALLE,W.H.ZACHARIASEN		
102636	552		Ru1S2	Ru1S2	Ru	1	S	2																					1965																												FeS2(pyrite)			A	5.609													FeS2(pyrite), C2	K					0.32																																																																																																							The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102637	658		Rh3Y7	Rh3Y7	Rh	3	Y	7																					1967																												Fe3Th7																	Fe3Th7, D10[2]	K					0.32																																																																																																							Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
102638	469		Rh1Y2	Rh1Y2	Rh	1	Y	2																					1965																																														K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102639	469		Rh1Y1	Rh1Y1	Rh	1	Y	1																					1965																												CsCl			A	3.41													CsCl, B2	K					0.32																																																																																																							SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
102640	RMP0350001		Rh2Y1	Rh2Y1	Rh	2	Y	1																					1963																												MgCu2(Laves)																	MgCu2, C15	K					0.32																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102641	774	R measured upto P = 150 kbar.	Sb(II)	Sb1	Sb	1																							1969																																													Sb(III), hcp	K		3.55			0		3.55																																																																																																					A Study of the superconductivity of antimony under pressure and a search for superconductivity in arsenic				J.Phys.Chem.Solids, 30(1969)1407	J.Wittig		
102642	103		Sb1	Sb1	Sb	1																							1947																												alpha-As																	alpha-As, A7	K					0.152																																																																																																											J.PHYS.(U.S.S.R.),11(1947)95	L.MIGNOV,N.E.ALEKSEEVSKII		
102643	84		S1W2	S1W2	S	1	W	2																					1933																																														K					1.3																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102644	1918		S2W1	S2W1	S	2	W	1																					1974																																													hexagonal	K					1.25																																																																																																							Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides				J.SOLID STATE CHEM.,9(1974)323	A.M.TOXEN,G.V.SUBBA RAO,M.W.SHAFER,S.KAWARAZAKI		
102645	1582		S1V3	S1V3	S	1	V	3																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102646	84		S1Tl2	S1Tl2	S	1	Tl	2																					1933																																														K					1.3																																																																																																							From Roberts' Table				Ann.Phys., 17(1933)593	W.Meissner,H.Franz,H.Westerhoff		
102647	1191		S1Ti1	S1Ti1	S	1	Ti	1																					1972																																														K					1																																																																																																											SCI.,175(1972)884	A.S.COOPER,B.T.MATTHIAS,E.CORENZWIT,H.E.BARZ,M.MAREZIO,P.H.SCHMIDT		
102648	11		S1Sn1	S1Sn1	S	1	Sn	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102649	1219		S1Sc1	S1Sc1	S	1	Sc	1																					1970																												NaCl																	NaCl, B1	K					0.33																																																																																																											SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102650	11		S3Sb1	S3Sb1	S	3	Sb	1																					1952																																														K					1.28																																																																																																							A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
102651	1989		Ru1Y3	Ru1Y3	Ru	1	Y	3																					1972																																														K					4.2																																																																																																											IZV.AKAD.NAUK SSSR METAL.,5(1972)129	E.M.SAVITSKIY,N.R.ROSHAN,V.P.POLYAKOVA		
102652	1706	P = 1-20 kbar	Ru0.46V0.54	Ru0.46V0.54	Ru	0.46	V	0.54																					1971																																														K		5.05					5.05																																																																																																									PHYS.REV.B,3(1971)107	H.J.LEVINSTEIN,J.E.KUNZLER,J.H.WERNICK,J.P.MAITA,L.R.TESTARDI		
102653	744		Sc0.5Zr0.5	Sc0.5Zr0.5	Sc	0.5	Zr	0.5																					1966																																														K					0.022																																																										mj/mol.K2	4.5		325																																					arc-melting in He					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102654	25		Sc1Si2	Sc1Si2	Sc	1	Si	2																					1958																																														K					1																																																																																																							Superconductivity and ferromagnetism in isomorphous compounds				Phys.Rev., 112(1958)89	B.T.Matthias,E.Corenzwit,W.H.Zachariasen		
102655	1219		Sc1Se1	Sc1Se1	Sc	1	Se	1																					1970																												NaCl																	NaCl, B1	K					0.33																																																																																																											SOLID STATE COMMUN.,8(1970)1379	F.HLLIGER,G.W.HULL JR.		
102656	744		Sc1	Sc1	Sc	1																							1966																												Mg																	Mg, A3	K					0.032																																																										mj/mol.K2	10.9		344																																										Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102657	1994	P=0-160 kbar	Sc1	Sc1	Sc	1																							1974																																														K					0.014																																																																																																							From Roberts' Table.				LT-13(1974)490	J.Witting,C.Probst,W.Wiedemann		
102658	1582		Sb3Zr5	Sb3Zr5	Sb	3	Zr	5																					1968																												Mn5Si3																	Mn5Si3, D8[8]	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102659	1584		Sb2Zr1	Sb2Zr1	Sb	2	Zr	1																					1968																																														K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102660	RMP0350001		Sb1Y1	Sb1Y1	Sb	1	Y	1																					1963																												NaCl																	NaCl, B1	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102661	1377		Sb2V1	Sb2V1	Sb	2	V	1																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102662	1377		Sb2Ti1	Sb2Ti1	Sb	2	Ti	1																					1972																												CuAl2																	CuAl2, C16	K					0.07																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102663	1139		Sb1Te2Tl1	Sb1Te2Tl1	Sb	1	Te	2	Tl	1																			1970																																														K					0.015																																																																																																											PHYS.REV.LETT.,24(1970)53	E.M.SWIGGARD,R.A.HEIN		
102664	1508		Sb2Ta1	Sb2Ta1	Sb	2	Ta	1																					1972																																													monoclinic	K					0.3																																																																																																											J.MATERIALS SCI.,7(1972)344	F.HULLIGER,G.W.HULL,K.ANDRES		
102665	303		Si1	Si1	Si	1																																																																				cubic	K					0.33																																																																																																							From Roberts' Table.				Unpublished	H.R.Hart,Jr.,B.W.Roberts		
102666	103		Si1	Si1	Si	1																							1947																												diamond																	diamond, A4	K					0.073																																																																																																											J.PHYS.(U.S.S.R.),11(1947)95	L.MIGNOV,N.E.ALEKSEEVSKII		
102667	1965		Se4Y3	Se4Y3	Se	4	Y	3																					1975																																													orthorhombic	K					0.35																																																										mj/mol.K2	0.7		274																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
102668	675		Se2V1	Se2V1	Se	2	V	1																					1966																																														K					1																																																																																																											PHYS.LETT.,20(1966)131	G.M.SCHAEFFER,M.H.VAN MAAREN		
102669	1582		Se1.05Ti1	Se1.05Ti1	Se	1.05	Ti	1																					1968																												NiAs																	NiAs, B8[1]	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102670	1582		Se1Th1	Se1Th1	Se	1	Th	1																					1968																												NaCl																	NaCl, B1	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102671	1582		Se1Th1	Se1Th1	Se	1	Th	1																					1968																												NaCl																	NaCl, B1	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102672	797		Se2Ta1	Se2Ta1	Se	2	Ta	1																					1967																																														K		0.16					0.16																																																																																																									PHYS.LETT.A,24(1967)645	G.M.SCHSRFFER,M.H.VAN MAAREN		
102673	797		Se2Ta1	Se2Ta1	Se	2	Ta	1																					1967																																														K		0.13					0.13																																																																																																									PHYS.LETT.A,24(1967)645	G.M.SCHSRFFER,M.H.VAN MAAREN		
102674	527		Se1	Se1	Se	1																							1964																												SE(II)																		K		9.65					9.65																																																																																																					SPECIFIC HEAT OF MERCURY AND THALLIUM BETWEEN 0.35 AND 4.2K				PHYS.REV.,135(1964)A631	B.J.C.VAN DER HOEVEN,JR.,P.H.KEESOM		
102675	273		Se1	Se1	Se	1																							1930																												gamma-Se																	gamma-Se, A8	K					1.26																																																																																																											ANN.PHYS.,7(1930)892	B.VOIGT,W.MEISSNER		
102676	744		Sc0.4Zr0.6	Sc0.4Zr0.6	Sc	0.4	Zr	0.6																					1966																																														K					0.04																																																																																																							Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
102677	10		Si1Ti1	Si1Ti1	Si	1	Ti	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102678	10		Si2Ti1	Si2Ti1	Si	2	Ti	1																					1954																												TiSi2																	TiSi2, C54	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102679	927		Si2Th3	Si2Th3	Si	2	Th	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
102681	1377		Si0.35Ta0.65	Si1Ta1.86	Si	1	Ta	1.86																					1972																												CuAl2																	CuAl2, C16	K					0.1																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102682	10		Si0.16Ta0.84	Si0.16Ta0.84	Si	0.16	Ta	0.84																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102683	10		Si0.28Ta0.72	Si0.28Ta0.72	Si	0.28	Ta	0.72																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102684	10		Si0.4Ta0.6	Si0.4Ta0.6	Si	0.4	Ta	0.6																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102685	10		Si2Ta1	Si2Ta1	Si	2	Ta	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102686	961		Si2Sr1	Si2Sr1	Si	2	Sr	1																					1967																																													cubic	K					0.32																																																																																																											J.LESS-COMMON METALS,12(1967)75	D.B.MCWHAN,J.R.SOULEN,M.S.SILVERMAN,V.B.COMPTON		
102687	961		Si3Sr2	Si3Sr2	Si	3	Sr	2																					1967																												ThSi2																	ThSi2, C[c]	K		0.55					0.55																																																																																																									J.LESS-COMMON METALS,12(1967)75	D.B.MCWHAN,J.R.SOULEN,M.S.SILVERMAN,V.B.COMPTON		
102688	540	P=120-130 kbar	Si1	Si1	Si	1																							1965																																														K		7.1					7.1																																																																																																									PHYS.LETT.,17(1965)187	J.WITTIG,W.BUCKEL		
102690	10		Si2W1	Si2W1	Si	2	W	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102691	42		Si0.15V0.75X0.1	Si0.15V0.75X0.1	Si	0.15	V	0.75	X	0.1																			1953																																														K																																																																																																												Superconducting silicides and Germanides				Phys.Rev., 89(1953)884	G.F.Hardy,J.K.Hulm		
102692	1933	dTc/dP = 2.8 E-5 K/bar	Si0.25V0.75	Si0.25V0.75	Si	0.25	V	0.75																				3	1974																												Cr3Si(A15)																	Cr3Si, A15	K		16.7					16.7			K/GPa	0.28																																																																																																	Effect of lattice transformation on the pressure dependence of Tc of V3Si single crystals				PHYS.REV.B,10(1974)4030	C.W.CHU,S.HUANG		
102693	RMP0350001		Si2V5	Si2V5	Si	2	V	5																					1963																																													tetragonal	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102694	10		Si0.4V0.6	Si0.4V0.6	Si	0.4	V	0.6																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102695	10		Si2V1	Si2V1	Si	2	V	1																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102696	21		Si1U3	Si1U3	Si	1	U	3																					1958																																													tetragonal	K					1.1																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
102697	RMP0350001		Si2U1	Si2U1	Si	2	U	1																					1963																												ThSi2																	ThSi2, C[c]	K					0.35																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102698	927		Si2U3	Si2U3	Si	2	U	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
102699	1677		Si3U1	Si3U1	Si	3	U	1																					1974																												AuCu3																	AuCu3, L1[2]	K					1.3																																																																																																											SOLID STATE COMMUN.,14(1974)145	C.J.SCHINKEL,H.J.VAN DAAL,K.H.J.BUSCHOW,M.H.VAN MAAREN		
102700	10		Si3Ti5	Si3Ti5	Si	3	Ti	5																					1954																												Mn5Si3																	Mn5Si3, D8[8]	K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102701	363		Sn1	Sn1	Sn	1																							1958																												diamond																	diamond, A4	K					0.1																																																																																																											PHYSICA,24(1958)S176	R.A.HEIN,R.L.FALGE JR.		
102702	291		Sm1	Sm1	Sm	1																							1962																																													rhombohedral	K					0.37																																																																																																							From Roberts' Table.				LT-8 (London, 1962), paper 5.3	O.V.Lounasmaa		
102703	10		Si0.2Zr0.8	Si0.2Zr0.8	Si	0.2	Zr	0.8																					1954																																														K					1.2																																																																																																							The superconductivity of some transition metal compounds				Phys.Rev., 93(1954)1004	G.F.Hardy,J.K.Hulm		
102704	1377		Si1Zr2	Si1Zr2	Si	1	Zr	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102705	1377		Si1Zr2	Si1Zr2	Si	1	Zr	2																					1972																												CuAl2																	CuAl2, C16	K					0.06																																																																																																							Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
102706	262		Si3Zr5	Si3Zr5	Si	3	Zr	5																																																	Mn5Si3																	Mn5Si3, D8[8]	K					1.1																																																																																																							From Roberts' Table				Unpublished	C.Raub		
102707	927		Si2Zr3	Si2Zr3	Si	2	Zr	3																					1969																																													tetragonal	K					0.1																																																																																																											PHYS.LETT.A,29(1969)109	E.E.HAVINGA,H.DAMSMA,M.H.VAN MARREN		
102708	20		Si0.45Zr0.55	Si0.45Zr0.55	Si	0.45	Zr	0.55																					1932																																														K					1.2																																																																																																											Z.Phys.,  75(1932)521	W.Meissner,H.Franz,H.Westerhoff		
102710	RMP0350001		Si2Zr1	Si2Zr1	Si	2	Zr	1																					1963																												ZrSi2																	ZrSi2, C49	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102711	711		Si1Y1	Si1Y1	Si	1	Y	1																																																																			K					0.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102712	808		Si0.665Y0.335	Si0.665Y0.335	Si	0.665	Y	0.335																					1966																												ThSi2																	ThSi2, C[c]	K					0.1																																																																																																							FROM Roberts' Table.				Ann.Acad.Sci.Finnicae A, VI No.210(1966)p=92	T.Ohtsuka,T.Satoh		
102713	781	P = 0-150 kbar	Sr1	Sr1	Sr	1																							1970																																														K					1.2																																																																																																											PHYS.REV.LETT.,24(1970)812	J.WITTIG		
102714	RMP0350001		Sr1	Sr1	Sr	1																							1963																												Cu																	Cu, A1	K					0.017																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102715	711		Sn1Y2	Sn1Y2	Sn	1	Y	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102716	863		Sn3Y5	Sn3Y5	Sn	3	Y	5																					1969																																														K					1.4																																																																																																											J.APPL.PHYS.,40(1969)3161	E.O.THORLAND,J.GRAOT,R.W.GREEN,S.LEGVOLD		
102717	711		Sn3V2	Sn3V2	Sn	3	V	2																																																																			K					1.15																																																																																																							From Roberts' Table, unpublished results, Univ. of Geneva				Unpublished results	E.Bucher,I.L.Staudenmann		
102718	1677		Sn3U1	Sn3U1	Sn	3	U	1																					1974																												AuCu3																	AuCu3, L1[2]	K					1.3																																																																																																											SOLID STATE COMMUN.,14(1974)145	C.J.SCHINKEL,H.J.VAN DAAL,K.H.J.BUSCHOW,M.H.VAN MAAREN		
102719	1900	deposited at 0.3 K.	Sn0.1Tl0.9	Sn0.1Tl0.9	Sn	0.1	Tl	0.9																					1974																																														K		3.5					3.5																																																																																																									Z.PHYS.,269(1974)23	C.G.GRANQVIST,T.CLAAESON		
102720	900	prepared at 15 kbar, 170-305 K	Sn0.65Tl0.35	Sn0.65Tl0.35	Sn	0.65	Tl	0.35																					1969																																														K		7.1					7.1																																																																																																									ZH.ETF PIS.RED.,10(1969)289	A.G.RABIN'KIN,E.YU.YONKOV		
102721	RMP0350001		Sb1Ti3	Sn1Ti3	Sn	1	Ti	3																					1963																												Ni3Sn																	Ni3Sn, D0[19]	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102722	780	Sn(III), P=113 kbar	Sn1	Sn1	Sn	1																							1966																																														K		5.3					5.3																																																																																																									Z.PHYS.,195(1966)228	J.WITTIG		
102723	785	Sn(II), P=125,160 kbar	Sn1	Sn1	Sn	1																							1968																																														K		5.2					5.2																																																																																																									ZH.ETF PIS.RED.,7(1968)198	I.V.BERMAN,N.B.BRANDT		
102724	579		Sn1	Sn1	Sn	1																							1965																												beta-Sn																	beta-Sn, A5	K		3.722					3.722																																																																																																									PHYS.REV. A,140(1965)507	D.E.MAPOTHER,D.K.FINNEMORE		
102725	909	P-induced SC. Tc = 4.28 K. at P = 70 kbar. Te(III) for 68 < P < 70 kbar.  	Te(III) 	Te1	Te	1																						3	1971																																														K		4.28			0		4.28			K/GPa	-0.17																																																																																																					ZH.ETF PIS.RED.,13(1971)23	E.S.ITSKEVICH,M.A.IL'INA		
102726	1688	Te(II), P=40-70 kbar	Te1	Te1	Te	1																							1972																																														K		3.9					3.9																																																																																																									FIZ.TVERDOGO TELA,14(1972)2527	I.V.BERMAN,YU.P.KURKIN,ZH.I.BYNZAROV		
102727	1277		Te1	Te1	Te	1																							1968																												gamma-Se																	gamma-Se, A8	K					0.05																																																																																																											FIZ.TVERDOGO TELA,10(1968)1112	I.I.FARBSHTEIN,S.S.SHALYT,V.A.NOSKIN		
102728	524		Tc0.05W0.95	Tc0.05W0.95	Tc	0.05	W	0.95																					1965																																													cubic	K					0.8																																																																																																							SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
102729	836	Tc measured for P = 0-15 kbar. sample is 99 % purity. Tc = 8.0 K for sample #1, = 7.924 K for sample #2	Tc	Tc1	Tc	1																							1968																																														K		8					8	MTC102729		K/GPa	-0.125																																																																																																	dTc/dP for technetium and a comment on its sign relation to the other transition metal superconductors				PHYS.LETT.A,26(1968)627	C.W.CHU,T.F.SMITH,W.E.GARDNER		
102731	291		Tb1	Tb1	Tb	1																							1962																												Mg																	Mg, A3	K					0.37																																																																																																							From Roberts' Table.				LT-8 (London, 1962), paper 5.3	O.V.Lounasmaa		
102732	1969		Ta0.15Zr0.85	Ta0.15Zr0.85	Ta	0.15	Zr	0.85																					1971																																														K		4.3					4.3																																																																																																					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
102733	1400		Ta1V2	Ta1V2	Ta	1	V	2																					1973																																														K					1.5																																																																																																											JAPAN J.APPL.PHYS.,12(1973)1659	H.HAYASHI,T.TAKASHIMA		
102734	1391		Ta0.63Ti0.3Zr0.07	Ta0.63Ti0.3Zr0.07	Ta	0.63	Ti	0.3	Zr	0.07																			1967																																														K																																																																																																												Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
102735	797		Ta1Te2	Ta1Te2	Ta	1	Te	2																					1967																																														K					0.05																																																																																																											PHYS.LETT.A,24(1967)645	G.M.SCHSRFFER,M.H.VAN MAAREN		
102736	710	deposited at 4.2 K. d=100 A. 	Sr1	Sr1	Sr	1																							1975																																														K		3.6					3.6																																																																																																									PHYS.LETT.A,51(1975)353	C.REALE		
102737	1488	Tc measured for P=60 - 160 kbar. Tc(P=100kbar) = 0.05 K. Tc by resistive transition. 	Th1	Th1	Th	1																							1972																																														K		1.35					1.35			K/GPa	-0.13																																																																																																	Pressure dependence of the transition temperature of thorium				PHYS.LETT.A,38(1972)517	A.R.MOODENBAUGH,M.B.MAPLE,W.A.FERTIG		
102738	1123	RRR = 1200	Th1	Th1	Th	1																							1967																												Cu																	Cu, A1	K		1.39					1.39																																																																																																									PHYS.REV.LETT.,18(1967)899	D.K.FINNEMORE,D.T.PETERSON,W.R.DECKER		
102739	1582		Te3Zr1	Te3Zr1	Te	3	Zr	1																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102740	1584		Te2W1	Te2W1	Te	2	W	1																					1968																																														K					0.3																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	F.HULLIGER,G.W.HULL JR.,K.ANDRESS		
102741	1582		Te3V2	Te3V2	Te	3	V	2																					1968																																													monoclinic	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102742	1582		Te4Ti5	Te4Ti5	Te	4	Ti	5																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102743	1582		Te1Ti1	Te1Ti1	Te	1	Ti	1																					1968																												NiAs																	NiAs, B8[1]	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102744	1582		Te4Ti3	Te4Ti3	Te	4	Ti	3																					1968																																														K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102745	1583		Te2Ti1	Te2Ti1	Te	2	Ti	1																					1968																																														K					1.1																																																																																																											STRUCTUER AND BONDING,4(1968)83-229	F.HULLIGER,J.MULLER		
102746	1582		Te1Th1	Te1Th1	Te	1	Th	1																					1968																												CsCl																	CsCl, B2	K					1.13																																																																																																											STRUCTURE AND BONDING,4(1968)83-229	E.BUCHER,J.L.STAUDENMANN		
102747	1688	P=100-260 kbar	Te1	Te1	Te	1																							1972																																														K		3.3					3.3																																																																																																									FIZ.TVERDOGO TELA,14(1972)2527	I.V.BERMAN,YU.P.KURKIN,ZH.I.BYNZAROV		
102748	1688	Te(IV), P=80-100 kbar	Te1	Te1	Te	1																							1972																																														K		4.3					4.3																																																																																																									FIZ.TVERDOGO TELA,14(1972)2527	I.V.BERMAN,YU.P.KURKIN,ZH.I.BYNZAROV		
102750	AAAAA		Ti1N1	N1Ti1	N	1	Ti	1																					1973																																														K		4.86					4.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102751	AAAAA		Pr1N1	N1Pr1	N	1	Pr	1																					1973																																														K					1.38																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102753	AAAAA		Sc1N1	N1Sc1	N	1	Sc	1																					1973																																														K					1.38																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102754	253		Ti0.1Zr0.9	Ti0.1Zr0.9	Ti	0.1	Zr	0.9																					1961																																													hexagonal	K					1																																																																																																							SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102755	572		Ti0.25Zr0.75	Ti0.25Zr0.75	Ti	0.25	Zr	0.75																					1966																																														K																																																																																																																PHYS.KONDENS.MATERIE,5(1966)243	E.BUCHER,F.HEINIGER,J.MULLER		
102756	253		Ti0.8Zr0.2	Ti0.8Zr0.2	Ti	0.8	Zr	0.2																					1961																																													hexagonal	K					1																																																																																																							SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
102757	RMP0350001		Ti1Zn2	Ti1Zn2	Ti	1	Zn	2																					1963																												MgZn2(Laves)																	MgZn2, C14	K					1.02																																																																																																							Superconductivity				REV.MORDERN PHYS.,35(1963)1	V.B.Compton,B.T.Matthias,T.H.Geballe		
102758	688		Ti0.12V0.88	Ti0.12V0.88	Ti	0.12	V	0.88																					1966																																														K																																																																																																																PHYS.LETT.,23(1966)40	G.RUPP,K.KWASNITZA		
102759	21		Ti1U2	Ti1U2	Ti	1	U	2																					1958																												AlB2																	AlB2, C32	K					1.06																																																																																																											J.Phys.Chem.Solids, 7(1958)259	B.S.Chandrasekar,J.K.Hulm		
102760	980		Ti4Tl1	Ti4Tl1	Ti	4	Tl	1																					1967																												Cr3Si(A15)																	Cr3Si, A15	K					0.35																																																																																																											SOLID STATE COMMUN.,5(1967)221	E.VIELHABER,H.L.LUO		
102763	AAAAA		Yb1C2	C2Yb1	C	2	Yb	1																					1973																																														K					0.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102769	AAAAA		Ce1C2	C2Ce1	C	2	Ce	1																					1973																																														K					0.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102770	AAAAA		Y1C2	C2Y1	C	2	Y	1																					1973																																														K		3.88					3.88																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102771	AAAAA		Y1C1	C1Y1	C	1	Y	1																					1973																																														K					1.38																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102772	AAAAA		Sc1C1	C1Sc1	C	1	Sc	1																					1973																																														K					1.38																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102775	AAAAA		Zr1B1	B1Zr1	B	1	Zr	1																					1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102779	AAAAA		Tb1B6	B6Tb1	B	6	Tb	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102782	AAAAA		Y1B6	B6Y1	B	6	Y	1																					1973																																														K					1.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102785	AAAAA		Zr2Si1	Si1Zr2	Si	1	Zr	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102786	AAAAA		Zr4Si1	Si1Zr4	Si	1	Zr	4																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102787	AAAAA		Zr1Si1	Si1Zr1	Si	1	Zr	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102788	AAAAA		Zr6Si5	Si5Zr6	Si	5	Zr	6																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102790	AAAAA		Zr4Si3	Si3Zr4	Si	3	Zr	4																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102795	AAAAA		La1Si2	La1Si2	La	1	Si	2																					1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102796	AAAAA		Y1Si1	Si2Y1	Si	2	Y	1																					1973																																														K					0.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102803	AAAAA		Ti5Ge3	Ge3Ti5	Ge	3	Ti	5																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102808	AAAAA		Zr3Si2	Si2Zr3	Si	2	Zr	3																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102811	AAAAA		Re1N0.34	N0.34Re1	N	0.34	Re	1																					1973																																														K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102817	AAAAA		Ta1N1	N1Ta1	N	1	Ta	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102819	AAAAA		Nb2N1	N1Nb2	N	1	Nb	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102820	AAAAA		Nb1N1	N1Nb1	N	1	Nb	1																					1973																																														K		15.6					15.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102821	AAAAA		W1C1	C1W1	C	1	W	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102822	AAAAA		W2C1	C1W2	C	1	W	2																					1973																																														K		2.74					2.74																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102823	AAAAA		Mo1C1	C1Mo1	C	1	Mo	1																					1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102824	AAAAA		Mo2C1	C1Mo2	C	1	Mo	2																					1973																																														K		2.78					2.78																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102826	AAAAA		Cr7C3	C3Cr7	C	3	Cr	7																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102827	AAAAA		Cr4C1	C1Cr4	C	1	Cr	4																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102828	AAAAA		Ta1C1	C1Ta1	C	1	Ta	1																					1973																																														K		3.3					3.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102829	AAAAA		Ta2C1	C1Ta2	C	1	Ta	2																					1973																																														K					1.98																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102830	AAAAA		Nb2C1	C1Nb2	C	1	Nb	2																					1973																																														K					1.98																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102831	AAAAA		Nb1C1	C1Nb1	C	1	Nb	1																					1973																																														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102832	AAAAA		V1C1	C1V1	C	1	V	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102837	AAAAA		Ta2B1	B1Ta2	B	1	Ta	2																					1973																																														K		3.12					3.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102838	AAAAA		Nb3B1	B1Nb3	B	1	Nb	3																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102839	AAAAA		Nb2B1	B1Nb2	B	1	Nb	2																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102841	AAAAA		V1B2	B2V1	B	2	V	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102844	AAAAA	excess carbon occures in the sample.	Tc1C1	C1Tc1	C	1	Tc	1																					1973																																														K		3.85					3.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102845	AAAAA		V5Si3	Si3V5	Si	3	V	5																					1973																																														K					0.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102846	AAAAA		V0.6Si0.4	Si0.4V0.6	Si	0.4	V	0.6																					1973																																														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102848	AAAAA		Re2B1	B1Re2	B	1	Re	2																					1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102852	AAAAA		Mo2B5	B5Mo2	B	5	Mo	2																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102853	AAAAA		Mo1B1	B1Mo1	B	1	Mo	1																					1973																																														K		0.5					0.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102857	AAAAA		Mo3Si2	Mo3Si2	Mo	3	Si	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102858	AAAAA		Cr1B2	B2Cr1	B	2	Cr	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102859	AAAAA		Cr1B1	B1Cr1	B	1	Cr	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102860	AAAAA		Ta5Si1	Si1Ta5	Si	1	Ta	5																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102861	AAAAA		Ta5Si2	Si2Ta5	Si	2	Ta	5																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102863	AAAAA		Ta3Si2	Si2Ta3	Si	2	Ta	3																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102864	AAAAA		Ta1Si1	Si1Ta1	Si	1	Ta	1																					1973																																														K		4.28					4.28																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102867	AAAAA		Nb2Si1	Nb2Si1	Nb	2	Si	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102869	AAAAA		Mo3Ge2	Ge2Mo3	Ge	2	Mo	3																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102870	AAAAA		Mo1Ge0.7	Ge0.7Mo1	Ge	0.7	Mo	1																					1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102871	AAAAA		Cr3Ge2	Cr3Ge2	Cr	3	Ge	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102873	AAAAA		Nb1Ge2	Ge2Nb1	Ge	2	Nb	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102876	AAAAA		Mn3Si1	Mn3Si1	Mn	3	Si	1																					1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102877	AAAAA		W1Si2	Si2W1	Si	2	W	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102878	AAAAA		W3Si2	Si2W3	Si	2	W	3																					1973																																														K		2.84					2.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102880	AAAAA		Mo1Si0.7	Mo1Si0.7	Mo	1	Si	0.7																					1973																																														K		1.34					1.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102882	AAAAA		Rh2B1	B1Rh2	B	1	Rh	2																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102887	AAAAA		Rh1C1	C1Rh1	C	1	Rh	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102888	AAAAA		Ru1C1	C1Ru1	C	1	Ru	1																					1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102889	AAAAA		Fe3C1	C1Fe3	C	1	Fe	3																					1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102892	AAAAA	beta-phase.	Mo1Ge2	Ge2Mo1	Ge	2	Mo	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102898	AAAAA		Th1B6	B6Th1	B	6	Th	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102899	AAAAA		Th1B2	B2Th1	B	2	Th	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102900	AAAAA		Th1B1	B1Th1	B	1	Th	1																					1973																																														K					1.77																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102903	AAAAA		Os2B1	B1Os2	B	1	Os	2																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102905	AAAAA		Co1Ge3	Co1Ge3	Co	1	Ge	3																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102906	AAAAA		Fe1Ge2	Fe1Ge2	Fe	1	Ge	2																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102908	AAAAA		U1Si1	Si1U1	Si	1	U	1																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102909	AAAAA	beta-phase.	Th1Si2	Si2Th1	Si	2	Th	1																					1973																																														K		2.41					2.41																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102910	AAAAA	alpha-phase.	Th1Si2	Si2Th1	Si	2	Th	1																					1973																																														K		3.16					3.16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102911	AAAAA		Th3Si2	Si2Th3	Si	2	Th	3																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102917	AAAAA		Ya1C1	C1Ta1	C	1	Ta	1																					1973																																														K		10.2					10.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102918	AAAAA		Nb0.4Ta0.6C1	Nb0.4Ta0.6C1	Nb	0.4	Ta	0.6	C	1																			1973																																														K		11.8					11.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102919	AAAAA		Nb1C1	C1Nb1	C	1	Nb	1																					1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102920	AAAAA		Mo0.56Co0.44	Co0.44Mo0.56	Co	0.44	Mo	0.56																					1973																																														K		13					13																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102921	AAAAA		Mo1C1	C1Mo1	C	1	Mo	1																					1973																																														K		13					13																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102924	AAAAA		Th1Ge1	Ge1Th1	Ge	1	Th	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102927	AAAAA		Rh1Ge1	Ge1Rh1	Ge	1	Rh	1																					1973																																														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102928	AAAAA		Rh5Ge2	Ge2Rh5	Ge	2	Rh	5																					1973																																														K		2.12					2.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102934	AAAAA		W1S1	S1W1	S	1	W	1																					1973																																														K					1.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102935	AAAAA	single crystal. 	Nb1S2	Nb1S2	Nb	1	S	2																					1973																																														K		6.1					6.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102937	AAAAA		Ce3S4	Ce3S4	Ce	3	S	4																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102940	AAAAA		La3S4	La3S4	La	3	S	4																					1973																																														K		8.25					8.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102951	AAAAA		Ir1S2.6	Ir1S2.6	Ir	1	S	2.6																					1973																																														K					0.32																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102953	AAAAA	single crystal.	Nb1Se2	Nb1Se2	Nb	1	Se	2																					1973																												2H-NbSe2																		K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102954	AAAAA		La3Se4	La3Se4	La	3	Se	4																					1973																																														K		8.6					8.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102955	AAAAA		Ni0.16Co0.64P0.2	Ni0.16Co0.64P0.2	Ni	0.16	Co	0.64	P	0.2																			1973																																														K					0.99																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102956	AAAAA		Ni0.6Fe0.19P0.21	Ni0.6Fe0.19P0.21	Ni	0.6	Fe	0.19	P	0.21																			1973																																														K					0.99																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102957	AAAAA		Ph5P4	P4Ph5	P	4	Ph	5																					1973																																														K		1.22					1.22																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102959	AAAAA		Ru2P1	P1Ru2	P	1	Ru	2																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102962	AAAAA		Co1P1	Co1P1	Co	1	P	1																					1973																																														K					0.97																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102968	AAAAA		Pd2Se1	Pd2Se1	Pd	2	Se	1																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102971	AAAAA		Pd6Se1	Pd6Se1	Pd	6	Se	1																					1973																																														K		0.66					0.66																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102973	AAAAA		Rh1Se1.75	Rh1Se1.75	Rh	1	Se	1.75																					1973																												FeS2(pyrite)			A	6.015													FeS2(pyrite), C2	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102974	AAAAA		Rh0.53Se0.47	Rh0.53Se0.47	Rh	0.53	Se	0.47																					1973																																														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102977	AAAAA		Ni1Te2	Ni1Te2	Ni	1	Te	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102978	AAAAA		Ni1Te1	Ni1Te1	Ni	1	Te	1																					1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102980	AAAAA		Nb1Te2	Nb1Te2	Nb	1	Te	2																					1973																																														K					2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102981	AAAAA	sample melted in a Mo crucible. 	La3Te4	La3Te4	La	3	Te	4																					1973																																														K		3.75					3.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102982	AAAAA	metalloceramic sample annealed at 1450C for 1.5h. 	La3Te4	La3Te4	La	3	Te	4																					1973																																														K		2.45					2.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102983	AAAAA		Y1Te1	Te1Y1	Te	1	Y	1																					1973																																														K		1.02					1.02																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102984	AAAAA		Pd1Se1Te1	Pd1Se1Te1	Pd	1	Se	1	Te	1																			1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102985	AAAAA		Nb1Se0.2Te0.8	Nb1Se0.2Te0.8	Nb	1	Se	0.2	Te	0.8																			1973																																														K					2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102986	AAAAA		Nb1Se0.25te0.75	Nb1Se0.25Te0.75	Nb	1	Se	0.25	Te	0.75																			1973																																														K		4.4					4.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102987	AAAAA		Ir1Se2.9	Ir1Se2.9	Ir	1	Se	2.9																					1973																																														K					0.32																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102989	552		Pd1Te1.08	Pd1Te1.08	Pd	1	Te	1.08																					1965																												Fe3Zn10			A	4.135		5.647											Fe3Zn10, D8[1]	K		1.88					1.88																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102990	552		Pd1Te1.06	Pd1Te1.06	Pd	1	Te	1.06																					1965																												Fe3Zn10			A	4.138		5.652											Fe3Zn10, D8[1]	K		2.11					2.11																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102991	AAAAA		Pd1Te1.04	Pd1Te1.04	Pd	1	Te	1.04																					1973																																														K		2.11					2.11																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102992	552		Pd1Te1.02	Pd1Te1.02	Pd	1	Te	1.02																					1965																												Fe3Zn10			A	4.144		5.661											Fe3Zn10, D8[1]	K		2.56					2.56																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102993	AAAAA		Pd1Te1	Pd1Te1	Pd	1	Te	1																					1973																																														K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102994	552		Pd1.1Te1	Pd1.1Te1	Pd	1.1	Te	1																					1965																												Fe3Zn10			A	4.152		5.671											Fe3Zn10, D8[1]	K		4.07					4.07																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
102997	AAAAA	high temperature form.	Th1Te2	Te2Th1	Te	2	Th	1																					1973																																														K					1.06																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
102998	AAAAA	low temperature form. 	Rh1Te2	Rh1Te2	Rh	1	Te	2																					1973																																														K		1.51					1.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103004	AAAAA		Ir1Te1	Ir1Te1	Ir	1	Te	1																					1973																																														K					0.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103005	AAAAA		Pd1Te2.3	Pd1Te2.3	Pd	1	Te	2.3																					1973																																														K		1.85					1.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103006	AAAAA		Pd1Te2.1	Pd1Te2.1	Pd	1	Te	2.1																					1973																																														K		1.89					1.89																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103007	AAAAA	single crystal.  	Pd1Te1	Pd1Te1	Pd	1	Te	1																					1973																												CdI2																	CdI2, C6	K		1.53					1.53																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103009	AAAAA	unannealed sample. 	Pd1.05Te2	Pd1.05Te2	Pd	1.05	Te	2																					1973																																														K		1.77					1.77																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103010	AAAAA	unannealed sample. 	Pd1.25Te2	Pd1.25Te2	Pd	1.25	Te	2																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103011	AAAAA	unannealed sample. 	Pd1.5Te2	Pd1.5Te2	Pd	1.5	Te	2																					1973																																														K		2.21					2.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103012	AAAAA	unannealed sample. 	Pd1.75Te2	Pd1.75Te2	Pd	1.75	Te	2																					1973																																														K		2.25					2.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103013	AAAAA		As2Mo1	As2Mo1	As	2	Mo	1																					1973																																														K					1.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103014	AAAAA		As2Fe3	As2Fe3	As	2	Fe	3																					1973																																														K					1.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103015	AAAAA		As4Cu18Sb3	As4Cu18Sb3	As	4	Cu	18	Sb	3																			1973																																														K					0.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103020	AAAAA			Pd0.95Pt0.05Te2	Pd	0.95	Pt	0.05	Te	2																			1973																																														K		1.71					1.71																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103021	AAAAA			Pd0.9Pt0.1Te2	Pd	0.9	Pt	0.1	Te	2																			1973																																														K		1.65					1.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103022	AAAAA			Ni0.1Pd0.9Te2	Ni	0.1	Pd	0.9	Te	2																			1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103023	AAAAA			Ni0.05Pd0.95Te2	Ni	0.05	Pd	0.95	Te	2																			1973																																														K		1.4					1.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103025	AAAAA			As1Ru1	As	1	Ru	1																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103028	AAAAA			As2Pd5	As	2	Pd	5																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103029	AAAAA			As3Pd5	As	3	Pd	5																					1973																																														K		24.761					24.761																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103030	AAAAA			As1Pd3	As	1	Pd	3																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103033	AAAAA			As1Ni0.25Pd0.75	As	1	Ni	0.25	Pd	0.75																			1973																												NiAs			A	3.66		5.03											NiAs, B8[1]	K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103034	AAAAA			As1Ni0.12Pd0.88	As	1	Ni	0.12	Pd	0.88																			1973																																														K		1.39					1.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103035	AAAAA			As1Ni0.25Pd0.75	As	1	Ni	0.25	Pd	0.75																			1973																																														K		1.34					1.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103038	AAAAA			Cu1Te1	Cu	1	Te	1																					1973																																														K					1.26																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103046	AAAAA			As4Mo5	As	4	Mo	5																					1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103047	AAAAA			As0.26Sb0.74	As	0.26	Sb	0.74																					1973																																														K					1.32																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103048	AAAAA			As1Ru2	As	1	Ru	2																					1973																																														K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103051	AAAAA			Ca1Ce1	Ca	1	Ce	1																					1973																																														K					1.7																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103053	AAAAA			Al2Pb4Si1	Al	2	Pb	4	Si	1																			1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103054	AAAAA			Ag2Te1	Ag	2	Te	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103057	AAAAA			Ag1S1	Ag	1	S	1																					1973																																														K					1.9																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103058	AAAAA			Cu1Se1Te	Cu	1	Se	1	Te																				1973																																														K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103060	AAAAA			Cu1S1Se1	Cu	1	S	1	Se	1																			1973																																														K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103062	AAAAA			Sn1Te1	Sn	1	Te	1																					1973																																														K		0.012					0.012																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103064	AAAAA		GeTe(Ag)	Ge1Te1	Ge	1	Te	1																					1973																																														K		0.21					0.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103065	AAAAA			Ge0.976Te1	Ge	0.976	Te	1																					1973																																														K		0.1					0.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103066	AAAAA			Ge1Te1	Ge	1	Te	1																					1973																																														K		0.172					0.172																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103067	AAAAA			C1Si1	C	1	Si	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103068	AAAAA			In4Sb1Te3	In	4	Sb	1	Te	3																			1973																																														K		1.4					1.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103082	AAAAA			Pb1Te1	Pb	1	Te	1																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103088	AAAAA			Nb1O1	Nb	1	O	1																					1973																																														K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103089	AAAAA			Mo3O5	Mo	3	O	5																					1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103090	AAAAA			Mo2O5	Mo	2	O	5																					1973																																														K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103097	AAAAA		Cu0.28Ti0.573O0,14	Cu0.287Ti0.573O0.14	Cu	0.287	Ti	0.573	O	0.14																			1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103098	AAAAA		La1Ni1O3	La1Ni1O3	La	1	Ni	1	O	3																			1973																																														K					1.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103105	AAAAA		Ti1.1O1	O1Ti1.1	O	1	Ti	1.1																					1973																																														K					0.21																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103109	AAAAA		Ca0.31Sr0.7Ti1O3	Ca0.31Sr0.7Ti1O3	Ca	0.31	Sr	0.7	Ti	1	O	3																	1973																																														K		0.1					0.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103110	AAAAA	Tc = 0.1 - 0.6.   738 	Ba0.1Sr0.9Ti1O3	Ba0.1Sr0.9Ti1O3	Ba	0.1	Sr	0.9	Ti	1	O	3																	1973																																														K		0.1					0.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103111	AAAAA		Sr1Ti1O3(Nb) 	Sr1Ti1O3	Sr	1	Ti	1	O	3																			1973																																														K		0.38					0.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103112	AAAAA		Sr1Ti1O3	Sr1Ti1O3	Sr	1	Ti	1	O	3																			1973																																														K		0.2					0.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103113	AAAAA		Ba0.3W1O3	Ba0.3W1O3	Ba	0.3	W	1	O	3																			1973																																														K					1.25																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103114	AAAAA		In0.3W1O3	In0.3W1O3	In	0.3	W	1	O	3																			1973																																														K					1.25																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103115	AAAAA		Tl0.3W1O3	Tl0.3W1O3	Tl	0.3	W	1	O	3																			1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103116	AAAAA		Zr3V3O1	Zr3V3O1	Zr	3	V	3	O	1																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103117	AAAAA		Zr0.61Rh0.285O0.105	Zr0.61Rh0.285O0.105	Zr	0.61	Rh	0.285	O	0.105																			1973																																														K		11.8					11.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103118	AAAAA		Ti0.576Rh0.287O0.14	Ti0.576Rh0.287O0.14	Ti	0.576	Rh	0.287	O	0.14																			1973																																														K		3.37					3.37																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103119	AAAAA		Ti1Re1O1	Ti1Re1O1	Ti	1	Re	1	O	1																			1973																																														K		5.74					5.74																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103120	AAAAA		Pd0.285Zr0.61O0.105	Pd0.285Zr0.61O0.105	Pd	0.285	Zr	0.61	O	0.105																			1973																																														K		2.09					2.09																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103121	AAAAA		Mo0.6Ru0.4	Mo0.6Ru0.4	Mo	0.6	Ru	0.4																					1973																																														K		7					7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103122	AAAAA		W0.4Tc0.6	Tc0.6W0.4	Tc	0.6	W	0.4																					1973																																														K		7.9					7.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103123	AAAAA		Mo0.5Re0.5	Mo0.5Re0.5	Mo	0.5	Re	0.5																					1973																																														K		4.7					4.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103124	AAAAA		Mo0.42Re0.58	Mo0.42Re0.58	Mo	0.42	Re	0.58																					1973																																														K		8.4					8.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103125	AAAAA		Nb0.63Ir0.37	Ir0.37Nb0.63	Ir	0.37	Nb	0.63																					1973																																														K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103126	AAAAA		Nb3Ir2	Ir2Nb3	Ir	2	Nb	3																					1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103127	AAAAA		Mo0.3Tc0.7	Mo0.3Tc0.7	Mo	0.3	Tc	0.7																					1973																																														K		12					12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103128	AAAAA		Al0.25Nb0.75	Al0.25Nb0.75	Al	0.25	Nb	0.75																					1973																																														K		7					7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103129	AAAAA		Ca1Ti1O3	Ca1Ti1O3	Ca	1	Ti	1	O	3																			1973																																														K					0.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103130	AAAAA		Ba1Ti1O3	Ba1Ti1O3	Ba	1	Ti	1	O	3																			1973																																														K					0.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103131	AAAAA		Ba0.13W1P3	Ba0.13W1P3	Ba	0.13	W	1	P	3																			1973																																														K		1.9					1.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103132	AAAAA		Na0.3W1O3	Na0.3W1O3	Na	0.3	W	1	O	3																			1973																																														K					0.3																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103133	AAAAA		Nb3Rh2	Nb3Rh2	Nb	3	Rh	2																					1973																																														K		4.04					4.04																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103134	AAAAA		W0.72Ir0.28	Ir0.28W0.72	Ir	0.28	W	0.72																					1973																																														K		4.46					4.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103135	AAAAA		Ru0.5W0.5	Ru0.5W0.5	Ru	0.5	W	0.5																					1973																																														K		5.12					5.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103136	AAAAA		Re0.6W0.4	Re0.6W0.4	Re	0.6	W	0.4																					1973																																														K		4.9					4.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103137	AAAAA		Re0.7W0.3	Re0.7W0.3	Re	0.7	W	0.3																					1973																																														K		4.9					4.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103138	AAAAA		Re0.52W0.48	Re0.52W0.48	Re	0.52	W	0.48																					1973																																														K		5.2					5.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103139	AAAAA		Mo0.62Os0.38	Mo0.62Os0.38	Mo	0.62	Os	0.38																					1973																																														K		5.65					5.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103140	AAAAA		Re0.76V0.24	Re0.76V0.24	Re	0.76	V	0.24																					1973																																														K		4.52					4.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103141	AAAAA		Re3V1	Re3V1	Re	3	V	1																					1973																																														K		6.26					6.26																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103142	AAAAA		Fe3Re2	Fe3Re2	Fe	3	Re	2																					1973																																														K		6.55					6.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103143	AAAAA		Mo0.74Ir0.26	Ir0.26Mo0.74	Ir	0.26	Mo	0.74																					1973																																														K		6.7					6.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103145	AAAAA		Nb0.6Os0.4	Nb0.6Os0.4	Nb	0.6	Os	0.4																					1973																																														K		1.78					1.78																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103146	AAAAA		Cr0.5Ru0.5	Cr0.5Ru0.5	Cr	0.5	Ru	0.5																					1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103148	AAAAA		Cr0.6Ru0.4	Cr0.6Ru0.4	Cr	0.6	Ru	0.4																					1973																																														K		2.1					2.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103149	AAAAA		Ta3Rh2	Rh2Ta3	Rh	2	Ta	3																					1973																																														K		2.35					2.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103150	AAAAA		Cr0.4Re0.6	Cr0.4Re0.6	Cr	0.4	Re	0.6																					1973																																														K		2.15					2.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103151	AAAAA		Nb0.5Re0.5	Nb0.5Re0.5	Nb	0.5	Re	0.5																					1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103152	AAAAA		Nb0.4re0.6	Nb0.4Re0.6	Nb	0.4	Re	0.6																					1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103153	AAAAA		Nb1Re3	Nb1Re3	Nb	1	Re	3																					1973																																														K		5.27					5.27																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103154	AAAAA		Nb0.625Pt0.375	Nb0.625Pt0.375	Nb	0.625	Pt	0.375																					1973																																														K		3.73					3.73																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103155	AAAAA		Nb0.62Pt0.38	Nb0.62Pt0.38	Nb	0.62	Pt	0.38																					1973																																														K		0.41					0.41																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103156	AAAAA		W0.66Os0.34	Os0.34W0.66	Os	0.34	W	0.66																					1973																																														K		3.81					3.81																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103157	AAAAA		Ta1Re1	Re1Ta1	Re	1	Ta	1																					1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103158	AAAAA		Zr2Re1	Re1Zr2	Re	1	Zr	2																					1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103159	AAAAA		Pt0.2Ta0.8	Pt0.2Ta0.8	Pt	0.2	Ta	0.8																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103160	AAAAA		Os0.3Ta0.7	Os0.3Ta0.7	Os	0.3	Ta	0.7																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103162	AAAAA		Cr1Re1	Cr1Re1	Cr	1	Re	1																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103164	AAAAA		Au1Ta2	Au1Ta2	Au	1	Ta	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103166	AAAAA		Ta0.65Ir0.35	Ir0.35Ta0.65	Ir	0.35	Ta	0.65																					1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103167	AAAAA		Re0.6Ta0.4	Re0.6Ta0.4	Re	0.6	Ta	0.4																					1973																																														K		1.4					1.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103168	AAAAA		Pt0.3Ta0.7	Pt0.3Ta0.7	Pt	0.3	Ta	0.7																					1973																																														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103171	AAAAA		Cs1Bi2	Bi2Cs1	Bi	2	Cs	1																					1973																																														K		4.75					4.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103172	AAAAA		Ce1Ru2	Ce1Ru2	Ce	1	Ru	2																					1973																																														K		4.9					4.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103175	AAAAA		Ca1Ir2	Ca1Ir2	Ca	1	Ir	2																					1973																																														K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103180	AAAAA		Zr1V2	V2Zr1	V	2	Zr	1																					1973																																														K		8.8					8.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103183	AAAAA		Y1Pt2	Pt2Y1	Pt	2	Y	1																					1973																																														K		4.1					4.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103189	AAAAA		Y1Ir1Os1	Y1Ir1Os1	Y	1	Ir	1	Os	1																			1973																																														K		2.6					2.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103191	AAAAA		Th1Ru2	Ru2Th1	Ru	2	Th	1																					1973																																														K		3.56					3.56																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103195	AAAAA		Ca1Pt2	Ca1Pt2	Ca	1	Pt	2																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103196	AAAAA		Ca1Pd2	Ca1Pd2	Ca	1	Pd	2																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103198	AAAAA		Mg1La2	La2Mg1	La	2	Mg	1																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103200	AAAAA		Na1Au2	Au2Na1	Au	2	Na	1																					1973																															A	7.814														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103201	AAAAA		V1Ta2	Ta2V1	Ta	2	V	1																					1973																															A	7.17														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103202	AAAAA		Zr1Ni1.5V0.5	Zr1Ni1.5V0.5	Zr	1	Ni	1.5	V	0.5																			1973																															A	7.068														K		0.43					0.43																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103203	AAAAA		Sr1Pt2	Pt2Sr1	Pt	2	Sr	1																					1973																																														K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103204	AAAAA		Sc1Ir2	Ir2Sc1	Ir	2	Sc	1																					1973																															A	7.348														K		1.03					1.03																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103205	AAAAA		Gd1Pt2	Gd1Pt2	Gd	1	Pt	2																					1973																															A	7.637														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103206	AAAAA		Ce1Ir2	Ce1Ir2	Ce	1	Ir	2																					1973																															A	7.571														K					0.37																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103207	AAAAA		Ce1Rh2	Ce1Rh2	Ce	1	Rh	2																					1973																															A	7.538														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103208	AAAAA		La1Ir2	Ir2La1	Ir	2	La	1																					1973																															A	7.686														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103209	AAAAA		La1Rh2	La1Rh2	La	1	Rh	2																					1973																															A	7.646														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103210	AAAAA		La1Pt2	La1Pt2	La	1	Pt	2																					1973																															A	7.774														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103211	AAAAA		Sc1Al2	Al2Sc1	Al	2	Sc	1																					1973																															A	7.579														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103212	AAAAA		Y1Rh2	Rh2Y1	Rh	2	Y	1																					1973																															A	7.459														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103213	AAAAA		Y1Al2	Al2Y1	Al	2	Y	1																					1973																															A	7.86														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103214	AAAAA		Al1Lu2	Al1Lu2	Al	1	Lu	2																					1973																															A	7.744														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103215	AAAAA		Al1Cu1Zr1	Al1Cu1Zr1	Al	1	Cu	1	Zr	1																			1973																															A	7.322														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103216	AAAAA		Ba1Pt2	Ba1Pt2	Ba	1	Pt	2																					1973																															A	7.92														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103217	AAAAA		U1Os2	Os2U1	Os	2	U	1																					1973																															A	7.509														K					0.37																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103218	AAAAA		U1Ir2	Ir2U1	Ir	2	U	1																					1973																															A	7.496														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103220	AAAAA		U1Al2	Al2U1	Al	2	U	1																					1973																															A	7.811														K					1.12																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103221	AAAAA		Th1Os2	Os2Th1	Os	2	Th	1																					1973																															A	7.704														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103222	AAAAA		Hf1W2	Hf1W2	Hf	1	W	2																					1973																															A	7.594														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103223	AAAAA		Hf1Mo2	Hf1Mo2	Hf	1	Mo	2																					1973																																														K					0.05																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103224	AAAAA		Zr1Co2	Co2Zr1	Co	2	Zr	1																					1973																															A	6.935														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103226	AAAAA		Zr1W2	W2Zr1	W	2	Zr	1																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103227	AAAAA		Ti1Be2	Be2Ti1	Be	2	Ti	1																					1973																															A	6.451														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103228	AAAAA		Gd1Ru2	Gd1Ru2	Gd	1	Ru	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103229	AAAAA		Y1Os1Re1	Y1Os1Re1	Y	1	Os	1	Re	1																			1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103230	AAAAA		Y1Ir1.5Os0.5	Y1Ir1.5Os0.5	Y	1	Ir	1.5	Os	0.5																			1973																																														K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103231	AAAAA		Hf1Os2	Hf1Os2	Hf	1	Os	2																					1973																															A	5.184		8.468												K		2.69					2.69																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103232	AAAAA		Zr1Os2	Os2Zr1	Os	2	Zr	1																					1973																															A	5.219		8.538												K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103233	AAAAA		Lu1Os2	Lu1Os2	Lu	1	Os	2																					1973																															A	5.254		8.661												K		3.49					3.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103234	AAAAA		Sc1Re2	Re2Sc1	Re	2	Sc	1																					1973																																														K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103235	AAAAA		V0.045Nb0.5Zr1	V0.45Nb0.5Zr1	V	0.45	Nb	0.5	Zr	1																			1973																																														K		4.3					4.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103236	AAAAA		Sc1Os2	Os2Sc1	Os	2	Sc	1																					1973																															A	5.179		8.484												K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103237	AAAAA		Y1Os2	Os2Y1	Os	2	Y	1																					1973																															A	5.303		8.786												K		4.7					4.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103238	AAAAA		Hf1Re2	Hf1Re2	Hf	1	Re	2																					1973																															A	5.239		9.584												K		4.8					4.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103239	AAAAA		Zr1Re2	Re2Zr1	Re	2	Zr	1																					1973																															A	5.262		8.593												K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103240	AAAAA		Mn1Ni1Zr1	Mn1Ni1Zr1	Mn	1	Ni	1	Zr	1																			1973																															A	7.07														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103241	AAAAA		Tb1Re2	Re2Tb1	Re	2	Tb	1																					1973																															A	5.397		8.797												K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103242	AAAAA		Gd1Re2	Gd1Re2	Gd	1	Re	2																					1973																															A	5.412		8.827												K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103243	AAAAA		Sc1Re2	Re2Sc1	Re	2	Sc	1																					1973																															A	5.27		8.59												K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103244	AAAAA		Ca1Mg2	Ca1Mg2	Ca	1	Mg	2																					1973																															A	6.23		10.12												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103245	AAAAA		Be1Ge2	Be1Ge2	Be	1	Ge	2																					1973																															A	4.27		6.92												K					1.75																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103246	AAAAA		Zr1Al2	Al2Zr1	Al	2	Zr	1																					1973																															A	5.282		8.748												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103247	AAAAA		Lu1Ru2	Lu1Ru2	Lu	1	Ru	2																					1973																															A	5.204		8.725												K		0.86					0.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103248	AAAAA		Y1Ru2	Ru2Y1	Ru	2	Y	1																					1973																															A	5.256		8.792												K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103249	AAAAA		Sc1.2Ru2	Ru2Sc1.2	Ru	2	Sc	1.2																					1973																															A	5.119		8.542												K		1.67					1.67																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103251	AAAAA		Y1Re2	Re2Y1	Re	2	Y	1																					1973																															A	5.396		8.819												K		1.83					1.83																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103252	AAAAA		Zr1Ru2	Ru2Zr1	Ru	2	Zr	1																					1973																															A	5.144		8.504												K		1.84					1.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103253	AAAAA		Nb1Tc3	Nb1Tc3	Nb	1	Tc	3																					1973																															A	9.625														K		10.5					10.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103254	AAAAA		Hf1Mo2	Hf1Mo2	Hf	1	Mo	2																					1973																																														K		0.05					0.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103255	AAAAA		Nb1Co1V1	Nb1Co1V1	Nb	1	Co	1	V	1																			1973																															A	4.928		8.08												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103256	AAAAA		Zr1V0.5Co1.5	Zr1V0.5Co1.5	Zr	1	V	0.5	Co	1.5																			1973																															A	4.982		8.114												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103257	AAAAA		Re1Be2	Be2Re1	Be	2	Re	1																					1973																															A	4.354		7.101												K					1.68																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103258	AAAAA		W1Be2	Be2W1	Be	2	W	1																					1973																															A	4.446		7.289												K					1.68																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103260	AAAAA		Zr1Cr2	Cr2Zr1	Cr	2	Zr	1																					1973																															A	5.102		8.239												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103262	AAAAA		Ti1Zn2	Ti1Zn2	Ti	1	Zn	2																					1973																															A	5.064		8.21												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103263	AAAAA		Er1Re2	Er1Re2	Er	1	Re	2																					1973																															A	5.363		8.758												K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103264	AAAAA		Ho1Re2	Ho1Re2	Ho	1	Re	2																					1973																															A	5.378		8.785												K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103266	AAAAA		Nb0.4Re0.6	Nb0.4Re0.6	Nb	0.4	Re	0.6																					1973																															A	9.781														K		2.36					2.36																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103267	AAAAA		Nb0.14Re0.86	Nb0.14Re0.86	Nb	0.14	Re	0.86																					1973																															A	9.61														K		8.5					8.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103268	AAAAA		Nb0.2Re0.8	Nb0.2Rr0.8	Nb	0.2	Rr	0.8																					1973																															A	9.648														K		9.1					9.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103269	AAAAA		Nb0.26Re0.74	Nb0.26Re0.74	Nb	0.26	Re	0.74																					1973																															A	9.688														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103271	AAAAA		Nb0.32Re0.68	Nb0.32Re0.68	Nb	0.32	Re	0.68																					1973																															A	9.73														K		4.5					4.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103272	AAAAA		Nb0.38Re0.62	Nb0.38Re0.62	Nb	0.38	Re	0.62																					1973																															A	9.77														K		2.45					2.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103273	AAAAA		Nb0.18Re0.82	Nb0.18Re0.82	Nb	0.18	Re	0.82																					1973																															A	9.641														K		9.7					9.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103274	AAAAA		Tc6Zr1	Tc6Zr1	Tc	6	Zr	1																					1973																															A	9.636														K		9.7					9.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103275	AAAAA		Mo1Re4	Mo1Re4	Mo	1	Re	4																					1973																																														K		7.85					7.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103277	AAAAA		Nb1Os1	Nb1Os1	Nb	1	Os	1																					1973																															A	9.76														K		2.86					2.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103279	AAAAA		Zr5Re24	Re24Zr5	Re	24	Zr	5																					1973																																														K		4.75					4.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103280	AAAAA		Hf5Re24	Hf5Re24	Hf	5	Re	24																					1973																																														K		4.3					4.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103281	AAAAA		Hf0.14Re0.86	Hf0.14Re0.86	Hf	0.14	Re	0.86																					1973																																														K		5.86					5.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103282	AAAAA		Re0.83Ti0.17	Re0.83Ti0.17	Re	0.83	Ti	0.17																					1973																															A	9.595														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103283	AAAAA		Re24Ti5	Re24Ti5	Re	24	Ti	5																					1973																															A	9.587														K		6.6					6.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103284	AAAAA		Re0.64Ta0.36	Re0.64Ta0.36	Re	0.64	Ta	0.36																					1973																															A	9.765														K		1.46					1.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103285	AAAAA		Re0.65Ta0.35	Re0.65Ta0.35	Re	0.65	Ta	0.35																					1973																															A	9.762														K		1.58					1.58																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103286	AAAAA		Ta1Re3	Re3Ta1	Re	3	Ta	1																					1973																																														K		4.75					4.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103287	AAAAA		Re3Ta1	Re3Ta1	Re	3	Ta	1																					1973																																														K		6.78					6.78																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103288	AAAAA		Re6Zr1	Re6Zr1	Re	6	Zr	1																					1973																															A	9.698														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103289	AAAAA		Rh1Te2	Rh1Te2	Rh	1	Te	2																					1973																															A	6.441														K		1.51					1.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103290	AAAAA		Rh0.53Se0.47	Rh0.53Se0.47	Rh	0.53	Se	0.47																					1973																																														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103291	AAAAA		Rh0.36Se0.64	Rh0.36Se0.64	Rh	0.36	Se	0.64																					1973																															A	6.015														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103292	AAAAA		Fe5Si2V3	Fe5Si2V3	Fe	5	Si	2	V	3																			1973																															A	8.851														K					0.37																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103293	AAAAA		V2.8Si2Co5.2	V2.8Si2Co5.2	V	2.8	Si	2	Co	5.2																			1973																															A	8.774														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103294	AAAAA		V3Ni5Ge2	V3Ni5Ge2	V	3	Ni	5	Ge	2																			1973																															A	8.928														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103295	AAAAA		Hf0.5Re0.5	Hf0.5Re0.5	Hf	0.5	Re	0.5																					1973																																														K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103296	AAAAA		Al2Mg3	Al2Mg3	Al	2	Mg	3																					1973																															A	10.55														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103297	AAAAA		Ta1Os1	Os1Ta1	Os	1	Ta	1																					1973																															A	9.773														K		1.95					1.95																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103298	AAAAA		Sc5Re24	Re24Sc5	Re	24	Sc	5																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103299	AAAAA		Nb0.6Pd0.4	Nb0.6Pd0.4	Nb	0.6	Pd	0.4																					1973																															A	9.77														K		2.47					2.47																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103300	AAAAA		Nb1Os2	Nb1Os2	Nb	1	Os	2																					1973																															A	9.655														K		2.52					2.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103301	AAAAA		Pd1Se1Te1	Pd1Se1Te1	Pd	1	Se	1	Te	1																			1973																															A	6.533														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103302	AAAAA		Bi1Pd1Te1	Bi1Pd1Te1	Bi	1	Pd	1	Te	1																			1973																															A	6.656														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103303	AAAAA		Bi1Pt1Se1	Bi1Pt1Se1	Bi	1	Pt	1	Se	1																			1973																															A	6.42														K		1.45					1.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103304	AAAAA		As1Pd1Se1	As1Pd1Se1	As	1	Pd	1	Se	1																			1973																															A	6.092														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103306	AAAAA		Pt1Bi2	Pt1Bi2	Pt	1	Bi	2																					1973																																														K					1.45																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103307	AAAAA		Ir1Re2.67	Ir1Te2.67	Ir	1	Te	2.67																					1973																															A	6.41														K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103309	AAAAA		Au1Sb2	Au1Sb2	Au	1	Sb	2																					1973																															A	6.658														K		0.58					0.58																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103310	AAAAA		Pd1Sb2	Pd1Sb2	Pd	1	Sb	2																					1973																															A	6.459														K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103311	AAAAA		As1Ni0.25Pd0.75	As1Ni0.25Pd0.75	As	1	Ni	0.25	Pd	0.75																			1973																																														K		1.34					1.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103312	AAAAA		As1Ni0.12Pd0.88	As1Ni0.12Pd0.88	As	1	Ni	0.12	Pd	0.88																			1973																																														K		1.39					1.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103313	AAAAA		As1Ni0.25Pd0.75	As1Ni0.25Pd0.75	As	1	Ni	0.25	Pd	0.75																			1973																															A	3.66		5.23												K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103314	AAAAA		Bi0.1Pt1Sb0.9	Bi0.1Pt1Sb0.9	Bi	0.1	Pt	1	Sb	0.9																			1973																																														K		1.21					1.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103315	AAAAA		Bi1Rh1	Bi1Rh1	Bi	1	Rh	1																					1973																															A	4.094		5.663												K		2.02					2.02																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103317	AAAAA		Bi1Pt1	Bi1Pt1	Bi	1	Pt	1																					1973																															A	4.315		5.49												K		1.21					1.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103318	AAAAA		Bi2Pb3	Bi2Pd3	Bi	2	Pd	3																					1973																																														K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103319	AAAAA		Ni1Bi1	Bi1Ni1	Bi	1	Ni	1																					1973																															A	4.07		5.35												K		4.25					4.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103320	AAAAA		Pt1Sb1Te1	Pt1Sb1Te1	Pt	1	Sb	1	Te	1																			1973																															A	6.48														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103321	AAAAA		Pt1Sb1Se1	Pt1Sb1Se1	Pt	1	Sb	1	Se	1																			1973																															A	6.33														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103322	AAAAA		Pd1Sb1Se1	Pd1Sb1Se1	Pd	1	Sb	1	Se	1																			1973																															A	6.323														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103323	AAAAA		Bi1Pd1Se1	Bi1Pd1Se1	Bi	1	Pd	1	Se	1																			1973																															A	6.432														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103324	AAAAA		Bi1Pt1Te1	Bi1Pt1Te1	Bi	1	Pt	1	Te	1																			1973																															A	6.59														K		1.15					1.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103325	AAAAA		Rh3Th7	Rh3Th7	Rh	3	Th	7																					1973																															A	10.031		6.287												K		2.15					2.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103327	AAAAA		Ni1Sb1	Ni1Sb1	Ni	1	Sb	1																					1973																															A	3.942		5.155												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103328	AAAAA		Ir1Te1	Ir1Te1	Ir	1	Te	1																					1973																															A	3.93		5.386												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103329	AAAAA		Rh1Te1	Rh1Te1	Rh	1	Te	1																					1973																															A	3.99		5.66												K					1.06																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103330	AAAAA		Co1Te1	Co1Te1	Co	1	Te	1																					1973																																														K					1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103333	AAAAA		Bi1Mn1	Bi1Mn1	Bi	1	Mn	1																					1973																															A	4.3		6.1												K					1.28																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103334	AAAAA		Pt1Sn1	Pt1Sn1	Pt	1	Sn	1																					1973																															A	4.11														K		0.37					0.37																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103335	AAAAA		Au1Sn1	Au1Sn1	Au	1	Sn	1																					1973																															A	4.32														K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103336	AAAAA		Pb1Sb1	Pb1Sb1	Pb	1	Sb	1																					1973																												Fe3Zn10																	Fe3Zn10, D8[1]	K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103337	AAAAA		Au1Th2	Au1Th2	Au	1	Th	2																					1973																															A	7.42		5.95												K		3.08					3.08																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103338	AAAAA		Cu1Th2	Cu1Th2	Cu	1	Th	2																					1973																															A	7.28		5.75												K		3.49					3.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103339	AAAAA		Au1Pb2	Au1Pb2	Au	1	Pb	2																					1973																															A	7.325		5.655												K		4.42					4.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103340	AAAAA		Co1Zr2	Co1Zr2	Co	1	Zr	2																					1973																															A	6.367		5.543												K		6.3					6.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103341	AAAAA		Co3Th7	Co3Th7	Co	3	Th	7																					1973																															A	9.833		6.2												K		1.83					1.83																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103342	AAAAA		Pt3Th7	Pt3Th7	Pt	3	Th	7																					1973																															A	10.126		6.346												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103343	AAAAA		B3Rh7 	B3Rh7	B	3	Rh	7																					1973																															A	7.47		4.78												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103344	AAAAA		B3Ru7 	B3Ru7	B	3	Ru	7																					1973																															A	7.465		4.715												K					2.58																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103345	AAAAA		Os3Th7	Os3Th7	Os	3	Th	7																					1973																															A	10.02		6.285												K		1.51					1.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103346	AAAAA		Ir3Th7	Ir3Th7	Ir	3	Th	7																					1973																															A	10.06		6.29												K		1.52					1.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103347	AAAAA		Fe3Th7	Fe3Th7	Fe	3	Th	7																					1973																															A	9.823		6.211												K		1.86					1.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103348	AAAAA		Ni3Th7	Ni3Th7	Ni	3	Th	7																					1973																															A	9.885		6.225												K		1.98					1.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103349	AAAAA		Fe1Cu2	Cu2Fe1	Cu	2	Fe	1																					1973																															A	5.911		4.951												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103351	AAAAA		Al1Th2	Al1Th2	Al	1	Th	2																					1973																															A	7.614		5.857												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103352	AAAAA		B1W2	B1W2	B	1	W	2																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103353	AAAAA		B1Mo2	B1Mo2	B	1	Mo	2																					1973																																														K					4.74																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103356	AAAAA		Cu1Al2	Al2Cu1	Al	2	Cu	1																					1973																															A	6.06		4.874												K		1.02					1.02																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103357	AAAAA		Ag1Th2	Ag1Th2	Ag	1	Th	2																					1973																															A	7.56		5.84												K		2.26					2.26																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103358	AAAAA		Ag1In2	Ag1In2	Ag	1	In	2																					1973																															A	6.883		5.615												K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103359	AAAAA		Rh1Pb2	Pb2Rh1	Pb	2	Rh	1																					1973																															A	6.664		5.865												K		2.66					2.66																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103360	AAAAA		Pd1Pb2	Pb2Pd1	Pb	2	Pd	1																					1973																															A	6.849		5.833												K		2.95					2.95																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103361	AAAAA		Rh1Sb1	Rh1Sb1	Rh	1	Sb	1																					1973																															A	6.34	5.955	3.876												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103362	AAAAA		Ir1Si1	Ir1Si1	Ir	1	Si	1																					1973																															A	5.558	3.211	6.273												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103364	AAAAA		Ge1Pd1	Ge1Pd1	Ge	1	Pd	1																					1973																															A	6.259	5.782	3.481												K					0.35																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103365	AAAAA		As1Co1	As1Co1	As	1	Co	1																					1973																															A	5.9	5.1	3.5												K					1.1																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103366	AAAAA		Ge1Pt1	Ge1Pt1	Ge	1	Pt	1																					1973																															A	6.088	5.733	3.701												K		0.4					0.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103369	AAAAA		Ge1Rh1	Ge1Rh1	Ge	1	Rh	1																					1973																															A	5.7	6.48	3.25												K		0.96					0.96																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103370	AAAAA		Au1Ga1	Au1Ga1	Au	1	Ga	1																					1973																															A	6.4	6.27	3.42												K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103372	AAAAA		Co1Sn2	Co1Sn2	Co	1	Sn	2																					1973																															A	6.361		5.452												K					1.02																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103375	AAAAA		Pb1Bi2	Bi2Pb1	Bi	2	Pb	1																					1973																																														K		4.25					4.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103376	AAAAA		Nb0.85Ir1.15	Ir1.15Nb0.85	Ir	1.15	Nb	0.85																					1973																																														K		4.75					4.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103378	AAAAA		Nb3Sn2	Nb3Sn2	Nb	3	Sn	2																					1973																																														K		16.6					16.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103380	AAAAA		Au1Zn3	Au1Zn3	Au	1	Zn	3																					1973																																														K		1.28					1.28																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103381	AAAAA		Nb0.26U0.74	Nb0.26U0.74	Nb	0.26	U	0.74																					1973																																														K		1.85					1.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103385	AAAAA		Nb0.75Rh1.25	Nb0.75Rh1.25	Nb	0.75	Rh	1.25																					1973																																														K		2.7					2.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103386	AAAAA		Pd1Bi1	Bi1Pd1	Bi	1	Pd	1																					1973																															A	7.203	8.707	10.662											orthorhombic	K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103388	AAAAA		Nb0.85Ir1.15	Ir1.15Nb0.85	Ir	1.15	Nb	0.85																					1973																																														K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103392	AAAAA		La0.55Lu0.45	La0.55Lu0.45	La	0.55	Lu	0.45																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103393	AAAAA		beta-Th1Si1	Si1Th1	Si	1	Th	1																					1973																																														K		2.41					2.41																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103394	AAAAA			La0.75Y00.25	La	0.75	Y0	0.25																					1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103398	AAAAA		Pt1Pb4	Pb4Pt1	Pb	4	Pt	1																					1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103400	AAAAA		Nb0.86Rh1.04	Nb0.86Rh1.04	Nb	0.86	Rh	1.04																					1973																																														K		3.76					3.76																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103403	AAAAA		Ag3.3Al1	Ag3.3Al1	Ag	3.3	Al	1																					1973																																														K		0.34					0.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103408	AAAAA		Ir1Zn2	Ir1Zn2	Ir	1	Zn	2																					1973																																														K		0.78					0.78																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103409	AAAAA		Au1Ga2	Au1Ga2	Au	1	Ga	2																					1973																																														K					0.32																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103410	AAAAA		Au1Al2	Al2Au1	Al	2	Au	1																					1973																																														K					0.34																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103411	AAAAA	beta = 102.35 degree. alpha-type	Pd1Bi2	Bi2Pd1	Bi	2	Pd	1																					1973																															A	12.74	4.25	5.665											monoclinic	K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103413	AAAAA		Nb0.85Rh1.15	Nb0.85Rh1.15	Nb	0.85	Rh	1.15																					1973																																														K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103414	AAAAA		Nb0.9Rh1.1	Nb0.9Rh1.1	Nb	0.9	Rh	1.1																					1973																																														K		3.07					3.07																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103419	AAAAA		Tl1Al3	Al3Tl1	Al	3	Tl	1																					1973																																														K		0.75					0.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103421	AAAAA		Ag5Rb1	Ag5Rb1	Ag	5	Rb	1																					1973																																														K					0.34																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103424	AAAAA		In1Sb1	In1Sb1	In	1	Sb	1																					1973																																														K		2.1					2.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103429	AAAAA		V1Ir3	Ir3V1	Ir	3	V	1																					1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103431	AAAAA		Ca1Pt1	Ca1Pt1	Ca	1	Pt	1																					1973																																														K					0.34																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103432	AAAAA		Au1Zn2	Au1Zn2	Au	1	Zn	2																					1973																																														K					0.32																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103433	AAAAA		Mn2.91V0.09Si1	Mn2.91V0.09Si1	Mn	2.91	V	0.09	Si	1																			1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103434	AAAAA		Nb1Ir2.76Pt0.24	Nb1Ir2.76Pt0.24	Nb	1	Ir	2.76	Pt	0.24																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103437	AAAAA		Nb1Rh3	Nb1Rh3	Nb	1	Rh	3																					1973																																														K					1.43																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103440	AAAAA		Pt1Sn4	Pt1Sn4	Pt	1	Sn	4																					1973																																														K		2.38					2.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103442	AAAAA		Nb0.65Zr0.35Pt3	Nb0.65Zr0.35Pt3	Nb	0.65	Zr	0.35	Pt	3																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103445	AAAAA		Nb1Pt1	Nb1Pt1	Nb	1	Pt	1																					1973																																														K					1.39																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103446	AAAAA		alpha-V1Ir1	Ir1V1	Ir	1	V	1																					1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103447	AAAAA		Ti1V1Si1	Ti1V1Si1	Ti	1	V	1	Si	1																			1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103448	AAAAA		Nb1Os0.42Pt2.58	Nb1Os0.42Pt2.58	Nb	1	Os	0.42	Pt	2.58																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103449	AAAAA		Nb1Ir0.45Pt2.55	Nb1Ir0.45Pt2.55	Nb	1	Ir	0.45	Pt	2.55																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103450	AAAAA		Nb1Ir2.55Pt0.45	Nb1Ir2.55Pt0.45	Nb	1	Ir	2.55	Pt	0.45																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103451	AAAAA		Nb1Rh2.7Nb0.3	Nb1Rh2.7Nb0.3	Nb	1	Rh	2.7	Nb	0.3																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103452	AAAAA		Nb1Ru0.45Pt2.55	Nb1Ru0.45Pt2.55	Nb	1	Ru	0.45	Pt	2.55																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103453	AAAAA		Nb1Ru1.2Pt1.8	Nb1Ru1.2Pt1.8	Nb	1	Ru	1.2	Pt	1.8																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103454	AAAAA		Nb0.15Ir0.85Pt3	Nb0.15Ir0.85Pt3	Nb	0.15	Ir	0.85	Pt	3																			1973																																														K					1.6																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103455	AAAAA		Nb0.6Ru0.4	Nb0.6Ru0.4	Nb	0.6	Ru	0.4																					1973																																														K					1.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103456	AAAAA		Cd1Hg1	Cd1Hg1	Cd	1	Hg	1																					1973																																														K					1.77																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103457	AAAAA		Mg2In1	In1Mg2	In	1	Mg	2																					1973																																														K		3.2					3.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103461	AAAAA		In5Bi1	Bi1In5	Bi	1	In	5																					1973																																														K		4.1					4.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103462	AAAAA		In2Bi1	Bi1In2	Bi	1	In	2																					1973																																														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103463	AAAAA		Bi1Ru1	Bi1Ru1	Bi	1	Ru	1																					1973																																														K		4.12					4.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103464	AAAAA		Hg1Sn6	Hg1Sn6	Hg	1	Sn	6																					1973																																														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103466	AAAAA		Re1Ti1O5	Re1Ti1O5	Re	1	Ti	1	O	5																			1973																																														K		5.71					5.71																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103468	AAAAA		Nb1Pt2	Nb1Pt2	Nb	1	Pt	2																					1973																																														K					1.46																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103471	AAAAA		Bi3Fe1	Bi3Fe1	Bi	3	Fe	1																					1973																																														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103472	AAAAA		Bi1Mg1	Bi1Mg1	Bi	1	Mg	1																					1973																																														K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103473	AAAAA		Bi1Mg1	Bi4Mg1	Bi	4	Mg	1																					1973																																														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103475	AAAAA		Re1Y1Os1	Re1Y1Os1	Re	1	Y	1	Os	1																			1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103476	AAAAA		Bi2Ir1	Bi2Ir1	Bi	2	Ir	1																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103478	AAAAA		Ag1Bi1	Ag1Bi1	Ag	1	Bi	1																					1973																																														K		2.78					2.78																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103481	AAAAA		V2.61Nb0.39Si1	V2.61Nb0.39Si1	V	2.61	Nb	0.39	Si	1																			1973																																														K					14																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103482	AAAAA		V2.7Nb0.35Si1	V2.7Nb0.3Si1	V	2.7	Nb	0.3	Si	1																			1973																																														K		12.8					12.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103483	AAAAA		V2.97Nb0.03Si1	V2.97Nb0.03Si1	V	2.97	Nb	0.03	Si	1																			1973																																														K		15.8					15.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103484	AAAAA		V2.58Zr0.42Si1	V2.58Zr0.42Si1	V	2.58	Zr	0.42	Si	1																			1973																																														K		8.8					8.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103485	AAAAA		V2.7Zr0.3Si1	V2.7Zr0.3Si1	V	2.7	Zr	0.3	Si	1																			1973																																														K		13.2					13.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103486	AAAAA		V2.7Ti0.3Si1	V2.7Ti0.3Si1	V	2.7	Ti	0.3	Si	1																			1973																																														K		10.9					10.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103487	AAAAA		V2.88Ce0.12Si1	V2.88Ce0.12Si1	V	2.88	Ce	0.12	Si	1																			1973																																														K		15.32					15.32																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103488	AAAAA		V2.94La0.06Si1	V2.94La0.06Si1	V	2.94	La	0.06	Si	1																			1973																																														K		15.92					15.92																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103489	AAAAA		V2.994La0.006Si1	V2.994La0.006Si1	V	2.994	La	0.006	Si	1																			1973																																														K		16.48					16.48																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103493	AAAAA		V2.7Mn0.3Si1 	V2.7Mn0.3Si1	V	2.7	Mn	0.3	Si	1																			1973																																														K		11.9					11.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103494	AAAAA		V2.79Mn0.21Si1 	V2.79Mn0.21Si1	V	2.79	Mn	0.21	Si	1																			1973																																														K		15.5					15.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103495	AAAAA		V2.97Mn0.03Si1 	V2.97Mn0.03Si1	V	2.97	Mn	0.03	Si	1																			1973																																														K		16.25					16.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103496	AAAAA		V2.01Mo0.99Si1	V2.01Mo0.99Si1	V	2.01	Mo	0.99	Si	1																			1973																																														K					1.9																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103497	AAAAA		V2.4Mo0.6Si1	V2.4Mo0.6Si1	V	2.4	Mo	0.6	Si	1																			1973																																														K		4.54					4.54																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103498	AAAAA		V2.52Mo0.48Si1	V2.52Mo0.48Si1	V	2.52	Mo	0.48	Si	1																			1973																																														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103499	AAAAA		V2.79Mo0.21Si1	V2.79Mo0.21Si1	V	2.79	Mo	0.21	Si	1																			1973																																														K		5.59					5.59																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103500	AAAAA		V2.91Mo0.09Si1	V2.91Mo0.09Si1	V	2.91	Mo	0.09	Si	1																			1973																																														K		10.4					10.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103501	AAAAA		V2.964Mo0.036Si1	V2.964Mo0.036Si1	V	2.964	Mo	0.036	Si	1																			1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103502	AAAAA		V2.97Mo0.03Si1	V2.97Mo0.03Si1	V	2.97	Mo	0.03	Si	1																			1973																																														K		16					16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103503	AAAAA		V2.79Cr0.21Si1	V2.79Cr0.21Si1	V	2.79	Cr	0.21	Si	1																			1973																																														K					14																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103504	AAAAA		V2.7Cr0.3Si1	V2.7Cr0.3Si1	V	2.7	Cr	0.3	Si	1																			1973																																														K		11.3					11.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103505	AAAAA		V3Si0.76Be0.24	V3Si0.76Be0.24	V	3	Si	0.76	Be	0.24																			1973																																														K		15.6					15.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103506	AAAAA		V3Si0.99Be0.01	V3Si0.99Be0.01	V	3	Si	0.99	Be	0.01																			1973																																														K		16.6					16.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103507	AAAAA		V3Si0.9Ge0.1	V3Si0.9Ge0.1	V	3	Si	0.9	Ge	0.1																			1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103508	AAAAA		V3Si0.1Ga0.9	V3Si0.1Ga0.9	V	3	Si	0.1	Ga	0.9																			1973																																														K		10.6					10.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103509	AAAAA		V3Si0.25Ga0.75	V3Si0.25Ga0.75	V	3	Si	0.25	Ga	0.75																			1973																																														K		8.1					8.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103510	AAAAA		V2.67Pd0.33Si1	V2.67Pd0.33Si1	V	2.67	Pd	0.33	Si	1																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103511	AAAAA			V2.979Co0.021Si1	V	2.979	Co	0.021	Si	1																			1973																																														K		16.4					16.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103512	AAAAA			V2.7Ru0.3Si1	V	2.7	Ru	0.3	Si	1																			1973																																														K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103513	AAAAA			V2.94Fe0.06Si1	V	2.94	Fe	0.06	Si	1																			1973																																														K		13.4					13.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103514	AAAAA			V2.808Re0.192Si1	V	2.808	Re	0.192	Si	1																			1973																																														K		4.7					4.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103515	AAAAA			V2.82Re0.18Si1	V	2.82	Re	0.18	Si	1																			1973																																														K					14																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103516	AAAAA		 (V,Mn)3Si	V2.49Mn0.42Si1	V	2.49	Mn	0.42	Si	1																			1973																																														K		8.1					8.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103517	AAAAA			V3Si0.46Ga0.54	V	3	Si	0.46	Ga	0.54																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103518	AAAAA			V3Si0.5Ga0.5	V	3	Si	0.5	Ga	0.5																			1973																																														K		8.6					8.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103519	AAAAA			V3Si0.52Ga0.48	V	3	Si	0.52	Ga	0.48																			1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103520	AAAAA			V3Si0.68Ga0.32	V	3	Si	0.68	Ga	0.32																			1973																																														K		9.4					9.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103521	AAAAA			V3Si0.72Ga0.28	V	3	Si	0.72	Ga	0.28																			1973																																														K		10.5					10.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103522	AAAAA			V3Si0.79Ga0.21	V	3	Si	0.79	Ga	0.21																			1973																																														K		10.7					10.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103523	AAAAA			V3Si0.87Ga0.13	V	3	Si	0.87	Ga	0.13																			1973																																														K		13.3					13.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103524	AAAAA			V3Si0.6Al0.4	V	3	Si	0.6	Al	0.4																			1973																																														K		10.1					10.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103525	AAAAA			V3Si0.76Al0.24	V	3	Si	0.76	Al	0.24																			1973																																														K		11.2					11.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103526	AAAAA			V3Si0.8Al0.2	V	3	Si	0.8	Al	0.2																			1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103527	AAAAA			V3Si0.98Al0.02	V	3	Si	0.98	Al	0.02																			1973																																														K		16.12					16.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103528	AAAAA			V3Si0.9Al0.1	V	3	Si	0.9	Al	0.1																			1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103529	AAAAA		(V,Ti)3Ga 	V2.754Ti0.246Ga1	V	2.754	Ti	0.246	Ga	1																			1973																																														K		13.4					13.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103530	AAAAA			V2.79Ce0.21Ga1	V	2.79	Ce	0.21	Ga	1																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103531	AAAAA			V2.778La0.222Ga1	V	2.778	La	0.222	Ga	1																			1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103532	AAAAA			V2.67Ir0.33Jr1	V	2.67	Ir	0.33	Jr	1																			1973																																														K		11.39					11.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103533	AAAAA			V3Si0.986Sb0.014	V	3	Si	0.986	Sb	0.014																			1973																																														K		10.5					10.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103534	AAAAA			V3Si0.2Sn0.8	V	3	Si	0.2	Sn	0.8																			1973																																														K		6.4					6.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103535	AAAAA			V3Si0.4Sn0.6	V	3	Si	0.4	Sn	0.6																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103536	AAAAA			V3Si0.6Sn0.4	V	3	Si	0.6	Sn	0.4																			1973																																														K		9.7					9.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103537	AAAAA			V3Si0.8Sn0.2	V	3	Si	0.8	Sn	0.2																			1973																																														K		12.85					12.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103538	AAAAA			V3Si0.2Ge0.8	V	3	Si	0.2	Ge	0.8																			1973																																														K		6.1					6.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103539	AAAAA			V3Si0.4Ge0.6	V	3	Si	0.4	Ge	0.6																			1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103540	AAAAA			V3Si0.6Ge0.4	V	3	Si	0.6	Ge	0.4																			1973																																														K		8.7					8.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103541	AAAAA			V2.793Ni0.207Ga1	V	2.793	Ni	0.207	Ga	1																			1973																																														K		11.9					11.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103542	AAAAA			V2.781Co0.219Ga1	V	2.781	Co	0.219	Ga	1																			1973																																														K		8.4					8.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103543	AAAAA			V2.865Fe0.135Ga1	V	2.865	Fe	0.135	Ga	1																			1973																																														K		10.1					10.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103544	AAAAA			V2.928Re0.072Ga1	V	2.928	Re	0.072	Ga	1																			1973																																														K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103545	AAAAA			V2.898Mn0.102Ga1	V	2.898	Mn	0.102	Ga	1																			1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103546	AAAAA			V2.883W0.117Ga1	V	2.883	W	0.117	Ga	1																			1973																																														K		11.5					11.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103547	AAAAA			V2.799Mo0.201Ga1	V	2.799	Mo	0.201	Ga	1																			1973																																														K		11.7					11.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103548	AAAAA			V2.799Cr0.201Ga1	V	2.799	Cr	0.201	Ga	1																			1973																																														K		12.6					12.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103549	AAAAA			V2.802Ta0.198Ga1	V	2.802	Ta	0.198	Ga	1																			1973																																														K		12.3					12.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103550	AAAAA			V2.814Nb0.186Ga1	V	2.814	Nb	0.186	Ga	1																			1973																																														K		13.5					13.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103551	AAAAA			V2.739Hf0.261Ga1	V	2.739	Hf	0.261	Ga	1																			1973																																														K		6.4					6.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103552	AAAAA			V2.742Zr0.258Ga1	V	2.742	Zr	0.258	Ga	1																			1973																																														K		9.9					9.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103553	AAAAA			V0.5Nb2.5Sn1	V	0.5	Nb	2.5	Sn	1																			1973																																														K		14.2					14.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103554	AAAAA			V1Nb2Sn1	V	1	Nb	2	Sn	1																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103555	AAAAA			V1.5Nb1.5Sb1	V	1.5	Nb	1.5	Sb	1																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103556	AAAAA			V2Nb1Sn1	V	2	Nb	1	Sn	1																			1973																																														K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103557	AAAAA			V3Ga0.975Bi0.025	V	3	Ga	0.975	Bi	0.025																			1973																																														K		14.7					14.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103558	AAAAA			V3Ga0.793Sb0.207	V	3	Ga	0.793	Sb	0.207																			1973																																														K		6.9					6.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103559	AAAAA			V0.003Ga0.974Pb0.026	V	0.003	Ga	0.974	Pb	0.026																			1973																																														K		13.2					13.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103560	AAAAA			V3Ga0.78Sn0.22	V	3	Ga	0.78	Sn	0.22																			1973																																														K		6.9					6.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103561	AAAAA			V3Ga0.957Ge0.043	V	3	Ga	0.957	Ge	0.043																			1973																																														K		13.1					13.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103562	AAAAA			V3Ga0.937In0.063	V	3	Ga	0.937	In	0.063																			1973																																														K		11.5					11.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103563	AAAAA			V3Ga0.994Cd0.006	V	3	Ga	0.994	Cd	0.006																			1973																																														K		11.2					11.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103564	AAAAA			V3Ga0.999Zn0.001	V	3	Ga	0.999	Zn	0.001																			1973																																														K		10.2					10.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103565	AAAAA			Nb3Sn0.8Ga0.2	Nb	3	Sn	0.8	Ga	0.2																			1973																																														K		17.8					17.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103566	AAAAA			Nb3Sn0.9Ga0.1	Nb	3	Sn	0.9	Ga	0.1																			1973																																														K		18.1					18.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103567	AAAAA			Nb2.85Mo0.15Al1	Nb	2.85	Mo	0.15	Al	1																			1973																																														K		13.4					13.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103568	AAAAA			Nb1.71V1.29Au1	Nb	1.71	V	1.29	Au	1																			1973																																														K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103569	AAAAA			Nb2.01V0.99Au1	Nb	2.01	V	0.99	Au	1																			1973																																														K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103570	AAAAA			Nb2.25V0.75Au1	Nb	2.25	V	0.75	Au	1																			1973																																														K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103571	AAAAA			Nb2.49V0.51Au1	Nb	2.49	V	0.51	Au	1																			1973																																														K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103572	AAAAA			Nb2.55V0.45Au1	Nb	2.55	V	0.45	Au	1																			1973																																														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103573	AAAAA			Nb2.9V0.3Au1	Nb	2.9	V	0.3	Au	1																			1973																																														K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103574	AAAAA			Nb2.85V0.15Au1	Nb	2.85	V	0.15	Au	1																			1973																																														K		8.4					8.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103575	AAAAA			V1Ta2Sn1	V	1	Ta	2	Sn	1																			1973																																														K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103576	AAAAA			V2Ta1Sn1	V	2	Ta	1	Sn	1																			1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103577	AAAAA			Nb3Rh0.02Au0.98	Nb	3	Rh	0.02	Au	0.98																			1973																																														K		11.9					11.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103578	AAAAA			Nb3Rh0.05Au0.95	Nb	3	Rh	0.05	Au	0.95																			1973																																														K		11					11																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103579	AAAAA			Nb3Rh0.1Au0.9	Nb	3	Rh	0.1	Au	0.9																			1973																																														K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103580	AAAAA			Nb3Rh0.3Au0.7	Nb	3	Rh	0.3	Au	0.7																			1973																																														K		9.5					9.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103581	AAAAA			Nb3Rh0.5Au0.5	Nb	3	Rh	0.5	Au	0.5																			1973																																														K		6.6					6.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103582	AAAAA			Nb3Rh0.7Au0.3	Nb	3	Rh	0.7	Au	0.3																			1973																																														K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103583	AAAAA			Nb3Sn0.56Ge0.44	Nb	3	Sn	0.56	Ge	0.44																			1973																																														K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103584	AAAAA			Nb3Sn0.73Ge0.27	Nb	3	Sn	0.73	Ge	0.27																			1973																																														K		8.2					8.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103585	AAAAA			Nb3Sn0.81Ge0.19	Nb	3	Sn	0.81	Ge	0.19																			1973																																														K		14.3					14.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103586	AAAAA			Nb3Sn0.2Ga0.8	Nb	3	Sn	0.2	Ga	0.8																			1973																																														K		13.1					13.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103587	AAAAA			Nb3Sn0.4Ga0.6	Nb	3	Sn	0.4	Ga	0.6																			1973																																														K		14.6					14.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103588	AAAAA			Nb3Sn0.6Ga0.4	Nb	3	Sn	0.6	Ga	0.4																			1973																																														K		16					16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103589	AAAAA			Nb3Sn0.98Al0.02	Nb	3	Sn	0.98	Al	0.02																			1973																																														K		17.9					17.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103590	AAAAA			Nb1Ta2Sn1	Nb	1	Ta	2	Sn	1																			1973																																														K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103591	AAAAA			Nb2Ta1Sn1	Nb	2	Ta	1	Sn	1																			1973																																														K		16.4					16.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103592	AAAAA			Nb2.5Ta0.5Sn1	Nb	2.5	Ta	0.5	Sn	1																			1973																																														K		17.6					17.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103593	AAAAA			Nb2.75Ta0.25Sn1	Nb	2.75	Ta	0.25	Sn	1																			1973																																														K		17.8					17.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103594	AAAAA			Nb0.9Mo2.1Al1	Nb	0.9	Mo	2.1	Al	1																			1973																																														K		2.73					2.73																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103595	AAAAA			Nb1.2Mo1.8Al1	Nb	1.2	Mo	1.8	Al	1																			1973																																														K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103596	AAAAA			Nb1.5Mo1.5Al1	Nb	1.5	Mo	1.5	Al	1																			1973																																														K		4.9					4.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103597	AAAAA			Nb2.1Mo0.9Al1	Nb	2.1	Mo	0.9	Al	1																			1973																																														K		8.3					8.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103598	AAAAA			Nb2.7Mo0.3Al1	Nb	2.7	Mo	0.3	Al	1																			1973																																														K		11.4					11.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103599	AAAAA			Nb3Rh0.95Co0.05	Nb	3	Rh	0.95	Co	0.05																			1973																																														K		1.96					1.96																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103600	AAAAA			Nb3Rh0.98Co0.02	Nb	3	Rh	0.98	Co	0.02																			1973																																														K		2.28					2.28																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103601	AAAAA			Nb3Sn0.1Al0.9	Nb	3	Sn	0.1	Al	0.9																			1973																																														K		16.1					16.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103602	AAAAA			Nb3Sn0.2Al0.8	Nb	3	Sn	0.2	Al	0.8																			1973																																														K		14.6					14.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103603	AAAAA			Nb3Sn0.4Al0.6	Nb	3	Sn	0.4	Al	0.6																			1973																																														K		13.6					13.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103604	AAAAA			Nb3Sn0.5Al0.5	Nb	3	Sn	0.5	Al	0.5																			1973																																														K		16.3					16.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103605	AAAAA			Nb3Sn0.6Al0.4	Nb	3	Sn	0.6	Al	0.4																			1973																																														K		15.1					15.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103606	AAAAA			Nb3Sn0.61Al0.39	Nb	3	Sn	0.61	Al	0.39																			1973																																														K		14.1					14.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103607	AAAAA			Nb3Sn0.8Al0.2	Nb	3	Sn	0.8	Al	0.2																			1973																																														K		16.9					16.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103608	AAAAA			Nb3Sn0.81Al0.19	Nb	3	Sn	0.81	Al	0.19																			1973																																														K		14.6					14.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103609	AAAAA			Nb3Sn0.9Al0.1	Nb	3	Sn	0.9	Al	0.1																			1973																																														K		18.4					18.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103610	AAAAA			Nb3Sn0.92Al0.08	Nb	3	Sn	0.92	Al	0.08																			1973																																														K		17.9					17.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103611	AAAAA			Nb3Sn0.94Al0.06	Nb	3	Sn	0.94	Al	0.06																			1973																																														K		18					18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103612	AAAAA			Nb3Sn0.96Al0.04	Nb	3	Sn	0.96	Al	0.04																			1973																																														K		18					18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103613	AAAAA			Nb3Al0.81Ge0.19	Nb	3	Al	0.81	Ge	0.19																			1973																																														K		17.6					17.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103614	AAAAA			Nb3Sn0.1Sb0.9	Nb	3	Sn	0.1	Sb	0.9																			1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103615	AAAAA			Nb3Sn0.2Sb0.8	Nb	3	Sn	0.2	Sb	0.8																			1973																																														K					4.2																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103616	AAAAA			Nb3Sn0.25Sb0.75	Nb	3	Sn	0.25	Sb	0.75																			1973																																														K					5																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103617	AAAAA			Nb3Sn0.3Sb0.7	Nb	3	Sn	0.3	Sb	0.7																			1973																																														K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103618	AAAAA			Nb3Sn0.35Sb0.65	Nb	3	Sn	0.35	Sb	0.65																			1973																																														K		10.5					10.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103619	AAAAA			Nb3Sn0.4Sb0.6	Nb	3	Sn	0.4	Sb	0.6																			1973																																														K		12.4					12.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103620	AAAAA			Nb3Sn0.6Sb0.4	Nb	3	Sn	0.6	Sb	0.4																			1973																																														K		15.8					15.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103621	AAAAA			Nb3Sn0.8Ge0.2	Nb	3	Sn	0.8	Ge	0.2																			1973																																														K		18					18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103622	AAAAA			Nb3Sn0.39Ge0.61	Nb	3	Sn	0.39	Ge	0.61																			1973																																														K		7.6					7.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103623	AAAAA			Nb3Sn0.5Ge0.5	Nb	3	Sn	0.5	Ge	0.5																			1973																																														K		12.6					12.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103624	AAAAA			Nb3Sn0.5Zr0.5	Nb	3	Sn	0.5	Zr	0.5																			1973																																														K		16.5					16.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103625	AAAAA			Nb3Rh0.9Co0.1	Nb	3	Rh	0.9	Co	0.1																			1973																																														K		1.9					1.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103626	AAAAA			Nb3Rh0.9Au0.1	Nb	3	Rh	0.9	Au	0.1																			1973																																														K		2.7					2.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103627	AAAAA			Nb3Rh0.95Au0.05	Nb	3	Rh	0.95	Au	0.05																			1973																																														K		2.52					2.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103628	AAAAA			Nb3Rh0.98Au0.02	Nb	3	Rh	0.98	Au	0.02																			1973																																														K		2.53					2.53																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103629	AAAAA			Nb3Si0.5Sn0.5	Nb	3	Si	0.5	Sn	0.5																			1973																																														K		8.3					8.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103630	AAAAA			Nb3Si0.6Sn0.4	Nb	3	Si	0.6	Sn	0.4																			1973																																														K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103631	AAAAA			Nb3In0.5Zr0.5	Nb	3	In	0.5	Zr	0.5																			1973																																														K		6.4					6.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103632	AAAAA			Nb3Ge0.5Ga0.5	Nb	3	Ge	0.5	Ga	0.5																			1973																																														K		7.3					7.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103633	AAAAA			Nb3Al0.39Ge0.61	Nb	3	Al	0.39	Ge	0.61																			1973																																														K		7.3					7.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103634	AAAAA			Nb3Al0.5Ge0.5	Nb	3	Al	0.5	Ge	0.5																			1973																																														K		12.6					12.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103635	AAAAA			Nb3Al0.55Ge0.45	Nb	3	Al	0.55	Ge	0.45																			1973																																														K		11.7					11.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103636	AAAAA			Nb3Al0.62Ge0.38	Nb	3	Al	0.62	Ge	0.38																			1973																																														K		17.2					17.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103637	AAAAA			Nb3Rh0.1Os0.9	Nb	3	Rh	0.1	Os	0.9																			1973																																														K					1.7																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103638	AAAAA			Nb3Rh0.5Os0.5	Nb	3	Rh	0.5	Os	0.5																			1973																																														K					1.7																																																																																																							SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103639	AAAAA			Nb3Rh0.7Os0.3	Nb	3	Rh	0.7	Os	0.3																			1973																																														K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103640	AAAAA			Nb3Rh0.9Os0.1	Nb	3	Rh	0.9	Os	0.1																			1973																																														K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103641	AAAAA			Nb3Rh0.95Os0.05	Nb	3	Rh	0.95	Os	0.05																			1973																																														K		2.39					2.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103642	AAAAA			Nb3Rh0.98Os0.02	Nb	3	Rh	0.98	Os	0.02																			1973																																														K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103643	AAAAA			Nb3Rh0.9Pd0.1	Nb	3	Rh	0.9	Pd	0.1																			1973																																														K		2.55					2.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103644	AAAAA			Nb3Rh0.95Pd0.05	Nb	3	Rh	0.95	Pd	0.05																			1973																																														K		2.49					2.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103645	AAAAA			Nb3Rh0.98Pd0.02	Nb	3	Rh	0.98	Pd	0.02																			1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103646	AAAAA			Nb3Rh0.9Ru0.1	Nb	3	Rh	0.9	Ru	0.1																			1973																																														K		2.44					2.44																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103647	AAAAA			Nb3Rh0.95Ru0.05	Nb	3	Rh	0.95	Ru	0.05																			1973																																														K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103648	AAAAA			Nb3Rh0.98Ru0.02	Nb	3	Rh	0.98	Ru	0.02																			1973																																														K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103649	AAAAA			Nb77.3Sn18.1Al2.3Ge2.3	Nb	77.3	Sn	18.1	Al	2.3	Ge	2.3																	1973																																														K		13					13																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103650	AAAAA			Nb1Ta1V1Sn1	Nb	1	Ta	1	V	1	Sn	1																	1973																																														K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103651	AAAAA			Nb2Ta0.5V0.5Sn1	Nb	2	Ta	0.5	V	0.5	Sn	1																	1973																																														K		12.2					12.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103652	AAAAA			Nb3Rh0.02Pt0.98	Nb	3	Rh	0.02	Pt	0.98																			1973																																														K		9.6					9.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103653	AAAAA			Nb3Rh0.05Pt0.95	Nb	3	Rh	0.05	Pt	0.95																			1973																																														K		8.9					8.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103654	AAAAA			Nb3Rh0.1Pt0.9	Nb	3	Rh	0.1	Pt	0.9																			1973																																														K		7.9					7.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103655	AAAAA			Nb3Rh0.3Pt0.7	Nb	3	Rh	0.3	Pt	0.7																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103656	AAAAA			Nb3Rh0.5Pt0.5	Nb	3	Rh	0.5	Pt	0.5																			1973																																														K		6.25					6.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103657	AAAAA			Nb3Rh0.7Pt0.3	Nb	3	Rh	0.7	Pt	0.3																			1973																																														K		5.1					5.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103658	AAAAA			Nb3Rh0.9Pt0.1	Nb	3	Rh	0.9	Pt	0.1																			1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103659	AAAAA			Nb3Rh0.95Pt0.05	Nb	3	Rh	0.95	Pt	0.05																			1973																																														K		2.53					2.53																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103660	AAAAA			Nb3Rh0.98Pt0.02	Nb	3	Rh	0.98	Pt	0.02																			1973																																														K		2.52					2.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103661	AAAAA			Nb78.5Sn2.2Al9.6Ge9.6	Nb	78.5	Sn	2.2	Al	9.6	Ge	9.6																	1973																																														K		12.7					12.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103662	AAAAA			Nb79.2Sn5.2Al5.2Ge10.4	Nb	79.2	Sn	5.2	Al	5.2	Ge	10.4																	1973																																														K		10.9					10.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103663	AAAAA			Nb79.1Sn9.4Al2.1Ge9.4	Nb	79.1	Sn	9.4	Al	2.1	Ge	9.4																	1973																																														K		8.2					8.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103664	AAAAA			Nb78.5Sn2.2Al12.8Ge6.5	Nb	78.5	Sn	2.2	Al	12.8	Ge	6.5																	1973																																														K		17					17																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103665	AAAAA			Nb77.5Sn5.6Al11.3Ge5.6	Nb	77.5	Sn	5.6	Al	11.3	Ge	5.6																	1973																																														K		15.2					15.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103666	AAAAA			Nb78.1Sn7.3Al7.3Ge7.3	Nb	78.1	Sn	7.3	Al	7.3	Ge	7.3																	1973																																														K		12.5					12.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103667	AAAAA			Nb77.9Sn11.1Al5.5Ge5.5	Nb	77.9	Sn	11.1	Al	5.5	Ge	5.5																	1973																																														K		13					13																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103668	AAAAA			Nb78.4Sn12.9Al2.2Ge6.5	Nb	78.4	Sn	12.9	Al	2.2	Ge	6.5																	1973																																														K		13.3					13.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103669	AAAAA			Nb76Sn2.4Al19.2Ge2.4	Nb	76	Sn	2.4	Al	19.2	Ge	2.4																	1973																																														K		16					16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103670	AAAAA			Nb76.3Sn7.1Al14.3Ge2.3	Nb	76.3	Sn	7.1	Al	14.3	Ge	2.3																	1973																																														K		13.9					13.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103671	AAAAA			Nb76.3Sn10.5Ge2.3Al10.9	Nb	76.3	Sn	10.5	Ge	2.3	Al	10.9																	1973																																														K		14.4					14.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103672	AAAAA			Nb77Sn13.8Al6.9Ge2.3	Nb	77	Sn	13.8	Al	6.9	Ge	2.3																	1973																																														K		13.3					13.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103673	AAAAA			Ag2F1	Ag	2	F	1																					1973																																														K		0.066					0.066																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103674	AAAAA			Ag7F1O8	Ag	7	F	1	O	8																			1973																																													cubic	K		0.3					0.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103675	605	clathrate. Hc1 and G-L parameter (=100)  are at T=0.1 K.		Ag7O11N1	Ag	7	O	11	N	1																			1966																																														K		1.04					1.04											Oe		2																																																																																								METALIC CONDUCTTIVITY AND SUPERCONDUCTIVITY IN SOME SILVER CLATHRATE SALTS				PHYS.REV.LETT.,17(1966)917	D.B.MCWHAN,K.ANDRES,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
103677	AAAAA			Ag7Bf4O8	Ag	7	Bf	4	O	8																			1973																																													cubic	K		0.15					0.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103678	AAAAA			Si21.75V69.43	Si	21.75	V	69.43																					1973																																														K		16.2					16.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103679	AAAAA			Si23.27V75.15	Si	23.27	V	75.15																					1973																																														K		15.94					15.94																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103680	AAAAA			Si22.5V75	Si	22.5	V	75																					1973																																														K		16.4					16.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103681	AAAAA			Si23.8V74.65	Si	23.8	V	74.65																					1973																																														K		16.5					16.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103682	AAAAA			Nb80.7Sn1.9Al1.9Ge15.5	Nb	80.7	Sn	1.9	Al	1.9	Ge	15.5																	1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103683	AAAAA			Nb79.5Sn2.1Al6.1Ge12.3	Nb	79.5	Sn	2.1	Al	6.1	Ge	12.3																	1973																																														K		9.4					9.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103684	AAAAA			Nb79.7Sn6.1Al2Ge12.2	Nb	79.7	Sn	6.1	Al	2	Ge	12.2																	1973																																														K		7.15					7.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103685	AAAAA	carrier = 1.4 E+22 /cm3.		Ag0.1In0.9Te1	Ag	0.1	In	0.9	Te	1																			1973																												NaCl																		K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103686	AAAAA			Al2C1Mo3	Al	2	C	1	Mo	3																			1973																												beta-Mn																	beta-Mn, A13	K		10					10																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103687	AAAAA			Al1Au4	Al	1	Au	4																					1973																												beta-Mn																	beta-Mn, A13	K		0.4					0.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103688	AAAAA			Ag0.94Tl0.06	Ag	0.94	Tl	0.06																					1973																																														K		2.32					2.32																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103689	AAAAA			Ag0.03Tl0.97	Ag	0.03	Tl	0.97																					1973																																														K		2.67					2.67																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103692	605	clathrate	AgO8F0.25(NO3)0.75 	Ag7N0.75O10.25F0.25	Ag	7	N	0.75	O	10.25	F	0.25																	1966																																													cubic	K		0.85					0.85																																																																																																					METALIC CONDUCTTIVITY AND SUPERCONDUCTIVITY IN SOME SILVER CLATHRATE SALTS				PHYS.REV.LETT.,17(1966)917	D.B.MCWHAN,K.ANDRES,M.B.ROBIN,N.A.KUEBLER,T.H.GEBALLE		
103693	AAAAA			Ag1In2	Ag	1	In	2																					1973																												CuAl2																	CuAl2, C16	K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103696	AAAAA			Ag0.8Ga0.2	Ag	0.8	Ga	0.2																					1973																																														K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103699	AAAAA			Al0.8Ge0.2Nb3	Al	0.8	Ge	0.2	Nb	3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		20.7					20.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103700	AAAAA			Al0.5Ge0.5Nb1	Al	0.5	Ge	0.5	Nb	1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		12.6					12.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103702	AAAAA			Al0.131Cr0.088V0.781	Al	0.131	Cr	0.088	V	0.781																			1973																																													cubic	K		1.46					1.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103703	AAAAA			Al2Ca1Si1	Al	2	Ca	1	Si	1																			1973																																														K		5.8					5.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103704	AAAAA			Al2C1Mo3	Al	2	C	1	Mo	3																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103705	AAAAA			Al1	Al	1																							1973																												Cu																	Cu, A1	K		1.17					1.17																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103706	AAAAA			Al1	Al	1																							1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103708	AAAAA	carrier = 1.07 E+22 /cm3		Ag0.2In0.8Te1	Ag	0.2	In	0.8	Te	1																			1973																												NaCl																		K		0.77					0.77																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103709	AAAAA			As1Bi1Pb1	As	1	Bi	1	Pb	1																			1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103711	AAAAA			Al0.108V0.892	Al	0.108	V	0.892																					1973																																													cubic	K		1.82					1.82																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103714	AAAAA			Al2Pt1	Al	2	Pt	1																					1973																												CaF2																	CaF2, C1	K		0.48					0.48																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103715	AAAAA			Al1Pb1	Al	1	Pb	1																					1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103717	AAAAA			Al2N1Nb3	Al	2	N	1	Nb	3																			1973																												beta-Mn																	beta-Mn, A13	K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103720	AAAAA			Al2Mg2	Al	2	Mg	2																					1973																																													cubic	K		0.84					0.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103721	AAAAA	carrier = 2.14 E+22 /cm3		As1Sn1	As	1	Sn	1																					1973																												NaCl																		K		3.41					3.41																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103723	AAAAA			As1Rh1.4	As	1	Rh	1.4																					1973																																													hexagonal	K		0.03					0.03																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103725	AAAAA			As1Pd5	As	1	Pd	5																					1973																																													complex	K		0.46					0.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103729	AAAAA			As0.5Ni0.06Pd0.44	As	0.5	Ni	0.06	Pd	0.44																			1973																																														K		1.39					1.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103730	AAAAA	carrier = 0.97 E+22 /cm3		As0.5In1Te0.5	As	0.5	In	1	Te	0.5																			1973																												NaCl																		K		0.44					0.44																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103731	AAAAA	carrier = 1.24 E+22 /cm3		As0.33In1Te0.67	As	0.33	In	1	Te	0.67																			1973																												NaCl																		K		0.85					0.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103732	AAAAA			As1Bi1Pb1Sb1	As	1	Bi	1	Pb	1	Sb	1																	1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103733	AAAAA			Au1Nb3	Au	1	Nb	3																					1973																												W																	W, A2	K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103736	AAAAA			Au1In1	Au	1	In	1																					1973																																													complex	K		0.4					0.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103737	AAAAA			Au0.4Ge0.6	Au	0.4	Ge	0.6																					1973																																													complex	K		0.32					0.32																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103744	AAAAA			As2Sn3	As	2	Sn	3																					1973																																														K		3.5					3.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103746	AAAAA			Au1Th2	Au	1	Th	2																					1973																												CuAl2																	CuAl2, C16	K		3.08					3.08																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103748	AAAAA			Au5Sn1	Au	5	Sn	1																					1973																												Mg																	Mg, A3	K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103752	AAAAA			Au1Pb3	Au	1	Pb	3																					1973																																														K		4.25					4.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103756	AAAAA			Au0.02Nb3Rh0.98	Au	0.02	Nb	3	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.53					2.53																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103761	AAAAA			B6La1	B	6	La	1																					1973																																														K		5.7					5.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103763	AAAAA			B1C1Mo2	B	1	C	1	Mo	2																			1973																																														K		5.3					5.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103764	AAAAA			B0.03C0.51Mo0.47	B	0.03	C	0.51	Mo	0.47																			1973																																														K		12.5					12.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103765	AAAAA			B1C1Mo2	B	1	C	1	Mo	2																			1973																																														K		5.4					5.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103768	AAAAA			Au1V3	Au	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		0.74					0.74																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103769	AAAAA			Ba0.13O3W1	Ba	0.13	O	3	W	1																			1973																																													tetragonal	K		1.9					1.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103771	AAAAA			B12Zr1	B	12	Zr	1																					1973																																														K		5.82					5.82																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103773	AAAAA			B12Y1	B	12	Y	1																					1973																																														K		4.7					4.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103779	AAAAA			B0.3Ru0.7	B	0.3	Ru	0.7																					1973																												Fe3Th7																	Fe3Th7, D10[2]	K		2.58					2.58																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103781	AAAAA			Bi1Co1	Bi	1	Co	1																					1973																																														K		0.42					0.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103782	AAAAA	cubic,  like Be.		Bi0.5Cd0.25Pb0.25Sn0.12	Bi	0.5	Cd	0.25	Pb	0.25	Sn	0.12																	1973																																														K		8.2					8.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103784	AAAAA			Be1W1	Be	1	W	1																					1973																																													tetragonal	K		4.1					4.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103785	AAAAA	cubic,  like Be.		Be22W1	Be	22	W	1																					1973																																														K		4.12					4.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103787	AAAAA	cubic,  like Be.		Be0.957Re0.043	Be	0.957	Re	0.043																					1973																																														K		9.62					9.62																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103788	AAAAA			Be9.8Re0.02	Be	9.8	Re	0.02																					1973																																													cubic	K		9.5					9.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103789	AAAAA			Be8Nb5Zr2	Be	8	Nb	5	Zr	2																			1973																																														K		5.2					5.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103790	AAAAA	cubic,  like Be.		Be22Mo1	Be	22	Mo	1																					1973																																														K		2.51					2.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103792	AAAAA			Ba0.14O3W1	Ba	0.14	O	3	W	1																			1973																																													hexagonal	K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103794	AAAAA	cubic,  like Be.		Bi2Ir1	Bi	2	Ir	1																					1973																																														K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103795	AAAAA			Bi2Ir1	Bi	2	Ir	1																					1973																																														K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103798	AAAAA			Bi0.34In0.66	Bi	0.34	In	0.66																					1973																																														K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103799	AAAAA			Bi0.15In0.85	Bi	0.15	In	0.85																					1973																																														K		5.3					5.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103800	AAAAA			Bi10.1In0.9	Bi	10.1	In	0.9																					1973																																														K		5.05					5.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103801	AAAAA			Bi0.05In0.95	Bi	0.05	In	0.95																					1973																																														K		4.65					4.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103802	AAAAA			Bi0.019In0.981	Bi	0.019	In	0.981																					1973																																														K		3.86					3.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103805	AAAAA			Bi0.5Pb0.25Sn0.26	Bi	0.5	Pb	0.25	Sn	0.26																			1973																																														K		8.5					8.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103806	AAAAA	cubic,  like Be.		Bi0.5Pb0.31Sn0.19	Bi	0.5	Pb	0.31	Sn	0.19																			1973																																														K		8.5					8.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103807	AAAAA			Bi1Pb1Sb1	Bi	1	Pb	1	Sb	1																			1973																																														K		8.9					8.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103808	AAAAA	cubic,  like Be.		Bi0.06Pb0.95	Bi	0.06	Pb	0.95																					1973																																														K		7.35					7.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103809	AAAAA	cubic,  like Be.		Bi3Ni1	Bi	3	Ni	1																					1973																																														K		4.06					4.06																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103811	AAAAA	cubic,  like Be.		Bi1Nb3	Bi	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		3.05					3.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103814	AAAAA			Bi4Mg1	Bi	4	Mg	1																					1973																																														K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103815	AAAAA	cubic,  like Be.		Bi1Li1	Bi	1	Li	1																					1973																																														K		2.47					2.47																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103819	AAAAA			Bi1Pt1Te1	Bi	1	Pt	1	Te	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.15					1.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103820	AAAAA			Bi1Pt1Se1	Bi	1	Pt	1	Se	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.45					1.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103821	AAAAA			Bi1Pt1	Bi	1	Pt	1																					1973																												NiAs																	NiAs, B8[1]	K		1.21					1.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103822	AAAAA			Bi1Pd1Te1	Bi	1	Pd	1	Te	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103823	AAAAA			Bi1Pd1Se1	Bi	1	Pd	1	Se	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103825	AAAAA	cubic,  like Be.		Bi2Pd1	Bi	2	Pd	1																					1973																																														K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103826	AAAAA	cubic,  like Be.		Pt1Pd1	Pt	1	Pd	1																					1973																																														K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103827	AAAAA	cubic,  like Be.		Bi0.4Pd0.6	Bi	0.4	Pd	0.6																					1973																																														K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103828	AAAAA	beta-type		Bi1Pd2	Bi	1	Pd	2																					1973																															A	3.362		12.983											tetragonal	K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103830	AAAAA	cubic,  like Be.		Bi0.26Tl0.74	Bi	0.26	Tl	0.74																					1973																																														K		4.15					4.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103831	AAAAA	cubic,  like Be.		Bi0.26Tl0.74	Bi	0.26	Tl	0.74																					1973																																														K		4.4					4.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103833	AAAAA			Bi3Te1	Bi	3	Te	1																					1973																																														K		0.75					0.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103838	AAAAA	cubic,  like Be.		Bi3Rh1	Bi	3	Rh	1																					1973																																														K		3.2					3.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103839	AAAAA			Bi1Rh1	Bi	1	Rh	1																					1973																												NiAs			A	4.094		5.663											NiAs, B8[1]	K		2.06					2.06																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103841	AAAAA			C1Hf0.4Nb0.6	C	1	Hf	0.4	Nb	0.6																			1973																												NaCl																	NaCl, B1	K		5.6					5.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103842	AAAAA			C1Hf0.5Nb0.5	C	1	Hf	0.5	Nb	0.5																			1973																												NaCl																	NaCl, B1	K		4.8					4.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103843	AAAAA			C1Hf0.6Nb0.4	C	1	Hf	0.6	Nb	0.4																			1973																												NaCl																	NaCl, B1	K		4.5					4.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103844	AAAAA			C1Hf0.7Nb0.3	C	1	Hf	0.7	Nb	0.3																			1973																												NaCl																	NaCl, B1	K		6.1					6.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103845	AAAAA			C1Hf0.25Mo0.75	C	1	Hf	0.25	Mo	0.75																			1973																												NaCl																	NaCl, B1	K		6.6					6.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103846	AAAAA			C1Hf0.3Mo0.7	C	1	Hf	0.3	Mo	0.7																			1973																												NaCl																	NaCl, B1	K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103847	AAAAA			C1Hf0.5Mo0.5	C	1	Hf	0.5	Mo	0.5																			1973																												NaCl																	NaCl, B1	K		3.4					3.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103848	AAAAA	cubic,  like Be.		C1Ga1Mo2	C	1	Ga	1	Mo	2																			1973																																														K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103849	AAAAA	cubic,  like Be.		C8K1	C	8	K	1																					1973																																														K		0.55					0.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103851	AAAAA			Bi0.3Zn0.7	Bi	0.3	Zn	0.7																					1973																																														K		1.51					1.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103853	AAAAA			C1Mo0.5Ta0.5	C	1	Mo	0.5	Ta	0.5																			1973																												NaCl																	NaCl, B1	K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103854	AAAAA			C1Mo0.2Ta0.8	C	1	Mo	0.2	Ta	0.8																			1973																												NaCl																	NaCl, B1	K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103855	AAAAA			C0.6Mo4.8Si3	C	0.6	Mo	4.8	Si	3																			1973																												Mn5Si3																	Mn5Si3, D8[8]	K		7.6					7.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103856	AAAAA			C0.44Mo0.56	C	0.44	Mo	0.56																					1973																												NaCl																	NaCl, B1	K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103857	AAAAA			C1Mo2	C	1	Mo	2																					1973																																														K		12.2					12.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103858	AAAAA			C1Mo1	C	1	Mo	1																					1973																																														K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103859	AAAAA			C0.4Mo0.6	C	0.4	Mo	0.6																					1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103860	AAAAA			C8K1	C	8	K	1																					1973																																													hexagonal	K		0.39					0.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103861	AAAAA	cubic,  like Be.		C1K1	C	1	K	1																					1973																																													hexagonal	K		0.55					0.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103862	AAAAA			C1Hf0.9Ta0.1	C	1	Hf	0.9	Ta	0.1																			1973																												NaCl																	NaCl, B1	K		5					5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103863	AAAAA			C1Hf0.8Nb0.8	C	1	Hf	0.8	Nb	0.8																			1973																												NaCl																	NaCl, B1	K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103864	AAAAA			C1Hf0.25Nb0.75	C	1	Hf	0.25	Nb	0.75																			1973																												NaCl																	NaCl, B1	K		7					7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103865	AAAAA			C1Nb0.1Zr0.9	C	1	Nb	0.1	Zr	0.9																			1973																												NaCl																	NaCl, B1	K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103866	AAAAA			C1Nb0.6W0.4	C	1	Nb	0.6	W	0.4																			1973																												NaCl																	NaCl, B1	K		12.5					12.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103868	AAAAA			C0.7Nb0.3	C	0.7	Nb	0.3																					1973																												NaCl																	NaCl, B1	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103869	AAAAA	whiskers		C1Nb1	C	1	Nb	1																					1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103870	AAAAA			C0.984Nb1	C	0.984	Nb	1																					1973																												NaCl																	NaCl, B1	K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103871	AAAAA	whiskers		C1Nb1	C	1	Nb	1																					1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103872	AAAAA			C0.1N0.9Nb1	C	0.1	N	0.9	Nb	1																			1973																																														K		8.5					8.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103873	AAAAA			C1Mo0.83Ti0.17	C	1	Mo	0.83	Ti	0.17																			1973																												NaCl																	NaCl, B1	K		10.2					10.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103874	AAAAA			C1Mo0.85Ta0.15	C	1	Mo	0.85	Ta	0.15																			1973																												NaCl																	NaCl, B1	K		8.9					8.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103875	AAAAA			C1Mo0.8Ta0.2	C	1	Mo	0.8	Ta	0.2																			1973																												NaCl																	NaCl, B1	K		8.7					8.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103876	AAAAA			C1Mo0.75Ta0.25	C	1	Mo	0.75	Ta	0.25																			1973																												NaCl																	NaCl, B1	K		8.5					8.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103877	AAAAA			C1W1	C	1	W	1																					1973																																														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103878	AAAAA			C1Ti0.5W0.5	C	1	Ti	0.5	W	0.5																			1973																												NaCl																	NaCl, B1	K		6.7					6.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103879	AAAAA	whiskers		C1Tc1	C	1	Tc	1																					1973																																													cubic	K		3.85					3.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103880	AAAAA			C1Ta0.2Zr0.8	C	1	Ta	0.2	Zr	0.8																			1973																												NaCl																	NaCl, B1	K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103881	AAAAA			C1Ta0.4Ti0.6	C	1	Ta	0.4	Ti	0.6																			1973																												NaCl																	NaCl, B1	K		4.8					4.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103883	AAAAA	whiskers		C1Ta1	C	1	Ta	1																					1973																												NaCl																	NaCl, B1	K		5.09					5.09																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103884	AAAAA			C0.848Ta1	C	0.848	Ta	1																					1973																																														K		2.04					2.04																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103885	AAAAA			C0.987Ta1	C	0.987	Ta	1																					1973																																														K		9.7					9.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103886	AAAAA			C1Ta1	C	1	Ta	1																					1973																																														K		11					11																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103887	AAAAA			C1Re0.06W1	C	1	Re	0.06	W	1																			1973																																														K		5					5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103888	AAAAA			C1Re0.01W1	C	1	Re	0.01	W	1																			1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103889	AAAAA			Cd0.18Tl0.82	Cd	0.18	Tl	0.82																					1973																																														K		2.54					2.54																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103890	AAAAA			Cd0.17Tl0.83	Cd	0.17	Tl	0.83																					1973																																														K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103891	AAAAA			Cd1Sn1	Cd	1	Sn	1																					1973																																														K		3.65					3.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103892	AAAAA			Cd0.97Pd0.03	Cd	0.97	Pd	0.03																					1973																																														K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103893	AAAAA			Cd1Hg1	Cd	1	Hg	1																					1973																																													tetragonal	K		1.77					1.77																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103894	AAAAA			Cd0.3Hg0.7	Cd	0.3	Hg	0.7																					1973																																														K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103895	AAAAA			Ca1Rh2	Ca	1	Rh	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		6.4					6.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103896	AAAAA			Ca1Pb1	Ca	1	Pb	1																					1973																																														K		7					7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103897	AAAAA			Ca0.1O3W1	Ca	0.1	O	3	W	1																			1973																																													hexagonal	K		1.4					1.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103898	AAAAA			Ca1Ir2	Ca	1	Ir	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		6.15					6.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103899	AAAAA			C1W2	C	1	W	2																					1973																																													cubic	K		5.2					5.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103900	AAAAA			C1W2	C	1	W	2																					1973																												Fe2N																	Fe2N, L'[3]	K		2.74					2.74																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103901	AAAAA			Co0.5Rh0.5Si2	Co	0.5	Rh	0.5	Si	2																			1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103902	AAAAA			Co0.02Nb3Rh0.98	Co	0.02	Nb	3	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.28					2.28																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103903	AAAAA			Co1Lu3	Co	1	Lu	3																					1973																																														K		0.35					0.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103906	AAAAA			Ce1Ru2	Ce	1	Ru	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103907	AAAAA			Ce0.005La0.995	Ce	0.005	La	0.995																					1973																																														K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103910	AAAAA			Ce1Co1.67Rh0.33	Ce	1	Co	1.67	Rh	0.33																			1973																												MgCu2(Laves)																	MgCu2, C15	K		0.47					0.47																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103911	AAAAA			Ce1Co1.67Ni0.33	Ce	1	Co	1.67	Ni	0.33																			1973																												MgCu2(Laves)																	MgCu2, C15	K		0.46					0.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103912	AAAAA			Ce1Co2	Ce	1	Co	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		0.84					0.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103913	AAAAA	whiskers		Cr0.6Ir0.4	Cr	0.6	Ir	0.4																					1973																																														K		0.4					0.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103914	AAAAA			Co0.1Zr0.9	Co	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		3.9					3.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103915	AAAAA			Co1Zr2	Co	1	Zr	2																					1973																												CuAl2																	CuAl2, C16	K		6.3					6.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103917	AAAAA			Co0.28Y0.72	Co	0.28	Y	0.72																					1973																																														K		0.34					0.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103919	AAAAA	whiskers		Co1U1	Co	1	U	1																					1973																																														K		1.7					1.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103923	AAAAA			Co1Si2	Co	1	Si	2																					1973																												CaF2																	CaF2, C1	K		1.4					1.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103924	AAAAA			Co0.3Sc0.7	Co	0.3	Sc	0.7																					1973																																														K		0.35					0.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103925	AAAAA			Cr0.017U0.983	Cr	0.017	U	0.983																					1973																																														K		0.75					0.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103926	AAAAA			Cr0.1Ti0.3V0.6	Cr	0.1	Ti	0.3	V	0.6																			1973																																														K		5.6					5.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103927	AAAAA			Cr0.1Ru0.9	Cr	0.1	Ru	0.9																					1973																												Mg																	Mg, A3	K		0.34					0.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103928	AAAAA			Cr2Ru1	Cr	2	Ru	1																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.02					2.02																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103929	AAAAA	whiskers		Cr3Ru1	Cr	3	Ru	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		3.3					3.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103930	AAAAA			Cr0.8Rh0.2	Cr	0.8	Rh	0.2																					1973																												Mg																	Mg, A3	K		0.5					0.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103931	AAAAA			Cr0.4Re0.6	Cr	0.4	Re	0.6																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.15					2.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103932	AAAAA			Cr0.8Os0.2	Cr	0.8	Os	0.2																					1973																																													cubic	K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103933	AAAAA			Cr3Ir1	Cr	3	Ir	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		0.45					0.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103934	AAAAA			Cr0.72Ir0.28	Cr	0.72	Ir	0.28																					1973																																														K		0.83					0.83																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103935	AAAAA	whiskers		Cr0.7Ir0.3	Cr	0.7	Ir	0.3																					1973																																														K		0.76					0.76																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103936	AAAAA	whiskers		Cr0.65Ir0.35	Cr	0.65	Ir	0.35																					1973																																														K		0.59					0.59																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103937	AAAAA			Fe0.05Ni0.05Zr0.9	Fe	0.05	Ni	0.05	Zr	0.9																			1973																																														K		3.9					3.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103938	AAAAA			D0.13Nb1	D	0.13	Nb	1																					1973																																														K		9.12					9.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103941	AAAAA			Cu1Se1Te1	Cu	1	Se	1	Te	1																			1973																												FeS2(marcasite)																	FeS2, C18	K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103943	AAAAA			Cu1S1Se1	Cu	1	S	1	Se	1																			1973																												FeS2(marcasite)																	FeS2, C18	K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103947	AAAAA	whiskers		Cu0.15In0.85	Cu	0.15	In	0.85																					1973																																														K		3.75					3.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103948	AAAAA			Cs0.32O3W1	Cs	0.32	O	3	W	1																			1973																																													hexagonal	K		1.12					1.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103950	AAAAA			Ga0.7Pt0.3	Ga	0.7	Pt	0.3																					1973																												CaF2																	CaF2, C1	K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103952	AAAAA	film made at 10 K 		Ga1N1	Ga	1	N	1																					1973																												ZnS(wurtzite)																	ZnS(wurtzite), B4	K		5.85					5.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103957	AAAAA			Ga0.5Ge0.5Nb3	Ga	0.5	Ge	0.5	Nb	3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		7.3					7.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103958	AAAAA			Fe0.1Zr0.9	Fe	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103961	AAAAA			Ge0.29Nb0.71	Ge	0.29	Nb	0.71																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103962	AAAAA	film made at 10 K 		Ge1Nb3	Ge	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103964	AAAAA			Ge1Mo3	Ge	1	Mo	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.43					1.43																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103965	AAAAA	film made at 10 K 		Ge2La1	Ge	2	La	1																					1973																																														K		1.49					1.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103967	AAAAA			Ga3Zr1	Ga	3	Zr	1																					1973																																														K		1.38					1.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103968	AAAAA			Ga1V4.5	Ga	1	V	4.5																					1973																																														K		9.15					9.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103969	AAAAA			Ga1V2.1	Ga	1	V	2.1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		6.3					6.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103972	AAAAA	film made at 10 K 		Ga1Sb1	Ga	1	Sb	1																					1973																												beta-Sn																	beta-Sn, A5	K		4.24					4.24																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103973	AAAAA			H0.12Ta0.88	H	0.12	Ta	0.88																					1973																																													cubic	K		2.81					2.81																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103974	AAAAA			H0.05Nb0.95	H	0.05	Nb	0.95																					1973																																													cubic	K		7.83					7.83																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103975	AAAAA			H0.1Nb0.9	H	0.1	Nb	0.9																					1973																																													cubic	K		7.38					7.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103976	AAAAA			H00.33Nb0.67	H0	0.33	Nb	0.67																					1973																																													cubic	K		7.28					7.28																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103977	AAAAA			Ge1.62Y1	Ge	1.62	Y	1																					1973																																														K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103980	AAAAA	film made at 10 K 		Ge3Te4	Ge	3	Te	4																					1973																																														K		1.55					1.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103982	AAAAA	film made at 10 K 		Ge3Rh5	Ge	3	Rh	5																					1973																																														K		2.12					2.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103984	AAAAA			Ge0.5Nb3Sn0.5	Ge	0.5	Nb	3	Sn	0.5																			1973																																														K		11.3					11.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103986	AAAAA	film made at 10 K 		Hg2K1	Hg	2	K	1																					1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103988	AAAAA			Hf1V2	Hf	1	V	2																					1973																												MgCu2(Laves)																	MgCu2, C15	K		8.9					8.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103989	AAAAA			Hf0.99Rh0.01	Hf	0.99	Rh	0.01																					1973																																														K		0.85					0.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103990	AAAAA			Hf0.14Re0.86	Hf	0.14	Re	0.86																					1973																												alpha-Mn																	alpha-Mn, A12	K		5.8					5.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103991	AAAAA			Hf1Re2	Hf	1	Re	2																					1973																												MgZn2(Laves)																	MgZn2, C14	K		4.8					4.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103993	AAAAA			Hf0.76Nb0.25	Hf	0.76	Nb	0.25																					1973																																														K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103994	AAAAA			Hf1N0.989	Hf	1	N	0.989																					1973																												NaCl																	NaCl, B1	K		6.6					6.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103995	AAAAA			H0.04Ta0.96	H	0.04	Ta	0.96																					1973																																													cubic	K		3.62					3.62																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103996	AAAAA			H0.08Ta0.92	H	0.08	Ta	0.92																					1973																																													cubic	K		3.26					3.26																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103997	AAAAA			In0.11O3W1	In	0.11	O	3	W	1																			1973																																													hexagonal	K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103998	AAAAA			In0.5Nb3Zr0.5	In	0.5	Nb	3	Zr	0.5																			1973																																														K		6.4					6.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
103999	AAAAA	film made at 10 K 		In1Nb3	In	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104000	AAAAA	film made at 10 K 		In1La3	In	1	La	3																					1973																																														K		9.75					9.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104002	AAAAA			Hg5Tl2	Hg	5	Tl	2																					1973																																														K		3.86					3.86																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104008	AAAAA			Hg4K1	Hg	4	K	1																					1973																																														K		3.27					3.27																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104009	AAAAA			In0.78Tl0.22	In	0.78	Tl	0.22																					1973																																													tetragonal	K		3.18					3.18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104010	AAAAA			In0.62Tl0.38	In	0.62	Tl	0.38																					1973																																														K		2.76					2.76																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104011	AAAAA			In0.8Tl0.2	In	0.8	Tl	0.2																					1973																																														K		3.223					3.223																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104012	AAAAA	film made at 10 K 		In3Te4	In	3	Te	4																					1973																																														K		1.15					1.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104013	AAAAA			In1Te1.002	In	1	Te	1.002																					1973																												NaCl																	NaCl, B1	K		3.5					3.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104014	AAAAA	film made at 10 K 		In0.82Te1	In	0.82	Te	1																					1973																												NaCl																	NaCl, B1	K		1.02					1.02																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104015	AAAAA			In3Sn1	In	3	Sn	1																					1973																																														K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104016	AAAAA	film made at 10 K 		In1Sb1	In	1	Sb	1																					1973																												beta-Sn																	beta-Sn, A5	K		4.8					4.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104017	AAAAA			In1Pb1	In	1	Pb	1																					1973																												CsCl																	CsCl, B2	K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104018	AAAAA			In1Pb1	In	1	Pb	1																					1973																																														K		6.65					6.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104019	AAAAA			In0.98Pb0.02	In	0.98	Pb	0.02																					1973																																														K		3.45					3.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104020	AAAAA			In0.95Pb0.05	In	0.95	Pb	0.05																					1973																																														K		3.6					3.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104021	AAAAA			Ir0.4Nb0.6	Ir	0.4	Nb	0.6																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104022	AAAAA			Ir1Nb3	Ir	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.9					1.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104023	AAAAA			Ir1Mo3	Ir	1	Mo	3																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104032	AAAAA			In0.69Tl0.31	In	0.69	Tl	0.31																					1973																																													cubic	K		2.98					2.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104034	AAAAA			Ir1Sn2	Ir	1	Sn	2																					1973																												CaF2																	CaF2, C1	K		0.65					0.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104035	AAAAA			Ir2.5Sc1	Ir	2.5	Sc	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		2.46					2.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104036	AAAAA			Ir2Sc1	Ir	2	Sc	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		2.07					2.07																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104037	AAAAA			Ir0.5Os0.5	Ir	0.5	Os	0.5																					1973																												MgZn2(Laves)																	MgZn2, C14	K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104038	AAAAA			Ir1Os1Y1	Ir	1	Os	1	Y	1																			1973																												MgCu2(Laves)																	MgCu2, C15	K		2.6					2.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104039	AAAAA			Ir0.265O0.035Ti0.65	Ir	0.265	O	0.035	Ti	0.65																			1973																												Fe3W3C																	Fe3W3C, E9[3]	K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104040	AAAAA			Ir0.287O0.14Ti0.578	Ir	0.287	O	0.14	Ti	0.578																			1973																												Fe3W3C																	Fe3W3C, E9[3]	K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104041	AAAAA			Ir0.05Nb3Rh0.95	Ir	0.05	Nb	3	Rh	0.95																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.38					2.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104042	AAAAA			Ir0.02Nb3Rh0.98	Ir	0.02	Nb	3	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.43					2.43																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104043	AAAAA			Ir1Nb1	Ir	1	Nb	1																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		7.9					7.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104044	AAAAA			Ir0.37Nb0.63	Ir	0.37	Nb	0.63																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.32					2.32																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104046	AAAAA			Ir0.28W0.72	Ir	0.28	W	0.72																					1973																																														K		4.49					4.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104048	AAAAA			Ir1V2	Ir	1	V	2																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.39					1.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104049	AAAAA			Ir1Ti3	Ir	1	Ti	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		5.4					5.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104053	AAAAA			Ir2Th1	Ir	2	Th	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104059	AAAAA	hexagonal La type. 		La0.8Lu0.2	La	0.8	Lu	0.2																					1973																																														K		3.4					3.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104060	AAAAA	hexagonal La type. 		La0.55Lu0.45	La	0.55	Lu	0.45																					1973																																														K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104061	AAAAA	Phys.Let., 15(1965)108		K0.4O3W1	K	0.4	O	3	W	1																			1973																															A	12.3		3.8											tetragonal	K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104062	AAAAA	Phys.Lett., 15(1965)108		K0.27O3W1	K	0.27	O	3	W	1																			1973																															A	7.4		7.6											hexagonal	K		0.5					0.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104063	AAAAA			Ir0.1Zr0.9	Ir	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104066	AAAAA			Ir2Y1	Ir	2	Y	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		1.09					1.09																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104067	AAAAA			Ir0.7Y0.3	Ir	0.7	Y	0.3																					1973																												MgCu2(Laves)																	MgCu2, C15	K		2.16					2.16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104068	AAAAA			Ir0.69Y0.31	Ir	0.69	Y	0.31																					1973																												MgCu2(Laves)																	MgCu2, C15	K		1.98					1.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104072	AAAAA			La3Sc4	La	3	Sc	4																					1973																												Th3P4																	Th3P4, D7[3]	K		8.6					8.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104073	AAAAA			La3S4	La	3	S	4																					1973																												Th3P4																	Th3P4, D7[3]	K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104078	AAAAA			La0.28Pt0.72	La	0.28	Pt	0.72																					1973																												MgCu2(Laves)																	MgCu2, C15	K		0.54					0.54																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104082	AAAAA			M0.62Os0.38	M	0.62	Os	0.38																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		5.65					5.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104083	AAAAA			Mo3Os1	Mo	3	Os	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104088	AAAAA			Mg0.47Tl0.53	Mg	0.47	Tl	0.53																					1973																												CsCl																	CsCl, B2	K		2.75					2.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104091	AAAAA			Lu0.275Rh0.725	Lu	0.275	Rh	0.725																					1973																												MgCu2(Laves)																	MgCu2, C15	K		1.27					1.27																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104094	AAAAA			Mo0.2Ru0.8	Mo	0.2	Ru	0.8																					1973																												Mg																	Mg, A3	K		1.66					1.66																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104095	AAAAA			Mo0.61Ru0.39	Mo	0.61	Ru	0.39																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		7.18					7.18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104096	AAAAA			Mo1Ru1	Mo	1	Ru	1																					1973																												Mg																	Mg, A3	K		9.5					9.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104098	AAAAA			Mo0.6Re0.395	Mo	0.6	Re	0.395																					1973																																														K		10.6					10.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104099	AAAAA			Mo0.57Re0.43	Mo	0.57	Re	0.43																					1973																																														K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104100	AAAAA			Mo0.52Re0.48	Mo	0.52	Re	0.48																					1973																																														K		11.1					11.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104101	AAAAA			Mo0.42Re0.58	Mo	0.42	Re	0.58																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		6.35					6.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104103	AAAAA			Mo3Re1	Mo	3	Re	1																					1973																																														K		0.01					0.01																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104104	AAAAA			Mo0.5Pb0.5	Mo	0.5	Pb	0.5																					1973																												Mg																	Mg, A3	K		3.52					3.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104105	AAAAA			N0.824Nb1	N	0.824	Nb	1																					1973																												NaCl																	NaCl, B1	K		14.4					14.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104106	AAAAA			N0.988Nb1	N	0.988	Nb	1																					1973																												NaCl																	NaCl, B1	K		14.9					14.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104107	AAAAA	film made at 10 K. 		N1Nb1	N	1	Nb	1																					1973																												NaCl																	NaCl, B1	K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104108	AAAAA	whiskers		N1Nb1	N	1	Nb	1																					1973																																														K		16					16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104109	AAAAA	whiskers		N1Nb1	N	1	Nb	1																					1973																																														K		10					10																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104110	AAAAA			Mo2Zr1	Mo	2	Zr	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		4.27					4.27																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104111	AAAAA			Mo0.025Ti0.975	Mo	0.025	Ti	0.975																					1973																																														K		1.8					1.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104112	AAAAA			Mo0.04Ti0.96	Mo	0.04	Ti	0.96																					1973																																													cubic	K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104113	AAAAA			Mo0.913Ti0.087	Mo	0.913	Ti	0.087																					1973																																														K		2.95					2.95																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104114	AAAAA			Mo0.16Ti0.84	Mo	0.16	Ti	0.84																					1973																																														K		4.18					4.18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104115	AAAAA			Mo1Si0.7	Mo	1	Si	0.7																					1973																																														K		1.34					1.34																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104116	AAAAA			Mo3Si1.3	Mo	3	Si	1.3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104118	AAAAA			Na0.28Pb0.72	Na	0.28	Pb	0.72																					1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104119	AAAAA			Na0.28O3W1	Na	0.28	O	3	W	1																			1973																																													tetragonal	K		0.56					0.56																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104120	AAAAA			N0.906Zr1	N	0.906	Zr	1																					1973																												NaCl																	NaCl, B1	K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104121	AAAAA			N1Zr1	N	1	Zr	1																					1973																												NaCl																	NaCl, B1	K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104122	AAAAA			N0.82V1	N	0.82	V	1																					1973																												NaCl																	NaCl, B1	K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104123	AAAAA			N0.6Ti1	N	0.6	Ti	1																					1973																												NaCl																	NaCl, B1	K		1.17					1.17																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104124	AAAAA	whiskers		N1Ta1	N	1	Ta	1																					1973																												NaCl																	NaCl, B1	K		4.84					4.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104125	AAAAA			N1Ta1	N	1	Ta	1																					1973																												NaCl																	NaCl, B1	K		12					12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104126	AAAAA			N0.34Re1	N	0.34	Re	1																					1973																																													cubic	K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104127	AAAAA			N0.93Nb0.85Zr0.15	N	0.93	Nb	0.85	Zr	0.15																			1973																												NaCl																	NaCl, B1	K		13.8					13.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104128	AAAAA	whiskers		N0.7Nb1	N	0.7	Nb	1																					1973																																														K		11.3					11.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104130	AAAAA			Nb0.38Re0.62	Nb	0.38	Re	0.62																					1973																												alpha-Mn																	alpha-Mn, A12	K		2.43					2.43																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104131	AAAAA			Nb3Pt0.02Rh0.98	Nb	3	Pt	0.02	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.52					2.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104132	AAAAA			Nb5Pt3	Nb	5	Pt	3																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		3.73					3.73																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104134	AAAAA			Nb0.62Pt0.38	Nb	0.62	Pt	0.38																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.21					4.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104135	AAAAA			Nb3Pd0.02Rh0.98	Nb	3	Pd	0.02	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.49					2.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104136	AAAAA	whiskers		Nb0.6Pd0.4	Nb	0.6	Pd	0.4																					1973																																														K		1.6					1.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104137	AAAAA			Nb3Os0.02Rh0.98	Nb	3	Os	0.02	Rh	0.98																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104138	AAAAA			Nb0.6Os0.4	Nb	0.6	Os	0.4																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		1.89					1.89																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104139	AAAAA			Nb3Os1	Nb	3	Os	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.05					1.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104140	AAAAA			Nb1Os2	Nb	1	Os	2																					1973																												alpha-Mn																	alpha-Mn, A12	K		2.52					2.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104142	AAAAA	whiskers		Nb1Sn2	Nb	1	Sn	2																					1973																																														K		2.6					2.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104143	AAAAA			Nb0.8Sn0.2	Nb	0.8	Sn	0.2																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		18.18					18.18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104144	AAAAA			Nb3Sn1	Nb	3	Sn	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		18.05					18.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104145	AAAAA			Nb3Si1Sn1V3	Nb	3	Si	1	Sn	1	V	3																	1973																																														K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104146	AAAAA			Nb3Si1	Nb	3	Si	1																					1973																												AuCu3																	AuCu3, L1[2]	K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104147	AAAAA	whiskers		Nb1Se2	Nb	1	Se	2																					1973																												2H-NbSe2																		K		2.2					2.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104148	AAAAA	whiskers		Nb1Se2	Nb	1	Se	2																					1973																												2H-NbSe2																		K		5.15					5.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104149	AAAAA	whiskers		Nb1S2	Nb	1	S	2																					1973																																														K		5					5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104150	AAAAA	whiskers		Nb1S2	Nb	1	S	2																					1973																																														K		6.1					6.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104151	AAAAA			Nb3Rh0.98Ru0.02	Nb	3	Rh	0.98	Ru	0.02																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.42					2.42																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104152	AAAAA	whiskers		Nb0.6Rh0.4	Nb	0.6	Rh	0.4																					1973																																														K		4.21					4.21																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104153	AAAAA			Nb0.88V0.12	Nb	0.88	V	0.12																					1973																												W																	W, A2	K		5.7					5.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104154	AAAAA			Nb0.6Ti0.4	Nb	0.6	Ti	0.4																					1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104155	AAAAA			Nb1Tc3	Nb	1	Tc	3																					1973																												alpha-Mn																	alpha-Mn, A12	K		10.5					10.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104156	AAAAA			Nb2.5Sn1V0.5	Nb	2.5	Sn	1	V	0.5																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		14.2					14.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104157	AAAAA			Nb2Sn1V1	Nb	2	Sn	1	V	1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104158	AAAAA			Nb1Sn1V2	Nb	1	Sn	1	V	2																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104159	AAAAA			Nb2Sn1Ta0.5V0.5	Nb	2	Sn	1	Ta	0.5	V	0.5																	1973																												Cr3Si(A15)																	Cr3Si, A15	K		12.2					12.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104160	AAAAA			Nb1Sn1Ta1V1	Nb	1	Sn	1	Ta	1	V	1																	1973																												Cr3Si(A15)																	Cr3Si, A15	K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104161	AAAAA			Nb2.75Sn1Ta0.25	Nb	2.75	Sn	1	Ta	0.25																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104162	AAAAA			Nb2.5Sn1Ta0.5	Nb	2.5	Sn	1	Ta	0.5																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104163	AAAAA			Nb2Sn1Ta1	Nb	2	Sn	1	Ta	1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104164	AAAAA			Nb1Sn1Ta2	Nb	1	Sn	1	Ta	2																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104165	AAAAA			O3Tl0.03W1	O	3	Tl	0.03	W	1																			1973																																													hexagonal	K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104166	AAAAA			O3Sr0.08W1	O	3	Sr	0.08	W	1																			1973																																													hexagonal	K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104167	AAAAA			O1Ti1	O	1	Ti	1																					1973																																														K		0.58					0.58																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104168	AAAAA	whiskers		O3Sr1Ti1	O	3	Sr	1	Ti	1																			1973																																														K		0.47					0.47																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104169	AAAAA	whiskers		O3Sr1Ti1	O	3	Sr	1	Ti	1																			1973																																														K		0.05					0.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104170	AAAAA	whiskers		O3Sr1Ti1	O	3	Sr	1	Ti	1																			1973																																														K		0.12					0.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104171	AAAAA	Phys.Lett., 15(1965)108		O3Rb0.27W1	O	3	Rb	0.27	W	1																			1973																															A	7.4		7.6											hexagonal	K		1.98					1.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104172	AAAAA			Ni0.1Zr0.9	Ni	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		1.5					1.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104173	AAAAA			Ni1Zr2	Ni	1	Zr	2																					1973																																														K		1.52					1.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104174	AAAAA			Ni0.3Th0.7	Ni	0.3	Th	0.7																					1973																												Fe3Th7																	Fe3Th7, D10[2]	K		1.98					1.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104175	AAAAA			Nb0.66Zr0.33	Nb	0.66	Zr	0.33																					1973																																														K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104176	AAAAA			Nb0.75Zr0.25	Nb	0.75	Zr	0.25																					1973																																														K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104177	AAAAA	whiskers		P3Pd7	P	3	Pd	7																					1973																																														K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104178	AAAAA			P1Pd3	P	1	Pd	3																					1973																												Fe3C																	Fe3C, D0[11]	K		0.35					0.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104182	AAAAA			Os1W3	Os	1	W	3																					1973																																														K		3					3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104186	AAAAA			Os1Re1Y1	Os	1	Re	1	Y	1																			1973																												MgZn2(Laves)																	MgZn2, C14	K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104188	AAAAA			O1V3Zr3	O	1	V	3	Zr	3																			1973																												Fe3W3C																	Fe3W3C, E9[3]	K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104189	AAAAA			Pb1Tl0.17	Pb	1	Tl	0.17																					1973																																														K		6.73					6.73																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104190	AAAAA			Pb1Tl0.27	Pb	1	Tl	0.27																					1973																																														K		6.43					6.43																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104191	AAAAA	whiskers		Pb1Te1	Pb	1	Te	1																					1973																																														K		5.24					5.24																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104192	AAAAA	whiskers		Pb1Te1	Pb	1	Te	1																					1973																																														K		5.19					5.19																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104195	AAAAA	whiskers		Pb4Pt1	Pb	4	Pt	1																					1973																																														K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104198	AAAAA			P1Rh2	P	1	Rh	2																					1973																												CaF2			A	5.516													CaF2, C1	K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104199	AAAAA			P1Rh1	P	1	Rh	1																					1973																																														K		1.22					1.22																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104200	AAAAA	whiskers		P3Pd7	P	3	Pd	7																					1973																																													complex	K		0.7					0.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104201	AAAAA			Pd1Sb1Se1	Pd	1	Sb	1	Se	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104204	AAAAA	whiskers		Pd2.2S1	Pd	2.2	S	1																					1973																																													cubic	K		1.63					1.63																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104205	AAAAA			Pd0.05Ru0.05Zr0.9	Pd	0.05	Ru	0.05	Zr	0.9																			1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104206	AAAAA			Pb0.9Pt0.1Te2	Pb	0.9	Pt	0.1	Te	2																			1973																																														K		1.65					1.65																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104209	AAAAA			Pb1Tl2	Pb	1	Tl	2																					1973																																														K		3.75					3.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104210	AAAAA			Pb1Tl0.04	Pb	1	Tl	0.04																					1973																																														K		7.06					7.06																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104211	AAAAA			Pb1Tl0.075	Pb	1	Tl	0.075																					1973																																														K		6.98					6.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104212	AAAAA			Pb1Tl0.12	Pb	1	Tl	0.12																					1973																																														K		6.88					6.88																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104213	AAAAA			Pd1Te1.02	Pd	1	Te	1.02																					1973																												NiAs																	NiAs, B8[1]	K		2.56					2.56																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104220	AAAAA			Pd2.8Se1	Pd	2.8	Se	1																					1973																																														K		2.3					2.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104221	AAAAA	like Pd4Te                                                                        00003180		Pd6Se1	Pd	6	Se	1																					1973																																														K		0.66					0.66																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104223	AAAAA			Pd1Sb1Te1	Pd	1	Sb	1	Te	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104224	AAAAA			Pd1Sb1Se1	Pd	1	Sb	1	Se	1																			1973																												FeS2(pyrite)																	FeS2(pyrite), C2	K		1					1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104231	AAAAA			Pd0.1Zr0.9	Pd	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104233	AAAAA			Pd1.1Te1	Pd	1.1	Te	1																					1973																												NiAs																	NiAs, B8[1]	K		4.07					4.07																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104234	AAAAA			Pd1Te2.3	Pd	1	Te	2.3																					1973																												CdI2																	CdI2, C6	K		1.85					1.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104235	AAAAA			Pd1Te2.1	Pd	1	Te	2.1																					1973																												CdI2																	CdI2, C6	K		1.89					1.89																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104236	552			Pd1Te2	Pd	1	Te	2																					1965																												CdI2			A	4.036		5.132											CdI2, C6	K		1.69					1.69																																																																																																					The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
104237	AAAAA			Re0.64Ta0.36	Re	0.64	Ta	0.36																					1973																												alpha-Mn																	alpha-Mn, A12	K		1.46					1.46																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104241	AAAAA			Pt2Y8	Pt	2	Y	8																					1973																																														K		0.9					0.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104242	AAAAA			Pt0.5W0.5	Pt	0.5	W	0.5																					1973																												Cu																	Cu, A1	K		1.45					1.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104243	AAAAA			Pt1V3.5	Pt	1	V	3.5																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.26					1.26																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104244	AAAAA			Pt1V3	Pt	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.87					2.87																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104245	AAAAA			Pt1V2.5	Pt	1	V	2.5																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		1.36					1.36																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104246	AAAAA			Pt0.02U0.98	Pt	0.02	U	0.98																					1973																																														K		0.87					0.87																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104249	AAAAA			Rh0.4Ta0.6	Rh	0.4	Ta	0.6																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		2.35					2.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104250	AAAAA			Rh2Sr1	Rh	2	Sr	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104251	AAAAA			Rh0.24Sc0.76	Rh	0.24	Sc	0.76																					1973																																														K		0.88					0.88																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104253	AAAAA			Re6Zr1	Re	6	Zr	1																					1973																												alpha-Mn																	alpha-Mn, A12	K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104256	AAAAA			Re0.5W0.5	Re	0.5	W	0.5																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		5.12					5.12																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104257	AAAAA			Re0.6W0.4	Re	0.6	W	0.4																					1973																																														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104258	AAAAA			Re0.92V0.08	Re	0.92	V	0.08																					1973																												Mg																	Mg, A3	K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104259	AAAAA			Re0.76V0.24	Re	0.76	V	0.24																					1973																												sigma-CrFe																	sigma-CrFe, D8[b]	K		4.52					4.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104260	AAAAA			Re24Ti6	Re	24	Ti	6																					1973																												alpha-Mn																	alpha-Mn, A12	K		6.6					6.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104261	AAAAA	like Pd4Te                                                                        00003180		Rh0.005Zr1	Rh	0.005	Zr	1																					1973																																														K		5.8					5.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104262	AAAAA			Rh1Zr2	Rh	1	Zr	2																					1973																												CuAl2																	CuAl2, C16	K		10.8					10.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104266	AAAAA			Rh1V3	Rh	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		0.38					0.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104267	AAAAA			Rh0.02U0.98	Rh	0.02	U	0.98																					1973																																														K		0.98					0.98																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104271	AAAAA			Rh0.67Te0.33	Rh	0.67	Te	0.33																					1973																																														K		0.49					0.49																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104273	AAAAA	like Pd4Te                                                                        00003180		Sb1Sn1	Sb	1	Sn	1																					1973																																														K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104274	AAAAA			Ru0.1Zr0.9	Ru	0.1	Zr	0.9																					1973																												Mg																	Mg, A3	K		5.7					5.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104275	AAAAA			Ru2Zr1	Ru	2	Zr	1																					1973																												MgZn2(Laves)																	MgZn2, C14	K		1.84					1.84																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104278	AAAAA			Ru0.45V0.55	Ru	0.45	V	0.55																					1973																												CsCl																	CsCl, B2	K		4					4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104279	AAAAA			Ru0.1Ti0.9	Ru	0.1	Ti	0.9																					1973																																														K		3.5					3.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104280	AAAAA			Ru0.05Ti0.95	Ru	0.05	Ti	0.95																					1973																																														K		2.5					2.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104284	AAAAA	like Pd4Te                                                                        00003180		Rh0.1Zr0.9	Rh	0.1	Zr	0.9																					1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104285	AAAAA			Si0.9V3Ge0.1	Si	0.9	V	3	Ge	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		14					14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104286	AAAAA			Si1V2.7Cr0.3	Si	1	V	2.7	Cr	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		11.3					11.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104287	AAAAA			Si10.9V3C0.1	Si	10.9	V	3	C	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104288	AAAAA			Si10.9V3B0.1	Si	10.9	V	3	B	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		15.8					15.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104289	AAAAA			Si10.9V3Al0.1	Si	10.9	V	3	Al	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		14.05					14.05																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104290	AAAAA			Si1V3	Si	1	V	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		17.1					17.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104291	AAAAA	like Pd4Te                                                                        00003180		Si2Th1	Si	2	Th	1																					1973																																														K		2.4					2.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104292	AAAAA	like Pd4Te                                                                        00003180		Si2Th1	Si	2	Th	1																					1973																																														K		3.2					3.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104294	AAAAA			Sb0.01V0.99	Sb	0.01	V	0.99																					1973																												W																	W, A2	K		3.76					3.76																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104295	AAAAA			Sb2Tl7	Sb	2	Tl	7																					1973																																														K		5.2					5.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104296	AAAAA			Sb1Ti3	Sb	1	Ti	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		5.8					5.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104298	AAAAA			Sn1Ta2V1	Sn	1	Ta	2	V	1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		3.7					3.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104299	AAAAA			Sn1Ta1V2	Sn	1	Ta	1	V	2																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.8					2.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104300	AAAAA	like Pd4Te                                                                        00003180		Sn1Ta3	Sn	1	Ta	3																					1973																																														K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104301	AAAAA	like Pd4Te                                                                        00003180		Sn1Ta3	Sn	1	Ta	3																					1973																																														K		8.35					8.35																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104302	AAAAA			Sn0.174Ta0.826	Sn	0.174	Ta	0.826																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104304	AAAAA			Si1V2.7Zr0.3	Si	1	V	2.7	Zr	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		13.2					13.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104305	AAAAA			Si1V2.7Ti0.3	Si	1	V	2.7	Ti	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		10.9					10.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104306	AAAAA			Si1V2.7Ru0.3	Si	1	V	2.7	Ru	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104307	AAAAA			Si1V2.7Nb0.3	Si	1	V	2.7	Nb	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		12.8					12.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104308	AAAAA			Mo0.3Si1	Mo	0.3	Si	1																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		11.7					11.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104309	AAAAA			Ti0.5Zr0.5	Ti	0.5	Zr	0.5																					1973																																														K		2					2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104310	AAAAA	like Pd4Te                                                                        00003180		Ti0.5Zr0.5	Ti	0.5	Zr	0.5																					1973																																														K		1.23					1.23																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104311	AAAAA			Ti0.7V0.3	Ti	0.7	V	0.3																					1973																																													cubic	K		6.14					6.14																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104313	AAAAA			Tc0.6W0.4	Tc	0.6	W	0.4																					1973																																														K		7.88					7.88																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104314	AAAAA			Tc0.5W0.5	Tc	0.5	W	0.5																					1973																																														K		7.52					7.52																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104315	AAAAA			Tc0.1W0.9	Tc	0.1	W	0.9																					1973																																													cubic	K		1.25					1.25																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104316	AAAAA			Ta0.8W0.2	Ta	0.8	W	0.2																					1973																												W																	W, A2	K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104317	AAAAA			Ta0.05V0.095	Ta	0.05	V	0.095																					1973																												W																	W, A2	K		4.3					4.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104318	AAAAA			Ta0.05Ti0.95	Ta	0.05	Ti	0.95																					1973																																													hexagonal	K		2.9					2.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104319	AAAAA			Ta0.025Ti0.975	Ta	0.025	Ti	0.975																					1973																																													hexagonal	K		1.3					1.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104320	AAAAA			Sn0.02V0.98	Sn	0.02	V	0.98																					1973																												W																	W, A2	K		2.87					2.87																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104322	AAAAA			Bi0.52Pb0.32Sn0.16	Bi	0.52	Pb	0.32	Sn	0.16																			1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104323	AAAAA			Bi0.02Pb0.98	Bi	0.02	Pb	0.98																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104324	AAAAA			Bi0.094Pb0.901	Bi	0.094	Pb	0.901																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104325	AAAAA			Bi7.5Pb92.5	Bi	7.5	Pb	92.5																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104326	AAAAA			Bi0.56Pb0.44	Bi	0.56	Pb	0.44																					1973																																														K		8.8					8.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104327	AAAAA			Bi0.5Cd0.1Pb0.27Sn0.13	Bi	0.5	Cd	0.1	Pb	0.27	Sn	0.13																	1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104328	AAAAA			Al1Nb3	Al	1	Nb	3																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104329	AAAAA			Al2C1Mo3	Al	2	C	1	Mo	3																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104330	AAAAA			W2Zr1	W	2	Zr	1																					1973																												MgCu2(Laves)																	MgCu2, C15	K		2.16					2.16																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104331	AAAAA			V0.26Zr0.74	V	0.26	Zr	0.74																					1973																																														K		5.9					5.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104333	AAAAA			Ga1V1.95	Ga	1	V	1.95																					1973																																														K		5.3					5.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104334	AAAAA	like Pd4Te                                                                        00003180		Ga1Sb1	Ga	1	Sb	1																					1973																																														K		4.24					4.24																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104336	AAAAA			Cr0.1Ti0.3V0.6	Cr	0.1	Ti	0.3	V	0.6																			1973																																														K		5.6					5.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104337	AAAAA			Cd0.05Hg0.95	Cd	0.05	Hg	0.95																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104338	AAAAA	like Pd4Te                                                                        00003180		Cd0.1Hg0.9	Cd	0.1	Hg	0.9																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104339	AAAAA			C1Ta1	C	1	Ta	1																					1973																																														K		9					9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104340	AAAAA			C1Nb0.4Ta0.6	C	1	Nb	0.4	Ta	0.6																			1973																																														K		0.01					0.01																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104341	AAAAA			C1Nb1	C	1	Nb	1																					1973																																														K		8					8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104342	AAAAA			C0.44M0.56	C	0.44	M	0.56																					1973																																														K		12.5					12.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104343	AAAAA			C8K1	C	8	K	1																					1973																																														K		0.39					0.39																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104344	AAAAA	like Pd4Te                                                                        00003180		C8K1	C	8	K	1																					1973																																														K		0.55					0.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104345	AAAAA			In1Te1.002	In	1	Te	1.002																					1973																																														K		3.5					3.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104346	AAAAA			In0.17Pb0.83	In	0.17	Pb	0.83																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104347	AAAAA			In0.913Pb0.087	In	0.913	Pb	0.087																					1973																																														K		4.2					4.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104348	AAAAA			In0.94Pb0.06	In	0.94	Pb	0.06																					1973																																														K		3.9					3.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104349	AAAAA			In0.96Pb0.04	In	0.96	Pb	0.04																					1973																																														K		3.68					3.68																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104350	AAAAA			In0.98Pb0.02	In	0.98	Pb	0.02																					1973																																														K		3.45					3.45																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104351	AAAAA			Hg0.15Pb0.85	Hg	0.15	Pb	0.85																					1973																																														K		6.75					6.75																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104352	AAAAA			Hg0.101Pb0.899	Hg	0.101	Pb	0.899																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104353	AAAAA			Hg0.05Pb0.95	Hg	0.05	Pb	0.95																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104354	AAAAA			Ga1V4.5	Ga	1	V	4.5																					1973																																														K		9.15					9.15																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104355	AAAAA			Ga1V3	Ga	1	V	3																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104356	AAAAA			Ga1V2.1	Ga	1	V	2.1																					1973																																														K		6.3					6.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104357	AAAAA			Mo0.913Ti0.037	Mo	0.913	Ti	0.037																					1973																																														K		2.95					2.95																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104358	AAAAA			Mo0.16Ti0.84	Mo	0.16	Ti	0.84																					1973																																														K		4.18					4.18																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104359	AAAAA			Mo0.5Tc0.5	Mo	0.5	Tc	0.5																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104360	AAAAA			Mo0.5Re0.395	Mo	0.5	Re	0.395																					1973																																														K		10.6					10.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104361	AAAAA			Mo0.52Re0.48	Mo	0.52	Re	0.48																					1973																																														K		11.1					11.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104363	AAAAA			La3S4	La	3	S	4																					1973																																														K		6.5					6.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104365	AAAAA			In0.75Tl0.25	In	0.75	Tl	0.25																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104366	AAAAA			In0.83Tl0.17	In	0.83	Tl	0.17																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104367	AAAAA			In0.9Tl0.1	In	0.9	Tl	0.1																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104368	AAAAA			In0.95Tl0.05	In	0.95	Tl	0.05																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104369	AAAAA			Nb1C0.9N0.1	Nb	1	C	0.9	N	0.1																			1973																																														K		16.97					16.97																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104370	AAAAA			Nb1C0.3N0.7	Nb	1	C	0.3	N	0.7																			1973																																														K		17.8					17.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104371	AAAAA			Nb1C0.28N0.78	Nb	1	C	0.28	N	0.78																			1973																																														K		17.9					17.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104372	AAAAA			Si22.5V75	Si	22.5	V	75																					1973																																														K		15.8					15.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104373	AAAAA			Nb1Sc1	Nb	1	Sc	1																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104374	AAAAA			Na0.016Pb0.984	Na	0.016	Pb	0.984																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104375	AAAAA			Na0.086Pb0.914	Na	0.086	Pb	0.914																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104376	AAAAA			N0.93Nb0.85Zr0.15	N	0.93	Nb	0.85	Zr	0.15																			1973																																														K		13.8					13.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104377	AAAAA	like Pd4Te                                                                        00003180		N1Nb1	N	1	Nb	1																					1973																																														K		16.1					16.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104378	AAAAA			N12.8Nb1	N	12.8	Nb	1																					1973																																														K		16.1					16.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104379	AAAAA			Mo0.17Zr0.53	Mo	0.17	Zr	0.53																					1973																																														K																																																																																																												SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104380	AAAAA			Mo0.1U0.9	Mo	0.1	U	0.9																					1973																																														K		1.85					1.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104381	AAAAA			Nb25Ti70Zr5	Nb	25	Ti	70	Zr	5																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104382	AAAAA			Nb25Ti74Zr1	Nb	25	Ti	74	Zr	1																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104383	AAAAA			Nb25Ti75	Nb	25	Ti	75																					1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104384	AAAAA			Nb0.97Cr0.03N1	Nb	0.97	Cr	0.03	N	1																			1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104385	AAAAA			Nb0.99Cr0.01N1	Nb	0.99	Cr	0.01	N	1																			1973																																														K		1.2					1.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104386	AAAAA			Hf1Ti1C1	Hf	1	Ti	1	C	1																			1973																																														K		1.38					1.38																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104387	AAAAA			Hf1Zr1C1	Hf	1	Zr	1	C	1																			1973																																														K		1.68					1.68																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104388	AAAAA			Ti0.5W0.5C1	Ti	0.5	W	0.5	C	1																			1973																																														K		6.7					6.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104389	AAAAA			Hf1Nb1C1	Hf	1	Nb	1	C	1																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104390	AAAAA			Hf1Ta1C1	Hf	1	Ta	1	C	1																			1973																																														K		7.9					7.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104391	AAAAA			Nb0.8W0.2C1	Nb	0.8	W	0.2	C	1																			1973																																														K		12.7					12.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104392	AAAAA			Mo0.95Hf0.05C0.75	Mo	0.95	Hf	0.05	C	0.75																			1973																																														K		14.2					14.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104393	AAAAA			Nb50Zr45Hf5	Nb	50	Zr	45	Hf	5																			1973																																														K		10					10																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104394	AAAAA			Nb50Ti25Zr25	Nb	50	Ti	25	Zr	25																			1973																																														K		9.7					9.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104395	AAAAA			Nb50Ti10Zr40	Nb	50	Ti	10	Zr	40																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104396	AAAAA			Nb50Ti5Zr45	Nb	50	Ti	5	Zr	45																			1973																																														K		10.2					10.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104397	AAAAA			Nb50Zr50	Nb	50	Zr	50																					1973																																														K		10.2					10.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104398	AAAAA			Nb25Zr75	Nb	25	Zr	75																					1973																																														K		8.3					8.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104399	AAAAA			Nb25Ti10Zr65	Nb	25	Ti	10	Zr	65																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104400	AAAAA			Nb25Ti20Zr55	Nb	25	Ti	20	Zr	55																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104401	AAAAA			Nb25Ti30Zr45	Nb	25	Ti	30	Zr	45																			1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104402	AAAAA			Nb25Ti40Zr35	Nb	25	Ti	40	Zr	35																			1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104403	AAAAA			Nb25Ti50Zr25	Nb	25	Ti	50	Zr	25																			1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104404	AAAAA			Nb25Ti65Zr10	Nb	25	Ti	65	Zr	10																			1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104405	SSC0520837			H0.827Pd1	H	0.827	Pd	1																					1984																																														K		1.449					1.449																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104406	SSC0520837			H0.886Pd1	H	0.886	Pd	1																					1984																																														K		3.478					3.478																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104407	AAAAA			Nb5V50Ti45	Nb	5	V	50	Ti	45																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104408	AAAAA			Nb1V50Ti49	Nb	1	V	50	Ti	49																			1973																																														K		7.5					7.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104409	AAAAA			Ti50V50	Ti	50	V	50																					1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104410	AAAAA			Nb49.8Zr24.45Mo25.75	Nb	49.8	Zr	24.45	Mo	25.75																			1973																																														K		5.3					5.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104411	AAAAA			Nb50.2Zr39.4Mo10.4	Nb	50.2	Zr	39.4	Mo	10.4																			1973																																														K		8.8					8.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104412	AAAAA			Nb50.35Zr44.45Mo5.2	Nb	50.35	Zr	44.45	Mo	5.2																			1973																																														K		9.9					9.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104413	AAAAA			Nb50.9Zr48.05Mo1.05	Nb	50.9	Zr	48.05	Mo	1.05																			1973																																														K		9.8					9.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104414	AAAAA			Nb40.6Zr19.9Ta39.5	Nb	40.6	Zr	19.9	Ta	39.5																			1973																																														K		9.9					9.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104415	AAAAA			Nb46Zr36.1Ta17.9	Nb	46	Zr	36.1	Ta	17.9																			1973																																														K		10.3					10.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104416	AAAAA			Nb48.15Zr42.5Ta9.35	Nb	48.15	Zr	42.5	Ta	9.35																			1973																																														K		10.4					10.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104417	AAAAA			Nb50Zr25Hf25	Nb	50	Zr	25	Hf	25																			1973																																														K		10.1					10.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104418	AAAAA			Nb50Zr40Hf10	Nb	50	Zr	40	Hf	10																			1973																																														K		10.1					10.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104419	AAAAA			Nb20Ti75Ta5	Nb	20	Ti	75	Ta	5																			1973																																														K		7.1					7.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104420	AAAAA			Nb24Ti75Ta1	Nb	24	Ti	75	Ta	1																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104421	AAAAA			Nb25Ti50Ta25	Nb	25	Ti	50	Ta	25																			1973																																														K		8.6					8.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104422	AAAAA			Nb25Ti65Ta10	Nb	25	Ti	65	Ta	10																			1973																																														K		8.4					8.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104423	AAAAA			Nb25Ti70Ta5	Nb	25	Ti	70	Ta	5																			1973																																														K		7.85					7.85																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104424	AAAAA			Nb25Ti74Ta1	Nb	25	Ti	74	Ta	1																			1973																																														K		7.55					7.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104425	AAAAA			Nb25Ti75	Nb	25	Ti	75																					1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104426	AAAAA			Nb25V25Ti50	Nb	25	V	25	Ti	50																			1973																																														K		7.3					7.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104427	AAAAA			Nb25V10Ti65	Nb	25	V	10	Ti	65																			1973																																														K		8					8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104428	AAAAA			Nb25V5Ti70	Nb	25	V	5	Ti	70																			1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104429	AAAAA			Nb25Ti75	Nb	25	Ti	75																					1973																																														K		7.2					7.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104430	AAAAA			Nb10V50Ti40	Nb	10	V	50	Ti	40																			1973																																														K		7.1					7.1																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104431	AAAAA			V50Ti49.5Ta0.5	V	50	Ti	49.5	Ta	0.5																			1973																																														K		4.505					4.505																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104432	AAAAA			Ti50V50	Ti	50	V	50																					1973																																														K		4.5					4.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104433	AAAAA			V50Ti40Zr10	V	50	Ti	40	Zr	10																			1973																																														K		5.5					5.5																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104434	AAAAA			V50Ti45Zr5	V	50	Ti	45	Zr	5																			1973																																														K		7					7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104435	AAAAA			V50Ti49Zr1	V	50	Ti	49	Zr	1																			1973																																														K		7.7					7.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104436	AAAAA			Ti50V50	Ti	50	V	50																					1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104437	AAAAA			Nb25Ti50Mo25	Nb	25	Ti	50	Mo	25																			1973																																														K		4.3					4.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104438	AAAAA			Nb25Ti65Mo10	Nb	25	Ti	65	Mo	10																			1973																																														K		6.8					6.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104439	AAAAA			Nb25Ti70Mo5	Nb	25	Ti	70	Mo	5																			1973																																														K		7.4					7.4																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104440	AAAAA			Nb25Ti74Mo1	Nb	25	Ti	74	Mo	1																			1973																																														K		7.3					7.3																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104441	AAAAA			Ta25Ti75	Ta	25	Ti	75																					1973																																														K		6					6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104442	AAAAA			Nb15Ti75Ta10	Nb	15	Ti	75	Ta	10																			1973																																														K		6.7					6.7																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104443	PR0520839	dTc/dP in K/GPa.		Yb1Pd2Sn1	Yb	1	Pd	2	Sn	1																			1984																												Heusler			A	6.657													Cu2MnAl, L2<1>	K		1.82					1.82			K/GPa	0.193																																																							118																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104444	PR0520839	dTc/dP in K/GPa.		Tm1Pd2Sn1	Tm	1	Pd	2	Sn	1																			1984																												Heusler			A	6.668													Cu2MnAl, L2<1>	K		1.92					1.92			K/GPa	0.262																																																							120																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104445	PR0520839	dTc/dP in K/GPa.		Y1Pd2Pb1	Y	1	Pd	2	Pb	1																			1984																												Heusler			A	6.786													Cu2MnAl, L2<1>	K		4.13					4.13			K/GPa	0.195																																																							198																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104446	PR0520839	dTc/dP in K/GPa.		Y1Pd2Sn1	Y	1	Pd	2	Sn	1																			1984																												Heusler			A	6.719													Cu2MnAl, L2<1>	K		5.02					5.02			K/GPa	0.226																																																							165																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104447	PR0520839	dTc/dP in K/GPa.		Sc1Pd2Sn1	Sc	1	Pd	2	Sn	1																			1984																												Heusler			A	6.509													Cu2MnAl, L2<1>	K		2.29					2.29			K/GPa	0.145																																																							232																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104448	AAAAA			V50Ti40Mo10	V	50	Ti	40	Mo	10																			1973																																														K		6.2					6.2																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104449	AAAAA			V50Ti45Mo5	V	50	Ti	45	Mo	5																			1973																																														K		6.9					6.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104450	AAAAA			V50Ti49Mo1	V	50	Ti	49	Mo	1																			1973																																														K		6.9					6.9																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104451	AAAAA			Ti50V50	Ti	50	V	50																					1973																																														K		7.8					7.8																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104452	AAAAA			V50Ti40Ta10	V	50	Ti	40	Ta	10																			1973																																														K		4.6					4.6																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104453	AAAAA			V50Ti45Ta5	V	50	Ti	45	Ta	5																			1973																																														K		4.55					4.55																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104454	AAAAA			V50Ti49Ta1	V	50	Ti	49	Ta	1																			1973																																														K		4.51					4.51																																																																																																					SUPERCONDUCTING MATERIALS			A.A.BAIKOV INSTITUTE OF METALLURGY,ACADEMY OF SCIENCES OF THEUSSR,MOSKOW,	PRENUM PRESS 1973	E.M.SAVITSKII,L.F.MYZENKOVA,M.I.BYCHKOVA,V.V.BARON,YU.V.EFIMOV		
104455	SSC0520837			H0.983Pd1	H	0.983	Pd	1																					1984																																														K		7.355					7.355																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104456	SSC0520837			H0.963Pd1	H	0.963	Pd	1																					1984																																														K		6.377					6.377																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104457	SSC0520837			H0.938Pd1	H	0.938	Pd	1																					1984																																														K		5.523					5.523																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104458	SSC0520837			H0.886Pd1	H	0.886	Pd	1																					1984																																														K		3.478					3.478																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104459	SSC0520837			H0.827Pd1	H	0.827	Pd	1																					1984																																														K		1.449					1.449																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104460	SSC0520837			D0.952Pd1	D	0.952	Pd	1																					1984																																														K		7.536					7.536																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104461	SSC0520837			D0.85Pd1	D	0.85	Pd	1																					1984																																														K		3.558					3.558																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104462	SSC0520837			D0.77Pd1	D	0.77	Pd	1																					1984																																														K		1.449					1.449																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104463	SSC0520837			Pd1T0.81	Pd	1	T	0.81																					1984																																														K		4.087					4.087																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104464	SSC0520837			Pd1T0.786	Pd	1	T	0.786																					1984																																														K		2.493					2.493																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104465	SSC0520837			Pd1T0.734	Pd	1	T	0.734																					1984																																														K		1.449					1.449																																																																																																					SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
104466	PR0520839	dTc/dP in K/GPa.		Lu1Pd2Sn1	Lu	1	Pd	2	Sn	1																			1984																												Heusler			A	6.644													Cu2MnAl, L2<1>	K		3.02					3.02			K/GPa	0.168																																																							118																																										PRESSURE EFFECT ON THE SUPERCONDUCTIVITY OF TERNARY RARE EARTH PALLADIUM HEUSLER ALLOYS	198412	PRESSURE EFFECT          ,HEUSLER ALLOYS	AMES LABORATORY-USDOE AND DEPARTMENT OF PHYSICS IOWA STATE UNIVERSITY,AMES,IOWA,USA	SOLID STATE COMMUN.,52(1984)839	M.J.JOHNSON,R.N.SHELTON	SC,Y,TM,YB,LU,PD,SN,PB	
104467	MAT0130743			Cu1.3Mo6S8	Cu	1.3	Mo	6	S	8																			1978									5.64	kg/mm2	261																	Chevrel			A	9.479		10.34												K		10.3					10.3																																																																																																					Single crystals of Chevrel-type compounds: growth, stoichimetry and electrical resistivity				Mat.Res.Bull., 13(1978)743	R.Flukiger,R.Baillif,E.Walker		
104468	MAT0130743			Cu2Mo6S8	Cu	2	Mo	6	S	8																			1978									5.82	kg/mm2	276																	Chevrel			A	9.605		10.225												K		10.8					10.8																																																																																																single crystals grown by Bridgman-Stockbarger technique.					Single crystals of Chevrel-type compounds: growth, stoichimetry and electrical resistivity				Mat.Res.Bull., 13(1978)743	R.Flukiger,R.Baillif,E.Walker		
104469	PRL0663079	thickness = 1-2 micron.m. 1-1.5 % As-rich GaAs by x-ray analysis. SC observed by microwave absorption.	LT-GaAs	As1Ga1	As	1	Ga	1																				4	1991																																														K		10					10																																																																																																samples were grown by MBE at low temp (200C).					Evidence for superconductivity in low-temperature-grown GaAs	199106		DEPARTMENT PF MATERIALS SCIENCE AND MINERAL ENGINEERING,UNIVERSITY OF CALOFORNIA,BERKELEY,CALIFORNIA 94720	PHYS.REV.LETT.66(1991)3079	E.R.WEBER,J.M.BARANOWSKI,W.-F.YAU,Z.LILIENTAL-WEBER	GA,ASS	
104470	MAT0130743		Cu3Mo6S8	Cu3Mo6S8	Cu	3	Mo	6	S	8																			1978									6.05																			Chevrel			A	9.72		10.213												K		5.5					5.5																																																																																																					Single crystals of Chevrel-type compounds: growth, stoichimetry and electrical resistivity				Mat.Res.Bull., 13(1978)743	R.Flukiger,R.Baillif,E.Walker		
105006	3SC800089	Maki's parameter(alpha)=2.1, e-p coupling=1.15	SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1980																												Chevrel																		K		10.5					10.5																						280									39																																																																													
105007	3SC800079	Maki's parameter(alpha)=1.3, e-p coupling=0.8	Mo6Se8	Mo6Se8	Mo	6	Se	8																					1980																												Chevrel																		K		6.3					6.3																						110									23																																																																						Ternary Superconductors				Proc.Int'l Conf. on Ternary S/C,Lake Geneva,USA,1980,North Holland	B.D.Dunlap,F.Y.Fradin,G.K.Shenoy		
105008	3SC800079	Maki's parameter(alpha)=1.4, e-p coupling=1.0	SnFe0.05Mo6S8	Sn1Fe0.05Mo6S8	Sn	1	Fe	0.05	Mo	6	S	8																	1980																												Chevrel																		K		7.05					7.05																						60									26																																																																						Ternary Superconductors				Proc.Int'l Conf. on Ternary S/C,Lake Geneva,USA,1980,North Holland	B.D.Dunlap,F.Y.Fradin,G.K.Shenoy		
105009	3SC800079	Maki's parameter(alpha)=3.2, e-p coupling=1.25	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1980																												Chevrel																		K		12.7					12.7																						530									60																																																																						Ternary Superconductors				Proc.Int'l Conf. on Ternary S/C,Lake Geneva,USA,1980,North Holland	B.D.Dunlap,F.Y.Fradin,G.K.Shenoy		
105010	3SC800079	Maki's parameter(alpha)=3.0, e-p coupling=1.1	(Sn,Eu)Mo6S8	Sn0.5Eu0.5Mo6S8	Sn	0.5	Eu	0.5	Mo	6	S	8																	1980																												Chevrel																		K		10.2					10.2																						410									56																																																																						Ternary Superconductors				Proc.Int'l Conf. on Ternary S/C,Lake Geneva,USA,1980,North Holland	B.D.Dunlap,F.Y.Fradin,G.K.Shenoy		
105011	3SC800083	R(300K)=61 microOhm.cm, RH(300K)=3.8 E-4 cm3/C	CuxMo6S8	Cu1.6Mo6S8	Cu	1.6	Mo	6	S	8																		3	1980																												Chevrel																		K		11.3					11.3																																																																																																floating zone												
105012	3SC800083	R(300K)=275 microOhm.cm, RH(300K)=5.5 E-4 cm3/C	CuxMo6S8	Cu2.6Mo6S8	Cu	2.6	Mo	6	S	8																		3	1980																												Chevrel																		K		10.5					10.5																																																																																																floating zone												
105013	3SC800083	R(300K)=190 microOhm.cm, RH(300K)=6.0 E-4 cm3/C	CuxMo6S8	Cu2.6Mo6S8	Cu	2.6	Mo	6	S	8																		3	1980																												Chevrel																		K		8					8																																																																																																floating zone												
105014	3SC800083	R(300K)=100 microOhm.cm, RH(300K)=8.0E-4 cm3/C	CuxMo6S8	Cu3.2Mo6S8	Cu	3.2	Mo	6	S	8																		3	1980																												Chevrel																		K		8.5					8.5																																																																																																floating zone												
105015	3SC800083	R(300K)=156 microOhm.cm, RH(300K)=9.0E-4 cm3/C	CuxMo6S8	Cu3.2Mo6S8	Cu	3.2	Mo	6	S	8																		3	1980																												Chevrel																		K		7.6					7.6																																																13																																																floating zone												
105016	PHC2330367	Hirr=81koe	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C			A	3.524		10.535												K		15.5					15.5													83.5									47.6												MHC5016				100					3500																																																					Ar arc-melting-ANN(950C,several days)					Magnetic properties of YNi2B2C superconductor	199411			Physica C.,233(1994) 367-372	E.R.Yacoby,I.Felner,R.Prozorov,Y.Yeshurun	Y,B,Ni,C	
105017	PR04912384	RESRT 22micro Ohm.cm	LaPt2B2C	La1Pt2B2C1	La	1	Pt	2	B	2	C	1																	1994																												LuNi2B2C			A	3.868		10.705												K		10.5					10.5		2											220																									110					1650													mj/mol.K2	4.9																																							arc melting					Superconductivity in RPt2B2C				Phys.Rev.B, 49(1994)12384	R.J.Cava,B.Batlogg,T.Siegrist,J.J.Krajewski,W.F.Peck,,Jr,S.Carter,R.J.Felder,H.Takagi,R.B.van Dover		
105018	PR04912384		LaPt2B2C	La1Pt2.2B2C1	La	1	Pt	2.2	B	2	C	1																	1994																												LuNi2B2C																		K		6.5					6.5		2											65																									90					3550													mj/mol.K2	4.8																																							ANN(1275C,3days)					Superconductivity in RPt2B2C				Phys.Rev.B, 49(1994)12384	R.J.Cava,B.Batlogg,T.Siegrist,J.J.Krajewski,W.F.Peck,,Jr,S.Carter,R.J.Felder,H.Takagi,R.B.van Dover		
105019	PR04912384		PrPt2B2C	Pr1Pt2B2C1	Pr	1	Pt	2	B	2	C	1																	1994																																														K		6					6		2																																																																																																			Superconductivity in RPt2B2C				Phys.Rev.B, 49(1994)12384	R.J.Cava,B.Batlogg,T.Siegrist,J.J.Krajewski,W.F.Peck,,Jr,S.Carter,R.J.Felder,H.Takagi,R.B.van Dover		
105020	PR04912384	broad trunsition	YPt2B2C	Y1Pt2B2C1	Y	1	Pt	2	B	2	C	1																	1994																																														K		10.5					10.5		2																																																																																																			Superconductivity in RPt2B2C				Phys.Rev.B, 49(1994)12384	R.J.Cava,B.Batlogg,T.Siegrist,J.J.Krajewski,W.F.Peck,,Jr,S.Carter,R.J.Felder,H.Takagi,R.B.van Dover		
105021	NAT3720245	RESRT  70micro Ohm.cm	La3Ni2B2N3	La3Ni2B2N3	La	3	Ni	2	B	2	N	3																1	1994																															A	3.721		20.516												K		12.3					12.3		2																																																																																														arc-melted La3Ni2B2 was arc-melted under N2-then ANN(1050C,2days)					Superconductivity in lanthanum nickel boro-nitride	11		AT&T Bell Laboratories,Murray Hill,New Jersey 07974,USA	NATURE.,372(1994)245	B.Batlogg,E.M.Gyorgy,H.Eisali,H.Takagi,H.W.Zandbergen,J.J.Krajewski,R.J.CaVa,S.Uchida,W.F.Peck Jr	La,Ni,B,N	
105022	NAT3720245		LaNiBN	La1Ni1B1N1	La	1	Ni	1	B	1	N	1																1	1994																															A	3.725		7.59												K					4.2																																																																																																		by arc-melting LaNiB under N2,then ANN(950,1000,1050,1100,1150,1200C)					Superconductivity in lanthanum nickel boro-nitride	11		AT&T Bell Laboratories,Murray Hill,New Jersey 07974,USA	NATURE.,372(1994)245	B.Batlogg,E.M.Gyorgy,H.Eisali,H.Takagi,H.W.Zandbergen,J.J.Krajewski,R.J.CaVa,S.Uchida,W.F.Peck Jr	La,Ni,B,N	
105023	JPS0632853	Moment 3.31/f.u	UNi2B2C	U1Ni2B2C1	U	1	Ni	2	B	2	C	1																	1994							-280	218																				LuNi2B2C			A	3.513		10.54												K					4.2																																																																																																		Ar arc-melting,ANN(1000-1100C,4days in Ar)					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
105024	JPS0632853	ferro mag Curie=185KMoment 2.59/f.u	URh2B2C	U1Rh2B2C1	U	1	Rh	2	B	2	C	1																	1994							153																								A	3.782		10.214												K					4.2																																																																																																		Ar arc-melting, ANN(1000-1100C,4days in Ar)					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
105025	JPS0632853		ThNi2B2C	Th1Ni2B2C1	Th	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C			A	3.695		10.197												K		6.5					6.5																																																																																																Ar arc-melting, ANN(1000-1100C, 4days in Ar)					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
105026	JPS0632853		ThRh2B2C	Th1Rh2B2C1	Th	1	Rh	2	B	2	C	1																	1994																															A	3.863		10.177												K					4.2																																																																																																							Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
105027	JPS0632853		ThPt2B2C	Th1Pt2B2C1	Th	1	Pt	2	B	2	C	1																	1994																															A	3.828		10.853												K		6.7					6.7																																																																																																					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
105028	PR05100420	RESRT 139.6 micro Ohm.cmDENS    5.53g/cm3	ThNi2B2C	Th1Ni2B2C1	Th	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C			A	3.683		10.22												K		8.4					8.4													900									1																230					860																																																					arc-melting					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105029	PR05100420	multi phaseRESRT 111.3 micro Ohm.cm	UNi2B2C	U1Ni2B2C1	U	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C			A	3.486		10.7												K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105030	PR05100420		La0.5Th0.5Ni2B2C	La0.5Th0.5Ni2B2C1	La	0.5	Th	0.5	Ni	2	B	2	C	1															1995																												LuNi2B2C			A	3.746		9.929												K		3.9					3.9																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105031	PR05100420		Sc0.5Lu0.5Ni2C2	Sc0.5Lu0.5Ni2B2C1	Sc	0.5	Lu	0.5	Ni	2	B	2	C	1															1995																												LuNi2B2C			A	3.441		10.66												K		15.6					15.6																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105032	PR05100420		La0.5Lu0.5Ni2B2C	La0.5Lu0.5Ni2B2C1	La	0.5	Lu	0.5	Ni	2	B	2	C	1															1995																												LuNi2B2C			A	3.577		10.44												K		14.8					14.8																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105033	PR05100420		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		16.6					16.6																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105034	PR05100420		LaNi2B2C	La1Ni2B2C1	La	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105035	PR05100420		CeNi2B2C	Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105036	PR05100420		PrNi2B2C	Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105037	PR05100420		NdNi2B2C	Nd1Ni2B2C1	Nd	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105038	PR05100420		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		11.1					11.1																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105039	PR05100420		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		10					10																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105040	PR05100420		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		5.8					5.8																																																																																																					Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105041	PR05100420		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105042	PR05100420		GdNi2B2C	Gd1Ni2B2C1	Gd	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					2																																																																																																							Systematic variation of superconductivity for the quaternary borocarbide system  RNi2B2C(R=Sc,Y,La,Th,U, or a lanthanide)	199501			Phys.Rev.B.,51(1995) 420-423	C.C.Lai,H.C.Ku,M.S.Lin,Y.B.You	Ni,B,C,Sc,Y,La,Th,U,R	
105043	PR05100489	(dTc/gamma*Tc) = 3.6.  RESRT = 120micro-Ohm.cm. Moment= 0.18 /f.u	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1995							54																					LuNi2B2C			A	3.526		10.543												K		15.3					15.3																																		MHC5043				80																		mj/mol.K2	8.9		415																																					Y or Er,Ni,B,C were arc-melted under Ar-ANN(1050C,12H in sealed quartz)					Structural, superconducting, and magnetic properties of YNi2B2C and ErNi2B2C	199501			Phys.Rev.B.,51(1995) 489-496	B.D.Padalia,C.Godart,C.Levy-Clement,Chandan Mazumdar,G.Schiffmacher,H.Noel,L.C.Gupta,M.Potel,R.Nagarajan,R.Vijayaraghavan,S.K.Dhar,Zakir Hossain	Y,Ni,B,C,Er	
105044	PR05100489	Sp heat was measured. RESRT=150 micro-Ohm.cm. Moment = 9.32/f.u	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1995							-2																					LuNi2B2C			A	3.503		10.56												K		10.3					10.3																																																																																																Y or Er,Ni,B,C were arc-melted under Ar-ANN(1050C,12H in sealed quartz)					Structural, superconducting, and magnetic properties of YNi2B2C and ErNi2B2C	199501			Phys.Rev.B.,51(1995) 489-496	B.D.Padalia,C.Godart,C.Levy-Clement,Chandan Mazumdar,G.Schiffmacher,H.Noel,L.C.Gupta,M.Potel,R.Nagarajan,R.Vijayaraghavan,S.K.Dhar,Zakir Hossain	Y,Ni,B,C,Er	
105045	PR05012966		LaNi2B2C	La1Rh2B2C1	La	1	Rh	2	B	2	C	1																	1994																												LuNi2B2C			A	3.902		10.246												K					1.4																																																																																																		pellet from powder-arc-melting under Ar					Elementary physical properties and crystal structures of LaRh2B2C and LaIr2B2C	199411			Phys.Rev.B.,50(1994) 12966-12968	B.Batlogg,H.Eisaki,H.Takagi,J.J.Krajewski,R.J.Cava,S.A.Carter,T.Siegrist,W.F.Peck,Jr	La,Rh,B,C,Ir	
105046	PR05012966		LaIr2B2C	La1Ir2B2C1	La	1	Ir	2	B	2	C	1																	1994																												LuNi2B2C			A	3.897		10.454												K					1.4																																																																																																		pellet from powder-arc-melting under Ar					Elementary physical properties and crystal structures of LaRh2B2C and LaIr2B2C	199411			Phys.Rev.B.,50(1994) 12966-12968	B.Batlogg,H.Eisaki,H.Takagi,J.J.Krajewski,R.J.Cava,S.A.Carter,T.Siegrist,W.F.Peck,Jr	La,Rh,B,C,Ir	
105047	PHC2280389	Fig=Hc2. G-L parameter = 11.8	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C																		K		16.6					16.6													800									90									0.8			MHC5047				60					710													mj/mol.K2	35																																							arc melt					Superconducting properties of the new boride-carbide superconductors	199407			Physica C, 228 (1994) 389-392	B.Batlogg,H.Eisaki,H.Takagi,J.J.Krajewski,J.O.Lee,K.Mizuhashi,R.J.Cava,S.Uchida,W.F.Peck Jr		
105048	PHC2280389	Fig=Hc2	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C																		K		15.6					15.6													800									90									0.8			MHC5048				60																																																															Superconducting properties of the new boride-carbide superconductors	199407			Physica C, 228 (1994) 389-392	B.Batlogg,H.Eisaki,H.Takagi,J.J.Krajewski,J.O.Lee,K.Mizuhashi,R.J.Cava,S.Uchida,W.F.Peck Jr		
105049	PHC2280389	Fig=Hc2	YPd5B3C0.3	Y1Pd5B3C0.3	Y	1	Pd	5	B	3	C	0.3																1	1994																																														K		23					23													100									120									0.8			MHC5049				52																																																															Superconducting properties of the new boride-carbide superconductors	199407			Physica C, 228 (1994) 389-392	B.Batlogg,H.Eisaki,H.Takagi,J.J.Krajewski,J.O.Lee,K.Mizuhashi,R.J.Cava,S.Uchida,W.F.Peck Jr		
105050	PHC2270381	(dTc/gamma*Tc) = 1.77.  gao(0)/kTc=1.95	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C																		K		14.6					14.6																																																					MSP5050			mj/mol.K2	18.7		489																																					(arc-melted+Ni2B)-heat(1490C)-cool to 1200C at 10 C/H					Specific heat of single-crystal YNi2B2C and TmNi2B2C superconductors	199407			Physica C, 227(1994)381-386	A.V.Chubukov,B.K.Cho,J.D.Thompson,M.F.Hundley,P.C.Canfield,R.Movshovich	Y,Ni,B,C,Tm	
105051	PHC2270381		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																	1994								1.5																				LuNi2B2C																		K		10.2					10.2																																																					MSP5051			mj/mol.K2	35		320																																					(arc-melted+Ni2B)-heat(1490C)-cool to 1200C at 10C/H					Specific heat of single-crystal YNi2B2C and TmNi2B2C superconductors	199407			Physica C, 227(1994)381-386	A.V.Chubukov,B.K.Cho,J.D.Thompson,M.F.Hundley,P.C.Canfield,R.Movshovich	Y,Ni,B,C,Tm	
105052	PHC2270321	H is parallel to the c-axis. G-L parameter = 14	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C																		K		14.5					14.5													230									32									3.2			MHC5052				100					1500																																																					flux meltod,flux=Ni2B					Superconducting state magnetization and critical fields of single crystal YNi2B2C	199407			Physica C, 227(1994)321-326	B.K.Cho,D.C.Johnson,D.K.Finnemore,J.E.Ostenson,Ming Xu,P.C.Canfield,Z.R.Wang	Y,Ni,B,C	
105053	PHC2430183	small level of impurity phase	Y(Ni,Co)2B2C	Y1Ni1.94Co0.06B2C1	Y	1	Ni	1.94	Co	0.06	B	2	C	1															1995																												LuNi2B2C																		K		11.5					11.5																																																																																																arc-melting in Ar(250Torr),mixture of B and C were pressed before melting					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105054	PHC2430183	small level of impurity phase	Y(Ni,Co)2B2C	Y1Ni1.9Co0.1B2C1	Y	1	Ni	1.9	Co	0.1	B	2	C	1															1995																												LuNi2B2C																		K		9.8					9.8																																																																																																arc-melting in Ar(250Torr),mixture of B and C were pressed before melting					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105055	PHC2430183	small level of impurity phase	Y(Ni,Co)2B2C	Y1Ni1.86Co0.14B2C1	Y	1	Ni	1.86	Co	0.14	B	2	C	1															1995																												LuNi2B2C																		K		7.76					7.76																																																																																																arc-melting in Ar(250Torr),mixture of B and C were pressed before melting					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105056	PHC2430183	small level of impurity phase	Y(Ni,Co)2B2C	Y1Ni1.8Co0.2B2C1	Y	1	Ni	1.8	Co	0.2	B	2	C	1															1995																												LuNi2B2C																		K		6.7					6.7																																																																																																arc-melting in Ar(250Torr),mixture of B and C were pressed before melting					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105057	PHC2430183	small level of impurity phese	Y(Ni,Co)2B2C	Y1Ni1Co1B2C1	Y	1	Ni	1	Co	1	B	2	C	1															1995																												LuNi2B2C																		K		0					0																																																																																																arc-melting in Ar(250Torr),mixture of B and C were pressed before melting					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105058	PHC2430183		Y(Ni,Ru)2B2C	Y1Ni1.98Ru0.02B2C1	Y	1	Ni	1.98	Ru	0.02	B	2	C	1															1995																												LuNi2B2C																		K		12.8					12.8																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105059	PHC2430183		Y(Ni,Ru)2B2C	Y1Ni1.94Ru0.06B2C1	Y	1	Ni	1.94	Ru	0.06	B	2	C	1															1995																												LuNi2B2C																		K		8.7					8.7																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105060	PHC2430183		Y(Ni,Ru)2B2C	Y1Ni1.9Ru0.1B2C1	Y	1	Ni	1.9	Ru	0.1	B	2	C	1															1995																												LuNi2B2C																		K		7					7																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105061	PHC2430183		Y(Ni,Fe)2B2C	Y1Ni1.98Fe0.02B2C1	Y	1	Ni	1.98	Fe	0.02	B	2	C	1															1995																												LuNi2B2C																		K		13.4					13.4																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105062	PHC2430183		Y(Ni,Fe)2B2C	Y1Ni1.94Fe0.06B2C1	Y	1	Ni	1.94	Fe	0.06	B	2	C	1															1995																												LuNi2B2C																		K		10.2					10.2																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105063	PHC2430183		Y(Ni,Fe)2B2C	Y1Ni1.9Fe0.1B2C1	Y	1	Ni	1.9	Fe	0.1	B	2	C	1															1995																												LuNi2B2C																		K		8.2					8.2																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105064	PHC2430183		Y(Ni,Fe)2B2C	Y1Ni1.86Fe0.14B2C1	Y	1	Ni	1.86	Fe	0.14	B	2	C	1															1995																												LuNi2B2C																		K		6.2					6.2																																																																																																					Effect of the Ni site substitution on superconducting properties of YNi2B2C	199502		Centro Brasileiro de Pesquisas Fisicas,CBPF/CNPq,R.Dr. Xavier Sigaud 150,Urca,Rio de Janeiro,RJ,22290-180,Brazil	Physica C.,243(1995)183-186	B.Giordanengo,E.M.Baggio-Saitovitch,J.Mondragon,M.B.Fontes,M.Elmassalami,S.L.Bud'ko,W.Vanoni	Y,Ni,B,C,Co,Fe,Ru	
105065	PHC2330273	carrier=2.9 E+22/cm3	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C																		K		15					15													369									6												MHC5065				81					1030																																																					Ar arc-melting					A uSR determination of the penetration depth in superconducting YNi2B2C	199411			Physica  C.,233(1994) 273-280	E.M.Forgan,M.T.Wylie,M.Warden,R.Bewley,R.Cubitt,R.Cywinski,S.H.Kilcoyne,S.L.Lee,Z.P.Han	Y.Ni.B.C	
105066	PHC2300435		YPd5B3C0.3	Y1Pd5B3C0.3	Y	1	Pd	5	B	3	C	0.3																	1994																																														K		23					23																																																																																																(Y,Pd,B,C,Ni),arc-,melted					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105067	PHC2300435		YPd4.2B3C0.3	Y1Pd4.2B3C0.3	Y	1	Pd	4.2	B	3	C	0.3																	1994																																														K		24					24																																																																																																(Y,Pd,B,C,Ni),arc-,melted					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105068	PHC2300435		YPd5B3C0.3	Y1Pd5B3C0.3	Y	1	Pd	5	B	3	C	0.3																	1994																																														K					4.2																																																																																																		arc-melting,then annealed in vac(900C,48H in Ta-foil)					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105069	PHC2300435		YNi2PdB2C	Y1Ni2Pd	Y	1	Ni	2	Pd																				1994																															A	3.524		10.521												K		16.3					16.3																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105070	PHC2300435		Y(Ni,Pd)2B2C	Y1Ni1.8Pd0.2B2C1	Y	1	Ni	1.8	Pd	0.2	B	2	C	1															1994																												LuNi2B2C			A	3.543		10.58												K		14					14																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105071	PHC2300435		Y(Ni,Pd)2B2C	Y1Ni1.5Pd0.5B2C1	Y	1	Ni	1.5	Pd	0.5	B	2	C	1															1994																												LuNi2B2C			A	3.554		10.641												K		12.1					12.1																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105072	PHC2300435		Y(Ni,Pd)2B2C	Y1Ni1.3Pd0.7B2C1	Y	1	Ni	1.3	Pd	0.7	B	2	C	1															1994																												LuNi2B2C			A	3.576		10.641												K		12.1					12.1																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105073	PHC2300435		YNiPdB2C	Y1Ni1Pd1B2C1	Y	1	Ni	1	Pd	1	B	2	C	1															1994																												LuNi2B2C			A	3.59		10.651												K		11.8					11.8																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105074	PHC2300435		Y(Ni,Pd)2B2C	Y1Ni0.8Pd1.2B2C1	Y	1	Ni	0.8	Pd	1.2	B	2	C	1															1994																												LuNi2B2C			A	3.586		10.64												K		11.8					11.8																																																																																																arc-melting					The 23 K superconducting phase YPd2B2C	199409			Physica C 230 (1994) 435-442	C.W.Chu,I.Rusakova,P.Gautier-Picard,R.L.Meng,Y.Y.Sun,Y.cao	Y.Pd.B.C	
105075	PHC2270063	Hc2 is close to Hirr, 600<penet<1800.   Jc was mesured by M-H loop. G-L parameter = 10.	YPd3B3C0.3	Y1Pd3B3C0.3	Y	1	Pd	3	B	3	C	0.3																	1994																																														K		22					22		2																				9									0.62							60					600																																																					arc-melting (Pd+B)is first melted,then Y,C added					Magnetic properties of superconducting Y-Pd-B-C	199406			Physica C, 227(1994)63-67	C.Kinalidis,C.W.Chu,R.L.Meng,Y.Cao,Y.Y.Xue	Y,Pd,B,C	
105076	PHC2280319	Fig. is for Hc2(p=1), HIR(P=2)	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C																		K		15.5					15.5																																		MHC5076																																																														Y,Ni,B,C were arc melted under Ar-seal in quartz(vac)-ANN(1050C,12H)-cool to RT(5H)					Magnetization studies on YNi2B2C	199407			Physica C, 228 (1994) 319-322	A.K.Pradhan,C.Godart,Chandan Mazumdar,L.C.Gupta,P.Chaddah,R.Nagarajan,S.B.Roy,Zakir Hossain		
105077	PHC2260170		LaPt1.5Au0.6B2C	La1Pt1.5Au0.6B2C1	La	1	Pt	1.5	Au	0.6	B	2	C	1															1994																															A	3.873		10.74												K		10.2					10.2		2																																																																																														powder of Rt,Au,C,B - pellet - (arcmelt in Ar )  - ANN(1050C- 1175C, several days in Ta					Stabilization of superconducting LnPt2B2C by partial substitution of gold for platinum	199406			Physica C, 226 (1994) 170-174	B.Batlogg,H.Takagi,J.J.Krajewski,L.W.Rupp Jr,R.B.van Dover,R.J.Cava,R.J.Felder,R.M.Fleming,S.Carter,T.Siegrist,W.F.Peck Jr		
105078	PHC2260170		CePt1.5Au0.6B2C	Ce1Pt1.5Au0.6B2C1	Ce	1	Pt	1.5	Au	0.6	B	2	C	1															1994																															A	3.851		10.721												K									2																																																																																														powder of Rt,Au,C,B - pellet - (arcmelt in Ar )  - ANN(1050C- 1175C, several days in Ta					Stabilization of superconducting LnPt2B2C by partial substitution of gold for platinum	199406			Physica C, 226 (1994) 170-174	B.Batlogg,H.Takagi,J.J.Krajewski,L.W.Rupp Jr,R.B.van Dover,R.J.Cava,R.J.Felder,R.M.Fleming,S.Carter,T.Siegrist,W.F.Peck Jr		
105079	PHC2260170		PrPt1.5Au0.6B2C	Pr1Pt1.5Au0.6B2C1	Pr	1	Pt	1.5	Au	0.6	B	2	C	1															1994																															A	3.836		10.744												K		6					6		2																																																																																														powder of Rt,Au,C,B - pellet - (arcmelt in Ar )  - ANN(1050C- 1175C, several days in Ta					Stabilization of superconducting LnPt2B2C by partial substitution of gold for platinum	199406			Physica C, 226 (1994) 170-174	B.Batlogg,H.Takagi,J.J.Krajewski,L.W.Rupp Jr,R.B.van Dover,R.J.Cava,R.J.Felder,R.M.Fleming,S.Carter,T.Siegrist,W.F.Peck Jr		
105080	PHC2260170		NdPt1.5Au0.6B2C	Nd1Pt1.5Au0.6B2C1	Nd	1	Pt	1.5	Au	0.6	B	2	C	1															1994																															A	3.829		10.754												K									2																																																																																														powder of Rt,Au,C,B - pellet - (arcmelt in Ar )  - ANN(1050C- 1175C, several days in Ta					Stabilization of superconducting LnPt2B2C by partial substitution of gold for platinum	199406			Physica C, 226 (1994) 170-174	B.Batlogg,H.Takagi,J.J.Krajewski,L.W.Rupp Jr,R.B.van Dover,R.J.Cava,R.J.Felder,R.M.Fleming,S.Carter,T.Siegrist,W.F.Peck Jr		
105081	PR05108398	Beta(lattice term of SP) = 0.51mJ/mol.K4	Sc3.5Dy1.5Ir4Si10	Sc3.5Dy1.5Ir4Si10	Sc	3.5	Dy	1.5	Ir	4	Si	10																	1995								3.6																				Sc5Co4Si10																		K		5					5																																																					SP105081																																											arc-melt in Ar					Superconductivity and magnetism in the Sc5-xDyxIr4Si10system	199504		Tata Institute of Fundamental Research,Bombay,India 400 005	Phys.Rev.B.,51(1995)8398	Aravind D.Chinchure,Girish Chandra,K.Ghosh,Kristian Jonason,S.Ramakrishnan,V.R.Marathe	Sc,Dy,Ir,Si	
105082	PR05108398	e-ph coupling const =0.7. Hc(0)=642Oe. G-L parameter = 8.9.	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1995																												Sc5Co4Si10																		K		8.5					8.5											Oe		114								T	0.82														A	calculated from Hc(0)	200			A	calculated from Hc(0)	1780										SP105082			mj/mol.K2	17.7		315																																					arc-melt in Ar					Superconductivity and magnetism in the Sc5-xDyxIr4Si10system	199504		Tata Institute of Fundamental Research,Bombay,India 400 005	Phys.Rev.B.,51(1995)8398	Aravind D.Chinchure,Girish Chandra,K.Ghosh,Kristian Jonason,S.Ramakrishnan,V.R.Marathe	Sc,Dy,Ir,Si	
105083	JJP0330590	plate like crystal	YPd5B3C	Y1Pd5B3C0.3	Y	1	Pd	5	B	3	C	0.3																	1994																												LuNi2B2C			A	3.8		1.08												K																																																																																																							arc-melting in Ar					Structure and Superconducting Properties of Y-Pd-B-C System	199404			Jpn.J.Appl.Phys.Lett.,33(1994)L590-593	Hazuto Hirata,Hiroaki Kumakura,Hiroki Fujii,Kazumasa Togano,Kazuo Kadowaki,Shozo Ikeda,Shun-ichi Arisawa,Takashi Kimura	Y,Pd,B,C	
105084	PR05106159		Cu1+xCo2-xS4	Cu1Co2S4	Cu	1	Co	2	S	4																			1995																												spinel																		K					0.3																																																																																																							Nuclear spin-lattice relaxation and antiferromagnetic spin correlations in superconducting thiospinel Cu1.5Co1.5S4	199503		Graduate School of Science & Technology,Kobe University,Nada,Kobe 657,Japan	Phys.Rev.B.,51(1995)6159	K.Miyatani,M.Fukugauchi,M.Ishikawa,S.Wada,T.Tnaka,Y.Furukawa	Cu,Co,S	
105085	PR05106159		Cu1+xCo2-xS4	Cu0.9Co1.9S4	Cu	0.9	Co	1.9	S	4																			1995																												spinel																		K		1.6					1.6																																																																																																					Nuclear spin-lattice relaxation and antiferromagnetic spin correlations in superconducting thiospinel Cu1.5Co1.5S4	199503		Graduate School of Science & Technology,Kobe University,Nada,Kobe 657,Japan	Phys.Rev.B.,51(1995)6159	K.Miyatani,M.Fukugauchi,M.Ishikawa,S.Wada,T.Tnaka,Y.Furukawa	Cu,Co,S	
105086	PR05106159		Cu1+xCo2-xS4	Cu1.2Co1.8S4	Cu	1.2	Co	1.8	S	4																			1995																												spinel																		K		2.3					2.3																																																																																																					Nuclear spin-lattice relaxation and antiferromagnetic spin correlations in superconducting thiospinel Cu1.5Co1.5S4	199503		Graduate School of Science & Technology,Kobe University,Nada,Kobe 657,Japan	Phys.Rev.B.,51(1995)6159	K.Miyatani,M.Fukugauchi,M.Ishikawa,S.Wada,T.Tnaka,Y.Furukawa	Cu,Co,S	
105087	PR05106159	u-parameter=0.39  HC1=100Oe at 1.4K	Cu1+xCo2-xS4	Cu1.5Co1.5S4	Cu	1.5	Co	1.5	S	4																			1995																												spinel			A	9.47														K		3.3					3.3																																																																																																					Nuclear spin-lattice relaxation and antiferromagnetic spin correlations in superconducting thiospinel Cu1.5Co1.5S4	199503		Graduate School of Science & Technology,Kobe University,Nada,Kobe 657,Japan	Phys.Rev.B.,51(1995)6159	K.Miyatani,M.Fukugauchi,M.Ishikawa,S.Wada,T.Tnaka,Y.Furukawa	Cu,Co,S	
105088	PHC2230111	stannides. RRR=0.96. sublattice[Sn1-xTmx] is important for SC.	(Sn,Tm)Tm4Rh6Sn18	Tm1Rh1.3Sn4	Tm	1	Rh	1.3	Sn	4																		3	1994			emu.K/g	0.084	myuB/Tm	7.52	-0.68		11.22																	A4B6C18					A	13.72		27.44												K		2.07				0.03	2.07																													T/K		0.415			MHC5088																																					mOhm.cm											0.32														heat(1050C,2h) - cool to 560C(5C/h)					Superconductivity and magnetism of TmRh1.3Sn4.0 single crystals	199404			Physica C, 223(1994)111-116	A.Rojek,C.Sulkowski,K.Rogacki	Tm,Rh,Sn,	
105089	PRL0732364	-Tc=18.4mk	VPt3	Pt3V1	Pt	3	V	1																					1994																																														K		0.508					0.508																																		MHC5089																																																																			Angular Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UPt3	199410		Centre de Recherches sur les Tres Basses Temperatures-Centre National de la Recherche Scientifique,BP166,38042 Grenoble Cedex 9,France	Phys.Rev.Lett.,73(1994)2364	A.Huxley,J.Flouquet,J.L.Tholence,N.Keller	V,Pt	
105090	PR05013879		Lu2Ni3Si5	Lu2Ni3Si5	Lu	2	Ni	3	Si	5																			1994																																														K																																																																																																												Superconductivity in the ternary nickel silicide Lu2Ni3Si5	199411			Phys.Rev.B.,50(1994) 13879-13882	B.D.Padalia,R.Vijayaraghavan	Lu,Ni,Si	
105094	PHC2300159	SP-jump dC = 174 mJ/mol.K2. (dC/gamma*Tc) = 1.43. e-ph coupling = 0.58	Th(Fe1-xCox)3	Fe3Th7	Fe	3	Th	7																					1994																																														K		2.09					2.09																													kOe/K		3.4			MHC105094																						mj/mol.K2	58		178																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
105095	PHC2300159	SP-jump dC = 54 mJ/mol.K2. (dC/gamma*Tc) = 1.53. e-ph coupling = 0.5	Th7(Fe1-xCox)3	Th7Fe1.86Co1.14	Th	7	Fe	1.86	Co	1.14																			1994																																														K		1.07					1.07																																																								mj/mol.K2	33		175																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
105096	PHC2300159	SP-jump dC = 183 mJ/mol.K2. (dC/gamma*Tc) = 1.53. e-ph coupling = 0.61	Th7(Fe1-xCox)3	Th7Fe0.72Co2.28	Th	7	Fe	0.72	Co	2.28																			1994																																														K		2.27					2.27																													kOe/K		8.5			MHC105096																						mj/mol.K2	53		173																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
105097	PHC2300159	SP-jump dC = 117 mJ/mol.K2. (dC/gamma*Tc) = 1.51. e-ph coupling = 0.55	Th7(Fe1-xCox)3	Co3Th7	Co	3	Th	7																					1994																																														K		1.8					1.8																													kOe/K		2.7			MHC105097																						mj/mol.K2	43		184																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
105098	PHC2300159	SP-jump dC = 61 mJ/mol.K2. (dC/gamma*Tc) = 1.45. e-ph coupling = 0.5	Th7(Fe0.81Ni0.19)3	Th7Fe2.43Ni0.57	Th	7	Fe	2.43	Ni	0.57																			1994																																														K		1.05					1.05																																																								mj/mol.K2	40		170																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
105099	PHC2300159	SP-jump dC = 174 mJ/mol.K2. (dC/gamma*Tc) = 1.43. e-ph coupling = 0.58	Th	Th1	Th	1																							1994																																														K		1.36					1.36																																																								mj/mol.K2	4.1		162																																										Low-temperature specific heat of the Th7(Fe,Co,Ni)3 pseudobinary superconductors	199409			Physica C, 230(1994)159-162	G.L.Nieva,J.G.Huber,J.G.Sereni,L.E.DeLong	Th,Fe,Co,Ni	
106002	PR05609021	DOS=0.38/eV.spin	(Y,Ca)C2	Y0.8Ca0.2C2	Y	0.8	Ca	0.2	C	2																			1997																												CaC2			A	3.6844		6.1989												K		2.82					2.82																																																																																																induction heating					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106003	PR05609021	DOS=0.40/eV.spin	(Y,Ca)C2	Y0.7Ca0.3C2	Y	0.7	Ca	0.3	C	2																			1997																												CaC2			A	3.6986		6.2027												K		2.4					2.4																																																																																																induction heating					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106004	PRL0770374		Y2C2I2	Y2C2I2	Y	2	C	2	I	2																		1	1996																																														K		9.97					9.97																																																								mj/mol.K2	8.56																																							heat(1320K, in Ta-crucible)					Bulk superconductivity at 10K in the layered compounds Y2C2I2 and Y2C2Br2			Max-Planck Institute, Stuttgart, Germany	Phys.Rev.Lett., 77(1996)374	A.Simon,R.K.Kremer,R.W.Henn,W.Schnelle		
106005	PRL0770374		Y2C2Br2	Y2C2Br2	Y	2	C	2	Br	2																		1	1996																																														K		5.04					5.04																																																								mj/mol.K2	4.22																																							heat(1320K, in Ta-crucible)					Bulk superconductivity at 10K in the layered compounds Y2C2I2 and Y2C2Br2			Max-Planck Institute, Stuttgart, Germany	Phys.Rev.Lett., 77(1996)374	A.Simon,R.K.Kremer,R.W.Henn,W.Schnelle		
106006	PCH0570211		LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																		1	1996																												skutterudite			A	8.0561													LaFe4P12,	K		7					7																				T		3.65														A		95																																																										high-pressure synthesis(1100C. 4GPa)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure (J.Phys.Chem.Solids)					I.Shirotani,K.Nozawa,K.Tachi,M.Kinoshita,S.Todo,T.Adachi,T.Yagi		
106007	PCH0570211		LaOs4P12	La1Os2P12	La	1	Os	2	P	12																		1	1996																												skutterudite			A	8.0844													LaFe4P12,	K					2																																																																																																		high-pressure synthesis(1100C. 4GPa)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure (J.Phys.Chem.Solids)					I.Shirotani,K.Nozawa,K.Tachi,M.Kinoshita,S.Todo,T.Adachi,T.Yagi		
106008	PCH0570211	Tc is defined as onset in R(T).	LaOsRu3P12	La1Os1Ru3P12	La	1	Os	1	Ru	3	P	12																1	1996																												skutterudite			A	8.065													LaFe4P12,	K		7					7																																																																																																high-pressure synthesis(1100C. 4GPa)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure (J.Phys.Chem.Solids)					I.Shirotani,K.Nozawa,K.Tachi,M.Kinoshita,S.Todo,T.Adachi,T.Yagi		
106009	PCH0570211	Tc is defined as onset in R(T).	LaRu2Os2P12	La1Os2Ru2P12	La	1	Os	2	Ru	2	P	12																1	1996																												skutterudite			A	8.077													LaFe4P12,	K		7					7																																																																																																high-pressure synthesis(1100C. 4GPa)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure (J.Phys.Chem.Solids)					I.Shirotani,K.Nozawa,K.Tachi,M.Kinoshita,S.Todo,T.Adachi,T.Yagi		
106010	PCH0570211		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1996																																														K		13					13																				T		17.5																43.4																																																															Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure (J.Phys.Chem.Solids)					I.Shirotani,K.Nozawa,K.Tachi,M.Kinoshita,S.Todo,T.Adachi,T.Yagi		
106011	PR05609021	G-L = 1.07. GAPENE from SP-heat.	YC2	C2Y1	C	2	Y	1																					1997																												CaC2			A	3.6638		6.177												K		4.02					4.02						0.51	C		-0.17											mT	magnetization	59														A	from Hc2	740			A		810					3.64					SP6011M			mj/mol.K2	2.782		418																																					arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106012	PR05609021	kaizero=12.2E-6 emu/mol, DOS=0.48/eV.spin.fu	YC2	C2Y1	C	2	Y	1																					1997																												CaC2			A	3.6644		6.1762												K		3.98					3.98																																																																																																arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106013	PR05609021	kaizero=14.0E-6 emu/mol, DOS=0.51/eV.spin.fu	YC2	C2Y1	C	2	Y	1																					1997																												CaC2																		K		3.95					3.95																				mT		59												HC106013																																																														arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106014	PR05609021	kaizero=16.0E-6 emu/mol, DOS=0.53/eV.spin.fu	YC2	C2Y1	C	2	Y	1																					1997																												CaC2																		K		3.95					3.95																				mT		60																																																																										arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106015	PR05609021	kaizero=11.6E-6 emu/mol, DOS=0.47/eV.spin.fu	YC2	C1.95Y1	C	1.95	Y	1																					1997																												CaC2			A	3.6637		6.1732												K		3.86					3.86																																																																																																arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106016	PR05609021	kaizero=12.6E-6 emu/mol, DOS=0.50/eV.spin.fu	(Y,Th)C2	Y0.91Th0.09C2	Y	0.91	Th	0.09	C	2																			1997																												CaC2			A	3.6772		6.1938												K		3.7					3.7																																																																																																arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106017	PR05609021	GAPENE from SP-heat.	(Y,Th)C2	Y0.81Th0.19C2	Y	0.81	Th	0.19	C	2																			1997																												CaC2			A	3.6918		6.2119												K		3.52					3.52																																																3.74								mj/mol.K2	3.23		368																																					arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106018	PR05609021	kaizero=16.6E-6 emu/mol, DOS=0.58/eV.spin.fu	(Y,Th)C2	Y0.7Th0.3C2	Y	0.7	Th	0.3	C	2																			1997																												CaC2			A	3.7056		6.2321												K		3.43					3.43																				mT		500																																																																										arc-melting					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106019	PR05609021	GAPENE from SP-heat.	(Y,Ca)C2	Y0.9Ca0.1C2	Y	0.9	Ca	0.1	C	2																			1997																												CaC2			A	3.6804		6.1927												K		3.15					3.15																				mT		300																										3.66								mj/mol.K2	2.82		427																																					induction heating					Electronic properties of the yttriumdicarbide superconductors YC2, Y1-xThxC2, Y1-xCaxC2 (0<x=<0.3)			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	Phys.Rev.B, 56(1997)9021	Th.Gulden,R.W.Henn,O.Jepsen,R.K.Kremer,W.Schnelle,A.Simon,C.Felser		
106020	PR05607866	specific heat jump=1290mJ/mol.K	LaRu4As12	La1Ru4As12	La	1	Ru	4	As	12																			1997																												skutterudite			A	8.5081														K		10.3					10.3																																																					SP6020M			mj/mol.K2	73		233																																					4GPa, (800-900C)					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106021	PR05607866		LaRu4Sb12	La1Ru4Sb12	La	1	Ru	4	Sb	12																			1997																												skutterudite			A	9.27														K		2.8					2.8																																																																																																4GPa, (800-900C)					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106022	PR05607866		PrRu4As12	Pr1Ru4As12	Pr	1	Ru	4	As	12																			1997																												skutterudite			A	8.4963														K		2.4					2.4																																																																																																4GPa, (800-900C)					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106023	PR05607866		LaFe4As12	La1Fe4P12	La	1	Fe	4	P	12																			1997																												skutterudite			A	7.8316														K		4.1					4.1																																																																																																					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106024	PR05607866		LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																			1997																												skutterudite			A	8.0561														K		7.2					7.2																																																																																																					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106025	PR05607866		LaOs4P12	La1Os4P12	La	1	Os	4	P	12																			1997																												skutterudite			A	8.0844														K		1.8					1.8																																																																																																					Superconductivity of filled skutterudites LaRu4As12 and PrRu4As12			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050, Japan	Phys.Rev.B, 56(1997)7866	C.Sekine,I.Shirotani,K.Kanoda,K.Ohno,S.Todo,T.Uchiumi,T.Yagi,Y.Nakazawa		
106026	LTP0540149			C1.35La1	C	1.35	La	1																					1984																												Pu2C3			A	8.8095														K		11					11																																																								mj/mol.K2	4.8		318																																										Specific Heat Studies of Lanthanum and Yttrium Sesquicarbides*			Los Alamos National Laboratory, Los Aloamos, New Mexico	J.Low Temp.Phys.54(1984)149	A.L. Giorgi,B. Cort,G.R. Stewart		
106027	LTP0540149			La1.9Th0.1C1.35	La	1.9	Th	0.1	C	1.35																			1984																												Pu2C3			A	8.788														K		12.7					12.7																																																								mj/mol.K2	2.3		274																																										Specific Heat Studies of Lanthanum and Yttrium Sesquicarbides*			Los Alamos National Laboratory, Los Aloamos, New Mexico	J.Low Temp.Phys.54(1984)149	A.L. Giorgi,B. Cort,G.R. Stewart		
106028	LTP0540149			C1.35Y1	C	1.35	Y	1																					1984																												Pu2C3			A	8.2283														K		10					10																																																								mj/mol.K2	2.8		557																																										Specific Heat Studies of Lanthanum and Yttrium Sesquicarbides*			Los Alamos National Laboratory, Los Aloamos, New Mexico	J.Low Temp.Phys.54(1984)149	A.L. Giorgi,B. Cort,G.R. Stewart		
106029	LTP0540149			Y0.7Th0.3C1.35	Y	0.7	Th	0.3	C	1.35																			1984																												Pu2C3			A	8.362														K		17					17																																																								mj/mol.K2	4.7		346																																										Specific Heat Studies of Lanthanum and Yttrium Sesquicarbides*			Los Alamos National Laboratory, Los Aloamos, New Mexico	J.Low Temp.Phys.54(1984)149	A.L. Giorgi,B. Cort,G.R. Stewart		
106030	PR0368660			La1Fe4P12	La	1	Fe	4	P	12																		3	1987																												skutterudite																		K		4					4																																																																																																Sn-flux method					Low-temperature properties of rare-earth and actinide iron phosphide compounds MFe4P12(M=La, Pr, Nd, and Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B,36(1987)8660	C. Rossel,G.P. Meisner,J.W. Chen,M.B. Maple,M.S. Torikachvili,M.W. McElfresh,R.P. Guertin,Y. Dalichaouch		
106031	PR0368660	Ferromagnetic below 2K		Nd1Fe4P12	Nd	1	Fe	4	P	12																		3	1987							2																					skutterudite																		K					1.2																																																																																																		Sn-flux method					Low-temperature properties of rare-earth and actinide iron phosphide compounds MFe4P12(M=La, Pr, Nd, and Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B,36(1987)8660	C. Rossel,G.P. Meisner,J.W. Chen,M.B. Maple,M.S. Torikachvili,M.W. McElfresh,R.P. Guertin,Y. Dalichaouch		
106032	PR0368660	antiferromagnetic below 6.2K		Pr1Fe4P12	Pr	1	Fe	4	P	12																		3	1987								6.2																				skutterudite																		K					1.2																																																																																																		Sn-flux method					Low-temperature properties of rare-earth and actinide iron phosphide compounds MFe4P12(M=La, Pr, Nd, and Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B,36(1987)8660	C. Rossel,G.P. Meisner,J.W. Chen,M.B. Maple,M.S. Torikachvili,M.W. McElfresh,R.P. Guertin,Y. Dalichaouch		
106033	NAT3920580	Li0.48(THF)yHfNCl, THF=C4H4O, y=0.3 - 0.4	beta-HfNCl, Li0.48(THF)yHfNCl	Hf1N1Cl1	Hf	1	N	1	Cl	1																			1998																												CdCl2			A	3.573		27.68												K		25.5					25.5																																																																																																beta-HfNCl by reaction of Hf powder and NH4Cl.					Superconductivity at 25.5 K in electron-doped layered hafnium nitride	4		Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Nature.392(1998)580	Hitoshi Kawaji,Ken-ichi Hotehama,Shoji Yamanaka		
106034	NAT3920580		bata-ZrNCl	Zr1N1Cl1	Zr	1	N	1	Cl	1																			1998																															A	3.606		27.67												K		13					13																																																																																																					Superconductivity at 25.5 K in electron-doped layered hafnium nitride	4		Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Nature.392(1998)580	Hitoshi Kawaji,Ken-ichi Hotehama,Shoji Yamanaka		
106035	PRL0741427	silicon clathrate	Ba6Na2Si46	Na2.9Ba4.5Si46	Na	2.9	Ba	4.5	Si	46																			1995																												clathrate			A	10.26														K		3.5					3.5		2																																																																																														Nasi, BaSi2, finstly,					Superconductivity in the Silicon Clathrate Compound(Na,Ba)xSi46	199502		Department of Applied Chemistry,Faculty of Engineering,Hiroshima University,Higashi-Hiroshima 724,Japan	Phys.Rev.Lett.,74(1995)1427	Hiro-omi,Hiro-omi Horie,Hitoshi Kawaji,Mitsuo Ishikawa,Shoji Yamanaka,Syoji Yamanaka	Na,Ba,Si	
106036	SSC0920341	multi-phase, Meissner volume fraction is very small. S/C phase is not determined	YPd4BC0.2	Y1Pd4B1C0.2	Y	1	Pd	4	B	1	C	0.2																1	1994																																														K		21					21		2																																																																																														arc melting					SUPERCONDUCTIVITY AT 22 AND 10K IN THE QUATERNARY BOROCARBIDES PRd4BCx(R=Y, Lu)			Tata Institute of Fundamental Research,Bombey 400 005, India	Solid State Commun.92(1994)341	B.D. Padaria,C. Gosart,C. Levy-Clement,Chandan Mazumdar,L.C. Gupta,R. Nagarajan,R. Vijayaraghavan,S.K. Dhar,Zakir Hossain		
106037	SSC0920341	multi-phase,resistivity shows non-zero at 4.2K	YPd4B	Y1Pd4B1	Y	1	Pd	4	B	1																			1994																																														K					4.2																																																																																																		arc melting					SUPERCONDUCTIVITY AT 22 AND 10K IN THE QUATERNARY BOROCARBIDES PRd4BCx(R=Y, Lu)			Tata Institute of Fundamental Research,Bombey 400 005, India	Solid State Commun.92(1994)341	B.D. Padaria,C. Gosart,C. Levy-Clement,Chandan Mazumdar,L.C. Gupta,R. Nagarajan,R. Vijayaraghavan,S.K. Dhar,Zakir Hossain		
106038	SSC0920341		LuPd4BC0.2	Lu1Pd4B1C0.2	Lu	1	Pd	4	B	1	C	0.2																	1994																																														K		10					10		2																																																																																														arc melting					SUPERCONDUCTIVITY AT 22 AND 10K IN THE QUATERNARY BOROCARBIDES PRd4BCx(R=Y, Lu)			Tata Institute of Fundamental Research,Bombey 400 005, India	Solid State Commun.92(1994)341	B.D. Padaria,C. Gosart,C. Levy-Clement,Chandan Mazumdar,L.C. Gupta,R. Nagarajan,R. Vijayaraghavan,S.K. Dhar,Zakir Hossain		
106039	SSC1000393	Si-clathrate	(Na,Ba)Si46	Na1.5Ba6Si46	Na	1.5	Ba	6	Si	46																			1996																												clathrate																		K		2.6					2.6																																																																																																solid state reaction (NaSi+BaSi2					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SILICON CLATHRATE COMPOUND NaxBa6Si46			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 729, Japan	Solid State Commun.100(1996)393	Hitoshi Kawaji,Kazuhito Iwai,Mitsuo Ishikawa,Shoji Yamanaka		
106040	SSC1000393	Si-clathrate	(Na,Ba)Si46	Na0.3Ba6.2Si46	Na	0.3	Ba	6.2	Si	46																			1996																												clathrate																		K		4					4																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SILICON CLATHRATE COMPOUND NaxBa6Si46			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 729, Japan	Solid State Commun.100(1996)393	Hitoshi Kawaji,Kazuhito Iwai,Mitsuo Ishikawa,Shoji Yamanaka		
106041	SSC1000393	Si-clathrate	(Na,Ba)Si46	Na0.2Ba6Si46	Na	0.2	Ba	6	Si	46																			1996																												clathrate																		K		4.8					4.8																																																																																																					COMPOSITION DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF SILICON CLATHRATE COMPOUND NaxBa6Si46			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 729, Japan	Solid State Commun.100(1996)393	Hitoshi Kawaji,Kazuhito Iwai,Mitsuo Ishikawa,Shoji Yamanaka		
106042	PHC2450012	structure is trigonal	BaSi2	Ba1Si2	Ba	1	Si	2																					1995																															A	4.06		5.28												K		5.3					5.3																																																																																																ortho BaSi2-press(5.5GPa,400C,2H)					Superconductivity of trigonal BaSi2	199504		National Research Institute for Metals,1-2-1 Sengen,Tsukuba,Ibaraki 305,Japan	Physica C.,245(1995)12-14	Kazuto Hirata,Motoharu Imai,Toshiyuki Hirano		
106043	PHC2510183	FIG shows Hc2(T), Hc1(0). G-L parameter = 10.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C			A	3.5351		10.5598												K		13.8					13.8											Oe		800							KOe		80												HC6043M		A		60			A		480																																																					melt with 2-4% excess Y					Field and temperature dependent transport and mabnetic properties of superconducting YNi2B2C	199509		(a)Department of Physics,University of Manitoba,Winnipeg MB, Canada R3T 2N2	Physica C,251(1995)183-191	Gwyn williams (b),H.P. Kunkel (a),J.A. Cowen (b),P.A. Stampe (a),X.Z. Zhou (a)	Y, Ni, B, C	
106044	PRL0770163		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																3	1996								5.2																				LuNi2B2C																		K		8.5					8.5																																																																																																Ni2B high-temp. flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106045	PRL0770163		PrRu4As12	Ho0.9Dy0.1Ni2B2C1	Ho	0.9	Dy	0.1	Ni	2	B	2	C	1														3	1996								5.6																				LuNi2B2C																		K		8					8																																																																																																Ni2B high-temp.flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106046	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.85Dy0.15Ni2B2C1	Ho	0.85	Dy	0.15	Ni	2	B	2	C	1														3	1996								5.9																				LuNi2B2C																		K		7.9					7.9																																																																																																Ni2B high-temp.flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106047	PRL0770163		(Ho,Dy)Ni2B2C	Ho1.8Dy0.2Ni2B2C1	Ho	1.8	Dy	0.2	Ni	2	B	2	C	1														3	1996								6.2																				LuNi2B2C																		K		6.6					6.6																																																																																																Ni2B high-temp.flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106048	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.7Dy0.3Ni2B2C1	Ho	0.7	Dy	0.3	Ni	2	B	2	C	1														3	1996								6.7																				LuNi2B2C																		K		5.8					5.8	MTC106048																																																																																															Ni2B high-temp.flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106049	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.65Dy0.35Ni2B2C1	Ho	0.65	Dy	0.35	Ni	2	B	2	C	1														3	1996								6.9																				LuNi2B2C																		K		5.9					5.9																																																																																																Ni2B high-temp.flux growth method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106050	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.6Dy0.4Ni2B2C1	Ho	0.6	Dy	0.4	Ni	2	B	2	C	1														3	1996								7.2																				LuNi2B2C																		K		6					6																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106051	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.5Dy0.5Ni2B2C1	Ho	0.5	Dy	0.5	Ni	2	B	2	C	1														3	1996								7.6																				LuNi2B2C																		K		5.9					5.9																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106052	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.4Dy0.6Ni2B2C1	Ho	0.4	Dy	0.6	Ni	2	B	2	C	1														3	1996								8																				LuNi2B2C																		K		5.85					5.85																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106053	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.2Dy0.8Ni2B2C1	Ho	0.2	Dy	0.8	Ni	2	B	2	C	1														3	1996								9																				LuNi2B2C																		K		6.23					6.23																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106054	PRL0770163		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1996								10.2																				LuNi2B2C																		K		6.23					6.23																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106055	PRL0770163		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1996																												LuNi2B2C																		K		15.9					15.9																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106056	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.8Dy0.2Ni2B2C1	Lu	0.8	Dy	0.2	Ni	2	B	2	C	1															1996																												LuNi2B2C																		K		11.8					11.8																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106057	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.6Dy0.4Ni2B2C1	Lu	0.6	Dy	0.4	Ni	2	B	2	C	1															1996																												LuNi2B2C																		K		7.5					7.5																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106058	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.4Dy0.6Ni2B2C1	Lu	0.4	Dy	0.6	Ni	2	B	2	C	1															1996																												LuNi2B2C																		K		4.3					4.3	MTC106058																																																																																																				Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106059	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.3Dy0.7Ni2B2C1	Lu	0.3	Dy	0.7	Ni	2	B	2	C	1															1996																												LuNi2B2C																		K		2					2																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106060	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.25Dy0.75Ni2B2C1	Lu	0.25	Dy	0.75	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K																																																																																																												Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106061	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.15Dy0.85Ni2B2C1	Lu	0.15	Dy	0.85	Ni	2	B	2	C	1														3	1996								7																				LuNi2B2C																		K																																																																																																												Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106062	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.1Dy0.9Ni2B2C1	Lu	0.1	Dy	0.9	Ni	2	B	2	C	1														3	1996								8.4																				LuNi2B2C																		K		2.5					2.5																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106063	PRL0770163		(Lu,Dy)Ni2B2C	Lu0.05Dy0.95Ni2B2C1	Lu	0.05	Dy	0.95	Ni	2	B	2	C	1														3	1996								9.2																				LuNi2B2C																		K		4.3					4.3																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106064	PRL0770163		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1996								10.3																				LuNi2B2C																		K		6.2					6.2																																																																																																					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
106065	PHC3000067	volume fraction=80%	EuNd2S5	Eu1Nd2S5	Eu	1	Nd	2	S	5																			1998																															A	3.3556		23.44												K		3					3																																																																																																mixture of EuS,Nb,S-silica tube-hear(1050C,48H					A new superconducting sulfide-EuNb2S5	199805		Chemical Department, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,300(1998)67-70	A. Yu. Grippa,E.V. Antipov,G. Svensson,J.L. Tholence,O.G. D'yachenko,S.Ya. Istomin		
106066	JSC1160392	S/C volum=65%, Rn(5K)=28 microOhm, cm	BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																		1	1995																															A	3.3204		25.005												K		3.14					3.14																																																																																											RH6066M					mixture-(700C,1day)-(900C,3days) in CS2 atmosphere-cool(100/min)					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
106067	JSC1160392	S/C volum=38%, Rn(5K)=96 microOhm, cm	BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																		1	1995																															A	3.3258		25.208												K		2.88					2.88																																																																																											RH6067M					mixture-(600C,1day)-(700C,1day)-(900C,1day) in CS2 gas-(900C,3days in sillca)-cool to RT					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
106068	JSC0940294	not S/C (1.9K)	BaNb2O5	Ba1Nb2O5	Ba	1	Nb	2	O	5																		1	1991																															A	3.32		24.8												K					1.9																																																																								TP6068M																										mixture(BaCO3,Nb2O5)-CAL(800C,5H in H2S+Ar)-pellet-heat(800C in H2S+Ar)-SIN(800C, 60H in silica tube)					Physical Properties of a New Barium Niobium Sulfide, BaNb2S5			Superconductivity Research Laboratory, International Superconductivity Technology Center, 10-13 Shinonome 1-chome, Koto-ku, Tokyo 135, Japan	J.Solid State Chem.94(1991)294-297	H. YAMAUCHI,KIYOTAKA MATSUURA,SHOJI TANAKA,TAHASHI NAKAMIZO,TAKAHIRO WADA		
106069	PRL0814476			Be13U1	Be	13	U	1																				3	1998																																														K		0.9					0.9																				T		12.5												HC6069M																																																																			Revision of the Phase Diagram of Superconducting U1-xThxBe13			Max-Planck Institute for Chemical Physics of Solides, D-01187 Dresden, Germany	Phys.Lev.Lett.,81(1998)4476	A. Bach,C. Langhammer,F. Koromer,F. Steglich,G.R. Stewart,J.S. Kim,M. Lang,R. Helfrich,T. Michels		
106070	PR05600846	RRR=28	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			1997								13.8																				PrNi2Al3			A	5.386		4.188												K		1.89					1.89																																																								mj/mol.K2	148																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106071	PR05600846	RRR=18	UPd2(Al,Ga)3	U1Pd2Al2.97Ga0.03	U	1	Pd	2	Al	2.97	Ga	0.03																	1997																												PrNi2Al3			A	5.362		4.486												K		1.64					1.64																																																																																																arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106072	PR05600846	RRR=9.4	UPd2(Al,Ga)3	U1Pd2Al2.94Ga0.06	U	1	Pd	2	Al	2.94	Ga	0.06																	1997								13.9																				PrNi2Al3			A	5.362		4.184												K		1.51					1.51																																																																																																arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106073	PR05600846	RRR=7.0	UPd2(Al,Ga)3	U1Pd2Al2.85Ga0.15	U	1	Pd	2	Al	2.85	Ga	0.15																	1997								13.9																				PrNi2Al3			A	5.356		4.185												K		1.15					1.15																																																																																																arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106074	PR05600846	RRR=3.5	UPd2(Al,Ga)3	U1Pd2Al2.7Ga0.3	U	1	Pd	2	Al	2.7	Ga	0.3																	1997								13.7																				PrNi2Al3			A	5.353		4.188												K		0.52					0.52																																																								mj/mol.K2	149																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106075	PR05600846	RRR=4.0	UPd2(Al,Ga)3	U1Pd2Al2.55Ga0.45	U	1	Pd	2	Al	2.55	Ga	0.45																	1997								13.5																				PrNi2Al3			A	5.347		4.187												K		0.76					0.76																																																																																																arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106076	PR05600846	RRR=4.4	UPd2(Al,Ga)3	U1Pd2Al2.4Ga0.6	U	1	Pd	2	Al	2.4	Ga	0.6																	1997								13.6																				PrNi2Al3			A	5.344		4.187												K		0.33					0.33																																																								mj/mol.K2	144																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106077	PR05600846	RRR=2.9	UPd2(Al,Ga)3	U1Pd2Al2.01Ga0.99	U	1	Pd	2	Al	2.01	Ga	0.99																	1997								13.2																				PrNi2Al3			A	5.336		4.196												K					0.05																																																										mj/mol.K2	147																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106078	PR05600846	RRR=2.6	UPd2(Al,Ga)3	U1Pd2Al1.02Ga1.98	U	1	Pd	2	Al	1.02	Ga	1.98																	1997								11.5																				PrNi2Al3			A	5.322		4.212												K					0.05																																																										mj/mol.K2	184																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106079	PR05600846	RRR=1.8	UPd2(Al,Ga)3	U1Pd2Al0.6Ga2.4	U	1	Pd	2	Al	0.6	Ga	2.4																	1997								9.46																				PrNi2Al3			A	5.323		4.227												K					0.05																																																										mj/mol.K2	191																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106080	PR05600846	RRR=2.7	UPd2(Al,Ga)3	U1Pd2Al0.3Ga2.7	U	1	Pd	2	Al	0.3	Ga	2.7																	1997								12																				BaBa2Pt3			A	5.303		8.469												K					0.05																																																										mj/mol.K2	226																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106081	PR05600846	RRR=30	UPd2(Al,Ga)3	U1Pd2Ga3	U	1	Pd	2	Ga	3																			1997								12.2																				BaBa2Pt3			A	5.3015		8.5112												K					0.05																																																										mj/mol.K2	230																																							arc melting-ANN(900C,1week in ampoule)					Superconductivity and magnetism in heavy-fermion UPd2(Al,Ga)3	199707		Kamerlingh Onnes Laboratory, Leiden University, 2300 RA Leiden, The Netherlands	Phys.Rev,B56(1997)846	"A.A. Menovsky,B. Becker,B. Ludoph,G.J. Nieuwenhuys,J.A. Mydosh,S.Su""llow"		
106082	PR05600437	single crystal	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1997								10.5																				LuNi2B2C																		K		6					6																																																																																																Ni2B flux method.					Electrical resistivity and thermopower of single-crystal RNi2B2C (R=Dy,Ho,er,Tm) magnetic superconductors	199707		Physics Department , Taxas A&M University, College Station, Texas 77843-4242 and Physics Department, University of Hyderabad, Hyderabad 500046, India	Phys.Rev,B56(1997)437-445	A.K. Bhatnagar,D.G. Naugle,K.D.D. Rathnayaka,P.C. Canfield		
106083	PR05600437	single crystal	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																3	1997								5.2																				LuNi2B2C																		K		8.6					8.6																																																																																																Ni2B flux method.					Electrical resistivity and thermopower of single-crystal RNi2B2C (R=Dy,Ho,er,Tm) magnetic superconductors	199707		Physics Department , Taxas A&M University, College Station, Texas 77843-4242 and Physics Department, University of Hyderabad, Hyderabad 500046, India	Phys.Rev,B56(1997)437-445	A.K. Bhatnagar,D.G. Naugle,K.D.D. Rathnayaka,P.C. Canfield		
106084	PR05600437	single crystal	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		10.8					10.8																																																																																																Ni2B flux method.					Electrical resistivity and thermopower of single-crystal RNi2B2C (R=Dy,Ho,er,Tm) magnetic superconductors	199707		Physics Department , Taxas A&M University, College Station, Texas 77843-4242 and Physics Department, University of Hyderabad, Hyderabad 500046, India	Phys.Rev,B56(1997)437-445	A.K. Bhatnagar,D.G. Naugle,K.D.D. Rathnayaka,P.C. Canfield		
106086	PHC2500128	Fig shows Hc2(T): P=1 for H//a and P=2 for H//C. Rn=10 microOhm. Cm, single crystal		U1Ru2Si2	U	1	Ru	2	Si	2																		3	1995																																														K		1.53					1.53																				T		13												HC6086M																																																														arc-mrlting-ANN(1050C in UHV)					Anisotropy of the upper critical field in URu2Si2 and FFLO state in antiferromagnetic superconductors	199507		Centre de Recherches sur les Tres Basses Temperatures,Laboratoire associe al'Universite Joseph Fourier,CNRS,BP 166,38042 Grenoble Cedex 9,France	Physica C.,250(1995)128-138	A. Buzdin (b,c),A. Vernie're (a),A.Buzdin,A.Verniere,G.G. Lonzarich (d),G.G.Lonzarich,J. Flouquet (c),J.Flouquet,J.P. Brison (a),J.P.Brison,L. Schmidt (b),L.Schmidt,N. Keller (a),N.Keller,P. Lejay (a),P.Lejay,S.R. Julian (d),S.R.Julian		
106087	PR05506584	no magnetic order	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C																		K		15.5					15.5																																																																																																arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106088	PR05506584	not S/C. no magnetic order		Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C			A	3.637		10.227												K																																																																																																							arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106089	PR05506584			Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																1	1997								4																				LuNi2B2C			A	3.706		9.999												K																																																																																																							arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106090	PR05506584			Nd1Ni2B2C1	Nd	1	Ni	2	B	2	C	1																1	1997								4.78																				LuNi2B2C			A	3.678		10.081												K																																																																																																							arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106091	PR05506584			Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																1	1997								15																				LuNi2B2C			A	3.553		10.435												K																																																																																																							arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106092	PR05506584		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1997								10.6																				LuNi2B2C			A	3.534		10.487												K		6					6																																																																																																arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106093	PR05506584		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1997								5																				LuNi2B2C			A	3.517		10.527												K		8					8																																																																																																arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106094	PR05506584		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1997								6.8																				LuNi2B2C			A	3.501		10.558												K		11					11																																																																																																arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106095	PR05506584		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	1997								1.53																				LuNi2B2C			A	3.486		10.586												K		11					11																																																																																																arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106096	PR05506584	not S/C. no magnetic order. Heary fermion		Yb1Ni2B2C1	Yb	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C			A	3.478		10.607												K																																																																																																							arc melting.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106097	PHC2520138	d(x-ray)=11.4g/cm3, Tc(zero)=2K		Nd1.72Ta3.28S2	Nd	1.72	Ta	3.28	S	2																			1995																															A	3.3203		21.619												K		4.3					4.3																																																																																																					Superconductivitiy in the transition metal-rich layered compound NbxTa5-xS2(x=1.72)	199510		(a)Ames Laboratory and Department of Physics and Astronomy,Iowa State University, Ames, IA 50011, USA (b)Ames Laboratory and Department of Chemistry, Iowa State University, Ames, IA 50011, USA	Physica C,252(1995)138-140	David C. Johnston (a),Hugo F. Franzen (b),Xiaoqiang Yao (b),Zhaorong Wang (a)	Nb, Ta, S	
106098	PHC2520199		Y(Ni,Co)2B2C	Y1Ni1.8Co0.2B2C1	Y	1	Ni	1.8	Co	0.2	B	2	C	1															1995																												LuNi2B2C																		K		6.7					6.7																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106099	PHC2520199		Y(Ni,Co)2B2C	Y1Ni1.86Co0.14B2C1	Y	1	Ni	1.86	Co	0.14	B	2	C	1															1995																												LuNi2B2C																		K		8.5					8.5																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106100	PHC2520199		Y(Ni,Co)2B2C	Y1Ni1.9Co0.1B2C1	Y	1	Ni	1.9	Co	0.1	B	2	C	1															1995																												LuNi2B2C																		K		9.5					9.5																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106101	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.94Co0.06B2C1	Y	1	Ni	1.94	Co	0.06	B	2	C	1															1995																												LuNi2B2C																		K		12.1					12.1																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106102	PHC2520199		Y(Ni,Co)2B2C	Y1Ni1.985Cu0.015B2C1	Y	1	Ni	1.985	Cu	0.015	B	2	C	1															1995																												LuNi2B2C																		K		14.3					14.3																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106103	PHC2520199		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		15.3					15.3																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106104	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.95Cu0.05B2C1	Y	1	Ni	1.95	Cu	0.05	B	2	C	1															1995																												LuNi2B2C																		K		14.7					14.7																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106105	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.9Cu0.1B2C1	Y	1	Ni	1.9	Cu	0.1	B	2	C	1															1995																												LuNi2B2C																		K		13.7					13.7																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106106	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.85Cu0.15B2C1	Y	1	Ni	1.85	Cu	0.15	B	2	C	1															1995																												LuNi2B2C																		K		13					13																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106107	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.8Cu0.2B2C1	Y	1	Ni	1.8	Cu	0.2	B	2	C	1															1995																												LuNi2B2C																		K		11.5					11.5																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106108	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.7Cu0.3B2C1	Y	1	Ni	1.7	Cu	0.3	B	2	C	1															1995																												LuNi2B2C																		K		10.8					10.8																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106109	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.6Cu0.4B2C1	Y	1	Ni	1.6	Cu	0.4	B	2	C	1															1995																												LuNi2B2C																		K		10.6					10.6																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106110	PHC2520199		Y(Ni,Cu)2B2C	Y1Ni1.4Cu0.6B2C1	Y	1	Ni	1.4	Cu	0.6	B	2	C	1															1995																												LuNi2B2C																		K		10.5					10.5																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106111	PHC2520199		YCu2B2C	Y1Cu2B2C1	Y	1	Cu	2	B	2	C	1																	1995																												LuNi2B2C																		K		10					10																																																																																																arc-melting.					Effect of hydrostatic pressure on Tc in supercoducting YNi2-xMxB2C(M=Co,Cu)	199510		Department of Physics, Washington University,Campus Box 1105, One Brookings Dr.,St. Louis, Mo 63130-4899, USA	Physica C,252(1995)199-202	A-K. Klehe,A.K. Gangopadhyay,C. Looney,J.s. schilling	Y, Ni, Co, Cu, B, C	
106112	PHC3080243	RRR=9.5	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1998																												LuNi2B2C			A	3.5271		10.542												K		15.6					15.6																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106113	PHC3080243	RRR=7.0	(Y,Tb)Ni2B2C	Y0.9Tb0.1Ni2B2C1	Y	0.9	Tb	0.1	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5297		10.531												K		12.7					12.7																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106114	PHC3080243	RRR=8.0	(Y,Tb)Ni2B2C	Y0.8Tb0.2Ni2B2C1	Y	0.8	Tb	0.2	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5322		10.423												K		11					11																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106115	PHC3080243	RRR=4.8	(Y,Tb)Ni2B2C	Y0.7Tb0.3Ni2B2C1	Y	0.7	Tb	0.3	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5353		10.513												K		8.1					8.1																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106116	PHC3080243		(Y,Tb)Ni2B2C	Y0.65Tb0.35Ni2B2C1	Y	0.65	Tb	0.35	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5356		10.508												K		4.6					4.6																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106117	PHC3080243		(Y,Tb)Ni2B2C	Y0.6Tb0.4Ni2B2C1	Y	0.6	Tb	0.4	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5374		10.503												K		2					2																																																																																																arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106118	PHC3080243		(Y,Tb)Ni2B2C	Y0.55Tb0.45Ni2B2C1	Y	0.55	Tb	0.45	Ni	2	B	2	C	1															1998								6.1																				LuNi2B2C			A	3.539		10.498												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106119	PHC3080243		(Y,Tb)Ni2B2C	Y0.5Tb0.5Ni2B2C1	Y	0.5	Tb	0.5	Ni	2	B	2	C	1															1998								7.3																				LuNi2B2C			A	3.5401		10.494												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106120	PHC3080243	RRR=3.4	(Y,Tb)Ni2B2C	Y0.4Tb0.6Ni2B2C1	Y	0.4	Tb	0.6	Ni	2	B	2	C	1															1998								8.8																				LuNi2B2C			A	3.5429		10.478												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106121	PHC3080243		(Y,Tb)Ni2B2C	Y0.3Tb0.7Ni2B2C1	Y	0.3	Tb	0.7	Ni	2	B	2	C	1															1998								10.3																				LuNi2B2C			A	3.5457		10.467												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106122	PHC3080243	RRR=3.6	(Y,Tb)Ni2B2C	Y0.25Tb0.75Ni2B2C1	Y	0.25	Tb	0.75	Ni	2	B	2	C	1															1998								11.8																				LuNi2B2C																		K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106123	PHC3080243	RRR=4.4	(Y,Tb)Ni2B2C	Y0.2Tb0.8Ni2B2C1	Y	0.2	Tb	0.8	Ni	2	B	2	C	1															1998								12																				LuNi2B2C			A	3.5498		10.463												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106124	PHC3080243	RRR=1.9	(Y,Tb)Ni2B2C	Y0.1Tb0.9Ni2B2C1	Y	0.1	Tb	0.9	Ni	2	B	2	C	1															1998								13.5																				LuNi2B2C			A	3.551		10.439												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106125	PHC3080243	RRR=1.5	(Y,Tb)Ni2B2C	Y0.05Tb0.95Ni2B2C1	Y	0.05	Tb	0.95	Ni	2	B	2	C	1															1998								13.3																				LuNi2B2C			A	3.5509		10.447												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106126	PHC3080243	RRR=3.3	TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																	1998								15.4																				LuNi2B2C			A	3.5532		10.436												K																																																																																																							arc melting.					Magnetic ordering and superconductivity in TbxY1-xNi2B2C	199811		Institut fur Festkorper und Werkstofforschung Dresden, PF 27 00 16, D-01171 Dresden, Germany	Physica.C,308(1998)243-250	A. Belger,G. Behr,G. Fuchs,H. Bitterlich,K. Nenkov,L. Schultz,W. Loser		
106127	PRL0741427		(Na,Ba)xSi46	Na2.9Ba4.5Si46	Na	2.9	Ba	4.5	Si	46																			1995																												clathrate																		K		3.5					3.5																																																																																																siliside was heated(773K,8-10H in vac)					Superconductivity in the Silicon Clathrate Compound(Na,Ba)xSi46	199502		Department of Applied Chemistry,Faculty of Engineering,Hiroshima University,Higashi-Hiroshima 724,Japan	Phys.Rev.Lett.,74(1995)1427	Hiro-omi,Hiro-omi Horie,Hitoshi Kawaji,Mitsuo Ishikawa,Shoji Yamanaka,Syoji Yamanaka	Na,Ba,Si	
106128	JPS0670272	Figure shows Hc1(P=1) and Hc2(P=2). G-L parameter = 25.	CeRu2	Ce1Ru2	Ce	1	Ru	2																				3	1998																																													Laves	K		6.3					6.3											Oe		175							KOe		52.3														A		79.3			A		1980					1								mj/mol.K2	27		120																																					czochralski method					Superconducting Properties of CeRu2	199801		Gradvate School of Science, Osaka University, Toyonaka 560	J.Phys.Soc.Japan67(1998)272	Etsuji YAMAMOTO,Hdeyuki SATO,Msato HEDO,Saburo TAKAHASHI,Tatsuma D. MATSUDA,Yoshichika ONUKI,Yoshihiko INADA,Yoshinori HAGA,Yuji AOKI		
106130	JSC1360151		LaxMo6Se8	La0.84Mo6Se8	La	0.84	Mo	6	Se	8																		3	1998																												Chevrel			A	6.7551														K		9.4					9.4																																																																																																mixture((MoSe2,Mo,La2se3)-heart(1675C)-slow cooling					Single-Crystal Studies of the Chevrel-Phase Superconductor LaxMo6Se8			Chimie du Solide et Inorganique Moleculaire, UMR CNRS 6511, Universite de Rennes I, 35042 Rennes Cedex, France	J.Solid State Chem.136(1998)151-159	A. Wojakowski,C. Perrin,F. Le Berre,M. Sergent,O. Pena,R. Horyn'		
106131	JSC1360151		LaxMo6Se8	La0.88Mo6Se8	La	0.88	Mo	6	Se	8																		3	1998																												Chevrel			A	6.7577														K		10.25					10.25																																																																																																mixture((MoSe2,Mo,La2se3)-heart(1675C)-slow cooling					Single-Crystal Studies of the Chevrel-Phase Superconductor LaxMo6Se8			Chimie du Solide et Inorganique Moleculaire, UMR CNRS 6511, Universite de Rennes I, 35042 Rennes Cedex, France	J.Solid State Chem.136(1998)151-159	A. Wojakowski,C. Perrin,F. Le Berre,M. Sergent,O. Pena,R. Horyn'		
106132	JSC1360151		LaxMo6Se8	La0.94Mo6Se8	La	0.94	Mo	6	Se	8																		3	1998																												Chevrel			A	6.7618														K		11					11																																																																																																mixture((MoSe2,Mo,La2se3)-heart(1675C)-slow cooling					Single-Crystal Studies of the Chevrel-Phase Superconductor LaxMo6Se8			Chimie du Solide et Inorganique Moleculaire, UMR CNRS 6511, Universite de Rennes I, 35042 Rennes Cedex, France	J.Solid State Chem.136(1998)151-159	A. Wojakowski,C. Perrin,F. Le Berre,M. Sergent,O. Pena,R. Horyn'		
106133	JSC1360160	Figre shows Hc2(T)defined as Tc(onset)Jc(1.7K,H=0)=4.0E+A/cm2		La0.94Mo6Se8	La	0.94	Mo	6	Se	8																		3	1998																												Chevrel																		K		11					11																				T		55																																																																															Single-Crystal Studies of the Chevrel-Phase Superconductor LaxMo6Se8			Chimie du Solide et Inorganique Moleculare, UMR CNRS 6511, Universite de Rennes I, 35042 Rennes Cedex, France	J.Solid State Chem.136(1998)160-166	A. Wojakowski,F. Le Berre,J. Padiou,O. Pena,R. Horyn',T. Marchand		
106134	JSC1360160	Figre shows Hc2(T)defined as Tc(onset)Jc(1.7K,H=0)=2.8E+4 A/cm2		Mo3Se4	Mo	3	Se	4																				3	1998																												Chevrel																		K		6.6					6.6																																																																																																					Single-Crystal Studies of the Chevrel-Phase Superconductor LaxMo6Se8			Chimie du Solide et Inorganique Moleculare, UMR CNRS 6511, Universite de Rennes I, 35042 Rennes Cedex, France	J.Solid State Chem.136(1998)160-166	A. Wojakowski,F. Le Berre,J. Padiou,O. Pena,R. Horyn',T. Marchand		
106136	JPC0097419	quenched sample	Pr3Ni	Ni1Pr3	Ni	1	Pr	3																				1	1997																															A	7.182	9.786	6.479											orthorhombic	K					2																																																																																																		arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
106137	JPC0097419	quenched sample	Gd3Ni	Gd3Ni1	Gd	3	Ni	1																				1	1997								100																							A	6.952	9.688	6.367											orthorhombic	K					2																																																																																																		arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
106138	JPC0097419	quenched sample	Tb3Ni	Ni1Tb3	Ni	1	Tb	3																				1	1997								62																							A	6.921	9.605	6.31											orthorhombic	K					2																																																																																																		arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
106139	JPC0097419	quenched sample	Ho3Ni	Ho3Ni1	Ho	3	Ni	1																				1	1997								18																							A	6.852	9.549	6.288											orthorhombic	K					2																																																																																																		arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
106140	JPC0097419	quenched sample	Er3Ni	Er3Ni1	Er	3	Ni	1																				1	1997								9																							A	6.804	9.432	6.245											orthorhombic	K					2																																																																																																		arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
106141	LTP0690203		Sn Mo6S8	Sn0.875Mo6S8	Sn	0.875	Mo	6	S	8																		1	1987																												Chevrel			A	9.137		11.371												K		14.048					14.048																																																																																																mixing of metal-powders					The Effects of Tungsten Doping on the Tin Chevrel-Phase Compound SnMo6S8			Department of Physics and Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois	J.Low Temp.Phys.69(1987)203	D.M. Ginsberg,W.H. Wright		
106142	LTP0690203		(W,Sn)Mo6S8	W0.25Sn0.875Mo6S8	W	0.25	Sn	0.875	Mo	6	S	8																1	1987																												Chevrel			A	9.144		11.371												K		13.635					13.635																																																																																																mixing of metal-powders					The Effects of Tungsten Doping on the Tin Chevrel-Phase Compound SnMo6S8			Department of Physics and Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois	J.Low Temp.Phys.69(1987)203	D.M. Ginsberg,W.H. Wright		
106143	PR0363941	Laser power density=2.53 E+12 W/cm2, peak pressure=1200kbar.		Cu2Mo6S8	Cu	2	Mo	6	S	8																		1	1987																												Chevrel																		K		10.43					10.43																																																																																																sintering.sample was disordered by shock pressure					Superconductivity in shocked Cu2Mo6S8	9		Nuclear Ohysics Division, Bhabha Atomic Research Centre, Trombay 400085, India	Phys.Rev.B36(1987)3941	B.K. Godwal,I.K. Gopalakrishnan,J.V. Yakhmi,P. Chaddah		
106144	JSC1350325	metallic	sulturiqation method using CS2	Sr1Nb2S5	Sr	1	Nb	2	S	5																			1998																															A	3.361		24.06											hexagonal	K					1.45																																																																																																							BRIEF COMMUNICATION Evidence for Siperconductivity in SrTa2S5 and Matallic Characteristics of SrNb2S5			Department of Materials Science and Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050, Japan	J.Solid State Chem135(1998)325	Masatomo Takahashi,Nobuhiro Matsumoto,Norihito Kijima,Shoichi Nagata		
106145	JSC1350325		sulturiqation method using CS2	Sr1Ta2S5	Sr	1	Ta	2	S	5																			1998																															A	3.306		24.26											hexagonal	K		2.75					2.75																																																																																																					BRIEF COMMUNICATION Evidence for Siperconductivity in SrTa2S5 and Matallic Characteristics of SrNb2S5			Department of Materials Science and Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050, Japan	J.Solid State Chem135(1998)325	Masatomo Takahashi,Nobuhiro Matsumoto,Norihito Kijima,Shoichi Nagata		
106146	PHC2550019	96H annealed		La1Pt1.5Au0.6B2.4C1.2	La	1	Pt	1.5	Au	0.6	B	2.4	C	1.2															1995																															A	3.8657		10.729												K		11					11																																																																																																arc-melting					Synthesis and phase characterization of the intermetallic conpounds Ln(Pt,Au)2+zB2C, where Ln=La,Pr,Nd,Dy and Y	199512		"(a)Institut Fu""r Festko""rper-und Werkstofforschung Dresden e.V.,Postfach 270016,d-01171 Dresden,Germany (b)Institute of Physics,Polish Academy Sciences, 02-668 Warsaw,Poland"	Physica.C,255(1995)19-29	G. Fuchs,J. Klosowski,J. Zawadzki,M. Buchgeister,U. Wiesner	La, Pr, Nd, Dy, Y, Pt, Au, B, C	
106147	PHC2550019			Pr1Pt1.5Au0.6B2.4C1.2	Pr	1	Pt	1.5	Au	0.6	B	2.4	C	1.2															1995																															A	3.8307		10.7448												K		6.2					6.2																																																																																																arc-melting					Synthesis and phase characterization of the intermetallic conpounds Ln(Pt,Au)2+zB2C, where Ln=La,Pr,Nd,Dy and Y	199512		"(a)Institut Fu""r Festko""rper-und Werkstofforschung Dresden e.V.,Postfach 270016,d-01171 Dresden,Germany (b)Institute of Physics,Polish Academy Sciences, 02-668 Warsaw,Poland"	Physica.C,255(1995)19-29	G. Fuchs,J. Klosowski,J. Zawadzki,M. Buchgeister,U. Wiesner	La, Pr, Nd, Dy, Y, Pt, Au, B, C	
106148	PHC2550019	broad transition		Y1Pt1.5Au0.6B2.4C1.2	Y	1	Pt	1.5	Au	0.6	B	2.4	C	1.2															1995																																														K		5.8					5.8																																																																																																arc-melting					Synthesis and phase characterization of the intermetallic conpounds Ln(Pt,Au)2+zB2C, where Ln=La,Pr,Nd,Dy and Y	199512		"(a)Institut Fu""r Festko""rper-und Werkstofforschung Dresden e.V.,Postfach 270016,d-01171 Dresden,Germany (b)Institute of Physics,Polish Academy Sciences, 02-668 Warsaw,Poland"	Physica.C,255(1995)19-29	G. Fuchs,J. Klosowski,J. Zawadzki,M. Buchgeister,U. Wiesner	La, Pr, Nd, Dy, Y, Pt, Au, B, C	
106149	PHC2550019			Dy1Pt1.5Au0.6B2.4C1.2	Dy	1	Pt	1.5	Au	0.6	B	2.4	C	1.2															1995								5.9																																						K					4.5																																																																																																		arc-melting					Synthesis and phase characterization of the intermetallic conpounds Ln(Pt,Au)2+zB2C, where Ln=La,Pr,Nd,Dy and Y	199512		"(a)Institut Fu""r Festko""rper-und Werkstofforschung Dresden e.V.,Postfach 270016,d-01171 Dresden,Germany (b)Institute of Physics,Polish Academy Sciences, 02-668 Warsaw,Poland"	Physica.C,255(1995)19-29	G. Fuchs,J. Klosowski,J. Zawadzki,M. Buchgeister,U. Wiesner	La, Pr, Nd, Dy, Y, Pt, Au, B, C	
106150	PHC2550019			Nd1Pt1.5Au0.6B2.4C1.2	Nd	1	Pt	1.5	Au	0.6	B	2.4	C	1.2															1995								9.6																							A	3.8229	10.7358													K					4.5																																																																																																		arc-melting					Synthesis and phase characterization of the intermetallic conpounds Ln(Pt,Au)2+zB2C, where Ln=La,Pr,Nd,Dy and Y	199512		"(a)Institut Fu""r Festko""rper-und Werkstofforschung Dresden e.V.,Postfach 270016,d-01171 Dresden,Germany (b)Institute of Physics,Polish Academy Sciences, 02-668 Warsaw,Poland"	Physica.C,255(1995)19-29	G. Fuchs,J. Klosowski,J. Zawadzki,M. Buchgeister,U. Wiesner	La, Pr, Nd, Dy, Y, Pt, Au, B, C	
106151	PHC2530048	2 gap/RTc=4.9(upper limit)	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		15.4					15.4																																																3.2	1																																															grown from Ni2B flux					Energy gap of quatemary compound superconductor YNi2B2C and LuNi2B2C by point-cotact spectroscopy	199510		Department of Physics,Seoul National University, Seoul 151-742, South Korea	Physica C,253(1995)48-52	B.K. Cho,D.C. Johnston,G.T. Geong,G.T. Jeong,J.I. Kye,P.C. Canfield,S.H. Chun,W.C. Lee,Z.G. Khim	Y< Ni, B, C, Lu	
106152	PHC2530048	2 gap/RTc=4.9(upper limit), temp.dep. Good agreement with BCS.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		15.7					15.7																																																3.3	1																																															grown from Ni2B flux					Energy gap of quatemary compound superconductor YNi2B2C and LuNi2B2C by point-cotact spectroscopy	199510		Department of Physics,Seoul National University, Seoul 151-742, South Korea	Physica C,253(1995)48-52	B.K. Cho,D.C. Johnston,G.T. Geong,G.T. Jeong,J.I. Kye,P.C. Canfield,S.H. Chun,W.C. Lee,Z.G. Khim	Y< Ni, B, C, Lu	
106153	PHC2450159	Tc vaue fol Boyon mass=10,Carbon mas=12.011	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		15.48					15.48						0.25	B																																																																																									arc-melting					Boron isotope effect in Ni and Pd based borocarbide superconductors	199504		Department of Physics,University of Alberta,Edmonton,AB,T6G 2Ji,Canada	Physica C.,245(1995)159-163	D.D. Kawrie,D.D.Lawrie,J.P. Franck,J.P.Franck		
106154	PHC2450159	Tc vaue fol Boyon mass=10,Carbon mas=12.011	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		15.48					15.48						0.08	C																																																																																									arc-melting					Boron isotope effect in Ni and Pd based borocarbide superconductors	199504		Department of Physics,University of Alberta,Edmonton,AB,T6G 2Ji,Canada	Physica C.,245(1995)159-163	D.D. Kawrie,D.D.Lawrie,J.P. Franck,J.P.Franck		
106155	PHC2450159	Tc is for B-mass=10		Y1Pd5B3C0.3	Y	1	Pd	5	B	3	C	0.3																	1995																																														K		23.32					23.32						0.32	B																																																																																									arc-melting					Boron isotope effect in Ni and Pd based borocarbide superconductors	199504		Department of Physics,University of Alberta,Edmonton,AB,T6G 2Ji,Canada	Physica C.,245(1995)159-163	D.D. Kawrie,D.D.Lawrie,J.P. Franck,J.P.Franck		
106156	PHC2490403	no reentrant behavior . G-L parameter = 3.7	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1995								10.1																				LuNi2B2C			A	3.532		10.483												K		3.8					3.8											G									KG		3																																																																										arc-melting and annealing					Coexistence of antiferromagnetic order and superconductivity with TN higher than Tc in DyNi2B2C	199507		Department of Physics,National Tsing Hua University,Hsinchu,300 Taiwan	Physica C.,249(1995)403-408	H.C. Ku,H.C. Ku a,H.C.Ku,J.C. Ho,J.C. Ho d,J.C.Ho,J.H. Shieh,J.H. Shieh a,J.H.Shieh,J.W. Chen,J.W. Chen b,J.W.Chen,M. S. Lin a,M.S. Lin,M.S.Lin,S.H. Lin,S.H. Lin c,S.H.Lin,Y.B. You,Y.B. You a,Y.B.You,Y.D. Yao,Y.D. Yao c,Y.D.Yao,Y.Y. Chen,Y.Y. Chen c,Y.Y. Hsu,Y.Y. Hsu a,Y.Y.Chen,Y.Y.Hsu		
106157	PHC2460317		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1995																												LuNi2B2C			A	3.526		10.538												K		15.5					15.5																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106158	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1.9Cu0.1B2C1	Y	1	Ni	1.9	Cu	0.1	B	2	C	1														1	1995																												LuNi2B2C			A	3.526		10.545												K		13.8					13.8																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106159	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1.8Cu0.2B2C1	Y	1	Ni	1.8	Cu	0.2	B	2	C	1														1	1995																												LuNi2B2C			A	3.527		10.562												K		11.6					11.6																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106160	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1.7Cu0.3B2C1	Y	1	Ni	1.7	Cu	0.3	B	2	C	1														1	1995																												LuNi2B2C			A	3.5275		10.575												K		10.9					10.9																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106161	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1.6Cu0.4B2C1	Y	1	Ni	1.6	Cu	0.4	B	2	C	1														1	1995																												LuNi2B2C			A	3.529		10.598												K		10.6					10.6																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106162	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1.4Cu0.6B2C1	Y	1	Ni	1.4	Cu	0.6	B	2	C	1														1	1995																												LuNi2B2C			A	3.5295		10.601												K		10.4					10.4																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106163	PHC2460317		Y(Ni,Cu)2B2C	Y1Ni1Cu1B2C1	Y	1	Ni	1	Cu	1	B	2	C	1														1	1995																												LuNi2B2C			A	3.531		10.62												K		10.1					10.1																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106164	PHC2460317		Y(Ni,Co)2B2C	Y1Ni1.98Co0.02B2C1	Y	1	Ni	1.98	Co	0.02	B	2	C	1														1	1995																												LuNi2B2C			A	3.526		10.537												K		14.3					14.3																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106165	PHC2460317		Y(Ni,Co)2B2C	Y1Ni1.9Co0.1B2C1	Y	1	Ni	1.9	Co	0.1	B	2	C	1														1	1995																												LuNi2B2C			A	3.5255		10.534												K		9.5					9.5																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106166	PHC2460317		Y(Ni,Co)2B2C	Y1Ni1.8Co0.2B2C1	Y	1	Ni	1.8	Co	0.2	B	2	C	1														1	1995																												LuNi2B2C			A	3.525		10.532												K		6.8					6.8																																																																																																arc-melting					The effect of alloying on Tc in superconducting YNi2-xMxB2C(M=Co,Cu)	199505		Department of Physics,Campus Box 1105,Washington University,One Brookings Drive,St.Louis,MO 63130-4899,USA	Physica C.,246(1995)317-322	Aaron J. Schuetz,Aaron J.Schuetz,Anup K. Gangopadhyay,Anup K.Gangopadhyay,James S. Schilling,James S.Schilling		
106167	JPS0632853		UNi2B2C	U1Ni2B2C1	U	1	Ni	2	B	2	C	1																1	1994							280	218																				LuNi2B2C			A	3.513		10.54												K					4.2																																																																																																							Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
106168	JPS0632853	ferromagnetic temp=185K		U1Rh2B2C1	U	1	Rh	2	B	2	C	1																1	1994							153																					LuNi2B2C			A	3.782		10.214												K					4.2																																																																																																		arc-melting-ANN(1100C, 4days in Ar)					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
106169	JPS0632853		ThNi2B2C	Th1Ni2B2C1	Th	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.695		10.197												K		6.5					6.5																																																																																																					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
106170	JPS0632853		ThRh2B2C	Th1Rh2B2C1	Th	1	Rh	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.863		10.177												K					4.2																																																																																																							Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
106171	JPS0632853			Th1Pt2B2C1	Th	1	Pt	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.828		10.853												K		6.7					6.7																																																																																																					Superconductivity in ThT2B2C and Strong Magnetism in UT2B2C(T=Ni,Rh and Pt)	199408		Faculty of Integrated Arts and Sciences,Hiroshima University,Kagamiyama 1-7-1,Higashi-Hiroshiima 724	J. Phys. Soc.Japan.,632(1994)2853	Hironobu FUJII,Taku KONISHI,Toshiro TAKABATAKE,Toshiro TAKANABATAKE,Yasuomi MAEDA	Th,B,C,V,Ni,Rh,Pt	
106172	NAT3720245	zero-resistivity at 11.4K.		La3Ni2B2N3	La	3	Ni	2	B	2	N	3																1	1994																															A	3.721		20.516												K		12.3					12.3																																																																																																arc-melting in N2, 1050C annealing					Superconductivity in lanthanum nickel boro-nitride	11		AT&T Bell Laboratories,Murray Hill,New Jersey 07974,USA	NATURE.,372(1994)245	B.Batlogg,E.M.Gyorgy,H.Eisali,H.Takagi,H.W.Zandbergen,J.J.Krajewski,R.J.CaVa,S.Uchida,W.F.Peck Jr	La,Ni,B,N	
106173	NAT3720245	resistance decreases bellow 10K, maybe due to La3Ni2B2N3		La1Ni1B1N1	La	1	Ni	1	B	1	N	1																	1994																															A	3.725		7.59												K																																																																																																												Superconductivity in lanthanum nickel boro-nitride	11		AT&T Bell Laboratories,Murray Hill,New Jersey 07974,USA	NATURE.,372(1994)245	B.Batlogg,E.M.Gyorgy,H.Eisali,H.Takagi,H.W.Zandbergen,J.J.Krajewski,R.J.CaVa,S.Uchida,W.F.Peck Jr	La,Ni,B,N	
106174	PR05800603	annealed (800C)Sample, Transition width=1.3mK, sinezle crystal	Upt3	Pt3U1	Pt	3	U	1																				3	1998																																														K		0.553					0.553																																																																																																vertical floating-zone					Suppression of superconductivity in UPt3 single crystals	7		Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208	Phys.Rev.B,58(1998)R603	D.N. Seidman,J.A. Sauls,J.B. Kycia,J.I. Hong,M.J. Graf,W.P. Halperin		
106175	PHC2490271	Figure shows Hc1(P=1), Hc2(P=2), Hirr(P=3). G-L parameter = 20.4	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1995																												LuNi2B2C			A	3.5403		10.4998												K		15.45					15.45											Oe		220							KOe		52												HC6175M		A		80			A		1630																																																					arc-melting-ANN(900C, 1 week)					Magnetic phase diagram of YNi2B2C	199507		Solid State Physics  Division,Bhabha Atomic Research Centre,Bombay-400085,India	Physica C.,249(1995)271-288	A. K. Grover,A.K.Grover,G. Ravikumar,G.Ravikumar,Girish Chandora,Girish Chandra,K. Ghosh,K.Ghosh,P. K. Mishra,P.K.Mishra,S. Ramakrishnan,S.Ramakrishnan,T. V. Chandrasekuhae Rao,T.V.Chandrasekhar Rao,V. C. Sahni,V.C.Sahni		
106176	PHC2540124	Curie T=-31.5K, 5.5K for H//C and H//ab, respectively, Figure shows Hirr(t) for H//C.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1995							-31.5	6.5																				LuNi2B2C																		K		10.5					10.5																																		HC6176M																																																																			Magnetization studies on ErNi2B2C single crystals	199511		Institute of Physics Polish Academy of Sciences,al. Lotnko'w 32/46,02-668 Warsaw, Poland	Physica C,254(1995)124-130	A. Winiarska,H. Szymczak,L. Gladczuk,M. Baran,R. Szymczak,Z. Drzazga	Er, Ni, B, C	
106177	PR05403772	Curie temp=-191K(H//ab), -63.6K(H//C)	YbNi2B2C	Yb1Ni2B2C1	Yb	1	Ni	2	B	2	C	1																3	1996							-63.6																					LuNi2B2C			A	3.575		10.606												K					1.8																																																										mj/mol.K2	530																																							flux method					Heavy-electron behavior in single-crystal YbNi2B2C	199608		University of California, Riverside, California 92521	Phys.Rev.B,54(1996)R3772	A. Yatskar,N.K. Budraa,P.C. Canfield,S.L.Bud'ko,W.P. Beyermann		
106178	PR05403772	Beta=0.35mj/mole,K4, deltaC/gamma.Tc=3.4	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																1	1996																												LuNi2B2C																		K		16					16																																																								mj/mol.K2	11																																							arc-melting					Heavy-electron behavior in single-crystal YbNi2B2C	199608		University of California, Riverside, California 92521	Phys.Rev.B,54(1996)R3772	A. Yatskar,N.K. Budraa,P.C. Canfield,S.L.Bud'ko,W.P. Beyermann		
106179	PHC2660027		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1996																												LuNi2B2C																		K		15.4					15.4																																		HC6179M																																																														arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106180	PHC2660027		(Ho,Y)Ni2B2C	Ho0.25Y0.75Ni2B2C1	Ho	0.25	Y	0.75	Ni	2	B	2	C	1														1	1996																												LuNi2B2C																		K		13.8					13.8																																																																																																arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106181	PHC2660027		(Ho,Y)Ni2B2C	Ho0.5Y0.5Ni2B2C1	Ho	0.5	Y	0.5	Ni	2	B	2	C	1														1	1996								1.53																				LuNi2B2C																		K		11.6					11.6																																																																																																arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106182	PHC2660027		(Ho,Y)Ni2B2C	Ho0.75Y0.25Ni2B2C1	Ho	0.75	Y	0.25	Ni	2	B	2	C	1														1	1996								3.65																				LuNi2B2C																		K		10.2					10.2																																																																																																arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106183	PHC2660027		(Ho,Y)Ni2B2C	Ho0.85Y0.15Ni2B2C1	Ho	0.85	Y	0.15	Ni	2	B	2	C	1														1	1996								4.3																				LuNi2B2C																		K		9.3					9.3																																																																																																arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106184	PHC2660027		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1996								5.2																				LuNi2B2C																		K		7.6					7.6																																																																																																arc-melting					Superconductivity and magnetism in (HoxY1-x)Ni2B2C	07		"Institut Fu""r Festko""rper-und Werkstofforschung Dresden, Germany"	Physica.C,266(1996)27-32	"A. Handstein,G. Fuchs,K. Eversmann,K.-H. Mu""ller,L. Cao"	Ho, Y, Ni, B, C	
106185	PR05000647	reentrant superconductivity, Tc2=5.0K	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1994							-1.5																					LuNi2B2C																		K		7.5					7.5																																		HC6185M																																																														arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106186	PR05000647	reentrant behavior at T=5.5K	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1994							-2.2																					LuNi2B2C																		K		10.4					10.4																																		HC6185M																																																														arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106187	PR05000647		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	1994							10.8																					LuNi2B2C																		K		10.9					10.9																																		HC6185M																																																														arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106188	PR05000647	resistivity drop at 2K(maybe, due to S/C	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1994							-9.8																					LuNi2B2C																		K		0.75					0.75																																																																																																arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106189	PR05000647	not S/C	TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																1	1994							-10.2																					LuNi2B2C																		K					2																																																																																																		arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106190	PR05000647		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C																		K		16.6					16.6																																		HC6185M																																																														arc-melting, ANN					Competition between magnetism and superconductivity in rare-earth nickel boride carbides	199407		Department of Applied Physics, University of Tokyo, Tokyo 113, Japan	Phys.Rev.B,50(1994)647	B. Batlogg,H. Eisaki,H. Takagi,J.J. Krajewski,J.O. Lee,K. Mizuhashi,R.J. Cava,S. Uchida,W.F. Peck, Jr.		
106191	PHC2420169	dTc/dP in K/GPa.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	1995																												LuNi2B2C																		K		15.76					15.76			K/GPa	0.032																																																																																												crystal grown by M. Xu etal					Infnluence of pressure on the superconducting state of RNi2B2C(R=Y,Ho,Er,and Tm)componds	199502		Condensed Matter and Thermal Physics Group MST-10,Los Alamos National Laboratory	Physica C.,242(1995)169-173	B.K.Cho,E.Alleno,J.D.Thompson,J.J.Neumeier,P.C.Canfield		
106192	PHC2420169	dTc/dp=-0.255 K/Gpa for liniar fitting	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																3	1995																												LuNi2B2C																		K		8.67					8.67			K/GPa	-0.187																																																																																												crystal grown by M. Xu etal					Infnluence of pressure on the superconducting state of RNi2B2C(R=Y,Ho,Er,and Tm)componds	199502		Condensed Matter and Thermal Physics Group MST-10,Los Alamos National Laboratory	Physica C.,242(1995)169-173	B.K.Cho,E.Alleno,J.D.Thompson,J.J.Neumeier,P.C.Canfield		
106193	PHC2420169	dTc/dP in K/GPa.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1995																												LuNi2B2C																		K		10.96					10.96			K/GPa	0.168																																																																																												crystal grown by M. Xu etal					Infnluence of pressure on the superconducting state of RNi2B2C(R=Y,Ho,Er,and Tm)componds	199502		Condensed Matter and Thermal Physics Group MST-10,Los Alamos National Laboratory	Physica C.,242(1995)169-173	B.K.Cho,E.Alleno,J.D.Thompson,J.J.Neumeier,P.C.Canfield		
106194	PHC2420169	dTc/dp=-0.453 K/Gpa for liniar fitting	TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																3	1995																												LuNi2B2C																		K		10.88					10.88			K/GPa	-0.41																																																																																												crystal grown by M. Xu etal					Infnluence of pressure on the superconducting state of RNi2B2C(R=Y,Ho,Er,and Tm)componds	199502		Condensed Matter and Thermal Physics Group MST-10,Los Alamos National Laboratory	Physica C.,242(1995)169-173	B.K.Cho,E.Alleno,J.D.Thompson,J.J.Neumeier,P.C.Canfield		
106195	PR05406865	gamma derived from thermal expansion throughEhrenfest relation. Thermal expansion coeff. alpha=28E-6  l/K. gamma= in mj/mol.K2		C60K3	C	60	K	3																					1996																												fullerene																		K		20					20																																																								mj/mol.K2	64																																												High-resolution thermal expansion of superconducting fillerides A3C60(A=K,Rb)	199609		"Forschungszentrum Karlsruhe Technik und Umwelt,Institut fu""r Nukleare Festko""rperphysik, Postfach 3640,76021 Karlsruhe, Germany"	Phys.Rev.B,54(1996)R6865	C. Meingast,G.J. Burkhart		
106196	PR05406865	gamma derived from thermal expansion throughEhrenfest relation. Thermal expansion coeff. alpha=29E-6  l/K. gamm= in mj/mol.K2		C60Rb3	C	60	Rb	3																					1996																												fullerene																		K		30.5					30.5																																																								mj/mol.K2	75																																												High-resolution thermal expansion of superconducting fillerides A3C60(A=K,Rb)	199609		"Forschungszentrum Karlsruhe Technik und Umwelt,Institut fu""r Nukleare Festko""rperphysik, Postfach 3640,76021 Karlsruhe, Germany"	Phys.Rev.B,54(1996)R6865	C. Meingast,G.J. Burkhart		
106197	PHC2660138	RRR=21, R(4.0K)=9.0 micro Ohm.cm		La1Ni1C2	La	1	Ni	1	C	2																		1	1996																												CeNiC2			A	3.975	4.558	6.119												K		3					3																																																								mj/mol.K2	7.83		496																																					arc-melting					Superconductivity in the Ni based ternary carbide LaNiC2	07		Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan	Physica.C,266(1996)138-142	H.K. Zeng,W.H. Lee,Y.D. Yao,Y.Y. Chen	La, Ni, C	
106198	PHC2590265	N-content is unkown, Figure shows P=1for Hc1(Oe), P=2 for Hc2	A3C60	Li2Na1N1C60	Li	2	Na	1	N	1	C	60																	1996																												fullerene																		K		12					12											Oe		14							kOe		38							kOe/K		-4.61					A		93			A		7200																																																					meta-stable					A new metastable superconductor Li2Na1NyC60 prepared from azides			Department of Electoronic Engineering, Faculty of Engineering, Osaka University, 2-1Yamada-Oka, Suita, Osaka 565, Japan	Physica.C,259(1996)265-270	A.A. Zakhidov,H. Araki,H. Mizobuchi,K. Yakushi,K. Yoshino,N. Yamasaki		
106199	SSC0990479	FCC single phase, compositions is nominal nalues. SC volume=65%	(NaH)4C60	Na4H4C60	Na	4	H	4	C	60																		1	1996																												fullerene			A	14.356														K		15					15																																																																																																					SUPERCONDUCTIVITY IN NaH INTERCALATED C60			Institute for Molecular Science,Myodaiji, Osaka444, Japan	Solid State Commun.99(1996)479-489	"H. Inokuchi,J. Kro""ber,J. Krober,K. Ichimura,K. Imaeda,Y. Yonehara"	Na, H, C	
106200	JPS0651924	pressure-induced s/c. Resistivity did not reach to zero ever under 100GPa Tc(max)=15K at P=150 GPa. dTc/dP = 0.14 K/GPa at Pc(=50 GPa).		Ca1	Ca	1																							1996																																														K		15			0		15	TC6200M																																																																																																				Superconductivity of Calcium under High Pressures	199607		Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Phys.Soc.Japan 65(1996)1924	Katsuya SHIMIZU,Kiichi AMAYA,Shingo OKADA,Shoichi ENDO,Tatsuo C. KOBAYASHI		
106201	PR05312318	dTc/dP in K/GPa.	LuNiBC	Lu1Ni1B1C1	Lu	1	Ni	1	B	1	C	1																	1996																												LuNiBC																		K		2.96					2.96		1	K/GPa	-0.17																																																																																												arc-melting					Doping and high-pressure study on Lu(Ni1-xAx)BC with A=Cu and V	05		Department of Physics and Texas Center for Superconductivity, University of Houston,Texas 77204-5932	Phys.Rev.B,53(1996)12318	C.W. Chu,L. Gao,R.L. Meng,X.D. Qui,Y.Y. Sun,Y.Y. Xue	Lu, Ni, Cu, V, B, C	
106202	PR05312318	dTc/dP in K/GPa.	Lu(Ni,V)BC	Lu1Ni0.9V0.1B1C1	Lu	1	Ni	0.9	V	0.1	B	1	C	1															1996																												LuNiBC																		K		2.94					2.94		1	K/GPa	-0.17																																																																																												arc-melting					Doping and high-pressure study on Lu(Ni1-xAx)BC with A=Cu and V	05		Department of Physics and Texas Center for Superconductivity, University of Houston,Texas 77204-5932	Phys.Rev.B,53(1996)12318	C.W. Chu,L. Gao,R.L. Meng,X.D. Qui,Y.Y. Sun,Y.Y. Xue	Lu, Ni, Cu, V, B, C	
106203	PR05312318	dTc/dP in K/GPa.	Lu(Ni,V)BC	Lu1Ni0.8V0.2B1C1	Lu	1	Ni	0.8	V	0.2	B	1	C	1															1996																												LuNiBC																		K		2.6					2.6		1	K/GPa	-0.17																																																																																												arc-melting					Doping and high-pressure study on Lu(Ni1-xAx)BC with A=Cu and V	05		Department of Physics and Texas Center for Superconductivity, University of Houston,Texas 77204-5932	Phys.Rev.B,53(1996)12318	C.W. Chu,L. Gao,R.L. Meng,X.D. Qui,Y.Y. Sun,Y.Y. Xue	Lu, Ni, Cu, V, B, C	
106204	PR05312318	dTc/dP in K/GPa.	Lu(Ni,Cu)BC	Lu1Ni0.9Cu0.1B1C1	Lu	1	Ni	0.9	Cu	0.1	B	1	C	1															1996																												LuNiBC																		K		3.3					3.3		1	K/GPa	-0.17																																																																																												arc-melting					Doping and high-pressure study on Lu(Ni1-xAx)BC with A=Cu and V	05		Department of Physics and Texas Center for Superconductivity, University of Houston,Texas 77204-5932	Phys.Rev.B,53(1996)12318	C.W. Chu,L. Gao,R.L. Meng,X.D. Qui,Y.Y. Sun,Y.Y. Xue	Lu, Ni, Cu, V, B, C	
106205	PR05312318	dTc/dP in K/GPa.	Lu(Ni,Cu)BC	Lu1Ni0.8Cu0.2B1C1	Lu	1	Ni	0.8	Cu	0.2	B	1	C	1															1996																												LuNiBC																		K		3.38					3.38		1	K/GPa	-0.17																																																																																												arc-melting					Doping and high-pressure study on Lu(Ni1-xAx)BC with A=Cu and V	05		Department of Physics and Texas Center for Superconductivity, University of Houston,Texas 77204-5932	Phys.Rev.B,53(1996)12318	C.W. Chu,L. Gao,R.L. Meng,X.D. Qui,Y.Y. Sun,Y.Y. Xue	Lu, Ni, Cu, V, B, C	
106206	SUP0070921	morecular crystal. s/c under 22 GPa.		I2	I	2																							1994																																														K		1.2					1.2		1																																																																																																			The Pressure-Induced Superconductivity of Iodine			Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka, Osaka 560	J.Superconductivity 7(1994)921	K. Amaya,K. Shimizu,M. Ishizuka,N. Takeshita,N. Tamitani,S. Endo,T. Yamauchi		
106207	PR05508497		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C																		K		16.6					16.6		2																											kOe/K		5.59			HC6207M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106208	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.97Co0.06B2C1	Lu	1	Ni	1.97	Co	0.06	B	2	C	1														1	1997																												LuNi2B2C																		K		14					14		2																											kOe/K		4.89			HC6208M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106209	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni0.91Co0.18B2C1	Lu	1	Ni	0.91	Co	0.18	B	2	C	1														1	1997																												LuNi2B2C																		K		8.8					8.8		2																											kOe/K		3.27			HC6209M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106210	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.85Co0.3B2C1	Lu	1	Ni	1.85	Co	0.3	B	2	C	1														1	1997																												LuNi2B2C																		K		4.8					4.8		2																											kOe/K		2.47			HC6210M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106212	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.995Co0.01B2C1	Ho	1	Ni	1.995	Co	0.01	B	2	C	1														1	1997								5.4																				LuNi2B2C																		K		6.72					6.72		2																																																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106213	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.95Co0.03B2C1	Ho	1	Ni	1.95	Co	0.03	B	2	C	1														1	1997																												LuNi2B2C																		K		4.51					4.51		2																																																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106214	PR05508497		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1997								6.1																				LuNi2B2C																		K		10.6					10.6		2																																HC6214M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106215	PR05508497		Er(Ni,Co)2B2C	Er1Ni1.98Co0.04B2C1	Er	1	Ni	1.98	Co	0.04	B	2	C	1														1	1997								5.9																				LuNi2B2C																		K		8.2					8.2		2																																HC6214M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106216	PR05508497		Er(Ni,Co)2B2C	Er1Ni1.97Co0.06B2C1	Er	1	Ni	1.97	Co	0.06	B	2	C	1														1	1997								5.8																				LuNi2B2C																		K		6.6					6.6		2																																HC6214M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106217	PR05508497	reentrant at 5.6K	Er(Ni,Co)2B2C	Er1Ni1.9675Co0.065B2C1	Er	1	Ni	1.9675	Co	0.065	B	2	C	1														1	1997																												LuNi2B2C																		K		6.2					6.2		2																																HC6214M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106218	PR05508497		Er(Ni,Co)2B2C	Er1Ni1.9625Co0.075B2C1	Er	1	Ni	1.9625	Co	0.075	B	2	C	1														1	1997																												LuNi2B2C																		K		5.1					5.1		2																																HC6214M																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106219	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.991Co0.018B2C1	Lu	1	Ni	1.991	Co	0.018	B	2	C	1														1	1997																												LuNi2B2C																		K		15.6					15.6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106220	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.95Co0.1B2C1	Lu	1	Ni	1.95	Co	0.1	B	2	C	1														1	1997																												LuNi2B2C																		K		12.3					12.3																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106221	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.93Co0.14B2C1	Lu	1	Ni	1.93	Co	0.14	B	2	C	1														1	1997																												LuNi2B2C																		K		10.5					10.5																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106222	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.89Co0.22B2C1	Lu	1	Ni	1.89	Co	0.22	B	2	C	1														1	1997																												LuNi2B2C																		K		7.5					7.5																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106223	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.87Co0.26B2C1	Lu	1	Ni	1.87	Co	0.26	B	2	C	1														1	1997																												LuNi2B2C																		K		6					6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106224	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.83Co0.34B2C1	Lu	1	Ni	1.83	Co	0.34	B	2	C	1														1	1997																												LuNi2B2C																		K		3.8					3.8																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106225	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.81Co0.38B2C1	Lu	1	Ni	1.81	Co	0.38	B	2	C	1														1	1997																												LuNi2B2C																		K		2.9					2.9																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106226	PR05508497		Lu(Ni,Co)2B2C	Lu1Ni1.8Co0.4B2C1	Lu	1	Ni	1.8	Co	0.4	B	2	C	1														1	1997																												LuNi2B2C																		K		2.6					2.6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106227	PR05508497		TmNi2B2C 	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C																		K		11					11																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106228	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.99Co0.02B2C1	Tm	1	Ni	1.99	Co	0.02	B	2	C	1														1	1997																												LuNi2B2C																		K		10.3					10.3																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106229	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.98Co0.04B2C1	Tm	1	Ni	1.98	Co	0.04	B	2	C	1														1	1997																												LuNi2B2C																		K		9.2					9.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106230	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.97Co0.06B2C1	Tm	1	Ni	1.97	Co	0.06	B	2	C	1														1	1997																												LuNi2B2C																		K		8.7					8.7																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106231	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.96Co0.08B2C1	Tm	1	Ni	1.96	Co	0.08	B	2	C	1														1	1997																												LuNi2B2C																		K		7.7					7.7																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106232	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.94Co0.12B2C1	Tm	1	Ni	1.94	Co	0.12	B	2	C	1														1	1997																												LuNi2B2C																		K		5.9					5.9																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106233	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.92Co0.16B2C1	Tm	1	Ni	1.92	Co	0.16	B	2	C	1														1	1997																												LuNi2B2C																		K		4.4					4.4																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106234	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.91Co0.18B2C1	Tm	1	Ni	1.91	Co	0.18	B	2	C	1														1	1997																												LuNi2B2C																		K		3.2					3.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106235	PR05508497		Tm(Ni,Co)2B2C	Tm1Ni1.88Co0.24B2C1	Tm	1	Ni	1.88	Co	0.24	B	2	C	1														1	1997																												LuNi2B2C																		K		1.6					1.6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106236	PR05508497		Er(Ni,Co)2B2C	Er1Ni0.199Co0.02B2C1	Er	1	Ni	0.199	Co	0.02	B	2	C	1														1	1997								6																				LuNi2B2C																		K		9.2					9.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106237	PR05508497		Er(Ni,Co)2B2C	Er1Ni0.973Co0.054B2C1	Er	1	Ni	0.973	Co	0.054	B	2	C	1														1	1997								5.9																				LuNi2B2C																		K		7.2					7.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106238	PR05508497		Er(Ni,Co)2B2C	Er1Ni1.96Co0.08B2C1	Er	1	Ni	1.96	Co	0.08	B	2	C	1														1	1997																												LuNi2B2C																		K		4.2					4.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106239	PR05508497		Er(Ni,Co)2B2C	Er1Ni1.955Co0.09B2C1	Er	1	Ni	1.955	Co	0.09	B	2	C	1														1	1997																												LuNi2B2C																		K		2.6					2.6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106240	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.998Co0.004B2C1	Ho	1	Ni	1.998	Co	0.004	B	2	C	1														1	1997																												LuNi2B2C																		K		7.2					7.2																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106241	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.993Co0.014B2C1	Ho	1	Ni	1.993	Co	0.014	B	2	C	1														1	1997								5.3																				LuNi2B2C																		K		5					5																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106242	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.99Co0.02B2C1	Ho	1	Ni	1.99	Co	0.02	B	2	C	1														1	1997																												LuNi2B2C																		K		4.8					4.8																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106243	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.98Co0.04B2C1	Ho	1	Ni	1.98	Co	0.04	B	2	C	1														1	1997																												LuNi2B2C																		K		3.7					3.7																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106244	PR05508497		Ho(Ni,Co)2B2C	Ho1Ni1.972Co0.056B2C1	Ho	1	Ni	1.972	Co	0.056	B	2	C	1														1	1997																												LuNi2B2C																		K		2.4					2.4																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106245	PR05508497		DyNi2B2C 	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C																		K		4.6					4.6																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106246	PR05508497		Dy(Ni,Co)2B2C	Dy1Ni1.995Co0.01B2C1	Dy	1	Ni	1.995	Co	0.01	B	2	C	1														1	1997																												LuNi2B2C																		K		4.1					4.1																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106247	PR05508497		Dy(Ni,Co)2B2C	Dy1Ni1.99Co0.02B2C1	Dy	1	Ni	1.99	Co	0.02	B	2	C	1														1	1997																												LuNi2B2C																		K		3.1					3.1																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106248	PR05508497		Dy(Ni,Co)2B2C	Dy1Ni1.985Co0.03B2C1	Dy	1	Ni	1.985	Co	0.03	B	2	C	1														1	1997																												LuNi2B2C																		K		2.1					2.1																																																																																																					Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
106249	PR05508506	Resistive transition. All values are for field parallel to c-axis. G-L parameter = 17	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		15.6					15.6		1									Oe		369							kOe		65.2														A		71			A		1207																																																										Transport and superconducting properties of RNi2B2C(R=Y,Lu) single crystals	199704		Physics Department, Texas A&M University, College Station, Texas 77843-4242	Phys.Rev.B,55(1997)8506	A. Parasiris,A.K. Bhatnagar,A.K.Bhatnagar,A.Parasiris,B.K. Cho,B.K.Cho,D.G. Naugle,D.G.Naugle,K.D.D. Rathnayaka,K.D.D.Rathnayaka,P.C. Canfield,P.C.Canfield		
106250	PR05508506	Resistive transition. All values are for field parallel to c-axis. G-L parameter = 10.4	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		16.1					16.1		1									Oe		800							kOe		61.5														A		73			A		759																																																										Transport and superconducting properties of RNi2B2C(R=Y,Lu) single crystals	199704		Physics Department, Texas A&M University, College Station, Texas 77843-4242	Phys.Rev.B,55(1997)8506	A. Parasiris,A.K. Bhatnagar,A.K.Bhatnagar,A.Parasiris,B.K. Cho,B.K.Cho,D.G. Naugle,D.G.Naugle,K.D.D. Rathnayaka,K.D.D.Rathnayaka,P.C. Canfield,P.C.Canfield		
106251	JPS0682495		(Cu,Zn)Ir2S4	Cu0.7Zn0.3Ir2S4	Cu	0.7	Zn	0.3	Ir	2	S	4																	1999																												spinel																		K		2.8					2.8																																																																																																					Metal-Insulator Transition and Superconductivity in Spinel-Type System Cu1-xZnxIr2S4	199908		National Research Institute for Metals, Tsukuba 305-0047	J.Phys.Soc.Japan,68(1999)2495-2497	Akira Kamimura,Guanghan Cao,Hideaki Kitazawa,Hiroyuki Suzuki,Kazuto Hirata,Takao Furubayashi,Takehiko Matsumoto		
106252	JPS0682495		(Cu,Zn)Ir2S4	Cu0.5Zn0.5Ir2S4	Cu	0.5	Zn	0.5	Ir	2	S	4																	1999																												spinel																		K		2.2					2.2																																																																																																					Metal-Insulator Transition and Superconductivity in Spinel-Type System Cu1-xZnxIr2S4	199908		National Research Institute for Metals, Tsukuba 305-0047	J.Phys.Soc.Japan,68(1999)2495-2497	Akira Kamimura,Guanghan Cao,Hideaki Kitazawa,Hiroyuki Suzuki,Kazuto Hirata,Takao Furubayashi,Takehiko Matsumoto		
106253	PHC3200239	e-ph coupling constant = 0.38	Zr2Fe	Fe1Zr2	Fe	1	Zr	2																					1999																												CuAl2																	CuAl2, C16	K		0.17					0.17																																																								mj/mol.K2	14.5		261																																										Electrons, phonons and superconductivity in C16 structured Zr2Fe	199907		Condensed Matter Physics Division, Bhabha Atomic Research center, Trombay, Mumbai 400 085, India	Physica C,320(1999)239-244	A. Sathyamoorthy,G.P. Das,H.G. Salunke,K. Shashikala,P. Raj,R. Mittal,S.K. Dhar,S.L. Chaplot		
106254	PHC3120035	delta-Tc = 0.29 K, Tc by M(T)	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	1999																												LuNi2B2C																		K		14.91					14.91		2				0.21																																																																																										flux grown method					Boron isotope effect in single-crystal YNi2B2C and LuNi2B2C superconductors	199901		Ames Laboraratory and Department of Physics and Astronomy, IowaState University, Ames, IA 50011, USA	Physica.C,312(1998)35-39	I.R. Fisher,K.O. Cheon,P.C. Canfield		
106255	PHC3120035	delta-Tc = 0.16 K, Tc by M(T)	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1999																												LuNi2B2C																		K		15.75					15.75		2				0.11																																																																																										flux grown method					Boron isotope effect in single-crystal YNi2B2C and LuNi2B2C superconductors	199901		Ames Laboraratory and Department of Physics and Astronomy, IowaState University, Ames, IA 50011, USA	Physica.C,312(1998)35-39	I.R. Fisher,K.O. Cheon,P.C. Canfield		
106256	PHC3120001	T<sub>=700-900C. Debye-T calculated from resistivity	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																4	1999							3.2	6																				LuNi2B2C			A	3.51		10.57												K		9.5					9.5		1																																																									310																																					thin films by magnetron sputtering. Substrate = MgO					Properties of ErNi2B2C superconducting thin films	199901		Instituto Nazionale per la Fisica della Materia (INFM), Dipartimento di Scienze Fisiche, Universita di Napoli Federirico II, Piazzale Tecchio 80,1-80125 Naples, Italy	Physica.C,312(1998)1-6	A. Andreone,C. Aruta,F. Fontana,G.W. Crabtree,M. Iavarone,M. Polichetti,M.L. Russo,R. Vaglio,Y.De Wilde		
106257	JPS0682326		Sc5Co4Si10	Sc5Co4Si10	Sc	5	Co	4	Si	10																		1	1999																																														K		4.9					4.9																				kOe		7																																																																															NMR Investigation of the Electronic State in a Ternary Superconductor Sc5Co4Si10	199907		Graduate School of Science Technology and Faculty of Science, Kobe University, Nada, Kobe 657-0013	J.Phys.Soc.Japan,68(1999)2326-2330	Hiroshi Sugita,Kitomi Tsutsumi,Shinji Wada,Takehide Koyama		
106258	PMB0651445	not s/c. I-to-M transition at x=10 in Si36Nax. The resistivity shows more metallic as x increases beyond 10	Si36Nax	Na14Si36	Na	14	Si	36																					1992							1																					clathrate																		K					5																																																																																																							The insulator-to-metal transition in Si-Na 'clathrate' compounds: a search for superconductivity	199206		Physics Department and Centre for High Temperature Superconductivity, Blackett Laboratory, Imperial College, London SW7 2BZ, England	Philosophical Magazine B,65(1992)1445-1450	A.D.Caplin,K.E.Sim,S.B.Roy		
106259	NAT3720759	La2.8Ni2.0B2.2N3.0 by EPMA	La3Ni2B2N3	La3Ni2B2N3	La	3	Ni	2	B	2	N	3																	1994																															A	3.73		20.67											bct	K		13.2					13.2																																																																																																					Structure of the 13-K superconductor La3Ni2B2N3 and the related phase LaNiBN	12		National Centre for High Resolution Electron Microscopy, Laboratory of Materials Science, Delft University of Technology, Rotterdamseweg 137, 2628 AL Delft, The Netherlands	Nature,372(1994)759-761	H.W.Zandbergen,J.J.Krajewski,J.Jansen,R.J.Cava,W.F.Peck Jr		
106260	PHC3210108	dTc/dP in K/Gpa. Hc2(0) by linear extraporation. G-L parameter=9.5. coherence=84 A at 15 K.	YPd2B2C	Y1Pd2B2C1	Y	1	Pd	2	B	2	C	1																	1999																												LuNi2B2C																		K		22.6					22.6			K/GPa	-0.9							Oe		310							kG		133							kG/K		5.9					A		84																																																										arc-melting					Magnetic and high-pressure studies in the YPd2B2C system	199908		Department of Physics, Brock University, St. Chatharines, Ontario, Canada, L2S 3AI	Physica C,321(1999)108-112	F.S. Razavi,G. Quirion,H. Salamati,J. Murdoch		
106261	PHC3210093	RRR=6.9	(Tb,Er)Ni2B2C	Tb0.2Er0.8Ni2B2C1	Tb	0.2	Er	0.8	Ni	2	B	2	C	1														1	1999								7.1																				LuNi2B2C			A	3.5143		10.551												K		7.1					7.1																																																																																																Ar-arc melting					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
106262	PHC3210093	RRR=7.3	(Tb,Er)Ni2B2C	Tb0.225Er0.775Ni2B2C1	Tb	0.225	Er	0.775	Ni	2	B	2	C	1														1	1999								7																				LuNi2B2C			A	3.513		10.543												K		5.9					5.9																																																																																																Ar-arc melting					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
106263	PHC3210093	RRR=7.2	(Tb,Er)Ni2B2C	Tb0.25Er0.75Ni2B2C1	Tb	0.25	Er	0.75	Ni	2	B	2	C	1														1	1999								7.1																				LuNi2B2C			A	3.518		10.552												K		4.9					4.9																																																																																																Ar-arc melting					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
106264	PHC3340033	2gap/kTc = 3.63,	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																	2000								10.2																				LuNi2B2C																		K		6.51					6.51																																																1.02	1																																																				Point-contact spectroscopy of superconducting energy gap in DyNi2B2C	200006		B. Verkin Institute for Low Temperature Physics and Engineering, National Academy of Sciences, Lenin avenue, 47, 310164 Kharkiv, Ukraine	Physica C,334(2000)33-43	C.V. Tomy,D.McK. Paul,I.K. Yanson,N.L. Bobrov		
106265	PHC3330187	as-grown sample is not s/c. Rn=7.5 microOhm.cm. Effectve moment=4.34	YbPd2Sn	Yb1Pd2Sn1	Yb	1	Pd	2	Sn	1																			2000							-5.2	0.22																				Heusler			A	6.651													Cu2MnAl, L2<1>	K		2.3					2.3																																																								mj/mol.K2	6																																							arc-melting,then ANN(800C, 7days in vac)					Anomalous magnetic properties of Heusler superconductor YbPd2Sn	200005		Department of Physics, Faculty of Science, Tokyo Metropolitan University, Minami-Ohsawa 1-1, Hachioji-shi, Tokyo 192-0397, Japan 		Hideyuki Sato,Hiroki R. Sato,Hitoshi Sugawara,Yuji Aoki		
106266	PRL0825353		CeCu2Si2	Ce0.975Cu2Si2	Ce	0.975	Cu	2	Si	2																			1999								0.6																				CeCu2Si2																		K																																																																																																												Evolution from Magnetism to Unconventional Superconductivity in a Series of CexCu2Si2 Compounds Probed by Cu NQR			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett.82(1999)5353	C.Geible,F.Steglich,K.Asayama,K.Ishida,K.Kashima,K.Tabuchi,Y.Kawasaki,Y.Kitaoka		
106267	PRL0825353		CeCu2Si2	Ce1.025Cu2Si2	Ce	1.025	Cu	2	Si	2																			1999																												CeCu2Si2																		K		0.6					0.6																																																																																																					Evolution from Magnetism to Unconventional Superconductivity in a Series of CexCu2Si2 Compounds Probed by Cu NQR			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett.82(1999)5353	C.Geible,F.Steglich,K.Asayama,K.Ishida,K.Kashima,K.Tabuchi,Y.Kawasaki,Y.Kitaoka		
106268	PRL0825353		CeCu2Si2	Ce1Cu2.05Si2	Ce	1	Cu	2.05	Si	2																			1999																												CeCu2Si2																		K		0.7					0.7																																																																																																					Evolution from Magnetism to Unconventional Superconductivity in a Series of CexCu2Si2 Compounds Probed by Cu NQR			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett.82(1999)5353	C.Geible,F.Steglich,K.Asayama,K.Ishida,K.Kashima,K.Tabuchi,Y.Kawasaki,Y.Kitaoka		
106269	JSC1470399		SnEr4Rh6Sn18	Sn19Er4Rh6	Sn	19	Er	4	Rh	6																			1999							0.34																								A	13.733		27.418												K		1.32					1.32																																																																																																Sn melt technique. Single crystals were extracted from the melt.					Competition between Magnetism and Superconductivity in Erbium Stannide			Laboratoire de Cristallographie CNRS, BP166, 38042 Grenoble Cedex 9, France	J.Solid State Chem.147(1999)399-409	J.L. Hodeau,J.L.Hodeau,M. Marezio,M.Marezio,P. Bordet,P.Bordet,S. Miraglia,S.Miraglia		
106270	JSC1470399	re-entrant s/c. low temperature phase=ferromagnetic	(Sn,Er)Er4Rh6Sn18	Sn18.59Er4.41Rh6	Sn	18.59	Er	4.41	Rh	6																			1999							0.5																																							K		1					1																																																																																																Sn melt technique. Single crystals were extracted from the melt.					Competition between Magnetism and Superconductivity in Erbium Stannide			Laboratoire de Cristallographie CNRS, BP166, 38042 Grenoble Cedex 9, France	J.Solid State Chem.147(1999)399-409	J.L. Hodeau,J.L.Hodeau,M. Marezio,M.Marezio,P. Bordet,P.Bordet,S. Miraglia,S.Miraglia		
106271	JSC1470399	re-entrant s/c. low temperature phase=ferromagnetic	(Sn,Er)Er4Rh6Sn18	Sn18.43Er4.57Rh6	Sn	18.43	Er	4.57	Rh	6																			1999							0.5																																							K		0.97					0.97																																																																																																Sn melt technique. Single crystals were extracted from the melt.					Competition between Magnetism and Superconductivity in Erbium Stannide			Laboratoire de Cristallographie CNRS, BP166, 38042 Grenoble Cedex 9, France	J.Solid State Chem.147(1999)399-409	J.L. Hodeau,J.L.Hodeau,M. Marezio,M.Marezio,P. Bordet,P.Bordet,S. Miraglia,S.Miraglia		
106272	JSC1470399	ferromagnetic, not s/c	(Sn,Er)Er4Rh6Sn18	Sn18.39Er4.61Rh6	Sn	18.39	Er	4.61	Rh	6																			1999							0.64																																							K																																																																																																							Sn melt technique. Single crystals were extracted from the melt.					Competition between Magnetism and Superconductivity in Erbium Stannide			Laboratoire de Cristallographie CNRS, BP166, 38042 Grenoble Cedex 9, France	J.Solid State Chem.147(1999)399-409	J.L. Hodeau,J.L.Hodeau,M. Marezio,M.Marezio,P. Bordet,P.Bordet,S. Miraglia,S.Miraglia		
106273	PRL0830404	powder sample.  Tc defined as maximum dR/dT.  99% C<13> isotope	Rb3C60	C60Rb3	C	60	Rb	3																					1999																												fullerene																		K		30.8					30.8		1				0.21	C																																																																																														Carbon Isotope Effect in Single-Crystal R b3C60			Department of Physics, University of California at Berkeley, Berkeley,California 94720	Phys.Rev.Lett.83(1999)404	A. Zettl,A.Zettl,K. Cherrey,K.Cherrey,M.S. Fuhrer,M.S.Fuhrer,Marvin L. Cohen,Marvin L.Cohen		
106274	PHC3230071		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	1999																												LuNi2B2C																		K		7.8					7.8																																																																																																arc-melting-ANN(800C)					The effect of thermal treatment on superconductivity in HoNi2B2C	199910		Physikalisches Institut, Universitat Bayreuth, D-95440 Bayreuth, Germany	Physica C,323(1999)71-78	A. Dertinger,A. Krause,H. Schmidt,H.F. Braun,T.A. Wagner,W. Ettig		
106275	PHC3230071		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	1999																												LuNi2B2C																		K		7.1					7.1																																																																																																arc-melting-ANN(1100C)					The effect of thermal treatment on superconductivity in HoNi2B2C	199910		Physikalisches Institut, Universitat Bayreuth, D-95440 Bayreuth, Germany	Physica C,323(1999)71-78	A. Dertinger,A. Krause,H. Schmidt,H.F. Braun,T.A. Wagner,W. Ettig		
106276	PHC3330031	solid solution. P-type conductivity	(Sn,In)Te	Sn0.95In0.05Te1	Sn	0.95	In	0.05	Te	1																		1	2000																																														K		1.2					1.2																													kG/T		4.73																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106277	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.9405Ge0.0095In0.05Te1	Sn	0.9405	Ge	0.0095	In	0.05	Te	1																1	2000																																														K		1.61					1.61																													kG/T		5.27																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106278	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.9215Ge0.0285In0.05Te1	Sn	0.9215	Ge	0.0285	In	0.05	Te	1																1	2000																																														K		1.74					1.74																													kG/T		6.34																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106279	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.9025Ge0.0475In0.05Te1	Sn	0.9025	Ge	0.0475	In	0.05	Te	1																1	2000																																														K		1.72					1.72																													kG/T		6.25																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106280	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.874Ge0.076In0.05Te1	Sn	0.874	Ge	0.076	In	0.05	Te	1																1	2000																																														K		1.64					1.64																													kG/T		6.87																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106281	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.855Ge0.095In0.05Te1	Sn	0.855	Ge	0.095	In	0.05	Te	1																1	2000																																														K		1.48					1.48																													kG/T		8.21																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106282	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.8075Ge0.1425In0.05Te1	Sn	0.8075	Ge	0.1425	In	0.05	Te	1																1	2000																																														K		1.09					1.09																													kG/T		9.82																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106283	PHC3330031	solid solution. P-type conductivity. Structural transformation at 210 K.	(Sn,Ge,In)Te	Sn0.76Ge0.19In0.05Te1	Sn	0.76	Ge	0.19	In	0.05	Te	1																1	2000																																														K		0.68					0.68																													kG/T		8.57																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106284	PHC3330031	solid solution. P-type conductivity	(Sn,In)Te	Sn0.84In0.16Te1	Sn	0.84	In	0.16	Te	1																		1	2000																																														K		2.48					2.48																													kG/T		0.64																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106285	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.798Ge0.042In0.16Te1	Sn	0.798	Ge	0.042	In	0.16	Te	1																1	2000																																														K		2.36					2.36																													kG/T		0.74																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106286	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.756Ge0.084In0.16Te1	Sn	0.756	Ge	0.084	In	0.16	Te	1																1	2000																																														K		2.32					2.32																													kG/T		0.99																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106287	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.714Ge0.126In0.16Te1	Sn	0.714	Ge	0.126	In	0.16	Te	1																1	2000																																														K		2.23					2.23																													kG/T		0.97																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106288	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.672Ge0.168In0.16Te1	Sn	0.672	Ge	0.168	In	0.16	Te	1																1	2000																																														K		1.93					1.93																													kG/T		0.85																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106289	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.63Ge0.21In0.16Te1	Sn	0.63	Ge	0.21	In	0.16	Te	1																1	2000																																														K		1.87					1.87																													kG/T		1.38																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106290	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.588Ge0.252In0.16Te1	Sn	0.588	Ge	0.252	In	0.16	Te	1																1	2000																																														K		1.42					1.42																													kG/T		1.52																																																																						Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106291	PHC3330031	solid solution. P-type conductivity	(Sn,Ge,In)Te	Sn0.504Ge0.336In0.16Te1	Sn	0.504	Ge	0.336	In	0.16	Te	1																1	2000																																														K		0.42					0.42																																																																																																					Observation of superconducting and structural phase transitions in Sn1-zGezTe:In solid solutions	200005		State Technical University, Politechnicheskaya str. 29, 195251 St. Petersburg, Russia	Physica C,333(2000)31-40	D. Kaczorowski,D.I. Popov,D.V. Shamshur,J. Stepien-Damm,M.O. Safonchik,P.P. Konstantinov,R.V. Parfeniev,S.A. Nemov		
106292	PRL0552727			U1Ru2Si2	U	1	Ru	2	Si	2																		1	1985								17.5																				ThCr2Si2			A	4.121		9.681												K		1.1					1.1																																																					MSP6292			mj/mol.K2	180		312																																					arc-melting - ANN(1000C 7days in vac)					Superconducting and Magnetic Transitions in the Heavy-Fermion System URu2Si2	198512		Kamerlingh Onnes Laboratorium der Rijks-Universiteit Leiden, 2300 RA Leiden ,The Netherlands	Phys.Rev.Lett.,55(1985)2727-2730	A.A.Menovsky,A.J.Dirkmaat,G.J.Nieuwenhuys,J.A.Mydosh,J.van den Berg,P.H.Kes,T.T.M.Palstra		
106293	PRL0552727	dHc2/dT is for H//both a-and c-axis Hc1= d675mK, H//ar b clirection. G-L parameter = 33		U1Ru2Si2	U	1	Ru	2	Si	2																		3	1985							-65	17.5																							A	4.1279		9.5918												K																				14																		4			MHC6293																																																														Czochralski tri-arc method.					Superconducting and Magnetic Transitions in the Heavy-Fermion System URu2Si2	198512		Kamerlingh Onnes Laboratorium der Rijks-Universiteit Leiden, 2300 RA Leiden ,The Netherlands	Phys.Rev.Lett.,55(1985)2727-2730	A.A.Menovsky,A.J.Dirkmaat,G.J.Nieuwenhuys,J.A.Mydosh,J.van den Berg,P.H.Kes,T.T.M.Palstra		
106294	PHC2290079			U1Ru2Si2	U	1	Ru	2	Si	2																			1994																																														K		1.24					1.24																																																					MSP6294																																																Specific heat of the antiferromagnetic heavy-fermion superconductor URu2Si2	1994		Centre de Recherches sur les Tre's Basses Temperatures, Laboratoire associe a l'Universite Joseph Fourier, CNRS, BP 166,38042 Grenoble-Cedex 9, france	Physica.C,229(1994)79-89	A. Buzdin,J. Flouquet,J.P. Brison,P. Lejay		
106295	EPL0330557	gap values for along a-axis. For c-axis, gap= 1.4meV, 2*gap/kTc=12.  Hc2 defined by (dI/dV) measurements	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	1996																																														K		1.3					1.3		1																		T						8	2	0.05																				5	1																																																				Anisotropy of the superconducting energy gap in URu2Si2 studied by point-contact spectroscopy	199603		Physikalisches Institut, Universitat Karlsruhe- 76128 Karlsruhe, Germany	Europhys.Lett.,33(1996)557-562	A.A.Menovsky,G.Goll,H.V.Lohneysen,I.K.Yanson,Yu.G.Naidyuk		
106296	SSC0930021		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C			A	3.528		10.546												K		14.5					14.5													0.0435									6.38									0.44							97					1200																220																																					ANN (1200K, 5days) - slow cool to RT					Synthesis and Physical properties of the YNi2B2C superconducting phase	199501		Istituto di Chimica Fisica, Universita di Genova, C.so Europa 26, 16132 Genova Italia	SolidState Commun.,93(1995)21-24	A.Palenzona,C.Ferdeghini,D.Marre,F.Canepa,P.Manfrinetti,V.Calzona		
106297	PHC2500227	values of super conducting paramete are at 21C. G-L parameter = 8.7		Cu1.5Rh1.5S4	Cu	1.5	Rh	1.5	S	4																			1995																												spinel			A	9.7885														K		4.5					4.5													470									13.5																156					1340																																																					vacuum shield ampoul method					63 Cu NMR study of the superconducting thiospinel Cu1.5Rh1.5S4	199508		(a)Department of Physics,Faculty of Engineering,Tokushima University,   Tokushima 770,Japan (b)Department of Physics,Faculty of Science,Ehime University,Matsuyama 790,Japan (c)Instute Solid State Physics,University of Tokyo,Roppongi,Tokyo 106, Japan	Physica C,250(1995)227-234	Kazuo Miyatani (b),Masayasu Ishikawa (c),Takashi ohno,Yutaka Kishimoto (a)	Cu, Rh, S	
106298	PHC3210108	Hc2(O) by linecr extrporation. At 15K, coherence = 84A, G-L= 9.5		Y1Pd2B2C1	Y	1	Pd	2	B	2	C	1																	1999																																														K		22.6					22.6			K/GPa	-0.09									310									133									-5.9																																																																	arc- melting					Magnetic and high-pressure studies in the YPd2B2C system	199908		Department of Physics, Brock University, St. Chatharines, Ontario, Canada, L2S 3AI	Physica C,321(1999)108-112	F.S. Razavi,G. Quirion,H. Salamati,J. Murdoch		
106299	PR05912054			Y2Rh3Sn5	Y	2	Rh	3	Sn	5																		1	1999																												Y2Rh3Sn5			A	4.395	26.151	7.137												K																																																																		222																																					arc-melting					Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106300	PR05912054			La2Rh3Sn5	La	2	Rh	3	Sn	5																		1	1999																												U2Co3Si5			A	10.667	12.891	6.315												K		1.85					1.85																																																											190																																					arc-melting					Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106301	PR05912054			Ce2Rh3Sn5	Ce	2	Rh	3	Sn	5																		1	1999							-52	5																				Y2Rh3Sn5			A	4.506	26.383	7.212												K																																																																																																							arc-melting					Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106302	PR05912054			Pr2Rh3Sn5	Pr	2	Rh	3	Sn	5																		1	1999							-5.4																					Y2Rh3Sn5			A	4.481	26.444	7.208												K																																																																		333																																					arc-melting					Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106303	PR05912054	GAMMA is in unit of mJ/Nd-mole.K2		Nd2Rh3Sn5	Nd	2	Rh	3	Sn	5																		1	1999							-8.2																					Y2Rh3Sn5			A	4.467	26.363	7.205												K																																																															mj/mol.K2	300		201																																					arc-melting					Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106304	PR05912054			Gd2Rh3Sn5	Gd	2	Rh	3	Sn	5																		1	1999							-0.34	10																				Y2Rh3Sm5			A	4.419	26.132	7.167												K																																																																		244																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106305	PR05912054			Tb2Rh3Sn5	Tb	2	Rh	3	Sn	5																		1	1999							-7.4	7																				Y2Rh3Sm5			A	4.402	26.183	7.14												K																																																																		248																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106306	PR05912054			Dy2Rh3Sn5	Dy	2	Rh	3	Sn	5																		1	1999							-1.47	6.5																				Y2Rh3Sm5			A	4.396	26.188	7.138												K																																																																		230																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106307	PR05912054			Ho2Rh3Sn5	Ho	2	Rh	3	Sn	5																		1	1999							-1.02	4.5																				Y2Rh3Sm5			A	4.38	26.111	7.132												K																																																																		267																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106308	PR05912054			Er2Rh3Sn5	Er	2	Rh	3	Sn	5																		1	1999							-9.98	3.2																				Y2Rh3Sm5			A	4.355	26.128	7.132												K																																																																		175																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106309	PR05912054			Tm2Rh3Sn5	Tm	2	Rh	3	Sn	5																		1	1999							-14.57	2.3																				Y2Rh3Sm5			A	4.341	26.198	7.147												K		1.8					1.8																																																											185																																										Magnetic ordering and superconductivity in R2Rh3Sn5(R=La-Tm,Y) systems	199905		Tata Institute Of Fundamental Research, Bombay-400005, India	Phys.Rev.B,59(1999)12054-12063	N.G.Patil,S.Ramakrishnan		
106310	JPS0651555	values in TBL are for H//a-axis, Hc2(O)=2.9KOe and dHc2/dT=4.2KOe/K for H//c-axis. Hc1(O)estimated from Hc1(0.53K)=200Oe. G-L parameter = 11.		U1Ni2Al3	U	1	Ni	2	Al	3																		3	1996								4.2																				PrNi2Al3																		K		1					1											Oe		27.8							KOe			7.9	2.9					KOe/K			11.4	4.2	MHC6310																																																														single crystal by Czochralski method					Anisotropy of Upper Critical Magnetic Fields in Heavy Fermion Superconductor UNi2Al3	199606		Physics Department, Graduate School of Science, Tohoku University, Sendai 980-77	J.Phys.Soc.Japan,65(1996)1555-1558	Nobuhiko Koga,Noriaki Sato,Takemi komatsubara		
106311	PRL0824914	Hc1(O), Hc2(O) are calculated from Hc1(2.3K)=250Oe and Hc2(2.3K)=2.9T assuming Hc=Ho(1-t2)	NbSe2	Nb1Se2	Nb	1	Se	2																					1999																												2H-NbSe2																		K		7					7											Oe		280							T		3.25																																		mj/mol.K2	15.7		218																																										Low Field Anomaly in the Specific Heat of s-Wave Superconductors due to the Expansion of the Vortex Cores			Los Alamos National Laboratory, Los Aloamos, New Mexico 87545	Phys.Rev.Lett.82(1999)1914	J.D.Thompson,J.E.Sonier,J.W.Brill,M.F.Hundley		
106312	PR05506584			Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	1997																															A	3.6378		10.2273											bct	K																																																																																																							arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106313	PR05506584			Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																1	1997								4																							A	3.7066		9.9993												K																																																																																																							arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106314	PR05506584			Nd1Ni2B2C1	Nd	1	Ni	2	B	2	C	1																1	1997								4.8																							A	3.678		10.0814												K																																																																																																							arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106315	PR05506584			Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																1	1997								15																							A	3.5536		10.4352												K																																																																																																							arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106316	PR05506584		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	1997								10.6																				LuNi2B2C			A	3.5342		10.4878												K		6					6																																																																																																arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106317	PR05506584		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1997								8.5																				LuNi2B2C			A	3.5177		10.5278												K		8					8																																																																																																arc-melting in Ar.					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106318	PR05506584		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																	1997								4.8																				LuNi2B2C			A	3.5019		10.558												K		11					11																																																																																																					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106319	PR05506584		TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																	1997								1.53																				LuNi2B2C			A	3.4866		10.586												K		11					11																																																																																																					Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106320	PR05506584			Yb1Ni2B2C1	Yb	1	Ni	2	B	2	C	1																	1997																															A	3.4782		10.607												K																																																																																																												Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106321	PR05506584			Gd1Ni2B2C1	Gd	1	Ni	2	B	2	C	1																	1997								19																																						K																																																																																																												Magnet order and crystal structure in the superconducting RNi2B2C materials	199703		Reactor Radiation, National Institute of Standards and Technology, Gaithersburg, maryland 20899	Phys.Rev.B,55(1997)6584	C. Gadart,J.W.Lynn,L.C.Gupta,Q.Huang,R.Nagarajan,S.K.Sinha,S.Skanthakumar,Z.Hossain		
106322	JSC1450159	stuble. by high-temp synthesis. Figure shows Tc vs x in. HT-Mo6Se8-xSx	HT-Mo6Se8-xSx	Mo6Se8	Mo	6	Se	8																					1999																												Chevrel																		K		6.28					6.28	MTC6322																																																																																																				First Example of Molybdenum Atoms in the Network of High Temperature Chevrel Phases: Moy[Mo6Se8-xSx]			Laboratoire de Chimie du Solide et Inorganique Moleculaire(LCSIM), UMR CNRS 6511,Universite de Rennes-1, Avenue du General Leclerc, 35042 Rennes Cedex, France	J.Solid State Chem.145(1999)159-166	Marcel Sergent,Roger Chevrel,Stephanie Belin		
106323	JSC1450159	metastable. obtained by soft chemistry process from HT-Mo6Se8-xSx. Figure shows Tc vs x in alpha-Mo6Se8-xSx	alpha-Mo6Se8-xSx	Mo6Se8	Mo	6	Se	8																					1999																												Chevrel																		K		6.13					6.13	MTC6323																																																																																																				First Example of Molybdenum Atoms in the Network of High Temperature Chevrel Phases: Moy[Mo6Se8-xSx]			Laboratoire de Chimie du Solide et Inorganique Moleculaire(LCSIM), UMR CNRS 6511,Universite de Rennes-1, Avenue du General Leclerc, 35042 Rennes Cedex, France	J.Solid State Chem.145(1999)159-166	Marcel Sergent,Roger Chevrel,Stephanie Belin		
106324	PLA0750386		Sc2Fe3Si5	Sc2Fe3Si5	Sc	2	Fe	3	Si	5																			1980																												R2Fe3Si5			A	10.225		5.275												K		4.52					4.52		2																																																																																														arc-melting, then annealing in vac					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
106325	PLA0750386		Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																			1980																												R2Fe3Si5			A	10.43		5.47												K		2.4					2.4		2																																																																																														arc-melting, then annealing in vac					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
106326	PLA0750386		Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																			1980																												R2Fe3Si5			A	10.34		5.375												K		6.1					6.1		2																																																																																														arc-melting, then annealing in vac					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
106327	PR02802732		Yb2Fe3Si5	Yb2Fe3Si5	Yb	2	Fe	3	Si	5																			1983								1.7																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106328	PR02802732		Tm2Fe3Si5	Tm2Fe3Si5	Tm	2	Fe	3	Si	5																			1983								1.06																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106329	PR02802732	Three more Neel-T (=2.401,2.381,2.352 K) are found.	Er2Fe3Si5	Er2Fe3Si5	Er	2	Fe	3	Si	5																			1983								2.79																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106330	PR02802732		Ho2Fe3Si5	Ho2Fe3Si5	Ho	2	Fe	3	Si	5																			1983								2.82																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106331	PR02802732		Dy2Fe3Si5	Dy2Fe3Si5	Dy	2	Fe	3	Si	5																			1983								4.2																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106332	PR02802732	Another Neel-T (=7.06 K) is found.	Tb2Fe3Si5	Tb2Fe3Si5	Tb	2	Fe	3	Si	5																			1983								10.02																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106333	PR02802732		Gd2Fe3Si5	Gd2Fe3Si5	Gd	2	Fe	3	Si	5																			1983								8.4																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106334	PR02802732	Three more Neel-T (=7.35, 6.19, 5.05 K) are found.	Sm2Fe3Si5	Sm2Fe3Si5	Sm	2	Fe	3	Si	5																			1983								8.96																				R2Fe3Si5																		K					0.5																																																																																																		arc-melting					Low-temperature heat capacity of antiferromagnetic ternary rare-earth iron silicides M2Fe3Si5	198309		Ames Laboratory and Department of Physics, Iowa State University, Ames, Iowa 50011	Phys.Rev.B,28(1983)2732-2742	C.B.Vining,R.N.Shelton		
106335	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.57. Sus(300)=0.39 E-4 emu/mol.	Th7Ni3	Ni3Th7	Ni	3	Th	7																					2000																												Fe3Th7																		K		1.97					1.97																													kG																											mj/mol.K2	53		169																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106336	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.55. Sus(300)=6.9 E-4 emu/mol.	Th7Co3	Co3Th7	Co	3	Th	7																					2000																												Fe3Th7																		K		1.8					1.8																				kG		3.4							kG		2.7																									mj/mol.K2	43		184																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106337	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.58.	Th7Fe3	Fe3Th7	Fe	3	Th	7																					2000																												Fe3Th7																		K		2.1					2.1																				kG		5							kG		3.4																									mj/mol.K2	57		178																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106338	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.55. Sus(300)=1.0 E-4 emu/mol.	La7Pd3	La7Pd3	La	7	Pd	3																					2000																												Fe3Th7																		K		1.48					1.48																				kG		2.8							kG		2.7																									mj/mol.K2	47		152																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106339	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.64. Sus(300)=3.3 E-4 emu/mol.	La7Rh3	La7Rh3	La	7	Rh	3																					2000																												Fe3Th7																		K		2.6					2.6																				kG		7.28							kG		4																									mj/mol.K2	48		160																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106340	PHC3360010	Hc2(0) estimated from dHc2/dT. Ugamma=mJ/mol.K2. E-ph coupling const.=0.58. Sus(300)=2.8 E-4 emu/mol.	La7Ru3	La7Ru3	La	7	Ru	3																					2000																												Fe3Th7																		K		1.92					1.92																				kG		8.06							kG		6																									mj/mol.K2	42		165																																					arc-melt,then ANN using Ta-foil					Magnetic and superconducting properties of A7B3 compounds (A=Th or La and B=Ni,Co,Fe or Pd,Rh,Ru)	200007		Lab. de Bajas Temperaturas, Centro Atomico Bariloche (CNEA) and CONICET, 8400 S.C. de Bariloche, Argentina	Physica C,336(2000)10-18	G.Schmerber,J.G.Sereni,J.P.Kappler,M.Gomez Berisso,P.Pedrazzini		
106341	LTP1051511		SrTa2S5	Sr1Ta2S5	Sr	1	Ta	2	S	5																			1996																															A	3.32		24.1											hexagonal	K		3.16					3.16																																																																																																					Superconductivity in SrTa2S5				J.Low Temp.Phys., 105(1996)1511	Norihiko Kijima,Kenichi Morie,Shoichi Nagata,Isao Shimono		
106342	JSC1160392		BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																			1995																															A	3.3258		25.208											hexagonal	K		2.88					2.88																																																																																																					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
106343	JSC1160392		BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																			1995																															A	3.3204		25.005											hexagonal	K		3.14					3.14																																																																																																					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
106344	EPJ0120013	Tc from ESR and M/H measurements. Gap=2delta/kTc	NaxWO3	Na0.05W1O3	Na	0.05	W	1	O	3																			1999																												CaTiO3																	CaTiO3, perovskite	K		91					91																																																3.5																																																					Electron spin resonance and magnetic susceptibility suggest superconductivity in Na doped WO3 samples	199901		Physik-Institut der Universitat Zurich, 8057 Zurich, Switzerland	Eur.Phys.J.B,12(1999)13-15	A.Shengelaya,K.A.Muller,S.Reich,Y.Tsabba		
106345	EPJ0090001	surface superconductor. Zero resistivity was not observed.	NaxWO3	Na0.05W1O3	Na	0.05	W	1	O	3																			1999																												CaTiO3																	CaTiO3, perovskite	K		91					91																																																																																																0.5 at % Na-WO3 powder, then heat treated.					Possible nucleation of a 2D superconducting phase on WO3 single crystals surface doped with Na+	199901		Department of Materials and Interfaces, The Weizmann Institute of Science, Rehovot 76100, Israel	Eur.Phys.J.B,9(1999)1-4	S.Reich,Y.Tsabba		
106346	PR05312389	not s/c under 1 atm. Pressure induced s/c. Tc(max)=3.13 K at about 9 kBar. dTc/dP is in K/GPa for s/c state.	Tm2Fe3Si5	Tm2Fe3Si5	Tm	2	Fe	3	Si	5																		1	1996								1.1																				R2Fe3Si5			A	10.37		5.405												K		3.13			0		3.13			K/GPa	4.7																																																																																												arc-melting, then annealing in vac					Influence of phase composition on the reentrant superconducting properties of Tm2Fe3Si5	05		"Physikalisches Institut, Universita""t Bayreuth,95440 Bayreuth, Germany"	Phys.Rev.B,53(1996)12389	H.F.Braun,H.Schmidt,M.Muller	Tm, Fe, Si	
106347	PHC3150091		(Ho,La)Ni2B2C	Ho0.8La0.2Ni2B2C1	Ho	0.8	La	0.2	Ni	2	B	2	C	1														1	1999																												LuNi2B2C			A	3.55		10.4554												K		1.3					1.3																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106348	PHC3150091		(Ho,La)Ni2B2C	Ho0.9La0.1Ni2B2C1	Ho	0.9	La	0.1	Ni	2	B	2	C	1														1	1999																												LuNi2B2C			A	3.522		10.5138												K		2.25					2.25																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106349	PHC3150091		(Ho,La)Ni2B2C	Ho0.93La0.07Ni2B2C1	Ho	0.93	La	0.07	Ni	2	B	2	C	1														1	1999																												LuNi2B2C																		K		3					3																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106350	PHC3150091		(Ho,La)Ni2B2C	Ho0.95La0.05Ni2B2C1	Ho	0.95	La	0.05	Ni	2	B	2	C	1														1	1999																												LuNi2B2C																		K		6.62					6.62																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106351	PHC3150091		(Ho,La)Ni2B2C	Ho0.97La0.03Ni2B2C1	Ho	0.97	La	0.03	Ni	2	B	2	C	1														1	1999																												LuNi2B2C																		K		7.44					7.44																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106352	PHC3150091		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1999																												LuNi2B2C			A	3.5146		10.5262												K		8.56					8.56																																																																																																arc-melting					Suppression of superconductivity by non magnetic impurities, structural properties and magnetic ordering in HoxLa1-xNi2B2C	199904		Institute fur Festkorper-und Werkstofforschung Dresden, Postfach 270016, D-01171 Dresden, Germany	Physica C,315(1999)91-98	A. Kreyssig,A.Kreyssig,C. Ritter,C.Ritter,G. Fuchs,G.Fuchs,J. Freudenberger,J.Freudenberger,K-H. Muller,K. Nenkov,K.-H.Muller,K.Nenkov,L. Schultz,L.Schultz,M. Loewenhaupt,M.Loewenhaupt,S.-L. Drechsler,S.-L.Drechsler		
106435	JPC0097419	quenched sample	La3Ni	La3Ni1	La	3	Ni	1																				1	1997																															A	7.271	10.243	6.647											orthorhombic	K		2.4					2.4																																																																																																arc melting-ANN(500C,1week)					Magnetic and superconducting behaviour of the R3Ni (R=La, Gd, Tb, Ho and Er) systems			Low-Teperature Physics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400 005, India	J.Phys.C,9(1997)7419	C S  Garde,J  Ray		
108000	LTP0510179	Delta-C/gamma*Tc=2.1, gamma (in mJ/K2.gat)	Nb3Al	Al0.24Nb0.76	Al	0.24	Nb	0.76																				1	1983																												Cr3Si(A15)			A	5.186													Cr3Si, A15	K		18.7					18.7		3																																														5.6	2							mj/mol.K2	9		283																																					arc-melting					Effect of Self-Annealing and Reirradiation on the Specific Heat of Nb3Al			Los Alamos National Laboratory, Los Alamos, New Mexico	J.Low Temp.Phys., 51(1983)179	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108001	LTP0510179	neutron fluence = 0.18E+19 n/cm2. Delta-C/gamma*Tc=2.4, gamma (in mJ/K2.gat)	Nb3Al	Al0.24Nb0.76	Al	0.24	Nb	0.76																				1	1983																												Cr3Si(A15)																	Cr3Si, A15	K		16.9					16.9		3																																														4.7	2							mj/mol.K2	7.5		315																																					arc-melting + neutron irrad.					Effect of Self-Annealing and Reirradiation on the Specific Heat of Nb3Al			Los Alamos National Laboratory, Los Alamos, New Mexico	J.Low Temp.Phys., 51(1983)179	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108002	LTP0510179	neutron fluence = 1.5E+19 n/cm2. Delta-C/gamma*Tc=1.6,  gamma (in mJ/K2.gat)	Nb3Al	Al0.24Nb0.76	Al	0.24	Nb	0.76																				1	1983																												Cr3Si(A15)																	Cr3Si, A15	K		7.1					7.1		3																																														3.4	2							mj/mol.K2	4.5																																							arc-melting + neutron irrad.					Effect of Self-Annealing and Reirradiation on the Specific Heat of Nb3Al			Los Alamos National Laboratory, Los Alamos, New Mexico	J.Low Temp.Phys., 51(1983)179	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108003	LTP0510179	neutron fluence = 3.8E+19 n/cm2. Delta-C/gamma*Tc=1.4, gamma (in mJ/K2.gat)	Nb3Al	Al0.24Nb0.76	Al	0.24	Nb	0.76																				1	1983																												Cr3Si(A15)																	Cr3Si, A15	K		3.9					3.9		3																																														3.2	2							mj/mol.K2	3.5		367																																					arc-melting + neutron irrad.					Effect of Self-Annealing and Reirradiation on the Specific Heat of Nb3Al			Los Alamos National Laboratory, Los Alamos, New Mexico	J.Low Temp.Phys., 51(1983)179	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108004	PR0291189	Delta-C/gamma*Tc=2.29, gamma (in mJ/K2.gat)	Nb3Al	Al1Nb3	Al	1	Nb	3																					1984																												Cr3Si(A15)			A	5.18													Cr3Si, A15	K		16.84					16.84																																																								mj/mol.K2	9.4		328																																					arc-melt + ANN+Q					Specific heat and magnetic susceptibility of nearly stoichiometric and homogeneous Nb3Al	198402			Phys.Rev.B, 29(1984)1189	A.Junod,J.-L.Jorda,J.Muller,M.Pelizzone		
108005	PR0291189	Delta-C/gamma*Tc=2.35, gamma (in mJ/K2.gat)	Nb3Al	Al1Nb3	Al	1	Nb	3																					1984																												Cr3Si(A15)			A	5.18													Cr3Si, A15	K		18.45					18.45																																																								mj/mol.K2	11.24		296																																					arc-melt + ANN+Q+ANN					Specific heat and magnetic susceptibility of nearly stoichiometric and homogeneous Nb3Al	198402			Phys.Rev.B, 29(1984)1189	A.Junod,J.-L.Jorda,J.Muller,M.Pelizzone		
108006	LTP0480503	gap parameter derived from BCS-relation.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1982																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																4.1	2							mj/mol.K2	11.4		170																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108007	LTP0480503	gap parameter derived from BCS-relation.	Nb3Al	Al1Nb3	Al	1	Nb	3																					1982																												Cr3Si(A15)																	Cr3Si, A15	K		18.2					18.2																																																3.55	2							mj/mol.K2	13.9		171																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108008	LTP0480503	gap parameter derived from BCS-relation.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1982																												Cr3Si(A15)																	Cr3Si, A15	K		5.9					5.9																																																3.36	2							mj/mol.K2	7.64		230																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108009	LTP0480503	gap parameter derived from BCS-relation.	Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.3					6.3																																																3.75	2							mj/mol.K2	40		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108010	LTP0480503	gap parameter derived from BCS-relation.	Mo6Se6Br2	Mo6Se6Br2	Mo	6	Se	6	Br	2																			1982																												Chevrel																		K		6.7					6.7																																																3.92	2							mj/mol.K2	44		130																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108011	LTP0480503	gap parameter derived from BCS-relation.	CuMo6Se8	Cu1Mo6Se8	Cu	1	Mo	6	Se	8																			1982																												Chevrel																		K		5.9					5.9																																																3.23	2							mj/mol.K2	40		155																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108012	LTP0480503	gap parameter derived from BCS-relation.	LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		11.6					11.6																																																3.57	2							mj/mol.K2	83		150																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108013	LTP0480503		CdMo6Se8	Cd1Mo6Se8	Cd	1	Mo	6	Se	8																			1982																												Chevrel																		K		2.4					2.4																																																								mj/mol.K2	55		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108014	LTP0480503		SnMo6Se8	Sn1Mo6Se8	Sn	1	Mo	6	Se	8																			1982																												Chevrel																		K		3.4					3.4																																																								mj/mol.K2	26.3		140																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108015	LTP0480503		PbMo6Se8	Pb1Mo6Se8	Pb	1	Mo	6	Se	8																			1982																												Chevrel																		K		4					4																																																								mj/mol.K2	31		125																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108016	LTP0480503	gap parameter derived from BCS-relation.	AgMo6S8	Ag1Mo6S8	Ag	1	Mo	6	S	8																			1982																												Chevrel																		K		7.7					7.7																																																3.58	2							mj/mol.K2	30		180																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108017	LTP0480503		GdMo6S8	Gd1Mo6S8	Gd	1	Mo	6	S	8																			1982																												Chevrel																		K		1.8					1.8																																																								mj/mol.K2	27		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108018	LTP0480503	gap parameter derived from BCS-relation.	SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.7					11.7																																																3.53	2							mj/mol.K2	107		135																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108019	LTP0480503	gap parameter derived from BCS-relation.	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		13.7					13.7																																																3.48	2							mj/mol.K2	125		140																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108020	LTP0480503	gap parameter derived from BCS-relation.	LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1982																												Chevrel																		K		6.8					6.8																																																3.31	2							mj/mol.K2	22.6		180																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108021	LTP0480503		Mo6S8	Mo6S8	Mo	6	S	8																					1982																												Chevrel																		K		1.8					1.8																																																								mj/mol.K2	28.3		230																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108022	LTP0480503	gap parameter derived from BCS-relation.	Mo6S6Br2	Mo6S6Br2	Mo	6	S	6	Br	2																			1982																												Chevrel																		K		13					13																																																3.5	2							mj/mol.K2	71.5		195																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108023	LTP0480503	gap parameter derived from BCS-relation.	Mo6S6I2	Mo6S6I2	Mo	6	S	6	I	2																			1982																												Chevrel																		K		13					13																																																3.55	2							mj/mol.K2	64		170																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108024	LTP0480503	gap parameter derived from BCS-relation.	Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10.7					10.7																																																3.46	2							mj/mol.K2	48.5		250																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108025	LTP0480503		ZnMo6S8	Zn1Mo6S8	Zn	1	Mo	6	S	8																			1982																												Chevrel																		K		2.8					2.8																																																								mj/mol.K2	25.3		225																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
108026	PR0243794	C(T) measured  upto 16 K.	Nb3Al	Al1Nb3	Al	1	Nb	3																					1981																												Cr3Si(A15)																	Cr3Si, A15	K		18.7					18.7																																																								mj/mol.K2	36		272																																					arc-melt+ANN					Specific-heat studies of neutron-irradiated A15 Nb3Al	198110			Phys.Rev.B, 24(1981)3794	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108027	PR0243794	neutron irrad. (1.3E+18 n/cm2). C(T) measured upto 16 K.	Nb3Al	Al1Nb3	Al	1	Nb	3																					1981																												Cr3Si(A15)																	Cr3Si, A15	K		17.9					17.9																																																								mj/mol.K2	34		276																																					arc-melt+ANN+irrad.					Specific-heat studies of neutron-irradiated A15 Nb3Al	198110			Phys.Rev.B, 24(1981)3794	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108028	PR0243794	neutron irrad. (1.3E+19 n/cm2). C(T) measured upto 16 K.	Nb3Al	Al1Nb3	Al	1	Nb	3																					1981																												Cr3Si(A15)																	Cr3Si, A15	K		9.9					9.9																																																								mj/mol.K2	17		325																																					arc-melt+ANN+irrad.					Specific-heat studies of neutron-irradiated A15 Nb3Al	198110			Phys.Rev.B, 24(1981)3794	A.R.Sweedler,B.Cort,C.L.Snead,Jr,G.R.Stewart,S.Moehlecke		
108029	APL0470640	Hc2(0) estimated from dHc2/dT using WHH theory	Nb-Al	Al0.245Nb0.725	Al	0.245	Nb	0.725																					1985																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																				T		32							T/K		2.49			MHC8029																																																														arc-melt+ANN+Q					High magnetic field transport properties of liquid quenched Nb3Al and Nb3Al(Si,Ge) superconducting compounds			Division of Applied Science, Harvard University, Cambridge, Massachusetts, USA	Appl.Phys. Lett., 47(1985)640	D.Turnbull,F.Habbal,F.Habbal,,G.Clemente,J.Bevk		
108030	APL0470640	Hc2(0) estimated from dHc2/dT using WHH theory	Nb-Al-Si	Nb0.747Al0.239Si0.014	Nb	0.747	Al	0.239	Si	0.014																			1985																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																				T		36							T/K		2.88			MHC8030																																																														arc-melt+ANN+Q					High magnetic field transport properties of liquid quenched Nb3Al and Nb3Al(Si,Ge) superconducting compounds			Division of Applied Science, Harvard University, Cambridge, Massachusetts, USA	Appl.Phys. Lett., 47(1985)640	D.Turnbull,F.Habbal,F.Habbal,,G.Clemente,J.Bevk		
108031	APL0470640	Hc2(0) estimated from dHc2/dT using WHH theory	Nb-Al-Ge	Nb0.758Al0.174Ge0.069	Nb	0.758	Al	0.174	Ge	0.069																			1985																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																				T		42							T/K		3.06			MHC8031																																																														arc-melt+ANN+Q					High magnetic field transport properties of liquid quenched Nb3Al and Nb3Al(Si,Ge) superconducting compounds			Division of Applied Science, Harvard University, Cambridge, Massachusetts, USA	Appl.Phys. Lett., 47(1985)640	D.Turnbull,F.Habbal,F.Habbal,,G.Clemente,J.Bevk		
108032	LTP0560051		Nb3Al	Al1Nb3	Al	1	Nb	3																					1984																												Cr3Si(A15)			A	5.183													Cr3Si, A15	K		18.6					18.6																													T/K		2.45																																																																	arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108033	SLB0750423		Nb3Al	Al1Nb3	Al	1	Nb	3																					1975																												Cr3Si(A15)																	Cr3Si, A15	K		18.7					18.7																				T		33							T/K		2.56																																																																	arc-melt+ANN									Colloq.Int. CNRS, No.242 (1975)423	S.Foner		
108034	LTP0560051		(Nb,Zr)3Al	Nb2.97Zr0.03Al1	Nb	2.97	Zr	0.03	Al	1																			1984																												Cr3Si(A15)			A	5.187													Cr3Si, A15	K		17.4					17.4																													kG/K		22.4																																																																	arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108035	LTP0560051		(Nb,Zr)3Al	Nb2.91Zr0.09Al1	Nb	2.91	Zr	0.09	Al	1																			1984																												Cr3Si(A15)			A	5.198													Cr3Si, A15	K		14.6					14.6																													kG/K		21.3																																																																	arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108036	LTP0560051		Nb3(Al,Ge)	Nb3Al0.75Ge0.25	Nb	3	Al	0.75	Ge	0.25																			1984																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		19.8					19.8																													kG/K		26.8																																																																	arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108037	LTP0560051		Nb3(Al,Ga)	Nb3Al0.75Ga0.3	Nb	3	Al	0.75	Ga	0.3																			1984																												Cr3Si(A15)			A	5.179													Cr3Si, A15	K		19.1					19.1																													kG/K		25.6																																																																	arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108038	LTP0560051		(Nb,Zr)3Al	Nb2.9925Zr0.0075Al1	Nb	2.9925	Zr	0.0075	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108039	LTP0560051		(Nb,Zr)3Al	Nb2.973Zr0.027Al1	Nb	2.973	Zr	0.027	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		16.6					16.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108040	LTP0560051		(Nb,Zr)3Al	Nb2.927Zr0.073Al1	Nb	2.927	Zr	0.073	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		14.8					14.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108041	LTP0560051		(Nb,Zr)3Al	Nb2.859Zr0.141Al1	Nb	2.859	Zr	0.141	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		13.6					13.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108042	LTP0560051		(Nb,Hf)3Al	Nb2.985Hf0.015Al1	Nb	2.985	Hf	0.015	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108043	LTP0560051		(Nb,Hf)3Al	Nb2.919Hf0.081Al1	Nb	2.919	Hf	0.081	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		16.5					16.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108044	LTP0560051		(Nb,Hf)3Al	Nb2.85Hf0.15Al1	Nb	2.85	Hf	0.15	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		14.4					14.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108045	LTP0560051		(Nb,Ti)3Al	Nb2.976Ti0.024Al1	Nb	2.976	Ti	0.024	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108046	LTP0560051		(Nb,Ti)3Al	Nb2.9175Ti0.0825Al1	Nb	2.9175	Ti	0.0825	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		16					16																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108047	LTP0560051		(Nb,Ti)3Al	Nb2.88Ti0.12Al1	Nb	2.88	Ti	0.12	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		15					15																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108048	LTP0560051		(Nb,Ti)3Al	Nb2.778Ti0.222Al1	Nb	2.778	Ti	0.222	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		13					13																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108049	LTP0560051		(Nb,Ti)3Al	Nb2.73Ti0.27Al1	Nb	2.73	Ti	0.27	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		11.5					11.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108050	LTP0560051		(Nb,Ti)3Al	Nb2.58Ti0.42Al1	Nb	2.58	Ti	0.42	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		9					9																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108051	LTP0560051		(Nb,W)3Al	Nb2.97W0.03Al1	Nb	2.97	W	0.03	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108052	LTP0560051		(Nb,W)3Al	Nb2.94W0.06Al1	Nb	2.94	W	0.06	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.2					17.2																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108053	LTP0560051		(Nb,W)3Al	Nb2.895W0.105Al1	Nb	2.895	W	0.105	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		16					16																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108054	LTP0560051		(Nb,W)3Al	Nb2.85W0.15Al1	Nb	2.85	W	0.15	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		15.2					15.2																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108055	LTP0560051		(Nb,Mo)3Al	Nb2.85Mo0.15Al1	Nb	2.85	Mo	0.15	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		15.5					15.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108056	LTP0560051		(Nb,Mo)3Al	Nb2.775Mo0.225Al1	Nb	2.775	Mo	0.225	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		13.8					13.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108057	LTP0560051		(Nb,Mo)3Al	Nb2.7Mo0.3Al1	Nb	2.7	Mo	0.3	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		12.3					12.3																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108058	LTP0560051		(Nb,Ta)3Al	Nb2.94Ta0.06Al1	Nb	2.94	Ta	0.06	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108059	LTP0560051		(Nb,Ta)3Al	Nb2.85Ta0.15Al1	Nb	2.85	Ta	0.15	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		16.8					16.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108060	LTP0560051		(Nb,Ta)3Al	Nb2.739Ta0.261Al1	Nb	2.739	Ta	0.261	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108061	LTP0560051		(Nb,Ta)3Al	Nb2.64Ta0.36Al1	Nb	2.64	Ta	0.36	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		14.5					14.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108062	LTP0560051		(Nb,V)3Al	Nb2.859V0.141Al1	Nb	2.859	V	0.141	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.2					17.2																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108063	LTP0560051		(Nb,V)3Al	Nb2.706V0.294Al1	Nb	2.706	V	0.294	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		15.6					15.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108064	LTP0560051		(Nb,V)3Al	Nb2.55V0.45Al1	Nb	2.55	V	0.45	Al	1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		14					14																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108065	LTP0560051		Nb3(Al,Se)	Nb3Al0.98Se0.02	Nb	3	Al	0.98	Se	0.02																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108066	LTP0560051		Nb3(Al,Se)	Nb3Al0.967Se0.033	Nb	3	Al	0.967	Se	0.033																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108067	LTP0560051		Nb3(Al,Se)	Nb3Al0.952Se0.048	Nb	3	Al	0.952	Se	0.048																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108068	LTP0560051		Nb3(Al,Se)	Nb3Al0.94Se0.06	Nb	3	Al	0.94	Se	0.06																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108069	LTP0560051		Nb3(Al,Se)	Nb3Al0.924Se0.076	Nb	3	Al	0.924	Se	0.076																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108070	LTP0560051		Nb3(Al,Se)	Nb3Al0.9Se0.1	Nb	3	Al	0.9	Se	0.1																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		17.6					17.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108071	LTP0560051		Nb3(Al,Si)	Nb3Al0.985Si0.015	Nb	3	Al	0.985	Si	0.015																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.6					18.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108072	LTP0560051		Nb3(Al,Si)	Nb3Al0.975Si0.025	Nb	3	Al	0.975	Si	0.025																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108073	LTP0560051		Nb3(Al,Si)	Nb3Al0.964Si0.036	Nb	3	Al	0.964	Si	0.036																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108074	LTP0560051		Nb3(Al,Si)	Nb3Al0.956Si0.044	Nb	3	Al	0.956	Si	0.044																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108075	LTP0560051		Nb3(Al,Si)	Nb3Al0.945Si0.055	Nb	3	Al	0.945	Si	0.055																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108076	LTP0560051		Nb3(Al,Si)	Nb3Al0.935Si0.065	Nb	3	Al	0.935	Si	0.065																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108077	LTP0560051		Nb3(Al,Ga)	Nb3Al0.983Ga0.017	Nb	3	Al	0.983	Ga	0.017																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		18.8					18.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108078	LTP0560051		Nb3(Al,Ga)	Nb3Al0.967Ga0.033	Nb	3	Al	0.967	Ga	0.033																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19					19																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108079	LTP0560051		Nb3(Al,Ga)	Nb3Al0.95Ga0.05	Nb	3	Al	0.95	Ga	0.05																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.2					19.2																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108080	LTP0560051		Nb3(Al,Ga)	Nb3Al0.927Ga0.073	Nb	3	Al	0.927	Ga	0.073																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.2					19.2																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108081	LTP0560051		Nb3(Al,Ga)	Nb3Al0.907Ga0.093	Nb	3	Al	0.907	Ga	0.093																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.1					19.1																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108082	LTP0560051		Nb3(Al,Ge)	Nb3Al0.991Ge0.009	Nb	3	Al	0.991	Ge	0.009																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19					19																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108083	LTP0560051		Nb3(Al,Ge)	Nb3Al0.98Ge0.02	Nb	3	Al	0.98	Ge	0.02																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.3					19.3																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108084	LTP0560051		Nb3(Al,Ge)	Nb3Al0.97Ge0.03	Nb	3	Al	0.97	Ge	0.03																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.6					19.6																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108085	PR05600437	single crystal	TmNi2B2C 	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		10.9					10.9																																																																																																Ni2B flux method.					Electrical resistivity and thermopower of single-crystal RNi2B2C (R=Dy,Ho,er,Tm) magnetic superconductors	199707		Physics Department , Taxas A&M University, College Station, Texas 77843-4242 and Physics Department, University of Hyderabad, Hyderabad 500046, India	Phys.Rev,B56(1997)437-445	A.K. Bhatnagar,D.G. Naugle,K.D.D. Rathnayaka,P.C. Canfield		
108086	LTP0560051		Nb3(Al,Ge)	Nb3Al0.96Ge0.04	Nb	3	Al	0.96	Ge	0.04																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108087	LTP0560051		Nb3(Al,Ge)	Nb3Al0.95Ge0.05	Nb	3	Al	0.95	Ge	0.05																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108088	LTP0560051		Nb3(Al,Ge)	Nb3Al0.94Ge0.06	Nb	3	Al	0.94	Ge	0.06																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108089	LTP0560051		Nb3(Al,Ge)	Nb3Al0.93Ge0.07	Nb	3	Al	0.93	Ge	0.07																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108090	LTP0560051		Nb3(Al,Ge)	Nb3Al0.92Ge0.08	Nb	3	Al	0.92	Ge	0.08																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.9					19.9																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108091	LTP0560051		Nb3(Al,Ge)	Nb3Al0.91Ge0.09	Nb	3	Al	0.91	Ge	0.09																			1984																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+ANN					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
108092	PLA0380323	Hc2(4.2K)=336 kG	Nb-Ga	Ga0.32Nb0.68	Ga	0.32	Nb	0.68																					1972																																														K		20.2					20.2																																																																																																arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108093	PLA0380323		Nb-Ga	Ga0.245Nb0.755	Ga	0.245	Nb	0.755																					1972																																														K		20.2					20.2																				kG		341							kG/K		24.3																																																																	arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108094	PLA0380323	Hc2(4.2K)=199 kG	Nb-Ga	Ga0.3Nb0.7	Ga	0.3	Nb	0.7																					1972																																														K		16.3					16.3																				kG		220							kG/K		19.5																																																																	arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108095	PLA0380323	Hc2(4.2K)=295 kG	Nb-Ga	Ga0.19Nb0.81	Ga	0.19	Nb	0.81																					1972																																														K		13.3					13.3																																																																																																arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108096	PLA0380323	Hc2(4.2K)=310 kG	Nb3(Al,Ga)	Nb3Al0.5Ga0.5	Nb	3	Al	0.5	Ga	0.5																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		19					19																				kG		316							kG/K		24																																																																	arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108097	PLA0380323	Hc2(4.2K)=295 kG	Nb3Al	Al1Nb3	Al	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		18.6					18.6																				kG		330							kG/K		25.6																																																																	arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108098	PLA0380323	Hc2(4.2K)=410 kG	Nb3(Al,Ga)	Nb0.79Al0.164Ga0.057	Nb	0.79	Al	0.164	Ga	0.057																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		20.7					20.7																				kG		439							kG/K		30.6																																																																	arc-melt+ANN					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
108099	JPS0350108		Nb3(Al,B)	Nb3Al0.9B0.1	Nb	3	Al	0.9	B	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108100	JPS0350108		Nb3(Al,B)	Nb3Al0.8B0.2	Nb	3	Al	0.8	B	0.2																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108101	JPS0350108		Nb3(Al,B)	Al1Nb3	Al	1	Nb	3																					1973																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108102	JPS0350108		Nb3(Al,Be)	Nb3Al0.95Be0.05	Nb	3	Al	0.95	Be	0.05																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108103	JPS0350108		Nb3(Al,Be)	Nb3Al0.9Be0.1	Nb	3	Al	0.9	Be	0.1																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108104	JPS0350108		Nb3(Al,Be)	Nb3Al0.8Be0.2	Nb	3	Al	0.8	Be	0.2																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		17					17																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108105	JPS0350108		Nb3(Al,Be)	Nb3Al0.7Be0.3	Nb	3	Al	0.7	Be	0.3																			1973																												Cr3Si(A15)																	Cr3Si, A15	K		14					14																																																																																																arc-melt+WQ+ANN					Superconductivity near 20K in Ternary and Quaternary Alloys Based upon Nb3Al			Central Research Laboratory, Hitachi,Ltd.,Kokubunji,Tokyo	J.Phys.Soc.Jpn, 35(1973)108	Mitsuhiro Kudo,Shigeo Fukase,Ushio Kawabe		
108106	PHC3070245	delta-C/gamma*Tc = 1.06. G-L parameter = 44.85	Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1998																												CuAl2																	CuAl2, C16	K		11.2					11.2											Oe		254							T		7														A		28.24			A		1266.72													mj/mol.K2	68		214																																					arc-melting					Superconducting state parameters of C-16 structured Zr2Rh	199810		Technical Physics and Prototype Engineering Division, Bhabha Atomic Research Centre, Bombay 400 085, india	Physica.C,307(1998)245-253	A. Sathyamoorthy,H.G. Salunke,K. Shashikala,P. Raj,S. Ramakrishnan,S.K. Dhar,V.C. Sahni		
108107	PHC3070245		Zr2RhHx	Zr2Rh1H0.08	Zr	2	Rh	1	H	0.08																			1998																												CuAl2																	CuAl2, C16	K		11.1					11.1																																																																																																heating Zr2RhH2 in vac					Superconducting state parameters of C-16 structured Zr2Rh	199810		Technical Physics and Prototype Engineering Division, Bhabha Atomic Research Centre, Bombay 400 085, india	Physica.C,307(1998)245-253	A. Sathyamoorthy,H.G. Salunke,K. Shashikala,P. Raj,S. Ramakrishnan,S.K. Dhar,V.C. Sahni		
108108	PHC3070245		Zr2RhHx	Zr2Rh1H0.1	Zr	2	Rh	1	H	0.1																			1998																												CuAl2																	CuAl2, C16	K		10.8					10.8																																																																																																heating Zr2RhH2 in vac					Superconducting state parameters of C-16 structured Zr2Rh	199810		Technical Physics and Prototype Engineering Division, Bhabha Atomic Research Centre, Bombay 400 085, india	Physica.C,307(1998)245-253	A. Sathyamoorthy,H.G. Salunke,K. Shashikala,P. Raj,S. Ramakrishnan,S.K. Dhar,V.C. Sahni		
108109	PHC3070245		Zr2RhHx	Zr2Rh1H0.28	Zr	2	Rh	1	H	0.28																			1998																												CuAl2																	CuAl2, C16	K		8.8					8.8																																																																																																heating Zr2RhH2 in vac					Superconducting state parameters of C-16 structured Zr2Rh	199810		Technical Physics and Prototype Engineering Division, Bhabha Atomic Research Centre, Bombay 400 085, india	Physica.C,307(1998)245-253	A. Sathyamoorthy,H.G. Salunke,K. Shashikala,P. Raj,S. Ramakrishnan,S.K. Dhar,V.C. Sahni		
108110	PHC3070245		Zr2RhHx	Zr2Rh1H0.7	Zr	2	Rh	1	H	0.7																			1998																												CuAl2																	CuAl2, C16	K		6					6																																																																																																heating Zr2RhH2 in vac					Superconducting state parameters of C-16 structured Zr2Rh	199810		Technical Physics and Prototype Engineering Division, Bhabha Atomic Research Centre, Bombay 400 085, india	Physica.C,307(1998)245-253	A. Sathyamoorthy,H.G. Salunke,K. Shashikala,P. Raj,S. Ramakrishnan,S.K. Dhar,V.C. Sahni		
108111	PHC3070079	2*delta/k:Tc = 4.0 +-0.5. Energy gap by Raman spectroscopy.	Rb3C60	C60Rb3	C	60	Rb	3																					1998																												fullerene																		K		31					31																																																4																																																By annealing sublimation grown C60 single crystal					Determination of the superconducting energy gap of Rb3C60 by electronic Raman scattering	199810		2. Physikalisches Institut, RWTH-Aachen, 52056, Aachen, Germany	Physica.C,307(1998)79-86	G. Els,G. Guntherodt,H.-J. Guntherodt,H.P. Lang,P. Lemmens,P.H.M. van Loosdrecht,V. Thommen-Geiser		
108112	PSS0770759			Nb0.75Al0.19Ge0.06	Nb	0.75	Al	0.19	Ge	0.06																			1983																												Cr3Si(A15)			A	5.182													Cr3Si, A15	K		20.9					20.9																													T/K		3.1																																																																	sintering + ANN					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
108113	PR06006668	not s/c	U(Pt,Pd)3	U1Pt2.97Pd0.03	U	1	Pt	2.97	Pd	0.03																			1999								1.6																																						K																																																																																																												Neutron-diffraction study of the evolution of antiferromagnetic order in UPt3 doped with Pd	199909		Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B,60(1999)6668-6677	A. A. Menovsky,A. de Visser,B. Fak,J. J. M. Franse,J.-M. Mignot,R. J. Keizer		
108114	PR06006668	not s/c	U(Pt,Pd)3	U1Pt2.94Pd0.06	U	1	Pt	2.94	Pd	0.06																			1999								3.4																																						K																																																																																																												Neutron-diffraction study of the evolution of antiferromagnetic order in UPt3 doped with Pd	199909		Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B,60(1999)6668-6677	A. A. Menovsky,A. de Visser,B. Fak,J. J. M. Franse,J.-M. Mignot,R. J. Keizer		
108115	PR06006668	not s/c	U(Pt,Pd)3	U1Pt2.85Pd0.15	U	1	Pt	2.85	Pd	0.15																			1999								5.8																																						K																																																																																																												Neutron-diffraction study of the evolution of antiferromagnetic order in UPt3 doped with Pd	199909		Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B,60(1999)6668-6677	A. A. Menovsky,A. de Visser,B. Fak,J. J. M. Franse,J.-M. Mignot,R. J. Keizer		
108116	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	Be13U1	Be	13	U	1																					1998																																														K		0.941					0.941																																																								mj/mol.K2	995																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108117	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.99Th0.01Be13	U	0.99	Th	0.01	Be	13																			1998																															A	10.2564														K		0.624					0.624																																																								mj/mol.K2	1630																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108118	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.983Th0.017Be13	U	0.983	Th	0.017	Be	13																			1998																															A	10.2573														K		0.525					0.525																																																								mj/mol.K2	1700																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108119	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.9822Th0.0178Be13	U	0.9822	Th	0.0178	Be	13																			1998																															A	10.2574														K		0.519					0.519																																																								mj/mol.K2	2060																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108120	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.9815Th0.0185Be13	U	0.9815	Th	0.0185	Be	13																			1998																															A	10.2576														K		0.519					0.519																																																								mj/mol.K2	2000																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108121	PR05815153	second Tc=0.425. gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.978Th0.022Be13	U	0.978	Th	0.022	Be	13																			1998																															A	10.2584														K		0.558					0.558																																																								mj/mol.K2	2610																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108122	PR05815153	second Tc=0.353. gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.97Th0.03Be13	U	0.97	Th	0.03	Be	13																			1998																															A	10.2588														K		0.585					0.585																																																								mj/mol.K2	2615																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108123	PR05815153	second Tc=0.396. gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.962Th0.038Be13	U	0.962	Th	0.038	Be	13																			1998																															A	10.2607														K		0.532					0.532																																																								mj/mol.K2	2820																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108124	PR05815153	second Tc=0.465. gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.957Th0.043Be13	U	0.957	Th	0.043	Be	13																			1998																															A	10.261														K		0.533					0.533																																																								mj/mol.K2	2230																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108125	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.9545Th0.0455Be13	U	0.9545	Th	0.0455	Be	13																			1998																															A	10.2618														K		0.46					0.46																																																								mj/mol.K2	2535																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108126	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.9535Th0.0465Be13	U	0.9535	Th	0.0465	Be	13																			1998																															A	10.262														K		0.415					0.415																																																								mj/mol.K2	2415																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108127	PR05815153	gamma in mj/mol.K2. Tc by specific heat	(U,Th)Be13	U0.948Th0.052Be13	U	0.948	Th	0.052	Be	13																			1998																															A	10.2626														K		0.38					0.38																																																								mj/mol.K2	1935																																							arc-melting					Specific heat study in U1-xThxBe13: Enormous delta C and strong coupling at x = xc1 and			Institut fue Physik, Universitat Augsburg, Universitatsstrasse 1, 86159 Augsburg, Germany	Phys.Rev.B,58(1998)15153-15159	E.-W. Scheidt,G. R. Stewart,P. Kumar,T. Schreiner		
108128	PR06003056	single crystal	U(Pt,Pd)3	Pt3U1	Pt	3	U	1																				3	1999																																														K		0.547					0.547																																																																																																Czochralski method					Suppression of superconductivity in single crystals of UPt3 by Pd substitution	199908		Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467	Phys.Rev.B,60(1999)3056-3059	A. A. Menovsky,A. de Visser,J. J. M. Franse,M. J. Graf,R. J. Keizer		
108129	PR06003056	single crystal	U(Pt,Pd)3	U1Pt2.997Pd0.003	U	1	Pt	2.997	Pd	0.003																		3	1999																																														K		0.447					0.447																																																																																																Czochralski method					Suppression of superconductivity in single crystals of UPt3 by Pd substitution	199908		Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467	Phys.Rev.B,60(1999)3056-3059	A. A. Menovsky,A. de Visser,J. J. M. Franse,M. J. Graf,R. J. Keizer		
108130	PR06003056	single crystal	U(Pt,Pd)3	U1Pt2.994Pd0.006	U	1	Pt	2.994	Pd	0.006																		3	1999																																														K		0.4					0.4																																																																																																Czochralski method					Suppression of superconductivity in single crystals of UPt3 by Pd substitution	199908		Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467	Phys.Rev.B,60(1999)3056-3059	A. A. Menovsky,A. de Visser,J. J. M. Franse,M. J. Graf,R. J. Keizer		
108131	PHB2590666	poly crystal, heavy Fermion	U(Pt,Pd)3	Pt3U1	Pt	3	U	1																					1999																																														K		0.57					0.57																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
108132	PHB2590666	poly crystal, heavy Fermion	U(Pt,Pd)3	U1Pt2.991Pd0.009	U	1	Pt	2.991	Pd	0.009																			1999																																														K		0.35					0.35																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
108133	PHB2590666	poly crystal, heavy Fermion	U(Pt,Pd)3	U1Pt2.988Pd0.012	U	1	Pt	2.988	Pd	0.012																			1999																																														K		0.24					0.24																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
108134	PHC2260385	gamma in mj/mol.K2. E-ph coupling = 0.38	Zr2Fe	Fe1Zr2	Fe	1	Zr	2																					1994																												CuAl2			A	6.385		5.593											CuAl2, C16	K		0.17					0.17																																																								mj/mol.K2	16.5		248																																										Band filling and superconductivity in Zr2M compounds	199406			Physica C, 226(1994)385-390	G.P.Das,H.G.Salunke,P.Raj,S.K.Dhar,V.C.Sahni	Zr,Fe,Co,Ni,Rh	
108135	PHC2260385	gamma in mj/mol.K2. E-ph coupling = 0.72	Zr2Co	Co1Zr2	Co	1	Zr	2																					1994																												CuAl2			A	6.364		5.524											CuAl2, C16	K		5.2					5.2																																																								mj/mol.K2	23.7		256																																										Band filling and superconductivity in Zr2M compounds	199406			Physica C, 226(1994)385-390	G.P.Das,H.G.Salunke,P.Raj,S.K.Dhar,V.C.Sahni	Zr,Fe,Co,Ni,Rh	
108136	PHC2260385	gamma in mj/mol.K2. E-ph coupling = 0.49	Zr2Ni	Ni1Zr2	Ni	1	Zr	2																					1994																												CuAl2			A	6.263		5.263											CuAl2, C16	K		2					2																																																								mj/mol.K2	20.1		252																																										Band filling and superconductivity in Zr2M compounds	199406			Physica C, 226(1994)385-390	G.P.Das,H.G.Salunke,P.Raj,S.K.Dhar,V.C.Sahni	Zr,Fe,Co,Ni,Rh	
108137	PHC2260385	gamma in mj/mol.K2. E-ph coupling = 1.13	Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1994																												CuAl2			A	6.629		5.629											CuAl2, C16	K		11.2					11.2																																																								mj/mol.K2	68		214																																										Band filling and superconductivity in Zr2M compounds	199406			Physica C, 226(1994)385-390	G.P.Das,H.G.Salunke,P.Raj,S.K.Dhar,V.C.Sahni	Zr,Fe,Co,Ni,Rh	
108138	PR05800497	gamma in mj/mol.K2 by fitting for 1.5<T<5.5K.  Gap estimated from specific heat.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																			1998																												CeNiC2																		K		2.7					2.7																																																4.62								mj/mol.K2	6.5		388																																					arc-melting					Low-temperature behavior of two ternary lanthanide nickel carbides: Superconducting LaNiC2			Ames Laboratory, Iowa State University, Ames, Iowa 50011-3020	Phys.Rev.B,58(1998)497-502	K. A. Gschneidner, Jr.,L. L. Miller,V. K. Pecharsky		
108139	PR05800497	not s/c. Low temperature phase = ferro- or ferri-magnet.	CeNiC2	Ce1Ni1C2	Ce	1	Ni	1	C	2																			1998								2.4																				CeNiC2																		K					1.5																																																																																																		arc-melting					Low-temperature behavior of two ternary lanthanide nickel carbides: Superconducting LaNiC2			Ames Laboratory, Iowa State University, Ames, Iowa 50011-3020	Phys.Rev.B,58(1998)497-502	K. A. Gschneidner, Jr.,L. L. Miller,V. K. Pecharsky		
108140	SSC1110153	single crystal, RRR=130. Hc2(0) estimated from dHc2/dT using WHH theory.	LaNiSn	La1Ni1Sn1	La	1	Ni	1	Sn	1																		3	1999																																														K		0.59					0.59																				mT		22							mT/K		60					A		1200																																																										Chochralsky method					Superconductivity and magnetoresistance in a single-crystal LaNiSn	199906		Department of Quantum Matter, ADSM, Hiroshima University, Kagamiyama 1-3-1, Higashi-Hiroshima 739-8526, Japan	Solid State Commun.,111(1999)153-157	K. Umeo,T. Takabatake,Y. Echizen		
108141	PR05206784	feroo-magnet. Tm=14.4K.	SmPtSi	Sm1Pt1Si1	Sm	1	Pt	1	Si	1																		1	1995							14.4																					alpha-ThSi2			A	4.1232		14.3742												K																																																																		235																																					arc-melting + ANN(700C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108142	PR05206784	Values of s/c properties were estimated from specific heat and resistivity measurements. E-ph coupling const.= 0.56	LaPtSi	La1Pt1Si1	La	1	Pt	1	Si	1																		1	1995																												alpha-ThSi2			A	4.2494		14.5388												K		3.9					3.9											Oe		117							Oe		2180							T/K		0.75					A		338			A		1425													mj/mol.K2	3.56		250																																					arc-melting + ANN(700C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108143	PR05206784		CePtSi	Ce1Pt1Si1	Ce	1	Pt	1	Si	1																		1	1995							-3.9																					alpha-ThSi2			A	4.1979		14.4884												K																																																																																																							arc-melting + ANN(700C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108144	PR05206784		NdPtSi	Nd1Pt1Si1	Nd	1	Pt	1	Si	1																		1	1995								3.8																				alpha-ThSi2			A	4.1628		14.4152												K																																																																		225																																					arc-melting + ANN(700C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108145	PR05206784		(La,Nd)PtSi	La0.99Nd0.01Pt1Si1	La	0.99	Nd	0.01	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		3.71					3.71																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108146	PR05206784		(La,Nd)PtSi	La0.98Nd0.02Pt1Si1	La	0.98	Nd	0.02	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		3.42					3.42																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108147	PR05206784		(La,Nd)PtSi	La0.97Nd0.03Pt1Si1	La	0.97	Nd	0.03	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		3.27					3.27																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108148	PR05206784		(La,Nd)PtSi	La0.96Nd0.04Pt1Si1	La	0.96	Nd	0.04	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		3.04					3.04																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108149	PR05206784		(La,Nd)PtSi	La0.95Nd0.05Pt1Si1	La	0.95	Nd	0.05	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		2.76					2.76																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108150	PR05206784		(La,Nd)PtSi	La0.94Nd0.06Pt1Si1	La	0.94	Nd	0.06	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		2.56					2.56																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108151	PR05206784		(La,Nd)PtSi	La0.93Nd0.07Pt1Si1	La	0.93	Nd	0.07	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		2.29					2.29																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108152	PR05206784		(La,Nd)PtSi	La0.92Nd0.08Pt1Si1	La	0.92	Nd	0.08	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		2.04					2.04																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108153	PR05206784		(La,Nd)PtSi	La0.91Nd0.09Pt1Si1	La	0.91	Nd	0.09	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		1.73					1.73																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108154	PR05206784		(La,Nd)PtSi	La0.9Nd0.1Pt1Si1	La	0.9	Nd	0.1	Pt	1	Si	1																1	1995																												alpha-ThSi2																		K		1.42					1.42																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108155	PR05206784		(La,Ce)PtSi	La0.9997Ce0.0003Pt1Si1	La	0.9997	Ce	0.0003	Pt	1	Si	1																	1995																												alpha-ThSi2																		K		3.2					3.2																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108156	PR05206784		(La,Ce)PtSi	La0.9991Ce0.0009Pt1Si1	La	0.9991	Ce	0.0009	Pt	1	Si	1																	1995																												alpha-ThSi2																		K		2.03					2.03																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108157	PR05206784		(La,Ce)PtSi	La0.9989Ce0.0011Pt1Si1	La	0.9989	Ce	0.0011	Pt	1	Si	1																	1995																												alpha-ThSi2																		K		1.5					1.5																																																																																																arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108158	PR05206784	not s/c	(La,Ce)PtSi	La0.998Ce0.002Pt1Si1	La	0.998	Ce	0.002	Pt	1	Si	1																	1995																												alpha-ThSi2																		K					0.6																																																																																																		arc-melting + ANN(850C)					Magnetism and superconductivity in  RPtSi (R=La, Ce, Nd, and Sm)	199509			Phys.Rev.B.52(1995)6784	Arvind D. Chinchure,Girish  Chandra,K. Ghosh,S. Ramakrishnan,V.R. Marathe	La, Ce, Nd, Sm, Pt, Si	
108159	PSS1770475		alpha-(C,W)Si:H	C0.78W0.22Si1	C	0.78	W	0.22	Si	1																		4	1993																												diamond																	diamond	K		2.9					2.9	MTC8160																																																																																															sputtering					Electron Transport and Superconductivity in Transition Metal-Containing Diamond-Like Films			Department of Physics, Moscow State University	Physica Stat.Solidi B,177(1993)475	A.Briggs,A.D.Bozhko,B.N.Pypkin,D.Yu.Rodichev,M.Berrettoni,S.M.Chudinov,S.Stizza		
108160	PSS1770475		alpha-(C,W)Si:H	C0.74W0.26Si1	C	0.74	W	0.26	Si	1																		4	1993																												diamond																	diamond	K		3.3					3.3	MTC8160																																																																																															sputtering					Electron Transport and Superconductivity in Transition Metal-Containing Diamond-Like Films			Department of Physics, Moscow State University	Physica Stat.Solidi B,177(1993)475	A.Briggs,A.D.Bozhko,B.N.Pypkin,D.Yu.Rodichev,M.Berrettoni,S.M.Chudinov,S.Stizza		
108161	PSS1770475		alpha-(C,W)Si:H	C0.72W0.28Si1	C	0.72	W	0.28	Si	1																		4	1993																												diamond																	diamond	K		3.9					3.9	MTC8160																																																																																															sputtering					Electron Transport and Superconductivity in Transition Metal-Containing Diamond-Like Films			Department of Physics, Moscow State University	Physica Stat.Solidi B,177(1993)475	A.Briggs,A.D.Bozhko,B.N.Pypkin,D.Yu.Rodichev,M.Berrettoni,S.M.Chudinov,S.Stizza		
108162	PR06208695	RRR=22.2. Resistivity(T=Tc)=2.25 micro-Ohm.cm	Ti1-xAlx	Ti1	Ti	1																						1	2000																																													hcp	K		0.49					0.49																				kG		0.46							kG/K		1.3																																																																	arc-melting +ANN(900C,1week)					Upper critical field of Ti and alpha -TiAl alloys: Evidence of an intrinsic type-II superconductivity in pure Ti	200010		Institute of Physics & Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,62(2000)8695-8698	J. J. Lin,Jing Xiunian,Kang Ning,Li Shanlin,Liu Shumei,Lu Li,Wu Xiaosong,Zhang Dianlin		
108163	PR06208695	RRR=2.1. Resistivity(T=Tc)=40 micro-Ohm.cm	Ti1-xAlx	Al0.029Ti0.971	Al	0.029	Ti	0.971																				1	2000																																													hcp	K		0.65					0.65																				kG		3.05							kG/K		6.9																																																																	arc-melting +ANN(900C,1week)					Upper critical field of Ti and alpha -TiAl alloys: Evidence of an intrinsic type-II superconductivity in pure Ti	200010		Institute of Physics & Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,62(2000)8695-8698	J. J. Lin,Jing Xiunian,Kang Ning,Li Shanlin,Liu Shumei,Lu Li,Wu Xiaosong,Zhang Dianlin		
108164	PR06208695	RRR=1.6. Resistivity(T=Tc)=68 micro-Ohm.cm	Ti1-xAlx	Al0.053Ti0.947	Al	0.053	Ti	0.947																				1	2000																																													hcp	K		0.7					0.7																				kG		5							kG/K		11.3																																																																	arc-melting +ANN(900C,1week)					Upper critical field of Ti and alpha -TiAl alloys: Evidence of an intrinsic type-II superconductivity in pure Ti	200010		Institute of Physics & Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,62(2000)8695-8698	J. J. Lin,Jing Xiunian,Kang Ning,Li Shanlin,Liu Shumei,Lu Li,Wu Xiaosong,Zhang Dianlin		
108165	PR06208695	RRR=1.2. Resistivity(T=Tc)=113 micro-Ohm.cm	Ti1-xAlx	Al0.102Ti0.898	Al	0.102	Ti	0.898																				1	2000																																													hcp	K		0.73					0.73																				kG		7.28							kG/K		16																																																																	arc-melting +ANN(900C,1week)					Upper critical field of Ti and alpha -TiAl alloys: Evidence of an intrinsic type-II superconductivity in pure Ti	200010		Institute of Physics & Center for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Phys.Rev.B,62(2000)8695-8698	J. J. Lin,Jing Xiunian,Kang Ning,Li Shanlin,Liu Shumei,Lu Li,Wu Xiaosong,Zhang Dianlin		
108166	JSP0692708	gap (delta)=1.8 meV	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	2000																												LuNi2B2C																		K		11			6		11																																																3.8																																																arc-melting +ANN(1050C, 1week)					Electron Tunneling Measurements of Antiferromagnetic Superconductor ErNi2B2C	200008		Department of Applied Chemistry, University of Tokyo,  Tokyo 113-8656	J.Phys.Soc.Japan,69(2000)2708-2709	K. Kitazawa,L. C. Gupta,R. Nagarajan,T. Hasegawa,T. Watanabe,Z. Hossain		
108167	PR06214350	average grain size=1 micron meter. Packing fraction=0.67. Intra-granular s/c	Pt	Pt1	Pt	1																							2000																																														K		0.0019					0.0019																																																																																																					Inter- and intragranular effects in superconducting compacted platinum powders	200012		Physikalisches Institut, Universitat Bayreuth, D-95440 Bayreuth, Germany	Phys.Rev.B,62(2000)14350-14358	Alexander Schindler,Hans F. Braun,Reinhard Konig,Thomas Herrmannsdorfer		
108168	PR06214350	average grain size=1 micron meter. Packing fraction=0.67. Inter-granular s/c	Pt	Pt1	Pt	1																							2000																																														K		0.00104					0.00104																																																																																																					Inter- and intragranular effects in superconducting compacted platinum powders	200012		Physikalisches Institut, Universitat Bayreuth, D-95440 Bayreuth, Germany	Phys.Rev.B,62(2000)14350-14358	Alexander Schindler,Hans F. Braun,Reinhard Konig,Thomas Herrmannsdorfer		
108169	PR06213919	p-cohere=120A, n-cohere=100.  Aeffective mass=180	UPt3	Pt3U1	Pt	3	U	1																					2000																																														K		0.55					0.55																																				A		120																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108170	PR06213919	Aeffective mass=260	UBe13	Be13U1	Be	13	U	1																					2000																																														K		0.9					0.9																																				A		100																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108171	PR06213919	Aeffective mass=48	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																			2000																																														K		1					1																																				A		240																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108172	PR06213919	Aeffective mass=66	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			2000																																														K		2					2																																				A		85																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108173	PR06213919	p-cohere=150A, n-cohere=100.  Aeffective mass=140	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																			2000																																														K		1.2					1.2																																				A		150																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108174	PR06213919	Aeffective mass=380	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																			2000																																														K		0.7					0.7																																				A		90																																																										See Comments Condens.Mater Phys,.17(1996)361					Tc for non-s-wave pairing superconductors correlated with coherence length and effective mass	200012		Dipartimento di Fisica e Astronomia, Universita degli Studi di Catania, and Istituto Nazionale per la Fisica della Materia, Sezione di Catania, Corso Italia, 57, I-95129 Catania, Italy	Phys.Rev.B,62(2000)13919-13921	G. G. N. Angilella,N. H. March,R. Pucci		
108175	PR06214469	structure / alpha=99.99	Y2C2Br2	Y2C2Br2	Y	2	C	2	Br	2																			2000																															A	6.954	3.765	9.931												K		5.05					5.05																																									A		5530																																																					1300C in Ta crucible					Transverse-field muon spin relaxation investigations of the magnetic penetration depth in the carbide superconductors Y2C2(Br,I)2 and YC2	200012		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrae 1, D-70569 Stuttgart, Germany	Phys.Rev.B,62(2000)14469-14475	A. Simon,C. Bernhard,Ch. Niedermayer,R. K. Kremer,R. W. Henn,Th. Blasius,Th. Gulden		
108176	PR06214469	structure / alpha=93.90	Y2C2(Br,I)2	Y2C2Br0.5I1.5	Y	2	C	2	Br	0.5	I	1.5																	2000																															A	7.153	3.852	10.384												K		11.6					11.6																																									A		6980																																																					1300C in Ta crucible					Transverse-field muon spin relaxation investigations of the magnetic penetration depth in the carbide superconductors Y2C2(Br,I)2 and YC2	200012		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrae 1, D-70569 Stuttgart, Germany	Phys.Rev.B,62(2000)14469-14475	A. Simon,C. Bernhard,Ch. Niedermayer,R. K. Kremer,R. W. Henn,Th. Blasius,Th. Gulden		
108177	PR06214469	structure / alpha=93.68	Y2C2I2	Y2C2I2	Y	2	C	2	I	2																			2000																															A	7.217	2.883	10.437												K		9.97					9.97																																									A		3170																																																					1300C in Ta crucible					Transverse-field muon spin relaxation investigations of the magnetic penetration depth in the carbide superconductors Y2C2(Br,I)2 and YC2	200012		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrae 1, D-70569 Stuttgart, Germany	Phys.Rev.B,62(2000)14469-14475	A. Simon,C. Bernhard,Ch. Niedermayer,R. K. Kremer,R. W. Henn,Th. Blasius,Th. Gulden		
108178	PR06214469	non-stoichiometry  YC2-z	YC2-z	C2Y1	C	2	Y	1																					2000																															A	3.6637		6.1732												K		3.85					3.85																																									A		8100																																																					1300C in Ta crucible					Transverse-field muon spin relaxation investigations of the magnetic penetration depth in the carbide superconductors Y2C2(Br,I)2 and YC2	200012		Max-Planck-Institut fur Festkorperforschung, Heisenbergstrae 1, D-70569 Stuttgart, Germany	Phys.Rev.B,62(2000)14469-14475	A. Simon,C. Bernhard,Ch. Niedermayer,R. K. Kremer,R. W. Henn,Th. Blasius,Th. Gulden		
108179	JPS0690868	RRR=69. Gamma in mj/mol.K2. Delta-C/gamma*Tc = 2.22	LaRu4Sb12	La1Ru4Sb12	La	1	Ru	4	Sb	12																			2000																															A	9.274													bcc	K		3.58					3.58																				kOe		3							kOe/K		1.2																									mj/mol.K2	37		253																																					Sb-flux method					Superconducting and Magnetic Properties of Filled Skutterudite Compounds RERu4Sb12 (RE=La, Ce, Pr, Nd and Eu)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.jpn , 69(2000)868-873	Masayasu Ishikawa,Naoya Takeda		
108180	JPS0690868		CeRu4Sb12	Ce1Ru4Sb12	Ce	1	Ru	4	Sb	12																			2000								1																							A	9.273													bcc	K					1																																																																																																		Sb-flux method					Superconducting and Magnetic Properties of Filled Skutterudite Compounds RERu4Sb12 (RE=La, Ce, Pr, Nd and Eu)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.jpn , 69(2000)868-873	Masayasu Ishikawa,Naoya Takeda		
108181	JPS0690868	RRR=25. Gamma in mj/mol.K2. Delta-C/gamma*Tc = 1.87	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																			2000							-11																								A	9.269													bcc	K		1.04					1.04																				kOe		2							kOe/K		2.4																									mj/mol.K2	59		232																																					Sb-flux method					Superconducting and Magnetic Properties of Filled Skutterudite Compounds RERu4Sb12 (RE=La, Ce, Pr, Nd and Eu)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.jpn , 69(2000)868-873	Masayasu Ishikawa,Naoya Takeda		
108182	JPS0690868		NdRu4Sb12	Nd1Ru4Sb12	Nd	1	Ru	4	Sb	12																			2000							-28	1																							A	9.261													bcc	K					1																																																																																																		Sb-flux method					Superconducting and Magnetic Properties of Filled Skutterudite Compounds RERu4Sb12 (RE=La, Ce, Pr, Nd and Eu)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.jpn , 69(2000)868-873	Masayasu Ishikawa,Naoya Takeda		
108183	JPS0690868		EuRu4Sb12	Eu1Ru4Sb12	Eu	1	Ru	4	Sb	12																			2000								1																							A	9.291													bcc	K					1																																																																																																		Sb-flux method					Superconducting and Magnetic Properties of Filled Skutterudite Compounds RERu4Sb12 (RE=La, Ce, Pr, Nd and Eu)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.jpn , 69(2000)868-873	Masayasu Ishikawa,Naoya Takeda		
108184	JPS0693017	s/c properties for single crystal are also shown. Gamma in mj/mol.K2. RRR=18. Thermodynamic Hc(0) = 0.442 kOe. G-L parameter = 7.1	NiBi3	Bi3Ni1	Bi	3	Ni	1																					2000																												NiBi3																		K		4.1					4.1											Oe		86							kOe		4.45							kOe/K		1.58					A		263			A		1940													mj/mol.K2	12.7		144																																										Superconducting and Normal State Properties of NiBi3			Department of Physics, Faculty of Science, Graduate School of Kyushu University, Ropponmatu, Fukuoka 810-8560	J.Phys.Soc.jpn , 69(2000)3017-3026	Bunjyu Shinozaki,Shin-ichi Kan,Takasi Kawaguti,Yasunobu Fujimori		
108185	PSC0570211	metal. Resistivity(300K)=1.6 mOhm.cm	NiP3	Ni1P3	Ni	1	P	3																				1	1996																															A	7.8192														K					1.8																																																																																																		high pressure synthesis (4GPa, 100-1200C)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108186	PSC0570211	semiconductor	CeRu4P12	Ce1Ru4P12	Ce	1	Ru	4	P	12																		1	1996																															A	8.0376														K					1.8																																																																																																		high pressure synthesis (4GPa, 100-1200C)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108187	PSC0570211	semiconductor	CoP3	Co1P3	Co	1	P	3																				1	1996																															A	7.7073														K					1.8																																																																																																		high pressure synthesis (4GPa, 100-1200C)					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108188	PSC0570211	not s/c	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																			1996																												skutterudite			A	7.832														K																																																																																																												Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108189	PSC0570211		LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																			1996																												skutterudite			A	8.0561														K		7					7																				T		3.65												MHC8189		A		95																																																															Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108190	PSC0570211	not s/c	LaOs4P12	La1Os4P12	La	1	Os	4	P	12																			1996																												skutterudite			A	8.0844														K					2																																																																																																							Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108191	PSC0570211		La(Ru,Os)4P12	La1Ru3Os1P12	La	1	Ru	3	Os	1	P	12																	1996																															A	8.065														K		7					7																																																																																																					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108192	PSC0570211		La(Ru,Os)4P12	La1Ru2Os2P12	La	1	Ru	2	Os	2	P	12																	1996																															A	8.077														K		7					7																																																																																																					Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
108193	PSC0570211	density=8.151 g/cm3	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1996																																														K		13					13																				T		17.5														A		43.4																																																															Electrical conductivity and superconductivity of metal phosphides with skutterudite-type structure prepared at high pressure			Muroran Institute of Technology, 27-1, Mizumoto, Muroran-shi 050,Japan	J.Phys.Chem.Solids, 57(1996)211-216	Ichimin Shirotani,Kenji Tachi,Kiyokazu Nozawa,Minoru Kinoshita,Sakae Todo,Takafumi Adachi,Takehiko Yagi		
109000	LB80MAT1	<93>Nb NQR measured.		Nb0.75Al0.225Ga0.025	Nb	0.75	Al	0.225	Ga	0.025																			1980																												Cr3Si(A15)																	Cr3Si, A15	K		19.1					19.1																																																																																																arc-melt + ANN									Fiz. Met. Metallovd, 50(1980)526	I.A.Safin,V.F.Shamrai,V.L.Matukhin		
109001	LB82LEV1	Tc shows the maximum value. SEM, EDX		Nb0.75Al0.16Ga0.09	Nb	0.75	Al	0.16	Ga	0.09																			1982																												Cr3Si(A15)			A	5.188													Cr3Si, A15	K		19.45					19.45																																																																																																film 0n Nb, evaporation									Phys.Met.,4(1982)719	G.P.Motulevich,I.S.Levchenko,N.V.Anshukova,S.P.Merkulova		
109002	LTP0560051			Nb0.75Al0.175Ga0.075	Nb	0.75	Al	0.175	Ga	0.075																			1984																												Cr3Si(A15)			A	5.179													Cr3Si, A15	K		19.1					19.1																													T/K		2.56																																																																	arc-melt +ANN(1923K) +ANN(973K					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
109003	MSE0990195	This Tc value was obtained on splat cooled samples of 0.15 mm thickness.		Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1988																												Cr3Si(A15)																	Cr3Si, A15	K		16.5					16.5																																																																																																melt +splat cool					Dependence of Tc on the Cooling Conditions for Liquid-quenched A15 Chemical Compounds			Department of Materials Science, Tokai University, Hiratsuka, Japan	Mater.Sci.Eng., 99(1988)195	A.Hara,E.Yajima,H.Harano,M.Kawakami,N.Ninomiya,S.Tokunaga,Y.Nishi,Y.Tachiya		
109004	SSC0580277	EXAFS		Nb0.75Al0.185Ge0.065	Nb	0.75	Al	0.185	Ge	0.065																			1986																												Cr3Si(A15)			A	5.173													Cr3Si, A15	K		20.26					20.26																																																																																																not given					Extended X-ray Absorption Fine Structure Investigations of Nb3Ge0.26Al0.74			Department of Physics, State University of New York at Stony Brook, Stony Brook, NY 11794, USA	Solid State Commun.,58(1986)277	A.I.Goldman,E.Canova,Y.H.Kao		
109005	JPF0161299	Raman		Nb0.75Al0.1875Ge0.0625	Nb	0.75	Al	0.1875	Ge	0.0625																			1986																																														K		20					20																																																																																																arc-melt +ANN(973K)									J.Phys.F:Met.Phys., 16(1986)1299	A.Muller,R.Hackl,R.Kaiser,W.Weber		
109006	APL0490046	The reactin to A15 took place during the electron beam irradiation(20kV, 5-30mA). Jc(4.2K)=1E+4 A/cm2 at 25T.		Nb0.75Al0.02Ge0.05	Nb	0.75	Al	0.02	Ge	0.05																			1986																																														K		19.8					19.8																																																																																																tape(100 um) +ANN(973K)					Fabrication of Nb3Al and Nb3(Al,Ge) superconducting composite tapes by electron beam irradiation			National Research Institute for Metals, Tsukuba Laboratories 1-2-1, Sengen, Tsukuba, Ibaraki 305, JAPAN	Appl.Phys.Lett.,49(1986)46	H.Kumakura,K.Tachikawa,K.Togano		
109007	APL0470640	minor phase = D8(b). Jc(4.2K)=2E+4 A/cm2 at 28T. Nb2Al precipitates are located in the A15 grain boundaries (grain size = 300 nm) 		Nb0.75Al0.19Ge0.06	Nb	0.75	Al	0.19	Ge	0.06																			1985																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																				T		43							T/K		3.12																																																																	arc-melt +ANN(1123K)					High magnetic field transport properties of liquid quenched Nb3Al and Nb3Al(Si,Ge) superconducting compounds			Division of Applied Science, Harvard University, Cambridge, Massachusetts, USA	Appl.Phys. Lett., 47(1985)640	D.Turnbull,F.Habbal,F.Habbal,,G.Clemente,J.Bevk		
109008	LTP0560051	minor phase = D8(b) 		Nb0.75Al0.18Ge0.07	Nb	0.75	Al	0.18	Ge	0.07																			1984																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		19.8					19.8																													T/K		2.68																																																																	arc-melt +ANN(1123K)					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
109009	BL83BAR1	Thermal conductivity was measured upto 50K at 0 and 10T of magnetic field.		Nb0.79Al0.16Ge0.05	Nb	0.79	Al	0.16	Ge	0.05																			1983																																														K		21					21																																																																																																not given									Izv.VMEI Lenin, 5(1983)133	G.V.Barboutov		
109010	BL83PLE1	For irradiation fluence = 0, 0.05, 0.5, 1.0, 4.0 *E+18 n/cm2, Tc = 17.9, 18.05, 18.6, 18.25, 17.95 K.		Nb0.75Al0.175Ge0.075	Nb	0.75	Al	0.175	Ge	0.075																			1983																																														K		17.9					17.9																																																																																																arc-melt +ANN +irradiation									Fizikas un technisko zinatnu serija, 4(1983)41	A.Petrov,E.Plechkens,V.Radzus		
109011	EEE0190414	Minor phase = A2. Splat cooled on a Cu  held at 873K. The A2 to A15 phase transformation takes place gradually. Jc = 4E+5 A/cm2 at 16 T. 		Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1983																												Cr3Si(A15)			A	5.183													Cr3Si, A15	K		18.6					18.6																																																																																																foil, splat cool +ANN(973-1173K)					Nb3(Al.Ge) superconductors prepared by hot-substrate liquid-quenching and subsequent annealing			National Research Institute for Metals 1-2-1, Sengen, Tukuba, Ibaraki 305, JAPAN	IEEE Trans.Magn., MAG-19(1983)414	H.Kumakura,K.Tachikawa,K.Togano,T.Takeuchi		
109012	BL81DUK1	Tape prepared by diffusion couples of Nb and Al-Ge. Hc2(4.2K)=41 T.		Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1981																												Cr3Si(A15)			A	5.179													Cr3Si, A15	K		20					20																													T/K		3.8																																																																	tape, react(1673 ...2323 K)									Phys.Mat.,3(1981)55	A.A.Fridman,I.S.Dukhovnii,V.P.Korzhov,V.V.Shmidt		
109013	SSC0280005	minor phase = Tetra. C(T) measured upto 25 K. 2*delta/kTc = 4.9. 		Nb0.75Al0.21Ge0.04	Nb	0.75	Al	0.21	Ge	0.04																			1978																												Cr3Si(A15)			A	5.1728													Cr3Si, A15	K		20					20																																																								mj/mol.K2	8.75		278																																					arc-melt +ANN(1273K)					Specific Heat of A-15 Nb3Al0.83Ge0.21			Los Alamos Scientific Laboratory, University of California, Los Alamos, N.M. 87545 USA	Solid State Commun., 28(1978)5	A.L.Giorgi,E.G.Szklarz,G.R.Stewart		
109014	SSC0210519			Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1977																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																								mj/mol.K2	7.71		303																																					arc-melt					Heat Capacity of the Nb3Al0.8Ge0.2 Compounds			Bergakademie, Freiberg, DDR	Solid State Commun., 21(1977)519	E.P.Krasnoperov,G.Wolf,K.Bohmhammel,N.E.Alekseevskii		
109015	SSC0210519			Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1977																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																																																								mj/mol.K2	7.54		295																																					arc-melt +ANN(1273K)					Heat Capacity of the Nb3Al0.8Ge0.2 Compounds			Bergakademie, Freiberg, DDR	Solid State Commun., 21(1977)519	E.P.Krasnoperov,G.Wolf,K.Bohmhammel,N.E.Alekseevskii		
109016	PSS0770129			Al0.25Nb0.75	Al	0.25	Nb	0.75																					1976																												Cr3Si(A15)																	Cr3Si, A15	K		18.6					18.6																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109017	PSS0770129			Nb0.75Al0.23Ge0.02	Nb	0.75	Al	0.23	Ge	0.02																			1976																												Cr3Si(A15)																	Cr3Si, A15	K		19.2					19.2																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109018	PSS0770129			Nb0.75Al0.21Ge0.04	Nb	0.75	Al	0.21	Ge	0.04																			1976																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109019	PSS0770129			Nb0.75Al0.19Ge0.06	Nb	0.75	Al	0.19	Ge	0.06																			1976																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109020	PSS0770129			Nb0.75Al0.17Ge0.08	Nb	0.75	Al	0.17	Ge	0.08																			1976																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109021	PSS0770129			Nb0.75Al0.16Ge0.09	Nb	0.75	Al	0.16	Ge	0.09																			1976																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																																																																																																arc-melt+ANN(1925K +973K)					Superconductivity of Nb3Al Base Ternary Solid Solutions			Institute of Metallurgy and Institute of Physical Problems, Moscow	Phys.Status Solidi (b), 77(1976)K129	N.E.Alekseevskii,N.V.Ageev,V.F.Shamray		
109022	JET0380525	dTc/dp=0.09 K/Gpa		Nb0.768Al0.146Ge0.086	Nb	0.768	Al	0.146	Ge	0.086																			1974																												Cr3Si(A15)			A	5.175													Cr3Si, A15	K		17.4					17.4			K/GPa	0.09																																																																																												melt +ANN(1923K)					Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109023	JET0380525	dTc/dp=0.12 K/Gpa		Nb0.76Al0.18Ge0.06	Nb	0.76	Al	0.18	Ge	0.06																			1974																												Cr3Si(A15)			A	5.177													Cr3Si, A15	K		17.88					17.88			K/GPa	0.12																																																																																												melt +ANN(1923K)					Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109024	JET0380525	dTc/dp= -0.02 K/Gpa		Nb0.75Al0.225Ge0.025	Nb	0.75	Al	0.225	Ge	0.025																			1974																												Cr3Si(A15)			A	5.18													Cr3Si, A15	K		17.9					17.9			K/GPa	-0.02																																																																																												melt +ANN(1923K)					Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109025	BL72ASH1			Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		15					15																				T		30																																																																										film( on Al2O3) by sputter									AIP Conf.Proc.No.4, ed by D.H.Douglass: Am.Inst.Phys., (1972)204	C.K.Jones,D.W.Deis,J.R.Gavaler,M.Ashkin		
109026	APJ0090845			Nb0.75Al0.2Ge0.05	Nb	0.75	Al	0.2	Ge	0.05																			1970																												Cr3Si(A15)																	Cr3Si, A15	K																											T		48																																																																										arc-melt +ANN(1023K)					Upper Critical Field of High Superconducting Transition Temperature Nb3Al0.75Ge0.25 Alloy at 4.2K			Department of Physics, College of Science and Engineering, Nihon University, Chiyoda-ku, Tokyo	Jpn.J.Appl.Phys.,9(1970)845	K.Yasukochi,N.Usui,R.Akihama		
109027	JTL0090016			Nb0.71Al0.203Ge0.087	Nb	0.71	Al	0.203	Ge	0.087																			1969																												Cr3Si(A15)			A	5.1744													Cr3Si, A15	K																											T		38							T/K		3																																																																	arc-melt									JETP Lett.,9(1969)16	N.E.Alekseevskii,N.N.Mikhailov,N.V.Ageev,V.F.Shamrai		
109028	ZPS2150323			Nb0.75Al0.178Ge0.072	Nb	0.75	Al	0.178	Ge	0.072																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		20.1					20.1																													T/K		2.9																																																																	arc-melt +ANN(1073K)					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.Phys., 215(1968)323	G.Otto		
109029	APL0470640	Jc(4.2K)=1*E+4 A/cm2 at 27 T.		Nb0.73Al0.255Si0.015	Nb	0.73	Al	0.255	Si	0.015																			1985																																														K		18.7					18.7																				T		35							T/K		2.74																																																																	arc-melt +ANN(1123K)					High magnetic field transport properties of liquid quenched Nb3Al and Nb3Al(Si,Ge) superconducting compounds			Division of Applied Science, Harvard University, Cambridge, Massachusetts, USA	Appl.Phys. Lett., 47(1985)640	D.Turnbull,F.Habbal,F.Habbal,,G.Clemente,J.Bevk		
109030	LB74YAS1	Hc2(4.2K)=27 T		Al0.25Nb0.75	Al	0.25	Nb	0.75																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		17.1					17.1																													T/K		2.6																																																																	arc-melt									Proc.5th Int.Cryog.Eng.Conf.(ICEC5),Kyoto,(1974)473	K.Yasukochi,N.Usui,R.Akihama		
109031	LB74YAS1	Hc2(4.2K)=29.2 T		Nb0.75Al0.225Si0.025	Nb	0.75	Al	0.225	Si	0.025																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																													T/K		2.9																																																																	arc-melt									Proc.5th Int.Cryog.Eng.Conf.(ICEC5),Kyoto,(1974)473	K.Yasukochi,N.Usui,R.Akihama		
109032	LB74YAS1	Hc2(4.2K)=22.4 T		Nb0.75Al0.2Si0.05	Nb	0.75	Al	0.2	Si	0.05																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																													T/K		2.65																																																																	arc-melt									Proc.5th Int.Cryog.Eng.Conf.(ICEC5),Kyoto,(1974)473	K.Yasukochi,N.Usui,R.Akihama		
109033	LB74YAS1	Hc2(4.2K)=22.3 T		Nb0.75Al0.15Si0.1	Nb	0.75	Al	0.15	Si	0.1																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																													T/K		2.45																																																																	arc-melt									Proc.5th Int.Cryog.Eng.Conf.(ICEC5),Kyoto,(1974)473	K.Yasukochi,N.Usui,R.Akihama		
109034	LTP0560051			Nb0.7275Zr0.0225Al0.25	Nb	0.7275	Zr	0.0225	Al	0.25																			1984																												Cr3Si(A15)			A	5.198													Cr3Si, A15	K		14.6					14.6																													T/K		2.13																																																																	arc-melt +ANN(1923K)					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
109035	LTP0560051			Nb0.7425Zr0.0075Al0.25	Nb	0.7425	Zr	0.0075	Al	0.25																			1984																												Cr3Si(A15)			A	5.187													Cr3Si, A15	K		17.4					17.4																													T/K		2.24																																																																	arc-melt +ANN(1923K)					The Volume Dependence of Tc of Ternary A-15 Phases			International Laboratory of High Magnetic Fields and Low Temperatures, Wroclaw, Poland	J.Low Temp.Phys., 56(1984)51	V.Shamrai		
109036	LB63JOH1			Nb3Al2C1	Nb	3	Al	2	C	1																			1963																															A	2.67		8.02											hexagonal	K					4.2																																																																																																		Hot-press +ANN(1270K)									Univ.Calif.EO.Lawrence Red.Lab Annual Report(1963)131	E.R.Parker,J.Johnston,K.Kennedy,L.Toth		
109037	LB84KUH1			Nb3Al2Cr1C1	Nb	3	Al	2	Cr	1	C	1																	1984																												Fe3W3C																	Fe3W3C, E9[3]	K					1.5																																																																																																		arc-melt +ANN(1070-1520K)									J.Phys.,22(1984)59	D.C.Johnston,H.C.Ku		
109038	LB84KUH1			Nb3Al2Cu1C1	Nb	3	Al	2	Cu	1	C	1																	1984																												Fe3W3C																	Fe3W3C, E9[3]	K					1.5																																																																																																		arc-melt +ANN(1070-1520K)									J.Phys.,22(1984)59	D.C.Johnston,H.C.Ku		
109039	LB84KUH1			Nb3Al2V1C1	Nb	3	Al	2	V	1	C	1																	1984																												Fe3W3C																	Fe3W3C, E9[3]	K					1.5																																																																																																		arc-melt +ANN(1070-1520K)									J.Phys.,22(1984)59	D.C.Johnston,H.C.Ku		
109040	LES0100029			Nb3Al2N1	Nb	3	Al	2	N	1																			1966																												beta-Mn																	beta-Mn, A13	K					1.3																																																																																																		powder, SIN(1073K)+Hot press(1473K)					The Superconducting Behavior of Several Complex Carbides and Nitrides			School of Mineral and Metallurgical Engineering, University of Minnesota, Minneapolis, Minn. U.S.A.	J.Less-Common Metals,10(1966)29	C.M.Yen,L.E.Toth,W.Jeitschko		
109041	JAP0533719	minor phase = Ti3P. Ti3P phase: a=10.298 , c=5.195 A.		As1Nb3	As	1	Nb	3																					1982																												Cr3Si(A15)																	Cr3Si, A15	K		6.5					6.5																				T		1.82																																																																										SIN(973K+1273K) +WQ					Superconductivity of the Nb3As system			Department of Physics, McMaster University, Hamilton, L8S4M1, Ontario, Canada	J.Appl.Phys.,53(1982)3719	C.V.Stager,J.P.Carbotte,P.K.Ummat,W.B.Cowan,W.R.Datars		
109042	PR0204538	dTc/dp=0.01 K/Gpa. K<B>=0.0017 Gpa		As1Nb3	As	1	Nb	3																					1979																												Ti3P																		K		0.25					0.25			K/GPa	0.01																																																																																												melt +ANN(1873K)					Effects of pressure on the structural and superconducting properties of Nb3As, Nb3Si, Nb3Ge, and Nb0.82Ge0.18			Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.B,20(1979)4538	A.R.Sweedler,D.U.Gubser,E.F.Skelton,I.L.Spain,J.O.Willis,R.A.Hein,R.M.Waterstrat,S.C.Yu		
109043	PR0143856	gamma=3.6 mJ/formula.K2		As1Nb3	As	1	Nb	3																					1976																												Ti3P																		K		0.31					0.31																													T/K		0.206																									mj/mol.K2	3.6		400																																					melt(in BeO  40 atm Ar)					Electronic and superconducting properties of the Ti3P-type compounds Nb3As and Nb3Si			U.S.Naval Research Laboratory, Washington, D.C.	Phys.Rev.B14(1976)3856	A.Junod,D.U.Gubser,R.A.Hein,R.M.Waterstrat		
109044	LB84PER1	two phases (A1, A3). composition not precisely given		Au1Nb3	Au	1	Nb	3																					1984																																														K		11.1					11.1																																																																																																Ssphere, ANN(1323K)									LT-17, vol.3(1984)617	E.Meyer,M.F.Da Silveira,R.F.R.Pereira		
109045	ZPS0230149			Au0.2Nb0.8	Au	0.2	Nb	0.8																					1976																												Cr3Si(A15)			A	5.22													Cr3Si, A15	K		7.9					7.9																																																																																																arc-melt +ANN(1473K)					Superconductivity of some splat cooled Nb-Au-Pt alloys				Z.Phys.B23(1976)149	C.J.Raub,H.R.Khan		
109046	JAP0414958	composition not specified.		Au1Nb3	Au	1	Nb	3																					1970																												Cr3Si(A15)			A	5.202													Cr3Si, A15	K		10.6					10.6																																																																																																sputter					Radio-Frequency-Sputtered Films of beta-Tungsten Structure Compounds			RCA Laboratories, Princeton, New Jersey 08540	J.Appl.Phys.,41(1970)4958	J.I.Gittleman,J.J.Hanak,J.P.Pellicane,S.Bozowski		
109047	SSC0260669	gamma=19.2 mJ/mole.K2. Ramda(e-p)=0.48		Au1Nb3	Au	1	Nb	3																					1978																												W			A	3.28													W, A2	K		1.5					1.5																																																								mj/mol.K2	19.2		305																																					arc-melt, splat cooling					The Density of States of b.c.c. Nb3Au: A Comparison with A-15 Nb3Au			Work completed under the auspices of the Department of Energy.	Solid State Commun., 26(1978)669	A.L.Giorgi,G.R.Stewart		
109048	PLA0300170	gamma=9.2 mJ/gat.K2. Ramda(e-p)=0.85		Au1Nb3	Au	1	Nb	3																					1969																												Cr3Si(A15)																	Cr3Si, A15	K		10.8					10.8																																																								mj/mol.K2	36.8		280																																					arc-melt +ANN					Specific Heat and Superconductivity of Nb-based A15-type Compounds			Institut de Physique de la matiere condensee, Universite de Geneve 1211 Geneve, Switzerland	Phys.Lett.A, 30A(1969)170	F.Heiniger,J.Muller,P.Spitzli,R.Flukiger		
109049	SSC0300723	rho<0>=83 uOhm.cm. Hc2(4.2K)=18.0 T.		Au1Nb3	Au	1	Nb	3																					1979																												Cr3Si(A15)			A	5.202													Cr3Si, A15	K		10.7					10.7																				T		23.5							T/K		3.2																																																																	arc-melt +ANN(1323K)					Upper Critical Fields of Nb-3Au, Nb3Au0.7Pt0.3 and Nb3Pt			Francis Bitter National Magnet Laboratory, Massachusetts, Institute of Technology, Cambridge, Massachusetts 02139, USA	Solid State Commun., 30(1979)723	E.J.Mcniff,Jr.,O.Fischer,R.Flukiger,S.Foner		
109050	SSC0480125	irradiation (5.3*E+19 n/cm2)		Au0.242Nb0.758	Au	0.242	Nb	0.758																					1983																												Cr3Si(A15)			A	5.205													Cr3Si, A15	K		10.56					10.56																																																																																																arc-melt +ANN +irradiation					The effect of atomic order on the superconducting properties of A-15 Nb3Au and Nb3Au1-xPtx alloys			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093, U.S.A.	Solid State Commun., 48(1983)125	A.R.Sweedler,C.L.Snead,Jr.,D.E.Cox,G.W.Webb,M.S.Wire		
109051	SSC0210239	DOS by XPS		Au0.24Nb0.76	Au	0.24	Nb	0.76																					1977																												Cr3Si(A15)																	Cr3Si, A15	K		10.56					10.56																																																																																																arc-melt +ANN(1773 +1473K)					X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
109052	LB74MUL1			Au0.2Nb0.8	Au	0.2	Nb	0.8																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		5					5																																																																																																arc-melt +ANN(1073K)									LT-13, vol.3(1974)446	A.Junod,C.Susz,F.Heiniger,J.Muller,R.Flukiger		
109053	LB74MUL1			Au0.22Nb0.78	Au	0.22	Nb	0.78																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		7.6					7.6																																																																																																arc-melt +ANN(1073K)									LT-13, vol.3(1974)446	A.Junod,C.Susz,F.Heiniger,J.Muller,R.Flukiger		
109054	LB74MUL1			Au0.24Nb0.76	Au	0.24	Nb	0.76																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		11					11																																																																																																arc-melt +ANN(1073K)									LT-13, vol.3(1974)446	A.Junod,C.Susz,F.Heiniger,J.Muller,R.Flukiger		
109055	LB74MUL1			Au0.25Nb0.75	Au	0.25	Nb	0.75																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		11					11																																																																																																arc-melt +ANN(1073K)									LT-13, vol.3(1974)446	A.Junod,C.Susz,F.Heiniger,J.Muller,R.Flukiger		
109056	LTP0060171	dTc/dP in K/GPa.		Au1Nb3	Au	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		11.08					11.08			K/GPa	0.039																																																																																												arc-melt +ANN(1053K)					Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
109057	LTP0060171	dTc/dP in K/GPa.		Au1Nb3	Au	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		11.23					11.23			K/GPa	0.042																																																																																												arc-melt +ANN(1053K)					Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
109058	LB80FLU1			Nb3Au0.7Pt0.3	Nb	3	Au	0.7	Pt	0.3																			1980																												Cr3Si(A15)			A	5.196													Cr3Si, A15	K		10					10																				T		21							T/K		2.9																																																																	arc-melt +ANN(1823K) +Q									Supercon.in d- and f-band metal,(1980)265	E.J.Mcniff,Jr.,R.Flukiger,S.Foner		
109059	LB80FLU1			Nb0.75Au0.175Pt0.075	Nb	0.75	Au	0.175	Pt	0.075																			1980																												Cr3Si(A15)			A	5.196													Cr3Si, A15	K		12.9					12.9																				T		30							T/K		3.3																																																																	arc-melt +ANN(1023K) +Q									Supercon.in d- and f-band metal,(1980)265	E.J.Mcniff,Jr.,R.Flukiger,S.Foner		
109060	PLA0300170	C measured between 1.2 and 20 K. ramda(e-p)=0.90		Nb0.75Au0.175Pt0.075	Nb	0.75	Au	0.175	Pt	0.075																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.8					12.8																																																								mj/mol.K2	8.6		305																																					arc-melt +ANN					Specific Heat and Superconductivity of Nb-based A15-type Compounds			Institut de Physique de la matiere condensee, Universite de Geneve 1211 Geneve, Switzerland	Phys.Lett.A, 30A(1969)170	F.Heiniger,J.Muller,P.Spitzli,R.Flukiger		
109061	LB60SCH1			Au2Nb3	Au	2	Nb	3																					1960																															A	3.37		3.03											tetragonal	K					1.2																																																																																																											Z.Metallkde,51(1960)329	E.Stolz,H.G.Meissner,K.Schubert,M.Potzschke,T.R.Anantharaman,W.Rossteutscher		
109062	LB60SCH1			Au9Nb11	Au	9	Nb	11																					1960																												beta-Mn			A	7.04														K					1.2																																																																																																											Z.Metallkde,51(1960)329	E.Stolz,H.G.Meissner,K.Schubert,M.Potzschke,T.R.Anantharaman,W.Rossteutscher		
109063	LB87GUS1	gamma=2.63 mJ/gat.K2. C(T) measured upto 16 K.		C0.98Nb1	C	0.98	Nb	1																					1987																																														K		11.8					11.8																																																								mj/mol.K2	5.207		350																																					SIN									Sov.Phys. Solid State, 29(1984)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109064	JCP0640581	gamma=3.20 mJ/mole.K2. C(T) measured between 1.5 and 100K.		C0.93Nb1	C	0.93	Nb	1																					1976																												NaCl																	NaCl, B1	K		6.5					6.5																																																								mj/mol.K2	3.2		496																																										Low temperature specific heat and phonon anomalies in transition metal compounds			Max planck Institut fur Festkorperforschung, Stuttgart, Federal Republic of Germany	J.Chem.Phys., 64(1976)581	E.Gmelin,K.H.Rieder,P.Roedhammer,W.Weber		
109065	APL0190090	gamma=2.83 mJ/mole.K2.		C1Nb1	C	1	Nb	1																					1971																												NaCl																	NaCl, B1	K		10.95					10.95																																																								mj/mol.K2	2.83		546																																										Effects of Radiation on Surface Resistance of Superconducting Niobium Cavity			Brookhaven National Laboratory, Upton, New York 11973	Appl.Phys.Lett., 19(1971)90	H.J.Halama		
109066	LB68TOT1	gamma=1.57 mJ/gat.K2. C(T) measured between 2 and 18 K.		C0.48Nb1	C	0.48	Nb	1																					1968																															A	5.402		4.959											epsiron-Fe2N	K					1.6																																																										mj/mol.K2	2.32		464																																					Hot-press +ANN(1900K)					Low Temperature Heat Capacities of Superconducting Niobium and Tantalum Carbides			School of Mineral and Metallurgical Engineering, University of Minnesota, Minneapolis, Minnesota.	Acta Metall., 16(1968)1183	L.E.Toth,M.Ishikawa,Y.A.Chang		
109067	LB68TOT1	gamma=2.83mJ/gat.K2. C(T) measured between 2 and 18 K.	see ref	Nb1C0.96	Nb	1	C	0.96																					1968																												NaCl																	NaCl, B1	K																																																															mj/mol.K2	5.55		604																																					Hot-press +ANN(1900K)					Low Temperature Heat Capacities of Superconducting Niobium and Tantalum Carbides			School of Mineral and Metallurgical Engineering, University of Minnesota, Minneapolis, Minnesota.	Acta Metall., 16(1968)1183	L.E.Toth,M.Ishikawa,Y.A.Chang		
109068	LB68TOT1	gamma=2.22 mJ/gat.K2. C(T) measured between 2 and 18 K.	see ref	Nb1C0.86	Nb	1	C	0.86																					1968																												NaCl																	NaCl, B1	K																																																															mj/mol.K2	4.13		542																																					Hot-press +ANN(1900K)					Low Temperature Heat Capacities of Superconducting Niobium and Tantalum Carbides			School of Mineral and Metallurgical Engineering, University of Minnesota, Minneapolis, Minnesota.	Acta Metall., 16(1968)1183	L.E.Toth,M.Ishikawa,Y.A.Chang		
109069	LB68TOT1	gamma=2.11 mJ/gat.K2. C(T) measured between 2 and 18 K.	see ref	Nb1C0.77	Nb	1	C	0.77																					1968																												NaCl																	NaCl, B1	K																																																															mj/mol.K2	3.73		500																																					Hot-press +ANN(1900K)					Low Temperature Heat Capacities of Superconducting Niobium and Tantalum Carbides			School of Mineral and Metallurgical Engineering, University of Minnesota, Minneapolis, Minnesota.	Acta Metall., 16(1968)1183	L.E.Toth,M.Ishikawa,Y.A.Chang		
109070	LB76BUR1			C0.9Nb1	C	0.9	Nb	1																					1976																																														K		5					5																				T		3.2																																																																																			Stud.Cercet.Fiz., 28(1976)549	D.Ungur,E.Burzo,E.Gruceanu,I.Bradea		
109071	APL0060183	Hc2(4.2K)=1.2 T. Jc(4.2K, 8T)=20 A/cm2.		C0.985Nb1	C	0.985	Nb	1																					1965																																														K		12					12																																																																																																hot-press					Low Critical Currents in Superconducting NbC			Union Carbide Research Institute P.O.Box 278, Tarrytown, N.Y.	Appl.Phys.Lett.,6(1965)183	J.Piper		
109072	LB78KAR1			C1Nb1	C	1	Nb	1																					1978																																														K		10.5					10.5																				T		5																																																																										irradiation +ANN					Influence of Reactor Irradiation on the Superconductive Properties of Niobium Carbide			Institute of Metal Physics, Urals Scientific Centre, Academy of Sciences U.S.S.R.	Phys.Met.Metallogr., 45(1978)193	A.Ye.Kar'kin,B.N.Goshchitskiy,E.Z.Valiyev,S.A.Davydov,S.P.Kurushin,V.I.Savin,V.Ye.Arkhipov		
109073	APL0360856	irradiation effect. Tirr=420K		C1Nb1	C	1	Nb	1																					1980																												NaCl																	NaCl, B1	K		11.2					11.2																																																																																																					The effect of neutron irradiation upon the superconducting critical temperature of some transition-metal carbides, nitrides, and carbonitrides			Brookhaven National Laboratory, Upton, New York 11973	Appl.Phys.Lett., 36(1980)856	D.Dew-Hughes,R.Jones		
109074	PR0040084	Anodized tips of Ta were used for point contact.		C0.96Nb1	C	0.96	Nb	1																					1971																																														K		9.8					9.8																																																3.2	1																																																				Gap Energy of Superconducting Niobium Carbide			Department of Physics and Materials Research Laboratory, University of Illinois, Urbana, Illinois 61801	Phys.Rev.B4(1971)84	L.G.Radosevich,L.W.Shacklette,W.S.Williams		
109075	JTL0410115	C-content is not enhanced by the high pressure treatment		Nb0.71Mo0.29C1	Nb	0.71	Mo	0.29	C	1																			1975																												NaCl																	NaCl, B1	K		13.45					13.45																																																																																																hot-press(1770K, 0.5h, 12GPa)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure			Institute of Chemistry, Urals Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP, 41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109076	LB64Jei1	structure= H phase		Nb2Sn1C1	Nb	2	Sn	1	C	1																			1964																															A	3.172		14.37												K					1.2																																																																																																		sintering (1123K, 600h)									Monatsh.Chem.95(1964)431	F.Benesovsky,H.Nowotny,W.Jeitschko		
109077	LB87GUS1	C(T) measured up to 16K. Gamma in mJ/K2.gat		Nb0.8Ta0.2C1	Nb	0.8	Ta	0.2	C	1																			1987																																														K																																																															mj/mol.K2	2.5		504																																					sintering									Sov.Phys. Solid State, 29(1984)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109078	LB87GUS1	C(T) measured up to 16K. Gamma in mJ/K2.gat		Nb0.6Ta0.4C1	Nb	0.6	Ta	0.4	C	1																			1987																																														K																																																															mj/mol.K2	2.64		421																																					sintering									Sov.Phys. Solid State, 29(1984)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109079	MRB0120657	The highest Tc among 0.817>Nb>0.749		Ga0.251Nb0.749	Ga	0.251	Nb	0.749																					1977																												Cr3Si(A15)																	Cr3Si, A15	K		19.9					19.9																																																																																																					The effect of composition on Tc in some high Tc A-15 structure super conductors				Mater.Res.Bull.,12(1977)657	A.R.Sweedler,G.W.Webb,S.Moehlecke		
109080	SSC0331015	C(T) measured between 1.4 and 27K. Gamma in mJ/K2.gat. Impurity phase is W5Si3 phase.		Ga1Nb3	Ga	1	Nb	3																					1980																												Cr3Si(A15)			A	5.168													Cr3Si, A15	K		20.1					20.1																																																								mj/mol.K2	11.4		280																																					arc-melting+ANN(2103K,4min)+ANN(973K,123h)					Specific Heat of High Tc, A-15 Nb0.75Ga0.25			Los Alamos Scientific Laboratory, University of California, Los Alamos, N.M. 87545	Solid State Commun., 33(1980)1015	G.R.Stewart,G.W.Webb		
109081	LB75FON1	nominal compo.=Nb0.68Ga0.32. Impurity phase = W5Si3 phase. Hc2(0) estimated using WHH theory by Y.Asada.	Nb3Ga	Ga0.25Nb0.75	Ga	0.25	Nb	0.75																					1975																												Cr3Si(A15)																	Cr3Si, A15	K		20					20																				T		35.8							T/K		2.56																																																																	arc-melting + ANN(973K,24h)									Colloq.Int.CNRS, No.242,Paris,(1975)423	S.Foner		
109082	PLA0380323		Nb3Ga	Ga0.19Nb0.81	Ga	0.19	Nb	0.81																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		13.3					13.3																				T		16							T/K		1.6																																																																	arc-melting + ANN(2073K)+Q + ANN(973K)					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
109083	PLA0380323		Nb3Ga	Ga0.245Nb0.755	Ga	0.245	Nb	0.755																					1972																												Cr3Si(A15)			A	5.165													Cr3Si, A15	K		20.2					20.2																				T		34.1							T/K		2.43																																																																	arc-melting + ANN(2073K)+Q + ANN(973K)					Upper critical fields of NbxGa1-x: A binary high temperature superconductor	197202		Francis Bitter National Magnet Laboratory, Massachusetts,USA	Phys.Lett.A,38()323	A.Wicklund,E.J.McNiff Jr.,E.J.Mcniff Jr.,G.W.Webb,L.J.Vieland,R.E.Miller,S.Foner		
109084	LTP0060171	dTc/dP in K/Gpa	Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		14.5					14.5			K/GPa	-0.07																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
109085	PR0215055	minor phase = A2. gamma in mJ/mol.K2	Nb3(Nb,Ge)	Ge0.02Nb0.98	Ge	0.02	Nb	0.98																					1980																												Cr3Si(A15)			A	5.239													Cr3Si, A15	K		5.2					5.2																																																								mj/mol.K2	18.6		260																																					Powder by CVD					Impurity stabilized A15 Nb3Nb- a new superconductor	198006		Universtiy of California. Los Alamos Scientific Laboratory. Los Alamos. New Mexico 87545	Phys.Rev.B, 21(1980)5055	F.A.Valencia,G.R.Stewart,L.R.Newkirk		
109086	PR0215055	gamma in mJ/mol.K2	Nb3(Nb,Ge)	Ge0.045Nb0.955	Ge	0.045	Nb	0.955																					1980																												Cr3Si(A15)			A	5.23													Cr3Si, A15	K		4.15					4.15																																																								mj/mol.K2	18.9		271																																					Powder by CVD					Impurity stabilized A15 Nb3Nb- a new superconductor	198006		Universtiy of California. Los Alamos Scientific Laboratory. Los Alamos. New Mexico 87545	Phys.Rev.B, 21(1980)5055	F.A.Valencia,G.R.Stewart,L.R.Newkirk		
109088	JTL0260394		Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1977																																														K		6.2					6.2																				T		5.7							T/K		1.33																																																																										Sov.Phys.JETP Lett., 26(1977)394	E.P.Khlybov,L.F.Vereshchagin,V.I.Novikshonov,V.L.Vvedenskii,V.V.Evdokimov		
109089	JTL0260394	starting material is mixture of Nb3Ge+Ge	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1977																												Cr3Si(A15)																	Cr3Si, A15	K		15.7					15.7																				T		11.5							T/K		1.05																																																																	hot press (7GPa,2273K)									Sov.Phys.JETP Lett., 26(1977)394	E.P.Khlybov,L.F.Vereshchagin,V.I.Novikshonov,V.L.Vvedenskii,V.V.Evdokimov		
109090	JTL0260394		Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1977																																														K		19.4					19.4																				T		23.5							T/K		1.76																																																																	hot press (7GPa,1673K)									Sov.Phys.JETP Lett., 26(1977)394	E.P.Khlybov,L.F.Vereshchagin,V.I.Novikshonov,V.L.Vvedenskii,V.V.Evdokimov		
109091	JTL0260394		Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1977																																														K		15.7					15.7																				T		17							T/K		1.6																																																																	hot press (7GPa,1473K)									Sov.Phys.JETP Lett., 26(1977)394	E.P.Khlybov,L.F.Vereshchagin,V.I.Novikshonov,V.L.Vvedenskii,V.V.Evdokimov		
109092	SSC0460197	dTc/dP in K/Gpa. Quasihydrostatic pressure.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1983																												Am																		K		4.05					4.05			K/GPa	-0.008																																																																																												sputter					Anomalous Behavior of Superconducting Transition Temperature of Amorphous and Crystalline Nb3Ge Under Pressure			Institut fur Experimentalphysik IV, Universitat Bochum, D-4630 Bochum 1, West Germany	Solid State Commun., 46(1983)197	F.S.Razavi,J.S.Schilling		
109093	SSC0460197	dTc/dP in K/Gpa. Quasihydrostatic pressure.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1983																												Cr3Si(A15)																	Cr3Si, A15	K		16.7					16.7			K/GPa	-0.25																																																																																												sputter					Anomalous Behavior of Superconducting Transition Temperature of Amorphous and Crystalline Nb3Ge Under Pressure			Institut fur Experimentalphysik IV, Universitat Bochum, D-4630 Bochum 1, West Germany	Solid State Commun., 46(1983)197	F.S.Razavi,J.S.Schilling		
109094	PR0204538	dTc/dP in K/Gpa.	Nb-Ge	Ge0.18Nb0.82	Ge	0.18	Nb	0.82																				1	1979																												Cr3Si(A15)																	Cr3Si, A15	K		6.05					6.05			K/GPa	-0.35																																																																																												arc-melting					Effects of pressure on the structural and superconducting properties of Nb3As, Nb3Si, Nb3Ge, and Nb0.82Ge0.18			Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.B,20(1979)4538	A.R.Sweedler,D.U.Gubser,E.F.Skelton,I.L.Spain,J.O.Willis,R.A.Hein,R.M.Waterstrat,S.C.Yu		
109095	PR0204538	dTc/dP in K/Gpa.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1979																												Cr3Si(A15)																	Cr3Si, A15	K		21.2					21.2			K/GPa	-0.116																																																																																												CVD					Effects of pressure on the structural and superconducting properties of Nb3As, Nb3Si, Nb3Ge, and Nb0.82Ge0.18			Naval Research Laboratory, Washington, D.C. 20375	Phys.Rev.B,20(1979)4538	A.R.Sweedler,D.U.Gubser,E.F.Skelton,I.L.Spain,J.O.Willis,R.A.Hein,R.M.Waterstrat,S.C.Yu		
109096	JET0380525	dTc/dP in K/Gpa.	Nb-Ge	Ge0.18Nb0.82	Ge	0.18	Nb	0.82																				1	1974																												Cr3Si(A15)			A	5.17													Cr3Si, A15	K		6.12					6.12			K/GPa	-0.17																																																																																												melting+ANN(1923K, 20h)					Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109097	LTP0060171	dTc/dP in K/Gpa.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				1	1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.281					6.281			K/GPa	-0.114																																																																																												melting					Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
109098	SSC0260417	thickness=6 um on Cu. C(T) measured within 4 - 29 K. gamma in mJ/mol.K2. 2*delta/kTc = 4.2	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1978																												Cr3Si(A15)			A	5.139													Cr3Si, A15	K		21.8					21.8																																																								mj/mol.K2	30.3		302																																					CVD					Specific heat of single phase Nb3Ge			Los Alamos Scientific Laboratory, University of California, Los Alamos, N.M. 87545, USA	Solid State Commun., 26(1978)417	F.A.Valencia,G.R.Stewart,L.R.Newkirk		
109099	PRL0410664	Thickness=8 um on quartz. C(T) measured within 1.2 - 13 K. gamma in mJ/mol.K. 2*delta/kTc = 3.5.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1978																												Am																		K		3.9					3.9																																																								mj/mol.K2	12		222																																					sputter					Comparison between the Amorphous and Crystalline (A-15) Phases on Nb3Ge	197808		IBM Thomas J. Watson Research Center, Yorktown Heights, New York 10598	Phys.Rev.Lett., 41(1978)664	C.C.Tsuei,J.M.Coey,S.von Molnar		
109100	LES0430005	Films contain 10 to 15 vol% Nb5Ge3 and 1.15wt% O2. Thickness=32 um. C(T) measured within 4.2 - 65 K. gamma in mJ/mol.K. 2*delta/kTc = 3.5.	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				4	1975																												Cr3Si(A15)			A	5.1405													Cr3Si, A15	K		21.2					21.2																																																								mj/mol.K2	60		280																																					CVD					Low Temperature Thermal and Electrical Properties of Chemical-Vapor-Deposited Nb3Ge			Department of Applied Physics, Stanford University, Stanford, Calif. 94305 (U.S.A.)	J.Less-Common Met., 43(1975)5	F.A.Valencia,J.M.E.Harper,L.R.Newkirk,T.H.Geballe		
109200	PSS0630693		Nb0.8Ga0.2	Ga0.2Nb0.8	Ga	0.2	Nb	0.8																					1981																												Cr3Si(A15)																	Cr3Si, A15	K		15.3					15.3																				T		20.9							T/K		2																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109201	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.19Ni0.01	Nb	0.8	Ga	0.19	Ni	0.01																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		14.1					14.1																				T		18.3							T/K		1.9																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109202	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.18Ni0.02	Nb	0.8	Ga	0.18	Ni	0.02																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		12.4					12.4																				T		16							T/K		1.9																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109203	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.17Ni0.03	Nb	0.8	Ga	0.17	Ni	0.03																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		11.8					11.8																				T		13.4							T/K		1.8																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109204	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.16Ni0.04	Nb	0.8	Ga	0.16	Ni	0.04																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		10.6					10.6																				T		11.9							T/K		1.75																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109205	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.15Ni0.05	Nb	0.8	Ga	0.15	Ni	0.05																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		9.4					9.4																				T		9.8							T/K		1.6																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109206	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.14Ni0.06	Nb	0.8	Ga	0.14	Ni	0.06																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		8.7					8.7																				T		8.8							T/K		1.5																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109207	PSS0630693		Nb0.8(Ga,Ni)0.2	Nb0.8Ga0.13Ni0.07	Nb	0.8	Ga	0.13	Ni	0.07																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		8.1					8.1																				T		8.1							T/K		1.5																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109208	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.195Cr0.005	Nb	0.8	Ga	0.195	Cr	0.005																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		14.9					14.9																				T		21.4							T/K		2																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109209	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.19Cr0.01	Nb	0.8	Ga	0.19	Cr	0.01																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		13.6					13.6																				T		19.9							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109210	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.18Cr0.02	Nb	0.8	Ga	0.18	Cr	0.02																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		13.1					13.1																				T		19.1							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109211	PR05508497		HoNi2B2C 	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1997								5.3																				LuNi2B2C																		K		7.77					7.77		2																																																																																																			Superconductivity magnetism, and their coexistence in R(Ni1-xCox)2B2C(R=Lu,Tm,Er,Ho,Dy)	199704		"Physikalisches Institut, Universita""t Bayreuth, D-95440 Bayreuth, Germany"	Phys.Rev.B,55(1997)8497	H. Schmidt,H.F. Braun		
109212	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.17Cr0.03	Nb	0.8	Ga	0.17	Cr	0.03																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		11.5					11.5																				T		16.6							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109213	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.16Cr0.04	Nb	0.8	Ga	0.16	Cr	0.04																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		10.6					10.6																				T		14.2							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109214	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.15Cr0.05	Nb	0.8	Ga	0.15	Cr	0.05																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		9.7					9.7																				T		13.2							T/K		2																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109215	PSS0630693		Nb0.8(Ga,Cr)0.2	Nb0.8Ga0.14Cr0.06	Nb	0.8	Ga	0.14	Cr	0.06																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		8.6					8.6																				T		11.9							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109216	PSS0640771	phases = A15, Nb5Ga3.  RRR=1.84	Nb75(Ga,Al)25	Ga25Nb75	Ga	25	Nb	75																					1981																												Cr3Si(A15)			A	5.176													Cr3Si, A15	K		17.6					17.6																				T		29.3							T/K		2.4																																																																	arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109217	PSS0640771	phases = A15, sigma phase. RRR=2.03	Nb75(Ga,Al)25	Nb75Ga15Al10	Nb	75	Ga	15	Al	10																			1981																												Cr3Si(A15)			A	5.181													Cr3Si, A15	K		18.55					18.55																				T		30.8							T/K		2.4																																																																	arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109218	PSS0640771	phases = A15, sigma phase. RRR=1.82	Nb75(Ga,Al)25	Nb75Ga10Al15	Nb	75	Ga	10	Al	15																			1981																												Cr3Si(A15)			A	5.181													Cr3Si, A15	K		17.2					17.2																				T		28							T/K		2.35																																																																	arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109219	PSS0640771	phases = A15, sigma phase. RRR=1.54	Nb75(Ga,Al)25	Nb75Ga7.5Al17.5	Nb	75	Ga	7.5	Al	17.5																			1981																												Cr3Si(A15)			A	5.184													Cr3Si, A15	K		18.3					18.3																				T									T/K																																																																			arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109220	PSS0640771	phases = A15, sigma phase. RRR=1.48	Nb75(Ga,Al)25	Nb75Ga5Al20	Nb	75	Ga	5	Al	20																			1981																												Cr3Si(A15)			A	5.184													Cr3Si, A15	K		18.25					18.25																				T		29.1							T/K		2.3																																																																	arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109221	PSS0640771	phases = A15, sigma phase. RRR=1.65	Nb75(Ga,Al)25	Al25Nb75	Al	25	Nb	75																					1981																												Cr3Si(A15)			A	5.19													Cr3Si, A15	K		17.5					17.5																				T		29.1							T/K		2.4																																																																	arc-melting, then ANN(800C,1 week)					The Superconducting Properties of Nb75Ga25-xAlx A15-Type Alloys Annealed at 800C for One Week			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,64(1981)771	J.Sosnowski		
109222	PR1401581	(NbC)1-x(NbN)x, x is not given. Whiskers grown along <111>direction	NbC/NbN	Nb1C0.5Ni0.5	Nb	1	C	0.5	Ni	0.5																			1965																												NaCl																		K		17.3					17.3																				T		10.7							T/K		0.9																																																																	reaction of NbF5 or NbCl5 with C and N					Superconductivity of NbC/NbN whiskers				Phys.Rev. 140 A(1965)1581	F.J.Darnel,P.E.Bierstedt,W.O.Forshey,R.K.Waring,Jr		
109223	SPS0291082	gamma in mj/gat.K2	NbC	C0.98Nb1	C	0.98	Nb	1																					1987																												NaCl																		K		11.8					11.8																																																								mj/mol.K2	2.63		350																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109224	SPS0291082	gamma in mj/gat.K2	NbC	C0.99Nb1	C	0.99	Nb	1																					1987																												NaCl																		K		10.6					10.6																																																								mj/mol.K2	3.12		321																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109225	SPS0291082	gamma in mj/gat.K2	(Nb,Ta)C	Nb0.8Ta0.2C1	Nb	0.8	Ta	0.2	C	1																			1987																												NaCl																		K		9.9					9.9																																																								mj/mol.K2	2.5		504																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109226	SPS0291082	gamma in mj/gat.K2	(Nb,Ta)C	Nb0.6Ta0.4C1	Nb	0.6	Ta	0.4	C	1																			1987																												NaCl																		K		9.4					9.4																																																								mj/mol.K2	2.64		421																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109227	SPS0291082	gamma in mj/gat.K2	(Nb,Ta)C	Nb0.4Ta0.6C1	Nb	0.4	Ta	0.6	C	1																			1987																												NaCl																		K		9.7					9.7																																																								mj/mol.K2	2.72		440																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109228	SPS0291082	gamma in mj/gat.K2	(Nb,Ta)C	Nb0.25Ta0.75C1	Nb	0.25	Ta	0.75	C	1																			1987																												NaCl																		K		9.8					9.8																																																								mj/mol.K2	2.89		499																																					solid state reaction					Low-temperature specific heat and magnetic susceptibility of superconducting solid solutions of niobium and tantalum carbides	198706		Institute of Chemistry, Ural Scientific Center of the Academy of Sciences of the USSR, Sverdlovsk	Sov.Phys.Solid State,29(1987)1082	A.I.Gusev,N.I.Kourov,S.Z.Nazarova		
109229	JET0410115		(Nb,Mo)C	Nb0.95Mo0.05C1	Nb	0.95	Mo	0.05	C	1																			1974																												NaCl			A	4.4674														K		12.1					12.1																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109230	JET0410115		(Nb,Mo)C	Nb0.85Mo0.15C1	Nb	0.85	Mo	0.15	C	1																			1974																												NaCl			A	4.442														K		12.7					12.7																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109231	JET0410115		(Nb,Mo)C	Nb0.71Mo0.29C1	Nb	0.71	Mo	0.29	C	1																			1974																												NaCl			A	4.4341														K		13.45					13.45																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109232	JET0410115		(Nb,Mo)C	Nb0.51Mo0.49C1	Nb	0.51	Mo	0.49	C	1																			1974																												NaCl			A	4.3926														K		12.22					12.22																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109233	JET0410115		(Nb,Mo)C	Nb0.3Mo0.7C1	Nb	0.3	Mo	0.7	C	1																			1974																												NaCl			A	4.3629														K		12.1					12.1																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109234	JET0410115		(Nb,Mo)C	Nb0.15Mo0.85C1	Nb	0.15	Mo	0.85	C	1																			1974																												NaCl			A	4.319														K		11.673					11.673																																																																																																heat(1500C, 120 kbar, 30min)					Superconductivity of solid solutions of niobium and molybdenum monocarbides under high hydrostatic pressure	197406		Institute of Chemistry, Ural Scientific Center, USSR Academy of Sciences	Sov.Phys.JETP,41(1975)115	L.B.Dubrovskaya,S.Z.Nazarova		
109235	PSS0620413	A15,Nb,Nb5Ga3 phases. RRR=1.5	Nb80Ga20	Ga20Nb80	Ga	20	Nb	80																					1980																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		15.4					15.4																				T		20.6							T/K		2																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109236	PSS0620413	A15,Nb,sigma phases. RRR=1.5	Nb80(Ga,Co)20	Nb80Ga19Co1	Nb	80	Ga	19	Co	1																			1980																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		13.7					13.7																				T		17.4							T/K		1.85																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109237	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga18Co2	Nb	80	Ga	18	Co	2																			1980																												Cr3Si(A15)			A	5.173													Cr3Si, A15	K		12.2					12.2																				T		15.5							T/K		1.8																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109238	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga17Co3	Nb	80	Ga	17	Co	3																			1980																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		11					11																				T		12.9							T/K		1.75																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109239	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga16Co4	Nb	80	Ga	16	Co	4																			1980																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		9.85					9.85																				T		11.3							T/K		1.71																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109240	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga15Co5	Nb	80	Ga	15	Co	5																			1980																												Cr3Si(A15)			A	5.175													Cr3Si, A15	K		9.17					9.17																				T		10.4							T/K		1.66																																																																	arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109241	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga14Co6	Nb	80	Ga	14	Co	6																			1980																												Cr3Si(A15)																	Cr3Si, A15	K		8.1					8.1																																																																																																arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109242	PSS0620413	A15,Nb,sigma phases.	Nb80(Ga,Co)20	Nb80Ga13Co7	Nb	80	Ga	13	Co	7																			1980																												Cr3Si(A15)																	Cr3Si, A15	K		7.92					7.92																																																																																																arc-melting					The Influence of Co Impurities on Superconducting Properties of the Nb80Ga20 Alloy with A15 Type Structure			Institute for Low Temperature snd Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,62(1980)413	J.Sosnowski,M.Drys,T.Mydlarz		
109243	LB78SOS1		Nb80Ga20	Ga20Nb80	Ga	20	Nb	80																					1978																												Cr3Si(A15)																	Cr3Si, A15	K		18.2					18.2																				T		27.1																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109244	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga19.7Fe0.03	Nb	80	Ga	19.7	Fe	0.03																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		17.3					17.3																				T		24.6																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109245	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga19.4Fe0.06	Nb	80	Ga	19.4	Fe	0.06																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		16.2					16.2																				T		22.6																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109246	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga19Fe1	Nb	80	Ga	19	Fe	1																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		15					15																				T		19.5																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109247	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga18Fe2	Nb	80	Ga	18	Fe	2																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		13.1					13.1																				T		15.5																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109248	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga17Fe3	Nb	80	Ga	17	Fe	3																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		11.6					11.6																				T		12.5																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109249	LB78SOS1		Nb80(Ga,Fe)20	Nb80Ga16Fe4	Nb	80	Ga	16	Fe	4																			1978																												Cr3Si(A15)																	Cr3Si, A15	K		10.3					10.3																				T		12.1																																																																										arc-melt + ANN(700C,50h)					The Effect of Fe Impurities on Superconducting and Magnetic Properties of Nb-Ga Alloys with A15 Structure			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	LT-15,1(1978)393	J.Sosnowski,M.Drys,M.Horobiowski,T.Mydlarz		
109250	PSS0570337	A15,Nb,Nb5Ga3 phases	Nb80Ga20	Ga20Nb80	Ga	20	Nb	80																					1980																												Cr3Si(A15)			A	5.173													Cr3Si, A15	K		15.2					15.2																				T		20.9							T/K		2																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109251	PSS0570337	A15,Nb,sigma phases	Nb80(Ga,Mn)20	Nb80Ga19Mn1	Nb	80	Ga	19	Mn	1																			1980																												Cr3Si(A15)			A	5.172													Cr3Si, A15	K		11.2					11.2																				T		13.7							T/K		1.81																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109252	PSS0570337	A15,Nb,sigma phases	Nb80(Ga,Mn)20	Nb80Ga18Mn2	Nb	80	Ga	18	Mn	2																			1980																												Cr3Si(A15)			A	5.169													Cr3Si, A15	K		7.79					7.79																				T		9.6							T/K		1.8																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109253	PSS0570337	A15,Nb,sigma phases	Nb80(Ga,Mn)20	Nb80Ga17Mn3	Nb	80	Ga	17	Mn	3																			1980																												Cr3Si(A15)			A	5.169													Cr3Si, A15	K		7.1					7.1																				T		8.38							T/K		1.76																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109254	PSS0570337	A15,Nb,sigma phases	Nb80(Ga,Mn)20	Nb80Ga16Mn4	Nb	80	Ga	16	Mn	4																			1980																												Cr3Si(A15)			A	5.166													Cr3Si, A15	K		6.03					6.03																				T		6.13							T/K		1.5																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109255	PSS0570337	A15,Nb,sigma phases	Nb80(Ga,Mn)20	Nb80Ga15Mn5	Nb	80	Ga	15	Mn	5																			1980																												Cr3Si(A15)																	Cr3Si, A15	K		5					5																				T		5.17							T/K		1.5																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109256	PSS0570337	A15,Nb,Nb5Ga3 phases	Nb78Ga22	Ga22Nb78	Ga	22	Nb	78																					1980																												Cr3Si(A15)			A	5.174													Cr3Si, A15	K		15.6					15.6																				T		21.3							T/K		1.9																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109257	PSS0570337	A15,Nb,sigma phases	Nb78(Ga,Mn)22	Nb78Ga21Mn1	Nb	78	Ga	21	Mn	1																			1980																												Cr3Si(A15)			A	5.17													Cr3Si, A15	K		11.2					11.2																				T		14.5							T/K		1.85																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109258	PSS0570337	A15,Nb,sigma phases	Nb78(Ga,Mn)22	Nb78Ga20Mn2	Nb	78	Ga	20	Mn	2																			1980																												Cr3Si(A15)			A	5.169													Cr3Si, A15	K		8.87					8.87																				T		10.4							T/K		1.7																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109259	PSS0570337	A15,Nb,sigma phases	Nb78(Ga,Mn)22	Nb78Ga19Mn3	Nb	78	Ga	19	Mn	3																			1980																												Cr3Si(A15)			A	5.167													Cr3Si, A15	K		7.42					7.42																																																																																																arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109260	PSS0570337	A15,Nb,sigma phases	Nb78(Ga,Mn)22	Nb78Ga18Mn4	Nb	78	Ga	18	Mn	4																			1980																												Cr3Si(A15)			A	5.166													Cr3Si, A15	K		5.97					5.97																				T		7.42							T/K		1.68																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109261	PSS0570337	A15,Nb,sigma phases	Nb78(Ga,Mn)22	Nb78Ga16Mn6	Nb	78	Ga	16	Mn	6																			1980																												Cr3Si(A15)			A	5.162													Cr3Si, A15	K		5.53					5.53																				T		5.96							T/K		1.62																																																																	arc-melting					The Influence of Magnetic Mn Impurities on the Superconducting Properties of A15-Type Nb78Ga22 and Nb80Ga20 Alloys			Institute for Low Temperature and Structure Research, Polish Academy of Science, Wroclaw	Physica Stat.Solidi A,57(1980)337	J.Sosnowski,M.Drys,T.Mydlarz		
109262	JET0380525	dTc/dP in K/Gpa	Nb3Al	Al1Nb3	Al	1	Nb	3																					1974																												Cr3Si(A15)			A	5.186													Cr3Si, A15	K		17.5					17.5			K/GPa	-0.09																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109263	JET0380525	dTc/dP in K/Gpa	Nb3(Al,Ge)	Nb3Al0.9Ge0.1	Nb	3	Al	0.9	Ge	0.1																			1974																												Cr3Si(A15)			A	5.18													Cr3Si, A15	K		18.4					18.4			K/GPa	-0.02																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109264	JET0380525	dTc/dP in K/Gpa	Nb3(Al,Ge)	Nb3.05Al0.7125Ge0.19	Nb	3.05	Al	0.7125	Ge	0.19																			1974																												Cr3Si(A15)			A	5.177													Cr3Si, A15	K		17.9					17.9			K/GPa	0.12																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109265	JET0380525	dTc/dP in K/Gpa	Nb3(Al,Ge)	Nb3.07Al0.5859Ge0.279	Nb	3.07	Al	0.5859	Ge	0.279																			1974																												Cr3Si(A15)			A	5.175													Cr3Si, A15	K		17.4					17.4			K/GPa	0.09																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109266	JET0380525	dTc/dP in K/Gpa	Nb3(Al,Ge)	Nb3.2Al0.24Ge0.4	Nb	3.2	Al	0.24	Ge	0.4																		1	1974																												Cr3Si(A15)			A	5.171													Cr3Si, A15	K		10.2					10.2			K/GPa	-0.1																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109267	JET0380525	dTc/dP in K/Gpa	Nb3Al	Al0.72Nb3.28	Al	0.72	Nb	3.28																				1	1974																												Cr3Si(A15)			A	5.17													Cr3Si, A15	K		6.2					6.2			K/GPa	-0.17																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109268	JET0380525	dTc/dP in K/Gpa	Nb3(Al,Ge)	Nb2.96Al0.7592Ge0.3224	Nb	2.96	Al	0.7592	Ge	0.3224																		1	1974																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8			K/GPa	-0.18																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109269	JET0380525	dTc/dP in K/Gpa	Nb3Al	Al1Nb3	Al	1	Nb	3																				1	1974																												Cr3Si(A15)																	Cr3Si, A15	K		17.11					17.11			K/GPa	-0.07																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109270	JET0380525	dTc/dP in K/Gpa	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				1	1974																												Cr3Si(A15)																	Cr3Si, A15	K		6.28					6.28			K/GPa	-0.114																																																																																																	Effect of high hydrostatic pressure and residual strain on the superconductivity of Nb-Al-Ge alloys with an A15-type structure	197403		Institute of Chemical Physics, USSR Academy of Sciences	Sov.Phys.JETP, 38(1973)525	A.G.Rabin'kin,V.N.Galev		
109271	PSS0770759		Nb3Al	Al1Nb3	Al	1	Nb	3																					1983																												Cr3Si(A15)																	Cr3Si, A15	K		18.8					18.8																													T/K		2.87																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109272	PSS0770759		Nb3(Al,Ge)	Nb3Al0.9Ge0.1	Nb	3	Al	0.9	Ge	0.1																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																													T/K		3.1																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109273	PSS0770759		Nb3(Al,Ge)	Nb3Al0.83Ge0.17	Nb	3	Al	0.83	Ge	0.17																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		19.6					19.6																													T/K		3.3																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109274	PSS0770759		Nb3(Al,Ge)	Nb3Al0.76Ge0.24	Nb	3	Al	0.76	Ge	0.24																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		20.4					20.4																													T/K		2.9																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109275	PSS0770759		Nb3(Al,Ge)	Nb3Al0.71Ge0.29	Nb	3	Al	0.71	Ge	0.29																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		20.7					20.7																													T/K		2.77																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109276	PSS0770759		Nb3(Al,Ge)	Nb3Al0.66Ge0.34	Nb	3	Al	0.66	Ge	0.34																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		20.4					20.4																													T/K		2.37																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109277	PSS0770759		Nb3(Al,Ge)	Nb3Al0.5Ge0.5	Nb	3	Al	0.5	Ge	0.5																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		15.9					15.9																													T/K		2.29																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109278	PSS0770759		Nb3(Al,Ge)	Nb3Al0.3Ge0.7	Nb	3	Al	0.3	Ge	0.7																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		9.1					9.1																																																																																																W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109279	PSS0770759		Nb3(Al,Ge)	Nb3Al0.15Ge0.85	Nb	3	Al	0.15	Ge	0.85																			1983																												Cr3Si(A15)																	Cr3Si, A15	K		7.4					7.4																													T/K		0.95																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109280	PSS0770759		Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1983																												Cr3Si(A15)																	Cr3Si, A15	K		6.4					6.4																													T/K		0.59																																																																	W-resistance furnace					Superconductivity and Decay Phenomena of Nb3Al-Nb3Ge Solid Solutions			Institute of Inorganic Chemistry, Academy of Sciences of the USSR, Siberian Branch, Novosibirsk	Physica Stat.Solidi A,77(1983)759	M.A.Starikov,S.P.Zakovryashin,Yu.F.Eltsev,Yu.I.Vesnin		
109281	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho. Rho=49.6 microOhm.cm	Nb3Al	Nb3Al1	Nb	3	Al	1																					1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		2.42																									mj/mol.K2	77.8																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109282	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho. Rho=55.6 microOhm.cm	Nb3(Al,Ge)	Nb3Al0.9Ge0.1	Nb	3	Al	0.9	Ge	0.1																			1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		2.86																									mj/mol.K2	81.4																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109283	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho. Rho=54.8 microOhm.cm	Nb3(Al,Ge)	Nb3Al0.8Ge0.2	Nb	3	Al	0.8	Ge	0.2																			1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		2.94																									mj/mol.K2	80.7																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109284	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho. Rho=57.4 microOhm.cm	Nb3(Al,Ge)	Nb3Al0.72Ge0.28	Nb	3	Al	0.72	Ge	0.28																			1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		2.89																									mj/mol.K2	80.7																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109285	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho.	Nb3(Al,Ge)	Nb3Al0.5Ge0.5	Nb	3	Al	0.5	Ge	0.5																			1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		2.41																									mj/mol.K2	69.3																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109286	PSS0760357	gamma in E+3 erg/cm3.K2 estimated from dHc2dT and rho. Rho=54.1 microOhm.cm	Nb3Ge	Nb3Ge1	Nb	3	Ge	1																					1983																												Cr3Si(A15)																	Cr3Si, A15	K																																				T/K		1.46																									mj/mol.K2	42.9																																												Reliability of n-Channel and p-Channel MOSTs in CMOS Integrated Circuits			Faculty of Electronic Engineering, University of Nis	Physica Stat.Solidi A,76(1983)357	N.Stojadinovic,S.Dimitrijev,S.Mijalkovic,Z.Zivic		
109287	PSS0630693		Nb80(Ga,Cr)20	Nb80Ga17.5Cr2.5	Nb	80	Ga	17.5	Cr	2.5																			1981																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5																				T		17.8							T/K		2.1																																																																	arc-melting					The Influence of Cr and Ni Impurities on Superconducting Properties of Nb80Ga20 Alloys with A15 Type Structure			Department of Fundamental Researches in Electrotechnics, Ministry of Machine Industry, Warsaw	Physica Stat.Solidi A,63(1981)693	J.Sosnowski,M.Drys,T.Mydlarz		
109288	PRL0860320	H<tr> in FIGURE is the 1st order phase transition in FLL state.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C																		K		16.6					16.6																																		MHC9288																																																																			Flux Line Lattice Reorientation in the Borocarbide Superconductors with H //  a			Riso National Laboratory, P.O. Box 49, DK-4000 Roskilde, Denmark	Phys.Rev.Lett., 86(2001)320-323	A.B.Abrahamsen,D.J.Bishop,D.Lopez,K.Mortensen,M.R.Eskildsen,N.H.Andersen,P.C.Canfield,P.L.Gammel		
109289	PRL0860320	CurieT shows ferromagnetic Tm.  Below Tm(=2.3K) sample shows weak ferromagnetism.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																	2001							2.3	6																				LuNi2B2C																		K		10.5					10.5																																		MHC9289																																																																			Flux Line Lattice Reorientation in the Borocarbide Superconductors with H //  a			Riso National Laboratory, P.O. Box 49, DK-4000 Roskilde, Denmark	Phys.Rev.Lett., 86(2001)320-323	A.B.Abrahamsen,D.J.Bishop,D.Lopez,K.Mortensen,M.R.Eskildsen,N.H.Andersen,P.C.Canfield,P.L.Gammel		
109290	PRL0860512	sandwitch of 3 layers. Misfit = 8.3 %	PbTe/PbS	Pb1Te1Pb1S1	Pb	1	Te	1	Pb	1	S	1																4	2001																																														K		6.03					6.03																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109291	PRL0860512	sandwitch of 3 layers. Misfit = 2.0 %	PbTe/SnTe	Pb1Te1Sn1Te1	Pb	1	Te	1	Sn	1	Te	1																4	2001																																														K		2.97					2.97																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109292	PRL0860512	sandwitch of 3 layers. Misfit = 3.16%	PbS/PbSe	Pb1S1Pb1Se1	Pb	1	S	1	Pb	1	Se	1																4	2001																																														K		4.59					4.59																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109293	PRL0860512	sandwitch of 3 layers. Misfit = 13.0 %	PbTe/YbS	Pb1Te1Yb1S1	Pb	1	Te	1	Yb	1	S	1																4	2001																																														K		5.93					5.93																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109294	NAT3620433	Meissner 8%	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1993																												fullerene			A	14.132														K		10.5					10.5																																																																																																					Increased transition temperature in superconducting Na2CsC60			AT & T Bell Lab, Murray Hill, New Jersey, USA	Nature , 362(1993)433	A.P.Ramirez,D.W.Murphy,M.J.Rosseinsky,O.Zhou,R.B.van Dover,R.C.Haddon,R.M.Fleming		
109295	NAT3620433	Tc defined as onset in M(T). Meissner 6%	(NH3)4Na2CsC60	N4H12Na2Cs1C60	N	4	H	12	Na	2	Cs	1	C	60															1993																												fullerene			A	14.473														K		29.6					29.6																																																																																																					Increased transition temperature in superconducting Na2CsC60			AT & T Bell Lab, Murray Hill, New Jersey, USA	Nature , 362(1993)433	A.P.Ramirez,D.W.Murphy,M.J.Rosseinsky,O.Zhou,R.B.van Dover,R.C.Haddon,R.M.Fleming		
109296	LES0670249	gamma in mj/mol.K2. C<es>/gamma.Tc = 1.25	NbB2	B2Nb1	B	2	Nb	1																					1979																												AlB2																	AlB2, C32	K		0.62					0.62																				kOe		1.6																																		mj/mol.K2	4																																												A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109297	LES0670249		TiB2	B2Ti1	B	2	Ti	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109298	LES0670249		ZrB2	B2Zr1	B	2	Zr	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109299	LES0670249		HfB2	B2Hf1	B	2	Hf	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109300	LES0670249		VB2	B2V1	B	2	V	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109301	LES0670249		TaB2	B2Ta1	B	2	Ta	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109302	LES0670249		CrB2	B2Cr1	B	2	Cr	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109303	LES0670249		MoB2	B2Mo1	B	2	Mo	1																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109304	LES0670249		Mo2B5	B5Mo2	B	5	Mo	2																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109305	LES0670249		W2B5	B5W2	B	5	W	2																					1979																												AlB2																	AlB2, C32	K					0.42																																																																																																							A search for superconductivity below 1K in transition metal borides				J.Less-Common Metals, 67(1979)249-255	E.Leyarovski,L.Leyarovska		
109306	EPL0530762	DOS estimated to be 12.76 states/eV.spin C60.	(NH3)xNaK2C60	N0.75H2.25Na1K2C60	N	0.75	H	2.25	Na	1	K	2	C	60															2001																												fullerene			A	14.36														K		11.8					11.8																																																																																																					Electronic properties of (NH3)xNaK2C60			Dipartimento di Fisica and Istituto Nazionale di Fisica della Materia Universita di Parma, Parco Area delle Scienze 7/a, 43100 Parma, Italy	Europhys.Lett., 53(2001)762-768	A.Sartori,F.Bolzoni,M.Ricco,M.Tomaselli,T.Shiroka		
109307	EPL0530762	DOS estimated to be 14.86 states/eV.spin C60.	(NH3)xNaK2C60	N0.85H2.55Na1K2C60	N	0.85	H	2.55	Na	1	K	2	C	60															2001																												fullerene			A	14.38														K		9					9																																																																																																					Electronic properties of (NH3)xNaK2C60			Dipartimento di Fisica and Istituto Nazionale di Fisica della Materia Universita di Parma, Parco Area delle Scienze 7/a, 43100 Parma, Italy	Europhys.Lett., 53(2001)762-768	A.Sartori,F.Bolzoni,M.Ricco,M.Tomaselli,T.Shiroka		
109308	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaRb2C60	N0.74H2.22Na1Rb2C60	N	0.74	H	2.22	Na	1	Rb	2	C	60															1996																												fullerene			A	14.5														K		17					17																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109309	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaRb2C60	N0.86H2.58Na1Rb2C60	N	0.86	H	2.58	Na	1	Rb	2	C	60															1996																												fullerene			A	14.52														K		12					12																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109310	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaRb2C60	N0.93H2.79Na1Rb2C60	N	0.93	H	2.79	Na	1	Rb	2	C	60															1996																												fullerene			A	14.531														K		8.5					8.5																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109311	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaK2C60	N0.84H2.52Na1K2C60	N	0.84	H	2.52	Na	1	K	2	C	60															1996																												fullerene			A	14.35														K		13					13																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109312	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaK2C60	N0.87H2.61Na1K2C60	N	0.87	H	2.61	Na	1	K	2	C	60															1996																												fullerene			A	14.369														K		11					11																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109313	PR05415653	ammonia content (x) by XRD. S/c volume = 40 %.	(NH3)xNaK2C60	N1H3Na1K2C60	N	1	H	3	Na	1	K	2	C	60															1996																												fullerene			A	14.4														K		8					8																																																																																																reaction in Liq.ammonia					Superconductivity of fcc fullerides containing off-centered octahedral cations			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-12, Japan	Phys.Rev.B, 54(1996)15653	H.Shimoda,T.Mitani,Y.Iwasa,Y.Maniwa,Y.Miyamoto		
109314	PRL0860512	sandwitch of 3 layers. Misfit = 4.8 %	PbS/YbS	Pb1S1Yb1S1	Pb	1	S	1	Yb	1	S	1																4	2001																																														K		6.39					6.39																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109315	PRL0860512	sandwitch of 3 layers. Misfit = 2.5 %	PbSe/EuS	Pb1Se1Eu1S1	Pb	1	Se	1	Eu	1	S	1																4	2001																																														K		2.48					2.48																																																																																																epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109316	PRL0860512	sandwitch of 3 layers. Misfit = 5.3 %. Not s/c.	YbS/EuS	Yb1S1Eu1S1	Yb	1	S	1	Eu	1	S	1																4	2001																																														K					1.5																																																																																																		epitaxial growth on (001)KCl					Novel Superconducting Semiconducting Superlattices: Dislocation-Induced Superconductivity?			Institute for Low Temperature Physics and Engineering, 47 Lenin Avenue, Kharkov 310164, Ukraine	Phys.Rev.Lett., 86(2001)512-515	A.I.Fedorenko,A.S.Pokhila,A.Yu.Sipatov,N.Ya.Fogel,R.I.Shekhter,Yu.V.Bomze		
109317	PRL0530497	For -[S8-xSex] series, 3.6K<Tc<4.1 K magnetic field induced s/c observed.	(Eu,Sn)Mo6(S,Se)8	Eu0.75Sn0.25Mo6S7.2Se0.8	Eu	0.75	Sn	0.25	Mo	6	S	7.2	Se	0.8														1	1984																												Chevrel																		K		3.9					3.9																																																																																																					Observation of Magnetic-Field-Induced Superconductivity			Departement de Physique de la Matiere Condensee, Universite de Geneve, CH-1211 Geneve 4, Switzerland	Phys.Rev.Lett., 53(1984)497	A.Briggs,C.Rossel,F.Fischer,G.Remenyi,H. W. Meul,M.Decroux		
109318	MAT0103571	penet estimated from cohere and Hc1(0). G-L parameter = 18	TaB2	B2Ta1	B	2	Ta	1																				1	2001																												AlB2			A	3.082		3.243											AlB2, C32	K		9.5					9.5											Oe		100							T		2.36												MHC9318		nm		13.4			nm		250																																																					powder made by borothermic method					Incipient superconductivity in TaB2			Institute of Low Temperature and Structure Research, Wroclaw, Poland	cond-mat/0103571(2001)	A.J.Zalesky,D.Kaczorowsky,J.Klamut,O.J.Zogal		
109319	MAT0103169		MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.083		3.52											AlB2, C32	K		38.8					38.8																																																																																																high-press-synthesis(850C)-ANN(500C in Ar)					Carbon substitution effect inMgB2			Seoul National University, Korea	cond-mat/0103169(2001)	Eun Jip Choi,Jai Seok		
109320	MAT0103169	two step transition,. onset=41K, endpoint=33K	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		1	2001																												AlB2			A	3.07		3.52											AlB2, C32	K		41					41																																																																																																high-press-synthesis(850C)-ANN(500C in Ar)					Carbon substitution effect inMgB2			Seoul National University, Korea	cond-mat/0103169(2001)	Eun Jip Choi,Jai Seok		
109321	MAT0103077		MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.0841		3.522											AlB2, C32	K		37.4					37.4																																																																																																solid state reaction in Ta tube. Heat(950C)					Effect of Li doping on structure and superconducting transition temperature of Mg1-xLixB2			Tsinghua University, Beijing, P.R.China	cond-mat/0103077(2001)	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109322	MAT0103077		(Mg,Li)B2	Mg0.9Li0.1B2	Mg	0.9	Li	0.1	B	2																			2001																												AlB2			A	3.0813		3.5195											AlB2, C32	K		37.4					37.4																																																																																																solid state reaction in Ta tube. Heat(950C)					Effect of Li doping on structure and superconducting transition temperature of Mg1-xLixB2			Tsinghua University, Beijing, P.R.China	cond-mat/0103077(2001)	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109323	MAT0103077		(Mg,Li)B2	Mg0.7Li0.3B2	Mg	0.7	Li	0.3	B	2																			2001																												AlB2			A	3.0692		3.5233											AlB2, C32	K		32.1					32.1																																																																																																solid state reaction in Ta tube. Heat(950C)					Effect of Li doping on structure and superconducting transition temperature of Mg1-xLixB2			Tsinghua University, Beijing, P.R.China	cond-mat/0103077(2001)	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109324	MAT0103077	not s/c. multi-phase.	(Mg,Li)B2	Mg0.5Li0.5B2	Mg	0.5	Li	0.5	B	2																			2001																												AlB2																	AlB2, C32	K					4.5																																																																																																		solid state reaction in Ta tube. Heat(950C)					Effect of Li doping on structure and superconducting transition temperature of Mg1-xLixB2			Tsinghua University, Beijing, P.R.China	cond-mat/0103077(2001)	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109325	PRL0861877	(delta-C/gamma*Tc )=1. Gamma in mj/mol.K2. Tc for B<11>	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.1432		3.5193											AlB2, C32	K		39.2					39.2						0.26	B																																																		3		750																																					react(950C, 2h, in Ta tube)					Boron isotope effect in superconducting MgB2			Ames Lab, Ioa State University, Ames, Ioa,USA	Phys.Rev.Lett., 86(2001)1877	C.E.Cunningham,C.Petrovic,G.Lapertot,N.Anderson,P.C.Canfield,S.L.Bud'ko		
109326	PRL0861877	Tc for MgB<10>2	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40.2					40.2																																																																																																react(950C, 2h, in Ta tube)					Boron isotope effect in superconducting MgB2			Ames Lab, Ioa State University, Ames, Ioa,USA	Phys.Rev.Lett., 86(2001)1877	C.E.Cunningham,C.Petrovic,G.Lapertot,N.Anderson,P.C.Canfield,S.L.Bud'ko		
109327	MAT0102289	dens=2.4 g/cm3. RRR=25.3, carrier=6.7 E+22/cm3. Mean free path=600A. G-L parameter = 26	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.14		3.52											AlB2, C32	K		39.4					39.4																																				A		50																																																										react(950C, 2h, in Ta tube)					Superconductivity in dense MgB2 wires			Ames Lab, Ioa State University, Ames, Ioa,USA	Phys.Rev.Lett., 86(2001)2423-2426	C.E.Cunningham,C.Petrovic,D.K.Finnemore,G.Lapertot,J.E.Ostenson,P.C.Canfield,S.L.Bud'ko		
109328	MAT0104303	dTc/dP in K/Gpa. Hydrostatic pressure, He-gas upto 1 Gpa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.2					39.2			K/GPa	-1.07																																																																																												react(950C, 2h, in Ta tube)					Hydrostatic Pressure Effect on the Superconducting Transition Temperature of MgB2				cond-mat/0104303(2001)	B.Lorenz,C.W.Chu,R.L.Meng		
109329	MAT0104242	using Mg<24>	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40.25					40.25						0.3	B																																																																																									react(850C, 1.5h, 50 bar Ar in BN crucible)					The reduced total isotope effect and its implications on the nature of superconductivity in MgB2			Metal Science Division, Argonne National Lab., Argonne, USA	cond-mat/0104242(2001)	D.G.Hinks,H.Claus,J.D.Jorgensen		
109330	MAT0104242	natural abundance Mg	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40.23					40.23						0.29	B																																																																																									react(850C, 1.5h, 50 bar Ar in BN crucible)					The reduced total isotope effect and its implications on the nature of superconductivity in MgB2			Metal Science Division, Argonne National Lab., Argonne, USA	cond-mat/0104242(2001)	D.G.Hinks,H.Claus,J.D.Jorgensen		
109331	MAT0104242	using Mg<26>	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40.21					40.21						0.31	B																																																																																									react(850C, 1.5h, 50 bar Ar in BN crucible)					The reduced total isotope effect and its implications on the nature of superconductivity in MgB2			Metal Science Division, Argonne National Lab., Argonne, USA	cond-mat/0104242(2001)	D.G.Hinks,H.Claus,J.D.Jorgensen		
109332	MAT0104206	gamma in mj/mol.K2. Delta-C=133 mj/mol.K. e-ph coupling const.=0.62	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.7					38.7																																																									2.6		1050																																					react(850C, 1.5h, 50 bar Ar in BN crucible)					Specific heat of MgB<11>2: Evidence for a second energy gap			University of California, Berkeley, CA, USA	Phys.Rev.Lett., 87(2001)047001	D.G.Hinks,F.Bouquet,J.D.Jorgensen,N.E.Phillips,R.A.Fisher		
109333	NAT3940039	s/c observed pressure range p=21kbar < s/c < 32 kbar only in high-quality sample. Tc represent Tc(max) at p=27 kbar.	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																		3	1998								10.2																				ThCr2Si2																		K		0.37			0		0.37	MPH9333																												T/K		6					A		150																																																										melt by RF					Magnetically mediated superconductivity in heavy fermion compounds			Cavendish Lab and IRC, University of Cambridge, UK	Nature, 394(1998)39-43	D.M.Freye,F.M.Grosche,G.G.Lonzarich,I.R.Walker,N.D.Mathur,R.K.W.Haselwimmer,S.R.Julian		
109334	NAT3940039	s/c observed pressure range p=22.7kbar < s/c < 28 kbar only in high-quality sample. Tc represent Tc(max) at p=25.6 kbar.	CeIn3	Ce1In3	Ce	1	In	3																				3	1998								10																																						K		0.17			0		0.17																																																																																																melt by RF					Magnetically mediated superconductivity in heavy fermion compounds			Cavendish Lab and IRC, University of Cambridge, UK	Nature, 394(1998)39-43	D.M.Freye,F.M.Grosche,G.G.Lonzarich,I.R.Walker,N.D.Mathur,R.K.W.Haselwimmer,S.R.Julian		
109335	P063104508	gamm in mj/mol.K2	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C																		K		16.01					16.01																				T		8.2																																			20.6																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109336	P063104508	gamm in mj/mol.K2	(Y,Lu)Ni2B2C	Y0.9Lu0.1Ni2B2C1	Y	0.9	Lu	0.1	Ni	2	B	2	C	1															2001																												LuNi2B2C																		K		15.56					15.56																				T		7.6																																			19.7																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109337	P063104508	gamm in mj/mol.K2	(Y,Lu)Ni2B2C	Y0.5Lu0.5Ni2B2C1	Y	0.5	Lu	0.5	Ni	2	B	2	C	1															2001																												LuNi2B2C																		K		14.9					14.9																				T		7.1																																			18.7																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109338	P063104508	gamm in mj/mol.K2	(Y,Lu)Ni2B2C	Y0.2Lu0.8Ni2B2C1	Y	0.2	Lu	0.8	Ni	2	B	2	C	1															2001																												LuNi2B2C																		K		14.68					14.68																				T		7																																			18.5																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109339	P063104508	gamm in mj/mol.K2	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C																		K		15.45					15.45																				T		7.6																																			19.7																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109340	P063104508	gamm in mj/mol.K2	La3Ni2B2N3	La3Ni2B2N3	La	3	Ni	2	B	2	N	3																	2001																																														K		11.73					11.73																				T		7.9																																			24																																												Superconducting properties of YxLu1-xNi2B2C and La3Ni2B2N3-z: A comparison between experiment and Eliashberg theory			Institut fur Experimentalphysik, Technische Universitut Wien, Wiedner Hauptstrasse 8-10, A-1040 Wien, Austria	Phys.Rev.B, 63(2001)104508	E.Schachinger,G.Hilscher,H.Michor,M.EL-Hagary,S.Manalo		
109341	P063144528	De Gennes factor=0	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2001																												LuNi2B2C																		K		15.41					15.41																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109342	P063144528	RRR=11.6. De Gennes factor=0.5	(Y,Tb)Ni2B2C	Y0.95Tb0.05Ni2B2C1	Y	0.95	Tb	0.05	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		14.42					14.42																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109343	P063144528	RRR=9.15. De Gennes factor=1.1	(Y,Tb)Ni2B2C	Y0.9Tb0.1Ni2B2C1	Y	0.9	Tb	0.1	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		13.48					13.48																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109344	P063144528	RRR=8.94. De Gennes factor=1.6	(Y,Tb)Ni2B2C	Y0.85Tb0.15Ni2B2C1	Y	0.85	Tb	0.15	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		12.54					12.54																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109345	P063144528	RRR=8.94. De Gennes factor=2.2	(Y,Tb)Ni2B2C	Y0.8Tb0.2Ni2B2C1	Y	0.8	Tb	0.2	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		11.43					11.43																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109346	P063144528	RRR=6.64. De Gennes factor=2.7	(Y,Tb)Ni2B2C	Y0.75Tb0.25Ni2B2C1	Y	0.75	Tb	0.25	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		10.02					10.02																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109347	P063144528	RRR=7.8. De Gennes factor=3.2	(Y,Tb)Ni2B2C	Y0.7Tb0.3Ni2B2C1	Y	0.7	Tb	0.3	Ni	2	B	2	C	1														3	2001																												LuNi2B2C																		K		9.03					9.03																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109348	P063144528	De Gennes factor=4.3	(Y,Tb)Ni2B2C	Y0.6Tb0.4Ni2B2C1	Y	0.6	Tb	0.4	Ni	2	B	2	C	1														3	2001								5.16																				LuNi2B2C																		K		5.04					5.04																																																																																																flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109349	P063144528		(Y,Tb)Ni2B2C	Y0.5Tb0.5Ni2B2C1	Y	0.5	Tb	0.5	Ni	2	B	2	C	1														3	2001								7.21																				LuNi2B2C																		K					2																																																																																																		flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109350	P063144528		(Y,Tb)Ni2B2C	Y0.4Tb0.6Ni2B2C1	Y	0.4	Tb	0.6	Ni	2	B	2	C	1														3	2001								9.2																				LuNi2B2C																		K					2																																																																																																		flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109351	P063144528		(Y,Tb)Ni2B2C	Y0.2Tb0.8Ni2B2C1	Y	0.2	Tb	0.8	Ni	2	B	2	C	1														3	2001								12.1																				LuNi2B2C																		K					2																																																																																																		flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109352	P063144528		TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																3	2001								15.1																				LuNi2B2C																		K					2																																																																																																		flux method by Ni2B solvent					Magnetism and superconductivity in Y1-xTbxNi2B2C single crystals			Center for Frontier Materials, Department of Materials Science and Engineering, Kwangju Institute of Science and Technology, Kwangju, 500-712, Korea	Phys.Rev.B, 63(2001)144528	B.K.Cho,H.B.Kim,Sung-Ik Lee		
109353	P063134519	TBL values for H//ab. Hc1//c=87mT, Hc2//c=9.3T, xi//ab=60A, xi//c=46A, ramda//ab=690A, ramda//c=1010A . G-L parameter = 11.6	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2001																												LuNi2B2C																		K		16.2					16.2											mT		67.2							T		12.1												MHC9353		A		60			A		690																																																					flux method by Ni2B solvent					Critical fields and specific heat of LuNi2B2C			Department of Physics, Occidental College, Los Angeles, California 90041	Phys.Rev.B, 63(2001)134519	A.H.Lacerda,G.M.Schmiedeshoff,J.A.Detwiler,J.L.Smith,P.C.Canfield,W.P.Beyermann		
109354	PR05600678	heavy fermion s/c. specific heat measured	CeCu2(Si,Ge)2	Ce1Cu2Si1.8Ge0.2	Ce	1	Cu	2	Si	1.8	Ge	0.2																	1997																												ThCr2Si2																		K		0.21					0.21																				T		1.5							T/K		27																																																																						Evolution of magnetism and superconductivity in CeCu2(Si1-xGex)2			Centro Atuico Bariloche (CNEA), 8400 S. C. de Bariloche, Argentina	Phys.Rev.B, 56(1997)678	C.Geibel,F.Steglich,J.G.Sereni,M.Deppe,M.Gomez-Berisso,M.Weiden,O.Trovarelli,P.Gegenwart,R.Muller-Reisener		
109355	PR05600678	heavy fermion s/c. specific heat measured	CeCu2(Si,Ge)2	Ce1Cu2Si1.9Ge0.1	Ce	1	Cu	2	Si	1.9	Ge	0.1																	1997																												ThCr2Si2																		K		0.2					0.2																																																																																																					Evolution of magnetism and superconductivity in CeCu2(Si1-xGex)2			Centro Atuico Bariloche (CNEA), 8400 S. C. de Bariloche, Argentina	Phys.Rev.B, 56(1997)678	C.Geibel,F.Steglich,J.G.Sereni,M.Deppe,M.Gomez-Berisso,M.Weiden,O.Trovarelli,P.Gegenwart,R.Muller-Reisener		
109356	PR05600678		CeCu2(Si,Ge)2	Ce1Cu2Si1.7Ge0.3	Ce	1	Cu	2	Si	1.7	Ge	0.3																	1997																												ThCr2Si2																		K		0.1					0.1																																																																																																					Evolution of magnetism and superconductivity in CeCu2(Si1-xGex)2			Centro Atuico Bariloche (CNEA), 8400 S. C. de Bariloche, Argentina	Phys.Rev.B, 56(1997)678	C.Geibel,F.Steglich,J.G.Sereni,M.Deppe,M.Gomez-Berisso,M.Weiden,O.Trovarelli,P.Gegenwart,R.Muller-Reisener		
109357	NAT4100063	Meissner fraction=49%	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.086		3.524											AlB2, C32	K		39					39																																																																																																HIP(973K, 196MPa)					Superconductivity at 39K in magnesium diboride			Aoyama-Gakuin University,Tokyo, Japan	Nature 410(2001)63-64	Jun Akimitsu,Jun Nagamatsu,Norimasa Nakagawa,Takahiro Muranaka,Yuji Zentani		
109358	NAT4060587	pressure induced s/c. p=0.9 Gpa<s/c<1.7 Gpa. Tc(max)=0.62K (p=1.3 Gpa).	UGe2	Ge2U1	Ge	2	U	1																				3	2000							53																																							K		0.62			0		0.62																																																																																																melt					Superconductivity on the border of itinerant-electron ferromagnetism in UGe2			Department of Physics, Cavendish Lab, Univ. of Cambridge, Cambridge, UK	Nature 406(2000)587	A.Huxley,D.Bralthwalte,E.Pugh,F.M.Groshe,G.G.Lonzarlich,I.Shelkin,J.Flouquet,K.Ahllan,M.J.Stelner,P.Agarwal,P.Monthoux,R.K.W.Haselwlmmer,S.R.Jullan,S.S.Saxena		
109359	PRL0862420	B is B<10>. RRR=20. Hc2(0) from dHc2/dT. G-L parameter = 26	MgB<10>2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		40.2					40.2																				T		12.5							T/K		0.44			MHC9359		nm		5.2			nm		140																																																					sintering(950C)					Thermodynamic and transport properties of superconducting MgB<10>2			Ames Lab., Iowa State University, Ames, Iowa, USA	Phys.Rev.Lett., 86(2001)2420	D.K.Finnemore,G.Lapertot,J.E.Ostenson,P.C.Canfield,S.L.Bud'ko		
109360	NAT4080549	Caution (Schon's data).  hole density=3.3-3.5/C60	hole-doped C60	C60	C	60																							2000																												fullerene																		K		52					52																																																																																																carrier doping by field-effect transistor(FET)					Superconductivity at 52 K in hole-doped C60			Bell Laboratories, Lucent Technologies, Murray Hill, New Jersey 07974, USA	Nature 408(2000)549	B.Batlog,Ch.Kloc,J.H.Schon		
109361	NAT4080549	Caution (Schon's FET data). hole density=2.0-2.5/C60	hole-doped C60	C60	C	60																							2000																												fullerene																		K		41.5					41.5																				T		20							T/K		0.7			MHC9361		A		40																																																										carrier doping by field-effect transistor(FET)					Superconductivity at 52 K in hole-doped C60			Bell Laboratories, Lucent Technologies, Murray Hill, New Jersey 07974, USA	Nature 408(2000)549	B.Batlog,Ch.Kloc,J.H.Schon		
109362	JSC1350325		SrNb2S5	Sr1Nb2S5	Sr	1	Nb	2	S	5																			1998																															A	3.361		24.06											hexagonal	K					1.45																																																																																																							BRIEF COMMUNICATION Evidence for Siperconductivity in SrTa2S5 and Matallic Characteristics of SrNb2S5			Department of Materials Science and Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050, Japan	J.Solid State Chem135(1998)325	Masatomo Takahashi,Nobuhiro Matsumoto,Norihito Kijima,Shoichi Nagata		
109363	JSC1350325		SrTa2S5	Sr1Ta2S5	Sr	1	Ta	2	S	5																			1998																															A	3.306		24.26											hexagonal	K		2.75					2.75																																																																																																					BRIEF COMMUNICATION Evidence for Siperconductivity in SrTa2S5 and Matallic Characteristics of SrNb2S5			Department of Materials Science and Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050, Japan	J.Solid State Chem135(1998)325	Masatomo Takahashi,Nobuhiro Matsumoto,Norihito Kijima,Shoichi Nagata		
109364	JSC1160392	resistivity(5K)=96 uOhm.cm. Hall coeffic. = 2.0 E-3 cm3/C	BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																			1995																															A	3.3258		25.208											hexagonal	K		2.88					2.88																																																																																																					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
109365	JSC1160392	resistivity(5K)=28 uOhm.cm. Hall coeffic. = 3.8 E-3 cm3/C	BaTa2S5	Ba1Ta2S5	Ba	1	Ta	2	S	5																			1995																															A	3.3204		25.005											hexagonal	K		3.14					3.14																																																																																																					Superconducting and Normal State Properties of Barium Tantalum Sulfide			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305, Japan	J.Solid State Chem.116(1991)392-399	H.Nozaki,Hiroshi Nozaki,M.Onoda,M.Saeki,Masanobu Saeki,Mitsuko Onoda		
109366	SSC0260943	needles	Nb3S4	Nb3S4	Nb	3	S	4																					1978																															A	9.604		3.378												K		4					4																																																																																																					Superconductivity in the Nb cluster compounds Nb3(X,Y)4 with X,Y = S, Se, Te			Universitat Munchen, FRG	Solid State Commun., 26(1978)943-947	A.Amberger,B.Obst,K.Polbom,M.Dietrich,P.Grimm		
109367	SSC0260943	parallel needles	Nb3Se4	Nb3Se4	Nb	3	Se	4																					1978																																														K		2					2																																																																																																					Superconductivity in the Nb cluster compounds Nb3(X,Y)4 with X,Y = S, Se, Te			Universitat Munchen, FRG	Solid State Commun., 26(1978)943-947	A.Amberger,B.Obst,K.Polbom,M.Dietrich,P.Grimm		
109368	SSC0260943	parallel needles	Nb3Te4	Nb3Te4	Nb	3	Te	4																					1978																																														K		1.8					1.8																																																																																																					Superconductivity in the Nb cluster compounds Nb3(X,Y)4 with X,Y = S, Se, Te			Universitat Munchen, FRG	Solid State Commun., 26(1978)943-947	A.Amberger,B.Obst,K.Polbom,M.Dietrich,P.Grimm		
109369	SSC0260943	not s/c	Nb3S1.7Se2.3	Nb3S1.7Se2.3	Nb	3	S	1.7	Se	2.3																			1978																																														K					1.3																																																																																																							Superconductivity in the Nb cluster compounds Nb3(X,Y)4 with X,Y = S, Se, Te			Universitat Munchen, FRG	Solid State Commun., 26(1978)943-947	A.Amberger,B.Obst,K.Polbom,M.Dietrich,P.Grimm		
109370	PLA0400353	gamma in mj/mol.K2	SnTaS3	Sn1Ta1S3	Sn	1	Ta	1	S	3																			1972																															A	4.06		11.87												K		2.9					2.9																																																								mj/mol.K2	8.4		203																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109371	PLA0400353	gamma in mj/mol.K2	NbSe2	Nb2Se2	Nb	2	Se	2																					1972																															A	3.44		12.54											hexagonal	K		6.9					6.9																																																								mj/mol.K2	20.5		210																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109372	PLA0400353	gamma in mj/mol.K2	SnNbSe3	Sn1Nb1Se3	Sn	1	Nb	1	Se	3																			1972																															A	4.21		24.54												K		3.02					3.02																																																								mj/mol.K2	17.5		181																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109373	PLA0400353		NbS2	Nb1S2	Nb	1	S	2																					1972																															A	3.31		11.89											hexagonal	K		6					6																																																								mj/mol.K2	10.7		265																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109374	PLA0400353		PbNbS3	Pb1Nb1S3	Pb	1	Nb	1	S	3																			1972																															A	4.07		11.91												K		2.66					2.66																																																								mj/mol.K2	11.7		200																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109375	PLA0400353		SnNbS3	Sn1Nb1S3	Sn	1	Nb	1	S	3																			1972																															A	4.05		11.77												K		2.75					2.75																																																								mj/mol.K2	9		198																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109376	PLA0400353		TaS2	S2Ta1	S	2	Ta	1																					1972																															A	3.32		12.07											hexagonal	K		1.9					1.9																																																								mj/mol.K2	9.1		205																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109377	PLA0400353		PbTaS3	Pb1Ta1S3	Pb	1	Ta	1	S	3																			1972																															A	4.08		11.97												K		3.11					3.11																																																								mj/mol.K2	11.7		189																																										Superconductivity in tin-group V<a> trichalcogenides			Philips Research Lab, Eindhoven, the Netherlands	Physics Lett. 40A(1972)353	M.H.van Maaren		
109378	PLA0310551		PbTiS3	Pb1Ti1S3	Pb	1	Ti	1	S	3																			1970																												PbTiS3			A	4.11		11.75												K					0.05																																																																																																							Superconductivity in PbNbS3 and PbTaS3			University of California, San Diego, California, USA	Phys.Lett., 31A(1970)551	L.Schmidt		
109379	PLA0310551		PbNbS3	Pb1Nb1S3	Pb	1	Nb	1	S	3																			1970																												PbTiS3			A	4.07		11.92												K		2.26					2.26																																																								mj/mol.K2	11.7		201																																										Superconductivity in PbNbS3 and PbTaS3			University of California, San Diego, California, USA	Phys.Lett., 31A(1970)551	L.Schmidt		
109380	PLA0310551		PbTaS3	Pb1Ta1S3	Pb	1	Ta	1	S	3																			1970																												PbTiS3			A	4.08		11.97												K		3.07					3.07																																																																																																					Superconductivity in PbNbS3 and PbTaS3			University of California, San Diego, California, USA	Phys.Lett., 31A(1970)551	L.Schmidt		
109381	PLA0310551	Debye-T, gamma from PLA0290571	NbS2	Nb1S2	Nb	1	S	2																					1970																															A	3.31		11.88											hexagonal	K		5.99					5.99																																																								mj/mol.K2	10.7		265																																										Superconductivity in PbNbS3 and PbTaS3			University of California, San Diego, California, USA	Phys.Lett., 31A(1970)551	L.Schmidt		
109382	PLA0310551	Debye-T, gamma from PLA0290571	TaS2	S2Ta1	S	2	Ta	1																					1970																															A	3.32		12.04											hexagonal	K		1.9					1.9																																																								mj/mol.K2	9.1		205																																										Superconductivity in PbNbS3 and PbTaS3			University of California, San Diego, California, USA	Phys.Lett., 31A(1970)551	L.Schmidt		
109383	EPL0530354	gamma in mj/mol.K2. Resistivity goes to zero at 1.2K. (Delta-C/gamma.T2)=0.76.CurieT=12.5K for H//C and -67.4K for H//a	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001							12.5																					HoCoGa5			A	4.668		7.515												K		0.4					0.4																																		MHC9383																						mj/mol.K2	720																																							heat(1100C)-slow cool to 600C					A new heavy-fermion superconductor CeIrIn5: A relative of the cuprates?			Los Alamos National Lab, Los Alamos, NM, USA	Europhys.Lett., 53(2001)354-359	C.Petrovic,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Jaime,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109384	PR05112673	gamma in mj/formula.K2. E-ph interaction = 0.68. (2*gap/kTc)=3.51. G-L parameter = 21	CuRh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			1995																												spinel			A	9.787														K		4.7					4.7											Oe		70							kOe		20												MHC9384		A		128			A		2670					3.51								mj/mol.K2	25		230																																					heat(850C)-SIN(850C)					Superconductivity in spinel-type compounds CuRh2S4 and CuRh2Se4	199505		Department of Materials Science and Engineering,Muroran Institute of Technology,Mizumoto-cho 27-1,Muroran 050,Japan	Phys.Rev.B.,51(1995)12673-12684	Ken-ichi Kumagai,Nobuo Wada,Seigo Tsuji,Shoichi Nagata,Takashi Shirane,Takatsugu Hagino,Yoshitaka Seki		
109385	PR05112673	gamma in mj/formula.K2. E-ph interaction = 0.64. (2*gap/kTc)=3.51. G-L parameter = 6.6	CuRh2Se4	Cu1Rh2Se4	Cu	1	Rh	2	Se	4																			1995																												spinel			A	10.269														K		3.48					3.48											Oe		95							kOe		4.4												MHC9385		A		274			A		1810					3.51								mj/mol.K2	26		211																																					heat(850C)-SIN(850C)					Superconductivity in spinel-type compounds CuRh2S4 and CuRh2Se4	199505		Department of Materials Science and Engineering,Muroran Institute of Technology,Mizumoto-cho 27-1,Muroran 050,Japan	Phys.Rev.B.,51(1995)12673-12684	Ken-ichi Kumagai,Nobuo Wada,Seigo Tsuji,Shoichi Nagata,Takashi Shirane,Takatsugu Hagino,Yoshitaka Seki		
109386	PR05308241	P-induced SC. SC data for P=11 kbar.  Tc(max)=0.43 K at P = 6 kbar. Tc defined as Tc(onset).	CeRh2Si2	Ce1Rh2Si2	Ce	1	Rh	2	Si	2																			1996								36																				ThCr2Si2																		K	0.2	0.26	0.35		0		0.26	MPH9386																												T/K		1.4																									mj/mol.K2	80														uOhm.cm							2																		arc-melting					Superconductivity in heavy-fermion CeRh2Si2	04		Los Alamos National Laboratory,Los Alamos,New Mexico 87545	Phys.Rev.B,53(1996)8241	D.Mandrus,J.D.Thompson,J.L.Smith,R.Movshovich,T.Graf,Z.Fisk	Ce, Rh, Si	
109387	JPS0682495	Hc1=250 Oe, and Hc2=20 kOe at 2.0 K	(Cu,Zn)Ir2S4	Cu0.7Zn0.3Ir2S4	Cu	0.7	Zn	0.3	Ir	2	S	4																1	1999																												spinel			A	9.8934														K		2.8					2.8																				kOe		35																																		mj/mol.K2	13		287																																					SIN(850C)					Metal-Insulator Transition and Superconductivity in Spinel-Type System Cu1-xZnxIr2S4	199908		National Research Institute for Metals, Tsukuba 305-0047	J.Phys.Soc.Japan,68(1999)2495-2497	Akira Kamimura,Guanghan Cao,Hideaki Kitazawa,Hiroyuki Suzuki,Kazuto Hirata,Takao Furubayashi,Takehiko Matsumoto		
109388	JPS0682495		(Cu,Zn)Ir2S4	Cu0.5Zn0.5Ir2S4	Cu	0.5	Zn	0.5	Ir	2	S	4																1	1999																												spinel			A	9.9206														K		2.2					2.2																																																																																																SIN(850C)					Metal-Insulator Transition and Superconductivity in Spinel-Type System Cu1-xZnxIr2S4	199908		National Research Institute for Metals, Tsukuba 305-0047	J.Phys.Soc.Japan,68(1999)2495-2497	Akira Kamimura,Guanghan Cao,Hideaki Kitazawa,Hiroyuki Suzuki,Kazuto Hirata,Takao Furubayashi,Takehiko Matsumoto		
109389	PRL0844986	pressure-induced-s/c. s/c properties are at p=21 kbar. P=16.3 kbar<s/c<22 kbar. Bulk modulus B=650 kbar	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																			2001							-79	3.8																				HoCoGa5			A	4.652		7.542												K		2.1			0		2.1																													T/K		14																									mj/mol.K2	420																																							from In-flux					Pressure-Induced Superconductivity in Quasi-2D CeRhIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545 ,USA	Phys.Rev.Lett., 84(2000)4986	C.Petrovic,E.G.Moshopoulou,H.Hegger,J.D.Thompson,J.L.Sarrao,M.F.Hundley,Z.Fisk		
109390	MAT0102413	Hc2(0) estimated by extraporation. Sample is 100 micron fiber.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.5					39.5																				T		16.4																																																																										B fiber react with Mg(950C)					Magnetoresistivity and complete Hc2(T) in MgB2			Ames Lab., Iowa State University, Ames, Iowa,USA	Phys.Rev.B, 63(2001)220503, cond-mat/0102413	A.H.Lacerda,C.E.Cunningham,C.Petrovic,G.Lapertot,M-H.Jung,P.C.Canfield,S.L.Bud'ko		
109391	MAT0103296	c-content: nominal value. Maybe, stoichiometric sample is the best.	MgCNi3	Mg1C1.25Ni3	Mg	1	C	1.25	Ni	3																			2001																												CaTiO3			A	3.8122														K		7.3					7.3																																																																																																(Mg-flakes+Ni-powder+glassy-C)-react(900C)					Superconductivity in the non-oxide Perovskite MgCNi3			Princeton University, Princeton,NJ,USA	cond-mat/0103296(2001), Nature 411(2001)54	A.P.Ramirez,H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.P.Ong,N.Rogado,Q.Huang,R.J.Cava,T.He,Y.Wang		
109392	MAT0103296	gamma in mj/mole-Ni.K2. c-content: nominal value. Maybe, stoichiometric sample is the best.	MgCNi3	Mg1C1.5Ni3	Mg	1	C	1.5	Ni	3																			2001																												CaTiO3			A	3.816														K		8.4					8.4																																																								mj/mol.K2	10																																							(Mg-flakes+Ni-powder+glassy-C)-react(900C)					Superconductivity in the non-oxide Perovskite MgCNi3			Princeton University, Princeton,NJ,USA	cond-mat/0103296(2001), Nature 411(2001)54	A.P.Ramirez,H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.P.Ong,N.Rogado,Q.Huang,R.J.Cava,T.He,Y.Wang		
109393	MAT0104541		MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2001																												CaTiO3			A	3.81														K		7					7																																																																																																mixture in Ta foil-heat(max 900C)					The suppression of superconductivity in MgCNi3 by Ni-site doping			Princeton University, Princeton,NJ,USA	cond-mat/0104541(2001)?,  Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109394	MAT0104541		MgC(Ni,Cu)3	Mg1C1Ni2.97Cu0.03	Mg	1	C	1	Ni	2.97	Cu	0.03																	2001																												CaTiO3			A	3.81														K		6.8					6.8																																																																																																mixture in Ta foil-heat(max 900C)					The suppression of superconductivity in MgCNi3 by Ni-site doping			Princeton University, Princeton,NJ,USA	cond-mat/0104541(2001)?,  Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109395	MAT0104541		MgC(Ni,Cu)3	Mg1C1Ni2.94Cu0.06	Mg	1	C	1	Ni	2.94	Cu	0.06																	2001																												CaTiO3			A	3.81														K		6.3					6.3																																																																																																mixture in Ta foil-heat(max 900C)					The suppression of superconductivity in MgCNi3 by Ni-site doping			Princeton University, Princeton,NJ,USA	cond-mat/0104541(2001)?,  Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109396	MAT0104541		MgC(Ni,Cu)3	Mg1C1Ni2.91Cu0.09	Mg	1	C	1	Ni	2.91	Cu	0.09																	2001																												CaTiO3			A	3.81														K		6					6																																																																																																mixture in Ta foil-heat(max 900C)					The suppression of superconductivity in MgCNi3 by Ni-site doping			Princeton University, Princeton,NJ,USA	cond-mat/0104541(2001)?,  Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109397	PHC2820303	pressure-induced s/c. Neel temp. decreases with pressure. S/c properties are measured at p=24.1 kbar.	CeIn3	Ce1In3	Ce	1	In	3																					1997								10.1																																					cubic	K		0.15			0		0.15																																																																																																					The normal and superconducting states of CeIn3 near the border of antiferromagnetic order			Cavendish Lab, Univ. of Cambridge	Physica C, 282(1997)303	D.M.Freye,F.M.Grosche,G.G.Lonzarich,I.R.Walker		
109398	PHC1470001	gamma in mj/mol.K2	CeCu2Si2	Ce1Cu2.53Si2	Ce	1	Cu	2.53	Si	2																		3	1987																												ThCr2Si2																		K		0.62					0.62																				T		2.06							T/K		20																									mj/mol.K2	630																																												Magnetic properties of heavy fermion superconductors				Physica B+C, 147(1987)1	Ulrich Rauchschwalbe		
109399	ZPB0830305	gamma in mj/mol.K2	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																			1991								4.6																				PrNi2Al3			A	5.207		4.018												K		1					1																																																								mj/mol.K2	120																																							arc-melting					A new heavy-fermion superconductor: UNi2Al3				Z.Phys.B, 83(1991)305	A.Grauel,A.Mehner,B.Seidel,C.D.Bredl,C.Geibel,D.Kaczorowsky,F.Steglich,K.Petersen,R.Helfrich,S.Thies,U.Ahlheim		
109400	ZPB0840001	gamma in mj/mol.K2. G-L parameter = 50	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			1991								14																				PrNi2Al3			A	5.365		4.186												K		2					2																													T/K		4.3					A		85			A		4000													mj/mol.K2	210																																							arc-melting					Heavy-fermion superconductivity at Tc=2 K in the antiferromagnet UPd2Al3				Z.Phys.B, 84(1991)1	A.Bohm,A.Grauel,C.D.Bredl,C.Geibel,C.Schank,F.Steglich,G.Weber,H.Kitazawa,M.Rau,R.Caspary,R.Helfrich,S.Thies,U.Ahlheim		
109401	ZPB1030263	pressure-induced s/c. Tc at p=28 kbar.	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																			1997																																														K		0.43			0		0.43																																																																																																					Quantum critical behaviour in the CePd2Si2/CeNi2Ge2 system				Z.Phys.B, 103(1997)263	F.M.Grosche,F.V.Carter,G.G.Lonzarich,N.D.Mathur,R.K.W.Haselwimmer,S.J.S.Lister,S.R.Julian,S.S.Saxena		
109402	ZPB1030263	pressure-induced s/c. Tc at p=18 kbar. Tc(max) = 0.4 K at p=26 kbar.	CeNi2Ge2	Ce1Ni2Ge2	Ce	1	Ni	2	Ge	2																			1997																																														K		0.22			0		0.22																																																																																																					Quantum critical behaviour in the CePd2Si2/CeNi2Ge2 system				Z.Phys.B, 103(1997)263	F.M.Grosche,F.V.Carter,G.G.Lonzarich,N.D.Mathur,R.K.W.Haselwimmer,S.J.S.Lister,S.R.Julian,S.S.Saxena		
109403	PRL0864915	gap measured by photoemission. Gap(0) estimated to be 5 meV from 4.5 meV at 15 K using BCS.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.5					39.5																																																3	9																																																				High-Resolution Photoemission Study of MgB2			Department of Physics, Tohoku University, 980-8578 Sendai, Japan	Phys.Rev.Lett., 86(2001)4915	J.Akimitsu,S.Souma,T.Muranaka,T.Sato,T.Takahashi		
109404	PRL0864374	gap by STM. after correction (Tc of surface region = 35 K), (2*gap/kTc) = 3.5	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39																																																3	11																																															react(850C in Ar)					Scanning Tunneling Spectroscopy in MgB2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439 ,USA	Phys.Rev.Lett., 86(2001)4374	D.G.Hinks,G.Karapetrov,G.W.Crabtree,M.Iavarone,W.K.Kwok		
109405	PRL0864664	gap by NMR. R shows zero-resistance at 1.2 K.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001																												HoCoGa5																		K		0.4					0.4																																																5	6																																															In-flux method					Unique Spin Dynamics and Unconventional Superconductivity in the Layered Heavy Fermion Compound CeIrIn5: NQR Evidence			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.Lett., 86(2001)4664	D.Aoki,G.-q. Zheng,K.Tanabe,S.Kawasaki,T.Mito,Y.Haga,Y.Kitaoka,Y.Onuki		
109406	PLA1630475	pressure-induced s/c. s/c properties were measured at p=101 kbar for H//c. critical pressure = 75 kbar.	CeCu2Ge2	Ce1Cu2Ge2	Ce	1	Cu	2	Ge	2																			1992								4.1																																						K		0.64			0		0.64																				T		2							T/K		11					A		90																																																															Pressure induced heavy fermion superconductivity of CeCu2Ge2			Universite de Geneve, Switzerland	Phys.Lett., A 163(1992)475	D.Jaccard,J.Sierro,K.Behnia		
109407	MAT0105293	space group = Cmcm	Re3B	B1Re3	B	1	Re	3																					2001																															A	2.8905	9.3039	7.2641												K		4.7					4.7																																																																																																heat ReB2(950-100C)					Superconductivity in the Re-B system				cond-mat/0105293(2001)	A.N.Chaika,D.V.Shovkun,G.K.Strukova,V.F.Degtyareva,V.M.Ionov,V.N.Zverev		
109408	MAT0105293	Tc = 4.5 - 6.3 depending on B-content	ReB2	B2Re1	B	2	Re	1																					2001																																														K		6.3					6.3																																																																																																					Superconductivity in the Re-B system				cond-mat/0105293(2001)	A.N.Chaika,D.V.Shovkun,G.K.Strukova,V.F.Degtyareva,V.M.Ionov,V.N.Zverev		
109409	MAT0105271	Hc1//c = 27.2 mT, Hc1//ab = 38.4 mT, Hc2//c = 9.2 T, Hc2//ab = 25.5 T, ksi//c = 2.5 nm, ksi//ab = 6.5 nm, anisotropy factor = 2.6	MgB2	B2Mg1	B	2	Mg	1																				3	2001																												AlB2			A	3.047		3.404											AlB2, C32	K		38.6					38.6											mT		38.4							T		25.5														nm		6.5																																																										vapor transport method					Single crystal MgB2 with anisotropic superconducting properties			National Research Institute for Metals, Tsukuba-si, Ibaraki,Japan	cond-mat/0105271(2001)	A.Matsushita,G.Kido,H.Abe,H.Kitazawa,J.Ye,K.Nishida,M.Xu,Y.Takano		
109410	JPS0700877	Curie-T = -10.7 K for [001] and = -92.1 K for [110]	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001							-10.7																																							K		0.4					0.4																																																																																																self-flux method					Magnetic and Thermal Properties of CeIrIn5 and CeRhIn5			Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 70(2001)877	D.Aoki,K.Kindo,K.Sugiyama,T.Inoue,T.Takeuchi,Y.Haga,Y.Onuki,Y.Tokiwa		
109411	JPS0700877	P-induced SC. P<crit> = 15 kbar.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2001							5.8	3.8																				HoCoGa5																		K		2.1			0		2.1																																																																																																self-flux method					Magnetic and Thermal Properties of CeIrIn5 and CeRhIn5			Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 70(2001)877	D.Aoki,K.Kindo,K.Sugiyama,T.Inoue,T.Takeuchi,Y.Haga,Y.Onuki,Y.Tokiwa		
109412	PRL0865152	gamma in mj/mol.K2. Delta-C/gamma.Tc = 0.76	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001																																														K		0.4					0.4																																				A		241										3.73								mj/mol.K2	110								MTHC9412																															excess In flux					Unconventional Superconductivity in CeIrIn5 and CeCoIn5: Specific Heat and Thermal Conductivity Studies			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett., 86(2001)5152	C.Petrovic,J.D.Thompson,J.L.Sarrao,M.Jaime,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109413	PRL0865152	gamma in mj/mol.K2. Delta-C/gamma.Tc = 4.5	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2001																																														K		2.3					2.3																																																								mj/mol.K2	40								MTHC9413																															excess In flux					Unconventional Superconductivity in CeIrIn5 and CeCoIn5: Specific Heat and Thermal Conductivity Studies			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.Lett., 86(2001)5152	C.Petrovic,J.D.Thompson,J.L.Sarrao,M.Jaime,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109414	MAT0105429	RRR=5.4. Thermopower(300K)=8.6 microV/K. Figure shows thermal conductivity.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		38.7					38.7																																																																	MTHC9414																															solid state reaction					Heat and charge transport properties of MgB2			Technishe Universitat Dresden, Dresden, Germany	cond-mat/0105429(2001)	A.Gladun,A.Handstein,D.Lipp,G.Fuchs,H.Rosner,K-H.Muller,M.Richter,M.Schneider,P.Zahn,S-L.Drechsler		
109415	PR05216165	gamma in mj/mol.K2	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		14.25					14.25																				T		9.2																										4.2								mj/mol.K2	18.2		490																																					induction melting + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109416	PR05216165	gamma in mj/mol.K2	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		16.1					16.1																				T		5.5																										4.4								mj/mol.K2	19.5		360																																					induction melting + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109417	PR05216165	gamma in mj/mol.K2. Not s/c	LaNi2B2C	La1Ni2B2C1	La	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K					5																																																										mj/mol.K2	8.4		495																																					induction melting + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109418	PR05216165	gamma in mj/mol.K2.	La(Pt,Au)2B2C	La1Pt1.5Au0.5B2C1	La	1	Pt	1.5	Au	0.5	B	2	C	1															1995																												LuNi2B2C																		K		10.65					10.65																				T		1.1																										4.2								mj/mol.K2	6.4		250																																					induction melting + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109419	PR05216165	gamma in mj/mol.K2. Not s/c	La(Pt,Au)2B2C	La1Pt1.7Au0.3B2C1	La	1	Pt	1.7	Au	0.3	B	2	C	1															1995																												LuNi2B2C																		K					5																																																										mj/mol.K2	7.5		220																																					induction melting + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109420	MAT0102167	density=2.26 g/cm3. Vickers hardness=1700-2800. Jc(20K,1T)=4E+4 A/cm2	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39											mT		32							T		18							T/K		0.74			MHC9420																																																														high-pressure synthesis (3.5GPa, 775C)					Superconducting properties of MgB2 bulk materials prepared by high pressure sintering			National Research Institute for Metals, Tsukuba-si, Ibaraki,Japan	cond-mat/0102167(2001)	H.Fujii,H.Ihara,H.Kito,H.Kumakura,H.Takeya,T.Hatano,T.Togano,Y.Takano		
109421	P063220507	pressure induced s/c. critical pressure=1.6 Gpa. S/c data at p=2.1 Gpa. Gap by NMR	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																			2001																												HoCoGa5																		K		2.2			0		2.2	MTC9421																																															5																																																					Pressure-induced anomalous magnetism and unconventional superconductivity in CeRhIn5: 115In-NQR study under pressure			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 63(2001)220507	D.Aoki,G.-q.Zheng,K.Ishida,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
109422	PRL0865582	0.2% Mg impurity phase. STM using Au-tip. Gapene=1.24 estimated from gap=2.0 meV at 2.5 K.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		37.5					37.5																																																1.24																																																					Tunneling Spectroscopy in Small Grains of Superconducting MgB2			Instituto Universitario de Ciencia de Materiales , Universidad Automa de Madrid, E-28049 Madrid, Spain	Phys.Rev.Lett., 86(2001)5582	G.Rubio-Bollinger,H.Suderow,S.Vieira		
109423	P063220504	point contact using Au-tip. Gap(delta)=4.3-4.6 meV.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39																																																2.56																																																(Mg rod+B<11> powder)-(850C, in 50 bar Ar)					Energy gap from tunneling and metallic contacts onto MgB2: Possible evidence for a weakened surface layer			Materials Sciences Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B, 63(2001)220504	D.G.Hinks,H.Schmidt,J.F.Zasadzinski,K.E.Gray		
109424	P064012507	weak trace of MgO. dTc/dP in K/GPa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.084		3.523											AlB2, C32	K		38.5					38.5			K/GPa	-1.6																																																																																																	High-pressure study on MgB2			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204-5932	Phys.Rev.B, 64(2001)012507	B.Lorenz,C.W.Chu,R.L.Meng		
109425	P063220505	bulk modulus=151 Gpa. Space group=P6/mmm	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0859		3.5212											AlB2, C32	K		38.2					38.2																																																																																																commercial powder					Compressibility and electronic structure of MgB2 up to 8 Gpa			Department of Physics, Brookhaven National Laboratory, Upton, New York 11973-5000	Phys.Rev.B, 63(2001)220505	G.Schneider,G.Yang,J.A.Hriljac,J.S.Abell,T.Vogt		
109426	PHB2590666	specific heat shows two Tc. Tc represent the upper Tc.	UPt3	Pt3U1	Pt	3	U	1																					1999																																														K		0.57					0.57																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
109427	PHB2590666	specific heat shows two Tc. Tc represent the upper Tc.	U(Pt,Pd)3	U1Pt2.997Pd0.003	U	1	Pt	2.997	Pd	0.003																			1999																																														K		0.51					0.51																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
109428	PHB2590666	specific heat shows two Tc. Tc represent the upper Tc.	U(Pt,Pd)3	U1Pt2.994Pd0.006	U	1	Pt	2.994	Pd	0.006																			1999																																														K		0.42					0.42																																																																																																					Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
109429	PHB2590666	specific heat shows two Tc. Tc represent the upper Tc.	U(Pt,Pd)3	U1Pt2.991Pd0.009	U	1	Pt	2.991	Pd	0.009																			1999																																														K		0.34					0.34	MTC9429																																																																																																				Studies of superconductivity in U(Pt1-xPdx)3 for x<0.006	199901		Department of Physics, Boston College, Chestnut Hill, MA 02167, USA	Physica B,259(1999)666-667	A. de Visser,A.de Visser,J.J.M. Franse,J.J.M.Franse,M.J. Graf,M.J.Graf,R.J. Keizer,R.J.Keizer		
109450	PR06212477	thermal expansion coefficient	(U,Th)Be13	U0.978Th0.022Be13	U	0.978	Th	0.022	Be	13																			2000																																														K		0.52					0.52																																		MHC9450																																																																			Thermal expansion studies of superconducting U1-xThxBe13 (0<=x<=0.052): Implications for the interpretation of the T-x phase diagram	200010		Max Planck Institute of Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B,62(2000)12477-12488	C.Langhammer,F.Kromer,F.Steglich,G.R.Stewart,J.S.Kim,M.Lang,MN.Oeschler,P.Hinze		
109451	PR06212477	thermal expansion coefficient	(U,Th)Be13	U0.97Th0.03Be13	U	0.97	Th	0.03	Be	13																			2000																																														K		0.6					0.6																																		MHC9451																																																																			Thermal expansion studies of superconducting U1-xThxBe13 (0<=x<=0.052): Implications for the interpretation of the T-x phase diagram	200010		Max Planck Institute of Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B,62(2000)12477-12488	C.Langhammer,F.Kromer,F.Steglich,G.R.Stewart,J.S.Kim,M.Lang,MN.Oeschler,P.Hinze		
109452	PR06212477	thermal expansion coefficient	(U,Th)Be13	U0.962Th0.038Be13	U	0.962	Th	0.038	Be	13																			2000																																														K		0.56					0.56																																		MHC9452																																																																			Thermal expansion studies of superconducting U1-xThxBe13 (0<=x<=0.052): Implications for the interpretation of the T-x phase diagram	200010		Max Planck Institute of Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B,62(2000)12477-12488	C.Langhammer,F.Kromer,F.Steglich,G.R.Stewart,J.S.Kim,M.Lang,MN.Oeschler,P.Hinze		
109453	PR06212477	thermal expansion coefficient	(U,Th)Be13	U0.957Th0.043Be13	U	0.957	Th	0.043	Be	13																			2000																																														K		0.53					0.53																																		MHC9453																																																																			Thermal expansion studies of superconducting U1-xThxBe13 (0<=x<=0.052): Implications for the interpretation of the T-x phase diagram	200010		Max Planck Institute of Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B,62(2000)12477-12488	C.Langhammer,F.Kromer,F.Steglich,G.R.Stewart,J.S.Kim,M.Lang,MN.Oeschler,P.Hinze		
109454	PR06212477	thermal expansion coefficient	(U,Th)Be13	U0.948Th0.052Be13	U	0.948	Th	0.052	Be	13																			2000																																														K		0.38					0.38																																		MHC9454																																																																			Thermal expansion studies of superconducting U1-xThxBe13 (0<=x<=0.052): Implications for the interpretation of the T-x phase diagram	200010		Max Planck Institute of Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B,62(2000)12477-12488	C.Langhammer,F.Kromer,F.Steglich,G.R.Stewart,J.S.Kim,M.Lang,MN.Oeschler,P.Hinze		
109455	NAT4100343		MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.0878		3.5204											AlB2, C32	K		39					39																																																																																																					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109456	NAT4100343		(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																			2001																												AlB2			A	3.0816		3.5163											AlB2, C32	K		36					36																																																																																																					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109457	NAT4100343	two phases(s/c phase(Tc=36K) + not s/c phase)	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2001																												AlB2			A	3.0735													AlB2, C32	K		36					36																																																																																																					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109458	NAT4100343	not s/c	(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																			2001																												AlB2			A	3.0551		3.3735											AlB2, C32	K					10																																																																																																							Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109459	P063224522	structure by NED. Thermal expansion coefficient = 5.4E-6 /K for a-axis, =11.4E-6 /K for c-axis.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.0849		3.5211											AlB2, C32	K		39					39																																																																																																					Lattice properties of MgB2 versus temperature and pressure			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B, 63(2001)224522	D.G.Hinks,J.D.Jorgensen,S.Short		
109460	P063220508	energy gap = 5-7 meV by STM.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.11		3.519											AlB2, C32	K		39					39											Oe		450																																			3.5	11																																															heat(950C in Ta tube)					Tunneling spectroscopy and magnetization measurements of the superconducting properties of MgB2			Racah Institute for Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B, 63(2001)220508	A.Sharoni,I.Felner,O.Millo		
109461	P063224510	Three CDW transitions at 42K, 36K, 23K. RRR=115. Tc(on)=0.78K, Tc(end)=0.22K. Hc2 means Hc because of type-I s/c.	alpha-U	U1	U	1																							2001																																														K		0.78					0.78																				mT		74																																		mj/mol.K2	9.13		256																																					electrotransport					Low-temperature specific heat and critical magnetic field of alpha-uranium single crystals			Department of Chemistry and Biochemistry, Brigham Young University, Provo, Utah 84602	Phys.Rev.B, 63(2001)224510	B.E.Lang,B.F.Woodfield,C.C.McPheeters,D.J.Thoma,E.C.Gay,G.M.Schmiedeshoff,J.Boerio-Goates,J.C.Cooley,J.C.Lashley,J.L.Smith,R.J.Hanrahan.Jr.,W.L.Hults		
109462	PR0124929	gamma in mJ/mol.K2	U	U1	U	1																						1	1975																																														K		0.27					0.27																																																								mj/mol.K2	9.59																																							polycrystal					Low-temperature heat capacity of alpha -uranium and its relation to the pressure dependence of Tc				Phys.Rev.B, 12(1975)4929	D.Bader,E.S.Fisher,N.E.Phillips		
109463	PR0124929	gamma in mJ/mol.K2	U	U1	U	1																						1	1975																																														K		0.2					0.2																																																								mj/mol.K2	9.86																																							polycrystal					Low-temperature heat capacity of alpha -uranium and its relation to the pressure dependence of Tc				Phys.Rev.B, 12(1975)4929	D.Bader,E.S.Fisher,N.E.Phillips		
109464	PR0124929	gamma in mJ/mol.K2	U	U1	U	1																						1	1975																																														K		0.27					0.27																																																								mj/mol.K2	9.82																																							large-grained					Low-temperature heat capacity of alpha -uranium and its relation to the pressure dependence of Tc				Phys.Rev.B, 12(1975)4929	D.Bader,E.S.Fisher,N.E.Phillips		
109465	PR0124929	gamma in mJ/mol.K2	U	U1	U	1																						3	1975																																														K					0.1																																																										mj/mol.K2	9.14																																							single crystal. Not s/c					Low-temperature heat capacity of alpha -uranium and its relation to the pressure dependence of Tc				Phys.Rev.B, 12(1975)4929	D.Bader,E.S.Fisher,N.E.Phillips		
109466	ASD0010151		(Na,Rb,Cs)3C60	Na2Rb0.5Cs0.5C60	Na	2	Rb	0.5	Cs	0.5	C	60																	1993																												fullerene			A	14.148														K		8					8																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109467	ASD0010151		Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1993																												fullerene			A	14.132														K		10.5					10.5																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109468	ASD0010151		Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1993																												fullerene			A	14.176														K		14					14																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109469	ASD0010151		K3C60	C60K3	C	60	K	3																					1993																												fullerene			A	14.253														K		19.3					19.3																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109470	ASD0010151		K2RbC60	K2Rb1C60	K	2	Rb	1	C	60																			1993																												fullerene			A	14.299														K		21.8					21.8																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109471	ASD0010151		Rb2KC60	Rb2K1C60	Rb	2	K	1	C	60																			1993																												fullerene			A	14.336														K		24.4					24.4																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109472	ASD0010151		Rb2KC60	Rb2K1C60	Rb	2	K	1	C	60																			1993																												fullerene			A	14.364														K		26.4					26.4																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109473	ASD0010151		Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene			A	14.436														K		29.4					29.4																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109474	ASD0010151		Rb2CsC60	Rb2Cs1C60	Rb	2	Cs	1	C	60																			1993																												fullerene			A	14.493														K		31.3					31.3																																																																																																					Synthesis and characterization of alkali metal fullerides: AxC60			AT&T Bell Lab, Murray Hill, NJ, USA	The Fullerences' Pergamon Press, 1993, p151	A.P.Ramirez,D.W.Murphy,G.Dabbagh,J.C.Tully,M.J.Rosseinsky,R.C.Haddon,R.E.Walstedt,R.M.Fleming,R.Tycko,T.Siegrist		
109475	PRL0681228	compressibility d(lna)/dp=1.52 E-2/Gpa. G-L parameter = 124	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene			A	14.425														K		29.6					29.6			K/GPa	-9.7							mT		12							T		78							T/K		3.9			MHC9475		nm		2			nm		247																																																										Pressure and field dependence of superconductivity in Rb3C60					F.Diederich,G.Gruner,G.Spam,J.D.Thompson,K.Holczer,R.B.Kaner,R.L.Whetten,S.-M.Huang		
109476	PRL0681228	compressibility d(lna)/dp=1.20 E-2/Gpa. G-L parameter = 92	K3C60	C60K3	C	60	K	3																					1992																												fullerene			A	14.24														K		19.3					19.3			K/GPa	-7.8							mT		13							T		49														nm		2.6			nm		240																																																										Pressure and field dependence of superconductivity in Rb3C60					F.Diederich,G.Gruner,G.Spam,J.D.Thompson,K.Holczer,R.B.Kaner,R.L.Whetten,S.-M.Huang		
109477	PR05003466	structure=simple cubic, space group=Pa3(upper bar).  S/c volume fraction=59%. dTc/dP in K/GPa.	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1994																																													cubic	K		12					12			K/GPa	-12.5																																																																																												react(C60,Na,Cs) in Ta-cell sealed glass					Pressure dependence of superconductivity in simple-cubic Na2CsC60	199408			Phys.Rev.B, 50(1994)3466	H.Takahashi,I.Hirosawa,J.Mizuki,K.Prassides,K.Tanigaki,M.Takai,N.Mori	Na,Cs,C	
109478	PR05003466		Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		29.5					29.5																																																																																																					Pressure dependence of superconductivity in simple-cubic Na2CsC60	199408			Phys.Rev.B, 50(1994)3466	H.Takahashi,I.Hirosawa,J.Mizuki,K.Prassides,K.Tanigaki,M.Takai,N.Mori	Na,Cs,C	
109479	PHC3410739	MX2 structure. dTc dP in K/GPa.	CuSe2	Cu1Se2	Cu	1	Se	2																					2000																												FeS2(pyrite)																		K		2.5					2.5			K/GPa	-0.2																																																																																												sintered (1000C,1h,p=5GPa)-anneal(400C)					Superconducting Properties of CuS2-xSex under High Pressure			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba 305-0047 Japan	Physica C, 341(2000)739	A.Ishii,K.Togano,N.Mori,N.Uchiyama,S.Arisawa,S.Ogawa,T.Hatano,Y.Kimishima,Y.Takano		
109480	PHC3410739	MX2 structure	Cu(S,Se)2	Cu1S1.8Se0.2	Cu	1	S	1.8	Se	0.2																			2000																												FeS2(pyrite)																		K		2.2					2.2																																																																																																sintered (1000C,1h,p=5GPa)-anneal(400C)					Superconducting Properties of CuS2-xSex under High Pressure			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba 305-0047 Japan	Physica C, 341(2000)739	A.Ishii,K.Togano,N.Mori,N.Uchiyama,S.Arisawa,S.Ogawa,T.Hatano,Y.Kimishima,Y.Takano		
109481	PHC3410739	MX2 structure	CuS2	Cu1Se2	Cu	1	Se	2																					2000																												FeS2(pyrite)																		K		1.6					1.6																																																																																																sintered (1000C,1h,p=5GPa)-anneal(400C)					Superconducting Properties of CuS2-xSex under High Pressure			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba 305-0047 Japan	Physica C, 341(2000)739	A.Ishii,K.Togano,N.Mori,N.Uchiyama,S.Arisawa,S.Ogawa,T.Hatano,Y.Kimishima,Y.Takano		
109482	PHC3410735		(Cu,Zn)Ir2S4	Cu0.78Zn0.22Ir2S4	Cu	0.78	Zn	0.22	Ir	2	S	4																	2000																												spinel																		K		3.3					3.3																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109483	PHC3410735		(Cu,Zn)Ir2S4	Cu0.75Zn0.25Ir2S4	Cu	0.75	Zn	0.25	Ir	2	S	4																	2000																												spinel																		K		3.3					3.3																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109484	PHC3410735	Hc1(2.0K)=250 Oe. Hc2(2.0K)=20 kOe. Delta-C(at Tc)=44 mj/mol.K. (delta-C/gamma*Tc)=1.1	(Cu,Zn)Ir2S4	Cu0.7Zn0.3Ir2S4	Cu	0.7	Zn	0.3	Ir	2	S	4																	2000																												spinel																		K		3					3																				T		3.5																																		mj/mol.K2	13		287																																										Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109485	PHC3410735		(Cu,Zn)Ir2S4	Cu0.65Zn0.35Ir2S4	Cu	0.65	Zn	0.35	Ir	2	S	4																	2000																												spinel																		K		2.8					2.8																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109486	PHC3410735		(Cu,Zn)Ir2S4	Cu0.6Zn0.4Ir2S4	Cu	0.6	Zn	0.4	Ir	2	S	4																	2000																												spinel																		K		2.6					2.6																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109487	PHC3410735		(Cu,Zn)Ir2S4	Cu0.55Zn0.45Ir2S4	Cu	0.55	Zn	0.45	Ir	2	S	4																	2000																												spinel																		K		2.41					2.41																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109488	PHC3410735		(Cu,Zn)Ir2S4	Cu0.5Zn0.5Ir2S4	Cu	0.5	Zn	0.5	Ir	2	S	4																	2000																												spinel																		K		2.2					2.2																																																																																																					Superconductivity in Zn-doped CuIr2S4			National Research Institute for Metals, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 341(2000)735	G.Cao,H.Kitazawa,H.Suzuki,K.Hirata,T.Furubayashi,T.Matsumoto		
109489	PHC3530011	two phase(MgB2 + BeB2)	(Mg,Be)B2	Mg0.7Be0.3B2	Mg	0.7	Be	0.3	B	2																			2001																												AlB2																	AlB2, C32	K		39					39																																																																																																(950C,2h) in Ta tube sealed in quartz.					Absence of superconductivity in BeB2			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Physica C, 353(2001)11	I.Felner		
109490	PHC3530011	moment=0.048 Bohr magneton. Kai(zero)=1.4 E-7 emu/mol.Oe	BeB2	B2Be1	B	2	Be	1																					2001							0																					AlB2			A	9.749		9.52											AlB2, C32	K					5																																																																																																		arc-melting					Absence of superconductivity in BeB2			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Physica C, 353(2001)11	I.Felner		
109491	PLA1640355	C<13> 60% substitution. Alpha=2.0-2.25	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		28.6					28.6						2	C																																																																																														Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
109492	PLA1640355	C<13> 60% substitution. Alpha=1.2 - 1.43	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		20					20						1.2	C																																																																																														Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
109493	PR0465880		K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		18					18																				T		28							T/K		2			MHC9493		A		34																																																															UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
109494	PR0465880		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		30					30																				T		38							T/K		2			MHC9494		A		30																																																															UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
109495	PR0465876	Hc2 follows linear relation, not WHH theory.	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		18.7					18.7																				T		38							T/K		2.14					A		29																																																															EVIDENCE OF UPPER-CRITICAL-FIELD ENHAMCEMENT IN K3C60 POWDERS	199209		AT&T BELL LABORATORIES, NEW JERSEY	PHYS.REN.B,46(1992)5876	A.PASSNER,D.W.MURPHY,G.S.BOEBINGER,I.I.MAZIN,M.J.ROSSEINSKY,T.T.PALSTRA	K,C	
109496	SSC0870375	Maybe, NaxNyC60 (x = 3-4, y = unknown). N is detected in the sample. Na-doped fullerene prepared by thermal decomposition of NaN3.	Na3N1C60	Na3N1C60	Na	3	N	1	C	60																			1993																												fullerene			A	14.204														K		14.7					14.7																																																																																																					NEW SUPERCONDUCTING SODIUM-NITROGEN-C60 THRNARY COMPOUND				SOLID STATE COMMUN.,87(1993)375	H.INOKUCHI,H.KITAGAWA,I.I.KHAIRULLIN,K.IMAEDA,K.YAKUSHI,M.NAGATA,N.MIZUTANI	C,NA,N	
109497	SSC0850073	gamma in micro-J/g.K2. 80%C60+18%C70+2%solvent. Debye-T estimated from specific heat below 9K. Two anomalies(90K, 250K) in specific heat.	C60	C60	C	60																							1993																												fullerene																		K																																																															mj/mol.K2	893		188																																										SPECIFIC HEAT OF FULLERENES EXTRACT	199301			SOLID STATE COMMUN.,85(1993)73	A.DEMAIN,B.NYSTEN,E.GRIVEI,J-P.ISSI,M.CASSART	C,	
109498	PHC2280175	BCS coherence length=44A. Hc2 from analyzing R(H) curve using fluctuation theory.	Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		30					30																				T		62							T/K		3.28					A		24			A		3200																																																										Magnetotransport in single-crystal Rb3C60	199407			Physica C, 228(1994)175-180	A.Zettl,J.G.Hou,Marvin L.Cohen,Vincent H.Crespi,X.-D.Xiang	Rb,C	
109499	SSC0930327		Cs3C60	C60Cs3	C	60	Cs	3																					1995																												fullerene																		K		18					18																																																																																																					SUPERCONDUCTIVITY AT 40K IN CECIUM DOPED C60				Solid State Commun.,93(1995)327-330	B.R. Zegarski,O. Zhou,P.E. Sulewski,R.M. Fleming,T.T.M. Palstra,Y. Iwasa	C, CS	
109500	NAT3750126	space group=Pcab. Yb occupy off-centered interstitial sites.	Yb3C60	C60Yb2.75	C	60	Yb	2.75																					1995																															A	27.874	27.98	27.873												K		5.4					5.4																																																																																																					Superconductivity and cation-vacancy ordering in the rare-earth fulleride Yb2.75C60	5		AT&T Bell Laboratories, Murray Hill, new Jersey 07974, USA	Nature 375(1995)126	A.P. Ramirez,A.R. Kortan,E. Ozdas,H.E. Bair,K.M. Rabe,N. Kopylov,P.H. Cltrin,S. Schuppler,T. Siegrist		
109501	PR04614936	Hc2 using rf technique in pulsed field. Spin orbit parameter=1	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		19.5					19.5																				T		32.7							T/K		2.8					A		31																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
109502	PR04614936	Hc2 using rf technique in pulsed field. Spin orbit parameter=0.7	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		28.4					28.4																				T		57.4							T/K		3.86					A		24																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
109503	LTP1220591	s/c properties were measured at p=27 kbar. RRR=45. dHc2/dT and coherence length are : =12.7 T/K, 300A for H//a and =16 T/K, 230 A for H//c. dTc/dP in K/GPa.	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																		3	2001								10.5																				ThCr2Si2																		K		0.395					0.395			K/GPa	2.8																									T/K		16			MHC9503		A		230																																																															Superconductivity, upper critical field and anomalous normal state in CePd2Si2 near the quantum critical point			Grenoble Cedex, France	J.Low Temp. Phys., 122(2001)591	D.Braithwaite,D.Jaccard,E.Steep,I.Sheikin,J.-P.Brison,J.Flouquet,S.Raymond		
109504	PR0315756	reentrant Tc2=4.07 K. FM order at Curie Temp.	(Er,Ho)Rh4B4	Er0.25Ho0.75Rh4B4	Er	0.25	Ho	0.75	Rh	4	B	4																	1985							4.75																			AB4C4		RT4B4																	LuRh4B4 type	K		6.44					6.44	MTC9504																																																																																																				Magnetic and superconducting properties of holmium-rich (Er1-xHox)Rh4B4				Phys.Rev.B, 31(1985)5756	C.J.Glinka,H.E.Horng,J.A.Gotaas,J.W.Lynn,R.N.Shelton		
109506	PR0315756	reentrant Tc2=4.95 K. FM order at Curie Temp.	(Er,Ho)Rh4B4	Er0.16Ho0.84Rh4B4	Er	0.16	Ho	0.84	Rh	4	B	4																	1985							5.33																			AB4C4		RT4B4																	LuRh4B4 type	K		5.95					5.95																																																																																																					Magnetic and superconducting properties of holmium-rich (Er1-xHox)Rh4B4				Phys.Rev.B, 31(1985)5756	C.J.Glinka,H.E.Horng,J.A.Gotaas,J.W.Lynn,R.N.Shelton		
109507	PR0315756	reentrant Tc2=5.33 K. FM order at Curie Temp.	(Er,Ho)Rh4B4	Er0.11Ho0.89Rh4B4	Er	0.11	Ho	0.89	Rh	4	B	4																	1985							5.56																			AB4C4		RT4B4																	LuRh4B4 type	K		5.71					5.71																																																																																																					Magnetic and superconducting properties of holmium-rich (Er1-xHox)Rh4B4				Phys.Rev.B, 31(1985)5756	C.J.Glinka,H.E.Horng,J.A.Gotaas,J.W.Lynn,R.N.Shelton		
109508	PR0315756	reentrant Tc2=4.07 K. FM order at Curie Temp.	(Er,Ho)Rh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1985							6.47																			AB4C4		RT4B4																	LuRh4B4 type	K																																																																																																												Magnetic and superconducting properties of holmium-rich (Er1-xHox)Rh4B4				Phys.Rev.B, 31(1985)5756	C.J.Glinka,H.E.Horng,J.A.Gotaas,J.W.Lynn,R.N.Shelton		
109509	SSC0270761	FM order at Curie Temp.	GdMo6S8	Gd1.2Mo6S8	Gd	1.2	Mo	6	S	8																			1978							0.95																					Chevrel																		K		1.4					1.4																																																																																																1100C in quartz tube + (1250C, 10h)					Low temperature magnetization measurements on heavy rare earth molybdenum sulfides, (RE)1.2Mo6S8				Solid State Commun., 27(1978)761	J.Muller,M.Ishikawa		
109510	SSC0270761	FM order at Curie Temp.	TbMo6S8	Tb1.2Mo6S8	Tb	1.2	Mo	6	S	8																			1978							1.05																					Chevrel																		K		1.8					1.8																																																																																																1100C in quartz tube + (1250C, 10h)					Low temperature magnetization measurements on heavy rare earth molybdenum sulfides, (RE)1.2Mo6S8				Solid State Commun., 27(1978)761	J.Muller,M.Ishikawa		
109511	SSC0270761	FM order at Curie Temp.	DyMo6S8	Dy1.2Mo6S8	Dy	1.2	Mo	6	S	8																			1978							0.45																					Chevrel																		K		2.15					2.15																																																																																																1100C in quartz tube + (1250C, 10h)					Low temperature magnetization measurements on heavy rare earth molybdenum sulfides, (RE)1.2Mo6S8				Solid State Commun., 27(1978)761	J.Muller,M.Ishikawa		
109512	SSC0270761	FM order at Curie Temp.	HoMo6S8	Ho1.2Mo6S8	Ho	1.2	Mo	6	S	8																			1978							0.75																					Chevrel																		K		2.15					2.15																																																																																																1100C in quartz tube + (1250C, 10h)					Low temperature magnetization measurements on heavy rare earth molybdenum sulfides, (RE)1.2Mo6S8				Solid State Commun., 27(1978)761	J.Muller,M.Ishikawa		
109513	SSC0270761	FM order at Curie Temp.	ErMo6S8	Er1.2Mo6S8	Er	1.2	Mo	6	S	8																			1978							0.22																					Chevrel																		K		2.2					2.2																																																																																																1100C in quartz tube + (1250C, 10h)					Low temperature magnetization measurements on heavy rare earth molybdenum sulfides, (RE)1.2Mo6S8				Solid State Commun., 27(1978)761	J.Muller,M.Ishikawa		
109514	SSC0170721	density=5.62 g/cm3.	LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1975																												Chevrel			A	9.12		11.48												K		6.95					6.95																				T		6.5																																																																										mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109515	SSC0170721	density=5.80 g/cm3.	CeMo6S8	Ce1Mo6S8	Ce	1	Mo	6	S	8																			1975							-23																					Chevrel			A	9.1		11.45												K					1.1																																																																																																		mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109516	SSC0170721	density=5.80 g/cm3.	PrMo6S8	Pr1Mo6S8	Pr	1	Mo	6	S	8																			1975							-20																					Chevrel			A	9.1		11.44												K		2.55					2.55																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109517	SSC0170721	density=5.86 g/cm3.	NdMo6S8	Nd1Mo6S8	Nd	1	Mo	6	S	8																			1975							-30																					Chevrel			A	9.1		11.42												K		3.5					3.5																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109518	SSC0170721	density=5.92 g/cm3.	SmMo6S8	Sm1.2Mo6S8	Sm	1.2	Mo	6	S	8																			1975																												Chevrel			A	9.09		11.37												K		2.4					2.4																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109519	SSC0170721	density=5.77 g/cm3.	EuMo6S8	Eu1.2Mo6S8	Eu	1.2	Mo	6	S	8																			1975																												Chevrel			A	9.17		11.54												K					1.1																																																																																																		mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109520	SSC0170721	density=5.74 g/cm3.	EuMo6S8	Eu1Mo6.35S8	Eu	1	Mo	6.35	S	8																			1975							1																					Chevrel			A	9.18		11.45												K					1.1																																																																																																		mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109521	SSC0170721	density=5.96 g/cm3.	GdMo6S8	Gd1.2Mo6S8	Gd	1.2	Mo	6	S	8																			1975							-4																					Chevrel			A	9.1		11.35												K		1.4					1.4																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109522	SSC0170721	density=6.06 g/cm3.	TbMo6S8	Tb1.2Mo6S8	Tb	1.2	Mo	6	S	8																			1975							-6																					Chevrel			A	9.09		11.3												K		1.4					1.4																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109523	SSC0170721	density=6.02 g/cm3.	DyMo6S8	Dy1.2Mo6S8	Dy	1.2	Mo	6	S	8																			1975							-10																					Chevrel			A	9.09		11.27												K		1.7					1.7																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109524	SSC0170721	density=6.17 g/cm3.	HoMo6S8	Ho1.2Mo6S8	Ho	1.2	Mo	6	S	8																			1975							-10																					Chevrel			A	9.08		11.26												K		1.25					1.25																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109525	SSC0170721	density=6.20 g/cm3.	ErMo6S8	Er1.2Mo6S8	Er	1.2	Mo	6	S	8																			1975							-6																					Chevrel			A	9.09		11.23												K					1.1																																																																																																		mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109526	SSC0170721	density=6.18 g/cm3.	TmMo6S8	Tm1.2Mo6S8	Tm	1.2	Mo	6	S	8																			1975							-15																					Chevrel			A	9.1		11.2												K		1.95					1.95																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109527	SSC0170721	density=6.06 g/cm3.	YbMo6S8	Yb1.2Mo6S8	Yb	1.2	Mo	6	S	8																			1975							-60																					Chevrel			A	9.14		11.36												K		8.6					8.6																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109528	SSC0170721	density=6.33 g/cm3.	LuMo6S8	Lu1.2Mo6S8	Lu	1.2	Mo	6	S	8																			1975																												Chevrel			A	9.08		11.15												K		1.95					1.95																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109529	SSC0170721	density=6.65 g/cm3.	YMo6S8	Y1.2Mo6S8	Y	1.2	Mo	6	S	8																			1975																												Chevrel			A	9.08		11.25												K		2.1					2.1																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109530	SSC0170721	density=5.96 g/cm3.	YbMo6S8	Yb1Mo6S8	Yb	1	Mo	6	S	8																			1975							-65																					Chevrel			A	9.16		11.35												K		8.45					8.45																																																																																																mixture-heat(950C+1250C+800C)					Superconductivity in the RExMo6S8				Solid State Commun., 17(1975)721	A.Treyvaud,M.Sergent,R.Chevrel,fF.Fischer		
109531	PR0344566		YPd2Si2	Y1Pd2Si2	Y	1	Pd	2	Si	2																		1	1986																												ThCr2Si2			A	4.129		9.84												K		0.47					0.47																				mT		5.4																																																																										exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109532	PR0344566		LaPd2Si2	La1Pd2Si2	La	1	Pd	2	Si	2																		1	1986																												ThCr2Si2			A	4.283		9.88												K		0.39					0.39																				mT		3.1																																																																										exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109533	PR0344566	gamma in mj/mol.K2(calculated from 78 J/m3.K2)	LuPd2Si2	Lu1Pd2Si2	Lu	1	Pd	2	Si	2																		1	1986																												ThCr2Si2			A	4.089		9.85												K		0.67					0.67																				mT		7																																		mj/mol.K2	7.72																																							exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109534	PR0344566		YRh2Si2	Y1Rh2Si2	Y	1	Rh	2	Si	2																		1	1986																												ThCr2Si2			A	4.031		9.92												K					0.33																																																																																																		exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109535	PR0344566		LaRh2Si2	La1Rh2Si2	La	1	Rh	2	Si	2																		1	1986																												ThCr2Si2			A	4.112		10.29												K		0.074					0.074																																																																																																exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109536	PR0344566		LuRh2Si2	Lu1Rh2Si2	Lu	1	Rh	2	Si	2																		1	1986																												ThCr2Si2			A	4.09		10.18												K					0.33																																																																																																		exothermic reaction					Superconductivity in the ternary rare-earth (Y,La, and Lu) compounds RPd2Si2 and RRh2Si2				Phys. Rev.B, 34(1986)4566	A.A.Menovsky,G.J.Nieuwenhuys,G.Lu,J.A.Mydosh,P.H.Kes,T.T.M.Palstra		
109537	PRL0542375	pressure-induced s/c. Tc=8.2K at p=15 Gpa. p-type Si(acceptor=E+16/cm3). Phases: diamond(Si-I) for P < 12 GPa, beta-Sn(Si-II) for 11 < P < 17 GPa, simple hexagonal(Si-IV)  for p > 13 Gpa	Si	Si1	Si	1																							1985																																													hexagonal	K		8.2			0		8.2	MTC9537		K/GPa	-0.4																																																																																																	Superconductivity in high-pressure metallic phases of Si			Department of Physics, University of California, and Materials and Molecular Research Division, Lawrence Berkeley Laborator,  Berkeley, California 94720	Phys.Rev.Lett., 54(1985)2375	G.Chouteau,G.Martinez,J.M.Mignot,K.J.Chang,M.L.Cohen,Michel M.Dacorogna		
109538	PR06103800	this phase has Tc(max)=6K at p=10 Gpa.	CaSi2	Ca1Si2	Ca	1	Si	2																					2000																												alpha-ThSi2																		K		1.51					1.51	MTC109538																																																																																															(trigonal-CaSi2) - ANN(800C, 8GPa)					Superconducting high pressure CaSi2 phase with Tc up to 14 K	200002		Centre de Recherches sur les Tres Basses Temperatures, CNRS, Boite Postale 166, Cedex 09, 38042 Grenoble, France	Phys.Rev.B,61(2000)R3800-R3803	A.Palenzona,G.L.Olcese,H.Elsinger,M.Affronte,M.Nunez-Regueiro,O.Laborde,S.LeFloch,S.Sanfilippo		
109539	PR06103800	P-induced SC. Pcrit = 12 GPa. TCFIG shows Tc(P).  trigonal-CaSi2 sample transformed to AlB2 structure under pressure p>15 Gpa. Debye-T = 300K for P>12 GPa.	CaSi2	Ca1Si2	Ca	1	Si	2																					2000																												AlB2			A	10.4													alpha = 21deg 30'	K		14			0		14	MTC109539		K/GPa		22																																																						456	resistivity																																				melting in Ta-crucible. then ANN(900C,7d)					Superconducting high pressure CaSi2 phase with Tc up to 14 K	200002		Centre de Recherches sur les Tres Basses Temperatures, CNRS, Boite Postale 166, Cedex 09, 38042 Grenoble, France	Phys.Rev.B,61(2000)R3800-R3803	A.Palenzona,G.L.Olcese,H.Elsinger,M.Affronte,M.Nunez-Regueiro,O.Laborde,S.LeFloch,S.Sanfilippo		
109540	L087077003	transition width = 0.2K. Hc2(0) estimated from Hc2(1.9K)=1T using WHH theory. Hc1(1.9K)=20 Oe.	Sr(Ga,Si)2	Sr1Ga0.74Si1.26	Sr	1	Ga	0.74	Si	1.26																			2001																												AlB2			A	4.1427		4.7998											AlB2, C32	K		3.5					3.5											Oe		20							T		1.53																																																																										arc-melting + floating zone with infrared heating					Superconductivity of Ternary Silicide with the AlB2-Type Structure Sr(Ga0.37, Si0.63)2			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.Lett., 87(2001)077003	E.Abe,H.Abe,H.Kitazawa,J.Ye,K.Honma,K.Nishida,M.Imai,T.Kimura		
109541	P064064514		Gd2Rh3Si5	Gd2Rh3Si5	Gd	2	Rh	3	Si	5																			2001							-15.3																					U2Co3Si5			A	9.86	11.81	5.77												K					4																																																													352																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109542	P064064514		Dy2Rh3Si5	Dy2Rh3Si5	Dy	2	Rh	3	Si	5																			2001							1.25	4																				U2Co3Si5			A	9.84	11.77	5.75												K					4																																																													403																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109543	P064064514		Er2Rh3Si5	Er2Rh3Si5	Er	2	Rh	3	Si	5																			2001							12.8	2.5																				U2Co3Si5			A	9.8	11.721	5.73												K					4																																																																																																		arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109544	P064064514		Ho2Rh3Si5	Ho2Rh3Si5	Ho	2	Rh	3	Si	5																			2001							0.77	3																				U2Co3Si5			A	9.82	11.75	5.74												K					4																																																													477																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109545	P064064514		Tm2Rh3Si5	Tm2Rh3Si5	Tm	2	Rh	3	Si	5																			2001							-5.98																					U2Co3Si5			A	9.78	11.68	5.72												K					4																																																													430																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109546	P064064514		Lu2Rh3Si5	Lu2Rh3Si5	Lu	2	Rh	3	Si	5																			2001																												U2Co3Si5			A	9.76	11.66	5.71												K					4																																																																																																		arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109547	P064064514		La2Rh3Si5	La2Rh3Si5	La	2	Rh	3	Si	5																			2001																												U2Co3Si5			A	10	11.96	5.88												K		4.4					4.4																																																											338																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109548	P064064514	no Curie-Weis behavior. Strongly hybridized Ce system.	Ce2Rh3Si5	Ce2Rh3Si5	Ce	2	Rh	3	Si	5																			2001																												U2Co3Si5			A	9.89	11.87	5.82												K					4																																																																																																		arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109549	P064064514		Pr2Rh3Si5	Pr2Rh3Si5	Pr	2	Rh	3	Si	5																			2001							-9.15																					U2Co3Si5			A	9.88	11.85	5.8												K					4																																																													335																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109550	P064064514		Nd2Rh3Si5	Nd2Rh3Si5	Nd	2	Rh	3	Si	5																			2001							-2.75	2.7																				U2Co3Si5			A	9.87	11.83	5.78												K					4																																																																																																		arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109551	P064064514		Tb2Rh3Si5	Tb2Rh3Si5	Tb	2	Rh	3	Si	5																			2001							-17.95	7.5																				U2Co3Si5			A	9.85	11.79	5.76												K					4																																																													558																																					arc-melting					Magnetism and crystal-field effects in the R2Rh3Si5  (R = La, Ce, Pr, Nd, Tb, Gd, Dy, Er, Ho, and Tm) system			Tata Institute Of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 64(2001)064514	Aravind D.Chinchure,N.G.Patil,S.Ramakrishnan,V.R.Marathe		
109552	P064060506	Tunneling using Au-tip. Fitting by BTK theory. Temperature dependence of gap is BCS-like.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39																																																2.8	1																																																				Symmetry and temperature dependence of the order parameter in MgB2 from point contact measurements			School of Physics and Astronomy, Raymond and Beverly Sackler Faculty of Exact Sciences, Tel Aviv University, 69978 Tel Aviv, Israel	Phys.Rev.B, 64(2001)060506	A.Kohen,G.Deutscher		
109553	MAT0107584	pressure induced s/c. s/c properties = at p=1.22GPa. P=1.06 Gpa<s/c<1.44 Gpa. Rho(RT)=0.26 microOhm.cm. RRR=600	UGe2	Ge2U1	Ge	2	U	1																				3	2001																																														K		0.72			0		0.72																													T/K		5.3			MHC9553																																																														Czochralski method					Pressure-induced superconductivity in a ferromagnet UGe2 -Resistivity measurements in magnetic field-			Research Center for Materials Science at Extreme Conditions, Osaka Univ., Toyonaka, Osaka, Japan	cond-mat/0107584(2001)	K.Amaya,K.Hanazono,N.Tateiwa,R.Settai,T.C.Kobayashi,Y.Haga,Y.Onuki		
109554	MAT0106166	penetration depth using tunnel diode oscillator. Gap calculated from penetration depth.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		39					39																																									nm		160					1.7																																																made from commercial powder					Exponential temperature dependence of penetration depth in MgB2			H.H.Wills Physics Lab, University of Bristol,England	cond-mat/0106166	A.Carrington,F.Manzano		
109555	MAT0108107	wire around W-wire. Penetration depth by LC resonator.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39																																																1.54																																																					Energy gap and proximity effect in MgB2 superconducting wires				cond-mat/0108107	P.C.Canfield,R.Prozorov,R.W.Giannetta,S.L.Bud'ko		
109556	MAT0106585	Tc measured upto 40 Gpa. dTc/dP shows sample dependency.  Bulk modulus = 150 Gpa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.5					39.5			K/GPa	-0.35																																																																																												powder-HIP(10 kbar, 1h, 700C)					Absence of a structural transition up to 40 Gpa in MgB2 and the relevance of magnesium non-stoichiometry			SNRS, Grenoble Cedex, France	cond-mat/0106585	K.A.Regan,M.A.Hayward,M.D.Nunez-Reguiro,M.Mezouar,M.Monteverde,M.Nunez-Regueiro,N.Rogado,P.Bordet,R.J.Cava,S.M.Loureiro,T.He		
109557	MAT0105475	ceramic density=2.23 g/cm3. Pressure using diamond anvil. Tc by ac-susceptibility. dTc/dP in K/GPa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.086		3.52											AlB2, C32	K		37.3					37.3			K/GPa	-2																																																																																												1400C in Mo crucible					Effect of pressure on the superconducting Tc of MgB2				cond-mat/0105475	M.P.Kulakov,M.V.Nefedova,N.N.Kolesnikov,V.G.Tissen		
109558	P064092505	bulk modulus = 147 Gpa. Hydrostatic (He-gas) pressure upto 0.7 Gpa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K										K/GPa	-1.11																																																																																												(B<11>+Mg)-capped BN crucible - (800C in air)					Dependence of Tc on hydrostatic pressure in superconducting MgB2			Department of Physics, Washington University, C. B. 1105, One Brookings Dr., St. Louis, Missouri 63130	Phys.Rev.B, 64(2001)092505	D.G.Hinks,J.D.Jorgensen,J.J.Hamlin,J.S.Schilling,T.Tomita		
109559	MAT0107205	compressibility k(a)=1.6 E-3 /Gpa. K(c)=2.2 E-3 /Gpa. Bulk modulus=196 Gpa. Pressure by diamond anvil.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.082		3.522											AlB2, C32	K		37.5					37.5			K/GPa	-1.13																																																																																												commercial powder					High pressure studies of Tc and lattice parameters of MgB2				cond-mat/0107205	K.Grube,S.I.Schlachter,W.Goldacker,W.H.Fietz		
109560	P064094514	in-plane penetration depth measured by transverse-field muon-SR. ramda shows T2 dependency.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		37.5					37.5																																									nm		85																																																					commercial powder					Penetration depth measurements in MgB2: Evidence for unconventional superconductivity			IRC , University of Cambridge, Cambridge, UK	Phys.Rev.B, 64(2001)094514	B.D.Rainford,C.A.Scott,C.Panagopoulos,I.H.Inoue,M.Kambara,T.Xiang		
109561	P064094522	density=2.2 g/cm3. Hc1 determined by delta-M=E-4 emu. Ramda calculated from Hc1 assuming G-L = 26.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39					39											Oe		176																												A		1700																																																					high pressure synthesis (6GPa,950C,0.5h)					Linear temperature dependence of lower critical field in MgB2			National Lab for Superconductivity, Institute of Physics and Center for Condenced Matter Physics, Beijing,China	Phys.Rev.B, 64(2001)094522	G.C.Che,H.H.Wen,H.P.Yang,S.L.Li,Y.M.Ni,Z.A.Ren,Z.W.Zhao,Z.X.Zhao,Z.Y.Liu		
109562	P064100503	not s/c	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2001								3.8																				HoCoGa5			A	4.6521		7.5416												K																																																																																																							using In flux					Coexistence of magnetism and superconductivity in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B, 64(2001)100503	C.Petrovic,D.Hall,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109563	P064100503	R=0 at T=1.01K	Ce(Rh,Ir)In5	Ce1Rh0.6Ir0.4In5	Ce	1	Rh	0.6	Ir	0.4	In	5																3	2001								3.5																				HoCoGa5			A	4.6594		7.535												K		0.62					0.62																																																																																																using In flux					Coexistence of magnetism and superconductivity in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B, 64(2001)100503	C.Petrovic,D.Hall,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109564	P064100503	R=0 at T=1.01K	Ce(Rh,Ir)In5	Ce1Rh0.5Ir0.5In5	Ce	1	Rh	0.5	Ir	0.5	In	5																3	2001								3.6																				HoCoGa5			A	4.6598		7.5368												K		0.84					0.84	MTC9564																																																																																															using In flux					Coexistence of magnetism and superconductivity in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B, 64(2001)100503	C.Petrovic,D.Hall,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109565	P064100503	R=0 at T=0.99K	Ce(Rh,Ir)In5	Ce1Rh0.25Ir0.75In5	Ce	1	Rh	0.25	Ir	0.75	In	5																3	2001																												HoCoGa5			A	4.6641		7.525												K		0.62					0.62																																																																																																using In flux					Coexistence of magnetism and superconductivity in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B, 64(2001)100503	C.Petrovic,D.Hall,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109566	P064100503	R=0 at T=1.1K	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001																												HoCoGa5			A	4.6682		7.5151												K		0.4					0.4																																																																																																using In flux					Coexistence of magnetism and superconductivity in CeRh1-xIrxIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545	Phys.Rev.B, 64(2001)100503	C.Petrovic,D.Hall,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,R.Movshovich,Z.Fisk		
109567	JPC0130337	Hc2 for H//c. CurieT=-83K for H//c-axis, =-54K for H//ab. Delta-C/gamma*Tc = 4.5	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2001							-83																					HoCoGa5																		K		2.3					2.3																				T				5																																																																								using In flux					Heavy-fermion superconductivity in CeCoIn5 at 2.3 K			National High Magnetic Field Lab, Florida State Univ., Tallahassee, FL, USA	J.Phys.:Condens.Matter, 13(2001)L337	C.Petrovic,J.D.Thompson,J.L.Sarrao,M.F.Hundley,P.G.Pagliuso,P.Monthoux,R.Movshovich		
109568	P064100505	gap(=2.1 meV) estimated by fitting of penetration depth. At low temperature, gap=1.2 meV. Penet by surface impedance measurements.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																4	2001																												LuNi2B2C																		K		14.2					14.2																																				nm		7			nm		275					3.4																																																dc magnetron sputtering on (100)MgO					Superconducting gap anisotropy of LuNi2B2C thin films from microwave surface impedance measurements				Phys.Rev.B, 64(2001)100505	A.Andreone,A.Cassinese,F.Palomba,L.Gianni,M.Iavarone,R.Vaglio		
109569	P064132505	starting (Mg1.2C1.4Ni3). RRR=2.5. Hall coeff.(100K)=-6.1 E-10 m3/C. carrier is electron.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2001																												CaTiO3			A	3.8115													CaTiO3, perovskite	K		8					8																				T		15												MHC9569		A		47																																																										pellet-heat(900C)					Normal state resistivity, upper critical field, and Hall effect in superconducting perovskite MgCNi3			Structural Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, People's Republic of China	Phys.Rev.B, 64(2001)132505	C.H.Wang,H.T.Zhang,K.Q.Ruan,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109570	P064132509	density=2.66 g/cm3. Bulk modulus=172 Gpa.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		39.6					39.6			K/GPa	-1.03																																																																																												high-pressure sintering					Lattice parameter and Tc dependence of sintered MgB2 superconductor on hydrostatic pressure			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Phys.Rev.B, 64(2001)132509	A.Matsushita,H.Ihara,H.Kito,J.Tang,K.Togano,Lu-Chang Qin,Y.Takano		
109571	P064134513		MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0851		3.5213											AlB2, C32	K		38.3					38.3																																																																																																(amouphous B + C, Mg)-(900C,2h)					Intralayer carbon substitution in the MgB2 superconductor			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-1292, Japan	Phys.Rev.B, 64(2001)134513	D.H.Chi,K.Prassides,T.Ito,T.Takenobu,Y.Iwasa		
109572	P064134513	dTc/dx = -57 K. -dln(Tc)/dV = 0.85 for MgB2-xCx.	Mg(B,C)2	Mg1B1.98C0.02	Mg	1	B	1.98	C	0.02																		1	2001																												AlB2			A	3.0804		3.5211											AlB2, C32	K		37.2					37.2																																																																																																(amouphous B + C, Mg)-(900C,2h)					Intralayer carbon substitution in the MgB2 superconductor			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-1292, Japan	Phys.Rev.B, 64(2001)134513	D.H.Chi,K.Prassides,T.Ito,T.Takenobu,Y.Iwasa		
109573	P064134513		Mg(B,C)2	Mg1B1.96C0.04	Mg	1	B	1.96	C	0.04																		1	2001																												AlB2			A	3.0767		3.5214											AlB2, C32	K		36.1					36.1																																																																																																(amouphous B + C, Mg)-(900C,2h)					Intralayer carbon substitution in the MgB2 superconductor			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-1292, Japan	Phys.Rev.B, 64(2001)134513	D.H.Chi,K.Prassides,T.Ito,T.Takenobu,Y.Iwasa		
109574	P064134513		Mg(B,C)2	Mg1B1.94C0.06	Mg	1	B	1.94	C	0.06																		1	2001																												AlB2			A	3.0706		3.5212											AlB2, C32	K		34.8					34.8																																																																																																(amouphous B + C, Mg)-(900C,2h)					Intralayer carbon substitution in the MgB2 superconductor			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-1292, Japan	Phys.Rev.B, 64(2001)134513	D.H.Chi,K.Prassides,T.Ito,T.Takenobu,Y.Iwasa		
109575	P064134513	inhomogeneous sample (0.07<x in Mg2B2-xCx). Tc very broad.	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																			2001																												AlB2			A	3.0686		3.5213											AlB2, C32	K		34					34																																																																																																					Intralayer carbon substitution in the MgB2 superconductor			Japan Advanced Institute of Science and Technology, Tatsunokuchi, Ishikawa 923-1292, Japan	Phys.Rev.B, 64(2001)134513	D.H.Chi,K.Prassides,T.Ito,T.Takenobu,Y.Iwasa		
109576	P064094520	G-L parameter=2.5. S/c parameters (0) are the values at 0.1K. Structure is rhombohedral (alpha=89.5 degree)	DyMo6S8	Dy1Mo6S8	Dy	1	Mo	6	S	8																		3	2001								0.4																				Chevrel			A	6.452														K		1.6					1.6																				Oe		900														A		600																																																										cool from 1880C at 5C/h in Mo ampoule					Interaction of the spin-flop phase and superconductivity in DyMo6S8 single crystals			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, 50-950 Wroclaw, Poland	Phys.Rev.B, 64(2001)094520	E.Tjukanoff,K.Rogacki,S.Jaakkola		
109577	NAT4110457	isotope effect=mean value for several Mg mass samples.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40					40						0.3	B																																																																																									mixture-heat(850C, 1.5h, p=50 bar Ar)					The complex nature of superconductivity in MgB2 as revealed by the reduced total isotope effect			Argonne, Illinois,USA	Nature, 411(2001)457	D.G.Hinks,H.Claus,J.D.Jorgensen		
109578	NAT4110457	For B<10> materials, Mg isotope effect is very small but non-zero.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		40					40						0.02	Mg																																																																																									mixture-heat(850C, 1.5h, p=50 bar Ar)					The complex nature of superconductivity in MgB2 as revealed by the reduced total isotope effect			Argonne, Illinois,USA	Nature, 411(2001)457	D.G.Hinks,H.Claus,J.D.Jorgensen		
109579	NAT4110561	Tc's are 37.5, 37.5, 35, 34.5 for displacement = 0, 0.04, 1, 5 % dpa (displacement per atom)	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		37.5					37.5																																		MHIR9579																																																														damage given by irradiation					Enhancement of the high-magnetic field critical current density of superconducting MgB2 by proton irradiation			Imperial College, London,UK	Nature, 411(2001)561	A.D.Caplin,G.K.Perkins,L.F.Cohen,M.Polichetti,R.Gwilliam,T.J.Tate,Y.Bugoslavsky		
109580	EPJ0210159	2*gap = 3 - 4 meV (2*gap/kTc =1.79 - 2.38). Gap measured by far-infrared reflectivity.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.086		3.524											AlB2, C32	K		39					39																																																2.38																																																sintered(900C, in Ar)					Optical measurements of the superconducting gap in MgB2			Universitat Stuttgart,Germany	Eur.Phys.J.B, 21(2001)159	A.B.Kuz'menko,B.Gorshunov,C.A.Kuntscher,D.van der Marel,F.P.Mena,J.Akimitsu,M.Dressel,P.Haas,T.Muranaka		
109581	NAT4120058	s/c for only high quality sample. R is not zero at 0.01 K. s/c and ferromag disappear at p=21 kbar. Sp.heat shows no gap at Tc. Moment=0.17 myu-B	ZrZn2	Zn2Zr1	Zn	2	Zr	1																					2001							28.5																					MgCu2(Laves)			A	7.393													MgCu2, C15	K		0.29					0.29																				T		0.4														A		290																																																															Coexistence of superconductivity and ferromagnetism in the d-band metal ZrZn2			Universitat Karlsruhe, Karlsruhe, Germany	Nature, 412(2001)58	C.Pfleiderer,G.G.Lonzarich,H.v.Lohneysen,M.Uhlarz,N.R.Bernhoeft,R.Vollmer,S.M.Hayden		
109582	NAT4100343		MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0865		3.5231											AlB2, C32	K		38					38																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109583	NAT4100343		(Mg,Al)B2	Mg0.97Al0.03B2	Mg	0.97	Al	0.03	B	2																		1	2001																												AlB2			A	3.0865		3.5173											AlB2, C32	K		37.3					37.3																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109584	NAT4100343		(Mg,Al)B2	Mg0.94Al0.06B2	Mg	0.94	Al	0.06	B	2																		1	2001																												AlB2			A	3.0865		3.5173											AlB2, C32	K		37					37																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109585	NAT4100343		(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																		1	2001																												AlB2			A	3.0827		3.5154											AlB2, C32	K		36					36																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109586	NAT4100343	two phases (c=3.500 and c=3.4365)	(Mg,Al)B2	Mg0.86Al0.14B2	Mg	0.86	Al	0.14	B	2																			2001																												AlB2			A	3.0808		3.5											AlB2, C32	K		35.1					35.1																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109587	NAT4100343	two phases (c=3.4827 and c=3.4269)	(Mg,Al)B2	Mg0.82Al0.18B2	Mg	0.82	Al	0.18	B	2																			2001																												AlB2			A	3.0769		3.4827											AlB2, C32	K		33.5					33.5																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109588	NAT4100343	two phases (c=3.4885 and c=3.4269)	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2001																												AlB2			A	3.0769		3.4885											AlB2, C32	K		33					33																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109589	NAT4100343		(Mg,Al)B2	Mg0.75Al0.25B2	Mg	0.75	Al	0.25	B	2																		1	2001																												AlB2			A	3.0712		3.4231											AlB2, C32	K		32.4					32.4																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109590	NAT4100343	no bulk s/c	(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																		1	2001																												AlB2			A	3.0692		3.4077											AlB2, C32	K		27.1					27.1																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109591	NAT4100343	no bulk s/c	(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																		1	2001																												AlB2			A	3.0538		3.375											AlB2, C32	K		12.2					12.2																																																																																																several steps of heat treatment					Loss of superconductivity with the addition of Al to MgB2 and a structural transition in Mg1-xAlxB2			Department of Chemistry and Princeton Materials Institute, PrincetonUniversity, Princeton,USA	Nature 410(2001)343	H.W.Zandbergen,J.S.Slusky,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,P.Khalifah,R.J.Cava,S.M.Loureiro,T.He		
109592	JPS0701889		MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.082		3.5216											AlB2, C32	K		38					38																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109593	JPS0701889		(Mg,Mn)B2	Mg0.99Mn0.01B2	Mg	0.99	Mn	0.01	B	2																			2001																												AlB2			A	3.0839		3.521											AlB2, C32	K		36.2					36.2																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109594	JPS0701889		(Mg,Mn)B2	Mg0.98Mn0.02B2	Mg	0.98	Mn	0.02	B	2																			2001																												AlB2			A	3.0842		3.521											AlB2, C32	K		34.5					34.5																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109595	JPS0701889		(Mg,Mn)B2	Mg0.97Mn0.03B2	Mg	0.97	Mn	0.03	B	2																			2001																												AlB2			A	3.0823		3.5185											AlB2, C32	K		33.3					33.3																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109596	JPS0701889		(Mg,Mn)B2	Mg0.96Mn0.04B2	Mg	0.96	Mn	0.04	B	2																			2001																												AlB2			A	3.0825		3.5176											AlB2, C32	K		32.3					32.3																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109597	JPS0701889		(Mg,Mn)B2	Mg0.95Mn0.05B2	Mg	0.95	Mn	0.05	B	2																			2001																												AlB2			A	3.083		3.5182											AlB2, C32	K		30					30																																																																																																mixture-heat(900C,2h)					Mn-Substitution Effects on MgB2 Superconductor			Department of Crystalline Materials Science, Nagoya University, Nagoya	J.Phys.Soc.Jpn, 70(2001)1889	A.Nakamura,K.Kato,S.Xu,Y.Moritomo		
109599	SCI2920075	powder sample. dTc/dP in K/GPa.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.6					38.6			K/GPa	-0.8																																																																																												heat(900C,3h, in Ta-tube)					Pressure dependence of the superconducting transition temperature of magnesium diboride				Science 292(2001)75	K.A.Regan,M.A.Hayward,M.Monteverde,M.Nunez-Regueiro,N.Rogado,R.J.Cava,S.M.Loureiro,T.He		
109600	JEL0730532	Debye-T from resistivity(Bloch-Gruneisen)	ZrB2	B2Zr1	B	2	Zr	1																					2001																												AlB2			A	3.17		3.532											AlB2, C32	K		5.5					5.5																				T		0.1														A		570																					280																																					pellet from powder-heat(1700C,2h in W-foil)					Electron Transport in diborides: Observation of superconductivity in ZrB2			Institute of Solid State Physics, Russian Academy of Science, Moscow, Russia	JETP Lett., 73(2001)532	I.I.Zver'kova,M.P.Kulakov,N.S.Sidorov,V.A.Gasparov		
109601	JEL0730532	Debye-T from resistivity(Bloch-Gruneisen), not s/c	NbB2	B2Nb1	B	2	Nb	1																					2001																												AlB2			A	3.111		3.267											AlB2, C32	K					0.37																																																													460																																					pellet from powder-heat(1700C,2h in W-foil)					Electron Transport in diborides: Observation of superconductivity in ZrB2			Institute of Solid State Physics, Russian Academy of Science, Moscow, Russia	JETP Lett., 73(2001)532	I.I.Zver'kova,M.P.Kulakov,N.S.Sidorov,V.A.Gasparov		
109602	JEL0730532	not s/c	TaB2	B2Ta1	B	2	Ta	1																					2001																												AlB2			A	3.087		3.247											AlB2, C32	K					0.37																																																																																																		pellet from powder-heat(1700C,2h in W-foil)					Electron Transport in diborides: Observation of superconductivity in ZrB2			Institute of Solid State Physics, Russian Academy of Science, Moscow, Russia	JETP Lett., 73(2001)532	I.I.Zver'kova,M.P.Kulakov,N.S.Sidorov,V.A.Gasparov		
109603	JET0730570	as-synthesized	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0878		3.5216											AlB2, C32	K		39					39																													T/K		0.4																																																																						Superconducting properties of the atomically disordered MgB2 compound			Institute of Metal Physics, Ural Division,Russia	JETP Lett., 73(2001)570	A.E.Kar'kin,A.P.Tyutyunik,B.N.Goshchitskii,M.V.Sadovskii,N.I.Kadyrova,T.V.D'yachkova,V.G.Zubkov,V.I.Voronin,Yu.G.Zainulin		
109604	JET0730570	thermal neutron irradiation. Fluence=1 E+19 /cm2	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0953		3.5533											AlB2, C32	K		5					5																													T/K		0.4																																																																						Superconducting properties of the atomically disordered MgB2 compound			Institute of Metal Physics, Ural Division,Russia	JETP Lett., 73(2001)570	A.E.Kar'kin,A.P.Tyutyunik,B.N.Goshchitskii,M.V.Sadovskii,N.I.Kadyrova,T.V.D'yachkova,V.G.Zubkov,V.I.Voronin,Yu.G.Zainulin		
109605	SCI2550833	powder sample. Dln(a)/dp=1.52 E-3 /kbar. Volume compressibility=4.08 E-3 /kbar. By XRD	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		29.6					29.6																																																																																																					Compressibility of M3C60 fulleren superconductors: Relation between Tc and lattice parameter				Science 255(1992)833	A.B.Smith III,G.B.M.Vaughan,J.E.Fischer,J.P.MaCauley,Jr.,N.Coustel,Otto Zhou,P.A.Heiney,Q.Zhu		
109606	SCI2550833	powder sample. Dln(a)/dp=1.20 E-3 /kbar. Volume compressibility=4.08 E-3 /kbar. By XRD	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		19.3					19.3																																																																																																					Compressibility of M3C60 fulleren superconductors: Relation between Tc and lattice parameter				Science 255(1992)833	A.B.Smith III,G.B.M.Vaughan,J.E.Fischer,J.P.MaCauley,Jr.,N.Coustel,Otto Zhou,P.A.Heiney,Q.Zhu		
109607	MAT0104063	Hc2,cohere for T=0.1T. Mass of B =10.8(natural abandance)	BeB2	B2.75Be1	B	2.75	Be	1																					2001																															A	9.7738		9.5467												K		0.72					0.72																				T		0.19							T/K		0.3			MHC9607		A		300																																																										slow cool from Be-rich arc melted bulk					"tructure and Superconducting Properties of ""BeB2"""				cond-mat/0104063(2001)	D.P.Young,F.R.Fronczek,J.Y.Chan,P.W.Adams		
109608	MAT0104063	mass of B = 10.0 isotope. Stoichiometric sample shows not AlB2 structure.	BeB2	B2.75Be1	B	2.75	Be	1																					2001																																														K		0.79					0.79																																																																																																slow cool from Be-rich arc melted bulk					"tructure and Superconducting Properties of ""BeB2"""				cond-mat/0104063(2001)	D.P.Young,F.R.Fronczek,J.Y.Chan,P.W.Adams		
109609	LTP1180113	RR=7.8 microOhm.cm. dTc/dp=0.9 K/Gpa forp>1GPa. dHc2dT=23T/K for H//a, = 18.5 T/K for H//c. Hc2(0)//c = 2.06 T.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																			2000																																														K		0.677					0.677		R	K/GPa	0.05																T		1.75							T/K		23			MHC9609																																																																			Transport measurements of the heavy Fermion superconductor CeCu2Si2 under pressure			Grenoble, Cedex,France	J.Low Temp.Phys., 118(2000)113	D.Braithwaite,I.Sheikin,J.-P.Brison,J.Flouquet,W.Assmus		
109610	PHC2800001		Yb3Rh4Sn13	Yb3Rh4Sn13	Yb	3	Rh	4	Sn	13																		3	1997																																														K		7.2					7.2																																		MHC9610		A		100																																																										Sn-flux-method					Regions of enhansd pinning in the mixed state of the superconductor Yb3Rh4S 13	199706		Department of Physics, University of Worwick, Coventry CV4 7AL, UK	Physica.C,280(1997)1-8	C.V. Tomy,D.McK. Paul,G. Balakrishnan		
109611	PR05608346	Hc2 measured by ac susceptibility. Phase-I structure.	Ca3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																		3	1997																																														K		8.2					8.2																																		MHC9611																																																														Sn-flux-method					Observation of the peak effect in the superconductor Ca3Rh4Sn13			Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 56(1997)8346	C.V.Tomy,D.McK.Paul,G.Balakrishnan		
109612	JPS0643175	gamma in mj/K2.mol-Yb. Gamma and Debye-T by specific heat measurement. G-L parameter = 21	Yb3Rh4Sn13	Yb3Rh4Sn13	Yb	3	Rh	4	Sn	13																		3	1995																												Pr3Rh4Sn13			A	9.681														K		7.7					7.7																													kOe/K		3.5			MHC9612		A		100			A		2100													mj/mol.K2	28		158																																					Sn-flux-method					Peak Effect in the Superconducting Mixed State of Yb3Rh4Sn13 Single Crystals			Department of Physics, Faculty of Science, Tokyo Metropolitan University, Hachioji 192-03	J.Phys.Soc.Jpn, 64(1995)3175	H.Sato,H.Sugawara,T.Fukuhara,Y.Aoki		
109613	NAT3560419	fraction of fcc phase = 60 %	RbCs2C60	Rb1Cs2C60	Rb	1	Cs	2	C	60																			1992																												fullerene			A	14.555														K		33					33																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109614	NAT3560419	fraction of fcc phase = 60 %	Rb2CsC60	Rb2Cs1C60	Rb	2	Cs	1	C	60																			1992																												fullerene			A	14.431														K		31					31																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109615	NAT3560419	fraction of fcc phase = 70 %	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene			A	14.384														K		29					29																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109616	NAT3560419	fraction of fcc phase = 84 %	KRb2C60	K1Rb2C60	K	1	Rb	2	C	60																			1992																												fullerene			A	14.323														K		27					27																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109617	NAT3560419	fraction of fcc phase = 60 %	K2CsC60	K2Cs1C60	K	2	Cs	1	C	60																			1992																												fullerene			A	14.292														K		24					24																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109618	NAT3560419	fraction of fcc phase = 75 %	K2RbC60	K2Rb1C60	K	2	Rb	1	C	60																			1992																												fullerene			A	14.243														K		23					23																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109619	NAT3560419	fraction of fcc phase = 70 %	K3C60	C60K3	C	60	K	3																					1992																												fullerene			A	14.24														K		19					19																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109620	P064144516	95 % AlB2 phase. Impurity phase =B. not s/c. RRR=1.05. Gamma in mj/mol.K2	TaB2	B2Ta1	B	2	Ta	1																					2001																												AlB2			A	3.098		3.224											AlB2, C32	K					1.5																																																										mj/mol.K2	2.8		415																																					arc-melting in pure Ar					Electronic structure and weak electron-phonon coupling in TaB2			Department of Physics, University of California, Davis, California , USA	Phys.Rev.B, 64(2001)144516	A.Handstein,G.Behr,G.Fuchs,H.Eschrig,H.Rosner,K.-H.Muller,K.Nenkov,S.-L.Drechsler,W.E.Pickett		
109621	P064144516	97 % AlB2 phase. Impurity phase =Ta3B4. not s/c. RRR=1.2. Gamma in mj/mol.K2	TaB2	B2Ta1	B	2	Ta	1																					2001																												AlB2			A	3.067		3.286											AlB2, C32	K					1.5																																																										mj/mol.K2	2		419																																					arc-melting in pure Ar					Electronic structure and weak electron-phonon coupling in TaB2			Department of Physics, University of California, Davis, California , USA	Phys.Rev.B, 64(2001)144516	A.Handstein,G.Behr,G.Fuchs,H.Eschrig,H.Rosner,K.-H.Muller,K.Nenkov,S.-L.Drechsler,W.E.Pickett		
109622	SSC1100691	multi-phase sample. Data of Hc1,Hc2 are for T=1.7 K.	LuReBC	Lu1Re1B1C1	Lu	1	Re	1	B	1	C	1																	1999																																														K		6.1					6.1											Oe		200							kOe		8																																																																										arc-melting					Superconductivity in new quaternary borocarbide system R-Re-B-C (R=Y, Gd, Tb and Lu),			Tata Institute of Fundamental Research,Munbai,India	Solid State Commun., 110(1999)691	A.D.Chinchure,Aravind D.Chinchure,L.C.Gupta,R.Nagarajan		
109623	SSC1100691	multi-phase sample. Data of Hc1,Hc2 are for T=1.7 K.	YReBC	Y1Re1B1C1	Y	1	Re	1	B	1	C	1																	1999																																														K		4.7					4.7											Oe		100							kOe		4																																																																										arc-melting					Superconductivity in new quaternary borocarbide system R-Re-B-C (R=Y, Gd, Tb and Lu),			Tata Institute of Fundamental Research,Munbai,India	Solid State Commun., 110(1999)691	A.D.Chinchure,Aravind D.Chinchure,L.C.Gupta,R.Nagarajan		
109624	SSC1100691	multi-phase sample	TbReBC	Tb1Re1B1C1	Tb	1	Re	1	B	1	C	1																	1999								30																																						K		4					4																																																																																																arc-melting					Superconductivity in new quaternary borocarbide system R-Re-B-C (R=Y, Gd, Tb and Lu),			Tata Institute of Fundamental Research,Munbai,India	Solid State Commun., 110(1999)691	A.D.Chinchure,Aravind D.Chinchure,L.C.Gupta,R.Nagarajan		
109625	SSC1100691	multi-phase sample	GdReBC	Gd1Re1B1C1	Gd	1	Re	1	B	1	C	1																	1999																																														K		4					4																																																																																																arc-melting					Superconductivity in new quaternary borocarbide system R-Re-B-C (R=Y, Gd, Tb and Lu),			Tata Institute of Fundamental Research,Munbai,India	Solid State Commun., 110(1999)691	A.D.Chinchure,Aravind D.Chinchure,L.C.Gupta,R.Nagarajan		
109626	NAT3560419	fraction of fcc phase = 72 %	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1992																												fullerene			A	14.134														K		12					12																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109627	NAT3560419	fraction of fcc phase = 1 %	Li2CsC60	Li2Cs1C60	Li	2	Cs	1	C	60																			1992																												fullerene			A	14.12														K		12					12																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109628	NAT3560419	fraction of fcc phase = 2 %	Na2RbC60	Na2Rb1C60	Na	2	Rb	1	C	60																			1992																												fullerene			A	14.028														K		2.5					2.5																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109629	NAT3560419	fraction of fcc phase = 0.1 %	Na2KC60	Na2K1C60	Na	2	K	1	C	60																			1992																												fullerene			A	14.025														K		2.5					2.5																																																																																																(C60+dopant) in quartz tube ,then heat					Superconductivity in sodium- and lithium-containing alkali-metal fullerens			Fundamental Research Lab, NEC, Tsukuba,Japan	Nature , 356(1992)419	I.Hirosawa,J.Mizuki,J.S.Tsai,K.Tanigaki,S.Kuroshima,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109630	SCI2590655	using 99% C<13> sample. Tc for C<13> sample=28.9 K [isotope] = 0.30 +- 0.05	Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene																		K		29.6					29.6						0.3	C	99	0.7																																																																																												Isotope effect and superconductivity in metal-doped C60			Department of Chemistry , Harvard University, Cambridge, MA, USA	Science 259(1993)655	Charles M.Lieber,Chia-Chun Chen		
109631	AMC1143141	using 99% C<13> sample. Tc for C<13> sample=18.8 K	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		19.2					19.2						0.3	C																																																																																														Synthesis of pure <13>C60 and determination of the isotope effect for fullerene superconductors			Department of Chemistry , Harvard University, Cambridge, MA, USA	J.Am.Chem.Soc., 114(1992)3141	Charles M.Lieber,Chia-Chun Chen		
109632	SSC0930269		Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1995																												fullerene																		K		11.7					11.7																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109633	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.25Cs0.75C60	Na	2	Rb	0.25	Cs	0.75	C	60																	1995																												fullerene																		K		9.4					9.4																																																																																																mix(Na2RbC60+Na2CsC60)-react(400-450C,1 month)					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109634	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.5Cs0.5C60	Na	2	Rb	0.5	Cs	0.5	C	60																	1995																												fullerene																		K		8.4					8.4																																																																																																mix(Na2RbC60+Na2CsC60)-react(400-450C,1 month)					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109635	SSC0930269		Na2(Rb,Cs)C60	Na2Rb0.75Cs0.25C60	Na	2	Rb	0.75	Cs	0.25	C	60																	1995																												fullerene																		K		5.2					5.2																																																																																																mix(Na2RbC60+Na2CsC60)-react(400-450C,1 month)					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109636	SSC0930269		Na2(Rb,Cs)C60	Na2Rb1C60	Na	2	Rb	1	C	60																			1995																												fullerene			A	14.097														K		3.4					3.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109637	SYN0563027	82 % C<13> sample used. Tc of this sample = 17.8K. Gap by NMR.	K3C60	C60K3	C	60	K	3																					1993																												fullerene																		K		19.6					19.6						1.45	C																																									3.4																																																					Isotope effect on 82% <13>C substituted K3C60			Unversite Paris-Sud,Orsay, France	Synthetic Metals 56(1993)3027	A.Rassat,C.Fabre,D.Jerome,G.Quirion,P.Auban-Senzier,P.Bernier,S.Della-Negra		
109638	SYN0562845	penetration depth by muon-SR.	Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene																		K		28					28																																									A		4200																																																										Muon spin relaxation studies in organic superconductors and organic magnets			Department of Physics,Columbia Univ., New York,USA	Synthetic Metals 56(1993)2845	G.M.Luke,L.P.Le,Y.J.Uemura		
109639	SYN0562845	penetration depth by muon-SR.	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1993																												fullerene																		K		11					11																																									A		8000																																																										Muon spin relaxation studies in organic superconductors and organic magnets			Department of Physics,Columbia Univ., New York,USA	Synthetic Metals 56(1993)2845	G.M.Luke,L.P.Le,Y.J.Uemura		
109640	SYN0770201	gap by STM. Gap values spatially fluctuate from 2.6 to 5.2 meV at 2.8K. Value is calculated for 2.6 meV.	Rb3C60	C60Rb3	C	60	Rb	3																					1996																												fullerene																		K		30.5					30.5																																																2																																																C60 single + Rb)-heat(400C,80h)					Spatially resolved electron tunneling spectroscopy on single crystalline Rb3C60			Institute of Physics, University of Basel,Basel,Switzerland	Synthetic Metals 77(1996)201	H.-J.Guntherodt,H.P.Lang,P.Pess,S.Behler,U.Hubler,V.Thommen-Geiser		
109641	NAT3520605	muon-SR	K3C60	C60K3	C	60	K	3																					1991																												fullerene																		K		19.3					19.3																																									A		4800																																																					press and sintering					Magnetic-field penetration depth in K3C60 measured by muon spin relaxation			Columbia Univ., New York,USA	Nature 352(1991)605	A.Keren,B.J.Sternlieb,F.Diederich,G.Gruner,G.M.Luke,J.H.Brewer,K.Holczer,L.P.Le,R.B.Kaner,R.L.Whetten,S.Donovan,S.M.Huang,Sophia Lin,W.D.Wu,Y.J.Uemura		
109642	NAT3690541	reflectivity measurement between 2 meV and 6 meV.	K3C60	C60K3	C	60	K	3																					1994																												fullerene																		K		20.3					20.3																																																3.44																																																vapor-transport method					Optical measurements of the superconducting gap in single-crystal K3C60 and Rb3C60			ETH-Zurich, Zurich, Switzerland	Nature 369(1994)541	A.Zettl,G.Briceno,L.Degiorgi,M.S.Fuhrer,P.Wachter		
109643	NAT3690541		Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		30.5					30.5																																																3.45																																																vapor-transport method					Optical measurements of the superconducting gap in single-crystal K3C60 and Rb3C60			ETH-Zurich, Zurich, Switzerland	Nature 369(1994)541	A.Zettl,G.Briceno,L.Degiorgi,M.S.Fuhrer,P.Wachter		
109644	NAT3550620	Tc measured for three different C<13> content (1.1, 33, 33 %) . Tc by M(T)	Rb3C60	C60Rb3	C	60	Rb	3																				1	1992																												fullerene																		K		30.5					30.5						1.4	C																																																																																									400C,3d in sealed quartz tube					Isotope effect on superconductivity in Rb3C60			Fundamental Research Lab,NEC, Tsukuba,Japan	Nature 355(1992)620	I.Hirosawa,J.Mizuki,J.S.Tsai,J.Tabuchi,K.Tanigaki,T.W.Ebbesen,Y.Kubo,Y.Shimakawa		
109645	PRL0681912	gap by NMR of C<13>. Gap value estimated using Tc(NMR)=23 K. penetration depth from NMR assuming Gaussian FWHM.	Rb3C60	C60Rb3	C	60	Rb	3																				1	1992																												fullerene																		K		29.4					29.4																																									A		4600					4.1																																																					Electronic properties of normal and superconducting alkali fullerides probed by 13C nuclear magnetic resonance			AT&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys. Rev. Lett., 68(1992)1912	A.P.Ramirez,D.W.Murphy,G.Dabbagh,M.J.Rosseinsky,R.M.Fleming,R.Tycko		
109646	PRL0681912	gap by NMR of C<13>. Gap value estimated using Tc(NMR)=14 K. penetration depth from NMR assuming Gaussian FWHM.	K3C60	C60K3	C	60	K	3																				1	1992																												fullerene																		K		19.4					19.4																																									A		6000					3																																																					Electronic properties of normal and superconducting alkali fullerides probed by 13C nuclear magnetic resonance			AT&T Bell Laboratories, 600 Mountain Avenue, Murray Hill, New Jersey 07974	Phys. Rev. Lett., 68(1992)1912	A.P.Ramirez,D.W.Murphy,G.Dabbagh,M.J.Rosseinsky,R.M.Fleming,R.Tycko		
109647	PRL0692987	energy gap and penetration depth were estimated from infrared conductivity.	K3C60	C60K3	C	60	K	3																				1	1992																												fullerene																		K		19					19																																									A		8000					3.6																																																					Optical response of the superconducting state of K3C60 and Rb3C60			Laboratorium fur Festkoperphysik, Eidgenosische Technische Hochschule Zuich, CH-8093 Zuich, Switzerland	Phys. Rev. Lett., 69(1992)2987	G.Gruner,J.Wiley,L.Degiorgi,P.Wachter,R.B.Kaner,S.-M.Huang		
109648	PRL0692987	energy gap and penetration depth were estimated from infrared conductivity.	Rb3C60	C60Rb3	C	60	Rb	3																				1	1992																												fullerene																		K		29					29																																									A		8000					2.98																																																(Rb2.8C60+K4C60)-heat(200C)					Optical response of the superconducting state of K3C60 and Rb3C60			Laboratorium fur Festkoperphysik, Eidgenosische Technische Hochschule Zuich, CH-8093 Zuich, Switzerland	Phys. Rev. Lett., 69(1992)2987	G.Gruner,J.Wiley,L.Degiorgi,P.Wachter,R.B.Kaner,S.-M.Huang		
109649	PRL0681058	sample prepared using 90 % C<13> D-glucose. C<13> isotope effect. Delta-Tc = 0.65 K for 75 % C<13> sample.	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		30					30						0.37	C																																																																																														ISOTOPE EFFECT IN SUPERCONDUCTING RB3C60	199202			PHYS.REV.LETT.,68(1992)1058	A.M.MUJSCE,A.M.Mujsce,A.P.RAMIREZ,A.P.Ramirez,A.R.KORTAN,A.R.Kortan,A.V.MAKHIJA,A.V.Makhija,D.W.MURPHY,D.W.Murphy,K.B.LYONS,K.B.Lyons,M.J.ROSSEINSKY,M.J.Rosseinsky,R.C.HADDON,R.C.Haddon,S.J.DUCLOS,S.J.Duclos,S.M.ZAHURAK,S.M.Zahurak	RB,C	
109650	PRL0703987	impurity phase = 5 % Rb4C60. Gap and penetration depth by muon-SR.	Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene																		K		29.4					29.4																																									A		3700					3.6																																																					Coherence peak and superconducting energy gap in Rb3C60 observed by muon spin relaxation			TRIUMF, Department of Physics and Canadian Institute of Advanced Research, University of British Columbia, Vancouver, British Columbia		A.B.Smith,III,J.E.Fischer,J.Sonier,J.W.Schneider,K.H.Chow,L.Brand,R.F.Kiefl,R.M.Strongin,S.Dunsiger,T.L.Duty,T.M.Johnston,W.A.MacFarlane		
109651	JPS0631670	volume fraction = 60%. Gap by NMR of C<13>. Gap(0K) = 3.52 meV.	K3C60	C60K3	C	60	K	3																					1994																												fullerene																		K		17.1					17.1																																																4.31																																																					Fermi-Liquid Behavior and BCS s-Wave Pairing of K3C60 Observed by 13C-NMR			NTT Basic Research Laboratories, 3-1, Morinosato Wakamiya, Atsugi-shi, Kanagawa,Japan	J.Phys.Soc.Jpn, 63(1994)1670	A.Matsuda,C.W.Chu,S.Sasaki		
109652	PRL0770167		Na2CsxC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1996																												fullerene																		K		11.6					11.6																																																																																																direct reaction and mixing					Tc vs Carrier Concentration in Cubic Fulleride Superconductors			University of Maryland, College Park, Maryland 20742 and National Institute of Standards and Technology, Gaithersburg, Maryland	Phys. Rev. Lett., 77(1996)167	C.L.Lin,J.E.Fischer,J.Robert,L.Barbedette,P.Petit,T.T.M.Palstra,T.Yildirim		
109653	PRL0770167		Na2CsxC60	Na2Cs0.93C60	Na	2	Cs	0.93	C	60																			1996																												fullerene																		K		9.6					9.6																																																																																																direct reaction and mixing					Tc vs Carrier Concentration in Cubic Fulleride Superconductors			University of Maryland, College Park, Maryland 20742 and National Institute of Standards and Technology, Gaithersburg, Maryland	Phys. Rev. Lett., 77(1996)167	C.L.Lin,J.E.Fischer,J.Robert,L.Barbedette,P.Petit,T.T.M.Palstra,T.Yildirim		
109654	PRL0770167		Na2CsxC60	Na2Cs0.88C60	Na	2	Cs	0.88	C	60																			1996																												fullerene																		K		8.3					8.3																																																																																																direct reaction and mixing					Tc vs Carrier Concentration in Cubic Fulleride Superconductors			University of Maryland, College Park, Maryland 20742 and National Institute of Standards and Technology, Gaithersburg, Maryland	Phys. Rev. Lett., 77(1996)167	C.L.Lin,J.E.Fischer,J.Robert,L.Barbedette,P.Petit,T.T.M.Palstra,T.Yildirim		
109655	PRL0770167		Na2CsxC60	Na2Cs0.75C60	Na	2	Cs	0.75	C	60																			1996																												fullerene																		K		7					7																																																																																																direct reaction and mixing					Tc vs Carrier Concentration in Cubic Fulleride Superconductors			University of Maryland, College Park, Maryland 20742 and National Institute of Standards and Technology, Gaithersburg, Maryland	Phys. Rev. Lett., 77(1996)167	C.L.Lin,J.E.Fischer,J.Robert,L.Barbedette,P.Petit,T.T.M.Palstra,T.Yildirim		
109656	PRL0770167		(K,Ba)3C60	K2.75Ba0.25C60	K	2.75	Ba	0.25	C	60																			1996																												fullerene																		K		15					15																																																																																																direct reaction and mixing					Tc vs Carrier Concentration in Cubic Fulleride Superconductors			University of Maryland, College Park, Maryland 20742 and National Institute of Standards and Technology, Gaithersburg, Maryland	Phys. Rev. Lett., 77(1996)167	C.L.Lin,J.E.Fischer,J.Robert,L.Barbedette,P.Petit,T.T.M.Palstra,T.Yildirim		
109657	P064180501	gap calculated from temperature dependence of penetration depth which measured LC resonator.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.4					39.4																																																1.54																																																wire using W-core, 950C					Energy gap and proximity effect in MgB2 superconducting wires			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, 1110 West Green Street, Urbana, Illinois 61801	Phys.Rev.B., 64(2001)180501	P.C.Canfield,R.Prozorov,R.W.Giannetta,S.L.Bud'ko		
109658	P064172501	ceramic sample. Hc1(0)=160 Oe from ac-susceptibility. Penetration depth by ac-sus of sphere sample. anisotropy < 1.5	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.08		3.52											AlB2, C32	K		38					38											Oe		130																T/K		0.4										A		1800																																																					solid state reaction (950C)					Penetration depth and anisotropy in MgB2			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas	Phys.Rev.B., 64(2001)172501	C.W.Chu,R.L.Meng,X.H.Chen,Y.Y.Xue		
109659	P064172504	gap by photoemission spectroscopy. Fine structure are observed upto 70 meV.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2001																												clathrate																		K		8					8																																																3.51	9																																															high-pressure synthesis					Electronic structure and superconducting gap of silicon clathrate Ba8Si46 studied with ultrahigh-resolution photoemission spectroscopy			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B., 64(2001)172504	A.Fukushima,A.Shintani,H.Fukuoka,K.Kobayashi,K.Moriguchi,S.Shin,S.Yamanaka,T.Kiss,T.Yokoya		
109660	PHC3630219		MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.0845		3.5195											AlB2, C32	K		38.5					38.5																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109661	PHC3630219		(Mg,Na)B2	Mg0.97Na0.03B2	Mg	0.97	Na	0.03	B	2																		1	2001																												AlB2			A	3.0868		3.5251											AlB2, C32	K		38					38																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109662	PHC3630219		(Mg,Na)B2	Mg0.93Na0.07B2	Mg	0.93	Na	0.07	B	2																		1	2001																												AlB2			A	3.0865		3.5237											AlB2, C32	K		38					38																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109663	PHC3630219		(Mg,Na)B2	Mg0.85Na0.15B2	Mg	0.85	Na	0.15	B	2																		1	2001																												AlB2			A	3.0804		3.5171											AlB2, C32	K		38					38																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109664	PHC3630219		(Mg,Na)B2	Mg0.8Na0.2B2	Mg	0.8	Na	0.2	B	2																		1	2001																												AlB2			A	3.0795		3.5159											AlB2, C32	K		38					38																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109665	PHC3630219		(Mg,Li)B2	Mg0.93Li0.07B2	Mg	0.93	Li	0.07	B	2																		1	2001																												AlB2			A	3.0819		3.5166											AlB2, C32	K		37.8					37.8																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109666	PHC3630219		(Mg,Li)B2	Mg0.85Li0.15B2	Mg	0.85	Li	0.15	B	2																		1	2001																												AlB2			A	3.0731		3.5113											AlB2, C32	K		37.5					37.5																																																																																																solid state reaction (950C, 2h in Ar)					Alkali metal substitution effects in Mg1-xAxB2 (A=Li and  Na)			Structure Research Laboratory, Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Physica C, 363(2001)219	C.H.Wang,H.T.Zhang,L.Li,L.Z.Cao,R.Fan,S.Y.Li,W.Q.Mo,X.G.Luo,X.H.Chen,Y.M.Xiong,Z.Sun		
109667	PHC3630001	RR=5.2 microOhm.cm. RRR=3.46. Tc-width=0.75 K. delta-C at Tc = 92 mJ/mol.K. Hc2(0)=0.69Tc*(dHc2/dT).	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		38.5					38.5																				T		15.2							T/K		0.568			HC9667		A		47																					800																																					HIP(200 MPa) method					Improved superconducting properties of MgB2			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093-0360, USA	Physica C, 363(2001)1	M.B.Maple,N.A.Frederick,S.Li,S.S.Indrakanti,V.F.Nesterenko		
109668	PHC3610091		MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2			A	3.084		3.529											AlB2, C32	K		37.8					37.8																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109669	PHC3610091		(Mg,Li)B2	Mg0.9Li0.1B2	Mg	0.9	Li	0.1	B	2																		1	2001																												AlB2			A	3.081		3.5273											AlB2, C32	K		37.8					37.8																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109670	PHC3610091		(Mg,Li)B2	Mg0.85Li0.15B2	Mg	0.85	Li	0.15	B	2																		1	2001																												AlB2			A	3.0791		3.5322											AlB2, C32	K		35.7					35.7																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109671	PHC3610091		(Mg,Li)B2	Mg0.8Li0.2B2	Mg	0.8	Li	0.2	B	2																		1	2001																												AlB2			A	3.0742		3.5324											AlB2, C32	K		34					34																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109672	PHC3610091		(Mg,Li)B2	Mg0.75Li0.25B2	Mg	0.75	Li	0.25	B	2																		1	2001																												AlB2			A	3.0721		3.5297											AlB2, C32	K		33.7					33.7																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109673	PHC3610091		(Mg,Li)B2	Mg0.7Li0.3B2	Mg	0.7	Li	0.3	B	2																		1	2001																												AlB2			A	3.0681		3.5322											AlB2, C32	K		31					31																																																																																																solid state reaction (950C, 2h in Ta tube with Ar)					Effect of Li doping on structure and superconducting  transition temperature of Mg1-xLixB2			Department of Physics, Tsinghua University, Beijing 100084, China	Physica C, 361(2001)91	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
109674	PHC3630041	Hc1 defined as deviation point from linear M-H.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C			A	3.5271		10.5428												K		16.18					16.18											Oe		224.4																					HC9674																																																														arc-melt, ANN(1100C,5days in vac)					Magnetic and superconducting properties of  Y(Ni1xMnx)2B2C borocarbides			I.F., UFRGS, Porto Alegre, Brazil	Physica C, 363(2001)41	A.A.Gomes,D.E.Brando,F.S.da Rocha,G.L.F.Fraga		
109675	PHC3630041	Hc1 defined as deviation point from linear M-H.	Y(Ni,Mn)2B2C	Y1Ni1.98Mn0.02B2C1	Y	1	Ni	1.98	Mn	0.02	B	2	C	1															2001																												LuNi2B2C			A	3.5266		10.5449												K		15.48					15.48											Oe		167.3																					HC9674																																																														arc-melt, ANN(1100C,5days in vac)					Magnetic and superconducting properties of  Y(Ni1xMnx)2B2C borocarbides			I.F., UFRGS, Porto Alegre, Brazil	Physica C, 363(2001)41	A.A.Gomes,D.E.Brando,F.S.da Rocha,G.L.F.Fraga		
109676	PHC3630041	Hc1 defined as deviation point from linear M-H.	Y(Ni,Mn)2B2C	Y1Ni1.9Mn0.1B2C1	Y	1	Ni	1.9	Mn	0.1	B	2	C	1															2001																												LuNi2B2C			A	3.5272		10.5477												K		12.7					12.7											Oe		96.7																					HC9674																																																														arc-melt, ANN(1100C,5days in vac)					Magnetic and superconducting properties of  Y(Ni1xMnx)2B2C borocarbides			I.F., UFRGS, Porto Alegre, Brazil	Physica C, 363(2001)41	A.A.Gomes,D.E.Brando,F.S.da Rocha,G.L.F.Fraga		
109677	PHC3630041	Hc1 defined as deviation point from linear M-H.	Y(Ni,Mn)2B2C	Y1Ni1.8Mn0.2B2C1	Y	1	Ni	1.8	Mn	0.2	B	2	C	1															2001																												LuNi2B2C			A	3.5264		10.5525												K		8.7					8.7																																																																																																arc-melt, ANN(1100C,5days in vac)					Magnetic and superconducting properties of  Y(Ni1xMnx)2B2C borocarbides			I.F., UFRGS, Porto Alegre, Brazil	Physica C, 363(2001)41	A.A.Gomes,D.E.Brando,F.S.da Rocha,G.L.F.Fraga		
109678	PHC3630041	Hc1 defined as deviation point from linear M-H.	Y(Ni,Mn)2B2C	Y1Ni1.7Mn0.3B2C1	Y	1	Ni	1.7	Mn	0.3	B	2	C	1															2001																												LuNi2B2C			A	3.5275		10.5605												K		5.7					5.7																																																																																																arc-melt, ANN(1100C,5days in vac)					Magnetic and superconducting properties of  Y(Ni1xMnx)2B2C borocarbides			I.F., UFRGS, Porto Alegre, Brazil	Physica C, 363(2001)41	A.A.Gomes,D.E.Brando,F.S.da Rocha,G.L.F.Fraga		
109679	PHC3630006	RR=7.1 microOhm.cm. RRR=5.38. Thermopower(300K)=8.3 uV/K. Thermopower and thermal conductivity were measured.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		38.7					38.7																																																																	THC9679																																				Heat and charge transport properties of MgB2			Institut fur Tieftemperaturphysik, Technische Universitut Dresden, D-01062 Dresden, Germany	Physica C, 363(2001)6	A.Gladun,A.Handstein,D.Lipp,G.Fuchs,H.Rosner,K.H.Muller,M.Richter,M.Schneider,P.Zahn,S.L.Drechsler		
109680	PHC3610095	phase-I, not s/c.	ScNi2B2C	Sc1Ni2B2C1	Sc	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C			A	3.32		10.04												K					4.2																																																																																																							Influence of annealing on the superconductivity of ScNi2B2C			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus, Republic of Belarus, 220072 Minsk, P. Brovka 17, Byelorussia	Physica C, 361(2001)95	A.S.Shestak,N.A.Prytkova,P.V.Molchan,S.N.Ustinovich,V.M.Finskaya,Zh.M.Tomilo		
109681	PHC3610095	phase-II. zero resistance at 14 K.	ScNi2B2C	Sc1Ni2B2C1	Sc	1	Ni	2	B	2	C	1																	2001																												LuNi2B2C			A	3.54		10.55												K		16					16																																																																																																					Influence of annealing on the superconductivity of ScNi2B2C			Institute of Solid State and Semiconductor Physics, National Academy of Sciences of Belarus, Republic of Belarus, 220072 Minsk, P. Brovka 17, Byelorussia	Physica C, 361(2001)95	A.S.Shestak,N.A.Prytkova,P.V.Molchan,S.N.Ustinovich,V.M.Finskaya,Zh.M.Tomilo		
109682	PHC3610227	using 98.46 at % Mg<11>. ac-sus measured upto 20 GPa.	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		39.1					39.1	MTC9682		K/GPa	-1.11																																																																																												(B<11>+Mg)-(800C in 50 bar Ar)					Dependence of the superconducting transition temperature of MgB2 on pressure to 20 GPa			Department of Physics, Washington University, C.B. 1105, One Brookings Drive, St. Louis, MO, USA	Physica C, 361(2001)227	D.G.Hinks,J.D.Jorgensen,J.S.Schilling,S.Deemyad		
109683	PR05000351	zero resistance at 14.6 K.	ScNi2B2C	Sc1Ni2B2C1	Sc	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C			A	3.34		10.2												K		16.5					16.5																																																																																																					Superconductivity at 15 K in the metastable ScNi2B2C compound			Department of Physics,National Tsing Hua University, Hsinchu, Taiwan, Republic of China	Phys.Rev.B, 50(1994)351	C.C.Lai,H.C.Ku,J.H.Shieh,W.Y.Guan,Y.B.You		
109684	PR05204432	s/c volume fraction=40%. Hc2(0) estimated using WHH theory. G-L parameter(= 67) from dM/dH.	RbCs2C60	Rb1Cs2C60	Rb	1	Cs	2	C	60																		1	1995																												fullerene																		K		33					33											mT		8.1							T		17							T/K		0.8			MHC9684		nm		4.4			nm		300																																																					decomposition method (RbN3,CsN3,C60)					Critical fields of the superconducting fullerene RbCs2C60	199508			Phys.Rev.B,52(1995)4432	F. Bolzoni,H. W. Weber,L. Cristofolini,M. Ricco',V. Buntar	Rb, Cs, C	
109685	PR05013890	Hc2(0) estimated using WHH theory. Hc1 determined as the deviation from linear M-H. G-L parameter = 15	Ba6C60	Ba6C60	Ba	6	C	60																					1994																												fullerene																		K		7					7											Oe		130							T		2.2							T/K		0.45					A		120			A		1800																																																					metal azide route (BaN6,C60)					Critical magnetic fields of superconducting Ba6C60	199411			Phys.Rev.B.,50(1994) 13890-13893	K.V.Rao,V.Korenivski,Z.Iqbal	Ba,C	
109686	PRL0681058	delta-Tc =0.65 K, for 75% substitution of C<13>.	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		29.8					29.8						0.37	C																																		A		4000																																																										ISOTOPE EFFECT IN SUPERCONDUCTING RB3C60	199202			PHYS.REV.LETT.,68(1992)1058	A.M.MUJSCE,A.M.Mujsce,A.P.RAMIREZ,A.P.Ramirez,A.R.KORTAN,A.R.Kortan,A.V.MAKHIJA,A.V.Makhija,D.W.MURPHY,D.W.Murphy,K.B.LYONS,K.B.Lyons,M.J.ROSSEINSKY,M.J.Rosseinsky,R.C.HADDON,R.C.Haddon,S.J.DUCLOS,S.J.Duclos,S.M.ZAHURAK,S.M.Zahurak	RB,C	
109687	PRL0681054	thickness = 1600 A. grain size = 70 A.	K3C60	C60K3	C	60	K	3																				3	1992																												fullerene																		K		12.8					12.8																				T		47							T/K		5.5					A		26																																																															ELECTRONIC TRANSPORT PROPERTIES OF K3C60 FILMS	199202			PHYS.REV.LETT.,68(1992)1054	A.F.HEBARD,J.ZAANEN,R.C.HADDON,T.T.M.PALSTRA	K,C	
109688	JJP0310166	the film deposited on quartz substrate by vacuum evaporation. thickness = 1000A. Tc(on)=30K, Tc(end)=26 K. resistivity(RT)=80 microOhm.cm	Rb3C60	C60Rb3	C	60	Rb	3																				3	1992																												fullerene																		K		28					28																																																																																																vac.evap.					Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
109689	JJP0310166	Tc(on)=22K, Tc(end)=2.5 K. resistivity(RT)=140 microOhm.cm	Rb3C60	C60Rb3	C	60	Rb	3																				3	1992																												fullerene																		K		12.5					12.5																																																																																																vac.evap.					Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
109690	JJP0310166	Tc(on)=14.5K, Tc(end)=2.5 K. resistivity(RT)=20 microOhm.cm	K3C60	C60K3	C	60	K	3																				3	1992																												fullerene																		K		8.5					8.5																																																																																																					Charge Transport and Superconducting Transitions in C60 Single Crystal and Thin Films Doped with Rubidium	199202		The Graduate University for Advanced Studies, Institute for Molecular Science, Myodaiji, Okazaki 444	Jpn.J.Appl.Phys.Lett.31(1992)L166-L168	Hajime HOSHI,Hironori OGATA,Isao IKEMOTO,Koichi KIKUCHI,Shinzo SUZUKI,Tamotsu INABE,Yohji ACHIBA,Yusei MARUYAMA		
109691	NAT3520223	(CsMx)3C60 where M=Hg,Tl,Bi, having all the same Tc.	Cs3C60	C60Cs3	C	60	Cs	3																					1991																												fullerene																		K		29.5					29.5																																																																																																					Superconductivity at 30K in cesium-doped C60	7		Department of Chemistry and Division of Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA	Nature 352(1991)223	Charles M. Lieber,Chia-Chun Chen,Stephen P. Kelty		
109692	NAT3520222	compositions are nominal values. s/c volume fraction = 60 %.	(Cs,Rb)3C60	Cs2Rb1C60	Cs	2	Rb	1	C	60																			1991																												fullerene																		K		33					33																																																																																																					SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
109693	NAT3520222	compositions are nominal values. s/c volume fraction = 30 %.	(Cs,Rb)3C60	Cs1Rb2C60	Cs	1	Rb	2	C	60																			1991																												fullerene																		K		31					31																																																																																																					SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
109694	NAT3520222	compositions are nominal values. s/c volume fraction = 10 %.	Rb3C60	C60Rb3	C	60	Rb	3																					1991																												fullerene																		K		29					29																																																																																																					SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
109695	NAT3520222	compositions are nominal values. s/c volume fraction = 14 %.	Rb2C60	C60Rb2	C	60	Rb	2																					1991																												fullerene																		K		29					29																																																																																																					SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
109696	NAT3520222	compositions are nominal values. s/c volume fraction = 18 %.	Rb4C60	C60Rb4	C	60	Rb	4																					1991																												fullerene																		K		29					29																																																																																																					SUPERCONDUCTIVITY AT 33K IN CSXRBYC60	7			NATURE,350(1991)222	J.MIZUKI,J.S.TSAI,K.TANIGAKI,S.KUROSHIMA,S.SAITO,T.W.EBBESEN,Y.KUDO	CS,RB,C	
109697	PRL0670271	density = 1.91	K3C60	C60K3	C	60	K	3																					1991																												fullerene																		K		19.3					19.3											Oe		132							T		49							T/K		3.73					A		26			A		2400																																																										CRITICAL MAGNETIC FIELDS IN THE SUPERCONDUCTING STATE OF K3C60	199107			PHYS.REV.LETT.,67(1991)271	F.DIEDERICH,G.GRUNER,J.D.THOMPSON,K.HOLCZER,O.KLEIN,R.L.WHETTEN	K,C	
109698	NAT3500600	Tc(on)=18 K, Tc(end)=8 K. thickness=960 A. van der Pauw's method for ac resistivity.	K3C60	C60K3	C	60	K	3																				3	1991																												fullerene																		K		13					13																																																																																																film					Superconductivity at 18K in potassium-doped C60	6		AT&T Bell Laboratories, Murray Hill, New Jersey 07974-2070, USA	Nature.35(1991)600	A.F. Hebard,A.R. Kortan,D.W. Murphy,D.W. Ramirez,M.J. Rosseinsky,R.C. Haddon,S.H. Glarum,T.T.M. Palstra		
109699	NAT3500600	Tc by Meissner effect.	K3C60	C60K3	C	60	K	3																				1	1991																												fullerene																		K		18					18																																																																																																					Superconductivity at 18K in potassium-doped C60	6		AT&T Bell Laboratories, Murray Hill, New Jersey 07974-2070, USA	Nature.35(1991)600	A.F. Hebard,A.R. Kortan,D.W. Murphy,D.W. Ramirez,M.J. Rosseinsky,R.C. Haddon,S.H. Glarum,T.T.M. Palstra		
109700	PLA1640355	60 % substitution of C<13>. ISOTOPE = 2.0 - 2.25.	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		28.6					28.6						2	C																																																																																														Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
109701	PLA1640355	60 % substitution of C<13>. ISOTOPE = 1.2 - 1.43	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		20					20						1.2	C																																																																																														Enhanced isotope effect in 13C-rich superconducting MxC60 (M=K,Rb): support for vibronic pairing	1992		Institute for Molecular Science, Okazaki, Aichi 444, Japan	Phys.Lett.A,164(1992)355-361	A.A. Zakhidov,D.M. Petty,H. Inokuchi,I. Ikemoto,K. Imaeda,K. Kikuchi,K. Yakushi,S. Suzuki,Y. Achiba		
109702	PR0465880		K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		18					18																				T		28							T/K		2					A		34																																																															UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
109703	PR0465880		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		30					30																				T		38							T/K		2					A		30																																																															UPPER-CRITICAL-FIELD-TEMPERATURE PHASE DIAGRAM OF ALKALI-METAL-INTERCALATED C60 SUPERCONDUCTORS	199209		DEPARTMENT OF PHYSICS, UNIVERSITY OF CALIFORNIA AT LOS ANGELES	PHYS.REV.B,46(1992)5880	C.E.JOHNSON,F.DIEDERICH,H.W.JIANG,K.HOLCZER,R.B.KANER,R.L.WHETTEN	K,C,RB	
109704	PR0465876	Hc2 follows the linear relation, not WHH theory.	K3C60	C60K3	C	60	K	3																				1	1992																												fullerene																		K		18.7					18.7																				T		38							T/K		2.14					A		29																																																															EVIDENCE OF UPPER-CRITICAL-FIELD ENHAMCEMENT IN K3C60 POWDERS	199209		AT&T BELL LABORATORIES, NEW JERSEY	PHYS.REN.B,46(1992)5876	A.PASSNER,D.W.MURPHY,G.S.BOEBINGER,I.I.MAZIN,M.J.ROSSEINSKY,T.T.PALSTRA	K,C	
109705	PR04614936	RF technique in pulsed field. spin-orbit parameter=1.	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K		19.5					19.5																				T		32.7							T/K		2.8					A		31																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
109706	PR04614936	RF technique in pulsed field. spin-orbit parameter=0.7.	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K																											T		57.4							T/K		3.86					A		24																																																															MEASUREMENTS OF THE UPPER CRITICAL FIELD OF K3C60 AND RB3C60 POWDERS TO 60 T	199212		FRANCIS BITTER NATIONAL MAGNET LABORATORY, MASSACHUSETTS INSTITUTE OF TECHNOLOGY	PHYS.REV.B,46(1992)14936	D.HEIMAN,E.J.MCNIFF JR.,R.B.KANER,S.FONER,S.M.HUANG	K,C,RB	
109707	SSC0870375	compositions are estimated from synthesis condition.		Na3.5N0.5C60	Na	3.5	N	0.5	C	60																			1993																												fullerene			A	14.204														K		14.7					14.7																																																																																																heat(370-390C, 20 min) of (NaN3:C60=4:1)					NEW SUPERCONDUCTING SODIUM-NITROGEN-C60 THRNARY COMPOUND				SOLID STATE COMMUN.,87(1993)375	H.INOKUCHI,H.KITAGAWA,I.I.KHAIRULLIN,K.IMAEDA,K.YAKUSHI,M.NAGATA,N.MIZUTANI	C,NA,N	
109708	SSC0850073	gamma in micro-J/g.K2. 80%C60+18%C70+2% solvent. Debye-T estimated from sp.heat below 9K. Two anomaries (90K, 250K) in sp.heat.	C60	C60	C	60																							1993																												fullerene																		K																																																															mj/mol.K2	893		188																																										SPECIFIC HEAT OF FULLERENES EXTRACT	199301			SOLID STATE COMMUN.,85(1993)73	A.DEMAIN,B.NYSTEN,E.GRIVEI,J-P.ISSI,M.CASSART	C,	
109709	PHC2320022	granular, grain size = 150 A. Tc not shown. transition width=0.9 K.	K3C60	K3C60	K	3	C	60																					1994																												fullerene																		K																											T		40							T/K		2.8																																																																						Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
109710	PHC2320022	granular, grain size = 250 A. Tc not shown(about 18.8 K).	K3C60	K3C60	K	3	C	60																					1994																												fullerene																		K																											T		33							T/K		2.33																																																																						Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
109711	PHC2320022	granular, grain size = 310 A. Tc not shown(about 18.8 K).	K3C60	K3C60	K	3	C	60																					1994																												fullerene																		K																											T		28							T/K		2.18																																																																						Granularity and upper critical fields in K3C60	199410			Physica C,232 (1994) 22-26	A.Zettl,J.G.Hou,Marvin L.Cohen,X.-D.Xiang	K,C	
109712	PHC2280181	volume fraction = 44%. ac susceptibility measurements. BCS coherence=150A.	K3C60	C60K3	C	60	K	3																					1994																												fullerene																		K		17.8					17.8																				T		17							T/K		1.4					A		44																																																															Inter- and intragrain AC response of the granular superconductors K3C60 and Rb3C60	199407			Physica C, 228(1994)181-189	E.Straube,H.-J.Guntherodt,H.Werner,K.Luders,M.Baenitz,M.Heinze,R.Schlogl,V.Thommen	K,C,Rb	
109713	PHC2280181	single grain. volume fraction = 29%. BCS coherence=50A.	Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		29.5					29.5																				T		44							T/K		2.3					A		27																																																															Inter- and intragrain AC response of the granular superconductors K3C60 and Rb3C60	199407			Physica C, 228(1994)181-189	E.Straube,H.-J.Guntherodt,H.Werner,K.Luders,M.Baenitz,M.Heinze,R.Schlogl,V.Thommen	K,C,Rb	
109714	PHC2280175	Analizing R(H) using fluctuation theory. BCS coherence = 44A	Rb3C60	C60Rb3	C	60	Rb	3																					1994																												fullerene																		K		30					30																				T		62							T/K		3.28					A		24			A		3200																																																										Magnetotransport in single-crystal Rb3C60	199407			Physica C, 228(1994)175-180	A.Zettl,J.G.Hou,Marvin L.Cohen,Vincent H.Crespi,X.-D.Xiang	Rb,C	
109715	SUP0080067	G-L parameter=15. e-ph coupling = 0.8. Hc1 defined as deviation from linear M-H curve.	Ba6C60	Ba6C60	Ba	6	C	60																					1995																												fullerene																		K		7					7											Oe		130							T		2.2							T/K		0.45					A		120			A		1800																																																										On the Normal and Superconducting Properties of Ba6C60	1995		Department of Condensed Matter Physics, Royal Institute of Technology, S-100 44 Stockholm, Sweden	J.Superconductivity,8(1995)67	K.V. Rao,Vladislav Korenivski		
109716	NAT3750126	space-G=Pcab. Z=32 per formula unit cell. X-ray density=2.92 g/cm3.  s/c volume fraction = 5.6%	Yb3C60	C60Yb2.75	C	60	Yb	2.75																					1995																												fullerene			A	27.874	27.98	27.873												K		6					6																																																																																																					Superconductivity and cation-vacancy ordering in the rare-earth fulleride Yb2.75C60	5		AT&T Bell Laboratories, Murray Hill, new Jersey 07974, USA	Nature 375(1995)126	A.P. Ramirez,A.R. Kortan,E. Ozdas,H.E. Bair,K.M. Rabe,N. Kopylov,P.H. Cltrin,S. Schuppler,T. Siegrist		
109717	SSC0930327	mixture of A15(a=11.770) and bct (a=12.957, c=11.432A). Tc=40 K under 15 kbar.	Cs3C60	Cs3C60	Cs	3	C	60																					1995																												fullerene																		K		40					40																																																																																																					SUPERCONDUCTIVITY AT 40K IN CECIUM DOPED C60				Solid State Commun.,93(1995)327-330	B.R. Zegarski,O. Zhou,P.E. Sulewski,R.M. Fleming,T.T.M. Palstra,Y. Iwasa	C, CS	
109719	SSC0930269	not single phase.	Na2RbC60	Na2Rb1C60	Na	2	Rb	1	C	60																			1995																												CaTiO3			A	14.096													CaTiO3, perovskite	K		3.4					3.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109720	SSC0930269	not single phase.	Na2(Rb,Cs)C60	Na2Rb0.75Cs0.25C60	Na	2	Rb	0.75	Cs	0.25	C	60																	1995																																														K		5.2					5.2																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109721	SSC0930269	not single phase.	Na2(Rb,Cs)C60	Na2Rb0.5Cs0.5C60	Na	2	Rb	0.5	Cs	0.5	C	60																	1995																																														K		8.4					8.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109722	SSC0930269	not single phase.	Na2(Rb,Cs)C60	Na2Rb0.25Cs0.75C60	Na	2	Rb	0.25	Cs	0.75	C	60																	1995																																														K		9.4					9.4																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109723	SSC0930269	not single phase.	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			1995																																														K		11.7					11.7																																																																																																					FULLERIDE SUPERCONDUCTORYS AND ORIENTATIONAL ORDER: Tc VS LATTICE CONSTANT IN Na2RbxCs1-xC60				Solid State Commun.,93(1995)269-274	C.L. Lin,C.L.Lin,J.E. Fischer,J.E.Fischer,P.W. Stephens,P.W.Stephens,R. Dinnebier,R.Dinnebier,T. Yildirin,T.Yildirim	Na, Rb, Cs, C	
109724	PR05215534	space-G=Pcab	Sm3C60	C60Sm3	C	60	Sm	3																					1995																															A	28.17	28.07	28.27												K		8					8																																																																																																					Supercondutivity at 8 K in samarium-doped C60	199512			Phys.Rev.B,52(1995)15534	G. Roth,X.H. Chen		
109726	PR05215517	Hc1 defined as deviation from linear M-H curve.	K3C60	C60K3	C	60	K	3																					1995																												fullerene																		K		19.3					19.3											Oe		42																																																																																								Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
109727	PR05215517	Hc1 defined as deviation from linear M-H curve.	Rb3C60	C60Rb3	C	60	Rb	3																					1995																												fullerene																		K		30					30											Oe		32																																																																																								Magnetic properties of superconducting K3C60 and Rb3C60 synthesized From large single-crystal fullerenes	199512			Phys.Rev.B,52(1995)15517	J.Z. Liu,P. Klavins,R.N. Shelton,S.H. Irons		
109728	EPL0170175		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		27.5					27.5											Oe		250							T		58														A		23.5																																																															Magnetic properties of superconducting Rb3C60			Karlsruhe,Germany	Europhys.Lett. 17(1992)175	A.Gurevich,C.Politis,V.Buntar,W.Krauss		
109729	EPL0180079	density=1.91 g/cm3. measurements of EPL,NMR,susceptibility.	K3C60	C60K3	C	60	K	3																					1992																												fullerene																		K																																											A		26			A		2400																																																										Normal-state magnetic properties of K3C60			Univ. California, Los Angels	Europhys.Lett. 18(1992)79	F.Diederich,G.Gruner,J.-J.Andre,J.D.Thompson,K.Holczer,M.E.Hanson,P.Petit,R.B.Kaner,R.L.Whetten,S.-M.Huang,W.G.Clark,W.H.Wong		
109730	MPL0060351		Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K																											T		63.8							T/K		2.5					A		23			A		1400																																																										Penetration depth and coherence length in superconducting fullerene Rb3C60			Karlsruhe,Germany	Mod.Phys.Lett.B 6(1992)351	A.I.Sokolov,C.Politis,V.Buntar		
109731	MPL0061037	Hc1 defined as the deviation from linear M-H cuves. Jc(1T, 7K)=4E+6 A/cm2.	Rb3C60	C60Rb3	C	60	Rb	3																					1992																												fullerene																		K		28.5					28.5											mT		16.2																												nm		215																																																										Lower critical magnetic field of superconducting Rb3C60			Karlsruhe,Germany	Mod.Phys.Lett.B 6(1992)1037	C.Politis,U.Eckern,V.Buntar		
109732	NAT3520223		(CsTl2)C60	Cs1.2Tl2.4C60	Cs	1.2	Tl	2.4	C	60																			1991																												fullerene																		K		29.5					29.5																																																																																																react(220C,1h, in inert gas) of (CsTl2 + C60)					Superconductivity at 30K in cesium-doped C60	7		Department of Chemistry and Division of Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA	Nature 352(1991)223	Charles M. Lieber,Chia-Chun Chen,Stephen P. Kelty		
109733	NAT3520223		(Cs,Hg)3C60	Cs3Hg3.3C60	Cs	3	Hg	3.3	C	60																			1991																												fullerene																		K		29					29																																																																																																					Superconductivity at 30K in cesium-doped C60	7		Department of Chemistry and Division of Applied Sciences, Harvard University, Cambridge, Massachusetts 02138, USA	Nature 352(1991)223	Charles M. Lieber,Chia-Chun Chen,Stephen P. Kelty		
109734	P064212509	density = 2.63 g/cm3. grain size=1 - 5 um.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.2					38.2																																		MHIR9734																																																														high-pressure synthesis (3.5GPa,1000C in BN)					Electrical transport and anisotropic superconducting properties in single crystalline and dense polycrystalline MgB2			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 64(2001)212509	A.K.Pradhan,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
109735	P064212509	density = 2.63 g/cm3. grain size=50 -200 um. long grains	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.2					38.2																																		MHIR9735																																																														high-pressure synthesis (3.5GPa,1000C in BN)					Electrical transport and anisotropic superconducting properties in single crystalline and dense polycrystalline MgB2			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 64(2001)212509	A.K.Pradhan,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
109736	P064212509	anisotropy=3.0 from Hc2. values of Hc2,Dhc2/dT show for H//ab. Hc2(0),dHc2/dT are 4.8T, 0.17 for H//c. cohere(c)=27 A.	MgB2	B2Mg1	B	2	Mg	1																				3	2001																												AlB2																	AlB2, C32	K		38.2					38.2																				T		15							T/K		0.55			MHIR9736		A		82																																																										extracted from #9735 sample					Electrical transport and anisotropic superconducting properties in single crystalline and dense polycrystalline MgB2			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 64(2001)212509	A.K.Pradhan,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
109737	L087247003	gamma in mj/mol.K2. Tc = 0.14 K from sp-heat. Tc increases with pressure (Tc(max)=3.8K at p=2.7 GPa. sp-heat fitting for T<3K.	Ba6Ge25	Ba6Ge25	Ba	6	Ge	25																				1	2001																												clathrate			A	14.5564														K		0.24					0.24																				T		0.6							T/K		2.9					A		280																		mj/mol.K2	21		250																																										Superconductivity in the Filled Cage Compounds Ba6Ge25 and Ba4Na2Ge25			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, D-01187 Dresden, Germany	Phys.Rev.Lett., 87(2001)247003	C.Langhammer,F.Kromer,F.M.Grosche,F.Steglich,G.Sparn,H.Q.Yuan,M.Baenitz,S.Paschen,W.Carrillo-Cabrera,Yu.Grin		
109738	L087247003	gamma in mj/mol.K2.   sp-heat fitting for T<3K.	Ba4Na2Ge25	Ba4Na2Ge25	Ba	4	Na	2	Ge	25																		1	2001																												clathrate			A	14.4703														K		0.84					0.84																																																								mj/mol.K2	33		250																																										Superconductivity in the Filled Cage Compounds Ba6Ge25 and Ba4Na2Ge25			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, D-01187 Dresden, Germany	Phys.Rev.Lett., 87(2001)247003	C.Langhammer,F.Kromer,F.M.Grosche,F.Steglich,G.Sparn,H.Q.Yuan,M.Baenitz,S.Paschen,W.Carrillo-Cabrera,Yu.Grin		
109739	P064214514		(Cu,Zn)Ir2S4	Cu0.8Zn0.2Ir2S4	Cu	0.8	Zn	0.2	Ir	2	S	4																	2001							-1.7																					spinel			A	9.8792														K		3.32					3.32																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109740	P064214514	Hc1 is for T=2K. Hc2(0) estimated by assuming WHH theory using Hc2(2K)=2.0 T.	(Cu,Zn)Ir2S4	Cu0.7Zn0.3Ir2S4	Cu	0.7	Zn	0.3	Ir	2	S	4																	2001																												spinel			A	9.8934														K		3.05					3.05											Oe		300							T		3.5																																																																															Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109741	P064214514		(Cu,Zn)Ir2S4	Cu0.6Zn0.4Ir2S4	Cu	0.6	Zn	0.4	Ir	2	S	4																1	2001																												spinel			A	9.9058														K		2.61					2.61																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109742	P064214514		(Cu,Zn)Ir2S4	Cu0.5Zn0.5Ir2S4	Cu	0.5	Zn	0.5	Ir	2	S	4																1	2001																												spinel			A	9.9199														K		2.19					2.19																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109743	P064214514		(Cu,Zn)Ir2S4	Cu0.4Zn0.6Ir2S4	Cu	0.4	Zn	0.6	Ir	2	S	4																1	2001																												spinel			A	9.9336														K		1.73					1.73																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109744	P064214514		(Cu,Zn)Ir2S4	Cu0.3Zn0.7Ir2S4	Cu	0.3	Zn	0.7	Ir	2	S	4																1	2001																												spinel			A	9.9469														K		1.36					1.36																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109745	P064214514		(Cu,Zn)Ir2S4	Cu0.2Zn0.8Ir2S4	Cu	0.2	Zn	0.8	Ir	2	S	4																1	2001																												spinel			A	9.9584														K		0.47					0.47																																																																																																					Suppression of metal-to-insulator transition and appearance of superconductivity in Cu1-xZnxIr2S4			National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 64(2001)214514	G.Cao,H.Kitazawa,H.Suzuki,T.Furubayashi,T.Matsumoto,Y.Uwatoko		
109746	APL0791154	Hc2(T) is the same as x=0.1 sample(num=9749)	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		38.6					38.6																																		MHIR9746																																																														solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109747	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix.	(Mg,Ti)B2	Mg0.99Ti0.01B2	Mg	0.99	Ti	0.01	B	2																			2001																												AlB2																	AlB2, C32	K		38.6					38.6																																																																																																solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109748	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix.	(Mg,Ti)B2	Mg0.95Ti0.05B2	Mg	0.95	Ti	0.05	B	2																			2001																												AlB2																	AlB2, C32	K		38.5					38.5																																																																																																solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109749	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix.	(Mg,Ti)B2	Mg0.9Ti0.1B2	Mg	0.9	Ti	0.1	B	2																			2001																												AlB2																	AlB2, C32	K		38.3					38.3																																		MHIR9749																																																														solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109750	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix. Hc2(T) is the same as x=0.1 sample(num=9749).	(Mg,Ti)B2	Mg0.8Ti0.2B2	Mg	0.8	Ti	0.2	B	2																			2001																												AlB2																	AlB2, C32	K		37.8					37.8																																		MHIR9750																																																														solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109751	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix.	(Mg,Ti)B2	Mg0.6Ti0.4B2	Mg	0.6	Ti	0.4	B	2																			2001																												AlB2																	AlB2, C32	K		37.5					37.5																																																																																																solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109752	APL0791154	majority of doping Ti form impurity phase, not introduce in MgB2 matrix.	(Mg,Ti)B2	Mg0.4Ti0.6B2	Mg	0.4	Ti	0.6	B	2																			2001																												AlB2																	AlB2, C32	K		37.6					37.6																																																																																																solid state reaction at ambient pressure					High critical current density of MgB2 bulk superconductor doped with Ti and sintered at ambient pressure			ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)1154	C.H.Cheng,L.Zhou,M.Murakami,N.Koshizuka,T.Machi,Y.Feng,Y.Fudamoto,Y.Wu,Y.Zhao		
109753	NAT4120316	Pressure-induced s/c. Fe is superconducting at pressures between 15 and 30 GPa. Tc(max)=2 K at p=22 GPa. dTc/dP =0.4 K/GPa at Pc(=16 GPa).	Fe	Fe1	Fe	1																							2001																																														K		2			0		2	MTC9753		K/GPa	0.4																																																																																																	Superconductivity in the non-magnetic state of iron under pressure				Nature 412(2001)316	K.Amaya,K.Kotani,K.Shimizu,K.Takeda,S.Furumoto,T.Kimura,Y.Onuki		
109754	NAT4130831	Caution (Schon's FET data). single crystal of electric-field-doped C70. Tc(max) achieved for 4 electron/C70.	C70	C70	C	70																						3	2001																												fullerene			A	10.602		17.263												K		7					7	MTC9754																																																																																															grown from vapour phase					Superconductivity in single crystals of the fullerene C70				Nature 413(2001)831	B.Batlogg,C.Svensson,Ch.Kloc,J.H.Schon,M.Steigerwald,T.Siegrist		
109755	APL0791649	inner Ta, outer Cu tube. anisotropy factore = 1.3. H//means along wire direction .	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.3					38.3																				T		15							T/K		0.39			MHC9755		nm		4.5																																																										PIT method using Ta,Cu tube. sintered(900-950C in air)					Transport behavior and critical current densities in MgB2 wires			Superconductivity Research Laboratory, ISTEC, 1-10-13 Shinonome, Koto-ku, Tokyo 135-0062, Japan	Appl.Phys.Lett., 79(2001)1649	A.K.Pradhan,C.F.Liu,L.Zhou,N.Koshizuka,P.Ji,P.X.Zhang,S.J.Du,X.H.Liu,Y.Feng,Y.Zhao		
109756	SCI2932432	Caution (Schon's FET data). hole-doped sample (by FET). Tc shows Tc(max), which is obtained for hole/C60 = 3.2.	(CHBr3)C60	H1Br3C61	H	1	Br	3	C	61																			2001																												fullerene			A	14.43														K		115					115																																				A		18																																																										intercalation by solution method					High-temperature superconductivity in lattice-expanded C60				Science 293(2001)2432	B.Batlogg,Ch.Kloc,J.H.Schon		
109757	SCI2932432	Caution (Schon's FET data). hole-doped sample (by FET). Tc shows Tc(max), which is obtained for hole/C60 = 3.2.	(CHCl3)C60	H1Cl3C61	H	1	Cl	3	C	61																			2001																												fullerene			A	14.28														K		80					80																																				A		20																																																										intercalation by solution method					High-temperature superconductivity in lattice-expanded C60				Science 293(2001)2432	B.Batlogg,Ch.Kloc,J.H.Schon		
109758	SCI2932432	Caution (Schon's FET data). hole-doped sample (by FET). Tc shows Tc(max), which is obtained for hole/C60 = 3.2.	C60	C60	C	60																							2001																												fullerene																		K		50					50																																				A		40																																																															High-temperature superconductivity in lattice-expanded C60				Science 293(2001)2432	B.Batlogg,Ch.Kloc,J.H.Schon		
109759	P064220503	pressure-induced s/c. Coherence length at 15 kbar are 210, 140, 700 A for a-, b-, and c-axis, respectively.	UGe2	Ge2U1	Ge	2	U	1																				3	2001																																														K		0.258			0		0.258																																		MHC9759		A		210																																																															Anisotropy and pressure dependence of the upper critical field of the ferromagnetic superconductor UGe2			Departement de Recherche Fondamentale sur la Matie`re Condensee, SPSMS, CEA/Grenoble, 17 rue des Martyrs,  Grenoble Cedex, France		A.Huxley,D.Braithwaite,I.Sheikin,J.Flouquet,J.P.Brison,K.Miyake,S.Watanabe		
109760	P063144519	pressure-induced s/c. Tc=Tc(max)=0.752 K at p=12 kbar. S/c and ferro-  disappear at p=16 kbar.	UGe2	Ge2U1	Ge	2	U	1																				3	2001							53																																							K		0.752			0		0.752	MPH9760																																																																																															Czochralsky method + annealed					UGe2 : A ferromagnetic spin-triplet superconductor			SPSMS, CEA-Grenoble, Grenoble 38054, France	Phys.Rev.B, 63(2001)144519	A.Huxley,D.Braithwaite,E.Ressouche,I.Sheikin,J.Flouquet,N.Kernavanois,R.Calemczuk		
109761	PHB2811021	not s/c	LaFe4As12	La1Fe4As12	La	1	Fe	4	As	12																			2000																												skutterudite			A	8.3252														K					2																																																																																																		high-pressure synthesis					Electrical conductivity and superconductivity of LaT4As12(T=Fe, Ru and Os) withskutterudite-type structure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1021	A.Matsushita,C.Sekine,H.Takahashi,I.Shirotani,J.Tang,K.Ohno,T.Kawakami,T.Matsumoto,T.Nakanishi,T.Yagi		
109762	PHB2811021	dTc/dP in K/GPa	LaRu4As12	La1Ru4As12	La	1	Ru	4	As	12																			2000																												skutterudite			A	8.5081														K		10.3					10.3			K/GPa	-0.4																																																																																												high-pressure synthesis					Electrical conductivity and superconductivity of LaT4As12(T=Fe, Ru and Os) withskutterudite-type structure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1021	A.Matsushita,C.Sekine,H.Takahashi,I.Shirotani,J.Tang,K.Ohno,T.Kawakami,T.Matsumoto,T.Nakanishi,T.Yagi		
109763	PHB2811021		LaOs4As12	La1Os4As12	La	1	Os	4	As	12																			2000																												skutterudite			A	8.5437														K		3.2					3.2																																																																																																high-pressure synthesis					Electrical conductivity and superconductivity of LaT4As12(T=Fe, Ru and Os) withskutterudite-type structure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1021	A.Matsushita,C.Sekine,H.Takahashi,I.Shirotani,J.Tang,K.Ohno,T.Kawakami,T.Matsumoto,T.Nakanishi,T.Yagi		
109764	PHB2811024	density=9.098 g/cm3	Mo3P	Mo3P1	Mo	3	P	1																					2000																																														K		7					7																																																																																																high-pressure synthesis (1200-1700C,4GPa)					Superconductivity of molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1024	C.Sekine,I.Kaneko,I.Shirotani,M.Takeya,T.Yagi		
109765	PHB2811024	density=8.251 g/cm3	Mo8P5	Mo8P5	Mo	8	P	5																					2000																																														K		5.8					5.8																																																																																																high-pressure synthesis (1200-1700C,4GPa)					Superconductivity of molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1024	C.Sekine,I.Kaneko,I.Shirotani,M.Takeya,T.Yagi		
109766	PHB2811024	density=7.861 g/cm3	Mo4P3	Mo4P3	Mo	4	P	3																					2000																																														K		3					3																																																																																																high-pressure synthesis (1200-1700C,4GPa)					Superconductivity of molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Physica B, 281-282(2000)1024	C.Sekine,I.Kaneko,I.Shirotani,M.Takeya,T.Yagi		
109767	SSC1080967		TiRhSi	Ti1Rh1Si1	Ti	1	Rh	1	Si	1																			1998																															A	6.248	7.234	3.816												K		5.1					5.1																																																																																																high-pressure synthesis (1600,4GPa)					Superconductivity of MRhSi (M=Ti,Zr, and Hf) prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 108(1998)967	C.Sekine,I.Shirotani,S.Todo,T.Yagi,Y.Konno,Y.Okada		
109768	SSC1080967		ZrRhSi	Zr1Rh1Si1	Zr	1	Rh	1	Si	1																			1998																															A	6.549	7.459	3.918												K		10.3					10.3																																																																																																high-pressure synthesis (1200-1600C,4GPa)					Superconductivity of MRhSi (M=Ti,Zr, and Hf) prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 108(1998)967	C.Sekine,I.Shirotani,S.Todo,T.Yagi,Y.Konno,Y.Okada		
109769	SSC1080967		HfRhSi	Hf1Rh1Si1	Hf	1	Rh	1	Si	1																			1998																															A	6.476	7.415	3.901												K		2.3					2.3																																																																																																high-pressure synthesis (1200-1600C,4GPa)					Superconductivity of MRhSi (M=Ti,Zr, and Hf) prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 108(1998)967	C.Sekine,I.Shirotani,S.Todo,T.Yagi,Y.Konno,Y.Okada		
109770	PR05206197	synthesis of single phase of h-ZrRuSi is difficult.	h-ZrRuSi	Zr1Ru1Si1	Zr	1	Ru	1	Si	1																			1995																															A	6.6812		3.6715												K		12					12																				T		1														A		181.5																																																										high-pressure synthesis (1400,4GPa)					Superconductivity of ZrRuSi prepared at high pressure	199509			Phys.Rev.B,52(1995)6197	Ichimin Shirotani,Kazushi Kanoda,Keiki Takeda,Kenji Tachi,Sakae Todo,Takehiko Yagi	Zr, Ru, Si	
109771	PR05206197	synthesis of single phase of o-ZrRuSi is difficult.	o-ZrRuSi	Zr1Ru1Si1	Zr	1	Ru	1	Si	1																			1995																												Co2P																		K		5					5																																																																																																high-pressure synthesis (950,4GPa)					Superconductivity of ZrRuSi prepared at high pressure	199509			Phys.Rev.B,52(1995)6197	Ichimin Shirotani,Kazushi Kanoda,Keiki Takeda,Kenji Tachi,Sakae Todo,Takehiko Yagi	Zr, Ru, Si	
109772	SSC1040217		ZrNi4P2	Zr1Ni4P2	Zr	1	Ni	4	P	2																			1997																															A	6.944		3.576												K					2																																																																																																		high-pressure synthesis (1100C,4GPa)					Electrical conductivity and superconductivity of ZrNi4P2 and ZrRu4P2 prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 104(1997)217	C.Sekine,G.Iwasaki,I.Kaneko,I.Shirotani,S.Todo,T.Yagi		
109773	SSC1040217	density=9.894	ZrRu4P2	Zr1Ru4P2	Zr	1	Ru	4	P	2																			1997																															A	6.992		3.699												K		11					11																				T		12.2												MHC9773		A		52																																																										high-pressure synthesis (850C,4GPa)					Electrical conductivity and superconductivity of ZrNi4P2 and ZrRu4P2 prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 104(1997)217	C.Sekine,G.Iwasaki,I.Kaneko,I.Shirotani,S.Todo,T.Yagi		
109774	SSC1040217		HfRu4P2	Hf1Ru4P2	Hf	1	Ru	4	P	2																			1997																																														K		9.5					9.5																																																																																																high-pressure synthesis (850C,4GPa)					Electrical conductivity and superconductivity of ZrNi4P2 and ZrRu4P2 prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Japan	Solid State Commun., 104(1997)217	C.Sekine,G.Iwasaki,I.Kaneko,I.Shirotani,S.Todo,T.Yagi		
109775	IST990101		MoNiP	Mo1Ni1P1	Mo	1	Ni	1	P	1																			2000																												Fe2P			A	5.858		3.668												K		15.5					15.5																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109776	IST990101		MoRuP	Mo1Ru1P1	Mo	1	Ru	1	P	1																			2000																												Co2P			A	6.035	6.944	3.857												K		15.5					15.5																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109777	IST990101		h-ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			2000																												Fe2P			A	6.459		3.778												K		13					13																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109778	IST990101		h-ZrRuSi	Zr1Ru1Si1	Zr	1	Ru	1	Si	1																			2000																												Fe2P			A	6.684		3.672												K		12.2					12.2																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109779	IST990101		o-ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			2000																												Co2P			A	6.417	7.323	3.862												K		4					4																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109780	IST990101		ZrRhSi	Zr1Rh1Si1	Zr	1	Rh	1	Si	1																			2000																												Co2P			A	6.549	7.459	3.918												K		10.5					10.5																																																																																																high-pressure synthesis (4GPa,1500-1700C in BN crucible)					High pressure synthesis of new superconductors MoNiP and MoRuP with Tc of about 15 K			Muroran Institute of Technology, Muroran,Hokkaido, Japan	Advances in Superconductivity, 12(2000)101	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
109781	JPS0702248	values in table are for H//[100]. Hc2(0)=49.5 kOe, -dHc2/dT=110 kOe/K, cohere=35 A, G-L=50 for H//[001]. delta-C/gamma.Tc=4.7. gamma in mj/mol.K2. G-L parameter = 108	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																			2001																																														K		2.25					2.25																				kOe			116						kOe/K		240					A		82															MSP9781			mj/mol.K2	820																																							self-flux method					Unconventional superconductivity in CeCoIn5 studied by the specific heat and magnetization measurements			Osaka University, Toyonaka, Osaka, Japan	J.Phys. Soc. Jpn, 70(2001)2248	D.Aoki,H.Harima,H.Sato,H.Shishido,M.Nakashima,R.Settai,S.Ikeda,T.Namiki,Y.Aoki,Y.Haga,Y.Onuki		
109782	P065014506		CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2002							-60																					HoCoGa5			A	4.6627		7.5373												K																																																																																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109783	P065014506	gamma in mj/mol.K2.	Ce(Rh,Co)In5	Ce1Rh0.8Co0.2In5	Ce	1	Rh	0.8	Co	0.2	In	5																3	2002								3.7																				HoCoGa5			A	4.6512		7.5415												K																																																															mj/mol.K2	340																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109784	P065014506	gamma in mj/mol.K2. delta-C=340 mj/mol.K. delta-C/gamma*Tc=0.7	Ce(Rh,Co)In5	Ce1Rh0.6Co0.4In5	Ce	1	Rh	0.6	Co	0.4	In	5																3	2002							-50	3.6																				HoCoGa5			A	4.6469		7.5423												K		1.5					1.5																																																								mj/mol.K2	320																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109785	P065014506	gamma in mj/mol.K2. delta-C=580 mj/mol.K. delta-C/gamma*Tc=0.7	Ce(Rh,Co)In5	Ce1Rh0.5Co0.5In5	Ce	1	Rh	0.5	Co	0.5	In	5																3	2002							-60	3.2																				HoCoGa5			A	4.6342		7.5546												K		1.4					1.4																																																								mj/mol.K2	580																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109786	P065014506	gamma in mj/mol.K2. delta-C=1560 mj/mol.K. delta-C/gamma*Tc=1.8	Ce(Rh,Co)In5	Ce1Rh0.4Co0.6In5	Ce	1	Rh	0.4	Co	0.6	In	5																3	2002								2.9																				HoCoGa5			A	4.6304		7.5504												K		1.43					1.43																																																								mj/mol.K2	620																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109787	P065014506	gamma in mj/mol.K2. delta-C=1540 mj/mol.K. delta-C/gamma*Tc=1.3	Ce(Rh,Co)In5	Ce1Rh0.3Co0.7In5	Ce	1	Rh	0.3	Co	0.7	In	5																3	2002							-70																					HoCoGa5			A	4.6285		7.5515												K		1.42					1.42																																																								mj/mol.K2	820																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109788	P065014506	gamma in mj/mol.K2. delta-C=1720 mj/mol.K. delta-C/gamma*Tc=1.5	Ce(Rh,Co)In5	Ce1Rh0.2Co0.8In5	Ce	1	Rh	0.2	Co	0.8	In	5																3	2002							-60																					HoCoGa5			A	4.6208		7.5508												K		1.57					1.57																																																								mj/mol.K2	720																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109789	P065014506	gamma in mj/mol.K2. delta-C=3890 mj/mol.K. delta-C/gamma*Tc=4.9	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5			A	4.6154		7.5531												K		2.27					2.27																																																								mj/mol.K2	350																																							flux method (5C/h from 1100C to 600C)					Coexistence of superconductivity and antiferromagnetism in CeRh1-xCoxIn5			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego,La Jolla, California	Phys.Rev.B, 65(2002)14506	C.Sirvent,E.D.Bauer,E.J.Freeman,J.Petricka,M.B.Maple,N.A.Frederick,R.P.Dickey,V.S.Zapf		
109790	P065014514		CeCo2	Ce1Co2	Ce	1	Co	2																				1	2002																																														K		0.82					0.82											Oe		75							T		0.275							T/K		0.45					A		481			A		2914																																																					arc-melt + ANN(900C,1 week)					Anomalous behavior in the superconducting state of CeCo2			Department of Physics and Institute of Basic Science, Sung Kyun Kwan University, Suwon 440-746, Korea		J.-G.Park,K.A.McEwen,P.C.Canfield,Seok-Hoon Lee		
109791	P065014514		CeCo2	Ce1Co1.95	Ce	1	Co	1.95																				1	2002																																														K		0.87					0.87																																																																																																arc-melt + ANN(900C,1 week)					Anomalous behavior in the superconducting state of CeCo2			Department of Physics and Institute of Basic Science, Sung Kyun Kwan University, Suwon 440-746, Korea		J.-G.Park,K.A.McEwen,P.C.Canfield,Seok-Hoon Lee		
109792	P065014514	containing ferromag-impurities. values of s/c properties are at T=0.4 K.	CeCo2	Ce1Co1.85	Ce	1	Co	1.85																				1	2002																																														K		0.86					0.86																																																																																																arc-melt + ANN(900C,1 week)					Anomalous behavior in the superconducting state of CeCo2			Department of Physics and Institute of Basic Science, Sung Kyun Kwan University, Suwon 440-746, Korea		J.-G.Park,K.A.McEwen,P.C.Canfield,Seok-Hoon Lee		
109793	P065014514		CeCo2	Ce1Co2	Ce	1	Co	2																				3	2002																																														K		1.29					1.29																																																																																																flux method					Anomalous behavior in the superconducting state of CeCo2			Department of Physics and Institute of Basic Science, Sung Kyun Kwan University, Suwon 440-746, Korea		J.-G.Park,K.A.McEwen,P.C.Canfield,Seok-Hoon Lee		
109794	P065020504	pressure-induced s/c. Tc-value represent Tc(max). phase diagram investigated by In<115>NQR	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2002																												HoCoGa5																		K		2.23			0		2.23	MPH9794																																																																																															self-flux method					Pressure-temperature phase diagram of antiferromagnetism and superconductivity in CeRhIn5 and CeIn3 : <115> In-NQR study under pressure			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 65(2002)20504	C.Thessieu,D.Aoki,G.-q.Zheng,K.Ishida,R.Settai,S.Araki,S.Kawasaki,T.C.Kobayashi,T.Mito,T.Muramatsu,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
109795	P065020504	pressure-induced s/c. Tc-value represent Tc(max). phase diagram investigated by In<115>NQR	CeIn3	Ce1In3	Ce	1	In	3																				3	2002																																														K		0.2			0		0.2	MPH9795																																																																																															Czochralski					Pressure-temperature phase diagram of antiferromagnetism and superconductivity in CeRhIn5 and CeIn3 : <115> In-NQR study under pressure			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 65(2002)20504	C.Thessieu,D.Aoki,G.-q.Zheng,K.Ishida,R.Settai,S.Araki,S.Kawasaki,T.C.Kobayashi,T.Mito,T.Muramatsu,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
109796	P065024505	Tc defined as R=0. bulk modulus=200 GPa	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	2002								10.8																				LuNi2B2C																		K		4.8					4.8	MTC9796		K/GPa	-0.7																																																																																																	High-pressure effects in single crystals: RNi2B2C (R=Dy, Pr )			Instituto de Investigaciones en Materiales, Universidad Nacional Autonoma de Mexico, Apartado Postal 70-360, Mexico D.F.,Mexico	Phys.Rev.B, 65(2002)24505	A.Duran,R.Escudero,R.Falconi		
109797	P065024520	dTn/dp = 0.48 K/GPa (Neel Temp).	(Ho,Dy)Ni2B2C	Ho0.9Dy0.1Ni2B2C1	Ho	0.9	Dy	0.1	Ni	2	B	2	C	1														3	2002																												LuNi2B2C																		K		8.15					8.15	MPH9797		K/GPa	-0.64																																																																																												high temp-Ni2B flux method + ANN(950C,6h)					Effect of pressure on the superconductivity and magnetism of Ho1-xDyxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science		Eun-Mi Choi,Hyeonjin Doh,Jae-Hyuk Choi,M.Ohashi,N.Mori,Sung-Ik Lee		
109798	P065024520	dTc/dp and dTn/dp = 0.5 K/GPa (Neel Temp) are estimated from Fig. Tn(p=0 GPa) not shown.	(Ho,Dy)Ni2B2C	Ho0.6Dy0.4Ni2B2C1	Ho	0.6	Dy	0.4	Ni	2	B	2	C	1														3	2002								6.92																				LuNi2B2C																		K		5.92					5.92	MPH9798		K/GPa	0																																																																																												high temp-Ni2B flux method + ANN(950C,6h)					Effect of pressure on the superconductivity and magnetism of Ho1-xDyxNi2B2C			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science		Eun-Mi Choi,Hyeonjin Doh,Jae-Hyuk Choi,M.Ohashi,N.Mori,Sung-Ik Lee		
109799	PR05112644	dTc/dP = 0.07 K/kbar. dTn/dp = 0.25 K/kbar  (Neel Temp).	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	1995								5																				LuNi2B2C																		K		8.4					8.4			K/GPa	0.7																														MHC9799																									348																																										Pressure effects and specific heat in superconducting HoNi2B2C	199505		AT&T Bell Laboratories,Mountain Avenue,Murray Hill,New Jersey 07974	Phys.Rev.B.,51(1995)12644-12648	B.Batlogg,J.J.Krajewski,R.J.Cava,S.A.Carter,W.F.Peck,Jr,W.F.Peck,Jr.		
109800	SSC1190491	s/c volume fraction is very small.	MgC(Ni,Co)3	Mg1Co1Ni2.97Co0.03	Mg	1	Co	1	Ni	2.97	Co	0.03																	2001																												CaTiO3																	CaTiO3, perovskite	K		6.7					6.7																																																																																																					The suppression of superconductivity in MgCNi3 by Ni-site doping			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton, NJ,USA	Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109801	SSC1190491	s/c volume fraction is very small.	MgC(Ni,Co)3	Mg1Co1Ni2.94Co0.06	Mg	1	Co	1	Ni	2.94	Co	0.06																	2001																												CaTiO3																	CaTiO3, perovskite	K		6					6																																																																																																					The suppression of superconductivity in MgCNi3 by Ni-site doping			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton, NJ,USA	Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109802	SSC1190491	s/c volume fraction is very small.	MgC(Ni,Co)3	Mg1Co1Ni2.91Co0.09	Mg	1	Co	1	Ni	2.91	Co	0.09																	2001																												CaTiO3																	CaTiO3, perovskite	K		6					6																																																																																																					The suppression of superconductivity in MgCNi3 by Ni-site doping			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton, NJ,USA	Solid State Commun., 119(2001)491	A.P.Ramirez,K.A.Regan,K.Inumaru,M.A.Hayward,M.K.Haas,N.Rogado,R.J.Cava,T.He		
109803	PLA0770487		GdMo6Se8	Gd1.2Mo6Se8	Gd	1.2	Mo	6	Se	8																			1980								0.75																				Chevrel																		K		5.6					5.6																																																																																																					Coexistence of superconductivity and long-range antiferromagnetic order in  Gd1.2Mo6Se8			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA, USA	Physics Letters, 77A(1980)487	C.F.Majkrzak,D.E.Moncton,G.Shirane,L.D.Woolf,M.B.Maple,W.Thomlinson		
109804	PHC2290315	dTc/dP in K/GPa.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.462		10.629												K		16.1					16.1			K/GPa	0.188																																																																																												arc-melt + ANN					Effect of pressure on superconductivity in the quaternary compounds RENi2B2C (RE=Lu,Y,Tm,Er,Ho)	199408			Physica C, 229(1994)315-319	H.F.Braun,H.Schmidt,H.Schumidt	Lu,Y,Tm,Er,Ho,Ni,C,B	
109805	PHC2290315	dTc/dP in K/GPa.	TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.484		10.579												K		10					10			K/GPa	-0.176																																																																																												arc-melt + ANN					Effect of pressure on superconductivity in the quaternary compounds RENi2B2C (RE=Lu,Y,Tm,Er,Ho)	199408			Physica C, 229(1994)315-319	H.F.Braun,H.Schmidt,H.Schumidt	Lu,Y,Tm,Er,Ho,Ni,C,B	
109806	PHC2290315	dTc/dP in K/GPa.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.5		10.553												K		10.4					10.4			K/GPa	-0.082																																																																																												arc-melt + ANN					Effect of pressure on superconductivity in the quaternary compounds RENi2B2C (RE=Lu,Y,Tm,Er,Ho)	199408			Physica C, 229(1994)315-319	H.F.Braun,H.Schmidt,H.Schumidt	Lu,Y,Tm,Er,Ho,Ni,C,B	
109807	PHC2290315	dTc/dP in K/GPa.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.525		10.536												K		15.3					15.3			K/GPa	-0.058																																																																																												arc-melt + ANN					Effect of pressure on superconductivity in the quaternary compounds RENi2B2C (RE=Lu,Y,Tm,Er,Ho)	199408			Physica C, 229(1994)315-319	H.F.Braun,H.Schmidt,H.Schumidt	Lu,Y,Tm,Er,Ho,Ni,C,B	
109808	PHC2290315	two step diamagnetism (T1=7.1 K and T2=5.3 K)	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.515		10.518												K		7.1					7.1																																																																																																arc-melt + ANN					Effect of pressure on superconductivity in the quaternary compounds RENi2B2C (RE=Lu,Y,Tm,Er,Ho)	199408			Physica C, 229(1994)315-319	H.F.Braun,H.Schmidt,H.Schumidt	Lu,Y,Tm,Er,Ho,Ni,C,B	
109809	JPS0702255	anisotropy factor=2.7	MgB2	B2Mg1	B	2	Mg	1																				3	2001																												AlB2			A	3.0851		3.5201											AlB2, C32	K		38.3					38.3																																		MHC9809																																																														grown from (Mg-MgB2-BN) by high pressure synthesis (4-6 GPa, 1400-1700C)					Growth, structure analysis and anisotropic superconducting properties of MgB2 single crystals			ISTEC, Shinonome, Koto-ku, Tokyo,Japan	J.Phys. Soc. Jpn, 70(2001)2255	A.Yamamoto,H.Mori,S.Lee,S.Tajima,T.Masui,Y.Eltsev		
109810	SSC1200095	phase transition at about 160 K.	InV6S8	In1V6S8	In	1	V	6	S	8																			2001																												Nb3Te4																		K		3.9					3.9																																																																																																heat(V6S8+In) 773 K, 30d					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109811	SSC1200095	phase transition at about 160 K.	TlV6S8	Tl1V6S8	Tl	1	V	6	S	8																			2001																												Nb3Te4																		K		4.1					4.1																																																																																																(Tl,V,S) heat(1073K,5d, in sealed silica)					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109812	SSC1200095	phase transition at about 160 K.	KV6S8	K1V6S8	K	1	V	6	S	8																			2001																												Nb3Te4																		K		0.71					0.71																																																																																																by ion exchange method from TlV6S8.					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109813	SSC1200095	phase transition at about 160 K.	RbV6S8	Rb1V6S8	Rb	1	V	6	S	8																			2001																												Nb3Te4																		K		0.65					0.65																																																																																																by ion exchange method from TlV6S8.					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109814	SSC1200095	phase transition at about 160 K.	CsV6S8	Cs1V6S8	Cs	1	V	6	S	8																			2001																												Nb3Te4																		K		0.32					0.32																																																																																																by ion exchange method from TlV6S8.					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109815	SSC1200095	phase transition at about 160 K.	V6S8	S8V6	S	8	V	6																					2001																												Nb3Te4																		K		0.76					0.76																																																																																																deintercalation of Tl from TlV6S8.					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109816	SSC1200095	phase transition at about 160 K.	TlV6S8	Tl0.61V6S8	Tl	0.61	V	6	S	8																			2001																																														K		3.5					3.5																																																																																																					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109817	SSC1200095	phase transition at about 160 K.	TlV6S8	Tl0.26V6S8	Tl	0.26	V	6	S	8																			2001																																														K		0.74					0.74																																																																																																					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109818	SSC1200095		InV6S8	In0.63V6S8	In	0.63	V	6	S	8																			2001																																														K		0.95					0.95																																																																																																					Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109819	SSC1200095	not s/c	InV6S8	In0.46V6S8	In	0.46	V	6	S	8																			2001																																														K					0.02																																																																																																							Superconductivity and phase transition in quasi-one-dimensional sulfide AV6S8 (A=In, Tl, K, Rb, Cs)			Laboratory for Solid State Chemistry, Okayama University of Science, Okayama, Japan	Solid State Commun., 120(2001)95	K.Minami,T.Koyakumaru,T.Kusano,T.Ohtani,Y.Fujii,Y.Miyoshi		
109820	SSC1210073	nominal carbon x=1.25	MgCxNi3	Mg1C0.978Ni3	Mg	1	C	0.978	Ni	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		7.3					7.3																																																																																																MgCxNi3 + then adding Mg, heat(600C, 920C)					Carbon concentration dependence of the superconducting transition temperature and structure of MgCxNi3			NIST Center for Neutron Research, Gaithersburg, MD, USA	Solid State Commun., 121(2002)73	J.W.Lynn,Q.Huang,R.J.Cava,T.G.Amos,T.He		
109821	SSC1210073	nominal carbon x=0.95	MgCxNi3	Mg1C0.965Ni3	Mg	1	C	0.965	Ni	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		6.3					6.3																																																																																																MgCxNi3 + then adding Mg, heat(600C, 920C)					Carbon concentration dependence of the superconducting transition temperature and structure of MgCxNi3			NIST Center for Neutron Research, Gaithersburg, MD, USA	Solid State Commun., 121(2002)73	J.W.Lynn,Q.Huang,R.J.Cava,T.G.Amos,T.He		
109822	SSC1210073	nominal carbon x=0.9	MgCxNi3	Mg1C0.906Ni3	Mg	1	C	0.906	Ni	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		3.38					3.38																																																																																																MgCxNi3 + then adding Mg, heat(600C, 920C)					Carbon concentration dependence of the superconducting transition temperature and structure of MgCxNi3			NIST Center for Neutron Research, Gaithersburg, MD, USA	Solid State Commun., 121(2002)73	J.W.Lynn,Q.Huang,R.J.Cava,T.G.Amos,T.He		
109823	PHC3660073	Figure shows Tc(p) by measuring dc-sus(hydrostatic) and resistivity(quasi-hydrostatic)	MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.0849		3.5211											AlB2, C32	K		39					39			K/GPa	-1.18																																																																																												heat(950C,2h,in sealed Ta tube with 2 bar Ar)					Effect of pressure on the superconductivity of MgB2			Department of Physics, Brock University, St.Catharines, Ont., Canada	Physica C, 366(2002)73	F.S.Razavi,H.Ploczek,S.K.Bose		
109824	SSC1210165		InV6S8	In0.71V6S8	In	0.71	V	6	S	8																			2002																												Nb3Te4																		K		5.4					5.4											Oe		170							T		0.6														A		200			um		0.15																																																										Characteristic inter-grain superconducting transition in quasi-one-dimensional sulfide AV6S8 (A=In,Tl)			Department of Applied Physics, Faculty of Science, Okayama University of Science, Okayama, Japan	Solid State Commun., 121(2002)165	M.Sugino,S.Sunagawa,T.Koyakumaru,T.Ohtani,Y.Fujii,Y.Miyoshi		
109825	JPS0702876	Ferromag at 52 K. pressure induced s/c. Tc shows Tc(max), where it is at p=1.2 GPa.	UGe2	Ge2U1	Ge	2	U	1																					2001							52																																							K		0.72			0		0.72	MPH9825																																																																																																				Magnetic Properties of a Pressure-induced Superconductor UGe2			Department of Physical Science,Graduate School of Engineering Science,Osaka University,Toyonaka,Osaka	J.Phys.Soc.Jpn, 70(2001)2876	K.Amaya,K.Hanazono,K.Kindo,N.Metoki,N.Tateiwa,R.Settai,T.C.Kobayashi,T.Inoue,Y.Haga,Y.Koike,Y.Onuki		
109826	JPS0703362	pressure-induced s/c.  values of s/c properties  in table are for H//c-axis, under p=2.5 GPa.. G-L parameter = 50	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2001																												HoCoGa5																		K		2.25			0		2.25	MPH9826																			T		10.2							T/K		15					A		57																																																										In-flux method					Superconductivity of CeRhIn5 under High Pressure			Research Center for aterials Science under Extreme Conditions,Osaka University,Toyonaka,Osaka ,Japan	J.Phys.Soc.Jpn, 70(2001)3362	D.Aoki,H.Shishido,K.Amaya,K.Shimizu,N.Tateiwa,T.C.Kobayashi,T.Muramatsu,Y.Haga,Y.Onuki		
109827	P065052505	sample contains 20 % MgB2C2 phase.	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2002																												AlB2			A	3.055		3.524											AlB2, C32	K		32					32																																																																																																(Mg+B4C)-Ta foil - (600C,then 700C in Ar)					Effects of carbon doping on superconductivity in magnesium diboride			Department of Physics, University of California at Berkeley, Berkeley, California, USA	Phys.Rev.B, 65(2002)52505	A.Zettl,J.Cumings,W.Mickelson,W.Q.Han		
109828	P065052506	s/c observed for nominal 1.1<x<1.2, 1.2<y<1.50 in MgxCyNi3. (x=1.2, y=1.4) is the best. having inhomogeneous microstructure.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2002																												CaTiO3			A	3.83													CaTiO3, perovskite	K		7					7																																																																																																					Microstructural features of Mgx Cy Ni3 superconducting materials			Material Science Division, Brookhaven National Laboratory, Upton, New York , USA	Phys.Rev.B, 65(2002)52506	J.Q.Li,L.J.Wu,L.Li,Y.Zhu		
109829	P065064534	actual C-content = 0.97 by XRD. graph shows thermopower and thermal conductivity	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2002																												CaTiO3			A	3.8111													CaTiO3, perovskite	K		8					8																																																																						MTP9829																															Thermopower and thermal conductivity of superconducting perovskite MgCNi3			Structural Research Laboratory and Department of Physics, University of Science and Technology of China, Hefei, People? Republic of China	Phys.Rev.B, 65(2002)64534	B.M.Wu,C.H.Wang,H.S.Yang,L.Z.Cao,M.Yu,R.Fan,S.Y.Li,W.H.Zheng,W.Q.Mo,X.H.Chen,Y.M.Xiong		
109830	L088047002	single(0.35*0.22*0.1 mm3). values in table show cohere(ab), penet(ab). penet from susceptibility. gap=30 K(2.58 meV)	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38					38																																				A		55			A		1100					1.57																																																high pressure synthesis					Exponential Temperature Dependence of the Penetration Depth in Single Crystal MgB2			H. H. Wills Physics Laboratory, University of Bristol, Bristol, England	Phys.Rev.Lett., 88(2002)47002	A.Carrington,A.Yamamoto,F.Manzano,N.E.Hussey,S.Lee,S.Tajima		
109831	L088047005	penet(ab) from surface impedance.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																																														K		2.17					2.17																																									A		1900																																																										Microwave Conductivity and Penetration Depth in the Heavy Fermion Superconductor CeCoIn5			School of Physics and Astronomy, The University of Birmingham, Edgbaston, Birmingham, UK	Phys.Rev.Lett., 88(2002)47005	A.Sibley,C.E.Gough,I.R.Fisher,R.J.Ormeno,S.Sebastian		
109832	SSC0510671	structure not known. quasi two-dimensional. phase transition(CDW) at 24 K.	LiMo6O17	Li0.9Mo6O17	Li	0.9	Mo	6	O	17																		3	1984																												bronze																		K		1.89					1.89																																																																																																temperature gradient flux method					Quasi two dimensional electronic properties of the lithium molybdenum bronze, Li0.9Mo6O17			The State University of New Jersey, New Brunswick, NJ.USA	Solid State Commun., 51(1984)671	J.V.Waszczak,M.Croft,M.Greenblatt,R.Niefeld,W.H.McCarroll		
109833	CEM1320188	precise structure not known.	BaNb2Se5	Ba1Nb2Se5	Ba	1	Nb	2	Se	5																			1997																												BaTa2S5			A	3.4501		25.795												K		2.5					2.5																																																																																																sealed (Ba,Nb,Se) in silica tube, then heat(800C)					Phase transitions in quasi-one-dimensional selenide BaNbSe3 and superconductivity in BaNb2Se5			Okayama University of Science,Ridai-cho,Okayama,Japan	J.Solid State Chem., 132(1997)188	M.Takano,S.Honji,T.Ohtani		
109834	LES0300167	density=9.4 g/cm3. resistivity(RT)=213 microOhm.cm.	Ag2Pd3S	Ag2Pd3S1	Ag	2	Pd	3	S	1																			1973																																														K		1.13					1.13																																																																																																(Ag,Pd,S) - heat(1000C)					A superconducting ternary sulfide			Forschungsinstitut fur Edelmetalle und Metallchemie, Schwabisch Gmund, Germany	J.Less-Common Metals, 30(1973)167	Ch.J.Raub,H.R.Khan,H.Trunk		
109835	PCS0380355		AgSnSe2	Ag1Sn1Se2	Ag	1	Sn	1	Se	2																			1977																												NaCl			A	5.678														K		4.71					4.71																																																																																																melt(700-1000C)+ANN(500C)					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109836	PCS0380355		AgSnSe2	Ag0.95Sn1.05Se2	Ag	0.95	Sn	1.05	Se	2																			1977																												NaCl			A	5.695														K		5.28					5.28																																																																																																melt(700-1000C)+ANN(500C)					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109837	PCS0380355		AgSnSe2	Ag0.92Sn1.08Se2	Ag	0.92	Sn	1.08	Se	2																			1977																												NaCl			A	5.703														K		5.57					5.57																																																																																																melt(700-1000C)+ANN(500C)					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109838	PCS0380355		AgSnSe2	Ag0.85Sn1.15Se2	Ag	0.85	Sn	1.15	Se	2																			1977																												NaCl			A	5.726														K		6.23					6.23																																																																																																melt(700-1000C)+ANN(500C)					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109839	PCS0380355		AgSnSe2	Ag0.81Sn1.19Se2	Ag	0.81	Sn	1.19	Se	2																			1977																												NaCl			A	5.736														K		6.47					6.47																																																																																																melt(700-1000C)+ANN(500C)					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109840	PCS0380355		AgSn(Se,S)2	Ag1Sn1Se1.8S0.2	Ag	1	Sn	1	Se	1.8	S	0.2																	1977																												NaCl			A	5.673														K		5.79					5.79																																																																																																melt - ANN(400C9					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109841	PCS0380355		AgSn(Se,S)2	Ag0.9Sn1.1Se1.8S0.2	Ag	0.9	Sn	1.1	Se	1.8	S	0.2																	1977																												NaCl			A	5.693														K		6.79					6.79																																																																																																melt - quench					Superconducting and normal state properties of Ag1-xSn1+xSe2-y			University of California, San Diego, La Jolla,USA	J.Phys.Chem.Solids, 38(1977)355	D.C.Johnston,H.Adrian		
109842	PR0351452	"gamma in mj/mol.K2. Authors say ""UAuPt4 may be heavy-electron s/c."	UAuPt4	U1Au1Pt4	U	1	Au	1	Pt	4																			1987							-135																					AuBe5																	AuBe5, C15[b]	K																																																															mj/mol.K2	725																																												Formation and destruction of the heavy-electron ground state in U compounds with AuBe5 crystal structure			Eidgenossische Technische Hochschule Zurich-Honggerberg,Zurich,Switzerland	Phys.Rev.B, 35(1987)1452	E.Felder,H.R.Ott,H.Rudigier,J.D.Thompson,Z.Fisk		
109843	PRL0510312	gamma(in mj/mol.K2) and Debye-T from SP-curve fitting. Hc2(0) estimated using WHH theory.	U6Fe	Fe1U6	Fe	1	U	6																					1983																																														K		3.8					3.8																				kOe		89.7							kOe/K		34.2			MHC9843																						mj/mol.K2	145		115																																					arc-melting					Observation of High-Field Superconductivity of a Strongly Interacting Fermi Liquid in U6Fe			University of Kentucky, Lexington, Kentucky,USA	Phys.Rev.Lett., 51(1983)312	J.G.Huber,K.N.Yang,L.E.DeLong,M.B.Maple		
109844	PR0301583	RRR=150	UPt3	Pt3U1	Pt	3	U	1																				3	1984																																														K		0.52					0.52																				kOe		22.7							kOe/K		63			MHC9844		A		120																																																															Upper critical magnetic field of the heavy-fermion superconductor UPt3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego,California,USA	Phys.Rev.B, 30(1984)1583	G.R.Stewart,J.L.Smith,J.O.Willis,J.W.Chen,M.B.Maple,S.E.Lambert,Z.Fisk		
109845	APL0792779	MgB1.9 by EPMA. Hc1(0)=27.5 mT, Hc2(0)=9.2 T for H//c. Hc2(0) by linear extraporation. cohere<c>=25 A. Anisotropy=2.6. Resistivity well-fitted by a+bT+cT2.	MgB2	B2Mg1	B	2	Mg	1																				3	2001																												AlB2			A	3.072		3.404											AlB2, C32	K		38.6					38.6											mT		38.4							T		25.5														A		65																																																										vapor transport method					Anisotropy of superconductivity from MgB2 single crysdtals			National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Appl.Phys.Lett., 79(2001)2779	A.Matsushita,G.Kido,H.Abe,H.Kitazawa,J.Ye,K.Nishida,M.Xu,N.Tsuji,Y.Takano		
109846	APL0793983	impurity phase = ZrB2	(Mg,Zr)B2	Mg0.9Zr0.1B2	Mg	0.9	Zr	0.1	B	2																		1	2001																												AlB2																	AlB2, C32	K		37.3					37.3																																		MHC9846																																																														solid state reaction					Improvement of critical current density in MgB2 superconductors by Zr doping at ambient pressure			Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome, 1-chome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)3983	B.Q.Fu,C.H.Cheng,F.C.Liu,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.P.Sun,Y.Zhao		
109847	APL0793983	14% ZrB2 phase included.	(Mg,Zr)B2	Mg0.8Zr0.2B2	Mg	0.8	Zr	0.2	B	2																		1	2001																												AlB2																	AlB2, C32	K		37.3					37.3																																																																																																solid state reaction					Improvement of critical current density in MgB2 superconductors by Zr doping at ambient pressure			Superconductivity Research Laboratory, ISTEC, 10-13 Shinonome, 1-chome, Koto-ku, Tokyo 135, Japan	Appl.Phys.Lett., 79(2001)3983	B.Q.Fu,C.H.Cheng,F.C.Liu,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.P.Sun,Y.Zhao		
109848	APL0801019		Ca(Al,Si)2	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2002																												AlB2			A	4.1905		4.3992											AlB2, C32	K		7.7					7.7																																																																																																arc-melting in 0.06 MPa Ar					Superconductivity of Ca(Al0.5,Si0.5)2, a ternary silicide with the AlB2 -type structure			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Appl.Phys.Lett., 80(2002)1019	H.Abe,K.Nishida,M.Imai,T.Kimura		
109849	APL0801019	not s/c	CaAl2Si2	Ca1Al2Si2	Ca	1	Al	2	Si	2																			2002																																														K					2																																																																																																		arc-melting in 0.06 MPa Ar					Superconductivity of Ca(Al0.5,Si0.5)2, a ternary silicide with the AlB2 -type structure			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Appl.Phys.Lett., 80(2002)1019	H.Abe,K.Nishida,M.Imai,T.Kimura		
109850	PCS2757	Pressure induce s/c. Tc shows Tc(max) at p=8 GPa. Figure shows phase diagram.	beta-NaV2O5	Na0.33V2O5	Na	0.33	V	2	O	5																		3	2002																												bronze																		K		9			0		9	MPH9850																																																																																															self-flux method					Superconductivity under high pressure in beta(beta')-vanadium bronzes			Materials Design and Characterization Lab, Institute for Solid State Physics, University of Tokyo, Tokyo, Japan	J.Phys.Chem.Solids, 63(2002)951	M.Isobe,T.Yamauchi,Y.Ueda		
109851	NAT4130613	gamma in mj/mol.K2. ferromag-Tc = 9.5K. moment=0.42 m<B>/U. delta-C/gamma*Tc = 0.6.	URhGe	U1Rh1Ge1	U	1	Rh	1	Ge	1																			2001							9.5																					TiNiSi																		K		0.25					0.25																				kOe		7.1												MHC9851		A		180																		mj/mol.K2	160																																							RF-heating in pressurized Ar					Coexistence of superconductivity and ferromagnetism in URhGe			CEA, Departement de Recherche Fondamentale sur la Matiere Condensee, SPSMS, Grenoble Cedex, France	Nature , 413(2001)613	Andrew Huxley,C.Paulsen,D.Braithwaite,Dai Aoki,E.Lhotel,Eric Ressouche,J.Flouquet,J.P.Brison		
109852	SSC1210575	penet calculated from Hc1. density=0.67 g/cm3. G-L parameter = 50	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		38.6					38.6											Oe		120							T		12.5														A		46			A		2300																																																					wrapped(Ta), then heat(925C, in sealed quartz)					Thermal fluctuation and upper critical field of MgB2 superconductor			Department of Physics, National Hsing University, Taichung,Taiwan,ROC	Solid State Commun., 121(2002)575	J.J.Cheng,M.D.Lan,P.L.Tsai,Y.L.Chang		
109853	P065094510	Theoretical candidate for high-Tc s/c. Interatomic distance=1.51 a<B>, too large.	Li2BeH4	Li2Be1H4	Li	2	Be	1	H	4																			2002																																														K					5																																																																																																		Ashby & Prasad method					Magnetic properties of LiBeH3 and Li2BeH4			Physics Department, Purdue University, West Lafayette, Indiana,USA	Phys.Rev.B, 65(2002)94510	L.Messerle,M.McElfresh,P.Metcalf,S.Li,V.Souw		
109854	P065094510	Theoretical candidate for high-Tc s/c. Interatomic distance=1.64 a<B>, too large.	LiBeH3	Li1Be1H3	Li	1	Be	1	H	3																			2002																																														K					5																																																																																																		Ashby & Prasad method					Magnetic properties of LiBeH3 and Li2BeH4			Physics Department, Purdue University, West Lafayette, Indiana,USA	Phys.Rev.B, 65(2002)94510	L.Messerle,M.McElfresh,P.Metcalf,S.Li,V.Souw		
109855	P065094512	penet<ab> by muon-SR. two gap analysis (2*delta/kTc = 3.6 and 1.6)	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2			A	3.0853		3.5238											AlB2, C32	K		38.2					38.2																																									A		1000					3.6																																																reaction(850C,2d, in Ar)					Muon spin relaxation study of the magnetic penetration depth in MgB2			Universitat Konstanz, Fachbereich Physik, D-78457 Konstanz, Germany	Phys.Rev.B, 65(2002)94512	C.Bernhard,Ch.Niedermayer,K.Ahn,P.K.Kremer,T.Holden		
109856	P065100510	RRR=5. Debye-T was obtained using Bloch-Gruneizen equation for R(T). anisotropy factor = 3.0 (Hc2 at 32K)	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2			A	3.09													AlB2, C32	K		38					38																																																											1100																																					slow cool (1050C to 700C within 5 - 15 days)					Superconducting properties of well-shaped MgB2 single crystals			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang, Republic of Korea	Phys.Rev.B, 65(2002)100510	C.U.Jung,Eun-Mi Choi,Gun Yong Sung,Heon-Jung Kim,Hyun-Sook Lee,J.Y.Kim,Jae-Hyuk Choi,Jeong Yong Lee,Kijoon H.P.Kim,Min-Seok Park,Mun-Seog Kim,P.Chowdhury,Sung-IK Lee,W.N.Kang,Zhonglian Du		
109857	P065100506	Skutterudite structure. RRR=33. moment = 2.97 mu-B. gamma in mj/mol.K2	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2002							-16																					skutterudite			A	9.3017													LaFe4P12	K		1.85					1.85																				T		2.45							T/K		1.9					A		116																		mj/mol.K2	350		304																																					Sb flux method					Superconductivity and heavy fermion behavior in PrOs4Sb12			Department of Physics and Institute For Pure and Applied Physical Sciences, University of California, San Diego, La Jolla,California,USA	Phys.Rev.B, 65(2002)100506	E.D.Bauer,M.B.Maple,N.A.Frederick,P.-C.Ho,V.S.Zapf		
109858	L087147001	23 wt%S-C comosites.H(Tc) was observed in M-H curves. Resistivity not to zero .	S-C	C0.9S0.1	C	0.9	S	0.1																					2001																																		6.709												K		35					35																																																																																																press then heat(650K,1h, in Ar) + ANN(400K,10h)					Indication of Superconductivity at 35 K in Graphite-Sulfur Composites			"Instituto Fisica ""Gleb Wataghin"" Universidade Estadual de Campinas, Unicamp,Campinas, San Paulo, Brasil"	Phys.Rev.Lett., 87(2001)147001	J.H.S.Torres,R.Ricardo da Ailva,Y.Kopelevich		
109859	PR05216165	Data from specific heat measurements. delta-C=460 mj/mol.K. delta-C/gamma*Tc=1.77. thermodynamic Hc(0)=0.229T.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		14.25					14.25																																																4.2	11							mj/mol.K2	18.2		490																																					HF-induction + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109860	PR05216165	Data from specific heat measurements. delta-C=693 mj/mol.K. delta-C/gamma*Tc=2.21. thermodynamic Hc(0)=0.306T.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K		16.1					16.1																																																4.4	11							mj/mol.K2	19.5		360																																					HF-induction + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109861	PR05216165	not single phase	LaNi2B2C	La1Ni2B2C1	La	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C																		K																																																															mj/mol.K2	8.4		495																																					HF-induction + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109862	PR05216165	Data from specific heat measurements. delta-C=120 mj/mol.K. delta-C/gamma*Tc=1.8. thermodynamic Hc(0)=0.10T.	La(Pt,Au)2B2C	La1Pt1.5Au0.5B2C1	La	1	Pt	1.5	Au	0.5	B	2	C	1															1995																												LuNi2B2C																		K		10.65					10.65																																																4.2	11							mj/mol.K2	6.4		250																																					HF-induction + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109863	PR05216165	not s/c	YCo2B2	Y1Co2B2	Y	1	Co	2	B	2																			1995																												LuNi2B2C																		K																																																															mj/mol.K2	6.7		570																																					HF-induction + ANN(1050C,24h)					Specific-heat analysis of rare-earth transition-metal borocarbides: An estimation of the electron-phonon coupling strength	199512			Phys.Rev.B,52(1995)16165	C. Dusek,C.Dusek,G. Hilscher,G.Hilscher,H. Michor,H.Michor,T. Holubar,T.Holubar		
109864	P065132517	Dens=2.66 g/cm3. Bulk modulus=114 GPa, Shear modulus=136.6 GPa, Young's modulus=292.8 GPa.	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2			A	3.086		3.522											AlB2, C32	K		39					39																																																																																																HIP					Ultrasound studies of MgB2 superconductor under hydrostatic pressure			Laboratory for Extreme Condition Physics, Institute of Physics and Center for Condensed Matter Physics,		Chang-Qing Jin,Feng-Ying Li,Jia-Lin Zhu,Liang-Chen Chen,Ri-Cheng Yu,Ru-Ju Wang,Shao-Chun Li,Zhen-Xing Liu		
109865	P065134508	c-axis oriented film. RRR=3. Hall effect measured at 5T. RH(100K)=3.0 E-11 m3/C. cot(Hall angle) obeys T**2 law above 130K.	MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2																	AlB2, C32	K		39.2					39.2																																																																																											MRH9865					pulsedlaser on Al2O3(1,-1,0,2) single crystal					Hall effect in c-axis-oriented MgB2 thin films			National Creative Research Initiative Center for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang, Republic of Korea	Phys.Rev.B, 65(2002)134508	Eun-Mi Choi,H.S.Lee,Heon Jung Kim,Hyeong-Jin Kim,Kijoon H.P.Kim,Sung-Ik Lee,W.N.Kang		
109866	P065132505		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.0857		3.5327											AlB2, C32	K		38.4					38.4																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109867	P065132505		(Mg,Al)B2	Mg0.95Al0.05B2	Mg	0.95	Al	0.05	B	2																			2002																												AlB2			A	3.0796		3.5265											AlB2, C32	K		36.3					36.3																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109868	P065132505	phase separation. another phase c=3.4622.	(Mg,Al)B2	Mg0.91Al0.09B2	Mg	0.91	Al	0.09	B	2																			2002																												AlB2			A	3.0796		3.5143											AlB2, C32	K		34.7					34.7																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109869	P065132505	phase separation. another phase c=3.4408.	(Mg,Al)B2	Mg0.81Al0.19B2	Mg	0.81	Al	0.19	B	2																			2002																												AlB2			A	3.0765		3.4959											AlB2, C32	K		30.8					30.8																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109870	P065132505		(Mg,Al)B2	Mg0.75Al0.25B2	Mg	0.75	Al	0.25	B	2																			2002																												AlB2			A	3.0765		3.4286											AlB2, C32	K		28					28																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109871	P065132505		(Mg,Al)B2	Mg0.71Al0.29B2	Mg	0.71	Al	0.29	B	2																			2002																												AlB2			A	3.0643		3.401											AlB2, C32	K		24					24																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109872	P065132505		(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																			2002																															A	3.0582		3.3888												K		14.6					14.6																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109873	P065132505	MgAlB4 superstructure.	(Mg,Al)B2	Mg0.5Al0.5B2	Mg	0.5	Al	0.5	B	2																			2002																															A	3.052		3.3704												K		12.9					12.9																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109874	P065132505	MgAlB4 superstructure.	(Mg,Al)B2	Mg0.4Al0.6B2	Mg	0.4	Al	0.6	B	2																			2002																															A	3.0429		3.3643												K		12					12																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109875	P065132505	MgAlB4 superstructure.	(Mg,Al)B2	Mg0.31Al0.69B2	Mg	0.31	Al	0.69	B	2																			2002																															A	3.0367		3.3643												K		11.1					11.1																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109876	P065132505	phase separation. another phase c=3.300.	(Mg,Al)B2	Mg0.23Al0.77B2	Mg	0.23	Al	0.77	B	2																			2002																												AlB2			A	3.0367		3.3459											AlB2, C32	K		5.1					5.1																																																																																																solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109877	P065132505	not s/c	(Mg,Al)B2	Mg0.15Al0.85B2	Mg	0.15	Al	0.85	B	2																			2002																												AlB2			A	3.0276		3.2939											AlB2, C32	K																																																																																																							solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109878	P065132505	not s/c	MgAl2	Al1B2	Al	1	B	2																					2002																												AlB2			A	3.0245		3.2541											AlB2, C32	K																																																																																																							solid state reaction					Superconductivity, superstructure, and structure anomalies in Mg1-xAlxB2			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, People? Republic of China	Phys.Rev.B, 65(2002)132505	C.Dong,F.M.Liu,J.Q.Li,J.Y.Xiang,L.Li,Z.X.Zhao		
109879	P065132519		LaPt2B2C	La1Pt2.1B2.4C1.2	La	1	Pt	2.1	B	2.4	C	1.2																	2002																												LuNi2B2C																		K		10.5					10.5																																																																																																arc melt in Ar					Nonmagnetic ground state of the superconductor PrPt2B2C and magnetic pairbreaking in La0.9R0.1Pt2B2C (R = Ce, Pr, Nd)			Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, India	Phys.Rev.B, 65(2002)132519	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
109880	P065132519	effective moment=3.63 myuB/Pr	PrPt2B2C	Pr1Pt2.1B2.4C1.2	Pr	1	Pt	2.1	B	2.4	C	1.2																	2002							-33																					LuNi2B2C																		K		6					6																																																																																																arc melt in Ar					Nonmagnetic ground state of the superconductor PrPt2B2C and magnetic pairbreaking in La0.9R0.1Pt2B2C (R = Ce, Pr, Nd)			Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, India	Phys.Rev.B, 65(2002)132519	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
109881	P065132519		(La,Ce)Pt2B2C	La0.9Ce0.1Pt2.1B2.4C1.2	La	0.9	Ce	0.1	Pt	2.1	B	2.4	C	1.2															2002																												LuNi2B2C																		K					1.8																																																																																																		arc melt in Ar					Nonmagnetic ground state of the superconductor PrPt2B2C and magnetic pairbreaking in La0.9R0.1Pt2B2C (R = Ce, Pr, Nd)			Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, India	Phys.Rev.B, 65(2002)132519	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
109882	P065132519		(La,Nd)Pt2B2C	La0.9Nd0.1Pt2.1B2.4C1.2	La	0.9	Nd	0.1	Pt	2.1	B	2.4	C	1.2															2002																												LuNi2B2C																		K		8.5					8.5																																																																																																arc melt in Ar					Nonmagnetic ground state of the superconductor PrPt2B2C and magnetic pairbreaking in La0.9R0.1Pt2B2C (R = Ce, Pr, Nd)			Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, India	Phys.Rev.B, 65(2002)132519	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
109883	P065132519		(La,Pr)Pt2B2C	La0.9Pr0.1Pt2.1B2.4C1.2	La	0.9	Pr	0.1	Pt	2.1	B	2.4	C	1.2															2002																												LuNi2B2C																		K		9					9																																																																																																arc melt in Ar					Nonmagnetic ground state of the superconductor PrPt2B2C and magnetic pairbreaking in La0.9R0.1Pt2B2C (R = Ce, Pr, Nd)			Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai, India	Phys.Rev.B, 65(2002)132519	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
109884	L088087001	energy gap measured by Raman shift. Temperature dependence of gap obeys BCS.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38.2					38.2																																																3.96	4																																															1400-1700C,5-60min,p=4-6 GPa in BN					Superconducting Gap in MgB2 : Electronic Raman Scattering Measurements of Single Crystals			SRL, International Superconductivity Technology Center, Shinonome, Koto-ku, Tokyo, Japan	Phys.Rev.Lett., 88(2002)87001	A.Yamamoto,J.W.Quilty,S.Lee,S.Tajima		
109885	MMM2260307	not s/c. no sign of s/c and magnetic transition down to 2 K.	CeIr2B2C	Ce1Ir2B2C1	Ce	1	Ir	2	B	2	C	1																1	2001																												LuNi2B2C			A	3.845		10.347												K					2																																																																																																		arc melting					Magnetic and valence properties of the Ce-based quaternary borocarbide CeIr2B2C				J.Magn.Magn,Mater. 226-230(2001)307	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109886	MMM2260307	not s/c. no sign of s/c and magnetic transition down to 2 K.	CeRh2B2C	Ce1Rh2B2C1	Ce	1	Rh	2	B	2	C	1																1	2001																												LuNi2B2C			A	3.855		10.175												K					2																																																																																																		arc melting					Magnetic and valence properties of the Ce-based quaternary borocarbide CeIr2B2C				J.Magn.Magn,Mater. 226-230(2001)307	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109887	MMM2260330	Li and THF(tetrahydrofuran) intercalated to HfNCl. dHc2/dT=19 and 5.1 kOe/K for H//ab and H//c. cohere(ab)=50A, cohere(c)=13.5A.	Lix(THF)yHfNCl	Li0.48M0.3Hf1N1Cl1	Li	0.48	M	0.3	Hf	1	N	1	Cl	1															2001																																														K		25.5					25.5																													kOe/K		19			MHC9887		A		50																																																										intercalation					Magnetic properties of the layered superconductor Li0.48(THF)0.3HfNCl with Tc = 26K			Department of Physics,Tokyo Metropolitan University, Minami-Osawa, Hachi-oji,Tokyo,Japan	J.Magn.Magn,Mater. 226-230(2001)330	H.Tou,S.Yamanaka,T.Koiwasaki,Y.Maniwa		
109888	PR05201181	RRR=7.5. Another magnetic order at 5.7K clearly observed in specific heat. X-ray density=4.02 g/cm3	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1995								5.2																				LuNi2B2C			A	3.516		10.53												K		7.8					7.8											Oe		250							kOe		3.5																																																																										arc-melt in Ar + ANN(1100C)					Magnetic transitions and nearly reentrant superconducting properties of HoNi2B2C			Department of Physics, National Tsing Hua University, Hsinchu, Taiwan, ROC	Phys.Rev.B, 52(1995)1181	H.C.Ku,H.D.Yang,J.C.Ho,J.H.Shieh,M.S.Lin,W.Y.Guan,Y.B.You		
109889	PR06003064	Ba7.62Ga17.3Ge28.7 by ICP. A8T46 structure. penetration depth = 1-5 micron.m. Tc(onset)=4.8 K.	Ba8(Ga16Ge30)	Ba8Ga16Ge30	Ba	8	Ga	16	Ge	30																			1999																												clathrate			A	10.7844														K		7.5					7.5											Oe		100																																																																																			react(1080C,1h)					Superconductivity in germanium clathrate Ba8G16Ge30			Department of Chemistry, University of California, Santa Barbara, California, USA	Phys.Rev.B, 60(1999)3064	D.Schmidt,G.D.Stucky,J.D.Bryan,V.I.Srdanov		
109890	JAC3350270	not s/c.  A8T46 structure.	Sr8(Ga11Si35)	Sr8Ga11Si35	Sr	8	Ga	11	Si	35																		3	2002																												clathrate			A	10.4075														K					2																																																																																																		Floating zone method					Synthesis of a Si-clathrate compound, Sr8GaxSi46-x, and its electrical resistivity measurements			National Institute for Materials Science , Materials Engineering Laboratory ,1- 2- 1 Sengen , Tsukuba , Ibaraki, Japan	J.Alloys Compd., 335(2002)270	K.Nishida,K.Yamada,M.Imai,T.Kimura		
109891	JAC3350191	not s/c for 0.706<x<1.0 in NdRh3Bx. micro-Vickerrs = 4.9 GPa.	NdRh3B	Nd1Rh3B1	Nd	1	Rh	3	B	1																			2002																															A	4.2136														K					0.5																																																																																																							Solid solution range of boron and properties of the perovskite-type NdRh3B			Institute for Materials Research (IMR ), Tohoku University ,2- 1- 1 Katahira , Aoba-ku , Sendai, Japan	J.Alloys Compd., 335(2002)191	A.Yoshikawa,H.Horiuchi,I.Higashi,J.M.Ko,J.Ye,K.Kudou,K.Nakajima,M.Oku,S.Kohiki,S.Okada,T.Fukuda,T.Sasaki,T.Shishido		
109892	JAC3880069		Ba2Sn3Sb6	Ba2Sn3Sb6	Ba	2	Sn	3	Sb	6																		3	2002																												Zintl																		K		3.9					3.9																																																																																																Sn-flux method					Superconductivity in Ba2Sn3Sb6 and SrSn3Sb4			Department of Chemistry , University of Alberta , Edmonton , Canada	J.Alloys Compd., 388(2002)69	Arthur Mar,Frank Marsiglio,Laura Deakin,Robert Lam		
109893	JAC3880069		SrSn3Sb4	Sr1Sn3Sb4	Sr	1	Sn	3	Sb	4																		3	2002																												Zintl																		K		3.9					3.9																																																																																																Sn-flux method					Superconductivity in Ba2Sn3Sb6 and SrSn3Sb4			Department of Chemistry , University of Alberta , Edmonton , Canada	J.Alloys Compd., 388(2002)69	Arthur Mar,Frank Marsiglio,Laura Deakin,Robert Lam		
109894	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixHfNCl	Li1Hf1N1Cl1	Li	1	Hf	1	N	1	Cl	1																	2000																															A	3.572		27.721												K		25.3					25.3																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109895	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	Lix(Hf,Zr)NCl	Li1Hf0.7Zr0.3N1Cl1	Li	1	Hf	0.7	Zr	0.3	N	1	Cl	1															2000																															A	3.578		27.705												K		22.6					22.6																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109896	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	Lix(Hf,Zr)NCl	Li1Hf0.5Zr0.5N1Cl1	Li	1	Hf	0.5	Zr	0.5	N	1	Cl	1															2000																															A	3.586		27.688												K		21					21																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109897	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	Lix(Hf,Zr)NCl	Li1Hf0.2Zr0.8N1Cl1	Li	1	Hf	0.2	Zr	0.8	N	1	Cl	1															2000																															A	3.592		27.672												K		18.2					18.2																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109898	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrNCl	Li1Zr1N1Cl1	Li	1	Zr	1	N	1	Cl	1																	2000																															A	3.606		27.639												K		14.4					14.4																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109899	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrN(Cl,Br)	Li1Zr1N1Cl0.75Br0.25	Li	1	Zr	1	N	1	Cl	0.75	Br	0.25															2000																															A	3.613		28.255												K		14.4					14.4																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109900	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrN(Cl,Br)	Li1Zr1N1Cl0.525Br0.475	Li	1	Zr	1	N	1	Cl	0.525	Br	0.475															2000																															A	3.621		28.676												K		14.3					14.3																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109901	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrN(Cl,Br)	Li1Zr1N1Cl0.255Br0.745	Li	1	Zr	1	N	1	Cl	0.255	Br	0.745															2000																															A	3.63		29.019												K		14.1					14.1																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109902	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrNBr	Li1Zr1N1Br1	Li	1	Zr	1	N	1	Br	1																	2000																															A	3.638		29.235												K		14.1					14.1																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109903	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixHfN(Cl,Br)	Li1Hf1N1Cl0.75Br0.25	Li	1	Hf	1	N	1	Cl	0.75	Br	0.25															2000																															A	3.583		28.284												K		23.6					23.6																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109904	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixHfN(Cl,Br)	Li1Hf1N1Cl0.525Br0.475	Li	1	Hf	1	N	1	Cl	0.525	Br	0.475															2000																															A	3.594		28.726												K		22.7					22.7																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109905	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	Lix(Hf,Zr)NBr	Li1Hf0.45Zr0.55N1Br1	Li	1	Hf	0.45	Zr	0.55	N	1	Br	1															2000																															A	3.625		29.295												K		19					19																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109906	PHC3410699	Li-doped. Li-content not known. Li-intercalated between halogen layers.	Lix(Hf,Zr)NBr	Li1Hf0.22Zr0.78N1Br1	Li	1	Hf	0.22	Zr	0.78	N	1	Br	1															2000																															A	3.63		29.262												K		16					16																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109907	PHC3410699	High-pressure phase. Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixHfNBr	Li1Hf1N1Br1	Li	1	Hf	1	N	1	Br	1																	2000																															A	3.609		29.328												K		24.1					24.1																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109908	PHC3410699	High-pressure phase. Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixHfNI	Li1Hf1N1I1	Li	1	Hf	1	N	1	I	1																	2000																															A	3.688														K		22.2					22.2																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109909	PHC3410699	High-pressure phase. Li-doped. Li-content not known. Li-intercalated between halogen layers.	LixZrNI	Li1Zr1N1I1	Li	1	Zr	1	N	1	I	1																	2000																															A	3.719														K		14.2					14.2																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109910	PHC3410699	Na- intercalated	NaxHfNCl	Na0.28Hf1N1Cl1	Na	0.28	Hf	1	N	1	Cl	1																	2000																																														K		23					23																																																																																																					Substitution and cointercalation effects on superconducting electron-doped layer structured metal nitride halides			?epartment of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Physica C, 341(2000)699	H.Fukuoka,H.Kawaji,K.Hotehama,S.Shamoto,S.Yamanaka,T.Kajitani,T.Koiwasaki		
109911	PHC3680251	well understand by two gap scenario(gap=4 meV(Tc=20 K) + gap=2.6 meV(Tc=38 K))	MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2																	AlB2, C32	K		38					38																																																2.45																																																junction(In or Ag droplet on MgB2 wire					Superconducting gap parameters of MgB2 obtained on MgB2/Ag and MgB2/In junctions			Institute of Electrical Engineering,Slovak Academy of Sciences,Bratislava,Slovakia	Physica C, 368(2002)251	A.Plecenik,M.Grajcar,P.Kus,S.Benacka		
109912	PHC3530207	polymetric phase (not cubic). monoclinic (beta=133.084 degree). dTc/dP in k/GPa.	Na2CsC60	Na2Cs1C60	Na	2	Cs	1	C	60																			2001																												fullerene			A	13.776	14.343	9.375												K		8.5					8.5			K/GPa	-0.02																																																																																												pressure-induced polymerization					Superconductivity in the polymetric phase of Na2CsC60			Advanced Materials Physics and Devices, Sandia National Lab, MS,Albuquerque, NM, USA	Physica C, 353(2001)207	B.Morosin,G.H.Kwei,J.D.Jorgensen,J.E.Fischer,J.E.Schirber,T.Yildirim		
109913	PHC3530207	polymetric phase . not s/c	Na2RbC60	Na2Rb1C60	Na	2	Rb	1	C	60																			2001																												fullerene																		K					4.2																																																																																																		pressure-induced polymerization					Superconductivity in the polymetric phase of Na2CsC60			Advanced Materials Physics and Devices, Sandia National Lab, MS,Albuquerque, NM, USA	Physica C, 353(2001)207	B.Morosin,G.H.Kwei,J.D.Jorgensen,J.E.Fischer,J.E.Schirber,T.Yildirim		
109914	PHC3640571	RRR=21.8	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	2001																												LuNi2B2C			A	3.5277		10.565												K		15.6					15.6																																																																																																arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109915	PHC3640571	RRR=5.62	(Y,Pr)Ni2B2C	Y0.8Pr0.2Ni2B2C1	Y	0.8	Pr	0.2	Ni	2	B	2	C	1														1	2001																												LuNi2B2C			A	3.5464		10.461												K		8.74					8.74																																																																																																arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109916	PHC3640571	RRR=4.79. not s/c	(Y,Pr)Ni2B2C	Y0.6Pr0.4Ni2B2C1	Y	0.6	Pr	0.4	Ni	2	B	2	C	1														1	2001																												LuNi2B2C			A	3.5817		10.363												K					4.2																																																																																																		arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109917	PHC3640571	RRR=4.79. not s/c	(Y,Pr)Ni2B2C	Y0.4Pr0.6Ni2B2C1	Y	0.4	Pr	0.6	Ni	2	B	2	C	1														1	2001																												LuNi2B2C			A	3.626		10.265												K					4.2																																																																																																		arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109918	PHC3640571	RRR=6.03. not s/c	(Y,Pr)Ni2B2C	Y0.2Pr0.8Ni2B2C1	Y	0.2	Pr	0.8	Ni	2	B	2	C	1														1	2001																												LuNi2B2C			A	3.6633		10.133												K					4.2																																																																																																		arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109919	PHC3640571	RRR=11.9.  not s/c	PrNi2B2C	Pr1Ni2B2C1	Pr	1	Ni	2	B	2	C	1																1	2001																												LuNi2B2C			A	3.7002		9.974												K					0.35																																																																																																		arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109920	PHC3640571		(Y,Pr)Ni2B2C	Y0.95Pr0.05Ni2B2C1	Y	0.95	Pr	0.05	Ni	2	B	2	C	1														1	2001																												LuNi2B2C																		K		14					14																																																																																																arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109921	PHC3640571		(Y,Pr)Ni2B2C	Y0.85Pr0.15Ni2B2C1	Y	0.85	Pr	0.15	Ni	2	B	2	C	1														1	2001																												LuNi2B2C																		K		12					12																																																																																																arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109922	PHC3640571		(Y,Pr)Ni2B2C	Y0.75Pr0.25Ni2B2C1	Y	0.75	Pr	0.25	Ni	2	B	2	C	1														1	2001																												LuNi2B2C																		K		7.7					7.7																																																																																																arc-melt in Ar					Superconducting and normal state properties of Y1-xPrxNi2B2C			Institut fur Festkorper- und Werkstofforschung Dresden, Dresden, Germany	Physica C, 364-365(2001)571	G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,V.N.Narozhnyi		
109923	PHC3690250	Hc2 by resistive transition. RRR=4. RES(RT)=20 micro-Ohm.cm.	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		39.3					39.3																				T		25												MHC9923		A		36																																																										arc-melt in Ar					Magnetotransport and the upper critical magnetic field in MgB2			Institute of Experimental Physics,SAS,04353 Kosice,Slovakia	Physica C, 369(2002)250	A.G.M.Jansen,D.Fruchart,J.Marcus,P.Samuely,P.Szabo,S.Miraglia,T.Klein		
109924	PHC3700006	grain size=1-5 micron. density=2.63 g/cm3. penet estimated using G-L parameter=26.	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		38					38											Oe		245																					MHC9924																																																														high-pressure synthesis					Lower critical field of MgB2 measured by Hall probe			Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 370(2002)6	A.K.Pradhan,H.Ihara,H.Kito,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
109925	PHC3700006	anisotropy = 3	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38					38											Oe		280																					MHC9925							nm		146																																																					high-pressure synthesis					Lower critical field of MgB2 measured by Hall probe			Department of Applied Physics,The University of Tokyo,7-3-1 Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 370(2002)6	A.K.Pradhan,H.Ihara,H.Kito,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
109926	PHC3700039		MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2			A	3.085		3.523											AlB2, C32	K		37.5					37.5																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109927	PHC3700039	MgB2, Mg from XRD	(Mg,Co)B2	Mg0.99Co0.01B2	Mg	0.99	Co	0.01	B	2																		1	2002																												AlB2																	AlB2, C32	K		35.5					35.5																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109928	PHC3700039	Intensity of MgB2-peak is very weak.	(Mg,Co)B2	Mg0.9Co0.1B2	Mg	0.9	Co	0.1	B	2																		1	2002																												AlB2			A	3.0774		3.5195											AlB2, C32	K		34.5					34.5																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109929	PHC3700039		(Mg,Co)B2	Mg0.75Co0.25B2	Mg	0.75	Co	0.25	B	2																		1	2002																												AlB2			A	3.0773		3.5187											AlB2, C32	K		34					34																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109930	PHC3700039	XRD peak shows CoB. MgB2 structure not clear.	(Mg,Co)B2	Mg0.5Co0.5B2	Mg	0.5	Co	0.5	B	2																			2002																															A	3.0705		3.5051												K		31.5					31.5																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109931	PHC3700039	MgB2 structure + Mg2Sn	(Mg,Co)B2	Mg0.99Sn0.01B2	Mg	0.99	Sn	0.01	B	2																			2002																																														K		33.5					33.5																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109932	PHC3700039		(Mg,Fe)B2	Mg0.97Fe0.03B2	Mg	0.97	Fe	0.03	B	2																			2002																												AlB2																	AlB2, C32	K		36					36																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109933	PHC3700039		(Mg,Fe)B2	Mg0.9Fe0.1B2	Mg	0.9	Fe	0.1	B	2																			2002																												AlB2																	AlB2, C32	K		34					34																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109934	PHC3700039	MgB2 phase +Fe2B	(Mg,Fe)B2	Mg0.75Fe0.25B2	Mg	0.75	Fe	0.25	B	2																			2002																																														K		32					32																																																																																																solid state reaction (800C,4h,in 6.5%H2-Ar)					Effects of Sn,Co and Fe on MgB2			Institut fur Chemische Technologie Anorganischer Stoffe,Johannes Kepler Universitat,Linz,Austria	Physica C, 370(2002)39	Gerhard Gritzner,Markus Kuhberger		
109935	P065140501	RR(40K)=1.0 microOhm.cm. RRR=4.9. Anisotropy=2.2-3. Hc2(0)//ab=21T, Hc2(0)//c=7.3T, cohere//ab=68A, cohere//c=23A. mean free path=240A for ab, =60A for c.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38.5					38.5																				T		21														A		68																																																										grown in Mg-MgB2-BN system at 4-6 GPa, 1400-1700 C					Anisotropic superconducting properties of MgB2 single crystals probed by in-plane electrical transport measurements			SRL, ISTEC,  Shinonome 1-chome, Koto-ku, Tokyo , Japan	Phys.Rev.B., 65(2002)140501	K.Nakao,M.Murakami,N.Chikumoto,N.Koshizuka,S.Lee,S.Tajima,Yu.Eltsev		
109936	SSC1210575	Density=0.67 g/cm3. Hc2(T) from resistive transition. Hc1(T) from M-H curve. G-L parameter = 50	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		38.6					38.6											Oe		120							T		15.5														A		46			A		2300																																																					solid state reaction(925C, 200Torr-Ar)+ANN					Thermal fluctuation and upper critical field of MgB2 superconductor			Department of Physics, National Hsing University, Taichung,Taiwan,ROC	Solid State Commun., 121(2002)575	J.J.Cheng,M.D.Lan,P.L.Tsai,Y.L.Chang		
109937	P065144528	slow cool (RT to 90K within a few hours) for measurement.	RbxWO3	Rb0.23W1O3	Rb	0.23	W	1	O	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		2.6					2.6																																																																																																(Rb2WO4+WO3)-heat(900C, 2days)					Concentration dependence of superconductivity and the order-disorder transition in the hexagonal rubidium tungsten bronze RbxWO3: Interfacial and bulk properties			Centre de Recherches sur les Tres Basses Temperatures, CNRS, Boute, Grenoble Cedex 9, France	Phys.Rev.B, 65(2002)144528	J.Marcus,P.Haen,R.Brusetti		
109938	PR0201903	Values of Hc2(0), dHc2/dT are for H//c-axis. Rb-content dependence of Tc is not clear.	RbxWO3	Rb0.2W1O3	Rb	0.2	W	1	O	3																			1979																												CaTiO3																	CaTiO3, perovskite	K		4.16					4.16	MTC9938																			kOe		47.7							kOe/K		16.9																																																																	(RbWO4+W+WO3) - heat (1100C)					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Florida State University, Tallahassee,Florida	Phys.Rev.B, 20(1979)1903	R.C.Morris,R.K.Stanley,W.G.Moulton		
109939	JAC3390018	not s/c and not magnetic order	CeCo2B2C	Ce1Co2B2C1	Ce	1	Co	2	B	2	C	1																1	2002																												LuNi2B2C			A	3.58		10.244												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109940	JAC3390018	not s/c and not magnetic order	CeNi2B2C	Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	2002																												LuNi2B2C			A	3.635		10.225												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109941	JAC3390018	not s/c and not magnetic order	CeRh2B2C	Ce1Rh2B2C1	Ce	1	Rh	2	B	2	C	1																1	2002																												LuNi2B2C			A	3.856		10.175												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109942	JAC3390018	not s/c and not magnetic order	CePd2B2C	Ce1Pd2B2C1	Ce	1	Pd	2	B	2	C	1																1	2002							-37																					LuNi2B2C			A	3.917		10.298												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109943	JAC3390018	not s/c and not magnetic order	CeIr2B2C	Ce1Ir2B2C1	Ce	1	Ir	2	B	2	C	1																1	2002							-20																					LuNi2B2C			A	3.846		10.347												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109944	JAC3390018	not s/c and not magnetic order	CePt2B2C	Ce1Pt2.1B2.4C1.2	Ce	1	Pt	2.1	B	2.4	C	1.2																1	2002							-55																					LuNi2B2C			A	3.84		10.73												K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109945	JAC3390018	not s/c and not magnetic order. majority phase = YNi2B2C	CeOs2B2C	Ce1Os2B2C1	Ce	1	Os	2	B	2	C	1																	2002																												LuNi2B2C																		K					2																																																																																																		arc-melting					Investigations of the structural, magnetic and Ce-valence properties of quaternary CeM2B2C compounds (M=Co,Ni,Rh,Pd,Ir and Pt)				J.Alloys Compd, 339(2002)18	Arvind D.Chinchure,C.Godart,Chandan Mazumdar,E.Alleno,H.Noel,L.C.Gupta,M.Potel,O.Sologub,P.Salamakha,R.Nagarajan		
109946	MMM2260080	RR=1.3 microOhm.cm. RRR=110 for I//[001], =90 for I//[100]. s/c properties measured at p=1.1 GPa. Table values for H//[100]. For H//[001], Hc2=3.4 kOe, cohere=310 A.	CeRh2Si2	Ce1Rh2Si2	Ce	1	Rh	2	Si	2																		3	2001																																														K		0.38			0		0.38																				kOe		5.6												MHC9946		A		240																																																										Czochrulski method					High-quality single-crystal growth and a change of the electronic states under pressure in CeRh2Si2			Graduate School of Science,Osaka University,Toyonaka,Osaka 560-0043,Japan	J.Mag.Mag.Mater.,226(2001)80	R.Settai,S.Araki,T.C.Kobayashi,Y.Onuki		
109947	MMM2420829	Curie-T for H//c = 141K. Effective moment of Dy at 1.7K = 10.1	(Y,Dy)Ni2B2C	Y0.75Dy0.25Ni2B2C1	Y	0.75	Dy	0.25	Ni	2	B	2	C	1														3	2002							-46																					LuNi2B2C																		K		12					12																																																																																																					Magnetic anisotropy of Y1-xDyxNi2B2C single crystals			August Chelkowski Institute of Physics, University of Silesia, Katowice, Poland	J.Mag.Mag.Mater.,242(2002)829	A.Winiarska,D.Kaczorowski,Z.Drzazga		
109948	MMM2420829	Curie-T for H//c = -6 K. Effective moment of Dy at 1.7K = 9.1	(Y,Dy)Ni2B2C	Y0.65Dy0.35Ni2B2C1	Y	0.65	Dy	0.35	Ni	2	B	2	C	1														3	2002							30	2.1																				LuNi2B2C																		K		10.6					10.6																																																																																																					Magnetic anisotropy of Y1-xDyxNi2B2C single crystals			August Chelkowski Institute of Physics, University of Silesia, Katowice, Poland	J.Mag.Mag.Mater.,242(2002)829	A.Winiarska,D.Kaczorowski,Z.Drzazga		
109949	MMM2420829	Curie-T for H//c = -10 K. Effective moment of Dy at 1.7K = 9.6	(Y,Dy)Ni2B2C	Y0.45Dy0.55Ni2B2C1	Y	0.45	Dy	0.55	Ni	2	B	2	C	1														3	2002							42	5.5																				LuNi2B2C																		K		5.2					5.2																																																																																																					Magnetic anisotropy of Y1-xDyxNi2B2C single crystals			August Chelkowski Institute of Physics, University of Silesia, Katowice, Poland	J.Mag.Mag.Mater.,242(2002)829	A.Winiarska,D.Kaczorowski,Z.Drzazga		
109950	MMM2420829	Curie-T for H//c = -22 K. Effective moment of Dy at 1.7K = 9.6	(Y,Dy)Ni2B2C	Y0.15Dy0.85Ni2B2C1	Y	0.15	Dy	0.85	Ni	2	B	2	C	1														3	2002							27	9.5																				LuNi2B2C																		K		4.3					4.3																																																																																																					Magnetic anisotropy of Y1-xDyxNi2B2C single crystals			August Chelkowski Institute of Physics, University of Silesia, Katowice, Poland	J.Mag.Mag.Mater.,242(2002)829	A.Winiarska,D.Kaczorowski,Z.Drzazga		
109951	MAT0105280	Hc2 using WHH theory. Thermodynamic Hc(0)=0.22 T. delta-C/gamma*Tc=2.3. gap by tunneling. gamma in mj/mol-Ni.K2. G-L parameter = 46	MgCNi3	Mg1Co1Ni3	Mg	1	Co	1	Ni	3																			2001																																														K		7.63					7.63											Oe		130							T		14.4							T/K		2.72					A		46			A		2130					4.6	1				MSP9951			mj/mol.K2	9.2		280																																					solid state reaction					Experimental determination of superconducting parameters for the intermetallic perovskite superconductor MgCNi3			Department of Physics, The Pennsylvania State University, University Park, PA	cond-mat/ 0105280(2001)	I.G.Deac,K.A.Regan,K.D.Nelson,K.Wu,M.M.Rosario,P.Schiffer,R.J.Cava,T.He,Y.Liu,Z.Q.Mao		
109952	PHC3710321	2D-s/c. values of s/c properties are those at 2.0 K.. G-L parameter = 20.3	CsxWO3	Cs0.005W1O3	Cs	0.005	W	1	O	3																			2002																												bronze																		K		5.9					5.9											Oe		12							Oe		3800														A		330			A		6700																																																					crystal by thermal vapor growth					Interplay of Cs concentration, dimensionality and superconductivity in CsxWO3			Department of Materials and Interfaces, Weizmann Institute of Science,Rehovot, Israel	Physica C, 371(2002)321	G.Leitus,H.Cohen,S.Reich		
109953	SSC1120323	density = 6.85-7.03 g/cm3. single phase for 0.8<x<=0.95. layered structure	Nb2SCx	Nb2S1C0.9	Nb	2	S	1	C	0.9																		1	1999																															A	3.294		11.5525												K		5					5																																																																																																powder - react(T>1150C) in qualtz tube					Carbosulfide superconductor			Japan Science and Technology Corporation (JST), Japan	SSC112(1999)323	H.Nozaki,H.Wada,K.Sakamaki,Maki Kawai,Y.Onuku		
109954	SSC1120323	density = 6.85-7.03 g/cm3. single phase for 0.8<x<=0.95. layered structure	Nb2SCx	Nb2S1C0.85	Nb	2	S	1	C	0.85																		1	1999																																														K		4.68					4.68																																																																																																powder - react(T>1150C) in qualtz tube					Carbosulfide superconductor			Japan Science and Technology Corporation (JST), Japan	SSC112(1999)323	H.Nozaki,H.Wada,K.Sakamaki,Maki Kawai,Y.Onuku		
109955	SSC1120323	density = 6.85-7.03 g/cm3. single phase for 0.8<x<=0.95. layered structure	Nb2SCx	Nb2S1C0.82	Nb	2	S	1	C	0.82																		1	1999																																														K		4.43					4.43																																																																																																powder - react(T>1150C) in qualtz tube					Carbosulfide superconductor			Japan Science and Technology Corporation (JST), Japan	SSC112(1999)323	H.Nozaki,H.Wada,K.Sakamaki,Maki Kawai,Y.Onuku		
109956	SSC1180113	layered structure. 1T-Cu<2/3>Nb2S2C	1T-Cu<2/3>Nb2S2C	Cu0.67Nb2S2C1	Cu	0.67	Nb	2	S	2	C	1																	2001																															A	3.3168		9.0245												K		4.85					4.85											Oe		37							kOe		8.99														A		191			A		3600																																																					(Nb2SC,S,<2/3>Cu)-pellet-sintered in evacuated tube(1200C)					van der Waals type carbosulide superconductor			Japan Science and Technology Corporation (JST), Japan	SSC118(2001)113	H.Nozaki,H.Wada,K.Sakamaki,Maki Kawai,Y.Onuku		
109957	SSC1180113	layered structure. 75.6 wt% 1T-phase + 24.4 wt% 3R-phase(a=3.271,C=25.478). G-L parameter = 6.37	Nb2S2C	Nb2S2C1	Nb	2	S	2	C	1																			2001																															A	3.268		8.547												K		7.6					7.6											Oe		227							kOe		9.95														A		182			A		1160																																																					extract Cu from Cu<2/3>Nb2S2C + dry in vacuum(100C)					van der Waals type carbosulide superconductor			Japan Science and Technology Corporation (JST), Japan	SSC118(2001)113	H.Nozaki,H.Wada,K.Sakamaki,Maki Kawai,Y.Onuku		
109958	P065172503		MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2			A	3.0838		3.5224											AlB2, C32	K		38.3					38.3																																																																																																pelletized + heat(850C,20 atm Ar, in W-vessel)					Structural and superconducting properties of MgB2-xBex			Center for Strongly Correlated Materials Research, Seoul National University, Seoul, Republic of Korea	Phys.Rev.B., 65(2002)172503	E.J.Choi,J.S.Ahn,M.-S.Kim,S.-I.Lee,Young-Jin Kim		
109959	P065172503		Mg(B,Be)2	Mg1B1.8Be0.2	Mg	1	B	1.8	Be	0.2																		1	2002																												AlB2			A	3.0782		3.5412											AlB2, C32	K		36					36																																																																																																pelletized + heat(850C,20 atm Ar, in W-vessel)					Structural and superconducting properties of MgB2-xBex			Center for Strongly Correlated Materials Research, Seoul National University, Seoul, Republic of Korea	Phys.Rev.B., 65(2002)172503	E.J.Choi,J.S.Ahn,M.-S.Kim,S.-I.Lee,Young-Jin Kim		
109960	P065172503		Mg(B,Be)2	Mg1B1.7Be0.3	Mg	1	B	1.7	Be	0.3																		1	2002																												AlB2			A	3.073		3.597											AlB2, C32	K		32.9					32.9																																																																																																pelletized + heat(850C,20 atm Ar, in W-vessel)					Structural and superconducting properties of MgB2-xBex			Center for Strongly Correlated Materials Research, Seoul National University, Seoul, Republic of Korea	Phys.Rev.B., 65(2002)172503	E.J.Choi,J.S.Ahn,M.-S.Kim,S.-I.Lee,Young-Jin Kim		
109961	P065172503		Mg(B,Be)2	Mg1B1.6Be0.4	Mg	1	B	1.6	Be	0.4																		1	2002																												AlB2			A	3.073		3.6326											AlB2, C32	K		20.9					20.9																																																																																																pelletized + heat(850C,20 atm Ar, in W-vessel)					Structural and superconducting properties of MgB2-xBex			Center for Strongly Correlated Materials Research, Seoul National University, Seoul, Republic of Korea	Phys.Rev.B., 65(2002)172503	E.J.Choi,J.S.Ahn,M.-S.Kim,S.-I.Lee,Young-Jin Kim		
109962	P065172503		Mg(B,Be)2	Mg1B1.4Be0.6	Mg	1	B	1.4	Be	0.6																		1	2002																												AlB2			A	3.0624		3.6395											AlB2, C32	K		8.3					8.3																																																																																																pelletized + heat(850C,20 atm Ar, in W-vessel)					Structural and superconducting properties of MgB2-xBex			Center for Strongly Correlated Materials Research, Seoul National University, Seoul, Republic of Korea	Phys.Rev.B., 65(2002)172503	E.J.Choi,J.S.Ahn,M.-S.Kim,S.-I.Lee,Young-Jin Kim		
109963	P065180505	resistive Tc=38.1 K. s/c properties deduced from thermal conductivity measurements. cohere//c=2.8 nm. dHc2//c/dT=1.17 kOe/K. Hc2(0)//c=31 kOe. anisotropy=4.2. G-L parameter = 13	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		36.6					36.6											Oe		656							kOe		130							kOe/K		5.15					nm		11.8																																																															Temperature dependence and anisotropy of the bulk upper critical field Hc2 of MgB2			Laboratorium fur Festkoperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B., 65(2002)180505	A.V.Sologubenko,H.R.Ott,J.Jun,J.Karpinski,S.M.Kazakov		
109964	P065180518	using natural abundance of B(=10.8). delta-C/gamma*Tc = 2.3	BeB2.75	B2.75Be1	B	2.75	Be	1																				1	2002																															A	9.7738		9.5467												K		0.72					0.72																																																											1000																																					arc-melting in Ar					Superconducting properties of BeB2.75			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803	Phys.Rev.B., 65(2002)180518	D.P.Young,F.Drymiotis,Frank R.Fronczek,Julia Y.Chan,L.L.Henry,P.W.Adams,R.G.Goodrich		
109965	P065180518	using 100% B<10>. cohere shows the value at T=0.1 K.	BeB2.75	B2.75Be1	B	2.75	Be	1																				1	2002																																														K		0.79					0.79						1	B													T		0.18							T/K		0.2			MHC9965		A		300																																																										arc-melting in Ar					Superconducting properties of BeB2.75			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803	Phys.Rev.B., 65(2002)180518	D.P.Young,F.Drymiotis,Frank R.Fronczek,Julia Y.Chan,L.L.Henry,P.W.Adams,R.G.Goodrich		
109966	P065184514	Hc2//c = 25 kOe. anisotropy = 5.6. Anisotropy estimated from M(H,T) measurement using fitting to PRL087047002.	(Mg,Al)B2	Mg0.99Al0.01B2	Mg	0.99	Al	0.01	B	2																		1	2002																												AlB2			A	3.085		3.5202											AlB2, C32	K		37.9					37.9																				kOe		140																																																																										liquid vapor to solid state reaction					Magnetization and <11>B NMR study of Mg1-xAlxB2 superconductors			Institute of Materials Science, NCSR, Demokritos, Aghia Paraskevi, Athens, Greece	Phys.Rev.B., 65(2002)184514	C.Christides,G.Papavassiliou,I.Margiolaki,I.Maurin,K.Prassides,M.Fardis,M.Karayanni,M.Pissas		
109967	P065184516	Two gaps. main gap is small one (DB value).  second gap = 4.5 * small one. using MgB2/Pb planar junction. RRR=8	MgB2	Mg1B2	Mg	1	B	2																					2002																												AlB2																	AlB2, C32	K																		T		0.2																																			1.18																																																950C in Ta-tube					Temperature and field dependence of the energy gap of MgB2/Pb planar junctions			Department of Physics and Astronomy, University of Kentucky, Lexington, Kentucky 40506-0055	Phys.Rev.B., 65(2002)184516	K.-W.Ng,Mario Freamat,Mohamed H.Badr,Yuri Sushko		
109968	CHM0131778	RESRT = 1.26 E-4 Ohm.cm. RRR=1.94	La13Ga8Sb21	La13Ga8Sb21	La	13	Ga	8	Sb	21																			2001																																														K		2.4					2.4																																																																																																					Electronic Structures and Properties of RE12Ga4Sb23 (RE = La-Nd, Sm) and Superconducting La13Ga8Sb21			Department of Chemistry, University of Alberta, Edmonton, Alberta, Canada	Chem.Mater., 13(2001)1778	Allison M.Mills,Arthur Mar,Laura Deakin		
109969	JAP0575093	Film thickness = 210 A (highest Tc). substrate = Si-wafer. T<sub>=RT. RRR=0.95	Be	Be1	Be	1																						3	1985																																														K		5.8					5.8																																																																																																vapor deposition by ion beam					Superconducting beryllium thin films prepared by ion-beam sputtering			NTT Tokai, Ibaraki, Japan	J.Appl.Phys., 57(1985)5093	K.Nakamura,K.Takei,Kito Nakamura,Koji Takei,Y.Maeda,Yasushi Maeda		
109970	SSC1040663	(PO2)4(WO3)2m m=7. Peieris transition (188 K, 60 K). Tc(R=0)=0.31 K. CDW-s/c	(PO2)4(WO3)14	P4W14O50	P	4	W	14	O	50																		3	1997																																														K		0.39					0.39																																																																																																chemical vapor transition method					CDW state and superconductivity in the quasi-two-dimensional monophosphate tungsten bronze P4W14O50			CNRS, Grenoble Cedex,France	Solid State Commun., 104(1997)663	C.Hess,C.Paulsen,C.Schlenker,D.Dumas,G.Bonfait,J.Marcus,M.Almeida,M.Greenblatt,T.Ohm,Z.Teweldemedhin		
109971	P065224509	Pressure induced s/c(Pc=15 kbar). sp.heat measured at P=21 kbar. Hc2(0) assuming T2 dependence. gamma in mj/mol/K2.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																			2002																												HoCoGa5																		K		2.12			0		2.12	MPH9971																			kOe		159																																		mj/mol.K2	382																																												Specific heat of CeRhIn5 : Pressure-driven evolution of the ground state from antiferromagnetism to superconductivity			Lawrence Berkeley National Laboratory and Department of Chemistry, University of California, Berkeley, California	Phys.Rev.B., 65(2002)224509	F.Bouquet,J.D.Thompson,J.L.Sarrao,M.F.Hundley,N.E.Phillips,P.G.Pagliuso,R.A.Fisher,Z.Fisk		
109972	P065144528	rapid cool (RT to 4.2K within  a few minutes) for measurement.	RbxWO3	Rb0.23W1O3	Rb	0.23	W	1	O	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		3.9					3.9																																																																																																(Rb2WO4+WO3)-heat(900C, 2days)					Concentration dependence of superconductivity and the order-disorder transition in the hexagonal rubidium tungsten bronze RbxWO3: Interfacial and bulk properties			Centre de Recherches sur les Tres Basses Temperatures, CNRS, Boute, Grenoble Cedex 9, France	Phys.Rev.B, 65(2002)144528	J.Marcus,P.Haen,R.Brusetti		
109973	PHC50407	impurity phase = YPt2Ge2. RESRT=0.44 mOhm.cm. RRR=1.8. Hc1(1.8K)= 50 Oe.	Y(Pt,Ge)2	Y1Pt0.5Ge1.5	Y	1	Pt	0.5	Ge	1.5																			2002																												AlB2			A	4.1959		3.9941											AlB2, C32	K		3.3					3.3																																																																																																arc-melting					Superconductivity in ternary germanide Y(Pt0.5Ge1.5) with the AlB2-type structure			AIST, Tsukuba Central, Tsukuba, Ibaraki, Japan	Physica C, 377(2002)185-189	Hijiri Kito,Kazumasa Togano,Yoshihiko Takano		
109974	P063172407	gamma in mj/mol.K2. delta-C/gamma*Tc = 3	Y2PdGe3	Y2Pd1Ge3	Y	2	Pd	1	Ge	3																			2001																												AlB2			A	4.192		4											AlB2, C32	K		3					3																																																								mj/mol.K2	2.5		130																																					arc-melting + ANN(850C)					Observation of enhanced magnetic transition temperature in Nd2PdGe3 and superconductivity in Y2PdGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Phys.Rev.B., 63(2001)172407	E.V.Sampathkumaran,Subham Majumdar		
109975	P063172407	magnetic order (maybe FM) at 6K.  moment=3.7 Bohr-M/Nd.	Nd2PdGe3	Nd2Pd1Ge3	Nd	2	Pd	1	Ge	3																			2001							-5.4																					AlB2			A	4.241		4.193											AlB2, C32	K																																																																																																							arc-melting + ANN(850C)					Observation of enhanced magnetic transition temperature in Nd2PdGe3 and superconductivity in Y2PdGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Phys.Rev.B., 63(2001)172407	E.V.Sampathkumaran,Subham Majumdar		
109976	SSI1410407	impurity phase= Mo, Cd	CdMo6Se8	Cd1.3Mo6Se7.5	Cd	1.3	Mo	6	Se	7.5																			2001																												Chevrel																		K		2.5					2.5																																																																																																sintered in silica tube(1273K, 7days)					Phase study of Chevrel compounds of PbxMo6Se8-y and CdxMo6Se8-y			Okayama University of Science, Okayama,Japan	Solid State Ionics, 141-142(2001)407	J.Kaneyasu,K.Muroi,M.Date,T.0tani		
109978	SSI1410407	Tc (R=0) = 2.0 K.	PbMo6Se8	Pb1Mo6Se7.55	Pb	1	Mo	6	Se	7.55																			2001																												Chevrel			A	9.529		11.946												K		5					5																																																																																																sintered in silica tube(1273K, 7days)					Phase study of Chevrel compounds of PbxMo6Se8-y and CdxMo6Se8-y			Okayama University of Science, Okayama,Japan	Solid State Ionics, 141-142(2001)407	J.Kaneyasu,K.Muroi,M.Date,T.0tani		
109979	SIC0320799	composition by Rietveld analysis.	(Ba,K)8Si46	K2.9Ba4.9Si46	K	2.9	Ba	4.9	Si	46																			1995																												clathrate			A	10.273														K		3.2					3.2																																																																																																(KSi+BaSi2)-(Ta tube in stainless tube)-heat(600C,several days)					Preparation and superconductivity of barium containing silicon clathrate compound, (Ba,K)xSi46			Hiroshima University	Eur.J.Solid State Inorg.Chem., 32(1995)799-807	H.-O.Horie,H.Kawaji,M.Ishikawa,S.Yamanaka		
109980	ANG0362683		BaSn3	Ba1Sn3	Ba	1	Sn	3																					1997																												Ni3Sn			A	7.253		5.496												K		4.3					4.3																																																																																																					BaSn3: A superconductor at the Border of Zintl phases and intermetallic compounds. Real space Analysis of band structure				Angew.Chem.Int.Ed.Engl., 36(1997)2683-2686	C.Kronseder,T.F.Fassler		
109981	PRL0390161	pressure induced s/c. Tc value shows for P=8 kbar. dTc/dP (in K/GPa) at 1 bar. CDW-temp = 59 K.	NbSe3	Nb1Se3	Nb	1	Se	3																					1977																																														K		2.5			0		2.5			K/GPa	6																																																																																												direct reaction (Nb,Se)-heat(700C,15 days)					Superconductivity of the Linear Trichalcogenide NbSe3 under pressure			Grenoble-Cedex, France	Phys.Rev.Lett., 39(1977)161	J.Peyrard,J.Richard,P.Molinie,P.MonceauJ.Peyrared		
109982	PRL0481212	pressure induced s/c. Figure shows Tc and CDW-temp(Td). Tc in TBL shows Tc(max).	EuMo6S8	Eu1.2Mo6S8	Eu	1.2	Mo	6	S	8																			1982																												Chevrel																		K		9.8			0		9.8	MTC9982																																																																																																				Partial gapping of the Fermi surface and superconductivity in EuxMo6S8			Department of Physics, University of California,Los Angeles, California,USA	Phys.Rev.Lett., 48(1982)1212	C.F.Huang,H.L.Luo,P.M.Chaikin,R.C.Lacoe,S.A.Wolf		
109983	PR04908931	CDW-s/c. CDW-temp(Td)=80 K. Hc2 is for H//c-axis. Hall effect, thermopower are measured.	Tl2Mo6Se6	Tl2Mo6Se6	Tl	2	Mo	6	Se	6																			1994																												Tl2Fe6Te6																		K		6.5					6.5																				T		4.9																																																																															Superconducting and dielectric instabilities in Tl2Mo6Se8: Unusual transport properties and unsaturating critical field	4			Phys.Rev.B, 49(1994)8931	A.Briggs,M.Potel,O.Laborde,P.Gougeon,R.Brusetti	Tl,Mo,Se	
109984	PR04307668	dTc/dp in K/GPa. CDW-s/c. CDW-temp=80.1 K 	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		3.8					3.8			K/GPa	-0.098																																																							366																																										Thermal-expansion measurements for Lu5Ir4Si10, Lu5Rh4Si10, Sc5Ir4Si10, and Tm5Ir4Si10: Charge-density-wave effects			Ames Lab-US, Iowa State University, Ames, Iowa	Phys.Rev.B, 43(1991)7668	C.A.Swenson,H.D,Yang,P.Klavins,R.N.Shelton		
109985	PR04307668	dTc/dp in K/GPa. not CDW-s/c. 	Sc]5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		8.3					8.3			K/GPa	-0.256																																																							401																																										Thermal-expansion measurements for Lu5Ir4Si10, Lu5Rh4Si10, Sc5Ir4Si10, and Tm5Ir4Si10: Charge-density-wave effects			Ames Lab-US, Iowa State University, Ames, Iowa	Phys.Rev.B, 43(1991)7668	C.A.Swenson,H.D,Yang,P.Klavins,R.N.Shelton		
109986	PR04307668	CDW-s/c. CDW-temp=134 K	Tm5Ir4Si10	Tm5Ir4Si10	Tm	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		1.9					1.9																																																											355																																										Thermal-expansion measurements for Lu5Ir4Si10, Lu5Rh4Si10, Sc5Ir4Si10, and Tm5Ir4Si10: Charge-density-wave effects			Ames Lab-US, Iowa State University, Ames, Iowa	Phys.Rev.B, 43(1991)7668	C.A.Swenson,H.D,Yang,P.Klavins,R.N.Shelton		
109987	PR04307668	dTc/dp in K/GPa. CDW-s/c. CDW-temp=140 K 	Lu5Rh4Si10	Lu5Rh4Si10	Lu	5	Rh	4	Si	10																			1991																												Sc5Co4Si10																		K		3.3					3.3			K/GPa	-0.07																																																							297																																										Thermal-expansion measurements for Lu5Ir4Si10, Lu5Rh4Si10, Sc5Ir4Si10, and Tm5Ir4Si10: Charge-density-wave effects			Ames Lab-US, Iowa State University, Ames, Iowa	Phys.Rev.B, 43(1991)7668	C.A.Swenson,H.D,Yang,P.Klavins,R.N.Shelton		
109988	PR04307681	dTc/dp in K/GPa. Tc jump tp 9.12 K at Pc=20.5 kbar. CDW-temp=81 K. 	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		3.72					3.72			K/GPa	-0.117																																																																																												arc-melting+ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109989	PR04307681	dTc/dp in K/GPa. Tc jump tp 9.14 K at Pc=20.8 kbar. CDW-temp=82 K. 	Lu5Ir4(Si,C)10	Lu5Ir4Si9C1	Lu	5	Ir	4	Si	9	C	1																	1991																												Sc5Co4Si10																		K		3.74					3.74			K/GPa	-0.134																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109990	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu4.75Sc0.25Ir4Si10	Lu	4.75	Sc	0.25	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		6.06					6.06			K/GPa	0.314																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109991	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu4.5Sc0.5Ir4Si10	Lu	4.5	Sc	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		6.09					6.09			K/GPa	0.123																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109992	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu4Sc1Ir4Si10	Lu	4	Sc	1	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		6.54					6.54			K/GPa	0.176																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109993	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu3.5Sc1.5Ir4Si10	Lu	3.5	Sc	1.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		7.64					7.64			K/GPa	-0.059																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109994	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu2.5Sc2.5Ir4Si10	Lu	2.5	Sc	2.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		7.9					7.9			K/GPa	-0.26																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109995	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu1Sc4Ir4Si10	Lu	1	Sc	4	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		7.68					7.68			K/GPa	-0.311																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109996	PR04307681	dTc/dp in K/GPa. 	(Lu,Sc)5Ir4Si10	Lu0.25Sc4.75Ir4Si10	Lu	0.25	Sc	4.75	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		7.95					7.95			K/GPa	-0.291																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109997	PR04307681	Tc jump to 8.9 K at Pc= 20.2 kbar. CDW-temp= 73, 270 K.	(Lu,Y)5Ir4Si10	Lu4.5Y0.5Ir4Si10	Lu	4.5	Y	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		3.9					3.9																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109998	PR04307681	CDW-temp= 105 K.	(Lu,Th)5Ir4Si10	Lu4.5Th0.5Ir4Si10	Lu	4.5	Th	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		4.88					4.88																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
109999	PR04307681	Tc jump to 7.84 K at Pc= 23.4 kbar. CDW-temp= 86 K.	(Lu,Tm)5Ir4Si10	Lu4.5Tm0.5Ir4Si10	Lu	4.5	Tm	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		2.84					2.84																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
110000	PHC2560090		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1996																												LuNi2B2C																		K		15.2					15.2		1																				83.7									5.5							1984																																																										by arc-melting under flowing Ar,ANN(1050C,12H in quartz ampoules					Anomalous temperature dependence of Hc2 in YNi2B2C	199601		(a)Centre for Advanced Technology, Indore-452013, India (b)Tata Institute of Fundamental Research, Bombay-400 005, India	Physica.C,256(1996)90-94	A.K. Pradhan (a),L.C. Gupta (b),P. Chaddah (a),R. Nagarajian (b),S.B. Roy (a),Z. Hossain (b)	Y, Ni, B, C	
110001	PR05215086		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1995																												LuNi2B2C																		K		15					15		1																																																																																														arc-melting, see Nature 367(1994)252					Normal-state transport and magnetic properties of RNi2B2C (R=Y,Ho,La)	199512			Phys.Rev.B,52(1995)15086	I.R. Fisher,J.R. Cooper,R.,R.J. Cava		
110002	PR05215086	moment=10.4	HoNi2B2C 	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																1	1995																												LuNi2B2C																		K		7.5					7.5																																																																																																arc-melting, see Nature 367(1994)252					Normal-state transport and magnetic properties of RNi2B2C (R=Y,Ho,La)	199512			Phys.Rev.B,52(1995)15086	I.R. Fisher,J.R. Cooper,R.,R.J. Cava		
110003	PR05215086		YNi2B2C	La1Ni2B2C1	La	1	Ni	2	B	2	C	1																1	1995																												LuNi2B2C																		K					1.5																																																																																																		arc-melting, see Nature 367(1994)252					Normal-state transport and magnetic properties of RNi2B2C (R=Y,Ho,La)	199512			Phys.Rev.B,52(1995)15086	I.R. Fisher,J.R. Cooper,R.,R.J. Cava		
110100	BOOK1982	Proc.Natl.Acad.Sci.USA 74,1336	YRh4B4	Y1Rh4B4	Y	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	5.308		7.403											CeCo4B4 type	K		11.3					11.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110101	BOOK1982	Proc.Natl.Acad.Sci.USA 74,1336	NdRh4B4	Nd1Rh4B4	Nd	1	Rh	4	B	4																			1982								1.31																		AB4C4		RT4B4			A	5.333		7.468											CeCo4B4 type	K		5.3					5.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110102	BOOK1982	Proc.Natl.Acad.Sci.USA 74,1336	SmRh4B4	Sm1Rh4B4	Sm	1	Rh	4	B	4																			1982								0.87																		AB4C4		RT4B4			A	5.312		7.43											CeCo4B4 type	K		2.7					2.7																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110103	BOOK1982	not s/c. Proc.Natl.Acad.Sci.USA 74,1336	GdRh4B4	Gd1Rh4B4	Gd	1	Rh	4	B	4																			1982								5.62																		AB4C4		RT4B4			A	5.309		7.417											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110104	BOOK1982	not s/c. Proc.Natl.Acad.Sci.USA 74,1336	TbRh4B4	Tb1Rh4B4	Tb	1	Rh	4	B	4																			1982								7.08																		AB4C4		RT4B4			A	5.303		7.404											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110105	BOOK1982	not s/c. Proc.Natl.Acad.Sci.USA 74,1336	DyRh4B4	Dy1Rh4B4	Dy	1	Rh	4	B	4																			1982								12.08																		AB4C4		RT4B4			A	5.302		7.395											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110106	BOOK1982	not s/c. Proc.Natl.Acad.Sci.USA 74,1336	HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1982								6.56																		AB4C4		RT4B4			A	5.293		7.379											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110107	BOOK1982		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1982								0.9																		AB4C4		RT4B4			A	5.292		7.374											CeCo4B4 type	K		8.7					8.7																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110108	BOOK1982		TmRh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1982								0.4																		AB4C4		RT4B4			A	5.287		7.359											CeCo4B4 type	K		9.8					9.8																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110109	BOOK1982		LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	5.294		7.359											CeCo4B4 type	K		11.7					11.7																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110110	BOOK1982		ThRh4B4	Th1Rh4B4	Th	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	5.356		7.538											CeCo4B4 type	K		4.3					4.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110111	BOOK1982	Solid State Commun. 32(1979)937	HoIr4B4	Ho1Ir4B4	Ho	1	Ir	4	B	4																			1982																										AB4C4		RT4B4																	CeCo4B4 type	K		2					2																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110112	BOOK1982	Solid State Commun. 32(1979)937	ErIr4B4	Er1Ir4B4	Er	1	Ir	4	B	4																			1982																										AB4C4		RT4B4			A	5.408		7.278											CeCo4B4 type	K		2.1					2.1																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110113	BOOK1982	Solid State Commun. 32(1979)937	TmIr4B4	Tm1Ir4B4	Tm	1	Ir	4	B	4																			1982																										AB4C4		RT4B4			A	5.404		7.281											CeCo4B4 type	K		1.6					1.6																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110114	BOOK1982	not s/c. J.Less Common Metals, 67(1979)51	ScCo4B4	Sc1Co4B4	Sc	1	Co	4	B	4																			1982																										AB4C4		RT4B4																	CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110115	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	YCo4B4	Y1Co4B4	Y	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.028		7.015											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110116	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	CeCo4B4	Ce1Co4B4	Ce	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.059		7.063											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110117	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	GdCo4B4	Gd1Co4B4	Gd	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.043		7.049											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110118	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	TbCo4B4	Tb1Co4B4	Tb	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.038		7.03											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110119	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	DyCo4B4	Dy1Co4B4	Dy	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.026		7.014											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110120	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	HoCo4B4	Ho1Co4B4	Ho	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.02		7.003											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110121	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	ErCo4B4	Er1Co4B4	Er	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.016		6.989											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110122	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	TmCo4B4	Tm1Co4B4	Tm	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	5.009		6.98											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110123	BOOK1982	not s/c. J.Less Common Metals, 67(1979)51	YbCo4B4	Yb1Co4B4	Yb	1	Co	4	B	4																			1982																										AB4C4		RT4B4																	CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110124	BOOK1982	not s/c. Soviet Phys.Cryst., 16(1972)897	LuCo4B4	Lu1Co4B4	Lu	1	Co	4	B	4																			1982																										AB4C4		RT4B4			A	4.998		6.947											CeCo4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110125	BOOK1982		ScRu4B4	Sc1Ru4B4	Sc	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.346		14.895											LuRu4B4 type	K		7.2					7.2																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110126	BOOK1982		YRu4B4	Y1Ru4B4	Y	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.454		14.994											LuRu4B4 type	K		1.4					1.4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110127	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	CeRu4B4	Ce1Ru4B4	Ce	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.47		15.085											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110128	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	PrRu4B4	Pr1Ru4B4	Pr	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.505		15.066											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110129	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	NdRu4B4	Nd1Ru4B4	Nd	1	Ru	4	B	4																			1982								1.62																		AB4C4		RT4B4			A	7.502		15.053											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110130	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	SmRu4B4	Sm1Ru4B4	Sm	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.482		15.049											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110131	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	EuRu4B4	Eu1Ru4B4	Eu	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.477		15.035											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110132	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	GdRu4B4	Gd1Ru4B4	Gd	1	Ru	4	B	4																			1982								4.55																		AB4C4		RT4B4			A	7.47		15.009											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110133	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	TbRu4B4	Tb1Ru4B4	Tb	1	Ru	4	B	4																			1982								4.3																		AB4C4		RT4B4			A	7.456		14.995											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110134	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	DyRu4B4	Dy1Ru4B4	Dy	1	Ru	4	B	4																			1982								2.65																		AB4C4		RT4B4			A	7.453		14.983											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110135	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	HoRu4B4	Ho1Ru4B4	Ho	1	Ru	4	B	4																			1982								2.58																		AB4C4		RT4B4			A	7.442		14.975											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110136	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	ErRu4B4	Er1Ru4B4	Er	1	Ru	4	B	4																			1982								2.16																		AB4C4		RT4B4			A	7.438		14.972											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110137	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	TmRu4B4	Tm1Ru4B4	Tm	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.429		14.965											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110138	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	YbRu4B4	Yb1Ru4B4	Yb	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.427		14.962											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110139	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	LuRu4B4	Lu1Ru4B4	Lu	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.419		14.955											LuRu4B4 type	K		2					2																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110140	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	ThRu4B4	Th1Ru4B4	Th	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.54		15.143											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110141	BOOK1982	not s/c. no magnetic phase. Solid State Commun.,24(1977)699	URu4B4	U1Ru4B4	U	1	Ru	4	B	4																			1982																										AB4C4		RT4B4			A	7.459		14.986											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110142	BOOK1982		Y(Rh,Ru)4B4	Y1Th3.4Ru0.6B4	Y	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.484		14.895											LuRu4B4 type	K		9.4					9.4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110143	BOOK1982		Pr(Rh,Ru)4B4	Pr1Th3.4Ru0.6B4	Pr	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.543		14.995											LuRu4B4 type	K		2.3					2.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110144	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	Nd(Rh,Ru)4B4	Nd1Th3.4Ru0.6B4	Nd	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.537		14.969											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110145	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	Sm(Rh,Ru)4B4	Sm1Th3.4Ru0.6B4	Sm	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.516		14.945											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110146	BOOK1982		Eu(Rh,Ru)4B4	Eu1Th3.4Ru0.6B4	Eu	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.505		14.932											LuRu4B4 type	K		1.5					1.5																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110147	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	Gd(Rh,Ru)4B4	Gd1Th3.4Ru0.6B4	Gd	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.502		14.916											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110148	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	Tb(Rh,Ru)4B4	Tb1Th3.4Ru0.6B4	Tb	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.49		14.898											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110149	BOOK1982	not s/c. no magnetic phase. Monatsh.Chem. 111(1980)517	UOs4B4	U1Th3.4Ru0.6B4	U	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.512		15.053											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110150	BOOK1982	Solid State Commun.,24(1977)699	Dy(Rh,Ru)4B4	Dy1Th3.4Ru0.6B4	Dy	1	Th	3.4	Ru	0.6	B	4																	1982								1.5																		AB4C4		RT4B4			A	7.479		14.885											LuRu4B4 type	K		4					4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110151	BOOK1982	Solid State Commun.,24(1977)699	Ho(Rh,Ru)4B4	Ho1Th3.4Ru0.6B4	Ho	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.476		14.872											LuRu4B4 type	K		6.3					6.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110152	BOOK1982	Solid State Commun.,24(1977)699	Er(Rh,Ru)4B4	Er1Th3.4Ru0.6B4	Er	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.468		14.862											LuRu4B4 type	K		7.9					7.9																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110153	BOOK1982	Solid State Commun.,24(1977)699	Tm(Rh,Ru)4B4	Tm1Th3.4Ru0.6B4	Tm	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.458		14.853											LuRu4B4 type	K		8.3					8.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110154	BOOK1982	not s/c.  Solid State Commun.,24(1977)699	Yb(Rh,Ru)4B4	Yb1Th3.4Ru0.6B4	Yb	1	Th	3.4	Ru	0.6	B	4																	1982								0.2																		AB4C4		RT4B4			A	7.449		14.851											LuRu4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110155	BOOK1982	Solid State Commun.,24(1977)699	Lu(Rh,Ru)4B4	Lu1Th3.4Ru0.6B4	Lu	1	Th	3.4	Ru	0.6	B	4																	1982																										AB4C4		RT4B4			A	7.445		14.837											LuRu4B4 type	K		9					9																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110156	BOOK1982		HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1982																										AB4C4		RT4B4																	LuRh4B4 type	K		1.4					1.4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110157	BOOK1982		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	7.444	22.3	7.465											LuRh4B4 type	K		4.3					4.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110158	BOOK1982		TmRh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	7.432	22.28	7.455											LuRh4B4 type	K		5.4					5.4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110159	BOOK1982	not s/c	YbRh4B4	Yb1Rh4B4	Yb	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	7.424	22.26	7.458											LuRh4B4 type	K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110160	BOOK1982		LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																			1982																										AB4C4		RT4B4			A	7.41	22.26	7.44											LuRh4B4 type	K		6.2					6.2																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110161	BOOK1982		YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																			1982																												LuRuB2			A	5.918	5.297	6.377												K		7.8					7.8																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110162	BOOK1982	not s/c	TbRuB2	Tb1Ru1B2	Tb	1	Ru	1	B	2																			1982								45.6																				LuRuB2			A	5.897	5.311	6.367												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110163	BOOK1982	not s/c	DyRuB2	Dy1Ru1B2	Dy	1	Ru	1	B	2																			1982								21.9																				LuRuB2			A	5.886	5.3	6.352												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110164	BOOK1982	not s/c	HoRuB2	Ho1Ru1B2	Ho	1	Ru	1	B	2																			1982								15.5																				LuRuB2			A	5.875	5.287	6.332												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110165	BOOK1982	not s/c	ErRuB2	Er1Ru1B2	Er	1	Ru	1	B	2																			1982								5.21																				LuRuB2			A	5.868	5.262	6.323												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110166	BOOK1982	not s/c	TmRuB2	Tm1Ru1B2	Tm	1	Ru	1	B	2																			1982								4.07																				LuRuB2			A	5.831	5.254	6.299												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110167	BOOK1982		LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																			1982																												LuRuB2			A	5.809	5.229	6.284												K		9.99					9.99																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110168	BOOK1982		YRu3B2	Y1Ru3B2	Y	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.481		3.028												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110169	BOOK1982		CeRu3B2	Ce1Ru3B2	Ce	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.527		2.991												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110170	BOOK1982		PrRu3B2	Pr1Ru3B2	Pr	1	Ru	3	B	2																			1982								6.85																				CeCo3B2			A	5.554		3.006												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110171	BOOK1982		NdRu3B2	Nd1Ru3B2	Nd	1	Ru	3	B	2																			1982								33.2																				CeCo3B2			A	5.544		3.01												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110172	BOOK1982	Tm>45 K	SmRu3B2	Sm1Ru3B2	Sm	1	Ru	3	B	2																			1982								45																				CeCo3B2			A	5.536		2.997												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110173	BOOK1982	Tm>45 K	GdRu3B2	Gd1Ru3B2	Gd	1	Ru	3	B	2																			1982								45																				CeCo3B2			A	5.508		3.018												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110174	BOOK1982	Tm>45 K	TbRu3B2	Tb1Ru3B2	Tb	1	Ru	3	B	2																			1982								45																				CeCo3B2			A	5.495		3.01												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110175	BOOK1982		DyRu3B2	Dy1Ru3B2	Dy	1	Ru	3	B	2																			1982								40.1																				CeCo3B2			A	5.485		3.011												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110176	BOOK1982		ScOsB2	Sc1Os1B2	Sc	1	Os	1	B	2																			1982																												LuRuB2			A	5.647	5.178	6.184												K		1.34					1.34																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110177	BOOK1982		YOsB2	Y1Os1B2	Y	1	Os	1	B	2																			1982																												LuRuB2			A	5.905	5.299	6.391												K		2.22					2.22																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110178	BOOK1982	not s/c	TbOsB2	Tb1Os1B2	Tb	1	Os	1	B	2																			1982								39.2																				LuRuB2			A	5.885	5.309	6.392												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110179	BOOK1982	not s/c	DyOsB2	Dy1Os1B2	Dy	1	Os	1	B	2																			1982								25.3																				LuRuB2			A	5.869	5.297	6.369												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110180	BOOK1982	not s/c	HoOsB2	Ho1Os1B2	Ho	1	Os	1	B	2																			1982								14.2																				LuRuB2			A	5.85	5.286	6.355												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110181	BOOK1982	not s/c	ErOsB2	Er1Os1B2	Er	1	Os	1	B	2																			1982								3.8																				LuRuB2			A	5.834	5.274	6.341												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110182	BOOK1982	not s/c	TmOsB2	Tm1Os1B2	Tm	1	Os	1	B	2																			1982								2.26																				LuRuB2			A	5.817	5.258	6.328												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110183	BOOK1982		LuOsB2	Lu1Os1B2	Lu	1	Os	1	B	2																			1982																												LuRuB2			A	5.809	5.231	6.318												K		2.66					2.66																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110184	BOOK1982	not s/c	HoRu3B2	Ho1Ru3B2	Ho	1	Ru	3	B	2																			1982								16.1																				CeCo3B2			A	5.474		3.017												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110185	BOOK1982	not s/c	ErRu3B2	Er1Ru3B2	Er	1	Ru	3	B	2																			1982								27.3																				CeCo3B2			A	5.467		3.017												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110186	BOOK1982	not s/c	TmRu3B2	Tm1Ru3B2	Tm	1	Ru	3	B	2																			1982								18.3																				CeCo3B2			A	5.461		3.012												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110187	BOOK1982	not s/c	YbRu3B2	Yb1Ru3B2	Yb	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.464		3.006												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110188	BOOK1982	not s/c	LuRu3B2	Lu1Ru3B2	Lu	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.454		3.004												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110189	BOOK1982		ThRu3B2	Th1Ru3B2	Th	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.526		3.07												K		1.79					1.79																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110190	BOOK1982	not s/c	URu3B2	U1Ru3B2	U	1	Ru	3	B	2																			1982																												CeCo3B2			A	5.476		2.96												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110191	BOOK1982		(Y,Th)Ru3B2	Y0.5Th0.5Ru3B2	Y	0.5	Th	0.5	Ru	3	B	2																	1982																												CeCo3B2			A	5.499		3.048												K		1.53					1.53																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110192	BOOK1982		LuOs3B2	Lu1Os3B2	Lu	1	Os	3	B	2																			1982																												CeCo3B2			A	5.457		3.052												K		4.62					4.62																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110193	BOOK1982		UOs3B2	U1Os3B2	U	1	Os	3	B	2																			1982																												CeCo3B2			A	5.523		2.976												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110194	BOOK1982		(Lu,Th)Os3B2	Lu0.5Th0.5Os3B2	Lu	0.5	Th	0.5	Os	3	B	2																	1982																												CeCo3B2			A	5.523		3.062												K		4.14					4.14																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110195	BOOK1982	not s/c. not magnetic	ScCo3B2	Sc1Co3B2	Sc	1	Co	3	B	2																			1982																												CeCo3B2			A	4.889		2.977												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110196	BOOK1982	not s/c. not magnetic	YCo3B2	Y1Co3B2	Y	1	Co	3	B	2																			1982																												CeCo3B2			A	5.033		3.038												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110197	BOOK1982	not s/c. not magnetic	CeCo3B2	Ce1Co3B2	Ce	1	Co	3	B	2																			1982																												CeCo3B2			A	5.057		3.036												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110198	BOOK1982	not s/c	SmCo3B2	Sm1Co3B2	Sm	1	Co	3	B	2																			1982								40																				CeCo3B2			A	5.101		2.991												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110199	BOOK1982	not s/c	GdCo3B2	Gd1Co3B2	Gd	1	Co	3	B	2																			1982								58																				CeCo3B2			A	5.059		3.019												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110200	BOOK1982	not s/c. not magnetic	TbCo3B2	Tb1Co3B2	Tb	1	Co	3	B	2																			1982																												CeCo3B2			A	5.048		3.005												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110201	BOOK1982	not s/c. not magnetic	DyCo3B2	Dy1Co3B2	Dy	1	Co	3	B	2																			1982																												CeCo3B2			A	5.028		3.015												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110202	BOOK1982	not s/c. not magnetic	HoCo3B2	Ho1Co3B2	Ho	1	Co	3	B	2																			1982																												CeCo3B2			A	5.026		3.029												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110203	BOOK1982	not s/c	ErCo3B2	Er1Co3B2	Er	1	Co	3	B	2																			1982								20																				CeCo3B2			A	5.003		3.024												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110204	BOOK1982	not s/c. not magnetic	TmCo3B2	Tm1Co3B2	Tm	1	Co	3	B	2																			1982																												CeCo3B2			A	4.991		3.019												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110205	BOOK1982	not s/c. not magnetic	YbCo3B2	Yb1Co3B2	Yb	1	Co	3	B	2																			1982																												CeCo3B2			A	4.985		3.02												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110206	BOOK1982	not s/c. not magnetic	LuCo3B2	Lu1Co3B2	Lu	1	Co	3	B	2																			1982																												CeCo3B2			A	4.959		3.035												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110207	BOOK1982	not s/c. not magnetic	UCo3B2	U1Co3B2	U	1	Co	3	B	2																			1982																												CeCo3B2			A	4.956		3.072												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110208	BOOK1982		LaRh3B2	La1Rh3B2	La	1	Rh	3	B	2																			1982																												CeCo3B2			A	5.48		3.137												K		2.82					2.82																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110209	BOOK1982		CeRh3B2	Ce1Rh3B2	Ce	1	Rh	3	B	2																			1982								115																				CeCo3B2			A	5.474		3.085												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110210	BOOK1982		PrRh3B2	Pr1Rh3B2	Pr	1	Rh	3	B	2																			1982								1.68																				CeCo3B2			A	5.461		3.105												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110211	BOOK1982		NdRh3B2	Nd1Rh3B2	Nd	1	Rh	3	B	2																			1982								13.5																				CeCo3B2			A	5.466		3.109												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110212	BOOK1982	Tm>45 K	SmRh3B2	Sm1Rh3B2	Sm	1	Rh	3	B	2																			1982								45																				CeCo3B2			A	5.437		3.09												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110213	BOOK1982		EuRh3B2	Eu1Rh3B2	Eu	1	Rh	3	B	2																			1982								41.7																				CeCo3B2			A	5.601		2.906												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110214	BOOK1982	Tm>45 K	GdRh3B2	Gd1Rh3B2	Gd	1	Rh	3	B	2																			1982								45																				CeCo3B2			A	5.404		3.115												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110215	BOOK1982		(Y,La)Rh3B2	Y0.5La0.5Rh3B2	Y	0.5	La	0.5	Rh	3	B	2																	1982																												CeCo3B2			A	5.434		3.127												K		1.88					1.88																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110216	BOOK1982		LaIr3B2	La1Ir3B2	La	1	Ir	3	B	2																			1982																												CeCo3B2			A	5.543		3.116												K		1.65					1.65																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110217	BOOK1982		ThIr3B2	Th1Ir3B2	Th	1	Ir	3	B	2																			1982																												CeCo3B2			A	5.449		3.23												K		2.09					2.09																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110218	BOOK1982		UIr3B2	U1Ir3B2	U	1	Ir	3	B	2																			1982																												CeCo3B2			A	5.369		3.181												K					1.2																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110219	BOOK1982		TiRuP	Ti1Ru1P1	Ti	1	Ru	1	P	1																			1982																												Fe2P			A	6.325		3.542												K		1.33					1.33																																																																																																arc melted					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110220	BOOK1982		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1982																												Fe2P			A	6.459		3.778												K		12.34					12.34																																																																																																arc melted + ANN(900C) - Q					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110221	BOOK1982		HfRuP	Hf1Ru1P1	Hf	1	Ru	1	P	1																			1982																												Fe2P			A	6.414		3.753												K		12.7					12.7																																																																																																SIN(1000C)-slow cool					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110222	BOOK1982		TiOsP	Ti1Os1P1	Ti	1	Os	1	P	1																			1982																												Fe2P			A	6.285		3.625												K					1.2																																																																																																		SIN(1000C)-slow cool					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110223	BOOK1982		ZrOsP	Zr1Os1P1	Zr	1	Os	1	P	1																			1982																												Fe2P			A	6.46		3.842												K		7.44					7.44																																																																																																SIN(1000C)-slow cool					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110224	BOOK1982		HfOsP	Hf1Os1P1	Hf	1	Os	1	P	1																			1982																												Fe2P			A	6.417		3.792												K		6.1					6.1																																																																																																SIN(1000C)-slow cool					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110225	BOOK1982		YRu3Si2	Y1Ru3Si2	Y	1	Ru	3	Si	2																			1982																												LaRu3Si2			A	5.543		7.152												K		3.51					3.51																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110226	BOOK1982		LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																			1982																												LaRu3Si2			A	5.676		7.12												K		7.6					7.6																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110227	BOOK1982		ThRu3Si2	Th1Ru3Si2	Th	1	Ru	3	Si	2																			1982																												LaRu3Si2			A	5.605		7.201												K		3.98					3.98																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110228	BOOK1982		BaPt3B2	Ba0.67Pt3B2	Ba	0.67	Pt	3	B	2																			1982																												LaRu3Si2			A	6.161		5.268												K		5.6					5.6																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110229	BOOK1982		SrPt3B2	Sr0.67Pt3B2	Sr	0.67	Pt	3	B	2																			1982																												LaRu3Si2			A	6.092		5.184												K		2.78					2.78																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110230	BOOK1982		CaPt3B2	Ca0.67Pt3B2	Ca	0.67	Pt	3	B	2																			1982																												LaRu3Si2			A	5.989		5.127												K		1.57					1.57																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110231	BOOK1982			Ca1Rh1.2Sn4.5	Ca	1	Rh	1.2	Sn	4.5																			1982																												Pr3Rh4Sn13			A	9.702														K		8.7					8.7																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110232	BOOK1982			Yb1Rh1.4Sn4.6	Yb	1	Rh	1.4	Sn	4.6																			1982																												Pr3Rh4Sn13			A	9.675														K		8.6					8.6																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110233	BOOK1982			La1Ru1.5Sn4.5	La	1	Ru	1.5	Sn	4.5																			1982																												Pr3Rh4Sn13			A	9.772														K		3.9					3.9																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110234	BOOK1982			Ca1Pt1.4Sn4.3	Ca	1	Pt	1.4	Sn	4.3																			1982																												Pr3Rh4Sn13			A	9.76														K					1.1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110235	BOOK1982		Y3Ru4Ge13	Y3Ru4Ge13	Y	3	Ru	4	Ge	13																			1982																												Pr3Rh4Sn13			A	8.962														K		1.7					1.7																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110236	BOOK1982	not s/c	Ce3Ru4Ge13	Ce3Ru4Ge13	Ce	3	Ru	4	Ge	13																			1982								6.7																				Pr3Rh4Sn13			A	9.045														K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110237	BOOK1982	not s/c	Pr3Ru4Ge13	Pr3Ru4Ge13	Pr	3	Ru	4	Ge	13																			1982								14.2																				Pr3Rh4Sn13			A	9.069														K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110238	BOOK1982	not s/c	Er3Ru4Ge13	Er3Ru4Ge13	Er	3	Ru	4	Ge	13																			1982								1.2																				Pr3Rh4Sn13			A	8.941														K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110239	BOOK1982		Lu3Ru4Ge13	Lu3Ru4Ge13	Lu	3	Ru	4	Ge	13																			1982																												Pr3Rh4Sn13			A	8.912														K		2.3					2.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110240	BOOK1982		Y3Os4Ge13	Y3Os4Ge13	Y	3	Os	4	Ge	13																			1982																												Pr3Rh4Sn13			A	8.985														K		3.9					3.9																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110241	BOOK1982		Lu3Os4Ge13	Lu3Os4Ge13	Lu	3	Os	4	Ge	13																			1982																												Pr3Rh4Sn13			A	8.938														K		3.6					3.6																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110242	BOOK1982	p-49		Er1Rh1.1Sn3.6	Er	1	Rh	1.1	Sn	3.6																			1982																															A	13.733		27.418												K		1.36					1.36																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110243	BOOK1982	p-49		Lu1Rh1.2Sn4	Lu	1	Rh	1.2	Sn	4																			1982																															A	13.693		9.648												K		4					4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110244	BOOK1982	p-49		Y1Rh1.1Sn3.1	Y	1	Rh	1.1	Sn	3.1																			1982																															A	13.772														K		1.3					1.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110245	BOOK1982		Sc2Fe3Si5	Sc2Fe3Si5	Sc	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.225		5.275												K		4.52					4.52																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110246	BOOK1982		Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.43		5.47												K		2.4					2.4																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110247	BOOK1982		Sm2Fe3Si5	Sm2Fe3Si5	Sm	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.47		5.55												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110248	BOOK1982		Gd2Fe3Si5	Gd2Fe3Si5	Gd	2	Fe	3	Si	5																			1982								8.6																				Sc2Fe3Si5			A	10.47		5.513												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110249	BOOK1982		Tb2Fe3Si5	Tb2Fe3Si5	Tb	2	Fe	3	Si	5																			1982								10.3																				Sc2Fe3Si5			A	10.43		5.48												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110250	BOOK1982		Dy2Fe3Si5	Dy2Fe3Si5	Dy	2	Fe	3	Si	5																			1982								4.4																				Sc2Fe3Si5			A	10.423		5.465												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110251	BOOK1982		Ho2Fe3Si5	Ho2Fe3Si5	Ho	2	Fe	3	Si	5																			1982								2.9																				Sc2Fe3Si5			A	10.39		5.44												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110252	BOOK1982		Er2Fe3Si5	Er2Fe3Si5	Er	2	Fe	3	Si	5																			1982								2.9																				Sc2Fe3Si5			A	10.385		5.425												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110253	BOOK1982		Tm2Fe3Si5	Tm2Fe3Si5	Tm	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.37		5.4												K		1.3					1.3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110254	BOOK1982	not s/c	Yb2Fe3Si5	Yb2Fe3Si5	Yb	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.36		5.385												K					1																																																																																																							"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110255	BOOK1982		Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.34		5.375												K		6.1					6.1																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110256	BOOK1982	not s/c. not magnetic phase	Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																			1982																												Sc2Fe3Si5			A	10.68		5.623												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110257	BOOK1982	not s/c. not magnetic phase	Lu2Os3Si5	Lu2Os3Si5	Lu	2	Os	3	Si	5																			1982																												Sc2Fe3Si5			A	10.63		5.588												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110258	BOOK1982	not s/c. not magnetic phase	Y2Os3Si5	Y2Os3Si5	Y	2	Os	3	Si	5																			1982																												Sc2Fe3Si5			A	10.68		5.658												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110259	BOOK1982		Y2Re3Si5	Y2Re3Si5	Y	2	Re	3	Si	5																			1982																												Sc2Fe3Si5			A	10.88		5.533												K		1.76					1.76																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110260	BOOK1982		Sc5Co4Si10	Sc5Co4Si10	Sc	5	Co	4	Si	10																			1982																												Sc5Co4Si10			A	12.01		3.936												K		5					5																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110261	BOOK1982		Sc5Rh4Si10	Sc5Rh4Si10	Sc	5	Rh	4	Si	10																			1982																												Sc5Co4Si10			A	12.325		4.032												K		8.54					8.54																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110262	BOOK1982		Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1982																												Sc5Co4Si10			A	12.316		4.076												K		8.46					8.46																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110263	BOOK1982		Y5Ir4Si10	Y5Ir4Si10	Y	5	Ir	4	Si	10																			1982																												Sc5Co4Si10			A	12.599		4.234												K		3					3																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110264	BOOK1982		Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1982																												Sc5Co4Si10			A	12.475		4.171												K		3.76					3.76																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110265	BOOK1982	not s/c	Tm5Ir4Si10	Tm5Ir4Si10	Tm	5	Ir	4	Si	10																			1982								1																				Sc5Co4Si10			A	12.52		4.195												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110266	BOOK1982	not s/c	Er5Ir4Si10	Er5Ir4Si10	Er	5	Ir	4	Si	10																			1982								2.3																				Sc5Co4Si10			A	12.543		4.203												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110267	BOOK1982	not s/c	Ho5Ir4Si10	Ho5Ir4Si10	Ho	5	Ir	4	Si	10																			1982								1.5																				Sc5Co4Si10			A	12.554		4.215												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110268	BOOK1982	not s/c	Dy5Ir4Si10	Dy5Ir4Si10	Dy	5	Ir	4	Si	10																			1982								5																				Sc5Co4Si10			A	12.569		4.227												K																																																																																																												"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110269	BOOK1982		Yr5Ir4Si10	Y5Ir4Si10	Y	5	Ir	4	Si	10																			1982																												Sc5Co4Si10			A	12.927		4.308												K		2.62					2.62																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110270	BOOK1982		Y5Os4Ge10	Y5Os4Ge10	Y	5	Os	4	Ge	10																			1982																												Sc5Co4Si10			A	13.006		4.297												K		8.68					8.68																																																																																																					"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
110271	LES0620197	single phase	(Au,Pd)Ga2	Au0.098Pd0.02Ga2	Au	0.098	Pd	0.02	Ga	2																			1978																																														K		1.51					1.51																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110272	LES0620197	single phase	(Au,Pd)Ga2	Au0.93Pd0.07Ga2	Au	0.93	Pd	0.07	Ga	2																			1978																																														K		1.773					1.773																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110273	LES0620197	two phase	(Au,Pd)Ga2	Au0.85Pd0.15Ga2	Au	0.85	Pd	0.15	Ga	2																			1978																																														K		1.79					1.79																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110274	LES0620197	single phase (AuGa)	(Au,Ga)	Au0.499Ga0.501	Au	0.499	Ga	0.501																					1978																																														K		1.17					1.17																													kOe/K		0.106																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110275	LES0620197	two phase (AuGa + AuGa2)	(Au,Ga)	Au0.427Ga0.573	Au	0.427	Ga	0.573																					1978																																														K		1.378					1.378																													kOe/K		0.123																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110276	LES0620197	two phase (AuGa + AuGa2)	(Au,Ga)	Au0.388Ga0.612	Au	0.388	Ga	0.612																					1978																																														K		1.355					1.355																													kOe/K		0.112																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110277	LES0620197	single phase (AuGa2)	(Au,Ga)	Au0.328Ga0.672	Au	0.328	Ga	0.672																					1978																																														K		1.668					1.668																													kOe/K		0.412																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110278	LES0620197	single phase (AuGa2)	(Au,Ga)	Au0.293Ga0.707	Au	0.293	Ga	0.707																					1978																																														K		1.63					1.63																													kOe/K		0.252																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110279	LES0620197	single phase (AuGa2)	(Au,Ga)	Au0.281Ga0.719	Au	0.281	Ga	0.719																					1978																																														K		1.587					1.587																													kOe/K		0.241																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110280	LES0620197	two phase (AuGa2 + Ga)	(Au,Ga)	Au0.278Ga0.722	Au	0.278	Ga	0.722																					1978																																														K		1.615					1.615																													kOe/K		0.243																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110281	LES0620197	two phase (AuGa2 + Ga)	(Au,Ga)	Au0.2Ga0.8	Au	0.2	Ga	0.8																					1978																																														K		1.587					1.587																													kOe/K		0.243																																																																						Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
110282	LES0840107	density=4.40 g/cm3. S=-4.7 uV/K	YB2C2	Y1B2C2	Y	1	B	2	C	2																			1982																																														K																																																																																																												Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
110283	LES0840107	density=7.52  g/cm3. S=-2.5 uV/K	LuB2C2	Lu1B2C2	Lu	1	B	2	C	2																			1982																																														K																																																																																																												Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
110284	LES0840107	density=5.29 g/cm3. S=-5.2 uV/K	LaB2C2	La1B2C2	La	1	B	2	C	2																			1982																																														K																																																																																																												Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
110285	SSC0320937		(Y,Lu)Ir4B4	Y0.2Lu0.8Ir4B4	Y	0.2	Lu	0.8	Ir	4	B	4																	1979																												RT4B4			A	5.4		7.251											CeCo4B4-type	K		3.04					3.04																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110286	SSC0320937		(Y,Lu)Ir4B4	Y0.3Lu0.7Ir4B4	Y	0.3	Lu	0.7	Ir	4	B	4																	1979																												RT4B4			A	5.402		7.272											CeCo4B4-type	K		2.98					2.98																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110287	SSC0320937		(Y,Lu)Ir4B4	Y0.4Lu0.6Ir4B4	Y	0.4	Lu	0.6	Ir	4	B	4																	1979																												RT4B4			A	5.403		7.268											CeCo4B4-type	K		3.07					3.07																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110288	SSC0320937		(Y,Lu)Ir4B4	Y0.5Lu0.5Ir4B4	Y	0.5	Lu	0.5	Ir	4	B	4																	1979																												RT4B4			A	5.405		7.28											CeCo4B4-type	K		3.21					3.21																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110289	SSC0320937		(Y,Lu)Ir4B4	Y0.6Lu0.4Ir4B4	Y	0.6	Lu	0.4	Ir	4	B	4																	1979																												RT4B4																	CeCo4B4-type	K		3.06					3.06																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110290	SSC0320937		Ho(Ir,Rh)4B4	Ho1Ir3.6Rh0.4B4	Ho	1	Ir	3.6	Rh	0.4	B	4																	1979																												RT4B4																	CeCo4B4-type	K		1.9					1.9																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110291	SSC0320937		Ho(Ir,Rh)4B4	Er1Ir3.6Rh0.4B4	Er	1	Ir	3.6	Rh	0.4	B	4																	1979																												RT4B4																	CeCo4B4-type	K		1.83					1.83																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110292	SSC0320937		Ho(Ir,Rh)4B4	Tm1Ir3.6Rh0.4B4	Tm	1	Ir	3.6	Rh	0.4	B	4																	1979																												RT4B4																	CeCo4B4-type	K		1.48					1.48																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110293	SSC0320937		Ho(Ir,Rh)4B4	Lu1Ir3.6Rh0.4B4	Lu	1	Ir	3.6	Rh	0.4	B	4																	1979																												RT4B4																	CeCo4B4-type	K		2.67					2.67																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110294	SSC0320937		(Sc,Y)(Ir,Rh)4B4	Sc0.1Y0.9Ir3.6Rh0.4B4	Sc	0.1	Y	0.9	Ir	3.6	Rh	0.4	B	4															1979																												RT4B4																	CeCo4B4-type	K		3.45					3.45																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110295	SSC0320937		(Sc,Y)(Ir,Rh)4B4	Sc0.2Y0.8Ir3.6Rh0.4B4	Sc	0.2	Y	0.8	Ir	3.6	Rh	0.4	B	4															1979																												RT4B4																	CeCo4B4-type	K		3.01					3.01																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110296	SSC0320937		(Sc,Y)(Ir,Rh)4B4	Sc0.25Y0.75Ir3.6Rh0.4B4	Sc	0.25	Y	0.75	Ir	3.6	Rh	0.4	B	4															1979																												RT4B4																	CeCo4B4-type	K		2.92					2.92																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110297	SSC0320937		(Sc,Y)(Ir,Rh)4B4	Sc0.3Y0.7Ir3.6Rh0.4B4	Sc	0.3	Y	0.7	Ir	3.6	Rh	0.4	B	4															1979																												RT4B4																	CeCo4B4-type	K		3.09					3.09																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110298	SSC0320937		(Sc,Y)(Ir,Rh)4B4	Sc0.5Y0.5Ir3.6Rh0.4B4	Sc	0.5	Y	0.5	Ir	3.6	Rh	0.4	B	4															1979																												RT4B4																	CeCo4B4-type	K		3.01					3.01																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110299	SSC0320937		Dy(Ir,Rh)4B4	Dy1Ir2Rh2B4	Dy	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		4.64					4.64																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110300	SSC0320937		Ho(Ir,Rh)4B4	Ho1Ir2Rh2B4	Ho	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		6.41					6.41																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110301	SSC0320937		Er(Ir,Rh)4B4	Er1Ir2Rh2B4	Er	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		7.37					7.37																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110302	SSC0320937		Tm(Ir,Rh)4B4	Tm1Ir2Rh2B4	Tm	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		4.38					4.38																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110303	SSC0320937		Lu(Ir,Rh)4B4	Lu1Ir2Rh2B4	Lu	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		3.08					3.08																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110304	SSC0320937		Y(Ir,Rh)4B4	Y1Ir2Rh2B4	Y	1	Ir	2	Rh	2	B	4																	1979																												RT4B4																	CeCo4B4-type	K		8.92					8.92																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
110305	SSC0410063			Tb1Os1.5Sn2.6	Tb	1	Os	1.5	Sn	2.6																			1982							-7																								A	13.812														K		1.4					1.4																																																																																																					Magnetic and superconducting properties of rare earth osmium stannides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 41(1982)63	A.S.Cooper,G.P.Espinosa,H.Barz,J.P.Remeika,M.B.Maple,S.E.Lambert,S.Oseroff,Z.Fisk		
110306	SSC0410063			Ho1Os1.2Sn2.5	Ho	1	Os	1.2	Sn	2.5																			1982							-2																								A	13.776														K		1.4					1.4																																																																																																					Magnetic and superconducting properties of rare earth osmium stannides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 41(1982)63	A.S.Cooper,G.P.Espinosa,H.Barz,J.P.Remeika,M.B.Maple,S.E.Lambert,S.Oseroff,Z.Fisk		
110307	SSC0410063			Er1Os1.1Sn2.7	Er	1	Os	1.1	Sn	2.7																			1982							-3																								A	13.76														K		1.3					1.3																																																																																																					Magnetic and superconducting properties of rare earth osmium stannides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 41(1982)63	A.S.Cooper,G.P.Espinosa,H.Barz,J.P.Remeika,M.B.Maple,S.E.Lambert,S.Oseroff,Z.Fisk		
110308	SSC0340923	density=8.9 g/cm3		Yb1Rh1.4Sn4.6	Yb	1	Rh	1.4	Sn	4.6																			1980																																														K		8.6					8.6																													kG/K		3.5																																																																						A new famili of ternary intermetallic superconducting/magnetic stannides			Bell Lab, Murray Hill, NJ, USA	Solid State Commun., 34(1980)923	A.S.Cooper,D.B.McWhan,D.E.Moncton,G.P.Espinosa,G.Shirane,H.Barz,H.C.Hamaker,J.M.Rowell,J.M.Vandenberg,J.P.Remeika,L.D.Woolf,M.B.Maple,W.Thomlinson,Z.Fisk		
110309	SSC0340923	density=9.6 g/cm3		Lu1Rh1.2Sn4	Lu	1	Rh	1.2	Sn	4																			1980																																														K		4					4																													kG/K		20.3																																																																						A new famili of ternary intermetallic superconducting/magnetic stannides			Bell Lab, Murray Hill, NJ, USA	Solid State Commun., 34(1980)923	A.S.Cooper,D.B.McWhan,D.E.Moncton,G.P.Espinosa,G.Shirane,H.Barz,H.C.Hamaker,J.M.Rowell,J.M.Vandenberg,J.P.Remeika,L.D.Woolf,M.B.Maple,W.Thomlinson,Z.Fisk		
110310	SSC0340923	density=8.3 g/cm3		Ca1Rh1.2Sn4.5	Ca	1	Rh	1.2	Sn	4.5																			1980																															A	9.702														K		8.7					8.7																													kG/K		4																																																																						A new famili of ternary intermetallic superconducting/magnetic stannides			Bell Lab, Murray Hill, NJ, USA	Solid State Commun., 34(1980)923	A.S.Cooper,D.B.McWhan,D.E.Moncton,G.P.Espinosa,G.Shirane,H.Barz,H.C.Hamaker,J.M.Rowell,J.M.Vandenberg,J.P.Remeika,L.D.Woolf,M.B.Maple,W.Thomlinson,Z.Fisk		
110311	MRB0101169		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1975																												Chevrel																		K		13.5					13.5																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110312	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S7.9Se0.1	Pb	1	Mo	6	S	7.9	Se	0.1																	1975																												Chevrel																		K		12.7					12.7																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110313	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S7.5Se0.5	Pb	1	Mo	6	S	7.5	Se	0.5																	1975																												Chevrel																		K		10.6					10.6																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110314	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S7Se1	Pb	1	Mo	6	S	7	Se	1																	1975																												Chevrel																		K		8.4					8.4																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110315	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S6Se2	Pb	1	Mo	6	S	6	Se	2																	1975																												Chevrel																		K		5.4					5.4																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110316	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S5Se3	Pb	1	Mo	6	S	5	Se	3																	1975																												Chevrel																		K		4.3					4.3																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110317	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S4Se4	Pb	1	Mo	6	S	4	Se	4																	1975																												Chevrel																		K		3.2					3.2																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110318	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S4Se5	Pb	1	Mo	6	S	4	Se	5																	1975																												Chevrel																		K		3.64					3.64																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110319	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S2Se6	Pb	1	Mo	6	S	2	Se	6																	1975																												Chevrel																		K		4.92					4.92																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110320	MRB0101169		PbMo6(S,Se)8	Pb1Mo6S1Se7	Pb	1	Mo	6	S	1	Se	7																	1975																												Chevrel																		K		7.13					7.13																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110321	MRB0101169		PbMo6Se8	Pb1Mo6Se8	Pb	1	Mo	6	Se	8																			1975																												Chevrel																		K		3.54					3.54																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110322	MRB0101169		(Pb,Yb)Mo6S8	Pb0.9Yb0.1Mo6Se8	Pb	0.9	Yb	0.1	Mo	6	Se	8																	1975																												Chevrel																		K		12.3					12.3																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110323	MRB0101169		(Pb,Yb)Mo6S8	Pb0.8Yb0.2Mo6Se8	Pb	0.8	Yb	0.2	Mo	6	Se	8																	1975																												Chevrel																		K		12.2					12.2																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110324	MRB0101169		(Pb,Yb)Mo6S8	Pb0.7Yb0.3Mo6Se8	Pb	0.7	Yb	0.3	Mo	6	Se	8																	1975																												Chevrel																		K		10.2					10.2																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110325	MRB0101169		(Pb,Yb)Mo6S8	Pb0.6Yb0.4Mo6Se8	Pb	0.6	Yb	0.4	Mo	6	Se	8																	1975																												Chevrel																		K		9.2					9.2																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110326	MRB0101169		(Pb,Yb)Mo6S8	Pb0.5Yb0.5Mo6Se8	Pb	0.5	Yb	0.5	Mo	6	Se	8																	1975																												Chevrel																		K		8.7					8.7																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110327	MRB0101169		(Pb,Yb)Mo6S8	Pb0.4Yb0.6Mo6Se8	Pb	0.4	Yb	0.6	Mo	6	Se	8																	1975																												Chevrel																		K		7.9					7.9																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110328	MRB0101169		(Pb,Yb)Mo6S8	Pb0.3Yb0.7Mo6Se8	Pb	0.3	Yb	0.7	Mo	6	Se	8																	1975																												Chevrel																		K		7.1					7.1																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110329	MRB0101169		(Pb,Yb)Mo6S8	Pb0.2Yb0.8Mo6Se8	Pb	0.2	Yb	0.8	Mo	6	Se	8																	1975																												Chevrel																		K		6.7					6.7																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110330	MRB0101169		(Pb,Yb)Mo6S8	Pb0.1Yb0.9Mo6Se8	Pb	0.1	Yb	0.9	Mo	6	Se	8																	1975																												Chevrel																		K		6.3					6.3																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110331	MRB0101169		(Pb,Yb)Mo6S8	Yb1Mo6Se8	Yb	1	Mo	6	Se	8																			1975																												Chevrel																		K		6					6																																																																																																					A study of the solid solutions PbyMo6X8−xX'x and Mo6X8-xX'x (X, X' = S, Se, Te) and their superconducting properties				Mat.Res.Bull., 10(1975)1169	F.Fischer,M.Sergent,R.Chevrel		
110332	PTUG1980MDEC		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1980																												Chevrel																		K		6.38					6.38																													T/K		1.81																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110333	PTUG1980MDEC		Mo6(Se,S)8	Mo6Se7.85S0.15	Mo	6	Se	7.85	S	0.15																			1980																												Chevrel																		K		6.3					6.3																													T/K		4.17																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110334	PTUG1980MDEC		Mo6(Se,S)8	Mo6Se7.7S0.3	Mo	6	Se	7.7	S	0.3																			1980																												Chevrel																		K		5.83					5.83																													T/K		4.34																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110335	PTUG1980MDEC		Mo6(Se,S)8	Mo6Se7.5S0.5	Mo	6	Se	7.5	S	0.5																			1980																												Chevrel																		K		5.45					5.45																													T/K		4.39																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110336	PTUG1980MDEC		Mo6(Se,S)8	Mo6Se7.3S0.7	Mo	6	Se	7.3	S	0.7																			1980																												Chevrel																		K		5.03					5.03																													T/K		4.51																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110337	PTUG1980MDEC		Mo6(Se,S)8	Mo6Se7S1	Mo	6	Se	7	S	1																			1980																												Chevrel																		K		4.48					4.48																													T/K		4.6																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110338	PTUG1980MDEC		Mo6(Se,Te)8	Mo6Se7.9Te0.1	Mo	6	Se	7.9	Te	0.1																			1980																												Chevrel																		K		6.3					6.3																													T/K		4.14																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110339	PTUG1980MDEC		Mo6(Se,Te)8	Mo6Se7.7Te0.3	Mo	6	Se	7.7	Te	0.3																			1980																												Chevrel																		K		6.66					6.66																													T/K		3.88																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110340	PTUG1980MDEC		Mo6(Se,Te)8	Mo6Se7.5Te0.5	Mo	6	Se	7.5	Te	0.5																			1980																												Chevrel																		K		6.69					6.69																													T/K		4.45																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110341	PTUG1980MDEC		Mo6(Se,Te)8	Mo6Se6.5Te1.5	Mo	6	Se	6.5	Te	1.5																			1980																												Chevrel																		K		6.23					6.23																													T/K		4.73																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110342	PTUG1980MDEC		Mo6(Se,Te)8	Mo6Se6Te2	Mo	6	Se	6	Te	2																			1980																												Chevrel																		K		5.88					5.88																													T/K		4.57																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110343	PTUG1980MDEC		Mo6(Se,Cl)8	Mo6Se7.5Cl0.5	Mo	6	Se	7.5	Cl	0.5																			1980																												Chevrel																		K		6.33					6.33																													T/K		3.86																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110344	PTUG1980MDEC		Mo6(Se,Cl)8	Mo6Se7Cl1	Mo	6	Se	7	Cl	1																			1980																												Chevrel																		K		6.52					6.52																													T/K		4.63																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110345	PTUG1980MDEC		Mo6(Se,Cl)8	Mo6Se6.5Cl1.5	Mo	6	Se	6.5	Cl	1.5																			1980																												Chevrel																		K		6.49					6.49																													T/K		4.96																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110346	PTUG1980MDEC		Mo6(Se,Cl)8	Mo6Se6Cl2	Mo	6	Se	6	Cl	2																			1980																												Chevrel																		K		6.39					6.39																													T/K		5.06																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110348	PTUG1980MDEC		(Mo,Ru)6Se8	Mo5.8Ru0.2Se8	Mo	5.8	Ru	0.2	Se	8																			1980																												Chevrel																		K		6.21					6.21																													T/K		4.01																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110349	PTUG1980MDEC		(Mo,Ru)6Se8	Mo5.6Ru0.4Se8	Mo	5.6	Ru	0.4	Se	8																			1980																												Chevrel																		K		5.69					5.69																													T/K		4.48																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110350	PTUG1980MDEC		(Mo,Ru)6Se8	Mo5.5Ru0.5Se8	Mo	5.5	Ru	0.5	Se	8																			1980																												Chevrel																		K		5.43					5.43																													T/K		4.4																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110351	PTUG1980MDEC		(Mo,Ru)6Se8	Mo5Ru1Se8	Mo	5	Ru	1	Se	8																			1980																												Chevrel																		K		3.7					3.7																													T/K		4.38																																																																						"From ""Superconductivity in ternary compounds II""ed by M.B.Maple & F.Fischer"				Phd thesis, University of Geneva, 1980	M.Decroux		
110352	TER1981		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1981																												Chevrel																		K		6.3					6.3																				T		8.6							T/K		1.7																																																																									ed. By G.K.Shenoy, B.D.Dunlop, F.Y.Fradin (North Holland, Amsterdam 1981) pp 65 - 68	"""Ternary Superconductors"""	B.Lachal,C.Rossel,F.Fischer,M.Decroux,M.Sergent,R.Baillif,R.Chevrel		
110353	TER1981		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1981																												Chevrel																		K		6.2					6.2																				T		16.5							T/K		3.6																																																																									ed. By G.K.Shenoy, B.D.Dunlop, F.Y.Fradin (North Holland, Amsterdam 1981) pp 65 - 68	"""Ternary Superconductors"""	B.Lachal,C.Rossel,F.Fischer,M.Decroux,M.Sergent,R.Baillif,R.Chevrel		
110354	PLA0570345		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1976																												Chevrel																		K		11.3					11.3																				T									T/K		7																																																																										Phys.Lett.A, 57(1976)345	E.J.McNiff,M.B.Maple,R.N.Shelton,R.W.MaCallum,S.Foner		
110355	JPH0390257		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1978																												Chevrel																		K		10.8					10.8																				T		44.5							T/K		7.5																																																																										J.Physique, 39(1978)C2 - 257	F.Fischer,M.Decroux,M.Sergent,R.Chevrel		
110356	APL0160001		LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1978																												Chevrel																		K		5.8					5.8																				T		5.4							T/K		1.5																																																																										Appl.Phys., 16(1978)1	F.Fischer		
110357	SSC0250141		CuMo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1978																												Chevrel																		K		10					10																				T		19.2							T/K		2.5																																																																						Upper critical field of copper molybdenum sulfide				Solid State Commun., 25(1978)141	J.A.Woolam,S.A.Alterovitz		
110358	SSC0250141		CuMo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1978																												Chevrel																		K		10.5					10.5																				T		15.3							T/K		1.9																																																																						Upper critical field of copper molybdenum sulfide				Solid State Commun., 25(1978)141	J.A.Woolam,S.A.Alterovitz		
110359	PLA0490269		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1974																												Chevrel																		K		13.4					13.4																				T		34.4							T/K		3.7																																																																										Phys.Lett.A, 49(1974)269	E.J.Alexander,E.J.McNiff,S.Foner		
110360	JPH0390257		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1978																												Chevrel																		K		11.8					11.8																				T		34							T/K		4.7																																																																										J.Physique, 39(1978)C2 - 257	F.Fischer,M.Decroux,M.Sergent,R.Chevrel		
110361	CRY2570001		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1980																												Chevrel																		K		11.7					11.7																				T		36							T/K		3.7																																																																						Some physical properties of multicomponent molybdenum chalcogenides				Cryogenics,  20(1980)257	N.E.Alekseevskii		
110362	PLA0490269		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1974																												Chevrel																		K		14.4					14.4																				T		60							T/K		6																																																																										Phys.Lett.A, 49(1974)269	E.J.Alexander,E.J.McNiff,S.Foner		
110363	DF1976		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1976																												Chevrel																		K		12.6					12.6																				T		50							T/K		5.8																																																																									ed. By D.H.Douglass (Plenum Press, New York 1976) p 175	"""Superconductivity in d- and f-band Metals"""	F.Fischer,M.Decroux,M.Sergent,R.Chevrel		
110364	JPS0482157		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1980																												Chevrel																		K		13.3					13.3																				T		60							T/K		6																																																																						Upper critical field measurements up to 600 kG in PbMo6S8				J.Phys.Soc.Jpn, 48(1980)2157	K.Okuda,M.Date,M.Kitagawa,T.Sakakibara		
111000	PR04307681	Tc jump to 8.14 K at Pc= 23.1 kbar. CDW-temp= 82 K.	(Lu,Er)5Ir4Si10	Lu4.5Er0.5Ir4Si10	Lu	4.5	Er	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		2.74					2.74																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111001	PR04307681	Tc jump to 7.29 K at Pc= 20.8 kbar. CDW-temp= 82 K.	(Lu,Ho)5Ir4Si10	Lu4.5Ho0.5Ir4Si10	Lu	4.5	Ho	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		1.89					1.89																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111002	PR04307681	Tc jump to 6.3 K at Pc= 20.5 kbar. CDW-temp= 78 K.	(Lu,Dy)5Ir4Si10	Lu4.5Dy0.5Ir4Si10	Lu	4.5	Dy	0.5	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		1					1																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111003	PR04307681	dTc/dp in K/GPa. 	Lu5(Ir,Rh)4Si10	Lu5Ir3.44Rh0.56Si10	Lu	5	Ir	3.44	Rh	0.56	Si	10																	1991																												Sc5Co4Si10																		K		5.72					5.72			K/GPa	0.304																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111004	PR04307681	dTc/dp in K/GPa. 	Lu5(Ir,Rh)4Si10	Lu5Ir3.12Rh0.88Si10	Lu	5	Ir	3.12	Rh	0.88	Si	10																	1991																												Sc5Co4Si10																		K		5.68					5.68			K/GPa	0.11																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111005	PR04307681	dTc/dp in K/GPa. 	Lu5(Ir,Co)4Si10	Lu5Ir3.8Co0.2Si10	Lu	5	Ir	3.8	Co	0.2	Si	10																	1991																												Sc5Co4Si10																		K		5.52					5.52			K/GPa	0.338																																																																																												arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111006	PR04307681	CDW-temp=70.9	(Lu,Sc)5Ir4Si10	Lu4.975Sc0.025Ir4Si10	Lu	4.975	Sc	0.025	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		4					4																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111007	PR04307681	CDW-temp=61.8	(Lu,Sc)5Ir4Si10	Lu4.95Sc0.05Ir4Si10	Lu	4.95	Sc	0.05	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		4.5					4.5																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111008	PR04307681	CDW-temp=45.9	(Lu,Sc)5Ir4Si10	Lu4.9Sc0.1Ir4Si10	Lu	4.9	Sc	0.1	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		5.77					5.77																																																																																																arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111009	PR04307681	"s/c parameters calculated using data of ""Usp.Fiz.Nauk, 115(1975)263"". G-L parameter = 11.9"	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		8.23					8.23																				T		0.9							T/K		0.15					A		150			A		1920													mj/mol.K2	8.4																																							arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111010	PR04307681	"s/c parameters calculated using data of ""Usp.Fiz.Nauk, 115(1975)263"". G-L parameter = 35.8"	Lu5Rh4Si10	Lu5Rh4Si10	Lu	5	Rh	4	Si	10																			1991																												Sc5Co4Si10																		K		3.91					3.91																				T		1.48							T/K		0.64					A		115			A		4110													mj/mol.K2	17.4																																							arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111011	PR04307681	"s/c parameters calculated using data of ""Usp.Fiz.Nauk, 115(1975)263"". G-L parameter = 30.9"	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1991																												Sc5Co4Si10																		K		3.88					3.88																				T		1.04							T/K		0.39					A		160			A		4550													mj/mol.K2	8.8																																							arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111012	PR04307681	gamma in mj/mol.K2 calculated using dHc2/dT, R, etc. G-L parameter = 37.1	(Lu,Sc)5Ir4Si10	Lu4.9Sc0.1Ir4Si10	Lu	4.9	Sc	0.1	Ir	4	Si	10																	1991																												Sc5Co4Si10																		K		5.9					5.9																				T		2.3							T/K		0.57					A		100			A		3670													mj/mol.K2	12.9																																							arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111013	PR04307681	gamma in mj/mol.K2 calculated using dHc2/dT, R, etc. G-L parameter = 56.3	Lu5(Ir,Rh)4Si10	Lu5Ir3.12Rh0.88Si10	Lu	5	Ir	3.12	Rh	0.88	Si	10																	1991																												Sc5Co4Si10																		K		5.8					5.8																				T		3.12							T/K		0.78					A		85			A		4810													mj/mol.K2	10.5																																							arc-melting + ANN(1250C,1d+1050C,3days)					Competition between superconductivity and charge-density wavws in the pseudoternary system (Lu1-xScx)5Ir4Si10			Department of Physics, National Sun Yat-sen University, Taiwan, Republic of China	Phys.Rev.B, 43(1991)7681	H.D.Yang,P.Klavins,R.N.Shelton		
111014	PCS0631165	sample is #50 in the text. slightly reentrant behavior in the resistive transition. specific heat were measured.	CeCu2Si2	Ce1Cu1.95Si2.01	Ce	1	Cu	1.95	Si	2.01																		3	2002																															A	4.098		9.911												K		0.62					0.62																																		MHC11014																																																														levitation melting (850C,10d) + ANN(750C,6d)					Ferromagnetic interaction and superconductivity of CeCu2Si2			Institute for Solid State Physics, University of Tokyo,Kashiwa,Chiba,Japan	J.Phys.Chem.Solids, 63(2002)1165	D.Huo,H.Ishimoto,J.Sakurai,M.Ishikawa,N.Takeda,P.Ahmet,Y.Karaki		
111015	PCS0631141	Tc(P) was measured. Tc=0.65, 0.64, 0.64, 0.64, 0.75 K, at p=0, 0.3, 0.9, 1.4, 2.6 GPa , respectively.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																			2002																																														K		0.65					0.65																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111016	PCS0631141		CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																			2002																																														K		0.64					0.64																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111017	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.98Ge0.02	Ce	1	Cu	2	Si	1.98	Ge	0.02																	2002																																														K		0.54					0.54																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111018	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.96Ge0.04	Ce	1	Cu	2	Si	1.96	Ge	0.04																	2002								0.69																																						K		0.37					0.37																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111019	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.92Ge0.08	Ce	1	Cu	2	Si	1.92	Ge	0.08																	2002								0.74																																						K		0.27					0.27																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111020	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.88Ge0.12	Ce	1	Cu	2	Si	1.88	Ge	0.12																	2002								0.89																																						K		0.2					0.2																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111021	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.8Ge0.2	Ce	1	Cu	2	Si	1.8	Ge	0.2																	2002								1																																						K		0.19					0.19																																																																																																					Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111022	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.6Ge0.4	Ce	1	Cu	2	Si	1.6	Ge	0.4																	2002								1.48																																						K																																																																																																												Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111023	PCS0631141		CeCu2(Si,Ge)2	Ce1Cu2Si1.4Ge0.6	Ce	1	Cu	2	Si	1.4	Ge	0.6																	2002								1.99																																						K																																																																																																												Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems			Department of Physical Science, Graduate of Engineering Science, Osaka University, Toyonaka, Osaka, Japan]	J.Phys.Chem.Solids, 63(2002)1141	C.Geibel,D.Aoki,F.Steglich,G.-q.Zheng,K.Ishida,R.Settai,S.Kawasaki,T.Mito,Y.Haga,Y.Kawasaki,Y.Kitaoka,Y.Onuki		
111024	P066014504	single crystal 0.5*0.17*0.035 mm3. Hc2 for H//c. ab-plane thermal conductivity at various magnetic fields (H//c) was measured.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38.1					38.1																				kOe		30																																											MTHC11024																															high-pressure cubic anvil technique					Thermal conductivity of single-crystalline MgB2			Laboratorium fur Festkorperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B, 66(2002)14504	A. V. Sologubenko,H.R.Ott,J.Jun,J.Karpinski,S.M.Kazakov		
111025	P066014505	density=2.48 g/cm3. R(RT)=50 uOhm.cm. RRR=2.5. carrier=1.5 E+23 /cm3. penet by microwave analysis. Hirr exponent=1.4.	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		38.3					38.3																													T/K		0.51			MHC11025							nm		450					2.1																																																high-pressure(3 GPa) - SIN(950C) - Q					Magnetization and microwave study of superconducting MgB2			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 66(2002)14505	A.Dulcic,C.U.Jung,D.Paar,G,V,M.Williams,M.Pozek,Min-Seok Park,S.Kramer,Sung IK Lee		
111026	JAP0837321	G-L parameter = 60	Y2C2I2	Y2C2I2	Y	2	C	2	I	2																			1998																																														K		10					10											mT		6							T		11.8																																					210																																										Specific heat, magnetization and C-isotope effect of Y2C2(Br,I)2 superconductors			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	J.Appl.Phys., 83(1998)7321	A.Simon,R.K.Kremer,R.W.Henn,Th.Gulden,W.Schnelle		
111027	JAP0837321	G-L parameter = 50	Y2C2Br2	Y2C2Br2	Y	2	C	2	Br	2																			1998																																														K		5					5											mT		1.5							T		3																																					240																																										Specific heat, magnetization and C-isotope effect of Y2C2(Br,I)2 superconductors			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	J.Appl.Phys., 83(1998)7321	A.Simon,R.K.Kremer,R.W.Henn,Th.Gulden,W.Schnelle		
111028	JAP0837321		Y2C2(Br,I)2	Y2C2Br0.5I1.5	Y	2	C	2	Br	0.5	I	1.5																	1998																																														K		11.6					11.6																																																																																																					Specific heat, magnetization and C-isotope effect of Y2C2(Br,I)2 superconductors			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse, Stuttgart, Germany	J.Appl.Phys., 83(1998)7321	A.Simon,R.K.Kremer,R.W.Henn,Th.Gulden,W.Schnelle		
111029	P066012510	in-plane and out-of-plane penet = 0.26 and 1.3 um. x = 1.99 in Y2CxI2 by XRD Rietveld.	Y2C2I2	Y2Cu2I2	Y	2	Cu	2	I	2																		1	2002																																														K		10.1					10.1																																									um		0.26																																																					sintering in Ta crucible					Far-infrared optical properties of the carbide superconductor Y2C2I2			Physikalisches Institut, Universitat Stuttgart,Stuttgart, Germany	Phys.Rev.B, 66(2002)012510	A.Simon,B.Gorshunov,K.Ahn,M.Dressel,R.K.Kremer,T.Room		
111030	P065214518	nominal = MgC1.5Ni3. porocity < 5%. graphite included. grain size = 100-300 nm. Jc(4.2K,1T)=1.8 E+6 A/cm2.	MgCNi3	Mg1Cu1Ni3	Mg	1	Cu	1	Ni	3																			2002																												CaTiO3																		K		7.2					7.2																				T		12.8							T/K		2.3					nm		5																																																										See Nature 411(2001)54					Core pinning by intragranular nanoprecipitates in polycrystalline MgCNi3			Applied Superconductivity Center, University of Wisconsin, Madison, Wisconsin , USA	Phys.Rev.B, 65(2002)214518	D.C.Larbalestier,J.Jiang,K.A.Regan,L.D.Cooley,R.J.Cava,T.He,X.Song		
111031	PLA2990282	P-induced s/c. Hc2 defined as 0.95Rn. s/c properties measured at p = 22.2 GPa.	Fe	Fe1	Fe	1																							2002																																													hcp	K		2			0		2																				T		0.3																																																																										purification					Superconductivity of epsiron-Fe: complete resistive transition			DPMC, University of Geneva, 24 Quai Ernest-Ansermet,  Geneve, Switzerland	Phys.Lett.A, 299(2002)282	A.T.Holmes,D.Jaccard,G.Behr,Y.Inada,Y.Onuki		
111032	P065180504	Hc2(0) = 11.7 T for H//a and 5.0 T for H//c. 1st order phase transition for lower temperature.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5			A	4.612		7.549												K		2.3					2.3																				T			11.7	5										MHC11032																																																														In-self flux method					Unconventional heavy-fermion superconductor CeCoIn5 : dc magnetization study at temperatures down to 50 mK			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba , Japan	Phys.Rev.B, 65(2002)180504	A.Harita,H.Shishido,R.Settai,T.Sakakibara,T.Tayama,Y.Haga,Y.Onuki		
111033	JPF0152333	R(Tc) = 88.9 uOhm.cm. e-ph coupling const = 0.854	V2Hf	Hf1V2	Hf	1	V	2																				1	1985																												MgCu2(Laves)			A	7.396													MgCu2, C15	K		9.27					9.27																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111034	JPF0152333	R(Tc) = 81.4 uOhm.cm. e-ph coupling const = 0.852	V2(Hf,Y)	V2Hf0.95Y0.05	V	2	Hf	0.95	Y	0.05																		1	1985																												MgCu2(Laves)			A	7.383													MgCu2, C15	K		9.22					9.22																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111035	JPF0152333	R(Tc) = 70.4 uOhm.cm. e-ph coupling const = 0.851	V2(Hf,Y)	V2Hf0.9Y0.1	V	2	Hf	0.9	Y	0.1																		1	1985																												MgCu2(Laves)			A	7.395													MgCu2, C15	K		9.19					9.19																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111036	JPF0152333	R(Tc) = 85.5 uOhm.cm. e-ph coupling const = 0.851	V2(Hf,Ti)	V2Hf0.9Ti0.1	V	2	Hf	0.9	Ti	0.1																		1	1985																												MgCu2(Laves)			A	7.409													MgCu2, C15	K		9.19					9.19																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111037	JPF0152333	R(Tc) = 77.7 uOhm.cm. e-ph coupling const = 0.835	V2(Hf,Ti)	V2Hf0.8Ti0.2	V	2	Hf	0.8	Ti	0.2																		1	1985																												MgCu2(Laves)			A	7.429													MgCu2, C15	K		8.8					8.8																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111039	JPF0152333	R(Tc) = 72.6 uOhm.cm. e-ph coupling const = 0.883	V2(Hf,Nb)	V2Hf0.9Nb0.1	V	2	Hf	0.9	Nb	0.1																			1985																												MgCu2(Laves)			A	7.388													MgCu2, C15	K		9.93					9.93																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111040	JPF0152333	R(Tc) = 63.3 uOhm.cm. e-ph coupling const = 0.915	V2(Hf,Nb)	V2Hf0.84Nb0.16	V	2	Hf	0.84	Nb	0.16																			1985																												MgCu2(Laves)			A	7.39													MgCu2, C15	K		10.67					10.67																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111041	JPF0152333	R(Tc) = 71.0 uOhm.cm. e-ph coupling const = 0.878	V2(Hf,Ta)	V2Hf0.9Ta0.1	V	2	Hf	0.9	Ta	0.1																			1985																												MgCu2(Laves)			A	7.384													MgCu2, C15	K		9.82					9.82																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111042	JPF0152333	R(Tc) = 64.9 uOhm.cm. e-ph coupling const = 0.905	V2(Hf,Ta)	V2Hf0.87Ta0.13	V	2	Hf	0.87	Ta	0.13																			1985																												MgCu2(Laves)			A	7.395													MgCu2, C15	K		10.45					10.45																																																																																																arc-melting					Superconductivity and structural transformation in V2Hf-based C15 pseudobinary compounds			Toyohashi University of Technology,Japan	J.Phys.F: Met.Phys., 15(1985)2333	A.Oota,H.Takei,M.Yamawaki,S.Noguchi		
111043	AAC6220123	structure beta = 93.55	Y2I2C2	Y2I2C2	Y	2	I	2	C	2																			1996																															A	7.217	3.879	10.435												K		9.85					9.85																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111044	AAC6220123	structure beta = 93.75	Y2(I,Br)2C2	Y2I1.75Br0.25C2	Y	2	I	1.75	Br	0.25	C	2																	1996																															A	7.184	3.864	10.411												K		10.35					10.35																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111045	AAC6220123	structure beta = 93.50	Y2(I,Br)2C2	Y2I1.6Br0.4C2	Y	2	I	1.6	Br	0.4	C	2																	1996																															A	7.123	3.844	10.391												K		11.2					11.2																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111046	AAC6220123	structure beta = 93.92	Y2(I,Br)2C2	Y2I1.5Br0.5C2	Y	2	I	1.5	Br	0.5	C	2																	1996																															A	7.154	3.851	10.388												K		11.1					11.1																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111047	AAC6220123	structure beta = 93.72	Y2(I,Br)2C2	Y2I1.4Br0.6C2	Y	2	I	1.4	Br	0.6	C	2																	1996																															A	7.14	3.842	10.37												K		10.5					10.5																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111048	AAC6220123	structure beta = 93.0	Y2(I,Br)2C2	Y2I1.3Br0.7C2	Y	2	I	1.3	Br	0.7	C	2																	1996																															A	7.124	3.84	10.319												K		10.5					10.5																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111049	AAC6220123	structure beta = 94.02	Y2(I,Br)2C2	Y2I1.25Br0.75C2	Y	2	I	1.25	Br	0.75	C	2																	1996																															A	7.122	3.834	10.342												K		10.05					10.05																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111050	AAC6220123	structure beta = 93.36	Y2(I,Br)2C2	Y2I1.2Br0.8C2	Y	2	I	1.2	Br	0.8	C	2																	1996																															A	7.1	3.828	10.32												K		9.6					9.6																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111051	AAC6220123	structure beta = 94.08	Y2(I,Br)2C2	Y2I1Br1C2	Y	2	I	1	Br	1	C	2																	1996																															A	7.079	3.818	10.274												K		7.9					7.9																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111052	AAC6220123	structure beta = 100.06	Y2(I,Br)2C2	Y2I0.75Br1.25C2	Y	2	I	0.75	Br	1.25	C	2																	1996																															A	7.054	3.808	10.321												K		7					7																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111053	AAC6220123	structure beta = 99.97	Y2(I,Br)2C2	Y2I0.6Br1.4C2	Y	2	I	0.6	Br	1.4	C	2																	1996																															A	7.03	3.796	10.248												K		6.4					6.4																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111054	AAC6220123	structure beta = 99.97	Y2(I,Br)2C2	Y2I0.5Br1.5C2	Y	2	I	0.5	Br	1.5	C	2																	1996																															A	7.023	3.79	10.21												K		6					6																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111055	AAC6220123	structure beta = 100.22	Y2(I,Br)2C2	Y2I0.4Br1.6C2	Y	2	I	0.4	Br	1.6	C	2																	1996																															A	6.997	3.785	10.183												K		5.8					5.8																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111056	AAC6220123	structure beta = 99.91	Y2(I,Br)2C2	Y2I0.25Br1.75C2	Y	2	I	0.25	Br	1.75	C	2																	1996																															A	6.986	3.781	10.082												K		5.5					5.5																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111057	AAC6220123	structure beta = 100.09	Y2(I,Br)2C2	Y2I0.2Br1.8C2	Y	2	I	0.2	Br	1.8	C	2																	1996																															A	6.973	3.775	10.051												K																																																																																																												Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111058	AAC6220123	structure beta = 99.97	Y2Br2C2	Y2Br2C2	Y	2	Br	2	C	2																			1996																															A	6.958	3.767	9.932												K		5.05					5.05																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111059	AAC6220123	structure beta = 93.79	Y2(I,Cl)2C2	Y2I1.75Cl0.25C2	Y	2	I	1.75	Cl	0.25	C	2																	1996																															A	7.172	3.857	10.452												K		10.7					10.7																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111060	AAC6220123	structure beta = 93.84	Y2(I,Cl)2C2	Y2I1.5Cl0.5C2	Y	2	I	1.5	Cl	0.5	C	2																	1996																															A	7.127	3.839	10.441												K		8.25					8.25																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111061	AAC6220123	structure beta = 99.94	Y2(Br,Cl)2C2	Y2Br1.75Cl0.25C2	Y	2	Br	1.75	Cl	0.25	C	2																	1996																															A	6.941	3.761	9.898												K		4.7					4.7																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111062	AAC6220123	structure beta = 99.95	Y2(Br,Cl)2C2	Y2Br1.5Cl0.5C2	Y	2	Br	1.5	Cl	0.5	C	2																	1996																															A	6.928	3.754	9.862												K		4.4					4.4																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111063	AAC6220123	structure beta = 99.92	Y2(Br,Cl)2C2	Y2Br1.25Cl0.75C2	Y	2	Br	1.25	Cl	0.75	C	2																	1996																															A	6.906	3.744	9.812												K		4.15					4.15																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111064	AAC6220123	structure beta = 99.99	Y2(Br,Cl)2C2	Y2Br1Cl1C2	Y	2	Br	1	Cl	1	C	2																	1996																															A	6.883	3.738	9.766												K		3.85					3.85																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111065	AAC6220123	structure beta = 94.83	Y2(Br,Cl)2C2	Y2Br0.9Cl1.1C2	Y	2	Br	0.9	Cl	1.1	C	2																	1996																															A	6.887	3.737	9.631												K																																																																																																												Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111066	AAC6220123	structure beta = 94.69	Y2(Br,Cl)2C2	Y2Br0.8Cl1.2C2	Y	2	Br	0.8	Cl	1.2	C	2																	1996																															A	6.869	3.731	9.605												K																																																																																																												Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111067	AAC6220123	structure beta = 99.97	Y2(Br,Cl)2C2	Y2Br0.75Cl1.25C2	Y	2	Br	0.75	Cl	1.25	C	2																	1996																															A	6.872	3.733	9.728												K		3.7					3.7																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111068	AAC6220123	structure beta = 94.82	Y2(Br,Cl)2C2	Y2Br0.7Cl1.3C2	Y	2	Br	0.7	Cl	1.3	C	2																	1996																															A	6.866	3.731	9.568												K																																																																																																												Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111069	AAC6220123	structure beta = 94.79	Y2(Br,Cl)2C2	Y2Br0.5Cl1.5C2	Y	2	Br	0.5	Cl	1.5	C	2																	1996																															A	6.862	3.725	9.52												K		3.25					3.25																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111070	AAC6220123	structure beta = 94.81	Y2(Br,Cl)2C2	Y2Br0.25Cl1.75C2	Y	2	Br	0.25	Cl	1.75	C	2																	1996																															A	6.839	3.718	9.44												K		2.85					2.85																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111071	AAC6220123	structure beta = 95.01	Y2Cl2C2	Y2Cl2C2	Y	2	Cl	2	C	2																			1996																															A	6.83	3.712	9.332												K		2.3					2.3																																																																																																					Superconductivity in rare earth metal carbide halides of the type SE2X2C2			Max-Planck Institut, Stuttgart, Germany	Z.anorg.allg.Chem., 622(1996)123	A.Simon,A.Yoshiasa,C.Felser,Hj.Mattausch,M.Backer,R.K.Kremer,R.W.Henn		
111072	JPS0711023	penet<ab> measured by muon-SR at H=402 G	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2002																												HoCoGa5																		K		0.4					0.4																																									A		6700																																																					In-serlf flux method					Muon-SR Studies on Heavy Fermion Superconductors CeIrIn5 and CeCoIn5			Institute of Materials Structure Science,High Energy Accelerator Research Organization,Tsukuba,Ibaraki,Japan	J.Phys.Soc.Jpn, 71(2002)1023	A.Koda,D.Aoki,H.Shishido,R.Kadono,R.Settai,W.Higemoto,Y.Haga,Y.Kawasaki,Y.Onuki		
111073	JPS0711023	penet<ab> measured by muon-SR at H=3 kG	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5																		K		2					2																																									A		5500																																																					In-serlf flux method					Muon-SR Studies on Heavy Fermion Superconductors CeIrIn5 and CeCoIn5			Institute of Materials Structure Science,High Energy Accelerator Research Organization,Tsukuba,Ibaraki,Japan	J.Phys.Soc.Jpn, 71(2002)1023	A.Koda,D.Aoki,H.Shishido,R.Kadono,R.Settai,W.Higemoto,Y.Haga,Y.Kawasaki,Y.Onuki		
111074	JPC0130627	Hc2(0) = 116, 49.5 kOe for [110], [001] direction. cohere <a>=82 A, cohere<c> = 35 A. dHvA measured. gamma in mj/mol.K2	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2001																												HoCoGa5			A	4.612		7.549												K		2.3					2.3																				kOe			116													A		82																		mj/mol.K2	1000																																							In-serlf flux method					Quasi-two-dimensional Fermi surfaces and the de Haas-van Alphen oscillation in both the normal and superconducting mixed states of CeCoIn5			Graduate School of Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys: Condens.Mater, 13(2001)L627	D.Aoki,H.Harima,H.Shishido,M.Nakashima,R.Settai,S.Ikeda,Y.Haga,Y.Murakawa,Y.Onuki		
111075	JPS0710162	pressure-induced s/c..1.6 GPa<SC<7.5 GPa. RRR=330	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2002								3.8																				HoCoGa5																		K		2.2			0		2.2	MTC11075																																																																																															In-serlf flux method					Fermi Surface,Magnetic and Superconducting Properties of LaRhIn5 and CeTIn5 (T:Co,Rh and Ir)			Graduate School of Science,Osaka University,Toyonaka,Osaka,Japan	J.Phys.Soc.Jpn, 71(2002)162	D.Aoki,H.Harima,H.Nakawaki,H.Sato,H.Shishido,K.Kindo,K.Sugiyama,N.Nakamura,R.Settai,S.Ikeda,T.C.Kobayashi,T.IIzuka,T.Namiki,T.Takeuchi,Y.Aoki,Y.Haga,Y.Inada,Y.Onuki		
111076	JPS0710162	Tc(max) = 2.6 K(P=1.3 GPa)	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5																		K		2.2					2.2	MTC11076																																																																																															In-serlf flux method					Fermi Surface,Magnetic and Superconducting Properties of LaRhIn5 and CeTIn5 (T:Co,Rh and Ir)			Graduate School of Science,Osaka University,Toyonaka,Osaka,Japan	J.Phys.Soc.Jpn, 71(2002)162	D.Aoki,H.Harima,H.Nakawaki,H.Sato,H.Shishido,K.Kindo,K.Sugiyama,N.Nakamura,R.Settai,S.Ikeda,T.C.Kobayashi,T.IIzuka,T.Namiki,T.Takeuchi,Y.Aoki,Y.Haga,Y.Inada,Y.Onuki		
111077	JPS0710162	bulk s/c Tc=0.38 K. Figure shows Hc2(T) by resistivity and susceptibility measurement.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2002																												HoCoGa5																		K		1.3					1.3																																		MHC11077																																																														In-serlf flux method					Fermi Surface,Magnetic and Superconducting Properties of LaRhIn5 and CeTIn5 (T:Co,Rh and Ir)			Graduate School of Science,Osaka University,Toyonaka,Osaka,Japan	J.Phys.Soc.Jpn, 71(2002)162	D.Aoki,H.Harima,H.Nakawaki,H.Sato,H.Shishido,K.Kindo,K.Sugiyama,N.Nakamura,R.Settai,S.Ikeda,T.C.Kobayashi,T.IIzuka,T.Namiki,T.Takeuchi,Y.Aoki,Y.Haga,Y.Inada,Y.Onuki		
111078	MAT0107266	c/a = 1.610	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																			2001																												HoCoGa5																		K		0.4					0.4																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111079	MAT0107266	c/a = 1.6131	Ce(Rh,Ir)In5	Ce1Rh0.25Ir0.75In5	Ce	1	Rh	0.25	Ir	0.75	In	5																	2001																												HoCoGa5																		K		0.64					0.64																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111080	MAT0107266	c/a = 1.6146	Ce(Co,Ir)In5	Ce1Co0.5Ir0.5In5	Ce	1	Co	0.5	Ir	0.5	In	5																	2001																												HoCoGa5																		K		0.64					0.64																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111081	MAT0107266	c/a = 1.617	Ce(Rh,Ir)In5	Ce1Rh0.5Ir0.5In5	Ce	1	Rh	0.5	Ir	0.5	In	5																	2001																												HoCoGa5																		K		0.97					0.97																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111082	MAT0107266	c/a = 1.6256	Ce(Rh,Co)In5	Ce1Co0.5Rh0.5In5	Ce	1	Co	0.5	Rh	0.5	In	5																	2001																												HoCoGa5																		K		1.6					1.6																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111083	MAT0107266	c/a = 1.636	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																			2001																												HoCoGa5																		K		2.3					2.3																																																																																																					Multiple phase transition in Ce(Rh,Ir,Co)In5 heavy-fermion superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	Cond-mat/0107266(2001)	A.D.Bianchi,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Nicklas,N.O.Moreno,P.G.Pagliuso,R.Movshovich,Z.Fisk		
111084	CEM1630385	space group=P6/mmm. XRD measured at 120 K.	BeB3	B3Be1.09	B	3	Be	1.09																				3	2002																															A	9.7738		9.5467												K		0.72					0.72																																																																																																arc-melting					Synthesis, structure, and superconductivity in Be1.09B3			Department of Chemistry,Louisiana State University,Baton Rouge,Louisiana,USA	J.Solid State Chem., 163(2002)385	D.P.Young,Frank R.Fronczek,J.F.DiTusa,Julia Y.Chan,P.W.Adams		
111085	JPC0130759	pressure-induced s/c. Tc observed for 8.8<p<14 kbar. Curie temp. defined as dR/dT vs T. crossover temp. = 32 K.	UGe2	Ge2U1	Ge	2	U	1																				1	2001							54.5																					ZrGa2																		K		0.8			0		0.8																																																																																																arc-melting + ANN(1100C,1week)					Coexistence of superconductivity and ferromagnetism in polycrystalline UGe2			Department of Physics and Institute For Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA , USA	J.Phys.:Condens.Mater, 13(2001)L759	E.D.Bauer,M.B.Maple,R.P.Dickey,V.S.Zapf		
111086	JPC0140377	pressure-induced s/c. R=0 region is for 1.03 < p < 1.08 GPa. Values of s/c properties are for p = 1.06 GPa. RRR=100. RR=0.75 microOhm.cm.	CeRh2Si2	Ce1Rh2Si2	Ce	1	Rh	2	Si	2																		3	2002								36																																						K		0.43			0		0.43																																		MHC11086		A		340																																																										Czochralski method					Pressure-induced superconductivity in an antiferromagnet CeRh2Si2			Graduate School of Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Mater, 14(2002)L377	M.Nakashima,R.Settai,S.Araki,T.C.Kobayashi,Y.Onuki		
111087	JPC014L529	pressure-induced s/c. Tc shows Tc(max) for p=3.9 GPa//c-axis. p//c-axis pressure enhanced Tc(max) and s/c region.	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																		3	2002																																														K		0.52			0		0.52	MTC11087																																																																																																				Strain enhancement of superconductivity in CePd2Si2 under pressure			DPMC, University of Geneva, Quai E-Ansermet 24, 1211 Geneva 4, Switzerland	J.Phys.:Condens.Mater, 14(2002)L529	A.Demuer,A.T.Holmes,D.Jaccard		
111088	JP01403663	dTc/dp in K/GPa. impurity MgO<5%. RRR=4.2. pressure using diamond anvil(non-hydrostatic)	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2			A	3.086		3.5204											AlB2, C32	K		39.8					39.8	MTC11088		K/GPa	-1.1																																																																																												heat(950C,Ar-gas,Ta tube)					Anomalous non-linear pressure dependence of TC for MgB2			Instituto de Investigaciones en Materiales, Universidad Nacional,Apartado Postal, Mexico, Mexico	J.Phys.:Condens.Mater, 14(2002)3663	A.Duran,R.Escudero,R.Falconi		
111089	JP014L0261	dTc/dp(K/GPa) calculated from thermal expansion. Figure shows volume thermal expansion coefficient for [001], [100] direction.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5			A	4.612		7.549												K		2.25					2.25	MTE11089		K/GPa	0.34																																																																																												self-flux method					Thermal expansion and magnetostriction studies in a heavy-fermion superconductor, CeCoIn5			Low Temperature Centre, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Mater, 14(2002)L261	H.Shishido,R.Settai,S.Ikeda,T.Takeuchi,Y.Haga,Y.Onuki		
111090	PHC3770190	density = 97 % of x-ray density. Thermal expansion measured for H=0, 36, 42 kOe by dilatometer.	MgB2	B2Mg1	B	2	Mg	1																				1	2002																												AlB2																	AlB2, C32	K		39					39	MTE11090																																																																																															sintered(50 kbar,950-1000C)					Thermal expansion anomaly of MgB2 at low temperatures and magnetic field influence			P.N. Lebedev Physical Institute RAS, 119991 Moscow, Russia	Physica C, 377(2002)190	A.I.Golovashkin,A.P.Rusakov,B.M.Bulichev,I.B.Krinetskii,L.I.Ivanova,N.V.Anshukova		
111091	SSC0600517	Tc(zero)=0.17 K. carrier n=3.3 E+25 /cm3. R(300K)=4.1 mOhm.cm.	Sr(Ti,Zr)O3	Sr1Ti0.97Zr0.03O3	Sr	1	Ti	0.97	Zr	0.03	O	3																	1986																												CaTiO3																		K		0.3					0.3																																																																																																sinter (1100-1250C)					Superconducting transitions from states with low normal conductivity in ceramic SrTi0.97Zr0.03O3			CSIRO Division of Applied Physics, Sydney,Australia	Solid State Commun., 60(1986)517	C.Andrikidis,R.J.Tainsh		
111092	PR03404920	Amorphous film. substrate = glazed alumina. Ts= less than 18 K.	Ga	Ga1	Ga	1																						3	1986																																													amorphous	K		8.2					8.2																																																																																																evaporation					Threshold for superconductivity in ultrathin amorphous gallium films			University of Minnesota,Minneapolis,Mennesota,USA	Phys.Rev.B, 34(1986)4920	A.M.Goldman,B.G.Orr,D.B.Haviland,H.M.Jaeger		
111093	PR03404590	Phase transition at 79 K. 2nd phase(Tc=9.1 K) for p>Pc=21 kbar. bulk modulus B=1370 kbar. delta-C/gamma*Tc = 1.41	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1986																												Sc5Co4Si10			A	12.486		4.178												K		3.77					3.77																				T		1.04							T/K		0.39			MHC111093																						mj/mol.K2	23.42		366																																					arc-melting					Electronic phase transition and partially gapped Fermi surface in superconducting Lu5Ir4Si10			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)4590	C.A.Swenson,H.D.Yang,L.S.Hausermann-Berg,M.S.Anderson,P.Klavins,R.N.Shelton		
111094	PR03304680	RRR=1.70	ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																		3	1986								0.65																																					bct	K		7.8					7.8																																		MHC11094																																																														induction heating					Superconductivity and magnetism of a body-centered tetragonal ErRh4B4 single crystal. II. Large anisotropy of Hc2			Tohoku University, Sendai,Japan	Phys.Rev.B, 33(1986)4680	H.Iwasaki,Y.Muto		
111095	PR03304680	RRR=1.65. small amount of impurity (RhB)	LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																		1	1986																																													bct	K		8.61					8.61																													T/K		2.08			MHC11095																																																														induction heating + ANN(1050C)					Superconductivity and magnetism of a body-centered tetragonal ErRh4B4 single crystal. II. Large anisotropy of Hc2			Tohoku University, Sendai,Japan	Phys.Rev.B, 33(1986)4680	H.Iwasaki,Y.Muto		
111096	PR03400199	av. grain size = 180 micron. RRR = 4.9	ErPd2Sn	Er1Pd2Sn1	Er	1	Pd	2	Sn	1																		1	1986							-5.8	1																				Heusler			A	6.6834													Cu2MnAl, L2<1>	K		1.17					1.17																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111097	PR03400199		(Er,Y)Pd2Sn	Er0.95Y0.05Pd2Sn1	Er	0.95	Y	0.05	Pd	2	Sn	1																1	1986																												Heusler			A	6.6864													Cu2MnAl, L2<1>	K		1.26					1.26																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111098	PR03400199		(Er,Y)Pd2Sn	Er0.9Y0.1Pd2Sn1	Er	0.9	Y	0.1	Pd	2	Sn	1																1	1986																												Heusler			A	6.6873													Cu2MnAl, L2<1>	K		1.6					1.6																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111099	PR03400199		(Er,Y)Pd2Sn	Er0.8Y0.2Pd2Sn1	Er	0.8	Y	0.2	Pd	2	Sn	1																1	1986																												Heusler			A	6.689													Cu2MnAl, L2<1>	K		2.08					2.08																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111100	PR03400199		(Er,Y)Pd2Sn	Er0.6Y0.4Pd2Sn1	Er	0.6	Y	0.4	Pd	2	Sn	1																1	1986																												Heusler			A	6.6973													Cu2MnAl, L2<1>	K		2.59					2.59																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111101	PR03400199		(Er,Y)Pd2Sn	Er0.4Y0.6Pd2Sn1	Er	0.4	Y	0.6	Pd	2	Sn	1																1	1986																												Heusler			A	6.7024													Cu2MnAl, L2<1>	K		3.66					3.66																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111102	PR03400199		(Er,Y)Pd2Sn	Er0.2Y0.8Pd2Sn1	Er	0.2	Y	0.8	Pd	2	Sn	1																1	1986																												Heusler			A	6.7096													Cu2MnAl, L2<1>	K		4.38					4.38																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111103	PR03400199		YPd2Sn	Y1Pd2Sn1	Y	1	Pd	2	Sn	1																		1	1986																												Heusler			A	6.7165													Cu2MnAl, L2<1>	K		5.26					5.26																																																																																																					Coexistence of superconductivity and long-range magnetic order in ErPd2Sn			Ames Lab, Iowa State University,Ames,Iowa,USA	Phys.Rev.B, 34(1986)199	H.D.Yang,L.S.Hausermann-Berg,M.J.Johnson,P.Klavins,R.N.Shelton		
111104	SSC0590839		ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																			1986																												TiNiSi																		K		2.04					2.04																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111105	SSC0590839		HfIrSi	Hf1Ir1Si1	Hf	1	Ir	1	Si	1																			1986																												TiNiSi																		K		3.5					3.5																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111106	SSC0590839		TiOsSi	Ti1Os1Si1	Ti	1	Os	1	Si	1																			1986																												TiFeSi			A	7.062	11.217	6.479												K					1.6																																																																																																		arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111107	SSC0590839		ZrOsSi	Zr1Os1Si1	Zr	1	Os	1	Si	1																			1986																												TiNiSi			A	6.411	4.041	7.453												K		1.72					1.72																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111108	SSC0590839		HfOsSi	Hf1Os1Si1	Hf	1	Os	1	Si	1																			1986																												Fe2P			A	6.614		3.678												K					1.6																																																																																																		arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111109	SSC0590839		HfRuSi	Hf1Ru1Si1	Hf	1	Ru	1	Si	1																			1986																												Fe2P			A	6.643		3.646												K					1.6																																																																																																		arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111110	SSC0590839		ZrRhSi	Zr1Rh1Si1	Zr	1	Rh	1	Si	1																			1986																												TiNiSi			A	6.52	3.926	7.41												K					1.6																																																																																																		arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111111	SSC0590839		HfRhSi	Hf1Rh1Si1	Hf	1	Rh	1	Si	1																			1986																												TiNiSi			A	6.47	3.91	7.397												K					1.6																																																																																																		arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111112	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.82Re0.18	Mo	0.82	Re	0.18																				3	1986																																													bcc	K		8.5					8.5																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111113	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.75Re0.25	Mo	0.75	Re	0.25																				3	1986																																													bcc	K		10					10																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111114	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.7Re0.3	Mo	0.7	Re	0.3																				3	1986																																													bcc	K		10.5					10.5																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111115	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.65Re0.35	Mo	0.65	Re	0.35																				3	1986																												Cr3Si(A15)																	Cr3Si, A15	K		10.2					10.2																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111116	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.57Re0.43	Mo	0.57	Re	0.43																				3	1986																																													bcc	K		10					10																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111117	LOW0640395	Thin film. substrate=sapphire(1,1,-2,0)	(Mo,Re)	Mo0.62Re0.38	Mo	0.62	Re	0.38																				3	1986																												Cr3Si(A15)																	Cr3Si, A15	K		11.5					11.5																																																																																																coevaporation by EB					Properties of evaporated Mo-Re thin-film superconductors			Westinghouse R & D Center, Pittsburgh, Pa, USA	J.Low Temp.Phys., 64(1986)395	J.Greggi,J.Talvacchio,M.A.Janocko		
111118	L089037002	T<SDW> = 4.5 K. spin-triplet s/c. Hc2(T=0.1K)=8 kOe for H//a-axis	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																		3	2002								4.5																				PrNi2Al3																		K		0.9					0.9																																																																																																					Spin-Triplet Superconductivity in UNi2Al3 Revealed by the <27>Al Knight Shift Measurement			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	Phys.Rev.Lett., 89(2002)037002	C.Geibel,D.Ozaki,F.Steglich,H.Tou,K.Ishida,M.Kyogaku,N.Aso,N.K.Sato,N.Tateiwa,T.Kamatsuka,Y.Kitaoka		
111119	PHC3770096	volume fraction = 97 %	Ca(Ga,Si)2	Ca1Ga1Si1	Ca	1	Ga	1	Si	1																			2002																												AlB2			A	4.12		4.4401											AlB2, C32	K		4.3					4.3																																																																																																arc-melting					Superconductivity of ternary silicides A(Gax,Si1-x)2, A = Ca,Sr,and Ba)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, Japan	Physica C, 377(2002)96	H.Abe,K.Nishida,M.Imai,T.Kimura		
111120	PHC3770096	volume fraction = 75 %	Ca(Ga,Si)2	Ca1Ga0.74Si1.26	Ca	1	Ga	0.74	Si	1.26																			2002																												AlB2			A	4.1037		4.4135											AlB2, C32	K		3.5					3.5																																																																																																arc-melting					Superconductivity of ternary silicides A(Gax,Si1-x)2, A = Ca,Sr,and Ba)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, Japan	Physica C, 377(2002)96	H.Abe,K.Nishida,M.Imai,T.Kimura		
111121	PHC3770096	volume fraction = 92 %	Sr(Ga,Si)2	Sr1Ga0.74Si1.26	Sr	1	Ga	0.74	Si	1.26																			2002																												AlB2			A	4.1446		4.7917											AlB2, C32	K		4.2					4.2																																																																																																arc-melting					Superconductivity of ternary silicides A(Gax,Si1-x)2, A = Ca,Sr,and Ba)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, Japan	Physica C, 377(2002)96	H.Abe,K.Nishida,M.Imai,T.Kimura		
111122	PHC3770096	volume fraction = 96 %	Ba(Ga,Si)2	Ba1Ga0.78Si1.22	Ba	1	Ga	0.78	Si	1.22																			2002																												AlB2			A	4.1949		5.129											AlB2, C32	K		4					4																																																																																																arc-melting					Superconductivity of ternary silicides A(Gax,Si1-x)2, A = Ca,Sr,and Ba)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, Japan	Physica C, 377(2002)96	H.Abe,K.Nishida,M.Imai,T.Kimura		
111123	PHC3770202	gap(delta)=8 meV. having two gaps. another gap = 2.7 meV. Temperature dependence is BCS-like. measured by point contact, Andreev reflection.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38					38																																																4.89	1																																																				Measurement of the superconducting gap of MgB2 by point contact spectroscopy			School of Physics and Condensed Matter Research Institute, Seoul National University, Seoul, South Korea	Physica C, 377(2002)202	B.Oh,Eun Jip Choi,H.G.Kim,NH.N.Lee,S.H.Moon,Suyoun Lee,Yonuk Chong,Z.G.Khim		
111124	P066092503	ortho-NdNiGa2 type(Cmmm). RR=14.1 uOhm.cm. RRR=5.2. Tc(R=0)=2.05 K. delta-C = 32 mj/mol.K. delta-C/gamma*Tc = 1.40.	LaNiGa2	La1Ni1Ga2	La	1	Ni	1	Ga	2																		1	2002																															A	4.268	17.7	4.226											orthorhombic	K		1.97					1.97																																																3.2								mj/mol.K2	11.64		560																																					arc-melting					Superconductivity in the Ni-based ternary compound LaNiGa2			Department of Physics, National Chung Cheng University, Ming-Hsiung,Taiwan	Phys.Rev.B, 66(2002)92503	N.L.Zeng,W.H.Lee		
111125	LOW0640329	Neel-T by susceptibility. sp-heat measured.	Ho(Rh,Ru)4B4	Ho1Rh3.72Ru0.28B4	Ho	1	Rh	3.72	Ru	0.28	B	4																	1986								1.25																																						K		6.42					6.42																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111126	LOW0640329	Neel-T by NED.	Ho(Rh,Ru)4B4	Ho1Rh3.6Ru0.4B4	Ho	1	Rh	3.6	Ru	0.4	B	4																	1986								1.56																																						K		6.42					6.42																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111127	LOW0640329	Neel-T by Hc2(T)	Ho(Rh,Ru)4B4	Ho1Rh3.4Ru0.6B4	Ho	1	Rh	3.4	Ru	0.6	B	4																	1986								1.04																																						K		6.14					6.14																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111128	LOW0640329	Neel-T by Hc2(T)	Ho(Rh,Ru)4B4	Ho1Rh3Ru1B4	Ho	1	Rh	3	Ru	1	B	4																	1986								0.94																																						K		6.35					6.35																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111129	LOW0640329	Neel-T by NED.	Ho(Rh,Ru)4B4	Ho1Rh2.6Ru1.4B4	Ho	1	Rh	2.6	Ru	1.4	B	4																	1986								1.46																																						K		4.68					4.68																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111130	LOW0640329		Ho(Rh,Ru)4B4	Ho1Rh2.4Ru1.6B4	Ho	1	Rh	2.4	Ru	1.6	B	4																	1986								1.25																																						K		1.6					1.6																																																																																																					Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111131	LOW0640329	not s/c. magnetic order measured by susceptibility.	Ho(Rh,Ru)4B4	Ho1Rh2Ru2B4	Ho	1	Rh	2	Ru	2	B	4																	1986								1.14																																						K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111132	LOW0640329	not s/c. magnetic order measured by susceptibility.	Ho(Rh,Ru)4B4	Ho1Rh1.6Ru2.4B4	Ho	1	Rh	1.6	Ru	2.4	B	4																	1986								0.94																																						K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111133	LOW0640329	not s/c. magnetic order measured by susceptibility.	Ho(Rh,Ru)4B4	Ho1Rh1.2Ru2.8B4	Ho	1	Rh	1.2	Ru	2.8	B	4																	1986								0.94																																						K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111134	LOW0640329	not s/c. magnetic order measured by susceptibility.	Ho(Rh,Ru)4B4	Ho1Rh0.8Ru3.2B4	Ho	1	Rh	0.8	Ru	3.2	B	4																	1986							0.97																																							K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111135	LOW0640329	not s/c. magnetic order measured by susceptibility.	Ho(Rh,Ru)4B4	Ho1Rh0.4Ru3.6B4	Ho	1	Rh	0.4	Ru	3.6	B	4																	1986							1.73																																							K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111136	LOW0640329	not s/c. magnetic order measured by susceptibility.	HoRu4B4	Ho1Ru4B4	Ho	1	Ru	4	B	4																			1986							2.46																																							K					1.5																																																																																																							Superconductivity, magnetic properties, and specific heat of the pseudoternary, body-centered tetragonal system Ho(Rh1-xRux)4B4			Universitat Erlangen-Nurnberg, Erlangen, FRG	J.Low Temp.Phys., 64(1986)329	A.Meinelt,A.Thoma,H.Adrian		
111137	P066104521	400 nm thickness. c-axis oriented. surface impedance measured. s/c parameters obtained by fitting using BCS theory. gap(0)=3.8 meV.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		39					39																																									nm		102					2.26																																																laser deposition on [1102] sapphire substrate					Energy gap, penetration depth, and surface resistance of MgB2 thin films determined by microwave resonator measurements			Forschungszentrum Julich, Institute of Thin Films and Interfaces, Julich,Germany	Phys.Rev.B, 66(2002)104521	B.B.Jin,Eum-Mi Choi,Hyeong-Jin Kim,K.Maki,N.Klein,Sung-Ik Lee,T.Dahm,W.N.Kang		
111138	P066104521	400 nm thickness. c-axis oriented. surface impedance measured. s/c parameters obtained by fitting using BCS theory. gap(0)=3.2 meV.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		36					36																																									nm		107					2.06																																																laser deposition on [1102] sapphire substrate					Energy gap, penetration depth, and surface resistance of MgB2 thin films determined by microwave resonator measurements			Forschungszentrum Julich, Institute of Thin Films and Interfaces, Julich,Germany	Phys.Rev.B, 66(2002)104521	B.B.Jin,Eum-Mi Choi,Hyeong-Jin Kim,K.Maki,N.Klein,Sung-Ik Lee,T.Dahm,W.N.Kang		
111139	SSC1230391	susceptibility starts to be minus at Tc. no resistivity data. s/c volume fraction <15 %.	YbFe4Al8	Yb1Fe4Al8	Yb	1	Fe	4	Al	8																			2002								107																							A	8.702		8.025											tetragonal	K		50					50																																																																																																arc-melting + ANN(500C, 8 weeks)					Magnetic properties of YbFe4Al8 intermetallic compound. New antiferromagnetic superconductor			Institute of Low Temperature and Structure Research, Wrochaw, Poland	Solid State Commun., 123(2002)391	B.Ya.Kotur,H.Drulis,P.Gaczynski,W.Iwasieczko,W.Suski		
111140	SSC1230283	RESRT=137 uOhm.cm. Debye-T from Bloch-Gruneizen equation.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2002																												Ir3Ge7			A	9.582		2.08												K		2.08					2.08																				T		1.7							T/K		1.4			MHC11140																									162																																					peritectical reaction.					Single crystal growth and superconductivity of Mo3Sb7			Institute of Low Temperature and Structure Research, Wrochaw, Poland	Solid State Commun., 123(2002)283	D.Badurski,J.Stepien-Damm,R.Troc,Z.Bukowski		
111141	JAP0922614		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.037		3.524											AlB2, C32	K		38.4					38.4																																		MHC11141																																																																			Enhanced flux pinning in Zr-doped MgB2 bulk superconductors prepared at ambient pressure			Northwest Institute for Nonferrous Metal Research, China	J.Appl.Phys., 92(2002)2614	A.K.Pradhan,C.H.Cheng,K.F.Yau,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.Zhao		
111142	JAP0922614		(Mg,Zr)B2	Mg0.95Zr0.05B2	Mg	0.95	Zr	0.05	B	2																			2002																												AlB2			A	3.076		3.524											AlB2, C32	K		37.7					37.7																																		MHC11142																																																																			Enhanced flux pinning in Zr-doped MgB2 bulk superconductors prepared at ambient pressure			Northwest Institute for Nonferrous Metal Research, China	J.Appl.Phys., 92(2002)2614	A.K.Pradhan,C.H.Cheng,K.F.Yau,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.Zhao		
111143	JAP0922614	Jc(T=5K,H=0.56T) = 2.1 E+6 A/cm2	(Mg,Zr)B2	Mg0.9Zr0.1B2	Mg	0.9	Zr	0.1	B	2																			2002																												AlB2			A	3.08		3.524											AlB2, C32	K		37.3					37.3																				T		20							T/K		0.56			MHC11143		nm		3.9																																																															Enhanced flux pinning in Zr-doped MgB2 bulk superconductors prepared at ambient pressure			Northwest Institute for Nonferrous Metal Research, China	J.Appl.Phys., 92(2002)2614	A.K.Pradhan,C.H.Cheng,K.F.Yau,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.Zhao		
111144	JAP0922614		(Mg,Zr)B2	Mg0.8Zr0.2B2	Mg	0.8	Zr	0.2	B	2																			2002																												AlB2			A	3.081		3.524											AlB2, C32	K		37.3					37.3																																		MHC11144																																																																			Enhanced flux pinning in Zr-doped MgB2 bulk superconductors prepared at ambient pressure			Northwest Institute for Nonferrous Metal Research, China	J.Appl.Phys., 92(2002)2614	A.K.Pradhan,C.H.Cheng,K.F.Yau,L.Zhou,M.Murakami,N.Koshizuka,Y.Feng,Y.Zhao		
111145	PR05308836	impurity phase = (NH3)8K3C60. samples undergo M-I transition at 40 K. not s/c. unit volume= 763 A3/C60	NH3K3C60	N1H3K3C60	N	1	H	3	K	3	C	60																	1996																												fullerene																		K					4.2																																																																																																		(K3C60 + NH3) in glass tube					Metal-insulator transition in ammoniated K3C60			Japan Advanced Institute of Science and Technology, Ishikawa, Japan	Phys.Rev.B., 53(1996)R8836	H.Shimoda,O.Zhou,T.Mitani,T.T.M.Palstra,Y.Iwasa,Y.Maniwa		
111146	PHB3040006	pressure induced s/c. Tc(on)=2.0 K under 52 GPa. space group = P2<1>/C, beta=113.07 degree.	C6I4O2	C6Ir4O2	C	6	Ir	4	O	2																		3	2001																															A	7.63	5.268	14.222												K		2			0		2																																																																																																grown from ethylacetate solution					Pressure-induced insulator-to-metal transition and superconductivity in iodanil, C6I4O2			Faculty of Engineering, Muroran Institute of Technology, Muroran, Hokkaido,Japan	Physica B, 304(2001)6	A.Nakayama,I.Shirotani,J.Hayashi,K.Amaya,K.Aoki,K.Shimizu,K.Takeda,K.Yakushi,T.Yokota		
111147	JP01011179	molecular crystal. pressure-induced s/c. Tc(max)=1.2 K at p=28 GPa.	I2	I2	I	2																							1998																																														K		1.2			0		1.2	MTC11147																																																																																																				Observation of pressure-induced superconductivity in the megabar region			Faculty of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 10(1998)11179	K.Amaya,K.Shimizu,M.I.Eremets,S.Endo,T.C.Kobayashi		
111148	JP01011179	molecular crystal. pressure-induced s/c. Tc(max)=1.4 K at p=80 GPa. dTc/dP = 0 K/GPa at P (=80 GPa).	Br2	Br2	Br	2																							1998																																														K		1.4			0		1.4			K/GPa	0																																																																																																	Observation of pressure-induced superconductivity in the megabar region			Faculty of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 10(1998)11179	K.Amaya,K.Shimizu,M.I.Eremets,S.Endo,T.C.Kobayashi		
111149	JP01011179	molecular crystal. pressure-induced s/c. Tc(on)<max>=15 K at p=100 GPa.	S	S1	S	1																							1998																																														K		12			0		12	MTC11149																																																																																																				Observation of pressure-induced superconductivity in the megabar region			Faculty of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 10(1998)11179	K.Amaya,K.Shimizu,M.I.Eremets,S.Endo,T.C.Kobayashi		
111150	JP01011179	molecular crystal. pressure-induced s/c. Tc<max>=0.65 K at p=120 GPa.	O2	O2	O	2																							1998																																														K		0.65			0		0.65			K/GPa	0																														MHC11150																																																																			Observation of pressure-induced superconductivity in the megabar region			Faculty of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 10(1998)11179	K.Amaya,K.Shimizu,M.I.Eremets,S.Endo,T.C.Kobayashi		
111151	PHC3570099	powder sample. R by microwave response. conductivity(200K) = 1206 Ohm.cm. unit volume = 725 A3/C60	K3C60	C60K3	C	60	K	3																					2001																												fullerene																		K		19.4					19.4																																																																																																					Electrical conduction of (NH3)xNaRb2C60			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Physica C, 357-360(2001)99	A.Maeda,H.Kitano,R.Inoue,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111152	PHC3570099	powder sample. R by microwave response. conductivity(200K) = 391 Ohm.cm. unit volume = 763 A3/C60	(NH3)0.8NaRb2C60	N0.8H2.4Na1Rb2C60	N	0.8	H	2.4	Na	1	Rb	2	C	60															2001																												fullerene																		K		15.2					15.2																																																																																																					Electrical conduction of (NH3)xNaRb2C60			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Physica C, 357-360(2001)99	A.Maeda,H.Kitano,R.Inoue,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111153	PHC3570099	powder sample. R by microwave response. conductivity(200K) = 126 Ohm.cm. unit volume = 766 A3/C60	(NH3)0.9NaRb2C60	N0.9H2.7Na1Rb2C60	N	0.9	H	2.7	Na	1	Rb	2	C	60															2001																												fullerene																		K		12.1					12.1																																																																																																					Electrical conduction of (NH3)xNaRb2C60			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Physica C, 357-360(2001)99	A.Maeda,H.Kitano,R.Inoue,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111154	L088096401	not s/c. powder sample. R by microwave response. conductivity(200K) = 0.0091 Ohm.cm. unit volume = 764 A3/C60	(NH3)K3C60	N1H3K3C60	N	1	H	3	K	3	C	60																	2002																												fullerene																		K					4.2																																																																																																							Evidence for insulating behavior in the electric conduction of (NH3)K3C60 system			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Phys.Rev.Lett., 88(2002)96401	A.Maeda,H.Kitano,K.Miwa,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111155	L088096401	not s/c. powder sample. R by microwave response. conductivity(200K) = 0.0010 Ohm.cm. unit volume = 782 A3/C60	(NH3)KRb2C60	N1H3K1Rb2C60	N	1	H	3	K	1	Rb	2	C	60															2002																												fullerene																		K					4.2																																																																																																							Evidence for insulating behavior in the electric conduction of (NH3)K3C60 system			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Phys.Rev.Lett., 88(2002)96401	A.Maeda,H.Kitano,K.Miwa,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111156	L088096401	not s/c. powder sample. R by microwave response. conductivity(200K) = 0.0008 Ohm.cm. unit volume = 789 A3/C60	(NH3)Rb3C60	N1H3Rb3C60	N	1	H	3	Rb	3	C	60																	2002																												fullerene																		K					4.2																																																																																																							Evidence for insulating behavior in the electric conduction of (NH3)K3C60 system			Department of Basic Science, The University of Tokyo, Tokyo, Japan	Phys.Rev.Lett., 88(2002)96401	A.Maeda,H.Kitano,K.Miwa,R.Matsuo,T.Mitani,T.Takenobu,Y.Iwasa		
111157	APL0813603	gap measured by microwave surface resistance. gap(0K) = 1.92 meV.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		31					31																																																1.44																																																pulsed laser deposition					The superconducting gap of in situ MgB2 thin films by microwave surface impedance measurements			Physics Department, Northeastern University, Boston, Massachusetts, USA	Appl.Phys.Lett., 81(2002)3603	A.Soukiassian,C.Kusko,N.Hakim,S.Sridhar,X.H.Zeng,X.X.Xi		
111158	JAC3470072	needle like single crystal(3 mm long). space-G = P4/mmm. density=6.983 g/cm3. RRR=32.	V2Ga5	Ga5V2	Ga	5	V	2																				3	2002																															A	8.936		2.6831												K		3.59					3.59																																		MHC11158																																																														flux method(Ga-flux)					Single crystal growth, bonding analysis and superconductivity of V2Ga5			Department of Chemistry and Biochemistry, Northern Illinois University, DeKalb, IL,USA	J.Alloys Compd, 347(2002)72-78	C.E.Check,C.Zheng,J.Zhang,K.C.Lobring,K.Rogacki,S.Li		
111159	L089157001	unaligned powder sample. PENET measured by muon-SR measurement.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2002																												skutterudite																		K		1.85					1.85																																									A		3440					4.2																																																grown from Sb-flux					Muon spin relaxation and isotropic pairing in superconducting PrOs4Sb12			Department of Physics, Unversity of California, Riverside, California, USA	Phys.Rev.Lett., 89(2002)157001	Ben-Li Young,D.E.MacLaughlin,E.D.Bauer,G.D.Morris,J.E.Sonier,M.B.Maple,M.S.Rose,O.O.Bernal,R.H.Heffner,T.D.Do		
111160	PHC3820113		SrGa2	Ga2Sr1	Ga	2	Sr	1																					2002																												AlB2																	AlB2, C32	K					2																																																																																																		arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111161	PHC3820113		BaGa2	Ba1Ga2	Ba	1	Ga	2																					2002																												AlB2																	AlB2, C32	K					2																																																																																																		arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111162	PHC3820113		SrGaGe	Sr1Ga1Ge1	Sr	1	Ga	1	Ge	1																			2002																												AlB2																	AlB2, C32	K					2																																																																																																		arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111163	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.5Si1.5	Sr	1	Ga	0.5	Si	1.5																			2002																												AlB2			A	4.1153		4.7839											AlB2, C32	K		3.5					3.5																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111164	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.55Si1.45	Sr	1	Ga	0.55	Si	1.45																			2002																												AlB2			A	4.1172		4.7878											AlB2, C32	K		3.4					3.4																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111165	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.6Si1.4	Sr	1	Ga	0.6	Si	1.4																			2002																												AlB2			A	4.1123		4.8076											AlB2, C32	K		2.98					2.98																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111166	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.65Si1.35	Sr	1	Ga	0.65	Si	1.35																			2002																												AlB2			A	4.1045		4.7988											AlB2, C32	K		2.58					2.58																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111167	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.7Si1.3	Sr	1	Ga	0.7	Si	1.3																			2002																												AlB2			A	4.1328		4.8007											AlB2, C32	K		3.17					3.17																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111168	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.75Si1.25	Sr	1	Ga	0.75	Si	1.25																			2002																												AlB2			A	4.1318		4.7701											AlB2, C32	K		3.67					3.67																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111169	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.8Si1.2	Sr	1	Ga	0.8	Si	1.2																			2002																												AlB2			A	4.1513		4.777											AlB2, C32	K		4.24					4.24																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111170	PHC3820113		Sr(Ga,Si)2	Sr1Ga0.9Si1.1	Sr	1	Ga	0.9	Si	1.1																			2002																												AlB2			A	4.1601		4.7582											AlB2, C32	K		4.73					4.73																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111171	PHC3820113	sharp transition. delta-Tc = 0.1 K.	Sr(Ga,Si)2	Sr1Ga1Si1	Sr	1	Ga	1	Si	1																			2002																												AlB2			A	4.1786		4.7355											AlB2, C32	K		5.1					5.1																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111172	PHC3820113		Sr(Ga,Si)2	Sr1Ga1.1Si0.9	Sr	1	Ga	1.1	Si	0.9																			2002																												AlB2			A	4.1893		4.7296											AlB2, C32	K		5.04					5.04																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111173	PHC3820113		Sr(Ga,Si)2	Sr1Ga1.2Si0.8	Sr	1	Ga	1.2	Si	0.8																			2002																												AlB2			A	4.2097		4.7286											AlB2, C32	K		4.75					4.75																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111174	PHC3820113		Sr(Ga,Si)2	Sr1Ga1.3Si0.7	Sr	1	Ga	1.3	Si	0.7																			2002																												AlB2			A	4.2195		4.7188											AlB2, C32	K		3.52					3.52																																																																																																arc-melting					Study of binary and pseudo-binary intermetallic compounds with AlB2 structure			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 382(2002)113-116	B.Lorenz,C.W.Chu,J.Cmaidalka,J.K.Meen,R.L.Meng,Y.S.Wang,Y.Y.Sun,Y.Y.Xue		
111175	PHC3820153	x=0.85. Tc(on)=8.5K. R(300)=1.4 mOhm.cm. 98% AlB2 structure	(Mo,Zr)xB2	Mo0.816Zr0.034B2	Mo	0.816	Zr	0.034	B	2																			2002																												AlB2			A	3.0468		3.1615											AlB2, C32	K		8.14					8.14																																																																																																arc-melting					Structure and superconductivity in Zr-stabilized, nonstoichiometric molybdenum diboride			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton,NJ, USA	Physica C, 382(2002)153-165	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,L.E.Muzzy,M.Avdeev,M.K.Haas,R.J.Cava		
111176	PHC3820153	x=0.88. 98% AlB2 + 2% B. gamma in mj/mol.K2. delta-C/gamma*Tc = 1.19.Debye-T = 620, and 690 K for using B<11> and B<10> isotope.	(Mo,Zr)xB2	Mo0.8448Zr0.0352B2	Mo	0.8448	Zr	0.0352	B	2																			2002																												AlB2			A	3.0474		3.1596											AlB2, C32	K		8.11					8.11																																																								mj/mol.K2	4.4		620																																					arc-melting					Structure and superconductivity in Zr-stabilized, nonstoichiometric molybdenum diboride			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton,NJ, USA	Physica C, 382(2002)153-165	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,L.E.Muzzy,M.Avdeev,M.K.Haas,R.J.Cava		
111177	PHC3820153	x=0.91	(Mo,Zr)xB2	Mo0.8736Zr0.0364B2	Mo	0.8736	Zr	0.0364	B	2																			2002																												AlB2			A	3.05		3.1558											AlB2, C32	K		7.92					7.92																																																																																																arc-melting					Structure and superconductivity in Zr-stabilized, nonstoichiometric molybdenum diboride			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton,NJ, USA	Physica C, 382(2002)153-165	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,L.E.Muzzy,M.Avdeev,M.K.Haas,R.J.Cava		
111178	PHC3820153	x=0.96	(Mo,Zr)xB2	Mo0.9216Zr0.0384B2	Mo	0.9216	Zr	0.0384	B	2																			2002																												AlB2			A	3.0519		3.1417											AlB2, C32	K		7.51					7.51																																																																																																arc-melting					Structure and superconductivity in Zr-stabilized, nonstoichiometric molybdenum diboride			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton,NJ, USA	Physica C, 382(2002)153-165	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,L.E.Muzzy,M.Avdeev,M.K.Haas,R.J.Cava		
111179	PHC3820153	x=1.0. single phase. gamma in mj/mol.K2. delta-C/gamma*Tc = 1.8	(Mo,Zr)xB2	Mo0.96Zr0.04B2	Mo	0.96	Zr	0.04	B	2																			2002																												AlB2			A	3.0551		3.1282											AlB2, C32	K		5.74					5.74						0.11	B																																																	mj/mol.K2	3.65																																							arc-melting					Structure and superconductivity in Zr-stabilized, nonstoichiometric molybdenum diboride			Department of Chemistry, Princeton Materials Institute, Princeton University, Princeton,NJ, USA	Physica C, 382(2002)153-165	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,L.E.Muzzy,M.Avdeev,M.K.Haas,R.J.Cava		
111180	PHC3820361	density(theoretical)=3.14 g/cm3	Sr(Al,Si)2	Sr1Al1Si1	Sr	1	Al	1	Si	1																			2002																												AlB2			A	4.2475		4.7421											AlB2, C32	K		4.2					4.2																																																																																																arc-melting					Superconductivity of M1(M2<0.5>,Si<0.5>)2 (M1 = Si and Ba, M2 = Al and Ga), ternary silicides with the AlB2-type structure			National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 382(2002)361-366	H.Abe,H.Kitazawa,H.Kito,K.Nishida,K.Yoshii,M.Imai,T.Kimura		
111181	PHC3820361	density(theoretical)=3.84 g/cm3	Ba(Al,Si)2	Ba1Al1Si1	Ba	1	Al	1	Si	1																			2002																												AlB2			A	4.2973		5.1424											AlB2, C32	K					2																																																																																																		arc-melting					Superconductivity of M1(M2<0.5>,Si<0.5>)2 (M1 = Si and Ba, M2 = Al and Ga), ternary silicides with the AlB2-type structure			National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 382(2002)361-366	H.Abe,H.Kitazawa,H.Kito,K.Nishida,K.Yoshii,M.Imai,T.Kimura		
111182	PHC3820361	density(theoretical)=4.29 g/cm3	Sr(Ga,Si)2	Sr1Ga1Si1	Sr	1	Ga	1	Si	1																			2002																												AlB2			A	4.1875		4.7447											AlB2, C32	K		5.1					5.1																																																																																																arc-melting					Superconductivity of M1(M2<0.5>,Si<0.5>)2 (M1 = Si and Ba, M2 = Al and Ga), ternary silicides with the AlB2-type structure			National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 382(2002)361-366	H.Abe,H.Kitazawa,H.Kito,K.Nishida,K.Yoshii,M.Imai,T.Kimura		
111183	PHC3820361	not s/c. density(theoretical)=4.85 g/cm3	Ba(Ga,Si)2	Ba1Ga1Si1	Ba	1	Ga	1	Si	1																			2002																												AlB2			A	4.2587		5.1039											AlB2, C32	K		3.9					3.9																																																																																																arc-melting					Superconductivity of M1(M2<0.5>,Si<0.5>)2 (M1 = Si and Ba, M2 = Al and Ga), ternary silicides with the AlB2-type structure			National Institute for Materials Science, Tsukuba, Ibaraki, Japan	Physica C, 382(2002)361-366	H.Abe,H.Kitazawa,H.Kito,K.Nishida,K.Yoshii,M.Imai,T.Kimura		
111184	PRL0784273	Hc2(4.2K)=5.7 T for H//c-axis. gap(delta)=2.2 meV at 4.2 K. gap by STM. STM on the (001) surface.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		15.8					15.8																				T		5.7																										3.2																						MTP11184																										flux method using Ni2B					Scanning tunneling Microscopy observation of a square Abrikosov Lattice in LuNI2B2C			Material Science Division-Science and Technology Center for Superconductivity, Argonne National Lab, Argonne,Illinois,USA	Phys.Rev.Lett., 78(1997)4273	A.E.Koshelev,G.W.Crabtree,I.Aranson,M.Lavarone,P.C.Canfield,U.Welp,V.Metlushko,Y.De Wilde		
111185	PRL0780547	gap was measured by optical conductivity.  gap=3.46 meV	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1997																												LuNi2B2C																		K		15.6					15.6																																									A		4800					5.15																						MTP11185																															Optical conductivity of the superconductors LNi2B2C (L=Lu and Y)			Laboratorium fur Festkoperphysik, ETH-Zurich, Zurich, Switzerland	Phys.Rev.Lett., 78(1997)547	B.K.Cho,F.Bommeli,L.Dogiorgi,M.B.Maple,P.C.Canfield,P.Wachter,R.Chau		
111186	PRL0780547	gap was measured by optical conductivity.  gap=2.68 meV	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1997																												LuNi2B2C																		K		16.6					16.6																																									A		4900					3.75																																																					Optical conductivity of the superconductors LNi2B2C (L=Lu and Y)			Laboratorium fur Festkoperphysik, ETH-Zurich, Zurich, Switzerland	Phys.Rev.Lett., 78(1997)547	B.K.Cho,F.Bommeli,L.Dogiorgi,M.B.Maple,P.C.Canfield,P.Wachter,R.Chau		
111187	SSC1250017	LixBC is not s/c for 0.5<x<2.4	LixBC	Li0.25B1C1	Li	0.25	B	1	C	1																			2003																																														K					2																																																																																																							Synthesis and physical properties of LiBC intermetallics			Leibniz-Institute for Solid State and Materials Research Dresden, Dresden, Germany	Solid State Commun., 125(2003)17-21	C.Geibel,D.Souptel,G.Behr,W.Loser,Z.Hossain		
111188	PHC3830191		CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2002																												AlB2			A	4.189		4.4											AlB2, C32	K		7.8					7.8																																																																																																arc-melting					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111189	PHC3830191		SrAlSi	Sr1Al1Si1	Sr	1	Al	1	Si	1																			2002																												AlB2			A	4.22		4.752											AlB2, C32	K		5.1					5.1																																																																																																arc-melting					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111190	PHC3830191	not s/c	BaAlSi	Ba1Al1Si1	Ba	1	Al	1	Si	1																			2002																												AlB2			A	4.29		5.14											AlB2, C32	K					2																																																																																																		arc-melting					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111191	PHC3830191		Ca(Al,Si)2	Ca1Al1.4Si0.6	Ca	1	Al	1.4	Si	0.6																			2002																												AlB2			A	4.2333		4.431											AlB2, C32	K		4.6					4.6																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111192	PHC3830191		Ca(Al,Si)2	Ca1Al1.3Si0.7	Ca	1	Al	1.3	Si	0.7																			2002																												AlB2			A	4.2241		4.4249											AlB2, C32	K		4.5					4.5																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111193	PHC3830191		Ca(Al,Si)2	Ca1Al1.25Si0.75	Ca	1	Al	1.25	Si	0.75																			2002																												AlB2																	AlB2, C32	K		4.4					4.4																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111194	PHC3830191		Ca(Al,Si)2	Ca1Al1.2Si0.8	Ca	1	Al	1.2	Si	0.8																			2002																												AlB2			A	4.2134		4.4172											AlB2, C32	K		5.21					5.21																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111195	PHC3830191		Ca(Al,Si)2	Ca1Al1.1Si0.9	Ca	1	Al	1.1	Si	0.9																			2002																												AlB2			A	4.2011		4.4065											AlB2, C32	K		6.63					6.63																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111196	PHC3830191		Ca(Al,Si)2	Ca1Al0.9Si1.1	Ca	1	Al	0.9	Si	1.1																			2002																												AlB2			A	4.1751		4.3927											AlB2, C32	K		5.57					5.57																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111197	PHC3830191		Ca(Al,Si)2	Ca1Al0.8Si1.2	Ca	1	Al	0.8	Si	1.2																			2002																												AlB2			A	4.1628		4.3881											AlB2, C32	K		4.05					4.05																																																																																																					Superconductivity in the C32 intermetallic compounds AAl2-xSix, with A = Ca and Sr; and 0.6 < x < 1.2			Texas Center for Superconductivity ande Department of Physics, University of Houston, Houston, Texas, USA	Physica C, 383(2002)191-196	B.Lorenz,C.W.Chu,J.Cmaidalka,J.Lenzi,R.L.Meng,Y.Y.Sun,Y.Y.Xue		
111198	PHC3830197	Nb1-xB2 is superconducting for 0.04<x=<0.5 with AlB2 structure.	NbB2	B2Nb0.84	B	2	Nb	0.84																					2002																												AlB2			A	3.0979		3.321											AlB2, C32	K		9.1					9.1																																																																																																sinter(5 GPa, 1200C)					High-pressure synthesis of superconducting Nb1-xB2 (x = 0 - 0.48) with the maximum Tc = 9.2 K			SRL, ISTEC, Shinonome,Koto-ku, Tokyo, Japan	Physica C, 383(2002)197-206	A.Yamamoto,C.Takao,M.Izumi,S.Tajima,T.Masui		
111199	PHC3830197	not s/c for 0<x<0.24 in Ta1-xB2.	TaB2	B2Ta0.84	B	2	Ta	0.84																					2002																												AlB2			A	3.072		3.27											AlB2, C32	K					2																																																																																																		sinter(5 GPa, 1200C)					High-pressure synthesis of superconducting Nb1-xB2 (x = 0 - 0.48) with the maximum Tc = 9.2 K			SRL, ISTEC, Shinonome,Koto-ku, Tokyo, Japan	Physica C, 383(2002)197-206	A.Yamamoto,C.Takao,M.Izumi,S.Tajima,T.Masui		
111200	P066180502	Hc2//ab=17 T, Hc2//c=3.5 T. anisotropy factor = 5, but T-dependent. peak effect was observed for H=2T//c-axis.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38					38																				T		17												MHC11200																																																																			Anisotropy of the upper critical field and critical current in single crystal MgB2			CNRS, Grenoble Cedex, France	Phys.Rev.B, 66(2002)180502	A.G.M.Jansen,B.Kang,C.Marcenat,C.U.Jung,G.Karapetrov,H.-S.Lee,J.Marcus,K.H.P.Kim,L.Lyard,L.Paulius,P.Samuely,P.Szabo,S.-I.Lee,S.Blanchard,S.Choi,T.Klein,U.Welp,W.K.Kwok		
111201	P066180504	Hall effect is negative for H//ab. both hole and electron carrier coexist. anisotropy=3.6 at Tc, =3.4 at 273 K. Debye-T by fitting Bloch-Gruneisen eq.	MgB2	Mg1B2	Mg	1	B	2																				3	2002																												AlB2																	AlB2, C32	K																																																																		880																																MRH11201										Anisotropic resistivity and Hall effect in MgB2 single crystals			SRL, ISTEC, Shinonome,Tokyo,Japan	Phys.Rev.B, 66(2002)180504	K.Nakao,M.Murakami,N.Chikumoto,N.Koshizuka,S.Lee,S.Tajima,T.Masui,Yu.Eltsev		
111202	P066184511	RESN=0.87 uOhm.cm. skin depth at 44 GHz = 2200 A.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2002																												LuNi2B2C																		K		15.4					15.4																				T		8														A		65																																																															Effects of superconducting gap anisotropy on the flux flow resistivity in Y(Ni1-xPtx)2B2C			Department of Advanced Materials Science, The university of Tokyo, Hongo, Bunkyo-ku, Tokyo,Japan	Phys.Rev.B, 66(2002)184511	A.Koizumi,A.Maeda,H.Kitano,H.Takagi,K.Kitazawa,K.Takaki,M.Nohara,T.Hanaguri,Y.Kato,Y.Tsuchiya		
111203	P066184511	RESN=20.5 uOhm.cm. skin depth at 44 GHz = 1100 A.	Y(Ni,Pt)2B2C	Y1Ni1.9Pt0.1B2C1	Y	1	Ni	1.9	Pt	0.1	B	2	C	1														3	2002																												LuNi2B2C																		K		13.7					13.7																				T		5														A		80																																																															Effects of superconducting gap anisotropy on the flux flow resistivity in Y(Ni1-xPtx)2B2C			Department of Advanced Materials Science, The university of Tokyo, Hongo, Bunkyo-ku, Tokyo,Japan	Phys.Rev.B, 66(2002)184511	A.Koizumi,A.Maeda,H.Kitano,H.Takagi,K.Kitazawa,K.Takaki,M.Nohara,T.Hanaguri,Y.Kato,Y.Tsuchiya		
111204	P066184511	RESN=35.5 uOhm.cm. skin depth at 44 GHz = 14000 A.	Y(Ni,Pt)2B2C	Y1Ni1.6Pt0.4B2C1	Y	1	Ni	1.6	Pt	0.4	B	2	C	1														3	2002																												LuNi2B2C																		K		12.1					12.1																				T		4.3														A		90																																																															Effects of superconducting gap anisotropy on the flux flow resistivity in Y(Ni1-xPtx)2B2C			Department of Advanced Materials Science, The university of Tokyo, Hongo, Bunkyo-ku, Tokyo,Japan	Phys.Rev.B, 66(2002)184511	A.Koizumi,A.Maeda,H.Kitano,H.Takagi,K.Kitazawa,K.Takaki,M.Nohara,T.Hanaguri,Y.Kato,Y.Tsuchiya		
111205	P066214501	weak ferromagnet below 2 K. Tc defined as R=0. Neel-T defined as dM/dH peak.	(Er,Tb)Ni2B2C	Er0.75Tb0.25Ni2B2C1	Er	0.75	Tb	0.25	Ni	2	B	2	C	1														3	2002								7																				LuNi2B2C																		K		4					4																																																																																																					Magnetic pair breaking and weak ferromagnetism in single crystals of Er1-xTbxNi2B2C			Kwangju Institute of Science and Technology, Gwangju, Korea	Phys.Rev.B, 66(2002)214501	B.K.Cho,Chang-An Kim		
111206	P066214501	Tc defined as R=0. Neel-T defined as dM/dH peak.	(Er,Tb)Ni2B2C	Er0.7Tb0.3Ni2B2C1	Er	0.7	Tb	0.3	Ni	2	B	2	C	1														3	2002								7																				LuNi2B2C																		K		2					2																																																																																																					Magnetic pair breaking and weak ferromagnetism in single crystals of Er1-xTbxNi2B2C			Kwangju Institute of Science and Technology, Gwangju, Korea	Phys.Rev.B, 66(2002)214501	B.K.Cho,Chang-An Kim		
111207	P066214501	Tc defined as Tc(on). Neel-T defined as dM/dH peak.	(Er,Tb)Ni2B2C	Er0.4Tb0.6Ni2B2C1	Er	0.4	Tb	0.6	Ni	2	B	2	C	1														3	2002								11																				LuNi2B2C																		K		2					2																																																																																																					Magnetic pair breaking and weak ferromagnetism in single crystals of Er1-xTbxNi2B2C			Kwangju Institute of Science and Technology, Gwangju, Korea	Phys.Rev.B, 66(2002)214501	B.K.Cho,Chang-An Kim		
111208	PHC3210093	adding 5 mol % (Tb,Er)B2C2	ErNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1999								6																				LuNi2B2C																		K		11.3					11.3																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111209	PHC3210093	adding 5 mol % (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.9Tb0.1Ni2B2C1	Er	0.9	Tb	0.1	Ni	2	B	2	C	1															1999								6.48																				LuNi2B2C																		K		9.2					9.2																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111210	PHC3210093	adding 5 mol % (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.85Tb0.15Ni2B2C1	Er	0.85	Tb	0.15	Ni	2	B	2	C	1															1999								6.85																				LuNi2B2C																		K		8.3					8.3																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111211	PHC3210093	adding 5 mol % (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.8Tb0.2Ni2B2C1	Er	0.8	Tb	0.2	Ni	2	B	2	C	1															1999								7.1																				LuNi2B2C																		K		7.1					7.1																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111212	PHC3210093	adding 5 mol % (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.775Tb0.225Ni2B2C1	Er	0.775	Tb	0.225	Ni	2	B	2	C	1															1999								7.1																				LuNi2B2C																		K		5.9					5.9																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111213	PHC3210093	adding 5 mol % (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.75Tb0.25Ni2B2C1	Er	0.75	Tb	0.25	Ni	2	B	2	C	1															1999								7.1																				LuNi2B2C																		K		4.9					4.9																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111214	PHC3210093	adding 5 mol % Ni2B	ErNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1999																												LuNi2B2C																		K		11					11																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111215	PHC3210093	adding 5 mol % Ni2B	(Er,Tb)Ni2B2C	Er0.9Tb0.1Ni2B2C1	Er	0.9	Tb	0.1	Ni	2	B	2	C	1															1999																												LuNi2B2C																		K		7.84					7.84																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111216	PHC3210093	adding 5 mol % Ni2B	(Er,Tb)Ni2B2C	Er0.85Tb0.15Ni2B2C1	Er	0.85	Tb	0.15	Ni	2	B	2	C	1															1999																												LuNi2B2C																		K		6.15					6.15																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111217	PHC3210093	adding 5 mol % Ni2B	(Er,Tb)Ni2B2C	Er0.82Tb0.18Ni2B2C1	Er	0.82	Tb	0.18	Ni	2	B	2	C	1															1999								7.1																				LuNi2B2C																		K		5.63					5.63																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111218	PHC3210093	adding 5 mol % Ni2B	(Er,Tb)Ni2B2C	Er0.8Tb0.2Ni2B2C1	Er	0.8	Tb	0.2	Ni	2	B	2	C	1															1999																												LuNi2B2C																		K		4.8					4.8																																																																																																arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111219	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.8Tb0.3Ni2B2C1	Er	0.8	Tb	0.3	Ni	2	B	2	C	1															1999								7.1																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111220	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.8Tb0.35Ni2B2C1	Er	0.8	Tb	0.35	Ni	2	B	2	C	1															1999								6.38																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111221	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.8Tb0.5Ni2B2C1	Er	0.8	Tb	0.5	Ni	2	B	2	C	1															1999								6.1																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111222	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2	(Er,Tb)Ni2B2C	Er0.8Tb0.7Ni2B2C1	Er	0.8	Tb	0.7	Ni	2	B	2	C	1															1999								10.8																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111223	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2. below Curie-T(in table) shows weak ferro-.	(Er,Tb)Ni2B2C	Er0.8Tb0.8Ni2B2C1	Er	0.8	Tb	0.8	Ni	2	B	2	C	1															1999							6.3	12																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111224	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2. below Curie-T(in table) shows weak ferro-.	(Er,Tb)Ni2B2C	Er0.8Tb0.9Ni2B2C1	Er	0.8	Tb	0.9	Ni	2	B	2	C	1															1999							8.2	13.1																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111225	PHC3210093	not s/c. adding 5 mol % Ni2B or (Tb,Er)B2C2. below Curie-T(in table) shows weak ferro-.	TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																	1999							10.7	15.4																				LuNi2B2C																		K					4.2																																																																																																		arc-melting + ANN					Metallurgy, superconductivity and field-dependent magnetic ordering in TbxEr1-xNi2B2C	199908		Institut Festkorper- und Werkstofforschung dresden, PF 27 00 16, D-01171Dresden, Germany	Physica C,321(1999)93-102	A. Gumbel,A.Gumbel,G. Behr,G. Fuchs,G.Behr,G.Fuchs,H. Bitterlich,H.Bitterlich,K. Nenkov,K.Nenkov,L. Schultz,L.Schultz,W. Loser,W.Loser		
111226	PRL0770163		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																3	1996								5.22																				LuNi2B2C																		K		8.53					8.53																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111227	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.9Dy0.1Ni2B2C1	Ho	0.9	Dy	0.1	Ni	2	B	2	C	1														3	1996								5.6																				LuNi2B2C																		K		8					8																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111228	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.85Dy0.15Ni2B2C1	Ho	0.85	Dy	0.15	Ni	2	B	2	C	1														3	1996								5.89																				LuNi2B2C																		K		7.89					7.89																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111229	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.8Dy0.2Ni2B2C1	Ho	0.8	Dy	0.2	Ni	2	B	2	C	1														3	1996								6.2																				LuNi2B2C																		K		6.61					6.61																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111230	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.7Dy0.3Ni2B2C1	Ho	0.7	Dy	0.3	Ni	2	B	2	C	1														3	1996								6.66																				LuNi2B2C																		K		5.86					5.86																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111231	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.65Dy0.35Ni2B2C1	Ho	0.65	Dy	0.35	Ni	2	B	2	C	1														3	1996								6.94																				LuNi2B2C																		K		5.91					5.91																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111232	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.6Dy0.4Ni2B2C1	Ho	0.6	Dy	0.4	Ni	2	B	2	C	1														3	1996								7.28																				LuNi2B2C																		K		6.02					6.02																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111233	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.5Dy0.5Ni2B2C1	Ho	0.5	Dy	0.5	Ni	2	B	2	C	1														3	1996								7.61																				LuNi2B2C																		K		5.91					5.91																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111234	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.4Dy0.6Ni2B2C1	Ho	0.4	Dy	0.6	Ni	2	B	2	C	1														3	1996								8.05																				LuNi2B2C																		K		5.86					5.86																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111235	PRL0770163		(Ho,Dy)Ni2B2C	Ho0.2Dy0.8Ni2B2C1	Ho	0.2	Dy	0.8	Ni	2	B	2	C	1														3	1996								8.97																				LuNi2B2C																		K		6.2					6.2																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111236	PRL0770163		DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1996								10.13																				LuNi2B2C																		K		6.2					6.2																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111237	PRL0770163		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1996																												LuNi2B2C																		K		15.96					15.96																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111238	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.772Dy0.228Ni2B2C1	Lu	0.772	Dy	0.228	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K		11.77					11.77																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111239	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.574Dy0.426Ni2B2C1	Lu	0.574	Dy	0.426	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K		7.54					7.54																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111240	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.418Dy0.582Ni2B2C1	Lu	0.418	Dy	0.582	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K		4.35					4.35																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111241	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.37Dy0.63Ni2B2C1	Lu	0.37	Dy	0.63	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K		3.59					3.59																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111242	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.32Dy0.68Ni2B2C1	Lu	0.32	Dy	0.68	Ni	2	B	2	C	1														3	1996																												LuNi2B2C																		K		2					2																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111243	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.1Dy0.9Ni2B2C1	Lu	0.1	Dy	0.9	Ni	2	B	2	C	1														3	1996								8.42																				LuNi2B2C																		K		2.47					2.47																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111244	PRL0770163	Dy-content (x) estimated from de Gennes factor	(Lu,Dy)Ni2B2C	Lu0.05Dy0.95Ni2B2C1	Lu	0.05	Dy	0.95	Ni	2	B	2	C	1														3	1996								9.22																				LuNi2B2C																		K		6.35					6.35																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111245	PRL0770163	Dy-content (x) estimated from de Gennes factor	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1996								10.33																				LuNi2B2C																		K		6.26					6.26																																																																																																Ni2B flux method					Breakdown of de Gennes Scaling in (R1-xR'x)Ni2B2C Compounds			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Lev.Lett.,77(1998)163	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,P.C. Canfield,P.C.Canfield		
111246	PR05308499	not s/c. Curie-T=16 K for H//[100], = -60 K for H//[001], = 0 K for powder. Figure shows phase diagram.	TbNi2B2C	Tb1Ni2B2C1	Tb	1	Ni	2	B	2	C	1																3	1996							16	14.8																				LuNi2B2C																		K																																																																																																							Ni2B flux method					Magnetic anisotropy and weak ferromagnetism of single-crystal TbNi2B2C			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa, USA	Phys.Rev.B, 53(1996)8499	B.K.Cho,D.C.Johnston,P.C.Canfield		
111247	PR05203676	H//ab. anisotropy = 1.29. G-L parameter = 7.7	TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																3	1995							-36	1.52																				LuNi2B2C																		K		10.8					10.8																				kG		27.2							T/K		0.36			MHC11247		A		110			A		850																																																					Ni2B flux method					Magnetic and superconductig properties of single-crystal TmNi2B2C	199508			Phys.Rev.B.52(1995)3676	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,L.L. Miller,L.L.Miller,MIg. Xu,Ming Xu,P.C. Canfield,P.C.Canfield	Tm, Ni, B, C	
111248	PR05203676	H//c, anisotropy = 1.29. G-L parameter = 6.3	TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																3	1995							20.8	1.52																				LuNi2B2C																		K		10.8					10.8																				kG		21.2							T/K		0.28					A		124			A		780																																																					Ni2B flux method					Magnetic and superconductig properties of single-crystal TmNi2B2C	199508			Phys.Rev.B.52(1995)3676	B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,L.L. Miller,L.L.Miller,MIg. Xu,Ming Xu,P.C. Canfield,P.C.Canfield	Tm, Ni, B, C	
111249	PR05203684	anisotropy = 1.31, Neel-T decreases as increasing H.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1995							-7.4	5.85																				LuNi2B2C																		K		10.5					10.5																				kG		14.7							T/K		0.2			MHC11249		A		150																																																										Ni2B flux method					Magnetism and superconductivity in single-crystal ErNi2B2C	199508			Phys.Rev.B,52(1995)3684	A. Yatskar,A.Yatskar,B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,L.L. Miller,L.L.Miller,P.C. Canfield,P.C.Canfield,W.P. Beyermann,W.P.Beyermann	Er, Ni, B, C	
111250	PR05203684	anisotropy = 1.31, Neel-T independent of H. G-L parameter = 8.8	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1995							-5.7	9.5																				LuNi2B2C																		K		10.5					10.5																				kG		19.1							T/K		0.26					A		131			A		1160																																																					Ni2B flux method					Magnetism and superconductivity in single-crystal ErNi2B2C	199508			Phys.Rev.B,52(1995)3684	A. Yatskar,A.Yatskar,B.K. Cho,B.K.Cho,D.C. Johnston,D.C.Johnston,L.L. Miller,L.L.Miller,P.C. Canfield,P.C.Canfield,W.P. Beyermann,W.P.Beyermann	Er, Ni, B, C	
111251	PHC3830197	not AlB2 structure, not s/c.  MoB2 compositions also measured. But not s/c, not AlB2 structure.	MoB2	B2Mo0.84	B	2	Mo	0.84																					2002																												Mo2B5																		K					2				1																																																																																														sinter(5 GPa, 1200C)					High-pressure synthesis of superconducting Nb1-xB2 (x = 0 - 0.48) with the maximum Tc = 9.2 K			SRL, ISTEC, Shinonome,Koto-ku, Tokyo, Japan	Physica C, 383(2002)197-206	A.Yamamoto,C.Takao,M.Izumi,S.Tajima,T.Masui		
111252	JPS0712836	three step resistivity drops (1.4, 1.0, 0.4 K). gamma in mj/K2.mol-Ce.	Ce2CoIn8	Ce2Co1In8	Ce	2	Co	1	In	8																		3	2002																												Ho2CoGa8			A	4.643		12.25												K		0.4					0.4																				T		1																																		mj/mol.K2	250																																							In flux method					Observation of superconductivity in heavy-fermion compounds of Ce2CoIn8			Nagoya Institute of Technology, Nagoya,Japan	J.Phys.Soc.jpn, 71(2002)2836	G.Chen,I.Sakamoto,K.Saito,M.Hedo,M.Sorai,S.Ohara,Y.Uwatoko		
111253	MAT0204064	p-induced s/c. Tc shows Tc(max). Pc = 10 kbar. s/c properties shows for p=16.3 kbar. P(Tn=0)=30 kbar. Tn=2.65 K, another transition at 1.65 K under 1 atm. gamma in mj/K2.mol-Ce from dHc2/dT	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																		3	2002								2.65																				Ho2CoGa8			A	4.665		12.244												K		2			0		2	MTC11253																			kOe		53.6							kOe/K		91.8					A		77																		mj/mol.K2	200																																							In flux method					Magnetism, structure and superconductivity in Ce2RhIn8			Los Alamos National Lab, Los Alamos, NM, USA	cond-mat/0204064	C.Petrovic,H.A.Borges,J.D.Thompson,J.L.Sarrao,M.Nicklas,P.G.Pagliuso,V.A.Sidorov,Z.Fisk		
111254	MMM2260005	p-induced s/c. Tc shows Tc(max). s/c for p>Pc=15 kbar. gamma in mj/K2.mol-Ce. delta-C/gamma*Tc = 1.5	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2001								3.8																				HoCoGa5			A	4.652		7.542												K		1.62			0		1.62	MTC11254																																																							mj/mol.K2	400																																							In flux method					Superconductivity and magnetism in a new class of heavy-fermion materials			Los Alamos National Lab, Los Alamos, NM, USA	J.Mag.Mag.Mater., 226-230(2001)5-10	C.Petrovic,F.Bouquet,H.Hegger,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Jaime,N.E.Phillip,N.J.Curro,P.C.Hammel,P.G.Pagliuso,R.A.Fisher,R.Movshovich,Z.Fisk		
111255	MMM2260005	gamma in mj/K2.mol-Ce. Tc = 1.2 K by R=0. Tc = 0.4 K from susceptibility.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001								0.4																				HoCoGa5			A	4.668		7.515												K		1.2					1.2																																																								mj/mol.K2	720																																							In flux method					Superconductivity and magnetism in a new class of heavy-fermion materials			Los Alamos National Lab, Los Alamos, NM, USA	J.Mag.Mag.Mater., 226-230(2001)5-10	C.Petrovic,F.Bouquet,H.Hegger,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Jaime,N.E.Phillip,N.J.Curro,P.C.Hammel,P.G.Pagliuso,R.A.Fisher,R.Movshovich,Z.Fisk		
111256	MMM2260005	gamma in mj/K2.mol-Ce.	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																		3	2001								2.8																				Ho2CoGa8			A	4.665		12.244												K																																																															mj/mol.K2	400																																							In flux method					Superconductivity and magnetism in a new class of heavy-fermion materials			Los Alamos National Lab, Los Alamos, NM, USA	J.Mag.Mag.Mater., 226-230(2001)5-10	C.Petrovic,F.Bouquet,H.Hegger,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Jaime,N.E.Phillip,N.J.Curro,P.C.Hammel,P.G.Pagliuso,R.A.Fisher,R.Movshovich,Z.Fisk		
111257	MMM2260005	gamma in mj/K2.mol-Ce.	Ce2IrIn8	Ce2Ir1In8	Ce	2	Ir	1	In	8																		3	2001																												Ho2CoGa8			A	4.671		12.214												K					0.05																																																										mj/mol.K2	700																																							In flux method					Superconductivity and magnetism in a new class of heavy-fermion materials			Los Alamos National Lab, Los Alamos, NM, USA	J.Mag.Mag.Mater., 226-230(2001)5-10	C.Petrovic,F.Bouquet,H.Hegger,J.D.Thompson,J.L.Sarrao,M.F.Hundley,M.Jaime,N.E.Phillip,N.J.Curro,P.C.Hammel,P.G.Pagliuso,R.A.Fisher,R.Movshovich,Z.Fisk		
111258	P066220504	skutterudite. RR=2.8 uOhm.cm. RRR=100. delta-C/gamma*Tc = 1.5.	LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																		3	2002																																														K		0.74					0.74																																																								mj/mol.K2	56																																							Sb-self-flux method					Fermi surface of the heavy-fermion superconductor PrOs4Sb12			Tokyo Metropolitan University, Hachioji,Tokyo,Japan	Phys.Rev.B, 66(2002)220504	H.Harima,H.Sato,H.Shishido,H.Sugawara,K.Oikawa,R.Settai,S.Osaki,S.R.Saha,Y.Aoki,Y.Inada,Y.Onuki		
111259	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.98Ge0.02	Ce	1	Cu	2	Si	1.98	Ge	0.02																	2002								0.7																				CeCu2Si2																		K		0.5					0.5																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111260	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.96Ge0.04	Ce	1	Cu	2	Si	1.96	Ge	0.04																	2002								0.75																				CeCu2Si2																		K		0.4					0.4																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111261	P066224502		CeCu2(Si,Ge)2	Ce1Cu2Si1.92Ge0.08	Ce	1	Cu	2	Si	1.92	Ge	0.08																	2002																												CeCu2Si2																		K		0.27					0.27																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111262	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.88Ge0.12	Ce	1	Cu	2	Si	1.88	Ge	0.12																	2002								0.9																				CeCu2Si2																		K		0.2					0.2																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111263	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.8Ge0.2	Ce	1	Cu	2	Si	1.8	Ge	0.2																	2002								1																				CeCu2Si2																		K		0.15					0.15																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111264	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.6Ge0.4	Ce	1	Cu	2	Si	1.6	Ge	0.4																	2002								1.5																				CeCu2Si2																		K																																																																																																												Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111265	P066224502	Neel-T from NMR	CeCu2(Si,Ge)2	Ce1Cu2Si1.4Ge0.6	Ce	1	Cu	2	Si	1.4	Ge	0.6																	2002								2																				CeCu2Si2																		K																																																																																																												Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111266	P066224502		CeCu2(Si,Ge)2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																			2002																												CeCu2Si2																		K		0.64					0.64																																																																																																					Exotic magnetism and superconductivity in Ge-substituted CeCu2Si2: A Cu NQR study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.B, 66(2002)224502	C.Geibel,F.Steglich,K.Ishida,K.Kashima,K.Obinata,K.Tabuchi,O.Trovarelli,Y.Kawasaki,Y.Kitaoka		
111267	PHC3830295		Y2PdGe3	Y2Pd1Ge3	Y	2	Pd	1	Ge	3																			2003																												AlB2			A	4.1853		4.0009											AlB2, C32	K		3.58					3.58																																																																																																arc-melting					Chemical substitution effects of Si and C on AlB2-type superconductor Y2PdGe3			Department of Physics, Faculty of Engineering, Yokohama National University, Yokohama,Japan	Physica C, 383(2003)295	M.Uehara,S.Takano,Y.Iriyama,Y.Kimishima		
111268	PHC3830295		Y2PdSi3	Y2Pd1Si3	Y	2	Pd	1	Si	3																			2003																												AlB2			A	4.0686		4.0354											AlB2, C32	K					1.8																																																																																																		arc-melting					Chemical substitution effects of Si and C on AlB2-type superconductor Y2PdGe3			Department of Physics, Faculty of Engineering, Yokohama National University, Yokohama,Japan	Physica C, 383(2003)295	M.Uehara,S.Takano,Y.Iriyama,Y.Kimishima		
111269	PHC3830295		Y2Pd(Si,C)3	Y2Pd1Si2.25C0.75	Y	2	Pd	1	Si	2.25	C	0.75																	2003																												AlB2			A	4.1305		3.9425											AlB2, C32	K		2.27					2.27																																																																																																arc-melting					Chemical substitution effects of Si and C on AlB2-type superconductor Y2PdGe3			Department of Physics, Faculty of Engineering, Yokohama National University, Yokohama,Japan	Physica C, 383(2003)295	M.Uehara,S.Takano,Y.Iriyama,Y.Kimishima		
111270	PHC3830295		Y2Pd(Si,C)3	Y2Pd1Si2C1	Y	2	Pd	1	Si	2	C	1																	2003																												AlB2			A	4.1269		3.9238											AlB2, C32	K		2.2					2.2																																																																																																arc-melting					Chemical substitution effects of Si and C on AlB2-type superconductor Y2PdGe3			Department of Physics, Faculty of Engineering, Yokohama National University, Yokohama,Japan	Physica C, 383(2003)295	M.Uehara,S.Takano,Y.Iriyama,Y.Kimishima		
111271	PHC3830421		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	2003																												LuNi2B2C																		K		15.6					15.6																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111272	PHC3830421		(Y,Gd)Ni2B2C	Y0.95Gd0.05Ni2B2C1	Y	0.95	Gd	0.05	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		14					14																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111273	PHC3830421		(Y,Gd)Ni2B2C	Y0.9Gd0.1Ni2B2C1	Y	0.9	Gd	0.1	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		12.3					12.3																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111274	PHC3830421		(Y,Gd)Ni2B2C	Y0.85Gd0.15Ni2B2C1	Y	0.85	Gd	0.15	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		10.6					10.6																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111275	PHC3830421		(Y,Gd)Ni2B2C	Y0.8Gd0.2Ni2B2C1	Y	0.8	Gd	0.2	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		8.1					8.1																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111276	PHC3830421		(Y,Gd)Ni2B2C	Y0.78Gd0.22Ni2B2C1	Y	0.78	Gd	0.22	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		7.4					7.4																																		MHC11276																																																														arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111277	PHC3830421		(Y,Gd)Ni2B2C	Y0.77Gd0.23Ni2B2C1	Y	0.77	Gd	0.23	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		4.2					4.2																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111278	PHC3830421		(Y,Gd)Ni2B2C	Y0.75Gd0.25Ni2B2C1	Y	0.75	Gd	0.25	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		4.2					4.2																																																																																																arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111279	PHC3830421		(Y,Gd)Ni2B2C	Y0.65Gd0.35Ni2B2C1	Y	0.65	Gd	0.35	Ni	2	B	2	C	1															2003								4.8																				LuNi2B2C																		K					1.8																																																																																																		arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111280	PHC3830421		(Y,Gd)Ni2B2C	Y0.6Gd0.4Ni2B2C1	Y	0.6	Gd	0.4	Ni	2	B	2	C	1															2003								6.1																				LuNi2B2C																		K					1.8																																																																																																		arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111281	PHC3830421	spin reorientation temp. = 6.83	(Y,Gd)Ni2B2C	Y0.5Gd0.5Ni2B2C1	Y	0.5	Gd	0.5	Ni	2	B	2	C	1															2003								8.62																				LuNi2B2C																		K					1.8																																																																																																		arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111282	PHC3830421	spin reorientation temp. = 11.0	(Y,Gd)Ni2B2C	Y0.25Gd0.75Ni2B2C1	Y	0.25	Gd	0.75	Ni	2	B	2	C	1															2003								14.4																				LuNi2B2C																		K					1.8																																																																																																		arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111283	PHC3830421	spin reorientation temp. = 12.5	GdNi2B2C	Gd1Ni2B2C1	Gd	1	Ni	2	B	2	C	1																	2003								18.3																				LuNi2B2C																		K					1.8																																																																																																		arc-melting					The interplay of magnetic order and superconductivity in GdxY1-xNi2B2C			Institut fur Festkorper-und Werkstofforschung Dresden, Dresden, Germany	Physica C, 383(2003)421	A.Handstein,G.Fuchs,K.-H.Muller,K.Nenkov,Z.Drzazga		
111284	PHC3840071	RR=28.35 uOhm.cm. RRR=4.4. Tc defined as R=0. gamma in mj/K2.mol-La. delta-C/gamma*Tc = 0.66	La6Ni2Sn	La6Ni2Sn1	La	6	Ni	2	Sn	1																			2003																												Ho6Ni2Sn																		K		2.25					2.25																				kOe		6.24							kOe/K		4					A		230															MSP11284			mj/mol.K2	6.3		135																																					arc-melting					Superconductivity in the Ni-based ternary compound La6Ni2Sn			Department of Physics, National Taiwan University, Taipei,Taiwan,ROC	Physica C, 384(2003)71-74	B.K.Wang,Ching-Ray Chang,J.W.Chen,N.S.Jou,R.C.Yang		
111285	PHC2330367	G-L parameter = 35	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	1994																												LuNi2B2C			A	3.524		10.535												K		15.5					15.5											Oe		83.5							T		4.76												MHC11285		A		100			A		3500																																																					induction furnace under Ar					Magnetic properties of YNi2B2C superconductor	199411			Physica C.,233(1994) 367-372	E.R.Yacoby,I.Felner,R.Prozorov,Y.Yeshurun	Y,B,Ni,C	
111286	PHC2270321	Hirr(T)=A(1-T/Tc)**n ,  n = 1.16. properties are for H//c-axis. G-L parameter = 15	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	1994																												LuNi2B2C																		K		15.5					15.5											Oe		230							T		3.2							T/K		0.32					nm		10			nm		15																																																					Ni2B flux method					Superconducting state magnetization and critical fields of single crystal YNi2B2C	199407			Physica C, 227(1994)321-326	B.K.Cho,D.C.Johnson,D.K.Finnemore,J.E.Ostenson,Ming Xu,P.C.Canfield,Z.R.Wang	Y,Ni,B,C	
111287	PSS1890489		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1995																												LuNi2B2C			A	3.526		10.5824												K		15.5					15.5																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111288	PSS1890489		(Y,Gd)Ni2B2C	Y0.95Gd0.05Ni2B2C1	Y	0.95	Gd	0.05	Ni	2	B	2	C	1															1995																												LuNi2B2C			A	3.5317		10.5788												K		13					13																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111289	PSS1890489		(Y,Gd)Ni2B2C	Y0.9Gd0.1Ni2B2C1	Y	0.9	Gd	0.1	Ni	2	B	2	C	1															1995								2																				LuNi2B2C			A	3.5308		10.5647												K		11.2					11.2																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111290	PSS1890489		(Y,Gd)Ni2B2C	Y0.85Gd0.15Ni2B2C1	Y	0.85	Gd	0.15	Ni	2	B	2	C	1															1995								2.63																				LuNi2B2C			A	3.5327		10.5541												K		9.3					9.3																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111291	PSS1890489		(Y,Gd)Ni2B2C	Y0.78Gd0.22Ni2B2C1	Y	0.78	Gd	0.22	Ni	2	B	2	C	1															1995								4.29																				LuNi2B2C			A	3.5346		10.5471												K		6.64					6.64																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111292	PSS1890489		(Y,Gd)Ni2B2C	Y0.75Gd0.25Ni2B2C1	Y	0.75	Gd	0.25	Ni	2	B	2	C	1															1995																												LuNi2B2C			A	3.5337		10.5224												K		4.84					4.84																																																																																																arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111293	PSS1890489		(Y,Gd)Ni2B2C	Y0.6Gd0.4Ni2B2C1	Y	0.6	Gd	0.4	Ni	2	B	2	C	1															1995								6.36																				LuNi2B2C			A	3.5356		10.5047												K					4.2																																																																																																		arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111294	PSS1890489		(Y,Gd)Ni2B2C	Y0.4Gd0.6Ni2B2C1	Y	0.4	Gd	0.6	Ni	2	B	2	C	1															1995								10.8																				LuNi2B2C			A	3.55		10.4376												K					4.2																																																																																																		arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111295	PSS1890489		(Y,Gd)Ni2B2C	Y0.2Gd0.8Ni2B2C1	Y	0.2	Gd	0.8	Ni	2	B	2	C	1															1995								15.2																				LuNi2B2C			A	3.5596		10.3953												K					4.2																																																																																																		arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111296	PSS1890489		GdNi2B2C	Gd1Ni2B2C1	Gd	1	Ni	2	B	2	C	1																	1995								20																				LuNi2B2C			A	3.5769		10.3706												K					4.2																																																																																																		arc-melting					Pair-breaking and magnetic ordering in the pseudo-quaternary intermetallic series (Y,Gd)Ni2B2C			Rio de Janeiro,Brazil	Phys.stat.sol.(b), 189(1995)489	A.Sulpice,B.Giordanengo,E.M.Baggio-Saitovitch,J.C.Mondragon,M.B.Fontes,M.El Massalami,S.L.Budko		
111297	PHC3840227	RRR=1.6. Anisotropy factor=2. Jc(1.8K,H=0)=30 kA/cm2. delta-C at Tc = 23 mj/mol.K. data from sp-hat.	Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																		1	2003																												AlB2																	AlB2, C32	K		22					22																				T		16												MHC11297																						mj/mol.K2	1.9		685																																					heat(1100C,24h) using (Mg + B4C)					Carbon doping of superconducting magnesium diboride			Ames Lab, Iowa State University, Ames, Iowa,USA	Physica C, 384(2003)227-236	C.Petrovic,P.C.Canfield,R.A.Ribeiro,S.L.Bud'ko		
111298	L087137005	point contact tunneling. two gaps (7meV and 2.8meV)  coexist. 2*delta/kTc = 4.14 and 1.67.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		39.3					39.3																																																4.14	1																																																				Evidence for two superconducting energy gaps in MgB2 by point-contact spectroscopy			Institute of Experimental Physics,Solvac Academy of Sciences,Kosice,Slovakia	Phys.Rev.Lett., 87(2001)137005	A.G.M.Jansen,C.Marcenat,D.Fruchart,J.Kcmarcik,J.Marcus,P.Samuely,P.Szabo,S.Miraglia,T.Klein		
111299	L087047001	sample is MgB<11>2. specific heat measurement under H. e-ph coupling = 0.62. delta-C=133 mj/mol.K at Tc.	MgB2	B2Mg1	B	2	Mg	1																				1	2001																												AlB2																	AlB2, C32	K		38.7					38.7																																																								mj/mol.K2	2.6		1050																																					(B<11>+Mg) - heat(850C, 1.5h, p=50 bar Ar)					Specific heat of MgB<11>2: Evidence for a second energy gap			University of California,Berkeley,California,USA	Phys.Rev.Lett., 87(2001)47001	D.G.Hinks,F.Bouquet,J.D.Jorgensen,N.E.Phillips,R.A.Fisher		
111300	PR05203844	RRR=27. Neel-T by NED. Curie-T is estimated for poly using -82K for H//c and =25K for H//ab.	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	1995							1	10.3																				LuNi2B2C			A	3.534		10.484												K		6.4					6.4																													kG/K		1.2																																																																	Ni2B flux method					Onset of superconductivity in the antiferromagnetically ordered state of single-crystal DyNi2B2C	199508		Ames Laboratory and Department of Physics and Astonomy,lowa State University,Ames,Iowa 50011	Phys.Rev.B,52(1955)R3844	B.K.Cho,D.C.Johnston,P.C.Canfield		
111301	SSC0590839		ZrOsSi	Zr1Os1Si1	Zr	1	Os	1	Si	1																			1986																												TiNiSi			A	6.411	4.041	7.453												K		1.72					1.72																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111302	SSC0590839		ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																			1986																												TiNiSi			A	6.5578	3.9537	7.3762												K		2.04					2.04																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111303	SSC0590839		HfIrSi	Hf1Ir1Si1	Hf	1	Ir	1	Si	1																			1986																												TiNiSi			A	6.471	3.938	7.3763												K		3.5					3.5																																																																																																arc-melting					Relationships between occurrence of superconductivity and crystal structure in new equiatomic ternary silisides MTSi (M=Ti, Zr, Hf and T=Ru, Os, Rh)				Solid State Commun., 59(1986)839	B.Chevalier,J.Etourneau,P.Hagenmuller,W.X.Zhong		
111304	SCI2981213	pressure-induced s/c. Tc(max)=17 K at p=66 GPa (cI16-phase).	Li	Li1	Li	1																							2002																																														K		17			0		17	MTC11304																																																																																																				Superconductivity in dense Lithium				Science,  298(2002)1213	Ho-kwang Mao,M.I.Eremets,R.J.Hemley,V.V.Struzhkin,Wei Gan		
111305	NAT4190597	pressure-induced s/c. Pc = 23 GPa. Tc(fcc,max)=15 K. Tc(cI16-phase)=20 K. Hc2(T) at p=34 GPa.	Li	Li1	Li	1																							2002																																														K		20			0		20																				T		3												MHC11305																																																														Jonson-Mathey Li(99.999%)					Superconductivity in compressed lithium at 20 K			Osaka University	Nature, 419(2002)597	D.Takao,H.Ishikawa,K.Amaya,K.Shimizu,T.Yagi		
111306	NAT4200297	Tc decrease at 0.2 K/month. Hc2(0) by WHH fitting. delta-C/Tc = 110 mj/mol.K2. G-L parameter = 32	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2002																												HoCoGa5			A	4.232		6.786												K		18.5					18.5											Oe		350							T		74							T/K		5.9					A		21			A		1240										MSP11306			mj/mol.K2	77		240																																					(Pu+Co) with excess Ga in alumina, heat(1100C) - cool to 600C(10C/h)					Plutonium-based superconductivity with a transition temperature above 18 K			Los Alamos National Lab, Los Alamos, New Mexico,USA	Nature, 420(2002)297	B.L.Scott,E.Colineau,F.Wastin,G.H.Lander,G.R.Stewart,J.D.Thompson,J.L.Sarrao,J.Reblzant,L.A.Morales,P.Boulet		
111307	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.2Nx	Nb1C0.2N0.64	Nb	1	C	0.2	N	0.64																			1967																																														K		16.3					16.3																				kG		43.7																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111308	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.2Nx	Nb1C0.2N0.7	Nb	1	C	0.2	N	0.7																			1967																																														K		17.2					17.2																				kG		85.6																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111309	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.2Nx	Nb1C0.2N0.74	Nb	1	C	0.2	N	0.74																			1967																																														K		17.5					17.5																				kG		108.8																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111310	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.3Nx	Nb1C0.3N0.57	Nb	1	C	0.3	N	0.57																			1967																																														K		16.4					16.4																				kG		46.5																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111311	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.3Nx	Nb1C0.3N0.62	Nb	1	C	0.3	N	0.62																			1967																																														K		17.3					17.3																				kG		85.6																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111312	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.3Nx	Nb1C0.3N0.64	Nb	1	C	0.3	N	0.64																			1967																																														K		17.8					17.8																				kG		105.1																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111313	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.3Nx	Nb1C0.3N0.7	Nb	1	C	0.3	N	0.7																			1967																																														K		17.7					17.7																				kG		111.6																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111314	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.5Nx	Nb1C0.5N0.36	Nb	1	C	0.5	N	0.36																			1967																																														K		15.6					15.6																				kG		48.4																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111315	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.5Nx	Nb1C0.5N0.42	Nb	1	C	0.5	N	0.42																			1967																																														K		17					17																				kG		80																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111316	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.5Nx	Nb1C0.5N0.47	Nb	1	C	0.5	N	0.47																			1967																																														K		17.4					17.4																				kG		79.1																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111317	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.5Nx	Nb1C0.5N0.5	Nb	1	C	0.5	N	0.5																			1967																																														K		17.9					17.9																				kG		94																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111318	SSC1230001		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.08		3.56											AlB2, C32	K		37					37																																																																																																					Fluoride doping and boron particle size effect on MgB2-xFx superconductor			Department of Chemistry, Faculty of Science, Tanta university, Tanta, Egypt	Solid State Commun., 123(2002)1-6	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111319	SSC1230001		Mg(B,F)2	Mg1B1.96F0.04	Mg	1	B	1.96	F	0.04																			2002																												AlB2			A	3.083		3.67											AlB2, C32	K		30					30																																																																																																mixture(Mg,MgF,B) - sinter(970C)					Fluoride doping and boron particle size effect on MgB2-xFx superconductor			Department of Chemistry, Faculty of Science, Tanta university, Tanta, Egypt	Solid State Commun., 123(2002)1-6	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111320	SSC1230001		Mg(B,F)2	Mg1B1.92F0.08	Mg	1	B	1.92	F	0.08																			2002																												AlB2			A	3.091		3.71											AlB2, C32	K		21					21																																																																																																mixture(Mg,MgF,B) - sinter(970C)					Fluoride doping and boron particle size effect on MgB2-xFx superconductor			Department of Chemistry, Faculty of Science, Tanta university, Tanta, Egypt	Solid State Commun., 123(2002)1-6	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111321	SSC1230001		Mg(B,F)2	Mg1B1.84F0.16	Mg	1	B	1.84	F	0.16																			2002																												AlB2			A	3.093		3.86											AlB2, C32	K		16					16																																																																																																mixture(Mg,MgF,B) - sinter(970C)					Fluoride doping and boron particle size effect on MgB2-xFx superconductor			Department of Chemistry, Faculty of Science, Tanta university, Tanta, Egypt	Solid State Commun., 123(2002)1-6	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111322	SSC1210575	porous(d=0.67 g/cm3).Hc2(0) value by empirical curve fitting.  Hc2(0)=12.5 T by WHH fitting. Hc1(0) by magnetization. G-L parameter = 50	MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.14		3.52											AlB2, C32	K		38.6					38.6											Oe		120							T		15.5												MHC11322		A		46			A		2300																																																					solid state reaction					Thermal fluctuation and upper critical field of MgB2 superconductor			Department of Physics, National Hsing University, Taichung,Taiwan,ROC	Solid State Commun., 121(2002)575	J.J.Cheng,M.D.Lan,P.L.Tsai,Y.L.Chang		
111323	PCS0280333	Hc2(0) means Hc2(4.2K).	NbC0.2Nx	Nb1C0.2N0.8	Nb	1	C	0.2	N	0.8																			1967																																														K		17.6					17.6																				kG		113.5																																																																										NbCx + nitriding under N2 pressure.					Superconductivity of cubic niobium carbo-nitrides			University of California,Berkeley,California,USA	J.Phys.Chem.Solids, 28(1967)333-341	K.M.Ralls,M.R.Pickus,M.W.Williams		
111324	SSC1210497		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2																	AlB2, C32	K		38.14					38.14																																																																																																					Effects of copper doping in MgB2 superconductor			Faenza,Italy	Solid State Commun., 121(2002)497	A.Tampieri,D.Rinaldi,G.Barucca,G.Celotti,R.Caciuffo,S.Sprio		
111325	SSC1210497		(Mg,Cu)B2	Mg0.996Cu0.004B2	Mg	0.996	Cu	0.004	B	2																			2002																												AlB2			A	3.084		3.5215											AlB2, C32	K		38.11					38.11																																																																																																mix(Mg+CuB24) - heat pellet in Ar					Effects of copper doping in MgB2 superconductor			Faenza,Italy	Solid State Commun., 121(2002)497	A.Tampieri,D.Rinaldi,G.Barucca,G.Celotti,R.Caciuffo,S.Sprio		
111326	SSC1210497		(Mg,Cu)B2	Mg0.989Cu0.011B2	Mg	0.989	Cu	0.011	B	2																			2002																												AlB2			A	3.0824		3.52											AlB2, C32	K		38.05					38.05																																																																																																mix(Mg+CuB24) - heat pellet in Ar					Effects of copper doping in MgB2 superconductor			Faenza,Italy	Solid State Commun., 121(2002)497	A.Tampieri,D.Rinaldi,G.Barucca,G.Celotti,R.Caciuffo,S.Sprio		
111327	SSC1210497		(Mg,Cu)B2	Mg0.982Cu0.018B2	Mg	0.982	Cu	0.018	B	2																			2002																												AlB2			A	3.0809		3.519											AlB2, C32	K		37.8					37.8																																																																																																mix(Mg+CuB24) - heat pellet in Ar					Effects of copper doping in MgB2 superconductor			Faenza,Italy	Solid State Commun., 121(2002)497	A.Tampieri,D.Rinaldi,G.Barucca,G.Celotti,R.Caciuffo,S.Sprio		
111328	SSC1210497		(Mg,Cu)B2	Mg0.97Cu0.03B2	Mg	0.97	Cu	0.03	B	2																			2002																												AlB2			A	3.0779		3.5165											AlB2, C32	K		37.58					37.58																																																																																																mix(Mg+CuB24) - heat pellet in Ar					Effects of copper doping in MgB2 superconductor			Faenza,Italy	Solid State Commun., 121(2002)497	A.Tampieri,D.Rinaldi,G.Barucca,G.Celotti,R.Caciuffo,S.Sprio		
111329	P067020506	pressure-induced s/c. incommensulate AF=1.65 K. dTn/dP=-0.76 K/GPa. s/c properties at P=1.63 GPa. gamma in mj/mol-Ce.K2 at P=1.63 GPa. Tc shows Tc(max).	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																			2003								2.8																				Ho2CoGa8			A	4.4665		12.244												K		2			0		2	MPH11329																			kOe		53.6							kOe/K		91.8					A		77																		mj/mol.K2	200																																							excess In flux					Magnetism and superconductivity in Ce2RhIn8			Los Alamos National Lab, Los Alamos, New Mexico,USA	Phys.Rev.B, 67(2003)020506	C.Petrovic,H.A.Borges,J.D.Thompson,J.L.Sarrao,M.Nicklas,P.G.Pagliuso,V.A.Sidorov,Z.Fisk		
111330	P067024519	powder(av. d=2 um). s/c volume fraction=20%. Hc2(0) by WHH.	(NH3)0.72NaK2C60	N0.72H2.16Na1K3C60	N	0.72	H	2.16	Na	1	K	3	C	60															2003																												fullerene																		K		12					12											Oe		0.87							T		40							T/K		5					A		28.6			um		1.4																																																					After intercalation, NH3 was evaporated. Then ANN(100C,10d)					Muon spin rotation and SQUID investigation of superconductivity in (NH3)xNaK2C60 (x=0.7)			Universita di Parma, Parma,Italy	Phys.Rev.B, 67(2003)024519	C.Bucci,E.Zannoni,F.Barbieri,F.Bolzoni,M.Ricco,T.Shiroka		
111331	L090027001	gap by NMR	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2003																																														K		1.85					1.85																																																5.2																																																Sb-flux method					Evidence for unconventional strong-coupling superconductivity in PrOs4Sb12: An Sb nuclear quadrupole resonance study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.Lett., 90(2003)27001	G.-q.Zheng,H.Kotegawa,H.Sato,H.Sugawara,M.Yogi,S.Ohsaki,Y.Aoki,Y.Imamura,Y.Kawasaki,Y.Kitaoka		
111332	L090027001	gap by NMR. conventional s-wave s/c.	LaOs4Sb12	La1Os4Sb12	La	1	Os	4	Sb	12																			2003																																														K		0.75					0.75																																																3.2																																																Sb-flux method					Evidence for unconventional strong-coupling superconductivity in PrOs4Sb12: An Sb nuclear quadrupole resonance study			Osaka University, Toyonaka,Osaka,Japan	Phys.Rev.Lett., 90(2003)27001	G.-q.Zheng,H.Kotegawa,H.Sato,H.Sugawara,M.Yogi,S.Ohsaki,Y.Aoki,Y.Imamura,Y.Kawasaki,Y.Kitaoka		
111333	L090057001	scutterudite. H//principal axis. sample has twoTc, second Tc = 1.75 K. delta-C/gamma*Tc = 3.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2003																																														K		1.85					1.85																				T		2.1																															MSP11333			mj/mol.K2	313		165																																					Sb-flux method					Low-temperature specific heat of the heavy-fermion superconductor PrOs4Sb12			Universitat Karlsruhe, Karlsruhe,Germany	Phys.Rev.Lett., 90(2003)57001	A.Faisst,C.Pfleiderer,E.D.Bauer,H.v.Lohneysen,M.B.Maple,P.-C.Ho,R.Vollmer,V.Zapf		
111334	PR05200483	pressure-induced s/c. Tc=28 K at P=14.8 kbar. shielding = 5 %.	K3(NH3)C60	K3N1H3C60	K	3	N	1	H	3	C	60																	1995																												fullerene																		K		28			0		28																																																																																																exposing K3C60 to NH3					Structural and electronic Propeerties of(NH3)xK3C60	199507		AT&T bell Lavoratories,600 Mountain Avenue,Murray Hill,New Jersey	Phys.Rev.B,52(1995)483	A.F.Hebaed,B.R.Zegarski,D.W.Murphy,O.Zhou,P.E.Sulewski,R.M.Fleming,T.T.M.Palstra,Y.Iwasa		
111335	NAT3980047	epitaxial thin film on LaAlO3(111). gap(T=0 K)=0.235 meV by tunneling.	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			1999								12																																						K		1.6					1.6																																																3.41	1																																															Thin film by MBE					Superconductivity mediated by spin fluctuations in the heavy-fermion compound UPd2Al3			Institute of Physics,Johannes Gutenberg-University, Staudingerweg,Mainz,Germany	Nature, 398(1999)47	H.Adrian,M.Huth,M.Jourdan		
111336	P067094502	s/c properties estimated from Hc2, sp-heat, tunneling measurements. Hc(0)=0.19 T. delta-C/gamma*Tc = 2.1. G-L parameter = 54	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2003																																														K		7.63					7.63											mT		10							T		14.4														A		46			A		2480					4.6	1				MSP11336			mj/mol.K2	30.1		284																																					solid state reaction					Experimental determination of superconducting parameters for the intermetallic perovskite superconductor MgCNi3			Department of Physics,The Pennsylvania State University,Pennsylvania,USA	Phys.Rev.B., 67(2003)094502	I.G.Deac,K.A.Regan,K.D.Nelson,K.Wu,M.M.Rosario,P.Schiffer,R.J.Cava,T.He,Y.Liu,Z.Q.Mao		
111337	NAT3900382	pressure-induced s/c. Pc=10 GPa<s/c state <157 GPa. value of dTc/dP = 0.055 K/GPa  at 10 K.	Li	Li1	Li	1																							1997																																														K		14			0		14			K/GPa	0.055																																																																																																	Superconductivity at 10 - 17 K in compressed sulphur			Carnegie Institution of Washington, Washington DC,USA	Nature, 390(1997)382	Ho-Kwang Mao,R.J.Hemley,V.V.Struzhkin,Y.A.Timofeev		
111338	P067094501	nominal composition (La:Ge = 1:8). space group= I/mmm	LaGe5	Ge5La1	Ge	5	La	1																				3	2003																															A	4.029	6.307	9.978											orthorhombic	K		7					7																																																																																																high-pressure synthesis (1200C,30 min, 5 GPa)					High-pressure synthesis and superconductivity of LaGe5 containing a tunnel germanium network			Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Phys.Rev.B., 67(2003)094501	H.Fukuoka,S.Yamanaka		
111339	L090117001	single crystal(0.40*0.37*2.20 mm). c-axis thermal conductivity k<zz> measured by steady state method.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2003																												skutterudite																		K		1.82					1.82																				T		2.2																																											MTHC11339																															Sb-flux method					Multiple Superconducting Phases in New Heavy Fermion Superconductor PrOs4Sb12			Institute for Solid State Physics, University of Tokyo, Kashiwanoha 5-1-5, Kashiwa, Chiba , Japan	Phys.Rev.Lett., 90(2003)117001	H.Sato,H.Sugawara,J.Goryo,K.Izawa,K.Maki,P.Thalmeier,S.Osaki,Y.Matsuda,Y.Nakajima		
111340	P067094504	RRR=3.6-4.1. multiple gaps observed by tunneling. table value shows the largest gap. The smallest is 2*delta/k*Tc = 1.2	MgB2	B2Mg1	B	2	Mg	1																				1	2003																												AlB2																	AlB2, C32	K		39.2					39.2																																																5	1																																															heat(973 K,200 atm-Ar) + ANN(1623 K, 5.5 GPa)					Tunneling spectroscopy of the superconducting gap in MgB2			Hiroshima University, Higashi-Hiroshima, Japan	Phys.Rev.B., 67(2003)094504	H.Fujii,J.Akimitsu,T.Ekino,T.Muranaka,T.Takasaki		
111341	L087257601	C<13> enriched sample. gap from NMR.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2001																																														K		7					7																																																3.2	6																																																				<13>C NMR investigation of the superconductor MgCNi3 up to 800 K			MIT, Cambridge, Massachusetts, USA	Phys.Rev.Lett., 87(2001)257601	M.A.Hayward,P.M.Singer,R.J.Cava,T.He,T.Imai		
111342	MRB0351743	electron doped s/c.	HxLiNbO2	H0.3Li1Nb1O2	H	0.3	Li	1	Nb	1	O	2																	2000																															A	2.922		10.48												K		5.5					5.5																																																																																																H-spill over method. insertion in H2PtCl6.6H2O ethanol solution					Superconductivity of hydrogen inserted LiNbO2			Yamanashi University,Kofu,Japan	Mater.Res.Bull., 35(2000)1743	I.Tanaka,N.Kinomura,N.Kumada,S.Watauchi		
111343	MRB0351743	electron doped s/c.	HxLiNbO2	H0.5Li1Nb1O2	H	0.5	Li	1	Nb	1	O	2																	2000																															A	2.923		10.46												K		5.5					5.5																																																																																																H-spill over method. insertion in H2PtCl6.6H2O ethanol solution					Superconductivity of hydrogen inserted LiNbO2			Yamanashi University,Kofu,Japan	Mater.Res.Bull., 35(2000)1743	I.Tanaka,N.Kinomura,N.Kumada,S.Watauchi		
111344	P067064505	density=2.4 g/cm3. using crystalline B(-325 mesh). RRR=7.1. Debye-T obtained by fitting of n-state thermal conductivity.	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2																	AlB2, C32	K		38.9					38.9																																																											1130						MTHC11344																															Ta-tube, heat(950C)					Thermal conductivity of MgB2 in the superconducting state			Genova,Italy	Phys.Rev.B., 67(2003)064505	A.Palenzona,A.S.Siri,E.Galleani d'Agliano,F.Napoli,I.Pallecchi,M.Putti,P.Manfrinetti,V.Braccini		
111345	P067064505	using enriched crystalline B<11> (-325 mesh). RRR=15.3. Debye-T obtained by fitting of n-state thermal conductivity.	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2																	AlB2, C32	K		38.7					38.7																																																											1190						MTHC11345																															Ta-tube, heat(950C)					Thermal conductivity of MgB2 in the superconducting state			Genova,Italy	Phys.Rev.B., 67(2003)064505	A.Palenzona,A.S.Siri,E.Galleani d'Agliano,F.Napoli,I.Pallecchi,M.Putti,P.Manfrinetti,V.Braccini		
111346	JAP0917125		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.086		3.524											AlB2, C32	K		39					39																																																																																																SIN(950C,2h)					Superconductivity of Mg(B1-xCx)2 ternary compounds			Beijing,China	J.Appl.Phys., 91(2002)7125	Bao-gen Shen,Hong-wu Zhao,Jian Zhang,Shao-ying Ahang,Tong-yun Zhao,Zhao-hua Cheng		
111347	JAP0917125		Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2002																												AlB2																	AlB2, C32	K		37					37																																																																																																SIN(950C,2h)					Superconductivity of Mg(B1-xCx)2 ternary compounds			Beijing,China	J.Appl.Phys., 91(2002)7125	Bao-gen Shen,Hong-wu Zhao,Jian Zhang,Shao-ying Ahang,Tong-yun Zhao,Zhao-hua Cheng		
111348	JAP0917125	Hc1, Jc not explicitly given	Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																			2002																												AlB2			A	3.07		3.524											AlB2, C32	K		34					34																																																																																																SIN(950C,2h)					Superconductivity of Mg(B1-xCx)2 ternary compounds			Beijing,China	J.Appl.Phys., 91(2002)7125	Bao-gen Shen,Hong-wu Zhao,Jian Zhang,Shao-ying Ahang,Tong-yun Zhao,Zhao-hua Cheng		
111349	EPL0580885	bulk. not s/c. kai-zero=2.96E-4. mag. impurity=11 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.923														K																																																															mj/mol.K2	6.44		239																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111350	EPL0580885	Hc2(0) =<0.07 mT. ave.grain=4.2 micron.m.  kai-zero=3.25E-4. mag. impurity=3 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.923														K		0.0019					0.0019																																																								mj/mol.K2	6.42		234																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111351	EPL0580885	ave.grain=1.3 micron.m. Hc2(0) =<0.07 mT.  kai-zero=2.96E-4. mag. impurity=4 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.923														K		0.0019					0.0019																																																								mj/mol.K2	6.48		240																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111352	EPL0580885	ave.grain=0.27 micron.m.   kai-zero=2.11E-4. mag. impurity=17 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.917														K		0.02					0.02																				T		0.018																																		mj/mol.K2	5.77		210																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111353	EPL0580885	ave.grain=0.19 micron.m.  not s/c. kai-zero=2.39E-4. mag. impurity=49 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.919														K																																																															mj/mol.K2	6.14		207																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111354	EPL0580885	ave grain=0.11 micron.m.  not s/c. kai-zero=2.52E-4. mag. impurity=143 ppm. gamma=in mj/mol.K2	Pt	Pt1	Pt	1																							2002																															A	3.919														K																																																															mj/mol.K2	6.24		206																																										Tc-enhancement in superconducting granular platinum			Physikalisches Institut, Universitat Bayreuth, Bayreuth, Germany	Europhys.Lett., 58(2002)885	A.Schindler,D.Gunther,G.Eska,H.F.Braun,M.Meissner,M.Mertig,R.Konig,R.Wahl,T.Herrmannsdorfer,W.Pompe		
111355	JAP0917122		MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2																	AlB2, C32	K		37.6					37.6																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111356	JAP0917122		(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																			2002																												AlB2																	AlB2, C32	K		36.1					36.1																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111357	JAP0917122		(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2002																												AlB2																	AlB2, C32	K		29.6					29.6																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111358	JAP0917122		(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																			2002																												AlB2																	AlB2, C32	K		22.1					22.1																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111359	JAP0917122		(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																			2002																												AlB2																	AlB2, C32	K		12.2					12.2																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111360	JAP0917122		(Mg,Al)B2	Mg0.4Al0.6B2	Mg	0.4	Al	0.6	B	2																			2002																												AlB2																	AlB2, C32	K		5.85					5.85																																																																																																SIN(600C,1h + 800C,1h + 900C,1h)					Study of Al doping effect on superconductivity of Mg1-xAlxB2			National Lab of Solid State Microstructures, Department of Physics, Nanjing University, Nanjing, China	J.Appl.Phys., 91(2002)7122	C.M.Li,H.Luo,H.M.Luo,S.Y.Ding		
111361	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.24Pd0.76B2C1	Y	1	Ni	1.24	Pd	0.76	B	2	C	1														1	2002																												LuNi2B2C			A	3.6509		10.6893												K		10.4					10.4																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111362	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.34Pd0.66B2C1	Y	1	Ni	1.34	Pd	0.66	B	2	C	1														1	2002																												LuNi2B2C			A	3.6379		10.6857												K		10.4					10.4																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111363	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.4Pd0.6B2C1	Y	1	Ni	1.4	Pd	0.6	B	2	C	1														1	2002																												LuNi2B2C			A	3.6117		10.6655												K		9.92					9.92																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111364	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.46Pd0.54B2C1	Y	1	Ni	1.46	Pd	0.54	B	2	C	1														1	2002																												LuNi2B2C			A	3.5921		10.6488												K		10.1					10.1																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111365	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.54Pd0.46B2C1	Y	1	Ni	1.54	Pd	0.46	B	2	C	1														1	2002																												LuNi2B2C																		K		10.3					10.3																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111366	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.7Pd0.3B2C1	Y	1	Ni	1.7	Pd	0.3	B	2	C	1														1	2002																												LuNi2B2C			A	3.5537		10.5976												K		10.7					10.7																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111367	MLT0570059		Y(Ni,Pd)2B2C	Y1Ni1.82Pd0.18B2C1	Y	1	Ni	1.82	Pd	0.18	B	2	C	1														1	2002																												LuNi2B2C			A	3.5416		10.5726												K		11.8					11.8																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111368	MLT0570059		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	2002																												LuNi2B2C			A	3.5276		10.5429												K		15					15																																																																																																arc-melting + ANN(1300C)					Constitution and superconductivity of Y(Ni1-xPdx)2B2C alloys			Institut fur Festkorper-und Werkstoffororschung Dresden, Dresden,Germany	Materials Lett., 57(2002)59	G.Behr,H.Bitterlich,W.Loser		
111369	PHC3900191	RRR=2 - 3. Thermopower, thermal conductivity were measured (Fig.).	MgB2	B2Mg1	B	2	Mg	1																				1	2003																												AlB2			A	3.14		3.52											AlB2, C32	K		39					39																																																																						MTP11369																										solid state reaction (700C,1h)					Studies of transport properties of MgB2 superconductor			Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Kolkata 700 064, India	Physica C, 390(2003)191	A. Poddar,B. Bandyopadhyay,B. Ghosh,D. Bhattacharya,P. Choudhury,P. Mandal,U. Sinha		
111370	P067180501	gap by NMR. typical weak-coupling s-wave s/c.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																			2003																												skutterudite																		K		1.3					1.3																																																3.1	6																																															Sb-flux method					Sb-NQR probe for superconducting properties in the Pr-based filled-skutterudite compound PrRu4Sb12			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 67(2003)180501	G.-q.Zheng,H.Kotegawa,H.Sato,H.Sugawara,M.Yogi,Y.Imamura,Y.Kitaoka		
111371	P067180501	gap by NMR. typical weak-coupling s-wave s/c.	LaRu4Sb12	La1Ru4Sb12	La	1	Ru	4	Sb	12																			2003																												skutterudite																		K		3.5					3.5																																																3.6	6																																															Sb-flux method					Sb-NQR probe for superconducting properties in the Pr-based filled-skutterudite compound PrRu4Sb12			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 67(2003)180501	G.-q.Zheng,H.Kotegawa,H.Sato,H.Sugawara,M.Yogi,Y.Imamura,Y.Kitaoka		
111372	P067180508	Hc1 from M-H curve. Authors say Hc1(0) is underestimation, then G-L parameter(= 31) overestimation. H//[001] direction.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2003																												skutterudite																		K		1.85					1.85											Oe		23																																																																																			Sb-flux method					High-field ordered and superconducting phases in the heavy-fermion compound PrOs4Sb12			University of California, San Diego, La Jolla, California,USA	Phys.Rev.B, 67(2003)180508	A.D.Christianson,A.H.Lacerda,E.D.Bauer,M.B.Maple,N.A.Frederick,P.-C.Ho,T.D.Do,V.S.Zapf		
111373	P067172508	amorphous films. alpha-MgxB1-x films.	Mg-B film	B0.67Mg0.33	B	0.67	Mg	0.33																				3	2003																																														K		6.1					6.1	MTC11373																			T		3.3																																																																										co-evaporation of Mg and B by e-gun on glass.					Observation of superconductivity in thick amorphous MgxB1-x films			Research Center for Low Temperature Physics, Tokyo Institute of Technology, Ohokayama, Meguro-ku, Tokyo, Japan	Phys.Rev.B, 67(2003)172508	K.Amemori,S.Okuma,S.Togo		
111374	P067212504	pressure-induced s/c. Pc = 2 kbar. values of s/c properties are at P = 5 kbar. At ambient pressure, sort-range ferro- (Tm=6 K) and AF (Tn=4.3 K)	CeTe2	Ce1Te1.82	Ce	1	Te	1.82																				3	2003								4.3																				Cu2Sb																		K		2.7			0		2.7																																		MHC11374																																																																			Superconductivity in magnetically ordered CeTe1.82			National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico, USA	Phys.Rev.B, 67(2003)212504	A.Alsmadi,A.H.Lacerda,H.C.Kim,H.C.Ri,H.Nakotte,K.H.Ahn,K.Umeo,M.H.Jung,T.Takabatake,Yunkyu Bang		
111375	PHC3660001	impurity phase = MgO	MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2			A	3.0872		3.5207											AlB2, C32	K		38.3					38.3																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111376	PHC3660001	impurity phase = MgB4	MgxB2	B2Mg0.9	B	2	Mg	0.9																					2001																												AlB2			A	3.0837		3.5219											AlB2, C32	K		38.2					38.2																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111377	PHC3660001	impurity phase = MgB4	MgxB2	B2Mg0.8	B	2	Mg	0.8																					2001																												AlB2			A	3.0818		3.5268											AlB2, C32	K		38					38																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111378	PHC3660001	impurity phase = MgB4	MgxB2	B2Mg0.7	B	2	Mg	0.7																					2001																												AlB2			A	3.0845		3.532											AlB2, C32	K		37.2					37.2																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111379	PHC3660001	impurity phase = MgB4	MgxB2	B2Mg0.6	B	2	Mg	0.6																					2001																												AlB2			A	3.0753		3.5283											AlB2, C32	K		36.9					36.9																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111380	PHC3660001	impurity phase = MgB4	MgxB2	B2Mg0.5	B	2	Mg	0.5																					2001																												AlB2			A	3.0762		3.531											AlB2, C32	K		36					36																																																																																																solid state reaction					Influence of the starting composition Mg1-xB2 on the structural and superconducting properties of the MgB2 phase			Department of Physics, Tsinghua University, Beijing, China	Physica C, 366(2001)1	B.L.Gu,B.S.Cao,H.T.Zhang,M.H.Zhu,P.T.Qiao,S.L.Jia,X.L.Wang,X.P.Zhang,Y.G.Zhao,Z.H.Han		
111381	SSC1190001		MgB2	B2Mg1	B	2	Mg	1																					2001																												AlB2																	AlB2, C32	K		38.6					38.6																																																																																																solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111382	SSC1190001		(Mg,Zn)B2	Mg0.95Zn0.05B2	Mg	0.95	Zn	0.05	B	2																			2001																												AlB2																	AlB2, C32	K		38.3					38.3																																																																																																solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111383	SSC1190001		(Mg,Zn)B2	Mg0.9Zn0.1B2	Mg	0.9	Zn	0.1	B	2																			2001																												AlB2																	AlB2, C32	K		38.4					38.4			K/GPa	-1.5																																																																																												solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111384	SSC1190001		(Mg,Zn)B2	Mg0.8Zn0.2B2	Mg	0.8	Zn	0.2	B	2																			2001																												AlB2																	AlB2, C32	K		38.4					38.4																																																																																																solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111385	SSC1190001	composition = nominal values. multi-phase sample. Cu does not substitute for Mg.	(Mg,Cu)B2	Mg0.9Cu0.1B2	Mg	0.9	Cu	0.1	B	2																			2001																												AlB2																	AlB2, C32	K		38.6					38.6																																																																																																solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111386	SSC1190001	composition = nominal values. multi-phase sample. Cu does not substitute for Mg.	(Mg,Cu)B2	Mg0.8Cu0.2B2	Mg	0.8	Cu	0.2	B	2																			2001																												AlB2																	AlB2, C32	K		38.6					38.6																																																																																																solid state reaction (600,800,900C, in V-container)					Substitution effect of Zn and Cu in MgB2 on Tc and structure			Solid State Physics Lab, ETH, Zurich, Switzerland	Solid State Commun., 119(2001)1	I.M.Fita,J.Karpinski,M.Angst,R.Puzniak,S.M.Kazakov		
111387	MAT0301025	major phase=Mg(B,C)2 73.4 wt %. impurity phases = MgB2C2, Mg, MgO. compositions determined by NED.	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2003																												AlB2			A	3.0529		3.5253											AlB2, C32	K		22					22																																																																																																(Mg, B4C) - heat(1200C,24h) in Ta crucible					Crystal Chemistry of Carbon-Substituted MgB2			Materials Science Division, Argonne National Laboratory, Argonne, IL 60439 USA	cond-mat/0301025(2003)	J.D.Jorgensen,M.Avdeev,P.C.Canfield,R.A.Ribeiro,S.L.Bud'ko		
111388	PHC3900185		MgB2	B2Mg1	B	2	Mg	1																				1	2003																												AlB2			A	3.0869		3.5238											AlB2, C32	K		38.3					38.3																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111389	PHC3900185	nominal C-composition. Jc(H), Hirr(T) were measured.	Mg(B,C)2	Mg1B1.95C0.05	Mg	1	B	1.95	C	0.05																		1	2003																												AlB2			A	3.0841		3.5248											AlB2, C32	K		38					38																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111390	PHC3900185	nominal C-composition. Jc(H), Hirr(T) were measured.	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		1	2003																												AlB2			A	3.082		3.5233											AlB2, C32	K		37.3					37.3																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111391	PHC3900185	nominal C-composition. Jc(H), Hirr(T) were measured.	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		1	2003																												AlB2			A	3.0796		3.5237											AlB2, C32	K		36.8					36.8																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111392	PHC3900185	nominal C-composition. Jc(H), Hirr(T) were measured.	Mg(B,C)2	Mg1B1.7C0.3	Mg	1	B	1.7	C	0.3																		1	2003																												AlB2			A	3.0788		3.5218											AlB2, C32	K		36.4					36.4																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111393	PHC3900185	nominal C-composition. Jc(H), Hirr(T) were measured.	Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																		1	2003																												AlB2			A	3.076		3.5243											AlB2, C32	K		35.8					35.8																																																																																																(Mg,a-B,nano-C) - heat(770C,in Fe tube) in Ar					Effect of nano-carbon particle doping on the flux pinning properties of MgB2 superconductor			Institute for Superconducting and Electronic Materials, ISEM, University of Wollongong, Wollongong, Australia	Physica C, 390(2003)185	J.Horvat,P.Munroe,S.Soltanian,S.X.Dou,X.L.Wang		
111394	PHC3700211	impurity phase = MgO<1 %. Debye-T calculated from R(T). e-ph coupling const. = 0.847	MgB2	B2Mg1	B	2	Mg	1																					2002																												AlB2			A	3.0848		3.5224											AlB2, C32	K		39.1					39.1																																																											898.5																																					(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111395	PHC3700211		Mg(B,C)2	Mg1B1.98C0.02	Mg	1	B	1.98	C	0.02																			2002																												AlB2			A	3.0813		3.5224											AlB2, C32	K		38.4					38.4																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111396	PHC3700211		Mg(B,C)2	Mg1B1.96C0.04	Mg	1	B	1.96	C	0.04																			2002																												AlB2			A	3.0805		3.525											AlB2, C32	K		38.4					38.4																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111397	PHC3700211		Mg(B,C)2	Mg1B1.94C0.06	Mg	1	B	1.94	C	0.06																			2002																												AlB2			A	3.0782		3.5226											AlB2, C32	K		37.8					37.8																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111398	PHC3700211	Debye-T calculated from R(T). e-ph coupling const. = 0.878	Mg(B,C)2	Mg1B1.92C0.08	Mg	1	B	1.92	C	0.08																			2002																												AlB2			A	3.0751		3.5229											AlB2, C32	K		38.3					38.3																																																											823.3																																					(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111399	PHC3700211		Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																			2002																												AlB2			A	3.073		3.5245											AlB2, C32	K		36.2					36.2																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111400	PHC3700211	Debye-T calculated from R(T). e-ph coupling const. = 0.892	Mg(B,C)2	Mg1B1.85C0.15	Mg	1	B	1.85	C	0.15																			2002																												AlB2			A	3.0686		3.5214											AlB2, C32	K		36.3					36.3																																																											760.1																																					(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111401	PHC3700211		Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2002																												AlB2			A	3.0664		3.525											AlB2, C32	K		34.2					34.2																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111402	PHC3700211		Mg(B,C)2	Mg1B1.75C0.25	Mg	1	B	1.75	C	0.25																			2002																												AlB2			A	3.0597		3.5258											AlB2, C32	K		30					30																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111403	PHC3700211		Mg(B,C)2	Mg1B1.7C0.3	Mg	1	B	1.7	C	0.3																			2002																												AlB2			A	3.0541		3.5196											AlB2, C32	K		29.2					29.2																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111404	PHC3700211		Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																			2002																												AlB2			A	3.0504		3.5189											AlB2, C32	K		24.9					24.9																																																																																																(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111405	PHC3700211	Debye-T calculated from R(T). e-ph coupling const. = 0.912	Mg(B,C)2	Mg1B1.5C0.5	Mg	1	B	1.5	C	0.5																			2002																												AlB2			A	3.0498		3.5181											AlB2, C32	K		26.2					26.2																																																											527.1																																					(Mg,B,C) in Ta crucible, heat(900C, 1.5h, 50 bar-Ar)					Carbon solubility and superconductivity in MgB2			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Physica C, 370(2002)211	A.Bharathi,G.L.N.Reddy,S.Jemima Balaselvi,S.Kalavathi,T.S.Radhakrishnan,V.Sankara Sastry,Y.Hariharan		
111406	P067012505	Hc2(0) is for H//c. cohere=cohere<ab>. anisotropy factor increases from 2(at Tc) to 4.5 (22K). precise phase diagram obtained. sp-heat also measured.	MgB2	B2Mg1	B	2	Mg	1																				3	2003																												AlB2																	AlB2, C32	K		36					36																				T		3.5														A		94																																																										heat treatment under high-pressure					Superconducting transition and phase diagram of single-crystal MgB2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439	Phys.Rev.B, 67(2003)12505	A.Rydh,B.Kang,C.U.Jung,Ch.Marcenat,G.Karapetrov,G.W.Crabtree,H.-S.Lee,J.Marcus,K.H.P.Kim,L.Paulius,S.-I.Lee,T.Klein,U.Welp,W.K.Kwok		
111407	PHB3280023	THF=C4H8O, y-value is not given explicitly. gap (2*delta/kTc = 5 - 6) from tunneling.	Li0.5(THF)yHfNCl	Li0.5Hf1N1Cl1	Li	0.5	Hf	1	N	1	Cl	1																	2003																																														K		26					26																																																5	1																																															(Hf powder+NH4Cl) - 650C, then Li in THF					Tunneling spectroscopy of MgB2 and Li0.5(THF)yHfNCl			Faculty of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Physica B, 328(2003)23	H.Fujii,J.Akimitsu,S.Yamanaka,T.Ekino,T.Muranaka,T.Takasaki		
111408	PHB3280023	gap (2*delta/kTc = 5 - 6) from tunneling.	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2																	AlB2, C32	K		39					39																																																5	1																																																				Tunneling spectroscopy of MgB2 and Li0.5(THF)yHfNCl			Faculty of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Physica B, 328(2003)23	H.Fujii,J.Akimitsu,S.Yamanaka,T.Ekino,T.Muranaka,T.Takasaki		
111409	PHC3570329	Mo-Mo distance = 2.565 A	Mo3P	Mo3P1	Mo	3	P	1																					2001																																														K		7					7																																																																																																high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111410	PHC3570329	Mo-Mo distance = 2.900 A	Mo8P5	Mo8P5	Mo	8	P	5																					2001																																														K		5.8					5.8																																																																																																high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111411	PHC3570329	Mo-Mo distance = 2.839 A	Mo4P3	Mo4P3	Mo	4	P	3																					2001																																														K		3					3																																																																																																high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111412	PHC3570329	Mo-Mo distance = 3.191 A	MoP	Mo1P1	Mo	1	P	1																					2001																																														K					2																																																																																																		high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111413	PHC3570329	Mo-Mo distance = 3.006 A	MoRuP	Mo1Ru1P1	Mo	1	Ru	1	P	1																			2001																												Co2P																		K		15.5					15.5																																																																																																high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111414	PHC3570329	Mo-Mo distance = 3.0059 A	MoNiP	Mo1Ni1P1	Mo	1	Ni	1	P	1																			2001																												Fe2P																		K		15.5					15.5																																																																																																high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111415	PHC3570329	Mo-Mo distance = 3.329 A	MoNiP2	Mo1Ni1P2	Mo	1	Ni	1	P	2																			2001																																														K					2																																																																																																		high-pressure synthesis(4GPa, 1200-1700C)					Superconductivity of binary and ternary molybdenum phosphides prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi, Hokkaido,Japan	Physica C, 357-360(2001)329	C.Sekine,I.Kaneko,I.Shirotani,M.Takaya,T.Yagi		
111416	PRL0500064	Tc=0.325 mK. impurities=Si(30), Ir(25), Fe(15), S(4), Ru(15), Ni(2), Cu(500), Cr(1 ppm). RRR=450, type-I s/c.	Rh	Rh1	Rh	1																							1983																																														K		0.000325					0.000325																				micro-T		4.9														mm		0.06																																																										ANN(1750 C)					Superconductivity of rhodium at ultralow temperature			Institut fur Festkorperforshung, Jurich, West Germany	Phys.Rev.Lett., 50(1983)66	Ch.Buchal,F.Pobell,J.R.Owers-Bradley,M.Kubota,R.M.Mueller		
111417	PRL0852573	single crystal. RRR=740. NMR measurements.	Rh	Rh1	Rh	1																						3	2000																																														K		0.00021					0.00021																				micro-T		3.4																																																																															Relaxation of polarized nuclei in superconducting rhodium			Helsinki University of Technology, Finland	Phys.Rev.Lett., 85(2000)2573	J.T.Tuoriniemi,K.Lefmann,T.A.Knuuttila		
111418	PRL0824528	Tc=1.38 mK. average grain size=2 micron-m. packing fraction = 0.50.	Pt	Pt1	Pt	1																							1999																																														K		0.00138					0.00138																																		MHC11418																																																																			Superconductivity of compacted platinum powder at very low temperatures			Universitat Bayreuth, Bayreuth, Germany	Phys.Rev.Lett., 82(1999)4528	A.Schindler,R.Konig,T.Herrmannsdorfer		
111419	PRL0824528	Tc = 1.04 mK. average grain size=2 micron-m. packing fraction = 0.67.	Pt	Pt1	Pt	1																							1999																																														K		0.00104					0.00104																																		MHC11419																																																																			Superconductivity of compacted platinum powder at very low temperatures			Universitat Bayreuth, Bayreuth, Germany	Phys.Rev.Lett., 82(1999)4528	A.Schindler,R.Konig,T.Herrmannsdorfer		
111420	PRL0824528	Tc = 0.62 mK. average grain size=2 micron-m. packing fraction = 0.80.	Pt	Pt1	Pt	1																							1999																																														K		0.00062					0.00062																																		MHC11420																																																																			Superconductivity of compacted platinum powder at very low temperatures			Universitat Bayreuth, Bayreuth, Germany	Phys.Rev.Lett., 82(1999)4528	A.Schindler,R.Konig,T.Herrmannsdorfer		
111421	JAC2130148	dhcp. Tc < 1.3 K at ambient pressure. Tc=0.79 K from onother paper.  dTc/dP estimated from Tc=0.79 K at ambient pressure and Tc(p=2GPa)) = 1.6 K.	Am	Am1	Am	1																						1	1994																															A	3.467		11.24											dhcp	K		0.79			1.3		0.79	MTC11421		K/GPa	0.45																																																																																												vapor deposition  + ANN					Resistivity and superconductivity of americium metal under pressure up to 25 GPa				J.Alloys Compd, 213/214(1994)148	D.Braithwaite,J.Wittig,P.Link,R.G.Haire,U.Benedict		
111422	JAC2130148	fcc. Tc <1.3 K at ambient  pressure. Tc=0.79 K from onother paper. Tc(max) = 1.83 K (P=4.7 GPa)	Am	Am1	Am	1																						1	1994																															A	4.849													fcc	K		0.79			1.3		0.79	MTC11422																																																																																															vapor deposition  + ANN					Resistivity and superconductivity of americium metal under pressure up to 25 GPa				J.Alloys Compd, 213/214(1994)148	D.Braithwaite,J.Wittig,P.Link,R.G.Haire,U.Benedict		
111423	SSC0420043	Tc < 38 micro-K.	Au	Au1	Au	1																							1982																																														K					0.000038																																																																																																							Superconductivity investigations of Au-In alloys and Au at ultralow temperatures			Kernforschungsanlage Julich, Julich, West Germany	Solid State Commun., 42(1982)43	Ch.Buchal,F.Pobell,H.R.Folle,M.Kubota,R.M.Mueller		
111424	SSC0420043	Tc < 55 micro-K.	Au1-xInx	Au0.99In0.01	Au	0.99	In	0.01																					1982																																														K					0.000055																																																																																																							Superconductivity investigations of Au-In alloys and Au at ultralow temperatures			Kernforschungsanlage Julich, Julich, West Germany	Solid State Commun., 42(1982)43	Ch.Buchal,F.Pobell,H.R.Folle,M.Kubota,R.M.Mueller		
111425	SSC0420043	gap estimated from critical field data.	Au1-xInx	Au0.978In0.022	Au	0.978	In	0.022																					1982																																														K		0.0005					0.0005											micro-T		1.5							micro-T		2.8																										3.8																																																					Superconductivity investigations of Au-In alloys and Au at ultralow temperatures			Kernforschungsanlage Julich, Julich, West Germany	Solid State Commun., 42(1982)43	Ch.Buchal,F.Pobell,H.R.Folle,M.Kubota,R.M.Mueller		
111426	SSC0420043		Au1-xInx	Au0.915In0.085	Au	0.915	In	0.085																					1982																																														K		0.031					0.031																																																																																																					Superconductivity investigations of Au-In alloys and Au at ultralow temperatures			Kernforschungsanlage Julich, Julich, West Germany	Solid State Commun., 42(1982)43	Ch.Buchal,F.Pobell,H.R.Folle,M.Kubota,R.M.Mueller		
111427	SSC0420043		Au1-xInx	Au0.9In0.1	Au	0.9	In	0.1																					1982																																														K		0.077					0.077																																																																																																					Superconductivity investigations of Au-In alloys and Au at ultralow temperatures			Kernforschungsanlage Julich, Julich, West Germany	Solid State Commun., 42(1982)43	Ch.Buchal,F.Pobell,H.R.Folle,M.Kubota,R.M.Mueller		
111428	PRL0160101		W	W1	W	1																							1966																																														K		0.016					0.016																																																																																																					Superconductivity of Tungsten				Phys.Rev.Lett., 16(1966)101	J.C.Wheatley,O.E.Vilches,R.T.Johnson		
111429	SSC0180139		Ag-Ga	Ag0.9Ga0.1	Ag	0.9	Ga	0.1																					1976																																														K		0.0065					0.0065																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111430	SSC0180139		Au-In	Au0.94In0.06	Au	0.94	In	0.06																					1976																																														K		0.0111					0.0111																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111431	SSC0180139		Au-In	Au0.93In0.07	Au	0.93	In	0.07																					1976																																														K		0.0164					0.0164																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111432	SSC0180139		Au-In	Au0.92In0.08	Au	0.92	In	0.08																					1976																																														K		0.0256					0.0256																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111433	SSC0180139		Au-In	Au0.91In0.09	Au	0.91	In	0.09																					1976																																														K		0.0423					0.0423																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111434	SSC0180139		Au-In	Au0.9In0.1	Au	0.9	In	0.1																					1976																																														K		0.0641					0.0641																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
111435	LOW0010641	gamma and gap are estimated from Hc measurements. G-L parameter = 0.0026	W	W1	W	1																							1969																																														K		0.0154					0.0154																				Oe		1.15												MHC11435														3.52								mj/mol.K2	0.9																																												Critical magnetic field curve of superconducting tungsten			University of Illinois, Urbana, Illinois,USA	J.Low Temp. Phys., 1(1969)641	J.C.Wheatley,R.T.Johnson,W.C.Black		
111436	LOW1311181	dTn/dP = 0.48 K/GPa. Tc(P) and Tn(P) measured for P=<2 GPa.	(Ho,Dy)Ni2B2C	Ho0.9Dy0.1Ni2B2C1	Ho	0.9	Dy	0.1	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		8.2					8.2			K/GPa	-0.64																																																																																												Ni2B flux method					Pressure effect on the coexistence of magnetism and superconductivity in Ho1-xDyxNi2B2C			Pohang University of Science and Technology, Pohang, Republic of Korea	J.Low Temp.Phys., 131(2003)1181	Eun-Mi Choi,Hyeonjin Doh,Jae-Hyuk Choi,M.Ohashi,N.Mori,Sung-Ik Lee		
111437	LOW1311181		(Ho,Dy)Ni2B2C	Ho0.6Dy0.4Ni2B2C1	Ho	0.6	Dy	0.4	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		6					6			K/GPa	0																																																																																												Ni2B flux method					Pressure effect on the coexistence of magnetism and superconductivity in Ho1-xDyxNi2B2C			Pohang University of Science and Technology, Pohang, Republic of Korea	J.Low Temp.Phys., 131(2003)1181	Eun-Mi Choi,Hyeonjin Doh,Jae-Hyuk Choi,M.Ohashi,N.Mori,Sung-Ik Lee		
111438	PHC3910217		MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2			A	3.0827		3.5612											AlB2, C32	K		37.3					37.3																																																																																																sinter(950C)					Narrow range of iridium-substitution on Mg1-xIrxB2 superconductor			Department of Chemistry, Faculty of Science, Tanta University, Tanta, Egypt	Physica C, 391(2003)217	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111439	PHC3910217		(Mg,Ir)B2	Mg0.98Ir0.02B2	Mg	0.98	Ir	0.02	B	2																			2003																												AlB2			A	3.0835		3.4817											AlB2, C32	K		33.2					33.2																																																																																																sinter(950C)					Narrow range of iridium-substitution on Mg1-xIrxB2 superconductor			Department of Chemistry, Faculty of Science, Tanta University, Tanta, Egypt	Physica C, 391(2003)217	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111440	PHC3910217		(Mg,Ir)B2	Mg0.94Ir0.06B2	Mg	0.94	Ir	0.06	B	2																			2003																												AlB2			A	3.0841		3.4142											AlB2, C32	K		28.1					28.1																																																																																																sinter(950C)					Narrow range of iridium-substitution on Mg1-xIrxB2 superconductor			Department of Chemistry, Faculty of Science, Tanta University, Tanta, Egypt	Physica C, 391(2003)217	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111441	PHC3910217	impurity phase = MgO, B	(Mg,Ir)B2	Mg0.88Ir0.12B2	Mg	0.88	Ir	0.12	B	2																			2003																												AlB2			A	3.0844		3.3686											AlB2, C32	K		18					18																																																																																																sinter(950C)					Narrow range of iridium-substitution on Mg1-xIrxB2 superconductor			Department of Chemistry, Faculty of Science, Tanta University, Tanta, Egypt	Physica C, 391(2003)217	Khaled M.Elsabawy,Morsy M.A.Sekkina		
111442	L091027002	RRR=7.8. G-L parameter = 125	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2003																												Chevrel																		K		15.05					15.05																				T		45							T/K		4.6					A		22																																																										bulk, conventional sample					Disordered Nanocrystalline Superconducting PbMo6S8 with aVery Large Upper Critical Field			Superconductivity Group, Department of Physics, University of Durham, United Kingdom	Phys.Rev.Lett., 91(2003)27002	D.P.Hampshire,H.J.Niu		
111443	L091027002	RRR=2.0. G-L parameter = 240	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2003																												Chevrel																		K		14.4					14.4																				T		65							T/K		7.3					A		19																																																										mechanically milled, then HIP, then ANN(1000C, 40h)					Disordered Nanocrystalline Superconducting PbMo6S8 with aVery Large Upper Critical Field			Superconductivity Group, Department of Physics, University of Durham, United Kingdom	Phys.Rev.Lett., 91(2003)27002	D.P.Hampshire,H.J.Niu		
111444	L091027002	RRR=1.4. G-L parameter = 520	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2003																												Chevrel																		K		12.3					12.3																				T		110							T/K		14.1					A		14																																																										mechanically milled, then HIP, then ANN(800C, 8h)					Disordered Nanocrystalline Superconducting PbMo6S8 with aVery Large Upper Critical Field			Superconductivity Group, Department of Physics, University of Durham, United Kingdom	Phys.Rev.Lett., 91(2003)27002	D.P.Hampshire,H.J.Niu		
111445	L091027002	RRR=3.3. G-L parameter = 160	(Pb,Cu)MO6S8	Pb0.98Cu0.036Mo6S8	Pb	0.98	Cu	0.036	Mo	6	S	8																	2003																												Chevrel																		K		14.8					14.8																				T		50							T/K		5.1					A		21																																																										HIP(2000 bar, 800C,8h)					Disordered Nanocrystalline Superconducting PbMo6S8 with aVery Large Upper Critical Field			Superconductivity Group, Department of Physics, University of Durham, United Kingdom	Phys.Rev.Lett., 91(2003)27002	D.P.Hampshire,H.J.Niu		
111446	L091027002	RRR=1.6. G-L parameter = 260	(Pb,Cu)MO6S8	Pb0.9Cu0.18Mo6S8	Pb	0.9	Cu	0.18	Mo	6	S	8																	2003																												Chevrel																		K		13.65					13.65																				T		45							T/K		5					A		23																																																										HIP(2000 bar, 800C,8h)					Disordered Nanocrystalline Superconducting PbMo6S8 with aVery Large Upper Critical Field			Superconductivity Group, Department of Physics, University of Durham, United Kingdom	Phys.Rev.Lett., 91(2003)27002	D.P.Hampshire,H.J.Niu		
111447	PR05009445	impurity phase<5%. dTc/dP in K/GPa	LuNiBC	Lu1Ni1B1C1	Lu	1	Ni	1	B	1	C	1																	1994																															A	3.492		7.552												K		2.9					2.9			K/GPa	-0.14																																																																																												arc-melting					Superconductivity in (LuC)2(Ni2B2) and (LuC)(Ni2B2)	199409			Phys.Rev.B,50 (1994) 9445-9448	C.W.Chu,L.Gao,R.L.Meng,X.D.Qiu,Y.Cao,Y.Y.Sun,Y.Y.Xue	Lu,C,Ni,B	
111448	PR05009445	10<impurity phase<20%. dTc/dP in K/GPa	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C			A	3.467		10.633												K		16.7					16.7			K/GPa	-0.05																																																																																												arc-melting					Superconductivity in (LuC)2(Ni2B2) and (LuC)(Ni2B2)	199409			Phys.Rev.B,50 (1994) 9445-9448	C.W.Chu,L.Gao,R.L.Meng,X.D.Qiu,Y.Cao,Y.Y.Sun,Y.Y.Xue	Lu,C,Ni,B	
111449	P068024523	gap by fitting specific heat data.	MgCNi3	Mg1C0.977Ni3	Mg	1	C	0.977	Ni	3																			2003																															A	3.812														K		7					7																				T		11.8																										5								mj/mol.K2	11.3		351																																					powder method					Influence of carbon concentration on the superconductivity in MgCxNi3			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, China	Phys.Rev.B., 68(2003)024523	G.C.Che,H.H.Wen,K.Xia,L.Shan,Z.A.Ren,Z.X.Zhao,Z.Y.Liu		
111450	P068024523	not s/c. C-content is close to the critical value of s/c estimated from lattice constant.	MgCNi3	Mg1C0.85Ni3	Mg	1	C	0.85	Ni	3																			2003																															A	3.79														K																																																															mj/mol.K2	5.8		434																																					powder method					Influence of carbon concentration on the superconductivity in MgCxNi3			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, Beijing, China	Phys.Rev.B., 68(2003)024523	G.C.Che,H.H.Wen,K.Xia,L.Shan,Z.A.Ren,Z.X.Zhao,Z.Y.Liu		
111451	P068020501	space-G=Pm3<->m. RRR=3. thickness d=60 nm. carrier n = -4.2 E+22 /cm3.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																															A	3.807														K		8.2					8.2																				T		12.8							T/K		2.3			MHC11451		A		50																																																										evaporation on CNi3 film on sapphire					Superconducting properties of MgCNi3 films			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B., 68(2003)020501	D.D.Craig,D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams		
111452	P068020501	space-G=Pm3<->m. thickness d = 75 nm	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																																														K		3.9					3.9																																																																																																evaporation on CNi3 film on sapphire					Superconducting properties of MgCNi3 films			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B., 68(2003)020501	D.D.Craig,D.P.Young,Julia Y.Chan,M.Moldovan,P.W.Adams		
111453	P068014512	Tc(by specific heat) = 7.7 K. 2*gap = 2.7 meV. gamma in mj/mol.K2.	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2003																												AlB2			A	4.189		4.4											AlB2, C32	K		7.9					7.9	MTC11453		K/GPa	0.21																																												4.07								mj/mol.K2	5.04		226																																					arc-melting					Thermodynamic properties and pressure effect on the superconductivity in CaAlSi and SrAlSi			Department of Physics and TCSAM, University of Houston, Houston, Texas, USA	Phys.Rev.B., 68(2003)014512	B.Lorenz,C.W.Chu,J.Cmaidalka,R.L.Meng		
111454	P068014512	Tc(by specific heat) = 4.9 K. 2*gap = 1.49 meV. gamma in mj/mol.K2.	SrAlSi	Sr1Al1Si1	Sr	1	Al	1	Si	1																			2003																												AlB2			A	4.22		4.754											AlB2, C32	K		5					5	MTC11454		K/GPa	-0.12																																												3.5								mj/mol.K2	5.42		218																																					arc-melting					Thermodynamic properties and pressure effect on the superconductivity in CaAlSi and SrAlSi			Department of Physics and TCSAM, University of Houston, Houston, Texas, USA	Phys.Rev.B., 68(2003)014512	B.Lorenz,C.W.Chu,J.Cmaidalka,R.L.Meng		
111455	JPS0721724	impurity phase = ReB2 < 5%. space-G = P6<3>/mc. RRR = 6. G-L parameter = 17	Re7B3	B3Re7	B	3	Re	7																					2003																															A	7.516		4.89												K		3.3					3.3											mT		6							T		0.9														A		191			A		3310																																																					arc-melting					The Superconductivity in Re-B System			Department of Physics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa,Japan	J.Phys.Soc.Jpn, 72(2003)1724	A.Kawano,H.Takagiwa,J.Akimitsu,T.Muranaka,Y.Mizuta		
111456	JPS0721724	space-G = Cmcm. RRR = 2.3. delta-C/gamma*Tc = 1.92. G-L parameter = 35	Re3B	B1Re3	B	1	Re	3																					2003																															A	2.896	9.317	7.27												K		4.8					4.8											mT		8							T		5.2							T/K		1.5					A		80			A		2870					3.53								mj/mol.K2	6.3		600																																					arc-melting					The Superconductivity in Re-B System			Department of Physics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa,Japan	J.Phys.Soc.Jpn, 72(2003)1724	A.Kawano,H.Takagiwa,J.Akimitsu,T.Muranaka,Y.Mizuta		
111457	CHC0121348	two phases(Li0.56BC(a,c in table) + Li0.90BC(a=2.726, c=7.1112)). not s/c.	LixBC	Li0.78B1C1	Li	0.78	B	1	C	1																			2003																												AlB2			A	2.6263		7.439											AlB2, C32	K					2																																																																																																		reaction(1500C, 24h)					Synthesis and characteristion of LixBC-hole doping does not induce superconductivity			Department of Chemistry, University of Liverpool, Liverpool, UK	Chem.Commun.,12(2003)1348	A.M.Fogg,G.R.Darling,J.B.Claridge,M.J.Rosseinsky		
111458	PR05811698	space-G = I4mcm	Zr2Co	Co1Zr2	Co	1	Zr	2																					1998								-10																				Al2Cu																	Al2Cu, C16	K		5.5					5.5																				T		0.9																																																																										arc-melting					Nuclear-magnetic-resonance investigation of the itinerant nearly antiferromagnetic behavior in superconducting Zr2(Co1-xNix)			Graduate School of Science & Technology and Faculty of Science, Kobe University, Nada, Kobe 657, Japan	Phys.Rev.B., 58(1998)11698	H.Sugita,M.Takekuni,S.Wada		
111459	PR05811698	space-G = I4mcm	Zr2(Co,Ni)	Zr2Co0.85Ni0.15	Zr	2	Co	0.85	Ni	0.15																			1998								-22																				Al2Cu																	Al2Cu, C16	K		6					6																				T		2																																																																										arc-melting					Nuclear-magnetic-resonance investigation of the itinerant nearly antiferromagnetic behavior in superconducting Zr2(Co1-xNix)			Graduate School of Science & Technology and Faculty of Science, Kobe University, Nada, Kobe 657, Japan	Phys.Rev.B., 58(1998)11698	H.Sugita,M.Takekuni,S.Wada		
111460	PR05811698	space-G = I4mcm	Zr2(Co,Ni)	Zr2Co0.6Ni0.4	Zr	2	Co	0.6	Ni	0.4																			1998								-2.5																				Al2Cu																	Al2Cu, C16	K		4.2					4.2																																																																																																arc-melting					Nuclear-magnetic-resonance investigation of the itinerant nearly antiferromagnetic behavior in superconducting Zr2(Co1-xNix)			Graduate School of Science & Technology and Faculty of Science, Kobe University, Nada, Kobe 657, Japan	Phys.Rev.B., 58(1998)11698	H.Sugita,M.Takekuni,S.Wada		
111461	L091076402	dTc/dP calculated from uniaxial values (dTc/dP)//c = -0.890 K/GPa and (dTc/dP)//a = 0.540 K/GPa using thermal expansion.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																			2003																												HoCoGa5																		K		0.38					0.38	MTE11461		K/GPa	0.19																																																																																																	Uniaxial Pressure Effects on CeIrIn5 and CeCoIn5 Studied by Low-Temperature Thermal Expansion			Max Planck Institute for Chemical Physics of Solids, Dresden, Germany	Phys.Rev.Lett., 91(2003)076402	F.Steglich,J.D.Thompson,J.D.Tompson,J.L.Sarrao,M.Lang,N.Oeschler,P.Gegenwart,R.Movshovich		
111462	L091076402	dTc/dP calculated from uniaxial values (dTc/dP)//c = 0.075 K/GPa and (dTc/dP)//a = 0.290 K/GPa using thermal expansion.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																			2003																												HoCoGa5																		K		2.23					2.23			K/GPa	0.655																																																																																																	Uniaxial Pressure Effects on CeIrIn5 and CeCoIn5 Studied by Low-Temperature Thermal Expansion			Max Planck Institute for Chemical Physics of Solids, Dresden, Germany	Phys.Rev.Lett., 91(2003)076402	F.Steglich,J.D.Thompson,J.D.Tompson,J.L.Sarrao,M.Lang,N.Oeschler,P.Gegenwart,R.Movshovich		
111463	L091077001	s/c vanishes at Pc = 5 - 5.6 GPa, where S-I transition occures. dTc/dP estimated from Tc(P=1.5 GPa) = 5.8 K. T*(in Fig) = metal-insulator transition temp.	CuRh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			2003																												spinel			A	9.787														K		4.7					4.7	MTC11463		K/GPa	0.73																																																																																												sinter (1000C, 3d)					Pressure-Induced Superconductor-Insulator Transition in the Spinel Compound CuRh2S4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima, Japan	Phys.Rev.Lett., 91(2003)077001	A.J.Perez Kuroki,F.Nakamura,H.Fujii,H.Kurisaki,H.Okada,J.Hori,M.Ito,M.Udagawa,N.Ogita,T.Fujita,T.Suzuki		
111464	JPS0633333	M-I transition at 230 K. lattice const.(T=10 K): a=6.8645, c=10.0257	CuIr2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			1994																												spinel			A	9.8474														K					5																																																																																																		heat(850C, 10d)					Structural and magnetic studies of metal-insulator transition in thiospinel CuIr2S4			National Research Institute for Metals, Sengen, Tsukuba, Ibaraki, Japan	J.Phys.Soc.Jpn, 63(1994)3333	S.Nagata,T.Furubayashi,T.Hagino,T.Matsumoto		
111465	PHB3120136	delta-C/gamma*Tc = 0.8	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2002																												HoCoGa5			A	4.668		7.515												K		0.43					0.43			K/GPa	0.25																																																																																												In-flux method					Heat capacity of the heavy fermion superconductor CeIrIn5 under hydrostatic pressure			Max-Planck-Institute for the Chemical Physics of Solids, D-01187 Dresden, Germany	Physica B, 312-313(2002)136	E.Lengyel,F.Steglich,G.Sparn,J.D.Thompson,J.L.Sarrao,P.G.Pagliuso,R.Borth		
111466	PHB3120138	Tc(P) measured by specific heat. Tc seems to saturate with Tc(max)=2.7 K at P=1.5 GPa. delta-C/gamma*Tc = 5.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																												HoCoGa5			A	4.614		7.552												K		2.26					2.26			K/GPa	0.4																																																																																																	Effect of pressure on unconventional superconductivity in CeCoIn5			Max-Planck-Institute for the Chemical Physics of Solids, D-01187 Dresden, Germany	Physica B, 312-313(2002)138	E.Lengyel,F.Steglich,G.Sparn,J.D.Thompson,J.L.Sarrao,P.G.Pagliuso,R.Borth		
111467	P068064503	gamma in mj/mol.K2. Debye-T from sp-heat. From R(T) fitting, Debye-T = 238 K.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																												CaTiO3			A	3.811													CaTiO3, perovskite	K		6.6					6.6																																																								mj/mol.K2	32		256																																					solid state reaction					Suppression of superconductivity in Mn-substituted MgCNi3			Max-Planck-Institut fur Festkorperforschung, 70569 Stuttgart, Germany	Phys.Rev.B, 68(2003)64503	A.Das,R.K.Kremer		
111468	P068064503	gamma in mj/mol.K2. Debye-T from sp-heat.	MgC(Ni,Mn)3	Mg1C1Ni2.99Mn0.01	Mg	1	C	1	Ni	2.99	Mn	0.01																	2003																												CaTiO3			A	3.8115													CaTiO3, perovskite	K					0.3																																																										mj/mol.K2	28.2		288																																					solid state reaction					Suppression of superconductivity in Mn-substituted MgCNi3			Max-Planck-Institut fur Festkorperforschung, 70569 Stuttgart, Germany	Phys.Rev.B, 68(2003)64503	A.Das,R.K.Kremer		
111469	P068064503	gamma in mj/mol.K2. Debye-T from sp-heat.	MgC(Ni,Mn)3	Mg1C1Ni2.97Mn0.03	Mg	1	C	1	Ni	2.97	Mn	0.03																	2003																												CaTiO3			A	3.8122													CaTiO3, perovskite	K					0.3																																																										mj/mol.K2	32.4		294																																					solid state reaction					Suppression of superconductivity in Mn-substituted MgCNi3			Max-Planck-Institut fur Festkorperforschung, 70569 Stuttgart, Germany	Phys.Rev.B, 68(2003)64503	A.Das,R.K.Kremer		
111470	P068064503	gamma in mj/mol.K2. Debye-T from sp-heat.	MgC(Ni,Mn)3	Mg1C1Ni2.95Mn0.05	Mg	1	C	1	Ni	2.95	Mn	0.05																	2003																												CaTiO3			A	3.8127													CaTiO3, perovskite	K					0.3																																																										mj/mol.K2	35		296																																					solid state reaction					Suppression of superconductivity in Mn-substituted MgCNi3			Max-Planck-Institut fur Festkorperforschung, 70569 Stuttgart, Germany	Phys.Rev.B, 68(2003)64503	A.Das,R.K.Kremer		
111471	P068064512	s/c parameters in table shows for H//ab. For H//c, Hc1(0)=250 Oe, Hc2(0)=0.81 T, cohere=73 A, penet=2060 A. anisotropy=2.3. RRR=4.9. carrier=8.6E+26 /m3. R(Tc)=20 um.	Ca(Al,Si)2	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2003																												AlB2			A	4.19002		4.3978											AlB2, C32	K		7.8					7.8											Oe		160							T		1.8														A		170			A		870																																																					floating zone method					Superconducting properties of single-crystalline Ca(Al0.5,Si0.5)2 : A ternary silicide with the AlB2-type structure			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 68(2003)64512	El-Hadi S.Sadki,H.Abe,H.Kitazawa,K.Hirata,K.Nishida,M.Imai,T.Kimura,T.Sato		
111472	P066064510	space-G = Pm3<->m	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2002																												CaTiO3																	CaTiO3, perovskite	K		7.69					7.69	MTC11472																																																																																															solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111473	P066064510	space-G = Pm3<->m	MgC(Ni,Co)3	Mg1C1Ni2.95Co0.05	Mg	1	C	1	Ni	2.95	Co	0.05																	2002																												CaTiO3																	CaTiO3, perovskite	K		7.42					7.42																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111474	P066064510	space-G = Pm3<->m	MgC(Ni,Co)3	Mg1C1Ni2.9Co0.1	Mg	1	C	1	Ni	2.9	Co	0.1																	2002																												CaTiO3																	CaTiO3, perovskite	K		7.29					7.29																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111475	P066064510	space-G = Pm3<->m	MgC(Ni,Co)3	Mg1C1Ni2.8Co0.2	Mg	1	C	1	Ni	2.8	Co	0.2																	2002																												CaTiO3																	CaTiO3, perovskite	K		7.2					7.2																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111476	P066064510	space-G = Pm3<->m	MgC(Ni,Co)3	Mg1C1Ni2.6Co0.4	Mg	1	C	1	Ni	2.6	Co	0.4																	2002																												CaTiO3																	CaTiO3, perovskite	K		7.1					7.1																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111477	P066064510		MgC(Ni,Fe)3	Mg1C1Ni2.9Fe0.1	Mg	1	C	1	Ni	2.9	Fe	0.1																	2002																												CaTiO3																	CaTiO3, perovskite	K		8.58					8.58																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111478	P066064510		MgC(Ni,Fe)3	Mg1C1Ni2.8Fe0.2	Mg	1	C	1	Ni	2.8	Fe	0.2																	2002																												CaTiO3																	CaTiO3, perovskite	K		8					8																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111479	P066064510		MgC(Ni,Fe)3	Mg1C1Ni2.7Fe0.3	Mg	1	C	1	Ni	2.7	Fe	0.3																	2002																												CaTiO3																	CaTiO3, perovskite	K		6.88					6.88																																																																																																solid state reaction in (0.92Ar+0.08He)					Normal and superconducting states of MgCNi3 upon Fe and Co substitution and external pressure			Materials Science Division, Indira Gandhi Centre for Atomic Research, Kalpakkam , India	Phys.Rev.B, 66(2002)64510	Awadhesh Mani,J.Janaki,M.C.Valsakumar,S.Mathi Jaya,T.Geetha Kumary,T.S.Radhakrishnan,V.S.Sastry,Y.Hariharan		
111480	P067100509	M=THF(tetrahydrofuran: C4H8O). c-axis oriented sample. isotope effect (N<14> - N<15>). NMR of N<15> measured.	Li0.48M0.3HfNCl	Li0.48M0.3Hf1N1Cl1	Li	0.48	M	0.3	Hf	1	N	1	Cl	1															2003																																		18.7												K		25.5					25.5						0.07	N																																																																																									using N<15> enriched anmonium					Superconducting characteristics in electron-doped layered hafnium nitride: <15>N isotope effect studies			Department of Quantum Matter, AdSM, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Phys.Rev.B, 67(2003)100509	H.Tou,S.Yamanaka,Y.Maniwa		
111481	P068092507	C-content = nominal value.d(lnTc)/dP = 0.002 /kbar	MgCxNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																												CaTiO3																	CaTiO3, perovskite	K		6.9					6.9			K/GPa	0.155																																																																		MTP11481																															Pressure effects on the transition temperature of superconducting MgCxNi3			Department of Physics, National Sun Yat Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B, 68(2003)92507	C.-J.Liu,C.-Q.Jin,H.D.Yang,H.L.Huang,J.-Y.Lin,P.L.Ho,R.-C.Yu,S.Mollah,W.L.Huang,Y.-L.Zhang		
111482	P068092507	C-content = nominal value.	MgCxNi3	Mg1C1.25Ni3	Mg	1	C	1.25	Ni	3																			2003																												CaTiO3																	CaTiO3, perovskite	K		7.4					7.4			K/GPa	0.134																																																																																																	Pressure effects on the transition temperature of superconducting MgCxNi3			Department of Physics, National Sun Yat Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B, 68(2003)92507	C.-J.Liu,C.-Q.Jin,H.D.Yang,H.L.Huang,J.-Y.Lin,P.L.Ho,R.-C.Yu,S.Mollah,W.L.Huang,Y.-L.Zhang		
111483	P068092507	C-content = nominal value.	MgCxNi3	Mg1C1.5Ni3	Mg	1	C	1.5	Ni	3																			2003																												CaTiO3																	CaTiO3, perovskite	K		7.9					7.9			K/GPa	0.152																																																																																																	Pressure effects on the transition temperature of superconducting MgCxNi3			Department of Physics, National Sun Yat Sen University, Kaohsiung 804, Taiwan, Republic of China	Phys.Rev.B, 68(2003)92507	C.-J.Liu,C.-Q.Jin,H.D.Yang,H.L.Huang,J.-Y.Lin,P.L.Ho,R.-C.Yu,S.Mollah,W.L.Huang,Y.-L.Zhang		
111484	PR06103823	Tc increases linearly with P. Tc(on) reaches 17.2 K at P=120 GPa. diamond anvil cell.	V	V1	V	1																							2000																																														K		5.3					5.3	MTC11484		K/GPa	0.1																																																																																																	Pressure effect on superconductivity of vanadium at megabar pressures	200002		Research Center for Materials Science at Extreme Conditions (KYOKUGEN), Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B,61(2000)R3823-R3825	M.Iketani,M.Ishizuka,S.Endo		
111485	JPS0644049	foil. Tc(max)=9.2 K at P=49 GPa.	V	V1	V	1																							1995																																														K		5.3					5.3	MTC11485		K/GPa	0.096																																																																																																	Pressure effect on superconductivity of V and V-Cr alloys up to 50 GPa			Department of Material Science, Himeji Institute of Technology, Hyogo, Japan	J.Phys.Soc.Jpn, 64(1995)4049	H.Kawamura,M.Kobayashi,Y.Akahama		
111486	JPS0644049	Tc=5.04 K at P=27.6 GPa.	V9Cr1	Cr0.1V0.9	Cr	0.1	V	0.9																					1995																																														K		3.3					3.3			K/GPa	0.062																																																																																												arc-melting					Pressure effect on superconductivity of V and V-Cr alloys up to 50 GPa			Department of Material Science, Himeji Institute of Technology, Hyogo, Japan	J.Phys.Soc.Jpn, 64(1995)4049	H.Kawamura,M.Kobayashi,Y.Akahama		
111487	JPS0644049	Tc=3.01 K at P=31.1 GPa.	V8Cr2	Cr0.2V0.8	Cr	0.2	V	0.8																					1995																																														K		1.66					1.66			K/GPa	0.047																																																																																												arc-melting					Pressure effect on superconductivity of V and V-Cr alloys up to 50 GPa			Department of Material Science, Himeji Institute of Technology, Hyogo, Japan	J.Phys.Soc.Jpn, 64(1995)4049	H.Kawamura,M.Kobayashi,Y.Akahama		
111489	P068104513	anisotropy = 3 at Tc from Hc2. Hc2//ab, //c are obtained using Bud'ko's method.	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2																	AlB2, C32	K		38					38																																		MHC11489																																																														Heat (Mg,B) at 1400C					Out-of-plane and in-plane anisotropy of upper critical field in MgB2			Department of Applied Physics, The University of Tokyo,  Hongo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 68(2003)104513	H.Ihara,H.Kito,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
111490	P068104513	Hc2(0)//ab = 14.1 T, cohere(c) = 17.6 A. anisotropy = 4.5 at Tc from Hc2.	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2																	AlB2, C32	K		37					37																				T		3.51							T/K		0.13			MHC11490		A		95																																																										grown from MgB2+0.1Mg at P=3.5 GPa					Out-of-plane and in-plane anisotropy of upper critical field in MgB2			Department of Applied Physics, The University of Tokyo,  Hongo, Bunkyo-ku, Tokyo, Japan	Phys.Rev.B, 68(2003)104513	H.Ihara,H.Kito,K.Togano,M.Tokunaga,T.Tamegai,Y.Takano,Z.X.Shi		
111491	P068094514	specific heat fitting (C=aT+bT<3>+cT<5>) for 2<T<300K. gap estimated from sp-heat using two band model. table shows for sigma-band. For pai-band, gap=1.17	MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2			A	3.085		3.525											AlB2, C32	K		38					38																																																3.77								mj/mol.K2	3		670																																					mixture(Mg,B) powder in Ta crucible, heat(100C, 15h)					Effects of Al doping on the normal and superconducting properties of MgB2: A specific heat study			INFM-LAMIA, CNR-IMEM and Dipartimento di Fisica, Universita di Genova, via Dodecaneso,  Genova, Italy	Phys.Rev.B, 68(2003)94514	A.Palenzona,M.Affronte,M.Putti,P.Manfrinetti		
111492	P068094514	specific heat fitting (C=aT+bT<3>+cT<5>) for 2<T<300K. gap estimated from sp-heat using two band model. table shows for sigma-band. For pai-band, gap=1.51	(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																			2003																												AlB2			A	3.08		3.483											AlB2, C32	K		31					31																																																3.31								mj/mol.K2	2.8		740																																					mixture(Mg,Al,B) powder in Ta crucible, heat(100C, 15h)					Effects of Al doping on the normal and superconducting properties of MgB2: A specific heat study			INFM-LAMIA, CNR-IMEM and Dipartimento di Fisica, Universita di Genova, via Dodecaneso,  Genova, Italy	Phys.Rev.B, 68(2003)94514	A.Palenzona,M.Affronte,M.Putti,P.Manfrinetti		
111493	P068094514	specific heat fitting (C=aT+bT<3>+cT<5>) for 2<T<300K. gap estimated from sp-heat using two band model. table shows for sigma-band. For pai-band, gap=1.61	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2003																												AlB2			A	3.077		3.462											AlB2, C32	K		25					25																																																2.87								mj/mol.K2	2.55		650																																					mixture(Mg,Al,B) powder in Ta crucible, heat(100C, 15h)					Effects of Al doping on the normal and superconducting properties of MgB2: A specific heat study			INFM-LAMIA, CNR-IMEM and Dipartimento di Fisica, Universita di Genova, via Dodecaneso,  Genova, Italy	Phys.Rev.B, 68(2003)94514	A.Palenzona,M.Affronte,M.Putti,P.Manfrinetti		
111494	P068094514	specific heat fitting (C=aT+bT<3>+cT<5>) for 2<T<300K. gap estimated from sp-heat using two band model. table shows for sigma-band. For pai-band, gap=1.24	(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																			2003																												AlB2			A	3.069		3.425											AlB2, C32	K		18					18																																																2.16								mj/mol.K2	2.1		680																																					mixture(Mg,Al,B) powder in Ta crucible, heat(100C, 15h)					Effects of Al doping on the normal and superconducting properties of MgB2: A specific heat study			INFM-LAMIA, CNR-IMEM and Dipartimento di Fisica, Universita di Genova, via Dodecaneso,  Genova, Italy	Phys.Rev.B, 68(2003)94514	A.Palenzona,M.Affronte,M.Putti,P.Manfrinetti		
111495	P068094514	specific heat fitting (C=aT+bT<3>+cT<5>) for 2<T<300K	(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																			2003																												AlB2			A	3.064		3.398											AlB2, C32	K		12					12																																																								mj/mol.K2	1.9		690																																					mixture(Mg,Al,B) powder in Ta crucible, heat(100C, 15h)					Effects of Al doping on the normal and superconducting properties of MgB2: A specific heat study			INFM-LAMIA, CNR-IMEM and Dipartimento di Fisica, Universita di Genova, via Dodecaneso,  Genova, Italy	Phys.Rev.B, 68(2003)94514	A.Palenzona,M.Affronte,M.Putti,P.Manfrinetti		
111496	PHC3970007	RRR=2.2	Mg(B,C)2	Mg1B1.96C0.04	Mg	1	B	1.96	C	0.04																		3	2003																												AlB2			A	3.0776		3.5217											AlB2, C32	K		35.5					35.5																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111497	PHC3970007	RRR=1.7	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		3	2003																												AlB2			A	3.0641		3.5226											AlB2, C32	K		30					30																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111498	PHC3970007	RRR=1.4	Mg(B,C)2	Mg1B1.85C0.15	Mg	1	B	1.85	C	0.15																		3	2003																												AlB2			A	3.0524		3.5224											AlB2, C32	K		24					24																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111499	PHC3970007	RRR=1.3	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		3	2003																												AlB2			A	3.0449		3.5215											AlB2, C32	K		13.5					13.5																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111500	PHC3970007	RRR=1.2	Mg(B,C)2	Mg1B1.75C0.25	Mg	1	B	1.75	C	0.25																		3	2003																												AlB2			A	3.0356		3.5209											AlB2, C32	K		2.5					2.5																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111501	PHC3970007	nearly solubility limit. not s/c.	Mg(B,C)2	Mg1B1.7C0.3	Mg	1	B	1.7	C	0.3																		3	2003																												AlB2			A	3.0322		3.5213											AlB2, C32	K					2																																																																																																		high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111502	PHC3970007	multi-phase powder. impurity phase=MgB2C2, BN, MgO. not s/c.	Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																			2003																												AlB2			A	3.0236		3.5223											AlB2, C32	K					2																																																																																																		high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111503	PHC3970007	RRR=5.5.  rapid quenched sample.	MgB2	B2Mg1	B	2	Mg	1																				3	2003																												AlB2			A	3.0852		3.5202											AlB2, C32	K		38					38																																																																																																high-pressure synthesis (1600-1700C, 5 GPa)					Carbon-substituted MgB2 single crystals			Superconductivity Research Laboratory, ISTEC,  Shinonome, Koto-ku, Tokyo, Japan	Physica C, 397(2003)7-13	A.Yamamoto,H.Uchiyama,S.Lee,S.Tajima,T.Masui		
111504	L091167001	p-induced s/c. Tc(max)=13.8 K at P=30.2 GPa. dTc/dP=0.9 K/GPa for 20<P<30 GPa and =-0.4 K/GPa for 30<P<50 GPa.	Li	Li1	Li	1																							2003																																														K		13.8			0		13.8	MTC11504		K/GPa	0.9																																																																																																	Superconducting Phase Diagram of Li Metal in Nearly Hydrostatic Pressures up to 67 GPa			Department of Physics,Washington University, C.B. 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.Lett., 91(2003)167001	J.S.Schilling,S.Deemyad		
111505	L091167001	p-induced s/c. values of s/c properties in TBL are at P=21.9 GPa.	Li	Li1	Li	1																							2003																																														K		5.95			0		5.95			K/GPa	0.9																Oe		800							Oe/K		270																																																																						Superconducting Phase Diagram of Li Metal in Nearly Hydrostatic Pressures up to 67 GPa			Department of Physics,Washington University, C.B. 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.Lett., 91(2003)167001	J.S.Schilling,S.Deemyad		
111506	P068144510	gap by tunneling using PtIr/MgCNi3 point contact. gap(delta) = 1.3 meV.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																																														K		7					7																																																4.3	1																																															solid state reaction					s-wave pairing in MgCNi3 revealed by point contact tunneling			National Laboratory for Superconductivity, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, China	Phys.Rev.B, 68(2003)144510	G.C.Che,H.Gao,H.H.Wen,H.J.Tao,L.Shan,Z.A.Ren,Z.Z.Li		
111507	P068134503	RRR=2.7. Hc2(0)//c estimated from thermodynamic Hc(0) (=0.45 kG). penet<ab>, cohere<ab>, G-L<ab> are estimated to be 20. Jc measured from M.	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2003																												AlB2																	AlB2, C32	K		6					6																				T		1.27												MHC11507		A		196			A		3140																																																					arc-melting, floating zone method					Anisotropic vortex pinning in the layered intermetallic superconductor CaAlSi			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 68(2003)134503	Ajay Kumar Ghosh,M.Tokunaga,T.Tamegai,Y.Hiraoka		
111508	PHC3990008		MgB2	B2Mg1	B	2	Mg	1																					2003																												AlB2			A	3.0857		3.5231											AlB2, C32	K		38.6					38.6	MHIR11508																																	MHIR11508																																																														solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111509	PHC3990008		(Mg,Al,Li)B2	Mg0.9Al0.05Li0.05B2	Mg	0.9	Al	0.05	Li	0.05	B	2																	2003																												AlB2			A	3.0783		3.5241											AlB2, C32	K		37.8					37.8																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111510	PHC3990008		(Mg,Al,Li)B2	Mg0.8Al0.1Li0.1B2	Mg	0.8	Al	0.1	Li	0.1	B	2																	2003																												AlB2			A	3.0779		3.4546											AlB2, C32	K		31					31																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111511	PHC3990008		(Mg,Al,Li)B2	Mg0.7Al0.15Li0.15B2	Mg	0.7	Al	0.15	Li	0.15	B	2																	2003																												AlB2			A	3.074		3.4361											AlB2, C32	K		25.1					25.1																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111512	PHC3990008		(Mg,Al,Li)B2	Mg0.6Al0.2Li0.2B2	Mg	0.6	Al	0.2	Li	0.2	B	2																	2003																												AlB2			A	3.0662		3.4073											AlB2, C32	K		16.1					16.1																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111513	PHC3990008		(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																			2003																												AlB2			A	3.0806		3.5056											AlB2, C32	K		37.8					37.8																																		MHIR11513																																																														solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111514	PHC3990008		(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																			2003																												AlB2			A	3.0716		3.4287											AlB2, C32	K		29					29																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111515	PHC3990008		(Mg,Al)B2	Mg0.7Al0.3B2	Mg	0.7	Al	0.3	B	2																			2003																												AlB2			A	3.0643		3.3963											AlB2, C32	K		18					18																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111516	PHC3990008		(Mg,Al)B2	Mg0.6Al0.4B2	Mg	0.6	Al	0.4	B	2																			2003																												AlB2			A	3.0538		3.3741											AlB2, C32	K		7					7																																																																																																solid state reaction					Structure and superconductivity of double-doped Mg1-x(Al0.5Li0.5)xB2			Materials Research Department, Riso National Laboratory, Roskilde, Denmark	Physica C, 399(2003)8	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111517	PRL0801730	Hc2 defined as mid point (resistive transition). H//c-axis	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	1998																												LuNi2B2C																		K		15.7					15.7																				T		10.6												MHC11517																																																														Ni2B flux method					Upper Critical Field Peculiarities of Superconducting YNi2B2C and LuNi2B2C	1		Institut fur Festkorper-und Werkstofforschung Dresden e.V., Postfach 270016, D-01171 Dresden, Germany	Phys.Rev.Lett.,80(1998)1730-1733	G. Fuchs,K. Krug,K. Winzer,K.-H. Muller,M. Heinecke,S.-L. Drechsler,S.V. Shulga		
111518	PRL0801730	Hc2 defined as mid point (resistive transition). H//c-axis	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	1998																												LuNi2B2C																		K		16.5					16.5																				T		7.6												MHC11518																																																														Ni2B flux method					Upper Critical Field Peculiarities of Superconducting YNi2B2C and LuNi2B2C	1		Institut fur Festkorper-und Werkstofforschung Dresden e.V., Postfach 270016, D-01171 Dresden, Germany	Phys.Rev.Lett.,80(1998)1730-1733	G. Fuchs,K. Krug,K. Winzer,K.-H. Muller,M. Heinecke,S.-L. Drechsler,S.V. Shulga		
111519	PHC3980107	SP-heat measured in the field cooling condition. H//c. gamma(mj/mol.K2), Debye-T in TBL analyzed without T^5 term. gamma=20.6 mj/mol.K2, Debye-T=680K with T^5 term. gap from sp-heat.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2003																												LuNi2B2C																		K		14.5					14.5																																																3.64								mj/mol.K2	19.1		495																																										Complementary study of heat capacity and magnetization for intermetallic YNi2B2C single crystal			Korea Electrotechnology Research Institute, Changwon, Kyungnam, South Korea	Physica C, 398(2003)107	C.Park,C.V.Tomy,D.G.Mandrus,D.McK.Paul,J.R.Thompson,K.J.Song,S.S.Oh,Y.K.Kwon		
111520	SCI2930273	p-induced s/c. Tc(max)=11 K at 250 GPa. Pc=160 GPa(Tc=6 K). dTc/dP for 180 < P < 250 GPa.	B	B1	B	1																							2001																																														K		11			0		11	MTC11520		K/GPa	0.05																																																																																																	Superconductivity in Boron			Carnegie Institution of Washington,Washington DC,USA	Science 293(2001)272	Ho-Kwang Mao,M.I.Eremets,R.J.Hemley,V.V.Struzhkin		
111521	NAT3900382	P-induced s/c. Pc=93 GPa. Tc(max) = 14 K at 157 GPa (max-pressure in this paper). Another Tc(=17K) at 157 GPa observed(beta-Po phase)	S	S1	S	1																							1997																																														K		14			0		14	MTC11521		K/GPa	0.055																																																																																																	Superconductivity at 10 - 17 K in compressed sulphur			Carnegie Institution of Washington, Washington DC,USA	Nature, 390(1997)382	Ho-Kwang Mao,R.J.Hemley,V.V.Struzhkin,Y.A.Timofeev		
111522	JPC013L905	resistivity R reaches max at Tm. Tm/dP = 28 K/GPa. Tm(P=0) = 50 K. Tc(max) = 2.61 K at P=1.5 GPa.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																			2001																												HoCoGa5																		K		2.26					2.26			K/GPa	0.5																																																																																																	Response of the heavy-fermion superconductor CeCoIn5 to pressure: roles of dimensionality and proximity to a quantum-critical point			Los Alamos National Laboratory Los Alamos, NM 87545, USA	J.Phys.: Condens.Matter, 13(2001)L905	E.Lengyel,F.Steglich,G.Sparn,J.D.Thompson,J.L.Sarrao,M.Nicklas,P.G.Pagliuso,R.Borth,V.A.Sidorov		
111523	SSC0840803	P-induced s/c. phase diagram and Tc(P) were measured. Tc shows Tc(max). dTc/dP = 0 K/GPa at Pc (=26 GPa)	Se	Se1	Se	1																							1992																																														K		5.4			0		5.4	MTC11523		K/GPa	0																																																																																												210C, 20h, in vac.					Pressure-induced superconductivity and phase transition in selenium and tellurium 			Himeji Institute of Technology 1479-1 Kanaji, Kamigohri, Hyogo, 678-12, Japan 	Solid State Commun., 84(1992)803	H.Kawamura,M.Kobayashi,Y.Akahama		
111524	SSC0840803	P-induced s/c. phase diagram and Tc(P) were measured. Tc shows Tc(max).	Te	Te1	Te	1																							1992																																														K		7.4			0		7.4	MTC11524																																																																																																				Pressure-induced superconductivity and phase transition in selenium and tellurium 			Himeji Institute of Technology 1479-1 Kanaji, Kamigohri, Hyogo, 678-12, Japan 	Solid State Commun., 84(1992)803	H.Kawamura,M.Kobayashi,Y.Akahama		
111525	JAP0575093	substrate: oxidized Si wafer. T<sub> = RT. Tc(thickness) measured. Tc in TBL shows Tc(max).	Be	Be1	Be	1																							1985																																														K		6					6	MTC11525																																																																																															ion beam sputtering					Superconducting beryllium thin films prepared by ion-beam sputtering			NTT Tokai, Ibaraki, Japan	J.Appl.Phys., 57(1985)5093	K.Nakamura,K.Takei,Kito Nakamura,Koji Takei,Y.Maeda,Yasushi Maeda		
111526	PR135A0631	Type-I s/c. dHc2/dT, Hc2(0) in DB represent dHc/dT, Hc(0), respectively.	Hg	Hg1	Hg	1																							1964																																														K		4.16					4.16																				Oe		380							Oe/K		203.3																									mj/mol.K2	1.79		71.9																																										Specific heat of mercury and thallium between 0.35 and 4.2 K			Purdue University, Lafayette, Indiana	Phys.Rev., 135(1964)A631	B. J. C. van der Hoeven, Jr.,P. H. Keesom		
111527	PR135A0631	Type-I s/c. dHc2/dT, Hc2(0) in DB represent dHc/dT, Hc(0), respectively.	Tl	Tl1	Tl	1																							1964																																														K		2.38					2.38																				Oe		176.5							Oe/K		128																									mj/mol.K2	1.47		78.5																																										Specific heat of mercury and thallium between 0.35 and 4.2 K			Purdue University, Lafayette, Indiana	Phys.Rev., 135(1964)A631	B. J. C. van der Hoeven, Jr.,P. H. Keesom		
111528	PHC3990165	Tc(off) = 2.8 K. Hc2(0), Hc1(0) measured at 2K.	Nd(Pt,Au)2B2C	Nd1Pt1.5Au0.6B2C1	Nd	1	Pt	1.5	Au	0.6	B	2	C	1															2003																												LuNi2B2C			A	3.835		10.781												K		3.2					3.2											Oe		100							kOe		2																																																																										arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111529	PHC3990165	Tc(off) = 9.4 K.	LaPt2B2C	La1Pt2.1B2.4C1.2	La	1	Pt	2.1	B	2.4	C	1.2																	2003																												LuNi2B2C																		K		10.2					10.2																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111530	PHC3990165	Tc(off) = 9.5 K.	(La,Nd)Pt2B2C	La0.9Nd0.1Pt2.1B2.4C1.2	La	0.9	Nd	0.1	Pt	2.1	B	2.4	C	1.2															2003																												LuNi2B2C																		K		10.3					10.3																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111531	PHC3990165	Tc(off) = 6.42 K.	(La,Nd)Pt2B2C	La0.7Nd0.3Pt2.1B2.4C1.2	La	0.7	Nd	0.3	Pt	2.1	B	2.4	C	1.2															2003																												LuNi2B2C																		K		7.84					7.84																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111532	PHC3990165	Tc(off) = 5.35 K.	(La,Nd)Pt2B2C	La0.5Nd0.5Pt2.1B2.4C1.2	La	0.5	Nd	0.5	Pt	2.1	B	2.4	C	1.2															2003																												LuNi2B2C																		K		6.36					6.36																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111533	PHC3990165	Tc(off) = 2.55 K.	(La,Nd)Pt2B2C	La0.3Nd0.7Pt2.1B2.4C1.2	La	0.3	Nd	0.7	Pt	2.1	B	2.4	C	1.2															2003																												LuNi2B2C																		K		4.28					4.28																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111534	PHC3990165	Tc(off) < 1.7 K.	(La,Nd)Pt2B2C	La0.1Nd0.9Pt2.1B2.4C1.2	La	0.1	Nd	0.9	Pt	2.1	B	2.4	C	1.2															2003																												LuNi2B2C																		K		3.45					3.45																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111535	PHC3990165	Tc(off) < 1.7 K.	NdPt2B2C	Nd1Pt2.1B2.4C1.2	Nd	1	Pt	2.1	B	2.4	C	1.2																	2003								1.5																				LuNi2B2C																		K		2.91					2.91																																																																																																arc-melting, ANN(1100C,1w)					Coexistence of superconductivity and magnetic order in NdPt2B2C			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 399(2003)165-170	A.D.Chinchure,C.Godart,E.Alleno,L.C.Gupta,P.L.Paulose,R.Nagarajan,S.K.Dhar		
111536	PHC4000160	Tc from SP-heat. lattice term beta=0.58 mJ/mol.K4.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																															A	3.81														K		6.84					6.84																																																					MSP11536			mj/mol.K2	28.8		253																																					solid state reaction					Specific heat study of (Mg0.85Zn0.15)CNi3 and MgCNi3			Korea Basic Science Institute, Daejeon 305-333, Republic of Korea	Physica C, 400(2003)160-164	E.J.Choi,H.C.Ri,J.Giim,S.-H.Park,Sung-Hoon Jung,Y.W.Lee		
111537	PHC4000160	Tc from SP-heat. lattice term beta=0.13 mJ/mol.K4.	(Mg,Zn)CNi3	Mg0.85Zn0.15C1Ni3	Mg	0.85	Zn	0.15	C	1	Ni	3																	2003																															A	3.79														K		4.12					4.12																																																					MSP11537			mj/mol.K2	24.4		350																																					solid state reaction					Specific heat study of (Mg0.85Zn0.15)CNi3 and MgCNi3			Korea Basic Science Institute, Daejeon 305-333, Republic of Korea	Physica C, 400(2003)160-164	E.J.Choi,H.C.Ri,J.Giim,S.-H.Park,Sung-Hoon Jung,Y.W.Lee		
111538	MTL0580142	Tc(on) = 37.6 K.	(Mg,Au)B2	Mg0.854Au0.146B2	Mg	0.854	Au	0.146	B	2																		1	2003																															A	4.612		8.525											hexagonal	K		25.6					25.6																																																																																																					Au-doping effects in the Mg1-xAuxB2 series			Department of Physics and State Key Laboratory for Microscopic Physics, Peking University, Beijing 100871, China	Materials Lett., 58(2003)142-145	J.D.Guo,X.L.Xu,X.Wang,Y.Z.Wang		
111539	MTL0580142	Tc(on) = 35 K.	(Mg,Au)B2	Mg0.764Au0.236B2	Mg	0.764	Au	0.236	B	2																		1	2003																																													hexagonal	K		24.5					24.5																																																																																																					Au-doping effects in the Mg1-xAuxB2 series			Department of Physics and State Key Laboratory for Microscopic Physics, Peking University, Beijing 100871, China	Materials Lett., 58(2003)142-145	J.D.Guo,X.L.Xu,X.Wang,Y.Z.Wang		
111540	MTL0580142	For x => 0.382, not single phase.	(Mg,Au)B2	Mg0.618Au0.382B2	Mg	0.618	Au	0.382	B	2																			2003																																													hexagonal	K					10																																																																																																							Au-doping effects in the Mg1-xAuxB2 series			Department of Physics and State Key Laboratory for Microscopic Physics, Peking University, Beijing 100871, China	Materials Lett., 58(2003)142-145	J.D.Guo,X.L.Xu,X.Wang,Y.Z.Wang		
111541	NMT0020653	Si-isotope, <30>Si and <28>Si were used. 437 cm(-1) phonon is important for s/c. delta-C/gamma*Tc = 1.52. gap from SP-heat measurements.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2003																												clathrate																		K		8.07					8.07						0.17	Si																																									3.6	10							mj/mol.K2	144		370																																										Mechanism of superconductivity in the polyhedral-network compound Ba8Si46			Graduate School of Science,Materials Science Osaka City University, 3-3-138, Osaka 558-8585, Japan	Nature Mat.Lett., 2(2003)653	J.Teraoka,K.M.Itoh,K.Tanigaki,S.Yamanaka,T.Shimizu,Y.Moritomo		
111542	P068180502	PENET measured using LC resonator.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2003																																														K		7.2					7.2																																									A		2500																																																										Evidence for unconventional superconductivity in the nonoxide perovskite MgCNi3 from penetration depth measurements			Department of Physics & Astronomy and USC NanoCenter, University of South Carolina, Columbia, South Carolina, USA	Phys.Rev.B, 68(2003)180502	A.Snezhko,R.J.Cava,R.Prozorov,T.He		
111543	SSC1270279	space-G = Imma. Int'l No. =74. delta-C = 13.2 mj/mol.K2. delta-C/gamma*Tc = 1.33.	La3Pd5Si	La3Pd5Si1	La	3	Pd	5	Si	1																			2003																															A	13.1316	7.4365	7.6496											orthorhombic	K		1.4					1.4																				kOe		1.405							kOe/K		1.454			MHC11543																						mj/mol.K2	13.4		164																																					arc-melting					Superconductivity in the new intermetallic compound La3Pd5Si			Department of CMP and MS, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Solid State Commun., 127(2003)279	D.C.Kundaliya,S.K.Malik		
111544	JPC0154809	amorphous.	Zr-Ti-Cu-Ni-Be	Zr46.75Ti8.25Cu7.5Ni10Be27.5	Zr	46.75	Ti	8.25	Cu	7.5	Ni	10	Be	27.5															2003																																													amorphous	K		1.84					1.84																				T		3.6							T/K		2.5																																																																	arc-melting. melt-quench method					Superconductivity of bulk Zr46.75Ti8.25Cu7.5Ni10Be27.5 metallic glass			Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	J. Phys.: Condens. Matter, 15(2003)4809	H.Y.Bai,P.Wen,Y.Li,Z.F.Zhao,Z.X.Liu		
111545	JPC0154809	crystallization of sample 11544. glass temp. = 623 K. cryst.temp. = 698 K.	Zr-Ti-Cu-Ni-Be	Zr46.75Ti8.25Cu7.5Ni10Be27.5	Zr	46.75	Ti	8.25	Cu	7.5	Ni	10	Be	27.5															2003																																														K		3.76					3.76																				T		3.2							T/K		1.2																																																																	crystallization of sample 11544.					Superconductivity of bulk Zr46.75Ti8.25Cu7.5Ni10Be27.5 metallic glass			Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	J. Phys.: Condens. Matter, 15(2003)4809	H.Y.Bai,P.Wen,Y.Li,Z.F.Zhao,Z.X.Liu		
111547	PR0489858	epsilon-TiNiSi type. space-G = Pnma. delta-C/gamma*Tc = 1.53	LaRhSb	La1Rh1Sb1	La	1	Rh	1	Sb	1																			1993																															A	7.547	4.696	7.898											orthorhombic	K		2.1					2.1																																																					MSP11547			mj/mol.K2	7.7		252																																					arc-melting					OBSERVATION OF SUPERCONDUCTIVITY IN LARHSB	199310			PHYS.REV.B,48(1993)9858	H.TAKEYA,H.Takeya,JR.,K.A.GSCHNEIDNER,K.A.Gschneider,Jr,S.K.MALIK,S.K.Malik		
111548	EPL0610254	penetration depth by muon-SR. two gaps. table value is the higher one. the lower gap, 2*gap/kTc = 1.25	Mg(B,C)2	Mg1B1.98C0.02	Mg	1	B	1.98	C	0.02																			2003																												AlB2																	AlB2, C32	K		37.2					37.2																																									nm		97.2					3.62																																																(Mg,a-B,C) mixture, heat(900C,2h)					Muon-SR study of carbon-doped MgB2 superconductors			School of Chemistry, Physics and Environmental Science, University of Sussex Brighton BN1 9QJ, UK	Europhys.Lett., 61(2003)254	A.Schenck,J.Arvanitidis,K.Papagelis,K.Prassides,T.Takenobu,Y.Iwasa		
111549	EPL0610254	penetration depth by muon-SR. two gaps. table value is the higher one. the lower gap, 2*gap/kTc = 0.966	Mg(B,C)2	Mg1B1.96C0.04	Mg	1	B	1.96	C	0.04																			2003																												AlB2																	AlB2, C32	K		36.1					36.1																																									nm		98.5					3.35																																																(Mg,a-B,C) mixture, heat(900C,2h)					Muon-SR study of carbon-doped MgB2 superconductors			School of Chemistry, Physics and Environmental Science, University of Sussex Brighton BN1 9QJ, UK	Europhys.Lett., 61(2003)254	A.Schenck,J.Arvanitidis,K.Papagelis,K.Prassides,T.Takenobu,Y.Iwasa		
111550	EPL0610254	penetration depth by muon-SR. two gaps. table value is the higher one. the lower gap, 2*gap/kTc = 0.869	Mg(B,C)2	Mg1B1.94C0.06	Mg	1	B	1.94	C	0.06																			2003																												AlB2																	AlB2, C32	K		34.8					34.8																																									nm		100.6					3.21																																																(Mg,a-B,C) mixture, heat(900C,2h)					Muon-SR study of carbon-doped MgB2 superconductors			School of Chemistry, Physics and Environmental Science, University of Sussex Brighton BN1 9QJ, UK	Europhys.Lett., 61(2003)254	A.Schenck,J.Arvanitidis,K.Papagelis,K.Prassides,T.Takenobu,Y.Iwasa		
111551	P065224416	Hc2 defined as onset of ac-sus.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2002																												LuNi2B2C																		K																																									MHC11551																																																														floating zone, ANN(1435C in Ar)					Tuning of upper critical field anisotropy in TbxY1-xNi2B2C			Leibniz-Institut fur Festkorper- und Werkstoffforschung Dresden, Dresden, Germany	Phys.Rev.B, 65(2002)224416	G.Behr,G.Fuchs,H.Bitterlich,K.-H.Muller,K.Kenkov,L.Schultz,S.-L.Drechsler,W.Loser		
111552	P065224416	Hc2 defined as onset of ac-sus.	(Y,Tb)Ni2B2C	Y0.9Tb0.1Ni2B2C1	Y	0.9	Tb	0.1	Ni	2	B	2	C	1														3	2002																												LuNi2B2C																		K																																									MHC11552																																																														floating zone, ANN(1435C in Ar)					Tuning of upper critical field anisotropy in TbxY1-xNi2B2C			Leibniz-Institut fur Festkorper- und Werkstoffforschung Dresden, Dresden, Germany	Phys.Rev.B, 65(2002)224416	G.Behr,G.Fuchs,H.Bitterlich,K.-H.Muller,K.Kenkov,L.Schultz,S.-L.Drechsler,W.Loser		
111553	P065224416	Hc2 defined as onset of ac-sus.	(Y,Tb)Ni2B2C	Y0.8Tb0.2Ni2B2C1	Y	0.8	Tb	0.2	Ni	2	B	2	C	1														3	2002																												LuNi2B2C																		K																																									MHC11553																																																														floating zone, ANN(1435C in Ar)					Tuning of upper critical field anisotropy in TbxY1-xNi2B2C			Leibniz-Institut fur Festkorper- und Werkstoffforschung Dresden, Dresden, Germany	Phys.Rev.B, 65(2002)224416	G.Behr,G.Fuchs,H.Bitterlich,K.-H.Muller,K.Kenkov,L.Schultz,S.-L.Drechsler,W.Loser		
111554	P065224416	Hc2 defined as onset of ac-sus.	(Y,Tb)Ni2B2C	Y0.7Tb0.3Ni2B2C1	Y	0.7	Tb	0.3	Ni	2	B	2	C	1														3	2002																												LuNi2B2C																		K																																									MHC11554																																																														floating zone, ANN(1435C in Ar)					Tuning of upper critical field anisotropy in TbxY1-xNi2B2C			Leibniz-Institut fur Festkorper- und Werkstoffforschung Dresden, Dresden, Germany	Phys.Rev.B, 65(2002)224416	G.Behr,G.Fuchs,H.Bitterlich,K.-H.Muller,K.Kenkov,L.Schultz,S.-L.Drechsler,W.Loser		
111555	P065224416	Hc2 defined as onset of ac-sus.	(Y,Tb)Ni2B2C	Y0.6Tb0.4Ni2B2C1	Y	0.6	Tb	0.4	Ni	2	B	2	C	1														3	2002																												LuNi2B2C																		K																																									MHC11555																																																														floating zone, ANN(1435C in Ar)					Tuning of upper critical field anisotropy in TbxY1-xNi2B2C			Leibniz-Institut fur Festkorper- und Werkstoffforschung Dresden, Dresden, Germany	Phys.Rev.B, 65(2002)224416	G.Behr,G.Fuchs,H.Bitterlich,K.-H.Muller,K.Kenkov,L.Schultz,S.-L.Drechsler,W.Loser		
111556	PR03100656		LaRh3B2	La1Rh3B2	La	1	Rh	3	B	2																			1985																																														K		2.32					2.32																																																																																																arc-melting					Anomalous ferromagnetism in CeRh3B2: Possibility of a new Kondo-lattice state				Phys.Rev.B, 31(1985)656	J.S.Schilling,R.N.Shelton,S.A.Shaheen		
111557	PR03100656		(La,Ce)Rh3B2	La0.9989Ce0.0011Rh3B2	La	0.9989	Ce	0.0011	Rh	3	B	2																	1985																																														K		1.67					1.67																																																																																																arc-melting					Anomalous ferromagnetism in CeRh3B2: Possibility of a new Kondo-lattice state				Phys.Rev.B, 31(1985)656	J.S.Schilling,R.N.Shelton,S.A.Shaheen		
111558	PR03100656		(La,Ce)Rh3B2	La0.9978Ce0.0022Rh3B2	La	0.9978	Ce	0.0022	Rh	3	B	2																	1985																																														K		1.07					1.07																																																																																																arc-melting					Anomalous ferromagnetism in CeRh3B2: Possibility of a new Kondo-lattice state				Phys.Rev.B, 31(1985)656	J.S.Schilling,R.N.Shelton,S.A.Shaheen		
111559	PR03100656		(La,Ce)Rh3B2	La0.9973Ce0.0027Rh3B2	La	0.9973	Ce	0.0027	Rh	3	B	2																	1985																																														K		0.38					0.38																																																																																																arc-melting					Anomalous ferromagnetism in CeRh3B2: Possibility of a new Kondo-lattice state				Phys.Rev.B, 31(1985)656	J.S.Schilling,R.N.Shelton,S.A.Shaheen		
111560	PLA1130330	not CeCo3B2-type. kaizero = 6.88 E-4 emu/mol. e-ph interaction = 0.47.	CeOs3B2	Ce1Os3B2	Ce	1	Os	3	B	2																			1985							0																																							K		3.5					3.5																																																								mj/mol.K2	40.1		450																																					arc-melting					Superconductivity in the ternary borides CeOs3B2 and CeRu3B2: magnetic susceptibility and specific heat measurements				Phys.Lett., 113A(1985)330	A.M.Umarji,G.K.Shenoy,K.S.Athreya,L.S.Hausermann-Berg,R.N.Shelton,S.K.Malik		
111561	PLA1130330	kaizero = 2.74 E-4 emu/mol. e-ph interaction = 0.41. (delta-C/gamma*Tc) = 1.42	CeRu3B2	Ce1Ru3B2	Ce	1	Ru	3	B	2																			1985							0																					CeCo3B2			A	5.533		2.997												K		1.1					1.1																																																								mj/mol.K2	15.6		288																																					arc-melting					Superconductivity in the ternary borides CeOs3B2 and CeRu3B2: magnetic susceptibility and specific heat measurements				Phys.Lett., 113A(1985)330	A.M.Umarji,G.K.Shenoy,K.S.Athreya,L.S.Hausermann-Berg,R.N.Shelton,S.K.Malik		
111562	EPL0620412	PENET measured by surface impedance (5.5 GHz), well described by T^1.5.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2003																																														K		2.25					2.25																																									A		2810																																																					self-flux method					London penetration depth measurements of the heavy-fermion superconductor CeCoIn5 near a magnetic quantum critical point			Cavendish Laboratory, University of Cambridge, Madingley Road, Cambridge CB3 0HE, UK	Eur.Phys.JLett., 62(2003)412	B.Morgan,C.P.Bidinosti,D.M.Broun,J.L.Sarrao,J.R.Waldram,M.Raudsepp,P.J.Turner,R.K.W.Haselwimmer,S.Ozcan,Saeid Kamal		
111563	L092027003	space-G: P4mm (No.99). moment = 2.54 myu-B/Ce.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																			2004							-46	2.2																				CePt3B			A	4.072		5.442												K		0.75					0.75																				T		5							T/K		8.5			MHC11563																						mj/mol.K2	360																																							arc-melting, heat (870C,3w,in vac)					Heavy Fermion Superconductivity and Magnetic Order in Noncentrosymmetric CePt3Si			1Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.Lett., 92(2004)27003	A.Gribanov,Ch.Paul,E.Bauer,E.W.Scheidt,G.Hilscher,H.Michor,H.Noel,M.Sigrist,P.Rogl,Yu.Seropegin		
111564	L092027003	not s/c.	LaPt3Si	La1Pt3Si1	La	1	Pt	3	Si	1																			2004																												CePt3B			A	4.115		5.438												K					3																																																										mj/mol.K2	9		255																																					arc-melting, heat (870C,3w,in vac)					Heavy Fermion Superconductivity and Magnetic Order in Noncentrosymmetric CePt3Si			1Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.Lett., 92(2004)27003	A.Gribanov,Ch.Paul,E.Bauer,E.W.Scheidt,G.Hilscher,H.Michor,H.Noel,M.Sigrist,P.Rogl,Yu.Seropegin		
111565	P068214518	space-G: I4/mmm. dTc/dx = -100 K/mol(Fe). Re-entrant to normal (5.7 K), then s/c (5.5 K). Weak ferromagnetism at 2.2 K. Mossbauer also measured.	Er(Ni,Fe)2B2C	Er1Ni1.96Fe0.04B2C0.99	Er	1	Ni	1.96	Fe	0.04	B	2	C	0.99														1	2003								5.9																				LuNi2B2C			A	3.501		10.563												K		7.3					7.3																																																																																																induction furnace, ANN(1100C,6d)					Magnetic structure in the zero-applied-field reentrant superconductor ErNi1.96Fe0.04B2C0.99			LCMTR-CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Phys.Rev.B, 68(2003)214518	C.Godart,E.Alleno,G.Andre,L.C.Gupta,P.Bonville,R.Nagarajan,S.K.Dhar,S.M.Pattalwar		
111566	P069024509	Table balues of Hc1, Hc2 are for H//a. For H//c, Hc1 = 165 Oe and Hc2 = 0.25 T. Neel-T from sp-heat.	(Er,Tb)Ni2B2C	Er0.8Tb0.2Ni2B2C1	Er	0.8	Tb	0.2	Ni	2	B	2	C	1														3	2004								6.8																				LuNi2B2C																		K		3.7					3.7											Oe		115							T		0.22												MHC11566																						mj/mol.K2	18.9																																							floating zone, ANN(1400C,100h)					Magnetic and superconducting phase diagrams of single-crystal Er0.8R0.2Ni2B2C (R=Tb, Lu) and ErNi1.9Co0.1B2C: Identification of pair-breaking mechanisms			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0047, Japan	Phys.Rev.B, 69(2004)24509	H.Takeya,M.El Massalami		
111567	P069024509	Table balues of Hc1, Hc2 are for H//a. For H//c, Hc1 = 625 Oe and Hc2 = 2.39 T. Neel-T from sp-heat.	(Er,Lu)Ni2B2C	Er0.8Lu0.2Ni2B2C1	Er	0.8	Lu	0.2	Ni	2	B	2	C	1														3	2004								4.9																				LuNi2B2C																		K		10.8					10.8											Oe		585							T		1.47												MHC11567																						mj/mol.K2	16.2																																							floating zone, ANN(1400C,100h)					Magnetic and superconducting phase diagrams of single-crystal Er0.8R0.2Ni2B2C (R=Tb, Lu) and ErNi1.9Co0.1B2C: Identification of pair-breaking mechanisms			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0047, Japan	Phys.Rev.B, 69(2004)24509	H.Takeya,M.El Massalami		
111568	P069024509	Table balues of Hc1, Hc2 are for H//a. For H//c, Hc1 = 54 Oe and Hc2 = 0.13 T. Neel-T from sp-heat.	Er(Ni,Co)2B2C	Er1Ni1.9Co0.1B2C1	Er	1	Ni	1.9	Co	0.1	B	2	C	1														3	2004								5.4																				LuNi2B2C																		K		3.1					3.1											Oe		45							T		0.08												MHC11568																						mj/mol.K2	17.7																																							floating zone, ANN(1400C,100h)					Magnetic and superconducting phase diagrams of single-crystal Er0.8R0.2Ni2B2C (R=Tb, Lu) and ErNi1.9Co0.1B2C: Identification of pair-breaking mechanisms			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0047, Japan	Phys.Rev.B, 69(2004)24509	H.Takeya,M.El Massalami		
111569	P069024523	RRR=93. R(300K) = 155 uOhm.cm.  R(0 K) = 1.67 uOhm.cm.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2004																												skutterudite			A	9.301														K		1.83					1.83																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111570	P069024523	RRR=13. R(300K) = 235 uOhm.cm.  R(0 K) = 18.7 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os3.8Ru0.2Sb12	Pr	1	Os	3.8	Ru	0.2	Sb	12																3	2004																												skutterudite			A	9.3051														K		1.68					1.68																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111571	P069024523	RRR=5.6. R(300K) = 259 uOhm.cm.  R(0 K) = 46.0 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os3.6Ru0.4Sb12	Pr	1	Os	3.6	Ru	0.4	Sb	12																3	2004																												skutterudite			A	9.2995														K		1.58					1.58																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111572	P069024523	RRR=8.0. R(300K) = 215 uOhm.cm.  R(0 K) = 27.0 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os3.4Ru0.6Sb12	Pr	1	Os	3.4	Ru	0.6	Sb	12																3	2004																												skutterudite			A	9.295														K		1.53					1.53																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111573	P069024523	RRR=9.4. R(300K) = 510 uOhm.cm.  R(0 K) = 54.0 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os3.2Ru0.8Sb12	Pr	1	Os	3.2	Ru	0.8	Sb	12																3	2004																												skutterudite			A	9.3004														K		1.44					1.44																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111574	P069024523		Pr(Os,Ru)4Sb12	Pr1Os2.8Ru1.2Sb12	Pr	1	Os	2.8	Ru	1.2	Sb	12																3	2004																												skutterudite			A	9.2895														K		1.05					1.05																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111575	P069024523	RRR=5.9. R(300K) = 343 uOhm.cm.  R(0 K) = 58.2 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os2.4Ru1.6Sb12	Pr	1	Os	2.4	Ru	1.6	Sb	12																3	2004																												skutterudite			A	9.2875														K		1.14					1.14																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111576	P069024523		Pr(Os,Ru)4Sb12	Pr1Os2Ru2Sb12	Pr	1	Os	2	Ru	2	Sb	12																3	2004																												skutterudite			A	9.2875														K		0.8					0.8																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111577	P069024523	RRR=4.5. R(300K) = 305 uOhm.cm.  R(0 K) = 67.4 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os1.6Ru2.4Sb12	Pr	1	Os	1.6	Ru	2.4	Sb	12																3	2004																												skutterudite			A	9.2804														K		0.76					0.76																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111578	P069024523	RRR=4.8. R(300K) = 166 uOhm.cm.  R(0 K) = 34.8 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os1.2Ru2.8Sb12	Pr	1	Os	1.2	Ru	2.8	Sb	12																3	2004																												skutterudite			A	9.2802														K		0.81					0.81																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111579	P069024523		Pr(Os,Ru)4Sb12	Pr1Os1Ru3Sb12	Pr	1	Os	1	Ru	3	Sb	12																3	2004																												skutterudite			A	9.2774														K		0.84					0.84																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111580	P069024523		Pr(Os,Ru)4Sb12	Pr1Os0.6Ru3.4Sb12	Pr	1	Os	0.6	Ru	3.4	Sb	12																3	2004																												skutterudite			A	9.2723														K		0.97					0.97																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111581	P069024523	RRR=7.8. R(300K) = 330 uOhm.cm.  R(0 K) = 42.4 uOhm.cm.	Pr(Os,Ru)4Sb12	Pr1Os0.4Ru3.6Sb12	Pr	1	Os	0.4	Ru	3.6	Sb	12																3	2004																												skutterudite			A	9.27														K		1.04					1.04																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111582	P069024523		Pr(Os,Ru)4Sb12	Pr1Os0.2Ru3.8Sb12	Pr	1	Os	0.2	Ru	3.8	Sb	12																3	2004																												skutterudite			A	9.2693														K		1.16					1.16																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111583	P069024523	RRR=14. R(300K) = 578 uOhm.cm.  R(0 K) = 41.8 uOhm.cm.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																		3	2004																												skutterudite			A	9.27														K		1.11					1.11																																																																																																Sb-flux method					Superconductivity and crystalline electric field effects in the filled skutterudite series Pr(Os1-xRux)4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California, USA	Phys.Rev.B, 69(2004)24523	M.B.Maple,N.A.Frederick,N.P.Butch,P.-C.Ho,T.D.Do,V.S.Zapf		
111584	1702	pressure-induced s/c. Tc(P=90 kbar) = 8.7 K, Tc(P=153 kbar) = 7.4 K. dTc/dP = -2.3 E-5 K/kbar at P=90 kbar.	Bi	Bi1	Bi	1																							1971																																														K		8.7			0		8.7			K/GPa	-0.23																																																																																																	Superconductivity of Bismuth, Barium, and Lead at pressures exceeding 100 kbar				ZH.EKSP.TEOR.FIZ.,61(1971)2357, Soviet Physics JETP, 34(1972)1263	E.M.DIZHUR,E.S.ITSKEVICH,M.A.IL'INA		
111585	172	dTc/dP = -1.1 E-5 K/kbar.  dTc/dP = -2.2 E-5 K/kbar for Pb(II).	Pb	Pb1	Pb	1																							1959																																														K										K/GPa	-0.11																																																																																																					PHYS.REV.LETT.,2(1959)500	B.T.MATTHIAS,E.CORENZWIT,R.A.HEIN,R.L.FALGE		
111586	SSC0490879	pressure-induced s/c. simple cubic. Tc(P=15 GPa) = 6 K.	P	P1	P	1																							1984																																													cubic	K		6			0		6																																																																																																					Anomalous superconductivity in black phosphorus under high pressures				Solid State Commun., 49(1984)879	H.Kawamura,I.Shirotani,K.Tachikawa		
111587	SSC0490879	pressure-induced s/c.  Ortho phase. Tc = 4 K, 5 K, 10.5 K, at P = 11, 13, 29 GPa, respectively.	P	P1	P	1																							1984																																													orthorhombic	K		4			0		4																																																																																																					Anomalous superconductivity in black phosphorus under high pressures				Solid State Commun., 49(1984)879	H.Kawamura,I.Shirotani,K.Tachikawa		
111588	SSC0490879	pressure-induced s/c. Rhombo-phase. Tc(P=8.7GPa) = 5.5 K, Tc(P=25.2GPa) = 6.2 K.	P	P1	P	1																							1984																																													rhombohedral	K		5.5			0		5.5																																																																																																					Anomalous superconductivity in black phosphorus under high pressures				Solid State Commun., 49(1984)879	H.Kawamura,I.Shirotani,K.Tachikawa		
111590	L089247004	two band gap. the higher=7.1 meV in TBL, the lower = 2.80 meV (2*gap/kTc = 1.096). measured by point contact tunneling.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38.2					38.2	GAP11590																																															4.32	1																																															high pressure (30-35 kbar) synthesis					Direct Evidence for Two-Band Superconductivity in MgB2 Single Crystals from Directional Point-Contact Spectroscopy in Magnetic Fields			INFM-Dipartimento di Fisica, Politecnico di Torino, Corso Duca degli Abruzzi 24, 10129 Torino, Italy	Phys.Rev.Lett., 89(2002)247004	D.Daghero,G.A.Ummarino,J.Jun,J.Karpinski,R.S.Gonnelli,S.M.Kazakov,V.A.Stepanov		
111591	PHC4030113		(Mg,Zn,Al)B2	Mg0.95Zn0.025Al0.025B2	Mg	0.95	Zn	0.025	Al	0.025	B	2																1	2004																												AlB2																	AlB2, C32	K		38.5					38.5																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111592	PHC4030113		(Mg,Zn,Al)B2	Mg0.9Zn0.05Al0.05B2	Mg	0.9	Zn	0.05	Al	0.05	B	2																1	2004																												AlB2			A	3.5192		3.0827											AlB2, C32	K		38.5					38.5																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111593	PHC4030113		(Mg,Zn,Al)B2	Mg0.8Zn0.1Al0.1B2	Mg	0.8	Zn	0.1	Al	0.1	B	2																1	2004																												AlB2			A	3.5034		3.079											AlB2, C32	K		34					34																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111594	PHC4030113		(Mg,Zn,Al)B2	Mg0.7Zn0.15Al0.15B2	Mg	0.7	Zn	0.15	Al	0.15	B	2																1	2004																												AlB2			A	3.4436		3.0744											AlB2, C32	K		28.6					28.6																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111595	PHC4030113		(Mg,Zn,Al)B2	Mg0.6Zn0.2Al0.2B2	Mg	0.6	Zn	0.2	Al	0.2	B	2																1	2004																												AlB2			A	3.4188		3.0685											AlB2, C32	K		7.5					7.5																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111596	PHC4030113	not s/c.	(Mg,Zn,Al)B2	Mg0.4Zn0.3Al0.3B2	Mg	0.4	Zn	0.3	Al	0.3	B	2																1	2004																												AlB2			A	3.3872		3.0602											AlB2, C32	K					4																																																																																																		solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111597	PHC4030113	not s/c.	(Mg,Zn,Al)B2	Mg0.2Zn0.4Al0.4B2	Mg	0.2	Zn	0.4	Al	0.4	B	2																1	2004																												AlB2			A	3.3184		3.0355											AlB2, C32	K					10																																																																																																		solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111600	JPS0730190	gap by NQR.	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	2004																															A	5.67		7.12												K		6.5					6.5																																																5.5	6																																															arc-melting					La-NQR Probe of Strong-Coupling s-Wave Superconductivity in LaRu3Si2			Department of Physics, Faculty of Engineering, Tokushima University, Tokushima ,Japan	J.Phys.Soc.Jpn, 73(2004)190	G.Ghosh,L.C.Gupta,T.Ohno,Y.Kawasaki,Y.Kishimoto		
111601	JPS0712035	Hc1(0), Hc2(0) are estimated from the data of Hc1(2.0K)=712Oe, Hc1(4.2K)=410Oe, Hc2(2.0K)=2.0T,Hc2(4.2K)=1.25T. Curie Const. = 5.54 E-4 K.emu/mol. G-L parameter = 4.7	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	2002							7.23																								A	5.67		7.12												K		6.5					6.5											Oe		1004							T		2.68														A		107			A		504																																																					arc-melting					Magnetic Susceptibility Study of LaRu3Si2			Department of Physics, Faculty of Engineering, Tokushima University, Tokushima ,Japan	J.Phys.Soc.Jpn, 71(2002)2035	G.Ghosh,K.Sumiyama,L.C.Gupta,T.Hihara,T.Ohno,Y.Kishimoto		
111602	PR04912051	G-L parameter = 10	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	1994																															A	5.675		7.115												K		7.5					7.5											Oe		100							T		2																																																																										arc-melting					Type-II superconductivity in a dilute magnetic system: La1-xTmxRu3Si2			Centre National de la Recherche Scientifique, 1 place A.Briand, Meudon,France	Phys.Rev.B, 49(1994)12051	A.Mauger,C.Godart,L.C.Gupta,M.Escorne		
111603	PR04912051	moment = 8.6 myu< B >/Tm. dTc/dx = -8 K/x.	(La,Tm)Ru3Si2	La0.92Tm0.08Ru3Si2	La	0.92	Tm	0.08	Ru	3	Si	2																1	1994							13.7																																							K		6.8					6.8																																																																																																arc-melting					Type-II superconductivity in a dilute magnetic system: La1-xTmxRu3Si2			Centre National de la Recherche Scientifique, 1 place A.Briand, Meudon,France	Phys.Rev.B, 49(1994)12051	A.Mauger,C.Godart,L.C.Gupta,M.Escorne		
111604	PR04912051	moment = 8.1 myu< B >/Tm. dTc/dx = -8 K/x.	(La,Tm)Ru3Si2	La0.84Tm0.16Ru3Si2	La	0.84	Tm	0.16	Ru	3	Si	2																1	1994							18.4																								A	5.635		7.08												K		6.1					6.1																																																																																																arc-melting					Type-II superconductivity in a dilute magnetic system: La1-xTmxRu3Si2			Centre National de la Recherche Scientifique, 1 place A.Briand, Meudon,France	Phys.Rev.B, 49(1994)12051	A.Mauger,C.Godart,L.C.Gupta,M.Escorne		
111605	PR03000444	R(300K)=67 uOhm.cm. R(Tn)=13 uOhm.cm. delta-C/gamma*Tc = 1.1. Debye-T from beta=0.8 mj/mol.K4.	CeRu3Si2	Ce1Ru3Si2	Ce	1	Ru	3	Si	2																			1984																															A	5.55		7.12												K		1.25					1.25																				T		0.24							T/K		0.25																									mj/mol.K2	39		245																																					arc-melting					Superconductivity in a mixed-valent system: CeRu3Si2			Institut fur Festkorperphysik,Technische Hochschule Darmstadt,Darmstadt, Germany	Phys.Rev.B, 30(1984)444	C.Godart,F.Steglich,L.C.Gupta,R.D.Parks,U.Rauchschwalbe,W.Lieke		
111606	P069054505	delta-C = 110 mj/mol.K. gamma from delta-C/gamma*Tc = 1.43. Three magnetic transitions (AF (5.2K), FM (6K), and another magnetic transition at 5.5 K) are observed in SP-heat.	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	2004							6	5.2																				LuNi2B2C																		K		8.04					8.04																																																								mj/mol.K2	9.6																																							flux method using Ni2B solvent					Specific heat study of the magnetic superconductor HoNi2B2C			Department of Physics and Material Research Laboratory, University of Illinois at Urbana-Champaign, Illinois 61801, USA	Phys.Rev.B, 69(2004)054505	Eun Mi Choi,Heon Jung Kim,M.B.Salamon,Sung-Il Lee,Tuson Park		
111607	P069060504	gap(0.19 K) = 270 ueV. Tunneling spectra by TEM.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2004																																														K		1.85					1.85																																																3.4	11																																															melt in rich of Os, Sb					Very-low-temperature tunneling spectroscopy in the heavy-fermion superconductor PrOs4Sb12				Phys.Rev.B, 69(2004)060504	H.Suderow,J.D.Strand,P.C.Canfield,S.Bud'ko,S.Vieira		
111608	L092057001	For H//c, Hc1(0)=0.11 T and Hc2(0)=3 T estimated from figure. Anisotropy factor = 5 at low temperature.	MgB2	B2Mg1	B	2	Mg	1																				3	2004																												AlB2																	AlB2, C32	K		36.5					36.5											Oe		1120							T		13																																																																															Anisotropies of the Lower and Upper Critical Fields in MgB2 Single Crystals				Phys.Rev.Lett., 92(2004)57001	B.W.Kang,C.Marcenat,H.S.Lee,J.Marcus,K.H.Kim,L.Lyard,P.Azabo,S.I.Lee,T.Klein		
111609	P069100506	gap from ARPES measurements. gap=1.2 meV (at T=5.4 K). second gap=1.1 meV (at T=5.4 K)	Ca(Al,Si)2	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2004																												AlB2			A	4.19		4.3978											AlB2, C32	K		7.7					7.7																																																4.2	12																																															floating zone					Identical superconducting gap on different Fermi surfaces of Ca(Al0.5Si0.5)2 with the AlB2 structure			Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwa-no-ha, Kashiwa, Chiba, Japan	Phys.Rev.B, 69(2004)100506	I.Hase,M.Imai,S.Shin,S.Tsuda,T.Yokoya		
111610	PCS0312653	Thermopower = -6.53 uV/K at 30 C.	La(In,Sn)3	La1In2.25Sn0.75	La	1	In	2.25	Sn	0.75																		1	1970																												Cu3Au																		K		0.75					0.75	MTC11610																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111611	PCS0312653	Thermopower = 6.65 uV/K at 30 C.	La(In,Sn)3	La1In1.5Sn1.5	La	1	In	1.5	Sn	1.5																		1	1970																												Cu3Au																		K		1.19					1.19	MTC11610																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111612	PCS0312653	Thermopower = -6.88 uV/K at 30 C.	La(In,Sn)3	La1In0.75Sn2.25	La	1	In	0.75	Sn	2.25																		1	1970																												Cu3Au																		K		0.67					0.67	MTC11610																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111613	PCS0312653	Thermopower = 4.75 uV/K at 30 C.	(La,Th)Sn3	La0.87Th0.13Sn3	La	0.87	Th	0.13	Sn	3																		1	1970																												Cu3Au																		K		6.26					6.26	MTC11613																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111614	PCS0312653	Thermopower = 1.47 uV/K at 30 C.	(La,Th)Sn3	La0.5Th0.5Sn3	La	0.5	Th	0.5	Sn	3																		1	1970																												Cu3Au																		K		4.67					4.67	MTC11613																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111615	PCS0312653	Thermopower = -1.25 uV/K at 30 C.	(La,Th)Sn3	La0.25Th0.75Sn3	La	0.25	Th	0.75	Sn	3																		1	1970																												Cu3Au																		K		3.94					3.94	MTC11613																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111616	PCS0312653	Thermopower = -5.47 uV/K at 30 C.	La(Tl,Pb)3	La1Tl2.19Pb0.81	La	1	Tl	2.19	Pb	0.81																		1	1970																												Cu3Au																		K		1.37					1.37	MTC11616																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111617	PCS0312653	Thermopower = 6.86 uV/K at 30 C.	La(Tl,Pb)3	La1Tl1.5Pb1.5	La	1	Tl	1.5	Pb	1.5																		1	1970																												Cu3Au																		K		1.75					1.75	MTC11616																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111618	PCS0312653	Thermopower = 2.79 uV/K at 30 C.	La(Tl,Pb)3	La1Tl0.24Pb2.76	La	1	Tl	0.24	Pb	2.76																		1	1970																												Cu3Au																		K		4.46					4.46	MTC11616																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111619	PCS0312653		(La,Th)Pb3	La0.76Th0.24Pb3	La	0.76	Th	0.24	Pb	3																		1	1970																												Cu3Au																		K		1.46					1.46	MTC11619																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111620	PCS0312653	Thermopower = 18.5 uV/K at 30 C.	(La,Th)Pb3	La0.23Th0.77Pb3	La	0.23	Th	0.77	Pb	3																		1	1970																												Cu3Au																		K		2.61					2.61	MTC11619																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111621	PCS0312653	Thermopower = -4.77uV/K at 30 C.	(La,Th)Pb3	La0.06Th0.94Pb3	La	0.06	Th	0.94	Pb	3																		1	1970																												Cu3Au																		K		5.58					5.58	MTC11619																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111622	PCS0312653	Thermopower = -6.2uV/K at 30 C.	La(Tl,Sn)3	La1Tl2.25Sn0.75	La	1	Tl	2.25	Sn	0.75																		1	1970																												Cu3Au																		K		1.05					1.05	MTC11622																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111623	PCS0312653	Thermopower = 5.45uV/K at 30 C.	La(Tl,Sn)3	La1Tl1.5Sn1.5	La	1	Tl	1.5	Sn	1.5																		1	1970																												Cu3Au																		K		1.5					1.5	MTC11622																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111624	PCS0312653	Thermopower = -5.56uV/K at 30 C.	La(Tl,Sn)3	La1Tl0.75Sn2.25	La	1	Tl	0.75	Sn	2.25																		1	1970																												Cu3Au																		K		1.19					1.19	MTC11622																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111625	PCS0312653	Thermopower = -5.32uV/K at 30 C.	Y(In,Pb)3	Y1In2.25Pb0.75	Y	1	In	2.25	Pb	0.75																		1	1970																												Cu3Au																		K		0.6					0.6	MTC11625																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111626	PCS0312653	Thermopower = 4.68uV/K at 30 C.	Y(In,Pb)3	Y1In1.5Pb1.5	Y	1	In	1.5	Pb	1.5																		1	1970																												Cu3Au																		K		1					1	MTC11625																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111627	PCS0312653		Y(In,Pb)3	Y1In0.75Pb2.25	Y	1	In	0.75	Pb	2.25																		1	1970																												Cu3Au																		K		1.94					1.94	MTC11625																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111628	PCS0312653		Y(In,Sn)3	Y1In2.73Sn0.27	Y	1	In	2.73	Sn	0.27																		1	1970																												Cu3Au																		K		0					0	MTC11628																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111629	PCS0312653	Thermopower = -3.59uV/K at 30 C.	Y(In,Sn)3	Y1In2.25Sn0.75	Y	1	In	2.25	Sn	0.75																		1	1970																												Cu3Au																		K		0.69					0.69	MTC11628																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111630	PCS0312653	Thermopower = 3.2uV/K at 30 C.	Y(In,Sn)3	Y1In1.71Sn1.29	Y	1	In	1.71	Sn	1.29																		1	1970																												Cu3Au																		K		1.49					1.49	MTC11628																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111631	PCS0312653		Th(In,Sn)3	Th1In2.25Sn0.75	Th	1	In	2.25	Sn	0.75																		1	1970																												Cu3Au																		K		0.21					0.21	MTC11631																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111632	PCS0312653		Th(In,Sn)3	Th1In1.5Sn1.5	Th	1	In	1.5	Sn	1.5																		1	1970																												Cu3Au																		K		1.03					1.03	MTC11631																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111633	PCS0312653		Th(In,Sn)3	Th1In0.75Sn2.25	Th	1	In	0.75	Sn	2.25																		1	1970																												Cu3Au																		K		3.36					3.36	MTC11631																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111634	PCS0312653		Ca(Tl,Pb)3	Ca1Tl2.4Pb0.6	Ca	1	Tl	2.4	Pb	0.6																		1	1970																												Cu3Au																		K		3.18					3.18	MTC11634																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111635	PCS0312653		Ca(Tl,Pb)3	Ca1Tl1.8Pb1.2	Ca	1	Tl	1.8	Pb	1.2																		1	1970																												Cu3Au																		K		2.8					2.8	MTC11634																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111636	PCS0312653		Ca(Tl,Pb)3	Ca1Tl0.75Pb2.25	Ca	1	Tl	0.75	Pb	2.25																		1	1970																												Cu3Au																		K		3.68					3.68	MTC11634																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111637	PCS0312653		La(Pb,Sn)3	La1Pb2.25Sn0.75	La	1	Pb	2.25	Sn	0.75																		1	1970																												Cu3Au			A	4.8702														K		1.11					1.11	MTC11637																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111638	PCS0312653		La(Pb,Sn)3	La1Pb1.5Sn1.5	La	1	Pb	1.5	Sn	1.5																		1	1970																												Cu3Au			A	4.8368														K		1.18					1.18	MTC11637																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111639	PCS0312653		La(Pb,Sn)3	La1Pb0.75Sn2.25	La	1	Pb	0.75	Sn	2.25																		1	1970																												Cu3Au			A	4.805														K		2.54					2.54	MTC11637																																																																																															arc melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
111640	CEM1750237		Ba8Si46	Ba8Si46	Ba	8	Si	46																				1	2003																												clathrate			A	10.3446														K		8.1					8.1																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111641	CEM1750237	Ba deficiency at Ba-site.	Ba8(Si,Ge)46	Ba8Si43Ge3	Ba	8	Si	43	Ge	3																		1	2003																												clathrate			A	10.3446														K		7.1					7.1																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111642	CEM1750237	Ba deficiency at Ba-site.	Ba8(Si,Ge)46	Ba8Si40Ge6	Ba	8	Si	40	Ge	6																		1	2003																												clathrate			A	10.3533														K		6					6																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111643	CEM1750237	Ba deficiency at Ba-site.	Ba8(Si,Ge)46	Ba8Si37Ge9	Ba	8	Si	37	Ge	9																		1	2003																												clathrate			A	10.3815														K		5					5																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111644	CEM1750237	Ba deficiency at Ba-site.	Ba8(Si,Ge)46	Ba8Si34Ge12	Ba	8	Si	34	Ge	12																		1	2003																												clathrate			A	10.4054														K		4					4																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111645	CEM1750237		Ba8(Si,Ge)46	Ba8Si31Ge15	Ba	8	Si	31	Ge	15																		1	2003																												clathrate			A	10.4315														K		3.91					3.91																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111646	CEM1750237		Ba8(Si,Ge)46	Ba8Si28Ge18	Ba	8	Si	28	Ge	18																		1	2003																												clathrate			A	10.463														K		3.12					3.12																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111647	CEM1750237		Ba8(Si,Ge)46	Ba8Si25Ge21	Ba	8	Si	25	Ge	21																		1	2003																												clathrate			A	10.4815														K		2.8					2.8																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111648	CEM1750237		Ba8(Si,Ge)46	Ba8Si23Ge23	Ba	8	Si	23	Ge	23																		1	2003																												clathrate			A	10.499														K		2.28					2.28																																																																																																high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111649	CEM1750237	not s/c	Ba8(Si,Ge)46	Ba8Si19Ge27	Ba	8	Si	19	Ge	27																			2003																												clathrate			A	10.5663														K					2																																																																																																		high pressure synthesis (3GPa,800C) from BaSi2&BaGe2					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111650	CEM1750237		Ba8Si46	Ba7.76Si46	Ba	7.76	Si	46																					2003																												clathrate																		K		8					8																																																																																																					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111651	CEM1750237		Ba8Si46	Ba6.63Si46	Ba	6.63	Si	46																					2003																												clathrate																		K		6					6																																																																																																					Superconductivity and crystal structure of the solid solutions of Ba8-dSi46-xGex (0= < x= < 23) with Type I clathrate structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 175(2003)237	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111652	PHB3280023	two gaps, higher one is gap=9 - 10 meV(table value). small one (2*gap/kTc = 1.3). gap measured by break junction tunneling.	MgB2	B2Mg1	B	2	Mg	1																				1	2003																												AlB2																	AlB2, C32	K		39					39																																																3.8	1																																																				Tunneling spectroscopy of MgB2 and Li0.5(THF)yHfNCl			Faculty of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Physica B, 328(2003)23	H.Fujii,J.Akimitsu,S.Yamanaka,T.Ekino,T.Muranaka,T.Takasaki		
111653	PHB3280023	M is THF( = C4H8O). 2*gap = 11 - 12 meV. gap measured by break junction tunneling.	Li(THF)HfNCl	Li0.5M0.3Hf1N1Cl1	Li	0.5	M	0.3	Hf	1	N	1	Cl	1														1	2003																																														K		26					26																																																5.6	1																																																				Tunneling spectroscopy of MgB2 and Li0.5(THF)yHfNCl			Faculty of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Physica B, 328(2003)23	H.Fujii,J.Akimitsu,S.Yamanaka,T.Ekino,T.Muranaka,T.Takasaki		
111654	PHC4020283	pristine phase=beta-HfNCl. powder sample. Na-content is average value. lattice constant at 8K.	NaxHfNCl	Na0.18Hf1N1Cl1	Na	0.18	Hf	1	N	1	Cl	1																	2004																															A	3.5864		29.58												K		22					22																																																																																																					Structural Study on NaxHfNCl System			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physica C, 402(2004)283	K.Takeuchi,S.Shamoto,S.Yamanaka,T.Kajitani		
111655	PHC4020283	pristine phase=beta-HfNCl. powder sample. Na-content is average value. lattice constant at 4K.	NaxHfNCl	Na0.29Hf1N1Cl1	Na	0.29	Hf	1	N	1	Cl	1																	2004																															A	3.5892		29.722												K		19					19																																																																																																					Structural Study on NaxHfNCl System			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physica C, 402(2004)283	K.Takeuchi,S.Shamoto,S.Yamanaka,T.Kajitani		
111656	PHC4020283	pristine phase=beta-HfNCl. powder sample. Na-content is average value. lattice constant at 4K. sample is mixture of s/c phase and non-s/c phase (x=0.9).	NaxHfNCl	Na0.8Hf1N1Cl1	Na	0.8	Hf	1	N	1	Cl	1																	2004																															A	3.583		29.74												K		19					19																																																																																																					Structural Study on NaxHfNCl System			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physica C, 402(2004)283	K.Takeuchi,S.Shamoto,S.Yamanaka,T.Kajitani		
111657	P063020508	powder sample oriented ab-plane. M is THF(=C4H8O).  Hc2 defined by magnetization. For H//c, Hc1(0)=33.5Oe, Hc2(0)=9.3T, -dHc2/dT=0.51T/K, cohere=15.9A, penet=1.73 um, G-L=78.	Li(THF)HfNCl	Li0.48M0.3Hf1N1Cl1	Li	0.48	M	0.3	Hf	1	N	1	Cl	1															2001																																														K		26					26											Oe		8.9							T		34.8							T/K		1.88			MHC11657		A		59.6			A		4630																																																										Evidence for quasi-two-dimensional superconductivity in electron-doped Li0.48(THF)yHfNCl			Department of Physics, Tokyo Metropolitan University, Minami-osawa, Hachi-oji, Tokyo, 192-0397, Japan	Phys.Rev.B, 63(2001)20508	H.Tou,S.Yamanaka,T.Koiwasaki,Y.Maniwa		
111658	PHC3060007	space group = R3(-)m (#166). lattice constant at 4K.	LixZrNCl	Li0.16Zr1N1Cl1	Li	0.16	Zr	1	N	1	Cl	1																	1998																															A	3.6016		27.694												K		15					15																																																																																																ZrH2,NH4Cl react (650C,30min) in NH3 gas.					Structures of beta-ZrNCl and superconducting Li0.16ZrNCl: double honeycomb lattice superconductor			Department of Applied Physics, Tohoku UniIersity, Sendai 980-8579, Japan	Physica C, 306(1998)7	K.Ohoyama,M.Ohashi,S.Shamoto,T.Kajitani,T.Kato,Y.Miyazaki,Y.Ono,Y.Yamaguchi		
111659	CHM0092127	M is PC(propylene carbonate). PC-content not given. basal spacing = 2.24 nm by co-intercalation of Li and PC.	Li(PC)xZrNCl	Li0.16M1Zr1N1Cl1	Li	0.16	M	1	Zr	1	N	1	Cl	1															1997																																														K		14					14																																																																																																					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111660	CHM0092127	M is DMF(dimethylformamide). DMF-content not given. basal spacing = 1.98 nm by co-intercalation of Li and DMF.	Li(DMF)xZrNCl	Li0.16M1Zr1N1Cl1	Li	0.16	M	1	Zr	1	N	1	Cl	1															1997																																														K		14					14																																																																																																					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111661	CHM0092127		LixZrNCl	Li0.14Zr1N1Cl1	Li	0.14	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111662	CHM0092127		LixZrNCl	Li0.28Zr1N1Cl1	Li	0.28	Zr	1	N	1	Cl	1																	1997																																														K		15.2					15.2																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111663	CHM0092127		LixZrNCl	Li0.55Zr1N1Cl1	Li	0.55	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111664	CHM0092127		LixZrNCl	Li0.65Zr1N1Cl1	Li	0.65	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111665	CHM0092127		LixZrNCl	Li0.95Zr1N1Cl1	Li	0.95	Zr	1	N	1	Cl	1																	1997																																														K		13.4					13.4																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111666	CHM0092127		LixZrNCl	Li1.3Zr1N1Cl1	Li	1.3	Zr	1	N	1	Cl	1																	1997																																														K		11					11																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111667	CHM0092127		LixZrNCl	Li1.4Zr1N1Cl1	Li	1.4	Zr	1	N	1	Cl	1																	1997																																														K		10					10																																																																																																reaction(beta-ZrNCl + Li-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111668	CHM0092127		NaxZrNCl	Na0.5Zr1N1Cl1	Na	0.5	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + Na-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111669	CHM0092127		NaxZrNCl	Na0.59Zr1N1Cl1	Na	0.59	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + Na-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111670	CHM0092127		NaxZrNCl	Na0.66Zr1N1Cl1	Na	0.66	Zr	1	N	1	Cl	1																	1997																																														K		14.5					14.5																																																																																																reaction(beta-ZrNCl + Na-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111671	CHM0092127		NaxZrNCl	Na0.75Zr1N1Cl1	Na	0.75	Zr	1	N	1	Cl	1																	1997																																														K		14.3					14.3																																																																																																reaction(beta-ZrNCl + Na-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111672	CHM0092127		NaxZrNCl	Na1.38Zr1N1Cl1	Na	1.38	Zr	1	N	1	Cl	1																	1997																																														K		11					11																																																																																																reaction(beta-ZrNCl + Na-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111673	CHM0092127		KxZrNCl	K0.22Zr1N1Cl1	K	0.22	Zr	1	N	1	Cl	1																	1997																																														K		15.2					15.2																																																																																																reaction(beta-ZrNCl + K-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111674	CHM0092127		KxZrNCl	K0.4Zr1N1Cl1	K	0.4	Zr	1	N	1	Cl	1																	1997																																														K		15.2					15.2																																																																																																reaction(beta-ZrNCl + K-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111675	CHM0092127		KxZrNCl	K0.46Zr1N1Cl1	K	0.46	Zr	1	N	1	Cl	1																	1997																																														K		15					15																																																																																																reaction(beta-ZrNCl + K-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111676	CHM0092127		KxZrNCl	K0.6Zr1N1Cl1	K	0.6	Zr	1	N	1	Cl	1																	1997																																														K		14.4					14.4																																																																																																reaction(beta-ZrNCl + K-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111677	CHM0092127		KxZrNCl	K0.77Zr1N1Cl1	K	0.77	Zr	1	N	1	Cl	1																	1997																																														K		13.5					13.5																																																																																																reaction(beta-ZrNCl + K-naphthalenes)					Superconductivity of alkali metal intercalated beta-zirconium nitride chloride, AxZrNCl (A = Li, Na, K)			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739, Japan	Chem.Mater., 9(1997)2127	H.Kawaji,K.Hotehama,S.Yamanaka		
111678	JPS0730530	space-G=I4<->3d. impurity phase(C, Y2O3, YC2, Y2OxCy). s/c volume fraction=10 %. PENET frm Hc1.	Y2C3	C3Y2	C	3	Y	2																					2004																															A	8.226													bcc	K		18					18	MTC11678										Oe		35																												A		4340																																																					heat(1600C,30min,P=4-5GPa) in BN					Superconductivity at 18K in Yttrium Sesquicarbide System, Y2C3			Department of Physics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa,Japan	J.Phys.Soc.Jpn, 73(2004)530	G.Amano,J.Akimitsu,S.Akutagawa,T.Muranaka,Y.Zenitani		
111681	MPB0173664	no structure change upto 15 GPa at RT. compressibility k<a>=1.3 E-3/GPa, k<c>=2.6 E-3/GPa. bulk modulus B=192 GPa. hydrostatic P. dTn/dP = +0.70 K/GPa.	HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																3	2003								5.2																				LuNi2B2C																		K		8.7					8.7	MTC11681		K/GPa	-0.46																																																																																												flux method					Electronic properties of magnetic superconductor HoNi2B2C under high pressure			Department of Physics, Kyushu University,Fukuoka,Japan	Int'l.J.Mod.Phys.B, 17(2003)3664	C.K.Cho,G.Oomi,N.Matsuda,P.C.Canfield,T.Kagayama		
111682	PHC4030113		(Mg,Li,Al)B2	Mg0.95Li0.025Al0.025B2	Mg	0.95	Li	0.025	Al	0.025	B	2																1	2004																												AlB2			A	3.5226		3.0822											AlB2, C32	K		38.2					38.2																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111683	PHC4030113		(Mg,Li,Al)B2	Mg0.9Li0.05Al0.05B2	Mg	0.9	Li	0.05	Al	0.05	B	2																1	2004																												AlB2			A	3.5214		3.0799											AlB2, C32	K		37.8					37.8																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111684	PHC4030113		(Mg,Li,Al)B2	Mg0.8Li0.1Al0.1B2	Mg	0.8	Li	0.1	Al	0.1	B	2																1	2004																												AlB2			A	3.4526		3.0763											AlB2, C32	K		31					31																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111685	PHC4030113		(Mg,Li,Al)B2	Mg0.7Li0.15Al0.15B2	Mg	0.7	Li	0.15	Al	0.15	B	2																1	2004																												AlB2			A	3.4312		3.0726											AlB2, C32	K		25.1					25.1																																																																																																solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111686	PHC4030113	Tc not given.	(Mg,Li,Al)B2	Mg0.6Li0.2Al0.2B2	Mg	0.6	Li	0.2	Al	0.2	B	2																1	2004																												AlB2			A	3.403		3.0648											AlB2, C32	K																																																																																																							solid state reaction					Superconducting properties of Zn and Al double-doped Mg1-x(Zn0.5Al0.5)xB2			Materials Research Department, Riso National Laboratory, P.O. Box 49, 4000 Roskilde, Denmark	Physica C, 403(2004)113	A.B.Abrahamsen,G.J.Xu,J.-C.Grivel,N.H.Andersen,X.P.Chen		
111689	MPB0173493	thermopower s = 0.12 uV/K at RT.	(Lu,Gd)Ni2B2C	Lu0.88Gd0.12Ni2B2C1	Lu	0.88	Gd	0.12	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		7.3					7.3																																		MHC11689																																																																			Transport properties and upper critical field of single crystal non-magnetic LuxY1-xNi2B2C and magnetic LuxGd1-xNi2B2C			Department of Physics,Texas A&M University,Collge Station,USA	Int'l.J.Mod.Phys.B, 17(2003)3493	A.C.Dumar,D.G.Naugle,K.D.D.Rathnayaka,M.P.Anatska,P.C.Canfield		
111690	MPB0173493		(Lu,Y)Ni2B2C	Lu0.5Y0.5Ni2B2C1	Lu	0.5	Y	0.5	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		14.9					14.9																																		MHC11690																																																																			Transport properties and upper critical field of single crystal non-magnetic LuxY1-xNi2B2C and magnetic LuxGd1-xNi2B2C			Department of Physics,Texas A&M University,Collge Station,USA	Int'l.J.Mod.Phys.B, 17(2003)3493	A.C.Dumar,D.G.Naugle,K.D.D.Rathnayaka,M.P.Anatska,P.C.Canfield		
111691	MPB0173493		(Lu,Y)Ni2B2C	Lu0.25Y0.75Ni2B2C1	Lu	0.25	Y	0.75	Ni	2	B	2	C	1															2003																												LuNi2B2C																		K		14.2					14.2																																		MHC11691																																																																			Transport properties and upper critical field of single crystal non-magnetic LuxY1-xNi2B2C and magnetic LuxGd1-xNi2B2C			Department of Physics,Texas A&M University,Collge Station,USA	Int'l.J.Mod.Phys.B, 17(2003)3493	A.C.Dumar,D.G.Naugle,K.D.D.Rathnayaka,M.P.Anatska,P.C.Canfield		
111692	PRL0240812	p-induced s/c. Pcr =100 kbar. s/c phase = Cs<5>.	Cs	Cs1	Cs	1																							1970																																														K		1.5			0		1.5	MPH11692																																																																																																				Pressure-induced superconductivity in cesium and yttrium			University of California,San Diego,La Jolla,California,USA	Phys.Rev.Lett., 24(1970)812	J.Wittig		
111693	PRL0240812	p-induced s/c. P,crit>=110 kbar. Tc at P=170 kbar. dTc/dP at P=110 kbar.	Y	Y1	Y	1																							1970																																														K		2.7			0		2.7	MTC11693		K/GPa	0.26																																																																																																	Pressure-induced superconductivity in cesium and yttrium			University of California,San Diego,La Jolla,California,USA	Phys.Rev.Lett., 24(1970)812	J.Wittig		
111694	INC0390056	density=3.60 g/cm3 by XRD. Hc2(2K)=6 T.	Ba8Si46	Ba8Si46	Ba	8	Si	46																				1	2000																												clathrate			A	10.328														K		8					8																																																																																																(arc-melt) - pellet - heat(1-5GPa,800c,1h)					High-Pressure Synthesis of a New Silicon Clathrate Superconductor, Ba8Si46			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima, Japan	Inorg.Chem., 39(2000)56	E.Enishi,H.Fukuoka,M.Yasukawa,S.Yamanaka		
111695	JP01011519	p-induced s/c. metallization at 115GPa. P<crit>=180 GPa. Tc(max)=2 K at 180 GPa. Tc=1.3 K at P=216 GPa.	CsI	Cs1I1	Cs	1	I	1																					1998																																														K		2					2																																																																																																					Metallization and superconductivity in CsI at pressures up to 220 GPa			Research Centre for Materials Science at Extreme Conditions, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Mater 10(1998)11519	K.Amaya,K.Shimizu,M.I.Eremets,T.C.Kobayashi		
111696	PCS0650333		BaxSi46	Ba6.62Si46	Ba	6.62	Si	46																					2004																												clathrate			A	10.288														K		5					5																																																																																																(3GPa,1273-973K,3h) - ANN(800K,24h)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111697	PCS0650333		BaxSi46	Ba6.63Si46	Ba	6.63	Si	46																					2004																												clathrate			A	10.262														K		6					6																																																																																																(3GPa,1573-973K,3h) - ANN(800K,24h)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111698	PCS0650333		BaxSi46	Ba7.61Si46	Ba	7.61	Si	46																					2004																												clathrate			A	10.331														K		8.2					8.2																																																																																																(3GPa,1573-973K,3h)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111699	PCS0650333		BaxSi46	Ba7.76Si46	Ba	7.76	Si	46																					2004																												clathrate			A	10.314														K		9					9																																																																																																(3GPa,1573-1073K,3h)					Synthesis and superconductivity of barium deficient type I silicon clathrate compounds, Ba8-xSi46			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Kagamiyama 1-4-1, Higashi?Hiroshima, Japan	J.Phys.Chem.Solids, 65(2004)333	H.Fukuoka,J.Kiyoto,S.Yamanaka		
111700	JPS0730194	Tc increases to 0.45 K under P=0.19 GPa. NQR measuements.	CeCu2(Si,Ge)2	Ce1Cu2Si1.96Ge0.04	Ce	1	Cu	2	Si	1.96	Ge	0.04																	2004								0.75																																						K		0.4					0.4																																																																																																					Exotic Superconductivity in the Coexistent Phase of Antiferromagnetism and Superconductivity in CeCu2(Si0:98Ge0:02)2: A Cu-NQR Study under Hydrostatic Pressure			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.Soc.Jpn, 73(2004)194	C.Geibel,F.Steglich,Guo-qing Zheng,K.Ishida,S.Kawasaki,T.Mito,Y.Kitaoka,Yu Kawasaki		
111701	P069134522	penet(in TBL) from muon-SR. penet from M is 4700 A. Hc2//c determined from M (Hao & Clem theory). layer distance c/3 = 9.4 A.. G-L parameter = 56	LixZrNCl	Li0.17Zr1N1Cl1	Li	0.17	Zr	1	N	1	Cl	1																	2004																																														K		14.2					14.2																				T		4.7												MHC11701		A		83			A		3700																																																										Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111702	P069134522	penet(in TBL) from muon-SR. layer distance c/3 = 9.4 A	LixZrNCl	Li0.4Zr1N1Cl1	Li	0.4	Zr	1	N	1	Cl	1																	2004																																														K		12.5					12.5																																									A		3900																																																										Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111703	P069134522	layer distance c/3 = 9.4 A	LixZrNCl	Li0.6Zr1N1Cl1	Li	0.6	Zr	1	N	1	Cl	1																	2004																																														K		11.7					11.7																																																																																																					Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111704	P069134522	M is THF(tetrahydrofuran). penet(in TBL) from muon-SR. penet from M is 4700 A. Hc2//c determined from M (Hao & Clem theory). layer distance c/3 = 13.3 A.. G-L parameter = 76	LixTHFyZrNCl	Li0.15M0.08Zr1N1Cl1	Li	0.15	M	0.08	Zr	1	N	1	Cl	1															2004																																														K		14.4					14.4																				T		4.2												MHC11704		A		88			A		5200																																																										Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111705	P069134522	M is PC(propyrene carbonate). layer distance c/3 = 13.3 A.	LixPCyZrNCl	Li0.18M0.15Zr1N1Cl1	Li	0.18	M	0.15	Zr	1	N	1	Cl	1															2004																																														K		14.6					14.6																																																																																																					Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111706	P069134522	M is THF(tetrahydrofuran). layer distance c/3 = 13.3 A.	LixTHFyHfNCl	Li0.24M0.14Hf1N1Cl1	Li	0.24	M	0.14	Hf	1	N	1	Cl	1															2004																																														K		25.5					25.5																																																																																																					Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111707	P069134522	M is THF(tetrahydrofuran). layer distance c/3 = 18.7 A. penet by muon-SR.	LixTHFyHfNCl	Li0.5M0.3Hf1N1Cl1	Li	0.5	M	0.3	Hf	1	N	1	Cl	1															2004																																														K		25.5					25.5																																									A		3900																																																										Two-dimensional nature of superconductivity in the intercalated layered systems LixHfNCl and LixZrNCl: Muon spin relaxation and magnetization measurements			Department of Physics, Columbia University, 538W 120th Street, New York, New York 10027, USA	Phys.Rev.B, 69(2004)134522	A.Fukaya,A.Savici,G.M.Luke,I.M.Gat-Malureanu,K.Groves,K.Hotehama,K.M.Kojima,M.I.Larkin,M.Rovers,P.Kyriakou,P.L.Russo,R.Breslow,S.Yamanaka,T.Ito,Y.Fudamoto,Y.J.Uemura		
111708	JP015S2201	Tc(onset)=7 K. Tc(sp-heat)=5.5 K. delta-C/gamma*Tc = 1.33	YFe4P12	Y1Fe4P12	Y	1	Fe	4	P	12																			2003																												skutterudite			A	7.789														K		7					7																																																					MSP11708			mj/mol.K2	27.2		553																																					high-P-synthesis(1050C,4GPa)					Superconductivity of new filled skutterudite YFe4P12 prepared at high pressure			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Matter, 15(2003)S2201	C.Sekine,I.Shirotani,K.Kihou,M.Ishikawa,N.Takeda,T.Yagi,Y.Shimaya		
111709	CEM1740032	density=5.292 g/cm3	TbFe4P12	Tb1Fe4P12	Tb	1	Fe	4	P	12																			2003																												skutterudite			A	7.7926														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111710	CEM1740032	density=5.324 g/cm3	DyFe4P12	Dy1Fe4P12	Dy	1	Fe	4	P	12																			2003																												skutterudite			A	7.789														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111711	CEM1740032	density=5.349 g/cm3	HoFe4P12	Ho1Fe4P12	Ho	1	Fe	4	P	12																			2003																												skutterudite			A	7.7854														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111712	CEM1740032	density=5.370 g/cm3	ErFe4P12	Er1Fe4P12	Er	1	Fe	4	P	12																			2003																												skutterudite			A	7.7832														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111713	CEM1740032	density=5.388 g/cm3	TmFe4P12	Tm1Fe4P12	Tm	1	Fe	4	P	12																			2003																												skutterudite			A	7.7802														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111714	CEM1740032	density=5.410 g/cm3	YbFe4P12	Yb1Fe4P12	Yb	1	Fe	4	P	12																			2003																												skutterudite			A	7.7832														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111715	CEM1740032	density=5.437 g/cm3	LuFe4P12	Lu1Fe4P12	Lu	1	Fe	4	P	12																			2003																												skutterudite			A	7.7771														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111716	CEM1740032	density=5.806 g/cm3	YFe4P12	Y1Fe4P12	Y	1	Fe	4	P	12																			2003																												skutterudite			A	7.7896														K		7					7																																																																																																high-P-synthesis(1000-1100C,4-5GPa)					Systematic high-pressure synthesis of newfilled skutterudites with heavy lanthanide, LnFe4P12 (Ln=heavy lanthanide, including Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	J.Solid State Chem., 174(2003)32	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111717	MRB0390317	density=8.069 g/cm3. moment = 7.94 m<B>. ferromag-.	EuOs4P12	Eu1Os4P12	Eu	1	Os	4	P	12																			2004																												skutterudite			A	8.0792														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111718	MRB0390317	density=8.163 g/cm3. moment = 8.54 m<B>. ferromag-.	GdOs4P12	Gd1Os4P12	Gd	1	Os	4	P	12																			2004																												skutterudite			A	8.0657														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111719	MRB0390317	density=8.182 g/cm3	TbOs4P12	Tb1Os4P12	Tb	1	Os	4	P	12																			2004																												skutterudite			A	8.0631														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111720	MRB0390317	density=8.214 g/cm3. moment = 10.63 m<B>. not magnetic order down to 2 K.	DyOs4P12	Dy1Os4P12	Dy	1	Os	4	P	12																			2004																												skutterudite			A	8.0601														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111721	MRB0390317	density=8.235 g/cm3	HoOs4P12	Ho1Os4P12	Ho	1	Os	4	P	12																			2004																												skutterudite			A	8.0579														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111722	MRB0390317	density=8.743 g/cm3	YOs4P12	Y1Os4P12	Y	1	Os	4	P	12																			2004																												skutterudite			A	8.0615														K		3					3																																																																																																high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111723	MRB0390317	density=8.113 g/cm3	SmOs4P12	Sm1Os4P12	Sm	1	Os	4	P	12																			2004																												skutterudite			A	8.0697														K					4																																																																																																		high-P-synthesis(1000-1100C,4-5GPa)					High-pressure synthesis, electrical and magnetic properties of new filled skutterudites LnOs4P12 (Ln = Eu, Gd, Tb, Dy, Ho, Y)			Muroran Institute of Technology, Mizumoto, Muroran-shi 050-8585, Japan	Mater.Res.Bull., 39(2004)317	C.Sekine,I.Shirotani,K.Kihou,T.Yagi,Y.Shimaya		
111724	PHB1350239	p-induced s/c. P<crit> = 10 GPa. Tc(P=10GPa) = 0.05 K. Tc(P=24GPa) = 2.7 K.	As	As1	As	1																							1985																																														K		2.7			0		2.7																																																																																																					Pressure-induced superconductivity of arsenic: Evidence for a structural phase transition				Physica B+C, 135(1985)239	H.Kawamura,J.Wittig		
111725	LT13-490	p-induced s/c. P<crit> = 4.5 GPa. Tc(max) = 0.6 K at 13 GPa.	Lu	Lu1	Lu	1																							1972																																														K		0.6			0		0.6																																																																																																					Superconductivity of lutetium at very high pressure: Implications with respect to the superconductivity of lanthanum				LT13(1972) vol.3 p=490,Boulder	C.Probst,J.Wittig,W.Wiedemann		
111726	LT13-490	p-induced s/c. P<crit> = 11 GPa(Tc=1.3 K). Tc(max) = 2.7 K at 17 GPa.	Y	Y1	Y	1																							1972																																														K		2.7					2.7																																																																																																					Superconductivity of lutetium at very high pressure: Implications with respect to the superconductivity of lanthanum				LT13(1972) vol.3 p=490,Boulder	C.Probst,J.Wittig,W.Wiedemann		
111727	P069180509	RRR=76. PENET measured using 21 MHz tunnel diode oscillator.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																			2004																												skutterudite																		K		1.25					1.25																																									A		2900					1.9																																																					Probing the superconducting gap symmetry of PrRu4Sb12 : A comparison with PrOs4Sb12			Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois, USA	Phys.Rev.B, 69(2004)180509	E.E.M.Chia,H.Sato,H.Sugawara,M.B.Salamon		
111728	L092217003	R = 0.5 uOhm.cm at 40 K	MgB2	B2Mg1	B	2	Mg	1																					2004																												AlB2																	AlB2, C32	K		39.2					39.2																				T		16												MHC11728																																																														(BCl3,H2,CH4), fiber heated(1100-1300C)					Systematic Effects of Carbon Doping on the Superconducting Properties of Mg(B1-xCx)2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 92(2004)217003	D.K.Finnemore,P.C.Canfield,R.H.T.Wilke,R.J.Suplinskas,S.L.Bud'ko,S.T.Hannahs		
111729	L092217003		Mg(B,C)2	Mg1B1.9906C0.0094	Mg	1	B	1.9906	C	0.0094																			2004																												AlB2																	AlB2, C32	K		38.5					38.5																				T		20												MHC11729																																																														(BCl3,H2,CH4), fiber heated(1100-1300C)					Systematic Effects of Carbon Doping on the Superconducting Properties of Mg(B1-xCx)2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 92(2004)217003	D.K.Finnemore,P.C.Canfield,R.H.T.Wilke,R.J.Suplinskas,S.L.Bud'ko,S.T.Hannahs		
111730	L092217003		Mg(B,C)2	Mg1B1.958C0.042	Mg	1	B	1.958	C	0.042																			2004																												AlB2																	AlB2, C32	K		37.9					37.9																				T		25												MHC11730																																																														(BCl3,H2,CH4), fiber heated(1100-1300C)					Systematic Effects of Carbon Doping on the Superconducting Properties of Mg(B1-xCx)2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 92(2004)217003	D.K.Finnemore,P.C.Canfield,R.H.T.Wilke,R.J.Suplinskas,S.L.Bud'ko,S.T.Hannahs		
111731	L092217003	R = 10 uOhm.cm at 40 K	Mg(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																			2004																												AlB2																	AlB2, C32	K		36.2					36.2																				T		32.5												MHC11731																																																														(BCl3,H2,CH4), fiber heated(1100-1300C)					Systematic Effects of Carbon Doping on the Superconducting Properties of Mg(B1-xCx)2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 92(2004)217003	D.K.Finnemore,P.C.Canfield,R.H.T.Wilke,R.J.Suplinskas,S.L.Bud'ko,S.T.Hannahs		
111732	PHC4050245	Tc(on) = 16 K	(Sc,Y)Ni2B2C	Sc0.9Y0.1Ni2B2C1	Sc	0.9	Y	0.1	Ni	2	B	2	C	1															2004																												LuNi2B2C			A	3.463		10.675												K		15.1					15.1																																																																																																arc-melting, ANN(900C,1w)					Y-induced stabilization of the superconducting phase in the Sc1-xYxNi2B2C system			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 405(2004)245	G.Behr,G.V.M.Kiruthika,L.C.Gupta,Ruta Kulkarni,S.K.Dhar		
111733	PHC4050245	Tc(on) = 15 K	(Sc,Y)Ni2B2C	Sc0.8Y0.2Ni2B2C1	Sc	0.8	Y	0.2	Ni	2	B	2	C	1															2004																												LuNi2B2C			A	3.477		10.646												K		14.8					14.8																																																																																																arc-melting, ANN(900C,1w)					Y-induced stabilization of the superconducting phase in the Sc1-xYxNi2B2C system			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 405(2004)245	G.Behr,G.V.M.Kiruthika,L.C.Gupta,Ruta Kulkarni,S.K.Dhar		
111734	PHC4050245		(Sc,Y)Ni2B2C	Sc0.7Y0.3Ni2B2C1	Sc	0.7	Y	0.3	Ni	2	B	2	C	1															2004																												LuNi2B2C			A	3.484		10.595												K		14.5					14.5																																																																																																arc-melting, ANN(900C,1w)					Y-induced stabilization of the superconducting phase in the Sc1-xYxNi2B2C system			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 405(2004)245	G.Behr,G.V.M.Kiruthika,L.C.Gupta,Ruta Kulkarni,S.K.Dhar		
111735	PHC3060001	RRR=45. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1998																												LuNi2B2C			A	3.4643		10.6346												K		16.6					16.6																				T		11.5																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111736	PHC3060001	RRR=11.5. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	(Y,Lu)Ni2B2C	Y0.16Lu0.84Ni2B2C1	Y	0.16	Lu	0.84	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4761		10.6217												K		15.2					15.2																				T		9.06																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111737	PHC3060001	RRR=10.2.	(Y,Lu)Ni2B2C	Y0.3Lu0.7Ni2B2C1	Y	0.3	Lu	0.7	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4856		10.6068												K		15					15																																																																																																arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111738	PHC3060001	RRR=10.2. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	(Y,Lu)Ni2B2C	Y0.5Lu0.5Ni2B2C1	Y	0.5	Lu	0.5	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4968		10.5949												K		14.5					14.5																				T		7.67																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111739	PHC3060001	RRR=9.6. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	(Y,Lu)Ni2B2C	Y0.75Lu0.25Ni2B2C1	Y	0.75	Lu	0.25	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5098		10.5732												K		14.9					14.9																				T		7.89																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111740	PHC3060001	RRR=8.4. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	(Y,Lu)Ni2B2C	Y0.84Lu0.16Ni2B2C1	Y	0.84	Lu	0.16	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5172		10.5593												K		14.8					14.8																				T		8																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111741	PHC3060001	RRR=13.9. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	(Y,Lu)Ni2B2C	Y0.92Lu0.08Ni2B2C1	Y	0.92	Lu	0.08	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5222		10.5529												K		15.2					15.2																				T		8.28																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111742	PHC3060001	RRR=22.9. Hc2(T) shown in Fig.4. Hc2(0) estimated from Hc2(T) by fitting.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	1998																												LuNi2B2C			A	3.5274		10.5437												K		15.5					15.5																				T		8.67																																																																										arc-melting					Superconductivity and disorder in YxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	Physica C, 306(1998)1	A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,S.-L.Drechsler,S.V.Shulga		
111743	MMM1870309		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	1998																												LuNi2B2C			A	3.4593		10.6294												K		16.6					16.6																																		MHC11743																																																														arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111744	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.15Lu0.85Ni2B2C1	Ho	0.15	Lu	0.85	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4729		10.6103												K		15.1					15.1																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111745	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.3Lu0.7Ni2B2C1	Ho	0.3	Lu	0.7	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4804		10.6032												K		13.3					13.3																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111746	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.45Lu0.55Ni2B2C1	Ho	0.45	Lu	0.55	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4961		10.573												K		10					10																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111747	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.6Lu0.4Ni2B2C1	Ho	0.6	Lu	0.4	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.4957		10.5734												K		9.82					9.82																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111748	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.7Lu0.3Ni2B2C1	Ho	0.7	Lu	0.3	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5029		10.5623												K		8.72					8.72																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111749	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.75Lu0.25Ni2B2C1	Ho	0.75	Lu	0.25	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5046		10.5592												K		8.81					8.81																																		MHC11749																																																														arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111750	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.8Lu0.2Ni2B2C1	Ho	0.8	Lu	0.2	Ni	2	B	2	C	1															1998																												LuNi2B2C			A	3.5079		10.5539												K		8.77					8.77																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111751	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.85Lu0.15Ni2B2C1	Ho	0.85	Lu	0.15	Ni	2	B	2	C	1															1998								4.26																				LuNi2B2C			A	3.5111		10.549												K		8.72					8.72																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111752	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.9Lu0.1Ni2B2C1	Ho	0.9	Lu	0.1	Ni	2	B	2	C	1															1998								5.03																				LuNi2B2C			A	3.5136		10.5446												K		8.77					8.77																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111753	MMM1870309		(Ho,Lu)Ni2B2C	Ho0.95Lu0.05Ni2B2C1	Ho	0.95	Lu	0.05	Ni	2	B	2	C	1															1998								5.7																				LuNi2B2C			A	3.5179		10.537												K		8.77					8.77																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111754	MMM1870309		HoNi2B2C	Ho1Ni2B2C1	Ho	1	Ni	2	B	2	C	1																	1998								6.47																				LuNi2B2C			A	3.52		10.5294												K		8.48					8.48																																																																																																arc-melting					Breakdown of de Gennes scaling in HoxLu1-xNi2B2C			Institut fur Festkorper- und Werkstfforschung Dresden, Postfach, Dresden, Germany	J.Mag.Mag.Mat., 187(1998)309	A.Handstein,A.Kreyssig,G.Fuchs,J.Freudenberger,K.-H.Muller,K.Nenkov,L.Schultz,M.Loewenhaupt,M.Wolf		
111755	P069174503	grain size = 2000 nm. G-L parameter = 125	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2004																												Chevrel																		K		14.4					14.4											Oe		58							T		45							T/K		4.6					A		22			A		2750																																																					HIP(2000bar,800C,8h)					Critical parameters of disordered nanocrystalline superconducting Chevrel-phase PbMo6S8			Superconductivity Group, Department of Physics, University of Durham, Durham DH1 3LE, United Kingdom	Phys.Rev.B, 69(2004)174503	D.P.Hampshire,H.J.Niu		
111756	P069174503	grain size = 90 nm. lattice strain = 0.02 %. G-L parameter = 240	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2004																												Chevrel																		K		12.9					12.9											Oe		20							T		65							T/K		7.3					A		19			A		4550																																																					HIP(2000bar,600C,8h) + ANN(1000C,40h)					Critical parameters of disordered nanocrystalline superconducting Chevrel-phase PbMo6S8			Superconductivity Group, Department of Physics, University of Durham, Durham DH1 3LE, United Kingdom	Phys.Rev.B, 69(2004)174503	D.P.Hampshire,H.J.Niu		
111757	P069174503	grain size = 20 nm. lattice strain = 0.07 %. G-L parameter = 520	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			2004																												Chevrel																		K		11.5					11.5											Oe		10							T		110							T/K		14.1					A		14			A		7450																																																					HIP(2000bar,800C,8h)					Critical parameters of disordered nanocrystalline superconducting Chevrel-phase PbMo6S8			Superconductivity Group, Department of Physics, University of Durham, Durham DH1 3LE, United Kingdom	Phys.Rev.B, 69(2004)174503	D.P.Hampshire,H.J.Niu		
111758	PHC4060015	Tc shows Tc(on).	CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		1	2004																												AlB2			A	4.184		4.375											AlB2, C32	K		7.13					7.13																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111759	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.9Ga0.1Si1	Ca	1	Al	0.9	Ga	0.1	Si	1																1	2004																												AlB2			A	4.182		4.392											AlB2, C32	K		6.54					6.54																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111760	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.8Ga0.2Si1	Ca	1	Al	0.8	Ga	0.2	Si	1																1	2004																												AlB2			A	4.177		4.384											AlB2, C32	K		5.6					5.6																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111761	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.7Ga0.3Si1	Ca	1	Al	0.7	Ga	0.3	Si	1																1	2004																												AlB2			A	4.17		4.388											AlB2, C32	K		4.78					4.78																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111762	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.6Ga0.4Si1	Ca	1	Al	0.6	Ga	0.4	Si	1																1	2004																												AlB2			A	4.159		4.39											AlB2, C32	K		4.51					4.51																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111763	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.5Ga0.5Si1	Ca	1	Al	0.5	Ga	0.5	Si	1																1	2004																												AlB2			A	4.152		4.402											AlB2, C32	K		3.73					3.73																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111764	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.4Ga0.6Si1	Ca	1	Al	0.4	Ga	0.6	Si	1																1	2004																												AlB2			A	4.147		4.405											AlB2, C32	K		3.45					3.45																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111765	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.3Ga0.7Si1	Ca	1	Al	0.3	Ga	0.7	Si	1																1	2004																												AlB2			A	4.135		4.414											AlB2, C32	K		3					3																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111766	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.2Ga0.8Si1	Ca	1	Al	0.2	Ga	0.8	Si	1																1	2004																												AlB2			A	4.128		4.421											AlB2, C32	K		3.24					3.24																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111767	PHC4060015	Tc shows Tc(on).	Ca(Al,Ga)Si	Ca1Al0.1Ga0.9Si1	Ca	1	Al	0.1	Ga	0.9	Si	1																1	2004																												AlB2			A	4.119		4.414											AlB2, C32	K		3.34					3.34																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111768	PHC4060015	Tc shows Tc(on).	CaGaSi	Ca1Ga1Si1	Ca	1	Ga	1	Si	1																		1	2004																												AlB2			A	4.118		4.438											AlB2, C32	K		4.05					4.05																																																																																																arc-melting					Substitute effects of Ga on AlB2-type superconductor CaAlSi			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, ROC	Physica C, 406(2004)15	H.H.Sung,W.H.Lee		
111769	JPS0731657	TBL-values are for H//[100]. Hc2(0)=2.7T, COHERE(0)=100 A for H//[001]. RRR=106 for J//[001].	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		3	2004								2.3																																						K		0.63					0.63																				T		3.2							T/K		6.3			MHC11769		A		110																																																										Bridgeman method					Superconducting Property in CePt3Si under Pressure			Graduate School of Science, Osaka University, Toyonaka, Osaka	J.Phys.Soc.Jpn, 73(2004)1657	H.Shishido,R.Settai,S.Hashimoto,T.D.Matsuda,T.Takeuchi,T.Ueda,T.Yasuda,Y.Haga,Y.Oonuki		
111770	P069212508	type-I s/c. Hc2(0), dHc2/dT in TBL are Hc(0), dHc/dT. gap(4.2K)=0.97 meV. G-L parameter = 0.71	ZeB12	B12Zr1	B	12	Zr	1																				3	2004																												UB12			A	7.407														K		6.06					6.06																				Oe		390							Oe/K		110																	4.75																																																grown by Kiev group					Tunneling and magnetic characteristics of superconducting ZrB12 single crystals			The Racah Institute of Physics, The Hebrew University of Jerusalem, 91904 Jerusalem, Israel	Phys.Rev.B, 69(2004)212508	A.Sharoni,G.I.Leviev,I.Asulin,I.Felner,M.A.Belogolovskii,M.L.Tsindlekht,O.Millo,V.B.Filippov,Yu.B.Pademo		
111771	SSC1290081	acceptor-doped fullerene. not s/c. EPR,NMR measured. KAIZERO=-0.01E-6 emu/g. Curie-C =34.9 emu.K/g.	C60(AsF6)2	C60As2F12	C	60	As	2	F	12																			2004							-8.7																					fullerene																		K					5																																																																																																							Magnetic susceptibility and magnetic resonance study of acceptor doped fullerenes C60(MF6)2 (M = As, Sb, P)			Department of Physics, Ben-Gurion University of the Negev, P.O. Box 653, Beer Sheva 84105, Israel	Solid State Commun., 129(2004)81	A.I.Shames,A.M.Panich,I.Felner,P.K.Ummat,S.Goren,W.R.Datars		
111772	SSC1290081	acceptor-doped fullerene. not s/c. EPR,NMR measured. KAIZERO=-0.42E-6 emu/g. Curie-C =28.7 emu.K/g.	C60(SbF6)2	C60Sb2F12	C	60	Sb	2	F	12																			2004							-0.7																					fullerene																		K					5																																																																																																							Magnetic susceptibility and magnetic resonance study of acceptor doped fullerenes C60(MF6)2 (M = As, Sb, P)			Department of Physics, Ben-Gurion University of the Negev, P.O. Box 653, Beer Sheva 84105, Israel	Solid State Commun., 129(2004)81	A.I.Shames,A.M.Panich,I.Felner,P.K.Ummat,S.Goren,W.R.Datars		
111773	SSC1290081	acceptor-doped fullerene. not s/c. EPR,NMR measured. KAIZERO=0.66E-6 emu/g. Curie-C =15.6 emu.K/g.	C60(PF6)2	C60P2F12	C	60	P	2	F	12																			2004							-3.2																					fullerene																		K					5																																																																																																							Magnetic susceptibility and magnetic resonance study of acceptor doped fullerenes C60(MF6)2 (M = As, Sb, P)			Department of Physics, Ben-Gurion University of the Negev, P.O. Box 653, Beer Sheva 84105, Israel	Solid State Commun., 129(2004)81	A.I.Shames,A.M.Panich,I.Felner,P.K.Ummat,S.Goren,W.R.Datars		
111774	SSC1310261	multi-phase, nominal compositions. Hc1, Hc2 are at 5K.	YRh4Si2B	Y1Rh4Si2B1	Y	1	Rh	4	Si	2	B	1																	2004																																														K		9					9											Oe		70							kOe		30																																																																										arc-melting					Superconductivity at Tc = 9 K in the multiphase samples of a new quaternary system R-Rh-Si-B (R = Y, Lu, Er)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research	Solid State Commun., 131(2004)261	A.K.Jain,G.V.M.Kiruthika,L.C.Gupta,V.Bhattacharya		
111775	SSC1310261	multi-phase, nominal compositions.	LaRh4Si2B	La1Rh4Si2B1	La	1	Rh	4	Si	2	B	1																	2004																																														K		8					8																																																																																																arc-melting					Superconductivity at Tc = 9 K in the multiphase samples of a new quaternary system R-Rh-Si-B (R = Y, Lu, Er)			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research	Solid State Commun., 131(2004)261	A.K.Jain,G.V.M.Kiruthika,L.C.Gupta,V.Bhattacharya		
111776	SSC0360493	PENET<ab> (H//c) = 124 nm, PENET<c>(H//ab) = 496 nm. anisotropy =4	NbSe2	Nb1Se2	Nb	1	Se	2																					1980																																														K		7.007					7.007																																									nm		124																																																										Measurements of the penetration depth in the superconducting layer crystals NbSe2 and TaS2(pyridine)#sub(1/2)				Solid State Commun., 36(1980)493	B.S.Deaver.Jr.,J.J.Finley		
111777	SSC0360493	PENET<c>(H//ab) = 124 nm	2H-TaS2	S2Ta1	S	2	Ta	1																					1980																																														K		3.96					3.96																																									nm																																																												Measurements of the penetration depth in the superconducting layer crystals NbSe2 and TaS2(pyridine)#sub(1/2)				Solid State Commun., 36(1980)493	B.S.Deaver.Jr.,J.J.Finley		
111778	SSC0440001	dTc/dP in K/GPa. COHERE<c> = 120 A. anisotropy factor = 20.	C8KHg	C8K1Hg1	C	8	K	1	Hg	1																			1982																																														K		1.88					1.88			K/GPa	-0.63																																A		1900																																																										react (C8K, Hg)					Effect of pressure on the superconductivity of C8KHg and C8RbHg				Solid State Commun., 44(1982)1-6	S.Tanuma,Y.Iye		
111779	SSC0440001	dTc/dP in K/GPa. COHERE<c> = 50 A. anisotropy factor = 20.	C8RbHg	C8Rb1Hg1	C	8	Rb	1	Hg	1																			1982																																														K		1.41					1.41			K/GPa	-0.53																																A		2300																																																										react (C8Rb, Hg)					Effect of pressure on the superconductivity of C8KHg and C8RbHg				Solid State Commun., 44(1982)1-6	S.Tanuma,Y.Iye		
111780	SSC0330385	RRR=40 - 65. Hc2//c = 0.5 T. COHERE(0)<c>=120 A. anisotropy = 4.6. e-ph = 0.55. (delta-C/gamma*Tc )=0.95	Nb3S4	Nb3S4	Nb	3	S	4																					1980																																														K		3.65					3.65																				T		2.1												MHC11780		A		540																		mj/mol.K2	16		380																																					vapor phase transport					Critical field and specific heat of the anisotropic superconductor Nb3S4				Solid State Commun., 33(1980)385	H.Schwenk,W.Biberacher		
111781	P070014511	not SC. In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.75Ir0.25In5	Ce	1	Rh	0.75	Ir	0.25	In	5																3	2004																												HoCoGa5																		K					0.1																																																																																																		grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111782	P070014511	In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.65Ir0.35In5	Ce	1	Rh	0.65	Ir	0.35	In	5																3	2004																												HoCoGa5																		K		0.22					0.22																																																																																																grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111783	P070014511	In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.55Ir0.45In5	Ce	1	Rh	0.55	Ir	0.45	In	5																3	2004								4																				HoCoGa5																		K		0.94					0.94	MTC11783																																																																																															grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111784	P070014511	In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.5Ir0.5In5	Ce	1	Rh	0.5	Ir	0.5	In	5																3	2004								3																				HoCoGa5																		K		0.9					0.9																																																																																																grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111785	P070014511	In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.45Ir0.55In5	Ce	1	Rh	0.45	Ir	0.55	In	5																3	2004																												HoCoGa5																		K		0.82					0.82																																																																																																grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111786	P070014511	In<115> NQR measured.	Ce(Rh,Ir)In5	Ce1Rh0.25Ir0.75In5	Ce	1	Rh	0.25	Ir	0.75	In	5																3	2004																												HoCoGa5																		K		0.64					0.64																																																																																																grown by In-flux method					Coexistence of antiferromagnetic order and unconventional superconductivity in heavy-fermion CeRh1-xIrxIn5 compounds: Nuclear quadrupole resonance studies			Department of Physical Science, Graduate School of Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.B, 70(2004)014511	Guo-qing Zheng,H.Kan,J.D.Thompson,J.L.Sarrao,N.O.Moreno,N.Yamaguchi,P.G.Pagliuso,Y.Kitaoka		
111788	JJP032S448	Tc(R=0) = 4.82	CuRh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			1993																												spinel																		K		4.75					4.75																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111789	JJP032S448		Cu1+xRh2-xS4	Cu1.2Rh1.8S4	Cu	1.2	Rh	1.8	S	4																			1993																												spinel																		K		5.08					5.08																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111790	JJP032S448		Cu1+xRh2-xS4	Cu1.5Rh1.5S4	Cu	1.5	Rh	1.5	S	4																			1993																												spinel																		K		4.6					4.6																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111791	JJP032S448		CuCo2S4	Cu1Co2S4	Cu	1	Co	2	S	4																			1993								17.5																				spinel																		K		4					4																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111792	JJP032S448		Cu1+xCo2-xS4	Cu1.2Co1.8S4	Cu	1.2	Co	1.8	S	4																			1993																												spinel																		K		1.7					1.7																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111793	JJP032S448		Cu1+xCo2-xS4	Cu1.5Co1.5S4	Cu	1.5	Co	1.5	S	4																			1993																												spinel																		K		2.3					2.3																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111794	JJP032S448		Cu1+xCo2-xS4	Cu1.75Co1.25S4	Cu	1.75	Co	1.25	S	4																			1993																												spinel																		K		2.2					2.2																																																																																																					Magnetism and superconductivity in copper spinels				Jpn J.Appl.Phys. Suppl., 32(1993)448	K.Miyatani,M.Ishikawa,N.Shirakawa,S.Sakita,T.Tanaka		
111795	JP0160L333	Tc,Tn obtained by SP-heat. Curie-T=-74.8K(H//[100], =-44.9(H//[001]. Hc2=3.4T (H//[001], =2.8T (H//[110]. RRR=106. SP-heat, thermal expansion, magnetostriction were measured.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		3	2004							-74.8	2.3																																						K		0.51					0.51																				T		3.4												MHC11795																																																														Bridgeman method					Magnetism and superconductivity in a heavy-fermion superconductor, CePt3Si			Research Centre for Materials Science at Extreme Conditions, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 16(2004)L333	A.Aoki,H.Kohara,H.Sato,H.Shishido,K.Kindo,K.Sugiyama,M.Shiimoto,M.Yamada,R.Settai,S.Hashimoto,T.D.Matsuda,T.Takeuchi,T.Ueda,T.Yamamoto,T.Yasuda,Y.Haga,Y.Obiraki,Y.Onuki		
111796	JP01605979	B/Nb = 2.32. PENET estimated from Hc1. G-L parameter = 2.49	NbB2+x	B2.32Nb1	B	2.32	Nb	1																					2004																															A	3.104		3.319												K		9.8					9.8			K/GPa	-0.054							Oe		196							kOe		2.226														A		400			A		870																																																					sintering(stainless tube, Ar-gas, 1000C),quench					Crystalline structure and the superconducting properties of NbB2+x			Instituto de Investigaciones en Materiales, Apartado Postal 70-360, Mexico	J.Phys.:Condens.Matter, 16(2004)5979	A.Duran,F.Morales,O.Lovera,R.Escamilla,R.Escudero,R.Falconi,T.Akachi		
111797	JP01605979	B/Nb = 2.26	NbB2+x	B2.26Nb1	B	2.26	Nb	1																					2004																															A	3.104		3.317												K		9.2					9.2			K/GPa	-0.104																																																																																												sintering(stainless tube, Ar-gas, 1000C),quench					Crystalline structure and the superconducting properties of NbB2+x			Instituto de Investigaciones en Materiales, Apartado Postal 70-360, Mexico	J.Phys.:Condens.Matter, 16(2004)5979	A.Duran,F.Morales,O.Lovera,R.Escamilla,R.Escudero,R.Falconi,T.Akachi		
111798	SSC1310489	space G = Pnma(#62). delta-C = 5.93 mj/mol.K2. (delta-C/gamma*Tc) = 1.08	YRhAl	Y1Rh1Al1	Y	1	Rh	1	Al	1																		1	2004																												TiNiSi			A	6.8535	4.1786	7.9286												K		0.9					0.9																																																								mj/mol.K2	6.1		197																																					arc-melting					Superconductivity in the intermetallic compound YRhAl			Tata Institute of Fundamental Research, Colaba, Mumbai, India	Solid State Commun., 131(2004)489	D.C.Kundaliya,S.K.Malik		
111799	PR06200127	space G = Pnma(#62).	LaRhAl	La1Rh1Al1	La	1	Rh	1	Al	1																			2000																												Pd2(MnPd)Ge2			A	7.246	4.256	16.256												K		2.4					2.4																																																																																																arc-melting					Superconductivity in LaRhAl and mixed valent behavior in CeRhAl			Tata Institute of Fundamental Research, Munbai,India	Phys.Rev.B, 62(2000)127	N.H.Kumar,S.K.Malik		
111800	PR06200127	space G = Pnma(#62).	CeRhAl	Ce1Rh1Al1	Ce	1	Rh	1	Al	1																			2000							-24.8																					Pd2(MnPd)Ge2			A	7.099	4.21	15.934												K					1.7																																																																																																		arc-melting					Superconductivity in LaRhAl and mixed valent behavior in CeRhAl			Tata Institute of Fundamental Research, Munbai,India	Phys.Rev.B, 62(2000)127	N.H.Kumar,S.K.Malik		
111801	PR06200127	space G = Pnma(#62).	LaRhSb	Y1Rh1Sb1	Y	1	Rh	1	Sb	1																			2000																												Pd2(MnPd)Ge2																		K		2.1					2.1																																																																																																arc-melting					Superconductivity in LaRhAl and mixed valent behavior in CeRhAl			Tata Institute of Fundamental Research, Munbai,India	Phys.Rev.B, 62(2000)127	N.H.Kumar,S.K.Malik		
111802	PR06200127	space G = Pnma(#62).	LuRhSb	Lu1Rh1Sb1	Lu	1	Rh	1	Sb	1																			2000																												Pd2(MnPd)Ge2																		K					1.7																																																																																																		arc-melting					Superconductivity in LaRhAl and mixed valent behavior in CeRhAl			Tata Institute of Fundamental Research, Munbai,India	Phys.Rev.B, 62(2000)127	N.H.Kumar,S.K.Malik		
111803	SSC1140223	space G = Pnma(#62). paramag-Curie-T = -5.4 K. effective moment = 3.49 myu-B.	PrRhAl	Pr1Rh1Al1	Pr	1	Rh	1	Al	1																			2000							4.7																					Pd2(MnPd)Ge2			A	7.022	4.275	8.079												K					1.7																																																																																																		arc-melting					Magnetic behaviour of RRhAl (R=La,Ce,Pr,Nd and Gd) compounds			Tata Institute of Fundamental Research, Munbai,India	Solid State Commun., 114(2000)223	N.H.Kumar,S.K.Malik		
111804	SSC1140223	space G = Pnma(#62). paramag-Curie-T = 6.2 K. effective moment = 3.37 myu-B.	NdRhAl	Nd1Rh1Al1	Nd	1	Rh	1	Al	1																			2000							10.5																					Pd2(MnPd)Ge2			A	6.994	4.246	8.056												K					1.7																																																																																																		arc-melting					Magnetic behaviour of RRhAl (R=La,Ce,Pr,Nd and Gd) compounds			Tata Institute of Fundamental Research, Munbai,India	Solid State Commun., 114(2000)223	N.H.Kumar,S.K.Malik		
111805	SSC1140223	space G = Pnma(#62). paramag-Curie-T = 32.9 K. effective moment = 7.82 myu-B.	GdRhAl	Gd1Rh1Al1	Gd	1	Rh	1	Al	1																			2000							29.8																					Pd2(MnPd)Ge2			A	6.918	4.194	7.989												K					1.7																																																																																																		arc-melting					Magnetic behaviour of RRhAl (R=La,Ce,Pr,Nd and Gd) compounds			Tata Institute of Fundamental Research, Munbai,India	Solid State Commun., 114(2000)223	N.H.Kumar,S.K.Malik		
111806	HEL0550755	M = K0.33(H2O)0.66.  COHERE<c>=9.0 A. PENET<c> = 71 micro-m. anisotropy (Hc<ab>/Hc<c>) = 60 at 5 K.	(M)TaS2	M1Ta1S2	M	1	Ta	1	S	2																		3	1982																												TX2																	2H-TaS2,	K		5.6					5.6																																		MHC11806		A		295			um		3.4																																																					vapor transport method					Superconducting parameters of a strongly anisotropic intercalated TaS2 compound: K0.33(H2O)0.66TaS2				Helv.Phys.Acta, 55(1982)755	A.Lerf,S.Gygax,W.Biberacher,W.Meissner		
111807	CEM1771244		CaBxPd3	Ca1B0.75Pd3	Ca	1	B	0.75	Pd	3																		1	2004																																														K					0.3																																																																																																							Formation of transition metal boride and carbide perovskites related to superconducting MgCNi3			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	J.Solid State Chem., 177(2004)1244	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,M.Avdeev,N.P.Ong,R.E.Schaak,R.J.Cava,W.-L.Lee		
111808	CEM1771244	impurity phase = 0.32 wt% CaB6. gamma in mj/mol.K2.	CaBxPd3	Ca1B1.05Pd3	Ca	1	B	1.05	Pd	3																		1	2004																																														K		0.8					0.8																																																								mj/mol.K2	5																																												Formation of transition metal boride and carbide perovskites related to superconducting MgCNi3			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	J.Solid State Chem., 177(2004)1244	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,M.Avdeev,N.P.Ong,R.E.Schaak,R.J.Cava,W.-L.Lee		
111809	CEM1771244	multiple phases. impurity phase not identified.	CaBxPd3	Ca1B1.25Pd3	Ca	1	B	1.25	Pd	3																			2004																																														K		1					1																																																																																																					Formation of transition metal boride and carbide perovskites related to superconducting MgCNi3			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	J.Solid State Chem., 177(2004)1244	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,M.Avdeev,N.P.Ong,R.E.Schaak,R.J.Cava,W.-L.Lee		
111810	CEM1771244	Two phases(NbB0.2Rh3, NbRh2B2-x) are detected. Which is superconducting?	NbBxRh3	Nb1B0.2Rh3	Nb	1	B	0.2	Rh	3																			2004																																														K		6.4					6.4																																																																																																					Formation of transition metal boride and carbide perovskites related to superconducting MgCNi3			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	J.Solid State Chem., 177(2004)1244	A.P.Ramirez,G.Lawes,H.W.Zandbergen,J.D.Jorgensen,M.Avdeev,N.P.Ong,R.E.Schaak,R.J.Cava,W.-L.Lee		
111811	P070014519	using B<10>. No B-isotope effect on PENET (by muon-SR).	MgB2	B2Mg1	B	2	Mg	1																				1	2004																												AlB2																	AlB2, C32	K		40.36					40.36						0.29	B																																																																																									(Mg + B<10>) in a Ta-tube					Absence of a boron isotope effect in the magnetic penetration depth of MgB2			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B, 70(2004)014519	A.Shengelaya,D.Di.Castro,D.G.Eshchenko,H.Keller,I.M.Savic,J.Karpinski,J.Roos,K.Conder,M.Angst,P.C.Canfield,R.A.Ribeiro,R.Khasanov,S.L.Bud'ko,S.M.Kazakov		
111812	P070014519	using B<11>. No B-isotope effect on PENET (by muon-SR).	MgB2	B2Mg1	B	2	Mg	1																				1	2004																												AlB2																	AlB2, C32	K		39.36					39.36																																																																																																(Mg + B<11>) in a Ta-tube					Absence of a boron isotope effect in the magnetic penetration depth of MgB2			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	Phys.Rev.B, 70(2004)014519	A.Shengelaya,D.Di.Castro,D.G.Eshchenko,H.Keller,I.M.Savic,J.Karpinski,J.Roos,K.Conder,M.Angst,P.C.Canfield,R.A.Ribeiro,R.Khasanov,S.L.Bud'ko,S.M.Kazakov		
111813	1840		YB6	B6Y1	B	6	Y	1																					1974																															A	4.1014														K		6.8					6.8																																																																																																					Remarks on the mutual solubilities and superconductivity of hexaborides				MAT.RES.BULL.,9(1974)633	A.C.LAWSON,R.W.FITZGERALD,Z.FISK		
111814	1840		(Y,La)B6	Y0.9La0.1B6	Y	0.9	La	0.1	B	6																			1974																																														K		6.8					6.8																																																																																																					Remarks on the mutual solubilities and superconductivity of hexaborides				MAT.RES.BULL.,9(1974)633	A.C.LAWSON,R.W.FITZGERALD,Z.FISK		
111815	1840		(Y,La)B6	Y0.8La0.2B6	Y	0.8	La	0.2	B	6																			1974																															A	4.113														K		5.8					5.8																																																																																																					Remarks on the mutual solubilities and superconductivity of hexaborides				MAT.RES.BULL.,9(1974)633	A.C.LAWSON,R.W.FITZGERALD,Z.FISK		
111816	1840		(Y,La)B6	Y0.65La0.35B6	Y	0.65	La	0.35	B	6																			1974																															A	4.1221														K		4					4																																																																																																					Remarks on the mutual solubilities and superconductivity of hexaborides				MAT.RES.BULL.,9(1974)633	A.C.LAWSON,R.W.FITZGERALD,Z.FISK		
111817	1390		Be1-xRex	Be0.99Re0.01	Be	0.99	Re	0.01																					1967																																														K		9.25					9.25																				T		0.32																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111818	1390		Be1-xRex	Be0.98Re0.02	Be	0.98	Re	0.02																					1967																																														K		9.45					9.45																				T		0.325																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111819	1390		Be1-xRex	Be0.96Re0.04	Be	0.96	Re	0.04																					1967																																														K		9.5					9.5																				T		0.32																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111820	1390	Hc2(T) curve shown in Fig.4.	Re22Re1	Be22Re1	Be	22	Re	1																					1967																																														K		9.55					9.55																				T		0.34																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111821	1390		Be22(Re,W)1	Be22Re0.95W0.05	Be	22	Re	0.95	W	0.05																			1967																																														K		9.45					9.45																				T		0.41																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111822	1390		Be22(Re,Os)1	Be22Re0.95Os0.05	Be	22	Re	0.95	Os	0.05																			1967																																														K		9.2					9.2																				T		0.35																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111823	1390		Be22(Re,Ru)1	Be22Re0.99Ru0.01	Be	22	Re	0.99	Ru	0.01																			1967																																														K		9.2					9.2																				T		0.355																																																																																			HELV.PHYS.ACTA,40(1967)1012	R.BURTON		
111824	1832		V1-xGax	Ga0.255V0.745	Ga	0.255	V	0.745																					1969																												Cr3Si(A15)			A	4.817													Cr3Si, A15	K		13.9					13.9																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111825	1832		V1-xGax	Ga0.247V0.753	Ga	0.247	V	0.753																					1969																												Cr3Si(A15)			A	4.817													Cr3Si, A15	K		13.8					13.8																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111826	1832		V1-xGax	Ga0.233V0.767	Ga	0.233	V	0.767																					1969																												Cr3Si(A15)			A	4.818													Cr3Si, A15	K		13.3					13.3																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111827	1832		V1-x-yGaxAly	V0.745Ga0.228Al0.027	V	0.745	Ga	0.228	Al	0.027																			1969																												Cr3Si(A15)			A	4.815													Cr3Si, A15	K		13.05					13.05																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111828	1832		V1-x-yGaxAly	V0.737Ga0.213Al0.05	V	0.737	Ga	0.213	Al	0.05																			1969																												Cr3Si(A15)			A	4.822													Cr3Si, A15	K		12.6					12.6																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111829	1832		V1-x-yGaxAly	V0.741Ga0.196Al0.063	V	0.741	Ga	0.196	Al	0.063																			1969																												Cr3Si(A15)			A	4.824													Cr3Si, A15	K		12.2					12.2																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111830	1832		V1-x-yGaxAly	V0.741Ga0.152Al0.107	V	0.741	Ga	0.152	Al	0.107																			1969																												Cr3Si(A15)			A	4.828													Cr3Si, A15	K		11.4					11.4																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111831	1832	impurity phase=A2	V1-x-yGaxAly	V0.747Ga0.131Al0.122	V	0.747	Ga	0.131	Al	0.122																			1969																												Cr3Si(A15)			A	4.829													Cr3Si, A15	K		11.7					11.7																																																																																																ANN(800C,20h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111832	1832	impurity phase=A2	V1-x-yGaxAly	V0.767Ga0.086Al0.147	V	0.767	Ga	0.086	Al	0.147																			1969																												Cr3Si(A15)			A	4.828													Cr3Si, A15	K		12.1					12.1																																																																																																ANN(800C,210h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111833	1832		V1-x-yGaxAly	V0.784Ga0.172Al0.044	V	0.784	Ga	0.172	Al	0.044																			1969																												Cr3Si(A15)			A	4.818													Cr3Si, A15	K		9.4					9.4																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111834	1832		V1-x-yGaxAly	V0.767Ga0.18Al0.053	V	0.767	Ga	0.18	Al	0.053																			1969																												Cr3Si(A15)			A	4.821													Cr3Si, A15	K		11.5					11.5																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111835	1832		V1-x-yGaxAly	V0.725Ga0.203Al0.072	V	0.725	Ga	0.203	Al	0.072																			1969																												Cr3Si(A15)			A	4.826													Cr3Si, A15	K		12.3					12.3																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111836	1832		V1-x-yGaxAly	V0.683Ga0.22Al0.097	V	0.683	Ga	0.22	Al	0.097																			1969																												Cr3Si(A15)			A	4.835													Cr3Si, A15	K		9.4					9.4																																																																																																ANN(800C,14d)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111837	1832	impurity phase=A2	V1-x-yGaxAly	V0.783Ga0.138Al0.079	V	0.783	Ga	0.138	Al	0.079																			1969																												Cr3Si(A15)			A	4.822													Cr3Si, A15	K		10.2					10.2																																																																																																ANN(800C,20h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111838	1832	impurity phase=A2	V1-x-yGaxAly	V0.709Ga0.151Al0.14	V	0.709	Ga	0.151	Al	0.14																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		9					9																																																																																																ANN(800C,20h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111839	1832	impurity phase=A2	V1-x-yGaxAly	V0.767Ga0.214Al0.022	V	0.767	Ga	0.214	Al	0.022																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		12.1					12.1																																																																																																ANN(1200C,50h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111840	1832		V1-x-yGaxAly	V0.743Ga0.181Al0.076	V	0.743	Ga	0.181	Al	0.076																			1969																												Cr3Si(A15)			A	4.822													Cr3Si, A15	K		12					12																																																																																																ANN(1000C,24h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111841	1832	impurity phase=A2	V1-x-yGaxAly	V0.746Ga0.169Al0.085	V	0.746	Ga	0.169	Al	0.085																			1969																												Cr3Si(A15)			A	4.825													Cr3Si, A15	K		11.8					11.8																																																																																																ANN(1000C,24h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111842	1832		V1-xAlx	Al0.25V0.75	Al	0.25	V	0.75																					1969																												Cr3Si(A15)			A	4.724													Cr3Si, A15	K		16.9					16.9																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111843	1832		V1-x-ySixAly	V0.75Si0.225Al0.025	V	0.75	Si	0.225	Al	0.025																			1969																												Cr3Si(A15)			A	4.731													Cr3Si, A15	K		13.5					13.5																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111844	1832		V1-x-ySixAly	V0.75Si0.22Al0.03	V	0.75	Si	0.22	Al	0.03																			1969																												Cr3Si(A15)			A	4.732													Cr3Si, A15	K		13.3					13.3																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111845	1832		V1-x-ySixAly	V0.75Si0.2125Al0.0375	V	0.75	Si	0.2125	Al	0.0375																			1969																												Cr3Si(A15)			A	4.734													Cr3Si, A15	K		12.6					12.6																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111846	1832		V1-x-ySixAly	V0.77Si0.21Al0.02	V	0.77	Si	0.21	Al	0.02																			1969																												Cr3Si(A15)			A	4.737													Cr3Si, A15	K		11.7					11.7																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111847	1832	impurity phase=A2	V1-x-ySixAly	V0.75Si0.2Al0.05	V	0.75	Si	0.2	Al	0.05																			1969																												Cr3Si(A15)			A	4.734													Cr3Si, A15	K		11.8					11.8																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111848	1832	impurity phase=A2	V1-x-ySixAly	V0.75Si0.175Al0.075	V	0.75	Si	0.175	Al	0.075																			1969																												Cr3Si(A15)			A	4.749													Cr3Si, A15	K		11.1					11.1																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111849	1832	impurity phase=A2	V1-x-ySixAly	V0.75Si0.125Al0.125	V	0.75	Si	0.125	Al	0.125																			1969																												Cr3Si(A15)			A	4.751													Cr3Si, A15	K		10.4					10.4																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111850	1832	impurity phase=A2	V1-x-ySixAly	V0.75Si0.025Al0.225	V	0.75	Si	0.025	Al	0.225																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		9.8					9.8																																																																																																ANN(1000C,150h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111851	1832	impurity phase=A2	V1-x-ySixAly	V0.72Si0.17Al0.11	V	0.72	Si	0.17	Al	0.11																			1969																												Cr3Si(A15)			A	4.746													Cr3Si, A15	K		10.3					10.3																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111852	1832	impurity phase=A2	V1-x-ySixAly	V0.65Si0.1Al0.25	V	0.65	Si	0.1	Al	0.25																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		9.9					9.9																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111853	1832	impurity phase=V5Si3	V1-x-ySixAly	V0.73Si0.25Al0.02	V	0.73	Si	0.25	Al	0.02																			1969																												Cr3Si(A15)			A	4.727													Cr3Si, A15	K		14					14																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111854	1832	impurity phase=A2, V5Si3	V1-x-ySixAly	V0.73Si0.23Al0.04	V	0.73	Si	0.23	Al	0.04																			1969																												Cr3Si(A15)			A	4.737													Cr3Si, A15	K		10.4					10.4																																																																																																ANN(1000C,200h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111855	1832	impurity phase=A2, V5Si3	V1-x-ySixAly	V0.7Si0.2Al0.1	V	0.7	Si	0.2	Al	0.1																			1969																												Cr3Si(A15)			A	4.74													Cr3Si, A15	K		10.6					10.6																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111856	1832	impurity phase=A2, V5Si3	V1-x-ySixAly	V0.63Si0.14Al0.23	V	0.63	Si	0.14	Al	0.23																			1969																												Cr3Si(A15)			A	4.745													Cr3Si, A15	K		9.7					9.7																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111857	1832	impurity phase=V5Ge3	V1-xGex	Ge0.27V0.73	Ge	0.27	V	0.73																					1969																												Cr3Si(A15)			A	4.782													Cr3Si, A15	K		6.6					6.6																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111858	1832	impurity phase=V5Ge3	V1-xGex	Ge0.25V0.75	Ge	0.25	V	0.75																					1969																												Cr3Si(A15)			A	4.78													Cr3Si, A15	K		6.5					6.5																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111859	1832	impurity phase=A2	V1-xGex	Ge0.23V0.77	Ge	0.23	V	0.77																					1969																												Cr3Si(A15)			A	4.784													Cr3Si, A15	K		6.4					6.4																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111860	1832	impurity phase=A2	V1-xGex	Ge0.21V0.79	Ge	0.21	V	0.79																					1969																												Cr3Si(A15)			A	4.784													Cr3Si, A15	K		6.4					6.4																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111861	1832		V1-x-yGexAly	V0.75Ge0.2375Al0.0125	V	0.75	Ge	0.2375	Al	0.0125																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		7.6					7.6																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111862	1832		V1-x-yGexAly	V0.75Ge0.225Al0.025	V	0.75	Ge	0.225	Al	0.025																			1969																												Cr3Si(A15)			A	4.786													Cr3Si, A15	K		8.6					8.6																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111863	1832		V1-x-yGexAly	V0.75Ge0.2125Al0.0375	V	0.75	Ge	0.2125	Al	0.0375																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		8.9					8.9																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111864	1832		V1-x-yGexAly	V0.75Ge0.2Al0.05	V	0.75	Ge	0.2	Al	0.05																			1969																												Cr3Si(A15)			A	4.792													Cr3Si, A15	K		10.3					10.3																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111865	1832	impurity phase=A2	V1-x-yGexAly	V0.75Ge0.1875Al0.0625	V	0.75	Ge	0.1875	Al	0.0625																			1969																												Cr3Si(A15)			A	4.795													Cr3Si, A15	K		11.4					11.4																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111866	1832	impurity phase=A2	V1-x-yGexAly	V0.75Ge0.175Al0.075	V	0.75	Ge	0.175	Al	0.075																			1969																												Cr3Si(A15)			A	4.796													Cr3Si, A15	K		10.8					10.8																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111867	1832	impurity phase=A2	V1-x-yGexAly	V0.75Ge0.15Al0.1	V	0.75	Ge	0.15	Al	0.1																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		11.7					11.7																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111868	1832	impurity phase=A2	V1-x-yGexAly	V0.75Ge0.13Al0.12	V	0.75	Ge	0.13	Al	0.12																			1969																												Cr3Si(A15)			A	4.793													Cr3Si, A15	K		11.3					11.3																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111869	1832	impurity phase=A2	V1-x-yGexAly	V0.75Ge0.025Al0.225	V	0.75	Ge	0.025	Al	0.225																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		11.2					11.2																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111870	1832	impurity phase=A2	V1-x-yGexAly	V0.65Ge0.1Al0.25	V	0.65	Ge	0.1	Al	0.25																			1969																												Cr3Si(A15)			A	4.801													Cr3Si, A15	K		7					7																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111871	1832	impurity phase=A2, V5Al8	V1-x-yGexAly	V0.55Ge0.1Al0.35	V	0.55	Ge	0.1	Al	0.35																			1969																												Cr3Si(A15)			A	4.795													Cr3Si, A15	K		5.4					5.4																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111872	1832	impurity phase=A2, V5Al8	V1-x-yGexAly	V0.65Ge0.15Al0.2	V	0.65	Ge	0.15	Al	0.2																			1969																												Cr3Si(A15)			A	4.801													Cr3Si, A15	K		5.5					5.5																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111873	1832	impurity phase=V5Ge3, V5Al8	V1-x-yGexAly	V0.65Ge0.25Al0.1	V	0.65	Ge	0.25	Al	0.1																			1969																												Cr3Si(A15)			A	4.793													Cr3Si, A15	K		5.5					5.5																																																																																																ANN(1000C,300h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111874	1832	impurity phase=V3Sb2	V1-xSbx	Sb0.268V0.732	Sb	0.268	V	0.732																					1969																												Cr3Si(A15)			A	4.939													Cr3Si, A15	K					2.2																																																																																																		ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111875	1832	impurity phase=V3Sb2	V1-xSbx	Sb0.249V0.751	Sb	0.249	V	0.751																					1969																												Cr3Si(A15)			A	4.941													Cr3Si, A15	K					2																																																																																																		ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111876	1832		V1-xSbx	Sb0.236V0.764	Sb	0.236	V	0.764																					1969																												Cr3Si(A15)			A	4.939													Cr3Si, A15	K					1.5																																																																																																		ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111877	1832		V1-xSbx	Sb0.223V0.777	Sb	0.223	V	0.777																					1969																												Cr3Si(A15)			A	4.931													Cr3Si, A15	K					2																																																																																																		ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111878	1832	impurity phase=A2	V1-xSbx	Sb0.195V0.805	Sb	0.195	V	0.805																					1969																												Cr3Si(A15)			A	4.928													Cr3Si, A15	K					2.2																																																																																																		ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111879	1832		V1-x-ySbxAly	V0.745Sb0.208Al0.025	V	0.745	Sb	0.208	Al	0.025																			1969																												Cr3Si(A15)			A	4.936													Cr3Si, A15	K		2					2																																																																																																ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111880	1832		V1-x-ySbxAly	V0.751Sb0.208Al0.041	V	0.751	Sb	0.208	Al	0.041																			1969																												Cr3Si(A15)			A	4.93													Cr3Si, A15	K		3.4					3.4																																																																																																ANN(1000C,170h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111881	1832		V1-x-ySbxAly	V0.746Sb0.179Al0.075	V	0.746	Sb	0.179	Al	0.075																			1969																												Cr3Si(A15)			A	4.922													Cr3Si, A15	K		4.3					4.3																																																																																																ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111882	1832	impurity phase=A2	V1-x-ySbxAly	V0.749Sb0.157Al0.094	V	0.749	Sb	0.157	Al	0.094																			1969																												Cr3Si(A15)			A	4.914													Cr3Si, A15	K		5.1					5.1																																																																																																ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111883	1832	impurity phase=A2	V1-x-ySbxAly	V0.741Sb0.113Al0.146	V	0.741	Sb	0.113	Al	0.146																			1969																												Cr3Si(A15)			A	4.911													Cr3Si, A15	K		6.1					6.1																																																																																																ANN(1000C,100h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111884	1832	impurity phase=A2	V1-x-ySbxAly	V0.736Sb0.037Al0.227	V	0.736	Sb	0.037	Al	0.227																			1969																												Cr3Si(A15)																	Cr3Si, A15	K		6.4					6.4																																																																																																ANN(1000C,130h)					Supraleitung von A15-phasen der systeme V-Ga-Al, V-Si-Al, V-Ge-Al und V-Sb-Al				Z.NATURFORSCH.A,24(1969)1134	A.MULLER,A.Muller		
111885	1429	Tc was measured upto P=20 kbar. dTc/dP not given.	LaAl2	Al2La1	Al	2	La	1																					1973																															A	8.147														K		3.229					3.229																																																																																																arc-melting					The effect of pressure on the crystalline electric field levels of superconducting La1-xTbxAl2				SOLID STATE COMMUN.,13(1973)1889	A.R.SWEEDLER,J.E.CROW,M.B.MAPLE,R.P.GUERTIN,W.BOIVIN		
111886	1429	Tc was measured upto P=20 kbar. dTc/dP not given.	(La,Tb)Al2	La0.9941Tb0.0059Al2	La	0.9941	Tb	0.0059	Al	2																			1973																																														K		1.996					1.996																																																																																																arc-melting					The effect of pressure on the crystalline electric field levels of superconducting La1-xTbxAl2				SOLID STATE COMMUN.,13(1973)1889	A.R.SWEEDLER,J.E.CROW,M.B.MAPLE,R.P.GUERTIN,W.BOIVIN		
111887	1429	Tc was measured upto P=20 kbar. dTc/dP not given.	(La,Tb)Al2	La0.9911Tb0.0089Al2	La	0.9911	Tb	0.0089	Al	2																			1973																																														K		1.425					1.425																																																																																																arc-melting					The effect of pressure on the crystalline electric field levels of superconducting La1-xTbxAl2				SOLID STATE COMMUN.,13(1973)1889	A.R.SWEEDLER,J.E.CROW,M.B.MAPLE,R.P.GUERTIN,W.BOIVIN		
111888	1431		Al13Os4	Al13Os4	Al	13	Os	4																					1968																																														K		5.3					5.3																																																								mj/mol.K2	1.05		422																																										Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
111889	1431	R not zero down to 2 K.	Al13(Os,Ru)4	Al13Os3.2Ru0.8	Al	13	Os	3.2	Ru	0.8																			1968																																														K		4					4																																																								mj/mol.K2	0.46		415																																										Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
111890	1431	not s/c.	Al13(Os,Ru)4	Al13Os2.96Ru1.04	Al	13	Os	2.96	Ru	1.04																			1968																																														K					1																																																										mj/mol.K2	0.6		480																																										Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
111891	1431	not s/c.	Al13Ru4	Al13Ru4	Al	13	Ru	4																					1968																																														K					1																																																										mj/mol.K2	0.3		433																																										Supraconductive dans la phase monoclinique du systeme aluminium-osmium-ruthenium				HELV.PHYS.ACTA,41(1968)1052	F.HEINIGER,J.L.STAUDENMANN,J.MULLER		
111892	JPS0731938		Cu(Co,Rh)2S4	Cu1Co1.99Rh0.01S4	Cu	1	Co	1.99	Rh	0.01	S	4																	2004																												spinel																		K		2.61					2.61																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111893	JPS0731938		Cu(Co,Rh)2S4	Cu1Co1.98Rh0.02S4	Cu	1	Co	1.98	Rh	0.02	S	4																	2004																												spinel																		K		2.82					2.82																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111894	JPS0731938	R not zero at T=2.2 K.	Cu(Co,Rh)2S4	Cu1Co1.95Rh0.05S4	Cu	1	Co	1.95	Rh	0.05	S	4																	2004																												spinel																		K					2.2																																																																																																		mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111895	JPS0731938		Cu(Co,Ir)2S4	Cu1Co1.99Ir0.01S4	Cu	1	Co	1.99	Ir	0.01	S	4																	2004																												spinel																		K		3.04					3.04																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111896	JPS0731938		Cu(Co,Ir)2S4	Cu1Co1.98Ir0.02S4	Cu	1	Co	1.98	Ir	0.02	S	4																	2004																												spinel																		K		2.79					2.79																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111897	JPS0731938		Cu(Co,Ir)2S4	Cu1Co1.95Ir0.05S4	Cu	1	Co	1.95	Ir	0.05	S	4																	2004																												spinel																		K		2.13					2.13																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111898	JPS0731938	not s/c.	Cu(Co,Ir)2S4	Cu1Co1.9Ir0.1S4	Cu	1	Co	1.9	Ir	0.1	S	4																	2004																												spinel																		K					2.2																																																																																																		mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111899	JPS0731938	s/c transitions are not reproducible. The highest Tc = 3.8 K.	CuCo2S4	Cu1Co2S4	Cu	1	Co	2	S	4																			2004																												spinel																		K		3.8					3.8																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111900	JPS0731938		Cu(Co,Cr)2S4	Cu1Co1.99Cr0.01S4	Cu	1	Co	1.99	Cr	0.01	S	4																	2004																												spinel																		K		3.62					3.62																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111901	JPS0731938		Cu(Co,Cr)2S4	Cu1Co1.98Cr0.02S4	Cu	1	Co	1.98	Cr	0.02	S	4																	2004																												spinel																		K		3.4					3.4																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111902	JPS0731938		Cu(Co,Cr)2S4	Cu1Co1.95Cr0.05S4	Cu	1	Co	1.95	Cr	0.05	S	4																	2004																												spinel																		K		3.4					3.4																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111903	JPS0731938		Cu(Co,Cr)2S4	Cu1Co1.9Cr0.1S4	Cu	1	Co	1.9	Cr	0.1	S	4																	2004																												spinel																		K		3					3																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111904	JPS0731938		Cu(Co,Cr)2S4	Cu1Co1.8Cr0.2S4	Cu	1	Co	1.8	Cr	0.2	S	4																	2004																												spinel																		K		2.7					2.7																																																																																																mixed powder - heat(800-850C,48h,in evacuated silica)					Superconducting transition temperatures of Cu(Co1-xMx)2S4			Nagoya University, Nagoya,Japan	J.Phys.Soc.Jpn, 73(2004)1938	M.Sato,N.Aito		
111905	1520		CeRu2	Ce1Ru2	Ce	1	Ru	2																					1971																																														K		5.4					5.4																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111906	1520		Ce(Ru,Co)2	Ce1Ru1.99Co0.01	Ce	1	Ru	1.99	Co	0.01																			1971																																														K		4.74					4.74																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111907	1520		Ce(Ru,Co)2	Ce1Ru1.97Co0.03	Ce	1	Ru	1.97	Co	0.03																			1971																																														K		3.5					3.5																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111908	1520		Ce(Ru,Co)2	Ce1Ru1.95Co0.05	Ce	1	Ru	1.95	Co	0.05																			1971																																														K		2.4					2.4																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111909	1520		Ce(Ru,Co)2	Ce1Ru1.93Co0.07	Ce	1	Ru	1.93	Co	0.07																			1971																																														K		1.93					1.93																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111910	1520	not s/c for 0.1< x <1.6 in CeRu2-xCox.	Ce(Ru,Co)2	Ce1Ru0.3Co1.7	Ce	1	Ru	0.3	Co	1.7																			1971																															A	7.232														K		0.27					0.27																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111911	1520	not s/c for 0.1< x <1.6 in CeRu2-xCox.	Ce(Ru,Co)2	Ce1Ru0.2Co1.8	Ce	1	Ru	0.2	Co	1.8																			1971																															A	7.2024														K		0.35					0.35																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111912	1520		Ce(Ru,Co)2	Ce1Ru0.1Co1.9	Ce	1	Ru	0.1	Co	1.9																			1971																															A	7.1808														K		0.47					0.47																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111913	1520		Ce(Ru,Co)2	Ce1Co2	Ce	1	Co	2																					1971																															A	7.164														K		0.84					0.84																																																																																																					Superconductivity and magnetic susceptibility studies of the cubic Laves phase alloys CeRu2-xCox				J.PHYS.F:METAL.PHYS.,1(1971)896	H.L.LUO,I.R.HARRIS,M.B.MAPLE,T.F.SMITH		
111914	951		Th1-xCex	Ce0.025Th0.975	Ce	0.025	Th	0.975																					1970																																														K		0.58					0.58	MTC11914																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
111915	951		Th1-xUx	Th0.999U0.001	Th	0.999	U	0.001																					1970																																														K		0.654					0.654	MTC11915																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
111916	951		Al1-xMnx	Al0.999Mn0.001	Al	0.999	Mn	0.001																					1970																																														K		0.596					0.596	MTC11916																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
111917	1072		Nb3Al	Al3Nb3	Al	3	Nb	3																					1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.4					18.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111918	1072		Nb3(Al,Ge)	Nb3Al0.9Ge0.1	Nb	3	Al	0.9	Ge	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		19.5					19.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111919	1072		Nb3(Al,Ge)	Nb3Al0.8Ge0.2	Nb	3	Al	0.8	Ge	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		19.8					19.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111920	1072		Nb3(Al,Ge)	Nb3Al0.7Ge0.3	Nb	3	Al	0.7	Ge	0.3																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		19.9					19.9																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111921	1072		Nb3(Al,Ge)	Nb3Al0.6Ge0.4	Nb	3	Al	0.6	Ge	0.4																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		19.7					19.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111922	1072		Nb3(Al,Ge)	Nb3Al0.5Ge0.5	Nb	3	Al	0.5	Ge	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.4					17.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111923	1072		Nb3(Al,Ga)	Nb3Al0.9Ga0.1	Nb	3	Al	0.9	Ga	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111924	1072		Nb3(Al,Ga)	Nb3Al0.8Ga0.2	Nb	3	Al	0.8	Ga	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.54					18.54																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111925	1072		Nb3(Al,Ga)	Nb3Al0.67Ga0.33	Nb	3	Al	0.67	Ga	0.33																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.7					18.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111926	1072		Nb3(Al,Ga)	Nb3Al0.5Ga0.5	Nb	3	Al	0.5	Ga	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111927	1072		Nb3(Al,In)	Nb3Al0.9In0.1	Nb	3	Al	0.9	In	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111928	1072		Nb3(Al,In)	Nb3Al0.8In0.2	Nb	3	Al	0.8	In	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111929	1072		Nb3(Al,In)	Nb3Al0.67In0.33	Nb	3	Al	0.67	In	0.33																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16					16																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111930	1072		Nb3(Al,Zn)	Nb3Al0.9Zn0.1	Nb	3	Al	0.9	Zn	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111931	1072		Nb3(Al,Zn)	Nb3Al0.8Zn0.2	Nb	3	Al	0.8	Zn	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111932	1072		Nb3(Al,Zn)	Nb3Al0.67Zn0.33	Nb	3	Al	0.67	Zn	0.33																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.3					17.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111933	1072		Nb3(Al,Zn)	Nb3Al0.5Zn0.5	Nb	3	Al	0.5	Zn	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16					16																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111934	1072		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1968																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111935	1072		Nb3(Sn,Ga)	Nb3Sn0.9Ga0.1	Nb	3	Sn	0.9	Ga	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111936	1072		Nb3(Sn,Ga)	Nb3Sn0.8Ga0.2	Nb	3	Sn	0.8	Ga	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17					17																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111937	1072		Nb3(Sn,Ga)	Nb3Sn0.65Ga0.35	Nb	3	Sn	0.65	Ga	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.5					16.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111938	1072		Nb3(Sn,Ga)	Nb3Sn0.5Ga0.5	Nb	3	Sn	0.5	Ga	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111939	1072		Nb3(Sn,Ge)	Nb3Sn0.95Ge0.05	Nb	3	Sn	0.95	Ge	0.05																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111940	1072		Nb3(Sn,Ge)	Nb3Sn0.9Ge0.1	Nb	3	Sn	0.9	Ge	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111941	1072		Nb3(Sn,Ge)	Nb3Sn0.8Ge0.2	Nb	3	Sn	0.8	Ge	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111942	1072		Nb3(Sn,Ge)	Nb3Sn0.65Ge0.35	Nb	3	Sn	0.65	Ge	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111943	1072		Nb3(Sn,In)	Nb3Sn0.9In0.1	Nb	3	Sn	0.9	In	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111944	1072		Nb3(Sn,In)	Nb3Sn0.8In0.2	Nb	3	Sn	0.8	In	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111945	1072		Nb3(Sn,Al)	Nb3Sn0.9Al0.1	Nb	3	Sn	0.9	Al	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111946	1072		Nb3(Sn,Al)	Nb3Sn0.8Al0.2	Nb	3	Sn	0.8	Al	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.8					16.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111947	1072		Nb3(Sn,Al)	Nb3Sn0.7Al0.3	Nb	3	Sn	0.7	Al	0.3																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.8					15.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111948	1072		Nb3(Sn,Al)	Nb3Sn0.6Al0.4	Nb	3	Sn	0.6	Al	0.4																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.7					15.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111949	1072		Nb3(Sn,Al)	Nb3Sn0.5Al0.5	Nb	3	Sn	0.5	Al	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111950	1072		Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111951	1072		Nb3(Ga,Al)	Nb3Ga0.85Al0.15	Nb	3	Ga	0.85	Al	0.15																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.1					17.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111952	1072		Nb3(Ga,Al)	Nb3Ga0.67Al0.33	Nb	3	Ga	0.67	Al	0.33																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111953	1072		Nb3(Ga,Al)	Nb3Ga0.5Al0.5	Nb	3	Ga	0.5	Al	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111954	1072		Nb3(Ga,Zn)	Nb3Ga0.9Zn0.1	Nb	3	Ga	0.9	Zn	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111955	1072		Nb3(Ga,Zn)	Nb3Ga0.8Zn0.2	Nb	3	Ga	0.8	Zn	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.2					16.2																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111956	1072		Nb3(Ga,Zn)	Nb3Ga0.65Zn0.35	Nb	3	Ga	0.65	Zn	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.3					16.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111957	1072		Nb3(Ga,Zn)	Nb3Ga0.5Zn0.5	Nb	3	Ga	0.5	Zn	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111958	1072		Nb3(Ga,Ge)	Nb3Ga0.95Ge0.05	Nb	3	Ga	0.95	Ge	0.05																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.3					15.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
111959	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xSbx	Pb0.9904Sb0.0096	Pb	0.9904	Sb	0.0096																					1965																																														K		7.29					7.29	MTC11960																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111960	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xBix	Bi0.0105Pb0.9895	Bi	0.0105	Pb	0.9895																					1965																																														K		7.214					7.214	MTC11960																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111961	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xSnx	Pb0.9769Sn0.0231	Pb	0.9769	Sn	0.0231																					1965																																														K		7.213					7.213	MTC11960																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111962	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-x(TlBi)x	Pb0.95Tl0.025Bi0.025	Pb	0.95	Tl	0.025	Bi	0.025																			1965																																														K		7.214					7.214	MTC11960																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111963	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xHgx	Hg0.0307Pb0.9693	Hg	0.0307	Pb	0.9693																					1965																																														K		7.134					7.134	MTC11963																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111964	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xInx	In0.0293Pb0.9707	In	0.0293	Pb	0.9707																					1965																																														K		7.109					7.109	MTC11963																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111965	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xCdx	Cd0.0263Pb0.9737	Cd	0.0263	Pb	0.9737																					1965																																														K		7.124					7.124	MTC11965																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111966	1165	Tc calculated from Tc(Pb)=7.195 K (not given by the Authors)	Pb1-xTlx	Pb0.9848Tl0.0152	Pb	0.9848	Tl	0.0152																					1965																																														K		7.135					7.135	MTC11965																																																																																																				The superconducting transition temperatures of some dilute lead alloys				PROC.PHYS.SOC.,86(1965)1199	B.R.COLES,H.GAMARI-SEALE		
111967	1113		CeRu2	Ce1Ru2	Ce	1	Ru	2																					1970																																														K		6.1					6.1																																																																																																									PHYS.LETT.A,31(1970)448	B.HILLENBRAND,M.WILHELM		
111968	1113		(Ce,Tb)Ru2	Ce0.86Tb0.14Ru2	Ce	0.86	Tb	0.14	Ru	2																			1970																																														K		4.51					4.51																																																																																																									PHYS.LETT.A,31(1970)448	B.HILLENBRAND,M.WILHELM		
111969	1113		(Ce,Tb)Ru2	Ce0.8Tb0.2Ru2	Ce	0.8	Tb	0.2	Ru	2																			1970							4.43																																							K		2.52					2.52	MTC11969																																																																																																								PHYS.LETT.A,31(1970)448	B.HILLENBRAND,M.WILHELM		
111970	1658		(Ce,Y)Ru2	Ce0.84Y0.16Ru2	Ce	0.84	Y	0.16	Ru	2																			1972																																														K		4.92					4.92																																																																																																					On the anomalous dependence of the superconducting transition temperature Tc of CeRu2 on magnetic ion concentration				PHYS.LETT.A,41(1972)419	B.HILLENBRAND,M.WILHELM		
111971	1658		(Ce,Y,Gd)Ru2	Ce0.84Y0.1Gd0.06Ru2	Ce	0.84	Y	0.1	Gd	0.06	Ru	2																	1972																																														K		4.55					4.55	MTC11971																																																																																																				On the anomalous dependence of the superconducting transition temperature Tc of CeRu2 on magnetic ion concentration				PHYS.LETT.A,41(1972)419	B.HILLENBRAND,M.WILHELM		
111972	1658		(Ce,Y,Gd)Ru2	Ce0.84Y0.06Gd0.1Ru2	Ce	0.84	Y	0.06	Gd	0.1	Ru	2																	1972																																														K		3.32					3.32																																																																																																					On the anomalous dependence of the superconducting transition temperature Tc of CeRu2 on magnetic ion concentration				PHYS.LETT.A,41(1972)419	B.HILLENBRAND,M.WILHELM		
111973	1228		La3In	In1La3	In	1	La	3																					1972																																														K		9.45					9.45																																		MHC11975																																																																							SOLID STATE COMMUN., 10(1972)927	A.TREYVAUD,G.BONGI,H.JONES,O.FISCHER		
111974	1228		(La,Ce)3In	La2.98Ce0.02In1	La	2.98	Ce	0.02	In	1																			1972																																														K		8.2					8.2																																		MHC11975																																																																							SOLID STATE COMMUN., 10(1972)927	A.TREYVAUD,G.BONGI,H.JONES,O.FISCHER		
111975	1228		(La,Ce)3In	La2.96Ce0.04In1	La	2.96	Ce	0.04	In	1																			1972																																														K		7.01					7.01	MTC11975																																																																																																								SOLID STATE COMMUN., 10(1972)927	A.TREYVAUD,G.BONGI,H.JONES,O.FISCHER		
111976	1228		(La,Ce)3In	La2.94Ce0.06In1	La	2.94	Ce	0.06	In	1																			1972																																														K		5.58					5.58																																		MHC11975																																																																							SOLID STATE COMMUN., 10(1972)927	A.TREYVAUD,G.BONGI,H.JONES,O.FISCHER		
111977	1295		MoGa4	Ga4Mo1	Ga	4	Mo	1																					1972																																														K		7.98					7.98																																																																																																									HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111978	1295		(Mo,Nb)Ga4	Mo0.98Nb0.02Ga4	Mo	0.98	Nb	0.02	Ga	4																			1972																																														K		8					8	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111979	1295		(Mo,Nb)Ga4	Mo0.96Nb0.04Ga4	Mo	0.96	Nb	0.04	Ga	4																			1972																																														K		8					8	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111980	1295		(Mo,Ru)Ga4	Mo0.96Ru0.04Ga4	Mo	0.96	Ru	0.04	Ga	4																			1972																																														K		7.63					7.63	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111981	1295		(Mo,Co)Ga4	Mo0.96Co0.04Ga4	Mo	0.96	Co	0.04	Ga	4																			1972																																														K		7.07					7.07	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111982	1295		(Mo,Fe)Ga4	Mo0.97Fe0.03Ga4	Mo	0.97	Fe	0.03	Ga	4																			1972																																														K		5.13					5.13	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111983	1295		(Mo,Fe)Ga4	Mo0.94Fe0.06Ga4	Mo	0.94	Fe	0.06	Ga	4																			1972																																														K		2.6					2.6	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111984	1295		(Mo,Mn)Ga4	Mo0.99Mn0.01Ga4	Mo	0.99	Mn	0.01	Ga	4																			1972																																														K		3.94					3.94	MTC11980																																																																																																								HELVETIA PHYS.ACTA,45(1972)331	O.H.FISCHER		
111985	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc .	Mo	Mo1	Mo	1																							1974																																														K		0.92					0.92																				Oe		94.7												MHC11985																						mj/mol.K2	1960																																							ANN(2520C, P=1 E-10 Torr)					Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111986	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc . dTc/dx = 18 K/at % Co	Mo1-xCox	Co0.01Mo99.99	Co	0.01	Mo	99.99																					1974																																														K		0.71					0.71																				Oe		70												MHC11986																						mj/mol.K2	1950																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111987	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc .	Mo1-xCox	Co0.015Mo99.985	Co	0.015	Mo	99.985																					1974																																														K		0.59					0.59																				Oe		57.3												MHC11987																						mj/mol.K2	1960																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111988	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc .	Mo1-xCox	Co0.032Mo99.968	Co	0.032	Mo	99.968																					1974																																														K		0.31					0.31																				Oe		24.2												MHC11988																						mj/mol.K2	1950																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111989	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc .	Mo1-xCox	Co0.038Mo99.962	Co	0.038	Mo	99.962																					1974																																														K		0.22					0.22																				Oe		15.7												MHC11989																						mj/mol.K2	1910																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111990	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc . dTc/dx = 38 K/at % Fe	Mo1-xFex	Fe0.008Mo99.992	Fe	0.008	Mo	99.992																					1974																																														K		0.645					0.645																				Oe		45.6												MHC11990																						mj/mol.K2	1084																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111991	1833	unit of gamma = erg/cm3.K2 estimated from Hc.  Hc2 = Hc .	Mo1-xFex	Fe0.011Mo99.989	Fe	0.011	Mo	99.989																					1974																																														K		0.51					0.51																				Oe		32.7												MHC11990																						mj/mol.K2	726																																												Kondo effect in superconducting MoCo, MoFe, and MoMn alloys				J.LOW TEMP.PHYS.,16(1974)519	M.TAKANO,S.TAKAYANAGI,T.SUGAWARA,Y.KIMURA		
111992	1377		Pd(Tl,Pb)2	Pd1Tl1Pb1	Pd	1	Tl	1	Pb	1																			1972																												CuAl2																	CuAl2, C16	K		1.78					1.78	MTC11992																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111993	1377		(Rh,Pd)Pb2	Rh0.5Pd0.5Pb2	Rh	0.5	Pd	0.5	Pb	2																			1972																												CuAl2																	CuAl2, C16	K		1.7					1.7	MTC11993																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111994	1377		(Pd,Au)Pb2	Pd0.5Au0.5Pb2	Pd	0.5	Au	0.5	Pb	2																			1972																												CuAl2																	CuAl2, C16	K		3.02					3.02	MTC11993																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111995	1377		(Pd,Ag)Th2	Pd0.5Ag0.5Th2	Pd	0.5	Ag	0.5	Th	2																			1972																												CuAl2																	CuAl2, C16	K		1.2					1.2	MTC11995																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111996	1377		(Ag,Al)Th2	Ag0.5Al0.5Th2	Ag	0.5	Al	0.5	Th	2																			1972																												CuAl2																	CuAl2, C16	K		0.78					0.78	MTC11995																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111997	1377		(Al,Ge)Th2	Al0.5Ge0.5Th2	Al	0.5	Ge	0.5	Th	2																			1972																												CuAl2																	CuAl2, C16	K		0.21					0.21	MTC11995																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111998	1377		(Fe,Co)Zr2	Fe0.5Co0.5Zr2	Fe	0.5	Co	0.5	Zr	2																			1972																												CuAl2																	CuAl2, C16	K		1.26					1.26	MTC11998																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
111999	1377		(Co,Ni)Zr2	Co0.5Ni0.5Zr2	Co	0.5	Ni	0.5	Zr	2																			1972																												CuAl2																	CuAl2, C16	K		3.21					3.21	MTC11998																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112000	1377		(Ni,Cu)4Zr8	Ni2.5Cu1.5Zr8	Ni	2.5	Cu	1.5	Zr	8																			1972																												CuAl2																	CuAl2, C16	K		1.09					1.09	MTC11998																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112001	1377		(Co,Ni)Ta2	Co0.5Ni0.5Ta2	Co	0.5	Ni	0.5	Ta	2																			1972																												CuAl2																	CuAl2, C16	K		0.91					0.91	MTC12001																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112002	1377		Co(Ta,Zr)2	Co1Ta1.75Zr0.25	Co	1	Ta	1.75	Zr	0.25																			1972																												CuAl2																	CuAl2, C16	K		1					1																																																																																																					Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112003	1377		(Fe,Ni)Zr2	Fe0.5Ni0.5Zr2	Fe	0.5	Ni	0.5	Zr	2																			1972																												CuAl2																	CuAl2, C16	K		2.45					2.45	MTC12003																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112004	1377		B(Mo,Ta)2	B1Mo1.5Ta0.5	B	1	Mo	1.5	Ta	0.5																			1972																												CuAl2																	CuAl2, C16	K		1.82					1.82	MTC12004																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112005	1377		B(Mo,Re)	B1Mo1Re1	B	1	Mo	1	Re	1																			1972																												CuAl2																	CuAl2, C16	K		5.09					5.09	MTC12004																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112006	1377		B(Ta,W)2	B1Ta0.5W1.5	B	1	Ta	0.5	W	1.5																			1972																												CuAl2																	CuAl2, C16	K		1.94					1.94	MTC12006																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112007	1377		B(W,Re)2	B1W1.26Re0.74	B	1	W	1.26	Re	0.74																			1972																												CuAl2																	CuAl2, C16	K		5.1					5.1	MTC12006																																																																																																				Compounds and pseudo-binary alloys with the CuAl2 (C16)-type structure: IV Superconductivity				J.LESS-COMMON METALS,27(1972)281	E.E.HAVINGA,H.DAMSMA,P.HOKKELING		
112008	469	Tc = 0.35 K for 0.28<x<0.33 in Sc1-xCox.	Sc1-xCox	Co0.3Sc0.7	Co	0.3	Sc	0.7																					1965																																														K		0.35					0.35																																																																																																arc-melting					SUPERCONDUCTIVITY IN BINARY ALLOY SYSTEMS OF THE RARE EARTH AND OF THORIUM WITH PT-GROUP METALS				PHYS.REV.,137(1965)A119	B.T.MATTHIAS,E.COREZWIT,G.W.HULL,JR.,L.D.LONGINOTTI,T.H.GEBALLE,V.B.COMPTON		
112009	717		Ti1-xRhx	Rh0.106Ti0.894	Rh	0.106	Ti	0.894																					1964																																														K		4.28					4.28	MTC12009																																																																																															arc-melting					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
112010	717		Ti1-xIrx	Ti1	Ti	1																							1964																																														K								MTC12010																																																																																															arc-melting					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
112011	717		Zr1-xIrx	Ir0.03Zr0.97	Ir	0.03	Zr	0.97																					1964																																														K		3.19					3.19	MTC12011																																																																																															arc-melting					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
112012	717		Zr1-xCox	Co0.03Zr0.97	Co	0.03	Zr	0.97																					1964																																														K		2.61					2.61	MTC12012																																																																																															arc-melting					Superconductivity of Solid Solutions of Ti and Zr with Co, Rh, and Ir 				PHYS.REV.,133(1964)A932	CH.J.RAUB,G.W.HULL JR.		
112013	253	using zone refined Nb.	Nb1-xWx	Nb0.95W0.05	Nb	0.95	W	0.05																					1961																																														K		7.25					7.25	MTC12013																																																																																															arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112014	253	using zone refined Nb.	Nb1-xWx	Nb0.85W0.15	Nb	0.85	W	0.15																					1961																																														K		5.32					5.32																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112015	253	using zone refined Nb.	Zr1-xNbx	Nb0.4Zr0.6	Nb	0.4	Zr	0.6																					1961																																														K		8.86					8.86																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112016	253	using zone refined Nb.	Zr1-xNbx	Nb0.5Zr0.5	Nb	0.5	Zr	0.5																					1961																																														K		9.46					9.46																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112017	253	using zone refined Nb.	Zr1-xNbx	Nb0.6Zr0.4	Nb	0.6	Zr	0.4																					1961																																														K		10.3					10.3																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112018	253	using zone refined Nb.	Zr1-xNbx	Nb0.7Zr0.3	Nb	0.7	Zr	0.3																					1961																																														K		10.8					10.8																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112019	253	using zone refined Nb.	Zr1-xNbx	Nb0.8Zr0.2	Nb	0.8	Zr	0.2																					1961																																														K		10.9					10.9																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112020	253	using zone refined Nb.	Zr1-xNbx	Nb0.9Zr0.1	Nb	0.9	Zr	0.1																					1961																																														K		10.7					10.7																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112021	253		Nb	Nb1	Nb	1																							1961																																														K		9.2					9.2																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112022	253		Nb1-xMox	Mo0.02Nb0.98	Mo	0.02	Nb	0.98																					1961																																														K		8.24					8.24																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112023	253		Nb1-xMox	Mo0.05Nb0.95	Mo	0.05	Nb	0.95																					1961																																														K		7.63					7.63																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112024	253		Nb1-xMox	Mo0.1Nb0.9	Mo	0.1	Nb	0.9																					1961																																														K		6.72					6.72																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112025	253		Nb1-xMox	Mo0.2Nb0.8	Mo	0.2	Nb	0.8																					1961																																														K		4.57					4.57																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112026	253		Nb1-xMox	Mo0.3Nb0.7	Mo	0.3	Nb	0.7																					1961																																														K		2.67					2.67																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112027	253		Mo1-xRex	Mo0.75Re0.25	Mo	0.75	Re	0.25																					1961																																														K		10					10	MTC12027																																																																																															arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112028	253		Mo1-xRex	Mo0.33Re0.67	Mo	0.33	Re	0.67																					1961																																														K		5.89					5.89																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112029	253		Ti1-xVx	Ti0.91V0.09	Ti	0.91	V	0.09																					1961																																														K		6.3					6.3																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112030	253		Ti1-xVx	Ti0.2V0.8	Ti	0.2	V	0.8																					1961																																														K		7.46					7.46																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112031	253		V	V1	V	1																							1961																																														K		5.15					5.15																																																								mj/mol.K2	9.3		338																																					arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112032	253		V1-xCrx	Cr0.06V0.94	Cr	0.06	V	0.94																					1961																																														K		2.93					2.93																																																								mj/mol.K2	8.4		342																																					arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112033	253		V1-xCrx	Cr0.1V0.9	Cr	0.1	V	0.9																					1961																																														K		1.88					1.88																																																								mj/mol.K2	7.5		344																																					arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112034	253	not s/c.	V1-xCrx	Cr0.2V0.8	Cr	0.2	V	0.8																					1961																																														K					1																																																										mj/mol.K2	6.4		351																																					arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112035	253		Ti1-xNbx	Nb0.35Ti0.65	Nb	0.35	Ti	0.65																					1961																																														K		7.69					7.69	MTC12035																																																																																															arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112036	253		Hf1-xTax	Hf0.5Ta0.5	Hf	0.5	Ta	0.5																					1961																																														K		6.28					6.28																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112037	253		Hf1-xTax	Hf0.32Ta0.68	Hf	0.32	Ta	0.68																					1961																																														K		6.68					6.68																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112038	253		Hf1-xTax	Hf0.16Ta0.84	Hf	0.16	Ta	0.84																					1961																																														K		5.98					5.98																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112039	253		Hf1-xTax	Hf0.08Ta0.92	Hf	0.08	Ta	0.92																					1961																																														K		5.38					5.38																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112040	253		Ta	Ta1	Ta	1																							1961																																														K		4.42					4.42																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112041	253		Ta1-xWx	Ta0.96W0.04	Ta	0.96	W	0.04																					1961																																														K		3.5					3.5																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112042	253		Ta1-xWx	Ta0.92W0.08	Ta	0.92	W	0.08																					1961																																														K		2.85					2.85																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112043	253		Ta1-xWx	Ta0.85W0.15	Ta	0.85	W	0.15																					1961																																														K		1.95					1.95																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112044	253		Ta1-xWx	Ta0.8W0.2	Ta	0.8	W	0.2																					1961																																														K		1.2					1.2																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112045	253		W1-xRex	Re0.4W0.6	Re	0.4	W	0.6																					1961																																														K		5.08					5.08	MTC12045																																																																																															arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112046	253		Hf1-xNbx	Hf0.5Nb0.5	Hf	0.5	Nb	0.5																					1961																																														K		8.31					8.31																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112047	253		Hf1-xNbx	Hf0.2Nb0.8	Hf	0.2	Nb	0.8																					1961																																														K		9.48					9.48																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112048	253		Hf1-xNbx	Hf0.1Nb0.9	Hf	0.1	Nb	0.9																					1961																																														K		9.6					9.6																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112049	253		Hf1-xNbx	Hf0.05Nb0.95	Hf	0.05	Nb	0.95																					1961																																														K		9.52					9.52																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112050	253		Nb1-xCrx	Cr0.05Nb0.95	Cr	0.05	Nb	0.95																					1961																																														K		6.66					6.66																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112051	253		Nb1-xCrx	Cr0.1Nb0.9	Cr	0.1	Nb	0.9																					1961																																														K		4.66					4.66																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112052	253	not s/c.	Nb1-xCrx	Cr0.2Nb0.8	Cr	0.2	Nb	0.8																					1961																																														K					1																																																																																																		arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112053	253		Ti1-xZrx	Ti0.65Zr0.35	Ti	0.65	Zr	0.35																					1961																																														K		1.37					1.37																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112054	253		Ti1-xZrx	Ti0.5Zr0.5	Ti	0.5	Zr	0.5																					1961																																														K		1.57					1.57																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112055	253		Ti1-xZrx	Ti0.3Zr0.7	Ti	0.3	Zr	0.7																					1961																																														K		1.36					1.36																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112056	253		Ti1-xZrx	Ti0.2Zr0.8	Ti	0.2	Zr	0.8																					1961																																														K		1.01					1.01																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112057	253		V1-xNbx	Nb0.4V0.6	Nb	0.4	V	0.6																					1961																																														K		4.11					4.11																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112058	253		V1-xNbx	Nb0.55V0.45	Nb	0.55	V	0.45																					1961																																														K		4.11					4.11																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112059	253		V1-xNbx	Nb0.6V0.4	Nb	0.6	V	0.4																					1961																																														K		4.17					4.17																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112060	253		V1-xNbx	Nb0.85V0.15	Nb	0.85	V	0.15																					1961																																														K		6					6																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112061	253		Nb1-xTax	Nb0.8Ta0.2	Nb	0.8	Ta	0.2																					1961																																														K		7.82					7.82																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112062	253		Nb1-xTax	Nb0.63Ta0.37	Nb	0.63	Ta	0.37																					1961																																														K		6.84					6.84																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112063	253		Nb1-xTax	Nb0.4Ta0.6	Nb	0.4	Ta	0.6																					1961																																														K		5.54					5.54																																																																																																arc-melting					SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112064	224		Ru1-xCrx	Cr0.3Ru0.7	Cr	0.3	Ru	0.7																					1962																																														K		0.38					0.38	MTC12064																																																																																															arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112065	224	sigma phase	Cr2Ru	Cr1Ru2	Cr	1	Ru	2																					1962																																														K		2					2																																																																																																arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112066	224		Cr3Ru	Cr1Ru3	Cr	1	Ru	3																					1962																												Cr3Si(A15)																	Cr3Si, A15	K		3.3					3.3																																																																																																arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112067	224	not annealed.	Cr0.875Ru0.125	Cr0.125Ru0.875	Cr	0.125	Ru	0.875																					1962																																														K		1.2					1.2																																																																																																arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112068	224		Rh1-xCrx	Cr0.7Rh0.3	Cr	0.7	Rh	0.3																					1962																																														K		1.1					1.1	MTC12068																																																																																															arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112069	224		Cr1-xIrx	Cr0.28Ir0.72	Cr	0.28	Ir	0.72																					1962																																														K		0.83					0.83	MTC12069																																																																																															arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112070	224		Cr1-xIrx	Cr0.09Ir0.91	Cr	0.09	Ir	0.91																					1962																																														K		0.78					0.78																																																																																																arc-melting					SUPERCONDUCTIVITY OF CHROMIUM ALLOYS				PHYS.REV.,128(1962)588	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALIE,V.B.COMPTON		
112071	441		Nb1-xMox	Mo0.3Nb0.7	Mo	0.3	Nb	0.7																					1963																																														K		2.48					2.48	MTC12071																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112072	441		Nb1-xWx	Nb0.8W0.2	Nb	0.8	W	0.2																					1963																																														K		4.68					4.68	MTC12072																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112073	441		Nb1-xCrx	Cr0.1Nb0.9	Cr	0.1	Nb	0.9																					1963																																														K		5					5	MTC12073																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112074	441		V1-xCrx	Cr0.1V0.9	Cr	0.1	V	0.9																					1963																																														K		2.06					2.06	MTC12074																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112075	441		Ta1-xHfx	Hf0.2Ta0.8	Hf	0.2	Ta	0.8																					1963																																														K		6.26					6.26	MTC12075																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112076	441		Ta1-xWx	Ta0.8W0.2	Ta	0.8	W	0.2																					1963																																														K		0.88					0.88	MTC12076																																																																																															arc-melting					SIZE FACTOR AND SUPERCONDUCTING PROPERTIES OF SOME TRANSITION METAL SOLUTIONS				PHYS.REV.,130(1963)2177	WARREN DESORBO		
112077	788		V1-xCrx	Cr0.1V0.9	Cr	0.1	V	0.9																					1969																																														K		3.21					3.21																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112078	788		V1-xCrx	Cr0.2V0.8	Cr	0.2	V	0.8																					1969																																														K		1.9					1.9																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112079	788		V1-xCrx	Cr0.25V0.75	Cr	0.25	V	0.75																					1969																																														K		1.36					1.36																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112080	788		V1-xCrx	Cr0.39V0.61	Cr	0.39	V	0.61																					1969																																														K		0.37					0.37																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112081	788		V1-xCrx	Cr0.48V0.52	Cr	0.48	V	0.52																					1969																																														K		0.1					0.1																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112082	788	not s/c	V1-xCrx	Cr0.58V0.42	Cr	0.58	V	0.42																					1969																																														K					0.015																																																																																																		arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112083	788	not s/c	V1-xCrx	Cr0.945V0.055	Cr	0.945	V	0.055																					1969																																														K					0.015																																																																																																		arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112084	788		Mo1-xCrx	Cr0.06Mo0.94	Cr	0.06	Mo	0.94																					1969																																														K		0.71					0.71																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112085	788		Mo1-xCrx	Cr0.15Mo0.85	Cr	0.15	Mo	0.85																					1969																																														K		0.5					0.5																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112086	788		Mo1-xCrx	Cr0.25Mo0.75	Cr	0.25	Mo	0.75																					1969																																														K		0.155					0.155																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112087	788		Mo1-xCrx	Cr0.4Mo0.6	Cr	0.4	Mo	0.6																					1969																																														K		0.095					0.095																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112088	788		Mo1-xCrx	Cr0.476Mo0.524	Cr	0.476	Mo	0.524																					1969																																														K		0.045					0.045																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112089	788		Mo1-xCrx	Cr0.57Mo0.43	Cr	0.57	Mo	0.43																					1969																																														K		0.03					0.03																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112090	788	not s/c	Mo1-xCrx	Cr0.73Mo0.27	Cr	0.73	Mo	0.27																					1969																																														K					0.015																																																																																																		arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112091	788		V1-xMox	Mo0.15V0.85	Mo	0.15	V	0.85																					1969																																														K		2.28					2.28																																																								mj/mol.K2	6.94		395																																					arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112092	788		V1-xMox	Mo0.3V0.7	Mo	0.3	V	0.7																					1969																																														K		0.76					0.76																																																								mj/mol.K2	5.15		403																																					arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112093	788		V1-xMox	Mo0.5V0.5	Mo	0.5	V	0.5																					1969																																														K		0.11					0.11																																																								mj/mol.K2	3.02		412																																					arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112094	788		Ru1-xFex	Fe0.018Ru0.982	Fe	0.018	Ru	0.982																					1969																																														K		0.165					0.165																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112095	788		Ru1-xFex	Fe0.031Ru0.969	Fe	0.031	Ru	0.969																					1969																																														K		0.054					0.054																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112096	788		Ru1-xFex	Fe0.043Ru0.957	Fe	0.043	Ru	0.957																					1969																																														K		0.018					0.018																																																																																																arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112097	788	not s/c	Ru1-xFex	Fe0.05Ru0.95	Fe	0.05	Ru	0.95																					1969																																														K					0.015																																																																																																		arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112098	788	not s/c	Ru1-xFex	Fe0.5Ru0.5	Fe	0.5	Ru	0.5																					1969																																														K					0.015																																																										mj/mol.K2	7.78		447																																					arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112099	788	not s/c	Ru1-xFex	Fe0.7Ru0.3	Fe	0.7	Ru	0.3																					1969																																														K					0.015																																																										mj/mol.K2	7.56		445																																					arc-melting									PHYS.REV.,178(1969)702	E.BUCHER,J.P.MAITA,K.ANDRES,R.C.SHERWOOD		
112100	920		U6Mn	Mn1U6	Mn	1	U	6																					1968																																														K		2.4					2.4																																																																																																arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112101	920		U6Mn1-xFex	U6Mn0.5Fe0.5	U	6	Mn	0.5	Fe	0.5																			1968																																														K		2.86					2.86	MTC12101																																																																																															arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112102	920		U6Fe	Fe1U6	Fe	1	U	6																					1968																																														K		3.88					3.88																																																																																																arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112103	920		U6Fe1-xCox	U6Fe0.5Co0.5	U	6	Fe	0.5	Co	0.5																			1968																																														K		3.05					3.05	MTC12103																																																																																															arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112104	920		U6Co	Co1U6	Co	1	U	6																					1968																																														K		2.41					2.41																																																																																																arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112105	920		U6Co1-xNix	U6Co0.5Ni0.5	U	6	Co	0.5	Ni	0.5																			1968																																														K		1.37					1.37	MTC12105																																																																																															arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112106	920		U6Ni	Ni1U6	Ni	1	U	6																					1968																																														K		0.41					0.41																																																																																																arc-melting									PHYS.REV.,168(1968)464	B.T.MATTHIAS,H.H.HILL		
112107	1890	Hc(0)=1349  Oe. (delta-C/gamma*Tc) = 1.47	V1-xCux	Cu0.005V0.995	Cu	0.005	V	0.995																					1974																																														K		4.92					4.92																																																								mj/mol.K2	10.4		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112108	1890	Hc(0)= 1303 Oe. (delta-C/gamma*Tc) = 1.44	V1-xCux	Cu0.01V0.99	Cu	0.01	V	0.99																					1974																																														K		4.74					4.74																																																								mj/mol.K2	10.4		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112109	1890	Hc(0)= 1195 Oe. (delta-C/gamma*Tc) = 1.40	V1-xCux	Cu0.025V0.975	Cu	0.025	V	0.975																					1974																																														K		4.45					4.45																																																								mj/mol.K2	9.8		421																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112110	1890	Hc(0)= 986 Oe. (delta-C/gamma*Tc) = 1.25	V1-xCux	Cu0.05V0.95	Cu	0.05	V	0.95																					1974																																														K		3.85					3.85																																																								mj/mol.K2	9.4		421																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112111	1890	Hc(0)= 1320 Oe. (delta-C/gamma*Tc) = 1.44	V1-xSix	Si0.005V0.995	Si	0.005	V	0.995																					1974																																														K		4.75					4.75																																																								mj/mol.K2	10.4		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112112	1890	Hc(0)= 1279 Oe. (delta-C/gamma*Tc) = 1.36	V1-xSix	Si0.01V0.99	Si	0.01	V	0.99																					1974																																														K		4.66					4.66																																																								mj/mol.K2	10.4		402																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112113	1890	Hc(0)= 1134 Oe. (delta-C/gamma*Tc) = 1.25	V1-xSix	Si0.025V0.975	Si	0.025	V	0.975																					1974																																														K		4.06					4.06																																																								mj/mol.K2	10		385																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112114	1890	Hc(0)= 725 Oe. (delta-C/gamma*Tc) = 1.22	V1-xSix	Si0.05V0.95	Si	0.05	V	0.95																					1974																																														K		2.95					2.95																																																								mj/mol.K2	8.2		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112115	1890	Hc(0)= 1446 Oe. (delta-C/gamma*Tc) = 1.47	V	V1	V	1																							1974																																														K		5.2					5.2																																																								mj/mol.K2	10.4		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112116	1890	Hc(0)= 1324 Oe. (delta-C/gamma*Tc) = 1.46	V1-xAlx	Al0.005V0.995	Al	0.005	V	0.995																					1974																																														K		4.82					4.82																																																								mj/mol.K2	10.4		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112117	1890	Hc(0)= 1242 Oe. (delta-C/gamma*Tc) = 1.45	V1-xAlx	Al0.01V0.99	Al	0.01	V	0.99																					1974																																														K		4.49					4.49																																																								mj/mol.K2	10.3		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112118	1890	Hc(0)= 1091 Oe. (delta-C/gamma*Tc) = 1.34	V1-xAlx	Al0.02V0.98	Al	0.02	V	0.98																					1974																																														K		4.05					4.05																																																								mj/mol.K2	9.6		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112119	1890	Hc(0)= 849 Oe. (delta-C/gamma*Tc) = 1.34	V1-xAlx	Al0.04V0.96	Al	0.04	V	0.96																					1974																																														K		3.31					3.31																																																								mj/mol.K2	9.1		402																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112120	1890	Hc(0)= 692 Oe. (delta-C/gamma*Tc) = 1.34	V1-xAlx	Al0.06V0.94	Al	0.06	V	0.94																					1974																																														K		2.83					2.83																																																								mj/mol.K2	8.8		394																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112121	1890	Hc(0)= 574 Oe. (delta-C/gamma*Tc) = 1.37	V1-xAlx	Al0.08V0.92	Al	0.08	V	0.92																					1974																																														K		2.36					2.36																																																								mj/mol.K2	8.5		392																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112122	1890	Hc(0)= 420 Oe. (delta-C/gamma*Tc) = 1.37	V1-xAlx	Al0.1V0.9	Al	0.1	V	0.9																					1974																																														K		1.96					1.96																																																								mj/mol.K2	7.55		402																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112123	1890	Hc(0)= 408 Oe. (delta-C/gamma*Tc) = 1.33	V1-xAlx	Al0.12V0.88	Al	0.12	V	0.88																					1974																																														K		1.73					1.73																																																								mj/mol.K2	7.5		391																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112124	1890	Hc(0)= 1204 Oe. (delta-C/gamma*Tc) = 1.36	V1-xSnx	Sn0.005V0.995	Sn	0.005	V	0.995																					1974																																														K		4.57					4.57																																																								mj/mol.K2	10		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112125	1890	Hc(0)= 1080 Oe. (delta-C/gamma*Tc) = 1.28	V1-xSnx	Sn0.01V0.99	Sn	0.01	V	0.99																					1974																																														K		4.21					4.21																																																								mj/mol.K2	9.6		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112126	1890	Hc(0)= 732 Oe. (delta-C/gamma*Tc) = 1.26	V1-xSnx	Sn0.025V0.975	Sn	0.025	V	0.975																					1974																																														K		3.16					3.16																																																								mj/mol.K2	8.6		411																																					arc-melting					The superconductivity of alloys of a transition metal with non-transition elements				J.PHYS.SOC.JAPAN,37(1974)384	K.KUMAGAI,T.OHTSUKA		
112127	415		Cr1-xRex	Cr0.56Re0.44	Cr	0.56	Re	0.44																					1964																																													bcc	K		5.1					5.1	MTC12127																																																																																															arc-melting					Superconductivity and electronic properties of transition metal alloys				REV.MOD.PHYS.,36(1964)146	E.BUCHER,F.HEINIGER,J.MUHEIM,J.MULLER		
112128	415		Cr1-xRex	Cr0.8Re0.2	Cr	0.8	Re	0.2																					1964																																													bcc	K		1.31					1.31	MTC12127																																																																																															arc-melting					Superconductivity and electronic properties of transition metal alloys				REV.MOD.PHYS.,36(1964)146	E.BUCHER,F.HEINIGER,J.MUHEIM,J.MULLER		
112129	415	sigma-phase	Cr1-xRex	Cr0.33Re0.67	Cr	0.33	Re	0.67																					1964																																														K		2.29					2.29	MTC12127																																																																																															arc-melting					Superconductivity and electronic properties of transition metal alloys				REV.MOD.PHYS.,36(1964)146	E.BUCHER,F.HEINIGER,J.MUHEIM,J.MULLER		
112130	415	not s/c.	Cr1-xRex	Cr0.86Re0.14	Cr	0.86	Re	0.14																					1964								500																																					bcc	K					1			MTC12127																																																																																															arc-melting					Superconductivity and electronic properties of transition metal alloys				REV.MOD.PHYS.,36(1964)146	E.BUCHER,F.HEINIGER,J.MUHEIM,J.MULLER		
112131	984		CuRh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																			1967																												spinel			A	9.78														K		4.8					4.8																																																																																																arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112132	984		CuRh2Se4	Cu1Rh2Se4	Cu	1	Rh	2	Se	4																			1967																												spinel			A	10.34														K		3.49					3.49																																																																																																arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112133	984		CuV2S4	Cu1V2S4	Cu	1	V	2	S	4																			1967																												spinel			A	9.82														K		4.45					4.45																																																																																																arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112134	984		CuCo2S4	Cu1Co2S4	Cu	1	Co	2	S	4																			1967																												spinel			A	9.48														K					0.05																																																																																																		arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112135	984		CuTi2S4	Cu1Ti2S4	Cu	1	Ti	2	S	4																			1967																												spinel			A	9.88														K					0.05																																																																																																		arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112136	984		(Cu,Co)Rh2S4	Cu0.98Co0.02Rh2S4	Cu	0.98	Co	0.02	Rh	2	S	4																	1967																												spinel																		K		1					1																																																																																																arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112137	984		Cu(Rh,Cr)2S4	Cu1Rh1.992Cr0.008S4	Cu	1	Rh	1.992	Cr	0.008	S	4																	1967																												spinel																		K		0.9					0.9																																																																																																arc-melting					Superconductivity in sulpho- and selenospinels				PHYS.LETT.A25(1967)238	F.K.LOTGERING,G.M.SCHAEFFER,N.H.VAN MAAREN		
112138	1570		Mo1-xIrx	Ir0.49Mo0.51	Ir	0.49	Mo	0.51																					1971																																													hcp	K		1.81					1.81																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112139	1570		Mo1-xIrx	Ir0.66Mo0.34	Ir	0.66	Mo	0.34																					1971																																													hcp	K		0.25					0.25																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112140	1570		Mo1-xIrx	Ir0.71Mo0.29	Ir	0.71	Mo	0.29																					1971																																													hcp	K		0.12					0.12																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112141	1570		Mo1-xIrx	Ir0.75Mo0.25	Ir	0.75	Mo	0.25																					1971																																													hcp	K		0.13					0.13																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112142	1570		Mo1-xRhx	Mo0.5Rh0.5	Mo	0.5	Rh	0.5																					1971																																													hcp	K		1.91					1.91																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112143	1570		Mo1-xRhx	Mo0.4Rh0.6	Mo	0.4	Rh	0.6																					1971																																													hcp	K		0.91					0.91																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112144	1570		Mo1-xRhx	Mo0.33Rh0.67	Mo	0.33	Rh	0.67																					1971																																													hcp	K		0.1					0.1																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112145	1570		Mo1-xRhx	Mo0.28Rh0.72	Mo	0.28	Rh	0.72																					1971																																													hcp	K		0.03					0.03																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112146	1570		Ru1-xCox	Co0.007Ru0.993	Co	0.007	Ru	0.993																					1971																																														K		0.4					0.4																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112147	1570		Ru1-xCox	Co0.015Ru0.985	Co	0.015	Ru	0.985																					1971																																														K		0.32					0.32																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112148	1570		Ru1-xCox	Co0.022Ru0.978	Co	0.022	Ru	0.978																					1971																																														K		0.27					0.27																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112149	1570		Ru1-xCox	Co0.027Ru0.973	Co	0.027	Ru	0.973																					1971																																														K		0.25					0.25																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112150	1570		Ru1-xCox	Co0.034Ru0.964	Co	0.034	Ru	0.964																					1971																																														K		0.2					0.2																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112151	1570		Ru1-xCox	Co0.07Ru0.93	Co	0.07	Ru	0.93																					1971																																														K		0.09					0.09																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112152	1570		Ru1-xNix	Ni0.007Ru0.993	Ni	0.007	Ru	0.993																					1971																																														K		0.44					0.44																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112153	1570		Ru1-xNix	Ni0.031Ru0.969	Ni	0.031	Ru	0.969																					1971																																														K		0.36					0.36																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112154	1570		Ru1-xNix	Ni0.08Ru0.92	Ni	0.08	Ru	0.92																					1971																																														K		0.2					0.2																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112155	1570		Ru1-xRhx	Rh0.04Ru0.96	Rh	0.04	Ru	0.96																					1971																																														K		0.38					0.38																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112156	1570		Ru1-xRhx	Rh0.105Ru0.895	Rh	0.105	Ru	0.895																					1971																																														K		0.27					0.27																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112157	1570		Ru1-xRhx	Rh0.2Ru0.8	Rh	0.2	Ru	0.8																					1971																																														K		0.18					0.18																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112158	1570		Ru1-xRhx	Rh0.32Ru0.68	Rh	0.32	Ru	0.68																					1971																																														K		0.11					0.11																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112159	1570		Ru1-xPdx	Pd0.015Ru0.985	Pd	0.015	Ru	0.985																					1971																																														K		0.4					0.4																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112160	1570		Ru1-xPtx	Pt0.014Ru0.986	Pt	0.014	Ru	0.986																					1971																																														K		0.43					0.43																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112161	1570		Ru1-xPtx	Pt0.06Ru0.94	Pt	0.06	Ru	0.94																					1971																																														K		0.29					0.29																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112162	1570		Ru1-xPtx	Pt0.113Ru0.887	Pt	0.113	Ru	0.887																					1971																																														K		0.21					0.21																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112163	1570		Ru1-xIrx	Ir0.036Ru0.964	Ir	0.036	Ru	0.964																					1971																																														K		0.41					0.41																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112164	1570		Ru1-xIrx	Ir0.14Ru0.86	Ir	0.14	Ru	0.86																					1971																																														K		0.28					0.28																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112165	1570		Ru1-xIrx	Ir0.22Ru0.78	Ir	0.22	Ru	0.78																					1971																																														K		0.21					0.21																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112166	1570		Ru1-xIrx	Ir0.32Ru0.68	Ir	0.32	Ru	0.68																					1971																																														K		0.18					0.18																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112167	1570		Ru1-xIrx	Ir0.43Ru0.57	Ir	0.43	Ru	0.57																					1971																																														K		0.18					0.18																																																																																																arc-melting					Possible spin fluctuation effects on superconductivity in the 4d h.c.p. transition series				PHYSICA,55(1971)622	G.RIBLET,M.A.JENSEN		
112168	714		CuRh2Se4	Cu1Rh2Se4	Cu	1	Rh	2	Se	4																			1970																												spinel																		K		3.5					3.5																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112169	714		Cu(Rh,Sn)2Se4	Cu1Rh1.9Sn0.1Se4	Cu	1	Rh	1.9	Sn	0.1	Se	4																	1970																												spinel																		K		2.86					2.86																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112170	714		Cu(Rh,Sn)2Se4	Cu1Rh1.78Sn0.22Se4	Cu	1	Rh	1.78	Sn	0.22	Se	4																	1970																												spinel																		K		1.92					1.92																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112171	714		Cu(Rh,Sn)2Se4	Cu1Rh1.7Sn0.3Se4	Cu	1	Rh	1.7	Sn	0.3	Se	4																	1970																												spinel																		K		1.26					1.26																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112172	714		Cu(Rh,Sn)2Se4	Cu1Rh1.6Sn0.4Se4	Cu	1	Rh	1.6	Sn	0.4	Se	4																	1970																												spinel																		K		0.57					0.57																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112173	714		Cu(Rh,Sn)2Se4	Cu1Rh1.5Sn0.5Se4	Cu	1	Rh	1.5	Sn	0.5	Se	4																	1970																												spinel																		K		0.14					0.14																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112174	714		RhSe2	Rh1Se2	Rh	1	Se	2																					1970																												FeS2(pyrite)																		K		4.35					4.35																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112175	714		(Rh,Ru)Se2	Rh0.88Ru0.12Se2	Rh	0.88	Ru	0.12	Se	2																			1970																												FeS2(pyrite)																		K		2.28					2.28																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112176	714		(Rh,Ru)Se2	Rh0.8Ru0.2Se2	Rh	0.8	Ru	0.2	Se	2																			1970																												FeS2(pyrite)																		K		1.33					1.33																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112177	714		(Rh,Ru)Se2	Rh0.7Ru0.3Se2	Rh	0.7	Ru	0.3	Se	2																			1970																												FeS2(pyrite)																		K		0.62					0.62																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112178	714		(Rh,Ru)Se2	Rh0.6Ru0.4Se2	Rh	0.6	Ru	0.4	Se	2																			1970																												FeS2(pyrite)																		K		0.18					0.18																																																																																																arc-melting					Critical carrier concentration for superconductivity in mixed metal-semiconductor system				SOLID STATE COMM.,8(1970)1933	E.E.HAVINGA,H.B.HARLAND,M.H.VAN MAAREN		
112180	200		La1-xCex	La1	La	1																							1960																																														K		6.24					6.24																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112181	200		La1-xCex	Ce0.005La0.995	Ce	0.005	La	0.995																					1960																																														K		5.27					5.27	MTC12181																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112182	200		La1-xCex	Ce0.03La0.97	Ce	0.03	La	0.97																					1960																																														K		1.21					1.21																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112183	200		La1-xNdx	La0.99Nd0.01	La	0.99	Nd	0.01																					1960																																														K		5.18					5.18	MTC12181																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112184	200		La1-xNdx	La0.96Nd0.04	La	0.96	Nd	0.04																					1960																																														K		1.72					1.72																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112185	200		La1-xSmx	La0.9916Sm0.0084	La	0.9916	Sm	0.0084																					1960																																														K		4.22					4.22	MTC12185																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112186	200		La1-xSmx	La0.9795Sm0.0205	La	0.9795	Sm	0.0205																					1960																																														K		1.27					1.27																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112187	200		La1-xHox	Ho0.0105La0.9895	Ho	0.0105	La	0.9895																					1960																																														K		5.2					5.2	MTC12185																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112188	200		La1-xHox	Ho0.0422La0.9578	Ho	0.0422	La	0.9578																					1960																																														K		1.2					1.2																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112189	200		La1-xEux	Eu0.0028La0.9972	Eu	0.0028	La	0.9972																					1960																																														K		5.51					5.51	MTC12189																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112190	200		La1-xEux	Eu0.0153La0.9847	Eu	0.0153	La	0.9847																					1960																																														K		1.58					1.58																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112191	200		La1-xTbx	La0.9974Tb0.0026	La	0.9974	Tb	0.0026																					1960																																														K		5.28					5.28	MTC12189																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112192	200		La1-xTbx	La0.987Tb0.013	La	0.987	Tb	0.013																					1960																																														K		1.38					1.38																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112193	200		La1-xErx	Er0.005La0.995	Er	0.005	La	0.995																					1960																																														K		5.94					5.94	MTC12193																																																																																															arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112194	200		La1-xErx	Er0.08La0.92	Er	0.08	La	0.92																					1960																																														K		1.44					1.44																																																																																																arc-melting					Further experiments concerning the spin-electron interactions in superconductors				J.PHYS.CHEM.SOLIDS,13(1960)156	B.T.MATTHIAS,E.CRENZWIT,H.SUHL		
112195	1242		KxW(O,F)3	K0.1W1O2.9F0.1	K	0.1	W	1	O	2.9	F	0.1																	1971																												bronze																		K		2.1					2.1	MTC12195																																																																																																				Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112196	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 100 %.	CsxW(O,F)3	Cs0.1W1O2.9F0.1	Cs	0.1	W	1	O	2.9	F	0.1																	1971																												bronze																		K		4.4					4.4	MTC12195																			kOe		8.5																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112197	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 100 %.	RbxW(O,F)3	Rb0.1W1O2.9F0.1	Rb	0.1	W	1	O	2.9	F	0.1																	1971																												bronze																		K		3.6					3.6	MTC12195																			kOe		9.4																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112198	1242		K0.1LixW(O,F)3	K0.1Li0.02W1O2.88F0.12	K	0.1	Li	0.02	W	1	O	2.88	F	0.12															1971																												bronze																		K		1.1					1.1																																																																																																					Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112199	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 80 %.	Rb0.1LixW(O,F)3	Rb0.1Li0.02W1O2.88F0.12	Rb	0.1	Li	0.02	W	1	O	2.88	F	0.12															1971																												bronze																		K		3.4					3.4																				kOe		6.9																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112200	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 80 %.	Rb0.1LixW(O,F)3	Rb0.1Li0.05W1O2.85F0.15	Rb	0.1	Li	0.05	W	1	O	2.85	F	0.15															1971																												bronze																		K		3.1					3.1																				kOe		5.7																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112201	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 80 %.	Rb0.1LixW(O,F)3	Rb0.1Li0.1W1O2.8F0.2	Rb	0.1	Li	0.1	W	1	O	2.8	F	0.2															1971																												bronze																		K		2					2																				kOe		4.3																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112202	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 100 %.	Cs0.1LixW(O,F)3	Cs0.1Li0.02W1O2.88F0.12	Cs	0.1	Li	0.02	W	1	O	2.88	F	0.12															1971																												bronze																		K		4					4																				kOe		6.2																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112203	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 60 %.	Cs0.1LixW(O,F)3	Cs0.1Li0.05W1O2.85F0.15	Cs	0.1	Li	0.05	W	1	O	2.85	F	0.15															1971																												bronze																		K		3.3					3.3																				kOe		5.2																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112204	1242	Hc2(0) maybe in kOe (not given). s/c volume fraction = 80 %.	Cs0.1LixW(O,F)3	Cs0.1Li0.1W1O2.8F0.2	Cs	0.1	Li	0.1	W	1	O	2.8	F	0.2															1971																												bronze																		K		2.1					2.1																				kOe		4.8																																																																															Superconductivity in the K, Rb, and Cs tungsten fkuoroxide bronzes				J.PHYS.CHEM.SOLIDS,32(1971)2345	F.F.HUBBLE,J.M.GULICK,W.G.MOULTON		
112205	601	not s/c. P-content not given.	NixFeyP	Ni0.48Fe0.31P1	Ni	0.48	Fe	0.31	P	1																			1965																																														K					0.99																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
112206	601	not s/c. P-content not given.	NixFeyP	Ni0.64Co0.16P1	Ni	0.64	Co	0.16	P	1																			1965																																														K					0.99																																																																																																							Superconducting phosphides of the transition metals				J.PHYS.CHEM.SOL.,26(1965)2037	J.K.HULM,P.N.YOCOM,R.D.BLAUGHER		
112207	194	Vickers hardness = 182-252	Ti1-xMox	Mo0.0708Ti0.9292	Mo	0.0708	Ti	0.9292																					1961																																													bcc	K		2.8					2.8																																																																																																arc-melting					Electrical resistivity, Hall effect and superconductivity of some b.c.c. titanium-molybdenum alloys				J.PHYS.CHEM.SOLIDS,20(1961)177	D.H.LEALIE,R.R.HAKE,T.G.BERLINCOURT		
112208	194	Vickers hardness = 239-252	Ti1-xMox	Mo0.0905Ti0.9095	Mo	0.0905	Ti	0.9095																					1961																																													bcc	K		3.05					3.05																																																																																																arc-melting					Electrical resistivity, Hall effect and superconductivity of some b.c.c. titanium-molybdenum alloys				J.PHYS.CHEM.SOLIDS,20(1961)177	D.H.LEALIE,R.R.HAKE,T.G.BERLINCOURT		
112209	194	Vickers hardness = 224-248	Ti1-xMox	Mo0.1215Ti0.8785	Mo	0.1215	Ti	0.8785																					1961																																													bcc	K		3.5					3.5																																																																																																arc-melting					Electrical resistivity, Hall effect and superconductivity of some b.c.c. titanium-molybdenum alloys				J.PHYS.CHEM.SOLIDS,20(1961)177	D.H.LEALIE,R.R.HAKE,T.G.BERLINCOURT		
112210	194	Vickers hardness = 239-271	Ti1-xMox	Mo0.1633Ti0.8367	Mo	0.1633	Ti	0.8367																					1961																																													bcc	K		4					4																																																																																																arc-melting					Electrical resistivity, Hall effect and superconductivity of some b.c.c. titanium-molybdenum alloys				J.PHYS.CHEM.SOLIDS,20(1961)177	D.H.LEALIE,R.R.HAKE,T.G.BERLINCOURT		
112211	1117		ThH3.63	H3.63Th1	H	3.63	Th	1																					1970																																														K		8.35					8.35																																																																																																direct reaction of Th and H2					Superconductivity of hydrides and deuterides of thorium				PHYS.REV.LETT.,25(1970)741	C.B.SATTERTHWAITE,I.L.TOEPKE		
112212	1117	x-ray pattern of Th4H15	ThD3.63	D3.63Th1	D	3.63	Th	1																					1970																																														K		8.05					8.05																																																																																																direct reaction of Th and D2					Superconductivity of hydrides and deuterides of thorium				PHYS.REV.LETT.,25(1970)741	C.B.SATTERTHWAITE,I.L.TOEPKE		
112213	1125		(La,Gd)3In	In1La3	In	1	La	3																					1967																																														K		9.2					9.2																																		MHC12213																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112214	1125		(La,Gd)3In	La2.9952Gd0.0048In1	La	2.9952	Gd	0.0048	In	1																			1967																																														K		8.5					8.5																																		MHC12213																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112215	1125		(La,Gd)3In	La2.9889Gd0.0111In1	La	2.9889	Gd	0.0111	In	1																			1967																																														K		7.92					7.92																																		MHC12213																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112216	1125		(La,Gd)3In	La2.9745Gd0.0255In1	La	2.9745	Gd	0.0255	In	1																			1967																																														K		6.92					6.92																																		MHC12213																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112217	1125		(La,Gd)3In	La2.9706Gd0.0294In1	La	2.9706	Gd	0.0294	In	1																			1967																																														K		6					6																																		MHC12217																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112218	1125		(La,Gd)3In	La2.9628Gd0.0372In1	La	2.9628	Gd	0.0372	In	1																			1967																																														K		5.04					5.04																																		MHC12217																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112219	1125		(La,Gd)3In	La2.9553Gd0.0447In1	La	2.9553	Gd	0.0447	In	1																			1967																																														K		4.3					4.3																																																																																																arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112220	1125		(La,Gd)3In	La2.952Gd0.048In1	La	2.952	Gd	0.048	In	1																			1967																																														K		3.48					3.48																																		MHC12220																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112221	1125		(La,Gd)3In	La2.9451Gd0.0549In1	La	2.9451	Gd	0.0549	In	1																			1967																																														K		2.71					2.71																																		MHC12220																																																														arc-melting					Superconductivity in the presence of magnetic exchange fields				PHYS.REV.LETT.,19(1967)77	J.E.CROW,R.D.PARKS,R.P.GUERTIN		
112222	1131		LaSn3	La1Sn3	La	1	Sn	3																					1968																												Cu3Au																		K		6.4					6.4																																																																																																					Relationship between the critical temperature and normal-state magnetic properties of a superconductor containing magnetic impurities				PHYS.REV.LETT.,21(1968)792	A.M.TOXEN,P.C.KWOK,R.J.GAMBINO		
112223	1131		(La,Gd)Sn3	La0.987Gd0.013Sn3	La	0.987	Gd	0.013	Sn	3																			1968							-0.99																					Cu3Au																		K		5.94					5.94	MTC12223																																																																																																				Relationship between the critical temperature and normal-state magnetic properties of a superconductor containing magnetic impurities				PHYS.REV.LETT.,21(1968)792	A.M.TOXEN,P.C.KWOK,R.J.GAMBINO		
112224	1131	x(critical) = 0.115 in this system.	(La,Gd)Sn3	La0.936Gd0.064Sn3	La	0.936	Gd	0.064	Sn	3																			1968							-4.72																					Cu3Au																		K		3.76					3.76	MTC12223																																																																																																				Relationship between the critical temperature and normal-state magnetic properties of a superconductor containing magnetic impurities				PHYS.REV.LETT.,21(1968)792	A.M.TOXEN,P.C.KWOK,R.J.GAMBINO		
112225	1131	not s/c	(La,Gd)Sn3	Gd1Sn3	Gd	1	Sn	3																					1968								31																				Cu3Au																		K																																																																																																												Relationship between the critical temperature and normal-state magnetic properties of a superconductor containing magnetic impurities				PHYS.REV.LETT.,21(1968)792	A.M.TOXEN,P.C.KWOK,R.J.GAMBINO		
112226	115		La1-xCex	Ce0.01La0.99	Ce	0.01	La	0.99																					1958																																														K		3.63					3.63																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112227	115		La1-xPrx	La0.99Pr0.01	La	0.99	Pr	0.01																					1958																																														K		5.23					5.23																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112228	115		La1-xNdx	La0.99Nd0.01	La	0.99	Nd	0.01																					1958																																														K		4.65					4.65																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112229	115		La1-xSmx	La0.99Sm0.01	La	0.99	Sm	0.01																					1958																																														K		4.5					4.5																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112230	115		La1-xEux	Eu0.01La0.99	Eu	0.01	La	0.99																					1958																																														K		3.79					3.79																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112231	115		La1-xGdx	Gd0.01La0.99	Gd	0.01	La	0.99																					1958																																														K		0.62					0.62																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112232	115		La1-xTbx	La0.99Tb0.01	La	0.99	Tb	0.01																					1958																																														K		2.53					2.53																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112233	115		La1-xDyx	Dy0.01La0.99	Dy	0.01	La	0.99																					1958																																														K		3.74					3.74																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112234	115		La1-xHox	Ho0.01La0.99	Ho	0.01	La	0.99																					1958																																														K		5.18					5.18																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112235	115		La1-xErx	Er0.01La0.99	Er	0.01	La	0.99																					1958																																														K		5.31					5.31																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112236	115		La1-xYbx	La0.99Yb0.01	La	0.99	Yb	0.01																					1958																																														K		5.5					5.5																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112237	115		La1-xLux	La0.99Lu0.01	La	0.99	Lu	0.01																					1958																																														K		5.59					5.59																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112238	115		La1-xGdx	Gd0.004La0.996	Gd	0.004	La	0.996																					1958																																														K		3.59					3.59	MTC12238																																																																																																				SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112239	115		ScRu2	Ru2Sc1	Ru	2	Sc	1																					1958																																														K		1.67					1.67																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112240	115		YRu2	Ru2Y1	Ru	2	Y	1																					1958																																														K		1.52					1.52																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112241	115		LaRu2	La1Ru2	La	1	Ru	2																					1958																																														K		1.63					1.63																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112242	115		CeRu2	Ce1Ru2	Ce	1	Ru	2																					1958																																														K		4.9					4.9																																																																																																					SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112243	115	Ferromagnetic	PrRu2	Pr1Ru2	Pr	1	Ru	2																					1958							40																																							K																																																																																																												SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112244	115	Ferromagnetic	NdRu2	Nd1Ru2	Nd	1	Ru	2																					1958							35																																							K																																																																																																												SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112245	115	Ferromagnetic	ErRu2	Er1Ru2	Er	1	Ru	2																					1958							13																																							K																																																																																																												SPIN EXCHANGE IN SUPERCONDUCTORS				PHYS.REV.LETT.,1(1958)92,152E	B.T.MATTHIAS,E.CORENZWIT		
112246	143	type-I s/c. Hc2 = H0, (dHc2/dT) = (dH0/dT)	In	In1	In	1																							1960																																														K		3.407					3.407																				Oe		293							Oe/K		155.5																																																																						SUPERCONDUCTIVITY OF DILUTE INDIUM-MERCURY ALLOYS				PHYS.REV.,117(1960)1476	MORTON D.REEBER		
112247	143		In1-xHgx	Hg0.004In0.996	Hg	0.004	In	0.996																					1960																																														K		3.396					3.396																																																																																																					SUPERCONDUCTIVITY OF DILUTE INDIUM-MERCURY ALLOYS				PHYS.REV.,117(1960)1476	MORTON D.REEBER		
112248	143		In1-xHgx	Hg0.016In0.984	Hg	0.016	In	0.984																					1960																																														K		3.342					3.342	MTC12248																																																																																																				SUPERCONDUCTIVITY OF DILUTE INDIUM-MERCURY ALLOYS				PHYS.REV.,117(1960)1476	MORTON D.REEBER		
112249	143		In1-xHgx	Hg0.048In0.952	Hg	0.048	In	0.952																					1960																																														K		3.427					3.427																																																																																																					SUPERCONDUCTIVITY OF DILUTE INDIUM-MERCURY ALLOYS				PHYS.REV.,117(1960)1476	MORTON D.REEBER		
112250	1896	e-ph coupling = 0.86	V3Ga	Ga1V3	Ga	1	V	3																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		14.5					14.5																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112251	1896	e-ph coupling = 0.70	V3(Ga,Si)	V3Ga0.8Si0.2	V	3	Ga	0.8	Si	0.2																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		11.9					11.9																																																											388																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112252	1896	e-ph coupling = 0.67	V3(Ga,Si)	V3Ga0.2Si0.8	V	3	Ga	0.2	Si	0.8																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		10.5					10.5																																																											472																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112253	1896	e-ph coupling = 0.65	V3(Ga,Si)	V3Ga0.6Si0.4	V	3	Ga	0.6	Si	0.4																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		9.5					9.5																																																											416																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112254	1896	e-ph coupling = 0.64	V3(Ga,Si)	V3Ga0.4Si0.6	V	3	Ga	0.4	Si	0.6																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		8.7					8.7																																																											444																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112255	1896	e-ph coupling = 0.76	V3Si	Si1V3	Si	1	V	3																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		16.7					16.7																																																											498																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112256	1896	e-ph coupling = 0.73	V3(Ga,Sn)	V3Ga0.9Sn0.1	V	3	Ga	0.9	Sn	0.1																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		10.7					10.7																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112257	1896	e-ph coupling = 0.63	V3(Ga,Sn)	V3Ga0.7Sn0.3	V	3	Ga	0.7	Sn	0.3																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		7.2					7.2																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112258	1896	e-ph coupling = 0.60	V3(Ga,Sn)	V3Ga0.5Sn0.5	V	3	Ga	0.5	Sn	0.5																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		5.6					5.6																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112259	1896	e-ph coupling = 0.53	V3(Ga,Sn)	V3Ga0.1Sn0.9	V	3	Ga	0.1	Sn	0.9																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		3.8					3.8																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112260	1896	e-ph coupling = 0.48	V3Sn	Sn1V3	Sn	1	V	3																					1974																												Cr3Si(A15)																	Cr3Si, A15	K		3.4					3.4																																																											360																																										Relationship between Tc and N(0): An NMR study of V3Ga1-xSix				PHYS.REV.B,10(1974)2803	F.Y.FRADIN,J.D.WWILLIAMSON		
112261	1663	gap = 1.38 meV.  RRR = 59.5	Pb	Pb1	Pb	1																							1972																																														K		7.19					7.19																																																4.45																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112262	1663	gap = 1.39 meV.  RRR = 17.2	Pb1-xInx	In0.005Pb0.995	In	0.005	Pb	0.995																					1972																																														K		7.181					7.181																																																4.48																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112263	1663	gap = 1.40 meV.  RRR = 16.3	Pb1-xInx	In0.01Pb0.99	In	0.01	Pb	0.99																					1972																																														K		7.173					7.173																																																4.54																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112264	1663	gap = 1.40 meV.  RRR = 12.3	Pb1-xInx	In0.02Pb0.98	In	0.02	Pb	0.98																					1972																																														K		7.15					7.15																																																4.53																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112265	1663	gap = 1.39 meV.  RRR = 6.9	Pb1-xInx	In0.04Pb0.96	In	0.04	Pb	0.96																					1972																																														K		7.075					7.075																																																4.54																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112266	1663	gap = 1.39 meV.  RRR = 5.9	Pb1-xInx	In0.06Pb0.94	In	0.06	Pb	0.94																					1972																																														K		7.061					7.061																																																4.56																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112267	1663	gap = 1.38 meV.  RRR = 4.2	Pb1-xInx	In0.08Pb0.92	In	0.08	Pb	0.92																					1972																																														K		7.025					7.025																																																4.56																																																flash evaporation, quench					Electron-tunneling studies of dilute Pb-based In alloys				PHYS.REV.B,6(1972)136	B.R.SOOD		
112268	576		Sn	Sn1	Sn	1																							1965																																														K		3.73					3.73																																																																																																heat in quartz tube, quench					SUPERCONDUCTIVITY IN THE TIN-GALLIUM SYSTEM				PHYS.REV.,140(1965)A528	GORDON KNAPP,M.F.MERRIAM		
112269	576		Sn1-xGax	Ga0.01Sn0.99	Ga	0.01	Sn	0.99																					1965																																														K		3.726					3.726																																																																																																heat in quartz tube, quench					SUPERCONDUCTIVITY IN THE TIN-GALLIUM SYSTEM				PHYS.REV.,140(1965)A528	GORDON KNAPP,M.F.MERRIAM		
112270	576		Sn1-xGax	Ga0.02Sn0.98	Ga	0.02	Sn	0.98																					1965																																														K		3.726					3.726																																																																																																heat in quartz tube, quench					SUPERCONDUCTIVITY IN THE TIN-GALLIUM SYSTEM				PHYS.REV.,140(1965)A528	GORDON KNAPP,M.F.MERRIAM		
112271	576		Sn1-xGax	Ga0.04Sn0.96	Ga	0.04	Sn	0.96																					1965																																														K		3.887					3.887																																																																																																heat in quartz tube, quench					SUPERCONDUCTIVITY IN THE TIN-GALLIUM SYSTEM				PHYS.REV.,140(1965)A528	GORDON KNAPP,M.F.MERRIAM		
112272	576		Sn1-xGax	Ga0.05Sn0.95	Ga	0.05	Sn	0.95																					1965																																														K		3.938					3.938																																																																																																heat in quartz tube, quench					SUPERCONDUCTIVITY IN THE TIN-GALLIUM SYSTEM				PHYS.REV.,140(1965)A528	GORDON KNAPP,M.F.MERRIAM		
112273	445	beta-phase. discontinuity in Tc at 10.5 at % In.	Hg1-xInx	Hg0.9In0.1	Hg	0.9	In	0.1																					1964																																														K		3.73					3.73	MTC12273																																																																																																				Brillouin zone effects in superconductivity				REV.MOD.PHYS.,36(1964)152	M.F.MERRIAM		
112274	445		In1-xSnx	In0.92Sn0.08	In	0.92	Sn	0.08																					1964																																														K		4.25					4.25	MTC12274																																																																																																				Brillouin zone effects in superconductivity				REV.MOD.PHYS.,36(1964)152	M.F.MERRIAM		
112275	445		In1-xPbx	In0.9Pb0.1	In	0.9	Pb	0.1																					1964																																														K		4.36					4.36	MTC12275																																																																																																				Brillouin zone effects in superconductivity				REV.MOD.PHYS.,36(1964)152	M.F.MERRIAM		
112276	1490		(La,Gd)Ru2	La1Ru2	La	1	Ru	2																					1972																												MgCu2(Laves)																	MgCu2, C15	K		4.07					4.07																																																																																																arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112277	1490		(La,Gd)Ru2	La0.98Gd0.02Ru2	La	0.98	Gd	0.02	Ru	2																			1972																												MgCu2(Laves)																	MgCu2, C15	K		3.23					3.23																																																																																																arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112278	1490		(La,Gd)Ru2	La0.97Gd0.03Ru2	La	0.97	Gd	0.03	Ru	2																			1972																												MgCu2(Laves)																	MgCu2, C15	K		2.73					2.73																																																																																																arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112279	1490		(La,Gd)Ru2	La0.96Gd0.04Ru2	La	0.96	Gd	0.04	Ru	2																			1972																												MgCu2(Laves)																	MgCu2, C15	K		2.27					2.27																																																																																																arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112280	1490		(La,Gd)Ru2	La0.95Gd0.05Ru2	La	0.95	Gd	0.05	Ru	2																			1972																												MgCu2(Laves)																	MgCu2, C15	K		1.61					1.61																																																																																																arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112281	1490	not s/c	(La,Gd)Ru2	La0.94Gd0.06Ru2	La	0.94	Gd	0.06	Ru	2																			1972							2.3																					MgCu2(Laves)																	MgCu2, C15	K																																																																																																							arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112282	1490	not s/c	(La,Gd)Ru2	La0.92Gd0.08Ru2	La	0.92	Gd	0.08	Ru	2																			1972							3.67																					MgCu2(Laves)																	MgCu2, C15	K																																																																																																							arc-melting					Superconducting and magnetic properties of La1-xGdxRu2 and La1-xPrxRu2 mixed crystals				PHYS.LETT.A,40(1972)387	B.HILLENBRAND,M.WILHELM		
112283	1816		Hf1-xTax	Hf0.61Ta0.39	Hf	0.61	Ta	0.39																					1972																																														K		5.71					5.71			K/GPa	0.05																																																							160																																					arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112284	1816		Hf1-xTax	Hf0.52Ta0.48	Hf	0.52	Ta	0.48																					1972																																														K		6.61					6.61			K/GPa	0.052																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112285	1816		Hf1-xTax	Hf0.4Ta0.6	Hf	0.4	Ta	0.6																					1972																															A	3.591														K		6.85					6.85			K/GPa	0.039																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112286	1816		Hf1-xTax	Hf0.2Ta0.8	Hf	0.2	Ta	0.8																					1972																															A	3.341														K		6.9					6.9			K/GPa	0.025																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112287	1816		Hf1-xTax	Hf0.1Ta0.9	Hf	0.1	Ta	0.9																					1972																																														K		5.6					5.6			K/GPa	-0.015																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112288	1816		Hf1-xTax	Ta1	Ta	1																							1972																																														K		4.21					4.21			K/GPa	-0.026																																																							259																																					arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112289	1816	dTc/dP is for P>1 GPa. For P=0, dTc/dp = +0.0003 K/GPa	Ta1-xWx	Ta0.96W0.04	Ta	0.96	W	0.04																					1972																																														K		3.3					3.3			K/GPa	-0.019																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112290	1816	dTc/dP is for P>1 GPa. For P=0, dTc/dp = +0.012 K/GPa	Ta1-xWx	Ta0.91W0.09	Ta	0.91	W	0.09																					1972																																														K		2.78					2.78			K/GPa	-0.022																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112291	1816	dTc/dP is for P>1 GPa. For P=0, dTc/dp = +0.0093 K/GPa	Ta1-xWx	Ta0.84W0.16	Ta	0.84	W	0.16																					1972																																														K		1.86					1.86			K/GPa	-0.021																																																							266																																					arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112292	1816	dTc/dP is for P>1 GPa. For P=0, dTc/dp = +0.0057 K/GPa	Ta1-xWx	Ta0.78W0.22	Ta	0.78	W	0.22																					1972																																														K		1.36					1.36			K/GPa	-0.016																																																																																												arc-melting					Superconductivity of Hf-Ta and Ta-W alloys under pressure				Z.PHYS.,255(1972)308	W.GEY		
112293	1596		In1-xMgx	In0.966Mg0.034	In	0.966	Mg	0.034																					1974																																														K		3.61					3.61	MTC12293																																																																																																				Superconducting transition temperature of indium-magnesium alloys				PHYS.LETT.A,49(1974)73	C.SULKOWSKI,J.MAZUR		
112294	1596		In1-xMgx	In0.82Mg0.18	In	0.82	Mg	0.18																					1974																																														K		3.67					3.67																																																																																																					Superconducting transition temperature of indium-magnesium alloys				PHYS.LETT.A,49(1974)73	C.SULKOWSKI,J.MAZUR		
112295	1982		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1964																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																					Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112296	1982		Nb3(Ga,Sn)	Nb3Ga0.05Sn0.95	Nb	3	Ga	0.05	Sn	0.95																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3	MTC12297																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112297	1982		Nb3(In,Sn)	Nb3In0.15Sn0.85	Nb	3	In	0.15	Sn	0.85																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3	MTC12297																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112298	1982		Nb3(Tl,Sn)	Nb3Tl0.1Sn0.9	Nb	3	Tl	0.1	Sn	0.9																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.25					18.25	MTC12297																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112299	1982		Nb3(Ge,Sn)	Nb3Ge0.1Sn0.9	Nb	3	Ge	0.1	Sn	0.9																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		17.97					17.97	MTC12299																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112300	1982		Nb3(Pb,Sn)	Nb3Pb0.15Sn0.85	Nb	3	Pb	0.15	Sn	0.85																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.24					18.24	MTC12299																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112301	1982		Nb3(As,Sn)	Nb3As0.05Sn0.95	Nb	3	As	0.05	Sn	0.95																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.19					18.19	MTC12302																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112302	1982		Nb3(Sb,Sn)	Nb3Sb0.1Sn0.9	Nb	3	Sb	0.1	Sn	0.9																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		17.04					17.04	MTC12302																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112303	1982		Nb3(Bi,Sn)	Nb3Bi0.15Sn0.85	Nb	3	Bi	0.15	Sn	0.85																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.28					18.28	MTC12302																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112304	1982		Nb3(Al,Sn)	Nb3Al0.05Sn0.95	Nb	3	Al	0.05	Sn	0.95																			1964																												Cr3Si(A15)																	Cr3Si, A15	K		18.2					18.2	MTC12299																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112305	1982		Nb3(In,Sb,Sn)	Nb3In0.2Sb0.2Sn0.6	Nb	3	In	0.2	Sb	0.2	Sn	0.6																	1964																																														K		16					16	MTC12305																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112306	1982		Nb3(Ge,Pb,Sn)	Nb3Ge0.2Pb0.2Sn0.6	Nb	3	Ge	0.2	Pb	0.2	Sn	0.6																	1964																																														K		17.84					17.84	MTC12305																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112307	1982		Nb3(Ga,Bi,Sn)	Nb3Ga0.2Bi0.2Sn0.6	Nb	3	Ga	0.2	Bi	0.2	Sn	0.6																	1964																																														K		18.06					18.06	MTC12305																																																																																																				Zur Suraleitung in Mischsystemen mit Nb3Sn				Z.PHYS.,177(1964)10	R.HAGNER		
112308	1072		Nb3(Al,Ge)	Nb3Al0.72Ge0.28	Nb	3	Al	0.72	Ge	0.28																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		19.9					19.9	MTC12308																																																																																																				Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112309	1072		Nb3(Al,Ga)	Nb3Al0.67Ga0.33	Nb	3	Al	0.67	Ga	0.33																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.7					18.7	MTC12308																																																																																																				Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112310	1072		Nb3(Al,In)	Nb3Al0.8In0.2	Nb	3	Al	0.8	In	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1	MTC12308																																																																																																				Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112311	1072		Nb3(Al,Sn)	Nb3Al0.5Sn0.5	Nb	3	Al	0.5	Sn	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16					16	MTC12308																																																																																																				Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112312	1072		Nb3(Sn,Ga)	Nb3Sn0.91Ga0.09	Nb	3	Sn	0.91	Ga	0.09																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.3					18.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112313	1072		Nb3(Sn,Ga)	Nb3Sn0.65Ga0.35	Nb	3	Sn	0.65	Ga	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.5					16.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112314	1072		Nb3(Sn,Ga)	Nb3Sn0.49Ga0.51	Nb	3	Sn	0.49	Ga	0.51																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112315	1072		Nb3(Sn,Ge)	Nb3Sn0.95Ge0.05	Nb	3	Sn	0.95	Ge	0.05																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112316	1072		Nb3(Sn,Ge)	Nb3Sn0.8Ge0.2	Nb	3	Sn	0.8	Ge	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.65					17.65																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112317	1072		Nb3(Sn,Ge)	Nb3Sn0.65Ge0.35	Nb	3	Sn	0.65	Ge	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112318	1072		Nb3(Sn,In)	Nb3Sn0.9In0.1	Nb	3	Sn	0.9	In	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112319	1072		Nb3(Sn,In)	Nb3Sn0.8In0.2	Nb	3	Sn	0.8	In	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112320	1072		Nb3(Sn,Al)	Nb3Sn0.91Al0.09	Nb	3	Sn	0.91	Al	0.09																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.8					17.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112321	1072		Nb3(Sn,Al)	Nb3Sn0.8Al0.2	Nb	3	Sn	0.8	Al	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.8					16.8																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112322	1072		Nb3(Sn,Al)	Nb3Sn0.7Al0.3	Nb	3	Sn	0.7	Al	0.3																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.75					15.75																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112323	1072		Nb3(Sn,Al)	Nb3Sn0.6Al0.4	Nb	3	Sn	0.6	Al	0.4																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.7					15.7																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112324	1072		Nb3(Sn,Al)	Nb3Sn0.5Al0.5	Nb	3	Sn	0.5	Al	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112325	1072		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1968																												Cr3Si(A15)																	Cr3Si, A15	K		18					18																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112326	1072		Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112327	1072		Nb3(Ga,Ge)	Nb3Ga0.95Ge0.05	Nb	3	Ga	0.95	Ge	0.05																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		15.4					15.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112328	1072		Nb3(Ga,Al)	Nb3Ga0.85Al0.15	Nb	3	Ga	0.85	Al	0.15																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		17.1					17.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112329	1072		Nb3(Ga,Al)	Nb3Ga0.65Al0.35	Nb	3	Ga	0.65	Al	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112330	1072		Nb3(Ga,Al)	Nb3Ga0.5Al0.5	Nb	3	Ga	0.5	Al	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		18.5					18.5																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112331	1072		Nb3(Ga,Sn)	Nb3Ga0.9Sn0.1	Nb	3	Ga	0.9	Sn	0.1																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.1					16.1																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112332	1072		Nb3(Ga,Sn)	Nb3Ga0.8Sn0.2	Nb	3	Ga	0.8	Sn	0.2																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.2					16.2																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112333	1072		Nb3(Ga,Sn)	Nb3Ga0.65Sn0.35	Nb	3	Ga	0.65	Sn	0.35																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.3					16.3																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112334	1072		Nb3(Ga,Sn)	Nb3Ga0.5Sn0.5	Nb	3	Ga	0.5	Sn	0.5																			1968																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																					Zur Supraleitung einiger Mischsysteme von Verbindungen mit A15-Struktur auf Niobbasis				Z.PHYS.,215(1968)323	G.OTTO		
112335	956		Hf1-xWx	Hf0.909W0.091	Hf	0.909	W	0.091																					1970																																													bcc	K		2.38					2.38																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112336	956		Hf1-xWx	Hf0.834W0.166	Hf	0.834	W	0.166																					1970																																													bcc	K		2.79					2.79																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112337	956		Hf1-xWx	Hf0.78W0.22	Hf	0.78	W	0.22																					1970																																													bcc	K		2.77					2.77																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112338	956		Hf1-xWx	Hf0.661W0.339	Hf	0.661	W	0.339																					1970																																													bcc	K		2.51					2.51																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112339	956		Hf1-xWx	Hf0.33W0.67	Hf	0.33	W	0.67																					1970																																													bcc	K					0.05																																																																																																							Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112340	956		Zr1-xWx	W0.054Zr0.946	W	0.054	Zr	0.946																					1970																															A	3.561														K		3.88					3.88																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112341	956		Zr1-xWx	W0.014Zr0.986	W	0.014	Zr	0.986																					1970																															A	3.56														K		3.64					3.64	MTC12341																																																																																																				Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112342	956		Zr1-xWx	W0.801Zr0.199	W	0.801	Zr	0.199																					1970																															A	3.182														K		2.01					2.01																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112344	956		Zr1-xWx	W0.9Zr0.1	W	0.9	Zr	0.1																					1970																																														K					1.18																																																																																																							Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112345	956		Hf1-xMox	Hf0.915Mo0.085	Hf	0.915	Mo	0.085																					1970																															A	3.513														K		2.13					2.13																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112346	956		Hf1-xMox	Hf0.654Mo0.346	Hf	0.654	Mo	0.346																					1970																															A	3.391														K		2.92					2.92	MTC12346																																																																																																				Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112347	956		Hf1-xMox	Hf0.34Mo0.66	Hf	0.34	Mo	0.66																					1970																															A	3.254														K		1					1																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112348	956		Zr1-xMox	Mo0.059Zr0.941	Mo	0.059	Zr	0.941																					1970																															A	3.567														K		4.15					4.15	MTC12348																																																																																																				Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112349	956		Zr1-xMox	Mo0.202Zr0.798	Mo	0.202	Zr	0.798																					1970																															A	3.492														K		5.25					5.25																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112350	956		Zr1-xMox	Mo0.67Zr0.33	Mo	0.67	Zr	0.33																					1970																															A	3.262														K		1.56					1.56																																																																																																					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112351	956		Zr1-xMox	Mo0.724Zr0.276	Mo	0.724	Zr	0.276																					1970																																														K					1.08																																																																																																							Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112352	956		ZrMo2	Mo2Zr1	Mo	2	Zr	1																					1970																												MgCu2(Laves)			A	7.5888													MgCu2, C15	K					0.35																																																																																																		arc-melting					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112353	956		ZrW2	W2Zr1	W	2	Zr	1																					1970																												MgCu2(Laves)			A	7.6187													MgCu2, C15	K					0.35																																																																																																		arc-melting					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112354	956		HfMo2	Hf1Mo2	Hf	1	Mo	2																					1970																												MgCu2(Laves)			A	7.545													MgCu2, C15	K		0.07					0.07																																																																																																arc-melting					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112355	956		HfW2	Hf1W2	Hf	1	W	2																					1970																												MgCu2(Laves)			A	7.5825													MgCu2, C15	K					0.35																																																																																																		arc-melting					Superconductivity and lattice parameters in the Zr-Mo, Zr-W, Hf-Mo, and Hf-W alloy systems				J.LESS-COMMON METALS,21(1970)27	O.RAPP		
112356	1058		Hf1-xRhx	Hf0.96Rh0.04	Hf	0.96	Rh	0.04																					1966																																														K		2.34					2.34	MTC12356																																																																																																								Z.PHYS.,197(1966)276	H.WUHL		
112357	1058		Hf1-xRhx	Hf0.9Rh0.1	Hf	0.9	Rh	0.1																					1966																																														K		1.9					1.9																																																																																																									Z.PHYS.,197(1966)276	H.WUHL		
112358	1058		Hf1-xRhx	Hf0.8Rh0.2	Hf	0.8	Rh	0.2																					1966																																														K		1.95					1.95																																																																																																									Z.PHYS.,197(1966)276	H.WUHL		
112359	1456		V3(Si,Ge)	V75Si20Ge5	V	75	Si	20	Ge	5																			1973																																														K		12.15					12.15																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112360	1456		V3(Si,Ge)	V75Si12.5Ge12.5	V	75	Si	12.5	Ge	12.5																			1973																																														K		8.58					8.58																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112361	1456		V3(Si,Ge)	V75Si5Ge20	V	75	Si	5	Ge	20																			1973																																														K		6.76					6.76																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112362	1456		V3(Ge,Sn)	V75Ge20Sn5	V	75	Ge	20	Sn	5																			1973																																														K		5.46					5.46																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112363	1456	not s/c	V3(Ge,Sn)	V75Ge12.5Sn12.5	V	75	Ge	12.5	Sn	12.5																			1973																																														K																																																																																																							arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112364	1456	not s/c	V3(Ge,Sn)	V75Ge5Sn20	V	75	Ge	5	Sn	20																			1973																																														K																																																																																																							arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112365	1456		V3(Ge,Sb)	V75Ge20Sb5	V	75	Ge	20	Sb	5																			1973																																														K		5.86					5.86																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112366	1456		V3(Ge,Sb)	V75Ge12.5Sb12.49	V	75	Ge	12.5	Sb	12.49																			1973																																														K		4.71					4.71																																																																																																arc-melting					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112367	1456		V3(Si,Ga)	V75Si20Ga5	V	75	Si	20	Ga	5																			1973																												Cr3Si(A15)			A	4.734													Cr3Si, A15	K		12.33					12.33																																																																																																as-melted					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112368	1456		V3(Si,Ga)	V75Si12.5Ga12.5	V	75	Si	12.5	Ga	12.5																			1973																												Cr3Si(A15)			A	4.755													Cr3Si, A15	K		8.15					8.15																																																																																																as-melted					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112369	1456	A15 + unknown phase	V3(Si,Ga)	V75Si5Ga20	V	75	Si	5	Ga	20																			1973																												Cr3Si(A15)			A	4.795													Cr3Si, A15	K		10.58					10.58																																																																																																as-melted					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112370	1456	A15 + unknown phase	V3(Si,Ga)	V75Si2.57Ga22.4	V	75	Si	2.57	Ga	22.4																			1973																												Cr3Si(A15)			A	4.82													Cr3Si, A15	K		13.32					13.32																																																																																																sintered					The structure and superconducting transitions of some pseudobinary 'beta-W' alloys				J.LOW TEMP.PHYS.,10(1973)285	B.A.HATT,J.K.R.PAGE,V.G.RIVLIN		
112371	1311	not s/c	PdHx	H0.73Pd1	H	0.73	Pd	1																					1972																																														K					1.17																																																																																																											PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112372	1311		PdHx	H0.81Pd1	H	0.81	Pd	1																					1972																																														K		1.21					1.21																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112373	1311		PdHx	H0.87Pd1	H	0.87	Pd	1																					1972																																														K		2.95					2.95																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112374	1311	Tc is Tc (on). Tc(mid) < 1.32.	(Pd,Ni)Hx	Pd0.985Ni0.015H0.75	Pd	0.985	Ni	0.015	H	0.75																			1972																																														K		1.72					1.72																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112375	1311		(Pd,Ni)Hx	Pd0.985Ni0.015H0.79	Pd	0.985	Ni	0.015	H	0.79																			1972																																														K		2.8					2.8																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112376	1311	Tc(on) = 5.44 K. broad transition.	(Pd,Ni)Hx	Pd0.985Ni0.015H0.84	Pd	0.985	Ni	0.015	H	0.84																			1972																																														K		2.52					2.52																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112377	1311	not s/c	(Pd,Ni)Hx	Pd0.95Ni0.05H0.81	Pd	0.95	Ni	0.05	H	0.81																			1972																																														K					1.17																																																																																																											PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112378	1311	Tc = Tc(on). Tc(mid) <1.21	(Pd,Ni)Hx	Pd0.95Ni0.05H0.86	Pd	0.95	Ni	0.05	H	0.86																			1972																																														K		1.49					1.49																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112379	1311		(Pd,Ni)Hx	Pd0.95Ni0.05H0.9	Pd	0.95	Ni	0.05	H	0.9																			1972																																														K		2.95					2.95																																																																																																									PHYS.STAT.SOL.A,11(1972)K123	T.SKOSKIEWICZ		
112380	171	alpha-pase	Ti1-xCrx	Cr0.027Ti0.973	Cr	0.027	Ti	0.973																					1960																																														K		3.5					3.5	MTC12380																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112381	171	beta-phase	Ti1-xCrx	Cr0.152Ti0.848	Cr	0.152	Ti	0.848																					1960																																														K		4.18					4.18																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112382	171	alpha-pase	Ti1-xMnx	Mn0.025Ti0.975	Mn	0.025	Ti	0.975																					1960																																														K		2.33					2.33	MTC12382																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112383	171	beta-phase	Ti1-xMnx	Mn0.101Ti0.899	Mn	0.101	Ti	0.899																					1960																																														K		3					3																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112384	171		Ti1-xFex	Fe0.025Ti0.975	Fe	0.025	Ti	0.975																					1960																																														K		3.08					3.08	MTC12384																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112385	171		Ti1-xFex	Fe0.101Ti0.899	Fe	0.101	Ti	0.899																					1960																																														K		3.67					3.67																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112386	171		Ti1-xCox	Co0.032Ti0.968	Co	0.032	Ti	0.968																					1960																																														K		2.84					2.84	MTC12386																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112387	171		Ti1-xCox	Co0.15Ti0.85	Co	0.15	Ti	0.85																					1960																																														K		3.8					3.8																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112388	171		(Y,Gd)Os2	Y0.96Gd0.04Ru2	Y	0.96	Gd	0.04	Ru	2																			1960																																														K		3.5					3.5	MTC12388																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112389	171		(Y,Gd)Os2	Y0.92Gd0.08Ru2	Y	0.92	Gd	0.08	Ru	2																			1960																																														K		2.2					2.2																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112390	171		(Ce,Gd)Ru2	Ce0.97Gd0.03Ru2	Ce	0.97	Gd	0.03	Ru	2																			1960																																														K		4.69					4.69	MTC12390																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112391	171		(Ce,Gd)Ru2	Ce0.93Gd0.07Ru2	Ce	0.93	Gd	0.07	Ru	2																			1960																																														K		3.38					3.38																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112392	171		(Ti,V)1-xFex	Ti0.6V0.4	Ti	0.6	V	0.4																					1960																																														K		7.5					7.5																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112393	171		(Ti,V)1-xFex	Ti0.588V0.392Fe0.02	Ti	0.588	V	0.392	Fe	0.02																			1960																																														K		6.79					6.79																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112394	171		(Ti,V)1-xFex	Ti0.576V0.384Fe0.04	Ti	0.576	V	0.384	Fe	0.04																			1960																																														K		6.08					6.08																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112395	171		(Ti,V)1-xFex	Ti0.564V0.376Fe0.06	Ti	0.564	V	0.376	Fe	0.06																			1960																																														K		5.32					5.32																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112396	171		(Ti,V)1-xRux	Ti0.588V0.392Ru0.02	Ti	0.588	V	0.392	Ru	0.02																			1960																																														K		6.58					6.58																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112397	171		(Ti,V)1-xRux	Ti0.576V0.384Ru0.04	Ti	0.576	V	0.384	Ru	0.04																			1960																																														K		5.57					5.57																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112398	171		(Ti,V)1-xRux	Ti0.564V0.376Ru0.06	Ti	0.564	V	0.376	Ru	0.06																			1960																																														K		4.72					4.72																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112399	171		La	La1	La	1																							1960																																														K		6.23					6.23																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112400	171		La1-xErx	Er0.03La0.97	Er	0.03	La	0.97																					1960																																														K		4.49					4.49	MTC12400																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112401	171		La1-xErx	Er0.08La0.92	Er	0.08	La	0.92																					1960																																														K		1.43					1.43																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112402	171		La1-xNdx	La0.98Nd0.02	La	0.98	Nd	0.02																					1960																																														K		3.94					3.94	MTC12400																																																																																																								J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112403	171		La1-xNdx	La0.96Nd0.04	La	0.96	Nd	0.04																					1960																																														K		1.69					1.69																																																																																																									J.APPL.PHYS.,31(1960)23S	B.T.MATTHIAS		
112404	1203		(Nb,Ti)Nx	Nb0.96Ti0.04N0.9	Nb	0.96	Ti	0.04	N	0.9																			1967																												NaCl			A	4.3806													NaCl, B1	K		13.8					13.8																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112405	1203		(Nb,Ti)Nx	Nb0.92Ti0.08N0.93	Nb	0.92	Ti	0.08	N	0.93																			1967																												NaCl			A	4.3792													NaCl, B1	K		15.2					15.2																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112406	1203		(Nb,Ti)Nx	Nb0.75Ti0.25N0.94	Nb	0.75	Ti	0.25	N	0.94																			1967																												NaCl			A	4.3583													NaCl, B1	K		16.1					16.1																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112407	1203		(Nb,Ti)Nx	Nb0.5Ti0.5N0.95	Nb	0.5	Ti	0.5	N	0.95																			1967																												NaCl			A	4.3347													NaCl, B1	K		15.1					15.1																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112408	1203		(Nb,Ti)Nx	Nb0.35Ti0.65N0.97	Nb	0.35	Ti	0.65	N	0.97																			1967																												NaCl			A	4.3194													NaCl, B1	K		13.2					13.2																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112409	1203		(Nb,Ti)Nx	Nb0.25Ti0.75N0.98	Nb	0.25	Ti	0.75	N	0.98																			1967																												NaCl			A	4.3													NaCl, B1	K		10.5					10.5																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112410	1203		(Nb,Ti)Nx	Nb0.1Ti0.9N0.98	Nb	0.1	Ti	0.9	N	0.98																			1967																												NaCl			A	4.2694													NaCl, B1	K		6.48					6.48																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112411	1203		TiNx	N0.99Ti1	N	0.99	Ti	1																					1967																												NaCl			A	4.2472													NaCl, B1	K		4.41					4.41																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112412	1203		(Nb,Hf)Nx	Nb0.92Hf0.08N0.93	Nb	0.92	Hf	0.08	N	0.93																			1967																												NaCl			A	4.4083													NaCl, B1	K		13.7					13.7																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112413	1203		(Nb,Hf)Nx	Nb0.85Hf0.15N0.94	Nb	0.85	Hf	0.15	N	0.94																			1967																												NaCl			A	4.4194													NaCl, B1	K		12.3					12.3																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112414	1203		(Nb,Hf)Nx	Nb0.67Hf0.33N1	Nb	0.67	Hf	0.33	N	1																			1967																												NaCl			A	4.4486													NaCl, B1	K		10.2					10.2																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112415	1203		(Nb,Hf)Nx	Nb0.5Hf0.5N0.98	Nb	0.5	Hf	0.5	N	0.98																			1967																												NaCl			A	4.475													NaCl, B1	K		7.33					7.33																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112416	1203		(Nb,Hf)Nx	Nb0.35Hf0.65N1	Nb	0.35	Hf	0.65	N	1																			1967																												NaCl			A	4.4917													NaCl, B1	K		6.05					6.05																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112417	1203		(Nb,Hf)Nx	Nb0.1Hf0.9N1	Nb	0.1	Hf	0.9	N	1																			1967																												NaCl			A	4.5125													NaCl, B1	K		5.47					5.47																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112418	1203		(Nb,V)Nx	Nb0.95V0.05N0.85	Nb	0.95	V	0.05	N	0.85																			1967																												NaCl			A	4.3736													NaCl, B1	K		7.12					7.12																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112419	1203		(Nb,V)Nx	Nb0.85V0.15N0.92	Nb	0.85	V	0.15	N	0.92																			1967																												NaCl			A	4.3569													NaCl, B1	K		3.88					3.88																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112420	1203		(Nb,V)Nx	Nb0.67V0.33N0.94	Nb	0.67	V	0.33	N	0.94																			1967																												NaCl			A	4.3278													NaCl, B1	K		1.86					1.86																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112421	1203		(Nb,V)Nx	Nb0.5V0.5N0.94	Nb	0.5	V	0.5	N	0.94																			1967																												NaCl			A	4.2861													NaCl, B1	K		1.86					1.86																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112422	1203		(Nb,V)Nx	Nb0.25V0.75N0.94	Nb	0.25	V	0.75	N	0.94																			1967																												NaCl			A	4.2236													NaCl, B1	K		2.92					2.92																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112423	1203		(Nb,V)Nx	N0.99V1	N	0.99	V	1																					1967																												NaCl			A	4.1361													NaCl, B1	K		7.91					7.91																																																																																																					Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112424	1203		(Nb,V)Nx	Nb0.85Zr0.15N1	Nb	0.85	Zr	0.15	N	1																			1967																												NaCl																	NaCl, B1	K		13.7					13.7	MTC12424																																																																																																				Superconducting Hc-Jc and Tc measurements in the Nb-Ti-N, Nb-Hf-N, and Nb-V-N ternary systems				J.APPL.PHYS.,38(1967)2268	C.M.YEN,D.E.ANDERSON,L.E.TOTH,L.G.ROSNER,Y.M.SHY		
112425	1304		Hg1-xSnx	Hg0.06Sn0.94	Hg	0.06	Sn	0.94																					1968																																														K		5.05					5.05	MTC12425																																																																																																				Superconductivity in the mercury-tin system				PHYS.STAT.SOL.,25(1968)K95	T.CLAESON		
112426	1482	Debye-T from other papers. 2*gap = 8.7 cm-1 from Far-InfraRed measurements.	In1-xPbx	In1	In	1																							1971																																														K		3.4					3.4																																																											110																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112427	1482	Debye-T from other papers. 2*gap = 9.7 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.95Pb0.05	In	0.95	Pb	0.05																					1971																																														K		3.77					3.77																																																											104.5																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112428	1482	2*gap = 12.9 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.9Pb0.1	In	0.9	Pb	0.1																					1971																																														K		4.51					4.51																																																																																																					Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112429	1482	2*gap = 14.8 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.85Pb0.15	In	0.85	Pb	0.15																					1971																																														K		5.1					5.1																																																																																																					Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112430	1482	2*gap = 16.8 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.75Pb0.25	In	0.75	Pb	0.25																					1971																																														K		5.65					5.65																																																																																																					Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112431	1482	Debye-T from other papers. 2*gap = 18.8 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.6Pb0.4	In	0.6	Pb	0.4																					1971																																														K		6.2					6.2																																																											78.7																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112432	1482	Debye-T from other papers. 2*gap = 20.0 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.5Pb0.5	In	0.5	Pb	0.5																					1971																																														K		6.43					6.43																																																											82.2																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112433	1482	Debye-T from other papers. 2*gap = 21.0 cm-1 from Far-InfraRed measurements.	In1-xPbx	In0.2Pb0.8	In	0.2	Pb	0.8																					1971																																														K		6.95					6.95																																																											97.5																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112434	1482	Debye-T from other papers. 2*gap = 21.5 cm-1 from Far-InfraRed measurements.	Pb	Pb1	Pb	1																							1971																																														K		7.19					7.19																																																											104.1																																										Strong-coupling parameters in superconducting In-Pb alloys				PHYS.LETT.A,36(1971)431	G.BRANDLI,P.N.TROFIMENKOFF		
112435	1722		HfV2	Hf1V2	Hf	1	V	2																					1973																																														K		8.85					8.85			K/GPa	0.63																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112436	1722		(Hf,Ta)V2	Hf0.99Ta0.01V2	Hf	0.99	Ta	0.01	V	2																			1973																																														K		9.11					9.11			K/GPa	0.66																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112437	1722		(Hf,Ta)V2	Hf0.95Ta0.05V2	Hf	0.95	Ta	0.05	V	2																			1973																																														K		9.49					9.49			K/GPa	0.53																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112438	1722		(Hf,Ta)V2	Hf0.9Ta0.1V2	Hf	0.9	Ta	0.1	V	2																			1973																																														K		9.49					9.49			K/GPa	0.39																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112439	1722		(Hf,Ta)V2	Hf0.8Ta0.2V2	Hf	0.8	Ta	0.2	V	2																			1973																																														K		9.54					9.54			K/GPa	0.27																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112440	1722		(Hf,Ta)V2	Hf0.8Zr0.2V2	Hf	0.8	Zr	0.2	V	2																			1973																																														K		9.73					9.73			K/GPa	0.48																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112441	1722		(Hf,Ta)V2	Hf0.6Zr0.4V2	Hf	0.6	Zr	0.4	V	2																			1973																																														K		9.97					9.97			K/GPa	0.3																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112442	1722		(Hf,Ta)V2	Hf0.4Zr0.6V2	Hf	0.4	Zr	0.6	V	2																			1973																																														K		8.98					8.98			K/GPa	0.036																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112443	1722		(Hf,Ta)V2	Hf0.2Zr0.8V2	Hf	0.2	Zr	0.8	V	2																			1973																																														K		8.85					8.85			K/GPa	-0.018																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112444	1722		ZrV2	V2Zr1	V	2	Zr	1																					1973																																														K		7.83					7.83			K/GPa	0.024																																																																																												arc-melting, ANN(100C)					Superconductivity and structural instability of (Hf,Zr)V2 and (Hf,Ta)V2 alloys at high pressure				J.PHYS.F:METAL PHYS.,3(1973)2157	A.C.LAWSON,R.N.SHELTON,T.F.SMITH		
112445	P070064519	majority phase = 3R-Ta2S2C, minority = 1T-Ta2S2C. s/c parameters were calculated from Hc1(0) and Hc2(0). G-L parameter = 20.5	Ta2S2C	Ta2S2C2	Ta	2	S	2	C	2																			2004																															A	3.276		25.62												K		3.61					3.61											Oe		27.7							kOe		7.73							kOe/K		2.5					A		210			A		4200																																																										Successive superconducting transitions and Anderson localization effect in Ta2S2C			Department of Materials Science and Processing, Graduate School of Engineering, Osaka University, Yamada-oka, Suita, 565-0879, Japan	Phys.Rev.B, 70(2004)064519	I.S.Suzuki,J.Walter,M.Suzuki		
112446	P070052511	space-G = Cmcm. impurity phase = Ge. Exact Ge-content not known. RRR=47.6.	LuGe2	Ge2Lu1	Ge	2	Lu	1																					2004																												ZrSi2			A	3.969	15.553	3.839												K		2.6					2.6																																																																																																arc-melting + ANN(1000C,2h, in Ar)					Superconductivity in LuGe2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, Republic of China	Phys.Rev.B, 70(2004)052511	H.H.Sung,W.H.Lee,Y.R.Chung		
112447	SST0170274	space-G = Pm3m. RRR=40.	ZnCNi3	Zn1C1Ni3	Zn	1	C	1	Ni	3																			2004																												CaTiO3			A	3.66													CaTiO3, perovskite	K					2																																																										mj/mol.K2	6.77		421.3																																					solid state reaction(900C, 1000C)					Physical properties of ZnCNi3: comparison with superconducting MgCNi3			National Creative Research Initiative Centre for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Supercond.Sci.Technol., 17(2004)274	E.J.Choi,JinSoo Giim,Min-Seok Park,S.I.Lee,Soo-Hyeon Park,Y.W.Lee		
112448	SST0170274	space-G = Pm3m. RRR=2.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2004																												CaTiO3			A	3.81													CaTiO3, perovskite	K		6.7					6.7																																																								mj/mol.K2	29.5		255.9																																					solid state reaction(900C, 1000C)					Physical properties of ZnCNi3: comparison with superconducting MgCNi3			National Creative Research Initiative Centre for Superconductivity and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Supercond.Sci.Technol., 17(2004)274	E.J.Choi,JinSoo Giim,Min-Seok Park,S.I.Lee,Soo-Hyeon Park,Y.W.Lee		
112449	APL085TKN	<111>oriented film. B-concentration, carrier density not given. Hirr(0K) = 5.12 T. Jc(H=0,T=0) = 200 A/cm2.	diamond	C1	C	1																							2004																												diamond																	diamond	K		7.4					7.4																				T		7																																																																										deposited on Si(001) substrate using MPCVD method					Superconductivity in diamond thin films well above liquid helium temperature			National Institute for Materials Science,Sengen,Tsukuba,Japan	Appl.Phys.Lett., 85(2004)No14	H.Kawarada,H.Umezawa,I.Sakaguchi,K.Kobayashi,M.Nagao,M.Tachiki,T.Hatano,Y.Takano		
112450	NAT4280542	B-doped diamond. carrier n>=2 E+21 /cm3. B-concentration from ICP and NMR shows 2.8 at % B.	diamond	B2.8C97.2	B	2.8	C	97.2																					2004																												diamond																	diamond	K		4					4			K/GPa	-0.0642																T		3.4							T/K		1.7					A		100																																																										(graphite+B4C) - high pressure synthesis(8-9 GPa,2500-2800K)					Superconductivity in diamond			Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow region, Russia	Nature, 428(2004)542	E.A.Ekimov,E.D.Bauer,J.D.Thompson,N.J.Gurro,N.N.Mel'nik,S.M.Stishov,V.A.Sidorov		
112451	PR0468671	space-G = P6/mmm. Hc2(0) calculated using WHH theory.	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																		1	1992								4.6																				PrNi2Al3			A	5.217		4.024												K		1.02					1.02																				kOe		9.1							kOe/K		13			MHC12451		A		190																																																										arc-melting + ANN(1000C,8d)					Superconducting and magnetic properties of the heavy-fermion compounds UT2Al3 (T=Ni,Pd)			Department of Physics and Institute for Pure and Applied Physical Science, University of California,San Diego,La Jolla,California	Phys.Rev.B, 46(1992)8671	M.B.Maple,M.C.de Andrade,Y.Dalichaouch		
112452	PR0468671	space-G = P6/mmm. Hc2(0) calculated using WHH + Maki theory. (spin-orbit) = 0.37	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																		1	1992								15																				PrNi2Al3			A	5.419		4.052												K		1.93					1.93																				kOe		57.5							kOe/K		43			MHC12452		A		77																																																										arc-melting + ANN(900C,8d)					Superconducting and magnetic properties of the heavy-fermion compounds UT2Al3 (T=Ni,Pd)			Department of Physics and Institute for Pure and Applied Physical Science, University of California,San Diego,La Jolla,California	Phys.Rev.B, 46(1992)8671	M.B.Maple,M.C.de Andrade,Y.Dalichaouch		
112453	L093097001	thickness = 2000A. Tc depends on the current direction. Tc(I//c) = 0.93 K.	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																		3	2004								5																							A	5.211	5.221	4.017												K		0.98					0.98																																		MHC12453																																																														coevaporation on (010)YAlO3					Evidence for Multiband Superconductivity in the Heavy Fermion Compound UNi2Al3			Institut fur Physik, Johannes Gutenberg-Universitat, Staudingerweg 7, 55128 Mainz, Germany	Phys.Rev.Lett., 93(2004)097001	A.Zakharov,H.Adrian,M.Foerster,M.Jourdan		
112454	L093126403	P-induced s/c. Pcr = 13 GPa. Tc and dTc/dP are at P = Pcr. Hc2(0) and COHERE are at P=20 GPa. cluster compound.	GaNb4Se8	Ga1Nb4Se8	Ga	1	Nb	4	Se	8																			2004																															A	10.44														K		2.9					2.9			K/GPa	0.4																T		1.7														A		130																																																															Transition from Mott Insulator to Superconductor in GaNb4Se8 and GaTa4Se8 under High Pressure			 Physikalisches Institut, Universitat zu Koln, Zulpicher Strasse 77, 50937 Koln, Germany	Phys.Rev.Lett., 93(2004)126403	B.Ni,D.I.Khomskii,D.Johrendt,K.Syassen,M.M.Abd-Elmeguid,R.Pocha,X.Wang		
112455	L093126403	P-induced s/c. Pcr = 11.5 GPa. Tc and dTc/dP are at P = Pcr. Hc2(0) and COHERE are at P=17 GPa. cluster compound.	GaTa4Se8	Ga1Ta4Se8	Ga	1	Ta	4	Se	8																			2004																															A	10.358														K		5.8					5.8			K/GPa	0.2																T		8														A		61																																																															Transition from Mott Insulator to Superconductor in GaNb4Se8 and GaTa4Se8 under High Pressure			 Physikalisches Institut, Universitat zu Koln, Zulpicher Strasse 77, 50937 Koln, Germany	Phys.Rev.Lett., 93(2004)126403	B.Ni,D.I.Khomskii,D.Johrendt,K.Syassen,M.M.Abd-Elmeguid,R.Pocha,X.Wang		
112456	1493	Hc2 defined as Tc(on).  G-L parameter = 6.11	La1-x(Lu,Tb)x	La98Lu2	La	98	Lu	2																					1973																																														K		4.643					4.643																				kOe		10																																																																										melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112457	1493	Hc2 defined as Tc(on).  G-L parameter = 5.69	La1-x(Lu,Tb)x	La98Lu1.7Tb0.3	La	98	Lu	1.7	Tb	0.3																			1973																																														K		3.959					3.959																				kOe		6.2																																																																										melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112458	1493	Hc2 defined as Tc(on).  G-L parameter = 6.12	La1-x(Lu,Tb)x	La98Lu1.4Tb0.6	La	98	Lu	1.4	Tb	0.6																			1973																																														K		3.127					3.127																				kOe		2.4																																																																										melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112459	1493	G-L parameter = 4.91	La1-x(Lu,Tb)x	La98Lu0.934Tb1.066	La	98	Lu	0.934	Tb	1.066																			1973																																														K		1.608					1.608																																																																																																melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112460	1493	G-L parameter = 4.69	La1-x(Lu,Tb)x	La98Lu0.877Tb1.123	La	98	Lu	0.877	Tb	1.123																			1973																																														K		1.602					1.602																																																																																																melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112461	1493	G-L parameter = 4.62	La1-x(Lu,Tb)x	La98Lu0.815Tb1.185	La	98	Lu	0.815	Tb	1.185																			1973																																														K		1.248					1.248																																																																																																melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112462	1493	G-L parameter = 4.71	La1-x(Lu,Tb)x	La98Lu0.754Tb1.246	La	98	Lu	0.754	Tb	1.246																			1973																																														K		0.907					0.907																																																																																																melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112463	1493	G-L parameter = 4.46	La1-x(Lu,Tb)x	La98Lu0.697Tb1.303	La	98	Lu	0.697	Tb	1.303																			1973																																														K		0.632					0.632																																																																																																melt,swaging, wire, ANN					Superconductivity in the presence of short-range magnetic order				J.LOW TEMP.PHYS.,12(1973)171	B.J.BEAUDRY,D.K.FINNEMORE,H.L.WATSON,W.J.KEELER		
112464	1271	Hc2 defined as Tc(on).	La1-x(Lu,Tb)x	La98Lu1.15Tb0.85	La	98	Lu	1.15	Tb	0.85																			1970																																														K		2.582					2.582																				kOe		1.38																																																																															Coexistence of superconductivity and short-range magnetic order				PHYS.REV.B,2(1970)1287	D.K.FINNEMORE,L.J.WILLIAMS,W.R.DECKER		
112465	1271	Hc2 defined as Tc(on).	La1-x(Lu,Tb)x	La98Lu1Tb1	La	98	Lu	1	Tb	1																			1970																																														K		2.108					2.108																				kOe		0.82																																																																															Coexistence of superconductivity and short-range magnetic order				PHYS.REV.B,2(1970)1287	D.K.FINNEMORE,L.J.WILLIAMS,W.R.DECKER		
112466	1201		Sn1-xInx	In0.017Sn0.983	In	0.017	Sn	0.983																					1965																																														K		3.625					3.625																													G/K		150																																																																	melt, quench, ANN					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
112467	1201		Sn1-xInx	In0.046Sn0.954	In	0.046	Sn	0.954																					1965																																														K		3.655					3.655																													G/K		193																																																																	melt, quench, ANN					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
112468	1201		Sn1-xInx	In0.075Sn0.925	In	0.075	Sn	0.925																					1965																																														K		3.766					3.766																													G/K		265																																																																	melt, quench, ANN					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
112469	1201		Sn1-xAlx	Al0.152Sn0.848	Al	0.152	Sn	0.848																					1965																																														K		3.677					3.677																													G/K		152																																																																	melt, quench, ANN					Nonideal behaviour of inhomogeneous superconducting alloys				J.APPL.PHYS.,36(1965)3895	W.C.H.JOINER		
112470	SSC0140443	A15 + hexagonal phase	Mo1-x(Pt,Re)x	Mo0.75Pt0.15Re0.1	Mo	0.75	Pt	0.15	Re	0.1																			1974																												Cr3Si(A15)			A	4.986													Cr3Si, A15	K		5.3					5.3																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112471	SSC0140443	A15 + A2 phase	Mo1-x(Pt,Re)x	Mo0.7Pt0.075Re0.225	Mo	0.7	Pt	0.075	Re	0.225																			1974																												Cr3Si(A15)			A	4.98													Cr3Si, A15	K		7.4					7.4																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112472	SSC0140443	A15 + hexagonal phase	Mo1-x(Pt,Re)x	Mo0.65Pt0.1Re0.25	Mo	0.65	Pt	0.1	Re	0.25																			1974																												Cr3Si(A15)			A	4.978													Cr3Si, A15	K		7.4					7.4																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112473	SSC0140443	A15 + A2 phase	Mo1-x(Pt,Re)x	Mo0.65Pt0.05Re0.3	Mo	0.65	Pt	0.05	Re	0.3																			1974																												Cr3Si(A15)			A	4.977													Cr3Si, A15	K		8.9					8.9																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112474	SSC0140443	A15 + hexagonal phase	Mo1-x(Pt,Re)x	Mo0.6Pt0.1Re0.3	Mo	0.6	Pt	0.1	Re	0.3																			1974																												Cr3Si(A15)			A	4.975													Cr3Si, A15	K		8.5					8.5																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112475	SSC0140443	single phase	Mo1-x(Pt,Re)x	Mo0.6Pt0.05Re0.35	Mo	0.6	Pt	0.05	Re	0.35																		1	1974																												Cr3Si(A15)			A	4.974													Cr3Si, A15	K		9.8					9.8																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112476	SSC0140443	A15 + hexagonal, sigma phase	Mo1-x(Pt,Re)x	Mo0.35Pt0.075Re0.375	Mo	0.35	Pt	0.075	Re	0.375																			1974																												Cr3Si(A15)			A	4.973													Cr3Si, A15	K		10.6					10.6																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112477	SSC0140443	A15 + sigma phase	Mo1-x(Pt,Re)x	Mo0.55Pt0.05Re0.4	Mo	0.55	Pt	0.05	Re	0.4																			1974																												Cr3Si(A15)			A	4.973													Cr3Si, A15	K		10.2					10.2																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112478	SSC0140443	A15 + alpha phase	Mo1-x(Pt,Re)x	Mo0.55Pt0.05Re0.425	Mo	0.55	Pt	0.05	Re	0.425																			1974																												Cr3Si(A15)																	Cr3Si, A15	K		11.25					11.25																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112479	SSC0140443		Mo1-x(Pt,Re)x	Mo0.5Pt0.05Re0.45	Mo	0.5	Pt	0.05	Re	0.45																		1	1974																																													sigma-phase	K		5.32					5.32																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112480	SSC0140443		Mo1-x(Pt,Re)x	Mo0.5Re0.5	Mo	0.5	Re	0.5																				1	1974																																													sigma-phase	K		6.5					6.5																																																																																																ANN(1600C,48h)					Electronically 'ATYPICAL' A15-type compounds based on chromium and molybdenum				Solid State Commun., 14(1974)443	A.Paoli,J.Muller,R.Flukiger		
112481	1118		Ir1-xRhx	Ir0.7Os0.3	Ir	0.7	Os	0.3																					1971																																														K		0.0167					0.0167	MTC12481																																																																																															arc-melting					Toward the superconductivity of rhodium				PHYS.LETT.A,34(1971)160	A.C.LAWSON,A.C.MOTA,J.H.BISHOP,P.M.BREWSTER,R.W.FITZGERRALD,W.S.BLACK		
112482	1118		Os1-xRhx	Os0.32Rh0.68	Os	0.32	Rh	0.68																					1971																																														K		0.0376					0.0376	MTC12482																																																																																																				Toward the superconductivity of rhodium				PHYS.LETT.A,34(1971)160	A.C.LAWSON,A.C.MOTA,J.H.BISHOP,P.M.BREWSTER,R.W.FITZGERRALD,W.S.BLACK		
112483	454		Y1-xRhx	Rh0.8Y0.2	Rh	0.8	Y	0.2																					1964																																														K		1.18					1.18	MTC12483																																																																																																				Superconductivity in the Y-Rh and Y-Ir systems				REV.MOD.PHYS.,36(1964)155	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
112484	454		Y1-xIrx	Ir0.8Y0.2	Ir	0.8	Y	0.2																					1964																																														K		3.66					3.66	MTC12484																																																																																																				Superconductivity in the Y-Rh and Y-Ir systems				REV.MOD.PHYS.,36(1964)155	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
112485	1050		Sn1-x(InSb)x	Sn99.2In0.4Sb0.4	Sn	99.2	In	0.4	Sb	0.4																			1963																																														K		3.669					3.669	MTC12485																																																																																																				Superconductivity of the first and second kind in tin alloys				CRYOGENICS,3(1963)225	S.L.WIPS		
112486	1050		Sn1-x(InSb)x	Sn93In3.5Sb3.5	Sn	93	In	3.5	Sb	3.5																			1963																																														K		3.743					3.743																																																																																																					Superconductivity of the first and second kind in tin alloys				CRYOGENICS,3(1963)225	S.L.WIPS		
112487	1050		Sn1-xInx	In3Sn97	In	3	Sn	97																					1963																																														K		3.628					3.628	MTC12487																																																																																																				Superconductivity of the first and second kind in tin alloys				CRYOGENICS,3(1963)225	S.L.WIPS		
112488	1050		Sn1-xInx	In6Sn94	In	6	Sn	94																					1963																																														K		3.644					3.644																																																																																																					Superconductivity of the first and second kind in tin alloys				CRYOGENICS,3(1963)225	S.L.WIPS		
112489	768		Th1-xTmx	Th1	Th	1																							1968																																														K		1.37					1.37																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112490	768		Th1-xTmx	Th90.9Tm9.1	Th	90.9	Tm	9.1																					1968																																														K		1.07					1.07																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112491	768		Th1-xTmx	Th81.3Tm18.7	Th	81.3	Tm	18.7																					1968																																														K		0.97					0.97																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112492	768		Th1-xTmx	Th70.2Tm29.8	Th	70.2	Tm	29.8																					1968																																														K		0.67					0.67																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112493	768		Th1-xPrx	Pr0.102Th0.898	Pr	0.102	Th	0.898																					1968																																														K		0.95					0.95																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112494	768		Th1-xPrx	Pr0.179Th0.821	Pr	0.179	Th	0.821																					1968																																														K		0.75					0.75																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112495	768		Th1-xPrx	Pr0.251Th0.749	Pr	0.251	Th	0.749																					1968																																														K		0.53					0.53																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112496	768		Th1-xPrx	Pr0.342Th0.658	Pr	0.342	Th	0.658																					1968																																														K		0.32					0.32																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112497	768		LaTl3	La1Tl3	La	1	Tl	3																					1968																																														K		1.5					1.5																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112498	768		La1-xPrxTl3	La0.967Pr0.033Tl3	La	0.967	Pr	0.033	Tl	3																			1968																																														K		1.16					1.16																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112499	768		La1-xPrxTl3	La0.93Pr0.07Tl3	La	0.93	Pr	0.07	Tl	3																			1968																																														K		0.8					0.8																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112500	768		La1-xPrxTl3	La0.901Pr0.099Tl3	La	0.901	Pr	0.099	Tl	3																			1968																																														K		0.55					0.55																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112501	768		LaSn3	La1Sn3	La	1	Sn	3																					1968																																														K		6.55					6.55																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112502	768		La1-xTmxSn3	La0.962Tm0.038Sn3	La	0.962	Tm	0.038	Sn	3																			1968																																														K		5.49					5.49																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112503	768		La1-xTmxSn3	La0.908Tm0.092Sn3	La	0.908	Tm	0.092	Sn	3																			1968																																														K		4.18					4.18																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112504	768	not s/c	La1-xPrxSn3	La0.978Pr0.022Sn3	La	0.978	Pr	0.022	Sn	3																			1968																																														K					0.28																																																																																																							Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112505	768		LaPb3	La1Pb3	La	1	Pb	3																					1968																																														K		4.09					4.09																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112506	768		La1-xPrxPb3	La0.95Pr0.05Pb3	La	0.95	Pr	0.05	Pb	3																			1968																																														K		3.3					3.3																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112507	768		La1-xPrxPb3	La0.9Pr0.1Pb3	La	0.9	Pr	0.1	Pb	3																			1968																																														K		2.58					2.58																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112508	768		La1-xPrxPb3	La0.85Pr0.15Pb3	La	0.85	Pr	0.15	Pb	3																			1968																																														K		1.88					1.88																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112509	768		La1-xPrxPb3	La0.8Pr0.2Pb3	La	0.8	Pr	0.2	Pb	3																			1968																																														K		1.34					1.34																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112510	768		La1-xPrxPb3	La0.75Pr0.25Pb3	La	0.75	Pr	0.25	Pb	3																			1968																																														K		0.8					0.8																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112511	768		La1-xPrxPb3	La0.7Pr0.3Pb3	La	0.7	Pr	0.3	Pb	3																			1968																																														K		0.37					0.37																																																																																																					Superconductors with magnetic impurities in a singlet ground state				HELV.PHYS.ACTA,41(1968)723	E.BUCHER,G.W.HULL JR.,J.P.MAITA,K.ANDERSON		
112512	PR1650522	6N-pure Al wire. H0 = 104.93 G.	Al	Al1	Al	1																							1968																																													fcc	K		1.1793					1.1793																																																								mj/mol.K2	1.349																																							ANN(633C, 20h, in CO2)					Critical field of superconducting aluminum as a function of pressure and temperature above 0.3 K				Phys.Rev., 165(1968)522	D. E. Mapother,E. P. Harris		
112513	1156	ANN sample.	Tl1-xInx	In0.1Tl0.9	In	0.1	Tl	0.9																					1967																																													hcp	K		2.97					2.97																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112514	1156	ANN sample.	Tl1-xInx	In0.17Tl0.83	In	0.17	Tl	0.83																					1967																																													hcp	K		3.45					3.45																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112515	1156	ANN sample.	Tl1-xInx	In0.25Tl0.75	In	0.25	Tl	0.75																					1967																																													hcp	K		3.64					3.64																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112516	1156	ANN sample.	Tl1-xInx	In0.4Tl0.6	In	0.4	Tl	0.6																					1967																																													fcc	K		2.52					2.52																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112517	1156	ANN sample.	Tl1-xInx	In0.45Tl0.55	In	0.45	Tl	0.55																					1967																																													fcc	K		2.48					2.48																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112518	1156	ANN sample.	Tl1-xInx	Tl1	Tl	1																							1967																																														K		2.39					2.39																																																																																																induction melting in Al crucible					Superconducting transitions in body-centered cubic thallium-indium alloys				PHYS.REV.,154(1967)436	H.L.LUO,R.H.WILLENS		
112519	1255	d=11000A film. 5-10 % dhcp phase. RRR=3.63. gap(0)=1.526 meV. gap by tunneling.	La	La1	La	1																							1967																																													fcc	K		4.94					4.94																																																3.58	1																																															evaporation on slide glass					Electron tunneling measurements on lanthanum and lanthanum-lutetium alloy films				PHYS.REV.,164(1967)510	A.S.EDELSTEIN		
112520	1255	d=2200A film.  RRR=1.78. gap(0)=0.980 meV. gap by tunneling.	La1-xLux	La0.91Lu0.09	La	0.91	Lu	0.09																					1967																																													dhcp	K		3.28					3.28																																																3.43	1																																															evaporation on slide glass					Electron tunneling measurements on lanthanum and lanthanum-lutetium alloy films				PHYS.REV.,164(1967)510	A.S.EDELSTEIN		
112521	1255	d=1600A film. RRR=1.33. gap(0)=1.290 meV. gap by tunneling.	La1-xLux	La0.951Lu0.049	La	0.951	Lu	0.049																					1967																																													dhcp	K		4.37					4.37																																																3.43	1																																															evaporation on slide glass					Electron tunneling measurements on lanthanum and lanthanum-lutetium alloy films				PHYS.REV.,164(1967)510	A.S.EDELSTEIN		
112522	963		Ir	Ir1	Ir	1																							1968																																														K		0.11					0.11																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112523	963		Ir1-xRex	Ir0.96Re0.04	Ir	0.96	Re	0.04																					1968																																														K		0.142					0.142																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112524	963		Ir1-xRex	Ir0.93Re0.07	Ir	0.93	Re	0.07																					1968																																														K		0.22					0.22																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112525	963		Ir1-xRex	Ir0.9Re0.1	Ir	0.9	Re	0.1																					1968																																														K		0.34					0.34																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112526	963		Ir1-xRex	Ir0.8Re0.2	Ir	0.8	Re	0.2																					1968																																														K		0.66					0.66																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112527	963		Ir1-xRex	Ir0.7Re0.3	Ir	0.7	Re	0.3																					1968																																														K		1.7					1.7																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112528	963		Ir1-xRex	Ir0.95Re0.02	Ir	0.95	Re	0.02																					1968																																														K		0.112					0.112																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112529	963		Ir1-xRex	Ir0.55Re0.15	Ir	0.55	Re	0.15																					1968																																														K		0.61					0.61																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112530	963		Ir1-xOsx	Ir0.7Os0.3	Ir	0.7	Os	0.3																					1968																																														K		0.48					0.48																																																								mj/mol.K2	6.82		410																																					arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112531	963		Ir1-xOsx	Ir0.6Os0.4	Ir	0.6	Os	0.4																					1968																																														K		0.73					0.73																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112532	963		Ir1-xMox	Ir0.987Mo0.013	Ir	0.987	Mo	0.013																					1968																																														K		0.107					0.107																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112533	963		Ir1-xMox	Ir0.973Mo0.027	Ir	0.973	Mo	0.027																					1968																																														K		0.133					0.133																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112534	963		Ir1-xMox	Ir0.953Mo0.047	Ir	0.953	Mo	0.047																					1968																																														K		0.168					0.168																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112535	963		Ir1-xMox	Ir0.9Mo0.1	Ir	0.9	Mo	0.1																					1968																																														K		0.29					0.29																																																								mj/mol.K2	5		470																																					arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112536	963		Ir1-xMox	Ir0.82Mo0.18	Ir	0.82	Mo	0.18																					1968																																														K		0.5					0.5																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112537	963		Ir1-xWx	Ir0.987W0.013	Ir	0.987	W	0.013																					1968																																														K		0.107					0.107																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112538	963		Ir1-xWx	Ir0.973W0.027	Ir	0.973	W	0.027																					1968																																														K		0.125					0.125																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112539	963		Ir1-xWx	Ir0.953W0.047	Ir	0.953	W	0.047																					1968																																														K		0.162					0.162																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112540	963		Ir1-xWx	Ir0.9W0.1	Ir	0.9	W	0.1																					1968																																														K		0.23					0.23																																																								mj/mol.K2	6.1		417																																					arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112541	963		Ir1-xWx	Ir0.85W0.15	Ir	0.85	W	0.15																					1968																																														K		0.41					0.41																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112542	963		Ir1-xVx	Ir0.99V0.01	Ir	0.99	V	0.01																					1968																																														K		0.11					0.11																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112543	963		Ir1-xVx	Ir0.98V0.02	Ir	0.98	V	0.02																					1968																																														K		0.115					0.115																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112544	963		Ir1-xVx	Ir0.965V0.035	Ir	0.965	V	0.035																					1968																																														K		0.147					0.147																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112545	963		Ir1-xVx	Ir0.85V0.15	Ir	0.85	V	0.15																					1968																																														K		0.26					0.26																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112546	963		Ir1-xNbx	Ir0.99Nb0.01	Ir	0.99	Nb	0.01																					1968																																														K		0.102					0.102																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112547	963		Ir1-xNbx	Ir0.98Nb0.02	Ir	0.98	Nb	0.02																					1968																																														K		0.115					0.115																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112548	963		Ir1-xNbx	Ir0.965Nb0.035	Ir	0.965	Nb	0.035																					1968																																														K		0.138					0.138																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112549	963		Ir1-xNbx	Ir0.925Nb0.075	Ir	0.925	Nb	0.075																					1968																																														K		0.172					0.172																																																								mj/mol.K2	6.5		416																																					arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112550	963		Ir1-xNbx	Ir0.9Nb0.1	Ir	0.9	Nb	0.1																					1968																																														K		0.06					0.06																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112551	963		Ir1-xTax	Ir0.99Ta0.01	Ir	0.99	Ta	0.01																					1968																																													bcc	K		0.116					0.116																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112552	963		Ir1-xTax	Ir0.97Ta0.03	Ir	0.97	Ta	0.03																					1968																																													bcc	K		0.127					0.127																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112553	963		Ir1-xTax	Ir0.94Ta0.06	Ir	0.94	Ta	0.06																					1968																																													bcc	K		0.15					0.15																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112554	963		Ir1-xTax	Ir0.925Ta0.075	Ir	0.925	Ta	0.075																					1968																																													bcc	K		0.125					0.125																																																								mj/mol.K2	6.13		408																																					arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112555	963		Ir1-xTax	Ir0.9Ta0.1	Ir	0.9	Ta	0.1																					1968																																													fcc	K		0.067					0.067																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112556	963		Ir1-xRux	Ir0.925Ru0.075	Ir	0.925	Ru	0.075																					1968																																														K		0.11					0.11																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112557	963		Ir1-xRux	Ir0.89Ru0.11	Ir	0.89	Ru	0.11																					1968																																														K		0.105					0.105																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112558	963		Ir1-xRux	Ir0.845Ru0.155	Ir	0.845	Ru	0.155																					1968																																														K		0.11					0.11																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112559	963		Ir1-xRux	Ir0.8Ru0.2	Ir	0.8	Ru	0.2																					1968																																														K		0.13					0.13																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112560	963		Ir1-xRux	Ir0.765Ru0.235	Ir	0.765	Ru	0.235																					1968																																														K		0.142					0.142																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112561	963		Ir1-xRux	Ir0.71Ru0.29	Ir	0.71	Ru	0.29																					1968																																														K		0.18					0.18																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112562	963		Ir1-xRhx	Ir0.95Rh0.05	Ir	0.95	Rh	0.05																					1968																																														K		0.075					0.075																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112563	963		Ir1-xRhx	Ir0.89Rh0.11	Ir	0.89	Rh	0.11																					1968																																														K		0.06					0.06																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112564	963		Ir1-xRhx	Ir0.815Rh0.185	Ir	0.815	Rh	0.185																					1968																																														K		0.028					0.028																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112565	963		Ir1-xRhx	Ir0.8Rh0.2	Ir	0.8	Rh	0.2																					1968																																														K		0.03					0.03																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112566	963		Ir1-xRhx	Ir0.75Rh0.25	Ir	0.75	Rh	0.25																					1968																																														K		0.026					0.026																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112567	963		Ir1-xRhx	Ir0.7Rh0.3	Ir	0.7	Rh	0.3																					1968																																														K					0.014																																																																																																		arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112568	963		Ir1-xPdx	Ir0.96Pd0.04	Ir	0.96	Pd	0.04																					1968																																														K		0.069					0.069																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112569	963		Ir1-xPdx	Ir0.95Pd0.05	Ir	0.95	Pd	0.05																					1968																																														K		0.05					0.05																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112570	963		Ir1-xPdx	Ir0.91Pd0.09	Ir	0.91	Pd	0.09																					1968																																														K		0.047					0.047																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112571	963		Ir1-xPdx	Ir0.9Pd0.1	Ir	0.9	Pd	0.1																					1968																																														K		0.032					0.032																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112572	963		Ir1-xPdx	Ir0.88Pd0.12	Ir	0.88	Pd	0.12																					1968																																														K		0.035					0.035																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112573	963		Ir1-x-yRexRhy	Ir0.72Re0.18Rh0.1	Ir	0.72	Re	0.18	Rh	0.1																			1968																																														K		0.6					0.6																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112574	963		Ir1-x-yRexRhy	Ir0.64Re0.16Rh0.2	Ir	0.64	Re	0.16	Rh	0.2																			1968																																														K		0.55					0.55																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112575	963		Ir1-x-yRexRhy	Ir0.56Re0.14Rh0.3	Ir	0.56	Re	0.14	Rh	0.3																			1968																																														K		0.25					0.25																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112576	963		Ir1-x-yRexRhy	Ir0.46Re0.115Rh0.425	Ir	0.46	Re	0.115	Rh	0.425																			1968																																														K		0.13					0.13																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112577	963		Ir1-x-yRexRhy	Ir0.4Re0.1Rh0.5	Ir	0.4	Re	0.1	Rh	0.5																			1968																																														K		0.08					0.08																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112578	963		Ir1-x-yOsxRhy	Ir0.63Os0.27Rh0.1	Ir	0.63	Os	0.27	Rh	0.1																			1968																																														K		0.4					0.4																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112579	963		Ir1-x-yOsxRhy	Ir0.56Os0.24Rh0.2	Ir	0.56	Os	0.24	Rh	0.2																			1968																																														K		0.28					0.28																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112580	963		Ir1-x-yOsxRhy	Ir0.49Os0.21Rh0.3	Ir	0.49	Os	0.21	Rh	0.3																			1968																																														K		0.27					0.27																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112581	963		Ir1-x-yOsxRhy	Ir0.406Os0.174Rh0.42	Ir	0.406	Os	0.174	Rh	0.42																			1968																																														K		0.095					0.095																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112582	963		(IrRh)1-xOsx	Ir0.07Rh0.07Os0.86	Ir	0.07	Rh	0.07	Os	0.86																			1968																																														K		0.064					0.064																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112583	963		(IrRh)1-xOsx	Ir0.0875Rh0.0875Os0.825	Ir	0.0875	Rh	0.0875	Os	0.825																			1968																																														K		0.095					0.095																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112584	963		(IrRh)1-xOsx	Ir0.1Rh0.1Os0.8	Ir	0.1	Rh	0.1	Os	0.8																			1968																																														K		0.14					0.14																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112585	963		(IrRh)1-xOsx	Ir0.135Rh0.135Os0.73	Ir	0.135	Rh	0.135	Os	0.73																			1968																																														K		0.22					0.22																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112586	963		(IrRh)1-xOsx	Ir0.165Rh0.165Os0.67	Ir	0.165	Rh	0.165	Os	0.67																			1968																																														K		0.35					0.35																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112587	963		Ir1-x-yOsxRhy	Ir0.125Os0.2Rh0.675	Ir	0.125	Os	0.2	Rh	0.675																			1968																																														K		0.05					0.05																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112588	963		Ir1-x-yOsxRhy	Ir0.54Os0.1Rh0.36	Ir	0.54	Os	0.1	Rh	0.36																			1968																																														K		0.038					0.038																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112589	963		Ir1-x-yOsxRhy	Ir0.1Os0.25Rh0.65	Ir	0.1	Os	0.25	Rh	0.65																			1968																																														K		0.1					0.1																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112590	963		Ir1-x-yOsxRhy	Ir0.6Os0.1Rh0.3	Ir	0.6	Os	0.1	Rh	0.3																			1968																																														K		0.55					0.55																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112591	963		Ir1-x-yOsxRhy	Ir0.1Os0.3Rh0.6	Ir	0.1	Os	0.3	Rh	0.6																			1968																																														K		0.21					0.21																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112592	963		Ir1-x-yOsxRhy	Ir0.55Os0.15Rh0.3	Ir	0.55	Os	0.15	Rh	0.3																			1968																																														K		0.095					0.095																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112593	963		Ir1-x-yOsxRhy	Ir0.765Os0.085Rh0.15	Ir	0.765	Os	0.085	Rh	0.15																			1968																																														K		0.096					0.096																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112594	963		Ir1-x-yOsxRhy	Ir0.6Os0.2Rh0.2	Ir	0.6	Os	0.2	Rh	0.2																			1968																																														K		0.22					0.22																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112595	963		Ir1-x-yOsxRhy	Ir0.725Os0.175Rh0.1	Ir	0.725	Os	0.175	Rh	0.1																			1968																																														K		0.16					0.16																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112596	963		Ir1-x-yOsxRhy	Ir0.125Os0.375Rh0.5	Ir	0.125	Os	0.375	Rh	0.5																			1968																																														K		0.46					0.46																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112597	963		Ir1-x-yOsxRhy	Ir0.4Os0.3Rh0.3	Ir	0.4	Os	0.3	Rh	0.3																			1968																																														K		0.37					0.37																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112598	963		Ir1-x-yOsxRhy	Ir0.1Os0.2Rh0.7	Ir	0.1	Os	0.2	Rh	0.7																			1968																																														K					0.014																																																																																																		arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112599	963		Ir1-x-yRuxRhy	Ir0.2Ru0.3Rh0.5	Ir	0.2	Ru	0.3	Rh	0.5																			1968																																														K		0.055					0.055																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112600	963		Ir1-x-yRuxRhy	Ir0.7Ru0.25Rh0.5	Ir	0.7	Ru	0.25	Rh	0.5																			1968																																														K		0.033					0.033																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112601	963		Ir1-x-yRuxRhy	Ir0.7Ru0.1Rh0.2	Ir	0.7	Ru	0.1	Rh	0.2																			1968																																														K		0.05					0.05																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112602	963		Ir1-x-yRuxRhy	Ir0.8Ru0.05Rh0.15	Ir	0.8	Ru	0.05	Rh	0.15																			1968																																														K		0.064					0.064																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112603	963		Ir1-x-yRuxRhy	Ir0.3Ru0.2Rh0.5	Ir	0.3	Ru	0.2	Rh	0.5																			1968																																														K		0.02					0.02																																																																																																arc-melting					Superconductivity, susceptibility, and specific heat in the noble transition elements and alloys. I. Experimental results				PHYS.REV.,165(1968)533 545	K.ANDRES,M.A.JENSEN		
112604	1625	hardness =  965 kg/mm2. e-ph = 0.495	Nb1-xIrx	Ir0.34Nb0.66	Ir	0.34	Nb	0.66																				1	1971																															A	9.892		5.072											sigma-phase	K		2.25					2.25																																																								mj/mol.K2	3.037		388																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112605	1625	hardness = 1010  kg/mm2. e-ph = 0.495	Nb1-xIrx	Ir0.37Nb0.63	Ir	0.37	Nb	0.63																				1	1971																															A	9.869		5.062											sigma-phase	K		2.23					2.23																																																								mj/mol.K2	3.043		384																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112606	1625	hardness = 975  kg/mm2. e-ph = 0.497	Nb1-xIrx	Ir0.4Nb0.6	Ir	0.4	Nb	0.6																				1	1971																															A	9.842		5.045											sigma-phase	K		2.2					2.2																																																								mj/mol.K2	2.985		371																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112607	1625	hardness = 1500  kg/mm2. e-ph = 0.639	Mo1-xRex	Mo0.45Re0.55	Mo	0.45	Re	0.55																				1	1971																															A	9.602		4.984											sigma-phase	K		6.47					6.47																																																								mj/mol.K2	3.434		388																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112608	1625	hardness = 1500  kg/mm2. e-ph = 0.657	Mo1-xRex	Mo0.4Re0.6	Mo	0.4	Re	0.6																				1	1971																															A	9.595		4.984											sigma-phase	K		6.49					6.49																																																								mj/mol.K2	3.2		355																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112609	1625	hardness =  1505 kg/mm2. e-ph = 0.614	Mo1-xRex	Mo0.35Re0.65	Mo	0.35	Re	0.65																				1	1971																															A	9.588		4.983											sigma-phase	K		5.6					5.6																																																								mj/mol.K2	3.116		386																																					arc-melting									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112610	1625		Nb1-xIrx	Ir0.375Nb0.625	Ir	0.375	Nb	0.625																					1971																																													sigma-phase	K		7.9					7.9																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112611	1625		Nb1-xIrx	Ir0.385Nb0.615	Ir	0.385	Nb	0.615																					1971																																													sigma-phase	K		9.7					9.7																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112612	1625		Nb1-xIrx	Ir0.41Nb0.59	Ir	0.41	Nb	0.59																					1971																																													sigma-phase	K		9.8					9.8																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112613	1625		Mo1-xRex	Mo0.45Re0.55	Mo	0.45	Re	0.55																					1971																																													sigma-phase	K		5.9					5.9																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112614	1625		Mo1-xRex	Mo0.42Re0.58	Mo	0.42	Re	0.58																					1971																																													sigma-phase	K		6.35					6.35																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112615	1625		Mo1-xRex	Mo0.38Re0.62	Mo	0.38	Re	0.62																					1971																																													sigma-phase	K		5.7					5.7																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112616	1625		Mo1-xRex	Mo0.33Re0.67	Mo	0.33	Re	0.67																					1971																																													sigma-phase	K		5.8					5.8																																																																																																									PHYS.REV.B,3(1971)742	C.C.KOCH,J.O.SCARBROUGH		
112617	1646		Re1-xMox	Mo0.0006Re0.9994	Mo	0.0006	Re	0.9994																					1971																																														K		1.697					1.697																																																																																																arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112618	1646	Debye-T by interpolation	Re1-xWx	Re0.994W0.006	Re	0.994	W	0.006																					1971																																														K		1.84					1.84																																																											413																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112619	1646	Debye-T by interpolation	Re1-xWx	Re0.976W0.024	Re	0.976	W	0.024																					1971																																														K		3					3																																																											402																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112620	1646		Re1-xRhx	Re0.98Rh0.02	Re	0.98	Rh	0.02																					1971																																														K		2.014					2.014																																																																																																arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112621	1646		Re1-xRux	Re0.9865Ru0.0135	Re	0.9865	Ru	0.0135																					1971																																														K		1.937					1.937	MTC12621																																																																																															arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112622	1646		Re1-xIrx	Ir0.02Re0.98	Ir	0.02	Re	0.98																					1971																																														K		1.968					1.968																																																																																																arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112623	1646		Re1-xOsx	Os0.02Re0.98	Os	0.02	Re	0.98																					1971																																														K		1.807					1.807	MTC12623																																																																																															arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112624	1646		Re1-xOsx	Re1	Re	1																							1971																																													hcp	K		1.695					1.695																																																								mj/mol.K2	2.31		417																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112625	1646		Re1-xOsx	Os0.058Re0.942	Os	0.058	Re	0.942																					1971																																													hcp	K		1.93					1.93																																																								mj/mol.K2	2.28		412																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112626	1646	Debye-T by interpolation	Re1-xOsx	Os0.115Re0.885	Os	0.115	Re	0.885																					1971																																													hcp	K		1.79					1.79																																																											398																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112627	1646	Debye-T by interpolation	Re1-xOsx	Os0.232Re0.768	Os	0.232	Re	0.768																					1971																																													hcp	K		1.67					1.67																																																											365																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112628	1646		Re1-xOsx	Os0.3Re0.7	Os	0.3	Re	0.7																					1971																																													hcp	K		1.54					1.54																																																								mj/mol.K2	2.05		351																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112629	1646	Debye-T by interpolation	Re1-xOsx	Os0.362Re0.638	Os	0.362	Re	0.638																					1971																																													hcp	K		1.35					1.35																																																											346																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112630	1646	Debye-T by interpolation	Re1-xOsx	Os0.432Re0.568	Os	0.432	Re	0.568																					1971																																													hcp	K		1.18					1.18																																																											344																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112631	1646	Debye-T by interpolation	Re1-xOsx	Os0.56Re0.44	Os	0.56	Re	0.44																					1971																																													hcp	K		0.94					0.94																																																											355																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112632	1646		Re1-xOsx	Os0.7Re0.3	Os	0.7	Re	0.3																					1971																																													hcp	K		0.8					0.8																																																								mj/mol.K2	1.86		380																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112633	1646	Debye-T by interpolation	Re1-xOsx	Os0.81Re0.19	Os	0.81	Re	0.19																					1971																																													hcp	K		0.73					0.73																																																											413																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112634	1646	Debye-T by interpolation	Re1-xOsx	Os0.89Re0.11	Os	0.89	Re	0.11																					1971																																													hcp	K		0.7					0.7																																																											443																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112635	1646		Re1-xOsx	Os1	Os	1																							1971																																													hcp	K		0.62					0.62																																																								mj/mol.K2	2.35		500																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112636	1646		Ru1-xOsx	Ru1	Ru	1																							1971																																													hcp	K		0.478					0.478																																																								mj/mol.K2	3.35		505																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112637	1646		Ru1-xOsx	Os0.333Ru0.667	Os	0.333	Ru	0.667																					1971																																													hcp	K		0.47					0.47																																																								mj/mol.K2	2.74		480																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112638	1646		Ru1-xOsx	Os0.666Ru0.334	Os	0.666	Ru	0.334																					1971																																													hcp	K		0.569					0.569	MTC12638																																																							mj/mol.K2	2.5		448																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112639	1646		Ru1-xOsx	Os0.9Ru0.1	Os	0.9	Ru	0.1																					1971																																													hcp	K		0.584					0.584																																																								mj/mol.K2	2.2		432																																					arc-melting									PHYS.REV.B,3(1971)3757	C.W.CHU,H.L.LUO,W.L.MACMILLAN		
112640	1154	(delta-C/T) at Tc  = 42  mJ/mol.K2	La3Tl	La3Tl1	La	3	Tl	1																					1972																															A	5.06													fcc	K		8.95					8.95																																																																																																arc-melting									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112641	1154	(delta-C/T) at Tc  = 42  mJ/mol.K2	(La,Pr)3Tl	La2.916Pr0.084Tl1	La	2.916	Pr	0.084	Tl	1																			1972																																													fcc	K		7.7					7.7																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112642	1154		(La,Pr)3Tl	La2.91Pr0.09Tl1	La	2.91	Pr	0.09	Tl	1																			1972																																													fcc	K		7.55					7.55																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112643	1154	(delta-C/T) at Tc  = 41.7  mJ/mol.K2	(La,Pr)3Tl	La2.92Pr0.18Tl1	La	2.92	Pr	0.18	Tl	1																			1972																																													fcc	K		6.51					6.51	MTC12643																																																																																															two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112644	1154	(delta-C/T) at Tc  = 37.2  mJ/mol.K2	(La,Pr)3Tl	La2.706Pr0.294Tl1	La	2.706	Pr	0.294	Tl	1																			1972																																													fcc	K		5.25					5.25																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112645	1154	(delta-C/T) at Tc  = 31.1  mJ/mol.K2	(La,Pr)3Tl	La2.574Pr0.426Tl1	La	2.574	Pr	0.426	Tl	1																			1972																																													fcc	K		3.92					3.92																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112646	1154	(delta-C/T) at Tc  = 28.0  mJ/mol.K2	(La,Pr)3Tl	La2.55Pr0.45Tl1	La	2.55	Pr	0.45	Tl	1																			1972																																													fcc	K		3.68					3.68																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112647	1154	(delta-C/T) at Tc  = 22.4  mJ/mol.K2	(La,Pr)3Tl	La2.406Pr0.594Tl1	La	2.406	Pr	0.594	Tl	1																			1972																																													fcc	K		2.4					2.4																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112648	1154		(La,Pr)3Tl	La2.25Pr0.75Tl1	La	2.25	Pr	0.75	Tl	1																			1972																																													fcc	K		1.24					1.24																																																																																																two-step-arc-melting (La1-xPrx + Tl)									PHYS.REV.B,6(1972)2709	A.S.COOPER,E.BUCHER,J.P.MAITA		
112649	1965		(La,Pr)Se	La0.95Pr0.05Se1	La	0.95	Pr	0.05	Se	1																			1975																																														K		0.7					0.7																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112650	1965		(La,Pr)Se	La0.9Pr0.1Se1	La	0.9	Pr	0.1	Se	1																			1975																																														K		0.48					0.48																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112651	1965		(La,Pr)Se	La0.8Pr0.2Se1	La	0.8	Pr	0.2	Se	1																			1975																																														K		0.03					0.03																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112652	1965		(La,Pr)3Se4	La2.85Pr0.15Se4	La	2.85	Pr	0.15	Se	4																			1975																																														K		4.81					4.81																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112653	1965		(La,Pr)3Se4	La2.7Pr0.3Se4	La	2.7	Pr	0.3	Se	4																			1975																																														K		3.36					3.36																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112654	1965		(La,Pr)3Se4	La2.4Pr0.6Se4	La	2.4	Pr	0.6	Se	4																			1975																																														K		1.49					1.49																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112655	1965		(La,Pr)3Se4	La2.25Pr0.75Se4	La	2.25	Pr	0.75	Se	4																			1975																																														K		0.76					0.76																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112656	1965		(La,Pr)3S4	La2.82Pr0.18S4	La	2.82	Pr	0.18	S	4																			1975																																														K		4.33					4.33																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112657	1965		(La,Pr)3S4	La2.58Pr0.42S4	La	2.58	Pr	0.42	S	4																			1975																																														K		2.69					2.69																																																																																																					Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
112658	JPS0732065	Hirr determined from torque measurement(Hirr<Hc2). COHERE from Hirr. Hirr//c = 2.9 T(COHERE//c = 18.3 A). Anisotropy=5.62.	MgB2	B2Mg1	B	2	Mg	1																				3	2004																												AlB2																	AlB2, C32	K		39					39																				T		16.4												MHC12658		A		104																																																										high-pressure synthesis					Enhancement of Irreversibility Field in Carbon-substituted MgB2 Single Crystals			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 73(2004)2065	E.Ohmichi,S.Lee,S.Tajima,T.Masui,T.Osada		
112659	JPS0732065	Hirr determined from torque measurement(Hirr<Hc2). COHERE from Hirr. Hirr//c = 5.5 T(COHERE//c = 14.5 A). Anisotropy=4.87.	Mg(B,C)2	Mg1B1.96C0.04	Mg	1	B	1.96	C	0.04																		3	2004																												AlB2																	AlB2, C32	K		35					35																				T		26.8												MHC12659		A		74																																																										high-pressure synthesis					Enhancement of Irreversibility Field in Carbon-substituted MgB2 Single Crystals			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 73(2004)2065	E.Ohmichi,S.Lee,S.Tajima,T.Masui,T.Osada		
112660	JPS0732065	Hirr determined from torque measurement(Hirr<Hc2). COHERE from Hirr. Hirr//c = 8.1 T(COHERE//c = 15.3 A). Anisotropy=4.11.	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		3	2004																												AlB2																	AlB2, C32	K		27					27																				T		33.4												MHC12660		A		62																																																										high-pressure synthesis					Enhancement of Irreversibility Field in Carbon-substituted MgB2 Single Crystals			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 73(2004)2065	E.Ohmichi,S.Lee,S.Tajima,T.Masui,T.Osada		
112661	JPS0732065	Hirr determined from torque measurement(Hirr<Hc2). COHERE from Hirr. Hirr//c = 9.0 T(COHERE//c = 26 A). Anisotropy=2.24.	Mg(B,C)2	Mg1B1.85C0.15	Mg	1	B	1.85	C	0.15																		3	2004																												AlB2																	AlB2, C32	K		20					20																				T		20												MHC12661		A		58																																																										high-pressure synthesis					Enhancement of Irreversibility Field in Carbon-substituted MgB2 Single Crystals			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba ,Japan	J.Phys.Soc.Jpn, 73(2004)2065	E.Ohmichi,S.Lee,S.Tajima,T.Masui,T.Osada		
112662	JPS0732370	P-induced SC. Pcr = 12 GPa. M-I transition at 62 K.(P=0). diamond anvil with NaCl medium.	PrRu4P12	Pr1Ru4P12	Pr	1	Ru	4	P	12																		3	2004																												skutterudite			A	8.0497														K		1.8			0		1.8																				T		2																																																																										Sn-flux method					Pressure-Induced Superconductivity in Filled Skutterudite PrRu4P12			Department of Materials Science and Engineering, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 73(2004)2370	A.Miyake,C.Sekine,I.Shirotani,K.Kihou,K.Shimizu		
112663	P070134514		(Mg,Sc)B2	Mg0.98Sc0.02B2	Mg	0.98	Sc	0.02	B	2																			2004																												AlB2																	AlB2, C32	K		39					39																																																																																																heat(1280-950C) in Ta-crucible					Substitution of Sc for Mg in MgB2: Effects on transition temperature and Kohn anomaly			Dipartimento di Fisica, Universita di Roma,  Roma, Italy	Phys.Rev.B, 70(2004)134514	A.Bianconi,A.Latini,A.Saccone,C.Metallo,C.Sanipoli,E.Liarokapis,G.Campi,L.Simonelli,M.Filippi,M.Giovannini,S.Agrestini,S.De.Negri		
112664	P070134514		(Mg,Sc)B2	Mg0.88Sc0.12B2	Mg	0.88	Sc	0.12	B	2																			2004																												AlB2			A	3.094		3.529											AlB2, C32	K		30					30	MTC12664																																																																																															heat(1280-950C) in Ta-crucible					Substitution of Sc for Mg in MgB2: Effects on transition temperature and Kohn anomaly			Dipartimento di Fisica, Universita di Roma,  Roma, Italy	Phys.Rev.B, 70(2004)134514	A.Bianconi,A.Latini,A.Saccone,C.Metallo,C.Sanipoli,E.Liarokapis,G.Campi,L.Simonelli,M.Filippi,M.Giovannini,S.Agrestini,S.De.Negri		
112665	P070134514		(Mg,Sc)B2	Mg0.73Sc0.27B2	Mg	0.73	Sc	0.27	B	2																			2004																												AlB2			A	3.103		3.527											AlB2, C32	K		6					6																																																																																																heat(1280-950C) in Ta-crucible					Substitution of Sc for Mg in MgB2: Effects on transition temperature and Kohn anomaly			Dipartimento di Fisica, Universita di Roma,  Roma, Italy	Phys.Rev.B, 70(2004)134514	A.Bianconi,A.Latini,A.Saccone,C.Metallo,C.Sanipoli,E.Liarokapis,G.Campi,L.Simonelli,M.Filippi,M.Giovannini,S.Agrestini,S.De.Negri		
112666	P070134518	Tc=30.1,25.6,23.5,18.7,12.6,7.2 K for P=3.8,6.8,8.9,13.4,17.1,20.5 GPa, respectively.	MgB2	B2Mg1	B	2	Mg	1																					2004																												AlB2																	AlB2, C32	K		37.6					37.6				-1.1																														MHC12666																																																																			Pressure dependence of the upper critical field of MgB2 and of YNi2B2C				Phys.Rev.B, 70(2004)134518	H.Suderow,J.L.Martinez,J.P.Brison,P.Lejay,S.Lee,S.Tajima,S.Vieira,V.G.Tissen		
112667	P070134518	Tc=15.2,14.9,13.2,11.3,9.87,8.0 K for P=2.3,3.3,5.4,7.6,9.0,10.6 GPa, respectively. not linear dependence.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																	2004																												LuNi2B2C																		K		15.7					15.7																																		MHC12667																																																																			Pressure dependence of the upper critical field of MgB2 and of YNi2B2C				Phys.Rev.B, 70(2004)134518	H.Suderow,J.L.Martinez,J.P.Brison,P.Lejay,S.Lee,S.Tajima,S.Vieira,V.G.Tissen		
112668	P070094511		MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																			2004																															A	3.8091														K		7.1					7.1																																																								mj/mol.K2	31.7																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112669	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.995Ru0.005	Mg	1	C	1	Ni	2.995	Ru	0.005																	2004																																														K		6.91					6.91																																																								mj/mol.K2	31																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112670	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.99Ru0.01	Mg	1	C	1	Ni	2.99	Ru	0.01																	2004																															A	3.8105														K		6.72					6.72																																																								mj/mol.K2	28.8																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112671	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.98Ru0.02	Mg	1	C	1	Ni	2.98	Ru	0.02																	2004																															A	3.8107														K		6.5					6.5																																																								mj/mol.K2	27																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112672	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.967Ru0.033	Mg	1	C	1	Ni	2.967	Ru	0.033																	2004																															A	3.8118														K		6.1					6.1																																																								mj/mol.K2	25.5																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112673	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.934Ru0.066	Mg	1	C	1	Ni	2.934	Ru	0.066																	2004																															A	3.8136														K		5.6					5.6																																																								mj/mol.K2	23.8																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112674	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.9Ru0.1	Mg	1	C	1	Ni	2.9	Ru	0.1																	2004																															A	3.8171														K		4.72					4.72																																																								mj/mol.K2	23.7																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112675	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.8Ru0.2	Mg	1	C	1	Ni	2.8	Ru	0.2																	2004																															A	3.8259														K		3.49					3.49																																																								mj/mol.K2	21.3																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112676	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.7Ru0.3	Mg	1	C	1	Ni	2.7	Ru	0.3																	2004																															A	3.8333														K		2.8					2.8																																																								mj/mol.K2	19.7																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112677	P070094511		MgC(Ni,Ru)3	Mg1C1Ni2.6Ru0.4	Mg	1	C	1	Ni	2.6	Ru	0.4																	2004																															A	3.8417														K		2.14					2.14																																																								mj/mol.K2	17.5																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112678	P070094511	not SC	MgC(Ni,Ru)3	Mg1C1Ni2.5Ru0.5	Mg	1	C	1	Ni	2.5	Ru	0.5																	2004																															A	3.8509														K					1.8																																																										mj/mol.K2	15.9																																							solid reaction(wrapped in Ta-foil)					Effect of Ru substitution for Ni on the superconductivity in MgCNi3-xRux			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 70(2004)094511	A.P.Ramirez,G.Lawes,R.J.Cava,T.Klimczuk,V.Gupta		
112679	P070104506	(1/a)(da/dP) = -2.8E-3 /GPa. (1/c)(dc/dP) = -3.6E-3 /GPa.	ZrNCl0.7	Zr1N1Cl0.7	Zr	1	N	1	Cl	0.7																			2004																																														K		12.7					12.7			K/GPa	-0.034																																																																																																	High-pressure study of layered nitride superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.B, 70(2004)104506	M.Hisakabe,S.Yamanaka,Y.Iwasa,Y.Ohishi,Y.Taguchi		
112680	P070104506	M is THF(tetrahydrofun; C4H8O). Li and THF cointercalated to HfNCl. M-content not given(nearly 3).	Li0.5(THF)HfNCl	Li0.5M3Hf1N1Cl1	Li	0.5	M	3	Hf	1	N	1	Cl	1															2004																																														K		25.2					25.2			K/GPa	-0.054																																																																																																	High-pressure study of layered nitride superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.B, 70(2004)104506	M.Hisakabe,S.Yamanaka,Y.Iwasa,Y.Ohishi,Y.Taguchi		
112681	P070094509		CeRu2	Ce1Ru2	Ce	1	Ru	2																					2004																												MgCu2(Laves)			A	7.544													MgCu2, C15	K		6.17					6.17																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112682	P070094509		(Ce,La)Ru2	Ce0.97La0.03Ru2	Ce	0.97	La	0.03	Ru	2																			2004																												MgCu2(Laves)			A	7.547													MgCu2, C15	K		6.45					6.45																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112683	P070094509		(Ce,La)Ru2	Ce0.94La0.06Ru2	Ce	0.94	La	0.06	Ru	2																			2004																												MgCu2(Laves)			A	7.551													MgCu2, C15	K		6.55					6.55																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112684	P070094509		(Ce,La)Ru2	Ce0.91La0.09Ru2	Ce	0.91	La	0.09	Ru	2																			2004																												MgCu2(Laves)			A	7.555													MgCu2, C15	K		6.57					6.57																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112685	P070094509		(Ce,La)Ru2	Ce0.88La0.12Ru2	Ce	0.88	La	0.12	Ru	2																			2004																												MgCu2(Laves)			A	7.561													MgCu2, C15	K		6.14					6.14																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112686	P070094509		(Ce,La)Ru2	Ce0.85La0.15Ru2	Ce	0.85	La	0.15	Ru	2																			2004																												MgCu2(Laves)			A	7.565													MgCu2, C15	K		5.35					5.35																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112687	P070094509		(Ce,La)Ru2	Ce0.8La0.2Ru2	Ce	0.8	La	0.2	Ru	2																			2004																												MgCu2(Laves)			A	7.573													MgCu2, C15	K		4.77					4.77																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112688	P070094509		(Ce,La)Ru2	Ce0.25La0.75Ru2	Ce	0.25	La	0.75	Ru	2																			2004																												MgCu2(Laves)			A	7.671													MgCu2, C15	K		1.42					1.42																																																																																																arc-melting					Local structure and superconductivity of the Ce1-xLaxRu2 Laves phase system				Phys.Rev.B, 70(2004)094509	A.Bianconi,A.Marcelli,A.Palenzona,D.Di.Castro,E.Amato,M.Filippi,N.L.Saini,P.Manfrinetti,S.Agrestini		
112689	JP01307391	not SC. PENET estimation. G-L parameter = 60	Yb3Co4(Sn,Co)13	Yb3Co4.3Sn12.7	Yb	3	Co	4.3	Sn	12.7																			2001																															A	9.5361														K		3.4					3.4																				T		2.5														A		115			A		6800													mj/mol.K2	46		207																																					ANN(773K,3w)-Q					Physical properties and superconductivity of skutterudite-related Yb3Co4.3Sn12.7 and Yb3Co4Ge13				J.Phys.:Condens.Matter, 13(2001)7391	A.Galatanu,A.Grytsiv,C.Dusek,C.Godart,D.Kaczorowski,E.Bauer,E.Idl,H.Michor,L.Romaka,O.Bodak,P.Rogl,Ya Mudryk		
112690	JP01307391		Yb3Co4Ge13	Yb3Co4Ge13	Yb	3	Co	4	Ge	13																			2001																															A	8.7286														K					0.3																																																																																																		ANN(1073K,10d)-Q					Physical properties and superconductivity of skutterudite-related Yb3Co4.3Sn12.7 and Yb3Co4Ge13				J.Phys.:Condens.Matter, 13(2001)7391	A.Galatanu,A.Grytsiv,C.Dusek,C.Godart,D.Kaczorowski,E.Bauer,E.Idl,H.Michor,L.Romaka,O.Bodak,P.Rogl,Ya Mudryk		
112691	PR00803479		AuGa2	Au1Ga2	Au	1	Ga	2																					1973																																														K		1.15					1.15	MTC12691																																																																																																				Pressure Dependence of Tc for (Au1-xPdx)Ga2 Alloys				Phys.Rev.B, 8(1973)3479	J.E.Schirber,R.N.Shelton,T.F.Smith		
112692	PR00803479		(Au,Pd)Ga2	Au0.988Pd0.012Ga2	Au	0.988	Pd	0.012	Ga	2																			1973																																														K		1.25					1.25	MTC12692																																																																																																				Pressure Dependence of Tc for (Au1-xPdx)Ga2 Alloys				Phys.Rev.B, 8(1973)3479	J.E.Schirber,R.N.Shelton,T.F.Smith		
112693	PR00803479		(Au,Pd)Ga2	Au0.976Pd0.024Ga2	Au	0.976	Pd	0.024	Ga	2																			1973																																														K		1.56					1.56	MTC12693																																																																																																				Pressure Dependence of Tc for (Au1-xPdx)Ga2 Alloys				Phys.Rev.B, 8(1973)3479	J.E.Schirber,R.N.Shelton,T.F.Smith		
112694	PR03300162	gamma (=14.6 mj/atom.K2) calculated from Hc(0) (=0.350 T). G-L parameter = 1.2	ThRu2	Ru2Th1	Ru	2	Th	1																					1986																												MgCu2(Laves)																	MgCu2, C15	K		3.47					3.47			K/GPa	0																T		0.8																																		mj/mol.K2	43.8																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112695	PR03300162	gamma (=2.4 mj/atom.K2) calculated from Hc(0) (=0.206 T). G-L parameter = 8.9	(Th,Nd)Ru2	Th0.8Nd0.2Ru2	Th	0.8	Nd	0.2	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		4.55					4.55	MTC12695		K/GPa	0.15																T		1.29																																		mj/mol.K2	7.2																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112696	PR03300162	gamma (=3.1 mj/atom.K2) calculated from Hc(0) (=0.081 T). G-L parameter = 2.5	(Th,Nd)Ru2	Th0.67Nd0.33Ru2	Th	0.67	Nd	0.33	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		1.51					1.51			K/GPa	0.165																T		0.16																																		mj/mol.K2	9.3																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112697	PR03300162	gamma (=4.0 mj/atom.K2) calculated from Hc(0) (=0.290 T). G-L parameter = 7	(Th,La)Ru2	Th0.9La0.1Ru2	Th	0.9	La	0.1	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		4.73					4.73																				T		3.56																																		mj/mol.K2	12																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112698	PR03300162	gamma (=3.6 mj/atom.K2) calculated from Hc(0) (=0.338 T). G-L parameter = 7	(Th,La)Ru2	Th0.9La0.2Ru2	Th	0.9	La	0.2	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		5.87					5.87	MTC12698																			T		4.12																																		mj/mol.K2	10.8																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112699	PR03300162	gamma (=3.1 mj/atom.K2) calculated from Hc(0) (=0.244 T). G-L parameter = 5.6	(Th,La)Ru2	Th0.9La0.3Ru2	Th	0.9	La	0.3	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		4.45					4.45																				T		2.44																																		mj/mol.K2	9.3																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112700	PR03300162	gamma (=9.0 mj/atom.K2) calculated from Hc(0) (=0.284 T). G-L parameter =4	(Th,La)Ru2	Th0.9La0.9Ru2	Th	0.9	La	0.9	Ru	2																			1986																												MgCu2(Laves)																	MgCu2, C15	K		3.05					3.05																				T		1.86																																		mj/mol.K2	27																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112701	PR03300162	gamma (=10.9 mj/atom.K2) calculated from Hc(0) (=0.402 T). G-L parameter = 2.8	LaRu2	La1Ru2	La	1	Ru	2																					1986																												MgCu2(Laves)																	MgCu2, C15	K		4.3					4.3																				T		2.01																																		mj/mol.K2	32.7																																												Superconducting and magnetic properties of (Th1-xNdx)Ru2 and (Th1-xLax)Ru2 intermetallic compounds				Phys.Rev.B, 33(1986)162	D.Huser,G.J.Nieuwenhuys,J.A.Mydosh,R.C.Brouwer		
112702	PHC4110059	weak ferro at Curie-T.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																	2004							2.41	6																				LuNi2B2C			A	3.5012		10.563												K		10.5					10.5																																																																																																arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112703	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.98Fe0.02B2C1	Er	1	Ni	1.98	Fe	0.02	B	2	C	1															2004																												LuNi2B2C																		K		8.8					8.8																																																																																																arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112704	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.965Fe0.035B2C1	Er	1	Ni	1.965	Fe	0.035	B	2	C	1															2004																												LuNi2B2C			A	3.5006		10.5626												K		7.31					7.31																																																																																																arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112705	PHC4110059	re-entrant SC at 5.50 K. weak ferro at Curie-T.	Er(Ni,Fe)2B2C	Er1Ni1.96Fe0.04B2C1	Er	1	Ni	1.96	Fe	0.04	B	2	C	1															2004							2.2	5.8																				LuNi2B2C			A	3.5008		10.564												K		7.21					7.21																																		MHC12705																																																														arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112706	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.93Fe0.07B2C1	Er	1	Ni	1.93	Fe	0.07	B	2	C	1															2004								5.61																				LuNi2B2C			A	3.501		10.5648												K		0					0																																																																																																arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112707	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.9Fe0.1B2C1	Er	1	Ni	1.9	Fe	0.1	B	2	C	1															2004								5.47																				LuNi2B2C			A	3.5013		10.5675												K																																																																																																							arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112708	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.8Fe0.2B2C1	Er	1	Ni	1.8	Fe	0.2	B	2	C	1															2004								4.01																				LuNi2B2C			A	3.5011		10.5704												K																																																																																																							arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112709	PHC4110059		Er(Ni,Fe)2B2C	Er1Ni1.96Fe0.04B2C0.99	Er	1	Ni	1.96	Fe	0.04	B	2	C	0.99															2004								5.9																				LuNi2B2C			A	3.501		10.5635												K		7.4					7.4	MTC12709																																																																																															arc-melting					Structural, superconducting and magnetic properties of ErNi2-xFexB2C (0=<x=<0.2) and ErNi1.96Fe0.04B2Cy (0.9=<y=<1.05)			LCMTR??CNRS, ISCSA, 2-8 rue H. Dunant, 94320 Thiais, France	Physica C, 411(2004)59	C.Godart,E.Alleno,E.Leroy,S.Vivet		
112710	JAC2620462		Ho(Ni,Fe)2B2C	Ho1Ni1.99Fe0.01B2C1	Ho	1	Ni	1.99	Fe	0.01	B	2	C	1															1997								6																				LuNi2B2C																		K		7					7																																																																																																					Superconductivity and magnetism in the Ho---Ni---B---C system			C.N.R.S., U.P.R. 209, 1 place Aristide Briand, 92195, Meudon Cedex, France	J.Alloys Compd., 262(1997)462	C.Codart,E.Alleno,E.Tominez,J.A.Hodges,P.Bonville		
112711	JP01502284	resistive transition. moment = 0.60 Bohr-M.	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2003							-36																					HoCoGa5			A	4.3012		6.8569												K		8.7					8.7																				T		2.1																																																																										arc-melting using Ti-getter					Advances in the preparation and characterization of transuranium systems				J.Phys.:Condens.Matter, 15(2003)S2279	E.Colineau,F.Wastin,G.H.Lander,J.Rebizant,P.Boulet		
112712	PHC4120258	COHERE<c> = 17 A, PENET<c> = 1039 A.	MgB2	B2Mg1	B	2	Mg	1																				3	2004																												AlB2																	AlB2, C32	K		37.6					37.6																																		MHC12712		A		109			A		366																																																					grown in stainless tube.					Anisotropy in the upper and lower critical fields of MgB2 single crystals			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 412-414(2004)258	H.Bando,N.Shirakawa,T.Yanagisawa,Y.Yamaguchi		
112713	PHC4120266	B-content = nominal value. RRR=2.1. gap(0) = 2.4 meV by break junction tunneling.	NbB2	B2.1Nb1	B	2.1	Nb	1																				1	2004																												AlB2																	AlB2, C32	K		9.1					9.1																																																4.4	1																																															heat(1873 K, 5.5 GPa)					Energy gap structure in the binary superconductor MB2 :(M = Nb and Mg)			Graduate school of Advanced Sciences of Matter, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica C, 412-414(2004)266	H.Fujii,H.Takagiwa,J.Akimitsu,T.Ekino,T.Muranaka,T.Takasaki		
112714	PR0150973	Amorphous film. P-induced SC. Tc at Pc=100 kbar.	As2Te3	As2Te3	As	2	Te	3																					1977																																														K		4.4					4.4																																																																																																depositted on mica by flash evaporation					Semiconductor-metal and superconducting transitions induced by pressure in amorphous As2Te3			University of Chicago,Illinois, USA	Phys.Rev.B, 15(1977)973	H.Fritzsche,N.Sakai		
112715	PR0150973	Amorphous film. P-induced SC. Tc at Pc=100 kbar.	As	As1	As	1																							1977																																														K		0.2			0		0.2																																																																																																depositted on mica by flash evaporation					Semiconductor-metal and superconducting transitions induced by pressure in amorphous As2Te3			University of Chicago,Illinois, USA	Phys.Rev.B, 15(1977)973	H.Fritzsche,N.Sakai		
112716	PR0150973	Amorphous film. P-induced SC. Tc at Pc=56 kbar.	Te	Te1	Te	1																							1977																																														K		3.3					3.3																																																																																																depositted on mica by flash evaporation					Semiconductor-metal and superconducting transitions induced by pressure in amorphous As2Te3			University of Chicago,Illinois, USA	Phys.Rev.B, 15(1977)973	H.Fritzsche,N.Sakai		
112717	1257		Re	Re1	Re	1																						1	1970																																														K		1.694					1.694	MTC12717		K/GPa	-0.023																																																																																												ANN(1350C,1h,in vac)					Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
112718	1257		Re	Re1	Re	1																						3	1970																																														K		1.694					1.694			K/GPa	-0.023																																																																																												ANN(1500C,1h,in vac)					Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
112719	1257		Re1-xOsx	Os2.76Re97.24	Os	2.76	Re	97.24																				1	1970																																														K		1.844					1.844																																																																																																					Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
112720	1257		Re1-xOsx	Os8.33Re91.67	Os	8.33	Re	91.67																				1	1970																																														K		1.876					1.876	MTC12720																																																																																																				Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
112721	1855	e-ph coupling const. = 0.518	Zr1-xMox	Mo3.29Zr96.71	Mo	3.29	Zr	96.71																				1	1974																																														K		2.12					2.12																																																								mj/mol.K2	3.58		292.7																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112722	1855	e-ph coupling const. = 0.547	Zr1-xMox	Mo3.95Zr96.05	Mo	3.95	Zr	96.05																				1	1974																																														K		2.53					2.53																																																								mj/mol.K2	4.01		273.3																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112723	1855	e-ph coupling const. = 0.648	Zr1-xMox	Mo5.22Zr94.78	Mo	5.22	Zr	94.78																				1	1974																																														K		4					4																																																								mj/mol.K2	5.27		230.4																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112724	1855	e-ph coupling const. = 0.695	Zr1-xMox	Mo6.86Zr93.14	Mo	6.86	Zr	93.14																				1	1974																																														K		4.74					4.74																																																								mj/mol.K2	6.17		219.2																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112725	1855	e-ph coupling const. = 0.71	Zr1-xMox	Mo8.75Zr91.25	Mo	8.75	Zr	91.25																				1	1974																																														K		5					5																																																								mj/mol.K2	6.79		217.2																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112726	1855	e-ph coupling const. = 0.71	Zr1-xMox	Mo13Zr87	Mo	13	Zr	87																				1	1974																																														K		4.91					4.91																																																								mj/mol.K2	5.84		213.6																																					arc-melting					Specific heat and superconducting properties of Zr-Mo alloys				J.PHYS.SOC.JAPAN,36(1974)1349	K.YASOHAMA,T.OGASAWARA		
112727	492		Nb3Rh	Nb3Rh1	Nb	3	Rh	1																				1	1965																												Cr3Si(A15)			A	5.1317													Cr3Si, A15	K		2.64					2.64																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112728	492		Nb3Os	Nb3Os1	Nb	3	Os	1																				1	1965																												Cr3Si(A15)			A	5.1359													Cr3Si, A15	K					1.7																																																																																																							SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112729	492		Nb3Ir	Ir1Nb3	Ir	1	Nb	3																				1	1965																												Cr3Si(A15)			A	5.1356													Cr3Si, A15	K					1.7																																																																																																							SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112730	492		Nb3Pt	Nb3Pt1	Nb	3	Pt	1																				1	1965																												Cr3Si(A15)			A	5.1547													Cr3Si, A15	K		10.9					10.9																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112731	492		Nb3Au	Au1Nb3	Au	1	Nb	3																				1	1965																												Cr3Si(A15)			A	5.2027													Cr3Si, A15	K		11.5					11.5																																																																																																					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112732	492		Nb3(Rh,Co)	Nb3Rh0.98Co0.02	Nb	3	Rh	0.98	Co	0.02																		1	1965																												Cr3Si(A15)			A	5.132													Cr3Si, A15	K		2.28					2.28																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112733	492		Nb3(Rh,Co)	Nb3Rh0.95Co0.05	Nb	3	Rh	0.95	Co	0.05																		1	1965																												Cr3Si(A15)			A	5.135													Cr3Si, A15	K		1.96					1.96																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112734	492		Nb3(Rh,Co)	Nb3Rh0.9Co0.1	Nb	3	Rh	0.9	Co	0.1																			1965																												Cr3Si(A15)			A	5.1347													Cr3Si, A15	K		1.9					1.9																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112735	492		Nb3(Rh,Ru)	Nb3Rh0.98Ru0.02	Nb	3	Rh	0.98	Ru	0.02																		1	1965																												Cr3Si(A15)			A	5.132													Cr3Si, A15	K		2.42					2.42																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112736	492		Nb3(Rh,Ru)	Nb3Rh0.95Ru0.05	Nb	3	Rh	0.95	Ru	0.05																		1	1965																												Cr3Si(A15)			A	5.135													Cr3Si, A15	K		2.42					2.42																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112737	492		Nb3(Rh,Ru)	Nb3Rh0.9Ru0.1	Nb	3	Rh	0.9	Ru	0.1																			1965																												Cr3Si(A15)			A	5.1346													Cr3Si, A15	K		2.44					2.44																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112738	492		Nb3(Rh,Pd)	Nb3Rh0.98Pd0.02	Nb	3	Rh	0.98	Pd	0.02																		1	1965																												Cr3Si(A15)			A	5.133													Cr3Si, A15	K		2.5					2.5																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112739	492		Nb3(Rh,Pd)	Nb3Rh0.95Pd0.05	Nb	3	Rh	0.95	Pd	0.05																		1	1965																												Cr3Si(A15)			A	5.134													Cr3Si, A15	K		2.49					2.49																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112740	492		Nb3(Rh,Pd)	Nb3Rh0.9Pd0.1	Nb	3	Rh	0.9	Pd	0.1																		1	1965																												Cr3Si(A15)			A	5.1345													Cr3Si, A15	K		2.55					2.55																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112741	492		Nb3(Rh,Os)	Nb3Rh0.98Os0.02	Nb	3	Rh	0.98	Os	0.02																		1	1965																												Cr3Si(A15)			A	5.134													Cr3Si, A15	K		2.42					2.42																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112742	492		Nb3(Rh,Os)	Nb3Rh0.95Os0.05	Nb	3	Rh	0.95	Os	0.05																		1	1965																												Cr3Si(A15)			A	5.132													Cr3Si, A15	K		2.39					2.39																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112743	492		Nb3(Rh,Os)	Nb3Rh0.9Os0.1	Nb	3	Rh	0.9	Os	0.1																		1	1965																												Cr3Si(A15)			A	5.1302													Cr3Si, A15	K		2.3					2.3																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112744	492		Nb3(Rh,Os)	Nb3Rh0.7Os0.3	Nb	3	Rh	0.7	Os	0.3																		1	1965																												Cr3Si(A15)			A	5.1315													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112745	492		Nb3(Rh,Os)	Nb3Rh0.5Os0.5	Nb	3	Rh	0.5	Os	0.5																		1	1965																												Cr3Si(A15)			A	5.1334													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112746	492		Nb3(Rh,Os)	Nb3Rh0.3Os0.7	Nb	3	Rh	0.3	Os	0.7																		1	1965																												Cr3Si(A15)			A	5.1345													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112747	492		Nb3(Rh,Os)	Nb3Rh0.1Os0.9	Nb	3	Rh	0.1	Os	0.9																		1	1965																												Cr3Si(A15)			A	5.1354													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112748	492		Nb3(Rh,Ir)	Nb3Rh0.98Ir0.02	Nb	3	Rh	0.98	Ir	0.02																		1	1965																												Cr3Si(A15)			A	5.131													Cr3Si, A15	K		2.43					2.43																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112749	492		Nb3(Rh,Ir)	Nb3Rh0.95Ir0.05	Nb	3	Rh	0.95	Ir	0.05																		1	1965																												Cr3Si(A15)			A	5.132													Cr3Si, A15	K		2.38					2.38																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112750	492		Nb3(Rh,Ir)	Nb3Rh0.9Ir0.1	Nb	3	Rh	0.9	Ir	0.1																		1	1965																												Cr3Si(A15)			A	5.1329													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112751	492		Nb3(Rh,Ir)	Nb3Rh0.7Ir0.3	Nb	3	Rh	0.7	Ir	0.3																		1	1965																												Cr3Si(A15)			A	5.134													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112752	492		Nb3(Rh,Ir)	Nb3Rh0.5Ir0.5	Nb	3	Rh	0.5	Ir	0.5																		1	1965																												Cr3Si(A15)			A	5.1349													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112753	492		Nb3(Rh,Ir)	Nb3Rh0.3Ir0.7	Nb	3	Rh	0.3	Ir	0.7																		1	1965																												Cr3Si(A15)			A	5.1349													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112754	492		Nb3(Rh,Ir)	Nb3Rh0.1Ir0.9	Nb	3	Rh	0.1	Ir	0.9																		1	1965																												Cr3Si(A15)			A	5.1345													Cr3Si, A15	K					1.7																																																																																																		arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112755	492		Nb3(Rh,Pt)	Nb3Rh0.98Pt0.02	Nb	3	Rh	0.98	Pt	0.02																		1	1965																												Cr3Si(A15)			A	5.132													Cr3Si, A15	K		2.52					2.52																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112756	492		Nb3(Rh,Pt)	Nb3Rh0.95Pt0.05	Nb	3	Rh	0.95	Pt	0.05																		1	1965																												Cr3Si(A15)			A	5.133													Cr3Si, A15	K		2.53					2.53																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112757	492		Nb3(Rh,Pt)	Nb3Rh0.9Pt0.1	Nb	3	Rh	0.9	Pt	0.1																		1	1965																												Cr3Si(A15)			A	5.1336													Cr3Si, A15	K		2.8					2.8																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112758	492		Nb3(Rh,Pt)	Nb3Rh0.7Pt0.3	Nb	3	Rh	0.7	Pt	0.3																		1	1965																												Cr3Si(A15)			A	5.1395													Cr3Si, A15	K		5.1					5.1																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112759	492		Nb3(Rh,Pt)	Nb3Rh0.5Pt0.5	Nb	3	Rh	0.5	Pt	0.5																		1	1965																												Cr3Si(A15)			A	5.145													Cr3Si, A15	K		6.25					6.25																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112760	492		Nb3(Rh,Pt)	Nb3Rh0.3Pt0.7	Nb	3	Rh	0.3	Pt	0.7																		1	1965																												Cr3Si(A15)			A	5.1487													Cr3Si, A15	K		7.4					7.4																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112761	492		Nb3(Rh,Pt)	Nb3Rh0.1Pt0.9	Nb	3	Rh	0.1	Pt	0.9																		1	1965																												Cr3Si(A15)			A	5.1534													Cr3Si, A15	K		7.9					7.9																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112762	492		Nb3(Rh,Pt)	Nb3Rh0.05Pt0.95	Nb	3	Rh	0.05	Pt	0.95																		1	1965																												Cr3Si(A15)			A	5.16													Cr3Si, A15	K		8.9					8.9																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112763	492		Nb3(Rh,Pt)	Nb3Rh0.02Pt0.98	Nb	3	Rh	0.02	Pt	0.98																		1	1965																												Cr3Si(A15)			A	5.157													Cr3Si, A15	K		9.6					9.6																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112764	492		Nb3(Rh,Au)	Nb3Rh0.98Au0.02	Nb	3	Rh	0.98	Au	0.02																		1	1965																												Cr3Si(A15)			A	5.133													Cr3Si, A15	K		2.53					2.53																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112765	492		Nb3(Rh,Au)	Nb3Rh0.95Au0.05	Nb	3	Rh	0.95	Au	0.05																		1	1965																												Cr3Si(A15)			A	5.137													Cr3Si, A15	K		2.52					2.52																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112766	492		Nb3(Rh,Au)	Nb3Rh0.9Au0.1	Nb	3	Rh	0.9	Au	0.1																		1	1965																												Cr3Si(A15)			A	5.1412													Cr3Si, A15	K		2.7					2.7																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112767	492		Nb3(Rh,Au)	Nb3Rh0.7Au0.3	Nb	3	Rh	0.7	Au	0.3																		1	1965																												Cr3Si(A15)			A	5.1573													Cr3Si, A15	K		4.6					4.6																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112768	492		Nb3(Rh,Au)	Nb3Rh0.5Au0.5	Nb	3	Rh	0.5	Au	0.5																		1	1965																												Cr3Si(A15)			A	5.1688													Cr3Si, A15	K		6.6					6.6																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112769	492		Nb3(Rh,Au)	Nb3Rh0.3Au0.7	Nb	3	Rh	0.3	Au	0.7																		1	1965																												Cr3Si(A15)			A	5.1827													Cr3Si, A15	K		9.5					9.5																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112770	492		Nb3(Rh,Au)	Nb3Rh0.1Au0.9	Nb	3	Rh	0.1	Au	0.9																		1	1965																												Cr3Si(A15)			A	5.196													Cr3Si, A15	K		10.8					10.8																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112771	492		Nb3(Rh,Au)	Nb3Rh0.05Au0.95	Nb	3	Rh	0.05	Au	0.95																		1	1965																												Cr3Si(A15)			A	5.2													Cr3Si, A15	K		11					11																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112772	492		Nb3(Rh,Au)	Nb3Rh0.02Au0.98	Nb	3	Rh	0.02	Au	0.98																		1	1965																												Cr3Si(A15)			A	5.203													Cr3Si, A15	K		10.9					10.9																																																																																																arc-melting					SUPERCONDUCTIVITY CR3SI-TYPE TERNARY PHASES WITH NIOBIUM AND GROUP VIII METALS				PHYS.REV.,137(1965)A1438	S.T.ZEGLER		
112773	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 151 . micro-hardness = 61  kg/mm2.	Nb1-xOx	Nb99.976O0.024	Nb	99.976	O	0.024																				1	1974																															A	3.3002													bcc	K		9.23					9.23																				T		0.291																																		mj/mol.K2	7.95		278																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112774	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 17.6 . micro-hardness = 74  kg/mm2.	Nb1-xOx	Nb99.861O0.139	Nb	99.861	O	0.139																				1	1974																															A	3.3													bcc	K		9.03					9.03																				T		0.415																																		mj/mol.K2	7.67		256																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112775	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 6.30 . micro-hardness = 134  kg/mm2.	Nb1-xOx	Nb99.445O0.555	Nb	99.445	O	0.555																				1	1974																															A	3.3025													bcc	K		8.5					8.5																				T		0.586																																		mj/mol.K2	7.43		260																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112776	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 4.12 . micro-hardness = 177  kg/mm2.	Nb1-xOx	Nb99.078O0.922	Nb	99.078	O	0.922																				1	1974																															A	3.3023													bcc	K		8.1					8.1																				T		0.745																																		mj/mol.K2	7.23		260																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112777	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 3.09 . micro-hardness = 222  kg/mm2.	Nb1-xOx	Nb98.68O1.32	Nb	98.68	O	1.32																				1	1974																															A	3.306													bcc	K		7.85					7.85																				T		0.842																																		mj/mol.K2	6.92		268																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112778	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 2.56 . micro-hardness = 265  kg/mm2.	Nb1-xOx	Nb98O2	Nb	98	O	2																				1	1974																															A	3.3093													bcc	K		7.33					7.33																				T		0.917																																		mj/mol.K2	6.67		274																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112779	1776	Hc2(0) in DB shows Hc2(4.2K). RRR= 1.86 . micro-hardness = 375  kg/mm2.	Nb1-xOx	Nb96.5O3.5	Nb	96.5	O	3.5																				1	1974																															A	3.313													bcc	K		6.13					6.13																				T		0.851																																		mj/mol.K2	5.94		296																																					O-content controlled by ANN time(1000C, P(O2)=1.0E-5 Torr)					Effects of intersticial oxygen on the superconductivity of niobium				PHYS.REV.B,9(1974)888	C.C.KOCH,D.M.KROEGER,J.O.SCARBROUGH		
112780	PRB1490231	RRR = 1500 (three samples with RRR = 1480, 1360, 1670)	Nb	Nb1	Nb	1																						1	1966																																													bcc	K		9.25					9.25											Oe		1735							T		0.404												MHC12780																																																														heat without O2					Superconducting properties of high-purity niobium			Iowa State University,Iowa,USA	Phys.Rev., 149(1966)231	C.A.Swenson,D.K.Finnemore,T.F.Stromberg		
112781	1300	RRR = 100. Hc2(0) in DB shows Hc2(1.5 K) for H//<110>. Hc2(1.5 K)<001> = 3.92 kOe.	Nb	Nb1	Nb	1																						3	1968																																													bcc	K		9.21					9.21																				T		0.416																																																																															Precision measurement of anisotropy in the upper critical field of superconducting niobium				PHYS.REV.,176(1968)562	B.S.CHANDRASEKHAR,D.E.FARRELL,S.HUANG		
112782	P070174512	lattice const is for 4 unit cell. S-I transition at 215K(P=0) and 0 K(P=2.6GPa). Tc = 7.5*exp(-2*R), where R is residual resistivity in mOhm.cm.	Ba6Ge25	Ba6Ge25	Ba	6	Ge	25																				1	2004																												clathrate			A	14.5564														K		0.24					0.24			K/GPa	1.49																T		0.31							T/K		1.49			MHC12782																																																														HF-melting					Interplay of superconductivity and structural phase transition in the clathrate Ba6Ge25		M-12782	Max-Planck-Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 70(2004)174512	F.M.Groshe,F.Steglich,G.Spam,H.Q.Yuan,M.Baenitz,U.Schwarz,V.Pacheco,W.Camillo-Cabrera,Yu.Grin		
112783	P070174512	-(dHc2/dT)=1.0 (P=0.74 GPa), 1.03(P=1.85), 1.08 (P=2.73).	Ba4Na2Ge25	Ba4Na2Ge25	Ba	4	Na	2	Ge	25																		1	2004																												clathrate																		K		0.84					0.84																													T/K		1.11																																																																	HF-melting					Interplay of superconductivity and structural phase transition in the clathrate Ba6Ge25		M-12782	Max-Planck-Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 70(2004)174512	F.M.Groshe,F.Steglich,G.Spam,H.Q.Yuan,M.Baenitz,U.Schwarz,V.Pacheco,W.Camillo-Cabrera,Yu.Grin		
112784	L088167004	Hc2(0)//c = 3.1 T. anisotropy (from Hc2) decreases from 7-8 (T=0K) to 2.3-2.7 (T=Tc). Anisotropy has field dependence.	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38.5					38.5																				T		23																																																																										heat(1700-1800C, in BN)					Temperature and Field Dependence of the Anisotropy of MgB2		M-12784	Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland 	Phys.Rev.Lett., 88(2002)167004	A.Wisniewski,H.Keller,J.Jun,J.Karpinski,J.Roos,M.Angst,R.Puzniak,S.M.Kazakov		
112785	SST0151156	Hc1, Hc2 for H//c. Anisotropy factor is independent of temperature (=2.1). Hc1(T=28 K) = 31 mT for H//ab.. G-L parameter = 2.1	MgB2	B2Mg1	B	2	Mg	1																				3	2002																												AlB2																	AlB2, C32	K		38					38											T		0.28							T		3												MHC12785		A		100			A		220																																																										Superconducting critical fields and anisotropy of a MgB2 single crystal		M-12785	Centre for High Temperature Superconductivity, Blackett Laboratory, Imperial College of Science, Technology and Medicine, London, UK	Supercond.Sci.Technol., 15(2002)1156	A.D.Caplin,G.K.Perkins,J.Jun,J.Karpinski,J.Moore,L.F.Cohen,S.M.Kazakov,Y.Bugoslavski		
112786	P069144514	Hc2  is for H//c. SC properties calculated using Hao-Clem model (M-H curve). Hc2(0)//c = 2.80 T by curve fitting. G-L parameter = 6.4	MgB2	B2Mg1	B	2	Mg	1																				3	2004																												AlB2																	AlB2, C32	K		37.9					37.9																				T		2.86														A		107			A		764																																																										Reversible magnetization of MgB2 single crystals with a two-gap nature		M-12786	University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B, 69(2004)144514	B.Kang,H.Kim,K.Kim,M.Park,S.Lee		
112787	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 0.6	Ti64Nb36	Nb0.36Ti0.64	Nb	0.36	Ti	0.64																					1969																																														K		9.05					9.05																				T		10.9																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112788	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 1.0	Ti64(Nb,Ta)36	Ti0.64Nb0.34Ta0.02	Ti	0.64	Nb	0.34	Ta	0.02																			1969																																														K		8.99					8.99																				T		11.7																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112789	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 1.3	Ti64(Nb,Ta)36	Ti0.64Nb0.32Ta0.04	Ti	0.64	Nb	0.32	Ta	0.04																			1969																																														K		8.9					8.9																				T		11.9																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112790	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 2.5	Ti64(Nb,Ta)36	Ti0.64Nb0.28Ta0.08	Ti	0.64	Nb	0.28	Ta	0.08																			1969																																														K		8.74					8.74																				T		11.9																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112791	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 4.2	Ti64(Nb,Ta)36	Ti0.64Nb0.26Ta0.1	Ti	0.64	Nb	0.26	Ta	0.1																			1969																																														K		8.56					8.56																				T		11.8																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112792	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 7.9	Ti64(Nb,Ta)36	Ti0.64Nb0.24Ta0.12	Ti	0.64	Nb	0.24	Ta	0.12																			1969																																														K		8.32					8.32																				T		11.5																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112793	1398	HC2ZERO in DB means Hc2(4.2K). spin-orbit parameter = 18.2	Ti64(Nb,Ta)36	Ti0.64Nb0.18Ta0.18	Ti	0.64	Nb	0.18	Ta	0.18																			1969																																														K		8.18					8.18																				T		11.01																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112794	1398	HC2ZERO in DB means Hc2(4.2K).	Ti64(Nb,Ta)36	Ti0.64Nb0.1Ta0.26	Ti	0.64	Nb	0.1	Ta	0.26																			1969																																														K		7.78					7.78																				T		9.97																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112795	1398	HC2ZERO in DB means Hc2(4.2K).	Ti64Ta36	Ta0.36Ti0.64	Ta	0.36	Ti	0.64																					1969																																														K		7.53					7.53																																																																																																					Some superconducting properties of Ti-Nb-Ta ternary alloys				J.APPL.PHYS.,40(1969)4457	K.M.RALLS,M.SUENAGA		
112796	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Hf	Nb0.4Zr0.3Hf0.3	Nb	0.4	Zr	0.3	Hf	0.3																			1967																																														K																											T		8.71																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112797	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr-Hf	Nb0.4Ti0.2Zr0.2Hf0.2	Nb	0.4	Ti	0.2	Zr	0.2	Hf	0.2																	1967																																														K																											T		9.11																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112798	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.35Zr0.35Ti0.3	Nb	0.35	Zr	0.35	Ti	0.3																			1967																																														K																											T		9.98																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112799	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.35Zr0.2Ti0.45	Nb	0.35	Zr	0.2	Ti	0.45																			1967																																														K																											T		10.4																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112800	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Hf	Nb0.32Ti0.64Hf0.04	Nb	0.32	Ti	0.64	Hf	0.04																			1967																																														K																											T		11.4																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112801	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr-Ta	Nb0.39Ti0.53Zr0.04Ta0.04	Nb	0.39	Ti	0.53	Zr	0.04	Ta	0.04																	1967																																														K																											T		11.86																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112802	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Ta	Nb0.36Ti0.6Ta0.04	Nb	0.36	Ti	0.6	Ta	0.04																			1967																																														K																											T		12.41																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112803	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti	Nb0.4Ti0.6	Nb	0.4	Ti	0.6																					1967																																														K																											T		11.79																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112804	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-W	Nb0.35Ti0.64W0.01	Nb	0.35	Ti	0.64	W	0.01																			1967																																														K																											T		11.39																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112805	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Mo	Nb0.34Ti0.65Mo0.01	Nb	0.34	Ti	0.65	Mo	0.01																			1967																																														K																											T		11.23																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112806	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Hf-V	Nb0.4Ti0.52Hf0.04V0.04	Nb	0.4	Ti	0.52	Hf	0.04	V	0.04																	1967																																														K																											T		11.02																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112807	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ta-Ti-Hf	Nb0.42Ta0.04Ti0.5Hf0.04	Nb	0.42	Ta	0.04	Ti	0.5	Hf	0.04																	1967																																														K																											T		10.79																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112808	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.5Ti0.45Zr0.05	Nb	0.5	Ti	0.45	Zr	0.05																			1967																																														K																											T		9.84																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112809	1391	HC2ZERO in DB means Hc2(4.2K). 	Ta-Ti	Ta0.53Ti0.47	Ta	0.53	Ti	0.47																					1967																																														K																											T		8.73																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112810	1391	HC2ZERO in DB means Hc2(4.2K). 	Ta-Ti-Zr	Ta0.63Ti0.3Zr0.07	Ta	0.63	Ti	0.3	Zr	0.07																			1967																																														K																											T		7.77																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112811	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Ti	Nb0.77Zr0.13Ti0.1	Nb	0.77	Zr	0.13	Ti	0.1																			1967																																														K																											T		8.02																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112812	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Ti	Nb0.8Ti0.1Zr0.1	Nb	0.8	Ti	0.1	Zr	0.1																			1967																																														K																											T		7.71																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112813	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti	Nb0.76Ti0.24	Nb	0.76	Ti	0.24																					1967																																														K																											T		6																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112814	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Ti	Nb0.78Ti0.21Zr0.01	Nb	0.78	Ti	0.21	Zr	0.01																			1967																																														K																											T		5.59																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112815	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Fe	Nb0.8Ti0.19Fe0.01	Nb	0.8	Ti	0.19	Fe	0.01																			1967																																														K																											T		4.09																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112816	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Ti	Nb0.58Ti0.3Zr0.12	Nb	0.58	Ti	0.3	Zr	0.12																			1967																																														K																											T		9.14																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112817	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.6Ti0.3Zr0.1	Nb	0.6	Ti	0.3	Zr	0.1																			1967																																														K																											T		8.79																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112818	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.69Ti0.15Zr0.16	Nb	0.69	Ti	0.15	Zr	0.16																			1967																																														K																											T		7.73																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112819	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Ti-Zr	Nb0.66Ti0.15Zr0.19	Nb	0.66	Ti	0.15	Zr	0.19																			1967																																														K																											T		7.61																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112820	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Hf-Ti	Nb0.67Zr0.11Hf0.11Ti0.11	Nb	0.67	Zr	0.11	Hf	0.11	Ti	0.11																	1967																																														K																											T		7.16																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112821	1391	HC2ZERO in DB means Hc2(4.2K). 	Nb-Zr-Hf	Nb0.74Zr0.13Hf0.13	Nb	0.74	Zr	0.13	Hf	0.13																			1967																																														K																											T		6.59																																																																															Probable upper limit of Hc2 for some higher-order ductile transition-metal superconducting alloys				J.APPL.PHYS.,38(1967)903	P.E.LAWRENCE,W.A.HEALDY,W.DESORBO		
112822	1775	Hc2 by permeability. PENET is London penetration depth.	Nb	Nb1	Nb	1																							1974																																														K		9.273					9.273																																				A		387			A		314																																																										Surface superconductivity in niobium and niobium-tantalum alloys				PHYS.REV.B,9(1974)108	D.K.FINNEMORE,J.R.HOPKINS		
112823	1775	Hc2 by permeability. PENET is London penetration depth.	Nb1-xTax	Nb0.995Ta0.005	Nb	0.995	Ta	0.005																					1974																																														K		9.226					9.226																																				A		343			A		353																																																										Surface superconductivity in niobium and niobium-tantalum alloys				PHYS.REV.B,9(1974)108	D.K.FINNEMORE,J.R.HOPKINS		
112824	1775	Hc2 by permeability. PENET is London penetration depth.	Nb1-xTax	Nb0.99Ta0.01	Nb	0.99	Ta	0.01																					1974																																														K		9.079					9.079																																				A		268			A		456																																																										Surface superconductivity in niobium and niobium-tantalum alloys				PHYS.REV.B,9(1974)108	D.K.FINNEMORE,J.R.HOPKINS		
112825	253		Ti1-xVx	Ti0.415V0.585	Ti	0.415	V	0.585																					1961																																														K		7.49					7.49																																																								mj/mol.K2	10.5		376																																										SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112826	253		Ti1-xVx	Ti0.106V0.894	Ti	0.106	V	0.894																					1961																																														K		6.86					6.86																																																								mj/mol.K2	11.3		348																																										SUPERCONDUCTING SOLID SOLUTION ALLOYS OF THE TRANSITION ELEMENTS				PHYS.REV.,123(1961)1569	J.K.HULM,R.D.BLAUGHER		
112827	1352	NMR of Nb< 93 > measured	Nb	Nb1	Nb	1																							1967																																														K		9.2					9.2																																																								mj/mol.K2	7.9		242																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
112828	1352	NMR of Nb< 93 > measured	Nb1-xZrx	Nb0.75Zr0.25	Nb	0.75	Zr	0.25																					1967																																														K		10.6					10.6																																																								mj/mol.K2	10.2		215																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
112829	1352	NMR of Nb< 93 > measured	Nb1-xZrx	Nb0.65Zr0.35	Nb	0.65	Zr	0.35																					1967																																														K		10.6					10.6																																																								mj/mol.K2	9.5		225																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
112830	1352	NMR of Nb< 93 > measured	Nb1-xZrx	Nb0.5Zr0.5	Nb	0.5	Zr	0.5																					1967																																														K		9.7					9.7																																																								mj/mol.K2	8.5		202																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
112831	1352	NMR of Nb< 93 > measured	Nb1-xZrx	Nb0.25Zr0.75	Nb	0.25	Zr	0.75																					1967																																														K		8.3					8.3																																																								mj/mol.K2	6.7		183																																										Nuclear magnetic resonance and specific heat measurements of transition metal and alloys; Ti-V-Fe and Zr-Nb-Mo systems				J.PHYS.SOC.JAPAN,22(1967)238	M.NISHIOKA,N.WATANABE,Y.MASUDA		
112832	1356	thermodynamic Hc(0) = 797   Oe. G-L parameter = 0.59	Ta1-xNbx	Nb0.016Ta0.984	Nb	0.016	Ta	0.984																					1970																																														K		4.47					4.47																				Oe		847																																																																															Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112833	1356	thermodynamic Hc(0) =  800  Oe. G-L parameter = 0.71	Ta1-xNbx	Nb0.025Ta0.975	Nb	0.025	Ta	0.975																					1970																																														K		4.465					4.465											Oe		773							Oe		993																																																																															Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112834	1356	thermodynamic Hc(0) =  817  Oe. G-L parameter = 0.841	Ta1-xNbx	Nb0.04Ta0.96	Nb	0.04	Ta	0.96																					1970																																														K		4.47					4.47											Oe		772							Oe		1172																																																																															Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112835	1356	thermodynamic Hc(0) =  882  Oe. G-L parameter = 1.21	Ta1-xNbx	Nb0.08Ta0.92	Nb	0.08	Ta	0.92																					1970																																														K		4.54					4.54											Oe		768							Oe		1780																																																																															Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112836	1356		Ta1-xNbx	Nb0.16Ta0.84	Nb	0.16	Ta	0.84																					1970																																														K		4.67					4.67																				Oe		2980																																																																															Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112837	1356		Ta	Ta1	Ta	1																							1970																																														K		4.48					4.48																																																																																																					Magnetic Properties of Superconducting Tantalum-Niobium Alloys				J.Phys.Soc.Japan, 29(1970)1209	Y.Kubota,T.Ogasawara,K.Yasukochi		
112838	1781	Hc(0) = 815  Oe. (delta-C/gamma*Tc) = 1.57. e-ph coupling = 0.648.	Ta	Ta1	Ta	1																							1972																																														K		4.425					4.425																																																3.57								mj/mol.K2	5.96		254																																										Specific heat and magnetic measurements in superconducting Ta-Nb alloys				PHYS.REV.B,6(1972)2609	L.C.CLUNE,R.W.ROLLINS		
112839	1781	Hc(0) =  842 Oe. (delta-C/gamma*Tc) = 1.61. e-ph coupling = 0.650.	Ta1-xNbx	Nb0.037Ta0.963	Nb	0.037	Ta	0.963																					1972																																														K		4.51					4.51																																																3.59								mj/mol.K2	6.06		256																																										Specific heat and magnetic measurements in superconducting Ta-Nb alloys				PHYS.REV.B,6(1972)2609	L.C.CLUNE,R.W.ROLLINS		
112840	1781	Hc(0) =  894 Oe. (delta-C/gamma*Tc) = 1.62. e-ph coupling = 0.660.	Ta1-xNbx	Nb0.14Ta0.86	Nb	0.14	Ta	0.86																					1972																																														K		4.76					4.76	MTC12840																																															3.62								mj/mol.K2	6.17		258																																										Specific heat and magnetic measurements in superconducting Ta-Nb alloys				PHYS.REV.B,6(1972)2609	L.C.CLUNE,R.W.ROLLINS		
112841	1781	Hc(0) = 1100  Oe. (delta-C/gamma*Tc) = 1.68. e-ph coupling = 0.698.	Ta1-xNbx	Nb0.405Ta0.595	Nb	0.405	Ta	0.595																					1972																																														K		5.72					5.72																																																3.66								mj/mol.K2	6.46		260																																										Specific heat and magnetic measurements in superconducting Ta-Nb alloys				PHYS.REV.B,6(1972)2609	L.C.CLUNE,R.W.ROLLINS		
112842	1781	Hc(0) =  1295 Oe. (delta-C/gamma*Tc) = 1.72. e-ph coupling = 0.731.	Ta1-xNbx	Nb0.58Ta0.42	Nb	0.58	Ta	0.42																					1972																																														K		6.54					6.54																																																3.69								mj/mol.K2	6.73		261																																										Specific heat and magnetic measurements in superconducting Ta-Nb alloys				PHYS.REV.B,6(1972)2609	L.C.CLUNE,R.W.ROLLINS		
112843	1307		V	V1	V	1																							1970																																														K		5.17					5.17																				E+3 A/m		106																																		mj/mol.K2	9.45		377																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112844	1307		V1-xNbx	Nb0.15V0.85	Nb	0.15	V	0.85																					1970																																														K		4.3					4.3																				E+3 A/m		84.7																																		mj/mol.K2	9.19		364																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112845	1307		V1-xNbx	Nb0.2V0.8	Nb	0.2	V	0.8																					1970																																														K		4.03					4.03																				E+3 A/m		76.3																																		mj/mol.K2	8.72		326																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112846	1307		V1-xNbx	Nb0.5V0.5	Nb	0.5	V	0.5																					1970																																														K		4.25					4.25																				E+3 A/m		76.2																																		mj/mol.K2	8.3		298																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112847	1307		V1-xNbx	Nb0.69V0.31	Nb	0.69	V	0.31																					1970																																														K		4.9					4.9																				E+3 A/m		84.4																																		mj/mol.K2	7.97		285																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112848	1307		V1-xNbx	Nb0.8V0.2	Nb	0.8	V	0.2																					1970																																														K		5.76					5.76																				E+3 A/m		97																																		mj/mol.K2	7.9		275																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112849	1307		V1-xNbx	Nb0.9V0.1	Nb	0.9	V	0.1																					1970																																														K		6.95					6.95																				E+3 A/m		119.1																																		mj/mol.K2	7.77		266																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112850	1307		Nb	Nb1	Nb	1																							1970																																														K		9.18					9.18																				E+3 A/m		150																																		mj/mol.K2	7.74		248																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112851	1307		V1-xTax	Ta0.1V0.9	Ta	0.1	V	0.9																					1970																																														K		4.47					4.47																				E+3 A/m		87																																		mj/mol.K2	8.78		341																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112852	1307		V1-xTax	Ta0.24V0.76	Ta	0.24	V	0.76																					1970																																														K		3.58					3.58																				E+3 A/m		67																																		mj/mol.K2	8.48		300																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112853	1307		V1-xTax	Ta0.5V0.5	Ta	0.5	V	0.5																					1970																																														K		2.73					2.73																				E+3 A/m		46.5																																		mj/mol.K2	7.62		273																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112854	1307		V1-xTax	Ta0.7V0.3	Ta	0.7	V	0.3																					1970																																														K		3					3																				E+3 A/m		45.6																																		mj/mol.K2	6.41		256																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112855	1307		V1-xTax	Ta0.9V0.1	Ta	0.9	V	0.1																					1970																																														K		3.58					3.58																				E+3 A/m		50																																		mj/mol.K2	5.7		250																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112856	1307		Ta	Ta1	Ta	1																							1970																																														K		4.33					4.33																				E+3 A/m		61.2																																		mj/mol.K2	5.85		251																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112857	1307		Nb1-xTax	Nb0.8Ta0.2	Nb	0.8	Ta	0.2																					1970																																														K		7.42					7.42																				E+3 A/m		117.2																																		mj/mol.K2	7.25		257																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112858	1307		Nb1-xTax	Nb0.7Ta0.3	Nb	0.7	Ta	0.3																					1970																																														K		6.8					6.8																				E+3 A/m		103.5																																		mj/mol.K2	6.76		263																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112859	1307		Nb1-xTax	Nb0.5Ta0.5	Nb	0.5	Ta	0.5																					1970																																														K		5.93					5.93																				E+3 A/m		88.3																																		mj/mol.K2	6.53		260																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112860	1307		Nb1-xTax	Nb0.3Ta0.7	Nb	0.3	Ta	0.7																					1970																																														K		5.15					5.15																				E+3 A/m		72.8																																		mj/mol.K2	6.2		260																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112861	1307		Nb1-xTax	Nb0.15Ta0.85	Nb	0.15	Ta	0.85																					1970																																														K		4.58					4.58																				E+3 A/m		65.6																																		mj/mol.K2	5.99		255																																														PHYS.STAT.SOL.,40(1970)657	A.J.COOK,J.M.CORSAN		
112862	314		V	V1	V	1																							1959																																														K		5.32					5.32																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112863	314		V1-xCrx	Cr0.0018V0.9982	Cr	0.0018	V	0.9982																					1959																																														K		5.15					5.15																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112864	314		V1-xCrx	Cr0.0033V0.9967	Cr	0.0033	V	0.9967																					1959																																														K		5.07					5.07																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112865	314		V1-xCrx	Cr0.0081V0.9919	Cr	0.0081	V	0.9919																					1959																																														K		4.78					4.78																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112866	314		V1-xCrx	Cr0.0132V0.9868	Cr	0.0132	V	0.9868																					1959																																														K		4.57					4.57																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112867	314		V1-xCrx	Cr0.0265V0.9735	Cr	0.0265	V	0.9735																					1959																																														K		3.89					3.89																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112868	314		V1-xTix	Ti0.5V0.5	Ti	0.5	V	0.5																					1959																																														K		6.71					6.71																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112869	314		V1-xTix	Ti0.1V0.9	Ti	0.1	V	0.9																					1959																																														K		6.03					6.03																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112870	314		V1-xTix	Ti0.03V0.97	Ti	0.03	V	0.97																					1959																																														K		5.58					5.58																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112871	314		V1-xTix	Ti0.01V0.99	Ti	0.01	V	0.99																					1959																																														K		5.42					5.42																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112872	314		V1-xCrx	Cr0.01V0.99	Cr	0.01	V	0.99																					1959																																														K		4.8					4.8																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112873	314		V1-xCrx	Cr0.02V0.98	Cr	0.02	V	0.98																					1959																																														K		4.08					4.08																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112874	314		V1-xCrx	Cr0.026V0.974	Cr	0.026	V	0.974																					1959																																														K		3.66					3.66																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112875	314		V1-xCrx	Cr0.055V0.945	Cr	0.055	V	0.945																					1959																																														K		1.89					1.89																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112876	314		V1-xCox	Co0.007V0.993	Co	0.007	V	0.993																					1959																																														K		4.52					4.52																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112877	314		V1-xCox	Co0.017V0.983	Co	0.017	V	0.983																					1959																																														K		3.28					3.28																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112878	314		V1-xCox	Co0.02V0.98	Co	0.02	V	0.98																					1959																																														K		2.61					2.61																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112879	314		V1-xCox	Co0.03V0.97	Co	0.03	V	0.97																					1959																																														K		1.48					1.48																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112880	314		V1-xNix	Ni0.011V0.989	Ni	0.011	V	0.989																					1959																																														K		3.82					3.82																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112881	314		V1-xNix	Ni0.02V0.98	Ni	0.02	V	0.98																					1959																																														K		3.29					3.29																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112882	314		V1-xNix	Ni0.03V0.97	Ni	0.03	V	0.97																					1959																																														K		2.11					2.11																																																																																																					Supraleitung in Mischkristallen des Vanadiums mit Ubergangselementen				HELV.PHYS.ACTA,32(1959)141	J.MULLER		
112883	1579		Zr1-xNbx	Nb0.25Zr0.75	Nb	0.25	Zr	0.75																					1972																																														K		8.6					8.6																																																																																																					The superconducting transition behavior of Zr-Nb binary alloys				J.NUCLEAR MATERIALS,43(1972)258	F.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
112884	1579		Zr1-xNbx	Nb0.35Zr0.65	Nb	0.35	Zr	0.65																					1972																																														K		9.45					9.45	MTC12884																																																																																																				The superconducting transition behavior of Zr-Nb binary alloys				J.NUCLEAR MATERIALS,43(1972)258	F.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
112885	1579		Zr1-xNbx	Nb0.5Zr0.5	Nb	0.5	Zr	0.5																					1972																																														K		10.3					10.3																																																																																																					The superconducting transition behavior of Zr-Nb binary alloys				J.NUCLEAR MATERIALS,43(1972)258	F.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
112886	847	alpha-phase	Zr1-xNbx	Nb0.005Zr0.995	Nb	0.005	Zr	0.995																					1968																																														K		1.86					1.86																																																																																																					Superconducting transition temperatures of zirconium-niobium alloys				J.LESS-COMMON METALS,15(1968)437	A.J.COOK,I.WILLIAMS,J.A.CATTERALL,J.M.CORSAN		
112887	847		Zr1-xNbx	Nb0.5Zr0.5	Nb	0.5	Zr	0.5																					1968																																														K		10.4					10.4	MTC12887																																																																																																				Superconducting transition temperatures of zirconium-niobium alloys				J.LESS-COMMON METALS,15(1968)437	A.J.COOK,I.WILLIAMS,J.A.CATTERALL,J.M.CORSAN		
112888	847		Zr1-xNbx	Nb0.75Zr0.25	Nb	0.75	Zr	0.25																					1968																																														K		10.7					10.7																																																																																																					Superconducting transition temperatures of zirconium-niobium alloys				J.LESS-COMMON METALS,15(1968)437	A.J.COOK,I.WILLIAMS,J.A.CATTERALL,J.M.CORSAN		
112889	1236	a'-phase	Nb3(Sn,Sb)	Nb3Sn1	Nb	3	Sn	1																					1967																															A	5.2921														K		18.1					18.1																																																																																																					Superconducting transition temperature and electronic structure in the pseudobinary Nb3Al-Nb3Sn and Nb3Sn-Nb3Sb				J.PHYS.CHEM.SOLIDS, 28(1967)889	F.J.BACHNER,H.C.GATOS,J.B.GOODENOUGH		
112890	1236	a'-phase	Nb3(Sn,Sb)	Nb3Sn0.8Sb0.2	Nb	3	Sn	0.8	Sb	0.2																			1967																															A	5.2862														K		16.5					16.5	MTC12890																																																																																																				Superconducting transition temperature and electronic structure in the pseudobinary Nb3Al-Nb3Sn and Nb3Sn-Nb3Sb				J.PHYS.CHEM.SOLIDS, 28(1967)889	F.J.BACHNER,H.C.GATOS,J.B.GOODENOUGH		
112891	1236	a'+a'' phase. For a''-phase, a = 5.2704	Nb3(Sn,Sb)	Nb3Sn0.7Sb0.3	Nb	3	Sn	0.7	Sb	0.3																			1967																															A	5.283														K		15.8					15.8	MTC12890																																																																																																				Superconducting transition temperature and electronic structure in the pseudobinary Nb3Al-Nb3Sn and Nb3Sn-Nb3Sb				J.PHYS.CHEM.SOLIDS, 28(1967)889	F.J.BACHNER,H.C.GATOS,J.B.GOODENOUGH		
112892	1236	a'+a'' phase. For a''-phase, a = 5.2694	Nb3(Sn,Sb)	Nb3Sn0.5Sb0.5	Nb	3	Sn	0.5	Sb	0.5																			1967																															A	5.2822														K		14.4					14.4																																																																																																					Superconducting transition temperature and electronic structure in the pseudobinary Nb3Al-Nb3Sn and Nb3Sn-Nb3Sb				J.PHYS.CHEM.SOLIDS, 28(1967)889	F.J.BACHNER,H.C.GATOS,J.B.GOODENOUGH		
112893	1066		Nb3Al	Al1Nb3	Al	1	Nb	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K		18.2					18.2	MTC12893																																																																																																								Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112894	1066		V3Si	Si1V3	Si	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K		17					17	MTC12894																																																																																																								Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112895	1066		Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K		16					16	MTC12895																																																																																																								Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112896	1066		Nb3Sn	Nb1Sn3	Nb	1	Sn	3																					1966																												Cr3Si(A15)			A	5.2872													Cr3Si, A15	K		18					18																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112897	1066		(Nb,Ti)3Sn	Nb2.85Ti0.15Sn1	Nb	2.85	Ti	0.15	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		17.9					17.9																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112898	1066		(Nb,Ti)3Sn	Nb2.7Ti0.3Sn1	Nb	2.7	Ti	0.3	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		16.4					16.4																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112899	1066		(Nb,Ti)3Sn	Nb2.55Ti0.45Sn1	Nb	2.55	Ti	0.45	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		15.6					15.6																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112900	1066		(Nb,Zr)3Sn	Nb2.85Zr0.15Sn1	Nb	2.85	Zr	0.15	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112901	1066		(Nb,Zr)3Sn	Nb2.7Zr0.3Sn1	Nb	2.7	Zr	0.3	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		18.1					18.1																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112902	1066		(Nb,Zr)3Sn	Nb2.55Zr0.45Sn1	Nb	2.55	Zr	0.45	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		17.9					17.9																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112903	1066		(Nb,Zr)3Sn	Nb2.34Zr0.66Sn1	Nb	2.34	Zr	0.66	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112904	1066		(Nb,Zr)3Sn	Nb2.1Zr0.9Sn1	Nb	2.1	Zr	0.9	Sn	1																			1966																												Cr3Si(A15)																	Cr3Si, A15	K		17.7					17.7																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112905	1066		(Nb,V)3Sn	Nb2.934V0.066Sn1	Nb	2.934	V	0.066	Sn	1																			1966																												Cr3Si(A15)			A	5.2844													Cr3Si, A15	K		17.7					17.7																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112906	1066		(Nb,V)3Sn	Nb2.85V0.15Sn1	Nb	2.85	V	0.15	Sn	1																			1966																												Cr3Si(A15)			A	5.2791													Cr3Si, A15	K		17.1					17.1																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112907	1066		(Nb,V)3Sn	Nb2.7V0.3Sn1	Nb	2.7	V	0.3	Sn	1																			1966																												Cr3Si(A15)			A	5.2731													Cr3Si, A15	K		15.9					15.9																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112908	1066		(Nb,V)3Sn	Nb2.55V0.45Sn1	Nb	2.55	V	0.45	Sn	1																			1966																												Cr3Si(A15)			A	5.2671													Cr3Si, A15	K		15					15																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112909	1066		(Nb,Ta)3Sn	Nb2.85Ta0.15Sn1	Nb	2.85	Ta	0.15	Sn	1																			1966																												Cr3Si(A15)			A	5.2858													Cr3Si, A15	K		18.3					18.3																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112910	1066		(Nb,Ta)3Sn	Nb2.7Ta0.3Sn1	Nb	2.7	Ta	0.3	Sn	1																			1966																												Cr3Si(A15)			A	2.2849													Cr3Si, A15	K		18					18																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112911	1066		(Nb,Ta)3Sn	Nb2.4Ta0.6Sn1	Nb	2.4	Ta	0.6	Sn	1																			1966																												Cr3Si(A15)			A	5.2837													Cr3Si, A15	K		17.3					17.3																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112912	1066		(Nb,Ta)3Sn	Nb2.1Ta0.9Sn1	Nb	2.1	Ta	0.9	Sn	1																			1966																												Cr3Si(A15)			A	5.2826													Cr3Si, A15	K		16					16																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112913	1066		(Nb,Ta)3Sn	Nb1.8Ta1.2Sn1	Nb	1.8	Ta	1.2	Sn	1																			1966																												Cr3Si(A15)			A	5.2809													Cr3Si, A15	K		14.1					14.1																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112914	1066		V3Ga	Ga1V3	Ga	1	V	3																					1966																												Cr3Si(A15)																	Cr3Si, A15	K		14.5					14.5																																																																																																									Z.PHYS.,189(1966)401	E.SAUR,W.KUNZ		
112915	1513	RRR = 2.60. Thermal conductivity measured.	Nb1-xMox	Mo0.2Nb0.8	Mo	0.2	Nb	0.8																					1969																																														K		4.23					4.23																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112916	1513	RRR = 3.20. Thermal conductivity measured.	Nb1-xMox	Mo0.15Nb0.85	Mo	0.15	Nb	0.85																					1969																																														K		5.3					5.3																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112917	1513	RRR = 6.00. Thermal conductivity measured.	Nb1-xMox	Mo0.02Nb0.98	Mo	0.02	Nb	0.98																					1969																																														K		8.58					8.58																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112918	1513	RRR = 700. Thermal conductivity measured.	Nb	Nb1	Nb	1																							1969																																														K		9.1					9.1																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112919	1513	RRR = 3.58. Thermal conductivity measured.	Ta1-xNbx	Nb0.4Ta0.6	Nb	0.4	Ta	0.6																					1969																																														K		5.4					5.4																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112920	1513	RRR = 6.60. Thermal conductivity measured.	Ta1-xNbx	Nb0.2Ta0.8	Nb	0.2	Ta	0.8																					1969																																														K		4.64					4.64																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112921	1513	RRR = 13.5. Thermal conductivity measured.	Ta1-xNbx	Nb0.1Ta0.9	Nb	0.1	Ta	0.9																					1969																																														K		4.55					4.55																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112922	1513	RRR = 32. Thermal conductivity measured.	Ta1-xNbx	Nb0.05Ta0.95	Nb	0.05	Ta	0.95																					1969																																														K		4.45					4.45																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112923	1513	RRR = 160. Thermal conductivity measured.	Ta	Ta1	Ta	1																							1969																																														K		4.48					4.48																																																																																																					Lattice thermal conductivity of Ta-Nb and Nb-Mo solid solution alloys in normal and superconducting states				J.PHYS.C,(SOLID ST.PHYS.),2(1969)629	J.B.SOUSA		
112924	301		PdxTe2	Pd1Te2	Pd	1	Te	2																				3	1961																																														K		1.53					1.53																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
112925	301		PdxTe2	Pd1.05Te2	Pd	1.05	Te	2																				1	1961																																														K		1.77					1.77																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
112926	301		PdxTe2	Pd1.25Te2	Pd	1.25	Te	2																				1	1961																																														K		2.2					2.2																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
112927	301		PdxTe2	Pd1.5Te2	Pd	1.5	Te	2																				1	1961																																														K		2.21					2.21																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
112928	301		PdxTe2	Pd1.75Te2	Pd	1.75	Te	2																				1	1961																																														K		2.25					2.25																																																																																																					PdTe2, ein Supraleiter mit CdJ2-Structur				HELV.PHYS.ACTA,34(1961)408	F.HULLIGER,J.GUGGENHEIM,J.MULLER		
112929	1758	poly powder. Tc-width = 0.15 K.	NbSe2.2	Nb1Se2.2	Nb	1	Se	2.2																				1	1974																												2H-NbSe2																		K		6.35					6.35			K/GPa	0.45																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112930	1758	poly powder. Tc-width = 0.05 K.	NbSe2.2	Nb1Se2.2	Nb	1	Se	2.2																				1	1974																												2H-NbSe2																		K		6.35					6.35			K/GPa	0.7																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112931	1758	poly powder. Tc-width = 0.15 K.	NbSe2.2	Nb1Se2.2	Nb	1	Se	2.2																				1	1974																												2H-NbSe2			A	3.44		25.2												K		7					7			K/GPa	0.45																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112932	1758	single flake. Tc-width = 0.02 K.	NbSe2	Nb1Se2	Nb	1	Se	2																				3	1974																												2H-NbSe2			A	3.45		12.54												K		7.17					7.17			K/GPa	0.495																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112933	1758	poly powder. Tc-width = 0.03 K.	NbSe2	Nb1Se2	Nb	1	Se	2																				1	1974																												2H-NbSe2																		K		7.02					7.02			K/GPa	0.7																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112934	1758	poly powder. Tc-width = 0.02 K.	NbxSe2	Nb1.01Se2	Nb	1.01	Se	2																					1974																												2H-NbSe2			A	3.44		12.55												K		7.05					7.05			K/GPa	0.45																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112935	1758	poly powder. Tc-width = 0.03 K.	NbxSe2	Nb1.02Se2	Nb	1.02	Se	2																					1974																												2H-NbSe2			A	3.45		12.57												K		6.75					6.75			K/GPa	0.41																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112936	1758	poly powder. Tc-width = 0.3 K.	NbxSe2	Nb1.05Se2	Nb	1.05	Se	2																					1974																												2H-NbSe2			A	3.45		12.59												K		4.86					4.86			K/GPa	0.8																																																																																																	Pressure enhanced superconductivity in NbSe2				J.PHYS.F:METAL PHYS.,4(1974)2009	R.E.SCHWALL,R.N.SHELTON,T.F.SMITH		
112937	318	thermodynamic H0 = 302.9 Oe. impurity effect (In, Cd, Sb, Hg, Zn, Bi, Pb < 0.3 at %) was investigated.	Sn	Sn1	Sn	1																							1957																																														K		3.734					3.734																																																								mj/mol.K2	1.72																																												The superconductive critical temperature and the electronic specific heat of impure TiN				J.PHYS.CHEM.SOLIDS,3(1957)165	B.SERIN,E.A.LYNTON,M.ZUCKER		
112938	1771	Hc2(0) at 4.2 K. HRRR = 33.4	Nb	Nb1	Nb	1																							1975																																														K		9.16					9.16																				kOe		3.19																																																																										ANN(1500C)					The effect of yttrium or gadorinium on the superconducting transition temperature of niobium				J.LESS-COMMON.MET.,40(1975)29	C.C.KOCH,D.M.KROEGER		
112939	1771	Hc2(0) at 4.2 K. RRR = 59.7	Nb1-xYx	Nb0.999Y0.001	Nb	0.999	Y	0.001																					1975																																														K		9.27					9.27																				kOe		2.91																																																																										ANN(1500C)					The effect of yttrium or gadorinium on the superconducting transition temperature of niobium				J.LESS-COMMON.MET.,40(1975)29	C.C.KOCH,D.M.KROEGER		
112940	1771	Hc2(0) at 4.2 K. RRR = 67.6	Nb1-xYx	Nb0.98Y0.02	Nb	0.98	Y	0.02																					1975																																														K		9.26					9.26																				kOe		3.01																																																																										ANN(1500C)					The effect of yttrium or gadorinium on the superconducting transition temperature of niobium				J.LESS-COMMON.MET.,40(1975)29	C.C.KOCH,D.M.KROEGER		
112941	1771	Hc2(0) at 4.2 K. RRR = 78.4	Nb1-xGdx	Gd0.001Nb0.999	Gd	0.001	Nb	0.999																					1975																																														K		9.18					9.18																				kOe		2.95																																																																										ANN(1500C)					The effect of yttrium or gadorinium on the superconducting transition temperature of niobium				J.LESS-COMMON.MET.,40(1975)29	C.C.KOCH,D.M.KROEGER		
112942	1771	Hc2(0) at 4.2 K. RRR = 71.3	Nb1-xGdx	Gd0.01Nb0.99	Gd	0.01	Nb	0.99																					1975																																														K		9.19					9.19																				kOe		2.93																																																																										ANN(1500C)					The effect of yttrium or gadorinium on the superconducting transition temperature of niobium				J.LESS-COMMON.MET.,40(1975)29	C.C.KOCH,D.M.KROEGER		
112943	786	P-induced SC. SC observed for 170 < P < 26 kbar. Tc and Hc2(0) at P = 170 kbar.	P	P1	P	1																							1968																																														K		5.8					5.8																				kOe		4.8																																																																															Superconductivity of phosphorus at high pressure				JETP Lett., 7(1968)323	I.V.BERMAN,N.B.BRANDT		
112944	1450		TiOx	O0.95Ti1	O	0.95	Ti	1																					1972																																														K		0.8					0.8																													kOe/K		3.7																									mj/mol.K2	0.89																																												Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
112945	1450		TiOx	O1Ti1	O	1	Ti	1																					1972																																														K		0.64					0.64																													kOe/K		3.4																									mj/mol.K2	0.6																																												Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
112946	1450		TiOx	O1.06Ti1	O	1.06	Ti	1																					1972																																														K		0.54					0.54																													kOe/K		4.4																									mj/mol.K2	0.52																																												Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
112947	1450		TiOx	O1.07Ti1	O	1.07	Ti	1																					1972																																														K		1					1																																																																																																					Superconductivity in the TiO and NbO systems				J.LOW TEMP.PHYS.,7(1972)291	C.K.JONES,J.K.HULM,J.W.GIBSON,R.A.HEIN		
112948	356	G-L parameter = 0.92	Pb1-xTlx	Pb0.975Tl0.025	Pb	0.975	Tl	0.025																					1962																																														K																		Oe		470							Oe		700																																																																															Observation du comportement magnetique quasi reversible d'un supraconducteur de deuxieme espece				PHYS.LETT.,2(1962)321	A.LACAZE,B.B.GOODMAN,G.BON MARDION		
112949	356	G-L parameter = 1.35	Pb1-xTlx	Pb0.95Tl0.05	Pb	0.95	Tl	0.05																					1962																																														K																		Oe		385							Oe		1060																																																																															Observation du comportement magnetique quasi reversible d'un supraconducteur de deuxieme espece				PHYS.LETT.,2(1962)321	A.LACAZE,B.B.GOODMAN,G.BON MARDION		
112950	356	G-L parameter = 2.25	Pb1-xTlx	Pb0.9Tl0.1	Pb	0.9	Tl	0.1																					1962																																														K																		Oe		270							Oe		1685																																																																															Observation du comportement magnetique quasi reversible d'un supraconducteur de deuxieme espece				PHYS.LETT.,2(1962)321	A.LACAZE,B.B.GOODMAN,G.BON MARDION		
112951	356	G-L parameter = 5.2	Pb1-xTlx	Pb0.75Tl0.25	Pb	0.75	Tl	0.25																					1962																																														K																		Oe		155							Oe		2880																																																																															Observation du comportement magnetique quasi reversible d'un supraconducteur de deuxieme espece				PHYS.LETT.,2(1962)321	A.LACAZE,B.B.GOODMAN,G.BON MARDION		
112952	356	G-L parameter = 8	Pb1-xTlx	Pb0.5Tl0.5	Pb	0.5	Tl	0.5																					1962																																														K																		Oe		60							Oe		2100																																																																															Observation du comportement magnetique quasi reversible d'un supraconducteur de deuxieme espece				PHYS.LETT.,2(1962)321	A.LACAZE,B.B.GOODMAN,G.BON MARDION		
112953	928		Nb	Nb1	Nb	1																							1969																																													bcc	K		9.23					9.23																				kOe		4.2																																		mj/mol.K2	7.8		280																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112954	928		Nb1-xTax	Nb0.98Ta0.02	Nb	0.98	Ta	0.02																					1969																																													bcc	K		9.02					9.02																				kOe		5.08																																		mj/mol.K2	7.98		279																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112955	928		Nb1-xTax	Nb0.96Ta0.04	Nb	0.96	Ta	0.04																					1969																																													bcc	K		8.87					8.87																				kOe		6.14																																		mj/mol.K2	7.98		272																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112956	928		Nb1-xTax	Nb0.94Ta0.06	Nb	0.94	Ta	0.06																					1969																																													bcc	K		8.76					8.76																				kOe		6.15																																		mj/mol.K2	7.95		270																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112957	928		Nb1-xTax	Nb0.9Ta0.1	Nb	0.9	Ta	0.1																					1969																																													bcc	K		8.4					8.4																				kOe		7.7																																		mj/mol.K2	7.85		271																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112958	928		Nb1-xTax	Nb0.85Ta0.15	Nb	0.85	Ta	0.15																					1969																																													bcc	K		8.08					8.08																				kOe		8.5																																		mj/mol.K2	7.35		260																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112959	928		Nb1-xTax	Nb0.7Ta0.3	Nb	0.7	Ta	0.3																					1969																																													bcc	K		7.17					7.17																				kOe		9.2																																		mj/mol.K2	6.95		259																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112960	928		Nb1-xTax	Nb0.6Ta0.4	Nb	0.6	Ta	0.4																					1969																																													bcc	K		6.56					6.56																				kOe																																				mj/mol.K2	6.7		260																																										The normal state specific heat of niobium-tantalum alloys				PHYS.LETT.A29(1969)284	T.MATSUI,T.MIZUSAKI,T.OHTSUKA,Y.KIMURA		
112961	427	c/a = 0.416	WBe13	Be13W1	Be	13	W	1																					1962																															A	10.14													tetragonal	K		4.1					4.1																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112962	427	c/a = 10633	ZrRe2	Re2Zr1	Re	2	Zr	1																					1962																												MgZn2(Laves)			A	5.262													MgZn2, C14	K		5.9					5.9																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112963	427		Zr5Re24	Re24Zr5	Re	24	Zr	5																					1962																																														K		3					3																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112964	427		Ga7Pt3	Ga7Pt3	Ga	7	Pt	3																					1962																												CaF2																		K		2.9					2.9																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112965	427		GaPt	Ga1Pt1	Ga	1	Pt	1																					1962																												FeS			A	4.91														K		1.74					1.74																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112966	427		AlGe2	Al1Ge2	Al	1	Ge	2																					1962																																														K		1.75					1.75																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112967	427		Al2CaSi	Al2Ca1Si1	Al	2	Ca	1	Si	1																			1962																																														K		5.8					5.8																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112968	427		AlPdMo6	Al1Pd1Mo6	Al	1	Pd	1	Mo	6																			1962																																														K		2.1					2.1																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112969	427		Nb3(Sn,Ge)	Nb3Sn0.5Ge0.5	Nb	3	Sn	0.5	Ge	0.5																			1962																																														K		11.3					11.3																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112970	427		Nb3(Sn,Zr)	Nb3Sn0.5Zr0.5	Nb	3	Sn	0.5	Zr	0.5																			1962																																														K		16.7					16.7																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112971	427		Nb3(Zr,In)	Nb3Zr0.5In0.5	Nb	3	Zr	0.5	In	0.5																			1962																																														K		6.4					6.4																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112972	427		Nb5Zr2Be8	Nb5Zr2Be8	Nb	5	Zr	2	Be	8																			1962																																														K		5.2					5.2																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112973	427		Nb4.4Re	Nb4.4Re1	Nb	4.4	Re	1																					1962																																														K		4.8					4.8																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112974	427		NbMg2	Mg2Nb1	Mg	2	Nb	1																					1962																																														K		5.6					5.6																																																																																																					Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112975	427		AgTe	Ag1Te1	Ag	1	Te	1																					1962																																														K					1.34																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112976	427		Al5Y2	Al5Y2	Al	5	Y	2																					1962																																														K					1.55																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112977	427		Al4Ca	Al4Ca1	Al	4	Ca	1																					1962																															A	4.36		11.09												K					1.7																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112978	427		Al2Ca	Al2Ca1	Al	2	Ca	1																					1962																												MgCu2(Laves)			A	8.038													MgCu2, C15	K					1.7																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112979	427		As2Pd3	As2Pd3	As	2	Pd	3																					1962																																														K					1.4																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112980	427		AsW	As1W1	As	1	W	1																					1962																																														K					1.4																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112981	427		AsZn	As1Zn1	As	1	Zn	1																					1962																																														K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112982	427		AuSb2	Au1Sb2	Au	1	Sb	2																					1962																															A	6.657														K					1.4																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112983	427		AuTe2	Au1Te2	Au	1	Te	2																					1962																																														K					1.34																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112984	427		BeCr2	Be1Cr2	Be	1	Cr	2																					1962																												MgZn2(Laves)			A	4.27		6.94											MgZn2, C14	K					1.75																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112985	427		Be2Mo	Be2Mo1	Be	2	Mo	1																					1962																												MgZn2(Laves)																	MgZn2, C14	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112986	427		Be2Re	Be2Re1	Be	2	Re	1																					1962																												MgZn2(Laves)			A	4.354		7.101											MgZn2, C14	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112987	427		Be2W	Be2W1	Be	2	W	1																					1962																												MgZn2(Laves)			A	4.446		7.289											MgZn2, C14	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112988	427		Be2Zr	Be2Zr1	Be	2	Zr	1																					1962																												AlB2			A	3.82		3.24											AlB2, C32	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112989	427		Be13Mo	Be13Mo1	Be	13	Mo	1																					1962																															A	7.271		4.234												K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112990	427		Be13Zr	Be13Zr1	Be	13	Zr	1																					1962																												NaZn13			A	10.047														K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112991	427		Ca3Ge	Ca3Ge1	Ca	3	Ge	1																					1962																																														K					0.15																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112992	427		Ca2Si	Ca2Si1	Ca	2	Si	1																					1962																															A	4.743														K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112993	427		CaSi	Ca1Si1	Ca	1	Si	1																					1962																															A	3.91	4.59	10.795												K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112994	427		CaSi2	Ca1Si2	Ca	1	Si	2																					1962																												CaSi2			A	10.4													CaSi2, C12	K					1.68																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112995	427		FeSb2	Fe1Sb2	Fe	1	Sb	2																					1962																															A	3.195	5.831	6.53												K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112996	427		Ge2Pd	Ge2Pd1	Ge	2	Pd	1																					1962																																														K					1.47																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112997	427		K2Te3	K2Te3	K	2	Te	3																					1962																																														K					1.46																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112998	427		NaTe	Na1Te1	Na	1	Te	1																					1962																																														K					1.3																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
112999	427		Na3Sb	Na3Sb1	Na	3	Sb	1																					1962																															A	5.366		9.515												K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
113000	427		NiSb3	Ni1Sb3	Ni	1	Sb	3																					1962																																														K					1.45																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
113001	427		NiP	Ni1P1	Ni	1	P	1																					1962																																														K					1.57																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
113002	427		Ga3Zr	Ga3Zr1	Ga	3	Zr	1																					1962																																														K					1.38																																																																																																							Superconductivity of some binary and ternary alloys				JETP  16(1963)1493	N.E.ALEKSEEVSKII,N.N.MIKHAILOV		
113003	1707	hardness = 370   kg/mm2	Zr-V	V66.6Zr33.3	V	66.6	Zr	33.3																					1968																															A	7.435													gamma	K		9.64					9.64																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113004	1707	hardness = 395   kg/mm2	Zr-V-Nb	Zr33.3V61.8Nb4.8	Zr	33.3	V	61.8	Nb	4.8																			1968																															A	7.437													gamma	K		6.13					6.13																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113005	1707	hardness =  440  kg/mm2	Zr-V-Nb	Zr33.3V59.25Nb7.35	Zr	33.3	V	59.25	Nb	7.35																			1968																															A	7.449													gamma	K		6.3					6.3																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113006	1707	hardness =  450  kg/mm2	Zr-V-Nb	Zr33.3V56.7Nb9.9	Zr	33.3	V	56.7	Nb	9.9																			1968																															A	7.464													gamma	K		5.34					5.34																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113007	1707	hardness =  475  kg/mm2	Zr-V-Nb	Zr33.3V53.95Nb12.05	Zr	33.3	V	53.95	Nb	12.05																			1968																															A	5.27		8.68												K																																																																																																												Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113008	1707	hardness =  503  kg/mm2	Zr-V-Nb	Zr33.3V51.2Nb15.4	Zr	33.3	V	51.2	Nb	15.4																			1968																															A	5.27		8.64											delta	K																																																																																																												Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113009	1707		Zr-V-Nb	Zr33.3V48Nb18.27	Zr	33.3	V	48	Nb	18.27																			1968																															A	5.28		8.66											delta	K																																																																																																												Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113010	1707	hardness =  545  kg/mm2	Zr-V-Nb	Zr33.3V45.5Nb21.12	Zr	33.3	V	45.5	Nb	21.12																			1968																																													delta	K		4.36					4.36																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113011	1707	hardness =  500  kg/mm2	Zr-V-Nb	Zr33.3V39.3Nb27.4	Zr	33.3	V	39.3	Nb	27.4																			1968																																														K		5.45					5.45																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113012	1707	hardness =  465  kg/mm2	Zr-V-Nb	Zr33.3V35.9Nb30.7	Zr	33.3	V	35.9	Nb	30.7																			1968																																														K																																																																																																												Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113013	1707	hardness =  440  kg/mm2	Zr-V-Nb	Zr32.2V64.3Nb3.53	Zr	32.2	V	64.3	Nb	3.53																			1968																															A	7.435													gamma	K																																																																																																												Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113014	1707	hardness =  464  kg/mm2	Zr-V-Nb	Zr31V61.8Nb7.2	Zr	31	V	61.8	Nb	7.2																			1968																															A	7.435													gamma	K		9.65					9.65																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113015	1707	hardness =  514  kg/mm2	Zr-V-Nb	Zr29.8V59.4Nb10.8	Zr	29.8	V	59.4	Nb	10.8																			1968																															A	7.432													gamma	K		9.58					9.58																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113016	1707	hardness =  542  kg/mm2	Zr-V-Nb	Zr28.4V56.8Nb14.8	Zr	28.4	V	56.8	Nb	14.8																			1968																															A	7.433													gamma	K		8.56					8.56																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113017	1707	hardness =  548  kg/mm2	Zr-V-Nb	Zr27.1V54.1Nb18.8	Zr	27.1	V	54.1	Nb	18.8																			1968																															A	5.258		8.585												K		4.46					4.46																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113018	1707	hardness =  542  kg/mm2	Zr-V-Nb	Zr25.8V51.3Nb22.9	Zr	25.8	V	51.3	Nb	22.9																			1968																																														K		4.34					4.34																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113019	1707	hardness =  490  kg/mm2	Zr-V-Nb	Zr24.3V48.5Nb27.2	Zr	24.3	V	48.5	Nb	27.2																			1968																																														K		4.6					4.6																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113020	1707	hardness =  421  kg/mm2	Zr-V-Nb	Zr23V45.5Nb31.5	Zr	23	V	45.5	Nb	31.5																			1968																																														K		5.42					5.42																																																																																																					Influence of niobium on the superconducting properties of alloys on a base of the compound ZrV2				Soviet Physics - Doklady 13(1968)162	L.N.GUSEVA,N.E.ALEKSEEVSKII,N.M.MATVEEVA		
113021	1472	homogeneity range  0.8 < x < 1.30	TiOx	O0.92Ti1	O	0.92	Ti	1																					1972																																														K		0.72					0.72	MTC13021																																																																																															ANN(1500C)					"Superconductivity in cubic and monoclinic ""TiO"""				J.APPL.PHYS.,43(1972)2478	M.D.BANUS,M.SJOSTRAND,P.H.DEESOM,T.B.REED		
113022	1472		TiOx	O0.86Ti1	O	0.86	Ti	1																					1972																																														K		0.47					0.47																																																																																																ANN(60 kbar, 1300C)					"Superconductivity in cubic and monoclinic ""TiO"""				J.APPL.PHYS.,43(1972)2478	M.D.BANUS,M.SJOSTRAND,P.H.DEESOM,T.B.REED		
113023	1472		TiOx	O0.91Ti1	O	0.91	Ti	1																					1972																																														K		0.7					0.7																																																																																																ANN(60 kbar, 1300C)					"Superconductivity in cubic and monoclinic ""TiO"""				J.APPL.PHYS.,43(1972)2478	M.D.BANUS,M.SJOSTRAND,P.H.DEESOM,T.B.REED		
113024	1133	Tc calculated from Tc(Pb) = 7.20 K (not shown)	Pb1-xSbx	Pb0.95Sb0.05	Pb	0.95	Sb	0.05																					1966																																														K		7.83					7.83	MTC13024																																																																																																				Superconducting transition temperatures of lead alloys				J.PHYS.SOC.JAPAN,21(1966)1617	M.MITANI,M.SATO,N.KUMASAKA		
113025	1133	Tc calculated from Tc(Pb) = 7.20 K (not shown)	Pb1-xBix	Bi0.05Pb0.95	Bi	0.05	Pb	0.95																					1966																																														K		7.388					7.388	MTC13024																																																																																																				Superconducting transition temperatures of lead alloys				J.PHYS.SOC.JAPAN,21(1966)1617	M.MITANI,M.SATO,N.KUMASAKA		
113026	1133	Tc calculated from Tc(Pb) = 7.20 K (not shown)	Pb1-xSnx	Pb0.95Sn0.05	Pb	0.95	Sn	0.05																					1966																																														K		7.268					7.268	MTC13024																																																																																																				Superconducting transition temperatures of lead alloys				J.PHYS.SOC.JAPAN,21(1966)1617	M.MITANI,M.SATO,N.KUMASAKA		
113027	1133	Tc calculated from Tc(Pb) = 7.20 K (not shown)	Pb1-xInx	In0.05Pb0.95	In	0.05	Pb	0.95																					1966																																														K		7.091					7.091	MTC13024																																																																																																				Superconducting transition temperatures of lead alloys				J.PHYS.SOC.JAPAN,21(1966)1617	M.MITANI,M.SATO,N.KUMASAKA		
113028	1133	Tc calculated from Tc(Pb) = 7.20 K (not shown)	Pb1-xTlx	Pb0.95Tl0.05	Pb	0.95	Tl	0.05																					1966																																														K		7.055					7.055	MTC13024																																																																																																				Superconducting transition temperatures of lead alloys				J.PHYS.SOC.JAPAN,21(1966)1617	M.MITANI,M.SATO,N.KUMASAKA		
113029	736	small dip of Tc in the vicinity of Pb0.5Tl0.5	Pb1-xTlx	Pb0.4Tl0.6	Pb	0.4	Tl	0.6																					1966																																														K		4.67					4.67	MTC13029																																																																																																				Superconductivity and electronic structure in the alloy system lead-thallium				PHYS.REV.,147(1966)340	T.CLAESON		
113030	1296		Pd1-xSbx	Pd0.52Sb0.48	Pd	0.52	Sb	0.48																					1968																															A	4.077	5.587													K		1.65					1.65																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113031	1296		Pd1-xSbx	Pd0.51Sb0.49	Pd	0.51	Sb	0.49																					1968																															A	4.078	5.592													K		1.67					1.67																																																								mj/mol.K2	1.42		229																																										3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113032	1296		Pd1-xSbx	Pd0.5Sb0.5	Pd	0.5	Sb	0.5																					1968																															A	4.076	5.586													K		1.48					1.48																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113033	1296		Pd1-xSbx	Pd0.49Sb0.51	Pd	0.49	Sb	0.51																					1968																															A	4.07	5.579													K		1.44					1.44																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113034	1296		(Pd,Ti)1-xSbx	Pd50.745Ti0.255Sb49	Pd	50.745	Ti	0.255	Sb	49																			1968																																														K		1.61					1.61																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113035	1296		(Pd,V)1-xSbx	Pd49.75V0.25Sb50	Pd	49.75	V	0.25	Sb	50																			1968																																														K		1.13					1.13																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113036	1296		(Pd,V)1-xSbx	Pd50.745V0.255Sb49	Pd	50.745	V	0.255	Sb	49																			1968																																														K		0.91					0.91																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113037	1296		(Pd,Sc)1-xSbx	Pd50.745Sc0.255Sb49	Pd	50.745	Sc	0.255	Sb	49																			1968																																														K		1.56					1.56																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113038	1296		(Pd,V)1-xSbx	Pd50.49V0.51Sb49	Pd	50.49	V	0.51	Sb	49																			1968																																														K		0.5					0.5																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113039	1296		(Pd,Cr)1-xSbx	Pd50.99745Cr0.00255Sb49	Pd	50.99745	Cr	0.00255	Sb	49																			1968																																														K		1.35					1.35	MTC13039																																																																																																				3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113040	1296		(Pd,Mn)1-xSbx	Pd50.9745Mn0.0255Sb49	Pd	50.9745	Mn	0.0255	Sb	49																			1968																																														K		1.46					1.46	MTC13040																																																																																																				3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113041	1296		(Pd,Fe)1-xSbx	Pd50.93625Fe0.06375Sb49	Pd	50.93625	Fe	0.06375	Sb	49																			1968																																														K		1.22					1.22																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113042	1296		(Pd,Fe)1-xSbx	Pd50.8725Fe0.1275Sb49	Pd	50.8725	Fe	0.1275	Sb	49																			1968																																														K		1.03					1.03																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113043	1296		(Pd,Co)1-xSbx	Pd49.75Co0.25Sb50	Pd	49.75	Co	0.25	Sb	50																			1968																																														K		1.57					1.57																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113044	1296		(Pd,Ni)1-xSbx	Pd49.75Ni0.25Sb50	Pd	49.75	Ni	0.25	Sb	50																			1968																																														K		1.5					1.5																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113045	1296		(Pd,Ni)1-xSbx	Pd45.9Ni5.1Sb49	Pd	45.9	Ni	5.1	Sb	49																			1968																																														K		1.23					1.23																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113046	1296		(Pd,Cu)1-xSbx	Pd49.75Cu0.25Sb50	Pd	49.75	Cu	0.25	Sb	50																			1968																																														K		1.56					1.56																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113047	1296		(Pd,Nb)1-xSbx	Pd50.745Nb0.255Sb49	Pd	50.745	Nb	0.255	Sb	49																			1968																																														K		1.6					1.6																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113048	1296		(Pd,Mo)1-xSbx	Pd50.745Mo0.255Sb49	Pd	50.745	Mo	0.255	Sb	49																			1968																																														K		1.67					1.67																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113049	1296		(Pd,Ru)1-xSbx	Pd50.745Ru0.255Sb49	Pd	50.745	Ru	0.255	Sb	49																			1968																																														K		1.57					1.57																																																																																																					3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113050	1296		Cd	Cd1	Cd	1																							1968																																														K		0.55					0.55																																																								mj/mol.K2	0.711		300																																										3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113051	1296		PdSb	Pd1Sb1	Pd	1	Sb	1																					1968																																														K		1.66					1.66																																																								mj/mol.K2	1.42		229																																										3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113052	1296		In	In1	In	1																							1968																																														K		3.4					3.4																																																								mj/mol.K2	1.82		109																																										3d elements in superconducting PdSb				PHYS.REV.,169(1968)457	B.CAROLI,B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,J.P.MAITA,T.H.GEBALLE		
113053	952		Re	Re1	Re	1																							1968																																														K		1.7					1.7			K/GPa	-0.023																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113054	952		Re1-xOsx	Os0.001Re0.999	Os	0.001	Re	0.999																					1968																																														K		1.71					1.71			K/GPa	-0.0092																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113055	952		Re1-xOsx	Os0.002Re0.998	Os	0.002	Re	0.998																					1968																																														K		1.71					1.71			K/GPa	-0.0001																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113056	952		Re1-xOsx	Os0.006Re0.994	Os	0.006	Re	0.994																					1968																																														K		1.76					1.76			K/GPa	-0.014																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113057	952		Re1-xOsx	Os0.0275Re0.9725	Os	0.0275	Re	0.9725																					1968																																														K		1.84					1.84			K/GPa	-0.0253																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113058	952		Re1-xOsx	Os0.046Re0.954	Os	0.046	Re	0.954																					1968																																														K		1.92					1.92			K/GPa	-0.0274																																																																																																	Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113059	952		Re1-xOsx	Os0.065Re0.935	Os	0.065	Re	0.935																					1968																																														K		1.92					1.92																																																																																																					Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113060	952		Re1-xOsx	Os0.084Re0.916	Os	0.084	Re	0.916																					1968																																														K		1.88					1.88																																																																																																					Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113061	952		Re1-xOsx	Os0.113Re0.887	Os	0.113	Re	0.887																					1968																																														K		1.79					1.79																																																																																																					Superconductivity of rhenium and some rhenium-osmium alloys at high pressure				PHYS.REV.LETT.,20(1968)198	C.W.CHU,T.F.SMITH,W.E.GARDNER		
113062	P070214526	bulk moduluc = 78.4  GPa. c/a = 1.621 . initial compressibility  = 3.96 E-3/GPa for a-axis,  4.22 E-3/GPa for c-axis. Specific heat measurements.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2004																												HoCoGa5																		K		2.2			0		2.2																																																																																																self-flux method					Compressibility of CeMIn5 and Ce2MIn8 (M=Rh, Ir, and Co) compounds		M-13062	Department of Physics, University of Nevada, Las Vegas, Nevada 89154-4002, USA	Phys.Rev.B, 70(2004)214526	A.L.Comelius,J.L.Sarrao,R.S.Kumar		
113063	P070214526	bulk moduluc = 87.6 GPa. c/a = 1.612 . initial compressibility  = 3.44 E-3/GPafor a-axis,   3.48 E-3 /GPa for c-axis. Specific heat measurements.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2004																																														K		0.4					0.4																																																																																																self-flux method					Compressibility of CeMIn5 and Ce2MIn8 (M=Rh, Ir, and Co) compounds		M-13062	Department of Physics, University of Nevada, Las Vegas, Nevada 89154-4002, USA	Phys.Rev.B, 70(2004)214526	A.L.Comelius,J.L.Sarrao,R.S.Kumar		
113064	P070214526	bulk moduluc = 78.2 GPa. c/a = 1.638 . initial compressibility  = 4.35 E-3/GPafor a-axis,   3.43 E-3 /GPa for c-axis. Specific heat measurements.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2004																																														K		2.3					2.3																																																																																																self-flux method					Compressibility of CeMIn5 and Ce2MIn8 (M=Rh, Ir, and Co) compounds		M-13062	Department of Physics, University of Nevada, Las Vegas, Nevada 89154-4002, USA	Phys.Rev.B, 70(2004)214526	A.L.Comelius,J.L.Sarrao,R.S.Kumar		
113065	P070214526	bulk moduluc = 71.4 GPa. c/a = 2.624 . initial compressibility  = 4.20 E-3/GPafor a-axis,   4.85 E-3 /GPa for c-axis. Specific heat measurements.	Ce2RhIn8	Ce2Rh1In8	Ce	2	Rh	1	In	8																		3	2004																												Ho2CoGa8																		K		2			0		2																																																																																																self-flux method					Compressibility of CeMIn5 and Ce2MIn8 (M=Rh, Ir, and Co) compounds		M-13062	Department of Physics, University of Nevada, Las Vegas, Nevada 89154-4002, USA	Phys.Rev.B, 70(2004)214526	A.L.Comelius,J.L.Sarrao,R.S.Kumar		
113066	P070214526	bulk moduluc = 69.4 GPa. c/a = 2.610 . initial compressibility  = 4.02 E-3/GPafor a-axis,   4.93 E-3 /GPa for c-axis. Specific heat measurements.	Ce2IrIn8	Ce2Ir1In8	Ce	2	Ir	1	In	8																		3	2004																																														K					0.05																																																																																																		self-flux method					Compressibility of CeMIn5 and Ce2MIn8 (M=Rh, Ir, and Co) compounds		M-13062	Department of Physics, University of Nevada, Las Vegas, Nevada 89154-4002, USA	Phys.Rev.B, 70(2004)214526	A.L.Comelius,J.L.Sarrao,R.S.Kumar		
113067	713	Hc2(0) shows Hc(0) because 1st kind SC. (delta-C/gamma*Tc) = 1.60  . e-ph coupling const. = 0.62. Specific heat measurements.	Ta	Ta1	Ta	1																							1970																																													bcc	K		4.463					4.463																				Oe		831																										3.59	11							mj/mol.K2	6.15		250																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113068	713	Hc2(0) shows Hc(0) because 1st kind SC. (delta-C/gamma*Tc) = 1.46  . e-ph coupling const. = 0.56. Specific heat measurements.	Ta1-xRex	Re0.025Ta0.975	Re	0.025	Ta	0.975																					1970																																													bcc	K		3.458					3.458																				Oe		613																										3.54	11							mj/mol.K2	5.7		261																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113069	713	Hc2(0) shows Hc(0) because 1st kind SC. (delta-C/gamma*Tc) = 1.48  . e-ph coupling const. = 0.52. Specific heat measurements.	Ta1-xRex	Re0.05Ta0.95	Re	0.05	Ta	0.95																					1970																																													bcc	K		2.77					2.77																				Oe		460																										3.48	11							mj/mol.K2	5.12		277																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113070	713	Hc2(0) shows Hc(0) because 1st kind SC. (delta-C/gamma*Tc) = 1.40  . e-ph coupling const. =0.48. Specific heat measurements.	Ta1-xRex	Re0.075Ta0.925	Re	0.075	Ta	0.925																					1970																																													bcc	K		2.08					2.08																				Oe		342																										3.47	11							mj/mol.K2	5.05		285																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113071	713	Hc2(0) shows Hc(0) because 1st kind SC. (delta-C/gamma*Tc) = 1.40  . e-ph coupling const. = 0.45. Specific heat measurements.	Ta1-xRex	Re0.1Ta0.9	Re	0.1	Ta	0.9																					1970																																													bcc	K		1.49					1.49																				Oe		232																										3.4	11							mj/mol.K2	4.1		296																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113072	713	Hc2(0) shows Hc(0) because 1st kind SC.  e-ph coupling const. = 0.39. Specific heat measurements.	Ta1-xRex	Re0.15Ta0.85	Re	0.15	Ta	0.85																					1970																																													bcc	K		0.75					0.75																																																								mj/mol.K2	3.75		307																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113073	713	e-ph coupling const. = 0.34. Specific heat measurements.	Ta1-xRex	Re0.2Ta0.8	Re	0.2	Ta	0.8																					1970																																													bcc	K		0.21					0.21																																																								mj/mol.K2	3		317																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113074	713	e-ph coupling const. = (0.29). Specific heat measurements.	Ta1-xRex	Re0.25Ta0.75	Re	0.25	Ta	0.75																					1970																																													bcc	K					0.06																																																										mj/mol.K2	2.42		330																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113075	713	e-ph coupling const. = (0.23). Specific heat measurements.	Ta1-xRex	Re0.3Ta0.7	Re	0.3	Ta	0.7																					1970																																													bcc	K					0.06																																																										mj/mol.K2	1.9		345																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113076	713	e-ph coupling const. = (0.13). Specific heat measurements.	Ta1-xRex	Re0.4Ta0.6	Re	0.4	Ta	0.6																					1970																																													bcc	K					0.06																																																										mj/mol.K2	1		361																																					electron beam melting in VAC					Superconductivity of tantalum-rhenium alloys				J.PHYS.SOC.JAPAN,28(1970)380	K.NOMURA,T.MAMIYA,Y.MASUDA		
113077	P070212514	used C<12>. isotope effect (alpha) calculated from num=13078 data.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2004																															A	3.8109														K		7.12					7.12						0.54	C		0.3																																																																																							final heat treatment(900C)					Carbon isotope effect in superconducting MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey, USA	Phys.Rev.B, 70(2004)212514	R.J.Cava,T.Klimczuk		
113078	P070212514	used C<13>. see num = 13077 data.	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		1	2004																															A	3.8116														K		6.8					6.8																																																																																																final heat treatment(900C)					Carbon isotope effect in superconducting MgCNi3			Department of Chemistry, Princeton University, Princeton, New Jersey, USA	Phys.Rev.B, 70(2004)212514	R.J.Cava,T.Klimczuk		
113079	709	Tc vs carrier concentration	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1	O	3																			1967																																														K								MTC13071																																																																																																								PHYS.REV.,163(1967)380	C.S.KOONCE,E.R.PFEIFFER,J.F.SCHOOLEY,M.L.COHEN,W.R.HOSLER		
113080	239		Os1-xIrx	Ir0.15Os0.85	Ir	0.15	Os	0.85																					1963																																													hcp	K		0.54					0.54	MTC13067																																																																																																				SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
113081	239		Os1-xIrx	Ir0.6Os0.4	Ir	0.6	Os	0.4																					1963																																													fcc	K		0.73					0.73																																																																																																					SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
113082	239		W1-xPtx	Pt0.035W0.965	Pt	0.035	W	0.965																					1963																																													bcc	K		1.98					1.98	MTC13069																																																																																																				SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
113083	239		W1-xPtx	Pt0.5W0.5	Pt	0.5	W	0.5																					1963																																													fcc	K		1.45					1.45																																																																																																					SUPERCONDUCTIVITY OF SOILD SOLUTIONS OF NOBEL METALS				PHYS.REV.,129(1963)182	B.T.MATTHIAS,E.CORENZWIT,G.W.HULL,JR.,T.H.GEBALLE,V.B.COMPTON		
113084	1109	Tc from sp-heat measurements.	Ti	Ti1	Ti	1																							1969																																														K		0.4					0.4																																																								mj/mol.K2	3.31																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113085	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.005Ti0.995	Rh	0.005	Ti	0.995																					1969																																														K		0.79					0.79																																																								mj/mol.K2	3.54																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113086	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.01Ti0.99	Rh	0.01	Ti	0.99																					1969																																														K		1.16					1.16																																																								mj/mol.K2	3.94																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113087	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.015Ti0.985	Rh	0.015	Ti	0.985																					1969																																														K		1.6					1.6																																																								mj/mol.K2	4.04																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113088	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.02Ti0.98	Rh	0.02	Ti	0.98																					1969																																														K		1.73					1.73																																																								mj/mol.K2	4.13																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113089	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.025Ti0.975	Rh	0.025	Ti	0.975																					1969																																														K		1.79					1.79																																																								mj/mol.K2	4.31																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113090	1109	Tc from sp-heat measurements.	Ti1-xRhx	Rh0.03Ti0.97	Rh	0.03	Ti	0.97																					1969																																														K		1.34					1.34																																																								mj/mol.K2	3.91																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113091	766		Ti1-xRhx	Rh0.005Ti0.995	Rh	0.005	Ti	0.995																					1963																												alpha-Ti																		K		1.8					1.8																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113092	766		Ti1-xRhx	Rh0.01Ti0.99	Rh	0.01	Ti	0.99																					1963																												alpha-Ti																		K		2.4					2.4																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113093	766		Ti1-xRhx	Rh0.02Ti0.98	Rh	0.02	Ti	0.98																					1963																												alpha-Ti																		K		3.2					3.2																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113094	766		Ti1-xRhx	Rh0.03Ti0.97	Rh	0.03	Ti	0.97																					1963																												alpha-Ti																		K		1.9					1.9																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113095	766		Ti1-xRhx	Rh0.04Ti0.96	Rh	0.04	Ti	0.96																					1963																												alpha-Ti																		K		2					2																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113096	766		Zr1-xRhx	Rh0.005Zr0.995	Rh	0.005	Zr	0.995																					1963																												alpha-Zr																		K		3.5					3.5																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113097	766		Zr1-xRhx	Rh0.01Zr0.99	Rh	0.01	Zr	0.99																					1963																												alpha-Zr																		K		4.5					4.5																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113098	766		Zr1-xRhx	Rh0.02Zr0.98	Rh	0.02	Zr	0.98																					1963																												alpha-Zr																		K		4.8					4.8																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113099	766		Zr1-xRhx	Rh0.027Zr0.973	Rh	0.027	Zr	0.973																					1963																												alpha-Zr																		K		3.6					3.6																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113100	766		Zr1-xRhx	Rh0.035Zr0.965	Rh	0.035	Zr	0.965																					1963																												alpha-Zr			A	3.568														K		5					5																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113101	766		Zr1-xRhx	Rh0.04Zr0.96	Rh	0.04	Zr	0.96																					1963																												alpha-Zr			A	3.568														K		5					5																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113102	766		Zr1-xRhx	Rh0.05Zr0.95	Rh	0.05	Zr	0.95																					1963																												alpha-Zr			A	3.565														K		5.2					5.2																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113103	766		Zr1-xRhx	Rh0.06Zr0.94	Rh	0.06	Zr	0.94																					1963																															A	3.555														K		5.9					5.9																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113104	766		Zr1-xRhx	Rh0.065Zr0.935	Rh	0.065	Zr	0.935																					1963																															A	3.555														K		5.9					5.9																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113105	766		Zr1-xRhx	Rh0.075Zr0.925	Rh	0.075	Zr	0.925																					1963																															A	3.538														K		6.4					6.4																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113106	766		Zr1-xRhx	Rh0.08Zr0.92	Rh	0.08	Zr	0.92																					1963																															A	3.54														K		9.6					9.6																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113107	766		Zr1-xRhx	Rh0.09Zr0.91	Rh	0.09	Zr	0.91																					1963																															A	3.542														K		10.1					10.1																																																																																																					Uber die Supraleitfahigkeit von Ti- und Zr-Rh-Legierungen				Z.PHYS.,175(1963)105	C.A.ANDERSON,CH.J.RAUB		
113108	1002	e-ph coupling const = 0.66	Ti3Sb	Sb1Ti3	Sb	1	Ti	3																					1970																												Cr3Si(A15)			A	5.225													Cr3Si, A15	K		5.3					5.3																																																								mj/mol.K2	7.85		282																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113109	1002	e-ph coupling const = 0.50	(Ti,Nb)3Sb	Ti0.5Nb0.25Sb0.25	Ti	0.5	Nb	0.25	Sb	0.25																			1970																												Cr3Si(A15)			A	5.24													Cr3Si, A15	K		1.95					1.95																																																								mj/mol.K2	4.85		325																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113110	1002	e-ph coupling const = 0.55	(Ti,Nb)3Sb	Ti0.25Nb0.5Sb0.25	Ti	0.25	Nb	0.5	Sb	0.25																			1970																												Cr3Si(A15)			A	5.253													Cr3Si, A15	K		3.05					3.05																																																								mj/mol.K2	4.3		330																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113111	1002	e-ph coupling const = 0.42	V3Sb	Sb1V3	Sb	1	V	3																					1970																												Cr3Si(A15)			A	4.945													Cr3Si, A15	K		0.5					0.5																																																								mj/mol.K2	2.5		400																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113112	1002	e-ph coupling const = 0.38	Ti	Ti1	Ti	1																							1970																																														K		0.39					0.39																																																								mj/mol.K2	3.32		425																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113113	1002	e-ph coupling const = 0.82	Nb	Nb1	Nb	1																							1970																																														K		9.4					9.4																																																								mj/mol.K2	7.8		277																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113114	1002	e-ph coupling const = 0.60	V	V1	V	1																							1970																																														K		5.3					5.3																																																								mj/mol.K2	9.9		399																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113115	1002		(Ti,V)3Sb	Ti1.38V1.62Sb1	Ti	1.38	V	1.62	Sb	1																			1970																															A	5.0331														K		1.49					1.49	MTC13115																																																																																																				Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113116	1002		(Ti,Nb)3Sb	Ti2.01Nb0.99Sb1	Ti	2.01	Nb	0.99	Sb	1																			1970																																														K		1.96					1.96	MTC13116																																																							mj/mol.K2	4.83		325																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113117	1002		(Ti,Nb)3Sb	Ti0.99Nb2.01Sb1	Ti	0.99	Nb	2.01	Sb	1																			1970																																														K		2.84					2.84																																																								mj/mol.K2	4.27		329																																										Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113118	1002		Ti1-xSbx	Sb0.25Ti0.75	Sb	0.25	Ti	0.75																					1970																																														K		5.32					5.32	MTC13118																																																																																																				Supraconductivite et chaleur specifique d'alliages bases sur Ti3Sb				HELVETIA PHYS.ACTA,43(1970)59	A.JUNOD,F.HEINIGER,J.MULLER,P.SPITZLI		
113119	552	(delta-C/gamma*Tc) = 1.8	PdTe	Pd1Te1	Pd	1	Te	1																					1965																																														K		4.36					4.36																																																								mj/mol.K2	5.66		277																																										The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
113120	552	(delta-C/gamma*Tc) = 1.2	PdTe1.04	Pd1Te1.04	Pd	1	Te	1.04																					1965																																														K		2.45					2.45																																																								mj/mol.K2	4.15		239																																										The occurrence of superconductivity in sulfides, selenides, tellurides of Pt-group metals				J.PHYS.CHEM.SOLIDS,26(1965)2051	B.T.MATTHIAS,C.J.RAUB,G.W.HULL JR.,T.H.GEBALLE,V.B.COMPTON		
113121	648		Zr1-xRhx	Rh0.01Zr0.99	Rh	0.01	Zr	0.99																					1965																																														K		4.26					4.26	MTC13121																																																																																															ANN(1000C,72h), then water quenched					Superconductivity in zirconium-rhodium alloys				J.PHYS.CHEM.SOLIDS,26(1965)1347	S.T.ZEGLER		
113122	648		Zr1-xRhx	Rh0.03Zr0.97	Rh	0.03	Zr	0.97																					1965																																														K		3.38					3.38	MTC13121																																																																																															ANN(1000C,72h), then water quenched					Superconductivity in zirconium-rhodium alloys				J.PHYS.CHEM.SOLIDS,26(1965)1347	S.T.ZEGLER		
113123	648		Zr1-xRhx	Rh0.06Zr0.94	Rh	0.06	Zr	0.94																					1965																																														K		5.95					5.95	MTC13121																																																																																															ANN(1000C,72h), then water quenched					Superconductivity in zirconium-rhodium alloys				J.PHYS.CHEM.SOLIDS,26(1965)1347	S.T.ZEGLER		
113124	648		Zr1-xRhx	Rh0.1Zr0.9	Rh	0.1	Zr	0.9																					1965																																														K		10.8					10.8	MTC13121																																																																																															ANN(1000C,72h), then water quenched					Superconductivity in zirconium-rhodium alloys				J.PHYS.CHEM.SOLIDS,26(1965)1347	S.T.ZEGLER		
113125	1757		V1-xRux	Ru0.42V0.58	Ru	0.42	V	0.58																					1974																																														K		2.12					2.12			K/GPa	-0.041																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113126	1757		V1-xRux	Ru0.43V0.57	Ru	0.43	V	0.57																					1974																																														K		2.92					2.92			K/GPa	-0.049																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113127	1757		V1-xRux	Ru0.445V0.555	Ru	0.445	V	0.555																					1974																																														K		3.48					3.48			K/GPa	-0.049																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113128	1757		V1-xRux	Ru0.46V0.54	Ru	0.46	V	0.54																					1974																																														K		5.67					5.67			K/GPa	0.2																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113129	1757		V1-xRux	Ru0.47V0.53	Ru	0.47	V	0.53																					1974																																														K		4.53					4.53			K/GPa	0.298																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113130	1757		V1-xRux	Ru0.475V0.525	Ru	0.475	V	0.525																					1974																																														K		3.12					3.12			K/GPa	0.164																																																																																												annealed sample					Superconductivity and stability of near equiatomic V-Ru compounds at high pressure				J.PHYS.F:METAL PHYS.,4(1974)1423	A.C.LAWSON,C.W.CHU,R.N.SHELTON,T.F.SMITH		
113131	846		Pd1-xWx	Pd0.56W0.44	Pd	0.56	W	0.44																					1968																															A	3.9215														K		1.58					1.58																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113132	846		Pd1-xWx	Pd0.6W0.4	Pd	0.6	W	0.4																					1968																															A	3.9179														K		1.29					1.29																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113133	846		Pd1-xWx	Pd0.72W0.28	Pd	0.72	W	0.28																					1968																															A	3.9027														K		0.345					0.345																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113134	846		Pt1-xWx	Pt0.73W0.27	Pt	0.73	W	0.27																					1968																															A	3.9221														K		0.213					0.213																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113135	846		Pt1-xWx	Pt0.52W0.48	Pt	0.52	W	0.48																					1968																															A	3.9367														K		1.35					1.35																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113136	846		Pt1-xWx	Pt0.33W0.67	Pt	0.33	W	0.67																					1968																															A	3.9606														K		3.02					3.02																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113137	846		Pt1-xWx	Pt0.43W0.57	Pt	0.43	W	0.57																					1968																															A	3.9465														K		2.09					2.09																																																																																																					Superconductivity and lattice parameters in face-centered cubic Pt-W and Pd-W solid solutions				J.LESS-COMMON METALS,15(1968)299	H.L.LUO		
113138	1061	sp-heat measured between 0.9 and 12 K.. not SC.	Zr1-xRhx	Zr1	Zr	1																							1965																																														K					0.9																																																										mj/mol.K2	2.77		289																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113139	1061	sp-heat measured between 0.9 and 12 K.. not SC.	Zr1-xRhx	Rh0.01Zr0.99	Rh	0.01	Zr	0.99																					1965																																														K					0.9																																																										mj/mol.K2	3.62		275																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113140	1061	sp-heat measured between 0.9 and 12 K.. not SC.	Zr1-xRhx	Rh0.015Zr0.985	Rh	0.015	Zr	0.985																					1965																																														K					0.9																																																										mj/mol.K2	3.83		273																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113141	1061	sp-heat measured between 0.9 and 12 K.. not SC.	Zr1-xRhx	Rh0.02Zr0.98	Rh	0.02	Zr	0.98																					1965																																														K					0.9																																																										mj/mol.K2	3.83		261																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113142	1061	sp-heat measured between 0.9 and 12 K.. not SC.	Zr1-xRhx	Rh0.025Zr0.975	Rh	0.025	Zr	0.975																					1965																																														K					0.9																																																										mj/mol.K2	4.12		262																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113143	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.03Zr0.97	Rh	0.03	Zr	0.97																					1965																																														K		3.1					3.1																																																								mj/mol.K2	3.62		244																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113144	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.0375Zr0.925	Rh	0.0375	Zr	0.925																					1965																																														K		3.65					3.65																																																								mj/mol.K2	3.95		244																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113145	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.04Zr0.96	Rh	0.04	Zr	0.96																					1965																																														K		3.8					3.8																																																								mj/mol.K2	3.83		226																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113146	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.05Zr0.95	Rh	0.05	Zr	0.95																					1965																																														K		4.8					4.8																																																								mj/mol.K2	5.08		210																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113147	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.06Zr0.94	Rh	0.06	Zr	0.94																					1965																																														K		5.75					5.75																																																								mj/mol.K2	6.8		196																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113148	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.07Zr0.93	Rh	0.07	Zr	0.93																					1965																																														K		5.95					5.95																																																								mj/mol.K2	7.36		192																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113149	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.075Zr0.925	Rh	0.075	Zr	0.925																					1965																																														K		6.05					6.05																																																								mj/mol.K2	7.6		193																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113150	1061	sp-heat measured between 0.9 and 12 K..	Zr1-xRhx	Rh0.08Zr0.92	Rh	0.08	Zr	0.92																					1965																																														K		6.1					6.1																																																								mj/mol.K2	7.88		192																																										Messung der spezifischen Warme an Zr-Rh-Legierungen zwischen 0.9 und 12 K				Z.PHYS.,186(1965)249	G.DUMMER		
113151	1109		Ti1-xRhx	Ti1	Ti	1																							1969																																														K		0.4					0.4																																																								mj/mol.K2	3.31																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113152	1109		Ti1-xRhx	Rh0.005Ti0.995	Rh	0.005	Ti	0.995																					1969																																														K		0.79					0.79																																																								mj/mol.K2	3.54																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113153	1109		Ti1-xRhx	Rh0.01Ti0.99	Rh	0.01	Ti	0.99																					1969																																														K		1.16					1.16																																																								mj/mol.K2	3.94																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113154	1109		Ti1-xRhx	Rh0.015Ti0.985	Rh	0.015	Ti	0.985																					1969																																														K		1.6					1.6																																																								mj/mol.K2	4.04																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113155	1109		Ti1-xRhx	Rh0.02Ti0.98	Rh	0.02	Ti	0.98																					1969																																														K		1.73					1.73																																																								mj/mol.K2	4.13																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113156	1109		Ti1-xRhx	Rh0.025Ti0.975	Rh	0.025	Ti	0.975																					1969																																														K		1.79					1.79																																																								mj/mol.K2	4.31																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113157	1109		Ti1-xRhx	Rh0.03Ti0.97	Rh	0.03	Ti	0.97																					1969																																														K		1.34					1.34																																																								mj/mol.K2	3.91																																												Kalorimetische Bestimmung der Ubergangstemperatur zur Supraleitung von verdunnten Titan-Rhodium-Legierungen				Z.PHYS.,222(1969)243	G.DUMMER,S.DANNER		
113158	744		Zr1-xScx	Sc0.1Zr0.9	Sc	0.1	Zr	0.9																					1966																																														K					0.024																																																										mj/mol.K2	2.4		309																																					arc-melting in He					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
113159	744		Zr1-xScx	Sc0.25Zr0.75	Sc	0.25	Zr	0.75																					1966																																														K					0.036																																																										mj/mol.K2	2.7		321																																					arc-melting in He					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
113160	744		Zr1-xScx	Sc0.8Zr0.2	Sc	0.8	Zr	0.2																					1966																																														K					0.02																																																										mj/mol.K2	7.4		330																																					arc-melting in He					Superconductivity and electronic specific heat in the scandium-zirconium system				PHYS.REV.,149(1966)409	J.P.MAITA,M.A.JENSEN		
113161	1933	dTc/dP = 2.5 E-5 K/bar	V3Si	Si1V3	Si	1	V	3																				3	1974																												Cr3Si(A15)																	Cr3Si, A15	K		15.9					15.9			K/GPa	0.25																																																																																																	Effect of lattice transformation on the pressure dependence of Tc of V3Si single crystals				PHYS.REV.B,10(1974)4030	C.W.CHU,S.HUANG		
113162	1209	annealed wire  Tc=8.02 K	Ta1-xTix	Ta0.685Ti0.315	Ta	0.685	Ti	0.315																					1966																																														K		8.28					8.28																																																																																																cold worked wire					Superconducting transition temperature of solid-solution Ta-Ti alloys				J.APPL.PHYS.,37(1966)4750	D.A.COLLING,J.WULFF,K.M.RALLS		
113163	1209	annealed wire  Tc=8.26 K	Ta1-xTix	Ta0.462Ti0.538	Ta	0.462	Ti	0.538																					1966																																														K		9.05					9.05	MTC13163																																																																																															cold worked wire					Superconducting transition temperature of solid-solution Ta-Ti alloys				J.APPL.PHYS.,37(1966)4750	D.A.COLLING,J.WULFF,K.M.RALLS		
113164	1038		NbN	N1Nb1	N	1	Nb	1																					1965																												NaCl			A	4.381													NaCl, B1	K		15					15																				kG		80																																																																															Critical supercurrents in niobium carbonitrides				APPL.PHYS.LETT.,7(1965)38	C.K.LONES,H.A.JOHANSEN,J.K..HULM,N.PESSALL		
113165	1038		Nb(N,C)	Nb1N0.8C0.2	Nb	1	N	0.8	C	0.2																			1965																												NaCl																	NaCl, B1	K																											kG		120												MHC13165																																																																			Critical supercurrents in niobium carbonitrides				APPL.PHYS.LETT.,7(1965)38	C.K.LONES,H.A.JOHANSEN,J.K..HULM,N.PESSALL		
113166	1038		Nb(N,C)	Nb1N0.5C0.5	Nb	1	N	0.5	C	0.5																			1965																												NaCl																	NaCl, B1	K																											kG		68.6												MHC13165																																																																			Critical supercurrents in niobium carbonitrides				APPL.PHYS.LETT.,7(1965)38	C.K.LONES,H.A.JOHANSEN,J.K..HULM,N.PESSALL		
113167	1361	(delta-C/gamma*Tc) = 1.48 . e-ph coupling = 0.52.	Th	Th1	Th	1																						1	1973																																													fcc	K		1.28					1.28																																																								mj/mol.K2	4.24		166																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113168	1361	(delta-C/gamma*Tc) =  1.48. e-ph coupling = 0.54.	Th1-xYx	Th0.95Y0.05	Th	0.95	Y	0.05																				1	1973																																													fcc	K		1.4					1.4																																																								mj/mol.K2	4.35		165																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113169	1361	(delta-C/gamma*Tc) =  1.41. e-ph coupling = 0.55.	Th1-xYx	Th0.9Y0.1	Th	0.9	Y	0.1																				1	1973																																													fcc	K		1.51					1.51																																																								mj/mol.K2	4.43		163																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113170	1361	(delta-C/gamma*Tc) = 1.45 . e-ph coupling = 0.55.	Th1-xYx	Th0.8Y0.2	Th	0.8	Y	0.2																				1	1973																																													fcc	K		1.64					1.64																																																								mj/mol.K2	4.87		172																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113171	1361	(delta-C/gamma*Tc) = 1.51 . e-ph coupling = 0.55.	Th1-xYx	Th0.75Y0.25	Th	0.75	Y	0.25																				1	1973																																													fcc	K		1.63					1.63																																																								mj/mol.K2	4.93		174																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113172	1361	(delta-C/gamma*Tc) =  1.43. e-ph coupling = 0.53	Th1-xYx	Th0.65Y0.35	Th	0.65	Y	0.35																				1	1973																																													fcc	K		1.53					1.53																																																								mj/mol.K2	5.1		180																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113173	1361		Th1-xYx	Th0.4Y0.6	Th	0.4	Y	0.6																				1	1973																																													hcp	K					1.2																																																										mj/mol.K2	5.26		203																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113174	1361		Th1-xYx	Th0.25Y0.75	Th	0.25	Y	0.75																				1	1973																																													hcp	K					1.2																																																										mj/mol.K2	6.85		210																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113175	1361		Th1-xYx	Th0.1Y0.9	Th	0.1	Y	0.9																				1	1973																																													hcp	K					1.2																																																										mj/mol.K2	7.58		227																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113176	1361		Th1-xYx	Th1	Th	1																						1	1973																																													hcp	K					0.08																																																										mj/mol.K2	10.3		330																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113177	1361	(delta-C/gamma*Tc) =  1.45. e-ph coupling = 0.53	Th1-xLax	La0.05Th0.95	La	0.05	Th	0.95																				1	1973																																													fcc	K		1.3					1.3																																																								mj/mol.K2	4.17		166																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113178	1361	(delta-C/gamma*Tc) =  1.49. e-ph coupling = 0.54	Th1-xLax	La0.1Th0.9	La	0.1	Th	0.9																				1	1973																																													fcc	K		1.48					1.48																																																								mj/mol.K2	4.26		165																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113179	1361	(delta-C/gamma*Tc) =  1.44. e-ph coupling = 0.58	Th1-xLax	La0.2Th0.8	La	0.2	Th	0.8																				1	1973																																													fcc	K		1.87					1.87																																																								mj/mol.K2	4.45		163																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113180	1361	(delta-C/gamma*Tc) =  1.56. e-ph coupling = 0.82	Th1-xLax	La0.7Th0.3	La	0.7	Th	0.3																				1	1973																																													fcc	K		4.88					4.88																																																								mj/mol.K2	8.6		150																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113181	1361	(delta-C/gamma*Tc) =  1.80. e-ph coupling = 0.83	Th1-xLax	La0.8Th0.2	La	0.8	Th	0.2																				1	1973																																													fcc	K		5.15					5.15																																																								mj/mol.K2	10		151																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113182	1361	e-ph coupling = 0.9	Th1-xLax	La0.9Th0.1	La	0.9	Th	0.1																					1973																																														K		5.62					5.62																																																								mj/mol.K2	10.5		148																																					arc-melting, then annealed					The specific heat and superconductivity of Th-Y and Th-La alloys				J.PHYS.SOC.JAPAN,34(1973)391	K.KUMAGAI,T.SATOH		
113183	524		W1-xTcx	Tc0.05W0.95	Tc	0.05	W	0.95																				1	1965																															A	3.1617													bcc	K					0.8																																																																																																		powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113184	524		W1-xTcx	Tc0.1W0.9	Tc	0.1	W	0.9																				1	1965																															A	3.1553													bcc	K		1.25					1.25																																																																																																powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113185	524		W1-xTcx	Tc0.2W0.8	Tc	0.2	W	0.8																				1	1965																															A	3.147													bcc	K		3.85					3.85																																																																																																powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113186	524	Hc2(4.2K)= 7.5 kG	W1-xTcx	Tc0.3W0.7	Tc	0.3	W	0.7																				1	1965																															A	3.134													bcc	K		5.75					5.75																				kG		18.3																																																																										powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113187	524	Hc2(4.2K)= 19.0 kG.	W1-xTcx	Tc0.4W0.6	Tc	0.4	W	0.6																				1	1965																															A	3.126													bcc	K		7.18					7.18																				kG		31.3																																																																										powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113188	524	Hc2(4.2K)= 29.0 kG. alpha- and sigma-phase detected.	W1-xTcx	Tc0.5W0.5	Tc	0.5	W	0.5																					1965																															A	3.117														K		7.52					7.52																				kG		45.5																																																																										powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113189	524	Hc2(4.2K)= 43.5 kG. alpha-phase detected.	W1-xTcx	Tc0.6W0.4	Tc	0.6	W	0.4																					1965																															A	3.117														K		7.88					7.88																				kG		65.1																																																																										powder, press, arc-melting					SUPERCONDUCTING THECHNETIUM-TUNGSTEN ALLOYS				PHYS.REV.,140(1965)A1177	J.K.HULM,R.S.KEMPER,S.H.AULTER		
113190	1416	Tc, Hc1(0), Hc2(0) increase with increasing pressure.	alpha-U	U1	U	1																						3	1970																																														K		0.2					0.2	MTC113190		K/GPa	1.8							Oe		120							Oe		240												MHC113190																																																																			Superconductivity of an alpha-uranium single crystal under pressure				SOLID STATE COMMUN.,8(1970)655	C.PALMY,E.S.FISHER		
113191	1698		V1-xScx	Sc0.01V0.99	Sc	0.01	V	0.99																					1964																																														K		5.67					5.67																				kG		4.97																																																																															Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113192	1698		V1-xScx	Sc0.07V0.93	Sc	0.07	V	0.93																					1964																																														K		6.09					6.09																				kG		3.01																																																																															Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113193	1698		V1-xScx	Sc0.3V0.7	Sc	0.3	V	0.7																					1964																																														K		6.76					6.76																				kG		2.59																																																																															Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113194	1698		V1-xScx	Sc0.4V0.6	Sc	0.4	V	0.6																					1964																																														K		6.94					6.94																				kG		1.77																																																																															Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113195	1698		V1-xScx	Sc0.5V0.5	Sc	0.5	V	0.5																					1964																																														K		7.03					7.03																																																																																																					Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113196	1698		V1-xScx	Sc0.6V0.4	Sc	0.6	V	0.4																					1964																																														K		6.84					6.84																																																																																																					Investigation of the superconductivity of alloys in the V-Sc system				Soviet Physics-JETP, 20(1965)543	E.V.GLOSHINA,N.V.VOLKENSHTEIN		
113197	1969		Zr1-xTax	Ta0.03Zr0.97	Ta	0.03	Zr	0.97																					1971																																														K		2.01					2.01																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113198	1969		Zr1-xTax	Ta0.07Zr0.93	Ta	0.07	Zr	0.93																					1971																																														K		3.25					3.25																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113199	1969		Zr1-xTax	Ta0.1Zr0.9	Ta	0.1	Zr	0.9																					1971																																														K		3.76					3.76																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113200	1969		Zr1-xTax	Ta0.125Zr0.875	Ta	0.125	Zr	0.875																					1971																																														K		4.14					4.14																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113201	1969		Zr1-xTax	Ta0.15Zr0.85	Ta	0.15	Zr	0.85																					1971																																														K		4.28					4.28																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113202	1969		Zr1-xTax	Ta0.17Zr0.83	Ta	0.17	Zr	0.83																					1971																																														K		5.28					5.28																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113203	1969		Zr1-xTax	Ta0.2Zr0.8	Ta	0.2	Zr	0.8																					1971																																														K		5.56					5.56																																																																																																ANN(1340C), Quench to RT					The metastable constitution and the superconducting transition behavior of Zr-Ta alloys				J.NUCLEAR MATERIALS,38(1971)83	D.H.POLONIS,R.TAGGART,S.L.NARASIMHAN		
113204	998		Tl	Tl1	Tl	1																							1965																																														K								MTC13204																																																																																																								ZH.EKSP.TEOR.FIZ.,49(1965)85	B.G.LAZAREV,L.S.LAZAREVA,N.B.BRANDT,N.I.GINZBURG,T.A.IGNAT'EVA,V.I.MAKAROV		
113205	998		Tl1-xHgx	Hg0.0045Tl0.9955	Hg	0.0045	Tl	0.9955																					1965																																														K								MTC13204																																																																																																								ZH.EKSP.TEOR.FIZ.,49(1965)85	B.G.LAZAREV,L.S.LAZAREVA,N.B.BRANDT,N.I.GINZBURG,T.A.IGNAT'EVA,V.I.MAKAROV		
113206	998		Tl1-xHgx	Hg0.009Tl0.991	Hg	0.009	Tl	0.991																					1965																																														K								MTC13204																																																																																																								ZH.EKSP.TEOR.FIZ.,49(1965)85	B.G.LAZAREV,L.S.LAZAREVA,N.B.BRANDT,N.I.GINZBURG,T.A.IGNAT'EVA,V.I.MAKAROV		
113207	472	P-induced SC. P(cr)=110 kbar. Tc(110kbar)= 1.8 K. Y(II) for P < 125 kbar. RRR=8.	Y(II)	Y1	Y	1																							1974																																														K		1.8			0		1.8			K/GPa	-0.32																																																																																																	New superconducting modifications of yttrium				JETP Lett., 20(1974)8 	I.V.BERMAN,N.B.BRANDT,YU.P.KURKIN		
113208	472	P-induced SC. P(cr)=110 kbar. Y(III) for 125 < P < 160 kbar. RRR=8.	Y(III)	Y1	Y	1																							1974																																														K					0					K/GPa	0.35																																																																																																	New superconducting modifications of yttrium				JETP Lett., 20(1974)8 	I.V.BERMAN,N.B.BRANDT,YU.P.KURKIN		
113209	909	P-induced SC. Tc = 2.05 K at P(cr)=43 kbar. Te(II) for 40 < P < 70 kbar. hole conc. = 1 - 4 E+18 /cm3.	Te(II)	Te1	Te	1																						3	1971																																														K		2.05			0		2.05			K/GPa	0.85																																																																																																					ZH.ETF PIS.RED.,13(1971)23	E.S.ITSKEVICH,M.A.IL'INA		
113210	909	P-induced SC. Tc = 4.3 K. at P = 80 kbar. Te(IV) for 80 < P < 100 kbar.	Te(IV)	Te1	Te	1																						3	1971																																														K		4.3			0		4.3			K/GPa	-0.34																																																																																																					ZH.ETF PIS.RED.,13(1971)23	E.S.ITSKEVICH,M.A.IL'INA		
113211	951	Tc(Th) = 1.36 K	Th1-xCex	Ce0.02Th0.98	Ce	0.02	Th	0.98																					1970																																														K		0.7					0.7	MTC13211																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
113212	951	Tc(Th) = 1.36 K	Th1-xUx	Th0.9988U0.0012	Th	0.9988	U	0.0012																					1970																																														K		0.55					0.55	MTC13212																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
113213	951	Tc(Al) = 1.17 K	Al1-xMnx	Al0.998Mn0.002	Al	0.998	Mn	0.002																					1970																																														K		0.262					0.262	MTC13213																																																																																																				Superconducting-normal phase boundary of superconductors containing nearly nonmagnetic impurities				Solid State Commun.,8(1970)1987	J.G.HUBER,M.B.MAPLE		
113214	1519	Tc(P) is measured.	Al1-xMnx	Al99.925Mn0.075	Al	99.925	Mn	0.075																					1971																																														K		0.7					0.7	MTC13214																																																																																																				Superconductivity of AlMn and ThU alloys under pressure				J.PHYS.F:METAL.PHYS.,1(1971)893	J.G.HUBER,M.B.MAPLE		
113215	1519	Tc(P) is measured.	Th1-xUx	Th99.92U0.08	Th	99.92	U	0.08																					1971																																														K		0.77					0.77	MTC13215																																																																																																				Superconductivity of AlMn and ThU alloys under pressure				J.PHYS.F:METAL.PHYS.,1(1971)893	J.G.HUBER,M.B.MAPLE		
113216	514		Ti-V-Al	Ti0.63V0.27Al0.1	Ti	0.63	V	0.27	Al	0.1																			1964																																														K		3.62					3.62																																																								mj/mol.K2	8.63		255																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113217	514		Ti-V-Al	Ti0.595V0.255Al0.15	Ti	0.595	V	0.255	Al	0.15																			1964																																														K		2.36					2.36																																																								mj/mol.K2	7.54		290																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113218	514		Ti-V-Al	Ti0.525V0.255Al0.25	Ti	0.525	V	0.255	Al	0.25																			1964																																														K																																																															mj/mol.K2	6.03		333																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113219	514		Ti-V-Al	Ti0.49V0.21Al0.3	Ti	0.49	V	0.21	Al	0.3																			1964																																														K																																																															mj/mol.K2	4.86		344																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113220	514		Ti-V-Al	Ti0.72V0.18Al0.1	Ti	0.72	V	0.18	Al	0.1																			1964																																														K		3.52					3.52																																																								mj/mol.K2	8.17		251																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113221	514		Ti-V-Al	Ti0.54V0.36Al0.1	Ti	0.54	V	0.36	Al	0.1																			1964																																														K		3.44					3.44																																																								mj/mol.K2	8.67		353																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113222	514		Ti-V-Al	Ti0.36V0.54Al0.1	Ti	0.36	V	0.54	Al	0.1																			1964																																														K		2.7					2.7																																																								mj/mol.K2	8.13		412																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113223	514		Ti-V-Al	Ti0.18V0.72Al0.1	Ti	0.18	V	0.72	Al	0.1																			1964																																														K		2.05					2.05																																																								mj/mol.K2	7.63		416																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113224	514		V-Cr-Al	V0.81Cr0.09Al0.1	V	0.81	Cr	0.09	Al	0.1																			1964																																														K		1.46					1.46																																																								mj/mol.K2	6.7		393																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113225	514		V-Cr-Al	V0.63Cr0.27Al0.1	V	0.63	Cr	0.27	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	5.78		424																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113226	514		V-Cr-Al	V0.45Cr0.45Al0.1	V	0.45	Cr	0.45	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	4.19		332																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113227	514		V-Cr-Al	V0.27Cr0.63Al0.1	V	0.27	Cr	0.63	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	3.73		445																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113228	514		V-Cr-Al	V0.18Cr0.72Al0.1	V	0.18	Cr	0.72	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	3.02		537																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113229	514		V-Cr-Al	V0.09Cr0.81Al0.1	V	0.09	Cr	0.81	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	2.85		507																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113230	514		V-Cr-Al	V0.045Cr0.855Al0.1	V	0.045	Cr	0.855	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	2.64		592																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113231	514	Constant term in SP-heat, A = 2.4 E-4 cal/mol.K	Cr-Fe-Al	Cr0.855Fe0.045Al0.1	Cr	0.855	Fe	0.045	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	3.31		894																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113232	514	Constant term in SP-heat, A = 22.8 E-4 cal/mol.K	Cr-Fe-Al	Cr0.81Fe0.09Al0.1	Cr	0.81	Fe	0.09	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	8.84		588																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113233	514	Constant term in SP-heat, A = 15.3 E-4 cal/mol.K	Cr-Fe-Al	Cr0.765Fe0.135Al0.1	Cr	0.765	Fe	0.135	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	14.2		578																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113234	514	Constant term in SP-heat, A = 15.4 E-4 cal/mol.K	Cr-Fe-Al	Cr0.72Fe0.18Al0.1	Cr	0.72	Fe	0.18	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	16.2		570																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113235	514	Constant term in SP-heat, A = 6.5 E-4 cal/mol.K	Cr-Fe-Al	Cr0.675Fe0.225Al0.1	Cr	0.675	Fe	0.225	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	13		562																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113236	514	Constant term in SP-heat, A = 13.3 E-4 cal/mol.K	Cr-Fe-Al	Cr0.63Fe0.27Al0.1	Cr	0.63	Fe	0.27	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	8.42		209																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113237	514		Cr-Fe-Al	Cr0.54Fe0.36Al0.1	Cr	0.54	Fe	0.36	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	7.28		404																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113238	514		Cr-Fe-Al	Cr0.45Fe0.45Al0.1	Cr	0.45	Fe	0.45	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	5.78		501																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113239	514		Cr-Fe-Al	Cr0.225Fe0.675Al0.1	Cr	0.225	Fe	0.675	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	4.69		421																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113240	514		Cr-Fe-Al	Cr0.045Fe0.855Al0.1	Cr	0.045	Fe	0.855	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	4.65		344																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113241	514	(1/T)-term in SP-heat, a =  2.493  E-4 cal/mol.K	Fe-Co-Al	Fe0.81Co0.09Al0.1	Fe	0.81	Co	0.09	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	3.98		430																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113242	514	(1/T)-term in SP-heat, a =  5.141  E-4 cal/mol.K	Fe-Co-Al	Fe0.72Co0.18Al0.1	Fe	0.72	Co	0.18	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	3.14		332																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113243	514	(1/T)-term in SP-heat, a =  5.406  E-4 cal/mol.K	Fe-Co-Al	Fe0.63Co0.27Al0.1	Fe	0.63	Co	0.27	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	2.47		496																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113244	514	(1/T)-term in SP-heat, a =  5.472  E-4 cal/mol.K	Fe-Co-Al	Fe0.54Co0.36Al0.1	Fe	0.54	Co	0.36	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	1.8		494																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113245	514	(1/T)-term in SP-heat, a =  5.077  E-4 cal/mol.K	Fe-Co-Al	Fe0.45Co0.45Al0.1	Fe	0.45	Co	0.45	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	1.01		506																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113246	514	(1/T)-term in SP-heat, a =  13.563  E-4 cal/mol.K	Fe-Co-Al	Fe0.36Co0.54Al0.1	Fe	0.36	Co	0.54	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	2.18		328																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113247	514	(1/T)-term in SP-heat, a =  7.537  E-4 cal/mol.K	Fe-Co-Al	Fe0.27Co0.63Al0.1	Fe	0.27	Co	0.63	Al	0.1																			1964																																														K					1.5																																																										mj/mol.K2	4.02		471																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113248	514		Cr	Cr1	Cr	1																							1964																																														K					1.5																																																										mj/mol.K2	1.42		606																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113249	514		Cr1-xAlx	Al0.049Cr0.951	Al	0.049	Cr	0.951																					1964																																														K					1.5																																																										mj/mol.K2	2.05		460																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113250	514		Cr1-xAlx	Al0.1Cr0.9	Al	0.1	Cr	0.9																					1964																																														K					1.5																																																										mj/mol.K2	1.8		581																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113251	514		Cr1-xAlx	Al0.146Cr0.854	Al	0.146	Cr	0.854																					1964																																														K					1.5																																																										mj/mol.K2	1.17		528																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113252	514		Cr1-xAlx	Al0.2Cr0.8	Al	0.2	Cr	0.8																					1964																																														K					1.5																																																										mj/mol.K2	4.61		529																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113253	514		Cr1-xAlx	Al0.25Cr0.75	Al	0.25	Cr	0.75																					1964																																														K					1.5																																																										mj/mol.K2	3.6		446																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113254	514		Cr1-xAlx	Al0.3Cr0.7	Al	0.3	Cr	0.7																					1964																																														K					1.5																																																										mj/mol.K2	1.05		425																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113256	514		V1-xAlx	Al0.188V0.812	Al	0.188	V	0.812																					1964																																														K					1.5																																																										mj/mol.K2	5.49		323																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113257	514		V1-xAlx	Al0.308V0.692	Al	0.308	V	0.692																					1964																																														K					1.5																																																										mj/mol.K2	4.19		332																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113258	514		V1-xAlx	Al0.402V0.598	Al	0.402	V	0.598																					1964																																														K					1.5																																																										mj/mol.K2	3.44		324																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113259	514		V1-xSnx	Sn0.02V0.98	Sn	0.02	V	0.98																					1964																																														K		2.87					2.87																																																								mj/mol.K2	8		315																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113260	514		V1-xSnx	Sn0.04V0.96	Sn	0.04	V	0.96																					1964																																														K		1.86					1.86																																																								mj/mol.K2	7.12		382																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113261	514		V1-xSnx	Sn0.057V0.943	Sn	0.057	V	0.943																					1964																																														K		1.6					1.6																																																								mj/mol.K2	6.66		393																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113262	514		V1-xSbx	Sb0.01V0.99	Sb	0.01	V	0.99																					1964																																														K		3.76					3.76																																																								mj/mol.K2	8.84		352																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113263	514		V1-xSbx	Sb0.02V0.98	Sb	0.02	V	0.98																					1964																																														K		3.29					3.29																																																								mj/mol.K2	8.17		319																																										Low temperature specific heat of bcc alloys of 3d transition elements and aluminum				J.PHYS.CHEM.SOLIDS,25(1964)993	C.H.CHENG,K.P.GUPTA,N.PESSALL,P.A.BECK		
113264	1704	Tc(R) = 5.21. RRR=24. (delta-C/gamma*Tc) = 1.40	V	V1	V	1																							1973																															A	3.029													bcc	K		5.24					5.24																																																								mj/mol.K2	9.8		373																																										Alteration of the superconducting properties of vanadium by introduction of tantalum impurity atoms				Soviet Phys. JETP 37(1973)102 	A.A.SHIKOV,B.N.SAMOILOV,G.KH.PANOVA,N.A.CHERNOPLEKOV		
113265	1704	Tc(R) = 4.95. RRR=9.6. (delta-C/gamma*Tc) = 1.41	V1-xTax	Ta0.0082V0.9918	Ta	0.0082	V	0.9918																					1973																															A	3.031													bcc	K		4.9					4.9																																																								mj/mol.K2	9.5		370																																										Alteration of the superconducting properties of vanadium by introduction of tantalum impurity atoms				Soviet Phys. JETP 37(1973)102 	A.A.SHIKOV,B.N.SAMOILOV,G.KH.PANOVA,N.A.CHERNOPLEKOV		
113266	1704	Tc(R)= 4.57. RRR=5.6. (delta-C/gamma*Tc) = 1.42	V1-xTax	Ta0.0355V0.9645	Ta	0.0355	V	0.9645																					1973																															A	3.037													bcc	K		4.55					4.55																																																								mj/mol.K2	9.25		359																																										Alteration of the superconducting properties of vanadium by introduction of tantalum impurity atoms				Soviet Phys. JETP 37(1973)102 	A.A.SHIKOV,B.N.SAMOILOV,G.KH.PANOVA,N.A.CHERNOPLEKOV		
113267	1704	Tc(R) = 4.46. RRR=4.8. (delta-C/gamma*Tc) = 1.43	V1-xTax	Ta0.0568V0.9432	Ta	0.0568	V	0.9432																					1973																															A	3.049													bcc	K		4.46					4.46																																																								mj/mol.K2	9.16		350																																										Alteration of the superconducting properties of vanadium by introduction of tantalum impurity atoms				Soviet Phys. JETP 37(1973)102 	A.A.SHIKOV,B.N.SAMOILOV,G.KH.PANOVA,N.A.CHERNOPLEKOV		
113268	1563	Hc2 = Hc derived from Hc(T) using simple BCS extraporation.	Th1-xUx	Th0.99975U0.025	Th	0.99975	U	0.025																					1973																																														K		1.182					1.182																				Oe		136.6												MHC13268																																																																							PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113269	1563	Hc2 = Hc derived from Hc(T) using simple BCS extraporation.	Th1-xUx	Th0.9995U0.05	Th	0.9995	U	0.05																					1973																																														K		1.014					1.014																				Oe		117												MHC13268																																																																							PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113270	1563	Hc2 = Hc derived from Hc(T) using simple BCS extraporation.	Th1-xUx	Th0.999U0.1	Th	0.999	U	0.1																					1973																																														K		0.725					0.725																				Oe		84.5												MHC13270																																																																							PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113271	1563	Hc2 = Hc derived from Hc(T) using simple BCS extraporation.	Th1-xUx	Th0.99873U0.127	Th	0.99873	U	0.127																					1973																																														K		0.658					0.658																				Oe		76.5												MHC13270																																																																							PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113272	1563		Th1-xUx	Th0.9985U0.15	Th	0.9985	U	0.15																					1973																																														K		0.495					0.495																																		MHC13270																																																																							PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113273	1563		Th1-xUx	Th0.998U0.2	Th	0.998	U	0.2																					1973																																														K		0.304					0.304	MTC13273																																																																																																								PHYS.REV.B,8(1973)3179	D.K.FINNEMORE,D.T.PETERSON,H.L.WATSON		
113274	PR1720430	RRR=1200. Hc2=Hc. Energy gap deduced from Hc(T) curve.	Th1-xUx	Th1	Th	1																							1968																																														K		1.39					1.39																				Oe		159.22												MHC13274														3.53								mj/mol.K2	4.31																																												Critical-field curves for gapless superconductors				Phys.Rev., 172(1968)430	D.K.Finnemore,W.R.Decker		
113275	PR1720430	Hc2=Hc. Energy gap deduced from Hc(T) curve.	Th1-xUx	Th0.999U0.001	Th	0.999	U	0.001																					1968																																														K		1.11					1.11																				Oe		123.06												MHC13274														3.91																																																					Critical-field curves for gapless superconductors				Phys.Rev., 172(1968)430	D.K.Finnemore,W.R.Decker		
113276	PR1720430	Hc2=Hc. Energy gap deduced from Hc(T) curve.	Th1-xUx	Th0.9985U0.0015	Th	0.9985	U	0.0015																					1968																																														K		0.9					0.9																				Oe		96.16												MHC13276														4.3																																																					Critical-field curves for gapless superconductors				Phys.Rev., 172(1968)430	D.K.Finnemore,W.R.Decker		
113277	PR1720430	Hc2=Hc. Energy gap deduced from Hc(T) curve.	Th1-xUx	Th0.998U0.002	Th	0.998	U	0.002																					1968																																														K		0.761					0.761																				Oe		78.63												MHC13276														4.66																																																					Critical-field curves for gapless superconductors				Phys.Rev., 172(1968)430	D.K.Finnemore,W.R.Decker		
113278	LTP0030137		Th1-xUx	Th0.999U0.001	Th	0.999	U	0.001																					1970																																														K		0.66					0.66	MTC13278																																																																																																								J.Low Temp.Phys., 3(1970)137	A.C.Lawson,B.R.Coles,J.G.Huber,M.B.Maple		
113279	JPS0733129	P-induced SC. P(cr)=2.61 GPa. SC properties for P=2.61 GPa. SC region shown in FIG(from JPS076051007). gamma calculated from Hc2(T). RR=0.44 microOhm.cm. RRR=250.	UIr	Ir1U1	Ir	1	U	1																				3	2004							46																					PbBi	P2<1>																monoclinic-PbBi	K		0.14			0		0.14	MPH113279																			mT		25.8														A		1100																		mj/mol.K2	48.5																																							Czochralski method					Pressure-induced Superconductivity in UIr			Faculty of Maritime Sciences, Kobe University, Higashi-Nada, Kobe, Japan	J.Phys.Soc.Jpn, 73(2004)3129	E.Yamamoto,H.Hidaka,H.Kotegawa,R.Settai,T.Akazawa,T.C.Kobayashi,T.Fujiwara,Y.Haga,Y.Onuki		
113280	JPS0732639	AgB2 phase not detected by XRD. But authors believe that AgB2 films were synthesized. Tc-width = 0.7 K. thickness = 130 nm.	AgB2	Ag1B2	Ag	1	B	2																					2004																																														K		6.7					6.7																																																																																																deposit Ag/B on MgO,then ANN(820C,4h)					Superconductivity in Silver Boron Intermetallic Compound			Department of Physics, Tokyo Institute of Technology, 2-12-1 O-okayama, Meguro-ku, Tokyo, Japan	J.Phys.Soc.Jpn, 73(2004)2639	H.Koga,I.Iguchi,R.Tomita,T.Uchiyama		
113281	P071020501	Hc2 by thermal conductivity.	Mg(B,C)2	Mg1B1.94C0.06	Mg	1	B	1.94	C	0.06																		3	2005																												AlB2																	AlB2, C32	K																																									MMHC13281																																																														high-pressure synthesis using cubic anvil					Influence of carbon substitution on the heat transport in single crystalline MgB2			Laboratorium fur Festkorperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)020501	A.V.Sologubenko,H.R.Ott,J.Karpinski,N.D.Zhigadlo,S.M.Kazakov		
113282	P071020501	Hc2 by thermal conductivity. Tc-width=0.1 K. R = R0+a*T^3 (R0=12.3 uOhm.cm, a=5.4E-7 uOhm.cm/K^3). Wiedemann-Franz law is valid.	Mg(B,C)2	Mg1B1.88C0.12	Mg	1	B	1.88	C	0.12																		3	2005																												AlB2																	AlB2, C32	K		32.9					32.9																																		MHC13282																																																														high-pressure synthesis using cubic anvil					Influence of carbon substitution on the heat transport in single crystalline MgB2			Laboratorium fur Festkorperphysik, ETH Honggerberg, CH-8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)020501	A.V.Sologubenko,H.R.Ott,J.Karpinski,N.D.Zhigadlo,S.M.Kazakov		
113283	JPS0613054	gap from NMR of <205>Tl	TlMoSe7.5	Tl1Mo6Se7.5	Tl	1	Mo	6	Se	7.5																			1992																												Chevrel																		K		12.2					12.2																																																4.5																																																sintering					Nuclear relaxation study in strong coupling superconductors -A comparison with high-Tc superconductors - 			Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka,Osaka,Japan	J.Phys.Soc.Jpn, 61(1992)3054	K.Asauama,K.Ishida,M.Kyogaku,S.Ohsugi,T.Ohtani,Y.Kitaoka		
113284	JPS0613054	gap from NMR of <119>Sn	SnMo6Se7.5	Sn1.1Mo6Se7.5	Sn	1.1	Mo	6	Se	7.5																			1992																												Chevrel																		K		4.2					4.2																																																3.6																																																sintering					Nuclear relaxation study in strong coupling superconductors -A comparison with high-Tc superconductors - 			Department of Material Physics, Faculty of Engineering Science, Osaka University, Toyonaka,Osaka,Japan	J.Phys.Soc.Jpn, 61(1992)3054	K.Asauama,K.Ishida,M.Kyogaku,S.Ohsugi,T.Ohtani,Y.Kitaoka		
113285	P064224420	space-G = Pbcm.	La3Rh2Ge2	La3Rh2Ge2	La	3	Rh	2	Ge	2																			2001																															A	5.76	8.189	13.596												K		3.5					3.5																																																																																																arc-melting					Superconductivity in La3Rh2Ge2 and dense Kondo behavior in Ce3Rh2Ge2				Phys.Rev.B, 64(2001)224420	D.Kaczorowski,Yu.Grin,Yu.Prots		
113286	P064224420	space-G = Pbcm. spin reordering at 5 K. effective M = 2.52 my-B/Ce.	Ce3Rh2Ge2	Ce3Rh2Ge2	Ce	3	Rh	2	Ge	2																			2001							-90	7.5																							A	5.679	8.073	13.421												K					4.2																																																																																																		arc-melting					Superconductivity in La3Rh2Ge2 and dense Kondo behavior in Ce3Rh2Ge2				Phys.Rev.B, 64(2001)224420	D.Kaczorowski,Yu.Grin,Yu.Prots		
113287	PR0246715	ANN(670C,2w, in Yb atmosphere). SC volume fraction = 100%. X-ray extra line(Yb, Pd4Yb3, PdGe, Pd2Ge, GeO2).	YbPd2Ge2	Yb1Pd2Ge2	Yb	1	Pd	2	Ge	2																			1981																																														K		1.17					1.17																																																																																																induction melting					Superconductivity in the ternary intermetallics YbPd2Ge2, LaPd2Ge2, and LaPt2Ge2			Bell Lab, Murray Hill, New Jersey	Phys.Rev.B, 24(1981)6715	G.W.Hull,J.E.Bernardini,J.H.Wernik,J.V.Waszczak,T.H.Geballe		
113288	PR0246715	ANN(670C, 5d)	LaPd2Ge2	La1Pd2Ge2	La	1	Pd	2	Ge	2																		1	1981																																														K		1.12					1.12																																																																																																induction melting					Superconductivity in the ternary intermetallics YbPd2Ge2, LaPd2Ge2, and LaPt2Ge2			Bell Lab, Murray Hill, New Jersey	Phys.Rev.B, 24(1981)6715	G.W.Hull,J.E.Bernardini,J.H.Wernik,J.V.Waszczak,T.H.Geballe		
113289	PR0246715	ANN(650C, 5d)	LaPt2Ge2	La1Pt2Ge2	La	1	Pt	2	Ge	2																		1	1981																																														K		0.55					0.55																																																																																																induction melting					Superconductivity in the ternary intermetallics YbPd2Ge2, LaPd2Ge2, and LaPt2Ge2			Bell Lab, Murray Hill, New Jersey	Phys.Rev.B, 24(1981)6715	G.W.Hull,J.E.Bernardini,J.H.Wernik,J.V.Waszczak,T.H.Geballe		
113290	PR0246715	ANN(670C, 5d)	YbCu2Ge2	Yb1Cu2Ge2	Yb	1	Cu	2	Ge	2																			1981																																														K					0.47																																																																																																		induction melting					Superconductivity in the ternary intermetallics YbPd2Ge2, LaPd2Ge2, and LaPt2Ge2			Bell Lab, Murray Hill, New Jersey	Phys.Rev.B, 24(1981)6715	G.W.Hull,J.E.Bernardini,J.H.Wernik,J.V.Waszczak,T.H.Geballe		
113291	P071024509		LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																	2005																												LuNi2B2C			A	3.463		10.626												K		16.5					16.5																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113292	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.98La0.02Ni2B2C1	Lu	0.98	La	0.02	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.47		10.615												K		16.2					16.2																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113293	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.95La0.05Ni2B2C1	Lu	0.95	La	0.05	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.48		10.605												K		15.3					15.3																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113294	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.94La0.06Ni2B2C1	Lu	0.94	La	0.06	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.484		10.601												K		15.1					15.1																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113295	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.93La0.07Ni2B2C1	Lu	0.93	La	0.07	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.486		10.596												K		13.6					13.6																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113296	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.92La0.08Ni2B2C1	Lu	0.92	La	0.08	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.487		10.59												K		13.6					13.6																																																																																																arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113297	P071024509	La-content calculated from lattice constant assuming Vegards law.	(Lu,La)Ni2B2C	Lu0.91La0.09Ni2B2C1	Lu	0.91	La	0.09	Ni	2	B	2	C	1															2005																												LuNi2B2C			A	3.764		9.894												K					2																																																																																																		arc-melting					Influence of structural parameters on Tc in superconducting RNi2B2C compounds			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Urca,  Rio de Janeiro, Brazil	Phys.Rev.B, 71(2005)024509	D.R.Sanchez,E.M.Baggio-Saitovitch,H.Micklitz		
113298	P071024533		MgB2	B2Mg1	B	2	Mg	1																				3	2005																												AlB2			A	3.0849		3.5187											AlB2, C32	K		38.5					38.5																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113299	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.896C0.104	Mg	1	B	1.896	C	0.104																		3	2005																												AlB2			A	3.0683		3.521											AlB2, C32	K		35					35																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113300	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		3	2005																												AlB2			A	3.0687		3.5217											AlB2, C32	K		34.3					34.3																																		MHC13300																																																														high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113301	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.874C0.126	Mg	1	B	1.874	C	0.126																		3	2005																												AlB2			A	3.0647		3.522											AlB2, C32	K		33.3					33.3																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113302	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.84C0.16	Mg	1	B	1.84	C	0.16																		3	2005																												AlB2			A	3.0592		3.5208											AlB2, C32	K		33					33	MTC13302																																																																																															high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113303	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.826C0.174	Mg	1	B	1.826	C	0.174																		3	2005																												AlB2			A	3.0569		3.5204											AlB2, C32	K		30.8					30.8																																		MHC13303																																																														high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113304	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.81C0.19	Mg	1	B	1.81	C	0.19																		3	2005																												AlB2			A	3.0544		3.518											AlB2, C32	K		30.1					30.1																																		MHC13303																																																														high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113305	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		3	2005																												AlB2			A	3.0529		3.5164											AlB2, C32	K		28					28																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113306	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.792C0.208	Mg	1	B	1.792	C	0.208																		3	2005																												AlB2			A	3.0517		3.5205											AlB2, C32	K		25.5					25.5																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113307	P071024533	C-content estimated from lattice constant  a  using PHC3870301(2003)	Mg(B,C)2	Mg1B1.7C0.3	Mg	1	B	1.7	C	0.3																		3	2005																												AlB2			A	3.0369		3.5182											AlB2, C32	K		10.2					10.2																																																																																																high-pressure synthesis					Carbon substitution in MgB2 single crystals: Structural and superconducting properties			Solid State Physics Laboratory ETH, 8093 Zurich, Switzerland	Phys.Rev.B, 71(2005)024533	A.V.Mironov,B.Batlogg,Ch.Soltmann,J.Jun,J.Karpinski,K.Rogacki,N.D.Zhigadlo,R.Puzniak,S.M.Kazakov		
113308	PRL0862416	single-walled carbon nanotube. Hc defined as the inflection point in R(H). I-V characteristics are measured.	CNT	C1	C	1																							2001																												CNT																		K		0.37					0.37																				T		1.35							T/K		3.65																																																																	electrical arc method with a mixture of Ni and Y as a catalyst					Superconductivity in Ropes of Single-Walled Carbon Nanotubes				Phys.Rev.Lett., 86(2001)2416	A.Yu.Kasumov,B.Reulet,H.Bouchiat,I.I.Khodos,L.Vaccarini,M.Kociak,S.Gueron,V.T.Volkov,Yu.B.Gorbatov		
113309	PHC4070031		MgB2	B2Mg1	B	2	Mg	1																					2004																												AlB2			A	3.0841		3.5281											AlB2, C32	K		38.81					38.81																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113310	PHC4070031	C-content (estimated from lat-a) = 0.06864	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																			2004																												AlB2			A	3.071		3.5265											AlB2, C32	K		33.98					33.98																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113311	PHC4070031	C-content (estimated from lat-a) = 0.06864	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																			2004																												AlB2			A	3.0719		3.5247											AlB2, C32	K		34.16					34.16																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113312	PHC4070031	C-content (estimated from lat-a) = 0.07258	Mg(B,C)2	Mg1B1.7C0.3	Mg	1	B	1.7	C	0.3																			2004																												AlB2			A	3.071		3.5251											AlB2, C32	K		34.27					34.27																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113313	PHC4070031	C-content (estimated from lat-a) = 0.09452	Mg(B,C)2	Mg1B1.6C0.4	Mg	1	B	1.6	C	0.4																			2004																												AlB2			A	3.0683		3.5291											AlB2, C32	K		33.3					33.3																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113314	PHC4070031	C-content (estimated from lat-a) = 0.12884	Mg(B,C)2	Mg1B1.5C0.5	Mg	1	B	1.5	C	0.5																			2004																												AlB2			A	3.0593		3.5275											AlB2, C32	K		28.3					28.3																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
113315	PHC4070031	C-content (estimated from lat-a) = 0.19692	Mg(B,C)2	Mg1B1.4C0.6	Mg	1	B	1.4	C	0.6																			2004																												AlB2			A	3.0505		3.5289											AlB2, C32	K		19.45					19.45																																																																																																solid vapour reaction(900C,24h)					Peculiarities in the carbon substitution of MgB2				Physica C, 407(2004)31	A.Bharathi,N.Gayathri,S.J,Balaselvi,S.J.Balaselvi,V.S.Sastry,Y.Hariharan		
120001	MRB0200517		YIrSi	Y1Ir1Si1	Y	1	Ir	1	Si	1																			1985																												TiNiSi			A	6.789	4.188	7.462												K		2.7					2.7																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120002	MRB0200517		TiIrSi	Ti1Ir1Si1	Ti	1	Ir	1	Si	1																			1985																												TiNiSi			A	6.2578	3.8581	7.2006												K					1.7																																																																																																							New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120003	MRB0200517		ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																			1985																												TiNiSi			A	6.5578	3.9537	7.3762												K		2.04					2.04																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120004	MRB0200517		HfIrSi	Hf1Ir1Si1	Hf	1	Ir	1	Si	1																			1985																												TiNiSi			A	6.471	3.938	7.3763												K		3.5					3.5																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120005	LES0920177		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1983																												TiNiSi			A	6.4169	3.8623	7.3215												K		3.82					3.82																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120006	LES0920177		NbRuP	Nb1Ru1P1	Nb	1	Ru	1	P	1																			1983																												TiNiSi			A	6.318	3.719	7.173												K					1.1																																																																																																		arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120007	LES0920177		TaRuP	Ta1Ru1P1	Ta	1	Ru	1	P	1																			1983																												TiNiSi			A	6.288	3.713	7.164												K					1.1																																																																																																		arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120008	LES0920177		ZrRhP	Zr1Rh1P1	Zr	1	Rh	1	P	1																			1983																												TiNiSi			A	6.483	3.787	7.393												K		1.55					1.55																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120009	LES0920177		NbRhP	Nb1Rh1P1	Nb	1	Rh	1	P	1																			1983																												TiNiSi			A	6.306	3.737	7.187												K		4.42					4.42																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120010	LES0920177		TaRhP	Ta1Rh1P1	Ta	1	Rh	1	P	1																			1983																												TiNiSi			A	6.253	3.736	7.18												K		4.86					4.86																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120011	NAC0773132		TiRuP	Ti1Ru1P1	Ti	1	Ru	1	P	1																			1980																										ABC		Fe2P			A	6.303		3.567												K			1.33				1.33																																																																																																mixture - SIN(800-1200c, in Ar) - arc melting					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120012	NAC0773132		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1980																										ABC		Fe2P			A	6.459		3.778												K	10.56		12.34				11.45																																																																																																mixture - SIN(800-1200c, in Ar) - arc melting - ANN(900C) - quench					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120013	NAC0773132		HfRuP	Hf1Ru1P1	Hf	1	Ru	1	P	1																			1980																										ABC		Fe2P			A	6.414		3.753												K	11.08		12.7				11.89																																																																																																mixture - SIN(800-1200c, in Ar) - SIN(1000 C) - slow cooling					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120014	NAC0773132		TiOsP	Ti1Os1P1	Ti	1	Os	1	P	1																			1980																										ABC		Fe2P			A	6.285		3.625												K					1.2																																																																																																		mixture - SIN(800-1200c, in Ar) - SIN(1000 C) - slow cooling					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120015	NAC0773132		ZrOsP	Zr1Os1P1	Zr	1	Os	1	P	1																			1980																										ABC		Fe2P			A	6.46		3.842												K	5.7		7.44				6.57																																																																																																mixture - SIN(800-1200c, in Ar) - SIN(1000 C) - slow cooling					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120016	NAC0773132		HfOsP	Hf1Os1P1	Hf	1	Os	1	P	1																			1980																										ABC		Fe2P			A	6.417		3.792												K	4.96		6.1				5.53																																																																																																mixture - SIN(800-1200c, in Ar) - SIN(1000 C) - slow cooling					Ternary transition metal phosphides: High-temperature superconductors				Proc.Natl.Acad.Sci.USA, 77(1980)3132	B.T.Matthias,C.Ku,G.P.Meisner,H.Barz,Z.Fisk		
120017	MRB0180983		ZrRuAs	Zr1Ru1As1	Zr	1	Ru	1	As	1																			1983																												ZrNiAl			A	6.586		3.891												K		11.9					11.9																																																																																																arc-melting					SUPERCONDUCTING EQUIATOMIC TERNARY TRANSITION METAL ARSENIDES				Mater.Res.Bull., 18(1983)983	G. P. Meisner,H. C. Ku,H. Barz		
120018	MRB0180983		HfRuAs	Hf1Ru1As1	Hf	1	Ru	1	As	1																			1983																												ZrNiAl			A	6.568		3.842												K		4.93					4.93																																																																																																arc-melting					SUPERCONDUCTING EQUIATOMIC TERNARY TRANSITION METAL ARSENIDES				Mater.Res.Bull., 18(1983)983	G. P. Meisner,H. C. Ku,H. Barz		
120019	MRB0180983		ZrOsAs	Zr1Os1As1	Zr	1	Os	1	As	1																			1983																												ZrNiAl			A	6.602		3.794												K		8					8																																																																																																arc-melting					SUPERCONDUCTING EQUIATOMIC TERNARY TRANSITION METAL ARSENIDES				Mater.Res.Bull., 18(1983)983	G. P. Meisner,H. C. Ku,H. Barz		
120020	MRB0180983		HfOsAs	Hf1Os1As1	Hf	1	Os	1	As	1																			1983																												ZrNiAl			A	6.569		3.808												K		3.2					3.2																																																																																																arc-melting					SUPERCONDUCTING EQUIATOMIC TERNARY TRANSITION METAL ARSENIDES				Mater.Res.Bull., 18(1983)983	G. P. Meisner,H. C. Ku,H. Barz		
120021	MRB0151441		YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																			1980																												LuRuB2			A	5.918	5.297	6.377												K		7.8					7.8																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120022	MRB0151441		(Y,Sc)RuB2	Y0.8Sc0.2Ru1B2	Y	0.8	Sc	0.2	Ru	1	B	2																	1980																												LuRuB2																		K		8.1					8.1																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120023	MRB0151441		LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																			1980																												LuRuB2			A	5.809	5.229	6.284												K		9.99					9.99																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120024	MRB0151441		ScOsB2	Sc1Os1B2	Sc	1	Os	1	B	2																			1980																												LuRuB2			A	5.647	5.178	6.184												K		1.34					1.34																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120025	MRB0151441		YOsB2	Y1Os1B2	Y	1	Os	1	B	2																			1980																												LuRuB2			A	5.905	5.299	6.391												K		2.22					2.22																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120026	MRB0151441		LuOsB2	Lu1Os1B2	Lu	1	Os	1	B	2																			1980																												LuRuB2			A	5.809	5.231	6.318												K		2.66					2.66																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120027	LES0840107		YB2C2	Y1B2C2	Y	1	B	2	C	2																			1982																												YB2C2			A	3.78		7.111												K		3.6					3.6																																																																																																					Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
120028	LES0840107		LaB2C2	La1B2C2	La	1	B	2	C	2																			1982																												YB2C2			A	3.823		7.927												K					1.8																																																																																																							Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
120029	LES0840107		DyB2C2	Dy1B2C2	Dy	1	B	2	C	2																			1982																												YB2C2			A	3.779		7.119												K					1.8																																																																																																							Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
120030	LES0840107		LuB2C2	Lu1B2C2	Lu	1	B	2	C	2																			1982																												YB2C2			A	3.762		6.89												K		2.4					2.4																																																																																																					Electrical properties of rare earth diborodicarbides (RB2C2-type layer compounds)			Department of Applied Chemistry, Faculty of Engineering, Osaka University, Japan	J.Less-Common Metals, 84(1982)107	G.Adachi,J.Shiokawa,T.Sakai		
120031	MRB0171211		Y2Rh3Si5	Y2Rh3Si5	Y	2	Rh	3	Si	5																			1982																												U2Co3Si5			A	9.78	11.69	5.672												K		2.7					2.7																																																																																																arc-melting					Structure, superconductivity and magnetism of new rare earth-rhodium silisides RE2Rh3Si5 of U2Co3Si5-type				Mat.Res.Bull., 17(1982)1211	B.Chevalier,J.Etourneau,P.Lejay		
120032	PLA0750386		Sc2Fe3Si5	Sc2Fe3Si5	Sc	2	Fe	3	Si	5																			1980																												U2Co3Si5																		K		4.5					4.5																																																																																																arc-melting					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
120033	PLA0750386		Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																			1980																												U2Co3Si5																		K		2.4					2.4																																																																																																arc-melting					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
120034	PLA0750386		Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																			1980																												U2Co3Si5																		K		6					6																																																																																																arc-melting					Superconductivity of Rare Earth-Iron Silicides	198002		Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Lett.A,75(1980)386-388	H.F.Braun,Hans F.Braun		
120035	MRB0151441	not s/c. CurieT shows magnetic transition.	TbRuB2	Tb1Ru1B2	Tb	1	Ru	1	B	2																			1980							45.6																					LuRuB2			A	5.897	5.311	6.367												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120036	MRB0151441	not s/c. CurieT shows magnetic transition.	DyRuB2	Dy1Ru1B2	Dy	1	Ru	1	B	2																			1980							21.9																					LuRuB2			A	5.886	5.3	6.352												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120037	MRB0151441	not s/c. CurieT shows magnetic transition.	HoRuB2	Ho1Ru1B2	Ho	1	Ru	1	B	2																			1980							15.5																					LuRuB2			A	5.875	5.287	6.332												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120038	MRB0151441	not s/c. CurieT shows magnetic transition.	ErRuB2	Er1Ru1B2	Er	1	Ru	1	B	2																			1980							5.21																					LuRuB2			A	5.868	5.262	6.323												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120039	MRB0151441	not s/c. CurieT shows magnetic transition.	TmRuB2	Tm1Ru1B2	Tm	1	Ru	1	B	2																			1980							4.07																					LuRuB2			A	5.831	5.254	6.299												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120040	MRB0151441	not s/c. CurieT shows magnetic transition.	TbOsB2	Tb1Os1B2	Tb	1	Os	1	B	2																			1980							39.2																					LuRuB2			A	5.885	5.309	6.392												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120041	MRB0151441	not s/c. CurieT shows magnetic transition.	DyOsB2	Dy1Os1B2	Dy	1	Os	1	B	2																			1980							25.3																					LuRuB2			A	5.869	5.297	6.369												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120042	MRB0151441	not s/c. CurieT shows magnetic transition.	HoOsB2	Ho1Os1B2	Ho	1	Os	1	B	2																			1980							14.2																					LuRuB2			A	5.85	5.286	6.355												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120043	MRB0151441	not s/c. CurieT shows magnetic transition.	ErOsB2	Er1Os1B2	Er	1	Os	1	B	2																			1980							3.8																					LuRuB2			A	5.834	5.274	6.341												K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120044	MRB0151441	not s/c. CurieT shows magnetic transition.	TmOsB2	Tm1Os1B2	Tm	1	Os	1	B	2																			1980							2.26																					LuRuB2																		K					1																																																																																																		arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120045	MRB0151441		YRu4B4	Y1Ru4B4	Y	1	Ru	4	B	4																			1980																										AB4C4		RT4B4																	LuRu4B4 type	K		1.4					1.4																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120046	MRB0151441		YRuB4	Y1Ru1B4	Y	1	Ru	1	B	4																			1980																												YCrB4																		K		1.38					1.38																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120047	MRB0151441		YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																			1980																												LuRuB2																		K		7.8					7.8																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120048	MRB0151441		YOs3B2	Y1Os3B2	Y	1	Os	3	B	2																			1980																												YOs3B2																		K		6					6																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120049	MRB0151441		YOsB4	Y1Os1B4	Y	1	Os	1	B	4																			1980																												YCrB4																		K		1.4					1.4																																																																																																arc-melting					Superconductivity of new ternary borides with the LuRuB2-type structure				Mat.Res.Bull., 15(1980)1441	H.C.Ku,R.N.Shelton		
120050	MRB0151489		YRu3.5Si2	Y1Ru3.5Si2	Y	1	Ru	3.5	Si	2																			1980																																														K		3.51					3.51																																																																																																arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120051	MRB0151489		LaRu3.5Si2	La1Ru3.5Si2	La	1	Ru	3.5	Si	2																			1980																																														K		7.6					7.6																																																																																																arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120052	MRB0151489		ThRu3.5Si2	Th1Ru3.5Si2	Th	1	Ru	3.5	Si	2																			1980																																														K		3.98					3.98																																																																																																arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120053	MRB0151489	not s/c. CurieT shows magnetic transition.	NdRu3.5Si2	Nd1Ru3.5Si2	Nd	1	Ru	3.5	Si	2																			1980							17.95																																							K					1																																																																																																		arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120054	MRB0151489	not s/c. CurieT shows magnetic transition.	DyRu3.5Si2	Dy1Ru3.5Si2	Dy	1	Ru	3.5	Si	2																			1980							14.95																																							K					1																																																																																																		arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120055	MRB0151489	not s/c. CurieT shows magnetic transition.	HoRu3.5Si2	Ho1Ru3.5Si2	Ho	1	Ru	3.5	Si	2																			1980							14.17																																							K					1																																																																																																		arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120056	MRB0151489	not s/c. CurieT shows magnetic transition.	ErRu3.5Si2	Er1Ru3.5Si2	Er	1	Ru	3.5	Si	2																			1980							16.19																																							K					1																																																																																																		arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120057	MRB0151489	not s/c. CurieT shows magnetic transition.	TmRu3.5Si2	Tm1Ru3.5Si2	Tm	1	Ru	3.5	Si	2																			1980							7.5																																							K					1																																																																																																		arc-melting					New ternary superconductors with silicon				Mat.Res.Bull., 15(1980)1489	H.Barz		
120058	PR0335062	dTc/dP in K/GPa 	Sc5Co4Si10	Sc5Co4Si10	Sc	5	Co	4	Si	10																			1986																												Sc5Co4Si10			A	12.01		3.936												K		4.53					4.53			K/GPa	-0.27																																																							580																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120059	PR0335062	dTc/dP in K/GPa 	Sc5Rh4Si10	Sc5Rh4Si10	Sc	5	Rh	4	Si	10																			1986																												Sc5Co4Si10			A	12.325		4.032												K		8.27					8.27			K/GPa	-0.153																																																							450																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120060	PR0335062	dTc/dP in K/GPa 	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			1986																												Sc5Co4Si10			A	12.316		4.076												K		8.29					8.29			K/GPa	-0.256																																																							400																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120061	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Y5Ir4Si10	Y5Ir4Si10	Y	5	Ir	4	Si	10																			1986																												Sc5Co4Si10			A	12.599		4.234												K		3.1					3.1			K/GPa	-0.062																																																							370																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120062	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Lu5Rh4Si10	Lu5Rh4Si10	Lu	5	Rh	4	Si	10																			1986																												Sc5Co4Si10			A	12.502		4.137												K		3.95					3.95			K/GPa	-0.07																																																							340																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120063	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			1986																												Sc5Co4Si10			A	12.475		4.171												K		3.91					3.91			K/GPa	-0.0098																																																							330																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120064	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Y5Rh4Ge10	Y5Rh4Ge10	Y	5	Rh	4	Ge	10																			1986																												Sc5Co4Si10			A	12.953		4.272												K		1.35					1.35			K/GPa	-0.086																																																							340																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120065	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Y5Ir4Ge10	Y5Ir4Ge10	Y	5	Ir	4	Ge	10																			1986																												Sc5Co4Si10			A	12.927		4.308												K		2.76					2.76			K/GPa	-0.059																																																							320																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120066	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Y5Os4Ge10	Y5Os4Ge10	Y	5	Os	4	Ge	10																			1986																												Sc5Co4Si10			A	13.006		4.297												K		9.06					9.06			K/GPa	-0.342																																																							320																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120067	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Lu5Rh4Ge10	Lu5Rh4Ge10	Lu	5	Rh	4	Ge	10																			1986																												Sc5Co4Si10			A	12.85		4.208												K		2.79					2.79			K/GPa	-0.107																																																							300																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120068	PR0335062	dTc/dP in K/GPa. Debye-T estimated using scaling law. 	Lu5Ir4Ge10	Lu5Ir4Ge10	Lu	5	Ir	4	Ge	10																			1986																												Sc5Co4Si10			A	12.831		4.252												K		2.6					2.6			K/GPa	0.021																																																							290																																										Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120069	PR0335062		(Lu,Sc)5Ir4Si	Lu4.5Sc0.5Ir4Si10	Lu	4.5	Sc	0.5	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		6.03					6.03																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120070	PR0335062		(Lu,Sc)5Ir4Si	Lu4Sc1Ir4Si10	Lu	4	Sc	1	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		6.64					6.64																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120071	PR0335062		(Lu,Sc)5Ir4Si	Lu3.5Sc1.5Ir4Si10	Lu	3.5	Sc	1.5	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		7.69					7.69																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120072	PR0335062		(Lu,Sc)5Ir4Si	Lu2.5Sc2.5Ir4Si10	Lu	2.5	Sc	2.5	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		7.93					7.93																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120073	PR0335062		(Lu,Sc)5Ir4Si	Lu1Sc4Ir4Si10	Lu	1	Sc	4	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		7.63					7.63																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120074	PR0335062		(Lu,Sc)5Ir4Si	Lu0.25Sc4.75Ir4Si10	Lu	0.25	Sc	4.75	Ir	4	Si	10																	1986																												Sc5Co4Si10																		K		7.87					7.87																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120075	PR0335062		Lu5(Ir,Rh)4Si10	Lu5Ir3.4Rh0.6Si10	Lu	5	Ir	3.4	Rh	0.6	Si	10																	1986																												Sc5Co4Si10																		K		5.7					5.7																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120076	PR0335062		Lu5(Ir,Rh)4Si10	Lu5Ir3.1Rh0.9Si10	Lu	5	Ir	3.1	Rh	0.9	Si	10																	1986																												Sc5Co4Si10																		K		5.77					5.77																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120077	PR0335062		Lu5(Ir,Rh)4Si10	Lu5Ir2.8Rh1.2Si10	Lu	5	Ir	2.8	Rh	1.2	Si	10																	1986																												Sc5Co4Si10																		K		5.66					5.66																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120078	PR0335062		Lu5(Ir,Rh)4Si10	Lu5Ir2Rh2Si10	Lu	5	Ir	2	Rh	2	Si	10																	1986																												Sc5Co4Si10																		K		5.45					5.45																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120079	PR0335062		Lu5(Ir,Rh)4Si10	Lu5Ir1.2Rh2.8Si10	Lu	5	Ir	1.2	Rh	2.8	Si	10																	1986																												Sc5Co4Si10																		K		4.8					4.8																																																																																																					Superconductivity and electronic instability at high pressure in Sc5Co4Si10-type compounds			Iowa State University,	Phys.Rev.B, 33(1986)5062	H.D.Yang,H.F.Braun,R.N.Shelton		
120080	PR0316971		Pd2ScSn	Pd2Sc1Sn1	Pd	2	Sc	1	Sn	1																			1985																												Heusler			A	6.503													Cu2MnAl, L2<1>	K		2.15					2.15																																																																																																arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120081	PR0316971		Pd2YSn	Pd2Y1Sn1	Pd	2	Y	1	Sn	1																			1985																												Heusler			A	6.716													Cu2MnAl, L2<1>	K		4.55					4.55																																																																																																arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120082	PR0316971		Pd2TbSn	Pd2Tb1Sn1	Pd	2	Tb	1	Sn	1																			1985							-8.6	9																				Heusler			A	6.74													Cu2MnAl, L2<1>	K																																																																																																							arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120083	PR0316971		Pd2DySn	Pd2Dy1Sn1	Pd	2	Dy	1	Sn	1																			1985							-9.3	15																				Heusler			A	6.722													Cu2MnAl, L2<1>	K																																																																																																							arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120084	PR0316971	no magnetic order.	Pd2HoSn	Pd2Ho1Sn1	Pd	2	Ho	1	Sn	1																			1985							-6.2																					Heusler			A	6.705													Cu2MnAl, L2<1>	K																																																																																																							arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120085	PR0316971	no magnetic order.	Pd2ErSn	Pd2Er1Sn1	Pd	2	Er	1	Sn	1																			1985							-7.6																					Heusler			A	6.692													Cu2MnAl, L2<1>	K																																																																																																							arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120086	PR0316971		Pd2TmSn	Pd2Tm1Sn1	Pd	2	Tm	1	Sn	1																			1985							0																					Heusler			A	6.67													Cu2MnAl, L2<1>	K		2.82					2.82																																																																																																arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120087	PR0316971		Pd2YbSn	Pd2Yb1Sn1	Pd	2	Yb	1	Sn	1																			1985							-4.3																					Heusler			A	6.658													Cu2MnAl, L2<1>	K		2.42					2.42																																																																																																arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120088	PR0316971	coexistence of s/c and AF.	Pd2LuSn	Pd2Lu1Sn1	Pd	2	Lu	1	Sn	1																			1985								0.23																				Heusler			A	6.645													Cu2MnAl, L2<1>	K		3.05					3.05																																																																																																arc-melting					Magnetic and Mossbauer studies on rare-earth-containing Heusler alloys Pd2RSn (R=Tb - YB)			Argonne National Lab.	Phys.Rev.B, 31(1985)6971	A.M.Umarji,G.K.Shenoy,S.K.Malik		
120089	MRB0211203		Sc4Rh6Sn19	Sc4Rh6Sn19	Sc	4	Rh	6	Sn	19																			1986																												Tb4Rh6Sn19			A	12.605														K		1.9					1.9																																																																																																					New superconducting ternary compounds in the systems M-M'-X (M=Ca,Sr,Sc,Y,La-Lu; M'=Co,Rh,Ir; X=Ge,Pb)				Mat.Res.Bull., 21(1986)1203	B.Malaman,B.Roques,E.Mc Rae,G.Venturini,J.F.Mareche,M.Kamta		
120090	MRB0211203		Sc4Ir6Sn19	Sc4Ir6Sn19	Sc	4	Ir	6	Sn	19																			1986																												Tb4Rh6Sn19			A	12.629														K		1.4					1.4																																																																																																					New superconducting ternary compounds in the systems M-M'-X (M=Ca,Sr,Sc,Y,La-Lu; M'=Co,Rh,Ir; X=Ge,Pb)				Mat.Res.Bull., 21(1986)1203	B.Malaman,B.Roques,E.Mc Rae,G.Venturini,J.F.Mareche,M.Kamta		
120091	MRB0211203		Ca4Rh6Pb19	Ca4Rh6Pb19	Ca	4	Rh	6	Pb	19																			1986																												Tb4Rh6Sn19			A	14.23														K		3.3					3.3																																																																																																					New superconducting ternary compounds in the systems M-M'-X (M=Ca,Sr,Sc,Y,La-Lu; M'=Co,Rh,Ir; X=Ge,Pb)				Mat.Res.Bull., 21(1986)1203	B.Malaman,B.Roques,E.Mc Rae,G.Venturini,J.F.Mareche,M.Kamta		
120092	CEM0090323	heat treated in NH3 gas	Sr0.2(NH3)xTaS2	Sr0.2Ta1S2	Sr	0.2	Ta	1	S	2																			1974																															A			18.3												K		2.8					2.8																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides			IBM Thomas I.Watson Research Center, New York, USA	J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,S. Kawarazaki,W.W.Shafer		
120093	CEM0090323	heat treated in NH3 gas	Sr0.2(NH3)xMoS2	Sr0.2Mo1S2	Sr	0.2	Mo	1	S	2																			1974																															A			18.7												K		5					5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides			IBM Thomas I.Watson Research Center, New York, USA	J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,S. Kawarazaki,W.W.Shafer		
120094	CEM0090323	heat treated in NH3 gas	Sr0.2(NH3)xWS2	Sr0.2W1S2	Sr	0.2	W	1	S	2																			1974																															A			18.7												K		3.5					3.5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides			IBM Thomas I.Watson Research Center, New York, USA	J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,S. Kawarazaki,W.W.Shafer		
120095	CEM0090323	heat treated in NH3 gas	Sr0.2(NH3)xMoSe2	Sr0.2Mo1Se2	Sr	0.2	Mo	1	Se	2																			1974																															A			19.3												K		5					5																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides			IBM Thomas I.Watson Research Center, New York, USA	J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,S. Kawarazaki,W.W.Shafer		
120096	CEM0090323	heat treated in NH3 gas	Yb0.4(NH3)xWSe2	Yb0.2W1Se2	Yb	0.2	W	1	Se	2																			1974																															A			18.6												K		2.2					2.2																																																																																																					Superconductivity in alkaline earth metal and Yb intercalated group VI layered dichalcogenides			IBM Thomas I.Watson Research Center, New York, USA	J.Solid State Chem., 9(1974)323	A.M.Toxen,G.V.Subba Rao,S. Kawarazaki,W.W.Shafer		
120097	LES0190113		(Y,Th)2C3	Y1.8Th0.2C2.7	Y	1.8	Th	0.2	C	2.7																			1969																												Pu2C3			A	8.2719														K		12					12																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120098	LES0190113		(Y,Th)2C3	Y1.6Th0.4C2.7	Y	1.6	Th	0.4	C	2.7																			1969																												Pu2C3			A	8.302														K		14.7					14.7																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120099	LES0190113		(Y,Th)2C3	Y1.4Th0.6C2.7	Y	1.4	Th	0.6	C	2.7																			1969																												Pu2C3			A	8.334														K		16.4					16.4																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120100	LES0190113		(Y,Th)2C3	Y1.3Th0.7C2.7	Y	1.3	Th	0.7	C	2.7																			1969																												Pu2C3			A	8.376														K		16.8					16.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120101	LES0190113		(Y,Th)2C3	Y1.2Th0.8C2.7	Y	1.2	Th	0.8	C	2.7																			1969																												Pu2C3			A	8.394														K		16					16																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120102	LES0190113		(Y,Th)2C3	Y1Th1C2.7	Y	1	Th	1	C	2.7																			1969																												Pu2C3																		K		15.5					15.5																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120103	LES0190113		(Y,Th)2C3	Y0.8Th1.2C2.7	Y	0.8	Th	1.2	C	2.7																			1969																												Pu2C3			A	8.455														K		15.1					15.1																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120104	LES0190113		(Y,Th)2C3	Y0.6Th1.4C2.7	Y	0.6	Th	1.4	C	2.7																			1969																												Pu2C3			A	8.494														K		14.4					14.4																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120105	LES0190113		(Y,Th)2C3	Y1.4Th0.6C2.4	Y	1.4	Th	0.6	C	2.4																			1969																												Pu2C3			A	8.306														K		15.4					15.4																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120106	LES0190113		(Y,Th)2C3	Y0.6Th1.4C2.5	Y	0.6	Th	1.4	C	2.5																			1969																												Pu2C3			A	8.473														K		14.6					14.6																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120107	LES0190113		(Y,Th)2C3	Y1.4Th0.6C2.8	Y	1.4	Th	0.6	C	2.8																			1969																												Pu2C3			A	8.3552														K		16.3					16.3																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120108	LES0190113		(Y,Th)2C3	Y1.4Th0.6C2.9	Y	1.4	Th	0.6	C	2.9																			1969																												Pu2C3			A	8.364														K		16.3					16.3																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120109	LES0190113		(Y,Th)2C3	Y1.2Th0.8C2.9	Y	1.2	Th	0.8	C	2.9																			1969																												Pu2C3			A	8.383														K		15.8					15.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120110	LES0190113		(Y,Th)2C3	Y0.6Th1.4C2.9	Y	0.6	Th	1.4	C	2.9																			1969																												Pu2C3			A	8.481														K		14.6					14.6																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120111	LES0190113		(Y,Th)2C3	Y1.5Th0.5C3	Y	1.5	Th	0.5	C	3																			1969																												Pu2C3			A	8.34														K		16.7					16.7																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120112	LES0190113		(Y,Th)2C3	Y1.4Th0.6C3	Y	1.4	Th	0.6	C	3																			1969																												Pu2C3			A	8.364														K		16.8					16.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120113	LES0190113		(Y,Th)2C3	Y1.4Th0.6C3.1	Y	1.4	Th	0.6	C	3.1																			1969																												Pu2C3			A	8.362														K		17					17																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120114	LES0190113		(Y,Au)2C3	Y1.8Au0.2C2.6	Y	1.8	Au	0.2	C	2.6																			1969																												Pu2C3			A	8.2503														K		10.1					10.1																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120115	LES0190113		(Y,Ge)2C3	Y1.8Ge0.2C2.7	Y	1.8	Ge	0.2	C	2.7																			1969																												Pu2C3			A	8.286														K		10.6					10.6																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120116	LES0190113		(Y,Si)2C3	Y1.8Si0.2C2.7	Y	1.8	Si	0.2	C	2.7																			1969																												Pu2C3			A	8.272														K		11.3					11.3																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120117	LES0190113		(Y,Sn)2C3	Y1.8Sn0.2C2.7	Y	1.8	Sn	0.2	C	2.7																			1969																												Pu2C3			A	8.2431														K		10.2					10.2																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120118	LES0190113		(Y,Ru)2C3	Y1.8Ru0.2C2.7	Y	1.8	Ru	0.2	C	2.7																			1969																												Pu2C3			A	8.2408														K		11.2					11.2																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120119	LES0190113		(Y,Nb)2C3	Y1.8Nb0.2C2.7	Y	1.8	Nb	0.2	C	2.7																			1969																												Pu2C3			A	8.2389														K		10.8					10.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120120	LES0190113		(Y,Ti)2C3	Y1.8Ti0.2C2.7	Y	1.8	Ti	0.2	C	2.7																			1969																												Pu2C3			A	8.23														K		10.7					10.7																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120121	LES0190113		(Y,Ti)2C3	Y1.8Ti0.2C2.9	Y	1.8	Ti	0.2	C	2.9																			1969																												Pu2C3			A	8.2363														K		14.2					14.2																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120122	LES0190113		(Y,Zr)2C3	Y1.8Zr0.2C2.9	Y	1.8	Zr	0.2	C	2.9																			1969																												Pu2C3			A	8.236														K		13					13																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120123	LES0190113		(Y,Mo)2C3	Y1.8Mo0.2C2.9	Y	1.8	Mo	0.2	C	2.9																			1969																												Pu2C3			A	8.239														K		13.8					13.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120124	LES0190113		(Y,W)2C3	Y1.8W0.2C2.9	Y	1.8	W	0.2	C	2.9																			1969																												Pu2C3			A	8.242														K		14.5					14.5																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120125	LES0190113		(Y,Bi)2C3	Y1.8Bi0.2C2.9	Y	1.8	Bi	0.2	C	2.9																			1969																												Pu2C3			A	8.2396														K		9.35					9.35																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120126	LES0190113		(Y,U)2C3	Y1.7U0.3C2.9	Y	1.7	U	0.3	C	2.9																			1969																												Pu2C3			A	8.217														K					4																																																																																																		arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120127	LES0190113		(Y,V)2C3	Y1.8V0.2C2.9	Y	1.8	V	0.2	C	2.9																			1969																												Pu2C3			A	8.24														K		11.5					11.5																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120128	LES0190113		(Y,Cr)2C3	Y1.8Cr0.2C2.9	Y	1.8	Cr	0.2	C	2.9																			1969																												Pu2C3			A	8.2384														K		12.4					12.4																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120129	LES0190113		(Y,Ti)2C3	Y1.4Ti0.6C3	Y	1.4	Ti	0.6	C	3																			1969																												Pu2C3			A	8.237														K		12.9					12.9																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120130	LES0190113		(Y,Ti)2C3	Y1.8Ti0.2C3.1	Y	1.8	Ti	0.2	C	3.1																			1969																												Pu2C3			A	8.2382														K		14.5					14.5																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120131	LES0190113		(Y,W)2C3	Y1.8W0.2C3.1	Y	1.8	W	0.2	C	3.1																			1969																												Pu2C3			A	8.24														K		14.8					14.8																																																																																																arc-melting, then high-T high-P synthesis					High-pressure synthesis of yttrium-thorium sesquicarbide: A new high-temperature superconductor			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 19(1969)113	A.L.Giorgi,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120132	LES0300217		(Th,Ce)2C3	Th1.8Ce0.2C3	Th	1.8	Ce	0.2	C	3																			1973																												Pu2C3			A	8.5445														K					4																																																																																																		high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120133	LES0300217		(Th,Pr)2C3	Th1.8Pr0.2C3	Th	1.8	Pr	0.2	C	3																			1973																												Pu2C3			A	8.5563														K					4																																																																																																		high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120134	LES0300217		(Th,Pr)2C3	Th1.6Pr0.4C3	Th	1.6	Pr	0.4	C	3																			1973																												Pu2C3			A	8.5602														K					4																																																																																																		high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120135	LES0300217		(Th,Nd)2C3	Th1.8Nd0.2C3	Th	1.8	Nd	0.2	C	3																			1973																												Pu2C3			A	8.5555														K					4																																																																																																		high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120136	LES0300217		(Th,Ho)2C3	Th1.8Ho0.2C3	Th	1.8	Ho	0.2	C	3																			1973																												Pu2C3			A	8.5448														K		5.4					5.4																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120137	LES0300217		(Th,Ho)2C3	Th1.6Ho0.4C3	Th	1.6	Ho	0.4	C	3																			1973																												Pu2C3			A	8.526														K		5.5					5.5																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120138	LES0300217		(Th,Ho)2C3	Th1.4Ho0.6C3	Th	1.4	Ho	0.6	C	3																			1973																												Pu2C3			A	8.499														K		5.2					5.2																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120139	LES0300217		(Th,Er)2C3	Th1.9Er0.1C3	Th	1.9	Er	0.1	C	3																			1973																												Pu2C3			A	8.5434														K		6.8					6.8																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120140	LES0300217		(Th,Er)2C3	Th1.8Er0.2C3	Th	1.8	Er	0.2	C	3																			1973																												Pu2C3			A	8.54														K		8.2					8.2																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120141	LES0300217		(Th,Er)2C3	Th1.6Er0.4C3	Th	1.6	Er	0.4	C	3																			1973																												Pu2C3			A	8.523														K		8.2					8.2																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120142	LES0300217		(Th,Er)2C3	Th1.4Er0.6C3	Th	1.4	Er	0.6	C	3																			1973																												Pu2C3			A	8.486														K		8.1					8.1																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120143	LES0300217		(Th,Er)2C3	Th1.2Er0.8C3	Th	1.2	Er	0.8	C	3																			1973																												Pu2C3			A	8.455														K		7					7																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120144	LES0300217		(Th,Er)2C3	Th1Er1C3	Th	1	Er	1	C	3																			1973																												Pu2C3			A	8.412														K		4.6					4.6																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120145	LES0300217		(Th,Lu)2C3	Th1.8Lu0.2C3	Th	1.8	Lu	0.2	C	3																			1973																												Pu2C3			A	8.5278														K		10.3					10.3																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120146	LES0300217		(Th,Lu)2C3	Th1.6Lu0.4C3	Th	1.6	Lu	0.4	C	3																			1973																												Pu2C3			A	8.495														K		10.9					10.9																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120147	LES0300217		(Th,Lu)2C3	Th1.4Lu0.3C3	Th	1.4	Lu	0.3	C	3																			1973																												Pu2C3			A	8.461														K		11.7					11.7																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120148	LES0300217		(Th,Lu)2C3	Th1.2Lu0.8C3	Th	1.2	Lu	0.8	C	3																			1973																												Pu2C3			A	8.426														K		11.6					11.6																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120149	LES0300217		(Th,Sc)2C3	Th1.8Sc0.2C3	Th	1.8	Sc	0.2	C	3																			1973																												Pu2C3			A	8.5362														K		6.7					6.7																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120150	LES0300217		(Th,Sc)2C3	Th1.6Sc0.4C3	Th	1.6	Sc	0.4	C	3																			1973																												Pu2C3			A	8.531														K		6.8					6.8																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120151	LES0300217		(Th,Sc)2C3	Th1.4Sc0.6C3	Th	1.4	Sc	0.6	C	3																			1973																												Pu2C3			A	8.5297														K		7.2					7.2																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120152	LES0300217		(Th,Sc)2C3	Th1.2Sc0.8C3	Th	1.2	Sc	0.8	C	3																			1973																												Pu2C3			A	8.529														K		7.1					7.1																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120153	LES0300217		(Th,Sc)2C3	Th1Sc1C3	Th	1	Sc	1	C	3																			1973																												Pu2C3			A	8.543														K		6.5					6.5																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120154	LES0300217		(Th,Sc)2C3	Th0.8Sc1.2C3	Th	0.8	Sc	1.2	C	3																			1973																												Pu2C3			A	8.55														K		6					6																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120155	LES0300217		(Th,Sc)2C3	Th0.6Sc1.4C3	Th	0.6	Sc	1.4	C	3																			1973																												Pu2C3																		K		5.4					5.4																																																																																																high-p (3-4 Gpa) synthesis					High pressure thorium-rare-earth carbide superconductors			Los Alamos National Lab, Los Alamos, New Mexico,USA	J.Less-Common Metals, 30(1973)217	A.L.Giorgi,E.G.Szklarz,M.C.Krupka		
120156	MRB0210859		In3.3Mo15Se19	In3.3Mo15Se19	In	3.3	Mo	15	Se	19																			1986																												Mo15Se19			A	9.406		18.915												K		4					4																																																																																																					On several new ternary molybdenum sulfide phase M3.4Mo15S19 (M=vacancy, Li,Na,K,Zn,Cd,Sn,and Tl)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 21(1986)859	G.W.Hull,J.M.Tarascon		
120157	MRB0210859		Mo15Se19	Mo15Se19	Mo	15	Se	19																					1986																												Mo15Se19			A	9.218		18.077												K		4.3					4.3																																																																																																					On several new ternary molybdenum sulfide phase M3.4Mo15S19 (M=vacancy, Li,Na,K,Zn,Cd,Sn,and Tl)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 21(1986)859	G.W.Hull,J.M.Tarascon		
120158	MRB0200935		In3Mo15Se19	In3Mo15Se19	In	3	Mo	15	Se	19																			1985																												Mo15Se19			A	9.8		19.49												K		3.32					3.32																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120159	MRB0200935		Li3Mo15Se19	Li3Mo15Se19	Li	3	Mo	15	Se	19																			1985																												Mo15Se19			A	9.724		19.47												K		3.5					3.5																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120160	MRB0200935		Li7Mo15Se19	Li7Mo15Se19	Li	7	Mo	15	Se	19																			1985																												Mo15Se19			A	10.028		19.28												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120161	MRB0200935		Na3Mo15Se19	Na3Mo15Se19	Na	3	Mo	15	Se	19																			1985																												Mo15Se19			A	9.712		19.68												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120162	MRB0200935		K2InMo15Se19	K2In1Mo15Se19	K	2	In	1	Mo	15	Se	19																	1985																												Mo15Se19			A	9.79		19.59												K		1.3					1.3																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120163	MRB0200935		Sn2Mo15Se19	Sn2.1Mo15Se19	Sn	2.1	Mo	15	Se	19																			1985																												Mo15Se19			A	9.776		19.79												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120164	MRB0200935		Sn2Mo15Se19	Sn2.6Mo15Se19	Sn	2.6	Mo	15	Se	19																			1985																												Mo15Se19			A	9.89		19.57												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120165	MRB0200935		Pb2.3Mo15Se19	Pb2.3Mo15Se19	Pb	2.3	Mo	15	Se	19																			1985																												Mo15Se19			A	9.611		19.59												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120166	MRB0200935		Tl3.3Mo15Se19	Tl3.3Mo15Se19	Tl	3.3	Mo	15	Se	19																			1985																												Mo15Se19			A	9.853		19.41												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120167	MRB0200935		In2Mo15Se19	In2Mo15Se19	In	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.69		58.1												K		1.5					1.5																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120168	MRB0200935		Li2Mo15Se19	Li2Mo15Se19	Li	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.637		58.16												K		2.6					2.6																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120169	MRB0200935		Li7Mo15Se19	Li7Mo15Se19	Li	7	Mo	15	Se	19																			1985																												Mo15Se19			A	10.077		57.3												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120170	MRB0200935		Na2Mo15Se19	Na2Mo15Se19	Na	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.611		58.51												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120171	MRB0200935		K2Mo15Se19	K2Mo15Se19	K	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.727		58.17												K		2.1					2.1																																																																																																					Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120172	MRB0200935		Sn2Mo15Se19	Sn2Mo15Se19	Sn	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.676		57.98												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120173	MRB0200935		Sn2.5Mo15Se19	Sn2.5Mo15Se19	Sn	2.5	Mo	15	Se	19																			1985																												Mo15Se19			A	9.776		57.79												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120174	MRB0200935		Pb2Mo15Se19	Pb2Mo15Se19	Pb	2	Mo	15	Se	19																			1985																												Mo15Se19			A	9.683		57.78												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120175	MRB0200935		Pb2.15Mo15Se19	Pb2.15Mo15Se19	Pb	2.15	Mo	15	Se	19																			1985																												Mo15Se19			A	9.68		57.77												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120176	MRB0200935		Cd2.5Mo15Se19	Cd2.5Mo15Se19	Cd	2.5	Mo	15	Se	19																			1985																												Mo15Se19			A	9.97		56.7												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120177	MRB0200935		Cd4Mo15Se19	Cd4Mo15Se19	Cd	4	Mo	15	Se	19																			1985																												Mo15Se19			A	10.03		56.89												K					0.5																																																																																																							Synthesis, structural and physical properties of the ternary molybdenum chalcogenide phase Mo16Se19 and of the related compounds M2Mo15Se19 and M3Mo15Se19 (M=group IA metal; Sn,Pb:Cd)			Bell, Murray Hill,NJ,USA	Mat.Res.Bull., 20(1985)935	G.W.Hull,J.M.Tarascon,J.V.Waszczak		
120178	PCS0312653		NaPb3	Na1Pb3	Na	1	Pb	3																					1970																												Cu3Al			A	4.888														K		5.62					5.62																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120179	PCS0312653		CaTl3	Ca1Tl3	Ca	1	Tl	3																					1970																												Cu3Al			A	4.796														K		2.04					2.04																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120180	PCS0312653		CaPb3	Ca1Pb3	Ca	1	Pb	3																					1970																												Cu3Al			A	4.91														K		0.65					0.65																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120181	PCS0312653		SrBi3	Bi3Sr1	Bi	3	Sr	1																					1970																												Cu3Al			A	5.035														K		5.7					5.7																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120182	PCS0312653		YIn3	In3Y1	In	3	Y	1																					1970																												Cu3Al			A	4.592														K		0.78					0.78																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120183	PCS0312653		YTl3	Tl3Y1	Tl	3	Y	1																					1970																												Cu3Al			A	4.678														K		1.52					1.52																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120184	PCS0312653		YPb3	Pb3Y1	Pb	3	Y	1																					1970																												Cu3Al			A	4.813														K		4.72					4.72																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120185	PCS0312653		LaIn3	In3La1	In	3	La	1																					1970																												Cu3Al			A	4.739														K		0.7					0.7																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120186	PCS0312653		LaTl3	La1Tl3	La	1	Tl	3																					1970																												Cu3Al			A	4.799														K		1.63					1.63																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120187	PCS0312653		LaPb3	La1Pb3	La	1	Pb	3																					1970																												Cu3Al			A	4.905														K		4.1					4.1																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120188	PCS0312653		LaSn3	La1Sn3	La	1	Sn	3																					1970																												Cu3Al			A	4.771														K		6.02					6.02																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120189	PCS0312653		YbAl3	Al3Yb1	Al	3	Yb	1																					1970																												Cu3Al			A	4.203														K		0.94					0.94																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120190	PCS0312653		YbIn3	In3Yb1	In	3	Yb	1																					1970																												Cu3Al			A	4.616														K					0.05																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120191	PCS0312653		YbPb3	Pb3Yb1	Pb	3	Yb	1																					1970																												Cu3Al			A	4.859														K		0.23					0.23																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120192	PCS0312653		LuGa3	Ga3Lu1	Ga	3	Lu	1																					1970																												Cu3Al			A	4.191														K		2.3					2.3																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120193	PCS0312653		LuIn3	In3Lu1	In	3	Lu	1																					1970																												Cu3Al			A	4.547														K		0.24					0.24																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120194	PCS0312653		ThIn3	In3Th1	In	3	Th	1																					1970																												Cu3Al			A	4.694														K					0.05																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120195	PCS0312653		ThTl3	Th1Tl3	Th	1	Tl	3																					1970																												Cu3Al			A	4.748														K		0.87					0.87																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120196	PCS0312653		ThPb3	Pb3Th1	Pb	3	Th	1																					1970																												Cu3Al			A	4.853														K		5.55					5.55																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120197	PCS0312653		ThSn3	Sn3Th1	Sn	3	Th	1																					1970																												Cu3Al			A	4.714														K		3.33					3.33																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120198	PCS0312653		ZrHg3	Hg3Zr1	Hg	3	Zr	1																					1970																												Cu3Al			A	4.368														K		3.28					3.28																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120199	PCS0312653		UAl3	Al3U1	Al	3	U	1																					1970																												Cu3Al			A	4.266														K					0.05																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120200	PCS0312653		UIn3	In3U1	In	3	U	1																					1970																												Cu3Al			A	4.595														K					0.05																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120201	PCS0312653		CeIn3	Ce1In3	Ce	1	In	3																					1970																												Cu3Al			A	4.687														K					0.07																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120202	PCS0312653		CeSn3	Ce1Sn3	Ce	1	Sn	3																					1970																												Cu3Al			A	4.717														K					0.07																																																																																																		arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120203	PCS0312653		BaBi3	Ba1Bi3	Ba	1	Bi	3																					1970																												Cu3Al			A	5.19		5.16												K		5.8					5.8																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120204	PCS0312653		SrPb3	Pb3Sr1	Pb	3	Sr	1																					1970																												Cu3Al			A	4.962		5.025												K		1.85					1.85																																																																																																arc-melting					Oscillatory dependence of superconductive critical temperature on number of valency electrons in Cu3Au-type alloys			Philips Research Lab, Netherlands	J.Phys.Chem.Solids, 31(1970)2653	E.E.Havinga,H.Damsma,M.H.van Maaren		
120205	LES0780099	monoclinic beta=90.9	YRh3B2	Y1Rh3B2	Y	1	Rh	3	B	2																			1981																															A	5.377	9.325	3.102											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120206	LES0780099	monoclinic beta=91	TbRh3B2	Tb1Rh3B2	Tb	1	Rh	3	B	2																			1981								45																							A	5.39	9.335	3.1											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120207	LES0780099	monoclinic beta=90.9	DyRh3B2	Dy1Rh3B2	Dy	1	Rh	3	B	2																			1981								35																							A	5.379	9.331	3.093											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120208	LES0780099	monoclinic beta=91	HoRh3B2	Ho1Rh3B2	Ho	1	Rh	3	B	2																			1981								24.2																							A	5.366	9.307	3.1											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120209	LES0780099	monoclinic beta=90.9	ErRh3B2	Er1Rh3B2	Er	1	Rh	3	B	2																			1981								20.4																							A	5.362	9.288	3.099											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120210	LES0780099	monoclinic beta=90.8	TmRh3B2]	Tm1Rh3B2	Tm	1	Rh	3	B	2																			1981								11.8																							A	5.357	9.285	3.091											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120211	LES0780099	monoclinic beta=90.9	YbRh3B2	Yb1Rh3B2	Yb	1	Rh	3	B	2																			1981																															A	5.355	9.28	3.09											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120212	LES0780099	monoclinic beta=90.9	LuRh3B2	Lu1Rh3B2	Lu	1	Rh	3	B	2																			1981																															A	5.353	9.276	3.089											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120213	LES0780099	monoclinic beta=92.1	ScIr3B2	Sc1Ir3B2	Sc	1	Ir	3	B	2																			1981																															A	5.344	9.307	3.062											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120214	LES0780099	monoclinic beta=92.8	YIr3B2	Y1Ir3B2	Y	1	Ir	3	B	2																			1981																															A	5.428	9.406	3.107											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120215	LES0780099	monoclinic beta=90.8	CeIr3B2	Ce1Ir3B2	Ce	1	Ir	3	B	2																			1981																															A	5.502	9.526	3.09											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120216	LES0780099	monoclinic beta=90.8	NdIr3B2	Nd1Ir3B2	Nd	1	Ir	3	B	2																			1981								4.72																							A	5.513	9.54	3.084											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120217	LES0780099	monoclinic beta=90.8	SmIr3B2	Sm1Ir3B2	Sm	1	Ir	3	B	2																			1981								12.6																							A	5.492	9.506	3.076											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120218	LES0780099	monoclinic beta=91	GdIr3B2	Gd1Ir3B2	Gd	1	Ir	3	B	2																			1981								29.8																							A	5.466	9.473	3.092											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120219	LES0780099	monoclinic beta=91.1	TbIr3B2	Tb1Ir3B2	Tb	1	Ir	3	B	2																			1981								6.1																							A	5.459	9.464	3.084											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120220	LES0780099	monoclinic beta=91.1	DyIr3B2	Dy1Ir3B2	Dy	1	Ir	3	B	2																			1981								17.7																							A	5.437	9.393	3.106											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120221	LES0780099	monoclinic beta=91.2	HoIr3B2	Ho1Ir3B2	Ho	1	Ir	3	B	2																			1981								12.9																							A	5.42	9.393	3.107											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120222	LES0780099	monoclinic beta=91.2	ErIr3B2	Er1Ir3B2	Er	1	Ir	3	B	2																			1981								11.9																							A	5.409	9.399	3.101											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120223	LES0780099	monoclinic beta=91.3	TmIr3B2	Tm1Ir3B2	Tm	1	Ir	3	B	2																			1981								5.69																							A	5.404	9.371	3.097											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120224	LES0780099	monoclinic beta=91.3	YbIr3B2	Yb1Ir3B2	Yb	1	Ir	3	B	2																			1981																															A	5.401	9.353	3.099											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120225	LES0780099	monoclinic beta=91.4	LuIr3B2	Lu1Ir3B2	Lu	1	Ir	3	B	2																			1981																															A	5.394	9.354	3.08											monoclinic	K					1.2																																																																																																		arc-melting					Crystal structure and physical properties of new ternary rare earth borides			University of California, San Diego	J.Less-Common Met., 78(1981)99-107	G.P.Meisner,H.C.Ku		
120226	LES0920177		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1983																															A	6.4169	7.3215	3.8623												K		3.46					3.46																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120227	LES0920177		NbRuP	Nb1Ru1P1	Nb	1	Ru	1	P	1																			1983																															A	6.318	7.173	3.719												K																																																																																																							arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120228	LES0920177		TaRuP	Ta1Ru1P1	Ta	1	Ru	1	P	1																			1983																															A	6.288	7.164	3.713												K																																																																																																							arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120229	LES0920177		ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1983																												Fe2P			A	6.459		3.778												K		13					13																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120230	LES0920177		ZrRhP	Zr1Rh1P1	Zr	1	Rh	1	P	1																			1983																															A	6.483	7.393	3.787												K		1.55					1.55																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120231	LES0920177		NbRhP	Nb1Rh1P1	Nb	1	Rh	1	P	1																			1983																															A	6.306	7.187	3.737												K		4.08					4.08																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120232	LES0920177		TaRhP	Ta1Rh1P1	Ta	1	Rh	1	P	1																			1983																															A	6.253	7.18	3.736												K		4.41					4.41																																																																																																arc-melting					Superconductivity and crystal structure of a new class of ternary transition metal phosphides TT'P (T=Zr,Nb,Ta and T'=Ru,Rh)				J.Less Comon Met., 92(1983)177	J.W.Richardson,J.W.Richardson,Jr.,R.A.Jacobson,R.Muller,R.N.Shelton		
120233	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	TiOsP	Ti1Os1P1	Ti	1	Os	1	P	1																			1985																																														K					1.7																																																																																																							New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120234	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	ZrOsP	Zr1Os1P1	Zr	1	Os	1	P	1																			1985																																														K		6.57					6.57																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120235	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	HfOsP	Hf1Os1P1	Hf	1	Os	1	P	1																			1985																																														K		5.53					5.53																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120236	MRB0200517		YRhSi	Y1Rh1Si1	Y	1	Rh	1	Si	1																			1985																																														K					1.7																																																																																																							New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120237	MRB0200517		YIrSi	Y1Ir1Si1	Y	1	Ir	1	Si	1																			1985																																														K		2.7					2.7																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120238	MRB0200517	details in J.Less-Common Metals, 92(1983)177	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1985																																														K		3.82					3.82																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120239	MRB0200517	details in J.Less-Common Metals, 92(1983)177	NbRuP	Nb1Ru1P1	Nb	1	Ru	1	P	1																			1985																																														K					1.7																																																																																																							New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120240	MRB0200517	details in J.Less-Common Metals, 92(1983)177	TaRuP	Ta1Ru1P1	Ta	1	Ru	1	P	1																			1985																																														K					1.7																																																																																																							New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120241	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	TiRuP	Ti1Ru1P1	Ti	1	Ru	1	P	1																			1985																																														K		1.33					1.33																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120242	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1985																																														K		11.45					11.45																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120243	MRB0200517	details in Proc.Natl.Acad.Sci.USA, 77(1980)3132	HfRuP	Hf1Ru1P1	Hf	1	Ru	1	P	1																			1985																																														K		11.89					11.89																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120244	MRB0200517	details in Mater.Res.Bull., 18()983	ZrRuAs	Zr1Ru1As1	Zr	1	Ru	1	As	1																			1985																																														K		11.05					11.05																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120245	MRB0200517	details in Mater.Res.Bull., 18()983	HfRuAs	Hf1Ru1As1	Hf	1	Ru	1	As	1																			1985																																														K		4.65					4.65																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120246	MRB0200517	details in Mater.Res.Bull., 18()983	ZrOsAs	Zr1Os1As1	Zr	1	Os	1	As	1																			1985																																														K		8					8																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120247	MRB0200517	details in Mater.Res.Bull., 18()983	HfOsAs	Hf1Os1As1	Hf	1	Os	1	As	1																			1985																																														K		3.2					3.2																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120248	MRB0200517	details in J.Less-Common Metals, 92(1983)177	ZrRhP	Zr1Rh1P1	Zr	1	Rh	1	P	1																			1985																																														K		1.55					1.55																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120249	MRB0200517	details in J.Less-Common Metals, 92(1983)177	NbRhP	Nb1Rh1P1	Nb	1	Rh	1	P	1																			1985																																														K		4.42					4.42																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120250	MRB0200517	details in J.Less-Common Metals, 92(1983)177	TaRhP	Ta1Rh1P1	Ta	1	Rh	1	P	1																			1985																																														K		4.86					4.86																																																																																																					New superconducting equiatomic ternary silisides MIrSi (M=Y,Zr,Hf) with TiNiSi-type structure (ANTI-PbCl2)				Mat.Res.Bull., 20(1985)517	B.Chevalier,J.Etourneau,P.Hagenmuller,Wang Xian-Zhong		
120251	LES1050139	high temperature phase	YIr2Si2	Y1Ir2Si2	Y	1	Ir	2	Si	2																			1985																												CaBe2Ge2																		K		2.6					2.6																																																																																																arc-melting					Influence of composition on the structural and superconducting properties of the two polymorphic forms of iridium- or silicon-substituted YIr2Si2				J.Less-Common Met., 105(1985)139	B.Chevalier,J.Etourneau,M.Hirjak,P.Hagenmuller,P.Lejay		
120252	LES1050139	low temperature phase. Tc(on)=2.5 K. R is not zero at 1.5 K.	YIr2Si2	Y1Ir2Si2	Y	1	Ir	2	Si	2																			1985																												ThCr2Si2																		K		2.5					2.5																																																																																																arc-melting					Influence of composition on the structural and superconducting properties of the two polymorphic forms of iridium- or silicon-substituted YIr2Si2				J.Less-Common Met., 105(1985)139	B.Chevalier,J.Etourneau,M.Hirjak,P.Hagenmuller,P.Lejay		
120253	LES1050139	quenched sample	Y2Ir3Si5	Y2Ir3Si5	Y	2	Ir	3	Si	5																			1985																												U2Co3Si5			A	9.877	11.693	5.714												K		3.05					3.05																																																																																																arc-melting					Influence of composition on the structural and superconducting properties of the two polymorphic forms of iridium- or silicon-substituted YIr2Si2				J.Less-Common Met., 105(1985)139	B.Chevalier,J.Etourneau,M.Hirjak,P.Hagenmuller,P.Lejay		
120254	LES0190253	Ge stabilized Sc4C3 phase.	Sc(C,Ge)0.75	Sc1C0.75Ge0.01	Sc	1	C	0.75	Ge	0.01																			1969																												Sc4C3			A	7.214														K					4																																																																																																		arc-melting + ANN(1300C)					Preparation and superconductivity of germanium-stabilized Sc13C10				J.Less-Common Met., 19(1969)253	A.L.Giorgi,B.T.Matthias,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120255	LES0190253	Ge stabilized Sc13C10 phase.	Sc(C,Ge)0.75	Sc1C0.75Ge0.02	Sc	1	C	0.75	Ge	0.02																			1969																												Sc13C10			A	8.5283														K		8.5					8.5																																																																																																arc-melting + ANN(1300C)					Preparation and superconductivity of germanium-stabilized Sc13C10				J.Less-Common Met., 19(1969)253	A.L.Giorgi,B.T.Matthias,E.G.Szklarz,M.C.Krupka,N.H.Krikorian		
120256	LES0830L47		ThIr2	Ir2Th1	Ir	2	Th	1																					1982																															A	7.6644														K		5.72					5.72																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120257	LES0830L47		Th(Ir,Os)2	Th1Ir1.8Os0.2	Th	1	Ir	1.8	Os	0.2																			1982																															A	7.6672														K		5.66					5.66																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120258	LES0830L47		Th(Ir,Os)2	Th1Ir1.6Os0.4	Th	1	Ir	1.6	Os	0.4																			1982																															A	7.6747														K		5.15					5.15																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120259	LES0830L47		Th(Ir,Os)2	Th1Ir1.4Os0.6	Th	1	Ir	1.4	Os	0.6																			1982																															A	7.6793														K		4.41					4.41																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120260	LES0830L47		Th(Ir,Os)2	Th1Ir1.3Os0.7	Th	1	Ir	1.3	Os	0.7																			1982																															A	7.6793														K		2.36					2.36																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120261	LES0830L47		Th(Ir,Os)2	Th1Ir1.2Os0.8	Th	1	Ir	1.2	Os	0.8																			1982																															A	7.6891														K		3.16					3.16																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120262	LES0830L47		Th(Ir,Os)2	Th1Ir1Os1	Th	1	Ir	1	Os	1																			1982																															A	7.6879														K		3.61					3.61																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120263	LES0830L47		Th(Ir,Os)2	Th1Ir0.8Os1.2	Th	1	Ir	0.8	Os	1.2																			1982																															A	7.6937														K		3.22					3.22																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120264	LES0830L47		Th(Ir,Os)2	Th1Ir0.6Os1.4	Th	1	Ir	0.6	Os	1.4																			1982																															A	7.696														K		3.73					3.73																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120265	LES0830L47		Th(Ir,Os)2	Th1Ir0.4Os1.6	Th	1	Ir	0.4	Os	1.6																			1982																															A	7.6983														K		3.56					3.56																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120266	LES0830L47		Th(Ir,Os)2	Th1Ir0.2Os1.8	Th	1	Ir	0.2	Os	1.8																			1982																															A	7.7006														K		2.93					2.93																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120267	LES0830L47		Th(Ir,Os)2	Th1Ir0.1Os1.9	Th	1	Ir	0.1	Os	1.9																			1982																																														K		2.25					2.25																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120268	LES0830L47		Th(Ir,Ru)2	Th1Ir1.8Ru0.2	Th	1	Ir	1.8	Ru	0.2																			1982																															A	7.6632														K		4.86					4.86																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120269	LES0830L47		Th(Ir,Ru)2	Th1Ir1.6Ru0.4	Th	1	Ir	1.6	Ru	0.4																			1982																															A	7.6603														K		2.87					2.87																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120270	LES0830L47		Th(Ir,Ru)2	Th1Ir1.4Ru0.6	Th	1	Ir	1.4	Ru	0.6																			1982																															A	7.6598														K		2.08					2.08																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120271	LES0830L47	R=not zero at 1 K	Th(Ir,Ru)2	Th1Ir1.2Ru0.8	Th	1	Ir	1.2	Ru	0.8																			1982																															A	7.6563														K		1.45					1.45																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120272	LES0830L47		Th(Ir,Ru)2	Th1Ir1Ru1	Th	1	Ir	1	Ru	1																			1982																															A	7.6575														K		2.53					2.53																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120273	LES0830L47		Th(Ir,Ru)2	Th1Ir0.8Ru1.2	Th	1	Ir	0.8	Ru	1.2																			1982																															A	7.6563														K		2.53					2.53																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120274	LES0830L47		Th(Ir,Ru)2	Th1Ir0.6Ru1.4	Th	1	Ir	0.6	Ru	1.4																			1982																															A	7.6552														K		2.87					2.87																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120275	LES0830L47		Th(Ir,Ru)2	Th1Ir0.4Ru1.6	Th	1	Ir	0.4	Ru	1.6																			1982																															A	7.6534														K		2.87					2.87																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120276	LES0830L47		Th(Ir,Ru)2	Th1Ir0.2Ru1.8	Th	1	Ir	0.2	Ru	1.8																			1982																															A	7.6546														K		3.1					3.1																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120277	LES0830L47		ThRu2	Ru2Th1	Ru	2	Th	1																					1982																															A	7.6523														K		4.01					4.01																																																																																																arc-melting + ANN(1100C)					Superconductivity of Th(Ir,Os)2 and Th(Ir,Ru)2 alloys				J.Less-Common Met., 83(1982)L47	A.C.Lawson,J.L.Smith,J.S.Houghton,M.Dewees		
120278	PHC2290065	Tc shows Tc(on). Delta-Tc = 0.5 K.	ThPt2B2C	Th1Pt2B2C1	Th	1	Pt	2	B	2	C	1																	1994																												LuNi2B2C			A	3.83		10.86												K		6.5					6.5																																																																																																arc-melting					Superconductivity to 21K in intermetallic thorium-based boride carbides	1994		Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093-0319, USA	Physica.C,229(1994)65-69	J. Herrmann,J.Herrmann,J.L. Sarrao,J.L.Sarrao,M.B. Maple,M.B.Maple,M.C. de Andrade,M.C.de Andrade,R.J. Cava,R.J.Cava,S.H. Han,S.H.Han,Z. Fisk,Z.Fisk		
120279	PHC2290065	Tc shows Tc(on). Delta-Tc = 1 K.	ThNi2B2C	Th1Ni2B2C1	Th	1	Ni	2	B	2	C	1																	1994																												LuNi2B2C			A	3.7		10.19												K		6					6																																																																																																arc-melting					Superconductivity to 21K in intermetallic thorium-based boride carbides	1994		Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093-0319, USA	Physica.C,229(1994)65-69	J. Herrmann,J.Herrmann,J.L. Sarrao,J.L.Sarrao,M.B. Maple,M.B.Maple,M.C. de Andrade,M.C.de Andrade,R.J. Cava,R.J.Cava,S.H. Han,S.H.Han,Z. Fisk,Z.Fisk		
120280	PHC2290065	Tc shows Tc(on). Delta-Tc = 0.5 K.	ThPd2B2C	Th1Pd2B2C1	Th	1	Pd	2	B	2	C	1																	1994																												LuNi2B2C			A	3.84		10.67												K		14.5					14.5																																																																																																arc-melting					Superconductivity to 21K in intermetallic thorium-based boride carbides	1994		Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093-0319, USA	Physica.C,229(1994)65-69	J. Herrmann,J.Herrmann,J.L. Sarrao,J.L.Sarrao,M.B. Maple,M.B.Maple,M.C. de Andrade,M.C.de Andrade,R.J. Cava,R.J.Cava,S.H. Han,S.H.Han,Z. Fisk,Z.Fisk		
120281	PHC2290065	compositions are nominal value. 1221-phase = minor phase. dTc/dP in K/GPa. Hc2(0) using WHH theory. Tc shows Tc(on). 	ThPd3B3C	Th1Pd3B3C1	Th	1	Pd	3	B	3	C	1																	1994																																														K		21.5					21.5			K/GPa	-0.12																T		1.6							T/K		0.15																																																																	arc-melting					Superconductivity to 21K in intermetallic thorium-based boride carbides	1994		Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093-0319, USA	Physica.C,229(1994)65-69	J. Herrmann,J.Herrmann,J.L. Sarrao,J.L.Sarrao,M.B. Maple,M.B.Maple,M.C. de Andrade,M.C.de Andrade,R.J. Cava,R.J.Cava,S.H. Han,S.H.Han,Z. Fisk,Z.Fisk		
120282	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	LaRu2	La1Ru2	La	1	Ru	2																					1987																												MgCu2(Laves)																	MgCu2, C15	K		4.416					4.416			K/GPa	-0.091																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120283	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.95Ce0.05Ru2	La	0.95	Ce	0.05	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		3.616					3.616			K/GPa	-0.107																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120284	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.9Ce0.1Ru2	La	0.9	Ce	0.1	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		3.012					3.012			K/GPa	-0.109																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120285	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.85Ce0.15Ru2	La	0.85	Ce	0.15	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		2.444					2.444			K/GPa	-0.11																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120286	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.8Ce0.2Ru2	La	0.8	Ce	0.2	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		2.01					2.01			K/GPa	-0.099																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120287	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.76Ce0.24Ru2	La	0.76	Ce	0.24	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		1.468					1.468			K/GPa	-0.072																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120288	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.72Ce0.28Ru2	La	0.72	Ce	0.28	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		1.278					1.278			K/GPa	-0.048																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120289	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.6Ce0.4Ru2	La	0.6	Ce	0.4	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		0.727					0.727			K/GPa	-0.032																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120290	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.5Ce0.5Ru2	La	0.5	Ce	0.5	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		0.449					0.449			K/GPa	-0.013																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120291	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.46Ce0.54Ru2	La	0.46	Ce	0.54	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		0.668					0.668																																																																																																arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120292	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.4Ce0.6Ru2	La	0.4	Ce	0.6	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		1.3					1.3			K/GPa	0.018																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120293	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.35Ce0.65Ru2	La	0.35	Ce	0.65	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		1.647					1.647			K/GPa	0.045																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120294	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.3Ce0.7Ru2	La	0.3	Ce	0.7	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		2.134					2.134			K/GPa	0.051																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120295	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.25Ce0.75Ru2	La	0.25	Ce	0.75	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		3.196					3.196			K/GPa	0.107																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120296	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.2Ce0.8Ru2	La	0.2	Ce	0.8	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		4.227					4.227			K/GPa	0.11																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120297	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.15Ce0.85Ru2	La	0.15	Ce	0.85	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		5.872					5.872			K/GPa	0.084																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120298	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.1Ce0.9Ru2	La	0.1	Ce	0.9	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		7.194					7.194			K/GPa	0.016																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120299	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	(La,Ce)Ru2	La0.05Ce0.95Ru2	La	0.05	Ce	0.95	Ru	2																			1987																												MgCu2(Laves)																	MgCu2, C15	K		7.181					7.181			K/GPa	0.018																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120300	SSC0240465	dTc/dp in K/Gpa. Hydrostatic pressure.	CeRu2	Ce1Ru2	Ce	1	Ru	2																					1987																												MgCu2(Laves)																	MgCu2, C15	K		6.221					6.221			K/GPa	0.022																																																																																												arc-melting					Superconducting transition temperature, its pressure dependence and structural transformation in (La,Ce)Ru2 alloys				Solid State Commun., 24(1977)465	A.C.Lawson,K.Baberschke,R.N.Shelton		
120301	LES0950267	melting point=1490 C. space-G=P4. density=5.77 g/cm3. Tc from [ref].	La5B2C6	La5B2C6	La	5	B	2	C	6																			1983																												Ce5B2C6			A	8.585		12.313												K		6.9					6.9																																																																																																melt in induction furnace in Ar					The crystal structure of the superconducting lanthanum borocarbide La5B2C6				J.Less-Common Met., 95(1983)267	Josef Bauer,Odile Bars		
130000	LTP0480503	e-ph = 0.45.	Mo6S8	Mo6S8	Mo	6	S	8																					1982																												Chevrel																		K		1.8					1.8																																																								mj/mol.K2	28.3		230																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130001	LTP0480503	e-ph = 0.93. Hc(0)=0.2 T.	Mo6S6Br2	Mo6S6Br2	Mo	6	S	6	Br	2																			1982																												Chevrel																		K		13					13																																																								mj/mol.K2	71.5		195																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130002	LTP0480503	e-ph = 1.01. Hc(0)=0.195 T.	Mo6S6I2	Mo6S6I2	Mo	6	S	6	I	2																			1982																												Chevrel																		K		13					13																																																								mj/mol.K2	64		170																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130003	LTP0480503	e-ph = 0.75. Hc(0)=0.14 T.	Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10.7					10.7																																																								mj/mol.K2	48.5		250																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130004	LTP0480503	e-ph = 0.5. Hc(0)=0.028 T.	ZnMo6S8	Zn1Mo6S8	Zn	1	Mo	6	S	8																			1982																												Chevrel																		K		2.8					2.8																																																								mj/mol.K2	25.3		225																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130005	LTP0480503	e-ph = 0.75. Hc(0)=0.075 T.	AgMo6S8	Ag1Mo6S8	Ag	1	Mo	6	S	8																			1982																												Chevrel																		K		7.7					7.7																																																								mj/mol.K2	30		180																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130006	LTP0480503	e-ph = 0.5.	CdMo6S8	Cd1Mo6S8	Cd	1	Mo	6	S	8																			1982																												Chevrel																		K		1.8					1.8																																																								mj/mol.K2	27		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130007	LTP0480503	e-ph = 1.10. Hc(0)=0.197 T.	SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.7					11.7																																																								mj/mol.K2	107		135																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130008	LTP0480503	e-ph = 1.20. Hc(0)=0.272 T.	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		13.7					13.7																																																								mj/mol.K2	125		140																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130009	LTP0480503	e-ph = 0.71. Hc(0)=0.056 T.	LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1982																												Chevrel																		K		6.8					6.8																																																								mj/mol.K2	22.6		180																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130010	LTP0480503	e-ph = 0.76. Hc(0)=0.077 T.	Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.3					6.3																																																								mj/mol.K2	40		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130011	LTP0480503	e-ph = 0.81. Hc(0)=0.089 T.	Mo6Se6Br2	Mo6Se6Br2	Mo	6	Se	6	Br	2																			1982																												Chevrel																		K		6.7					6.7																																																								mj/mol.K2	44		133																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130012	LTP0480503	e-ph = 0.71. Hc(0)=0.067 T.	CuMo6Se8	Cu1Mo6Se8	Cu	1	Mo	6	Se	8																			1982																												Chevrel																		K		5.9					5.9																																																								mj/mol.K2	40		155																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130013	LTP0480503	e-ph = 0.54. Hc(0)=0.03 T.	CdMo6Se8	Cd1Mo6Se8	Cd	1	Mo	6	Se	8																			1982																												Chevrel																		K		2.4					2.4																																																								mj/mol.K2	55		145																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130014	LTP0480503	e-ph = 0.6. Hc(0)=0.03 T.	SnMo6Se8	Sn1Mo6Se8	Sn	1	Mo	6	Se	8																			1982																												Chevrel																		K		3.4					3.4																																																								mj/mol.K2	26.3		140																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130015	LTP0480503	e-ph = 0.66. Hc(0)=0.04 T.	PbMo6Se8	Pb1Mo6Se8	Pb	1	Mo	6	Se	8																			1982																												Chevrel																		K		4					4																																																								mj/mol.K2	31		125																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130016	LTP0480503	e-ph = 1.04. Hc(0)=0.184 T.	LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		11.6					11.6																																																								mj/mol.K2	83		150																																										Determination of the Energy Gap of Superconducting Chevrel and A15 Compounds from Heat Capacity Measurements			Sektion Chemie der Bergakademie Freiberg, Freiberg,East Germany	J.Low Temp.Phys., 48(1982)503	B.Pietrass,C.Hohlfeld		
130017	REV198201		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		15					15																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130018	REV198201		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		14					14																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130019	REV198201		LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1982																												Chevrel																		K		7.1					7.1																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130020	REV198201		GdMo6S8	Gd1Mo6S8	Gd	1	Mo	6	S	8																			1982																												Chevrel																		K		1.4					1.4																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130021	REV198201		LuMo6S8	Lu1Mo6S8	Lu	1	Mo	6	S	8																			1982																												Chevrel																		K		2.2					2.2																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130022	REV198201		Mo6S8	Mo6S8	Mo	6	S	8																					1982																												Chevrel																		K		1.6					1.6																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130023	REV198201		Mo6S6I2	Mo6S6I2	Mo	6	S	6	I	2																			1982																												Chevrel																		K		1.4					1.4																																																																																																					"""Superconducting ternary compounds I: prospect and prospectives"""				Springer-Verlag, 1982, p1-24	F.Fisher,M.B.Maple		
130024	REV1976137		Pb0.92Mo6S7.5	Pb0.92Mo6S7.5	Pb	0.92	Mo	6	S	7.5																			1976																												Chevrel																		K		13.98					13.98			K/GPa	-1.6																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130025	REV1976137		PbMo5.1S4	Pb1Mo5.1S4	Pb	1	Mo	5.1	S	4																			1976																												Chevrel																		K		14.51					14.51			K/GPa	-1.05																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130026	REV1976137		Sn0.6Mo3S4	Sn0.6Mo3S4	Sn	0.6	Mo	3	S	4																			1976																												Chevrel																		K		14.45					14.45			K/GPa	-1.78																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130027	REV1976137		Sn0.6Mo3S4	Sn0.6Mo3S4	Sn	0.6	Mo	3	S	4																			1976																												Chevrel																		K		13.05					13.05			K/GPa	-1.382																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130028	REV1976137		CuMo3S4	Cu1Mo3S4	Cu	1	Mo	3	S	4																			1976																												Chevrel																		K		10.66					10.66			K/GPa	-1.072																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130029	REV1976137		AgMo4S5	Ag1Mo4S5	Ag	1	Mo	4	S	5																			1976																												Chevrel																		K		7.77					7.77			K/GPa	-0.6																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130030	REV1976137		Tl0.45Bi0.46Mo6S7.5	Tl0.45Bi0.46Mo6S7.5	Tl	0.45	Bi	0.46	Mo	6	S	7.5																	1976																												Chevrel																		K		6.41					6.41			K/GPa	-0.34																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130031	REV1976137	Tc(p) non-linear	ZnMo5S6	Zn1Mo5S6	Zn	1	Mo	5	S	6																			1976																												Chevrel																		K		3.12					3.12																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130032	REV1976137	Tc(p) non-linear	CdMo5S6	Cd1Mo5S6	Cd	1	Mo	5	S	6																			1976																												Chevrel																		K		2.67					2.67																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130033	REV1976137		ScMo6S7	Sc1Mo6S7	Sc	1	Mo	6	S	7																			1976																												Chevrel																		K		2.67					2.67			K/GPa	1.093																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130034	REV1976137		YMo6S7	Y1Mo6S7	Y	1	Mo	6	S	7																			1976																												Chevrel																		K		2.66					2.66			K/GPa	-0.581																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130035	REV1976137		MgMo6S7	Mg1Mo6S7	Mg	1	Mo	6	S	7																			1976																												Chevrel																		K		2.72					2.72			K/GPa	-0.25																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130036	REV1976137		Cu0.7Mo3Se4	Cu0.7Mo3Se4	Cu	0.7	Mo	3	Se	4																			1976																												Chevrel																		K		5.9					5.9			K/GPa	-1.12																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130037	REV1976137	Tc(p) non-linear	Ag0.7Mo4Se5	Ag0.7Mo4Se5	Ag	0.7	Mo	4	Se	5																			1976																												Chevrel																		K		5.96					5.96																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130038	REV1976137		Sn0.7Mo3Se4	Sn0.7Mo3Se4	Sn	0.7	Mo	3	Se	4																			1976																												Chevrel																		K		4.85					4.85			K/GPa	-0.403																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130039	REV1976137		Pb1.2Mo6Se8	Pb1.2Mo6Se8	Pb	1.2	Mo	6	Se	8																			1976																												Chevrel																		K		4.32					4.32			K/GPa	-0.645																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130040	REV1976137		YMo6Se8	Y1Mo6Se8	Y	1	Mo	6	Se	8																			1976																												Chevrel																		K		6.38					6.38			K/GPa	-1.052																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130041	BOOK1982		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.3					6.3																				T		8.6							T/K		1.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130042	BOOK1982		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.2					6.2																				T		16.5							T/K		3.6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130043	BOOK1982		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		11.3					11.3																				T									T/K		7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130044	BOOK1982		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		10.8					10.8																				T		44.5							T/K		7.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130045	BOOK1982		LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1982																												Chevrel																		K		5.8					5.8																				T		5.4							T/K		1.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130046	BOOK1982		Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10					10																				T		19.2							T/K		2.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130047	BOOK1982		Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10.5					10.5																				T		15.3							T/K		1.9																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130048	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		13.4					13.4																				T		34.4							T/K		3.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130049	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.8					11.8																				T		34							T/K		4.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130050	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.7					11.7																				T		36							T/K		3.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130051	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		14.4					14.4																				T		60							T/K		6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130052	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		12.6					12.6																				T		50							T/K		5.8																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130053	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		13.3					13.3																				T		60							T/K		6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130054	LTP0430371	tunnel	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1981																												Chevrel																		K																																																							4.8	1																																																				Tunneling spectroscopy on the superconducting Chevrel-phase compounds Cu1.8Mo6S8 and PbMo6S8				J.Low Temp.Phys., 43(1981)371	H.Wuhl,U.Poppe		
130055	SSC0330419	NMR	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1980																												Chevrel																		K																																																							3.5	6																																																				NMR study of Chevrel phase superconductor				Solid State Commun., 33(1980)419	K.Asayama,N.Sano,T.Taniguchi		
130056	LTP0060171	dTc/dP = 3.7 E-5  K/bar.	V3Si	Si1V3	Si	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		16.85					16.85	MTC130056		K/GPa	0.37																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130057	LTP0060171		V3Si	Si1V3	Si	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		16.83					16.83			K/GPa	0.31																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130058	LTP0060171		V0.78Si0.22	Si0.22V0.78	Si	0.22	V	0.78																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		14.38					14.38			K/GPa	0.26																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130059	LTP0060171		V3Ga	Ga1V3	Ga	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		13.87					13.87			K/GPa	0.105																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130060	LTP0060171		V3Sn	Sn1V3	Sn	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.65					3.65			K/GPa	0.049																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130061	LTP0060171		V3Ge	Ge1V3	Ge	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.1					6.1			K/GPa	0.81																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130062	LTP0060171		V3Ge0.9Al0.1	V3Ge0.9Al0.1	V	3	Ge	0.9	Al	0.1																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		8.8					8.8			K/GPa	0.347																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130063	LTP0060171		V3Ge0.8Al0.2	V3Ge0.8Al0.2	V	3	Ge	0.8	Al	0.2																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		11.02					11.02			K/GPa	0.253																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130064	LTP0060171		V3Ge0.7Al0.3	V3Ge0.7Al0.3	V	3	Ge	0.7	Al	0.3																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		11.17					11.17			K/GPa	0.263																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130065	LTP0060171	Heat treatment(800C, 1 d))	V3Au	Au1V3	Au	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		1.755					1.755			K/GPa	0.0875																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130066	LTP0060171	Heat treatment(600C, 4 w)	V3Au	Au1V3	Au	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.731					2.731			K/GPa	0.13																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130067	LTP0060171		V3Pt	Pt1V3	Pt	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.63					2.63			K/GPa	-0.041																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130068	LTP0060171	Heat treatment(800C, 2 d)	V3Pt	Pt1V3	Pt	1	V	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.18					3.18			K/GPa	-0.086																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130069	LTP0060171		V0.67Ir0.33	Ir0.33V0.67	Ir	0.33	V	0.67																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		1.6					1.6			K/GPa	-0.021																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130070	LTP0060171		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		17.832					17.832	MTC130070		K/GPa	-0.14																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130071	LTP0060171		Nb3Al	Al1Nb3	Al	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		17.11					17.11			K/GPa	-0.07																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130072	LTP0060171		Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		6.281					6.281			K/GPa	-0.114																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130073	LTP0060171		Nb0.78(Al0.75Ge0.25)0.22	Nb0.78Al0.165Ge0.055	Nb	0.78	Al	0.165	Ge	0.055																			1972																												Cr3Si(A15)																	Cr3Si, A15	K		20.29					20.29			K/GPa	-0.02																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130077	LTP0060171		Nb3Ir	Ir1Nb3	Ir	1	Nb	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.07					2.07			K/GPa	0.055																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130078	LTP0060171		Nb3Rh	Nb3Rh1	Nb	3	Rh	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.797					2.797			K/GPa	-0.032																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130079	LTP0060171		Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		8.111					8.111			K/GPa	-0.063																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130080	LTP0060171	Heat treatment(800C, 1 d)	Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		8.174					8.174																																																																																																					Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130081	LTP0060171	Heat treatment(900C, 10 d)	Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		10.53					10.53			K/GPa	0.188																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130082	LTP0060171	Heat treatment(650C, 1 d + 1200C,5h)	Ta3Sn	Sn1Ta3	Sn	1	Ta	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		5.82					5.82			K/GPa	-0.116																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130083	LTP0060171		Ti3Sb	Sb1Ti3	Sb	1	Ti	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		5.1					5.1			K/GPa	-0.005																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130084	LTP0060171	Heat treatment(800C, 36h)	Ti3Sb	Sb1Ti3	Sb	1	Ti	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		5.47					5.47			K/GPa	0.016																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130085	LTP0060171	Heat treatment(1000C, 1 d + 600C,2w)	Ti3Ir	Ir1Ti3	Ir	1	Ti	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		4.97					4.97			K/GPa	0.147																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130086	LTP0060171	Heat treatment(900C, 1 month)	Cr0.72Ru0.28	Cr0.72Ru0.28	Cr	0.72	Ru	0.28																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.468					3.468			K/GPa	0.013																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130087	LTP0060171	Heat treatment(1200C, 1 d, then quench)	Cr0.72Os0.28	Cr0.72Os0.28	Cr	0.72	Os	0.28																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		3.862					3.862			K/GPa	0.006																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130088	LTP0060171		Mo3Si	Mo3Si1	Mo	3	Si	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		1.402					1.402			K/GPa	-0.035																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130089	LTP0060171		Mo3Ge	Ge1Mo3	Ge	1	Mo	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		2.166					2.166			K/GPa	-0.045																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130090	LTP0060171		Mo3Ge	Ge1Mo3	Ge	1	Mo	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		1.6					1.6			K/GPa	-0.047																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130091	LTP0060171	Heat treatment(1800C, 2h + 600C,2w)	Mo3Os	Mo3Os1	Mo	3	Os	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		11.69					11.69			K/GPa	-0.095																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130092	LTP0060171	Heat treatment(2000C, 4h + 1100C,2w)	Mo3Os	Mo3Os1	Mo	3	Os	1																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		12.5					12.5			K/GPa	-0.096																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130093	LTP0060171	Heat treatment(1800C, 2h + 600C,2w)	Mo3Ir	Ir1Mo3	Ir	1	Mo	3																					1972																												Cr3Si(A15)																	Cr3Si, A15	K		8.174					8.174			K/GPa	-0.081																																																																																																	Superconductivity at high pressure in the A15 compounds				J.Low Temp.Phys., 6(1972)171	T.F.Smith		
130094	SCI2000535		Am	Am1	Am	1																							1978																																													dhcp	K		0.79					0.79																																																																																																					Superconductivity of Americium				Science, 2000(1978)535	J.L.Smith,R.G.Haire		
130095	SSC0310961	gamma in mj/mol.K2. gap from specific heat.	La3S4	La3S4	La	3	S	4																				3	1979																																														K																											T		15.1														A		46										5.2								mj/mol.K2	8.3		224																																										High critical magnetic field superconductor La3S4				Solid State Commun., 31(1979)961	H.Bach,K.Westerholt,R.Wendemuth,S.Methfessel		
130096	JPC008L474		Sn1.2Mo6S8	Sn1.2Mo6.35S8	Sn	1.2	Mo	6.35	S	8																			1975																												Chevrel																		K		10.7					10.7																				T		27.5												MHC30096																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130097	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn1.08Eu0.1Mo6.35S8	Sn	1.08	Eu	0.1	Mo	6.35	S	8																	1975																												Chevrel																		K		10.9					10.9																				T		30.9																																																																															Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130098	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.96Eu0.2Mo6.35S8	Sn	0.96	Eu	0.2	Mo	6.35	S	8																	1975																												Chevrel																		K		10.7					10.7																				T		37.1																																																																															Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130099	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.84Eu0.3Mo6.35S8	Sn	0.84	Eu	0.3	Mo	6.35	S	8																	1975																												Chevrel																		K		10.6					10.6																				T		37.1																																																																															Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130100	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.72Eu0.4Mo6.35S8	Sn	0.72	Eu	0.4	Mo	6.35	S	8																	1975																												Chevrel																		K		10.1					10.1																				T		39.6																																																																															Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130101	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.6Eu0.5Mo6.35S8	Sn	0.6	Eu	0.5	Mo	6.35	S	8																	1975																												Chevrel																		K		10.2					10.2																				T		40.7												MHC30101																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130102	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.48Eu0.6Mo6.35S8	Sn	0.48	Eu	0.6	Mo	6.35	S	8																	1975																												Chevrel																		K		9.2					9.2																																																																																																					Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130103	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.36Eu0.7Mo6.35S8	Sn	0.36	Eu	0.7	Mo	6.35	S	8																	1975																												Chevrel																		K		7.94					7.94																				T		36.3												MHC30103																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130104	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.24Eu0.8Mo6.35S8	Sn	0.24	Eu	0.8	Mo	6.35	S	8																	1975																												Chevrel																		K		6					6																				T		32.4												MHC30104																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130105	JPC008L474		(Sn,Eu)1.2Mo6S8	Sn0.12Eu0.9Mo6.35S8	Sn	0.12	Eu	0.9	Mo	6.35	S	8																	1975																												Chevrel																		K		0.94					0.94																																																																																																					Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130106	JPC008L474		(Pb,Eu,Gd)Mo6S8	Pb0.7Eu0.3Gd0.2Mo6S8	Pb	0.7	Eu	0.3	Gd	0.2	Mo	6	S	8															1975																												Chevrel																		K		14.3					14.3																				T		66.3												MHC30106																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130107	JPC008L474		(Pb,Eu)Mo6S8	Pb0.7Eu0.3Mo6.35S8	Pb	0.7	Eu	0.3	Mo	6.35	S	8																	1975																												Chevrel																		K		13.6					13.6																				T		63.5												MHC30107																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130108	JPC008L474		(Pb,Eu)Mo6S8	Pb0.7Eu0.3Mo6.35S8	Pb	0.7	Eu	0.3	Mo	6.35	S	8																	1975																												Chevrel																		K		11					11																				T		48.4												MHC30108																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130109	JPC008L474		PbMo6S8	Pb1Mo6.35S8	Pb	1	Mo	6.35	S	8																			1975																												Chevrel																		K		12					12																				T		42.1												MHC30109																																																																			Compensation of the paramagnetic effect on Hc2 by magnetic moments: 700 kG superconductors				J.Phys.C: Solid State Phys., 8(1975)L474	F.Fischer,M.Decroux,M.Sergent,R.Chevrel,S.Roth		
130110	SSC0240747		Tb1.2Mo6S8	Tb1.2Mo6S8	Tb	1.2	Mo	6	S	8																			1977																												Chevrel																		K		1.64					1.64																																		MHC30110																																																																			Magnetic ordering i the superconducting state of rare earth molybdenum sulphides, (RE)1.2Mo6S8 (RE=Tb, Dy, and Er)				Solid State Commun., 24(1977)747	F.Fischer,M.Ishikawa		
130111	SSC0240747		Dy1.2Mo6S8	Dy1.2Mo6S8	Dy	1.2	Mo	6	S	8																			1977																												Chevrel																		K		1.72					1.72																																		MHC30111																																																																			Magnetic ordering i the superconducting state of rare earth molybdenum sulphides, (RE)1.2Mo6S8 (RE=Tb, Dy, and Er)				Solid State Commun., 24(1977)747	F.Fischer,M.Ishikawa		
130112	SSC0240747	re-entrant s/c	Er1.2Mo6S8	Er1.2Mo6S8	Er	1.2	Mo	6	S	8																			1977																												Chevrel																		K		2.1					2.1	MRES30112																																																																																																				Magnetic ordering i the superconducting state of rare earth molybdenum sulphides, (RE)1.2Mo6S8 (RE=Tb, Dy, and Er)				Solid State Commun., 24(1977)747	F.Fischer,M.Ishikawa		
130113	CEM0330043	semicond.	Mo2Re4S2	Mo2Re4S2	Mo	2	Re	4	S	2																			1980																												Chevrel			A	9.34		10.42												K																																																																																																							Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130114	CEM0330043		Mo6S6Br2	Mo6S6Br2	Mo	6	S	6	Br	2																			1980																												Chevrel			A	9.54		10.36												K		13.8					13.8																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130115	CEM0330043		Mo6S6I2	Mo6S6I2	Mo	6	S	6	I	2																			1980																												Chevrel			A	9.64		10.44												K		14					14																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130116	CEM0330043		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1980																												Chevrel			A	9.57		11.15												K		6.25					6.25																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130117	CEM0330043	semicond.	Mo2Re4Se8	Mo2Re4Se8	Mo	2	Re	4	Se	8																			1980																												Chevrel			A	9.67		10.74												K																																																																																																							Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130118	CEM0330043	semicond.	Mo4Ru2Se8	Mo4Ru2Se8	Mo	4	Ru	2	Se	8																			1980																												Chevrel			A	9.69		10.82												K																																																																																																							Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130119	CEM0330043		Mo6Se5Cl3	Mo6Se5Cl3	Mo	6	Se	5	Cl	3																			1980																												Chevrel			A	9.64		11.05												K		5.7					5.7																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130120	CEM0330043		Mo6Se5Br3	Mo6Se5Br3	Mo	6	Se	5	Br	3																			1980																												Chevrel			A	9.82		10.83												K		7.1					7.1																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130121	CEM0330043		Mo6Se5I3	Mo6Se5I3	Mo	6	Se	5	I	3																			1980																												Chevrel			A	10.02		10.73												K		4.2					4.2																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130122	CEM0330043		Mo5.25Nb0.75Se8	Mo5.25Nb0.75Se8	Mo	5.25	Nb	0.75	Se	8																			1980																												Chevrel			A	9.6		11.16												K		6.2					6.2																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130123	CEM0330043		Mo6Te8	Mo6Te8	Mo	6	Te	8																					1980																												Chevrel			A	10.2		11.66												K					1.7																																																																																																		Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130124	CEM0330043		Mo4Re2Te8	Mo4Re2Te8	Mo	4	Re	2	Te	8																			1980																												Chevrel			A	10.22		11.51												K		3.5					3.5																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130125	CEM0330043		Mo4Ru2Te8	Mo4Ru2Te8	Mo	4	Ru	2	Te	8																			1980																												Chevrel			A	10.28		11.35												K					1.7																																																																																																		Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130126	CEM0330043		Mo6Te6Cl2	Mo6Te6Cl2	Mo	6	Te	6	Cl	2																			1980																												Chevrel			A	10.19		11.68												K																																																																																																							Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130127	CEM0330043		Mo6Te5Br3	Mo6Te5Br3	Mo	6	Te	5	Br	3																			1980																												Chevrel			A	10.2		11.66												K																																																																																																							Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130128	CEM0330043		Mo6Te5I3	Mo6Te5I3	Mo	6	Te	5	I	3																			1980																												Chevrel			A	10.32		11.51												K		2.4					2.4																																																																																																Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130129	CEM0330043		Mo5.25Nb0.75Te8	Mo5.25Nb0.75Te8	Mo	5.25	Nb	0.75	Te	8																			1980																												Chevrel			A	10.21		11.7												K					1.7																																																																																																		Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130130	CEM0330043		Mo5.25Ta0.75Te8	Mo5.25Ta0.75Te8	Mo	5.25	Ta	0.75	Te	8																			1980																												Chevrel			A	10.21		11.7												K					1.7																																																																																																		Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130131	CEM0330043		Mo4.66Rh1.33Te8	Mo4.66Rh1.33Te8	Mo	4.66	Rh	1.33	Te	8																			1980																												Chevrel			A	10.25		11.53												K					1.7																																																																																																		Heat(1150C) in sealed quartz					Synthesis and electrical properties of new chalcogenide compounds containing mixed (Mo, Me)6 octahedral clusters (Me=Ru or Rh)				J.Solid State Chem., 33(1980)43	A.Perrin,F.Fischer,M.Sergent,R.Chevrel		
130132	MRB0151025	not s/c. R(300K)=13 mOhm. thermopower(300K)=-3.6 uV/K.	Mo6S6O2	Mo6S6O2	Mo	6	S	6	O	2																			1980																												Chevrel			A	9.14		10.82												K																																																																																																							solid state reaction					Synthesis and properties of O-containing chevrel phases, AxMo6S6O2 (A=Co, Ni, Cu, and Pb)				Mat.Res.Bull., 15(1980)1025	A.M.Umarji,G.Rangarajan,G.V.Subba Rao,R.Srinivasan,V.Sankaranarayanan		
130133	MRB0151025	R(300K)=0.9 mOhm. thermopower(300K)=4.4 uV/K.	Cu2Mo6S6O2	Cu2Mo6S6O2	Cu	2	Mo	6	S	6	O	2																	1980																												Chevrel			A	9.67		10.19												K		9					9																																																																																																solid state reaction					Synthesis and properties of O-containing chevrel phases, AxMo6S6O2 (A=Co, Ni, Cu, and Pb)				Mat.Res.Bull., 15(1980)1025	A.M.Umarji,G.Rangarajan,G.V.Subba Rao,R.Srinivasan,V.Sankaranarayanan		
130134	MRB0151025	semicond. R(300K)=0.6 mOhm. thermopower(300K)=0.4 uV/K.	Ni2Mo6S6O2	Ni2Mo6S6O2	Ni	2	Mo	6	S	6	O	2																	1980																												Chevrel			A	9.47		10.19												K																																																																																																							solid state reaction					Synthesis and properties of O-containing chevrel phases, AxMo6S6O2 (A=Co, Ni, Cu, and Pb)				Mat.Res.Bull., 15(1980)1025	A.M.Umarji,G.Rangarajan,G.V.Subba Rao,R.Srinivasan,V.Sankaranarayanan		
130135	MRB0151025	semicond. R(300K)=0.8 mOhm. thermopower(300K)=13.8 uV/K.	Co2Mo6S6O2	Co2Mo6S6O2	Co	2	Mo	6	S	6	O	2																	1980																												Chevrel			A	9.49		10.11												K																																																																																																							solid state reaction					Synthesis and properties of O-containing chevrel phases, AxMo6S6O2 (A=Co, Ni, Cu, and Pb)				Mat.Res.Bull., 15(1980)1025	A.M.Umarji,G.Rangarajan,G.V.Subba Rao,R.Srinivasan,V.Sankaranarayanan		
130136	MRB0151025	R(300K)=3.2 mOhm. thermopower(300K)=5.1 uV/K.	PbMo6S6O2	Pb1Mo6S6O2	Pb	1	Mo	6	S	6	O	2																	1980																												Chevrel			A	9.14		11.5												K		11.7					11.7																																																																																																solid state reaction					Synthesis and properties of O-containing chevrel phases, AxMo6S6O2 (A=Co, Ni, Cu, and Pb)				Mat.Res.Bull., 15(1980)1025	A.M.Umarji,G.Rangarajan,G.V.Subba Rao,R.Srinivasan,V.Sankaranarayanan		
130137	LTP0440553	specific heat, thermal conductivity, thermal expansion were measured. magnetic order at 0.4 K. effective moment = 7.51.  s/c persist to 60 mK.	TmRh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1981							-0.46																			AB4C4		RT4B4																	LuRh4B4 type	K		9.8					9.8																																		MHC30137																																																														arc-melting + ANN(1200C, 800C)					Observation of the coexistence of superconductivity and long-range magnetic order in TmRh4B4				J.Low Temp.Phys., 44(1981)553	H.B.MacKay,H.C.Hamaker,H.R.Ott,L.D.Woolf,M.B.Maple,M.S.Torikachvili,W.Odoni		
130138	SSC0310139	NdRh4B4+RhB+NdRh6B4. excess RhB stabilized NdRh4B4 phase. Specific heat anomaly due to magnetic order of Nd appears at 1.31K  and 0.89 K.	NdRh6B6	Nd1Rh6B6	Nd	1	Rh	6	B	6																			1979							-6.2																			AB4C4		RT4B4																	LuRh4B4 type	K		5.4					5.4																																		MHC30138																																																																			Possible observation of the coexistence of superconductivity and long-range magnetic order in NdRh4B4				Solid State Commun., 31(1979)139	H.B.MacKay,H.C.Hamaker,L.D.Woolf		
130139	SSC0320289	magnetic order at 0.87 K (by specific heat). moment = 0.632.	SmRh4B4	Sm1Rh4B4	Sm	1	Rh	4	B	4																			1979							-1.93																			AB4C4		RT4B4																	LuRh4B4 type	K		2.72					2.72																																		MHC30139																																																														arc-melting + ANN(1200C, 800C)					Coexistence of superconductivity and antiferromagnetic order in SmRh4B4				Solid State Commun., 32(1979)289	H.B.MacKay,H.C.Hamaker,L.D.Woolf,M.B.Maple,Z.Fisk		
130140	BOOK1982		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.3					6.3																				T		8.6							T/K		1.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130141	BOOK1982		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1982																												Chevrel																		K		6.2					6.2																				T		16.5							T/K		3.6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130142	BOOK1982		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		11.3					11.3																				T									T/K		7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130143	BOOK1982		LaMo6Se8	La1Mo6Se8	La	1	Mo	6	Se	8																			1982																												Chevrel																		K		10.8					10.8																				T		44.5							T/K		7.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130144	BOOK1982		LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1982																												Chevrel																		K		5.8					5.8																				T		5.4							T/K		1.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130145	BOOK1982		Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10					10																				T		19.2							T/K		2.5																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130146	BOOK1982		Cu1.8Mo6S8	Cu1.8Mo6S8	Cu	1.8	Mo	6	S	8																			1982																												Chevrel																		K		10.5					10.5																				T		15.3							T/K		1.9																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130147	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		13.4					13.4																				T		34.4							T/K		3.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130148	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.8					11.8																				T		34							T/K		4.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130149	BOOK1982		SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																			1982																												Chevrel																		K		11.7					11.7																				T		36							T/K		3.7																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130150	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		14.4					14.4																				T		60							T/K		6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130151	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		12.6					12.6																				T		50							T/K		5.8																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130152	BOOK1982		PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1982																												Chevrel																		K		13.3					13.3																				T		60							T/K		6																																																																						"Topics in current physics ""Superconductivity in ternary compounds II"""				Springer-Verlag, 1982,	F.Fischer,M.B.Maple		
130153	LTP0430371	gap by tunneling	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1981																												Chevrel																		K																																																							4.8	1																																																				Tunneling spectroscopy on the superconducting Chevrel-phase compounds Cu1.8Mo6S8 and PbMo6S8				J.Low Temp.Phys., 43(1981)371	H.Wuhl,U.Poppe		
130154	SSC0330419	gap by NMR	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																			1980																												Chevrel																		K																																																							3.5	6																																																				NMR study of Chevrel phase superconductor				Solid State Commun., 33(1980)419	K.Asayama,N.Sano,T.Taniguchi		
130155	REV1976137		Pb0.92Mo6S7.5	Pb0.92Mo6S7.5	Pb	0.92	Mo	6	S	7.5																			1976																												Chevrel																		K		13.98					13.98			K/GPa	-1.6																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130156	REV1976137		PbMo5.1S4	Pb1Mo5.1S4	Pb	1	Mo	5.1	S	4																			1976																												Chevrel																		K		14.51					14.51			K/GPa	-1.05																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130157	REV1976137		Sn0.6Mo3S4	Sn0.6Mo3S4	Sn	0.6	Mo	3	S	4																			1976																												Chevrel																		K		14.45					14.45			K/GPa	-1.78																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130158	REV1976137		Sn0.6Mo3S4	Sn0.6Mo3S4	Sn	0.6	Mo	3	S	4																			1976																												Chevrel																		K		13.05					13.05			K/GPa	-1.382																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130159	REV1976137		CuMo3S4	Cu1Mo3S4	Cu	1	Mo	3	S	4																			1976																												Chevrel																		K		10.66					10.66			K/GPa	-1.072																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130160	REV1976137		AgMo4S5	Ag1Mo4S5	Ag	1	Mo	4	S	5																			1976																												Chevrel																		K		7.77					7.77			K/GPa	-0.6																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130161	REV1976137		Tl0.45Bi0.46Mo6S7.5	Tl0.45Bi0.46Mo6S7.5	Tl	0.45	Bi	0.46	Mo	6	S	7.5																	1976																												Chevrel																		K		6.41					6.41			K/GPa	-0.34																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130162	REV1976137	Tc(P) non-linear	ZnMo5S6	Zn1Mo5S6	Zn	1	Mo	5	S	6																			1976																												Chevrel																		K		3.12					3.12																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130163	REV1976137	Tc(P) non-linear	CdMo5S6	Cd1Mo5S6	Cd	1	Mo	5	S	6																			1976																												Chevrel																		K		2.67					2.67																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130164	REV1976137		ScMo6S7	Sc1Mo6S7	Sc	1	Mo	6	S	7																			1976																												Chevrel																		K		2.67					2.67			K/GPa	1.093																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130165	REV1976137		YMo6S7	Y1Mo6S7	Y	1	Mo	6	S	7																			1976																												Chevrel																		K		2.66					2.66			K/GPa	-0.581																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130166	REV1976137		MgMo6S7	Mg1Mo6S7	Mg	1	Mo	6	S	7																			1976																												Chevrel																		K		2.72					2.72			K/GPa	-0.25																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130167	REV1976137		Cu0.7Mo3Se4	Cu0.7Mo3Se4	Cu	0.7	Mo	3	Se	4																			1976																												Chevrel																		K		5.9					5.9			K/GPa	-1.12																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130168	REV1976137	Tc(P) non-linear	Ag0.7Mo3Se4	Ag0.7Mo3Se4	Ag	0.7	Mo	3	Se	4																			1976																												Chevrel																		K		5.96					5.96																																																																																																					"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130169	REV1976137		Sn0.7Mo3Se4	Sn0.7Mo3Se4	Sn	0.7	Mo	3	Se	4																			1976																												Chevrel																		K		4.85					4.85			K/GPa	-0.403																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130170	REV1976137		Pb1.2Mo6Se8	Pb1.2Mo6Se8	Pb	1.2	Mo	6	Se	8																			1976																												Chevrel																		K		4.32					4.32			K/GPa	-0.645																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130171	REV1976137		YMo6Se8	Y1Mo6Se8	Y	1	Mo	6	Se	8																			1976																												Chevrel																		K		6.38					6.38			K/GPa	-1.052																																																																																																	"The effect of high pressure on superconducting molybdenum chalcogenides in ""Superconductivity in d- and f- band metals"" eds. Douglous"				Plenum Press, 1976, p137-160	R.N.Shelton		
130172	PR0232219	Tc<1.2 for 0.22=<x=<0.30 from susceptibility measurements. thermopower also measured.	KxWO3	K0.18W1O3	K	0.18	W	1	O	3																		3	1981																												CaTiO3																	CaTiO3, perovskite	K		3.9					3.9	MTC30172																																																																																															single crystals by solid state reaction					Normal and superconducting properties of KxWO3				Phys.Rev.B, 23(1981)2219	L.H.Cadwell,R.C.Morris,W.G.Moulton		
130173	PR0203670	Hc2, thermopower also measured.	CsxWO3	Cs0.19W1O3	Cs	0.19	W	1	O	3																		3	1979																												CaTiO3																	CaTiO3, perovskite	K		6.7					6.7	MTC30173																																																																																															crystals by thermal vapor growth method					Normal and superconducting properties of CsxWO3				Phys.Rev.B, 20(1979)3670	M.R.Skokan,R.C.Morris,W.G.Moulton		
131000	HPLT1978-1		Ru0.46V0.54	Ru0.46V0.54	Ru	0.46	V	0.54																					1978																										AB																			B2	K		4.92					4.92			K/GPa	0.091																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131001	HPLT1978-1		ZrV2	V2Zr1	V	2	Zr	1																					1978																										AB2																			C15	K		7.9					7.9			K/GPa	0																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131002	HPLT1978-1		La3S4	La3S4	La	3	S	4																					1978																										A3B4																			D7<3>	K		8.1					8.1			K/GPa	1.1																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131003	HPLT1978-1		La3Se4	La3Se4	La	3	Se	4																					1978																										A3B4																			D7<3>	K		7.6					7.6			K/GPa	0.7																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131004	HPLT1978-1		CuMo3S4	Cu1Mo3S4	Cu	1	Mo	3	S	4																			1978																										AB3C4		Chevrel																		K		10.5					10.5			K/GPa	2																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131005	HPLT1978-1		2H-TaSe2	Se2Ta1	Se	2	Ta	1																					1978																										AB2		TX2																	2H-TaSe2	K		0.14					0.14			K/GPa	0.13																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131006	HPLT1978-1		2H-TaS2	S2Ta1	S	2	Ta	1																					1978																										AB2		TX2																	2H-TaS2	K		0.49					0.49			K/GPa	0.93																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131007	HPLT1978-1		4Hb-TaS2	S2Ta1	S	2	Ta	1																					1978																										AB2		TX2																	4Hb-TaS2	K		2.5					2.5			K/GPa	0.35																																																																																																	High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131008	HPLT1978-1		Nb3(Sn,Al)	Al0.05Nb3Sn0.95	Al	0.05	Nb	3	Sn	0.95																			1978																										AB3		Cr3Si(A15)																		K		18					18	MTC131008																																																																																																				High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131009	HPLT1978-1		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1978																										AB3		Cr3Si(A15)																		K		17.77					17.77	MTC131009																																																																																																				High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131010	HPLT1978-1	Tc(P) = 16.9, 16.9, 16.85 K for P = 0, 3.7, 10.5 kbar, respectively.	Nb3(Sn,Sb)	Nb3Sn0.05Sn0.95	Nb	3	Sn	0.05	Sn	0.95																			1978																										AB3		Cr3Si(A15)																		K		16.9					16.9																																																																																																					High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131011	HPLT1978-1	Tc(P) = 16.2, 16.17, 16.09 K for P = 0, 3.78, 10.5 kbar, respectively.	Nb3(Sn,Sb)	Nb3Sn0.1Sn0.9	Nb	3	Sn	0.1	Sn	0.9																			1978																										AB3		Cr3Si(A15)																		K		16.2					16.2																																																																																																					High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131012	HPLT1978-1	Tc(P) = 15.89 15.88 15.78 K for P = 0, 3.82 10.5 kbar, respectively.	Nb3(Sn,Sb)	Nb3Sn0.2Sn0.8	Nb	3	Sn	0.2	Sn	0.8																			1978																										AB3		Cr3Si(A15)																		K		15.89					15.89																																																																																																					High temperature superconductivity and instabilities: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	C.W.Chu		
131013	HPLT1978-2		LaAg	Ag1La1	Ag	1	La	1																					1978																										AB		CsCl																		K		1.06					1.06	MTC131013																																																																																																				LaAg under hydrostatic pressure, Superconductivity and phase transformation: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	J.S.Schilling,S.Methfessel,R.N.Shelton		
131014	HPLT1978-3		NdRh4B4	Nd1Rh4B4	Nd	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		5.31					5.31	MTC131014		K/GPa	-0.0565																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131015	HPLT1978-3		ThRh4B4	Th1Rh4B4	Th	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		4.41					4.41	MTC131014		K/GPa	-0.0654																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131016	HPLT1978-3		SmRh4B4	Sm1Rh4B4	Sm	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		2.66					2.66	MTC131014		K/GPa	-0.0506																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131017	HPLT1978-3		LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		11.249					11.249	MTC131017		K/GPa	0.0714																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131018	HPLT1978-3		YRh4B4	Y1Rh4B4	Y	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		10.591					10.591	MTC131017		K/GPa	0.056																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131019	HPLT1978-3		TmRh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		9.78					9.78	MTC131019		K/GPa	0.062																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131020	HPLT1978-3		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																		K		8.55					8.55	MTC131019		K/GPa	0.0495																																																																																																	Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131021	HPLT1978-3	not SC. magnetic ordering temperature Tm, (dTm/dP) =  0.118 K/GPa	GdRh4B4	Gd1Rh4B4	Gd	1	Rh	4	B	4																			1978								5.74																		AB4C4		RT4B4																		K					0																																																																																																							Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131022	HPLT1978-3	not SC. magnetic ordering temperature Tm, (dTm/dP) = 0.219  K/GPa	TbRh4B4	Tb1Rh4B4	Tb	1	Rh	4	B	4																			1978								7.17																		AB4C4		RT4B4																		K					0																																																																																																							Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131023	HPLT1978-3	not SC. magnetic ordering temperature Tm, (dTm/dP) =  0.152 K/GPa	DyRh4B4	Dy1Rh4B4	Dy	1	Rh	4	B	4																			1978								11.78																		AB4C4		RT4B4																		K					0																																																																																																							Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131024	HPLT1978-3	not SC. magnetic ordering temperature Tm, (dTm/dP) =  0.088 K/GPa	HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1978								6.75																		AB4C4		RT4B4																		K					0																																																																																																							Pressure dependences of the superconducting and magnetic critical temperatures of ternary rhodium borides: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.N.Shelton,D.C.Johnston		
131025	HPLT1978-4		AuGa2	Au1Ga2	Au	1	Ga	2																					1978																										AB2		CaF2																		K		1.14					1.14																																		MHC131025																																																																			The AuGa2 dilemma - superconducting version: High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	R.A.hein,J.E.Cox,R.W.McCallum		
131026	HPLT1978-5		(V,Cr)75Ga25	Cr4.84Ga25V70.16	Cr	4.84	Ga	25	V	70.16																			1978																										AB3		Cr3Si(A15)																		K		12.14					12.14	MTC131026																																																																																																				Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131027	HPLT1978-5		(V,Cr)75Ga25	Cr34.9Ga25V40.1	Cr	34.9	Ga	25	V	40.1																			1978																										AB3		Cr3Si(A15)																		K		5.48					5.48																																																																																																					Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131028	HPLT1978-5		(V,Mn)75Ga25	Ga25Mn4.92V70.08	Ga	25	Mn	4.92	V	70.08																			1978																										AB3		Cr3Si(A15)																		K		10.1					10.1	MTC131028																																																																																																				Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131029	HPLT1978-5		(V,Mn)75Ga25	Ga25Mn14V61	Ga	25	Mn	14	V	61																			1978																										AB3		Cr3Si(A15)																		K		4.22					4.22				0.0595																																																																																																	Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131030	HPLT1978-5		(V,Fe)75Ga25	Fe4.97Ga25V70.03	Fe	4.97	Ga	25	V	70.03																			1978																										AB3		Cr3Si(A15)																		K		8.59					8.59	MTC131030																																																																																																				Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131031	HPLT1978-5		(V,Fe)75Ga25	Fe9.92Ga25V65.08	Fe	9.92	Ga	25	V	65.08																			1978																										AB3		Cr3Si(A15)																		K		4.65					4.65																																																																																																					Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131032	HPLT1978-5		(V,Co)75Ga25	Co4.95Ga25V70.05	Co	4.95	Ga	25	V	70.05																			1978																										AB3		Cr3Si(A15)																		K		7.56					7.56	MTC131032			0.0839																																																																																																	Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131033	HPLT1978-5		(V,Co)75Ga25	Co7.32Ga25V67.68	Co	7.32	Ga	25	V	67.68																			1978																										AB3		Cr3Si(A15)																		K		5.03					5.03				0.0604																																																																																																	Pressure dependence of Tc in the superconducting A15 compounds V75-xTMxGa25 (TM = Cr, Mn, Fe, and Co):  High-pressure and low temperature physics, P-359, Plenum Press ed by C.W.Chu & J.A.Woollam				Plenum Press (1978)	D.U.Gubser,K.Girgis,H.R.Ott		
131034	PL-0230435	carrier n = 10.5E+20 /cc.  GL parameter = 2.57.	SnTe	Sn1Te1	Sn	1	Te	1																					1966																										AB																				K		0.06					0.06											Oe					0.46			0.012	Oe					5.2			0.012																																																																n/cm3	1050000000000000000000								Critical magnetic fields of superconducting SnTe			U.S.Naval Research Lab, Washington, D.C.	Phys.Lett., 23(1966)435	R.A.Hein		
131035	PL-0230435	carrier n = 12.5E+20 /cc	SnTe	Sn1Te1	Sn	1	Te	1																					1966																										AB																				K																																																																																																			n/cm3	1250000000000000000000								Critical magnetic fields of superconducting SnTe			U.S.Naval Research Lab, Washington, D.C.	Phys.Lett., 23(1966)435	R.A.Hein		
131036	PL-0230435	carrier n = 16.5E+20 /cc	SnTe	Sn1Te1	Sn	1	Te	1																					1966																										AB																				K																																																																																																			n/cm3	1650000000000000000000								Critical magnetic fields of superconducting SnTe			U.S.Naval Research Lab, Washington, D.C.	Phys.Lett., 23(1966)435	R.A.Hein		
131037	PL-0230435	carrier n = 20.0E+20 /cc	SnTe	Sn1Te1	Sn	1	Te	1																					1966																										AB																				K																																																																																																			n/cm3	2000000000000000000000								Critical magnetic fields of superconducting SnTe			U.S.Naval Research Lab, Washington, D.C.	Phys.Lett., 23(1966)435	R.A.Hein		
131038	PLA0290590	Nb-doped SrTiO3. carrier n = 5.0 E+19/cc. Tc defined by ac-SUS.	SrTiO3(Nb)	Sr1Ti1O3	Sr	1	Ti	1																	O	3			1969																										ABC3																				K		4					4																																																																																												n/cm3	50000000000000000000								Superconducting transition temperatures of Nb-doped SrTiO3				Phys.Lett.A, 29(1969)589	E.R.Pfeiffer,J.F.Schooley		
131039	PLA0290590	Nb-doped SrTiO3. carrier n = 2.5 E+19/cc. Tc defined by ac-SUS.	SrTiO3(Nb)	Sr1Ti1O3	Sr	1	Ti	1																	O	3			1969																										ABC3																				K		2.7					2.7																																																																																												n/cm3	25000000000000000000								Superconducting transition temperatures of Nb-doped SrTiO3				Phys.Lett.A, 29(1969)589	E.R.Pfeiffer,J.F.Schooley		
131040	PRL0120320	p-type semiconductor. carrier from Hall effect. Tc defined by SUS. cubic to rhonbohedral transition at 400C.	GeTe	Ge0.937Te1	Ge	0.937	Te	1																					1964																										AB																				K		0.311					0.311																																																																																												n/cm3	1520000000000000000000			press to pellet - SIN					Superconductivity in Germanium telluride				Phys.Rev.Lett., 12(1964)320	R.A.Hein,J.W.Gibson,R.Mazelsky,R.C.Miller,J.K.Hulm		
131041	PRL0120320	p-type semiconductor. carrier from Hall effect. Tc defined by SUS. cubic to rhonbohedral transition at 400C.	GeTe	Ge0.95Te1	Ge	0.95	Te	1																					1964																										AB																				K		0.246					0.246																																																																																												n/cm3	1170000000000000000000			press to pellet - SIN					Superconductivity in Germanium telluride				Phys.Rev.Lett., 12(1964)320	R.A.Hein,J.W.Gibson,R.Mazelsky,R.C.Miller,J.K.Hulm		
131042	PRL0120320	p-type semiconductor. carrier from Hall effect. Tc defined by SUS. cubic to rhonbohedral transition at 400C.	GeTe	Ge0.963Te1	Ge	0.963	Te	1																					1964																										AB																				K		0.171					0.171																																																																																												n/cm3	933000000000000000000			press to pellet - SIN					Superconductivity in Germanium telluride				Phys.Rev.Lett., 12(1964)320	R.A.Hein,J.W.Gibson,R.Mazelsky,R.C.Miller,J.K.Hulm		
131043	PRL0120320	p-type semiconductor. carrier from Hall effect. Tc defined by SUS. cubic to rhonbohedral transition at 400C.	GeTe	Ge0.976Te1	Ge	0.976	Te	1																					1964																										AB																				K		0.071					0.071																																																																																												n/cm3	861000000000000000000			press to pellet - SIN					Superconductivity in Germanium telluride				Phys.Rev.Lett., 12(1964)320	R.A.Hein,J.W.Gibson,R.Mazelsky,R.C.Miller,J.K.Hulm		
131044	PRL0190784	uniaxial and hydrostatic pressure effect of Tc (see FIG)	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3			1967																										ABC3																				K				0.27			0.27	MTC131044																																																																																											n/cm3	63000000000000000000								Effect of stress on the superconductive transition temperature of strontium titanate				Phys.Rev.Lett., 19(1967)783	E.R.Pfeiffer,J.F.Schooley		
131045	PRL0240053	rhombohedral distortion (RT)	TlBiTe2	Tl1Bi1Te2	Tl	1	Bi	1	Te	2																			1970																										ABC		NaCl																		K				0.141			0.141																				Oe	extrapolation	10												MHC131045																																					uOhm.cm	7.8																				n/cm3	620000000000000000000								Superconductivity in TlBiTe2: A low carrier density (III-V)VI2 compound				Phys.Rev.Lett., 24(1970)53	R.A.Hein,E.M.Swiggard		
131046	PRL0130233	SP-heat measured for T <0.9 K.	GeTe	Ge0.95Te1	Ge	0.95	Te	1																					1964																										AB																				K		0.246					0.246																																																					MSP131046			mJ/mol.K2	1.32	SP-heat	166	SP-heat																																				ANN(485C10d)					Germanium telluride: Specific heat and superconductivity				Phys.Rev.Lett., 13(1964)233	Leonard Finegold		
131047	PRL0240053		GeTe	Ge1Te1	Ge	1	Te	1																					1970																										AB																				K		0.08					0.08																				Oe		20																																																																						n/cm3	860000000000000000000			ANN(485C10d)					Superconductivity in TlBiTe2: A low carrier density (III-V)VI2 compound				Phys.Rev.Lett., 24(1970)53	R.A.Hein,E.M.Swiggard		
131048	PRL0240053	GL parameter = 6.1	GeTe	Ge1Te1	Ge	1	Te	1																					1970																										AB																				K		0.172					0.172																				Oe		130																																																																						n/cm3	930000000000000000000			ANN(485C10d)					Superconductivity in TlBiTe2: A low carrier density (III-V)VI2 compound				Phys.Rev.Lett., 24(1970)53	R.A.Hein,E.M.Swiggard		
131049	PRL0240053	GL parameter = 9.3	GeTe	Ge1Te1	Ge	1	Te	1																					1970																										AB																				K		0.25					0.25																				Oe		270																																																																						n/cm3	1180000000000000000000			ANN(485C10d)					Superconductivity in TlBiTe2: A low carrier density (III-V)VI2 compound				Phys.Rev.Lett., 24(1970)53	R.A.Hein,E.M.Swiggard		
131050	PCS0340183	Mn-doped Sn0.87Ag0.10Te. Mn-concentration in ppm	(Sn,Ag,Mn)Te	Sn0.87Ag0.1Te1	Sn	0.87	Ag	0.1	Te	1																			1973																																														K		1.78					1.78	MTC131050																																																																																																				SUPERCONDUCTIVITY AS A FUNCTION OF CARRIER DENSITY AND MAGNETIC SPIN CONCENTRATION IN THE SnTe-MnTe SYSTEM				J.Phys.Chem.Solids, 34(1973)183	M. P. MATHUR,D. W. DEIS,C. K. JONES,W. J. CARR Jr		
131051	PCS0340183	Mn-doped Sn0.90Ag0.07Te. Mn-concentration in ppm	(Sn,Ag,Mn)Te	Sn0.9Ag0.07Te1	Sn	0.9	Ag	0.07	Te	1																			1973																																														K		1.73					1.73	MTC131051																																																																																																				SUPERCONDUCTIVITY AS A FUNCTION OF CARRIER DENSITY AND MAGNETIC SPIN CONCENTRATION IN THE SnTe-MnTe SYSTEM				J.Phys.Chem.Solids, 34(1973)183	M. P. MATHUR,D. W. DEIS,C. K. JONES,W. J. CARR Jr		
131052	PCS0340183	Mn-doped Sn0.92Ag0.05Te. Mn-concentration in ppm	(Sn,Ag,Mn)Te	Sn0.92Ag0.05Te1	Sn	0.92	Ag	0.05	Te	1																			1973																																														K		1.66					1.66	MTC131052																																																																																																				SUPERCONDUCTIVITY AS A FUNCTION OF CARRIER DENSITY AND MAGNETIC SPIN CONCENTRATION IN THE SnTe-MnTe SYSTEM				J.Phys.Chem.Solids, 34(1973)183	M. P. MATHUR,D. W. DEIS,C. K. JONES,W. J. CARR Jr		
131053	LES0620197	Tc from ac-SUS. single phase	AuGa	Au0.499Ga0.501	Au	0.499	Ga	0.501																					1978																																														K				1.17			1.17																													Oe/K		106			MHC131053																																																														melt in evacuated quartz tube - ANN(400C,1w)					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131054	LES0620197	Tc from ac-SUS. two phases(AuGa+AuGa2)	AuGa	Au0.427Ga0.573	Au	0.427	Ga	0.573																					1978																																														K				1.378			1.378																													Oe/K		123			MHC131054																																																														melt in evacuated quartz tube - ANN(400C,1w)					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131055	LES0620197	Tc from ac-SUS. two phases(AuGa+AuGa2)	AuGa2	Au0.388Ga0.612	Au	0.388	Ga	0.612																					1978																																														K				1.355			1.355																													Oe/K		112																																																																	melt in evacuated quartz tube - ANN(400C,1w)					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131056	LES0620197	Tc from ac-SUS. single phase (AuGa2)	AuGa2	Au0.293Ga0.707	Au	0.293	Ga	0.707																					1978																																														K				1.63			1.63																													Oe/K		253			MHC131056																																																														melt in evacuated quartz tube - ANN(400C,1w)					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131057	LES0620197		(Au,Pd)Ga2	Au0.98Pd0.02Ga2	Au	0.98	Pd	0.02	Ga	2																		1	1978																										AB2		CaF2																		K				1.51			1.51																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131058	LES0620197		(Au,Pd)Ga2	Au0.93Pd0.07Ga2	Au	0.93	Pd	0.07	Ga	2																		1	1978																										AB2		CaF2																		K				1.773			1.773																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131059	LES0620197	two phase	(Au,Pd)Ga2	Au0.85Pd0.15Ga2	Au	0.85	Pd	0.15	Ga	2																		2	1978																										AB2		CaF2																		K				1.79			1.79																																																																																																					Superconducting properties of AuGa and AuGa2 compounds			Naval Research Lab, Washington, D.C. USA	J.Less-Common Metals, 62(1978)197	Ch.J.Raub,H.R.Khan,J.E.Cox,J.Willis,R.A.Hein		
131060	SSC0190265	quenched from 1250 C. Tc(SP) = 13.5 K	V3Ga	Ga1V3	Ga	1	V	3																					1976																										AB3		Cr3Si(A15)																		K				13.8			13.8																																																								mJ/gat.K2	19.9	SP-heat	310	SP-heat																																									SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY VS LONG RANGE ORDER IN V3Ga				Solid State Commun., 19(1976)265	A. Junod,R. Flukiger,A. Treyvaud,J. Muller		
131061	SSC0190265	slow cooled from 610 C. Tc(SP) = 15.1 K	V3Ga	Ga1V3	Ga	1	V	3																					1976																										AB3		Cr3Si(A15)																		K				15.3			15.3																																																								mJ/gat.K2	24	SP-heat	297	SP-heat																																									SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY VS LONG RANGE ORDER IN V3Ga				Solid State Commun., 19(1976)265	A. Junod,R. Flukiger,A. Treyvaud,J. Muller		
131062	SSC0190265	annealed at 560 C. Tc(SP) = 2.87 K	V3Au	Au1V3	Au	1	V	3																					1976																										AB3		Cr3Si(A15)																		K				2.9			2.9																																																								mJ/gat.K2	13.1	SP-heat	329	SP-heat																																									SPECIFIC HEAT AND MAGNETIC SUSCEPTIBILITY VS LONG RANGE ORDER IN V3Ga				Solid State Commun., 19(1976)265	A. Junod,R. Flukiger,A. Treyvaud,J. Muller		
131063	SSC0210239	ANN(1750C,24h)	Nb3Os	Nb3Os1	Nb	3	Os	1																					1977																										AB3		Cr3Si(A15)																		K		0.94					0.94																																																								mJ/gat.K2	2.34	SP-heat	373	SP-heat																																									X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
131064	SSC0210239	ANN(1650C,16h)	Nb3Ir3	Ir1Nb3	Ir	1	Nb	3																					1977																										AB3		Cr3Si(A15)																		K		1.66					1.66																																																								mJ/gat.K2	2.05	SP-heat	378	SP-heat																																									X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
131065	SSC0210239	ANN(1750C,24h)	Nb3Pt	Nb3Pt1	Nb	3	Pt	1																					1977																										AB3		Cr3Si(A15)																		K		9.2					9.2																																																								mJ/gat.K2	5.55	SP-heat	340	SP-heat																																									X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
131066	SSC0210239	ANN(1500C,48h + 1200C,48h). Nb0.76Au0.24	Nb3Au	Au1Nb3	Au	1	Nb	3																					1977																										AB3		Cr3Si(A15)																		K		10.56					10.56																																																								mJ/gat.K2	9	SP-heat	251	SP-heat																																									X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
131067	SSC0210239	stage annealing between 1100 C and 500C). V0.76Au0.24	V3Au	Au1V3	Au	1	V	3																					1977																										AB3		Cr3Si(A15)																		K		2.97					2.97																																																								mJ/gat.K2	13.08	SP-heat	329	SP-heat																																									X-Rey Photoemission spectra of valence electrons in V3x and Nb3x Compounds			Institute of Metal Physics, Ural Scientific Centre, Academy of Sciences of the USSR, Sverdlovsk, USSR	Solid State Commun., 21(1977)239	E.Z.Kurmaev,F.Werfel,O.Brummer,R.Flukiger		
131068	SSC0110061	single phase.  ANN(1600C,70h)	(Mo,Pt)	Mo0.81Pt0.19	Mo	0.81	Pt	0.19																					1972																															A	4.989													A15 phase	K		4.53					4.53																																																								mJ/gat.K2	3.86	SP-heat	390	SP-heat																																									IDENTIFICATION OF THE SUPERCONDUCTING PHASES IN THE MOLYBDENUM-PLATINUM SYSTEM				Solid State Commun., 11(1972)61	R. Flukiger,A. Paoli,R. Roggen,K. Yvon,J. Muller		
131069	SSC0030097	Tc by self-induction method	ZrMo2	Mo2Zr1	Mo	2	Zr	1																					1965																										AB2		MgCu2(Laves)																	MgCu2, C15	K	4.27	4.57	4.75				4.57																																																																																																arc-melting					SUPERCONDUCTING TRANSITION TEMPERATURES OF ZrMo2, HfV2 AND PbAu2				Solid State Commun., 3(1965)97	V. Sadagopan,E. Pollard,H. C. Gatos		
131070	SSC0030097	Tc by self-induction method	HfV2	Hf1V2	Hf	1	V	2																					1965																										AB2		MgCu2(Laves)																	MgCu2, C15	K	8.9	9.15	9.57				9.15																																																																																																arc-melting					SUPERCONDUCTING TRANSITION TEMPERATURES OF ZrMo2, HfV2 AND PbAu2				Solid State Commun., 3(1965)97	V. Sadagopan,E. Pollard,H. C. Gatos		
131071	SSC0030097	Tc by self-induction method	PbAu2	Au2Pb1	Au	2	Pb	1																					1965																										AB2		MgCu2(Laves)																	MgCu2, C15	K	5.98	6.95	7.12				6.95																																																																																																arc-melting					SUPERCONDUCTING TRANSITION TEMPERATURES OF ZrMo2, HfV2 AND PbAu2				Solid State Commun., 3(1965)97	V. Sadagopan,E. Pollard,H. C. Gatos		
131072	SSC0180139		(Au,Ga)	Au0.9Ga0.1	Au	0.9	Ga	0.1																					1976																																													fcc	K		0.264					0.264	MTC131072																																																																																																				Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131073	SSC0180139		(Au,Ga)	Au0.95Ga0.05	Au	0.95	Ga	0.05																					1976																																													fcc	K		0.032					0.032																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131074	SSC0180139		(Au,Al)	Al0.14Au0.86	Al	0.14	Au	0.86																					1976																																													fcc	K		0.385					0.385	MTC131074																																																																																																				Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131075	SSC0180139		(Au,Al)	Al0.05Au0.95	Al	0.05	Au	0.95																					1976																																													fcc	K		0.0138					0.0138																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131076	SSC0180139		(Au,Sn)	Au0.95Sn0.05	Au	0.95	Sn	0.05																					1976																																													fcc	K		0.047					0.047																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131077	SSC0180139		(Ag,Ga)	Ag0.828Ga0.172	Ag	0.828	Ga	0.172																					1976																																													fcc	K		0.116					0.116	MTC131077																																																																																																				Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131078	SSC0180139		(Ag,Ga)	Ag0.875Ga0.125	Ag	0.875	Ga	0.125																					1976																																													fcc	K		0.019					0.019																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131079	SSC0180139		(Ag,In)	Ag0.81In0.19	Ag	0.81	In	0.19																					1976																																													fcc	K		0.0074					0.0074																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131080	SSC0180139		(Ag,Zn)	Ag0.7Zn0.3	Ag	0.7	Zn	0.3																					1976																																													fcc	K		0.0125					0.0125																																																																																																					Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131081	SSC0180139		(Cu,Ga)	Cu0.81Ga0.19	Cu	0.81	Ga	0.19																					1976																																													fcc	K		0.048					0.048	MTC131081																																																																																																				Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131082	SSC0180139		(Au,In)	Au0.9In0.1	Au	0.9	In	0.1																					1976																																													fcc	K		0.0625					0.0625	MTC131082																																																																																																				Superconductivity in alpha-phase alloys of Cu, Ag and Au				Solid State Commun., 18(1976)139	A.C.Mota,R.F.Hoyt		
131083	PRL0281127	Tc defined as midpoint of inductance change. Tc measured upto 8 kbar	AuGa2	Au1Ga2	Au	1	Ga	2																					1972																										AB2		CaF2																		K		1.15					1.15			K/GPa	0.3																																																																																																	Pressure-induced electron transition in AuGa2				Phys.Rev.Lett., 28(1972)1127	J.E.Schirber		
131084	LES0460339		CuY	Cu1Y1	Cu	1	Y	1																					1976																												CsCl																		K		0.47					0.47																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131085	LES0460339		AuSc	Au1Sc1	Au	1	Sc	1																					1976																												CsCl																		K		2					2																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131086	LES0460339		AuLu	Au1Lu1	Au	1	Lu	1																					1976																												CsCl																		K		0.37					0.37																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131087	LES0460339		ScAlAu2	Al1Sc1Au2	Al	1	Sc	1	Au	2																			1976																												CsCl																		K		4.4					4.4																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131088	LES0460339		ScInAu2	In1Sc1Au2	In	1	Sc	1	Au	2																			1976																												CsCl																		K		3.02					3.02																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131089	LES0460339		YInAu2	In1Y1Au2	In	1	Y	1	Au	2																			1976																												CsCl																		K		1.9					1.9																																																																																																					Obstacles to superconductivity in CsCl phases				J.Less-Common Met., 46(1976)339	B. T. MATTHIAS,E. CORENZWIT,J. M. VANDENBERG,H. BARZ,M. B. MAPLE,R. N. SHELTON		
131090	LES0620183		(Au,Al)	Al0.08Au0.92	Al	0.08	Au	0.92																					1978																																														K	0.0751	0.088	0.0934				0.088																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131091	LES0620183		(Au,Al,In)	Al0.07Au0.92In0.01	Al	0.07	Au	0.92	In	0.01																			1978																																														K	0.0653	0.0763	0.0833				0.0763																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131092	LES0620183		(Au,Al,In)	Al0.06Au0.92In0.02	Al	0.06	Au	0.92	In	0.02																			1978																																														K	0.0526	0.0619	0.0676				0.0619																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131093	LES0620183		(Au,Al,In)	Al0.0563Au0.92In0.0237	Al	0.0563	Au	0.92	In	0.0237																			1978																																														K	0.051	0.0609	0.0655				0.0609																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131094	LES0620183		(Au,Al,In)	Al0.05Au0.92In0.03	Al	0.05	Au	0.92	In	0.03																			1978																																														K	0.0552	0.0672	0.0741				0.0672																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131095	LES0620183		(Au,Al,In)	Al0.04Au0.92In0.04	Al	0.04	Au	0.92	In	0.04																			1978																																														K	0.0321	0.0555	0.0615				0.0555																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131096	LES0620183		(Au,Al,In)	Al0.03Au0.92In0.05	Al	0.03	Au	0.92	In	0.05																			1978																																														K	0.034	0.045	0.05				0.045																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131097	LES0620183		(Au,Al,In)	Al0.02Au0.92In0.06	Al	0.02	Au	0.92	In	0.06																			1978																																														K	0.0289	0.034	0.038				0.034																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131098	LES0620183		(Au,Al,In)	Al0.01Au0.92In0.07	Al	0.01	Au	0.92	In	0.07																			1978																																														K	0.0215	0.0278	0.03				0.0278																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131099	LES0620183		(Au,In)	Au0.92In0.08	Au	0.92	In	0.08																					1978																																														K	0.0151	0.022	0.025				0.022																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131100	LES0620183		(Au,Ga)	Au0.92Ga0.08	Au	0.92	Ga	0.08																					1978																																														K	0.144	0.168	0.172				0.168																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131101	LES0620183		(Au,Ga,In)	Au0.92Ga0.068In0.012	Au	0.92	Ga	0.068	In	0.012																			1978																																														K	0.129	0.137	0.139				0.137																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131102	LES0620183		(Au,Ga,In)	Au0.92Ga0.06In0.02	Au	0.92	Ga	0.06	In	0.02																			1978																																														K	0.11	0.13	0.136				0.13																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131103	LES0620183		(Au,Ga,In)	Au0.92Ga0.04In0.04	Au	0.92	Ga	0.04	In	0.04																			1978																																														K	0.0613	0.0682	0.0782				0.0682																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131104	LES0620183		(Au,Ga,In)	Au0.92Ga0.02In0.06	Au	0.92	Ga	0.02	In	0.06																			1978																																														K	0.034	0.0425	0.05				0.0425																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131105	LES0620183		(Au,Ga,Al)	Al0.02Au0.92Ga0.06	Al	0.02	Au	0.92	Ga	0.06																			1978																																														K	0.15	0.158	0.163				0.158																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131106	LES0620183		(Au,Ga,Al)	Al0.04Au0.92Ga0.04	Al	0.04	Au	0.92	Ga	0.04																			1978																																														K	0.0901	0.101	0.108				0.101																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131107	LES0620183		(Au,Ga,Al)	Al0.06Au0.92Ga0.02	Al	0.06	Au	0.92	Ga	0.02																			1978																																														K	0.0846	0.09	0.0972				0.09																																																																																																					ELASTIC STRAIN ENERGY DEPENDENCE OF Tc, IN TERNARY GOLDBASED SOLID SOLUTIONS				J.Less-Common Met., 62(1978)183	R. F. HOYT,A. C. MOTA		
131108	SSC0710369	P-induced SC. small chips cut from GaAs-wafer. P=20 GPa (GaAs-II)	GaAs	As1Ga1	As	1	Ga	1																					1989																										AB																				K		4.5			0		4.5																																																																																																					Metallic properties of orthorhombic high pressure phase of GaAs: Theory and Experiment				Solid State Commun., 71(1989)369	S.B. Zhang,David Erskine,Marvin L. Cohen,Peter Y. Yu		
131109	JPS0613845		ErPb2	Er1Pb2	Er	1	Pb	2																					1992					myu-B/Er	9.5	-7.7	3.5																		AB2																				K				7.4			7.4										25																																																																																						arc-melting					Coexistence of superconductivity and antiferromagnetic ordering in ErPb2				J.Phys.Soc.Jpn, 61(1992)3845	Y.Hattori,K.Fukamichi,T.Goto,K.Suzuki		
131110	JPS0351257	purity: 5N. Debye-T = 271 K at 4 K.. (Ces/[gamma]*Tc) = 2.0	CuS	Cu1S1	Cu	1	S	1																					1973																										AB																				K		1.65					1.65																													Oe/K		130																									mJ/mol.K2	2.5		285																																										Specific heats of superconductive copper sulfide CuS				J.Phys.Soc.Jpn, 35(1973)1257	M.Isino,E.Kanda		
131111	JPS0351257	impurity: 0.085 at% Ag.  (Ces/[gamma]*Tc) = 2.0	CuS	Cu1S1	Cu	1	S	1																					1973																										AB																				K		1.52					1.52																																																								mJ/mol.K2	2.5																																												Specific heats of superconductive copper sulfide CuS				J.Phys.Soc.Jpn, 35(1973)1257	M.Isino,E.Kanda		
131112	JPS0540877		LaCu6	Cu6La1	Cu	6	La	1																				3	1985																										AB6																				K		0.042					0.042																																																								mJ/mol.K2	8		230																																					Czochralski method					Low twmperature magnetic resistivity in a dense Kondo substance: CexLa1-xCu6				J.Phys.Soc.Jpn, 54(1985)877	A.Sumiyama,Y.Oda,H.Nagano,Y.Onuki,T.Komatsubara		
131113	SSC0720279	RRR = 19	ThCu6	Cu6Th1	Cu	6	Th	1																					1989																										AB6					A	8.107	5.078	10.104												K				0.2			0.2										80																																																													uOhm.cm											139														arc-melting - ANN(750C,4d, in vac)					Low temperature electrical and magnetic properties of RCu6(R = La,Ce,Pr,Nd,Sm,Gd, and Th) compounds				Solid State Commun., 72(1989)279	H.D. YANG,P. KLAVINS,R.N. SHELTON		
131114	SSC0720279	RRR = 31. ortho-to-monoclinic transformation at 500K.	LaCu6	Cu6La1	Cu	6	La	1																					1989																										AB6					A	8.117	5.113	10.194												K					0.06																																																																									uOhm.cm											30														arc-melting - ANN(750C,4d, in vac)					Low temperature electrical and magnetic properties of RCu6(R = La,Ce,Pr,Nd,Sm,Gd, and Th) compounds				Solid State Commun., 72(1989)279	H.D. YANG,P. KLAVINS,R.N. SHELTON		
131115	SSC0720279	RRR = 80. ortho-to-monoclinic transformation at 200K.	CeCu6	Ce1Cu6	Ce	1	Cu	6																					1989					myu-B/Ce	2.67	-47.2																			AB6					A	8.101	5.097	10.171												K					0.06																																																																									uOhm.cm											80														arc-melting - ANN(750C,4d, in vac)					Low temperature electrical and magnetic properties of RCu6(R = La,Ce,Pr,Nd,Sm,Gd, and Th) compounds				Solid State Commun., 72(1989)279	H.D. YANG,P. KLAVINS,R.N. SHELTON		
131116	SSC0200233	Tc by mutual inductance. (dTc/dx) = -200 K/at%-Mn.	(Cd,Mn)	Cd99.995Mn0.005	Cd	99.995	Mn	0.005																					1976																																														K		0.39					0.39																																																																																																Cd(6N) used					Superconductivity and magnetism in dilute CdMn alloys. Strong depression in Tc				Solid State Commun., 20(1976)233	T. Claeson,M. Hanson,J. Ivarsson		
131117	NAT3550529	ANN(600C,15h). Tc by dc-magnetization	Ca5C60	C60Ca5	C	60	Ca	5																					1992																																													simple cubic	K				8.4			8.4																																																																																																					Superconductivity at 8.4K in calcium-doped C60			AT&T Bell Lab, New Jersey,USA	Nature, 355(1992)529	A.R.Kortan,N.Kopylov,S.Glarum,E.M.Gyorgy,A.P.Ramirez,R.M.Fleming,F.A.Thiel,R.C.Haddon		
131118	SSC0910345	0.20 mm-dia-wire. Tc by resistivity. RRR = 4.37.	(Cu,Nb)	Cu0.7Nb0.3	Cu	0.7	Nb	0.3																					1994																																														K		9.39				0.34	9.39																																																																							uOhm.cm											1.66														arc-melting					Influence of Indium and Tantalum as an impurity on the normal and superconducting state properties of in situ prepared Cu-Nb composite wires				Solid State Commun., 91(1994)345	S.S. Dubey,P.N. Dheer,R.G. Sharma,M.M. Krishna,Y.S. Reddy		
131119	SSC0910345	0.20 mm-dia-wire. Tc by resistivity. RRR = 2.23.	(Cu,Nb,In)	Cu0.7In0.01Nb0.29	Cu	0.7	In	0.01	Nb	0.29																			1994																																														K		9.04				0.24	9.04																																																																							uOhm.cm											3.4														arc-melting					Influence of Indium and Tantalum as an impurity on the normal and superconducting state properties of in situ prepared Cu-Nb composite wires				Solid State Commun., 91(1994)345	S.S. Dubey,P.N. Dheer,R.G. Sharma,M.M. Krishna,Y.S. Reddy		
131120	SSC0910345	0.20 mm-dia-wire. Tc by resistivity. RRR = 2.51.	(Cu,Nb,Ta)	Cu0.7Nb0.29Ta0.01	Cu	0.7	Nb	0.29	Ta	0.01																			1994																																														K		9.25				0.12	9.25																																																																							uOhm.cm											1.79														arc-melting					Influence of Indium and Tantalum as an impurity on the normal and superconducting state properties of in situ prepared Cu-Nb composite wires				Solid State Commun., 91(1994)345	S.S. Dubey,P.N. Dheer,R.G. Sharma,M.M. Krishna,Y.S. Reddy		
131121	SSC0710369	P-induced SC. small chips cut from GaAs-wafer. P=40.8 GPa (GaAs-III)	GaAs	As1Ga1	As	1	Ga	1																					1989																										AB																				K		3			0		3																																																																																																					Metallic properties of orthorhombic high pressure phase of GaAs: Theory and Experiment				Solid State Commun., 71(1989)369	S.B. Zhang,David Erskine,Marvin L. Cohen,Peter Y. Yu		
131122	PHB1941727	break junction of Zn and UBe13.	UBe13	Be13U1	Be	13	U	1																					1994																										AB13		NaZn13																		K		0.88					0.88																																														meV	0.145	4.21	1																																															arc-melting - ANN(1000C,2w,in inert gas)					The superconducting energy gap of bulk UBe13				Physica B, 194-196(1994)1727	John Moreland,Alan F. Clark,Robert J. Soulen, Jr,J. L. Smith		
131123	PRL0501595		UBe13	Be13U1	Be	13	U	1																				3	1988					myu-B/U	2.6	-53																			AB13		NaZn13			A	10.2607														K			0.86	0.85			0.85																													T/K		25.7																									mJ/mol.K2	1100	SP-heat																																						arc-melting - heat(1400C,in Al-flux) - slow cool					UBe13: An unconventional actinide superconductor				Phys. Rev.Lett., 50(1983)1595	H.R.Ott,H.Rudigier,Z.Fisk,J.L.Smith		
131124	SSC0480005	0 < Tc < 2.8 K: depends on preparation procedure. [ Curie-T] shows ferromagnetic one.	Y4Co3	Co3Y4	Co	3	Y	4																				1	1983							7																			A3B4		Ho4Co3																		K				2.5			2.5																																																																																																arc-melting - ANN(450-550 C,200h)					NMR study of Y4Co3 compound				Solid State Commun., 48(1983)5	S. Wada,T.Kohara,K. Asayama,Y. Kitaoka,Y. Kohori,N. Ishikawa		
131125	SSC0550193	muon-SR measurements.	Y9Co7	Co7Y9	Co	7	Y	9																					1985							6																			A7B9																				K		2.7					2.7																																																																																																					Study of the hybrid state of Y9Co7(2.0 =<T=<6 K) by means of zero field muon spin relaxation				Solid State Commun., 55(1985)193	E.J. Ansaldo,D.R. Noakes,J.H. Brewer,R. Keitel,D.R. Harshman,M. Senba,C.Y. Huang,B.V.B. Sarkissian		
131126	SSC0091611	P-induced SC. Tc = 1.6 , 0.9, 0.36 K at 14 , 12, 10.5 GPa, respectively. P<cr> = 0.9 GPa.  Kondo-T = 18 K(P=0).	(Y,Ce)	Ce0.01Y0.99	Ce	0.01	Y	0.99																					1971																																														K		1.6			0		1.6																																																																																																					Low temperature electrical resistiity of YCe under pressure				Solid State Commun., 9(1971)1611	MB. Maple,J. Wittig		
131127	PRL0652816	Hc1(0) extrapolated using T^2 approx.	UBe13	Be13U1	Be	13	U	1																					1990																										AB13		NaZn13																		K		0.86					0.86											Oe	M-H curve	43.2																					MHC131127																																																																			New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131128	PRL0652816	Hc1(0) extrapolated using T^2 approx.	(U,Th)Be13	Be13U0.9934Th0.0066	Be	13	U	0.9934	Th	0.0066																			1990																										AB13		NaZn13																		K		0.67					0.67											Oe	M-H curve	32.7																																																																																								New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131129	PRL0652816	Hc1(0) extrapolated using T^2 approx.	(U,Th)Be13	Be13U0.9899Th0.0101	Be	13	U	0.9899	Th	0.0101																			1990																										AB13		NaZn13																		K		0.65					0.65											Oe	M-H curve	26.4																																																																																								New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131130	PRL0652816	Hc1(0) extrapolated using T^2 approx. 2nd (lower Tc = 0.44 K) appears. Hc1(0) = 37.9 Oe.	(U,Th)Be13	Be13U0.9807Th0.0193	Be	13	U	0.9807	Th	0.0193																			1990																										AB13		NaZn13																		K		0.48					0.48											Oe	M-H curve	22.8																																																																																								New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131131	PRL0652816	Hc1(0) extrapolated using T^2 approx. 2nd (lower Tc = 0.41 K) appears. Hc1(0) = 49.1 Oe.	(U,Th)Be13	Be13U0.9755Th0.0245	Be	13	U	0.9755	Th	0.0245																			1990																										AB13		NaZn13																		K		0.59					0.59	MTC131131										Oe	M-H curve	28.9																																																																																								New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131132	PRL0652816	Hc1(0) extrapolated using T^2 approx. 2nd (lower Tc = 0.39 K) appears. Hc1(0) = 55.9 Oe.	(U,Th)Be13	Be13U0.9645Th0.0355	Be	13	U	0.9645	Th	0.0355																			1990																										AB13		NaZn13																		K		0.55					0.55											Oe	M-H curve	35.3																					MHC131132																																																																			New phase diagram for (U,Th)Be13: A muon-spin-resonance and Hc1 study			Los Alamos National Lab	Phys.Rev.Lett., 65(1990)2816	R.H.Heffner,J.L.Smith,J.O.Willis,P.Birrer,C.Baines,F.N.gygax,B.Hitti,E.Lippelt,H.R.Ott,A.Schenck,E.A.Knetsch,J.A.Mydosh,D.E.MacLaughlin		
131133	SSC0280153	33.3at%Bi-In. decompose (In5Bi3 + In-rich phase) for P>20 kbar.	In2Bi	Bi1In2	Bi	1	In	2																					1978																										AB2																				K		5.766					5.766	MTC131133																																																																																													In(5N),Bi(5N)		melt in Pyrex tube (vac)					PRESSURE-INDUCED PHASE TRANSFORMATION IN In2Bi			Department of Physics, Monash University, Clayton, Victoria 3168, Australia	Solid State Commun., 28(1978)153	M.J. Clark,M. Simpson		
131134	SSC0280153		In5Bi3	Bi3In5	Bi	3	In	5																					1978																										A3B5																				K		4.227					4.227	MTC131134		K/GPa	-0.49																																																																																										In(5N),Bi(5N)		melt in Pyrex tube (vac)					PRESSURE-INDUCED PHASE TRANSFORMATION IN In2Bi			Department of Physics, Monash University, Clayton, Victoria 3168, Australia	Solid State Commun., 28(1978)153	M.J. Clark,M. Simpson		
131135	SSC0520659		YB6	B6Y6	B	6	Y	6																				3	1984																										AB6		CaB6																		K		7.5					7.5																																														meV	1.22	3.8																																																					Electron tunneling into superconducting YB6			Tohoku University, Sendai	Solid State Commun., 52(1984)659	S.Kunii,T.Kasuya,K.Kadowaki,M.Date,S.B.Woods		
131136	SSC0070381		Cr3Ir	Cr3Ir1	Cr	3	Ir	1																					1969																										AB3		Cr3Si(A15)																		K		0.15					0.15																													T/K		1.053																																																																						Superconducting behavior of A15 compounds			Naval Research Laboratory, Washington, D.C.	Solid State Commun., 7(1969)381	Robert A.Hein,J.E.Cox,R.D.Blaugher,R.M.Waterstrat		
131137	SSC0070381		Cr3Rh	Cr3Rh1	Cr	3	Rh	1																					1969																										AB3		Cr3Si(A15)																		K		0.07					0.07																													T/K		0.909																																																																						Superconducting behavior of A15 compounds			Naval Research Laboratory, Washington, D.C.	Solid State Commun., 7(1969)381	Robert A.Hein,J.E.Cox,R.D.Blaugher,R.M.Waterstrat		
131138	SSC0070381		Nb3Os	Nb3Os1	Nb	3	Os	1																					1969																										AB3		Cr3Si(A15)																		K		0.94					0.94																													T/K		0.126																																																																						Superconducting behavior of A15 compounds			Naval Research Laboratory, Washington, D.C.	Solid State Commun., 7(1969)381	Robert A.Hein,J.E.Cox,R.D.Blaugher,R.M.Waterstrat		
131139	SSC0070381		V3Pd	Pd1V3	Pd	1	V	3																					1969																										AB3		Cr3Si(A15)																		K		0.08					0.08																																																																																																					Superconducting behavior of A15 compounds			Naval Research Laboratory, Washington, D.C.	Solid State Commun., 7(1969)381	Robert A.Hein,J.E.Cox,R.D.Blaugher,R.M.Waterstrat		
131140	SSC0500189	liquid quenching onsubstrates (Ts=RT)	alpha-Zr	Zr1	Zr	1																							1984																																													alpha-phase	K		0.52					0.52																																																																																																melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131141	SSC0500189	liquid quenching onsubstrates (Ts=RT)	omega-Zr	Zr1	Zr	1																							1984																																													omega-phase	K		0.92					0.92																																																																																																melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131142	SSC0500189	liquid quenching onsubstrates (Ts=RT)	Zr1-xMox	Zr0.8Mo0.2	Zr	0.8	Mo	0.2																					1984																																													beta-phase	K		5.18					5.18	MTC131142																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131143	SSC0500189	liquid quenching onsubstrates (Ts=RT)	Zr1-xAlx	Zr0.8Mo0.2	Zr	0.8	Mo	0.2																					1984																																													beta-phase	K		4.1					4.1	MTC131142																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131144	SSC0500189	liquid quenching onsubstrates (Ts=RT)	Zr1-xPdx	Zr0.9Mo0.1	Zr	0.9	Mo	0.1																					1984																																													beta-phase	K		4.92					4.92	MTC131144																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131145	SSC0500189	liquid quenching onsubstrates (Ts=RT)	Zr1-xGex	Zr0.9Mo0.1	Zr	0.9	Mo	0.1																					1984																																													beta-phase	K		3.68					3.68	MTC131144																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131146	SSC0500189	amorphous. liquid quenching onsubstrates (Ts=RT)	a-Zr	Zr1	Zr	1																							1984																												AMOR																		K		3.5					3.5																																																																																																melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131147	SSC0500189	amorphous. liquid quenching onsubstrates (Ts=RT)	a-(Zr,Ge)	Zr0.87Ge0.13	Zr	0.87	Ge	0.13																					1984																												AMOR																		K		2.94					2.94	MTC131148																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131148	SSC0500189	amorphous. liquid quenching onsubstrates (Ts=RT)	a-(Zr,Pd)	Zr0.75Pd0.25	Zr	0.75	Pd	0.25																					1984																												AMOR																		K		3					3	MTC131148																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131149	SSC0500189	amorphous. liquid quenching onsubstrates (Ts=RT)	a-(Zr,Ni)	Zr0.8Ni0.2	Zr	0.8	Ni	0.2																					1984																												AMOR																		K		3.59					3.59	MTC131148																																																																																															melt in arc-furnace, liquid quench on RT-substrates					Superconductivity of the allotropic forms of zirconium-based alloys obtained by liquid quenching on hot substrates			Department of Physics, University of Virginia, Charlottesvdle, VA 22901, U S A	Solid State Commun., 50(1984)189	S.J.Poon,T.E.Dowling		
131150	PRB0302542	martensitic phase transformation . fraction of rhombo-phase determined to be 0.58 from SP. Tc shows for rhombo-phase.	V2Zr	V2Zr1	V	2	Zr	1																					1984																										AB2		MgCu2(Laves)																	MgCu2, C15	K		8					8																																																								mJ/mol.K2	18.9	SP-heat	189	SP-heat																																									Phase instability, spin fluctuations, and superconductivity in the C15 compound V2Zr			Department of Applied Physics and Information Science, University of California, San Diego, La Jolla, Catif. 92093 (U.S.A.)	Phys.Rev.B, 30(1984)2542	H.Keiber,C.Geibel,B.Renker,H.Rietschel,H.Schmidt,H.Wuhl,G.R.Stewart		
131151	PRB0302542	martensitic phase transformation . fraction of rhombo-phase determined to be 0.80 from SP. Tc shows for rhombo-phase.	V2Zr	V2Zr1	V	2	Zr	1																					1984																										AB2		MgCu2(Laves)																	MgCu2, C15	K		8					8																																																								mJ/mol.K2	17.8	SP-heat	195	SP-heat																																									Phase instability, spin fluctuations, and superconductivity in the C15 compound V2Zr			Department of Applied Physics and Information Science, University of California, San Diego, La Jolla, Catif. 92093 (U.S.A.)	Phys.Rev.B, 30(1984)2542	H.Keiber,C.Geibel,B.Renker,H.Rietschel,H.Schmidt,H.Wuhl,G.R.Stewart		
131152	PRB0302542	martensitic phase transformation . fraction of rhombo-phase determined to be 0.96 from SP. Tc shows for rhombo-phase.	V2Zr	V2Zr1	V	2	Zr	1																					1984																										AB2		MgCu2(Laves)																	MgCu2, C15	K		7.7					7.7																																																								mJ/mol.K2	16.2	SP-heat	203	SP-heat																																									Phase instability, spin fluctuations, and superconductivity in the C15 compound V2Zr			Department of Applied Physics and Information Science, University of California, San Diego, La Jolla, Catif. 92093 (U.S.A.)	Phys.Rev.B, 30(1984)2542	H.Keiber,C.Geibel,B.Renker,H.Rietschel,H.Schmidt,H.Wuhl,G.R.Stewart		
131153	PRB0302542	martensitic phase transformation . fraction of rhombo-phase determined to be 0.90 from SP. Tc shows for rhombo-phase.	V2Zr	V2Zr1	V	2	Zr	1																					1984																										AB2		MgCu2(Laves)																	MgCu2, C15	K		8					8																																																								mJ/mol.K2	17	SP-heat	195	SP-heat																																									Phase instability, spin fluctuations, and superconductivity in the C15 compound V2Zr			Department of Applied Physics and Information Science, University of California, San Diego, La Jolla, Catif. 92093 (U.S.A.)	Phys.Rev.B, 30(1984)2542	H.Keiber,C.Geibel,B.Renker,H.Rietschel,H.Schmidt,H.Wuhl,G.R.Stewart		
131154	LES0650013	fast quenched alloy. fcc	(Th,Zr)	Th0.95Zr0.05	Th	0.95	Zr	0.05																				1	1979																												fcc			A	5.0605													fcc	K		0.69					0.69	MTC131155																																																																																																				Superconductivity in Th-Zr alloys				J.Less-Common Met., 65(1979)13	H.L.Luo,J.G.Huber		
131155	LES0650013	fast quenched alloy. bcc	(Th,Zr)	Th0.3Zr0.7	Th	0.3	Zr	0.7																				1	1979																												bcc			A	3.7272													bcc	K		2.7					2.7	MTC131155																																																																																																				Superconductivity in Th-Zr alloys				J.Less-Common Met., 65(1979)13	H.L.Luo,J.G.Huber		
131156	LES0650013	fast quenched alloy. hcp	(Th,Zr)	Th0.05Zr0.95	Th	0.05	Zr	0.95																				1	1979																												hcp																	hcp	K		0.73					0.73	MTC131155																																																																																																				Superconductivity in Th-Zr alloys				J.Less-Common Met., 65(1979)13	H.L.Luo,J.G.Huber		
131157	LES0600115	quenched from 905 C (beta-phase).	(Th,Zr)	Th0.25Zr0.75	Th	0.25	Zr	0.75																				1	1978																															A	3.701													bcc	K		6.29					6.29																																																																																																arc-melting, then quenched from melt					Superconducting temperatures of quenched thorium-zirconium alloys			Ames Laboratory, U.S. DOE and Department of Materials Science and Engineering, Iowa State University, Ames, Iowa 5001 I (U.S.A.)	J.Less-Common Met., 60(1978)115	D.T.Peterson,J.E.Ostenson,W.A.Taylor		
131158	LES0600115	quenched from 905 C (beta-phase).	(Th,Zr)	Th0.2Zr0.8	Th	0.2	Zr	0.8																				1	1978																															A	3.392	5.541	5.332											ortho	K		3.3					3.3																																																																																																arc-melting, then quenched from melt					Superconducting temperatures of quenched thorium-zirconium alloys			Ames Laboratory, U.S. DOE and Department of Materials Science and Engineering, Iowa State University, Ames, Iowa 5001 I (U.S.A.)	J.Less-Common Met., 60(1978)115	D.T.Peterson,J.E.Ostenson,W.A.Taylor		
131159	LES0600115	quenched from 905 C (beta-phase).	(Th,Zr)	Th0.1Zr0.9	Th	0.1	Zr	0.9																				1	1978																															A	3.258		5.248											hcp	K		2.58					2.58																																																																																																arc-melting, then quenched from melt					Superconducting temperatures of quenched thorium-zirconium alloys			Ames Laboratory, U.S. DOE and Department of Materials Science and Engineering, Iowa State University, Ames, Iowa 5001 I (U.S.A.)	J.Less-Common Met., 60(1978)115	D.T.Peterson,J.E.Ostenson,W.A.Taylor		
131160	LES0440177	as-cast	(Tc,Ti)	Tc0.97Ti0.03	Tc	0.97	Ti	0.03																					1976																																													hcp	K	10.23		10.89				10.56																																																																																																arc-melting, ANN(700 - 1500C, in vac)					Superconductivity in the technetium-titanium alloy system			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37830 (U.S.A.)	J.Less-Common Met., 44(1976)177	C.C.Koch		
131161	LES0440177	ANN(1500C). Hardness = 960 kg/mm2.	(Tc,Ti)	Tc0.875Ti0.125	Tc	0.875	Ti	0.125																					1976																												alpha-Mn			A	9.5													alpha-Mn + hcp	K	7.9		9.5				8.7																																																																																																arc-melting, ANN(700 - 1500C, in vac)					Superconductivity in the technetium-titanium alloy system			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37830 (U.S.A.)	J.Less-Common Met., 44(1976)177	C.C.Koch		
131162	LES0440177	as-cast	(Tc,Ti)	Tc0.75Ti0.25	Tc	0.75	Ti	0.25																					1976																																													bcc	K	4.2		6				5.1																																																																																																arc-melting, ANN(700 - 1500C, in vac)					Superconductivity in the technetium-titanium alloy system			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37830 (U.S.A.)	J.Less-Common Met., 44(1976)177	C.C.Koch		
131163	LES0440177	ANN(700C). not SC.	(Tc,Ti)	Tc0.5Ti0.5	Tc	0.5	Ti	0.5																					1976																															A	3.091													CsCl	K					1.7																																																																																																		arc-melting, ANN(700 - 1500C, in vac)					Superconductivity in the technetium-titanium alloy system			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37830 (U.S.A.)	J.Less-Common Met., 44(1976)177	C.C.Koch		
131164	LES0440177	as-cast. Hardness = 443 kg/mm2	(Tc,Ti)	Tc0.25Ti0.75	Tc	0.25	Ti	0.75																					1976																															A	3.181													bcc	K	2.65		2.75				2.7																																																																																																arc-melting, ANN(700 - 1500C, in vac)					Superconductivity in the technetium-titanium alloy system			Metals and Ceramics Division, Oak Ridge National Laboratory, Oak Ridge, Tenn. 37830 (U.S.A.)	J.Less-Common Met., 44(1976)177	C.C.Koch		
131165	LES0420285	(dC/gamma*Tc) = 1.35 . lattice term in SP (beta) = 0.035 mJ/mol.K4	(Ti,V)	Ti0.85V0.15	Ti	0.85	V	0.15																					1975																																														K	1.9		2				1.95																																																								mJ/mol.K2	5.9	SP-heat	381	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131166	LES0420285	(dC/gamma*Tc) = 1.70 . lattice term in SP (beta) = 0.085 mJ/mol.K4	(Ti,V)	Ti0.8V0.2	Ti	0.8	V	0.2																					1975																																													beta-phase	K	4		4.2				4.1																																																								mJ/mol.K2	7.1	SP-heat	284	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131167	LES0420285	(dC/gamma*Tc) = 2.09 . lattice term in SP (beta) = 0.126 mJ/mol.K4	(Ti,V)	Ti0.7V0.3	Ti	0.7	V	0.3																					1975																																													beta-phase	K	6.2		6.3				6.25																																																								mJ/mol.K2	9.2	SP-heat	249	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131168	LES0420285	(dC/gamma*Tc) = 2.0 . lattice term in SP (beta) = 0.098 mJ/mol.K4	(Ti,V)	Ti0.6V0.4	Ti	0.6	V	0.4																					1975																																													beta-phase	K	6.9		7				6.95	MTC131168																																																							mJ/mol.K2	10.5	SP-heat	271	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131169	LES0420285	(dC/gamma*Tc) = 1.96 . lattice term in SP (beta) = 0.084 mJ/mol.K4	(Ti,V)	Ti0.5V0.5	Ti	0.5	V	0.5																					1975																																													beta-phase	K	7		7.2				7.1																																																								mJ/mol.K2	10.5	SP-heat	285	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131170	LES0420285	(dC/gamma*Tc) = 1.96 . lattice term in SP (beta) = 0.068 mJ/mol.K4	(Ti,V)	Ti0.4V0.6	Ti	0.4	V	0.6																					1975																																													beta-phase	K	7.2		7.4				7.3																																																								mJ/mol.K2	10.6	SP-heat	306	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131171	LES0420285	(dC/gamma*Tc) = 1.75 . lattice term in SP (beta) = 0.054 mJ/mol.K4	(Ti,V)	Ti0.2V0.8	Ti	0.2	V	0.8																					1975																																													beta-phase	K	7		7.3				7.15																																																								mJ/mol.K2	10.5	SP-heat	330	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131172	LES0420285	(dC/gamma*Tc) = 1.56 . lattice term in SP (beta) = 0.041 mJ/mol.K4	(Ti,V)	Ti0.1V0.9	Ti	0.1	V	0.9																					1975																																													beta-phase	K	5.7		5.8				5.75																																																								mJ/mol.K2	10.2	SP-heat	362	SP-heat																																				arc-melting. ANN(1000C,1h) - Q to iced brine.					Low-temperature-calorimetric studies of superconductivity and microstructure in titanium-vanadium alloys			Battelle Columbus Laboratories, Columbus, Chio 43201 (U.S.A.)	J.Less-Common Met., 42(1975)285	E.W.Collings,P.E.Upton,J.C.Ho		
131173	JPC0024559	bcc, metastable sample. broad transition.	(Zr,Si)	Si0.108Zr0.892	Si	0.108	Zr	0.892																					1990																																													bcc	K			3.54			0.21	3.54																																																											194	SP-heat																																									Specific heat of metastable Zr1-xSix alloys				J.Phys.:Condens.Matter, 2(1990)4559	G.Flinspach,C.Surgers,H von Lohneysen		
131174	JPC0024559	amorphous. sharp transition in SUS and SP measurements. (dC/gamma*Tc) = 1.87	(Zr,Si)	Si0.132Zr0.868	Si	0.132	Zr	0.868																					1990																												AMOR																		K		3.21				0.03	3.21																																																																																																					Specific heat of metastable Zr1-xSix alloys				J.Phys.:Condens.Matter, 2(1990)4559	G.Flinspach,C.Surgers,H von Lohneysen		
131175	JPS0490839	not SC. large peak of R(T) at 150 K. R(RT) = 0.7 mOhm.cm  for I//chain axis.	ZrTa5	Ta5Zr1	Ta	5	Zr	1																				3	1980																										AB5			Cmcm		A	3.9876	14.502	13.727												K					1.2																																																																																																		iodine vapor transport method from (ZrTe3 + Te). heat)520C,7w)					Giant resistivity anomaly in ZrTe5			Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 49(1980)839	S.Okada,T.Sambongi,M.Ido		
131176	JPS0490839	by-product of ZrTa5. RRR = 20. R(RT) = 0.13 mOhm.cm  for I//chain axis.	1T-ZrTa2	Ta2Zr1	Ta	2	Zr	1																				3	1980																										AB2																				K		2.3					2.3																																																																																																iodine vapor transport method from (ZrTe3 + Te). heat)520C,7w)					Giant resistivity anomaly in ZrTe5			Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 49(1980)839	S.Okada,T.Sambongi,M.Ido		
131177	SSC0151643	(dC/gamma*Tc) = 1.16	TaV2	Ta1V2	Ta	1	V	2																					1974																										AB2		MgCu2(Laves)			A	7.153													C15	K		3.6					3.6																																																								mJ/gat.K2	11	SP-heat	278	SP-heat																																				arc-melting.  Wrapped in Zr-foil, then ANN(1000C,35d, in silica tube)					Superconductivity of TaV2			University of California, San Diego	Solid State Commun., 15(1974)1643	P.F.Schippnick,A.C.Lawson		
131178	SSC0151643	(dC/gamma*Tc) = 1.45	TaV2	Ta1V2	Ta	1	V	2																					1974																										AB2					A	3.15													bcc	K		2.8					2.8																																																								mJ/gat.K2	9	SP-heat	325	SP-heat																																				arc-melting.  Wrapped in Zr-foil, then ANN(1000C,35d, in silica tube)					Superconductivity of TaV2			University of California, San Diego	Solid State Commun., 15(1974)1643	P.F.Schippnick,A.C.Lawson		
131179	SSC0481089	samples beyond solubility limit were prepared by recrystalization of amorphous films	(Ta,Zr)	Ta0.455Zr0.545	Ta	0.455	Zr	0.545																					1983																															A	3.44														K		7.7					7.7																																																																																																films prepared by coevaporation using electron beam. as-prepared films (AMOR) - recrystalize					Formation of superconductive supersaturated TaZr solid solution by pulsed electronbeam treatment				Solid State Commun., 48(1983)1089	G.Linker,J.Geerk		
131180	SSC0481089	samples beyond solubility limit were prepared by recrystalization of amorphous films	(Ta,Zr)	Ta0.745Zr0.255	Ta	0.745	Zr	0.255																					1983																															A	3.361														K		7.1					7.1																																																																																																films prepared by coevaporation using electron beam. as-prepared films (AMOR) - recrystalize					Formation of superconductive supersaturated TaZr solid solution by pulsed electronbeam treatment				Solid State Commun., 48(1983)1089	G.Linker,J.Geerk		
131181	JPS0562225	monoclinic, beta = 106.26.  RRR = 50 - 65. I//needle axis	TaSe3	Se3Ta1	Se	3	Ta	1																					1987																										AB3			P2<1>/m		A	10.402	3.495	9.829											monoclinic, beta=106.26 deg.	K		2.1					2.1																																																																							Ohm.cm											1																			Normal-state electrical resistivity in quasi-one-dimensional conductor TaSe3			Muroran Institute of Technology, Japan	J.Phys.Soc.Jpn, 56(1987)2225	S.Nagata,Y.Hodosawa,S.Taniguchi,K.Yamaya		
131182	LES1190337		(V,Re)	Re0.8V0.2	Re	0.8	V	0.2																					1986																																													alloy	K		5.2					5.2																																																																																																arc-melting. ANN(1400C,90h, in vac, wrapped in W-foils)					The vanadium-rhenium system: Phase diagram and superconductivity			University of Geneva	J.Less-Common Met., 119(1986)337	J.L.Jorda,J.Muller		
131183	LES1190337		(V,Re)	Re0.8V0.2	Re	0.8	V	0.2																					1986																																													A15-phase	K		7.2					7.2																																																																																																arc-melting. ANN(1400C,90h, in vac, wrapped in W-foils)					The vanadium-rhenium system: Phase diagram and superconductivity			University of Geneva	J.Less-Common Met., 119(1986)337	J.L.Jorda,J.Muller		
131184	LES1250261	heat treatment(1150C,1h). not SC. paramag at LT. SUS = 82.3E-6 emu/gat.	(Hf,Os)	Hf0.77Os0.23	Hf	0.77	Os	0.23																					1986																																														K					1.4																																																										mJ/gat.K2	3.6	SP-heat	225	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131185	LES1250261	heat treatment(1000C,1h). not SC. super-paramag at LT. SUS = 199 E-6 emu/gat.	TiFe	Fe1Ti1	Fe	1	Ti	1																					1986																										AB		CsCl																	CsCl, B2	K					1.4																																																										mJ/gat.K2	1.7	SP-heat	540	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131186	LES1250261	heat treatment(1000C,1h). not SC.  SUS = 44.6 E-6 emu/gat.	ZrRu	Ru1Zr1	Ru	1	Zr	1																					1986																										AB		CsCl																	CsCl, B2	K					1.4																																																										mJ/gat.K2	1	SP-heat	404	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131187	LES1250261	heat treatment(2000C,2h). not SC. paramag at LT. SUS = 24.5 E-6 emu/gat.	HfOs	Hf1Os1	Hf	1	Os	1																					1986																										AB		CsCl																	CsCl, B2	K					1.4																																																										mJ/gat.K2	0.66	SP-heat	348	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131188	LES1250261	as-cast. not SC.	TiFe2	Fe2Ti1	Fe	2	Ti	1																					1986																										AB2		MgZn2(Laves)																	MgZn2(Laves), C14	K					1.4																																																										mJ/gat.K2	7.26	SP-heat	518	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131189	LES1250261	heat treatment(1700C,1h). SUS = 116 E-6 emu/gat. (dC/gamma*Tc) = 1.32. e-ph coupling = 0.49.	ZrRu2	Ru2Zr1	Ru	2	Zr	1																					1986																										AB2		MgZn2(Laves)																	MgZn2(Laves), C14	K		1.92					1.92																																																								mJ/gat.K2	4.72	SP-heat	361	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131190	LES1250261	heat treatment(1600C,1h). SUS = 71.9 E-6 emu/gat. (dC/gamma*Tc) = 1.46. e-ph coupling = 0.49.	HfOs2	Hf1Os2	Hf	1	Os	2																					1986																										AB2		MgZn2(Laves)																	MgZn2(Laves), C14	K		1.85					1.85																																																								mJ/gat.K2	2.84	SP-heat	330	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131191	LES1250261	as-cast.  SUS = 87.6 E-6 emu/gat. (dC/gamma*Tc) = 1.26. e-ph coupling = 0.55.	ZrOs2	Os2Zr1	Os	2	Zr	1																					1986																										AB2		MgZn2(Laves)																	MgZn2(Laves), C14	K		2.9					2.9																																																								mJ/gat.K2	3.7	SP-heat	308	SP-heat																																									Electronic, magnetic, superconducting and amorphous forming properties versus stability of the Ti-Fe, Zr-Ru, and Hf-Os ordered alloys				J.Less-Common Met., 125(1986)261	R.Kuentzler,R.M.Waterstrat		
131192	LES1340079	Se-concentration x = 0.183 in Pd1-xSex. Tc defined as mid of SUS-change.	Pd9Se2	Pd9Se2	Pd	9	Se	2																					1987																										A2B9																				K		0.7		0.64			0.7																																																																																																					Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131193	LES1340079	Se-concentration x = 0.20 in Pd1-xSex. Tc defined as mid of SUS-change.	Pd4Se	Pd4Se1	Pd	4	Se	1																					1987																										AB4																				K					0.38																																																																																																							Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131194	LES1340079	Se-concentration x = 0.222 in Pd1-xSex. Tc defined as mid of SUS-change.	Pd7Se2	Pd7Se2	Pd	7	Se	2																					1987																										A2B7																				K				0.53			0.53																																																																																																					Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131195	LES1340079	Se-concentration x = 0.245 in Pd1-xSex. Tc defined as mid of SUS-change.	Pd34Se11	Pd34Se11	Pd	34	Se	11																					1987																										A11B34																				K				2.66			2.66																																																																																																					Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131196	LES1340079	Se-concentration x = 0.364 in Pd1-xSex. Tc defined as mid of SUS-change.	Pd7Se4	Pd7Se4	Pd	7	Se	4																					1987																										A4B7																				K					0.38																																																																																																							Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131197	LES1340079	Amorphous. Se-concentration x = 0.30 in Pd1-xSex. Tc defined as mid of SUS-change.	a-PdSe	Pd0.7Se0.3	Pd	0.7	Se	0.3																					1987																												AMOR																		K				2.04			2.04																																																																																																					Superconductivity and phase relations in the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Less-Common Met., 134(1987)79	T.Takabatake,M.Ishikawa,J.L.Jorda		
131198	JPS0572763	Se-concentration x = 0.183 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 5.6	Pd9Se2	Pd9Se2	Pd	9	Se	2																					1988																										A2B9																				K				0.64			0.64																													T/K	resistivity	0.42			MHC131198																																																																			Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131199	JPS0572763	Se-concentration x = 0.20 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 259	Pd4Se	Pd4Se1	Pd	4	Se	1																					1988																										AB4																				K					0.38																																																																																																							Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131200	JPS0572763	Se-concentration x = 0.222 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 228	Pd7Se2	Pd7Se2	Pd	7	Se	2																					1988																										A2B7																				K				0.53			0.53																															0.28			MHC131198																																																																			Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131201	JPS0572763	Se-concentration x = 0.245 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 39.9. (dC/gamma*Tc) = 1.86	Pd34Se11	Pd34Se11	Pd	34	Se	11																					1988																										A11B34																				K				2.66			2.66																															0.44			MHC131201																						mJ/gat.K2	1.67	SP-heat	173	SP-heat																																									Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131202	JPS0572763	Se-concentration x = 0.364 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 283	Pd7Se4	Pd7Se4	Pd	7	Se	4																					1988																										A4B7																				K					0.38																																																																																																							Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131203	JPS0572763	Amorphous. Se-concentration x = 0.30 in Pd1-xSex. Tc defined as mid of SUS-change. RRR = 0.96	a-PdSe	Pd0.7Se0.3	Pd	0.7	Se	0.3																					1988																												AMOR																		K				2.04			2.04																															1.67			MHC131201																																																																			Superconducting properties of the Pd-Se system			Institute for Solid State Physics, University of Tokyo	J.Phys.Soc.Jpn, 57(1988)2763	T.Takabatake,M.Ishikawa,Alain Junod		
131204	LES1710171	SUS = 80 E-6 emu/mol	Re2Si	Re2Si1	Re	2	Si	1																					1991																										AB2			P2<1>/b		A	6.4444	5.3898	9.6019											monoclinic, gamma = 94.214	K		3.8					3.8																																																																							mOhm.cm											0.12														modified tri-arc furnace					Crystal structure and superconductivity in Re2Si			AT&T Bell Lab.	J.Less-Common Met., 171(1991)171	T.Siegrist,J.E.Greedan,J.D.Garrett,Gong Wenhe,C.V.Stager		
131205	PRL0491030	tunneling at (100) cleaved surface	YSe	Se1Y1	Se	1	Y	1																					1982																										AB		NaCl																		K		4					4																																														meV	0.67	3.9	1																																																				Electron tunneling into intermediate-valence materials				Phys.Rev.Lett., 49(1982)1030	G.Guntherodt,W.A.Thompson,F.Holtzberg,Z.Fisk		
131206	PRB0301253		(Ti,Mo)	Mo0.15Ti0.85	Mo	0.15	Ti	0.85																					1984																																													meta-stable	K		4.08					4.08																				T		6.55																																																	mOhm.cm											0.115														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131207	PRB0301253		(Ti,Pd)	Pd0.15Ti0.85	Pd	0.15	Ti	0.85																					1984																																													meta-stable	K		3.82					3.82																				T		6.63																																																	mOhm.cm											0.21														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131208	PRB0301253	rapid quenched sample.	a-(Zr,Rh)	Rh0.25Zr0.75	Rh	0.25	Zr	0.75																					1984																												AMOR																	amorphous-like	K		4.3					4.3																				T		8																																																	mOhm.cm											0.16														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131209	PRB0301253		(Zr,Rh)	Rh0.25Zr0.75	Rh	0.25	Zr	0.75																					1984																																													meta-stable	K		3.97					3.97																				T		7.2																																																	mOhm.cm											0.155														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131210	PRB0301253		(Zr,Pd)	Pd0.15Zr0.85	Pd	0.15	Zr	0.85																					1984																																													meta-stable	K		4.8					4.8																				T		7.69																																																	mOhm.cm											0.13														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131211	PRB0301253		(Zr,Mo)	Mo0.07Zr0.93	Mo	0.07	Zr	0.93																					1984																																													meta-stable	K		4.91					4.91																				T		6.81																																																	mOhm.cm											0.13														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131212	PRB0301253		(Zr,Mo)	Mo0.04Zr0.96	Mo	0.04	Zr	0.96																					1984																																													meta-stable	K		4.47					4.47																				T		5.57																																																	mOhm.cm											0.119														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131213	PRB0301253		(Hf,Mo)	Hf0.906Mo0.094	Hf	0.906	Mo	0.094																					1984																																													meta-stable	K		2.71					2.71																				T		4.58																																																	mOhm.cm											0.165														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131214	PRB0301253		(Ta,Hf)	Hf0.25Zr0.75	Hf	0.25	Zr	0.75																					1984																																													meta-stable	K		6.62					6.62																				T		5.84																																																	mOhm.cm											0.06														liquid quenched sample					Upper critical fields in liquid-quenched metastable superconductors			Unversity of Virginia	Phys.Rev.B, 30(1984)1253	K.M.Wong,E.J.Cotts,S.J.Poon		
131215	JAP0393003	mobility= 2.0 cm2/V.sec	Tl5Te3	Te3Tl5	Te	3	Tl	5																					1968									9.52																	A3B5					A	8.92		12.63											gamma-phase, bct	K	2.19		2.23				2.21																				T					0.11			1.5																																																																n/cm3	15000000000000000000000								Electrical conductivity and superconductivity in the gamma phase of the Tl-Te system			Northwestern University	J.Appl.Phys., 39(1968)3003	A.Juodakis,C.R.Kannewurf		
131216	PRB0311329	lattice term in SP (beta) = 0.435 mJ/mol.K4	UAl2Si2	Al2Si2U1	Al	2	Si	2	U	1																			1985																										AB2C2					A	4.145														K		1.34					1.34																																																								mJ/mol.K2	27.9	SP-heat																																						arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131217	PRB0311329		UAl2Ge2	Al2Ge2U1	Al	2	Ge	2	U	1																			1985																										AB2C2					A	4.219														K		1.6					1.6																																																																																																arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131218	PRB0311329		UGa2Ge2	Ga2Ge2U1	Ga	2	Ge	2	U	1																			1985																										AB2C2					A	4.218														K		0.87					0.87																																																																																																arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131219	PRB0311329	lattice term in SP (beta) = 0.413 mJ/mol.K4	URu3	Ru3U1	Ru	3	U	1																					1985																										AB3					A	3.977														K		0.145					0.145																																																								mJ/mol.K2	12.2	SP-heat																																						arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131220	PRB0311329		URu2Rh	Rh1Ru2U1	Rh	1	Ru	2	U	1																			1985																										ABC2					A	3.977														K					0.02																																																																																																		arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131221	PRB0311329		USi3	Si3U1	Si	3	U	1																					1985																										AB3					A	4.0348														K					0.02																																																																																																		arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131222	PRB0311329	AF at 67 K.	UGa3	Ga3U1	Ga	3	U	1																					1985								67																		AB3					A	4.256														K					0.02																																																																																																		arc-melting					Superconductivity in uranium compounds with Cu3Au structure				Phys.Rev.B, 31(1985)1329	H.R.Ott,F.Hulliger,H.Rudigier,Z.Fisk		
131223	PRL0350062	R//layer shows two step at 315 and 21 K.	4Hb-TaS2	S2Ta1	S	2	Ta	1																				3	1975																										AB2		TaSe2																		K		2.5					2.5																																																																																																iodine vapor transport method					Tunneling conductivity in 4Hb-TaS2			Simon Fraser University, Canada	Phys.Rev.Lett., 35(1975)62	W.J.Wattamaniuk,J.P.Tidman,R.F.Frindt		
131224	CHM0410315	Hc2(1.6K) = 0.2 T.	TaSe3	Se3Ta1	Se	3	Ta	1																					1982									8.11																	AB3					A	101.02	3.48	15.56											monoclinic, beta = 109.6	K		1.9					1.9																				T					0.6			1.4																																											mOhm.cm											2														mixture - high pressure synthesis(700C,2GPa, in BN)					High-Pressure Syntheses of TaS3, NbS3, TaSe3, and NbSe3 with NbSe3-Type Crystal Structure				J.Solid State Chem., 41(1982)315	S.Kikkawa,N.Ogawa,M.Koizumi,Y.Onuki		
131225	CHM0410315	semiconductor. two transitions at 200K and 250 K.	TaS3	S3Ta1	S	3	Ta	1																					1982									6.18																	AB3					A	9.52	3.35	14.92											monoclinic, beta = 110.0	K					1.4																																																																																																		mixture - high pressure synthesis(700C,2GPa, in BN)					High-Pressure Syntheses of TaS3, NbS3, TaSe3, and NbSe3 with NbSe3-Type Crystal Structure				J.Solid State Chem., 41(1982)315	S.Kikkawa,N.Ogawa,M.Koizumi,Y.Onuki		
131226	CHM0410315	semiconductor. X-ray density in DB	NbS3	Nb1S3	Nb	1	S	3																					1982									4.15																	AB3					A	9.68	3.37	14.83											monoclinic, beta = 109.9	K					1.4																																																																																																		mixture - high pressure synthesis(700C,2GPa, in BN)					High-Pressure Syntheses of TaS3, NbS3, TaSe3, and NbSe3 with NbSe3-Type Crystal Structure				J.Solid State Chem., 41(1982)315	S.Kikkawa,N.Ogawa,M.Koizumi,Y.Onuki		
131227	CHM1140486	Tc defined as diamagnetic onset. X-ray density in DB	6R-TaS2	S2Ta1	S	2	Ta	1																				1	1995																										AB2																				K			2.3				2.3			K/GPa	1.3																																																																																												mixture - heat(1220K,8d, in vac)					Physical properties of 6R-TaS2				J.Solid State Chem., 114(1995)486	E.Figueroa,Y.-K.Kuo,A.Olinger,M.A.Lloyd,L.D.Bastin,S.Petrotsatos,Q.Chen,B.Dobbs,S.Dev,J.P.Selegue,L.E.DeLong,C.P.Brock,J.W.Brill		
131228	SSC0310627	P: hydrostatic. I//b-axis. RRR = 59.2.	TaSe3	Se3Ta1	Se	3	Ta	1																					1979																										AB3		TaSe3																	TaSe3	K		2.3					2.3			K/GPa	-0.75																																																																																												mixture - sealed in quartz - heat(700C,2w)					The effect of pressure on the superconducting transition temperature in TaSe3				Solid State Commun., 31(1979)627	K.Yamaya,T.H.Ceballe,J.F.Kwak,R.L.Greene		
131229	LES0220246		ThRe2	Re2Th1	Re	2	Th	1																					1970																										AB2		MgZn2(Laves)			A	5.4927		9.101											MgZn2, C14	K		5					5																																																																																																melt using EB. water-cooled copper heath.					Superconductivity and lattice parameters of the dirhenides and ditechnides of thorium, hafnium and zirconium				J.Less-Common Met., 22(1970)246	A.L.Giorgi,E.G.Szklarz		
131231	LES0220246		HfRe2	Hf1Re2	Hf	1	Re	2																					1970																										AB2		MgZn2(Laves)			A	5.254		8.6											MgZn2, C14	K		5.2					5.2																																																																																																melt using EB. water-cooled copper heath.					Superconductivity and lattice parameters of the dirhenides and ditechnides of thorium, hafnium and zirconium				J.Less-Common Met., 22(1970)246	A.L.Giorgi,E.G.Szklarz		
131233	LES0220246	chemical analysis: Zr0.332Tc0.668	ZrRe2	Re2Zr1	Re	2	Zr	1																					1970																										AB2		MgZn2(Laves)			A	5.267		8.632											MgZn2, C14	K		6.4					6.4																																																																																																melt using EB. water-cooled copper heath.					Superconductivity and lattice parameters of the dirhenides and ditechnides of thorium, hafnium and zirconium				J.Less-Common Met., 22(1970)246	A.L.Giorgi,E.G.Szklarz		
131235	LES0610231		NbS	Nb1S0.899	Nb	1	S	0.899																					1978																										AB		FeAs			A	4.897	3.319	6.559												K		3.83					3.83			K/GPa	0.28																																																																																												react(450C, in silica tube) - ANN(1450C,5h) - Q					Superconductivity in the niobium and scandium mono-sulfide systems at pressures up to 20 kbar				J.Less-Common Met., 61(1978)231	P.B.V.Narayan,D.K.Finnemore		
131236	LES0610231		NbS	Nb1S1.06	Nb	1	S	1.06																					1978																										AB		FeAs																		K		3.3					3.3																																																																																																react(450C, in silica tube) - ANN(1450C,5h) - Q					Superconductivity in the niobium and scandium mono-sulfide systems at pressures up to 20 kbar				J.Less-Common Met., 61(1978)231	P.B.V.Narayan,D.K.Finnemore		
131237	LES0610231		ScS	S1.005Sc1	S	1.005	Sc	1																					1978																										AB		NaCl			A	5.1917														K		5.37					5.37			K/GPa	-0.2																																																				mJ/mol.K2	1.7																																							react(900C, in quartz tube) - ANN(1300-1700C)					Superconductivity in the niobium and scandium mono-sulfide systems at pressures up to 20 kbar				J.Less-Common Met., 61(1978)231	P.B.V.Narayan,D.K.Finnemore		
131238	PRL0500853	RRR = 50. martensitic transformation at 50.6 K.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1983																										AB3		Cr3Si(A15)																		K		18					18																																																3.78	4																																																				Electronic Raman scattering by superconducting-gap excitations in Nb3Sn and V3Si				Phys.Rev.Lett., 50(1983)853	S.B.Dierker,M.V.Klein,G.W.Webb,Z.Fisk		
131239	PRL0500853	RRR = 15.	V3Si	Si1V3	Si	1	V	3																					1983																										AB3		Cr3Si(A15)																		K		16.9					16.9																																																3.4	4																																																				Electronic Raman scattering by superconducting-gap excitations in Nb3Sn and V3Si				Phys.Rev.Lett., 50(1983)853	S.B.Dierker,M.V.Klein,G.W.Webb,Z.Fisk		
131240	SSC0810179	G-L parameter = 28.	(Nb,Zr)	Nb0.15Zr0.85	Nb	0.15	Zr	0.85																					1992																																														K		6.5					6.5																																				A		58			A		2630																																																					films deposited using coevaporation on polished saphire by EB					PINNING,CREEP AND POSSIBLE MELTING IN THE MIXED STATE OF NBZRFILMS	199201			J.SOLID STATE COMMUN.,81(1992)179	D.O.WELCH,M.SUENAGA,R.C.BUDHANI	NB,ZR	
131241	SSC0270291	lattice term coeffic. (beta) = 0.0285 mJ/gat.K4.	VRe3	Re0.71V0.29	Re	0.71	V	0.29																					1978																												Cr3Si(A15)																		K		8.4					8.4																																																3.4	14							mJ/gat.K2	4.03	SP-heat	409	SP-heat																																				arc-melting. ANN(1750C)					Discovery of a superconducting A-15 phase in the V-Re system				Solid State Commun., 27(1978)291	A.L.Giorgi,B.T.Matthias,G.R.Stewart		
131242	SSC0270291		(V,Os)	Os0.5V0.5	Os	0.5	V	0.5																					1978																																														K		5.15					5.15																																																								mJ/gat.K2	4.34	SP-heat	395	SP-heat																																									Discovery of a superconducting A-15 phase in the V-Re system				Solid State Commun., 27(1978)291	A.L.Giorgi,B.T.Matthias,G.R.Stewart		
131243	SSC0270291		(V,Ir)	Ir0.37V0.67	Ir	0.37	V	0.67																					1978																																														K		1.71					1.71																																																								mJ/gat.K2	4.76	SP-heat	385	SP-heat																																									Discovery of a superconducting A-15 phase in the V-Re system				Solid State Commun., 27(1978)291	A.L.Giorgi,B.T.Matthias,G.R.Stewart		
131244	SSC0270291		(V,Pt)	Pt0.25V0.75	Pt	0.25	V	0.75																					1978																																														K		3.2					3.2																																																								mJ/gat.K2	7.19	SP-heat	511	SP-heat																																									Discovery of a superconducting A-15 phase in the V-Re system				Solid State Commun., 27(1978)291	A.L.Giorgi,B.T.Matthias,G.R.Stewart		
131245	SSC0280969	lattice term coeffic. (beta) = 0.05639 mJ/gat.K4.	(Mo,Re)	Mo0.6Re0.4	Mo	0.6	Re	0.4																					1978																															A	3.124													A2, bcc	K		12					12																																																5	14							mJ/gat.K2	4.55	SP-heat	325	SP-heat																																									A search for strong coupling superconductivity				Solid State Commun., 28(1978)969	G.R.Stewart,A.L.Giorgi		
131246	SSC0280969	lattice term coeffic. (beta) = 0.04881 mJ/gat.K4.	(Mo,Re)	Mo0.4Re0.6	Mo	0.4	Re	0.6																					1978																															A	9.586		4.978											D8<b>, tetra	K		6					6																																																3.4	14							mJ/gat.K2	3.6	SP-heat	342	SP-heat																																									A search for strong coupling superconductivity				Solid State Commun., 28(1978)969	G.R.Stewart,A.L.Giorgi		
131247	SSC0280969	lattice term coeffic. (beta) = 0.06599 mJ/gat.K4.	(W,Re)	Re0.35W0.65	Re	0.35	W	0.65																					1978																															A	3.139													A2, bcc	K		6.75					6.75																																																3.1	14							mJ/gat.K2	2.49	SP-heat	309	SP-heat																																									A search for strong coupling superconductivity				Solid State Commun., 28(1978)969	G.R.Stewart,A.L.Giorgi		
131248	SSC0280969	lattice term coeffic. (beta) = 0.03396 mJ/gat.K4.	(Mo,Tc)	Mo0.18Tc0.82	Mo	0.18	Tc	0.82																					1978																															A	2.752		4.443											A3, hcp	K		13.7					13.7																																																3.6	14							mJ/gat.K2	8	SP-heat	385	SP-heat																																									A search for strong coupling superconductivity				Solid State Commun., 28(1978)969	G.R.Stewart,A.L.Giorgi		
131249	SSC0470431		(Ti,Pd)	Pd0.07Ti0.93	Pd	0.07	Ti	0.93																					1983																																													alpha+beta phase	K		3.26					3.26																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131250	SSC0470431		(Ti,Pd)	Pd0.1Ti0.9	Pd	0.1	Ti	0.9																					1983																																													alpha+beta phase	K		3.67					3.67																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131251	SSC0470431		(Ti,Pd)	Pd0.14Ti0.86	Pd	0.14	Ti	0.86																					1983																																													beta phase	K		3.74					3.74																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131252	SSC0470431		(Ti,Pd)	Pd0.19Ti0.81	Pd	0.19	Ti	0.81																					1983																																													beta phase	K		3.08					3.08																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131253	SSC0470431		(Ti,Pd)	Pd0.24Ti0.76	Pd	0.24	Ti	0.76																					1983																																													beta phase	K		2					2																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131254	SSC0470431		(Ti,Pd)	Pd0.26Ti0.74	Pd	0.26	Ti	0.74																					1983																																													beta phase	K		1.66					1.66																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131255	SSC0470431		(Zr,Pd)	Pd0.05Ti0.95	Pd	0.05	Ti	0.95																					1983																																													alpha+beta phase	K		4.64					4.64																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131256	SSC0470431		(Zr,Pd)	Pd0.074Ti0.926	Pd	0.074	Ti	0.926																					1983																																													alpha+beta phase	K		4.85					4.85																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131257	SSC0470431		(Zr,Pd)	Pd0.1Ti0.9	Pd	0.1	Ti	0.9																					1983																																													beta phase	K		5					5																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131258	SSC0470431		(Zr,Pd)	Pd0.15Ti0.85	Pd	0.15	Ti	0.85																					1983																																													beta phase	K		4.82					4.82																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131259	SSC0470431		(Zr,Pd)	Pd0.18Ti0.82	Pd	0.18	Ti	0.82																					1983																																													beta phase	K		4.73					4.73																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131260	SSC0470431		(Zr,Pd)	Pd0.2Ti0.8	Pd	0.2	Ti	0.8																					1983																																													beta phase	K		4.71					4.71																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131261	SSC0470431		(Hf,Mo)	Hf0.93Mo0.07	Hf	0.93	Mo	0.07																					1983																															A	3.4877													alpha+beta phase	K		2.11					2.11																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131262	SSC0470431		(Hf,Mo)	Hf0.87Mo0.13	Hf	0.87	Mo	0.13																					1983																															A	3.4887													beta phase	K		2.6					2.6																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131263	SSC0470431		(Hf,Mo)	Hf0.8Mo0.2	Hf	0.8	Mo	0.2																					1983																															A	3.4581													beta phase	K		2.89					2.89																																																																																																arc-melting. then liquid quenched.					Structural dependence of the superconducting transition temperatiure in liquid-quenched alloys based on the group IV B elements				Solid State Commun., 47(1983)431	S.J.Poon		
131264	SSC0500453	as-obtained. RRR = 15.	V3Si	Si1V3	Si	1	V	3																					1984																										AB3		Cr3Si(A15)																		K		16.84				0.16	16.84																													T/K		2																																																																	sample obtained by fusion in a HF furnace					Magnetoresistance measurements of V3Si . Evidence for precursor effects of the martensitic transformation				Solid State Commun., 50(1984)453	X.Zotos,O.Laborde,J.P.Senateur		
131265	SSC0500453	ANN(1200C,24h), the cooled(15 C/h). martensitic transformation. RRR = 29.4.	V3Si	Si1V3	Si	1	V	3																					1984																										AB3		Cr3Si(A15)																		K		16.98				0.07	16.98																													T/K		1.9																																																																	sample obtained by fusion in a HF furnace					Magnetoresistance measurements of V3Si . Evidence for precursor effects of the martensitic transformation				Solid State Commun., 50(1984)453	X.Zotos,O.Laborde,J.P.Senateur		
131266	SSC0441439	RRR=80. [pcohere] in (001) plane. anisotropy (cohere) = 5.7, effective mass ratio = 32.7.	Nb3Se4	Nb3Se4	Nb	3	Se	4																				3	1982																										A3B4																			hexagonal	K		1.85		1.75			1.85																																		MHC131266		A	from Hc2		852	149																															uOhm.cm			1.14										86.4												CVD method					Electrical conduction and critical magnetic field for superconductivity of a Nb3Se4 single crystal				Solid State Commun., 44(1982)1439	Y.Ishihara,I.Nakada		
131272	SSC0390005	A15(50-70%) + tetra-Nb3Si(15-20%) * Nb5Si3(10-20%) + bcc-Nb(5-10%). DOS = 0.94 states /eV-atom for A15. (dC/gamma*Tc) = 2.0.	Nb3Si	Nb3Si1	Nb	3	Si	1																				2	1981																										AB3		Cr3Si(A15)			A	5.091													A15	K		18				0.7	18																																																								mJ/mol.K2	14.2	SP-heat	352	SP-heat																																				arc-melting. ANN(1775-1790C,3-5h)					Specific heat of A-15 Nb3Si produced by explosive compression				Solid State Commun., 39(1981)5	G.R.Stewart,Bart Olinger,L.R.Newkirk		
131273	SSC0390005	Tc defined as lower-Tc of #131272 sample.	Nb3Si	Nb3Si1	Nb	3	Si	1																				2	1981																										AB3																			tetragonal	K		9					9																																																								mJ/mol.K2	8.6	SP-heat	400	SP-heat																																				arc-melting. ANN(1775-1790C,3-5h)					Specific heat of A-15 Nb3Si produced by explosive compression				Solid State Commun., 39(1981)5	G.R.Stewart,Bart Olinger,L.R.Newkirk		
131274	SSC0360983		NbSe3	Nb1Se3	Nb	1	Se	3																					1980																										AB3																				K		2.5					2.5																																				A		20																																																										heat(800C,2w) - cool to RT within 6h.					Superconductivity in niobium triselenide				Solid State Commun., 36(1980)983	C.M.Bastuscheck,R.A.Buhrman,J.D.Kulick,J.C.Scott		
131275	SSC0360493		2H-NbSe2	Nb1Se2	Nb	1	Se	2																					1980																												TX2																		K		7.007					7.007																																									A			4960	1240																																																								Measurements of the penetration depth in the superconducting layer crystals NbSe2 and TaS2(pyridine)#sub(1/2)				Solid State Commun., 36(1980)493	B.S.Deaver.Jr.,J.J.Finley		
131276	SSC0360493	M-intercalated. M = pyridine.	M0.5TaS2	M0.5Ta1S2	M	0.5	Ta	1	S	2																			1980																												TX2																		K		3.96					3.96																																									um			130																																																				intercalation by heating the crystals in liquid pyridine in sealed tube(130C, 12h)					Measurements of the penetration depth in the superconducting layer crystals NbSe2 and TaS2(pyridine)#sub(1/2)				Solid State Commun., 36(1980)493	B.S.Deaver.Jr.,J.J.Finley		
131277	SSC0370613	bulk conversion to A15-phase (50-70%). SP-heat shows Tc=18.0 K.	Nb3Si	Nb3Si1	Nb	3	Si	1																				2	1981																										AB3		Cr3Si(A15)			A	5.091														K		18.6					18.6																																																																																																bulk A15-phase synthesized by exlosive compression					Bulk A15, high Tc Nb3Si synthesized by shock compression				Solid State Commun., 37(1981)613	Bart Olinger,L.R.Newkirk		
131278	SSC0380923	impurity phase with low-Tc contained.	Nb3Si	Nb3Si1	Nb	3	Si	1																				2	1981																										AB3		Cr3Si(A15)																		K		17.5	18				17.5																																																																																																A15-phase synthesized by shock wave compression.					Superconducting properties of Nb-Si compounds produced by shock synthesis				Solid State Commun., 38(1981)923	S.Ohshima,N.Sone,T.Wakiyama,T.Goto,Y.Syono		
131279	SSC0200305		Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				4	1976																										AB3		Cr3Si(A15)																		K		17.2					17.2																																														meV	3.2	4.3	1																																															films deposited on sapphire substrates(T<sub> = 700-800 C) by coevaporation technique.					Superconductive tunneling into niobium-tin thin films				Solid State Commun., 20(1976)305	D.F.Moore,J.M.Rowell,M.R.Beasley		
131280	SSC0190455	RRR=46. T<CDW>=33.5 K. properties estimated from SP-data using G-L theory. lattice term of SP (beta) = 0.586 mJ/mol.K4. thermodynamic Hc(0) = 1260 G.	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	1976																												TX2																	2H-phase	K		7.11				0.15	7.11																													T/K			2.1	0.69			A			110	37	A			1600	4800			3.7	14					mJ/mol.K	280	mJ/mol.K2	18.5														uOhm.cm									3.5																standard iodine vapor transport method at 780 C					Experimental investigation of superconductivity in 2H-NbSe2 single crystal				Solid State Commun., 19(1976)455	P.Garoche,J.J.Veyssie,P.Manuel,P.Molinie		
131281	LES0420019		Nb1-xPdx	Nb0.9Pd0.1	Nb	0.9	Pd	0.1																					1975																																														K		3.34					3.34																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131282	LES0420019		Nb1-xPdx	Nb0.85Pd0.15	Nb	0.85	Pd	0.15																					1975																															A	3.26													bcc	K		2.26					2.26																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131283	LES0420019		Nb1-xPdx	Nb0.83Pd0.17	Nb	0.83	Pd	0.17																					1975																																														K		2.2					2.2																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131284	LES0420019		Nb1-xPdx	Nb0.8Pd0.2	Nb	0.8	Pd	0.2																					1975																																														K		1.98					1.98																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131285	LES0420019		Nb1-xPdx	Nb0.76Pd0.24	Nb	0.76	Pd	0.24																					1975																															A	3.21													bcc	K		1.9					1.9																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131286	LES0420019		Nb1-xPdx	Nb0.72Pd0.28	Nb	0.72	Pd	0.28																					1975																																														K		1.89					1.89																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131287	LES0420019		Nb1-xPdx	Nb0.69Pd0.31	Nb	0.69	Pd	0.31																					1975																																														K		1.84					1.84																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131288	LES0420019		Nb1-xPdx	Nb0.65Pd0.35	Nb	0.65	Pd	0.35																					1975																																														K		1.84					1.84																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131289	LES0420019		(Mo,Nb,Pd)	Mo0.1Nb0.765Pd0.135	Mo	0.1	Nb	0.765	Pd	0.135																			1975																																														K		1.53					1.53																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131290	LES0420019		(Mo,Nb,Pd)	Mo0.1Nb0.72Pd0.18	Mo	0.1	Nb	0.72	Pd	0.18																			1975																																														K		1.45					1.45																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131291	LES0420019		(Mo,Nb,Pd)	Mo0.15Nb0.68Pd0.17	Mo	0.15	Nb	0.68	Pd	0.17																			1975																																														K		1.22					1.22																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131292	LES0420019		(Mo,Nb,Pd)	Mo0.2Nb0.64Pd0.16	Mo	0.2	Nb	0.64	Pd	0.16																			1975																																														K		0.94					0.94																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131293	LES0420019		(Mo,Nb,Pd)	Mo0.2Nb0.608Pd0.192	Mo	0.2	Nb	0.608	Pd	0.192																			1975																																														K		1.34					1.34																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131294	LES0420019		(Mo,W,Pd)	Nb0.72Pd0.18W0.1	Nb	0.72	Pd	0.18	W	0.1																			1975																																														K		1.5					1.5																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131295	LES0420019		(H,Nb,Pd)	H0.64Nb0.85Pd0.15	H	0.64	Nb	0.85	Pd	0.15																			1975																																														K		4.3					4.3																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131296	LES0420019		(H,Nb,Pd)	H0.75Nb0.85Pd0.15	H	0.75	Nb	0.85	Pd	0.15																			1975																																														K		4.66					4.66																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131297	LES0420019		(H,Nb,Pd)	H0.63Nb0.87Pd0.17	H	0.63	Nb	0.87	Pd	0.17																			1975																																														K		3.89					3.89																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131298	LES0420019		(H,Nb,Pd)	H0.12Nb0.8Pd0.2	H	0.12	Nb	0.8	Pd	0.2																			1975																																														K		1.52					1.52																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131299	LES0420019		(H,Nb,Pd)	H0.51Nb0.8Pd0.2	H	0.51	Nb	0.8	Pd	0.2																			1975																																														K		3.4					3.4																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131300	LES0420019		(H,Nb,Pd)	H0.6Nb0.8Pd0.2	H	0.6	Nb	0.8	Pd	0.2																			1975																																														K		3.46					3.46																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131301	LES0420019		(H,Nb,Pd)	H0.69Nb0.8Pd0.2	H	0.69	Nb	0.8	Pd	0.2																			1975																																														K		3.56					3.56																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131302	LES0420019		(H,Nb,Pd)	H0.74Nb0.8Pd0.2	H	0.74	Nb	0.8	Pd	0.2																			1975																																														K		4.07					4.07																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131303	LES0420019		(H,Nb,Pd)	H0.61Nb0.76Pd0.24	H	0.61	Nb	0.76	Pd	0.24																			1975																																														K		3.38					3.38																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131304	LES0420019		(H,Nb,Pd)	H0.34Nb0.72Pd0.28	H	0.34	Nb	0.72	Pd	0.28																			1975																																														K		1.64					1.64																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131305	LES0420019		(H,Nb,Pd)	H0.59Nb0.72Pd0.28	H	0.59	Nb	0.72	Pd	0.28																			1975																																														K		3.12					3.12																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131306	LES0420019		(H,Nb,Pd)	H0.46Nb0.69Pd0.31	H	0.46	Nb	0.69	Pd	0.31																			1975																																														K		3.05					3.05																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131307	LES0420019		(H,Nb,Pd)	H0.54Nb0.65Pd0.35	H	0.54	Nb	0.65	Pd	0.35																			1975																																														K		1.67					1.67																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131308	LES0420019		(H,Mo,Nb,Pd)	H0.51Mo0.1Nb0.765Pd0.135	H	0.51	Mo	0.1	Nb	0.765	Pd	0.135																	1975																																														K		5.46					5.46																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131309	LES0420019		(H,Mo,Nb,Pd)	H0.37Mo0.1Nb0.72Pd0.18	H	0.37	Mo	0.1	Nb	0.72	Pd	0.18																	1975																																														K		4.44					4.44																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131310	LES0420019		(H,Mo,Nb,Pd)	H0.46Mo0.1Nb0.72Pd0.18	H	0.46	Mo	0.1	Nb	0.72	Pd	0.18																	1975																																														K		4.82					4.82																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131311	LES0420019		(H,Mo,Nb,Pd)	H0.28Mo0.15Nb0.68Pd0.17	H	0.28	Mo	0.15	Nb	0.68	Pd	0.17																	1975																																														K		4.92					4.92																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131312	LES0420019		(H,Nb,Pd,W)	H0.47Nb0.72Pd0.18W0.1	H	0.47	Nb	0.72	Pd	0.18	W	0.1																	1975																																														K		3.48					3.48																																																																																																					The effect of hydrogen on the superconducting transition temperature of some body-centered cubic niobium-palladium, niobium-palladium molybdenum and niobium-palladium-tangsten alloys				J.Less-Common Met., 42(1975)19	C.G.Robbins,J.Muller		
131313	SSC0200869		Ta(C,N)	C0.002N0.937Ta1	C	0.002	N	0.937	Ta	1																			1976																															A	4.34														K		8.91		8.58			8.91			K/GPa	0.072																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131314	SSC0200869		Ta(C,N)	C0.198N0.747Ta1	C	0.198	N	0.747	Ta	1																			1976																															A	4.3733														K		10.74		9.99			10.74			K/GPa	0.052																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131315	SSC0200869		Ta(C,N)	C0.148N0.638Ta1	C	0.148	N	0.638	Ta	1																			1976																															A	4.364														K		12.01		9.51			12.01			K/GPa	0.029																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131316	SSC0200869		Ta(C,N)	C0.017N0.632Ta1	C	0.017	N	0.632	Ta	1																			1976																															A	4.3741														K		11.84		9.37			11.84			K/GPa	0.05																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131317	SSC0200869		Ta(C,N)	C0.571N0.271Ta1	C	0.571	N	0.271	Ta	1																			1976																															A	4.4309														K		10.92		10.8			10.92			K/GPa	-0.067																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131318	SSC0200869		TaC	C0.97Ta1	C	0.97	Ta	1																					1976																															A	4.4548														K		11.84		9.46			11.84			K/GPa	-0.15																																																																																												nitriding by heating Ta-wire in pure N2 atmosphere upto 80 bar					Superconducting and normal state properties of tantalum carbonitrides under hydrostatic pressure				Solid State Commun., 20(1976)869	E.Thorwarth,M.Dietrich,C.Politis		
131319	JPC01410767	filamentary SC. Tc defined as onset. T<CDW> defined as maximum of (dR/dT). T<CDW> = 63 K. (dT<CDW>/dP) = 4.41 K/GPa.	ZrTe3	Te3Zr1	Te	3	Zr	1																				3	2002																										AB3																				K		4					4			K/GPa	-5.6																																																																																												chemical transport method					The effect of pressure on the charge-density wave and superconductivity in ZrTe3				J.Phys. Condens.Matter, 14(2002)10767	K.Yamaya,M.Yoneda,S.Yasuzuka,Y.Okajima,S.Tanda		
131320	SSC0220303		SN	S1N1	S	1	N	1																					1977																										AB																				K		0.205					0.205																																		MHC131320																																																																			A.C.susceptibility and magnetisation measurements on polysulphur nitride, (SN)x				Solid State Commun., 22(1977)303	R.H.Dee,A.J.Berlinsky,J.F.Carolan,E.Klein,N.J.Stone,B.G.Turrell,G.B.Street		
131321	SSC0220303		SN	S1N1	S	1	N	1																					1977																										AB																				K		0.235					0.235																																		MHC131320																																																																			A.C.susceptibility and magnetisation measurements on polysulphur nitride, (SN)x				Solid State Commun., 22(1977)303	R.H.Dee,A.J.Berlinsky,J.F.Carolan,E.Klein,N.J.Stone,B.G.Turrell,G.B.Street		
131322	SSC0250119	Tc(max) = 0.52 K at P=0.8 GPa.. R//b-axis	SN	S1N1	S	1	N	1																					1978																										AB																				K		0.26					0.26	MTC131322		K/GPa	0.34																																																																																																	Superconductivity in polymeric sulphur nitride (SN)x at high pressure				Solid State Commun., 25(1978)119	W.H.G.Muller,F.Baumann,G.Dammer,L.Pintschovious		
131323	PRB0296198	foil.  x = 0.97 in VNx.	VN	V1N1	V	1	N	1																					1984																										AB					A	4.127														K		9.25				0.2	9.25																																																																																																V-foil, reaction (740 Torr-N2 for 22h)					Superconducting and normal-state properties of vanadium nitride				Phys.Rev.B, 29(1984)6198	B.R.Zhao,L.Chen,H.L.Luo,M.D.Jack,D.P.Mullin		
131324	PRB0296198	film. x = 0.96 in VNx.	VN	V1N1	V	1	N	1																				4	1984																										AB					A	4.138														K		8.65				0.23	8.65																																																3.95	1																																															sputtering. substrate temperature = 700 C.					Superconducting and normal-state properties of vanadium nitride				Phys.Rev.B, 29(1984)6198	B.R.Zhao,L.Chen,H.L.Luo,M.D.Jack,D.P.Mullin		
131325	PRB0251565	film. sheet resistance = 8.0 Ohm at 300 K.	NbN	Nb1N1	Nb	1	N	1																				4	1982																										AB																				K																																																					meV	3.23	4.4	2																																															sputtering					Far-infrared transmission of superconducting homogeneous NbN films: Scattering time effects				Phys.Rev.B, 25(1982)1565	D.Karecki,R.E.Pena,S.Perkowitz		
131326	PRB0251565	film. sheet resistance = 65 Ohm at 300K.	NbN	Nb1N	Nb	1	N																					4	1982																										AB																				K																																																					meV	2.45	4.1	2																																															sputtering					Far-infrared transmission of superconducting homogeneous NbN films: Scattering time effects				Phys.Rev.B, 25(1982)1565	D.Karecki,R.E.Pena,S.Perkowitz		
131327	PRL0351732	hydrostatic pressure. (dHc2/dT) = 0.09 T/K at P=0.9 GPa.	SN	S1N1	S	1	N	1																					1975																										AB																				K								MTC131327																												T/K		0.17																																																																						Pressure dependence of superconductivity and normal conductivity in polymeric sulphur nitride, (SN)x				Phys.Rev.Lett., 35(1975)1732	W.D.Gill,R.L.Greene,G.B.Street,W.A.Little		
131328	SSC0630141	ANN(1770K, 0.25h, under 6GPa)	delta-MoN	Mo1N1	Mo	1	N	1																					1987																										AB					A	5.745		5.622												K		15.1				1.9	15.1																																																																																																MoCl5 - react (920K, in NH3 flow)					HIGH-PRESSURE HIGH-TEMPERATURE EXPERIMENTS ON Z-MON				SOLID STATE COMMUN.,63(1987)141	A.BEZINGE,J.MULLER,K.YVON,P.ETTMAYER,W.LENGAUER	MO,N	
131329	SSC0630141	as-grown	delta-MoN	Mo1N1	Mo	1	N	1																					1987																										AB					A	2.85		2.784												K		3.2				1.9	3.2																																																																																																MoCl5 - react (920K, in NH3 flow)					HIGH-PRESSURE HIGH-TEMPERATURE EXPERIMENTS ON Z-MON				SOLID STATE COMMUN.,63(1987)141	A.BEZINGE,J.MULLER,K.YVON,P.ETTMAYER,W.LENGAUER	MO,N	
131330	SSC0610101	inductive penetration depth	U6Fe	Fe1U6	Fe	1	U	6																					1987																										AB6		U6Mn																		K		3.86					3.86																																									um	induction	0.8																																																					arc-melting - ANN(700C,1w, in vac)					Penetration depths of superconducting U6X (X=Fe,Co,Mn)				Solid State Commun., 61(1987)101	M.K.Hou,C.Y.Huang,C.E.Olsen		
131331	SSC0610101	inductive penetration depth	U6Co	Co1U6	Co	1	U	6																					1987																										AB6		U6Mn																		K		2.43					2.43																																									um	induction	1.3																																																					arc-melting - ANN(700C,1w, in vac)					Penetration depths of superconducting U6X (X=Fe,Co,Mn)				Solid State Commun., 61(1987)101	M.K.Hou,C.Y.Huang,C.E.Olsen		
131332	SSC0610101	chemical analysis: U6Mn0.95Fe0.05.   inductive penetration depth	U6Mn	Mn1U6	Mn	1	U	6																					1987																										AB6		U6Mn																		K		2.88					2.88																																									um	induction	1.6																																																					arc-melting - ANN(700C,1w, in vac)					Penetration depths of superconducting U6X (X=Fe,Co,Mn)				Solid State Commun., 61(1987)101	M.K.Hou,C.Y.Huang,C.E.Olsen		
131333	SSC0470519	R not to zero down to 1.5 K.	Lu3Si5	Lu3Si5	Lu	3	Si	5																					1983																										A3B5																				K			7				7																																																																																																					Transport and magnetic properties of layered rare earth disilisides				Solid State Commun., 47(1983)519	L.D.Woolf		
131334	CEM0770401	Tc defined as 0.9Rn.	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4			1988																										AB2C4		spinel																	MgAl2O4-type	K	11.8		12				11.9																				T	resistivity, WHH	12.9							T/K	resistivity	1.53			HC131334																																																														Firstly Li1.333Ti1.667O4 synthesized by solid state reaction. Then mixed with TiO2, Ti powder, heat(760C,1w, in evacuated silica tube					Superconducting properties in the Li1+xTi2-xO4 system with the spinel structure				J.Solid State Chem., 77(1988)401	Y.Ueda,T.Tanaka,K.Kosuge,M.Ishikawa,H.Yasuoka		
131335	CEM0770401	Tc defined as 0.9Rn.	LiTi2O4	Li1.035Ti1.965O4	Li	1.035	Ti	1.965																	O	4			1988																										AB2C4		spinel																	MgAl2O4-type	K	11.5		12				11.75																				T	resistivity, WHH	21.4							T/K	resistivity	2.62			HC131335																																																														Firstly Li1.333Ti1.667O4 synthesized by solid state reaction. Then mixed with TiO2, Ti powder, heat(760C,1w, in evacuated silica tube					Superconducting properties in the Li1+xTi2-xO4 system with the spinel structure				J.Solid State Chem., 77(1988)401	Y.Ueda,T.Tanaka,K.Kosuge,M.Ishikawa,H.Yasuoka		
131336	CEM0770401	Tc defined as 0.9Rn.	LiTi2O4	Li1.07Ti1.93O4	Li	1.07	Ti	1.93																	O	4			1988																										AB2C4		spinel																	MgAl2O4-type	K	11.4		12				11.7																				T	resistivity, WHH	24.8							T/K	resistivity	3.03			HC131336																																																														Firstly Li1.333Ti1.667O4 synthesized by solid state reaction. Then mixed with TiO2, Ti powder, heat(760C,1w, in evacuated silica tube					Superconducting properties in the Li1+xTi2-xO4 system with the spinel structure				J.Solid State Chem., 77(1988)401	Y.Ueda,T.Tanaka,K.Kosuge,M.Ishikawa,H.Yasuoka		
131337	CEM0770401	Tc defined as 0.9Rn.	LiTi2O4	Li1.1Ti1.9O4	Li	1.1	Ti	1.9																	O	4			1988																										AB2C4		spinel																	MgAl2O4-type	K	8.5		12				10.25																				T	resistivity, WHH	36.9							T/K	resistivity	4.47			HC131337																																																														Firstly Li1.333Ti1.667O4 synthesized by solid state reaction. Then mixed with TiO2, Ti powder, heat(760C,1w, in evacuated silica tube					Superconducting properties in the Li1+xTi2-xO4 system with the spinel structure				J.Solid State Chem., 77(1988)401	Y.Ueda,T.Tanaka,K.Kosuge,M.Ishikawa,H.Yasuoka		
131338	JPS0280263	as-grown	LaSi2	La1Si2	La	1	Si	2																					1970																										AB2		ThSi2			A	4.312		13.841											alpha-ThSi2	K		2.3					2.3																																																																																																arc-melting					Superconductivity of LaSi2				J.Phys.Soc.Jpn, 28(1970)263	T.Satoh,Y.Asada		
131339	JPS0280263	ANN(1450C,50h, in vac)	LaSi2	La1Si2	La	1	Si	2																					1970																										AB2		ThSi2			A	4.29	4.2	14.06											alpha-ThSi2, ortho-	K					1.2																																																																																																		arc-melting					Superconductivity of LaSi2				J.Phys.Soc.Jpn, 28(1970)263	T.Satoh,Y.Asada		
131340	JPS0280263	as-grown	LaSi1.75	La1Si1.75	La	1	Si	1.75																					1970																										AB2		ThSi2			A	4.28	4.19	14.02											alpha-ThSi2, ortho-, distorted	K					1.2																																																																																																		arc-melting					Superconductivity of LaSi2				J.Phys.Soc.Jpn, 28(1970)263	T.Satoh,Y.Asada		
131341	PL0200565	SUS(300K) = -15.0 E-5 emu/mol	YSi1.9	Si1.9Y1	Si	1.9	Y	1																					1966																										AB2		ThSi2																		K					0.1																																																										mJ/mol.K2	1.9																																							arc-melting					Anomalous specific heat of superconducting lanthanum and yttrium compounds				Phys.Lett., 20(1966)565	T.Satoh,T.Ohtsuka		
131342	PL0200565	(dC/gamma*Tc) = 0.90. SUS(300K) = 4.5 E-5 emu/mol	LaSi2	La1Si2	La	1	Si	2																					1966																										AB2		ThSi2																		K		2.3					2.3																																																								mJ/mol.K2	5.8																																							arc-melting					Anomalous specific heat of superconducting lanthanum and yttrium compounds				Phys.Lett., 20(1966)565	T.Satoh,T.Ohtsuka		
131343	PL0200565	(dC/gamma*Tc) = 0.76. SUS(300K) = -6.8 E-5 emu/mol	LaGe2	Ge2La1	Ge	2	La	1																					1966																										AB2		ThSi2																		K		2.2					2.2																																																								mJ/mol.K2	6.1																																							arc-melting					Anomalous specific heat of superconducting lanthanum and yttrium compounds				Phys.Lett., 20(1966)565	T.Satoh,T.Ohtsuka		
131344	CEM0980291		La2Sn5	La2Sn5	La	2	Sn	5																					1992																										A2B5		Ce2Sn5	Cmmm		A	4.6233	35.7425	4.6817												K		5.4					5.4																																																																																																					Crystal chemistry and magnetism of neodymium stannides including compounds of the structural series REnSn3n-2				J.Solid State Chem., 98(1992)291	F.Weitzer,K.Hiebl,P.Rogl		
131345	CEM0980291		LaSn2	La1Sn2	La	1	Sn	2																					1992																										AB2		NdSn2	Cmmm		A	4.4267	15.8552	4.5136												K		3.6					3.6																																																																																																					Crystal chemistry and magnetism of neodymium stannides including compounds of the structural series REnSn3n-2				J.Solid State Chem., 98(1992)291	F.Weitzer,K.Hiebl,P.Rogl		
131346	CEM0980291		La3Sn7	La3Sn7	La	3	Sn	7																					1992																										A3B7		Ce3Sn5	Cmmm		A	4.5643	26.1558	4.671												K					2																																																																																																							Crystal chemistry and magnetism of neodymium stannides including compounds of the structural series REnSn3n-2				J.Solid State Chem., 98(1992)291	F.Weitzer,K.Hiebl,P.Rogl		
131347	SSC0180725	mother metal: dhcp-La	(La,Lu)	La0.92Lu0.08	La	0.92	Lu	0.08																					1976																																													dhcp-La	K		3.72					3.72																																																																																																arc-melting - cold roll(25% reduction) - heat(725K,2h) - cool to 375 K - ANN(540K,1w)					Superconductivity in singlet La-Pr and in nonmagnetic La-rare earth alloys				Solid State Commun., 18(1976)725	S.Legvold,R.W.Green,B.J.Beaudry,J.E.Ostenson		
131348	SSC0180725	mother metal: dhcp-La	(La,Y)	La0.8Y0.2	La	0.8	Y	0.2																					1976																																													dhcp-La	K		2.7					2.7																																																																																																arc-melting - cold roll(25% reduction) - heat(725K,2h) - cool to 375 K - ANN(540K,1w)					Superconductivity in singlet La-Pr and in nonmagnetic La-rare earth alloys				Solid State Commun., 18(1976)725	S.Legvold,R.W.Green,B.J.Beaudry,J.E.Ostenson		
131349	SSC0180725	mother metal: dhcp-La	(La,Pr)	La0.84Pr0.16	La	0.84	Pr	0.16																					1976																																													dhcp-La	K		2.2					2.2																																																																																																arc-melting - cold roll(25% reduction) - heat(725K,2h) - cool to 375 K - ANN(540K,1w)					Superconductivity in singlet La-Pr and in nonmagnetic La-rare earth alloys				Solid State Commun., 18(1976)725	S.Legvold,R.W.Green,B.J.Beaudry,J.E.Ostenson		
131350	SSC0180725	mother metal: dhcp-La	(La,Yb)	La0.93Yb0.07	La	0.93	Yb	0.07																					1976																																													dhcp-La	K		3.56					3.56																																																																																																arc-melting - cold roll(25% reduction) - heat(725K,2h) - cool to 375 K - ANN(540K,1w)					Superconductivity in singlet La-Pr and in nonmagnetic La-rare earth alloys				Solid State Commun., 18(1976)725	S.Legvold,R.W.Green,B.J.Beaudry,J.E.Ostenson		
131351	SSC0180725	mother metal: dhcp-La	(La,Nd)	La0.98Nd0.02	La	0.98	Nd	0.02																					1976																																													dhcp-La	K		3.6					3.6																																																																																																arc-melting - cold roll(25% reduction) - heat(725K,2h) - cool to 375 K - ANN(540K,1w)					Superconductivity in singlet La-Pr and in nonmagnetic La-rare earth alloys				Solid State Commun., 18(1976)725	S.Legvold,R.W.Green,B.J.Beaudry,J.E.Ostenson		
131352	JPS0370673	Tc defined as mid of SP-jump	La3Al	Al1La3	Al	1	La	3																					1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		6					6																				T	SP-heat, extrapolation	2.7												MHC131352																																																												La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131353	JPS0370673	Tc defined as mid of SP-jump	(La,Ce)3Al	Al1Ce0.01La3	Al	1	Ce	0.01	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		3.92					3.92																																		MHC131353																																																												La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131354	JPS0370673	Tc defined as mid of SP-jump	(La,Ce)3Al	Al1Ce0.0165La3	Al	1	Ce	0.0165	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		1.45					1.45	MTC131354																																																																																													La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131355	JPS0370673	Tc defined as mid of SP-jump	(La,Ce)3Al	Al1Ce0.017La3	Al	1	Ce	0.017	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		0.77					0.77																																																																																														La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131356	JPS0370673	Tc defined as mid of SP-jump	(La,Gd)3Al	Al1Gd0.001La3	Al	1	Gd	0.001	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		5.6					5.6																																																																																														La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131357	JPS0370673	Tc defined as mid of SP-jump	(La,Gd)3Al	Al1Gd0.003La3	Al	1	Gd	0.003	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		4.58					4.58	MTC131357																																																																																													La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131358	JPS0370673	Tc defined as mid of SP-jump	(La,Gd)3Al	Al1Gd0.0065La3	Al	1	Gd	0.0065	La	3																			1974																										AB3	7	Mg3Cd																	DO<19>, Mg3Cd, hexagonal	K		2.79					2.79																																																																																														La(4N),Ce(3N),Al(5N)		melt by EB in vac.  - wrapped in Ta-foil - sealed in evacuated quartz tube - ANN(500C,18h)					Magnetic impurity effects in Kondo superconductor, La3Al(Ce)				J.Phys.Soc.Jpn, 37(1974)673	Toshio Aoi,Yoshika Masuda		
131359	SSC0160409	Tc by ac inductance	LaSn3	La1Sn3	La	1	Sn	3																					1975																										AB3		Cu3Au			A	4.773														K		5.98					5.98	MTC131359																																																																																																				Anomalous Tc-behavior of LaSn3 under pressure				Solid State Commun., 16(1975)409	S.Huang,C.W.Chu,F.Y.Fradin,L.B.Welsh		
131360	SSC0170241	RRR=31. Longtudinal ultrasonic attenuation measured.	LaSn3	La1Sn3	La	1	Sn	3																					1975																										AB3		Cu3Au																		K		6.628					6.628																																																																																																					Ultrasonic attenuation in pure and Gd-doped superconductors: LaSn3 and LaAl2				Solid State Commun., 17(1975)241	G.Herrmann,H.E.Bommel		
131361	SSC0170241	RRR=50. Longtudinal ultrasonic attenuation measured.	LaAl2	Al2La1	Al	2	La	1																					1975																										AB2		MgCu2(Laves)																	MgCu2, C15	K		3.273					3.273																																																																																																					Ultrasonic attenuation in pure and Gd-doped superconductors: LaSn3 and LaAl2				Solid State Commun., 17(1975)241	G.Herrmann,H.E.Bommel		
131362	SSC0260469		LaSn3	La1Sn3	La	1	Sn	3																					1978																										AB3		Cu3Au																		K		6.43					6.43																																																								mJ/mol.K2	11.66	SP-heat	220	SP-heat																																									Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131363	SSC0260469		(La,Ce)Sn3	La0.9837Ce0.0163Sn3	La	0.9837	Ce	0.0163	Sn	3																			1978																										AB3		Cu3Au																		K		4.33					4.33	MTC131365																																																																																																				Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131364	SSC0260469		(La,Ce)Sn3	La0.9647Ce0.0333Sn3	La	0.9647	Ce	0.0333	Sn	3																			1978																										AB3		Cu3Au																		K		3.03					3.03	MTC131364																																																																																																				Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131365	SSC0260469		(La,Ce)Sn3	La0.9462Ce0.0538Sn3	La	0.9462	Ce	0.0538	Sn	3																			1978																										AB3		Cu3Au																		K		1.86					1.86	MTC131365																																																																																																				Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131366	SSC0260469		(La,Ce)Sn3	La0.9709Ce0.0291Sn3	La	0.9709	Ce	0.0291	Sn	3																			1978																										AB3		Cu3Au																		K		3.47					3.47	MTC131365																																																							mJ/mol.K2	11.49	SP-heat	232	SP-heat																																									Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131367	SSC0260469		(La,Ce)Sn3	La0.9481Ce0.0519Sn3	La	0.9481	Ce	0.0519	Sn	3																			1978																										AB3		Cu3Au																		K		1.92					1.92	MTC131365																																																							mJ/mol.K2	16.1	SP-heat	220	SP-heat																																									Superconducting and normal state properties of dilute alloys of LaSn3 containing Ce impurities				Solid State Commun., 26(1978)469	L.E.DeLong,M.B.Maple,M.Tovar		
131368	SSC0740621	Jc = 20 A/cm2	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		1	1990																										AB2C4		spinel																	MgAl2O4-type	K		12.7					12.7																																																																																																					MAGNETIC SUPERCONDUCTING PROPERTIES OF LITI2O4 SINGLE CRYSTAL			IPCMS-GEMME (UMR 46 CNRS), UNIVERSITE LOUIS KPASTEUR, 4 RUE BLAISE PASCAL, 67070 STRASBOURG, FRANCE	SOLID STATE COMMUN,74(1990)621	A.DERORY,J.J.JCAPPONI,J.P.KAPPLER,M.DRILLON,O.DURMEYER	LI,TI,O	
131369	SSC0740621	Jc = 4E+3 A/cm2	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		3	1990																										AB2C4		spinel			A	8.409													MgAl2O4-type	K		10.7					10.7											Oe	magnetization	230			150			4.2															HC131369		A		19			A		2000																																																					electrolysing at 780C. molten bath (NaBO2,LiBO2,NaF,TiO2)					MAGNETIC SUPERCONDUCTING PROPERTIES OF LITI2O4 SINGLE CRYSTAL			IPCMS-GEMME (UMR 46 CNRS), UNIVERSITE LOUIS KPASTEUR, 4 RUE BLAISE PASCAL, 67070 STRASBOURG, FRANCE	SOLID STATE COMMUN,74(1990)621	A.DERORY,J.J.JCAPPONI,J.P.KAPPLER,M.DRILLON,O.DURMEYER	LI,TI,O	
131370	JPS0440402		(La,Y)	La0.85Y0.15	La	0.85	Y	0.15																					1978																																														K		3.06					3.06																																																						mJ/mol.K	35.04	mJ/mol.K2	6.9	SP-heat																																											Magnetic impurities in superconductors; La(Ce)Sn3-xPbx and La1-yYy(Ce) systems				J.Phys.Soc.Jpn, 44(1978)402	Jun Takeuchi,Yoshika Masuda		
131371	JCG1420087	Jc(6K, 0T) = 1.0 E+6 A/cm2	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4			1994																										AB2C4		spinel	Fd3[-]m		A	8.372													MgAl2O4-type	K			11.5			1.5	11.5										70	Oe	magnetization				250			6																																																																													electrolysis method. bath(TiO2,LiBO2)					Crystal growth of superconducting LiTi2O4				J.Cryst.Growth, 142(1994)87	J.A.Campa,M.Velez,C.Cascales,E.Gutierrez Puebla,M.A.Monge,I.Rasines,C.Ruiz-Valero		
131372	PRL0572987	tunneling with barrier film(40A).	(Mo,Re)	Mo0.6Re0.4	Mo	0.6	Re	0.4																					1986																																														K		12.3					12.3																																																3.86	1																																																				Enhanced superconductivity by electron renormalization of a directly observed Brout-Visscher local phonon: Re in Mo1-xRex				Phys.Rev.Lett., 57(1986)2987	D.P.Shum,A.Bevolo,J.L.Staudenmann,E.L.Wolf		
131373	PRL0761525	d=4000A. RRR = nearly one.	NbN	N1Nb1	N	1	Nb	1																				5	1996																																														K		16.5					16.5																																														meV	6	4	2																																															films prepared by dc reactive magnetron sputtering on MgO substrate (Tsub = 840C)					Grazing incidence infrared reflectivity of La1.85Sr0.15CuO4 and NbN				Phys.Rev.Lett., 76(1996)1525	H.S.Somal,B.J.Feenstra,J.Schutzmann,Jae Hoon Kim,Z.H.Barber,V.H.M.Duijn,N.T.Hien,A.A.Menovsky,Mario Palumbo,D.van der Marel		
131374	LES0620329		Mo6S8	Mo6S8	Mo	6	S	8																					1978																										A3B4																				K							2																																																								mJ/mol.K2	27.3	SP-heat	126.5	SP-heat																																									Heat capacity and magnetic properties of Mo6S8 and Mo6Se8 at low temperatures				J.Les-Comm. Metals, 62(1978)329	N.E.Alekseevskii,N.M.Dobrovolskii,G.Wolf,C.Hohlfeld,K.Bohmhammel		
131375	LES0620329		Mo6Se8	Mo6Se8	Mo	6	Se	8																					1978																										A3B4																				K		6.4					6.4																																																								mJ/mol.K2	73	SP-heat	84	SP-heat																																									Heat capacity and magnetic properties of Mo6S8 and Mo6Se8 at low temperatures				J.Les-Comm. Metals, 62(1978)329	N.E.Alekseevskii,N.M.Dobrovolskii,G.Wolf,C.Hohlfeld,K.Bohmhammel		
131376	SSC0211007	irradiation effect of Tc measured. irradiation at 140 C.	Mo3Os	Mo3Os1	Mo	3	Os	1																				1	1977																										AB3		Cr3Si(A15)			A	4.968													Cr3Si, A15	K		12.7					12.7	MTC131376																																																																																															arc-melting. ANN(1850 C,15h+1450C,25h+1000C,10d+950C,9d+800C,20d)					Superconductivity of neutron irradiated Mo3Os				Solid State Commun., 21(1977)1007	A.R.Sweedler,S.Moehlecke,R.H.Jones,R.Viswanathan,D.C.Johnston		
131377	PRL0280681	data from other papers.	(Nb,Mo)	Mo0.15Nb0.85	Mo	0.15	Nb	0.85																					1972																																														K		5.85					5.85																																																								mJ/mol.K2	6.3		265																																										Acoustic plasmons, phonon anomalies, and superconductivity in transition-metal systems				Phys.Rev.Lett., 28(1972)681	B.N.Ganguly,R.F.Wood		
131378	PRL0280681	data from other papers.	(Nb,Mo)	Mo0.4Nb0.6	Mo	0.4	Nb	0.6																					1972																																														K		0.6					0.6																																																								mJ/mol.K2	2.87		371																																										Acoustic plasmons, phonon anomalies, and superconductivity in transition-metal systems				Phys.Rev.Lett., 28(1972)681	B.N.Ganguly,R.F.Wood		
131379	PRL0280681	data from other papers.	(Nb,Mo)	Mo0.8Nb0.2	Mo	0.8	Nb	0.2																					1972																																														K		0.095					0.095																																																								mJ/mol.K2	1.49		461																																										Acoustic plasmons, phonon anomalies, and superconductivity in transition-metal systems				Phys.Rev.Lett., 28(1972)681	B.N.Ganguly,R.F.Wood		
131380	SSC0900321	Tc(P=0.1 MPa) = 2.1 K. Under ambient p, Tc not given.	La7Ni3	La7Ni3	La	7	Ni	3																				1	1994																										A3B7	7	Th7Fe3																	hexagonal	K		2.1					2.1																																																																																																arc-melting					Electrical resistivity of Ce7Ni3 under high pressure				Solid State Commun., 90(1994)321	K.Umeo,K.Ishii,H.Kadomatsu		
131381	SSC0900321	R(min) at 3.5 K. R(peak) = 1.7 K due to magneic order	Ce7Ni3	Ce7Ni3	Ce	7	Ni	3																				3	1994																										A3B7		Th7Fe3																		K					1.5																																																																																																		arc-melting					Electrical resistivity of Ce7Ni3 under high pressure				Solid State Commun., 90(1994)321	K.Umeo,K.Ishii,H.Kadomatsu		
131382	LES0320173	Tc determined by measuring M(T) at H = 30 Oe.	LaOs2	La1Os2	La	1	Os	2																					1973																										AB2		MgCu2(Laves)																	MgCu2, C15	K		8.9					8.9																																																																																																					Superconductivity of LaOs2				J.Les-Comm. Metals, 32(1973)173	A.C.Lawson,J.F.Cannon,D.L.Robertson,H.T.Hall		
131383	LES0320173	Tc determined by measuring M(T) at H = 30 Oe. MgZn2-phase induced by high-T and P	LaOs2	La1Os2	La	1	Os	2																					1973																										AB2		MgZn2(Laves)																	MgZn2, C14	K		5.9					5.9																																																																																																					Superconductivity of LaOs2				J.Les-Comm. Metals, 32(1973)173	A.C.Lawson,J.F.Cannon,D.L.Robertson,H.T.Hall		
131384	SSC0160923	Tc by spin resonance of 4000 ppmGd-LaOs2	LaOs2	La1Os2	La	1	Os	2																					1975																										AB2		MgCu2(Laves)																	MgCu2, C15	K		9					9																																																								mJ/mol.K2	15																																												Spin resonance of Gd in LaOs2				Solid State Commun., 16(1975)923	W.Schrittenlacher,K.Baberschke,G.Koopmann,S.Hufner		
131385	SSC0391293	(dTc/dP) calculated from thermal expansion. At T=5K, a=8.754, c=8.613. linear thermal expansion coeff. = 8 E-8 /K at 8 K.. (dHc2/dP) = 418 T/GPa at P=0.	La3S4	La3S4	La	3	S	4																				3	1981																										A3B4					A	8.724														K		8.05					8.05			K/GPa	1.35																																																																																												Bridgman method					Thermal expansion of La3S4 at low temperatures				Solid State Commun., 39(1981)1293	R.Pott,G.Guntherodt,H.Bach		
131386	MRB0101111	structural transformation T0: (dT0/dP) = 1.6 K/kbar.   hydrostatic and non-hydrostatic Tc(P) were measured.	La3S4	La3S4	La	3	S	4																				1	1975																										A3B4		Th3P4																		K		8.12					8.12	MTC131386																																																																																															mixture - sealed in quartz tube - heat(800C,24h) - press to pellet - sealed in Ta in Ar-gas - heat(1700C, inductive)					The effect of pressure on the superconducting and crystallographic transitions of La3S4, La3Se4 and La3Te4				Mat.Res.Bull., 10(1975)1111	R.N.Shelton,A.R.Moodenbaugh,P.D.Dernier,B.T.Matthias		
131387	MRB0101111	hydrostatic and non-hydrostatic Tc(P) were measured.	La3Se4	La3Se4	La	3	Se	4																				1	1975																										A3B4		Th3P4																		K		7.63					7.63	MTC131387																																																																																															mixture - sealed in quartz tube - heat(800C,24h) - press to pellet - sealed in Ta in Ar-gas - heat(1700C, inductive)					The effect of pressure on the superconducting and crystallographic transitions of La3S4, La3Se4 and La3Te4				Mat.Res.Bull., 10(1975)1111	R.N.Shelton,A.R.Moodenbaugh,P.D.Dernier,B.T.Matthias		
131388	MRB0101111	hydrostatic and non-hydrostatic Tc(P) were measured.	La3Te4	La3Te4	La	3	Te	4																				1	1975																										A3B4		Th3P4																		K		4.61					4.61	MTC131388		K/GPa	-0.635																																																																																												mixture - sealed in quartz tube - heat(800C,24h) - press to pellet - sealed in Ta in Ar-gas - heat(1700C, inductive)					The effect of pressure on the superconducting and crystallographic transitions of La3S4, La3Se4 and La3Te4				Mat.Res.Bull., 10(1975)1111	R.N.Shelton,A.R.Moodenbaugh,P.D.Dernier,B.T.Matthias		
131389	LES0550103	microanalysis: LaSb1.95-2.03	LaSb2	La1Sb2	La	1	Sb	2																					1977																										AB2	3	SmSb2																	ortho-	K		0.4					0.4																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131390	LES0550103		LaN	La1N1	La	1	N	1																					1977																										AB	1	NaCl																	cubic	K		1					1																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131391	LES0550103		LaP	La1P1	La	1	P	1																					1977																										AB	1	NaCl																	cubic	K					0.015																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131392	LES0550103		LaAs	As1La1	As	1	La	1																					1977																										AB	1	NaCl																	cubic	K					0.08																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131393	LES0550103		LaSb	La1Sb1	La	1	Sb	1																					1977																										AB	1	NaCl																	cubic	K					0.03																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131394	LES0550103		LaBi	Bi1La1	Bi	1	La	1																					1977																										AB	1	NaCl																	cubic	K					0.08																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131395	LES0550103		La4As3	As3La4	As	3	La	4																					1977																										A3B4	1	Th3P4			A	9.203													cubic, anti-Th3P4	K		6.5					6.5																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131396	LES0550103		La4Sb3	La4Sb3	La	4	Sb	3																					1977																										A3B4	1	Th3P4			A	9.6485													cubic, anti-Th3P4	K		0.25					0.25																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131397	LES0550103		La4(Sb,Bi)3	Bi1.5La4Sb1.5	Bi	1.5	La	4	Sb	1.5																			1977																										A3B4	1	Th3P4			A	9.804													cubic, anti-Th3P4	K		0.158					0.158																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131398	LES0550103		La4Bi3	Bi3La4	Bi	3	La	4																					1977																										A3B4	1	Th3P4			A	9.79													cubic, anti-Th3P4	K		0.155					0.155																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131399	LES0550103		La3YSb3	La3Sb3Y1	La	3	Sb	3	Y	1																			1977																										A3B4	1	Th3P4			A	9.553													cubic, anti-Th3P4	K		0.13					0.13																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131400	LES0550103		La4Sb2Sn	La4Sb2Sn1	La	4	Sb	2	Sn	1																			1977																										A3B4	1	Th3P4			A	9.686													cubic, anti-Th3P4	K					0.08																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131401	LES0550103		La4Sb2Pb	La4Pb1Sb2	La	4	Pb	1	Sb	2																			1977																										A3B4	1	Th3P4			A	9.707													cubic, anti-Th3P4	K					0.08																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131402	LES0550103		La4Bi2Sn	Bi2La4Sn1	Bi	2	La	4	Sn	1																			1977																										A3B4	1	Th3P4			A	9.779													cubic, anti-Th3P4	K					0.08																																																																																																		mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131403	LES0550103		La4Bi2Pb	Bi2La4Pb1	Bi	2	La	4	Pb	1																			1977																										A3B4	1	Th3P4			A	9.798													cubic, anti-Th3P4	K		2.3					2.3																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131404	LES0550103		La4(Bi,Pb)3	Bi1.5La4Pb1.5	Bi	1.5	La	4	Pb	1.5																			1977																										A3B4	1	Th3P4			A	9.805													cubic, anti-Th3P4	K		2.4					2.4																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131405	LES0550103		La4BiPb2	Bi1La4Pb2	Bi	1	La	4	Pb	2																			1977																										A3B4	1	Th3P4			A	9.809													cubic, anti-Th3P4	K		2.5					2.5																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131406	LES0550103		La5Bi3	Bi3La5	Bi	3	La	5																					1977																										A3B5	3	Mo5Si3																	hexagonal	K		0.64					0.64																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131407	LES0550103		La2Sb	La2Sb1	La	2	Sb	1																					1977																										AB2	2	Ti2Bi																	tetragonal	K		0.75					0.75																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131408	LES0550103		La2Bi	Bi1La2	Bi	1	La	2																					1977																										AB2	2	Ti2Bi																	tetragonal	K		0.76					0.76																																																																																																mixture - react in sealed Ta-tube - molten ingot - ANN(50-100C, 8h)					Superconductivity of lanthanum pnictides				J.Les-Comm. Metals, 55(1977)103	F.Hulliger,H.R.Ott		
131409	JAC2050049		La3Ru	La3Ru1	La	3	Ru	1																					1994	emu/mol-La	0.00013																								AB3	3	Fe3C																	ortho-	K		5.55					5.55											Oe	M-H curve				300			4.2	T	M-H curve				0.35			4.2																																											mOhm.cm							0.075																							Superconductivity in the La-Ru system				J.Alloys Compd., 205(1994)49	A.Palenzona,R.Eggenhoffner,F.Canepa		
131410	JAC2050049		La5Ru2	La5Ru2	La	5	Ru	2																					1994	emu/mol-La	0.00018																								A2B5	4	Mn5C2																	monoclinic	K		2.35					2.35											Oe	M-H curve				200			1.5	T	M-H curve				0.9			1.5																																											mOhm.cm							0.24																							Superconductivity in the La-Ru system				J.Alloys Compd., 205(1994)49	A.Palenzona,R.Eggenhoffner,F.Canepa		
131411	JAC2050049		La7Ru3	La7Ru3	La	7	Ru	3																					1994	emu/mol-La	0.00012																								A3B7	3	Sr7Pt3																	ortho	K		1.75					1.75											Oe	M-H curve				200			1.5	T	M-H curve				0.22			1.5																																											mOhm.cm							0.22																							Superconductivity in the La-Ru system				J.Alloys Compd., 205(1994)49	A.Palenzona,R.Eggenhoffner,F.Canepa		
131412	JAC1980165	RRR = 15.0. thermopowor S(T) measured.	La3Ga	Ga1La3	Ga	1	La	3																					1993																										AB3	1				A	5.61														K		5.8					5.8																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131413	JAC1980165	RRR = 17.0. thermopowor S(T) measured.	La3In	In1La3	In	1	La	3																					1993																										AB3	1				A	5.07														K		9.7					9.7																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131414	JAC1980165	RRR = 5.6. thermopowor S(T) measured.	La3Sn	La3Sn1	La	3	Sn	1																					1993																										AB3	1				A	5.102														K		6.2					6.2																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131415	JAC1980165	RRR = 4.2. thermopowor S(T) measured.	La3Al	Al1La3	Al	1	La	3																					1993																										AB3	7				A	7.192		5.528												K		5.8					5.8																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131416	JAC1980165	RRR = 13.5. thermopowor S(T) measured.	La3Ge	Ge1La3	Ge	1	La	3																					1993																										AB3	3				A	7.416	9.954	6.497												K		3.7					3.7																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131417	JAC1980165	RRR = 2.14. thermopowor S(T) measured.	La3Ni	La3Ni1	La	3	Ni	1																					1993																										AB3	3				A	7.189	10.16	6.65												K		6.2					6.2																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131418	JAC1980165	RRR = 1.9. thermopowor S(T) measured.	La3Ir	Ir1La3	Ir	1	La	3																					1993																										AB3	3				A	7.458	10.096	6.662												K					1.7																																																																																																		arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131419	JAC1980165	RRR = 3.7. thermopowor S(T) measured.	La3Ru	La3Ru1	La	3	Ru	1																					1993																										AB3	3				A	7.465	10.016	6.57												K		4.2					4.2																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131420	JAC1980165	RRR = 10.0. thermopowor S(T) measured.	La3Co	Co1La3	Co	1	La	3																					1993																										AB3	3				A	7.282	10.02	6.594												K		4					4																																																																																																arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131421	JAC1980165		(La,Gd)3In	Gd0.02In1La2.98	Gd	0.02	In	1	La	2.98																			1993																										AB3																				K		7.9					7.9																																																																						MTP131421																										arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131422	JAC1980165		(La,Gd)3In	Gd0.06In1La2.94	Gd	0.06	In	1	La	2.94																			1993																										AB3																				K		4.1					4.1																																																																						MTP131422																										arc-melting					Resistivity and thermopower studies on La3X (X = Al, Sn, In, Ru, Ir, Co, Ni, Ge, Ga) system				J.Alloys Compd., 198(1993)165	C.S.Garde,J.Ray,G.Chandra		
131423	JPS0632061	Two SC transition (2.2K and 1.5 K). See SP-fig. (dHc2/dT) = 0.29 T/K for lower-Tc phase. T^3 and T^5 term coeff. of SP are 1.70 mj/mol.K4 and 0.016 mJ/mol.K6.	La3Ni	La3Ni1	La	3	Ni	1																					1994																										AB3	3	Fe3C			A	7.22	10.24	6.6												K		2.2					2.2																													T/K	SP	0.74			MHC131423																			MSP131423			mJ/mol.K2	20.6	SP-heat	170	SP-heat																																				arc-melting					Is La3Ni a new unconventional superconductor?				J.Phys.Soc.Jpn, 63(1994)2061	Noriaki Sato,Kimihiro Imamura,Takuo Sakon,Takemi Komatsubara,Izuru Umehara,Kiyoo Sato		
131424	JAP0736621	RRR = 7.1. (dC/gamma*Tc) = 1.75. Hc2(2.17K) = 1.51 T,  Hc2(3.6K) = 0.66 T	La3Co	Co1La3	Co	1	La	3																					1993																										AB3	3	Fe3C	Pmma																	K		4.4					4.4											Oe		1000							T	resistivity, extrapolation	2.1			1.78			1.67	T/K	resistivity, extrapolation	0.95															meV	1.3		14				MSP131424			mJ/mol.K2	26	SP-heat	127	SP-heat											mOhm.cm							0.031																		arc-melting					Superconductivity in intermetallic compound La3Co				J.Appl.Phys., 73(1993)6621	Kiyoo Sato,Izuru Umehara,Kunihiko Maezawa,Tadashi Fukuhara,Yoshikazu Isikawa,Katsunori Mori		
131425	LES0110186	ANN(-50C, 6w)	Hg1-xInx	Hg0.5In0.5	Hg	0.5	In	0.5																					1966																																														K	3.8		3.82				3.81																																																																																																					New phase in the mercury-indium system				J.Less-Common Metals, 11(1966)186	T.Claeson,M.F.Merriam		
131426	LES0110186	ANN(-50C, 6w)	Hg1-xInx	Hg0.333In0.667	Hg	0.333	In	0.667																					1966																																														K	4.08		4.15				4.115																																																																																																					New phase in the mercury-indium system				J.Less-Common Metals, 11(1966)186	T.Claeson,M.F.Merriam		
131427	LES0420355	as-cast. sigma-phase + (alpha)1 trace	(Nb,Ir)	Ir0.42Nb0.58	Ir	0.42	Nb	0.58																					1975																																														K		4.2					4.2																																																																																																					Superconductivity of new metastable phases of niobium-iridium, tantalum-iridium and tantalum-rhodium				J.Less-Common Metals, 42(1975)355	W.L.Johnson,S.Poon		
131428	LES0420355	as-cast	(Nb,Ir,O)	Ir0.4Nb0.55O0.05	Ir	0.4	Nb	0.55																	O	0.05			1975																																														K		10.5					10.5																																																																																																					Superconductivity of new metastable phases of niobium-iridium, tantalum-iridium and tantalum-rhodium				J.Less-Common Metals, 42(1975)355	W.L.Johnson,S.Poon		
131429	LES0420355	ANN(900C,2d). (alpha)1-phase + sigma trace.	(Nb,Ir,O)	Ir0.455Nb0.455O0.09	Ir	0.455	Nb	0.455																	O	0.09			1975																																														K		9.2					9.2																																																																																																					Superconductivity of new metastable phases of niobium-iridium, tantalum-iridium and tantalum-rhodium				J.Less-Common Metals, 42(1975)355	W.L.Johnson,S.Poon		
131430	LES0420355	ANN(1150C, 1d).  sigma-phase + new phase.	(Ta,Rh,C)	C0.03Rh0.43Ta0.54	C	0.03	Rh	0.43	Ta	0.54																			1975																																														K		10					10																																																																																																					Superconductivity of new metastable phases of niobium-iridium, tantalum-iridium and tantalum-rhodium				J.Less-Common Metals, 42(1975)355	W.L.Johnson,S.Poon		
131431	LES0420355	quench.  sigma-phase + new phase.	(Ta,Ir)	Ir0.42Ta0.58	Ir	0.42	Ta	0.58																					1975																																														K		6.6					6.6																																																																																																					Superconductivity of new metastable phases of niobium-iridium, tantalum-iridium and tantalum-rhodium				J.Less-Common Metals, 42(1975)355	W.L.Johnson,S.Poon		
131432	CEM0010143	chemical compositions not investigated. Tc range of 1.5 - 4.2 measured by magnetization	GeP	Ge1P1	Ge	1	P	1																					1970									4.73																	AB	2				A	3.544		5.581												K		4.2					4.2																																																																							mOhm.cm	0.09										0.1																			Synthesis, structure, and superconductivity of new high pressure phases in the systems Ge-P and Ge-As				J.Solid State Chem., 1(1970)143	P.C.Donohue,H.S.Young		
131433	CEM0010143	chemical compositions not investigated. Tc range of 3 - 3.5 measured by magnetization	GeAs	As1Ge1	As	1	Ge	1																					1970									6.06																	AB	2				A	3.712		5.832												K		3.5					3.5																																																																							mOhm.cm	2.5										3.8																			Synthesis, structure, and superconductivity of new high pressure phases in the systems Ge-P and Ge-As				J.Solid State Chem., 1(1970)143	P.C.Donohue,H.S.Young		
131434	JPS0610293	ANN(600C,5d). [resrt]  = R(280 K.)	U7Ge	Ge1U7	Ge	1	U	7																					1992																										AB7																				K		1.4					1.4																																																								mJ/mol.K2	16									uV/K	9.1				uOhm.cm				2.57							6.59												U(3N),Ge(6N)		arc-melting - wrapped in Ta, Zr foil - sealed (quartz tube) - ANN(5d)					Magnetic and electrical properties of U-Ge intermetallic compounds				J.Phys.Soc.Jpn, 61(1992)293	Y.Onuki,I.Ukon,Sung Won Yun,I.Umehara,K.Satoh,T.Fukuhara,H.Sato,S.Takayanagi,M.Shikama,A.Ochiai		
131435	JPS0610293	ANN(900C,5d). [resrt]  = R(280 K.)	U5Ge3	Ge3U5	Ge	3	U	5																					1992																										A3B5	7				A	8.72		5.84											hexagonal	K		0.99					0.99																																																								mJ/mol.K2	36									uV/K	10.4				uOhm.cm				87							123												U(3N),Ge(6N)		arc-melting - wrapped in Ta, Zr foil - sealed (quartz tube) - ANN(5d)					Magnetic and electrical properties of U-Ge intermetallic compounds				J.Phys.Soc.Jpn, 61(1992)293	Y.Onuki,I.Ukon,Sung Won Yun,I.Umehara,K.Satoh,T.Fukuhara,H.Sato,S.Takayanagi,M.Shikama,A.Ochiai		
131436	JPS0610293	ANN(900C,5d). Ferromag (92K)	U3Ge4	Ge4U3	Ge	4	U	3																					1992							94																			A3B4	3				A	5.88	9.92	8.94											ortho-	K					1																																																																																																U(3N),Ge(6N)		arc-melting - wrapped in Ta, Zr foil - sealed (quartz tube) - ANN(5d)					Magnetic and electrical properties of U-Ge intermetallic compounds				J.Phys.Soc.Jpn, 61(1992)293	Y.Onuki,I.Ukon,Sung Won Yun,I.Umehara,K.Satoh,T.Fukuhara,H.Sato,S.Takayanagi,M.Shikama,A.Ochiai		
131437	JPS0610293	ANN(900C,5d). [resrt]  = R(280 K.). Ferromag(52K)	UGe2	Ge2U1	Ge	2	U	1																				3	1992							52																			AB2	3				A	4.09	15.2	3.96											ortho-	K					1																																																										mJ/mol.K2	35									uV/K	25.8				uOhm.cm				187							246												U(3N),Ge(6N)		arc-melting - wrapped in Ta, Zr foil - sealed (quartz tube) - ANN(5d)					Magnetic and electrical properties of U-Ge intermetallic compounds				J.Phys.Soc.Jpn, 61(1992)293	Y.Onuki,I.Ukon,Sung Won Yun,I.Umehara,K.Satoh,T.Fukuhara,H.Sato,S.Takayanagi,M.Shikama,A.Ochiai		
131438	LES1540187	90%-A15 phase. chemical comp. = Nb82.68Ge17.32. RRR = 1.93	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																				1	1989																										AB3		Cr3Si(A15)			A	5.168													Cr3Si, A15	K		4.8					4.8																																																3.34	14																						uOhm.cm							35.9																		arc-melting - ANN(950C,5d)					Electronic and phononic thermal conductivity of A15 polycristalline superconductors				J.Less-Common Metals, 154(1989)187	C.Ferdeghini,M.Putti,A.S.Siri,M.Ferretti,R.Masini		
131439	LES1540187	chemical comp. = V75.18Si24.82. RRR = 16.98	V3Si	Si1V3	Si	1	V	3																				1	1989																										AB3		Cr3Si(A15)			A	4.7262													Cr3Si, A15	K		16					16																																																3.9	14																						uOhm.cm							3.55																		arc-melting - ANN(950C,5d)					Electronic and phononic thermal conductivity of A15 polycristalline superconductors				J.Less-Common Metals, 154(1989)187	C.Ferdeghini,M.Putti,A.S.Siri,M.Ferretti,R.Masini		
131440	LES1540187	partially hydrogenated(interstitial H). chemical comp. = V74.8Ge25.2. RRR = 11.23	V3GeHx	Ge1H0.005V3	Ge	1	H	0.005	V	3																		1	1989																										AB3		Cr3Si(A15)			A	4.7832													Cr3Si, A15	K		5.8					5.8																																																3.77	14																						uOhm.cm							8.42																		arc-melting - ANN(950C,5d)					Electronic and phononic thermal conductivity of A15 polycristalline superconductors				J.Less-Common Metals, 154(1989)187	C.Ferdeghini,M.Putti,A.S.Siri,M.Ferretti,R.Masini		
131441	SSC0441083	24.9%-Ge.  neutron irradiated ( n - 2.2 E+19 /cm2) at 70C. (dC/gamma*Tc) = 1.5. e-ph coupling = 0.54	Mo3Ge	Ge1Mo3	Ge	1	Mo	3																					1982																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		4.25					4.25																																																					MSP131441			mJ/gmol.K2	5.4	SP-heat	322	SP-heat																																				arc-melting - ANN(1600C,16h  + 800C,2h)					Heat capacity measurements on irradiated and non-irradiated Mo3Ge and Mo5Ge3				Solid State Commun., 44(1982)1083	A.K.ghosh,R.Caton		
131442	SSC0441083	24.9%-Ge.	Mo3Ge	Ge1Mo3	Ge	1	Mo	3																					1982																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		1.45					1.45																																																								mJ/gmol.K2	4.9	SP-heat	392	SP-heat																																				arc-melting - ANN(1600C,16h  + 800C,2h)					Heat capacity measurements on irradiated and non-irradiated Mo3Ge and Mo5Ge3				Solid State Commun., 44(1982)1083	A.K.ghosh,R.Caton		
131443	SSC0441083	36.7%-Ge.  neutron irradiated ( n - 2.2 E+19 /cm2) at 70C.   (dC/gamma*Tc) = 1.2. e-ph coupling = 0.50	Mo5Ge3	Ge3Mo5	Ge	3	Mo	5																					1982																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		3.3					3.3																																																					MSP131443			mJ/gmol.K2	12.8	SP-heat	320	SP-heat																																				arc-melting - ANN(1600C,16h  + 800C,2h)					Heat capacity measurements on irradiated and non-irradiated Mo3Ge and Mo5Ge3				Solid State Commun., 44(1982)1083	A.K.ghosh,R.Caton		
131444	SSC0441083	36.7%-Ge	Mo5Ge3	Ge3Mo5	Ge	3	Mo	5																					1982																										AB3		Cr3Si(A15)																	Cr3Si, A15	K					1.6																																																										mJ/gmol.K2	12.3	SP-heat	377	SP-heat																																				arc-melting - ANN(1600C,16h  + 800C,2h)					Heat capacity measurements on irradiated and non-irradiated Mo3Ge and Mo5Ge3				Solid State Commun., 44(1982)1083	A.K.ghosh,R.Caton		
131445	JPS0580795	lattice term in SP (beta) = 1.20 mJ/mol.K4	U5Ge3	Ge3U5	Ge	3	U	5																					1989																										A3B5	7				A	8.56		5.83											hexagonal	K	0.87	0.99	1.3				0.99																				T	resistivity, WHH	0.38							T/K	resistivity	0.55			MHC131445																						mJ/gmol.K2	180	SP-heat	118	SP-heat																																				arc-melting. - wrapped in Ta- and Zr-foil  - ANN(900C,5d, in 1 E-6 Torr vac)					Superconductivity in U5Ge3				J.Phys.Soc.Jpn, 58(1989)795	Y.Onuki,I.Ukon,T.Komatsubara,S.Takayanagi,N.Wada,T.Watanabe		
131446	SSC0170281	Debye-T from resistivity measurements	PdH0.995	H0.995Pd1	H	0.995	Pd	1																					1975																										AB		NaCl																		K	9		9.55				9.275																																																											210																																										Electrical resistivity of Pd-Hx:  II.Phonon resistivity				Solid State Commun., 17(1975)281	D.S.MacLachlan,R.Mailfert,J.P.Burger,B.Souffache		
131447	SSC0240733	target: arc-melted V3Ge. T<sub> = 1060 K.	V3Ge	Ge1V3	Ge	1	V	3																				4	1977																										AB3		Cr3Si(A15)																	Cr3Si, A15	K	7.3	8.6	11.2				8.6																																																																																																sputtered on sapphire substrates					The sputtering of high Tc A15 Nb3Si and V3Ge				Solid State Commun., 24(1977)733	R.E.Somekh,J.E.Evetts		
131448	SSC0240733	target: arc-melted Nb3Si. T<sub> = 1370 K. Tc(R=0.1Rn) < 4.2	Nb3Si	Nb3Si1	Nb	3	Si	1																				4	1977																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		8.6	14				8.6																																																																																																sputtered on sapphire substrates					The sputtering of high Tc A15 Nb3Si and V3Ge				Solid State Commun., 24(1977)733	R.E.Somekh,J.E.Evetts		
131449	SSC0390825	He-ion(2MeV, RT) irradiation effect for V3Ge film. Tc = 4.5 K and 1.2 K for 2 E+16 and 2 E+17 /cm2 fluence, respectively.	V3Ge	Ge1V3	Ge	1	V	3																				5	1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		6					6																																																																																																					Radiation damage in the non-metal sublattices of V3Ge and V3Si single crystals				Solid State Commun., 39(1981)825	O.Meyer,R.Kaufmann,B.P.Appleton,Y.K.Chang		
131450	SSC0390825	He-ion(300keV, RT) irradiation effect for V3Si film. Tc = 3.5 K and 2.5 K for 4 E+16 and 6 E+16 /cm2 fluence, respectively.	V3Si	Si1V3	Si	1	V	3																				5	1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		16.6					16.6																																																																																																					Radiation damage in the non-metal sublattices of V3Ge and V3Si single crystals				Solid State Commun., 39(1981)825	O.Meyer,R.Kaufmann,B.P.Appleton,Y.K.Chang		
131451	SSC0161085		Th4H15	H15Th4	H	15	Th	4																					1975																										A4B15																				K		7.6					7.6																																																								mJ/gmol.K2	0.82	SP-heat	200	SP-heat																																									The heat capacity of Th and Th4H15 in the temperature range above 2 K				Solid State Commun., 16(1975)1085	H.-G.Schmidt,G.Wolf		
131452	SSC0210603	Debye-T calculated from phonon spectrum obtained inelastic neutron scattering measurements.	ThH2	H2Th1	H	2	Th	1																					1977																										AB2																				K					1																																																													170	netron																																									Phonon densities of states of the thorium hydrides				Solid State Commun., 21(1977)603	M.Dietrich,W.Reichardt,H.Rietschel		
131453	SSC0210603	Debye-T calculated from phonon spectrum obtained inelastic neutron scattering measurements.	Th4H15	H15Th4	H	15	Th	4																					1977																										A4B15																				K		7.6				0.3	7.6																																																											250	netron																																									Phonon densities of states of the thorium hydrides				Solid State Commun., 21(1977)603	M.Dietrich,W.Reichardt,H.Rietschel		
131454	SSC0230223		YGe2	Ge2Y1	Ge	2	Y	1																				4	1977																										AB2																			Cc	K		3.8					3.8																																																																																																rf sputtering					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131455	SSC0230223		ZrGe2	Ge2Zr1	Ge	2	Zr	1																				4	1977																										AB2																			Cc	K		8					8																																																																																																rf sputtering					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131456	SSC0230223		HfGe2	Ge2Hf1	Ge	2	Hf	1																				4	1977																										AB2																			Cc	K		2.2					2.2																																																																																																rf sputtering					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131457	SSC0820111	P-induced SC. Tc shows for P=1.5 GPa. Resistivity anomaly at 15.2 K, which comes from AFM-AFM transition.	TbGa6	Ga6Tb1	Ga	6	Tb	1																					1992								18.8																		AB6					A	5.936		7.56											PuGa5	K	4		6		0		5	MTC131457																																																																																															arc-melting - ANN(570C,3d, in quartz tube)					PRESSURE-INDUCED SUPERCONDUCTIVITY IN TBGA6 AND DYGA6				SOLID STATE COMMUN.82(1992)111	H.FUJIWARA,H.KADOMATSU,J.SAKURAI,J.SUGAMOTO	TB,GA,DY	
131458	SSC0820111	P-induced SC. P<crit> = 1.1 GPa. (Tc,P) = (5.89K,1.25GPa), (5.97K, 1.5GPa). (Tn,P) = (11.3K, 0.5GPa), (10.7K, 1.0GPa), (9.83K, 1.5GPa). (dTn/dP) = -1.5 K/GPa.	DyGa6	Dy1Ga6	Dy	1	Ga	6																					1992								12.2																		AB6					A	5.928		7.56											PuGa5	K			5.9		0		5.9																																																																																																arc-melting - ANN(570C,3d, in quartz tube)					PRESSURE-INDUCED SUPERCONDUCTIVITY IN TBGA6 AND DYGA6				SOLID STATE COMMUN.82(1992)111	H.FUJIWARA,H.KADOMATSU,J.SAKURAI,J.SUGAMOTO	TB,GA,DY	
131459	SSC0390773	S-O coupling (ramda<SO>) = 0.25	V3Ga	Ga26.5V73.5	Ga	26.5	V	73.5																					1981																										AB3		Cr3Si(A15)			A	4.82													Cr3Si, A15	K		13.6					13.6																				T	resstivity, so-coupling	21.8							T/K	resistivity	5.5																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131460	SSC0390773	S-O coupling (ramda<SO>) = 0.3	V3Ga	Ga25V75	Ga	25	V	75																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		15.3					15.3																				T	resstivity, so-coupling	23.4							T/K	resistivity	4.3			MHC131460																																																												V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131461	SSC0390773	S-O coupling (ramda<SO>) = 0.1	V3Ga	Ga20.5V79.5	Ga	20.5	V	79.5																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		9.7					9.7																				T	resstivity, so-coupling	13							T/K	resistivity	4.3																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131462	SSC0390773	S-O coupling (ramda<SO>) = 0.2	V3Ga	Ga22.2V77.8	Ga	22.2	V	77.8																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		12.3					12.3																				T	resstivity, so-coupling	17.8							T/K	resistivity	4.3																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131463	SSC0390773	S-O coupling (ramda<SO>) = 0.3	V3Ga	Ga23.6V76.4	Ga	23.6	V	76.4																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		14.6					14.6																				T	resstivity, so-coupling	22.3							T/K	resistivity	4.3																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131464	SSC0390773	S-O coupling (ramda<SO>) = 0.25	V3Ga	Ga24.8V75.2	Ga	24.8	V	75.2																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		15.1					15.1																				T	resstivity, so-coupling	22.5							T/K	resistivity	4.3																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131465	SSC0390773	S-O coupling (ramda<SO>) = 0.3	V3Ga	Ga25.3V74.7	Ga	25.3	V	74.7																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		14.9					14.9																				T	resstivity, so-coupling	22.8							T/K	resistivity	4.3																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131466	SSC0390773	S-O coupling (ramda<SO>) = 0.3	V3Ga	Ga28.1V71.9	Ga	28.1	V	71.9																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		12.2					12.2																				T	resstivity, so-coupling	20.3							T/K	resistivity	5.5																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131467	SSC0390773	S-O coupling (ramda<SO>) = 0.25	V3Ga	Ga29.6V70.4	Ga	29.6	V	70.4																					1981																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		12.1					12.1																				T	resstivity, so-coupling	19.4							T/K	resistivity	5.5																																																															V,Ga(6N)		arc-melting - ANN(1400C,6h) - ANN(1100-1200C,24h)					Effect of composition on the upper critical field of V-Ga				Solid State Commun., 39(1981)773	S.Foner,E.J.McNiff,Jr,S.Moehlecke,A.R.Sweedler		
131468	SSC0141051	24.6 at%Gd. Two step transitions. (dC/Tc) = 125 mJ/g-mol.K2 at 13.4 K.	V3Ga	Ga1V3	Ga	1	V	3																					1974																										AB3		Cr3Si(A15)			A	4.819													Cr3Si, A15	K		15.2					15.2																																																								mJ/gmol.K2	96	SP-heat	302	SP-heat																																				arc-melting. ANN(1300C,2h) + ANN(700C,3d)					Low temperature heat-capacity measurements of V3Ga and Nb3Al				Solid State Commun., 14(1974)1051	R.Viswanathan,C.T.Wu,H.L.Luo,G.W.Webb		
131469	SSC0141051	24.6 At%Al. Two step transitions. (dC/Tc) = 60 mJ/g-mol.K2 at 15.7 K.	Nb3Al	Al1Nb3	Al	1	Nb	3																					1974																										AB3		Cr3Si(A15)			A	5.182													Cr3Si, A15	K		18.7					18.7																																																								mJ/gmol.K2	30	SP-heat	230	SP-heat																																				arc-melting. heat(1940C,12min) and ANN(725C,50h)					Low temperature heat-capacity measurements of V3Ga and Nb3Al				Solid State Commun., 14(1974)1051	R.Viswanathan,C.T.Wu,H.L.Luo,G.W.Webb		
131470	LES0990L27	composition: MoGa6	Mo8Ga41	Ga41Mo8	Ga	41	Mo	8																					1984																													R3[-]		A	14.039		15.039											rhomb-Mo8Ga41 phase	K		9.7					9.7																				T	resistivity	8.6												MHC131470																																																														mixture in alumina crucible - sealed in quartz tube(150 Torr-Ar) - heat(300C,1h) - heat(1000C,5h) - slow cool to RT					On the existence of binary Mo8Ga41 and its properties				J.Less-Common Metals, 99(1984)L27	A.Bezinge,K.Yvon,M.Decroux,J.Muller		
131471	LES0990L27	composition: MoGa5.3Au(1/6)	Mo8Ga40Au	Au1Ga40Mo8	Au	1	Ga	40	Mo	8																			1984																													R3[-]		A	13.991		15.083											rhomb-Mo8Ga41 phase	K		9.4					9.4																				T	resistivity	8.9																																																																										mixture in alumina crucible - sealed in quartz tube(150 Torr-Ar) - heat(300C,1h) - heat(1000C,5h) - slow cool to RT					On the existence of binary Mo8Ga41 and its properties				J.Less-Common Metals, 99(1984)L27	A.Bezinge,K.Yvon,M.Decroux,J.Muller		
131472	LES0960191	Ga-ion implanted in V-single crystals and annealed.	V3Ga	Ga0.21V0.79	Ga	0.21	V	0.79																				3	1984																										AB3		Cr3Si(A15)			A	4.812													Cr3Si, A15	K		10					10																																																																																																Ga-ion inplanted on surface [111] of V-single crystals					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131473	LES0960191	Ga-ion implanted in V-single crystals and annealed.	V3Ga	Ga0.25V0.75	Ga	0.25	V	0.75																				3	1984																										AB3		Cr3Si(A15)			A	4.814													Cr3Si, A15	K		14.5					14.5																																																																																																Ga-ion inplanted on surface [111] of V-single crystals					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131474	LES0960191	Ga-ion implanted in V-single crystals and annealed.	V3Ga	Ga0.31V0.69	Ga	0.31	V	0.69																				3	1984																										AB3		Cr3Si(A15)			A	4.819													Cr3Si, A15	K		15.4					15.4																																																																																																Ga-ion inplanted on surface [111] of V-single crystals					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131475	LES0960191	Ga-ion implanted in V-films, deposited on heated sapphire substrates. RRR = 1.29	V3Ga	Ga0.2V0.8	Ga	0.2	V	0.8																				4	1984																										AB3		Cr3Si(A15)			A	4.813													Cr3Si, A15	K		12.5					12.5																																																																							uOhm.cm							93				120														Ga-ion inplanted into V-films deposited on heated sapphire substrates					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131476	LES0960191	Ga-ion implanted in V-films, deposited on heated sapphire substrates. RRR = 1.18	V3Ga	Ga0.25V0.75	Ga	0.25	V	0.75																				4	1984																										AB3		Cr3Si(A15)			A	4.815													Cr3Si, A15	K		12.7					12.7																																																																							uOhm.cm							140				165														Ga-ion inplanted into V-films deposited on heated sapphire substrates					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131477	LES0960191	Ga-ion implanted in V-films, deposited on heated sapphire substrates. RRR = 1.11	V3Ga	Ga0.3V0.7	Ga	0.3	V	0.7																				4	1984																										AB3		Cr3Si(A15)			A	4.824													Cr3Si, A15	K		14.1					14.1																																																																							uOhm.cm							167				186														Ga-ion inplanted into V-films deposited on heated sapphire substrates					Nucleation and growth of A15 V3Ga from ion-implanted superstructured Ga-V solid solutions				J.Less-Common Metals, 96(1984)191	J.M.Lombaard,G.Linker,O.Meyer		
131478	LES1190269		YGa6	Ga6Y1	Ga	6	Y	1																					1986																										AB6	2	PuGa6	P4/nbm																tetragonal-PuGa6	K		2					2																																																																																																arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131479	LES1190269		LaGa6	Ga6La1	Ga	6	La	1																					1986																										AB6	2	PuGa6	P4/nbm		A	6.1005		7.6935											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131480	LES1190269	Curie-T from SUS.	CeGa6	Ce1Ga6	Ce	1	Ga	6																					1986					myu-B/R	2.37	-1.4																			AB6	2	PuGa6	P4/nbm		A	6.0451		7.6698											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131481	LES1190269	Curie-T from SUS.	PrGa6	Ga6Pr1	Ga	6	Pr	1																					1986					myu-B/R	3.31	6	9.1																		AB6	2	PuGa6	P4/nbm		A	6.0092		7.6589											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131482	LES1190269	Curie-T from SUS.	NdGa6	Ga6Nd1	Ga	6	Nd	1																					1986					myu-B/R	3.37	2.2	10.4																		AB6	2	PuGa6	P4/nbm		A	5.9908		7.6382											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131483	LES1190269	Curie-T from SUS.	SmGa6	Ga6Sm1	Ga	6	Sm	1																					1986					myu-B/R	0.88	-30	4.2																		AB6	2	PuGa6	P4/nbm		A	5.9646		7.6129											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131484	LES1190269	Curie-T from SUS.	GdGa6	Ga6Gd1	Ga	6	Gd	1																					1986					myu-B/R	7.59	-32.8	12.6																		AB6	2	PuGa6	P4/nbm		A	5.9379		7.5742											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131485	LES1190269	Curie-T from SUS.	TbGa6	Ga6Tb1	Ga	6	Tb	1																					1986					myu-B/R	9.8	-20.8	18																		AB6	2	PuGa6	P4/nbm		A	5.9344		7.5597											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131486	LES1190269	Curie-T from SUS.	DyGa6	Dy1Ga6	Dy	1	Ga	6																					1986					myu-B/R	10.87	-10.9	11.7																		AB6	2	PuGa6	P4/nbm		A	5.9251		7.5499											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131487	LES1190269	Curie-T from SUS.	HoGa6	Ga6Ho1	Ga	6	Ho	1																					1986					myu-B/R	10.12	-5.9	6.3																		AB6	2	PuGa6	P4/nbm		A	5.919		7.5411											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131488	LES1190269	Curie-T from SUS.	ErGa6	Er1Ga6	Er	1	Ga	6																					1986					myu-B/R	7	-0.9	3.9																		AB6	2	PuGa6	P4/nbm		A	5.9113		7.5271											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131489	LES1190269		YbGa6	Ga6Yb1	Ga	6	Yb	1																					1986																										AB6	2	PuGa6	P4/nbm		A	6.0723		7.6501											tetragonal-PuGa6	K					1.7																																																																																																		arc-melting - ANN(570K,3d,in evacuated quartz tube)					Magnetic susceptibility and electrical resistivity of RGa6 (R = rare earth metals)				J.Less-Common Metals, 119(1986)269	Y.Tagawa,J.Sakurai,Y.Komura,T.Ishimasa		
131490	SSC0040533	SUS(RT) = 0.29 E-6 emu/g	CuS2	Cu1S2	Cu	1	S	2																					1966									4.354																	AB2		FeS2(pyrite)			A	5.79														K	1.48		1.53				1.505																																																																							uOhm.cm	0.25										150														high pressure ssynthesis. P=65 kbar					New transition metal dichalcogenides formed at high pressure				Solid State Commun., 4(1966)533	T.A.Btther,C.T.Prewitt,J.L.Gillson,P.E.Bierstedt,R.B.Flippen,H.S.Young		
131491	SSC0040533		CuSSe	Cu1S1Se1	Cu	1	S	1	Se	1																			1966																										AB2		FeS2(pyrite)			A	5.923														K	1.5		2				1.75																																																																							uOhm.cm	38										95														high pressure ssynthesis. P=65 kbar					New transition metal dichalcogenides formed at high pressure				Solid State Commun., 4(1966)533	T.A.Btther,C.T.Prewitt,J.L.Gillson,P.E.Bierstedt,R.B.Flippen,H.S.Young		
131492	SSC0040533	SUS(RT) = 0.42 E-6 emu/g	CuSe2	Cu1Se2	Cu	1	Se	2																					1966																										AB2		FeS2(pyrite)			A	6.123														K	2.3		2.43				2.365																																																																							uOhm.cm	0.12										75														high pressure ssynthesis. P=65 kbar					New transition metal dichalcogenides formed at high pressure				Solid State Commun., 4(1966)533	T.A.Btther,C.T.Prewitt,J.L.Gillson,P.E.Bierstedt,R.B.Flippen,H.S.Young		
131493	SSC0040533	SUS(RT) = 0.39 E-6 emu/g	CuSeTe	Cu1Se1Te1	Cu	1	Se	1	Te	1																			1966																										AB2		FeS2(pyrite)			A	6.302														K	1.6		2				1.8																																																																							uOhm.cm	260										680														high pressure ssynthesis. P=65 kbar					New transition metal dichalcogenides formed at high pressure				Solid State Commun., 4(1966)533	T.A.Btther,C.T.Prewitt,J.L.Gillson,P.E.Bierstedt,R.B.Flippen,H.S.Young		
131494	SSC0040533	SUS(RT) = -0.40 E-6 emu/g	CuTe2	Cu1Te2	Cu	1	Te	2																					1966																										AB2		FeS2(pyrite)			A	6.6														K			1.3				1.3																																																																							uOhm.cm	55										560														high pressure ssynthesis. P=65 kbar					New transition metal dichalcogenides formed at high pressure				Solid State Commun., 4(1966)533	T.A.Btther,C.T.Prewitt,J.L.Gillson,P.E.Bierstedt,R.B.Flippen,H.S.Young		
131495	SSC0220109	ANN(650C,1 month), ordered crystal	Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1977																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		20.5					20.5																																																																																																arc-melting					The effects of composition and atomic ordering on superconductivity in the systems Nb3Ga and V3Ga				Solid State Commun., 22(1977)109	R.Flukiger,J.L.Jorda		
131496	SSC0220109	ordered crystal. Tc(max) = 15.9 K.	V3Ga	Ga1V3	Ga	1	V	3																					1977																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		15.9					15.9																																																																																																arc-melting					The effects of composition and atomic ordering on superconductivity in the systems Nb3Ga and V3Ga				Solid State Commun., 22(1977)109	R.Flukiger,J.L.Jorda		
131497	SSC0331015	15%Nb5Ga3 contained. total analysis: Nb0.74Ga0.26. SP-heat data shows after phase volume correction. DOS=1.7 states/eV-atom using e-ph = 1.8.	Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1980																										AB3		Cr3Si(A15)			A	5.17													Cr3Si, A15	K		19.8					19.8																																																								mJ/gat.K2	11.4	SP-heat	280	SP-heat																																				arc-melting - heat(1830C,4min) - Q to RT - ANN(700C,123h)					Specific Heat of High Tc, A-15 Nb0.75Ga0.25			Los Alamos Scientific Laboratory, University of California, Los Alamos, N.M. 87545	Solid State Commun., 33(1980)1015	G.R.Stewart,G.W.Webb		
131498	CEM0340045	reaction(1800C,0.01h, P(N2)=2.0 MPa)	NbNx	N1.07Nb1	N	1.07	Nb	1																				1	1980																																														K		14.4					14.4																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131499	CEM0340045	zone annealing (2200C,111h, P(N2)=1.9 MPa)	NbNx	N0.78Nb1	N	0.78	Nb	1																					1980																																														K		10.5					10.5																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131500	CEM0340045	zone annealing (2320C,191h, P(N2)=1.7 MPa)	NbNx	N0.89Nb1	N	0.89	Nb	1																					1980																																														K		12.1					12.1																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131501	CEM0340045	zone annealing (2320C,307h, P(N2)=1.7 MPa)	NbNx	N0.93Nb1	N	0.93	Nb	1																					1980																																														K		13.3					13.3																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131502	CEM0340045	heat(1800C, 0.01h, P(N2) = 2.0 MPa)	Nb(NC)	C0.28N0.76Nb1	C	0.28	N	0.76	Nb	1																			1980																																														K		16.4					16.4																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131503	CEM0340045	zone melting growth rate = 10 mm/h, P(He) = 1.0 MPa	Nb3Al	Al1Nb3	Al	1	Nb	3																					1980																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		17.4					17.4																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131504	CEM0340045	zone melting growth rate = 10 mm/h, P(He) = 0.1 MPa	Nb3Ge	Ge1Nb3	Ge	1	Nb	3																					1980																										AB3		Cr3Si(A15)																	Cr3Si, A15	K					6.4																																																																																																							Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131505	CEM0340045	zone melting growth rate = 20 mm/h, P(He) = 0.3 MPa	Nb3Ga	Ga1Nb3	Ga	1	Nb	3																					1980																										AB3		Cr3Si(A15)																	Cr3Si, A15	K		8.2					8.2																																																																																																					Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131506	CEM0340045	zone melting growth rate = 10 mm/h, P(He) = 0.5 MPa	VB	B1V1	B	1	V	1																					1980																										AB																				K					7.2																																																																																																							Superconductivity of some transition metal compounds				J.Solid State Chem., 34(1980)45	A.Norlund Christensen,S.E.Rasmussen,G.Thirup		
131507	PCS0190130		ZrW2	W2Zr1	W	2	Zr	1																					1961																										AB2		MgCu2(Laves)			A	7.621													C15	K		2.16					2.16																																																																																																					Some new superconducting compounds				J.Phys.Chem.Solids, 19(1961)130	B.T.Matthias,V.B.Compton,E.Corenzwit		
131508	PCS0190130		ZrRu2	Ru2Zr1	Ru	2	Zr	1																					1961																										AB2		MgZn2(Laves)			A	5.144		8.504											C14	K		1.84					1.84																																																																																																					Some new superconducting compounds				J.Phys.Chem.Solids, 19(1961)130	B.T.Matthias,V.B.Compton,E.Corenzwit		
131509	PCS0190130		Nb3Os2	Nb3Os2	Nb	3	Os	2																					1961																										A2B3		sigma-CrFe			A	9.844		5.056											sigma-phase	K		1.78					1.78																																																																																																					Some new superconducting compounds				J.Phys.Chem.Solids, 19(1961)130	B.T.Matthias,V.B.Compton,E.Corenzwit		
131510	PCS0190130		Nb5Pt3	Nb5Pt3	Nb	5	Pt	3																					1961																										A3B5		sigma-CrFe			A	9.91		5.12											sigma-phase	K		3.73					3.73																																																																																																					Some new superconducting compounds				J.Phys.Chem.Solids, 19(1961)130	B.T.Matthias,V.B.Compton,E.Corenzwit		
131511	PRL0260305	impuritiy: Mo3Ga < 5at%	MoGa4	Ga4Mo1	Ga	4	Mo	1																					1971																										AB4																				K		8					8																				T		7.37												MHC131511																																																														heat(1300C, in 2atm-Ar) - pellet - ANN(700C,1w) - Q					Compensation of the paramagnetic effect on Hc2 by magnetic impurities				Phys.Rev.Lett., 26(1971)305	F.Fischer,H.jones,G.Bongi,C.Frei,A.Treyvaud		
131512	PRL0260305	impuritiy: Mo3Ga < 5at%	(Mo,Mn)Ga4	Ga4Mn0.006Mo0.994	Ga	4	Mn	0.006	Mo	0.994																			1971																										AB4																				K		7.14					7.14																																		MHC131511																																																														heat(1300C, in 2atm-Ar) - pellet - ANN(700C,1w) - Q					Compensation of the paramagnetic effect on Hc2 by magnetic impurities				Phys.Rev.Lett., 26(1971)305	F.Fischer,H.jones,G.Bongi,C.Frei,A.Treyvaud		
131513	PRL0260305	impuritiy: Mo3Ga < 5at%	(Mo,Mn)Ga4	Ga4Mn0.01Mo0.99	Ga	4	Mn	0.01	Mo	0.99																			1971																										AB4																				K		4					4																																		MHC131511																																																														heat(1300C, in 2atm-Ar) - pellet - ANN(700C,1w) - Q					Compensation of the paramagnetic effect on Hc2 by magnetic impurities				Phys.Rev.Lett., 26(1971)305	F.Fischer,H.jones,G.Bongi,C.Frei,A.Treyvaud		
131514	JAC2060047	SUS(RT) = 3.7 E-4 emu/mol. (dC/Tc) = 72 mJ/mol.K2, (dC/gamma*Tc) = 1.06	Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1994																										AB2		CuAl2			A	6.497		5.614											CuAl2, C16	K		11.2					11.2																																																					MSP131514			mJ/mol.K2	68	SP-heat	214	SP-heat																																				arc-melting					Effect of hydrogen absorption on structure, superconductivity, magnetic susceptibility and heat capacity of Zr2Rh				J.Alloys and Compound, 206(1994)47	P.Raj,P.Suryanarayana,A.Sathyamoorthy,K.Shashikala,R.M.Iyer,S.K.Dhar,L.C.Gupta,V.C.Sahni,R.J.Begum		
131515	JAC2060047	SUS(RT) = 1.8 E-4 emu/mol. lattice term in SP (beta) = 0.0312 mJ/mol.K4	Zr2RhH4.25	H4.25Rh1Zr2	H	4.25	Rh	1	Zr	2																			1994																												CuAl2			A	6.81		5.603											CuAl2, C16	K					1.8																																																										mJ/mol.K2	6	SP-heat	396	SP-heat																																				Hydriding(10atm-H2, RT) in stainless steel reactor					Effect of hydrogen absorption on structure, superconductivity, magnetic susceptibility and heat capacity of Zr2Rh				J.Alloys and Compound, 206(1994)47	P.Raj,P.Suryanarayana,A.Sathyamoorthy,K.Shashikala,R.M.Iyer,S.K.Dhar,L.C.Gupta,V.C.Sahni,R.J.Begum		
131516	JPS0610395	SC parameters estimated from resistivity and SP measurements using conventional SC relations. RRR=100. Thermodynamic Hc(0) = 85 Oe. (dC/gamma*Tc) = 1.4. GL = 1.4	LaGa2	Ga2La1	Ga	2	La	1																					1992																										AB2		AlB2			A	4.32		4.42											AlB2, C32	K		1.15					1.15											Oe		14							Oe		173							Oe/K		260					A		1400			A		2000			K	1.4		14							mJ/mol.K2	4														uOhm.cm							1																La(4N),Ga(5N)		arc-melting - wrapped in Zr foil - ANN(800C,2d, in evacuated quartz tube)					Superconductivity in LaGa2				J.Phys.Soc.Jpn, 61(1992)395	Y.Fujimaki,K.Satoh,Y.Onuki		
131517	JPS0651034	Two-step transition (maybe inhomogeneous)	U6Fe	Fe1U6	Fe	1	U	6																				3	1996																										AB6		U6Mn																		K	3.96	4.03	4.1				4.03																																																																																														U(3N),Fe(5N)		arc-melting. single crystal grown by zone melting (2mm/h)					Single crystal growth and upper critical field of the superconductor U6Fe				J.Phys.Soc.Jpn, 65(1996)1034	E.Yamamoto,M.Hedo,Y.Inada,T.Ishida,Y.Haga,Y.Onuki		
131518	JPS0651034		U6Fe	Fe1U6	Fe	1	U	6																				3	1996																										AB6		U6Mn																		K	3.98	3.99	4				3.99																				T	resistivity, WHH		13.1	10.4										MHC131518		A	from Hc2		56	50																																																						U(3N),Fe(5N)		arc-melting. single crystal grown byCzochralski method (10-15 mm/h).					Single crystal growth and upper critical field of the superconductor U6Fe				J.Phys.Soc.Jpn, 65(1996)1034	E.Yamamoto,M.Hedo,Y.Inada,T.Ishida,Y.Haga,Y.Onuki		
131519	SSC0220501	magnetic orderring T measured by Mossbauer and bulk SUS. Tm = 0.325 K	La1-xEux	Eu0.0034La0.9966	Eu	0.0034	La	0.9966																					1977																																														K		3.95					3.95	MTC131519																																																																																																				Magnetism and superconductivity in LaEu				Solid State Commun., 22(1977)501	P.Steiner,G.Gumprecht		
131520	SSC0220501	magnetic orderring T measured by Mossbauer and bulk SUS. Tm = 0.625 K	La1-xEux	Eu0.011La0.989	Eu	0.011	La	0.989																					1977																																														K		2.16					2.16																																																																																																					Magnetism and superconductivity in LaEu				Solid State Commun., 22(1977)501	P.Steiner,G.Gumprecht		
131521	SSC0520837	Tritium concentration x, determined by pressure-volume-temperature techniques.	PdTx	Pd1T0.81	Pd	1	T	0.81																					1984																																														K		4.04					4.04	MTC131521																																																																																																				SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
131522	SSC0520837		PdDx	D0.966Pd1	D	0.966	Pd	1																					1984																												NaCl																		K		8.25					8.25	MTC131521																																																																																																				SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
131523	SSC0520837		PdHx	H0.985Pd1	H	0.985	Pd	1																					1984																												NaCl																		K		7.39					7.39	MTC131521																																																																																																				SUPERCONDUCTIVITY OF PALLADIUM TRITIDE	198412	ISOTOPE EFFECT	SANDIA NATIONAL LABORATORIES ALBUQUERQUE,NM	SOLID STATE COMMUN.,52(1984)837	J.E.SCHIRBER,J.M.MINTZ,W.WALL	PD,H,D,T	
131530	BOOK2000		Y3Ru4Ge13	Y3Ru4Ge13	Y	3	Ru	4	Ge	13																			2000																												Yb3Rh4Sn13			A	8.962													ternary stannide	K		1.7					1.7																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131531	BOOK2000		Lu3Rh4Ge13	Lu3Rh4Ge13	Lu	3	Rh	4	Ge	13																			2000																												Yb3Rh4Sn13			A	8.912													ternary stannide	K		2.3					2.3																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131532	BOOK2000		Y3Os4Ge13	Y3Os4Ge13	Y	3	Os	4	Ge	13																			2000																												Yb3Rh4Sn13			A	8.985													ternary stannide	K		3.9					3.9																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131533	BOOK2000		Lu3Os4Ge13	Lu3Os4Ge13	Lu	3	Os	4	Ge	13																			2000																												Yb3Rh4Sn13			A	8.938													ternary stannide	K		3.6					3.6																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131534	BOOK2000		Ca3Rh4Ge13	Ca3Rh4Ge13	Ca	3	Rh	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.025													ternary stannide	K		2.1					2.1																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131535	BOOK2000		Ca3Ir4Ge13	Ca3Ir4Ge13	Ca	3	Ir	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.055													ternary stannide	K		1.7					1.7																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131536	BOOK2000		La3Ru4Sn13	La3Ru4Ge13	La	3	Ru	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.772													ternary stannide	K		3.9					3.9																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131537	BOOK2000		La3RuPd3Sn13	La3Ru1Pd3Ge13	La	3	Ru	1	Pd	3	Ge	13																	2000																												Yb3Rh4Sn13			A	9.78													ternary stannide	K		4.8					4.8																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131538	BOOK2000		Th3Os4Sn13	Th3Os4Ge13	Th	3	Os	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.721													ternary stannide	K		5.6					5.6																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131539	BOOK2000		Ca3Co4Sn13	Ca3Co4Ge13	Ca	3	Co	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.584													ternary stannide	K		5.9					5.9																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131540	BOOK2000		La3Co4Sn13	La3Co4Ge13	La	3	Co	4	Ge	13																			2000																												Yb3Rh4Sn13			A	9.641													ternary stannide	K		2.8					2.8																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131541	BOOK2000		Yb3Co4Sn13	Yb3Co4Sn13	Yb	3	Co	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.563													ternary stannide	K		2.5					2.5																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131542	BOOK2000		Ca3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.702													ternary stannide	K		8.7					8.7																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131543	BOOK2000		Sr3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.8													ternary stannide	K		4.3					4.3																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131544	BOOK2000		Yb3Rh4Sn13	Yb3Rh4Sn13	Yb	3	Rh	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.675													ternary stannide	K		8.6					8.6																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131545	BOOK2000		Th3Rh4Sn13	Th3Rh4Sn13	Th	3	Rh	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.692													ternary stannide	K		1.9					1.9																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131546	BOOK2000		Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.718													ternary stannide	K		7.1					7.1																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131547	BOOK2000		Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.807													ternary stannide	K		5.1					5.1																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131548	BOOK2000		La3Ir4Sn13	La3Ir4Sn13	La	3	Ir	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.755													ternary stannide	K		2.6					2.6																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131549	BOOK2000		Th3Ir4Sn13	Th3Ir4Sn13	Th	3	Ir	4	Sn	13																			2000																												Yb3Rh4Sn13			A	9.695													ternary stannide	K		2.6					2.6																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131550	BOOK2000		La3Rh4Pb13	La3Rh4Pb13	La	3	Rh	4	Pb	13																			2000																												Yb3Rh4Sn13			A	10.031													ternary stannide	K		2.2					2.2																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p229	Charles P.Poole Jr		
131551	BOOK2000-2	Idealized compounds	Sc4Rh6Ge19	Sc4Rh6Ge19	Sc	4	Rh	6	Ge	19																			2000																												Tb4Rh6Sn19			A	12.605													ternary stannide	K		1.9					1.9																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131552	BOOK2000-2	Idealized compounds	Sc4Ir6Ge19	Sc4Ir6Ge19	Sc	4	Ir	6	Ge	19																			2000																												Tb4Rh6Sn19			A	12.629													ternary stannide	K		1.4					1.4																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131553	BOOK2000-2	Idealized compounds. chemical analysis: YRu1.1Sn3.1	Y4Ru6Sn19	Y4Ru6Sn19	Y	4	Ru	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.772													ternary stannide	K		1.3					1.3																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131554	BOOK2000-2	Idealized compounds	Sc4Os6Sn19	Sc4Os6Sn19	Sc	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.606													ternary stannide	K		1.5					1.5																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131555	BOOK2000-2	Idealized compounds	Y4Os6Sn19	Y4Os6Sn19	Y	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.801													ternary stannide	K		2.5					2.5																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131556	BOOK2000-2	Idealized compounds	Tb4Os6Sn19	Tb4Os6Sn19	Tb	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.813													ternary stannide	K		1.4					1.4																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131557	BOOK2000-2	Idealized compounds	Ho4Os6Sn19	Ho4Os6Sn19	Ho	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.774													ternary stannide	K		1.4					1.4																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131558	BOOK2000-2	Idealized compounds	Er4Os6Sn19	Er4Os6Sn19	Er	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.76													ternary stannide	K		1.25					1.25																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131559	BOOK2000-2	Idealized compounds	Tm4Os6Sn19	Tm4Os6Sn19	Tm	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.744													ternary stannide	K		1.1					1.1																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131560	BOOK2000-2	Idealized compounds	Lu4Os6Sn19	Lu4Os6Sn19	Lu	4	Os	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.72													ternary stannide	K		1.8					1.8																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131561	BOOK2000-2	Idealized compounds. not SC	Tb4Rh6Sn19	Tb4Rh6Sn19	Tb	4	Rh	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.774													ternary stannide	K					1.1																																																																																																							Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131562	BOOK2000-2	Idealized compounds	Y4Ir6Sn19	Y4Ir6Sn19	Y	4	Ir	6	Sn	19																			2000																												Tb4Rh6Sn19			A	13.773													ternary stannide	K		2.2					2.2																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131563	BOOK2000-2	Idealized compounds	Ca4Rh6Pb19	Ca4Rh6Pb19	Ca	4	Rh	6	Pb	19																			2000																												Tb4Rh6Sn19			A	14.23													ternary stannide	K		3.3					3.3																																																																																																					Handbook of superconductivity: Academic Press				Academic Press(2000)p232	Charles P.Poole Jr		
131570	SSC0230223	details not given. samples were prepared by rf-sputtering .	Ge2Ta	Ta1Ge2	Ta	1	Ge	2																					1977																										AB2																				K		2.3					2.3																																																																																																rf-sputtering at high temperature substrates					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131571	SSC0230223	details not given. samples were prepared by rf-sputtering .	Ge2Re	Re1Ge2	Re	1	Ge	2																					1977																										AB2																				K		2.7					2.7																																																																																																rf-sputtering at high temperature substrates					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131572	SSC0230223	details not given. samples were prepared by rf-sputtering .	Ge2Ti	Ti1Ge2	Ti	1	Ge	2																					1977																										AB2																				K					1.8																																																																																																		rf-sputtering at high temperature substrates					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131573	SSC0230223	details not given. samples were prepared by rf-sputtering .	Ge2V	V1Ge2	V	1	Ge	2																					1977																										AB2																				K					1.8																																																																																																		rf-sputtering at high temperature substrates					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
131574	SSC0230223	details not given. samples were prepared by rf-sputtering .	Ge2Mo	Mo1Ge2	Mo	1	Ge	2																					1977																										AB2																				K					1.8																																																																																																		rf-sputtering at high temperature substrates					Superconductivity in non-cubic crystal structures				Solid State Commun., 23(1977)223	A.K.Gosh,D.H.Douglass		
140000	1617		Ag1-xAlx	Ag0.7Al0.3	Ag	0.7	Al	0.3																					1970																																													fcc	K		0.11					0.11																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140001	1617		Ag1-xAlx	Ag0.667Al0.333	Ag	0.667	Al	0.333																					1970																																													fcc	K		0.126					0.126																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140002	1617		Ag1-xAlx	Ag0.65Al0.35	Ag	0.65	Al	0.35																					1970																																													fcc	K		0.1					0.1																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140003	1617		Ag1-xAlx	Ag0.625Al0.375	Ag	0.625	Al	0.375																					1970																																													fcc	K		0.106					0.106																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140004	1617		Ag1-xAlx	Ag0.6Al0.4	Ag	0.6	Al	0.4																					1970																																													fcc	K		0.088					0.088																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140005	1617		Ag1-xSbx	Ag0.885Sb0.115	Ag	0.885	Sb	0.115																					1970																																													fcc	K		0.019					0.019																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140006	1617		Ag1-xSbx	Ag0.865Sb0.135	Ag	0.865	Sb	0.135																					1970																																													fcc	K		0.028					0.028																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140007	1617		Ag1-xSbx	Ag0.845Sb0.155	Ag	0.845	Sb	0.155																					1970																																													fcc	K		0.037					0.037																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140008	1617		Ag1-xSnx	Ag0.845Sn0.155	Ag	0.845	Sn	0.155																					1970																																														K		0.025					0.025																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140009	1617		Ag1-xSnx	Ag0.835Sn0.165	Ag	0.835	Sn	0.165																					1970																																														K		0.047					0.047																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140010	1617		Ag1-xSnx	Ag0.825Sn0.175	Ag	0.825	Sn	0.175																					1970																																														K		0.055					0.055																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140011	1617		Ag1-xSnx	Ag0.82Sn0.18	Ag	0.82	Sn	0.18																					1970																																														K		0.066					0.066																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140012	1617		Ag1-xSnx	Ag0.815Sn0.185	Ag	0.815	Sn	0.185																					1970																																														K		0.06					0.06																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140013	1617		Ag1-xSnx	Ag0.795Sn0.205	Ag	0.795	Sn	0.205																					1970																																														K		0.09					0.09																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140014	1617		Ag1-xSnx	Ag0.775Sn0.225	Ag	0.775	Sn	0.225																					1970																																														K		0.09					0.09																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140015	1617		Cu1-xGex	Cu0.86Ge0.14	Cu	0.86	Ge	0.14																					1970																																														K		0.025					0.025																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140016	1617		Cu1-xGex	Cu0.85Ge0.15	Cu	0.85	Ge	0.15																					1970																																														K		0.084					0.084																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140017	1617		Cu1-xGex	Cu0.84Ge0.16	Cu	0.84	Ge	0.16																					1970																																														K		0.117					0.117																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140018	1617		Cu1-xGex	Cu0.83Ge0.17	Cu	0.83	Ge	0.17																					1970																																														K		0.072					0.072																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140019	1617		Cu1-xGex	Cu0.825Ge0.175	Cu	0.825	Ge	0.175																					1970																																														K		0.145					0.145																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140020	1617		Cu1-xGex	Cu0.82Ge0.18	Cu	0.82	Ge	0.18																					1970																																														K		0.13					0.13																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140021	1617		Cu1-xGex	Cu0.815Ge0.185	Cu	0.815	Ge	0.185																					1970																																														K		0.175					0.175																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140022	1617		Cu1-xGex	Cu0.81Ge0.19	Cu	0.81	Ge	0.19																					1970																																														K		0.24					0.24																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140023	1617		Cu1-xSix	Cu0.86Si0.14	Cu	0.86	Si	0.14																					1970																																														K		0.05					0.05																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140024	1617		Au1-xSnx	Au0.885Sn0.115	Au	0.885	Sn	0.115																					1970																																														K		0.21					0.21																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140025	1617		Au1-xSnx	Au0.875Sn0.125	Au	0.875	Sn	0.125																					1970																																														K		0.33					0.33																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140026	1617		Au1-xSnx	Au0.865Sn0.135	Au	0.865	Sn	0.135																					1970																																														K		0.435					0.435																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140027	1617		Au1-xSnx	Au0.855Sn0.145	Au	0.855	Sn	0.145																					1970																																														K		0.43					0.43																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140028	1617		Au1-xSnx	Au0.845Sn0.155	Au	0.845	Sn	0.155																					1970																																														K		0.53					0.53																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140029	1617		Au1-xSnx	Au0.835Sn0.165	Au	0.835	Sn	0.165																					1970																																														K		0.59					0.59																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140030	1617		Au1-xInx	Au0.84In0.16	Au	0.84	In	0.16																					1970																																														K		0.035					0.035																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140031	1617		Au1-xInx	Au0.8In0.2	Au	0.8	In	0.2																					1970																																														K		0.28					0.28																																																																																																									PHYS.REV.B,1(1970)3002	H.L.LUO,K.ANDRES		
140032	1605	carrier = 20 E+20 /cm3	SnTe	Sn1Te1	Sn	1	Te	1																					1968																																														K		0.207					0.207																																																																																												n/cm3	2000000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140033	1605	carrier = 16.9 E+20 /cm3	SnTe	Sn1Te1	Sn	1	Te	1																					1968																																														K		0.168					0.168																																																																																												n/cm3	1690000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140034	1605	carrier = 12.8 E+20 /cm3	SnTe	Sn1Te1	Sn	1	Te	1																					1968																																														K		0.1					0.1																																																																																												n/cm3	1280000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140035	1605	carrier = 10.5 E+20 /cm3	SnTe	Sn1Te1	Sn	1	Te	1																					1968																																														K		0.065					0.065																																																																																												n/cm3	1050000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140036	1605	carrier = 13.4 E+20 /cm3	SnxTe	Sn0.965Te1	Sn	0.965	Te	1																					1968																																														K		0.168					0.168																																																																																												n/cm3	1340000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140037	1605	carrier = 11.7 E+20 /cm3	SnxTe	Sn0.975Te1	Sn	0.975	Te	1																					1968																																														K		0.165					0.165																																																																																												n/cm3	1170000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140038	1605	carrier = 17.9 E+20 /cm3	SnxTe	Sn0.966Te1	Sn	0.966	Te	1																					1968																																														K		0.167					0.167																																																																																												n/cm3	1790000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140039	1605	carrier = 12.1 E+20 /cm3	SnxTe	Sn0.976Te1	Sn	0.976	Te	1																					1968																																														K		0.125					0.125																																																																																												n/cm3	1790000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140040	1605	carrier = 14.8 E+20 /cm3	SnxTe	Sn0.97Te1	Sn	0.97	Te	1																					1968																																														K		0.155					0.155																																																																																												n/cm3	1480000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140041	1605	carrier = 10.5 E+20 /cm3	SnxTe	Sn0.98Te1	Sn	0.98	Te	1																					1968																																														K		0.092					0.092																																																																																												n/cm3	1050000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140042	1605	carrier = 6.75 E+20 /cm3	SnxTe	Sn0.985Te1	Sn	0.985	Te	1																					1968																																														K		0.0485					0.0485																																																																																												n/cm3	675000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140043	1605	carrier = 6.75 E+20 /cm3	SnxTe	Sn0.985Te1	Sn	0.985	Te	1																					1968																																														K		0.0433					0.0433																																																																																												n/cm3	675000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140044	1605	carrier = 7.64 E+20 /cm3	SnxTe	Sn0.985Te1	Sn	0.985	Te	1																					1968																																														K		0.048					0.048																																																																																												n/cm3	764000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140045	1605	carrier = 5.06 E+20 /cm3	SnxTe	Sn0.99Te1	Sn	0.99	Te	1																					1968																																														K		0.0285					0.0285																																																																																												n/cm3	506000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140046	1605	carrier = 4.63 E+20 /cm3	SnxTe	Sn0.99Te1	Sn	0.99	Te	1																					1968																																														K		0.024					0.024																																																																																												n/cm3	463000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140047	1605	carrier = 2.98 E+20 /cm3	SnxTe	Sn0.995Te1	Sn	0.995	Te	1																					1968																																														K		0.0138					0.0138																																																																																												n/cm3	298000000000000000000												PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140048	1605	carrier = 13.3 E+20 /cm3	Sn(As,Te)	Sn0.97As0.005Te0.995	Sn	0.97	As	0.005	Te	0.995																			1968																																														K		0.108					0.108																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140049	1605	carrier = 10.9 E+20 /cm3	Sn(As,Te)	Sn0.97As0.01Te0.99	Sn	0.97	As	0.01	Te	0.99																			1968																																														K		0.073					0.073																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140050	1605	carrier = 8.03 E+20 /cm3	Sn(As,Te)	Sn0.97As0.015Te0.985	Sn	0.97	As	0.015	Te	0.985																			1968																																														K		0.051					0.051																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140051	1605	carrier = 7.52 E+20 /cm3	Sn(As,Te)	Sn0.97As0.017Te0.983	Sn	0.97	As	0.017	Te	0.983																			1968																																														K		0.058					0.058																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140052	1605	carrier = 5.9 E+20 /cm3	Sn(As,Te)	Sn0.97As0.02Te0.98	Sn	0.97	As	0.02	Te	0.98																			1968																																														K		0.0318					0.0318																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140053	1605	carrier = 5.08 E+20 /cm3	Sn(As,Te)	Sn0.97As0.022Te0.978	Sn	0.97	As	0.022	Te	0.978																			1968																																														K		0.0332					0.0332																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140054	1605	carrier = 4.02 E+20 /cm3	Sn(As,Te)	Sn0.97As0.025Te0.975	Sn	0.97	As	0.025	Te	0.975																			1968																																														K		0.0138					0.0138																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140055	1605	carrier = 10.4 E+20 /cm3	Sn(As,Te)	Sn0.97As0.005Te0.995	Sn	0.97	As	0.005	Te	0.995																			1968																																														K		0.068					0.068																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140056	1605	carrier = 7.0 E+20 /cm3	Sn(As,Te)	Sn0.97As0.006Te0.994	Sn	0.97	As	0.006	Te	0.994																			1968																																														K		0.048					0.048																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140057	1605	carrier = 6.83 E+20 /cm3	Sn(As,Te)	Sn0.97As0.007Te0.993	Sn	0.97	As	0.007	Te	0.993																			1968																																														K		0.038					0.038																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140058	1605	carrier =5.13  E+20 /cm3	Sn(As,Te)	Sn0.97As0.008Te0.992	Sn	0.97	As	0.008	Te	0.992																			1968																																														K		0.022					0.022																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140059	1605	carrier = 3.53 E+20 /cm3	Sn(As,Te)	Sn0.97As0.009Te0.991	Sn	0.97	As	0.009	Te	0.991																			1968																																														K		0.0195					0.0195																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140060	1605	carrier = 3.65 E+20 /cm3	Sn(As,Te)	Sn0.97As0.01Te0.99	Sn	0.97	As	0.01	Te	0.99																			1968																																														K		0.023					0.023																																																																																																									PHYS.REV.,169(1968)388	C.K.JONES,D.W.DEIS,H.A.FAIRBANK,J.K.HULM,P.A.LAWLESS		
140061	598	99.995 purity. Tc for samples with dilute elements of Ti,V,Cr,Mn,Fe,Ni,X were investigated	Al	Al1	Al	1																							1966																																														K		1.18					1.18																																																																																																					EFFECT OF TRANSITION-METAL IMPURITIES ON THE CRITICAL TEMPERATURE OF SUOERCONDUCTING AL,ZN,IN,AND SN				PHYS.REV.,148(1966)353	C.RIZZUTO,G.BOATO,G.GALLINARO		
140062	598	99.995 purity. Tc for samples with dilute elements of Ti,V,Cr,Mn,Fe,Ni,X were investigated	Zn	Zn1	Zn	1																							1966																																														K		0.85					0.85																																																																																																					EFFECT OF TRANSITION-METAL IMPURITIES ON THE CRITICAL TEMPERATURE OF SUOERCONDUCTING AL,ZN,IN,AND SN				PHYS.REV.,148(1966)353	C.RIZZUTO,G.BOATO,G.GALLINARO		
140063	598	99.999 purity. Tc for samples with dilute elements of Ti,V,Cr,Mn,Fe,Ni,X were investigated	In	In1	In	1																							1966																																														K		4.405					4.405																																																																																																					EFFECT OF TRANSITION-METAL IMPURITIES ON THE CRITICAL TEMPERATURE OF SUOERCONDUCTING AL,ZN,IN,AND SN				PHYS.REV.,148(1966)353	C.RIZZUTO,G.BOATO,G.GALLINARO		
140064	598	99.9995 purity. Tc for samples with dilute elements of Ti,V,Cr,Mn,Fe,Ni,X were investigated	Sn	Sn1	Sn	1																							1966																																														K		3.71					3.71																																																																																																					EFFECT OF TRANSITION-METAL IMPURITIES ON THE CRITICAL TEMPERATURE OF SUOERCONDUCTING AL,ZN,IN,AND SN				PHYS.REV.,148(1966)353	C.RIZZUTO,G.BOATO,G.GALLINARO		
140065	037		CoSi2	Co1Si2	Co	1	Si	2																					1953																																														K		1.3					1.3																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140066	037		NiSi2	Ni1Si2	Ni	1	Si	2																					1953																																														K					1																																																																																																							TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140067	037		AuAl2	Al2Au1	Al	2	Au	1																					1953																																														K					1																																																																																																							TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140068	037		PtAl2	Al2Pt1	Al	2	Pt	1																					1953																																														K					1																																																																																																							TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140069	037		Rh3Ge2	Ge2Rh3	Ge	2	Rh	3																					1953																																														K		2.12					2.12																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140070	037		IrGe	Ge1Ir1	Ge	1	Ir	1																					1953																												MnP																		K		4.7					4.7																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140071	037		PdSb	Pd1Sb1	Pd	1	Sb	1																					1953																												NiAs																		K		1.5					1.5																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140072	037		PtSb	Pt1Sb1	Pt	1	Sb	1																					1953																												NiAs																		K		2.1					2.1																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140073	37		PtBi	Bi1Pt1	Bi	1	Pt	1																					1953																												Fe3Zn10			A	4.31		5.49											Fe3Zn10, D8[1]	K		1.21					1.21																																																																																																					Transition temperatures of superconductors				Phys.Rev., 92(1953)874	B.T.Matthias		
140074	037		PdTe	Pd1Te1	Pd	1	Te	1																					1953																												Fe3Zn10																	Fe3Zn10, D8[1]	K		2.3					2.3																																																																																																					TRANSITION TEMPERATURES OF SUPERCONDUCTORS				PHYS.REV.,92(1953)874	B.T.MATTHIAS		
140075	1564	gamma in mj/gat.K2.	fcc-La	La1	La	1																							1973																															A	5.29													fcc	K		6.06					6.06																																																								mj/mol.K2	11.3		139																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140076	1564	gamma in mj/gat.K2. delta-C/gamma*Tc = 2.9. dHc/dT = -512 Oe/K	La3In	In1La3	In	1	La	3																					1973																															A	5.07														K		9.54					9.54																																																5.8								mj/mol.K2	14		170																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140077	1564	gamma in mj/gat.K2. delta-C/gamma*Tc = 2.4. dHc/dT = -440 Oe/K	La3Tl	La3Tl1	La	3	Tl	1																					1973																															A	5.06														K		8.86					8.86																																																5.3								mj/mol.K2	12.4		163																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140078	1564	gamma in mj/gat.K2.	La3(In,Ga)	La3In0.7Ga0.3	La	3	In	0.7	Ga	0.3																			1973																															A	5.05														K		9.25					9.25																																																								mj/mol.K2	10.6		170																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140079	1564	not s/c	La3AlC	La3Al1C1	La	3	Al	1	C	1																			1973																															A	5.12														K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140080	1564	not s/c	La3GaC	La3Ga1C1	La	3	Ga	1	C	1																			1973																															A	5.17														K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140081	1564	not s/c. gamma in mj/gat.K2.	La3InC	La3In1C1	La	3	In	1	C	1																			1973																															A	5.19														K					1.02																																																										mj/mol.K2	5.9		203																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140082	1564	not s/c	La3TlC	La3Tl1C1	La	3	Tl	1	C	1																			1973																															A	5.2														K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140083	1564	not s/c	La3SnC	La3Sn1C1	La	3	Sn	1	C	1																			1973																															A	5.18														K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140084	1564	not s/c	La3PbC	La3Pb1C1	La	3	Pb	1	C	1																			1973																															A	5.2														K					1.02																																																																																																							Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140085	1564		La3(In,Tl)	La3In0.5Tl0.5	La	3	In	0.5	Tl	0.5																			1973																															A	5.06														K		8.9					8.9																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140086	1564		La3(In,Al)	La3In0.7Al0.3	La	3	In	0.7	Al	0.3																			1973																															A	5.06														K		9.42					9.42																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140087	1564	gamma in mj/gat.K2.	La3(In,Ga)	La3In0.7Ga0.3	La	3	In	0.7	Ga	0.3																			1973																															A	5.05														K		9.25					9.25																																																								mj/mol.K2	10.6		170																																										Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140088	1564		La3(In,Sn)	La3In0.8Sn0.2	La	3	In	0.8	Sn	0.2																			1973																															A	5.05														K		7.8					7.8																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140089	1564		La3(In,Cd)	La3In0.9Cd0.1	La	3	In	0.9	Cd	0.1																			1973																															A	5.07														K		9.55					9.55																																																																																																					Superconducting and other electronic properties of La3In, La3Tl, and some related phases				PHYS.REV.B,8(1973)3194	E.BUCHER,F.HEINIGER,J.P.MAITA,P.DESCOUTS		
140090	1006		NbC	C1Nb1	C	1	Nb	1																					1967																															A	4.468														K		11.2					11.2																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140091	1006		(Nb,Mo)C	Nb0.75Mo0.25C1	Nb	0.75	Mo	0.25	C	1																			1967																															A	4.451														K		12					12																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140092	1006		(Nb,Mo)C	Nb0.5Mo0.5C1	Nb	0.5	Mo	0.5	C	1																			1967																															A	4.41														K		13.1					13.1																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140093	1006		(Nb,Mo)C	Nb0.25Mo0.75C1	Nb	0.25	Mo	0.75	C	1																			1967																															A	4.358														K		13.1					13.1																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140094	1006		(Nb,Mo)C	Nb0.05Mo0.95C1	Nb	0.05	Mo	0.95	C	1																			1967																															A	4.296														K		13.5					13.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140095	1006		MoC	C1Mo1	C	1	Mo	1																					1967																															A	4.277														K		14.3					14.3																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140096	1006		(Nb,W)C	Nb0.9W0.1C1	Nb	0.9	W	0.1	C	1																			1967																															A	4.457														K		11.6					11.6																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140097	1006		(Nb,W)C	Nb0.8W0.2C1	Nb	0.8	W	0.2	C	1																			1967																															A	4.445														K		13.7					13.7																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140098	1006		(Nb,W)C	Nb0.75W0.25C1	Nb	0.75	W	0.25	C	1																			1967																															A	4.443														K		13.1					13.1																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140099	1006		(Nb,W)C	Nb0.7W0.3C1	Nb	0.7	W	0.3	C	1																			1967																															A	4.434														K		13.2					13.2																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140100	1006		(Nb,W)C	Nb0.65W0.35C1	Nb	0.65	W	0.35	C	1																			1967																															A	4.425														K		13					13																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140101	1006		(Nb,W)C	Nb0.5W0.5C1	Nb	0.5	W	0.5	C	1																			1967																															A	4.404														K		12.5					12.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140102	1006		(Nb,W)C	Nb0.2W0.8C1	Nb	0.2	W	0.8	C	1																			1967																															A	4.335														K		11					11																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140103	1006		WC	C1W1	C	1	W	1																					1967																															A	4.265														K		9.93					9.93																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140104	1006		(Nb,Ta)C	Nb0.8Ta0.2C1	Nb	0.8	Ta	0.2	C	1																			1967																															A	4.467														K		10					10																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140105	1006		(Nb,Ta)C	Nb0.6Ta0.4C1	Nb	0.6	Ta	0.4	C	1																			1967																															A	4.466														K		9.4					9.4																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140106	1006		(Nb,Ta)C	Nb0.4Ta0.6C1	Nb	0.4	Ta	0.6	C	1																			1967																															A	4.459														K		9.33					9.33																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140107	1006		(Nb,Ta)C	Nb0.2Ta0.8C1	Nb	0.2	Ta	0.8	C	1																			1967																															A	4.456														K		9					9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140108	1006		(Mo,W)C	Mo0.9W0.1C1	Mo	0.9	W	0.1	C	1																			1967																															A	4.276														K		11.7					11.7																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140109	1006		(Mo,W)C	Mo0.8W0.2C1	Mo	0.8	W	0.2	C	1																			1967																															A	4.271														K		12					12																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140110	1006		(Mo,W)C	Mo0.6W0.4C1	Mo	0.6	W	0.4	C	1																			1967																															A	4.268														K		11.3					11.3																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140111	1006		(Mo,W)C	Mo0.4W0.6C1	Mo	0.4	W	0.6	C	1																			1967																															A	4.262														K		11.3					11.3																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140112	1006		(Mo,W)C	Mo0.2W0.8C1	Mo	0.2	W	0.8	C	1																			1967																															A	4.26														K		10.1					10.1																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140113	1006		(Mo,W)C	Mo0.1W0.9C1	Mo	0.1	W	0.9	C	1																			1967																																														K		9					9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140114	1006		TaC	C1Ta1	C	1	Ta	1																					1967																															A	4.456														K		10					10																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140115	1006		(Ta,Mo)C	Ta0.8Mo0.2C1	Ta	0.8	Mo	0.2	C	1																			1967																															A	4.445														K		8.5					8.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140116	1006		(Ta,Mo)C	Ta0.6Mo0.4C1	Ta	0.6	Mo	0.4	C	1																			1967																															A	4.438														K		8.67					8.67																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140117	1006		(Ta,Mo)C	Ta0.4Mo0.6C1	Ta	0.4	Mo	0.6	C	1																			1967																															A	4.416														K		9.18					9.18																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140118	1006		(Ta,Mo)C	Ta0.2Mo0.8C1	Ta	0.2	Mo	0.8	C	1																			1967																															A	4.329														K		10.5					10.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140119	1006		(Ta,Mo)C	Ta0.05Mo0.95C1	Ta	0.05	Mo	0.95	C	1																			1967																															A	4.286														K		11.8					11.8																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140120	1006		(Ta,W)C	Ta0.8W0.2C1	Ta	0.8	W	0.2	C	1																			1967																															A	4.441														K		9.92					9.92																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140121	1006		(Ta,W)C	Ta0.6W0.4C1	Ta	0.6	W	0.4	C	1																			1967																															A	4.432														K		10					10																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140122	1006		(Ta,W)C	Ta0.4W0.6C1	Ta	0.4	W	0.6	C	1																			1967																															A	4.403														K		9.41					9.41																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140123	1006		(Ta,W)C	Ta0.2W0.8C1	Ta	0.2	W	0.8	C	1																			1967																															A	4.32														K		8.96					8.96																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140124	1006		(Mo,V)C	Mo0.95V0.05C1	Mo	0.95	V	0.05	C	1																			1967																																														K		13.9					13.9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140125	1006		(Mo,Ti)C	Mo0.95Ti0.05C1	Mo	0.95	Ti	0.05	C	1																			1967																																														K		13.5					13.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140126	1006		(Mo,Zr)C	Mo0.95Zr0.05C1	Mo	0.95	Zr	0.05	C	1																			1967																																														K		13.2					13.2																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140127	1006		(Mo,Hf)C	Mo0.95Hf0.05C1	Mo	0.95	Hf	0.05	C	1																			1967																																														K		12.7					12.7																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140128	1006		(Mo,Re)C	Mo0.9Re0.1C1	Mo	0.9	Re	0.1	C	1																			1967																																														K		13.9					13.9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140129	1006		(Mo,Ru)C	Mo0.9Ru0.1C1	Mo	0.9	Ru	0.1	C	1																			1967																																														K		13.7					13.7																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140130	1006		(Mo,V)C	Mo0.9V0.1C1	Mo	0.9	V	0.1	C	1																			1967																																														K		13.3					13.3																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140131	1006		(Mo,Ti)C	Mo0.9Ti0.1C1	Mo	0.9	Ti	0.1	C	1																			1967																																														K		13.1					13.1																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140132	1006		(Mo,Hf)C	Mo0.9Hf0.1C1	Mo	0.9	Hf	0.1	C	1																			1967																																														K		11.9					11.9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140133	1006		(Mo,Zr)C	Mo0.9Zr0.1C1	Mo	0.9	Zr	0.1	C	1																			1967																																														K		11.5					11.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140134	1006		(Mo,V)C	Mo0.84V0.16C1	Mo	0.84	V	0.16	C	1																			1967																																														K		12.9					12.9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140135	1006		(Mo,Ti)C	Mo0.84Ti0.16C1	Mo	0.84	Ti	0.16	C	1																			1967																																														K		12.8					12.8																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140136	1006		(Mo,Hf)C	Mo0.84Hf0.16C1	Mo	0.84	Hf	0.16	C	1																			1967																																														K		11.5					11.5																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140137	1006		(Mo,Zr)C	Mo0.84Zr0.16C1	Mo	0.84	Zr	0.16	C	1																			1967																																														K		11					11																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140138	1006		(Mo,V)C	Mo0.8V0.2C1	Mo	0.8	V	0.2	C	1																			1967																																														K		12.8					12.8																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140139	1006		(Mo,Ti)C	Mo0.8Ti0.2C1	Mo	0.8	Ti	0.2	C	1																			1967																																														K		12					12																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140140	1006		(Mo,Hf)C	Mo0.8Hf0.2C1	Mo	0.8	Hf	0.2	C	1																			1967																																														K		11.4					11.4																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140141	1006		(Mo,Zr)C	Mo0.8Zr0.2C1	Mo	0.8	Zr	0.2	C	1																			1967																																														K		10.9					10.9																																																																																																					Superconductivity of the transition-metal carbides				PHYS.REV.,159(1967)327	B.T.MATTHIAS,E.BUEHLER,R.H.WILLENS		
140142	032		Zr1-xAux	Au0.12Zr0.88	Au	0.12	Zr	0.88																					1955																																														K		2.78					2.78																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140143	032		Zr1-xAux	Au0.1Zr0.9	Au	0.1	Zr	0.9																					1955																																														K		2.78					2.78																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140144	032		Zr1-xAux	Au0.07Zr0.93	Au	0.07	Zr	0.93																					1955																																														K		2.52					2.52																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140145	032		Zr1-xAux	Au0.05Zr0.95	Au	0.05	Zr	0.95																					1955																																														K		1.79					1.79																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140146	032		Zr1-xOsx	Os0.01Zr0.99	Os	0.01	Zr	0.99																					1955																																														K		1.52					1.52																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140147	032		Zr1-xOsx	Os0.025Zr0.975	Os	0.025	Zr	0.975																					1955																																														K		2.97					2.97																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140148	032		Zr1-xOsx	Os0.05Zr0.95	Os	0.05	Zr	0.95																					1955																																														K		5.38					5.38																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140149	032		Zr1-xOsx	Os0.06Zr0.94	Os	0.06	Zr	0.94																					1955																																														K		5.7					5.7																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140150	032		Zr1-xOsx	Os0.07Zr0.93	Os	0.07	Zr	0.93																					1955																																														K		5.66					5.66																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140151	032		Zr1-xOsx	Os0.1Zr0.9	Os	0.1	Zr	0.9																					1955																																														K		5.17					5.17																																																																																																					Superconductivity of zirconium alloys				PHYS.REV.,100(1955)626	B.T.MATTHIAS,E.CORENZWIT		
140152	1643		TexAu1-x	Au0.374Te0.626	Au	0.374	Te	0.626																					1969																															A	2.9514														K		1.3					1.3																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140153	1643	thermopower = -5.13 uV/K	TexAu1-x	Au0.35Te0.65	Au	0.35	Te	0.65																					1969																																														K		1.58					1.58																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140154	1643	thermopower = -5.89 uV/K	TexAu1-x	Au0.332Te0.668	Au	0.332	Te	0.668																					1969																															A	2.9667														K		1.89					1.89																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140155	1643	thermopower = -8.57 uV/K	TexAu1-x	Au0.3Te0.7	Au	0.3	Te	0.7																					1969																															A	2.9928														K		1.99					1.99																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140156	1643	thermopower = -5.32 uV/K	TexAu1-x	Au0.28Te0.72	Au	0.28	Te	0.72																					1969																															A	3.0007														K		1.96					1.96																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140157	1643	thermopower = -2.26uV/K	TexAu1-x	Au0.25Te0.75	Au	0.25	Te	0.75																					1969																															A	3.0355														K		1.85					1.85																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140158	1643	thermopower = +1.85 uV/K	TexAu1-x	Au0.24Te0.76	Au	0.24	Te	0.76																					1969																																														K		1.72					1.72																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140159	1643	thermopower = +4.24 uV/K	TexAu1-x	Au0.22Te0.78	Au	0.22	Te	0.78																					1969																															A	3.0493														K		1.54					1.54																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140160	1643	thermopower = +5.00 uV/K	TexAu1-x	Au0.2Te0.8	Au	0.2	Te	0.8																					1969																															A	3.0558														K		1.48					1.48																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140161	1643	thermopower = +8.44 uV/K	TexAu1-x	Au0.18Te0.82	Au	0.18	Te	0.82																					1969																															A	3.0841														K		1.56					1.56																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140162	1643		TexAu1-x	Au0.16Te0.84	Au	0.16	Te	0.84																					1969																																														K		1.71					1.71																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140163	1643	thermopower = +17.3 uV/K	TexAu1-x	Au0.15Te0.85	Au	0.15	Te	0.85																					1969																															A	3.0978														K		1.64					1.64																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140164	1643		TexAu1-x	Au0.14Te0.86	Au	0.14	Te	0.86																					1969																																														K		1.7					1.7																																																																																																					Fermi-surface-Brillouin-zone interaction in simple cubic Te-Au alloys				PHYS.REV.,183(1969)619	C.C.TSUEI,L.R.NEWKIRK		
140165	036		Sn1-xBix	Bi0.02Sn0.98	Bi	0.02	Sn	0.98																					1953																																														K		3.85					3.85											Oe		297																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140166	036		Sn1-xBix	Bi0.04Sn0.96	Bi	0.04	Sn	0.96																					1953																																														K		3.86					3.86											Oe		325																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140167	036		Sn1-xBix	Bi0.045Sn0.955	Bi	0.045	Sn	0.955																					1953																																														K		3.88					3.88											Oe		310																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140168	036		Sn1-xBix	Bi0.05Sn0.95	Bi	0.05	Sn	0.95																					1953																																														K		3.93					3.93											Oe		282																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140169	036		Sn1-xBix	Bi0.055Sn0.945	Bi	0.055	Sn	0.945																					1953																																														K		3.94					3.94											Oe		274																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140170	036		Sn1-xBix	Bi0.06Sn0.94	Bi	0.06	Sn	0.94																					1953																																														K		4.1					4.1											Oe		200																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140171	036		Sn1-xBix	Bi0.08Sn0.92	Bi	0.08	Sn	0.92																					1953																																														K		4.15					4.15											Oe		228																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140172	036		Sn1-xBix	Bi0.1Sn0.9	Bi	0.1	Sn	0.9																					1953																																														K		4.18					4.18											Oe		251																																																																																			melt(135C), then quench to liq. air					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140173	036		Sn1-xSbx	Sb0.02Sn0.98	Sb	0.02	Sn	0.98																					1953																																														K		2.64					2.64											Oe		304																																																																																			melt(225C), then quench to dry ice.					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140174	036		Sn1-xSbx	Sb0.04Sn0.96	Sb	0.04	Sn	0.96																					1953																																														K		3.76					3.76											Oe		345																																																																																			melt(225C), then quench to dry ice.					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140175	036		Sn1-xSbx	Sb0.06Sn0.94	Sb	0.06	Sn	0.94																					1953																																														K		3.96					3.96											Oe		321																																																																																			melt(225C), then quench to dry ice.					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140176	036		Sn1-xSbx	Sb0.08Sn0.92	Sb	0.08	Sn	0.92																					1953																																														K		3.89					3.89											Oe		330																																																																																			melt(225C), then quench to dry ice.					SUPERCONDUCTIVITY IN TIN-BISMUTH AND TIN-ANTIMONY ALLOYS				PHYS.REV.,92(1953)238	W.F.LOVE		
140177	1904	amorphous Ga film	amorphous-Ga	Ga1	Ga	1																						4	1975																																														K		7.84					7.84																																																																																																amorphous film obtained by sputtering at 77K in Ar									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140178	1904	amorphous Ga-Sb film	a-(Ga,Sb)	Ga0.8Sb0.2	Ga	0.8	Sb	0.2																				4	1975																																														K		6.18					6.18	MTC140178																																																																																															amorphous film obtained by sputtering at 77K in Ar									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140179	1904	amorphous Ga-Sb film	a-(Ga,Sb)	Ga0.58Sb0.42	Ga	0.58	Sb	0.42																				4	1975																																														K		1.17					1.17																																																																																																amorphous film obtained by sputtering at 77K in Ar									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140180	1904	amorphous Bi film	amorphous-Bi	Bi1	Bi	1																						4	1975																																														K		5.7					5.7																																																																																																amorphous film obtained by sputtering at 77K in Ar-H atmosphere									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140181	1904	amorphous Bi-Sb film	a-(Bi,Sb)	Bi0.9Sb0.1	Bi	0.9	Sb	0.1																				4	1975																																														K		5.2					5.2	MTC140181																																																																																															amorphous film obtained by sputtering at 77K in Ar-H atmosphere									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140182	1904	amorphous Bi-Sb film	a-(Bi,Sb)	Bi0.7Sb0.3	Bi	0.7	Sb	0.3																				4	1975																																														K		4.14					4.14																																																																																																amorphous film obtained by sputtering at 77K in Ar-H atmosphere									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140183	1904	amorphous Bi-Sb film	a-(Bi,Sb)	Bi0.5Sb0.5	Bi	0.5	Sb	0.5																				4	1975																																														K		2.94					2.94																																																																																																amorphous film obtained by sputtering at 77K in Ar-H atmosphere									PHYS.REV.B,11(1975)738	J.J.HAUSER		
140184	736		Pb1-xTlx	Pb0.52Tl0.48	Pb	0.52	Tl	0.48																					1966																																														K		5.54					5.54	MTC40184																																																																																																				Superconductivity and electronic structure in the alloy system lead-thallium				PHYS.REV.,147(1966)340	T.CLAESON		
140185	736		Pb1-xTlx	Pb0.06Tl0.94	Pb	0.06	Tl	0.94																					1966																																														K		2.7					2.7																																																																																																					Superconductivity and electronic structure in the alloy system lead-thallium				PHYS.REV.,147(1966)340	T.CLAESON		
140186	736		Bi1-xTlx	Bi0.6Tl0.4	Bi	0.6	Tl	0.4																					1966																																														K		6					6	MTC40186																																																																																																				Superconductivity and electronic structure in the alloy system lead-thallium				PHYS.REV.,147(1966)340	T.CLAESON		
140187	JPS0410026		(Ce,Pr)Ru2	Ce0.9Pr0.1Ru2	Ce	0.9	Pr	0.1	Ru	2																		1	1976																												Laves																	Laves, C15	K		6.55					6.55																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
140188	JPS0410026		(Ce,Pr)Ru2	Ce0.8Pr0.2Ru2	Ce	0.8	Pr	0.2	Ru	2																		1	1976																												Laves																	Laves, C15	K		5.82					5.82																																																																																																					Superconducting and ferromagnetic properties of PrxCe1-xRu2				J.Phys.Soc.Jpn, 41(1976)26	Yuji Asada		
148246	SST031065001	e-ph = 0.73. DOS = 4.14 states/eV. T<CDW> = 70.1 K from R(T) anomaly. GL(kappa) = 45.	2H-PdxTaS2	Pd0.04Ta1S2	Pd	0.04	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3148		12.1287											hexagonal , distorted 2H-structure	K			4.22	4.2			4.2	MPH158246										Oe	M-H curve, GL approx.	102							T	RES(0.5Rn), GL approx.	10.9												MHC158246		nm	from Hc2	5.5			nm	from Hc1	248										MSP158246			mJ/mol.K2	16.86	SP	208.5	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
150000	NAT3340510	compositions determined by EPME, ICP. O-content by non-dispersive infrared inert gas fusion method.	TlBa2Ca3Cu4O11	Tl1Ba2Ca3Cu4O11	Tl	1	Ba	2	Ca	3	Cu	4													O	11			1988																												Tl1234			A	3.85		19.1												K	120.4	122.1	126.6	122			122.1																																																																																														Tl2O3,CaO,BaO2,BaCu3O4	1	mixture - pellet - fire(1163K,10min, in flowing O2) - Q to RT(100C/h)					A new high-Tc TlBa2Ca3Cu4O11 superconductor with Tc > 120 K			Electronical Laboratory, 1-1-4 Umezono, Tsukuba, Ibaraki 305, Japan	Nature,  334(1988)510	H.Ihara,R.Sugise,M.Hirabayashi,N.Terada,M.Jo,K.Hayashi,A.Negishi,M.Tokumoto,Y.Kimura,T.Shimomura		
150001	SST0170423	As-synthesized. O-content by weight change. Hirr(77K) = 3.60 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O11.18	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	11.18	1	2004																												(Cu,C)1234			A	3.8569		17.955												K				117.5			117.5																																																																																														BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150002	SST0170423	ANN(300C,in N2). O-content by weight change. Hirr(77K) = 3.95 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.77	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.77	1	2004																												(Cu,C)1234			A	3.8564		17.952												K				116.7			116.7																																																																																														BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150003	SST0170423	ANN(400C,in N2). O-content by weight change. Hirr(77K) = 3.95 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.69	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.69	1	2004																												(Cu,C)1234			A	3.8569		17.956												K				116.3			116.3	TC150003																																																																																													BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150004	SST0170423	ANN(450C,in N2). O-content by weight change. Hirr(77K) = 4.00 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.66	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.66	1	2004																												(Cu,C)1234			A	3.8572		17.962												K				115.7			115.7																																																																																														BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150005	SST0170423	ANN(500C,in N2). O-content by weight change. Hirr(77K) = 4.60 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.57	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.57	1	2004																												(Cu,C)1234			A	3.8592		17.986												K				115.1			115.1																																		HIR150005																																																												BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150006	SST0170423	ANN(550C,in N2). O-content by weight change. Hirr(77K) = 1.66 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.45	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.45	1	2004																												(Cu,C)1234			A	3.8596		18.001												K				114.3			114.3																																																																																														BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150007	SST0170423	ANN(600C,in N2). O-content by weight change. Hirr(77K) = 1.20 T.	(Cu,C)Ba2Ca3Cu4Oz	C0.3Ba2Ca4Cu5.7O10.34	C	0.3	Ba	2	Ca	4	Cu	5.7													O	z	10.34	1	2004																												(Cu,C)1234			A	3.8609		18.003												K				113.5			113.5																																		HIR150005																																																												BaO2,CaCO3,Ca2CuO3,CuO,Cu2O		mixture - pellet - into Au-capsule - high pressure synthesis(3.5GPa,1000C,2h)					Anomalous behaviour of irreversibility lines in multi-layered superconductor (Cu, C)Ba2Ca3Cu4Oy			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, 2641 Yamazaki, Noda, Chiba 278-8510, Japan	Supercond. Sci. Technol., 17(2004)423	M.Hirai,A.Iyo,Y.Kodama,A.Sundaresan,J.Arai,Y.Tanaka		
150008	PHC3080198	O-content by coulometric titration. Tc is independent of O-content for 10.09=<z=<10.35.	CuBa2Ca3Cu4O10	Ba2Ca3Cu4O10.35	Ba	2	Ca	3	Cu	4															O	10+z	10.35	1	1998																												Cu1234			A	3.856		17.93												K				116			116																																																																																														BaCuO2.13,Ca2CuO3,CuO		mixture(precursor+CuO) - into Au-capsule - high pressure synthesis(5GPa,1100-1150C,30min) ANN(500C,O2+Ar atm, in Pt-crucible)					Oxygen content in high-pressure synthesized CuBa2Cu4O10+delta (Cu1234:P) superconductor			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Physica.C,308(1998)198-202	H. Suematsu,H. Yamauchi,M. Karppinen,T. Ito		
150009	DRM0160915	B-content = 1.75 E+21 /cm3. thickness = 1.5 - 3 um. ARPES, RAMAN measured.	B-doped diamond	C1	C	1																						4	2007																												diamond																		K			2.68				2.68	MTC150009																																																																																															microwave plasma CVD (MPCVD) at 835 C.					Highly and heavily boron doped diamond films			Laboratoire d'Etudes des Proprietes Electroniques des Solides, Centre National de la Recherche Scientifique and University of Grenoble, BP 166, 38042 Grenoble Cedex 9, France	Diamond Relat. Mater., 16(2007)915	A.Deneuville,C.Baron,S.Ghodbane,C.Agnes		
150010	SST0200452	single phase for 0 < x < 0.4.	(Nb,Mg)B2	Nb0.9Mg0.1B2	Nb	0.9	Mg	0.1	B	2																		1	2007																												AlB2			A	3.1061		3.3231												K	4		5				4.5																																																																																														NbB2,MgB2,Mg		mixture(12 wt% Mg was added) - pellet - into evacuated quartz tube - SIN(1100C,3h) -FC to RT.					Synthesis and characterization of a new superconductor Nb1-xMgxB2			National Laboratory for Superconductivity, Institute of Physics and Beijing National, People's Republic of China	Supercond. Sci. Technol., 20(2007)452	H.X.Geng,G.C.Che,W.W.Huang,S.L.Jia,H.Chen,Z.X.Zhao		
150011	SST0200452	single phase for 0 < x < 0.4.	(Nb,Mg)B2	Nb0.75Mg0.25B2	Nb	0.75	Mg	0.25	B	2																		1	2007																												AlB2			A	3.1		3.3203												K	4		5				4.5																																																								mJ/mol.K2	4.509	SP-heat	419	SP-heat																																		NbB2,MgB2,Mg		mixture(12 wt% Mg was added) - pellet - into evacuated quartz tube - SIN(1100C,3h) -FC to RT.					Synthesis and characterization of a new superconductor Nb1-xMgxB2			National Laboratory for Superconductivity, Institute of Physics and Beijing National, People's Republic of China	Supercond. Sci. Technol., 20(2007)452	H.X.Geng,G.C.Che,W.W.Huang,S.L.Jia,H.Chen,Z.X.Zhao		
150012	SST0200452	not SC.	NbB2	B2Nb1	B	2	Nb	1																				1	2007																												AlB2			A	3.1151		3.2843												K					1																																																																																																NbB2,MgB2,Mg		mixture(12 wt% Mg was added) - pellet - into evacuated quartz tube - SIN(1100C,3h) -FC to RT.					Synthesis and characterization of a new superconductor Nb1-xMgxB2			National Laboratory for Superconductivity, Institute of Physics and Beijing National, People's Republic of China	Supercond. Sci. Technol., 20(2007)452	H.X.Geng,G.C.Che,W.W.Huang,S.L.Jia,H.Chen,Z.X.Zhao		
150013	MMM3100340	P-induced SC. RRR = 180 (I//a-axis). SP-heat, Tc measured at P = 1.34 GPa.	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2007																												BaNiSn3																		K		0.45			0		0.45																																																					MSP150013																		mOhm.cm												420													Czochralski method in tetra-arc furnace under Ar.					Heat capacity of CeRhSi3 under pressure			Division of Physics, Faculty of Engineering, Yokohama National University, Yokohama, Kanagawa 240-8501, Japan	J.Mag.Mag.Mater., 310(2007)340	F.Tomioka,M.Hedo,I.Umehara,T.Ono,Y.Uwatoko,N.Kimura,S.Takayanagi		
150014	JTL0800763	Tc by SUS. Tc(P=0) data from E.Yu.Tonkov. (dTc/dp) = 0.05 for alpha-phase and = 0.16 K/GPa for omega-phase (see figure)	Hf	Hf1	Hf	1																							2004																																													alpha(hcp)	K		0.128					0.128	MTC150014		K/GPa	0.05																																																																																												zone melting in vac					Superconducting transition temperature in hafnium under pressures up to 64 GPa			Institute of Solid State Physics, Russian Academy of Science, Chemogolovka, Moscow region, Russia	JETP Lett., 80(2004)763	I.O.Bashkin,M.V.Nefedova,V.G.Tissen,E.G.Ponyatovsky		
150015	P068054401	compositions by EM. (dTc/dP) = 0.11 K/GPa for omega-phase. alpha-to-omega at P=11 GPa. omega-to-beta at 47 GPa.	Ti1-xZrx	Ti0.496Zr0.504	Ti	0.496	Zr	0.504																					2003																															A	3.104		4.923											alpha(hcp)	K				1.8			1.8	MTC150015		K/GPa	0.22																																																																																																	Crystal structure and superconductivity of TiZr up to 57 GPa			Institute of Solid State Physics RAS, Chernogolovka, Moscow District, 142432, Russia	Phys.Rev.B, 68(2003)054401	I.O.Bashkin,V.K.Fedotov,M.V.Nefedova,V.G.Tissen,E.G.Ponyatovsky,A.Schiwek,W.B.Holzapfel		
150016	P075140514	second AF order temperature(27 K) was observed.	YSr2(Nb,Cu)Cu2O8	Y1Sr2Nb0.9Cu2.1O7.9	Y	1	Sr	2	Nb	0.9	Cu	2.1													O	8	7.9	1	2007								257																				M1212																		K				27			27																																																																																														Nb2O5,SrO2,SrCuO2,Cu,Y2O3		mixture - Au-capsule in sealed pipe - high pressure systhesis(1450C, 2h, 6GPa)					Antiferromagnetism and superconductivity: Cuprate plane magnetic ordering in YSr2Cu2.1Nb0.9O8-z			Department of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USA	Phys.Rev.B, 75(2007)140514R	H.A.Blackstead,W.B.Yelon,M.Kornecki,M.P.Smylie,Q.Cai,J.Lamsal,V.P.S.Awana,S.Balamurugan,E.Takayama-Muromachi		
150017	P075144507	two gap system.  TBL value is for higher one. The lower gap = 2.41 meV, (2:gap/kTc) = 1.83.	(Mg,Al)B2	Mg0.9Al0.1B2	Mg	0.9	Al	0.1	B	2																		1	2007																												AlB2																		K		30.5					30.5																																														meV	4.9	3.73	1																																															two step synthesis at high temperature. See PRB071144512					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150018	P075144507	two gap system.  TBL value is for higher one. The lower gap = 1.97 meV, (2:gap/kTc) = 1.95.	(Mg,Al)B2	Mg0.8Al0.2B2	Mg	0.8	Al	0.2	B	2																		1	2007																												AlB2																		K		23.5					23.5																																														meV	3.46	3.41	1																																															two step synthesis at high temperature. See PRB071144512					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150019	P075144507	pellet. two gap system.  TBL value is for higher one. The lower gap = 2.24 meV, (2:gap/kTc) =1.58 .	Mb(B,C)2	Mg1B1.89C0.11	Mg	1	B	1.89	C	0.11																		1	2007																												AlB2																		K		33					33																																														meV	5.03	3.52	1																																															two step synthesis at high temperature. See PRB071144512					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150020	P075144507	pellet. two gap system.  TBL value is for higher one. The lower gap = 1.92 meV, (2:gap/kTc) = 1.58.	Mb(B,C)2	Mg1B1.87C0.13	Mg	1	B	1.87	C	0.13																		1	2007																												AlB2																		K		28					28																																														meV	4.71	3.88	1																																															two step synthesis at high temperature. See PRB071144512					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150021	P075144507	pellet. two gap system.  TBL value is for higher one. The lower gap = 1.52 meV, (2:gap/kTc) =1.62 .	Mb(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		1	2007																												AlB2																		K		22					22																																														meV	3.39	3.52	1																																															two step synthesis at high temperature. See PRB071144512					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150022	P075144507	wire. two gap system.  TBL value is for higher one. The lower gap = 2.32 meV, (2:gap/kTc) =1.42 .	Mb(B,C)2	Mg1B1.958C0.042	Mg	1	B	1.958	C	0.042																		1	2007																												AlB2																		K		37.5					37.5																																														meV	6.47	3.99	1																																															See PRL092217003					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150023	P075144507	wire. two gap system.  TBL value is for higher one. The lower gap = 2.34 meV, (2:gap/kTc) = 1.49.	Mb(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																		1	2007																												AlB2																		K		36.2					36.2																																														meV	6.05	3.84	1																																															See PRL092217003					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150024	P075144507	pellet. two gap system.  TBL value is for higher one. The lower gap = 2.34 meV, (2:gap/kTc) = 1.41.	MgB2	B2Mg1	B	2	Mg	1																				1	2007																												AlB2																		K		39					39																																														meV	6.6	3.93	1																																															See PRL092217003					Point-contact spectroscopy of Al- and C-doped MgB2: Superconducting energy gaps and scattering studies			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P. J. Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 75(2007)144507	P.Szabo,P.Samuely,Z.Pribulova,M.Angst,S.Bud'ko,P.C.Canfield,J.Marcus		
150025	PHB3780892		C6Yb	C6Yb1	C	6	Yb	1																					2006																												GIC																		K				6.52			6.52	MTC150025		K/GPa	0.389																																																																																																	Positive pressure dependence of the superconducting transition temperature in C6Yb			Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, UK	Physica B 378-380(2006)892	R.P.Smith,T.E.Weller,A.F.Kusmartseva,N.T.Skipper,M.Ellerby,S.S.Saxena		
150026	PR1201964	Sn<116>, Sn<124> were used. Tc value is for Sn<116> isotope. Tc(Nb3Sn<124>) = 17.89 K.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					1960																																														K		17.93					17.93						0.08	Sn																																																																																														Isotope effect in Nb3Sn				Phys.Rev., 120(1960)1964	G.E.Devlin,E.Corenzwit		
150027	PR1201964	Sn<116>, Sn<124> were used. Tc value is for Sn<116> isotope. Tc(Sn<124>) = 3.64 K.	Sn	Sn1	Sn	1																							1960																																														K		3.77					3.77						0.46	Sn																																																																																														Isotope effect in Nb3Sn				Phys.Rev., 120(1960)1964	G.E.Devlin,E.Corenzwit		
150028	PR1210086	(dHc/dM) = -3.80 gaus/amu)	Pb	Pb1	Pb	1																							1961																																														K		7.175					7.175						0.478	Pb																																																																																														Isotope effect in superconducting lead				Phys.Rev., 121(1961)86	R.W.Shaw,D.E.Mapother,D.C.Hopkins		
150029	PR1121522	M = 207.27. (dHc/dT) M   = 240 gaus. (dHc/dM)T  = -4.17 gaus/amu. Hc shows Hc(type-I) for M=206.54 sample.	Pb	Pb1	Pb	1																							1958																																														K		7.175					7.175						0.501	Pb													Oe		815																																																																															Isotope effect on the superconducting transition in lead				Phys.Rev., 112(1958)1522	R.R.Hake,D.E.Mapother,D.L.Decker		
150030	PR1121888	Hc2 shows Hc(type-I).	Pb	Pb1	Pb	1																							1958																																														K		7.175					7.175						0.461	Pb													Oe		802.6							Oe/K		238.4																							mJ/mol.K	53																																														Critical field measurements on superconducting lead isotopes				Phys.Rev., 112(1958)1888	D.L.Decker,D.E.Mapother,R.W.Shaw		
150031	PRL0060275	89.82% Ru<99>, 96.35%Ru<104> were used.	Ru	Ru1	Ru	1																							1961																																														K		0.493					0.493						0	Ru																																																																																									from Oak Ridge National Lab.					Absence of an isotope effect in superconducting ruthenium			Bell Telephone Lab, New Jesey	Phys.Rev.Lett., 6(1961)275	T.H.Geballe,B.T.Matthias,G.W.Hull,Jr,E.Corenzwit		
150032	P075172508	pulsed field. Hc2 defined as the field which the highest slope line meet to normal resistive line. Hc2(WHH) =   T using (dHc2/dT) at Tc.	(Pr,Ce)2CuO4	Pr1.87Ce0.13Cu1O4-z	Pr	1.87	Ce	0.13	Cu	1															O	4-z		5	2007																												T'																		K		10.8					10.8																				T			65																																																																									single crystal films were depositted on SrTiO3 substrates by pulsed laser deposition. optimized annealing for each Ce concentration.					Upper critical field of electron-doped Pr2-xCexCuO4-z in parallel magnetic fields			Center for Superconductivity Research and Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA	Phys.Rev.B, 75(2007)172508	Pengcheng Li,F.F.Balakirev,R.L.Greene		
150033	P075172508	d=2500A. pulsed field. Hc2 defined as the field which the highest slope line meet to normal resistive line. Hc2(WHH) = 170  T using (dHc2/dT) at Tc.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4-z	Pr	1.85	Ce	0.15	Cu	1															O	4-z		5	2007																												T'																		K		21.3					21.3																				T			73											HC150033																																																														single crystal films were depositted on SrTiO3 substrates by pulsed laser deposition. optimized annealing for each Ce concentration.					Upper critical field of electron-doped Pr2-xCexCuO4-z in parallel magnetic fields			Center for Superconductivity Research and Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA	Phys.Rev.B, 75(2007)172508	Pengcheng Li,F.F.Balakirev,R.L.Greene		
150034	P075172508	d=2500A. pulsed field. Hc2 defined as the field which the highest slope line meet to normal resistive line. Hc2(WHH) = 92.2  T using (dHc2/dT) at Tc.	(Pr,Ce)2CuO4	Pr1.84Ce0.16Cu1O4-z	Pr	1.84	Ce	0.16	Cu	1															O	4-z		5	2007																												T'																		K		16.9					16.9																				T			55											HC150034																																																														single crystal films were depositted on SrTiO3 substrates by pulsed laser deposition. optimized annealing for each Ce concentration.					Upper critical field of electron-doped Pr2-xCexCuO4-z in parallel magnetic fields			Center for Superconductivity Research and Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA	Phys.Rev.B, 75(2007)172508	Pengcheng Li,F.F.Balakirev,R.L.Greene		
150035	P075172508	d=2500A. pulsed field. Hc2 defined as the field which the highest slope line meet to normal resistive line. Hc2(WHH) = 58.6  T using (dHc2/dT) at Tc.	(Pr,Ce)2CuO4	Pr1.83Ce0.17Cu1O4-z	Pr	1.83	Ce	0.17	Cu	1															O	4-z		5	2007																												T'																		K		14					14																				T			44											HC150035																																																														single crystal films were depositted on SrTiO3 substrates by pulsed laser deposition. optimized annealing for each Ce concentration.					Upper critical field of electron-doped Pr2-xCexCuO4-z in parallel magnetic fields			Center for Superconductivity Research and Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA	Phys.Rev.B, 75(2007)172508	Pengcheng Li,F.F.Balakirev,R.L.Greene		
150036	P075172508	d=2500A. pulsed field. Hc2 defined as the field which the highest slope line meet to normal resistive line. Hc2(WHH) = 54.1T using (dHc2/dT) at Tc.	(Pr,Ce)2CuO4	Pr1.81Ce0.19Cu1O4-z	Pr	1.81	Ce	0.19	Cu	1															O	4-z		5	2007																												T'																		K		10.4					10.4																				T			32											HC150036																																																														single crystal films were depositted on SrTiO3 substrates by pulsed laser deposition. optimized annealing for each Ce concentration.					Upper critical field of electron-doped Pr2-xCexCuO4-z in parallel magnetic fields			Center for Superconductivity Research and Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA	Phys.Rev.B, 75(2007)172508	Pengcheng Li,F.F.Balakirev,R.L.Greene		
150037	P075174502	demagnetization factor = 0.97. Tc=7.1863-0.3847*P+0.01769*P^2. Hc2 shows H0(type-I). H0(P=0.5GPa)=770.88 Oe. H0(P=0.9)=739.99 Oe. H0(P=1.15)=729.01 Oe.	Pb	Pb1	Pb	1																							2007																																														K		7.186					7.186																				Oe		804.08																																		mJ/mol.K2	3.47	calculated from Hc																																											Thermodynamic properties of Pb determined from pressure-dependent critical-field measurements			MacDiarmid Institute for Advanced Materials and Nanotechnology, Industrial Research Ltd., P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 75(2007)174502	N.Suresh,J.L.Tallon		
150038	PR0881182		Pb	Pb1	Pb	1																							1952																																														K		7.17					7.17																																																								mJ/mol.K2	3.13	SP-heat	96.3	SP-heat																																									The specific heat of lead in the temperature range 1 K to 75 K				Phys.Rev., 88(1952)1182	M.Horowitz,A.A.Silvidi,S.F.Malaker,J.G.Daunt		
150039	P075184501	Hc2 measured from SP-heat. (dC/Tc) = 45 mJ/mol.K2. gamma estimated to be between 80 and 150 mJ/mol.K2.	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2007																												HoCoGa5																		K		9					9																													T/K	SP-heat		4	2	MHC150039																			SP150039																																																Specific heat and anisotropy of the nonconventional superconductors PuCoGa5 and PuRhGa5			Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Prague 2, The Czech Republic	Phys.Rev.B, 75(2007)184501	P.Javorsky,E.Colineau,F.Wastin,F.Jutier,J.-C.Griveau,P.Boulet,R.Jardin,J.Rebizant		
150040	P075184501		PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2007																												HoCoGa5																		K		17.8					17.8																													T/K	SP-heat		10	8	MHC150040																																																																			Specific heat and anisotropy of the nonconventional superconductors PuCoGa5 and PuRhGa5			Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Prague 2, The Czech Republic	Phys.Rev.B, 75(2007)184501	P.Javorsky,E.Colineau,F.Wastin,F.Jutier,J.-C.Griveau,P.Boulet,R.Jardin,J.Rebizant		
150041	PSS23200R4	not SC. TP(max) = 65 uV/K at 215 K. SP-heat, thermal conductivity, thermopower were measured.	URhGa5	U1Rh1Ga5	U	1	Rh	1	Ga	5																		3	2002																												HoCoGa5	P4/mmm		A	4.302		6.803												K					0.4																																																										mJ/mol.K2	7	SP-heat								uV/K	60.2																																		Transport Properties of URhGa5 Single Crystals			W. Trzebiatowski Institute of Low Temperature and Structure Research, Polish Academy of Sciences, ul. Okolna 2, 50-950 Wroclaw 2,  Poland	Phys.Stat.Sol. (b), 232(2002)R4	R.Wawryk,Z.Henkie,T.Cichorek,C.Geibel,F.Steglich		
150042	PR06012467	Tc,Hc2 defined as 0.5Rn(resistive transition).	Bi2Sr2CuOz	Bi2Sr2Cu1Oz	Bi	2	Sr	2	Cu	1															O	z		1	1999																												Bi2201																		K																											T	resistive		43	16										HC150042		A			35	15																																																													Temperature dependence of the upper critical field of Bi2Sr2CuOx single crystals			High Magnetic Field Laboratory, Max-Planck-Institut fur Festkorperforschung and Centre National de la Recherche Scientifique, Boite Postale, Grenoble Cedex 9, France	Phys.Rev.B, 60(1999)12467	S.I.Vedeneev,A.G.M.Jansen,E.Haanappel,P.Wyder		
150043	PR06101584	film thickness d = 250 nm. c-axis growth direction.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		5	2000																												Y123																		K		87.2					87.2																																		HC150043																	3140000																																													on-axis dc magnetron sputtering on MgO(001) at 770C.					Experimental determination of the B-T phase diagram of YBa2Cu3O7-z to 150 T for B-n-c	200001		National Pulsed Magnet Laboratory and Semiconductor Nanofabrication Facility, School of Physics, University of New South Wales, Sydney 2052, Australia	Phys.Rev.B,61(2000)1584-1587	A.S.Dzurak,B.E.Kane,D.G.Rickel,E.E.Mitchell,H.Nakagawa,J.D.Goettee,J.L.O'Brien,J.S.Brooks,N.E.Lumpkin,N.Muira,R.G.Clark,R.P.Starrett		
150044	P075184513		MgB2	B2Mg1	B	2	Mg	1																				1	2007																												AlB2																		K		38.8					38.8																																																											1076	using Bloch-Gruneizen eq. from R(T)						uV/K	10.29				uOhm.cm							16.3																		solid state reaction					Effects of Fe substitution on the transport properties of the superconductor MgB2			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr. K. S. Krishnan Road, New Delhi 110012, India	Phys.Rev.B, 75(2007)184513	Bhasker Gahtori,Ratan Lal,S.K.Agarwal,Y.K.Kuo,K.M.Sivakumar,J.K.Hsu,J.Y.Lin,Ashok Rao,S.K.Chen,J.L.MacManus-Driscoll		
150045	P075184513		(Mg,Fe)B2	Mg0.997Fe0.003B2	Mg	0.997	Fe	0.003	B	2																		1	2007																												AlB2																		K		37.9					37.9																																																											1043	using Bloch-Gruneizen eq. from R(T)						uV/K	10.05				uOhm.cm							25.1																		solid state reaction					Effects of Fe substitution on the transport properties of the superconductor MgB2			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr. K. S. Krishnan Road, New Delhi 110012, India	Phys.Rev.B, 75(2007)184513	Bhasker Gahtori,Ratan Lal,S.K.Agarwal,Y.K.Kuo,K.M.Sivakumar,J.K.Hsu,J.Y.Lin,Ashok Rao,S.K.Chen,J.L.MacManus-Driscoll		
150046	P075184513		(Mg,Fe)B2	Mg0.994Fe0.006B2	Mg	0.994	Fe	0.006	B	2																		1	2007																												AlB2																		K		37					37																																																											1021	using Bloch-Gruneizen eq. from R(T)						uV/K	10.88				uOhm.cm							37.3																		solid state reaction					Effects of Fe substitution on the transport properties of the superconductor MgB2			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr. K. S. Krishnan Road, New Delhi 110012, India	Phys.Rev.B, 75(2007)184513	Bhasker Gahtori,Ratan Lal,S.K.Agarwal,Y.K.Kuo,K.M.Sivakumar,J.K.Hsu,J.Y.Lin,Ashok Rao,S.K.Chen,J.L.MacManus-Driscoll		
150047	P075184513		(Mg,Fe)B2	Mg0.988Fe0.012B2	Mg	0.988	Fe	0.012	B	2																		1	2007																												AlB2																		K		34.9					34.9																																																											1152	using Bloch-Gruneizen eq. from R(T)						uV/K	9.14				uOhm.cm							73.1																		solid state reaction					Effects of Fe substitution on the transport properties of the superconductor MgB2			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr. K. S. Krishnan Road, New Delhi 110012, India	Phys.Rev.B, 75(2007)184513	Bhasker Gahtori,Ratan Lal,S.K.Agarwal,Y.K.Kuo,K.M.Sivakumar,J.K.Hsu,J.Y.Lin,Ashok Rao,S.K.Chen,J.L.MacManus-Driscoll		
150048	P075184513		(Mg,Fe)B2	Mg0.97Fe0.03B2	Mg	0.97	Fe	0.03	B	2																		1	2007																												AlB2																		K		32.9					32.9																																																											1131	using Bloch-Gruneizen eq. from R(T)						uV/K	11.54				uOhm.cm							110.4																		solid state reaction					Effects of Fe substitution on the transport properties of the superconductor MgB2			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr. K. S. Krishnan Road, New Delhi 110012, India	Phys.Rev.B, 75(2007)184513	Bhasker Gahtori,Ratan Lal,S.K.Agarwal,Y.K.Kuo,K.M.Sivakumar,J.K.Hsu,J.Y.Lin,Ashok Rao,S.K.Chen,J.L.MacManus-Driscoll		
150049	P075184535	impurity phase=Rh3P2,LaPO. Chemical formula = La0.82Rh3.9P12.1 by EPMA. Hc2 defined as 0.5Rn. RRR = 1.75. e-ph coupling = 0.7.	La0.8Rh4P12	La0.8Rh4P12	La	0.8	Rh	4	P	12																			2007									5.59																			skutterudite			A	8.0785														K				14.9			14.9																				T	resistive	16.7							T/K	resistive	1.2			MHC150049		A		44.1																		mJ/mol.K2	25.1	SP-heat	459	SP-heat											mOhm.cm							0.3173				0.5482												La(3N),Rh(3N),P(5N)		mixture of powder(La:Rh:P = 1:4:12) - high pressure synthesis(1473K,9.4GPa, using belt-type aparatus)					Superconducting properties of filled skutterudite La0.8Rh4P12			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 75(2007)184535	M.Imai,M.Akaishi,E.H.Sadki,T.Aoyagi,T.Kimura,I.Shirotani		
150050	PCS0600689	(dC/gamma*Tc) = 1.48. e-ph coupling = 0.57.	LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																			1999																												skutterudite			A	8.0605														K				7.2			7.2																				T		3.65														A		95															MSP150050	mJ/mol.K	270	mJ/mol.K2	26	SP-heat	446	SP-heat																																				high pressure synthesis (800-1100C,4GPa)					Superconductivity of LaRu4X12 (X = P, As and Sb) with skutterudite structure			Muroran Institute of Technology, 27-1 Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.Chem.Solids, 60(1999)689	T.Uchiumi,I.Shirotani,C.Sekine,S.Todo,T.Yagi,Y.Nakazawa,K.Kanoda		
150051	PCS0600689	e-ph coupling = 0.86.	LaRu4As12	La1Ru4As12	La	1	Ru	4	As	12																			1999																												skutterudite			A	8.5097														K				10.3			10.3																				T		0.72														A		206																		mJ/mol.K2	73	SP-heat	233	SP-heat																																				high pressure synthesis (800-1100C,4GPa)					Superconductivity of LaRu4X12 (X = P, As and Sb) with skutterudite structure			Muroran Institute of Technology, 27-1 Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.Chem.Solids, 60(1999)689	T.Uchiumi,I.Shirotani,C.Sekine,S.Todo,T.Yagi,Y.Nakazawa,K.Kanoda		
150052	PCS0600689		LaRu4Sb12	La1Ru4Sb12	La	1	Ru	4	Sb	12																			1999																												skutterudite			A	9.2781														K				2.8			2.8																				T		0.46												MHC150052		A		266																																																										high pressure synthesis (800-1100C,4GPa)					Superconductivity of LaRu4X12 (X = P, As and Sb) with skutterudite structure			Muroran Institute of Technology, 27-1 Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.Chem.Solids, 60(1999)689	T.Uchiumi,I.Shirotani,C.Sekine,S.Todo,T.Yagi,Y.Nakazawa,K.Kanoda		
150053	PCS0600689		(La,Ce)Ru4P12	La0.95Ce0.05Ru4P12	La	0.95	Ce	0.05	Ru	4	P	12																	1999																												skutterudite																		K	6.7		7	6.8			6.8																																																																																																					Superconductivity of LaRu4X12 (X = P, As and Sb) with skutterudite structure			Muroran Institute of Technology, 27-1 Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.Chem.Solids, 60(1999)689	T.Uchiumi,I.Shirotani,C.Sekine,S.Todo,T.Yagi,Y.Nakazawa,K.Kanoda		
150054	PCS0600689		(La,Ce)Ru4P12	La0.9Ce0.1Ru4P12	La	0.9	Ce	0.1	Ru	4	P	12																	1999																												skutterudite																		K	2.5		5	4.8			4.8																																																																																																					Superconductivity of LaRu4X12 (X = P, As and Sb) with skutterudite structure			Muroran Institute of Technology, 27-1 Mizumoto, Muroran-shi 050-8585, Japan	J.Phys.Chem.Solids, 60(1999)689	T.Uchiumi,I.Shirotani,C.Sekine,S.Todo,T.Yagi,Y.Nakazawa,K.Kanoda		
150055	JCG3050222		Bi2(Sr,Bi)2CuO6	Bi2.12Sr1.88Cu1O6+z	Bi	2.12	Sr	1.88	Cu	1															O	6+z		3	2007																												Bi2201																		K				6.38			6.38																																																																																														Bi2O3,SrCO3,CuO		traveling-solvent floating-zone method(TSFZ) under the pressure of P(O2) = 2 atm.					Growth and characterization of Bi2+xSr2-xCuO6+z single crystals			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, Beijing, PR China	J.Crys.Growth, 305(2007)222	H.Luo,L.Fang,G.Mu,H.-H.Wen		
150056	SSC1420421	e-ph coupling = 0.382, estimated from McMillan's eq.	Al	Al1	Al	1																							2007																																														K				1.16			1.16																																																								mJ/mol.K2	1.34		435																																										Superconducting transition parameters in aluminum-lithium alloys (0-10 at.% Li)			Department of Electrophysics, National Chiao Tung University, Hsinchu, Taiwan	Solid State Commun., 142(2007)421	M.N.Ou,T.J.Yang,B.J.Chen,Y.Y.Chen,J.C.Ho		
150057	SSC1420421	e-ph coupling = 0.377, estimated from McMillan's eq.	Al1-xLix	Al0.99Li0.01	Al	0.99	Li	0.01																					2007																																														K				1.07			1.07																																																								mJ/mol.K2	1.3		442																																										Superconducting transition parameters in aluminum-lithium alloys (0-10 at.% Li)			Department of Electrophysics, National Chiao Tung University, Hsinchu, Taiwan	Solid State Commun., 142(2007)421	M.N.Ou,T.J.Yang,B.J.Chen,Y.Y.Chen,J.C.Ho		
150058	SSC1420421	e-ph coupling = 0.375, estimated from McMillan's eq.	Al1-xLix	Al0.97Li0.03	Al	0.97	Li	0.03																					2007																																														K				1.05			1.05																																																								mJ/mol.K2	1.23		444																																										Superconducting transition parameters in aluminum-lithium alloys (0-10 at.% Li)			Department of Electrophysics, National Chiao Tung University, Hsinchu, Taiwan	Solid State Commun., 142(2007)421	M.N.Ou,T.J.Yang,B.J.Chen,Y.Y.Chen,J.C.Ho		
150059	SSC1420421	e-ph coupling = 0.378, estimated from McMillan's eq.	Al1-xLix	Al0.95Li0.05	Al	0.95	Li	0.05																					2007																																														K				1.13			1.13																																																								mJ/mol.K2	1.2		456																																										Superconducting transition parameters in aluminum-lithium alloys (0-10 at.% Li)			Department of Electrophysics, National Chiao Tung University, Hsinchu, Taiwan	Solid State Commun., 142(2007)421	M.N.Ou,T.J.Yang,B.J.Chen,Y.Y.Chen,J.C.Ho		
150060	SSC1420421	e-ph coupling = 0.385, estimated from McMillan's eq.	Al1-xLix	Al0.9Li0.1	Al	0.9	Li	0.1																					2007																																														K				1.29			1.29																																																								mJ/mol.K2	1.16		468																																										Superconducting transition parameters in aluminum-lithium alloys (0-10 at.% Li)			Department of Electrophysics, National Chiao Tung University, Hsinchu, Taiwan	Solid State Commun., 142(2007)421	M.N.Ou,T.J.Yang,B.J.Chen,Y.Y.Chen,J.C.Ho		
150061	DRM0140335	diamond film containing 2.6 at% B	B-doped diamond	C1	C	1																							2005																												diamond																		K		3.8				0.3	3.8																				T	WHH extraporation	11							T/K		4.3			MHC150061																																																														CVD on (111) natural diamond					Superconductivity in boron-doped diamond			Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow, Russia	Diamond Relat.Mater., 14(2005)335	V.A.Sidorov,E.A.Ekimov,E.D.Bauer,N.N.Mel'nik,N.J.Curro,V.Fnitsch,J.D.Thompson,S.M.Stishov,A.E.Alexenko,B.V.Spitsyn		
150062	JCG3050222		Bi2(Sr,Bi)2CuO6	Bi2.05Sr1.95Cu1O6+z	Bi	2.05	Sr	1.95	Cu	1															O	6+z		3	2007																												Bi2201																		K				8.94			8.94	TC150062																																																																																													Bi2O3,SrCO3,CuO		traveling-solvent floating-zone method(TSFZ) under the pressure of P(O2) = 2 atm.					Growth and characterization of Bi2+xSr2-xCuO6+z single crystals			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, Beijing, PR China	J.Crys.Growth, 305(2007)222	H.Luo,L.Fang,G.Mu,H.-H.Wen		
150063	P075212503	O-exchange rate by weight change. Tc defined as R=0.5Rn. isotope effect of structural transformation(LTO-to-LTT) = -0.32.	(La,Nd,Sr)2CuO4	La1.5Nd0.4Sr0.1Cu1O4	La	1.5	Nd	0.4	Sr	0.1	Cu	1													O	4		1	2007																												T																		K		11					11						1.24	O	80	1.3																																																																																						1	solid state reaction. ANN(980C,90h, then 500C,10h in 1bar <16>O2 or <18>O2) - FC to RT					Oxygen isotope effect on the superconductivity and stripe phase in La1.6-xNd0.4SrxCuO4			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 75(2007)212503	G.Y.Wang,J.D.Zhang,R.L.Yang,X.H.Chen		
150064	P075212503	O-exchange rate by weight change. Tc defined as R=0.5Rn. isotope effect of structural transformation(LTO-to-LTT) = -0.19.	(La,Nd,Sr)2CuO4	La1.475Nd0.4Sr0.125Cu1O4	La	1.475	Nd	0.4	Sr	0.125	Cu	1													O	4		1	2007																												T																		K		7.9					7.9						1.89	O	80																																																																																							1	solid state reaction. ANN(980C,90h, then 500C,10h in 1bar <16>O2 or <18>O2) - FC to RT					Oxygen isotope effect on the superconductivity and stripe phase in La1.6-xNd0.4SrxCuO4			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 75(2007)212503	G.Y.Wang,J.D.Zhang,R.L.Yang,X.H.Chen		
150065	P075212503	O-exchange rate by weight change. Tc defined as R=0.5Rn. isotope effect of structural transformation(LTO-to-LTT) = -0.20.	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		1	2007																												T																		K		17.8					17.8						0.98	O	80																																																																																							1	solid state reaction. ANN(980C,90h, then 500C,10h in 1bar <16>O2 or <18>O2) - FC to RT					Oxygen isotope effect on the superconductivity and stripe phase in La1.6-xNd0.4SrxCuO4			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 75(2007)212503	G.Y.Wang,J.D.Zhang,R.L.Yang,X.H.Chen		
150066	P075212503	O-exchange rate by weight change. Tc defined as R=0.5Rn. isotope effect of structural transformation(LTO-to-LTT) = -0.17.	(La,Nd,Sr)2CuO4	La1.425Nd0.4Sr0.175Cu1O4	La	1.425	Nd	0.4	Sr	0.175	Cu	1													O	4		1	2007																												T																		K		25					25						0.33	O	80																																																																																							1	solid state reaction. ANN(980C,90h, then 500C,10h in 1bar <16>O2 or <18>O2) - FC to RT					Oxygen isotope effect on the superconductivity and stripe phase in La1.6-xNd0.4SrxCuO4			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 75(2007)212503	G.Y.Wang,J.D.Zhang,R.L.Yang,X.H.Chen		
150067	PRL0590912	ratio of <16>O:<18>O measured by RBS. Tc by M measurement.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K				35			35						0.16	O	52	0.39																																																																																												Nonzero isotope effect in La1.85Sr0.15CuO4			AT&T Bell Laboratories, New Jersey	Phys.Rev.Lett., 59(1987)912	B.Batlogg,G.Kourouklis,W.Weber,R.J.Cava,A.Jayaraman,A.E.White,K.T.Short,L.W.Rupp,E.A.Rietman		
150068	PRL0590912	ratio of <16>O:<18>O measured by RBS. Tc by M measurement.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K				35			35						0.16	O	73	0.46																																																																																												Nonzero isotope effect in La1.85Sr0.15CuO4			AT&T Bell Laboratories, New Jersey	Phys.Rev.Lett., 59(1987)912	B.Batlogg,G.Kourouklis,W.Weber,R.J.Cava,A.Jayaraman,A.E.White,K.T.Short,L.W.Rupp,E.A.Rietman		
150069	JP0109055	<18>O-sample (90% exchange by weight change). O-content(=4.0) by titration method.	(La,Sr)2CuO4	La1.94Sr0.06Cu1O4	La	1.94	Sr	0.06	Cu	1															O	4	4	1	1998																												T																		K				8			8						1.05	O		1																																																																																					La2O3,SrCO3,CuO	1	ANN(900C,12h,in air), diffusion process(900C,40h,in 1bar <16>O2 or <18>O2) - cool to RT(4h)					Oxygen isotope effects in La2-xSrxCuO4: evidence for polaronic charge carriers and their condensation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.Condens.Matter, 10(1998)9055	G.Zhao,K.Conder,H.Keller,K.A.Muller		
150070	JP0109055	<18>O-sample (90% exchange by weight change). O-content(=4.0) by titration method.	(La,Sr)2CuO4	La1.91Sr0.09Cu1O4	La	1.91	Sr	0.09	Cu	1															O	4	4	1	1998																												T																		K				27.5			27.5	TC150070					0.34	O		1																																																																																					La2O3,SrCO3,CuO	1	ANN(900C,12h,in air), diffusion process(900C,40h,in 1bar <16>O2 or <18>O2) - cool to RT(4h)					Oxygen isotope effects in La2-xSrxCuO4: evidence for polaronic charge carriers and their condensation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.Condens.Matter, 10(1998)9055	G.Zhao,K.Conder,H.Keller,K.A.Muller		
150071	JP0109055	<18>O-sample (90% exchange by weight change). O-content(=4.0) by titration method.	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4	4	1	1998																												T																		K				30.2			30.2						0.62	O		2.1																																																																																					La2O3,SrCO3,CuO	1	ANN(900C,12h,in air), diffusion process(900C,40h,in 1bar <16>O2 or <18>O2) - cool to RT(4h)					Oxygen isotope effects in La2-xSrxCuO4: evidence for polaronic charge carriers and their condensation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.Condens.Matter, 10(1998)9055	G.Zhao,K.Conder,H.Keller,K.A.Muller		
150072	JP0109055	original data in Nature 385(1997)236	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4	4	1	1998																												T																		K				37			37						0.12	O		1																																																																																					La2O3,SrCO3,CuO	1	ANN(900C,12h,in air), diffusion process(900C,40h,in 1bar <16>O2 or <18>O2) - cool to RT(4h)					Oxygen isotope effects in La2-xSrxCuO4: evidence for polaronic charge carriers and their condensation			Physik-Institut der Universitat Zurich, CH-8057 Zurich, Switzerland	J.Phys.Condens.Matter, 10(1998)9055	G.Zhao,K.Conder,H.Keller,K.A.Muller		
150073	PCS0681390	R(25 K) = 9.62mOhm.cm. lattice term of SP-heat(beta) = 0.288 mJ/mol.K4. constant-term of SP-heat(A) =  1.159 mJ.K/mol.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4.175	Pr	1.85	Ce	0.15	Cu	1															O	4+z	4.175	1	2007																												T'																		K	14		18.5			2.8	16.25																																																								mJ/mol.K2	4.001	SP fitting													mOhm.cm											5.65														final annealing (850C,12h, in air) - FC to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150074	PCS0681390	R(25 K) = 12.47 mOhm.cm. lattice term of SP-heat(beta) = 0.292 mJ/mol.K4. constant-term of SP-heat(A) =  0.768 mJ.K/mol.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4.161	Pr	1.85	Ce	0.15	Cu	1															O	4+z	4.161	1	2007																												T'																		K	17.2		20.5			2	18.85																																																								mJ/mol.K2	5.018	SP fitting													mOhm.cm											6.78														final annealing (850C,12h, in air) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150075	PCS0681390	R(25 K) = 15.36 mOhm.cm. lattice term of SP-heat(beta) = 0.199 mJ/mol.K4. constant-term of SP-heat(A) =  1.099 mJ.K/mol.	(Pr,Ce)2CuO4	Pr1.85Ce0.15Cu1O4.065	Pr	1.85	Ce	0.15	Cu	1															O	4+z	4.065	1	2007																												T'																		K	13.5		20			3.2	16.75																																																								mJ/mol.K2	4.003	SP fitting													mOhm.cm											1.96														final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150076	PCS0681390		(Pr,Ce)2(Cu,Zn)O4	Pr1.85Ce0.15Cu0.995Zn0.005O4.065	Pr	1.85	Ce	0.15	Cu	0.995	Zn	0.005													O	4+z	4.065	1	2007																												T'																		K			18.9				18.9																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150077	PCS0681390		(Pr,Ce)2(Cu,Zn)O4	Pr1.85Ce0.15Cu0.99Zn0.01O4.065	Pr	1.85	Ce	0.15	Cu	0.99	Zn	0.01													O	4+z	4.065	1	2007																												T'																		K			18.41				18.41																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150078	PCS0681390		(Pr,Ce)2(Cu,Zn)O4	Pr1.85Ce0.15Cu0.985Zn0.015O4.065	Pr	1.85	Ce	0.15	Cu	0.985	Zn	0.015													O	4+z	4.065	1	2007																												T'																		K			18.28				18.28																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150079	PCS0681390		(Pr,Ce)2(Cu,Zn)O4	Pr1.85Ce0.15Cu0.98Zn0.02O4.065	Pr	1.85	Ce	0.15	Cu	0.98	Zn	0.02													O	4+z	4.065	1	2007																												T'																		K			18.01				18.01																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150080	PCS0681390		(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.998Ni0.002O4.065	Pr	1.85	Ce	0.15	Cu	0.998	Ni	0.002													O	4+z	4.065	1	2007																												T'																		K			15.89				15.89																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150081	PCS0681390		(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.995Ni0.005O4.065	Pr	1.85	Ce	0.15	Cu	0.995	Ni	0.005													O	4+z	4.065	1	2007																												T'																		K			11.92				11.92																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150082	PCS0681390		(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.993Ni0.007O4.065	Pr	1.85	Ce	0.15	Cu	0.993	Ni	0.007													O	4+z	4.065	1	2007																												T'																		K			7.02				7.02																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150083	PCS0681390		(Pr,Ce)2(Cu,Ni)O4	Pr1.85Ce0.15Cu0.99Ni0.01O4.065	Pr	1.85	Ce	0.15	Cu	0.99	Ni	0.01													O	4+z	4.065	1	2007																												T'																		K			0.93				0.93																																																																																																final annealing (850C,9h, in vac of 1.0E-3 Torr) - Q to RT					Superconductivity and calorimetric studies of Pr1.85Ce0.15CuO4+z under different annealing conditions			Department of Electronic Engineering, National Formosa University, Hu-Wei, Yunlin 632, Taiwan, ROC	J.Phys.Chem.Solids, 68(2007)1390	T.H.Meen,W.R.Chen,S.M.Chao,L.W.Ji,T.H.Fang,C.J.Huang		
150084	PHC4550063		(Cu,Tl)Ba2(Ca,Mg)4Cu5O14	Tl0.5Ba2Ca2Mg2Cu5.5O14-z	Tl	0.5	Ba	2	Ca	2	Mg	2	Cu	5.5											O	14-z			2007																												M1245	P4/mmm		A	3.916		21.254												K	94			100			100																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,MgO	1	mixture - heat(890C, in quartz) - addition(Tl2O3) - pellet - wrapped in Al-foil - SIN(890C, 10min) - Q to RT					Normal pressure synthesis of Mg-doped Cu0.5Tl0.5Ba2Ca2Mg2Cu5O14-z superconductor			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 455(2007)63	N.A.Khan,M.Irfan,S.Nawaz		
150085	PHC4550063	ANN(600C, 3h)	(Cu,Tl)Ba2(Ca,Mg)4Cu5O14	Tl0.5Ba2Ca2Mg2Cu5.5O14-z	Tl	0.5	Ba	2	Ca	2	Mg	2	Cu	5.5											O	14-z			2007																												M1245																		K	132.6						132.6																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN)2,MgO	1	mixture - heat(890C, in quartz) - addition(Tl2O3) - pellet - wrapped in Al-foil - SIN(890C, 10min) - Q to RT					Normal pressure synthesis of Mg-doped Cu0.5Tl0.5Ba2Ca2Mg2Cu5O14-z superconductor			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 455(2007)63	N.A.Khan,M.Irfan,S.Nawaz		
150086	PHC2350981	composition analyzed by SEM-EDX.  Ag:Cu:Ba:Cu = 0.72:4.18:1.99:3.12	(Ag,Cu)Ba2Ca2Cu3O9	Ag1Ba2Ca2Cu3O9-z	Ag	1	Ba	2	Ca	2	Cu	3													O	9-z			1994																												Ag1223			A	3.865		14.872												K		110					110																																																																																																mixture(Ba2Can-1CunO2n+4, AgO,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150087	PHC2350981	composition analyzed by SEM-EDX.  Ag:Cu:Ba:Cu = 0.47:4.48:2.24:2.81	(Ag,Cu)Ba2Ca3Cu4O11	Ag1Ba2Ca3Cu4O11-z	Ag	1	Ba	2	Ca	3	Cu	4													O	11-z			1994																												Ag1234			A	3.8635		18.111												K		117					117																																																																																																mixture(Ba2Can-1CunO2n+4, AgO,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150088	PHC2350981	composition analyzed by SEM-EDX.  Ag:Cu:Ba:Cu = 0.22:4.65:2.17:2.96	(Ag,Cu)Ba2Ca4Cu5O13	Ag1Ba2Ca4Cu5O13-z	Ag	1	Ba	2	Ca	4	Cu	5													O	13-z			1994																												Ag1245			A	3.8558		21.192												K		105					105																																																																																																mixture(Ba2Can-1CunO2n+4, AgO,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150089	PHC2350981	composition analyzed by SEM-EDX.  Ag:Cu:Ba:Cu = 0.13:4.73:2.15:2.99	(Ag,Cu)Ba2Ca5Cu6O15	Ag1Ba2Ca5Cu6O15-z	Ag	1	Ba	2	Ca	5	Cu	6													O	15-z			1994																												Ag1256			A	3.8574		24.85												K		80					80																																																																																																mixture(Ba2Can-1CunO2n+4, AgO,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150090	PHC2350981		CuBa2Ca2Cu3O10	Ba2Ca2Cu4O10-z	Ba	2	Ca	2	Cu	4															O	10-z			1994																												Cu1223			A	3.8571		14.788												K		106					106																																																																																																mixture(Ba2Can-1CunO2n+4, CaO2,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150091	PHC2350981		CuBa2Ca3Cu4O12	Ba2Ca3Cu5O12-z	Ba	2	Ca	3	Cu	5															O	12-z			1994																												Cu1234			A	3.8557		17.993												K		116					116																																																																																																mixture(Ba2Can-1CunO2n+4, CaO2,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150092	PHC2350981		CuBa2Ca4Cu5O14	Ba2Ca4Cu6O14-z	Ba	2	Ca	4	Cu	6															O	14-z			1994																												Cu1245			A	3.8511		21.167												K		102					102																																																																																																mixture(Ba2Can-1CunO2n+4, CaO2,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150093	PHC2350981		CuBa2Ca5Cu6O16	Ba2Ca5Cu7O16-z	Ba	2	Ca	5	Cu	7															O	16-z			1994																												Cu1256			A	3.8588		24.443												K		78					78																																																																																																mixture(Ba2Can-1CunO2n+4, CaO2,CuO) - SIN(950-1100 C,1-3 h, 4 GPa, in Au-capsule)					New high-Tc superconductor families of Ag1-xCuxBa2Can-1CunO2n+4-y with Tc>116 K			Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Physica C, 235-240(1994)981	H.Ihara,K.Tokiwa,A.Iyo,M.Hirabayashi,N.Terada,M.Tokumoto,Y.S.Song		
150094	PR05809504	anisotropy = 1.46 from coherence-L.	CuBa2(Ca,Mg)3Cu4O12	Ba2Ca2.85Mg0.15Cu5O12-z	Ba	2	Ca	2.85	Mg	0.15	Cu	5													O	12-z			1998																												Cu1234			A	3.855		17.954												K	116.6						116.6																				T	using WHH theory		127	86												A			19	13.2																																																				E+21/cm3	7.61			precursor(Cu-Ba-Ca-Mg-O) - mixed with AgO(oxidizer) and AgCO3(phase stabilizer) - SIN(1000C, 3.5 GPa, in Au capsule) - Q to RT - P release					Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
150095	PR05809504	anisotropy = 1.41 from coherence-L.	CuBa2(Ca,Mg)3Cu4O12	Ba2Ca2.7Mg0.3Cu5O12-z	Ba	2	Ca	2.7	Mg	0.3	Cu	5													O	12-z			1998																												Cu1234			A	3.848		17.907												K	116.4						116.4																				T	using WHH theory		103	74												A			20	14.2																																																				E+21/cm3	7.05			precursor(Cu-Ba-Ca-Mg-O) - mixed with AgO(oxidizer) and AgCO3(phase stabilizer) - SIN(1000C, 3.5 GPa, in Au capsule) - Q to RT - P release					Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
150096	PR05809504	anisotropy = 1.43 from coherence-L.	CuBa2(Ca,Mg)3Cu4O12	Ba2Ca2.4Mg0.6Cu5O12-z	Ba	2	Ca	2.4	Mg	0.6	Cu	5													O	12-z			1998																												Cu1234			A	3.848		17.907												K	116.8						116.8																				T	using WHH theory		115	80												A			20	14																																																				E+21/cm3	7.86			precursor(Cu-Ba-Ca-Mg-O) - mixed with AgO(oxidizer) and AgCO3(phase stabilizer) - SIN(1000C, 3.5 GPa, in Au capsule) - Q to RT - P release					Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
150097	PR05809504	anisotropy = 1.38 from coherence-L.	CuBa2(Ca,Mg)3Cu4O12	Ba2Ca2.01Mg0.99Cu5O12-z	Ba	2	Ca	2.01	Mg	0.99	Cu	5													O	12-z			1998																												Cu1234			A	3.847		17.917												K	116.6						116.6																				T	using WHH theory		110	79												A			20	14.5																																																				E+21/cm3	5.19			precursor(Cu-Ba-Ca-Mg-O) - mixed with AgO(oxidizer) and AgCO3(phase stabilizer) - SIN(1000C, 3.5 GPa, in Au capsule) - Q to RT - P release					Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
150098	PR05809504	anisotropy = 1.6 from coherence-L.	CuBa2(Ca,Mg)3Cu4O12	Ba2Ca3Cu5O12-z	Ba	2	Ca	3	Cu	5															O	12-z			1998																												Cu1234			A	3.856		17.993												K	117.5						117.5																				T	using WHH theory		195	121												A			16	10																																																				E+21/cm3	5.4			precursor(Cu-Ba-Ca-Mg-O) - mixed with AgO(oxidizer) and AgCO3(phase stabilizer) - SIN(1000C, 3.5 GPa, in Au capsule) - Q to RT - P release					Superconductivity in the Mg-doped CuBa2Ca3Cu4O12-y system	10		Electrotechnical Laboratory, 1-1-4, Umezono, Tsukuba, Ibaraki 305, Japan	Phys.Rev.B, 58(1998)9504	A.Iyo,A.V.Narlikar,H.Ihara,K.Tokiwa,M.Hamao,M.Tokumoto,M.Umeda,N.Terada,S.K.Agarwal,T.Saya,T.Watanabe,Y.Tanaka		
150099	PHC3880365	annealing time = 6h. TCFIG shows Tc(annealing temp).	TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9-z	Tl	1	Ba	2	Ca	2	Cu	3													O	9-z			2003																												Tl1223																		K				131			131	TC150099																																																																																															See Supercond.Sci.Technol., 14(2001)504					Anomalous suppression of Tc in an overdoped region of TlBa2Ca2Cu3O9-z			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 388-389(2003)365	A.Iyo,M.Hirai,K.Tokiwa,T.Watanabe,M.Tokumoto,M.Ariyama,Y.Tanaka		
150100	L099037006	Tc(SP) = 2.3 K. R=R0 + A*T^2 (R0=104 uOhm.cm, A=6.5 E-3 uOhm.cm./K2. C(T) shown in Fig.1. lattice term = 0.65 mJ/mol.K4. (dC/gamma*Tc) = 1.04. e-ph = 0.56-0.62.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				1	2007																												Ir3Ge7	Im3m																	K	2.25						2.25																																																								mJ/mol.K2	34.2	SP heat	310																																					melt in quartz ampoule - heat(750C,10d) - powdered - HIP(600C, 2h, P=51 MPa)					Spin Fluctuations and Superconductivity in Mo3Sb7			Laboratoire de Physique des Materiaux, Nancy Universite, CNRS, Ecole Nationale Superieure des Mines de Nancy, Parc de Saurupt, 54042 Nancy cedex, France	Phys.Rev.Lett., 99(2007)037006	C.Candolfi,B.Lenoir,A.Dauscher,C.Bellouard,J.Hejtmanek,E.Santava,J.Tobola		
150101	L099027001	graphite layer distance = 4.95 A. lattice term(SP) beta = 0.191 mJ/mol.K4. delta = 0.801 uJ/mol.K6. (dC/gamma`Tc) = 1.426. e-ph = 0.54.	SrC6	C6Sr1	C	6	Sr	1																					2007																												GIC	P63/mmc																	K				1.65		0.06	1.65	MTC150101		K/GPa	0.35																Oe			276	138										MHC150101		A			1510	700								3.34								mJ/mol.K2	5.92	SP heat	414																																					vapor phase reaction at 470C(Sr) or 500C(Ba).					Superconductivity in Heavy Alkaline-Earth Intercalated Graphites			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.Lett., 99(2007)027001	J.S.Kim,L.Boeri,J.R.O'Brien,F.S.Razavi,R.K.Kremer		
150102	L099027001	not SC. graphite layer distance = 5.25 A.	BaC6	Ba1C6	Ba	1	C	6																					2007																												GIC	P63/mmc																	K					0.3																																																																																																		vapor phase reaction at 470C(Sr) or 500C(Ba).					Superconductivity in Heavy Alkaline-Earth Intercalated Graphites			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.Lett., 99(2007)027001	J.S.Kim,L.Boeri,J.R.O'Brien,F.S.Razavi,R.K.Kremer		
150103	P098257004	microwave (27 GHz) penetration depth. second Tc = 8 K. G-L parameter = 82.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2007																												pyrochlore																		K		9.4					9.4																																									A	microwave	2600			K	24.5	5.1	7																																																				Effects of Rattling Phonons on the Dynamics of Quasiparticle Excitation in the beta-Pyrochlore KOs2O6 Superconductor			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.Lett., 98(2007)257004	Y.Shimono,T.Shibauchi,Y.Kasahara,T.Kato,K.Hashimoto,Y.Matsuda,J.Yamaura,Y.Nagao,Z.Hiroi		
150104	L098257002	F in apical sites. NMR study. Inner CO2-plane has M=0.16 m<B>, hole = 0.06 - 0.08. Outer plane has M=0.29 m<B>, ele = 0.06 - 0.08.	Ba2Ca3Cu4O8F2	Ba2Ca3Cu4F2O8	Ba	2	Ca	3	Cu	4	F	2													O	8			2007								100																				0234																		K				55			55																																																																																																high pressure synthesis					Uniform mixing of antiferromagnetism and high-temperature superconductivity in electron-doped layers of four-layered Ba2Ca3Cu4O8F2: A new phenomenon in an electron underdoped regime			Department of Materials Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.Lett., 98(2007)257002	S.Shimizu,H.Mukuda,Y.Kitaoka,A.Iyo,Y.Tanaka,Y.Kodama,K.Tokiwa,T.Watanabe		
150105	L098257002	F in apical sites. NMR study. Inner CO2-plane has ( hole = 0.13 - 0.15).	Ba2Ca2Cu3O6F2	Ba2Ca2Cu3F2O6	Ba	2	Ca	2	Cu	3	F	2													O	6			2007																												0223																		K				76			76																																																																																																high pressure synthesis					Uniform mixing of antiferromagnetism and high-temperature superconductivity in electron-doped layers of four-layered Ba2Ca3Cu4O8F2: A new phenomenon in an electron underdoped regime			Department of Materials Engineering Science, Osaka University, Osaka, Japan	Phys.Rev.Lett., 98(2007)257002	S.Shimizu,H.Mukuda,Y.Kitaoka,A.Iyo,Y.Tanaka,Y.Kodama,K.Tokiwa,T.Watanabe		
150106	SST0190573	point contact tunneling (Ag/Mo3Sb7).  Hc2 obtained from (dV/dI) vs H curves.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																					2006																												Ir3Ge7	Im3m																D8f	K		2.25	2.3				2.25																				T	parabolic T-dependence	1.65							T/K		1.42															meV	0.32	3.2	1																																															peritectic reaction (Liq. Sb + sol. Mo) in Ar					Energy gap and upper critical field of the new magnetic superconductor Mo3Sb7 found by the Andreev reflection method			B Verkin Institute for Low Temperature Physics and Engineering, National Academy of Science of Ukraine, Kharkiv, Ukraine	Supercond.Sci.Technol., 19(2006)573	V.M.Dmitriev,L.F.Rybaltchenko,L.A.Ishchenko,E.V.Khristenko,Z.Bukowski,R.Troc		
150107	PHB3980360	Tc defined as maximum of (dR/dT)	YBa2(Cu,PO4)3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			2007																												Y123																		K		92.842					92.842																																																						J/kg.K	7.392																																								1	ANN(850C,16h) - cool to RT					Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7-z material			Universidad Nacional de Colombia, Bogota, Colombia	Physica B, 398(2007)360	M.P.Rojas Sarmiento,M.A.Uribe Laverde,E.Vera Lopez,D.A.Landinez Tellez,J.Roa-Rojas		
150108	PHB3980360	Tc defined as maximum of (dR/dT)	YBa2(Cu,PO4)3O7	Y1Ba2Cu2.97P0.03O7-z	Y	1	Ba	2	Cu	2.97	P	0.03													O	7-z			2007																												Y123																		K		96.663					96.663																																																						J/kg.K	7.172																																								1	ANN(850C,16h) - cool to RT					Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7-z material			Universidad Nacional de Colombia, Bogota, Colombia	Physica B, 398(2007)360	M.P.Rojas Sarmiento,M.A.Uribe Laverde,E.Vera Lopez,D.A.Landinez Tellez,J.Roa-Rojas		
150109	PHB3980360	Tc defined as maximum of (dR/dT)	YBa2(Cu,PO4)3O7	Y1Ba2Cu2.94P0.06O7-z	Y	1	Ba	2	Cu	2.94	P	0.06													O	7-z			2007																												Y123																		K		88.259					88.259																																																						J/kg.K	6.962																																								1	ANN(850C,16h) - cool to RT					Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7-z material			Universidad Nacional de Colombia, Bogota, Colombia	Physica B, 398(2007)360	M.P.Rojas Sarmiento,M.A.Uribe Laverde,E.Vera Lopez,D.A.Landinez Tellez,J.Roa-Rojas		
150110	PHB3980360	Tc defined as maximum of (dR/dT)	YBa2(Cu,PO4)3O7	Y1Ba2Cu2.91P0.09O7-z	Y	1	Ba	2	Cu	2.91	P	0.09													O	7-z			2007																												Y123																		K		80.97					80.97																																																						J/kg.K	6.792																																								1	ANN(850C,16h) - cool to RT					Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7-z material			Universidad Nacional de Colombia, Bogota, Colombia	Physica B, 398(2007)360	M.P.Rojas Sarmiento,M.A.Uribe Laverde,E.Vera Lopez,D.A.Landinez Tellez,J.Roa-Rojas		
150111	PHB3980360	Tc defined as maximum of (dR/dT)	YBa2(Cu,PO4)3O7	Y1Ba2Cu2.88P0.12O7-z	Y	1	Ba	2	Cu	2.88	P	0.12													O	7-z			2007																												Y123																		K		75.985					75.985																																																						J/kg.K	6.562																																								1	ANN(850C,16h) - cool to RT					Conductivity fluctuation and superconducting parameters of the YBa2Cu3-x(PO4)xO7-z material			Universidad Nacional de Colombia, Bogota, Colombia	Physica B, 398(2007)360	M.P.Rojas Sarmiento,M.A.Uribe Laverde,E.Vera Lopez,D.A.Landinez Tellez,J.Roa-Rojas		
150112	PHC3870187	oz by iodometric titration. (dC/Tc) = 53.4 mJ/mol.K2)	TmBa2Cu3O7	Tm1Ba2Cu3O6.95	Tm	1	Ba	2	Cu	3															O	7-z	6.95	1	2003																												Y123																		K		89.93				1.5	89.93																																																																		uV/K	-0.46				mOhm.cm											0.709													1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150113	PHC3870187	oz by iodometric titration. (dC/Tc) = 62.4 mJ/mol.K2)	TmBa2Cu3O7	Tm1Ba2Cu3O6.99	Tm	1	Ba	2	Cu	3															O	7-z	6.99	1	2003																												Y123																		K		89.8				1.7	89.8																																																																		uV/K	-0.4			TP150113	mOhm.cm											0.57									RH150113	E+21/cm3	11.3		1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150114	PHC3870187	oz calculated using linear relation in TP300 vs oz. (dC/Tc) = 42.3 mJ/mol.K2)	TmBa2Cu3O7	Tm1Ba2Cu3O6.96	Tm	1	Ba	2	Cu	3															O	7-z	6.96	1	2003																												Y123																		K		89.88				0.6	89.88																																																																		uV/K	0				mOhm.cm											0.41													1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150115	PHC3870187	oz calculated using linear relation in TP300 vs oz. (dC/Tc) = 36.5 mJ/mol.K2)	TmBa2Cu3O7	Tm1Ba2Cu3O6.91	Tm	1	Ba	2	Cu	3															O	7-z	6.91	1	2003																												Y123																		K		90.36				1	90.36																																																																		uV/K	3.8				mOhm.cm											0.8													1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150116	PHC3870187	oz calculated using linear relation in TP300 vs oz.	TmBa2Cu3O7	Tm1Ba2Cu3O6.94	Tm	1	Ba	2	Cu	3															O	7-z	6.94	1	2003																												Y123																		K		89.88				0.7	89.88																																																																		uV/K	2				mOhm.cm											0.83													1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150117	PHC3870187	oz by iodometric titration	TmBa2Cu3O7	Tm1Ba2Cu3O6.86	Tm	1	Ba	2	Cu	3															O	7-z	6.86	1	2003																												Y123																		K		87.2				2.5	87.2																																																																		uV/K	6.45				mOhm.cm											1.1									RH150117	E+21/cm3	5.9		1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150118	PHC3870187	oz by iodometric titration	TmBa2Cu3O7	Tm1Ba2Cu3O6.87	Tm	1	Ba	2	Cu	3															O	7-z	6.87	1	2003																												Y123																		K		83.6				7	83.6																																																																		uV/K	8.2				mOhm.cm																								1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150119	PHC3870187	oz by iodometric titration. (dC/Tc) = 0 mJ/mol.K2)	TmBa2Cu3O7	Tm1Ba2Cu3O6.8	Tm	1	Ba	2	Cu	3															O	7-z	6.8	1	2003																												Y123																		K		79.8				6	79.8																																																																		uV/K	10.5			TP150119	mOhm.cm																								1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150120	PHC3870187	oz by iodometric titration	TmBa2Cu3O7	Tm1Ba2Cu3O6.72	Tm	1	Ba	2	Cu	3															O	7-z	6.72	1	2003																												Y123																		K		64.5				4.4	64.5																																																																		uV/K	18.5				mOhm.cm											1.69									RH150120	E+21/cm3	3.9		1	ANN(400 - 560, in air) for different oxygen content(oz)					Superconducting and transport properties of TmBa2Cu3O7-z and comparison to YBa2Cu3O7-z			Institute of Low Temperature and Structure Research of the Polish Academy of Sciences, Wroclaw, Poland	Physica C, 387(2003)187	C.Sulkowski,D.Wlosewicz,M.Matusiak,T.Plackowski,A.Sikora,R.Horyn		
150121	SSC0970131	mixed phase( (Cu,C)-1223, (Cu,C)-1234, unknown phase). Tc(P) shows Tc1(n=3), Tc2(n=4), Tc3(unknown). (dTc/dP) estimated from Tc2(P) in Fig.	(Cu,C)Ba2Ca3Cu4Oz	C0.5Ba2Ca3Cu4.5Oz	C	0.5	Ba	2	Ca	3	Cu	4.5													O	z			1996																												Cu1234			A	3.865		18.027												K		117					117	TC150121		K/GPa	1.7																																																																																												precursor(Ba2Ca3Cu4.5C0.5Oz) + AgO, sealed in Au capsule, heat(700 900C, 4 - 8 GPa, 1 h)					THE INFLUENCE OF PRESSURE ON THE SUPERCONDUCTING PROPERTIES OF THE (CuxC1-x)Ba2Can-1CunOy FAMILY OF THSC MATERIALS			CRTBT. CNRS-UJF,BP 166,38042 Grenoble cedex 09, France	Solid State Commun.97(1996)131-135	A. Sulpice,B. Souletie,C. Chaillout,J. Chenavas,J.J. Capponi,J.L. Tholence,M. Jaime,M. Marezio,M. Nunez Regueiro,M.A. Alario Franco,P. Borded,S. de Brion	Cu, C, Ba, Ca, O	
150122	PHC2190200		Tl(CO3)Sr2Ba2Cu2O7	Tl1C1Sr2Ba2Cu2O10	Tl	1	C	1	Sr	2	Ba	2	Cu	2											O	10			1994																												Tl1201																		K		68.2					68.2	TC150122																																																																																													Tl2O3,Sr2CuO3,BaO2,CuO		mixture(Tl2Sr4-xBaxCu2Oz) - wrapped in Au foil - heat(750-850C) - heat to 950C(200C/h) - keep(30min) - Q to RT - ANN(1.2-4.0 % CO2/O2 gas flow)					Synthesis and superconductivity of oxycarbonates of the Tl-1201 phase	199401		Institute for Materials Research,Tohoku University,  Sendai,Japan	Physica C, 219(1994)200-204	E.Aoyagi,E.Ohshima,J.Akimitsu,K.Hiraga,M.Kikuchi,M.Ogawa,N.Ohnishi,S.Nakajima,T.Oku,Y.Muraoka,Y.Syono	Tl,Ba,Sr,Cu,O,C	
150123	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2PdGe3	Y2Pd1Ge3	Y	2	Pd	1	Ge	3																			2007																												AlB2			A	4.221		3.9365												K	2.7	2.82	3.2			0.5	2.82																																																											255	SP-heat																																				arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150124	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.9Pt0.1Ge3	Y	2	Pd	0.9	Pt	0.1	Ge	3																	2007																												AlB2			A	4.2212		3.9422												K	2.57	2.68	2.83				2.68																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150125	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.8Pt0.2Ge3	Y	2	Pd	0.8	Pt	0.2	Ge	3																	2007																												AlB2			A	4.2185		3.9452												K	2.51	2.62	2.71				2.62																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150126	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.7Pt0.3Ge3	Y	2	Pd	0.7	Pt	0.3	Ge	3																	2007																												AlB2			A	4.217		3.9522												K	2.43	2.52	2.59				2.52																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150127	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.6Pt0.4Ge3	Y	2	Pd	0.6	Pt	0.4	Ge	3																	2007																												AlB2			A	4.216		3.9552												K	2.41	2.46	2.5				2.46																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150128	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.5Pt0.5Ge3	Y	2	Pd	0.5	Pt	0.5	Ge	3																	2007																												AlB2			A	4.2109		3.9635												K	2.32	2.42	2.49				2.42																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150129	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2(Pd,Pt)Ge3	Y2Pd0.3Pt0.7Ge3	Y	2	Pd	0.3	Pt	0.7	Ge	3																	2007																												AlB2			A	4.2059		3.9739												K	2.22	2.26	2.3				2.26																																																											320	SP-heat																																				arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150130	PHC4660051	main phase = Y2(Pd,Pt)1.3Ge2.5 by EDX. impurity phase = ThCr2Si2-type structure. gamma = 6-7 mJ/mol.K2 by fitting (3 < T < 5 K).	Y2PtGe3	Y2Pt1Ge3	Y	2	Pt	1	Ge	3																			2007																												AlB2			A	4.1953		3.9878												K	2.08	2.14	2.16				2.14																																																																																																arc-melting. sealed in quartz tube - ANN(1123K,1w)					Superconducting behavior of the solid solution, Y2Pd1-xPtxGe3			Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai, India	Physica C, 466(2007)51	K.K.Iyer,E.V.Sampathkumaran		
150131	PHC4630170		(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	2007																											2	T'			A	3.9445		12.0524												K				24			24																																																																																														Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150132	PHC4630170	paramag-Curie-temp.	(Nd,Ce)2(Cu,Mn)O4	Nd1.85Ce0.15Cu0.995Mn0.005O4	Nd	1.85	Ce	0.15	Cu	0.995	Mn	0.005													O	4		1	2007							12.6																				3	T'			A	3.9424	3.9438	12.06												K				22.1			22.1																																																																																														Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150133	PHC4630170	paramag-Curie-temp.	(Nd,Ce)2(Cu,Mn)O4	Nd1.85Ce0.15Cu0.98Mn0.02O4	Nd	1.85	Ce	0.15	Cu	0.98	Mn	0.02													O	4		1	2007							13.6																				3	T'			A	3.9348	3.9507	12.0859												K				21.1			21.1																																																																																														Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150134	PHC4630170	paramag-Curie-temp.	(Nd,Ce)2(Cu,Mn)O4	Nd1.85Ce0.15Cu0.96Mn0.04O4	Nd	1.85	Ce	0.15	Cu	0.96	Mn	0.04													O	4		1	2007							17																				3	T'			A	3.9176	3.9548	12.0742												K				21			21																																																																																														Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150135	PHC4630170	paramag-Curie-temp.	(Nd,Ce)2(Cu,Mn)O4	Nd1.85Ce0.15Cu0.91Mn0.09O4	Nd	1.85	Ce	0.15	Cu	0.91	Mn	0.09													O	4		1	2007							40																				3	T'			A	3.9383	3.9472	12.0656												K				17.9			17.9																																																																																														Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150136	PHC4630170	multi-phase. not SC.	(Nd,Ce)2(Cu,Mn)O4	Nd1.85Ce0.15Cu0.8Mn0.2O4	Nd	1.85	Ce	0.15	Cu	0.8	Mn	0.2													O	4		2	2007																																														K					5																																																																																																Nd2O3,CeO2,CuO,MnO2	1	mixture - CAL(950C,24h,in air) - pellet - SIN(1050C,10h,in air) - Q to RT - ANN(900C,6h,in flowing Ar) - Q to RT					Mn doping effect on superconductivity and magnetic properties of Nd1.85Ce0.15CuO4 system			Key Laboratory of Advanced Technologies of Materials, Superconductivity R&D Center, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 463-465(2007)170	H.M.Zhou,Y.Yang,G.Li,C.H.Cheng,M.H.Pu,Y.Zhao		
150137	PHC4630190	nearly single phase for 0.2 < x < 0.5. Semicond-like resistivity. not SC.	RuSr2(Nd,Dy,Ce,Sr)3Cu2Oz	Ru1Sr2.2Nd0.6Dy0.4Ce1.8Cu2Oz	Ru	1	Sr	2.2	Nd	0.6	Dy	0.4	Ce	1.8	Cu	2									O	z		1	2007																															A	3.842		16.98											Ru-1232	K					4.2																																																																																																RuO2,SrCO3,Nd2O3,Dy2O3,CeO2,CuO	1	SIN(1025C,24h,in 1 atm O2) - FC to RT - ANN(400C,24h,in 1 atm O2) - cool to RT(0.5C/min)					Synthesis of the Ru-1232 compound in the RuSr2(Nd1-xDyxCe1.8Sr0.2)Cu2Oz system			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Hamamatsu, Shizuoka 431-3192, Japan	Physica C, 463-465(2007)190	Y.Akagi,H.Sasakura,S.Tsukui,T.Oka,M.Adachi		
150138	SUP0170449	Two-step Tc in R-T curve. The lower(Ru-1232) = 15 K. The higher(Ru-1222) shown in T3 of TBL. Curie-T shows ferromagnetic temp.	RuSr2(Gd,Ce,Sr)3Cu2Oz	Ru1Sr2.2Gd1Ce1.8Cu2Oz	Ru	1	Sr	2.2	Gd	1	Ce	1.8	Cu	2											O	z			2004							90																								A	3.836		16.97											Ru-1232	K			22	20			20																																																																																														Sr2CuO3,RuO2,Gd2O3,CeO2,CuO,Nb2O5	1	mixture - pellet - CAL(950C,24h,in air) - cool to RT - pellet - SIN(1050C,24h,in O2) - ANN(400C,24h,in O2) - cool to RT(0.5C/min)					Superconductivity and Ferromagnetism of the Ru-1232 Compounds in the (Ru1¿xNbx)Sr2(GdCe1.8Sr0.2)Cu2Oz System			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Hamamatsu, Shizuoka 431-3192, Japan.	J.Supercond.,17(2004)449	Y.Akagi,H.Sasakura,S.Noguchi,S.Tsukui,T.Oka,M.Adachi		
150139	SUP0170449	Two-step Tc in R-T curve. The lower(Ru-1232) = 10 K. The higher(Ru-1222) shown in T3 of TBL. Curie-T shows ferromagnetic temp.	(Ru,Nb)Sr2(Gd,Ce,Sr)3Cu2Oz	Ru0.9Nb0.1Sr2.2Gd1Ce1.8Cu2Oz	Ru	0.9	Nb	0.1	Sr	2.2	Gd	1	Ce	1.8	Cu	2									O	z			2004							60																								A	3.839		16.99											Ru-1232	K			18	17			17																																																																																														Sr2CuO3,RuO2,Gd2O3,CeO2,CuO,Nb2O5	1	mixture - pellet - CAL(950C,24h,in air) - cool to RT - pellet - SIN(1050C,24h,in O2) - ANN(400C,24h,in O2) - cool to RT(0.5C/min)					Superconductivity and Ferromagnetism of the Ru-1232 Compounds in the (Ru1¿xNbx)Sr2(GdCe1.8Sr0.2)Cu2Oz System			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Hamamatsu, Shizuoka 431-3192, Japan.	J.Supercond.,17(2004)449	Y.Akagi,H.Sasakura,S.Noguchi,S.Tsukui,T.Oka,M.Adachi		
150140	SUP0170449	Two-step Tc in R-T curve. The lower(Ru-1232) = 6 K. The higher(Ru-1222) shown in T3 of TBL. Curie-T shows ferromagnetic temp.	(Ru,Nb)Sr2(Gd,Ce,Sr)3Cu2Oz	Ru0.8Nb0.2Sr2.2Gd1Ce1.8Cu2Oz	Ru	0.8	Nb	0.2	Sr	2.2	Gd	1	Ce	1.8	Cu	2									O	z			2004							45																								A	3.842		17											Ru-1232	K			15	10			10																																																																																														Sr2CuO3,RuO2,Gd2O3,CeO2,CuO,Nb2O5	1	mixture - pellet - CAL(950C,24h,in air) - cool to RT - pellet - SIN(1050C,24h,in O2) - ANN(400C,24h,in O2) - cool to RT(0.5C/min)					Superconductivity and Ferromagnetism of the Ru-1232 Compounds in the (Ru1¿xNbx)Sr2(GdCe1.8Sr0.2)Cu2Oz System			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Hamamatsu, Shizuoka 431-3192, Japan.	J.Supercond.,17(2004)449	Y.Akagi,H.Sasakura,S.Noguchi,S.Tsukui,T.Oka,M.Adachi		
150141	SUP0170449		(Ru,Nb)Sr2(Gd,Ce,Sr)3Cu2Oz	Ru0.7Nb0.3Sr2.2Gd1Ce1.8Cu2Oz	Ru	0.7	Nb	0.3	Sr	2.2	Gd	1	Ce	1.8	Cu	2									O	z			2004																															A	3.845		17.02											Ru-1232	K			10	5			5																																																																																														Sr2CuO3,RuO2,Gd2O3,CeO2,CuO,Nb2O5	1	mixture - pellet - CAL(950C,24h,in air) - cool to RT - pellet - SIN(1050C,24h,in O2) - ANN(400C,24h,in O2) - cool to RT(0.5C/min)					Superconductivity and Ferromagnetism of the Ru-1232 Compounds in the (Ru1¿xNbx)Sr2(GdCe1.8Sr0.2)Cu2Oz System			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Hamamatsu, Shizuoka 431-3192, Japan.	J.Supercond.,17(2004)449	Y.Akagi,H.Sasakura,S.Noguchi,S.Tsukui,T.Oka,M.Adachi		
150142	PHC3880567	e-ph = 0.66 from McMillan's eq.	Y2PdGe3	Y2Pd1Ge3	Y	2	Pd	1	Ge	3																			2003																												AlB2			A	4.1988		3.9626												K		3.1					3.1																																																								mJ/Ymol.K2	1.35		127	SP-heat																																				arc-melting. ANN(850C,1w, in evacuated quartz tube)					Superconductivity in Y2PdGe3-xSix: interplay between Debye temperature and coupling constant			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113, Japan	Physica C, 388-389(2003)567	A.K.Ghosh,H.Nakamura,M.Tokunaga,T.Tamegai		
150143	PHC3880567	e-ph = 0.63 from McMillan's eq.	Y2Pd(Ge,Si)3	Y2Pd1Ge2.5Si0.5	Y	2	Pd	1	Ge	2.5	Si	0.5																	2003																												AlB2			A	4.1646		3.9864												K		3.3					3.3	MTC150143																																																							mJ/Ymol.K2	1.58		151	SP-heat																																				arc-melting. ANN(850C,1w, in evacuated quartz tube)					Superconductivity in Y2PdGe3-xSix: interplay between Debye temperature and coupling constant			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113, Japan	Physica C, 388-389(2003)567	A.K.Ghosh,H.Nakamura,M.Tokunaga,T.Tamegai		
150144	PHC3880567	e-ph = 0.53 from McMillan's eq.	Y2Pd(Ge,Si)3	Y2Pd1Ge2Si1	Y	2	Pd	1	Ge	2	Si	1																	2003																												AlB2			A	4.1297		4.0094												K		2.24					2.24																																																								mJ/Ymol.K2	2.91		177	SP-heat																																				arc-melting. ANN(850C,1w, in evacuated quartz tube)					Superconductivity in Y2PdGe3-xSix: interplay between Debye temperature and coupling constant			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113, Japan	Physica C, 388-389(2003)567	A.K.Ghosh,H.Nakamura,M.Tokunaga,T.Tamegai		
150145	PHC4450440	anisotropy factor(=SQRT(Rc/Rab) = 36 at 50K. Tc = 43.8 K for Rc measurement.	(Bi,Pb)2(Sr,La)2CuO6	Bi1.6Pb0.4Sr1.9La0.1Cu1O6+z	Bi	1.6	Pb	0.4	Sr	1.9	La	0.1	Cu	1											O	6+z		3	2006																												Bi2201																		K	43.3					4.4	43.3																																																																																																Floating zone method					A new aspect of superconductivity observed (Bi,Pb)2(Sr,La)2CuO6+d single crystals			Faculty of Frontier Science, Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305 8571, Japan	Physica C, 445-448(2006)440	Y.Arao,M.Tange,H.Ikeda,T.Koyano,R.Yoshizaki		
150146	JJP046L167		Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr1.9Cu1O6+z	Bi	2.1	Sr	1.9	Cu	1															O	6+z			2007																												Bi2201			A	5.35	5.38	24.49												K				6.8			6.8																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150147	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr1.7Ca0.2Cu1O6+z	Bi	2.1	Sr	1.7	Ca	0.2	Cu	1													O	6+z			2007																												Bi2201			A	5.35	5.37	24.5												K				79.2			79.2																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150148	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr1.5Ca0.4Cu1O6+z	Bi	2.1	Sr	1.5	Ca	0.4	Cu	1													O	6+z			2007																												Bi2201			A	5.33	5.35	24.33												K				83			83																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150149	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr1.3Ca0.6Cu1O6+z	Bi	2.1	Sr	1.3	Ca	0.6	Cu	1													O	6+z			2007																												Bi2201			A	5.34	5.37	24.39												K				77.8			77.8																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150150	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr1.1Ca0.8Cu1O6+z	Bi	2.1	Sr	1.1	Ca	0.8	Cu	1													O	6+z			2007																												Bi2201			A	5.35	5.37	24.31												K				77.4			77.4																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150151	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr0.95Ca0.95Cu1O6+z	Bi	2.1	Sr	0.95	Ca	0.95	Cu	1													O	6+z			2007																												Bi2201			A	5.35	5.36	24.32												K				74.8			74.8																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150152	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr0.9Ca1Cu1O6+z	Bi	2.1	Sr	0.9	Ca	1	Cu	1													O	6+z			2007																												Bi2201			A	5.32	5.35	24.19												K				74.6			74.6																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150153	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr0.7Ca1.2Cu1O6+z	Bi	2.1	Sr	0.7	Ca	1.2	Cu	1													O	6+z			2007																												Bi2201			A	5.34	5.42	24.15												K				75			75																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150154	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr0.5Ca1.4Cu1O6+z	Bi	2.1	Sr	0.5	Ca	1.4	Cu	1													O	6+z			2007																												Bi2201			A	5.34	5.38	23.91												K				73.9			73.9																																																																																														Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150155	JJP046L167	Bi2212 phase <7-14 %	Bi2(Sr,Bi,Ca)2CuO6	Bi2.1Sr0.3Ca1.6Cu1O6+z	Bi	2.1	Sr	0.3	Ca	1.6	Cu	1													O	6+z			2007																												Bi2201			A	5.31	5.35	23.89												K						7																																																																																															Bi2O3,SrCO3,CaCO3,CuO	1	mixture - CAL(750C,24h) - CAL(800C,24h) - SIN(800-850C,48h)					Ca Substitution Effect for Sr upon Superconductivity of Bi2.1CaySr1.9-yCuO6+d			Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan	Jpn.J.Appl.Phys., 46(2007)L167	R.Yoshizaki,T.Nakajima,M.Tange		
150156	PHC4660011	G-L parameter = 13.8 layered diamond-like structure.	NaAlSi	Na1Al1Si1	Na	1	Al	1	Si	1																			2007																													P4/mmm	129	A	4.119		7.362											anti-PbFCl-type	K				7			7										100	Oe	M-H curve	101							T	magnetization, WHH fitting	1.91							T/K		0.402			MHC150156		A	Hc2	131.3			A	Hc1 using GL eq.	1813																																																			Na(3N),Al(4N),Si(5N)		high-pressure synthesis (1300-1400C, 30min, P=5.5 GPa) - Q to RT.					Superconductivity in ternary siliside NaAlSi with layered diamond-like structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa, Japan	Physica C, 466(2007)11	S.Kuroiwa,H.Kawashima,H.Kinoshita,H.Okabe,J.Akimitsu		
150157	PHC4630111	Tc by SP-heat. (dC/gamma*Tc) = 2.1	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																			2007																													P4<3>32																	K		7					7																																																								mJ/mol.K2	8.3		202	SP-heat																																		Li-lump,Pd-plate,B-flake		arc-melting(Pd-B), then react quickly (Pd-B & Li-lump) in arc furnace.					Specific heat of lithium ternary borides under magnetic field			Superconducting Materials Center, National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 463-465(2007)111	H.Takeya,S.Kasahara,M.El.Massalami,K.Hirata,K.Togano		
150158	PHC4630111	Tc by SP-heat. (dC/gamma*Tc) = 0.75	Li2Pt3B	Li2Pt3B1	Li	2	Pt	3	B	1																			2007																													P4<3>32																	K		2.6					2.6																																																								mJ/mol.K2	9.6		240	SP-heat																																		Li-lump,Pt-plate,B-flake		arc-melting(Pt-B), then react quickly (Pt-B & Li-lump) in arc furnace.					Specific heat of lithium ternary borides under magnetic field			Superconducting Materials Center, National Institute for Materials Science, Sengen 1-2-1, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 463-465(2007)111	H.Takeya,S.Kasahara,M.El.Massalami,K.Hirata,K.Togano		
150159	J076024713	Tc depends on sintering conditions.	Y2C3	C3Y2	C	3	Y	2																					2007																												Pu2C3																		K				11.6			11.6																				T	SP-heat, WHH fitting	22.7							T/K		2.91					A		38										3.6	14							mJ/mol.K2	4.7		540	SP-heat																																		Y(3N),C(3N) powder		mixture - arc melting. heat(1400-1600C, 10-30 min, P=4.0-5.5 GPa) , then Quench to RT					Superconductivity of Y2C3 Investigated by Specific Heat Measurement			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)024713	S.Akutagawa,J.Akimitsu		
150160	J076024713	Tc depends on sintering conditions.	Y2C3	C3Y2	C	3	Y	2																					2007																												Pu2C3																		K				13.9			13.9																				T	SP-heat, WHH fitting	24.7							T/K		2.57					A		36										3.9	14							mJ/mol.K2	6		530	SP-heat																																		Y(3N),C(3N) powder		mixture - arc melting. heat(1400-1600C, 10-30 min, P=4.0-5.5 GPa) , then Quench to RT					Superconductivity of Y2C3 Investigated by Specific Heat Measurement			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)024713	S.Akutagawa,J.Akimitsu		
150161	J076024713	Tc depends on sintering conditions.	Y2C3	C3Y2	C	3	Y	2																					2007																												Pu2C3																		K				15.2			15.2											Oe	M-H curve	32.8							T	SP-heat, WHH fitting	26.8							T/K		2.55					A		55			A	from Hc1using GL-eq	4470					4.1	14				MSP150161			mJ/mol.K2	6.3		530	SP-heat																																		Y(3N),C(3N) powder		mixture - arc melting. heat(1400-1600C, 10-30 min, P=4.0-5.5 GPa) , then Quench to RT					Superconductivity of Y2C3 Investigated by Specific Heat Measurement			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)024713	S.Akutagawa,J.Akimitsu		
150162	J076024713	data from reference 13 of J076024713.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																					2007																												Cr3Si(A15)																	Cr3Si, A15	K				18			18																				T		25														A		115										4.8								mJ/gat.K2	13		230																																					Pb-flux method					Superconductivity of Y2C3 Investigated by Specific Heat Measurement			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)024713	S.Akutagawa,J.Akimitsu		
150163	J076063701	typical size=1x1x0.5 mm3. Hc2(0)=3.66 T for H//[110]. G-L parameter = 28. Curie-T(para) = -42 K for H//[100], = -139 K for H//[001]. gamma = 200 mJ/mol.K2 at Tc. (dC/gamma*Tc) = 2.33 (Tc=4.9 K)	NpPd5Al2	Np1Pd5Al2	Np	1	Pd	5	Al	2																		3	2007																												ZrNi2Al5	I4/mmm		A	4.148		14.716												K	5						5											Oe	M-H curve	80							T			14.3	3.7					T/K			31	6.4	MHC150163		A	from Hc2		94		A	from Hc1using GL-eq		2600									MSP150163			mJ/mol.K2	390		175	SP-heat																																				arc-melting - ANN(500C,1w,in vac)					Unconventional Heavy-Fermion Superconductivity of a New Transuranium Compound NpPd5Al2			Institute for Materials Research, Tohoku University, Oarai, Ibaraki 311-1313	J.Phys.Soc.Jpn, 76(2007)063701	D.Aoki,Y.Haga,T.D.Matsuda,N.Tateiwa,S.Ikeda,Y.Homma,H.Sakai,Y.Shiokawa,E.Yamamoto,A.Nakamura,R.Settai,Y.Onuki		
150164	J076073708	RRR=150. (dC/Tc) = 11.3 mJ/mol.K2. (dC/gamma*Tc) = 1.4. Thermodynamic Hc(0) = 126 Oe. G-L parameter = 0.7(type-I SC).	Rh2Ga9	Ga9Rh2	Ga	9	Rh	2																				1	2007																												Co2Al9	Pc	7															distorted Co2Al9 type	K				1.9			1.9																				Oe	type-I SC (Hc)	130												MHC150164																						mJ/mol.K2	7.9		312	SP-heat											uOhm.cm							1																							Superconductivity in Rh2Ga9 and Ir2Ga9 without Inversion Symmetry			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561	J.Phys.Soc.Jpn, 76(2007)073708	T.Shibayama,M.Nohara,H.A.Katori,Y.Okamoto,Z.Hiroi,H.Takagi		
150165	J076073708	RRR=150. (dC/Tc) = 9.8 mJ/mol.K2. (dC/gamma*Tc) = 1.4. Thermodynamic Hc(0) = 133 Oe. G-L parameter = 1.1.	Ir2Ga9	Ga9Ir2	Ga	9	Ir	2																				1	2007																												Co2Al9	Pc	7															distorted Co2Al9 type	K				2.2			2.2																				Oe	linear approx.	250												MHC150164		A	from Hc2	1000																		mJ/mol.K2	6.9		264	SP-heat											uOhm.cm							1																							Superconductivity in Rh2Ga9 and Ir2Ga9 without Inversion Symmetry			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561	J.Phys.Soc.Jpn, 76(2007)073708	T.Shibayama,M.Nohara,H.A.Katori,Y.Okamoto,Z.Hiroi,H.Takagi		
150166	J076083706	RRR=120. P-induced SC. Pcrit(AF) = 2.25 GPa. SC properties at P=2.19 GPa.	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2007								1.88																				BaNiSn3																		K	1.4				0		1.4	MTC150166																																																																																															Czochralski method					Strong-Coupling Superconductivity of CeIrSi3 with the Non-centrosymmetric Crystal Structure			Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195	J.Phys.Soc.Jpn, 76(2007)083706	N.Tateiwa,Y.Haga,T.D.Matsuda,S.Ikeda,E.Yamamoto,Y.Okuda,Y.Miyauchi,R.Settai,Y.Onuki		
150167	J076093704	impurity phase: RuAs2.  (dC/gamma*Tc) = 0.83	PrRu4As12	Pr1Ru4As12	Pr	1	Ru	4	As	12																		1	2007					uB/mol	3.3	-11																					skutterudite			A	8.491														K		2.33					2.33																				T	SP-heat, WHH fitting	0.62							T/K		0.365			MHC150167																						mJ/mol.K2	95																																							high pressure synthesis (900C, 4GPa)					Superconducting Properties of Pr-Based Filled Skutterudite PrRu4As12			Faculty of Engineering Science, Muroran Institute of Technology, Muroran, Hokkaido 050-8585	J.Phys.Soc.Jpn, 76(2007)093704	T.Namiki,Y.Aoki,H.Sato,C.Sekine,I.Shirotani,T.D.Matsuda,Y.Haga,T.Yagi		
150168	J076094705	RRR = 2. energy gap by break junction. G-L parameter = 2.2.  (dC/gamma*Tc) = 0.73	NbB2	B2Nb1	B	2	Nb	1																				1	2007																												AlB2			A	3.098		3.317												K		9.5		9.6		0.6	9.5										70	Oe	M-H curve	830							T	SP-heat, linear fitting	0.395												MHC150168		A	from Hc2	290			A	from Hc1using GL-eq	630			meV	1.36	3.5	1				MSP150168			mJ/mol.K2	4.2		650	SP-heat																																		NbB2,B		mixture(nominal B/Nb=2.5) - pellet - sealed in quartz tube - heat(1000C,2h)					Specific Heat and Tunneling Spectroscopy Study of NbB2 with Maximum Tc = 10K			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)094705	S.Kuroiwa,Y.Tomita,A.Sugimoto,T.Ekino,J.Akimitsu		
150169	P076012505	70um-dia X 35 um-thickness. nearly hydrostatic pressure ( He medium). Tc by ac-SUS.	Sc	Sc1	Sc	1																							2007																																														K		8.2			0		8.2	MTC150169																																																																																																				Pressure-induced superconductivity in Sc to 74 Gpa			Department of Physics, Washington University, Campus Box 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.B, 76(2007)012505	J.J.Hamlin,J.S.Schilling		
150170	P076014501	SC properties due to minor phase: YSr2Cu3Oz which are on the grain boundaries.	Sr2Y(Ru,Cu)O6	Sr2Y1Ru0.5Cu0.5O6	Sr	2	Y	1	Ru	0.5	Cu	0.5													O	6			2007																												2126			A	5.715	5.771	8.165												K				64			64																																																																																															1	usual solid state reaction.					Origin of the superconductivity in the Y-Sr-Ru-O and Y-Sr-Cu-O systems			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 76(2007)014501	E.Galstyan,Y.Xue,M.Iliev,Y.Sun,C.W.Chu		
150171	P076014528	RRR = 1.16. resistivity R = R0 + A*T^2. thermodynamic Hc(0) = 7.6 mT. SC parameters calculated from Hc2, Hc(0) using GLAG theory. G-L parameter = 13.	beta-Al3Mg2	Al3Mg2	Al	3	Mg	2																				3	2007																																														K		0.87					0.87																				T	R(T)	0.14							T/K	R(T)	0.23			MHC150171		A	from Hc2	485			A	from Hc, Hc2 using GLAG	5300										MSP150171			mJ/mol.K2	6.6		373	SP-heat											uOhm.cm							33																		flux growth method. ANN(190 C, 48h)					Superconductivity in the complex metallic alloy  beta-Al3Mg2			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 76(2007)014528	E.Bauer,H.Kaldarar,R.Lackner,H.Michor,W.Steiner,E.-W.Scheidt,A.Galatanu,F.Marabelli,T.Wazumi,K.Kumagai,M.Feuerbacher		
150172	PHC3410581		Sr2Ca3Cu4O8F2	Sr2Ca3Cu4F2O8.6	Sr	2	Ca	3	Cu	4	F	2													O	8+z	8.6	1	2000																												0234			A	3.851		32.35												K				38			38																																																																																														SrF2,CaF2,SrO2,SrCuO2,CaCuO3,CuO		mixture - high pressure synthesis(1250C,3h,P=5.5 GPa) - Q to RT					High-Pressure Synthesis of Oxyfluoride Superconductors, Sr2Can-1CunO2n+zF2 (n=4,5)			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 341-348(2000)581	T.Kawashima,E.Takayama-Muromachi		
150173	PHC3410581		Sr2Ca3Cu4O8F2	Sr2Ca3Cu4F2O8.8	Sr	2	Ca	3	Cu	4	F	2													O	8+z	8.8		2000																												0234																		K				72			72																																																																																														SrF2,CaF2,SrO2,SrCuO2,CaCuO3,CuO		mixture - high pressure synthesis(1250C,3h,P=5.5 GPa) - Q to RT					High-Pressure Synthesis of Oxyfluoride Superconductors, Sr2Can-1CunO2n+zF2 (n=4,5)			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 341-348(2000)581	T.Kawashima,E.Takayama-Muromachi		
150174	PHC3410581		Sr2Ca3Cu4O8F2+z	Sr2Ca3Cu4F3.8O8	Sr	2	Ca	3	Cu	4	F	3.8													O	8+z	8		2000																												0234																		K				95			95																																																																																														SrF2,CaF2,SrO2,SrCuO2,CaCuO3,CuO		mixture - high pressure synthesis(1250C,3h,P=5.5 GPa) - Q to RT					High-Pressure Synthesis of Oxyfluoride Superconductors, Sr2Can-1CunO2n+zF2 (n=4,5)			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 341-348(2000)581	T.Kawashima,E.Takayama-Muromachi		
150175	PHC3410581		Sr2Ca4Cu5O10F2	Sr2Ca4Cu5F2O10.57	Sr	2	Ca	4	Cu	5	F	2													O	10+z	10.57		2000																												0245			A	3.852		38.77												K				40			40																																																																																														SrF2,CaF2,SrO2,SrCuO2,CaCuO3,CuO		mixture - high pressure synthesis(1250C,3h,P=5.5 GPa) - Q to RT					High-Pressure Synthesis of Oxyfluoride Superconductors, Sr2Can-1CunO2n+zF2 (n=4,5)			National Institute for Research in Inorganic Materials, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 341-348(2000)581	T.Kawashima,E.Takayama-Muromachi		
150176	PHC4530024	(dTm/dP) = 5.2 K/GPa, Tm is magnetic ordering tempeature.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8			2007																												Ru1212																		K	40		58				49			K/GPa	1.4																																																																																												solid state reacton of precursor(Ru,Rh)Sr2GdO6 and CuO.					Pressure study of superconductivity and magnetism in pure and Rh-doped RuSr2GdCu2O8 materials			Department of Physics, San Diego State University, San Diego, CA 92182-1233, USA	Physica C, 453(2007)24	M.Steiger,C.Kongmark,F.Rueckert,L.Harding,M.S.Torikachvili		
150177	PHC4530024	(dTm/dP) = 3.7 K/GPa, Tm is magnetic ordering tempeature.	(Ru,Rh)Sr2GdCu2O8	Ru0.95Rh0.05Sr2Gd1Cu2O8	Ru	0.95	Rh	0.05	Sr	2	Gd	1	Cu	2											O	8			2007																												Ru1212																		K	24.7		41				32.85			K/GPa	1.1																																																																																												solid state reacton of precursor(Ru,Rh)Sr2GdO6 and CuO.					Pressure study of superconductivity and magnetism in pure and Rh-doped RuSr2GdCu2O8 materials			Department of Physics, San Diego State University, San Diego, CA 92182-1233, USA	Physica C, 453(2007)24	M.Steiger,C.Kongmark,F.Rueckert,L.Harding,M.S.Torikachvili		
150178	PHC4530024	(dTm/dP) = 6.0 K/GPa, Tm is magnetic ordering tempeature.	(Ru,Rh)Sr2GdCu2O8	Ru0.9Rh0.1Sr2Gd1Cu2O8	Ru	0.9	Rh	0.1	Sr	2	Gd	1	Cu	2											O	8			2007																												Ru1212																		K			31				31			K/GPa	1.8																																																																																												solid state reacton of precursor(Ru,Rh)Sr2GdO6 and CuO.					Pressure study of superconductivity and magnetism in pure and Rh-doped RuSr2GdCu2O8 materials			Department of Physics, San Diego State University, San Diego, CA 92182-1233, USA	Physica C, 453(2007)24	M.Steiger,C.Kongmark,F.Rueckert,L.Harding,M.S.Torikachvili		
150179	PHC4530024	(dTm/dP) = 7.9 K/GPa, Tm is magnetic ordering tempeature.	(Ru,Rh)Sr2GdCu2O8	Ru0.85Rh0.15Sr2Gd1Cu2O8	Ru	0.85	Rh	0.15	Sr	2	Gd	1	Cu	2											O	8			2007																												Ru1212																		K			19				19			K/GPa	1.7																																																																																												solid state reacton of precursor(Ru,Rh)Sr2GdO6 and CuO.					Pressure study of superconductivity and magnetism in pure and Rh-doped RuSr2GdCu2O8 materials			Department of Physics, San Diego State University, San Diego, CA 92182-1233, USA	Physica C, 453(2007)24	M.Steiger,C.Kongmark,F.Rueckert,L.Harding,M.S.Torikachvili		
150180	PR0538238	impurity: F(540ppm), O(300ppm), H(275ppm), Fe(<20ppm). Tc(P) of  La(dhcp) was measured	alpha-La	La1	La	1																							1996																																													dhcp	K		5					5	MTC150180																																																																																																				Effect of pressure on the superconducting Tc of lanthanum			Institute of Solid State Physics, 142432 Chernogolovka, Moscow District, Russia	Phys.Rev.B, 53(1996)8238	V.G.Tissen,E.G.Ponyatovskii,M.V.Nefedova,F.Porsch,W.B.Holzapfel		
150181	PHC4600066	P-induced SC. Two SC phases: Low-Tc phase(Tc=4.5 K, P<crit> = 8.0 GPa)  and high-Tc phase (Tc=8.5 K, P<crit> = 10.1 GPa.). Charge order disappear at P<crit> = 10.1 GPa.	beta-LixV2O5	Li0.33V2O5	Li	0.33	V	2																	O	5			2007																												bronze																	beta-bronze	K		8.5			0		8.5	MPH150181																																																																																																				Observation of pressure-induced superconductivity in beta-LixV2O5			Material Design and Characterization Laboratory, Institute for Solid State Physics, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Physica C, 460-462(2007)66	T.Yamauchi,H.Ueda,Y.Ueda		
150182	PHC4600700	T-dependence of PENET<c> is measured by ARPES. Energy gap by fitting using eq. of d(PENET) = f(gap). T<CDW> = 32 K.	NbSe2	Nb1Se2	Nb	1	Se	2																				3	2007																												2H-NbSe2																		K		7.2					7.2																																																2.6	12																																																				Anisotropic superconductivity in NbSe2 probed by magnetic penetration depth			Institut Neel, CNRS/UJF, BP 166, 38042 Grenoble Cedex 9, France	Physica C, 460-462(2007)700	P.Diener,P.Rodiere,J.D.Fletcher,A.Carrington,J.P.Brison,R.Prozorov,T.Olheiser,R.W.Giannetta		
150183	PHC4600708	(dC/gamma*Tc) = 1.09.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2007																												U2Mn3Si5																		K				4.5			4.5																																		MHC150183																																																														floating zone method using image furnace. Then ANN(1150C,5d) - ANN(850C,5d).					Anisotropic superconductivity in Lu2Fe3Si5			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 460-462(2007)708	T.Tamegai,T.Nakagawa,M.Tokunaga		
150184	PHC4600708	Tc by SP-Heat.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		1	2007																												U2Mn3Si5																		K				5.6			5.6																																																					MSP150184			mJ/mol.K2	20.5		485																																					arc melting					Anisotropic superconductivity in Lu2Fe3Si5			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 460-462(2007)708	T.Tamegai,T.Nakagawa,M.Tokunaga		
150185	PR0272800	(dC/gamma*Tc) = 0.99. e-ph coupling = 0.51.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		1	1983																												U2Mn3Si5																		K		6.25					6.25																																																						mJ/mol.K	173	mJ/mol.K2	27.8		561																																					arc-melting - ANN(1250C,5d) - ANN(800C, 5d)					Low temperature heat capacity of superconducting ternary iron silisides			Ames Laboratory and Department of Physics,Iowa State University,Ames,Iowa	Phys.Rev.B, 27(1983)2800	C.B.Vining,R.N.Shelton,H.F.Braun,M.Pelizzone		
150186	PR0272800	(dC/gamma*Tc) = 0.81. e-ph coupling = 0.45.	Sc2Fe3Si5	Sc2Fe3Si5	Sc	2	Fe	3	Si	5																		1	1983																												U2Mn3Si5																		K		4.46					4.46																																																						mJ/mol.K	80.3	mJ/mol.K2	22.2		290																																					arc-melting - ANN(1250C,5d) - ANN(800C, 5d)					Low temperature heat capacity of superconducting ternary iron silisides			Ames Laboratory and Department of Physics,Iowa State University,Ames,Iowa	Phys.Rev.B, 27(1983)2800	C.B.Vining,R.N.Shelton,H.F.Braun,M.Pelizzone		
150187	PR0272800	(dC/gamma*Tc) = 0.78. e-ph coupling = 0.39.	Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																		1	1983																												U2Mn3Si5																		K		1.68					1.68																																																						mJ/mol.K	25.4	mJ/mol.K2	19.4																																							arc-melting - ANN(1250C,5d) - ANN(800C, 5d)					Low temperature heat capacity of superconducting ternary iron silisides			Ames Laboratory and Department of Physics,Iowa State University,Ames,Iowa	Phys.Rev.B, 27(1983)2800	C.B.Vining,R.N.Shelton,H.F.Braun,M.Pelizzone		
150188	LTP0210377	20 um foil. RRR = 70-100	alpha-La	La1	La	1																							1975																																													dhcp	K		4.9					4.9	MTC150188		K/GPa	1.15																																																																																												ANN(220C, in vac)					Pressure-induced lattice instability in fcc lanthanum at low temperature			Institut fur Festkorperforschung der KernforschungsanlageJulich, Julich, Germany	J.Low Temp.Phys., 21(1975)377	H.Balster,J.Wittig		
150189	LTP0210377	20 um foil. RRR = 30. Tc(max) = 12.9 K at P=180 kbar.	beta-La	La1	La	1																							1975																																													fcc	K		6					6	MTC150188		K/GPa	1.01																																																																																												ANN(240C, in vac)					Pressure-induced lattice instability in fcc lanthanum at low temperature			Institut fur Festkorperforschung der KernforschungsanlageJulich, Julich, Germany	J.Low Temp.Phys., 21(1975)377	H.Balster,J.Wittig		
150190	PLA0850372	RRR = 20. magnetic reentrant behaviour below Tc.	Tm2Fe3Si5	Tm2Fe3Si5	Tm	2	Fe	3	Si	5																			1981																												U2Mn3Si5																		K		1.1	1.7				1.1																																																																																																arc-melting - Homogeneize(1150C,4d) - ANN(800C,8d, in Ar)					Reentrant superconductivity in Tm2Fe3Si5			Institute for Pure and Applied Physical Science, University of California, San Diego,CA,USA	Phys.Lett., 85A(1981)372	C.U.Segre,H.F.Braun		
150191	PLA0850372		(Tm,Lu)2Fe3Si5	Tm0.9Lu0.1Fe3Si5	Tm	0.9	Lu	0.1	Fe	3	Si	5																	1981																												U2Mn3Si5																		K		1.65					1.65	MTC150191																																																																																															arc-melting - Homogeneize(1150C,4d) - ANN(800C,8d, in Ar)					Reentrant superconductivity in Tm2Fe3Si5			Institute for Pure and Applied Physical Science, University of California, San Diego,CA,USA	Phys.Lett., 85A(1981)372	C.U.Segre,H.F.Braun		
150192	PLA0850372		(Tm,Lu)2Fe3Si5	Tm0.84Lu0.16Fe3Si5	Tm	0.84	Lu	0.16	Fe	3	Si	5																	1981																												U2Mn3Si5																		K		2.44					2.44																																																																																																arc-melting - Homogeneize(1150C,4d) - ANN(800C,8d, in Ar)					Reentrant superconductivity in Tm2Fe3Si5			Institute for Pure and Applied Physical Science, University of California, San Diego,CA,USA	Phys.Lett., 85A(1981)372	C.U.Segre,H.F.Braun		
150193	PLA0850372		(Tm,Lu)2Fe3Si5	Tm0.8Lu0.2Fe3Si5	Tm	0.8	Lu	0.2	Fe	3	Si	5																	1981																												U2Mn3Si5																		K		2.79					2.79																																																																																																arc-melting - Homogeneize(1150C,4d) - ANN(800C,8d, in Ar)					Reentrant superconductivity in Tm2Fe3Si5			Institute for Pure and Applied Physical Science, University of California, San Diego,CA,USA	Phys.Lett., 85A(1981)372	C.U.Segre,H.F.Braun		
150194	PHC4600636		LaPt2B2C	La1Pt2B2C1	La	1	Pt	2	B	2	C	1																	2007																												LuNi2B2C																		K				10			10																																																																							mOhm.cm											0.06														arc-melting and induction heating, then ANN(1500C,1w, in Ar)					Superconducting and magnetic properties of Pt-based borocarbides RPt2B2C (R = La, Ce, Pr)			Department of Physics, Indian Institute of Technology, Kanpur 208 016, India	Physica C, 460-462(2007)636	V.K.Anand,C.Geibel,Z.Hossain		
150195	PHC4600636		PrPt2B2C	Pr1Pt2B2C1	Pr	1	Pt	2	B	2	C	1																	2007																												LuNi2B2C																		K				6			6																																																																																																arc-melting and induction heating, then ANN(1500C,1w, in Ar)					Superconducting and magnetic properties of Pt-based borocarbides RPt2B2C (R = La, Ce, Pr)			Department of Physics, Indian Institute of Technology, Kanpur 208 016, India	Physica C, 460-462(2007)636	V.K.Anand,C.Geibel,Z.Hossain		
150196	PHC4600636	not SC.	CePt2B2C	Ce1Pt2B2C1	Ce	1	Pt	2	B	2	C	1																	2007					myu-B	2.5																						LuNi2B2C																		K					2																																																																																																		arc-melting and induction heating, then ANN(1500C,1w, in Ar)					Superconducting and magnetic properties of Pt-based borocarbides RPt2B2C (R = La, Ce, Pr)			Department of Physics, Indian Institute of Technology, Kanpur 208 016, India	Physica C, 460-462(2007)636	V.K.Anand,C.Geibel,Z.Hossain		
150197	PHC4600542	RRR=1300. Anomalies at 90 and 180 K in resistivity and specific heat , come from phase transition.	Ag6O8Ag(NO3)	Ag7N1O11	Ag	7	N	1																	O	11		3	2007																												clathrate	Fm3[-]m																	K		1.04				0.04	1.04																				Oe	resistive transition, WHH fitting	710												MHC150197		A	from Hc2	681																																																										electro chemical reaction					Superconductivity in clathrate-type silver oxides: Ag6O8MX (M = cation, X = anion)			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Kanagawa 229-8558, Japan	Physica C, 460-462(2007)542	K.Kawashima,M.Ishii,S.Date,T.Tsutsumi,H.Okabe,J.Akimitsu		
150198	PSP1981381	Tc by ac-SUS. hydrostatic pressure.	Lu2Fe3Si5	Lu1Fe3Si5	Lu	1	Fe	3	Si	5																		1	1981																												Sc2Fe3Si5			A	10.342		5.385												K		6					6	MTC150198		K/GPa	-1.02																																																																																												arc-melting					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150199	PSP1981381	Tc by ac-SUS. hydrostatic pressure.	Sc2Fe3Si5	Sc1Fe3Si5	Sc	1	Fe	3	Si	5																		1	1981																												Sc2Fe3Si5																		K		4.3					4.3	MTC150198		K/GPa	-0.77																																																																																												arc-melting					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150200	PSP1981381	Tc by ac-SUS. hydrostatic pressure.	Y2Fe3Si5	Y2Fe3Si5	Y	2	Fe	3	Si	5																		1	1981																												Sc2Fe3Si5			A	10.435		5.475												K		2.3					2.3	MTC150200		K/GPa	3.3																																																																																												arc-melting					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150201	PSP1981381	Tc by ac-SUS. hydrostatic pressure. Tc(max) in this series.	(Y,Lu)2Fe3Si5	Y1.968Lu0.032Fe3Si5	Y	1.968	Lu	0.032	Fe	3	Si	5																1	1981																												Sc2Fe3Si5																		K		2.9					2.9	MTC150201																																																																																															two step arc-melting. first (Y2Fe3Si5 and Y0.9R0.1Fe3Si5), then combining them					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150202	PSP1981381	Tc by ac-SUS. hydrostatic pressure.	(Y,Lu)2Fe3Si5	Y1.68Lu0.32Fe3Si5	Y	1.68	Lu	0.32	Fe	3	Si	5																1	1981																												Sc2Fe3Si5																		K		0.98					0.98																																																																																																two step arc-melting. first (Y2Fe3Si5 and Y0.9R0.1Fe3Si5), then combining them					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150203	PSP1981381	Tc by ac-SUS. hydrostatic pressure. Tc(max) in this series.	(Y,Dy)2Fe3Si5	Y1.9Dy0.1Fe3Si5	Y	1.9	Dy	0.1	Fe	3	Si	5																1	1981																												Sc2Fe3Si5																		K		2.75					2.75	MTC150203																																																																																															two step arc-melting. first (Y2Fe3Si5 and Y0.9R0.1Fe3Si5), then combining them					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150204	PSP1981381	Tc by ac-SUS. hydrostatic pressure.	(Y,Dy)2Fe3Si5	Y1.6Lu0.4Fe3Si5	Y	1.6	Lu	0.4	Fe	3	Si	5																1	1981																												Sc2Fe3Si5																		K		1.65					1.65																																																																																																two step arc-melting. first (Y2Fe3Si5 and Y0.9R0.1Fe3Si5), then combining them					Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150205	JPE0210841	Tc(p) = 7.20 - 0.365*P(GPa) for P < 13 GPa. Tc-discontinuity at 13 GPa (fcc-to-hcp) not detected.	Pb	Pb1	Pb	1																							1988																																														K		7.2					7.2	MTC150205		K/GPa	-0.365																																																																																																	A diamond anvil cell for the investigation of superconductivity under pressures of up to 50 GPa: Pb as a low temperature manometer				J.Phys.E: Sci.Instrum., 21(1988)841	B.Bireckoven,J.Wittig		
150206	JPE0210841	P-induced SC. P(crit) = 35 GPa. Tc shows Tc(max) at P=50 GPa.	Sr	Sr1	Sr	1																							1988																																														K		7			0		7	MTC150206																																																																																																				A diamond anvil cell for the investigation of superconductivity under pressures of up to 50 GPa: Pb as a low temperature manometer				J.Phys.E: Sci.Instrum., 21(1988)841	B.Bireckoven,J.Wittig		
150207	PSP1981381	"Original data in ""High pressure and low temperature physics"" Plenum,New York, 1978: p=409"	ThRh4B4	Th1Rh4B4	Th	1	Rh	4	B	4																			1981																										AB4C4		RT4B4																	CeCo4B4 type	K		4.5					4.5			K/GPa	-0.066																																																																																																	Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150208	PSP1981381	"Original data in ""Superconductivity in d- and f-band metals"" Plenum, New York,1976: p=137"	LaMo6S8	La1Mo6S8	La	1	Mo	6	S	8																			1981																												Chevrel																		K		7					7			K/GPa	-1.42																																																																																																	Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150209	PSP1981381		AgSnSe2	Ag1Sn1Se2	Ag	1	Sn	1	Se	2																			1981																																														K		4.7					4.7			K/GPa	-0.73																																																																																																	Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150210	PSP1981381	Original data in Mat.Res.Bull., 10(1975)1111	La3Se4	La3Se4	La	3	Se	4																					1981																																														K		7.6					7.6			K/GPa	3																																																																																																	Nonlinear pressure effects in superconducting rare earth-iron-silicides (North Holland)			Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, California	Phys.Solids under High Pres(1981)381	C.U.Segre,H.F.Braun		
150211	MRS1984017	P-induced SC. Tc=4K (Sb-III) at 250 kbar. P<crit> = 50 kbar.	Sb	Sb1	Sb	1																							1984																																													Sb-I(P<85kbar), Sb-II(85<P<250), Sb-III(P>250 kbar)	K		0.7			0		0.7	MTC150211																																																																																																				Superconductivity in elements and binary systems at high pressure				MRS Proc.No.22(1984)P=17	J.Wittig		
150212	MRS1984017	P-induced SC. P<crit> = 120 kbar.	As	As1	As	1																							1984																																														K		2			0		2	MTC150212																																																																																																				Superconductivity in elements and binary systems at high pressure				MRS Proc.No.22(1984)P=17	J.Wittig		
150213	MRS1984017	P-induced SC.  P<crit> = 275 kbar.	Lu	Lu1	Lu	1																							1984																																														K		1.5			0		1.5																																																																																																					Superconductivity in elements and binary systems at high pressure				MRS Proc.No.22(1984)P=17	J.Wittig		
150214	JPS0741903	SP-heat by ac calorimetry. Tc(SP) = 0.46 K. AF for P < 0.6 GPa. SC for P < 1.5 GPa.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		3	2005								2.25																				CePt3B	P4mm																	K		0.7					0.7	MTC150214																																																																																															See J.Phys:Condens.Matter, 16(2004)L333					Novel Pressure Phase Diagram of Heavy Fermion Superconductor CePt3Si Investigated by ac Calorimetry			Advanced Science Research Center, Japan Atomic Energy Research Institute, Tokai, Ibaraki 319-1195	J.Phys.Soc.Jpn, 74(2005)1903	N.Tateiwa,Y.Haga,T.D.Matsuda,S.Ikeda,T.Yasuda,T.Takeuchi,R.Settai,Y.Onuki		
150215	PHB3590360		CePt3(Si,Ge)	Ce1Pt3Si0.97Ge0.03	Ce	1	Pt	3	Si	0.97	Ge	0.03																	2005								2.65																				CePt3B			A	4.0771		5.4479												K		0.63					0.63																																																																																																					Unconventional superconductivity and magnetism in CePt3Si1-xGex			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Physica B, 359-361(2005)360	E.Bauer,G.Hilscher,H.Michor,M.Sieberer,E.W.Scheidt,A.Gribanov,Yu.Seropegin,P.Rogl,A.Amato,W.Y.Song,J.-G.Park,D.T.Adroja,M.Nicklas,G.Sparn,M.Yogi,Y.Kitaoka		
150216	PHB3590360		CePt3(Si,Ge)	Ce1Pt3Si0.94Ge0.06	Ce	1	Pt	3	Si	0.94	Ge	0.06																	2005								2.79																				CePt3B			A	4.0787		5.4529												K		0.56					0.56	MTC150215																																																																																																				Unconventional superconductivity and magnetism in CePt3Si1-xGex			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Physica B, 359-361(2005)360	E.Bauer,G.Hilscher,H.Michor,M.Sieberer,E.W.Scheidt,A.Gribanov,Yu.Seropegin,P.Rogl,A.Amato,W.Y.Song,J.-G.Park,D.T.Adroja,M.Nicklas,G.Sparn,M.Yogi,Y.Kitaoka		
150217	PHB3590360		CePt3(Si,Ge)	Ce1Pt3Si0.9Ge0.1	Ce	1	Pt	3	Si	0.9	Ge	0.1																	2005								3.2																				CePt3B			A	4.0805		5.4579												K		0.31					0.31																																																																																																					Unconventional superconductivity and magnetism in CePt3Si1-xGex			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Physica B, 359-361(2005)360	E.Bauer,G.Hilscher,H.Michor,M.Sieberer,E.W.Scheidt,A.Gribanov,Yu.Seropegin,P.Rogl,A.Amato,W.Y.Song,J.-G.Park,D.T.Adroja,M.Nicklas,G.Sparn,M.Yogi,Y.Kitaoka		
150218	PHB3590386	Tn defined as max of (dR/dT). (dTn/dP) = -0.9 K/GPa. AF for P < 0.5 GPa.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		1	2005								2.2																			2	CePt3B																		K		0.75					0.75	MTC150218		K/GPa	-0.18																																																																																												rf-melting, then ANN(870C,10d)					Effect of hydrostatic pressure on the ambient pressure superconductor CePt3Si			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Str. 40, 01187 Dresden, Germany	Physica B, 359-361(2005)386	M.Nicklas,G.Sparn,R.Lackner,E.Bauer,F.Steglich		
150219	P076024513		CuxTiSe2	Cu0.055Ti1Se2	Cu	0.055	Ti	1	Se	2																		3	2007																												1T-MX2			A			6.0266												K			2.24				2.24																																																																																																					Transport properties of single-crystalline CuxTiSe2 (0.015=<x=<0.110)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People¿s Republic of China	Phys.Rev.B, 76(2007)024513	G.Wu,H.X.Yang,L.Zhao,X.G.Luo,T.Wu,G.Y.Wang,X.H,Chen		
150220	P076024513		CuxTiSe2	Cu0.065Ti1Se2	Cu	0.065	Ti	1	Se	2																		3	2007																												1T-MX2			A			6.0315												K			3.4				3.4																																																																		uV/K				MTP150220															E-3 cm3/C						MRH150220										Transport properties of single-crystalline CuxTiSe2 (0.015=<x=<0.110)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People¿s Republic of China	Phys.Rev.B, 76(2007)024513	G.Wu,H.X.Yang,L.Zhao,X.G.Luo,T.Wu,G.Y.Wang,X.H,Chen		
150221	P076024513		CuxTiSe2	Cu0.08Ti1Se2	Cu	0.08	Ti	1	Se	2																		3	2007																												1T-MX2																		K			4.13				4.13																																																																																																					Transport properties of single-crystalline CuxTiSe2 (0.015=<x=<0.110)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People¿s Republic of China	Phys.Rev.B, 76(2007)024513	G.Wu,H.X.Yang,L.Zhao,X.G.Luo,T.Wu,G.Y.Wang,X.H,Chen		
150222	P076024513		CuxTiSe2	Cu0.1Ti1Se2	Cu	0.1	Ti	1	Se	2																		3	2007																												1T-MX2			A			6.0428												K			3.02				3.02																																																																																																					Transport properties of single-crystalline CuxTiSe2 (0.015=<x=<0.110)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People¿s Republic of China	Phys.Rev.B, 76(2007)024513	G.Wu,H.X.Yang,L.Zhao,X.G.Luo,T.Wu,G.Y.Wang,X.H,Chen		
150223	P076024513	not SC	CuxTiSe2	Cu0.11Ti1Se2	Cu	0.11	Ti	1	Se	2																		3	2007																												1T-MX2			A			6.0455												K					1.8																																																																				uV/K				MTP150223															E-3 cm3/C						MRH150223										Transport properties of single-crystalline CuxTiSe2 (0.015=<x=<0.110)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People¿s Republic of China	Phys.Rev.B, 76(2007)024513	G.Wu,H.X.Yang,L.Zhao,X.G.Luo,T.Wu,G.Y.Wang,X.H,Chen		
150224	P076052511	Hc2 defined as inflection point in R(H).	CaC6	C6Ca1	C	6	Ca	1																				3	2007																												GIC																		K				11.5			11.5																				T	resistive		1.7	0.38										MHC150224		A			290	57																			175	from R(T) using Bloch-Gruneizen model																																									Anisotropic superconductivity in bulk CaC6			Department of Physics and National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 76(2007)052511	E.Jobiliong,H.D.Zhou,J.A.Janik,Y.-J.Jo,L.Balicas,J.S.Brooks,C.R.Wiebe		
150225	L098197001	P-induced SC. noncentrosymmetric. SC properties at 26 kbar. PHc2 means H//c-axis	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2007																												BaNiSn3																		K		1.09			0		1.09																				T			24	7					T/K			27	27	MHC150225																																																																			Extremely High Upper Critical Magnetic Field of the Noncentrosymmetric Heavy Fermion Superconductor CeRhSi3			Graduate School of Science, Tohoku University, Sendai, Miyagi 980-8578, Japan	Phys.Rev.Lett., 98(2007)197001	N.Kimura,K.Ito,H.Aoki,S.Uji,T.Terashima		
150226	L098197001	P-induced SC. noncentrosymmetric. SC properties at 29 kbar. Hc2 much larger than paramagnetic limit (1 T). PHc2 means H//c-axis	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2007																												BaNiSn3																		K		1.07			0		1.07	MTC150226																			T			30									18.7		MHC150226																																																																			Extremely High Upper Critical Magnetic Field of the Noncentrosymmetric Heavy Fermion Superconductor CeRhSi3			Graduate School of Science, Tohoku University, Sendai, Miyagi 980-8578, Japan	Phys.Rev.Lett., 98(2007)197001	N.Kimura,K.Ito,H.Aoki,S.Uji,T.Terashima		
150227	J076104705	As<75> NMR measured.	PrRu4As12	Pr1Ru4As12	Pr	1	Ru	4	As	12																		1	2007																												skutterudite																		K		2.3					2.3																																																3.2	6																																																				75As-NQR Studies of Superconducting Filled Skutterudites PrRu4As12 and LaRu4As12			Department of Physics, Graduate School of Science, Chiba University, Chiba 263-8522	J.Phys.Soc.Jpn, 76(2007)104705	M.Shimizu,H.Amanuma,K.Hachitani,H.Fukazawa,Y.Kohori,T.Namiki,C.Sekine,I.Shirotani		
150228	J076104705	As<75> NMR measured.	LaRu4As12	La1Ru4As12	La	1	Ru	4	As	12																		1	2007																												skutterudite																		K		10.3					10.3																																																3.7	6																																																				75As-NQR Studies of Superconducting Filled Skutterudites PrRu4As12 and LaRu4As12			Department of Physics, Graduate School of Science, Chiba University, Chiba 263-8522	J.Phys.Soc.Jpn, 76(2007)104705	M.Shimizu,H.Amanuma,K.Hachitani,H.Fukazawa,Y.Kohori,T.Namiki,C.Sekine,I.Shirotani		
150229	MRB0190115	ANN(400C,13d). Tc = 2.7 K before ANN(broad transition)	LaRhSi3	La1Rh1Si3	La	1	Rh	1	Si	3																			1984																											2	BaPtSn3			A	4.272		9.83												K		2.2					2.2																																																																																																					Crystal structure of new superconducting materials LaIrSi3 and LaRhSi3. Structural relation between LaRh2Si2, La2Rh3Si5 and LaRhSi3				Mat.Res.Bull., 19(1984)115	P.Lejay,I.Higashi,B.Chevalier,J.Etourneau,P.Hagenmuller		
150230	MRB0190115	Tc= 1.9 - 2.7 K	LaIrSi3	La1Ir1Si3	La	1	Ir	1	Si	3																			1984																											2	BaPtSn3			A	4.278		9.83												K		2.2					2.2																																																																																																					Crystal structure of new superconducting materials LaIrSi3 and LaRhSi3. Structural relation between LaRh2Si2, La2Rh3Si5 and LaRhSi3				Mat.Res.Bull., 19(1984)115	P.Lejay,I.Higashi,B.Chevalier,J.Etourneau,P.Hagenmuller		
150231	LES0690389	Tc by mutual inductance.	CaSi2	Ca1Si2	Ca	1	Si	2																					1980																												a-ThSi2																		K		1.37					1.37																																																																																																melt by induction heat in Cu-boat. High-pressure synthesis(1000C,15min,P=40 kbar), then quench to RT					Superconductivity of SrSi2 and BaGe2 with the alpha-ThSi2-type structure				J.Less-Common Met., 69(1980)389	J.Evers,G.Oehlinger,H.R.Ott		
150232	LES0690389	Tc by mutual inductance.	CaSi1.9	Ca1Si1.9	Ca	1	Si	1.9																					1980																												a-ThSi2																		K		1.35					1.35																																																																																																melt by induction heat in Cu-boat. High-pressure synthesis(1000C,15min,P=40 kbar), then quench to RT					Superconductivity of SrSi2 and BaGe2 with the alpha-ThSi2-type structure				J.Less-Common Met., 69(1980)389	J.Evers,G.Oehlinger,H.R.Ott		
150233	LES0690389	Tc by mutual inductance.	CaSi2.2	Ca1Si2.2	Ca	1	Si	2.2																					1980																												a-ThSi2																		K		1.37					1.37																																																																																																melt by induction heat in Cu-boat. High-pressure synthesis(1000C,15min,P=40 kbar), then quench to RT					Superconductivity of SrSi2 and BaGe2 with the alpha-ThSi2-type structure				J.Less-Common Met., 69(1980)389	J.Evers,G.Oehlinger,H.R.Ott		
150234	LES0690389	Tc by mutual inductance.	SrSi2	Si2Sr1	Si	2	Sr	1																					1980																												a-ThSi2																		K		3.1					3.1																																																																																																melt by induction heat in Cu-boat. High-pressure synthesis(1000C,15min,P=40 kbar), then quench to RT					Superconductivity of SrSi2 and BaGe2 with the alpha-ThSi2-type structure				J.Less-Common Met., 69(1980)389	J.Evers,G.Oehlinger,H.R.Ott		
150235	LES0690389	Tc by mutual inductance.	BaGe2	Ba1Ge2	Ba	1	Ge	2																					1980																												a-ThSi2																		K		4.93					4.93																																																																																																melt by induction heat in Cu-boat. High-pressure synthesis(1000C,15min,P=40 kbar), then quench to RT					Superconductivity of SrSi2 and BaGe2 with the alpha-ThSi2-type structure				J.Less-Common Met., 69(1980)389	J.Evers,G.Oehlinger,H.R.Ott		
150236	LES0810349	Tc by mutual inductance.	YTc2	Tc2Y1	Tc	2	Y	1																					1981																												MgZn2(Laves)			A	5.371		8.862											MgZn2, C14, Laves	K		8.8				0.3	8.8																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150237	LES0810349	Tc by mutual inductance.	ScTc2	Sc1Tc2	Sc	1	Tc	2																					1981																												MgZn2(Laves)			A	5.224		8.57											MgZn2, C14, Laves	K		10.9				0.2	10.9																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150238	LES0810349	Tc by mutual inductance.	LuTc2	Lu1Tc2	Lu	1	Tc	2																					1981																												MgZn2(Laves)			A	5.31		8.736											MgZn2, C14, Laves	K		9.9				0.2	9.9																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150239	LES0810349	Tc by mutual inductance.	ScRe2	Re2Sc1	Re	2	Sc	1																					1981																												MgZn2(Laves)			A	5.263		8.584											MgZn2, C14, Laves	K		0.93				0.07	0.93																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150240	LES0810349	Tc by mutual inductance.	YRe2	Re2Y1	Re	2	Y	1																					1981																												MgZn2(Laves)			A	5.396		8.819											MgZn2, C14, Laves	K		1.83					1.83																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150241	LES0810349	Tc by mutual inductance.	LuRe2	Lu1Re2	Lu	1	Re	2																					1981																												MgZn2(Laves)			A	5.342		8.722											MgZn2, C14, Laves	K		1.7				0.07	1.7																																																																																																arc-melting, then ANN(1000C,24h)					Superconductivity of the Laves Phases YTc2, ScTc2 and LuTc2			Los Alamos Scientific Laboratory, University of California, Los Alamos, NM	J.Less-Common Met., 81(1981)349	E.G.Szklarz,A.L.Giorgi		
150242	LES0820193		(Mo,Zr)2BC	Mo1.965Zr0.035B1C1	Mo	1.965	Zr	0.035	B	1	C	1																	1981																												Mo2BC	Cmcm																	K		6.9					6.9	MTC150242																																																																																															arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150243	LES0820193		(Mo,Zr)2BC	Mo1.935Zr0.065B1C1	Mo	1.935	Zr	0.065	B	1	C	1																	1981																												Mo2BC	Cmcm																	K		6.2					6.2																																																																																																arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150244	LES0820193		(Mo,Nb])2BC	Mo1.9Nb0.1B1C1	Mo	1.9	Nb	0.1	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.0935	17.359	3.063												K		6.7					6.7	MTC150242																																																																																															arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150245	LES0820193		(Mo,Nb)2BC	Mo1.85Nb0.15B1C1	Mo	1.85	Nb	0.15	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.1043	17.373	3.0696												K		6.2					6.2																																																																																																arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150246	LES0820193		(Mo,Hf)2BC	Mo1.94Hf0.06B1C1	Mo	1.94	Hf	0.06	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.0955	17.378	3.0545												K		5.8					5.8	MTC150242																																																																																															arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150247	LES0820193		(Mo,Hf)2BC	Mo1.905Hf0.095B1C1	Mo	1.905	Hf	0.095	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.1045	17.408	3.0636												K		5					5																																																																																																arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150248	LES0820193		(Mo,Ta)2BC	Mo1.86Ta0.14B1C1	Mo	1.86	Ta	0.14	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.0932	17.366	3.0545												K		5.6					5.6	MTC150250																																																																																															arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150249	LES0820193		(Mo,Ta)2BC	Mo1.7Ta0.3B1C1	Mo	1.7	Ta	0.3	B	1	C	1																	1981																												Mo2BC	Cmcm		A	3.0977	17.375	3.0614												K		4.6					4.6																																																																																																arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150250	LES0820193		(Mo,W)2BC	Mo1.8W0.2B1C1	Mo	1.8	W	0.2	B	1	C	1																1	1981																												Mo2BC			A	3.0848	17.332	3.0467												K		6.82					6.82	MTC150250																																	MHC150250																																																														arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150251	LES0820193		(Mo,Rh)2BC	Mo1.8Rh0.2B1C1	Mo	1.8	Rh	0.2	B	1	C	1																1	1981																												Mo2BC			A	3.0828	17.325	3.0433												K		9.1					9.1	MTC150251																																	MHC150250																																																														arc-melting					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150252	LES0820193		Mo2BC	Mo2B1C1	Mo	2	B	1	C	1																		3	1981																												Mo2BC																		K		7.5					7.5																																		MHC150252																																																														Czochralski method					Influence of some metal substitutions on the superconducting behaviour of mokybdenum borocarbide				J.Less-Common Met., 82(1981)193	P.Lejay,B.Chevalier,J.Etourneau,P.Hagenmuller		
150253	P076064504	25-days-aged(RT) sample. nominal sample (Tc=18.5 K). Gap & PENET obtained using model fitting of muon-SR.	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2007																												HoCoGa5																		K		18.25					18.25																																									A	muon-SR	2650					6	16																																															crystals were grown using excess Ga flux. c-axis normal to surface.					Muon spin rotation measurements of the superfluid density in fresh and aged superconducting PuCoGa5			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	Phys.Rev.B, 76(2007)064504	K.Ohishi,R.H.Heffner,G.D.Morris,E.D.Bauer,M.J.Graf,J.-X.Zhu,L.A.Morales,J.L.Sarrao,M.J.Fluss,D.E.MacLaughlin,L.Shu,W.Higemoto,T.U.Ito		
150254	P076064508	isotope exponent = 0.07 +-0.04	LixZrNCl	Li0.18Zr1N1Cl1	Li	0.18	Zr	1	N	1	Cl	1																	2007																																														K				11.6			11.6						0.07	N																																																																																									beta-ZrNCl synthesized using CVT. Li-doping usig n-BuLi/hexane solution					Isotope effect in LixZrNCl superconductors			1Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.B, 76(2007)064508	Y.Taguchi,T.Kawabata,T.Takano,A.Kitora,K.Kato,M.Takata,Y.Iwasa		
150255	P076064527	"Authers say""[gamma] is 43.9 mJ/mol.K2, calculated from true SC volume"". Lattice term coeff.  in SP = 5.4 mJ/mol.K4. e-ph = 0.68."	Mg12Ir19B16	Mg12Ir19B16	Mg	12	Ir	19	B	16																			2007																													I-43m																	K				5.7			5.7																				T		2.48							T/K		0.63			MHC150255												meV	0.94	3.82	14							mJ/mol.K2	57.7		253	SP-heat																																		Mg,Ir,B		mixture - pellet - sealed in quartz(95%Ar + 5%H) - heat(600C,40min + 900C,80min) reground - ADD(execc upto 20%Mg) - heat(900C)					Possible nodeless superconductivity in the noncentrosymmetric superconductor Mg(12-delta)Ir19B16			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100080, China	Phys.Rev.B, 76(2007)064527	Gang Mu,Y.Wang,L.Shan,Hai-Hu Wen		
150256	MRB0180067		Th(Rh,Si)2	Th1Rh0.1Si1.9	Th	1	Rh	0.1	Si	1.9																			1983																												alpha-ThSi2			A	4.1106		14.1033												K		2.15					2.15																																																																																																					A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150257	MRB0180067		Th(Rh,Si)2	Th1Rh0.85Si1.15	Th	1	Rh	0.85	Si	1.15																			1983																												alpha-ThSi2			A	4.1024		14.3974												K		5.48					5.48	MTC150257																																																																																																				A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150258	MRB0180067		Th(Ir,Si)2	Th1Ir0.1Si1.9	Th	1	Ir	0.1	Si	1.9																			1983																												alpha-ThSi2			A	4.1167		14.0556												K		2.75					2.75																																																																																																					A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150259	MRB0180067		Th(Ir,Si)2	Th1Ir0.75Si1.25	Th	1	Ir	0.75	Si	1.25																			1983																												alpha-ThSi2			A	4.1214		14.4048												K		3.82					3.82	MTC150259																																																																																																				A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150260	P076064504	400-days-aged(RT) sample. nominal sample (Tc=18.5 K). Gap & PENET obtained using model fitting of muon-SR.	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2007																												HoCoGa5																		K		15					15																																									A	muon-SR	4980					4.8	16																																															crystals were grown using excess Ga flux. c-axis normal to surface.					Muon spin rotation measurements of the superfluid density in fresh and aged superconducting PuCoGa5			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	Phys.Rev.B, 76(2007)064504	K.Ohishi,R.H.Heffner,G.D.Morris,E.D.Bauer,M.J.Graf,J.-X.Zhu,L.A.Morales,J.L.Sarrao,M.J.Fluss,D.E.MacLaughlin,L.Shu,W.Higemoto,T.U.Ito		
150261	MRB0180067		ThIrSi	Th1Ir1Si1	Th	1	Ir	1	Si	1																			1983																												alpha-ThSi2			A	4.142		14.265												K		6.5					6.5																																																																																																					A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150262	MRB0180067		ThSi2	Si2Th1	Si	2	Th	1																					1983																												alpha-ThSi2																		K		3.14					3.14																																																																																																					A new family of superconducting silicides: The ThMxSi2-x compounds (M = Rh or Ir with 0< x <1 of alpha-ThSi2-type structure				Mat.Res.Bull., 18(1983)67	P.Lejay,B.Chevalier,J.Etourneau,J.M.Tarascon,P.Hagenmuller		
150264	SSC0410801	not SC down to 1.6 K.	GdIrSi	Gd1Ir1Si1	Gd	1	Ir	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150265	SSC0410801	not SC down to 1.6 K.	TbIrSi	Tb1Ir1Si1	Tb	1	Ir	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150266	SSC0410801	not SC down to 1.6 K.	DyIrSi	Dy1Ir1Si1	Dy	1	Ir	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150267	SSC0410801	not SC down to 1.6 K.	HoIrSi	Ho1Ir1Si1	Ho	1	Ir	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150268	SSC0410801	not SC down to 1.6 K.	ErIrSi	Er1Ir1Si1	Er	1	Ir	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150270	SSC0410801	not SC down to 1.6 K.	YRhSi	Y1Rh1Si1	Y	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150271	SSC0410801	not SC down to 1.6 K.	GdRhSi	Gd1Rh1Si1	Gd	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150272	SSC0410801	not SC down to 1.6 K.	TbRhSi	Tb1Rh1Si1	Tb	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150273	SSC0410801	not SC down to 1.6 K.	DyRhSi	Dy1Rh1Si1	Dy	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150274	SSC0410801	not SC down to 1.6 K.	HoRhSi	Ho1Rh1Si1	Ho	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150275	SSC0410801	not SC down to 1.6 K.	ErRhSi	Er1Rh1Si1	Er	1	Rh	1	Si	1																			1982																												TiNiSi																		K					1.6																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150276	SSC0410801		LaRhSi	La1Rh1Si1	La	1	Rh	1	Si	1																			1982									7.11																			ZrOs	P2<1>3		A	6.296														K		4.35					4.35																																																																																																arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150277	SSC0410801		LaIrSi	La1Ir1Si1	La	1	Ir	1	Si	1																			1982									9.18																			ZrOs	P2<1>3		A	6.337														K		2.3					2.3																																																																																																arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150278	SSC0410801	not SC down to 4.2 K.	NdIrSi	Nd1Ir1Si1	Nd	1	Ir	1	Si	1																			1982							10		10.237																			ZrOs	P2<1>3		A	6.185														K					4.2																																																																																																		arc-melting					Crystal structure, superconducting and magnetic properties of new ternary silicides LaRhSi, LaIrSi and NdIrSi				Solid State Commun., 41(1982)801	B.Chevalier,P.Lajay,A.Cole,M.Vlasse,J.Etourneau		
150279	PHC1620407	gamma'-phase	gamma'-Y5Os4Si15	Y5Os4Si15	Y	5	Os	4	Si	15																			1989																																														K		10.8					10.8			K/GPa	-0.58																																																																																																	Superconductivity under hydrostatic pressure in RE5Os4Si15 compounds (RE = Y, Tb, Er)				Physica C, 162-164(1989)407	M.Kuboth,H.F.Braun,L.Schellenberg,J.Muller		
150280	PHC1620407	gamma'-phase	gamma'-Er5Os4Si15	Er5Os4Si15	Er	5	Os	4	Si	15																			1989																																														K		5.5					5.5			K/GPa	-1.08																																																																																																	Superconductivity under hydrostatic pressure in RE5Os4Si15 compounds (RE = Y, Tb, Er)				Physica C, 162-164(1989)407	M.Kuboth,H.F.Braun,L.Schellenberg,J.Muller		
150281	PHC1620407	gamma'-phase	gamma'-Tb5Os4Si15	Tb5Os4Si15	Tb	5	Os	4	Si	15																			1989																																														K		3.2					3.2			K/GPa	-0.73																																																																																																	Superconductivity under hydrostatic pressure in RE5Os4Si15 compounds (RE = Y, Tb, Er)				Physica C, 162-164(1989)407	M.Kuboth,H.F.Braun,L.Schellenberg,J.Muller		
150282	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Gd5Os4Si15	Gd5Os4Si15	Gd	5	Os	4	Si	15																			1988																																														K					1.1																																																																																																		arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150283	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Tb5Os4Si15	Tb5Os4Si15	Tb	5	Os	4	Si	15																			1988																																														K		3.2					3.2																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150284	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Dy5Os4Si15	Dy5Os4Si15	Dy	5	Os	4	Si	15																			1988																																														K		3.5					3.5																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150285	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Ho5Os4Si15	Ho5Os4Si15	Ho	5	Os	4	Si	15																			1988																																														K		4.5					4.5																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150286	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Er5Os4Si15	Er5Os4Si15	Er	5	Os	4	Si	15																			1988																																														K		5.5					5.5																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150287	PHC1530485	gamma'-phase. Tc by inductive method.	gamma'-Y5Os4Si15	Y5Os4Si15	Y	5	Os	4	Si	15																			1988																																														K		10.8					10.8																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150288	PHC1530485	beta'-phase	beta'-Tb4Os4Si13	Tb4Os4Si13	Tb	4	Os	4	Si	13																			1988																																														K					1.1																																																																																																		arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150289	PHC1530485	beta'-phase	beta'-Dy4Os4Si13	Dy4Os4Si13	Dy	4	Os	4	Si	13																			1988																																														K					1.1																																																																																																		arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150290	PHC1530485	beta'-phase	beta'-Ho4Os4Si13	Ho4Os4Si13	Ho	4	Os	4	Si	13																			1988																																														K					1.1																																																																																																		arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150291	PHC1530485	beta'-phase	beta'-Er4Os4Si13	Er4Os4Si13	Er	4	Os	4	Si	13																			1988																																														K					1.1																																																																																																		arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150292	PHC1530485	beta'-phase	beta'-Tm4Os4Si13	Tm4Os4Si13	Tm	4	Os	4	Si	13																			1988																																														K		2.6					2.6																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150293	PHC1530485	beta'-phase	beta'-Y4Os4Si13	Y4Os4Si13	Y	4	Os	4	Si	13																			1988																																														K		9.8					9.8																																																																																																arc-melting - ANN(1150C,1d, in vac)					Superconductivity in silicon-rich RE-OS-Si compounds				Physica C, 153-155(1988)485	L.Schellenberg,H.F.Braun,C.U.Segre,M.Gueramian,B.Chabot,M.Decroux,D.Gattani,J.Muller		
150294	SCI1750884	superconducting for 0.1< x =<0.3 in LixTi1.1S2.	LixTiS2	Li0.3Ti1.1S2	Li	0.3	Ti	1.1	S	2																			1972																											7	Ti3S4			A	3.439		11.511												K		13					13																																																																																																ANN(600C)					Superconductivity of double chalcogenides: LixTi1.1S2				Science, 175(1972)884	H.E.Barz,A.S.Cooper,E.Corenzwit,M.Marezio,B.T.Matthias,P.H.Schmidt		
150295	SCI1750884		TiS2	S2Ti1	S	2	Ti	1																					1972																												CdI2																		K				45	1.12		45																																																																																																ANN(600C)					Superconductivity of double chalcogenides: LixTi1.1S2				Science, 175(1972)884	H.E.Barz,A.S.Cooper,E.Corenzwit,M.Marezio,B.T.Matthias,P.H.Schmidt		
150296	SCI2540826	ANN(400C,12h) + ANN(430C,6h)	Rb2.7Tl2.2C60	Rb2.7Tl2.2C60	Rb	2.7	Tl	2.2	C	60																			1991																												fullerene																		K				23.2			23.2																																																																																																					Superconductivity at 45 K in Rb/Tl codoped C60 and C60/C70 mixtures				Science, 254(1991)826	Z.Iqbal,R.H.Baughman,B.L.Ramakrishna,S.Khare,N.S.Murthy,H.J.Bornemann,D.E.Morris		
150297	SCI2540826	ANN(400C,12h) + ANN(430C,16h)	K3Tl4.5C60	K3Tl4.5C60	K	3	Tl	4.5	C	60																			1991																												fullerene																		K																																																																																																												Superconductivity at 45 K in Rb/Tl codoped C60 and C60/C70 mixtures				Science, 254(1991)826	Z.Iqbal,R.H.Baughman,B.L.Ramakrishna,S.Khare,N.S.Murthy,H.J.Bornemann,D.E.Morris		
150298	PHB1350397	as-quenched. (dC/gamma*Tc) = 1.3	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																		1	1985																												CaBe2Ge2			A	4.188		9.94											pt(primitive tetragonal)	K		1.56					1.56																																																								mJ/gat.K2	1.7	SP heat	300																																					arc-melting					Specific heat and bandstructure of two polymorphs of LaIr2Si2				Physica B, 135(1985)397	H.F.Braun,T.Jarlborg,A.Junod		
150299	PHB1350397	ANN(1000C,6d). not SC (Tc < 1.2)	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																		1	1985																												ThCr2Si2			A	4.107		10.292											bct(body centered tetragonal)	K					1.2																																																										mJ/gat.K2	0.9	SP heat	385																																					arc-melting					Specific heat and bandstructure of two polymorphs of LaIr2Si2				Physica B, 135(1985)397	H.F.Braun,T.Jarlborg,A.Junod		
150300	SSC0390797	Tc by ac method. (dTc/dP) determined from the least squares fit.	AgSnSe2	Ag1Sn1Se2	Ag	1	Sn	1	Se	2																			1981																												NaCl																		K		4.66				0.02	4.66			K/GPa	-0.73																																																																																																	Hydrostatic pressure effects on the superconducting properties of Ag1-xSn1+xSe2			Ames Laboratory, Iowa State University,Ames, IA	Solid State Commun., 39(1981)797	R.N.Shelton,C.U.Segre,D.C.Johnston		
150301	SSC0390797	Tc by ac method. (dTc/dP) determined from the least squares fit.	Ag1-xSn1+xSe2	Ag0.95Sn1.05Se2	Ag	0.95	Sn	1.05	Se	2																			1981																												NaCl																		K		5.21				0.01	5.21			K/GPa	-0.756																																																																																																	Hydrostatic pressure effects on the superconducting properties of Ag1-xSn1+xSe2			Ames Laboratory, Iowa State University,Ames, IA	Solid State Commun., 39(1981)797	R.N.Shelton,C.U.Segre,D.C.Johnston		
150302	SSC0390797	Tc by ac method. (dTc/dP) determined from the least squares fit.	Ag1-xSn1+xSe2	Ag0.85Sn1.15Se2	Ag	0.85	Sn	1.15	Se	2																			1981																												NaCl																		K		6.12				0.08	6.12			K/GPa	-0.767																																																																																																	Hydrostatic pressure effects on the superconducting properties of Ag1-xSn1+xSe2			Ames Laboratory, Iowa State University,Ames, IA	Solid State Commun., 39(1981)797	R.N.Shelton,C.U.Segre,D.C.Johnston		
150303	SSC0390797	Tc by ac method. (dTc/dP) determined from the least squares fit.	Ag1-xSn1+xSe2	Ag0.81Sn1.19Se2	Ag	0.81	Sn	1.19	Se	2																			1981																												NaCl																		K		6.36				0.03	6.36			K/GPa	-0.784																																																																																																	Hydrostatic pressure effects on the superconducting properties of Ag1-xSn1+xSe2			Ames Laboratory, Iowa State University,Ames, IA	Solid State Commun., 39(1981)797	R.N.Shelton,C.U.Segre,D.C.Johnston		
150304	SSC0390797	Tc by ac method. (dTc/dP) determined from the least squares fit.	Ag1-xSn1+xSe2	Ag0.76Sn1.24Se2	Ag	0.76	Sn	1.24	Se	2																			1981																												NaCl																		K		6.72				0.1	6.72			K/GPa	-0.68																																																																																																	Hydrostatic pressure effects on the superconducting properties of Ag1-xSn1+xSe2			Ames Laboratory, Iowa State University,Ames, IA	Solid State Commun., 39(1981)797	R.N.Shelton,C.U.Segre,D.C.Johnston		
150305	PR0281389	HT-phase(T>1750C),	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																			1983																												CaBe2Ge2			A	4.191		9.944											CaBe2Ge2, tP10	K		1.58				0.18	1.58																																																																																																arc-melting - ANN(1000C,in vac)					Polymorphism and superconductivity of LaIr2Si2				Phys.Rev.B, 28(1983)1389	H.F.Braun,N.Engel,E.Parthe		
150306	PR0281389	LT-phase(T < 1750C)	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																			1983																												ThCr2Si2			A	4.109		10.299											ThCr2Si2, tI10	K					1																																																																																																		arc-melting - ANN(1000C,in vac)					Polymorphism and superconductivity of LaIr2Si2				Phys.Rev.B, 28(1983)1389	H.F.Braun,N.Engel,E.Parthe		
150307	L099067006	nominal(U1.02Co1.02Ge). RRR = 25. Weak itinerant ferro. SP-heat & thermal expansion measured.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																			2007							3																					TiNiSi			A	6.845	4.206	7.222												K	0.66			0.8			0.8																													T/K		5.2			MHC150307		A	from dHc2/dT	150																		mJ/mol.K2	57														mOhm.cm							0.012																		arc-melting - ANN(850C,10d)					Superconductivity on the Border of Weak Itinerant Ferromagnetism in UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.Lett., 99(2007)067006	N.T.Huy,A.Gasparini,D.E.de Nijs,Y.Huang,J.C.P.Klaasse,T.Gortenmulder,A.de Visser,A.Hamann,T.Gorlach,H.v.Lohneysen		
150308	L099067006	nominal(U1.02CoGe). RRR = 10.  SP-heat & thermal expansion measured.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																			2007																												TiNiSi																		K		0.45					0.45																													T/K		7.2			MHC150307		A	from dHc2/dT	200																																																										arc-melting - ANN(850C,10d)					Superconductivity on the Border of Weak Itinerant Ferromagnetism in UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.Lett., 99(2007)067006	N.T.Huy,A.Gasparini,D.E.de Nijs,Y.Huang,J.C.P.Klaasse,T.Gortenmulder,A.de Visser,A.Hamann,T.Gorlach,H.v.Lohneysen		
150309	P076092501	Na,H-content not given. Mn-doping confiemed by EXAFS. (dTc/dz) = 0.64 K/%Mn	Nax(Co,Mn)O2/yH2O	Na0.3Co0.995Mn0.005H2.6O3.3	Na	0.3	Co	0.995	Mn	0.005	H	2.6													O		3.3		2007																																																4.05					4.05																																																																																																					Effect of Mn impurities on the superconductivity in NaxCoO2 /yH2O			Institute of Physics, National Chiao Tung University, Hsinchu 300, Taiwan	Phys.Rev.B, 76(2007)092501	Y.-J.Chen,C.-J.Liu,J.-S.Wang,J.-Y.Lin,C.P.Sun,S.W.Huang,J.M.Lee,J.M.Chen,J.F.Lee,D.G.Liu,H.D.Yang		
150310	P076092501	Na,H-content not given. Mn-doping confiemed by EXAFS. (dTc/dz) = 0.64 K/%Mn	Nax(Co,Mn)O2/yH2O	Na0.3Co0.985Mn0.015H2.6O3.3	Na	0.3	Co	0.985	Mn	0.015	H	2.6													O		3.3		2007																																																3.34					3.34	MTC150310																																																																																																				Effect of Mn impurities on the superconductivity in NaxCoO2 /yH2O			Institute of Physics, National Chiao Tung University, Hsinchu 300, Taiwan	Phys.Rev.B, 76(2007)092501	Y.-J.Chen,C.-J.Liu,J.-S.Wang,J.-Y.Lin,C.P.Sun,S.W.Huang,J.M.Lee,J.M.Chen,J.F.Lee,D.G.Liu,H.D.Yang		
150311	P076094505		(Ca,Na)2CuO2Cl2	Ca1.89Na0.11Cu1Cl2O2	Ca	1.89	Na	0.11	Cu	1	Cl	2													O	2			2007																												T																		K				15.14			15.14																																									A	from intrinsic SUS		4300																																																				precursor(Ca2CuO2Cl2) mixed with NaClO4, NaCl. Then  high-pressure synthesis(1350-1700 C, 1.5h, P=40 -45 kbar)					In-plane magnetic penetration depth ramda<ab>  in Ca2-xNaxCuO2Cl2: Role of the apical sites			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 76(2007)094505	R.Khasanov,N.D.Zhigadlo,J.Karpinski,H.Keller		
150312	P076094505	PPENET = 3900 A from muon-SR.	(Ca,Na)2CuO2Cl2	Ca1.88Na0.12Cu1Cl2O2	Ca	1.88	Na	0.12	Cu	1	Cl	2													O	2			2007																												T																		K				18.4			18.4																																									A	from intrinsic SUS		4060																																																				precursor(Ca2CuO2Cl2) mixed with NaClO4, NaCl. Then  high-pressure synthesis(1350-1700 C, 1.5h, P=40 -45 kbar)					In-plane magnetic penetration depth ramda<ab>  in Ca2-xNaxCuO2Cl2: Role of the apical sites			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 76(2007)094505	R.Khasanov,N.D.Zhigadlo,J.Karpinski,H.Keller		
150313	P076094505		(Ca,Na)2CuO2Cl2	Ca1.85Na0.15Cu1Cl2O2	Ca	1.85	Na	0.15	Cu	1	Cl	2													O	2			2007																												T																		K				23.45			23.45																																									A	from intrinsic SUS		3210																																																				precursor(Ca2CuO2Cl2) mixed with NaClO4, NaCl. Then  high-pressure synthesis(1350-1700 C, 1.5h, P=40 -45 kbar)					In-plane magnetic penetration depth ramda<ab>  in Ca2-xNaxCuO2Cl2: Role of the apical sites			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 76(2007)094505	R.Khasanov,N.D.Zhigadlo,J.Karpinski,H.Keller		
150314	P076094505	PPENET = 3170 A from muon-SR.	(Ca,Na)2CuO2Cl2	Ca1.82Na0.18Cu1Cl2O2	Ca	1.82	Na	0.18	Cu	1	Cl	2													O	2			2007																												T																		K				27.11			27.11																																									A	from intrinsic SUS		3170																																																				precursor(Ca2CuO2Cl2) mixed with NaClO4, NaCl. Then  high-pressure synthesis(1350-1700 C, 1.5h, P=40 -45 kbar)					In-plane magnetic penetration depth ramda<ab>  in Ca2-xNaxCuO2Cl2: Role of the apical sites			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 76(2007)094505	R.Khasanov,N.D.Zhigadlo,J.Karpinski,H.Keller		
150315	P076094505		(Ca,Na)2CuO2Cl2	Ca1.81Na0.19Cu1Cl2O2	Ca	1.81	Na	0.19	Cu	1	Cl	2													O	2			2007																												T																		K				27.7			27.7																																									A	from intrinsic SUS		3160																																																				precursor(Ca2CuO2Cl2) mixed with NaClO4, NaCl. Then  high-pressure synthesis(1350-1700 C, 1.5h, P=40 -45 kbar)					In-plane magnetic penetration depth ramda<ab>  in Ca2-xNaxCuO2Cl2: Role of the apical sites			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 76(2007)094505	R.Khasanov,N.D.Zhigadlo,J.Karpinski,H.Keller		
150316	P076100506	Na-content (=0.26 - 0.28) estimated from lattice constant.	NaxCoO2/1.3H2O	Na0.3Co1H2.6O3.3	Na	0.3	Co	1	H	2.6															O	3.3			2007																																														K		4.8					4.8	MTC150316																																																																																															See Nature, 422(2003)53					Pressure dependence of the superconducting transition and electron correlations in NaxCoO2/1.3H2O			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 76(2007)100506	E.Kusano,S.Kawasaki,K.Matano,Guo-qing Zheng,R.L.Meng,J.Cmaidalka,C.W.Chu		
150317	P076104506	RRR = 1.3. lattice term of SP(beta) = 1.1 mJ/mol.K4. Field dependent SP measured.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																			2007																													P4<3>32																	K		6.95					6.95																																																								mJ/mol.K2	9.3														mOhm.cm							0.115																		Two stage arc-melting					Specific-heat studies of the spin-orbit interaction in noncentrosymmetric Li2(Pd1-xPtx)3B (x=0,0.5,1) superconductors			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 76(2007)104506	H.Takeya,M.ElMassalami,S.Kasahara,K.Hirata		
150318	P076104506	RRR = 1.1. lattice term of SP(beta) = 0.95 mJ/mol.K4. Field dependent SP measured.	Li2(Pd,Pt)3B	Li2Pd1.5Pt1.5B1	Li	2	Pd	1.5	Pt	1.5	B	1																	2007																													P4<3>32																	K		3.9					3.9																																																								mJ/mol.K2	9.1														mOhm.cm							0.16																		Two stage arc-melting					Specific-heat studies of the spin-orbit interaction in noncentrosymmetric Li2(Pd1-xPtx)3B (x=0,0.5,1) superconductors			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 76(2007)104506	H.Takeya,M.ElMassalami,S.Kasahara,K.Hirata		
150319	P076104506	RRR = 1.2. lattice term of SP(beta) = 0.92 mJ/mol.K4. Field dependent SP measured.	Li2Pt3B	Li2Pt3B1	Li	2	Pt	3	B	1																			2007																													P4<3>32																	K		2.56					2.56																																																								mJ/mol.K2	9.3														mOhm.cm							0.105																		Two stage arc-melting					Specific-heat studies of the spin-orbit interaction in noncentrosymmetric Li2(Pd1-xPtx)3B (x=0,0.5,1) superconductors			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 76(2007)104506	H.Takeya,M.ElMassalami,S.Kasahara,K.Hirata		
150320	P076104508	2*Energy gap = (3.8-3.9) kTc by beak junction.	1H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2007																												AlB2																		K		6.1					6.1																																																3.9	1																																																				Superconducting energy gap from break-junction tunneling spectroscopy in the ternary silicide CaAlSi			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 76(2007)104508	S.Kuroiwa,T.Takasaki,T.Ekino,J.Akimitsu		
150321	P076104508	super lattice (5H-type). 2*Energy gap = (3.8-4.2) kTc by beak junction.	5H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2007																																														K		5.6					5.6																																																4.2	1																																																				Superconducting energy gap from break-junction tunneling spectroscopy in the ternary silicide CaAlSi			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 76(2007)104508	S.Kuroiwa,T.Takasaki,T.Ekino,J.Akimitsu		
150322	P076104508	super lattice (6H-type). 2*Energy gap = (4.4-4.9) kTc by beak junction.	6H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2007																																														K		7.1					7.1																																																4.9	1																																																				Superconducting energy gap from break-junction tunneling spectroscopy in the ternary silicide CaAlSi			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 76(2007)104508	S.Kuroiwa,T.Takasaki,T.Ekino,J.Akimitsu		
150323	P074014517		6H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2006																																														K		7.67					7.67																				kOe			17.1	9.6										MHC150323		A			185	104						meV	1.74	5.25	14							mJ/mol.K2	5.07	SP-heat	323																																					single crystals grown by floating zone method under Ar.					Correlation between crystal structures of CaAlSi with and without superlattice and superconducting properties			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 74(2006)014517	S.Kuroiwa,H.Sagayama,T.Kakiuchi,H.Sawa,Y.Noda,J.Akimitsu		
150324	P074014517		5H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2006																																														K		5.68					5.68																				kOe			14.6	7.3										MHC150324		A			212	106						meV	1.11	4.41	14							mJ/mol.K2	3.86	SP-heat	322																																					single crystals grown by floating zone method under Ar.					Correlation between crystal structures of CaAlSi with and without superlattice and superconducting properties			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 74(2006)014517	S.Kuroiwa,H.Sagayama,T.Kakiuchi,H.Sawa,Y.Noda,J.Akimitsu		
150325	P074014517		1H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2006																												AlB2	P-6m2		A	4.196		4.414												K		6.5					6.5																				kOe			4	3.7										MHC150325		A			298	276						meV	0.98	3.5	14							mJ/mol.K2	6.1	SP-heat	307																																					single crystals grown by floating zone method under Ar.					Correlation between crystal structures of CaAlSi with and without superlattice and superconducting properties			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 74(2006)014517	S.Kuroiwa,H.Sagayama,T.Kakiuchi,H.Sawa,Y.Noda,J.Akimitsu		
150326	L094217002	x=0.12 by ICP. SP-heat measured for H//c-axis. gamma(H) increases linearly for H<0.7 T. (2*gap/kTc) = 4.6 - 5.2. (dC/gamma*Tc) = 1.8. (dC/Tc) = 1.79 mJ/mol.K2.	beta-LixZrNCl	Zr0.12N1Cl1	Zr	0.12	N	1	Cl	1																		1	2005																																														K				12.7			12.7																				T	WHH model	5																										5.2	14							mJ/mol.K2	1	SP-heat																																						beta-ZrNCl prepared by CVT. Li-doping using n-butyl-Li solution in hexane.					Specific Heat Measurement of the Layered Nitride Superconductor LixZrNCl			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 94(2005)217002	Y.Taguchi,M.Hisakabe,Y.Iwasa		
150327	MURO-DR		LaPdSi3	La1Pd1Si3	La	1	Pd	1	Si	3																			2000																												BaNiSn3	I4mm		A	4.352		9.661												K		2.6					2.6																																																								mJ/mol.K2	4.98	SP-heat	334																																										Dr.Y.Muro, Dr-Thesis, Faculty of Science, University of Tokyo, in Japanese(2000)				Dr.Thesis,Tokyo-u(2000)	Y.Muro		
150328	P076132501	Aligned materials. Hc2(T) measured by SUS(subtracting impurity contribution). Pauli-limit = 8.3 T.	Na0.33(H3O)0.02CoCo2/1.4H2O	Na0.33H2.86Co1O3.42	Na	0.33	H	2.86	Co	1															O	3.42			2007																																														K				4.5			4.5																				T	extraporation	7.8												HC150328																																																														Na0.7CoO2 by solid state reaction. deintercalating, hydrated in NaCl at RT					Upper critical field of an aligned Nax(H3O)zCoO2/yH2O superconductor from magnetization measurements			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 76(2007)132501	Z.Ren,C.Feng,Z.Xu,M.Fang,G.Cao		
150329	P076132512	gap measured by photoemission spectroscopy. gap(0) = 0.6 and 2.1 meV, (2gap/kTc) = 2.1 and 7.2 for small and large gap, respectively.	La2C3	C3La2	C	3	La	2																				3	2007																												Pu2C3																		K				6.5			6.5																																														meV	2.1	7.2	9																																															grown by self-flux method					Anomalous superconducting-gap symmetry of noncentrosymmetric La2C3 observed by ultrahigh-resolution photoemission spectroscopy			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.B, 76(2007)132512	K.Sugawara,T.Sato,S.Souma,T.Takahashi,A.Ochiai		
150330	P076140502	oz calculated from oz vs latc relation. optimaly doped sample. O-isotope exchange by ANN(650C,96h). confirmation by IR. Tc by SUS.	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6.36	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z	6.36	3	2007																												Bi2201	I4/mmm		A	5.4		24.33												K				31.2			31.2						0.25	O	80	0.79																																																																																							TSFZ(traveling-solvent floating zone)					Oxygen isotope effect in Bi2Sr2Can-1CunO2n+4+z (n=1,2,3) single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 76(2007)140502	X.J.Chen,B.Liang,C.Ulrich,C.T.Lin,V.V.Struzhkin,Z.Wu,R.J.Hemley,H.K.Mao,H.Q.Lin		
150331	P076140502	oz calculated from oz vs latc relation. optimaly doped sample. O-isotope exchange by ANN(650C,96h). confirmation by IR. Tc by SUS.	Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8.12	Bi	2	Sr	2	Ca	1	Cu	2													O	8+z	8.12	3	2007																												Bi2212	I4/mmm		A	5.4		30.8												K				81.3			81.3						0.14	O	80	1.19																																																																																							TSFZ(traveling-solvent floating zone)					Oxygen isotope effect in Bi2Sr2Can-1CunO2n+4+z (n=1,2,3) single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 76(2007)140502	X.J.Chen,B.Liang,C.Ulrich,C.T.Lin,V.V.Struzhkin,Z.Wu,R.J.Hemley,H.K.Mao,H.Q.Lin		
150332	P076140502	oz calculated from oz vs latc relation. optimaly doped sample. O-isotope exchange by ANN(650C,96h). confirmation by IR. Tc by SUS.	Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10.28	Bi	2	Sr	2	Ca	2	Cu	3													O	10+z	10.28	3	2007																												Bi2223	I4/mmm		A	5.4		37.07												K				108.7			108.7						0.02	O	80	0.27																																																																																							TSFZ(traveling-solvent floating zone)					Oxygen isotope effect in Bi2Sr2Can-1CunO2n+4+z (n=1,2,3) single crystals			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev.B, 76(2007)140502	X.J.Chen,B.Liang,C.Ulrich,C.T.Lin,V.V.Struzhkin,Z.Wu,R.J.Hemley,H.K.Mao,H.Q.Lin		
150333	SSC1440419		Ti2InC	Ti2In1C1	Ti	2	In	1	C	1																		1	2007																												Cr2AlC	P6<3>/mmc		A	3.132		14.06											H-phase	K	2.9		3.1	3.1		0.2	3.1																																																																																														graphite,Ti,In		mixture - pellet - sealed in quartz ampoule - heat(800C,24h) - reground - heat(800C,96h)					Superconductivity in the hexagonal-layered nanolaminates Ti2InC compound			Departamento de Engenharia de Materiais, Escola de Engenharia de Lorena - USP, P.O. Box 116, Lorena ? SP, 12600-970, Brazil	Solid State Commun., 144(2007)419	A.D.Bortolozo,O.H.Sant'Anna,C.A.M.dos Santos,A.J.S.Machado		
150334	P074174501		Nb2AsC	Nb2As1C1	Nb	2	As	1	C	1																		1	2006																												Cr2AlC																	H-phase	K		2					2																																																								mJ/mol.K2	4.7	SP-heat	520																																										Electron-phonon coupling in Mn+1AXn-phase carbides			Department of Physics and Astronomy, Rowan University, Glassboro, New Jersey 08028, USA	Phys.Rev.B, 74(2006)174501	S.E.Lofland,J.D.Hettinger,T.Meehan,A.Bryan,P.Finkel		
150335	L099107001	in-plane THC was  measured. (THC/T) = a + b*T^2(p-1) = 0.355 mW/K2 with p=2.24. single gap s-wave SC.	CuxTiSe2	Cu0.06Ti1Se2	Cu	0.06	Ti	1	Se	2																		3	2007																																														K		2.3					2.3																				T	resistivity	0.52			0.52			0.08																																					MTHC150335																															vapor transport method					Single-gap s-wave superconductivity near the charge-density-wave quantum critical point in CuxTiSe2			Departement de physique and RQMP, Universite de Sherbrooke, Sherbrooke,Canada	Phys.Rev.Lett., 99(2007)107001	S.Y.Li,G.Wu,X.H.Chen,Louis Taillfer		
150336	L099217001	G-L = 24. Hc(0) = 53 mT. e-ph coupling = 0.7. (dC/Tc)=58. (dC/gamma*Tc) = 1.35.	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																			2007																												skutterudite			A	8.6928													LaFe4Sb12	K		5.35					5.35																				T		1.8							T/K		0.46			MHC150336		A		140			A		3200					3.6								mJ/mol.K2	42		247																																					Ar arc melting - ANN(800C,2w, in quartz tube)					Superconductivity in Novel Ge-Based Skutterudites: {Sr,Ba}Pt4Ge12			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.Lett., 99(2007)217001	E.Bauer,A.Grytsiv,Xing-Qiu Chen,N. Melnychenko-Koblyuk,G. Hilscher,H. Kaldarar,H. Michor,E. Royanian,G. Giester,M. Rotter,R. Podloucky,P. Rogl		
150337	L099217001	G-L = 14. Hc(0) = 52 mT. e-ph coupling = 0.7. (dC/Tc)=57. (dC/gamma*Tc) = 1.35.	SrPt4Ge12	Sr1Pt4Ge12	Sr	1	Pt	4	Ge	12																			2007																												skutterudite			A	8.6601													LaFe4Sb12	K		5.1					5.1																				T		1							T/K		0.275			MHC150337		A		180			A		2500					3.6								mJ/mol.K2	41		220																																					Ar arc melting - ANN(800C,2w, in quartz tube)					Superconductivity in Novel Ge-Based Skutterudites: {Sr,Ba}Pt4Ge12			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.Lett., 99(2007)217001	E.Bauer,A.Grytsiv,Xing-Qiu Chen,N. Melnychenko-Koblyuk,G. Hilscher,H. Kaldarar,H. Michor,E. Royanian,G. Giester,M. Rotter,R. Podloucky,P. Rogl		
150338	P075104505	Cu-content by lat-C vs x calibration. I//ab. RRR=6.5. anisotropy factor = 1.7 at 0.35 K. G-L//ab = 25. G-L//c = 13.4.	CuxTiSe2	Cu0.7Ti1Se2	Cu	0.7	Ti	1	Se	2																		3	2007																												1T-MX2																		K		3.9		3.9		0.1	3.9											Oe			32	53					T			1.238	0.729										MHC150338		A			213	125	A			2850	5840																										uOhm.cm							80				520														Cl-vapor transport. CuCl2:TiSe2 = 0.10:1, in silica tube.					Anisotropic properties of the layered superconductor Cu0.07TiSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08540, USA	Phys.Rev.B, 75(2007)104505	E.Morosan,Lu Li,N.P.Ong,R.J.Cava		
150339	L099217207		URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2007																												ThCr2Si2																		K		1.41					1.41	MTC150339																																	MHC150339																																																														single crystal were grown by Czochralski method. then ANN(900C,7d)					Competing Ordered Phases in URu2Si2: Hydrostatic Pressure and Rhenium Substitution			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 99(2007)217207	J. R. Jeffries,N. P. Butch,B. T. Yukich,M. B. Maple		
150340	L094046401		URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		1	2005								17.5																				ThCr2Si2																		K		1.5					1.5																																																																																																					Non-Fermi-Liquid Behavior within the Ferromagnetic Phase in URu2-xRexSi2			Department of Physics and Institute For Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 94(2005)046401	E. D. Bauer,V. S. Zapf,P.-C. Ho,N. P. Butch,E. J. Freeman,C. Sirvent,M. B. Maple		
150341	L094046401		U(Ru,Re)2Si2	U1Ru1.99Re0.01Si2	U	1	Ru	1.99	Re	0.01	Si	2																1	2005								13.5																				ThCr2Si2																		K		0.23					0.23	MPH150341																																																																																																				Non-Fermi-Liquid Behavior within the Ferromagnetic Phase in URu2-xRexSi2			Department of Physics and Institute For Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 94(2005)046401	E. D. Bauer,V. S. Zapf,P.-C. Ho,N. P. Butch,E. J. Freeman,C. Sirvent,M. B. Maple		
150342	PHC4670009		ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																	2007					uB/f.u	9.12		5.19																				LuNi2B2C			A	3.5004		10.558												K		10.23					10.23																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150343	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.98Fe0.02B2C1	Er	1	Ni	1.98	Fe	0.02	B	2	C	1															2007					uB/f.u	9.08		5.6																				LuNi2B2C			A	3.503		10.562												K		10.27					10.27																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150344	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.96Fe0.04B2C1	Er	1	Ni	1.96	Fe	0.04	B	2	C	1															2007					uB/f.u	8.95		5.48																				LuNi2B2C			A	3.4972		10.552												K		9.5					9.5	MTC150344																																																																																															arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150345	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.94Fe0.06B2C1	Er	1	Ni	1.94	Fe	0.06	B	2	C	1															2007					uB/f.u	9		5.23																				LuNi2B2C			A	3.5001		10.562												K		8.5					8.5																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150346	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.92Fe0.08B2C1	Er	1	Ni	1.92	Fe	0.08	B	2	C	1															2007					uB/f.u	8.97		5.11																				LuNi2B2C			A	3.5004		10.567												K		4.63					4.63																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150347	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.9Fe0.1B2C1	Er	1	Ni	1.9	Fe	0.1	B	2	C	1															2007					uB/f.u	8.99		5.03																				LuNi2B2C			A	3.4972		10.552												K		4.31					4.31																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150348	PHC4670009		Er(Ni,Fe)2B2C	Er1Ni1.88Fe0.12B2C1	Er	1	Ni	1.88	Fe	0.12	B	2	C	1															2007					uB/f.u	9.05		4.91																				LuNi2B2C			A	3.5004		10.565												K		0					0																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150349	PHC4670009		ErNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																	2007																												LuNi2B2C			A	3.4849		10.5931												K		10.79					10.79																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150350	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.96Fe0.04B2C1	Tm	1	Ni	1.96	Fe	0.04	B	2	C	1															2007																												LuNi2B2C			A	3.4832		10.582												K		7.97					7.97																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150351	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.92Fe0.08B2C1	Tm	1	Ni	1.92	Fe	0.08	B	2	C	1															2007																												LuNi2B2C			A	3.4858		10.592												K		7.39					7.39	MTC150351																																																																																															arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150352	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.9Fe0.1B2C1	Tm	1	Ni	1.9	Fe	0.1	B	2	C	1															2007																												LuNi2B2C			A	3.48		10.576												K		6.64					6.64																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150353	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.88Fe0.12B2C1	Tm	1	Ni	1.88	Fe	0.12	B	2	C	1															2007																												LuNi2B2C			A	3.4842		10.586												K		5.52					5.52																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150354	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.84Fe0.16B2C1	Tm	1	Ni	1.84	Fe	0.16	B	2	C	1															2007																												LuNi2B2C			A	3.4781		10.579												K		3.99					3.99																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150355	PHC4670009		Er(Ni,Fe)2B2C	Tm1Ni1.8Fe0.2B2C1	Tm	1	Ni	1.8	Fe	0.2	B	2	C	1															2007																												LuNi2B2C			A	3.4781		10.578												K		0					0																																																																																																arc-melting. final annealing (1050C,72h, in evacuated quartz tube)					Superconductivity and magnetism in R(Ni-xFex)2B2C (R = Er and Tm) systems			Faculty of Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 467(2007)9	Lingwei Li,K.Nishimura,K.Mori		
150356	L100026404	(dC/T) = 0.24 J/mol.K2 at Tc. (dC/gamma*Tc) = 2. lattice term, beta = 0.82 mJ/mol.K2. e-ph = 0.58. Hc2(T) = Hc2(0)[1-t^1.5]^1.5.	Rh17S15	Rh17S15	Rh	17	S	15																				1	2008																													Pm3m		A	9.9093													Miasite(mineral)	K		5.4					5.4																				T	extraporation	23.5												MHC150356																			MSP150356			mJ/mol.K2	104.8														uOhm.cm							26.7													MRH150356			Rh(powder),S(powder)		mixture - heat(950C, in evacuated quartz) - cool to RT(30C/h)					Strongly Correlated Superconductivity in Rh17S15			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.Lett., 100(2008)026404	H. R. Naren,A. Thamizhavel,A. K. Nigam,S. Ramakrishnan		
150357	L100017003	RRR=9.3. Energy gap measured by laser-PES. below Neel-T, gap deviate from BCS prediction.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	2008								6																				LuNi2B2C																		K				9.3			9.3	MGAP150357																																													meV	1.4	3.49																																																floating zone method					Bulk Electronic Structure of the Antiferromagnetic Superconducting Phase in ErNi2B2C			Institute for Solid State Physics (ISSP), University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 100(2008)017003	T. Baba,T. Yokoya,S. Tsuda,T. Kiss,T. Shimojima,K. Ishizaka,H. Takeya,K. Hirata,T. Watanabe,M. Nohara,H. Takagi,N. Nakai,K. Machida,T. Togashi,S. Watanabe,X.-Y. Wang,C. T. Chen,S. Shin		
150358	MRB0430009	not SC	Mg6Ni16Si7	Mg6Ni16Si7	Mg	6	Ni	16	Si	7																		1	2008																												Mg6Cu16Si7			A	11.3164														K					0.3																																																																																																		20% excess Mg, wrapped in Ta foil, heat(500C,1h + 900C,1h in 5%H2-95%Ar), cool to RT					Crystal structure and physical properties of Mg6Cu16Si7-type M6Ni16Si7, for M = Mg, Sc, Ti, Nb, and Ta			Department of Chemistry, Princeton University, Princeton, NJ 08540, USA	Mater.Res.Bull., 43(2008)9	K.L. Holman,E. Morosan,P.A. Casey,Lu Li,N.P. Ong,T. Klimczuk,C. Felser,R.J. Cava		
150359	MRB0430009	not SC	Sc6Ni16Si7	Sc6Ni16Si7	Sc	6	Ni	16	Si	7																		1	2008																												Mg6Cu16Si7			A	11.4442														K					0.3																																																																																																		arc-melting					Crystal structure and physical properties of Mg6Cu16Si7-type M6Ni16Si7, for M = Mg, Sc, Ti, Nb, and Ta			Department of Chemistry, Princeton University, Princeton, NJ 08540, USA	Mater.Res.Bull., 43(2008)9	K.L. Holman,E. Morosan,P.A. Casey,Lu Li,N.P. Ong,T. Klimczuk,C. Felser,R.J. Cava		
150360	MRB0430009	not SC	Ti6Ni16Si7	Ti6Ni16Si7	Ti	6	Ni	16	Si	7																		1	2008																												Mg6Cu16Si7			A	11.2566														K					0.3																																																																																																		arc-melting					Crystal structure and physical properties of Mg6Cu16Si7-type M6Ni16Si7, for M = Mg, Sc, Ti, Nb, and Ta			Department of Chemistry, Princeton University, Princeton, NJ 08540, USA	Mater.Res.Bull., 43(2008)9	K.L. Holman,E. Morosan,P.A. Casey,Lu Li,N.P. Ong,T. Klimczuk,C. Felser,R.J. Cava		
150361	MRB0430009	not SC	Nb6Ni16Si7	Nb6Ni16Si7	Nb	6	Ni	16	Si	7																		1	2008																												Mg6Cu16Si7			A	11.244														K					0.3																																																																																																		arc-melting					Crystal structure and physical properties of Mg6Cu16Si7-type M6Ni16Si7, for M = Mg, Sc, Ti, Nb, and Ta			Department of Chemistry, Princeton University, Princeton, NJ 08540, USA	Mater.Res.Bull., 43(2008)9	K.L. Holman,E. Morosan,P.A. Casey,Lu Li,N.P. Ong,T. Klimczuk,C. Felser,R.J. Cava		
150362	MRB0430009	not SC	Ta6Ni16Si7	Ta6Ni16Si7	Ta	6	Ni	16	Si	7																		1	2008																												Mg6Cu16Si7			A	11.2168														K					0.3																																																																																																		arc-melting					Crystal structure and physical properties of Mg6Cu16Si7-type M6Ni16Si7, for M = Mg, Sc, Ti, Nb, and Ta			Department of Chemistry, Princeton University, Princeton, NJ 08540, USA	Mater.Res.Bull., 43(2008)9	K.L. Holman,E. Morosan,P.A. Casey,Lu Li,N.P. Ong,T. Klimczuk,C. Felser,R.J. Cava		
150363	L100017002	SP-heat(relaxation type), R(ac-method),Tc from SP-heat.RR = 5.3 uOhm.cm, RRR = 177, (dC/gamma*Tc) = 1.49.	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																			2008																												skutterudite			A	8.6235													LaFe4P12	K		8.27					8.27																				T		1.6												MHC150363														1.94								mJ/mol.K2	76	SP-heat	209	SP-heat																																				arc-melting - ANN(800C,7d, in sealed Ta ampoule)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150364	L100017002	SP-heat(relaxation type), R(ac-method),Tc from SP-heat.RR = 2.6 uOhm.cm, RRR = 110, (dC/gamma*Tc) = 1.56.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																			2008					uB/Pr	3.67	-16.4																					skutterudite			A	8.6111													LaFe4P12	K		7.91					7.91																				T		2.06																										2.35								mJ/mol.K2	87	SP-heat	198	SP-heat																																				arc-melting - ANN(800C,7d, in sealed Ta ampoule)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150365	L100017002	SP-heat(relaxation type), R(ac-method),Tc from SP-heat.RR = 50 uOhm.cm, RRR = 239, (dC/gamma*Tc) = 1.13.	SrPt4Ge12	Sr1Pt4Ge12	Sr	1	Pt	4	Ge	12																			2008																												skutterudite			A	8.6509													LaFe4P12	K		5.4					5.4																																																											198	SP-heat																																				arc-melting - ANN(800C,7d, in sealed Ta ampoule)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150366	L100017002	SP-heat(relaxation type), R(ac-method),Tc from SP-heat.RR = 36 uOhm.cm, RRR = 191, (dC/gamma*Tc) = 1.17.	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																			2008																												skutterudite			A	8.6838													LaFe4P12	K		5					5																																																											209	SP-heat																																				arc-melting - ANN(800C,7d, in sealed Ta ampoule)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150367	PHC2240001	Tc defined as Tc(on). Impurity phase detected.	(Hg,Cr)Sr2CuO4	Hg0.9Cr0.1Sr2Cu1O4	Hg	0.9	Cr	0.1	Sr	2	Cu	1													O	4			1994																												Hg1201																		K				62.3			62.3																																																																																														HgO,SrCO3,CuO,Cr2O3		SrCo3+CuO+Cr2O3-mix and CAL(950C,24H)-mix with HgO-pellet-SIN(880C,8H in evacuated quartq am poule)-Q to RT					A new mercury-based superconductor : (Hg,Cr)Sr2CuOz			Department of Industrial Chemistry,University of Tokyo,Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 224(1994)1-5	J.Shimoyama,K.Kishio,K.Kitazawa,K.Yamafuji,S.Hahakura	Hg,Cr,Sr,Cu,O	
150368	PHC2240001	Tc defined as Tc(on). Impurity phase detected.	(Hg,Cr)Sr2CuO4	Hg0.2Cr0.8Sr2Cu1O4	Hg	0.2	Cr	0.8	Sr	2	Cu	1													O	4			1994																												Hg1201																		K				53.6			53.6																																																																																														HgO,SrCO3,CuO,Cr2O3		SrCo3+CuO+Cr2O3-mix and CAL(950C,24H)-mix with HgO-pellet-SIN(880C,8H in evacuated quartq am poule)-Q to RT					A new mercury-based superconductor : (Hg,Cr)Sr2CuOz			Department of Industrial Chemistry,University of Tokyo,Hongo,Bunkyo-ku,Tokyo,Japan	Physica C, 224(1994)1-5	J.Shimoyama,K.Kishio,K.Kitazawa,K.Yamafuji,S.Hahakura	Hg,Cr,Sr,Cu,O	
150369	PHC4670174	MOMENT shows remanent momentb per Ru.	RuSr2(Gd,Ce)2Cu2Oz	Ru1Sr2Gd1.4Ce0.6Cu2Oz	Ru	1	Sr	2	Gd	1.4	Ce	0.6	Cu	2											O	z		1	2007					uB/Ru	0.48																						Ru1222			A	3.827		28.37												K			20				20																																																																																														RuO2,Gd2O3,SnO2,CeO2,SrCO3,CuO	1	mixture - heat(600C,48h,in air + 1000C,24h,in flowing O2) - reground - SIN(1060C,96h,in flowing O2) - ANN(350C,48h,in flowing O2)					Superconducting and magnetic properties of Sn-doped Ru-1222			Institute of Solid State Physics, Bulgarian Academy of Sciences, bd. Tsarigradsko Chaussee 72, 1784 Sofia, Bulgaria	Physica C, 467(2007)174	N. Balchev,K. Nenkov,G. Mihova,B. Kunev,J. Pirov		
150370	PHC4670174	MOMENT shows remanent momentb per Ru.	RuSr2(Gd,Ce)2Cu2Oz	Ru0.97Sn0.03Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.97	Sn	0.03	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z		1	2007					uB/Ru	0.39			5.4																			Ru1222			A	3.827		28.53												K			35				35																																																																																														RuO2,Gd2O3,SnO2,CeO2,SrCO3,CuO	1	mixture - heat(600C,48h,in air + 1000C,24h,in flowing O2) - reground - SIN(1060C,96h,in flowing O2) - ANN(350C,48h,in flowing O2)					Superconducting and magnetic properties of Sn-doped Ru-1222			Institute of Solid State Physics, Bulgarian Academy of Sciences, bd. Tsarigradsko Chaussee 72, 1784 Sofia, Bulgaria	Physica C, 467(2007)174	N. Balchev,K. Nenkov,G. Mihova,B. Kunev,J. Pirov		
150371	PHC4670174		(Ru,Sn)Sr2(Gd,Ce)2Cu2Oz	Ru0.95Sn0.05Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.95	Sn	0.05	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z		1	2007																												Ru1222			A	3.846		28.69												K			24				24																																																																																														RuO2,Gd2O3,SnO2,CeO2,SrCO3,CuO	1	mixture - heat(600C,48h,in air + 1000C,24h,in flowing O2) - reground - SIN(1060C,96h,in flowing O2) - ANN(350C,48h,in flowing O2)					Superconducting and magnetic properties of Sn-doped Ru-1222			Institute of Solid State Physics, Bulgarian Academy of Sciences, bd. Tsarigradsko Chaussee 72, 1784 Sofia, Bulgaria	Physica C, 467(2007)174	N. Balchev,K. Nenkov,G. Mihova,B. Kunev,J. Pirov		
150372	PHC4670174	not SC. MOMENT shows remanent momentb per Ru.	(Ru,Sn)Sr2(Gd,Ce)2Cu2Oz	Ru0.9Sn0.1Sr2Gd1.4Ce0.6Cu2Oz	Ru	0.9	Sn	0.1	Sr	2	Gd	1.4	Ce	0.6	Cu	2									O	z		1	2007					uB/Ru	0.24			6.12																			Ru1222			A	3.808		28.22												K					2																																																																																																RuO2,Gd2O3,SnO2,CeO2,SrCO3,CuO	1	mixture - heat(600C,48h,in air + 1000C,24h,in flowing O2) - reground - SIN(1060C,96h,in flowing O2) - ANN(350C,48h,in flowing O2)					Superconducting and magnetic properties of Sn-doped Ru-1222			Institute of Solid State Physics, Bulgarian Academy of Sciences, bd. Tsarigradsko Chaussee 72, 1784 Sofia, Bulgaria	Physica C, 467(2007)174	N. Balchev,K. Nenkov,G. Mihova,B. Kunev,J. Pirov		
150373	P076212504	SP-heat for 0.6<T<10 K. GAMMA(H) measured for H//c, H//ab. Two gap model fitting, (2d/kTc) = 4.5 and 2.6. (dC/gamma*Tc) = 2.12. CDW-temp = 33 K.	NbSe2	Nb1Se2	Nb	1	Se	2																				3	2007																												2H-NbSe2																		K		6.7					6.7																																																4.5								mJ/mol.K2	19.09	SP-heat	224	SP-heat																																				standard iodine vapor transport method					Experimental evidence for a two-gap structure of superconducting NbSe2: A specific-heat study in external magnetic fields			Department of Physics, Center of Nanoscience and Nanotechnology, National Sun Yat-Sen University, Kaohsiung 804, Taiwan	Phys.Rev.B, 76(2007)212504	C. L. Huang,J.-Y. Lin,Y. T. Chang,C. P. Sun,H. Y. Shen,C. C. Chou,H. Berger,T. K. Lee,H. D. Yang		
150374	P076212508	optimum sample. single crystals aligned under magnetic field. Anisotropy factor = 41. Hirr(T) fitting using two fluid model.	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		1	2007																												Hg1245																		K				107			107																																		HIR150374																																																																			Coexistence of superconductivity and antiferromagnetism in HgBa2Ca4Cu5Oy: Multiharmonic susceptibility and vortex dynamics study			National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan	Phys.Rev.B, 76(2007)212508	A. Crisan,Y. Tanaka,A. Iyo,D. D. Shivagan,P. M. Shirage,K. Tokiwa,T. Watanabe,L. Cosereanu,T. W. Button,J. S. Abell		
150375	P076214510	RRR = 22. (dC/gamma*Tc) = 0.94. lattice term(SP) = 0.031 mJ/mol.K4. e-ph coupling = 0.41. RESN at 2.2 K. value.	OsB2	B2Os1	B	2	Os	1																					2007																											3	RuB2	Pmmn	59	A	4.6851	2.8734	4.0771												K	2.14		2.2			0.04	2.17																				Oe					420			0.6						MHC150375							A		3800					3.8								mJ/mol.K2	1.9	SP-heat	550	SP-heat											uOhm.cm							1.7				36									MRH150375					arc melting					Superconducting and normal-state properties of the layered boride OsB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 76(2007)214510	Yogesh Singh,A. Niazi,M. D. Vannette,R. Prozorov,D. C. Johnston		
150376	P076214510	RRR = 51.  lattice term(SP) = 0.015 mJ/mol.K4. RESN at 1.8 K. value.	RuB2	B2Ru1	B	2	Ru	1																					2007																											3	RuB2	Pmmn	59	A	4.6457	2.8657	4.0442												K					1.1																																																										mJ/mol.K2	1.72	SP-heat	701	SP-heat											uOhm.cm							1.1				53														arc melting					Superconducting and normal-state properties of the layered boride OsB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 76(2007)214510	Yogesh Singh,A. Niazi,M. D. Vannette,R. Prozorov,D. C. Johnston		
150377	P076214510	RRR = 41. (dC/gamma*Tc) = 1.38. lattice term(SP) = 0.035 mJ/mol.K4. RESN at 2.2 K. value.	OsB2	B2Os1	B	2	Os	1																					2007																											3	RuB2	Pmmn	59																K	2.12						2.12																				Oe					330			1	Oe/K		180			MHC150377							A		4000										MSP150377			mJ/mol.K2	1.47	SP-heat													uOhm.cm							0.87				36			cm3/C	0.000203										arc melting - wrapped in Zr foil - ANN(1150C,10d, in sealed quartz)					Superconducting and normal-state properties of the layered boride OsB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 76(2007)214510	Yogesh Singh,A. Niazi,M. D. Vannette,R. Prozorov,D. C. Johnston		
150378	P076220502	SIS, SIN tunnel junction	CaC6	C6Ca1	C	6	Ca	1																					2007																																														K				11.6			11.6																																														meV	2.3	4.6																																																					Large energy gaps in CaC6 from tunneling spectroscopy: Possible evidence of strong-coupling superconductivity			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 76(2007)220502(R)	Cihan Kurter,Lutfi Ozyuzer,Daniel Mazur,John F. Zasadzinski,Daniel Rosenmann,Helmut Claus,Dave G. Hinks,Kenneth E. Gray		
150379	SSC1330427	epitaxial thin film.	(La,Y)2CuO4	La1.91Y0.09Cu1O4+z	La	1.91	Y	0.09	Cu	1															O	4+z		4	2005																												T'																		K	21.4						21.4																																																																																																molecular beam epitaxy on SrTiO3 at 650 C(Tsub) using coevaporation of metal targets					New class of T'-structure cuprate superconductors			NTT Basic Research Laboratories, 3-1 Morinosato, Atsugi, Kanagawa 243, Japan	Solid State Commun., 133(2005)427	A. Tsukada,Y. Krockenberger,M. Noda,H. Yamamoto,D. Manske,L. Alff,M. Naito		
150380	SSC1330427	epitaxial thin film. T'-phase for x>0.1 in La2-xYbxCuO4	(La,Tb)2CuO4	La1.67Tb0.33Cu1O4+z	La	1.67	Tb	0.33	Cu	1															O	4+z		4	2005																												T'																		K	12						12																																																																																																molecular beam epitaxy on SrTiO3 at 650 C(Tsub) using coevaporation of metal targets					New class of T'-structure cuprate superconductors			NTT Basic Research Laboratories, 3-1 Morinosato, Atsugi, Kanagawa 243, Japan	Solid State Commun., 133(2005)427	A. Tsukada,Y. Krockenberger,M. Noda,H. Yamamoto,D. Manske,L. Alff,M. Naito		
150381	L098067002	Tc(max) = 15.1 K at P = 7.5 GPa.	CaC6	C6Ca1	C	6	Ca	1																					2007																												GIC																		K		11.6					11.6	MTC150381		K/GPa	0.5																																																																																																	Enhancement of Superconductivity and Evidence of Structural Instability in Intercalated Graphite CaC6 under High Pressure			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 98(2007)067002	A. Gauzzi,S. Takashima,N. Takeshita,C. Terakura,H. Takagi,N. Emery,C. Herold,P. Lagrange,G. Loupias		
150382	P076212508	slightly under doped. single crystals aligned under magnetic field. Anisotropy factor = 48.3. Hirr(T) fitting using two fluid model.	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		1	2007																												Hg1245																		K				100			100																																		HIR150374																																																																			Coexistence of superconductivity and antiferromagnetism in HgBa2Ca4Cu5Oy: Multiharmonic susceptibility and vortex dynamics study			National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan	Phys.Rev.B, 76(2007)212508	A. Crisan,Y. Tanaka,A. Iyo,D. D. Shivagan,P. M. Shirage,K. Tokiwa,T. Watanabe,L. Cosereanu,T. W. Button,J. S. Abell		
150383	P076212508	underdoped sample. single crystals aligned under magnetic field. Hirr(T) fitting using two fluid model.	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		1	2007																												Hg1245																		K				87			87																																		HIR150374																																																																			Coexistence of superconductivity and antiferromagnetism in HgBa2Ca4Cu5Oy: Multiharmonic susceptibility and vortex dynamics study			National Institute of Advanced Industrial Science and Technology, Tsukuba 305-8568, Japan	Phys.Rev.B, 76(2007)212508	A. Crisan,Y. Tanaka,A. Iyo,D. D. Shivagan,P. M. Shirage,K. Tokiwa,T. Watanabe,L. Cosereanu,T. W. Button,J. S. Abell		
150384	PR06112447	thin films, thickness = 150-4500 A. high Tc(= 44 K) due to strain effect from lattice mismatch. Tc depends on lat-c: dTc/dc = 200 K/A.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		4	2000																												T																		K		44					44																																																																																																coevaporation from metal sources. T(sub) = 650-750 C. substrate = (001)LaSrAlO3. growth rate = 0.5-3 A/s. cooled in O2.					La2-xSrxCuOy epitaxial thin films (x = 0 to 2): Structure, strain, and superconductivity			NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B, 61(2000)12447	H. Sato,A. Tsukada,M. Naito,A. Matsuda		
150385	PR06112447	thin film (d = 170 A). Tc depends on RESN: for RESN=31 uOhm.cm, Tc < 4.2 K.	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		4	2000																												T																		K		16					16																																																																							uOhm.cm							16																		coevaporation from metal sources. T(sub) = 650-750 C. substrate = (001)LaSrAlO3. growth rate = 0.5-3 A/s. cooled in O2.					La2-xSrxCuOy epitaxial thin films (x = 0 to 2): Structure, strain, and superconductivity			NTT Basic Research Laboratories, 3-1 Morinosato Wakamiya, Atsugi-shi, Kanagawa 243-0198, Japan	Phys.Rev.B, 61(2000)12447	H. Sato,A. Tsukada,M. Naito,A. Matsuda		
150386	MRB0100889		RuB2	B2Ru1	B	2	Ru	1																				1	1975																											3	RuB2																		K		1.6					1.6																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150387	MRB0100889		OsB2	B2Os1	B	2	Os	1																				1	1975																											3	RuB2																		K		2.1					2.1																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150388	MRB0100889		Rh7B3	B3Rh7	B	3	Rh	7																				1	1975																												Th7Fe3																	hexagonal	K					0.35																																																																																																		arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150389	MRB0100889		RuB1.1	B1.1Ru1	B	1.1	Ru	1																				1	1975																												WC																	hexagonal	K					1.1																																																																																																		arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150390	MRB0100889		NbB	B1Nb1	B	1	Nb	1																				1	1975																												CrB																	orthorhombic	K					1.1																																																																																																		arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150391	MRB0100889		LaB6	B6La1	B	6	La	1																				1	1975																																													cubic	K		0.45					0.45																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150392	MRB0100889		MoB2.5	B2.5Mo1	B	2.5	Mo	1																				1	1975																												AlB2																	hexagonal	K		8.1					8.1																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150393	MRB0100889	e/a ratio = 6.5	Ru7B3	B3Ru7	B	3	Ru	7																					1975																												Th7Fe3																	hexagonal	K		3.38					3.38																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150394	MRB0100889	e/a ratio = 5.8	Re7B3	B3Re7	B	3	Re	7																					1975																												Th7Fe3																	hexagonal	K		3.08					3.08																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150395	MRB0100889	e/a ratio = 5.0	V2IrB2	V2Ir1B2	V	2	Ir	1	B	2																			1975																												Mo2IrB2			A	9.221	7.145	3.126											orthorhombic	K		1.12					1.12																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150396	MRB0100889	e/a ratio = 5.4	Mo2IrB2	Mo2Ir1B2	Mo	2	Ir	1	B	2																			1975																												Mo2IrB2			A	9.422	7.356	3.231											orthorhombic	K		3.6					3.6																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150397	MRB0100889	e/a ratio = 5.3	(Mo,Ru)3B2	Mo1.75Ru1.25B2	Mo	1.75	Ru	1.25	B	2																			1975																												Mo2IrB2			A	9.599	7.48	3.094											orthorhombic	K		3.7					3.7																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150398	MRB0100889	e/a ratio = 5.3	(W,Ru)3B2	W1.75Ru1.25B2	W	1.75	Ru	1.25	B	2																			1975																												Mo2IrB2			A	9.579	7.459	3.072											orthorhombic	K		3.38					3.38																																																																																																arc melting					Superconductivity of some binary and ternary transition-metal borides			Bell Lab, Murray Hill, New Jersey, USA	Mat.Res.Bull., 10(1975)889	J.M.Vandenberg,B.T.Matthias,E.Corenzwit,H.Barz		
150399	MTL0620659		(Cu,Tl)Ba2Ca(Cu,Zn)3O10	Tl0.5Ba2Ca2Cu1Zn2.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	1	Zn	2.5											O	10-z			2008																											2	Cu1223			A	3.879		14.581											(Cu,Tl)-1223	K	120						120																																																																																																two step synthesis. precursor(Cu-Ba-Ca-Mg-Cu-Zn-O) - ADD(Tl2O3) - wrapped in Au-foil  - SIN(860C,10min) - Q to RT					Enhanced superconductivity by Mg doping in Cu1-xTlxBa2Ca2-yMgyCu0.5Zn2.5O10-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Lett., 62(2008)659	Nawazish A. Khan,M. Mumtaz		
150400	MTL0620659	Mg at Ca-site.	(Cu,Tl)Ba2(Ca2-xMgx)(Cu,Zn)3O10	Tl0.5Ba2Ca1.5Mg0.5Cu1Zn2.5O10-z	Tl	0.5	Ba	2	Ca	1.5	Mg	0.5	Cu	1	Zn	2.5									O	10-z			2008																											2	Cu1223																	(Cu,Tl)-1223	K	100						100																																																																																																two step synthesis. precursor(Cu-Ba-Ca-Mg-Cu-Zn-O) - ADD(Tl2O3) - wrapped in Au-foil  - SIN(860C,10min) - Q to RT					Enhanced superconductivity by Mg doping in Cu1-xTlxBa2Ca2-yMgyCu0.5Zn2.5O10-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Lett., 62(2008)659	Nawazish A. Khan,M. Mumtaz		
150401	MTL0620659	Mg at Ca-site.	(Cu,Tl)Ba2(Ca2-xMgx)(Cu,Zn)3O10	Tl0.5Ba2Ca1Mg1Cu1Zn2.5O10-z	Tl	0.5	Ba	2	Ca	1	Mg	1	Cu	1	Zn	2.5									O	10-z			2008																											2	Cu1223																	(Cu,Tl)-1223	K	112						112																																																																																																two step synthesis. precursor(Cu-Ba-Ca-Mg-Cu-Zn-O) - ADD(Tl2O3) - wrapped in Au-foil  - SIN(860C,10min) - Q to RT					Enhanced superconductivity by Mg doping in Cu1-xTlxBa2Ca2-yMgyCu0.5Zn2.5O10-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Lett., 62(2008)659	Nawazish A. Khan,M. Mumtaz		
150402	MTL0620659	Mg at Ca-site.	(Cu,Tl)Ba2(Ca2-xMgx)(Cu,Zn)3O10	Tl0.5Ba2Ca0.5Mg1.5Cu1Zn2.5O10-z	Tl	0.5	Ba	2	Ca	0.5	Mg	1.5	Cu	1	Zn	2.5									O	10-z			2008																											2	Cu1223			A	3.3439		14.3723											(Cu,Tl)-1223	K	115						115																																																																																																two step synthesis. precursor(Cu-Ba-Ca-Mg-Cu-Zn-O) - ADD(Tl2O3) - wrapped in Au-foil  - SIN(860C,10min) - Q to RT					Enhanced superconductivity by Mg doping in Cu1-xTlxBa2Ca2-yMgyCu0.5Zn2.5O10-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Lett., 62(2008)659	Nawazish A. Khan,M. Mumtaz		
150403	SSC1450475		Pd2HfAl	Pd2Hf1Al1	Pd	2	Hf	1	Al	1																		1	2008																												Heusler																	L2<1>, Cu2MnAl	K				3.4			3.4																																																																																																arc-melting - ANN(1073K,7d, in evacuated quartz tube)					Electronic and structural properties of palladium-based Heusler superconductors			Institut fur Anorganische Chemie und Analytische Chemie, Johannes Gutenberg-Universitat Mainz, D-55099 Mainz, Germany	Solid State.Commun., 145(2008)475	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser		
150404	SSC1450475		Pd2ZrAl	Pd2Zr1Al1	Pd	2	Zr	1	Al	1																		1	2008																												Heusler																	L2<1>, Cu2MnAl	K				3.2			3.2																																																																																																arc-melting - ANN(1073K,7d, in evacuated quartz tube)					Electronic and structural properties of palladium-based Heusler superconductors			Institut fur Anorganische Chemie und Analytische Chemie, Johannes Gutenberg-Universitat Mainz, D-55099 Mainz, Germany	Solid State.Commun., 145(2008)475	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser		
150405	SSC1450493	not SC down to 80 mK.	BaC6	Ba1C6	Ba	1	C	6																					2008							-0.0151																				7	GIC	P6<3>/mmc																	K					0.08																																																																																																		vapor transport technique, 500C,8h,					Absence of superconductivity down to 80 mK in graphite intercalated BaC6			Service de Physique de l'Etat Condense, CEA-Saclay, 91191 Gif sur Yvette, France	Solid State.Commun., 145(2008)493	S. Nakamae,A. Gauzzi,F. Ladieu,D. L'Hote,N. Emery,C. Herold,J.F. Marech,P. Lagrange,G. Loupias		
150406	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0. Jc(64K) = 100 A/cm2. RRR = 3.27. .	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1											O	z			2007																												Bi2212																		K	67.8		76.6				72.2																																																																							uOhm.cm							8.35																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150407	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0.1. Jc(64K) = 405 A/cm2. RRR = 2.29. Nd maybe replaced by Ca	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Nd0.1Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1	Nd	0.1									O	z			2007																												Bi2212																		K	75.6		90.7				83.15																																																																							uOhm.cm							16.65																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150408	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0.2. Jc(64K) = 717 A/cm2. RRR = 1.92. Nd maybe replaced by Ca	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Nd0.2Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1	Nd	0.2									O	z			2007																												Bi2212																		K	80.9		94.4				87.65																																																																							uOhm.cm							29.51																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150409	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0.3. Jc(64K) = 462 A/cm2. RRR = 1.83. Nd maybe replaced by Ca	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Nd0.3Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1	Nd	0.3									O	z			2007																												Bi2212																		K	81.1		95.5				88.3																																																																							uOhm.cm							54.48																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150410	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0.4. Jc(64K) = 355 A/cm2. RRR = 1.56. Nd maybe replaced by Ca	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Nd0.4Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1	Nd	0.4									O	z			2007																												Bi2212																		K	80.5		95.3				87.9																																																																							uOhm.cm							79.38																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150411	MRB0422057	nominal(Bi:Pb:Sr:Ca:Cu:Nd = 1.7:0.4:2.0:1.1:2.1:x ) x = 0.5. Jc(64K) = 147 A/cm2. RRR = 1.41. Nd maybe replaced by Ca	(Bi,Pb)2Sr2CaCu2NdxOz	Bi1.7Pb0.4Sr2Ca1.1Cu2.1Nd0.5Oz	Bi	1.7	Pb	0.4	Sr	2	Ca	1.1	Cu	2.1	Nd	0.5									O	z			2007																												Bi2212																		K	76.2		95.1				85.65																																																																							uOhm.cm							81.69																		mixture - pellet (under uniaxial stress = 500 MPa) - heat(845 C,100h)					Structural and superconducting properties of neodymium added (Bi,Pb)2Sr2CaCu2Oy			Regional Research Laboratory (CSIR), Trivandrum, Kerala 695019, India	Mater.Res.Bull., 42(2007)2057	A. Biju,P.M. Sarun,R.P. Aloysius,U. Syamaprasad		
150412	SSC1450201	definition of T1(SC) is not clear.	TlBa2Ca2Cu3O9	Tl1Ba2Ca2Cu3O9-z	Tl	1	Ba	2	Ca	2	Cu	3													O	9-z			2008																												Tl1223																		K	111.98						111.98																																																																		uV/K				TP150412																								Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150413	SSC1450201	definition of T1(SC) is not clear.	TlBa2(Ca,Na)2Cu3O9	Tl1Ba2Ca1.9Na0.1Cu3O9-z	Tl	1	Ba	2	Ca	1.9	Na	0.1	Cu	3											O	9-z			2008																												Tl1223																		K	106.01						106.01																																																																																														Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150414	SSC1450201	definition of T1(SC) is not clear.	TlBa2(Ca,Na)2Cu3O9	Tl1Ba2Ca1.85Na0.15Cu3O9-z	Tl	1	Ba	2	Ca	1.85	Na	0.15	Cu	3											O	9-z			2008																												Tl1223																		K	105.51						105.51																																																																																														Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150415	SSC1450201	definition of T1(SC) is not clear.	TlBa2(Ca,Na)2Cu3O9	Tl1Ba2Ca1.8Na0.2Cu3O9-z	Tl	1	Ba	2	Ca	1.8	Na	0.2	Cu	3											O	9-z			2008																												Tl1223																		K	103.03						103.03																																																																		uV/K				TP150415																								Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150416	SSC1450201	definition of T1(SC) is not clear.	TlBa2(Ca,Na)2Cu3O9	Tl1Ba2Ca1.7Na0.3Cu3O9-z	Tl	1	Ba	2	Ca	1.7	Na	0.3	Cu	3											O	9-z			2008																												Tl1223																		K	100.31						100.31																																																																																														Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150417	SSC1450201	definition of T1(SC) is not clear.	TlBa2(Ca,Na)2Cu3O9	Tl1Ba2Ca1.6Na0.4Cu3O9-z	Tl	1	Ba	2	Ca	1.6	Na	0.4	Cu	3											O	9-z			2008																												Tl1223																		K	99.3						99.3																																																																		uV/K				TP150417																								Tl2O3,BaO2,CaO,Na2O2,CuO	1	mixture - pellet - wrapped in Ag foil - heat to 860C(4C/min) - hold(860C,4h) - cool to RT(6C/min)					Investigation of specific heat and thermopower properties of Tl-1223 substituted by sodium			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State.Commun., 145(2008)201	R. Awad,A.I. Abou-Aly,S. Isber,W. Malaeb		
150418	PHB4031038	Tc defined as midpoint of ac-SUS.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2008																												skutterudite																		K		1.83					1.83																				T		2.18												MHC150418																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150419	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os3.8Ru0.2Sb12	Pr	1	Os	3.8	Ru	0.2	Sb	12																3	2008																												skutterudite																		K		1.68					1.68																				T		1.89												MHC150418																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150420	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os3.6Ru0.4Sb12	Pr	1	Os	3.6	Ru	0.4	Sb	12																3	2008																												skutterudite																		K		1.58					1.58	MTC150420																			T		1.48												MHC150418																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150421	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os2.8Ru1.2Sb12	Pr	1	Os	2.8	Ru	1.2	Sb	12																3	2008																												skutterudite																		K		1.05					1.05																				T		0.76												MHC150421																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150422	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os2.4Ru1.6Sb12	Pr	1	Os	2.4	Ru	1.6	Sb	12																3	2008																												skutterudite																		K		1.13					1.13																				T		0.34												MHC150421																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150423	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os2Ru2Sb12	Pr	1	Os	2	Ru	2	Sb	12																3	2008																												skutterudite																		K		0.81					0.81																				T		0.52												MHC150423																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150424	PHB4031038	Tc defined as midpoint of ac-SUS.	Pr(Os,Ru)4Sb12	Pr1Os1.2Ru2.8Sb12	Pr	1	Os	1.2	Ru	2.8	Sb	12																3	2008																												skutterudite																		K		0.8					0.8	MTC150420																			T		0.39												MHC150423																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150425	PHB4031038	Tc defined as midpoint of ac-SUS.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																		3	2008																												skutterudite																		K		1.11					1.11																				T		0.245												MHC150423																																																														molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150426	PHB4031038	Tc defined as midpoint of ac-SUS.	(Pr,Nd)Os4Sb12	Pr0.8Nd0.2Os4Sb12	Pr	0.8	Nd	0.2	Os	4	Sb	12																3	2008																												skutterudite																		K		1.43					1.43																																																																																																molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150427	PHB4031038	Tc defined as midpoint of ac-SUS.	(Pr,Nd)Os4Sb12	Pr0.55Nd0.45Os4Sb12	Pr	0.55	Nd	0.45	Os	4	Sb	12																3	2008																												skutterudite																		K		1.01					1.01	MTC150427																																																																																															molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150428	PHB4031038	not SWC. Curie-T shows ferromagnetic Curie-T; T<FM> defined as peak point of as-SUS.	(Pr,Nd)Os4Sb12	Pr0.4Nd0.6Os4Sb12	Pr	0.4	Nd	0.6	Os	4	Sb	12																3	2008							0.45																					skutterudite																		K					0.2																																																																																																		molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150429	PHB4031038	not SWC. Curie-T shows ferromagnetic Curie-T; T<FM> defined as peak point of as-SUS.	(Pr,Nd)Os4Sb12	Pr0.2Nd0.8Os4Sb12	Pr	0.2	Nd	0.8	Os	4	Sb	12																3	2008							0.59																					skutterudite																		K					0.2			MTC150427																																																																																															molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150430	PHB4031038	not SWC. Curie-T shows ferromagnetic Curie-T; T<FM> defined as peak point of as-SUS.	NdOs4Sb12	Nd1Os4Sb12	Nd	1	Os	4	Sb	12																		3	2008							0.83																					skutterudite																		K					0.2																																																																																																		molten-metal flux method					A comparison of the normal and superconducting state properties of Pr(Os1-xRuxT4Sb12 and Pr1-xNdxOs4Sb12				Physica B, 403(2008)1038	P.-C. Ho,T. Yanagisawa,N.P. Butch,W.M. Yuhasz,C.C. Robinson,A.A. Dooraghi,M.B. Maple		
150431	L097056404		CeCo(In,Cd)5	Ce1Co1In4.75Cd0.25	Ce	1	Co	1	In	4.75	Cd	0.25																	2006																												HoCoGa5																		K		2.13					2.13																																																																																																In-flux method					Reversible Tuning of the Heavy-Fermion Ground State in CeCoIn5			University of California, Davis, California 95616, USA	Phys.Rev.Lett., 97(2006)056404	L. D. Pham,Tuson Park,S. Maquilon,J. D. Thompson,Z. Fisk		
150432	L097056404		CeCo(In,Cd)5	Ce1Co1In4.5Cd0.5	Ce	1	Co	1	In	4.5	Cd	0.5																	2006																												HoCoGa5																		K		1.35					1.35	MTC150432																																																																																															In-flux method					Reversible Tuning of the Heavy-Fermion Ground State in CeCoIn5			University of California, Davis, California 95616, USA	Phys.Rev.Lett., 97(2006)056404	L. D. Pham,Tuson Park,S. Maquilon,J. D. Thompson,Z. Fisk		
150433	L097056404		CeCo(In,Cd)5	Ce1Co1In4.25Cd0.75	Ce	1	Co	1	In	4.25	Cd	0.75																	2006																												HoCoGa5																		K					0.78			MPH150433																																																																																															In-flux method					Reversible Tuning of the Heavy-Fermion Ground State in CeCoIn5			University of California, Davis, California 95616, USA	Phys.Rev.Lett., 97(2006)056404	L. D. Pham,Tuson Park,S. Maquilon,J. D. Thompson,Z. Fisk		
150434	PHB4031065	half Heusler compound. Carrier is hole. Hc2 < 1.5T(paramag-limit).	LaBiPt	La1Bi1Pt1	La	1	Bi	1	Pt	1																		3	2008																													F4[-]3m																	K		0.9					0.9																																																																																												E+18/cm3	6			Bridgeman method					Thermodynamic and transport properties of the non-centrosymmetric superconductor LaBiPt			Physikalisches Institut, Universitat Karlsruhe, 76128 Karlsruhe, Germany	Physica B, 403(2008)1065	G. Goll,M. Marz,A. Hamann,T. Tomanic,K. Grube,T. Yoshino,T. Takabatake		
150435	1965	refno=1965(PR01100500)	LaTe	La1Te1	La	1	Te	1																					1975																												NaCl			A	6.421														K		1.48					1.48																																																								mJ/mol.K2	4.65		175																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
150436	1965	refno=1965(PR01100500)	La3Te4	La3Te4	La	3	Te	4																					1975																												Th3P4			A	9.63														K		5.3					5.3																																																								mJ/mol.K2	4.3		162																																										Magnetic and some thermal properties of chalcogenides of Pr and Tm and a few other rare earths				PHYS.REV.B,11(1975)500	A.C.GOSSARD,A.S.COOPER,E.BUCHER,F.J.DISALVO,G.W.HULL JR.,J.P.MAITA,K.ANDRES		
150437	SSC0140161		LaAl2	Al2La1	Al	2	La	1																					1974																												MgCu2(Laves)																		K		3.24					3.24																																		MHC150437																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150438	SSC0140161		(La,Gd)Al2	La0.999Gd0.001Al2	La	0.999	Gd	0.001	Al	2																			1974																												MgCu2(Laves)																		K		2.78					2.78																																		MHC150437																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150439	SSC0140161		(La,Gd)Al2	La0.998Gd0.002Al2	La	0.998	Gd	0.002	Al	2																			1974																												MgCu2(Laves)																		K		2.39					2.39																																		MHC150437																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150440	SSC0140161		(La,Gd)Al2	La0.997Gd0.003Al2	La	0.997	Gd	0.003	Al	2																			1974																												MgCu2(Laves)																		K		1.89					1.89																																		MHC150440																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150441	SSC0140161		(La,Gd)Al2	La0.996Gd0.004Al2	La	0.996	Gd	0.004	Al	2																			1974																												MgCu2(Laves)																		K		1.38					1.38																																		MHC150440																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150442	SSC0140161		(La,Gd)Al2	La0.995Gd0.005Al2	La	0.995	Gd	0.005	Al	2																			1974																												MgCu2(Laves)																		K		0.932					0.932																																		MHC150440																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150443	PR01201778	(dC/Tc) = 41.0 mJ/gat.K2. For x=0.02, 0.05, 0.15 in (La1-xPrx)3In, Hc2(0) = 64.2, 52.7, 23 kOe, and (dHce/dT) = 8.04, 7.64, 5.72 kOe/K, respectively.	La3In	In1La3	In	1	La	3																					1975																												AuCu3																	AuCu3, L1<2>	K		9.95					9.95																				T		7.11							T/K		0.804																									mJ/gat.K2	14		170																																										Thermodynamic properties of superconductors containing impurities in a crystal-field singlet ground state				Phys.Rev.B, 12(1975)1778	F.Heiniger,E.Bucher,J.P.Maita,L.D.Longinotti		
150444	PR01201778	(dC/Tc) = 27.5 mJ/gat.K2.	(La,Pr)3In	La3Pr0.3In1	La	3	Pr	0.3	In	1																			1975																												AuCu3																	AuCu3, L1<2>	K		6.2					6.2																				T		3.52							T/K		0.639																									mJ/gat.K2	16.2																																												Thermodynamic properties of superconductors containing impurities in a crystal-field singlet ground state				Phys.Rev.B, 12(1975)1778	F.Heiniger,E.Bucher,J.P.Maita,L.D.Longinotti		
150445	PR01201778	(dC/Tc) = 18.6 mJ/gat.K2.	(La,Pr)3In	La3Pr0.6In1	La	3	Pr	0.6	In	1																			1975																												AuCu3																	AuCu3, L1<2>	K		3.2					3.2																																																								mJ/gat.K2	18.1		161																																										Thermodynamic properties of superconductors containing impurities in a crystal-field singlet ground state				Phys.Rev.B, 12(1975)1778	F.Heiniger,E.Bucher,J.P.Maita,L.D.Longinotti		
150446	PR01201778	(dC/Tc) = 15.2 mJ/gat.K2.	(La,Pr)3In	La3Pr0.75In1	La	3	Pr	0.75	In	1																			1975																												AuCu3																	AuCu3, L1<2>	K		1.94					1.94																																																								mJ/gat.K2	18.2		159																																										Thermodynamic properties of superconductors containing impurities in a crystal-field singlet ground state				Phys.Rev.B, 12(1975)1778	F.Heiniger,E.Bucher,J.P.Maita,L.D.Longinotti		
150447	PR01201778		Pr3In	Pr3In1	Pr	3	In	1																					1975								16.8																				AuCu3																	AuCu3, L1<2>	K																																																															mJ/gat.K2	24.3		160																																										Thermodynamic properties of superconductors containing impurities in a crystal-field singlet ground state				Phys.Rev.B, 12(1975)1778	F.Heiniger,E.Bucher,J.P.Maita,L.D.Longinotti		
150450	L097056404		CeIr(In,Cd)5	Ce1Ir1In4.875Cd0.125	Ce	1	Ir	1	In	4.875	Cd	0.125																	2006																												HoCoGa5																		K		0.194					0.194	MTC150450																																																																																															In-flux method					Reversible Tuning of the Heavy-Fermion Ground State in CeCoIn5			University of California, Davis, California 95616, USA	Phys.Rev.Lett., 97(2006)056404	L. D. Pham,Tuson Park,S. Maquilon,J. D. Thompson,Z. Fisk		
150452	SSC0140161		(La,Tb)Al2	La0.9985Tb0.0015Al2	La	0.9985	Tb	0.0015	Al	2																			1974																												MgCu2(Laves)																		K		2.9					2.9																																		MHC150452																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150453	SSC0140161		(La,Tb)Al2	La0.996Tb0.004Al2	La	0.996	Tb	0.004	Al	2																			1974																												MgCu2(Laves)																		K		2.4					2.4	MTC150453																																	MHC150452																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150454	SSC0140161		(La,Tb)Al2	La0.992Tb0.008Al2	La	0.992	Tb	0.008	Al	2																			1974																												MgCu2(Laves)																		K		1.61					1.61																																		MHC150454																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150455	SSC0140161		(La,Tb)Al2	La0.988Tb0.012Al2	La	0.988	Tb	0.012	Al	2																			1974																												MgCu2(Laves)																		K		0.94					0.94																																		MHC150454																																																														melt in HF-inductance furnace					The influence of crystal field split impurities(Tb) on the superconducting properties of LaAl2				Solid State Commun., 14(1974)161	G.Pepperl,E.Umlauf,A.Meyer,J.Keller		
150456	INT0160096		LaAl2	Al2La1	Al	2	La	1																					2008																												MgCu2(Laves)			A	8.1495														K	3.2		3.3				3.25																																																																																																arc-melting					Phase relationship in LaAl2-xSix (0 =< x = <1.03) and their electrical resistivity			National Institute for Materials Science, Advanced Electronic Materials Center, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Intermetallics, 16(2008)96	M.Imai,T.Aoyagi,T.Kimura		
150457	INT0160096	solubility limit sample with MgCu2-structure(0 =< x =<0.005)	La(Al,Si)2	La1Al1.995Si0.005	La	1	Al	1.995	Si	0.005																			2008																												MgCu2(Laves)			A	8.1494														K		2.9					2.9																																																																																																arc-melting					Phase relationship in LaAl2-xSix (0 =< x = <1.03) and their electrical resistivity			National Institute for Materials Science, Advanced Electronic Materials Center, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Intermetallics, 16(2008)96	M.Imai,T.Aoyagi,T.Kimura		
150458	INT0160096	AlB2-phase for 0.14 =< x =<0.62	La(Al,Si)2	La1Al1.825Si0.175	La	1	Al	1.825	Si	0.175																			2008																												AlB2			A	4.4275		4.387												K					2																																																																																																		arc-melting					Phase relationship in LaAl2-xSix (0 =< x = <1.03) and their electrical resistivity			National Institute for Materials Science, Advanced Electronic Materials Center, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Intermetallics, 16(2008)96	M.Imai,T.Aoyagi,T.Kimura		
150459	INT0160096	alpha-ThSi2-phase for 0.72 =< x =<1.03.	La(Al,Si)2	La1Al1.26Si0.74	La	1	Al	1.26	Si	0.74																			2008																												ThSi2			A	4.3377		14.868											alpha-ThSi2	K					2																																																																																																		arc-melting					Phase relationship in LaAl2-xSix (0 =< x = <1.03) and their electrical resistivity			National Institute for Materials Science, Advanced Electronic Materials Center, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Intermetallics, 16(2008)96	M.Imai,T.Aoyagi,T.Kimura		
150460	PR03200135	Tc defined as midpoint of SUS-transition. magnetic transition(T=0.23 K) was observed in SP. lattice term of SP, beta = 1.80 mJ/mol.K4.	Pd2YbSn	Pd2Yb1Sn1	Pd	2	Yb	1	Sn	1																			1985							0.23																					Heusler																	Heusler, Cu2MnAl, L1<2>	K	2.3	2.36	2.7	2.36			2.36																																																								mJ/mol.K2	0.1	SP-heat	114	SP-heat																																				arc-melting, then ANN(900C,8d, in vac)					Coexistence of ordered magnetism and superconductivity in Pd2YbSn			Argonne National Lab.	Phys.Rev.B, 32(1985)135	H.A.Kierstead,B.D.Dunlap,S.K.Malik,A.M.Umarji,G.K.Shenoy		
150461	MTL0020090	ANN(900C,6d). SUS(300 K) = -3.17 E-5 emu/mol.	Au2InY	Au2In1Y1	Au	2	In	1	Y	1																			1983																												Heusler			A	6.905													Heusler, Cu2MnAl, L1<2>	K		1.74				0.1	1.74																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150462	MTL0020090	not ANN. SUS(300 K) = -0.81 E-5 emu/mol.	(Au,Pd)2InY	Au1.8Pd0.2In1Y1	Au	1.8	Pd	0.2	In	1	Y	1																	1983																												Heusler			A	6.876													Heusler, Cu2MnAl, L1<2>	K		2.27				0.02	2.27																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150463	MTL0020090	ANN(900C) - Q. SUS(300 K) = 1.57 E-5 emu/mol.	(Au,Pd)2InY	Au1.6Pd0.4In1Y1	Au	1.6	Pd	0.4	In	1	Y	1																	1983																												Heusler			A	6.873													Heusler, Cu2MnAl, L1<2>	K		2.64				0.1	2.64																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150464	MTL0020090	ANN(900C) - Q. SUS(300 K) = 2.83 E-5 emu/mol.	(Au,Pd)2InY	Au1.3Pd0.7In1Y1	Au	1.3	Pd	0.7	In	1	Y	1																	1983																												Heusler			A	6.85													Heusler, Cu2MnAl, L1<2>	K		2.68				0.12	2.68																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150465	MTL0020090	ANN(900C) - Q. SUS(300 K) = 2.03 E-5 emu/mol.	(Au,Pd)2InY	Au1Pd1In1Y1	Au	1	Pd	1	In	1	Y	1																	1983																												Heusler			A	6.832													Heusler, Cu2MnAl, L1<2>	K		2.3				0.14	2.3																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150466	MTL0020090	as-prepared.  SUS(300 K) = 0.695 E-5 emu/mol.	(Au,Pd)2InY	Au0.2Pd1.8In1Y1	Au	0.2	Pd	1.8	In	1	Y	1																	1983																												Heusler			A	6.727													Heusler, Cu2MnAl, L1<2>	K		1.24				0.04	1.24																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150467	MTL0020090	as-prepared. SUS(300 K) = 1.12 E-5 emu/mol.	Pd2InY	Pd2In1Y1	Pd	2	In	1	Y	1																			1983																												Heusler			A	6.72													Heusler, Cu2MnAl, L1<2>	K		1.04				1.12	1.04																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150468	MTL0020090	as-prepared. SUS(300 K) = 2.35 E-5 emu/mol.	Pd2SnY	Pd2Sn1Y1	Pd	2	Sn	1	Y	1																			1983																												Heusler			A	6.718													Heusler, Cu2MnAl, L1<2>	K		4.9				0.2	4.9																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150469	MTL0020090	as-prepared. SUS(300 K) = 24.70 E-5 emu/mol.	Ni2HfAl	Ni2Hf1Al1	Ni	2	Hf	1	Al	1																			1983																												Heusler			A	6.069													Heusler, Cu2MnAl, L1<2>	K		0.74				0.03	0.74																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150470	MTL0020090	as-prepared. SUS(300 K) = 29.68 E-5 emu/mol.	Ni2ZrAl	Ni2Zr1Al1	Ni	2	Zr	1	Al	1																			1983																												Heusler			A	6.106													Heusler, Cu2MnAl, L1<2>	K		1.38				0.17	1.38																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150471	MTL0020090	as-prepared. SUS(300 K) = 22.56 E-5 emu/mol.	Ni2HfGa	Ni2Hf1Ga1	Ni	2	Hf	1	Ga	1																			1983																												Heusler			A	6.045													Heusler, Cu2MnAl, L1<2>	K		1.12				0.03	1.12																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150472	MTL0020090	ANN(900C,12d). SUS(300 K) = 7.40 E-5 emu/mol.	Ni2NbSn	Ni2Nb1Sn1	Ni	2	Nb	1	Sn	1																			1983																												Heusler			A	6.179													Heusler, Cu2MnAl, L1<2>	K		3.4				0.4	3.4																																																																																																arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150473	MTL0020090	not SC.	Au2GaY	Au2Ga1Y1	Au	2	Ga	1	Y	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150474	MTL0020090	not SC.	Au2InEr	Au2In1Er1	Au	2	In	1	Er	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150475	MTL0020090	not SC.	Au2InTm	Au2In1Tm1	Au	2	In	1	Tm	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150476	MTL0020090	not SC.	Pd2AlY	Pd2Al1Y1	Pd	2	Al	1	Y	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150477	MTL0020090	not SC.	Pd2GeY	Pd2Ge1Y1	Pd	2	Ge	1	Y	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150478	MTL0020090	not SC.	Pt2InY	Pt2In1Y1	Pt	2	In	1	Y	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150479	MTL0020090	not SC.	Au2InYb	Au2In1Yb1	Au	2	In	1	Yb	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150480	MTL0020090	not SC.	Cu2ZrAl	Cu2Zr1Al1	Cu	2	Zr	1	Al	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150481	MTL0020090	not SC.	Cu2InTi	Cu2In1Ti1	Cu	2	In	1	Ti	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150482	MTL0020090	not SC.	Cu2TiSn	Cu2Ti1Sn1	Cu	2	Ti	1	Sn	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150483	MTL0020090	not SC.	Ti2MoGa	Ti2Mo1Ga1	Ti	2	Mo	1	Ga	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150484	MTL0020090	not SC.	Ni2TiSn	Ni2Ti1Sn1	Ni	2	Ti	1	Sn	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150485	MTL0020090	not SC.	Ni2TiIn	Ni2Ti1In1	Ni	2	Ti	1	In	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150486	MTL0020090	not SC.	Ni2VSn	Ni2V1Sn1	Ni	2	V	1	Sn	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150487	MTL0020090	not SC.	Ni2HfSn	Ni2Hf1Sn1	Ni	2	Hf	1	Sn	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150488	MTL0020090	not SC.	Ni2ZnSn	Ni2Zn1Sn1	Ni	2	Zn	1	Sn	1																			1983																												Heusler																	Heusler, Cu2MnAl, L1<2>	K					0.5																																																																																																		arc-melting or melt by induction furnace					Superconductivity in ternary heusler intermetallic compounds			Bell Lab, Murray Hill	Mater.Lett., 2(1983)90	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
150489	SSC0130025		(La,Tm)Sn3	La0.92Tm0.08Sn3	La	0.92	Tm	0.08	Sn	3																			1973																																														K		5.17					5.17																																		MHC150489																																																																			Upper critical fields of superconducting Gd and Tm doped LaSn3: Effects of crystalline electric fields			Tufts University, Medford, Mass., USA	Solid State Commun., 13(1973)25	R.P.Guertin,J.E.Crow,A.R.Sweedler,S.Foner		
150490	SSC0130025		(La,Tm)Sn3	La0.84Tm0.16Sn3	La	0.84	Tm	0.16	Sn	3																			1973																																														K		3.33					3.33																																		MHC150489																																																																			Upper critical fields of superconducting Gd and Tm doped LaSn3: Effects of crystalline electric fields			Tufts University, Medford, Mass., USA	Solid State Commun., 13(1973)25	R.P.Guertin,J.E.Crow,A.R.Sweedler,S.Foner		
150491	SSC0130025		(La,Gd)Sn3	La0.933Gd0.067Sn3	La	0.933	Gd	0.067	Sn	3																			1973																																														K		4.64					4.64																				Oe		687												MHC150491																																																																			Upper critical fields of superconducting Gd and Tm doped LaSn3: Effects of crystalline electric fields			Tufts University, Medford, Mass., USA	Solid State Commun., 13(1973)25	R.P.Guertin,J.E.Crow,A.R.Sweedler,S.Foner		
150492	SSC0130025		(La,Gd)Sn3	La0.92Gd0.08Sn3	La	0.92	Gd	0.08	Sn	3																			1973																																														K		4.28					4.28																				Oe		603												MHC150491																																																																			Upper critical fields of superconducting Gd and Tm doped LaSn3: Effects of crystalline electric fields			Tufts University, Medford, Mass., USA	Solid State Commun., 13(1973)25	R.P.Guertin,J.E.Crow,A.R.Sweedler,S.Foner		
150493	L100097002	There are two gaps. GAP and GAPENE shows for higher one. For lower one, GAP = 0.6 meV, GAPENE = 1.3.	La2C3	C3La2	C	3	La	2																					2008																												Pu2C3			A	8.808														K		11.2					11.2																				T		16.7												MHC150493							A	muon-SR	3800			meV	2.7	5.6																																																arc-melting - pellet - in sealed Ta tube - SIN(1000C,200h, in vac) - cool to RT(5C/h)					Multigap Superconductivity in Sesquicarbides La2C3 and Y2C3			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.Lett., 100(2008)097002	S. Kuroiwa,Y. Saura,J. Akimitsu,M. Hiraishi,M. Miyazaki,K. H. Satoh,S. Takeshita,R. Kadono		
150494	L100097002	There are two gaps. GAP and GAPENE shows for higher one. For lower one, GAP = 0.7 meV, GAPENE = 1.1.	Y2C3	C3Y2	C	3	Y	2																					2008																												Pu2C3			A	8.238														K		15.2					15.2																				T		25.6												MHC150494							A	muon-SR	4600			meV	3.1	4.9																																																arc-melting - heat(1300-1400C,30min, P= 5GPa)					Multigap Superconductivity in Sesquicarbides La2C3 and Y2C3			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.Lett., 100(2008)097002	S. Kuroiwa,Y. Saura,J. Akimitsu,M. Hiraishi,M. Miyazaki,K. H. Satoh,S. Takeshita,R. Kadono		
150495	P077064506	T2 defined as max of (dM/dT).	NbB2	B2.2Nb1	B	2.2	Nb	1																					2008																																														K		3.6		4.79			3.6																																																																																																					Correlation between the transition temperature and the superfluid density in BCS superconductor NbB2+x			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 77(2008)064506	R. Khasanov,A. Shengelaya,A. Maisuradze,D. Di Castro,R. Escamilla,H. Keller		
150496	P077064506	T2 defined as max of (dM/dT).	NbB2	B2.34Nb1	B	2.34	Nb	1																					2008																																														K		9.16		9.76			9.16																																																																																																					Correlation between the transition temperature and the superfluid density in BCS superconductor NbB2+x			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 77(2008)064506	R. Khasanov,A. Shengelaya,A. Maisuradze,D. Di Castro,R. Escamilla,H. Keller		
150497	P077092505	(CaO)12(Al2O3)7, popular name = C12A7:e.  el-concentration = 2 E+21 /cm3 from reflectance. e-ph coupling = 0.46. (dC/gamma*Tc) = 1.22. lattice term in SP = 0.46 mJ/mol.K4	Ca24Al28O64:(4e)	Ca24Al28O66	Ca	24	Al	28																	O	66			2008																																														K		0.195					0.195																																																					MSP150497	mJ/mol.K	3.4	mJ/mol.K2	14.2	SP-HEAT	628	SP-HEAT																																				single crystal grown by FZ method. heat(1100C,24h, in evacuated silicon tube with Ti)					Evidence for Bardeen-Cooper-Schrieffer-type superconducting behavior in the electride (Ca)12(Al2O3)7 :e- from heat capacity measurements			Materials and Structures Laboratory, Tokyo Institute of Technology, Mail-Box R3-7, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 77(2008)092505	Yoshimitsu Kohama,Sung Wng Kim,Takeo Tojo,Hitoshi Kawaji,Tooru Atake,Satoru Matsuishi,Hideo Hosono		
150498	PHB3120129		Ce(Ir,Co)In5	Ce1Ir0.75Co0.25In5	Ce	1	Ir	0.75	Co	0.25	In	5																	2002																												HoCoGa5																		K		1.52					1.52																																																																																																					Multiple phase transitions in Ce(Rh,Ir,Co)In5			Los Alamos National Laboratory, MS K 764, MST-10, Los Alamos, NM 87545, USA	Physica B, 312-312(2002)129	P.G. Pagliuso,R. Movshovich,A.D. Bianchi,M. Nicklas,N.O. Moreno,J.D. Thompson,M.F. Hundley,J.L. Sarrao,Z. Fisk		
150499	PHB3120129		Ce(Ir,Co)In5	Ce1Ir0.3Co0.7In5	Ce	1	Ir	0.3	Co	0.7	In	5																	2002																												HoCoGa5																		K		2					2																																																																																																					Multiple phase transitions in Ce(Rh,Ir,Co)In5			Los Alamos National Laboratory, MS K 764, MST-10, Los Alamos, NM 87545, USA	Physica B, 312-312(2002)129	P.G. Pagliuso,R. Movshovich,A.D. Bianchi,M. Nicklas,N.O. Moreno,J.D. Thompson,M.F. Hundley,J.L. Sarrao,Z. Fisk		
150500	PHB4031074	P-induced SC.	Li0.9Mg0.1	Li0.9Mg0.1	Li	0.9	Mg	0.1																					2008																																														K		11			0		11	MTC150500		K/GPa	0.34																																																																																																	Superconductivity in Sc metal and Li(Mg) alloy under extreme pressure			Department of Physics, Washington University, CB 1105, One Brookings Drive, St. Louis, MO 63130, USA	Physica B, 403(2008)1074	J.J. Hamlin,M. Debessai,J.S. Schilling		
150501	PHB4031129		CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																			2008								2.29																				CePt3B			A	4.075		5.442												K		0.745					0.745																																																								mJ/mol.K2	420																																												Evolution of superconductivity and magnetic order in heavy fermion superconductor Ce(Pt1-xNix)3Si			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Physica B, 403(2008)1129	H. Kaldarar,H. Michor,M. Reissner,E.W. Scheidt,P. Rogl,E. Bauer		
150502	PHB4031129		Ce(Pt,Ni)3Si	Ce1Pt2.94Ni0.06Si1	Ce	1	Pt	2.94	Ni	0.06	Si	1																	2008								2.59																				CePt3B			A	4.0751		5.4412												K		0.545					0.545																																																								mJ/mol.K2	380																																												Evolution of superconductivity and magnetic order in heavy fermion superconductor Ce(Pt1-xNix)3Si			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Physica B, 403(2008)1129	H. Kaldarar,H. Michor,M. Reissner,E.W. Scheidt,P. Rogl,E. Bauer		
150503	PHB4031129		Ce(Pt,Ni)3Si	Ce1Pt2.82Ni0.18Si1	Ce	1	Pt	2.82	Ni	0.18	Si	1																	2008								2.2																				CePt3B			A	4.0776		5.4406												K		0.473					0.473																																																																																																					Evolution of superconductivity and magnetic order in heavy fermion superconductor Ce(Pt1-xNix)3Si			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Physica B, 403(2008)1129	H. Kaldarar,H. Michor,M. Reissner,E.W. Scheidt,P. Rogl,E. Bauer		
150504	P077113103	CDW observed in R(T) and C(T). T<CDW> = 83 K.	Lu5Ir4Si10	Lu5Ir4Si10	Lu	5	Ir	4	Si	10																			2008																												Sc5Co4Si10																		K		3.9					3.9																																																																																																arc-melting, remelted with 5% excess Yb for compensate the weight loss.					Kondo effect in the charge-density-wave state of Lu5-xYbxIr4Si10			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 77(2008)113103	Manjusha Inamdar,S. Ramakrishnan		
150505	P077113103	CDW observed in R(T) and C(T). T<CDW> = 78 K. Kondo-Temp = 4.7 K from SUS measurements.	(Lu,Yb)5Ir4Si10	Lu4.98Yb0.02Ir4Si10	Lu	4.98	Yb	0.02	Ir	4	Si	10																	2008																												Sc5Co4Si10																		K		3					3																																																																																																arc-melting, remelted with 5% excess Yb for compensate the weight loss.					Kondo effect in the charge-density-wave state of Lu5-xYbxIr4Si10			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 77(2008)113103	Manjusha Inamdar,S. Ramakrishnan		
150506	P077113103	CDW observed in R(T) and C(T). T<CDW> = 73 K. Kondo-Temp = 4.8 K from SUS measurements.	(Lu,Yb)5Ir4Si10	Lu4.95Yb0.05Ir4Si10	Lu	4.95	Yb	0.05	Ir	4	Si	10																	2008																												Sc5Co4Si10																		K		2					2																																																																																																arc-melting, remelted with 5% excess Yb for compensate the weight loss.					Kondo effect in the charge-density-wave state of Lu5-xYbxIr4Si10			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 77(2008)113103	Manjusha Inamdar,S. Ramakrishnan		
150507	P077113103	CDW observed in R(T) and C(T). T<CDW> = 69 K. Kondo-Temp = 5.0 K from SUS measurements.	(Lu,Yb)5Ir4Si10	Lu4.93Yb0.07Ir4Si10	Lu	4.93	Yb	0.07	Ir	4	Si	10																	2008																												Sc5Co4Si10																		K		1.5					1.5																																																								mJ/mol.K2	40																																							arc-melting, remelted with 5% excess Yb for compensate the weight loss.					Kondo effect in the charge-density-wave state of Lu5-xYbxIr4Si10			Tata Institute of Fundamental Research, Mumbai-400005, India	Phys.Rev.B, 77(2008)113103	Manjusha Inamdar,S. Ramakrishnan		
150508	P077100505	RRR = 1000. bulk SC confirmed by SUS and SP-heat measurements at P = 0.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																												HoCoGa5																		K				0.11			0.11										70																																														mJ/mol.K2	56														nOhm.cm							37																		self flux method					Ambient-pressure bulk superconductivity deep in the magnetic state of CeRhIn5			Department of Physics, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 77(2008)100505(R)	Johnpierre Paglione,P.-C. Ho,M. B. Maple,M. A. Tanatar,Louis Taillefer,Y. Lee,C. Petrovic		
150509	P077100505	RRR > 100.	RhIn3	In3Rh1	In	3	Rh	1																				3	2008																																														K				0.19			0.19																																																																																																self flux method					Ambient-pressure bulk superconductivity deep in the magnetic state of CeRhIn5			Department of Physics, University of California at San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 77(2008)100505(R)	Johnpierre Paglione,P.-C. Ho,M. B. Maple,M. A. Tanatar,Louis Taillefer,Y. Lee,C. Petrovic		
150510	PHC1820132	O-exchange by diffusion (600-700 C, 1 bar O2)	(Bi,Pb)2Sr2Ca2Cu3O10	Bi1.6Pb0.4Sr2Ca2Cu3O10	Bi	1.6	Pb	0.4	Sr	2	Ca	2	Cu	3											O	10		1	1991																												Bi2223																		K		108					108						-0.013	O	90	-0.14																																																																																												NEGATIVE OXYGEN ISOTOPE SHIFT IN BI-2223 (BI1.6PB0.4SR2CA2CU3O10) WITH TC=108K	199110		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY CA 94704,USA	PHYSICA C,182(1991)132	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN	BI,PB,SR,CA,CU,O	
150511	PHC1820132	Details not given.	Y(Ba,Sr)2Cu3O7	Y1Ba1.8Sr0.2Cu3O7-z	Y	1	Ba	1.8	Sr	0.2	Cu	3													O	7-z		1	1991																												Y123																		K		90					90						0.023	O																																																																																														NEGATIVE OXYGEN ISOTOPE SHIFT IN BI-2223 (BI1.6PB0.4SR2CA2CU3O10) WITH TC=108K	199110		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY CA 94704,USA	PHYSICA C,182(1991)132	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN	BI,PB,SR,CA,CU,O	
150512	PHC1820132	Details not given.	Y(Ba,Sr)2Cu3O7	Y1Ba1.5Sr0.5Cu3O7-z	Y	1	Ba	1.5	Sr	0.5	Cu	3													O	7-z		1	1991																												Y123																		K		85.5					85.5						-0.001	O																																																																																														NEGATIVE OXYGEN ISOTOPE SHIFT IN BI-2223 (BI1.6PB0.4SR2CA2CU3O10) WITH TC=108K	199110		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY CA 94704,USA	PHYSICA C,182(1991)132	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN	BI,PB,SR,CA,CU,O	
150513	PHC1820132	Details not given.	Y(Ba,Sr)2Cu3O7	Y1Ba1Sr1Cu3O7-z	Y	1	Ba	1	Sr	1	Cu	3													O	7-z		1	1991																												Y123																		K		81					81						-0.014	O																																																																																														NEGATIVE OXYGEN ISOTOPE SHIFT IN BI-2223 (BI1.6PB0.4SR2CA2CU3O10) WITH TC=108K	199110		MORRIS RESEARCH INC.,1918 UNIVERSITY AVENUE,BERKELEY CA 94704,USA	PHYSICA C,182(1991)132	D.E.MORRIS,H.B.LIU,H.J.BORNEMANN	BI,PB,SR,CA,CU,O	
150514	P077054507		(Cu,Tl)Ba2Ca3Cu4O12	Tl0.5Ba2Ca3Cu4.5O12-z	Tl	0.5	Ba	2	Ca	3	Cu	4.5													O	12-z			2008																												Tl1234	P4/mmm		A			18.3164												K	108.5						108.5																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150515	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu4Zn0.5O12-z	Tl	0.5	Ba	2	Ca	3	Cu	4	Zn	0.5											O	12-z			2008																												Tl1234	P4/mmm		A															K	110.5						110.5																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150516	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu3.5Zn1O12-z	Tl	0.5	Ba	2	Ca	3	Cu	3.5	Zn	1											O	12-z			2008																												Tl1234	P4/mmm		A			18.0211												K	112.5						112.5																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150517	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu3Zn1.5O12-z	Tl	0.5	Ba	2	Ca	3	Cu	3	Zn	1.5											O	12-z			2008																												Tl1234	P4/mmm		A			17.9464												K	113.3						113.3																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150518	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu2.5Zn2O12-z	Tl	0.5	Ba	2	Ca	3	Cu	2.5	Zn	2											O	12-z			2008																												Tl1234	P4/mmm		A			17.6643												K	115.3						115.3																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150519	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu2Zn2.5O12-z	Tl	0.5	Ba	2	Ca	3	Cu	2	Zn	2.5											O	12-z			2008																												Tl1234	P4/mmm		A			17.5894												K	119.8						119.8																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150520	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu1.5Zn3O12-z	Tl	0.5	Ba	2	Ca	3	Cu	1.5	Zn	3											O	12-z			2008																												Tl1234	P4/mmm		A			17.5013												K	121.3						121.3																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150521	P077054507		(Cu,Tl)Ba2Ca3(Cu,Zn)4O12	Tl0.5Ba2Ca3Cu1Zn3.5O12-z	Tl	0.5	Ba	2	Ca	3	Cu	1	Zn	3.5											O	12-z			2008																												Tl1234	P4/mmm		A			17.5718												K	122.2						122.2																																																																																															1	precursor(Cu0.5Ba2Ca3Cu4-xZnxO12-z) was prepared by heating(880 C,24h, in quarts tube), then mixed with Tl2O3 - pellet - ANN(880C,10min, in Au-capsoule)					Absence of a pair-breaking mechanism in Cu0.5Tl0.5Ba2Ca3Cu4-yZnyO12-z			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan, 45320	Phys.Rev.B, 77(2008)054507	Nawazish Ali Khan,Muhammad Mumtaz		
150522	J077024707	crystals kept in dry air. two structural transitions(90K, 185K). RRR = 500-1400. (dC/gamma*Tc) = 0.94. G-L = 4.2.	Ag6O8AgNO3	Ag7N1O11	Ag	7	N	1																	O	11		3	2008																												clathrate	Fm3[-]m	225																K	1.04					0.04	1.04											Oe		22							Oe		770							Oe/K		1058			HC150522		A		660			A		2700					2.35	14							mJ/mol.K2	46.5	SP-HEAT	243	SP-HEAT											uOhm.cm							0.2																		electrochemical reaction					Superconducting State of Silver-Oxide Clathrate Ag6O8AgNO3			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 77(2008)024707	Kenji KAWASHIMA,Masaru ISHII,Hirotaka OKABE,Jun AKIMITSU,Markus KRIENER1,Hiroshi TAKATSU,Shingo YONEZAWA,Yoshiteru MAENO		
150523	PCS0312673	(lattice constant): c/a = 0.9603 (T=10 K).  Tc determined by SP.  thermodynamic Hc(0) = 130 Oe.	Ag7O8NO3	Ag7N1O11	Ag	7	N	1																	O	11			1970																												clathrate																		K	1.004	1.025	1.046				1.025																																																								mJ/mol.K2	44.6	SP-heat	85.3	SP-heat																																									Low-temperature heat capacities of the clathrate salts Ag7O8NO3 and Ag7O8HF2			University of California, Berkeley, Calif. USA	J.Phys.Chem.Solids, 31(1970)2673	Mary M.Conway,Norman E.Phillips,T.H.Gebelle,N.A.Kuebler		
150524	PCS0312673	Tc = 0.5 - 1.5 K.	Ag7O8HF2	Ag7H1F2O8	Ag	7	H	1	F	2															O	8			1970																												clathrate																		K		1.5					1.5																																																								mJ/mol.K2	72.5	SP-heat	125	SP-heat																																									Low-temperature heat capacities of the clathrate salts Ag7O8NO3 and Ag7O8HF2			University of California, Berkeley, Calif. USA	J.Phys.Chem.Solids, 31(1970)2673	Mary M.Conway,Norman E.Phillips,T.H.Gebelle,N.A.Kuebler		
150525	PRL0622751	LTT-phase = 66.9 %.	(La,Ba)2CuO4	La1.901Ba0.099Cu1O4	La	1.901	Ba	0.099	Cu	1															O	4			1989																												T																		K		12.3					12.3																																																																																														La2O3,BaCO3,CuO	1						STRUCTURAL PHASE TRANSFORMATIONS AND SUPERCONDUCTIVITY IN LA2-XBAXCUO4	198906		BROOKHAVEN NATIONAL LABORATORY,UPRON,NEW YORK 11973	PHYS.REV.LETT.,62(1989)2751	A.H.MOUDDEN,A.R.MOODENBAUGH,D.E.COX,D.HOHLWEIN,J.D.AXE,K.M.MOHANTY,YOUWEN XU	LA,BA,CU,O	
150526	PRL0622751	LTT-phase = 55 %.	(La,Ba)2CuO4	La1.87Ba0.13Cu1O4	La	1.87	Ba	0.13	Cu	1															O	4			1989																												T																		K		5.94					5.94	TC150526																																																																																													La2O3,BaCO3,CuO	1						STRUCTURAL PHASE TRANSFORMATIONS AND SUPERCONDUCTIVITY IN LA2-XBAXCUO4	198906		BROOKHAVEN NATIONAL LABORATORY,UPRON,NEW YORK 11973	PHYS.REV.LETT.,62(1989)2751	A.H.MOUDDEN,A.R.MOODENBAUGH,D.E.COX,D.HOHLWEIN,J.D.AXE,K.M.MOHANTY,YOUWEN XU	LA,BA,CU,O	
150527	PRL0622751	LTT-phase = 40 %.	(La,Ba)2CuO4	La1.825Ba0.175Cu1O4	La	1.825	Ba	0.175	Cu	1															O	4			1989																												T																		K		25.7					25.7																																																																																														La2O3,BaCO3,CuO	1						STRUCTURAL PHASE TRANSFORMATIONS AND SUPERCONDUCTIVITY IN LA2-XBAXCUO4	198906		BROOKHAVEN NATIONAL LABORATORY,UPRON,NEW YORK 11973	PHYS.REV.LETT.,62(1989)2751	A.H.MOUDDEN,A.R.MOODENBAUGH,D.E.COX,D.HOHLWEIN,J.D.AXE,K.M.MOHANTY,YOUWEN XU	LA,BA,CU,O	
150528	PRL0622751		(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4			1989																												T																		K		9.38					9.38																																																																																														La2O3,BaCO3,CuO	1						STRUCTURAL PHASE TRANSFORMATIONS AND SUPERCONDUCTIVITY IN LA2-XBAXCUO4	198906		BROOKHAVEN NATIONAL LABORATORY,UPRON,NEW YORK 11973	PHYS.REV.LETT.,62(1989)2751	A.H.MOUDDEN,A.R.MOODENBAUGH,D.E.COX,D.HOHLWEIN,J.D.AXE,K.M.MOHANTY,YOUWEN XU	LA,BA,CU,O	
150529	PHC2821233		(La,Sr)2(Cu,Zn)O4	La1.89Sr0.11Cu0.885Zn0.115O4	La	1.89	Sr	0.11	Cu	0.885	Zn	0.115													O	4			1997																												T																		K																																																																																																												Possibility of the Pinning of the Stripe Pattern of Holes and Spins by Zn in La2-xSrxCu1-yZny with x ~0.115			Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980-77, Japan	Physica C, 282-287(1997)1233	Y. Koike,S. Takeuchi,Y. Hama,H. Sato,T. Adachi,M. Kato		
150530	PHC2821233		(La,Sr)2(Cu,Zn)O4	La1.88Sr0.12Cu0.885Zn0.115O4	La	1.88	Sr	0.12	Cu	0.885	Zn	0.115													O	4			1997																												T																		K								TC150530																																																																																																				Possibility of the Pinning of the Stripe Pattern of Holes and Spins by Zn in La2-xSrxCu1-yZny with x ~0.115			Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980-77, Japan	Physica C, 282-287(1997)1233	Y. Koike,S. Takeuchi,Y. Hama,H. Sato,T. Adachi,M. Kato		
150531	PHC2821233		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.885Zn0.115O4	La	1.85	Sr	0.15	Cu	0.885	Zn	0.115													O	4			1997																												T																		K																																																																																																												Possibility of the Pinning of the Stripe Pattern of Holes and Spins by Zn in La2-xSrxCu1-yZny with x ~0.115			Department of Applied Physics, Faculty of Engineering, Tohoku University, Sendai 980-77, Japan	Physica C, 282-287(1997)1233	Y. Koike,S. Takeuchi,Y. Hama,H. Sato,T. Adachi,M. Kato		
150532	SSC0660387	VOLS estimated from SUS(7K).	(La,Na)2CuO4	La1.89Na0.11Cu1O4	La	1.89	Na	0.11	Cu	1															O	4			1988																												T																		K		16	21			3	16										7																																																																																				La2O3,Na2CO3,CuO	1	mixture - pelletize in covered alumina crucible - CAL(840C,12h, in air) - SIN(900C,20h, in air) - SIN(1000C,24h, in flowing O2) - cool to RT(100C/h)					SUPERCONDUCTIVITY IN La2-xNaxCuO4-y			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Solid State Commun., 66(1988)387	J. T. Marked,C. L. Seaman,H. Zhou,M. B. Maple		
150533	SSC0660387	VOLS estimated from SUS(7K).	(La,Na)2CuO4	La1.59Na0.41Cu1O4	La	1.59	Na	0.41	Cu	1															O	4			1988																												T																		K		18	25			3	18										18																																																																																				La2O3,Na2CO3,CuO	1	mixture - pelletize in covered alumina crucible - CAL(840C,12h, in air) - SIN(900C,20h, in air) - SIN(1000C,24h, in flowing O2) - cool to RT(100C/h)					SUPERCONDUCTIVITY IN La2-xNaxCuO4-y			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Solid State Commun., 66(1988)387	J. T. Marked,C. L. Seaman,H. Zhou,M. B. Maple		
150534	PHC1621681		(Sm,La,Sr)2CuO4	Sm1La0.82Sr0.18Cu1O4	Sm	1	La	0.82	Sr	0.18	Cu	1													O	4			1989																												T*																		K			37				37																																																																																																					T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150535	PHC1621681		(Sm,La,Sr)2CuO4	Sm0.96La0.84Sr0.2Cu1O4	Sm	0.96	La	0.84	Sr	0.2	Cu	1													O	4			1989																												T*																		K			35				35																																																																																																					T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150536	PHC1621681	Tc defined as 5% of SUS(max). oxygenation at 150 bar, 550 C.	(Sm,La,Sr)2CuO4	Sm1La0.802Sr0.198Cu1O4	Sm	1	La	0.802	Sr	0.198	Cu	1													O	4			1989																												T*																		K		17.2					17.2	TC150536																																																																																																				T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150537	PHC1621681	oxygenation at 150 bar	(Sm,La,Sr)2CuO4	Sm0.716La1.084Sr0.2Cu1O4	Sm	0.716	La	1.084	Sr	0.2	Cu	1													O	4			1989																												T*																		K		18.1					18.1	TC150537																																																																																																				T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150538	PHC1621681		(Eu,La,Sr)2CuO4	Eu1.007La0.793Sr0.2Cu1O4	Eu	1.007	La	0.793	Sr	0.2	Cu	1													O	4			1989																												T*																		K		29.2					29.2	TC150538																																																																																																				T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150539	PHC1621681		(Gd,La,Sr)2CuO4	Gd0.91La0.89Sr0.2Cu1O4	Gd	0.91	La	0.89	Sr	0.2	Cu	1													O	4			1989																												T*																		K		13.5					13.5	TC150539																																																																																																				T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150540	PHC1621681		(Sm,La,Sr)2CuO4	Sm0.9La0.9Sr0.2Cu1O4	Sm	0.9	La	0.9	Sr	0.2	Cu	1													O	4			1989																												T*																		K			34				34																																																																																																					T* -phase superconductivity			Los Alamos National Laboratory, Los Alamos, NM 87545	Physica C, 162-164(1989)1681	Z. FISK,S-W. CHEONG,J. D. THOMPSON,M. F. HUNDLEY,R. B. SCHWARZ,G. H. KWEI,J. E. SCHIRBER		
150541	PHC2510238	volume fraction of SC < 5%.	(Bi,La,Y)2SrCu2Oz	Bi0.5La0.5Y1Sr1Cu2O6.04	Bi	0.5	La	0.5	Y	1	Sr	1	Cu	2											O	z	6.04		1995																												Bi0212	I4/mmm		A	3.824		19.77												K																																																																																																												Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150542	PHC2510238	volume fraction of SC < 5%.	(Bi,La,Y)2SrCu2Oz	Bi0.5La1Y0.5Sr1Cu2O6.04	Bi	0.5	La	1	Y	0.5	Sr	1	Cu	2											O	z	6.04		1995																												Bi0212	I4/mmm		A	3.849		19.81												K				30			30																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150543	PHC2510238	volume fraction of SC < 5%.	(Bi,La)2SrCu2Oz	Bi0.5La1.5Sr1Cu2O6.02	Bi	0.5	La	1.5	Sr	1	Cu	2													O	z	6.02		1995																												Bi0212	I4/mmm		A	3.864		19.98												K				28			28																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150544	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.3Pb0.2La1.5Sr1Cu2O5.94	Bi	0.3	Pb	0.2	La	1.5	Sr	1	Cu	2											O	z	5.94		1995																												Bi0212	I4/mmm		A	3.866		19.97												K				24			24																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150545	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.3Pb0.3La1.2Sr1.2Cu2O5.81	Bi	0.3	Pb	0.3	La	1.2	Sr	1.2	Cu	2											O	z	5.81		1995																												Bi0212	I4/mmm		A	3.852		19.94												K				55			55																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150546	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.2Pb0.4La1.2Sr1.3Cu1.9O5.78	Bi	0.2	Pb	0.4	La	1.2	Sr	1.3	Cu	1.9											O	z	5.78		1995																												Bi0212	I4/mmm		A	3.867		20.01												K				75			75																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150547	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.2Pb0.3La1.3Sr1.2Cu2O5.78	Bi	0.2	Pb	0.3	La	1.3	Sr	1.2	Cu	2											O	z	5.78		1995																												Bi0212	I4/mmm		A	3.863		19.96												K				50			50																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150548	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.1Pb0.4La1.2Sr1.3Cu2O5.78	Bi	0.1	Pb	0.4	La	1.2	Sr	1.3	Cu	2											O	z	5.78		1995																												Bi0212	I4/mmm		A	3.852		19.93												K				44			44																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150549	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.1Pb0.4La1.3Sr1.2Cu2O5.83	Bi	0.1	Pb	0.4	La	1.3	Sr	1.2	Cu	2											O	z	5.83		1995																												Bi0212	I4/mmm		A	3.856		19.94												K				25			25																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150550	PHC2510238	volume fraction of SC < 5%.	(Bi,Pb,La,Sr)2SrCu2Oz	Bi0.1Pb0.4La1.4Sr1.1Cu2O5.84	Bi	0.1	Pb	0.4	La	1.4	Sr	1.1	Cu	2											O	z	5.84		1995																												Bi0212	I4/mmm		A	3.855		19.83												K				25			25																																																																																																					Neutron powder diffraction and magnetic properties of Bi-0212	199509		"Institute fu""r Anorganische Chemie der Universia""t, Auf der Morgrnstelle 18,72076 Tu""bingen, Germany"	Physica C,251(1995)238-246	A. Ehmann (a),B. Seling (a),C. Schinzer (a),G. Filoti (b),J. Linhart (d),M. Rosenberg (c),S. Kemmler-Sack (a),W. Reimers (d)	Bi, Sr, Ca, Cu, O	
150551	PHC4680169	Tc,Hc2 plotted for lattice constant, nat Nb- and Ta-concentrations. values in DB show for a = 4.465 A.	(Ta,Nb)C	Ta0.5Nb0.5C1	Ta	0.5	Nb	0.5	C	1																		1	2008																												NaCl			A	4.4637														K		11.1					11.1	MTC150551																			T														MHC150551																																																												C,Nb-Ta		using pulsed arc discharge method under partial pressure P(He) = 100 - 300 Torr.					A sharp change of Tc in polycrystalline NbxTa1-xCy and nanocrystals encapsulated in multiwall carbon nanocages			Department of Life and Environmental Science, College of Science and Engineering, Iwaki Meisei University, Iwaki, Fukushima 970-8551, Japan	Physica C, 468(2008)169	Yositaka Yosida		
150552	PHC4680244	Hc2(0) = 6.21 T using linear approx. G-L parameter = 15.5 . thermodynamic Hc(0) = 2094 Oe.	Li2Pd3B	Li2Pd3B1B1	Li	2	Pd	3	B	1	B	1																1	2008																													P4<2>32		A	6.751														K		8.19		8.08			8.19											Oe	M-H curve	230							T	M-H curve	4.64														A		85.3			A	from Hc1, G-L parameter	1330																																																					two-step arc-melting					Ni substitution effect on structure and superconductivity properties in Li2(Pd1-xNix)3B boride system			Graduate School of Science and Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 468(2008)244	Lingwei Li,Katsuhiko Nishimura,Jyungo Ishiyama,Katsunori Mori		
150553	PHC4680244	Hc2(0) = 4.91 T using linear approx. G-L parameter = 19.3 . thermodynamic Hc(0) = 1400 Oe.	Li2(Pd,Ni)3B	Li2Pd2.85Ni0.15B1	Li	2	Pd	2.85	Ni	0.15	B	1																1	2008																													P4<2>32		A	6.7497														K		7.58		7.38			7.58											Oe	M-H curve	135							T	M-H curve	3.91														A		92.2			A	from Hc1, G-L parameter	1790																																																					two-step arc-melting					Ni substitution effect on structure and superconductivity properties in Li2(Pd1-xNix)3B boride system			Graduate School of Science and Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 468(2008)244	Lingwei Li,Katsuhiko Nishimura,Jyungo Ishiyama,Katsunori Mori		
150554	PHC4680244	Hc2(0) = 3.91 T using linear approx. G-L parameter = 18.7 . thermodynamic Hc(0) = 1089 Oe.	Li2(Pd,Ni)3B	Li2Pd2.7Ni0.3B1	Li	2	Pd	2.7	Ni	0.3	B	1																1	2008																													P4<2>32		A	6.7419														K		7		6.79			7											Oe	M-H curve	110							T	M-H curve	2.82														A		108			A	from Hc1, G-L parameter	2020																																																					two-step arc-melting					Ni substitution effect on structure and superconductivity properties in Li2(Pd1-xNix)3B boride system			Graduate School of Science and Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 468(2008)244	Lingwei Li,Katsuhiko Nishimura,Jyungo Ishiyama,Katsunori Mori		
150555	PHC4680244	Hc2(0) = 3.52 T using linear approx. G-L parameter = 19.4 . thermodynamic Hc(0) = 853 Oe.	Li2(Pd,Ni)3B	Li2Pd2.55Ni0.45B1	Li	2	Pd	2.55	Ni	0.45	B	1																1	2008																													P4<2>32		A	6.7311														K		6.58		6.4			6.58											Oe	M-H curve	91							T	M-H curve	2.33														A		121			A	from Hc1, G-L parameter	2350																																																					two-step arc-melting					Ni substitution effect on structure and superconductivity properties in Li2(Pd1-xNix)3B boride system			Graduate School of Science and Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 468(2008)244	Lingwei Li,Katsuhiko Nishimura,Jyungo Ishiyama,Katsunori Mori		
150556	PHC4680244	Hc2(0) = 3.24 T using linear approx. G-L parameter = 23.2 . thermodynamic Hc(0) = 673 Oe.	Li2(Pd,Ni)3B	Li2Pd2.4Ni0.6B1	Li	2	Pd	2.4	Ni	0.6	B	1																1	2008																													P4<2>32		A	6.7263														K		6.5		6.4			6.5											Oe	M-H curve	70							T	M-H curve	2.21														A		123			A	from Hc1, G-L parameter	2850																																																					two-step arc-melting					Ni substitution effect on structure and superconductivity properties in Li2(Pd1-xNix)3B boride system			Graduate School of Science and Engineering, University of Toyama, Toyama 930-8555, Japan	Physica C, 468(2008)244	Lingwei Li,Katsuhiko Nishimura,Jyungo Ishiyama,Katsunori Mori		
150557	ARX080329	compositions: 29.2Mo-70.8Sb by EDX. lattice term in SP = 0.85 mJ/mol.K4. e-ph = 0.6. G-L = 54.6. thermodynamic Hc(0) = 0.029 T from SP. two gap analysis, lower one: GAPENE(L) = 2.5.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																					2008																															A	9.551														K		2.2					2.2																				T	SP and parabolicapprox.	2.24							T/K	SP	1.25			MHC150557		A		120			A		4200					4	14				MSP150557			mJ/mol.K2	34.5	SP	283												uOhm.cm							95																Mo,Sb		mixture - ANN(700C,3d, in evacuated silica) - press - ANN(600C,2d)					Low-temperature specific heat of the superconductor Mo3Sb7			W. Trzebiatowski Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc law, Poland	Acta Materialia, 56(2008)5694	V. H. Tran,W. Miiller,Z. Bukowski		
150558	L100157001	sharp decrease of C at T=Tc/5, shows two gaps. lattice term of SP = 0.276 mJ/mol.K4. (dC/gamma*Tc) = 1.05. lower gap(2d) = 1.1 kTc.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2008																												Sc2Fe3Si5																		K		6.2					6.2																																		MHC150558																			MSP150558	mJ/mol.K	150	mJ/mol.K2	23.7	SP fitting for T2>40																																	MRH150558					floating zone method - ANN(800C,4w) - ANN(1250C,5d)					Specific-Heat Evidence for Two-Gap Superconductivity in the Ternary-Iron Silicide Lu2Fe3Si5			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.Lett., 100(2008)157001	Y. Nakajima,T. Nakagawa,T. Tamegai,H. Harima		
150559	PHB1941975	Hc2 defined as T2. two transitions : 2.8 K(incommensurate AFM) and 2.4 K(commensurate)	Er2Fe3Si5	Er2Fe3Si5	Er	2	Fe	3	Si	5																		1	1994																												Sc2Fe3Si5	P4/mnc		A	10.39		5.429												K	0.47	0.93	1.3			0.67	0.93																				T	resistive, WHH	0.13							T/K	resistive	0.19			MHC150559		A		500																																	uOhm.cm											254														arc-melting - wrapped in Ta-foil - ANN(1000C,4d + 900C,2d + 800C,2d, in evacuated quartz tube)					A new magnetic superconductor Er2Fe3Si5			University of Osaka Prefecture, Sakai, Osaka, Japan	Physica B, 194-196(1994)1975	S.Noguchi,K.Okuda		
150560	P077140506	RRR = 27 Curie-T from SUS( Curie-Weis law)	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		1	2008							2.81																					TiNiSi			A	6.864	4.196	7.261												K		0.766		0.604			0.766																																																																							uOhm.cm							26																U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150561	P077140506	Curie-T from SUS( Curie-Weis law)	UCo(Ge,Si)	U1Co1Ge0.98Si0.02	U	1	Co	1	Ge	0.98	Si	0.02																1	2008							2.34																					TiNiSi																		K		0.667		0.541			0.667																																																																																														U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150562	P077140506	Curie-T from SUS( Curie-Weis law)	UCo(Ge,Si)	U1Co1Ge0.96Si0.04	U	1	Co	1	Ge	0.96	Si	0.04																1	2008							1.8																					TiNiSi																		K		0.541		0.459			0.541																																																																																														U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150563	P077140506	Curie-T from SUS( Curie-Weis law)	UCo(Ge,Si)	U1Co1Ge0.94Si0.06	U	1	Co	1	Ge	0.94	Si	0.06																1	2008							1.27																					TiNiSi																		K		0.423		0.333			0.423																																																																																														U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150564	P077140506	Curie-T from SUS( Curie-Weis law)	UCo(Ge,Si)	U1Co1Ge0.92Si0.08	U	1	Co	1	Ge	0.92	Si	0.08																1	2008							0.775																					TiNiSi																		K		0.288					0.288																																																																																														U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150565	P077140506	Curie-T from SUS( Curie-Weis law)	UCo(Ge,Si)	U1Co1Ge0.9Si0.1	U	1	Co	1	Ge	0.9	Si	0.1																1	2008							0.37																					TiNiSi																		K		0.153					0.153																																																																																														U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150566	P077140506	not SC	UCoSi	U1Co1Si1	U	1	Co	1	Si	1																		1	2008																												TiNiSi			A	6.876	4.108	7.154												K					0.23																																																																																																U,Co,Ge,Si		nominal(U1.02Co1.02Ge1-xSix) - arcmelting - ANN(875C,10d)					Simultaneous suppression of ferromagnetism and superconductivity in UCoGe by Si substitution			Van der Waals?Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.B, 77(2008)140506	D. E. de Nijs,N. T. Huy,A. de Visser		
150567	P077165129		(Nd,Ce)CoIn5	Nd0.4Ce0.6Co1In5	Nd	0.4	Ce	0.6	Co	1	In	5																3	2008					myu-B	2.83		1.98																				HoCoGa5			A	4.605														K																																																																																																							excess In-flux method					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
150568	P077165129		(Nd,Ce)CoIn5	Nd0.4Ce0.83Co1In5	Nd	0.4	Ce	0.83	Co	1	In	5																3	2008					myu-B	2.73																						HoCoGa5																		K		0.74					0.74																																																																																																excess In-flux method					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
150569	P077165129		(Nd,Ce)CoIn5	Nd0.4Ce0.85Co1In5	Nd	0.4	Ce	0.85	Co	1	In	5																3	2008					myu-B	2.67																						HoCoGa5																		K		1.42					1.42																																																																																																excess In-flux method					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
150570	P077165129		(Nd,Ce)CoIn5	Nd0.4Ce0.6Co1In5	Nd	0.4	Ce	0.6	Co	1	In	5																3	2008																												HoCoGa5			A	4.61														K		1.74					1.74																																																																																																excess In-flux method					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
150571	P077165129		CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2008					myu-B	2.59																						HoCoGa5			A	4.613														K		2.25					2.25	MTC150568																																																																																															excess In-flux method					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
150572	J077043701	P-induced SC. SC properties at P = 10.8 GPa. another magnetic transition at 2.9 K. Moment & Curie-T for H//[001] from Curie-Weis law(T<200K).	CePd5Al2	Ce1Pd5Al2	Ce	1	Pd	5	Al	2																		3	2008					myu-B/Ce	2.41	54	4.1																				ZrNi2Al5			A	4.156		14.883												K		0.57			0		0.57	MPH150572																			T		0.25							T/K		1.04			MHC150572																						mJ/mol.K2	56																																							Bridgeman method. arc-melting - heat(1130C,2h,in evacuated quartz tube) - cool to RT(2days)					Pressure-Induced Superconductivity in Antiferromagnet CePd5Al2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)043701	F.Honda,Marie-Aude MEASSON,Yasunori NAKANO,Naohisa YOSHITANI,Etsuji YAMAMOTO,Yoshinori HAGA,Tetsuya TAKEUCHI,Hiroshi YAMAGAMI,Katsuya SHIMIZU,Rikio SETTAI,Yoshichika Onuki		
150573	J077043701	ANN(800C).  not SC.	LuPd5Al2	Lu1Pd5Al2	Lu	1	Pd	5	Al	2																		3	2008																												ZrNi2Al5			A	4.0894		14.615												K					0.1																																																										mJ/mol.K2	8		310																																					Bridgeman method. arc-melting - heat(1130C,2h,in evacuated quartz tube) - cool to RT(2days)					Pressure-Induced Superconductivity in Antiferromagnet CePd5Al2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)043701	F.Honda,Marie-Aude MEASSON,Yasunori NAKANO,Naohisa YOSHITANI,Etsuji YAMAMOTO,Yoshinori HAGA,Tetsuya TAKEUCHI,Hiroshi YAMAGAMI,Katsuya SHIMIZU,Rikio SETTAI,Yoshichika Onuki		
150574	J077043704	impurity = OsO2. a=0.00756 /GPa, b = 0.000198 /(GPa)^2 in (dV/V0) = -a*P + b*P^2.	CsOs2O6	Cs1Os2O6	Cs	1	Os	2																	O	6		1	2008																												pyrochlore																		K				3.3			3.3	TC150574																																																																																															solid state reaction					Superconducting Transition in the beta-Pyrochlore AOs2O6 (A = Cs, Rb, K) under Pressure			Department of Material Science, Shimane University, Matsue 690-8504	J.Phys.Soc.Jpn, 77(2008)043704	Kiyotaka MIYOSHI,Yuta TAKAICHI,Yusuke TAKAMATSU,Motonobu MIURA,Jun TAKEUCHI		
150575	J077043704	impurity = OsO2. a=0.00777 /GPa, b = 0  /(GPa)^2 in (dV/V0) = -a*P + b*P^2.	RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		1	2008																												pyrochlore																		K				6.3			6.3	TC150575																																																																																															solid state reaction					Superconducting Transition in the beta-Pyrochlore AOs2O6 (A = Cs, Rb, K) under Pressure			Department of Material Science, Shimane University, Matsue 690-8504	J.Phys.Soc.Jpn, 77(2008)043704	Kiyotaka MIYOSHI,Yuta TAKAICHI,Yusuke TAKAMATSU,Motonobu MIURA,Jun TAKEUCHI		
150576	J077043704	impurity = OsO2. a=0.00726 /GPa, b = 0  /(GPa)^2 in (dV/V0) = -a*P + b*P^2.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		1	2008																												pyrochlore																		K				9.6			9.6	TC150576																																																																																															solid state reaction					Superconducting Transition in the beta-Pyrochlore AOs2O6 (A = Cs, Rb, K) under Pressure			Department of Material Science, Shimane University, Matsue 690-8504	J.Phys.Soc.Jpn, 77(2008)043704	Kiyotaka MIYOSHI,Yuta TAKAICHI,Yusuke TAKAMATSU,Motonobu MIURA,Jun TAKEUCHI		
150577	J076014702	Tc(R)=0.75 K. from resistive transition. large difference between Tc(R) and Tc(SP). Hc2 determined by SP. lattice term (beta) = 165 mJ/mol.K4. below Tc(SP), Cs/T = 34.1(mJ/mol.K2) + 1290(mJ/mol.K3)*T	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																		3	2007																												CePt3B																		K		0.46					0.46																				T	SP heat	2.3							T/K	SP heat	7.2			MHC150577																			MSP150577			mJ/mol.K2	335	SP																																						Bridgeman method.					Specific Heat and de Haas-van Alphen Experiments on the Heavy-Fermion Superconductor CePt3Si			Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)014702	Tetsuya TAKEUCHI,Takashi YASUDA,Masahiko TSUJINO,Hiroaki SHISHIDO,Rikio SETTAI,Hisatomo HARIMA,Y.Onuki		
150578	J076014702	Tc defined from SP.	LaPt3Si	La1Pt3Si1	La	1	Pt	3	Si	1																		3	2007																												CePt3B																		K		0.6					0.6																																																2.7	14				MSP150578			mJ/mol.K2	11	SP	170	SP																																				Bridgeman method.					Specific Heat and de Haas-van Alphen Experiments on the Heavy-Fermion Superconductor CePt3Si			Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 76(2007)014702	Tetsuya TAKEUCHI,Takashi YASUDA,Masahiko TSUJINO,Hiroaki SHISHIDO,Rikio SETTAI,Hisatomo HARIMA,Y.Onuki		
150579	JAC25600L1	ANN(1000C, 1w)	ZrRuGe	Zr1Ru1Ge1	Zr	1	Ru	1	Ge	1																		1	1997																											3	TiFeSi			A	7.479	11.669	6.777												K	7		11				9																				T	resistive, midpoint	0.5																																																																										high-P, high-T synthesis(stoichiometric powder mixture, 1400C, 4 GPa)					Superconductivity of ZrRuGe with TiFeSi-type structure			Muroran I.stitute of Technology. 27-I. Mizumoto. Muroran-shi 050. Japan	J.Alloys Compd., 256(1997)L1	Ichimim Shirotani,Masahisa Hori,Kenji Tachi,Sakae Todo,Takehiko Yagi		
150580	JAC4440114	using 94% enriched Pu<239>. KAIZERO: DB-value for H//[100], =4.5 E-4 emu/mol for H//[001].	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2007	emu/mol	0.00043			myu-B/Pu	0.85																						HoCoGa5																		K				8.6			8.6																													T/K	SUS		3.5	2	MHC150580																																																														Ga- and In-flux method, heat(1100C,2h)					Single crystal growth, superconductivity and Fermi surface study of plutonium compounds			Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Alloys Compd., 444(2007)114	Y. Haga,D. Aoki,H. Yamagami,T.D. Matsuda,K. Nakajima,Y. Arai,E. Yamamoto,A. Nakamura,Y. Homma,Y. Shiokawa,Y. Onuki		
150581	JAC4520241	lattice term of C = 6.2 E-4 J/mol.K4	LaRhSn	La1Rh1Sn1	La	1	Rh	1	Sn	1																		3	2008																												ZrNiAl	P6[-]2m		A	7.479		4.217												K	1.85						1.85																				T	extraporation to 0 K.		0.84	0.52	0.1		0.5							MHC150581																			MSP150581			mJ/mol.K2	10.9	SP, relaxation method	211	SP																																				modified Czochralski method in a tri-arc furnace.					Superconductivity and physical properties of a LaRhSn single crystal			Charles University, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Prague 2, Czech Republic	J.Alloys Compd., 452(2008)241	Matus Mihalik,Vladimir Sechovsky,Martin Divis,Slavomir Gabani,Marian Mihalik		
150582	JAC2320071		LaRhSn	La1Rh1Sn1	La	1	Rh	1	Sn	1																			1996																												ZrNiAl			A	7.478		4.223												K	1.7			1.9			1.9																																																																							uOhm.cm							16																		arc-melting					Equiatomic ternary lanthanum-transition metal-tin phases: structural and electrical results			Istituto di Chimica Fisica, Universitri di Genova, Corso Europa 26, 16132 Genova, Italy	J.Alloys Compd., 232(1996)71	F. Canepa,S. Cirafici		
150583	PHI0842119	some weak magnetic transition at 6.2 K.	CeRhSn	Ce1Rh1Sn1	Ce	1	Rh	1	Sn	1																		1	2004																												ZrNiAl																	or Fe2P	K					0.1																																																							MSP150583																		uOhm.cm							27.4																		arc-melting, ANN(800C,8d)					Non-Fermi-liquid behaviour in CeRhSn			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093-0360, USA	Philos.Mag., 84(2004)2119	P.-C. Ho,V. S. Zapf,A. Slebarski,M. B. Maple		
150584	SSC0500061		LaPtSi	La1Pt1Si1	La	1	Pt	1	Si	1																		1	1984																												LaPtSi			A	4.245		14.54												K		3.3					3.3																																																																																																melt by induction method					SUPRACONDUCTIVITY OF LaPtSi AND LaPtGe			Institut fur Anorganische Chemie der Universitat Mtinchen, Meiserstr. 1, D-8000 Miinchen 2, Federal Republic of Germany	Solid State Commun., 50(1984)61	J. Evers,G. Oehlinger,A. Weiss,C. Probst		
150585	SSC0500061		LaPtGe	La1Pt1Ge1	La	1	Pt	1	Ge	1																		1	1984																												LaPtSi			A	4.266		14.96												K		3.4					3.4																																																																																																melt by induction method					SUPRACONDUCTIVITY OF LaPtSi AND LaPtGe			Institut fur Anorganische Chemie der Universitat Mtinchen, Meiserstr. 1, D-8000 Miinchen 2, Federal Republic of Germany	Solid State Commun., 50(1984)61	J. Evers,G. Oehlinger,A. Weiss,C. Probst		
150586	PHI0842119		LaRhSn	La1Rh1Sn1	La	1	Rh	1	Sn	1																		1	2004																												ZrNiAl																		K		2					2																				T	extraporation to 0 K., resistive	0.7												MHC150586																																					uOhm.cm							11																		arc-melting, ANN(800C,8d)					Non-Fermi-liquid behaviour in CeRhSn			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093-0360, USA	Philos.Mag., 84(2004)2119	P.-C. Ho,V. S. Zapf,A. Slebarski,M. B. Maple		
150587	L100197003	P-induced SC. impurity phase < 5vol%. Pressure by DAC. Tc  by as(13Hz) resistivity. RRR=170	CaLi2	Ca1Li2	Ca	1	Li	2																				1	2008																												MgZn2(Laves)			A	6.293		10.236											MgZn2(Laves),C14	K		13			1.1		13	MTC150587																																																																																													Ca(3N),Li(4N)		melting (stoichiometric amount of Ca,Li in stainless crucible), then stirring them at 235 C for 30 min.					Pressure-Induced Superconductivity in CaLi2			Department of Physics, Washington University, CB 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.Lett., 100(2008)197003	T. Matsuoka,M. Debessai,J. J. Hamlin,A. K. Gangopadhyay,J. S. Schilling,K. Shimizu		
150588	MRB0430779		RbxWO3	Rb0.14W1O3	Rb	0.14	W	1																	O	3		1	2008																												bronze	P6<3>/mcm																	K	4.9		5.3				5.1																																																																																														Rb2CO3,WO3		mixture - CAL(750C,24h) - pellet - microwave heating(400W,10min), hybrid microwave method					Crystal structure and superconductivity of rubidium tungsten bronzes RbxWO3 prepared by a hybrid microwave method			School of Physics and Engineering, Zhengzhou University, Zhengzhou, Henan 450052, China	Mater.Res.Bull., 43(2008)779	Juan Guo,Cheng Dong,Lihong Yang,Hong Chen		
150589	MRB0430779		RbxWO3	Rb0.16W1O3	Rb	0.16	W	1																	O	3		1	2008																												bronze	P6<3>/mcm																	K	4.9		5.3				5.1																																																																																														Rb2CO3,WO3		mixture - CAL(750C,24h) - pellet - microwave heating(400W,10min), hybrid microwave method					Crystal structure and superconductivity of rubidium tungsten bronzes RbxWO3 prepared by a hybrid microwave method			School of Physics and Engineering, Zhengzhou University, Zhengzhou, Henan 450052, China	Mater.Res.Bull., 43(2008)779	Juan Guo,Cheng Dong,Lihong Yang,Hong Chen		
150590	MRB0430779		RbxWO3	Rb0.2W1O3	Rb	0.2	W	1																	O	3		1	2008																												bronze	P6<3>/mcm																	K	4.5		4.9				4.7																																																																																														Rb2CO3,WO3		mixture - CAL(750C,24h) - pellet - microwave heating(400W,10min), hybrid microwave method					Crystal structure and superconductivity of rubidium tungsten bronzes RbxWO3 prepared by a hybrid microwave method			School of Physics and Engineering, Zhengzhou University, Zhengzhou, Henan 450052, China	Mater.Res.Bull., 43(2008)779	Juan Guo,Cheng Dong,Lihong Yang,Hong Chen		
150591	P077174501	RRR = 1.69	MgB2	B2Mg1	B	2	Mg	1																					2008																												AlB2			A	3.0837		3.5287												K		37					37																																																				MJC150591																			uOhm.cm							49				83												Mg,a-B,C6H8O7		mixture(Mg,B,C6H8O7) -sealed in iron tube - SIN(850C,0.5h,in Ar) - FC to RT					Effects of C substitution on the pinning mechanism of MgB2			Institute for Superconducting and Electronic Materials, University of Wollongong, Northfields Avenue, Wollongong, New South Wales 2522, Australia	Phys.Rev.B, 77(2008)174501	J. L. Wang,R. Zeng,J. H. Kim,L. Lu,S. X. Dou		
150592	P077174501	RRR = 1.71	Mg(B,C)2	Mg1B1.924C0.076	Mg	1	B	1.924	C	0.076																			2008																												AlB2			A	3.0758		3.5233												K		35.8					35.8																																																																							uOhm.cm							156				267												Mg,a-B,C6H8O7		mixture(Mg,B,C6H8O7) -sealed in iron tube - SIN(850C,0.5h,in Ar) - FC to RT					Effects of C substitution on the pinning mechanism of MgB2			Institute for Superconducting and Electronic Materials, University of Wollongong, Northfields Avenue, Wollongong, New South Wales 2522, Australia	Phys.Rev.B, 77(2008)174501	J. L. Wang,R. Zeng,J. H. Kim,L. Lu,S. X. Dou		
150593	P077174501	SIN(950C,0.5h).  RRR = 1.62	Mg(B,C)2	Mg1B1.904C0.096	Mg	1	B	1.904	C	0.096																			2008																												AlB2			A	3.0724		3.5239												K		35.5					35.5																																																																							uOhm.cm							142				230												Mg,a-B,C6H8O7		mixture(Mg,B,C6H8O7) -sealed in iron tube - SIN(850C,0.5h,in Ar) - FC to RT					Effects of C substitution on the pinning mechanism of MgB2			Institute for Superconducting and Electronic Materials, University of Wollongong, Northfields Avenue, Wollongong, New South Wales 2522, Australia	Phys.Rev.B, 77(2008)174501	J. L. Wang,R. Zeng,J. H. Kim,L. Lu,S. X. Dou		
150594	P077174503	impurity phase = La4.67(SiO4)3O.	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89	0.89	1	2008																											2	oxypnictide	P4/nmm	129	A	4.0277		8.7125											ZrCuSiAs-type	K			28.2	27.5		4.5	27.5																				T	resistive, WHH	25							T/K	resistive, midpoint	1.41			HC150594		A		36																			4.1	SP	325	SP					THC150594	uV/K	-42			TP150594	mOhm.cm											2.7									RH150594	/cm3	1700000000000000000000	LaAs,Fe2As,La2O3,LaF3,As		mixture - pellet - heat(1250C,15h,in silica tube) - FC to RT - ANN(1250C)					Electronic correlations in the superconductor LaFeAsO0.89F0.11 with low carrier density			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 77(2008)174503	Athena S. Sefat,Michael A. McGuire,Brian C. Sales,Rongying Jin,Jane Y. Howe,David Mandrus		
150595	ACS1303296	undoped-F. not SC. R(drop) at 150 K. R(min) at 100K.	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2008																											2	oxypnictide	P4/nmm		A	4.0355		8.7393											ZrCuSiAs-type	K					1.8																																																																																																LaAs,Fe2As,La2O3		mixture - put in silica tube(Ar) - heat(1250C,40h) - ADD(LaF3,La)					Iron-Based Layered Superconductor La[O1-xFx]FeAs  (x = 0.05 - 0.12) with Tc = 26 K			Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 130(2008)3296	Yoichi Kamihara,Takumi Watanabe,Masahiro Hirano,Hideo Hosono		
150596	ACS1303296	5 at% F-doped. R(min) at 60 K.	La(O,F)FeAs	La1F0.05Fe1As1O0.95	La	1	F	0.05	Fe	1	As	1													O	0.95			2008																											2	oxypnictide	P4/nmm		A	4.032		8.7263											ZrCuSiAs-type	K		26					26	TC150596																																																																																													LaAs,Fe2As,La2O3		mixture - put in silica tube(Ar) - heat(1250C,40h) - ADD(LaF3,La)					Iron-Based Layered Superconductor La[O1-xFx]FeAs  (x = 0.05 - 0.12) with Tc = 26 K			Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 130(2008)3296	Yoichi Kamihara,Takumi Watanabe,Masahiro Hirano,Hideo Hosono		
150597	IOC0467719	impurity phase = LaNi2P2(8 vol%), La3PO7(1 vol%)	LaONiP	La1Ni1P1O1	La	1	Ni	1	P	1															O	1			2007																												oxypnictide																	ZrCuSiAs-type	K	2.1	3	3.8				3										40	Oe					20			1.8	Oe					800			1.8																																																																									Nickel-Based Oxyphosphide Superconductor with a Layered Crystal Structure, LaNiOP			Frontier CollaboratiVe Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama, Japan	Inorg.Chem., 46(2007)7719	Takumi Watanabe,Hiroshi Yanagi,Toshio Kamiya,Yoichi Kamihara,Hidenori Hiramatsu,Masahiro Hirano,Hideo Hosono		
150598	SST0200687		LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1			2007																											2	oxypnictide			A	3.962		8.511											ZrCuSiAs-type	K	4.1			4.1			4.1																																																																							mOhm.cm											0.342														(La-Fe alloy + red P) - heat(650-800C,12h,in quartz tube), then (La-Fe-P alloy + La2O3) - heat(1240C,48h,in quartz tube)					Synthesis and structural characterization of LaOFeP superconductors			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, People's Republic of China	Supercond.Sci.Technol., 20(2007)687	C Y Liang,R C Che,H X Yang,H F Tian,R J Xiao,J B Lu,R Li,J Q Li		
150599	NAT4470187	Tc measured by pick-up coil. Tc extraporated to zero field from Tc values in the static field produced by pick-up coil. Tc=0.2-0.4 mK. magnetic transition at 80 K.	Li	Li1	Li	1																							2007																																														K				0.0004			0.0004																																																																																																nominal Li(92 %Li<7>. magnetic contamination of 4 ppm.					Superconductivity in lithium below 0.4 millikelvin at ambient pressure			Low Temperature Laboratory, Helsinki University of Technology, PO Box 2200 FI-02015 TKK, Finland. {Present address: Philips Medical Systems,Ayritie 4, FI-01510 Vantaa, Finland.	Nature, 447(2007)187	Juha Tuoriniemi,Kirsi Juntunen-Nurmilaukas,Johanna Uusvuori,Elias Pentti,Anssi Salmela,Alexander Sebedash		
150600	P077180504	RRR=100. Tc=4.62 K from SP measurement. G-L = 14.	ThPt4Ge12	Th1Pt4Ge12	Th	1	Pt	4	Ge	12																		1	2008																												skutterudite	Im3{-}		A	8.5924														K		4.8		4.4			4.8											mT	deviation from linear M				3			1.72	T	WHH approx.	0.29			0.2			1.72	T/K		0.085					A	from Hc2	350			A	from Hc1,G-L,	1500													mJ/mol.K2	40	SP	217	SP											nOhm.cm							6.5					750													arc-melting - wrapped in Ta foil - ANN(800C,3w,in evacuated quartz tube)					Superconductivity in the actinoid-bearing filled skutterudite ThPt4Ge12			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.B, 77(2008)180504	D. Kaczorowski,V. H. Tran		
150601	P077184512	Muon-SR. G-L. = 17.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2			2008																												IL																		K		43					43																				T	WHH approx.			10.7																	A	u-SR	930																																																					See Physica C, 366(2002)299.					Nodeless superconductivity in the infinite-layer electron-doped cuprate superconductor Sr0.9La0.1CuO2			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 77(2008)184512	R. Khasanov,A. Shengelaya,A. Maisuradze,D. Di Castro,I. M. Savic,S. Weyeneth,M. S. Park,D. J. Jang,S.-I. Lee,H. Keller		
150602	P077193106	purple bronze. ANN(200C,10h) leads to non-SC. a = 0.43, b = -1.6 in R = A*T^a + B*T^b	Li0.9Mo6O17	Li0.9Mo6O17	Li	0.9	Mo	6																	O	17		3	2008																												bronze																		K	1.2		1.92				1.56																																																																																																See Phys.Rev.Lett., 98(2007)266405					Electrical transport in single-crystalline Li0.9Mo6O17: A two-band Luttinger liquid exhibiting Bose metal behavior			Department of Physics, Montana State University, P.O. Box 173840, Bozeman, Montana 59717-3840, USA	Phys.Rev.B, 77(2008)193106	C. A. M. dos Santos,M. S. da Luz,Yi-Kuo Yu,J. J. Neumeier,J. Moreno,B. D. White		
150603	P077193106	purple bronze. insulator(not SC). M-I transition at 28 K.	Li0.9Mo6O17	Li0.9Mo6O17	Li	0.9	Mo	6																	O	17		3	2008																												bronze																		K					0.4																																																																																																		See Phys.Rev.Lett., 98(2007)266405					Electrical transport in single-crystalline Li0.9Mo6O17: A two-band Luttinger liquid exhibiting Bose metal behavior			Department of Physics, Montana State University, P.O. Box 173840, Bozeman, Montana 59717-3840, USA	Phys.Rev.B, 77(2008)193106	C. A. M. dos Santos,M. S. da Luz,Yi-Kuo Yu,J. J. Neumeier,J. Moreno,B. D. White		
150604	PCS0682178		MgCyNi3	Mg1C0.98Ni3	Mg	1	C	0.98	Ni	3																			2007																												CaTiO3																		K		6.5					6.5																																																																																														Mg,Zn,C,Ni-powder		nominal=(Mg1-xZnx)1.5CyNi3. reaction temperature = 900C for y => 0.95 and = 800-900C for y < 0.95.					Magnetism on Mg1-xZnxCyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Japan	J.Phys.Chem.Solids, 68(2007)2178	M. Uehara,T. Yamazaki,T. Kori,T. Kashida,Y. Kimishima,K. Ohishi		
150605	PCS0682178		MgCyNi3	Mg1C0.69Ni3	Mg	1	C	0.69	Ni	3																			2007																												CaTiO3																		K		1.8					1.8																																																																																														Mg,Zn,C,Ni-powder		nominal=(Mg1-xZnx)1.5CyNi3. reaction temperature = 900C for y => 0.95 and = 800-900C for y < 0.95.					Magnetism on Mg1-xZnxCyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Japan	J.Phys.Chem.Solids, 68(2007)2178	M. Uehara,T. Yamazaki,T. Kori,T. Kashida,Y. Kimishima,K. Ohishi		
150606	PCS0682178	sample contains impurity phases.	(Mg,Zn)CyNi3	Mg0.9Zn0.1C0.98Ni3	Mg	0.9	Zn	0.1	C	0.98	Ni	3																	2007																												CaTiO3																		K		4.5					4.5	MPH150606																																																																																													Mg,Zn,C,Ni-powder		nominal=(Mg1-xZnx)1.5CyNi3. reaction temperature = 900C for y => 0.95 and = 800-900C for y < 0.95.					Magnetism on Mg1-xZnxCyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Japan	J.Phys.Chem.Solids, 68(2007)2178	M. Uehara,T. Yamazaki,T. Kori,T. Kashida,Y. Kimishima,K. Ohishi		
150607	PCS0682178	sample contains impurity phases.	(Mg,Zn)CyNi3	Mg0.8Zn0.2C1.05Ni3	Mg	0.8	Zn	0.2	C	1.05	Ni	3																	2007																												CaTiO3																		K		4					4																																																																																														Mg,Zn,C,Ni-powder		nominal=(Mg1-xZnx)1.5CyNi3. reaction temperature = 900C for y => 0.95 and = 800-900C for y < 0.95.					Magnetism on Mg1-xZnxCyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Japan	J.Phys.Chem.Solids, 68(2007)2178	M. Uehara,T. Yamazaki,T. Kori,T. Kashida,Y. Kimishima,K. Ohishi		
150608	PCS0682178	sample contains impurity phases.	(Mg,Zn)CyNi3	Mg0.7Zn0.3C0.99Ni3	Mg	0.7	Zn	0.3	C	0.99	Ni	3																	2007																												CaTiO3																		K		2.5					2.5																																																																																														Mg,Zn,C,Ni-powder		nominal=(Mg1-xZnx)1.5CyNi3. reaction temperature = 900C for y => 0.95 and = 800-900C for y < 0.95.					Magnetism on Mg1-xZnxCyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Japan	J.Phys.Chem.Solids, 68(2007)2178	M. Uehara,T. Yamazaki,T. Kori,T. Kashida,Y. Kimishima,K. Ohishi		
150609	PHC4680405	R,XPS,FITR were measured.	(Cu,Tl)Ba2Ca2Cu3O10	Tl0.5Ba2Ca2Cu3.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3.5													O	10-z			2008																												M1223			A			14.852											(Cu,Tl)-1223	K		95.5				17.3	95.5																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO		precursor(Cu0.5Ba2Ca2-xMgxCu3O10) prepared by SIN(840C,24h).then mixed with Tl2O3					Enhanced inter-plane coupling of Mg doped Cu0.5Tl0.5Ba2Ca2-xMgxCu3O10-z superconductors: XPS and FTIR studies			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 468(2008)405	A.A. Khurram,Nawazish A. Khan,M.M. Ahadian,Azam Iraji-zad		
150610	PHC4680405	R,XPS,FITR were measured.	(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Tl0.5Ba2Ca1.5Mg0.5Cu3.5O10-z	Tl	0.5	Ba	2	Ca	1.5	Mg	0.5	Cu	3.5											O	10-z			2008																												M1223			A			14.606											(Cu,Tl)-1223	K		96.5				13.5	96.5																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO		precursor(Cu0.5Ba2Ca2-xMgxCu3O10) prepared by SIN(840C,24h).then mixed with Tl2O3					Enhanced inter-plane coupling of Mg doped Cu0.5Tl0.5Ba2Ca2-xMgxCu3O10-z superconductors: XPS and FTIR studies			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 468(2008)405	A.A. Khurram,Nawazish A. Khan,M.M. Ahadian,Azam Iraji-zad		
150611	PHC4680405	R,XPS,FITR were measured.	(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Tl0.5Ba2Ca1Mg1Cu3.5O10-z	Tl	0.5	Ba	2	Ca	1	Mg	1	Cu	3.5											O	10-z			2008																												M1223																	(Cu,Tl)-1223	K		96.5				14.5	96.5																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO		precursor(Cu0.5Ba2Ca2-xMgxCu3O10) prepared by SIN(840C,24h).then mixed with Tl2O3					Enhanced inter-plane coupling of Mg doped Cu0.5Tl0.5Ba2Ca2-xMgxCu3O10-z superconductors: XPS and FTIR studies			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 468(2008)405	A.A. Khurram,Nawazish A. Khan,M.M. Ahadian,Azam Iraji-zad		
150612	PHC4680405	R,XPS,FITR were measured.	(Cu,Tl)Ba2(Ca,Mg)2Cu3O10	Tl0.5Ba2Ca0.5Mg1.5Cu3.5O10-z	Tl	0.5	Ba	2	Ca	0.5	Mg	1.5	Cu	3.5											O	10-z			2008																												M1223			A			14.198											(Cu,Tl)-1223	K		98				15	98																																																																																														Ba(NO3)2,Ca(NO3)2,Cu(CN),MgO		precursor(Cu0.5Ba2Ca2-xMgxCu3O10) prepared by SIN(840C,24h).then mixed with Tl2O3					Enhanced inter-plane coupling of Mg doped Cu0.5Tl0.5Ba2Ca2-xMgxCu3O10-z superconductors: XPS and FTIR studies			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	Physica C, 468(2008)405	A.A. Khurram,Nawazish A. Khan,M.M. Ahadian,Azam Iraji-zad		
150613	PHC4680411	SIN(600C). not SC	NbB2	B2Nb1	B	2	Nb	1																				1	2008																												AlB2			A	3.108		3.285												K		0					0																																																																																														NbB2,a-B		solid state reaction					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150614	PHC4680411	SIN(1000C)	NbxB2	B2Nb0.83	B	2	Nb	0.83																				1	2008																												AlB2			A	3.102		3.322												K		9.77					9.77	MTC150614																																																																																													NbB2,a-B		solid state reaction					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150615	PHC4680411	SIN(1500C). not SC.	NbxBy	B1.92Nb0.86	B	1.92	Nb	0.86																				1	2008																												AlB2			A	3.082		3.303												K		0					0																																																																																														NbB2,a-B		solid state reaction					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150616	PHC4680411	ratio of Nb/B not determined. table values are tentative.	NbB2	B2Nb1	B	2	Nb	1																				1	2008																												AlB2																		K		5.53					5.53																																																								mJ/mol.K2	3.69	SP	644	SP																																				high-P-synthesis (1500C, P=3-3.5 GPa)					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150617	PHC4680411	ratio of Nb/B not determined. table values are tentative.	NbB2	B2Nb1	B	2	Nb	1																				1	2008																												AlB2																		K		6.13					6.13																																																								mJ/mol.K2	3.82	SP	642	SP																																				high-P-synthesis (1500C, P=3-3.5 GPa)					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150618	PHC4680411	ratio of Nb/B not determined. table values are tentative. (dC/gamma*Tc) = 0.71	NbB2	B2Nb1	B	2	Nb	1																				1	2008																												AlB2																		K		7.83					7.83																																																2.78	14							mJ/mol.K2	3.99	SP	737	SP																																				high-P-synthesis (1500C, P=3-3.5 GPa)					Structural phase evolution and superconductivity in the non-stoichiometric intermetallic compound niobium diboride			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 468(2008)411	Zhi-An Ren,Sogo Kuroiwa,Yoko Tomita,Jun Akimitsu		
150619	CEM0690093		LaRu2P2	La1Ru2P2	La	1	Ru	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.031		10.675												K		4.1					4.1																																																																																																					Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150620	CEM0690093		CaRu2P2	Ca1Ru2P2	Ca	1	Ru	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.048		9.773												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150621	CEM0690093		SrRu2P2	Sr1Ru2P2	Sr	1	Ru	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.032		11.122												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150622	CEM0690093		BaRu2P2	Ba1Ru2P2	Ba	1	Ru	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.031		12.062												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150623	CEM0690093		YRu2P2	Y1Ru2P2	Y	1	Ru	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.03		9.545												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150624	CEM0690093		SrOs2P2	Sr1Os2P2	Sr	1	Os	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.035		11.283												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150625	CEM0690093		BaOs2P2	Ba1Os2P2	Ba	1	Os	2	P	2																			1987																												ThCr2Si2	I4/nmm		A	4.028		12.193												K					1.8																																																																																																							Superconducting LaRu2P2 and Other Alkaline Earth and Rare Earth Metal Ruthenium and Osmium Phosphides and Arsenides with ThCr2Si2 Structure			Anorganisch-Chemisches Institut, Universitat Munster, Corrensstrasse 36, D-4400 Munster, West Germany	J.Solid State Chem., 69(1987)93	W.Jeitschko,R.Glaum,L.Boonk		
150626	LES1130231		LaIr2Ge2	La1Ir2Ge2	La	1	Ir	2	Ge	2																			1985																												CaBe2Ge2	P4/nmm		A	4.273		10.134												K		1.5					1.5																																																																																																					De nouvelles Series de Germaniures, Isotypes de U4Re7Si6, ThCr2Si2 et CaBe2Ge2, dans less Systemes Ternarires R-T-Ge ou R est un Element des Terres Rares et T = Ru,Os,Rh,Ir: Superconductivite de LaIr2Ge2				J.Less-Comm.Metals,113(1985)231	M.Francois,G.Venturini,J.F.Mareche,B.Malaman,B.Roques		
150627	SSC1470111	impurity phases: BaNi9P5(9%),Ba(PO3)2(2%), BaNi2(PO4)2 (1%)	BaNi2P2	Ba1Ni2P2	Ba	1	Ni	2	P	2																			2008																												ThCr2Si2	I4/nmm																	K	2.7		3	3			3											Oe					150			1.9	Oe					550			1.9																																											mOhm.cm											2.8												Ba,P,Ni	1	solid state reaction. mixture(powder sample) - pellet - heat(400C,12h) - SIN(1000C,12h, in evacuated silica tube)					Nickel-based phosphide superconductor with infinite-layer structure, BaNi2P2			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 147(2008)111	Takashi Mine,Hiroshi Yanagi,Toshio Kamiya,Yoichi Kamihara,Masahiro Hirano,Hideo Hosono		
150628	EP08217009		(La,Sr)OFeAs	La0.87Sr0.13Fe1As1O1	La	0.87	Sr	0.13	Fe	1	As	1													O	1			2008																												oxypnictide			A	4.035		8.771												K	15		25.6				20.3	TC150628																																																																																				E-8 m3/C	0.06					RH150628					mixture(Fe,As) - heat(700C,10h), then mix(FeAs powder + SrCO3 + La2O3 + La) - heat(940C,4h + 1150C,48h,in sealed quartz tube)					Superconductivity at 25K in hole-doped (La1-xSrx)OFeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100080, PRC	EuroPhys.Lett.,  82(2008)17009	Hai-Hu Wen,Gang Mu,Lei Fang,Huan Yang,Xiyu Zhu		
150629	EP08217009	impurity phases: FeAs,LaAs. Tc shows Tc(on).	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9			2008																												oxypnictide																		K			25.8				25.8	TC150629																																																																																															mixture(Fe,As) - heat(700C,10h), then mix(FeAs powder + SrCO3 + La2O3 + La) - heat(940C,4h + 1150C,48h,in sealed quartz tube)					Superconductivity at 25K in hole-doped (La1-xSrx)OFeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100080, PRC	EuroPhys.Lett.,  82(2008)17009	Hai-Hu Wen,Gang Mu,Lei Fang,Huan Yang,Xiyu Zhu		
150630	L100247005	interlayer spacing d = 9.37..	LixHfNCl	Li0.37Hf1N1Cl1	Li	0.37	Hf	1	N	1	Cl	1																	2008																																														K		20					20	MTC150630									93																																																																																											Interlayer-Spacing Dependence of Tc in LixMyHfNCl (M: Molecule) Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 100(2008)247005	T. Takano,T. Kishiume,Y. Taguchi,Y. Iwasa		
150631	L100247005	M=NH3. interlayer spacing d = 12.1.	LixMyHfNCl	Li0.37M0.3Hf1N1Cl1	Li	0.37	M	0.3	Hf	1	N	1	Cl	1															2008																																														K		22.5					22.5	MTC150630																																																																																																				Interlayer-Spacing Dependence of Tc in LixMyHfNCl (M: Molecule) Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 100(2008)247005	T. Takano,T. Kishiume,Y. Taguchi,Y. Iwasa		
150632	L100247005	M=THF(tetrahydrofuran). interlayer spacing d = 13.6.	LixMyHfNCl	Li0.37M0.2Hf1N1Cl1	Li	0.37	M	0.2	Hf	1	N	1	Cl	1															2008																																														K		25.6					25.6	MTC150630																																																																																																				Interlayer-Spacing Dependence of Tc in LixMyHfNCl (M: Molecule) Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 100(2008)247005	T. Takano,T. Kishiume,Y. Taguchi,Y. Iwasa		
150633	L100247005	M=PC(propylene carbonate). interlayer spacing d = 22.1	LixMyHfNCl	Li0.37M0.2Hf1N1Cl1	Li	0.37	M	0.2	Hf	1	N	1	Cl	1															2008																																														K		25					25																																																																																																					Interlayer-Spacing Dependence of Tc in LixMyHfNCl (M: Molecule) Superconductors			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 100(2008)247005	T. Takano,T. Kishiume,Y. Taguchi,Y. Iwasa		
150634	L093237005	diamond film with B in E+20 - E+21 /cm3. thickness d = 3.0 micron-m. carrier n = 9 E+20 /cm3. ratio (B/C) = 1730 ppm.	B-doped diamond	C1	C	1																							2004																												diamond																		K		0.9					0.9	MTC150635																												T/K		1			MHC150634																																																														substrate: [001]1b diamond. 0.5 buffer layer at 820C. dibrome introduced in the vertical Si wall reactor in (B/C) = 1500 - 3000 ppm					Dependence of the Superconducting Transition Temperature on the Doping Level in Single-Crystalline Diamond Films			Laboratoire d'Etudes des Proprietes Electroniques des Solides, CNRS, B.P.166, 38042 Grenoble Cedex 9, France	Phys.Rev.Lett., 93(2004)237005	E. Bustarret,J. Kacmarcik,C. Marcenat,E. Gheeraert,C. Cytermann,J. Marcus,T. Klein		
150635	L093237005	diamond film with B in E+20 - E+21 /cm3. thickness d = 0.15 micron-m. carrier n = 19 E+20 /cm3. ratio (B/C) = 2800 ppm.	B-doped diamond	C1	C	1																							2004																												diamond																		K			2.1	2			2	MTC150635																			T	RES, Tc(on)	1.4							T/K		1			MHC150634		A		150																																																										substrate: [001]1b diamond. 0.5 buffer layer at 820C. dibrome introduced in the vertical Si wall reactor in (B/C) = 1500 - 3000 ppm					Dependence of the Superconducting Transition Temperature on the Doping Level in Single-Crystalline Diamond Films			Laboratoire d'Etudes des Proprietes Electroniques des Solides, CNRS, B.P.166, 38042 Grenoble Cedex 9, France	Phys.Rev.Lett., 93(2004)237005	E. Bustarret,J. Kacmarcik,C. Marcenat,E. Gheeraert,C. Cytermann,J. Marcus,T. Klein		
150636	NAT4280542	B-doped diamond. grain size = a few micron-meter. carrier n => 2E+21 /cm3. d(lnTc)/dP = 0.0279 /GPa.	B-doped diamond	C1	C	1																							2004																												diamond																		K		2.9	4				2.9			K/GPa	-0.0642																T	resistive,WHH	3.4							T/K		1.7					A		100																																																										high-pressure synthesis(100000 ATM, 2500-2800K). (B4C + graphite) - heat(8-9 GPa, 2500-2800 K, 5s)					Superconductivity in diamond			Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190 Troitsk, Moscow region, Russia	Nature, 428(2004)542	E.A.Ekimov,E.D.Bauer,J.D.Thompson,N.J.Gurro,N.N.Mel'nik,S.M.Stishov,V.A.Sidorov		
150637	L100227001	Hc2 measured by Andreev bound states(ABS) using 24 and 30 degree GBJ(grain boundary junction). Hc2(0) = 25 T by ABS method.	(La,Ce)2CuO4	La1.92Ce0.08Cu1O4	La	1.92	Ce	0.08	Cu	1															O	4			2008																												T'																		K		29					29																				T	Andreev junction	25												HC150637																																																														900 nm films were deposited by MBE on SrTiO3 symmetric [001]-tilt bicrystal substrates.					Phase Diagram of the Electron-Doped La2-xCexCuO4 Cuprate Superconductor from Andreev Bound States at Grain Boundary Junctions			Physikalisches Institut?Experimentalphysik II and Center for Collective Quantum Phenomena, Universitat Tubingen, Auf der Morgenstelle 14, D-72076 Tubingen, Germany	Phys.Rev.Lett., 100(2008)227001	M. Wagenknecht,D. Koelle,R. Kleiner,S. Graser,N. Schopohl,B. Chesca,A. Tsukada,S. T. B. Goennenwein,R. Gross		
150638	L101017005	P-induced SC. Tc shows Tc(max). Hc2(0) and cohere(0) at P=15.2 kbar.	(Ce,La)RhIn5	Ce0.9La0.1Rh1In5	Ce	0.9	La	0.1	Rh	1	In	5																3	2008																												HoCoGa5																		K		1.6			0.3		1.6	MTC150638																			T		8												MHC150638		A		60																																																										single crystals grown by In-flux method					Tuning the Pressure-Induced Superconducting Phase in Doped CeRhIn5			Instituto de F?sica Gleb Wataghin, UNICAMP, C.P. 6165, 13083-970, Campinas, Brazil	Phys.Rev.Lett., 100(2008)017005	L. Mendonca Ferreira,T. Park,V. Sidorov,M. Nicklas,E. M. Bittar,R. Lora-Serrano,E. N. Hering,M. B. Fontes,E. Baggio-Saitovich,Hanoh Lee,J. L. Sarrao,J. D. Thompson,P. G. Pagliuso		
150639	L101017005	P-induced SC. Tc shows Tc(max). Hc2(0) and cohere(0) at P=15.2 kbar. P(crit) = 4 kbar.	CeRh(In,Sn)5	Ce1Rh1In4.84Sn0.16	Ce	1	Rh	1	In	4.84	Sn	0.16																3	2008																												HoCoGa5																		K		1.2			0.3		1.2	MTC150639																			T		7												MHC150639		A		70																																																										single crystals grown by In-flux method					Tuning the Pressure-Induced Superconducting Phase in Doped CeRhIn5			Instituto de F?sica Gleb Wataghin, UNICAMP, C.P. 6165, 13083-970, Campinas, Brazil	Phys.Rev.Lett., 100(2008)017005	L. Mendonca Ferreira,T. Park,V. Sidorov,M. Nicklas,E. M. Bittar,R. Lora-Serrano,E. N. Hering,M. B. Fontes,E. Baggio-Saitovich,Hanoh Lee,J. L. Sarrao,J. D. Thompson,P. G. Pagliuso		
150640	P077212502		NpPd5Al2	Np1Pd5Al2	Np	1	Pd	5	Al	2																		3	2008					myu-B	3.02	-42																					ZrNi2Al5	I4/mmm		A	4.141		14.6851												K		5					5											mT					10			2	T			15	4.3					T/K			5.2	3.3	MHC150640																						mJ/mol.K2	190									uV/K				MTP150640																					MRH150640					arc-melting					Transport and magnetic properties of the superconductor NpPd5Al2			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, Karlsruhe 76125, Germany	Phys.Rev., 77(2008)212502	J.-C. Griveau,K. Gofryk,J. Rebizant		
150641	P077212503		delta-MoN	Mo1N1	Mo	1	N	1																					2008																																													delta-phase	K		13.5					13.5																				T		9.6												MHC150641		A		60														MJC150641																																												MoN by reacting Mo-coated carbon fibers in 1 atm stream of ammonia gas(NH3) at 850-1000C.  (900C,90min is the best)					Critical current behavior of superconducting MoN and Mo3Sb7 microfibers			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev., 77(2008)212503	A. B. Karki,D. P. Young,P. W. Adams,E. K. Okudzeto,Julia Y. Chan		
150642	P077212503		Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																					2008																												Ir3Ge7																		K		7.5					7.5																				T		9.6												MHC150641		A		60														MJC150642																																												Mo-coated carbon fibers in evacuated quartz tube with Sb shot - heat(900C,80min) - Q to RT					Critical current behavior of superconducting MoN and Mo3Sb7 microfibers			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev., 77(2008)212503	A. B. Karki,D. P. Young,P. W. Adams,E. K. Okudzeto,Julia Y. Chan		
150643	P077214507	formula-weight = 45.44,  unit cell volume = 29.09 A^3	MgB2	B2Mg0.98	B	2	Mg	0.98																				3	2008																												AlB2			A	3.0875		3.5239												K		38.4	38.5				38.4																																																																																																High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150644	P077214507	formula-weight = 45.06,  unit cell volume = 28.968 A^3	(Mg,Li)B2	Mg0.95Li0.05B2	Mg	0.95	Li	0.05	B	2																		3	2008																												AlB2			A	3.0837		3.5176												K		38.25	38.5				38.25	LAT150644																																																																																															High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150645	P077214507	formula-weight = 44.19,  unit cell volume = 28.91 A^3	(Mg,Li)B2	Mg0.9Li0.1B2	Mg	0.9	Li	0.1	B	2																		3	2008																												AlB2																		K		35.55	35.6				35.55	MTC150645																																																																																															High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150646	P077214507		(Mg,Li)B2	Mg0.92Li0.08B2	Mg	0.92	Li	0.08	B	2																		3	2008																												AlB2																		K		38					38																				T														MHC150646																																																														High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150647	P077214507	formula-weight = 44.02,  unit cell volume = 28.89 A^3	(Mg,Li)B2	Mg0.89Li0.11B2	Mg	0.89	Li	0.11	B	2																		3	2008																												AlB2			A	3.0826		3.5109												K		35.3	35.8				35.3																				T														MHC150647																																																														High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150648	P077214507		Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		3	2008																												AlB2																		K		34.3					34.3																				T														MHC150648																																																														High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150649	P077214507	formula-weight = 44.94,  unit cell volume = 28.84 A^3	(Mg,Li)(B,C)2	Mg0.94Li0.06B1.96C0.04	Mg	0.94	Li	0.06	B	1.96	C	0.04																3	2008																												AlB2			A	3.075		3.522												K		35.6	35.8				35.6																																																																																																High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150650	P077214507	formula-weight = 44.56,  unit cell volume = 28.46 A^3	(Mg,Li)(B,C)2	Mg0.91Li0.09B1.84C0.16	Mg	0.91	Li	0.09	B	1.84	C	0.16																3	2008																												AlB2			A	3.0561		3.519												K		30.15	30.6				30.15																																																																																																High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150651	P077214507	formula-weight = 44.41,  unit cell volume = 28.43 A^3	(Mg,Li)(B,C)2	Mg0.9Li0.1B1.82C0.18	Mg	0.9	Li	0.1	B	1.82	C	0.18																3	2008																												AlB2			A	3.053		3.522												K		28.5	28.5				28.5																																																																																																High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150652	P077214507	formula-weight = 44.16,  unit cell volume = 28.58 A^3	(Mg,Li)(B,C)2	Mg0.89Li0.11B1.88C0.12	Mg	0.89	Li	0.11	B	1.88	C	0.12																3	2008																												AlB2			A	3.0602		3.5243												K		29.9	30.2				29.9																				T														MHC150652																																																														High-pressure synthesis					MgB2 single crystals substituted with Li and with Li-C: Structural and superconducting properties			Laboratory for Solid State Physics, Eidgenossische Technische Hochschule, 8093 Zurich, Switzerland	Phys.Rev., 77(2008)214507	J. Karpinski,N. D. Zhigadlo,S. Katrych,K. Rogacki,B. Batlogg,M. Tortello,R. Puzniak		
150653	P077214524	optimally doped.  LTO-LTT transition at 77 K.	(La,Nd,Sr)2CuO4	La1.45Nd0.4Sr0.15Cu1O4	La	1.45	Nd	0.4	Sr	0.15	Cu	1													O	4		3	2008																												T																		K	13.6		30				21.8																																																																																																single crystals grown by TSFZ method					Two-dimensional superconductivity in stripe-ordered La1.6-xNd0.4SrxCuO4 single crystals			Hefei National Laboratory for Physical Sciences at Microscale, Department of Physics, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev., 77(2008)214524	J. F. Ding,X. Q. Xiang,Y. Q. Zhang,H. Liu,H. Liu		
150654	PHB3780142	not SC. Tn decreases as increasing x, and goes to zero at x = 0.35.	CeRh(In,Sn)5	Ce1Rh1In4.88Sn0.12	Ce	1	Rh	1	In	4.88	Sn	0.12																3	2006																												HoCoGa5																		K					0.5			MTN150654																																																																																																				Antiferromagnetic quantum critical point in CeRhIn5-xSnx			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Physica B, 378-380(2006)142	E.D. Bauer,D. Mixson,F. Ronning,N. Hur,R. Movshovich,J.D. Thompson,J.L. Sarrao,M.F. Hundley,P.H. Tobash,S. Bobev		
150655	PSS2360412	penetration depth measured by mutual inductance technique.	(La,Ce)2CuO4	La1.925Ce0.075Cu1O4	La	1.925	Ce	0.075	Cu	1															O	4		5	2003																												T'																		K		25					25																				T		7																																																																										MBE method					Vortex pinning in electron-doped cuprate superconductor La2-xCexCuO4			Department of Physics, Ohio State University, Columbus, OH 43210, USA	phys.stat.sol.(b), 236(2003)412	Yuri Zuev,Thomas R. Lemberger,John A. Skinta,Tine Greibe,Michio Naito		
150656	PSS2360412	penetration depth measured by mutual inductance technique.	(La,Ce)2CuO4	La1.89Ce0.11Cu1O4	La	1.89	Ce	0.11	Cu	1															O	4		5	2003																												T'																		K		29					29																				T		9																																																																										MBE method					Vortex pinning in electron-doped cuprate superconductor La2-xCexCuO4			Department of Physics, Ohio State University, Columbus, OH 43210, USA	phys.stat.sol.(b), 236(2003)412	Yuri Zuev,Thomas R. Lemberger,John A. Skinta,Tine Greibe,Michio Naito		
150657	PSS2360412	penetration depth measured by mutual inductance technique.	(La,Ce)2CuO4	La1.865Ce0.135Cu1O4	La	1.865	Ce	0.135	Cu	1															O	4		5	2003																												T'																		K		21.2					21.2																				T		10																																																																										MBE method					Vortex pinning in electron-doped cuprate superconductor La2-xCexCuO4			Department of Physics, Ohio State University, Columbus, OH 43210, USA	phys.stat.sol.(b), 236(2003)412	Yuri Zuev,Thomas R. Lemberger,John A. Skinta,Tine Greibe,Michio Naito		
150658	PR05802952	it composed of 5-15nm Be nanocrystallites.(amorphous-like XRD). d=4.0 nm. R(T) shows hysteresis for H//plane. tricritical point=190 mK.	Be	Be1	Be	1																						4	1998																																														K		0.6					0.6																																		MHC150658																																																														thermally evaporating 99.5 % pure Be powder onto fire-polished glass substrates held at 84 K.					First-order spin-paramagnetic transition and tricritical point in ultrathin Be films			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803	Phys.Rev.B, 85(1998)2952	P. W. Adams,P. Herron,E. I. Meletis		
150659	PRL0731412	R(H) shows great hysteresis for H//plane at a fixed T. tricritical point=250 mK.	Al	Al1	Al	1																						4	1994																																														K		1.8					1.8																																		MHC150659																																																														films were made by a standard electrochemical anodizetion process which reduced 20 nm Al films evaporated on glass substrates.					Superconductor-insulator transition in a parallel magnetic field			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803	Phys.Rev.Lett., 73(1994)1412	Wenhao Wu,P. W. Adams		
150660	PRL0813765	eutectic structure of Sr2RuO4 and Ru. Hc2 defined as Tc(mid). anisotropy (pcohere/ncohere) = 3.6 at 0 K.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1998																												Sr2RuO4																		K		2.69					2.69																				T	resistive		3.64	1.04										HC150660		A			180	50																																																								single crystals grown by floating zone method with Ru self-flux using Ru-rich feed and/or faster growth rate.					Enhancement of Superconductivity of Sr2RuO4 to 3 K by Embedded Metallic Microdomains			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett.81(1998)3765	E. Ohmichi,S. Ikeda,S. Nakatsuji,S. Nishizaki,T. Ando,Y. Maeno,Y. Mori		
150661	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	RuSr2EuCu2O8	Ru1Sr2Eu1Cu2O8	Ru	1	Sr	2	Eu	1	Cu	2													O	8		1	2008								128																				Ru1212																		K		32.9					32.9																									19.1			5						HC150661																																																														solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150662	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	(Ru,Sn)Sr2EuCu2O8	Ru0.9Sn0.1Sr2Eu1Cu2O8	Ru	0.9	Sn	0.1	Sr	2	Eu	1	Cu	2											O	8		1	2008								85.5																				Ru1212																		K		28.4					28.4																									25			5																																																																				solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150663	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	(Ru,Sn)Sr2EuCu2O8	Ru0.8Sn0.2Sr2Eu1Cu2O8	Ru	0.8	Sn	0.2	Sr	2	Eu	1	Cu	2											O	8		1	2008								82.5																				Ru1212																		K		30.3					30.3																									24			5																																																																				solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150664	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	(Ru,Sn)Sr2EuCu2O8	Ru0.7Sn0.3Sr2Eu1Cu2O8	Ru	0.7	Sn	0.3	Sr	2	Eu	1	Cu	2											O	8		1	2008																												Ru1212																		K		29.5					29.5																									26			5						HC150661																																																														solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150665	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	(Ru,Sn)Sr2EuCu2O8	Ru0.6Sn0.4Sr2Eu1Cu2O8	Ru	0.6	Sn	0.4	Sr	2	Eu	1	Cu	2											O	8		1	2008																												Ru1212																		K		24.2					24.2																									17			5																																																																				solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150666	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	RuSr2GdCu2O8	Ru1Sr2Gd1Cu2O8	Ru	1	Sr	2	Gd	1	Cu	2													O	8		1	2008								132																				Ru1212																		K		50.7					50.7																																		HC150666																																																														solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150667	P077214514	Tc defined as a sudden drop in microwave absorption. Tm : the peak of microwave absorption.	(Ru,Sn)Sr2GdCu2O8	Ru0.8Sn0.2Sr2Gd1Cu2O8	Ru	0.8	Sn	0.2	Sr	2	Gd	1	Cu	2											O	8		1	2008								70.4																				Ru1212																		K		48.1					48.1																																		HC150666																																																														solid state reaction					Microwave and magnetotransport properties of RuSr2RCu2O8 (R=Eu,Gd) doped with Sn			Department of Physics, Faculty of Science, University of Zagreb, P.O. Box 331, HR-10002 Zagreb, Croatia	Phys.Rev.B, 77(2008)214514	M. Pozek,I. Kupcic,A. Dulcic,A. Hamzic,D. Paar,M. Basletic,E. Tafra,G. V. M. Williams		
150668	P077224410	Td1(HTT-MTO transition) = 305 K, Td2(MTO-LTT transition) = 35 K, incommensulability : delta = 0.107	(La,Ba)2CuO4	La1.92Ba0.08Cu1O4	La	1.92	Ba	0.08	Cu	1															O	4		3	2008								39																				T																		K		29					29																																																																																																Floating zone image furnace					Incommensurate spin ordering and fluctuations in underdoped La2-xBaxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 77(2008)224410	S. R. Dunsiger,Y. Zhao,Z. Yamani,W. J. L. Buyers,H. A. Dabkowska,B. D. Gaulin		
150669	P077224410	Td1(HTT-MTO transition) = 272 K, Td2(MTO-LTT transition) = 45 K, incommensulability : delta = 0.112	(La,Ba)2CuO4	La1.905Ba0.095Cu1O4	La	1.905	Ba	0.095	Cu	1															O	4		3	2008								39.5																				T																		K		27					27																																																																																																Floating zone image furnace					Incommensurate spin ordering and fluctuations in underdoped La2-xBaxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 77(2008)224410	S. R. Dunsiger,Y. Zhao,Z. Yamani,W. J. L. Buyers,H. A. Dabkowska,B. D. Gaulin		
150670	P077224410	Td1(HTT-MTO transition) = 232 K, Td2(MTO-LTT transition) = 60 K, incommensulability : delta = 0.118	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		3	2008								50																				T																		K		4					4																																																																																																Floating zone image furnace					Incommensurate spin ordering and fluctuations in underdoped La2-xBaxCuO4			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 77(2008)224410	S. R. Dunsiger,Y. Zhao,Z. Yamani,W. J. L. Buyers,H. A. Dabkowska,B. D. Gaulin		
150671	P078014502	SC properties obtained from TF-muonSR data. GL parameter = 55 at 0 K.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2008																												Ir3Ge7																		K		2.1					2.1											mT	muon-SR	1.8							T	muon-SR	1.9														A		130			A	muon-SR	7200			meV	0.35	3.83	16																																															peritectic reaction between Mo and liquid Sb.					Muon-spin rotation measurements of the penetration depth of the Mo3Sb7 superconductor			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 78(2008)014502	R. Khasanov,P. W. Klamut,A. Shengelaya,Z. Bukowski,I. M. Savic,C. Baines,H. Keller		
150672	P077224503	impurity phase(LaCuO2.5)<a few %. penet(ab) derived from effective penet(104 nm) which measured by muon-SR.  sample shows phase separation (magnetic and nonmagnetic). T2 shows bulk Tc.	(Sr,La)CuO2	Sr0.9La0.1Cu1O2	Sr	0.9	La	0.1	Cu	1															O	2		1	2008																												IL																		K		39.9	41.8				39.9																																									A	muon-SR		800																																																				high pressure synthesis(1000C,6GPa)					Fermi-liquid behavior and weakly anisotropic superconductivity in the electron-doped cuprate Sr1-xLaxCuO2			Department of Materials Structure Science, The Graduate University for Advanced Studies, Tsukuba, Ibaraki 305-0801, Japan	Phys.Rev.B, 77(2008)224503	Kohki H. Satoh,Soshi Takeshita,Akihiro Koda,Ryosuke Kadono,Kenji Ishida,Sunsen Pyon,Takao Sasagawa,Hidenori Takagi		
150673	P077224503	impurity phase(LaCuO2.5)<a few %. penet(ab) derived from effective penet(105 nm) which measured by muon-SR.  sample shows phase separation (magnetic and nonmagnetic). T2 shows bulk Tc.	(Sr,La)CuO2	Sr0.875La0.125Cu1O2	Sr	0.875	La	0.125	Cu	1															O	2		1	2008																												IL																		K		36.9	41.8				36.9																																									A	muon-SR		808																																																				high pressure synthesis(1000C,6GPa)					Fermi-liquid behavior and weakly anisotropic superconductivity in the electron-doped cuprate Sr1-xLaxCuO2			Department of Materials Structure Science, The Graduate University for Advanced Studies, Tsukuba, Ibaraki 305-0801, Japan	Phys.Rev.B, 77(2008)224503	Kohki H. Satoh,Soshi Takeshita,Akihiro Koda,Ryosuke Kadono,Kenji Ishida,Sunsen Pyon,Takao Sasagawa,Hidenori Takagi		
150674	P077224503	impurity phase(LaCuO2.5)<a few %. penet(ab) derived from effective penet(119 nm) which measured by muon-SR.  sample shows phase separation (magnetic and nonmagnetic). T2 shows bulk Tc.	(Sr,La)CuO2	Sr0.85La0.15Cu1O2	Sr	0.85	La	0.15	Cu	1															O	2		1	2008																												IL																		K		31.9	42				31.9																																									A	muon-SR		915																																																				high pressure synthesis(1000C,6GPa)					Fermi-liquid behavior and weakly anisotropic superconductivity in the electron-doped cuprate Sr1-xLaxCuO2			Department of Materials Structure Science, The Graduate University for Advanced Studies, Tsukuba, Ibaraki 305-0801, Japan	Phys.Rev.B, 77(2008)224503	Kohki H. Satoh,Soshi Takeshita,Akihiro Koda,Ryosuke Kadono,Kenji Ishida,Sunsen Pyon,Takao Sasagawa,Hidenori Takagi		
150675	P077224507	RRR = 1.77. (dC/gamma*Tc) = 1.71. thermodynamic Hc(0) = 23 mT.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2008																		GPa		93								clathrate																		K		8.1					8.1																				T	SP, RES, WHH	5.75												MHC150675														4	14							mJ/mol.K2	123.7														Ohm.cm							0.68																		powder samples synthesized under high-T and high-P conditions					Phonon density of states, anharmonicity, electron-phonon coupling, and possible multigap superconductivity in the clathrate superconductors Ba8Si46 and Ba24Si100: Factors behind large difference in Tc			Department of Condensed Matter Physics, University of Geneva, 24 Quai Ernest-Ansermet, CH-1211 Geneva 4, Switzerland	Phys.Rev.B, 77(2008)224507	Rolf Lortz,Romain Viennois,Alexander Petrovic,Yuxing Wang,Pierre Toulemonde,Christoph Meingast,Michael Marek Koza,Hannu Mutka,Alexei Bossak,Alfonso San Miguel		
150676	P077224507	RRR = 4.33. (dC/gamma*Tc) = 1.1. thermodynamic Hc(0) = 2.8 mT.	Ba24Si100	Ba24Si100	Ba	24	Si	100																					2008																		GPa		90								clathrate																		K		1.55					1.55																				T	SP, RES, WHH	0.35												MHC150676														3	14							mJ/mol.K2	189.7														Ohm.cm							24.4																		powder samples synthesized under high-T and high-P conditions					Phonon density of states, anharmonicity, electron-phonon coupling, and possible multigap superconductivity in the clathrate superconductors Ba8Si46 and Ba24Si100: Factors behind large difference in Tc			Department of Condensed Matter Physics, University of Geneva, 24 Quai Ernest-Ansermet, CH-1211 Geneva 4, Switzerland	Phys.Rev.B, 77(2008)224507	Rolf Lortz,Romain Viennois,Alexander Petrovic,Yuxing Wang,Pierre Toulemonde,Christoph Meingast,Michael Marek Koza,Hannu Mutka,Alexei Bossak,Alfonso San Miguel		
150677	PHB4031154	detailed structure parameters are obtained.	FeSr2YCu2O6	Fe1Sr2Y1Cu2O6+z	Fe	1	Sr	2	Y	1	Cu	2													O	6+z		1	2008																												M1212	P4/mmm		A	3.822		11.365												K				59			59																																																																																															1	See J.Phys.Soc.Jpn, 71(2002)790. High-P annealed samples					Substitution of neodymium in the FeSr2YCu2O6+z superconductor			Quantum Beam Center, National Institute for Materials Science (NIMS), 1-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1154	T. Wuernisha,Y. Hata,T. Mochiku,H. Yasuoka,H. Kitazawa		
150678	PHB4031154	detailed structure parameters are obtained.	FeSr2(Y,Nd)Cu2O6	Fe1Sr2Y0.75Nd0.25Cu2O6+z	Fe	1	Sr	2	Y	0.75	Nd	0.25	Cu	2											O	6+z		1	2008																												M1212	P4/mmm		A	3.8304		11.3952												K				34			34																																																																																															1	See J.Phys.Soc.Jpn, 71(2002)790. High-P annealed samples					Substitution of neodymium in the FeSr2YCu2O6+z superconductor			Quantum Beam Center, National Institute for Materials Science (NIMS), 1-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1154	T. Wuernisha,Y. Hata,T. Mochiku,H. Yasuoka,H. Kitazawa		
150679	PHB4031154	detailed structure parameters are obtained.	FeSr2(Y,Nd)Cu2O6	Fe1Sr2Y0.5Nd0.5Cu2O6+z	Fe	1	Sr	2	Y	0.5	Nd	0.5	Cu	2											O	6+z		1	2008																												M1212	P4/mmm		A	3.8455		11.4212												K				23			23																																																																																															1	See J.Phys.Soc.Jpn, 71(2002)790. High-P annealed samples					Substitution of neodymium in the FeSr2YCu2O6+z superconductor			Quantum Beam Center, National Institute for Materials Science (NIMS), 1-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1154	T. Wuernisha,Y. Hata,T. Mochiku,H. Yasuoka,H. Kitazawa		
150680	PHB4031154	detailed structure parameters are obtained.	FeSr2(Y,Nd)Cu2O6	Fe1Sr2Y0.25Nd0.75Cu2O6+z	Fe	1	Sr	2	Y	0.25	Nd	0.75	Cu	2											O	6+z		1	2008																												M1212	P4/mmm		A	3.8498		11.4356												K					4.2																																																																																																	1	See J.Phys.Soc.Jpn, 71(2002)790. High-P annealed samples					Substitution of neodymium in the FeSr2YCu2O6+z superconductor			Quantum Beam Center, National Institute for Materials Science (NIMS), 1-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1154	T. Wuernisha,Y. Hata,T. Mochiku,H. Yasuoka,H. Kitazawa		
150681	PHB4031154	detailed structure parameters are obtained.	FeSr2(Y,Nd)Cu2O6	Fe1Sr2Nd1Cu2O6+z	Fe	1	Sr	2	Nd	1	Cu	2													O	6+z		1	2008																												M1212	P4/mmm		A	3.8436		11.4581												K					4.2																																																																																																	1	See J.Phys.Soc.Jpn, 71(2002)790. High-P annealed samples					Substitution of neodymium in the FeSr2YCu2O6+z superconductor			Quantum Beam Center, National Institute for Materials Science (NIMS), 1-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1154	T. Wuernisha,Y. Hata,T. Mochiku,H. Yasuoka,H. Kitazawa		
150682	PHB4031529	Bi-nanowire shows SC at ambient pressure.	Bi-nanowire	Bi1	Bi	1																						3	2008																													R3[-]c		A	4.5214		11.1775												K			0.64				0.64																																																																																																Bi-nanowires were electroplated into the pores of ion-track etched polycarbonate membranes.					Evidence for superconductivity in single crystalline Bi nanowires			Department of Physics, Texas A&M University, College Station, TX 77843, USA	Physica B, 403(2008)1529	Zuxin Ye,Hong Zhang,Haidong Liu,Wenhao Wu,Zhiping Luo		
150683	PHC4680925	single phase for 0 =< x =<0.6, 0=< y=< 0.6 in Sr2-xBax)(Y1-yCay)-series.	(Pb,B)(Sr,Ba)2(Y,Ca)Cu2Oz	Pb0.5B0.5Sr1.5Ba0.5Y0.4Ca0.4Cu2Oz	Pb	0.5	B	0.5	Sr	1.5	Ba	0.5	Y	0.4	Ca	0.4	Cu	2							O	z		1	2008																												Pb1212			A	3.827		11.95												K	40		50	45			45										28																																																																																				PbO,SrCO3,CaCO3,Y2O3,CuO,B2O3		precursors(Sr2CuO3, Ca2CuO3) used. SIN(950C,15h,in O2) - ANN(400C,24h, in O2) - cool to RT(0.5C/min)					New superconducting Pb-based 1212 cuprates containing boron, (Pb0.5B0.5)(Sr2-xBax)(Y1-yCay)Cu2Oz			Department of Physics, School of Medicine, Hamamatsu University, 1-20-1 Handayama, Higashi-ku, Hamamatsu, Shizuoka 431-3192, Japan	Physica C, 468(2008)925	Hiroyuki Sasakura,Yoshiya Akagi,Shigeki Tsukui,Motoaki Adachi		
150684	SSC1470027		MgB2	B2Mg1	B	2	Mg	1																				1	2008																												AlB2			A	3.0827		3.5217												K		39					39																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150685	SSC1470027	solubility limit: x =< 0.03	(Mg,Co)B2	Mg0.99Co0.01B2	Mg	0.99	Co	0.01	B	2																		1	2008																												AlB2			A	3.0828		3.5219												K		38.7					38.7																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150686	SSC1470027	solubility limit: x =< 0.03	(Mg,Co)B2	Mg0.98Co0.02B2	Mg	0.98	Co	0.02	B	2																		1	2008																												AlB2			A	3.0827		3.5224												K		37.4					37.4																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150687	SSC1470027	solubility limit: x =< 0.03	(Mg,Co)B2	Mg0.97Co0.03B2	Mg	0.97	Co	0.03	B	2																		1	2008																												AlB2			A	3.083		3.5226												K		36.2					36.2																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150688	SSC1470027	solubility limit: x =< 0.03	(Mg,Mn)B2	Mg0.99Mn0.01B2	Mg	0.99	Mn	0.01	B	2																		1	2008																												AlB2			A	3.0829		3.5178												K		30.6					30.6																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150689	SSC1470027	solubility limit: x =< 0.03	(Mg,Mn)B2	Mg0.98Mn0.02B2	Mg	0.98	Mn	0.02	B	2																		1	2008																												AlB2			A	3.082		3.5163												K		23.2					23.2																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150690	SSC1470027	solubility limit: x =< 0.03	(Mg,Mn)B2	Mg0.97Mn0.03B2	Mg	0.97	Mn	0.03	B	2																		1	2008																												AlB2			A	3.0806		3.5097												K		12.4					12.4																																																																																															1	mixture - pellet - put( stainless steal in quartz tube) - heat(950C,2h)					Effects of Co and Mn doping on the structure and superconductivity of MgB2			Hefei National Laboratory for Physical Science at Microscale, University of Science and Technology of China, Academia Sinica, Hefei, Anhui 230026, PR China	Solid State Commun., 147(2008)27	Lei Shi,Shangming Zhang,Huarong Zhang		
150691	PCS0450419	coexistence of itinerant AFM and SC	LaRh2Si2	La1Rh2Si2	La	1	Rh	2	Si	2																		1	1984							-41	7																				ThCr2Si2			A	4.114		10.31												K		3.8					3.8																																																																																																arc-melting using induction furnace					ITINERANT AND LOCAL MAGNETISM, SUPERCONDUCTIVITY AND MIXED VALENCY PHENOMENA IN RM2Si2, (R = RARE EARTH, M = Rh, Ru)			Hebrew University,Jerusalem,Israel	J.Phys.Chem.Solids, 45(1984)419	Israel Felner,Israel Nowik		
150692	PCS0450419		LuRh2Si2	Lu1Rh2Si2	Lu	1	Rh	2	Si	2																		1	1984							-28	17																				ThCr2Si2			A	4		9.87												K					1.4																																																																																																		arc-melting using induction furnace					ITINERANT AND LOCAL MAGNETISM, SUPERCONDUCTIVITY AND MIXED VALENCY PHENOMENA IN RM2Si2, (R = RARE EARTH, M = Rh, Ru)			Hebrew University,Jerusalem,Israel	J.Phys.Chem.Solids, 45(1984)419	Israel Felner,Israel Nowik		
150693	PCS0450419	coexistence of itinerant AFM and SC	YRh2Si2	Y1Rh2Si2	Y	1	Rh	2	Si	2																		1	1984							-8	5																				ThCr2Si2			A	4.031		9.92												K		3.1					3.1																																																																																																arc-melting using induction furnace					ITINERANT AND LOCAL MAGNETISM, SUPERCONDUCTIVITY AND MIXED VALENCY PHENOMENA IN RM2Si2, (R = RARE EARTH, M = Rh, Ru)			Hebrew University,Jerusalem,Israel	J.Phys.Chem.Solids, 45(1984)419	Israel Felner,Israel Nowik		
150694	PCS0450419		LaRu2Si2	La1Ru2Si2	La	1	Ru	2	Si	2																		1	1984							-10																					ThCr2Si2			A	4.219		9.935												K		3.5					3.5																																																																																																arc-melting using induction furnace					ITINERANT AND LOCAL MAGNETISM, SUPERCONDUCTIVITY AND MIXED VALENCY PHENOMENA IN RM2Si2, (R = RARE EARTH, M = Rh, Ru)			Hebrew University,Jerusalem,Israel	J.Phys.Chem.Solids, 45(1984)419	Israel Felner,Israel Nowik		
150695	PCS0450419		LuRu2Si2	Lu1Ru2Si2	Lu	1	Ru	2	Si	2																		1	1984																												ThCr2Si2			A	4.135		9.493												K		2.4					2.4																																																																																																arc-melting using induction furnace					ITINERANT AND LOCAL MAGNETISM, SUPERCONDUCTIVITY AND MIXED VALENCY PHENOMENA IN RM2Si2, (R = RARE EARTH, M = Rh, Ru)			Hebrew University,Jerusalem,Israel	J.Phys.Chem.Solids, 45(1984)419	Israel Felner,Israel Nowik		
150696	NAS0741334	Tc measured for MRh4B4 + 2[RhB] material. structure type not clear.	YRh4B4	Y1Rh4B4	Y	1	Rh	4	B	4																			1977																												RT4B4																		K	11.26	11.34					11.34																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150697	NAS0741334	Tc measured for MRh4B4 + 2[RhB] material. structure type not clear.	NdRh4B4	Nd1Rh4B4	Nd	1	Rh	4	B	4																			1977																												RT4B4																		K	5.26	5.36					5.36																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150698	NAS0741334	Tc measured for MRh4B4 + 2[RhB] material. structure type not clear.	SmRh4B4	Sm1Rh4B4	Sm	1	Rh	4	B	4																			1977																												RT4B4																		K	2.45	2.51					2.51																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150699	NAS0741334	Tc measured for MRh4B4 + 2[RhB] material. structure type not clear.	ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1977																												RT4B4																		K	8.49	8.55					8.55																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150700	MAT8042105	not SC.	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1			2008																												oxypnictide			A	3.9403		8.5014											ZrCuSiAs-type	K					4.91																																																																									mOhm.cm							3.05							E-9 m3/C						RH150700			SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150701	MAT8042105	not SC.	Sm(O,F)FeAs	Sm1Fe1As1F0.05O0.95	Sm	1	Fe	1	As	1	F	0.05													O	0.95			2008																												oxypnictide			A	3.9395		8.5006											ZrCuSiAs-type	K					4.91																																																																									mOhm.cm							1.93							E-9 m3/C						RH150700			SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150702	MAT8042105	R not to zero. Tc from Fig of R(T) by us.	Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9			2008																												oxypnictide			A	3.9353		8.4962											ZrCuSiAs-type	K		4.47	13				4.47																																																																							mOhm.cm							1.74							E-9 m3/C						RH150700			SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150703	MAT8042105	Tc from Fig of R(T) by us.	Sm(O,F)FeAs	Sm1Fe1As1F0.12O0.88	Sm	1	Fe	1	As	1	F	0.12													O	0.88			2008																												oxypnictide																	ZrCuSiAs-type	K	12.8	17.3	23.5				17.3																																																																							mOhm.cm							1.57																SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150704	MAT8042105	Tc from Fig of R(T) by us.	Sm(O,F)FeAs	Sm1Fe1As1F0.14O0.86	Sm	1	Fe	1	As	1	F	0.14													O	0.86			2008																												oxypnictide																	ZrCuSiAs-type	K	20.5	26.8	33.9				26.8																																																																							mOhm.cm							1.44																SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150705	MAT8042105	Tc from Fig of R(T) by us.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2008																												oxypnictide			A	3.9316		8.4931											ZrCuSiAs-type	K	40.4	42.3	44.7				42.3																																																																							mOhm.cm							0.988							E-9 m3/C						RH150705			SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150706	MAT8042105	Tc from Fig of R(T) by us.	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8			2008																												oxypnictide			A	3.926		8.4799											ZrCuSiAs-type	K	51.2	52.4	54	51.6			52.4																																																																							mOhm.cm							0.531							E-9 m3/C						RH150705			SmAs,SmF3,Fe,Fe2O3		solid state reaction. mixture - pellet - wrapped in Ta foil sealed in quartz tube - ANN(1160C,40h)					Phase Diagram and Quantum phase transition in Newly Discovered Superconductors: SmO1-xFxFeAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0804.2105(Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G. Wu,T. Wu,D. F. Fang,H. Chen,S. Y. Li,K. Liu,Y.L.Xie,X. F. Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
150707	CPL0252215		Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9			2008																												oxypnictide	P4/nmm		A	3.915		8.428											ZrCuSiAs-type	K	52.6		55	54.6			54.6																																																																																														Sm,As,Fe,Fe2O3,FeF2		high pressure synthesis (1250C,2h,P=6 GPa)					Superconductivity at 55 K in iron-based F-doped layered quaternary compound Sm[O1-xFx]FeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Chinese Phys.Lett.,25(2008)2215	Ren Zhi-An,Lu Wei,Yang Jie,Yi Wei,Shen Xiao-Li,Li Zheng-Cai,Che Guang-Can,Dong Xiao-Li,Sun Li-Ling,Zhou Fang,Zhong-Xian Zhao		
150708	T021082001	F-content shows nominal value.	GdOFeAs	Gd1Fe1As1O0.85	Gd	1	Fe	1	As	1															O	0.85			2008																												oxypnictide	P4/nmm		A	3.89		8.383											ZrCuSiAs-type	K	52.3		53.5	53.5			53.5																																																																																														Gd,As,Fe,Fe2O3,FeF2		high pressure synthesis (1350C,2h,P=6 GPa)					Superconductivity at 53.5 K in GdFeAsO1-z			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Supercond.Sci.Technol., 21(2008)082001	Jie Yang,Zheng-Cai Li,Wei Lu,Wei Yi,Xiao-Li Shen,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150709	T021082001	F- and O-contents show nominal value.	Gd(O,F)FeAs	Gd1Fe1As1F0.2O0.8	Gd	1	Fe	1	As	1	F	0.2													O	0.8			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K	45.5		51.2				48.35																																																																																														Gd,As,Fe,Fe2O3,FeF2		high pressure synthesis (1350C,2h,P=6 GPa)					Superconductivity at 53.5 K in GdFeAsO1-z			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Supercond.Sci.Technol., 21(2008)082001	Jie Yang,Zheng-Cai Li,Wei Lu,Wei Yi,Xiao-Li Shen,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150710	EP08257002		Nd(O,F)FeAs	Nd1Fe1As1F0.11O0.89	Nd	1	Fe	1	As	1	F	0.11													O	0.89			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K	48.8	50.1	51.9	51.7			50.1																																																																																														Nd,As,Fe,Fe2O3,FeF3		high pressure synthesis (1300C,2h,P=6 GPa)					Superconductivity in the iron-based F-doped layered quaternary compound Nd[O1-xFx]FeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 82(2008)57002	Zhi-An Ren,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150711	CPL0252235	not SC. R(T) anomaly at 145 K.	NdOFeAs	Nd1Fe1As1O1	Nd	1	Fe	1	As	1															O	1			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K					5																																																																																																		RAs obtained by reacting (R+As, 500C,15h - 850C,5h) then wrapped in Ta foil - ANN(1150C,24-50h)					Element substitution effect in transition metal oxypnictide Re(O1-xFx)TAs (Re=rare earth, T=transition metal)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Chinese Phys.Lett.,25(2008)2235	G. F. Chen,Z. Li,D. Wu,J. Dong,G. Li,W. Z. Hu,P. Zheng,J. L. Luo,N. L. Wang		
150712	CPL0252235	not SC. R(T) anomaly at 105 K.	Nd(O,F)FeAs	Nd1Fe1As1F0.04O0.96	Nd	1	Fe	1	As	1	F	0.04													O	0.96			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K					5																																																																																																		RAs obtained by reacting (R+As, 500C,15h - 850C,5h) then wrapped in Ta foil - ANN(1150C,24-50h)					Element substitution effect in transition metal oxypnictide Re(O1-xFx)TAs (Re=rare earth, T=transition metal)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Chinese Phys.Lett.,25(2008)2235	G. F. Chen,Z. Li,D. Wu,J. Dong,G. Li,W. Z. Hu,P. Zheng,J. L. Luo,N. L. Wang		
150713	CPL0252235		Nd(O,F)FeAs	Nd1Fe1As1F0.08O0.92	Nd	1	Fe	1	As	1	F	0.08													O	0.92			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K			35				35																																																																																																RAs obtained by reacting (R+As, 500C,15h - 850C,5h) then wrapped in Ta foil - ANN(1150C,24-50h)					Element substitution effect in transition metal oxypnictide Re(O1-xFx)TAs (Re=rare earth, T=transition metal)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Chinese Phys.Lett.,25(2008)2235	G. F. Chen,Z. Li,D. Wu,J. Dong,G. Li,W. Z. Hu,P. Zheng,J. L. Luo,N. L. Wang		
150714	CPL0252235		Nd(O,F)FeAs	Nd1Fe1As1F0.12O0.88	Nd	1	Fe	1	As	1	F	0.12													O	0.88			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K			48				48																																																																																																RAs obtained by reacting (R+As, 500C,15h - 850C,5h) then wrapped in Ta foil - ANN(1150C,24-50h)					Element substitution effect in transition metal oxypnictide Re(O1-xFx)TAs (Re=rare earth, T=transition metal)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Chinese Phys.Lett.,25(2008)2235	G. F. Chen,Z. Li,D. Wu,J. Dong,G. Li,W. Z. Hu,P. Zheng,J. L. Luo,N. L. Wang		
150715	CPL0252235		Nd(O,F)FeAs	Nd1Fe1As1F0.16O0.84	Nd	1	Fe	1	As	1	F	0.16													O	0.84			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K			46				46																																																																																																RAs obtained by reacting (R+As, 500C,15h - 850C,5h) then wrapped in Ta foil - ANN(1150C,24-50h)					Element substitution effect in transition metal oxypnictide Re(O1-xFx)TAs (Re=rare earth, T=transition metal)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Chinese Phys.Lett.,25(2008)2235	G. F. Chen,Z. Li,D. Wu,J. Dong,G. Li,W. Z. Hu,P. Zheng,J. L. Luo,N. L. Wang		
150716	EP08317002	O-content shows nominal value.	SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm		A	3.897		8.407											ZrCuSiAs-type	K	52.8		55	55			55	TC150716																																																																																															high pressure synthesis					Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1-z (Re = rare-earth metal) without fluorine doping			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 83(2008)17002	Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150717	EP08317002	O-content shows nominal value. lattice const(in Fig.) depends on O-content.	NdOFeAs	Nd1Fe1As1O0.85	Nd	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm		A	3.943		8.521											ZrCuSiAs-type	K	50.9		53.5	51			51	TC150717																																																																																															high pressure synthesis					Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1-z (Re = rare-earth metal) without fluorine doping			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 83(2008)17002	Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150718	EP08317002	O-content shows nominal value.	PrOFeAs	Pr1Fe1As1O0.85	Pr	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm		A	3.968		8.566											ZrCuSiAs-type	K	43.2		51.3	48.2			48.2	TC150716																																																																																															high pressure synthesis					Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1-z (Re = rare-earth metal) without fluorine doping			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 83(2008)17002	Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150719	EP08317002	O-content shows nominal value.	CeOFeAs	Ce1Fe1As1O0.85	Ce	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm		A	3.979		8.605											ZrCuSiAs-type	K	41		46.5	42.6			42.6	TC150716																																																																																															high pressure synthesis					Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1-z (Re = rare-earth metal) without fluorine doping			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 83(2008)17002	Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150720	EP08317002	O-content shows nominal value.	LaOFeAs	La1Fe1As1O0.85	La	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm		A	4.022		8.707											ZrCuSiAs-type	K	25.9		31.2	28.3			28.3	TC150716																																																																																															high pressure synthesis					Superconductivity and phase diagram in iron-based arsenic-oxides ReFeAsO1-z (Re = rare-earth metal) without fluorine doping			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P.O. Box 603, Beijing 100190, PRC	Europhys.Lett., 83(2008)17002	Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Jie Yang,Wei Lu,Wei Yi,Xiao-Li Shen,Zheng-Cai Li,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150721	MAT8044290	not SC. R-anomaly at 135K	GdOFeAs	Gd1Fe1As1O1	Gd	1	Fe	1	As	1															O	1			2008								4.2																				oxypnictide			A	3.9151		8.446											ZrCuSiAs-type	K					5																																																																																																		solid state reaction. ANN(1030C,12h)					Thorium-doping induced superconductivity in Gd1-xThxOFeAs			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	cond-mat/0804.4290	Cao Wang,Linjun Li,Shun Chi,Zengwei Zhu,Zhi Ren,Yuke Li,Yuetao Wang,Xiao Lin,Yongkang Luo,Xiangfan Xu,Guanghan Cao,Zhu'an Xu		
150722	MAT8044290		(Gd,Th)OFeAs	Gd0.8Th0.2Fe1As1O1	Gd	0.8	Th	0.2	Fe	1	As	1													O	1			2008																												oxypnictide			A	3.9167		8.44											ZrCuSiAs-type	K			56.3	56.5			56.5										50																																																																																						solid state reaction. ANN(1030C,12h)					Thorium-doping induced superconductivity in Gd1-xThxOFeAs			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	cond-mat/0804.4290	Cao Wang,Linjun Li,Shun Chi,Zengwei Zhu,Zhi Ren,Yuke Li,Yuetao Wang,Xiao Lin,Yongkang Luo,Xiangfan Xu,Guanghan Cao,Zhu'an Xu		
150723	MAT8061459		BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2008																												ThCr2Si2			A	3.961		13.017												K					5																																																																				uV/K				MTP150723																								BaAs,FeAs,Fe,K,		solid state reaction.					Transport properties and superconductivity in Ba1-xMxFe2As2 (M=La and K) with double FeAs layers			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0806.1459	G. Wu,R. H. Liu,H. Chen,Y. J. Yan,T. Wu,Y. L. Xie,J. J. Ying,X. F. Wang,D. F. Fang,X. H. Chen		
150724	MAT8061459		(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2008																												ThCr2Si2			A	3.921		13.228												K				38			38										34																																																								uV/K				MTP150724															E-9 m3/C						MRH150724			BaAs,FeAs,Fe,K,		solid state reaction.					Transport properties and superconductivity in Ba1-xMxFe2As2 (M=La and K) with double FeAs layers			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0806.1459	G. Wu,R. H. Liu,H. Chen,Y. J. Yan,T. Wu,Y. L. Xie,J. J. Ying,X. F. Wang,D. F. Fang,X. H. Chen		
150725	MAT8061459		(Ba,K)OFe2As2	Ba0.5K0.5Fe2As2O1	Ba	0.5	K	0.5	Fe	2	As	2													O	1			2008																																														K				36			36										26																																																																											E-9 m3/C						MRH150725			BaAs,FeAs,Fe,K,		solid state reaction.					Transport properties and superconductivity in Ba1-xMxFe2As2 (M=La and K) with double FeAs layers			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China	cond-mat/0806.1459	G. Wu,R. H. Liu,H. Chen,Y. J. Yan,T. Wu,Y. L. Xie,J. J. Ying,X. F. Wang,D. F. Fang,X. H. Chen		
150726	MAT8054630	no SDW anomaly in R(T). a=3.909, c=13.2122 A at 20 K. no structural transformation  down to 20 K.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2008																												ThCr2Si2			A	3.917		13.2968												K		38		38.3			38										93																																																																																						heat(923-1173K in Ar)					Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	cond-mat/0805.4630(Phys.Rev.Lett., 101(2008)107006)	Marianne Rotter,Marcus Tegel,Dirk Johrendt		
150727	MAT8061209	small anomaly (SDW) in R(T).	(Sr,K)Fe2As2	Sr0.6K0.4Fe2As2	Sr	0.6	K	0.4	Fe	2	As	2																	2008																												ThCr2Si2																		K		38					38																																																																																																solid state reaction.					Superconductivity in hole-doped (Sr1-xKx)Fe2As2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/0806.1209	G. F. Chen,Z. Li,G. Li,W. Z. Hu,J. Dong,X. D. Zhang,P. Zheng,N. L. Wang,J. L. Luo		
150728	MAT8061209	reannealed sample. no anomaly in R(T)	(Sr,K)Fe2As2	Sr0.6K0.4Fe2As2	Sr	0.6	K	0.4	Fe	2	As	2																1	2008																												ThCr2Si2																		K		20		20			20																																																																																					E-9 m3/C						MRH150728					solid state reaction.					Superconductivity in hole-doped (Sr1-xKx)Fe2As2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/0806.1209	G. F. Chen,Z. Li,G. Li,W. Z. Hu,J. Dong,X. D. Zhang,P. Zheng,N. L. Wang,J. L. Luo		
150729	P077180510	impurity phases: SmOF,SmAs < 10%. GAMMA = 83.7(H=8T) mJ/mol.K2 ,  obtained by fitting for 14<T<20 K. NEEL-T by C(T). Tc = mid point in C(T).	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2008																												oxypnictide																	ZrCuSiAs-type	K		40					40										60																																														mJ/mol.K2	81	SP																																						solid state reaction.					Specific heat of the iron-based high-Tc superconductor SmO1-xFxFeAs			Department of Physics and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 77(2008)180510	L. Ding,C. He,J. K. Dong,T. Wu,R. H. Liu,X. H. Chen,S. Y. Li		
150730	PHC4680464	RRR=15. anomaly at 110 K in R(T) & C(T). lattice term in C(T): beta = 1.3 mj/mol.K4 for 0.35 < T < 4K. Hc(0) = 110 Oe. GL = 15. (dC/gamma*Tc) = 0.67.	Ag6O8AgHF2	Ag7H1F2O8	Ag	7	H	1	F	2															O	8		3	2008																												clathrate	Fm3[-]m																	K		1.38				0.05	1.38											Oe	calculate from Hc(0)	6							T	resistive & WHH	0.22							T/K	resistive	0.228			HC150730		A	from Hc2	410			A	GL & cohere	5600					1.88	14							mJ/mol.K2	55.5	SP	295	SP											mOhm.cm											0.45														electrochemical method. AgF powder & HF solution used as starting materials. moisture is a crucial parameter.					Thermodynamic properties of the clathrate-type silver-oxide Ag6O8AgHF2			Department of Physics and Mathematics, Aoyama-Gakuin University, Kanagawa 229-8558, Japan	Physica C, 468(2008)464	K. Kawashima,M. Kriener,M. Ishii,Y. Maeno,J. Akimitsu		
150731	MAT8033603	impurity phase: SmOF	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2008																												oxypnictide	P4/nmm		A	3.943		8.514											ZrCuSiAs-type	K		41.7	43	41.8			41.7																																																																																																SmAs was obtained by heating(Sm+As) at (600C,3h) and (900C,5h). mixture(SmAs,SmF3,Fe,Fe2O3) - pellet - wrapped in Ta foil - heat(1160,1200C,40h)					Superconductivity at 43 K in Samarium-arsenide OxidesSmFeAsO1-xFx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	cond-mat/0803.3603(2008)	X. H. Chen,T. Wu,G. Wu,R. H. Liu,H. Chen,D. F. Fang		
150732	MAT8061668		Nd(O,F)FeAs	Nd1Fe1As1F0.18O0.82	Nd	1	Fe	1	As	1	F	0.18													O	0.82		3	2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K			50			4	50																																																																							mOhm.cm							0.2													RH150732					flux method using NaCl flux					Hall Effect and Magnetoresistance in Single Crystals of NdFeAsO0.82F0.18			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, China	cond-mat/0806.1668(2008)	Peng Cheng,Huan Yang,Ying Jia,Lei Fang,Xiyu Zhu,Gang Mu,Hai-Hu Wen		
150733	MAT8041726	Hc1 defined as critical point of SQR(B) vs H plot (Hall prove method)	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																												oxypnictide	P4/nmm																	K			26			3	26											Oe	B-H curve	54																					HC150733																																																														two step solid state reaction					Linear Temperature Dependence of the Lower Critical Field Hc1 in F-Doped LaOFeAs Superconductors			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, China	cond-mat/0804.1726(2008)	Cong Ren,Zhao-Sheng Wang,Huan Yang,Xiyu Zhu,Lei Fang,Gang Mu,Lei Shan,Hai-Hu Wen		
150734	MAT8033978		(La,Sr)ONiAs	La0.9Sr0.1Ni1As1O1	La	0.9	Sr	0.1	Ni	1	As	1													O	1			2008																												oxypnictide	P4/nmm																	K			3.7			0.4	3.7																				T		5.5												HC150734																																																												NiAs,Ni,La2O3,SrO		solid state reaction. mixture - pellet - heat(1150C,48h)					Synthesizing and characterization of hole doped nickel based layer superconductor (La1-xSrx)ONiAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, China	Phys.Rev.B, 78(2008)104528: cond-mat/0803.3978(2008)	Lei Fang,Huan Yang,Peng Cheng,Xiyu Zhu,Gang Mu,Hai-Hu Wen		
150735	MAT8033978		(La,Sr)ONiAs	La0.8Sr0.2Ni1As1O1	La	0.8	Sr	0.2	Ni	1	As	1													O	1			2008																												oxypnictide	P4/nmm		A	4.0453		8.7467												K			3.5			0.4	3.5										40																																																																																				NiAs,Ni,La2O3,SrO		solid state reaction. mixture - pellet - heat(1150C,48h)					Synthesizing and characterization of hole doped nickel based layer superconductor (La1-xSrx)ONiAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, China	Phys.Rev.B, 78(2008)104528: cond-mat/0803.3978(2008)	Lei Fang,Huan Yang,Peng Cheng,Xiyu Zhu,Gang Mu,Hai-Hu Wen		
150736	MAT8032572		LaONiAs	La1Ni1As1O1	La	1	Ni	1	As	1															O	1			2008																												oxypnictide	P4/nmm																	K			2.75				2.75																																																																																														NiAs,Ni,La2O3,SrO		solid state reaction. mixture - pellet - heat(1150C,48h)					Strong-coupling superconductivity in nickel-based LaO1-xFxNiAs			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/0803.2572(2008)	Z. Li,G. F. Chen,J. Dong,G. Li,W. Z. Hu,D. Wu,S.K.Su,P. Zheng,T. Xiang,N. L. Wang,J. L. Luo		
150737	MAT8033790	R-peak at 145 K.. Neel-T by SP-heat.	CeOFeAs	Ce1Fe1As1O1	Ce	1	Fe	1	As	1															O	1			2008								3.7																				oxypnictide	P4/nmm		A	3.996		8.648											ZrCuSiAs-type	K					1.8																																																																																																CeAs,Fe,CeO2,CeF3,Fe2As		mixture - pellet - wrapped in Ta foil - heat(1150,50h, in evacuated quartz tube)					Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Phys.Rev.Lett., 100(2008)247002	G. F. Chen,Z. Li,D. Wu,G. Li,W. Z. Hu,J. Dong,P. Zheng,J. L. Luo,N. L. Wang		
150738	MAT8033790		Ce(O,F)FeAs	Ce1Fe1As1F0.16O0.84	Ce	1	Fe	1	As	1	F	0.16													O	0.84			2008																												oxypnictide	P4/nmm		A	3.989		8.631											ZrCuSiAs-type	K			41				41																																																																																														CeAs,Fe,CeO2,CeF3,Fe2As		mixture - pellet - wrapped in Ta foil - heat(1150,50h, in evacuated quartz tube)					Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Phys.Rev.Lett., 100(2008)247002	G. F. Chen,Z. Li,D. Wu,G. Li,W. Z. Hu,J. Dong,P. Zheng,J. L. Luo,N. L. Wang		
150739	MAT8033790		Ce(O,F)FeAs	Ce1Fe1As1F0.12O0.88	Ce	1	Fe	1	As	1	F	0.12													O	0.88			2008																												oxypnictide	P4/nmm																ZrCuSiAs-type	K			40				40																				T	WHH approx.	107							T/K		3.86			HC150739																																																												CeAs,Fe,CeO2,CeF3,Fe2As		mixture - pellet - wrapped in Ta foil - heat(1150,50h, in evacuated quartz tube)					Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, Peoples Republic of China	Phys.Rev.Lett., 100(2008)247002	G. F. Chen,Z. Li,D. Wu,G. Li,W. Z. Hu,J. Dong,P. Zheng,J. L. Luo,N. L. Wang		
150740	MAT8034283	Tc(zero) = 35 K at H=9T.	Pr(O,F)FeAs	Ce1Fe1As1F0.11O0.89	Ce	1	Fe	1	As	1	F	0.11													O	0.89			2008																												oxypnictide	P4/nmm		A	3.967		8.561												K	44	47	52	43.5			47																																																																																														PrAs,Fe,Fe2O3,FeF3		high-pressure synthesis. mixture - pellet -  SIN(1250,2h, P=6GPa)					Superconductivity at 52 K in iron-based F-doped layered quaternary compound Pr[O1-xFx]FeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, P. R. China	cond-mat/0803.4283(2008)	Zhi-An Ren,Jie Yang,Wei Lu,Wei Yi,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Zhong-Xian Zhao		
150741	MAT8034266	impurity phase : LaOF, FeAs2. Tc defined as max(dKai/dT). Tc(on) shows no obvious change upto P = 1.03 Gpa.	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2008																												oxypnictide	P4/nmm		A	4.03		8.706											ZrCuSiAs-type	K	22.3		26.3	23			23			K/GPa	1.2																																																																																												LaFeAs alloy was prepared by arc-mwlting, then solid state reaction(1240C,50h, in muffle furnace)					Pressure Effect on the superconducting properties of LaO1-xFxFeAs(x=0.11) superconductor			National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/0803.4266(2008)	W. Lu,J. Yang,X.L. Dong,Z.A. Ren,G.C. Che,Z.X. Zhao		
150742	MAT8043725	large Meissner effect at 31 K.	La(O,F)FeAs	La1Fe1As1F0.6O0.4	La	1	Fe	1	As	1	F	0.6													O	0.4			2008																												oxypnictide	P4/nmm		A	3.991		8.7												K	30		41	40		11	40																																																																																																high-pressure synthesis.  SIN(1250C,2h, P=6 GPa)					Superconductivity at 41.0 K in the F-doped LaFeAsO1-xFx			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, P. R. China	Solid State Commun., 148(2008)168	Wei Lu,Xiao-Li Shen,Jie Yang,Zheng-Cai Li,Wei Yi,Zhi-An Ren,Xiao-Li Dong,Guang-Can Che,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
150743	MAT8060532	impurity phase: NdClO. Hc2 defined as R=0.95Rn. Hirr defined as R = 0.01Rn. Hc2(0) obtained using WHH and Tc=49 K.	Nd(O,F)FeAs	Nd1Fe1As1F0.18O0.82	Nd	1	Fe	1	As	1	F	0.18													O	0.82		3	2008																												oxypnictide	P4/nmm		A	3.962		8.555												K			52				52																				T	resistive		304	62					T/K	resistive		9	2.09	HC150743																																					mOhm.cm							0.127																		flux method using NaCl flux Heat and keep(1050C,10d) - cool to 850C(3C/h) - FC to RT					Critical Fields and Anisotropy of NdO0.82F0.18FeAs Single Crystals			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/0806.0532(2008)	Ying Jia,Peng Cheng,Lei Fang,Huiqian Luo,Huan Yang,Cong Ren,Lei Shan,Changzhi Gu,Hai-Hu Wen		
150744	MAT8040835		Gd(O,F)FeAs	Gd1Fe1As1F0.17O0.83	Gd	1	Fe	1	As	1	F	0.17													O	0.83			2008																												oxypnictide	P4/nmm		A	4.001		8.65												K			36.6	22			22										40																																																																																	RH150744					solid state reaction.					Superconductivity at 36 K in Gadolinium-arsenide Oxides GdO1-xFxFeAs			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	cond-mat/0804.0835(2008)	Peng Cheng,Lei Fang,Huan Yang,Xiyu Zhu,Gang Mu,Huiqian Luo,Zhaosheng Wang,Hai-Hu Wen		
150745	MAT8064798	[penet] estimated from muon-SR data and Hc2=50T. [ppenet] = [penet]/1.31. two gap superconductor: the lower gap (2:gap/kTc) = 1.1.	La(O,F)FeAs	La1Fe1As1F0.06O0.94	La	1	Fe	1	As	1	F	0.06													O	0.94	0.94		2008																												oxypnictide																	ZrCuSiAs-type	K		18					18																																									A	muon-SR	5950	4540				2.6	16																																																				Coexistence of Supercondcutivity and Magnetism in LaFeAs(O0.94F0.06) Probed by Muon Spin Relaxation			Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305-0801, Japan	cond-mat/0806.4798(2008)	Soshi Takeshita,Ryosuke Kadono,Masatoshi Hiraishi,Masanori Miyazaki,Akihiro Koda,Yohichi Kamihara,Hideo Hosono		
150746	MAT8054340	[vols] at t(=T/Tc) = 0.75. Hc1 and Hc2 measured at T=1.8 K>	LaONiAs	La1Ni1As1O1	La	1	Ni	1	As	1															O	1		1	2008																												oxypnictide	P4/nmm		A	4.1231		8.1885											ZrCuSiAs-type	K		2.4					2.4										20	Oe					15			1.8	Oe					400			1.8																																											mOhm.cm											3.5												La,As(3N),NiO(3N)	1	LaAs by heating (400C,12h) + (700C,6h), then press(LaAs+NiO) - pellet - heat(1000C,1d, in evacuated silica tube)					Nickel-based layered superconductor, LaNiOAs			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	cond-mat/0805.4340(2008)	Takumi Watanabe,Hiroshi Yanagi,Yoichi Kamihara,Toshio Kamiya,Masahiro Hirano,Hideo Hosono		
150747	MAT8064215	Tc defined as 0.8Rn. R(min) at 70 K. Hc2 defined as R(onset), R(off), and TDO(Tunnel Diode Oscillator method)	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95	0.95	1	2008																												oxypnictide																	ZrCuSiAs-type	K		26.3					26.3																																		HC150747																																																									RH150747	E+21/cm3	2.99			solid state reaction					Hall coefficient and Hc2 in underdoped LaFeAsO0.95F0.05			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545	cond-mat/0806.4215(2008)	Y. Kohama,Y. Kamihara,S.Riggs,F.F.Balakirev,T.Atake,M.Jaime,M.Hirano,H.Hosono		
150748	MAT8072223		SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		1	2008																															A	3.924		12.34												K					1.8																																																																																																SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150749	MAT8072223		Sr(Fe,Co)2As2	Sr1Fe1.85Co0.15As2	Sr	1	Fe	1.85	Co	0.15	As	2																1	2008	emu/mol	0.00078																														3.9272		12.3123												K					1.8																																																																									mOhm.cm											0.008												SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150750	MAT8072223	(dC/Tc) = 10 mJ/mol.K2	Sr(Fe,Co)2As2	Sr1Fe1.8Co0.2As2	Sr	1	Fe	1.8	Co	0.2	As	2																1	2008	emu/mol	0.0006																														3.9278		12.3026												K				19.2			19.2	MTC150750																																																							mJ/mol.K2	12.6		255																																			SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150751	MAT8072223		Sr(Fe,Co)2As2	Sr1Fe1.75Co0.25As2	Sr	1	Fe	1.75	Co	0.25	As	2																1	2008																																3.9296		12.2925												K				18.1			18.1																																																																																														SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150752	MAT8072223		Sr(Fe,Co)2As2	Sr1Fe1.6Co0.4As2	Sr	1	Fe	1.6	Co	0.4	As	2																1	2008	emu/mol	0.00036																														3.9293		12.2711												K				12.9			12.9																																																																																														SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150753	MAT8072223		Sr(Fe,Co)2As2	Sr1Fe1.5Co0.5As2	Sr	1	Fe	1.5	Co	0.5	As	2																1	2008																																3.9287		12.2187												K					1.8																																																																									mOhm.cm											0.002												SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150754	MAT8072223		Sr(Fe,Co)2As2	Sr1Fe1Co1As2	Sr	1	Fe	1	Co	1	As	2																1	2008					myu-B/f.u	2.06	-29																									3.9618		11.6378												K					1.8																																																																																																SrAs,Co2As,Fe2As		(powder mixture) - (welded in Ta container) - (sealed in quartz) - heat(900C,16h)					Superconductivity in SrFe2-xCoxAs2: Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.2223	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
150755	MAT8082026	P-induced SC. R not to zero at P=2.0 GPa, T=1.8 K. Pcrit = 2.0 GPa. SC properties at P=2.16 GPa. SDW-temperature = 180 K.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2008								20																				ThCr2Si2																		K			29.5		0		29.5	MTC150755																												T/K		0.368																																								mOhm.cm											1.6														Bridgman method					Possible re-entrant superconductivity in EuFe2As2 under pressure			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0808.2026:PRB079212509	C. F. Miclea,M. Nicklas,H. S. Jeevan,D. Kasinathan,Z.Hossain,H. Rosner,P. Gegenwart,C. Geibel,F. Steglich		
150800	NAS0741334	Tc was measured for MRh4B4 + 2[RhB] material. structure type not clear.	TmRh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1977																										AB4C4		RT4B4																		K	9.73	9.86					9.86																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150801	NAS0741334	Tc was measured for MRh4B4 + 2[RhB] material. structure type not clear.	LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																			1977																										AB4C4		RT4B4																		K	11.54	11.76					11.76																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150802	NAS0741334	Tc was measured for MRh4B4 + 2[RhB] material. structure type not clear.	(Lu,Th)Rh4B4	Lu0.75Th0.25Rh4B4	Lu	0.75	Th	0.25	Rh	4	B	4																	1977																										AB4C4		RT4B4																		K	11.3	11.93					11.93																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150803	NAS0741334	Tc was measured for MRh4B4 + 2[RhB] material. structure type not clear.	(Sc,Th)Rh4B4	Sc0.75Th0.25Rh4B4	Sc	0.75	Th	0.25	Rh	4	B	4																	1977																										AB4C4		RT4B4																		K	8.49	8.74					8.74																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150804	NAS0741334	Tc was measured for MRh4B4 + 2[RhB] material. structure type not clear.	ThRh4B4	Th1Rh4B4	Th	1	Rh	4	B	4																			1977																										AB4C4		RT4B4																		K	4.29	4.34					4.34																																																																																																					High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150805	NAS0741334	structure type not clear.	GdRh4B4	Gd1Rh4B4	Gd	1	Rh	4	B	4																			1977							5.62																			AB4C4		RT4B4																		K					1																																																																																																							High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150806	NAS0741334	structure type not clear.	TbRh4B4	Tb1Rh4B4	Tb	1	Rh	4	B	4																			1977							7.08																			AB4C4		RT4B4																		K					1																																																																																																							High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150807	NAS0741334	structure type not clear.	DyRh4B4	Dy1Rh4B4	Dy	1	Rh	4	B	4																			1977							12.03																			AB4C4		RT4B4																		K					1																																																																																																							High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150808	NAS0741334	structure type not clear.	HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1977							6.56																			AB4C4		RT4B4																		K					1																																																																																																							High superconducting transition temperatures of new rare earth ternary borides			Bell Laboratories, Murray Hill,New Jersey	Proc.Natl.Acad.Sci.USA, 74(1977)1334	Bernd T.Matthias,E.Corenzwit,J.M.Vandenberg,H.E.Barz		
150809	IOC0082690	Tc measured by self-inductance and resistivity.	NbPS	Nb1P1S1	Nb	1	P	1	S	1																		3	1969																												NbPS	Immm		A	3.438	11.88	4.725												K		12.5					12.5																																																																																																high pressure synthesis (1200C, 65 kbar) using excess P.					The Synthesis, Crystal Structure, and Superconducting Properties of Niobium Phosphorus Sulfide, Niobium Phosphorus Selenide, and Tantalum Phosphorus Sulfide				Inorg.Chem., 8(1969)2690	P.C.Donohue,P.E.Bierstedt		
150810	IOC0082690		NbPSe	Nb1P1Se1	Nb	1	P	1	Se	1																		3	1969																												NbPS	Immm		A	3.462	12.33	4.821												K					1.25																																																																																																		high pressure synthesis (1200C, 65 kbar) using excess P.					The Synthesis, Crystal Structure, and Superconducting Properties of Niobium Phosphorus Sulfide, Niobium Phosphorus Selenide, and Tantalum Phosphorus Sulfide				Inorg.Chem., 8(1969)2690	P.C.Donohue,P.E.Bierstedt		
150811	IOC0082690		TaPS	Ta1P1S1	Ta	1	P	1	S	1																		1	1969																												NbPS	Immm		A	3.43	11.85	4.728												K					1.25																																																																																																		high pressure synthesis (1200C, 65 kbar) using excess P.					The Synthesis, Crystal Structure, and Superconducting Properties of Niobium Phosphorus Sulfide, Niobium Phosphorus Selenide, and Tantalum Phosphorus Sulfide				Inorg.Chem., 8(1969)2690	P.C.Donohue,P.E.Bierstedt		
150812	BUL0070215		NbRuSi	Nb1Ru1Si1	Nb	1	Ru	1	Si	1																			1985																												TiFeSi			A	7.123	11.413	6.535												K		2.65					2.65																																																																		uV/K	-4.3																													arc-melting, then ANN(900C, 7-10d, in vac)					Structure and superconductivity studies on ternary equiatomic silisides, MM'Si			Indian Institute of Technology, Madras, India	Bull.Mater.Sci.(India), 7(1985)215	G.V.Subba Rao,K.Wagner,Geetha Balakrishnan,J.Janaki,W.Paulus,R.Schollhorn,V.S.Subramanian,U.Poppe		
150813	BUL0070215		TaRuSi	Ta1Ru1Si1	Ta	1	Ru	1	Si	1																			1985																												TiFeSi			A	7.222	11.111	6.482												K		3.15					3.15																																																																		uV/K	-7.5				mOhm.cm											3.3														arc-melting, then ANN(900C, 7-10d, in vac)					Structure and superconductivity studies on ternary equiatomic silisides, MM'Si			Indian Institute of Technology, Madras, India	Bull.Mater.Sci.(India), 7(1985)215	G.V.Subba Rao,K.Wagner,Geetha Balakrishnan,J.Janaki,W.Paulus,R.Schollhorn,V.S.Subramanian,U.Poppe		
150814	BUL0070215		NbReSi	Nb1Re1Si1	Nb	1	Re	1	Si	1																			1985																												TiFeSi			A	7.07	11.442	6.606												K		5.1					5.1																																																																																																arc-melting, then ANN(900C, 7-10d, in vac)					Structure and superconductivity studies on ternary equiatomic silisides, MM'Si			Indian Institute of Technology, Madras, India	Bull.Mater.Sci.(India), 7(1985)215	G.V.Subba Rao,K.Wagner,Geetha Balakrishnan,J.Janaki,W.Paulus,R.Schollhorn,V.S.Subramanian,U.Poppe		
150815	BUL0070215		TaReSi	Ta1Re1Si1	Ta	1	Re	1	Si	1																			1985																												TiFeSi			A	7.002	11.614	6.605												K		4.4					4.4																																																																																																arc-melting, then ANN(900C, 7-10d, in vac)					Structure and superconductivity studies on ternary equiatomic silisides, MM'Si			Indian Institute of Technology, Madras, India	Bull.Mater.Sci.(India), 7(1985)215	G.V.Subba Rao,K.Wagner,Geetha Balakrishnan,J.Janaki,W.Paulus,R.Schollhorn,V.S.Subramanian,U.Poppe		
150816	JP01011179	P-induced SC.  Tc at P=51 GPa. molecular metal. metallic for P > 35 GPa. Tc decreases as increasing P upto 78 GPa.	C6I4O2	C6I4O2	C	6	I	4																	O	2			1998																																														K		0.8	2.5		0		0.8																																																																																																					Observation of pressure-induced superconductivity in the megabar region			Faculty of Engineering Science, Osaka University, Toyonaka, Osaka, Japan	J.Phys.:Condens.Matter, 10(1998)11179	K.Amaya,K.Shimizu,M.I.Eremets,S.Endo,T.C.Kobayashi		
150817	JPS0653400	P-induced SC.  sample recrystalizes at about 60 GPa. SC properties are at P=64 GPa. Tc(P=35 GPa) = 1.32 K for amorphous phase.	SnI4	I4Sn1	I	4	Sn	1																					1996																																														K		1.96			0		1.96	MTC150817																			T		1.7																																																																															Pressure-induced superconductivity of SnI4			Osaka University,Osaka,Japan	J.Phys.Soc.Jpn, 65(1996)3400	N.Takeshita,S.Kometani,K.Shimizu,K.Amaya,N.Hamaya,S.Endo		
150818	ZPS1950228	Sn(II) - Sn(III) transition at P=113 kbar.	Sn(III)	Sn1	Sn	1																							1966																																														K		5.3					5.3	MTC150818		K/GPa	-0.1																																																																																																	Die Supraleitung von Zinn und Blei unter sehr hohem Druck				Z.Phys., 195(1966)228	Jorg Wittig		
150819	ZPS1950228	Pb(I) - Pb(II) transition at P=160 kbar.	Pb	Pb1	Pb	1																							1966																																														K		7.2					7.2	MTC150819		K/GPa	-0.48																																																																																																	Die Supraleitung von Zinn und Blei unter sehr hohem Druck				Z.Phys., 195(1966)228	Jorg Wittig		
150820	ZPS1950228	P-induced SC. Tc and (dTc/dP) shows at P=81 kbar.	Bi(V)	Bi1	Bi	1																							1966																																														K		8.3			0		8.3			K/GPa	-0.18																																																																																																	Die Supraleitung von Zinn und Blei unter sehr hohem Druck				Z.Phys., 195(1966)228	Jorg Wittig		
150821	JET0121082	P-induced SC. Tc at P=25.3 kbar.	Bi(II)	Bi1	Bi	1																							1961																																														K		3.93			0		3.93			K/GPa	-0.345																																																																																																	Superconductivity of crystalline modifications of bismuth				JETP, 12(1961)1082	N.B.Brandt,N.I.Ginzburg		
150822	JET0121082	P-induced SC. Tc at P=26.3 kbar. Bi(III) for 25.3 < P < 29.4.	Bi(III)	Bi1	Bi	1																							1961																																														K		7.25			0		7.25			K/GPa	0																																																																																																	Superconductivity of crystalline modifications of bismuth				JETP, 12(1961)1082	N.B.Brandt,N.I.Ginzburg		
150823	PLA0180228	P-induced SC. Tc and Hc measured at P=37 kbar.	Bi(III)	Bi1	Bi	1																							1965																																														K		6.55			0		6.55																				kOe														MHC150823																																																																			Critical fields of superconducting bismuth at high pressure			U.S.Naval Research Laboratory, Washington,D.C.	Phys.Lett., 18(1965)228	E.M.Compy		
150824	L101077001	Tc is for <16>O. Tc(<18>O) = 90.99 K. oz(<18>O) = 6.953. spin glass temp: Tg(<16>O = .	YBa2Cu3O7	Y1Ba2Cu3O6.951	Y	1	Ba	2	Cu	3															O	7-z	6.951	1	2008																												Y123																		K				91.19			91.19						0.018	O	80	0.2																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150825	L101077001	Tc is for <16>O. Tc(<18>O) = 73.27 K.	(Y,Pr)Ba2Cu3O7	Y0.8Pr0.2Ba2Cu3O7-z	Y	0.8	Pr	0.2	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K				74.07			74.07						0.086	O	80	0.8																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150826	L101077001	Tc is for <16>O. Tc(<18>O) = 56.79 K. spin glass temp: Tg(<16>O) = 1.13 K. Tg(<18>O) = 1.66 K. Tg  exponent: alpha-Tg = -3.8.	(Y,Pr)Ba2Cu3O7	Y0.7Pr0.3Ba2Cu3O7-z	Y	0.7	Pr	0.3	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K				57.97			57.97	PH150826					0.163	O	80	1.18																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150827	L101077001	Tc is for <16>O. Tc(<18>O) = 43.25 K. oz(<18>O) = 6.934. spin glass temp: Tg(<16>O) = 7.07 K. Tg(<18>O) = 7.56 K. Tg  exponent: alpha-Tg = -0.55.	(Y,Pr)Ba2Cu3O7	Y0.6Pr0.4Ba2Cu3O6.929	Y	0.6	Pr	0.4	Ba	2	Cu	3													O	7-z	6.929	1	2008																												Y123																		K				44.8			44.8						0.277	O	80	1.55																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150828	L101077001	Tc is for <16>O. Tc(<18>O) = 35.12 K. . spin glass temp: Tg(<16>O) = 15.54 K . Tg(<18>O) = 16.58 K. Tg  exponent: alpha-Tg = -0.54.	(Y,Pr)Ba2Cu3O7	Y0.55Pr0.45Ba2Cu3O7-z	Y	0.55	Pr	0.45	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K				36.5			36.5						0.302	O	80	1.38																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150829	L101077001	Tc is for <16>O. Tc(<18>O) = 20.16 K. . spin glass temp: Tg(<16>O) = 17.82 K. Tg(<18>O) = 18.46 K . Tg  exponent: alpha-Tg = -0.29.	(Y,Pr)Ba2Cu3O7	Y0.5Pr0.5Ba2Cu3O7-z	Y	0.5	Pr	0.5	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K				23.12			23.12						1.024	O	80	2.96																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150830	L101077001	Tc is for <16>O. Tc(<18>O) <1.7 K. oz(<18>O) = 6.954. spin glass temp: Tg(<16>O) = 21.05 K. Tg(<18>O) = 21.65 K. Tg  exponent: alpha-Tg = -0.23.	(Y,Pr)Ba2Cu3O7	Y0.45Pr0.55Ba2Cu3O6.953	Y	0.45	Pr	0.55	Ba	2	Cu	3													O	7-z	6.953	1	2008																												Y123																		K				14.4			14.4						7	O	80	14.4																																																																																						1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150831	L101077001	spin glass temp: Tg(<16>O) = 22.8 K. Tg(<18>O) = 23.2 K. Tg  exponent: alpha-Tg = -0.13.	(Y,Pr)Ba2Cu3O7	Y0.42Pr0.58Ba2Cu3O7-z	Y	0.42	Pr	0.58	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K					1.7																																																																																																	1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150832	L101077001	spin glass temp: Tg(<16>O) = 32.4 K. Tg(<18>O) = 34.4 K. Tg  exponent: alpha-Tg = -0.52.	(Y,Pr)Ba2Cu3O7	Y0.35Pr0.65Ba2Cu3O7-z	Y	0.35	Pr	0.65	Ba	2	Cu	3													O	7-z		1	2008																												Y123																		K					1.7																																																																																																	1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150833	L101077001	oz(<18>O) = 6.957. Tn(<18>O) = 116.8 K. Tn exponent: alpha-Tn = -1.30.	(Y,Pr)Ba2Cu3O7	Y0.3Pr0.7Ba2Cu3O6.946	Y	0.3	Pr	0.7	Ba	2	Cu	3													O	7-z	6.946	1	2008								100.5																				Y123																		K					1.7																																																																																																	1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150834	L101077001	Tn(<18>O) = 212.6 K. Tn exponent: alpha-Tn = -0.09.	(Y,Pr)Ba2Cu3O7	Y0.2Pr0.8Ba2Cu3O7-z	Y	0.2	Pr	0.8	Ba	2	Cu	3													O	7-z		1	2008								210.2																				Y123																		K					1.7																																																																																																	1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150835	L101077001	oz(<18>O) = 6.949. Tn(<18>O) = 282.5 K. Tn exponent: alpha-Tn = 0.02.	PrBa2Cu3O7	Pr1Ba2Cu3O6.953	Pr	1	Ba	2	Cu	3															O	7-z	6.953	1	2008								283.2																				Y123																		K					1.7																																																																																																	1	standard solid state reaction. <18>O content determined from the sample weight.					Oxygen Isotope Effects on the Superconducting Transition and Magnetic States Within the Phase Diagram of Y1-xPrxBa2Cu3O7-z			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.Lett., 101(2008)077001	R. Khasanov,A. Shengelaya,D. Di Castro,E. Morenzoni,A. Maisuradze,I. M. Savic,K. Conder,E. Pomjakushina,A. Bussmann-Holder,H. Keller		
150836	P078012505	Tc defined as inflection point in R-T curve. Tc(max) = 25.6 K at P=1.0 GPa.	Sm(O,F)FeAs	Sm1Fe1As1F0.13O0.87	Sm	1	Fe	1	As	1	F	0.13													O	0.87	0.87		2008																												oxypnictide																	ZrCuSiAs-type	K		24.7					24.7			K/GPa	0.9																																																																																																	Effect of pressure on the superconducting and spin-density-wave states of SmFeAsO1-xFx			Department of Physics and TCSUH, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)012505	B. Lorenz,K. Sasmal,R. P. Chaudhury,X. H. Chen,R. H. Liu,T. Wu,C. W. Chu		
150837	P078012505	Tc defined as inflection point in R-T curve. Tc(1.6 GPa) = 40 K	Sm(O,F)FeAs	Sm1Fe1As1F0.3O0.7	Sm	1	Fe	1	As	1	F	0.3													O	0.7	0.7		2008																												oxypnictide																	ZrCuSiAs-type	K		43.5					43.5			K/GPa	-2.3																																																																																																	Effect of pressure on the superconducting and spin-density-wave states of SmFeAsO1-xFx			Department of Physics and TCSUH, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)012505	B. Lorenz,K. Sasmal,R. P. Chaudhury,X. H. Chen,R. H. Liu,T. Wu,C. W. Chu		
150838	NAT4530376	Tc(max) = 43 K at P=4 GPa. (dTc/dP) = 6.5 K/GPa for 0 < P < 4 GPa and (dTc/dP) = -1.38 K/GPa for 4 < P .	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89	0.89		2008																												oxypnictide																	ZrCuSiAs-type	K		27.9					27.9	TC150838		K/GPa	6.5																																																																																																	Superconductivity at 43 K in an iron-based layered compound LaO1-xFxFeAs			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Nature, 453(2008)376	Hiroki Takahashi,Kazumi Igawa,Kazunobu Arii,Yoichi Kamihara,Masahiro Hirano,Hideo Hosono		
150839	NAT4530376	R(min) at T=60 K.	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95	0.95		2008																												oxypnictide																	ZrCuSiAs-type	K		23.3	24.7				23.3	TC150839		K/GPa	2																																																																																																	Superconductivity at 43 K in an iron-based layered compound LaO1-xFxFeAs			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Nature, 453(2008)376	Hiroki Takahashi,Kazumi Igawa,Kazunobu Arii,Yoichi Kamihara,Masahiro Hirano,Hideo Hosono		
150840	NAT4530903	Figure shows Hc2//n (perpendicular to the plane)	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89	0.89	1	2008																												oxypnictide																	ZrCuSiAs-type	K	23	26	28				26																																		HC150840																																																																			Two-band superconductivity in LaFeAsO0.89F0.11 at very high magnetic fields			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Nature, 453(2008)903	F. Hunte,J. Jaroszynski,A. Gurevich,D. C. Larbalestier,R. Jin,A. S. Sefat,M. A. McGuire,B. C. Sales,D. K. Christen,D. Mandrus		
150841	P078024509	monoclinic, beta=89.96. lattice term(beta) in SP = 2.7 mJ/mol.K4.	Bi2Pd3S2	Bi2Pd3S2	Bi	2	Pd	3	S	2																		1	2008																											4		C2/m		A	11.751	8.303	11.74											Bi2Ni3S2-type.parkerite	K					0.35																																																										mJ/mol.K2	5.9	SP	170	SP																																				mixture - pellet - heat(1270K,12h, in evacuated quartz tube with carbon coated)					Transport properties in normal-metal Bi2Pd3S2 and superconducting Bi2Pd3Se2			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	Phys.Rev.B, 78(2008)024509	Takeshi Sakamoto,Makoto Wakeshima,Yukio Hinatsu,Kazuyuki Matsuhira		
150842	P078024509	not the same structure as Bi2Ni3S2-type. Tc(mid) = 0.81 K in SP transition. Hc(0) = 5.72 mTfrom SP. GL-parameter = 38.9. (dC/gamma*Tc) = 1.15. lattice term(beta) in SP = 4.0 mJ/mol.K4.	Bi2Pd3Se2	Bi2Pd3Se2	Bi	2	Pd	3	Se	2																		1	2008																																														K	0.9	0.96	1.1				0.96											Oe	from Hc(0) using GL theory	3.8							T	resistive, WHH	0.315							T/K		0.473			MHC150842	resistive	A	from Hc2	323			um	from Hc(0) using GL theory	1.259										MSP150842			mJ/mol.K2	8.3	SP	150	SP						uV/K	-6.05																													mixture - pellet - heat(1270K,12h, in evacuated quartz tube with carbon coated)					Transport properties in normal-metal Bi2Pd3S2 and superconducting Bi2Pd3Se2			Division of Chemistry, Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	Phys.Rev.B, 78(2008)024509	Takeshi Sakamoto,Makoto Wakeshima,Yukio Hinatsu,Kazuyuki Matsuhira		
150843	P078052504	T2 defined as midpoint in SP-jump. (dC/Tc) = 48.5 mJ/mol.K2, (dC/gamma*Tc) = 1.03.	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																		1	2008	emu/mol	-0.0001																										skutterudite			A	8.6835														K		5.03		4.98			5.03																				T	resistive, extraporation	2												MHC150843																						mJ/mol.K2	47.3	SP	215	SP																																				melting in glassy carbon crucible. ANN(800C(x=0), 700C(x=0.25, 0.75), 600C(x=1, 2), in sealed Ta tube in vac ampoule), Q to cold water					Optimization of the superconducting transition temperature of the filled skutterudite BaPt4Ge12 by gold substitution			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 78(2008)052504	R. Gumeniuk,H. Rosner,W. Schnelle,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150844	P078052504	T2 defined as midpoint in SP-jump.	Ba(Pt,Au)4Ge12	Ba1Pt3.75Au0.25Ge12	Ba	1	Pt	3.75	Au	0.25	Ge	12																1	2008	emu/mol	-0.00017																										skutterudite			A	8.6895														K				5.05			5.05																																																																																																melting in glassy carbon crucible. ANN(800C(x=0), 700C(x=0.25, 0.75), 600C(x=1, 2), in sealed Ta tube in vac ampoule), Q to cold water					Optimization of the superconducting transition temperature of the filled skutterudite BaPt4Ge12 by gold substitution			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 78(2008)052504	R. Gumeniuk,H. Rosner,W. Schnelle,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150845	P078052504	T2 defined as midpoint in SP-jump. (dC/Tc) = 55.0 mJ/mol.K2.	Ba(Pt,Au)4Ge12	Ba1Pt3.5Au0.5Ge12	Ba	1	Pt	3.5	Au	0.5	Ge	12																1	2008	emu/mol	-0.00013																										skutterudite			A	8.6943														K		5.19		5.27			5.19																																																								mJ/mol.K2	49.1	SP	218	SP																																				melting in glassy carbon crucible. ANN(800C(x=0), 700C(x=0.25, 0.75), 600C(x=1, 2), in sealed Ta tube in vac ampoule), Q to cold water					Optimization of the superconducting transition temperature of the filled skutterudite BaPt4Ge12 by gold substitution			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 78(2008)052504	R. Gumeniuk,H. Rosner,W. Schnelle,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150846	P078052504	T2 defined as midpoint in SP-jump. (dC/Tc) = 70.4 mJ/mol.K2.	Ba(Pt,Au)4Ge12	Ba1Pt3.25Au0.75Ge12	Ba	1	Pt	3.25	Au	0.75	Ge	12																1	2008	emu/mol	-0.00003																										skutterudite			A	8.6985														K		6.25		6.27			6.25																																																								mJ/mol.K2	48.1	SP	217	SP																																				melting in glassy carbon crucible. ANN(800C(x=0), 700C(x=0.25, 0.75), 600C(x=1, 2), in sealed Ta tube in vac ampoule), Q to cold water					Optimization of the superconducting transition temperature of the filled skutterudite BaPt4Ge12 by gold substitution			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 78(2008)052504	R. Gumeniuk,H. Rosner,W. Schnelle,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150847	P078052504	T2 defined as midpoint in SP-jump. (dC/Tc) = 77.0 mJ/mol.K2, (dC/gamma*Tc) = 1.37.	Ba(Pt,Au)4Ge12	Ba1Pt3Au1Ge12	Ba	1	Pt	3	Au	1	Ge	12																1	2008	emu/mol	0.00001																										skutterudite			A	8.7124														K		7		7			7																				T	resistive, extraporation	2												MHC150847																						mJ/mol.K2	56.3	SP	224	SP																																				melting in glassy carbon crucible. ANN(800C(x=0), 700C(x=0.25, 0.75), 600C(x=1, 2), in sealed Ta tube in vac ampoule), Q to cold water					Optimization of the superconducting transition temperature of the filled skutterudite BaPt4Ge12 by gold substitution			Max-Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 78(2008)052504	R. Gumeniuk,H. Rosner,W. Schnelle,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
150848	P078012507	microwave surface impedance. RRR = 12.1. RESN = 0.2 mOhm(T=30 K). R shows T^2 dependence for T < 200K.	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																												oxypnictide																		K		23.7		22			23.7																				T	resistive, WHH	56							T/K	resistive	2.5																																								mOhm.cm							0.2																		solid state reaction, ANN in vac.					Upper critical field, penetration depth, and depinning frequency of the high-temperature superconductor LaFeAsO0.9F0.1 studied by microwave surface impedance			Institute for Solid State Research, IFW Dresden, D-01101 Dresden, Germany	Phys.Rev.B, 78(2008)012507	A. Narduzzo,M. S. Grbic,M. Pozek,A. Dulcic,D. Paar,A. Kondrat,C. Hess,I. Hellmann,R. Klingeler,J. Werner,A. Kohler,G. Behr,B. Buchner		
150849	P078014507	R(min) at T=85 K. tetra(H) to ortho(L) phase transition. not SC. lattice term of SP (beta) = 0.60 mJ/mol.K4.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																			2008																															A	3.9436		13.115												K					1.8																																																										mJ/mol.K2	37	SP	250	SP																																				Sn-flux method. (Ba,K)Fe2As2:Sn = 1:48 in MgO crucible..					Anisotropic thermodynamic and transport properties of single-crystalline Ba1-xKxFe2As2 (x=0 and 0.45)			Ames Laboratory US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)014507	N. Ni,S. L. Bud'ko,A. Kreyssig,S. Nandi,G. E. Rustan,A. I. Goldman,S. Gupta,J. D. Corbett,A. Kracher,P. C. Canfield		
150850	P078014507	K-content by wave length dispersive x-ray spectroscopy(WDS). lattice term of SP: beta=0.83 mJ/mol.K4.	(Ba,K)Fe2As2	Ba0.55K0.45Fe2As2	Ba	0.55	K	0.45	Fe	2	As	2																3	2008																															A	3.9186		13.256												K		29.5	30				29.5										50																								MHC150850	resistive																					mJ/mol.K2	23	SP	230	SP																																				Sn-flux method. (Ba,K)Fe2As2:Sn = 1:48 in MgO crucible..					Anisotropic thermodynamic and transport properties of single-crystalline Ba1-xKxFe2As2 (x=0 and 0.45)			Ames Laboratory US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)014507	N. Ni,S. L. Bud'ko,A. Kreyssig,S. Nandi,G. E. Rustan,A. I. Goldman,S. Gupta,J. D. Corbett,A. Kracher,P. C. Canfield		
150851	L101057007	Hc2 using pulse field(upto 55 T). [gapene]=3.5-4.2 by far-infrared reflectance.	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																												oxypnictide	P4/nmm		A	4.024		8.717											ZrCuSiAs-type	K			26				26																				T	resistive,TDO frequency													HC150851	resistive,TDO frequency													3.5	2																																													LaAs,Fe2O3,Fe,LaF3		mixture - pellet - Ta crucible in quartz tube(Ar). ANN(1150C,50h)					Superconducting Properties of the Fe-Based Layered Superconductor LaFeAsO0.9F0.1-z			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.Lett., 101(2008)057007	G. F. Chen,Z. Li,G. Li,J. Zhou,D. Wu,J. Dong,W. Z. Hu,P. Zheng,Z. J. Chen,H. Q. Yuan,J. Singleton,J. L. Luo,N. L. Wang		
150852	L101057006	P-induced SC. Pcrit = 2 kbar. Tc(max) = 12 K at P=3.5 kbar. Hc2(T) at P=3.5 and 5.0 kbar.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2008																																														K		12			0		12	MTC150852																																	MHC150852	resistive																																																													Sn-flux method					Pressure Induced Superconductivity in CaFe2As2			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 101(2008)057006	Milton S. Torikachvili,Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
150853	P078020512		LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2008																												oxypnictide																	ZrCuSiAs-type	K																																																															mJ/mol.K2	1.6	SP																																				LaAs,FeAs,Fe2As,La,LaF3,La2O3		solid state reaction					Ferromagnetic spin fluctuation in LaFeAsO1-xFx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)020512	Yoshimitsu Kohama,Yoichi Kamihara,Masahiro Hirano,Hitoshi Kawaji,Tooru Atake,Hideo Hosono		
150854	P078020512		La(O,F)FeAs	La1Fe1As1F0.025O0.975	La	1	Fe	1	As	1	F	0.025													O	0.975			2008																												oxypnictide																	ZrCuSiAs-type	K																																																															mJ/mol.K2	3.2	SP																																				LaAs,FeAs,Fe2As,La,LaF3,La2O3		solid state reaction					Ferromagnetic spin fluctuation in LaFeAsO1-xFx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)020512	Yoshimitsu Kohama,Yoichi Kamihara,Masahiro Hirano,Hitoshi Kawaji,Tooru Atake,Hideo Hosono		
150855	P078020512		La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95			2008																												oxypnictide																	ZrCuSiAs-type	K		20.5					20.5																																																								mJ/mol.K2	8.4	SP	319	SP																																		LaAs,FeAs,Fe2As,La,LaF3,La2O3		solid state reaction					Ferromagnetic spin fluctuation in LaFeAsO1-xFx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)020512	Yoshimitsu Kohama,Yoichi Kamihara,Masahiro Hirano,Hitoshi Kawaji,Tooru Atake,Hideo Hosono		
150856	P078020512		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2008																												oxypnictide																	ZrCuSiAs-type	K		21.1					21.1																																																								mJ/mol.K2	5.1	SP	308	SP																																		LaAs,FeAs,Fe2As,La,LaF3,La2O3		solid state reaction					Ferromagnetic spin fluctuation in LaFeAsO1-xFx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)020512	Yoshimitsu Kohama,Yoichi Kamihara,Masahiro Hirano,Hitoshi Kawaji,Tooru Atake,Hideo Hosono		
150857	P078020512		La(O,F)FeAs	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86			2008																												oxypnictide																	ZrCuSiAs-type	K																																																															mJ/mol.K2	3.8	SP	332	SP																																		LaAs,FeAs,Fe2As,La,LaF3,La2O3		solid state reaction					Ferromagnetic spin fluctuation in LaFeAsO1-xFx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)020512	Yoshimitsu Kohama,Yoichi Kamihara,Masahiro Hirano,Hitoshi Kawaji,Tooru Atake,Hideo Hosono		
150858	P078024514	two gaps((2d/kTc)=3.72, =1.08) were obtained from fitting of supercurrent density.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2008																												Sc2Fe3Si5																		K		6					6																																		MHC150858							um	tunnel diode resonator		0.2	0.2			3.72	1																																															floating zone method					Two-gap superconductivity seen in penetration-depth measurements of Lu2Fe3Si5 single crystals			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)024514	R. T. Gordon,M. D. Vannette,C. Martin,Y. Nakajima,T. Tamegai,R. Prozorov		
150859	P078024517	three phases(3C-SiC(main phase), 6H-SiC, Si). RRR=10.0. GL parameter = 0.35. beta(lattice term of SP) = 0.0193 mJ/mol.K4.type-I SC(Hc2 = Hc)	B-doped SiC	C1Si1	C	1	Si	1																					2008																																														K				1.45			1.45																				Oe		115														A		3600			A		130										MSP150859			mJ/mol.K2	0.294	SP	590	SP											uOhm.cm							60														E+21 /cm3	1.91	beta-SiC,Si,a-B		starting mixture: SiC:B:Si = 4:1.15:1. solid state reaction. SIN(1600C,12h, in flowing Ar/H2 gas (60/60 ml/min)					Specific heat and electronic states of superconducting boron-doped silicon carbide			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 78(2008)024517	M. Kriener,Y. Maeno,T. Oguchi,Z.-A. Ren,J. Kato,T. Muranaka,J. Akimitsu		
150860	J076103710	RRR = 10. carrier by Hall effect measurements. three phases(3C-SiC(main phase), 6H-SiC, Si) were included. Hc determined for S to N transition.	B-doped SiC	C1Si1	C	1	Si	1																					2007																															A	4.3575														K				1.45			1.45																				Oe	ac-SUS	110												MHC150860																																																										E+21 /cm3	1.91	beta-SiC,Si,a-B		starting mixture: SiC:B:Si = 4:1.15:1. solid state reaction. SIN(1600C,12h, in flowing Ar/H2 gas (60/60 ml/min)					Superconductivity in Boron-doped SiC			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)103710	Zhi-An REN,Junya KATO,Takahiro MURANAKA,Jun AKIMITSU,Markus KRIENER,Yoshiteru MAENO		
150861	NAT4440465	non-uniform distribution of B. Hc2 defined as 0.1Rn. RRR=1.2.	B-doped Si	Si1	Si	1																							2006																																														K		0.34	0.4				0.34																				T	resistive	0.4												MHC150861																																					uOhm.cm							130				160										E+21 /cm3	2.8			samples prepared by gas immersion layer doping: precursor gas(BCl3) chemisorbed on a (001) Si-wafer.					Superconductivity in doped cubic silicon			Laboratoire dEtudes des Proprietes Electroniques des Solides, CNRS, BP166, 38042 Grenoble, France	Nature, 444(2006)465	E. Bustarret,C. Marcenat,P. Achatz,J. Kacmarcik,F. Levy,A. Huxley,L. Ortega,E. Bourgeois,X. Blase,D. Debarre,J. Boulmer		
150862	P078060505		LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		1	2008																												PbFCl	P4/nmm	129	A	3.7914		6.3639												K				18			18																																		MHC150862																																				MTP150862																								Li,Fe,As		stoichiometric amount - sealed in Nb tube(Ar) - heat(740C,24h) - cool to RT (1d)					LiFeAs: An intrinsic FeAs-based superconductor with Tc=18 K			TCSUH and Department of Chemistry, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)060505	Joshua H. Tapp,Zhongjia Tang,Bing Lv,Kalyan Sasmal,Bernd Lorenz,Paul C. W. Chu,Arnold M. Guloy		
150863	P078064506	Tc drop around 9 GPa comes from lattice sotening.	CaC6	C6Ca1	C	6	Ca	1																					2008																												GIC			A	4.33		13.57							A/GPa	-0.0038		-0.081		K		11.6					11.6	MLAT150863																																																																																																				Maximum Tc at the verge of a simultaneous order-disorder and lattice-softening transition in superconducting CaC6			Institut de Mineralogie et de Physique des Milieux Condenses, Universite Pierre et Marie Curie Paris VI and CNRS, 75005 Paris, France	Phys.Rev.B, 78(2008)060506	A. Gauzzi,N. Bendiab,M. d'Astuto,B. Canny,M. Calandra,F. Mauri,G. Loupias,N. Emery,C. Herold,P. Lagrange,M. Hanfland,M. Mezouar		
150864	P078064510	Tc by ac-SUS. <123>Sb-NQR measured.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2008																												skutterudite																		K		1.87					1.87	MTC150864		K/GPa	-0.17																																																																																												Sb-flux method					<123>Sb-NQR study of unconventional superconductivity in the filled skutterudite heavy-fermion compound PrOs4Sb12 under high pressure up to 3.82 GPa			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 78(2008)064510	S. Kawasaki,K. Katayama,H. Sugawara,D. Kikuchi,H. Sato,Guo-qing Zheng		
150865	P078064511		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2008																												oxypnictide																		K	23	25	28				25																																		HC150865																																																			E-3 cm3/C	-3.774					RH150865					solid state reaction					Comparative high-field magnetotransport of the oxypnictide superconductors RFeAsO1-xFx (R=La, Nd) and SmFeAsO1-z			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 78(2008)064511	J. Jaroszynski,Scott C. Riggs,F. Hunte,A. Gurevich,D. C. Larbalestier,G. S. Boebinger,F. F. Balakirev,Albert Migliori,Z. A. Ren,W. Lu,J. Yang,X. L. Shen,X. L. Dong,Z. X. Zhao,R. Jin,A. S. Sefat,M. A. McGuire,B. C. Sales,D. K. Christen,D. Mandrus		
150866	P078064511		Nd(O,F)FeAs	Nd1Fe1As1F0.06O0.94	Nd	1	Fe	1	As	1	F	0.06													O	0.94		1	2008																												oxypnictide																		K	46	47.5	50.5				47.5																																		HC150866																																																			E-3 cm3/C	-1.253					RH150866					solid state reaction					Comparative high-field magnetotransport of the oxypnictide superconductors RFeAsO1-xFx (R=La, Nd) and SmFeAsO1-z			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 78(2008)064511	J. Jaroszynski,Scott C. Riggs,F. Hunte,A. Gurevich,D. C. Larbalestier,G. S. Boebinger,F. F. Balakirev,Albert Migliori,Z. A. Ren,W. Lu,J. Yang,X. L. Shen,X. L. Dong,Z. X. Zhao,R. Jin,A. S. Sefat,M. A. McGuire,B. C. Sales,D. K. Christen,D. Mandrus		
150867	P078064511		SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide																		K	51	52	53.5				52																																		HC150867																																																			E-3 cm3/C	-0.705					RH150867					solid state reaction					Comparative high-field magnetotransport of the oxypnictide superconductors RFeAsO1-xFx (R=La, Nd) and SmFeAsO1-z			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 78(2008)064511	J. Jaroszynski,Scott C. Riggs,F. Hunte,A. Gurevich,D. C. Larbalestier,G. S. Boebinger,F. F. Balakirev,Albert Migliori,Z. A. Ren,W. Lu,J. Yang,X. L. Shen,X. L. Dong,Z. X. Zhao,R. Jin,A. S. Sefat,M. A. McGuire,B. C. Sales,D. K. Christen,D. Mandrus		
150868	ZFP2080142		V	V1	V	1																							1968																																														K		5.16					5.16	MTC150868		K/GPa	0.176																																																																																																	Superleitung von Vanadium, Niob und Tantal unter hohem Druck				Z.Physik, 208(1968)142	D.Kohnlein		
150869	ZFP2080142		Nb	Nb1	Nb	1																							1968																																														K		9.4					9.4	MTC150869		K/GPa	0.12																																																																																																	Superleitung von Vanadium, Niob und Tantal unter hohem Druck				Z.Physik, 208(1968)142	D.Kohnlein		
150870	ZFP2080142		Ta	Ta1	Ta	1																							1968																																														K		4.43					4.43	MTC150870		K/GPa	-0.26																																																																																																	Superleitung von Vanadium, Niob und Tantal unter hohem Druck				Z.Physik, 208(1968)142	D.Kohnlein		
150871	JET0340342		Sn1-xBix	Bi0.1Sn0.9	Bi	0.1	Sn	0.9																					1972																																														K		6.5					6.5																				T					0.23			4.2																																																																				melt in pyrex ampoule - ANN(373K,100h,in vac)					Superconductivity of Bi-Sn alloys under high pressure			Institute of Chemical Physics, USSR Academy of Science	Sov.Phys.JETP, 34(1972)342	A.G.Rabin'kin,V.N.Laukhin		
150872	JET0340342		Sn1-xBix	Bi0.8Sn0.2	Bi	0.8	Sn	0.2																					1972																																														K		7.3					7.3																				T					0.7			4.2																																																																				melt in pyrex ampoule - ANN(373K,100h,in vac)					Superconductivity of Bi-Sn alloys under high pressure			Institute of Chemical Physics, USSR Academy of Science	Sov.Phys.JETP, 34(1972)342	A.G.Rabin'kin,V.N.Laukhin		
150873	USP0080202		Ta	Ta1	Ta	1																							1965																																														K		4.31					4.31	MTC150873		K/GPa	-0.243																																																																																																	Effect of high pressure on the superconducting properties of metals				Sov.Phys.USP, 8(1965)202	N.B.Brandt,N.I.Ginsburg		
150874	USP0080202	(dTc/dP) shows  for 20 < P < 28 katm	Tl	Tl1	Tl	1																							1965																																														K		2.376					2.376	MTC150874		K/GPa	-0.142																																																																																																	Effect of high pressure on the superconducting properties of metals				Sov.Phys.USP, 8(1965)202	N.B.Brandt,N.I.Ginsburg		
150875	USP0080202		Cd	Cd1	Cd	1																							1965																																														K		0.52					0.52	MTC150875		K/GPa	-0.182																																																																																																	Effect of high pressure on the superconducting properties of metals				Sov.Phys.USP, 8(1965)202	N.B.Brandt,N.I.Ginsburg		
150876	JET0230838	(dTc/dP) =-0.171 K/GPa   for 20 < P < 26 katm	Zn	Zn1	Zn	1																							1966																																														K		0.867					0.867	MTC150876		K/GPa	-0.243																																																																																																	Pressure dependence of the superconducting transition temperature in Zinc				Sov.Phys.JETP, 23(1966)838	N.B.Brandt,N.I.Ginsburg		
150877	JAP0404457		Ti-Ta-Nb	Nb0.36Ti0.64	Nb	0.36	Ti	0.64																					1969																																														K		9.05					9.05																				T		8.51																																																																															Some superconducting properties of Ti-Nb-Ta ternary alloys				J.Appl.Phys., 40(1969)4457	M.Suenaga,K.M.Ralls		
150878	JAP0404457		Ti-Ta-Nb	Ti0.64Ta0.075Nb0.285	Ti	0.64	Ta	0.075	Nb	0.285																			1969																																														K		8.73					8.73	MTC150878																			T		11.9												MHC150878																																																																			Some superconducting properties of Ti-Nb-Ta ternary alloys				J.Appl.Phys., 40(1969)4457	M.Suenaga,K.M.Ralls		
150879	L101107004	s-wave SC.. [penet] = 2000 +- 80 A from infrared spectroscopy.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2008																												ThCr2Si2																		K		37					37																																									A	infrared	2000																																																					single crystals grown by FeAs flux method					Probing the Superconducting Energy Gap from Infrared Spectroscopy on a Ba0:6K0:4Fe2As2 Single Crystal with Tc = 37 K			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev,Lett., 101(2008)107004	G. Li,W. Z. Hu,J. Dong,Z. Li,P. Zheng,G. F. Chen,J. L. Luo,N. L. Wang		
150880	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.038	NbB2-x	B2Nb1	B	2	Nb	1																					2008																												AlB2			A	3.1103		3.2639												K					1																																																																																																		solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150881	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.184	NbB2-x	B2.2Nb1	B	2.2	Nb	1																					2008																												AlB2			A	3.1013		3.3051												K		9.01					9.01																																																																																																solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150882	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.405	NbB2-x	B2.4Nb1	B	2.4	Nb	1																					2008																												AlB2			A	3.1042		3.3202												K		9.96					9.96																																																																																																solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150883	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.626	NbB2-x	B2.6Nb1	B	2.6	Nb	1																					2008																												AlB2			A	3.10187		3.3195												K		10.9					10.9																																																																																																solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150884	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.614	NbB2-x	B2.8Nb1	B	2.8	Nb	1																					2008																												AlB2			A	3.10397		3.3172												K		9.96					9.96																																																																																																solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150885	SSC1470439	B/Nb ratio(by rietveld analysis) = 2.674	NbB2-x	B3Nb1	B	3	Nb	1																					2008																												AlB2			A	3.1025		3.3196												K		9.96					9.96																																																																																																solid state reaction. heat(1100C,20h, in Ar flow					Superconductivity of non-stoichiometric intermetallic compound NbB2			National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	Solid State Commun., 147(2008)439	Monika Mudgel,V.P.S. Awana,G.L. Bhall,H. Kishan		
150886	L101097011	infrared ellipsometry. [penet]c => 6 um. anisotropy => 30.	Nd(O,F)FeAs	Nd1Fe1As1F0.18O0.82	Nd	1	Fe	1	As	1	F	0.18													O	0.82		1	2008																												oxypnictide																	ZrCuSiAs-type	K		52					52																																									um	infrared	6																																																					solid state reaction					Superconducting Energy Gap and c-Axis Plasma Frequency of (Nd,Sm)FeAsO0.82F0.18 Superconductors from Infrared Ellipsometry			Department of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Chemin du Musee 3, CH-1700 Fribourg, Switzerland	Phys.Rev,Lett., 101(2008)097011	A. Dubroka,K.W. Kim,M. Rossle,V. K. Malik,A. J. Drew,R. H. Liu,G. Wu,X. H. Chen,C. Bernhard		
150887	L101097009	grain size = 1-100 um. [penet] from muon-SR. [ppenet] using [penet] = 1.31*[ppenet].	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																												oxypnictide			A	4.0245		8.7099											ZrCuSiAs-type	K			26				26																																									A	muon-SR	333	254																																																				two step solid state reaction, then annealed in vac.					Field and Temperature Dependence of the Superfluid Density in LaFeAsO1-xFx Superconductors: A Muon Spin Relaxation Study			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev,Lett., 101(2008)097009	H. Luetkens,H.-H. Klauss,R. Khasanov,A. Amato,R. Klingeler,I. Hellmann,N. Leps,A. Kondrat,C. Hess,A. Kohler,G. Behr,J. Werner,B. Buchner		
150888	L101097009	grain size = 1-100 um. [penet] from muon-SR. [ppenet] using [penet] = 1.31*[ppenet].	La(O,F)FeAs	La1Fe1As1F0.075O0.925	La	1	Fe	1	As	1	F	0.075													O	0.925		1	2008																												oxypnictide			A	4.0266		8.7123											ZrCuSiAs-type	K			22				22																																									A	muon-SR	364	364																																																				two step solid state reaction, then annealed in vac.					Field and Temperature Dependence of the Superfluid Density in LaFeAsO1-xFx Superconductors: A Muon Spin Relaxation Study			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev,Lett., 101(2008)097009	H. Luetkens,H.-H. Klauss,R. Khasanov,A. Amato,R. Klingeler,I. Hellmann,N. Leps,A. Kondrat,C. Hess,A. Kohler,G. Behr,J. Werner,B. Buchner		
150889	L101107007		KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																			2008																												ThCr2Si2	I4/mmm		A	3.8414		13.837												K		3.8					3.8																																																																																																AFe2As2(A=Sr,K,Cs) by heating (1000, 950, 700C, 20-24h). Then mixture(K/Sr, Cs/Sr) - press - ANN(900C, 20-30h, in Nb container)					Superconducting Fe-Based Compounds (A1-xSrx)Fe2As2 with A = K and Cs with Transition Temperatures up to 37 K			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev,Lett., 101(2008)107007	Kalyan Sasmal,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Feng Chen,Yu-Yi Xue,Ching-Wu Chu		
150890	L101107007	Hc2(0) defined as T1 = 153 T.	(K,Sr)Fe2As2	K0.4Sr0.6Fe2As2	K	0.4	Sr	0.6	Fe	2	As	2																	2008																												ThCr2Si2	I4/mmm																	K		36					36	MTC150890																			T	resistive, GL theory	190												MHC150890																																uV/K	23.9			MTP150890																										AFe2As2(A=Sr,K,Cs) by heating (1000, 950, 700C, 20-24h). Then mixture(K/Sr, Cs/Sr) - press - ANN(900C, 20-30h, in Nb container)					Superconducting Fe-Based Compounds (A1-xSrx)Fe2As2 with A = K and Cs with Transition Temperatures up to 37 K			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev,Lett., 101(2008)107007	Kalyan Sasmal,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Feng Chen,Yu-Yi Xue,Ching-Wu Chu		
150891	L101107007		CsFe2As2	Cs1Fe2As2	Cs	1	Fe	2	As	2																			2008																												ThCr2Si2	I4/mmm		A	3.8894		15.066												K		2.6					2.6																																																																																																AFe2As2(A=Sr,K,Cs) by heating (1000, 950, 700C, 20-24h). Then mixture(K/Sr, Cs/Sr) - press - ANN(900C, 20-30h, in Nb container)					Superconducting Fe-Based Compounds (A1-xSrx)Fe2As2 with A = K and Cs with Transition Temperatures up to 37 K			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev,Lett., 101(2008)107007	Kalyan Sasmal,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Feng Chen,Yu-Yi Xue,Ching-Wu Chu		
150892	L101107007	Hc2(0) defined as T1 = 110 T.	(Cs,Sr)Fe2As2	Cs0.4Sr0.6Fe2As2	Cs	0.4	Sr	0.6	Fe	2	As	2																	2008																												ThCr2Si2	I4/mmm																	K		36.6					36.6																				T	resistive, GL theory	140												MHC150892																																																														AFe2As2(A=Sr,K,Cs) by heating (1000, 950, 700C, 20-24h). Then mixture(K/Sr, Cs/Sr) - press - ANN(900C, 20-30h, in Nb container)					Superconducting Fe-Based Compounds (A1-xSrx)Fe2As2 with A = K and Cs with Transition Temperatures up to 37 K			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev,Lett., 101(2008)107007	Kalyan Sasmal,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Feng Chen,Yu-Yi Xue,Ching-Wu Chu		
150893	L101117004		BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2008																												ThCr2Si2	I4/mmm		A	3.9635		13.022												K					1.8																																																																									mOhm.cm							5				5.9														FeAs flux method					Superconductivity at 22 K in Co-Doped BaFe2As2 Crystals			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev,Lett., 101(2008)117004	Athena S. Sefat,Rongying Jin,Michael A. McGuire,Brian C. Sales,David J. Singh,David Mandrus		
150894	L101117004		Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2008																												ThCr2Si2	I4/mmm		A	3.9639		12.98												K			22			0.6	22																																																																																					E-3 cm3/C	-1.14				8	MRH150894	E+21/cm3	6			FeAs flux method					Superconductivity at 22 K in Co-Doped BaFe2As2 Crystals			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev,Lett., 101(2008)117004	Athena S. Sefat,Rongying Jin,Michael A. McGuire,Brian C. Sales,David J. Singh,David Mandrus		
150895	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.03Ta1S2	Cu	0.03	Ta	1	S	2																			2008																												TX2			A	3.3198		12.1166											2H-TaS2	K		3.79					3.79																																																								mJ/mol.K2	13.78	SP-heat																																											Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150896	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.04Ta1S2	Cu	0.04	Ta	1	S	2																			2008																												TX2			A	3.3195		12.1243											2H-TaS2	K		4.2					4.2																				T		4.2												MHC150896																						mJ/mol.K2	11.61	SP-heat	165	SP-heat						uV/K	-4.97			MTP150896																															Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150897	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.06Ta1S2	Cu	0.06	Ta	1	S	2																			2008																												TX2			A	3.3213		12.1509											2H-TaS2	K		4.16					4.16																																																								mJ/mol.K2	10.1	SP-heat																																											Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150898	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.08Ta1S2	Cu	0.08	Ta	1	S	2																			2008																												TX2			A	3.3219		12.1629											2H-TaS2	K		3.45					3.45																																																								mJ/mol.K2	8.69	SP-heat																																											Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150899	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.1Ta1S2	Cu	0.1	Ta	1	S	2																			2008																												TX2			A	3.3245		12.2074											2H-TaS2	K		2.71					2.71																																																								mJ/mol.K2	9.87	SP-heat																																											Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150900	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.12Ta1S2	Cu	0.12	Ta	1	S	2																			2008																												TX2			A	3.3195		12.2091											2H-TaS2	K		1.82					1.82																																																								mJ/mol.K2	7.54	SP-heat								uV/K	-5.59			MTP150900																															Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150901	P078104520	T<CDW> = 72 K	2H-TaS2	S2Ta1	S	2	Ta	1																					2008																												TX2			A	3.3216		12.102											2H-TaS2	K		0.8					0.8																																																								mJ/mol.K2	8.13									uV/K	-0.556			MTP150901																															Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150902	P078100503	[isotope] = 0.08, 0.085, 0.090, 0.094   for P=0, 0.5, 1.0, 1.5 GPa, respectively. (d[isotope]/dP) = 0.0094 /GPa.	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			2008																												Y124																		K		81.6					81.6	TC150902		K/GPa	5.4		0.0805	O	95																																																																																							1	solid state reaction(945C, in 60 bar O2) - ANN(760C,6h, in 0.95 bar (95%-<18>O2 atmosphere)					Pressure dependence of the oxygen isotope effect in the superconductor YBa2Cu4O8			MacDiarmid Institute, Industrial Research Ltd., P.O. Box 31310, Lower Hutt, New Zealand	Phys.Rev.B, 78(2008)100503	N. Suresh,J. G. Storey,G. V. M. Williams,J. L. Tallon		
150903	PHC1680482	[oz] from volumetric analysis. Tc(max) = 108 K at P=12 GPa. (dL/dP) from Physica C, 167(1990)335.	YBa2Cu4O8	Y1Ba2Cu4O7.986	Y	1	Ba	2	Cu	4															O	8	7.986		1990																												Y124																		K		79.2					79.2	TC150903		K/GPa	5																																																																																												mixture(YBa2Cu3O7 + CuO) - heat(980C,30h, in 21 MPa-O2) - slow cool to RT(5C/min)					SUPERCONDUCTIVITY AT 108 K IN YBA2CU4O8 AT PRESSURES UP TO 12GPA			DEPARTMENT OF PHYSICS AND ASTRONOMY OF THE FREE UNIVERSITY, 1081 HV AMSTERDAM, THE NETHERLANDS	PHYSICA C,186(1990)482	E.JILEK,E.KALDIS,E.N.VAN EENIGE,J.KARPINSKI,R.GRIESSEN,R.J.WIJNGAARDEN,S.RUSIECKI	Y,BA,CU,O	
150904	P078104505	at 4K, space-G = Cmma, a=5.6823, b=5.7103, c=8.7117 A	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2008																												oxypnictide	P4/nmm	129	A	4.0345		8.7387											ZrCuSiAs-type	K					1.8																																																																																																LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150905	P078104505	at 4K, space-G = P4/nmm, a=4.02771, c=8.6860 A.	LaO(Fe,Co)As	La1Fe0.95Co0.05As1O1	La	1	Fe	0.95	Co	0.05	As	1													O	1			2008																												oxypnictide																	ZrCuSiAs-type	K				11		3.2	11																																		HC150905																																																												LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150906	P078104505		LaO(Fe,Co)As	La1Fe0.89Co0.11As1O1	La	1	Fe	0.89	Co	0.11	As	1													O	1			2008																												oxypnictide	P4/nmm	129	A	4.0351		8.7132											ZrCuSiAs-type	K				14		2.3	14																																		HC150906																																uV/K	-50			TP150906																								LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150907	P078104505		LaO(Fe,Co)As	La1Fe0.85Co0.15As1O1	La	1	Fe	0.85	Co	0.15	As	1													O	1			2008																												oxypnictide																	ZrCuSiAs-type	K				6		3.9	6																																		HC150907																																																												LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150908	P078104505		LaO(Fe,Co)As	La1Fe0.8Co0.2As1O1	La	1	Fe	0.8	Co	0.2	As	1													O	1			2008																												oxypnictide																	ZrCuSiAs-type	K					1.8																																																										mJ/mol.K2	1.405	SP-heat	342																																			LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150909	P078104505		LaO(Fe,Co)As	La1Fe0.5Co0.5As1O1	La	1	Fe	0.5	Co	0.5	As	1													O	1			2008																												oxypnictide																	ZrCuSiAs-type	K					1.8			LAT150909																																																							mJ/mol.K2	1.68	SP-heat	342																																			LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150910	P078104505	effective moment = 1.4 myu-B/Co. Ferromagnetic Curie T = 57K from Arrott plot.	LaOCoAs	La1Co1As1O1	La	1	Co	1	As	1															O	1			2008	emu/mol	-0.000006			myu-B/Co	1.4	90																					oxypnictide																	ZrCuSiAs-type	K					1.8																																																										mJ/mol.K2	4.02	SP-heat	342																																			LaAs,Co3O4,Fe2O3,Fe		mixture - pellet - sealed in silica tube - heat(1220C,12h, in Ar)					Superconductivity in LaFe1-xCoxAsO			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 78(2008)104505	Athena S. Sefat,Ashfia Huq,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Lachlan M. D. Cranswick,Peter W. Stephens,Kevin H. Stone		
150911	P078104520	Cu intercalated in TaS2 layers.	CuxTaS2	Cu0.01Ta1S2	Cu	0.01	Ta	1	S	2																			2008																												TX2			A	3.3181		12.1054											2H-TaS2	K		3.05					3.05																																																								mJ/mol.K2	11									uV/K	-3.71			MTP150911																															Tuning the charge density wave and superconductivity in CuxTaS2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)104520	K. E. Wagner,E. Morosan,Y. S. Hor,J. Tao,Y. Zhu,T. Sanders,T. M. McQueen,H. W. Zandbergen,A. J. Williams,D. V. West,R. J. Cava		
150912	P078092406	ZFC signal, SP-heat also measured. (dC/Tc) = 50 mJ/mol.K2.	(Eu,K)Fe2As2	Eu0.5K0.5Fe2As2	Eu	0.5	K	0.5	Fe	2	As	2																1	2008																												ThCr2Si2			A	3.8671		13.091												K		32					32																																																																																														Eu,K,Fe,As	1	solid state reaction. mixture - sealed in Ta crucible(Ar) - SIN(900C,24h) - (grounded, pressed) - heat treatment					High-temperature superconductivity in Eu0.5K0.5Fe2As2			I. Physik. Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 78(2008)092406	H. S. Jeevan,Z. Hossain,Deepa Kasinathan,H. Rosner,C. Geibel,P. Gegenwart		
150913	P078092406	SDW at 190 K.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																			2008																																														K																																																																																																												High-temperature superconductivity in Eu0.5K0.5Fe2As2			I. Physik. Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 78(2008)092406	H. S. Jeevan,Z. Hossain,Deepa Kasinathan,H. Rosner,C. Geibel,P. Gegenwart		
150914	P078064519	P-induced SC. Tc(max) = 19.6K at P=107 GPa. Phase transition (II-III) at 107 GPa. (dHc2/dT) = -0.25 T/K at P=102 GPa.	Sc	Sc1	Sc	1																							2008																																														K				19.6	0		19.6	MTC150914																																																																																																				Comparison of the pressure dependences of Tc in the trivalent d-electron superconductors Sc, Y, La, and Lu up to megabar pressures			Department of Physics, Washington University, CB 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.B, 78(2008)064519	M. Debessai,J. J. Hamlin,J. S. Schilling		
150915	P078064519	P-induced SC. Pcrit = 88 GPa. Tc(max) = 12.2 K at P=174 GPa. (dHc2/dT) = -0.162 T/K at P=140 GPa.	Lu	Lu1	Lu	1																							2008																																														K				12.2	0		12.2	MTC150915																																																																																																				Comparison of the pressure dependences of Tc in the trivalent d-electron superconductors Sc, Y, La, and Lu up to megabar pressures			Department of Physics, Washington University, CB 1105, One Brookings Drive, St. Louis, Missouri 63130, USA	Phys.Rev.B, 78(2008)064519	M. Debessai,J. J. Hamlin,J. S. Schilling		
150916	P078092503		(La,Sr)OzFeAs	La0.85Sr0.15Fe1As1O1-z	La	0.85	Sr	0.15	Fe	1	As	1													O	1-z		1	2008																												oxypnictide			A	4.019		8.723											ZrCuSiAs	K	23		26	23			23																																																																		uV/K	-10.8			TP150916															m3/C	-0.000000000752					RH150916			LaAs,SrCO3,Fe,As,Fe2O3		mixture - press - wrapped in Ta foil - sealed in quartz tube - ANN(1160C,40h)					Superconductivity induced by oxygen deficiency in La0.85Sr0.15FeAsO1-z			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 78(2008)092503	G. Wu,H. Chen,Y. L. Xie,Y. J. Yan,T. Wu,R. H. Liu,X. F. Wang,D. F. Fang,J. J. Ying,X. H. Chen		
150917	L101097010	[penet] from muon-SR.	Sm(O,F)FeAs	Sm1Fe1As1F0.18O0.82	Sm	1	Fe	1	As	1	F	0.18													O	0.82			2008																												oxypnictide																	ZrCuSiAs	K		45				3	45																																									A	muon-SR		1900																																																				conventional solid state reaction					Coexistence of Magnetic Fluctuations and Superconductivity in the Pnictide High Temperature Superconductor SmFeAsO1-xFx Measured by Muon Spin Rotation			Department of Physics and Fribourg Center for Nanomaterials, University of Fribourg, Chemin du Musee 3, CH-1700 Fribourg, Switzerland	Phys.Rev.Lett., 101(2008)097010	A. J. Drew,F. L. Pratt,T. Lancaster,S. J. Blundell,P. J. Baker,R. H. Liu,G. Wu,X. H. Chen,I. Watanabe,V. K. Malik,A. Dubroka,K.W. Kim,M. Rossle,C. Bernhard		
150918	ZFP2630001	as-synthesized sample. H-concentration not determined. R measured upto P=21.6 kbar.	PdHx	H1Pd1	H	1	Pd	1																					1973																																														K		3.5	4				3.5			K/GPa	-0.3																																																																																												H-doped into Pd using electrochemical-loading method.					Effect of high pressure on the superconducting transition temperature of Pd-H				Z.Physik, 263(1973)1	W.Buckel,A.Eichler,B.Stritzker		
150919	L096087001	under doped. ANN(280h,in Ar). Cu-NMR studies show that CuO2 planes composed of three AFM-CuO2 planes and two SC+AFM planes.	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		1	2006								290																				Hg1245																		K				72			72																																																																																															1	high-pressure synthesis					Uniform Mixing of High-Tc Superconductivity and Antiferromagnetism on a Single CuO2 Plane of a Hg-Based Five-Layered Cuprate			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)087001	H.Mukuda,M.Abe,Y.Araki,Y.Kitaoka,K.Tokiwa,T.Watanabe,A.Iyo,H.Kito,Y.Tanaka		
150920	L096087001	optimal doped. as-grown.  Cu-NMR studies show that CuO2 planes composed of three AFM-CuO2 planes(Tn=60K) +  two SC planes(Tc=108K).	HgBa2Ca4Cu5Oz	Hg1Ba2Ca4Cu5Oz	Hg	1	Ba	2	Ca	4	Cu	5													O	z		1	2006								60																				Hg1245																		K				108			108																																																																																															1	high-pressure synthesis					Uniform Mixing of High-Tc Superconductivity and Antiferromagnetism on a Single CuO2 Plane of a Hg-Based Five-Layered Cuprate			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)087001	H.Mukuda,M.Abe,Y.Araki,Y.Kitaoka,K.Tokiwa,T.Watanabe,A.Iyo,H.Kito,Y.Tanaka		
150921	L096087001	optimal doped. as-grown.  Cu-NMR studies show that CuO2 planes composed of three AFM-CuO2 planes(Tn=45K) +  two SC planes(Tc=100K).	TlBa2Ca4Cu5Oz	Tl1Ba2Ca4Cu5Oz	Tl	1	Ba	2	Ca	4	Cu	5													O	z		1	2006								45																				Tl1245																		K				100			100																																																																																															1	high-pressure synthesis					Uniform Mixing of High-Tc Superconductivity and Antiferromagnetism on a Single CuO2 Plane of a Hg-Based Five-Layered Cuprate			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.Lett., 96(2006)087001	H.Mukuda,M.Abe,Y.Araki,Y.Kitaoka,K.Tokiwa,T.Watanabe,A.Iyo,H.Kito,Y.Tanaka		
150922	L101027002	Films from 1.5at%B-target.	B-doped CNT	B0.015C0.985	B	0.015	C	0.985																				4	2008																																														K				12			12																				Oe	from (dHc2/dT) using WHH	1700							Oe/K		200			MHC150922		A		170			A		1000																																																					Films synthesized from target with 1.5at%B.					Superconductivity in Thin Films of Boron-Doped Carbon Nanotubes			School of Science and Engineering, Material Science Course, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.Lett., 101(2008)027002	N. Murata,J. Haruyama,J. Reppert,A. M. Rao,T. Koretsune,S. Saito,M. Matsudaira,Y. Yagi		
150923	P075184512		MoGe	Ge2Mo1	Ge	2	Mo	1																				4	2007																												AMOR																		K		6.11					6.11																													T/K		2.6																																								uOhm.cm							1.84																		films sputtered on Si-substrates (Tsub = RT)  mounted on rotating Cu					Dynamic ordering of driven vortex matter in the peak effect regime of amorphous MoGe films and 2H-NbSe2 crystals			Institute of Materials Science, University of Tsukuba, 1-1-1, Tennoudai, Tsukuba, Ibaraki 305-8573, Japan	Phys.Rev.B, 75(2007)184512	N.Kokubo,T.Asada,K.Kadowaki,K.Takita,T.G.Sorop,P.H.Kes		
150924	P075184512	RRR=30	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	2007																																														K		7.2				0.05	7.2																													T/K		0.72																																								uOhm.cm							0.034																		single crystals grown by iodine vapor transport method.					Dynamic ordering of driven vortex matter in the peak effect regime of amorphous MoGe films and 2H-NbSe2 crystals			Institute of Materials Science, University of Tsukuba, 1-1-1, Tennoudai, Tsukuba, Ibaraki 305-8573, Japan	Phys.Rev.B, 75(2007)184512	N.Kokubo,T.Asada,K.Kadowaki,K.Takita,T.G.Sorop,P.H.Kes		
150925	J077103704		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2008																												oxypnictide																	ZrCuSiAs	K				28			28	TC150926																																																																																															solid state reaction. heat(1150C,38h) - slow cool to 700C - FC to RT.					Superconductivity of LaFe1-yCoyAsO1-xFx			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc.Jpn, 77(2008)103704	A.Kawabata,S.C.Lee,T.Moyoshi,Y.Kobayashi,M.Sato		
150926	J077103704	Tc is correlated with resistivity(R300),  not with Co-content.	La(O,F)(Fe,Co)As	La1Fe0.9875Co0.0125As1F0.11O0.89	La	1	Fe	0.9875	Co	0.0125	As	1	F	0.11											O	0.89			2008																												oxypnictide																	ZrCuSiAs	K				25			25	TC150926																																																																																															solid state reaction. heat(1150C,38h) - slow cool to 700C - FC to RT.					Superconductivity of LaFe1-yCoyAsO1-xFx			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc.Jpn, 77(2008)103704	A.Kawabata,S.C.Lee,T.Moyoshi,Y.Kobayashi,M.Sato		
150927	J077103704	Tc is correlated with resistivity(R300),  not with Co-content. TCFIG shows Tc vs x (Co-content)	La(O,F)(Fe,Co)As	La1Fe0.98Co0.02As1F0.11O0.89	La	1	Fe	0.98	Co	0.02	As	1	F	0.11											O	0.89			2008																												oxypnictide																	ZrCuSiAs	K				10.3			10.3	TC150927																																																																																															solid state reaction. heat(1150C,38h) - slow cool to 700C - FC to RT.					Superconductivity of LaFe1-yCoyAsO1-xFx			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602	J.Phys.Soc.Jpn, 77(2008)103704	A.Kawabata,S.C.Lee,T.Moyoshi,Y.Kobayashi,M.Sato		
150928	J077094709	Field reentrant SC. magnetic easy axis changes from c- to b-axis at reentrant field.	URhGe	U1Rh1Ge1	U	1	Rh	1	Ge	1																		3	2008							9.5																					TiNiSi																		K		0.25					0.25	MPH150928																																																																																															Czochralski method. ANN(1300C,1d,in UHV) - ANN(900C,20d, in UHV-electrical furnace)					Field Re-entrant Superconductivity Induced by the Enhancement of Effective Mass in URhGe			INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Genoble, France	J.Phys.Soc.Jpn, 77(2008)094709	A.Miyake,D.Aoki,J.Flouquet		
150929	J077094715	Tc determined by SP-heat. (lattice term coefficient of C) = 0.15 mJ/mol.K4. (dC/gamma*Tc) = 0.29.	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1			2008																												oxypnictide																	ZrCuSiAs	K		3.3					3.3																																																								mJ/mol.K2	10.6	SP-heat	371	SP-heat																																/eV.cm3	67300000000000000000000								Possible Unconventional Superconductivity in Iron-Based Layered Compound LaFePO: Study of Heat Capacity			Materials and Structures Laboratory, Tokyo Institute of Technology, R3-7, 4259 Nagatsuta-cho, Midori-ku, Yokohama	J.Phys.Soc.Jpn, 77(2008)094715	Y.Kohama,Y.Kamihara,H.Kawaji,T.Atake,M.Hirano,H.Hosono		
150930	J077094715	Tc determined by SP-heat. (lattice term coefficient of C) = 0.17 mJ/mol.K4. (dC/gamma*Tc) = 0.44.	La(O,F)FeP	La1Fe1P1F0.06O0.94	La	1	Fe	1	P	1	F	0.06													O	0.94			2008																												oxypnictide																	ZrCuSiAs	K		5.8					5.8																																																								mJ/mol.K2	8.3	SP-heat	361	SP-heat																																/eV.cm3	52600000000000000000000								Possible Unconventional Superconductivity in Iron-Based Layered Compound LaFePO: Study of Heat Capacity			Materials and Structures Laboratory, Tokyo Institute of Technology, R3-7, 4259 Nagatsuta-cho, Midori-ku, Yokohama	J.Phys.Soc.Jpn, 77(2008)094715	Y.Kohama,Y.Kamihara,H.Kawaji,T.Atake,M.Hirano,H.Hosono		
150931	J077083702	Energy gap from <27>Al-NMR. Tc(H=4.06T) = 4 K.	NpPd5Al2	Np1Pd5Al2	Np	1	Pd	5	Al	2																		3	2008																												ZrNi2Al5																		K		4.9					4.9																																																6.4	6																																															Pb-flux method					<27>Al NMR Evidence for the Strong-Coupling d-Wave Superconductivity in NpPd5Al2			Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195	J.Phys.Soc.Jpn, 77(2008)083702	H.Chudo,H.Sakai,Y.Tokunaga,S.Kambe,D.Aoki,Y.Homma,Y.Shiokawa,Y.Haga,S.Ikeda,T.Matsuda,Y.Onuki,H.Yasuoka		
150932	J077054714	monoclinic. RRR = 18.5. G-L = 9.3. thermodynamic-Hc(0) = 207 Oe. (dC/gamma*Tc) = 1.1.	Y3Pt4Ge6	Y3Pt4Ge6	Y	3	Pt	4	Ge	6																			2008																													2P<1>/m		A	8.6922	4.3062	13.1615											monoclinic(YIrGe2 + BaAl4) type, beta=99.45	K	2.6		3.4	2.6		0.5	2.6										90	Oe		54							T	from (dHc2/dT) using WHH	0.273							T/K	resistive	0.146			MHC150932		A		347			A	using G-L eq.	3230			meV	0.35	3.2	14							mJ/mol.K2	12.7	SP-heat	355	SP-heat											mOhm.cm							0.021				0.37												Y(3N),Pt(3N),Ge(5N)		mixture - (arc-melting in Ar) - ANN(1050C,1w,in evacuated silica) - slow cool to RT(1d)					Superconductivity in the ternary germanide Y3Pt4Ge6			Department of Physics and Mathematics, Aoyana Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 77(2008)054714	N.Kase,T.Muranaka,J.Akimitsu		
150933	PHC1851379	<18>O-content determined by SIMS. <18>O-exchange: 75-94.3 %.	EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.955Zn0.045O6.92	Eu	1	Ba	2	Cu	2.955	Zn	0.045													O	7-z	6.92		1991																												Y123																		K														O																																																																																														The oxygen isotope effect in Pr, Ca, and Zn substituted YBa2Cu3O7-z and EuBa2Cu3O7-z				Physica C, 185-189(1991)1379	J.P.Franck,S.Gygax,G.Soerensen,E.Altshuler,A.Hnatiw,J.Jung,M.A.-K.Mohamed,M.K.Yu,G.I.Sproule,J.Chrzanowski,J.C.Irwin		
150934	PHC1851379	<18>O-content determined by SIMS. <18>O-exchange: 75-94.3 %.	EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.925Zn0.075O6.92	Eu	1	Ba	2	Cu	2.925	Zn	0.075													O	7-z	6.92		1991																												Y123																		K														O																																																																																														The oxygen isotope effect in Pr, Ca, and Zn substituted YBa2Cu3O7-z and EuBa2Cu3O7-z				Physica C, 185-189(1991)1379	J.P.Franck,S.Gygax,G.Soerensen,E.Altshuler,A.Hnatiw,J.Jung,M.A.-K.Mohamed,M.K.Yu,G.I.Sproule,J.Chrzanowski,J.C.Irwin		
150935	PHC1851379	<18>O-content determined by SIMS. <18>O-exchange: 75-94.3 %.	EuBa2(Cu,Zn)3O7	Eu1Ba2Cu2.895Zn0.105O6.92	Eu	1	Ba	2	Cu	2.895	Zn	0.105													O	7-z	6.92		1991																												Y123																		K														O																																																																																														The oxygen isotope effect in Pr, Ca, and Zn substituted YBa2Cu3O7-z and EuBa2Cu3O7-z				Physica C, 185-189(1991)1379	J.P.Franck,S.Gygax,G.Soerensen,E.Altshuler,A.Hnatiw,J.Jung,M.A.-K.Mohamed,M.K.Yu,G.I.Sproule,J.Chrzanowski,J.C.Irwin		
150936	PHC1851379		YBa2(Cu,Zn)3O7	Y1Ba2Cu2.82Zn0.18O7-z	Y	1	Ba	2	Cu	2.82	Zn	0.18													O	7-z			1991																												Y123																		K		32					32							O	92																																																																																													The oxygen isotope effect in Pr, Ca, and Zn substituted YBa2Cu3O7-z and EuBa2Cu3O7-z				Physica C, 185-189(1991)1379	J.P.Franck,S.Gygax,G.Soerensen,E.Altshuler,A.Hnatiw,J.Jung,M.A.-K.Mohamed,M.K.Yu,G.I.Sproule,J.Chrzanowski,J.C.Irwin		
150937	SCI2381558		(La,Ca)2CuO4	La1.85Ca0.15Cu1O4	La	1.85	Ca	0.15	Cu	1															O	4			1987																												T																		K				20.6			20.6						0.74	O	75	1.3																																																																																												Oxygen isotope effect in high-temperature oxide superconductors				Science, 238(1989)1558	Hans-Conrad zur Loye,K.J.Leary,S.W.Keller,W.K.Ham,T.A.Faltens,J.N.Michaels,A.M.Stacy		
150938	SSC0670789	O-exchange: 0.9<16>O-6.1<18>O	YBa2Cu3O7	Y1Ba2Cu3O7	Y	1	Ba	2	Cu	3															O	7			1988																												Y123																		K		92					92						0.06	O	85																																																																																													Effect of isotopic substitution of oxygen on Tc and the phonon frequencies of high Tc superconductors				Solid State Commun., 67(1988)789	M.Cardona,R.Liu,C.Thomsen,W.Kress,E.Schonherr,M.Bauer,L.Genzel,W.Konig		
150939	SCI2501390		(La,Ba)2CuO4	La1.925Ba0.075Cu1O4	La	1.925	Ba	0.075	Cu	1															O	4			1990																												T																		K				24			24						0.3	O	92	0.76																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150940	SCI2501390		(La,Ba)2CuO4	La1.91Ba0.09Cu1O4	La	1.91	Ba	0.09	Cu	1															O	4			1990																												T																		K				29.3			29.3						0.53	O	90	1.6																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150941	SCI2501390		(La,Ba)2CuO4	La1.9Ba0.1Cu1O4	La	1.9	Ba	0.1	Cu	1															O	4			1990																												T																		K				29.1			29.1	IS150941					0.62	O	91	1.9																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150942	SCI2501390	isotope effect not clear due to broadness of SC transition	(La,Ba)2CuO4	La1.89Ba0.11Cu1O4	La	1.89	Ba	0.11	Cu	1															O	4			1990																												T																		K				29.1			29.1							O																																																																																														Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150943	SCI2501390	isotope effect not clear due to broadness of SC transition	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4			1990																												T																		K				29			29							O																																																																																														Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150944	SCI2501390		(La,Ba)2CuO4	La1.85Ba0.15Cu1O4	La	1.85	Ba	0.15	Cu	1															O	4			1990																												T																		K				29.1			29.1						0.21	O	86	0.6																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150945	SCI2501390		(La,Ba)2CuO4	La1.825Ba0.175Cu1O4	La	1.825	Ba	0.175	Cu	1															O	4			1990																												T																		K				24.6			24.6						0.11	O	92	0.29																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150946	SCI2501390	isotope effect not clear due to broadness of SC transition	(La,Ba)2CuO4	La1.8Ba0.2Cu1O4	La	1.8	Ba	0.2	Cu	1															O	4			1990																												T																		K				23.4			23.4							O																																																																																														Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150947	SCI2501390	broad SC transition (Tc(SUS-mid) = 25.4 K.	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4			1990																												T																		K				29.4			29.4						0.78	O	92	2.2																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150948	SCI2501390	ANN(700C,72h). Lattice const(20K, LTO): a=5.3245, b=5.3629, C=13.1771. broad SC transition (Tc(SUS-mid) = 25.4 K.	(La,Sr)2CuO4	La1.88Sr0.12Cu1O4	La	1.88	Sr	0.12	Cu	1															O	4			1990																												T			A	3.7813		13.224												K				29.1			29.1						0.85	O	87	2.3																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150949	SCI2501390	broad SC transition (Tc(SUS-mid) = 29.8 K.	(La,Sr)2CuO4	La1.87Sr0.13Cu1O4	La	1.87	Sr	0.13	Cu	1															O	4			1990																												T																		K				34.4			34.4	IS150949					0.57	O	89	2																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150950	SCI2501390	broad SC transition (Tc(SUS-mid) = 32.4 K.	(La,Sr)2CuO4	La1.86Sr0.14Cu1O4	La	1.86	Sr	0.14	Cu	1															O	4			1990																												T																		K				36.9			36.9						0.15	O	90	0.59																																																																																												Oxygen isotope effect and structural phase transitions in La2CuO4-based superconductors				Science, 250(1990)1390	M.K.Crawford,W.E.Fameth,E.M.McCarron,R.L.Harlow,A.H.Moudden		
150951	PHC1851385	<18>O exchange > 85%. Tc defined as onset of Tc(SUS). [ISOTOPE] =< 0.05.	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		1	1991																												T'																		K				24.5			24.5						0.05	O	85	0.1																																																																																							same batch samples. Two halves of sample placed in the same furnace in <18>O and <18>O riched atmosphere at 900C.					Oxygen isotope effect in Nd1.85Ce0.15CuO4				Physica C, 185-189(1991)1385	B.Batlogg,S-W.Cheong,G.A.Thomas,S. L. Cooper,L. W. Rupp Jr,D. H. Rapkine,A. S. Cooper		
150952	PHC1851345	cell volume = 188.70 A3	(La,Ca)2CuO4	La1.875Ca0.125Cu1O4	La	1.875	Ca	0.125	Cu	1															O	4			1991																												T																		K				21.7			21.7						0.7	O	90	1.56																																																																																												Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150953	PHC1851345		(La,Sr,Ca)2CuO4	La1.84Sr0.05Ca0.11Cu1O4	La	1.84	Sr	0.05	Ca	0.11	Cu	1													O	4			1991																												T																		K				33.2			33.2						0.19	O	85	0.59																																																																																												Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150954	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.925Ca0.075Cu1O4	La	1.925	Ca	0.075	Cu	1															O	4			1991																												T																		K				9.2			9.2						0.81	O	92	0.78																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150955	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.912Ca0.0875Cu1O4	La	1.912	Ca	0.0875	Cu	1															O	4			1991																												T																		K				16			16						0.66	O	89	1.07																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150956	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4			1991																												T																		K				19.5			19.5						0.5	O	17	0.33																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150957	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4			1991																												T																		K				19.5			19.5						0.51	O	49	0.59																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150958	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4			1991																												T																		K				19.5			19.5						0.52	O	72	0.94																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150959	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4			1991																												T																		K				19.5			19.5						0.55	O	93	1.17																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150960	PHC1851345	Tc by SUS. <18>O-content by infrared spectroscopy.	(La,Ca)2CuO4	La1.887Ca0.1125Cu1O4	La	1.887	Ca	0.1125	Cu	1															O	4			1991																												T																		K				20.1			20.1						0.71	O	89	1.46																																																																																							See Phys.Rev.B, 41(1990)282					Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150961	PHC1850901		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1991																											2	T																		K				36.5			36.5						0.12	O	53	0.3																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150962	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.995Ni0.005O4	La	1.85	Sr	0.15	Cu	0.995	Ni	0.005													O	4		1	1991																											2	T																		K				33			33						0.14	O	54	0.3																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150963	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4		1	1991																											2	T																		K				29			29						0.2	O	53	0.4																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150964	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.985Ni0.015O4	La	1.85	Sr	0.15	Cu	0.985	Ni	0.015													O	4		1	1991																											2	T																		K				25.5			25.5						0.23	O	54	0.4																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150965	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.98Ni0.02O4	La	1.85	Sr	0.15	Cu	0.98	Ni	0.02													O	4		1	1991																											2	T																		K				21.5			21.5						0.27	O	55	0.3																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150966	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4		1	1991																											2	T																		K				16.5			16.5						0.37	O	52	0.4																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150967	PHC1850901		(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4		1	1991																											2	T																		K				13.5			13.5						0.45	O	53	0.4																																																																																							citration technique using sol-gel method. Heat treatment (<16>O2 or 93% enriched <18>O2 atmosphere)					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150968	PHC1850901		(La,Sr)2(Cu,Zn)O4	La1.834Sr0.166Cu1O4	La	1.834	Sr	0.166	Cu	1															O	4			1991																												T																		K				35			35						0.16	O	70	0.5																																																																																							isotope samples prepared in 93%-<18>O2 atmosphere.					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150969	PHC1850901		(La,Sr)2(Cu,Zn)O4	La1.834Sr0.166Cu0.99Zn0.01O4	La	1.834	Sr	0.166	Cu	0.99	Zn	0.01													O	4			1991																												T																		K				26.5			26.5						0.17	O	70	0.4																																																																																							isotope samples prepared in 93%-<18>O2 atmosphere.					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150970	PHC1850901		(La,Ca)2CuO4	La1.9Ca0.1Cu1O4	La	1.9	Ca	0.1	Cu	1															O	4			1991																												T																		K				20			20						0.6	O	67	1																																																																																							isotope samples prepared in 93%-<18>O2 atmosphere.					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150971	PHC1850901		(La,Ca)2CuO4	La1.92Ca0.08Cu1O4	La	1.92	Ca	0.08	Cu	1															O	4			1991																												T																		K				14			14						0.66	O	69	0.8																																																																																							isotope samples prepared in 93%-<18>O2 atmosphere.					Oxygen isotope effect in La-Sr-Cu-O system with Tc modified by Ni and Zn doping				Physica C, 185-189(1991)901	N.Babushkina,A.Inyushikin,V.Ozhogin,A.Taldenkov,I.Kobrin,T.Vorob'eva,L.Moichanova,L.Damyanets,T.Uvarova,A.Kuzakov		
150972	APS0010359	Tc by SUS.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1993																												T																		K				37.43			37.43						0.14	O	55	0.36																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150973	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.995Ni0.005O4	La	1.85	Sr	0.15	Cu	0.995	Ni	0.005													O	4			1993																												T																		K				34.41			34.41						0.13	O	55	0.29																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150974	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.99Ni0.01O4	La	1.85	Sr	0.15	Cu	0.99	Ni	0.01													O	4			1993																												T																		K				30			30						0.15	O	55	0.29																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150975	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.985Ni0.015O4	La	1.85	Sr	0.15	Cu	0.985	Ni	0.015													O	4			1993																												T																		K				25.9			25.9						0.25	O	55	0.43																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150976	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu98Ni0.02O4	La	1.85	Sr	0.15	Cu	98	Ni	0.02													O	4			1993																												T																		K				21.96			21.96						0.25	O	80	0.55																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150977	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.975Ni0.025O4	La	1.85	Sr	0.15	Cu	0.975	Ni	0.025													O	4			1993																												T																		K				16.6			16.6						0.37	O	55	0.4																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150978	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.97Ni0.03O4	La	1.85	Sr	0.15	Cu	0.97	Ni	0.03													O	4			1993																												T																		K				12.7			12.7						0.34	O	55	0.28																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150979	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.996Zn0.004O4	La	1.85	Sr	0.15	Cu	0.996	Zn	0.004													O	4			1993																												T																		K				32.7			32.7						0.16	O	80	0.49																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150980	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.992Zn0.008O4	La	1.85	Sr	0.15	Cu	0.992	Zn	0.008													O	4			1993																												T																		K				28.5			28.5						0.2	O	80	0.55																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150981	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.988Zn0.012O4	La	1.85	Sr	0.15	Cu	0.988	Zn	0.012													O	4			1993																												T																		K				23.7			23.7						0.26	O	80	0.58																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150982	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.984Zn0.016O4	La	1.85	Sr	0.15	Cu	0.984	Zn	0.016													O	4			1993																												T																		K				19			19						0.44	O	80	0.78																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150983	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.978Zn0.022O4	La	1.85	Sr	0.15	Cu	0.978	Zn	0.022													O	4			1993																												T																		K				13.6			13.6						0.68	O	80	0.8																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150984	APS0010359	Tc by SUS.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1993																												T																		K				37.5			37.5						0.15	O	80	0.53																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150985	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.997Fe0.003O4	La	1.85	Sr	0.15	Cu	0.997	Fe	0.003													O	4			1993																												T																		K				33.6			33.6						0.2	O	80	0.64																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150986	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.995Fe0.005O4	La	1.85	Sr	0.15	Cu	0.995	Fe	0.005													O	4			1993																												T																		K				30.82			30.82						0.27	O	80	0.79																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150987	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.993Fe0.007O4	La	1.85	Sr	0.15	Cu	0.993	Fe	0.007													O	4			1993																												T																		K				26.25			26.25						0.69	O	80	1.67																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150988	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.992Fe0.008O4	La	1.85	Sr	0.15	Cu	0.992	Fe	0.008													O	4			1993																												T																		K				24.73			24.73						0.81	O	80	1.83																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150989	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.991Fe0.009O4	La	1.85	Sr	0.15	Cu	0.991	Fe	0.009													O	4			1993																												T																		K				19.85			19.85						0.97	O	80	1.75																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150990	APS0010359	Tc by SUS.	(La,Sr)2(Cu,Fe)O4	La1.85Sr0.15Cu0.99Fe0.01O4	La	1.85	Sr	0.15	Cu	0.99	Fe	0.01													O	4			1993																												T																		K				17.7			17.7						1.3	O	80	2.06																																																																																							citration technique using sol-gel method.					Anomalously enhanced oxygen isotope effect in La1.85Sr0.15CuO4 doped with Fe			Kurchatov Institute, Moscow,Russia	Appl.Supercond., 1(1993)359	V.Ozhogin,N.Babushkina,A.Inyushikin,A.Taldenkov		
150991	PHC1851345	cell volume = 188.70 A3	(La,Ca)2CuO4	La1.85Ca0.15Cu1O4	La	1.85	Ca	0.15	Cu	1															O	4			1991																												T																		K				22.1			22.1						0.72	O	90	1.56																																																																																												Oxygen isotope effect and structural phase transitions in La2-xMxCuO4				Physica C, 185-189(1991)1345	M.K.Crawford,W.E.Fameth,R.Miao,R.L.Harlow,C.C.Torardi,E.M.McCarron,Du Pont Co		
150992	PHB1941433		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4			1994																												T																		K				38			38						0.15	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150993	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.9975Co0.0025O4	La	1.85	Sr	0.15	Cu	0.9975	Co	0.0025													O	4			1994																												T																		K				34.8			34.8						0.15	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150994	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.995Co0.005O4	La	1.85	Sr	0.15	Cu	0.995	Co	0.005													O	4			1994																												T																		K				33			33						0.15	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150995	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.9925Co0.0075O4	La	1.85	Sr	0.15	Cu	0.9925	Co	0.0075													O	4			1994																												T																		K				30.6			30.6						0.22	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150996	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.99Co0.01O4	La	1.85	Sr	0.15	Cu	0.99	Co	0.01													O	4			1994																												T																		K				25.2			25.2						0.4	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150997	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.9875Co0.0125O4	La	1.85	Sr	0.15	Cu	0.9875	Co	0.0125													O	4			1994																												T																		K				22.9			22.9						0.46	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150998	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.985Co0.015O4	La	1.85	Sr	0.15	Cu	0.985	Co	0.015													O	4			1994																												T																		K				13.5			13.5						1.07	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
150999	PHB1941433		(La,Sr)2(Cu,Co)O4	La1.85Sr0.15Cu0.9825Co0.0175O4	La	1.85	Sr	0.15	Cu	0.9825	Co	0.0175													O	4			1994																												T																		K				13.2			13.2						1.3	O	80																																																																																								heat treatment (950C in <16>O2, <18>O2 atmosphere)					Oxygen isotope effect in Tc of La2-ySryCu1-xMexO4 (Me=Ni, Zn, Co, Fe)			"Russian Scientific Center ""Kurchatov Institute"", 123182 Moscow, Russia"	Physica B, 194-196(1994)1433	N. Babushkina,V. Ozhogin,A. Inyushkin,A. Taldenkov,L. Molchanova		
151000	J077063707	ZrCuSiAs-type for 0 =< y =< 0.6 in NdFeAsO1-y.	NdOxFeAs	Nd1Fe1As1O0.6	Nd	1	Fe	1	As	1															O	0.6			2008																												oxypnictide	P4/nmm		A	3.943		8.529											ZrCuSiAs-type	K	52		54.2	53			53	TC151000									82																																																																																				NdAs,Fe,Fe2O3		high-P-synthesis using cubic anvil. Mixture - heat(1200C,2h, P=2GPa, in BN crucible)					Superconductivity at 54K in F-Free NdFeAsO1-y			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 77(2008)063707	Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151001	J077063707	impurity phase appears.	NdOxFeAs	Nd1Fe1As1O0.2	Nd	1	Fe	1	As	1															O	0.2			2008																												oxypnictide			A	3.9346		8.5324											ZrCuSiAs-type	K		54					54										19																																																																																				NdAs,Fe,Fe2O3		high-P-synthesis using cubic anvil. Mixture - heat(1200C,2h, P=2GPa, in BN crucible)					Superconductivity at 54K in F-Free NdFeAsO1-y			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 77(2008)063707	Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151002	J077063707		LaOxFeAs	La1Fe1As1O0.6	La	1	Fe	1	As	1															O	0.6			2008																												oxypnictide																	ZrCuSiAs-type	K				27			27																																																																																														NdAs,Fe,Fe2O3		high-P-synthesis using cubic anvil. Mixture - heat(1200C,2h, P=2GPa, in BN crucible)					Superconductivity at 54K in F-Free NdFeAsO1-y			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 77(2008)063707	Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151003	J077063707		PrOxFeAs	Pr1Fe1As1O0.6	Pr	1	Fe	1	As	1															O	0.6			2008																												oxypnictide																	ZrCuSiAs-type	K				44			44																																																																																														NdAs,Fe,Fe2O3		high-P-synthesis using cubic anvil. Mixture - heat(1200C,2h, P=2GPa, in BN crucible)					Superconductivity at 54K in F-Free NdFeAsO1-y			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 77(2008)063707	Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151004	PHC4682229	hydrostatic pressure. Diamond anvil cell.	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2008																												oxypnictide																	ZrCuSiAs-type	K		28					28	TC151004		K/GPa	2.2																																																																																																	Effect of pressure on the superconducting critical temperature of La[O0.89F0.11]FeAs and Ce[O0.88F0.12]FeAs			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, CA 92093, USA	Physica C, 468(2008)2229	D.A. Zocco,J.J. Hamlin,R.E. Baumbach,M.B. Maple,M.A. McGuire,A.S. Sefat,B.C. Sales,R. Jin,D. Mandrus,J.R. Jeffries,S.T. Weir,Y.K. Vohra		
151005	PHC4682229	Tc < 1.1 K at P=265 kbar.	Ce(O,F)FeAs	Ce1Fe1As1F0.12O0.88	Ce	1	Fe	1	As	1	F	0.12													O	0.88		1	2008																												oxypnictide																	ZrCuSiAs-type	K		47					47	TC151005																																																																																															sample prepared using Bridgman anvil cell.					Effect of pressure on the superconducting critical temperature of La[O0.89F0.11]FeAs and Ce[O0.88F0.12]FeAs			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California at San Diego, La Jolla, CA 92093, USA	Physica C, 468(2008)2229	D.A. Zocco,J.J. Hamlin,R.E. Baumbach,M.B. Maple,M.A. McGuire,A.S. Sefat,B.C. Sales,R. Jin,D. Mandrus,J.R. Jeffries,S.T. Weir,Y.K. Vohra		
151006	PHC4682341	post annealed sample.	(Cu,Tl)Ba2Ca2Cu3O10	Tl0.5Ba2Ca2Cu3O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3													O	10-z		2	2008																												Tl1223																	(Cu,Tl)1223	K	114		110				112																																																																																																Two step solid state reaction. precursor(Cu-Ba-Ca-Ge-O) was prepared. Then, addition(Tl2O3) - wrapped in Au - heat(860C,8min) - Q to RT					(Cu0.5Tl0.5)Ba2Can-1Cun-yGeyO2n+4-d (n = 3, 4 and y = 0.5, 0.75, 1.0); superconductors with GeO2 planes			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 468(2008)2341	Nawazish A. Khan,M. Irfan		
151007	PHC4682341		(Cu,Tl)Ba2Ca2(Cu,Ge)3O10	Tl0.5Ba2Ca2Cu3Ge0.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3	Ge	0.5											O	10-z		2	2008																												Tl1223																	(Cu,Tl)1223	K	104		102				103																																																																																																Two step solid state reaction. precursor(Cu-Ba-Ca-Ge-O) was prepared. Then, addition(Tl2O3) - wrapped in Au - heat(860C,8min) - Q to RT					(Cu0.5Tl0.5)Ba2Can-1Cun-yGeyO2n+4-d (n = 3, 4 and y = 0.5, 0.75, 1.0); superconductors with GeO2 planes			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 468(2008)2341	Nawazish A. Khan,M. Irfan		
151008	PHC4682341		(Cu,Tl)Ba2Ca2(Cu,Ge)3O10	Tl0.5Ba2Ca2Cu2.75Ge0.75O10-z	Tl	0.5	Ba	2	Ca	2	Cu	2.75	Ge	0.75											O	10-z		2	2008																												Tl1223																	(Cu,Tl)1223	K	112		104				108																																																																																																Two step solid state reaction. precursor(Cu-Ba-Ca-Ge-O) was prepared. Then, addition(Tl2O3) - wrapped in Au - heat(860C,8min) - Q to RT					(Cu0.5Tl0.5)Ba2Can-1Cun-yGeyO2n+4-d (n = 3, 4 and y = 0.5, 0.75, 1.0); superconductors with GeO2 planes			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 468(2008)2341	Nawazish A. Khan,M. Irfan		
151009	PHC4682341		(Cu,Tl)Ba2Ca2(Cu,Ge)3O10	Tl0.5Ba2Ca2Cu2.5Ge1O10-z	Tl	0.5	Ba	2	Ca	2	Cu	2.5	Ge	1											O	10-z		2	2008																												Tl1223																	(Cu,Tl)1223	K	108		100				104																																																																																																Two step solid state reaction. precursor(Cu-Ba-Ca-Ge-O) was prepared. Then, addition(Tl2O3) - wrapped in Au - heat(860C,8min) - Q to RT					(Cu0.5Tl0.5)Ba2Can-1Cun-yGeyO2n+4-d (n = 3, 4 and y = 0.5, 0.75, 1.0); superconductors with GeO2 planes			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Physica C, 468(2008)2341	Nawazish A. Khan,M. Irfan		
151010	JJP0262085	O<18>O exchange: 65 - 85%.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1987																												Y123																		K		92					92						0.05	O	85	0.4																																																																																							heat(650C,16h,in vac) - heat(950C,19h,in(98%<18>O+0.57%<17>O+1.32%<16>O)atmosphere)					Isotope effect in superconducting YBa2Cu3O7-z system				Jpn.J.Appl.Phys., 26(1987)L2085	H.Katayama-Yoshida,T.Hirooka,A.J.Mascarenhas,Y.Okabe,T.Takahashi,T.Sasaki,A.Ochiai,T.Suzuki,J.I.Pankove,T.Ciszek,S.K.Deb		
151011	JJP0262085	O<18>O exchange: 65 - 85%. No appreciable isotope effect for Cu.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z			1987																												Y123																		K		92					92						0	Cu	85																																																																																								heat(650C,16h,in vac) - heat(950C,19h,in(98%<18>O+0.57%<17>O+1.32%<16>O)atmosphere)					Isotope effect in superconducting YBa2Cu3O7-z system				Jpn.J.Appl.Phys., 26(1987)L2085	H.Katayama-Yoshida,T.Hirooka,A.J.Mascarenhas,Y.Okabe,T.Takahashi,T.Sasaki,A.Ochiai,T.Suzuki,J.I.Pankove,T.Ciszek,S.K.Deb		
151012	PHC1560481		Bi2Sr2CaCu2O8	Bi2Sr2Ca1Cu2O8	Bi	2	Sr	2	Ca	1	Cu	2													O	8			1988																												Bi2212																		K		75					75						0.034	O	100	0.3																																																																																							heat(in vav, 5h) - heat(850C,30h,in <18>O atmosphere)					OXYGEN ISOTOPE EFFECT IN THE SUPERCONDUCTING BI-SR-CA-CU-O SYSTEM				PHYSICA C,156(1988)481	CISZEK.T.F,DEB.S.K,GOLDFARB.R.B,HIROOKA.T,KATAYAMA-YOSHIDA.H,LI.Y,MASCARENHAS.A.J,OCHIAI.A,OKABE.Y,OYAMADA.A,PANKOVE.J.I,SASAKI.T,SUZUKI.T,TAKAHASHI.T		
151013	PHC1560481		Bi2Sr2Ca2Cu3O10	Bi2Sr2Ca2Cu3O10	Bi	2	Sr	2	Ca	2	Cu	3													O	10			1988																												Bi2223																		K		110					110						0.026	O	100	0.34																																																																																							heat(in vav, 5h) - heat(850C,30h,in <18>O atmosphere)					OXYGEN ISOTOPE EFFECT IN THE SUPERCONDUCTING BI-SR-CA-CU-O SYSTEM				PHYSICA C,156(1988)481	CISZEK.T.F,DEB.S.K,GOLDFARB.R.B,HIROOKA.T,KATAYAMA-YOSHIDA.H,LI.Y,MASCARENHAS.A.J,OCHIAI.A,OKABE.Y,OYAMADA.A,PANKOVE.J.I,SASAKI.T,SUZUKI.T,TAKAHASHI.T		
151014	NAT3350419	[isotope] = 0.41 or 0.48 assuming exchenge ratio = 100 or 85 %, respectively.	(Ba,K)BiO3	Ba0.625K0.375Bi1O3	Ba	0.625	K	0.375	Bi	1															O	3			1988																												BKBO																		K	29	29.4	30				29.4						0.41	O		1.4																																																																																												The oxygen isotope effect in Ba0.625K0.375BiO3			Argonne National Lab.	Nature, 335(1988)419	D.G.Hinks,D.R.Richards,B.Dabrowski,D.T.Marx,A.W.Mitchell		
151015	SCI2381558		Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			1987																												BPBO																		K				11		6	11						0.64	O	60	0.5																																																																																												Oxygen isotope effect in high-temperature oxide superconductors				Science, 238(1989)1558	Hans-Conrad zur Loye,K.J.Leary,S.W.Keller,W.K.Ham,T.A.Faltens,J.N.Michaels,A.M.Stacy		
151016	PHC1570469	x=0.25 in Ba1-xKxBiO3 from lattice constant, EPMA.	(Ba,K)BiO3	Ba0.7K0.6Bi1O3	Ba	0.7	K	0.6	Bi	1															O	3			1989																												BKBO																		K				29.35			29.35						0.35	O																																																											uV/K				TP151016															cm3/C						RH151016			BaO2,KO2,Bi2O3		using <18>O-riched oxide					Normal state properties and oxygen isotope effect of (Ba,K)BiO3				Physica C, 157(1989)469	S.Kondoh,M.Sera,Y.Ando,M.Sato		
151017	JJP027L553	two samples(average Ba mass = 134.57, 137.34) were measured. dM = 2.8. no significant difference in Tc (dTc < 0.1 K)	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1988																												Y123																		K				89.9			89.9						0	Ba																																																																																									two samples - heat(930C,5h, in Pt crucible) - pellet - heat(950C, 1 atm O2 flow)					Ba isotope effect in a Ba2YCu3O7-z superconductor			Electrotechnical Laboratory, Umezono,Tsukuba City, Ibaraki	Jpn.J.Appl.Phys., 27(1988)L553	T.Hidaka,T.Matsui,Y.Nakagawa		
151018	PR0363990	[isotope] = 0 +- 0.07. Tc(99.7%<65>Cu) - Tc(99.6%<63>Cu) = 0.2 K.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1987																												Y123																		K		89.7					89.7						0	Cu																																																																																														Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity			University of California, Berkeley, California	Phys.Rev.B, 36(1987)3990	L.C.Bourne,A.Zettl,T.W.Barbee III,M.L.Cohen		
151019	PR0363990	[isotope] = 0 +- 0.10. Tc(99.7%<138>Ba) - Tc(78.8%<135>Ba) = 0.1 K.	YBa2Cu3O7	Y1Ba2Cu3O7-z	Y	1	Ba	2	Cu	3															O	7-z		1	1987																												Y123																		K		91.95					91.95						0	Ba																																																																																														Complete absence of isotope effect in YBa2Cu3O7: Consequences for phonon-mediated superconductivity			University of California, Berkeley, California	Phys.Rev.B, 36(1987)3990	L.C.Bourne,A.Zettl,T.W.Barbee III,M.L.Cohen		
151020	SCI2590655	Tc(55%<13>C) - Tc(<12>C) = 0.5 K.	Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene																		K				29.55			29.55						0.39	C	55	0.5																																																																																												Isotope effect and superconductivity in metal-doped C60			Department of Chemistry , Harvard University, Cambridge, MA, USA	Science 259(1993)655	Charles M.Lieber,Chia-Chun Chen		
151021	SCI2590655	Tc(50%<13>C) - Tc(<12>C) = 0.9 K.	Rb3C60	C60Rb3	C	60	Rb	3																					1993																												fullerene																		K				29.55			29.55						0.77	C	50	0.9																																																																																												Isotope effect and superconductivity in metal-doped C60			Department of Chemistry , Harvard University, Cambridge, MA, USA	Science 259(1993)655	Charles M.Lieber,Chia-Chun Chen		
151022	MTL0624400	(Pb,M)SrLaCuOz (M=P,S) are not SC.	(Pb,B)SrLaCuOz	Pb0.5B0.5Sr1La1Cu1Oz	Pb	0.5	B	0.5	Sr	1	La	1	Cu	1											O	z		1	2008																												Pb1201			A	3.779		8.654												K	25		32	30			30										19																																																																																				Sr2CuO3,PbO,La2O3,CuO,B2O3		mixture - pellet - CAL(800C,24h,in air) - pellet - SIN(890C,24h,in air) - cool to RT					New superconducting lead cuprate with 1201 structure, (Pb0.5B0.5) (SrLa)CuOz			Department of Physics, Hamamatsu University School of Medicine, 1-20-1 Handayama, Higashi-ku, Hamamatsu, Shizuoka 431-3192, Japan	Mater.Lett., 62(2008)4400	Hiroyuki Sasakura,Yoshiya Akagi,Shigeki Tsukui,Motoaki Adachi		
151023	JAC4640550	as-grown sample	(Cu,Tl,Li)Ba2Ca2(Cu,Ni)3O10	Tl0.25Li0.25Ba2Ca2Cu2Ni1.5O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	2	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	108.4			110			110																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151024	JAC4640550	as-grown sample	(Cu,Tl,Li)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.25Li0.25Ba2Ca1.5Mg0.5Cu2Ni1.5O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	1.5	Mg	0.5	Cu	2	Ni	1.5							O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	106			107			107																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151025	JAC4640550	as-grown sample	(Cu,Tl,Li)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.25Li0.25Ba2Ca1Mg1Cu2Ni1.5O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	1	Mg	1	Cu	2	Ni	1.5							O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	101			105			105																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151026	JAC4640550	as-grown sample	(Cu,Tl,Li)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.25Li0.25Ba2Ca0.5Mg1.5Cu2Ni1.5O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	0.5	Mg	1.5	Cu	2	Ni	1.5							O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	96.5			103			103																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151027	JAC4640550	as-grown sample	(Cu,Tl)Ba2Ca2(Cu,Ni)3O10	Tl0.5Ba2Ca2Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	2	Ni	1.5											O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	90			97			97																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151028	JAC4640550	as-grown sample	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca1.5Mg0.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1.5	Mg	0.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	97			99.7			99.7																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151029	JAC4640550	as-grown sample	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca1Mg1Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1	Mg	1	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	97			99.8			99.8																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151030	JAC4640550	as-grown sample	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca0.5Mg1.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	0.5	Mg	1.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223																	(Cu,Tl)1223	K	95			100			100																																																																																																two step method. firstly precursor materials with Tl-free synthesized. Then, precursor + Tl2O3, solid state reaction in Au-capsule.					Effect of Mg doping in enhancing superconductivity in Ni doped (Cu0.5Tl0.25Li0.25)Ba2Ca2-yMgy (Cu1.5Ni1.5)O10-z (y = 0, 0.5, 1.0, 1.5) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloys & Compd., 464(2008)550	Nawazish A. Khan,Najmul Hassan		
151031	MCP1120412	95%-1223phase, 5%-1234phase	(Cu,Tl)Ba2(Ca,Be)2(Cu,Ni)3O10	Tl0.5Ba2Ca1.5Be0.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1.5	Be	0.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0303		14.8424											(Cu,Tl)1223	K	98			100			100																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151032	MCP1120412	90%-1223phase, 10%-1234phase	(Cu,Tl)Ba2(Ca,Be)2(Cu,Ni)3O10	Tl0.5Ba2Ca1Be1Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1	Be	1	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0156		14.8219											(Cu,Tl)1223	K	102			104			104																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151033	MCP1120412	93%-1223phase, 7%-1234phase	(Cu,Tl)Ba2(Ca,Be)2(Cu,Ni)3O10	Tl0.5Ba2Ca0.5Be1.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	0.5	Be	1.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0089		14.8007											(Cu,Tl)1223	K	104			107			107																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151034	MCP1120412	85%-1223phase, 11%-1234phase, 4%-1212phase	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca1.5Mg0.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1.5	Mg	0.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0455		14.8737											(Cu,Tl)1223	K	96			101			101																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151035	MCP1120412	84%-1223phase, 12%-1234phase, 4%-1212phase	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca1Mg1Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	1	Mg	1	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0281		14.8404											(Cu,Tl)1223	K	97			102.5			102.5																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151036	MCP1120412	80%-1223phase, 15%-1234phase, 5%-1212phase	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Ni)3O10	Tl0.5Ba2Ca0.5Mg1.5Cu2Ni1.5O10-z	Tl	0.5	Ba	2	Ca	0.5	Mg	1.5	Cu	2	Ni	1.5									O	10-z			2008																												Tl1223			A	4.0152		14.8108											(Cu,Tl)1223	K	98			103.5			103.5																																																																																																two step synthesis. Tl-free precursor firstly synthesized					Enhancement of superconducting properties in Cu0.5Tl0.5Ba2Ca0.5M1.5Cu1.5Ni1.5O10-z  (M= Mg, Be) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Mater.Chem.Phys., 112(2008)412	Najmul Hassan,Nawazish A. Khan		
151037	PRL0590915	Tc measured by magnetization.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K				35			35						0.22	O	68	0.6																																																																																							different <18>O concentration from different annealing conditions.					Observation of oxygen isotope shift in the superconducting transition temperature of La1.85Sr0.15CuO4				Phys.Rev.Lett., 59(1987)915	T.A.Faltens,W.K.Ham,S.W.Keller,K.J.Leary,J.N.Michaels,A.M.Stacy,Hans-Conrad zur Loye,D.E.Morris,T.W.Barbee III,L.C.Bourne,M.L.Cohen,S.Hoen,A.Zettl		
151038	PRL0590915	Tc measured by magnetization.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K				37			37						0.13	O	75	0.45																																																																																							different <18>O concentration from different annealing conditions.					Observation of oxygen isotope shift in the superconducting transition temperature of La1.85Sr0.15CuO4				Phys.Rev.Lett., 59(1987)915	T.A.Faltens,W.K.Ham,S.W.Keller,K.J.Leary,J.N.Michaels,A.M.Stacy,Hans-Conrad zur Loye,D.E.Morris,T.W.Barbee III,L.C.Bourne,M.L.Cohen,S.Hoen,A.Zettl		
151039	PRL0590915	Tc measured by resistive transition.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K			34.5				34.5						0.09	O	65	0.25																																																																																							different <18>O concentration from different annealing conditions.					Observation of oxygen isotope shift in the superconducting transition temperature of La1.85Sr0.15CuO4				Phys.Rev.Lett., 59(1987)915	T.A.Faltens,W.K.Ham,S.W.Keller,K.J.Leary,J.N.Michaels,A.M.Stacy,Hans-Conrad zur Loye,D.E.Morris,T.W.Barbee III,L.C.Bourne,M.L.Cohen,S.Hoen,A.Zettl		
151040	PRL0590915	Tc measured by resistive transition.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K			37				37						0.11	O	65	0.33																																																																																							different <18>O concentration from different annealing conditions.					Observation of oxygen isotope shift in the superconducting transition temperature of La1.85Sr0.15CuO4				Phys.Rev.Lett., 59(1987)915	T.A.Faltens,W.K.Ham,S.W.Keller,K.J.Leary,J.N.Michaels,A.M.Stacy,Hans-Conrad zur Loye,D.E.Morris,T.W.Barbee III,L.C.Bourne,M.L.Cohen,S.Hoen,A.Zettl		
151041	PRL0590915	Tc measured by resistive transition.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1987																												T																		K			37				37						0.1	O	65	0.3																																																																																							different <18>O concentration from different annealing conditions.					Observation of oxygen isotope shift in the superconducting transition temperature of La1.85Sr0.15CuO4				Phys.Rev.Lett., 59(1987)915	T.A.Faltens,W.K.Ham,S.W.Keller,K.J.Leary,J.N.Michaels,A.M.Stacy,Hans-Conrad zur Loye,D.E.Morris,T.W.Barbee III,L.C.Bourne,M.L.Cohen,S.Hoen,A.Zettl		
151042	P078100507	Tc(mid) defined as a peak of (dR/dT). [dTc/dP] for P > 0.2 GPa.	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																		GPa		78								oxypnictide			A	4.004		8.689												K		22.8	23.8				22.8	TC151042		K/Gpa	-0.73																																																																																										La2O3,LaF3,La or Fe,Fe2O3,As,LaAs		High-P-T(HIP) synthesis. T-dependence of lattice constant a(T), c(T) were measured.					Correlated pressure effects on the structure and superconductivity of LaFeAsO0.9F0.1			European Synchrotron Radiation Facility (ESRF), BP 220, 6 Rue Jules Horowitz, 38043 Grenoble Cedex, France	Phys.Rev.B, 78(2008)100507	G. Garbarino,P. Toulemonde,M. Alvarez-Murga,A. Sow,M. Mezouar,M. Nunez-Regueiro		
151043	P078104527	(dTc(on)/dP) = -1.5 K/GPa), (dTc(off)/dP) = -2.1 K/GPa),	(Ba,K)Fe2As2	Ba0.55K0.45Fe2As2	Ba	0.55	K	0.45	Fe	2	As	2																	2008																												ThCr2Si2																		K	28.6		30.2				29.4	MTC151043		K/Gpa	-1.5																														MHC151043																																																														Sn-flux method using high-temperature solution growth techniques.					Effect of pressure on the structural phase transition and superconductivity in (Ba1-xKx)Fe2As2 (x=0 and 0.45) and SrFe2As2 single crystals			Department of Physics, San Diego State University, San Diego, California 92182-1233, USA	Phys.Rev.B, 78(2008)104527	M. S. Torikachvili,S. L. Bud'ko,N. Ni,P. C. Canfield		
151044	P078104527	not SC. AFM phase: Tn(P) = 173(0), 144(2.3), 128(3.52): P in kbar.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																			2008								173																				ThCr2Si2																		K					0.5																																																																																																		Sn-flux method using high-temperature solution growth techniques.					Effect of pressure on the structural phase transition and superconductivity in (Ba1-xKx)Fe2As2 (x=0 and 0.45) and SrFe2As2 single crystals			Department of Physics, San Diego State University, San Diego, California 92182-1233, USA	Phys.Rev.B, 78(2008)104527	M. S. Torikachvili,S. L. Bud'ko,N. Ni,P. C. Canfield		
151045	P078104527	not SC. AFM phase: Tn(P) = 86.1(0), 79.5(5.49), 74.7(9.33), 69.8(15.2), 64.7(20.1): P in kbar).	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																			2008								86.1																				ThCr2Si2																		K					0.5																																																																																																		Sn-flux method using high-temperature solution growth techniques.					Effect of pressure on the structural phase transition and superconductivity in (Ba1-xKx)Fe2As2 (x=0 and 0.45) and SrFe2As2 single crystals			Department of Physics, San Diego State University, San Diego, California 92182-1233, USA	Phys.Rev.B, 78(2008)104527	M. S. Torikachvili,S. L. Bud'ko,N. Ni,P. C. Canfield		
151046	P078104527	not SC. AFM phase: Tn(P) : AFM151046 in [TCFIG]	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2008								205																				ThCr2Si2																		K					0.5			AFM151046																																																																																															Sn-flux method using high-temperature solution growth techniques.					Effect of pressure on the structural phase transition and superconductivity in (Ba1-xKx)Fe2As2 (x=0 and 0.45) and SrFe2As2 single crystals			Department of Physics, San Diego State University, San Diego, California 92182-1233, USA	Phys.Rev.B, 78(2008)104527	M. S. Torikachvili,S. L. Bud'ko,N. Ni,P. C. Canfield		
151047	MAT8071896	P-induced-SC. resistivity not measured. Tc(max) = 29K(P=4.0GPa), [VOLS](max) = 25%(P=4.0GPa). Pc = 2.8 GPa.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2008																												ThCr2Si2																		K				29	0		29	MTC151047																																																																																															single crystals grown by Sn-flux method.					Superconductivity up to 29 K in SrFe2As2 and BaFe2As2 at high pressures			Department of Physics, University of Cambridge, Cavendish Laboratory, JJ Thomson Avenue, Cambridge CB3 0HE, UK	cond-mat/0807.1896(2008)	Patricia L. Alireza,Y. T. Chris Ko,Jack Gillett,Chiara M. Petrone,Jacqueline M. Cole,Suchitra E. Sebastian,Gilbert G. Lonzarich		
151048	MAT8071896	P-induced-SC. resistivity not measured. Tc(max) = 27K(P=3.0GPa), [VOLS](max) = 25%(P=3.8GPa). Pc = 2.7 GPa.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2008																												ThCr2Si2																		K				27	0		27	MTC151048																																																																																															single crystals grown by Sn-flux method.					Superconductivity up to 29 K in SrFe2As2 and BaFe2As2 at high pressures			Department of Physics, University of Cambridge, Cavendish Laboratory, JJ Thomson Avenue, Cambridge CB3 0HE, UK	cond-mat/0807.1896(2008)	Patricia L. Alireza,Y. T. Chris Ko,Jack Gillett,Chiara M. Petrone,Jacqueline M. Cole,Suchitra E. Sebastian,Gilbert G. Lonzarich		
151049	MAT8074283	P-induced SC.Tc=27 K at P=2.8 GPa, but zero-resistivity not obtained. tetre-to-ortho transition at 205 K.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		1	2008																												ThCr2Si2																		K			27		0		27																																																																							mOhm.cm											0.83														mixture(Sr:Fe:As=1:2:2) in Al2O3 crucible - sealed in quartz tube(inert gas) - heat.					Effect of pressure on the magnetostructural transition in SrFe2As2			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Str. 40, 01187 Dresden, Germany	cond-mat/0807.4283(2008)	M. Kumar,M. Nicklas,A. Jesche,N. Caroca-Canales,M. Schmitt,M. Hanfland,D. Kasinathan,U. Schwarz,H. Rosner,C. Geibel		
151050	P078132506	not SC. R-anomaly(peak) at T* = 124 K.	TbOFeAs	Tb1Fe1As1O1	Tb	1	Fe	1	As	1															O	1		1	2008																												oxypnictide	P4/nmm		A	3.8994		8.4029											ZrCuSiAs-type	K					4																																																																				uV/K	-12.55			TP151052																								Tb,Tb4O7,ThO2,Fe,As		FeAs,TbAs firstly made. Then, mixture - pellet(at 200MPa, in Ar) - wrapped(Ta-foil) - sealed in evacuated quartz ampoule - heat(1453K,48h) - FC to RT					Superconductivity above 50 K in Tb1-xThxFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 78(2008)132506	Lin-Jun Li,Yu-Ke Li,Zhi Ren,Yong-Kang Luo,Xiao Lin,Mi He,Qian Tao,Zeng-Wei Zhu,Guang-Han Cao,Zhu-An Xu		
151051	P078132506	R-anomaly(peak) at T* = 120 K.	(Tb,Th)OFeAs	Tb0.9Th0.1Fe1As1O1	Tb	0.9	Th	0.1	Fe	1	As	1													O	1		1	2008																												oxypnictide	P4/nmm		A	3.8998		8.409											ZrCuSiAs-type	K			45				45																																																																		uV/K	-13.09			TP151052																								Tb,Tb4O7,ThO2,Fe,As		FeAs,TbAs firstly made. Then, mixture - pellet(at 200MPa, in Ar) - wrapped(Ta-foil) - sealed in evacuated quartz ampoule - heat(1453K,48h) - FC to RT					Superconductivity above 50 K in Tb1-xThxFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 78(2008)132506	Lin-Jun Li,Yu-Ke Li,Zhi Ren,Yong-Kang Luo,Xiao Lin,Mi He,Qian Tao,Zeng-Wei Zhu,Guang-Han Cao,Zhu-An Xu		
151052	P078132506		(Tb,Th)OFeAs	Tb0.8Th0.2Fe1As1O1	Tb	0.8	Th	0.2	Fe	1	As	1													O	1		1	2008																												oxypnictide	P4/nmm		A	3.9025		8.4131											ZrCuSiAs-type	K			52				52										50																																																								uV/K	-32.73			TP151052																								Tb,Tb4O7,ThO2,Fe,As		FeAs,TbAs firstly made. Then, mixture - pellet(at 200MPa, in Ar) - wrapped(Ta-foil) - sealed in evacuated quartz ampoule - heat(1453K,48h) - FC to RT					Superconductivity above 50 K in Tb1-xThxFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 78(2008)132506	Lin-Jun Li,Yu-Ke Li,Zhi Ren,Yong-Kang Luo,Xiao Lin,Mi He,Qian Tao,Zeng-Wei Zhu,Guang-Han Cao,Zhu-An Xu		
151053	P078134504	Tc by SP-heat. (dC/gamma*Tc) = 1.14. e-ph coupling = 0.41.	LuB12	B12Lu1	B	12	Lu	1																					2008																												UB12																		K		0.42					0.42																																																3.2	14				MSP151053			mJ/mol.K2	0.26	SP-heat																																						zone melting using high-frequency induction heating.					Effect of electron-phonon coupling on the superconducting transition temperature in dodecaboride superconductors: A comparison of LuB12 with ZrB12			Departement de Physique de la Matiere Condensee, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.B, 78(2008)134504	J. Teyssier,R. Lortz,A. Petrovic,D. van der Marel,V. Filippov,N. Shitsevalova		
151054	P078134508	magnetoresistance is very weak. [RESN] at 55 K.	Nd(O,F)FeAs	Nd1Fe1As1F0.18O0.82	Nd	1	Fe	1	As	1	F	0.18													O	0.82		3	2008																												oxypnictide																	ZrCuSiAs-type	K		50				2	50																																																																							mOhm.cm							0.2							m3/C	-0.00000000166					RH151054					flux method using NaCl-flux.					Hall effect and magnetoresistance in single crystals of NdFeAsO1-xFx (x=0 and 0.18)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 78(2008)134508	Peng Cheng,Huan Yang,Ying Jia,Lei Fang,Xiyu Zhu,Gang Mu,Hai-Hu Wen		
151055	JAC21700L1	resistivity measured for [100] direction. RRR=70.	LuB12	B12Lu1	B	12	Lu	1																				3	1995																												UB12																		K		0.44					0.44																																																																							uOhm.cm							0.16																		floating zone method.					Electrical resistivity and superconductivity of LaB6 and LuB12				J.Alloys Compd., 217(1995)L1	I.Bat'ko,M.Bat'kova,K.Flachbart,V.B.Filippov,Yu.B.Paderno,N.Yu.Shicevalova,Th.Wagner		
151056	JAC21700L1	not SC. resistivity measured for [100] direction. RRR=80. R shows Kondo-like increase of R below 12 K.	LaB6	B6La1	B	6	La	1																				3	1995																																														K					0.005																																																																									uOhm.cm							0.092																		floating zone method.					Electrical resistivity and superconductivity of LaB6 and LuB12				J.Alloys Compd., 217(1995)L1	I.Bat'ko,M.Bat'kova,K.Flachbart,V.B.Filippov,Yu.B.Paderno,N.Yu.Shicevalova,Th.Wagner		
151057	LTP1400339	RRR=70. Tc by SP-heat. [gamma] by fitting for T < 14K. (dC/gamma*Tc) = 1.3. gap by point contact tunneling. R = R0 + A*T^5,R0=1.6uOhm.cm, A=1.2E-9 Ohm.cm/K^5 for 1.6 < T < 30 K.	LuB12	B12Lu1	B	12	Lu	1																				3	2005																												UB12																		K		0.4					0.4																																														meV	0.06		1							mJ/mol.K2	4	SP-heat	1100	SP-heat																																				floating zone method.					Low Temperature Properties and Superconductivity of LuB12			Centre of Low Temperature Physics, Institute of Experimental Physics, Slovak Academy of Sciences, SK-04353 Kosice, Slovakia	J.Low Temp.Phys., 140(2005)339	K. Flachbart,S. Gabani,K. Gloos,M. Meissner,M. Opel,Y. Paderno,V. Pavlik,P. Samuely,E. Schuberth,N. Shitsevalova,K. Siemensmeyer,P. Szabo		
151058	LES0670167		YB6	B6Y1	B	6	Y	1																					1979																																														K		6					6																																																																																														LaB6(6N),La2O3(5N)		borothermal reaction: RO3 + 15B = 2RB6 + (3/2)B2O2					Superconductivity in the hexaborides				J.Less-Common Met., 67(1979)167	R.J.Sobczak,M.J.Sienko		
151059	LES0670167		(Y,La)B6	Y0.6La0.4B6	Y	0.6	La	0.4	B	6																			1979																																														K		4.4					4.4																																																																																														LaB6(6N),La2O3(5N)		borothermal reaction: RO3 + 15B = 2RB6 + (3/2)B2O2					Superconductivity in the hexaborides				J.Less-Common Met., 67(1979)167	R.J.Sobczak,M.J.Sienko		
151060	LES0670167		(Y,Fe)B6	Y0.9Fe0.1B6	Y	0.9	Fe	0.1	B	6																			1979																																														K		3.3					3.3																																																																																														LaB6(6N),La2O3(5N)		borothermal reaction: RO3 + 15B = 2RB6 + (3/2)B2O2					Superconductivity in the hexaborides				J.Less-Common Met., 67(1979)167	R.J.Sobczak,M.J.Sienko		
151061	LES0670167		(Y,Ce)B6	Y0.95Ce0.05B6	Y	0.95	Ce	0.05	B	6																			1979																																														K		1.6					1.6																																																																																														LaB6(6N),La2O3(5N)		borothermal reaction: RO3 + 15B = 2RB6 + (3/2)B2O2					Superconductivity in the hexaborides				J.Less-Common Met., 67(1979)167	R.J.Sobczak,M.J.Sienko		
151062	LES0670167		(Y,La)B6	Y0.5La0.5B6	Y	0.5	La	0.5	B	6																			1979																																														K		1.6					1.6																																																																																														LaB6(6N),La2O3(5N)		borothermal reaction: RO3 + 15B = 2RB6 + (3/2)B2O2					Superconductivity in the hexaborides				J.Less-Common Met., 67(1979)167	R.J.Sobczak,M.J.Sienko		
151063	PR134A385	Debye-T shows at zero-K-value. Hc2(0) shows Hc(0), type-I SC. (Ces(Tc)/gamma*Tc) = 2.44	Ga	Ga1	Ga	1																							1964																																														K		1.078					1.078																				Oe		58.9																															MSP151063			mJ/mol.K2	0.596	SP-heat	324.7	SP-heat																																									Low-temperature heat capacities of gallium, cadmium, and copper			University of California, Berkeley	Phys.Rev., 134(1964)A385	N.E.Phillips		
151064	PR134A385	Debye-T shows at zero-K-value. Hc2(0) shows Hc(0), type-I SC. (Ces(Tc)/gamma*Tc) = 2.32	Cd	Cd1	Cd	1																							1964																																														K		0.518					0.518																				Oe		29.6																															MSP151064			mJ/mol.K2	0.688	SP-heat	209	SP-heat																																									Low-temperature heat capacities of gallium, cadmium, and copper			University of California, Berkeley	Phys.Rev., 134(1964)A385	N.E.Phillips		
151065	PR137A748	lattice term of SP, beta = 1.42 mJ/mol.K4 for 0.1<T<4.2 K. Hc2(0) shows Hc(0) estimated using Hc=Hc0(1-t^2).	In	In1	In	1																							1965																																														K		3.405					3.405																				Oe		285																										3.77	14				MSP151065			mJ/mol.K2	1.69	SP-heat																																											Low-temperature heat capacities of indium and tin			University of California, Berkeley	Phys.Rev., 137(1965)A748	H.R.O'Neal,N.E.Phillips		
151066	PR137A748		Sn	Sn1	Sn	1																							1965																																														K																																																							3.45	14							mJ/mol.K2	1.78	SP-heat																																											Low-temperature heat capacities of indium and tin			University of California, Berkeley	Phys.Rev., 137(1965)A748	H.R.O'Neal,N.E.Phillips		
151067	PR1140676	Tc by SP-heat.	Al	Al1	Al	1																							1959																																														K		1.163					1.163																																																					MSP151067			mJ/mol.K2	1.35	SP-heat	427.7	SP-heat																																		Al(4N)		annealed in vac (450C,48h)					Heat capacities of aluminum between 0.1 K and 4.0 K			University of California, Berkeley	Phys.Rev., 114(1959)676	N.E.Phillips		
151068	PRL0010363	T calibrated using Laiden 1955 scale. lattice term coefficient is too small to caliculate accurate Debye-temp.	Zn	Zn1	Zn	1																							1958																																														K		0.825					0.825																																																					MSP151068			mJ/mol.K2	0.66	SP-heat																																				Zn(5N)		single crystals grown in He atmosphere.					Heat capacities of superconducting zinc			University of California, Berkeley	Phys.Rev.Lett., 1(1958)363	N.E.Phillips		
151069	SCI1591227	[isotope] = 0.09 +- 0.05.	ZrB12	B12Zr1	B	12	Zr	1																					1968																																														K		5.85					5.85						0.09	B	80																																																																																													Boron isotope effect in superconducting zirconium dodecaboride			University of California, San Diego, La Jolla	Science, 159(1968)1227	C.W.Chu,H.H.Hill		
151070	PLA0240579	Impurities: Fe=3,Ni=1, Mn=5, Si=10, Al=15, N=5 ppm. [gamma] calculated from (dHc/dT).	Be	Be1	Be	1																							1967																										A																				K		0.026					0.026																													Oe/K		68																									mJ/mol.K2	0.21																																												Superconductivity of hexagonal beryllium				Phys.Rev.Lett. A, 24(1967)579	R.L.Falge Jr.		
151071	NAT4340622	[gap] obtained by fitting using d-wave SC analysis for <71>Ga-NMR measurements.	PuCoGa5	Pu1Co1Ga5	Pu	1	Co	1	Ga	5																		3	2005																										ABC5		HoCoGa5																		K		18					18																																																8	6																																																				Unconventional superconductivity in PuCoGa5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Nature, 434(2005)622	N. J. Cur,T. Caldwell,E. D. Bauer,L. A. Morales,M. J. Graf,Y. Bang,A. V. Balatsky,J. D. Thompson,J. L. Sarrao		
151072	JPS0741710	<69>Ga, <71>Ga-NMR,NQR were measured. [gap] calculated from fitting of T1(T). Tc=9 K just after synthesis.	PuRhGa5	Pu1Rh1Ga5	Pu	1	Rh	1	Ga	5																		3	2005																										ABC5		HoCoGa5			A	4.2354		6.7939												K				8.5			8.5																																																5	6																																															Ga-flux method					Anisotropic Superconducting Gap in Transuranium Superconductor PuRhGa5: Ga NQR Study on a Single Crystal			Advanced Science Research Center, Japan Atomic Energy Research Institute, Tokai, Ibaraki 319-1195	J.Phys.Soc.Jpn, 74(2005)1710	H.Sakai,Y.Tokunaga,T.Fujimoto,S.Kambe,R.E.Walstedt,H.Yasuoka,D.Aoki,Y.Homma,E.Yamamoto,A.Nakamura,Y.Shiokawa,K.Nakajima,Y.Arai,T.D.Matsuda,Y.Haga,Y.Onuki		
151073	P064134526	<115>In, <59>Co-NMR, NQR measured. [gap] from fitting of T1(T).	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2001																										ABC5		HoCoGa5																		K		2.3					2.3																																																10	6																																															In-flux method					NMR and NQR studies of the heavy fermion superconductors CeTIn5 (T = Co and Ir)			Department of Material Science, Faculty of Science, Himeji Institute of Technology, Kamigori-cho Ako-gun, Hyogo 678-1297, Japan	Phys.Rev.B, 64(2001)134526	Y. Kohori,Y. Yamato,Y. Iwamoto,T. Kohara,E. D. Bauer,M. B. Maple,J. L. Sarrao		
151074	P064134526	<115>In, <59>Co-NMR, NQR measured. [gap] from fitting of T1(T).	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2001																										ABC5		HoCoGa5																		K		0.4					0.4																																																5	6																																															In-flux method					NMR and NQR studies of the heavy fermion superconductors CeTIn5 (T = Co and Ir)			Department of Material Science, Faculty of Science, Himeji Institute of Technology, Kamigori-cho Ako-gun, Hyogo 678-1297, Japan	Phys.Rev.B, 64(2001)134526	Y. Kohori,Y. Yamato,Y. Iwamoto,T. Kohara,E. D. Bauer,M. B. Maple,J. L. Sarrao		
151075	L101207004		SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2008																												BaAl4	I4/mmm		A	3.924		12.34												K					1.8																																																																																																SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151076	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.9Co0.1As2	Sr	1	Fe	1.9	Co	0.1	As	2																	2008																												BaAl4	I4/mmm		A	3.929		12.3321												K					1.8																																																																																																SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151077	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.85Co0.15As2	Sr	1	Fe	1.85	Co	0.15	As	2																	2008	emu/mol	0.00078																										BaAl4	I4/mmm		A	3.9272		12.3123												K					1.8																																																																									uOhm.cm											8												SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151078	L101207004	[gamma] is linear term below Tc under H=0.	Sr(Fe,Co)2As2	Sr1Fe1.8Co0.2As2	Sr	1	Fe	1.8	Co	0.2	As	2																	2008	emu/mol	0.0006																										BaAl4	I4/mmm		A	3.9278		12.3026												K				19.2			19.2	MTC151078																																																							mJ/mol.K2	12.6	SP-heat	255	SP-heat																																		SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151079	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.75Co0.25As2	Sr	1	Fe	1.75	Co	0.25	As	2																	2008	emu/mol	0.00085																										BaAl4	I4/mmm		A	3.9296		12.2925												K				18.1			18.1																																																																																														SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151080	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.7Co0.3As2	Sr	1	Fe	1.7	Co	0.3	As	2																	2008	emu/mol	0.00046																										BaAl4	I4/mmm		A	3.9291		12.2704												K				13.2			13.2																																																											255	SP-heat																																		SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151081	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.6Co0.4As2	Sr	1	Fe	1.6	Co	0.4	As	2																	2008	emu/mol	0.00036																										BaAl4	I4/mmm		A	3.9293		12.2711												K				12.9			12.9																																																																																														SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151082	L101207004		Sr(Fe,Co)2As2	Sr1Fe1.5Co0.5As2	Sr	1	Fe	1.5	Co	0.5	As	2																	2008																												BaAl4	I4/mmm		A	3.9287		12.2187												K					1.8																																																																									uOhm.cm											2												SrAs,Co2As,Fe2As		SIN(900C,16h,in Ta)					Superconducting State in SrFe2-xCoxAs2 by Internal Doping of the Iron Arsenide Layers			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett., 101(2008)207004	A. Leithe-Jasper,W. Schnelle,C. Geibel,H. Rosner		
151083	L101237003	compositions are nominal values. As-content=1-z, because As react with Ta. Hc2 defined as 0.9Rn without magnetoresistance.	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2008																												oxypnictide			A	4.0282		8.7239											ZrCuSiAs	K			28.5				28.5																				T	from (dHc2/dT) using WHH	106							T/K	resistive	5.4			HC151083																																																														Ta-foil was used to wrap the pellet					High-Field Pauli-Limiting Behavior and Strongly Enhanced Upper Critical Magnetic Fields near the Transition Temperature of an Arsenic-Deficient LaO0.9F0.1FeAs1-z Superconductor			IFW Dresden, P.O. Box 270116, D-01171 Dresden, Germany	Phys.Rev.Lett., 101(2008)237003	G. Fuchs,S.-L. Drechsler,N. Kozlova,G. Behr,A. Kohler,J. Werner,K. Nenkov,R. Klingeler,J. Hamann-Borrero,C. Hess,A. Kondrat,M. Grobosch,A. Narduzzo,M. Knupfer,J. Freudenberger,B.Buchner,L. Schultz		
151084	L101237005	THC(0)/T = 0.46 mW/cm.K2. THC(T)/T = THC(0)/T + beta*T2.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2008																												skutterudite																																																																																										MTHC151084																																				Multiband Order Parameters for the PrOs4Sb12 and PrRu4Sb12 Skutterudite Superconductors from Thermal Conductivity Measurements			Guelph-Waterloo Physics Institute and Department of Physics and Astronomy, University of Waterloo, Waterloo, Ontario, Canada	Phys.Rev.Lett., 101(2008)237005	R.W. Hill,Shiyan Li,M. B. Maple,Louis Taillefer		
151085	L101237005	THC(0)/T = 0.058 mW/cm.K2. THC(T)/T = THC(0)/T + beta*T2.	PrRu4Sb12	Pr1Ru4Sb12	Pr	1	Ru	4	Sb	12																		3	2008																												skutterudite																																																																																										MTHC151085																																				Multiband Order Parameters for the PrOs4Sb12 and PrRu4Sb12 Skutterudite Superconductors from Thermal Conductivity Measurements			Guelph-Waterloo Physics Institute and Department of Physics and Astronomy, University of Waterloo, Waterloo, Ontario, Canada	Phys.Rev.Lett., 101(2008)237005	R.W. Hill,Shiyan Li,M. B. Maple,Louis Taillefer		
151086	P078014520	Heat capacity measured. O-content determined by TGA.	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O3.908	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z	3.908	3	2008																												T'																		K		27					27																				T	from (dHc2/dT) using WHH			8.5												A			62																																																									single crystals grown by TSFZ method. samples with different Tc obtained by different ANN conditions in vac.					Impact of oxygen annealing on the heat capacity and magnetic resonance of superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 78(2008)014520	Shiliang Li,Songxue Chi,Jun Zhao,H.-H. Wen,M. B. Stone,J. W. Lynn,Pengcheng Dai		
151087	P078014520	Heat capacity measured. O-content determined by TGA.	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O3.934	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z	3.934	3	2008																												T'																		K		24					24																				T	from (dHc2/dT) using WHH			12												A			57																																																									single crystals grown by TSFZ method. samples with different Tc obtained by different ANN conditions in vac.					Impact of oxygen annealing on the heat capacity and magnetic resonance of superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 78(2008)014520	Shiliang Li,Songxue Chi,Jun Zhao,H.-H. Wen,M. B. Stone,J. W. Lynn,Pengcheng Dai		
151088	P078014520	Heat capacity measured. O-content determined by TGA.	(Pr,La,Ce)2CuO4	Pr0.88La1Ce0.12Cu1O3.947	Pr	0.88	La	1	Ce	0.12	Cu	1													O	4-z	3.947	3	2008																												T'																		K		22					22																				T	from (dHc2/dT) using WHH			15												A			47																																																									single crystals grown by TSFZ method. samples with different Tc obtained by different ANN conditions in vac.					Impact of oxygen annealing on the heat capacity and magnetic resonance of superconducting Pr0.88LaCe0.12CuO4-z			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 78(2008)014520	Shiliang Li,Songxue Chi,Jun Zhao,H.-H. Wen,M. B. Stone,J. W. Lynn,Pengcheng Dai		
151089	PHC4682403	Angular dependence of Hc2 obeys Tinkham model. [cohere] calculated using Hc2(T) = A*(1-(T/Tc)) near Tc. anisotyopy, (Hc2//ab)/(Hc2//c) = 2.1 at 2K.	YbC6	C6Yb1	C	6	Yb	1																				3	2008																												GIC																		K		6.47		6.5		0.1	6.47																																				A	resistive		370	170																																																						Yb,HOPG		vapor transport method. pellet(Yb,HOPG) - heat(400C,2d, in glass)					Anisotropic superconductivity in graphite intercalation compound YbC6			Department of Physics, Graduate School of Science, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan	Physica C, 468(2008)2403	N.F. Kawai,Hiroshi Fukuyama		
151090	MMM3210388	Mo-1212 phase(80%) is Mo0.5Sr2.2HoCu2.5Oz by SEM. impurity phase: SrMoO4. T-T curve shows two step SC transitions.	MoSr2HoCu2O8	Mo1Sr2Ho1Cu2O8	Mo	1	Sr	2	Ho	1	Cu	2													O	8			2009								13																				M1212			A	3.837		11.511											Mo-1212	K	22	27	30				27																																																																																														Mo,Ho2O3,SrCO3,CuO		mixture - pellet - heat(750C,24h,in air) - SIN(950C,24h,in O2-flow) - regrind - heat(1050C,48h,in O2-flow)					Structure, magnetic and superconducting properties of MoSr2HoCu2O8-z			aInstitute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	J.Magn,Magn,Mater., 321(2009)388	N. Balchev,K.Nenkov,G.Mihova,B.Kunev,J.Pirov,D.A.Dimitrov		
151091	P078180508	SDW temperature, T<SDW> = 139 and 129K at P=0 and 15 kbar, respectively.	(K,Sr)Fe2As2	K0.2Sr0.8Fe2As2	K	0.2	Sr	0.8	Fe	2	As	2																	2008																																														K		13					13	MTC151091																																																																																																				Pressure-induced shift of Tc in KxSr1-xFe2As2 (x=0.2, 0.4, 0.7): Analogy to the high-Tc cuprate superconductors			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)180508(R)	Melissa Gooch,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Ching-Wu Chu		
151092	P078180508		(K,Sr)Fe2As2	K0.4Sr0.6Fe2As2	K	0.4	Sr	0.6	Fe	2	As	2																	2008																																														K				37			37	MTC151092																																																																																																				Pressure-induced shift of Tc in KxSr1-xFe2As2 (x=0.2, 0.4, 0.7): Analogy to the high-Tc cuprate superconductors			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)180508(R)	Melissa Gooch,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Ching-Wu Chu		
151093	P078180508		(K,Sr)Fe2As2	K0.7Sr0.3Fe2As2	K	0.7	Sr	0.3	Fe	2	As	2																	2008																																														K		12.2					12.2	MTC151093																																																																																																				Pressure-induced shift of Tc in KxSr1-xFe2As2 (x=0.2, 0.4, 0.7): Analogy to the high-Tc cuprate superconductors			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 78(2008)180508(R)	Melissa Gooch,Bing Lv,Bernd Lorenz,Arnold M. Guloy,Ching-Wu Chu		
151094	P078174523		Nd(O,F)FeAs	Nd1Fe1As1F0.3O0.7	Nd	1	Fe	1	As	1	F	0.3													O	0.7		3	2008																												oxypnictide																	ZrCuSiAs	K			46				46																													T/K			9	1.2	HC151094		A	from (dHc2/dT)//c		23	2.6																																													m3/C	-0.0000000013								NdAs,NdF3,Fe2O3,Fe		NaCl-flux. Mass ratio of NaCl:NdFeAs(O,F) = 10:1. sealed in evacuated quartz tube - heat(1050C,10d) - cool to 850C(3C/h) - quick cool to RT					Upper critical fields and thermally-activated transport of NdFeAsO0.7F0.3 single crystal			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 78(2008)174523	J. Jaroszynski,F. Hunte,L. Balicas,Youn-jung Jo,I. Raicevic,A. Gurevich,D. C. Larbalestier,F. F. Balakirev,L. Fang,P. Cheng,Y. Jia,H. H. Wen		
151095	P078224503		FeSe0.82	Fe1Se0.8	Fe	1	Se	0.8																					2008																													P4/nmm		A	3.77		5.5204												K		10.3					10.3																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151096	P078224503		Fe(Se,Te)0.82	Fe1Se0.779Te0.041	Fe	1	Se	0.779	Te	0.041																			2008																													P4/nmm		A	3.7654		5.543												K		8.12					8.12																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151097	P078224503		Fe(Se,Te)0.82	Fe1Se0.656Te0.164	Fe	1	Se	0.656	Te	0.164																			2008																													P4/nmm		A	3.772		5.5656												K		10.7					10.7																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151098	P078224503		Fe(Se,Te)0.82	Fe1Se0.574Te0.246	Fe	1	Se	0.574	Te	0.246																			2008																													P4/nmm		A	3.7829		5.552												K		10.01					10.01																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151099	P078224503		Fe(Se,Te)0.82	Fe1Se0.492Te0.328	Fe	1	Se	0.492	Te	0.328																			2008																													P4/nmm		A	3.7824		5.9095												K		12.7					12.7																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151100	P078224503		Fe(Se,Te)0.82	Fe1Se0.41Te0.41	Fe	1	Se	0.41	Te	0.41																			2008																													P4/nmm		A	3.7933		5.9728												K		13.2					13.2																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151101	P078224503		Fe(Se,Te)0.82	Fe1Se0.328Te0.492	Fe	1	Se	0.328	Te	0.492																			2008																													P4/nmm		A	3.8021		6.0407												K		13.8					13.8	MTC151101																																																																																										MRH151101				1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151102	P078224503		Fe(Se,Te)0.82	Fe1Se0.246Te0.574	Fe	1	Se	0.246	Te	0.574																			2008																													P4/nmm		A	3.8067		6.1267												K		13.7					13.7																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151103	P078224503		Fe(Se,Te)0.82	Fe1Se0.164Te0.656	Fe	1	Se	0.164	Te	0.656																			2008																													P4/nmm		A	3.8083		6.1538												K		13.1					13.1																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151104	P078224503		Fe(Se,Te)0.82	Fe1Se0.082Te0.738	Fe	1	Se	0.082	Te	0.738																			2008																													P4/nmm		A	3.8176		6.2127												K		10.9					10.9																																																																																															1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151105	P078224503	magnetic anomaly at 125 K. R-anomaly at 65 K.	Fe(Se,Te)0.82	Fe1Te0.82	Fe	1	Te	0.82																					2008																													P4/nmm		A	3.8202		6.2443												K					2																																																																																													MRH151105				1	mixture - pellet - sealed in evacuated quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Superconductivity close to magnetic instability in Fe(Se1-xTex)0.82			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 78(2008)224503	M. H. Fang,H. M. Pham,B. Qian,T. J. Liu,E. K. Vehstedt,Y. Liu,L. Spinu,Z. Q. Mao		
151106	PRB078224512	T<SDW> = 200 K. dC = 185 J/mol.K. latent heat = 463 j/mol corresponding to structural and SDW transitions. anisotropy Rc/Rab = 130 at 25K.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2008																																														K					1.8																																																										mJ/mol.K2	6.5	SP-heat	245	SP-heat																															MRH151106	/cm3	15000000000000000000000			high-T solution method using Sn-flux.					Transport and anisotropy in single-crystalline SrFe2As2 and A0.6K0.4Fe2As2 (A=Sr, Ba) superconductors			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 78(2008)224512	G. F. Chen,Z. Li,J. Dong,G. Li,W. Z. Hu,X. D. Zhang,X. H. Song,P. Zheng,N. L. Wang,J. L. Luo		
151107	PRB078224512	(dC/Tc) = 48 mJ/mol.K2. anisotropy Rc/Rab = 21, (Hc2//ab)/(Hc2//c) = 2.0	(Sr,K)Fe2As2	Sr0.6K0.4Fe2As2	Sr	0.6	K	0.4	Fe	2	As	2																	2008																																														K		35.6					35.6																				T	resistivity. 0.9Rn		185.4	93.1					T/K	resistivity		7.57	3.8	MHC151107																																																														high-T solution method using Sn-flux.					Transport and anisotropy in single-crystalline SrFe2As2 and A0.6K0.4Fe2As2 (A=Sr, Ba) superconductors			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 78(2008)224512	G. F. Chen,Z. Li,J. Dong,G. Li,W. Z. Hu,X. D. Zhang,X. H. Song,P. Zheng,N. L. Wang,J. L. Luo		
151108	PRB078224512		(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2008																																														K		38					38																																																																																																high-T solution method using FeAs-flux. Sr or Ba & K:FeAs = 0.5:1.4 in alumina crucible - sealed in Ta(1.6atm Ar) - heat(1150C,5h) - cool to 800C(within 50h)					Transport and anisotropy in single-crystalline SrFe2As2 and A0.6K0.4Fe2As2 (A=Sr, Ba) superconductors			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 78(2008)224512	G. F. Chen,Z. Li,J. Dong,G. Li,W. Z. Hu,X. D. Zhang,X. H. Song,P. Zheng,N. L. Wang,J. L. Luo		
151109	PRL101107006		(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2008																												ThCr2Si2	I4/mmm		A	3.917		13.2968												K	37.2	38.1	39	38.3		1.5	38.1																																																																																																mixture - heat to 873K(50K/h) in alumina(Ar) - ANN(925K,15h) - SIN(1023K,12h)					Superconductivity at 38 K in the Iron Arsenide (Ba1-xKx)Fe2As2			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.Lett., 101(2008)107006	Marianne Rotter,Marcus Tegel,Dirk Johrendt		
151110	PRL102017002	underdoped sample. 28GHz microwave measurements. (2d/kTc) > 1.6 for all Fermi surface.	PrOFeAs	Pr1Fe1As1O1-z	Pr	1	Fe	1	As	1															O	1-z		3	2009																												oxypnictide																		K		35					35																																									A	microwave		2800				4	7																																															high-P synthesis. nominal(PrFeAsO0.6) - heat(1300C,2h,P=2GPa in BN crucible)					Microwave Penetration Depth and Quasiparticle Conductivity of PrFeAsO1-y Single Crystals: Evidence for a Full-Gap Superconductor			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.Lett., 102(2009)017002	K. Hashimoto,T. Shibauchi,T. Kato,K. Ikada,R. Okazaki,H. Shishido,M. Ishikado,H. Kito,A. Iyo,H. Eisaki,S. Shamoto,Y. Matsuda		
151111	PRB079014522	ANN(300C). lattice term of SP: beta = 0.463 mJ/mol.K4. (dC/kTc) = 1.3	FeSe	Fe1.01Se1	Fe	1.01	Se	1																					2009																													P4/nmm		A	3.7734		5.5258											beta-FeSe	K		8.5					8.5	MTC151111																																																							mJ/mol.K2	5.4	SP-heat	200	SP-heat																																				(Fe,Se) - sealed in silica tube - heat(750C,5d until Se vapor disappeaed) - heat(1075C,3d) - fast cool to 420C - Q to (-13C) - ANN(300-500C,2d) - Q to (-13C)					Extreme sensitivity of superconductivity to stoichiometry in Fe1+zSe			1Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 79(2009)014522	T. M. McQueen,Q. Huang,V. Ksenofontov,C. Felser,Q. Xu,H. Zandbergen,Y. S. Hor,J. Allred,A. J. Williams,D. Qu,J. Checkelsky,N. P. Ong,R. J. Cava		
151112	PRB079014522	ANN(380C)	FeSe	Fe1.02Se1	Fe	1.02	Se	1																					2009																													P4/nmm																beta-FeSe	K		6					6																																																																																																(Fe,Se) - sealed in silica tube - heat(750C,5d until Se vapor disappeaed) - heat(1075C,3d) - fast cool to 420C - Q to (-13C) - ANN(300-500C,2d) - Q to (-13C)					Extreme sensitivity of superconductivity to stoichiometry in Fe1+zSe			1Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 79(2009)014522	T. M. McQueen,Q. Huang,V. Ksenofontov,C. Felser,Q. Xu,H. Zandbergen,Y. S. Hor,J. Allred,A. J. Williams,D. Qu,J. Checkelsky,N. P. Ong,R. J. Cava		
151113	PRB079014522	ANN(400C). lattice term of SP: beta = 0.496 mJ/mol.K4	FeSe	Fe1.03Se1	Fe	1.03	Se	1																					2009																													P4/nmm																beta-FeSe	K					0.6																																																										mJ/mol.K2	1.3	SP-heat																																						(Fe,Se) - sealed in silica tube - heat(750C,5d until Se vapor disappeaed) - heat(1075C,3d) - fast cool to 420C - Q to (-13C) - ANN(300-500C,2d) - Q to (-13C)					Extreme sensitivity of superconductivity to stoichiometry in Fe1+zSe			1Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 79(2009)014522	T. M. McQueen,Q. Huang,V. Ksenofontov,C. Felser,Q. Xu,H. Zandbergen,Y. S. Hor,J. Allred,A. J. Williams,D. Qu,J. Checkelsky,N. P. Ong,R. J. Cava		
151114	PRB079014519	The best fit (Rietveld) is FeSe0.99. Structural transition(tetra-to-ortho) at 60-80 K. Low-Temp phase: space-G = Cmme, a=5.3081, b=5.3354, c=5.4879 at 6K.	FeSe	Fe1Se0.72	Fe	1	Se	0.72																					2009																													P4/nmm		A	3.7724		5.5217												K		8					8																																																																																																(Fe,Se powder) - mixture - sealed in tube - heat(670C,13h, in vac) - heat(670C,24h) - hold(400C,36h)					Neutron scattering measurements of the phonon density of states of FeSe1-x superconductors			NIST Center for Neutron Research, National Institute of Standards and Technology, Gaithersburg, Maryland 20899, USA	Phys.Rev.B, 79(2009)014519	D.Phelan,J.N.Millican,E.L.Thomas,J.B.Leao,Y.Qiu,R.Paul		
151115	PRB079012504	not SC. T<SDW> = 170 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2009																												ThCr2Si2	I4/mmm		A	3.8942		11.746												K					4.2																																																																																																		high-T solution method using Sn-flux. nominal composition, Ca:(Fe,Co):As:Sn = 1:2:2:19. sealed in quart - heat(1050C,24h)  - cool to 450C(3 weeks) - rapid cool to RT					Anisotropic magnetic and superconducting properties of CaFe2-xCoxAs2 (x=0, 0.06) single crystals			Department of Condensed Matter Physics and Material Sciences, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 79(2009)012504	Neeraj Kumar,R. Nagalakshmi,R. Kulkarni,P. L. Paulose,A. K. Nigam,S. K. Dhar,A. Thamizhavel		
151116	PRB079012504	parallel H means H//[100] . normal means H//[001]	Ca(Fe,Co)2As2	Ca1Fe2.94Co0.06As2	Ca	1	Fe	2.94	Co	0.06	As	2																3	2009																												ThCr2Si2	I4/mmm		A	3.8875		11.687												K				17			17										60										T	resistivity, WHH		22	17					T/K	resistivity		1.82	1.43	MHC151116		A			40																																																									high-T solution method using Sn-flux. nominal composition, Ca:(Fe,Co):As:Sn = 1:2:2:19. sealed in quart - heat(1050C,24h)  - cool to 450C(3 weeks) - rapid cool to RT					Anisotropic magnetic and superconducting properties of CaFe2-xCoxAs2 (x=0, 0.06) single crystals			Department of Condensed Matter Physics and Material Sciences, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 79(2009)012504	Neeraj Kumar,R. Nagalakshmi,R. Kulkarni,P. L. Paulose,A. K. Nigam,S. K. Dhar,A. Thamizhavel		
151117	LTP0680147	RRR=3.7. G-L = 19.4.	ScRu4B4	Sc1Ru4B4	Sc	1	Ru	4	B	4																		1	1987																										AB4C4		RT4B4	I4<1>/acd		A	7.357		14.924											LuRu4B4 type	K	7.1	7.34	7.7				7.34																				T	resistivity, WHH	3.95							T/K	resistivity	0.777			MHC151117		A		718																																	mOhm.cm							0.038																		arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151118	LTP0680147	RRR=1.4. G-L = 38.4.	LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																		1	1987																										AB4C4		RT4B4	I4<1>/acd		A	7.445		14.851											LuRu4B4 type	K	8.05	8.28	8.37				8.28																				T	resistivity, WHH	8.66							T/K	resistivity	1.51					A		762																																	mOhm.cm							0.077																		arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151119	LTP0680147	RRR=1.8. G-L = 10.5.	ThRh4B4	Th1Rh4B4	Th	1	Rh	4	B	4																		1	1987																										AB4C4		RT4B4	P4<2>/nnc		A	5.358		7.546											CeCo4B4 type	K	4.41	4.69	4.62				4.69																				T	resistivity, WHH	0.75							T/K	resistivity	0.239					A		4129																																	mOhm.cm							0.036																		arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151120	LTP0680147	G-L = 7.2.	YRh4B4	Y1Rh4B4	Y	1	Rh	4	B	4																		1	1987																										AB4C4		RT4B4	P4<2>/nnc		A	5.308		7.403											CeCo4B4 type	K		10.6					10.6																				T	resistivity, WHH	2.1							T/K	resistivity	0.286					A		585																																																										arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151121	LTP0680147	G-L = 5.4.	LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																		1	1987																										AB4C4		RT4B4	P4<2>/nnc		A	5.294		7.359											CeCo4B4 type	K		11.45					11.45																				T	resistivity, WHH	1.78							T/K	resistivity	0.224					A		492																																																										arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151122	LTP0680147	RRR=6.6. G-L = 19.1.	LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	1987																												LuRuB2	Pnma		A	5.815	5.23	6.29												K	10.4	10.6	10.7				10.6																				T	resistivity, WHH	5.73							T/K	resistivity	0.78			MHC151122		A		130																																	mOhm.cm							0.037																		arc-melting - sealed in Ta tube - ANN(1250C,2d,in quartz) - ANN(1000C,10-12d)					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151123	LTP0680147	RRR=12.4. G-L = 12.6.	YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																		1	1987																												LuRuB2	Pnma		A	5.91	5.306	6.363												K	7.61	7.7	8.07				7.7																				T	resistivity, WHH	4.8							T/K	resistivity	0.62			MHC151123		A		83																																	mOhm.cm							0.013																		arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151124	LTP0680147	RRR=6.5. G-L = 15.8.	LuOs3B2	Lu1Os3B2	Lu	1	Os	3	B	2																		1	1987																												CeCo3B2	P6/mmm		A	5.455		3.064												K	4.57	4.69	4.73				4.69																				T	resistivity, WHH	1.93							T/K	resistivity	0.595			MHC151124		A		1635																																	mOhm.cm							0.033																		arc-melting					Comparative critical field study of superconducting ternary borides				J.Low Temp. Phys, 68(1987)147	W.H.Lee,S.Appl,R.N.Shelton		
151125	PRB079012505	impurity phases: LaNiPO(10.0%), LaNi5P3(6.1%). coefficient of lattice term and Schottky in SP-heat are 0.14 mJ/mol-Ni.K4 and 0.49 mJ/mol-Ni.K. (dC/gamma*Tc) = 1.25	La3Ni4P4O2	La3Ni4P4O2	La	3	Ni	4	P	4															O	2		1	2009																												oxypnictide	I4/mmm	139	A	4.0107		26.1811											Pr3Cu4P4O2 type	K				2.2			2.2											Oe	deviation from linear M	520			90			1.9	T	resistivity, WHH	0.6							T/K	resistivity	0.31					A		240			A	estimation from Hc1	550													mJ/Ni.K2	6.2	SP-heat	360	SP-heat																																		Ni5P4,P,La2O3		mixture - pellet - alumina crucible in quartz tube - heat(750C to 1050C,overnight) - addition of 2% excess P - heat(1200C,overnight)					Superconductivity at 2.2 K in the layered oxypnictide La3Ni4P4O2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)012505	T. Klimczuk,T. M. McQueen,A. J. Williams,Q. Huang,F. Ronning,E. D. Bauer,J. D. Thompson,M. A. Green,R. J. Cava		
151126	PRB079014506	Co-content from EPMA.	Ba(Fe,Co)2As2	Ba1Fe1.91Co0.09As2	Ba	1	Fe	1.91	Co	0.09	As	2																3	2009																																														K				14.5			14.5	MTC151127																																																																																															self-flux method. Ba:As=1:4. (Ba,FeAs,Co) - heat(1150C,24h) - slow cool to 1000C.					Determination of the phase diagram of the electron-doped superconductor Ba(Fe1-xCox)2As2			Geballe Laboratory for Advanced Materials and Department of Applied Physics, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)014506	Jiun-Haw Chu,James G. Analytis,Chris Kucharczyk,Ian R. Fisher		
151127	PRB079014506	Co-content from EPMA. optimal Co content. (dC/Tc) = 23 mJ/mol.K2. SC for 0.05 < x < 0.368.	Ba(Fe,Co)2As2	Ba1Fe1.878Co0.122As2	Ba	1	Fe	1.878	Co	0.122	As	2																3	2009																																														K				24			24	MTC151127																																																																																															self-flux method. Ba:As=1:4. (Ba,FeAs,Co) - heat(1150C,24h) - slow cool to 1000C.					Determination of the phase diagram of the electron-doped superconductor Ba(Fe1-xCox)2As2			Geballe Laboratory for Advanced Materials and Department of Applied Physics, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)014506	Jiun-Haw Chu,James G. Analytis,Chris Kucharczyk,Ian R. Fisher		
151128	PRB079014506	Co-content from EPMA.	Ba(Fe,Co)2As2	Ba1Fe1.782Co0.218As2	Ba	1	Fe	1.782	Co	0.218	As	2																3	2009																																														K				14.1			14.1	MTC151127																																																																																															self-flux method. Ba:As=1:4. (Ba,FeAs,Co) - heat(1150C,24h) - slow cool to 1000C.					Determination of the phase diagram of the electron-doped superconductor Ba(Fe1-xCox)2As2			Geballe Laboratory for Advanced Materials and Department of Applied Physics, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)014506	Jiun-Haw Chu,James G. Analytis,Chris Kucharczyk,Ian R. Fisher		
151129	PRB079014514	under-doped sample. RRR=2.7. anisotropy = 2.7(24.8K) - 4.0(26.8K) from Hc2. vortex-glass transition at 20.7 K.	(Ba,K)Fe2As2	Ba0.64K0.36Fe2As2	Ba	0.64	K	0.36	Fe	2	As	2																3	2009																												ThCr2Si2																		K			26.2	25.6		1.2	25.6																													T/K	resistivity		6.58	3.14	MHC151129																850000																					mOhm.cm							0.4																		Sn-flux method. nominal molar volume:  Ba:K:Fe:As:Sn=0.6:0.8:2:20 - heat(850C) - cool(4C/h)					Vortex-glass phase transition and superconductivity in an underdoped (Ba,K)Fe2As2 single crystal			Department of Physics and Astronomy, CSCMR & FPRD, Seoul National University, Seoul 151-747, Republic of Korea	Phys.Rev.B, 79(2009)014514	Hyeong-Jin Kim,Yong Liu,Yoon Seok Oh,Seunghyun Khim,Ingyu Kim,G. R. Stewart,Kee Hoon Kim		
151130	PRB079020508	F-concentration not given. anisotropy = 4.0(penetration depth), =5.5(coherence length).	Nd(O,F)FeAs	Nd1Fe1As1F0.2O0.8	Nd	1	Fe	1	As	1	F	0.2													O	0.8		3	2009																												oxypnictide																		K		32.6					32.6											Oe	magnetization		40	140					T	SP-heat, WHH		170	85										HC151130							A			2700	12000																																																			high pressure synthesis using cubic multianvil apparatus.					Upper and lower critical magnetic fields of superconducting NdFeAsO1-xFx single crystals studied by Hall-probe magnetization and specific heat			Institut Neel, CNRS, BP 166, 38042 Grenoble Cedex 9, France	Phys.Rev.B, 79(2009)020508	Z. Pribulova,T. Klein,J. Kacmarcik,C. Marcenat,M. Konczykowski,S. L. Bud'ko,M. Tillman,P. C. Canfield		
151131	JPS078023701	Tc(P=0) not given. Tc in DB shows the extraporated value. Tc(max) = 8.8K  at P=0.8GPa.  a/a0 = 0.955, c/c0 = ** at P=10GPa. compressibility k = 10.4E-3 /GPa.	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2009																												oxypnictide													(GPa)^(-1)	0.00274		0.00495		K		4.8					4.8	TC151131		K/GPa	4																																																																																												solid state reaction					Pressure Study of Superconducting Oxypnictide LaFePO			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajousui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 78(2009)023701	K.Igawa,H.Okada,K.Arii,H.Takahashi,Y.Kamihara,M.Hirano,H.Hosono,S.Nakano,T.Kikegawa		
151132	JPS078023702	RRR=2.6. Hc2 defined as midpoint. anisotropy = 3-4 derived from Hc2. Jc > 1E+5 A/cm2 for T < 17K.	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2009																												ThCr2Si2																		K				24			24																				T	resistivity, WHH		8.5	28					T/K	resistivity		5.21	1.68	MHC151132																																																			cm3/C	-0.00122					MRH151132					FeAs/CoAs self flux method. mixture(Ba:FeAs:CoAs = 1:4.5:0.5) - (placed in almina crucible) - heat(1150C,10h) - slow cool to 1090C(1.3 C/h)					Possible Superconductivity above 25K in Single-Crystalline Co-Doped BaFe2As2			Department of Applied Physiscs, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656	J.Phys.Soc.Jpn, 78(2009)023702	Y.Nakajima,T.Taen,T.Tamegai		
151133	LES0620251	lattice term of SP: beta=0.2 mJ/mol.K4. e-ph coupling = 0.63.	LuRh4B4	Lu1Rh4B4	Lu	1	Rh	4	B	4																			1978																										AB4C4		RT4B4																	LuRh4B4 type	K				11.5			11.5																				T		6.5																																mJ/mol.K	474	mJ/mol.K2	24	SP-heat	444	SP-heat																																				arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151134	LES0620251	Tc and Tm by ac-SUS. x<crit> = 0.92.	(Lu,Ho)Rh4B4	Lu0.5Ho0.5Rh4B4	Lu	0.5	Ho	0.5	Rh	4	B	4																	1978																										AB4C4		RT4B4																	LuRh4B4 type	K		8.43					8.43	MPH151134																																																																																															arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151135	LES0620251	Tc and Tm by ac-SUS. x<crit> = 0.92.	(Lu,Ho)Rh4B4	Lu0.255Ho0.745Rh4B4	Lu	0.255	Ho	0.745	Rh	4	B	4																	1978																										AB4C4		RT4B4																	LuRh4B4 type	K								MPH151134																																																																																															arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151136	LES0620251	Tc and Tm by ac-SUS. x<crit> = 0.92.	(Lu,Ho)Rh4B4	Lu0.099Ho0.901Rh4B4	Lu	0.099	Ho	0.901	Rh	4	B	4																	1978																										AB4C4		RT4B4																	LuRh4B4 type	K								MPH151134																																																																																															arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151137	LES0620251	Tc and Tm by ac-SUS. x<crit> = 0.92.	(Lu,Ho)Rh4B4	Lu0.067Ho0.933Rh4B4	Lu	0.067	Ho	0.933	Rh	4	B	4																	1978																										AB4C4		RT4B4																	LuRh4B4 type	K																																																																																																							arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151138	LES0620251		HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1978							2	6.7																		AB4C4		RT4B4																	LuRh4B4 type	K																																																																																																							arc-melting  - sealed in Ta tube - ANN(1150C,2w + 900C,1h  + 800C,1w)					Interaction between superconductivity and magnetism in the pseudoternary system (Lu1-xHox)Rh4B4			University of California, San Diego,	J.Less-Common Metals, 62(1978)251	M.B.Maple,H.C.Hamaker,D.C.Johnston,H.B.Mackay,L.D.Woolf		
151139	APL093152505	impurity phase = NiAs-type FeSe. (dTc/dP) for Tc(on). Hc2, Hirr defined as Tc(on) and Tc(zero), respectively. Hc2(0) defined as Tcon = 72 T for P=1.48 GPa	FeSe	Fe1Se1	Fe	1	Se	1																					2008																													P4/nmm		A	3.7696		5.52												K	7.5	9.45	13.5	8			9.45	MTC151139		K/GPa	9.1						11										T	resistivity, linear extraporation	28												MHC151139																																																												Fe,Se	1	solid state reaction. mixture(Fe,Se powder) - (sealed in evacuated quartz tube) - heat(680C,12h) - reground - pellet -heat(680C,12-30h)					Superconductivity at 27 K in tetragonal FeSe under high pressure			National Institute for Materials Science, 1-2-1, Sengen, Tsukuba 305-0047, Japan	Appl.Phys.Lett., 93(2008)152505	Yoshikazu Mizuguchi,Fumiaki Tomioka,Shunsuke Tsuda,Takahide Yamaguchi,Yoshihiko Takano		
151140	SSC1490467		Nb5(Si,B)3	Nb5Si2.8B0.2	Nb	5	Si	2.8	B	0.2																			2009																												Cr5Si3			A	6.5288		11.829											alpha-Nb5Si3 type	K			5.9				5.9																																																																																														Nb,B,Si powder		mixture - (saled in quartz tube) - heat(1200C, 100h) - (reground) - pellet - heat(1700C,11h)					Superconductivity in the new Nb5Si3-xBx phase			Departamento de Engenharia de Materiais, EEL-USP, Lorena 12600970, SP, Brazil	Solid State Commun., 149(2009)467	A. Brauner,C.A. Nunes,A.D. Bortolozo,G. Rodrigues,A.J.S. Machado		
151141	SSC1490467		Nb5(Si,B)3	Nb5Si2.6B0.4	Nb	5	Si	2.6	B	0.4																			2009																												Cr5Si3			A	6.4895		11.787											alpha-Nb5Si3 type	K			6.4				6.4																																																																																														Nb,B,Si powder		mixture - (saled in quartz tube) - heat(1200C, 100h) - (reground) - pellet - heat(1700C,11h)					Superconductivity in the new Nb5Si3-xBx phase			Departamento de Engenharia de Materiais, EEL-USP, Lorena 12600970, SP, Brazil	Solid State Commun., 149(2009)467	A. Brauner,C.A. Nunes,A.D. Bortolozo,G. Rodrigues,A.J.S. Machado		
151142	SSC1490467		Nb5(Si,B)3	Nb5Si2.4B0.6	Nb	5	Si	2.4	B	0.6																			2009																												Cr5Si3			A	6.4503		11.748											alpha-Nb5Si3 type	K			7.8			0.5	7.8										32										T		4.2														A		88.6																																																								Nb,B,Si powder		mixture - (saled in quartz tube) - heat(1200C, 100h) - (reground) - pellet - heat(1700C,11h)					Superconductivity in the new Nb5Si3-xBx phase			Departamento de Engenharia de Materiais, EEL-USP, Lorena 12600970, SP, Brazil	Solid State Commun., 149(2009)467	A. Brauner,C.A. Nunes,A.D. Bortolozo,G. Rodrigues,A.J.S. Machado		
151143	SSC1490467		Nb5(Si,B)3	Nb5Si2.2B0.8	Nb	5	Si	2.2	B	0.8																			2009																												Cr5Si3			A	6.4096		11.705											alpha-Nb5Si3 type	K			6.6				6.6																																																																																														Nb,B,Si powder		mixture - (saled in quartz tube) - heat(1200C, 100h) - (reground) - pellet - heat(1700C,11h)					Superconductivity in the new Nb5Si3-xBx phase			Departamento de Engenharia de Materiais, EEL-USP, Lorena 12600970, SP, Brazil	Solid State Commun., 149(2009)467	A. Brauner,C.A. Nunes,A.D. Bortolozo,G. Rodrigues,A.J.S. Machado		
151144	SSC1490467		Nb5(Si,B)3	Nb5Si2B1	Nb	5	Si	2	B	1																			2009																												Cr5Si3			A	6.3834		11.68											alpha-Nb5Si3 type	K			6.4				6.4																																																																																														Nb,B,Si powder		mixture - (saled in quartz tube) - heat(1200C, 100h) - (reground) - pellet - heat(1700C,11h)					Superconductivity in the new Nb5Si3-xBx phase			Departamento de Engenharia de Materiais, EEL-USP, Lorena 12600970, SP, Brazil	Solid State Commun., 149(2009)467	A. Brauner,C.A. Nunes,A.D. Bortolozo,G. Rodrigues,A.J.S. Machado		
151145	SSC1490448		LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																			2009																												CeNiC2	Amm2		A	3.954	4.557	6.193												K	3.06		3.51	2.99			2.99																																																					MSP151145			mJ/mol.K2	8.23																																							arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151146	SSC1490448		(La,Y)NiC2	La0.95Y0.05Ni1C2	La	0.95	Y	0.05	Ni	1	C	2																	2009																												CeNiC2	Amm2		A	3.938	4.554	6.188												K	2.82		2.98	2.79			2.79																																																																																																arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151147	SSC1490448		(La,Y)NiC2	La0.9Y0.1Ni1C2	La	0.9	Y	0.1	Ni	1	C	2																	2009																												CeNiC2	Amm2		A	3.919	4.551	6.178												K	2.36		2.77	2.29			2.29																																																																																																arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151148	SSC1490448		(La,Y)NiC2	La0.85Y0.15Ni1C2	La	0.85	Y	0.15	Ni	1	C	2																	2009																												CeNiC2	Amm2		A	3.899	4.547	6.172												K	2.13		2.54	2.08			2.08																																																																																																arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151149	SSC1490448		(La,Y)NiC2	La0.8Y0.2Ni1C2	La	0.8	Y	0.2	Ni	1	C	2																	2009																												CeNiC2	Amm2		A	3.877	4.544	6.162												K		1.26					1.26																																																								mJ/mol.K2	6.47																																							arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151150	SSC1490448	two SC phases	(La,Y)NiC2	La0.75Y0.25Ni1C2	La	0.75	Y	0.25	Ni	1	C	2																	2009																												CeNiC2	Amm2		A	3.856	4.539	6.15												K		1.65					1.65																																																								mJ/mol.K2	6.45																																							arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151151	SSC1490448		YNiC2	Y1Ni1C2	Y	1	Ni	1	C	2																			2009																												CeNiC2	Amm2		A	3.568	4.5	6.02												K					1.5																																																																																																		arc-melting - ANN(1000C,7d)					Alloying effects of Y on Tc in superconducting (La1-xYx)NiC2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 149(2009)448	T.F. Liao,H.H. Sung,K.J. Syu,W.H. Lee		
151152	SSC1490181		CeO(Fe,Co)As	Ce1Fe0.9Co0.1As1O1	Ce	1	Fe	0.9	Co	0.1	As	1													O	1			2009																												oxypnictide	P4/nmm																	K			11.3	10		1.3	10																				T	resistivity, WHH	45.22							T/K	resistivity	5.8																																																															Ce,As,CeO2,Co3O4,FeAs		mixture - (sealed in silica ampoule) - heat(950C,24h) - (wrapped in Ta-foil) -  (sealed in silica ampoule) - heat(1180C,48h)					Superconductivity at 11.3 K induced by cobalt doping in CeFeAsO			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Solid State Commun., 149(2009)181	J. Prakash,S.J. Singh,S. Patnaik,A.K. Ganguli		
151153	SSC1490181	R not to zero down to 4.2 K.	CeO(Fe,Co)As	Ce1Fe0.85Co0.15As1O1	Ce	1	Fe	0.85	Co	0.15	As	1													O	1			2009																												oxypnictide	P4/nmm																	K			5				5																																																																																														Ce,As,CeO2,Co3O4,FeAs		mixture - (sealed in silica ampoule) - heat(950C,24h) - (wrapped in Ta-foil) -  (sealed in silica ampoule) - heat(1180C,48h)					Superconductivity at 11.3 K induced by cobalt doping in CeFeAsO			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Solid State Commun., 149(2009)181	J. Prakash,S.J. Singh,S. Patnaik,A.K. Ganguli		
151154	JPS078023706	(dC/gamma*Tc) = 0.87. latticeterm of SP = 0.54 mJ/mol.K4(beta)	BaRh2P2	Ba1Rh2P2	Ba	1	Rh	2	P	2																			2009	emu/mol	0.000134																										ThCr2Si2	I4/mmm		A	3.939		12.576												K		1					1																				T	resistivity, WHH	0.07							T/K	resistivity	1.13					A		690																		mJ/mol.K2	9.75	SP-heat	268	SP-heat																																				solid state reaction.  mixture(Ba,Rh(Ir),P-powder) - heat(400C,16h + 1000C,16h, in evacuated silica tube)					Superconductivity in Layered Pnictides BaRh2P2 and BaIr2P2			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561	J.Phys.Soc.Jpn, 78(2009)023706	D.Hirai,T.Takayama,R.Higashinaka,H.Aruga-Katori,H.Takagi		
151155	JPS078023706	(dC/gamma*Tc) = 1.53. latticeterm of SP = 0.390 mJ/mol.K4(beta)	BaIr2P2	Ba1Ir2P2	Ba	1	Ir	2	P	2																			2009	emu/mol	0.000121																										ThCr2Si2	I4/mmm		A	3.946		12.572												K		2.1					2.1																				T	resistivity, WHH	0.14							T/K	resistivity	1.05					A		480																		mJ/mol.K2	6.86	SP-heat	292	SP-heat																																				solid state reaction.  mixture(Ba,Rh(Ir),P-powder) - heat(400C,16h + 1000C,16h, in evacuated silica tube)					Superconductivity in Layered Pnictides BaRh2P2 and BaIr2P2			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561	J.Phys.Soc.Jpn, 78(2009)023706	D.Hirai,T.Takayama,R.Higashinaka,H.Aruga-Katori,H.Takagi		
151156	PHC4690082	impurity phases=CeAs,Fe2As.  RRR = 4.34.	Ce(O,F)FeAs	Ce1Fe1As1F0.1O0.9	Ce	1	Fe	1	As	1	F	0.1													O	0.9			2009																												oxypnictide	P4/nmm		A	3.991		8.613												K			38.4	38.2		2	38.2										75										T	resistivity, WHH	94							T/K	resistivity	3.52					A		19																																																								Ce,CeO2,CeF3,FeAs		mixture - heat(1000C,48h, in vac) - pellet - wrapped in Ta-foil  - heat(1180C,48h, in evacuated silica tube)					Superconductivity in CeO1-xFxFeAs with upper critical field of 94 T			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Physica C, 469(2009)82	J. Prakash,S.J. Singh,S. Patnaik,A.K. Ganguli		
151157	PHC4690082	impurity phases=CeAs,Fe2As.  RRR = 6.67.	Ce(O,F)FeAs	Ce1Fe1As1F0.2O0.8	Ce	1	Fe	1	As	1	F	0.2													O	0.8			2009																												oxypnictide	P4/nmm		A	3.988		8.607												K			42.5	40.4		7	40.4																				T	resistivity, WHH	43							T/K	resistivity	1.45					A		27																												uV/K	-21																											Ce,CeO2,CeF3,FeAs		mixture - heat(1000C,48h, in vac) - pellet - wrapped in Ta-foil  - heat(1180C,48h, in evacuated silica tube)					Superconductivity in CeO1-xFxFeAs with upper critical field of 94 T			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Physica C, 469(2009)82	J. Prakash,S.J. Singh,S. Patnaik,A.K. Ganguli		
151158	JET0221167	lathe-turned polycrystalline sample	Ti	Ti1	Ti	1																							1966																																														K		0.34					0.34			K/GPa	0.069																																																																																																	Investigation of the effects of hydrostatic pressure and plastic deformation on the superconducting properties of titanium			Moscow State University	Soviet Phys. JETP, 22(1966)1167	N.B.Brandt,N.I.Ginsburg		
151159	JET0240040		(Mo,Re)	Mo0.9Re0.1	Mo	0.9	Re	0.1																					1967																																														K		2.92					2.92			K/GPa	0																																																																																												heat by high-frequency furnace					The effect of high pressure on the superconducting transition temperature of alloys Mo90Re10 and Nb75Mo25			Moscow State University	Soviet Phys. JETP, 24(1967)40	N.B.Brandt,N.I.Ginsburg		
151160	JET0240040		(Nb,Mo)	Mo0.25Nb0.75	Mo	0.25	Nb	0.75																					1967																																														K		3.47					3.47			K/GPa	-0.04																																																																																												heat by high-frequency furnace					The effect of high pressure on the superconducting transition temperature of alloys Mo90Re10 and Nb75Mo25			Moscow State University	Soviet Phys. JETP, 24(1967)40	N.B.Brandt,N.I.Ginsburg		
151161	JPM0182955		GdBa2Cu3Oz	Gd1Ba2Cu3Oz	Gd	1	Ba	2	Cu	3															O	z			2006																												Y123																		K			90.52				90.52																																																						mJ/mol.K	4.1																																							Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151162	JPM0182955	R(100K) = 0.3 mOhm.cm	GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.985Mn0.015Oz	Gd	1	Ba	2	Cu	2.985	Mn	0.015													O	z			2006																												Y123																		K			91				91																																																						mJ/mol.K	3.5																																							Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151163	JPM0182955		GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.97Mn0.03Oz	Gd	1	Ba	2	Cu	2.97	Mn	0.03													O	z			2006																												Y123																		K			86.18				86.18	TC151163																																																																																													Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151164	JPM0182955		GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.94Mn0.06Oz	Gd	1	Ba	2	Cu	2.94	Mn	0.06													O	z			2006																												Y123																		K			71.08				71.08																																																																																														Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151165	JPM0182955		YBa2Cu3Oz	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			2006																												Y123																		K			91.58				91.58																																																						mJ/mol.K	5.7																																							Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151166	JPM0182955		YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.985Mn0.015Oz	Y	1	Ba	2	Cu	2.985	Mn	0.015													O	z			2006																												Y123																		K			92.41				92.41	TC151163																																																																																													Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151167	JPM0182955		YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.97Mn0.03Oz	Y	1	Ba	2	Cu	2.97	Mn	0.03													O	z			2006																												Y123																		K			92.17				92.17																																																																																														Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151168	JPM0182955		YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.94Mn0.06Oz	Y	1	Ba	2	Cu	2.94	Mn	0.06													O	z			2006																												Y123																		K			91.11				91.11																																																																																														Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Effect of Mn doping on the specific heat of the high Tc  superconductor REBa2Cu3Oy (RE = Y, Gd)			Department of Physics, Sikkim Manipal Institute of Technology, Majitar, Rangpo, Sikkim-737132, India	J.Phys. Condens.Matter, 18(2006)2955	Ashok Rao,S Radheshyam,Anirban Das,Bhasker Gahtori,S K Agarwal,Y F Lin,K M Sivakumar,Y-K Kuo		
151169	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	YBa2Cu3Oz	Y1Ba2Cu3Oz	Y	1	Ba	2	Cu	3															O	z			2007																												Y123																		K		91.2					91.2																																																5	3										384.5	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151170	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.985Mn0.015Oz	Y	1	Ba	2	Cu	2.985	Mn	0.015													O	z			2007																												Y123																		K		90.3					90.3																																																3.7	3										396.5	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151171	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.97Mn0.0225Oz	Y	1	Ba	2	Cu	2.97	Mn	0.0225													O	z			2007																												Y123																		K		89.9					89.9																																																3.7	3										393.5	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151172	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.97Mn0.03Oz	Y	1	Ba	2	Cu	2.97	Mn	0.03													O	z			2007																												Y123																		K		90.2					90.2																																																3.4	3										392.5	thermal conductivity					THC151172					TP151172																								Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151173	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	YBa2(Cu,Mn)3Oz	Y1Ba2Cu2.94Mn0.06Oz	Y	1	Ba	2	Cu	2.94	Mn	0.06													O	z			2007																												Y123																		K		86.5					86.5																																																3.2	3										391.5	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151174	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	GdBa2Cu3Oz	Gd1Ba2Cu3Oz	Gd	1	Ba	2	Cu	3															O	z			2007																												Y123																		K		91.8					91.8																																																4.1	3										383	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151175	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.985Mn0.015Oz	Gd	1	Ba	2	Cu	2.985	Mn	0.015													O	z			2007																												Y123																		K		91.8					91.8																																																2.9	3										393	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151176	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.97Mn0.0225Oz	Gd	1	Ba	2	Cu	2.97	Mn	0.0225													O	z			2007																												Y123																		K		90.4					90.4																																																2.6	3										388	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151177	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.97Mn0.03Oz	Gd	1	Ba	2	Cu	2.97	Mn	0.03													O	z			2007																												Y123																		K		89.2					89.2																																																2.3	3										384	thermal conductivity					THC151177					TP151177																								Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151178	JPM019256212	values of [Tc], [DebyeT], [Gapene] are obtained by curve fitting of thermal conductivity k(T).	GdBa2(Cu,Mn)3Oz	Gd1Ba2Cu2.94Mn0.06Oz	Gd	1	Ba	2	Cu	2.94	Mn	0.06													O	z			2007																												Y123																		K		86.3					86.3																																																2.2	3										393	thermal conductivity																																		Y2O3(Gd2O3),BaCO3,CuO,MnO	1	mixture - CAL(930C,12h,in air) - pellet - ANN(930C,72h, in O2) - slow cool to 450C - ANN(450C,6h)					Thermal transport in (Y, Gd)Ba2(Cu1-xMnx)3O7-z for x =< 0.02			Superconductivity and Cryogenics Division, National Physical Laboratory, Dr K S Krishnan Road, New Delhi-110012, India	J.Phys. Condens.Matter, 19(2007)256212	Bhasker Gahtori,Ratan Lal,S K Agarwal,MA H Ahsan,Ashok Rao,Y F Lin,K M Sivakumar,Y-K Kuo		
151180	JPS078034710	lattice term of SP (beta) = 0.626 mJ/mol.K4. (dC/gamma*Tc) = 1.45.	Rh2Ga9	Ga9Rh2	Ga	9	Rh	2																				3	2009																													Pc		A	6.4008	6.3944	8.7519												K		1.95					1.95																																														meV	0.295	3.5					MSP151180	mJ/mol.K	21.5	mJ/mol.K2	7.64	SP-heat	324	SP-heat																																		Rh(3N),Ir(3N),Ga(4N)	1	weight ratio: Rh(Ir) : Ga = 1 : 10, mixture - (sealed in evacuated quartz tube) - heat to 1050C(200C/h) - hold(1050C,5h) - cool to 100C(2C/h)					Thermodynamic Properties of the Non-centrosymmetric Type-I Superconductor Rh2Ga9 and Ir2Ga9			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 78(2009)034710	Kouhei WAKUI,Satoshi AKUTAGAWA,Naoki KASE,Kenji KAWASHIMA,Takahiro MURANAKA,Yasufumi IWAHORI,Jiro ABE,Jun AKIMITSU		
151181	JPS078034710	lattice term of SP (beta) = 0.618 mJ/mol.K4. (dC/gamma*Tc) = 1.42. G-L parameter = 0.377. HCFIG shows Hc(T), not Hc2.	Ir2Ga9	Ga9Ir2	Ga	9	Ir	2																				3	2009																													Pc		A	6.4185	6.3918	8.7761												K		2.25					2.25																																		MHC151181												meV	0.345	3.54					MSP151181	mJ/mol.K	23.4	mJ/mol.K2	7.32	SP-heat	325	SP-heat																																		Rh(3N),Ir(3N),Ga(4N)	1	weight ratio: Rh(Ir) : Ga = 1 : 10, mixture - (sealed in evacuated quartz tube) - heat to 1050C(200C/h) - hold(1050C,5h) - cool to 100C(2C/h)					Thermodynamic Properties of the Non-centrosymmetric Type-I Superconductor Rh2Ga9 and Ir2Ga9			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 78(2009)034710	Kouhei WAKUI,Satoshi AKUTAGAWA,Naoki KASE,Kenji KAWASHIMA,Takahiro MURANAKA,Yasufumi IWAHORI,Jiro ABE,Jun AKIMITSU		
151182	JPS078033702	N-content = 1.012 by Rietvelt analysis. G-L parameter = 16.7.	ZnNNi3	Zn1N1Ni3	Zn	1	N	1	Ni	3																			2009																													Pm3m		A	3.756														K			3				3											mT	M-H curve, T2 dependence	6.9							T	resistive, WHH	0.96														A	from Hc2	185			A	calculate from Hc1(0)	3089													mJ/mol.K2	13	SP-heat	336	SP-heat																																		Zn-, Ni-powder		mixture(Zn:Ni = 1.05:3) - pellet - SIN(40C,3h + 520C,15h + 600C,5h, in NH3 gas)					New Antiperovskite-Type Superconductor ZnNyNi3			Department of Physics, Faculty of Engineering, Yokohama National University, Hodogaya-ku, Yokohama 240-8501	J.Phys.Soc.Jpn, 78(2009)033702	Masatomo UEHARA,Akira UEHARA,Katsuya KOZAWA,Yoshihide KIMISHIMA		
151183	JPS078025003	<71>Ga-NQR measured. gap from curve fitting of T1(T) using isotropic gap model.	Ir2Ga9	Ga9Ir2	Ga	9	Ir	2																				3	2009																												Rh2Ga9																		K		2.2					2.2																																																4.4	6																																															Ga-flux method					Conventional s-Wave Superconductivity in Noncentrosymmetric Ir2Ga9: 71Ga-NQR Evidence			Department of Materials Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)025003	Atsushi HARADA,Nobukatsu TAMURA,Hidekazu MUKUDA,Yoshio KITAOKA,Kouhei WAKUI,Satoshi AKUTAGAWA,Jun AKIMITSU		
151184	JPS078025001	hydrostatic pressure. tetra-to-ortho transition at T0 defined as max of (dR/dT).	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		1	2009																												ThCr2Si2																		K			38		0		38	MPH151184																																																																																															solid state reaction					Pressure-Induced Superconductivity in Iron Pnictide Compound SrFe2As2			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 78(2009)025001	Kazumi IGAWA,Hironari OKADA,Hiroki TAKAHASHI,Satoru MATSUISHI,Yoichi KAMIHARA,Masahiro HIRANO,Hideo HOSONO,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
151185	JPS078023710	Energy gap measured by muon-SR. gap in DB obtained using isotropic model.  Using two gap model, gap= 12meV ([gapene]=7.3) and 6.8 meV ([gapnene]= 4.1) are obtained.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2009																																														K		38					38																																														meV	8.35	5.05	16																																															solid state reaction					Full Gap Superconductivity in Ba0:6K0:4Fe2As2 Probed by Muon Spin Rotation			Department of Materials Structure Science, School of High Energy Accelerator Science, The Graduate University for Advanced Studies, 1-1 Oho, Tsukuba, Ibaraki 305-0801	J.Phys.Soc.Jpn, 78(2009)023710	Masatoshi HIRAISHI,Ryosuke KADONO,Soshi TAKESHITA,Masanori MIYAZAKI,Akihiro KODA,Hirotaka OKABE,Jun AKIMITSU		
151186	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=2.0 GPa).	LaOFeAs	La1Fe1As1O0.7	La	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	4.0257		8.719												K	26.2	28.4	29	27.8			28.4										46																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151187	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=2.0 GPa).	CeOFeAs	Ce1Fe1As1O0.7	Ce	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.995		8.631												K	35.5	40.2	41.2	38.5			40.2										43																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151188	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=2.0 GPa).	PrOFeAs	Pr1Fe1As1O0.7	Pr	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.9627		8.5721												K	46	48.5	49.2	48.1			48.5										31																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151189	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=2.0 GPa).	NdOFeAs	Nd1Fe1As1O0.7	Nd	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.9432		8.529												K	52.1	53.7	54.3	53			53.7										80																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151190	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=5.0 GPa).	SmOFeAs	Sm1Fe1As1O0.7	Sm	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.9218		8.4522												K	50.5	52.1	53.3	52.5			52.1										60																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151191	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=5.0 GPa).	GdOFeAs	Gd1Fe1As1O0.7	Gd	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.8905		8.3928												K	52.4	53.6	54	53.5			53.6										70																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151192	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=5.0 GPa).	TbOFeAs	Tb1Fe1As1O0.7	Tb	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.8753		8.3527												K	50.2	52.2	52.6	52.4			52.2										64																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151193	JPS078034712	O-content is nominal. Tc depends on synthesized pressure. Tc in DB shows for the best sample (synthesized at P=5.5 GPa).	DyOFeAs	Dy1Fe1As1O0.7	Dy	1	Fe	1	As	1															O	0.7			2009																												oxypnictide	P4/nmm		A	3.8625		8.3216												K	49.8	51.2	51.6	51.2			51.2										63																																																																																						high-P-synthesis. RAs firstly made by reacting (500C,15h), then react(850C or 1000C,5h). mixture (RAs, Fe, Fe2O3) - pellet - heat(1050-1150C,2h, 2.0 =< P =< 5.0 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151194	PRB079054506	Tc defined as (dR/dT) = 0. T<intra> = 28.2 K defined as the peak of (dR/dT). (delta-Tc) = Tc - T<intra>.	NbSr2(Eu,Ce)2Cu2O10	Nb1Sr2Eu1.5Ce0.5Cu2O10	Nb	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10		1	2009																												Ru1222																		K			30.2			2.2	30.2																																																																																																standard solid state reaction. oxygenation(600C,5d)					Two-dimensional frustrated magnetic state in superconducting RuSr2Eu1.5Ce0.5Cu2O10			Instituto de Fisica, Universidade Federal do Rio de Janeiro, CP 68528, Rio de Janeiro RJ 21941-972, Brazil	Phys.Rev.B, 79(2009)054506	S. Garcia,L. Ghivelder,I. Felner		
151195	PRB079054506	Tc defined as (dR/dT) = 0. T<intra> = 34.1 K defined as the peak of (dR/dT). (delta-Tc) = Tc - T<intra>.	(Nb,Ru)Sr2(Eu,Ce)2Cu2O10	Nb0.6Ru0.4Sr2Eu1.5Ce0.5Cu2O10	Nb	0.6	Ru	0.4	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10		1	2009																												Ru1222																		K			37.3			3.36	37.3																																																																																																standard solid state reaction. oxygenation(600C,5d)					Two-dimensional frustrated magnetic state in superconducting RuSr2Eu1.5Ce0.5Cu2O10			Instituto de Fisica, Universidade Federal do Rio de Janeiro, CP 68528, Rio de Janeiro RJ 21941-972, Brazil	Phys.Rev.B, 79(2009)054506	S. Garcia,L. Ghivelder,I. Felner		
151196	PRB079054506	Tc defined as (dR/dT) = 0. T<intra> = 37.1 K defined as the peak of (dR/dT). (delta-Tc) = Tc - T<intra>.	(Nb,Ru)Sr2(Eu,Ce)2Cu2O10	Nb0.6Ru0.6Sr2Eu1.5Ce0.5Cu2O10	Nb	0.6	Ru	0.6	Sr	2	Eu	1.5	Ce	0.5	Cu	2									O	10		1	2009																												Ru1222																		K			41.4			4.17	41.4																																																																																																standard solid state reaction. oxygenation(600C,5d)					Two-dimensional frustrated magnetic state in superconducting RuSr2Eu1.5Ce0.5Cu2O10			Instituto de Fisica, Universidade Federal do Rio de Janeiro, CP 68528, Rio de Janeiro RJ 21941-972, Brazil	Phys.Rev.B, 79(2009)054506	S. Garcia,L. Ghivelder,I. Felner		
151197	PRB079054506	Tc defined as (dR/dT) = 0. T<intra> = 39.7 K defined as the peak of (dR/dT). (delta-Tc) = Tc - T<intra>.	RuSr2(Eu,Ce)2Cu2O10	Ru1Sr2Eu1.5Ce0.5Cu2O10	Ru	1	Sr	2	Eu	1.5	Ce	0.5	Cu	2											O	10		1	2009																												Ru1222																		K			44.3			4.71	44.3																																																																																																standard solid state reaction. oxygenation(600C,5d)					Two-dimensional frustrated magnetic state in superconducting RuSr2Eu1.5Ce0.5Cu2O10			Instituto de Fisica, Universidade Federal do Rio de Janeiro, CP 68528, Rio de Janeiro RJ 21941-972, Brazil	Phys.Rev.B, 79(2009)054506	S. Garcia,L. Ghivelder,I. Felner		
151198	PRB079054517	K-content not shown. two gaps ([gapene] = 6.8(large) and  < 3.0 (small)). momentum dependence of gaps are extracted from ARPES and IEDS using new model. [gapene] = 9 for X pocket.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2009																												ThCr2Si2																		K		32					32																																																6.8	12																																															Sn-flux method. heat(850C) - cool to 550C (3C/h)					Momentum dependence of the superconducting gap in Ba1-xKxFe2As2			Institute for Solid State Research, IFW Dresden, P.O. Box 270116, D-01171 Dresden, Germany	Phys.Rev.B, 79(2009)054517	D. V. Evtushinsky,D. S. Inosov,V. B. Zabolotnyy,A. Koitzsch,M. Knupfer,B. Buchner,M. S. Viazovska,G. L. Sun,V. Hinkov,A. V. Boris,C. T. Lin,B. Keimer,A. Varykhalov,A. A. Kordyuk,S. V. Borisenko		
151199	PRB079054520		ThPt4Ge12	Th1Pt4Ge12	Th	1	Pt	4	Ge	12																		1	2009																												skutterudite			A	8.5924														K		4.62					4.62																																																																		uV/K	-0.656			MTP151199															m3/C	0.0000000000576				9	MRH151199					See PRB077180504					Two-band conduction in superconducting ThPt4Ge12			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.B, 79(2009)054520	V. H. Tran,D. Kaczorowski,W. Miiller,A. Jezierski		
151200	PRB079054525	uniaxial P-dependence of Tc estimated from thermal expansion using Ehrenfest relation: (dTc/dP)a = -4.1, (dTc/dP)c = 1.7 K/kbar.  (dTc/dP) = 2*(dTc/dP)a + (dTc/dP)c. (dC/Tc) = 4 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2009																												ThCr2Si2																		K			10.6	6.48			6.48			K/GPa	-61																																																																																																	Thermal expansion and anisotropic pressure derivatives of Tc in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)054525	S. L. Bud'ko,N. Ni,S. Nandi,G. M. Schmiedeshoff,P. C. Canfield		
151201	PRB079054525	uniaxial P-dependence of Tc estimated from thermal expansion using Ehrenfest relation: (dTc/dP)a = 0.3, (dTc/dP)c = -2.6 K/kbar.  (dTc/dP) = 2*(dTc/dP)a + (dTc/dP)c. (dC/Tc) = 28 mJ/mol.K2.	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2009																												ThCr2Si2																		K			22.5				22.5			K/GPa	-18																																																																																																	Thermal expansion and anisotropic pressure derivatives of Tc in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)054525	S. L. Bud'ko,N. Ni,S. Nandi,G. M. Schmiedeshoff,P. C. Canfield		
151202	PRB079064507	Bi:Sr:Ca:Cu = 2.16:1.85:1.06:2 by ICP. optimal sample, but O-content not given.	Bi2Sr2CaCu2O8	Bi2.2Sr1.8Ca1Cu2O8+z	Bi	2.2	Sr	1.8	Ca	1	Cu	2													O	8+z		3	2009																												Bi2212																		K				92			92																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151203	PRB079064507	Bi:Sr:Ca:Y:Cu = 2.02:1.98:0.85:0.08:2 by ICP. optimal sample, but O-content not given.	Bi2Sr2(Ca,Y)Cu2O8	Bi2Sr2Ca0.92Y0.08Cu2O8+z	Bi	2	Sr	2	Ca	0.92	Y	0.08	Cu	2											O	8+z		3	2009																												Bi2212																		K				96			96																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151204	PRB079064507	Bi:Pb:Sr:Ca:Cu =1.69:0.33:1.96:0.92:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2CaCu2O8	Bi1.6Pb0.4Sr2Ca1Cu2O8+z	Bi	1.6	Pb	0.4	Sr	2	Ca	1	Cu	2											O	8+z		3	2009																												Bi2212																		K				96			96																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151205	PRB079064507	Bi:Pb:Sr:Ca:Cu = 1.42:0.55:1.97:0.96:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2CaCu2O8	Bi1.4Pb0.8Sr2Ca1Cu2O8+z	Bi	1.4	Pb	0.8	Sr	2	Ca	1	Cu	2											O	8+z		3	2009																												Bi2212																		K				97.5			97.5																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151206	PRB079064507	Bi:Pb:Sr:Ca:Cu = 1.31:0.66:1.94:1.08:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2CaCu2O8	Bi1.3Pb0.9Sr2Ca1Cu2O8+z	Bi	1.3	Pb	0.9	Sr	2	Ca	1	Cu	2											O	8+z		3	2009																												Bi2212																		K				94			94																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151207	PRB079064507	Bi:Pb:Sr:Ca:Y:Cu = 1.58:0.36:1.92:0.93:0.11:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.6Pb0.4Sr2Ca0.9Y0.1Cu2O8+z	Bi	1.6	Pb	0.4	Sr	2	Ca	0.9	Y	0.1	Cu	2									O	8+z		3	2009																												Bi2212																		K				94			94																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151208	PRB079064507	Bi:Pb:Sr:Ca:Y:Cu = 1.50:0.37:1.97:0.92:0.05:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.6Pb0.4Sr2Ca0.95Y0.05Cu2O8+z	Bi	1.6	Pb	0.4	Sr	2	Ca	0.95	Y	0.05	Cu	2									O	8+z		3	2009																												Bi2212																		K				96			96																																																																																																single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151209	PRB079064507	Bi:Pb:Sr:Ca:Y:Cu = 1.33:0.65:2.0:0.98:0.03:2 by ICP. optimal sample, but O-content not given.	(Bi,Pb)2Sr2(Ca,Y)Cu2O8	Bi1.4Pb0.7Sr2Ca0.97Y0.03Cu2O8+z	Bi	1.4	Pb	0.7	Sr	2	Ca	0.97	Y	0.03	Cu	2									O	8+z		3	2009																												Bi2212																		K				98			98	TC151209																																																																																															single crystals grown by TSFZ method. growth speed = 0.15-0.2 mm/h for Pb-free Bi2212, = 0.5 mm/h for Pb-doped Bi2212.					Enhancement of the superconducting critical temperature in Bi2Sr2CaCu2O8+z by controlling disorder outside CuO2 planes			Department of Physics, University of Tokyo, Tokyo 113-0033, Japan	Phys.Rev.B, 79(2009)064507	H. Hobou,S. Ishida,K. Fujita,M. Ishikado,K. M. Kojima,H. Eisaki,S. Uchida		
151210	PRB079052508	89.5% LixFeAs + 10.5% FeAs. [penet] at 1.6 K  from muon-SR .	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2009																													P4/nmm		A	3.774		6.353												K		16					16																																									A	muon-SR	1950																																																					mixture(Li + FeAs) - heat(800C, in Ta-tube)					Enhanced superfluid stiffness, lowered superconducting transition temperature, and field-induced magnetic state of the pnictide superconductor LiFeAs			ISIS Muon Facility, ISIS, Chilton, Oxon., OX11 0QX, United Kingdom	Phys.Rev.B, 79(2009)052508	F. L. Pratt,P. J. Baker,S. J. Blundell,T. Lancaster,H. J. Lewtas,P. Adamson,M. J. Pitcher,D. R. Parker,S. J. Clarke		
151211	PRB079052508	almost single phase. [penet] at 1.6 K  from muon-SR .	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		1	2009																													P4/nmm		A	3.774		6.354												K		12					12																																									A	muon-SR	2440																																																					mixture(Li3As+Fe+FeAs) - heat(800C,48h, in alumina crucible)					Enhanced superfluid stiffness, lowered superconducting transition temperature, and field-induced magnetic state of the pnictide superconductor LiFeAs			ISIS Muon Facility, ISIS, Chilton, Oxon., OX11 0QX, United Kingdom	Phys.Rev.B, 79(2009)052508	F. L. Pratt,P. J. Baker,S. J. Blundell,T. Lancaster,H. J. Lewtas,P. Adamson,M. J. Pitcher,D. R. Parker,S. J. Clarke		
151212	JP020472201	TCFIG shows the data from reference papers.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2008																												ThCr2Si2																		K	28.6				0		28.6	MTC151212																																																																																															FeAs-flux method					Pressure effects on the electron-doped high Tc superconductor BaFe2-xCoxAs2			Department of Physics and Astronomy, McMaster University, Hamilton, ON, L8S4M1, Canada	J.Phys.:Condens.Matter, 20(2008)472201	K Ahilan,J Balasubramaniam,F L Ning,T Imai1,A S Sefat,R Jin,M AMcGuire,B C Sales,D Mandrus		
151213	JP020472201	R=A+BT^n,  n = 1.6 for P=0 and n =1.4 for P=2.5 GPa.	Ba(Fe,Co)2As2	Ba1Fe1.92Co0.08As2	Ba	1	Fe	1.92	Co	0.08	As	2																3	2008																												ThCr2Si2																		K	11						11	MTC151213		K/GPa	4																																																																																												FeAs-flux method					Pressure effects on the electron-doped high Tc superconductor BaFe2-xCoxAs2			Department of Physics and Astronomy, McMaster University, Hamilton, ON, L8S4M1, Canada	J.Phys.:Condens.Matter, 20(2008)472201	K Ahilan,J Balasubramaniam,F L Ning,T Imai1,A S Sefat,R Jin,M AMcGuire,B C Sales,D Mandrus		
151214	JP020472201	R=A+BT^n,  n = 1.33 for  P < 2.5 GPa.	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2008																												ThCr2Si2																		K	22						22			K/GPa	0.65																																																																																												FeAs-flux method					Pressure effects on the electron-doped high Tc superconductor BaFe2-xCoxAs2			Department of Physics and Astronomy, McMaster University, Hamilton, ON, L8S4M1, Canada	J.Phys.:Condens.Matter, 20(2008)472201	K Ahilan,J Balasubramaniam,F L Ning,T Imai1,A S Sefat,R Jin,M AMcGuire,B C Sales,D Mandrus		
151215	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2008																												ThCr2Si2			A	3.9604		12.9964												K		10.5		6.5			10.5	MTC151215																																	MHC151215	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151216	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																3	2008																												ThCr2Si2			A	3.9605		12.9915												K		16.7		14			16.7																																		MHC151216	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151217	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.884Co0.116As2	Ba	1	Fe	1.884	Co	0.116	As	2																3	2008																												ThCr2Si2			A	3.9605		12.984												K		22.8					22.8	MTC151215																																	MHC151217	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151218	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2008																												ThCr2Si2			A	3.9598		12.9782												K		22.5					22.5																																		MHC151218	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151219	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2008																												ThCr2Si2			A	3.9598		12.9718												K		17.4					17.4																																		MHC151219	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151220	PRB078214515	Co-content determined by WDS(wavelength dispersive x-ray spectroscopy	Ba(Fe,Co)2As2	Ba1Fe1.772Co0.228As2	Ba	1	Fe	1.772	Co	0.228	As	2																3	2008																												ThCr2Si2			A	3.9592		12.9594												K		10.6					10.6	MTC151215																																	MHC151220	resistive, onset																																																													self-flux method using Ba:FeAs:CoAs = 1:4(1-x):4x solution. heat(1180C,2h) - cool to 100C (5 C/h)					Effects of Co substitution on thermodynamic and transport properties and anisotropic Hc2 in Ba(Fe1-xCox)2As2 single crystals			Ames Laboratory U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)214515	N. Ni,M. E. Tillman,J.-Q. Yan,A. Kracher,S. T. Hannahs,S. L. Bud'ko,P. C. Canfield		
151221	PRL099257004	C=[gamma]T+[beta]T^3+[delta]T^5 fitting. [gamma] corrected by subtracting impurity part. [beta]=3.97 mJ/mol.K4, [delta]=7.4 uJ/mol.K6. [Debye-T] obtained from Debye and Einstein(147 K) model.	Mg10Ir19B16	Mg10Ir19B16	Mg	10	Ir	19	B	16																			2007																													I-43m		A	10.5668														K		4.45					4.45											Oe	M-H curve	30							T	SP-heat	0.77												MHC151221	resistive, SP-heat	A	from Hc2	206			A	from Hc1	4040			meV	0.7	14								mJ/mol.K2	52.6	SP-heat	740	SP-heat																																		Mg,Ir,B		solid state reaction. ANN(850C,100h, in Ta-tube)					Physical Properties of the Noncentrosymmetric Superconductor Mg10Ir19B16			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 99(2007)257004	T. Klimczuk,F. Ronning,V. Sidorov,R. J. Cava,J. D. Thompson		
151222	PRB079064508	definition oh Hc1 not clear.	Pd2ZrAl	Pd2Zr1Al1	Pd	2	Zr	1	Al	1																			2009																												Heusler	Fm3[-]m																L2<1>	K		3.2		3.1			3.2											Oe		60																																																																																			arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151223	PRB079064508	definition oh Hc1 not clear.	Pd2HfAl	Pd2Hf1Al1	Pd	2	Hf	1	Al	1																			2009																												Heusler	Fm3[-]m																L2<1>	K		3.8		3.4			3.8											Oe		103																																																																																			arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151224	PRB079064508	definition oh Hc1 not clear.	Pd2ZrIn	Pd2Zr1In1	Pd	2	Zr	1	In	1																			2009																												Heusler	Fm3[-]m																L2<1>	K		3.1		3			3.1											Oe		123																																																																																			arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151225	PRB079064508	definition oh Hc1 not clear. anomalous R drop at around 3.1 K.	Pd2HfIn	Pd2Hf1In1	Pd	2	Hf	1	In	1																			2009																												Heusler	Fm3[-]m																L2<1>	K		2.4		2.3			2.4											Oe		62																																																																																			arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151226	PRB079064508	not SC. small drop in resistivity  at around 2.6 K.	Pd2(Zr,Y)Al	Pd2Zr0.9Y0.1Al1	Pd	2	Zr	0.9	Y	0.1	Al	1																	2009																												Heusler	Fm3[-]m		A	6.432														K					1.8																																																																																																		arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151227	PRB079064508		Pd2(Zr,Nb)Al	Pd2Zr0.9Nb0.1Al1	Pd	2	Zr	0.9	Nb	0.1	Al	1																	2009																												Heusler	Fm3[-]m		A	6.372														K		2.1					2.1																																																																																																arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151228	PRB079064508		Pd2(Hf,Y)Al	Pd2Hf0.75Y0.25Al1	Pd	2	Hf	0.75	Y	0.25	Al	1																	2009																												Heusler	Fm3[-]m		A	6.393														K		3.2					3.2																																																																																																arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151229	PRB079054521	T<SDW> = 147 K.	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1		1	2009																												oxypnictide			A	4.0349		8.736											ZrCuSiAs-type	K																																																																									uV/K	-28.7			TP151229																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151230	PRB079054521	T<SDW> = 135 K.	LaO(Fe,Co)As	La1Fe0.99Co0.01As1O1	La	1	Fe	0.99	Co	0.01	As	1													O	1		1	2009																												oxypnictide			A	4.0341		8.7321											ZrCuSiAs-type	K																																																																																																					LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151231	PRB079054521	Tmin(R shows minimum) = 111 K.	LaO(Fe,Co)As	La1Fe0.975Co0.025As1O1	La	1	Fe	0.975	Co	0.025	As	1													O	1		1	2009																												oxypnictide			A	4.0355		8.7235											ZrCuSiAs-type	K		8.58		11.17			8.58																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151232	PRB079054521	Tmin(R shows minimum) = 89.5 K.	LaO(Fe,Co)As	La1Fe0.95Co0.05As1O1	La	1	Fe	0.95	Co	0.05	As	1													O	1		1	2009																												oxypnictide			A	4.0343		8.7238											ZrCuSiAs-type	K		13.02		12.84			13.02	TC151232																																																																	uV/K	-60.6			TP151232																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151233	PRB079054521	Tmin(R shows minimum) = 51.4 K.	LaO(Fe,Co)As	La1Fe0.925Co0.075As1O1	La	1	Fe	0.925	Co	0.075	As	1													O	1		1	2009																												oxypnictide			A	4.0345		8.7152											ZrCuSiAs-type	K		12.66		12.48			12.66																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151234	PRB079054521	Tmin(R shows minimum) = 40.0 K.	LaO(Fe,Co)As	La1Fe0.9Co0.1As1O1	La	1	Fe	0.9	Co	0.1	As	1													O	1		1	2009																												oxypnictide			A	4.0353		8.7254											ZrCuSiAs-type	K		11.02		10.87			11.02	TC151232																																																																	uV/K	-73.4			TP151234																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151235	PRB079054521	Tmin(R shows minimum) = 35.3 K.	LaO(Fe,Co)As	La1Fe0.875Co0.125As1O1	La	1	Fe	0.875	Co	0.125	As	1													O	1		1	2009																												oxypnictide			A	4.0351		8.7075											ZrCuSiAs-type	K		6.6		6.97			6.6																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151236	PRB079054521	Tmin(R shows minimum) = 18.4 K.	LaO(Fe,Co)As	La1Fe0.85Co0.15As1O1	La	1	Fe	0.85	Co	0.15	As	1													O	1		1	2009																												oxypnictide			A	4.0351		8.6924											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151237	PRB079054521	Tmin(R shows minimum) = 20.3 K.	LaO(Fe,Co)As	La1Fe0.8Co0.2As1O1	La	1	Fe	0.8	Co	0.2	As	1													O	1		1	2009																												oxypnictide			A	4.0343		8.6767											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151238	PRB079054521	T<SDW> = 93.1 K. Tmin(R shows minimum) = 196.7 K.	SmO(Fe,Co)As	Sm1Fe0.975Co0.025As1O1	Sm	1	Fe	0.975	Co	0.025	As	1													O	1		1	2009																												oxypnictide			A	3.9385		8.4837											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151239	PRB079054521	T<SDW> = 42.8 K. Tmin(R shows minimum) = 174.3 K.	SmO(Fe,Co)As	Sm1Fe0.95Co0.05As1O1	Sm	1	Fe	0.95	Co	0.05	As	1													O	1		1	2009																												oxypnictide			A	3.939		8.4725											ZrCuSiAs-type	K		5.13					5.13																																																																		uV/K	-35			TP151239																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151240	PRB079054521	Tmin(R shows minimum) = 143.8 K.	SmO(Fe,Co)As	Sm1Fe0.925Co0.075As1O1	Sm	1	Fe	0.925	Co	0.075	As	1													O	1		1	2009																												oxypnictide			A	3.9396		8.4686											ZrCuSiAs-type	K		15					15																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151241	PRB079054521	Tmin(R shows minimum) = 117.5 K.	SmO(Fe,Co)As	Sm1Fe0.9Co0.1As1O1	Sm	1	Fe	0.9	Co	0.1	As	1													O	1		1	2009																												oxypnictide			A	3.9397		8.4668											ZrCuSiAs-type	K		17.3					17.3																																																																		uV/K	-51.5			TP151241																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151242	PRB079054521	Tmin(R shows minimum) = 52.4 K.	SmO(Fe,Co)As	Sm1Fe0.875Co0.125As1O1	Sm	1	Fe	0.875	Co	0.125	As	1													O	1		1	2009																												oxypnictide			A	3.9391		8.4558											ZrCuSiAs-type	K		15.8					15.8																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151243	PRB079054521		SmO(Fe,Co)As	Sm1Fe0.85Co0.15As1O1	Sm	1	Fe	0.85	Co	0.15	As	1													O	1		1	2009																												oxypnictide			A	3.9391		8.4459											ZrCuSiAs-type	K		11.75					11.75																																																																																														LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151244	PRB079054521	Tmin(R shows minimum) = 17.4 K.	SmO(Fe,Co)As	Sm1Fe0.8Co0.2As1O1	Sm	1	Fe	0.8	Co	0.2	As	1													O	1		1	2009																												oxypnictide			A	3.9393		8.4334											ZrCuSiAs-type	K		3.79					3.79																																																																		uV/K	-43.8			TP151244																								LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151245	PRB079054521	Tmin(R shows minimum) = 14.1 K.	SmO(Fe,Co)As	Sm1Fe0.775Co0.225As1O1	Sm	1	Fe	0.775	Co	0.225	As	1													O	1		1	2009																												oxypnictide			A	3.9393		8.4256											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151246	PRB079054521	Tmin(R shows minimum) = 13.0 K.	SmO(Fe,Co)As	Sm1Fe0.75Co0.25As1O1	Sm	1	Fe	0.75	Co	0.25	As	1													O	1		1	2009																												oxypnictide			A	3.9399		8.4203											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151247	PRB079054521	Tmin(R shows minimum) = 16.1 K.	SmO(Fe,Co)As	Sm1Fe0.7Co0.3As1O1	Sm	1	Fe	0.7	Co	0.3	As	1													O	1		1	2009																												oxypnictide			A	3.9401		8.4102											ZrCuSiAs-type	K					1.8																																																																																																LaAs(SmAs),La2O3(Sm2O3),FeAs,Fe2As,Co3O4		solid state reaction					Effects of cobalt doping and phase diagrams of LFe1-xCoxAsO (L=La and Sm)			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 79(2009)054521	C. Wang,Y. K. Li,Z. W. Zhu,S. Jiang,X. Lin,Y. K. Luo,S. Chi,L. J. Li,Z. Ren,M. He,H. Chen,Y. T. Wang,Q. Tao,G. H. Cao,Z. A. Xu		
151249	PRB079064508		Pd2(Hf,Y)Al	Pd2Hf0.5Y0.5Al1	Pd	2	Hf	0.5	Y	0.5	Al	1																	2009																												Heusler	Fm3[-]m		A	6.404														K		2.9					2.9																																																																																																arc-melting. ANN(1073K,2w, in evacuated quartz tube) - Q to 273 K.					Superconductivity in palladium-based Heusler compounds			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 79(2009)064508	Jurgen Winterlik,Gerhard H. Fecher,Anja Thomas,Claudia Felser		
151250	PRB079024520	Figure contains T<SPT> values which are structural phase transition. T<SPT> = 60.8 K. (dC/gamma*Tc) = 0.615.	(Sn,In)Te	Sn0.979In0.021Te1	Sn	0.979	In	0.021	Te	1																		3	2009																																														K		0.936		0.855			0.936																																																								mJ/mol.K2	0.964																																							starting materials(Sn:In:Te=85(1-x):85x:15) - sealed in quartz (vac) - heat(725C) - cool to 400C(2C/h) - (sn rich flux decanted) - ANN(550C,48h)					Enhanced superconducting pairing interaction in indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)024520	A. S. Erickson,J.-H. Chu,M. F. Toney,T. H. Geballe,I. R. Fisher		
151251	PRB079024520	(dC/gamma*Tc) = 1.039, 1.311.	(Sn,In)Te	Sn0.956In0.044Te1	Sn	0.956	In	0.044	Te	1																		3	2009																																														K				1.017			1.017																																																								mJ/mol.K2	1.035																																							starting materials(Sn:In:Te=85(1-x):85x:15) - sealed in quartz (vac) - heat(725C) - cool to 400C(2C/h) - (sn rich flux decanted) - ANN(550C,48h)					Enhanced superconducting pairing interaction in indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)024520	A. S. Erickson,J.-H. Chu,M. F. Toney,T. H. Geballe,I. R. Fisher		
151252	PRB079024520	(dC/gamma*Tc) = 1.186.	(Sn,In)Te	Sn0.949In0.051Te1	Sn	0.949	In	0.051	Te	1																		3	2009																																														K		1.653		1.121			1.653																																																								mJ/mol.K2	1.027																																							starting materials(Sn:In:Te=85(1-x):85x:15) - sealed in quartz (vac) - heat(725C) - cool to 400C(2C/h) - (sn rich flux decanted) - ANN(550C,48h)					Enhanced superconducting pairing interaction in indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)024520	A. S. Erickson,J.-H. Chu,M. F. Toney,T. H. Geballe,I. R. Fisher		
151253	PRB079024520		(Sn,In)Te	Sn0.901In0.099Te1	Sn	0.901	In	0.099	Te	1																		3	2009																																														K				1.746			1.746																																																																																																starting materials(Sn:In:Te=85(1-x):85x:15) - sealed in quartz (vac) - heat(725C) - cool to 400C(2C/h) - (sn rich flux decanted) - ANN(550C,48h)					Enhanced superconducting pairing interaction in indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.B, 79(2009)024520	A. S. Erickson,J.-H. Chu,M. F. Toney,T. H. Geballe,I. R. Fisher		
151254	PRB079064520	Hc1 obtained by measuring local magnetization and extraporation to 0 K.  Anisotropy = 2.5 at low temperature.	PrOFeAs	Pr1Fe1As1O1-z	Pr	1	Fe	1	As	1															O	1-z		3	2009																												oxypnictide																		K				34			34											Oe	M-H curve, extraporation		45	102																			HC151254							A			2800																																																		PrAs,Fe,Fe2O3		mixture(Pr:Fe:As:O=1:1:1:0.6) - pellet - heat(1300C,2h,P=2 GPa, in BN crucible)					Lower critical fields of superconducting PrFeAsO1-y single crystals			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 79(2009)064520	R. Okazaki,M. Konczykowski,C. J. van der Beek,T. Kato,K. Hashimoto,M. Shimozawa,H. Shishido,M. Yamashita,M. Ishikado,H. Kito,A. Iyo,H. Eisaki,S. Shamoto,T. Shibauchi,Y. Matsuda		
151255	PHC4690256	intercalation of In to Nb2C. lattice term  coeffic. in C (beta) = 0.54 mJ/mol.K4.	Nb2InC	Nb2In1C1	Nb	2	In	1	C	1																			2009																												Cr2AlC			A	3.172		14.37												K			7.5	7.5			7.5										33	Oe	M-H curve				90			1.8																						A		2710													mJ/mol.K2	12.6	SP-heat	154	SP-heat																																		graphite,Nb,In		mixture(graphite,Nb,In powder) - sealed in quartz ampoule - heat(1000C,48h) pellet - SIN(1000C,120h)					Superconductivity in Nb2InC			Departamento de Engenharia de Materiais, Escola de Engenharia de Lorena ? USP, P.O. Box 116, Lorena, SP 12600-970, Brazil	Physica C, 469(2009)256	A.D. Bortolozo,Z. Fisk,O.H. Sant'Anna,C.A.M. dos Santos,A.J.S. Machado		
151256	SCI3191506	P-induced SC. Tc(max) = 17.5 K at 96 GPa. molecular structure of SiH4 is SnBr4-like. (melting point = 88K, boiling point = 161 K from data book)	SiH4	H4Si1	H	4	Si	1																					2009																																														K			17		0		17	MTC151256																																																																																																				Superconductivity in Hydrogen Dominant Materials: Silane			Max Planck Institute fur Chemie, Postfach 3060, 55020 Mainz, Germany. 2Department of Physics and Engineering Physics, University of Saskatchewan, Saskatoon, S7N 5E2, Canada	Science 319(2009)1506	M. I. Eremets,I. A. Trojan,S. A. Medvedev,J. S. Tse,Y. Yao		
151257	PHC4690300	not SC. R-anomaly at 150 K.	(La,Na)(O,F)FeAs	La0.9Na0.1Fe1As1F0.1O0.9	La	0.9	Na	0.1	Fe	1	As	1	F	0.1											O	0.9			2009																															A	4.031		8.7381												K																																																																																																					La2O3,NaF,La,FeAs		mixture - (wrapped in Ta-foil and sealed in evacuated silica) - heat(800C,12h + 950C,24h) -pellet - (wrapped in Ta-foil and sealed in evacuated silica) - heat(1080C,48h)					Compositionally controlled semimetal to superconducting transition in NaF doped LaOFeAs: Enhancement in Tc due to Na-doping			Department of Chemistry, Indian Institute of Technology, New Delhi 110 016, India	Physica C, 469(2009)300	J. Prakash,S.J. Singh,J. Ahmed,S. Patnaik,A.K. Ganguli		
151258	PHC4690300	RRR = 7.27. R = A + B*T^2 for 45 < T < 151 K.	(La,Na)(O,F)FeAs	La0.85Na0.15Fe1As1F0.15O0.85	La	0.85	Na	0.15	Fe	1	As	1	F	0.15											O	0.85			2009																															A	4.0252		8.7208												K			30.9	28			28																				T	resistivity, WHH	63.5							T/K	resistivity	2.97			HC151258																																																												La2O3,NaF,La,FeAs		mixture - (wrapped in Ta-foil and sealed in evacuated silica) - heat(800C,12h + 950C,24h) -pellet - (wrapped in Ta-foil and sealed in evacuated silica) - heat(1080C,48h)					Compositionally controlled semimetal to superconducting transition in NaF doped LaOFeAs: Enhancement in Tc due to Na-doping			Department of Chemistry, Indian Institute of Technology, New Delhi 110 016, India	Physica C, 469(2009)300	J. Prakash,S.J. Singh,J. Ahmed,S. Patnaik,A.K. Ganguli		
151259	PHC4690300	RRR = 13.79.	(La,Na)(O,F)FeAs	La0.8Na0.2Fe1As1F0.2O0.8	La	0.8	Na	0.2	Fe	1	As	1	F	0.2											O	0.8			2009																															A	4.0232		8.6919												K			23.02				23.02																				T	resistivity, WHH	19							T/K	resistivity	1.18																																			uV/K	-34			TP151259																								La2O3,NaF,La,FeAs		mixture - (wrapped in Ta-foil and sealed in evacuated silica) - heat(800C,12h + 950C,24h) -pellet - (wrapped in Ta-foil and sealed in evacuated silica) - heat(1080C,48h)					Compositionally controlled semimetal to superconducting transition in NaF doped LaOFeAs: Enhancement in Tc due to Na-doping			Department of Chemistry, Indian Institute of Technology, New Delhi 110 016, India	Physica C, 469(2009)300	J. Prakash,S.J. Singh,J. Ahmed,S. Patnaik,A.K. Ganguli		
151260	PHC4690259	(dTc/dP) is the uniaxial pressure (P//c) dependence obtained from thermal expansion measurements. T<CDW> = 32 K from thermal expansion measurements.	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	2009																												2H-NbSe2																		K		7.2				0.02	7.2			K/GPa	1.45																									T/K	SP-heat	0.85			MHC151260																				mJ/mol.K	206																																									Chemical transport method. Thermal gradient of 1000 - 900C.					Heat capacity, thermal expansion and pressure derivative of critical temperature at the superconducting and charge density wave (CDW) transitions in NbSe2			B.I. Verkin Institute for Low Temperature Physics NASU, Kharkov, Ukraine	Physica C, 469(2009)259	V. Eremenko,V. Sirenko,V. Ibulaev,J. Bartolome,A. Arauzo,G. Remenyi		
151261	PRB079094505	SP-heat measured at various H. thermodynamic Hc(0) = 0.9 T using BCS. Hc2-anisotropy = 2.6.  (dC/Tc) = 0.1 J/mol.K2.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2009																												ThCr2Si2																		K		34.6					34.6																				T	SP-heat, WHH		415	155					T/K	SP-heat		17.4	6.5	MHC151261		A	from Hc2(0)		12	4.5	A			1250																																																				See Supercond.Sci.Technol. 2(2008)125014					Anisotropic phase diagram and strong coupling effects in Ba1-xKxFe2As2 from specific-heat measurements			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 79(2009)094505	U. Welp,R. Xie,A. E. Koshelev,W. K. Kwok,H. Q. Luo,Z. S. Wang,G. Mu,H. H. Wen		
151262	PRB079094507	optimally doped sample. Hc2 measured using tunnel diode resonator method (TDR). Hc2-anisotropy = 2.1 - 2.6	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2009																												ThCr2Si2																		K		23					23																													T/K	TDR		4.56	1.87	MHC151262																																																														flux-method using (FeAs/CoAS) flux. Starting material (Ba:FeAs:CoAs = 1:3.6:0.4)					Anisotropy of the iron pnictide superconductor Ba(Fe1-xCox)2As2 (x=0.074, Tc=23 K)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)094507	M. A. Tanatar,N. Ni,C. Martin,R. T. Gordon,H. Kim,V. G. Kogan,G. D. Samolyuk,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
151263	PRB079094508	tetra-to-ortho transition at 136 K. SUS<c)>= SUS<ab> = 6.7E-4 cm3/mol. R<ab> = 0.50 & R<c> = 16.44 mOhm.cm at 300K. RRR = 4. SP-fitting for T>150K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2009								132																				ThCr2Si2			A	3.9635		13.022												K					1.8																																																										mJ/mol.K2	6.1	SP-heat	260	SP-heat																																				(Ba:FeAs = 1:5) - heat(1180C,8h) - cool to 1090C(4C/h) - decant at 1090C.					Structure and anisotropic properties of BaFe2-xNixAs2 (x=0, 1, and 2) single crystals			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 79(2009)094508	Athena S. Sefat,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Filip Ronning,E. D. Bauer,Yurij Mozharivskyj		
151264	PRB079094508	R<ab> = 0.08 & R<c> = 2.25 mOhm.cm at 300K. RRR = 12	BaFeNiAs2	Ba1Fe1Ni1As2	Ba	1	Fe	1	Ni	1	As	2																3	2009																												ThCr2Si2	I4/mmm		A	4.0002		12.6767												K					1.8																																																																																																		(Ba:NiAs = 1:4) - heat(1180C,10h,in alumina) - cool to 1025C(3C/h)					Structure and anisotropic properties of BaFe2-xNixAs2 (x=0, 1, and 2) single crystals			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 79(2009)094508	Athena S. Sefat,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Filip Ronning,E. D. Bauer,Yurij Mozharivskyj		
151265	PRB079094508	tetra-to-triclinic transition below 130 K.  R<ab> = 0.07 & R<c> = 4.69 mOhm.cm at 300K. RRR = 8. (dC/gamma*Tc) = 1.38	BaNi2As2	Ba1Ni2As2	Ba	1	Ni	2	As	2																		3	2009																												ThCr2Si2			A	4.1441		11.6325												K	0.69		1.5				1.095																				T	SP-heat, WHH	0.069							T/K	SP-heat	0.142					A	from Hc2(0)	691																mJ/mol.K	12.6	mJ/mol.K2	13.2	SP-heat	250	SP-heat																																				FeAs:NiAs = 1:1					Structure and anisotropic properties of BaFe2-xNixAs2 (x=0, 1, and 2) single crystals			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 79(2009)094508	Athena S. Sefat,Michael A. McGuire,Rongying Jin,Brian C. Sales,David Mandrus,Filip Ronning,E. D. Bauer,Yurij Mozharivskyj		
151266	PRB079094521	not bulk SC. Fe1.06Te0.68Se0.32 from XDS analysis.	Fe(Te,Se)	Fe1Te0.67Se0.33	Fe	1	Te	0.67	Se	0.33																		3	2009																																3.803		6.118												K			14				14																																																								mJ/mol.K2	39	SP-heat	174	SP-heat																																				modified Bridgeman method. melt(1070C,36h) - cool to (350-750C) with a rate(3-6) C/h depending on Se composition.					Bulk superconductivity at 14 K in single crystals of Fe1+yTexSe1-x			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 79(2009)094521	B. C. Sales,A. S. Sefat,M. A. McGuire,R. Y. Jin,D. Mandrus,Y. Mozharivskyj		
151267	PRB079094521	Fe1.00Te0.54Se0.46 from XDS analysis. bulk SC ( large diamagnetic screening). gap (=1.3 kTc) estimasted using SP-SP(normal state of #151266 sample).	Fe(Te,Se)	Fe1Te0.5Se0.5	Fe	1	Te	0.5	Se	0.5																		3	2009																																3.815		6.069												K	14			14			14																																																2.6	14																																															modified Bridgeman method. melt(1070C,36h) - cool to (350-750C) with a rate(3-6) C/h depending on Se composition.					Bulk superconductivity at 14 K in single crystals of Fe1+yTexSe1-x			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 79(2009)094521	B. C. Sales,A. S. Sefat,M. A. McGuire,R. Y. Jin,D. Mandrus,Y. Mozharivskyj		
151268	NAS10514262	RRR = 6. impurity: beta-phase(NiAs-type). low-temp-phase transition(P4/nmm to P-1) at 105 K. (dC/gamma*Tc) = 0.61. Hc2(T) has (1-t^2) dependence.	alpha-FeSe	Fe1Se0.88	Fe	1	Se	0.88																					2008																												PbO	P4/nmm		A	3.7676		5.4847											alpha-phase	K	8			8			8																				T	resistivity	16.3												MHC151268		A	from Hc2(0)	45																		mJ/mol.K2	9.17																																							mixture(appropriate stoichiometry) - (press to disc) - heat to 700C(100C/h, in evacuated quartz) - SIN(700C,24h) - ANN(400C,36h)					Superconductivity in the PbO-type structure alpha-FeSe			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Proc.Nat.Acad.Sci., 105(2008)14262	Fong-Chi Hsu,Jiu-Yong Luo,Kuo-Wei Yeh,Ta-Kun Chen,Tzu-Wen Huang,Phillip M. Wu,Yong-Chi Lee,Yi-Lin Huang,Yan-Yi Chu,Der-Chung Yan,Maw-Kuen Wu		
151269	PRB079104515	[cohere] calculated asuming anisotropy factor.	Sm(O,F)FeAs	Sm1Fe1As1F0.07O0.93	Sm	1	Fe	1	As	1	F	0.07													O	0.93			2009																												oxypnictide																		K		33				3	33																													T/K	resistivity	7					A	from Hc2(0)		37	5.5																																																								See Supercond.Sci.Technol., 21(2008)095017.					Upper critical field and fluctuation conductivity in the critical regime of doped SmFeAsO			CNR-INFM-LAMIA, via Dodecaneso 33, 16146 Genova, Italy and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 79(2009)104515	I. Pallecchi,C. Fanciulli,M. Tropeano,A. Palenzona,M. Ferretti,A. Malagoli,A. Martinelli,I. Sheikin,M. Putti,C. Ferdeghini		
151270	PRB079104515	[cohere] calculated asuming anisotropy factor.	Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9			2009																												oxypnictide																		K		41.5				2	41.5																													T/K	resistivity	7.5					A	from Hc2(0)		32	4.8																																																								See Supercond.Sci.Technol., 21(2008)095017.					Upper critical field and fluctuation conductivity in the critical regime of doped SmFeAsO			CNR-INFM-LAMIA, via Dodecaneso 33, 16146 Genova, Italy and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 79(2009)104515	I. Pallecchi,C. Fanciulli,M. Tropeano,A. Palenzona,M. Ferretti,A. Malagoli,A. Martinelli,I. Sheikin,M. Putti,C. Ferdeghini		
151271	PRB079104515	[cohere] calculated asuming anisotropy factor.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2009																												oxypnictide																		K		51.5				2	51.5																				T		400							T/K	resistivity	12					A	from Hc2(0)		23	3.4																																																								See Supercond.Sci.Technol., 21(2008)095017.					Upper critical field and fluctuation conductivity in the critical regime of doped SmFeAsO			CNR-INFM-LAMIA, via Dodecaneso 33, 16146 Genova, Italy and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 79(2009)104515	I. Pallecchi,C. Fanciulli,M. Tropeano,A. Palenzona,M. Ferretti,A. Malagoli,A. Martinelli,I. Sheikin,M. Putti,C. Ferdeghini		
151272	PRB079104501	Hc2(0) = 52 T using Hc2(T)=Hc2(0)[(1-t^2)/(1+t^2)] dependence. R = R0 + AT^n where R0=0.306 mOhm.cm, n=2.00.	(Pr,Sr)OFeAs	Pr0.75Sr0.25Fe1As1O1	Pr	0.75	Sr	0.25	Fe	1	As	1													O	1		1	2009																												oxypnictide																		K			16.3				16.3										50										T	resistivity, WHH	45.1							T/K	resistivity	4																																																						cm3/C	-0.00000000065					RH151272					precursors(PrAs,SrAs) firstly synthesized. mixture(PrAs,SrAs,Fe,Fe2O3) - pellet - (sealed in quartz tube(20% Ar) - heat to 1150C (120C/h) - react(1150C,60h) cool to RT.					Synthesis, structural, and transport properties of the hole-doped superconductor Pr1-xSrxFeAsO			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)104501	Gang Mu,Bin Zeng,Xiyu Zhu,Fei Han,Peng Cheng,Bing Shen,Hai-Hu Wen		
151273	PLA3731482		Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			2009																												BPBO																	perovskite	K			12.5				12.5																																																																																																precursor(BaPb0.75-xBi0.25O3) by solid state reaction. mixture(precursor:HgO = 1:x) - heat(800C,48h) - slow cool to RT - add(30% excess HgO) ANN(500C,in flowing Ar(4h) and O2(20h))					Superconductivity in Hg-substituted BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Phys.Lett.A, 373(2009)1482	Y.L. Chen,Y.J. Cui,C.H. Cheng,Y. Zhang,H.T. Lin,Y. Zhao		
151274	PLA3731482		Ba(Pb,Hg,Bi)O3	Ba1Pb0.65Hg0.1Bi0.25O3	Ba	1	Pb	0.65	Hg	0.1	Bi	0.25													O	3			2009																												BPBO																		K			10				10	MTC151274																																																																																															precursor(BaPb0.75-xBi0.25O3) by solid state reaction. mixture(precursor:HgO = 1:x) - heat(800C,48h) - slow cool to RT - add(30% excess HgO) ANN(500C,in flowing Ar(4h) and O2(20h))					Superconductivity in Hg-substituted BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Phys.Lett.A, 373(2009)1482	Y.L. Chen,Y.J. Cui,C.H. Cheng,Y. Zhang,H.T. Lin,Y. Zhao		
151275	PLA3731482		Ba(Pb,Hg,Bi)O3	Ba1Pb0.55Hg0.2Bi0.25O3	Ba	1	Pb	0.55	Hg	0.2	Bi	0.25													O	3			2009																												BPBO																	distorted perovskite	K			3.83				3.83																																																																																																precursor(BaPb0.75-xBi0.25O3) by solid state reaction. mixture(precursor:HgO = 1:x) - heat(800C,48h) - slow cool to RT - add(30% excess HgO) ANN(500C,in flowing Ar(4h) and O2(20h))					Superconductivity in Hg-substituted BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Phys.Lett.A, 373(2009)1482	Y.L. Chen,Y.J. Cui,C.H. Cheng,Y. Zhang,H.T. Lin,Y. Zhao		
151276	PLA3731482		Ba(Pb,Hg,Bi)O3	Ba1Pb0.45Hg0.3Bi0.25O3	Ba	1	Pb	0.45	Hg	0.3	Bi	0.25													O	3			2009																												BPBO																	distorted perovskite	K			4.42				4.42																																																																																																precursor(BaPb0.75-xBi0.25O3) by solid state reaction. mixture(precursor:HgO = 1:x) - heat(800C,48h) - slow cool to RT - add(30% excess HgO) ANN(500C,in flowing Ar(4h) and O2(20h))					Superconductivity in Hg-substituted BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Phys.Lett.A, 373(2009)1482	Y.L. Chen,Y.J. Cui,C.H. Cheng,Y. Zhang,H.T. Lin,Y. Zhao		
151277	PLA3731482		Ba(Pb,Hg,Bi)O3	Ba1Pb0.35Hg0.4Bi0.25O3	Ba	1	Pb	0.35	Hg	0.4	Bi	0.25													O	3			2009																												BPBO																	perovskite	K			10.7				10.7	MTC151274																																																																																															precursor(BaPb0.75-xBi0.25O3) by solid state reaction. mixture(precursor:HgO = 1:x) - heat(800C,48h) - slow cool to RT - add(30% excess HgO) ANN(500C,in flowing Ar(4h) and O2(20h))					Superconductivity in Hg-substituted BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Phys.Lett.A, 373(2009)1482	Y.L. Chen,Y.J. Cui,C.H. Cheng,Y. Zhang,H.T. Lin,Y. Zhao		
151278	PRB079104521	composition determined by EDX.	(Ba,Rb,Sn)Fe2As2	Ba0.84Rb0.1Sn0.09Fe2As2	Ba	0.84	Rb	0.1	Sn	0.09	Fe	2	As	2														3	2009																												ThCr2Si2																		K				22.6			22.6																				T	resistivity, WHH		120	70					T/K	resistivity		7.1	4.2	MHC151278																																																												Ba,Rb,Fe2As,As,Sn		Sn-flux method(Fe:Sn = 1:24). mixture(in alumina crucible) - heat(850C,3h) - cool to 500C in 50h					Superconductivity at 23 K and low anisotropy in Rb-substituted BaFe2As2 single crystals			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 79(2009)104521	Z. Bukowski,S. Weyeneth,R. Puzniak,P. Moll,S. Katrych,N. D. Zhigadlo,J. Karpinski,H. Keller,B. Batlogg		
151279	PHC4690297	impurity: beta-FeSe	alpha-Fe(Se,S)	Fe1Se0.9S0.1	Fe	1	Se	0.9	S	0.1																			2009																												PbO	P4/nmm		A	3.758		5.468											alpha-phase	K		9.94					9.94																																																																																														Fe,S,Se		mixture - sealed in quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Sulfur substitution and pressure effect on superconductivity of alpha-FeSe			National High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 469(2009)297	Min Ge,Zhaorong Yang,Li Li,Lina Chen,Li Pi,Zhe Qu,Bosen Wang,Yuping Sun,Yuheng Zhang		
151280	PHC4690297		alpha-Fe(Se,S)	Fe1Se0.8S0.2	Fe	1	Se	0.8	S	0.2																			2009																												PbO	P4/nmm		A	3.751		5.453											alpha-phase	K		9.23					9.23																																																																																														Fe,S,Se		mixture - sealed in quartz tube - SIN(700C,24h) - reground - pellet - SIN(700C,24h)					Sulfur substitution and pressure effect on superconductivity of alpha-FeSe			National High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 469(2009)297	Min Ge,Zhaorong Yang,Li Li,Lina Chen,Li Pi,Zhe Qu,Bosen Wang,Yuping Sun,Yuheng Zhang		
151281	PRB079134507	RRR=40. Rn = 1.8 uOhm.cm(4.2K). SC properties from analysis of SP-heat data. (dC/gamma*Tc) = 1.27. G-L parameter = 2.1. beta(lattice term in SP) = 0.23 mJ/mol.K4.	SrNi2P2	Sr1Ni2P2	Sr	1	Ni	2	P	2																		3	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.951	11.853	10.432												K		1.415					1.415	MTC151281										Oe	from Hc(0)	88							T	SP-heat, WHH	0.039							T/K	SP-heat	0.039					A	from Hc2	920			A		1935													mJ/mol.K2	15	SP-heat	348	SP-heat											mOhm.cm	0.042										0.068														Sn-flux method. (Sr:Ni:P:Sn = 1.3:2:2.3:6) - (alumina crucible) -  (sealed in quartz) - heat(600C,4h + 900C,200h) - cool to 600C(3.5C/h)					Superconductivity and the effects of pressure and structure in single-crystalline SrNi2P2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)134507	F. Ronning,E. D. Bauer,T. Park,S.-H. Baek,H. Sakai,J. D. Thompson		
151282	PRB079113107	not SC upto 23 kbar.  RRR = 1.6. SP-heat measured. [gamma] using data below 2 K.	PrRh2B2C	Pr1Rh2B2C1	Pr	1	Rh	2	B	2	C	1																1	2009					myuB/mol	3.59	-3.9																			ABC2D2	2	LuNi2B2C	I4/mmm		A	3.855		10.257																																																																											mJ/mol.K2	250	SP-heat																																						arc-melting,  ANN(1200C,1w)					Heavy fermion behavior in PrRh2B2C: Excitonic mass enhancement			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	Phys.Rev.B, 79(2009)113107	V. K. Anand,Z. Hossain,G. Chen,M. Nicklas,C. Geibel		
151283	PRL102137002	RRR = 5.2. small R-peak appears at 16 K, which comes  from FM impurity.	EuFe2(As,P)2	Eu1Fe2As1.4P0.6	Eu	1	Fe	2	As	1.4	P	0.6																1	2009	emu/mol	0.044	emu.K/mol	8.1	myuB/mol	8	22																			AB2C2		ThCr2Si2	I4/mmm		A	3.889		11.831												K		26					26																				T	resistivity, linear approx.	30							T/K	resistivity	1.18			MHC151283																				mJ/mol.K	300				345	SP-heat, T>100K						uV/K				MTP151283																								EuAs,Fe2As,Fe2P	1	(mixture powder) - pellet - (sealed in evacuated quartz) - ANN(1273K,20h) - cool to RT					Superconductivity Induced by Phosphorus Doping and Its Coexistence with Ferromagnetism in EuFe2(As0.7P0.3)2			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.Lett., 102(2009)137002	Zhi Ren,Qian Tao,Shuai Jiang,Chunmu Feng,Cao Wang,Jianhui Dai,Guanghan Cao,Zhu'an Xu		
151284	PRL101037001	Cd-concentration shows actual values  (=0.11*nominal values) by wavelength dispersive spectroscopy. Tc by SP-heat.	CeCo(In,Cd)5	Ce1Co1In4.9945Cd0.0055	Ce	1	Co	1	In	4.9945	Cd	0.0055																3	2008																										ABC5		HoCoGa5																		K		2.222					2.222	MTC151284																																																																																															In-flux method					Anisotropic Effect of Cd and Hg Doping on the Pauli Limited Superconductor CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 101(2008)037001	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,P. Papin,A. D. Bianchi,J. F. Rauscher,S. M. Kauzlarich,Z. Fisk		
151285	PRL101037001	Cd-concentration shows actual values  (=0.11*nominal values) by wavelength dispersive spectroscopy. Tc by SP-heat.	CeCo(In,Cd)5	Ce1Co1In4.9835Cd0.0165	Ce	1	Co	1	In	4.9835	Cd	0.0165																3	2008																										ABC5		HoCoGa5																		K		2.15					2.15	MTC151284																																																																																															In-flux method					Anisotropic Effect of Cd and Hg Doping on the Pauli Limited Superconductor CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 101(2008)037001	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,P. Papin,A. D. Bianchi,J. F. Rauscher,S. M. Kauzlarich,Z. Fisk		
151286	PRL101037001	Hg-concentration shows actual values  (=0.11*nominal values) by wavelength dispersive spectroscopy. Tc by SP-heat.	CeCo(In,Hg)5	Ce1Co1In4.9992Hg0.0008	Ce	1	Co	1	In	4.9992	Hg	0.0008																3	2008																										ABC5		HoCoGa5																		K		2.254					2.254																																																																																																In-flux method					Anisotropic Effect of Cd and Hg Doping on the Pauli Limited Superconductor CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 101(2008)037001	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,P. Papin,A. D. Bianchi,J. F. Rauscher,S. M. Kauzlarich,Z. Fisk		
151287	PRL101037001	Hg-concentration shows actual values  (=0.11*nominal values) by wavelength dispersive spectroscopy. Tc by SP-heat.	CeCo(In,Hg)5	Ce1Co1In4.9976Hg0.0024	Ce	1	Co	1	In	4.9976	Hg	0.0024																3	2008																										ABC5		HoCoGa5																		K		2.252					2.252																																																																																																In-flux method					Anisotropic Effect of Cd and Hg Doping on the Pauli Limited Superconductor CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 101(2008)037001	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,P. Papin,A. D. Bianchi,J. F. Rauscher,S. M. Kauzlarich,Z. Fisk		
151288	PRB079140505	Boron-nanowire (BNW): 200 < diameter < 500 nm, 20 < length < 50 um.  P-induce SC. P<cr> = 84 GPa. Tc and (dTc/dP) at 84 GPa. Tc(max) = 5.56 K at 240 GPa.	B-nanowire	B105	B	105																							2009																										A		BNW																	(beta)-(gamma)-B, rhombohedral B105	K		1.5					1.5	MTC151288		K/GPa	0.02																																																																																												CVD method					Pressure-induced superconducting state in crystalline boron nanowires			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)140505	Liling Sun,Takahiro Matsuoka,Yasuyuki Tamari,Katsuya Shimizu,Jifa Tian,Yuan Tian,Chendong Zhang,Chengmin Shen,Wei Yi,Hongjun Gao,Jianqi Li,Xiaoli Dong,Zhongxian Zhao		
151289	PRB079140501	[penet] obtained by data analysis of radio frequency TDO results using two gap model ( higher and lower gaps are 1.7 and 1.01 kTc.	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		3	2009																										ABCD		oxypnictide																		K				45			45																																									A	TDO	1400			kTc	1.7	3.4																																																high-P synthesis using NaCl/KCl flux.					Magnetic penetration depth of single-crystalline SmFeAsO1-xFy			H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, BS8 1TL, United Kingdom	Phys.Rev.B, 79(2009)140501	L. Malone,J. D. Fletcher,A. Serafin,A. Carrington,N. D. Zhigadlo,Z. Bukowski,S. Katrych,J. Karpinski		
151290	PRB069184411	not SC. RRR = 80 at low pressure.	NpCoGa5	Np1Co1Ga5	Np	1	Co	1	Ga	5																		1	2004					myuB/Np	0.34	42	47																		ABC5		HoCoGa5	P4/mmm		A	4.2377		6.7871												K					0.4																																																										mJ/mol.K2	64	SP-heat																																						arc-melting					Magnetic and electronic properties of the antiferromagnet NpCoGa5			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 69(2004)184411	E. Colineau,P. Javorsky,P. Boulet,F. Wastin,J. C. Griveau,J. Rebizant,J. P. Sanchez,G. R. Stewart		
151291	JNM3850011	not SC.	PuPd5Al2	Pu1Pd5Al2	Pu	1	Pd	5	Al	2																		1	2009	emu/mol	0.00069			myuB/mol	1.05	-12.5	5.6																		AB2C5		ZrNi2Al5	I4/nmm		A	4.1302		14.8428												K					2																																																																																																Pd(4N),Al(5N),Pu(3N)		arc-melting					Crystal structure and physical properties of PuPd5Al2			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, 76125 Karlsruhe, Germany	J.Nuclear Mater., 385(2009)11	J.-C. Griveau,K. Gofryk,E. Colineau,J. Rebizant		
151292	JAC4760519	Tc determined as max-(dR/dT). Tc depends on Li-content.	LixNbO2	Li0.5Nb1O2	Li	0.5	Nb	1																	O	2			2009																										ABC2		NaCoO2			A	2.91		10.502												K		16.4					16.4										84.6										T	resistivity,WHH	12.1												HC151292																																																														SIN(1100C,70h) - SIN(1035C,50h) in quartz tube.					Structure and electrical characterization of Li1-xNbO2 superconductor with Tc =14-17K			Key Laboratory of Condition Monitoring and Control for Power Plant Equipment,Ministry of Education, North China Electrical Power University, Beijing 102206, China	J.Alloy Compd., 476(2009)519	Zhiyong Xue,Aifeng Dongb,Yongquan Guoa,Guangchan Che		
151293	PRB079144527	Hc2 defined as 0.8Rn. Hc2(0) calculated using two band theory. G-L  parameter = 190-270.	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95			2009																										ABCD		oxypnictide																		K			25.4				25.4											Oe	linear M-H curve	60							T	resistivity	121												HC151293		A	G-L theory	15			A	G-L theory	3600																																																				1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151294	PRB079144527	Hc2 defined as 0.8Rn. Hc2(0) calculated using two band theory	La(O,F)FeAs	La1Fe1As1F0.07O0.93	La	1	Fe	1	As	1	F	0.07													O	0.93			2009																										ABCD		oxypnictide																		K			25.2				25.2																				T	resistivity	69												HC151294																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151295	PRB079144527	Hc2 defined as 0.8Rn. Hc2(0) calculated using two band theory	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2009																										ABCD		oxypnictide																		K			27.9				27.9																				T	resistivity	59.5												HC151294																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151296	PRB079144527	Hc2 defined as 0.8Rn. Hc2(0) calculated using two band theory	La(O,F)FeAs	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86			2009																										ABCD		oxypnictide																		K			17.8				17.8																				T	resistivity	37.8												HC151294																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151297	JPS078044710	RRR=3.9 and 3.7, G=L parameter = 25.5 and 21.6 for H//[001] and H//[100], respectively. H// represent [001] direction. (dC/gamma*Tc) = 1.4. Hc(0) = 480 and 520 Oe for H// and H/n, respectively.	Ru7B3	Ru7B3	Ru	7	B	3																				3	2009																										A3B7		Th7Fe3	P6<3>mc	186	A	7.441		4.7											hexagonal	K				2.8			2.8											Oe	linear M-H curve		53	68					T	SP-heat		1.72	1.58					T/K	SP-heat		0.782	0.707	MHC151297		A	from Hc2		138	144	A	G-L theory, Hc(0)		3520	3110	meV	0.38	3.3	14							mJ/mol.K2	43.7	SP-heat	640	SP-heat											mOhm.cm		0.014	0.026									0.055	0.097												arc-melting (nominal: Ru/B = 2.0). single crystals grown by Czochralski pulling method in tetra-arc-furnace.					Superconducting State of the Binary Boride Ru7B3 with the Noncentrosymmetric Crystal Structure			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 78(2009)044710	Naoki KASE,Jun AKIMITSU		
151298	JPS078044710	higher Tc due to (maybe) lack of stoichiometry	Ru7B3	Ru7B3	Ru	7	B	3																				1	2009																										A3B7		Th7Fe3	P6<3>mc	186															hexagonal	K				3.3			3.3																																																																																																arc-melting (nominal: Ru/B = 2.0). single crystals grown by Czochralski pulling method in tetra-arc-furnace.					Superconducting State of the Binary Boride Ru7B3 with the Noncentrosymmetric Crystal Structure			Department of Physics and Mathematics, Aoyama Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 78(2009)044710	Naoki KASE,Jun AKIMITSU		
151299	SST022075008	impurity phase: SrFe2P2. Fe-Fe distance = 2.840A. large diamagnetic due to (maybe) porous microstructures.	Sr4Sc2O6Fe2P2	Sr4Sc2Fe2P2O6	Sr	4	Sc	2	Fe	2	P	2													O	6			2009																												22426	P4/nmm		A	4.016		15.543												K	9.8		17	17			17																																																																																														FeP,SrO(2N),Sr(2N),Sc2O3(4N)	1	mixture - heat(900-1200, 12-40h, in evacuated quartz ampoule)					Superconductivity at 17K in (Fe2P2)(Sr4Sc2O6):  a new superconducting layered oxypnictides with thick perovskite oxide layer			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond,Sci.Technol., 22(2009)075008	Hiraku Ogino,Yutaka Matsumura,Yukari Katsura,Koichi Ushiyama,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
151300	PRB079220512	impurity phases: FeAs, Sr2VO4. Hc2 and Hirr defined as 0.9Rn and 0.1Rn, respectively.	Sr4V2O6Fe2As2	Sr4V2Fe2As2O6	Sr	4	V	2	Fe	2	As	2													O	6			2009																												22426	P4/nmm		A	3.9302		15.6664												K	31		37.2	31.5			31.5																				T	resistivity, 0.9Rn	302							T/K	resistivity, 0.9Rn	11.3			HC151300																																																			m3/C					9	RH151300			SrAs,V2O5,SrO,Fe,Sr	1	mixture - sealed in silica tube(0.2bar Ar) - heat(1150C,40h) - slow cool to RT					Transition of stoichiometric Sr2VO3FeAs to a superconducting state at 37.2 K			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P. O. Box 603, Beijing 100190, China	cond-mat/0904.1732	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Bing Shen,Bin Zeng,Hai-Hu Wen		
151301	SSC1490899	Hc2(WHH) = 5.4 T.	Li2(Pd,Ni)3B	Li2Pd2.85Ni0.15B1	Li	2	Pd	2.85	Ni	0.15	B	1																	2009																										AB2C3			P4<2>32																	K		7.91					7.91																				T	resistivity, linear approx.	7.8							T/K	resistivity	1.02					A		78																																																															Upper critical field and thermopower studies in Ni substituted Li2Pd3B superconductor			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam - 603 102, Tamilnadu, India	Solid State Commun., 149(2009)899	Awadhesh Mani,N. Gayathri,A. Bharathi		
151302	SSC1490899	Hc2(WHH) = 5.3 T.	Li2(Pd,Ni)3B	Li2Pd2.7Ni0.3B1	Li	2	Pd	2.7	Ni	0.3	B	1																	2009																										AB2C3			P4<2>32																	K		7.4					7.4																				T	resistivity, linear approx.	7.5							T/K	resistivity	1.02					A		79																																																															Upper critical field and thermopower studies in Ni substituted Li2Pd3B superconductor			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam - 603 102, Tamilnadu, India	Solid State Commun., 149(2009)899	Awadhesh Mani,N. Gayathri,A. Bharathi		
151303	SSC1490899	Hc2(WHH) = 4.8 T.	Li2(Pd,Ni)3B	Li2Pd2.4Ni0.6B1	Li	2	Pd	2.4	Ni	0.6	B	1																	2009																										AB2C3			P4<2>32																	K		6.91					6.91																				T	resistivity, linear approx.	6.9							T/K	resistivity	1.02					A		83																																																															Upper critical field and thermopower studies in Ni substituted Li2Pd3B superconductor			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam - 603 102, Tamilnadu, India	Solid State Commun., 149(2009)899	Awadhesh Mani,N. Gayathri,A. Bharathi		
151304	1257		Re1-xWx	Re0.999W0.001	Re	0.999	W	0.001																					1970																																													bcc	K		1.723					1.723	MTC151304																																																																																																				Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
151305	1257		Re1-xMox	Re0.9993Mo0.0007	Re	0.9993	Mo	0.0007																					1970																																													bcc	K		1.694					1.694	MTC151305																																																																																																				Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
151306	1257		Re1-xOsx	Re0.9467Os0.0533	Re	0.9467	Os	0.0533																					1970																																													bcc	K		1.934					1.934	MTC151306																																																																																																				Study of fermi-surface topology changes in rhenium and dilute Re solid solutions from Tc measurements at high pressure				PHYS.REV.B,1(1970)214	C.W.CHU,T.F.SMITH,W.E.GARDNER		
151307	658	Tc measured upto P(max) = 0.9 GPa.	La7Rh3	La7Rh3	La	7	Rh	3																					1967																										A3B7																				K		2.58					2.58			K/GPa	-0.28																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
151308	658	Tc measured upto P(max) = 1.3 GPa.	La7Ir3	La7Ir3	La	7	Ir	3																					1967																										A3B7																				K		2.33					2.33			K/GPa	-0.22																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
151309	658	Tc measured upto P(max) = 1.1 GPa.	LaAl2	La1Al2	La	1	Al	2																					1967																										AB2																				K		3.23					3.23			K/GPa	-0.175																																																																																																	Superconductivity of lanthanum and lanthanum compounds at zero and high pressure				J.PHYS.CHEM.SOLIDS,28(1967)569	H.L.LUO,T.F.SMITH		
151310	NJP011025008	not SC	Ba(Fe,Ni)2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2			A			13.03												K					4																																																																				uV/K	-4.66			MTP151310																								Ba-rod,Fe and Ni-powder,As-pieces		self-flux method. Ba:(FeAs/NiAs) = 1:5, mixture - (sealed in quartz tube) - heat(973K,5h) - -heat(1453K,10h) - cool to 1363 K (2K/h)					Superconductivity induced by Ni doping in BaFe2As2 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)025008	L J Li,Y K Luo,Q B Wang,H Chen,Z Ren,Q Tao,Y K Li,X Lin,M He,Z W Zhu,G H Cao,Z A Xu		
151311	NJP011025008		Ba(Fe,Ni)2As2	Ba1Fe1.945Ni0.055As2	Ba	1	Fe	1.945	Ni	0.055	As	2																3	2009																										AB2C2		ThCr2Si2			A			13.016												K		7.4	12.56				7.4																																																																		uV/K	-18.2			MTP151310																								Ba-rod,Fe and Ni-powder,As-pieces		self-flux method. Ba:(FeAs/NiAs) = 1:5, mixture - (sealed in quartz tube) - heat(973K,5h) - -heat(1453K,10h) - cool to 1363 K (2K/h)					Superconductivity induced by Ni doping in BaFe2As2 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)025008	L J Li,Y K Luo,Q B Wang,H Chen,Z Ren,Q Tao,Y K Li,X Lin,M He,Z W Zhu,G H Cao,Z A Xu		
151312	NJP011025008		Ba(Fe,Ni)2As2	Ba1Fe1.904Ni0.096As2	Ba	1	Fe	1.904	Ni	0.096	As	2																3	2009																										AB2C2		ThCr2Si2			A			12.995												K		20.2	20.5			1	20.2																																																																		uV/K	-24.4			MTP151312																								Ba-rod,Fe and Ni-powder,As-pieces		self-flux method. Ba:(FeAs/NiAs) = 1:5, mixture - (sealed in quartz tube) - heat(973K,5h) - -heat(1453K,10h) - cool to 1363 K (2K/h)					Superconductivity induced by Ni doping in BaFe2As2 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)025008	L J Li,Y K Luo,Q B Wang,H Chen,Z Ren,Q Tao,Y K Li,X Lin,M He,Z W Zhu,G H Cao,Z A Xu		
151313	NJP011025008		Ba(Fe,Ni)2As2	Ba1Fe1.82Ni0.18As2	Ba	1	Fe	1.82	Ni	0.18	As	2																3	2009																										AB2C2		ThCr2Si2			A			12.985												K		17.4	18.4				17.4																																																																		uV/K	-25.7			MTP151312																								Ba-rod,Fe and Ni-powder,As-pieces		self-flux method. Ba:(FeAs/NiAs) = 1:5, mixture - (sealed in quartz tube) - heat(973K,5h) - -heat(1453K,10h) - cool to 1363 K (2K/h)					Superconductivity induced by Ni doping in BaFe2As2 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)025008	L J Li,Y K Luo,Q B Wang,H Chen,Z Ren,Q Tao,Y K Li,X Lin,M He,Z W Zhu,G H Cao,Z A Xu		
151314	NJP011025008		Ba(Fe,Ni)2As2	Ba1Fe1.77Ni0.23As2	Ba	1	Fe	1.77	Ni	0.23	As	2																3	2009																										AB2C2		ThCr2Si2			A			12.968												K		3.53	5.43				3.53																																																																																														Ba-rod,Fe and Ni-powder,As-pieces		self-flux method. Ba:(FeAs/NiAs) = 1:5, mixture - (sealed in quartz tube) - heat(973K,5h) - -heat(1453K,10h) - cool to 1363 K (2K/h)					Superconductivity induced by Ni doping in BaFe2As2 single crystals			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)025008	L J Li,Y K Luo,Q B Wang,H Chen,Z Ren,Q Tao,Y K Li,X Lin,M He,Z W Zhu,G H Cao,Z A Xu		
151315	PRB079132506	size = 0.50*0.13*0.013mm3. carrier is electron-type (toally). RRR=18.7 and 34.3 for in- and out-of plane. Tc=2.31 K for out-of plane resistivity. anisotropy (Hc2) = 2.2.	BaNi2P2	Ba1Ni2P2	Ba	1	Ni	2	P	2																		3	2009																										AB2C2		ThCr2Si2																		K		2.51					2.51										56	Oe	M-H curve					52	82	2	T	midpoint in R(T)		0.141	0.065										MHC151315	midpoint in R(T)	A	from Hc2(0)		710	330																															uOhm.cm								4.15	14.4			80	500							MRH151315					high-P-synthesis using cubic-anvil					Three-dimensional nature of normal and superconducting states in BaNi2P2 single crystals with the ThCr2Si2-type structure			Nano Electronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba 305-8562, Japan	Phys.Rev.B, 79(2009)132506	Y. Tomioka,S. Ishida,M. Nakajima,T. Ito,H. Kito,A. Iyo,H. Eisaki,S. Uchida		
151316	PRB079140509	structural and magnetic transition at 65 K.	FeTe	Fe1.05Te1	Fe	1.05	Te	1																				3	2009																										AB																				K					1.8																																																										mJ/mol.K2	34	SP-heat	141	SP-heat																																				Bridgeman method. mixture(Fe-Te,Fe-Se-Te) - (sealed in evacuated quartz tube) - heat(920C) - cool (4C/h)					Electronic properties of single-crystalline Fe1.05Te and Fe1.03Se0.30Te0.70			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)140509	G. F. Chen,Z. G. Chen,J. Dong,W. Z. Hu,G. Li,X. D. Zhang,P. Zheng,J. L. Luo,N. L. Wang		
151317	PRB079140509		Fe(Te,Se)	Fe1.03Te0.7Se0.3	Fe	1.03	Te	0.7	Se	0.3																		3	2009																										AB																				K		12.4					12.4																				T	midpoint in R(T)		51	31					T/K	midpoint in R(T)		5.96	3.69	MHC151317																																																									MRH151317					Bridgeman method. mixture(Fe-Te,Fe-Se-Te) - (sealed in evacuated quartz tube) - heat(920C) - cool (4C/h)					Electronic properties of single-crystalline Fe1.05Te and Fe1.03Se0.30Te0.70			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)140509	G. F. Chen,Z. G. Chen,J. Dong,W. Z. Hu,G. Li,X. D. Zhang,P. Zheng,J. L. Luo,N. L. Wang		
151318	PRB079144527	Hall coeffic. RH(50K)=0.253 cm3/C. DOS = 0.682 states/eV from SP-data.	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1		1	2009																										ABCD		oxypnictide																		K					5																																																																																																	1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151319	PRB079144527	Hall coeffic. RH(50K)=0.0621 cm3/C. DOS = 1.36 states/eV from SP-data.	La(O,F)FeAs	La1Fe1As1F0.025O0.975	La	1	Fe	1	As	1	F	0.025													O	0.975		1	2009																										ABCD		oxypnictide																		K					4																																																																																																	1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151320	PRB079144527	Hall coeffic. RH(50K)=11.3 E-3 cm3/C. DOS = 3.56 states/eV from SP-data. G-L parameter = 190-270. Hc2 defined as R=0.8Rn. [cohere]=15-19A. [penet]=3600-4100A.	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95		1	2009																										ABCD		oxypnictide																		K				25.5			25.5											Oe	M-H curve	60							T	R=0.8Rn, two band model	122												HC151320		A		15			A	from Hc1	3600																																																				1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151321	PRB079144527	Hall coeffic. RH(50K)=7.66 E-3 cm3/C. Hc2 defined as R=0.8Rn.	La(O,F)FeAs	La1Fe1As1F0.07O0.93	La	1	Fe	1	As	1	F	0.07													O	0.93		1	2009																										ABCD		oxypnictide																		K				25.2			25.2																				T	R=0.8Rn, two band model	69.6												HC151321																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151322	PRB079144527	Hall coeffic. RH(50K)=5.98 E-3 cm3/C. DOS = 2.18 states/eV from SP-data.  Hc2 defined as R=0.8Rn.	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2009																										ABCD		oxypnictide																		K				27.9			27.9																				T	R=0.8Rn, two band model	59.9												HC151322																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151323	PRB079144527	Hall coeffic. RH(50K)=2.55 E-3 cm3/C. DOS = 1.61 states/eV from SP-data.  Hc2 defined as R=0.8Rn.	La(O,F)FeAs	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86		1	2009																										ABCD		oxypnictide																		K				18			18																				T	R=0.8Rn, two band model	37.5												HC151323																																																													1	solid state reaction					Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1-xFx  (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 79(2009)144527	Y. Kohama,Y. Kamihara,S. A. Baily,L. Civale,S. C. Riggs,F. F. Balakirev,T. Atake,M. Jaime,M. Hirano,H. Hosono		
151324	PRB079172506	single crystal (surface: (001).  P-induce SC.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K			35		0		35	MTC151324																																																																																															high-P-synthesis using cubic anvil. mixture - heat(1473K,2h,P=3GPa, in BN crucible)					Zero-resistance superconducting phase in BaFe2As2 under high pressure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	Phys.Rev.B, 79(2009)172506	Fumihiro Ishikawa,Naoya Eguchi,Michihiro Kodama,Koji Fujimaki,Mari Einaga,Ayako Ohmura,Atsuko Nakayama,Akihiro Mitsuda,Yuh Yamada		
151325	JPS077105004		BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2008																										AB2C2		ThCr2Si2																		K			34		0		34	MTC151325																																																																																															high-p & high-T synthesis					Suppression of Magnetic Order by Pressure in BaFe2As2			Department of Physics, Chiba University, Chiba 263-8522	J.Phys.Soc,Jpn, 77(2008)105004	Hideto FUKAZAWA,Nao TAKESHITA,Takehiro YAMAZAKI,Kenji KONDO,Kenji HIRAYAMA,Yoh KOHORI,Kiichi MIYAZAWA,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
151326	PRB079172507	P-induced SC. several % impurity phases(CePt2Si2, CePtSi3). (dTn/dP) = -1 K/GPa. SC-properties at P=1.7 GPa. [lattice const] and [gamma] from PRB04206542.	CePtSi2	Ce1Pt1Si2	Ce	1	Pt	1	Si	2																		1	2009								1.8																		ABC2		CeNiSi2	Cmcm		A	4.288	16.718	4.238												K			0.14		0		0.14										30										T	P=1.7 GPa	0.7																																		mJ/mol.K2	145	SP-heat, 14 < T < 30 K	298	SP-heat, 14 < T < 30 K																																				arc-melting. ANN(1000C,3w, in vac)					Pressure-induced superconductivity in the orthorhombic Kondo compound CePtSi2			Department of Physics, Kyushu University, Hakozaki 6-10-1, Fukuoka 810-8581, Japan	Phys.Rev.B, 79(2009)172507	Tomohito Nakano,Masashi Ohashi,Gendo Oomi,Kazuyuki Matsubayashi,Yoshiya Uwatoko		
151327	PRB079174505	(dC/gamma*Tc) = 0.73. lattice term coeff. in C (beta) = 0.254 mJ/mol.K4	LaO(Fe,Ni)As	La1Fe0.96Ni0.04As1O1	La	1	Fe	0.96	Ni	0.04	As	1													O	1			2009																										ABCD		oxypnictide	P4/nmm		A	4.0376		8.7208											ZrCuSiAs	K			6.5				6.5	TC151327									45										T	R=0.5Rn, WHH	17							T/K	midpoint in R(T)	3.81			HC151327																						mJ/mol.K2	5.74	SP-heat	285	SP-heat																																		LaAs,La2O3,FeAs,Fe2As,NiO		solid state reaction.  Heat(1433K, 48h)					Narrow superconducting window in LaFe1-xNixAsO			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 79(2009)174505	Guanghan Cao,Shuai Jiang,Xiao Lin,Cao Wang,Yuke Li,Zhi Ren,Qian Tao,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Fu-Chun Zhang		
151328	NJP011025013		(Sr,K)Fe2As2	Sr0.8K0.2Fe2As2	Sr	0.8	K	0.2	Fe	2	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9071		12.613												K		13.6					13.6																				T	R=0.5Rn, GL theory	32.5												MHC151328																																																														mixture(KFe2As2, SrFe2As2) - (compress) - ANN(700C,100-120h, in welded Nb container)					The superconductor KxSr1-xFe2As2: normal state and superconducting properties			TCSUH and Department of Chemistry, University of Houston, Houston, TX 77204, USA	New J.Phys., 11(2009)025013	B Lv,M Gooch,B Lorenz,F Chen,A M Guloy,C W Chu		
151329	NJP011025013		(Sr,K)Fe2As2	Sr0.42K0.58Fe2As2	Sr	0.42	K	0.58	Fe	2	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.8852		12.988												K		36					36	MTC151329																			T	R=0.5Rn, GL theory	197.4												MHC151329																																																														mixture(KFe2As2, SrFe2As2) - (compress) - ANN(700C,100-120h, in welded Nb container)					The superconductor KxSr1-xFe2As2: normal state and superconducting properties			TCSUH and Department of Chemistry, University of Houston, Houston, TX 77204, USA	New J.Phys., 11(2009)025013	B Lv,M Gooch,B Lorenz,F Chen,A M Guloy,C W Chu		
151330	NJP011025013		(Sr,K)Fe2As2	Sr0.67K0.33Fe2As2	Sr	0.67	K	0.33	Fe	2	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.8711		13.309												K		21.7					21.7																				T	R=0.5Rn, GL theory	64.3												MHC151330																																																														mixture(KFe2As2, SrFe2As2) - (compress) - ANN(700C,100-120h, in welded Nb container)					The superconductor KxSr1-xFe2As2: normal state and superconducting properties			TCSUH and Department of Chemistry, University of Houston, Houston, TX 77204, USA	New J.Phys., 11(2009)025013	B Lv,M Gooch,B Lorenz,F Chen,A M Guloy,C W Chu		
151331	NJP011025013		(Sr,K)Fe2As2	Sr0.9K0.1Fe2As2	Sr	0.9	K	0.1	Fe	2	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.8551		13.745												K		5.11					5.11																				T	R=0.5Rn, GL theory	7.79												MHC151331																																																														mixture(KFe2As2, SrFe2As2) - (compress) - ANN(700C,100-120h, in welded Nb container)					The superconductor KxSr1-xFe2As2: normal state and superconducting properties			TCSUH and Department of Chemistry, University of Houston, Houston, TX 77204, USA	New J.Phys., 11(2009)025013	B Lv,M Gooch,B Lorenz,F Chen,A M Guloy,C W Chu		
151332	NJP011025013		(Sr,K)Fe2As2	Sr0.5K0.5Fe2As2	Sr	0.5	K	0.5	Fe	2	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm																	K		37.7					37.7																				T	R=0.5Rn, GL theory	204.5												MHC151332																																																														mixture(KFe2As2, SrFe2As2) - (compress) - ANN(700C,100-120h, in welded Nb container)					The superconductor KxSr1-xFe2As2: normal state and superconducting properties			TCSUH and Department of Chemistry, University of Houston, Houston, TX 77204, USA	New J.Phys., 11(2009)025013	B Lv,M Gooch,B Lorenz,F Chen,A M Guloy,C W Chu		
151333	NJP011025005	impurity phases: Ho2O3, HoAs, FeAs	HoO0.8FeAs	Ho1Fe1As1O0.85	Ho	1	Fe	1	As	1															O	0.85		1	2009																												oxypnictide	P4/nmm		A	3.846		8.295											ZrCuSiAs	K			50.3	49.1			49.1																																																																																																RAs obtained by reacting(650C,12h + 1180C,40h). mixture(RAs,Fe,Fe2O3) - sealed in BN crucible) - heat(100C,1h, P=5GPa) - rapid cool to RT					Superconductivity in some heavy rare-earth iron arsenide REFeAsO1-d  (RE=Ho, Y, Dy and Tb) compounds			National Laboratory for Superconductivity, Institute of Physics and BeijingNational Laboratory for Condensed Matter Physics, Chinese Academyof Sciences, Beijing 100190, People's Republic of China	New J.Phys., 11(2009)025005	Jie Yang,Xiao-Li Shen,Wei Lu,Wei Yi,Zheng-Cai Li,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
151334	NJP011025005	impurity phases: Y2O3, YAs, FeAs	YO0.8FeAs	Y1Fe1As1O0.85	Y	1	Fe	1	As	1															O	0.85		1	2009																												oxypnictide	P4/nmm		A	3.842		8.303											ZrCuSiAs	K			46.5	45.2			45.2																																																																																																RAs obtained by reacting(650C,12h + 1180C,40h). mixture(RAs,Fe,Fe2O3) - sealed in BN crucible) - heat(100C,1h, P=5GPa) - rapid cool to RT					Superconductivity in some heavy rare-earth iron arsenide REFeAsO1-d  (RE=Ho, Y, Dy and Tb) compounds			National Laboratory for Superconductivity, Institute of Physics and BeijingNational Laboratory for Condensed Matter Physics, Chinese Academyof Sciences, Beijing 100190, People's Republic of China	New J.Phys., 11(2009)025005	Jie Yang,Xiao-Li Shen,Wei Lu,Wei Yi,Zheng-Cai Li,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
151335	NJP011025005	impurity phases: Dy2O3, DyAs, FeAs	DyO0.8FeAs	Dy1Fe1As1O0.85	Dy	1	Fe	1	As	1															O	0.85		1	2009																												oxypnictide	P4/nmm		A	3.859		8.341											ZrCuSiAs	K			52.2	51			51																																																																																																RAs obtained by reacting(650C,12h + 1180C,40h). mixture(RAs,Fe,Fe2O3) - sealed in BN crucible) - heat(100C,1h, P=5GPa) - rapid cool to RT					Superconductivity in some heavy rare-earth iron arsenide REFeAsO1-d  (RE=Ho, Y, Dy and Tb) compounds			National Laboratory for Superconductivity, Institute of Physics and BeijingNational Laboratory for Condensed Matter Physics, Chinese Academyof Sciences, Beijing 100190, People's Republic of China	New J.Phys., 11(2009)025005	Jie Yang,Xiao-Li Shen,Wei Lu,Wei Yi,Zheng-Cai Li,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
151336	NJP011025005	impurity phases: Tb2O3, TbAs, FeAs	TbO0.8FeAs	Tb1Fe1As1O0.85	Tb	1	Fe	1	As	1															O	0.85		1	2009																												oxypnictide	P4/nmm		A	3.878		8.354											ZrCuSiAs	K			48.5	46.8	1.8		46.8																																																																																																RAs obtained by reacting(650C,12h + 1180C,40h). mixture(RAs,Fe,Fe2O3) - sealed in BN crucible) - heat(100C,1h, P=5GPa) - rapid cool to RT					Superconductivity in some heavy rare-earth iron arsenide REFeAsO1-d  (RE=Ho, Y, Dy and Tb) compounds			National Laboratory for Superconductivity, Institute of Physics and BeijingNational Laboratory for Condensed Matter Physics, Chinese Academyof Sciences, Beijing 100190, People's Republic of China	New J.Phys., 11(2009)025005	Jie Yang,Xiao-Li Shen,Wei Lu,Wei Yi,Zheng-Cai Li,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
151337	NJP011025005	not SC.	TbOFeAs	Tb1Fe1As1O1	Tb	1	Fe	1	As	1															O	1		1	2009																												oxypnictide	P4/nmm		A	3.898		8.404											ZrCuSiAs	K																																																																																																							RAs obtained by reacting(650C,12h + 1180C,40h). mixture(RAs,Fe,Fe2O3) - sealed in BN crucible) - heat(100C,1h, P=5GPa) - rapid cool to RT					Superconductivity in some heavy rare-earth iron arsenide REFeAsO1-d  (RE=Ho, Y, Dy and Tb) compounds			National Laboratory for Superconductivity, Institute of Physics and BeijingNational Laboratory for Condensed Matter Physics, Chinese Academyof Sciences, Beijing 100190, People's Republic of China	New J.Phys., 11(2009)025005	Jie Yang,Xiao-Li Shen,Wei Lu,Wei Yi,Zheng-Cai Li,Zhi-An Ren,Guang-Can Che,Xiao-Li Dong,Li-Ling Sun,Fang Zhou,Zhong-Xian Zhao		
151338	NJP011025006	T* = 110 K at ambient pressure. (dT*/dP) = -4.69 K/GPa estimated from Fig.7 where T* is the temperature of TP(max).	SmO0.85FeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85			2009																												oxypnictide	P4/nmm																ZrCuSiAs	K			53				53			K/GPa	-1.5																																																														uV/K				TP151338																										high-P-synthesis					Pressure dependence of the thermoelectric power of the iron-based high-Tc superconductor SmFeAsO0.85			Laboratoire de Physique des Solides, Universite Paris-Sud, 91405 Orsay, France	New J.Phys., 11(2009)025006	N Kang,P Auban-Senzier,C R Pasquier,Z A Ren,J Yang,G C Che,Z X Zhao		
151339	NJP011025012	not SC.	CaF(Fe,Co)As	Ca1Fe0.95Co0.05F1	Ca	1	Fe	0.95	Co	0.05	F	1																	2009																													P4/nmm		A	3.8801		8.5775											ZrCuSiAs	K					2																																																																																																CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151340	NJP011025012		CaF(Fe,Co)As	Ca1Fe0.93Co0.07F1	Ca	1	Fe	0.93	Co	0.07	F	1																	2009																													P4/nmm		A	3.8804		8.5626											ZrCuSiAs	K			9.1				9.1																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151341	NJP011025012		CaF(Fe,Co)As	Ca1Fe0.9Co0.1As1F1	Ca	1	Fe	0.9	Co	0.1	As	1	F	1															2009																													P4/nmm		A	3.8801		8.5517											ZrCuSiAs	K			23				23	MTC151341																																																																																													CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151342	NJP011025012		CaF(Fe,Co)As	Ca1Fe0.85Co0.15As1F1	Ca	1	Fe	0.85	Co	0.15	As	1	F	1															2009																													P4/nmm		A	3.8815		8.5374											ZrCuSiAs	K			21.2				21.2																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151343	NJP011025012		CaF(Fe,Co)As	Ca1Fe0.8Co0.2As1F1	Ca	1	Fe	0.8	Co	0.2	As	1	F	1															2009																													P4/nmm		A	3.8827		8.5261											ZrCuSiAs	K			16.6				16.6																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151344	NJP011025012		CaF(Fe,Co)As	Ca1Fe0.74Co0.26As1F1	Ca	1	Fe	0.74	Co	0.26	As	1	F	1															2009																													P4/nmm		A	3.8831		8.4997											ZrCuSiAs	K			3.49				3.49																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151345	NJP011025012	not SC	CaF(Fe,Ni)As	Ca1Fe0.95Ni0.05As1F1	Ca	1	Fe	0.95	Ni	0.05	As	1	F	1															2009																													P4/nmm		A	3.8794		8.5777											ZrCuSiAs	K					2																																																																																																CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151346	NJP011025012		CaF(Fe,Ni)As	Ca1Fe0.9Ni0.1As1F1	Ca	1	Fe	0.9	Ni	0.1	As	1	F	1															2009																													P4/nmm		A	3.8828		8.5541											ZrCuSiAs	K			15.4				15.4																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151347	NJP011025012		CaF(Fe,Ni)As	Ca1Fe0.85Ni0.15As1F1	Ca	1	Fe	0.85	Ni	0.15	As	1	F	1															2009																													P4/nmm		A	3.8845		8.5359											ZrCuSiAs	K			8.72				8.72	MTC151347																																																																																													CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151348	NJP011025012		CaF(Fe,Ni)As	Ca1Fe0.8Ni0.2As1F1	Ca	1	Fe	0.8	Ni	0.2	As	1	F	1															2009																													P4/nmm		A	3.8854		8.528											ZrCuSiAs	K			3.92				3.92																																																																																														CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151349	NJP011025012	not SC for 0=< x =<0.20 in CaFe1-xCrxAsF	CaF(Fe,Cr)As	Ca1Fe0.9Cr0.1As1F1	Ca	1	Fe	0.9	Cr	0.1	As	1	F	1															2009																													P4/nmm		A	3.8749		8.638											ZrCuSiAs	K					2																																																																																																CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151350	NJP011025012	not SC for 0=< x =<0.15 in CaFe1-xMnxAsF	CaF(Fe,Mn)As	Ca1Fe0.9Mn0.1As1F1	Ca	1	Fe	0.9	Mn	0.1	As	1	F	1															2009																													P4/nmm		A	3.887		8.6308											ZrCuSiAs	K					2																																																																																																CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151351	NJP011025012	not SC	CaF(Fe,Cu)As	Ca1Fe0.95Cu0.05As1F1	Ca	1	Fe	0.95	Cu	0.05	As	1	F	1															2009																													P4/nmm		A	3.8875		8.5884											ZrCuSiAs	K					2																																																																																																CaF2,CaAs,Fe2As,T2As(T=Co,Ni,Cu,Cr,Mn)		mixture - heat(1000C,10h, in evacuated silica tube)					Effect of 3d transition metal doping on the superconductivity in quaternary fluoroarsenide CaFeAsF			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	New J.Phys., 11(2009)025012	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Youichi Kamihara,Masahiro Hirano,Hideo Hosono		
151352	EPL08357002	(dTc/dP) = -1.3 and -2.0 K/GPa for the definition of Tc(on) and Tc(SUS), respectively	SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm																ZrCuSiAs	K			55				55			K/GPa	-2																																																																																												high-P synthesis					Pressure effect on superconductivity of iron-based arsenic-oxide ReFeAsO0.85 (Re = Sm and Nd)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - Beijing 100190, PRC	EuroPhys.Lett., 83(2008)57002	Wei Yi,Liling Sun,Zhian Ren,Wei Lu,Xiaoli Dong,Hai-jun Zhang,Xi Dai,Zhong Fang,Zhengcai Li,Guangcan Che,Jie Yang,Xiaoli Shen,Fang Zhou,Zhongxian Zhao		
151353	EPL08357002		NdOFeAs	Nd1Fe1As1O0.85	Nd	1	Fe	1	As	1															O	0.85		1	2008																												oxypnictide	P4/nmm																ZrCuSiAs	K			51.9				51.9			K/GPa	-2.6																																																																																												high-P synthesis					Pressure effect on superconductivity of iron-based arsenic-oxide ReFeAsO0.85 (Re = Sm and Nd)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - Beijing 100190, PRC	EuroPhys.Lett., 83(2008)57002	Wei Yi,Liling Sun,Zhian Ren,Wei Lu,Xiaoli Dong,Hai-jun Zhang,Xi Dai,Zhong Fang,Zhengcai Li,Guangcan Che,Jie Yang,Xiaoli Shen,Fang Zhou,Zhongxian Zhao		
151354	JPS077075003	nearly hydrostatic pressure upto 18 GPa. (dTc/dP) obtained for around 8 GPa.	NdOFeAs	Nd1Fe1As1O0.6	Nd	1	Fe	1	As	1															O	0.6			2008																												oxypnictide																		K			54				54	TC151354		K/GPa	-3																																																																																												high-P synthesis					Remarkable Suppression of Tc by Pressure in NdFeAsO1-y ( y = 0.4)			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8562	J.Phys.Soc.Jpn, 77(2008)075003	Nao TAKESHITA,Akira IYO,Hiroshi EISAKI,Hijiri KITO,Toshimitsu ITO		
151355	EPL08467007	not SC. phase transition(structural and magnetic) at 175 K. lattice term in SP (beta) = 0.2 mJ/mol.K4	SrFFeAs	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																	2008																													P4/nmm		A	3.993		8.9546											ZrCuSiAs	K					4																																																										mJ/mol.K2	1.5	SP-heat	339	SP-heat																																				(SrF2:Sr:Fe:As = 1:1:2:2, in sealed Nb tube) - heat to 1173K(50K/h) - hold(40h) - cool to RT - SIN(1273K,48h)					Synthesis, crystal structure and spin-density-wave anomaly of the iron arsenide-fluoride SrFeAsF			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen - Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany, EU	EuroPhys.Lett., 84(2008)67007	M. Tegel,S. Johansson,V. Weiss,I. Schellenberg,W. Hermes,R. Pottgen,D. Johrendt		
151356	PRB078180503	not SC. T<SDW> = 173 K. Hall coeff. RH(T) obtained from Rxy(H,T).	SrFFeAs	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																	2008																													P4/nmm		A	4.004		8.971											ZrCuSiAs	K					2																																																																																													MRH151356			FeAs,Fe,FeF3		mixture - pellet - sealed in quartz tube(0.2 bar Ar) - heat(950C,60h) - cool to RT					SrFeAsF as a parent compound for iron pnictide superconductors			National Laboratory for Superconductivity, Institute of Physics, and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 78(2008)180503	Fei Han,Xiyu Zhu,Gang Mu,,Peng Cheng,Hai-Hu Wen		
151357	PRB079174511	oriented crystal. applied field //<100> for muon-SR.	PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																			2009																												skutterudite																		K		1.85					1.85																																									A	muon-SR	3534					4.9	16																																																				Penetration depth, multiband superconductivity, and absence of muon-induced perturbation in superconducting PrOs4Sb12			Department of Physics, University of California, Riverside, California 92521, USA	Phys.Rev.B, 79(2009)174511	Lei Shu,D. E. MacLaughlin,W. P. Beyermann,R. H. Heffner,G. D. Morris,O. O. Bernal,F. D. Callaghan,J. E. Sonier,W. M. Yuhasz,N. A. Frederick,M. B. Maple		
151358	PRB079174523	T<SDW> = 138 K defined as R(T) anomaly.	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2009																												oxypnictide	P4/nmm		A	4.0328		8.7446											ZrCuSiAs	K					10																																																																																																(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151359	PRB079174523	T<SDW> = 130 K defined as R(T) anomaly.	(La,Y)OFeAs	La0.7Y0.3Fe1As1O1	La	0.7	Y	0.3	Fe	1	As	1													O	1			2009																												oxypnictide	P4/nmm		A	4.0009		8.6856											ZrCuSiAs	K					10																																																																																																(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151360	PRB079174523	T<SDW> = 125 K defined as R(T) anomaly.	(La,Y)OFeAs	La0.5Y0.5Fe1As1O1	La	0.5	Y	0.5	Fe	1	As	1													O	1			2009																												oxypnictide	P4/nmm		A	3.9761		8.6326											ZrCuSiAs	K					10																																																																																																(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151361	PRB079174523	T<SDW> = 120 K defined as R(T) anomaly.	(La,Y)OFeAs	La0.3Y0.7Fe1As1O1	La	0.3	Y	0.7	Fe	1	As	1													O	1			2009																												oxypnictide	P4/nmm		A	3.9623		8.5976											ZrCuSiAs	K					10																																																																																																(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151362	PRB079174523		LaOFeAs	La1Fe1As1F0.15O0.85	La	1	Fe	1	As	1	F	0.15													O	0.85			2009																												oxypnictide	P4/nmm		A	4.0269		8.7097											ZrCuSiAs	K			24.3				24.3																																																																																														(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151363	PRB079174523	impurity: (La,Y)As 6.4 %, (La,Y)OF  8%.	(La,Y)(O,F)FeAs	La0.7Y0.3Fe1As1F0.15O0.85	La	0.7	Y	0.3	Fe	1	As	1	F	0.15											O	0.85			2009																												oxypnictide	P4/nmm		A	3.9977		8.662											ZrCuSiAs	K			36.2				36.2										30																																																																																				(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151364	PRB079174523		(La,Y)(O,F)FeAs	La0.5Y0.5Fe1As1F0.15O0.85	La	0.5	Y	0.5	Fe	1	As	1	F	0.15											O	0.85			2009																												oxypnictide	P4/nmm		A	3.9759		8.6248											ZrCuSiAs	K			40.2				40.2																																																																																														(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151365	PRB079174523		(La,Y)(O,F)FeAs	La0.3Y0.7Fe1As1F0.15O0.85	La	0.3	Y	0.7	Fe	1	As	1	F	0.15											O	0.85			2009																												oxypnictide	P4/nmm		A	3.9519		8.5777											ZrCuSiAs	K			38				38										15																																																																																				(La,Y)As,Fe2O3,Fe,FeF3		solid state reaction. two step reaction using Ta-crucible. heat(1000C,70h) - ANN(1250C,25h)					Effect of chemical pressure on spin density wave and superconductivity in undoped and 15% F-doped La1-yYyFeAsO compounds			CNR/INFM-LAMIA, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 79(2009)174523	M. Tropeano,C. Fanciulli,F. Canepa,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,M. Putti,M. Vignolo,A. Palenzona		
151366	DRM0160911	<111> films. carrier n = 8.4 E+21/cm3 (B/C = 5 %). Hc2 = 15.7T and Hirr = 9 T from linear approx.  in-plane thermal expansion = 0.48 %.	B-doped C	C1	C	1																							2007																												diamond																		K	7.4		11.4				9.4																				T	resistivity, GL approx.	10.8														A		55.1																																																										microwave plasma-assisted CVD on Si<001> substrates.					Superconducting properties of homoepitaxial CVD diamond			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Diamond Relat.Mater., 16(2007)911	Y. Takano,T. Takenouchi,S. Ishii,S. Ueda,T. Okutsu,I. Sakaguchi,H. Umezawa,H. Kawarada,M. Tachiki		
151367	DRM0160911	<111> films. carrier n = 8.2 E+21/cm3. Hc2 = 7.7T and Hirr = 4.5 T from linear approx.  in-plane thermal expansion = 0.46 %.	B-doped C	C1	C	1																							2007																												diamond																		K	3.2		6.3				4.75																				T	resistivity, GL approx.	5.3														A		78.9																																																										microwave plasma-assisted CVD on Si<001> substrates.					Superconducting properties of homoepitaxial CVD diamond			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Diamond Relat.Mater., 16(2007)911	Y. Takano,T. Takenouchi,S. Ishii,S. Ueda,T. Okutsu,I. Sakaguchi,H. Umezawa,H. Kawarada,M. Tachiki		
151368	SST021065019	crystals contain Cr and Ga precipitation. SC maybe comes from Ga precipitation(beta-Ga)	Cr-doped GaP	Ga1P1	Ga	1	P	1																					2008																																														K		6.2					6.2																				T		0.06																																																																															The appearance of superconductivity in GaP and GaAs samples highly doped with Cr			Institute of Experimental Physics, University of Warsaw, Hoza 69, PL-00-681Warsaw, Poland	Supercond.Sci.Technol., 21(2008)065019	J BGosk,R Puzniak,G Strzelecka,A Materna,A Hruban,AWisniewski,A Szewczyk,G Kowalski,K Korona,MKaminska,A Twardowski		
151369	SST021065019	crystals contain Cr and Ga precipitation. SC properties maybe from beta-Ga precipitations.	Cr-doped GaAs	As1Ga1	As	1	Ga	1																					2008																																														K		6.2					6.2																				T		0.06																																																																															The appearance of superconductivity in GaP and GaAs samples highly doped with Cr			Institute of Experimental Physics, University of Warsaw, Hoza 69, PL-00-681Warsaw, Poland	Supercond.Sci.Technol., 21(2008)065019	J BGosk,R Puzniak,G Strzelecka,A Materna,A Hruban,AWisniewski,A Szewczyk,G Kowalski,K Korona,MKaminska,A Twardowski		
151370	STA007S112	InN[12[-]10] // Al2O3[101[-]0]. carrier n = 4.5 E+20/cm3.	InN	In1N1	In	1	N	1																					2006																															A	3.53		5.7											hexagonal	K	2	2.35	2.8				2.35																																																																																																Films grown by MBE, MOCVD method on sapphire (0001) substrates.					Electronic structure of superconducting InN			Department of Electronics, Tokai University, 1117 Kitakaname, Hiratsuka, Kanagawa 259-1292, Japan	Sci.Technol.Adv.Mater., 7(2006)S112	Takashi Inushima		
151371	STA007S112	previous data Fig.1 in this paper.	InN	In1N1	In	1	N	1																					2006																																													hexagonal	K		3					3	MTC151371																																																																																																				Electronic structure of superconducting InN			Department of Electronics, Tokai University, 1117 Kitakaname, Hiratsuka, Kanagawa 259-1292, Japan	Sci.Technol.Adv.Mater., 7(2006)S112	Takashi Inushima		
151372	STA009044204	3C-SiC:B, n = 1.91 E+21/cm3. type-I SC(GL=0.32).	B-doped SiC	Si1C1	Si	1	C	1																					2008																															A	4.3575														K			1.45				1.45										100										Oe	resistivity	132												MHC151372																																																												SiC,B		mixture(powders) - pellet - SIN(1600C,12h, in Ar/H2 gas)					Superconductivity in carrier-doped silicon carbide			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Sci.Technol.Adv.Mater., 9(2008)044204	Takahiro Muranaka,Yoshitake Kikuchi,Taku Yoshizawa,Naoki Shirakawa,Jun Akimitsu		
151373	STA009044204	6H-SiC:B,  n = 2.53 E+20/cm3. type-I SC(GL = 0.31).	B-doped SiC	Si1C1	Si	1	C	1																					2008																															A	3.064														K			1.45				1.45																				Oe	resistivity	125												MHC151373																																																												SiC,B		mixture(powders) - pellet - SIN(1600C,12h, in Ar/H2 gas)					Superconductivity in carrier-doped silicon carbide			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Sci.Technol.Adv.Mater., 9(2008)044204	Takahiro Muranaka,Yoshitake Kikuchi,Taku Yoshizawa,Naoki Shirakawa,Jun Akimitsu		
151374	STA009044204	three phases(3C-SiC(main phase), Si, Al). carrier n = 3.86-7.06)E+20/cm3 from Hall coeffic. type-II SC(GL = 1.8).  RRR = 5.3.	Al-doped SiC	Si1C1	Si	1	C	1																					2008																												ZnS			A	4.342													cubic Zn blende	K	1.35		1.5	1.4			1.4										100	Oe					53			0.45	Oe	resistivity, parabolic approx.	370												MHC151374		A		1480			A		2810																												mOhm.cm							0.746																							Superconductivity in carrier-doped silicon carbide			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan	Sci.Technol.Adv.Mater., 9(2008)044204	Takahiro Muranaka,Yoshitake Kikuchi,Taku Yoshizawa,Naoki Shirakawa,Jun Akimitsu		
151375	STA009044208	sample film (d=350nm) has x=0.01 in weight for In2O3-x(ZnO). as-grown sample(amorphous) annealed at 200C for 2h.	Zn-doped In2O3	In2O3	In	2																			O	3		4	2008																																														K		3.2					3.2	MTC151376																			T	resistivity, linear approx.	4.6							T/K		1.49			MHC151375		A		100																																																										dc-magnetron sputtering on glass substrates using the ceramic oxide In2O3-ZnO target under 0.3 Pa of Ar.					Superconductivity in transparent zinc-doped In2O3 films having low carrier density			High Voltage Electron Microscopy Station, National Institute for Material Science, 3?13 Sakura, Tsukuba, Ibaraki 305-3003, Japan	Sci.Technol.Adv.Mater., 9(2008)044208	Kazumasa Makise,Nobuhito Kokubo,Satoshi Takada,Takashi Yamaguti,Syunsuke Ogura,Kazumasa Yamada,Bunjyu Shinozaki,Koki Yano,Kazuyoshi Inoue,Hiroaki Nakamura		
151376	STA009044208	sample film (d=350nm) has x=0.02 in weight for In2O3-x(ZnO). as-grown sample(amorphous) annealed at 200C for 2h.	Zn-doped In2O3	In2O3	In	2																			O	3		4	2008																																														K		3.4					3.4	MTC151376																																																																																															dc-magnetron sputtering on glass substrates using the ceramic oxide In2O3-ZnO target under 0.3 Pa of Ar.					Superconductivity in transparent zinc-doped In2O3 films having low carrier density			High Voltage Electron Microscopy Station, National Institute for Material Science, 3?13 Sakura, Tsukuba, Ibaraki 305-3003, Japan	Sci.Technol.Adv.Mater., 9(2008)044208	Kazumasa Makise,Nobuhito Kokubo,Satoshi Takada,Takashi Yamaguti,Syunsuke Ogura,Kazumasa Yamada,Bunjyu Shinozaki,Koki Yano,Kazuyoshi Inoue,Hiroaki Nakamura		
151377	PRB079174501	lattice term in SP: (beta) = 0.473 mJ/mol.K4.  SP measured under pressure (upto 9 T).	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2009																												ThCr2Si2																		K		36.5				1	36.5																				T	resistivity, WHH		100						T/K	resistivity, 0.5Rn		4.1																								mJ/mol.K2	7.7																																							self-flux method using FeAs flux. melting(1273-1423 K)					Low temperature specific heat of the hole-doped Ba0.6K0.4Fe2As2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)174501	Gang Mu,Huiqian Luo,Zhaosheng Wang,Lei Shan,Cong Ren,Hai-Hu Wen		
151378	NJP011025014	Mossbauer effect also measured. tetra-ortho transition at T=125K. 10K-phase( Fmmm:a=5.6007,b=5.5620,c=13.0135).	(Ba,K)Fe2As2	Ba0.9K0.1Fe2As2	Ba	0.9	K	0.1	Fe	2	As	2																1	2009																												ThCr2Si2			A	3.9537		13.106												K			5				5																																																								mJ/mol.K2	47	SP-heat	418	SP-heat																																				mixture - (sealed in alumina crusible(Ar)) - heat(873 K, rate 50K/h) - keep(873K,15h) - cool to RT - ANN(923K,15h) - reground - pellet - SIN(1023K,15h)					Competition of magnetism and superconductivity in underdoped (Ba1-xKx)Fe2As2			Department Chemie und Biochemie der Ludwig-Maximilians-Universitat Munchen, Butenandtstr.-5-13 (Haus D), 81377 Munchen, Germany	New J.Phys., 11(2009)025014	Marianne Rotter,Marcus Tegel,Inga Schellenberg,Falko M Schappacher,Rainer Pottgen,Joachim Deisenhofer,Axel Gunther,Florian Schrettle,Alois Loidl,Dirk Johrendt		
151379	NJP011025014	Mossbauer effect also measured. tetra-ortho transition at T=105K. 10K-phase( Fmmm:a=5.5734,b=5.5464,c=13.0926).	(Ba,K)Fe2As2	Ba0.8K0.2Fe2As2	Ba	0.8	K	0.2	Fe	2	As	2																1	2009																												ThCr2Si2			A	3.9395		13.189												K				23.6			23.6																																																								mJ/mol.K2	5.6	SP-heat	238	SP-heat																																				mixture - (sealed in alumina crusible(Ar)) - heat(873 K, rate 50K/h) - keep(873K,15h) - cool to RT - ANN(923K,15h) - reground - pellet - SIN(1023K,15h)					Competition of magnetism and superconductivity in underdoped (Ba1-xKx)Fe2As2			Department Chemie und Biochemie der Ludwig-Maximilians-Universitat Munchen, Butenandtstr.-5-13 (Haus D), 81377 Munchen, Germany	New J.Phys., 11(2009)025014	Marianne Rotter,Marcus Tegel,Inga Schellenberg,Falko M Schappacher,Rainer Pottgen,Joachim Deisenhofer,Axel Gunther,Florian Schrettle,Alois Loidl,Dirk Johrendt		
151380	NJP011025014	impurity phase: FeAs(9%).	(Ba,K)Fe2As2	Ba0.7K0.3Fe2As2	Ba	0.7	K	0.3	Fe	2	As	2																	2009																												ThCr2Si2			A	3.9257		13.2702												K				37.5			37.5																																																																																																mixture - (sealed in alumina crusible(Ar)) - heat(873 K, rate 50K/h) - keep(873K,15h) - cool to RT - ANN(923K,15h) - reground - pellet - SIN(1023K,15h)					Competition of magnetism and superconductivity in underdoped (Ba1-xKx)Fe2As2			Department Chemie und Biochemie der Ludwig-Maximilians-Universitat Munchen, Butenandtstr.-5-13 (Haus D), 81377 Munchen, Germany	New J.Phys., 11(2009)025014	Marianne Rotter,Marcus Tegel,Inga Schellenberg,Falko M Schappacher,Rainer Pottgen,Joachim Deisenhofer,Axel Gunther,Florian Schrettle,Alois Loidl,Dirk Johrendt		
151381	NJP011025015	gap measured by point contact Andreev reflection method(PCAR). two gaps ((2d/kTc) = 2.1, 3.9 ) observed. summary of gap for this sample system shown in table.	Tb(O,F)FeAs	Tb1Fe1As1F0.1O0.9	Tb	1	Fe	1	As	1	F	0.1													O	0.9		1	2009																												oxypnictide																		K			50			3	50																																																3.9	1																																															high-P-synthesis					Investigation of superconducting gap structure in TbFeAsO0.9F0.1 using point contact Andreev reflection			The Blackett Laboratory, Physics Department, Imperial College London, London SW7 2AZ, UK	New J.Phys., 11(2009)025015	K A Yates,K Morrison,J A Rodgers,G B S Penny,J-W G Bos,J P Attfield,L F Cohen		
151382	NJP011025018	unannealed. RRR = 32. lattice term in SP: (beta) = 0.10 mJ/mol.K4.	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		3	2009																												oxypnictide																		K		6.6				1.3	6.6																																																								mJ/mol.K2	12.7	SP-heat	427	SP-heat											mOhm.cm							0.014																		single crystals grown from the melt using Sn:P flux.					Superconductivity in LnFePO (Ln=La, Pr and Nd) single crystals			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	New J.Phys., 11(2009)025018	R E Baumbach,J J Hamlin,L Shu,D A Zocco,N M Crisosto,M B Maple		
151383	NJP011025018	unannealed. RRR = 14. lattice term in SP: (beta) = 0.28 mJ/mol.K4.	PrFePO	Pr1Fe1P1O1	Pr	1	Fe	1	P	1															O	1		3	2009	cm3/mol	0					-46.7																					oxypnictide																		K		3.2				2	3.2																																																								mJ/mol.K2	10	SP-heat																				0.021																		single crystals grown from the melt using Sn:P flux.					Superconductivity in LnFePO (Ln=La, Pr and Nd) single crystals			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	New J.Phys., 11(2009)025018	R E Baumbach,J J Hamlin,L Shu,D A Zocco,N M Crisosto,M B Maple		
151384	NJP011025018	unannealed. RRR = 28	NdFePO	Nd1Fe1P1O1	Nd	1	Fe	1	P	1															O	1		3	2009	cm3/mol	0.039					-8.1																					oxypnictide																		K		3.1				3.1	3.1																																																																														0.0139																		single crystals grown from the melt using Sn:P flux.					Superconductivity in LnFePO (Ln=La, Pr and Nd) single crystals			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	New J.Phys., 11(2009)025018	R E Baumbach,J J Hamlin,L Shu,D A Zocco,N M Crisosto,M B Maple		
151385	NJP011025018	annealed. lattice term in SP: (beta) = 0.22 mJ/mol.K4.	PrFePO	Pr1Fe1P1O1	Pr	1	Fe	1	P	1															O	1		3	2009																												oxypnictide																		K		3.6					3.6																																																						mJ/mol.K	15.1	mJ/mol.K2	3	SP-heat																																						single crystals grown from the melt using Sn:P flux.					Superconductivity in LnFePO (Ln=La, Pr and Nd) single crystals			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	New J.Phys., 11(2009)025018	R E Baumbach,J J Hamlin,L Shu,D A Zocco,N M Crisosto,M B Maple		
151386	NJP011025023	not SC. T<SDW> = 165 K	Sr(Fe,Mn)2As2	Sr1Fe1.9Mn0.1As2	Sr	1	Fe	1.9	Mn	0.1	As	2																1	2009																												ThCr2Si2			A	3.9319		12.4161												K					4																																																																																																		solid state reaction					AFe2As2 (A= Ca, Sr, Ba, Eu) and SrFe2-xTMxAs2 (TM = Mn, Co, Ni): crystal structure, charge doping, magnetism and superconductivity			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	New J.Phys., 11(2009)025023	Deepa Kasinathan,Alim Ormeci,Katrin Koch,Ulrich Burkhardt,Walter Schnelle,Andreas Leithe-Jasper,Helge Rosner		
151387	NJP011025023	not SC. T<SDW> = 130 K	Sr(Fe,Mn)2As2	Sr1Fe1.8Mn0.2As2	Sr	1	Fe	1.8	Mn	0.2	As	2																1	2009																												ThCr2Si2			A	3.9384		12.4615												K					4																																																																																																		solid state reaction					AFe2As2 (A= Ca, Sr, Ba, Eu) and SrFe2-xTMxAs2 (TM = Mn, Co, Ni): crystal structure, charge doping, magnetism and superconductivity			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	New J.Phys., 11(2009)025023	Deepa Kasinathan,Alim Ormeci,Katrin Koch,Ulrich Burkhardt,Walter Schnelle,Andreas Leithe-Jasper,Helge Rosner		
151388	NJP011025023	not SC. T<SDW> = 130 K.	Sr(Fe,Mn)2As2	Sr1Fe1.7Mn0.3As2	Sr	1	Fe	1.7	Mn	0.3	As	2																1	2009																												ThCr2Si2			A	3.9441		12.4832												K					4																																																																																																		solid state reaction					AFe2As2 (A= Ca, Sr, Ba, Eu) and SrFe2-xTMxAs2 (TM = Mn, Co, Ni): crystal structure, charge doping, magnetism and superconductivity			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	New J.Phys., 11(2009)025023	Deepa Kasinathan,Alim Ormeci,Katrin Koch,Ulrich Burkhardt,Walter Schnelle,Andreas Leithe-Jasper,Helge Rosner		
151390	CC20092189	no impurity phases (XRD analysis). Na0.98FeAs0.98 (NPD). [vols] = 10 % at 2K.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm		A	3.9494		7.0396												K				9			9										10																																																																																						(Fe-,As-powders) - ground) - ADD(Na-pieces) - (sealed in Ta tube) - heat(800C,2d)					Structure, antiferromagnetism and superconductivity of the layered iron arsenide NaFeAs			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, UK	Chem.Commun., (2009) 2189	Dinah R. Parker,Michael J. Pitcher,Peter J. Baker,Isabel Franke,Tom Lancaster,Stephen J. Blundell,Simon J. Clarke		
151391	PRB079184516	SC volume fraction is very small.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm		A	3.9866		7.094												K				6			6																																																																																																FeAs firstly made(600-800C), then ADD(Na-ingot) - (sealed in Nb tube) heat(750C,3d) - cool to 300C - ANN(300-400C)					Unusual doping dependence of superconductivity in NayFeAs			Department of Physics and TCSUH, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 79(2009)184516	K. Sasmal,B. Lv,Z. J. Tang,F. Chen,Y. Y. Xue,B. Lorenz,A. M. Guloy,C. W. Chu		
151392	PRB079184516	[vols] = 75% at 2 K. R(H,T) and Hall effect measured.	NaFeAs	Na0.9Fe1As1	Na	0.9	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm																	K				7			7										75																																																																																						FeAs firstly made(600-800C), then ADD(Na-ingot) - (sealed in Nb tube) heat(750C,3d) - cool to 300C - ANN(300-400C)					Unusual doping dependence of superconductivity in NayFeAs			Department of Physics and TCSUH, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 79(2009)184516	K. Sasmal,B. Lv,Z. J. Tang,F. Chen,Y. Y. Xue,B. Lorenz,A. M. Guloy,C. W. Chu		
151393	PRB079184516	SC volume fraction is very small.	NaFeAs	Na0.5Fe1As1	Na	0.5	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm																	K				12			12																																																																																																FeAs firstly made(600-800C), then ADD(Na-ingot) - (sealed in Nb tube) heat(750C,3d) - cool to 300C - ANN(300-400C)					Unusual doping dependence of superconductivity in NayFeAs			Department of Physics and TCSUH, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 79(2009)184516	K. Sasmal,B. Lv,Z. J. Tang,F. Chen,Y. Y. Xue,B. Lorenz,A. M. Guloy,C. W. Chu		
151394	PRB079180502	RRR=16.5. (dC/gamma*Tc) = 1.41. BaIr2P2(85%), Ba3(PO4)2 (10%), a few % of Ir2P, IrP2	BaIr2P2	Ba1Ir2P2	Ba	1	Ir	2	P	2																		1	2009																										AB2C2		ThCr2Si2			A	3.9469		12.559												K		2.1					2.1										100										Oe	resistivity	410							Oe/K		279					A	from Hc2	800																		mJ/mol.K2	9.3	SP-heat																																						single crystals grown by metal flux method. Ba:Ir:P:Pb:Cu = 1.3:2:2:40:5 used					Superconductivity without Fe or Ni in the phosphides BaIr2P2 and BaRh2P2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697-4575, USA	Phys.Rev.B, 79(2009)180502	N. Berry,C. Capan,G. Seyfarth,A. D. Bianchi,J. Ziller,Z. Fisk		
151395	PRB079180502	RRR=7.5. (dC/gamma*Tc) = 1.17.	BaRh2P2	Ba1Rh2P2	Ba	1	Rh	2	P	2																		3	2009																										AB2C2		ThCr2Si2			A	3.9308		12.574												K		1					1																				Oe	resistivity	370							Oe/K		528					A	from Hc2	950																		mJ/mol.K2	9.2	SP-heat																																						single crystals grown by metal flux method. Ba:Ir:P:Pb:Cu = 1.3:2:2:40:5 used					Superconductivity without Fe or Ni in the phosphides BaIr2P2 and BaRh2P2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697-4575, USA	Phys.Rev.B, 79(2009)180502	N. Berry,C. Capan,G. Seyfarth,A. D. Bianchi,J. Ziller,Z. Fisk		
151396	PRB079180502		CaRh2P2	Ca1Rh2P2	Ca	1	Rh	2	P	2																		3	2009																										AB2C2		ThCr2Si2			A	4.0179		9.655												K					0.5																																																										mJ/mol.K2	10.7	SP-heat																																						single crystals grown by metal flux method. Ba:Ir:P:Pb:Cu = 1.3:2:2:40:5 used					Superconductivity without Fe or Ni in the phosphides BaIr2P2 and BaRh2P2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697-4575, USA	Phys.Rev.B, 79(2009)180502	N. Berry,C. Capan,G. Seyfarth,A. D. Bianchi,J. Ziller,Z. Fisk		
151397	PRB078104512	RRR = 5.3. lattice term in SP: (beta) = 1.93 mJ/mol.K4. no indication of SC, SDW, and structural transition.	BaRh2As2	Ba1Rh2As2	Ba	1	Rh	2	As	2																		3	2008																										AB2C2		ThCr2Si2	I4/mmm		A	4.0564		12.797												K					2																																																										mJ/mol.K2	4.7	SP-heat	171	SP-heat											mOhm.cm							0.029							cm3/C	0.00035				8		cm(-3)	18000000000000000000000			Pb-flux method					Single-crystal growth and physical properties of the layered arsenide BaRh2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 78(2008)104512	Yogesh Singh,Y. Lee,S. Nandi,A. Kreyssig,A. Ellern,S. Das,R. Nath,B. N. Harmon,A. I. Goldman,D. C. Johnston		
151398	PRB079184508		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2009																												T																		K			45.3				45.3																				T	resistivity, WHH			67.4										HC151398		A	from Hc2		22.1																																																									TSFZ method					Zn-doping effects on the electrical resistivity of La1.85Sr0.15CuO4 under a magnetic field			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.B, 79(2009)184508	M. Kofu,H. Kimura,H. Ishida,T. Matsumura,K. Hirota		
151399	PRB079184508		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.996Zn0.004O4	La	1.85	Sr	0.15	Cu	0.996	Zn	0.004													O	4		3	2009																												T																		K			39				39																				T	resistivity, WHH			53.1										HC151398		A	from Hc2		24.9																																																									TSFZ method					Zn-doping effects on the electrical resistivity of La1.85Sr0.15CuO4 under a magnetic field			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.B, 79(2009)184508	M. Kofu,H. Kimura,H. Ishida,T. Matsumura,K. Hirota		
151400	PRB079184508		(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.992Zn0.008O4	La	1.85	Sr	0.15	Cu	0.992	Zn	0.008													O	4		3	2009																												T																		K			35.7				35.7																				T	resistivity, WHH			38.1										HC151398		A	from Hc2		29.4																																																									TSFZ method					Zn-doping effects on the electrical resistivity of La1.85Sr0.15CuO4 under a magnetic field			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.B, 79(2009)184508	M. Kofu,H. Kimura,H. Ishida,T. Matsumura,K. Hirota		
151401	PRB079184508	Zn-content by ICP. Hc2 defined as 0.95Rn from H//c, J//ab measurements. Hc2(0) estimated by us.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.983Zn0.017O4	La	1.85	Sr	0.15	Cu	0.983	Zn	0.017													O	4		3	2009																												T																		K			22.8				22.8																				T	resistivity, WHH			13.8										HC151398		A	from Hc2		48.8																																																									TSFZ method					Zn-doping effects on the electrical resistivity of La1.85Sr0.15CuO4 under a magnetic field			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.B, 79(2009)184508	M. Kofu,H. Kimura,H. Ishida,T. Matsumura,K. Hirota		
151402	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 79	NiZr2	Ni1Zr2	Ni	1	Zr	2																					2009																										AB2		AMOR																		K		2.44					2.44																				T					4.7			0.33	T/K	resistive, 0.5Rn	3					A	from Hc2	81																																	uOhm.m							1.68																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151403	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 68	(Fe,Ni)Zr2	Fe0.1Ni0.9Zr2	Fe	0.1	Ni	0.9	Zr	2																			2009																										AB2		AMOR																		K		2.65					2.65																				T					5.3			0.33	T/K	resistive, 0.5Rn	2.2					A	from Hc2	80																																	uOhm.m							1.68																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151404	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 75	(Fe,Ni)Zr2	Fe0.15Ni0.85Zr2	Fe	0.15	Ni	0.85	Zr	2																			2009																										AB2		AMOR																		K		2.31					2.31																				T					4.5			0.33	T/K	resistive, 0.5Rn	2.8					A	from Hc2	83																																	uOhm.m							1.62																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151405	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 71	(Fe,Ni)Zr2	Fe0.2Ni0.8Zr2	Fe	0.2	Ni	0.8	Zr	2																			2009																										AB2		AMOR																		K		2.13					2.13	MTC151405																			T					4.29			0.33	T/K	resistive, 0.5Rn	2.4			MHC151405		A	from Hc2	82																																	uOhm.m							1.69																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151406	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 78	(Fe,Ni)Zr2	Fe0.3Ni0.7Zr2	Fe	0.3	Ni	0.7	Zr	2																			2009																										AB2		AMOR																		K		2.02					2.02																				T					4.03			0.33	T/K	resistive, 0.5Rn	2.8					A	from Hc2	88																																	uOhm.m							1.75																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151407	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 86	(Fe,Ni)Zr2	Fe0.33Ni0.67Zr2	Fe	0.33	Ni	0.67	Zr	2																			2009																										AB2		AMOR																		K		2.13					2.13																				T					3.81			0.33	T/K	resistive, 0.5Rn	3.2					A	from Hc2	87																																	uOhm.m							1.84																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151408	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 83	(Fe,Ni)Zr2	Fe0.36Ni0.64Zr2	Fe	0.36	Ni	0.64	Zr	2																			2009																										AB2		AMOR																		K		2.04					2.04																													T/K	resistive, 0.5Rn	3.2																																								uOhm.m							1.72																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151409	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 74	(Fe,Ni)Zr2	Fe0.4Ni0.6Zr2	Fe	0.4	Ni	0.6	Zr	2																			2009																										AB2		AMOR																		K		1.78					1.78																				T					3.35			0.33	T/K	resistive, 0.5Rn	2.6					A	from Hc2	96																																	uOhm.m							1.7																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151410	PRB079184525	Tc, Hc2 defined as 0.5 Rn. G-L parameter = 70	(Fe,Ni)Zr2	Fe0.5Ni0.5Zr2	Fe	0.5	Ni	0.5	Zr	2																			2009																										AB2		AMOR																		K		1.25					1.25																				T					1.69			0.33	T/K	resistive, 0.5Rn	2.3					A	from Hc2	123																																	uOhm.m							1.69																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151411	PRB079184525	Tc, Hc2 defined as 0.5 Rn.	(Fe,Ni)Zr2	Fe0.6Ni0.4Zr2	Fe	0.6	Ni	0.4	Zr	2																			2009																										AB2		AMOR																		K		0.2					0.2																				T					1.05			0.33	T/K	resistive, 0.5Rn						A	from Hc2	162																																	uOhm.m							1.67																		arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Superconductivity and short-range order in metallic glasses FexNi1-xZr2			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184525	J. Lefebvre,M. Hilke,Z. Altounian		
151412	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	NiZr2	Ni1Zr2	Ni	1	Zr	2																					2009																										AB2		AMOR																		K		2.44					2.44											Oe		4.7																					MHC151412																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151413	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	(Fe,Ni)Zr2	Fe0.1Ni0.9Zr2	Fe	0.1	Ni	0.9	Zr	2																			2009																										AB2		AMOR																		K		2.65					2.65											Oe		5.9																					MHC151413																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151414	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	(Fe,Ni)Zr2	Fe0.2Ni0.8Zr2	Fe	0.2	Ni	0.8	Zr	2																			2009																										AB2		AMOR																		K		2.13					2.13											Oe		5.9																					MHC151412																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151415	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	(Fe,Ni)Zr2	Fe0.3Ni0.7Zr2	Fe	0.3	Ni	0.7	Zr	2																			2009																										AB2		AMOR																		K		2.02					2.02											Oe		6																					MHC151415																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151416	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	(Fe,Ni)Zr2	Fe0.4Ni0.6Zr2	Fe	0.4	Ni	0.6	Zr	2																			2009																										AB2		AMOR																		K		1.78					1.78											Oe		6.9																					MHC151413																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151417	PRB079184524	local magnetization measured by Hall sensors. Tc from PRB079184525	(Fe,Ni)Zr2	Fe0.5Ni0.5Zr2	Fe	0.5	Ni	0.5	Zr	2																			2009																										AB2		AMOR																		K		1.25					1.25											Oe		3.4																					MHC151415																																																														arc-melting. melt-spinning the bottans(40 kPa-He, Cu-wheel  50 m/s, cooling rate = E;5-E;6 K/s)					Local magnetization fluctuations in superconducting glasses resolved by Hall sensors			Department of Physics, McGill University, Montreal, Canada H3A 2T8	Phys.Rev.B, 79(2009)184524	J. Lefebvre,M. Hilke,Z. Altounian,K. W. West,L. N. Pfeiffer		
151418	PRB079214505	Co-content confirmed by EMS. thermal expansin(TE) measured by capacitance dilatometer. (dTc/dP) calculated from SP and TE using Ehrenfest relation.	Ba(Fe,Co)2As2	Ba1Fe1.84Co0.16As2	Ba	1	Fe	1.84	Co	0.16	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9534		12.942												K		21.5					21.5			K/GPa	-1.7																																																		J/mol.K	0.471																																									FeAs-flux method					High-resolution measurements of the thermal expansion of superconducting Co-doped BaFe2As2			Department of Physics, Montana State University, Bozeman, P.O. Box 173840, Montana 59717-3840, USA	Phys.Rev.B, 79(2009)214505	M. S. da Luz,J. J. Neumeier,R. K. Bollinger,A. S. Sefat,M. A. McGuire,R. Jin,B. C. Sales,D. Mandrus		
151419	PRB079214505	Co-content confirmed by EMS. thermal expansin(TE) measured by capacitance dilatometer. (dTc/dP) calculated from SP and TE using Ehrenfest relation.	Ba(Fe,Co)2As2	Ba1Fe1.77Co0.23As2	Ba	1	Fe	1.77	Co	0.23	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9519		12.937												K		16.5					16.5			K/GPa	-13																																																		J/mol.K	0.281																																									FeAs-flux method					High-resolution measurements of the thermal expansion of superconducting Co-doped BaFe2As2			Department of Physics, Montana State University, Bozeman, P.O. Box 173840, Montana 59717-3840, USA	Phys.Rev.B, 79(2009)214505	M. S. da Luz,J. J. Neumeier,R. K. Bollinger,A. S. Sefat,M. A. McGuire,R. Jin,B. C. Sales,D. Mandrus		
151420	PRL102187004	RRR=4. uniaxial P-dependence of Tc measured by thermal expansion and SP. (dTc/dP)a = 3.1 K/GPa. (dTc/dP)c = -7.0 K/GPa. (dC/Tc) = 28 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.84Co0.16As2	Ba	1	Fe	1.84	Co	0.16	As	2																3	2009																										AB2C2		ThCr2Si2																		K		21.8		19.8			21.8			K/GPa	-0.9																																																		J/mol.K	0.554																																							FeAs,CoAs,Ba		mixture(Ba:Fe:Co:As=1:2.67:0.33:3) - (placed in Al2O3) - (sealed in evacuated SiO2) - heat(650C, then 1170C) - hold(5h) - cool (1.5C/h)					Large Anisotropic Uniaxial Pressure Dependencies of Tc in Single Crystalline Ba(Fe0.92Co0.08)2As2			Forschungszentrum Karlsruhe, Institut fur Festkorperphysik, PO Box 3640, 76021 Karlsruhe, Germany	Phys.Rev.Lett., 102(2009)187004	Frederic Hardy,Peter Adelmann,Thomas Wolf,Hilbert v. Lohneysen,Christoph Meingast		
151421	PRL102187005	K-content not given. two gaps ( higher 9.1 meV(DB), lower 1.5 meV) .  anisotropy(penet) increases from 1.1(Tc) to 1.9(low-T).	(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		32					32																																									A	muon-SR		3200		meV	9.1																																																						Two-Gap Superconductivity in Ba1-xKxFe2As2: A Complementary Study of the Magnetic Penetration Depth by Muon-Spin Rotation and Angle-Resolved Photoemission			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 102(2009)187005	R. Khasanov,D.V. Evtushinsky,A. Amato,H.-H. Klauss,H.-H. Klauss,Ch. Niedermayer,Ch. Niedermayer,B. Buchner,G. L. Sun,G. L. Sun,C. T. Lin,J. T. Park,D. S. Inosov,V. Hinkov		
151422	PRB078220505	K-content measured by X-ray spectroscopy. Hc2(T) and [penet] measured by rf field sensor using 60T pulsed field. anisotropy(Hc2) decreases from 3.5(at Tc) to 1.16 (14 K).	(Ba,K)Fe2As2	Ba0.55K0.45Fe2As2	Ba	0.55	K	0.45	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2																		K		32					32																																		MHC151422		A			34	29																																																													Determination of anisotropic Hc2 up to 60 T in Ba0.55K0.45Fe2As2 single crystals			MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 78(2008)220505	M. M. Altarawneh,K. Collar,C. H. Mielke,N. Ni,S. L. Bud'ko,P. C. Canfield		
151423	NAT4570565	K-content (nominal). anisotropy(Hc2) decreases from 2.0(Tc) to 1(10K). nHc2(0) by extraporation.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		28.2					28.2																				T	resistive, 0.5Rn			70					T/K	resistive, 0.5Rn		5.4	2.9	MHC151423																																																									MRH151423										Nearly isotropic superconductivity in (Ba,K)Fe2As2			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China.	Nature 457(2009)565	H. Q. Yuan,J. Singleton,F. F. Balakirev,S. A. Baily,G. F. Chen,J. L. Luo,N. L. Wang		
151424	PRL102187005	K-content not given. two gaps ( higher 9.1 meV(DB), lower  <4 meV) .	(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		32					32																																									A	ARPES		2700		meV	9.1																																																						Two-Gap Superconductivity in Ba1-xKxFe2As2: A Complementary Study of the Magnetic Penetration Depth by Muon-Spin Rotation and Angle-Resolved Photoemission			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 102(2009)187005	R. Khasanov,D.V. Evtushinsky,A. Amato,H.-H. Klauss,H.-H. Klauss,Ch. Niedermayer,Ch. Niedermayer,B. Buchner,G. L. Sun,G. L. Sun,C. T. Lin,J. T. Park,D. S. Inosov,V. Hinkov		
151425	PRL102227004	Na-deficiency < 1%. structural(52K), magnetic(41K) transition observed in R and SUS measurements.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2009																										ABC		PbFCl			A			7.028												K	8	15					15																				T	resistive, 0.5Rn, WHH		41.2	22.7					T/K	resistive, 0.5Rn		3.98	2.19	MHC151425																						mJ/mol.K2	5																																		MRH151425					single crystal grown by self-flux method. starting(Li1.5FeAs. mixture(Na,FeAs) - (sealed in Ta crucible) - (evacuated quartz ampoule) - heat(1100C) - cool(5C/h)					Multiple Phase Transitions in Single-Crystalline Na1-zFeAs			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.Lett., 102(2009)227004	G. F. Chen,W. Z. Hu,J. L. Luo,N. L. Wang		
151427	PRL102217003	Ga-ion inplantation. maximum Ga concentration = 8 at% (60 nm depth). flash annealing at 50.8 J/cm2. Hc2 measured for H// and H/n to sample plane.	Ga-doped Ge	Ge0.92Ga0.08	Ge	0.92	Ga	0.08																					2009																										AB																				K		0.45					0.45																				T	resistive, 0.5Rn, extraporation		1.1	0.3										MHC151427																																																																			Superconducting State in a Gallium-Doped Germanium Layer at Low Temperatures			Dresden High Magnetic Field Laboratory (HLD) and Institute of Ion Beam Physics and Materials Research, Forschungszentrum Dresden-Rossendorf (FZD), Dresden, Germany	Phys.Rev.Lett., 102(2009)217003	T. Herrmannsdorfer,V. Heera,O. Ignatchik,M. Uhlarz,A. Mucklich,M. Posselt,H. Reuther,B. Schmidt,K.-H. Heinig,W. Skorupa,M. Voelskow,C. Wundisch,R. Skrotzki,M. Helm,J. Wosnitza		
151428	PRL102197001	(dTc/dP) calculated from uniaxial values (dTc/dP)//c = -0.66 K/GPa and (dTc/dP)//a = 0.56 K/GPa. Tc defined as maximum of C/T. (dC/gamma*Tc) = 0.73	CeInIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2009																										ABC5		HoCoGa5																		K		0.4					0.4	MTC151428		K/GPa	0.46																																																																																												crystals grown in alumina crucible from the melt with excess In.					Anisotropic Dependence of Superconductivity on Uniaxial Pressure in CeIrIn5			Department of Physics, University of California Davis, Davis, California 95616, USA	Phys.Rev.Lett., 102(2009)197001	O. M. Dix,A. G. Swartz,R. J. Zieve,J. Cooley,T. R. Sayles,M. B. Maple		
151429	PRL102197002	P induced SC. Eu: 99.98 % from Ames Lab. pressure by DAC. P<crit> = 80 GPa, Tc=1.78 K. Tc<max> = 2.75 K at P=142 GPa.	Eu	Eu1	Eu	1																							2009																																														K				2.75	0		2.75	MTC151429		K/GPa	0.018																																																																																																	Pressure-Induced Superconducting State of Europium Metal at Low Temperatures			Department of Physics, Washington University, CB 1105, One Brookings Drive, Saint Louis, Missouri 63130, USA	Phys.Rev.Lett., 102(2009)197002	M. Debessai,T. Matsuoka,J. J. Hamlin,J. S. Schilling,K. Shimizu		
151430	PRL102206602	negative MR, field induced I-S transition, etc shows quasi-one-dimensional SC: Tc(onset) > 10 K.	Li0.9Mo6O17	Li0.9Mo6O17	Li	0.9	Mo	6																	O	17		3	2009																										AB6C17		bronze																		K			10				10																																																																																																Temperature gradient flux method					Directional Field-Induced Metallization of Quasi-One-Dimensional Li0.9Mo6O17			H. H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, BS8 1TL, United Kingdom	Phys.Rev.Lett., 102(2009)206602	Xiaofeng Xu,A. F. Bangura,J. G. Analytis,J. D. Fletcher,M. M. J. French,N. Shannon,J. He,S. Zhang,D. Mandrus,R. Jin,N. E. Hussey		
151431	NAP0040603	RRR = 300 for R//ab.  For RRR=70 sample, not SC (Tcn=0.03). [npenet] is preliminary data. structure data from Chem.Mater., 19(2007)1918.	beta-YbAlB4	Yb1Al1B4	Yb	1	Al	1	B	4																		3	2008					myu-B/Yb	3.1	-210																			ABC4	3	ThMoB4	Cmmm	65	A	7.308	9.315	3.498												K				0.08			0.08										15																															um				6																										uOhmcm							0.4																		Al-flux method					Superconductivity and quantum criticality in the heavy-fermion system beta-YbAlB4			Institute for Solid State Physics (ISSP), University of Tokyo, Kashiwa 277-8581, Japan	Nature Phys.. 4(2008)603	S. NAKATSUJI,K. KUGA,Y. MACHIDA,T. TAYAMA,T. SAKAKIBARA,Y. KARAKI,H. ISHIMOTO,S. YONEZAWA,Y. MAENO,E. PEARSON,G. G. LONZARICH,L. BALICAS,H. LEE,Z. FISK		
151432	JPS078083702	PM(tetra) to AFM(ortho) transition at 200K. uniaxial(c-axis)-P-dependence of Tc for various pressure mediums were measured. Table values show for Daphne7474.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2009								200																		AB2C2		ThCr2Si2																		K	30.1				0		30.1	MTC151432																																																																																																				Effect of Uniaxial Stress for Pressure-Induced Superconductor SrFe2As2			Department of Physics, Kobe University, Kobe 657-8501	J.Phys.Soc.Jpn, 78(2009)083702	Hisashi KOTEGAWA,Takayuki KAWAZOE,Hitoshi SUGAWARA,Keizo MURATA,Hideki TOU		
151433	JPS077064716	P-induced SC. SC properties for P=6.5 GPa. For P=5.4 GPa, Tc=0.13K and Hc2(0)//[001] = 1.5 kOe. Hc2-Fig for H//[001].	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		3	2008								21																		ABC3		BaNiSn3																		K	0.69				0		0.69	MTC151433																												T/K	resistivity		20		MHC151433																																																														Bi-flux method					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
151434	11		BaBi3	Ba1Bi3	Ba	1	Bi	3																					1952																										AB3																				K		5.69					5.69																																																																																																					A search for new superconducting compounds				Phys.Rev., 87(1952)799	B.T.Matthias,J.K.Hulm		
151435	JPS078083701	P-induced SC. SC properties show for P=28 kbar. (dHc2/dT) estimated from the data for H =< 0.5 T.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K		29	30		0		29										100																			T/K	resistivity		0.19	0.5	MHC151435																																																														Bridgman method					EuFe2As2 under High Pressure: An Antiferromagnetic Bulk Superconductor			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003	J.Phys.Soc.Jpn, 78(2009)083702	Taichi TERASHIMA,Motoi KIMATA,Hidetaka SATSUKAWA,Atsushi HARADA,Kaori HAZAMA,Shinya UJI,Hiroyuki S. SUZUKI,Takehiko MATSUMOTO,Keizo MURATA		
151436	JPS078063703	RRR=50. pressure medium = Daphne7373. Field(H//baxis) reentrant SC measured for various P (0 < P < 0.84 GPa). Tc(max) = 0.4 K for reentrant SC. (dTm/dP) = 0.95 K/GPa  and (dTc/dP) estimated from Fig.	URhGe	U1Rh1Ge1	U	1	Rh	1	Ge	1																		3	2009																										ABC		TiNiSi																		K		0.26					0.26	MTC151436		K/GPa	-0.036																																																																																												Czochralski method					Pressure Evolution of the Ferromagnetic and Field Re-entrant Superconductivity in URhGe			INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 78(2009)063703	Atsushi MIYAKE,Dai AOKI,Jacques FLOUQUET		
151437	JPS078063704	(dTc/dT) estimated from Fig for P < 0.5 GPa.	FeSe0.92	Fe1Se0.92	Fe	1	Se	0.92																				1	2009																										AB																				K		7.2					7.2	MTC151437		K/GPa	6.7																																																																																												Solid state reaction					Precise Pressure Dependence of the Superconducting Transition Temperature of FeSe: Resistivity and <77>Se-NMR Study			Department of Physics, Kobe University, Kobe 658-8530	J.Phys.Soc.Jpn, 78(2009)063704	Satoru MASAKI,Hisashi KOTEGAWA,Yudai HARA,Hideki TOU,Keizo MURATA,Yoshikazu MIZUGUCHI,Yoshihiko TAKANO		
151438	JPS078064702	Hc(0) = 1.5 mT. kappa(GL) = 14. (dHc/dT) = -24.7 mT/K. (dC/gamma*Tc) = 1.15.  data from PCS0631021.	alpha-Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7			2009																										A2B2C7		pyrochlore																		K		0.97					0.97											mT		2.1							T	SP-heat	0.29							T/K	SP-heat	0.42					A		340			A		4600																458	SP-heat																																									Rattling-Induced Superconductiviy in thebeta-Pyrochlore Oxides AOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)064702	Yohei NAGAO,Jun-ichi YAMAURA,Hiroki OGUSU,Yoshihiko OKAMOTO,Zenji HIROI		
151439	JPS078064702	RRR=550. Hc(0) = 59.0 mT. kappa(GL) = 14. (dHc/dT) = -30.3 mT/K. (dC/gamma*Tc) = 1.49. [gapene] using single gap model.	beta-CsOs2O6	Cs1Os2O6	Cs	1	Os	2																	O	6		3	2009																										AB2C6		pyrochlore																		K		3.25					3.25											mT		8.2							T	SP-heat	1.15							T/K	SP-heat	0.44			HC151439		A		170			A		2300					3.66	14							mJ/mol.K2	41.3	SP-heat													uOhmcm							0.75				410																			Rattling-Induced Superconductiviy in thebeta-Pyrochlore Oxides AOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)064702	Yohei NAGAO,Jun-ichi YAMAURA,Hiroki OGUSU,Yoshihiko OKAMOTO,Zenji HIROI		
151440	JPS078064702	RRR = 1250. Hc(0) = 125.9 mT. kappa(GL) = 27. (dHc/dT) = -36.5 mT/K. (dC/gamma*Tc) = 1.83. [gapene] using single gap model.	beta-RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6		3	2009																										AB2C6		pyrochlore																		K		6.28					6.28											mT		11.1							T	SP-heat	4.81							T/K	SP-heat	0.88			HC151440		A		83			A		2200					4	14							mJ/mol.K2	44.7	SP-heat													uOhmcm							1.1				1370																			Rattling-Induced Superconductiviy in thebeta-Pyrochlore Oxides AOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)064702	Yohei NAGAO,Jun-ichi YAMAURA,Hiroki OGUSU,Yoshihiko OKAMOTO,Zenji HIROI		
151441	JPS078064702	Hc(0) = 124.9 mT. kappa(GL) = 34. (dHc/dT) = -37.0 mT/K. (dC/gamma*Tc) = 1.9.  data from PRB071214517	beta-RbOs2O6	Rb1Os2O6	Rb	1	Os	2																	O	6			2009																										AB2C6		pyrochlore																		K		6.4					6.4											mT		9.2							T	SP-heat	6							T/K	SP-heat	1.2					A		74			A		2520																																																										Rattling-Induced Superconductiviy in thebeta-Pyrochlore Oxides AOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)064702	Yohei NAGAO,Jun-ichi YAMAURA,Hiroki OGUSU,Yoshihiko OKAMOTO,Zenji HIROI		
151442	JPS078064702	Hc(0) = 255 mT. kappa(GL) = 82. (dHc/dT) = -56.1 mT/K. (dC/gamma*Tc) = 2.87.  data from PRB07076014523	beta-KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2009																										AB2C6		pyrochlore																		K		9.6					9.6											mT		10.1							T	SP-heat	30.6							T/K	SP-heat	3.61					A		33			A		2700					5	14																																																				Rattling-Induced Superconductiviy in thebeta-Pyrochlore Oxides AOs2O6			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)064702	Yohei NAGAO,Jun-ichi YAMAURA,Hiroki OGUSU,Yoshihiko OKAMOTO,Zenji HIROI		
151443	PRB079233409	S-doped amorphous-C. mass ratio (m<C>/m<S>) = 3 for a-C + S) sample. resistivity not measured. Hc2=Hc2(0)(1-t^2)^n, Hc2(0)=650 kOe, n=2.4. S-content not given.	S-doped a-C	C0.9S0.1	C	0.9	S	0.1																					2009																										AB																				K				38			38											Oe	M-H curve	550																					MHC151443																																																														mixture(amorphous C + S(4N) powder) - press - sealed in evacuated quartz tube - heat(250C,24h) cool to RT					Magnetization measurement of a possible high-temperature superconducting state in amorphous carbon doped with sulfur			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B, 79(2009)233409	Israel Felner,Yakov Kopelevich		
151444	PRB079233409	a-C (amorphous-C). mass ratio (m<C>/m<S>) = 174 for a-C (amorphous-C).	a-C	C1	C	1																							2009																										A																				K				32			32																																																																																																mixture(amorphous C + S(4N) powder) - press - sealed in evacuated quartz tube - heat(250C,24h) cool to RT					Magnetization measurement of a possible high-temperature superconducting state in amorphous carbon doped with sulfur			Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel	Phys.Rev.B, 79(2009)233409	Israel Felner,Yakov Kopelevich		
151445	PMB0821335	composites of C & S. S-content not clear. resistivity not measured. remanent for H//a goes to zero at 570 K by extraporation. weak itinerant FM.	C1-xSx	C1S1	C	1	S	1																					2002																										AB					A			6.72												K				9			9											Oe	M-H curve	64																					MHC151445							A				2270																																																	graphite rod,S-chunk		mixture(C-powder + S-chunk) - press to pellet - sealed in evacuated quartz tube(0.5 atm-Ar) - heat(400C,1h) - cool to RT(4C/h)					Coexistence of superconductivity and ferromagnetism in the graphite-sulphur system			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093-0360, USA	Phylos.Mag. B, 82(2002)1335	S. MOEHLECKE,PEI-CHUN HO,M. B. MAPLES		
151446	PRB080014506		LixFeAs	Li0.8Fe1As1	Li	0.8	Fe	1	As	1																			2009																										ABC		PbFCl																		K		17.6					17.6	MTC151446		K/GPa	-1.48																																																																																																	Effect of pressure on the iron arsenide superconductor LixFeAs (x=0.8, 1.0, 1.1)			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 80(2009)014506	S. J. Zhang,X. C. Wang,R. Sammynaiken,J. S. Tse,L. X. Yang,Z. Li,,Q. Q. Liu,S. Desgreniers,Y. Yao,H. Z. Liu,C. Q. Jin		
151447	PRB080014506		LixFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2009																										ABC		PbFCl																		K		18.3					18.3	MTC151446		K/GPa	-1.38																																																																																																	Effect of pressure on the iron arsenide superconductor LixFeAs (x=0.8, 1.0, 1.1)			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 80(2009)014506	S. J. Zhang,X. C. Wang,R. Sammynaiken,J. S. Tse,L. X. Yang,Z. Li,,Q. Q. Liu,S. Desgreniers,Y. Yao,H. Z. Liu,C. Q. Jin		
151448	PRB080014506		LixFeAs	Li1.1Fe1As1	Li	1.1	Fe	1	As	1																			2009																										ABC		PbFCl																		K		20					20	MTC151446		K/GPa	-1.22																																																																																																	Effect of pressure on the iron arsenide superconductor LixFeAs (x=0.8, 1.0, 1.1)			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 80(2009)014506	S. J. Zhang,X. C. Wang,R. Sammynaiken,J. S. Tse,L. X. Yang,Z. Li,,Q. Q. Liu,S. Desgreniers,Y. Yao,H. Z. Liu,C. Q. Jin		
151449	JPS077113712	Tc defined as Tc(on). T0 is the temperature of maximum (dR/dT) .	LaOFeAs	La1Fe1As1O1.0	La	1	Fe	1	As	1															O	1.0		1	2008																										ABCD		oxypnictide																	ZrCuSiAs	K			10.2				10.2	MTC151449																																																																																														1	solid state reaction					Superconductivity under High Pressure in LaFeAsO			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 77(2008)113712	Hironari OKADA,Kazumi IGAWA,Hiroki TAKAHASHI,Yoichi KAMIHARA,Masahiro HIRANO,Hideo HOSONO,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
151450	JPS077113712	Tc defined as Tc(on).	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95		1	2008																										ABCD		oxypnictide																	ZrCuSiAs	K			24.8				24.8	MTC151450																																																																																														1	solid state reaction					Superconductivity under High Pressure in LaFeAsO			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 77(2008)113712	Hironari OKADA,Kazumi IGAWA,Hiroki TAKAHASHI,Yoichi KAMIHARA,Masahiro HIRANO,Hideo HOSONO,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
151451	JPS077113712	Tc defined as Tc(on).	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2008																										ABCD		oxypnictide																	ZrCuSiAs	K			28.5				28.5	MTC151451																																																																																														1	solid state reaction					Superconductivity under High Pressure in LaFeAsO			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 77(2008)113712	Hironari OKADA,Kazumi IGAWA,Hiroki TAKAHASHI,Yoichi KAMIHARA,Masahiro HIRANO,Hideo HOSONO,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
151452	JPS077113712	Tc defined as Tc(on).	La(O,F)FeAs	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86		1	2008																										ABCD		oxypnictide																	ZrCuSiAs	K			19				19	MTC151452																																																																																														1	solid state reaction					Superconductivity under High Pressure in LaFeAsO			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550	J.Phys.Soc.Jpn, 77(2008)113712	Hironari OKADA,Kazumi IGAWA,Hiroki TAKAHASHI,Yoichi KAMIHARA,Masahiro HIRANO,Hideo HOSONO,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
151453	JPS078064705	hole(outer plane) = 0.207. hole(inner plane) = 0.165 determined from NMR(Knight shift).	Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.2O8.8	Ba	2	Ca	3	Cu	4	F	1.2													O	8.8		1	2009																												0234																		K		102					102																																																																																																high pressure synthesis					Antiferromagnetic Phase Transition in Four-Layered High-Tc Superconductors Ba2Ca3Cu4O8(FyO1-y)2 with Tc=55-102 K: <63>Cu- and <19>F-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)064705	Sunao SHIMIZU,Hidekazu MUKUDA,Yoshio KITAOKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Akira IYO		
151454	JPS078064705	hole(outer plane) = 0.189. hole(inner plane) = 0.150 determined from NMR(Knight shift).  Neel-T from T1(NMR).	Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.4O8.6	Ba	2	Ca	3	Cu	4	F	1.4													O	8.6		1	2009								30																				0234																		K		91					91																																																																																																high pressure synthesis					Antiferromagnetic Phase Transition in Four-Layered High-Tc Superconductors Ba2Ca3Cu4O8(FyO1-y)2 with Tc=55-102 K: <63>Cu- and <19>F-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)064705	Sunao SHIMIZU,Hidekazu MUKUDA,Yoshio KITAOKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Akira IYO		
151455	JPS078064705	hole(outer plane) = 0.167. hole(inner plane) = 0.144 determined from NMR(Knight shift).  Neel-T from T1(NMR).	Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.6O8.4	Ba	2	Ca	3	Cu	4	F	1.6													O	8.4		1	2009								50																				0234																		K		77					77																																																																																																high pressure synthesis					Antiferromagnetic Phase Transition in Four-Layered High-Tc Superconductors Ba2Ca3Cu4O8(FyO1-y)2 with Tc=55-102 K: <63>Cu- and <19>F-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)064705	Sunao SHIMIZU,Hidekazu MUKUDA,Yoshio KITAOKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Akira IYO		
151456	JPS078064705	hole(outer plane) = 0.148. hole(inner plane) = 0.132 determined from NMR(Knight shift).  Neel-T from T1(NMR). spontaneous moment below Tn* = 30 K.	Ba2Ca3Cu4O10	Ba2Ca3Cu4F2O8	Ba	2	Ca	3	Cu	4	F	2													O	8		1	2009								80																				0234																		K		55					55																																																																																																high pressure synthesis					Antiferromagnetic Phase Transition in Four-Layered High-Tc Superconductors Ba2Ca3Cu4O8(FyO1-y)2 with Tc=55-102 K: <63>Cu- and <19>F-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)064705	Sunao SHIMIZU,Hidekazu MUKUDA,Yoshio KITAOKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Akira IYO		
151457	JPS076094711		HgBa2Ca5Cu6Oz	Hg1Ba2Ca5Cu6Oz	Hg	1	Ba	2	Ca	5	Cu	6													O	z			2007																												Hg12nm			A			25.34											Hg12(n-1)n, n = 6	K	106.9						106.9										86																																																																																				HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151458	JPS076094711		HgBa2Ca6Cu7Oz	Hg1Ba2Ca6Cu7Oz	Hg	1	Ba	2	Ca	6	Cu	7													O	z			2007																												Hg12nm			A			28.47											Hg12(n-1)n, n = 7	K	104.8						104.8																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151459	JPS076094711		HgBa2Ca7Cu8Oz	Hg1Ba2Ca7Cu8Oz	Hg	1	Ba	2	Ca	7	Cu	8													O	z			2007																												Hg12nm			A			31.64											Hg12(n-1)n, n = 8	K	105.1						105.1										82																																																																																				HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151460	JPS076094711		HgBa2Ca8Cu9Oz	Hg1Ba2Ca8Cu9Oz	Hg	1	Ba	2	Ca	8	Cu	9													O	z			2007																												Hg12nm			A			34.81											Hg12(n-1)n, n = 9	K	105.1						105.1																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151461	JPS076094711		HgBa2Ca9Cu10Oz	Hg1Ba2Ca9Cu10Oz	Hg	1	Ba	2	Ca	9	Cu	10													O	z			2007																												Hg12nm			A			37.99											Hg12(n-1)n, n = 10	K	105.1						105.1										83																																																																																				HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151462	JPS076094711		HgBa2Ca10Cu11Oz	Hg1Ba2Ca10Cu11Oz	Hg	1	Ba	2	Ca	10	Cu	11													O	z			2007																												Hg12nm			A			41.16											Hg12(n-1)n, n = 11	K	105.1						105.1																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151463	JPS076094711		HgBa2Ca11Cu12Oz	Hg1Ba2Ca11Cu12Oz	Hg	1	Ba	2	Ca	11	Cu	12													O	z			2007																												Hg12nm			A			44.33											Hg12(n-1)n, n = 12	K	105.1						105.1																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151464	JPS076094711		HgBa2Ca12Cu13Oz	Hg1Ba2Ca12Cu13Oz	Hg	1	Ba	2	Ca	12	Cu	13													O	z			2007																												Hg12nm			A			47.5											Hg12(n-1)n, n = 13	K	104.8						104.8																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151465	JPS076094711		HgBa2Ca13Cu14Oz	Hg1Ba2Ca13Cu14Oz	Hg	1	Ba	2	Ca	13	Cu	14													O	z			2007																												Hg12nm			A			50.68											Hg12(n-1)n, n = 14	K	105.1						105.1										69																																																																																				HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151466	JPS076094711		HgBa2Ca14Cu15Oz	Hg1Ba2Ca14Cu15Oz	Hg	1	Ba	2	Ca	14	Cu	15													O	z			2007																												Hg12nm			A			53.86											Hg12(n-1)n, n = 15	K	105.1						105.1																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151467	JPS076094711		HgBa2Ca15Cu16Oz	Hg1Ba2Ca15Cu16Oz	Hg	1	Ba	2	Ca	15	Cu	16													O	z			2007																												Hg12nm			A			57.03											Hg12(n-1)n, n = 16	K	105.1						105.1																																																																																														HgO,CuO,Cu2O,Ca2CuO3,Ba2Ca2Cu3Oz		mixture - pellet - encapsulated in Au - heat(950-1100C,2-5h, P=3.5 GPa)					Tc vs n Relationship for Multilayered High-Tc Superconductors			Nanoelectronics Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 76(2007)094711	Akira IYO,Yasumoto TANAKA,Hijiri KITO,Yasuharu KODAMA,Parasharam M. SHIRAGE,Dilip D. SHIVAGAN,Hirofumi MATSUHATA,Kazuyasu TOKIWA,Tsuneo WATANABE		
151468	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1O9.0	Ba	2	Ca	3	Cu	4	F	1													O	9.0			2003																												0234			A	3.8573														K	103						103																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151469	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.2O8.8	Ba	2	Ca	3	Cu	4	F	1.2													O	8.8			2003																												0234			A	3.8597														K	105						105																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151470	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.4O8.6	Ba	2	Ca	3	Cu	4	F	1.4													O	8.6			2003																												0234			A	3.8607														K	91						91																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151471	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.6O8.4	Ba	2	Ca	3	Cu	4	F	1.6													O	8.4			2003																												0234			A	3.8625														K	79						79																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151472	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F1.8O8.2	Ba	2	Ca	3	Cu	4	F	1.8													O	8.2			2003																												0234			A	3.8641														K	66						66																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151473	PHC3920140		Ba2Ca3Cu4O8(O,F)2	Ba2Ca3Cu4F2O8	Ba	2	Ca	3	Cu	4	F	2													O	8			2003																												0234			A	3.8666														K	56						56																																																																																														CuF2,CuO,Cu2O,Ba2Cu3O2		mixture - press to pellet - put into Au capsule - heat(1000-1150C,2h,P=4.5 GPa)					Preparation of polycrystals with various Tc and single crystal growth of Ba2Ca3Cu4O8(O1-yFy)2 under high pressure			AIST and CREST, AIST Central 2, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 392-396(2003)140	A. Iyo,M. Hirai,K. Tokiwa,T. Watanabe,Y. Tanaka		
151474	APL092222501	valence of Cu(calculated) = 2.06.	Ba2CaCu2O4(O,F)2	Ba2Ca1Cu2F1.4O4.6	Ba	2	Ca	1	Cu	2	F	1.4													O	4.6			2008																												0212			A	3.8689		21.093												K				106			106																																																																																														BaO2,BaF2,CaF2,Cu2O,CuO,Ba2Cu3Oz		mixture - pellet - sealed in Au capsule - heat(1323K,2h,P=5 GPa)					Simplest nontoxic double-layered cuprate Ba2CaCu2O4(O,F)2 superconductor with a transition temperature of 108 K			National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett., 92(2008)222501	P. M. Shirage,D. D. Shivagan,Y. Tanaka,Y. Kodama,H. Kito,A. Iyo		
151475	APL092222501	valence of Cu(calculated) = 2.05.	Ba2CaCu2O4(O,F)2	Ba2Ca1Cu2F1.6O4.4	Ba	2	Ca	1	Cu	2	F	1.6													O	4.4			2008																												0212			A	3.873		21.054												K				108			108																																																																																														BaO2,BaF2,CaF2,Cu2O,CuO,Ba2Cu3Oz		mixture - pellet - sealed in Au capsule - heat(1323K,2h,P=5 GPa)					Simplest nontoxic double-layered cuprate Ba2CaCu2O4(O,F)2 superconductor with a transition temperature of 108 K			National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett., 92(2008)222501	P. M. Shirage,D. D. Shivagan,Y. Tanaka,Y. Kodama,H. Kito,A. Iyo		
151476	APL092222501	valence of Cu(calculated) = 2.04.	Ba2CaCu2O4(O,F)2	Ba2Ca1Cu2F1.8O4.2	Ba	2	Ca	1	Cu	2	F	1.8													O	4.2			2008																												0212			A	3.8749		20.973												K				87			87																																																																																														BaO2,BaF2,CaF2,Cu2O,CuO,Ba2Cu3Oz		mixture - pellet - sealed in Au capsule - heat(1323K,2h,P=5 GPa)					Simplest nontoxic double-layered cuprate Ba2CaCu2O4(O,F)2 superconductor with a transition temperature of 108 K			National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett., 92(2008)222501	P. M. Shirage,D. D. Shivagan,Y. Tanaka,Y. Kodama,H. Kito,A. Iyo		
151477	APL092222501	valence of Cu(calculated) = 2.03.	Ba2CaCu2O4(O,F)2	Ba2Ca1Cu2F2O4	Ba	2	Ca	1	Cu	2	F	2													O	4			2008																												0212			A	3.879		20.975												K				82			82																																																																																														BaO2,BaF2,CaF2,Cu2O,CuO,Ba2Cu3Oz		mixture - pellet - sealed in Au capsule - heat(1323K,2h,P=5 GPa)					Simplest nontoxic double-layered cuprate Ba2CaCu2O4(O,F)2 superconductor with a transition temperature of 108 K			National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett., 92(2008)222501	P. M. Shirage,D. D. Shivagan,Y. Tanaka,Y. Kodama,H. Kito,A. Iyo		
151478	APL092222501	valence of Cu(calculated) = 2.03.	Ba2CaCu2O4(O,F)2	Ba2Ca1Cu2F2.2O3.8	Ba	2	Ca	1	Cu	2	F	2.2													O	3.8			2008																												0212			A	3.8814		20.939												K				40			40																																																																																														BaO2,BaF2,CaF2,Cu2O,CuO,Ba2Cu3Oz		mixture - pellet - sealed in Au capsule - heat(1323K,2h,P=5 GPa)					Simplest nontoxic double-layered cuprate Ba2CaCu2O4(O,F)2 superconductor with a transition temperature of 108 K			National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett., 92(2008)222501	P. M. Shirage,D. D. Shivagan,Y. Tanaka,Y. Kodama,H. Kito,A. Iyo		
151479	JPS078073701	Tc depends on R-site disorder	Nd(O,F)FeAs	Nd1Fe1As1F0.175O0.825	Nd	1	Fe	1	As	1	F	0.175													O	0.825			2009																												oxypnictide			A	3.964		8.572												K				53			53																																																																																																sintering(1050C,10h,in quartz tube)					Effect of Ln-Site Disorder on Tc of Oxypnictide Superconductor LnFeAsO1-xFx (Ln = Nd, Ce-Gd, and La-Dy)			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603	J.Phys.Soc.Jpn, 78(2009)073701	Koshi TAKENAKA,Ryotaro WATANABE,Hiroomi YAMADA,Masao TABUCHI,Yoshikazu TAKEDA,Hiroshi IKUTA		
151480	JPS078073701	Tc depends on R-site disorder	N(Ce,Gd)(O,F)FeAs	Ce0.62Gd0.38Fe1As1F0.175O0.825	Ce	0.62	Gd	0.38	Fe	1	As	1	F	0.175											O	0.825			2009																												oxypnictide			A	3.961		8.579												K				44			44																																																																																																sintering(1050C,10h,in quartz tube)					Effect of Ln-Site Disorder on Tc of Oxypnictide Superconductor LnFeAsO1-xFx (Ln = Nd, Ce-Gd, and La-Dy)			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603	J.Phys.Soc.Jpn, 78(2009)073701	Koshi TAKENAKA,Ryotaro WATANABE,Hiroomi YAMADA,Masao TABUCHI,Yoshikazu TAKEDA,Hiroshi IKUTA		
151481	JPS078073701	Tc depends on R-site disorder	(La,Dy)(O,F)FeAs	La0.62Dy0.38Fe1As1F0.175O0.825	La	0.62	Dy	0.38	Fe	1	As	1	F	0.175											O	0.825			2009																												oxypnictide			A	3.974		8.617												K				38			38																																																																																																sintering(1050C,10h,in quartz tube)					Effect of Ln-Site Disorder on Tc of Oxypnictide Superconductor LnFeAsO1-xFx (Ln = Nd, Ce-Gd, and La-Dy)			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603	J.Phys.Soc.Jpn, 78(2009)073701	Koshi TAKENAKA,Ryotaro WATANABE,Hiroomi YAMADA,Masao TABUCHI,Yoshikazu TAKEDA,Hiroshi IKUTA		
151482	JPS078073706	not SC upto 8 GPa. hydrostatic pressure using cubic anvil. structural transition at Ts = 138 K(P = 0). (dTs/dP) = -7.0 K/GPa.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K					0																																																																																																		FeAs self-flux method. heat(1100C,in quartz tube) - cool to 900C in 50h.					Intrinsic Properties of AFe2As2 (A= Ba, Sr) Single Crystal under Highly Hydrostatic Pressure Conditions			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)073706	Kazuyuki MATSUBAYASHI,Naoyuki KATAYAMA,Kenya OHGUSHI,Atsushi YAMADA,Koji MUNAKATA,Takehiko MATSUMOTO,Yoshiya UWATOKO		
151483	JPS078073706	P-induced SC. Tc(max) = 31.7 K at P= 5 GPa. Tc defined as R=0. hydrostatic pressure using cubic anvil.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K	31.7			26.3	0		26.3	MPH151483																																																																																															FeAs self-flux method. heat(1100C,in quartz tube) - cool to 900C in 50h.					Intrinsic Properties of AFe2As2 (A= Ba, Sr) Single Crystal under Highly Hydrostatic Pressure Conditions			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581	J.Phys.Soc.Jpn, 78(2009)073706	Kazuyuki MATSUBAYASHI,Naoyuki KATAYAMA,Kenya OHGUSHI,Atsushi YAMADA,Koji MUNAKATA,Takehiko MATSUMOTO,Yoshiya UWATOKO		
151484	JPS078073708	superparamagnetism start below 13K. Re-entrant SC. Tm in FIG shows reentrant temperature.	(Sn,Tm)Tm4Rh6Sn18	Tm5Rh6Sn18	Tm	5	Rh	6	Sn	18																		3	2009					myu-B/Tm	7.5																				A5B6C18			I4<1>/acd		A	13.73		27.41												K	2.2		2.3			0.07	2.25	MTC151484																																																																																															Sn-flux method. starting composition: Tm:Rh:Sn=1:1.2:10.  heat(1050C,3h) - cool to 200C(5C/h).					Coexistence of Superconductivity and Magnetism in the Tm-Based Reentrant Superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 78(2009)073708	Naoki KASE,Jun AKIMITSU,Yasuyuki ISHII,Takao SUZUKI,Isao WATANABE,Masanori MIYAZAKI,Masatoshi HIRAISHI,Soshi TAKESHITA,Ryosuke KADONO		
151485	JPS078074712		FeTe	Fe1Te1	Fe	1	Te	1																					2009																										AB		PbO	P4/nmm		A	3.8097		6.2756												K					2																																																																																																		solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151486	JPS078074712		FeTex	Fe1Te0.92	Fe	1	Te	0.92																					2009																										AB		PbO	P4/nmm		A	3.822		6.292												K					2																																																																																																		solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151487	JPS078074712		Fe(Se,Te)	Fe1Se0.25Te0.75	Fe	1	Se	0.25	Te	0.75																		1	2009																										AB		PbO	P4/nmm		A	3.814		6.157												K	11.8	13.2	13.4	9.5			13.2										100																																																																																						solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151488	JPS078074712		Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																		1	2009																										AB		PbO	P4/nmm		A	3.7909		5.957												K	10.8	12.3	14.7	10.5			12.3										100																																																																																						solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151489	JPS078074712		Fe(Se,Te)	Fe1Se0.75Te0.25	Fe	1	Se	0.75	Te	0.25																			2009																										AB		PbO	P4/nmm		A	3.7989		5.968												K	9.1	13.3	15.3	13.5			13.3										40																																																																																						solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151490	JPS078074712		Fe(Se,Te)	Fe1Se1	Fe	1	Se	1																					2009																										AB		PbO	P4/nmm		A	3.7696		5.52												K	7.51	9.51	13.5				9.51										27																																																																																						solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151491	JPS078074712		Fe(Se,S)	Fe1Se0.9S0.1	Fe	1	Se	0.9	S	0.1																			2009																										AB		PbO	P4/nmm		A	3.763		5.503												K	8.92	10.6	14.8				10.6										68																																																																																						solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151492	JPS078074712		Fe(Se,S)	Fe1Se0.8S0.2	Fe	1	Se	0.8	S	0.2																			2009																										AB		PbO	P4/nmm		A	3.754		5.442												K	8.92	10.8	15.5				10.8																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151493	JPS078074712		Fe(Se,S)	Fe1Se0.7S0.3	Fe	1	Se	0.7	S	0.3																			2009																										AB		PbO	P4/nmm		A	3.75		5.399												K	3.42	5.94	11.8				5.94																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151494	JPS078074712		Fe(Se,S)	Fe1Se0.6S0.4	Fe	1	Se	0.6	S	0.4																			2009																										AB		PbO	P4/nmm		A	3.747		5.342												K		3.73	11				3.73																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151495	JPS078074712		Fe(Se,S)	Fe1Se0.5S0.5	Fe	1	Se	0.5	S	0.5																			2009																										AB		PbO	P4/nmm		A	3.732		5.381												K		2.75	6.53				2.75																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151496	JPS078074712		(Fe,Co)Se	Fe0.95Co0.05Se1	Fe	0.95	Co	0.05	Se	1																			2009																										AB		PbO	P4/nmm		A	3.7675		5.512												K			10				10																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151497	JPS078074712		(Fe,Co)Se	Fe0.9Co0.1Se1	Fe	0.9	Co	0.1	Se	1																			2009																										AB		PbO	P4/nmm		A	3.7637		5.5043												K			5				5																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151498	JPS078074712		(Fe,Co)Se	Fe0.8Co0.2Se1	Fe	0.8	Co	0.2	Se	1																			2009																										AB		PbO	P4/nmm		A	3.7562		5.483												K					2																																																																																																		solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151499	JPS078074712		(Fe,Ni)Se	Fe0.95Ni0.05Se1	Fe	0.95	Ni	0.05	Se	1																			2009																										AB		PbO	P4/nmm		A	3.7714		5.508												K			10				10																																																																																																solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151500	JPS078074712		(Fe,Ni)Se	Fe0.9Ni0.1Se1	Fe	0.9	Ni	0.1	Se	1																			2009																										AB		PbO	P4/nmm		A	3.7713		5.503												K					2																																																																																																		solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151501	JPS078074712		(Fe,Ni)Se	Fe0.8Ni0.2Se1	Fe	0.8	Ni	0.2	Se	1																			2009																										AB		PbO	P4/nmm		A	3.775		5.489												K					2																																																																																																		solid state reaction.  heat(680-800C)					Substitution Effects on FeSe Superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047	J.Phys.Soc.Jpn, 78(2009)074712	Yoshikazu MIZUGUCHI,Fumiaki TOMIOKA,Shunsuke TSUDA,Takahide YAMAGUCHI,Yoshihiko TAKANO		
151502	PRB080024511	Compositions determined by WDS. T0 (in Figure) is structural transition temperature. Tc=23.2 K (SP-heat). (dC) and [gamma] estimated asuming BCS (dC/gamma*Tc) = 1.43	Ba(Fe,Rh)2As2	Ba1Fe1.886Rh0.114As2	Ba	1	Fe	1.886	Rh	0.114	As	2																3	2009																										AB2C2		ThCr2Si2																		K				24.9		0.7	24.9	MTC151502																																																					mJ/mol.K	700	mJ/mol.K2	20	SP-heat																																						self-flux method(Ba:MAs=1:4). heat(1180C,5h) - cool to 1050C(/36h) in sealed quartz tube.					Phase diagrams of Ba(Fe1-xMx)2As2 single crystals (M=Rh and Pd)			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)024511	N. Ni,A. Thaler,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
151503	PRB080024511	Compositions determined by WDS..	Ba(Fe,Rh)2As2	Ba1Fe1.808Rh0.192As2	Ba	1	Fe	1.808	Rh	0.192	As	2																3	2009																										AB2C2		ThCr2Si2																		K				17.8			17.8																																																																																																self-flux method(Ba:MAs=1:4). heat(1180C,5h) - cool to 1050C(/36h) in sealed quartz tube.					Phase diagrams of Ba(Fe1-xMx)2As2 single crystals (M=Rh and Pd)			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)024511	N. Ni,A. Thaler,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
151504	PRB080024511	Compositions determined by WDS. T0 (in Figure) is structural transition temperature.	Ba(Fe,Pd)2As2	Ba1Fe1.914Pd0.086As2	Ba	1	Fe	1.914	Pd	0.086	As	2																3	2009																										AB2C2		ThCr2Si2																		K				18.9		0.6	18.9	MTC151503																																																					mJ/mol.K	410	mJ/mol.K2	16	SP-heat																																						self-flux method(Ba:MAs=1:4). heat(1180C,5h) - cool to 1050C(/36h) in sealed quartz tube.					Phase diagrams of Ba(Fe1-xMx)2As2 single crystals (M=Rh and Pd)			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)024511	N. Ni,A. Thaler,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
151505	PRB080024511	Compositions determined by WDS. T0 (in Figure) is structural transition temperature. (dC) and [gamma] estimated asuming BCS (dC/gamma*Tc) = 1.43	Ba(Fe,Pd)2As2	Ba1Fe1.958Rh0.042As2	Ba	1	Fe	1.958	Rh	0.042	As	2																3	2009																										AB2C2		ThCr2Si2																		K				5.41			5.41																																																																																																self-flux method(Ba:MAs=1:4). heat(1180C,5h) - cool to 1050C(/36h) in sealed quartz tube.					Phase diagrams of Ba(Fe1-xMx)2As2 single crystals (M=Rh and Pd)			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)024511	N. Ni,A. Thaler,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
151506	PRB080024506	Tc defined as Tc(on).  sample has maximum-Tc for this system.	Sr(Fe,Rh)2As2	Sr1Fe1.75Rh0.25As2	Sr	1	Fe	1.75	Rh	0.25	As	2																1	2009																										AB2C2		ThCr2Si2			A	3.9478		12.232												K			21.9				21.9	MPH151506																																	MHC151506																																																												SrAs,FeAs,MAs(M=Rh,Ir,Pd)		two step solid state reaction. mixture(with Fe) - sealed in silica tube(Ar) - heat(900C,30h) - cool to RT					Superconductivity and phase diagrams of the 4d- and 5d-metal-doped iron arsenides SrFe2-xMxAs2 (M=Rh, Ir,Pd)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)024506	Fei Han,Xiyu Zhu,Peng Cheng,Gang Mu,Ying Jia,Lei Fang,Yonglei Wang,Huiqian Luo,Bin Zeng,Bing Shen,Lei Shan,Cong Ren,Hai-Hu Wen		
151507	PRB080024506	Tc defined as Tc(on).  sample has maximum-Tc for this system.	Sr(Fe,Ir)2As2	Sr1Fe1.57Ir0.43As2	Sr	1	Fe	1.57	Ir	0.43	As	2																1	2009																										AB2C2		ThCr2Si2			A	3.9501		12.25												K			24.2				24.2	MPH151507																																	MHC151507																																																												SrAs,FeAs,MAs(M=Rh,Ir,Pd)		two step solid state reaction. mixture(with Fe) - sealed in silica tube(Ar) - heat(900C,30h) - cool to RT					Superconductivity and phase diagrams of the 4d- and 5d-metal-doped iron arsenides SrFe2-xMxAs2 (M=Rh, Ir,Pd)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)024506	Fei Han,Xiyu Zhu,Peng Cheng,Gang Mu,Ying Jia,Lei Fang,Yonglei Wang,Huiqian Luo,Bin Zeng,Bing Shen,Lei Shan,Cong Ren,Hai-Hu Wen		
151508	PRB080024506	Tc defined as Tc(on).  sample has maximum-Tc for this system.	Sr(Fe,Pd)2As2	Sr1Fe1.85Pd0.15As2	Sr	1	Fe	1.85	Pd	0.15	As	2																1	2009																										AB2C2		ThCr2Si2			A	3.9537		12.278												K			8.7				8.7	MPH151508																																	MHC151508																																																												SrAs,FeAs,MAs(M=Rh,Ir,Pd)		two step solid state reaction. mixture(with Fe) - sealed in silica tube(Ar) - heat(900C,30h) - cool to RT					Superconductivity and phase diagrams of the 4d- and 5d-metal-doped iron arsenides SrFe2-xMxAs2 (M=Rh, Ir,Pd)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)024506	Fei Han,Xiyu Zhu,Peng Cheng,Gang Mu,Ying Jia,Lei Fang,Yonglei Wang,Huiqian Luo,Bin Zeng,Bing Shen,Lei Shan,Cong Ren,Hai-Hu Wen		
151509	PRB080024518	nominal: FeSe0.82. Thermal conductivity k:  (k/T) = a + b*T^(p-1), a=16 uW/K2.cm, p=2.47 from fitting.	FeSe	Fe1Se1	Fe	1	Se	1																				3	2009																										AB																				K		8.8	11.9				8.8																				T	resistivity, parabolic T-dependence of Hc2, Tc(on)	20.1			14.5			6.3																																					MTHC151509						mOhm.cm		0.0579																							single crystals grown by vapor self-transport method.					Multigap nodeless superconductivity in FeSex: Evidence from quasiparticle heat transport			Department of Physics, Surface Physics Laboratory (National Key Laboratory), and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 80(2009)024518	J. K. Dong,T. Y. Guan,S. Y. Zhou,X. Qiu,L. Ding,C. Zhang,U. Patel,Z. L. Xiao,S. Y. Li		
151510	PRB080024519	P-induced SC.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2009								171																		AB2C2		ThCr2Si2																		K		11.6			0		11.6	MTC151510																																																																																															Sn-flux method					Pressure-induced superconducting state of antiferromagnetic CaFe2As2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 80(2009)024519	Hanoh Lee,Eunsung Park,Tuson Park,V. A. Sidorov,F. Ronning,E. D. Bauer,J. D. Thompson		
151511	PRL103027003	Tc defined as R=0.1Rn. another transition at T=1.7 K. GL parameter = 21. e-ph coupling = 0.49. (dC/gamma*Tc) = 1.5.	Ce2PdIn8	Ce2Pd1In8	Ce	2	Pd	1	In	8																		3	2009					myu-B/Ce	2.51	-42.6	10																		AB2C8		Ho2CoGa8																		K	0.68						0.68																				T	resstivity, extraporation	4.8							T/K	resistivity	14.3			MHC151511		A	Hc2(0)	82			A		1740										MSP151511			mJ/mol.K2	1000	SP-heat																																						In-flux method					Emergence of a Superconducting State from an Antiferromagnetic Phase in Single Crystals of the Heavy Fermion Compound Ce2PdIn8			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.Lett., 103(2009)027003	D. Kaczorowski,A. P. Pikul,D. Gnida,V. H. Tran		
151512	PRB080060502	gap measured by point contact Andreev reflection. Two gaps: upper = 15 meV(ratio = 8.31), lower = 4.9 meV(ratio = 2.71)	Sm(O,F)FeAs	Sm1Fe1As1F0.09O0.91	Sm	1	Fe	1	As	1	F	0.09													O	0.91		1	2009																										ABCD		oxypnictide																		K		42					42																																														meV	15	8.31																																														SmAs,FeAs,SmF3,Fe2O3,Fe		mixture - heat(1350-1450C,5h,P=30 kbar)					Evidence for two-gap nodeless superconductivity in SmFeAsO1-xFx from point-contact Andreev-reflection spectroscopy			Dipartimento di Fisica and CNISM, Politecnico di Torino, 10129 Torino, Italy	Phys.Rev.B, 80(2009)060502	D. Daghero,M. Tortello,R. S. Gonnelli,V. A. Stepanov,N. D. Zhigadlo,J. Karpinski		
151513	PRB080060502	gap measured by point contact Andreev reflection. Two gaps: upper = 18 meV(ratio = 8.05), lower = 6.15 meV(ratio = 2.75)	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		1	2009																										ABCD		oxypnictide																		K		52					52																																														meV	18	8.05																																														SmAs,FeAs,SmF3,Fe2O3,Fe		mixture - heat(1350-1450C,5h,P=30 kbar)					Evidence for two-gap nodeless superconductivity in SmFeAsO1-xFx from point-contact Andreev-reflection spectroscopy			Dipartimento di Fisica and CNISM, Politecnico di Torino, 10129 Torino, Italy	Phys.Rev.B, 80(2009)060502	D. Daghero,M. Tortello,R. S. Gonnelli,V. A. Stepanov,N. D. Zhigadlo,J. Karpinski		
151514	PRB080054502		LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2009																										ABCD		oxypnictide			A	4.0328		8.7372											ZrCuSiAs	K					2																																																																																																La,Fe,Fe2O3,Ir,As		mixture - (sealed in Nb-tube) - heat(1180C,45h)					Superconductivity in Ir-doped LaFe1-xIrxAsO			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Phys.Rev.B, 80(2009)054502	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Zhiyu Zhang,Yanwei Ma		
151515	PRB080054502		LaO(Fe,Ir)As	La1Fe0.95Ir0.05As1O1	La	1	Fe	0.95	Ir	0.05	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0356		8.7146											ZrCuSiAs	K		7.18					7.18																																																																																														La,Fe,Fe2O3,Ir,As		mixture - (sealed in Nb-tube) - heat(1180C,45h)					Superconductivity in Ir-doped LaFe1-xIrxAsO			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Phys.Rev.B, 80(2009)054502	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Zhiyu Zhang,Yanwei Ma		
151516	PRB080054502	carrier = 3.71 E+20 /cm3 at 100K. from Hall coefficient.	LaO(Fe,Ir)As	La1Fe0.925Ir0.075As1O1	La	1	Fe	0.925	Ir	0.075	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0361		8.7071											ZrCuSiAs	K		11.85					11.85																				T	resistivity, WHH	54.3							T/K	resistivity	6.7			MHC151516																																																												La,Fe,Fe2O3,Ir,As		mixture - (sealed in Nb-tube) - heat(1180C,45h)					Superconductivity in Ir-doped LaFe1-xIrxAsO			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Phys.Rev.B, 80(2009)054502	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Zhiyu Zhang,Yanwei Ma		
151517	PRB080054502		LaO(Fe,Ir)As	La1Fe0.9Ir0.1As1O1	La	1	Fe	0.9	Ir	0.1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0381		8.6986											ZrCuSiAs	K		10.9					10.9																																																																																														La,Fe,Fe2O3,Ir,As		mixture - (sealed in Nb-tube) - heat(1180C,45h)					Superconductivity in Ir-doped LaFe1-xIrxAsO			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Phys.Rev.B, 80(2009)054502	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Zhiyu Zhang,Yanwei Ma		
151518	PRB080054502		LaO(Fe,Ir)As	La1Fe0.875Ir0.125As1O1	La	1	Fe	0.875	Ir	0.125	As	1													O	1			2009																										ABCD		oxypnictide			A	4.04		8.6921											ZrCuSiAs	K		4.56					4.56																																																																																														La,Fe,Fe2O3,Ir,As		mixture - (sealed in Nb-tube) - heat(1180C,45h)					Superconductivity in Ir-doped LaFe1-xIrxAsO			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Phys.Rev.B, 80(2009)054502	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Zhiyu Zhang,Yanwei Ma		
151519	PRL103037005	some samples are not SC. Maybe strain-induced SC. structural(tetra-to-ortho)transition with AFM at 198 K.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K		21		21			21																				T	resistivity													MHC151519																																																														FeAs self-flux method					Superconducting and Ferromagnetic Phases Induced by Lattice Distortions in Stoichiometric SrFe2As2 Single Crystals			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.Lett., 103(2009)037005	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione,P.Y. Zavalij		
151520	PRB078220510	[penet] measured using muon-SR. TBL values of gap are for anisotropic s-wave model. For two gap model, gap(0) = 1.60 and 0.38 meV, gap ratio = 4.49 and 1.07.respectively.	FeSe0.85	Fe1Se0.85	Fe	1	Se	0.85																					2008																										AB																				K				8.26			8.26																																									A	muon-SR	4050			meV	2.24	6.27	16																																																				Evidence of nodeless superconductivity in FeSe0.85 from a muon-spin-rotation study of the in-plane magnetic penetration depth			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 78(2008)220510	R. Khasanov,K. Conder,E. Pomjakushina,A. Amato,C. Baines,Z. Bukowski,J. Karpinski,S. Katrych,H.-H. Klauss,H. Luetkens,A. Shengelaya,N. D. Zhigadlo		
151521	PRL103067010	[penet] obtained using alpha-model for muon-SR. TBL values for dirty model.two gaps. [gapene] for the higher. for clean model,[penet]=315(ab), 870(c)nm. [gapene]=7.2(H), 2.7(L)	Sr(Fe,Co)2As2	Sr1Fe1.75Co0.25As2	Sr	1	Fe	1.75	Co	0.25	As	2																3	2009																										AB2C2		ThCr2Si2																		K				13.3			13.3										100																															A	muon-SR		3150	8700			5.8	16																																																				Superconductivity and Field-Induced Magnetism in SrFe1.75Co0.25As2			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 103(2009)067010	R. Khasanov,A. Maisuradze,H. Maeter,A. Kwadrin,H. Luetkens,A. Amato,W. Schnelle,H. Rosner,A. Leithe-Jasper,H.-H. Klauss		
151522	PRL103077004	SP-heat measured for H//c. [gamma] increases and [gapene] decreases with x (from 0.05 to 0.45).	LixZrNCl	Li0.1Zr1N1Cl1	Li	0.1	Zr	1	N	1	Cl	1																	2009																										ABCD																				K		14					14																																																4.14	14							mJ/mol.K2	0.99	SP-heat																																											Enhancement of Pairing Interaction and Magnetic Fluctuations toward a Band Insulator in an Electron-Doped LixZrNCl Superconductor			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 103(2009)077004	Yuichi Kasahara,Tsukasa Kishiume,Takumi Takano,Katsuki Kobayashi,Eiichi Matsuoka,Hideya Onodera,Kazuhiko Kuroki,Yasujiro Taguchi,Yoshihiro Iwasa		
151523	PRL103077004	SP-heat measured for H//c. [gamma] increases and [gapene] decreases with x (from 0.05 to 0.45).	LixZrNCl	Li0.28Zr1N1Cl1	Li	0.28	Zr	1	N	1	Cl	1																	2009																										ABCD																				K		11.6					11.6																																																2.9	14							mJ/mol.K2	1.14	SP-heat																																											Enhancement of Pairing Interaction and Magnetic Fluctuations toward a Band Insulator in an Electron-Doped LixZrNCl Superconductor			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Phys.Rev.Lett., 103(2009)077004	Yuichi Kasahara,Tsukasa Kishiume,Takumi Takano,Katsuki Kobayashi,Eiichi Matsuoka,Hideya Onodera,Kazuhiko Kuroki,Yasujiro Taguchi,Yoshihiro Iwasa		
151524	PRL103087001	structural transition (tetra-ortho) temperatureat 60 K, higher than AFM transition temperature( Tn = 47 K). Neutron diffraction method.	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																	2009								47																		AB2C2		ThCr2Si2																		K		17					17																																																																																																					Coexistence of Competing Antiferromagnetic and Superconducting Phases in the Underdoped Ba(Fe0.953Co0.047)2As2 Compound Using X-ray and Neutron Scattering Techniques			Department of Physics and Astronomy and Ames Laboratory, Iowa State University, Ames, Iowa 50011 USA	Phys.Rev.Lett., 103(2009)087001	D. K. Pratt,W. Tian,A. Kreyssig,J. L. Zarestky,S. Nandi,N. Ni,S. L. Bud'ko,P. C. Canfield,A. I. Goldman,R. J. McQueeney		
151525	SSC1491296	compositions confirmed by EDS. no sign of CDW. Tc measured for J//ab.	NixTaS2	Ni0.05Ta1S2	Ni	0.05	Ta	1	S	2																		3	2009																										AB2		2H-TaS2	P6<3>/mmc		A	3.3128		11.999												K	2.2		3.9			1.4	3.05																																																																																														Ni,Ta,S powder		mixture - heat(900C,4d, in evacuated quartz tube) - heat(850C,6h,with NaCl/KCl flux, in quartz tube) - cool to 650C(2C/h) - keep(2d) - FC to RT					Superconductivity and single crystal growth of Ni0.05TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Solid State Commun., 149(2009)1296	X.D. Zhu,Y.P. Sun,S.B. Zhang,H.C. Lei,L.J. Li,X.B. Zhu,Z.R. Yang,W.H. Song,J.M. Dai		
151526	PRL0341502	Fe intercalated TaS2	FexTaS2	Fe0.05Ta1S2	Fe	0.05	Ta	1	S	2																			1975																										AB2		2H-TaS2																		K		3					3																																																																																																SIN(TaS2+Fe)					Superconductivity in dilute alloys of TaS2 with Fe				Phys.Rev.Lett., 34(1975)1502	Robert m.Fleming,R.V.Coleman		
151527	PRL0341502	M=pyridine. M-intercalated TaS2	MxTaS2	M0.5Ta1S2	M	0.5	Ta	1	S	2																			1975																										AB2		2H-TaS2																		K		3.2					3.2																																																																																																SIN(TaS2+Fe)					Superconductivity in dilute alloys of TaS2 with Fe				Phys.Rev.Lett., 34(1975)1502	Robert m.Fleming,R.V.Coleman		
151528	PRB0152943	lattice term coeffic. off SP : (beta) = 0.55 mJ/mol.K4. CDW temperature(onset) = 33.5 K.	2H-NbSe2	Nb1Se2	Nb	1	Se	2																					1977																										AB2																				K		7.2					7.2																																																								mJ/mol.K2	16	SP-heat	222	SP-heat																																				vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151529	PRB0152943	lattice term coeffic. off SP : (beta) = 0.44 mJ/mol.K4. CDW temperature(onset) = 78.0 K.	2H-TaS2	Ta1S2	Ta	1	S	2																					1977																										AB2																				K		0.8					0.8																																																								mJ/mol.K2	7.5	SP-heat	236	SP-heat																																				vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151530	PRB0152943	lattice term coeffic. off SP : (beta) = 0.71 mJ/mol.K4. CDW temperature(onset) = 121 K.	2H-TaSe2	Ta1Se2	Ta	1	Se	2																					1977																										AB2																				K		0.15					0.15																																																								mJ/mol.K2	4.5	SP-heat	202	SP-heat																																				vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151531	PRB0152943	lattice term coeffic. off SP : (beta) = 0.45 mJ/mol.K4. CDW temperature(onset) = 317 K.	4Hb-TaS2	Ta1S2	Ta	1	S	2																					1977																										AB2																				K					1.1																																																										mJ/mol.K2	3	SP-heat	234	SP-heat																																				vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151532	PRB0152943	lattice term coeffic. off SP : (beta) = 0.83 mJ/mol.K4. CDW temperature(onset) = 75 K.	4Hb-TaSe2	Ta1Se2	Ta	1	Se	2																					1977																										AB2																				K					1.1																																																										mJ/mol.K2	4.5	SP-heat	192	SP-heat																																				vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151533	PRB0152943	CDW temperature(onset) = 110 K.	1T-VSe2	V1Se2	V	1	Se	2																					1977																										AB2																				K					1.1																																																																																																		vapor transport method					Thermal properties of layered transition-metal dichalcogenides at charge-density-wave transition				Phys.Rev.B, 15(1977)2943	J.M.E.Harper,T.H.Geballe,F.J.DiSalvo		
151534	PRB080060503	compositions by ICP. energy gap by NMR.	Mg10Ir19B16	Mg9.3Ir19B16.7	Mg	9.3	Ir	19	B	16.7																			2009																										A10B16C19																				K		5.8					5.8																																																3	6																																															mixture(powder) - pellet - wrapped in Ta foil - SIN(600C,30min + 950C,3h, in evacuated quartz tube) - reground - pellet - ANN(950C,12h)					Superconducting state in the noncentrosymmetric Mg9.3Ir19B16.7 and Mg10.5Ir19B17.1 revealed by NMR			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 80(2009)060503	K. Tahara,Z. Li,H. X. Yang,J. L. Luo,S. Kawasaki,Guo-qing Zheng		
151535	PRB080060503	compositions by ICP. energy gap by NMR.	Mg10Ir19B16	Mg10.5Ir19B17.1	Mg	10.5	Ir	19	B	17.1																			2009																										A10B16C19																				K		4.8					4.8																																																2.2	6																																															mixture(powder) - pellet - wrapped in Ta foil - SIN(600C,30min + 950C,3h, in evacuated quartz tube) - reground - pellet - ANN(950C,12h)					Superconducting state in the noncentrosymmetric Mg9.3Ir19B16.7 and Mg10.5Ir19B17.1 revealed by NMR			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 80(2009)060503	K. Tahara,Z. Li,H. X. Yang,J. L. Luo,S. Kawasaki,Guo-qing Zheng		
151536	PRB080064504	(dC/Tc) = 7.8 mJ/mol.K2. (dC/gamma*Tc) = 1.38. (dHc2/dT) = -0.1 T/K from resistive transition.	BaPtSi3	Ba1Pt1Si3	Ba	1	Pt	1	Si	3																			2009																										ABC3		BaNiSn3	I4mm		A	4.4013		10.013												K	2						2			K/GPa	-0.6																T	SP heat, WHH	0.053							T/K	SP heat	-0.033																									mJ/mol.K2	5.7	SP-heat	345	resistivity											uOhm.cm							6																		arc-melting. ANN(900C,100h, in quartz tube) - Q to water					BaPtSi3: A noncentrosymmetric BCS-like superconductor			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 80(2009)064504	E. Bauer,R. T. Khan,H. Michor,E. Royanian,A. Grytsiv,N. Melnychenko-Koblyuk,P. Rogl,D. Reith,R. Podloucky,E.-W. Scheidt,W. Wolf,M. Marsman		
151537	PRB080064514		CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.186		4.3972												K		7.8					7.8																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151538	PRB080064514		SrAlSi	Sr1Al1Si1	Sr	1	Al	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.2433		4.7435												K		4.7					4.7																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151539	PRB080064514		BaAlSi	Ba1Al1Si1	Ba	1	Al	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.3		5.1438												K					2																																																																																																		arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151540	PRB080064514		SrAlGe	Sr1Al1Ge1	Sr	1	Al	1	Ge	1																		1	2009																										ABC		SrPtSb	P6[-]m2		A	4.3043		4.7407												K		6.7					6.7																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151541	PRB080064514		BaAlGe	Ba1Al1Ge1	Ba	1	Al	1	Ge	1																		1	2009																										ABC		SrPtSb	P6[-]m2		A	4.3512		4.1401												K		6.3					6.3																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151542	PRB080064514		BaAlSn	Ba1Al1Sn1	Ba	1	Al	1	Sn	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.6331		5.1408												K		2.9					2.9																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151543	PRB080064514		CaGaSi	Ca1Ga1Si1	Ca	1	Ga	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.1101		4.4466												K		4.4					4.4																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151544	PRB080064514		SrGaSi	Sr1Ga1Si1	Sr	1	Ga	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.1835		4.7422												K		4.9					4.9																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151545	PRB080064514		BaGaSi	Ba1Ga1Si1	Ba	1	Ga	1	Si	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.2479		5.1106												K		4.2					4.2																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151546	PRB080064514		CaGaGe	Ca1Ga1Ge1	Ca	1	Ga	1	Ge	1																		1	2009																										ABC		YPtAs	P6<3>/mmc		A	4.2203		17.2876												K					2																																																																																																		arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151547	PRB080064514		SrGaGe	Sr1Ga1Ge1	Sr	1	Ga	1	Ge	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.2718		4.7179												K		2.6					2.6																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151548	PRB080064514		BsGaGe	Ba1Ga1Ge1	Ba	1	Ga	1	Ge	1																		1	2009																										ABC		AlB2	P6/mmm		A	4.3351		5.0947												K		2.4					2.4																																																																																																arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151549	PRB080064514		SrGaSn	Sr1Ga1Sn1	Sr	1	Ga	1	Sn	1																		1	2009																										ABC		YPtAs	P6<3>/mmc		A	4.5505		18.71												K					2																																																																																																		arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151550	PRB080064514		BaGaSn	Ba1Ca1Sn1	Ba	1	Ca	1	Sn	1																		1	2009																										ABC		CaIn2	P6<3>/mmc		A	4.5807		10.3303												K					2																																																																																																		arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151551	PRB080064514		BaInGe	Ba1In1Ge1	Ba	1	In	1	Ge	1																		1	2009																										ABC		EuGe2	P3[-]m1		A	4.5709		5.0994												K					2																																																																																																		arc-melting					Structural properties and superconductivity in the ternary intermetallic compounds MAB (M=Ca, Sr, Ba; A=Al, Ga, In; B=Si, Ge, Sn)			Department of Chemistry and Biochemistry, Arizona State University, Tempe, Arizona 85287-1604, USA	Phys.Rev.B, 80(2009)064514	Michael J. Evans,Yang Wu,Verina F. Kranak,N. Newman,Armin Reller,F. Javier Garcia-Garcia,Ulrich Haussermann		
151552	PRB080052501	The film exposed (air,6h) is SC. Tc(on) = 25 K. c-axis distance reduces due to water vapor.	(H2O)-SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2009								204																		AB2C2		ThCr2Si2																		K	21		25				23																																																																																																films grown on (La,Sr)(Al,Ta)O3[001] substrates by pulsed laser deposition using SrFe2As2 target. T<sub> = 700C.					Water-induced superconductivity in SrFe2As2			ERATO-SORST, Japan Science and Technology Agency, in Frontier Research Center, Tokyo Institute of Technology, S2-6F East, Mailbox S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 80(2009)052501	Hidenori Hiramatsu,Takayoshi Katase,Toshio Kamiya,Masahiro Hirano,Hideo Hosono		
151553	PRB080052508	optimal F-content. Tc depends on Fe-As-Fe angle.	Tb(O,F)FeAs	Tb1Fe1As1F0.1O0.9	Tb	1	Fe	1	As	1	F	0.1													O	0.9			2009																										ABCD		oxypnictide																		K				51			51																																																																																																					Suppression of the superconducting transition of RFeAsO1-xFx (R=Tb, Dy, and Ho)			Centre for Science at Extreme Conditions, University of Edinburgh, King's Buildings, Mayfield Road, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.B, 80(2009)052508	Jennifer A. Rodgers,George B. S. Penny,Andrea Marcinkova,Jan-Willem G. Bos,Dmitry A. Sokolov,Anna Kusmartseva,Andrew D. Huxley,J. Paul Attfield		
151554	PRB080052508	optimal F-content. Tc depends on Fe-As-Fe angle.	Dy(O,F)FeAs	Dy1Fe1As1F0.1O0.9	Dy	1	Fe	1	As	1	F	0.1													O	0.9			2009																										ABCD		oxypnictide																		K				45			45																																																																																																					Suppression of the superconducting transition of RFeAsO1-xFx (R=Tb, Dy, and Ho)			Centre for Science at Extreme Conditions, University of Edinburgh, King's Buildings, Mayfield Road, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.B, 80(2009)052508	Jennifer A. Rodgers,George B. S. Penny,Andrea Marcinkova,Jan-Willem G. Bos,Dmitry A. Sokolov,Anna Kusmartseva,Andrew D. Huxley,J. Paul Attfield		
151555	PRB080052508	optimal F-content. Tc depends on Fe-As-Fe angle.	Ho(O,F)FeAs	Ho1Fe1As1F0.1O0.9	Ho	1	Fe	1	As	1	F	0.1													O	0.9			2009																										ABCD		oxypnictide																		K				36			36																																																																																																					Suppression of the superconducting transition of RFeAsO1-xFx (R=Tb, Dy, and Ho)			Centre for Science at Extreme Conditions, University of Edinburgh, King's Buildings, Mayfield Road, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.B, 80(2009)052508	Jennifer A. Rodgers,George B. S. Penny,Andrea Marcinkova,Jan-Willem G. Bos,Dmitry A. Sokolov,Anna Kusmartseva,Andrew D. Huxley,J. Paul Attfield		
151556	PRB080052503	magnetic order detected by ZF-muonSR.	Sm(O,F)FeAs	Sm1Fe1As1F0.085O0.915	Sm	1	Fe	1	As	1	F	0.085													O	0.915		1	2009								22																		ABCD																				K				14			14	TC151556																																																																																															polycrystalline sample synthesized in sealed Ta-ampoules.					Magnetic-superconducting phase boundary of SmFeAsO1-xFx studied via muon spin rotation: Unified behavior in a pnictide family			Dipartimento di Fisica, Unita CNISM di Parma, I 43100 Parma, Italy	Phys.Rev.B, 80(2009)052503	S. Sanna,R. De Renzi,G. Lamura,C. Ferdeghini,A. Palenzona,M. Putti,M. Tropeano,T. Shiroka		
151557	PRB080052503	magnetic order detected by ZF-muonSR.	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		1	2009																										ABCD																				K				50			50	TC151556																																																																																															polycrystalline sample synthesized in sealed Ta-ampoules.					Magnetic-superconducting phase boundary of SmFeAsO1-xFx studied via muon spin rotation: Unified behavior in a pnictide family			Dipartimento di Fisica, Unita CNISM di Parma, I 43100 Parma, Italy	Phys.Rev.B, 80(2009)052503	S. Sanna,R. De Renzi,G. Lamura,C. Ferdeghini,A. Palenzona,M. Putti,M. Tropeano,T. Shiroka		
151560	JAP0374880	impurity phase: NbSn2 < 3%.	Nb6Sn5	Nb6Sn5	Nb	6	Sn	5																					1966																										A5B6	3				A	5.656	9.212	16.8												K	2.7	2.8	3			0.4	2.8																				Oe	resistivity				600			2.1																																																																				(Nb rod + Sn) - heat(temperature gradient range from 1000C to 800C for 2w). Unreacted Sn was removed by etching in 50 HCl + 50 H2O solution.					Superconducting properties of Nb6Sn5 and of multiphase Nb-Sn alloya			RCA Laboratories, Princeton, New Jersey	J.Appl.Phys., 37(1966)4880	R.E.Enstrom		
151561	JEL0140011	P-induced SC. P<cr> = 250 kbar, (dTc/dP) for 260 - 300 kbar. semicon to metal transition at P=250 kbar, RT.	GaAs	As1Ga1	As	1	Ga	1																					1971																										AB		ZnS																		K		4.8			0		4.8			K/GPa	0.02																																																																																																	Superconductivity of gallium arsenide at high pressures				JETP Lett., 14(1971)11	I.V.Berman,N.B.Brandt,V.I.Sidorov		
151562	PRB080094501	(2d/kTc) = 3.768 and 1.57 for higher and lower gap using two gap model fitting from muon-SR data.	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2009																										AB2C2		ThCr2Si2																		K	22.2	22.5	22.8	22.2			22.5																																																3.768	16																																																				Muon spin rotation measurement of the magnetic field penetration depth in Ba(Fe0.926Co0.074)2As2: Evidence for multiple superconducting gaps			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 80(2009)094501	T. J. Williams,A. A. Aczel,E. Baggio-Saitovitch,S. L. Bud'ko,P. C. Canfield,J. P. Carlo,T. Goko,J. Munevar,N. Ni,Y. J. Uemura,W. Yu,G. M. Luke		
151563	PRB080104501		TbOxFeAs	Tb1Fe1As1O1	Tb	1	Fe	1	As	1															O	1.0	1		2009																										ABCD		oxypnictide	P4/nmm																	K																																																																																																							high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151564	PRB080104501		TbOxFeAs	Tb1Fe1As1O0.9	Tb	1	Fe	1	As	1															O	0.9	0.9		2009																										ABCD		oxypnictide	P4/nmm		A	3.8912		8.3788												K		22.8					22.8																																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151565	PRB080104501		TbOxFeAs	Tb1Fe1As1O0.85	Tb	1	Fe	1	As	1															O	0.85	0.85		2009																										ABCD		oxypnictide	P4/nmm		A	3.8887		8.3744												K		42					42																																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151566	PRB080104501	(dC/Tc) = 5 mJ/mol.K2. X-ray density = 7.887 g/cm3	TbOxFeAs	Tb1Fe1As1O0.82	Tb	1	Fe	1	As	1															O	0.82	0.82		2009																										ABCD		oxypnictide	P4/nmm		A	3.8891		8.3744												K		43.8					43.8											Oe	M vs H curve				20																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151567	PRB080104501		TbOxFeAs	Tb1Fe1As1O0.8	Tb	1	Fe	1	As	1															O	0.8	0.8		2009																										ABCD		oxypnictide	P4/nmm		A	3.889		8.3793												K		35.7					35.7																																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151568	PRB080104501		TbOxFeAs	Tb1Fe1As1O0.75	Tb	1	Fe	1	As	1															O	0.75	0.75		2009																										ABCD		oxypnictide	P4/nmm		A	3.8919		8.3812												K		34.8					34.8																																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151569	PRB080104501		TbOxFeAs	Tb1Fe1As1O0.7	Tb	1	Fe	1	As	1															O	0.7	0.7		2009																										ABCD		oxypnictide	P4/nmm		A	3.8922		8.3828												K		14.9					14.9																																																																																																high pressure synthesis					Superconducting properties of the oxygen-deficient iron oxyarsenide TbFeAsO1-z from underdoped to overdoped compositions			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 80(2009)104501	Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,Y. Hata,H. Yasuoka,K. Yamaura,E. Takayama-Muromachi		
151570	PRB079220516	(dC/Tc) = 2.8 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2009																										AB2C2		ThCr2Si2																		K		6.85					6.85																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151571	PRB079220516	(dC/Tc) = 11.2 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																3	2009																										AB2C2		ThCr2Si2																		K		14.6					14.6																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151572	PRB079220516	(dC/Tc) = 26.8 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.884Co0.116As2	Ba	1	Fe	1.884	Co	0.116	As	2																3	2009																										AB2C2		ThCr2Si2																		K		22.7					22.7	MTC151572																																																																																															self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151573	PRB079220516	(dC/Tc) = 24.2 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.844Co0.156As2	Ba	1	Fe	1.844	Co	0.156	As	2																3	2009																										AB2C2		ThCr2Si2																		K		21.7					21.7																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151574	PRB079220516	(dC/Tc) = 11.8 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		15.5					15.5																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151575	PRB079220516	(dC/Tc) = 6.37 mJ/mol.K2	Ba(Fe,Co)2As2	Ba1Fe1.772Co0.228As2	Ba	1	Fe	1.772	Co	0.228	As	2																3	2009																										AB2C2		ThCr2Si2																		K		8.52					8.52																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151576	PRB079220516	(dC/Tc) =  0.51 mJ/mol.K2	Ba(Fe,Ni)2As2	Ba1Fe1.952Ni0.048As2	Ba	1	Fe	1.952	Ni	0.048	As	2																3	2009																										AB2C2		ThCr2Si2																		K		2.39					2.39																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151577	PRB079220516	(dC/Tc) = 11.8  mJ/mol.K2	Ba(Fe,Ni)2As2	Ba1Fe1.936Ni0.064As2	Ba	1	Fe	1.936	Ni	0.064	As	2																3	2009																										AB2C2		ThCr2Si2																		K		14.6					14.6																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151578	PRB079220516	(dC/Tc) = 20.8  mJ/mol.K2	Ba(Fe,Ni)2As2	Ba1Fe1.908Ni0.092As2	Ba	1	Fe	1.908	Ni	0.092	As	2																3	2009																										AB2C2		ThCr2Si2																		K		17.8					17.8	MTC151578																																																																																															self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151579	PRB079220516	(dC/Tc) = 12.4  mJ/mol.K2	Ba(Fe,Ni)2As2	Ba1Fe1.892Ni0.108As2	Ba	1	Fe	1.892	Ni	0.108	As	2																3	2009																										AB2C2		ThCr2Si2																		K		13.9					13.9																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151580	PRB079220516	(dC/Tc) = 0.76  mJ/mol.K2	Ba(Fe,Ni)2As2	Ba1Fe1.856Ni0.144As2	Ba	1	Fe	1.856	Ni	0.144	As	2																3	2009																										AB2C2		ThCr2Si2																		K		5.1					5.1																																																																																																self-flux method					Jump in specific heat at the superconducting transition temperature in Ba(Fe1-xCox)2As2 and Ba(Fe1-xNix)2As2 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 79(2009)220516	Sergey L. Bud'ko,Ni Ni,Paul C. Canfield		
151581	PRL103097003	RRR=30. Hc2(T) measured a various P for H//a and H//c. Tm(FM) defined as kink in R(T) curves. Tc defined as R=0.5Rn. P<cr> for FM is 1.46 Gpa. (dTm/dP) = -2.4 K/GPa	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2009																										ABC		TiNiSi	Pnma																	K		0.5					0.5	MPH151581		K/Gpa	0.2																														MHC151581																																																																			Enhancement of Superconductivity near the Ferromagnetic Quantum Critical Point in UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.Lett., 103(2009)097003	E. Slooten,T. Naka,A. Gasparini,Y. K. Huang,A. de Visser		
151582	PRL100077002	RRR=30 (I//a). Ordered moment = 0.07 myuB along c-axis. anisotropy (Hc2<a>/Hc2<c>) = 10.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2008																										ABC	3	TiNiSi	Pnma																	K		0.6				0.1	0.6																				T	resistivity		5						T/K	resistivity		7.9		MHC151582																						mJ/mol.K2	57														uOhm.cm								10.2																	polycristalline made using arc-melting. single crystal obtained using Czochralski method from the melt.					Unusual Upper Critical Field of the Ferromagnetic Superconductor UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev.Lett., 100(2008)077002	N. T. Huy,D. E. de Nijs,Y. K. Huang,A. de Visser		
151583	PHC4690332	structural(tetra-to-ortho) and magnetic(para-to-AF) transition at 90 K. Mossbauer effect measured.	(Ba,K)Fe2As2	Ba0.8K0.2Fe2As2	Ba	0.8	K	0.2	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		25.3					25.3	MTC151583																																																																																																				Superconductivity, magnetism and crystal chemistry of Ba1-xKxFe2As2			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5?13 (Haus D), 81377 Munchen, Germany	Physica C, 469(2009)332	Dirk Johrendt,Rainer Pottgen		
151584	PHC4690350	RRR=8. no structural phase transition down to 0.5 K.	BaCo2As2	Ba1Co2As2	Ba	1	Co	2	As	2																			2009																										AB2C2		ThCr2Si2	I4/mmm	139																K					0.5																																																										mJ/mol.K2	41.6														mOhm,cm								0.0057				0.07													(Ba:CoAs=1:5) - heat)1180C,15h) - cool(2-4 C/h)					BaT2As2 single crystals (T = Fe, Co, Ni) and superconductivity upon Co-doping			Materials Science and Technology Division, Oak Ridge National Laboratory, 1 Bethel Valley Road, Oak Ridge, TN 37831, USA	Physica C, 469(2009)350	Athena S. Sefat,David J. Singh,Rongying Jin,Michael A. McGuire,Brian C. Sales,Filip Ronning,David Mandrus		
151585	PHC4690350		Ba(Fe,Co)2As2	Ba1Fe1.84Co0.16As2	Ba	1	Fe	1.84	Co	0.16	As	2																	2009																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9639		12.98												K			22	22		0.6	22																																																																							mOhm,cm												0.32													(Ba:FeAs:CoAs=1:4.45:0.55) - heat(1180C, 10h) - cool(4C/h)					BaT2As2 single crystals (T = Fe, Co, Ni) and superconductivity upon Co-doping			Materials Science and Technology Division, Oak Ridge National Laboratory, 1 Bethel Valley Road, Oak Ridge, TN 37831, USA	Physica C, 469(2009)350	Athena S. Sefat,David J. Singh,Rongying Jin,Michael A. McGuire,Brian C. Sales,Filip Ronning,David Mandrus		
151586	PHC4690894		LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2009																										ABCD		oxypnictide			A	4.0312		8.7371												K					1.2																																																																																																		1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151587	PHC4690894		(La,Sr)OFeAs	La0.96Sr0.04Fe1As1O1	La	0.96	Sr	0.04	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.035		8.7497												K		3.65					3.65																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151588	PHC4690894		(La,Sr)OFeAs	La0.92Sr0.08Fe1As1O1	La	0.92	Sr	0.08	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0369		8.7698												K		18.9					18.9																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151589	PHC4690894		(La,Sr)OFeAs	La0.9Sr0.1Fe1As1O1	La	0.9	Sr	0.1	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0381		8.7849												K		24.6					24.6																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151590	PHC4690894		(La,Sr)OFeAs	La0.89Sr0.11Fe1As1O1	La	0.89	Sr	0.11	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0449		8.7887												K		25.5					25.5																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151591	PHC4690894		(La,Sr)OFeAs	La0.87Sr0.13Fe1As1O1	La	0.87	Sr	0.13	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0457		8.8189												K		25.9					25.9																																																																																					E-8 m3/C	-0.067					RH151591					1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151592	PHC4690894		(La,Sr)OFeAs	La0.85Sr0.15Fe1As1O1	La	0.85	Sr	0.15	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.0385		8.7774												K		25.4					25.4																				T	resistivity	112							T/K	resistivity, G-L fitting	4.6																																																																	1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151593	PHC4690894		(La,Sr)OFeAs	La0.8Sr0.2Fe1As1O1	La	0.8	Sr	0.2	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	4.04		8.7824												K		24.9					24.9																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151594	PHC4690894		PrOFeAs	Pr1Fe1As1O1	Pr	1	Fe	1	As	1															O	1			2009																										ABCD		oxypnictide			A	3.9831		8.6163												K					1.2																																																																																																		1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151595	PHC4690894		(Pr,Sr)OFeAs	Pr0.95Sr0.05Fe1As1O1	Pr	0.95	Sr	0.05	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9846		8.6226												K		4.86					4.86																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151596	PHC4690894		(Pr,Sr)OFeAs	Pr0.9Sr0.1Fe1As1O1	Pr	0.9	Sr	0.1	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9899		8.6402												K		12.8					12.8																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151597	PHC4690894		(Pr,Sr)OFeAs	Pr0.85Sr0.15Fe1As1O1	Pr	0.85	Sr	0.15	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9919		8.6516												K		15.5					15.5																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151599	PHC4690894		(Pr,Sr)OFeAs	Pr0.75Sr0.25Fe1As1O1	Pr	0.75	Sr	0.25	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9968		8.6591												K		16.2					16.2																				T	resistivity	52							T/K	resistivity, G-L fitting	4																																																						E-8 m3/C	-0.067					RH151599					1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151600	PRB080100503	P-induced SC. optimal-P(for Tc) = 3.8 GPa. P-dependence of NMR investigated. spin gap(D) plotted in figure (degree unit).	Sr2Ca12Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2009																										A2B3C5		LAD																		K	8.8		9.7		0		9.25	TC151600																																																																																																				NMR and NQR study of pressure-induced superconductivity and the origin of critical-temperature enhancement in the spin-ladder cuprate Sr2Ca12Cu24O41			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 80(2009)100503	N. Fujiwara,Y. Fujimaki,S. Uchida,K. Matsubayashi,T. Matsumoto,Y. Uwatoko		
151601	PRB080100502		Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2009																										A2B3C5		Sc2Fe3Si5																		K	6.1	6.15					6.15																																																																							uOhm.cm								22	7																floating zone method					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151602	PRB080100502		Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		1	2009																										A2B3C5		Sc2Fe3Si5																		K		5.85		5.85			5.85																																																																							uOhm.cm							30																							Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151603	PRB080100502		(Lu,Y)2Fe3Si5	Lu1.9Y0.1Fe3Si5	Lu	1.9	Y	0.1	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K		4.16		4.19			4.16																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151604	PRB080100502		(Lu,Sc)2Fe3Si5	Lu1.86Sc0.14Fe3Si5	Lu	1.86	Sc	0.14	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K		3.51		3.6			3.51																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151605	PRB080100502		(Lu,Dy)2Fe3Si5	Lu1.94Dy0.06Fe3Si5	Lu	1.94	Dy	0.06	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K	4.4	4.52		4.38			4.52																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151606	PRB080100502		(Lu,Dy)2Fe3Si5	Lu1.9Dy0.1Fe3Si5	Lu	1.9	Dy	0.1	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K				3.77			3.77																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151607	PRB080100502		(Lu,Sc)2Fe3Si5	Lu1.94Sc0.06Fe3Si5	Lu	1.94	Sc	0.06	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K		4.83					4.83																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151608	PRB080100502		(Lu,Sc)2Fe3Si5	Lu1.9Sc0.1Fe3Si5	Lu	1.9	Sc	0.1	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K		4.33					4.33																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151609	PRB080100502		(Lu,Y)2Fe3Si5	Lu1.86Y0.14Fe3Si5	Lu	1.86	Y	0.14	Fe	3	Si	5																1	2009																										A2B3C5		Sc2Fe3Si5																		K		3.51					3.51																																																																																																					Disorder-sensitive superconductivity in the doped iron silicide superconductor (Lu1-xRx)2Fe3Si5 (R=Sc, Y, and Dy)			Department of Physics, College of Science and Technology (CST), Nihon University, Chiyoda-ku, Tokyo 101-8308, Japan	Phys.Rev.B, 80(2009)100502	Tadataka Watanabe,Hiroki Sasame,Hiroaki Okuyama,Kouichi Takase,Yoshiki Takano		
151610	PHC4691921		SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																			2009																										AB2C2		ThCr2Si2			A	3.9207		12.3592												K					2																																																																																																Sr,Fe,Ru,As		mixture - sealed(Nb-tube) - heat(850C,35h) - cool to RT					Superconductivity induced by doping Ru in SrFe2-xRuxAs2			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Physica C, 469(2009)1921	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Yanwei Ma		
151611	PHC4691921		Sr(Fe,Ru)2As2	Sr1Fe1.7Ru0.3As2	Sr	1	Fe	1.7	Ru	0.3	As	2																	2009																										AB2C2		ThCr2Si2			A	3.9355		12.309												K					2																																																																																																Sr,Fe,Ru,As		mixture - sealed(Nb-tube) - heat(850C,35h) - cool to RT					Superconductivity induced by doping Ru in SrFe2-xRuxAs2			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Physica C, 469(2009)1921	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Yanwei Ma		
151612	PHC4691921	R not to zero at 2K.	Sr(Fe,Ru)2As2	Sr1Fe1.5Ru0.5As2	Sr	1	Fe	1.5	Ru	0.5	As	2																	2009																										AB2C2		ThCr2Si2			A	3.9551		12.196												K			13.5				13.5																																																																																														Sr,Fe,Ru,As		mixture - sealed(Nb-tube) - heat(850C,35h) - cool to RT					Superconductivity induced by doping Ru in SrFe2-xRuxAs2			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Physica C, 469(2009)1921	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Yanwei Ma		
151613	PHC4691921		Sr(Fe,Ru)2As2	Sr1Fe1.3Ru0.7As2	Sr	1	Fe	1.3	Ru	0.7	As	2																	2009																										AB2C2		ThCr2Si2			A	3.9709		12.093												K			13.5			5	13.5																																																																																														Sr,Fe,Ru,As		mixture - sealed(Nb-tube) - heat(850C,35h) - cool to RT					Superconductivity induced by doping Ru in SrFe2-xRuxAs2			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P.O. Box 2703, Beijing 100190, China	Physica C, 469(2009)1921	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Yanwei Ma		
151614	CAL0330027	not SC. small diamag-signal maybe from Bi-film on the surface.	beta-RhBi2	Bi2Rh1	Bi	2	Rh	1																				3	2009																										AB2			P1[-]		A	6.728	7.022	7.0655											alpha=104.916, beta-100.82, gamma=105.583 degree.	K					1.8																																																																																																		Bi-flux method					Phase relationship and superconductivity in the Bi-rich part of the binary system Rh-Bi			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	CALPHAD:phase diagram, 33(2009)27	Franz Weitzer,Walter Schnelle,Raul Cardoso Gil,Stefan Hoffmann,Rainer Giedigkeit,Yuri Grin		
151615	CAL0330027		RhBi4	Bi4Rh1	Bi	4	Rh	1																				3	2009																										AB4			Ia3[-]d		A	14.9304														K				3.15			3.15																																																																																																Bi-flux method					Phase relationship and superconductivity in the Bi-rich part of the binary system Rh-Bi			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	CALPHAD:phase diagram, 33(2009)27	Franz Weitzer,Walter Schnelle,Raul Cardoso Gil,Stefan Hoffmann,Rainer Giedigkeit,Yuri Grin		
151616	CAL0330027		Rh3Bi4	Bi14Rh3	Bi	14	Rh	3																				3	2009																										A3B14			Fddd		A	6.9041	17.3816	31.752												K				2.85			2.85																																																																																																Bi-flux method					Phase relationship and superconductivity in the Bi-rich part of the binary system Rh-Bi			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	CALPHAD:phase diagram, 33(2009)27	Franz Weitzer,Walter Schnelle,Raul Cardoso Gil,Stefan Hoffmann,Rainer Giedigkeit,Yuri Grin		
151617	CAL0330027	small Meissner effect	RhBi3	Bi3Rh1	Bi	3	Rh	1																				3	2009																										AB3			Pnma		A	8.8761	4.242	11.3627												K				3.15			3.15																																																																																																Bi-flux method					Phase relationship and superconductivity in the Bi-rich part of the binary system Rh-Bi			Max-Planck-Institut fur Chemische Physik fester Stoffe, Dresden, Germany	CALPHAD:phase diagram, 33(2009)27	Franz Weitzer,Walter Schnelle,Raul Cardoso Gil,Stefan Hoffmann,Rainer Giedigkeit,Yuri Grin		
151618	JPS078085001	RRR = 3. (dC/gamma*Tc) = 1.0. lattice term coeff.(beta) = 1.2 mJ/mol.K4. Hc2 defined as R=zero. H// means b-axis. H/n means a-axis. For H//c[001], Hc2(0)=0.35T, -(dHc2/dT)=0.32 T/K, cohere=260A	Ca2Pt3Sig	Ca2Pt3Si5	Ca	2	Pt	3	Si	5																		3	2009																										A2B3C5	3	U2Co3Si5	Ibam	72	A	10.0676	11.5465	5.9237												K		1.3				0.1	1.3																				T	resistivity		0.5	0.35					T/K			0.44	0.23	MHC151618		A			370	260																mJ/mol.K2	9.4	SP-heat	253	SP-heat											uOhm.cm								19																	Sn-flux method. Ca:Pt:Si:Sn = 1:1:3:20					Superconductivity in a Ternary Silicide Ca2Pt3Si5			Low Temperature Center, Osaka University, Toyonaka, Osaka 560-0043, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 78(2009)085001	Tetsuya TAKEUCHI,Hiroshi MURANAKA,Rikio SETTAI,Tatsuma D. MATSUDA,Etsuji YAMAMOTO,Yoshinori HAGA,Yoshichika ONUKI		
151619	JPS078084710	Tc defined from ac-SUS.	FeSe0.88	Fe1Se0.88	Fe	1	Se	0.88																					2009																										AB																				K				8.69			8.69	MTC151619		K/GPa	0.836																																																																																												solid state reaction					Pressure Effects on Superconductivity and Magnetism in FeSe1-xTex			Department of Physics, Center for Nanoscience and Nanotechnology, National Sun Yat-Sen University, Kaohsiung 804, Taiwan	J.Phys.Soc.Jpn, 78(2009)084710	Chien-Lung HUANG,Chih-Chieh CHOU,Kuo-Feng TSENG,Yi-Lin HUANG,Fong-Chi HSU,Kuo-Wei YEH,Mau-Kuen WU,Hung-Duen YANG		
151620	JPS078084710	Tc defined from ac-SUS.	FeSe0.5Te0.5	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																			2009																										AB																				K				8.47			8.47	MTC151620		K/GPa	14.7																																																																																												solid state reaction					Pressure Effects on Superconductivity and Magnetism in FeSe1-xTex			Department of Physics, Center for Nanoscience and Nanotechnology, National Sun Yat-Sen University, Kaohsiung 804, Taiwan	J.Phys.Soc.Jpn, 78(2009)084710	Chien-Lung HUANG,Chih-Chieh CHOU,Kuo-Feng TSENG,Yi-Lin HUANG,Fong-Chi HSU,Kuo-Wei YEH,Mau-Kuen WU,Hung-Duen YANG		
151621	PRL089166402	Pressure by miniature saphire anvil cell(Ar). Shubnikov-deHaas effect measured.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												Sr2RuO4																		K		1.5					1.5	TC151621		K/GPa	0.216																																																																																												floating zone method					Evolution of Fermi-Liquid Interactions in Sr2RuO4 under Pressure			Cavendish Laboratory, University of Cambridge, Madingley Road, Cambridge CB3 OHE, United Kingdom	Phys.Rev.Lett., 89(2002)166402	D. Forsythe,S. R. Julian,C. Bergemann,E. Pugh,M. J. Steiner,P. L. Alireza,G. J. McMullan,F. Nakamura,R. K.W. Haselwimmer,I. R.Walker,S. S. Saxena,G. G. Lonzarich,A. P. Mackenzie,Z.Q. Mao,Y. Maeno		
151622	PRB0567890	platelike(1.5*0.6*0.04 mm3). hydrastatic pressure.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	1997																												Sr2RuO4																		K	0.77	0.9	0.91				0.9	TC151622		K/GPa	0.3																																																							410																																					floating zone method					Pressure dependence of superconducting critical temperature of Sr2RuO4			Electrotechnical Laboratory, Tsukuba 305, Japan	Phys.Rev.B, 56(1997)7890	Naoki Shirakawa,Keizo Murata,Shuji Nishizaki,Yoshiteru Maeno,Toshizo Fujita		
151623	JPS078063705	P using cubic anvil, nearly hydrostatic. Tc(max) = 26.2 K at P=2 GPa. For P>2 GPa, dTc/dP = -2.8 K/GPa.	Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																			2009																										AB																				K	12.5		13.5				13	MTC151623		K/GPa	7.4																																																																																												solid state reaction					First Investigation of Pressure Effects on Transition from Superconductive to Metallic Phase in FeSe0.5Te0.5			WPI-AIMR, Tohoku University, Sendai 980-8577	J.Phys.Soc.Jpn, 78(2009)063705	Kazumasa HORIGANE,Nao TAKESHITA,Chul-Ho LEE,Haruhiro HIRAKA,Kazuyoshi YAMADA		
151624	JPS078063705		Fe(Se,Te)	Fe1Se0.38Te0.62	Fe	1	Se	0.38	Te	0.62																			2009																										AB																				K			13.5				13.5																																																																																																solid state reaction					First Investigation of Pressure Effects on Transition from Superconductive to Metallic Phase in FeSe0.5Te0.5			WPI-AIMR, Tohoku University, Sendai 980-8577	J.Phys.Soc.Jpn, 78(2009)063705	Kazumasa HORIGANE,Nao TAKESHITA,Chul-Ho LEE,Haruhiro HIRAKA,Kazuyoshi YAMADA		
151625	JPS078063705		Fe(Se,Te)	Fe1Se0.25Te0.75	Fe	1	Se	0.25	Te	0.75																			2009																										AB																				K			12				12																																																																																																solid state reaction					First Investigation of Pressure Effects on Transition from Superconductive to Metallic Phase in FeSe0.5Te0.5			WPI-AIMR, Tohoku University, Sendai 980-8577	J.Phys.Soc.Jpn, 78(2009)063705	Kazumasa HORIGANE,Nao TAKESHITA,Chul-Ho LEE,Haruhiro HIRAKA,Kazuyoshi YAMADA		
151626	JPS078063705		Fe(Se,Te)	Fe1Se0.13Te0.87	Fe	1	Se	0.13	Te	0.87																			2009																										AB																				K			6				6																																																																																																solid state reaction					First Investigation of Pressure Effects on Transition from Superconductive to Metallic Phase in FeSe0.5Te0.5			WPI-AIMR, Tohoku University, Sendai 980-8577	J.Phys.Soc.Jpn, 78(2009)063705	Kazumasa HORIGANE,Nao TAKESHITA,Chul-Ho LEE,Haruhiro HIRAKA,Kazuyoshi YAMADA		
151627	EPL08627001	impurity: alpha-FeSe(NiAs-type). tetra-to-ortho(space-G=Pbnm) transition at 12.5 GPa. SDW temperature T* = 125 K(P=0).	beta-FeSe	Fe1Se1	Fe	1	Se	1																					2009																		GPa		28.9						AB		PbO	P4/nmm		A	3.7699		5.5184												K		8.5					8.5	MTC151627		K/GPa	3.2																																																																																										Fe(4N),Se(5N)		Fe:Se=1:0.82, mixture - sealed in quartz tube - heat(700C,48h)					High-temperature superconductivity (Tc onset at 34 K) in the high-pressure orthorhombic phase of FeSe			European Synchrotron Radiation Facility (ESRF) - 6 Rue Jules Horowitz, BP 220, F-38043 Grenoble Cedex, France, EU	Euro.Phys.Lett., 86(2009)27001	G. Garbarino,A. Sow,P. Lejay,A. Sulpice,P. Toulemonde,M. Mezouar,M. Nunez-Regueiro		
151628	PRB080092502	Annealed sample. compositions and homogeneity measured by EDX analysis. Jc(5K,0 T) = 1 E+5 A/cm2 using Bean model.	Fe(Se,Te)	Fe1Se0.39Te0.61	Fe	1	Se	0.39	Te	0.61																		3	2009																										AB					A	3.798		6.052												K				14			14																																																																							mOhm.cm												0.4													nominal(FeSe0.5Te0.5) - sealed in silica tube - heat to 710 C(6C/h) - cool to RT - ANN(400C,10d) - Quench					Superconductivity at Tc = 14 K in single-crystalline FeTe0.61Se0.39			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 80(2009)092502	T. Taen,Y. Tsuchiya,Y. Nakajima,T. Tamegai		
151629	SSI1010009	(MX)n(TX2)m compounds.  periodic length = 24.306 A.	(BiSe)xTaSe2	Bi1.09Ta1Se3.09	Bi	1.09	Ta	1	Se	3.09																			1997																										ABC2																				K			1.8				1.8																																																																																																(BiSe)1.09(TaSe2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,12h + 800C,24h) - crush - heat(500-900C) - Q to water					Preparation, characterization and intercalation of ternary chalcogenides with layered composite crystal structures formed in the Bi-Ta-S and Bi-Ta-Se systems			National Institute of Materials and Chemical Research, Higashi,Tsukuba,Ibaraki,Japan	Solid State Ionics, 101-103(1997)9	Y.Oosawa,Y.Gotoh,J.Akimoto,M.Sohma,T.Tsunoda,H.Hayakawa,M.Onoda		
151630	SSI1010009	(MX)n(TX2)m compounds. periodic length = 18.445 A	(BiSe)x(TaSe2)2	Bi1.09Ta2Se5.09	Bi	1.09	Ta	2	Se	5.09																			1997																										AB2C4																				K			1.8				1.8																																																																																																(BiSe)1.09(TaSe2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,12h + 800C,24h) - crush - heat(500-900C) - Q to water					Preparation, characterization and intercalation of ternary chalcogenides with layered composite crystal structures formed in the Bi-Ta-S and Bi-Ta-Se systems			National Institute of Materials and Chemical Research, Higashi,Tsukuba,Ibaraki,Japan	Solid State Ionics, 101-103(1997)9	Y.Oosawa,Y.Gotoh,J.Akimoto,M.Sohma,T.Tsunoda,H.Hayakawa,M.Onoda		
151631	SSI1010009	(MX)n(TX2)m compounds	(BiS)xTaS2	Bi1.09Ta1S3.09	Bi	1.09	Ta	1	S	3.09																			1997																										ABC2																				K					1.5																																																																																																		(BiS)1.08(TaS2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,12h + 800C,24h) - crush - heat(500-900C) - Q to water					Preparation, characterization and intercalation of ternary chalcogenides with layered composite crystal structures formed in the Bi-Ta-S and Bi-Ta-Se systems			National Institute of Materials and Chemical Research, Higashi,Tsukuba,Ibaraki,Japan	Solid State Ionics, 101-103(1997)9	Y.Oosawa,Y.Gotoh,J.Akimoto,M.Sohma,T.Tsunoda,H.Hayakawa,M.Onoda		
151632	SSI1010009	(MX)n(TX2)m compounds	(BiS)x(TaS2)2	Bi1.09Ta2S5.09	Bi	1.09	Ta	2	S	5.09																			1997																										AB2C4																				K	2.5		2.8				2.65																																																																																																(BiS)1.08(TaS2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,12h + 800C,24h) - crush - heat(500-900C) - Q to water					Preparation, characterization and intercalation of ternary chalcogenides with layered composite crystal structures formed in the Bi-Ta-S and Bi-Ta-Se systems			National Institute of Materials and Chemical Research, Higashi,Tsukuba,Ibaraki,Japan	Solid State Ionics, 101-103(1997)9	Y.Oosawa,Y.Gotoh,J.Akimoto,M.Sohma,T.Tsunoda,H.Hayakawa,M.Onoda		
151633	JJP031L1096	(MX)n(TX2)m compounds	(Pb,Se)x(NbSe2)2	Pb1.14Nb2Se5.14	Pb	1.14	Nb	2	Se	5.14																			1992																										AB2C4																				K	3.4						3.4																																																																																														Pb(3N),Nb(2N),Se(3N)		(PbSe)1.09(NbSe2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,48h) - crush - heat(500-900C) - Q to water					Three types of ternary selenides with layered composite crystal structures formed in the Pb-Nb-Se system			National Chemical Laboratory for Industry, Higashi, Tsukuba, Ibaraki,Japan	Jpn.J.Appl.Phys., 31(1992)L1096	Y.Oosawa,Y.Gotoh,J.Akimoto,T.Tsunoda,M.Sohma,M.Onoda		
151634	JJP031L1096	(MX)n(TX2)m compounds	(Pb,Se)x(NbSe2)3	Pb1.14Nb3Se7.14	Pb	1.14	Nb	3	Se	7.14																			1992																										AB3C6																				K	4.8						4.8																																																																																														Pb(3N),Nb(2N),Se(3N)		(PbSe)1.09(NbSe2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,48h) - crush - heat(500-900C) - Q to water					Three types of ternary selenides with layered composite crystal structures formed in the Pb-Nb-Se system			National Chemical Laboratory for Industry, Higashi, Tsukuba, Ibaraki,Japan	Jpn.J.Appl.Phys., 31(1992)L1096	Y.Oosawa,Y.Gotoh,J.Akimoto,T.Tsunoda,M.Sohma,M.Onoda		
151635	JJP031L1096	(MX)n(TX2)m compounds. R starts to decrease at 2.0 K.	(Pb,Se)xNbSe2	Pb1.14Nb1Se3.14	Pb	1.14	Nb	1	Se	3.14																			1992																										ABC2																				K					2																																																																																																Pb(3N),Nb(2N),Se(3N)		(PbSe)1.09(NbSe2)m: m=1,2,3,  mixture - sealed in silica tube - heat(500C,48h) - crush - heat(500-900C) - Q to water					Three types of ternary selenides with layered composite crystal structures formed in the Pb-Nb-Se system			National Chemical Laboratory for Industry, Higashi, Tsukuba, Ibaraki,Japan	Jpn.J.Appl.Phys., 31(1992)L1096	Y.Oosawa,Y.Gotoh,J.Akimoto,T.Tsunoda,M.Sohma,M.Onoda		
151636	PRB080134523	anisotropic thermal expansion coeff. negative sign for <ab> and positive for <c> direction.	Fe(Te,Se)	Fe1.06Te0.5Se0.5	Fe	1.06	Te	0.5	Se	0.5																		3	2009																										AB																				K			14				14			K/GPa	-5.4																																																																																												Bridgman method					Anisotropic thermal expansion of Fe1.06Te and FeTe0.5Se0.5 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)134523	S. L. Bud'ko,P. C. Canfield,A. S. Sefat,B. C. Sales,M. A. McGuire,D. Mandrus		
151637	PRB080134523	not SC. tetra(H) to monocl(L) structural transition. anisotropic thermal expansion coeff. negative sign for <ab> and positive for <c> direction.	FeTe	Fe1.06Te1	Fe	1.06	Te	1																				3	2009																										AB																				K					2																																																										mJ/mol.K2	34																																							Bridgman method					Anisotropic thermal expansion of Fe1.06Te and FeTe0.5Se0.5 single crystals			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 80(2009)134523	S. L. Bud'ko,P. C. Canfield,A. S. Sefat,B. C. Sales,M. A. McGuire,D. Mandrus		
151638	PRB080140513	H//c-axis. Tc(max) = 0.63 K at P=0.4 GPa. Two SC regions (SC1 for low-P and SC2 for high-P region). (dC/[gamma]*Tc) for SC1 is larger than that of SC2.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2009																										AB2C2		ThCr2Si2			A	4.099		9.923												K		0.46					0.46	MTC151638																			T	SP-heat													MHC151638																																					mOhm.cm							0.01																		modified Bridgman method in Al-oxide crucible using Cu excess flux					Pressure-induced change of the pairing symmetry in superconducting CeCu2Si2			Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany	Phys.Rev.B, 80(2009)140513	E. Lengyel,M. Nicklas,H. S. Jeevan,G. Sparn,C. Geibel,F. Steglich,Y. Yoshioka,K. Miyake		
151639	PRB080144512	RRR = 4.5. Hc2(0)//c and Hc2(0)//ab obtained using two band theory and WHH theory, respectively. anisotropy(Hc2) = 3 for low-T.	SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85			2009																										ABCD		oxypnictide																	ZrCuSiAs type	K			50.5			0.5	50.5																				T	resistivity		150	110					T/K	resistivity		11	2.5	HC151639		A			17	3.6																																																								two-step solid state reaction. mixture - pellet(0.38GPa) - wrapped in Ta foil - heat(1150C,50h, in sealed quartz tube(Ar))					Effects of two gaps and paramagnetic pair breaking on the upper critical field of SmFeAsO0.85 and SmFeAsO0.8F0.2 single crystals			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B, 80(2009)144512	Hyun-Sook Lee,Marek Bartkowiak,Jae-Hyun Park,Jae-Yeap Lee,Ju-Young Kim,Nak-Heon Sung,B. K. Cho,Chang-Uk Jung,Jun Sung Kim,Hu-Jong Lee		
151640	PRB080144512	RRR = 2.2. Hc2(0)//c and Hc2(0)//ab obtained using two band theory and WHH theory, respectively. anisotropy(Hc2) = 4 for low T.	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8			2009																										ABCD		oxypnictide																	ZrCuSiAs type	K			42			0.8	42																				T	resistivity		100	50					T/K	resistivity		9.9	1.7	HC151640		A			26	3.6																																																								two-step solid state reaction. mixture - pellet(0.38GPa) - wrapped in Ta foil - heat(1150C,50h, in sealed quartz tube(Ar))					Effects of two gaps and paramagnetic pair breaking on the upper critical field of SmFeAsO0.85 and SmFeAsO0.8F0.2 single crystals			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea	Phys.Rev.B, 80(2009)144512	Hyun-Sook Lee,Marek Bartkowiak,Jae-Hyun Park,Jae-Yeap Lee,Ju-Young Kim,Nak-Heon Sung,B. K. Cho,Chang-Uk Jung,Jun Sung Kim,Hu-Jong Lee		
151641	PRB080144517	not SC.  structural transition(P4nmm-to-Cmma) at 150 K. T<SDW> = 105 K. F-content by WDS (not nominal).	Pr(O,F)FeAs	Pr1Fe1As1F0.044O0.956	Pr	1	Fe	1	As	1	F	0.044													O	0.956		1	2009																										ABCD		oxypnictide																	ZrCuSiAs type	K					1.5																																																																																																							Phase diagram of the PrFeAsO1-xFx superconductor			Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA	Phys.Rev.B, 80(2009)144517	C. R. Rotundu,D. T. Keane,B. Freelon,S. D. Wilson,A. Kim,P. N. Valdivia,E. Bourret-Courchesne,R. J. Birgeneau		
151642	PRB080144517	F-content by WDS (not nominal).	Pr(O,F)FeAs	Pr1Fe1As1F0.082O0.918	Pr	1	Fe	1	As	1	F	0.082													O	0.918		1	2009																										ABCD		oxypnictide																	ZrCuSiAs type	K			14.6				14.6	PH151642																																																																																																				Phase diagram of the PrFeAsO1-xFx superconductor			Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA	Phys.Rev.B, 80(2009)144517	C. R. Rotundu,D. T. Keane,B. Freelon,S. D. Wilson,A. Kim,P. N. Valdivia,E. Bourret-Courchesne,R. J. Birgeneau		
151643	PRB080144517	F-content by WDS (not nominal).	Pr(O,F)FeAs	Pr1Fe1As1F0.154O0.846	Pr	1	Fe	1	As	1	F	0.154													O	0.846		1	2009																										ABCD		oxypnictide																	ZrCuSiAs type	K			46.4				46.4	PH151642																																																																																																				Phase diagram of the PrFeAsO1-xFx superconductor			Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA	Phys.Rev.B, 80(2009)144517	C. R. Rotundu,D. T. Keane,B. Freelon,S. D. Wilson,A. Kim,P. N. Valdivia,E. Bourret-Courchesne,R. J. Birgeneau		
151644	PRB080144517	F-content by WDS (not nominal).	Pr(O,F)FeAs	Pr1Fe1As1F0.225O0.775	Pr	1	Fe	1	As	1	F	0.225													O	0.775		1	2009																										ABCD		oxypnictide																	ZrCuSiAs type	K			50				50	PH151642																																																																																																				Phase diagram of the PrFeAsO1-xFx superconductor			Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA	Phys.Rev.B, 80(2009)144517	C. R. Rotundu,D. T. Keane,B. Freelon,S. D. Wilson,A. Kim,P. N. Valdivia,E. Bourret-Courchesne,R. J. Birgeneau		
151645	JPS078113701	Hc2(0) = 95.9 T using WHH fitting from (dHc2/dT) at Tc. Tc defined as midpoint. Hc2  measured for  Tc(on) and Tc(zero) definitions.	Fe(Se,Te)	Fe1Se0.25Te0.75	Fe	1	Se	0.25	Te	0.75																		1	2009																										AB		PbO	P4/nmm																	K	13.2	13.7	14.2				13.7																				T	resistivity, extraporation	45							T/K	resistivity	10.1			MHC151645																																																														solid state reaction					Upper Critical Fields of the 11-System Iron-Chalcogenide Superconductor FeSe0.25Te0.75			KYOKUGEN, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531	J.Phys.Soc.Jpn, 78(2009)113701	Takanori KIDA,Takahiro MATSUNAGA,Masayuki HAGIWARA,Yoshikazu MIZUGUCHI,Yoshihiko TAKANO,Koichi KINDO		
151646	JPS078114707		(La,Sr)2CuO4	La1.943Sr0.057Cu1O4	La	1.943	Sr	0.057	Cu	1															O	4		3	2009																												T																		K				4.51			4.51	TC151648																																																							mJ/mol.K2	4.473																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151647	JPS078114707		(La,Sr)2CuO4	La1.943Sr0.076Cu1O4	La	1.943	Sr	0.076	Cu	1															O	4		3	2009																												T																		K				16.5			16.5																																																								mJ/mol.K2	3.53																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151648	JPS078114707		(La,Sr)2CuO4	La1.943Sr0.089Cu1O4	La	1.943	Sr	0.089	Cu	1															O	4		3	2009																												T																		K				24.6			24.6	TC151648																																																				SP151648			mJ/mol.K2	2.79																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151649	JPS078114707		(La,Sr)2CuO4	La1.943Sr0.115Cu1O4	La	1.943	Sr	0.115	Cu	1															O	4		3	2009																												T																		K				24.9			24.9	TC151648																																																				SP151648			mJ/mol.K2	1.648																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151650	JPS078114707		(La,Sr)2CuO4	La1.943Sr0.13Cu1O4	La	1.943	Sr	0.13	Cu	1															O	4		3	2009																												T																		K				33.3			33.3	TC151648																																																				SP151648			mJ/mol.K2	1.951																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151651	JPS078114707	[gamma] ratio of single and poly is minimum value(=0.15)	(La,Sr)2CuO4	La1.943Sr0.178Cu1O4	La	1.943	Sr	0.178	Cu	1															O	4		3	2009																												T																		K				34.3			34.3																																																								mJ/mol.K2	1.917																																							four crystal rods(0.04<x<0.10, 0.09<x<0.15, 0.11<x<0.16, 0.14<x<0.18) were grown at a rate of 0.7 mm/h in feed rod preparation. ANN(900C,50h) - cool to RT(8C/h)					Magnetic-Susceptibility and Specific-Heat Studies on the Inhomogeneity of Superconductivity in the Underdoped La2-xSrxCuO4			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579	J.Phys.Soc.Jpn, 78(2009)114707	Tadashi ADACHI,Keisuke OMORI,Yoichi TANABE,Yoji KOIKE		
151652	PHC2330395		(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		1	1994																												T																		K				31.8			31.8	TC151652																																																				SP151652			mJ/mol.K2	5.25																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151653	PHC2330395		(La,Sr)2CuO4	La1.885Sr0.115Cu1O4	La	1.885	Sr	0.115	Cu	1															O	4		1	1994																												T																		K				29.3			29.3																																																								mJ/mol.K2	3.81																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151654	PHC2330395		(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		1	1994																												T																		K				39			39																																																								mJ/mol.K2	10.9																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151655	PHC2330395		(La,Sr)2CuO4	La1.8Sr0.2Cu1O4	La	1.8	Sr	0.2	Cu	1															O	4		1	1994																												T																		K				30.6			30.6																																																								mJ/mol.K2	13.8																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151656	PHC2330395		(La,Sr)2CuO4	La1.74Sr0.26Cu1O4	La	1.74	Sr	0.26	Cu	1															O	4		1	1994																												T																		K				6.4			6.4																																																								mJ/mol.K2	11.7																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151657	PHC2330395	not SC. Zn substitutes for Cu successfully (from T-O transition temperature)	(La,Sr)2(Cu,Zn)O4	La1.9Sr0.1Cu0.98Zn0.02O4	La	1.9	Sr	0.1	Cu	0.98	Zn	0.02													O	4		1	1994																												T																		K					1																																																										mJ/mol.K2	5.89																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151658	PHC2330395	Zn substitutes for Cu successfully (from T-O transition temperature)	(La,Sr)2(Cu,Zn)O4	La1.84Sr0.16Cu0.985Zn0.015O4	La	1.84	Sr	0.16	Cu	0.985	Zn	0.015													O	4		1	1994																												T																		K				21.8			21.8																																																								mJ/mol.K2	6.39																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151659	PHC2330395	Zn substitutes for Cu successfully (from T-O transition temperature)	(La,Sr)2(Cu,Zn)O4	La1.82Sr0.18Cu0.98Zn0.02O4	La	1.82	Sr	0.18	Cu	0.98	Zn	0.02													O	4		1	1994																												T																		K				17.9			17.9																																																								mJ/mol.K2	7.64																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151660	PHC2330395	Zn substitutes for Cu successfully (from T-O transition temperature)	(La,Sr)2(Cu,Zn)O4	La1.78Sr0.22Cu0.98Zn0.02O4	La	1.78	Sr	0.22	Cu	0.98	Zn	0.02													O	4		1	1994																												T																		K				9.51			9.51																																																								mJ/mol.K2	10.2																																							SIN(1030-1070C,48h)  - ANN(600C,24h) - slow cool to RT					Low-temperature electronic specific heat of La2-xSrxCuO4 and La2-xSrxCu1-yZnyO4.  Evidence for a d wave superconductor	199411			Physica C.233(1994) 395-401	K.Yamaya,M.Ido,M.Oda,N.Momono,T.Nakano,Y.Okajima	La,Sr.Cu.Zn,O	
151661	PRB076064512	[gamma] shows gamma(H=0)	(La,Sr)2CuO4	La1.822Sr0.178Cu1O4	La	1.822	Sr	0.178	Cu	1															O	4		3	2007																												T																		K				36			36																																														meV	8.94	5.84	14							mJ/mol.K2	1.485																																												Weak-coupling d-wave BCS superconductivity and unpaired electrons in overdoped La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 76(2007)064512	Yue Wang,Jing Yan,Lei Shan,Hai-Hu Wen,Yoichi Tanabe,Tadashi Adachi,Yoji Koike		
151662	PRB076064512	[gamma] shows gamma(H=0)	(La,Sr)2CuO4	La1.798Sr0.202Cu1O4	La	1.798	Sr	0.202	Cu	1															O	4		3	2007																												T																		K				30.5			30.5																																														meV	6.28	4.824	14							mJ/mol.K2	2.079																																												Weak-coupling d-wave BCS superconductivity and unpaired electrons in overdoped La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 76(2007)064512	Yue Wang,Jing Yan,Lei Shan,Hai-Hu Wen,Yoichi Tanabe,Tadashi Adachi,Yoji Koike		
151663	PRB076064512	[gamma] shows gamma(H=0)	(La,Sr)2CuO4	La1.782Sr0.218Cu1O4	La	1.782	Sr	0.218	Cu	1															O	4		3	2007																												T																		K				25			25																																														meV	5.425	4.952	14							mJ/mol.K2	3.416																																												Weak-coupling d-wave BCS superconductivity and unpaired electrons in overdoped La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 76(2007)064512	Yue Wang,Jing Yan,Lei Shan,Hai-Hu Wen,Yoichi Tanabe,Tadashi Adachi,Yoji Koike		
151664	PRB076064512	[gamma] shows gamma(H=0)	(La,Sr)2CuO4	La1.762Sr0.238Cu1O4	La	1.762	Sr	0.238	Cu	1															O	4		3	2007																												T																		K				19.5			19.5																																														meV	3.404	4.308	14							mJ/mol.K2	8.578																																												Weak-coupling d-wave BCS superconductivity and unpaired electrons in overdoped La2-xSrxCuO4 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100080, People's Republic of China	Phys.Rev.B, 76(2007)064512	Yue Wang,Jing Yan,Lei Shan,Hai-Hu Wen,Yoichi Tanabe,Tadashi Adachi,Yoji Koike		
151665	PRB080144524	Ni-content shows actual value from EPMA. J//ab. no SDW. optimum doping in this series.	Ca(Fe,Ni)2As2	Ca1Fe1.94Ni0.06As2	Ca	1	Fe	1.94	Ni	0.06	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.892		11.732												K			15				15										75										T	resistivity, WHH			14					T/K	resistivity, WHH			1.3	MHC151665																																																														single crystals grown by Sn-flux method					Evolution of the bulk properties, structure, magnetic order, and superconductivity with Ni doping in CaFe2-xNixAs2			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 80(2009)144524	Neeraj Kumar,Songxue Chi,Ying Chen,Kumari Gaurav Rana,A. K. Nigam,A. Thamizhavel,William Ratcliff II,S. K. Dhar,Jeffrey W. Lynn		
151666	PRB080144524	T<SDW> = 172 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2			A	3.8852		11.764												K					2																																																																																																		single crystals grown by Sn-flux method					Evolution of the bulk properties, structure, magnetic order, and superconductivity with Ni doping in CaFe2-xNixAs2			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 80(2009)144524	Neeraj Kumar,Songxue Chi,Ying Chen,Kumari Gaurav Rana,A. K. Nigam,A. Thamizhavel,William Ratcliff II,S. K. Dhar,Jeffrey W. Lynn		
151667	PRB080144524	Ni-content shows actual value from EPMA. T<SDW> = 129 K. Filamentary SC appears at 15 K. R not to zero.	Ca(Fe,Ni)2As2	Ca1Fe1.973Ni0.027As2	Ca	1	Fe	1.973	Ni	0.027	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.8912		11.743												K					2																																																																																																		single crystals grown by Sn-flux method					Evolution of the bulk properties, structure, magnetic order, and superconductivity with Ni doping in CaFe2-xNixAs2			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 80(2009)144524	Neeraj Kumar,Songxue Chi,Ying Chen,Kumari Gaurav Rana,A. K. Nigam,A. Thamizhavel,William Ratcliff II,S. K. Dhar,Jeffrey W. Lynn		
151668	PRB080174512	Taps(1-100micron grains)	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2009																												oxypnictide																		K		29.4					29.4																				T	resistivity													HC151668																																																														Two step solid state reaction					Neutron-irradiation effects in polycrystalline LaFeAsO0.9F0.1 superconductors			Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, 620219 Ekaterinburg, Russia	Phys.Rev.B, 80(2009)174512	A. E. Karkin,J. Werner,G. Behr,B. N. Goshchitskii		
151669	PRB080174512	The sample prepared by N-irradiated (n= 1.6 E+19 /cm2) to #151668 sample, then annealed at 500C. Figs of Hc2, Tc, and RH shows ANN-T dependences	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2009																												oxypnictide																		K		17					17	TC151669																			T	resistivity													HC151669																																																									RH151669					Two step solid state reaction					Neutron-irradiation effects in polycrystalline LaFeAsO0.9F0.1 superconductors			Institute of Metal Physics, Ural Branch, Russian Academy of Sciences, 620219 Ekaterinburg, Russia	Phys.Rev.B, 80(2009)174512	A. E. Karkin,J. Werner,G. Behr,B. N. Goshchitskii		
151670	JPS078093703		FeSe	Fe1Se1	Fe	1	Se	1																				1	2009																										AB		PbO																		K				7.1			7.1	MTC151670																																																																																															solid state reaction					Anomalous Pressure Dependence of the Superconducting Transition Temperature in FeSe1 x Studied by DC Magnetic Measurements			Department of Material Science, Shimane University, Matsue 690-8504	J.Phys.Soc.Jpn, 78(2009)093703	Kiyotaka MIYOSHI,Yuta TAKAICHI,Eriko MUTOU,Kenji FUJIWARA,Jun TAKEUCHI		
151671	JPS078093703		FeSe0.8	Fe1Se0.8	Fe	1	Se	0.8																				1	2009																										AB		PbO																		K				7			7	MTC151671																																																																																															solid state reaction					Anomalous Pressure Dependence of the Superconducting Transition Temperature in FeSe1 x Studied by DC Magnetic Measurements			Department of Material Science, Shimane University, Matsue 690-8504	J.Phys.Soc.Jpn, 78(2009)093703	Kiyotaka MIYOSHI,Yuta TAKAICHI,Eriko MUTOU,Kenji FUJIWARA,Jun TAKEUCHI		
151672	PHB4043223	"P-induced SC. SC for 2.3 < x < 8.6 kbar. Hc2 defined as ""onset"". Hc2(0)//ab = 20 T for P=3.5 kbar, Hc2(0)//c = 15 T for P=4.3 kbar."	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K			12		0		12																				T	resistivity		20											MHC151672																																																														Sn-flux method					Hydrostatic pressure study of the structural phase transitions and superconductivity in single crystals of (Ba1-xKx)Fe2As2 (x = 0 and 0.45) and CaFe2As2			Department of Physics, San Diego State University, San Diego, CA92182-1233, USA	Physica B, 404(2009)3223	M.S. Torikachvili,S.L .Bud'ko,Ni Ni,P.C.Canfield		
151674	PHB4043223	"Hc2 defined as ""onset"". -(dHc2/dT) = 6.7 T/K for P=20.4 kbar"	(Ba,K)Fe2As2	Ba0.55K0.45Fe2As2	Ba	0.55	K	0.45	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K	28.8		30.7				29.75	MTC151674		K/GPa	-2.5																									T/K	resistivity	8			MHC151674																																																														Sn-flux method					Hydrostatic pressure study of the structural phase transitions and superconductivity in single crystals of (Ba1-xKx)Fe2As2 (x = 0 and 0.45) and CaFe2As2			Department of Physics, San Diego State University, San Diego, CA92182-1233, USA	Physica B, 404(2009)3223	M.S. Torikachvili,S.L .Bud'ko,Ni Ni,P.C.Canfield		
151675	SSC0040611	gamma-Ga. Tc = 6.20 K for beta-phase.	Ga	Gs1	Gs	1																							1966																										A																				K		7.62					7.62																				T	LC	0.308												MHC151675																																																																			Hysteresis effects in three superconducting phases of gallium				Solid State Commun., 4(1966)611	J.Feder,S.R.Kiser,F.Rothwarf,J.P.Burger,C.Valette		
151676	PHC4691958	T<SDW> = 101.6 K, structural transition T* = 83.2 K.	FeSe0.82	Fe1Se0.82	Fe	1	Se	0.82																					2009																										AB		PbO	P4/nmm		A	3.7729		5.523											alpha-phase	K	4.33		11.33				7.83																																																																																														Se(4N),Fe(3N),Ni(2N)		mixture - sealed in quartz tube - heat(700C,24h) - FC to RT - reground - heat(700C,24h) - ANN(400C,36h)					Divergency of SDW and structure transition in Fe1-xNixSe0.82 superconductors			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei, China	Physica C, 469(2009)1958	S.B. Zhang,H.C. Lei,X.D. Zhu,G. Li,B.S. Wang,L.J. Li,X.B. Zhu,W.H. Song,Z.R. Yang,Y.P. Sun		
151677	PHC4691958	T<SDW> = 145.1 K, structural transition T* = 84.9 K.	(Fe,Ni)Se0.82	Fe0.99Ni0.01Se0.82	Fe	0.99	Ni	0.01	Se	0.82																			2009																										AB		PbO	P4/nmm		A	3.7719		5.5209											alpha-phase	K	2		11.3				6.65																																																																																														Se(4N),Fe(3N),Ni(2N)		mixture - sealed in quartz tube - heat(700C,24h) - FC to RT - reground - heat(700C,24h) - ANN(400C,36h)					Divergency of SDW and structure transition in Fe1-xNixSe0.82 superconductors			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei, China	Physica C, 469(2009)1958	S.B. Zhang,H.C. Lei,X.D. Zhu,G. Li,B.S. Wang,L.J. Li,X.B. Zhu,W.H. Song,Z.R. Yang,Y.P. Sun		
151678	PHC4691958	T<SDW> = 156.5 K, structural transition T* = 85.1 K.	(Fe,Ni)Se0.82	Fe0.98Ni0.02Se0.82	Fe	0.98	Ni	0.02	Se	0.82																			2009																										AB		PbO	P4/nmm		A	3.7717		5.5202											alpha-phase	K			11.3				11.3																																																																																														Se(4N),Fe(3N),Ni(2N)		mixture - sealed in quartz tube - heat(700C,24h) - FC to RT - reground - heat(700C,24h) - ANN(400C,36h)					Divergency of SDW and structure transition in Fe1-xNixSe0.82 superconductors			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei, China	Physica C, 469(2009)1958	S.B. Zhang,H.C. Lei,X.D. Zhu,G. Li,B.S. Wang,L.J. Li,X.B. Zhu,W.H. Song,Z.R. Yang,Y.P. Sun		
151679	PHC4691958	not SC. T<SDW> = 187.8 K, structural transition T* = 83.7 K.	(Fe,Ni)Se0.82	Fe0.97Ni0.03Se0.82	Fe	0.97	Ni	0.03	Se	0.82																			2009																										AB		PbO	P4/nmm		A	3.7704		5.5119											alpha-phase	K					2																																																																																																Se(4N),Fe(3N),Ni(2N)		mixture - sealed in quartz tube - heat(700C,24h) - FC to RT - reground - heat(700C,24h) - ANN(400C,36h)					Divergency of SDW and structure transition in Fe1-xNixSe0.82 superconductors			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei, China	Physica C, 469(2009)1958	S.B. Zhang,H.C. Lei,X.D. Zhu,G. Li,B.S. Wang,L.J. Li,X.B. Zhu,W.H. Song,Z.R. Yang,Y.P. Sun		
151680	PHC4691958	not SC. T<SDW> = 185.0 K, structural transition T* = 85.9 K.	(Fe,Ni)Se0.82	Fe0.96Ni0.04Se0.82	Fe	0.96	Ni	0.04	Se	0.82																			2009																										AB		PbO	P4/nmm		A	3.7704		5.5115											alpha-phase	K					2																																																																																																Se(4N),Fe(3N),Ni(2N)		mixture - sealed in quartz tube - heat(700C,24h) - FC to RT - reground - heat(700C,24h) - ANN(400C,36h)					Divergency of SDW and structure transition in Fe1-xNixSe0.82 superconductors			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei, China	Physica C, 469(2009)1958	S.B. Zhang,H.C. Lei,X.D. Zhu,G. Li,B.S. Wang,L.J. Li,X.B. Zhu,W.H. Song,Z.R. Yang,Y.P. Sun		
151681	PHC4692000	x is not given.Tc decrease from 11.5 to 10 K for hydrogen exposure(500C,10 bar H2,15 min). SC volume fraction decreases due to CaH2 formation.	CaC6Hx	C6Ca1H	C	6	Ca	1	H																				2009																												GIC																		K			10				10																																																																																																CaC6 synthesized from molten Li-Cu and HOPG. hydrogenation(500C under 10 bar H2 in stainless reactor)					High temperature hydrogenation of CaC6			London Centre for Nanotechnology, University College London, 17-19 Gordon Street, London WC1H 0AH, UK	Physica C, 469(2009)2000	G. Srinivas,C.A. Howard,N.T. Skipper,S.M. Bennington,M. Ellerby		
151682	PRB080172501	RRR=45. Hc2 defined as R=0.5Rn. Anisotropy(cohere) = 1/0.35	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2009																										AB2C2		ThCr2Si2																	beta-phase	K		1.51					1.51																				T	resistivity								T/K	resistivity		11.5	4.1	MHC151682																						mJ/mol.K2	65																																							Czochralski method					Anisotropic inelastic scattering and its interplay with superconductivity in URu2Si2			Laboratoire Photons Et Matiere (UPMC-CNRS), ESPCI, 75005 Paris, France	Phys.Rev.B, 80(2009)172501	Zengwei Zhu,Elena Hassinger,Zhu'an Xu,Dai Aoki,Jacques Flouquet,Kamran Behnia		
151683	PRB080174509	EDX analysis: Fe1.03Te0.63Se0.37.	Fe(Te,Se)	Fe1Te0.6Se0.4	Fe	1	Te	0.6	Se	0.4																		3	2009																												PbO	P4/nmm																beta-phase	K			14.8			1.3	14.8																																																																																					m3/C	0.00000000117					MRH151683					flux method. mixture - sealed in quartz tube - heat(930C) - slow cool to 400C(3C/h) - FC to RT.					Charge-carrier localization induced by excess Fe in the superconductor Fe1+yTe1-xSex			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 80(2009)174509	T. J. Liu,X. Ke,B. Qian,J. Hu,D. Fobes,E. K. Vehstedt,H. Pham,J. H. Yang,M. H. Fang,L. Spinu,P. Schiffer,Y. Liu,Z. Q. Mao		
151684	PRB080174509	EDX analysis: Fe1.11Te0.64Se0.36	Fe(Te,Se)	Fe1.18Te0.6Se0.4	Fe	1.18	Te	0.6	Se	0.4																		3	2009																												PbO	P4/nmm																beta-phase	K			11.6			5.1	11.6																																																																																					m3/C	0.000000000632					MRH151684					flux method. mixture - sealed in quartz tube - heat(930C) - slow cool to 400C(3C/h) - FC to RT.					Charge-carrier localization induced by excess Fe in the superconductor Fe1+yTe1-xSex			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 80(2009)174509	T. J. Liu,X. Ke,B. Qian,J. Hu,D. Fobes,E. K. Vehstedt,H. Pham,J. H. Yang,M. H. Fang,L. Spinu,P. Schiffer,Y. Liu,Z. Q. Mao		
151685	PRB080174509	not SC. EDX analysis: Fe1.04Te.  structural transition at 72 K.	FeSex	Fe1.04Te1	Fe	1.04	Te	1																				3	2009																												PbO	P4/nmm																beta-phase	K					4																																																										mJ/mol.K2	33																												m3/C	0.000000001108										flux method. mixture - sealed in quartz tube - heat(930C) - slow cool to 400C(3C/h) - FC to RT.					Charge-carrier localization induced by excess Fe in the superconductor Fe1+yTe1-xSex			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 80(2009)174509	T. J. Liu,X. Ke,B. Qian,J. Hu,D. Fobes,E. K. Vehstedt,H. Pham,J. H. Yang,M. H. Fang,L. Spinu,P. Schiffer,Y. Liu,Z. Q. Mao		
151686	PRB080174509	not SC. EDX analysis: Fe1.11Te. structural transition at 65 K.	FeSex	Fe1.18Te1	Fe	1.18	Te	1																				3	2009																												PbO	P4/nmm																beta-phase	K					4																																																										mJ/mol.K2	27																												m3/C	0.000000000459										flux method. mixture - sealed in quartz tube - heat(930C) - slow cool to 400C(3C/h) - FC to RT.					Charge-carrier localization induced by excess Fe in the superconductor Fe1+yTe1-xSex			Department of Physics, Tulane University, New Orleans, Louisiana 70118, USA	Phys.Rev.B, 80(2009)174509	T. J. Liu,X. Ke,B. Qian,J. Hu,D. Fobes,E. K. Vehstedt,H. Pham,J. H. Yang,M. H. Fang,L. Spinu,P. Schiffer,Y. Liu,Z. Q. Mao		
151687	JPS0512375	first stage KC8.	C8KH0.19	C8K1H0.19	C	8	K	1	H	0.19																			1982																												GIC																		K				0.22			0.22																				Oe	SUS													MHC151687																																																														(HOPG + K) - heat(280C,5d). Hydrogenation by chemisorption (RT, 0.5 atm-H2)					Superconductivity in the potassium graphite hydride C8KH0.19			Kyoto University, Kyoto	J.Phys.Soc.Jpn, 51(1982)2375	Shinji Kaneiwa,Mototada Kobayashi,Ikuji Tsujikawa		
151688	JPS0512375	2nd stage KC8	C8KH0.67	C8K1H0.67	C	8	K	1	H	0.67																			1982																												GIC																		K					0.052																																																																																																		(HOPG + K) - heat(280C,5d). Hydrogenation by chemisorption (RT, 0.5 atm-H2)					Superconductivity in the potassium graphite hydride C8KH0.19			Kyoto University, Kyoto	J.Phys.Soc.Jpn, 51(1982)2375	Shinji Kaneiwa,Mototada Kobayashi,Ikuji Tsujikawa		
151689	PRB02200137	Tc(V3Ga) = 15.3 K. (dTc/dx) = -0.7 K/at%H.	V3GaHx	Ga1V3H0.37	Ga	1	V	3	H	0.37																			1980																												Cr3Si(A15)																		K		8.1					8.1	MTC151689																																																																																															V3Ga(or Ge) by arc-melting, then ANN(750C,25h). Hydrogenation(600C,12h, 150 bar-H2) - slow cool to RT					Study of some hydrogenated vanadium-based A15 compounds			University of Houston, Houston, Texas	Phys.Rev.B, 22(1980)137	S.Z.Huang,T.Skowskiewicz,C.W.Chu,J.L.Smith		
151690	PRB02200137	Tc(V3Ge) = 6.1 K.	V3GeHx	Ge1V3H0.033	Ge	1	V	3	H	0.033																			1980																												Cr3Si(A15)																		K		5.83					5.83	MTC151690																																																																																															V3Ga(or Ge) by arc-melting, then ANN(750C,25h). Hydrogenation(600C,12h, 150 bar-H2) - slow cool to RT					Study of some hydrogenated vanadium-based A15 compounds			University of Houston, Houston, Texas	Phys.Rev.B, 22(1980)137	S.Z.Huang,T.Skowskiewicz,C.W.Chu,J.L.Smith		
151691	PRB080140503	thermal conductivity k was measured down to 50 mK: k/T = a + b*T^(alpha), where a(=k0/T) = 5 uW/K2cm, alpha=1.65.	(Ba,K)Fe2As2	Ba0.75K0.25Fe2As2	Ba	0.75	K	0.25	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		26					26																																																																							mOhm.cm							0.047																		flux(FeAs) method					Quasiparticle heat transport in single-crystalline Ba1-xKxFe2As2: Evidence for a k-dependent superconducting gap without nodes			Departement de Physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec J1K 2R1, Canada	Phys.Rev.B, 80(2009)140503	X. G. Luo,M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,Huiqian Luo,Zhaosheng Wang,Hai-Hu Wen,R. Prozorov,Louis Taillefer		
151692	PRB080140503	thermal conductivity k was measured down to 50 mK: k/T = a + b*T^(alpha), where a(=k0/T) = 7 uW/K2cm, alpha=1.5.	(Ba,K)Fe2As2	Ba0.72K0.28Fe2As2	Ba	0.72	K	0.28	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K		30					30																																																																							mOhm.cm							0.028																		flux(FeAs) method					Quasiparticle heat transport in single-crystalline Ba1-xKxFe2As2: Evidence for a k-dependent superconducting gap without nodes			Departement de Physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec J1K 2R1, Canada	Phys.Rev.B, 80(2009)140503	X. G. Luo,M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,Huiqian Luo,Zhaosheng Wang,Hai-Hu Wen,R. Prozorov,Louis Taillefer		
151693	PRB080140511	magnetic phase volume measured by muon-SR. (P4/nmm) phase volume = 99 %.	Fe1.03(Se,Te)	Fe1.03Se0.25Te0.75	Fe	1.03	Se	0.25	Te	0.75																		3	2009																										AB		PbO	P4/nmm																	K			12.5				12.5	MPH151694																																																																																															Bridgeman method. melt and homogenize(1200C,4h) - cool to 750C (4C/h, then 50C/h)					Coexistence of incommensurate magnetism and superconductivity in Fe1+ySexTe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 80(2009)140511	R. Khasanov,M. Bendele,A. Amato,P. Babkevich,A. T. Boothroyd,A. Cervellino,K. Conder,S. N. Gvasaliya,H. Keller,H.-H. Klauss,H. Luetkens,V. Pomjakushin,E. Pomjakushina,B. Roessli		
151694	PRB080140511	magnetic phase volume measured by muon-SR. (P4/nmm) phase volume = 97 %.	Fe1.03(Se,Te)	Fe1.03Se0.45Te0.55	Fe	1.03	Se	0.45	Te	0.55																		3	2009																										AB		PbO	P4/nmm																	K		0	7.96				0	MPH151694																																																																																															Bridgeman method. melt and homogenize(1200C,4h) - cool to 750C (4C/h, then 50C/h)					Coexistence of incommensurate magnetism and superconductivity in Fe1+ySexTe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 80(2009)140511	R. Khasanov,M. Bendele,A. Amato,P. Babkevich,A. T. Boothroyd,A. Cervellino,K. Conder,S. N. Gvasaliya,H. Keller,H.-H. Klauss,H. Luetkens,V. Pomjakushin,E. Pomjakushina,B. Roessli		
151695	PRB080140511	magnetic phase volume measured by muon-SR. (P4/nmm) phase volume = 94 %.	Fe1.03(Se,Te)	Fe1.03Se0.5Te0.5	Fe	1.03	Se	0.5	Te	0.5																		3	2009																										AB		PbO	P4/nmm																	K		14.3	14.3				14.3																																																																																																Bridgeman method. melt and homogenize(1200C,4h) - cool to 750C (4C/h, then 50C/h)					Coexistence of incommensurate magnetism and superconductivity in Fe1+ySexTe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 80(2009)140511	R. Khasanov,M. Bendele,A. Amato,P. Babkevich,A. T. Boothroyd,A. Cervellino,K. Conder,S. N. Gvasaliya,H. Keller,H.-H. Klauss,H. Luetkens,V. Pomjakushin,E. Pomjakushina,B. Roessli		
151697	PRL103236401	P-induced SC. SC for 2<P<4 GPa. Hc2(T) measured for P=3.5 GPa, defined as 0.9Rn. T<CDW> defined as max of (dR/dT) .	1T-TiSe2	Ti1Se2	Ti	1	Se	2																				3	2009																										AB2		TX2																		K			1.8		0		1.8	MPH151697																																	MHC151697																																																														vapor transport method.					Pressure Induced Superconductivity in Pristine 1T-TiSe2			Ecole Polytechnique Federale de Lausanne, IPMC, CH-1015 Lausanne, Switzerland	Phys.Rev.Lett., 103(2009)236401	A. F. Kusmartseva,B. Sipos,H. Berger,L. Forro,E. Tutis		
151698	PRB080180507	composition determined by EDX ( Fe1.05Se0.15Te0.85). (dI/dV) measured for cleaved surface.	Fe(Se,Te)	Fe1Se0.25Te0.75	Fe	1	Se	0.25	Te	0.75																		3	2009																										AB																				K			14				14																																														meV	2.3	3.8	1																																															self-flux method. mixture(Fe:Se:Te = 1:0.25:0.75) - sealed in evacuated quartz tube - heat(950C,10h) - cool to 700C(5C/h) - ANN(400C,100h)					Local density of states and superconducting gap in the iron chalcogenide superconductor Fe1+zSe1-xTex observed by scanning tunneling spectroscopy			Department of Physics, Tokyo University of Science, 1-3 Kagurazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Phys.Rev.B, 80(2009)180507	Takuya Kato,Yoshikazu Mizuguchi,Hiroshi Nakamura,Tadashi Machida,Hideaki Sakata,Yoshihiko Takano		
151699	PRB080212501	Tc0 = 40K(perfect order). isotope(alpha) = 0.153 for Tc=40K. disorder(out-of-plane) increases isotope effect. dTc(<16>O2 -<18>O2)  = 0.80K.	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2009																												Bi2201																		K				32.83			32.83						0.214	O		0.8																																																																																							TSFZ method. (as-grown) - ANN(700C,96h,in air) - ANN(700C,168h,in 0.2 bar<16>O2 or <18>O2) - Q to RT.					Enhancement of oxygen isotope effect due to out-of-plane disorder in Bi2Sr2Ln0.4CuO6+z superconductors			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 80(2009)212501	K. Sato,H. Iwasawa,N. C. Plumb,T. Masui,Y. Yoshida,H. Eisaki,H. Bando,A. Ino,M. Arita,K. Shimada,H. Namatame,M. Taniguchi,S. Tajima,Y. Nishihara,D. S. Dessau,Y. Aiura		
151700	PRB080212501	Tc0 = 40K(perfect order). isotope(alpha) = 0.153 for Tc=40K. disorder(out-of-plane) increases isotope effect. dTc(<16>O2 -<18>O2)  = 0.71K.	Bi2(Sr,Nd)2CuO6	Bi2Sr1.6Nd0.4Cu1O6+z	Bi	2	Sr	1.6	Nd	0.4	Cu	1													O	6+z		3	2009																												Bi2201																		K				30.07			30.07						0.206	O		0.71																																																																																							TSFZ method. (as-grown) - ANN(700C,96h,in air) - ANN(700C,168h,in 0.2 bar<16>O2 or <18>O2) - Q to RT.					Enhancement of oxygen isotope effect due to out-of-plane disorder in Bi2Sr2Ln0.4CuO6+z superconductors			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 80(2009)212501	K. Sato,H. Iwasawa,N. C. Plumb,T. Masui,Y. Yoshida,H. Eisaki,H. Bando,A. Ino,M. Arita,K. Shimada,H. Namatame,M. Taniguchi,S. Tajima,Y. Nishihara,D. S. Dessau,Y. Aiura		
151701	PRB080212501	Tc0 = 40K(perfect order). isotope(alpha) = 0.153 for Tc=40K. disorder(out-of-plane) increases isotope effect. dTc(<16>O2 -<18>O2)  = 0.72K.	Bi2(Sr,Eu)2CuO6	Bi2Sr1.6Eu0.4Cu1O6+z	Bi	2	Sr	1.6	Eu	0.4	Cu	1													O	6+z		3	2009																												Bi2201																		K				16.9			16.9						0.38	O		0.72																																																																																							TSFZ method. (as-grown) - ANN(700C,96h,in air) - ANN(700C,168h,in 0.2 bar<16>O2 or <18>O2) - Q to RT.					Enhancement of oxygen isotope effect due to out-of-plane disorder in Bi2Sr2Ln0.4CuO6+z superconductors			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 80(2009)212501	K. Sato,H. Iwasawa,N. C. Plumb,T. Masui,Y. Yoshida,H. Eisaki,H. Bando,A. Ino,M. Arita,K. Shimada,H. Namatame,M. Taniguchi,S. Tajima,Y. Nishihara,D. S. Dessau,Y. Aiura		
151702	PRB080212501	Tc0 = 40K(perfect order). isotope(alpha) = 0.153 for Tc=40K. disorder(out-of-plane) increases isotope effect. dTc(<16>O2 -<18>O2)  = 0.97K.	Bi2(Sr,Gd)2CuO6	Bi2Sr1.6Gd0.4Cu1O6+z	Bi	2	Sr	1.6	Gd	0.4	Cu	1													O	6+z		3	2009																												Bi2201																		K				12.27			12.27						0.68	O		0.97																																																																																							TSFZ method. (as-grown) - ANN(700C,96h,in air) - ANN(700C,168h,in 0.2 bar<16>O2 or <18>O2) - Q to RT.					Enhancement of oxygen isotope effect due to out-of-plane disorder in Bi2Sr2Ln0.4CuO6+z superconductors			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 80(2009)212501	K. Sato,H. Iwasawa,N. C. Plumb,T. Masui,Y. Yoshida,H. Eisaki,H. Bando,A. Ino,M. Arita,K. Shimada,H. Namatame,M. Taniguchi,S. Tajima,Y. Nishihara,D. S. Dessau,Y. Aiura		
151703	PRB080214514	Curie-T estimated from high-T SUS.	Fe(Se,Te)	Fe1.12Se0.03Te0.97	Fe	1.12	Se	0.03	Te	0.97																		3	2009							-175																			AB																				K			6.5				6.5																																																																																																(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151704	PRB080214514	Curie-T estimated from high-T SUS.	Fe(Se,Te)	Fe1.13Se0.1Te0.85	Fe	1.13	Se	0.1	Te	0.85																		3	2009							-186																			AB																				K	2		8.5				5.25																																																																																																(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151705	PRB080214514	Curie-T estimated from high-T SUS. Anisotropy(Hc2) = 1.05.	Fe(Se,Te)	Fe1.12Se0.11Te0.83	Fe	1.12	Se	0.11	Te	0.83																		3	2009							-162																			AB																				K	3.5		8.6				6.05																				T	resistivity, WHH		19	18					T/K	resistivity, WHH		4.9	4.6	MHC151705		A	from Hc2		43	43																																																								(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151706	PRB080214514	Curie-T estimated from high-T SUS.  Jc from M-loops. Jc(1.8K, H=0T) = 0.6E+6 A/cm2 for H//ab.	Fe(Se,Te)	Fe1.06Se0.14Te0.83	Fe	1.06	Se	0.14	Te	0.83																		3	2009							-156																			AB																				K	7		8.7				7.85																				T	resistivity, WHH		56	44					T/K	resistivity, WHH		10.7	8.4	MHC151706		A	from Hc2		27	24																																																								(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151707	PRB080214514	Curie-T estimated from high-T SUS.	Fe(Se,Te)	Fe0.98Se0.15Te0.9	Fe	0.98	Se	0.15	Te	0.9																		3	2009							-167																			AB																				K			8.8				8.8																																																																																																(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151708	PRB080214514	not SC. two anomalies in SP-heat. lattice term in SP (beta) = 0.49 mJ/mol.K4.	Fe(Se,Te)	Fe1.14Te0.1	Fe	1.14	Te	0.1																				3	2009							-191																			AB																				K					1.8																																																										mJ/mol.K2	32	SP-heat	228	SP-heat																																				(Te-Se)-flux method. heat(430-450C, 24h) - heat(850-900C) - slow cool to (800-840C)					Superconductivity, magnetism, and stoichiometry of single crystals of Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 80(2009)214514	Rongwei Hu,Emil S. Bozin,J. B. Warren,C. Petrovic		
151709	PRB080214511	composition determined by X-ray Rietveld analysis (nominal = FeTe). structure/magnetic transition at 66K.	FeTe	Fe1.087Te1	Fe	1.087	Te	1																				3	2009																										AB																				K					5																																																																				uV/K	-0.886			MTP151709																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151710	PRB080214511	structure/magnetic transition at 39K. R is not zero at 5K.	Fe(Se,Te)	Fe1Se0.1Te0.9	Fe	1	Se	0.1	Te	0.9																		3	2009																										AB																				K			10				10																																																																		uV/K	0.955			MTP151710																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151711	PRB080214511	composition determined by X-ray Rietveld analysis (nominal = FeTe).	Fe(Se,Te)	Fe1.049Se0.2Te0.8	Fe	1.049	Se	0.2	Te	0.8																		3	2009																										AB																				K	11						11																																																																		uV/K	3			MTP151711																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151712	PRB080214511	composition determined by X-ray Rietveld analysis (nominal = FeTe).	Fe(Se,Te)	Fe1.053Se0.3Te0.7	Fe	1.053	Se	0.3	Te	0.7																		3	2009																										AB																				K	12.5						12.5																																																																		uV/K	6.07			MTP151712																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151713	PRB080214511	composition determined by X-ray Rietveld analysis (nominal = FeTe).	Fe(Se,Te)	Fe1.013Se0.3Te0.7	Fe	1.013	Se	0.3	Te	0.7																		3	2009																										AB																				K	13						13																																																																		uV/K	7.64			MTP151713																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151714	PRB080214511		Fe(Se,Te)	Fe1Se0.45Te0.55	Fe	1	Se	0.45	Te	0.55																		3	2009																										AB																				K	12.6						12.6																																																																		uV/K	7.16			MTP151714																										mixture - heat(930-960C in sealed quartz) - slow cool to RT					Seebeck effect in Fe1+xTe1-ySey single crystals			CNR-INFM-LAMIA and Universita di Genova, via Dodecaneso 33, 16146 Genova, Italy	Phys.Rev.B, 80(2009)214511	I. Pallecchi,G. Lamura,M. Tropeano,M. Putti,R. Viennois,E. Giannini,D. Van der Marel		
151715	JPS078123602	beta-pyrochlore. Anomalies in SP are found at 9.65K(SC) and 7.8K(1st order transition)  T^5 term coeff. in SP = 0.37 mJ/mol.K6. (dC/Tc) = 0.21 J/mol.K2. Tc by SP.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6		3	2009																												pyrochlore																		K		9.65					9.65	TC151715		T/GPa	7.5																																																																																																	Sudden Disappearance of the First-Order Transition in beta-Pyrochlore KOs2O6 under Low Pressure			N-BARD, Hiroshima University, Higashihiroshima, Hiroshima 739-8526	J.Phys.Soc.Jpn, 78(2009)123602	Kazunori UMEO,Hirokazu KUBO,Jun-ichi YAMAURA,Zenji HIROI,Toshiro TAKABATAKE		
151716	JPS078123707		Sr2VFeAsO3	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3		1	2009																												21113																		K	32.5		36.4				34.45	TC151716		T/GPa	4.6																																																																																												solid state reaction					Contrasting Pressure Effects in Sr2VFeAsO3 and Sr2ScFePO3			Department of Physics, Kobe University, Kobe 657-8501	J.Phys.Soc.Jpn, 78(2009)123707	Hisashi KOTEGAWA,Takayuki KAWAZOE,Hideki TOU,Keizo MURATA,Hiraku OGINO,Kohji KISHIO,Jun-ichi SHIMOYAMA		
151717	JPS078123707		Sr2ScFePO3	Sr2Sc1Fe1P1O3	Sr	2	Sc	1	Fe	1	P	1													O	3		1	2009																												21113																		K	8.4		15.6				12	TC151717		T/GPa	-3.6																																																																																												solid state reaction					Contrasting Pressure Effects in Sr2VFeAsO3 and Sr2ScFePO3			Department of Physics, Kobe University, Kobe 657-8501	J.Phys.Soc.Jpn, 78(2009)123707	Hisashi KOTEGAWA,Takayuki KAWAZOE,Hideki TOU,Keizo MURATA,Hiraku OGINO,Kohji KISHIO,Jun-ichi SHIMOYAMA		
151718	JPS078124713	P-induced SC. SC properties are for P = 7.1 GPa. parallel means H//[001], perpendicular means H//[100]. Tc = 0.58 K for [100] direction.	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		3	2009																										ABC3																			perovskite	K			0.64		0		0.64																				T	resistivity		24	3.1					T/K	resistivity		30	7.5																																																															Bi-flux method					Magnetic Properties of RCoGe3 (R: Ce, Pr, and Nd) and Strong Anisotropy of the Upper Critical Field in Non-centrosymmetric Compound CeCoGe3			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0044	J.Phys.Soc.Jpn, 78(2009)124713	Marie-aude ME ASSON1,Hiroshi MURANAKA,Tomoya KAWAI,Yuuki OTA,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Tetsuya TAKEUCHI,Katsuya SHIMIZU,Fuminori HONDA,Rikio SETTAI,Yoshichika ONUKI		
151719	JPS078124713	not SC. effective moment = 3.60 myu-B/Pr.	PrCoGe3	Pr1Co1Ge3	Pr	1	Co	1	Ge	3																		3	2009							-18																			ABC3																			perovskite	K					0																																																										mJ/mol.K2	6.1																																							Bi-flux method					Magnetic Properties of RCoGe3 (R: Ce, Pr, and Nd) and Strong Anisotropy of the Upper Critical Field in Non-centrosymmetric Compound CeCoGe3			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0044	J.Phys.Soc.Jpn, 78(2009)124713	Marie-aude ME ASSON1,Hiroshi MURANAKA,Tomoya KAWAI,Yuuki OTA,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Tetsuya TAKEUCHI,Katsuya SHIMIZU,Fuminori HONDA,Rikio SETTAI,Yoshichika ONUKI		
151720	JPS078124713	not SC. effective moment = 3.62 myu-B/Nd. Curie-T = -23.8 K for [001] direction.	NdeCoGe3	Nd1Co1Ge3	Nd	1	Co	1	Ge	3																		3	2009							-1.2	3.8																		ABC3																			perovskite	K					0																																																																																																		Bi-flux method					Magnetic Properties of RCoGe3 (R: Ce, Pr, and Nd) and Strong Anisotropy of the Upper Critical Field in Non-centrosymmetric Compound CeCoGe3			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0044	J.Phys.Soc.Jpn, 78(2009)124713	Marie-aude ME ASSON1,Hiroshi MURANAKA,Tomoya KAWAI,Yuuki OTA,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Tetsuya TAKEUCHI,Katsuya SHIMIZU,Fuminori HONDA,Rikio SETTAI,Yoshichika ONUKI		
151721	PRL101087001		Sm(O,F)FeAs	Sm1Fe1As1F0.12O0.88	Sm	1	Fe	1	As	1	F	0.12													O	0.88			2008																												oxypnictide																	ZrCuSiAs	K				17.1			17.1																																																																																														SmAs,SmF3,Fe,Fe2O3		pellet - ANN(1160C,40h, in Ta foil in quartz) - cool to 400C(4C/min) - FC to RT					Anomalous Transport Properties and Phase Diagram of the FeAs-Based SmFeAsO1-xFx Superconductors			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G.Wu,T.Wu,D. F. Fang,H. Chen,S.Y. Li,K. Liu,Y. L. Xie,X. F.Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
151722	PRL101087001		Sm(O,F)FeAs	Sm1Fe1As1F0.14O0.86	Sm	1	Fe	1	As	1	F	0.14													O	0.86			2008																												oxypnictide																	ZrCuSiAs	K				27			27																																																																																														SmAs,SmF3,Fe,Fe2O3		pellet - ANN(1160C,40h, in Ta foil in quartz) - cool to 400C(4C/min) - FC to RT					Anomalous Transport Properties and Phase Diagram of the FeAs-Based SmFeAsO1-xFx Superconductors			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G.Wu,T.Wu,D. F. Fang,H. Chen,S.Y. Li,K. Liu,Y. L. Xie,X. F.Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
151723	PRL101087001		Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2008																												oxypnictide			A	3.9316		8.4932											ZrCuSiAs	K				41.8			41.8																																																																																														SmAs,SmF3,Fe,Fe2O3		pellet - ANN(1160C,40h, in Ta foil in quartz) - cool to 400C(4C/min) - FC to RT					Anomalous Transport Properties and Phase Diagram of the FeAs-Based SmFeAsO1-xFx Superconductors			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G.Wu,T.Wu,D. F. Fang,H. Chen,S.Y. Li,K. Liu,Y. L. Xie,X. F.Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
151724	PRL101087001		Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8			2008																												oxypnictide			A	3.9261		8.4799											ZrCuSiAs	K			54	51.8			51.8																																																																																														SmAs,SmF3,Fe,Fe2O3		pellet - ANN(1160C,40h, in Ta foil in quartz) - cool to 400C(4C/min) - FC to RT					Anomalous Transport Properties and Phase Diagram of the FeAs-Based SmFeAsO1-xFx Superconductors			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G.Wu,T.Wu,D. F. Fang,H. Chen,S.Y. Li,K. Liu,Y. L. Xie,X. F.Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
151725	PRL101087001	R not to zero at 5K.	Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9			2008																												oxypnictide			A	3.9355		8.4962											ZrCuSiAs	K			12				12																																																																																														SmAs,SmF3,Fe,Fe2O3		pellet - ANN(1160C,40h, in Ta foil in quartz) - cool to 400C(4C/min) - FC to RT					Anomalous Transport Properties and Phase Diagram of the FeAs-Based SmFeAsO1-xFx Superconductors			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.Lett., 101(2008)087001	R. H. Liu,G.Wu,T.Wu,D. F. Fang,H. Chen,S.Y. Li,K. Liu,Y. L. Xie,X. F.Wang,R. L. Yang,L. Ding,C. He,D. L. Feng,X. H. Chen		
151726	PHC4690381	not SC. structural/AF transition at 173 K.	SrFeAsF	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																	2009																										ABCD		oxypnictide			A	4.004		8.971											ZrCuSiAs	K					2																																																																																																		Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151727	PHC4690381	not SC. structural/AF transition at 118 K.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																	2009																										ABCD		oxypnictide			A	3.88		8.594											ZrCuSiAs	K					2																																																																																																		Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151728	PHC4690381	not SC. structural/AF transition at 153 K.	EuFeAsF	Eu1Fe1As1F1	Eu	1	Fe	1	As	1	F	1																	2009																										ABCD		oxypnictide			A	3.974		8.929											ZrCuSiAs	K					2																																																																																																		Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151729	PHC4690381		(Sr,La)FeAsF	Sr0.6La0.4Fe1As1F1	Sr	0.6	La	0.4	Fe	1	As	1	F	1															2009																										ABCD		oxypnictide																		K	24.6		29.5				27.05																																																																																																Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151730	PHC4690381		(Ca,Nd)FeAsF	Ca0.4Nd0.6Fe1As1F1	Ca	0.4	Nd	0.6	Fe	1	As	1	F	1															2009																										ABCD		oxypnictide																		K			57.4	54			54																																																																																																Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151731	PHC4690381		(Ca,Pr)FeAsF	Ca0.4Pr0.6Fe1As1F1	Ca	0.4	Pr	0.6	Fe	1	As	1	F	1															2009																										ABCD		oxypnictide																		K			52.8	50			50																																																																																																Two step heating. pellet - heat(1000C,30h, in evacuated siloca)					Parent phase and superconductors in the fluorine derivative family			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, P.O. Box 603, Beijing 100190, PR China	Physica C, 469(2009)381	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Bin Zeng,Hai-Hu Wen		
151732	MCP1190208	Major phase(by EDX): Y1.0Ba1.9Cu4.1Ox	YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8			2010																												Y124			A	3.846	3.869	27.241												K	71		78			7	74.5																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151733	MCP1190208	Major phase(by EDX): Y0.95Sc0.05Ba1.8Cu4.2Ox	(Y,Sc)Ba2Cu4O8	Y0.95Sc0.05Ba2Cu4O8	Y	0.95	Sc	0.05	Ba	2	Cu	4													O	8			2010																												Y124			A	3.845	3.869	27.24												K			79				79																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151734	MCP1190208	Major phase(by EDX): Y0.90Sc0.10Ba2.1Cu3.9Ox	(Y,Sc)Ba2Cu4O8	Y0.9Sc0.1Ba2Cu4O8	Y	0.9	Sc	0.1	Ba	2	Cu	4													O	8			2010																												Y124			A	3.847	3.872	27.239												K			81				81																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151735	MCP1190208	Major phase(by EDX): Y0.79Sc0.21Ba1.7Cu4.3Ox.  small amount of ortho-Y123 phase. Tc(on)- increase maybe from Y123 phase.	(Y,Sc)Ba2Cu4O8	Y0.8Sc0.2Ba2Cu4O8	Y	0.8	Sc	0.2	Ba	2	Cu	4													O	8			2010																												Y124			A	3.845	3.874	27.232												K			87				87																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151736	MCP1190208	Major phase(by EDX): Y0.95Ga0.05Ba2.0Cu4.0Ox	(Y,Ga)Ba2Cu4O8	Y0.95Ga0.05Ba2Cu4O8	Y	0.95	Ga	0.05	Ba	2	Cu	4													O	8			2010																												Y124			A	3.844	3.868	27.237												K			75				75																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151737	MCP1190208	Major phase(by EDX): Y0.91Ga0.09Ba1.9Cu4.1Ox	(Y,Ga)Ba2Cu4O8	Y0.9Ga0.1Ba2Cu4O8	Y	0.9	Ga	0.1	Ba	2	Cu	4													O	8			2010																												Y124			A	3.846	3.871	27.233												K			74				74																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151738	MCP1190208	Major phase(by EDX): Y0.80Ga0.20Ba2.3Cu3.7Ox. Tc-decrease maybe from non-SC-tetragonal Y123 phase	(Y,Ga)Ba2Cu4O8	Y0.8Ga0.2Ba2Cu4O8	Y	0.8	Ga	0.2	Ba	2	Cu	4													O	8			2010																												Y124			A	3.847	3.872	27.229												K			69				69																																																																																														Y2O3,Sc2O3,Ga(HO3)3,BaM2,CuM2/H2O		M=Ch3COO. aqeous sol-gel method. (precursor gel powder) - CAL(700C,10h,in flowing O2) - reground - heat(780C,10h) - ANN(780C,20h,in flowing O2)					Scandium and gallium substitution effects in the (Y1-xScx)Ba2Cu4O8 and (Y1-xGax)Ba2Cu4O8 superconducting oxides			Department of General and Inorganic Chemistry, Vilnius University, Naugarduko 24, LT-03225 Vilnius, Lithuania	Mat.Chem.Phys., 119(2010)208	T. Klemkiene,R. Raudonis,A. Beganskiene,A. Zalga,I. Grigoraviciute,A. Kareiva		
151739	PHC4690905	single crystal: 0.5*0.2*0.02 mm3. Anisotropy(RES) = 6.3 at 300K. R(T) = a*T^n (n=5 for T < 20 K)	BaNi2P2	Ba1Ni2P2	Ba	1	Ni	2	P	2																		3	2009																										Ab2C2		ThCr2Si2																		K		3					3																																																																							mOhm.cm								4.1				0.078	0.494							MRH151739					High-P-synthesis					Transport properties of single crystal BaNi2P2			Department of Physics, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan	Physica C, 469(2009)905	Shigeyuki Ishida,Masamichi Nakajima,Hijiri Kito,Yasuhide Tomioka,Toshimitsu Ito,Akira Iyo,Hiroshi Eisaki,Shin-ichi Uchida		
151740	PHC4690898		PrO(Fe,Co)As	Pr1Fe0.925Co0.075As1O1	Pr	1	Fe	0.925	Co	0.075	As	1													O	1			2009																												oxypnictide	P4/nmm		A	3.9834		8.6102											ZrCuSiAs	K				15			15										50																																																																																				PrAs,Fe,Co,Fe2O3		high-P synthesis. mixture - heat(1150C,2h, P=2 GPa)					Search for new iron oxypnictide superconductors by using high-pressure synthesis technique			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 469(2009)898	P.M. Shirage,K. Miyazawa,H. Kito,H. Eisaki,A. Iyo		
151741	PHC4690985	O-content from iodometric method	GdBaSrCu3Oz	Gd1Ba1Sr1Cu3O6.9371	Gd	1	Ba	1	Sr	1	Cu	3													O	z	6.9371	1	2009																												Y123			A	3.854		11.571												K	70		83				76.5																																																																																														Gd2O3,CaCO3,BaCO3,SrCO3,CuO	1	mixture - pellet - heat(950C,24h) - ANN(950C,10h,in flowing O2) - cool to 600C (80C/h) - FC to RT					Effect of Ca doping on the superconducting properties of GdBaSrCu3O7 d bulk samples			Human Sensing Program, Graduate School of Science and Engineering, Yamagata University, 4-3-16 Johnan, Yonezawa City, Yamagata 992-8510, Japan	Physica C, 469(2009)985	T.V. Chong,S. Kambe,O. Ishii		
151742	PHC4690985	O-content from iodometric method	(Gd,Ca)BaSrCu3Oz	Gd0.99Ca0.01Ba1Sr1Cu3O6.9198	Gd	0.99	Ca	0.01	Ba	1	Sr	1	Cu	3											O	z	6.9198	1	2009																												Y123			A	3.841		11.536												K	64		77				70.5																																																																																														Gd2O3,CaCO3,BaCO3,SrCO3,CuO	1	mixture - pellet - heat(950C,24h) - ANN(950C,10h,in flowing O2) - cool to 600C (80C/h) - FC to RT					Effect of Ca doping on the superconducting properties of GdBaSrCu3O7 d bulk samples			Human Sensing Program, Graduate School of Science and Engineering, Yamagata University, 4-3-16 Johnan, Yonezawa City, Yamagata 992-8510, Japan	Physica C, 469(2009)985	T.V. Chong,S. Kambe,O. Ishii		
151743	PHC4690985	O-content from iodometric method	(Gd,Ca)BaSrCu3Oz	Gd0.96Ca0.04Ba1Sr1Cu3O6.9138	Gd	0.96	Ca	0.04	Ba	1	Sr	1	Cu	3											O	z	6.9138	1	2009																												Y123			A	3.84		11.53												K	65		77				71																																																																																														Gd2O3,CaCO3,BaCO3,SrCO3,CuO	1	mixture - pellet - heat(950C,24h) - ANN(950C,10h,in flowing O2) - cool to 600C (80C/h) - FC to RT					Effect of Ca doping on the superconducting properties of GdBaSrCu3O7 d bulk samples			Human Sensing Program, Graduate School of Science and Engineering, Yamagata University, 4-3-16 Johnan, Yonezawa City, Yamagata 992-8510, Japan	Physica C, 469(2009)985	T.V. Chong,S. Kambe,O. Ishii		
151744	PHC4690985	O-content from iodometric method	(Gd,Ca)BaSrCu3Oz	Gd0.93Ca0.07Ba1Sr1Cu3O6.8804	Gd	0.93	Ca	0.07	Ba	1	Sr	1	Cu	3											O	z	6.8804	1	2009																												Y123			A	3.842		11.54												K	50		57				53.5																																																																																														Gd2O3,CaCO3,BaCO3,SrCO3,CuO	1	mixture - pellet - heat(950C,24h) - ANN(950C,10h,in flowing O2) - cool to 600C (80C/h) - FC to RT					Effect of Ca doping on the superconducting properties of GdBaSrCu3O7 d bulk samples			Human Sensing Program, Graduate School of Science and Engineering, Yamagata University, 4-3-16 Johnan, Yonezawa City, Yamagata 992-8510, Japan	Physica C, 469(2009)985	T.V. Chong,S. Kambe,O. Ishii		
151745	PHC4690985	O-content from iodometric method	(Gd,Ca)BaSrCu3Oz	Gd0.9Ca0.1Ba1Sr1Cu3O6.8754	Gd	0.9	Ca	0.1	Ba	1	Sr	1	Cu	3											O	z	6.8754	1	2009																												Y123			A	3.851		11.569												K	34		52				43																																																																																														Gd2O3,CaCO3,BaCO3,SrCO3,CuO	1	mixture - pellet - heat(950C,24h) - ANN(950C,10h,in flowing O2) - cool to 600C (80C/h) - FC to RT					Effect of Ca doping on the superconducting properties of GdBaSrCu3O7 d bulk samples			Human Sensing Program, Graduate School of Science and Engineering, Yamagata University, 4-3-16 Johnan, Yonezawa City, Yamagata 992-8510, Japan	Physica C, 469(2009)985	T.V. Chong,S. Kambe,O. Ishii		
151746	PHC4690901	single crystal: 0.6*0.8*0.03 mm3. O-content not measured. Anisotropy = 5 from Hc2.	PrOFeAs	Pr1Fe1As1O0.7	Pr	1	Fe	1	As	1															O	0.7		3	2009																												oxypnictide																	ZrCuSiAs	K		44		44			44																				T	resistivity, 0.5Rn													HC151746																																																														high-P-synthesis. (1300-1400C,2h,P=2 GPa, in BN crucible)					Growth of single crystal PrFeAsO1-y and its characterization			Quantum Beam Science Directorate, Japan Atomic Energy Agency, Tokai, Naka, Ibaraki 319-1195, Japan	Physica C, 469(2009)901	M. Ishikado,S. Shamoto,H. Kito,A. Iyo,H. Eisaki,T. Ito,Y. Tomioka		
151747	PHC4690965	Whiskers.  Whiskers grown from precursor pellet composed of LuCaBa3Cu3OzTe0.5.  Compositions of whiskers not given.	LuBa2Cu3Oz	Lu1Ba2Cu3O7-z	Lu	1	Ba	2	Cu	3															O	7-z			2009																												Y123			A			11.72												K	79		83				81																																																																																																Whiskers gron from precursor pellet with Te					Growth of superconducting single-crystalline (Lu, Ca) Ba2Cu3O7 d whiskers			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Physica C, 469(2009)965	K. Deguchi,S. Ogawara,T. Okutsu,M. Nagao,T. Watanabe,Y. Mizuguchi,Y. Kubo,F. Tomioka,S. Ishii,S. Tsuda,T. Yamaguchi,M. Nagasawa,Y. Takano		
151748	PHC4692012	R(T) measured for H < 1.5 T. Tc(zero) sensitive to H.	Y3Ba5Cu8O18	Y3Ba5Cu8O18	Y	3	Ba	5	Cu	8															O	18		1	2009																												Y358	Pnm2		A	3.888	3.823	31.013												K	98	100.1	102			2.4	100.1																																																																																														Y2O3,BaCO3,CuO	1	mixture - react(840C,12h,in air) - pellet - heat to 1000C(20C/min) - SIN(890-930C,24h,in O2) - cool to 500C - ANN(500C,10h,in flowing O2) - FC to RT					A new Y-based HTSC with Tc above 100 K			Magnet Research Laboratory (MRL), Department of Physics, Sharif University of Technology, P.O. Box 11365-9161 Tehran, Iran	Physica C, 469(2009)2012	A. Aliabadi,Y. Akhavan Farshchi,M. Akhavan		
151749	PRB080220509	single crystal: 0.8*0.4*0.05 mm3. RRR=28	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		3	2009																												oxypnictide																		K		7.4					7.4																				T	thermal conductivity		8.6	1																																					W/K.m				THC151749						UOhm.cm								4.9																	Sn-flux method					Thermal conductivity measurements of the energy-gap anisotropy of superconducting LaFePO at low temperatures			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 80(2009)220509	M. Yamashita,N. Nakata,Y. Senshu,S. Tonegawa,K. Ikada,K. Hashimoto,H. Sugawara,T. Shibauchi,Y. Matsuda		
151750	JPS078044712	not SC	NpAl4	Np1Al4	Np	1	Al	4																				3	2009								49																		AB4			Imma		A	4.4036	6.226	13.7219												K					1																																																										mJ/mol.K2	20	SP-heat													UOhm.cm								2.9																	Al-flux method					Magnetic and Electrical Properties in NpAl4 and UAl4			Institute for Materials Research, Tohoku University, Oarai, Ibaraki 311-1313	J.Phys.Soc.Jpn, 78(2009)044712	Dai AOKI,Yoshinori HAGA,Yoshiya HOMMA,Yoshinobu SHIOKAWA,Etsuji YAMAMOTO,Akio NAKAMURA,Rikio SETTAI,Y. Onuki		
151751	JPS078044712	not SC	UAl4	U1Al4	U	1	Al	4																				3	2009																										AB4			Imma																	K					1																																																										mJ/mol.K2	89	SP-heat	275	SP-heat											UOhm.cm								3.2																	Al-flux method					Magnetic and Electrical Properties in NpAl4 and UAl4			Institute for Materials Research, Tohoku University, Oarai, Ibaraki 311-1313	J.Phys.Soc.Jpn, 78(2009)044712	Dai AOKI,Yoshinori HAGA,Yoshiya HOMMA,Yoshinobu SHIOKAWA,Etsuji YAMAMOTO,Akio NAKAMURA,Rikio SETTAI,Y. Onuki		
151752	PRL103257003	Fe-isotope effect. using original method to rule out K-concentration difference between two samples (<57>, <54>Fe). Higher Tc for large Fe mass. [isotope] shows average for 7 sets.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2009																												ThCr2Si2																		K			37.8				37.8						-0.18	Fe																																																																																									high-P-synthesis. using <57>Fe, <n>Fe, <54>Fe					Inverse Iron Isotope Effect on the Transition Temperature of the (Ba,K)Fe2As2 Superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.Lett., 103(2009)257003	Parasharam M. Shirage,Kunihiro Kihou,Kiichi Miyazawa,Chul-Ho Lee,Hijiri Kito,Hiroshi Eisaki,Takashi Yanagisawa,Yasumoto Tanaka,Akira Iyo		
151753	NAT4590064	not SC. T<SDW> = 130 K. isotope effect of SDW, a<SDW> = 0.05 and 0.39, for O- and Fe-isotope, respectively.	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1			2009																												oxypnictide																		K																																																																																																							solid state reaction					A large iron isotope effect in SmFeAsO1-xFx and Ba1-xKxFe2As2			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nature, 459(2009)64	R. H. Liu,T. Wu,G. Wu,H. Chen,X. F. Wang,Y. L. Xie,J. J. Ying,Y. J. Yan,Q. J. Li,B. C. Shi,W. S. Chu,Z. Y. Wu,X. H. Chen		
151754	NAT4590064	dTc(<n>O-<18>O) = -0.2 K.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2009																												oxypnictide																		K		41.5					41.5						-0.06	O	77	-0.2																																																																																							solid state reaction					A large iron isotope effect in SmFeAsO1-xFx and Ba1-xKxFe2As2			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nature, 459(2009)64	R. H. Liu,T. Wu,G. Wu,H. Chen,X. F. Wang,Y. L. Xie,J. J. Ying,Y. J. Yan,Q. J. Li,B. C. Shi,W. S. Chu,Z. Y. Wu,X. H. Chen		
151755	NAT4590064	dTc(<54>Fe-<56>Fe) = 0.5 K.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2009																												oxypnictide																		K		41					41						0.34	Fe	98	0.5																																																																																							solid state reaction					A large iron isotope effect in SmFeAsO1-xFx and Ba1-xKxFe2As2			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nature, 459(2009)64	R. H. Liu,T. Wu,G. Wu,H. Chen,X. F. Wang,Y. L. Xie,J. J. Ying,Y. J. Yan,Q. J. Li,B. C. Shi,W. S. Chu,Z. Y. Wu,X. H. Chen		
151756	NAT4590064	not SC. T<SDW> defined as the peak of (dR/dT). isotope effect of T<SDW>, a<SDW> = 0.36 using 92 %<54>Fe.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																			2009																												ThCr2Si2																		K																																																																																																							solid state reaction					A large iron isotope effect in SmFeAsO1-xFx and Ba1-xKxFe2As2			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nature, 459(2009)64	R. H. Liu,T. Wu,G. Wu,H. Chen,X. F. Wang,Y. L. Xie,J. J. Ying,Y. J. Yan,Q. J. Li,B. C. Shi,W. S. Chu,Z. Y. Wu,X. H. Chen		
151757	NAT4590064	sample purity is good.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2009																												ThCr2Si2																		K		37.3					37.3						0.37	Fe	91	0.5																																																																																							solid state reaction					A large iron isotope effect in SmFeAsO1-xFx and Ba1-xKxFe2As2			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nature, 459(2009)64	R. H. Liu,T. Wu,G. Wu,H. Chen,X. F. Wang,Y. L. Xie,J. J. Ying,Y. J. Yan,Q. J. Li,B. C. Shi,W. S. Chu,Z. Y. Wu,X. H. Chen		
151758	JPC021382203	impurity : Fe2P(10%). P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.87.  T<SDW> = 142 K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2009																										AB2C2		ThCr2Si2			A	3.9612		13.006												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151759	JPC021382203	P-content determined by Vegard's law. T<SDW> = 136 K.	BaFe2(As,P)2	Ba1Fe2As1.96P0.04	Ba	1	Fe	2	As	1.96	P	0.04																1	2009																										AB2C2		ThCr2Si2			A	3.9603		12.99												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151760	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 2.15.  T<SDW> = 97 K.	BaFe2(As,P)2	Ba1Fe2As1.74P0.26	Ba	1	Fe	2	As	1.74	P	0.26																1	2009																										AB2C2		ThCr2Si2			A	3.9471		12.992												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151761	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.97 T<SDW> = 70 K.	BaFe2(As,P)2	Ba1Fe2As1.6P0.4	Ba	1	Fe	2	As	1.6	P	0.4																1	2009																										AB2C2		ThCr2Si2			A	3.9376		12.876												K		7.2					7.2																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151762	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 0.267	BaFe2(As,P)2	Ba1Fe2As1.52P0.48	Ba	1	Fe	2	As	1.52	P	0.48																1	2009																										AB2C2		ThCr2Si2			A	3.9338		12.864												K		30.1					30.1																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151763	JPC021382203	P-content determined by Vegard's law.	BaFe2(As,P)2	Ba1Fe2As1.36P0.64	Ba	1	Fe	2	As	1.36	P	0.64																1	2009																										AB2C2		ThCr2Si2			A	3.9231		12.805												K		29.1		30			29.1										100																																																																																						solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151764	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.02	BaFe2(As,P)2	Ba1Fe2As1.28P0.72	Ba	1	Fe	2	As	1.28	P	0.72																1	2009																										AB2C2		ThCr2Si2			A	3.9206		12.792												K		22.4					22.4																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151765	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.58	BaFe2(As,P)2	Ba1Fe2As1.06P0.94	Ba	1	Fe	2	As	1.06	P	0.94																1	2009																										AB2C2		ThCr2Si2			A	3.9074		12.724												K		20.8					20.8																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151766	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.69	BaFe2(As,P)2	Ba1Fe2As0.88P1.12	Ba	1	Fe	2	As	0.88	P	1.12																1	2009																										AB2C2		ThCr2Si2			A	3.8952		12.678												K		13.9					13.9																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151767	JPC021382203	P-content determined by Vegard's law. R=R0 + a*T^n,  n = 1.9	BaFe2(As,P)2	Ba1Fe2As0.74P1.26	Ba	1	Fe	2	As	0.74	P	1.26																1	2009																										AB2C2		ThCr2Si2			A	3.8857		12.634												K		7.73					7.73																																																																																																solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151768	JPC021382203	RRR = 20. P-content determined by Vegard's law. R=R0 + a*T^n,  n = 2.16	BaFe2(As,P)2	Ba1Fe2As0.46P1.54	Ba	1	Fe	2	As	0.46	P	1.54																1	2009																										AB2C2		ThCr2Si2			A	3.8697		12.554												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151769	JPC021382203	RRR = 35.  P-content determined by Vegard's law. R=R0 + a*T^n,  n = 2.48	BaFe2(As,P)2	Ba1Fe2As0.2P1.8	Ba	1	Fe	2	As	0.2	P	1.8																1	2009																										AB2C2		ThCr2Si2			A	3.8509		12.489												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151770	JPC021382203	RRR = 75. P-content determined by Vegard's law. R=R0 + a*T^n,  n = 2.58	BaFe2P2	Ba1Fe2P2	Ba	1	Fe	2	P	2																		1	2009																										AB2C2		ThCr2Si2			A	3.8386		12.442												K					4																																																																																																		solid state reaction. mixture - pellet - (quartz tube) - ANN(600K,12h) - ANN(1173K,40h) - reground - (quartz tube) - ANN(1273K,24h) - FC to RT					Superconductivity up to 30 K in the vicinity of the quantum critical point in BaFe2(As1-xPx)2			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 21(2009)382203	Shuai Jiang,Hui Xing,Guofang Xuan,Cao Wang,Zhi Ren,Chunmu Feng,Jianhui Dai,Zhu'an Xu,Guanghan Cao		
151771	EPL08737004	[FeP4] tetradon slightly distorted. bulk-SC(SUS, SP-heat)	LiFeP	Li1Fe1P1	Li	1	Fe	1	P	1																			2009																										ABC			P4/nmm		A	3.692		6.031												K			6	6			6																																																								mJ/mol.K2	16.08																																					Li(3N),FeP		mixture - pellet - (wrapped in Au-foil) - SIN(800C,60min, P=1.8 GPa)					"A new ""111"" type iron pnictide superconductor LiFeP"			Institute of Physics, Chinese Academy of Sciences - Beijing, China	EuroPhys.Lett., 87(2009)37004	Z. Deng,X. C. Wang,Q. Q. Liu,S. J. Zhang,Y. X. Lv,J. L. Zhu,R. C. Yu,C. Q. Jin		
151772	PRB081024518		SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2																		K					1.8																																																																								MTP151772																					MRH151772					single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151773	PRB081024518		Sr(Fe,Ni)2As2	Sr1Fe1.92Ni0.08As2	Sr	1	Fe	1.92	Ni	0.08	As	2																3	2010																										AB2C2		ThCr2Si2																		K					1.8																																																																								MTP151772																					MRH151772					single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151774	PRB081024518	R not to zero at 1.8K. Anisotropy(Hc2) = 2.2 T-independent.	Sr(Fe,Ni)2As2	Sr1Fe1.88Ni0.12As2	Sr	1	Fe	1.88	Ni	0.12	As	2																3	2010																										AB2C2		ThCr2Si2																		K		3.74					3.74										7	Oe	M-H curve					510		1.8	T	resistive, R-0.5Rn								T/K			1.8		MHC151774																																				MTP151772																										single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151775	PRB081024518	optimal dope. Anisotropy(hc2) = 1.5 at T=0.5Tc. Jc(1.8K) = 3 E+4 A/cm2 for H//ab.	Sr(Fe,Ni)2As2	Sr1Fe1.84Ni0.16As2	Sr	1	Fe	1.84	Ni	0.16	As	2																3	2010																										AB2C2		ThCr2Si2																		K		8.65					8.65										95	Oe	M-H curve					800	3600	1.8	T	resistive, R-0.5Rn, linear approx.		25						T/K			2.9		MHC151775																																				MTP151775																										single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151776	PRB081024518		Sr(Fe,Ni)2As2	Sr1Fe1.7Ni0.3As2	Sr	1	Fe	1.7	Ni	0.3	As	2																3	2010																										AB2C2		ThCr2Si2																		K					1.8																																																																								MTP151775																										single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151777	PRB081024518		Sr(Fe,Ni)2As2	Sr1Fe1.8Ni0.2As2	Sr	1	Fe	1.8	Ni	0.2	As	2																3	2010																										AB2C2		ThCr2Si2																		K		7.4					7.4										95	Oe	M-H curve					600		1.8	T	resistive, R-0.5Rn													MHC151777																																																														single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151778	PRB081024518		Sr(Fe,Ni)2As2	Sr1Fe1.78Ni0.22As2	Sr	1	Fe	1.78	Ni	0.22	As	2																3	2010																										AB2C2		ThCr2Si2																		K		2.34					2.34										63	Oe	M-H curve					90		1.8	T	resistive, R-0.5Rn								T/K			1.1		MHC151777																																																														single crystals prepared fromexcess FeAs by annealing in inert gas.					Effective carrier type and field dependence of the reduced-Tc superconducting state in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 81(2010)024518	N. P. Butch,S. R. Saha,X. H. Zhang,K. Kirshenbaum,R. L. Greene,J. Paglione		
151779	EPL08647002		LaOFe(As,P)	La1Fe1As0.8P0.2O1	La	1	Fe	1	As	0.8	P	0.2													O	1		1	2009																												oxypnictide			A	4.0276		8.6846											ZrCuSiAs	K			7				7																																																																																														LaAs,La2O3,FeAs,Fe2As,FeP,Fe2P		solid state reaction. SIN(1373K,40h,in quartz tube) - FC to RT					Superconductivity in LaFeAs1-xPxO: Effect of chemical pressures and bond covalency			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett., 86(2009)47002	Cao Wang,Shuai Jiang,Qian Tao,Zhi Ren,Yuke Li,Linjun Li,Chunmu Feng,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
151780	EPL08647002		LaOFe(As,P)	La1Fe1As0.75P0.25O1	La	1	Fe	1	As	0.75	P	0.25													O	1		1	2009																												oxypnictide			A	4.0237		8.6632											ZrCuSiAs	K		10.3	11				10.3																																																																																														LaAs,La2O3,FeAs,Fe2As,FeP,Fe2P		solid state reaction. SIN(1373K,40h,in quartz tube) - FC to RT					Superconductivity in LaFeAs1-xPxO: Effect of chemical pressures and bond covalency			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett., 86(2009)47002	Cao Wang,Shuai Jiang,Qian Tao,Zhi Ren,Yuke Li,Linjun Li,Chunmu Feng,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
151781	EPL08647002		LaOFe(As,P)	La1Fe1As0.7P0.3O1	La	1	Fe	1	As	0.7	P	0.3													O	1		1	2009																												oxypnictide			A	4.0219		8.6616											ZrCuSiAs	K		10.8	11				10.8	TC151781									65										T	resistivity, WHH	27							T/K	resistivity, R=0.9Rn	3.59																																																						m3/C	-0.0000000057					RH151781			LaAs,La2O3,FeAs,Fe2As,FeP,Fe2P		solid state reaction. SIN(1373K,40h,in quartz tube) - FC to RT					Superconductivity in LaFeAs1-xPxO: Effect of chemical pressures and bond covalency			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett., 86(2009)47002	Cao Wang,Shuai Jiang,Qian Tao,Zhi Ren,Yuke Li,Linjun Li,Chunmu Feng,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
151782	EPL08647002		LaOFe(As,P)	La1Fe1As0.6P0.4O1	La	1	Fe	1	As	0.6	P	0.4													O	1		1	2009																												oxypnictide			A	4.0139		8.633											ZrCuSiAs	K		5					5																																																																																														LaAs,La2O3,FeAs,Fe2As,FeP,Fe2P		solid state reaction. SIN(1373K,40h,in quartz tube) - FC to RT					Superconductivity in LaFeAs1-xPxO: Effect of chemical pressures and bond covalency			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett., 86(2009)47002	Cao Wang,Shuai Jiang,Qian Tao,Zhi Ren,Yuke Li,Linjun Li,Chunmu Feng,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
151783	PRB079224519	mag/str transition at 134 K.	Sr(Fe,Ni)2As2	Sr1Fe1.92Ni0.08As2	Sr	1	Fe	1.92	Ni	0.08	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9222		12.321												K					1.8																																																																																																FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151784	PRB079224519	mag/str transition at 126 K.. R not to zero at 1.8K.	Sr(Fe,Ni)2As2	Sr1Fe1.9Ni0.1As2	Sr	1	Fe	1.9	Ni	0.1	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9221		12.295												K			5.5			5.51	5.5										0																																																																																				FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151785	PRB079224519	mag/str transition at 80 K.	Sr(Fe,Ni)2As2	Sr1Fe1.88Ni0.12As2	Sr	1	Fe	1.88	Ni	0.12	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.927		12.294												K		8.1		5.75		3.81	8.1										11																																																																																				FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151786	PRB079224519	mag/str transition at 36 K. (dC/gamma*Tc) = 0.12	Sr(Fe,Ni)2As2	Sr1Fe1.85Ni0.15As2	Sr	1	Fe	1.85	Ni	0.15	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9251		12.287												K		8.66		7.81		1.12	8.66										100																																														mJ/mol.K2	32	SP-heat	234	SP-heat																																		FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151787	PRB079224519		Sr(Fe,Ni)2As2	Sr1Fe1.82Ni0.18As2	Sr	1	Fe	1.82	Ni	0.18	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9322		12.264												K		9.6	9.8	8.5		0.245	9.6	MTC151786									95.2																																																																																				FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151788	PRB079224519	R not to zero at 1.8K.	Sr(Fe,Ni)2As2	Sr1Fe1.78Ni0.22As2	Sr	1	Fe	1.78	Ni	0.22	As	2																3	2009																										AB2C2		ThCr2Si2			A	3.9308		12.262												K		2.27	3.1			3.19	2.27										0																																																																																				FeAs,NiAs,Sr		mixture - (sealed in alumina crucible in quartz tube) - heat(1200C) - slow cool - quench to RT					Evolution of bulk superconductivity in SrFe2As2 with Ni substitution			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 79(2009)224519	S. R. Saha,N. P. Butch,K. Kirshenbaum,Johnpierre Paglione		
151790	PRB081020509	single crystal (2*0.5*0.1 mm3). R not zero due to dissipation for H//ab. Anisotropy from Hc2 decrease 2 (at Tc) to 0.95 (T=0).	Fe(Te,Se)	Fe1.11Te0.6Se0.4	Fe	1.11	Te	0.6	Se	0.4																		3	2010																										AB																				K		14					14																				T	resistivity, extraporation		47	47					T/K	resistivity		8.9	3.82	MHC151790		A	Hc2		26.5																																																									self-flux method. starting(Fe(Te0.6Se0.4)0.85) - sealed in quartz tube) - heat(920C) - slow cool					Weak anisotropy of the superconducting upper critical field in Fe1.11Te0.6Se0.4 single crystals			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 81(2010)020509	Minghu Fang,Jinhu Yang,F. F. Balakirev,Y. Kohama,J. Singleton,B. Qian,Z. Q. Mao,Hangdong Wang,H. Q. Yuan		
151791	PRB081020510	T-dependence of Nernst coefficient shows much difference between SC-Ca(Fe,Co)2As2 and non-SC-CaFe2As2.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.883		11.725												K																																																																									uV/K	5.03			MTP151791															m3/C	-0.00000000033					MRH151791					Sn-flux method. Ca:Fe:As:Sn = 1.1:2:2.1:40.  heat(1050C,5h) - slow cool(2K/h) to 600C - FC to RT.					Nernst effect in single crystals of the pnictide superconductor CaFe1.92Co0.08As2 and parent compound CaFe2As2			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.B, 81(2010)020510	Marcin Matusiak,Zbigniew Bukowski,Janusz Karpinski		
151792	PRB081020510	Co-content determined by EDX  Tc = 12.6 K at H=13T. T-dependence of Nernst coefficient shows much difference between SC-Ca(Fe,Co)2As2 and non-SC-CaFe2As2.	Ca(Fe,Co)2As2	Ca1Fe1.92Co0.08As2	Ca	1	Fe	1.92	Co	0.08	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.886		11.695												K		20.4					20.4																																																																		uV/K	-1.5			MTP151792															m3/C	-0.00000000048					MRH151792					Sn-flux method. Ca:Fe:Co:As:Sn = 1.1:1.85:0.2:2:40.  heat(1050C,5h) - slow cool(2K/h) to 600C - FC to RT.					Nernst effect in single crystals of the pnictide superconductor CaFe1.92Co0.08As2 and parent compound CaFe2As2			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.B, 81(2010)020510	Marcin Matusiak,Zbigniew Bukowski,Janusz Karpinski		
151793	PRB081014529	[gamma] obtained by fitting using Debye and Einstein models. Tc and [gapene] from SP-heat.	(Ba,K)Fe2As2	Ba0.7K0.3Fe2As2	Ba	0.7	K	0.3	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2																		K		36.5					36.5																																																3.73	14							mJ/mol.K2	53	SP-heat																																						See New J.Phys., 11(2009)025014.					Magnetic and superconducting transitions in Ba1-xKxFe2As2 studied by specific heat			Experimentalphysik V, Center for Electronic Correlations and Magnetism, Institute for Physics, Augsburg University, D-86135 Augsburg, Germany	Phys.Rev.B, 81(2010)014529	Ch. Kant,J. Deisenhofer,A. Gunther,F. Schrettle,A. Loidl,M. Rotter,D. Johrendt		
151794	PRB081014529	[gamma] obtained by fitting using Debye and Einstein models. Tc and [gapene] from SP-heat.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2																		K		37.3					37.3																																																4.14	14							mJ/mol.K2	49	SP-heat																																						See New J.Phys., 11(2009)025014.					Magnetic and superconducting transitions in Ba1-xKxFe2As2 studied by specific heat			Experimentalphysik V, Center for Electronic Correlations and Magnetism, Institute for Physics, Augsburg University, D-86135 Augsburg, Germany	Phys.Rev.B, 81(2010)014529	Ch. Kant,J. Deisenhofer,A. Gunther,F. Schrettle,A. Loidl,M. Rotter,D. Johrendt		
151795	PRB081014529	[gamma] obtained by fitting using Debye and Einstein models. Tc and [gapene] from SP-heat.	(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2																		K		36					36																																																3.67	14							mJ/mol.K2	54	SP-heat																																						See New J.Phys., 11(2009)025014.					Magnetic and superconducting transitions in Ba1-xKxFe2As2 studied by specific heat			Experimentalphysik V, Center for Electronic Correlations and Magnetism, Institute for Physics, Augsburg University, D-86135 Augsburg, Germany	Phys.Rev.B, 81(2010)014529	Ch. Kant,J. Deisenhofer,A. Gunther,F. Schrettle,A. Loidl,M. Rotter,D. Johrendt		
151796	PRB081014529	[gamma] obtained by fitting using Debye and Einstein models. Tc and [gapene] from SP-heat.	(Ba,K)Fe2As2	Ba0.4K0.6Fe2As2	Ba	0.4	K	0.6	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2																		K		29.7					29.7																																																3.57	14							mJ/mol.K2	58	SP-heat																																						See New J.Phys., 11(2009)025014.					Magnetic and superconducting transitions in Ba1-xKxFe2As2 studied by specific heat			Experimentalphysik V, Center for Electronic Correlations and Magnetism, Institute for Physics, Augsburg University, D-86135 Augsburg, Germany	Phys.Rev.B, 81(2010)014529	Ch. Kant,J. Deisenhofer,A. Gunther,F. Schrettle,A. Loidl,M. Rotter,D. Johrendt		
151797	PRB081054507	P-induced SC. P<crit> = 5 GPa. R not to zero at (5GPa, 4.2 K). magnetic transition at Tm = 112 K.. (dTm/dP) = 12.3 K/GPa.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																1	2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K			29		0		29	MTC151797																																																																																															solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151798	PRB081054507	Tc(max) = 24.7 K (P=1.0 GPa).	Ca(Fe,Co)AsF	Ca1Fe0.9Co0.1As1F1	Ca	1	Fe	0.9	Co	0.1	As	1	F	1														1	2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K			23.8				23.8	MTC151798																																																																																															solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151799	PRB081054507		Ca(Fe,Co)AsF	Ca1Fe0.85Co0.15As1F1	Ca	1	Fe	0.85	Co	0.15	As	1	F	1														1	2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K			20.4				20.4	MTC151799																																																																																															solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151800	PRB081054507	Tc(max) = 16.7 K (P=0.4 GPa).	Ca(Fe,Co)AsF	Ca1Fe0.8Co0.2As1F1	Ca	1	Fe	0.8	Co	0.2	As	1	F	1														1	2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K			16.4				16.4	MTC151800																																																																																															solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151801	PRB081054507	P-induced SC. Tc(max) = 21 K at P=12 GPa.	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1		1	2010																										ABCD		oxypnictide																		K			21		0		21																																																																																																solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151802	PRB081054507	Tc(max) = 29.3 K at P=3 GPa	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95		1	2010																										ABCD		oxypnictide																		K			24.9				24.9																																																																																																solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151803	PRB081054507	Tc(max) = 35.3 K at P=4 GPa	La(O,F)FeAs	La1Fe1As1F0.08O0.92	La	1	Fe	1	As	1	F	0.08													O	0.92		1	2010																										ABCD		oxypnictide																		K			30.4				30.4																																																																																																solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151804	PRB081054507	Tc(max) = 43.8 K at P=4 GPa	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2010																										ABCD		oxypnictide																		K			28.6				28.6																																																																																																solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151805	PRB081054507	Tc(max) = 43.5 K at P=6 GPa	La(O,F)FeAs	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86		1	2010																										ABCD		oxypnictide																		K			19				19																																																																																																solid state reaction					Pressure dependence of the superconductor transition temperature of Ca(Fe1-xCox)AsF compounds: A comparison with the effect of pressure on LaFeAsO1-xFx			Department of Physics, College of Humanities and Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Phys.Rev.B, 81(2010)054507	Hironari Okada,Hiroyuki Takahashi,Satoru Matsuishi,Masahiro Hirano,Hideo Hosono,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hiroki Takahashi		
151806	PRB081060501	Co-content by EDX. no traces of SDW. [vols] estimated tobe 75 % from finite [gamma] at 0 K. [gapene] = 4.4 and 1.9 from two gap model using SP-heat data.	Ba(Fe,Co)2As2	Ba1Fe1.85Co0.15As2	Ba	1	Fe	1.85	Co	0.15	As	2																3	2010																										AB2C2		ThCr2Si2																		K		21.4					21.4										75																																						4.4	14							mJ/mol.K2	23.8	SP-heat																																				FeAs,CoAs,Ba		self-flux method.  mixture - (sealed in SiO2 ampoule) - heat(1200C,5h) - cool to 1000C (1C/h).					Calorimetric evidence of multiband superconductivity in Ba(Fe0.925Co0.075)2As2 single crystals			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik, 76021 Karlsruhe, Germany	Phys.Rev.B, 81(2010)060501	F. Hardy,T. Wolf,R. A. Fisher,R. Eder,P. Schweiss,P. Adelmann,H. v. Lohneysen,C. Meingast		
151807	PRB081060501	not SC. Co-content by EDX.	Ba(Fe,Co)2As2	Ba1Fe1.697Co0.306As2	Ba	1	Fe	1.697	Co	0.306	As	2																3	2010																										AB2C2		ThCr2Si2																		K					0.5																																																										mJ/mol.K2	15.8	SP-heat																																				FeAs,CoAs,Ba		self-flux method.  mixture - (sealed in SiO2 ampoule) - heat(1200C,5h) - cool to 1000C (1C/h).					Calorimetric evidence of multiband superconductivity in Ba(Fe0.925Co0.075)2As2 single crystals			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik, 76021 Karlsruhe, Germany	Phys.Rev.B, 81(2010)060501	F. Hardy,T. Wolf,R. A. Fisher,R. Eder,P. Schweiss,P. Adelmann,H. v. Lohneysen,C. Meingast		
151808	PRB081060501	not SC. Co-content by EDX.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2																		K					0.5																																																										mJ/mol.K2	5.3	SP-heat																																				FeAs,CoAs,Ba		self-flux method.  mixture - (sealed in SiO2 ampoule) - heat(1200C,5h) - cool to 1000C (1C/h).					Calorimetric evidence of multiband superconductivity in Ba(Fe0.925Co0.075)2As2 single crystals			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik, 76021 Karlsruhe, Germany	Phys.Rev.B, 81(2010)060501	F. Hardy,T. Wolf,R. A. Fisher,R. Eder,P. Schweiss,P. Adelmann,H. v. Lohneysen,C. Meingast		
151809	MAT8110761	impurity phases: SrF2,SmAs.	(Sr,Sm)FeAsF	Sr0.5Sm0.5Fe1As1F1	Sr	0.5	Sm	0.5	Fe	1	As	1	F	1														1	2008																										ABCD		oxypnictide			A	3.918		8.956											ZrCuSiAs-type	K			56	53.5			53.5																																																																																														SrF2,SrAs,SmAs,Fe2As		solid state reaction					Superconductivity at 56 K in Samarium-doped SrFeAsF			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	cond-mat/0811.0761	G. Wu,Y. L. Xie,H. Chen,M. Zhong,R. H. Liu,B. C. Shi,Q.J.Li,X. F. Wang,T. Wu,Y. J. Yan,J. J. Ying,X. H. Chen		
151810	MAT8110761	impurity phase: SrF2.  R(T) anomaly at 163 K from SDW.	(Sr,Sm)FeAsF	Sr0.8Sm0.2Fe1As1F1	Sr	0.8	Sm	0.2	Fe	1	As	1	F	1														1	2008																										ABCD		oxypnictide			A	3.929		8.958											ZrCuSiAs-type	K					4																																																																																																SrF2,SrAs,SmAs,Fe2As		solid state reaction					Superconductivity at 56 K in Samarium-doped SrFeAsF			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	cond-mat/0811.0761	G. Wu,Y. L. Xie,H. Chen,M. Zhong,R. H. Liu,B. C. Shi,Q.J.Li,X. F. Wang,T. Wu,Y. J. Yan,J. J. Ying,X. H. Chen		
151811	MAT8110761	R(T) anomaly at 173 K from SDW.	SrFeAsF	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																1	2008																										ABCD		oxypnictide			A	3.995		8.961											ZrCuSiAs-type	K					4																																																																																																SrF2,SrAs,SmAs,Fe2As		solid state reaction					Superconductivity at 56 K in Samarium-doped SrFeAsF			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	cond-mat/0811.0761	G. Wu,Y. L. Xie,H. Chen,M. Zhong,R. H. Liu,B. C. Shi,Q.J.Li,X. F. Wang,T. Wu,Y. J. Yan,J. J. Ying,X. H. Chen		
151812	PRL104057001	Cu-intercalated between Se-layers, not substitute for Bi-site. SC for 0.10 < x < 0.15 in CuxBi2Se3. G-L parameter = 50.  R not to zero n-type semiconductor (carrier = 2 E+20 /cm3)	CuxBi2Se3	Cu0.12Bi2Se3	Cu	0.12	Bi	2	Se	3																		3	2010																										A2B3			R3[-]m		A			28.736												K				3.8			3.8										20										T	resistivity					4.6	1.7	0.3						MHC151812		A			140	52																																																						Bi(5N),Cu(4N),Se(5N)		mixture - heat(850C,overnight, in sealed quartz tube) - slow cool to 620C - Q to water.					Superconductivity in CuxBi2Se3 and its Implications for Pairing in the Undoped Topological Insulator			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.Lett., 104(2010)057001	Y. S. Hor,A. J. Williams,J. G. Checkelsky,P. Roushan,J. Seo,Q. Xu,H.W. Zandbergen,A. Yazdani,N. P. Ong,R. J. Cava		
151813	PRL104057001	not SC. Cu substitutes for Bi.	(Bi,Cu)2Se3	Cu0.1Bi1.9Se3	Cu	0.1	Bi	1.9	Se	3																		3	2010																										A2B3																				K					1.8																																																																																																Bi(5N),Cu(4N),Se(5N)		mixture - heat(850C,overnight, in sealed quartz tube) - slow cool to 620C - Q to water.					Superconductivity in CuxBi2Se3 and its Implications for Pairing in the Undoped Topological Insulator			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.Lett., 104(2010)057001	Y. S. Hor,A. J. Williams,J. G. Checkelsky,P. Roushan,J. Seo,Q. Xu,H.W. Zandbergen,A. Yazdani,N. P. Ong,R. J. Cava		
151814	PRL104057004	Pressure effect of structure (LTO,HTT, Charge order) studied.  For P=0, HTT(235K), LTO(54K), charge order(54K).	(La,Ba)2CuO4	La1.875Ba0.125Cu1O4	La	1.875	Ba	0.125	Cu	1															O	4		3	2010																												T																		K		3					3	TC151814																																																																																																				Spontaneous Symmetry Breaking by Charge Stripes in the High Pressure Phase of Superconducting La1.875Ba0.125CuO4			Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.Lett., 104(2010)057004	M.Hucker,M. v. Zimmermann,M. Debessai,J. S. Schilling,J. M. Tranquada,G. D. Gu		
151815	PRL104057007	structure distortion at 62.2 K.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																			2010								45.2																		ABC																				K				9			9																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151816	PRL104057007	structure distortion at 41.1 K.	Na(Fe,Co)As	Na1Fe0.99Co0.01As1	Na	1	Fe	0.99	Co	0.01	As	1																	2010								28																		ABC																				K				17.9			17.9																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151817	PRL104057007		Na(Fe,Co)As	Na1Fe0.975Co0.025As1	Na	1	Fe	0.975	Co	0.025	As	1																	2010																										ABC																				K				21.1			21.1	MTC151817																																																																																															mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151818	PRL104057007		Na(Fe,Co)As	Na1Fe0.95Co0.05As1	Na	1	Fe	0.95	Co	0.05	As	1																	2010																										ABC																				K				16			16																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151819	PRL104057007		Na(Fe,Co)As	Na1Fe0.93Co0.07As1	Na	1	Fe	0.93	Co	0.07	As	1																	2010																										ABC																				K				14			14																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151820	PRL104057007		Na(Fe,Co)As	Na1Fe0.9Co0.1As1	Na	1	Fe	0.9	Co	0.1	As	1																	2010																										ABC																				K				0			0																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151821	PRL104057007		Na(Fe,Ni)As	Na1Fe0.975Ni0.025As1	Na	1	Fe	0.975	Ni	0.025	As	1																	2010																										ABC																				K				15.4			15.4																																																																																																mixture - heat(200C,48h, in sealed Nb tube) - heat(750C,48h, in sealed Nb tube)					Control of the Competition between a Magnetic Phase and a Superconducting Phase in Cobalt-Doped and Nickel-Doped NaFeAs Using Electron Count			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX1 3QR, United Kingdom	Phys.Rev.Lett., 104(2010)057007	Dinah R. Parker,Matthew J. P. Smith,Tom Lancaster,Andrew J. Steele,Isabel Franke,Peter J. Baker,Francis L. Pratt,Michael J. Pitcher,Stephen J. Blundell,Simon J. Clarke		
151822	MMM3221137	impurity phase: U3Co4Ge7	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																			2010																										ABC		TiNiSi	Pnma		A	6.847	4.208	7.229												K		0.65					0.65																																																																																																arc-melting - ANN(800 or 900C,10d)					Magnetism of UCoGe and U3Co4Ge7			Charles University Prague, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Praha 2, Czech Republic	J.Mag.Mag.Mat., 322(2010)1137	Jiri Pospisil,Jana Poltierova Vejpravova,Vladimir Sechovsky		
151823	MMM3221137	not SC.  spontaneous magnetization (ferromagnetic) below Tm = 21 K.	U3Co4Ge7	U3Co4Ge7	U	3	Co	4	Ge	7																			2010							21.5																			A3B4C7					A	4.116		27.5												K					1.8																																																																																																		arc-melting - ANN(800 or 900C,10d)					Magnetism of UCoGe and U3Co4Ge7			Charles University Prague, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Praha 2, Czech Republic	J.Mag.Mag.Mat., 322(2010)1137	Jiri Pospisil,Jana Poltierova Vejpravova,Vladimir Sechovsky		
151824	PHB4050955	RRR = 13.0	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				1	2010																										AB2		2H-NbSe2			A	3.445		12.551												K			7.4				7.4																																																																		uV/K	-3.7			MTP151824	mOhm.cm											0.196												Ga(4N),Nb(2N),Se(5N)		mixture - heat(750C, in quartz tube) - pelletization - SIN(700C,7d)					Transport properties of 2H-NbSe2: Effect of Ga-intercalation			Department of Physics, North Orissa University, Takatpur, Baripada?757003, India	Physica B, 405(2010)955	I. Naik,A.K.Rastogi		
151825	PHB4050955	RRR = 66.7. T<CDW> = 35 K.	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	2010																										AB2		2H-NbSe2																		K			7.4				7.4																																																																		uV/K	-4.08			MTP151825	mOhm.cm											0.068												Ga(4N),Nb(2N),Se(5N)		mixture - heat(750C, in quartz tube) - pelletization - SIN(700C,7d)					Transport properties of 2H-NbSe2: Effect of Ga-intercalation			Department of Physics, North Orissa University, Takatpur, Baripada?757003, India	Physica B, 405(2010)955	I. Naik,A.K.Rastogi		
151826	PHB4050955	Ga-intercalated. RRR = 2.9.	2H-Ga0.05NbSe2	Ga0.05Nb1Se2	Ga	0.05	Nb	1	Se	2																		1	2010																										AB2		2H-NbSe2			A	3.45		12.592												K			5.6				5.6																																																																		uV/K	-6.33			MTP151826	mOhm.cm											0.418												Ga(4N),Nb(2N),Se(5N)		mixture - heat(750C, in quartz tube) - pelletization - SIN(700C,7d)					Transport properties of 2H-NbSe2: Effect of Ga-intercalation			Department of Physics, North Orissa University, Takatpur, Baripada?757003, India	Physica B, 405(2010)955	I. Naik,A.K.Rastogi		
151827	PHB4050955	Ga-intercalated.  RRR = 1.5.	2H-Ga0.1NbSe2	Ga0.1Nb1Se2	Ga	0.1	Nb	1	Se	2																		1	2010																										AB2		2H-NbSe2			A	3.453		12.605												K			2.7				2.7																																																																		uV/K	-11.21			MTP151827	mOhm.cm											1.23												Ga(4N),Nb(2N),Se(5N)		mixture - heat(750C, in quartz tube) - pelletization - SIN(700C,7d)					Transport properties of 2H-NbSe2: Effect of Ga-intercalation			Department of Physics, North Orissa University, Takatpur, Baripada?757003, India	Physica B, 405(2010)955	I. Naik,A.K.Rastogi		
151828	PLA0290571	[t2] from SP-heat. Hall coeffic(77 K) = 1.7 cm3/C. lattice term of SP-heat(beta) = 0.31 mJ/mol.K4	NbS2	Nb1S2	Nb	1	S	2																					1969																										AB2																				K		5.4		5.5			5.4																																																								mJ/mol.K2	10.7	SP-heat	265	SP-heat											mOhm.cm				0.05							0.15																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151829	PLA0290571	[t2] from SP-heat. Hall coeffic(77 K) = 0.6 cm3/C. lattice term of SP-heat(beta) = 0.62 mJ/mol.K4	NbSe2	Nb1Se2	Nb	1	Se	2																					1969																										AB2																				K		6.9		6.9			6.9																																																								mJ/mol.K2	20.5	SP-heat	210	SP-heat											mOhm.cm				0.04							0.18																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151830	PLA0290571	Hall coeffic(77 K) = 2.0 cm3/C. lattice term of SP-heat(beta) = 0.79 mJ/mol.K4	NbTe2	Nb1Te2	Nb	1	Te	2																					1969																										AB2																				K				0.6			0.6																																																								mJ/mol.K2	3	SP-heat	195	SP-heat											mOhm.cm				0.03							0.13																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151831	PLA0290571	[t2] from SP-heat. Hall coeffic(77 K) = 5.0 cm3/C. lattice term of SP-heat(beta) = 0.66 mJ/mol.K4	TaS2	Ta1S2	Ta	1	S	2																					1969																										AB2																				K		1.6		1.5			1.6																																																								mJ/mol.K2	9.1	SP-heat	205	SP-heat											mOhm.cm				0.3							0.6																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151832	PLA0290571	Hall coeffic(77 K) = -0.2 cm3/C. lattice term of SP-heat(beta) = 0.61 mJ/mol.K4	TaSe2	Ta1Se2	Ta	1	Se	2																					1969																										AB2																				K				0.2			0.2																																																								mJ/mol.K2	5.5	SP-heat	215	SP-heat											mOhm.cm				0.04							0.13																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151833	PLA0290571	Hall coeffic(77 K) = 3.2 cm3/C. lattice term of SP-heat(beta) = 0.90 mJ/mol.K4	TaTe2	Ta1Te2	Ta	1	Te	2																					1969																										AB2																				K					0.05																																																										mJ/mol.K2	3	SP-heat	185	SP-heat											mOhm.cm				0.4							0.21																			An energy band model of Nb- and Ta-dichalcogenide superconductors			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 29(1969)571	M.H.van Maaren,H.B.Harland		
151834	PHC4700165	impurity phase(<2%): Nd(OH)3. Metal-to semiconduct transition at 163 K.	NdO(Fe,Rh)As	Nd1Fe0.9Rh0.1As1O1	Nd	1	Fe	0.9	Rh	0.1	As	1													O	1			2010																												oxypnictide			A	3.978		8.537												K			18	15			15										20																																																												TP151834																								Nd,As,Fe,Rh,Fe2O3,FeF2		mixture - press(200MPa) - heat(1150C,48h,in air)					Superconductivity at 15 K in NdFe0.9Rh0.1AsO without F-doping			Institut de Chimie Moleculaire et des Materiaux d'Orsay (UMR CNRS 8182), Bat 410, Univ. Paris-Sud 11, 91405 Orsay, France	Physica C, 470(2010)165	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151835	PHC4700165		Nd(O,F)FeAs	Nd1Fe1As1F0.12O0.88	Nd	1	Fe	1	As	1	F	0.12													O	0.88			2010																												oxypnictide																		K			52				52																																																																						TP151835																								Nd,As,Fe,Rh,Fe2O3,FeF2		mixture - press(200MPa) - heat(1150C,48h,in air)					Superconductivity at 15 K in NdFe0.9Rh0.1AsO without F-doping			Institut de Chimie Moleculaire et des Materiaux d'Orsay (UMR CNRS 8182), Bat 410, Univ. Paris-Sud 11, 91405 Orsay, France	Physica C, 470(2010)165	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151836	PLA0240645	Tc by mutual inductance(21Hz). synthesized at 1200K.	NbTe2	Nb1Te2	Nb	1	Te	2																					1967																																														K		0.74					0.74																																																																																																					Some new superconducting group V<a> dichalcogenides			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 24(1967)645	M.H.van Maaren,G.M.Schaeffer		
151837	PLA0240645	Tc by mutual inductance(21Hz). synthesized at 1250K.	TaS2	Ta1S2	Ta	1	S	2																					1967																																														K		2.1					2.1																																																																																																					Some new superconducting group V<a> dichalcogenides			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 24(1967)645	M.H.van Maaren,G.M.Schaeffer		
151838	PLA0240645	Tc by mutual inductance(21Hz). synthesized at 1250K.	3s-TaSe2	Ta1Se2	Ta	1	Se	2																					1967																																														K		0.22					0.22																																																																																																					Some new superconducting group V<a> dichalcogenides			N.V.Philips Gloeilampenfabrieken, Philips Research Laboratories, Eindhoven, Netherlands	Phys.Lett. A, 24(1967)645	M.H.van Maaren,G.M.Schaeffer		
151840	PHC4700178	impurity phase: SrMoO4. microcrystals( 10 micron-m) = Mo0.45Sr2YCu2.87Ox by EDS	MoSr2YCu2O8	Mo1Sr2Y1Cu2O8	Mo	1	Sr	2	Y	1	Cu	2													O	8			2010									5																			M1212			A	3.815		11.446												K			21				21										14																																																																																				MoO3,Y2O3,CaCO3,SrCO3,CuO	1	mixture - pellet - SIN(750C,24h,in air) - SIN(950C,24h,in O2-flow) - ANN(600C,48h + 400C,24h, in O2-flow)					Superconducting properties of Ca-doped MoSr2YCu2O8-d			Institute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	Physica C, 470(2010)178	N. Balchev,K. Nenkov,G. Mihova,J. Pirov,B. Kunev		
151841	PHC4700178		MoSr2(Y,Ca)Cu2O8	Mo1Sr2Y0.8Ca0.2Cu2O8	Mo	1	Sr	2	Y	0.8	Ca	0.2	Cu	2											O	8			2010									4.8																			M1212			A	3.813		11.438												K			26				26										14																																																																																				MoO3,Y2O3,CaCO3,SrCO3,CuO	1	mixture - pellet - SIN(750C,24h,in air) - SIN(950C,24h,in O2-flow) - ANN(600C,48h + 400C,24h, in O2-flow)					Superconducting properties of Ca-doped MoSr2YCu2O8-d			Institute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	Physica C, 470(2010)178	N. Balchev,K. Nenkov,G. Mihova,J. Pirov,B. Kunev		
151842	PHC4700313	surface /n (001). lattice term in SP (beta) = 0.37 mJ/mol.K4.	2H-TaS2	Ta1S2	Ta	1	S	2																				3	2010																												2H-TaS2			A	3.3119		12.08												K	0.643		0.786				0.7145																																																								mJ/mol.K2	8.5																																							NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151843	PHC4700313	surface /n (001)	2H-NixTaS2	Ni0.02Ta1S2	Ni	0.02	Ta	1	S	2																		3	2010																												2H-TaS2			A	3.3109		12.041												K	3		3.65				3.325																																																																																																NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151844	PHC4700313	surface /n (001). Thermodynamic Hc(0) = 0.2 T. Anisotropy = 3.6. lattice term in SP (beta) = 0.398 mJ/mol.K4.	2H-NixTaS2	Ni0.04Ta1S2	Ni	0.04	Ta	1	S	2																		3	2010																												2H-TaS2			A	3.3109		12.033												K	4.04		4.15				4.095																				T	resistivity,WHH		17.3	4.85										MHC151844		A	from Hc2		82.4	23.1													MSP151844			mJ/mol.K2	13.02	SP-heat	244																																					NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151845	PHC4700313	surface /n (001)	2H-NixTaS2	Ni0.05Ta1S2	Ni	0.05	Ta	1	S	2																		3	2010																												2H-TaS2			A	3.31		12.024												K	1.99		2.62				2.305																																																																																																NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151846	PHC4700313	surface /n (001)	2H-NixTaS2	Ni0.06Ta1S2	Ni	0.06	Ta	1	S	2																		3	2010																												2H-TaS2			A	3.309		12.011												K			1.9				1.9																																																																																																NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151847	PHC4700313	surface /n (001)	2H-NixTaS2	Ni0.08Ta1S2	Ni	0.08	Ta	1	S	2																		3	2010																												2H-TaS2			A	3.308		11.976												K					1.8																																																																																																		NaCl/KCl flux method					Superconductivity of Ni-doping 2H-TaS2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 470(2010)313	L.J. Li,X.D. Zhu,Y.P. Sun,H.C. Lei,B.S. Wang,S.B. Zhang,X.B. Zhu,Z.R. Yang,W.H. Song		
151848	PHC4700357	impurity phase: La2O3,FeAs	(La,Sr)OFeAs	La0.87Sr0.13Fe1As1O1	La	0.87	Sr	0.13	Fe	1	As	1													O	1			2010																												oxypnictide																		K				20			20																																																																																														(La,Sm)As,FeAs,SrO,Fe,Fe2O3		mixture - press to pellet - sealed in quartz tube - heat(940C,4h) - heat(1150-1200C,48h) - slow cool to RT					Coexistence of magnetism and superconductivity in the hole doped FeAs-based superconducting compound			Department of Physics, National Chung Hsing University, Taiwan, ROC	Physica C, 470(2010)357	T.P. Lu,C.C. Wu,W.H. Chou,M.D. Lan		
151849	PHC4700357		(La,Sm,Sr)OFeAs	La0.77Sm0.1Sr0.13Fe1As1O1	La	0.77	Sm	0.1	Sr	0.13	Fe	1	As	1											O	1			2010																												oxypnictide																		K				18			18																																																																																														(La,Sm)As,FeAs,SrO,Fe,Fe2O3		mixture - press to pellet - sealed in quartz tube - heat(940C,4h) - heat(1150-1200C,48h) - slow cool to RT					Coexistence of magnetism and superconductivity in the hole doped FeAs-based superconducting compound			Department of Physics, National Chung Hsing University, Taiwan, ROC	Physica C, 470(2010)357	T.P. Lu,C.C. Wu,W.H. Chou,M.D. Lan		
151850	CEM1830338	not SC. R anomaly at 155K due to structural transformation. Hall coeffic. [RHN] and [carrier] at 30K	PrOFeAs	Pr1Fe1As1O1	Pr	1	Fe	1	As	1															O	1			2010																												oxypnictide	P4/nmm		A	3.9866		8.6042											ZrCuSiAs-type	K					2.5																																																																																							m3/C				-0.00000008397			n/cm3	74000000000000000000	Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151851	CEM1830338	Hall coeffic. [RHN] and [carrier] at 30K	PrO(Fe,Co)As	Pr1Fe0.95Co0.05As1O1	Pr	1	Fe	0.95	Co	0.05	As	1													O	1			2010																												oxypnictide	P4/nmm		A	3.9861		8.6002											ZrCuSiAs-type	K			4.7				4.7																																																																																					m3/C				-0.0000000247			n/cm3	270000000000000000000	Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151852	CEM1830338	Hall coeffic. [RHN] and [carrier] at 30K	PrO(Fe,Co)As	Pr1Fe0.9Co0.1As1O1	Pr	1	Fe	0.9	Co	0.1	As	1													O	1			2010																												oxypnictide	P4/nmm		A	3.986		8.59											ZrCuSiAs-type	K			14.2	13.8			13.8																				T	resistivity,WHH	50.2							T/K	resistivity	5.11																																			uV/K			-25.24	TP151852															m3/C				-0.00000000537			n/cm3	1160000000000000000000	Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151853	CEM1830338		PrO(Fe,Co)As	Pr1Fe0.85Co0.15As1O1	Pr	1	Fe	0.85	Co	0.15	As	1													O	1			2010																												oxypnictide	P4/nmm		A	3.9852		8.5772											ZrCuSiAs-type	K			5.9				5.9																																																																																														Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151854	CEM1830338	R not to zero at 2.5 K	PrO(Fe,Co)As	Pr1Fe0.8Co0.2As1O1	Pr	1	Fe	0.8	Co	0.2	As	1													O	1			2010																												oxypnictide	P4/nmm		A	3.9843		8.5569											ZrCuSiAs-type	K			4				4																																																																																														Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151855	CEM1830338	R not to zero at 2.5 K	PrO(Fe,Co)As	Pr1Fe0.7Co0.3As1O1	Pr	1	Fe	0.7	Co	0.3	As	1													O	1			2010																												oxypnictide	P4/nmm		A	3.9839		8.537											ZrCuSiAs-type	K			4				4																																																																																														Pr,Pr6O11,Co3O4,FeAs,As		mixture - heat(950C,24h,in sealed silica) - disk - wrapped in Ta foil - SIN(1100C,48h,in silica ampoule) - cool to RT					New oxypnictide superconductors: PrOFe1-xCoxAs			Department of Chemistry, Indian Institute of Technology, NewDelhi 110016, India	J.Solid State Chem., 183(2010)338	J. Prakash,S.J.Singh,D.Das,S.Patnaik,A.K.Ganguli		
151856	PRL104087004	two gaps: 1.27 meV(DB) and 0.487 meV. [penet] = 5220 A(DB) and 5320A for two gaps, respectively. [gap] and [penet] measured for various pressure from muon-SR.	FeSex	Fe1Se0.94	Fe	1	Se	0.94																					2010																																														K		8.3					8.3																																									A	muon-SR	5220			meV	1.27																																																	solid state reaction					Evolution of Two-Gap Behavior of the Superconductor FeSe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 104(2010)087004	R. Khasanov,M. Bendele,A. Amato,K. Conder,H. Keller,H.-H. Klauss,H. Luetkens,E. Pomjakushina		
151857	PRB081094506		NdO(Fe,Rh)As	Nd1Fe0.95Rh0.05As1O1	Nd	1	Fe	0.95	Rh	0.05	As	1													O	1		1	2010																												oxypnictide			A	3.9731		8.5638											ZrCuSiAs-type	K			7.1				7.1																																																																		uV/K	-25.7				mOhm.cm											2.59												Fe,Fe2O3,Rh,NdAs		solid state reaction. mixture - press to bar - heat(1150C,48h,in air)					Electronic phase diagram of NdFe1-xRhxAsO			Institut de Chimie Moleculaire et des Materiaux d'Orsay, UMR CNRS 8182, Bat. 410, Univ. Paris-Sud 11, 91405 Orsay, France	Phys.Rev.B, 81(2010)094506	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151858	PRB081094506		NdO(Fe,Rh)As	Nd1Fe0.9Rh0.1As1O1	Nd	1	Fe	0.9	Rh	0.1	As	1													O	1		1	2010																												oxypnictide			A	3.9782		8.5372											ZrCuSiAs-type	K			16.6			1.8	16.6	TC151858									20										T	resistivity,WHH	100							T/K	resistivity	9			HC151858																																uV/K	-33.7			TP151858	mOhm.cm											2.2												Fe,Fe2O3,Rh,NdAs		solid state reaction. mixture - press to bar - heat(1150C,48h,in air)					Electronic phase diagram of NdFe1-xRhxAsO			Institut de Chimie Moleculaire et des Materiaux d'Orsay, UMR CNRS 8182, Bat. 410, Univ. Paris-Sud 11, 91405 Orsay, France	Phys.Rev.B, 81(2010)094506	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151859	PRB081094506		NdO(Fe,Rh)As	Nd1Fe0.85Rh0.15As1O1	Nd	1	Fe	0.85	Rh	0.15	As	1													O	1		1	2010																												oxypnictide			A	3.9829		8.5139											ZrCuSiAs-type	K			14.7				14.7																																																																							mOhm.cm											1.76												Fe,Fe2O3,Rh,NdAs		solid state reaction. mixture - press to bar - heat(1150C,48h,in air)					Electronic phase diagram of NdFe1-xRhxAsO			Institut de Chimie Moleculaire et des Materiaux d'Orsay, UMR CNRS 8182, Bat. 410, Univ. Paris-Sud 11, 91405 Orsay, France	Phys.Rev.B, 81(2010)094506	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151860	PRB081094506		NdO(Fe,Rh)As	Nd1Fe0.8Rh0.2As1O1	Nd	1	Fe	0.8	Rh	0.2	As	1													O	1		1	2010																												oxypnictide			A	3.9875		8.4965											ZrCuSiAs-type	K			10				10																																																																		uV/K	-40.8			TP151860	mOhm.cm											1.53												Fe,Fe2O3,Rh,NdAs		solid state reaction. mixture - press to bar - heat(1150C,48h,in air)					Electronic phase diagram of NdFe1-xRhxAsO			Institut de Chimie Moleculaire et des Materiaux d'Orsay, UMR CNRS 8182, Bat. 410, Univ. Paris-Sud 11, 91405 Orsay, France	Phys.Rev.B, 81(2010)094506	David Berardan,Lidong Zhao,Loreynne Pinsard-Gaudart,Nita Dragoe		
151861	PRL104067002	underdoped. Thermal conductivity k: k/T = a + b*T^n, where n = 1 - 1.5 for T < 0.25 K.	Ba(Fe,Co)2As2	Ba1Fe1.904Co0.096As2	Ba	1	Fe	1.904	Co	0.096	As	2																	2010																										AB2C2		ThCr2Si2																		K	17.1						17.1																																																																							mOhm.cm							0.203																							Doping Dependence of Heat Transport in the Iron-Arsenide Superconductor Ba(Fe1-xCox)2As2 From Isotropic to a Strongly k-Dependent Gap Structure			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.Lett., 104(2010)067002	M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,X. G. Luo,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,R. Prozorov,Louis Taillefer		
151862	PRL104067002	optimal-doped. Thermal conductivity k: k/T = a + b*T^n, where n = 1 - 1.5 for T < 0.25 K.	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																	2010																										AB2C2		ThCr2Si2																		K	22.2						22.2																																																																							mOhm.cm							0.062																							Doping Dependence of Heat Transport in the Iron-Arsenide Superconductor Ba(Fe1-xCox)2As2 From Isotropic to a Strongly k-Dependent Gap Structure			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.Lett., 104(2010)067002	M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,X. G. Luo,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,R. Prozorov,Louis Taillefer		
151863	PRL104067002	overdoped. Thermal conductivity k: k/T = a + b*T^n, where n = 1 - 1.5 for T < 0.25 K.	Ba(Fe,Co)2As2	Ba1Fe1.784Co0.216As2	Ba	1	Fe	1.784	Co	0.216	As	2																	2010																										AB2C2		ThCr2Si2																		K	14.6						14.6																																																																							mOhm.cm							0.059																							Doping Dependence of Heat Transport in the Iron-Arsenide Superconductor Ba(Fe1-xCox)2As2 From Isotropic to a Strongly k-Dependent Gap Structure			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.Lett., 104(2010)067002	M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,X. G. Luo,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,R. Prozorov,Louis Taillefer		
151864	PRL104067002	overdoped. Thermal conductivity k: k/T = a + b*T^n, where n = 1 - 1.5 for T < 0.25 K.	Ba(Fe,Co)2As2	Ba1Fe1.772Co0.228As2	Ba	1	Fe	1.772	Co	0.228	As	2																	2010																										AB2C2		ThCr2Si2																		K	10.1						10.1																																																																							mOhm.cm							0.059																							Doping Dependence of Heat Transport in the Iron-Arsenide Superconductor Ba(Fe1-xCox)2As2 From Isotropic to a Strongly k-Dependent Gap Structure			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.Lett., 104(2010)067002	M. A. Tanatar,J.-Ph. Reid,H. Shakeripour,X. G. Luo,N. Doiron-Leyraud,N. Ni,S. L. Bud'ko,P. C. Canfield,R. Prozorov,Louis Taillefer		
151865	SSC1500411	resistivity masx: R(max) at 30 K. GL parameter: k = 37.  (dC/gamma*Tc) = 1.74	Ce2PdIn8	Ce2Pd1In8	Ce	2	Pd	1	In	8																		1	2010					nyu-B/mol	2.41	-41.8																			AB2C8		Ho2CoGa8																		K			0.7				0.7																				T	resistivity, extraporation	2.5							T/K	resistivity	13.5			MHC151865		A	from Hc2	115			A		4220											J/mol.K2	1.5	mJ/mol.K2	1220	SP-heat	193	SP-heat											uOhm.cm							6.4																		arc-melting in Ar with controlled (O2+H2O) gas. -- wrapped in Ta foil - ANN(700C,5w, in evacuated quartz tube)					Heavy-fermion superconductivity in Ce2PdIn8			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410, 50-950 Wrodaw 2, Poland	Solid State Commun., 150(2010)411	D. Kaczorowski,D. Gnida,A.P. Pikul,V.H. Tran		
151866	PRB081020503	consisting of single crystals (100*100*50 um3). NMR of <31>P and <75>As were measured.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																1	2010																										AB2C2		ThCr2Si2																		K				30			30																																																																																																					<31>P and <75>As NMR evidence for a residual density of states at zero energy in superconducting BaFe2(As0.67P0.33)2			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)020503	Yusuke Nakai,Tetsuya Iye,Shunsaku Kitagawa,Kenji Ishida,Shigeru Kasahara,Takasada Shibauchi,Yuji Matsuda,Takahito Terashima		
151867	PRB081060509	optical conductivity measured. thickness d = 90 nm.	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																4	2010																										AB2C2		ThCr2Si2																		K		20	22			2	20																																									A	optical conductivity	3600			meV	1.85	2.1	2																																															deposited on (001)(La,Sr)(Al,Ta)O3 substrates by PLD					Direct observation of the superconducting energy gap in the optical conductivity of the iron pnictide superconductor Ba(Fe0.9Co0.1)2As2			Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany	Phys.Rev.B, 81(2010)060509	B. Gorshunov,D. Wu,A. A. Voronkov,P. Kallina,K. Iida,S. Haindl,F. Kurth,L. Schultz,B. Holzapfel,M. Dressel		
151868	PRB081092506	epitaxial films, thickness d=1000 A. O-content not given. Tc sensitive to O-content. Hc2 defined as Tc(on) for H perpendicular to film plane. O may substituts for Te.	FeTe:O	Fe1.08Te1Ox	Fe	1.08	Te	1																	O	x		5	2010																										AB		PbO			A	3.821		6.275												K	8		12				10																				T	resistivity,WHH	200							T/K	resistivity	23			MHC151868																																																														epitaxial films grown on (100)STO substrates. deposited by laser under about  1 E-4 Torr O2 atmosphere.					Superconductivity in epitaxial thin films of Fe1.08Te:Ox			Department of Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 81(2010)092506	Weidong Si,Qing Jie,Lijun Wu,Juan Zhou,Genda Gu,P. D. Johnson,Qiang Li		
151869	APL094012503	small amount of impurity phase.	Fe(Te,S)	Fe1Te0.9S0.1	Fe	1	Te	0.9	S	0.1																		1	2009																																														K			10				10																																																																																														Fe,Te,S powder		mixture - heat(800C,12h,in evacuated quartz tube)					Superconductivity in S-substituted FeTe			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Appl.Phys.Lett., 94(2009)012503	Yoshikazu Mizuguchi,Fumiaki Tomioka,Shunsuke Tsuda,Takahide Yamaguchi,Yoshihiko Takano		
151870	APL094012503	small amount of impurity phase. Hc2(0) and Hirr(0) are 102 and 56 T using linear extraporation.	Fe(Te,S)	Fe1Te0.8S0.2	Fe	1	Te	0.8	S	0.2																		1	2009																																														K	7.8		10.5	8.6			8.6																				T	resistivity,WHH	70														A	from Hc2	22																																																								Fe,Te,S powder		mixture - heat(800C,12h,in evacuated quartz tube)					Superconductivity in S-substituted FeTe			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Appl.Phys.Lett., 94(2009)012503	Yoshikazu Mizuguchi,Fumiaki Tomioka,Shunsuke Tsuda,Takahide Yamaguchi,Yoshihiko Takano		
151871	APL094012503	no impurity phases. S-content less than starting compositions.	Fe(Te,S)	Fe1Te0.8S0.2	Fe	1	Te	0.8	S	0.2																		1	2009																													P4/nmm		A	3.8123		6.2444												K	2.8		8.8	8.6			8.6																																																																																														TaS,Fe,Te		mixture - heat(600C,12h) - reground - pellet - heat(600C,12h, in evacuated quartz tube)					Superconductivity in S-substituted FeTe			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Appl.Phys.Lett., 94(2009)012503	Yoshikazu Mizuguchi,Fumiaki Tomioka,Shunsuke Tsuda,Takahide Yamaguchi,Yoshihiko Takano		
151872	SSC0960539		Ba4C60	Ba4C60	Ba	4	C	60																					1995																												fullerene			A	11.25	11.69	10.9												K				6.8			6.8																				T	susceptibility, WHH	2.4							T/K	susceptibility	0.35			MHC151872		A	from Hc2	116																																																															Superconductivity of Ba doped C60 - Superconductivity results and upper critical field				Solid State Commun., 96(1995)539	M.Baenitz,M.Heinze,K.Luders,H.Werner,R.Schlogl,M.Weiden,G.Sparn,F.Steglich		
151873	PCS0710491	O-content determined to be 0.67(optimal). samples with 0.4=<x=<0.8 were measured. SP-heat analyzed using C<ph> = Debye + Einstein, where Einstein-T = 360 K.. (dC/gamma*Tc) = 1.1	SmOxFeAs	Sm1Fe1As1O0.67	Sm	1	Fe	1	As	1															O	0.6	0.67		2010																												oxypnictide	P4/nmm		A	3.90236		8.43148												K		55		55		1.4	55										100																																				meV	10.85	4.57	14										210	SP-heat											mOhm.cm							0.09														n/cm3	1000000000000000000000	SmAs,Fe,Fe2O3		mixture - sealed in BN crucible covered by Pt foil - SIN(1300C,2h,P=3GPa)					Superconducting properties of SmFeAsO1-x prepared under high-pressure condition			WPI and Department of Physics, Graduate School of Science, Tohoku University, Japan	J.Phys.Chem.Solids, 71(2010)491	Jing Ju,Khuong Huynh,Jun Tang,Zhaofei Li,Masanori Watahiki,Kazumi Sato,Hidenori Terasaki,Eiji Ohtani,Hirotsugu Takizawa,Katsumi Tanigaki		
151874	PCS0710700	single crystals from large grains. J//<110> parallel direction. Hc2 defined as R=0. RRR = 19. Hc1(T) = Hc1(0)(1-t^2). GL parameter = 120. thermodynamic-Hc(0) = 0.12 T.	Rh17S15	Rh17S15	Rh	17	S	15																				3	2010																																													cubic	K	5.4						5.4			K/GPa	-0.17							Oe	M -H deviation		33						T	resistivity,WHH			20.5					T/K	resistivity		6	5.6	MHC151874		A	from Hc2		40		A	from Hc1		4900																											uOhm.cm							3.5																Rh(4N),S(5N)		crystals grown by mineralization.  mixture - pellet(under pressure) - heat to 1150C - cool to 1100C (2 C/h) - rapid cool to RT					Superconducting properties in Rh17S15 under magnetic field and pressure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Chem.Solids, 71(2010)700	Rikio  Settai,Keisuke Katayama,Hiroshi Muranaka,Tetsuya Takeuchi,Arumugam Thamizhavel,Ilya Sheikin,Y. Onuki		
151875	CEM1830769	nominal = FeTe	Fe(Te,Se)	Fe1.087Te1	Fe	1.087	Te	1																				3	2010							67																					Cu2Sb	P4/nmm		A	3.826		6.273												K					1.8																																																																																																		crystals grown by Bridgeman-Stockbarger method					Effect of Fe excess on structural, magnetic and superconducting properties of single-crystalline Fe1+xTe1-ySey				J.Solid State Chem., 183(2010)769	R. Viennois,E. Giannini,D.van der Marel,R.  Cerny		
151876	CEM1830769	nominal = FeTe0.8Se0.2	Fe(Te,Se)	Fe1.049Te0.79Se0.21	Fe	1.049	Te	0.79	Se	0.21																		3	2010							14																					Cu2Sb	P4/nmm		A	3.815		6.187												K					1.8																																																																																																		crystals grown by Bridgeman-Stockbarger method					Effect of Fe excess on structural, magnetic and superconducting properties of single-crystalline Fe1+xTe1-ySey				J.Solid State Chem., 183(2010)769	R. Viennois,E. Giannini,D.van der Marel,R.  Cerny		
151877	CEM1830769	nominal = Fe0.9Te0.8Se0.2	Fe(Te,Se)	Fe1.035Te0.78Se0.22	Fe	1.035	Te	0.78	Se	0.22																		3	2010																												Cu2Sb	P4/nmm		A	3.803		6.136												K				6			6																																																																																																crystals grown by Bridgeman-Stockbarger method					Effect of Fe excess on structural, magnetic and superconducting properties of single-crystalline Fe1+xTe1-ySey				J.Solid State Chem., 183(2010)769	R. Viennois,E. Giannini,D.van der Marel,R.  Cerny		
151878	CEM1830769	nominal = Fe0.9Te0.7Se0.3	Fe(Te,Se)	Fe1.013Te0.68Se0.32	Fe	1.013	Te	0.68	Se	0.32																		3	2010																												Cu2Sb	P4/nmm		A	3.806		6.187												K				11			11																																																																																																crystals grown by Bridgeman-Stockbarger method					Effect of Fe excess on structural, magnetic and superconducting properties of single-crystalline Fe1+xTe1-ySey				J.Solid State Chem., 183(2010)769	R. Viennois,E. Giannini,D.van der Marel,R.  Cerny		
151879	JAC4810065	not annealed	(Cu,Te,Li)Ba2(Ca,Mg)2(Cu,Co)3O10	Tl0.25Li0.25Ba2Ca1Mg1Cu3.45Co0.05O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	1	Mg	1	Cu	3.45	Co	0.05							O	10-z			2009																												Cu1223																		K	112						112																																																																																																solid state reaction. (precursor+Tl2O3) - heat(840C,10min) - Q to RT					Superconductivity in Co doped Cu0.5Tl0.5Ba2(CaM)Cu2.95Co0.05O10-z (M= Mg, Be) samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloy Compd., 481(2009)65	A.A. Khurram,Anayat Ullah,Nawazish A. Khan		
151880	JAC4810065	post annealed in O2	(Cu,Tl,Li)Ba2(Ca,Be)2(Cu,Co)3O10	Tl0.25Li0.25Ba2Ca1Be1Cu3.45Co0.05O10-z	Tl	0.25	Li	0.25	Ba	2	Ca	1	Be	1	Cu	3.45	Co	0.05							O	10-z			2009																												Cu1223																		K	105						105																																																																																																solid state reaction. (precursor+Tl2O3) - heat(840C,10min) - Q to RT					Superconductivity in Co doped Cu0.5Tl0.5Ba2(CaM)Cu2.95Co0.05O10-z (M= Mg, Be) samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloy Compd., 481(2009)65	A.A. Khurram,Anayat Ullah,Nawazish A. Khan		
151881	JAC4810065	not annealed	(Cu,Tl)Ba2Ca2(Cu,Co)3O10	Tl0.5Ba2Ca2Cu3.45Co0.05O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3.45	Co	0.05											O	10-z			2009																												Cu1223																		K	104						104																																																																																																solid state reaction. (precursor+Tl2O3) - heat(840C,10min) - Q to RT					Superconductivity in Co doped Cu0.5Tl0.5Ba2(CaM)Cu2.95Co0.05O10-z (M= Mg, Be) samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloy Compd., 481(2009)65	A.A. Khurram,Anayat Ullah,Nawazish A. Khan		
151882	JAC4810065	not annealed	(Cu,Tl)Ba2(Ca,Mg)2(Cu,Co)3O10	Tl0.5Ba2Ca1Mg1Cu3.45Co0.05O10-z	Tl	0.5	Ba	2	Ca	1	Mg	1	Cu	3.45	Co	0.05									O	10-z			2009																												Cu1223																		K	96						96																																																																																																solid state reaction. (precursor+Tl2O3) - heat(840C,10min) - Q to RT					Superconductivity in Co doped Cu0.5Tl0.5Ba2(CaM)Cu2.95Co0.05O10-z (M= Mg, Be) samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloy Compd., 481(2009)65	A.A. Khurram,Anayat Ullah,Nawazish A. Khan		
151883	JAC4810065	not annealed	(Cu,Tl)Ba2(Ca,Be)2(Cu,Co)3O10	Tl0.5Ba2Ca1Be1Cu3.45Co0.05O10-z	Tl	0.5	Ba	2	Ca	1	Be	1	Cu	3.45	Co	0.05									O	10-z			2009																												Cu1223																		K	90						90																																																																																																solid state reaction. (precursor+Tl2O3) - heat(840C,10min) - Q to RT					Superconductivity in Co doped Cu0.5Tl0.5Ba2(CaM)Cu2.95Co0.05O10-z (M= Mg, Be) samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	J.Alloy Compd., 481(2009)65	A.A. Khurram,Anayat Ullah,Nawazish A. Khan		
151884	JPS079024702	P-induced SC. magnetic easy axis //[001]. Neel-T = 4.1 & 2.9 K for H//[001]. Curie-T = -129 K(H//[100] and 54 K (H//[001]. SC properties for P=10.8 GPa.	CePd5Al2	Ce1Pd5Al2	Ce	1	Pd	5	Al	2																		3	2010																										AB2C5		ZrNi2Al5																		K			0.9		0		0.9																				kOe	resistive, extraporation		6.8	4.5					T/K	resistivity		10	1.8	MHC151884																																																														Bridgman method					Magnetic and Fermi Surface Properties of CePd5Al2 and PrPd5Al2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 79(2010)024702	Yasunori NAKANO,Fuminori HONDA,Tetsuya TAKEUCHI,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Etsuji YAMAMOTO,Yoshinori HAGA,Rikio SETTAI,Hiroshi YAMAGAMI,Yoshichika ONUKI		
151885	JPS079033704	structural transition at 150 K.	LaRu2Zn20	La1Ru2Zn20	La	1	Ru	2	Zn	20																		3	2010																										AB2C20		CeCr2Al20			A	14.9263														K	0.2			0.2			0.2																																																																																																single crystals were grown by self-flux method					Superconductivity and Structural Phase Transitions in Caged Compounds RT2Zn20 (R=La,Pr, T=Ru,Ir)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 79(2010)033704	Takahiro ONIMARU,Keisuke T. MATSUMOTO,Yukihiro F. INOUE,Kazunori UMEO,Yuta SAIGA,Yoshitaka MATSUSHITA,Ryuji TAMURA,Kazue NISHIMOTO,Isao ISHII,Takashi SUZUKI,Toshiro TAKABATAKE		
151886	JPS079033704	structural transition at 138 K.	PrRu2Zn20	Pr1Ru2Zn20	Pr	1	Ru	2	Zn	20																		3	2010					nyu-B/Pr	3.5	-5.6																			AB2C20		CeCr2Al20			A	14.3467														K					0.04																																																																																																		single crystals were grown by self-flux method					Superconductivity and Structural Phase Transitions in Caged Compounds RT2Zn20 (R=La,Pr, T=Ru,Ir)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 79(2010)033704	Takahiro ONIMARU,Keisuke T. MATSUMOTO,Yukihiro F. INOUE,Kazunori UMEO,Yuta SAIGA,Yoshitaka MATSUSHITA,Ryuji TAMURA,Kazue NISHIMOTO,Isao ISHII,Takashi SUZUKI,Toshiro TAKABATAKE		
151887	JPS079033704	structural transition at 200 K..  (dC/gamma*Tc) = 0.53	LaIr2Zn20	La1Ir2Zn20	La	1	Ir	2	Zn	20																		3	2010																										AB2C20		CeCr2Al20			A	14.3535														K	0.6			0.6			0.6																																																					MSP151887			mJ/mol.K2	14.4																																							single crystals were grown by self-flux method					Superconductivity and Structural Phase Transitions in Caged Compounds RT2Zn20 (R=La,Pr, T=Ru,Ir)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 79(2010)033704	Takahiro ONIMARU,Keisuke T. MATSUMOTO,Yukihiro F. INOUE,Kazunori UMEO,Yuta SAIGA,Yoshitaka MATSUSHITA,Ryuji TAMURA,Kazue NISHIMOTO,Isao ISHII,Takashi SUZUKI,Toshiro TAKABATAKE		
151888	JPS079033704		PrIr2Zn20	Pr1Ir2Zn20	Pr	1	Ir	2	Zn	20																		3	2010					nyu-B/Pr	3.49	-2.3																			AB2C20		CeCr2Al20			A	14.2729														K	0.05			0.05			0.05																																																																																																single crystals were grown by self-flux method					Superconductivity and Structural Phase Transitions in Caged Compounds RT2Zn20 (R=La,Pr, T=Ru,Ir)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 79(2010)033704	Takahiro ONIMARU,Keisuke T. MATSUMOTO,Yukihiro F. INOUE,Kazunori UMEO,Yuta SAIGA,Yoshitaka MATSUSHITA,Ryuji TAMURA,Kazue NISHIMOTO,Isao ISHII,Takashi SUZUKI,Toshiro TAKABATAKE		
151889	MRB0450392		LaO(Fe,Rh)As	La1Fe0.95Rh0.05As1O1	La	1	Fe	0.95	Rh	0.05	As	1													O	1		1	2010																												oxypnictide			A	4.0364		8.7147												K			12				12																																																																																														La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151890	MRB0450392	Hc2(0) > 4T	LaO(Fe,Rh)As	La1Fe0.9Rh0.1As1O1	La	1	Fe	0.9	Rh	0.1	As	1													O	1		1	2010																												oxypnictide			A	4.0396		8.7												K			16	14			14																																																																																														La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151891	MRB0450392	R not zero at 5K.	LaO(Fe,Rh)As	La1Fe0.85Rh0.15As1O1	La	1	Fe	0.85	Rh	0.15	As	1													O	1		1	2010																												oxypnictide			A	4.0431		8.6838												K			14				14																																																																																														La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151892	MRB0450392		LaO(Fe,Rh)As	La1Fe0.8Rh0.2As1O1	La	1	Fe	0.8	Rh	0.2	As	1													O	1		1	2010																												oxypnictide			A	4.0503		8.6662												K					5																																																																																																La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151893	MRB0450392		LaORhAs	La1Rh1As1O1	La	1	Rh	1	As	1															O	1		1	2010																												oxypnictide			A	4.1226		8.4692												K					5																																																																																																La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151894	MRB0450392		La(O,F)RhAs	La1Rh1As1F0.13O0.87	La	1	Rh	1	As	1	F	0.13													O	0.87		1	2010																												oxypnictide																		K					5																																																																																																La2O3,La,LaF,Fe,Rh,As		mixture - pellet - heat(400C,12h - 850C,12h - 1090C,48h with ramp rate (300C/h), in evacuated fused silica)					Synthesis of LaRhAsO and superconductivity within the LaFe1-xRhxAsO system			Department of Chemistry, Oregon State University, Corvallis, OR 97331, USA	Mat.Res.Bull., 45(2010)392	Sean Muir,A.W. Sleight,M.A. Subramanian		
151895	JPS079014707	basal plane spacing d = 9.3 A.	Li0.16ZrNCl	Li0.16Zr1N1Cl1	Li	0.16	Zr	1	N	1	Cl	1																	2010																																														K				12.6			12.6																																																																																																					Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151896	JPS079014707	M=THF(=tetrahydrofuran). y not given(maybe 0.3). basal plane spacing d = 14.9 A	Li0.16(THF)yZrNCl	Li0.16M0.3Zr1N1Cl1	Li	0.16	M	0.3	Zr	1	N	1	Cl	1															2010																																														K				15			15																																																																																																					Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151897	JPS079014707	M=PC(=propylen carbonate). y is not given. basal plane spacing d = 27.8 A.	Li0.16(PC)yZrNCl	Li0.16M1Zr1N1Cl1	Li	0.16	M	1	Zr	1	N	1	Cl	1															2010																																														K				15			15																																																																																																					Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151898	JPS079014707	basal plane spacing d = 10.6 A.	Na0.28HfNCl	Na0.28Hf1N1Cl1	Na	0.28	Hf	1	N	1	Cl	1																	2010																																														K			23.1	22.8			22.8																																																																																																					Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151899	JPS079014707	M=PC(=propylen carbonate). y is not given. basal plane spacing d = 22.2 A.	Na0.28(PC)HfNCl	Na0.28M1Hf1N1Cl1	Na	0.28	M	1	Hf	1	N	1	Cl	1															2010																																														K			25.3	24.6			24.6																																																																																																					Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151900	JPS079014707	M=THF(=tetrahydrofuran). y not given(maybe 0.3). basal plane spacing d = 18.7 A.	Li0.50(THF)yHfNCl	Li0.5M0.3Hf1N1Cl1	Li	0.5	M	0.3	Hf	1	N	1	Cl	1															2010																																														K			25.5	25.5			25.5																																		MHC151900																																																																			Effect of Swelling on the Superconducting Characteristics in Electron-Doped beta-ZrNCl and HfNCl			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashihiroshima, Hiroshima 739-8527, Japan	J.Phys.Soc.Jpn, 79(2010)014707	Ken-ichi HOTEHAMA,Takeshi KOIWASAKI,Keita UMEMOTO,Shoji YAMANAKA,Hideki TOU		
151901	PRB081094511	P-induced SC. Tc(4.0 GPa) = 1.8 K. The values of Tc and Tn are measured by SP-heat and SUS at P=5.6 GPa.	Sr2Ca12Cu24O41	Sr2Ca12Cu24O41	Sr	2	Ca	12	Cu	24															O	41		3	2010								5.05																				LAD																		K				9.1	0		9.1	PH151901																																																																																															TSFZ method					Coexistence of bulk superconducting and antiferromagnetic order in the spin-ladder system Sr2Ca12Cu24O41			INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble, France	Phys.Rev.B, 81(2010)094511	S. Vanishri,D. Braithwaite,B. Salce,C. Marin,J. Flouquet		
151902	PHC2720335		YBa2Cu4O8	Y1Ba2Cu4O8	Y	1	Ba	2	Cu	4															O	8		1	1996																											3	Y124			A	3.8305	3.8659	27.19												K	78.1	79.8				3	79.8																																																																							mOhm.cm											0.89												Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151903	PHC2720335		YBa2(Cu,Co)4O8	Y1Ba2Cu3.96Co0.04O8	Y	1	Ba	2	Cu	3.96	Co	0.04													O	8		1	1996																											3	Y124			A	3.8393	3.8612	27.19												K	57.9						57.9																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151904	PHC2720335	dTc/dx = 21 K/at%Co	YBa2(Cu,Co)4O8	Y1Ba2Cu3.92Co0.08O8	Y	1	Ba	2	Cu	3.92	Co	0.08													O	8		1	1996																											3	Y124			A	3.8471	3.8561	27.19												K	36.2						36.2																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151905	PHC2720335		YBa2(Cu,Co)4O8	Y1Ba2Cu3.88Co0.12O8	Y	1	Ba	2	Cu	3.88	Co	0.12													O	8		1	1996																											2	Y124			A	3.8517		27.19												K	16.9						16.9																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151906	PHC2720335		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.96Ni0.04O8	Y	1	Ba	2	Cu	3.96	Ni	0.04													O	8		1	1996																											3	Y124			A	3.832	3.8648	27.191												K	62.4						62.4																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151907	PHC2720335		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.92Ni0.08O8	Y	1	Ba	2	Cu	3.92	Ni	0.08													O	8		1	1996																											3	Y124			A	3.831	3.8649	27.191												K	44.6						44.6																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151908	PHC2720335		YBa2(Cu,Ni)4O8	Y1Ba2Cu3.88Ni0.12O8	Y	1	Ba	2	Cu	3.88	Ni	0.12													O	8		1	1996																											3	Y124			A	3.831	3.8556	27.191												K	28.5						28.5																																																																																														Y2O3,Ba(NO3)2,CuO,Co3O4,NiO		mixture - preheat(700C,30min) - press to pellet - heat(815C,24h) - cool (4C/min).  process repeated several times.					Comparison of Co and Ni doping at copper sites in Y-124 high temperature superconductor			National Physical Laboratory, Dr.K.S. Krishnan Marg, New Delhi-110002, India	Physica.C,272(1996)335-341	M. Verma,V.S. Tomar		
151909	PRB081094524	RRR = 0.387. T<CDW> = 200K.	TiSe2	Ti1Se2	Ti	1	Se	2																					2010																												TX2				3.5382		6.01											1H-TiSe2	K					0.3																																																																																																Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151910	PRB081094524	Pd-intercalated to TiSe2 layers. RRR = 2.20	PdxTiSe2	Pd0.11Ti1Se2	Pd	0.11	Ti	1	Se	2																			2010																												TX2				3.5468		6.0339											1H-TiSe2	K	1.82						1.82																																																																																														Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151911	PRB081094524	Pd-intercalated to TiSe2 layers. RRR = 2.09	PdxTiSe2	Pd0.12Ti1Se2	Pd	0.12	Ti	1	Se	2																			2010																												TX2				3.5473		6.0337											1H-TiSe2	K	1.93						1.93																																																								mJ/mol.K2	3.31																																					Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151912	PRB081094524	Pd-intercalated to TiSe2 layers. RRR = 0.58. T<CDW> = 158 K.	PdxTiSe2	Pd0.08Ti1Se2	Pd	0.08	Ti	1	Se	2																			2010																												TX2				3.543		6.024											1H-TiSe2	K					0.3																																																										mJ/mol.K2	2.03																																					Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151913	PRB081094524	Pd-intercalated to TiSe2 layers. RRR = 1.95	PdxTiSe2	Pd0.14Ti1Se2	Pd	0.14	Ti	1	Se	2																			2010																												TX2				3.5516		6.0434											1H-TiSe2	K					0.3																																																										mJ/mol.K2	2.8																																					Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151914	PRB081094524	Pd-intercalated to TiSe2 layers. RRR = 1.49	PdxTiSe2	Pd0.1Ti1Se2	Pd	0.1	Ti	1	Se	2																			2010																												TX2				3.5449		6.0281											1H-TiSe2	K					0.3																																																										mJ/mol.K2	3.61																																					Pd,Ti,Se powder.		mixture - heat(650C,overnight) - Q - ANN(650C,1d) - Q to RT					Multiple electronic transitions and superconductivity in PdxTiSe2			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 81(2010)094524	E. Morosan,K. E. Wagner,Liang L. Zhao,Y. Hor,A. J. Williams,J. Tao,Y. Zhu,R. J. Cava		
151915	PRB081094520	nominal: BaFe1.7Co0.3As2. cleaved sample: d = 25 micron-m along c-axis. ab-plane thermal conductivity measured for T > 80 mK, H < 14.5 T.	Ba(Fe,Co)2As2	Ba1Fe1.73Co0.27As2	Ba	1	Fe	1.73	Co	0.27	As	2																3	2010																										AB2C2		ThCr2Si2																		K	8.1						8.1																				T	resistivity, R(on),parabolic approx,		17																																																mOhm.cm								0.0648																	self-flux method					Thermal conductivity of overdoped BaFe1.73Co0.27As2 single crystal: Evidence for nodeless multiple superconducting gaps and interband interactions			Department of Physics, Surface Physics Laboratory (National Key Laboratory), and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, China	Phys.Rev.B, 81(2010)094520	J. K. Dong,S. Y. Zhou,T. Y. Guan,X. Qiu,C. Zhang,P. Cheng,L. Fang,H. H. Wen,S. Y. Li		
151916	PRB081104525	nt SC. Tn = 140 K. tetra-to-ortho transition at 125 K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2010								140																		AB2C2		ThCr2Si2			A	3.9609		13.017												K					0																																																																																																		two-step solid state reaction. mixture - pellet- -sealed in silica tube- -heat(900C,30h) - slow cool to RT					Superconductivity induced by doping platinum in BaFe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)104525	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Jun Tang,Jing Ju,Katsumi Tanigaki,Hai-Hu Wen		
151917	PRB081104525		Ba(Fe,Pt)2As2	Ba1Fe1.98Pt0.02As2	Ba	1	Fe	1.98	Pt	0.02	As	2																1	2010																										AB2C2		ThCr2Si2			A	3.9647		13.01												K			0		0		0																																																																																																two-step solid state reaction. mixture - pellet- -sealed in silica tube- -heat(900C,30h) - slow cool to RT					Superconductivity induced by doping platinum in BaFe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)104525	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Jun Tang,Jing Ju,Katsumi Tanigaki,Hai-Hu Wen		
151918	PRB081104525		Ba(Fe,Pt)2As2	Ba1Fe1.9Pt0.1As2	Ba	1	Fe	1.9	Pt	0.1	As	2																1	2010																										AB2C2		ThCr2Si2			A	3.9688		12.986												K			25.2				25.2																				T	resistivity, 0.9Rn, WHH	93							T/K	resistivity, 0.9Rn	5.4			MHC151918																																																														two-step solid state reaction. mixture - pellet- -sealed in silica tube- -heat(900C,30h) - slow cool to RT					Superconductivity induced by doping platinum in BaFe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)104525	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Jun Tang,Jing Ju,Katsumi Tanigaki,Hai-Hu Wen		
151919	PRB081104525		Ba(Fe,Pt)2As2	Ba1Fe1.85Pt0.15As2	Ba	1	Fe	1.85	Pt	0.15	As	2																1	2010																										AB2C2		ThCr2Si2			A	3.9745		12.96												K			23.4				23.4																																																																																																two-step solid state reaction. mixture - pellet- -sealed in silica tube- -heat(900C,30h) - slow cool to RT					Superconductivity induced by doping platinum in BaFe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)104525	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Jun Tang,Jing Ju,Katsumi Tanigaki,Hai-Hu Wen		
151920	PRB081104525		Ba(Fe,Pt)2As2	Ba1Fe1.75Pt0.25As2	Ba	1	Fe	1.75	Pt	0.25	As	2																1	2010																										AB2C2		ThCr2Si2			A	3.9819		12.95												K			21.1				21.1																																																																																																two-step solid state reaction. mixture - pellet- -sealed in silica tube- -heat(900C,30h) - slow cool to RT					Superconductivity induced by doping platinum in BaFe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)104525	Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Jun Tang,Jing Ju,Katsumi Tanigaki,Hai-Hu Wen		
151921	PRB081094115	structural data at 300K. At 2K, a = 3.8312, b = 3.7830, c = 6.2643 beta = 89.17 degree. tetra-mono transformation at 72.5 K.	FeTe	Fe1.05Te1	Fe	1.05	Te	1																					2010								72.5																					P4/nmm		A	3.8219		6.2851												K					2																																																																																																		two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151922	PRB081094115	Fe-content not given. tetra-mono transformation at 62.5 K	Fe(Te,Se)	Fe1Te0.975Se0.025	Fe	1	Te	0.975	Se	0.025																			2010								62.5																																						K					2																																																																																																		two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151923	PRB081094115	structural data at 300K. At 2K, a = 3.8216, b = 3.7893, c = 6.2331 beta = 89.37 degree. tetra-mono transformation at 50.0 K	Fe(Te,Se)	Fe1.04Te0.95Se0.05	Fe	1.04	Te	0.95	Se	0.05																			2010								50																							A	3.8184		6.2617												K		11					11																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151924	PRB081094115	Fe-content not given. tetra-mono transformation at 43.0 K	Fe(Te,Se)	Fe1Te0.925Se0.075	Fe	1	Te	0.925	Se	0.075																			2010								43																																						K		11.5					11.5																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151925	PRB081094115	structural data at 300K. At 2K, a = 3.8118,  c = 6.1898.	Fe(Te,Se)	Fe1.03Te0.9Se0.1	Fe	1.03	Te	0.9	Se	0.1																			2010																															A	3.816		6.2381												K		11.9					11.9																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151926	PRB081094115	structural data at 300K. At 2K, a = 3.8106,  c = 6.1606.	Fe(Te,Se)	Fe1.02Te0.85Se0.15	Fe	1.02	Te	0.85	Se	0.15																			2010																															A	3.8133		6.2116												K		12.7					12.7																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151927	PRB081094115	structural data at 300K. At 2K, a = 3.8089,  c = 6.1316.	Fe(Te,Se)	Fe1.02Te0.8Se0.2	Fe	1.02	Te	0.8	Se	0.2																			2010																															A	3.8114		6.1843												K		13.6					13.6																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151928	PRB081094115	Fe-content not given	Fe(Te,Se)	Fe1Te0.5Se0.5	Fe	1	Te	0.5	Se	0.5																			2010																																														K		15					15																																																																																																two-step solid state reaction. mixture - sealed in Pyrex (400-450C,15-20h) - pellet - heat(800C,7-8days)					From antiferromagnetism to superconductivity in Fe1+yTe1-xSex (0 =< x =< 0.20): Neutron powder diffraction analysis			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)094115	A. Martinelli,A. Palenzona,M. Tropeano,C. Ferdeghini,M. Putti,M. R. Cimberle,T. D. Nguyen,M. Affronte,C. Ritter		
151929	PRB081104522	gaps measured by STM using in situ cleaved grains. two gaps: large gap in DB, small gap = 0.9 meV (2d/kTc = 2.56)	Ba8Si46	Ba8Si46	Ba	8	Si	46																				1	2010																												clathrate																		K		8.1					8.1																																														meV	1.3	3.7	1																																															synthesized at high-P and high-T conditions					Two energy gaps in the tunneling-conductance spectra of the superconducting clathrate Ba8Si46			Institut des Nanosciences de Paris, Universite Pierre et Marie Curie-Paris 6, CNRS-UMR 7588, 4 place Jussieu, 75252 Paris, Franc	Phys.Rev.B, 81(2010)104522	Yves Noat,Tristan Cren,Pierre Toulemonde,Alfonso San Miguel,Francois Debontridder,Vincent Dubost,Dimitri Roditchev		
151930	PRB081134521	bars cleaved from crystals for transport measurements. I//[100]. RRR = 2.32. (dC/gamma*Tc) = 1.214.	(Pb,Tl)Te	Pb0.99Tl0.01Te1	Pb	0.99	Tl	0.01	Te	1																		3	2010																																														K		1.3					1.3																																																					MSP151930			mJ/mol.K2	0.504																																			n/cm3	91400000000000000000			vapor transport method					Correlation of anomalous normal state properties with superconductivity in Pb1-x-yTlxInyTe			Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA	Phys.Rev.B, 81(2010)134521	A. S. Erickson,N. P. Breznay,E. A. Nowadnick,T. H. Geballe,I. R. Fisher		
151931	PRB081134521	bars cleaved from crystals for transport measurements. I//[100]. RRR = 2.53. (dC/gamma*Tc) = 1.119.	(Pb,Tl,In)Te	Pb0.985Tl0.01In0.005Te1	Pb	0.985	Tl	0.01	In	0.005	Te	1																3	2010																																														K		0.954					0.954																																																								mJ/mol.K2	0.493																																			n/cm3	71900000000000000000			vapor transport method					Correlation of anomalous normal state properties with superconductivity in Pb1-x-yTlxInyTe			Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA	Phys.Rev.B, 81(2010)134521	A. S. Erickson,N. P. Breznay,E. A. Nowadnick,T. H. Geballe,I. R. Fisher		
151932	PRB081134521	bars cleaved from crystals for transport measurements. I//[100]. RRR = 2.58. (dC/gamma*Tc) = 0.656.	(Pb,Tl,In)Te	Pb0.982Tl0.01In0.008Te1	Pb	0.982	Tl	0.01	In	0.008	Te	1																3	2010																																														K		0.818					0.818																																																								mJ/mol.K2	0.497																																			n/cm3	73400000000000000000			vapor transport method					Correlation of anomalous normal state properties with superconductivity in Pb1-x-yTlxInyTe			Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA	Phys.Rev.B, 81(2010)134521	A. S. Erickson,N. P. Breznay,E. A. Nowadnick,T. H. Geballe,I. R. Fisher		
151933	PRB081134521	not SC. bars cleaved from crystals for transport measurements. I//[100]. RRR = 4.47.	(Pb,Tl,In)Te	Pb0.978Tl0.01In0.012Te1	Pb	0.978	Tl	0.01	In	0.012	Te	1																3	2010																																														K					0.05																																																										mJ/mol.K2	0.291																																			n/cm3	2900000000000000000			vapor transport method					Correlation of anomalous normal state properties with superconductivity in Pb1-x-yTlxInyTe			Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA	Phys.Rev.B, 81(2010)134521	A. S. Erickson,N. P. Breznay,E. A. Nowadnick,T. H. Geballe,I. R. Fisher		
151934	PRB081134521	not SC. bars cleaved from crystals for transport measurements. I//[100]. RRR = 8.26.	(Pb,Tl,In)Te	Pb0.969Tl0.01In0.021Te1	Pb	0.969	Tl	0.01	In	0.021	Te	1																3	2010																																														K					0.05																																																										mJ/mol.K2	0.135																																			n/cm3	2200000000000000000			vapor transport method					Correlation of anomalous normal state properties with superconductivity in Pb1-x-yTlxInyTe			Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA	Phys.Rev.B, 81(2010)134521	A. S. Erickson,N. P. Breznay,E. A. Nowadnick,T. H. Geballe,I. R. Fisher		
151935	PRB081140507	P-induced SC. J//[100]. zero resistivity appears at P=24 GPa. SC properties at 24 GPa. Hc2 measured for H//[001].	CeIrGe3	Ce1Ir1Ge3	Ce	1	Ir	1	Ge	3																			2010								8.3																				BaNiSn3																		K		1.61			0		1.61	MPH151935																												T/K		16			MHC151935																																																														Sn-flux method. sample:Sn = 1:20. sealed in alumina crucible, heat(1000C,2d) - cool to 800C - slow cool to 600C(1C/h) - Q to RT					Pressure-induced superconductivity and large upper critical field in the noncentrosymmetric antiferromagnet CeIrGe3			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	Phys.Rev.B, 81(2010)140507	F. Honda,I. Bonalde,K. Shimizu,S. Yoshiuchi,Y. Hirose,T. Nakamura,R. Settai,Y. Onuki		
151936	PRB081140509	NQR measured	LaONiAs	La1Ni1As1O1	La	1	Ni	1	As	1															O	1			2010																												oxypnictide																		K		2.98					2.98																																																																																														NiO,Ni,As,La,LaF3		solid state reaction. mixture - pellet ANN(1150C,50h)					Evidence for a full energy gap in the nickel pnictide superconductor LaNiAsO1-xFx from 75As nuclear quadrupole resonance			1Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 81(2010)140509	T. Tabuchi,Z. Li,T. Oka,G. F. Chen,S. Kawasaki,J. L. Luo,N. L. Wang,Guo-qing Zheng		
151937	PRB081140509	NQR measured	La(O,F)NiAs	La1Ni1As1F0.06O0.94	La	1	Ni	1	As	1	F	0.06													O	0.94			2010																												oxypnictide																		K		3.64					3.64																																																																																														NiO,Ni,As,La,LaF3		solid state reaction. mixture - pellet ANN(1150C,50h)					Evidence for a full energy gap in the nickel pnictide superconductor LaNiAsO1-xFx from 75As nuclear quadrupole resonance			1Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 81(2010)140509	T. Tabuchi,Z. Li,T. Oka,G. F. Chen,S. Kawasaki,J. L. Luo,N. L. Wang,Guo-qing Zheng		
151938	PRB081140509	NQR measured	La(O,F)NiAs	La1Ni1As1F0.1O0.9	La	1	Ni	1	As	1	F	0.1													O	0.9			2010																												oxypnictide																		K		4					4																																																3.2																																														NiO,Ni,As,La,LaF3		solid state reaction. mixture - pellet ANN(1150C,50h)					Evidence for a full energy gap in the nickel pnictide superconductor LaNiAsO1-xFx from 75As nuclear quadrupole resonance			1Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 81(2010)140509	T. Tabuchi,Z. Li,T. Oka,G. F. Chen,S. Kawasaki,J. L. Luo,N. L. Wang,Guo-qing Zheng		
151939	PRB081140509	NQR measured	La(O,F)NiAs	La1Ni1As1F0.12O0.88	La	1	Ni	1	As	1	F	0.12													O	0.88			2010																												oxypnictide																		K		3.59					3.59																																																3.1																																														NiO,Ni,As,La,LaF3		solid state reaction. mixture - pellet ANN(1150C,50h)					Evidence for a full energy gap in the nickel pnictide superconductor LaNiAsO1-xFx from 75As nuclear quadrupole resonance			1Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 81(2010)140509	T. Tabuchi,Z. Li,T. Oka,G. F. Chen,S. Kawasaki,J. L. Luo,N. L. Wang,Guo-qing Zheng		
151940	PRB081144513		FeSe0.88	Fe1Se0.88	Fe	1	Se	0.88																					2010																																														K		9.84					9.84																																																																																																					Magnetic fluctuations in FeSe1-z and Cu-doped FeSe1-z  : 77Se NMR experiments			Department of Electrophysics, National Chiao Tung University, Hsinchu 30010, Taiwan	Phys.Rev.B, 81(2010)144513	Ben-Li Young,Jack Wu,Tzu-Wen Huang,Kuo-Wei Yeh,Maw-Kuen Wu		
151941	PRB081144513		(Fe,Cu)Se0.88	Fe0.99Cu0.01Se0.88	Fe	0.99	Cu	0.01	Se	0.88																			2010																																														K		5.64					5.64																																																																																																					Magnetic fluctuations in FeSe1-z and Cu-doped FeSe1-z  : 77Se NMR experiments			Department of Electrophysics, National Chiao Tung University, Hsinchu 30010, Taiwan	Phys.Rev.B, 81(2010)144513	Ben-Li Young,Jack Wu,Tzu-Wen Huang,Kuo-Wei Yeh,Maw-Kuen Wu		
151942	PRB081144513		(Fe,Cu)Se0.88	Fe0.98Cu0.02Se0.88	Fe	0.98	Cu	0.02	Se	0.88																			2010																																														K		4					4																																																																																																					Magnetic fluctuations in FeSe1-z and Cu-doped FeSe1-z  : 77Se NMR experiments			Department of Electrophysics, National Chiao Tung University, Hsinchu 30010, Taiwan	Phys.Rev.B, 81(2010)144513	Ben-Li Young,Jack Wu,Tzu-Wen Huang,Kuo-Wei Yeh,Maw-Kuen Wu		
151943	PRB081144513		(Fe,Cu)Se0.88	Fe0.97Cu0.03Se0.88	Fe	0.97	Cu	0.03	Se	0.88																			2010																																														K					1.6																																																																																																							Magnetic fluctuations in FeSe1-z and Cu-doped FeSe1-z  : 77Se NMR experiments			Department of Electrophysics, National Chiao Tung University, Hsinchu 30010, Taiwan	Phys.Rev.B, 81(2010)144513	Ben-Li Young,Jack Wu,Tzu-Wen Huang,Kuo-Wei Yeh,Maw-Kuen Wu		
151944	SSC1501108	Two phases: Ca4(PO4)2O and CaO from XRD. Not clear which phase is SC. Samples were prepared by shock-wave pressure upto 65 GPa. Tc from SQUID.	CaO+Ca4(PO4)2O	Ca5P2O10	Ca	5	P	2																	O	10		2	2010																																														K				50			50																																																																																																Ca(4N, grain size:200micron) : Ca3(PO4)2 = 1:1.  pelletized - pressure(65 GPa) by shock wave. samples hold in Liq.N2.					Superconductivity at 50 K in a mixed-phase Ca P O compound system treated by shock-wave pressure up to 65 GPa			Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka, Moscow District, 142432, Russia	Solid State Commun., 150(2010)1108	N.S. Sidorov,A.V. Palnichenko,V.V. Avdonin,D.V. Shakhrai,O.G. Rybchenko,S.S. Khasanov,M.K. Sakharov		
151945	MAT09074001	beta-FeSe type	FeSe0.85	Fe1Se0.85	Fe	1	Se	0.85																					2009																												PbO																		K		10.6					10.6																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151946	MAT09074001	beta-FeSe type	(Cu,Fe)Se0.85	Cu0.01Fe0.99Se0.85	Cu	0.01	Fe	0.99	Se	0.85																			2009																												PbO																		K		8.6					8.6																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151947	MAT09074001	beta-FeSe type	(Cu,Fe)Se0.85	Cu0.02Fe0.98Se0.85	Cu	0.02	Fe	0.98	Se	0.85																			2009																												PbO																		K		4.1					4.1																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151948	MAT09074001	beta-FeSe type	(Mn,Fe)Se0.85	Mn0.1Fe0.9Se0.85	Mn	0.1	Fe	0.9	Se	0.85																			2009																												PbO																		K		11					11																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151949	MAT09074001	beta-FeSe type	(Mn,Fe)Se0.85	Mn0.2Fe0.8Se0.85	Mn	0.2	Fe	0.8	Se	0.85																			2009																												PbO																		K		11.1					11.1																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151950	MAT09074001	beta-FeSe type	(Mn,Fe)Se0.85	Mn0.3Fe0.7Se0.85	Mn	0.3	Fe	0.7	Se	0.85																			2009																												PbO																		K		9.7					9.7																																																																																																See Physica C, 469(2009)340					Structural phase transition in TmxFe1-xSe0.85 (Tm = Mn and Cu) and its relation to superconductivity				cond-mat/0907.4001	Tzu-Wen Huang,Ta-Kun Chen,Kuo-Wei Yeh,Chung-Ting Ke,Chi Liang Chen,Yi-Lin Huang,Fong-Chi Hsu,Maw-Kuen Wu,Phillip M. Wu,Maxim Avdeev,Andrew J. Studer		
151951	PHC4690340		FeSe0.85	Fe1Se0.85	Fe	1	Se	0.85																					2009																												PbO																		K			10				10																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151952	PHC4690340		(Al,Fe)Se0.85	Al0.1Fe0.9Se0.85	Al	0.1	Fe	0.9	Se	0.85																			2009																												PbO																		K			8.5				8.5																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151953	PHC4690340		(Al,Fe)Se0.85	Al0.25Fe0.75Se0.85	Al	0.25	Fe	0.75	Se	0.85																			2009																												PbO																		K			8.5				8.5																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151954	PHC4690340		(Ga,Fe)Se0.85	Ga0.1Fe0.9Se0.85	Ga	0.1	Fe	0.9	Se	0.85																			2009																												PbO																		K			6.8				6.8																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151955	PHC4690340		(Ga,Fe)Se0.85	Ga0.25Fe0.75Se0.85	Ga	0.25	Fe	0.75	Se	0.85																			2009																												PbO																		K			6.8				6.8																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151956	PHC4690340		(Sm,Fe)Se0.85	Sm0.1Fe0.9Se0.85	Sm	0.1	Fe	0.9	Se	0.85																			2009																												PbO																		K			10.6				10.6																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151957	PHC4690340		(Sm,Fe)Se0.85	Sm0.25Fe0.75Se0.85	Sm	0.25	Fe	0.75	Se	0.85																			2009																												PbO																		K			9.2				9.2																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151958	PHC4690894		(Pr,Sr)OFeAs	Pr0.8Sr0.2Fe1As1O1	Pr	0.8	Sr	0.2	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9926		8.6629												K		15.8					15.8																																																																																																1st step: LaAs(PrAs), SrAs were prepared by solid state reaction. Then, mixture(LaAs(PrAs),SrAs,Fe powder,Fe2O3) - pellet - heat(1150C,60h, in quartz tube with 20%Ar)					Superconductivity in the hole-doped oxy-arsenide RE1-xSrxFeAsO (RE = La, Pr)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Physica C, 469(2009)894	H.H. Wen,G. Mu,X.Y. Zhu,P. Cheng,L. Fang,F. Han,B. Zeng,B. Shen		
151960	PHC4690340		(Ba,Fe)Se0.85	Ba0.1Fe0.9Se0.85	Ba	0.1	Fe	0.9	Se	0.85																			2009																												PbO																		K			10.6				10.6																																																																																																(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151962	PHC4690340		Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																			2009																												PbO																		K			13.8				13.8																				T	resistivity, 0.9Rn	72.5												MHC151962																																																														(powder mixture) - pellet - heat(600-650C, 20h) - reground - pellet - SIN(650-700C, 20h)					The development of the superconducting PbO-type beta-FeSe and related compounds			Institute of Physics, Academia Sinica, Nankang, Taipei 115, Taiwan	Physica C, 469(2009)340	M.K. Wu,F.C. Hsu,K.W. Yeh,T.W. Huang,J.Y. Luo,M.J. Wang,H.H. Chang,T.K. Chen,S.M. Rao,B.H. Mok,C.L. Chen,Y.L. Huang,C.T. Ke,P.M. Wu,A.M. Chang,C.T. Wu,T.P. Perng		
151963	SPS0230817	carrier from Hall coeff. at 77K.	(Pb,Tl)Te	Pb0.99Tl0.01Te1	Pb	0.99	Tl	0.01	Te	1																			1981																																														K		1.14					1.14																																																																																												n/cm3	75000000000000000000			powder metallurgy method. mixture - evacuated quartz ampoules - ANN(650C,100h)					Bulk superconductivity of doped lead telluride at 1.4 K				Sov.Phys.Solid State, 23(1981)817	I.A.Chernik,S.N.Lykov		
151964	SPS0230817	carrier from Hall coeff. at 77K.	(Pb,Tl)Te	Pb0.9875Tl0.0125Te1	Pb	0.9875	Tl	0.0125	Te	1																			1981																																														K		1.35					1.35																																																																																												n/cm3	86000000000000000000			powder metallurgy method. mixture - evacuated quartz ampoules - ANN(650C,100h)					Bulk superconductivity of doped lead telluride at 1.4 K				Sov.Phys.Solid State, 23(1981)817	I.A.Chernik,S.N.Lykov		
151965	SPS0230817	carrier from Hall coeff. at 77K. G-L parameter = 80.	(Pb,Tl)Te	Pb0.985Tl0.015Te1	Pb	0.985	Tl	0.015	Te	1																			1981																																														K		1.4					1.4											Oe					0.6			1	T		0.5			0.25			1																															132	SP-heat																																n/cm3	96000000000000000000			powder metallurgy method. mixture - evacuated quartz ampoules - ANN(650C,100h)					Bulk superconductivity of doped lead telluride at 1.4 K				Sov.Phys.Solid State, 23(1981)817	I.A.Chernik,S.N.Lykov		
151966	PRB080184514	Tc defined as 0.9Rn. reentrant at 17 K due to magnetic order of Eu. R not zwro down to 4K.. Anisotropy(Hc2) = 30 at 17 K.	Eu(Fe,Co)2As2	Eu1Fe1.78Co0.22As2	Eu	1	Fe	1.78	Co	0.22	As	2																3	2009																										AB2C2		ThCr2Si2																		K				21			21																				T	resistivity, linear extrapolation		26						T/K	resistivity	1.3			MHC151696																																																														self-flux method. (Eu:Fe1-xCoxAs=1:4) - alumina in quartz tube) - heat(1053K,10h) - heat(1398K,5h) - cool to 1223 K(2K/h)					Superconductivity and local-moment magnetism in Eu(Fe0.89Co0.11)2As2			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 80(2009)184514	Shuai Jiang,Hui Xing,Guofang Xuan,Zhi Ren,Cao Wang,Zhu-an Xu,Guanghan Cao		
151980	SPS0241661		(Pb,Tl,Na)Te	Pb0.99Tl0.005Na0.005Te1	Pb	0.99	Tl	0.005	Na	0.005	Te	1																	1982																																														K		1.61					1.61																																																								mJ/mol.K2	0.72																												cm3/C	0.109															The nature of the superconducting state in PbTe doped with thallium				Sov.Phys.Solid State, 24(1982)1661	I.A.Chernik,S.N.Lykov,N.I.Grechko		
151981	SPS0241661		(Pb,Tl,Na)Te	Pb0.985Tl0.005Na0.01Te1	Pb	0.985	Tl	0.005	Na	0.01	Te	1																	1982																																														K		1.38					1.38																																																								mJ/mol.K2	0.37																												cm3/C	0.128															The nature of the superconducting state in PbTe doped with thallium				Sov.Phys.Solid State, 24(1982)1661	I.A.Chernik,S.N.Lykov,N.I.Grechko		
151982	SPS0241661		(Pb,Tl,Na)Te	Pb0.987Tl0.0125Na0.005Te1	Pb	0.987	Tl	0.0125	Na	0.005	Te	1																	1982																																														K		1.87					1.87	MTC151982																																																							mJ/mol.K2	0.851																												cm3/C	0.081															The nature of the superconducting state in PbTe doped with thallium				Sov.Phys.Solid State, 24(1982)1661	I.A.Chernik,S.N.Lykov,N.I.Grechko		
151983	SPS0241661		(Pb,Tl,Na)Te	Pb0.975Tl0.0125Na0.0125Te1	Pb	0.975	Tl	0.0125	Na	0.0125	Te	1																	1982																																														K		1.71					1.71																																																								mJ/mol.K2	0.486																												cm3/C	0.118															The nature of the superconducting state in PbTe doped with thallium				Sov.Phys.Solid State, 24(1982)1661	I.A.Chernik,S.N.Lykov,N.I.Grechko		
151984	PHC4700511	RRR = 4.5	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2010																										ABCD		oxypnictide			A	4.028		8.72											ZrCuSiAs	K			28				28																																																																		uV/K	-31.4			TP151984																					RH151984			La,La2O3,Y2O3,LaF3,FeAs		solid state reaction. mixture - sealed in evacuated silica ampoule - heat(900C,30h) - pelletized - wrapped in Ta foil - sealed in silica tube- -heat(1180C,30h)					Yttrium doped La1-xYxO0.9F0.1FeAs superconductors: Hall and thermopower studies			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)511	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
151985	PHC4700511	RRR = 1.5	(La,Y)(O,F)FeAs	La0.9Y0.1Fe1As1F0.1O0.9	La	0.9	Y	0.1	Fe	1	As	1	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide			A	4.0269		8.718											ZrCuSiAs	K			7				7																																																																																														La,La2O3,Y2O3,LaF3,FeAs		solid state reaction. mixture - sealed in evacuated silica ampoule - heat(900C,30h) - pelletized - wrapped in Ta foil - sealed in silica tube- -heat(1180C,30h)					Yttrium doped La1-xYxO0.9F0.1FeAs superconductors: Hall and thermopower studies			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)511	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
151986	PHC4700511	RRR = 7.1	(La,Y)(O,F)FeAs	La0.8Y0.2Fe1As1F0.1O0.9	La	0.8	Y	0.2	Fe	1	As	1	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide			A	4.02		8.7109											ZrCuSiAs	K			32				32																																																																		uV/K	-33.1			TP151986																								La,La2O3,Y2O3,LaF3,FeAs		solid state reaction. mixture - sealed in evacuated silica ampoule - heat(900C,30h) - pelletized - wrapped in Ta foil - sealed in silica tube- -heat(1180C,30h)					Yttrium doped La1-xYxO0.9F0.1FeAs superconductors: Hall and thermopower studies			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)511	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
151987	PHC4700511	RRR = 17.2	(La,Y)(O,F)FeAs	La0.7Y0.3Fe1As1F0.1O0.9	La	0.7	Y	0.3	Fe	1	As	1	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide			A	4.0159		8.7026											ZrCuSiAs	K			34.8				34.8																				T	resistivity, WHH	60.5							T/K	resistivity	2.51			HC151987																																uV/K	-30.3			TP151987																					RH151987	n/cm3	710000000000000000000	La,La2O3,Y2O3,LaF3,FeAs		solid state reaction. mixture - sealed in evacuated silica ampoule - heat(900C,30h) - pelletized - wrapped in Ta foil - sealed in silica tube- -heat(1180C,30h)					Yttrium doped La1-xYxO0.9F0.1FeAs superconductors: Hall and thermopower studies			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)511	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
151988	PHC4700511		(La,Y)(O,F)FeAs	La0.5Y0.5Fe1As1F0.1O0.9	La	0.5	Y	0.5	Fe	1	As	1	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide			A	4.01		8.6901											ZrCuSiAs	K			31.4				31.4																																																																		uV/K	-22.1			TP151988																					RH151988	n/cm3	1100000000000000000000	La,La2O3,Y2O3,LaF3,FeAs		solid state reaction. mixture - sealed in evacuated silica ampoule - heat(900C,30h) - pelletized - wrapped in Ta foil - sealed in silica tube- -heat(1180C,30h)					Yttrium doped La1-xYxO0.9F0.1FeAs superconductors: Hall and thermopower studies			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)511	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
151989	PRB081180511	Neel-T defined as a inflection point in R(T). Tc defined as R=0.1Rn and  0.9Rn.	CePt3(Si,Ge)	Ce1Pt3Si0.94Ge0.06	Ce	1	Pt	3	Si	0.94	Ge	0.06																	2010								2.14																		ABC3		CePt3B																		K	0.291		0.61				0.4505	MTC151989																																																																																																				Pair breaking by nonmagnetic impurities in the noncentrosymmetric superconductor CePt3Si			Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B, 81(2010)180511	M. Nicklas,F. Steglich,J. Knolle,I. Eremin,R. Lackner,E. Bauer		
151990	PRB081180511	Neel-T defined as a inflection point in R(T). Tc defined as R=0.1Rn and  0.9Rn.	CePt3Si	Ce1Pt3Si1	Ce	1	Pt	3	Si	1																			2010								2.25																		ABC3		CePt3B																		K	0.696		0.8				0.748	MTC151990																																																																																																				Pair breaking by nonmagnetic impurities in the noncentrosymmetric superconductor CePt3Si			Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B, 81(2010)180511	M. Nicklas,F. Steglich,J. Knolle,I. Eremin,R. Lackner,E. Bauer		
151991	PRB081180507	2 vol.% of Ce3Pt4In13. Pcr = 1 GPa. Tc(max) and SP-jump(max)  at 3.5 GPa. QCP = 3.58 GPa. [gamma] and beta (=2.88 mJ/mol.K4) obtained by fitting for 12<T<19 K. in SP. [dHc2/dT] at 3.0 GPa.	CePt2In7	Ce1Pt2In7	Ce	1	Pt	2	In	7																			2010								5.5																		AB2C7			I4/mmm		A	4.611		21.647											CePt2In7	K		2.1			0.05		2.1	MTC151991																												T/K		5.52																									mJ/mol.K2	340	SP-heat	189	SP-heat																																				arc-melting - wrapped in Ta foil - ANN(500C,2w, in vac)					Pressure-induced superconducting state and effective mass enhancement near the antiferromagnetic quantum critical point of CePt2In7			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 81(2010)180507	E. D. Bauer,H. O. Lee,V. A. Sidorov,N. Kurita,K. Gofryk,J.-X. Zhu,F. Ronning,R. Movshovich,J. D. Thompson,Tuson Park		
151992	PRB081174529	Hall coeff.(100K) = 1.40  E-9 m3/C.	(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9166		13.328												K		35					35																																																																							mOhm.cm							0.009													MRH151992			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151993	PRB081174529	Hall coeff.(100K) = 1.24 E-9 m3/C.	(Ba,K)(Fe,Mn)2As2	Ba0.5K0.5Fe1.96Mn0.04As2	Ba	0.5	K	0.5	Fe	1.96	Mn	0.04	As	2															2010																										AB2C2		ThCr2Si2			A	3.9216		13.318												K		28.4					28.4																																																																							mOhm.cm							0.145													MRH151993			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151994	PRB081174529	Hall coeff.(100K) = 1.90 E-9 m3/C.	(Ba,K)(Fe,Mn)2As2	Ba0.5K0.5Fe1.92Mn0.08As2	Ba	0.5	K	0.5	Fe	1.92	Mn	0.08	As	2															2010																										AB2C2		ThCr2Si2			A	3.924		13.323												K		15					15																																																																							mOhm.cm							0.322													MRH151994			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151995	PRB081174529	Hall coeff.(100K) = 0.685 E-9 m3/C.	(Ba,K)(Fe,Mn)2As2	Ba0.5K0.5Fe1.84Mn0.16As2	Ba	0.5	K	0.5	Fe	1.84	Mn	0.16	As	2															2010																										AB2C2		ThCr2Si2			A	3.9423		13.307												K		0					0																																																																							mOhm.cm							0.805													MRH151995			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151996	PRB081174529	Zn-content 0.062 by EDX.	(Ba,K)(Fe,Zn)2As2	Ba0.5K0.5Fe1.92Zn0.08As2	Ba	0.5	K	0.5	Fe	1.92	Zn	0.08	As	2															2010																										AB2C2		ThCr2Si2			A	3.9169		13.349												K		34.3					34.3																																																																							mOhm.cm							0.036																K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151997	PRB081174529	Hall coeff.(100K) = 1.30 E-9 m3/C.	(Ba,K)(Fe,Zn)2As2	Ba0.5K0.5Fe1.88Zn0.12As2	Ba	0.5	K	0.5	Fe	1.88	Zn	0.12	As	2															2010																										AB2C2		ThCr2Si2			A	3.9196		13.3475												K		33.5					33.5																																																																							mOhm.cm							0.049													MRH151997			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151998	PRB081174529	Hall coeff.(100K) = 1.23 E-9 m3/C.	(Ba,K)(Fe,Zn)2As2	Ba0.5K0.5Fe1.84Zn0.16As2	Ba	0.5	K	0.5	Fe	1.84	Zn	0.16	As	2															2010																										AB2C2		ThCr2Si2			A	3.9252		13.313												K		34.2					34.2																																																																							mOhm.cm							0.062													MRH151998			K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
151999	PRB081174529	Zn-content 0.09  by EDX.	(Ba,K)(Fe,Zn)2As2	Ba0.5K0.5Fe1.8Zn0.2As2	Ba	0.5	K	0.5	Fe	1.8	Zn	0.2	As	2															2010																										AB2C2		ThCr2Si2			A	3.924		13.323												K		34.3					34.3																																																																							mOhm.cm																							K3As,FeAs,BaAs,MnAs(ZnAs)		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN					Contrasting impurity scattering and pair-breaking effects by doping Mn and Zn in Ba0.5K0.5Fe2As2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 81(2010)174529	Peng Cheng,Bing Shen,Jiangping Hu,Hai-Hu Wen		
152000	PRB081180510	uniaxial pressure (P//c-axis) enhanced Tc. Tc(SUS) = 3.2 K at P//c = 0.2 GPa while Tc(P=0) = 1.5 K	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2010																												Sr2RuO4																		K				3.2			3.2																																																																																																floating zone method with Ru self-flux.					Higher-Tc superconducting phase in Sr2RuO4 induced by uniaxial pressure			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)180510	Shunichiro Kittaka,Haruka Taniguchi,Shingo Yonezawa,Hiroshi Yaguchi,Yoshiteru Maeno		
152001	P078140501	[RESN] at 38 K.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2																		K			36.5			0.5	36.5																				T	resistivity, WHH		235	138					T/K	resistivity	9.35	5.49		MHC152001																																					mOhm.cm							0.05																		self-flux method					Upper critical field, anisotropy, and superconducting properties of Ba1-xKxFe2As2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 78(2008)140501	Zhao-Sheng Wang,Hui-Qian Luo,Cong Ren,Hai-Hu Wen		
152002	P078140501		(Ba,K)Fe2As2	Ba0.77K0.23Fe2As2	Ba	0.77	K	0.23	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2																		K			24				24																				T	resistivity, WHH		84.3	55.9																																																																								self-flux method					Upper critical field, anisotropy, and superconducting properties of Ba1-xKxFe2As2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 78(2008)140501	Zhao-Sheng Wang,Hui-Qian Luo,Cong Ren,Hai-Hu Wen		
152003	P078140501		(Ba,K)Fe2As2	Ba0.75K0.25Fe2As2	Ba	0.75	K	0.25	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2																		K			28.3				28.3																				T	resistivity, WHH		125	60.4																																																																								self-flux method					Upper critical field, anisotropy, and superconducting properties of Ba1-xKxFe2As2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 78(2008)140501	Zhao-Sheng Wang,Hui-Qian Luo,Cong Ren,Hai-Hu Wen		
152004	P078140501		(Ba,K)Fe2As2	Ba0.72K0.28Fe2As2	Ba	0.72	K	0.28	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2																		K			36.7				36.7																				T	resistivity, WHH		162	90.5																																																																								self-flux method					Upper critical field, anisotropy, and superconducting properties of Ba1-xKxFe2As2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 78(2008)140501	Zhao-Sheng Wang,Hui-Qian Luo,Cong Ren,Hai-Hu Wen		
152005	P078144422		(Pr,Y)Ni2B2C	Y0.8Pr0.2Ni2B2C1	Y	0.8	Pr	0.2	Ni	2	B	2	C	1														1	2008																										ABC2D2		LuNi2B2C	I4/mmm		A	3.5533		10.4807											borocarbide	K		8.62					8.62																																																																																																arc-melting in Ar - pellet - melt to rod - wrapped in Ta sealed in quartz tube - ANN(1000C,10d) + ANN(1100C,1d) - Q to water					Crystalline electric field effects in PrNi2B2C: Inelastic neutron scattering			Experimental Condensed Matter Physics Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B, 78(2008)144422	Chandan Mazumdar,M. Rotter,M. Frontzek,H. Michor,M. Doerr,A. Kreyssig,M. Koza,A. Hiess,J. Voigt,G. Behr,L. C. Gupta,M. Prager,M. Loewenhaupt		
152006	P078144422		(Pr,Y)Ni2B2C	Y0.9Pr0.1Ni2B2C1	Y	0.9	Pr	0.1	Ni	2	B	2	C	1														1	2008																										ABC2D2		LuNi2B2C	I4/mmm		A	3.5403		10.5096											borocarbide	K		11.2					11.2																																																																																																arc-melting in Ar - pellet - melt to rod - wrapped in Ta sealed in quartz tube - ANN(1000C,10d) + ANN(1100C,1d) - Q to water					Crystalline electric field effects in PrNi2B2C: Inelastic neutron scattering			Experimental Condensed Matter Physics Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B, 78(2008)144422	Chandan Mazumdar,M. Rotter,M. Frontzek,H. Michor,M. Doerr,A. Kreyssig,M. Koza,A. Hiess,J. Voigt,G. Behr,L. C. Gupta,M. Prager,M. Loewenhaupt		
152007	P078144422		(Pr,Y)Ni2B2C	Y0.95Pr0.05Ni2B2C1	Y	0.95	Pr	0.05	Ni	2	B	2	C	1														1	2008																										ABC2D2		LuNi2B2C	I4/mmm		A	3.5351		10.5277											borocarbide	K		14.1					14.1																																																																																																arc-melting in Ar - pellet - melt to rod - wrapped in Ta sealed in quartz tube - ANN(1000C,10d) + ANN(1100C,1d) - Q to water					Crystalline electric field effects in PrNi2B2C: Inelastic neutron scattering			Experimental Condensed Matter Physics Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B, 78(2008)144422	Chandan Mazumdar,M. Rotter,M. Frontzek,H. Michor,M. Doerr,A. Kreyssig,M. Koza,A. Hiess,J. Voigt,G. Behr,L. C. Gupta,M. Prager,M. Loewenhaupt		
152008	P078144422		YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																1	2008																										ABC2D2		LuNi2B2C	I4/mmm		A	3.526		10.5422											borocarbide	K		15.6					15.6																																																																																																arc-melting in Ar - pellet - melt to rod - wrapped in Ta sealed in quartz tube - ANN(1000C,10d) + ANN(1100C,1d) - Q to water					Crystalline electric field effects in PrNi2B2C: Inelastic neutron scattering			Experimental Condensed Matter Physics Division, Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India	Phys.Rev.B, 78(2008)144422	Chandan Mazumdar,M. Rotter,M. Frontzek,H. Michor,M. Doerr,A. Kreyssig,M. Koza,A. Hiess,J. Voigt,G. Behr,L. C. Gupta,M. Prager,M. Loewenhaupt		
152009	P078172503		(La,Y)O0.6FeAsO	La0.9Y0.1Fe1As1O0.6	La	0.9	Y	0.1	Fe	1	As	1													O	0.6			2008																												oxypnictide	P4/nmm		A	4.0259		8.7249											ZrCuSiAs-type	K	22.6	25.6		22.6			25.6																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152010	P078172503		(La,Y)O0.6FeAsO	La0.8Y0.2Fe1As1O0.6	La	0.8	Y	0.2	Fe	1	As	1													O	0.6			2008																												oxypnictide	P4/nmm		A	4.0217		8.7096											ZrCuSiAs-type	K	26.6	32.5		29.9			32.5																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152011	P078172503		(La,Y)O0.6FeAsO	La0.7Y0.3Fe1As1O0.6	La	0.7	Y	0.3	Fe	1	As	1													O	0.6			2008																												oxypnictide	P4/nmm		A	4.0112		8.6891											ZrCuSiAs-type	K	27.4	35.6		31.9			35.6																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152012	P078172503		(La,Y)O0.6FeAsO	La0.6Y0.4Fe1As1O0.6	La	0.6	Y	0.4	Fe	1	As	1													O	0.6			2008																												oxypnictide	P4/nmm		A	3.9924		8.6527											ZrCuSiAs-type	K	26.3	38.8		36.7			38.8																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152013	P078172503	LnFeAsO<1-y>: Tc saturates at (1-y) < 0.65. For (1-y) = 0.65, Tc goes to zero.	(La,Y)O0.6FeAsO	La0.5Y0.5Fe1As1O0.6	La	0.5	Y	0.5	Fe	1	As	1													O	0.6			2008																												oxypnictide	P4/nmm		A	3.995		8.6586											ZrCuSiAs-type	K	22.5	39.3		37.9			39.3																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152014	P078172503		(La,Y)O0.6FeAsO	La1Fe1As1O0.6	La	1	Fe	1	As	1															O	0.6			2008																												oxypnictide	P4/nmm		A	4.0298		8.7292											ZrCuSiAs-type	K	16.9	21.8		16.9			21.8																																																																																														LaAs,YAs,Fe,Fe2O3		High-P-synthesis. mixture - heat(1150C,2h,P=2GPa,in BN crucible)					Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1-xYxFeAsOy			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.B, 78(2008)172503	Parasharam M. Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
152015	P078172504	lattice const. = at 24 K. RRR=11. Tc(SP) = 0.62 K. (dC/gamma*Tc) = 1.0. lattice term of SP (beta) = 0.67 mJ/mol.K4.  Hc2//ab < Hc2//c. (Hc2//c)/(Hc2//ab) = 1.4.	SrNi2As2	Sr1Ni2As2	Sr	1	Ni	2	As	2																		3	2008							14																			AB2C2		ThCr2Si2	I4/mmm	139	A	4.1374		10.188												K		0.66					0.66																																																					MSP152015			mJ/mol.K2	8.7	SP-heat	224												mOhm.cm	0.007																								Pb-flux method. heat(1050C,in alumina crucible in sealed quartz tube) - slow cool (5C/h) to 600 C.					Superconductivity in SrNi2As2 single crystals			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 78(2008)172504	E. D. Bauer,F. Ronning,B. L. Scott,J. D. Thompson		
152016	P078172504	not SC. lattice const. = at 24 K. magnetic order of Eu(2+) at 14 K (Curie-T).	EuNi2As2	Eu1Ni2As2	Eu	1	Ni	2	As	2																		3	2008																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.0964		10.029												K					0.4																						Oe	resistivity, WHH		150	210										MHC152015		A	from Hc2		1477	1250																																																								Pb-flux method. heat(1050C,in alumina crucible in sealed quartz tube) - slow cool (5C/h) to 600 C.					Superconductivity in SrNi2As2 single crystals			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 78(2008)172504	E. D. Bauer,F. Ronning,B. L. Scott,J. D. Thompson		
152017	P078140510	anisotropy = 4 from coherence length.	Nd(O,F)FeAs	Nd1Fe1As1F0.18O0.82	Nd	1	Fe	1	As	1	F	0.18													O	0.82		3	2008																												oxypnictide																	ZrCuSiAs-type	K		47					47																				T	SP, WHH		100	23					T/K	SP-heat		3.1	0.72	HC152017		A	from Hc2		3.7	0.9																																																								NaCl flux method					Calorimetric determination of the upper critical fields and anisotropy of NdFeAsO1-xFx single crystals			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 78(2008)140510(R)	U. Welp,R. Xie,A. E. Koshelev,W. K. Kwok,P. Cheng,L. Fang,H.-H. Wen		
152018	P078172505	muon-SR measured. SC properties obtained by curve-fitting of relaxation rate. two gaps:  higher one (written in DB), lower one (2d/kTc) = 2.73. effective mass = 18.7 m<e>	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																					2008																												Ir3Ge7																		K		2.2					2.2																																				A	muon-SR	125			A	muon-SR	6650					4.54	16																																											n/cm3	1200000000000000000000			solid state reaction of Mo, Sb powders					Muon-spin-rotation study of the superconducting properties of Mo3Sb7			W. Trzebiatowski Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc aw, Poland	Phys.Rev.B, 78(2008)172505	V. H. Tran,A. D. Hillier,D. T. Adroja,Z. Bukowski		
152019	P077214515		LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1			2008																												oxypnictide			A	3.962		8.511												K		5.5					5.5																																																																																														LaP,Fe2P,FeP,La2O3,LaF3		mixture - heat(1200C,40h, in vac)					Electromagnetic properties and electronic structure of the iron-based layered superconductor LaFePO			ERATO-SORST, JST, in Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13,259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 77(2008)214515	Yoichi Kamihara,Masahiro Hirano,Hiroshi Yanagi,Toshio Kamiya,Yuji Saitoh,Eiji Ikenaga,Keisuke Kobayashi,Hideo Hosono		
152020	P077214515		La(O,F)FeP	La1Fe1P1F0.06O0.94	La	1	Fe	1	P	1	F	0.06													O	0.94			2008																												oxypnictide			A	3.957		8.503												K		7.1					7.1																																																																																														LaP,Fe2P,FeP,La2O3,LaF3		mixture - heat(1200C,40h, in vac)					Electromagnetic properties and electronic structure of the iron-based layered superconductor LaFePO			ERATO-SORST, JST, in Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13,259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 77(2008)214515	Yoichi Kamihara,Masahiro Hirano,Hiroshi Yanagi,Toshio Kamiya,Yuji Saitoh,Eiji Ikenaga,Keisuke Kobayashi,Hideo Hosono		
152021	P077214515		(La,Ca)OFeP	La0.9Ca0.1Fe1P1O1	La	0.9	Ca	0.1	Fe	1	P	1													O	1			2008																												oxypnictide			A	3.961		8.516												K		5.67					5.67																																																																																														LaP,Fe2P,FeP,La2O3,LaF3		mixture - heat(1200C,40h, in vac)					Electromagnetic properties and electronic structure of the iron-based layered superconductor LaFePO			ERATO-SORST, JST, in Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13,259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 77(2008)214515	Yoichi Kamihara,Masahiro Hirano,Hiroshi Yanagi,Toshio Kamiya,Yuji Saitoh,Eiji Ikenaga,Keisuke Kobayashi,Hideo Hosono		
152022	P078184512	SC appears  for 18 < R(6 K) < 542 uOhm.cm,  in a narrow region of lattice constants. moment = 0.37 myu-B/Sm	SmOFeP	Sm1Fe1P1O1	Sm	1	Fe	1	P	1															O	1		1	2008								5																				oxypnictide			A	3.8807		8.2054												K	2		3				2.5																																																																																														Sm2O3,SmP,Fe2P,FeP		mixture - heat(1200C, 40h)					Coexistence of superconductivity and antiferromagnetic ordering in the layered superconductor SmFePO			ERATO-SORST, JST, Frontier Research Center, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 78(2008)184512	Yoichi Kamihara,Hidenori Hiramatsu,Masahiro Hirano,Yasuhiro Kobayashi,Shinji Kitao,Satoshi Higashitaniguchi,Yoshitaka Yoda,Makoto Seto,Hideo Hosono		
152023	P078184506	(dC/gamma*Tc) = 1.41. thermodynamic Hc(0) = 44.6 mT. G-L = 23.5	Ni2ZrGa	Ni2Zr1Ga1	Ni	2	Zr	1	Ga	1																			2008																												Heusler	Fm3[-]m		A	6.098													L2<1>	K		2.87	2.94	2.8			2.87											Oe	M-H curve				160			2	T	resistive	1.48							T/K	resistive	0.75			MHC152023		A		150			A		3500					3.53	14				MSP152023			mJ/mol.K2	17.3	SP-heat	300	SP-heat																																				arc-melting - ANN(1073K,2w) - Q to ice & water					Ni-based superconductor: Heusler compound ZrNi2Ga			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 78(2008)184506	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser,Martin Jourdan,Kai Grube,Frederic Hardy,Hilbert von Lohneysen,K. L. Holman,R. J. Cava		
152024	P078184506		Ni2(Zr,Nb)Ga	Ni2Zr0.85Nb0.15Ga1	Ni	2	Zr	0.85	Nb	0.15	Ga	1																	2008																												Heusler	Fm3[-]m		A	6.074													L2<1>	K		2.4					2.4																																																																																																arc-melting - ANN(1073K,2w) - Q to ice & water					Ni-based superconductor: Heusler compound ZrNi2Ga			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 78(2008)184506	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser,Martin Jourdan,Kai Grube,Frederic Hardy,Hilbert von Lohneysen,K. L. Holman,R. J. Cava		
152025	P078184506		Ni2(Zr,Nb)Ga	Ni2Zr0.7Nb0.3Ga1	Ni	2	Zr	0.7	Nb	0.3	Ga	1																	2008																												Heusler	Fm3[-]m		A	6.037													L2<1>	K		2.3					2.3																																																																																																arc-melting - ANN(1073K,2w) - Q to ice & water					Ni-based superconductor: Heusler compound ZrNi2Ga			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 78(2008)184506	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser,Martin Jourdan,Kai Grube,Frederic Hardy,Hilbert von Lohneysen,K. L. Holman,R. J. Cava		
152026	P078184506		Ni2(Zr,Nb)Ga	Ni2Zr0.5Nb0.5Ga1	Ni	2	Zr	0.5	Nb	0.5	Ga	1																	2008																												Heusler	Fm3[-]m		A	5.99													L2<1>	K		2					2																																																																																																arc-melting - ANN(1073K,2w) - Q to ice & water					Ni-based superconductor: Heusler compound ZrNi2Ga			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 78(2008)184506	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser,Martin Jourdan,Kai Grube,Frederic Hardy,Hilbert von Lohneysen,K. L. Holman,R. J. Cava		
152027	P078184506		Ni2(Zr,Nb)Ga	Ni2Zr0.3Nb0.7Ga1	Ni	2	Zr	0.3	Nb	0.7	Ga	1																	2008																												Heusler	Fm3[-]m		A	5.972													L2<1>	K					1.8																																																																																																		arc-melting - ANN(1073K,2w) - Q to ice & water					Ni-based superconductor: Heusler compound ZrNi2Ga			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, 55099 Mainz, Germany	Phys.Rev.B, 78(2008)184506	Jurgen Winterlik,Gerhard H. Fecher,Claudia Felser,Martin Jourdan,Kai Grube,Frederic Hardy,Hilbert von Lohneysen,K. L. Holman,R. J. Cava		
152028	PHB2690154	SC not investigated. Einstein-T = 95.1 K. SP-heat analyzed using Debye and Einstein model.	Ni2TiAl	Ni2Ti1Al1	Ni	2	Ti	1	Al	1																			1999																												Heusler			A	5.8948													L2<1>																																																																mJ/mol.K2	13.38	SP-heat	411	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152029	PHB2690154	SC not investigated. Einstein-T = 76.6 K. SP-heat analyzed using Debye and Einstein model.	Ni2ZrAl	Ni2Zr1Al1	Ni	2	Zr	1	Al	1																			1999																												Heusler			A	6.1147													L2<1>																																																																mJ/mol.K2	13.67	SP-heat	278	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152030	PHB2690154	SC not investigated. Einstein-T = 70.4 K. SP-heat analyzed using Debye and Einstein model.	Ni2HfAl	Ni2Hf1Al1	Ni	2	Hf	1	Al	1																			1999																												Heusler			A	6.081													L2<1>																																																																mJ/mol.K2	10.91	SP-heat	288	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152031	PHB2690154	SC not investigated. Einstein-T = 81.3 K. SP-heat analyzed using Debye and Einstein model.	Ni2VAl	Ni2V1Al1	Ni	2	V	1	Al	1																			1999																												Heusler			A	5.8031													L2<1>																																																																mJ/mol.K2	14.18	SP-heat	358	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152032	PHB2690154	SC not investigated. Einstein-T = 75.1 K. SP-heat analyzed using Debye and Einstein model.	Ni2NbAl	Ni2Nb1Al1	Ni	2	Nb	1	Al	1																			1999																												Heusler			A	5.9755													L2<1>																																																																mJ/mol.K2	11.03	SP-heat	300	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152033	PHB2690154	SC not investigated. Einstein-T = 73.4 K. SP-heat analyzed using Debye and Einstein model.	Ni2TaAl	Ni2Ta1Al1	Ni	2	Ta	1	Al	1																			1999																												Heusler			A	5.9608													L2<1>																																																																mJ/mol.K2	10.06	SP-heat	301	SP-heat																																				arc-melting - ANN(800C, 5d, in vac)					Specific heat and electronic structure of Heusler compounds Ni2TAl (T = Ti, Zr, Hf, V, Nb, Ta)			IF-UFRGS, Porto Alegre, 91501-970, Brazil	Physica B, 269(1999)154	F.S. da Rocha,G.L.F. Fraga,D.E. Brandao,C.M. da Silva,A.A. Gomes		
152034	JPS0541673	e-ph coupling = 0.52. (dC/gamma*Tc) = 1.8.	Ni2NbAl	Ni2Nb1Al1	Ni	2	Nb	1	Al	1																			1985																												Heusler			A	5.969													L2<1>	K		2.15				0.1	2.15																				T		1.35							T/K		0.65			MHC152034		A		160										4	14							mJ/mol.K2	8	SP-heat	280	SP-heat																																				arc-melting - ANN(850-950C,7d)					Superconductivity of Ni2NbX (X = Al, Ga and Sn)			Electrotechnical Laboratory, Ibaraki 305, Japan	J.Phys.Soc.Jpn, 54(1985)1673	S.Waki,Y.Yamaguchi,K.Mitsugi		
152035	JPS0541673	e-ph coupling = 0.50	Ni2NbGa	Ni2Nb1Ga1	Ni	2	Nb	1	Ga	1																			1985																												Heusler			A	5.956													L2<1>	K		1.54					1.54																				T		0.6							T/K		0.64			MHC152035		A		230																		mJ/mol.K2	6.5	SP-heat	240	SP-heat																																				arc-melting - ANN(850-950C,7d)					Superconductivity of Ni2NbX (X = Al, Ga and Sn)			Electrotechnical Laboratory, Ibaraki 305, Japan	J.Phys.Soc.Jpn, 54(1985)1673	S.Waki,Y.Yamaguchi,K.Mitsugi		
152036	JPS0541673	e-ph coupling = 0.61. (dC/gamma*Tc) = 1.6.	Ni2NbSn	Ni2Nb1Sn1	Ni	2	Nb	1	Sn	1																			1985																												Heusler			A	6.157													L2<1>	K		2.9					2.9																				T		0.63							T/K		0.37			MHC152035		A		230																		mJ/mol.K2	4	SP-heat	206	SP-heat																																				arc-melting - ANN(850-950C,7d)					Superconductivity of Ni2NbX (X = Al, Ga and Sn)			Electrotechnical Laboratory, Ibaraki 305, Japan	J.Phys.Soc.Jpn, 54(1985)1673	S.Waki,Y.Yamaguchi,K.Mitsugi		
152037	PHB3781118	G-L = 54. (dC/gamma*Tc) = 1.90.	W7Re13B	W7Re13B1	W	7	Re	13	B	1																			2006																												beta-Mn	P4<1>32																	K		7.1					7.1											Oe		77							T		11.4														A		54			A		2925													mJ/mol.K2	65.2	SP-heat																																				W(4N),Mo(4N),Re(4N),a-B,a-C		arc-melting					Superconductivity in M7Re13X (M = W, Mo,  X = B, C) compounds			Department of Physics and Mathematics, Aoyama-Gakuin University, Fushinobe 5-10-1, Sagamihara, Kanagawa, Japan	Physica B, 378-380(2006)1118	K.Kawashima,A.Kawano,T.Muranaka,J.Akimitsu		
152038	PHB3781118	G-L = 80. (dC/gamma*Tc) = 1.93.	W7Re13C	W7Re13C1	W	7	Re	13	C	1																			2006																												beta-Mn	P4<1>32																	K		7.3					7.3											Oe		40							T		12.6														A		51			A		4060													mJ/mol.K2	64.2	SP-heat																																				W(4N),Mo(4N),Re(4N),a-B,a-C		arc-melting					Superconductivity in M7Re13X (M = W, Mo,  X = B, C) compounds			Department of Physics and Mathematics, Aoyama-Gakuin University, Fushinobe 5-10-1, Sagamihara, Kanagawa, Japan	Physica B, 378-380(2006)1118	K.Kawashima,A.Kawano,T.Muranaka,J.Akimitsu		
152039	PHB3781118	G-L = 101. (dC/gamma*Tc) = 1.84.	Mo7Re13B	Mo7Re13B1	Mo	7	Re	13	B	1																			2006																												beta-Mn	P4<1>32																	K		8.3					8.3											Oe		30							T		15.4														A		46			A		4684													mJ/mol.K2	66.9	SP-heat																																				W(4N),Mo(4N),Re(4N),a-B,a-C		arc-melting					Superconductivity in M7Re13X (M = W, Mo,  X = B, C) compounds			Department of Physics and Mathematics, Aoyama-Gakuin University, Fushinobe 5-10-1, Sagamihara, Kanagawa, Japan	Physica B, 378-380(2006)1118	K.Kawashima,A.Kawano,T.Muranaka,J.Akimitsu		
152040	PHB3781118	G-L = 98. (dC/gamma*Tc) = 2.53.	Mo7Re13C	Mo7Re13C1	Mo	7	Re	13	C	1																			2006																												beta-Mn	P4<1>32																	K		8.1					8.1											Oe		31							T		14.8														A		47			A		4608													mJ/mol.K2	57.5	SP-heat																																				W(4N),Mo(4N),Re(4N),a-B,a-C		arc-melting					Superconductivity in M7Re13X (M = W, Mo,  X = B, C) compounds			Department of Physics and Mathematics, Aoyama-Gakuin University, Fushinobe 5-10-1, Sagamihara, Kanagawa, Japan	Physica B, 378-380(2006)1118	K.Kawashima,A.Kawano,T.Muranaka,J.Akimitsu		
152041	PCS0693011	gap measured by point contact tunneling. Heat capacity by ac-calorimetry. [gamma] estimated using entropy conservation law.  (dC/gamma*Tc) = 1.71	MgCNi3	Mg1C1Ni3	Mg	1	C	1	Ni	3																		3	2008																												CaTiO3																		K		6.6					6.6																																														meV	1	3.8	1																																															crystals grown by high pressure closed system.					Superconducting energy gap in MgCNi3 single crystals			Centre of Low Temperature Physics, Institute of Experimental Physics, Slovak Academy of Sciences,  Slovakia	J.Phys.Chem.Solids, 69(2008)3011	J.Kacmarcik,Z.Pribulova,P.Szabo,P.Samuely,C.Marcenat,T.Klein,D.-J. Jang,H.-G.Lee,H.-S.Lee,S.I.Lee		
152042	PCS0693074	slightly overdoped. Gaps measured by Raman.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2008																												Tl2201																		K		80					80																																																6.8	4																																															flux method. O-content [oz] controlled by annealing condition in Ar.					Superconducting gap of overdoped Tl2Ba2CuO6+d  observed by Raman scattering			Department of Physics, Graduate School of Science, Osaka University, Osaka 560-0043, Japan	J.Phys.Chem.Solids, 69(2008)3074	K. Nishikawa,T.Masui,S.Tajima,H.Eisaki,H.Kito,A.Iyo		
152043	PCS0693074	overdoped sample. hole concentration  estimated to be p = 0.22 from Tallon's eq. using Tc(max) = 90 K. Gaps measured by Raman.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2008																												Tl2201																		K		62					62																																																7.2	4																																															flux method. O-content [oz] controlled by annealing condition in Ar.					Superconducting gap of overdoped Tl2Ba2CuO6+d  observed by Raman scattering			Department of Physics, Graduate School of Science, Osaka University, Osaka 560-0043, Japan	J.Phys.Chem.Solids, 69(2008)3074	K. Nishikawa,T.Masui,S.Tajima,H.Eisaki,H.Kito,A.Iyo		
152044	PCS0693074	overdoped sample. hole concentration  estimated to be p = 0.23 from Tallon's eq. using Tc(max) = 90 K. Gaps measured by Raman.	Tl2Ba2CuO6	Tl2Ba2Cu1O6+z	Tl	2	Ba	2	Cu	1															O	6+z		3	2008																												Tl2201																		K		52					52																																																3.9	4																																															flux method. O-content [oz] controlled by annealing condition in Ar.					Superconducting gap of overdoped Tl2Ba2CuO6+d  observed by Raman scattering			Department of Physics, Graduate School of Science, Osaka University, Osaka 560-0043, Japan	J.Phys.Chem.Solids, 69(2008)3074	K. Nishikawa,T.Masui,S.Tajima,H.Eisaki,H.Kito,A.Iyo		
152045	PCS0693153	[gapene] from <11>B NMR measurements. e-ph coupling = 0.69 from McMillan's eq. Debye-T from PRB0331671	LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	2008																												LuRuB2																		K		10.2					10.2																																																3.52	6										487	SP-heat																																				arc-melting in Ar  -  ANN(1050C)					<11>B NMR relaxation in superconductors: YRuB2  and  LuRuB2			Department of Quantum Materials Science, University of Tokushima, 2-1 Minami-josanjima, Tokushima 770-8506, Japan	J.Phys.Chem.Solids, 69(2008)3153	Y.Kishimoto,Y.Kawasaki,M.Tanabe,Y.Ideta,T.Ohno,G.Ghosh,A.K.Tyagi,L.C.Gupta		
152046	PCS0693153	[gapene] from <11>B NMR measurements. e-ph coupling = 0.63 from McMillan's eq.	YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																		1	2008																												LuRuB2																		K		7.6					7.6																																																3.52	6																																															arc-melting in Ar  -  ANN(1050C)					<11>B NMR relaxation in superconductors: YRuB2  and  LuRuB2			Department of Quantum Materials Science, University of Tokushima, 2-1 Minami-josanjima, Tokushima 770-8506, Japan	J.Phys.Chem.Solids, 69(2008)3153	Y.Kishimoto,Y.Kawasaki,M.Tanabe,Y.Ideta,T.Ohno,G.Ghosh,A.K.Tyagi,L.C.Gupta		
152047	PRB0331671	RRR=6. [gamma] calculated from [dHc2/dT] and Rn.	LuRUB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	1986																												LuRuB2			A	5.7973	5.233	6.2817												K	10.44		10.72				10.58																													kOe/K	resistivity	7.5			MHC152047																						mJ/mol.K2	8.7	calc from (dHc2/dT) and RESN													uOhm.cm							55																		arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152048	PRB0331671	[gamma] calculated from [dHc2/dT] and Rn.	(Lu,Er)RUB2	Lu0.85Er0.15Ru1B2	Lu	0.85	Er	0.15	Ru	1	B	2																1	1986																												LuRuB2			A	5.8049	5.2389	6.2866												K	8.51		9.21				8.86																													kOe/K	resistivity	5.8			MHC152047																						mJ/mol.K2	8.4	calc from (dHc2/dT) and RESN													uOhm.cm							44																		arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152049	PRB0331671	[gamma] calculated from [dHc2/dT] and Rn.	(Lu,Er)RUB2	Lu0.65Er0.35Ru1B2	Lu	0.65	Er	0.35	Ru	1	B	2																1	1986																												LuRuB2																		K	6.85		7.03				6.94																													kOe/K	resistivity	2.5			MHC152047																						mJ/mol.K2	7.3	calc from (dHc2/dT) and RESN													uOhm.cm							22																		arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152050	PRB0331671	[gamma] calculated from [dHc2/dT] and Rn. magnetic order (re-entrant = 1.91 K) defined as the peak of ac-SUS.	(Lu,Er)RUB2	Lu0.6Er0.4Ru1B2	Lu	0.6	Er	0.4	Ru	1	B	2																1	1986																												LuRuB2			A	5.8157	5.2481	6.2908												K	6.17		6.42				6.295	MTC152050																												kOe/K	resistivity	2			MHC152050																						mJ/mol.K2	6.7	calc from (dHc2/dT) and RESN													uOhm.cm							19																		arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152051	PRB0331671	RRR=14. [gamma] calculated from [dHc2/dT] and Rn. magnetic order (re-entrant = 3.75 K) defined as the peak of ac-SUS.	(Lu,Er)RUB2	Lu0.55Er0.45Ru1B2	Lu	0.55	Er	0.45	Ru	1	B	2																1	1986																												LuRuB2			A	5.82	5.2514	6.2924												K	4.95		5.57				5.26	MTC152050																												kOe/K	resistivity	0.9			MHC152050																						mJ/mol.K2	3.6	calc from (dHc2/dT) and RESN													uOhm.cm							15																		arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152052	PRB0331671	Tc from SP-heat. e-ph coupling = 0.59. (dC/gamma*Tc) = 1.09. lattice term const.of SP: beta = 0.0675 mJ/mol.K4	LuRUB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	1986																												LuRuB2																		K		8.9					8.9																																																3.02	14					mJ/mol.K	68		7.05	SP-heat	487	SP-heat																																				arc-melting(Lu,Er) - arc-melting(Lu1-xErx, RuB2) - sealed in Ta-tube(Ar) - ANN(1250C,2d) - ANN(1000C,2-3w) Q to RT					Upper critical field and heat capacity in the reentrant superconducting system (Lu1-xErx)RuB2			Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 33(1986)1671	R.N.Shelton,H.E.Horng		
152053	SSC0400237		LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	1981																												LuRuB2			A	5.809	5.229	6.284												K	9.84			9.99			9.99																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152054	SSC0400237		(Lu,Tm)RuB2	Lu0.8Tm0.2Ru1B2	Lu	0.8	Tm	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				7.28			7.28																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152055	SSC0400237		(Lu,Tm)RuB2	Lu0.6Tm0.4Ru1B2	Lu	0.6	Tm	0.4	Ru	1	B	2																1	1981								1.08																				LuRuB2																		K				4.31			4.31	MTC152056																																																																																															arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152056	SSC0400237		(Lu,Tm)RuB2	Lu0.55Tm0.45Ru1B2	Lu	0.55	Tm	0.45	Ru	1	B	2																1	1981								1.69																				LuRuB2																		K				2.94			2.94	MTC152056																																																																																															arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152057	SSC0400237	not SC. magnetic ordering (AF) at 4.07 K.	(Lu,Tm)RuB2	Tm1Ru1B2	Tm	1	Ru	1	B	2																		1	1981								4.07																				LuRuB2			A	5.831	5.254	6.299												K					1.2																																																																																																		arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152058	SSC0400237		(Lu,Gd)RuB2	Lu0.9Gd0.1Ru1B2	Lu	0.9	Gd	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				6.4			6.4																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152059	SSC0400237		(Lu,Tb)RuB2	Lu0.9Tb0.1Ru1B2	Lu	0.9	Tb	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				4.76			4.76																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152060	SSC0400237		(Lu,Dy)RuB2	Lu0.9Dy0.1Ru1B2	Lu	0.9	Dy	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				7.34			7.34																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152061	SSC0400237		(Lu,Ho)RuB2	Lu0.9Ho0.1Ru1B2	Lu	0.9	Ho	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				7.53			7.53																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152062	SSC0400237		(Lu,Er)RuB2	Lu0.9Er0.1Ru1B2	Lu	0.9	Er	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				8.77			8.77																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152063	SSC0400237		(Lu,Tm)RuB2	Lu0.9Tm0.1Ru1B2	Lu	0.9	Tm	0.1	Ru	1	B	2																1	1981																												LuRuB2																		K				8.72			8.72																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152064	SSC0400237		(Lu,Gd)RuB2	Lu0.8Gd0.2Ru1B2	Lu	0.8	Gd	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				4.84			4.84																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152065	SSC0400237	not SC	(Lu,Tb)RuB2	Lu0.8Tb0.2Ru1B2	Lu	0.8	Tb	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K					1.2																																																																																																		arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152066	SSC0400237		(Lu,Dy)RuB2	Lu0.8Dy0.2Ru1B2	Lu	0.8	Dy	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				5.07			5.07																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152067	SSC0400237		(Lu,Ho)RuB2	Lu0.8Ho0.2Ru1B2	Lu	0.8	Ho	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				6.46			6.46																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152068	SSC0400237		(Lu,Er)RuB2	Lu0.8Er0.2Ru1B2	Lu	0.8	Er	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				7.85			7.85																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152069	SSC0400237		(Lu,Tm)RuB2	Lu0.8Tm0.2Ru1B2	Lu	0.8	Tm	0.2	Ru	1	B	2																1	1981																												LuRuB2																		K				7.31			7.31																																																																																																arc-melting - ANN(1000C,1w)					Reentrant superconductivity in the orthorhombic system (Tm1-xLux)RuB2			University of California,San Diego,La Jolla, CA 92093	Solid State Commun., 40(1981)237	H.C.Ku,R.N.Shelton		
152100	JAP0491392		(Y,Gd)Rh4B4	Y0.99Gd0.01Rh4B4	Y	0.99	Gd	0.01	Rh	4	B	4																	1978																										AB4C4		RT4B4																	CeCo4B4	K		10.1					10.1																																		MHC152100																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152101	JAP0491392		(Y,Gd)Rh4B4	Y0.9Gd0.1Rh4B4	Y	0.9	Gd	0.1	Rh	4	B	4																	1978																										AB4C4		RT4B4																	CeCo4B4	K		8.66					8.66																																		MHC152100																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152102	JAP0491392		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1978								0.77																		AB4C4		RT4B4																	CeCo4B4	K		8.66					8.66																																		MHC152102																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152103	JAP0491392		(Er,Gd)Rh4B4	Er0.98Gd0.02Rh4B4	Er	0.98	Gd	0.02	Rh	4	B	4																	1978								0.89																		AB4C4		RT4B4																	CeCo4B4	K		8.22					8.22																																		MHC152102																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152104	JAP0491392		(Er,Gd)Rh4B4	Er0.97Gd0.03Rh4B4	Er	0.97	Gd	0.03	Rh	4	B	4																	1978								0.94																		AB4C4		RT4B4																	CeCo4B4	K		8.06					8.06			K/GPa	0.05																														MHC152104																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152105	JAP0491392		(Er,Gd)Rh4B4	Er0.95Gd0.05Rh4B4	Er	0.95	Gd	0.05	Rh	4	B	4																	1978								0.98																		AB4C4		RT4B4																	CeCo4B4	K		7.61					7.61	MTC152105		K/GPa	0.05																														MHC152104																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152106	JAP0491392		(Er,Gd)Rh4B4	Er0.91Gd0.09Rh4B4	Er	0.91	Gd	0.09	Rh	4	B	4																	1978								1.26																		AB4C4		RT4B4																	CeCo4B4	K		6.87					6.87																																		MHC152106																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152107	JAP0491392		(Er,Gd)Rh4B4	Er0.8Gd0.2Rh4B4	Er	0.8	Gd	0.2	Rh	4	B	4																	1978								1.78																		AB4C4		RT4B4																	CeCo4B4	K		4.41					4.41	MTC152107																																	MHC152106																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152108	JAP0491392		(Er,Gd)Rh4B4	Er0.76Gd0.24Rh4B4	Er	0.76	Gd	0.24	Rh	4	B	4																	1978								1.89																		AB4C4		RT4B4																	CeCo4B4	K		4.18					4.18																																		MHC152106																																																														arc-melting(in Ar) - ANN(1000C, 1-14d)					Magnetic and superconducting transitions in GdxEr1-xRh4B4 and GdxY1-xEh4B4			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 49(1978)1392	R.H.Wang,R.J.Laskowski,C.Y.Huang,J.L.Smith,C.W.Chu		
152110	JAP0501862		(Er,Gd)Rh4B4	Er0.9Gd0.1Rh4B4	Er	0.9	Gd	0.1	Rh	4	B	4																	1979								1.34																		AB4C4		RT4B4																	CeCo4B4	K				6.88			6.88	MTC152110																																																																																															ANN(1000C,30d)					Magnetic ordering of GdxEr1-xRh4B4 near the superconducting region			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 50(1979)1862	S.Kohn,R.H.Wang,J.L.Smith,C.Y.Huang		
152111	JAP0501862		(Er,Gd)Rh4B4	Er0.72Gd0.28Rh4B4	Er	0.72	Gd	0.28	Rh	4	B	4																	1979								2.25																		AB4C4		RT4B4																	CeCo4B4	K				2.5			2.5																																																																																																ANN(1000C,30d)					Magnetic ordering of GdxEr1-xRh4B4 near the superconducting region			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	J.Appl.Phys., 50(1979)1862	S.Kohn,R.H.Wang,J.L.Smith,C.Y.Huang		
152112	PRB0220164		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1980																										AB4C4		RT4B4																	CeCo4B4	K		8.7					8.7																																																																																																					Crystal-field effects in magnetic superconducting Er1-xTmxRh4B4 and Er1-xHoxRh4B4				Phys.Rev.B, 22(1980)164	S.Maekawa,J.L.Smith,C.Y.Huang		
152113	PRB0220164		(Er,Tm)Rh4B4	Er0.97Tm0.15Rh4B4	Er	0.97	Tm	0.15	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		8.86					8.86	MTC152113																																																																																																				Crystal-field effects in magnetic superconducting Er1-xTmxRh4B4 and Er1-xHoxRh4B4				Phys.Rev.B, 22(1980)164	S.Maekawa,J.L.Smith,C.Y.Huang		
152114	PRB0220164		(Er,Tm)Rh4B4	Er0.97Tm0.3Rh4B4	Er	0.97	Tm	0.3	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		9.03					9.03	MTC152113																																																																																																				Crystal-field effects in magnetic superconducting Er1-xTmxRh4B4 and Er1-xHoxRh4B4				Phys.Rev.B, 22(1980)164	S.Maekawa,J.L.Smith,C.Y.Huang		
152115	PRB0220164		(Er,Tm)Rh4B4	Tm1Rh4B4	Tm	1	Rh	4	B	4																			1980																										AB4C4		RT4B4																	CeCo4B4	K		9.6					9.6																																																																																																					Crystal-field effects in magnetic superconducting Er1-xTmxRh4B4 and Er1-xHoxRh4B4				Phys.Rev.B, 22(1980)164	S.Maekawa,J.L.Smith,C.Y.Huang		
152116	SSC0320929		(Y,Gd)Rh4B4	Y0.7Gd0.3Rh4B4	Y	0.7	Gd	0.3	Rh	4	B	4																	1979																										AB4C4		RT4B4																	CeCo4B4	K		3.54					3.54																																		MHC152116																																																																			Anomalous temperature dependence of the upper critical fields in magnetic-superconducting Y1-xGdxRh4B4				Solid State Commun., 32(1979)929	C.Y.Huang,S.E.Kohn,S.Maekawa,J.L.Smith		
152117	SSC0320185		(Y,Er)Rh4B4	Y0.83Er0.17Rh4B4	Y	0.83	Er	0.17	Rh	4	B	4																	1979																										AB4C4		RT4B4																	CeCo4B4	K		10.4					10.4	MTC152117																																	MHC152117																																																														arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152118	SSC0320185		(Y,Er)Rh4B4	Y0.71Er0.29Rh4B4	Y	0.71	Er	0.29	Rh	4	B	4																	1979																										AB4C4		RT4B4																	CeCo4B4	K		10					10																																		MHC152118																																																														arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152119	SSC0320185	magnetic order: Ferromagnetic	(Y,Er)Rh4B4	Y0.56Er0.44Rh4B4	Y	0.56	Er	0.44	Rh	4	B	4																	1979							0.104																			AB4C4		RT4B4																	CeCo4B4	K		9.64					9.64																																		MHC152117																																																														arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152120	SSC0320185	magnetic order: Ferromagnetic	(Y,Er)Rh4B4	Y0.47Er0.53Rh4B4	Y	0.47	Er	0.53	Rh	4	B	4																	1979							0.306																			AB4C4		RT4B4																	CeCo4B4	K		9.5					9.5	MTC152117																																	MHC152118																																																														arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152121	SSC0320185	magnetic order: Ferromagnetic	(Y,Er)Rh4B4	Y0.28Er0.72Rh4B4	Y	0.28	Er	0.72	Rh	4	B	4																	1979							0.626																			AB4C4		RT4B4																	CeCo4B4	K		9.05					9.05																																		MHC152117																																																														arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152122	SSC0320185	magnetic order: Ferromagnetic	(Y,Er)Rh4B4	Y0.12Er0.88Rh4B4	Y	0.12	Er	0.88	Rh	4	B	4																	1979							0.766																			AB4C4		RT4B4																	CeCo4B4	K		8.74					8.74																																																																																																arc-melting(MB4 + Rh) - ANN(1050C, 1w)					Superconducting phase transitions in ErcY1-cRh4B4			Osaka University,Toyonaka,Osaka,Japan	Solid State Commun., 32(1979)185	K.Okuda,Y.Nakakura,K.Kadowaki		
152123	SSC0260141		ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1978								0.924																		AB4C4		RT4B4																	CeCo4B4	K		8.76					8.76																																																																																																arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152124	SSC0260141		(Er,Ho)Rh4B4	Er0.73Ho0.27Rh4B4	Er	0.73	Ho	0.27	Rh	4	B	4																	1978								0.721																		AB4C4		RT4B4																	CeCo4B4	K		8.06					8.06	MTC152124																																																																																															arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152125	SSC0260141		(Er,Ho)Rh4B4	Er0.187Ho0.813Rh4B4	Er	0.187	Ho	0.813	Rh	4	B	4																	1978								5.21																		AB4C4		RT4B4																	CeCo4B4	K		6.43					6.43																																																																																																arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152126	SSC0260141		(Er,Ho)Rh4B4	Er0.11Ho0.89Rh4B4	Er	0.11	Ho	0.89	Rh	4	B	4																	1978								5.87																		AB4C4		RT4B4																	CeCo4B4	K		5.96					5.96	MTC152124																																																																																															arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152127	SSC0260141	not SC	(Er,Ho)Rh4B4	Er0.085Ho0.915Rh4B4	Er	0.085	Ho	0.915	Rh	4	B	4																	1978								6.11																		AB4C4		RT4B4																	CeCo4B4	K					1																																																																																																		arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152128	SSC0260141	not SC	HoRh4B4	Ho1Rh4B4	Ho	1	Rh	4	B	4																			1978								6.69																		AB4C4		RT4B4																	CeCo4B4	K					1																																																																																																		arc-melting in Ar.  ANN(1200C,1w, in sealed Ta-tube) - ANN(900C,3w)					Re-entrant superconductivity and magnetic ordering in the pseudoternary system (Er1-xHox)Rh4B4				Solid State Commun., 26(1978)141	D.C.Johnston,W.A.Fertig,M.B.Maple,B.T.Matthias		
152129	SSC0350937		DyRh4B4	Dy1Rh4B4	Dy	1	Rh	4	B	4																			1980								11.2																		AB4C4		RT4B4			A	5.3023		7.3944												K					1																																																																																																		arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152130	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh3.6Ir0.4B4	Dy	1	Rh	3.6	Ir	0.4	B	4																	1980								4.78																		AB4C4		RT4B4			A	5.313		7.4039												K					1																																																																																																		arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152131	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh3.2Ir0.8B4	Dy	1	Rh	3.2	Ir	0.8	B	4																	1980																										AB4C4		RT4B4			A	5.3202		7.4089												K		1.78					1.78																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152132	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh2.8Ir1.2B4	Dy	1	Rh	2.8	Ir	1.2	B	4																	1980																										AB4C4		RT4B4			A	5.3251		7.4127												K		2.82					2.82	MTC152132																																																																																															arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152133	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh2.4Ir1.6B4	Dy	1	Rh	2.4	Ir	1.6	B	4																	1980																										AB4C4		RT4B4			A	5.3312		7.4141												K		3.83					3.83																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152134	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh2Ir2B4	Dy	1	Rh	2	Ir	2	B	4																	1980																										AB4C4		RT4B4			A	5.3442		7.4145												K		4.53					4.53																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152136	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh1.6Ir2.4B4	Dy	1	Rh	1.6	Ir	2.4	B	4																	1980								3.78																		AB4C4		RT4B4			A	5.3445		7.4148												K		4.3					4.3																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152137	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh1.2Ir2.8B4	Dy	1	Rh	1.2	Ir	2.8	B	4																	1980								4.39																		AB4C4		RT4B4			A	5.3598		7.3853												K		1.63					1.63	MTC152132																																																																																															arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152138	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh0.8Ir3.2B4	Dy	1	Rh	0.8	Ir	3.2	B	4																	1980																										AB4C4		RT4B4			A	5.3763		7.3545												K		1.17					1.17																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152139	SSC0350937		Dy(Rh,Ir)4B4	Dy1Rh0.56Ir3.44B4	Dy	1	Rh	0.56	Ir	3.44	B	4																	1980																										AB4C4		RT4B4			A	5.3845		7.3397												K		1.29					1.29																																																																																																arc-melting					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152140	SSC0320937		Er(Rh,Ir)4B4	Er1Rh3.6Ir0.4B4	Er	1	Rh	3.6	Ir	0.4	B	4																	1979																										AB4C4		RT4B4																		K		7.95					7.95																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152141	SSC0320937		Er(Rh,Ir)4B4	Er1Rh2.4Ir1.6B4	Er	1	Rh	2.4	Ir	1.6	B	4																	1979																										AB4C4		RT4B4																		K		7.56					7.56	MTC152141																																																																																																				Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152142	SSC0320937		Er(Rh,Ir)4B4	Er1Rh2Ir2B4	Er	1	Rh	2	Ir	2	B	4																	1979																										AB4C4		RT4B4																		K		6.76					6.76																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152143	SSC0320937		Er(Rh,Ir)4B4	Er1Rh1.6Ir2.4B4	Er	1	Rh	1.6	Ir	2.4	B	4																	1979																										AB4C4		RT4B4																		K		2.11					2.11																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152144	SSC0350937		Ho(Rh,Ir)4B4	Ho1Rh3.6Ir0.4B4	Ho	1	Rh	3.6	Ir	0.4	B	4																	1980																										AB4C4		RT4B4																		K		5.09					5.09																																																																																																					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152145	SSC0350937		Ho(Rh,Ir)4B4	Ho1Rh2Ir2B4	Ho	1	Rh	2	Ir	2	B	4																	1980																										AB4C4		RT4B4																		K		6.35					6.35	MTC152145																																																																																																				Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152146	SSC0350937		Ho(Rh,Ir)4B4	Ho1Rh1.6Ir2.4B4	Ho	1	Rh	1.6	Ir	2.4	B	4																	1980																										AB4C4		RT4B4																		K		2.2					2.2																																																																																																					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152147	SSC0350937		Ho(Rh,Ir)4B4	Ho1Rh0.8Ir3.2B4	Ho	1	Rh	0.8	Ir	3.2	B	4																	1980																										AB4C4		RT4B4																		K		1.26					1.26																																																																																																					Superconducting Dy(IrxRh1-x)4B4 system				Solid State Commun., 35(1980)937	H.C.Ku,F.Acker		
152148	SSC0330843	Tm is FM order (M//ab-plane). (dTc2/dP) = 0 K/GPa for normal-to-SC transition.	ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1980																										AB4C4		RT4B4																	CeCo4B4	K		8.7					8.7			K/GPa	0.05																																																																																												arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152149	SSC0330843	Tm is FM order (M//ab-plane). (dTc2/dP) = 0.019 K/GPa for normal-to-SC transition.	(Er,Ho)Rh4B4	Er0.79Ho0.21Rh4B4	Er	0.79	Ho	0.21	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		8.22					8.22			K/GPa	0.05																																																																																												arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152150	SSC0330843	Tm is FM order (M//ab-plane). (dTc2/dP) = 0.041 K/GPa for normal-to-SC transition.	(Er,Ho)Rh4B4	Er0.46Ho0.54Rh4B4	Er	0.46	Ho	0.54	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		7.32					7.32			K/GPa	0.028																																																																																												arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152151	SSC0330843	Tm is FM order (M//ab-plane). (dTc2/dP) = 0.085 K/GPa for normal-to-SC transition.	(Er,Ho)Rh4B4	Er0.134Ho0.866Rh4B4	Er	0.134	Ho	0.866	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		6.15					6.15	MTC152151		K/GPa	0.022																																																																																												arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152152	SSC0330843	Tm is FM order (M//ab-plane). (dTc2/dP) = 0.146 K/GPa for normal-to-SC transition.	(Er,Ho)Rh4B4	Er0.11Ho0.89Rh4B4	Er	0.11	Ho	0.89	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K		5.98					5.98	MTC152152		K/GPa	0.055																																																																																												arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152153	SSC0330843	For FM order, (dTm/dP) = 0.093 K/GPa.	(Er,Ho)Rh4B4	Er0.085Ho0.915Rh4B4	Er	0.085	Ho	0.915	Rh	4	B	4																	1980																										AB4C4		RT4B4																	CeCo4B4	K					0.3																																																																																																		arc-melting - ANN(1200C,1w, in Ta-tube) - ANN(900C,3w)					Pressure enhanced superconductive and magnetic interactions in the system (Er1-xHox)Rh4B4			Ames Lab, Iowa State University, Ames, Iowa	Solid State Commun., 33(1980)843	R.N.Shelton,C.U.Segre,D.C.Johnston		
152154	PRL0380987	XRD shows impurity phases(several %). long range magnetic order FM) at 0.9 K. lattice term coeff. in SP (beta) = 3.1 mJ/mol.K4.	ErRh4B4	Er1Rh4B4	Er	1	Rh	4	B	4																			1977					myu-B/Er	9.62	1																			AB4C4		RT4B4			A	5.299		7.388											CeCo4B4	K		8.7					8.7																																																								mJ/mol.K2	29	SP-heat																																						arc-melting - ANN					Destruction of superconductivity at the onset of long-range magnetic order in the compound ErRh4B4			University of California, San Diego, La Jolla, California	Phys.Rev.Lett., 38(1977)987	W.A.Fertig,D.C.Johnston,L..E..DeLong,R.W.McCallum,M.B.Maple,B.T.Matthias		
152160	PRB081174512		Ba(Fe,Ru)2As2	Ba1Fe1.5Ru0.5As2	Ba	1	Fe	1.5	Ru	0.5	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9774		12.934												K				0			0																																																																																														FeAs,RuAs,Ba		solid state reaction. heat(1173K,5h)					Superconductivity in Ru-substituted polycrystalline BaFe2-xRuxAs2			Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Phys.Rev.B, 81(2010)174512	Shilpam Sharma,A. Bharathi,Sharat Chandra,V. Raghavendra Reddy,S. Paulraj,A. T. Satya,V. S. Sastry,Ajay Gupta,C. S. Sundar		
152161	PRB081174512	Hall effect at H=2 T.	Ba(Fe,Ru)2As2	Ba1Fe1.25Ru0.75As2	Ba	1	Fe	1.25	Ru	0.75	As	2																	2010																										AB2C2		ThCr2Si2			A	4.0059		12.85												K				21			21																																		MHC152161																																																									MRH152161			FeAs,RuAs,Ba		solid state reaction. heat(1173K,5h)					Superconductivity in Ru-substituted polycrystalline BaFe2-xRuxAs2			Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Phys.Rev.B, 81(2010)174512	Shilpam Sharma,A. Bharathi,Sharat Chandra,V. Raghavendra Reddy,S. Paulraj,A. T. Satya,V. S. Sastry,Ajay Gupta,C. S. Sundar		
152162	PRB081174512		Ba(Fe,Ru)2As2	Ba1Fe1.125Ru0.875As2	Ba	1	Fe	1.125	Ru	0.875	As	2																	2010																										AB2C2		ThCr2Si2			A	4.0298		12.775												K				22.5			22.5	MTC152162																																	MHC152162																																																												FeAs,RuAs,Ba		solid state reaction. heat(1173K,5h)					Superconductivity in Ru-substituted polycrystalline BaFe2-xRuxAs2			Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Phys.Rev.B, 81(2010)174512	Shilpam Sharma,A. Bharathi,Sharat Chandra,V. Raghavendra Reddy,S. Paulraj,A. T. Satya,V. S. Sastry,Ajay Gupta,C. S. Sundar		
152163	PRB081174512		Ba(Fe,Ru)2As2	Ba1Fe0.875Ru1.125As2	Ba	1	Fe	0.875	Ru	1.125	As	2																	2010																										AB2C2		ThCr2Si2			A	4.0502		12.679												K				21.3			21.3																																		MHC152163																																																												FeAs,RuAs,Ba		solid state reaction. heat(1173K,5h)					Superconductivity in Ru-substituted polycrystalline BaFe2-xRuxAs2			Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Phys.Rev.B, 81(2010)174512	Shilpam Sharma,A. Bharathi,Sharat Chandra,V. Raghavendra Reddy,S. Paulraj,A. T. Satya,V. S. Sastry,Ajay Gupta,C. S. Sundar		
152164	PRB081174512		Ba(Fe,Ru)2As2	Ba1Fe0.75Ru1.25As2	Ba	1	Fe	0.75	Ru	1.25	As	2																	2010																										AB2C2		ThCr2Si2			A	4.0692		12.595												K				0			0																																																																																														FeAs,RuAs,Ba		solid state reaction. heat(1173K,5h)					Superconductivity in Ru-substituted polycrystalline BaFe2-xRuxAs2			Condensed Matter Physics Division, Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Phys.Rev.B, 81(2010)174512	Shilpam Sharma,A. Bharathi,Sharat Chandra,V. Raghavendra Reddy,S. Paulraj,A. T. Satya,V. S. Sastry,Ajay Gupta,C. S. Sundar		
152165	PRB081184519	T<SDW> = 134 K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2			A	3.9613		13.019												K			0				0																																																																																																mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152166	PRB081184519	P-content by EDX. T<SDW> = 94.4 K,  T<STR> = 101 K.	BaFe2(As,P)2	Ba1Fe2As1.72P0.28	Ba	1	Fe	2	As	1.72	P	0.28																3	2010																										AB2C2		ThCr2Si2																		K			0				0																																																																																																mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152167	PRB081184519	P-content by EDX. T<SDW> = 72.8 K,  T<STR> = 87 K.	BaFe2(As,P)2	Ba1Fe2As1.6P0.4	Ba	1	Fe	2	As	1.6	P	0.4																3	2010																										AB2C2		ThCr2Si2			A	3.9419		12.899												K	5.95		21				13.475	MPH152167																																																																																															mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152168	PRB081184519	P-content by EDX.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																3	2010																										AB2C2		ThCr2Si2			A	3.9247		12.813												K	30.5		30.5				30.5																																																																																																mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152169	PRB081184519	P-content by EDX.	BaFe2(As,P)2	Ba1Fe2As1.18P0.82	Ba	1	Fe	2	As	1.18	P	0.82																3	2010																										AB2C2		ThCr2Si2			A	3.9161		12.778												K	23.8		26.8				25.3																																																																																																mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152170	PRB081184519	P-content by EDX.	BaFe2(As,P)2	Ba1Fe2As0.72P1.28	Ba	1	Fe	2	As	0.72	P	1.28																3	2010																										AB2C2		ThCr2Si2			A	3.8839		12.632												K	6.69		10.4				8.545																																																																																																mixture in alumina - sealed in quartz tube - heat(1150C-1200C,12h) - cool to 800C(1.5C/h)					Evolution from non-Fermi- to Fermi-liquid transport via isovalent doping in BaFe2(As1-xPx)2 superconductors			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)184519	S. Kasahara,T. Shibauchi,K. Hashimoto,K. Ikada,S. Tonegawa,R. Okazaki,H. Shishido,H. Ikeda,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
152171	PRB081174524		Ba(Fe,Ni)2As2	Ba1Fe1.925Ni0.075As2	Ba	1	Fe	1.925	Ni	0.075	As	2																3	2010								58																		AB2C2		ThCr2Si2																		K				12.2			12.2																																																																																																self-flux method					Electron-doping evolution of the low-energy spin excitations in the iron arsenide superconductor BaFe2-xNixAs2			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 81(2010)174524	Miaoyin Wang,Huiqian Luo,Jun Zhao,Chenglin Zhang,Meng Wang,Karol Marty,Songxue Chi,Jeffrey W. Lynn,Astrid Schneidewind,Shiliang Li,Pengcheng Dai		
152172	PRB081174524		Ba(Fe,Ni)2As2	Ba1Fe1.85Ni0.15As2	Ba	1	Fe	1.85	Ni	0.15	As	2																3	2010																										AB2C2		ThCr2Si2																		K				13.8			13.8																																																																																																self-flux method					Electron-doping evolution of the low-energy spin excitations in the iron arsenide superconductor BaFe2-xNixAs2			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Phys.Rev.B, 81(2010)174524	Miaoyin Wang,Huiqian Luo,Jun Zhao,Chenglin Zhang,Meng Wang,Karol Marty,Songxue Chi,Jeffrey W. Lynn,Astrid Schneidewind,Shiliang Li,Pengcheng Dai		
152173	PRB081184509	P-induced SC. Tc defined as R-anomaly. single crystals(1*0.25*0.025 mm3)  was located in Be-Cu Bridgman anvil clamped cell. Quasihydrostatic pressure.	Bi2Sr2YCu2O8	Bi1.98Sr2.06Y0.68Cu2O8+z	Bi	1.98	Sr	2.06	Y	0.68	Cu	2													O	8+z		3	2010																												Bi2212																		K			8		0		8	TC152173																																																																																															floating zone method					Signatures of pressure-induced superconductivity in insulating Bi1.98Sr2.06Y0.68CaCu2O8+z			Materials Science Division, Lawrence Berkeley National Laboratory, University of California-Berkeley, Berkeley, California 94720, USA	Phys.Rev.B, 81(2010)184509	T. Cuk,D. A. Zocco,H. Eisaki,V. Struzhkin,F. M. Grosche,M. B. Maple,Z.-X. Shen		
152174	SSC0320937		ErIr4B4	Er1Ir4B4	Er	1	Ir	4	B	4																			1979																										AB4C4		RT4B4			A	5.408		7.278											CeCo4B4	K		2.34					2.34																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152175	SSC0320937		TmIr4B4	Tm1Ir4B4	Tm	1	Ir	4	B	4																			1979																										AB4C4		RT4B4			A	5.404		7.281											CeCo4B4	K		1.75					1.75																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152176	SSC0320937		HoIr4B4	Ho1.1Ir4B3.6	Ho	1.1	Ir	4	B	3.6																			1979																										AB4C4		RT4B4																	CeCo4B4	K		2.12					2.12																																																																																																					Superconductivity, Magnetism and metastability of new ternary iridium borides			Univ. California, San Diego, La Jolla, CA, USA	Solid State Commun., 32(1979)937	B.T.Matthias,H.Barz,H.C.Ku		
152177	PRB081184504	Hall coeff. RH(150K) = -4.10 E-9 m3/C.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85			2010																												oxypnictide	I4/nmm																	K		51.1					51.1																													T/K	resistivity	11.3			HC152177																																					mOhm.cm							0.286													RH152177			SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152178	PRB081184504	Hall coeff. RH(150K) = -3.87 E-9 m3/C.	Sm(O,F)(Fe,Ru)As	Sm1Fe0.95Ru0.05As1F0.15O0.85	Sm	1	Fe	0.95	Ru	0.05	As	1	F	0.15											O	0.85			2010																												oxypnictide	I4/nmm		A	3.9351		8.47												K		42.7					42.7																													T/K	resistivity	7.89			HC152177																																					mOhm.cm							0.921													RH152177			SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152179	PRB081184504	Hall coeff. RH(150K) = -3.29 E-9 m3/C.	Sm(O,F)(Fe,Ru)As	Sm1Fe0.9Ru0.1As1F0.15O0.85	Sm	1	Fe	0.9	Ru	0.1	As	1	F	0.15											O	0.85			2010																												oxypnictide	I4/nmm		A	3.9401		8.4702												K		21.7					21.7	TC152179																												T/K	resistivity	4.69			HC152177																																					mOhm.cm							1.33																SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152180	PRB081184504	Hall coeff. RH(150K) = -2.03 E-9 m3/C.	Sm(O,F)(Fe,Ru)As	Sm1Fe0.8Ru0.2As1F0.15O0.85	Sm	1	Fe	0.8	Ru	0.2	As	1	F	0.15											O	0.85			2010																												oxypnictide	I4/nmm		A	3.9507		8.4457												K		18.5					18.5																													T/K	resistivity	4.8																																								mOhm.cm							1.58													RH152177			SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152181	PRB081184504		Sm(O,F)(Fe,Ru)As	Sm1Fe0.7Ru0.3As1F0.15O0.85	Sm	1	Fe	0.7	Ru	0.3	As	1	F	0.15											O	0.85			2010																												oxypnictide	I4/nmm		A	3.9597		8.4211												K		13.9					13.9																													T/K	resistivity	4.29			HC152177																																					mOhm.cm							1.7																SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152182	PRB081184504	Hall coeff. RH(150K) = -1.403 E-9 m3/C.	Sm(O,F)(Fe,Ru)As	Sm1Fe0.64Ru0.36As1F0.15O0.85	Sm	1	Fe	0.64	Ru	0.36	As	1	F	0.15											O	0.85			2010																												oxypnictide	I4/nmm		A	3.9691		8.3905												K		15.9					15.9																													T/K	resistivity	5.2			HC152177																																					mOhm.cm							1.58													RH152177			SmAs,Fe2O3,RuO2,FeF2,Fe,Ru		mixture - pellet - sealed in pyrex flask - heat(450C,15-20h) - reground - pellet - sealed in quartz tube - heat(1000-1075C,50h)					Isoelectronic Ru substitution at the iron site in SmFe1-xRuxAsO0.85F0.15 and its effects on structural, superconducting, and normal-state properties			CNR-SPIN, Corso Perrone 24, 16152 Genova, Italy	Phys.Rev.B, 81(2010)184504	M. Tropeano,M. R. Cimberle,C. Ferdeghini,G. Lamura,A. Martinelli,A. Palenzona,I. Pallecchi,A. Sala,I. Sheikin,F. Bernardini,M. Monni,S. Massidda,M. Putti		
152183	PHC4690064	SP-heat measured semi-adiabatic heat pulse method	MgB2	Mg1B2	Mg	1	B	2																				1	2009																										AB2		AlB2			A	3.084		3.513												K		39					39																				T	resistivity, extrapolation	26.3																																mJ/mol.K	100																																									solid state reaction.  pellet - wrapped in Ta foil - ANN(900C,15min) - FC to RT					Low temperature specific heat (zero field and with field) of Fe and Mn-doped MgB2			Department of Physics, Manipal Institute of Technology, Manipal 576104, India	Physica C, 469(2009)64	Ashok Rao,Bhasker Gahtori,S.K. Agarwal,Tirthankar Chakraborty,Chandan Kumar Sarkar,Anirban Das		
152184	PHC4690064	SP-heat measured semi-adiabatic heat pulse method	(Mg,Mn)B2	Mg1.995Mn0.005B2	Mg	1.995	Mn	0.005	B	2																		1	2009																										AB2		AlB2			A	3.08		3.535												K		37.7					37.7																				T	resistivity, extrapolation	24.9																																mJ/mol.K	96.2																																									solid state reaction.  pellet - wrapped in Ta foil - ANN(900C,15min) - FC to RT					Low temperature specific heat (zero field and with field) of Fe and Mn-doped MgB2			Department of Physics, Manipal Institute of Technology, Manipal 576104, India	Physica C, 469(2009)64	Ashok Rao,Bhasker Gahtori,S.K. Agarwal,Tirthankar Chakraborty,Chandan Kumar Sarkar,Anirban Das		
152185	PHC4690064	SP-heat measured semi-adiabatic heat pulse method	(Mg,Mn)B2	Mg1.99Mn0.01B2	Mg	1.99	Mn	0.01	B	2																		1	2009																										AB2		AlB2			A	3.081		3.525												K		37.6					37.6																				T	resistivity, extrapolation	23.7																																mJ/mol.K	86.9																																									solid state reaction.  pellet - wrapped in Ta foil - ANN(900C,15min) - FC to RT					Low temperature specific heat (zero field and with field) of Fe and Mn-doped MgB2			Department of Physics, Manipal Institute of Technology, Manipal 576104, India	Physica C, 469(2009)64	Ashok Rao,Bhasker Gahtori,S.K. Agarwal,Tirthankar Chakraborty,Chandan Kumar Sarkar,Anirban Das		
152186	PHC4690064	SP-heat measured semi-adiabatic heat pulse method	(Mg,Mn)B2	Mg1.985Mn0.015B2	Mg	1.985	Mn	0.015	B	2																		1	2009																										AB2		AlB2			A	3.079		3.526												K		37.4					37.4																				T	resistivity, extrapolation	23.6																																mJ/mol.K	80																																									solid state reaction.  pellet - wrapped in Ta foil - ANN(900C,15min) - FC to RT					Low temperature specific heat (zero field and with field) of Fe and Mn-doped MgB2			Department of Physics, Manipal Institute of Technology, Manipal 576104, India	Physica C, 469(2009)64	Ashok Rao,Bhasker Gahtori,S.K. Agarwal,Tirthankar Chakraborty,Chandan Kumar Sarkar,Anirban Das		
152187	PHC4690064	SP-heat measured semi-adiabatic heat pulse method	(Mg,Mn)B2	Mg1.98Mn0.02B2	Mg	1.98	Mn	0.02	B	2																		1	2009																										AB2		AlB2			A	3.081		3.527												K		36.9					36.9																				T	resistivity, extrapolation	23.1																																mJ/mol.K	78																																									solid state reaction.  pellet - wrapped in Ta foil - ANN(900C,15min) - FC to RT					Low temperature specific heat (zero field and with field) of Fe and Mn-doped MgB2			Department of Physics, Manipal Institute of Technology, Manipal 576104, India	Physica C, 469(2009)64	Ashok Rao,Bhasker Gahtori,S.K. Agarwal,Tirthankar Chakraborty,Chandan Kumar Sarkar,Anirban Das		
152188	PRB081184522	Hc2(0),[cohere] are estimated by fitting using Maki parameters(alpha and ramda(s-o). WHH values ( Hc2//ab=75, Hc2//c=49 T) are different from experimental ones.	Fe(Te,S)	Fe1.14Te0.91S0.09	Fe	1.14	Te	0.91	S	0.09																		3	2010																										AB		PbO																		K			8.5				8.5																				T	resistivity, R=0.9Rn		27.83	28.28					T/K	resistivity		12.82	8.44	MHC152188		A	Hc2(0)		34.1	34.2																																																								self-flux method					Effects of excess Fe on upper critical field and magnetotransport in Fe1+y(Te1-xSx)z			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 81(2010)184522	Hechang Lei,Rongwei Hu,E. S. Choi,J. B. Warren,C. Petrovic		
152189	PRB081205119	striking correlation between Tc and anion hight( distance of anion from the nearest iron layer).	FeSe	Fe1Se0.99	Fe	1	Se	0.99																				1	2010																										AB		PbO																		K	6.99						6.99	MTC152189																																																																																															solid state reaction					Pressure-induced high-Tc superconducting phase in FeSe: Correlation between anion height and Tc			Department of Physics and Mathematics, Aoyama Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 81(2010)205119	H. Okabe,N. Takeshita,K. Horigane,T. Muranaka,J. Akimitsu		
152190	PRB081214510	as-grown sample. filamentary SC. R not zero at 2K.	Fe(Te,S)	Fe1Te0.8S0.2	Fe	1	Te	0.8	S	0.2																			2010																										AB		PbO			A	3.8158		6.2445												K	0		9				4.5																																																																																																mixture(Fe,Te,TeS) - sealed in quartz tube - heat(600C,15h)					Moisture-induced superconductivity in FeTe0.8S0.2			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Phys.Rev.B, 81(2010)214510	Y. Mizuguchi,K. Deguchi,S. Tsuda,T. Yamaguchi,Y. Takano		
152191	PRB081214510	110-days-air exposure sample. Moisture-induced SC. For 140-days sample, Tc(zero) = 7.2 K, SC volume = 49 %.	Fe(Te,S)	Fe1Te0.8S0.2	Fe	1	Te	0.8	S	0.2																			2010																										AB		PbO			A	3.8114		6.2421												K	6.93		10				8.465	MTC152191									42.8																																																																																						mixture(Fe,Te,TeS) - sealed in quartz tube - heat(600C,15h)					Moisture-induced superconductivity in FeTe0.8S0.2			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Phys.Rev.B, 81(2010)214510	Y. Mizuguchi,K. Deguchi,S. Tsuda,T. Yamaguchi,Y. Takano		
152192	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																1	2010					myu-B/R	10.32		10.1																		ABC2D2		LuNi2B2C	I4/mmm																	K			6.38				6.38																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152193	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.9Tm0.1Ni2B2C1	Dy	0.9	Tm	0.1	Ni	2	B	2	C	1														1	2010					myu-B/R	10.33		7.59																		ABC2D2		LuNi2B2C	I4/mmm																	K			4.55				4.55																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152194	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.85Tm0.15Ni2B2C1	Dy	0.85	Tm	0.15	Ni	2	B	2	C	1														1	2010					myu-B/R	10.08		7.41																		ABC2D2		LuNi2B2C	I4/mmm																	K			2.3				2.3																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152195	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.8Tm0.2Ni2B2C1	Dy	0.8	Tm	0.2	Ni	2	B	2	C	1														1	2010					myu-B/R	9.96		7.03																		ABC2D2		LuNi2B2C	I4/mmm																	K			3.42				3.42	MTC152195																																																																																															arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152196	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.6Tm0.4Ni2B2C1	Dy	0.6	Tm	0.4	Ni	2	B	2	C	1														1	2010					myu-B/R	9.29		5.77																		ABC2D2		LuNi2B2C	I4/mmm																	K			5.77				5.77																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152197	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.4Tm0.6Ni2B2C1	Dy	0.4	Tm	0.6	Ni	2	B	2	C	1														1	2010					myu-B/R	8.52		4.31																		ABC2D2		LuNi2B2C	I4/mmm																	K			9				9																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152198	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	(Dy,Tm)Ni2B2C	Dy0.2Tm0.8Ni2B2C1	Dy	0.2	Tm	0.8	Ni	2	B	2	C	1														1	2010					myu-B/R	8.13		2.67																		ABC2D2		LuNi2B2C	I4/mmm																	K			9.75				9.75																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152199	PRB081214517	magnetization and SP-heat also measured. Neel-T from SP-heat	TmNi2B2C	Tm1Ni2B2C1	Tm	1	Ni	2	B	2	C	1																1	2010					myu-B/R	7.35		2.3																		ABC2D2		LuNi2B2C	I4/mmm																	K			10.92				10.92																																																																																																arc-melting - ANN(1323K,7h, in vac)					Effects of Tm substitution on superconductivity and magnetism in the antiferromagnetic borocarbide superconductor Dy1-xTmxNi2B2C			Institute of Materials Physics, Hangzhou Dianzi University, Hangzhou 310018, China	Phys.Rev.B, 81(2010)214517	Lingwei Li,Katsuhiko Nishimura,Masakazu Fujii,Kenji Matsuda,Dexuan Huo		
152200	PRB081220505	Cu-content from XRD. [gap], [penet] calculated from muon-SR data.	CuxTiSe2	Cu0.044Ti1Se2	Cu	0.044	Ti	1	Se	2																			2010																																														K		1.5					1.5																																									A	muon-SR	9180			meV	0.095																			mV/K	-62.9																													See Nat.Phys., 2(2006)544					Possible evidence of a two-gap structure for the CuxTiSe2 superconductor			Physics Department, Technion?Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B, 81(2010)220505	Moran Zaberchik,Khanan Chashka,Larisa Patlgan,Ariel Maniv,Chris Baines,Philip King,Amit Kanigel		
152201	PRB081220505	Cu-content from XRD. [gap], [penet] calculated from muon-SR data.	CuxTiSe2	Cu0.057Ti1Se2	Cu	0.057	Ti	1	Se	2																			2010																																														K		3.49					3.49																																									A	muon-SR	5460			meV	0.48																			mV/K	-55.3																													See Nat.Phys., 2(2006)544					Possible evidence of a two-gap structure for the CuxTiSe2 superconductor			Physics Department, Technion?Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B, 81(2010)220505	Moran Zaberchik,Khanan Chashka,Larisa Patlgan,Ariel Maniv,Chris Baines,Philip King,Amit Kanigel		
152202	PRB081220505	Cu-content from XRD. [gap], [penet] calculated from muon-SR data.	CuxTiSe2	Cu0.064Ti1Se2	Cu	0.064	Ti	1	Se	2																			2010																																														K		3.62					3.62																																									A	muon-SR	4800																							mV/K	-56.3																													See Nat.Phys., 2(2006)544					Possible evidence of a two-gap structure for the CuxTiSe2 superconductor			Physics Department, Technion?Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B, 81(2010)220505	Moran Zaberchik,Khanan Chashka,Larisa Patlgan,Ariel Maniv,Chris Baines,Philip King,Amit Kanigel		
152203	PRB081220505	Cu-content from XRD. [gap], [penet] calculated from muon-SR data.	CuxTiSe2	Cu0.081Ti1Se2	Cu	0.081	Ti	1	Se	2																			2010																																														K		4.17					4.17																				T		0.85			0.64			1.7								A		180			A	muon-SR	3900			meV	0.6																			mV/K	-42.8																													See Nat.Phys., 2(2006)544					Possible evidence of a two-gap structure for the CuxTiSe2 superconductor			Physics Department, Technion?Israel Institute of Technology, Haifa 32000, Israel	Phys.Rev.B, 81(2010)220505	Moran Zaberchik,Khanan Chashka,Larisa Patlgan,Ariel Maniv,Chris Baines,Philip King,Amit Kanigel		
152204	PRL104187001	SC properties obtained from small angle neutron scattering and ARPES	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2010																										ABC		PbFCl																		K				17			17																																				A	ARPES		70		A	ARPES		2100		meV	3	4.1	12																																															self-flux method					Weak Superconducting Pairing and a Single Isotropic Energy Gap in Stoichiometric LiFeAs			Max Planck Institute for Solid State Research, Heisenbergstrase 1, D-70569 Stuttgart, Germany	Phys.Rev.Lett., 104(2010)187001	D. S. Inosov,J. S. White,D.V. Evtushinsky,I.V. Morozov,A. Cameron,U. Stockert,V. B. Zabolotnyy,T. K. Kim,A. A. Kordyuk,S.V. Borisenko,E. M. Forgan,R. Klingeler,J. T. Park,S. Wurmehl,A. N. Vasiliev,G. Behr,C. D. Dewhurst,V. Hinkov		
152205	PRL105027003	SP-heat measured by thermal relaxation method(2 - 200K). Two gaps (2D/kTc = 6.6(H) and 2.2 (L).). lattice term coeff. in SP (beta) = 0.496 mJ/mol.K4. Thermodynamic Hc(0) = 0.85 T.	(Ba,K)Fe2As2	Ba0.68K0.32Fe2As2	Ba	0.68	K	0.32	Fe	2	As	2																3	2010																										AB2C2		ThCr2Si2																		K				38.5			38.5																													T/K	SP-heat		6.7														meV	11	6.6	14							mJ/mol.K2	1.2																																												Specific Heat Measurements of Ba0:68K0:32Fe2As2 Single Crystals: Evidence for a Multiband Strong-Coupling Superconducting State			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	Phys.Rev.Lett., 105(2010)027003	P. Popovich,A.V. Boris,O.V. Dolgov,A. A. Golubov,D. L. Sun,C. T. Lin,R. K. Kremer,B. Keimer		
152206	PRB0302986	G-L parameter = 20 at T=0.35 K.	UPt3	Pt3U1	Pt	3	U	1																				1	1984																										AB3		Mg3Cd	P6<3>/mmc																	K		0.49					0.49										80	mT	dc-SUS				2.2			0.353	T	ac-SUS				0.6			0.35	T/K		4.4																																																																	arc-melting.  ANN(900C,48h)					Bulk superconductivity in the heavy-fermion superconductor UPt3				Phys.Rev.B, 30(1984)2986	T.T.M.Palstra,P.H.Kes,J.A.Mydosh,A.de Visser,J.J.M.Franse,A.Menovsky		
152207	PRL0693120	[cohere] calculated from vortex lattice structure by small-angle neutron scattering.	UPt3	Pt3U1	Pt	3	U	1																				3	1992																										AB3		Mg3Cd	P6<3>/mmc																	K		0.507					0.507																																				A		111			A	London	6000																																																					crystals grown by Czochralski and float zone purified.  ANN(1300C,150h) - slow cool to RT					Neutron diffraction from the vortex lattice in the heavy-fermion superconductor UPt3				Phys.Rev.Lett., 69(1992)3120	R.N.Kleiman,C.Broholm,G.Aeppli,E.Bucher,N.Stucheli,D.J.Bishop,K.N.Clausen,K.Mortensen,J.S.Pedersen,B.Howard		
152208	PRB0311654	pressure effect upto 19.1 kbar. twined sample. d(lnTc)/dP = 0.26 /GPa.	UPt3	Pt3U1	Pt	3	U	1																				3	1985																										AB3		Mg3Cd	P6<3>/mmc																	K		0.48					0.48			K/GPa	0.126																									T/K	resistivity	7.2																																																																	crystals grown by Bi-flux method. ANN(1200C,4h + 1100C,20h)					Effect of pressure on spin fluctuations and superconductivity in heavy-fermion UPt3				Phys.Rev.B, 31(1985)1654	J.O.Willis,J.D.Thompson,Z.Fisk,A.de Visser,J.J.M.Franse,AmMenovsky		
152209	PRL0741218	RRR = 190. SC properties extracted from SP-heat analysis. G-L parameter = 58.	UPt3	Pt3U1	Pt	3	U	1																				3	1995																										AB3		Mg3Cd	P6<3>/mmc																	K		0.55					0.55																																				A		120			A		7000																																																					crystals grown by Czochralski method					Magnetic Field Dependent Speciffic Heat Across the Middle and Upper Critical Field Lines In UPt3	199502		AT&T Bell Laboratories,600 Mountain Avenue,Murray Hill,New Jersey 07974	Phys.Rev.Lett.,74(1995)1218	A.P.Ramirez,E.Bucher,N.Stucheli	U,Pt	
152210	PRL0570234	For P = 0.38(0.89) GPa, Tc = 0.44(0.36) K, [gamma] = 384(334) mJ/mol.K2.	UPt3	Pt3U1	Pt	3	U	1																					1986																										AB3		Mg3Cd																		K		0.5					0.5																																																								mJ/mol.K2	426	SP-heat	141	SP-heat																																									Pressure dependence of spin-fluctuation effects in the specific heat of heavy-fermion superconductor UPt3				Phys.Rev.Lett., 57(1986)234	G.E.Brodale,R.A.Fisher,Norman E.Phillips,G.R.Stewart,A.L.Giorgi		
152211	PRL0571259	J//c. RRR = 155.	UPt3	Pt3U1	Pt	3	U	1																					1986																										AB3		Mg3Cd																		K		0.53					0.53																				T				2.81					T/K			7.76	4.51																																						uOhm.cm											125														See Phys.Rev.Lett., 56(1986)1078					Unusual angular and temperature dependence of the upper critical field in UPt3				Phys.Rev.Lett., 57(1986)1256	B.S.Shivaram,T.F.Rosenbaum,D.G.Hinks		
152212	PRL0571259	J//b-axis. RRR = 110.	UPt3	Pt3U1	Pt	3	U	1																					1986																										AB3		Mg3Cd																		K		0.53					0.53																				T			2.11	2.59					T/K			7.72	4.59																																						uOhm.cm											230														See Phys.Rev.Lett., 56(1986)1078					Unusual angular and temperature dependence of the upper critical field in UPt3				Phys.Rev.Lett., 57(1986)1256	B.S.Shivaram,T.F.Rosenbaum,D.G.Hinks		
152213	PRL0631723	Tc measured by LC method. Hc1(T) and Hc2(T) shown in Fig.	UPt3	Pt3U1	Pt	3	U	1																				3	1989																										AB3		Mg3Cd	P6<3>/mmc																	K		0.55					0.55																													T/K			4.6	8.15	MHC152213																																																																			Lower and upper critical fields in the heavy-electron superconductor UPt3				Phys.Rev.Lett., 63(1989)1723	B.S.Shivaram,J.J.Gannon,Jr.,David G.Hinks		
152214	SSC0630599	ultrasound attenuation measurement.	UPt3	Pt3U1	Pt	3	U	1																					1987																										AB3		Mg3Cd																		K		0.51				0.03	0.51																				T	attenuation	2																																																																															LONGITUDINAL SOUND MEASUREMENTS ON UPt3 IN A MAGNETIC F ELD				Solid State Commun.,63(1987)559	Y.J.Qian,M-F.Xu,A.Schenstrom,H-P.Baum,J.B.Ketterson,D.Hinks,M.Levy,Bimal K.Sarma		
152215	SSC0850355	nearly isotropic. Hc1(T) = Hc1(0)(1-t^2)^n  n=1.3.  Jc(0) = 3.8E+3 A/cm2	UPt3	Pt3U1	Pt	3	U	1																				3	1993																										AB3		Mg3Cd																		K		0.5					0.5											mT	M-H curve		6.5	6.5																																																																																						MAGNETIC PROPERTIES OF THE HEAVY-FERMION SUPERCONDUCTORS UPT3AND URU2SI2	199301	MAGNETIZATION       ,CRITICAL FIELD      ,CRITICAL CURRENTS   ,HEAVY-FERMION	CRTBT-C.N.R.S.,	SOLID STATE COMMUN.,85(1993)355	J.FLOUQUET,J.L.THOLENCE,N.KELLER,S.WUCHNER	V,PT,RU,SI	
152216	SSC0850355	nearly isotropic. Hc1(T) = Hc1(0)(1-t^2)^n  n=1.7. Jc(0) = 2.4E+4 A/cm2	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	1993																										AB2C2																				K		1.2					1.2											mT	M-H curve		3.3	3.3																																																																																						MAGNETIC PROPERTIES OF THE HEAVY-FERMION SUPERCONDUCTORS UPT3AND URU2SI2	199301	MAGNETIZATION       ,CRITICAL FIELD      ,CRITICAL CURRENTS   ,HEAVY-FERMION	CRTBT-C.N.R.S.,	SOLID STATE COMMUN.,85(1993)355	J.FLOUQUET,J.L.THOLENCE,N.KELLER,S.WUCHNER	V,PT,RU,SI	
152217	PHB1941981	RRR = 6.2. [resrt]  shows R(280K). R measured along the layer. Structure, beta = 134deg 35'. Hc1 < 0.5 Oe (estimated).	NbTe2	Nb1Te2	Nb	1	Te	2																				3	1994																										AB2		NbTe2	C2/m		A	19.39	3.642	9.375												K		0.5	0.58	0.5			0.5																																																																							uOhm.cm							29				180														crystals grown by chemical vapor transport method					Superconductivity in layered-structure compound NbTe2				Physica B., 194-196(1994)1981	Shoichi Nagata,Tsuyoshi Abe,Shinichi Terashima,Yutaka Ishihara,Kitomi Tsutsumi		
152218	SSC0680085		Ti	Ti1	Ti	1																							1988																										A																				K		0.4					0.4																																																								mJ/gat.K2	3.34	SP-heat	529	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152219	SSC0680085		Ti2Rh	Rh1Ti2	Rh	1	Ti	2																					1988																										AB2																				K					1.4																																																										mJ/gat.K2	1.58	SP-heat	478	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152220	SSC0680085		TiRh	Rh1Ti1	Rh	1	Ti	1																					1988																										AB																				K					1.4																																																										mJ/gat.K2	2.46	SP-heat	383	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152221	SSC0680085	ANN(1600C,3h)	TiRh3	Rh3Ti1	Rh	3	Ti	1																					1988																										AB3																				K					1.4																																																										mJ/gat.K2	2.85	SP-heat	526	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152222	SSC0680085		Zr	Zr1	Zr	1																							1988																										A																				K		0.55					0.55																																																								mJ/gat.K2	2.8	SP-heat	291	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152223	SSC0680085	ANN(1000C,3h).  Data from SSC0540517	Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1988																										AB2																				K		11.2					11.2																																																								mJ/gat.K2	25.6	SP-heat	212	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152224	SSC0680085	ANN(1500C,3h).  Data from SSC0540517	ZrRh	Rh1Zr1	Rh	1	Zr	1																					1988																										AB																				K					1.4																																																										mJ/gat.K2	1.2	SP-heat	300	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152225	SSC0680085	ANN(1550C,3h).  Data from SSC0540517	ZrRh3	Rh3Zr	Rh	3	Zr																						1988																										AB3																				K					1.4																																																										mJ/gat.K2	2.75	SP-heat	436	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152226	SSC0680085		Hf	Hf1	Hf	1																							1988																										A																				K		0.128					0.128																																																								mJ/gat.K2	2.15	SP-heat	252	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152227	SSC0680085	as-cast	Hf2Rh	Hf2Rh1	Hf	2	Rh	1																					1988																										AB2																				K		1.54					1.54																																																								mJ/gat.K2	2.72	SP-heat	176	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152228	SSC0680085	ANN(1300C,2h)	Hf2Rh	Hf2Rh1	Hf	2	Rh	1																					1988																										AB2																				K		1.6					1.6																																																								mJ/gat.K2	2.79	SP-heat	178	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152229	SSC0680085	ANN(1600C,3h)	HfRh	Hf1Rh1	Hf	1	Rh	1																					1988																										AB																				K					1.4																																																										mJ/gat.K2	1.52	SP-heat	270	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152230	SSC0680085	ANN(1700C,3h)	HfRh3	Hf1Rh3	Hf	1	Rh	3																					1988																										AB3																				K					1.4																																																										mJ/gat.K2	2.54	SP-heat	400	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152231	SSC0680085		Rh	Rh1	Rh	1																							1988																										A																				K		0.000325					0.000325																																																								mJ/gat.K2	4.7	SP-heat	500	SP-heat																																									ELECTRONIC PROPERTIES,SUPERCONDUCTIVITY AND STABILITY OF THE ORDERED ALLOYS OF THE TI-RH,ZR-RH AND HF-RH ISOELECTRONIC SYSTEMS				SOLID STATE COMMUN.,68(1988)85	R.KUENTZLER,R.M.WATERSTRAT	TI,RH,ZR,HF	
152232	PRB0530384	lattice term in SP (beta) = 0.328 mJ/mol.K4. (dC/gamma*Tc) = 1.11. e-ph coupling = 0.51. thermodynamic Hc(0) = 353 Oe.	Nb3S4	Nb3S4	Nb	3	S	4																					1996																										A3B4		Nb3Te4																		K		3.78				0.14	3.78																																																3.1	14				MSP152232			mJ/mol.K2	13.6	SP-heat	346	SP-heat																																				iodine vapor transport method					Specific heat of an anisotropic superconductor: Nb3X4 with X=S, Se, and Te			Department of Physics, Faculty of Science, Kanazawa University, Kanazawa 920-11, Japan	Phys.Rev.B, 53(1996)384	Hiroyuki Okamoto,Hiromi Taniguti,Yutaka Ishihara		
152233	PRB0530384	lattice term in SP (beta) = 1.27 mJ/mol.K4. (dC/gamma*Tc) = 0.66. e-ph coupling = 0.51. thermodynamic Hc(0) = 244 Oe.	Nb3Se4	Nb3Se4	Nb	3	Se	4																					1996																										A3B4		Nb3Te4																		K		2.31					2.31																																																2.8	14				MSP152233			mJ/mol.K2	21.4	SP-heat	220	SP-heat																																				iodine vapor transport method					Specific heat of an anisotropic superconductor: Nb3X4 with X=S, Se, and Te			Department of Physics, Faculty of Science, Kanazawa University, Kanazawa 920-11, Japan	Phys.Rev.B, 53(1996)384	Hiroyuki Okamoto,Hiromi Taniguti,Yutaka Ishihara		
152234	PRB0530384	lattice term in SP (beta) = 11.4 mJ/mol.K4.	Nb3Te4	Nb3Te4	Nb	3	Te	4																					1996																										A3B4		Nb3Te4																		K		1.95					1.95																																																								mJ/mol.K2	18.7	SP-heat	106	SP-heat																																				iodine vapor transport method					Specific heat of an anisotropic superconductor: Nb3X4 with X=S, Se, and Te			Department of Physics, Faculty of Science, Kanazawa University, Kanazawa 920-11, Japan	Phys.Rev.B, 53(1996)384	Hiroyuki Okamoto,Hiromi Taniguti,Yutaka Ishihara		
152235	SSC0450129	RRR = 3. T<CDW> = 80 K from R(T). anisotropy(Hc2) = 4.8	Nb3Te4	Nb3Te4	Nb	3	Te	4																					1983																										A3B4		Nb3Te4			A	10.671		3.6468												K		1.95				0.2	1.95																																		MHC152235		A			464	97																																																								iodine vapor transport method. T-gradient (3C/cm) at 1000C					ELECTRICAL TRANSPORT PROPERTIES OF A QUASI-ONE-DIMENSIONAL Nb3Te4 SINGLE CRYSTAL			Faculty of Science, Kanazawa University, Kanazawa, Japan	Solid State Commun., 45(1983)129	Y. Ishihara,I. Nakada		
152236	PRB05312299		Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1996																										AB2						6.53		5.629												K		11.2					11.2																																																								mJ/mol.K2	68	SP-heat	214	SP-heat																																									Electronic-structure effects in the suppression of superconductivity in hydrogenated Zr2Rh			Solid State Physics Division, Bhabha Atomic Research Centre, Bombay 400085, India	Phys.Rev.B, 53(1996)12299	H. G. Salunke,G. P. Das,P. Raj,K. Shashikala,A. Sathyamoorthy,S. K. Dhar		
152237	PRB05312299		Zr2RhH2	Zr2Rh1H2	Zr	2	Rh	1	H	2																			1996																																6.81		5.598												K					2																																																										mJ/mol.K2	6.5	SP-heat	350	SP-heat																																									Electronic-structure effects in the suppression of superconductivity in hydrogenated Zr2Rh			Solid State Physics Division, Bhabha Atomic Research Centre, Bombay 400085, India	Phys.Rev.B, 53(1996)12299	H. G. Salunke,G. P. Das,P. Raj,K. Shashikala,A. Sathyamoorthy,S. K. Dhar		
152238	PRB05312299		Zr2RhH4	Zr2Rh1H4	Zr	2	Rh	1	H	4																			1996																																6.867		5.624												K					2																																																										mJ/mol.K2	21	SP-heat	371	SP-heat																																									Electronic-structure effects in the suppression of superconductivity in hydrogenated Zr2Rh			Solid State Physics Division, Bhabha Atomic Research Centre, Bombay 400085, India	Phys.Rev.B, 53(1996)12299	H. G. Salunke,G. P. Das,P. Raj,K. Shashikala,A. Sathyamoorthy,S. K. Dhar		
152239	SSC0151797		Zr2Rh	Rh1Zr2	Rh	1	Zr	2																					1974																										AB2		CuAl2																		K		11.3					11.3																																																								mJ/mol.K2	46	SP-heat	188	SP-heat																																									The relation between normal state properties and Tc for some Zr2X compounds				Solid State Commun., 15(1974)1797	Z. Fisk,R. Viswanathan,G.W. Webb		
152240	SSC0151797		Zr2Ir	Ir1Zr2	Ir	1	Zr	2																					1974																										AB2		CuAl2																		K		7.5					7.5																																																								mJ/mol.K2	17	SP-heat	200	SP-heat																																									The relation between normal state properties and Tc for some Zr2X compounds				Solid State Commun., 15(1974)1797	Z. Fisk,R. Viswanathan,G.W. Webb		
152241	SSC0151797		Zr2Co	Co1Zr2	Co	1	Zr	2																					1974																										AB2		CuAl2																		K		5.5					5.5																																																								mJ/mol.K2	28	SP-heat	180	SP-heat																																									The relation between normal state properties and Tc for some Zr2X compounds				Solid State Commun., 15(1974)1797	Z. Fisk,R. Viswanathan,G.W. Webb		
152242	SSC0151797		Zr2Ni	Ni1Zr2	Ni	1	Zr	2																					1974																										AB2		CuAl2																		K		1.6					1.6																																																								mJ/mol.K2	18	SP-heat	221	SP-heat																																									The relation between normal state properties and Tc for some Zr2X compounds				Solid State Commun., 15(1974)1797	Z. Fisk,R. Viswanathan,G.W. Webb		
152243	PRB081224511	P-induced SC. (dTn/dP) = -7.0 K/GPa. Tc(max) = 13 K(P=11.5 GPa). R not to zero at P=16 GPa. Tn is sensitive to uniaxial stress.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2																		K	13				0		13																																																																																																crystals grown by FeAs self-flux method.					Appearance of pressure-induced superconductivity in BaFe2As2 under hydrostatic conditions and its extremely high sensitivity to uniaxial stress				Phys.Rev.B, 81(2010)224511			
152244	PRB081224520	refined stoichiometry: Fe1.045Se0.406Te0.594 by NPD. impurity phase(Fe7Se8). gap(S) = 0.51 meV, [gapene] = 0.84 for small gap from two-gap model fitting.	Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																		3	2010									6.04																	AB		PbO	P4/nmm		A	3.798		6.038												K				14.6			14.6											Oe	magnetization, extrapolation		20	45																			MHIR152244							A	muon-SR		4910	13200	meV	2.61	4.3	16																																															Bridgman method					Anisotropic superconducting properties of single-crystalline FeSe0.5Te0.5				Phys.Rev.B, 81(2010)224520			
152245	PRB081235107		(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		35					35																																																																		uV/K	13.84			MTP152245																										solid state reaction					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152246	PRB081235107		(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		36.9					36.9	MTC152246																																																																	uV/K	16.25			MTP152246																										solid state reaction					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152247	PRB081235107		(Ba,K)Fe2As2	Ba0.4K0.6Fe2As2	Ba	0.4	K	0.6	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		35.2					35.2																																																																		uV/K	20.36			MTP152247																										solid state reaction					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152248	PRB081235107		(Ba,K)Fe2As2	Ba0.2K0.8Fe2As2	Ba	0.2	K	0.8	Fe	2	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		13.9					13.9																																																																		uV/K	16.45			MTP152248																										solid state reaction					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152249	PRB081235107		Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		25.4					25.4																																																																		uV/K	-22.9			MTP152249																										self-flux method					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152250	PRB081235107		Ba(Fe,Co)2As2	Ba1Fe1.75Co0.25As2	Ba	1	Fe	1.75	Co	0.25	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		22					22																																																																		uV/K	-27.4			MTP152250																										self-flux method					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152251	PRB081235107		Ba(Fe,Co)2As2	Ba1Fe1.73Co0.27As2	Ba	1	Fe	1.73	Co	0.27	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																	K		17.1					17.1	MTC152251																																																																	uV/K	-34.3			MTP152251																										self-flux method					Thermoelectric properties of electron- and hole-doped BaFe2As2				Phys.Rev.B, 81(2010)235107			
152252	PRB082014503	Jc(H=0,T=0.5Tc) = 0.698 E+3 A/cm2.	Ca(Fe,Co)2As2	Ca1Fe1.898Co0.102As2	Ca	1	Fe	1.898	Co	0.102	As	2																	2010																										AB2C2		ThCr2Si2																		K		18.5	20.3				18.5																																																																																																					Critical current and vortex dynamics in single crystals of Ca(Fe1-xCox)2As2				Phys.Rev.B, 82(2010)014503			
152253	PRB082014503	Jc(H=0,T=0.5Tc) = 7.56 E+3 A/cm2. Jc(H=0) = 18,16.4,10,2.14,0.14 E+3 A/cm2 for T=1.92,4.96,9.92,14.9,18.0 K, respectively.	Ca(Fe,Co)2As2	Ca1Fe1.888Co0.112As2	Ca	1	Fe	1.888	Co	0.112	As	2																	2010																										AB2C2		ThCr2Si2																		K		19	20.3				19																																																																																																					Critical current and vortex dynamics in single crystals of Ca(Fe1-xCox)2As2				Phys.Rev.B, 82(2010)014503			
152254	PRB082014503	Jc(H=0,T=0.5Tc) = 15.7 E+3 A/cm2.	Ca(Fe,Co)2As2	Ca1Fe1.87Co0.13As2	Ca	1	Fe	1.87	Co	0.13	As	2																	2010																										AB2C2		ThCr2Si2																		K		17.2	18.6				17.2																																																																																																					Critical current and vortex dynamics in single crystals of Ca(Fe1-xCox)2As2				Phys.Rev.B, 82(2010)014503			
152255	PRB082014503	Jc(H=0,T=0.5Tc) = 9.53 E+3 A/cm2.	Ca(Fe,Co)2As2	Ca1Fe1.854Co0.146As2	Ca	1	Fe	1.854	Co	0.146	As	2																	2010																										AB2C2		ThCr2Si2																		K		16.8	17.2				16.8																																																																																																					Critical current and vortex dynamics in single crystals of Ca(Fe1-xCox)2As2				Phys.Rev.B, 82(2010)014503			
152256	PRB082024503	misfit crystal. RRR = 18.8 for in-plane resistivity.	(PbSe)1.16(TiSe2)2	Pb1.16Ti2Se5.16	Pb	1.16	Ti	2	Se	5.16																		3	2010																												TX2			A	3.553		18.247											layered TX2	K		2.3					2.3																																																																		uV/K	-54.2			MTP152256																										misfit crystals grown using vapor transport with iodine as transport agent					Superconductivity at 2.3 K in the misfit compound (PbSe)1.16(TiSe2)2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 82(2010)024503	N. Giang,Q. Xu,Y. S. Hor,A. J. Williams,S. E. Dutton,H. W. Zandbergen,R. J. Cava		
152257	SSC1020401	misfit layer compound.  RRR = 7.3. subsystems(NbSe2, PbSe) are monoclinic.	(PbSe)1.12(NbSe2)2	Pb1.12Nb2Se5.12	Pb	1.12	Nb	2	Se	5.12																			1997																												TX2																	layered TX2	K		2.9				0.12	2.9																				T	resistivity, extrapolation		4.9	1.01										MHC152257		A	from Hc2		168	34																																																													SUPERCONDUCTIVITY IN THE MISFIT LAYER COMPOUND (PbSe)1.12(NbSe2)2				Solid State Commun., 102(1997)401	A. Nader,A. Briggs,A. Meerschaut,A. Lafond		
152258	SSC1010149	misfit layer compound.  RRR = 4. anisotropy = 1.29 at Tc.	(BiSe)1.1(NbSe2)	Bi1.1Nb1Se3.1	Bi	1.1	Nb	1	Se	3.1																			1997																												TX2																	layered TX2	K		2.36				0.12	2.36																				T	resistivity, extrapolation		0.703	0.52					T/K	resistivity		0.305	0.237	MHC152258		A	from Hc2		240	186																																																													SUPERCONDUCTIVITY IN THE MISFIT LAYER COMPOUNDS (BiSe)1.10(NbSe2) and (BiS)1.11(NbS2)				Solid State Commun., 101(1997)149	A. Nader,A. Briggs,Y. Gotoh		
152259	SSC1010149	misfit layer compound.  RRR = 7	(BiS)1.11(NbS2)	Bi1.1Nb1S3.1	Bi	1.1	Nb	1	S	3.1																			1997																												TX2																	layered TX2	K		0.415				0.03	0.415																				T	resistivity, extrapolation		0.0385	0.0155					T/K	resistivity		0.093	0.039	MHC152259		A	from Hc2		1430	600																																																													SUPERCONDUCTIVITY IN THE MISFIT LAYER COMPOUNDS (BiSe)1.10(NbSe2) and (BiS)1.11(NbS2)				Solid State Commun., 101(1997)149	A. Nader,A. Briggs,Y. Gotoh		
152260	SYN0970147	RRR = 3.5.	(LaSe)1.14(NbSe2)	La1.14Nb1Se3.14	La	1.14	Nb	1	Se	3.14																			1998																												TX2			A	6.016	6.07	24.072											layered TX2	K		1.32				0.12	1.32																				T	resistivity, extrapolation			0.475										MHC152260																																																														mixture - heat(600C,a few days) - grind - heat(1000C,10d) - add(iodine) - vapor transport(T-gradient,100C)					Structural characterization and superconductivity in the misfit layer compound (LaSe)1.14(NbSe2)			Atomic Energy Commission of Syria, Physics Department, PO Box 6091, Damascus, Syria	Synth.Met.,97(1998)147	A. Nader,A. Lafond,A. Briggs,A. Meerschaut,R. Roesky		
152261	AAC6190117	misfit layer compound. LaNb2Se5	(LaSe)1.14(NbSe)2	La1.14Nb2Se5.14	La	1.14	Nb	2	Se	5.14																			1993																												TX2																		K		5.3					5.3																																																																																																					"Structure and Electronic Transport Properties of the Misfit Layer Compound (LaSe)1.14(NbSe2)2, ""LaNb2Se5"""				Z.anorg.allg.Chem., 619(1993)117	R.Roesky,A.Meerschaut,J.Rouxel,J.Chen		
152262	PRL104256402	P-induced SC. Pcrit = 3.0 kbar. Tc = 28, 29, 31.3, 32.7, 34.9 K for P=3.9, 4.8, 5.7, 6.6, 7.6 kbar, respectively.	Cs3C60	C60Cs3	C	60	Cs	3																					2010																										A3B60		fullerene																	fcc	K				34.9	2		34.9																																																																																																					NMR Study of the Mott Transitions to Superconductivity in the Two Cs3C60 Phases			Laboratoire de Physique des Solides, Universite Paris-Sud 11, CNRS UMR 8502, 91405 Orsay, France	Phys.Rev.Lett., 104(2010)256402	Y. Ihara,H. Alloul,P. Wzietek,D. Pontiroli,M. Mazzani,M. Ricco		
152263	PRL104256402	P-induced SC. Pcrit = 5.5 kbar.	Cs3C60	C60Cs3	C	60	Cs	3																					2010								47.1																		A3B60		fullerene																	A15	K				35.7	2		35.7	MTC152263																																																																																																				NMR Study of the Mott Transitions to Superconductivity in the Two Cs3C60 Phases			Laboratoire de Physique des Solides, Universite Paris-Sud 11, CNRS UMR 8502, 91405 Orsay, France	Phys.Rev.Lett., 104(2010)256402	Y. Ihara,H. Alloul,P. Wzietek,D. Pontiroli,M. Mazzani,M. Ricco		
152265	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.854Ru0.146As2	Ba	1	Fe	1.854	Ru	0.146	As	2																3	2010								105.6																		AB2C2		ThCr2Si2			A	3.9689		12.952												K					2																																																																																																		single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152266	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.748Ru0.252As2	Ba	1	Fe	1.748	Ru	0.252	As	2																3	2010								88.8																		AB2C2		ThCr2Si2			A	3.9735		12.935												K					2																																																																																																		single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152267	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.678Ru0.322As2	Ba	1	Fe	1.678	Ru	0.322	As	2																3	2010								70.5																		AB2C2		ThCr2Si2			A	3.9813		12.884												K			9.31				9.31																																																																																																single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152268	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.58Ru0.42As2	Ba	1	Fe	1.58	Ru	0.42	As	2																3	2010								41.5																		AB2C2		ThCr2Si2																		K	8.95		19.3				14.125	MTC152268																																																																																															single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152269	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.52Ru0.48As2	Ba	1	Fe	1.52	Ru	0.48	As	2																3	2010								29.7																		AB2C2		ThCr2Si2			A	3.9976		12.833												K	13.6		17.5				15.55																																																																																																single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152270	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.42Ru0.58As2	Ba	1	Fe	1.42	Ru	0.58	As	2																3	2010																										AB2C2		ThCr2Si2			A	4.0054		12.813												K	14.7		16.5				15.6																																																																																																single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152271	PRB082014534	Ru-content determined by WDS.	Ba(Fe,Ru)2As2	Ba1Fe1.28Ru0.72As2	Ba	1	Fe	1.28	Ru	0.72	As	2																3	2010																										AB2C2		ThCr2Si2			A	4.0132		12.773												K	4.3		13.6				8.95																																																																																																single crystals grown by self-flux method					Physical and magnetic properties of Ba(Fe1-xRux)2As2 single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)014534	A. Thaler,N. Ni,A. Kracher,J. Q. Yan,S. L. Bud'ko,P. C. Canfield		
152272	PHC4700689	anisotropy (Hc2) = 7.5	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4-z	Nd	1.85	Ce	0.15	Cu	1															O	4-z		3	2010																												T'																		K			26.2			0.7	26.2																				T	resistivity, WHH approx.		87	11.6					T/K	resistivity		4.8	0.64	HC152272		A	from Hc2		53.3	7.1																																																								TSFZ method					Anisotropic magnetotransport of superconducting and normal state in an electron-doped Nd1.85Ce0.15CuO4-z single crystal			State Key Laboratory for Mesoscopic Physics and School of Physics, Peking University, Beijing 100871, China	Physica C, 470(2010)689	Y. Wang,H. Gao		
152273	PHC4700682	SUS(300K) = 0.339 E-3 emu/mol.Oe.	(Rh,Ir)17S15	Rh16Ir1S15	Rh	16	Ir	1	S	15																			2010																										A15B17					A	9.9144														K		4.08					4.08																																		MHC152273																						mJ/mol.K2	89.1	SP-heat	349	SP-heat											mOhm.cm											0.3223												Rh(3N),Ir(3N),S(5N) powder		solid state reaction.					Suppression of electron correlations in the superconducting alloys of Rh17-xIrxS15			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Mumbai 400 005, India	Physica C, 470(2010)682	H.R. Naren,Arumugam Tamizhavel,A.K. Nigam,S. Ramakrishan		
152274	PHC4700682	SUS(300K) = 0.092 E-3 emu/mol.Oe.	(Rh,Ir)17S15	Rh15Ir2S15	Rh	15	Ir	2	S	15																			2010																										A15B17					A	9.9183														K		3.5					3.5																																		MHC152273																						mJ/mol.K2	80.5	SP-heat	327	SP-heat											mOhm.cm											0.3416												Rh(3N),Ir(3N),S(5N) powder		solid state reaction.					Suppression of electron correlations in the superconducting alloys of Rh17-xIrxS15			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Mumbai 400 005, India	Physica C, 470(2010)682	H.R. Naren,Arumugam Tamizhavel,A.K. Nigam,S. Ramakrishan		
152275	PHC4700682	SUS(300K) = 1.07 E-3 emu/mol.Oe.	Rh17S15	Rh17S15	Rh	17	S	15																					2010																										A15B17					A	9.9093														K		5.4					5.4																																		MHC152273																						mJ/mol.K2	104.8	SP-heat	424	SP-heat											mOhm.cm											0.1951												Rh(3N),Ir(3N),S(5N) powder		solid state reaction.					Suppression of electron correlations in the superconducting alloys of Rh17-xIrxS15			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Mumbai 400 005, India	Physica C, 470(2010)682	H.R. Naren,Arumugam Tamizhavel,A.K. Nigam,S. Ramakrishan		
152276	PRB082085318	epitaxial-(111) film. d =< 1000A.. critical B-content = 3 E+20 /cm3. B-content by SIMS. Tc not saturate at 1.0 E+22 /cm3.	B-doped C film	C1	C	1																							2010																												diamond																		K		8.3					8.3	MTC152276																																																																																															epitaxial films grown by microwave plasma-assisted CVD					Superconductor-to-insulator transition in boron-doped diamond films grown using chemical vapor deposition			School of Science and Engineering, Waseda University, 3-4-1 Okubo, Shinjuku, Tokyo 169-8555, Japan	Phys.Rev.B, 82(2010)085318	Akihiro Kawano,Hitoshi Ishiwata,Shingo Iriyama,Ryosuke Okada,Takahide Yamaguchi,Yoshihiko Takano,Hiroshi Kawarada		
152277	PRB082085318	epitaxial-(001) film. d =< 1000A.. critical B-content = 3 E+20 /cm3. B-content by SIMS. Tc  saturate for n >  1.0 E+21 /cm3.	B-doped C film	C1	C	1																							2010																												diamond																		K		4					4	MTC152276																																																																																															epitaxial films grown by microwave plasma-assisted CVD					Superconductor-to-insulator transition in boron-doped diamond films grown using chemical vapor deposition			School of Science and Engineering, Waseda University, 3-4-1 Okubo, Shinjuku, Tokyo 169-8555, Japan	Phys.Rev.B, 82(2010)085318	Akihiro Kawano,Hitoshi Ishiwata,Shingo Iriyama,Ryosuke Okada,Takahide Yamaguchi,Yoshihiko Takano,Hiroshi Kawarada		
152278	PRB082085318	epitaxial-(110) film. d =< 1000A.. critical B-content = 0.9 E+20 /cm3. B-content by SIMS. Tc  saturate for n >  2.0 E+21 /cm3.	B-doped C film	C1	C	1																							2010																												diamond																		K		3.5					3.5	MTC152276																																																																																															epitaxial films grown by microwave plasma-assisted CVD					Superconductor-to-insulator transition in boron-doped diamond films grown using chemical vapor deposition			School of Science and Engineering, Waseda University, 3-4-1 Okubo, Shinjuku, Tokyo 169-8555, Japan	Phys.Rev.B, 82(2010)085318	Akihiro Kawano,Hitoshi Ishiwata,Shingo Iriyama,Ryosuke Okada,Takahide Yamaguchi,Yoshihiko Takano,Hiroshi Kawarada		
152279	PRB082064511	G-L parameter = 76. (dC/gamma*Tc) = 2.28. thermodynamic Hc(0) = 0.146 T	Mo3Al2C	Al2C1Mo3	Al	2	C	1	Mo	3																			2010																										AB2C3		beta-Mn	P4<1>32		A	6.863													beta-Mn	K		9					9	MTC152279																			T	WHH approx.	15.7							T/K		3					A	from Hc2	46			A	London	3800													mJ/mol.K2	17.8	SP-heat	315	SP-heat																																				powder mixture - cold compact - heat(1500C,24h,in vac) - hot press(1250C,56 MPa)					Unconventional superconducting phase in the weakly correlated noncentrosymmetric Mo3Al2C compound			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 82(2010)064511	E. Bauer,G. Rogl,Xing-Qiu Chen,R. T. Khan,H. Michor,G. Hilscher,E. Royanian,K. Kumagai,D. Z. Li,Y. Y. Li,R. Podloucky,P. Rogl		
152280	PRB082064512	RRR = 1.09. G-L parameter = 88.56. (dC/gamma*Tc) = 2.14(dC/Tc = 40). Hc2(0) = 18.2 T from empirical eq. fitting .	Mo3Al2C	Al2C1Mo3	Al	2	C	1	Mo	3																			2010																										AB2C3		beta-Mn	P4<1>32		A	6.866													beta-Mn	K		9.1	9.2			0.2	9.1											Oe	M-H curve	47							T	WHH approx.	15.08							T/K	resistivity	2.39			MHC152280		A	from Hc2	46.84			A	from Hc1	3755					4.028	14				MSP152280			mJ/mol.K2	18.65	SP-heat	338.5	SP-heat											mOhm.cm											0.19														arc-melting					Structure and physical properties of the noncentrosymmetric superconductor Mo3Al2C			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 82(2010)064512	A. B. Karki,Y. M. Xiong,I. Vekhter,D. Browne,P. W. Adams,D. P. Young,K. R. Thomas,Julia Y. Chan,H. Kim,R. Prozorov		
152281	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2010																										AB2C2		ThCr2Si2																		K		7.4					7.4																																									A	TDR method		6730																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152282	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2010																										AB2C2		ThCr2Si2																		K		11.6					11.6																																									A	TDR method		9210																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152283	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.916Co0.084As2	Ba	1	Fe	1.916	Co	0.084	As	2																3	2010																										AB2C2		ThCr2Si2																		K		15.5					15.5																																									A	TDR method		9350																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152284	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																3	2010																										AB2C2		ThCr2Si2																		K		18.5					18.5																																									A	TDR method		2580																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152285	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																3	2010																										AB2C2		ThCr2Si2																		K		18.3					18.3																																									A	TDR method		2850																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152286	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.892Co0.108As2	Ba	1	Fe	1.892	Co	0.108	As	2																3	2010																										AB2C2		ThCr2Si2																		K		20.5					20.5																																									A	TDR method		3050																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152287	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.884Co0.116As2	Ba	1	Fe	1.884	Co	0.116	As	2																3	2010																										AB2C2		ThCr2Si2																		K		23.3					23.3																																									A	TDR method		1950																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152288	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.874Co0.126As2	Ba	1	Fe	1.874	Co	0.126	As	2																3	2010																										AB2C2		ThCr2Si2																		K		23.4					23.4																																									A	TDR method		1500																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152289	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.874Co0.126As2	Ba	1	Fe	1.874	Co	0.126	As	2																3	2010																										AB2C2		ThCr2Si2																		K		23.5					23.5																																									A	TDR method		2170																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152290	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2010																										AB2C2		ThCr2Si2																		K		22.8					22.8																																									A	TDR method		2700																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152291	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.824Co0.176As2	Ba	1	Fe	1.824	Co	0.176	As	2																3	2010																										AB2C2		ThCr2Si2																		K		21.1					21.1																																									A	TDR method		1210																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152292	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.824Co0.176As2	Ba	1	Fe	1.824	Co	0.176	As	2																3	2010																										AB2C2		ThCr2Si2																		K		21					21																																									A	TDR method		1400																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152293	PRB082054507	Co-content determined from WDS. [penet] from TDR method. Al-film coating (Tc=1.2 K, [penet] = 50 nm) to obtain absolute [penet] values.	Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2010																										AB2C2		ThCr2Si2																		K		17.2					17.2																																									A	TDR method		1820																																																				See Phys Rev.B, 78(2008)214515					Doping evolution of the absolute value of the London penetration depth and superfluid density in single crystals of Ba(Fe1-xCox)2As2			Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)054507	R. T. Gordon,H. Kim,N. Salovich,R. W. Giannetta,R. M. Fernandes,V. G. Kogan,T. Prozorov,S. L. Bud'ko,P. C. Canfield,M. A. Tanatar,R. Prozorov		
152294	PRB082054506		LaFeAsO0.85	La1Fe1As1O0.85	La	1	Fe	1	As	1															O	0.85			2010																												oxypnictide			A	4.0325		8.7134											ZrCuSiAs-type	K				24			24																																																																																																solid state reaction - sealed in Au - heat(1300C,2h,P=6 GPa, in h-BN cell) - Q to RT					Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 82(2010)054506	Y. F. Guo,Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,I. Nowik,I. Felner,V. P. S. Awana,K. Yamaura,E. Takayama-Muromachi		
152295	PRB082054506	lattice term in SP (beta) = 2.79 E-4 J/mol.K4	La(Fe,Zn)AsO0.85	La1Fe0.995Zn0.005As1O0.85	La	1	Fe	0.995	Zn	0.005	As	1													O	0.85			2010																												oxypnictide			A	4.0305		8.7141											ZrCuSiAs-type	K				14.1			14.1																																																								mJ/mol.K2	2	SP-heat	299	SP-heat																																				solid state reaction - sealed in Au - heat(1300C,2h,P=6 GPa, in h-BN cell) - Q to RT					Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 82(2010)054506	Y. F. Guo,Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,I. Nowik,I. Felner,V. P. S. Awana,K. Yamaura,E. Takayama-Muromachi		
152296	PRB082054506	(dTc/dx) = 9 K/at%Zn	La(Fe,Zn)AsO0.85	La1Fe0.99Zn0.01As1O0.85	La	1	Fe	0.99	Zn	0.01	As	1													O	0.85			2010																												oxypnictide			A	4.0292		8.7149											ZrCuSiAs-type	K				10.04			10.04																																																																																																solid state reaction - sealed in Au - heat(1300C,2h,P=6 GPa, in h-BN cell) - Q to RT					Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 82(2010)054506	Y. F. Guo,Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,I. Nowik,I. Felner,V. P. S. Awana,K. Yamaura,E. Takayama-Muromachi		
152297	PRB082054506		La(Fe,Zn)AsO0.85	La1Fe0.985Zn0.015As1O0.85	La	1	Fe	0.985	Zn	0.015	As	1													O	0.85			2010																												oxypnictide			A	4.0271		8.7155											ZrCuSiAs-type	K				6.01			6.01																																																																																																solid state reaction - sealed in Au - heat(1300C,2h,P=6 GPa, in h-BN cell) - Q to RT					Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 82(2010)054506	Y. F. Guo,Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,I. Nowik,I. Felner,V. P. S. Awana,K. Yamaura,E. Takayama-Muromachi		
152298	PRB082054506		La(Fe,Zn)AsO0.85	La1Fe0.98Zn0.02As1O0.85	La	1	Fe	0.98	Zn	0.02	As	1													O	0.85			2010																												oxypnictide			A	4.026		8.7159											ZrCuSiAs-type	K				4.32			4.32																																																																																																solid state reaction - sealed in Au - heat(1300C,2h,P=6 GPa, in h-BN cell) - Q to RT					Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 82(2010)054506	Y. F. Guo,Y. G. Shi,S. Yu,A. A. Belik,Y. Matsushita,M. Tanaka,Y. Katsuya,K. Kobayashi,I. Nowik,I. Felner,V. P. S. Awana,K. Yamaura,E. Takayama-Muromachi		
152299	PRL105087001	RH become positive below 115 K. [RH300] at 294 K.	Ba(Fe,Ru)2As2	Ba1Fe1.3Ru0.7As2	Ba	1	Fe	1.3	Ru	0.7	As	2																3	2010																										AB2C2		ThCr2Si2			A	4.0344		12.76												K		19.5					19.5																																																																																					m3/C	-0.000000000281					MRH152299					self-flux method					Significant Reduction of Electronic Correlations upon Isovalent Ru Substitution of BaFe2As2			Laboratoire de Physique des Solides, Universite Paris Sud, CNRS-UMR8502, 91405 Orsay, France	Phys.Rev.Lett., 105(2010)087001	V. Brouet,F. Rullier-Albenque,M. Marsi,B. Mansart,M. Aichhorn,S. Biermann,J. Faure,L. Perfetti,A. Taleb-Ibrahimi,P. Le Fevre,F. Bertran,A. Forget,D. Colson		
152300	PRB081224503	cleaved sample(d=20 micron-m). T<SDW> = 137 K	Ba(Fe,Ru)2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2				3.9633		13.022												K					4																																																																																																		FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152301	PRB081224503	cleaved sample(d=20 micron-m). T<SDW> = 77.8 K	Ba(Fe,Ru)2As2	Ba1Fe1.64Ru0.36As2	Ba	1	Fe	1.64	Ru	0.36	As	2																1	2010																										AB2C2		ThCr2Si2																		K		8.43					8.43																																																																																																FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152302	PRB081224503	cleaved sample(d=20 micron-m). T<SDW> = 54.9 K	Ba(Fe,Ru)2As2	Ba1Fe1.48Ru0.52As2	Ba	1	Fe	1.48	Ru	0.52	As	2																1	2010																										AB2C2		ThCr2Si2																		K		18.9					18.9	MTC152302																																																																																															FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152303	PRB081224503	cleaved sample(d=20 micron-m).	Ba(Fe,Ru)2As2	Ba1Fe1.3Ru0.7As2	Ba	1	Fe	1.3	Ru	0.7	As	2																1	2010																										AB2C2		ThCr2Si2			A	4.0347		12.766												K		19.6					19.6																																																																																																FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152304	PRB081224503	cleaved sample(d=20 micron-m).	Ba(Fe,Ru)2As2	Ba1Fe1.24Ru0.76As2	Ba	1	Fe	1.24	Ru	0.76	As	2																1	2010																										AB2C2		ThCr2Si2			A	4.0342		12.749												K		7.1					7.1																																																																																																FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152305	PRB081224503	cleaved sample(d=20 micron-m). T<SDW> = 132 K	Ba(Fe,Ru)2As2	Ba1Fe1.9Ru0.1As2	Ba	1	Fe	1.9	Ru	0.1	As	2																1	2010																										AB2C2		ThCr2Si2																		K					4																																																																																													MRH152305					FeAs/Ru + As self-flux method. mixture - sealed in evacuated quartz (aluminum crucible) - heat(1180C,4h) - slow cool to 1000C(3-6 C/h) - rapid cool to RT					Hole and electron contributions to the transport properties of Ba(Fe1-xRux)2As2 single crystals			Service de Physique de lEtat Condense, Orme des Merisiers, IRAMIS, CEA-Saclay (CNRS URA 2464), 91191 Gif sur Yvette Cedex, France	Phys.Rev.B, 81(2010)224503	F. Rullier-Albenque,D. Colson,A. Forget,P. Thuery,S. Poissonnet		
152306	PRB082054504	interlayer distance, d=9.35 A.	LixZrNCl	Li0.13Zr1N1Cl1	Li	0.13	Zr	1	N	1	Cl	1																	2010																																														K		12.2					12.2																																																3.4	14							mJ/mol.K2	1.1	SP-heat																																						See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152307	PRB082054504	M = C3H7NO. interlayer distance, d = 13.0 A..	LixMyZrNCl	Li0.13M0.26Zr1N1Cl1	Li	0.13	M	0.26	Zr	1	N	1	Cl	1															2010																																														K		13.7					13.7																																																4	14							mJ/mol.K2	1.2	SP-heat																																						See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152308	PRB082054504	M = (CH3)2SO. interlayer distance, d = 17.7 A..	LixMyZrNCl	Li0.13M0.39Zr1N1Cl1	Li	0.13	M	0.39	Zr	1	N	1	Cl	1															2010																																														K		13.1					13.1																																																4.2	14							mJ/mol.K2	1.2	SP-heat																																						See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152309	PRB082054504	interlayer distance, d=9.35 A.	LixZrNCl	Li0.05Zr1N1Cl1	Li	0.05	Zr	1	N	1	Cl	1																	2010																																														K		15					15																																																																																																See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152310	PRB082054504	M = C3H7NO. interlayer distance, d = 13.0 A..	LixMyZrNCl	Li0.05M0.26Zr1N1Cl1	Li	0.05	M	0.26	Zr	1	N	1	Cl	1															2010																																														K		15					15																																																																																																See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152311	PRB082054504	M = (CH3)2SO. interlayer distance, d = 17.7 A..	LixMyZrNCl	Li0.05M0.39Zr1N1Cl1	Li	0.05	M	0.39	Zr	1	N	1	Cl	1															2010																																														K		14.2					14.2																																																																																																See text.					Superconductivity in molecule-intercalated LixZrNCl with variable interlayer spacing			Quantum-Phase Electronics Center, School of Engineering, University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)054504	Yuichi Kasahara,Tsukasa Kishiume,Katsuki Kobayashi,Yasujiro Taguchi,Yoshihiro Iwasa		
152312	PRB082024519	structural transition (tetra-ortho) at 134 K. magnetic transition at 134 K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																			2010																										AB2C2		ThCr2Si2			A	3.9621		13.018												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152313	PRB082024519	structural transition (tetra-ortho) at 121 K. magnetic transition at 118 K.	Ba(Fe,Ni)2As2	Ba1Fe1.9866Ni0.0134As2	Ba	1	Fe	1.9866	Ni	0.0134	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9606		13.016												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152314	PRB082024519	structural transition (tetra-ortho) at 100 K. magnetic transition at 94 K.	Ba(Fe,Ni)2As2	Ba1Fe1.968Ni0.032As2	Ba	1	Fe	1.968	Ni	0.032	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9615		13.008												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152315	PRB082024519	structural transition (tetra-ortho) at 77 K. magnetic transition at 66 K.	Ba(Fe,Ni)2As2	Ba1Fe1.952Ni0.048As2	Ba	1	Fe	1.952	Ni	0.048	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9615		13.001												K	6.8		8.6	3.9			3.9																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152316	PRB082024519		Ba(Fe,Ni)2As2	Ba1Fe1.936Ni0.064As2	Ba	1	Fe	1.936	Ni	0.064	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9614		12.997												K	15.9		16.6	15.1			15.1																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152317	PRB082024519		Ba(Fe,Ni)2As2	Ba1Fe1.908Ni0.092As2	Ba	1	Fe	1.908	Ni	0.092	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9628		12.987												K	18.8		19.4	18.4			18.4																				T	resistivity(on), WHH		80	40					T/K	resistivity(on)		5.7	3	MHC152317		A	from Hc2		30	14																																																													Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152318	PRB082024519		Ba(Fe,Ni)2As2	Ba1Fe1.892Ni0.108As2	Ba	1	Fe	1.892	Ni	0.108	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9625		12.982												K	14.3		15.5	14.4			14.4																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152319	PRB082024519		Ba(Fe,Ni)2As2	Ba1Fe1.856Ni0.144As2	Ba	1	Fe	1.856	Ni	0.144	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9638		12.976												K	5.7		7.5	6			6																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152320	PRB082024519	structural transition (tetra-ortho) at 119 K. magnetic transition at 117 K.	Ba(Fe,Cu)2As2	Ba1Fe1.9846Cu0.0154As2	Ba	1	Fe	1.9846	Cu	0.0154	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9636		13.0136												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152321	PRB082024519	structural transition (tetra-ortho) at 93 K. magnetic transition at 86 K.	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.04As2	Ba	1	Fe	1.856	Cu	0.04	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9647		13.0046												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152322	PRB082024519	structural transition (tetra-ortho) at 79 K. magnetic transition at 71 K.	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.052As2	Ba	1	Fe	1.856	Cu	0.052	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9668		13.0063												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152323	PRB082024519	structural transition (tetra-ortho) at 57 K. magnetic transition at 48 K.	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.07As2	Ba	1	Fe	1.856	Cu	0.07	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9674		12.997												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152324	PRB082024519	SC regin is very small (maybe, 0.04 < x , 0.045 in Ba(Fe1-xCux)2As2)	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.088As2	Ba	1	Fe	1.856	Cu	0.088	As	2																	2010																										AB2C2		ThCr2Si2																		K	2.1		2.2				2.15																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152325	PRB082024519	structural transition (tetra-ortho) at 103 K. magnetic transition at 99 K.	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.1As2	Ba	1	Fe	1.856	Cu	0.1	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9723		13.001												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152326	PRB082024519	structural transition (tetra-ortho) at 85 K. magnetic transition at 78 K.	Ba(Fe,Cu)2As2	Ba1Fe1.856Cu0.122As2	Ba	1	Fe	1.856	Cu	0.122	As	2																	2010																										AB2C2		ThCr2Si2			A	3.9756		12.9937												K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152327	PRB082024519	structural transition (tetra-ortho) at 75 K. magnetic transition at 68 K.	Ba(Fe,Co)2As2	Ba1Fe1.952Co0.048As2	Ba	1	Fe	1.952	Co	0.048	As	2																	2010																										AB2C2		ThCr2Si2																		K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152328	PRB082024519	structural transition (tetra-ortho) at 41 K. magnetic transition at 29 K.	Ba(Fe,Co,Cu)2As2	Ba1Fe1.942Co0.048Cu0.01As2	Ba	1	Fe	1.942	Co	0.048	Cu	0.01	As	2															2010																										AB2C2		ThCr2Si2																		K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152329	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.936Co0.044Cu0.02As2	Ba	1	Fe	1.936	Co	0.044	Cu	0.02	As	2															2010																										AB2C2		ThCr2Si2																		K	0		4.7				2.35																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152330	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.918Co0.044Cu0.038As2	Ba	1	Fe	1.918	Co	0.044	Cu	0.038	As	2															2010																										AB2C2		ThCr2Si2																		K	9		11	8.7			8.7																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152331	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.906Co0.042Cu0.052As2	Ba	1	Fe	1.906	Co	0.042	Cu	0.052	As	2															2010																										AB2C2		ThCr2Si2																		K	11		12.1	11.6			11.6																				T	resistivity(on), WHH		64	28					T/K	resistivity(on)		7.8	3.5	MHC152331																																																																			Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152332	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.894Co0.042Cu0.064As2	Ba	1	Fe	1.894	Co	0.042	Cu	0.064	As	2															2010																										AB2C2		ThCr2Si2																		K	8.3		8.9	9.6			9.6																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152333	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.872Co0.042Cu0.086As2	Ba	1	Fe	1.872	Co	0.042	Cu	0.086	As	2															2010																										AB2C2		ThCr2Si2																		K	2		4.6	4.3			4.3																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152334	PRB082024519	structural transition (tetra-ortho) at 59 K. magnetic transition at 40 K.	Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																	2010																										AB2C2		ThCr2Si2																		K	16.5		17.8				17.15																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152335	PRB082024519	structural transition (tetra-ortho) at 48 K.	Ba(Fe,Co,Cu)2As2	Ba1Fe1.889Co0.102Cu0.009As2	Ba	1	Fe	1.889	Co	0.102	Cu	0.009	As	2															2010																										AB2C2		ThCr2Si2																		K	20.4		21.5				20.95																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152336	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.868Co0.094Cu0.038As2	Ba	1	Fe	1.868	Co	0.094	Cu	0.038	As	2															2010																										AB2C2		ThCr2Si2																		K	15.2		15.9				15.55																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152337	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.838Co0.094Cu0.068As2	Ba	1	Fe	1.838	Co	0.094	Cu	0.068	As	2															2010																										AB2C2		ThCr2Si2																		K	4.6		6				5.3																																																																																																					Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152338	PRB082024519		Ba(Fe,Co,Cu)2As2	Ba1Fe1.818Co0.09Cu0.092As2	Ba	1	Fe	1.818	Co	0.09	Cu	0.092	As	2															2010																										AB2C2		ThCr2Si2																		K					2																																																																																																							Temperature versus doping phase diagrams for Ba(Fe1-xTMx)2As2 (TM=Ni,Cu,Cu/Co) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)024519	N. Ni,A. Thaler,J. Q. Yan,A. Kracher,E. Colombier,S. L. Bud'ko,P. C. Canfield,S. T. Hannahs		
152339	PRB082024520	energy gap calculated from muon-SR(TF=500G) fitting. fitting Tc = 3.8 K.	Mg10Ir19B16	Mg10Ir19B16	Mg	10	Ir	19	B	16																			2010																										A10B16C19			I4[-]3m		A	10.5629														K		3.8		4.8			3.8																																									A	muon-SR	3570			meV	1.6	4.74	16																																															solid state reaction					Muon spin rotation/relaxation measurements of the noncentrosymmetric superconductor Mg10Ir19B16			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 82(2010)024520	A. A. Aczel,T. J. Williams,T. Goko,J. P. Carlo,W. Yu,Y. J. Uemura,T. Klimczuk,J. D. Thompson,R. J. Cava,G. M. Luke		
152340	PRB082024520	energy gap calculated from muon-SR(TF=500G) fitting. fitting Tc = 3.7 K.	Mg10Ir19B16	Mg10Ir19B16	Mg	10	Ir	19	B	16																			2010																										A10B16C19			I4[-]3m		A	10.5655														K		3.7		4.6			3.7																																									A	muon-SR	3230			meV	1.6	4.93	16																																															solid state reaction					Muon spin rotation/relaxation measurements of the noncentrosymmetric superconductor Mg10Ir19B16			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev.B, 82(2010)024520	A. A. Aczel,T. J. Williams,T. Goko,J. P. Carlo,W. Yu,Y. J. Uemura,T. Klimczuk,J. D. Thompson,R. J. Cava,G. M. Luke		
152341	NAT4440465	B-doped Si. two phases: 5.7at%B (2.8 E+21 B/cm3) and 8.4at%B (4.2 E+21 B/cm3)	B-doped Si	B0.057Si0.943	B	0.057	Si	0.943																					2006																												diamond																		K	0.15		0.4	0.34			0.34																				T	resistivity, extrapolation	0.39												MHC152341																																																														gas immersion laser doping method. chemical absorbed (BCl3) on (001) Si-wafer, then UV laser, melt and defuse into Si					Superconductivity in doped cubic silicon			Laboratoire dEtudes des Proprietes Electroniques des Solides, CNRS, BP166, 38042 Grenoble, France	Nature, 444(2006)465	E. Bustarret,C. Marcenat,P. Achatz,J. Kacmarcik,F. Levy,A. Huxley,L. Ortega,E. Bourgeois,X. Blase,D. Debarre,J. Boulmer		
152342	JPS076103710	B substitutes for C. GL parameter = 0.3 (type-I SC). supercooling appears. Hc(0) = 115 Oe for warming (S-to-N) .	B-doped SiC	B0.039C0.961Si1	B	0.039	C	0.961	Si	1																			2007																																														K		1.4				0.15	1.4																				Oe	resistivity, extrapolation	80												MHC152342																																																								7		n/cm3	1910000000000000000000	beta-SiC,Si,a-B		mixture - pellet - SIN(1620C,12h,in flowing gas(Ar + H))					Superconductivity in Boron-doped SiC			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)103710	Zhi-An REN,Junya KATO,Takahiro MURANAKA,Jun AKIMITSU,Markus KRIENER,Yoshiteru MAENO		
152343	JPS076103710	B substitutes for C.	B-doped SiC	B0.978C0.022Si1	B	0.978	C	0.022	Si	1																			2007																																														K		1.35				0.15	1.35																																																																																										7		n/cm3	1060000000000000000000	beta-SiC,Si,a-B		mixture - pellet - SIN(1620C,12h,in flowing gas(Ar + H))					Superconductivity in Boron-doped SiC			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara, Kanagawa 229-8558	J.Phys.Soc.Jpn, 76(2007)103710	Zhi-An REN,Junya KATO,Takahiro MURANAKA,Jun AKIMITSU,Markus KRIENER,Yoshiteru MAENO		
152344	PRB082054510	under doped sample. anisotropy depends on temperature and magnetic field.	SmBa2Cu3O7	Sm1Ba2Cu3O7-z	Sm	1	Ba	2	Cu	3															O	7-z		3	2010																												Y123			A	3.8619	3.9092	11.7738												K		42.8					42.8																				T	magnetization, WHH	7.5							T/K	magnetization	0.24																																																																	single crystals grown by top-seeded solution growth. ANN(490 - 505 C, in flowing O+He gas					Evidence for a temperature dependent anisotropy of the superconducting state parameters in underdoped SmBa2Cu3Ox			Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, PL-02-668 Warsaw, Poland	Phys.Rev.B, 82(2010)054510	A. Kortyka,R. Puzniak,A. Wisniewski,M. Zehetmayer,H. W. Weber,C. Y. Tang,X. Yao,K. Conder		
152345	PRB082054510	under doped sample. anisotropy depends on temperature and magnetic field.	SmBa2Cu3O7	Sm1Ba2Cu3O7-z	Sm	1	Ba	2	Cu	3															O	7-z		3	2010																												Y123			A	3.8573	3.9131	11.7585												K		51.5					51.5																				T	magnetization, WHH	16.8							T/K	magnetization	0.45																																																																	single crystals grown by top-seeded solution growth. ANN(490 - 505 C, in flowing O+He gas					Evidence for a temperature dependent anisotropy of the superconducting state parameters in underdoped SmBa2Cu3Ox			Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, PL-02-668 Warsaw, Poland	Phys.Rev.B, 82(2010)054510	A. Kortyka,R. Puzniak,A. Wisniewski,M. Zehetmayer,H. W. Weber,C. Y. Tang,X. Yao,K. Conder		
152346	PRB082054510	under doped sample. anisotropy depends on temperature and magnetic field.	SmBa2Cu3O7	Sm1Ba2Cu3O7-z	Sm	1	Ba	2	Cu	3															O	7-z		3	2010																												Y123			A	3.8533	3.9131	11.7491												K		56.5					56.5																				T	magnetization, WHH	24.6							T/K	magnetization	0.6																																																																	single crystals grown by top-seeded solution growth. ANN(490 - 505 C, in flowing O+He gas					Evidence for a temperature dependent anisotropy of the superconducting state parameters in underdoped SmBa2Cu3Ox			Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, PL-02-668 Warsaw, Poland	Phys.Rev.B, 82(2010)054510	A. Kortyka,R. Puzniak,A. Wisniewski,M. Zehetmayer,H. W. Weber,C. Y. Tang,X. Yao,K. Conder		
152347	PRB082054510	under doped sample. anisotropy depends on temperature and magnetic field.	SmBa2Cu3O7	Sm1Ba2Cu3O7-z	Sm	1	Ba	2	Cu	3															O	7-z		3	2010																												Y123			A	3.8516	3.9131	11.7438												K		63.6					63.6																				T	magnetization, WHH	48.5							T/K	magnetization	1.05																																																																	single crystals grown by top-seeded solution growth. ANN(490 - 505 C, in flowing O+He gas					Evidence for a temperature dependent anisotropy of the superconducting state parameters in underdoped SmBa2Cu3Ox			Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, PL-02-668 Warsaw, Poland	Phys.Rev.B, 82(2010)054510	A. Kortyka,R. Puzniak,A. Wisniewski,M. Zehetmayer,H. W. Weber,C. Y. Tang,X. Yao,K. Conder		
152348	PRL098047003	(111) diamond film, n = 8.4 E+21 /cm3.  B/C = 5%. energy gap measured by PES. gap(4.5K) = 0.78 meV. [gapene] obtained byasuming BCS-like T-dependency.	B-doped C	B0.048C0.952	B	0.048	C	0.952																					2007																												diamond																		K				6.6			6.6																																																3.56	9																																															microwave plasma CVD					Observation of a Superconducting Gap in Boron-Doped Diamond by Laser-Excited Photoemission Spectroscopy			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 98(2007)047003	K. Ishizaka,R. Eguchi,S. Tsuda,T. Yokoya,A. Chainani,T. Kiss,T. Shimojima,T. Togashi,S. Watanabe,C.-T. Chen,C. Q. Zhang,Y. Takano,M. Nagao,I. Sakaguchi,T. Takenouchi,H. Kawarada,S. Shin		
152349	PRB082094506	P-induced SC. P<crit> = 23 GPa. Tc(max) = 2 K(P=65GPa). lattice const. a = 4.879 A for fcc at P= 23 GPa.	BI3	B1I3	B	1	I	3																					2010																										AB3			P6<3>/m		A	4.879														K		1.86			0		1.86	MTC152349																																																																																															from Sigma Aldrich Japan					Pressure-induced phase transition, metallization, and superconductivity in boron triiodide			Graduate School of Humanities and Sciences, Ochanomizu University, 2-1-1 Ohtsuka, Bunkyo-ku, Tokyo 112-8610, Japan	Phys.Rev.B, 82(2010)094506	Nozomu Hamaya,Miyuki Ishizuka,Suzue Onoda,Jiang Guishan,Ayako Ohmura,Katsuya Shimizu		
152350	PRB082052501	difference of Tc comes from Ir-vacancies. [RH300] shows at 280 K.	Mg12Ir19B16	Mg12Ir19B16	Mg	12	Ir	19	B	16																			2010																										A12B16C19																				K		2.5					2.5																																																																																					m3/C	-0.000000000348				9	MRH152350										Multiband effect in the noncentrosymmetric superconductors Mg12-zIr19B16 revealed by Hall effect and magnetoresistance measurements			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 82(2010)052501	Gang Mu,Huan Yang,Hai-Hu Wen		
152351	PRB082052501	difference of Tc comes from Ir-vacancies. [RH300] shows at 280 K.	Mg12Ir19B16	Mg12Ir19B16	Mg	12	Ir	19	B	16																			2010																										A12B16C19																				K		4.7					4.7																																																																																					m3/C	-0.000000000329				9	MRH152351										Multiband effect in the noncentrosymmetric superconductors Mg12-zIr19B16 revealed by Hall effect and magnetoresistance measurements			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 82(2010)052501	Gang Mu,Huan Yang,Hai-Hu Wen		
152352	PRB082052501	difference of Tc comes from Ir-vacancies. [RH300] shows at 280 K.	Mg12Ir19B16	Mg12Ir19B16	Mg	12	Ir	19	B	16																			2010																										A12B16C19																				K		5.7					5.7																																																																																					m3/C	-0.000000000158				9	MRH152352										Multiband effect in the noncentrosymmetric superconductors Mg12-zIr19B16 revealed by Hall effect and magnetoresistance measurements			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 82(2010)052501	Gang Mu,Huan Yang,Hai-Hu Wen		
152353	JPC020095225	Tc defined as 0.5Rn. RRR=10.6. hidden order T0 and AFM order Tn shown in Fig. (dT0/dp) = 0.10 K/kbar. (dTn/dP) = 0.23 K/kbar.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2008																										AB2C2		ThCr2Si2			A	4.14		9.56												K		1.41					1.41	MPH152353																																	MHC152353																																																														tri-arc furnace equipped with Czochralski crystal puller. ANN(900C,7d,in 150 Torr Ar)					The evolution of the ordered states of single-crystal URu2Si2 under pressure			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	J.Phys.: Condens.Matter, 20(2008)095225	J R Jeffries,N P Butch,B T Yukich,M B Maple		
152354	PRB082064517		(Sm,Th)OFeAs	Sm0.9Th0.1Fe1As1O1	Sm	0.9	Th	0.1	Fe	1	As	1													O	1		1	2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K		51.4					51.4																																		HIR152354																																																												SmAs,ThAs,Fe2O3,Fe		high-P synthesis					Th-substituted SmFeAsO: Structural details and superconductivity with Tc above 50 K			Laboratory for Solid State Physics, ETH Zurich, Schafmattstrasse 16, CH-8093 Zurich, Switzerland	Phys.Rev.B, 82(2010)064517	N. D. Zhigadlo,S. Katrych,S. Weyeneth,R. Puzniak,P. J. W. Moll,Z. Bukowski,J. Karpinski,H. Keller,B. Batlogg		
152355	PRB082064517		(Sm,Th)OFeAs	Sm0.89Th0.11Fe1As1O1	Sm	0.89	Th	0.11	Fe	1	As	1													O	1		3	2010																										ABCD		oxypnictide			A	3.9369		8.451											ZrCuSiAs-type	K	47.4	48.9	49.7	49.5			48.9																													T/K			5.4	2.7																																																													SmAs,ThAs,Fe2O3,Fe		high-P synthesis					Th-substituted SmFeAsO: Structural details and superconductivity with Tc above 50 K			Laboratory for Solid State Physics, ETH Zurich, Schafmattstrasse 16, CH-8093 Zurich, Switzerland	Phys.Rev.B, 82(2010)064517	N. D. Zhigadlo,S. Katrych,S. Weyeneth,R. Puzniak,P. J. W. Moll,Z. Bukowski,J. Karpinski,H. Keller,B. Batlogg		
152356	PRB082064517		(Sm,Th)OFeAs	Sm0.65Th0.35Fe1As1O1	Sm	0.65	Th	0.35	Fe	1	As	1													O	1			2010																										ABCD		oxypnictide																	ZrCuSiAs-type	K			53				53																																																																																														SmAs,ThAs,Fe2O3,Fe		high-P synthesis					Th-substituted SmFeAsO: Structural details and superconductivity with Tc above 50 K			Laboratory for Solid State Physics, ETH Zurich, Schafmattstrasse 16, CH-8093 Zurich, Switzerland	Phys.Rev.B, 82(2010)064517	N. D. Zhigadlo,S. Katrych,S. Weyeneth,R. Puzniak,P. J. W. Moll,Z. Bukowski,J. Karpinski,H. Keller,B. Batlogg		
152357	PRB082094502	Anisotropy = 1.44 at P = 0.  P=0.94 GPa: Tc=28.0K, cohere(ab)=35.7A, cohere(c)=15.4A.   P=2.15GPa: Tc=24.5K, cohere(ab)=42.6A, cohere(c)=14.5A	BaFe2(As,P)2	Ba1Fe2As1.3P0.7	Ba	1	Fe	2	As	1.3	P	0.7																3	2010																										AB2C2		ThCr2Si2			A	3.9266		12.8271												K		30.5					30.5			K/GPa	-1.8																T	WHH approx.		50.7	35.1					T/K			2.4	1.67	MHC152357		A	from Hc2		30.6	21.2																																																								mixture - sealed in evacuated quartz tube - heat(1150C-1200C,12h) - slow cool to 900C(1.5C/h)					Anisotropic superconducting properties of optimally doped BaFe2(As0.65P0.35)2 under pressure			Cavendish Laboratory, University of Cambridge, J.J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.B, 82(2010)094502	Swee K. Goh,Y. Nakai,K. Ishida,L. E. Klintberg,Y. Ihara,S. Kasahara,T. Shibauchi,Y. Matsuda,T. Terashima		
152358	CHM0207201	Th:Nd:O:Fe:As = 5.5:22:24:26.1:22.4.  impurity phase : ThO2	(Nd,Th)OFeAs	Nd0.8Th0.2Fe1As1O1	Nd	0.8	Th	0.2	Fe	1	As	1													O	1			2008																										ABCD		oxypnictide			A	3.9802		8.6124											ZrCuSiAs-type	K		43	47	38		5	43																																																																																					m3/C	-0.0000000006					RH152358			NdAs,ThO2,FeAs,Fe,Fe2O3		solid state reaction. pellet - wrapped (Ta-foil) - sealed(quartz tube) - heat(940C,10h) - SIN(1150C,48h)					Synthesis of a New Member in Iron-Based Layered Superconductor: Nd0.8Th0.2OFeAs with Tc = 38 K			Department of Physics, Surface Physics Laboratory,  AdVanced Materials Laboratory, Fudan UniVersity, Shanghai 200433, P.R. China	Chem.Mater., 20(2008)7201	Min Xu,Fei Chen,Cheng He,Hong-Wei Ou,Jia-Feng Zhao,Dong-Lai Feng		
152359	SNM0230199		(Cu,Tl)Ba2Ca2Cu3O10	Tl0.5Ba2Ca2Cu3.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3.5													O	10-z			2010																												Tl1223			A	3.91		14.89												K	90		118				104																																																																																																solid state reaction. precursor(Cu-Ba-Ca-Cd-O) mixed with Tl2O3, then pelletized, heat(860C), quenched					Cd-doped Cu0.5Tl0.5Ba2Ca2Cu3-yCdyO10-z (y = 00.51.01.52.0) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	J.Supercond.Nov Magn., 23(2010)199	Nawazish A. Khan,Asad Raza		
152360	SNM0230199		(Cu,Tl)Ba2Ca2(Cu,Cd)3O10	Tl0.5Ba2Ca2Cu3Cd0.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	3	Cd	0.5											O	10-z			2010																												Tl1223			A	3.9		14.91												K	85		101				93																																																																																																solid state reaction. precursor(Cu-Ba-Ca-Cd-O) mixed with Tl2O3, then pelletized, heat(860C), quenched					Cd-doped Cu0.5Tl0.5Ba2Ca2Cu3-yCdyO10-z (y = 00.51.01.52.0) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	J.Supercond.Nov Magn., 23(2010)199	Nawazish A. Khan,Asad Raza		
152361	SNM0230199		(Cu,Tl)Ba2Ca2(Cu,Cd)3O10	Tl0.5Ba2Ca2Cu2.5Cd1O10-z	Tl	0.5	Ba	2	Ca	2	Cu	2.5	Cd	1											O	10-z			2010																												Tl1223			A	3.89		14.95												K	86		103				94.5																																																																																																solid state reaction. precursor(Cu-Ba-Ca-Cd-O) mixed with Tl2O3, then pelletized, heat(860C), quenched					Cd-doped Cu0.5Tl0.5Ba2Ca2Cu3-yCdyO10-z (y = 00.51.01.52.0) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	J.Supercond.Nov Magn., 23(2010)199	Nawazish A. Khan,Asad Raza		
152362	SNM0230199		(Cu,Tl)Ba2Ca2(Cu,Cd)3O10	Tl0.5Ba2Ca2Cu2Cd1.5O10-z	Tl	0.5	Ba	2	Ca	2	Cu	2	Cd	1.5											O	10-z			2010																												Tl1223			A	3.91		14.99												K	84		100				92																																																																																																solid state reaction. precursor(Cu-Ba-Ca-Cd-O) mixed with Tl2O3, then pelletized, heat(860C), quenched					Cd-doped Cu0.5Tl0.5Ba2Ca2Cu3-yCdyO10-z (y = 00.51.01.52.0) superconductors			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad 45320, Pakistan	J.Supercond.Nov Magn., 23(2010)199	Nawazish A. Khan,Asad Raza		
152363	PRB082104503	AFM at low temperature	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1			2010																										ABCD		oxypnictide			A	3.9367		8.5142												K					1.8																																																																																																		solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152364	PRB082104503	AFM at low temperature	SmO(Fe,Ir)As	Sm1Fe0.97Ir0.03As1O1	Sm	1	Fe	0.97	Ir	0.03	As	1													O	1			2010																										ABCD		oxypnictide			A	3.942		8.4947												K					1.8																																																																																																		solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152365	PRB082104503	AFM at low temperature	SmO(Fe,Ir)As	Sm1Fe0.96Ir0.04As1O1	Sm	1	Fe	0.96	Ir	0.04	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9435		8.4918												K					1.8																																																																																																		solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152366	PRB082104503		SmO(Fe,Ir)As	Sm1Fe0.94Ir0.06As1O1	Sm	1	Fe	0.94	Ir	0.06	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9468		8.477												K				18			18																																																																																																solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152367	PRB082104503		SmO(Fe,Ir)As	Sm1Fe0.89Ir0.11As1O1	Sm	1	Fe	0.89	Ir	0.11	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9518		8.4472												K				18.3			18.3																																																																																																solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152368	PRB082104503		SmO(Fe,Ir)As	Sm1Fe0.84Ir0.16As1O1	Sm	1	Fe	0.84	Ir	0.16	As	1													O	1			2010																										ABCD		oxypnictide			A	3.957		8.4335												K				17.3			17.3																																																																																																solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152369	PRB082104503	not any magnetic order	SmO(Fe,Ir)As	Sm1Fe0.85Ir0.25As1O1	Sm	1	Fe	0.85	Ir	0.25	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9686		8.3864												K					1.8																																																																																																		solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152370	PRB082104503	not any magnetic order	SmO(Fe,Ir)As	Sm1Fe0.725Ir0.275As1O1	Sm	1	Fe	0.725	Ir	0.275	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9719		8.3766												K					1.8																																																																																																		solid state reaction. mixture - wrapped in Ta foil - heat(1160C, 48h, in quartz tube)					Structural and physical properties of SmFe1-xIrxAsO (0 =< x =< 0.275) obtained by synchrotron x-ray diffraction, Raman spectroscopy, and magnetization measurements			"Dipartimento di Chimica Fisica ""M. Rolla,"" INSTM (UdR Pavia) and IENI-CNR, Universita di Pavia, Viale Taramelli 16, 27100 Pavia, Italy"	Phys.Rev.B, 82(2010)104503	Beatrice Maroni,Lorenzo Malavasi,M. Cristina Mozzati,Marco S. Grandi,Adrian H. Hill,Daniele Chermisi,Paolo Dore,Paolo Postorino		
152371	PRB082104507	final heat treatment(930-960C, total 72h)	(Cu,M0)Sr2YCu2O7	Mo0.25Sr2Y1Cu2.75O7+z	Mo	0.25	Sr	2	Y	1	Cu	2.75													O	7+z			2010																												Cu1212	P4/mmm		A	3.816		11.471											(Cu,Mo)-1212	K		87					87																																																																																																high-pressure-oxygenation (500C,30min,5 GPa) in cubic cell with KClO3					Superconductivity and oxygen ordering correlations in the homologous series of (Cu,Mo)Sr2(Ce,Y)sCu2O5+2s+z			Physics Department, Northern Illinois University, DeKalb, Illinois 60115, USA	Phys.Rev.B, 82(2010)104507	O. Chmaissem,I. Grigoraviciute,H. Yamauchi,M. Karppinen,M. Marezio		
152372	PRB082104507	final heat treatment(950-1005C, total 120h)	(Cu,M0)Sr2(Ce,Y)2Cu2O9	Mo0.25Sr2Ce1Y1Cu2.75O9+z	Mo	0.25	Sr	2	Ce	1	Y	1	Cu	2.75											O	9+z			2010																												Cu1222	I4/mmm		A	3.83		28.454											(Cu,Mo)-1222	K		56					56																																																																																																high-pressure-oxygenation (500C,30min,5 GPa) in cubic cell with KClO3					Superconductivity and oxygen ordering correlations in the homologous series of (Cu,Mo)Sr2(Ce,Y)sCu2O5+2s+z			Physics Department, Northern Illinois University, DeKalb, Illinois 60115, USA	Phys.Rev.B, 82(2010)104507	O. Chmaissem,I. Grigoraviciute,H. Yamauchi,M. Karppinen,M. Marezio		
152373	PRB082104507	final heat treatment(950-1005C, total 168h)	(Cu,Mo)Sr2(Ce,Y)3Cu2O11	Mo0.25Sr2Ce2Y1Cu2.75O11+z	Mo	0.25	Sr	2	Ce	2	Y	1	Cu	2.75											O	11+z			2010																												Cu1232	P4/mmm		A	3.8262		16.9047											(Cu,Mo)-1232	K		54.5					54.5																																																																																																high-pressure-oxygenation (500C,30min,5 GPa) in cubic cell with KClO3					Superconductivity and oxygen ordering correlations in the homologous series of (Cu,Mo)Sr2(Ce,Y)sCu2O5+2s+z			Physics Department, Northern Illinois University, DeKalb, Illinois 60115, USA	Phys.Rev.B, 82(2010)104507	O. Chmaissem,I. Grigoraviciute,H. Yamauchi,M. Karppinen,M. Marezio		
152374	PRB082104507	final heat treatment(950-985C, total 264h). structural data for as-synthesized sample.	(Cu,Mo)Sr2(Ce,Y)4Cu2O13	Mo0.25Sr2Ce3Y1Cu2.75O13+z	Mo	0.25	Sr	2	Ce	3	Y	1	Cu	2.75											O	13+z			2010																												Cu1242	I4/mmm		A	3.8308		39.344											(Cu,Mo)-1242	K		56					56																																																																																																high-pressure-oxygenation (500C,30min,5 GPa) in cubic cell with KClO3					Superconductivity and oxygen ordering correlations in the homologous series of (Cu,Mo)Sr2(Ce,Y)sCu2O5+2s+z			Physics Department, Northern Illinois University, DeKalb, Illinois 60115, USA	Phys.Rev.B, 82(2010)104507	O. Chmaissem,I. Grigoraviciute,H. Yamauchi,M. Karppinen,M. Marezio		
152375	PRL105126401	Tc(P) measured. P: hydrostatic. R(T) shows max at T=50 K.	CeCo(In,Sn)5	Ce1Co1In4.92Sn0.08	Ce	1	Co	1	In	4.92	Sn	0.08																3	2010																										ABC5		HoCoGa5																		K		1.22					1.22	MTC152375																																																																																															self-flux method					Superconducting Quantum Critical Point in CeCoIn5-xSnx			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, 22290-180, Rio de Janeiro, RJ, Brazil	Phys.Rev.Lett., 105(2010)126401	S. M. Ramos,M. B. Fontes,E. N. Hering,M. A. Continentino,E. Baggio-Saitovich,F. Dinola Neto,E. M. Bittar,P. G. Pagliuso,E. D. Bauer,J. L. Sarrao,J. D. Thompson		
152376	PRL105126401	Tc(P) measured. P: hydrostatic. R(T) shows max at T=51.5 K.	CeCo(In,Sn)5	Ce1Co1In4.9Sn0.1	Ce	1	Co	1	In	4.9	Sn	0.1																3	2010																										ABC5		HoCoGa5																		K		1.02					1.02	MTC152375																																																																																															self-flux method					Superconducting Quantum Critical Point in CeCoIn5-xSnx			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, 22290-180, Rio de Janeiro, RJ, Brazil	Phys.Rev.Lett., 105(2010)126401	S. M. Ramos,M. B. Fontes,E. N. Hering,M. A. Continentino,E. Baggio-Saitovich,F. Dinola Neto,E. M. Bittar,P. G. Pagliuso,E. D. Bauer,J. L. Sarrao,J. D. Thompson		
152377	PRL105126401	Tc(P) measured. P: hydrostatic. R(T) shows max at T=52.3 K.	CeCo(In,Sn)5	Ce1Co1In4.88Sn0.12	Ce	1	Co	1	In	4.88	Sn	0.12																3	2010																										ABC5		HoCoGa5																		K		0.81					0.81	MTC152375																																																																																															self-flux method					Superconducting Quantum Critical Point in CeCoIn5-xSnx			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, 22290-180, Rio de Janeiro, RJ, Brazil	Phys.Rev.Lett., 105(2010)126401	S. M. Ramos,M. B. Fontes,E. N. Hering,M. A. Continentino,E. Baggio-Saitovich,F. Dinola Neto,E. M. Bittar,P. G. Pagliuso,E. D. Bauer,J. L. Sarrao,J. D. Thompson		
152378	PRL105126401	Tc(P) measured. P: hydrostatic. R(T) shows max at T=55.7 K. x<crit> = 0.18 in CeCoIn5-xSnx)	CeCo(In,Sn)5	Ce1Co1In4.86Sn0.14	Ce	1	Co	1	In	4.86	Sn	0.14																3	2010																										ABC5		HoCoGa5																		K		0.556					0.556	MTC152375																																																																																															self-flux method					Superconducting Quantum Critical Point in CeCoIn5-xSnx			Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, 22290-180, Rio de Janeiro, RJ, Brazil	Phys.Rev.Lett., 105(2010)126401	S. M. Ramos,M. B. Fontes,E. N. Hering,M. A. Continentino,E. Baggio-Saitovich,F. Dinola Neto,E. M. Bittar,P. G. Pagliuso,E. D. Bauer,J. L. Sarrao,J. D. Thompson		
152379	JPS079074704	anisotropy (Hc2) = 1.54	Fe(Se,Te)	Fe1.12Se0.3Te0.7	Fe	1.12	Se	0.3	Te	0.7																		3	2010																															A	3.7982		6.0651												K			13.7				13.7																				T	magnetic, extrapolation		57	37					T/K	magnetic		6	3.9	MHC152379		A	from Hc2		30	24																																																								mixture - load into quartz - sealed in evacuated quartz tube - heat to 920C(over36h) - hold(12h) - cool to 400C(140h)					Magnetic and Superconducting Properties in Single Crystalline Fe1+zTe1-xSex (x < 0.50)  System			Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 79(2010)074704	Jinhu YANG,Mami MATSUI,Masatomo KAWA,Hiroto OHTA,Chishiro MICHIOKA,Chiheng DONG,Hangdong WANG,Huiqiu YUAN,Minghu FANG,Kazuyoshi YOSHIMURA		
152380	JPS079074704	anisotropy (Hc2) = 2.1	Fe(Se,Te)	Fe1.04Se0.33Te0.67	Fe	1.04	Se	0.33	Te	0.67																		3	2010																																														K			14.1				14.1																				T	magnetic, extrapolation		85	40					T/K	magnetic		8.7	4.2	MHC152380		A	from Hc2		29	20																																																								mixture - load into quartz - sealed in evacuated quartz tube - heat to 920C(over36h) - hold(12h) - cool to 400C(140h)					Magnetic and Superconducting Properties in Single Crystalline Fe1+zTe1-xSex (x < 0.50)  System			Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 79(2010)074704	Jinhu YANG,Mami MATSUI,Masatomo KAWA,Hiroto OHTA,Chishiro MICHIOKA,Chiheng DONG,Hangdong WANG,Huiqiu YUAN,Minghu FANG,Kazuyoshi YOSHIMURA		
152381	JPS079074706	composition by EDX. For WHH approx, Hc2(0) = 167 and 50.3 T for // and /n, respectively. anisotropy (Hc2) = 1(T=0) ,  2.5(near Tc).	Fe(Se,Te)	Fe1.05Se0.15Te0.85	Fe	1.05	Se	0.15	Te	0.85																		3	2010																																														K			14.1				14.1																				T	resistivity, extrapolation		47	47					T/K	resistivity		17.2	5.2	MHC152381		A	from Hc2		26	26																																																								self-flux method					Weak Superconducting Fluctuations and Small Anisotropy of the Upper Critical Fields in an Fe1.05Te0.85Se0.15 Single Crystal			KYOKUGEN, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 79(2010)074706	Takanori KIDA,Masahiro KOTANI,Yoshikazu MIZUGUCHI,Yoshihiko TAKANO,Masayuki HAGIWARA		
152382	PHC4701092	Fe-diffusion using micro-size Fe powder	(Mg,Fe)B2	Mg0.99Fe0.01B2	Mg	0.99	Fe	0.01	B	2																			2010																										AB2		AlB2																		K			38.2				38.2																																																																																																hybridized diffusion method					Iron doping effect on superconducting properties of MgB2			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1092	C.H. Cheng,Y. Yang,C. Ke,H.T. Lin		
152383	PHC4701092	Fe-diffusion using nano-size Fe powder	(Mg,Fe)B2	Mg0.99Fe0.01B2	Mg	0.99	Fe	0.01	B	2																			2010																										AB2		AlB2																		K			31.2				31.2																																																																																																hybridized diffusion method					Iron doping effect on superconducting properties of MgB2			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1092	C.H. Cheng,Y. Yang,C. Ke,H.T. Lin		
152384	PHC4701092	Fe-diffusion using nano-size Fe powder	(Mg,Fe)B2	Mg0.95Fe0.05B2	Mg	0.95	Fe	0.05	B	2																			2010																										AB2		AlB2																		K			29.5				29.5																																																																																																hybridized diffusion method					Iron doping effect on superconducting properties of MgB2			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1092	C.H. Cheng,Y. Yang,C. Ke,H.T. Lin		
152385	SSS0121058	O2-annealed sample. O-content by iodometric titration.	(Cu,Tl,Li)Ba2Ca2Cu3O10	Tl0.25Li0.25Ba2Ca2Cu3.5O7.955	Tl	0.25	Li	0.25	Ba	2	Ca	2	Cu	3.5											O	10-z	7.955		2010																												Cu1223	P4/mmm																(Cu,Tl)-1223	K		117					117																																																																																																two step synthesize. (precursor +Tl2O3)					Superconductivity in (Cu0.5Tl0.25Li0.25)Ba2Ca2Cu3-ySiyO10-z samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Solid State Sci., 12(2010)1058	Nawazish A. Khan,Irfan Qasim,A.A. Khurram		
152386	SSS0121058	O2-annealed sample. O-content by iodometric titration.	(Cu,Tl,Li)Ba2Ca2(Cu,Si)3O10	Tl0.25Li0.25Ba2Ca2Cu3Si0.5O7.835	Tl	0.25	Li	0.25	Ba	2	Ca	2	Cu	3	Si	0.5									O	10-z	7.835		2010																												Cu1223	P4/mmm																(Cu,Tl)-1223	K		111					111																																																																																																two step synthesize. (precursor +Tl2O3)					Superconductivity in (Cu0.5Tl0.25Li0.25)Ba2Ca2Cu3-ySiyO10-z samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Solid State Sci., 12(2010)1058	Nawazish A. Khan,Irfan Qasim,A.A. Khurram		
152387	SSS0121058	O2-annealed sample. O-content by iodometric titration.	(Cu,Tl,Li)Ba2Ca2(Cu,Si)3O10	Tl0.25Li0.25Ba2Ca2Cu2.5Si1O7.853	Tl	0.25	Li	0.25	Ba	2	Ca	2	Cu	2.5	Si	1									O	10-z	7.853		2010																												Cu1223	P4/mmm																(Cu,Tl)-1223	K		113					113																																																																																																two step synthesize. (precursor +Tl2O3)					Superconductivity in (Cu0.5Tl0.25Li0.25)Ba2Ca2Cu3-ySiyO10-z samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Solid State Sci., 12(2010)1058	Nawazish A. Khan,Irfan Qasim,A.A. Khurram		
152388	SSS0121058	O2-annealed sample. O-content by iodometric titration.	(Cu,Tl,Li)Ba2Ca2(Cu,Si)3O10	Tl0.25Li0.25Ba2Ca2Cu2.25Si1.25O7.719	Tl	0.25	Li	0.25	Ba	2	Ca	2	Cu	2.25	Si	1.25									O	10-z	7.719		2010																												Cu1223	P4/mmm																(Cu,Tl)-1223	K		99					99																																																																																																two step synthesize. (precursor +Tl2O3)					Superconductivity in (Cu0.5Tl0.25Li0.25)Ba2Ca2Cu3-ySiyO10-z samples			Materials Science Laboratory, Department of Physics, Quaid-i-Azam University, Islamabad, Pakistan	Solid State Sci., 12(2010)1058	Nawazish A. Khan,Irfan Qasim,A.A. Khurram		
152389	SSC1501364		Ti2InN	Ti2In1N1	Ti	2	In	1	N	1																			2010																										ABC2			P6<3>/mmc		A	3.074		13.975												K			7.3			1.3	7.3										18	Oe	M-H curve				70			1.8	T	resistivity, GL theory approx.	10.8												MHC152389		A	from Hc2	55																																																								TiN,Ti,In		mixture - sealed in quartz ampoule under Ar - heat(900C,24h) repeat - heat(900C,10h, 130bar-Ar)					Superconductivity at 7.3 K in Ti2InN			Departamento de Engenharia de Materiais, Escola de Engenharia de Lorena - USP, P.O. BOX 116, Lorena   SP, 12600-970, Brazil	Solid State Commun., 150(2010)1364	A.D. Bortolozo,G. Serrano,A. Serquis,D. Rodrigues Jr.,C.A.M. dos Santos,Z. Fisk,A.J.S. Machado		
152390	PHC4700986	K-content not given. Optimal concentration. natural Fe<55.85> Tc=37.76, F<54> Tc=37.51.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2010																										AB2C2		ThCr2Si2																		K			37.76				37.76						-0.18	Fe		-0.19																																																																																												Iron isotope effect on Tc in optimally-doped (Ba,K)Fe2As2 (Tc = 38 K) and SmFeAsO1-y (Tc = 54 K) superconductors			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 470(2010)986	P.M. Shirage,K. Kihou,K. Miyazawa,C.H. Lee,H. Kito,Y. Yoshida,H. Eisaki,Y. Tanaka,A.Iyo		
152391	PHC4700986	Tc depends on O-content.	SmOzFeAs	Sm1Fe1As1O1-z	Sm	1	Fe	1	As	1															O	1-z			2010																										ABCD		oxypnictide																		K			53.8				53.8						-0.02	Fe		-0.01																																																																																												Iron isotope effect on Tc in optimally-doped (Ba,K)Fe2As2 (Tc = 38 K) and SmFeAsO1-y (Tc = 54 K) superconductors			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 470(2010)986	P.M. Shirage,K. Kihou,K. Miyazawa,C.H. Lee,H. Kito,Y. Yoshida,H. Eisaki,Y. Tanaka,A.Iyo		
152392	PHC4700989	using nano-sized SmF3	Sm(O,F)FeAs	Sm1Fe1As1F0.05O0.95	Sm	1	Fe	1	As	1	F	0.05													O	0.95		1	2010																										ABCD		oxypnictide			A	3.9355		8.4883												K				39			39																																																																																															1	mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1100C,36h, in Ar)					Low temperature preparation and superconductivity of F-doped SmFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)989	Y.L.Chen,Y.J.Chi,C.H.Cheng,Y.Yang,L.Wang,Y.C.Li,Y.Zhang,Y.Zhao		
152393	PHC4700989	using nano-sized SmF3	Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9		1	2010																										ABCD		oxypnictide			A	3.9332		8.4823												K				47			47																																																																																															1	mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1100C,36h, in Ar)					Low temperature preparation and superconductivity of F-doped SmFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)989	Y.L.Chen,Y.J.Chi,C.H.Cheng,Y.Yang,L.Wang,Y.C.Li,Y.Zhang,Y.Zhao		
152394	PHC4700989	using nano-sized SmF3	Sm(O,F)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		1	2010																										ABCD		oxypnictide			A	3.9309		8.4768												K				49			49																																																																																															1	mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1100C,36h, in Ar)					Low temperature preparation and superconductivity of F-doped SmFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)989	Y.L.Chen,Y.J.Chi,C.H.Cheng,Y.Yang,L.Wang,Y.C.Li,Y.Zhang,Y.Zhao		
152395	PHC4700989	using nano-sized SmF3	Sm(O,F)FeAs	Sm1Fe1As1F0.3O0.7	Sm	1	Fe	1	As	1	F	0.3													O	0.7		1	2010																										ABCD		oxypnictide			A	3.9308		8.4781												K				53.56			53.56																																																																																															1	mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1100C,36h, in Ar)					Low temperature preparation and superconductivity of F-doped SmFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)989	Y.L.Chen,Y.J.Chi,C.H.Cheng,Y.Yang,L.Wang,Y.C.Li,Y.Zhang,Y.Zhao		
152396	PHC4700989		Sm(O,F)FeAs	Sm1Fe1As1F0.6O0.6	Sm	1	Fe	1	As	1	F	0.6													O	0.6		1	2010																										ABCD		oxypnictide																		K				55			55																																																																																															1	mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1100C,36h, in Ar)					Low temperature preparation and superconductivity of F-doped SmFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)989	Y.L.Chen,Y.J.Chi,C.H.Cheng,Y.Yang,L.Wang,Y.C.Li,Y.Zhang,Y.Zhao		
152397	PRB078060504	T<SDW> = 150 K from R(T).	LaONiAs	La1Ni1As1O1	La	1	Ni	1	As	1															O	1			2008																										ABCD		oxypnictide	P4/nmm		A	4.119		8.18											ZrCuSiAs	K			2.75				2.75																									2			2.36																																																															RH152397			NiO,N,La,As,LaF3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1150C, 50h)					Strong-coupling superconductivity in the nickel-based oxypnictide LaNiAsO1-xFx			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 78(2008)060504	Zheng Li,Gengfu Chen,Jing Dong,Gang Li,Wanzheng Hu,Dan Wu,Shaokui Su,Ping Zheng,Tao Xiang,Nanlin Wang,Jianlin Luo		
152398	PRB078060504	lattice term in SP (beta) = 0.808 mJ/mol.K4.	La(O,F)NiAs	La1Ni1As1F0.1O0.9	La	1	Ni	1	As	1	F	0.1													O	0.9			2008																										ABCD		oxypnictide	P4/nmm		A	4.115		8.169											ZrCuSiAs	K			3.8			0.05	3.8	TC152398									84										T	resistivity, GL theory approx.	4.6			1			3.08																												mJ/mol.K2	4.75																																		RH152398			NiO,N,La,As,LaF3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1150C, 50h)					Strong-coupling superconductivity in the nickel-based oxypnictide LaNiAsO1-xFx			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 78(2008)060504	Zheng Li,Gengfu Chen,Jing Dong,Gang Li,Wanzheng Hu,Dan Wu,Shaokui Su,Ping Zheng,Tao Xiang,Nanlin Wang,Jianlin Luo		
152399	PHC4701077	not SC, T<SDW> = 130 K.	GdOFeAs	Gd1Fe1As1O1	Gd	1	Fe	1	As	1															O	1			2010																										ABCD		oxypnictide			A	3.9214		8.4661											ZrCuSiAs	K																																																																																																					GdAs,Fe,Ir,Fe2O3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1200C,72h, in Ar) - FC to RT					Superconductivity and magnetism in Ir-doped GdFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1077	Y.J.Cui,Y.L.Chen,C.H.Cheng,Y.Yang,J.Jiang,Y.Z.Wang,Y.Zhang,Y.Zhao		
152400	PHC4701077	R not to zero.	GdO(Fe,Ir)As	Gd1Fe0.95Ir0.05As1O1	Gd	1	Fe	0.95	Ir	0.05	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9227		8.4415											ZrCuSiAs	K			0				0																																																																																														GdAs,Fe,Ir,Fe2O3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1200C,72h, in Ar) - FC to RT					Superconductivity and magnetism in Ir-doped GdFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1077	Y.J.Cui,Y.L.Chen,C.H.Cheng,Y.Yang,J.Jiang,Y.Z.Wang,Y.Zhang,Y.Zhao		
152401	PHC4701077		GdO(Fe,Ir)As	Gd1Fe0.8Ir0.2As1O1	Gd	1	Fe	0.8	Ir	0.2	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9339		8.4007											ZrCuSiAs	K			18.9	17.6			17.6	TC152401																			T	resistivity, WHH	24							T/K	resistivity	1.9			HC152401																																																												GdAs,Fe,Ir,Fe2O3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1200C,72h, in Ar) - FC to RT					Superconductivity and magnetism in Ir-doped GdFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1077	Y.J.Cui,Y.L.Chen,C.H.Cheng,Y.Yang,J.Jiang,Y.Z.Wang,Y.Zhang,Y.Zhao		
152402	PHC4701077		GdO(Fe,Ir)As	Gd1Fe0.7Ir0.3As1O1	Gd	1	Fe	0.7	Ir	0.3	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9413		8.3593											ZrCuSiAs	K			11.6				11.6	TC152401																																																																																													GdAs,Fe,Ir,Fe2O3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1200C,72h, in Ar) - FC to RT					Superconductivity and magnetism in Ir-doped GdFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1077	Y.J.Cui,Y.L.Chen,C.H.Cheng,Y.Yang,J.Jiang,Y.Z.Wang,Y.Zhang,Y.Zhao		
152403	PHC4701077	R not to zero.	GdO(Fe,Ir)As	Gd1Fe0.67Ir0.33As1O1	Gd	1	Fe	0.67	Ir	0.33	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9449		8.344											ZrCuSiAs	K			0				0																																																																																														GdAs,Fe,Ir,Fe2O3		mixture - pellet - wrapped(Ta-foil) - sealed in quartz tube) - ANN(1200C,72h, in Ar) - FC to RT					Superconductivity and magnetism in Ir-doped GdFeAsO			Key Laboratory of Magnetic Levitation Technologies and Maglev Trains (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 470(2010)1077	Y.J.Cui,Y.L.Chen,C.H.Cheng,Y.Yang,J.Jiang,Y.Z.Wang,Y.Zhang,Y.Zhao		
152404	PRB082132502	Tc defined as mid of SUS. hydrostatic P: He-gas(P<0.6 GPa) and DAC (P<32 GPa).  Tc < 2K for P > 20 GPa. First order phase transition at about 10 GPa.	CaC6	C6Ca1	C	6	Ca	1																					2010									2.53																	AB6		GIC			A	4.33		13.57												K				11.48			11.48	MTC152404		K/GPa	0.39																																																																																												heat(350C,10d) using HOPG(highly oriented pyrolitic graphite.					Superconductivity for CaC6 to 32 GPa hydrostatic pressure			Department of Physics, Washington University, CB 1105, One Brookings Dr., Saint Louis, Missouri 63130, USA	Phys.Rev.B, 82(2010)132502	M. Debessai,J. J. Hamlin,J. S. Schilling,D. Rosenmann,D. G. Hinks,H. Claus		
152405	PRL105157001	P-induced SC. P<crit> = 5 GPa. Tc defined as 0.9Rn. Tc(max) = 1.4 K (9.3GPa). values of SC properties are for P = 9.3 GPa.	SnO	Sn1O1	Sn	1																			O	1			2010																										AB																			alpha-PbO	K			1.4		0		1.4	TC152405		K/GPa	0.28																T	resistivity, extrapolation	0.58												HC152405		A	from Hc2	240																																																										single phase sample obtained from Alfa Aesar					Superconductivity in SnO: A Nonmagnetic Analog to Fe-Based Superconductors?			II. Physikalisches Institut, Universitat zu Koln, Zulpicher Strase 77, D-50937 Koln, Germany	Phys.Rev.Lett., 105(2010)157001	M. K. Forthaus,K. Sengupta,O. Heyer,N. E. Christensen,A. Svane,K. Syassen,D. I. Khomskii,T. Lorenz,M. M. Abd-Elmeguid		
152406	PRB082134520	RRR = 1.4. GL parameter = 13. (dC/gamma*Tc) = 1.7.	YRh2Sn	Y1Rh2Sn1	Y	1	Rh	2	Sn	1																			2010																										ABC2		Heusler	Fm3[-]m		A	6.7139													Cu2MnAl, L2<1>	K		4.1				0.5	4.1											Oe	M-H curve		98						T	resistivity, WHH	1.26												MHC152406		A	from Hc2	163			A	from Hc1	2070			meV	0.7	4	14							mJ/mol.K2	8.55	SP-heat	219	SP-heat																																				arc-melting. ANN(750C,1w)					Superconductivity in the Rh-based Heusler family MRh2Sn			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)134520	T. Klimczuk,K. Gofryk,C. H. Wang,J. M. Allred,F. Ronning,W. Sadowski,J.-C. Griveau,E. Colineau,D. Safarik,J. D. Thompson,R. J. Cava		
152407	PRB082134520	quenched to -13 C brine. RRR = 2.4. GL parameter = 8. (dC/gamma*Tc) = 1.49.	LuRh2Sn	Lu1Rh2Sn1	Lu	1	Rh	2	Sn	1																			2010																										ABC2		Heusler	Fm3[-]m		A	6.6417													Cu2MnAl, L2<1>	K		2.9					2.9											Oe	M-H curve		75						T	resistivity, WHH	0.5														A	from Hc2	257			A	from Hc1	2170			meV	0.44	3.6	14							mJ/mol.K2	6.74	SP-heat	228	SP-heat																																				arc-melting. ANN(750C,1w)					Superconductivity in the Rh-based Heusler family MRh2Sn			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)134520	T. Klimczuk,K. Gofryk,C. H. Wang,J. M. Allred,F. Ronning,W. Sadowski,J.-C. Griveau,E. Colineau,D. Safarik,J. D. Thompson,R. J. Cava		
152408	PRB082134520	quenched to -13 C brine. RRR = 21.	ScRh2Sn	Sc1Rh2Sn1	Sc	1	Rh	2	Sn	1																			2010																										ABC2		Heusler	Fm3[-]m		A	6.5079													Cu2MnAl, L2<1>	K		2					2																				T	resistivity, WHH	0.3														A	from Hc2	330								meV	0.27	3.2	14							mJ/mol.K2	6.57	SP-heat	282	SP-heat																																				arc-melting. ANN(750C,1w)					Superconductivity in the Rh-based Heusler family MRh2Sn			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)134520	T. Klimczuk,K. Gofryk,C. H. Wang,J. M. Allred,F. Ronning,W. Sadowski,J.-C. Griveau,E. Colineau,D. Safarik,J. D. Thompson,R. J. Cava		
152409	PRB082140507	nominal/ Sr:V:Fe(III)-oxide:As-oxide = 20:11:5:5.  SIN(1323 K, 60h)	Sr2VO3FeAs	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3			2010																												22426			A	3.9458		15.731												K			33				33																																																																																																					Possible magnetic order and suppression of superconductivity by V doping in Sr2VO3FeAs			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 82(2010)140507	Marcus Tegel,Tanja Schmid,Tobias Sturzer,Masamitsu Egawa,Yixi Su,Anatoliy Senyshyn,Dirk Johrendt		
152410	PRB082140507	not SC.  nomonal/ Sr:V:Fe(III)-oxide:As-oxide:V-oxide = 100:54:20:25:3.  SC sensitive to V impurity in FeAs layer.	Sr2VO3(Fe,V)As	Sr2V1.07Fe0.93As1O3	Sr	2	V	1.07	Fe	0.93	As	1													O	3			2010																												22426			A	3.9338		15.731												K					4																																																																																																							Possible magnetic order and suppression of superconductivity by V doping in Sr2VO3FeAs			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 82(2010)140507	Marcus Tegel,Tanja Schmid,Tobias Sturzer,Masamitsu Egawa,Yixi Su,Anatoliy Senyshyn,Dirk Johrendt		
152411	PRB082144118	bulk modulus = 57.7 GPa for 0 < P < 16.7 GPa. P-dependence of lattice parameter shown in MTC152411 with Tc(P).	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2010																		GPa		57.7						AB2C2		ThCr2Si2			A	3.9635		13.022												K			22				22	MTC152411																																																																																															FeAs flux method					Collapsed tetragonal phase and superconductivity of BaFe2As2 under high pressure			Department of Physics, University of Alabama at Birmingham (UAB), Birmingham, Alabama 35294, USA	Phys.Rev.B, 82(2010)144118	Walter Uhoya,Andrew Stemshorn,Georgiy Tsoi,Yogesh K. Vohra,Athena S. Sefat,Brian C. Sales,Kevin M. Hope,Samuel T. Weir		
152412	STAM007S22	( 111)-oriented films. B-concentration estimated to be n=6 E+21 /cm3 by tunneling(STM/STS). energy gap at 0.47 K.	B-doped C	C1	C	1																						4	2006																											3	diamond	Pmmn	59	A	4.6729	2.8702	4.0792												K		5.4					5.4																																														meV	0.87	3.7	1																																															oriented films grown by MPCVD. ANN(400C, in UHV)					Scanning tunneling microscopy and spectroscopy studies of superconducting boron-doped diamond films			Institute for Materials Research, Tohoku University, Sendai 980-8577, Japan	Sci.Tech.Adv.Mat., 7(2006)S22	Terukazu Nishizaki,Yoshihiko Takano,Masanori Nagao,Tomohiro Takenouchi,Hiroshi Kawarada,Norio Kobayashi		
152413	PRB082144532	RRR = 22 (R//b-axis). (dC/gamma*Tc) = 1.32. Thermodynamic Hc(0) = 153 Oe. GL-parameter = 2. Two gaps( higher in TBL. lower -[gapene]= 2.5.	OsB2	B2Os1	B	2	Os	1																				3	2010																										AB2																				K	2.14		2.2				2.17																				Oe		186														A	from Hc2	1330			A		3000					3.8								mJ/mol.K2	1.95	SP-heat	539	SP-heat											uOhm.cm								1.55																	OsB2 by arc-melting.  heat(1450C) - cool to 1020 C (2C/h)					Multigap superconductivity and Shubnikov-de Haas oscillations in single crystals of the layered boride OsB2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)144532	Yogesh Singh,C. Martin,S. L. Bud'ko,A. Ellern,R. Prozorov,D. C. Johnston		
152414	PRB082144518	[gamma] estimated from (dC/Tc)=17 mJ/mol.K and BCS value of 1.43.	Sr(Fe,Pt)2As2	Sr1Fe1.84Pt0.16As2	Sr	1	Fe	1.84	Pt	0.16	As	2																	2010																										AB2C2		ThCr2Si2			A			12.322												K			16				16	MTC152414																												T/K	resistivity			3.16	MHC152414																						mJ/mol.K2	12	BCS																																						self-flux method. mixture - in alumina crucible - heat(1150C) - cool (2C/h)					Superconductivity and magnetism in platinum-substituted SrFe2As2 single crystals			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 82(2010)144518	Kevin Kirshenbaum,Shanta R. Saha,Tyler Drye,Johnpierre Paglione		
152415	PRB082144527	[penet] by muon-SR. Hc2 defined as Tc(zero). Two gaps, large gap in DB, small gap(0) = 0.15 meV , (2d/kTc) = 1.4	RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2																		K		2.52					2.52																				T	resistivity. extrapolation	2.6												MHC152415							A	muon-SR	2670			meV	0.49	4.5	16																																																				Microscopic study of the superconducting state of the iron pnictide RbFe2As2 via muon spin rotation			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 82(2010)144527	Z. Shermadini,J. Kanter,C. Baines,M. Bendele,Z. Bukowski,R. Khasanov,H.-H. Klauss,H. Luetkens,H. Maeter,G. Pascua,B. Batlogg,A. Amato		
152416	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.7K0.3Fe1.66Co0.34As2	Ba	0.7	K	0.3	Fe	1.66	Co	0.34	As	2														3	2010																										AB2C2		ThCr2Si2																		K		12					12																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152417	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.7K0.3Fe1.72Co0.28As2	Ba	0.7	K	0.3	Fe	1.72	Co	0.28	As	2														3	2010																										AB2C2		ThCr2Si2			A	3.913		13.12												K		12					12																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152418	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.95K0.05Fe1.782Co0.212As2	Ba	0.95	K	0.05	Fe	1.782	Co	0.212	As	2														3	2010																										AB2C2		ThCr2Si2																		K		16					16																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152419	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.86K0.14Fe1.68Co0.32As2	Ba	0.86	K	0.14	Fe	1.68	Co	0.32	As	2														3	2010																										AB2C2		ThCr2Si2																		K		11					11																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152420	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.82K0.18Fe1.654Co0.346As2	Ba	0.82	K	0.18	Fe	1.654	Co	0.346	As	2														3	2010																										AB2C2		ThCr2Si2																		K		11					11																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152421	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.805K0.195Fe1.738Co0.262As2	Ba	0.805	K	0.195	Fe	1.738	Co	0.262	As	2														3	2010																										AB2C2		ThCr2Si2																		K		14					14																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152422	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.694K0.306Fe1.826Co0.174As2	Ba	0.694	K	0.306	Fe	1.826	Co	0.174	As	2														3	2010																										AB2C2		ThCr2Si2																		K		18					18																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152423	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.66K0.34Fe1.8Co0.2As2	Ba	0.66	K	0.34	Fe	1.8	Co	0.2	As	2														3	2010																										AB2C2		ThCr2Si2																		K		19					19																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152424	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.68K0.32Fe1.954Co0.046As2	Ba	0.68	K	0.32	Fe	1.954	Co	0.046	As	2														3	2010																										AB2C2		ThCr2Si2																		K		35					35																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152425	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.511K0.489Fe1.772Co0.228As2	Ba	0.511	K	0.489	Fe	1.772	Co	0.228	As	2														3	2010																										AB2C2		ThCr2Si2																		K		22					22																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152426	PRB082184510		(Ba,K)(Fe,Co)2As2	Ba0.49K0.51Fe1.79Co0.21As2	Ba	0.49	K	0.51	Fe	1.79	Co	0.21	As	2														3	2010																										AB2C2		ThCr2Si2																		K		15					15																																																																																														Ba,K,FeAs,CoAs		(mixture in alumina) - (sealed in quartz tube, Ar) - heat(1273 K, 2h) - slow cool to 1073 K(24h) - Q to RT					Transition from antiferromagnetism to superconductivity in the compensated metallic state of Ba1-xKx(Fe1-yCoy)2As2			Institute for Solid State Physics, University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 82(2010)184510	Shunpei Suzuki,Kenya Ohgushi,Yoko Kiuchi,Yutaka Ueda		
152427	SSC1502248	Tc from R<ab>. T<CDW> = 96.2 K. lattice term in SP = 0.77 mJ/mol.K4	2H-NixTaSe2	Ni0.02Ta1Se2	Ni	0.02	Ta	1	Se	2																		3	2010																												2H-TaS2			A			12.733												K	2.58		2.79	2.5			2.5																																																								mJ/mol.K2	8.13	SP-heat	196.8	SP-heat																																				stoichiometric polycrystals by solid state reaction. Then, zone melting					Growth and superconductivity of 2H-Ni0.02TaSe2 single crystals			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Solid State Commun., 150(2010)2248	L.J. Li,Y.P. Sun,X.D. Zhu,B.S. Wang,X.B. Zhu,Z.R. Yang,W.H. Song		
152428	SSC1502248	T<CDW> = 115.5 K (incommensulate) from SP-heat. T<CDW> = 110.5 K (commensulate)  lattice term in SP = 0.64 mJ/mol.K4	TaSe2	Se2Ta1	Se	2	Ta	1																				3	2010																										AB2		2H-TaS2			A			12.71												K		0.14					0.14																																																								mJ/mol.K2	6.83	SP-heat	208	SP-heat																																				stoichiometric polycrystals by solid state reaction. Then, zone melting					Growth and superconductivity of 2H-Ni0.02TaSe2 single crystals			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Solid State Commun., 150(2010)2248	L.J. Li,Y.P. Sun,X.D. Zhu,B.S. Wang,X.B. Zhu,Z.R. Yang,W.H. Song		
152429	PHC4701029	d nearly 800 A.	NdxCuO4	Nd1.4Cu1O4	Nd	1.4	Cu	1																	O	4		4	2010																												T'			A	3.9437		12.124												K	26.3		29.4				27.85	TC152429																																																																						mOhm.cm											0.985														MOD method using Nd- and Cu-naphthenate solutions. spin coated on SrTiO3(001) substrates. Finally films reduced in vac(<E-4 Torr)					Material characterization of superconducting T'-Nd2CuO4 films synthesized by metal organic decomposition			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1029	O. Matsumoto,A. Tsukada,H. Yamamoto,T. Manabe,M. Naito		
152430	PHC4701029	d nearly 800 A.	NdxCuO4	Nd1.7Cu1O4	Nd	1.7	Cu	1																	O	4		4	2010																												T'			A			12.121												K	29.1		32.3				30.7																																																																							mOhm.cm											0.828														MOD method using Nd- and Cu-naphthenate solutions. spin coated on SrTiO3(001) substrates. Finally films reduced in vac(<E-4 Torr)					Material characterization of superconducting T'-Nd2CuO4 films synthesized by metal organic decomposition			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1029	O. Matsumoto,A. Tsukada,H. Yamamoto,T. Manabe,M. Naito		
152431	PHC4701029	d nearly 800 A.	NdxCuO4	Nd1.8Cu1O4	Nd	1.8	Cu	1																	O	4		4	2010																												T'			A	3.9449		12.127												K	29.8		32.8				31.3																																																																							mOhm.cm											0.878														MOD method using Nd- and Cu-naphthenate solutions. spin coated on SrTiO3(001) substrates. Finally films reduced in vac(<E-4 Torr)					Material characterization of superconducting T'-Nd2CuO4 films synthesized by metal organic decomposition			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1029	O. Matsumoto,A. Tsukada,H. Yamamoto,T. Manabe,M. Naito		
152432	PHC4701029	d nearly 800 A.	NdxCuO4	Nd2Cu1O4	Nd	2	Cu	1																	O	4		4	2010																												T'			A	3.9429		12.12												K	30.6		33.4				32																																																																							mOhm.cm											0.77														MOD method using Nd- and Cu-naphthenate solutions. spin coated on SrTiO3(001) substrates. Finally films reduced in vac(<E-4 Torr)					Material characterization of superconducting T'-Nd2CuO4 films synthesized by metal organic decomposition			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1029	O. Matsumoto,A. Tsukada,H. Yamamoto,T. Manabe,M. Naito		
152433	PHC4701029	d nearly 800 A.	NdxCuO4	Nd2.1Cu1O4	Nd	2.1	Cu	1																	O	4		4	2010																												T'			A	3.9427		12.125												K	28.7		32				30.35																																																																							mOhm.cm											0.706														MOD method using Nd- and Cu-naphthenate solutions. spin coated on SrTiO3(001) substrates. Finally films reduced in vac(<E-4 Torr)					Material characterization of superconducting T'-Nd2CuO4 films synthesized by metal organic decomposition			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1029	O. Matsumoto,A. Tsukada,H. Yamamoto,T. Manabe,M. Naito		
152434	PHC4701173	post-ANN(700C,96h)	(La,Sm)2CuO4	La1.9Sm0.1Cu1O4	La	1.9	Sm	0.1	Cu	1															O	4		4	2010																												T'																		K			25				25										4																																																																																						mixture(La2O3+Sm2O3) - added quickly into 400C-melt(CaOh,CuO) in flowing N2 - Q to RT					Low temperature synthesis and superconducting properties of polycrystalline T'-(La,Sm)2CuO4			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Nakacho, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1173	S. Ueda,S. Asai,M. Naito		
152435	PHC4701173	post-ANN(700C,48h)	(La,Sm)2CuO4	La1.7Sm0.3Cu1O4	La	1.7	Sm	0.3	Cu	1															O	4		4	2010																												T'																		K			25				25										30																																																																																						mixture(La2O3+Sm2O3) - added quickly into 400C-melt(CaOh,CuO) in flowing N2 - Q to RT					Low temperature synthesis and superconducting properties of polycrystalline T'-(La,Sm)2CuO4			Department of Applied Physics, Tokyo University of Agriculture and Technology, 2-24-16 Nakacho, Koganei, Tokyo 184-8588, Japan	Physica C, 470(2010)1173	S. Ueda,S. Asai,M. Naito		
152436	PHC4701916	Amorphous CaCuOx coating films. C-content not given. structural analysis shows (Cu,C)-1201 structure.	(Cu,C)-1201	Ba2Cu1O4	Ba	2	Cu	1																	O	4		4	2010																												M1201																		K	47		60				53.5																																																																																																Films deposited on (100) of SrTiO3 at 450-530C by pulsed layser. target: BaCuyOz, reactive gas: O2+CO2+Ar.					Pulsed laser deposition synthesis of superconducting (Cu, C)Ba2CuOx thin films			National Institute of Advanced Industrial Science and Technology, Tosu 841-0052, Japan	Physica C, 470(2010)1916	K. Kikunaga,T. Yamamoto,Y. Tanaka,N. Kikuchi,K. Tokiwa,T. Watanabe,N. Terada		
152437	PHC4701916	Au coating films (deposited under P(CO2)=0.08 mTorr. C-content not given. structural analysis shows (Cu,C)-1201 structure.	(Cu,C)-1201	Ba2Cu1O4	Ba	2	Cu	1																	O	4		4	2010																												M1201																		K	41		44				42.5																																																																																																Films deposited on (100) of SrTiO3 at 450-530C by pulsed layser. target: BaCuyOz, reactive gas: O2+CO2+Ar.					Pulsed laser deposition synthesis of superconducting (Cu, C)Ba2CuOx thin films			National Institute of Advanced Industrial Science and Technology, Tosu 841-0052, Japan	Physica C, 470(2010)1916	K. Kikunaga,T. Yamamoto,Y. Tanaka,N. Kikuchi,K. Tokiwa,T. Watanabe,N. Terada		
152438	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.83Sr0.17Cu0.94Fe0.06O4	La	1.83	Sr	0.17	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7859		13.211												K				26.5			26.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152439	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.81Sr0.19Cu0.94Fe0.06O4	La	1.81	Sr	0.19	Cu	0.94	Fe	0.06													O	4		1	2010																												T																		K				28.6			28.6																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152440	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.79Sr0.21Cu0.94Fe0.06O4	La	1.79	Sr	0.21	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7832		13.222												K				2.8			2.8																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152441	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.77Sr0.23Cu0.94Fe0.06O4	La	1.77	Sr	0.23	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7802		13.228												K				30.5			30.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152442	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.75Sr0.25Cu0.94Fe0.06O4	La	1.75	Sr	0.25	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7778		13.231												K				30.5			30.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152443	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.73Sr0.27Cu0.94Fe0.06O4	La	1.73	Sr	0.27	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7758		13.238												K				32.5			32.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152444	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.71Sr0.29Cu0.94Fe0.06O4	La	1.71	Sr	0.29	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.774		13.244												K				32.5			32.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152445	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.69Sr0.31Cu0.94Fe0.06O4	La	1.69	Sr	0.31	Cu	0.94	Fe	0.06													O	4		1	2010																												T			A	3.7715		13.247												K				28.4			28.4																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152446	PHC4701920		(La,Sr)2(Cu,Fe)O4	La1.67Sr0.33Cu0.94Fe0.06O4	La	1.67	Sr	0.33	Cu	0.94	Fe	0.06													O	4		1	2010																												T																		K					4																																																																																																	1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152447	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.83Sr0.17Cu0.94Co0.06O4	La	1.83	Sr	0.17	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7837		13.185												K					4																																																																																																	1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152448	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.81Sr0.19Cu0.94Co0.06O4	La	1.81	Sr	0.19	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7837		13.192												K				31.8			31.8																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152449	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.79Sr0.21Cu0.94Co0.06O4	La	1.79	Sr	0.21	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7793		13.192												K				31.8			31.8																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152450	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.77Sr0.23Cu0.94Co0.06O4	La	1.77	Sr	0.23	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7761		13.197												K				32.5			32.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152451	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.75Sr0.25Cu0.94Co0.06O4	La	1.75	Sr	0.25	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7754		13.208												K				36.4			36.4																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152452	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.73Sr0.27Cu0.94Co0.06O4	La	1.73	Sr	0.27	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7729		13.211												K				34			34																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152453	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.71Sr0.29Cu0.94Co0.06O4	La	1.71	Sr	0.29	Cu	0.94	Co	0.06													O	4		1	2010																												T			A	3.7707		13.214												K				33			33																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152454	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.69Sr0.31Cu0.94Co0.06O4	La	1.69	Sr	0.31	Cu	0.94	Co	0.06													O	4		1	2010																												T																		K				31			31																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152455	PHC4701920		(La,Sr)2(Cu,Co)O4	La1.67Sr0.33Cu0.94Co0.06O4	La	1.67	Sr	0.33	Cu	0.94	Co	0.06													O	4		1	2010																												T																		K				29			29																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152456	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.83Sr0.17Cu0.94Ni0.06O4	La	1.83	Sr	0.17	Cu	0.94	Ni	0.06													O	4		1	2010																												T			A	5.3495		13.2006												K					4																																																																																																	1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152457	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.81Sr0.19Cu0.94Ni0.06O4	La	1.81	Sr	0.19	Cu	0.94	Ni	0.06													O	4		1	2010																												T																		K				26.4			26.4																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152458	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.79Sr0.21Cu0.94Ni0.06O4	La	1.79	Sr	0.21	Cu	0.94	Ni	0.06													O	4		1	2010																												T			A	5.3446		13.212												K				28.3			28.3																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152459	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.77Sr0.23Cu0.94Ni0.06O4	La	1.77	Sr	0.23	Cu	0.94	Ni	0.06													O	4		1	2010																												T			A	5.3389		13.211												K				31.5			31.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152460	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.75Sr0.25Cu0.94Ni0.06O4	La	1.75	Sr	0.25	Cu	0.94	Ni	0.06													O	4		1	2010																												T			A	5.336		13.22												K				36.5			36.5																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152461	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.73Sr0.27Cu0.94Ni0.06O4	La	1.73	Sr	0.27	Cu	0.94	Ni	0.06													O	4		1	2010																												T			A	5.3355		13.226												K				34.4			34.4																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152462	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.71Sr0.29Cu0.94Ni0.06O4	La	1.71	Sr	0.29	Cu	0.94	Ni	0.06													O	4		1	2010																												T																		K				30.4			30.4																																																																																															1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152463	PHC4701920		(La,Sr)2(Cu,Ni)O4	La1.69Sr0.31Cu0.94Ni0.06O4	La	1.69	Sr	0.31	Cu	0.94	Ni	0.06													O	4		1	2010																												T																		K					4																																																																																																	1	mixture - SIN(1000-1100C, 24h)					Superconductivity recurrence and charge carrier compensation effect in La2-xSrxCu0.94M0.06O4 (M = Fe, Co and Ni) system			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Physica C, 470(2010)1920	Junchao Lu,Li Pi,Shun Tan,Yuheng Zhang		
152464	PHC4701928	RRR = 5.8. (gap/k) = 18, gap = 1.6 meV. RH(220 K) = -3.9 E-9 m3/C.	Ce(O,F)(Fe,Co)As	Ce1Fe0.95Co0.05As1F0.1O0.9	Ce	1	Fe	0.95	Co	0.05	As	1	F	0.1											O	0.9		1	2010																												oxypnictide			A	3.9965		8.609												K			23.5				23.5																				T	resistivity, WHH	25.3							T/K	resistivity	1.56					A	from Hc2	36								meV	1.6																																																	two-step solod state reaction. mixture - pellet - wrapped in Ta foil - heat(1150C,48h, in silica tube)					Effects of simultaneous carrier doping in the charge reservoir and conducting layers of superconducting CeO0.9F0.1Fe1-xCoxAs			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)1928	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
152465	PHC4701928	RRR = 2.11.	Ce(O,F)(Fe,Co)As	Ce1Fe0.9Co0.1As1F0.1O0.9	Ce	1	Fe	0.9	Co	0.1	As	1	F	0.1											O	0.9		1	2010																												oxypnictide			A	3.9929		8.5939												K			9.8				9.8																																																																																																two-step solod state reaction. mixture - pellet - wrapped in Ta foil - heat(1150C,48h, in silica tube)					Effects of simultaneous carrier doping in the charge reservoir and conducting layers of superconducting CeO0.9F0.1Fe1-xCoxAs			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)1928	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
152466	PHC4701928	R not to zero down to 1.6 K.	Ce(O,F)(Fe,Co)As	Ce1Fe0.85Co0.15As1F0.1O0.9	Ce	1	Fe	0.85	Co	0.15	As	1	F	0.1											O	0.9		1	2010																												oxypnictide			A	3.9844		8.5919												K			4				4																																																																																																two-step solod state reaction. mixture - pellet - wrapped in Ta foil - heat(1150C,48h, in silica tube)					Effects of simultaneous carrier doping in the charge reservoir and conducting layers of superconducting CeO0.9F0.1Fe1-xCoxAs			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110 067, India	Physica C, 470(2010)1928	S.J. Singh,J. Prakash,S. Patnaik,A.K. Ganguli		
152467	NAT3390291	Tc defined as ac-SUS(on).	Ba(Pb,Sb)O3	Ba1Pb0.85Sb0.15O3	Ba	1	Pb	0.85	Sb	0.15															O	3		1	1989																												ABO3																		K				1.4			1.4																																																																																																solid state reaction					Superconductivity at 3.5 K in BaPb0.75Sb0.25O3: Why is Tc so low?				Nature, 339(1989)291	R.J.Cava,B.Batlogg,G.P.Espinosa,A.P.Ramirez,J.J.Krajewski,W.F.Peck Jr,L.W.Rupp Jr,A.S.Cooper		
152468	NAT3390291	Tc defined as ac-SUS(on).	Ba(Pb,Sb)O3	Ba1Pb0.8Sb0.2O3	Ba	1	Pb	0.8	Sb	0.2															O	3		1	1989																												ABO3																		K				1.7			1.7																																																																																																solid state reaction					Superconductivity at 3.5 K in BaPb0.75Sb0.25O3: Why is Tc so low?				Nature, 339(1989)291	R.J.Cava,B.Batlogg,G.P.Espinosa,A.P.Ramirez,J.J.Krajewski,W.F.Peck Jr,L.W.Rupp Jr,A.S.Cooper		
152469	NAT3390291	Tc defined as dc-SUS(on) at H=5 Oe.	Ba(Pb,Sb)O3	Ba1Pb0.75Sb0.25O3	Ba	1	Pb	0.75	Sb	0.25															O	3		3	1989																											2	ABO3			A	6.028		8.511												K				3.5			3.5																																																																																																single crystals grown by PbO-based flux method.					Superconductivity at 3.5 K in BaPb0.75Sb0.25O3: Why is Tc so low?				Nature, 339(1989)291	R.J.Cava,B.Batlogg,G.P.Espinosa,A.P.Ramirez,J.J.Krajewski,W.F.Peck Jr,L.W.Rupp Jr,A.S.Cooper		
152470	PRB0380225		Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		1	1988																												Tl2201	I4/mmm	139	A	3.866		23.239												K	83		90				86.5																																																																																														BaO2,Tl2O3,CuO	1	mixture - sealed in Au tube - heat(900C)					Structures of the superconducting oxides Tl2Ba2CuO6 and Bi2Sr2CuO6				Phys.Rev.B, 38(1988)225	C.C.Torardi,M.A.subramanian,J.C.Calabrese,J.Gopalakrishnan,E.M.McCarron,K.J.Morrissey,T.R.askew,R.B.Flippen,U.Chowdhry,A.W.Sleight		
152471	PRB080094523		(Sr,Ba)2CuOz	Sr1.84Ba0.16Cu1O3.4	Sr	1.84	Ba	0.16	Cu	1															O	3+z	3.4	1	2009																												T	I4/mmm		A	3.815		12.576												K				75			75																																																																																																high-T and high-P synthesis.					Out-of-plane effect on the superconductivity of Sr2-xBaxCuO3+d with Tc up to 98 K			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)094523	W. B. Gao,Q. Q. Liu,L. X. Yang,Y. Yu,F. Y. Li,C. Q. Jin,S. Uchida		
152472	PRB080094523	as-synthesized sample. Tc = 92K for after-ANN(200C in N2) sample.	(Sr,Ba)2CuOz	Sr1.68Ba0.32Cu1O3.4	Sr	1.68	Ba	0.32	Cu	1															O	3+z	3.4	1	2009																												T	I4/mmm		A	3.839		12.667												K				88			88																																																																																																high-T and high-P synthesis.					Out-of-plane effect on the superconductivity of Sr2-xBaxCuO3+d with Tc up to 98 K			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)094523	W. B. Gao,Q. Q. Liu,L. X. Yang,Y. Yu,F. Y. Li,C. Q. Jin,S. Uchida		
152473	PRB080094523	as-synthesized sample. not SC for after-ANN(150C in N2) sample.	(Sr,Ba)2CuOz	Sr1.4Ba0.6Cu1O3.4	Sr	1.4	Ba	0.6	Cu	1															O	3+z	3.4	1	2009																												T	I4/mmm		A	3.889		12.776												K				98			98																																																																																																high-T and high-P synthesis.					Out-of-plane effect on the superconductivity of Sr2-xBaxCuO3+d with Tc up to 98 K			Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 80(2009)094523	W. B. Gao,Q. Q. Liu,L. X. Yang,Y. Yu,F. Y. Li,C. Q. Jin,S. Uchida		
152474	PHC470S263	impurity < 10%. (dC/Tc) = 2.2 mJ/mol.K2	Sr2VO3-zFeAs	Sr2V1Fe1As1O2.9	Sr	2	V	1	Fe	1	As	1													O	3-z	2.9		2010																															A	3.93		15.67											STR=21311(tentative)	K			40				40										100																			T/K	resistivity	13.65			HC152474	resistivity																					mJ/mol.K2	14	SP-heat																																				SrAs,FeAs,V2O3,SrO,Fe	1	mixture - pellet - (sealed 9n silica tube, 0.2 bar Ar) - heat(1150C,40h) - slow cool to RT					Physical properties of the new superconducting system Sr2VO3-dFeAs (21311)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Physica C, 470(2010)S263	Hai-Hu Wen,Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Bing Shen,Bin Zeng		
152475	PHC470S263	impurity < 20%.	Sr2VO3-zFeAs	Sr2V1Fe1As1O2.5	Sr	2	V	1	Fe	1	As	1													O	3-z	2.5		2010																															A	3.93		15.67											STR=21311(tentative)	K			20				20										3.3																																																																																				SrAs,FeAs,V2O3,SrO,Fe	1	mixture - pellet - (sealed 9n silica tube, 0.2 bar Ar) - heat(1150C,40h) - slow cool to RT					Physical properties of the new superconducting system Sr2VO3-dFeAs (21311)			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Physica C, 470(2010)S263	Hai-Hu Wen,Xiyu Zhu,Fei Han,Gang Mu,Peng Cheng,Bing Shen,Bin Zeng		
152476	PHC470S541	Thermodynamic Hc(0) = 37.0 mT, GL-parameter = 16, (dC/gamma*Tc) = 1.84. Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	La3Rh4Sn13	La3Rh4Sn13	La	3	Rh	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.746													quasi-skutterudite, stannide	K		3.1					3.1											mT	Hc(0), GL theory	1.9							T	resistivity, GL fitting	0.82												MHC152476		nm	from Hc2	20			nm	Hc1, GL theory	373			meV	0.482	3.78	14							mJ/mol.K2	22.2	SP-heat	364	SP-heat																																									Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152477	PHC470S541	Thermodynamic Hc(0) = 37.1 mT, GL-parameter = 22, (dC/gamma*Tc) = 1.71. Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	La3Ir4Sn13	La3Ir4Sn13	La	3	Ir	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.755													quasi-skutterudite, stannide	K		2.5					2.5											mT	Hc(0), GL theory	2.7							T	resistivity, GL fitting	0.84												MHC152477		nm	from Hc2	19.8			nm	Hc1, GL theory	496			meV	0.44	3.61	14							mJ/mol.K2	19.2	SP-heat	381	SP-heat																																									Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152478	PHC470S541	Thermodynamic Hc(0) = 60.1 mT, GL-parameter = 29, (dC/gamma*Tc) = 1.78. Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	Sr3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.805													quasi-skutterudite, stannide	K		4.2					4.2											mT	Hc(0), GL theory	4.7							T	resistivity, GL fitting	2.5												MHC152478		nm	from Hc2	11.5			nm	Hc1, GL theory	363			meV	0.692	3.87	14							mJ/mol.K2	31	SP-heat	365	SP-heat																																									Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152479	PHC470S541	Thermodynamic Hc(0) = 78.2 mT, GL-parameter = 32, (dC/gamma*Tc) = 2.09. Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.807													quasi-skutterudite, stannide	K		5					5											mT	Hc(0), GL theory	9.7							T	resistivity, GL fitting	3.54												MHC152479		nm	from Hc2	9.65			nm	Hc1, GL theory	328			meV	0.87	4.08	14							mJ/mol.K2	39.3	SP-heat	345	SP-heat																																									Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152480	PHC470S541	Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	Ca3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.702													quasi-skutterudite, stannide	K		8.3					8.3																				T	resistivity, GL fitting	4												MHC152480		nm	from Hc2	9.11																																																															Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152481	PHC470S541	Hc2(0) using Hc(T)={(1-t^2)/(1+t^2)}Hc2(0)	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																			2010																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.709													quasi-skutterudite, stannide	K		6.8					6.8																				T	resistivity, GL fitting	6.01												MHC152481		nm	from Hc2	7.4																																																															Superconducting properties of R3T4Sn13 (R = La, Sr, Ca, T = Rh, Ir) with a quasi-skutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S541	H. Hayamizu,N. Kase,J. Akimitsu		
152482	PRB082174509	Tc from R(ab). gap from optical reflectance(ab-plasma) method. lower gap = 3.1 meV, (2*gap/kTc)=2.9. For higher one, see DB.	Ba(Fe,Co)2As2	Ba1Fe1.85Co0.15As2	Ba	1	Fe	1.85	Co	0.15	As	2																3	2010																										AB2C2		ThCr2Si2																		K		25				0.7	25																																									A	using plasma freq.= 5200cm(-1)	3000			meV	7.4	6.87	15																																															self-flux method					Optical properties of the iron arsenic superconductor BaFe1.85Co0.15As2			Department of Physics, The City College of New York, New York, New York 10031, USA	Phys.Rev.B, 82(2010)174509	J. J. Tu,J. Li,W. Liu,A. Punnoose,Y. Gong,Y. H. Ren,L. J. Li,G. H. Cao,Z. A. Xu,C. C. Homes		
152483	PHC470S539		Tm5Rh6Sn18	Tm5Rh6Sn18	Tm	5	Rh	6	Sn	18																		3	2010																										A5B6C18																				K		2.19					2.19																																																																																														Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152484	PHC470S539		(Tm,Y)5Rh6Sn18	Tm4Y1Rh6Sn18	Tm	4	Y	1	Rh	6	Sn	18																3	2010																										A5B6C18																				K		2.61					2.61	MTC152484																																																																																													Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152485	PHC470S539		(Tm,Y)5Rh6Sn18	Tm1.4Y3.6Rh6Sn18	Tm	1.4	Y	3.6	Rh	6	Sn	18																3	2010																										A5B6C18																				K		3.14					3.14	MTC152484																																																																																													Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152486	PHC470S539		Y5Rh6Sn18	Y5Rh6Sn18	Y	5	Rh	6	Sn	18																		3	2010																										A5B6C18																				K		3.14					3.14																																																																																														Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152487	PHC470S539		Tm5(Rh,Co)6Sn18	Tm5Rh4.8Co1.2Sn18	Tm	5	Rh	4.8	Co	1.2	Sn	18																3	2010																										A5B6C18																				K		1.97					1.97	MTC152488																																																																																													Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152488	PHC470S539		Tm5(Rh,Co)6Sn18	Tm5Rh3.6Co2.4Sn18	Tm	5	Rh	3.6	Co	2.4	Sn	18																3	2010																										A5B6C18																				K		1.57					1.57	MTC152488																																																																																													Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152489	PHC470S539		Tm5(Rh,Co)6Sn18	Tm5Rh2.4Co3.6Sn18	Tm	5	Rh	2.4	Co	3.6	Sn	18																3	2010																										A5B6C18																				K		1.27					1.27	MTC152488																																																																																													Tm(3N),Y(3N),Rh(3N),Co(3N),Sn(5N)		single crystals grown by Sn-flux method.  mixture - (sealed in quartz tube) - heat(1050C) - hold(3h) - cool to 200C(5C/h)					Substituted effects of superconducting and magnetic states in reentrant superconductor Tm5Rh6Sn18			Department of Physics and Mathematics, Aoyama-Gakuin University, Sagamihara, Kanagawa 229-8558, Japan	Physica C, 470(2010)S539	N. Kase,K. Wakui,H. Hayamizu,J. Akimitsu		
152490	PRB082180520	K:Fe:Se = 0.39:0.85:1 from chemical analysis. carrier from Hall constant at 70K.	K0.8Fe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																			2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9136		14.0367											KCo2Se2	K	27.2	28.3	30.1			1.3	28.3										60																																																																																		n/cm3	1760000000000000000000	Se(4N),Fe(3N)		mixture - alumina crucible in quartz tube - heat(973-1023K,30h) FC to RT					Superconductivity in the iron selenide KxFe2Se2 (0 =< x =<1.0)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 82(2010)180520	Jiangang Guo,Shifeng Jin,Gang Wang,Shunchong Wang,Kaixing Zhu,Tingting Zhou,Meng He,Xiaolong Chen		
152491	PRB082212504	Neel-T measured by muon-SR.	Fex(Se,Te)	Fe0.9Se0.25Te0.75	Fe	0.9	Se	0.25	Te	0.75																			2010								1.7																		AB			P4/nmm		A	3.8125		6.1699												K		9.7		11.5			9.7																																																																																																					Tuning the superconducting and magnetic properties of FeySe0.25Te0.75 by varying the iron content			Physik-Institut, Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 82(2010)212504	M. Bendele,P. Babkevich,S. Katrych,S. N. Gvasaliya,E. Pomjakushina,K. Conder,B. Roessli,A. T. Boothroyd,R. Khasanov,H. Keller		
152492	PRB082212504	Neel-T measured by muon-SR.	Fex(Se,Te)	Fe0.95Se0.25Te0.75	Fe	0.95	Se	0.25	Te	0.75																			2010								2.7																		AB			P4/nmm		A	3.8096		6.1524												K		8.5		10.6			8.5	MTC152492																																																																																																				Tuning the superconducting and magnetic properties of FeySe0.25Te0.75 by varying the iron content			Physik-Institut, Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 82(2010)212504	M. Bendele,P. Babkevich,S. Katrych,S. N. Gvasaliya,E. Pomjakushina,K. Conder,B. Roessli,A. T. Boothroyd,R. Khasanov,H. Keller		
152493	PRB082212504	Neel-T measured by muon-SR.	Fex(Se,Te)	Fe0.98Se0.25Te0.75	Fe	0.98	Se	0.25	Te	0.75																			2010								5																		AB																				K		6.5		8			6.5	MTC152492																																																																																																				Tuning the superconducting and magnetic properties of FeySe0.25Te0.75 by varying the iron content			Physik-Institut, Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 82(2010)212504	M. Bendele,P. Babkevich,S. Katrych,S. N. Gvasaliya,E. Pomjakushina,K. Conder,B. Roessli,A. T. Boothroyd,R. Khasanov,H. Keller		
152494	PRB082212504	Neel-T measured by muon-SR.	Fex(Se,Te)	Fe1.07Se0.25Te0.75	Fe	1.07	Se	0.25	Te	0.75																			2010								28																		AB																				K					1																																																																																																							Tuning the superconducting and magnetic properties of FeySe0.25Te0.75 by varying the iron content			Physik-Institut, Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 82(2010)212504	M. Bendele,P. Babkevich,S. Katrych,S. N. Gvasaliya,E. Pomjakushina,K. Conder,B. Roessli,A. T. Boothroyd,R. Khasanov,H. Keller		
152495	PRB082212506	grain size = 14*6*1 um3. hydrostatic-P. optimal O-content sample.	SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85	0.85		2010																												oxypnictide																		K		54.9					54.9	TC152495		K/GPa	-1.1																																																																																																	Effect of hydrostatic pressure on the superconducting transition temperature and superfluid density of SmFeAsO0.85 and PrFe0.925Co0.075AsO superconductors			National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 82(2010)212506	X. L. Dong,W. Lu,J. Yang,W. Yi,Z. C. Li,C. Zhang,Z. A. Ren,G. C. Che,L. L. Sun,F. Zhou,X. J. Zhou,Z. X. Zhao		
152496	PRB082212506	grain size = 20*20*1 um3. hydrostatic-P. optimal Co-content sample.	PrO(Fe,Co)As	Pr1Fe0.925Co0.075As1O1	Pr	1	Fe	0.925	Co	0.075	As	1													O	1			2010																												oxypnictide																		K		14.4					14.4	TC152496		K/GPa	0.92																																																																																																	Effect of hydrostatic pressure on the superconducting transition temperature and superfluid density of SmFeAsO0.85 and PrFe0.925Co0.075AsO superconductors			National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 82(2010)212506	X. L. Dong,W. Lu,J. Yang,W. Yi,Z. C. Li,C. Zhang,Z. A. Ren,G. C. Che,L. L. Sun,F. Zhou,X. J. Zhou,Z. X. Zhao		
152497	PRB082220502	Hc2 defined by SP-heat measurements.	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2010																										ABC5		HoCoGa5																		K		2.26					2.26																				T	SP-heat		11.7	5																																																																													Anomalous effect of doping on the superconducting state of CeCoIn5 in high magnetic fields			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)220502	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,A. D. Bianchi,Z. Fisk,J. D. Thompson		
152498	PRB082220502	Hc2 defined by SP-heat measurements.	CeCo(In,Cd)5	Ce1Co1In4.9945Cd0.0055	Ce	1	Co	1	In	4.9945	Cd	0.0055																3	2010																										ABC5		HoCoGa5																		K		2.23					2.23																				T	SP-heat		12.4	5.1																																																																													Anomalous effect of doping on the superconducting state of CeCoIn5 in high magnetic fields			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)220502	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,A. D. Bianchi,Z. Fisk,J. D. Thompson		
152499	PRB082220502	Hc2 defined by SP-heat measurements.	CeCo(In,Cd)5	Ce1Co1In4.989Cd0.011	Ce	1	Co	1	In	4.989	Cd	0.011																3	2010																										ABC5		HoCoGa5																		K		2.18					2.18																				T	SP-heat		12.8	5.16																																																																													Anomalous effect of doping on the superconducting state of CeCoIn5 in high magnetic fields			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)220502	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,A. D. Bianchi,Z. Fisk,J. D. Thompson		
152500	PRB082220502	Hc2 defined by SP-heat measurements. H// = H//[100], H/n = H//[001]	CeCo(In,Cd)5	Ce1Co1In4.9835Cd0.0165	Ce	1	Co	1	In	4.9835	Cd	0.0165																3	2010																										ABC5		HoCoGa5																		K		2.15					2.15																				T	SP-heat		12.5	5.22										MHC152500																																																																			Anomalous effect of doping on the superconducting state of CeCoIn5 in high magnetic fields			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)220502	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,A. D. Bianchi,Z. Fisk,J. D. Thompson		
152501	PRB082220502		CeCo(In,Sn)5	Ce1Co1In4.996Sn0.004	Ce	1	Co	1	In	4.996	Sn	0.004																3	2010																										ABC5		HoCoGa5																		K		2.21					2.21	MTC152501																																																																																																				Anomalous effect of doping on the superconducting state of CeCoIn5 in high magnetic fields			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 82(2010)220502	Y. Tokiwa,R. Movshovich,F. Ronning,E. D. Bauer,A. D. Bianchi,Z. Fisk,J. D. Thompson		
152502	PRB082180512	solubility of La is small under P=0. best condition for preparation: P = 2-4 GPa. Tc(on) do not depend on x for 0.2=<x=<0.5.	(Sr,La)Fe2As2	Sr0.6La0.4Fe2As2	Sr	0.6	La	0.4	Fe	2	As	2																	2010																										AB2C2		ThCr2Si2																		K	19		22				20.5										70																																																								uV/K	-12.5																											SrAs,LaAs,Fe2As	1	solid state reaction under high-P.  mixture - (sealed in Ta tube) - heat(1273K,2h,at P=2-4 GPa)					High-pressure synthesis of the indirectly electron-doped iron pnictide superconductor Sr1-xLaxFe2As2 with maximum Tc=22 K			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.B, 82(2010)180512	Yoshinori Muraba,Satoru Matsuishi,Sung-Wng Kim,Toshiyuki Atou,Osamu Fukunaga,Hideo Hosono		
152503	PRB082174513	RRR = 15.9. H//c-axis.	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2010																										ABC2D2		LuNi2B2C																		K	15.5		15.6				15.55																													T/K	SP-heat			0.433	MHC152503																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152504	PRB082174513	RRR = 14.2. H//c-axis	(Y,Gd)Ni2B2C	Y0.9Gd0.1Ni2B2C1	Y	0.9	Gd	0.1	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	12.4		12.6				12.5																													T/K	SP-heat			0.328	MHC152504																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152505	PRB082174513	RRR = 10.  H//c-axis	(Y,Gd)Ni2B2C	Y0.86Gd0.14Ni2B2C1	Y	0.86	Gd	0.14	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	10.15		10.8				10.475																													T/K	SP-heat			0.253	MHC152505																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152506	PRB082174513	RRR = 9.5.  H//c-axis	(Y,Gd)Ni2B2C	Y0.79Gd0.21Ni2B2C1	Y	0.79	Gd	0.21	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	7.58		8.04				7.81																													T/K	SP-heat			0.17	MHC152506																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152507	PRB082174513	RRR = 8.3.  H//c-axis	(Y,Gd)Ni2B2C	Y0.74Gd0.26Ni2B2C1	Y	0.74	Gd	0.26	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	5.51		6.36				5.935																													T/K	SP-heat			0.106	MHC152507																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152508	PRB082174513	RRR = 32.8.  H//c-axis. Hc2 defined as R=0.9Rn.	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2010																										ABC2D2		LuNi2B2C																		K	16		16.7				16.35																													T/K	SP-heat			0.438	MHC152508																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152509	PRB082174513	RRR = 10.5.  H//c-axis. Hc2 defined as R=0.9Rn.	(Lu,Gd)Ni2B2C	Lu0.945Gd0.055Ni2B2C1	Lu	0.945	Gd	0.055	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	12.96		13.6				13.28																													T/K	SP-heat			0.314	MHC152509																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152510	PRB082174513	RRR = 7.1.  H//c-axis. Hc2 defined as R=0.9Rn.	(Lu,Gd)Ni2B2C	Lu0.87Gd0.13Ni2B2C1	Lu	0.87	Gd	0.13	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	9.58		9.85				9.715																													T/K	SP-heat			0.278	MHC152510																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152511	PRB082174513	RRR = 5.6.  H//c-axis. Hc2 defined as R=0.9Rn.	(Lu,Gd)Ni2B2C	Lu0.81Gd0.19Ni2B2C1	Lu	0.81	Gd	0.19	Ni	2	B	2	C	1														3	2010																										ABC2D2		LuNi2B2C																		K	5.76		6.55				6.155																													T/K	SP-heat			0.174	MHC152511																																																														single crystals grown using Ni2B high temperature growth technique.					Evolution of ground state and upper critical field in R1-xGdxNi2B2C (R=Lu,Y): Coexistence of superconductivity and spin-glass state			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)174513	S. L. Bud'ko,V. G. Kogan,H. Hodovanets,S. Ran,S. A. Moser,M. J. Lampe,P. C. Canfield		
152512	NJP012073024	natural Fe(M=55.85 g/mol), <54>Fe(M=54.0 g/mol). tetra-to-ortho transition at 100K. at 5 K: Cmma, a=5.3343, b=5.3093, c=5.4879, vol=155.423 A3.	FeSe0.98	Fe1Se0.98	Fe	1	Se	0.98																					2010																										AB			P4/nmm		A	3.7698		5.5164											at 250 K	K				8.21			8.21						0.81	Fe	100	0.22																																																																																					Fe(3N),<54>Fe(4N),Se(5N)	1	solid state reaction					Iron isotope effect on the superconducting transition temperature and the crystal structure of FeSe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	New J.Phys., 12(2010)073024	R Khasanov,M Bendele,K Conder,H Keller,E Pomjakushina,V Pomjakushin		
152513	PRL105037004	optimum O-content sample(O-content not given). Tc depends on lattice parameter-a.	SmOFeAs	Sm1Fe1As1O0.85	Sm	1	Fe	1	As	1															O	0.85			2010																												oxypnictide			A	3.915														K				54			54	TC152513					-0.02	Fe	43																																																																																						Fe,Fe2O3,As,Sm(OH)3,SmAs	1	high-P synthesize.					Absence of an Appreciable Iron Isotope Effect on the Transition Temperature of the Optimally Doped SmFeAsO1-y Superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.Lett., 105(2010)037004	Parasharam M. Shirage,Kiichi Miyazawa,Kunihiro Kihou,Hijiri Kito,Yoshiyuki Yoshida,Yasumoto Tanaka,Hiroshi Eisaki,Akira Iyo		
152514	PRL105037004	H doped from Sm(OH)3.	Sm(O,H)FeAs	Sm1Fe1As1H0.3O0.6	Sm	1	Fe	1	As	1	H	0.3													O	0.6			2010																												oxypnictide																		K				51.4			51.4	TC152513																																																																																													Fe,Fe2O3,As,Sm(OH)3,SmAs	1	high-P synthesize.					Absence of an Appreciable Iron Isotope Effect on the Transition Temperature of the Optimally Doped SmFeAsO1-y Superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.Lett., 105(2010)037004	Parasharam M. Shirage,Kiichi Miyazawa,Kunihiro Kihou,Hijiri Kito,Yoshiyuki Yoshida,Yasumoto Tanaka,Hiroshi Eisaki,Akira Iyo		
152515	PRL105037004	H doped from Sm(OH)3.	Sm(O,H)FeAs	Sm1Fe1As1H0.12O0.77	Sm	1	Fe	1	As	1	H	0.12													O	0.77			2010																												oxypnictide																		K				54.2			54.2																																																																																														Fe,Fe2O3,As,Sm(OH)3,SmAs	1	high-P synthesize.					Absence of an Appreciable Iron Isotope Effect on the Transition Temperature of the Optimally Doped SmFeAsO1-y Superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.Lett., 105(2010)037004	Parasharam M. Shirage,Kiichi Miyazawa,Kunihiro Kihou,Hijiri Kito,Yoshiyuki Yoshida,Yasumoto Tanaka,Hiroshi Eisaki,Akira Iyo		
152516	PRL105037004		SmO0.8FeAs	Sm1Fe1As1O0.8	Sm	1	Fe	1	As	1															O	0.8			2010																												oxypnictide																		K				40.1			40.1																																																																																														Fe,Fe2O3,As,Sm(OH)3,SmAs	1	high-P synthesize.					Absence of an Appreciable Iron Isotope Effect on the Transition Temperature of the Optimally Doped SmFeAsO1-y Superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Phys.Rev.Lett., 105(2010)037004	Parasharam M. Shirage,Kiichi Miyazawa,Kunihiro Kihou,Hijiri Kito,Yoshiyuki Yoshida,Yasumoto Tanaka,Hiroshi Eisaki,Akira Iyo		
152517	PRB082220504	proton irradiation effect of Tc. under doped sample	Ba(Fe,Co)2As2	Ba1Fe1.91Co0.09As2	Ba	1	Fe	1.91	Co	0.09	As	2																3	2010																										AB2C2		ThCr2Si2																		K		15.1					15.1	MTC152517																																								A		2000																																																					FeAs/CoAs self-flux method. mixture in alumina crucible - sealed in silica tube - heat and keep(1150C,10h) - slow cool to 800C(5C/h)					Suppression of the critical temperature of superconducting Ba(Fe1-xCox)2As2 by point defects from proton irradiation			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)220504	Yasuyuki Nakajima,Toshihiro Taen,Yuji Tsuchiya,Tsuyoshi Tamegai,Hisashi Kitamura,Takeshi Murakami		
152518	PRB082220504	proton irradiation effect of Tc. optimum sample	Ba(Fe,Co)2As2	Ba1Fe1.85Co0.15As2	Ba	1	Fe	1.85	Co	0.15	As	2																3	2010																										AB2C2		ThCr2Si2			A			12.978												K		24.8					24.8	MTC152518																																								A		2000																																																					FeAs/CoAs self-flux method. mixture in alumina crucible - sealed in silica tube - heat and keep(1150C,10h) - slow cool to 800C(5C/h)					Suppression of the critical temperature of superconducting Ba(Fe1-xCox)2As2 by point defects from proton irradiation			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)220504	Yasuyuki Nakajima,Toshihiro Taen,Yuji Tsuchiya,Tsuyoshi Tamegai,Hisashi Kitamura,Takeshi Murakami		
152519	PRB082220504	proton irradiation effect of Tc. overdoped sample	Ba(Fe,Co)2As2	Ba1Fe1.774Co0.226As2	Ba	1	Fe	1.774	Co	0.226	As	2																3	2010																										AB2C2		ThCr2Si2																		K		12.8					12.8	MTC152519																																								A		2000																																																					FeAs/CoAs self-flux method. mixture in alumina crucible - sealed in silica tube - heat and keep(1150C,10h) - slow cool to 800C(5C/h)					Suppression of the critical temperature of superconducting Ba(Fe1-xCox)2As2 by point defects from proton irradiation			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 82(2010)220504	Yasuyuki Nakajima,Toshihiro Taen,Yuji Tsuchiya,Tsuyoshi Tamegai,Hisashi Kitamura,Takeshi Murakami		
152520	APL096072514		La(O,H)FeAs	La1Fe1As1H0.6O0.6	La	1	Fe	1	As	1	H	0.6													O	0.6		1	2010																												oxypnictide			A	3.9938		8.6898												K	34		38.5	35			35										56																																																																																				Fe,Fe2O3,As,La(Ce,Pr)As,La(OH)3		mixture(LaFeAsO1-xHx) - pellet heat(1100C,2h, P=3.5 GPa)					Possible hydrogen doping and enhancement of Tc  (=35 K) in a LaFeAsO-based superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett.,96(2010)072514	K. Miyazawa,S. Ishida,K. Kihou,P. M. Shirage,M. Nakajima,C. H. Lee,H. Kito,Y. Tomioka,T. Ito,H. Eisaki,H. Yamashita,H. Mukuda,K. Tokiwa,S. Uchida,A. Iyo		
152521	APL096072514		Ce(O,H)FeAs	Ce1Fe1As1H0.6O0.6	Ce	1	Fe	1	As	1	H	0.6													O	0.6		1	2010																												oxypnictide			A	3.974		8.5953												K	44.6		48	45.8			45.8																																																																																														Fe,Fe2O3,As,La(Ce,Pr)As,La(OH)3		mixture(LaFeAsO1-xHx) - pellet heat(1100C,2h, P=3.5 GPa)					Possible hydrogen doping and enhancement of Tc  (=35 K) in a LaFeAsO-based superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett.,96(2010)072514	K. Miyazawa,S. Ishida,K. Kihou,P. M. Shirage,M. Nakajima,C. H. Lee,H. Kito,Y. Tomioka,T. Ito,H. Eisaki,H. Yamashita,H. Mukuda,K. Tokiwa,S. Uchida,A. Iyo		
152522	APL096072514		Pr(O,H)FeAs	Pr1Fe1As1H0.6O0.6	Pr	1	Fe	1	As	1	H	0.6													O	0.6		1	2010																												oxypnictide			A	3.9522		8.5608												K	49.6		51.9	49.7			49.7																																																																																														Fe,Fe2O3,As,La(Ce,Pr)As,La(OH)3		mixture(LaFeAsO1-xHx) - pellet heat(1100C,2h, P=3.5 GPa)					Possible hydrogen doping and enhancement of Tc  (=35 K) in a LaFeAsO-based superconductor			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Lett.,96(2010)072514	K. Miyazawa,S. Ishida,K. Kihou,P. M. Shirage,M. Nakajima,C. H. Lee,H. Kito,Y. Tomioka,T. Ito,H. Eisaki,H. Yamashita,H. Mukuda,K. Tokiwa,S. Uchida,A. Iyo		
152523	JPS078034712	synthesized under P=3.5 GPa.	DyOxFeAs	Dy1Fe1As1O0.7	Dy	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.8748		8.345												K				37			37										53																																																																																						high-P synthesis. heat(1050-1150C, P=<5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152524	JPS078034712	synthesized under P43.5 GPa.	DyOxFeAs	Dy1Fe1As1O0.7	Dy	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.8668		8.3355												K				44			44										61																																																																																						high-P synthesis. heat(1050-1150C, P=<5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152525	JPS078034712	synthesized under P=5.5 GPa.	DyOxFeAs	Dy1Fe1As1O0.7	Dy	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.8625		8.3216												K	49.8	51.2	51.6	51.2			51.2										63																																																																																						high-P synthesis. heat(1050-1150C, P=<5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152526	JPS078034712	synthesized under P=5.5 GPa.	LaOxFeAs	La1Fe1As1O0.7	La	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	4.0257		8.719												K	26.2	28.4	29	27.8			28.4																																																																																																high-P synthesis. heat(1100-1150C, P=5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152527	JPS078034712	synthesized under P=5.5 GPa.	CeOxFeAs	Ce1Fe1As1O0.7	Ce	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.995		8.631												K	35.5	40.2	41.2	38.5			40.2																																																																																																high-P synthesis. heat(1100-1150C, P=5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152528	JPS078034712	synthesized under P=5.5 GPa.	PrOxFeAs	Pr1Fe1As1O0.7	Pr	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.9627		8.5721												K	46	48.5	49.2	48.1			48.5																																																																																																high-P synthesis. heat(1100-1150C, P=5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152529	JPS078034712	synthesized under P=5.5 GPa.	NdOxFeAs	Nd1Fe1As1O0.7	Nd	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.9432		8.529												K	52.1	53.7	54.3	53			53.7																																																																																																high-P synthesis. heat(1100-1150C, P=5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152530	JPS078034712	synthesized under P=5.5 GPa.	SmOxFeAs	Sm1Fe1As1O0.7	Sm	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.9218		8.4522												K	50.5	52.1	53.3	52.5			52.1																																																																																																high-P synthesis. heat(1100-1150C, P=5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152531	JPS078034712	synthesized under P=5.5 GPa.	GdOxFeAs	Gd1Fe1As1O0.7	Gd	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.8905		8.3928												K	52.4	53.6	54	53.5			53.6																																																																																																high-P synthesis. heat(1050-1150C, P=<5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152532	JPS078034712	synthesized under P=5.5 GPa.	TbOxFeAs	Tb1Fe1As1O0.7	Tb	1	Fe	1	As	1															O	0.7		1	2009																												oxypnictide			A	3.8753		8.3527												K	50.2	52.2	52.6	52.4			52.2																																																																																																high-P synthesis. heat(1050-1150C, P=<5.5 GPa)					Superconductivity above 50K in LnFeAsO1-y (Ln = Nd, Sm, Gd, Tb, and Dy) Synthesized by High-Pressure Technique			National Institute of Advanced Industrial Science and Technology, Tsukuba, Ibaraki 305-8568	J.Phys.Soc.Jpn, 78(2009)034712	Kiichi MIYAZAWA,Kunihiro KIHOU,Parasharam M. SHIRAGE,Chul-Ho LEE,Hijiri KITO,Hiroshi EISAKI,Akira IYO		
152533	SST023115005	impurity phaes: FeAs,CaFe2As2,Fe2As2Ca5(Al,Ti)3O9	Fe2As2Ca4(Al,Ti)2O6	Fe2As2Ca4Al1.34Ti0.66O6	Fe	2	As	2	Ca	4	Al	1.34	Ti	0.66											O	6		2	2010																											2		P4/nmm		A	3.77		15.4												K				12.5			12.5																																																																																																reaction(1000C,100h)					A new homologous series of iron pnictide oxide superconductors (Fe2As2)(Can+2(Al, Ti)nOy) (n = 2, 3, 4)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)115005	Hiraku Ogino,Kenji Machida,Akiyasu Yamamoto,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152534	SST023115005	impurity phaes: Fe2As2Ca6(Al,Ti)4O12	Fe2As2Ca5(Al,Ti)3O9	Fe2As2Ca5Al1.5Ti1.5O9	Fe	2	As	2	Ca	5	Al	1.5	Ti	1.5											O	9		2	2010																											2		P4mm		A	3.79		19												K				15			15																																																																																																reaction(1050C,100h)					A new homologous series of iron pnictide oxide superconductors (Fe2As2)(Can+2(Al, Ti)nOy) (n = 2, 3, 4)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)115005	Hiraku Ogino,Kenji Machida,Akiyasu Yamamoto,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152535	SST023115005	nearly single phase	Fe2As2Ca6(Al,Ti)4O12	Fe2As2Ca6Al1.32Ti2.68O12	Fe	2	As	2	Ca	6	Al	1.32	Ti	2.68											O	12		1	2010																											2		P4/nmm		A	3.815		22.68												K			39	36			36																																																																																																reaction(1100C,100h)					A new homologous series of iron pnictide oxide superconductors (Fe2As2)(Can+2(Al, Ti)nOy) (n = 2, 3, 4)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)115005	Hiraku Ogino,Kenji Machida,Akiyasu Yamamoto,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152536	APL097072506	SIN(1050C,72h). impurity phases: CaSc2O4, CaFe2As2	Fe2As2Ca4(Sc,Ti)3O7.5	Fe2As2Ca4Sc2.01Ti0.99O7.5	Fe	2	As	2	Ca	4	Sc	2.01	Ti	0.99											O	7.5			2010																													I4/mmm		A	3.922		33.56												K			33	31			31																																																																																														FeAs,CaO,Ti,TiO2,Sc2O3	1	solid state reaction. mixture - pellet - (sealed in quartz tube) - heat(1000-1200C,60-100h) - slow cool to RT					Homologous series of iron pnictide oxide superconductors  (Fe2As2)[Can+1(Sc,Ti)nOy]   (n=3,4,5) with extremely thick blocking layers			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656,	Appl.Phys.Lett., 97(2010)072506	Hiraku Ogino,Shinya Sato,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152537	APL097072506	SIN(1100C,72h)	Fe2As2Ca5(Sc,Ti)4O710	Fe2As2Ca5Sc2Ti2O10	Fe	2	As	2	Ca	5	Sc	2	Ti	2											O	10			2010																													I4/mmm		A	3.902		41.26												K			41	36			36																																																																																														FeAs,CaO,Ti,TiO2,Sc2O3	1	solid state reaction. mixture - pellet - (sealed in quartz tube) - heat(1000-1200C,60-100h) - slow cool to RT					Homologous series of iron pnictide oxide superconductors  (Fe2As2)[Can+1(Sc,Ti)nOy]   (n=3,4,5) with extremely thick blocking layers			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656,	Appl.Phys.Lett., 97(2010)072506	Hiraku Ogino,Shinya Sato,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152538	APL097072506	SIN(1200C,72h)	Fe2As2Ca6(Sc,Ti)5O13	Fe2As2Ca4Sc2Ti3O13	Fe	2	As	2	Ca	4	Sc	2	Ti	3											O	13			2010																													I4/mmm		A	3.884		49.16												K			42	36			36																																																																																														FeAs,CaO,Ti,TiO2,Sc2O3	1	solid state reaction. mixture - pellet - (sealed in quartz tube) - heat(1000-1200C,60-100h) - slow cool to RT					Homologous series of iron pnictide oxide superconductors  (Fe2As2)[Can+1(Sc,Ti)nOy]   (n=3,4,5) with extremely thick blocking layers			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656,	Appl.Phys.Lett., 97(2010)072506	Hiraku Ogino,Shinya Sato,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152539	JPS079114723	Tc by self-induction of NMR-coil. lattice term of SP (beta) = 0.90 mJ/mol.K4.	Rh17S15	Rh17S15	Rh	17	S	15																				1	2010																										A15B17		Pd17Se15	Pm3m																	K		5.4					5.4																				T					7.1			3.8																				4	14							mJ/mol.K2	110	SP-heat	410	SP-heat																																				solid state reaction					Electron Correlations in Superconductor Rh17S15 Studied by <103>Rh NMR and Specific Heat Measurements			Graduate School of Material Science, University of Hyogo, Kamigori, Hyogo 678-1297, Japan	J.Phys.Soc.Jpn, 79(2010)114723	Takehide KOYAMA,Keiji KANDA,Gaku MOTOYAMA,Takeshi MITO,Ko-ichi UEDA,Takao KOHARA,Hiroyuki NAKAMURA,Hisatomo HARIMA		
152540	JPS079083708	M-H curves measured for H//c-axis. samples show the absence of Meissner state, then lower critical field not observed	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2010							2.55																			ABC		TiNiSi																		K		0.48					0.48																																																																																																Czochralski method					Absence of Meissner State and Robust Ferromagnetism in the Superconducting State of UCoGe: Possible Evidence of Spontaneous Vortex State			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)083708	Kazuhiko DEGUCHI,Eisuke OSAKI,Seiko BAN,Nobuyuki TAMURA,Yasuyuki SIMURA,Toshiro SAKAKIBARA,Isamu SATOH,Noriaki K. SATO		
152541	JPS079093709	optimally F-doped sample. NMR and NQR of <75>As were measured.	La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2010																												oxypnictide			A			8.717												K			27.6	26.3			26.3	TC152541																																																																																																				<75>As-NMR Studies of LaFeAsO1-xFx for Various x Values			Department of Physics, Division of Material Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)093709	Yoshiaki KOBAYASHI,Erika SATOMI,Sang Chul LEE,Masatoshi SATO		
152542	JPS079114710	beta-pyrochlore.  Structural transition (low-T phase = monoclinic) at P=3.6 GPa.	KOs2O6	K1Os2O6	K	1	Os	2																	O	6			2010																										AB2C6		pyrochlore	Fd3[-]m																	K		9.62					9.62	TC152542																																																																																															flux method. KOsO4:OsO2 = 3:1 in quartz ampoule  -  heat(748K,24h)					Superconducting and Structural Transitions in the beta-Pyrochlore Oxide KOs2O6 under High Pressure			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 79(2010)114710	Hiroki OGUSU,Nao TAKESHITA,Koichi IZAWA,Jun-ichi YAMAURA,Yasuo OHISHI,Satoshi TSUTSUI,Yoshihiko OKAMOTO,Zenji HIROI		
152543	PHC4702040	major grain: Mo0.45Sr2YCu2.87Oz by EDX	MoSr2YCu2O8	Mo1Sr2Y1Cu2O8-z	Mo	1	Sr	2	Y	1	Cu	2													O	8-z			2010																												M1212				3.815		11.446												K				22			22										14	Oe	M-H curve				60			2	T	R=0.5Rn	2.5																																																																								MoO3,SnO2,Y2O3,SrCO3,CuO	1	mixture - pellet - preheat(750C,24h, in air) - (grind & pellet) - SIN(950C,24h, in O2-flow) - (grid & pellet) - (1050C,48h, in O2-flow) - ANN(600C,48h + 400C,24h, in O2-flow)					Superconductivity and critical fields in undoped and Sn-doped MoSr2YCu2O8			Institute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	Physica C, 470(2010)2040	N. Balchev,K. Nenkov,V. Antonov,J. Pirov,B. Kunev		
152545	PHC4702040	major grain: Mo0.4Sn0.1Sr1.5YCu2.9Oz by EDX position of Sn : Mo-site, grain boundary	Mo(Snx)Sr2YCu2O8	Mo1Sn0.075Sr2Y1Cu2O8-z	Mo	1	Sn	0.075	Sr	2	Y	1	Cu	2											O	8-z			2010																												M1212				3.793		11.379												K				22			22																				T																																																																										MoO3,SnO2,Y2O3,SrCO3,CuO	1	mixture - pellet - preheat(750C,24h, in air) - (grind & pellet) - SIN(950C,24h, in O2-flow) - (grid & pellet) - (1050C,48h, in O2-flow) - ANN(600C,48h + 400C,24h, in O2-flow)					Superconductivity and critical fields in undoped and Sn-doped MoSr2YCu2O8			Institute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	Physica C, 470(2010)2040	N. Balchev,K. Nenkov,V. Antonov,J. Pirov,B. Kunev		
152547	PHC470S631	P-induced SC. Tc measured by resistivity at P=159 GPa. Hc2 = 0, 1, 2, 3 T for T = 6.0, 5.43, 4.70, 3.74 K, respectively.	alpha-B	B1	B	1																							2010																										A																				K		6			0		6																				T	resistivity				3			3.74																																																																									Superconductivity in alpha-boron at Mbar pressure			KYOKUGEN, Center for Quantum Science and Technology under Extreme Conditions, Osaka University, Toyonaka, Osaka 560-8531, Japan	Physica C, 470(2010)S631	Katsuya Shimizu,Masahiro Kaneshige,Yoshifumi Hashimoto,Takenori Nagatochi,Hiroshi Hyodo,Kaoru Kimura		
152548	PHC470S328	Thermodynamic Hc(0) = 100 mT.	RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2			A	3.863		14.447												K		2.6					2.6											Oe	M-H curve	40							T	magnetization, WHH	2.5							T/K	magnetization	1.4			MHC152548																																																												RbAs,Fe2As2		mixture - pellet - ANN(650C,several days)					Bulk superconductivity at 2.6 K in undoped RbFe2As2			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Physica C, 470(2010)S328	Z. Bukowski,S. Weyeneth,R. Puzniak,J. Karpinski,B. Batlogg		
152549	PHC470S404	composition: YFe1.8Si2 by X-ray analysis. SP heat: C=gamma*T + beta*T^3 + delta*T5 (beta=0.115 mJ/mol.K4, delta=0.52E-4 mJ/mol.K6). no anomaly at Tc in C(T).	YFe2Si2	Y1Fe2Si2	Y	1	Fe	2	Si	2																		3	2010																										AB2C2		ThCr2Si2			A	3.915		9.936												K	2.8	2.9	3.5				2.9										0.6																																														mJ/mol.K2	26																																							Czochralski method. nominal(Y:Fe:Si=2:3:5) - (arc-melting) - Czochralski method					Superconductivity in ternary iron silicide YFe2-zSi2 single crystal			Department of Physics and Electronics, Osaka Prefecture University, Sakai, Osaka 599-8531, Japan	Physica C, 470(2010)S404	Ryosuke Goto,Satoru Noguchi,Takekazu Ishida		
152550	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.144, Zn=0.0044	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.996Zn0.004O4	La	1.85	Sr	0.15	Cu	0.996	Zn	0.004													O	4		3	2005																												T																		K				32.6		2.2	32.6																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152551	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.147, Zn=0.0083. structural transition Td1 = 192 K.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.992Zn0.008O4	La	1.85	Sr	0.15	Cu	0.992	Zn	0.008													O	4		3	2005																												T																		K				27.8		2.5	27.8																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152552	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.144, Zn=0.0112	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.989Zn0.011O4	La	1.85	Sr	0.15	Cu	0.989	Zn	0.011													O	4		3	2005																												T																		K				23.2		2.9	23.2																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152553	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.145, Zn=0.0170.  structural transition Td1 = 202 K.	(La,Sr)2(Cu,Zn)O4	La1.85Sr0.15Cu0.983Zn0.017O4	La	1.85	Sr	0.15	Cu	0.983	Zn	0.017													O	4		3	2005																												T																		K				16		3.8	16																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152554	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.142.  structural transition Td1 = 186 K.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		3	2005																												T																		K				36.8		1.7	36.8																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152555	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.145, Zn=0.0090	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.991Ni0.009O4	La	1.85	Sr	0.15	Cu	0.991	Ni	0.009													O	4		3	2005																												T																		K				30		2.8	30																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152556	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.144, Zn=0.0185.  structural transition Td1 = 184 K.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.982Ni0.018O4	La	1.85	Sr	0.15	Cu	0.982	Ni	0.018													O	4		3	2005																												T																		K				22.5		5.9	22.5																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152557	P072064502	Sr- and Zn-content by ICP. optimal doping: Sr=0.142, Zn=0.0287.  structural transition Td1 = 182 K.	(La,Sr)2(Cu,Ni)O4	La1.85Sr0.15Cu0.971Ni0.029O4	La	1.85	Sr	0.15	Cu	0.971	Ni	0.029													O	4		3	2005																												T																		K				11.6		9.2	11.6																																																																																																TSFZ. cylinder axis//-axis.					Zn and Ni doping effects on the low-energy spin excitations in La1.85Sr0.15CuO4			Institute for Solid State Physics, University of Tokyo, Kashiwa 277-8581, Japan	Phys.Rev.B, 72(2005)064502	M. Kofu,H. Kimura,K. Hirota		
152558	P072064503	thickness = 100A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		7.13				0.1	7.13																																									A	mivrowave	2174																												uOhm.cm							16.1																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152559	P072064503	thickness = 200A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		7.95				0.1	7.95																																									A	mivrowave	1361																												uOhm.cm							11.8																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152560	P072064503	thickness = 500A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		8.81				0.1	8.81																																									A	mivrowave	1191																												uOhm.cm							10.3																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152561	P072064503	thickness = 1000A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		9.09				0.1	9.09																																									A	mivrowave	1008																												uOhm.cm							5.37																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152562	P072064503	thickness = 2000A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		9.47				0.1	9.47																																									A	mivrowave	872																												uOhm.cm							4.48																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152563	P072064503	thickness = 3000A. [penet] measured by transmission microwavw method.	Nb	Nb1	Nb	1																						4	2005																												W																		K		9.71				0.1	9.71																																									A	mivrowave	772																												uOhm.cm							3.75																		dc magnetron sputtering in Ar. substrate: Si(100). deposition rate = 2 nm/s.					Dependence of magnetic penetration depth on the thickness of superconducting Nb thin films			Institut fur Schichten und Grenzflachen and CNI?Centre of Nanoelectronic Systems for Information Technology, Forschungszentrum Julich, D-52425 Julich, Germany	Phys.Rev.B, 72(2005)064503	A. I. Gubin,K. S. Il'in,S. A. Vitusevich,M. Siegel,N. Klein		
152564	PHC470S379	structural transition (tetra-to-ortho) at 198 K.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2010																										AB2C2		ThCr2Si2																		K					1.8																																																																																																		self-flux method. mixture(FeAs:NiAs:Sr=(4-2x):2x:1) - alumina crucible) - heat(1200C in quartz tube) - ANN(700C,14d, in Ar)					Annealing effects on superconductivity in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, MD 20742, USA	Physica C, 470(2010)S379	S.R. Saha,N.P. Butch,K. Kirshenbaum,Johnpierre Paglione		
152565	PHC470S379	annealing effect of Tc measured.	Sr(Fe,Ni)2As2	Sr1Fe1.85Ni0.15As2	Sr	1	Fe	1.85	Ni	0.15	As	2																3	2010																										AB2C2		ThCr2Si2																		K			9.8	9.2			9.2																																																																																																self-flux method. mixture(FeAs:NiAs:Sr=(4-2x):2x:1) - alumina crucible) - heat(1200C in quartz tube) - ANN(700C,14d, in Ar)					Annealing effects on superconductivity in SrFe2-xNixAs2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, MD 20742, USA	Physica C, 470(2010)S379	S.R. Saha,N.P. Butch,K. Kirshenbaum,Johnpierre Paglione		
152566	PHC470S296	(dC/gamma*Tc) = 0.87. no detail for Hc2.	BaRh2P2	Ba1Rh2P2	Ba	1	Rh	2	P	2																			2010																										AB2C2		ThCr2Si2			A	3.939		12.576												K		1		1			1																				T		0.07																																		mJ/mol.K2	9.75	SP-heat																																				In(3N),Rh(3N),Ba(3N),Sr(4N),P(5N),As(5N)		mixture - pellet - (alumina crucible) - heat(400C,16h + 1000C,12h, in sealed quartz tube)					Superconductivity in 4d and 5d transition metal layered pnictides BaRh2P2, BaIr2P2 and SrIr2As2			Department of Advanced Materials, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan	Physica C, 470(2010)S296	D. Hirai,T. Takayama,D. Hashizume,R. Higashinaka,A. Yamamoto,A.K. Hiroko,H. Takagi		
152567	PHC470S296	(dC/gamma*Tc) = 1.53. no detail for Hc2.	BaIr2P2	Ba1Ir2P2	Ba	1	Ir	2	P	2																			2010																										AB2C2		ThCr2Si2			A	3.946		12.572												K			2.1	2.1			2.1																				T		0.14																																		mJ/mol.K2	6.86	SP-heat																																				In(3N),Rh(3N),Ba(3N),Sr(4N),P(5N),As(5N)		mixture - pellet - (alumina crucible) - heat(400C,16h + 1000C,12h, in sealed quartz tube)					Superconductivity in 4d and 5d transition metal layered pnictides BaRh2P2, BaIr2P2 and SrIr2As2			Department of Advanced Materials, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan	Physica C, 470(2010)S296	D. Hirai,T. Takayama,D. Hashizume,R. Higashinaka,A. Yamamoto,A.K. Hiroko,H. Takagi		
152568	PHC470S296	more heat treatment: SIN(1150C,48h).    (dC/gamma*Tc) = 0.93. no detail for Hc2.	SrIr2As2	Sr1Ir2As2	Sr	1	Ir	2	As	2																			2010																										AB2C2		ThCr2Si2			A	4.068		11.794												K			2.9	2.8			2.8																				T		1.4																																		mJ/mol.K2	7.03	SP-heat																																				In(3N),Rh(3N),Ba(3N),Sr(4N),P(5N),As(5N)		mixture - pellet - (alumina crucible) - heat(400C,16h + 1000C,12h, in sealed quartz tube)					Superconductivity in 4d and 5d transition metal layered pnictides BaRh2P2, BaIr2P2 and SrIr2As2			Department of Advanced Materials, The University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8561, Japan	Physica C, 470(2010)S296	D. Hirai,T. Takayama,D. Hashizume,R. Higashinaka,A. Yamamoto,A.K. Hiroko,H. Takagi		
152569	JPS079063701	P-induced SC.  SC properties at P = 2.35 GPa. Hc2 measured for H//J//c-axis	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2010																										ABC3		BaNiSn3																		K		1.06			0		1.06	MTC152569																												T/K	resistivity			12.3	MHC152569																																																														See Phys.Rev.Lett., 98(2007)197001					Anomalous Behavior of the Upper-Critical-Field in Heavy-Fermion Superconductor CeRhSi3			Graduate School of Science, Tohoku University, Sendai 980-8578, Japan	J.Phys.Soc.Jpn, 79(2010)063701	Tetsuya SUGAWARA,Noriaki KIMURA,Haruyoshi AOKI,Florence LEVY,Ilya SHEIKIN,Taichi TERASHIMA		
152570	JPS079063701	P-induced SC.  SC properties at P = 2.85 GPa. Hc2 measured for H//J//c-axis	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2010																										ABC3		BaNiSn3																		K		1.09			0		1.09	MTC152569																												T/K	resistivity			19.1	MHC152570																																																														See Phys.Rev.Lett., 98(2007)197001					Anomalous Behavior of the Upper-Critical-Field in Heavy-Fermion Superconductor CeRhSi3			Graduate School of Science, Tohoku University, Sendai 980-8578, Japan	J.Phys.Soc.Jpn, 79(2010)063701	Tetsuya SUGAWARA,Noriaki KIMURA,Haruyoshi AOKI,Florence LEVY,Ilya SHEIKIN,Taichi TERASHIMA		
152571	JPS079023702		Nd(O,F)FeAs	Nd1Fe1As1F0.11O0.89	Nd	1	Fe	1	As	1	F	0.11													O	0.89		1	2010																										ABCD		oxypnictide			A	3.9562		8.5404												K		48					48																																																																		uV/K	-35.6			MTP152571															cm3/C						MRH152571			Nd,Nd2O3,NdF3,FeAs,RuAs,As		solid state reacton .  See J.Phys.Soc.Jpn, 78(2009)013701					Effects of Ru Doping on the Transport Behavior and Superconducting Transition Temperature of NdFeAsO0:89F0:11			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)023702	Sang Chul LEE,Erika SATOMI,Yoshiaki KOBAYASHI,Masatoshi SATO		
152572	JPS079023702		Nd(O,F)FeAs	Nd1Fe0.98Ru0.02As1F0.11O0.89	Nd	1	Fe	0.98	Ru	0.02	As	1	F	0.11											O	0.89		1	2010																										ABCD		oxypnictide			A	3.9591		8.5441												K		46.5					46.5	MTC152572																																																																	uV/K	-37.3			MTP152572															cm3/C						MRH152572			Nd,Nd2O3,NdF3,FeAs,RuAs,As		solid state reacton .  See J.Phys.Soc.Jpn, 78(2009)013701					Effects of Ru Doping on the Transport Behavior and Superconducting Transition Temperature of NdFeAsO0:89F0:11			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)023702	Sang Chul LEE,Erika SATOMI,Yoshiaki KOBAYASHI,Masatoshi SATO		
152573	JPS079023702		Nd(O,F)FeAs	Nd1Fe0.9Ru0.1As1F0.11O0.89	Nd	1	Fe	0.9	Ru	0.1	As	1	F	0.11											O	0.89		1	2010																										ABCD		oxypnictide			A	3.9687		8.5249												K		40					40																																																																		uV/K	-45																		cm3/C						MRH152573			Nd,Nd2O3,NdF3,FeAs,RuAs,As		solid state reacton .  See J.Phys.Soc.Jpn, 78(2009)013701					Effects of Ru Doping on the Transport Behavior and Superconducting Transition Temperature of NdFeAsO0:89F0:11			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)023702	Sang Chul LEE,Erika SATOMI,Yoshiaki KOBAYASHI,Masatoshi SATO		
152574	JPS079023702		Nd(O,F)FeAs	Nd1Fe0.85Ru0.15As1F0.11O0.89	Nd	1	Fe	0.85	Ru	0.15	As	1	F	0.11											O	0.89		1	2010																										ABCD		oxypnictide			A	3.973		8.5069												K		34					34																																																																		uV/K				MTP152574															cm3/C						MRH152574			Nd,Nd2O3,NdF3,FeAs,RuAs,As		solid state reacton .  See J.Phys.Soc.Jpn, 78(2009)013701					Effects of Ru Doping on the Transport Behavior and Superconducting Transition Temperature of NdFeAsO0:89F0:11			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)023702	Sang Chul LEE,Erika SATOMI,Yoshiaki KOBAYASHI,Masatoshi SATO		
152575	JPS079023702		Nd(O,F)FeAs	Nd1Fe0.5Ru0.5As1F0.11O0.89	Nd	1	Fe	0.5	Ru	0.5	As	1	F	0.11											O	0.89		1	2010																										ABCD		oxypnictide			A	4.0208		8.3778												K		14.5					14.5																																																																		uV/K	0																											Nd,Nd2O3,NdF3,FeAs,RuAs,As		solid state reacton .  See J.Phys.Soc.Jpn, 78(2009)013701					Effects of Ru Doping on the Transport Behavior and Superconducting Transition Temperature of NdFeAsO0:89F0:11			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)023702	Sang Chul LEE,Erika SATOMI,Yoshiaki KOBAYASHI,Masatoshi SATO		
152576	JPS079084705	RRR>700. Hc1 determined by micro Hall censor (first induction). anisotropy (Hc1) = 3 at Tc.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2010																										AB2C2		ThCr2Si2																		K		1.4					1.4											mT	magnetization																						MHC152576							um	from Hc1	0.8																																																					Czochralski method					Anomalous Temperature Dependence of Lower Critical Field in Ultraclean URu2Si2			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 79(2010)084705	Ryuji OKAZAKI,Masaaki SHIMOZAWA,Hiroaki SHISHIDO,Marcin KONCZYKOWSKI,Yoshinori HAGA,Tatsuma D. MATSUDA,Etsuji YAMAMOTO,Yoshiyuki Onuki,Yoichi YANASE,Takasada SHIBAUCHI,Yuji MATSUDA		
152577	JAC5091401	impurity phases: Y2O3, YPd6Al3. Tc(R) defined as max of (dR/dT). (dC/gamma*Tc) = 0.2.  e-ph coupling = 0.19	YPd2Al3	Y1Pd2Al3	Y	1	Pd	2	Al	3																			2011																										AB2C3		PrNi2Al3	P6/mmm		A	5.3704		4.1932												K		2.2	2.3				2.2																				T	resistivity, WHH	0.96							T/K	ac-SUS	0.7			MHC152577		A	from Hc2	192																		mJ/mol.K2	7.2	SP-heat	200	SP-heat																																									YPd2Al3-A new superconducting compound			Charles University Prague, Faculty of Mathematics and Physics, Department of Condensed Matter Physics, Ke Karlovu 5, 121 16 Prague, Czech Republic	J.Alloys Compd., 509(2011)1401	Jiri Pospisil,Marie Kratochvilova,Martin Divis,Jan Prokleska,Jana Poltierova Vejpravova,Vladimir Sechovsky		
152578	JPS080013702	Li/Rh = 0.95, B/Rh = 1.48 from ICP analysis.	LixRhBy	Li1Rh1B1.5	Li	1	Rh	1	B	1.5																			2011																										ABC2			P2<1>3																	K		2.5					2.5			K/GPa	0.15																																																																																												mixture(Rh,B) - addition(Li) - (Ta-foil or BN crucible) - (sealed in stainless, Ar) - heat(700-900C, 20h) FC to RT					A New Noncentrosymmetric Superconducting Phase in the Li-Rh-B System			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 80(2011)013702	Hiroyuki TAKEYA,Hiroki FUJII,Mohammed ELMASSALAMI,Francisco CHAVES,Shuuichi OOI,Takashi MOCHIKU,Yoshihiko TAKANO,Kazuto HIRATA,Kazumasa TOGANO		
152579	JPS080013702	Tc defined as R(mid). G-L parameter = 1. non-centrosymmetry sample.	LixRhBy	Li1.2Rh1B1.5	Li	1.2	Rh	1	B	1.5																			2011																										ABC2			P2<1>3																	K		2.5					2.5											Oe		65.5							T	resistivity, linear extrapolation	1.59												MHC152579		A		144			A	from Hc1	145																																																					mixture(Rh,B) - addition(Li) - (Ta-foil or BN crucible) - (sealed in stainless, Ar) - heat(700-900C, 20h) FC to RT					A New Noncentrosymmetric Superconducting Phase in the Li-Rh-B System			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 80(2011)013702	Hiroyuki TAKEYA,Hiroki FUJII,Mohammed ELMASSALAMI,Francisco CHAVES,Shuuichi OOI,Takashi MOCHIKU,Yoshihiko TAKANO,Kazuto HIRATA,Kazumasa TOGANO		
152580	JPS080014716	RRR = 5.7. (dC/gamma*Tc) = 1.45. Thermodynamic Hc(0) = 23.7 mT.  GL parameter = 38.	Y2AlGe3	Y2Al1Ge3	Y	2	Al	1	Ge	3																			2011																										AB2C3	3	Y2AlGe3	Pnma	62	A	6.785	4.189	17.676											ThCr2Si2-derivative	K	4.4		4.8	4.5		0.4	4.5										90	Oe	M-H curve	16.6							T	resistivity, extrapolation	1.26												MHC152580		A	from Hc2	162			A	from Hc1	6310			meV	0.595	3.54	14							mJ/mol.K2	6.91	SP-heat	407	SP-heat											uOhm.cm							37.6				214														mixture(Y:Al:Ge=2:1:3) - (arc-melting) - ANN(850C,1w, in vac)					Superconducting State in the Ternary Germanide Y2AlGe3 with Related ThCr2Si2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011)014716	Naoki KASE,Hironaga SASAKI,Hiroki HAYAMIZU,Jun AKIMITSU		
152581	PHC4710077	SC appears for 0.1=< x =<0.3 in FeTe1-xSx. Tc independent of x. SC volume increases with x.	Fe(Te,S)	Fe1Te0.75S0.25	Fe	1	Te	0.75	S	0.25																			2011																										AB	2		P4/nmm		A	3.806		6.226											tetragonal	K	5.5	7.28	10				7.28																				T	resistivity, WHH	65												MHC152581																																uV/K	-16			MTP152581																										solid state reaction.  mixture - pellet - (sealed in quartz, vac) - SIN(750C,12h) - ANN(200C,12h, in O2-flow) cool to RT					Superconductivity and thermal properties of sulphur doped FeTe with effect of oxygen post annealing			National Physical Laboratory (CSIR), Quantum Phenomena & Applications, Division Dr. K.S. Krishnan Marg, New Delhi 110 012, India	Physica C, 471(2011)77	V.P.S. Awana,Anand Pal,Arpita Vajpayee,Bhasker Gahtori,H. Kishan		
152582	PHC4710077	not SC. Structural phase transition at 78 K, obseved in R(T) , C(T).	FeTe	Fe1Te1	Fe	1	Te	1																					2011																										AB	2		P4/nmm		A	3.821		6.285												K					5																																																																																																		solid state reaction.  mixture - pellet - (sealed in quartz, vac) - SIN(750C,12h) - ANN(200C,12h, in O2-flow) cool to RT					Superconductivity and thermal properties of sulphur doped FeTe with effect of oxygen post annealing			National Physical Laboratory (CSIR), Quantum Phenomena & Applications, Division Dr. K.S. Krishnan Marg, New Delhi 110 012, India	Physica C, 471(2011)77	V.P.S. Awana,Anand Pal,Arpita Vajpayee,Bhasker Gahtori,H. Kishan		
152585	ZAN6220589		Y2AlGe3	Y2Al1Ge3	Y	2	Al	1	Ge	3																			1996									5.587																	AB2C3		Y2AlGe3	Pmma		A	6.785	4.189	17.676												K		4.5					4.5																																																																																																heat(950C)					Y2AlGe3 -  a Superconductive Metallic Zintl Compound			Dusseldorf, Institut fur Anorganische Chemie und Strukturchemie der Heinrich-Heine-Universitat	Z.anorg.allg.Chem., 622(1996)589	D. Johrendt,A. Mewis,K. Drescher,S. Wasser,G. Michels		
152586	PRB082235128	Tl-site occupancy = 0.94 from XRD. anisotropy(Hc2) = 12.6. GL parameter(kappa) = 202 for H//a, =1.3 for H//c.  thermodynamic Hc(0) = 0.0207 T.	Tl2Mo6Se6	Tl2Mo6Se6	Tl	2	Mo	6	Se	6																		3	2010																										A2B6C6		Tl2Fe6Te6	P6<3>/m		A	8.934		4.494												K		4.2					4.2																				T	resistivity		5.9	0.47												A	from Hc2		940	75	um	estimate from Hc(0),GL		0.12	1.5	meV	0.9	5								mJ/gat.K2	0.13																																							heat(1700C, in sealed Mo-crucible)					Phonon mode spectroscopy, electron-phonon coupling, and the metal-insulator transition in quasi-one-dimensional M2Mo6Se6			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.B, 82(2010)235128	A. P. Petrovic,R. Lortz,G. Santi,M. Decroux,H. Monnard,F. Fischer,L. Boeri,O. K. Andersen,J. Kortus,D. Salloum,P. Gougeon,M. Potel		
152587	PRB082235128	In-site occupancy = 0.95 from XRD. anisotropy(Hc2) = 17.2. GL parameter(kappa) = 260 for H//a, = 0.87 for H//c. thermodynamic Hc(0) = 0.0119 T.	In2Mo6Se6	In2Mo6Se6	In	2	Mo	6	Se	6																		3	2010																										A2B6C6		Tl2Fe6Te6	P6<3>/m		A	8.854		4.493												K		2.85					2.85																				T	resistivity		4.35	0.25												A	from Hc2		1500	87	um	estimate from Hc(0),GL		0.13	2.2		0.4	3.5								mJ/gat.K2	0.13																																							heat(1100C, in evacuated silica tube)					Phonon mode spectroscopy, electron-phonon coupling, and the metal-insulator transition in quasi-one-dimensional M2Mo6Se6			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.B, 82(2010)235128	A. P. Petrovic,R. Lortz,G. Santi,M. Decroux,H. Monnard,F. Fischer,L. Boeri,O. K. Andersen,J. Kortus,D. Salloum,P. Gougeon,M. Potel		
152588	PRB082235128	Rb-site occupancy = 0.95 from XRD. not SC.	Rb2Mo6Se6	Rb2Mo6Se6	Rb	2	Mo	6	Se	6																		3	2010																										A2B6C6		Tl2Fe6Te6	P6<3>/m		A	9.257		4.487												K					1.7																																																																																																		heat(1500C, in sealed Mo-crucible)					Phonon mode spectroscopy, electron-phonon coupling, and the metal-insulator transition in quasi-one-dimensional M2Mo6Se6			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.B, 82(2010)235128	A. P. Petrovic,R. Lortz,G. Santi,M. Decroux,H. Monnard,F. Fischer,L. Boeri,O. K. Andersen,J. Kortus,D. Salloum,P. Gougeon,M. Potel		
152589	PHC4600702	Thermodynamic Hc(0) = 208 Oe from SP-heat. GL-parameter(Hc2) = 340 for H//a and = 1.7 for H//c.	Tl2Mo6Se6	Tl2Mo6Se6	Tl	2	Mo	6	Se	6																			2007																										A2B6C6		Tl2Fe6Te6																		K		5					5											Oe	SQUID			19					T	resistivity, linear extrapolation		10	0.71												A	from Hc2		800	57	um	estimate from Hc(0),GL		0.14	1.9																																																								Unconventional resistive transitions in the extreme type-II superconductor Tl2Mo6Se6			Department of Condensed Matter Physics, University of Geneva, Quai Ernest-Ansermet 24, 1211 Geneva, Switzerland	Physica C, 460-462(2007)702	A. P. Petrovic,Y. Fasano,R. Lortz,M. Decroux,M. Potel,R. Chevrel,F. Fischer		
152590	PRL100037004	RRR=670. THCFIG shows THC/T vs T at H=3 T. HCFIG shows Hc2(T), 1st and 2nd order transition,  and lattice melting field Hm.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2008																										AB2C2		ThCr2Si2																		K		1.45				0.1	1.45																				T	resistivity													MHC152590																											W/m.K				MTHC152590						uOhm.cm							0.5																							Flux Line Lattice Melting and the Formation of a Coherent Quasiparticle Bloch State in the Ultraclean URu2Si2 Superconductor			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.Lett., 100(2008)037004	R. Okazaki,Y. Kasahara,H. Shishido,M. Konczykowski,K. Behnia,Y. Haga,T. D. Matsuda,Y. Onuki,T. Shibauchi,Y. Matsuda		
152591	JPS079073704	P-induced SC. P<crit> = 1.2 GPa. Tc(max) = 24 K at P= 2.14 GPa. T<SDW> decreases with increasing P. Neel-T = 4 K (nearly independent of P)	(Eu,Ca)Fe2As2	Eu0.5Ca0.5Fe2As2	Eu	0.5	Ca	0.5	Fe	2	As	2																3	2010								4																		AB2C2		ThCr2Si2			A	3.897		12.006												K	24						24																																																																																																Sn-flux method. (Eu:Ca:Fe:As:Sn = 0.5:0.5:2:2:48). heat(1000C,24h) - cool to 500C (14C/h) in sealed quartz tube (1/3 atm-Ar)					Pressure-Induced Superconductivity in Eu0.5Ca0.5Fe2As2: Wide Zero-Resistivity Region Due to Suppression of Eu Magnetic Order and Chemical Pressure			Department of Physics, Kyushu University, 6-10-1 Hakozaki, Higashi-ku, Fukuoka 812-8581, Japan	J.Phys.Soc.Jpn, 79(2010)073704	Akihiro MITSUDA,Tomohiro MATOBA,Fumihiro ISHIKAWA,Yuh YAMADA,Hirofumi WADA		
152592	PRB065024437	Neel-T and T<SG>( spin glass temp) defined as the peak of ac-SUS.	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			2001	cm3/mol	-0.0004			myu-B/mol	3.77	-52	14.6																		AB2C3		PrNi2Al3			A	5.3646		4.1876												K		1.9					1.9	MTC152593																																																																																															arc-melting.  - (wrapped in Ta-foil ) - ANN(900C,7d,in Ar)					Magnetic and non-Fermi-liquid properties of U1-xLaxPd2Al3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla	Phys.Rev.B, 65(2001)024437	V. S. Zapf,R. P. Dickey,E. J. Freeman,C. Sirvent,M. B. Maple		
152593	PRB065024437	Neel-T and T<SG>( spin glass temp) defined as the peak of ac-SUS.	(U,La)Pd2Al3	U0.85La0.15Pd2Al3	U	0.85	La	0.15	Pd	2	Al	3																	2001	cm3/mol	0.00036			myu-B/mol	2.5	-81	4.3																		AB2C3		PrNi2Al3			A	5.3828		4.1892												K							1.2	MTC152593																																																																																															arc-melting.  - (wrapped in Ta-foil ) - ANN(900C,7d,in Ar)					Magnetic and non-Fermi-liquid properties of U1-xLaxPd2Al3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla	Phys.Rev.B, 65(2001)024437	V. S. Zapf,R. P. Dickey,E. J. Freeman,C. Sirvent,M. B. Maple		
152594	PRB065024437	Neel-T and T<SG>( spin glass temp) defined as the peak of ac-SUS. T<SG> = 3.4 K.	(U,La)Pd2Al3	U0.7La0.3Pd2Al3	U	0.7	La	0.3	Pd	2	Al	3																	2001	cm3/mol	0.00035			myu-B/mol	3.1	-1																			AB2C3		PrNi2Al3			A	5.4096		4.2056												K							1.2	MTC152593																																																																																															arc-melting.  - (wrapped in Ta-foil ) - ANN(900C,7d,in Ar)					Magnetic and non-Fermi-liquid properties of U1-xLaxPd2Al3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla	Phys.Rev.B, 65(2001)024437	V. S. Zapf,R. P. Dickey,E. J. Freeman,C. Sirvent,M. B. Maple		
152595	PRB065024437	Neel-T and T<SG>( spin glass temp) defined as the peak of ac-SUS. T<SG> = 3.6 K.	(U,La)Pd2Al3	U0.4La0.6Pd2Al3	U	0.4	La	0.6	Pd	2	Al	3																	2001	cm3/mol	0.0004			myu-B/mol	2.5	-15																			AB2C3		PrNi2Al3			A	5.4465		4.2172												K							1.2																																																																																																arc-melting.  - (wrapped in Ta-foil ) - ANN(900C,7d,in Ar)					Magnetic and non-Fermi-liquid properties of U1-xLaxPd2Al3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla	Phys.Rev.B, 65(2001)024437	V. S. Zapf,R. P. Dickey,E. J. Freeman,C. Sirvent,M. B. Maple		
152596	PRB065024437	(dC/gamma*Tc) = 0.8	LaPd2Al3	La1Pd2Al3	La	1	Pd	2	Al	3																			2001							1																			AB2C3		PrNi2Al3			A	5.5086		4.2289												K	0.75	0.85	0.9				0.85																																																																																																arc-melting.  - (wrapped in Ta-foil ) - ANN(900C,7d,in Ar)					Magnetic and non-Fermi-liquid properties of U1-xLaxPd2Al3			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla	Phys.Rev.B, 65(2001)024437	V. S. Zapf,R. P. Dickey,E. J. Freeman,C. Sirvent,M. B. Maple		
152597	JPC022235701	reentrant temperature = 16.1 K due to FM. Hc2 extracted from R(T) figure defined as 0.5Rnby DB-stuffs	Eu(Fe,Co)2As2	Eu1Fe1.715Co0.285As2	Eu	1	Fe	1.715	Co	0.285	As	2																	2010																										AB2C2		ThCr2Si2																		K		21					21																																		MHC152597																																																														self-flux method					Evidence for competing magnetic and superconducting phases in superconducting Eu1-xSrxFe2-yCoyAs2 single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J. Phys.: Condens. Matter 22 (2010) 235701	Y. He,T.Wu,G.Wu,Q J Zheng,Y Z Liu,H Chen,J J Ying,R H Liu,X FWang,Y L Xie,Y J Yan,J K Dong,S Y Li,XH Chen		
152598	JPC022235701	no reentrant behaviour.	(Eu,Sr)(Fe,Co)2As2	Eu0.6Sr0.4Fe1.715Co0.285As2	Eu	0.6	Sr	0.4	Fe	1.715	Co	0.285	As	2															2010																										AB2C2		ThCr2Si2																		K		13.9					13.9	MTC152598																																																																																															self-flux method					Evidence for competing magnetic and superconducting phases in superconducting Eu1-xSrxFe2-yCoyAs2 single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J. Phys.: Condens. Matter 22 (2010) 235701	Y. He,T.Wu,G.Wu,Q J Zheng,Y Z Liu,H Chen,J J Ying,R H Liu,X FWang,Y L Xie,Y J Yan,J K Dong,S Y Li,XH Chen		
152599	JPC022235701	reentrant temperature = 6.2 K due to FM. Hc2 extracted from R(T) figure defined as 0.5Rnby DB-stuffs	(Eu,Sr)(Fe,Co)2As2	Eu0.7Sr0.3Fe1.715Co0.285As2	Eu	0.7	Sr	0.3	Fe	1.715	Co	0.285	As	2															2010																										AB2C2		ThCr2Si2																		K		10.2					10.2																																		MHC152599																																																														self-flux method					Evidence for competing magnetic and superconducting phases in superconducting Eu1-xSrxFe2-yCoyAs2 single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J. Phys.: Condens. Matter 22 (2010) 235701	Y. He,T.Wu,G.Wu,Q J Zheng,Y Z Liu,H Chen,J J Ying,R H Liu,X FWang,Y L Xie,Y J Yan,J K Dong,S Y Li,XH Chen		
152600	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2010																												oxypnictide			A	4.0286		8.7219												K		27.1					27.1																																																																		uV/K	-27.4			TP152600															cm3/C	-0.0016					RH152600					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152601	JPS079094702		La(O,F)(Fe,Ru)As	La1Fe0.985Ru0.015As1F0.11O0.89	La	1	Fe	0.985	Ru	0.015	As	1	F	0.11											O	0.89		1	2010																												oxypnictide			A	4.0309		8.7194												K				27.5			27.5																																																																		uV/K	-34.7			TP152601															cm3/C	-0.00208					RH152601					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152602	JPS079094702		La(O,F)(Fe,Ru)As	La1Fe0.97Ru0.03As1F0.11O0.89	La	1	Fe	0.97	Ru	0.03	As	1	F	0.11											O	0.89		1	2010																												oxypnictide			A	4.0297		8.7192												K		25.6					25.6																																																																		uV/K	-23.8			TP152602															cm3/C	-0.00189					RH152602					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152603	JPS079094702		La(O,F)(Fe,Ru)As	La1Fe0.9Ru0.1As1F0.11O0.89	La	1	Fe	0.9	Ru	0.1	As	1	F	0.11											O	0.89		1	2010																												oxypnictide			A	4.0393		8.7007												K		23.6		23.6			23.6																																																																		uV/K	-21.1			TP152603															cm3/C	-0.00373					RH152603					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152604	JPS079094702		La(O,F)(Fe,Ru)As	La1Fe0.85Ru0.15As1F0.11O0.89	La	1	Fe	0.85	Ru	0.15	As	1	F	0.11											O	0.89		1	2010																												oxypnictide			A	4.0402		8.6826												K		23.6					23.6																																																																																					cm3/C	-0.00161					RH152604					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152605	JPS079094702		La(O,F)(Fe,Ru)As	La1Fe0.7Ru0.3As1F0.11O0.89	La	1	Fe	0.7	Ru	0.3	As	1	F	0.11											O	0.89		1	2010																												oxypnictide			A	4.0555		8.6441												K		17.2		17.3			17.2																																																																		uV/K	-17.5			TP152605															cm3/C	-0.00098					RH152605					See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152606	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2010																												oxypnictide																		K		27.3					27.3																																																																		uV/K	-49.6			TP152606																										See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152607	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.13O0.87	La	1	Fe	1	As	1	F	0.13													O	0.87		1	2010																												oxypnictide																		K		25.4					25.4																																																																		uV/K	-33.4			TP152607																										See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152608	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.15O0.85	La	1	Fe	1	As	1	F	0.15													O	0.85		1	2010																												oxypnictide																		K		20					20																																																																		uV/K	-28.4			TP152608																										See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152609	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.2O0.8	La	1	Fe	1	As	1	F	0.2													O	0.8		1	2010																												oxypnictide																		K		4.52					4.52																																																																		uV/K	-29			TP152609																										See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152610	JPS079094702		La(O,F)FeAs	La1Fe1As1F0.18O0.82	La	1	Fe	1	As	1	F	0.18													O	0.82		1	2010																												oxypnictide																		K		14.3					14.3																																																																																																See J.Phys.Soc.Jpn. 77(2008) Suppl. C, p 147					Superconducting Transition Temperatures and Transport Properties of LaFe1-yRuyAsO0.89F0.11 and LaFeAsO0.89-xF0.11+x			Department of Physics, Division of Material Science, Nagoya University, Furocho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)094702	Erika SATOMI,Sang Chul LEE,Yoshiaki KOBAYASHI,Masatoshi SATO		
152611	PRB083024511		PrOs4Sb12	Pr1Os4Sb12	Pr	1	Os	4	Sb	12																		3	2011																										AB4C12		skutterudite																	LaFe4P12-type	K		1.86		1.82			1.86																				T	resistivity, extrapolation	2.22												MHC152611																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152612	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.9Nd0.1Os4Sb12	Pr	0.9	Nd	0.1	Os	4	Sb	12																3	2011							-1.06																			AB4C12		skutterudite																	LaFe4P12-type	K		1.73					1.73	MTC152612																			T	resistivity, extrapolation	1.87												MHC152611																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152613	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.8Nd0.2Os4Sb12	Pr	0.8	Nd	0.2	Os	4	Sb	12																3	2011							-0.45																			AB4C12		skutterudite																	LaFe4P12-type	K		1.61		1.43			1.61																				T	resistivity, extrapolation	1.44												MHC152611																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152614	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.75Nd0.25Os4Sb12	Pr	0.75	Nd	0.25	Os	4	Sb	12																3	2011																										AB4C12		skutterudite																	LaFe4P12-type	K		1.48					1.48																				T	resistivity, extrapolation	0.924												MHC152611																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152615	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.7Nd0.3Os4Sb12	Pr	0.7	Nd	0.3	Os	4	Sb	12																3	2011																										AB4C12		skutterudite																	LaFe4P12-type	K		1.27		1.26			1.27																				T	resistivity, extrapolation	0.389												MHC152611																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152616	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.6Nd0.4Os4Sb12	Pr	0.6	Nd	0.4	Os	4	Sb	12																3	2011																										AB4C12		skutterudite																	LaFe4P12-type	K		0.89					0.89																				T	resistivity, extrapolation	0.132																																																																										flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152617	PRB083024511		(Pr,Nd)Os4Sb12	Pr0.5Nd0.5Os4Sb12	Pr	0.5	Nd	0.5	Os	4	Sb	12																3	2011																										AB4C12		skutterudite																	LaFe4P12-type	K		0.6		0.71			0.6																																		MHC152617																																																														flux method					Superconductivity, magnetic order, and quadrupolar order in the filled skutterudite system Pr1-xNdxOs4Sb12			Department of Physics, University of California, San Diego, La Jolla, CA 92093-0319, USA	Phys.Rev.B, 83(2011)024511	P.-C. Ho,T. Yanagisawa,W. M. Yuhasz,A. A. Dooraghi,C. C. Robinson,N. P. Butch,R. E. Baumbach,M. B. Maple		
152618	PRB083024512	lattice const. at 100 K. RRR = 4. [vols]>100 maybe due to  demagneitizing factor. Hc2 defined as SUS(on). thermodynamic Hc(0) = 0. 023 T. GL-parameter = 8.3.	CaIrSi3	Ca1Ir1Si3	Ca	1	Ir	1	Si	3																		1	2011																										ABC3			I4mm	107	A	4.1833		9.8728												K		3.6		3.7			3.6										170										T	SUS, linear extrapolation	0.27												MHC152618		A	from Hc2	340			A	from GL, Hc(0)	2800													mJ/mol.K2	5.8	SP-heat	360	SP-heat																																				arc-melting. nominalcompositions are (Ca:Ir:Si=3:1:4.7) and (Ca:Pt:Si=3:1:5). single phase isolated using dilute hydrochloric acid.					Crystallographic and superconducting properties of the fully gapped noncentrosymmetric 5d-electron superconductors CaMSi3 (M = Ir, Pt)			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 83(2011)024512	G. Eguchi,D. C. Peets,M. Kriener,Y. Maeno,E. Nishibori,Y. Kumazawa,K. Banno,S. Maki,H. Sawa		
152619	PRB083024512	lattice const. at 100 K. RRR = 1.6. [vols] > 100 maybe due to  demagneitizing factor. Hc2 defined as SUS(on).  thermodynamic Hc(0) = 0.0094 T. GL-parameter = 11.	CaPtSi3	Ca1Pt1Si3	Ca	1	Pt	1	Si	3																		1	2011																										ABC3			I4mm	107	A	4.1988		9.8111												K		2.3		2.3			2.3										100										T	SUS, linear extrapolation	0.15												MHC152619		A	from Hc2	470			A	from GL, Hc(0)	5200													mJ/mol.K2	4	SP-heat	370	SP-heat																																				arc-melting. nominalcompositions are (Ca:Ir:Si=3:1:4.7) and (Ca:Pt:Si=3:1:5). single phase isolated using dilute hydrochloric acid.					Crystallographic and superconducting properties of the fully gapped noncentrosymmetric 5d-electron superconductors CaMSi3 (M = Ir, Pt)			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 83(2011)024512	G. Eguchi,D. C. Peets,M. Kriener,Y. Maeno,E. Nishibori,Y. Kumazawa,K. Banno,S. Maki,H. Sawa		
152620	PRB083014503	R(T) anomaly at 140 K due to AFM & structural transformation.	PrFeAsO	Pr1Fe1As1O1	Pr	1	Fe	1	As	1															O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9893		8.6148												K					2																																																																																																		mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152621	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities. R(T) anomaly at 80 K due to AFM & structural transformation.	Pr(Fe,Co)AsO	Pr1Fe0.975Co0.025As1O1	Pr	1	Fe	0.975	Co	0.025	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm																	K					2																																																																																																		mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152622	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	Pr(Fe,Co)AsO	Pr1Fe0.95Co0.05As1O1	Pr	1	Fe	0.95	Co	0.05	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9864		8.5964												K		8.76	9.28				8.76																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152623	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	Pr(Fe,Co)AsO	Pr1Fe0.925Co0.075As1O1	Pr	1	Fe	0.925	Co	0.075	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9855		8.5902												K		15.7	16.3				15.7																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152624	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	Pr(Fe,Co)AsO	Pr1Fe0.9Co0.1As1O1	Pr	1	Fe	0.9	Co	0.1	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9873		8.5815												K		16	16.6				16																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152625	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	Pr(Fe,Co)AsO	Pr1Fe0.85Co0.15As1O1	Pr	1	Fe	0.85	Co	0.15	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9859		8.5673												K		9.07	9.07				9.07																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152626	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	Pr(Fe,Co)AsO	Pr1Fe0.8Co0.2As1O1	Pr	1	Fe	0.8	Co	0.2	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9858		8.5549												K					2																																																																																																		mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152627	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)FeAsO	Pr0.8Sr0.2Fe1As1O1	Pr	0.8	Sr	0.2	Fe	1	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9945		8.6563												K		14	15.5				14																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152628	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.95Co0.05As1O1	Pr	0.8	Sr	0.2	Fe	0.95	Co	0.05	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9943		8.6495												K		7.05	11.1				7.05																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152629	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.925Co0.075As1O1	Pr	0.8	Sr	0.2	Fe	0.925	Co	0.075	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9939		8.645												K		3.5	7.81				3.5																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152630	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.9Co0.1As1O1	Pr	0.8	Sr	0.2	Fe	0.9	Co	0.1	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9925		8.6385												K		6.86	12.9				6.86																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152631	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.85Co0.15As1O1	Pr	0.8	Sr	0.2	Fe	0.85	Co	0.15	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9929		8.6204												K		16	18.7				16																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152632	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.8Co0.2As1O1	Pr	0.8	Sr	0.2	Fe	0.8	Co	0.2	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9926		8.6102												K		11.5	13.8				11.5																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152633	PRB083014503	small amount of Pr2O3, FeAs, SrFe2As2 impurities.	(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.7Co0.3As1O1	Pr	0.8	Sr	0.2	Fe	0.7	Co	0.3	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9924		8.5831												K		4.48	7.23				4.48																																																																																																mixture - pellet - heat(1173K,5h + 1433K,40h, in evacuated quartz) - FC to RT					Charge compensation effect in Pr1-ySryFe1-xCoxAsO codoped with Sr and Co			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	Phys.Rev.B, 83(2011)014503	X. Lin,H. J. Guo,C. Y. Shen,Y. K. Luo,Q. Tao,G. H. Cao,Z. A. Xu		
152634	PRL105197001	energy gap measured by ARPES.	Fe(Te,Se)	Fe1.03Te0.7Se0.3	Fe	1.03	Te	0.7	Se	0.3																		3	2010																										AB		Chevrel																		K		13					13																																														meV	4	7	12																																															Bridgeman method					Angle-Resolved Photoemission Spectroscopy of the Iron-Chalcogenide Superconductor Fe1.03Te0.7Se0.3: Strong Coupling Behavior and the Universality of Interband Scattering			Department of Physics, Tohoku University, Sendai 980-8578, Japan	Phys.Rev.Lett., 105(2010)197001	K. Nakayama,T. Sato,P. Richard,T. Kawahara,Y. Sekiba,T. Qian,G. F. Chen,J. L. Luo,N. L. Wang,H. Ding,T. Takahashi		
152635	PRL106017003	RT cleaved sample. Two gaps: small gap = 1.05 meV.	SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																		3	2011																										AB6C8		Chevrel																		K		14.2					14.2																																														meV	2.95	5	11																																																				Multiband Superconductivity in the Chevrel Phases SnMo6S8 and PbMo6S8			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.Lett.,106(2011)017003	A. P. Petrovic,R. Lortz,G. Santi,C. Berthod,C. Dubois,M. Decroux,A. Demuer,A. B. Antunes,A. Pare,D. Salloum,P. Gougeon,M. Potel,F. Fischer		
152636	PRL106017003	Two gaps: small one = 0.86 meV by SP-heat measurements	SnMo6S8	Sn1Mo6S8	Sn	1	Mo	6	S	8																		3	2011																										AB6C8		Chevrel																		K		14.2					14.2																				T		42																								meV	3.06		14							mJ/gat.K2	6.4																																												Multiband Superconductivity in the Chevrel Phases SnMo6S8 and PbMo6S8			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.Lett.,106(2011)017003	A. P. Petrovic,R. Lortz,G. Santi,C. Berthod,C. Dubois,M. Decroux,A. Demuer,A. B. Antunes,A. Pare,D. Salloum,P. Gougeon,M. Potel,F. Fischer		
152637	PRL106017003	RT cleaved sample. Two gaps: small gap = 1.36 meV.	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																		3	2011																										AB6C8		Chevrel																		K		14.9					14.9																																														meV	3.06	5	11																																																				Multiband Superconductivity in the Chevrel Phases SnMo6S8 and PbMo6S8			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.Lett.,106(2011)017003	A. P. Petrovic,R. Lortz,G. Santi,C. Berthod,C. Dubois,M. Decroux,A. Demuer,A. B. Antunes,A. Pare,D. Salloum,P. Gougeon,M. Potel,F. Fischer		
152638	PRL106017003	Two gaps: small one = 1.41 meV by SP-heat measurements	PbMo6S8	Pb1Mo6S8	Pb	1	Mo	6	S	8																		3	2011																										AB6C8		Chevrel																		K		14.9					14.9																				T		86																								meV	3.15		14							mJ/gat.K2	6.7																																												Multiband Superconductivity in the Chevrel Phases SnMo6S8 and PbMo6S8			DPMC-MaNEP, Universite de Geneve, Quai Ernest-Ansermet 24, 1211 Geneve 4, Switzerland	Phys.Rev.Lett.,106(2011)017003	A. P. Petrovic,R. Lortz,G. Santi,C. Berthod,C. Dubois,M. Decroux,A. Demuer,A. B. Antunes,A. Pare,D. Salloum,P. Gougeon,M. Potel,F. Fischer		
152639	PRL106017001	Hg2(2+) polycation, Debye-T from simple Debye model. GL-parameter = 38.	HgxReO3	Hg0.44Re1O3	Hg	0.44	Re	1																	O	3		1	2011																										ABC3		bronze	P6<3>/mcm		A	7.366		7.506												K		7.7					7.7	TC152639										Oe	M-H curve	60							T	resistivitymid),extrapolation	4.8												HC152639		A	from Hc2	82			A	from Hc1	3200													mJ/mol.K2	4.9	SP-heat	147	SP-heat																																				cubic-anvil-type high-P synthesis. mixture(HgO,ReO2) - in Au capsule - press(4GPa) - heat(873K,15min)					Superconducting Phase at 7.7 K in the HgxReO3 Compound with a Hexagonal Bronze Structure			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett.,106(2011)017001	Kenya Ohgushi,Ayako Yamamoto,Yoko Kiuchi,Chandreyee Ganguli,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hidenori Takagi		
152640	SSC1510227	RRR = 7.7. H//c. Hc2(0) = 0.6 T by parabolic fitting . T<CDW> = 120K 200K from kink in R(T).	Cu0.1TiSe2	Cu0.1Ti1Se2	Cu	0.1	Ti	1	Se	2																		3	2011																															A			6.042												K		3.9				0.12	3.9																				T	resistivity, WHH			0.67					T/K	resistivity, 0.5Rn			0.25			A	from Hc2		230		A			6100																											uOhm.cm		36										277													transport method					Superconducting and normal state parameters of single crystal Cu0.10TiSe2			Institute of Electrical Engineering, Slovak Academy of Sciences, Dubravska cesta 9, 841 04 Bratislava, Slovakia	Solid State Commun., 151(2011)227	P. Husanikova,J. Kacmarcik,V. Cambel,G. Karapetrov		
152641	CEM1270169	[gamma] < 20 mJ/mol.K2	NdPd2Al3	Nd1Pd2Al3	Nd	1	Pd	2	Al	3																			1996					myu-B/mole	2.28		7.7																				PrNi2Al3			A	5.4419		4.2069												K					1.5																																																										mJ/mol.K2	20																																												Sample Dependence of Magnetic Properties and Determination of Antiferromagnetic Structure of NdPd2Al3			Laboratory for Neutron Scattering, ETH Zurich and Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	J.Solid State Chem., 127(1996)169	A. Donni,H. Kitazawa,P. Fischer,T. Vogt,A. Matsushita,Y. Iimura,M. Zolliker		
152642	PHB1990128		(U,Y)Pd2Al3	U0.99Y0.01Pd2Al3	U	0.99	Y	0.01	Pd	2	Al	3																	1994								14.2																				PrNi2Al3																		K		1.09					1.09																																																																																																					Doping effects on UPd2A13			Institut fur Festkforperphysik, TH Darmstadt, SFB 252. D-64289 Darmstadt, Germany	Physica B, 199&200(1994)128	C. Geibel,C. Schank,F. Jahrling,B. Buschinger,A. Grauel,T. Luhmann,P. Gegenwart,R. Helfrich,P.H.P. Reinders,F. Steglich		
152643	PHB1990128		(U,Y)Pd2Al3	U0.98Y0.02Pd2Al3	U	0.98	Y	0.02	Pd	2	Al	3																	1994								13.7																				PrNi2Al3																		K					0																																																																																																							Doping effects on UPd2A13			Institut fur Festkforperphysik, TH Darmstadt, SFB 252. D-64289 Darmstadt, Germany	Physica B, 199&200(1994)128	C. Geibel,C. Schank,F. Jahrling,B. Buschinger,A. Grauel,T. Luhmann,P. Gegenwart,R. Helfrich,P.H.P. Reinders,F. Steglich		
152644	PHB1990128		(U,Gd)Pd2Al3	U0.99Gd0.01Pd2Al3	U	0.99	Gd	0.01	Pd	2	Al	3																	1994								14																				PrNi2Al3																		K		1.16					1.16																																																																																																					Doping effects on UPd2A13			Institut fur Festkforperphysik, TH Darmstadt, SFB 252. D-64289 Darmstadt, Germany	Physica B, 199&200(1994)128	C. Geibel,C. Schank,F. Jahrling,B. Buschinger,A. Grauel,T. Luhmann,P. Gegenwart,R. Helfrich,P.H.P. Reinders,F. Steglich		
152645	PHB1990128		(U,Gd)Pd2Al3	U0.92Gd0.02Pd2Al3	U	0.92	Gd	0.02	Pd	2	Al	3																	1994								13.8																				PrNi2Al3																		K		0.64					0.64																																																																																																					Doping effects on UPd2A13			Institut fur Festkforperphysik, TH Darmstadt, SFB 252. D-64289 Darmstadt, Germany	Physica B, 199&200(1994)128	C. Geibel,C. Schank,F. Jahrling,B. Buschinger,A. Grauel,T. Luhmann,P. Gegenwart,R. Helfrich,P.H.P. Reinders,F. Steglich		
152646	PHB1990128		(U,Gd)Pd2Al3	U0.95Gd0.05Pd2Al3	U	0.95	Gd	0.05	Pd	2	Al	3																	1994								12.7																				PrNi2Al3																		K					0																																																																																																							Doping effects on UPd2A13			Institut fur Festkforperphysik, TH Darmstadt, SFB 252. D-64289 Darmstadt, Germany	Physica B, 199&200(1994)128	C. Geibel,C. Schank,F. Jahrling,B. Buschinger,A. Grauel,T. Luhmann,P. Gegenwart,R. Helfrich,P.H.P. Reinders,F. Steglich		
152647	PHB3120448	Tc, Neel-T, spin-glass T measured.	(U,Th)Pd2Al3	U0.98Th0.02Pd2Al3	U	0.98	Th	0.02	Pd	2	Al	3																	2002								13.8																		AB2C3		PrNi2Al3																		K		1.97					1.97	MPH152647																																																																																																				Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152648	PHB3120448		(U,Th)Pd2Al3	U0.9Th0.1Pd2Al3	U	0.9	Th	0.1	Pd	2	Al	3																	2002								12.9																		AB2C3		PrNi2Al3																		K		1.28					1.28																																																																																																					Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152649	PHB3120448		(U,La)Pd2Al3	U0.9La0.1Pd2Al3	U	0.9	La	0.1	Pd	2	Al	3																	2002								9																		AB2C3		PrNi2Al3																		K					0																																																																																																							Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152650	PHB3120448	Tc, Neel-T, spin-glass T measured.	(U,La)Pd2Al3	U0.6La0.4Pd2Al3	U	0.6	La	0.4	Pd	2	Al	3																	2002								4.83																		AB2C3		PrNi2Al3																		K					0			MPH152650																																																																																																				Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152651	PHB3120448		(U,La)Pd2Al3	U0.4La0.6Pd2Al3	U	0.4	La	0.6	Pd	2	Al	3																	2002								5																		AB2C3		PrNi2Al3																		K					0																																																																																																							Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152652	PHB3120448	Tc, Neel-T, spin-glass T measured.	(U,Y)Pd2Al3	U0.99Y0.01Pd2Al3	U	0.99	Y	0.01	Pd	2	Al	3																	2002																										AB2C3		PrNi2Al3																		K		1.13					1.13	MPH152652																																																																																																				Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152653	PHB3120448		(U,Y)Pd2Al3	U0.98Y0.02Pd2Al3	U	0.98	Y	0.02	Pd	2	Al	3																	2002																										AB2C3		PrNi2Al3																		K					0																																																																																																							Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152654	PHB3120448		(U,Y)Pd2Al3	U0.8Y0.2Pd2Al3	U	0.8	Y	0.2	Pd	2	Al	3																	2002								6.16																		AB2C3		PrNi2Al3																		K					0																																																																																																							Comparison of magnetic and NFL behavior in U1-xMxPd2Al3 (M = La, Y, Th)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, 9500 Gilman Drive 0350, San Diego, La Jolla, CA 92093-0350, USA	Physica B, 312(2002)448	V.S. Zapf,E.J. Freeman,R.P. Dickey,P.-C. Ho,M.B. Maple		
152655	SSC0070299		KxMoO3	K0.5Mo1O3	K	0.5	Mo	1																	O	3			1969																										ABC3	2	bronze			A	12.36		3.86											tetragonal	K		4.2					4.2																																																																																																samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152656	SSC0070299		KxReO3	K0.3Re1O3	K	0.3	Re	1																	O	3			1969																										ABC3	7	bronze			A	7.335		7.48											hexagonal	K		3.6					3.6																																																																																																samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152657	SSC0070299		NaxMoO3	Na0.3Mo1O3	Na	0.3	Mo	1																	O	3			1969																										ABC3	1	bronze																	cubic	K					1.3																																																																																																		samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152658	SSC0070299		KxMoO3	K0.3Mo1O3	K	0.3	Mo	1																	O	3			1969																										ABC3	1	bronze																	cubic	K					1.3																																																																																																		samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152659	SSC0070299		NaxReO3	Na0.3Re1O3	Na	0.3	Re	1																	O	3			1969																										ABC3	1	bronze																	cubic	K					1.3																																																																																																		samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152660	SSC0070299		ReO3	Re1O3	Re	1																			O	3			1969																										ABC3	1	bronze																	cubic	K					1.3																																																																																																		samples prepared at P = 65 kbar					SUPERCONDUCTING OXIDES OF RHENIUM AND MOLYBDENUM WITH TUNGSTEN BRONZE TYPE STRUCTURES				Solid State Commun., 7(1969)299	A.W. Sleight,T.A. Bither,P.E. Bierstedt		
152661	PRB0203670	Hc2 measured for c-axis and in ab-plane, but absolute values of Hc2 not given (only T-dependency of Hc2)	CexWO3	Cs0.19W1O3	Cs	0.19	W	1																	O	3			1979																										ABC3		bronze																		K		6.7				0.1	6.7																																																																																																single crystals prepared by thermal vapor growth method. Heat(800C,24h, in vac) - heat to 950C(5 or 7 days) - cool to RT(over 24h)					Normal and superconducting properties of CsxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)3670	M.R.Skokan,W.G.Moulton,R.C.Morris		
152662	PRB0203670	[TP300] in DB shows the value at 250 K.	CexWO3	Cs0.23W1O3	Cs	0.23	W	1																	O	3			1979																										ABC3		bronze																		K		6					6	TC152662																																																																	uV/K	-37.1																													single crystals prepared by thermal vapor growth method. Heat(800C,24h, in vac) - heat to 950C(5 or 7 days) - cool to RT(over 24h)					Normal and superconducting properties of CsxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)3670	M.R.Skokan,W.G.Moulton,R.C.Morris		
152663	PRB0203670	[TP300] in DB shows the value at 250 K.	CexWO3	Cs0.25W1O3	Cs	0.25	W	1																	O	3			1979																										ABC3		bronze																		K		4					4	TC152662																																																																	uV/K	-32.5																													single crystals prepared by thermal vapor growth method. Heat(800C,24h, in vac) - heat to 950C(5 or 7 days) - cool to RT(over 24h)					Normal and superconducting properties of CsxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)3670	M.R.Skokan,W.G.Moulton,R.C.Morris		
152664	PRB0203670	[TP300] in DB shows the value at 250 K.	CexWO3	Cs0.3W1O3	Cs	0.3	W	1																	O	3			1979																										ABC3		bronze																		K		2					2	TC152662																																																																	uV/K	-25.2																													single crystals prepared by thermal vapor growth method. Heat(800C,24h, in vac) - heat to 950C(5 or 7 days) - cool to RT(over 24h)					Normal and superconducting properties of CsxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)3670	M.R.Skokan,W.G.Moulton,R.C.Morris		
152665	PRB0203670	angular dependence of Hc2 measured	CexWO3	Cs0.33W1O3	Cs	0.33	W	1																	O	3			1979																										ABC3		bronze																		K					1.4																																																													380	from the paper																																				single crystals prepared by thermal vapor growth method. Heat(800C,24h, in vac) - heat to 950C(5 or 7 days) - cool to RT(over 24h)					Normal and superconducting properties of CsxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)3670	M.R.Skokan,W.G.Moulton,R.C.Morris		
152666	PRB0201903	angular dependence of Hc2 measured	RbxWO3	Rb0.33W1O3	Rb	0.33	W	1																	O	3		3	1979									7.31																	ABC3		bronze																		K		1.98				0.03	1.98																				T	resistivity		0.0297						T/K			0.032																																																																solid state reaction.  Mixtures were heated at 90C for 5 days. Needles were grown.					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)1903	R.K.Stanley,R.C.Morris,W.G.Moulton		
152667	PRB0201903	angular dependence of Hc2 measured	RbxWO3	Rb0.2W1O3	Rb	0.2	W	1																	O	3		3	1979									6.98																	ABC3		bronze																		K		3.52				0.15	3.52																				T	resistivity		4.86	0.8					T/K			2.03	0.333																																																															solid state reaction.  Mixtures were heated at 90C for 5 days. Needles were grown.					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)1903	R.K.Stanley,R.C.Morris,W.G.Moulton		
152668	PRB0201903	angular dependence of Hc2 measured	RbxWO3	Rb0.18W1O3	Rb	0.18	W	1																	O	3		3	1979									6.93																	ABC3		bronze																		K		4.24				0.16	4.24																				T	resistivity			1.364					T/K				0.471																																																															solid state reaction.  Mixtures were heated at 90C for 5 days. Needles were grown.					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)1903	R.K.Stanley,R.C.Morris,W.G.Moulton		
152669	PRB0201903	angular dependence of Hc2 measured	RbxWO3	Rb0.16W1O3	Rb	0.16	W	1																	O	3		3	1979									6.88																	ABC3		bronze																		K		4.8				0.17	4.8																																																																																																solid state reaction.  Mixtures were heated at 90C for 5 days. Needles were grown.					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)1903	R.K.Stanley,R.C.Morris,W.G.Moulton		
152670	PRB0201903	angular dependence of Hc2 measured	RbxWO3	Rb0.25W1O3	Rb	0.25	W	1																	O	3		3	1979									7.11																	ABC3		bronze																		K					0.6																																																																																																		solid state reaction.  Mixtures were heated at 90C for 5 days. Needles were grown.					Conduction properties of the hexagonal tungsten bronze, RbxWO3			Department of Physics, Florida State University, Tallahassee, Florida	Phys.Rev.B, 20(1979)1903	R.K.Stanley,R.C.Morris,W.G.Moulton		
152671	PRB081092507	Tc by SP-heat. GL-parameter = 44. [gap], [cohere], [penet] from muon-SR.	CuxTiSe2	Cu0.06Ti1Se2	Cu	0.06	Ti	1	Se	2																			2010																																														K		2.5					2.5																																				A	muon-SR	150			A	muon-SR	6600			meV	0.27	2.5	16																																															mixture - pellet - (evacuated silica tube) - heat(350C,1h) - heat(650C,20h) cool to RT - ANN(650C,50h) - cool to RT(1C/min)					Probing the superconducting ground state near the charge density wave phase transition in Cu0.06TiSe2			ISIS facility, STFC, Rutherford Appleton Laboratory, Chilton, Oxfordshire OX11 0QX, United Kingdom	Phys.Rev.B, 81(2010)092507	A. D. Hillier,P. Manuel,D. T. Adroja,J. W. Taylor,A. K. Azad,T. S. Irvine		
152672	JPS079014710		La(O,F)(Fe,Mn)As	La1Fe0.9975Mn0.0025As1F0.11O0.89	La	1	Fe	0.9975	Mn	0.0025	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		10.1					10.1																																																																		uV/K	-31.1			TP152672																										See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152673	JPS079014710		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2010																										ABCD		oxypnictide																		K		27					27																																																																		uV/K	-50.1			TP152673																										See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152674	JPS079014710		La(O,F)(Fe,Co)As	La1Fe0.9875Co0.0125As1F0.11O0.89	La	1	Fe	0.9875	Co	0.0125	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		24					24	TC152674																																																																	uV/K	-40.9			TP152674																										See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152675	JPS079014710		La(O,F)(Fe,Co)As	La1Fe0.95Co0.05As1F0.11O0.89	La	1	Fe	0.95	Co	0.05	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		16.1					16.1	TC152674																																																																	uV/K	-45.1			TP152675																										See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152676	JPS079014710		Nd(O,F)(Fe,Mn)As	Nd1Fe0.97Mn0.03As1F0.11O0.89	Nd	1	Fe	0.97	Mn	0.03	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		11.9					11.9	TC152676																																																																																															See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152677	JPS079014710		Nd(O,F)(Fe,Mn)As	Nd1Fe0.98Mn0.02As1F0.11O0.89	Nd	1	Fe	0.98	Mn	0.02	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		27.1					27.1																																																																																																See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152678	JPS079014710		Nd(O,F)(Fe,Mn)As	Nd1Fe0.99Mn0.01As1F0.11O0.89	Nd	1	Fe	0.99	Mn	0.01	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		38					38																																																																																																See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152679	JPS079014710		Nd(O,F)(Fe,Co)As	Nd1Fe0.98Co0.02As1F0.11O0.89	Nd	1	Fe	0.98	Co	0.02	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		40.1					40.1	TC152679																																																																																															See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152680	JPS079014710		Nd(O,F)(Fe,Co)As	Nd1Fe0.95Co0.05As1F0.11O0.89	Nd	1	Fe	0.95	Co	0.05	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		30.1					30.1																																																																																																See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152681	JPS079014710		Nd(O,F)(Fe,Co)As	Nd1Fe0.9Co0.1As1F0.11O0.89	Nd	1	Fe	0.9	Co	0.1	As	1	F	0.11											O	0.89			2010																										ABCD		oxypnictide																		K		9					9																																																																																																See J.Phys.Soc.Jpn  77(2008)103704					Studies on Effects of Impurity Doping and NMR Measurements of La 1111 and/or Nd 1111 Fe-Pnictide Superconductors			Department of Physics, Division of Material Science, Nagoya University, Furo-cho, Chikusa-ku, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 79(2010)014710	Masatoshi SATO,Yoshiaki KOBAYASHI,Sang Chul LEE,Hidefumi TAKAHASHI,Erika SATOMI,Yoko MIURA		
152682	JAC2130509	RRR = 23.	UNi2Al3	U1Ni2Al3	U	1	Ni	2	Al	3																			1994																										AB2C3		PrNi2Al3																		K			1.126			0.46	1.126																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152683	JAC2130509	RRR = 7.	UNi2Al3	U1.02Ni2Al3	U	1.02	Ni	2	Al	3																			1994																										AB2C3		PrNi2Al3																		K			0.51				0.51																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152684	JAC2130509	RRR = 9.	UNi2Al3	U0.98Ni2Al3	U	0.98	Ni	2	Al	3																			1994																										AB2C3		PrNi2Al3																		K			1.145				1.145																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152685	JAC2130509	RRR = 5.	UNi2Al3	U1Ni2.02Al3	U	1	Ni	2.02	Al	3																			1994																										AB2C3		PrNi2Al3																		K			1.14				1.14																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152686	JAC2130509	RRR = 4.	UNi2Al3	U1Ni1.98Al3	U	1	Ni	1.98	Al	3																			1994																										AB2C3		PrNi2Al3																		K			1.13				1.13																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152687	JAC2130509	RRR = 8.	UNi2Al3	U1Ni2Al3.02	U	1	Ni	2	Al	3.02																			1994																										AB2C3		PrNi2Al3																		K			1.135				1.135																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152688	JAC2130509	RRR = 11.	UNi2Al3	U1Ni2Al2.98	U	1	Ni	2	Al	2.98																			1994																										AB2C3		PrNi2Al3																		K			1.155				1.155																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152690	JAC2130509	RRR = 7.	UNi2Al3	U1Ni1.95Al3.05	U	1	Ni	1.95	Al	3.05																			1994																										AB2C3		PrNi2Al3																		K			0.16				0.16																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152691	JAC2130509	RRR = 25.	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																			1994								14.5																		AB2C3		PrNi2Al3																		K		2				0.2	2																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152692	JAC2130509	RRR = 17.	UPd2Al3	U1.01Pd2Al3	U	1.01	Pd	2	Al	3																			1994								14.7																		AB2C3		PrNi2Al3																		K		1.88				0.14	1.88																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152693	JAC2130509	RRR = 15.	UPd2Al3	U0.99Pd2Al3	U	0.99	Pd	2	Al	3																			1994								14.8																		AB2C3		PrNi2Al3																		K		1.94				0.07	1.94																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152694	JAC2130509	RRR = 4.	UPd2Al3	U1Pd2.02Al3	U	1	Pd	2.02	Al	3																			1994								14.9																		AB2C3		PrNi2Al3																		K		0.83				0.25	0.83																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152695	JAC2130509	RRR = 3.	UPd2Al3	U1Pd1.98Al3	U	1	Pd	1.98	Al	3																			1994								14.9																		AB2C3		PrNi2Al3																		K		1.2				0.23	1.2																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152696	JAC2130509	RRR = 5.	UPd2Al3	U1Pd2Al3.03	U	1	Pd	2	Al	3.03																			1994								14.8																		AB2C3		PrNi2Al3																		K		0.61				0.19	0.61																																																																																																arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152697	JAC2130509	RRR = 3.	UPd2Al3	U1Pd2Al2.97	U	1	Pd	2	Al	2.97																			1994								14.5																		AB2C3		PrNi2Al3																		K					0.04																																																																																																		arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
152698	JPS0640378	[phc2]//c-axis ([001]), [nhc2]//c-plane ([100])	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																		3	1995																										AB2C3		PrNi2Al3																		K		2					2																				T			3.9	3.3										MHC152698																																																																			Anomalous susceptibility of UPd2Al3 near the upper critical field			Department of Physics,Faculty of Science,Tohoku University,Sendai	J.Phys.Soc.Jpn, 64(1995)378	A.Ishiguro,A.Sawada,Y.Inada,J.Kimura,M.Suzuki,N.Sato,T.Komatsubara		
152699	MAT1006.3769		Fe2As2Ca5(Mg,Ti)4O9.5	Fe2As2Ca5Mg0.8Ti3.2O9.8	Fe	2	As	2	Ca	5	Mg	0.8	Ti	3.2											O	9.8		1	2010																										AB2C3			I4/mmm		A	3.864		41.05											structure=2254(11)	K			43	39			39																																																																																																					A New Iron Pnictide Oxide superconductor (Fe2As2)(Ca5(Mg,Ti)4Oy)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	cond-mat/1006.3769	Yasuaki Shimizu,Hiraku Ogino,Naoto Kawaguchi,Kohji Kishio,Jun-ichi Shimoyama		
152700	APEX003063103	impurity phasa: CaTiO3, CaO	Fe2As2Ca4(Mg,Ti)3O7	Fe2As2Ca4Mg0.75Ti2.25O7.5	Fe	2	As	2	Ca	4	Mg	0.75	Ti	2.25											O	7.5			2010																													I4/mmm		A	3.877		33.37											structure=22438	K	42		47	43		5	43										100																																																																																						solid state reaction. mixture - pellet - sealed in evacuated quartz - heat(1000-1100C,60-100h) - slow cool to RT					Superconductivity Above 40K Observed in a New Iron Arsenide Oxide (Fe2As2)(Ca4(Mg,Ti)3Oy)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Express, 3(2010)063103	Hiraku Ogino,Yasuaki Shimizu,Koichi Ushiyama,Naoto Kawaguchi,Kohji Kishio,Jun-ichi Shimoyama		
152701	JPCONF234012025		Ni2P2Sr4Sc2O6	Ni2P2Sr4Sc2O6	Ni	2	P	2	Sr	4	Sc	2													O	6			2010																													P4/nmm		A	4.044		15.232											structure=22426, bond angle = 102.6	K		3.6					3.6																																																																																																solid state reaction. mixture - pellet - SIN(1100-1200C,40-120h, in evacuated quartz ampoule)					Structural investigation of new series of nickel-based pnictide oxide superconductors (Ni2Pn2)(Sr4M2O6) (Pn = P, As; M = Sc, V)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.: Conf.Ser., 234(2010)012025	Yutaka Matsumura,Hiraku Ogino,Shigeru Horii,Yukari Katsura,Koichi Ushiyama,Kenji Machida,Kohji Kishio,Jun-ichi Shimoyama		
152702	JPCONF234012025		Ni2As2Sr4Sc2O6	Ni2As2Sr4Sc2O6	Ni	2	As	2	Sr	4	Sc	2													O	6			2010																													P4/nmm		A	4.0787		15.414											structure=22426, bond angle = 104.4	K		2.7					2.7																																																																																																solid state reaction. mixture - pellet - SIN(1100-1200C,40-120h, in evacuated quartz ampoule)					Structural investigation of new series of nickel-based pnictide oxide superconductors (Ni2Pn2)(Sr4M2O6) (Pn = P, As; M = Sc, V)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.: Conf.Ser., 234(2010)012025	Yutaka Matsumura,Hiraku Ogino,Shigeru Horii,Yukari Katsura,Koichi Ushiyama,Kenji Machida,Kohji Kishio,Jun-ichi Shimoyama		
152703	JPCONF234012025		Ni2As2Sr4V2O6	Ni2As2Sr4V2O6	Ni	2	As	2	Sr	4	V	2													O	6			2010																													P4/nmm		A	3.949		15.582											structure=22426, bond angle = 109	K					2																																																																																																		solid state reaction. mixture - pellet - SIN(1100-1200C,40-120h, in evacuated quartz ampoule)					Structural investigation of new series of nickel-based pnictide oxide superconductors (Ni2Pn2)(Sr4M2O6) (Pn = P, As; M = Sc, V)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.: Conf.Ser., 234(2010)012025	Yutaka Matsumura,Hiraku Ogino,Shigeru Horii,Yukari Katsura,Koichi Ushiyama,Kenji Machida,Kohji Kishio,Jun-ichi Shimoyama		
152704	SST023045001		Fe2As2Sr4(Mg,Ti)2O6	Fe2As2Sr4Mg0.9Ti1.1O6	Fe	2	As	2	Sr	4	Mg	0.9	Ti	1.1											O	6			2010																													P4/nmm		A	3.935		15.929											structure=22426	K	14		33				23.5																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152705	SST023045001		Fe2As2Sr4(Mg,Ti)2O6	Fe2As2Sr4Mg0.8Ti1.2O6	Fe	2	As	2	Sr	4	Mg	0.8	Ti	1.2											O	6			2010																													P4/nmm		A	3.936		15.931											structure=22426	K	18		34				26																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152706	SST023045001	Tc(on): max = 43K at P=4.2 GPa.	Fe2As2Sr4(Mg,Ti)2O6	Fe2As2Sr4Mg0.6Ti1.4O6	Fe	2	As	2	Sr	4	Mg	0.6	Ti	1.4											O	6			2010																													P4/nmm		A	3.936		15.904											structure=22426	K	22		36				29			K/GPa	2.5																																																																																												solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152707	SST023045001		Fe2As2Sr4(Mg,Ti)2O6	Fe2As2Sr4Mg0.4Ti1.6O6	Fe	2	As	2	Sr	4	Mg	0.4	Ti	1.6											O	6			2010																													P4/nmm																structure=22426	K	17		39				28																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152708	SST023045001		Fe2As2Sr4(Mg,Ti)2O6	Fe2As2Sr4Mg1Ti1O6	Fe	2	As	2	Sr	4	Mg	1	Ti	1											O	6			2010																													P4/nmm		A	3.935		15.952											structure=22426	K	2		10				6										1.5																																																																																						solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152709	SST023045001		(Fe,Co)2As2Sr4(Mg,Ti)2O6	Fe1.9Co0.1As2Sr4Mg1Ti1O6	Fe	1.9	Co	0.1	As	2	Sr	4	Mg	1	Ti	1									O	6			2010																													P4/nmm		A	3.935		15.943											structure=22426	K	15		26	22			22																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152710	SST023045001		(Fe,Co)2As2Sr4(Mg,Ti)2O6	Fe1.8Co0.2As2Sr4Mg1Ti1O6	Fe	1.8	Co	0.2	As	2	Sr	4	Mg	1	Ti	1									O	6			2010																													P4/nmm		A	3.935		15.912											structure=22426	K	11		26	24			24																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152711	SST023045001		(Fe,Co)2As2Sr4(Mg,Ti)2O6	Fe1.7Co0.3As2Sr4Mg1Ti1O6	Fe	1.7	Co	0.3	As	2	Sr	4	Mg	1	Ti	1									O	6			2010																													P4/nmm		A	3.935		15.905											structure=22426	K	9		18	16			16																																																																																																solid state reaction. heat(1000-1250C,40-72h)					Superconductivity in a new iron pnictide oxide (Fe2As2)(Sr4(Mg, Ti)2O6)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 23(2010)045001	Shinya Sato,Hiraku Ogino,Naoto Kawaguchi,Yukari Katsura,KohjiKishio,Jun-ichi Shimoyama,Hisashi Kotegawa,Hideki Tou		
152712	ZAAC6352242		Fe2As2(Sr2CrO3)2	Fe1As1Sr2Cr1O3	Fe	1	As	1	Sr	2	Cr	1													O	3			2009					myu-B/Cr	3.83	-141	31																					P4/nmm		A	3.9112		15.7905											CuS(Sr2GaO3)-type	K					1.8																																																																																																							The Layered Iron Arsenide Oxides Sr2CrO3FeAs and Ba2ScO3FeAs			Universitat Munchen Butenandtstrasse 5?13 (Haus D) 81377 Munchen, Germany	Z. Anorg. Allg. Chem., 635(2009)2242	Marcus Tegel,Franziska Hummel,Sebastian Lackner,Inga Schellenberg,Rainer Pottgen,Dirk Johrendt		
152713	ZAAC6352242		Fe2As2(Ba2ScO3)2	Fe1As1Ba2Sc1O3	Fe	1	As	1	Ba	2	Sc	1													O	3			2009																													P4/nmm		A	4.1266		16.8											CuS(Sr2GaO3)-type	K					1.8																																																																																																							The Layered Iron Arsenide Oxides Sr2CrO3FeAs and Ba2ScO3FeAs			Universitat Munchen Butenandtstrasse 5?13 (Haus D) 81377 Munchen, Germany	Z. Anorg. Allg. Chem., 635(2009)2242	Marcus Tegel,Franziska Hummel,Sebastian Lackner,Inga Schellenberg,Rainer Pottgen,Dirk Johrendt		
152714	PRB079024516		Fe2As2(Sr3Sc2O5)	Fe2As2Sr3Sc2O5	Fe	2	As	2	Sr	3	Sc	2													O	5			2009																													I4/mmm		A	4.069		26.876											FeAs32522	K					2																																																																																							m3/C						RH152714					solid state reaction. mixture - pellet - sealed in quartz tube(0.2 bar-Ar) - heat(1000C,40h) - slow cool to RT					Sr3Sc2Fe2As2O5 as a possible parent compound for FeAs-based superconductors			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 79(2009)024516	Xiyu Zhu,Fei Han,Gang Mu,Bin Zeng,Peng Cheng,Bing Shen,Hai-Hu Wen		
152715	SST023022001	grain size= 20 um. impurity phase: SrFe2P2. point contact Andreev reflection. data analized using nodal d-wave model.	FeP(Sr2ScO3)	Fe1P1Sr2Sc1O3	Fe	1	P	1	Sr	2	Sc	1													O	3		1	2010																																														K		15					15																																														meV	4.34	6.7	1																																															solid state reaction					Evidence for nodal superconductivity in Sr2ScFePO3			Physics Department, The Blackett Laboratory, Imperial College London, London SW7 2AZ, UK	Supercond. Sci. Technol., 23(2010)022001	K AYates,I T M Usman,K Morrison,J D Moore,A M Gilbertson,A D Caplin,L F Cohen,HOgino,J Shimoyama		
152716	SST022085001		Fe2As2(Sr4Sc2O6)	Fe2As2Sr4Sc2O6	Fe	2	As	2	Sr	4	Sc	2													O	6		1	2009																													P4/nmm		A	4.05		15.809											Cu2S2(Sr4Cr2O6)-type	K					1.8																																																																																																FeAs,SrO,Sr,Cr,Sc2O3(Cr2O3)		solid state reaction. heat(1000-1200C, 24-50h)					New iron-based arsenide oxides (Fe2As2)(Sr4M2O6) (M = Sc, Cr)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond. Sci. Technol., 22(2009)085001	Hiraku Ogino,Yukari Katsura,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
152717	SST022085001	impurity phase: FeAs, SrO	Fe2As2(Sr4Cr2O6)	Fe2As2Sr4Cr2O6	Fe	2	As	2	Sr	4	Cr	2													O	6		1	2009																													P4/nmm		A	3.918		15.683											Cu2S2(Sr4Cr2O6)-type	K					1.8																																																																																																FeAs,SrO,Sr,Cr,Sc2O3(Cr2O3)		solid state reaction. heat(1000-1200C, 24-50h)					New iron-based arsenide oxides (Fe2As2)(Sr4M2O6) (M = Sc, Cr)			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond. Sci. Technol., 22(2009)085001	Hiraku Ogino,Yukari Katsura,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
152718	SST022075008		Fe2P2(Sr4Sc2O6)	Fe2P2Sr4Sc2O6	Fe	2	P	2	Sr	4	Sc	2													O	6		1	2009																													P4/nmm		A	4.016		15.543											22426-type	K	9.8		17	17			17																																																																																														FeP,SrO,Sr,Sc2O3		solid state reaction. mixture - pellet - sealed in evacuated quartz ampoule - heat(900-1200C, 12-40h)					Superconductivity at 17K in (Fe2P2)(Sr4Sc2O6):  a new superconducting layered oxypnictides with thick perovskite oxide layer			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond,Sci.Technol., 22(2009)075008	Hiraku Ogino,Yutaka Matsumura,Yukari Katsura,Koichi Ushiyama,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
152719	PRL106127004	Hall coeff. weak temperature dependence. lattice term of SP (beta=2.22 mJ/mol K4, delta=0.05 mJ/mol.K6). GL-parameter=128. thermal-Hc(0) = 16.7 mT.	CuxBi2Se3	Cu0.29Bi2Se3	Cu	0.29	Bi	2	Se	3																		3	2011																													R3[-]m	166																K	2.8		3.6	3.2			3.2										43	Oe	M-H curve		4.3						T	R=0.5Rn, WHH		3.02	1.71										MHC152719		A	from Hc2		139	79																mJ/mol.K2	1.95	SP-heat																																		n/cm3	130000000000000000000	Bi(6N),Se(5N)		single crystal of Bi2Se3 grown by: heat(800C,48h) - slow cool to 550C(over 48h) - keep(550C,24h) - Cu-intercalation from cleaved surface)					Bulk Superconducting Phase with a Full Energy Gap in the Doped Topological Insulator CuxBi2Se3			Institute of Scientific and Industrial Research, Osaka University, Osaka 567-0047, Japan	Phys.Rev.Lett., 106(2011)127004	M. Kriener,Kouji Segawa,Zhi Ren,Satoshi Sasaki,Yoichi Ando		
152720	JACS1302886	compositions: Yb0.98Ga1.15Si0.87 by EPMA.  RRR = 1.38	YbGaSi	Yb1Ga1.1Si0.9	Yb	1	Ga	1.1	Si	0.9																		1	2008	emu/mol-Yb	0.0000493	emu.K/Yb	0.00901			-4.152		7.336																	ABC		AlB2	P6/mmm	191	A	4.1275		4.2357												K	2.3		2.5	2.4		0.2	2.4										100																																																													mOhm.cm											0.219												Yb(3N),Ga(5N),Si(6N)		arc-melting. ANN(1273K,1h) - slow cool to 1073K(0.1K/min)					Superconductivity in the AlB2-Type Ternary Rare-Earth Silicide YbGa1.1Si0.9			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J. AM. CHEM. SOC., 130(2008)2886	Motoharu Imai,Akira Sato,Takeshi Aoyagi,Takashi Kimura,Yoshitaka Matsushita,Naohito Tsujii		
152721	IOC0468801	Curie-Weis-law for T>86 K. FM order below 8.8 K	EuGaSi	Eu1Ga1Si1	Eu	1	Ga	1	Si	1																		1	2007							8.8																			ABC		AlB2	P6/mmm	191	A	4.1687		4.5543												K					2																																																																																																		arc-melting					Planar versus Puckered Nets in the Polar Intermetallic Series EuGaTt  (Tt = Si, Ge, Sn)				Inorg.Chem., 46(2007)8801	Tae-Soo You,Yuri Grin,Gordon J. Miller		
152722	IOC0468801	Curie-Weis-law for T > 95 K. FM order below 14.5 K	EuGaGe	Eu1Ga1Ge1	Eu	1	Ga	1	Ge	1																		1	2007							14.5																			ABC		YPtAs	P6<3>mmc	194	A	4.2646		18.041												K					2																																																																																																		arc-melting					Planar versus Puckered Nets in the Polar Intermetallic Series EuGaTt  (Tt = Si, Ge, Sn)				Inorg.Chem., 46(2007)8801	Tae-Soo You,Yuri Grin,Gordon J. Miller		
152723	IOC0468801	Curie-Weis-law for T > 116 K. AFM order below 15.2 K	EuGaSn	Eu1Ga1Sn1	Eu	1	Ga	1	Sn	1																		1	2007								15.2																		ABC		YPtAs	P6<3>mmc	194	A	4.5243		18.067												K					2																																																																																																		arc-melting					Planar versus Puckered Nets in the Polar Intermetallic Series EuGaTt  (Tt = Si, Ge, Sn)				Inorg.Chem., 46(2007)8801	Tae-Soo You,Yuri Grin,Gordon J. Miller		
152724	PRB083054517	as-cast sample: Tc=4.8K. residual [gamma] = 7.21 mJ/mol.K2.  Two gaps: large (2d/kTc) =4.26 at Tc , smaller ()=1.02 at Tc/5. [penet] from muon-SR. lattice term in SP(beta) = 0.247 mJ/mol.K4	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		1	2011																										A2B3C5		Sc2Fe3Si5																		K				6.1			6.1																																									A	muon-SR	3530					4.26	14							mJ/mol.K2	24.9	SP-heat																																				Lu(4N),Fe(5N),Si(4N)		arc-melting -heat to 800C(200C/h) - ANN(800C,48h) - ANN(1100C,72h) - cool to 800C(200C/h) - ANN(800C,72h)					Two-gap superconductivity in Lu2Fe3Si5: A transverse-field muon spin rotation study			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 83(2011)054517	P. K. Biswas,G. Balakrishnan,D. McK. Paul,M. R. Lees,A. D. Hillier		
152725	PHC470S356		BiOCuS	Bi1Cu0.9S1O1	Bi	1	Cu	0.9	S	1															O	1			2010																															A	3.8686		8.5682												K				5.8			5.8										4																																																																																						solid sate reaction. SIN(520C)					BiOCuS: A new superconducting compound with oxypnictide-related structure			Departement de Physique de la Matiere Condensee, University of Geneva, 24 quai Ernest-Ansermet, CH-1211 Geneva, Switzerland	Physica C, 470(2010)S356	A. Ubaldini,E. Giannini,C. Senatore,D. van der Marel		
152726	PRB083054511		EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2011								19																		AB2C2		ThCr2Si2			A	3.907		12.114												K					2																																																																																																Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152727	PRB083054511		EuFe2(As,P)2	Eu1Fe2As1.74P0.26	Eu	1	Fe	2	As	1.74	P	0.26																3	2011								17.8																		AB2C2		ThCr2Si2																		K					2																																																																																																Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152728	PRB083054511		EuFe2(As,P)2	Eu1Fe2As1.7P0.3	Eu	1	Fe	2	As	1.7	P	0.3																3	2011																										AB2C2		ThCr2Si2			A	3.891		11.948												K		21					21	MPH152728																																																																																													Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152729	PRB083054511		EuFe2(As,P)2	Eu1Fe2As1.68P0.32	Eu	1	Fe	2	As	1.68	P	0.32																3	2011								18.4																		AB2C2		ThCr2Si2			A	3.89		11.93												K		22					22	MPH152728																																																																																													Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152730	PRB083054511	sharp SC transition. Tc(zero) = 25 K for H = 9 T.	EuFe2(As,P)2	Eu1Fe2As1.6P0.4	Eu	1	Fe	2	As	1.6	P	0.4																3	2011								18.9																		AB2C2		ThCr2Si2			A	3.887		11.89												K		29					29																																																																																														Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152731	PRB083054511	not SC for x >=0.26 in EuFe2(As1-xPx)2	EuFe2(As,P)2	Eu1Fe2As1.48P0.52	Eu	1	Fe	2	As	1.48	P	0.52																3	2011																										AB2C2		ThCr2Si2			A	3.889		11.87												K					2																																																																																																Eu(4N),Fe(4N),As(7N),P(4N)		Bridgman method. mixture - sealed in Ta crucible - heat to 1300C(50C/h) - keep(1300C,12h) - cool to 950C(3C/h)					Interplay of antiferromagnetism, ferromagnetism, and superconductivity in EuFe2(As1-xPx)2 single crystals			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 83(2011)054511	H. S. Jeevan,Deepa Kasinathan,Helge Rosner,Philipp Gegenwart		
152732	PRL105207003	R shows he peak at 18 K <Tc=25 K. Relations of SC and FM were investigated directly using magnetic Compton scattering.	EuFe2(As,P)2	Eu1Fe2As1.46P0.54	Eu	1	Fe	2	As	1.46	P	0.54																1	2010							18																			AB2C2		ThCr2Si2																		K		26					26																																																																																																solid state reaction					Competing Ferromagnetism and Superconductivity on FeAs Layers in EuFe2(As0.73P0.27)2			Department of Chemistry, University of Michigan, Ann Arbor, Michigan 48109, USA	Phys.Rev.Lett., 105(2010)207003	Aamir Ahmed,M. Itou,Shenggao Xu,Zhu'an Xu,Guanghan Cao,Y. Sakurai,James Penner-Hahn,Aniruddha Deb		
152733	PRB083054509	lattice term in SP, (beta) = 1.86 mJ/mol.K4, (delta) = 1.14 E-3 mJ/mol.K6.	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2011																												Bi2201																		K		28					28																																														meV	10.4	8.6	14										226	SP-heat																																				crystals grown by traveling solvent floating zone method					Determination of the superconducting gap in near optimally doped Bi2Sr2-xLaxCuO6+z (x ne 0.4) from low-temperature specific heat			State Key Laboratory for Mesoscopic Physics and School of Physics, Peking University, Beijing 100871, People's Republic of China	Phys.Rev.B, 83(2011)054509	Yue Wang,Zhi-Yong Liu,C. T. Lin,Hai-Hu Wen		
152734	PRL101207002	Energy gaps by STM. small gap = 10.5 meV. large one = 27.2 meV (in DB)	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2008																												Bi2201																		K		32					32																																														meV	27.2	11																																																crystals grown by traveling solvent floating zone method					Coexistence of Competing Orders with Two Energy Gaps in Real and Momentum Space in the High Temperature Superconductor Bi2Sr2-x LaxCuO6+z			Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467, USA	Phys.Rev.Lett., 101(2008)207002	J.-H. Ma,Z.-H. Pan,F. C. Niestemski,M. Neupane,Y.-M. Xu,P. Richard,K. Nakayama,T. Sato,T. Takahashi,H.-Q. Luo,L. Fang,H.-H. Wen,Ziqiang Wang,H. Ding,V. Madhavan		
152735	PRL101207002	Energy gaps by STM. small gap = 7.4 meV. large one = 20.7 meV (in DB)	Bi2(Sr,La)2CuO6	Bi2Sr1.9La0.1Cu1O6+z	Bi	2	Sr	1.9	La	0.1	Cu	1													O	6+z		3	2008																												Bi2201																		K		16					16																																														meV	20.7	11																																																crystals grown by traveling solvent floating zone method					Coexistence of Competing Orders with Two Energy Gaps in Real and Momentum Space in the High Temperature Superconductor Bi2Sr2-x LaxCuO6+z			Department of Physics, Boston College, Chestnut Hill, Massachusetts 02467, USA	Phys.Rev.Lett., 101(2008)207002	J.-H. Ma,Z.-H. Pan,F. C. Niestemski,M. Neupane,Y.-M. Xu,P. Richard,K. Nakayama,T. Sato,T. Takahashi,H.-Q. Luo,L. Fang,H.-H. Wen,Ziqiang Wang,H. Ding,V. Madhavan		
152736	PRB079024514	Energy gap measured by ARPES.	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2009																												Bi2201																		K		32				2	32																																														meV	15.5	12																																																crystals grown by traveling solvent floating zone method					Monotonic d-wave superconducting gap of the optimally doped Bi2Sr1.6La0.4CuO6 superconductor by laser-based angle-resolved photoemission spectroscopy			National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 79(2009)024514	Jianqiao Meng,Wentao Zhang,Guodong Liu,Lin Zhao,Haiyun Liu,Xiaowen Jia,Wei Lu,Xiaoli Dong,Guiling Wang,Hongbo Zhang,Yong Zhou,Yong Zhu,Xiaoyang Wang,Zhongxian Zhao,Zuyan Xu,Chuangtian Chen,X. J. Zhou		
152737	PRB083060512	R<ab>(T) shows maximum at 150 K. anisotropy(Hc2) = 3.0	RbxFe2Se2	Rb0.88Fe1.81Se2	Rb	0.88	Fe	1.81	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.925		14.5655												K	30		32.1	30.6			30.6																				T	R=0.9Rn, WHH		180	59					T/K	resistivity		8.09	2.66	MHC152737																																																												Rb,FeSe		Bridgman method. mixture in quartz tube(vac) - heat(980C,10h) - keep(4h) - melt(1080C,2h) - slow cool to 780C(6C/h) - RT					Superconductivity at 32 K in single-crystalline RbxFe2-ySe2			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 83(2011)060512	A. F. Wang,J. J. Ying,Y. J. Yan,R. H. Liu,X. G. Luo,Z. Y. Li,X. F. Wang,M. Zhang,G. J. Ye,P. Cheng,Z. J. Xiang,X. H. Chen		
152738	APL098042511	compositions: K0.6Fe1.5Se2 from EDX. R<ab>(T) shows maximum at 207 K.. Anisotropy(Hc2) = 3.6	KxFe2Se2	K0.8Fe1.5Se2	K	0.8	Fe	1.5	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9034		14.165												K	31.8		33				32.4																				T	R=0.9Rn, WHH		192	54										MHC152738																																																														nominal(K:FeSe=0.8:2) - alumina crucible in stainless tube - heat(1030C,2h) - cool to 750C(6C/h)					Transport properties of the new Fe-based superconductor KxFe2Se2 (Tc = 33 K)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Appl.Phys.Lett., 98(2011)042511	Yoshikazu Mizuguchi,Hiroyuki Takeya,Yasuna Kawasaki,Toshinori Ozaki,Shunsuke Tsuda,Takahide Yamaguchi,Yoshihiko Takano		
152739	JPCM023052203		CsxFe2Se2	Cs0.8Fe2Se1.96	Cs	0.8	Fe	2	Se	1.96																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9601		15.2846												K				27.4			27.4																																																																																																Bridgman method. ANN and melt(1030C,2h) - cool to 750C(6C/h) - cool to RT(200C/h)					Synthesis and crystal growth of Cs0.8(FeSe0.98)2: a new iron-based superconductor with Tc = 27 K			Laboratory for Developments and Methods, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	J. Phys.: Condens. Matter 23 (2011) 052203	A Krzton-Maziopa,Z Shermadini,E Pomjakushina,V Pomjakushin,M Bendele,A Amato,R Khasanov,H Luetkens,K Conder		
152740	JPCM023052203	lattice conct. a=3.9038, C=14.1148 from NPD.	KxFe2Se2	K0.8Fe2Se1.96	K	0.8	Fe	2	Se	1.96																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9092		14.1353												K				29.5			29.5																																																																																																Bridgman method. ANN and melt(1030C,2h) - cool to 750C(6C/h) - cool to RT(200C/h)					Synthesis and crystal growth of Cs0.8(FeSe0.98)2: a new iron-based superconductor with Tc = 27 K			Laboratory for Developments and Methods, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	J. Phys.: Condens. Matter 23 (2011) 052203	A Krzton-Maziopa,Z Shermadini,E Pomjakushina,V Pomjakushin,M Bendele,A Amato,R Khasanov,H Luetkens,K Conder		
152741	MAT1012.5552	R(max) at 125 K.	KxFe2Se2	K0.86Fe2Se1.82	K	0.86	Fe	2	Se	1.82																		3	2011																										AB2C2		ThCr2Si2	I4/mmm			3.8912		14.139												K	28.7		31	29			29										90										T	resistivity, WHH		208	67					T/K	resistivity		9.86	3.17	MHC152741																																																														self-flux method. K(Cs)+FeSe) - (quartz tube) - heat(1030C,4h) - keep(2h) - cool to 750C(6C/h) - FC to RT					Superconductivity and Magnetic Properties of single crystals of K0.75Fe1.66Se2 and Cs0.81Fe1.61Se2			cond-mat/1012.5552	Phys.Rev.B, 83(2011)212502	J. J. Ying,X. F. Wang,X. G. Luo,A. F. Wang,M. Zhang,Y. J. Yan,Z. J. Xiang,R. H. Liu,P. Cheng,G. J. Ye,X. H. Chen		
152742	MAT1012.5552	no peak in R(T).	CsxFe2Se2	Cs0.86Fe1.66Se2	Cs	0.86	Fe	1.66	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm			3.9618		15.285												K	26.5		30	25.5			25.5										100										T	resistivity, WHH		126	43					T/K	resistivity		6.21	2.13	MHC152742																																																														self-flux method. K(Cs)+FeSe) - (quartz tube) - heat(1030C,4h) - keep(2h) - cool to 750C(6C/h) - FC to RT					Superconductivity and Magnetic Properties of single crystals of K0.75Fe1.66Se2 and Cs0.81Fe1.61Se2			cond-mat/1012.5552	Phys.Rev.B, 83(2011)212502	J. J. Ying,X. F. Wang,X. G. Luo,A. F. Wang,M. Zhang,Y. J. Yan,Z. J. Xiang,R. H. Liu,P. Cheng,G. J. Ye,X. H. Chen		
152743	PRB083100503	gap measured by broad-band infrared spectroscopy. s-wave gap	EuFe2(As,P)2	Eu1Fe1As1.64P0.36	Eu	1	Fe	1	As	1.64	P	0.36																3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K		28					28																																									A	infrared spectroscopy	3000			meV	4.75	3.7	2																																															See Phys.Rev.B, 78(2008)092406					Optical investigations of chemically pressurized EuFe2(As1-xPx)2: An s-wave superconductor with strong interband interactions			Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, DE-70550 Stuttgart, Germany	Phys.Rev.B, 83(2011)100503	D. Wu,G. Chanda,H. S. Jeevan,P. Gegenwart,M. Dressel		
152744	PRB083100513	crystal size = 108*95*7 um3. [ncohere] estimated from anisotropy(=8). Thermodynamic Hc2(0) = 1.24 T. GL parameter = 99.	Sm(O,F)FeAs	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85		3	2011																										ABCD		oxypnictide																		K		49.5					49.5																													T/K	SP-heat			3.5			A	from Hc2		14	1.8																mJ/mol.K2	8	SP and entropy																																						high-P synthesis using NaCl/KCl flux.					Anisotropic phase diagram and superconducting fluctuations of single-crystalline SmFeAsO0.85F0.15			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 83(2011)100513	U. Welp,C. Chaparro,A. E. Koshelev,W. K. Kwok,A. Rydh,N. D. Zhigadlo,J. Karpinski,S. Weyeneth		
152745	PRB083104414	T<STR>(T-to-O) = 153 K and T<AFM> = 153 K by neutron diffraction. moment shows /Fe-stite.	Ca(Fe,Co)2As2	Ca1Fe1.936Co0.064As2	Ca	1	Fe	1.936	Co	0.064	As	2																3	2011					myu-B/mol	0.747		153																		AB2C2		ThCr2Si2	I4/mmm																	K					5																																																																																																CaAs,Fe2As,Co2As		mixture - pellet - sealed in quartz ampoule(vac) - heat(850C) - SIN(1090C,24h) slow cool to 600C					Effect of Co substitution on the magnetic order in Ca(Fe1-xCox)2As2 single crystals studied by neutron diffraction			Helmholtz-Zentrum Berlin fur Materialien und Energie, M-I1, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 83(2011)104414	K. Prokes,S. Mat'as,L. Harnagea,S. Singh,S. Wurmehl,D. N. Argyriou,B. Buchner		
152746	PRB083104414	T<STR>(T-to-O) = 136 K and T<AFM> = 133 K by neutron diffraction. moment shows /Fe-stite.	Ca(Fe,Co)2As2	Ca1Fe1.922Co0.078As2	Ca	1	Fe	1.922	Co	0.078	As	2																3	2011					myu-B/mol	0.703		133																		AB2C2		ThCr2Si2	I4/mmm																	K		21.2					21.2																																																																																														CaAs,Fe2As,Co2As		mixture - pellet - sealed in quartz ampoule(vac) - heat(850C) - SIN(1090C,24h) slow cool to 600C					Effect of Co substitution on the magnetic order in Ca(Fe1-xCox)2As2 single crystals studied by neutron diffraction			Helmholtz-Zentrum Berlin fur Materialien und Energie, M-I1, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 83(2011)104414	K. Prokes,S. Mat'as,L. Harnagea,S. Singh,S. Wurmehl,D. N. Argyriou,B. Buchner		
152747	PRB083104414	T<STR>(T-to-O) = 129 K and T<AFM> = 120 K by neutron diffraction. moment shows /Fe-stite.	Ca(Fe,Co)2As2	Ca1Fe1.898Co0.102As2	Ca	1	Fe	1.898	Co	0.102	As	2																3	2011					myu-B/mol	0.561		120																		AB2C2		ThCr2Si2	I4/mmm																	K		19.9					19.9																																																																																														CaAs,Fe2As,Co2As		mixture - pellet - sealed in quartz ampoule(vac) - heat(850C) - SIN(1090C,24h) slow cool to 600C					Effect of Co substitution on the magnetic order in Ca(Fe1-xCox)2As2 single crystals studied by neutron diffraction			Helmholtz-Zentrum Berlin fur Materialien und Energie, M-I1, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 83(2011)104414	K. Prokes,S. Mat'as,L. Harnagea,S. Singh,S. Wurmehl,D. N. Argyriou,B. Buchner		
152748	PRB083104414	T<STR>(T-to-O) = 105 K and T<AFM> = 94 K by neutron diffraction. moment shows /Fe-stite.	Ca(Fe,Co)2As2	Ca1Fe1.888Co0.112As2	Ca	1	Fe	1.888	Co	0.112	As	2																3	2011					myu-B/mol	0.475		94																		AB2C2		ThCr2Si2	I4/mmm																	K		16.5					16.5																																																																																														CaAs,Fe2As,Co2As		mixture - pellet - sealed in quartz ampoule(vac) - heat(850C) - SIN(1090C,24h) slow cool to 600C					Effect of Co substitution on the magnetic order in Ca(Fe1-xCox)2As2 single crystals studied by neutron diffraction			Helmholtz-Zentrum Berlin fur Materialien und Energie, M-I1, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 83(2011)104414	K. Prokes,S. Mat'as,L. Harnagea,S. Singh,S. Wurmehl,D. N. Argyriou,B. Buchner		
152749	PRB083104414	T<STR>(T-to-O)  and T<AFM> not obseved by neutron diffraction.	Ca(Fe,Co)2As2	Ca1Fe1.874Co0.126As2	Ca	1	Fe	1.874	Co	0.126	As	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K		14.8					14.8																																																																																														CaAs,Fe2As,Co2As		mixture - pellet - sealed in quartz ampoule(vac) - heat(850C) - SIN(1090C,24h) slow cool to 600C					Effect of Co substitution on the magnetic order in Ca(Fe1-xCox)2As2 single crystals studied by neutron diffraction			Helmholtz-Zentrum Berlin fur Materialien und Energie, M-I1, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 83(2011)104414	K. Prokes,S. Mat'as,L. Harnagea,S. Singh,S. Wurmehl,D. N. Argyriou,B. Buchner		
152750	PRB083064504	RRR = 12. R(max) at 26 K. P<crit> = 2.1 GPa(Tc(on) go to zero). For P=0.45 GPa, Hc2(0)=2.2 T, [cohere] = 122 A.	Ce2PdIn8	Ce2Pd1In8	Ce	2	Pd	1	In	8																		1	2011																										AB2C8		Ho2CoGa8																		K		0.7					0.7			K/GPa	0.15																T	resistivity, extrapolation	2.5							T/K	resistivity	16					A	from Hc2	105																																	uOhm.cm							6.58																Ce(3N),Pd(3N),In(6N)		arc-melting					Superconductivity and non-Fermi-liquid behavior of Ce2PdIn8			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410, PL-50-950 Wroc?aw, Poland	Phys.Rev.B, 83(2011)064504	V. H. Tran,D. Kaczorowski,R. T. Khan,E. Bauer		
152751	PRB083064522	RRR=60. Debye-T = 348 K from resistivity analysis. Type-I SC (GL parameter = 0.25, then Hc2 in DB shows thermodynamic Hc(0). e-ph coupling = 0.499. (dC/gamma*Tc) = 1.25	LaRhSi3	La1Rh1Si3	La	1	Rh	1	Si	3																		1	2011																										ABC3		BaNiSn3	I4mm		A	4.2694		9.8357												K		2.16	2.24				2.16										100										T	SP-heat	0.0171														A		1750			A		440			meV	0.3	3.24	14					mJ/mol.K	16	mJ/mol.K2	6.04	SP-heat	357	SP-heat											uOhm.cm							1.08																		arc-melting					Specific heat and myu-SR study on the noncentrosymmetric superconductor LaRhSi3			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom	Phys.Rev.B, 83(2011)064522	V. K. Anand,A. D. Hillier,D. T. Adroja,A. M. Strydom,H. Michor,K. A. McEwen,B. D. Rainford		
152752	PRB083100502	energy gap measured by tunneling diode resonator.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K		17.5	18.2				17.5																																									A	tunneling	2800					2.18	1																																															Bridgman method using W-crucible.					Nodeless two-gap superconducting state in single crystals of the stoichiometric iron pnictide LiFeAs			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)100502	H. Kim,M. A. Tanatar,Yoo Jang Song,Yong Seung Kwon,R. Prozorov		
152753	PRB083100501	RRR = 7. P-induced SC. SC properties measured at P=2.5 GPa. AFM ordered T of Eu moment =20 K, AFM ordered T in FeAs plane =190 K at P=0.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																		K		30			0		30																				T	resistivity, extrapolation		24.7	21.5										MHC152753																																																														Bridgman method					Upper critical field of the pressure-induced superconductor EuFe2As2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan	Phys.Rev.B, 83(2011)100501	Nobuyuki Kurita,Motoi Kimata,Kota Kodama,Atsushi Harada,Megumi Tomita,Hiroyuki S. Suzuki,Takehiko Matsumoto,Keizo Murata,Shinya Uji,Taichi Terashima		
152754	PRB083094511	lattice term coeff. in SP (beta)=0.75 mJ/mol.K4 Tc=2.65 K  from SP(mid).	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		3	2011																										AB2C2		ThCr2Si2			A	4.4129		10.1204												K				2.7			2.7																				T	magnetization, WHH		0.4927	0.4921					T/K	magnetization		0.2653	0.264			A	from Hc2		214.8	214.5																mJ/mol.K2	7.8	SP-heat	235	SP-heat																																				self-flux method. (Sr:Pd:Ge=1:5:5) - (sealed in quartz tube, Ar) - heat to 1100C (200C/h) - keep(1100C,2d) - cool to 850C (3C/h)					Superconductivity and anomalous transport in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	Phys.Rev.B, 83(2011)094511	N. H. Sung,Jong-Soo Rhyee,B. K. Cho		
152755	PRB079224522	RRR = 12. Thermodynamic Hc(0) = 770 Oe.	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.4088		10.127												K	3.03		3.09	3.04			3.04											Oe	M-H curve	180							T	magnetization, WHH	0.18							T/K	magnetization	0.084			MHC152755		A	from Hc2	433			A	Hc1, Hc(0)	711																												uOhm.cm							2.5				30												Sr(2N),Pd(3N),Ge(4N)		arc-melting - wrapped in Ti-foil  - ANN(1173 K. 1w, in silica tube)					Superconductivity in SrPd2Ge2			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 79(2009)224522	H. Fujii,A. Sato		
152756	PRL102147004	Hc2 defined as mid point of SP-transition. Thermal conductivity measured for current q//[100]	BaNi2As2	Ba1Ni2As2	Ba	1	Ni	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K		0.68					0.68																				T	SP-heat, WHH	0.11							T/K	SP-heat	0.226					A	from Hc2	550								meV	0.0946	3.22	14							mJ/mol.K2	12.3																																							Pb-flux method					Low-Temperature Magnetothermal Transport Investigation of a Ni-Based Superconductor BaNi2As2: Evidence for Fully Gapped Superconductivity			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 102(2009)147004	N. Kurita,F. Ronning,Y. Tokiwa,E. D. Bauer,A. Subedi,D. J. Singh,J. D. Thompson,R. Movshovich		
152757	JPCM020342203	T<SDW> = 130 K. Hc2 defined as R(zero). lattice term coeff. in SP (beta) = 1.10 mJ/mol.K4	BaNi2As2	Ba1Ni2As2	Ba	1	Ni	2	As	2																		3	2008																										AB2C2		ThCr2Si2			A	4.112		11.54												K		0.68					0.68																				T	resistivity, WHH		0.19	0.09					T/K	resistivity		0.396	0.186	MHC152757		A	from Hc2		420	610															11.15	mJ/mol.K2	10.8	SP-heat	206	SP-heat																																				Pb-flux method. (Ba:Ni:As:Pb=1:2:2:20) - alumina crucible - quartz tube - heat to 900C(100C/h) - hold(1075C,4h) - cool to 650C(7C/h)					The first order phase transition and superconductivity in BaNi2As2 single crystals			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	J. Phys.: Condens. Matter 20 (2008) 342203	F Ronning,N Kurita,E D Bauer,B L Scott,T Park,T Klimczuk,R Movshovich,J D Thompson		
152758	PRB083094523	not SC. RRR = 3.6. structural transition at T=166 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2011								155																		AB2C2		ThCr2Si2																		K																																																																																																							crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152759	PRB083094523	RRR = 1.97. structural transition at T=155 K. Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.94Co0.06As2	Ca	1	Fe	1.94	Co	0.06	As	2																3	2011								154																		AB2C2		ThCr2Si2																		K			15.5				15.5																																																																																																crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152760	PRB083094523	RRR = 1.29. structural transition at T=142 K. Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.9Co0.1As2	Ca	1	Fe	1.9	Co	0.1	As	2																3	2011								142																		AB2C2		ThCr2Si2																		K			17.7				17.7										0																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152761	PRB083094523	RRR = 5.08. structural transition at T=108 K.  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.85Co0.15As2	Ca	1	Fe	1.85	Co	0.15	As	2																3	2011								108																		AB2C2		ThCr2Si2																		K			18	15.2		2.9	15.2										43																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152762	PRB083094523	RRR = 15.1 Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.82Co0.18As2	Ca	1	Fe	1.82	Co	0.18	As	2																3	2011																										AB2C2		ThCr2Si2																		K			15.7			2.65	15.7										86																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152763	PRB083094523	RRR = 18.0  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.8Co0.2As2	Ca	1	Fe	1.8	Co	0.2	As	2																3	2011																										AB2C2		ThCr2Si2																		K			18	17.1		3.16	17.1										63																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152764	PRB083094523	RRR = 12.8  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.75Co0.25As2	Ca	1	Fe	1.75	Co	0.25	As	2																3	2011																										AB2C2		ThCr2Si2																		K			8.3	14.1		9.2	14.1										41																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152765	PRB083094523	RRR = 13.9  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.73Co0.27As2	Ca	1	Fe	1.73	Co	0.27	As	2																3	2011																										AB2C2		ThCr2Si2																		K			8.3	12		8.48	12										22.8																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152766	PRB083094523	RRR = 12.0  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.7Co0.3As2	Ca	1	Fe	1.7	Co	0.3	As	2																3	2011																										AB2C2		ThCr2Si2																		K			10.8				10.8										5.5																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152767	PRB083094523	RRR = 9.84  Co-content x shows nominal value. [EDX] = 0.7*[nominal]	Ca(Fe,Co)2As2	Ca1Fe1.6Co0.4As2	Ca	1	Fe	1.6	Co	0.4	As	2																3	2011																										AB2C2		ThCr2Si2																		K							2										0																																																																																						crystals grown by Sn-flux method. (pellet:Sn = 1:30) - (in alumina crucible) - heat(1090C,24h) - cool to 600C(2.5C/h) FC to RT					Phase diagram of the iron arsenide superconductors Ca(Fe1-xCox)2As2 (0 =< x =< 0.2)			Leibniz-Institute for Solid State and Materials Research, (IFW)-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 83(2011)094523	L. Harnagea,S. Singh,G. Friemel,N. Leps,D. Bombor,M. Abdel-Hafiez,A. U. B. Wolter,C. Hess,R. Klingeler,G. Behr,S. Wurmehl,B. Buchner		
152768	PRB083094520	Co-content by WDS. structural transition at T=130 K.	Sr(Fe,Co)2As2	Sr1Fe1.916Co0.084As2	Sr	1	Fe	1.916	Co	0.084	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9313		12.329												K							2																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152769	PRB083094520	Co-content by WDS. structural transition at T=105 K.	Sr(Fe,Co)2As2	Sr1Fe1.888Co0.112As2	Sr	1	Fe	1.888	Co	0.112	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9333		12.313												K							2																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152770	PRB083094520	Co-content by WDS. structural transition at T=57.6 K.	Sr(Fe,Co)2As2	Sr1Fe1.86Co0.14As2	Sr	1	Fe	1.86	Co	0.14	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9319		12.31												K	10.4		12.7	7.2			7.2																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152771	PRB083094520	Co-content by WDS. structural transition at T=28.4 K.	Sr(Fe,Co)2As2	Sr1Fe1.826Co0.174As2	Sr	1	Fe	1.826	Co	0.174	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9339		12.295												K	10.9		13.7	9.5			9.5																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152772	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.816Co0.184As2	Sr	1	Fe	1.816	Co	0.184	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9313		12.285												K	13.6		16.5	13.4			13.4	MTC152773																																																																																															self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152773	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.792Co0.208As2	Sr	1	Fe	1.792	Co	0.208	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9323		12.283												K	14.7		18	13.9			13.9	MTC152773																																																																																															self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152774	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.766Co0.234As2	Sr	1	Fe	1.766	Co	0.234	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9334		12.279												K	16.4		18.7	14.4			14.4																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152775	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.752Co0.248As2	Sr	1	Fe	1.752	Co	0.248	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9305		12.266												K	16.6		18.6	13.2			13.2																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152776	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.732Co0.268As2	Sr	1	Fe	1.732	Co	0.268	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9336		12.265												K	14.2		16.5	11			11																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152777	PRB083094520	Co-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.66Co0.34As2	Sr	1	Fe	1.66	Co	0.34	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9356		12.261												K	8.9		11.3	5.56			5.56																																																																																																self-flux method. nominal = (Sr:FeAs:CoAs = 1:(4-4x):4x).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152778	PRB083094520	Eu-content by WDS.	Sr(Fe,Co)2As2	Sr1Fe1.76Co0.24As2	Sr	1	Fe	1.76	Co	0.24	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.9333		12.278												K	16.6		18.6	13.5			13.5																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152779	PRB083094520	Eu-content by WDS.	(Sr,Eu)(Fe,Co)2As2	Sr0.958Eu0.042Fe1.76Co0.24As2	Sr	0.958	Eu	0.042	Fe	1.76	Co	0.24	As	2														3	2011																										AB2C2		ThCr2Si2			A	3.9312		12.274												K	16.2		19	13.3			13.3																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152780	PRB083094520	Eu-content by WDS.	(Sr,Eu)(Fe,Co)2As2	Sr0.85Eu0.15Fe1.76Co0.24As2	Sr	0.85	Eu	0.15	Fe	1.76	Co	0.24	As	2														3	2011																										AB2C2		ThCr2Si2			A	3.9314		12.258												K	15.6		17.8	12.5			12.5	MTC152780																																																																																															self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152781	PRB083094520	Eu-content by WDS.	(Sr,Eu)(Fe,Co)2As2	Sr0.81Eu0.19Fe1.76Co0.24As2	Sr	0.81	Eu	0.19	Fe	1.76	Co	0.24	As	2														3	2011																										AB2C2		ThCr2Si2			A	3.9302		12.228												K	15.3		16.3	12			12	MTC152780																																																																																															self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152782	PRB083094520	Eu-content by WDS.	(Sr,Eu)(Fe,Co)2As2	Sr0.66Eu0.34Fe1.76Co0.24As2	Sr	0.66	Eu	0.34	Fe	1.76	Co	0.24	As	2														3	2011																										AB2C2		ThCr2Si2			A	3.9276		12.189												K	11.6		14.9	9.82			9.82																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152783	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.57Eu0.43Fe1.76Co0.24As2	Sr	0.57	Eu	0.43	Fe	1.76	Co	0.24	As	2														3	2011								3.52																		AB2C2		ThCr2Si2			A	3.9252		12.168												K	11.7		13.5	8.78			8.78																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152784	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.5Eu0.5Fe1.76Co0.24As2	Sr	0.5	Eu	0.5	Fe	1.76	Co	0.24	As	2														3	2011								4.51																		AB2C2		ThCr2Si2			A	3.9258		12.16												K	10.2		15.3	8.45			8.45																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152785	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.4Eu0.6Fe1.76Co0.24As2	Sr	0.4	Eu	0.6	Fe	1.76	Co	0.24	As	2														3	2011								6.27																		AB2C2		ThCr2Si2			A	3.9243		12.133												K	9.97		13.4	7.97			7.97																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152786	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.28Eu0.72Fe1.76Co0.24As2	Sr	0.28	Eu	0.72	Fe	1.76	Co	0.24	As	2														3	2011								9.52																		AB2C2		ThCr2Si2			A	3.9258		12.112												K			12.3				12.3																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152787	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.15Eu0.85Fe1.76Co0.24As2	Sr	0.15	Eu	0.85	Fe	1.76	Co	0.24	As	2														3	2011								11.8																		AB2C2		ThCr2Si2			A	3.9211		12.073												K							2																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152788	PRB083094520	Eu-content by WDS. Tn by SUS.	(Sr,Eu)(Fe,Co)2As2	Sr0.05Eu0.95Fe1.76Co0.24As2	Sr	0.05	Eu	0.95	Fe	1.76	Co	0.24	As	2														3	2011								14.4																		AB2C2		ThCr2Si2			A	3.9226		12.047												K							2																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152789	PRB083094520	Eu-content by WDS. Tn by SUS.	Eu(Fe,Co)2As2	Eu1Fe1.76Co0.24As2	Eu	1	Fe	1.76	Co	0.24	As	2																3	2011								16.8																		AB2C2		ThCr2Si2			A	3.9194		12.023												K							2																																																																																																self-flux method. nominal = (Sr:Eu:FeAs:CoAs = 1:(1-x):x:3.44:0.56).  heat(1180C) - slow cool to 1000C, ANN(500C,24h, in Ar)					Phase diagram of superconductivity and antiferromagnetism in single crystals of Sr(Fe1-xCox)2As2 and Sr1-yEuy(Fe0.88Co0.12)2As2			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)094520	Rongwei Hu,Sergey L. Bud'ko,Warren E. Straszheim,Paul C. Canfield		
152790	PRB083140508	Energy gap (isotropic) measured by ARPES at near the M point.	KxFe2Se2	K0.68Fe1.79Se2	K	0.68	Fe	1.79	Se	2																		3	2011																																														K		32				1	32																																														meV	9		12																																															Bridgeman method					Common Fermi-surface topology and nodeless superconducting gap of K0.68Fe1.79Se2 and (Tl0.45K0.34)Fe1.84Se2 superconductors revealed via angle-resolved photoemission			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 83(2011)140508	Lin Zhao,Daixiang Mou,Shanyu Liu,Xiaowen Jia,Junfeng He,Yingying Peng,Li Yu,Xu Liu,Guodong Liu,Shaolong He,Xiaoli Dong,Jun Zhang,J. B. He,D. M. Wang,G. F. Chen,J. G. Guo,X. L. Chen,Xiaoyang Wang,Qinjun Peng,Zhimin Wang		
152791	PRB083140508	Energy gap (isotropic) measured by ARPES at near the M point.	(K,Tl)xFe2Se2	Tl0.45K0.34Fe1.84Se2	Tl	0.45	K	0.34	Fe	1.84	Se	2																3	2011																																														K		28				1	28																																														meV	8		12																																															Bridgeman method					Common Fermi-surface topology and nodeless superconducting gap of K0.68Fe1.79Se2 and (Tl0.45K0.34)Fe1.84Se2 superconductors revealed via angle-resolved photoemission			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 83(2011)140508	Lin Zhao,Daixiang Mou,Shanyu Liu,Xiaowen Jia,Junfeng He,Yingying Peng,Li Yu,Xu Liu,Guodong Liu,Shaolong He,Xiaoli Dong,Jun Zhang,J. B. He,D. M. Wang,G. F. Chen,J. G. Guo,X. L. Chen,Xiaoyang Wang,Qinjun Peng,Zhimin Wang		
152792	PRB083104508	compositions : K0.65Fe1.41Se2.0 by EDX. [penet] measured  at T=8K by NMR line broadening. gap by ARPES	KxFe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2011																																														K		33					33																																									A	NMR, 8K		2900				5.6	12																																															self-flux method					<77>Se NMR investigation of the KxFe2-ySe2 high-Tc superconductor (Tc = 33 K)			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada	Phys.Rev.B, 83(2011)104508	D. A. Torchetti,M. Fu,D. C. Christensen,K. J. Nelson,T. Imai,H. C. Lei,C. Petrovic		
152793	CM0224690		Yb(Ga,Si)2	Yb1Ga1.15Si0.85	Yb	1	Ga	1.15	Si	0.85																		1	2010			emu.K/mol	0.0234			-20																					AlB2	P6/mmm		A	4.1315		4.2378												K				2.6			2.6	MTC152793																																																																																															arc-melting - ANN(1073 K,10d, in Ta-foil)					Phase Stability and Superconducting Properties of AlB2-Type YbGaxSi2-x (1.12 =< x =< 1.49)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Chem.Mater., 22(2010)4690	Naohito Tsujii,Motoharu Imai,Ignace Jarrige,Hirofumi Oohashi,Tatsunori Tochio,Katsumi Handa,Junko Ide,Hideki Atsuta,Yoshiaki Ito,Hideki Yoshikawa,Hideaki Kitazawa		
152794	ACS1302886	RRR=1.38. Hc2(2.0K) is nearly 3.0 kOe	Yb(Ga,Si)2	Yb1Ga1.1Si0.9	Yb	1	Ga	1.1	Si	0.9																		3	2008	emu/mol-Yb	0.0000493	emu.K/mol	0.00901			-4.152		7.336																			AlB2	P6/mmm		A	4.1275		4.2357												K	2.3	2.4	2.5			0.2	2.4																																																																							mOhm.cm											0.219												Yb(3N),Ga(5N),Si(6N)		arc-melting(Yb:Ga:Si=1.1:15:0.85) - ANN(1273K, 1h) - cool to 1073 K(0.1 K/min)					Superconductivity in the AlB2-Type Ternary Rare-Earth Silicide YbGa1.1Si0.9			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Am.Chem.Soc., 130(2008)2886	Motoharu Imai,Akira Sato,Takeshi Aoyagi,Takashi Kimura,Yoshitaka Matsushita,Naohito Tsujii		
152795	PRB083104519	RRR=21. gap measured by point contact Andreev reflection. I /n [001]	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2011																												LuNi2B2C																		K	16					0.53	16																																														meV	2.4	3.48	1																																															solid state reaction. mixture(Sr,PtAs2,Pt) - (alumina crucible) - (evacuated silica tube) - heat(700C,10h+1100C,24h) - (wrapped in Ta-foil) - heat(700C,10h)					Superconducting order parameter in nonmagnetic borocarbides RNi2B2C (R =Y, Lu) probed by point-contact Andreev reflection spectroscopy			Department of Physics and the Frederick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 83(2011)104519	X. Lu,W. K. Park,S. Yeo,K.-H. Oh,S.-I. Lee,S. L. Bud'ko,P. C. Canfield,L. H. Greene		
152796	PRB083104519	RRR=21. gap measured by point contact Andreev reflection. I /n [110]	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2011																												LuNi2B2C																		K	16.1					0.2	16.1																																														meV	2.6	3.75	1																																															solid state reaction. mixture(Sr,PtAs2,Pt) - (alumina crucible) - (evacuated silica tube) - heat(700C,10h+1100C,24h) - (wrapped in Ta-foil) - heat(700C,10h)					Superconducting order parameter in nonmagnetic borocarbides RNi2B2C (R =Y, Lu) probed by point-contact Andreev reflection spectroscopy			Department of Physics and the Frederick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 83(2011)104519	X. Lu,W. K. Park,S. Yeo,K.-H. Oh,S.-I. Lee,S. L. Bud'ko,P. C. Canfield,L. H. Greene		
152797	PRB083104519	RRR=20. gap measured by point contact Andreev reflection. I /n [100]	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2011																												LuNi2B2C																		K	15					0.5	15																																														meV	2.3	3.56	1																																															solid state reaction. mixture(Sr,PtAs2,Pt) - (alumina crucible) - (evacuated silica tube) - heat(700C,10h+1100C,24h) - (wrapped in Ta-foil) - heat(700C,10h)					Superconducting order parameter in nonmagnetic borocarbides RNi2B2C (R =Y, Lu) probed by point-contact Andreev reflection spectroscopy			Department of Physics and the Frederick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 83(2011)104519	X. Lu,W. K. Park,S. Yeo,K.-H. Oh,S.-I. Lee,S. L. Bud'ko,P. C. Canfield,L. H. Greene		
152798	PRB083104519	RRR=26. gap measured by point contact Andreev reflection. I //ab-plane. gap=2.5 meV, (2d/kTc)=3.60 for [001] and 2.7 meV, 3.89 for [001]	LuNi2B2C	Lu1Ni2B2C1	Lu	1	Ni	2	B	2	C	1																3	2011																												LuNi2B2C																		K	16.1					0.56	16.1																																														meV	2.8	4.04	1																																															solid state reaction. mixture(Sr,PtAs2,Pt) - (alumina crucible) - (evacuated silica tube) - heat(700C,10h+1100C,24h) - (wrapped in Ta-foil) - heat(700C,10h)					Superconducting order parameter in nonmagnetic borocarbides RNi2B2C (R =Y, Lu) probed by point-contact Andreev reflection spectroscopy			Department of Physics and the Frederick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 83(2011)104519	X. Lu,W. K. Park,S. Yeo,K.-H. Oh,S.-I. Lee,S. L. Bud'ko,P. C. Canfield,L. H. Greene		
152799	PRB083104519	RRR=24. gap measured by point contact Andreev reflection. I //ab-plane. gap=2.0 meV, (2d/kTc)=3.00 for [001] and 2.5 meV, 4.04 for [001]	YNi2B2C	Y1Ni2B2C1	Y	1	Ni	2	B	2	C	1																3	2011																												LuNi2B2C																		K	15.5					0.15	15.5																																														meV	2.1	3.15	1																																															solid state reaction. mixture(Sr,PtAs2,Pt) - (alumina crucible) - (evacuated silica tube) - heat(700C,10h+1100C,24h) - (wrapped in Ta-foil) - heat(700C,10h)					Superconducting order parameter in nonmagnetic borocarbides RNi2B2C (R =Y, Lu) probed by point-contact Andreev reflection spectroscopy			Department of Physics and the Frederick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 83(2011)104519	X. Lu,W. K. Park,S. Yeo,K.-H. Oh,S.-I. Lee,S. L. Bud'ko,P. C. Canfield,L. H. Greene		
152800	JPS079123710	T<CDW> = 470 K. (dC/gamma*Tc) = 1.67	SrPt2As2	Sr1Pt2As2	Sr	1	Pt	2	As	2																		1	2010																										AB2C2		CaBe2Ge2	P4/nmm		A	4.46	4.51	9.81												K	5.2		5.7			0.4	5.45																				T	resistivity, WHH	2.5							T/K	resistivity, 0.5Rn	0.68			MHC152800		A	from Hc2	115															MSP152800			mJ/mol.K2	9.72	SP-heat	211	SP-heat																																									Coexistence of Superconductivity and Charge Density Wave in SrPt2As2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 79(2010)123710	Kazutaka KUDO,Yoshihiro NISHIKUBO,Minoru NOHARA		
152801	PRB083144525	RRR=1.35. GL = 83.14. (2d/kTc) = 3.67 from SP. (dC/gamma*Tc) = 1.86. e-ph coupling = 0.73. thermodynamic Hc(0) = 0.13 T. Hc2(0) = 14.04 T using WHH approx.	Nb1-xRex	Nb0.18Re0.82	Nb	0.18	Re	0.82																				1	2011																												alpha-Mn	I43m	217	A	9.6293														K		8.75					8.75											Oe	M-H curve,parabollic	55.67							T	resistivity, 0.5Rn,emperical eq.	17.3							T/K	resistivity, 0.5Rn	2.31			MHC152801		A	from Hc2	43.6			A	from Hc1, Hc	3625													mJ/mol.K2	53.5	SP-heat	383	SP-heat											uOhm.cm	189						189				250												Nb(3N),Re(5N)		arc-melting					Physical properties of the noncentrosymmetric superconductor Nb0.18Re0.82			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 83(2011)144525	A. B. Karki,Y. M. Xiong,N. Haldolaarachchige,S. Stadler,I. Vekhter,P. W. Adams,D. P. Young,W. A. Phelan,Julia Y. Chan		
152802	PRB083144511	2*2*0.5 mm3 for SP. a(H=0) =0.394, a(H=9T)=1.4 mJ/mol.K2, b=1.018 mJ/mol.K4, c=0.003 mJ/mol.K6, using C=a(H) + bT^3 + cT^5. (dC/Tc) = 11.6 mJ/mol.K2	KxFe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2011																																														K		32					32																																																								mJ/mol.K2	6	SP-heat	212	SP-heat																																				flux method					Nodeless superconductivity of single-crystalline KxFe2-ySe2 revealed by the low-temperature specific heat			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 83(2011)144511	B. Zeng,B. Shen,G. F. Chen,J. B. He,D. M. Wang,C. H. Li,H. H. Wen		
152803	PRB083144510	uniaxial (//c-axis) pressure effect	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2011																										ABC5		HoCoGa5																		K		2.325					2.325	MTC152803		K/GPa	0.17																																																																																												flux method. (Ce,Co,excess In) - (alumina crucible, in evacuated quartz tube) - heat(1150C) - slow cool to 450C					Nonlinear effect of uniaxial pressure on superconductivity in CeCoIn5			Physics Department, University of California, Davis, Davis, California 95616, USA	Phys.Rev.B, 83(2011)144510	S. D. Johnson,R. J. Zieve,J. C. Cooley		
152804	PRB083140504	P-induced SC. ambient-P phase(I, II), high-P phase (III,IV). (dTc/dP) = +0.50(I), -0.13 (II), +1.37 (III), -0.18 (IV) K/GPa. Hall const. measured at 30K, H=5T. Tc(max) = 9.5K(13.6GPa)	Bi2Te3	Bi2Te3	Bi	2	Te	3																				3	2011																																														K		9.5			0		9.5	MTC152804		K/GPa	0.5																														MHC152804																																																			m3/C					5	MRH152804					self-flux method. stoichiometric(Bi,Te) - (alumina crucible, in quatz tube) - heat(1000C,12h) - slow cool to500C over 100h - cool to RT					Phase diagram of a pressure-induced superconducting state and its relation to the Hall coefficient of Bi2Te3 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 83(2011)140504	Chao Zhang,Liling Sun,Zhaoyu Chen,Xingjiang Zhou,Qi Wu,Wei Yi,Jing Guo,Xiaoli Dong,Zhongxian Zhao		
152805	PRB083115131		La3Ni2B2N3	La3Ni2B2N2.7	La	3	Ni	2	B	2	N	2.7																1	2011	emu/mol	0.0002	emu.K/mol	0.004																						A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7184		20.539											borocarbide	K		12.5		13.2			12.5										10																																														mJ/mol.K2	26	SP-heat	329	SP-heat																																				inductive levitation melting. 1st(Ni+B, in Ar) - 2nd(La+Ce, in vac and with NiB) - 3rd((La,Ce)3Ni2b2, in Ar/La atmosphere) - ANN(1100C,1w, in vac)					Anderson lattice in the intermediate valence compound Ce3Ni2B2N3-z			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 83(2011)115131	Tahir Ali,Ernst Bauer,Gerfried Hilscher,Herwig Michor		
152806	PRB083115131	(dTc/dx) = -8.9 K/mol-Ce.	(La,Ce)3Ni2B2N3	La2.95Ce0.05Ni2B2N2.7	La	2.95	Ce	0.05	Ni	2	B	2	N	2.7														1	2011																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7165		20.542											borocarbide	K				10.2			10.2																																																																																																inductive levitation melting. 1st(Ni+B, in Ar) - 2nd(La+Ce, in vac and with NiB) - 3rd((La,Ce)3Ni2b2, in Ar/La atmosphere) - ANN(1100C,1w, in vac)					Anderson lattice in the intermediate valence compound Ce3Ni2B2N3-z			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 83(2011)115131	Tahir Ali,Ernst Bauer,Gerfried Hilscher,Herwig Michor		
152807	PRB083115131		(La,Ce)3Ni2B2N3	La2.9Ce0.1Ni2B2N2.7	La	2.9	Ce	0.1	Ni	2	B	2	N	2.7														1	2011																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7132		20.544											borocarbide	K				4.9			4.9																																																																																																inductive levitation melting. 1st(Ni+B, in Ar) - 2nd(La+Ce, in vac and with NiB) - 3rd((La,Ce)3Ni2b2, in Ar/La atmosphere) - ANN(1100C,1w, in vac)					Anderson lattice in the intermediate valence compound Ce3Ni2B2N3-z			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 83(2011)115131	Tahir Ali,Ernst Bauer,Gerfried Hilscher,Herwig Michor		
152808	PRB083115131		(La,Ce)3Ni2B2N3	La2.85Ce0.15Ni2B2N2.7	La	2.85	Ce	0.15	Ni	2	B	2	N	2.7														1	2011																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7108		20.545											borocarbide	K					0.35																																																																																																		inductive levitation melting. 1st(Ni+B, in Ar) - 2nd(La+Ce, in vac and with NiB) - 3rd((La,Ce)3Ni2b2, in Ar/La atmosphere) - ANN(1100C,1w, in vac)					Anderson lattice in the intermediate valence compound Ce3Ni2B2N3-z			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 83(2011)115131	Tahir Ali,Ernst Bauer,Gerfried Hilscher,Herwig Michor		
152809	PRB083115131	lattice term in SP (beta) = 0.36 mJ/mol.K4	Ce3Ni2B2N3	Ce3Ni2B2N2.7	Ce	3	Ni	2	B	2	N	2.7																1	2011	emu/mol	0.0016	emu.K/mol	0.009																						A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.576		20.263											borocarbide	K					0.35																																																										mJ/mol.K2	54	SP-heat	378	SP-heat											uOhm.cm							17.6																		inductive levitation melting. 1st(Ni+B, in Ar) - 2nd(La+Ce, in vac and with NiB) - 3rd((La,Ce)3Ni2b2, in Ar/La atmosphere) - ANN(1100C,1w, in vac)					Anderson lattice in the intermediate valence compound Ce3Ni2B2N3-z			Institut fur Festkorperphysik, Technische Universitat Wien, A-1040 Wien, Austria	Phys.Rev.B, 83(2011)115131	Tahir Ali,Ernst Bauer,Gerfried Hilscher,Herwig Michor		
152810	PRB05207428	impurity phase < 2%.  main impurity = CeB2C2	(Y,Ce)Ni2B2C	Y0.95Ce0.05Ni2B2C1	Y	0.95	Ce	0.05	Ni	2	B	2	C	1														1	1995																										ABC2D2		LuNi2B2C	I4/mmm																borocarbide	K				13.8			13.8																																																																																																arc-melting. 1st melting(Ce(Y)+Ni+B) , then C was added to (Ce(Y)+Ni+B). final ANN(1050C,4d, in vac)					Intermediate valence of Ce in y1-xCexNi2B2C (x=0, 0.05, 0.1, 0.25, 0.5, and 1)			CERS, Meudon, France	Phys.Rev.B, 83(1995)7428	E.Alleno,Z.Hossain,C.Godart,R.Nagarajan,L.C.Gupta		
152811	PRB05207428	impurity phase < 2%.  main impurity = CeB2C2	(Y,Ce)Ni2B2C	Y0.9Ce0.1Ni2B2C1	Y	0.9	Ce	0.1	Ni	2	B	2	C	1														1	1995																										ABC2D2		LuNi2B2C	I4/mmm																borocarbide	K				11.9			11.9																																																																																																arc-melting. 1st melting(Ce(Y)+Ni+B) , then C was added to (Ce(Y)+Ni+B). final ANN(1050C,4d, in vac)					Intermediate valence of Ce in y1-xCexNi2B2C (x=0, 0.05, 0.1, 0.25, 0.5, and 1)			CERS, Meudon, France	Phys.Rev.B, 83(1995)7428	E.Alleno,Z.Hossain,C.Godart,R.Nagarajan,L.C.Gupta		
152812	PRB05207428	impurity phase < 2%.  main impurity = CeB2C2	(Y,Ce)Ni2B2C	Y0.75Ce0.25Ni2B2C1	Y	0.75	Ce	0.25	Ni	2	B	2	C	1														1	1995																										ABC2D2		LuNi2B2C	I4/mmm																borocarbide	K					5																																																																																																		arc-melting. 1st melting(Ce(Y)+Ni+B) , then C was added to (Ce(Y)+Ni+B). final ANN(1050C,4d, in vac)					Intermediate valence of Ce in y1-xCexNi2B2C (x=0, 0.05, 0.1, 0.25, 0.5, and 1)			CERS, Meudon, France	Phys.Rev.B, 83(1995)7428	E.Alleno,Z.Hossain,C.Godart,R.Nagarajan,L.C.Gupta		
152813	PRB05207428	impurity phase < 2%.  main impurity = CeB2C2	(Y,Ce)Ni2B2C	Y0.5Ce0.5Ni2B2C1	Y	0.5	Ce	0.5	Ni	2	B	2	C	1														1	1995																										ABC2D2		LuNi2B2C	I4/mmm																borocarbide	K					5																																																																																																		arc-melting. 1st melting(Ce(Y)+Ni+B) , then C was added to (Ce(Y)+Ni+B). final ANN(1050C,4d, in vac)					Intermediate valence of Ce in y1-xCexNi2B2C (x=0, 0.05, 0.1, 0.25, 0.5, and 1)			CERS, Meudon, France	Phys.Rev.B, 83(1995)7428	E.Alleno,Z.Hossain,C.Godart,R.Nagarajan,L.C.Gupta		
152814	PRB05207428	impurity phase < 2%.  main impurity = CeB2C2	CeNi2B2C	Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	1995	emu/mol	0.00069																								ABC2D2		LuNi2B2C	I4/mmm		A	3.637		10.224											borocarbide	K					5																																																																																																		arc-melting. 1st melting(Ce(Y)+Ni+B) , then C was added to (Ce(Y)+Ni+B). final ANN(1050C,4d, in vac)					Intermediate valence of Ce in y1-xCexNi2B2C (x=0, 0.05, 0.1, 0.25, 0.5, and 1)			CERS, Meudon, France	Phys.Rev.B, 83(1995)7428	E.Alleno,Z.Hossain,C.Godart,R.Nagarajan,L.C.Gupta		
152815	PHC3040184	impurity phase < 6%.  main impurity = CeB2C2	CeNi2B2C	Ce1Ni2B2C1	Ce	1	Ni	2	B	2	C	1																1	1998																										ABC2D2		LuNi2B2C	I4/mmm		A	3.637		10.226											borocarbide	K				0.1			0.1																																																						mJ/mol.K	3	mJ/mol.K2	25	SP-heat																																						arc-melting					Superconductivity in the intermediate-valence CeNi2B2C			"""IF-UFRJ, CxP68-528, CEP21945-970, Riode Janeiro, Brazil"""	"""Physica C,304(1998)184-190"""	G.J.Nieuwenhuys,M.ElMassalami,R.E.Rapp		
152816	PHC3040184	impurity phase < 6%.  main impurity = CeB2C2	CeCo2B2C	Ce1Co2B2C1	Ce	1	Co	2	B	2	C	1																1	1998																										ABC2D2		LuNi2B2C	I4/mmm		A	3.581		10.249											borocarbide	K					0.1																																																										mJ/mol.K2	12	SP-heat																																						arc-melting					Superconductivity in the intermediate-valence CeNi2B2C			"""IF-UFRJ, CxP68-528, CEP21945-970, Riode Janeiro, Brazil"""	"""Physica C,304(1998)184-190"""	G.J.Nieuwenhuys,M.ElMassalami,R.E.Rapp		
152817	PHC3040184	impurity phase < 6%.  main impurity = LaB2C2	LaNi2B2C	La1Ni2B2C1	La	1	Ni	2	B	2	C	1																1	1998																										ABC2D2		LuNi2B2C	I4/mmm		A	3.801		9.861											borocarbide	K					0.1																																																										mJ/mol.K2	8	SP-heat																																						arc-melting					Superconductivity in the intermediate-valence CeNi2B2C			"""IF-UFRJ, CxP68-528, CEP21945-970, Riode Janeiro, Brazil"""	"""Physica C,304(1998)184-190"""	G.J.Nieuwenhuys,M.ElMassalami,R.E.Rapp		
152818	PRB083140501	sample is the compacted(5 kbar) nanostructured Bi3Ni. [cohere] calculated usind d=1nm. M-H loop shows FM + SC.	Bi3Ni	Bi3Ni1	Bi	3	Ni	1																					2011																										AB3																				K		3.85					3.85																				T	resistivity, 0.5Rn,emperical eq.	11												MHC152818		A	from Hc2, d=1nm																																																											using Bi12Ni4I3					Structure-induced coexistence of ferromagnetic and superconducting states of single-phase Bi3Ni seen via magnetization and resistance measurements			Dresden High Magnetic Field Laboratory (HLD), Helmholtz-Zentrum Dresden Rossendorf, D-01328 Dresden, Germany	Phys.Rev.B, 83(2011)140501	T. Herrmannsdorfer,R. Skrotzki,J. Wosnitza,D. Kohler,R. Boldt,M. Ruck		
152819	PRB083134521	compositions by EDS. From SP measurements, two gaps (2D/kTc) = 3.92 and 5.84 (DB) are obtained. (dC/Tc) = 51.0mJ/mol.K2. (dC/gamma*Tc) = 2.11	Fe(Te,Se)	Fe1Te0.57Se0.43	Fe	1	Te	0.57	Se	0.43																			2011																										AB			P4/nmm																	K		15		14		1	15																																																5.84	14							mJ/mol.K2	26.6	SP-heat																																						flux method					Calorimetric evidence of strong-coupling multiband superconductivity in Fe(Te0.57Se0.43) single crystal			Department of Physics and Engineering Physics, Tulane University, New Orleans, Louisiana, 70118, USA	Phys.Rev.B, 83(2011)134521	J. Hu,T. J. Liu,B. Qian,A. Rotaru,L. Spinu,Z. Q. Mao		
152820	PRB083184507	compositions : nominal values. Tc = 3.2 - 7 K, for 1.0 < x < 2.5 in LixB12.	LixB12	B12Li2.5	B	12	Li	2.5																					2011																																													rhombohedral	K		6.62					6.62																																																																																																vapor diffusion process in Ta or Mo tube. Raw alpha-B refined by ANN(amorphous-B, 1200C, 50h)					Superconductivity in Li-doped alpha-rhombohedral boron			Department of Advanced Materials Science, The University of Tokyo, Japan	Phys.Rev.B, 83(2011)184507	T. Nagatochi,H. Hyodo,A. Sumiyoshi,K. Soga,Y. Sato,M. Terauchi,F. Esaka,K. Kimura		
152821	PRB083184507	compositions : nominal values. Tc = 3.2 - 7 K, for 1.0 < x < 2.5 in LixB12.	LixB12	B12Li1.7	B	12	Li	1.7																					2011																																													rhombohedral	K		7.05					7.05										2.76																																																																																						vapor diffusion process in Ta or Mo tube. Raw alpha-B refined by ANN(amorphous-B, 1200C, 50h)					Superconductivity in Li-doped alpha-rhombohedral boron			Department of Advanced Materials Science, The University of Tokyo, Japan	Phys.Rev.B, 83(2011)184507	T. Nagatochi,H. Hyodo,A. Sumiyoshi,K. Soga,Y. Sato,M. Terauchi,F. Esaka,K. Kimura		
152822	PRL106117602	AFM confirmed by SP-heat. AFM order observed by muon-SR below Tc.	CsxFe2Se2	Cs0.8Fe2Se1.96	Cs	0.8	Fe	2	Se	1.96																		3	2011								478.5																		AB2C2		ThCr2Si2																		K			29.6	29.6			29.6																																																																																																Bridgman method					Coexistence of Magnetism and Superconductivity in the Iron-Based Compound Cs0.8(FeSe0.98)2			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 106(2011)117602	Z. Shermadini,A. Krzton-Maziopa,M. Bendele,R. Khasanov,H. Luetkens,K. Conder,E. Pomjakushina,S. Weyeneth,V. Pomjakushin,O. Bossen,A. Amato		
152823	JPS080014712	Ca(n+1)M(n)Fe2As2O(3n-1) series,  n=3	Ca4(Sc,Ti)3Fe2As2Oz	Ca4Sc2.01Ti0.99Fe2As2Oz	Ca	4	Sc	2.01	Ti	0.99	Fe	2	As	2											O	z			2011																															A	3.922													Ca-4322	K	28.4		34.8				31.6	TC152823																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152824	JPS080014712	Ca(n+1)M(n)Fe2As2O(3n-1) series,  n=4	Ca5(Sc,Ti)4Fe2As2Oz	Ca5Sc2Ti2Fe2As2Oz	Ca	5	Sc	2	Ti	2	Fe	2	As	2											O	z			2011																															A	3.902													Ca-5422	K	31.4		41.3				36.35	TC152824																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152825	JPS080014712	Ca(n+1)M(n)Fe2As2O(3n-1) series,  n=5	Ca6(Sc,Ti)5Fe2As2Oz	Ca6Sc2Ti3Fe2As2Oz	Ca	6	Sc	2	Ti	3	Fe	2	As	2											O	z			2011																															A	3.884													Ca-6522	K	29.4		43.3				36.35	TC152825																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152826	JPS080014712	Ca(n+1)M(n)Fe2As2O(3n-1) series,  n=3	Ca4(Mg,Ti)3Fe2As2Oz	Ca4Mg0.75Ti1.25Fe2As2Oz	Ca	4	Mg	0.75	Ti	1.25	Fe	2	As	2											O	z			2011																															A	3.877													Ca-4322	K	41.8		47.3				44.55	TC152826																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152827	JPS080014712	High-Tc phase	Sr2VFeAsO3	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3			2011																												21113			A	3.93														K			36.4				36.4	TC152827																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152828	JPS080014712	Low-Tc phase	Sr2VFeAsO3	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3			2011																												21113			A	3.93														K			26				26	TC152828																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152829	JPS080014712		Sr2(Mg,Ti)FeAsO3	Sr2Mg0.3Ti0.7Fe1As1O3	Sr	2	Mg	0.3	Ti	0.7	Fe	1	As	1											O	3			2011																												21113			A	3.936														K			36.7				36.7	TC152829																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152830	JPS080014712		Sr2(Mg,Ti)(Fe,Co)AsO3	Sr2Mg0.5Ti0.5Fe0.95Co0.05As1O3	Sr	2	Mg	0.5	Ti	0.5	Fe	0.95	Co	0.05	As	1									O	3			2011																												21113																		K			26.2				26.2	TC152830																																																																																															solid state reaction					Pressure Dependence of Superconducting Transition Temperature on Perovskite-Type Fe-Based Superconductors and NMR Study of Sr2VFeAsO3			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 80(2011)014712	Hisashi KOTEGAWA,Yuuki TAO,Hideki TOU,Hiraku OGINO,Sigeru HORII,Kohji KISHIO,Jun-ichi SHIMOYAMA		
152831	JPS080023715	RRR=40 (RRR=2.2 for P=4.0 GPa). Tc shows four different phases (See [TC152831], critical-p - 2.7 3.7 4.2 GPa). Fig-[HC152831] shows Hc2(T) for every phases.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2																	O	7			2011																										A2B2C7		pyroclore	Fd3[-]m																	K		0.97					0.97	TC152831																			T	resistivity, extrapolation	0.29												HC152831		A	from Hc2	370																																																															Superconductivity of Heavy Carriers in the Pressure-Induced Phases of Cd2Re2O7			Graduate School of Natural Science and Technology, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)023715	Tatsuo C. KOBAYASHI,Yuta IRIE,Jun-ichi YAMAURA,Zenji HIROI,Keizo MURATA		
152832	JPS080024702	impurity (WSi2) < 20%.). RRR=12. GL = 8. thermodynamic-Hc = 790 Oe. (dTc/gamma*Tc) = 1.49. SP-heat corrected by subtracted ones of WSi2(impurity phase).	W5SiB2	W5Si1B2	W	5	Si	1	B	2																		1	2011																										AB2C5		Mo5siB2	I4/mcm	140	A	6.032		11.02											T2-phase	K			5.8	5.8			5.8										25	Oe	M-H curves, T2 approx..	120							T	resistivity, extrapolation	0.52												MHC152832		A	from Hc2	252			A	from Hc1	2110													mJ/mol.K2	12.8	SP-heat	470																																					solid state reaction. mixture - pellet - heat(1300C,30h, in Ar)					Superconductivity in W5SiB2 with the T2 Phase Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 229-8558, Japan	J.Phys.Soc.Jpn, 80(2011)024702	Michinori FUKUMA,Kenji KAWASHIMA,Masaki MARUYAMA,Jun AKIMITSU		
152833	JAP0502863	high-temperaturephase. impurity phase(< 3%)	beta-Nb5Si3	Nb5Si3	Nb	5	Si	3																					1979																										A3B5		W5Si3			A	10.0289		5.0698												K		0.69				0.25	0.69																													T/K	resistivity	0.067			MHC152833																																																												Nb(3N),Si(5N)		arc-melting, then Q to RT					Superconductivity in Nb5Si3			Naval Research Laboratory, Washington, D.C. 20375	J.Appl.Phys., 50(1979)2863	J.O.Willis,R.M.Waterstrat		
152834	JAP0502863	low-temperature phase. not SC.	alpha-Nb5Si3	Nb5Si3	Nb	5	Si	3																					1979																										A3B5		Cr5B3			A	6.5698		11.8877												K					0.01																																																																																																Nb(3N),Si(5N)		arc-melting, then ANN(1600C)					Superconductivity in Nb5Si3			Naval Research Laboratory, Washington, D.C. 20375	J.Appl.Phys., 50(1979)2863	J.O.Willis,R.M.Waterstrat		
152835	JPCONF105052106	(dC/gamma*Tc) = 1.40.	W5Si3	Si3W5	Si	3	W	5																				3	2009																										A3B5		W5Si3	I4/mcm	140																K	2.6	2.7	2.8	2.7			2.7											Oe	M-H curve				33			1.8	T	resistivity, WHH	0.52							T/K	resistivity	0.27			MHC152835		A	from Hc2	250			A	from Hc1, T=1.8 K.	4500																																																			W(4N), Si(5N)		synthesized using tetra-arc furnace.					Superconductivity in transition metal-silicide W5Si3			Department of Physics and Mathematics, Aoyama Gakuin University, Fuchinobe, Kanagawa, Japan	J.Phys.:Conf.Ser., 150(2009)052106	K.Kawashima,T.Muranaka,Y.Kousaka,S.Akutagawa,J.Akimitsu		
152836	JPS080024711	P-induced SC. P<crit> = 7 GPa.	CeRhGe2	Ce1Ge2Rh1	Ce	1	Ge	2	Rh	1																		3	2011					myu-B/mol	2.41	-26.3	7.6																		ABC2		CeNiSi2			A	4.3335	17.115	4.3196												K		0.45			0		0.45	MTC152836																																																							mJ/mol.K2	70	SP-heat																																						Bridgman method					Magnetic and Superconducting Properties of CeRhGe2 and CePtSi2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 80(2011)024711	Yusuke HIROSE,Naoto NISHIMURA,Fuminori HONDA,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Tetsuya TAKEUCHI,Etsuji YAMAMOTO,Yoshinori HAGA,Masato MATSUURA,Kazuma HIROTA,Akira YASUI,Hiroshi YAMAGAMI,Rikio SETTAI,Yoshichika ONUKI		
152837	JPS080024711	P-induced SC. P<crit> = 7 GPa. (Tc, -(dTc/dT), Hc2(0)) are (0.14, 35, 1.1), (0.16, 24, 2.2) and (0.15, 8.9, 0.3)  in (K, T/K, T) unit for H// a-, b-, c-axis, respectively.	CePtSi2	Ce1Pt1Si2	Ce	1	Pt	1	Si	2																		3	2011								1.9																		ABC2		CeNiSi2																		K	0.14				0		0.14	MTC152837																			T	resistivity		2.2	0.3					T/K	resistivity		24	8.9	MHC152837																						mJ/mol.K2	800	SP-heat																																						Czochralski method from CePt1.1Si2.2 using tetra-arc furnace					Magnetic and Superconducting Properties of CeRhGe2 and CePtSi2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 80(2011)024711	Yusuke HIROSE,Naoto NISHIMURA,Fuminori HONDA,Kiyohiro SUGIYAMA,Masayuki HAGIWARA,Koichi KINDO,Tetsuya TAKEUCHI,Etsuji YAMAMOTO,Yoshinori HAGA,Masato MATSUURA,Kazuma HIROTA,Akira YASUI,Hiroshi YAMAGAMI,Rikio SETTAI,Yoshichika ONUKI		
152838	EPL09427009	Fe-site vacancy. not SC. AFM at 365 K,	TlFezSe2	Tl1Fe1.3Se2	Tl	1	Fe	1.3	Se	2																		3	2011								365																		AB2C2		ThCr2Si2	I4/mmm																	K					0																																																																																																Tl2Se,K2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 950C & hold for 6h - cool to 700C(3C/h) - FC to RT					Fe-based superconductivity with Tc = 31 K bordering an antiferromagnetic insulator in (TI,K) FexSe2			Department of Physics, Zhejiang University - Hangzhou 310027, China	Europhys.Lett.,94(2011)27009	Ming-Hu Fang,Hang-Dong Wang,Chi-Heng Dong,Zu-Juan Li,Chun-Mu Feng,Jian Chen,H. Q. Yuan		
152839	EPL09427009	Fe-site vacancy. SC volume fraction < 1%.	TlFezSe2	Tl1Fe1.7Se2	Tl	1	Fe	1.7	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K	20	22.4					22.4										1																																																																																				Tl2Se,K2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 950C & hold for 6h - cool to 700C(3C/h) - FC to RT					Fe-based superconductivity with Tc = 31 K bordering an antiferromagnetic insulator in (TI,K) FexSe2			Department of Physics, Zhejiang University - Hangzhou 310027, China	Europhys.Lett.,94(2011)27009	Ming-Hu Fang,Hang-Dong Wang,Chi-Heng Dong,Zu-Juan Li,Chun-Mu Feng,Jian Chen,H. Q. Yuan		
152840	EPL09427009	Fe-site vacancy. sharp transition in R (T).	(Tl,K)Fe2Se2	Tl0.63K0.37Fe1.78Se2	Tl	0.63	K	0.37	Fe	1.78	Se	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K		28.4					28.4	MTC152840																																																																																													Tl2Se,K2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 950C & hold for 6h - cool to 700C(3C/h) - FC to RT					Fe-based superconductivity with Tc = 31 K bordering an antiferromagnetic insulator in (TI,K) FexSe2			Department of Physics, Zhejiang University - Hangzhou 310027, China	Europhys.Lett.,94(2011)27009	Ming-Hu Fang,Hang-Dong Wang,Chi-Heng Dong,Zu-Juan Li,Chun-Mu Feng,Jian Chen,H. Q. Yuan		
152841	EPL09427009	Fe-site vacancy. two SC transition in R(T)	(Tl,K)Fe2Se2	Tl0.75K0.25Fe1.84Se2	Tl	0.75	K	0.25	Fe	1.84	Se	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K		29.8	33				29.8	MTC152840																																																																																													Tl2Se,K2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 950C & hold for 6h - cool to 700C(3C/h) - FC to RT					Fe-based superconductivity with Tc = 31 K bordering an antiferromagnetic insulator in (TI,K) FexSe2			Department of Physics, Zhejiang University - Hangzhou 310027, China	Europhys.Lett.,94(2011)27009	Ming-Hu Fang,Hang-Dong Wang,Chi-Heng Dong,Zu-Juan Li,Chun-Mu Feng,Jian Chen,H. Q. Yuan		
152842	EPL09427009	Fe-site vacancy. three SC transition in R(T)	(Tl,K)Fe2Se2	Tl0.54K0.46Fe1.88Se2	Tl	0.54	K	0.46	Fe	1.88	Se	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K		30.4	40.4				30.4	MTC152840																																																																																													Tl2Se,K2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 950C & hold for 6h - cool to 700C(3C/h) - FC to RT					Fe-based superconductivity with Tc = 31 K bordering an antiferromagnetic insulator in (TI,K) FexSe2			Department of Physics, Zhejiang University - Hangzhou 310027, China	Europhys.Lett.,94(2011)27009	Ming-Hu Fang,Hang-Dong Wang,Chi-Heng Dong,Zu-Juan Li,Chun-Mu Feng,Jian Chen,H. Q. Yuan		
152843	PRB083132502	RRR = 42. nominal : K0.8Fe2Se2. compositions by ICP. R(T) shows maximum at about 140 K. Anisotropy(Hc2) = 3.3	KxFe2Se2	K0.82Fe1.63Se2	K	0.82	Fe	1.63	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K	31.5	32					32										100										T	resistivity, WHH, R=0.5Rn		159	48					T/K	resistivity, R=0.5Rn		7.2	2.17	MHC152843																																																														Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 1050 C & hold for 2h - cool to 750 C(60-200 h) - FC to RT					Effect of varying iron content on the transport properties of the potassium-intercalated iron selenide KxFe2-ySe2			Department of Physics, Renmin University of China, 100872 Beijing, People's Republic of China	Phys.Rev.B, 83(2011)132502	D. M. Wang,J. B. He,T.-L. Xia,G. F. Chen		
152844	PRB083132502	nominal: K0.8Fe2Se2.  Two step transition in R(T), Tc(on) = 44K and 38 K.	KxFe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm																	K	22		44				33																																																																																																Bridgeman method. mixture - (alumina crucible) - (sealed in evacuated quartz) - slow heat to 1050 C & hold for 2h - cool to 750 C(60-200 h) - FC to RT					Effect of varying iron content on the transport properties of the potassium-intercalated iron selenide KxFe2-ySe2			Department of Physics, Renmin University of China, 100872 Beijing, People's Republic of China	Phys.Rev.B, 83(2011)132502	D. M. Wang,J. B. He,T.-L. Xia,G. F. Chen		
152845	PRB083094519	SC properties derived from magnetization measurements. Anisotropy factor = 1.8	(Ba,K)Fe2As2	Ba0.72K0.28Fe2As2	Ba	0.72	K	0.28	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2																		K				33.1			33.1																													T/K	magnetization			4.2			A			15	8.3																																																													Observation of anisotropic diamagnetism above the superconducting transition in iron pnictide Ba1-xKxFe2As2 single crystals due to thermodynamic fluctuations			Laboratorio de Baixas Temperaturas e Superconductividade (LBTS), Facultade de Fisica, Universidade de Santiago de Compostela, E-15782 Santiago de Compostela, Spain	Phys.Rev.B, 83(2011)094519	J. Mosqueira,J. D. Dancausa,F. Vidal,S. Salem-Sugui Jr.,A. D. Alvarenga,H.-Q. Luo,Z.-S. Wang,H.-H. Wen		
152846	PRB083174510	compositions by ICP. A0.8Fe1.6Se2-type (A=K.Rb,Cs). NMR measurements of <77>Se and <87>Rb	(Tl,Rb)FexSe2	Tl0.47Rb0.34Fe1.63Se2	Tl	0.47	Rb	0.34	Fe	1.63	Se	2																3	2011																										AB2C2		ThCr2Si2																		K		32					32																																																																																																					Superconducting and normal-state properties of single-crystalline Tl0.47Rb0.34Fe1.63Se2 as seen via <77>Se and <87>Rb NMR			Department of Physics, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 83(2011)174510	Long Ma,G. F. Ji,J. Zhang,J. B. He,D. M. Wang,G. F. Chen,Wei Bao,Weiqiang Yu		
152847	PRL106107002	Thermal conductivity THC(K) =  measured for various fields. multigaps were analyzed.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2011																										A2B3C5		Sc2Fe3Si5																		K		6					6																																																													W/K2.m				MTHC152847																															floating zone method					Enhanced Quasiparticle Heat Conduction in the Multigap Superconductor Lu2Fe3Si5			Department of Physics, Tokyo Institute of Technology, Meguro, Tokyo 152-8551, Japan	Phys.Rev.Lett., 106(2011)107002	Y. Machida,S. Sakai,K. Izawa,H. Okuyama,T. Watanabe		
152848	PRL106156403	[gamma] shows for T=2.3 K	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2011																										ABC5		HoCoGa5																		K		2.24					2.24																																																						mJ/mol.K	3460	mJ/mol.K2	359	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152849	PRL106156403	[gamma] shows for T=2.3 K	(Ce,Yb)CoIn5	Ce0.95Yb0.05Co1In5	Ce	0.95	Yb	0.05	Co	1	In	5																3	2011																										ABC5		HoCoGa5																		K		2.16					2.16																																																						mJ/mol.K	3040	mJ/mol.K2	373	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152850	PRL106156403	[gamma] shows for T=2.3 K	(Ce,Yb)CoIn5	Ce0.9Yb0.1Co1In5	Ce	0.9	Yb	0.1	Co	1	In	5																3	2011																										ABC5		HoCoGa5																		K		2.09					2.09																																																						mJ/mol.K	2240	mJ/mol.K2	347	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152851	PRL106156403	[gamma] shows for T=2.3 K	(Ce,Yb)CoIn5	Ce0.875Yb0.125Co1In5	Ce	0.875	Yb	0.125	Co	1	In	5																3	2011																										ABC5		HoCoGa5																		K		1.97					1.97																																																						mJ/mol.K	1810	mJ/mol.K2	332	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152852	PRL106156403	[gamma] shows for T=2.3 K	(Ce,Yb)CoIn5	Ce0.5Yb0.5Co1In5	Ce	0.5	Yb	0.5	Co	1	In	5																3	2011																										ABC5		HoCoGa5																		K		1.19					1.19																																																						mJ/mol.K	235	mJ/mol.K2	330	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152853	PRL106156403	[gamma] shows for T=2.3 K	(Ce,Yb)CoIn5	Ce0.225Yb0.775Co1In5	Ce	0.225	Yb	0.775	Co	1	In	5																3	2011																										ABC5		HoCoGa5																		K					0.4																																																										mJ/mol.K2	140	SP-heat																																						In-flux method					Correlated Electron State in Ce1-xYbxCoIn5 Stabilized by Cooperative Valence Fluctuations			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.Lett., 106(2011)156403	L. Shu,R. E. Baumbach,M. Janoschek,E. Gonzales,K. Huang,T. A. Sayles,J. Paglione,J. O'Brien,J. J. Hamlin,D. A. Zocco,P.-C. Ho,C. A. McElroy,M. B. Maple		
152854	PRB066054534		CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2002																										ABC5		HoCoGa5			A	4.613		7.542												K		2.3					2.3																				T	resistivity, WHH		37	17					T/K	resistivity		24	11																																																															self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152855	PRB066054534		(Ce,La)CoIn5	Ce0.98La0.02Co1In5	Ce	0.98	La	0.02	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.613		7.551												K		2					2																				T	resistivity, WHH		23.5	11.9					T/K	resistivity		17	8.6	MHC152855																																																														self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152856	PRB066054534		(Ce,La)CoIn5	Ce0.95La0.05Co1In5	Ce	0.95	La	0.05	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.614		7.551												K		1.68					1.68																				T	resistivity, WHH		21.4	10.7					T/K	resistivity		19	9.5	MHC152856																																																														self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152857	PRB066054534		(Ce,La)CoIn5	Ce0.925La0.075Co1In5	Ce	0.925	La	0.075	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.615		7.551												K		1.31					1.31																				T	resistivity, WHH		18.8	8.9					T/K	resistivity		20.7	9.8	MHC152857																																																														self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152858	PRB066054534		(Ce,La)CoIn5	Ce0.9La0.1Co1In5	Ce	0.9	La	0.1	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.615		7.537												K		1.22					1.22																																																																																																self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152859	PRB066054534		(Ce,La)CoIn5	Ce0.875La0.125Co1In5	Ce	0.875	La	0.125	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.623		7.546												K		0.86					0.86																																																																																																self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152860	PRB066054534		(Ce,La)CoIn5	Ce0.85La0.15Co1In5	Ce	0.85	La	0.15	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.619		7.563												K		0.78					0.78																				T	resistivity, WHH		12.7	5.5					T/K	resistivity		23.6	10.3	MHC152860																																																														self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152861	PRB066054534		(Ce,La)CoIn5	Ce0.825La0.175Co1In5	Ce	0.825	La	0.175	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.619		7.567												K					0.35																																																																																																		self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152862	PRB066054534		LaCoIn5	La1Co1In5	La	1	Co	1	In	5																		3	2002																										ABC5		HoCoGa5			A	4.638		7.612												K					0.35																																																																																																		self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152863	PRB066054534		(Ce,Nd)CoIn5	Ce0.95Nd0.05Co1In5	Ce	0.95	Nd	0.05	Co	1	In	5																3	2002																										ABC5		HoCoGa5			A	4.601		7.546												K		2					2																																																																																																self flux method					Effects of La substitution on the superconducting state of CeCoIn5			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011	Phys.Rev.B, 66(2002)054534	C. Petrovic,S. L. Bud'ko,V. G. Kogan,P. C. Canfield		
152864	JPS0573289	P-induced SC. Tc depends on pressurizing path. (A): P increases at RT, (B): P increases at 4.2 K. Tc shows Tc(max) = 7.7 K (P=13 GPa).	Si	Si1	Si	1																							1988																										A																				K		7.7			0		7.7	MTC152864																																																																																																				Tc enhancement observed in Si, Ge and GaP under low-temperature pressurizing			National Research Institute for Metals, 1-2-1, Sengen, Tsukuba, 305	J.Phys.Soc.Jpn, 57(1988)3289	Haruki Kawamura,Kyoji Tachikawa		
152865	JPS0573289	P-induced SC. Tc depends on pressurizing path. (A): P increases at RT, (B): P increases at 4.2 K. Tc shows Tc(max) = 5.5 K (P=11GPa).	Ge	Ge1	Ge	1																							1988																										A																				K		5.5			0		5.5	MTC152865																																																																																																				Tc enhancement observed in Si, Ge and GaP under low-temperature pressurizing			National Research Institute for Metals, 1-2-1, Sengen, Tsukuba, 305	J.Phys.Soc.Jpn, 57(1988)3289	Haruki Kawamura,Kyoji Tachikawa		
152866	JPS0573289	P-induced SC. Tc depends on pressurizing path. (A): P increases at RT, (B): P increases at 4.2 K. Tc shows Tc(max) = 10.3 K (P=22GPa).	GaP	Ga1P1	Ga	1	P	1																					1988																										AB																				K		10.3			0		10.3	MTC152866																																																																																																				Tc enhancement observed in Si, Ge and GaP under low-temperature pressurizing			National Research Institute for Metals, 1-2-1, Sengen, Tsukuba, 305	J.Phys.Soc.Jpn, 57(1988)3289	Haruki Kawamura,Kyoji Tachikawa		
152867	JPCONF215012036	P-induced SC. using Bridgman anvil cell. P<crit> = 9.0 GPa.  Phase II for P > 8GPa(RT)	Bi2Te3	Bi2Te3	Bi	2	Te	3																					2010																										A2B3					A	4.385		30.51												K	3.7		5		0		4.35	MTC152867																																																																																															Bi2Te3(99.99%) from Kojundo Chem.Lab.					New superconducting phase of Bi2Te3 under pressure above 11 GPa			Graduate School of Science & Technology, Niigata University, Niigata 950-2181,Japan	J.Phys.Conf.Ser., 215(2010)012036	M Einaga,Y Tanabe,A Nakayama,A Ohmura,F Ishikawa,Yuh Yamada		
152868	PNAS1080024	SC properties at P = 6.1 GPa.	Bi2Te3	Bi2Te3	Bi	2	Te	3																				3	2010																										A2B3																				K	2.6		3.2		0		2.9																				T	resistivity, WHH			1.8										MHC152868																																																																			Pressure-induced superconductivity in  topological parent compound Bi2Te3			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190	Proc.Natl,Acad.Sci.USA, 108(2010)24	J. L. Zhang,S. J. Zhang,H. M. Weng,W. Zhang,L. X. Yang,Q. Q. Liu,S. M. Feng,X. C. Wang,R. C. Yu,L. Z. Cao,L. Wang,W. G. Yang,H. Z. Liu,W. Y. Zhao,S. C. Zhang,X. Dai,Z. Fang,C. Q. Jin		
152869	PRL102237001	P-induced SC. Tc, Hc at P=10.7 GPa. Type-I SC, then Hc2 shows Hc. Ge-II for P > 10 Gpa.	Ge-II	Ge1	Ge	1																						3	2009																										A		beta-Sn																		K	4.89	4.94	5.07		0		4.94	MTC152869																			Oe	resistivity, R=0.9Rn,extrapolation	300												MHC152869																																																																			Pressure-Dependent Metallic and Superconducting Phases in a Germanium Artificial Metal			Department of Physics and National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.Lett., 102(2009)237001	H. B. Cui,D. Graf,J. S. Brooks,H. Kobayashi		
152870	PCS0720426	as grown. d=1000 A. not SC	FeTe-film	Fe1Te1	Fe	1	Te	1																				4	2011																										AB					A	3.8358		6.2734												K					1.5																																																																																																		films were grown on STO(100) substrates by pulsed laser depositions					SuperconductivityandpropertiesofFeTeOx films			Department of Physics, University of Connecticut, Storrs, CT06269, USA	J.Phys.Chem.Solids, 72(2011)426	Y.F. Nie,D.Telesca,J.I.Budnick,B.Sinkovic,R.Ramprasad,B.O.Wells		
152871	PCS0720426	d=1000 A. Annealing in O2. Oxygen incorporated into intersticial sites. nominal Fe valence = +3. O-content not given.	FeTe-film	Fe1Te1	Fe	1	Te	1																				4	2011																										AB					A	3.7782		6.2835												K			3				3																																																																																																films were grown on STO(100) substrates by pulsed laser depositions					SuperconductivityandpropertiesofFeTeOx films			Department of Physics, University of Connecticut, Storrs, CT06269, USA	J.Phys.Chem.Solids, 72(2011)426	Y.F. Nie,D.Telesca,J.I.Budnick,B.Sinkovic,R.Ramprasad,B.O.Wells		
152872	JAP0502863	as grown.	beta-Nb5Si3	Nb5Si3	Nb	5	Si	3																					1979																										A3B5		W5Si3			A	10.0289		5.0698											beta-phase	K		0.69				0.25	0.69																													T/K		0.067																																																															Nb(3N),Si(5N)		arc-melting					Superconductivity in Nb5Si3			Naval Research Laboratory, Washington, D.C. 20375	J.Appl.Phys., 50(1979)2863	J.O.Willis,R.M.Waterstrat		
152873	JAP0502863	ANN(1600C,4h, in vac)	alpha-Nb5Si3	Nb5Si3	Nb	5	Si	3																					1979																										A3B5		Cr5B3			A	6.5698		11.8877												K					0.01																																																																																																Nb(3N),Si(5N)		arc-melting					Superconductivity in Nb5Si3			Naval Research Laboratory, Washington, D.C. 20375	J.Appl.Phys., 50(1979)2863	J.O.Willis,R.M.Waterstrat		
152874	SSC0660181	needle (c-axis long).  GL parameter = 2500.	Tl2Mo6Se6	Tl2Mo6Se6	Tl	2	Mo	6	Se	6																		3	1988																										A2B6C6		Tl2Fe6Te6																		K		6.5					6.5											Oe				0.095					T			37.5			17.5	1.35	4.2	T/K			0.6																																																																					The exotic superconductor Tl2Mo6Se6 investigated by low field magnetization measurements				Solid State Commun., 66(1988)181	R.Brusetti,P.Monceau,M.Potel,P.Gougeon,M.Seagent		
152875	SSC0330607	needle (c-axis long). 0.1*0.1*5 mm3.	Tl2Mo6Se6	Tl2Mo6Se6	Tl	2	Mo	6	Se	6																		3	1980																										A2B6C6		Tl2Fe6Te6																		K		2.6					2.6																				T			5.2	0.2					T/K		2.6	0.1				A			2030	78																															uOhm.cm		35											220																	A new pseudo-one-dimensional superconductor: Tl2Mo6Se6				Solid State Commun., 33(1980)607	J.C.Armici,M.Decroux,F.Fischer,M.Potel,R.Chevrel,M.Seagent		
152876	PCS0720572	Pd-intercalated Bi2Se3. Tc is constant tobe 5.5 K for 0.15 < x < 1.0 in PdxBi2Te3.	PdxBi2Te3	Pd0.5Bi2Te3	Pd	0.5	Bi	2	Te	3																			2011																																														K				5.5			5.5																																																																																														Bi(5N),Te(5N),Pd(4N)		single crystal grown by modified Bridgman method. Mixture - heat(800C,16h) - slow cool to 550 C(3d)					Superconductivity and non-metallicity induced by doping the topological insulators Bi2Se3 and Bi2Te3			Department of Chemistry, Princeton University, NJ 08544, USA	J.Phys.Chem.Solids, 72(2011)572	Y.S. Hor,J.G.Checkelsky,N.P.Ong,R.J.Cava		
152877	PCS0720597		Ba(Pb,Bi)O3	Ba1Pb0.75Bi0.25O3	Ba	1	Pb	0.75	Bi	0.25															O	3			2011																												BKBO																		K				12			12																																																																																																precursor BaPb0.75-xBi0.25O3 was firstly made, then followed by reaction with HgO inside an evacuated quartz tube.					Metal-insulator transition and superconductivity in Hg-doped BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials(Ministry of Education o f China), Superconductivity R&D Center(SRDC), Mail Stop165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Phys.Chem.Solids, 72(2011)597	Y. Zhang,Y.L.Chen,C.H.Cheng,Y.J.Cui,Y.Zhao		
152878	PCS0720597		Ba(Pb,Hg,Bi)O3	Ba1Pb0.5Hg0.25Bi0.25O3	Ba	1	Pb	0.5	Hg	0.25	Bi	0.25													O	3			2011																												BKBO																		K				2.93			2.93	TC152878																																																																																															precursor BaPb0.75-xBi0.25O3 was firstly made, then followed by reaction with HgO inside an evacuated quartz tube.					Metal-insulator transition and superconductivity in Hg-doped BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials(Ministry of Education o f China), Superconductivity R&D Center(SRDC), Mail Stop165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Phys.Chem.Solids, 72(2011)597	Y. Zhang,Y.L.Chen,C.H.Cheng,Y.J.Cui,Y.Zhao		
152879	PCS0720597		Ba(Pb,Hg,Bi)O3	Ba1Pb0.4Hg0.35Bi0.25O3	Ba	1	Pb	0.4	Hg	0.35	Bi	0.25													O	3			2011																												BKBO																		K				9.97			9.97	TC152878																																																																																															precursor BaPb0.75-xBi0.25O3 was firstly made, then followed by reaction with HgO inside an evacuated quartz tube.					Metal-insulator transition and superconductivity in Hg-doped BaPb0.75Bi0.25O3			Key Laboratory of Advanced Technologies of Materials(Ministry of Education o f China), Superconductivity R&D Center(SRDC), Mail Stop165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Phys.Chem.Solids, 72(2011)597	Y. Zhang,Y.L.Chen,C.H.Cheng,Y.J.Cui,Y.Zhao		
152880	JPS080013704	Tc defined as onset of real part of surface impedance. Two isotropic gaps:	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2011																										ABC		PbFCl																		K		17					17																																									A	surface impedance		4500		meV	2.93	4	7																																															self flux method (Li:Fe:As=2:1:2). Mixture - (BN crucible) - (double well quartz tube) - heat (1000C,80h) - cool to RT (1d)					Microwave Surface Impedance Measurements of LiFeAs Single Crystals			Department of Basic Science, the University of Tokyo, Meguro, Tokyo 153-8902, Japan	J.Phys.Soc.Jpn, 80(2011)013704	Yoshinori IMAI,Hideyuki TAKAHASHI,Kentaro KITAGAWA,Kazuyuki MATSUBAYASHI,Noriyuki NAKAI,Yuki NAGAI,Yoshiya UWATOKO,Masahiko MACHIDA,Atsutaka MAEDA		
152881	JPS080013704	Tc defined as onset of real part of surface impedance. Two isotropic gaps: 2.97 and 1.65 meV, (2d/kTc) = 4.42, and 2.46	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2011																										ABC		PbFCl																		K		15.6					15.6																																									A	surface impedance		5100		meV	2.97	4.42	7																																															self flux method (Li:Fe:As=2:1:2). Mixture - (BN crucible) - (double well quartz tube) - heat (1000C,80h) - cool to RT (1d)					Microwave Surface Impedance Measurements of LiFeAs Single Crystals			Department of Basic Science, the University of Tokyo, Meguro, Tokyo 153-8902, Japan	J.Phys.Soc.Jpn, 80(2011)013704	Yoshinori IMAI,Hideyuki TAKAHASHI,Kentaro KITAGAWA,Kazuyuki MATSUBAYASHI,Noriyuki NAKAI,Yuki NAGAI,Yoshiya UWATOKO,Masahiko MACHIDA,Atsutaka MAEDA		
152882	JPS080013704	Tc defined as onset of real part of surface impedance. Two isotropic gaps: 2.98 and 1.10 meV, (2d/kTc) = 4.24, and 1.57	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2011																										ABC		PbFCl																		K		16.3					16.3																																									A	surface impedance		6000		meV	2.98	4.24	7																																															self flux method (Li:Fe:As=2:1:2). Mixture - (BN crucible) - (double well quartz tube) - heat (1000C,80h) - cool to RT (1d)					Microwave Surface Impedance Measurements of LiFeAs Single Crystals			Department of Basic Science, the University of Tokyo, Meguro, Tokyo 153-8902, Japan	J.Phys.Soc.Jpn, 80(2011)013704	Yoshinori IMAI,Hideyuki TAKAHASHI,Kentaro KITAGAWA,Kazuyuki MATSUBAYASHI,Noriyuki NAKAI,Yuki NAGAI,Yoshiya UWATOKO,Masahiko MACHIDA,Atsutaka MAEDA		
152883	JPS080013706	Hc2 defined as disappearance of H irreversibility. RRR = 45. Anisotropy (Hc2) = 3.1 at Tc.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																			2011																										ABC		PbFCl																		K				16			16										16										T	magnetization, WHH		47.2	15.3		26.3	15.5	0.3	T/K	magnetization		4.43	1.44	MHC152883		A	from Hc2		46.4	15																																																								self flux method (Li:Fe:As=2:1:2). Mixture - (BN crucible) - (double well quartz tube) - heat (1000C,80h) - cool to RT (1d)					Determination of the Upper Critical Field of a Single Crystal LiFeAs: The Magnetic Torque Study up to 35 Tesla			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan	J.Phys.Soc.Jpn, 80(2011)013706	Nobuyuki KURITA,Kentaro KITAGAWA,Kazuyuki MATSUBAYASHI,Ade KISMARAHARDJA,Eun-Sang CHOI,James S. BROOKS,Yoshiya UWATOKO,Shinya UJI,Taichi TERASHIMA		
152884	JPS078063702	RRR = 87. Anisotropy = 5.5 at Tc	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2009																										AB2C2		ThCr2Si2																		K		2.79					2.79																				T	resistivity, extrapolation		4.47	1.25					T/K	resistivity		3.8	0.71	MHC152884		A	from Hc2		163	24.5																mJ/mol.K2	51														uOhm.cm		5.6																							flux method					Resistivity and Upper Critical Field in KFe2As2 Single Crystals			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003	J.Phys.Soc.Jpn, 78(2009)063702	Taichi TERASHIMA,Motoi KIMATA,Hidetaka SATSUKAWA,Atsushi HARADA,Kaori HAZAMA,Shinya UJI,Hisatomo HARIMA,Gen-Fu CHEN,Jian-Lin LUO,Nan-Lin WANG		
152885	JAC5095216		(Ce,Th)Pt3Si	Ce0.98Th0.02Pt3Si1	Ce	0.98	Th	0.02	Pt	3	Si	1																1	2011																										ABC3		CePt3B	P4mm		A	4.0781		5.4491												K			0.4				0.4																																																																																																arc-melting. ANN(760C,7d in evacuated quartz tube) - Q to water					Effect of Th doping on superconductivity in CePt3Si			Institute of Physical Chemistry, University of Vienna, Wahringerstr. 42, A-1090 Wien, Austria	J.Alloys and Compounds, 509(2011)5216	A. Grytsiv,D. Kaczorowski,Cz. Marucha,P. Rogl		
152886	JAC5095216		(Ce,Th)Pt3Si	Ce0.96Th0.04Pt3Si1	Ce	0.96	Th	0.04	Pt	3	Si	1																1	2011																										ABC3		CePt3B	P4mm		A	4.0795		5.4484												K					0.07																																																																																																		arc-melting. ANN(760C,7d in evacuated quartz tube) - Q to water					Effect of Th doping on superconductivity in CePt3Si			Institute of Physical Chemistry, University of Vienna, Wahringerstr. 42, A-1090 Wien, Austria	J.Alloys and Compounds, 509(2011)5216	A. Grytsiv,D. Kaczorowski,Cz. Marucha,P. Rogl		
152887	PRB083172502	RRR = 650. Hc2t) = 7.08(1-t^2)	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																		K		3.7					3.7																				T	SP-onset,		7.1											MHC152887																			MSP152887			mJ/mol.K2	101	SP-heat																																						Kas self-flux method.KFe2As2:Kas = 1:6 in alumina crucible - heat (930C) - slow cool to 500 C.					Specific heat in KFe2As2 in zero and applied magnetic field			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 83(2011)172502	J. S. Kim,E. G. Kim,G. R. Stewart,X. H. Chen,X. F. Wang		
152888	PRB083172502	RRR = 90.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																		K		3.1					3.1																				T	SP-onset,		4.5																														MSP152888			mJ/mol.K2	91	SP-heat																																						FeAs  self-flux method					Specific heat in KFe2As2 in zero and applied magnetic field			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 83(2011)172502	J. S. Kim,E. G. Kim,G. R. Stewart,X. H. Chen,X. F. Wang		
152889	PRB083174520	RRR = 70 ~ 90. Anisotropy(Hc2) = 1.75 at T=0. Tc data shows for I//ab. For I//c, Tc(on) = 1.0 & Tc(zero)=0.5 K.	LaSb2	La1Sb2	La	1	Sb	2																				3	2011																										AB2		SmSb2			A	6.219	6.278	18.46												K	0.7		1.7				1.2																																																																							uOhm.cm		1.2																												Dimensional crossover in the electrical and magnetic properties of the layered LaSb2 superconductor under pressure: The role of phase fluctuations			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 83(2011)174520	S. Guo,D. P. Young,P. W. Adams,X. S. Wu,Julia Y. Chan,G. T. McCandless,J. F. DiTusa		
152890	PRL106237001	not SC.	LaCo2B2	La1Co2B2	La	1	Co	2	B	2																			2011																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.6108		10.2052												K					2																																																																				uV/K	-7.4				uOhm.cm											70														arc-melting from mixture of elements.  ANN(1273 K, in evacuated silica ampoule.					LaCo2B2: A Co-Based Layered Superconductor with a ThCr2Si2-Type Structure			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)237001	Hiroshi Mizoguchi,Toshiaki Kuroda,Toshio Kamiya,Hideo Hosono		
152891	PRL106237001		(La,Y)Co2B2	La0.9Y0.1Co2B2	La	0.9	Y	0.1	Co	2	B	2																	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K	4.1		4.4				4.25																																																																																																arc-melting from mixture of elements.  ANN(1273 K, in evacuated silica ampoule.					LaCo2B2: A Co-Based Layered Superconductor with a ThCr2Si2-Type Structure			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)237001	Hiroshi Mizoguchi,Toshiaki Kuroda,Toshio Kamiya,Hideo Hosono		
152892	PRL106237001	SC for x >= 0.1 in La(Co1-xFex)2B2	La(Co,Fe)2B2	La1Co1.4Fe0.6B2	La	1	Co	1.4	Fe	0.6	B	2																	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K		4					4																																																																																																arc-melting from mixture of elements.  ANN(1273 K, in evacuated silica ampoule.					LaCo2B2: A Co-Based Layered Superconductor with a ThCr2Si2-Type Structure			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)237001	Hiroshi Mizoguchi,Toshiaki Kuroda,Toshio Kamiya,Hideo Hosono		
152893	PRL106237001	not SC	LaCo2(B,Si)2	La1Co2B1.8Si0.2	La	1	Co	2	B	1.8	Si	0.2																	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K					2													Oe	M-H curve				90			2																																																																													arc-melting from mixture of elements.  ANN(1273 K, in evacuated silica ampoule.					LaCo2B2: A Co-Based Layered Superconductor with a ThCr2Si2-Type Structure			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)237001	Hiroshi Mizoguchi,Toshiaki Kuroda,Toshio Kamiya,Hideo Hosono		
152894	SSC1510425	impurities: Bi, NiBi less than 2%. Coercive field (750K) = 70 Oe. FM persists upto 750 K. (dHc1/dT) - -40 Oe/K. G-L parameter - 5.1. thermodynamic Hc(0) = 490 Oe	NiBi3	Bi3Ni1	Bi	3	Ni	1																				1	2011									10.884																	AB3		NiBi3	Pnma		A	8.879	4.0998	11.483												K				4.05			4.05										54.1	Oe	M-H curve, WHH approx.	110							T	magnetization. WHH approx.	0.362							T/K	magnetization	0.129					A	from Hc2	302			A	G-L theory	1549																																																			Bi(5N),Ni(3N)		mixture in evacuated quartz tube - melt(1000C,7d)					Possible coexistence of superconductivity and magnetism in intermetallic NiBi3			Instituto de Investigaciones en Materiales, Universidad Nacional Autonoma de Mexico, A. Postal 70-360, Mexico, D.F. 04510, Mexico	Solid State Commum., 151(2011)425	E.L.M.   Pineiro,B.L.R.  Herrera,Roberto Escudero,Lauro Bucio		
152895	PRB083214514	hole concentration P = 0.156 and 0.111 for outer and inner layers. P estimated from Knight shift in NMR.	Ba2Ca2Cu3O6(F,O)2	Ba2Ca2Cu3F1.2O6.8	Ba	2	Ca	2	Cu	3	F	1.2													O	6.8			2011																												0223																		K				120			120																																																																																																high-pressure synthesis					Antiferromagnetism, superconductivity, and pseudogap in three-layered high-Tc cuprates Ba2Ca2Cu3O6(F,O)2 probed by Cu-NMR			Department of Materials Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 83(2011)214514	Sunao Shimizu,Shin-ichiro Tabata,Hidekazu Mukuda,Yoshio Kitaoka,Parasharam M. Shirage,Hijiri Kito,Akira Iyo		
152896	PRB083214514	hole concentration P = 0.113 and 0.087 for outer and inner layers. P estimated from Knight shift in NMR. Critical p for AFM order (Pcr) = 0.075	Ba2Ca2Cu3O6(F,O)2	Ba2Ca2Cu3F1.6O6.4	Ba	2	Ca	2	Cu	3	F	1.6													O	6.4			2011																												0223																		K				102			102																																																																																																high-pressure synthesis					Antiferromagnetism, superconductivity, and pseudogap in three-layered high-Tc cuprates Ba2Ca2Cu3O6(F,O)2 probed by Cu-NMR			Department of Materials Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 83(2011)214514	Sunao Shimizu,Shin-ichiro Tabata,Hidekazu Mukuda,Yoshio Kitaoka,Parasharam M. Shirage,Hijiri Kito,Akira Iyo		
152897	PRB083214514	hole concentration P = 0.086 and 0.073 for outer and inner layers. P estimated from Knight shift in NMR.	Ba2Ca2Cu3O6(F,O)2	Ba2Ca2Cu3F1.8O6.2	Ba	2	Ca	2	Cu	3	F	1.8													O	6.2			2011																												0223																		K				81			81																																																																																																high-pressure synthesis					Antiferromagnetism, superconductivity, and pseudogap in three-layered high-Tc cuprates Ba2Ca2Cu3O6(F,O)2 probed by Cu-NMR			Department of Materials Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 83(2011)214514	Sunao Shimizu,Shin-ichiro Tabata,Hidekazu Mukuda,Yoshio Kitaoka,Parasharam M. Shirage,Hijiri Kito,Akira Iyo		
152898	PRL106227001	T<SDW> = 0.5 K. T<STR>(tetra-to-ortho) = 165 K.	SmFeAs(O,F)	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9			2011																												oxypnictide	P4/nmm																	K		38.9					38.9	PH152898																																																																																																				Retention of the Tetragonal to Orthorhombic Structural Transition in F-Substituted SmFeAsO: A New Phase Diagram for SmFeAs(O1-xFx)			SPIN-CNR, corso Perrone 24, 16152 Genova, Italy	Phys.Rev.Lett., 106(2011)227001	A. Martinelli,A. Palenzona,M. Tropeano,M. Putti,C. Ferdeghini,G. Profeta,E. Emerich		
152899	PRL106246404	e-ph coupling = 0.68. GL-parameter = 93 (//ab), =28 (//c).Thermodynamic Hc(0) = 240 (//ab) , =330 Oe (//c). Lattice term in SP (beta) = 1.21 mJ/mol.K2	CuxZrTe3	Cu0.05Zr1Te3	Cu	0.05	Zr	1	Te	3																		3	2011																															A	5.88	3.92	10.11												K			3.8				3.8											Oe	M-H curve, WHH approx.		8.3	27.7					T	resistivity. R=0.9Rn. WHH approx.		3.2	1.3										MHC152899		A	from Hc2		160	65	A	G-L theory		6050	14900											mJ/mol.K2	2.64	SP-heat	186	SP-heat																																				crystals grownby chemical vapor transport method T-gradient(1023 - 923 K)					Coexistence of Bulk Superconductivity and Charge Density Wave in CuxZrTe3			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.Lett., 106(2011)246404	Xiangde Zhu,Hechang Lei,C. Petrovic		
152900	PRL106246404		ZrTe3	Te3Zr1	Te	3	Zr	1																				3	2011																															A	5.86	3.92	10.09												K					1.8																																																																																																		crystals grownby chemical vapor transport method T-gradient(1023 - 923 K)					Coexistence of Bulk Superconductivity and Charge Density Wave in CuxZrTe3			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.Lett., 106(2011)246404	Xiangde Zhu,Hechang Lei,C. Petrovic		
152901	JPS080055002	SC with honeycom lattice	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																			2011																										ABC		KZnAs	P6<3>/mmc	194	A	4.244		8.989											hexagonal, KZnAs-type	K		2.4				0.06	2.4																				T	resistivity, linear approx. R=0.5Rn	0.22												MHC152901		A	from Hc2	387																																																										solid state reaction. mixture - (ground, pelletize, wrapped) - heat(700C,3h + 1000C,24h)  heat(950C,2h)					Superconductivity in the Honeycomb-Lattice Pnictide SrPtAs			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)055002	Yoshihiro NISHIKUBO,Kazutaka KUDO,Minoru NOHARA		
152902	PCS0720430		Ce(O,F)FeAs	Ce1Fe1As1F0.05O0.95	Ce	1	Fe	1	As	1	F	0.05													O	0.95			2011								2.73																		ADCD		oxypnictide	P4/nmm	129	A	3.999		8.6241												K			13.2	11.7			11.7																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152903	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.95P0.05F0.05O0.95	Ce	1	Fe	1	As	0.95	P	0.05	F	0.05											O	0.95			2011								2.92																		ADCD		oxypnictide																		K			17.5	17.2			17.2																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152904	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.9P0.1F0.05O0.95	Ce	1	Fe	1	As	0.9	P	0.1	F	0.05											O	0.95			2011								3.06																		ADCD		oxypnictide			A	3.9936		8.5872												K			19.3	19.3			19.3																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152905	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.85P0.15F0.05O0.95	Ce	1	Fe	1	As	0.85	P	0.15	F	0.05											O	0.95			2011								3.19																		ADCD		oxypnictide																		K			21.3	21.8			21.8																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152906	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.8P0.2F0.05O0.95	Ce	1	Fe	1	As	0.8	P	0.2	F	0.05											O	0.95			2011								3.26																		ADCD		oxypnictide			A	3.9877		8.5585												K			20.3	20.6			20.6																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152907	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.7P0.3F0.05O0.95	Ce	1	Fe	1	As	0.7	P	0.3	F	0.05											O	0.95			2011								3.52																		ADCD		oxypnictide			A	3.9823		8.5369												K			18.3	18.2			18.2																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152908	PCS0720430		Ce(O,F)Fe(As,P)	Ce1Fe1As0.6P0.4F0.05O0.95	Ce	1	Fe	1	As	0.6	P	0.4	F	0.05											O	0.95			2011								3.46																		ADCD		oxypnictide			A	3.9737		8.5072												K			16	16			16																																																																																																solid state reaction. mixture - pellet - (sealed in evacuated quartz tube) - heat(1448 K, 50h)					Chemical pressure effect in CeFeAs1-xPxO0.95F0.05				J.Phys.Chem. Solids, 72(2011)430	Yong kang Luo,Xiao Lin,Han Han,Shuai Jiang,Yuke Li,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
152909	PHC4710185	d=900 A. MBE method.	(Sr,Nd)CuO2	Sr0.95Nd0.05Cu1O2	Sr	0.95	Nd	0.05	Cu	1															O	2		5	2011																												IL			A			3.024												K	11.4		30				20.7																																																																																																epitaxial films were grown on (110)DSO (DySeO3) substrates by MBE. growth rate = 1.6 A/s. ANN(500C, 10min)					Growth of infinite-layer (Sr, Nd)CuO2 films by MBE			NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato-Wakamiya, Atsugi, Kanagawa 243-0198, Japan	Physica C, 471(2011)185	Y. Krockenberger,H. Yamamoto		
152910	PHC4710308		(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.95Ca0.05Ba2Cu2.8Zn0.2O6.74	Y	0.95	Ca	0.05	Ba	2	Cu	2.8	Zn	0.2											O	z	6.74		2011																												Y123																		K		3.5					3.5																																																																		uV/K	11.5			TP152910																										solid state reaction. SIN( 900, 920, 930C) - ANN(460C, 2h, in flowing O2)					Mechanism of a strong rise of Tc due to the calcium doping in Y1-xCaxBa2Cu2.8Zn0.2Oy			Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Polytechnical University, 29 Polytekhnicheskaya, St. Petersburg 195251, Russia	Physica C, 471(2011)308	O.A. Martynova,D.V. Potapov,V.E. Gasumyants,E.V. Vladimirskaya		
152911	PHC4710308		(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.9Ca0.1Ba2Cu2.8Zn0.2O6.74	Y	0.9	Ca	0.1	Ba	2	Cu	2.8	Zn	0.2											O	z	6.74		2011																												Y123																		K		15.8					15.8																																																																		uV/K	8.35																													solid state reaction. SIN( 900, 920, 930C) - ANN(460C, 2h, in flowing O2)					Mechanism of a strong rise of Tc due to the calcium doping in Y1-xCaxBa2Cu2.8Zn0.2Oy			Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Polytechnical University, 29 Polytekhnicheskaya, St. Petersburg 195251, Russia	Physica C, 471(2011)308	O.A. Martynova,D.V. Potapov,V.E. Gasumyants,E.V. Vladimirskaya		
152912	PHC4710308		(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.85Ca0.15Ba2Cu2.8Zn0.2O6.74	Y	0.85	Ca	0.15	Ba	2	Cu	2.8	Zn	0.2											O	z	6.74		2011																												Y123																		K		34.6					34.6																																																																		uV/K	3.77																													solid state reaction. SIN( 900, 920, 930C) - ANN(460C, 2h, in flowing O2)					Mechanism of a strong rise of Tc due to the calcium doping in Y1-xCaxBa2Cu2.8Zn0.2Oy			Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Polytechnical University, 29 Polytekhnicheskaya, St. Petersburg 195251, Russia	Physica C, 471(2011)308	O.A. Martynova,D.V. Potapov,V.E. Gasumyants,E.V. Vladimirskaya		
152913	PHC4710308		(Y,Ca)Ba2(Cu,Zn)3Oz	Y0.8Ca0.2Ba2Cu2.8Zn0.2O6.74	Y	0.8	Ca	0.2	Ba	2	Cu	2.8	Zn	0.2											O	z	6.74		2011																												Y123																		K		44					44																																																																		uV/K	3.09			TP152913																										solid state reaction. SIN( 900, 920, 930C) - ANN(460C, 2h, in flowing O2)					Mechanism of a strong rise of Tc due to the calcium doping in Y1-xCaxBa2Cu2.8Zn0.2Oy			Department of Semiconductor Physics and Nanoelectronics, St. Petersburg State Polytechnical University, 29 Polytekhnicheskaya, St. Petersburg 195251, Russia	Physica C, 471(2011)308	O.A. Martynova,D.V. Potapov,V.E. Gasumyants,E.V. Vladimirskaya		
152914	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 86/3	(Tl,Cr)Sr2CaCu2O7-z	Tl0.85Cr0.15Sr2Ca1Cu2O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	2											O	7-z			2011																											2	Tl1212			A	3.825		12.056												K	98.6		102.2				100.4																																																																																																precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152915	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 91/3	(Tl,Cr)Sr2Ca(Cu,Ge)2O7-z	Tl0.85Cr0.15Sr2Ca1Cu1.9Ge0.1O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	1.9	Ge	0.1									O	7-z			2011																											2	Tl1212			A	3.824		12.033												K	100.2		104.8				102.5																																																																																																precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152916	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 84/9	(Tl,Cr)Sr2Ca(Cu,Ge)2O7-z	Tl0.85Cr0.15Sr2Ca1Cu1.8Ge0.2O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	1.8	Ge	0.2									O	7-z			2011																											2	Tl1212			A	3.827		12.008												K	86.2		93.4				89.8																																																																																																precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152917	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 83/7	(Tl,Cr)Sr2Ca(Cu,Ge)2O7-z	Tl0.85Cr0.15Sr2Ca1Cu1.7Ge0.3O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	1.7	Ge	0.3									O	7-z			2011																											2	Tl1212			A	3.823		12.004												K	84.5		92.8				88.65																																																																																																precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152918	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 72/15	(Tl,Cr)Sr2Ca(Cu,Ge)2O7-z	Tl0.85Cr0.15Sr2Ca1Cu1.6Ge0.4O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	1.6	Ge	0.4									O	7-z			2011																											2	Tl1212			A	3.822		11.984												K			54				54																																																																																																precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152919	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 60/25	(Tl,Cr)Sr2Ca(Cu,Ge)2O7-z	Tl0.85Cr0.15Sr2Ca1Cu1.4Ge0.6O7-z	Tl	0.85	Cr	0.15	Sr	2	Ca	1	Cu	1.4	Ge	0.6									O	7-z			2011																											2	Tl1212			A	3.827		11.98												K																																																																																																							precursor(Sr2Ca(Cu,Ge)2Oz)  + (Tl2O3,  Cr2O3)  - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152920	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 85/7	(Tl,Pb)(Sr,Yb)2CaCu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Ca1Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Ca	1	Cu	2									O	7-z			2011																											2	Tl1212			A	3.793		12.151												K	89.6		107.3				98.45																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152921	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 85/5	(Tl,Pb)(Sr,Yb)2(Ca,Mg)Cu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Ca0.8Mg0.2Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Ca	0.8	Mg	0.2	Cu	2							O	7-z			2011																											2	Tl1212			A	3.8		12.129												K	86		107.6				96.8																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152922	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 90/4	(Tl,Pb)(Sr,Yb)2(Ca,Mg)Cu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Ca0.6Mg0.4Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Ca	0.6	Mg	0.4	Cu	2							O	7-z			2011																											2	Tl1212			A	3.798		12.113												K	93.6		108.6				101.1																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152923	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 90/4	(Tl,Pb)(Sr,Yb)2(Ca,Mg)Cu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Ca0.4Mg0.6Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Ca	0.4	Mg	0.6	Cu	2							O	7-z			2011																											2	Tl1212			A	3.817		12.063												K	95.9		109.6				102.75																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152924	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 66/11	(Tl,Pb)(Sr,Yb)2(Ca,Mg)Cu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Ca0.2Mg0.8Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Ca	0.2	Mg	0.8	Cu	2							O	7-z			2011																											2	Tl1212			A	3.798		12.143												K	55.1		95.3				75.2																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152925	PHC4710363	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 60/11	(Tl,Pb)(Sr,Yb)2(Ca,Mg)Cu2O7-z	Tl0.5Pb0.5Sr1.8Yb0.2Mg1Cu2O7-z	Tl	0.5	Pb	0.5	Sr	1.8	Yb	0.2	Mg	1	Cu	2									O	7-z			2011																											2	Tl1212			A	3.805		12.125												K	34.9		95				64.95																																																																																																precursor (Sr1.8Yb0.2(Ca,Mg)Cu2Oz  + (tl2O3, PbO) - SIN(1000C,5min, in flowing O2) - FC to RT					Effect of Ge4+ and Mg2+ doping on superconductivity, fluctuation induced conductivity and interplanar coupling of TlSr2CaCu2O7-d superconductors			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Physica C, 471(2011)363	A. Ali Yusuf,A.K. Yahya,Nawazish A. Khan,F. Md. Salleh,E. Marsom,N. Huda		
152926	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 85/15	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl1Sr1.8Yb0.2Ca1Cu2O7-z	Tl	1	Sr	1.8	Yb	0.2	Ca	1	Cu	2											O	7-z			2009																											2	Tl1212			A	3.79		12.017												K	52.5		77				64.75																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152927	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 71/29	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.9Sr1.8Yb0.2Ca1Cu2.1O7-z	Tl	0.9	Sr	1.8	Yb	0.2	Ca	1	Cu	2.1											O	7-z			2009																											2	Tl1212			A	3.79		12.063												K	55.4		81.7				68.55																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152928	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 73/27	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.8Sr1.8Yb0.2Ca1Cu2.2O7-z	Tl	0.8	Sr	1.8	Yb	0.2	Ca	1	Cu	2.2											O	7-z			2009																											2	Tl1212			A	3.79		12.011												K	71.3		85.4				78.35																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152929	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 66/34	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.7Sr1.8Yb0.2Ca1Cu2.3O7-z	Tl	0.7	Sr	1.8	Yb	0.2	Ca	1	Cu	2.3											O	7-z			2009																											2	Tl1212			A	3.79		12.009												K	73		86				79.5																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152930	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 69/31	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.6Sr1.8Yb0.2Ca1Cu2.4O7-z	Tl	0.6	Sr	1.8	Yb	0.2	Ca	1	Cu	2.4											O	7-z			2009																											2	Tl1212			A	3.79		12.093												K	77.6		92.5				85.05																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152931	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 70/30	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.5Sr1.8Yb0.2Ca1Cu2.5O7-z	Tl	0.5	Sr	1.8	Yb	0.2	Ca	1	Cu	2.5											O	7-z			2009																											2	Tl1212			A	3.79		12.012												K	63.8		88.5				76.15																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152932	INOV0130406	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 62/38	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.4Sr1.8Yb0.2Ca1Cu2.6O7-z	Tl	0.4	Sr	1.8	Yb	0.2	Ca	1	Cu	2.6											O	7-z			2009																											2	Tl1212			A	3.79		12.09												K	56.4		89.4				72.9																																																																																																Precursor made by calcination (900C,48h) - mix with tl2O3 - SIN(1000C,5min) - slow cool to RT					Effects of Cu substitution on superconductivity and excess conductivity of Tl1-xCuxSr1.8Yb0.2CaCu2O7-z (x=0-0.6) ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	Mat.Res.Innovations, 13(2009)406	H.Huda,A.K.Yahya		
152933	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 93/4	Tl(Sr,Yb)2CaCu2O7	Tl1Sr1.6Yb0.4Ca1Cu2O7-z	Tl	1	Sr	1.6	Yb	0.4	Ca	1	Cu	2											O	7-z			2010																											2	Tl1212			A	3.797		12.014												K	78		96				87																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152934	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 93/4	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.9Sr1.6Yb0.4Ca1Cu2.1O7-z	Tl	0.9	Sr	1.6	Yb	0.4	Ca	1	Cu	2.1											O	7-z			2010																											2	Tl1212			A	3.798		12.015												K	69		87				78																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152935	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 92/4	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.2Sr1.6Yb0.4Ca1Cu2.2O7-z	Tl	0.2	Sr	1.6	Yb	0.4	Ca	1	Cu	2.2											O	7-z			2010																											2	Tl1212			A	3.796		12.014												K	53		79				66																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152936	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 94/3	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.3Sr1.6Yb0.4Ca1Cu2.3O7-z	Tl	0.3	Sr	1.6	Yb	0.4	Ca	1	Cu	2.3											O	7-z			2010																											2	Tl1212			A	3.797		12.007												K	80		95				87.5																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152937	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 93/5	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.4Sr1.6Yb0.4Ca1Cu2.4O7-z	Tl	0.4	Sr	1.6	Yb	0.4	Ca	1	Cu	2.4											O	7-z			2010																											2	Tl1212			A	3.796		12.005												K	42		85				63.5																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152938	JAC4920473	major phase= Tl1212, minor phase = Tl1201. volume ratio(Tl1212/tl1201) = 92/4	(Tl,Cu)(Sr,Yb)2CaCu2O7	Tl0.5Sr1.6Yb0.4Ca1Cu2.5O7-z	Tl	0.5	Sr	1.6	Yb	0.4	Ca	1	Cu	2.5											O	7-z			2010																											2	Tl1212			A	3.798		12.004												K			64				64																																																																																																					Superconducting fluctuation behavior and infrared absorption properties of Tl1-xCuxSr1.6Yb0.4CaCu2O7-z and Tl0.5Pb0.5Sr2-yMgyCa0.8Yb0.2Cu2O7-z ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia	J.Alloys Compd, 492(2010)473	Nurul H. Ahmad,Nawazish A. Khan,A.K.Yahya		
152939	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2Ca2Cu3O9	Tl0.8Hg0.2Ba2Ca2Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	2	Cu	3											O	9-z			2009																												Tl1223																		K	134.8	137.4					137.4																																				A	GL theory			5.3																															mOhm.cm											1.05																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152940	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Sm)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.975Sm0.025Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.975	Sm	0.025	Cu	3									O	9-z			2009																												Tl1223																		K	119.5	123.4					123.4																																				A	GL theory			6.01																															mOhm.cm											1.41																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152941	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Sm)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.95Sm0.05Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.95	Sm	0.05	Cu	3									O	9-z			2009																												Tl1223																		K	114.6	114.1					114.1																																				A	GL theory			6.7																															mOhm.cm											1.78																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152942	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Sm)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.9Sm0.1Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.9	Sm	0.1	Cu	3									O	9-z			2009																												Tl1223																		K	91	97.9					97.9																																				A	GL theory			8.5																															mOhm.cm											2.75																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152943	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Sm)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.85Sm0.15Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.85	Sm	0.15	Cu	3									O	9-z			2009																												Tl1223																		K	84.25	90.5					90.5																																				A	GL theory			12.71																															mOhm.cm											4.33																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152944	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Yb)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.975Yb0.025Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.975	Yb	0.025	Cu	3									O	9-z			2009																												Tl1223																		K	119.6	124.5					124.5																																				A	GL theory			5.84																															mOhm.cm											1.55																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152945	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Yb)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.95Yb0.05Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.95	Yb	0.05	Cu	3									O	9-z			2009																												Tl1223																		K	108	112.2					112.2																																				A	GL theory			7.27																															mOhm.cm											1.89																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152946	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Yb)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.9Yb0.1Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.9	Yb	0.1	Cu	3									O	9-z			2009																												Tl1223																		K	99.65	105.7					105.7																																				A	GL theory			31.78																															mOhm.cm											2.94																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152947	SSC1490281	cohere(c) calculated using GL theory	(Tl,Hg)Ba2(Ca,Yb)2Cu3O9	Tl0.8Hg0.2Ba2Ca1.85Yb0.15Cu3O9-z	Tl	0.8	Hg	0.2	Ba	2	Ca	1.85	Yb	0.15	Cu	3									O	9-z			2009																												Tl1223																		K	87.78	90.5					90.5																																				A	GL theory			24.7																															mOhm.cm											4.4																			Excess conductivity analysis for Tl0:8Hg0:2Ba2Ca2Cu3O9-z  substituted by Sm and Yb			Physics Department, Faculty of Science, Alexandria University, Alexandria, Egypt	Solid State Commun., 149(2009)281	A.I. Abou-Aly,R. Awad,I.H. Ibrahim,W. Abdeen		
152948	PRB084024509	Rh-composition from WDXS. magnetic properties from Mossbauer measurements of <57>Fe. direct evidence of coexistence(SC& magnetic order). Structural transition (tetra- to orth- ) at 59 K.	Ba(Fe,Rh)2As2	Ba1Fe1.922Rh0.078As2	Ba	1	Fe	1.922	Rh	0.078	As	2																3	2011					myu-B/Fe	0.35		55.5																		AB2C2		ThCr2Si2	I4/mmm	139																K		14					14																																																											357																																					FeAs self flux method					Coexistence of antiferromagnetic ordering and superconductivity in the Ba(Fe0.961Rh0.039)2As2 compound studied by Mossbauer spectroscopy			Department of Physics, University of Ottawa, Ottawa, Ontario K1N 6N5, Canada	Phys.Rev.B, 84(2011)024509	P. Wang,Z. M. Stadnik,J. Zukrowski,A. Thaler,S. L. Bud'ko,P. C. Canfield		
152949	PRB084033101	not SC down to 50 mK, upto 120 GPa using designer diamond anvils.	Pr	Pr1	Pr	1																							2011																										A																				K					0.05																																																																																																							Low-temperature electrical resistivity of praseodymium at pressures up to 120 GPa			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 84(2011)033101	J. J. Hamlin,J. R. Jeffries,G. Samudrala,Y. K. Vohra,S. T. Weir,D. A. Zocco,M. B. Maple		
152950	SCI2050188	total impurity = 50 - 500 ppm.	Pa	Pa1	Pa	1																						3	1979																										A																				K		0.43					0.43																				T	ac-SUS	0.0056							T/K	ac-SUS	0.026			MHC152950																																																																			Superconducting Properties of Protactinium			Los Alamos Scientific Laboratory, Los Alamos, New Mexico	Science, 205(1979)188	J.L.Smith,J.C.Spirlet,W.Muller		
152951	PCS0720442	Tc defined as max of dR/dT	(La,Sm,Sr)FeAsO	La0.81Sm0.06Sr0.13Fe1As1O1	La	0.81	Sm	0.06	Sr	0.13	Fe	1	As	1											O	1			2011																										ABCD		oxypnictide			A			8.8034												K		18.5					18.5																																																																																																					Coexistence of superconductivity and magnetism in the La0.87-xLnxSr0.13FeAsO (Ln = Sm, Gd, Dy) system			Department of Physics, National Chung Hsing University, Taiwan, ROC	J.Phys.Chem. Solids, 72(2011)442	T.P. Lu,C.C.Wu,W.H.Chou,M.D.Lan		
152952	PCS0720442	Tc defined as max of dR/dT	(La,Gd,Sr)FeAsO	La0.81Gd0.06Sr0.13Fe1As1O1	La	0.81	Gd	0.06	Sr	0.13	Fe	1	As	1											O	1			2011																										ABCD		oxypnictide			A			8.7574												K		17.1					17.1																																																																																																					Coexistence of superconductivity and magnetism in the La0.87-xLnxSr0.13FeAsO (Ln = Sm, Gd, Dy) system			Department of Physics, National Chung Hsing University, Taiwan, ROC	J.Phys.Chem. Solids, 72(2011)442	T.P. Lu,C.C.Wu,W.H.Chou,M.D.Lan		
152953	PCS0720442	Tc defined as max of dR/dT	(La,Dy,Sr)FeAsO	La0.81Dy0.06Sr0.13Fe1As1O1	La	0.81	Dy	0.06	Sr	0.13	Fe	1	As	1											O	1			2011																										ABCD		oxypnictide			A			8.7441												K		16.5					16.5																																																																																																					Coexistence of superconductivity and magnetism in the La0.87-xLnxSr0.13FeAsO (Ln = Sm, Gd, Dy) system			Department of Physics, National Chung Hsing University, Taiwan, ROC	J.Phys.Chem. Solids, 72(2011)442	T.P. Lu,C.C.Wu,W.H.Chou,M.D.Lan		
152954	PRB083220512	Pressure by DAC. Phase transition  (Ca-VI to Ca-VII) at about 210 GPa. Tc(onset) defined as deviation from normal linear T dependence of R.	Ca-VII	Ca1	Ca	1																							2011																										A																				K			29		0		29	MTC152954																																																																																													Ca(4N)							Superconducting state of Ca-VII below a critical temperature of 29 K at a pressure of 216 GPa			KYOKUGEN, Osaka University, Machikaneyama-cho, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 83(2011)220512	Masafumi Sakata,Yuki Nakamoto,Katsuya Shimizu,Takahiro Matsuoka,Yasuo Ohishi		
152955	PRB083224512	RRR = 38. Two s-wave gaps (d = 1.2 and 2.6 meV) obtained using SP-heat analysis. (dC/gamma*Tc) = 1.24. [gamma] = 8.5 mJ/mol.K2 at H=9T.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl	P4/nmm																	K			16.9				16.9										91																																				meV	2.6		14							mJ/mol.K2	10	SP-heat	310	SP-heat											uOhm.cm											15.2														self-flux method					Specific heat and angle-resolved photoemission spectroscopy study of the superconducting gaps in LiFeAs			Institute for Solid State Research, IFW Dresden, DE-01171 Dresden, Germany	Phys.Rev.B, 83(2011)224512	U. Stockert,M. Abdel-Hafiez,D. V. Evtushinsky,V. B. Zabolotnyy,A. U. B. Wolter,S. Wurmehl,I. Morozov,R. Klingeler,S. V. Borisenko,B. Buchner		
152956	PHC4690326	Li:Fe:As = 1.00:1.03:1.00 from ICP. [gamma] obtained from analysis of the data for  10 < T < 20 K at H = 7T.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm		A	3.7914		6.364											anti-PbFCl type	K	18			18			18	MTC152956		K/GPa	-1.56						100																																														mJ/mol.K2	22.5	SP-heat																																				Li(Na),FeAs		mixture - (sealed in Nb-tube) - heat to 750C (1C/min) and hold(750C,4d) - slow cool to 150C(0.05C/min) - Q to RT					The synthesis and characterization of LiFeAs and NaFeAs			Department of Physics and TCSUH, University of Houston, Houston, TX 77204-5002, USA	Physica C, 469(2009)326	C.W. Chu,F. Chen,M. Gooch,A.M. Guloy,B. Lorenz,B. Lv,K. Sasmal,Z.J. Tang,J.H. Tapp,Y.Y. Xue		
152957	PHC4690326	nominal x = 0.9 for NaxFeAs. SUS shows possibility of Tc = 25 K.	NaFeAs	Na0.9Fe1As1	Na	0.9	Fe	1	As	1																		1	2009																										ABC		PbFCl	P4/nmm		A	3.9866		7.094											anti-PbFCl type	K	12			18			18										10																																																																																				Li(Na),FeAs		mixture - (sealed in Nb-tube) - heat to 750C (1C/min) and hold(750C,4d) - slow cool to 150C(0.05C/min) - Q to RT					The synthesis and characterization of LiFeAs and NaFeAs			Department of Physics and TCSUH, University of Houston, Houston, TX 77204-5002, USA	Physica C, 469(2009)326	C.W. Chu,F. Chen,M. Gooch,A.M. Guloy,B. Lorenz,B. Lv,K. Sasmal,Z.J. Tang,J.H. Tapp,Y.Y. Xue		
152958	PRB084024502	Two kinds of AF(Fe-itinerant(1) and Eu-localizedmoment(2)) observed. P-induced SC. SC appears only for 2.4 , P < 2.7 GPa.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																		K			25		0		25	MPH152958									100																																																																																						self-flux method. starting(Eu:Fe:As = 1:5:5) - (sealed in double-quartz tube) - heat(1120C) - slow cool to 900 C within 72h					Pressure-induced changes in the magnetic and valence state of EuFe2As2			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 84(2011)024502	K. Matsubayashi,K. Munakata,M. Isobe,N. Katayama,K. Ohgushi,Y. Ueda,N. Kawamura,M. Mizumaki,N. Ishimatsu,M. Hedo,I. Umehara,Y. Uwatoko		
152959	PRL107047002	<75>As NQR measured.	(Ca4Al2O6)Fe2As2	Ca4Al2Fe2As2O5.785	Ca	4	Al	2	Fe	2	As	2													O	6-z	5.785	1	2011																												ThCr2Si2			A	3.71		14.4											Al-42622	K				27			27																																																																																																					Antiferromagnetic Spin Fluctuations and Unconventional Nodeless Superconductivity in an Iron-Based New Superconductor (Ca4Al2O6-y)(Fe2As2) : <75>As Nuclear Quadrupole Resonance Study			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.Lett., 107(2011)047002	H. Kinouchi,H. Mukuda,M. Yashima,Y. Kitaoka,P. M. Shirage,H. Eisaki,A. Iyo		
152960	APL097172506	[vols] at 5 K. Phase and Tc depend on O-content of nominal materials	(Ca4Al2O6)Fe2As2	Ca4Al2Fe2As2O5.65	Ca	4	Al	2	Fe	2	As	2													O	6-z	5.65	1	2010																												ThCr2Si2			A	3.713		15.407											Al-42622	K	23		28.3	26.8			26.8										115																																																																																				CaO,Al,As,P,Fe,Fe2O3		high-P synthesis: mixture - pellet - heat(1150 C for As, 1300C for P, P=4.5 Gpa, for ih)					Homologous series of iron pnictide oxide superconductors (Fe2As2)[Can+1(Sc,Ti)nOy] (n=3,4,5) with extremely thick blocking layers			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan and JST-TRIP, Sanban-cho, Chiyoda-ku, Tokyo 102-0075, Japan	Appl.Phys.Lett., 97(2010)072506	Hiraku Ogino,Shinya Sato,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152961	APL097172506	[vols] at 5 K. Phase and Tc depend on O-content of nominal materials	(Ca4Al2O6)Fe2P2	Ca4Al2Fe2P2O5.8	Ca	4	Al	2	Fe	2	P	2													O	6-z	5.8	1	2010																												ThCr2Si2			A	3.692		14.934											Al-42622	K	6		17.1	17			17										96																																																																																				CaO,Al,As,P,Fe,Fe2O3		high-P synthesis: mixture - pellet - heat(1150 C for As, 1300C for P, P=4.5 Gpa, for ih)					Homologous series of iron pnictide oxide superconductors (Fe2As2)[Can+1(Sc,Ti)nOy] (n=3,4,5) with extremely thick blocking layers			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan and JST-TRIP, Sanban-cho, Chiyoda-ku, Tokyo 102-0075, Japan	Appl.Phys.Lett., 97(2010)072506	Hiraku Ogino,Shinya Sato,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
152962	APEX003063102	mean valence = 3.3.	Fe2As2(Sr4(Sc,Ti)3O8)	Fe2As2Sr4Sc1.8Ti1.2O8	Fe	2	As	2	Sr	4	Sc	1.8	Ti	1.2											O	8		1	2010																												22438	I4/mmm		A	4.024		35.546												K			30	28			28										13																																																																																				FeAs,SrO,Sr2O3,Ti,TiO2,Ba,BaO2		mixture - pellet - (sealed in evacuated quartz ampoule) - heat(1000-1250 C, 40-120 h)					New Iron Arsenide Oxides (Fe2As2)(Sr4(Sc,Ti)3O8), (Fe2As2)(Ba4Sc3O7.5), and (Fe2As2)(Ba3Sc2O5)			1Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japa	Appl.Phys.Exp., 3(2010)063102	Naoto Kawaguchi,Hiraku Ogino,Yasuaki Shimizu,Kohji Kishio,Jun-ichi Shimoyama		
152963	APEX003063102		Fe2As2(Sr4(Sc,Ti)3O8)	Fe2As2Sr4Sc1.5Ti1.5O8	Fe	2	As	2	Sr	4	Sc	1.5	Ti	1.5											O	8		1	2010																												22438	I4/mmm		A	4.01		35.294												K				22			22																																																																																														FeAs,SrO,Sr2O3,Ti,TiO2,Ba,BaO2		mixture - pellet - (sealed in evacuated quartz ampoule) - heat(1000-1250 C, 40-120 h)					New Iron Arsenide Oxides (Fe2As2)(Sr4(Sc,Ti)3O8), (Fe2As2)(Ba4Sc3O7.5), and (Fe2As2)(Ba3Sc2O5)			1Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japa	Appl.Phys.Exp., 3(2010)063102	Naoto Kawaguchi,Hiraku Ogino,Yasuaki Shimizu,Kohji Kishio,Jun-ichi Shimoyama		
152964	APEX003063102		Fe2As2(Sr4(Sc,Ti)3O8)	Fe2As2Sr4Sc1.2Ti1.8O8	Fe	2	As	2	Sr	4	Sc	1.2	Ti	1.8											O	8		1	2010																												22438	I4/mmm		A	4.006		35.032												K					2												0																																																																																				FeAs,SrO,Sr2O3,Ti,TiO2,Ba,BaO2		mixture - pellet - (sealed in evacuated quartz ampoule) - heat(1000-1250 C, 40-120 h)					New Iron Arsenide Oxides (Fe2As2)(Sr4(Sc,Ti)3O8), (Fe2As2)(Ba4Sc3O7.5), and (Fe2As2)(Ba3Sc2O5)			1Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japa	Appl.Phys.Exp., 3(2010)063102	Naoto Kawaguchi,Hiraku Ogino,Yasuaki Shimizu,Kohji Kishio,Jun-ichi Shimoyama		
152965	APEX003063102		Fe2As2Ba4Sc3O7.5	Fe2As2Ba4Sc3O7.5	Fe	2	As	2	Ba	4	Sc	3													O	7.5		1	2010																												22438	I4/mmm		A	4.123		37.565												K			13	11			11																																																																																														FeAs,SrO,Sr2O3,Ti,TiO2,Ba,BaO2		mixture - pellet - (sealed in evacuated quartz ampoule) - heat(1000-1250 C, 40-120 h)					New Iron Arsenide Oxides (Fe2As2)(Sr4(Sc,Ti)3O8), (Fe2As2)(Ba4Sc3O7.5), and (Fe2As2)(Ba3Sc2O5)			1Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japa	Appl.Phys.Exp., 3(2010)063102	Naoto Kawaguchi,Hiraku Ogino,Yasuaki Shimizu,Kohji Kishio,Jun-ichi Shimoyama		
152966	APEX003063102		Fe2As2Ba3Sc2O5	Fe2As2Ba3Sc2O5	Fe	2	As	2	Ba	3	Sc	2													O	5		1	2010																												22325	I4/mmm		A	4.133		28.355												K					2																																																																																																FeAs,SrO,Sr2O3,Ti,TiO2,Ba,BaO2		mixture - pellet - (sealed in evacuated quartz ampoule) - heat(1000-1250 C, 40-120 h)					New Iron Arsenide Oxides (Fe2As2)(Sr4(Sc,Ti)3O8), (Fe2As2)(Ba4Sc3O7.5), and (Fe2As2)(Ba3Sc2O5)			1Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japa	Appl.Phys.Exp., 3(2010)063102	Naoto Kawaguchi,Hiraku Ogino,Yasuaki Shimizu,Kohji Kishio,Jun-ichi Shimoyama		
152969	PRB084014519	magnetic transition = 54.4 K. Pseudogap temp (Rmax) = 174 K.	Ba(Fe,Rh)2As2	Ba1Fe1.922Rh0.078As2	Ba	1	Fe	1.922	Rh	0.078	As	2																3	2011																										AB2C2		ThCr2Si2																		K		17.8					17.8																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152970	PRB084014519	Pseudogap temp (Rmax) = 174 K.	Ba(Fe,Rh)2As2	Ba1Fe1.848Rh0.152As2	Ba	1	Fe	1.848	Rh	0.152	As	2																3	2011																										AB2C2		ThCr2Si2																		K		22.2					22.2																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152972	PRB084014519	Pseudogap temp (Rmax) = 122 K.	Ba(Fe,Rh)2As2	Ba1Fe1.738Rh0.262As2	Ba	1	Fe	1.738	Rh	0.262	As	2																3	2011																										AB2C2		ThCr2Si2																		K		8.3					8.3																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152973	PRB084014519	magnetic transition = 79.8 K. Pseudogap temp (Rmax) = 143 K. structural transition T<STR> = 90.0 K.	Ba(Fe,Pd)2As2	Ba1Fe1.958Pd0.042As2	Ba	1	Fe	1.958	Pd	0.042	As	2																3	2011																										AB2C2		ThCr2Si2																		K		4.1					4.1																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152974	PRB084014519	magnetic transition = 50.1 K. Pseudogap temp (Rmax) = 123 K. structural transition T<STR> = 66.0 K	Ba(Fe,Pd)2As2	Ba1Fe1.946Pd0.054As2	Ba	1	Fe	1.946	Pd	0.054	As	2																3	2011																										AB2C2		ThCr2Si2																		K		12.3					12.3																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152975	PRB084014519	Pseudogap temp (Rmax) = 109 K. structural transition T<STR> = 45.0 K	Ba(Fe,Pd)2As2	Ba1Fe1.94Pd0.06As2	Ba	1	Fe	1.94	Pd	0.06	As	2																3	2011																										AB2C2		ThCr2Si2																		K		16.4					16.4																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152976	PRB084014519	Pseudogap temp (Rmax) = 82.9 K.	Ba(Fe,Pd)2As2	Ba1Fe1.894Pd0.106As2	Ba	1	Fe	1.894	Pd	0.106	As	2																3	2011																										AB2C2		ThCr2Si2																		K		13.3					13.3																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152977	PRB084014519	Pseudogap temp (Rmax) = 38.4 K.	Ba(Fe,Pd)2As2	Ba1Fe1.866Pd0.134As2	Ba	1	Fe	1.866	Pd	0.134	As	2																3	2011																										AB2C2		ThCr2Si2																		K		7.16					7.16																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152978	PRB084014519	magnetic transition = 65.5 K. Pseudogap temp (Rmax) = 109 K. structural transition T<STR> = 81.8 K	Ba(Fe,Ni)2As2	Ba1Fe1.952Ni0.048As2	Ba	1	Fe	1.952	Ni	0.048	As	2																3	2011																										AB2C2		ThCr2Si2																		K		4.1					4.1																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152979	PRB084014519	magnetic transition = 36.3 K. Pseudogap temp (Rmax) = 92.1 K. structural transition T<STR> = 55.8 K	Ba(Fe,Ni)2As2	Ba1Fe1.936Ni0.064As2	Ba	1	Fe	1.936	Ni	0.064	As	2																3	2011																										AB2C2		ThCr2Si2																		K		14.8					14.8																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152980	PRB084014519	Pseudogap temp (Rmax) = 74.2 K	Ba(Fe,Ni)2As2	Ba1Fe1.908Ni0.092As2	Ba	1	Fe	1.908	Ni	0.092	As	2																3	2011																										AB2C2		ThCr2Si2																		K		18.9					18.9	MTC152980																																																																																																				Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152981	PRB084014519	Pseudogap temp (Rmax) = 59.8 K	Ba(Fe,Ni)2As2	Ba1Fe1.892Ni0.108As2	Ba	1	Fe	1.892	Ni	0.108	As	2																3	2011																										AB2C2		ThCr2Si2																		K		14.8					14.8																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152982	PRB084014519	Pseudogap temp (Rmax) = 36.3 K	Ba(Fe,Ni)2As2	Ba1Fe1.856Ni0.144As2	Ba	1	Fe	1.856	Ni	0.144	As	2																3	2011																										AB2C2		ThCr2Si2																		K		6.14					6.14																																																																																																					Systematics of the temperature-dependent interplane resistivity in Ba(Fe1-xMx)2As2 (M = Co, Rh, Ni, and Pd)			Ames Laboratory US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)014519	M. A. Tanatar,N. Ni,A. Thaler,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
152983	PHC2330077	d=2000 A   energy gap estimated by T-dependence of [penet]	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		4	1994																												T'																		K				20.9			20.9																																									A	ac-SUS	1810					4.28	5																																															pulsed laser deposition under N2O atmosphere, on YSZ substrates (720-820 C)					Penetration depth measurements for Nd1.85Ce0.15CuO4 and NbCN thin films using a kinetic inductance technique	199411			Physica C,233 (1994) 77-84	C.W.Schneider,J.E.Evetts,S.N.Mao,T.Venkatesan,X.X.Xi,Z.H.Barber	Nd,Ce,Cu,O	
152984	PHC2330077	d=1100 A  energy gap estimated by T-dependence of [penet]	(Nd,Ce)2CuO4	Nd1.85Ce0.15Cu1O4	Nd	1.85	Ce	0.15	Cu	1															O	4		4	1994																												T'																		K				19.4			19.4																																									A	ac-SUS	1610					4.2	5																																															pulsed laser deposition under N2O atmosphere, on YSZ substrates (720-820 C)					Penetration depth measurements for Nd1.85Ce0.15CuO4 and NbCN thin films using a kinetic inductance technique	199411			Physica C,233 (1994) 77-84	C.W.Schneider,J.E.Evetts,S.N.Mao,T.Venkatesan,X.X.Xi,Z.H.Barber	Nd,Ce,Cu,O	
152985	PHC2330077	substrats; silica,  d=800 A.  energy gap estimated by T-dependence of [penet]	NbCN	Nb1C1N1	Nb	1	C	1	N	1																		4	1994																																														K				15.75			15.75																																									A	ac-SUS	2250					4.46	5																																															reactive DC-magnetron sputtering. sputtering gas : 3.2 Pa(1.3%-C2H2, 30%-N2, Ar). deposition rates = 1.3 nm/s on substrates(850 C					Penetration depth measurements for Nd1.85Ce0.15CuO4 and NbCN thin films using a kinetic inductance technique	199411			Physica C,233 (1994) 77-84	C.W.Schneider,J.E.Evetts,S.N.Mao,T.Venkatesan,X.X.Xi,Z.H.Barber	Nd,Ce,Cu,O	
152986	PHC2330077	substrats; saphire(c-plane),  d=800 A.  energy gap estimated by T-dependence of [penet]	NbCN	Nb1C1N1	Nb	1	C	1	N	1																		5	1994																																														K				16.5			16.5																																									A	ac-SUS	1340					4.3	5																																															reactive DC-magnetron sputtering. sputtering gas : 3.2 Pa(1.3%-C2H2, 30%-N2, Ar). deposition rates = 1.3 nm/s on substrates(850 C					Penetration depth measurements for Nd1.85Ce0.15CuO4 and NbCN thin films using a kinetic inductance technique	199411			Physica C,233 (1994) 77-84	C.W.Schneider,J.E.Evetts,S.N.Mao,T.Venkatesan,X.X.Xi,Z.H.Barber	Nd,Ce,Cu,O	
152987	JPS080074706	RRR=500-1400. NMR for <1>H, <14>N, <19>F, <109>Ag were measured (B=1-16 T)	Ag6O8Ag(NO3)	Ag7N1O11	Ag	7	N	1																	O	11		3	2011																												clathrate			A	9.89														K		1.04					1.04																																																																							uOhm.cm							0.2																							Guest Molecular Dynamics in Superconducting Clathrates Ag6O8AgX (X = NO3 and HF2): NMR Investigation			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn., 80(2011)074706	Fumiya KANETAKE,Hirofumi NARUWA,Hidekazu MUKUDA,Yoshio KITAOKA,Kenji KAWASHIMA,Masaru ISHII,Jun AKIMITSU		
152988	JPS080074706	RRR=15. NMR for <1>H, <14>N, <19>F, <109>Ag were measured (B=1-16 T)	Ag6O8Ag(HF2)	Ag7H1F2O8	Ag	7	H	1	F	2															O	8		3	2011																												clathrate			A	9.82														K		1.38					1.38																																																																							uOhm.cm							29																							Guest Molecular Dynamics in Superconducting Clathrates Ag6O8AgX (X = NO3 and HF2): NMR Investigation			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn., 80(2011)074706	Fumiya KANETAKE,Hirofumi NARUWA,Hidekazu MUKUDA,Yoshio KITAOKA,Kenji KAWASHIMA,Masaru ISHII,Jun AKIMITSU		
152989	PRL0170917	R(T) anomalies at 220, 180(cubic-to-tetra transition), 110 K. GL-parameter=about 100. thermodynamic Hc(0) = 57 Oe.	Ag6O8Ag(NO3)	Ag7N1O11	Ag	7	N	1																	O	11		3	1966																												clathrate			A	9.893														K		1.04					1.04																																																								mJ/mol.K2	0.05																																							electrolytic oxidation of aqueous solutions of AgX					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
152990	PRL0170917		Ag6O8Ag(F)	Ag7F1O8	Ag	7	F	1																	O	8		3	1966																												clathrate			A	9.833														K		0.3					0.3																																																																																																electrolytic oxidation of aqueous solutions of AgX					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
152991	PRL0170917		Ag6O8Ag(BF4)	Ag7B1F4O8	Ag	7	B	1	F	4															O	8		3	1966																												clathrate			A	9.942														K		0.15					0.15																																																																																																electrolytic oxidation of aqueous solutions of AgX					Metallic conductivity and superconductivity in some silver clathrate salts			Bell Telephone Lab,New Jersey,USA	Phys.Rev.Lett., 17(1966)917	M.B.Robin,K.Andres,T.H.Geballe,N.A.Kuebler,D.B.McWhan		
152993	PHC4701048	main phase: Zr2Co	Zr55Co30Al15	Zr55Co30Al15	Zr	55	Co	30	Al	15																		2	2010																																														K			2.4				2.4										87																																																																																						Ar-arc-melting - tilt casting in Ar - metallic glass (thickness 5mm)					Superconducting property of Zr-Co and Zr-Co-Al alloys fabricated by rapid solidification			Department of Materials Science and Chemistry, Graduate School of Engineering, University of Hyogo, 2167 Shosha, Himeji 671-2280, Japan	Physica C, 470(2010)1048	D. Okai,R. Nagai,G. Motoyama,T. Fukami,T. Yamasaki,Y. Yokoyama,H.M. Kimura,A. Inoue		
152994	PHC4701048	ANN(1000K, in vac), ZrCo, Zr2Co, Zr6CoAl2 are in amorphous phase.  glass transition at 797 K.	Zr85Co15	Co15Zr85	Co	15	Zr	85																				2	2010																																														K			3.3				3.3	MTC152994																																																																																															rappid solidification using melt spun technique					Superconducting property of Zr-Co and Zr-Co-Al alloys fabricated by rapid solidification			Department of Materials Science and Chemistry, Graduate School of Engineering, University of Hyogo, 2167 Shosha, Himeji 671-2280, Japan	Physica C, 470(2010)1048	D. Okai,R. Nagai,G. Motoyama,T. Fukami,T. Yamasaki,Y. Yokoyama,H.M. Kimura,A. Inoue		
152995	MSE4490548	as-cast. amorphous.	Zr55Cu30Al10Ni5	Zr55Cu30Al10Ni5	Zr	55	Cu	30	Al	10	Ni	5																	2007																												AMOR																		K					1.7																																																																																																		arc-melting - squeeze casting method - amorphous sample					Temperature dependence of electrical resistivity of Zr-Cu-Al-Ni-Nb bulk metallic glasses below 300K			Department of Materials Science and Chemistry, Graduate School of Engineering, University of Hyogo, 2167 Shosha, Himeji 671-2280, Japan	Mat.Sci.Eng. A, 449(2007)548	D. Okai,A. Nanbu,T. Fukami,T. Yamasaki,T. Zhang,Y. Yokoyama,G. Motoyama,Y. Oda,H.M. Kimura,A. Inoue		
152996	MSE4490548	annealed sample. crystallized. Zr2Cu(Tc=2.2K), ZrCu, Zr2Ni(Tc=2.75K),Zr3Al, and unknown phases are observed.	Zr55Cu30Al10Ni5	Zr55Cu30Al10Ni5	Zr	55	Cu	30	Al	10	Ni	5																	2007																																														K	2.7						2.7																																																																																																arc-melting - squeeze casting method - amorphous sample					Temperature dependence of electrical resistivity of Zr-Cu-Al-Ni-Nb bulk metallic glasses below 300K			Department of Materials Science and Chemistry, Graduate School of Engineering, University of Hyogo, 2167 Shosha, Himeji 671-2280, Japan	Mat.Sci.Eng. A, 449(2007)548	D. Okai,A. Nanbu,T. Fukami,T. Yamasaki,T. Zhang,Y. Yokoyama,G. Motoyama,Y. Oda,H.M. Kimura,A. Inoue		
152997	MSE4490548	crystallites(grain size=5-8 nm) are in amorphous phase.	Zr55(Cu,Nb)30Al10Ni5	Zr55Cu25Nb5Al10Ni5	Zr	55	Cu	25	Nb	5	Al	10	Ni	5															2007																																														K			3				3																																																																																																arc-melting - squeeze casting method - amorphous sample					Temperature dependence of electrical resistivity of Zr-Cu-Al-Ni-Nb bulk metallic glasses below 300K			Department of Materials Science and Chemistry, Graduate School of Engineering, University of Hyogo, 2167 Shosha, Himeji 671-2280, Japan	Mat.Sci.Eng. A, 449(2007)548	D. Okai,A. Nanbu,T. Fukami,T. Yamasaki,T. Zhang,Y. Yokoyama,G. Motoyama,Y. Oda,H.M. Kimura,A. Inoue		
152998	PRB084052503	H//ab direction. Hc1, Hc2 from dc-M measurements. Hc3 from ac SUS. Hc3/Hc2 = 4.4. -(dHc3/dT) = 4.0 T/K at Tc. GL parameter = 58.	K0.75Fe1.68Se2	K0.75Fe1.68Se2	K	0.75	Fe	1.68	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K				31			31											Oe	M-H curve		130						T	dc-M		19.3						T/K	dc-M		0.9		MHC152998		A	from Hc2	100			A	from Hc1, Hc2,	5800																																																					flux method					Superconducting critical fields of single-crystalline K0.73Fe1.68Se2			The Racah Institute of Physics, The Hebrew University of Jerusalem, 91904 Jerusalem, Israel	Phys.Rev.B, 84(2011)052503	M. I. Tsindlekht,I. Felner,M. Zhang,A. F. Wang,X. H. Chen		
152999	PRB083100514	R(max) at 220 K. [pcohere] calculated from Hc2=60 T(extrapolated value, not WHH). Anisotropy(max) = 3.6 (27K). measured values = pHc2(18K)=54 T, nHc2(1.6K)=56 T.	K0.8Fe1.76Se2	K0.8Fe1.76Se2	K	0.8	Fe	1.76	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K	32.2						32.2																				T	resistivity,pulsed field, WHH		102	31					T/K			4.6	1.4	MHC152999		A			23	14																																																								single crystals from melt process					Anisotropic Hc2 of K0.8Fe1.76Se2 determined up to 60 T			National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 83(2011)100514	E. D. Mun,M. M. Altarawneh,C. H. Mielke,V. S. Zapf,R. Hu,S. L. Bud'ko,P. C. Canfield		
153000	EPL09347004	compositions from EDXS. Hc2 defined as onset. anisotropy = 30-80 (Rc/Rab), and 5.0 (Hc2) at Tc.	(Tl,Rb)Fe1.72Se2	Tl0.58Rb0.42Fe1.72Se2	Tl	0.58	Rb	0.42	Fe	1.72	Se	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.896		14.303												K	31.4	31.5	32				31.5										98										T	resistivity, WHH		221	44.2					T/K	resistivity		10	2	MHC153000																																																			m3/C	0.0000000024					MRH153000			Rb2Se,Tl2Se,Fe,Se		Bridgeman method. mixture - (alumina crucible in sealed silica) - heat(950C,6h) - cool to 700C (3C/h) - RT					Superconductivity at 32K and anisotropy in Tl0.58Rb0.42Fe1.72Se2 crystals			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett., 93(2011)47004	Hang-Dong Wang1,Chi-Heng Dong,Zu-Juan Li,Qian-Hui Mao,Sha-Sha Zhu,Chun-Mu Feng,H. Q. Yuan,Ming-Hu Fang		
153001	PRB084054513	topological SC. high-Tc samples have low SC volume fraction. SC appears for 0.1 < x < 0.6 in CuxBi2Se3.	CuxBi2Se3	Cu0.4Bi2Se3	Cu	0.4	Bi	2	Se	3																		3	2011																													R3[-]m	166																K				3.09			3.09	MTC153001									48.8																																																													mOhm.cm												1.16		m3/C	-0.0000000266								Bi(6N),Se(5N)		single crystal Bi2Se3 synthesized by melting, slow cooling.. Cu-doping by acting as working electrode of 0.5 mm Cu wire.					Electrochemical synthesis and superconducting phase diagram of CuxBi2Se3			Institute of Scientific and Industrial Research, Osaka University, Osaka 567-0047, Japan	Phys.Rev.B, 84(2011)054513	M. Kriener,Kouji Segawa,Zhi Ren,Satoshi Sasaki,Shohei Wada,Yoichi Ando		
153002	PRB084054507	isotropic energy gap without nodes from thermal conductivity measurements for heat current direction of J//c and J//ab.absolute gap values not given.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K		18					18																				T	thermopower, extrapolation			18										MHC153002																																uV/K				MTP153002																										Bridgeman method using W-crucible.					Isotropic three-dimensional gap in the iron arsenide superconductor LiFeAs from directional heat transport measurements			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)054507	M. A. Tanatar,J.-Ph. Reid,S. Rene de Cotret,N. Doiron-Leyraud,F. Laliberte,E. Hassinger,J. Chang,H. Kim,K. Cho,Yoo Jang Song,Yong Seung Kwon,R. Prozorov,Louis Taillefer		
153003	PRB083060502	anisotropy(Hc2) = 2.5 at Tc.  Hc2 =  51 and 22.3 T for H//ab and H//c, respectively, estimated using WHH theory.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K		17.8					17.8																				T	TDR, extrapolation		26	17										MHC153003																																																														Bridgeman method using W-crucible					Anisotropic upper critical field and possible Fulde-Ferrel-Larkin-Ovchinnikov state in the stoichiometric pnictide superconductor LiFeAs			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 83(2011)060502	K. Cho,H. Kim,M. A. Tanatar,Y. J. Song,Y. S. Kwon,W. A. Coniglio,C. C. Agosta,A. Gurevich,R. Prozorov		
153004	PRB083174506	compositions determined by ICP. RRR = 24. anisotropy = 1.5 (T=1.4K) and =2.5 at near Tc	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K		17.5		17			17.5																				T	resistivity, extrapolation		24.2	15					T/K	resistivity		3.3	1.2	MHC153004		A	from Hc2		48	17																															mOhm.cm								0.05															Li3As,Fe,As		self-flux method. heat(800C,10h) - heat(1100C,10h) - slow cool to 800C (5C/h)					Upper critical field and its anisotropy in LiFeAs			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 83(2011)174506	J. L. Zhang,L. Jiao,F. F. Balakirev,X. C. Wang,C. Q. Jin,H. Q. Yuan		
153005	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2011																										AB2C3																				K		7.46					7.46																				T	ac-SUS, extrapolation	4.08												MHC153005		A	from Hc2	90																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153006	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2(Pd,Pt)3B	Li2Pd2.85Pt0.15B1	Li	2	Pd	2.85	Pt	0.15	B	1																1	2011																										AB2C3																				K		6.4					6.4																				T	ac-SUS, extrapolation	3.6												MHC153006		A	from Hc2	96																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153007	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2(Pd,Pt)3B	Li2Pd2.4Pt0.6B1	Li	2	Pd	2.4	Pt	0.6	B	1																1	2011																										AB2C3																				K		5.47					5.47																				T	ac-SUS, extrapolation	3.25												MHC153007		A	from Hc2	100																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153008	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2(Pd,Pt)3B	Li2Pd1.5Pt1.5B1	Li	2	Pd	1.5	Pt	1.5	B	1																1	2011																										AB2C3																				K		4.36					4.36																				T	ac-SUS, extrapolation	2.17												MHC153008		A	from Hc2	123																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153009	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2(Pd,Pt)3B	Li2Pd0.48Pt2.52B1	Li	2	Pd	0.48	Pt	2.52	B	1																1	2011																										AB2C3																				K		3.07					3.07																				T	ac-SUS, extrapolation	1.41												MHC153009		A	from Hc2	155																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153010	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2(Pd,Pt)3B	Li2Pd0.3Pt2.7B1	Li	2	Pd	0.3	Pt	2.7	B	1																1	2011																										AB2C3																				K		3.37					3.37																				T	ac-SUS, extrapolation	1.56												MHC153010		A	from Hc2	147																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153011	PRB084054521	Hc2 defined by ac-SUS and SP-heat	Li2Pt3B	Li2Pt3B1	Li	2	Pt	3	B	1																		1	2011																										AB2C3																				K		3.12					3.12																				T	ac-SUS, extrapolation	1.48												MHC153011		A	from Hc2	151																																																								Li(3N),Pt(5N),Pd(3N),B(2N)		two step arc-melting using excess Li.					Magnetic phase diagram of Li2(Pd1-xPtx)3B by ac susceptometry			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 84(2011)054521	D. C. Peets,G. Eguchi,M. Kriener,S. Harada,Sk. Md. Shamsuzzamen,Y. Inada,G.-Q. Zheng,Y. Maeno		
153012	PHC470S762	RRR = 4.3, Hc2(0) = 0.385 T using WHH. thermodynamic Hc(0) = 6.5 mT. GL parameter = 48. TP300 shows one for 285 K.	CaIrSi3	Ca1Ir1Si3	Ca	1	Ir	1	Si	3																			2010																										ABC3			I4mm		A	4.19		9.86												K			3.2	3		0.22	3																				T	ac-SUS, extrapolation	0.44							T/K	ac-SUS	0.186			MHC153012		A	from Hc2	270																		mJ/mol.K2	0.377	SP-heat			W/K.m	3.84				uV/K	-100				mOhm.cm							0.013																CaSi(3N),Ir(4N),Si(5N)		mixture - press to rod - melt in image furnace(1900K) - cool slowly					Superconducting properties of noncentrosymmetric CaIrSi3			aDepartment of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Physica C, 470(2010)S762	G. Eguchi,D.C. Peets,M. Kriener,S. Maki,E. Nishibori,H. Sawa,Y. Maeno		
153013	PRB084054526	compositions by EDX. thermopower S/T = -0.48 uV/K2 for T=0 K extrapolated from normal values.	KxFeySe2	K0.64Fe1.44Se2	K	0.64	Fe	1.44	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K		31					31																																																								mJ/mol.K2	6	SP-heat			W/K.m	5.05				uV/K	-152																													single crystals were grown from nominal (K:Fe:Se:S = 0.8:2:2-z:z)					Evolution of correlation strength in KxFe2- ySe2 superconductor doped with S			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)054526	Kefeng Wang,Hechang Lei,C. Petrovic		
153014	PRB084054526	compositions by EDX. thermopower S/T = -0.38 uV/K2 for T=0 K extrapolated from normal values.	KxFey(Se,S)2	K0.73Fe1.44Se1.68S0.32	K	0.73	Fe	1.44	Se	1.68	S	0.32																3	2011																										AB2C2		ThCr2Si2																		K		31.4					31.4																																																								mJ/mol.K2	3.5	SP-heat								uV/K	-93.4																													single crystals were grown from nominal (K:Fe:Se:S = 0.8:2:2-z:z)					Evolution of correlation strength in KxFe2- ySe2 superconductor doped with S			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)054526	Kefeng Wang,Hechang Lei,C. Petrovic		
153015	PRB084054526	compositions by EDX. thermopower S/T = -0.11 uV/K2 for T=0 K extrapolated from normal values.	KxFey(Se,S)2	K0.7Fe1.55Se1.01S0.99	K	0.7	Fe	1.55	Se	1.01	S	0.99																3	2011																										AB2C2		ThCr2Si2																		K		21.4					21.4																																																								mJ/mol.K2	2.8	SP-heat			W/K.m	3.66				uV/K	-46.9																													single crystals were grown from nominal (K:Fe:Se:S = 0.8:2:2-z:z)					Evolution of correlation strength in KxFe2- ySe2 superconductor doped with S			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)054526	Kefeng Wang,Hechang Lei,C. Petrovic		
153016	PRB084054526	compositions by EDX. thermopower S/T = -0.13 uV/K2 for T=0 K extrapolated from normal values.	KxFey(Se,S)2	K0.76Fe1.61Se0.96S1.04	K	0.76	Fe	1.61	Se	0.96	S	1.04																3	2011																										AB2C2		ThCr2Si2																		K		16.4					16.4																																																								mJ/mol.K2	1.5	SP-heat			W/K.m	8.13				uV/K	-2.86																													single crystals were grown from nominal (K:Fe:Se:S = 0.8:2:2-z:z)					Evolution of correlation strength in KxFe2- ySe2 superconductor doped with S			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)054526	Kefeng Wang,Hechang Lei,C. Petrovic		
153017	PRB084054526	K and Fe content not given.	KxFey(Se,S)2	K0.8Fe2Se0.42S1.58	K	0.8	Fe	2	Se	0.42	S	1.58																3	2011																										AB2C2		ThCr2Si2																		K							1.9																																																																																																single crystals were grown from nominal (K:Fe:Se:S = 0.8:2:2-z:z)					Evolution of correlation strength in KxFe2- ySe2 superconductor doped with S			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)054526	Kefeng Wang,Hechang Lei,C. Petrovic		
153018	PRB083180503	XRD data shows K0.88Fe1.63S2. space-G = I4/m. spin glass state below 32 K. [RESN] = 11.7 mOhm.cm estimated from R(T) between 70 and 300 K.	KxFe2S2	K0.2Fe2S2	K	0.2	Fe	2	S	2																		3	2011																										AB2C2		ThCr2Si2	I4/m		A	8.3984		13.5988												K							1.8																																																								mJ/mol.K2	1.58	SP-heat	284	SP-heat											mOhm.cm							11.7				100														single crystals grown via self flux method with nominal (K:Fe:S = 0.8:2:2)					Spin-glass behavior of semiconducting KxFe2-yS2			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 83(2011)180503	Hechang Lei,Milinda Abeykoon,Emil S. Bozin,C. Petrovic		
153019	PRB083174503	TP(120 K) = -58.7 uV/K. THC has a peak value (3.27 W/K.m) at 23.5 K (from Fig.), but text says 17 K.	KxFe2Se2	K0.65Fe1.41Se2	K	0.65	Fe	1.41	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K		32					32																																																													W/K.m				MTHC153019	uV/K				MTP153019																										single crystals grown via self flux method					Thermoelectric studies of KxFe2-ySe2 indicating a weakly correlated superconductor			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 83(2011)174503	Kefeng Wang,Hechang Lei,C. Petrovic		
153020	PRB084054531	CDW not exist down to 0.1K by STM. Two-gap model is best fitting for penet(T) data by TDO. small gap = 1.05 , large gap = 1.8 kTc.	2H-NbS2	Nb1S2	Nb	1	S	2																				3	2011																										AB2		2H-NbSe2																	MX2	K		6.05				0.3	6.05																																																3.6																																																vapor transport method with excess S.					In-plane magnetic penetration depth in NbS2			Institut Neel, CNRS/UJF 25 rue des Martyrs, BP 166, F-38042 Grenoble cedex 9, France	Phys.Rev.B, 84(2011)054531	P. Diener,M. Leroux,L. Cario,T. Klein,P. Rodiere		
153021	PRB082014518	sample: 500*500*30 um3. SP-heat measured down to 0.6 K, up to 8T.Two-gap model fitting:  (2d/kTc) = 2.1 (small), and = 4.6 (large). Anisotropy (Hc2) = 7.5	2H-NbS2	Nb1S2	Nb	1	S	2																				3	2010																										AB2		2H-NbSe2																	MX2	K		6.05				0.4	6.05																				T	SP-heat													MHC153021														4.6	14																																															vapor transport method with excess S.					Specific heat measurements of a superconducting NbS2 single crystal in an external magnetic field: Energy gap structure			Centre of Very Low Temperature Physics at Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47, SK-04001 Kosice, Slovakia	Phys.Rev.B, 82(2010)014518	J. Kacmarcik,Z. Pribulova,C. Marcenat,T. Klein,P. Rodiere,L. Cario,P. Samuely		
153022	PRL101166407	STM, tunneling. Two gaps observed: d(S) = 0.53 meV, 2d(S) = 2.07 kTc and  d(L) = 0.93 meV, 2d(L) = 3.79 kTc. Ordered vortex lattice is observed at 0.1 K, H-0.15 T.	2H-NbS2	Nb1S2	Nb	1	S	2																				3	2008																										AB2		2H-NbSe2																	MX2	K		5.7					5.7																																														meV	0.93	3.79	1																																															See Inorg.Chem.,19(1980)39					Superconducting Density of States and Vortex Cores of 2H-NbS2			Laboratorio de Bajas Temperaturas, Departamento de Fisica de la Materia Condensada, E-28049 Madrid, Spain	Phys.Rev.Lett., 101(2008)166407	I. Guillamon,H. Suderow,S. Vieira,L. Cario,P. Diener,P. Rodiere		
153023	PRB076212504	SP-heat C(T,H) measured. gap(L) =  1.26 meV, gap(S) = 0.73 meV, DOS(SC) = 20 % are obtained from C(T,H) analysis. (dC/gamma*Tc) = 2.12. (delta) = 2.7E-4 mJ/mol.K6	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				3	2007																										AB2		2H-NbSe2																	MX2	K		6.7					6.7																																														meV	1.26	4.36	14							mJ/mol.K2	19.09	SP-heat	224	SP-heat																																		Nb(3N),Se(5N)		vapor transport method.					Experimental evidence for a two-gap structure of superconducting NbSe2: A specific-heat study in external magnetic fields			Department of Physics, Center of Nanoscience and Nanotechnology, National Sun Yat-Sen University, Kaohsiung 804, Taiwan	Phys.Rev.B, 76(2007)212504	C. L. Huang,J.-Y. Lin,Y. T. Chang,C. P. Sun,H. Y. Shen,C. C. Chou,H. Berger,T. K. Lee,H. D. Yang		
153024	MAT1104.2318	compositions by EDX. anisotropy (Hc2,T=0) = 4.25	KxFey(Se,S)2	Nb0.7Fe1.55Se1.01S0.99	Nb	0.7	Fe	1.55	Se	1.01	S	0.99																3	2011																										AB2C2		2H-NbSe2																	MX2	K			23.5				23.5																				T	resistivity, WHH		44.69	10.51					T/K	resistivity, R=0.9Rn		2.74	0.649	MHC153024		A	from Hc2		56	13.2																																																													Upper critical fields and superconducting anisotropy of K0.70Fe1.55Se1.01S0.99 and K0.76Fe1.61Se0.96S1.04 single crystals			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	cond-mat/1104.2318	Hechang Lei,C. Petrovic		
153025	MAT1104.2318	compositions by EDX. anisotropy (Hc2,T=0) = 6.34	KxFey(Se,S)2	Nb0.76Fe1.61Se0.96S1.04	Nb	0.76	Fe	1.61	Se	0.96	S	1.04																3	2011																										AB2C2		2H-NbSe2																	MX2	K			18				18																				T	resistivity, WHH		39.22	6.19					T/K	resistivity, R=0.9Rn		3.15	0.499	MHC153025		A	from Hc2		72.9	11.5																																																													Upper critical fields and superconducting anisotropy of K0.70Fe1.55Se1.01S0.99 and K0.76Fe1.61Se0.96S1.04 single crystals			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	cond-mat/1104.2318	Hechang Lei,C. Petrovic		
153026	PRB084054534	RRR = 11 . cleaved sample(ab-plane) . Co-content = 3.6% by EDX.	Li(Fe,Co)As	Li1Fe0.975Co0.025As1	Li	1	Fe	0.975	Co	0.025	As	1																3	2011																										ABC		PbFCl																		K	13.4			13.8		1.1	13.8																																																																																																self-flux method. small lumps of Li were added to mixture(fe,Co,As). nominal: Li:(Fe,Co):As = 3:2:3. heat(1363K,18h) - hold(5h) - cool to 873K (4.5 K/H)					Suppressed superconductivity in charge-doped Li(Fe1-xCox)As single crystals			Leibniz Institute for Solid State and Materials Research, D-01069 Dresden, Germany	Phys.Rev.B, 84(2011)054534	S. Aswartham,G. Behr,L. Harnagea,D. Bombor,A. Bachmann,I. V. Morozov,V. B. Zabolotnyy,A. A. Kordyuk,T. K. Kim,T. K. Kim,S. V. Borisenko,A. U. B. Wolter,C. Hess,S. Wurmehl,B. Buchner		
153027	PRB084054534	RRR = 7. cleaved sample(ab-plane) . Co-content = 5.6% by EDX.	Li(Fe,Co)As	Li1Fe0.95Co0.05As1	Li	1	Fe	0.95	Co	0.05	As	1																3	2011																										ABC		PbFCl																		K	11.2			10.8		1.2	10.8																																																																																																self-flux method. small lumps of Li were added to mixture(fe,Co,As). nominal: Li:(Fe,Co):As = 3:2:3. heat(1363K,18h) - hold(5h) - cool to 873K (4.5 K/H)					Suppressed superconductivity in charge-doped Li(Fe1-xCox)As single crystals			Leibniz Institute for Solid State and Materials Research, D-01069 Dresden, Germany	Phys.Rev.B, 84(2011)054534	S. Aswartham,G. Behr,L. Harnagea,D. Bombor,A. Bachmann,I. V. Morozov,V. B. Zabolotnyy,A. A. Kordyuk,T. K. Kim,T. K. Kim,S. V. Borisenko,A. U. B. Wolter,C. Hess,S. Wurmehl,B. Buchner		
153028	PRB084054534	RRR = 24	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K	15.6			16.8		0.7	16.8																																																																																																self-flux method. small lumps of Li were added to mixture(fe,Co,As). nominal: Li:(Fe,Co):As = 3:2:3. heat(1363K,18h) - hold(5h) - cool to 873K (4.5 K/H)					Suppressed superconductivity in charge-doped Li(Fe1-xCox)As single crystals			Leibniz Institute for Solid State and Materials Research, D-01069 Dresden, Germany	Phys.Rev.B, 84(2011)054534	S. Aswartham,G. Behr,L. Harnagea,D. Bombor,A. Bachmann,I. V. Morozov,V. B. Zabolotnyy,A. A. Kordyuk,T. K. Kim,T. K. Kim,S. V. Borisenko,A. U. B. Wolter,C. Hess,S. Wurmehl,B. Buchner		
153029	AMC13210467	XPD,NPD analysis: Li1.001Fe0.999As.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		1	2010																										ABC		PbFCl	P4/nmm		A	3.7768		6.3559												K				16.6			16.6																																																																																																Li added to mixture(Fe,As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153030	AMC13210467	XPD,NPD analysis: Li1.002Fe0.998As. Tc linearly increase with increasing volume.	Li(1-y)Fe(1+y)As	Li0.99Fe1.01As1	Li	0.99	Fe	1.01	As	1																		1	2010																										ABC		PbFCl	P4/nmm		A	3.776		6.3554												K				14			14																																																																																																Li added to mixture(Fe,As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153031	AMC13210467	XPD,NPD analysis: Li0.99Fe1.01As. Tc linearly increase with increasing volume.	Li(1-y)Fe(1+y)As	Li0.98Fe1.02As1	Li	0.98	Fe	1.02	As	1																		1	2010																										ABC		PbFCl	P4/nmm		A	3.7738		6.3485												K				4.61			4.61																																																																																																Li added to mixture(Fe,As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153032	AMC13210467	XPD,NPD analysis: Li0.982Fe1.018As. Tc linearly increase with increasing volume.	Li(1-y)Fe(1+y)As	Li0.97Fe1.03As1	Li	0.97	Fe	1.03	As	1																		1	2010																										ABC		PbFCl	P4/nmm		A	3.7725		6.3451												K					1.5																																																																																																		Li added to mixture(Fe,As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153033	AMC13210467	Tc = 13.52 from muon-SR.	Li(Fe,Co)As	Li1Fe0.975Co0.025As1	Li	1	Fe	0.975	Co	0.025	As	1																1	2010																										ABC		PbFCl	P4/nmm		A	3.7778		6.3502												K				13			13																																									A	muon-SR. fitting	2170																																																					Li added to mixture(Fe,Co or Ni), As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153034	AMC13210467	Tc = 10.00 from muon-SR.	Li(Fe,Co)As	Li1Fe0.95Co0.05As1	Li	1	Fe	0.95	Co	0.05	As	1																1	2010																										ABC		PbFCl	P4/nmm		A	3.7789		6.3424												K				9.78			9.78	MTC153034																																								A	muon-SR. fitting	2400																																																					Li added to mixture(Fe,Co or Ni), As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153035	AMC13210467	Tc = 7.35 from muon-SR.	Li(Fe,Co)As	Li1Fe0.925Co0.075As1	Li	1	Fe	0.925	Co	0.075	As	1																1	2010																										ABC		PbFCl	P4/nmm		A	3.7792		6.3322												K				7.66			7.66	MTC153034																																								A	muon-SR. fitting	3030																																																					Li added to mixture(Fe,Co or Ni), As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153036	AMC13210467	Tc = 13.41 from muon-SR.	Li(Fe,Ni)As	Li1Fe0.99Ni0.01As1	Li	1	Fe	0.99	Ni	0.01	As	1																1	2010																										ABC		PbFCl	P4/nmm																	K				13.35			13.35	MTC153036																																								A	muon-SR. fitting	2180																																																					Li added to mixture(Fe,Co or Ni), As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153037	AMC13210467	Tc = 10.93 from muon-SR.	Li(Fe,Ni)As	Li1Fe0.98Ni0.02As1	Li	1	Fe	0.98	Ni	0.02	As	1																1	2010																										ABC		PbFCl	P4/nmm		A	3.7773		6.3485												K				10.58			10.58	MTC153036																																								A	muon-SR. fitting	2730																																																					Li added to mixture(Fe,Co or Ni), As) - sealed in Nb tube(Ar) - heat 220K,12h) - reground - ANN(800C,48h)					Compositional Control of the Superconducting Properties of LiFeAs			Department of Chemistry, UniVersity of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, United Kingdom	J.Am.Chem.Soc., 132(2010)10467	Michael J. Pitcher,Tom Lancaster,Jack D. Wright,Isabel Franke,Andrew J. Steele,Peter J. Baker,Francis L. Pratt,William Trevelyan Thomas,Dinah R. Parker,Stephen J. Blundell,Simon J. Clarke		
153038	JPS080093704		Ca10(Pt4As8)((Fe,Pt)2As2)5	Ca10Fe8.2Pt4.8As18	Ca	10	Fe	8.2	Pt	4.8	As	18																	2011																													P1[-]		A	8.719	8.727	11.161											triclinic, alpha=99.04, beta=108.21, gamma=90.0	K				38			38																																																																																																mixture(Ca:Fe:Pt:As=23:23:10:44) - (alumina crucible sealed in quartz tube) - heat(700C,3h + 1000C,72h) - slow cool to RT					Superconductivity at 38K in Iron-Based Compound with Platinum-Arsenide Layers Ca10(Pt4As8)(Fe2-xPtxAs2)5			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)093704	Satomi KAKIYA,Kazutaka KUDO,Yoshihiro NISHIKUBO,Kenta OKU,Eiji NISHIBORI,Hiroshi SAWA,Takahisa YAMAMOTO,Toshio NOZAKA,Minoru NOHARA		
153039	JPS080093704		Ca10(Pt3As8)((Fe,Pt)2As2)5	Ca10Fe9.2Pt3.8As18	Ca	10	Fe	9.2	Pt	3.8	As	18																	2011																													P1[-]		A	8.795	8.789	21.008											triclinic, alpha=94.82, beta=99.62, gamma=89.99	K				13			13																																																																																					cm3/C	-0.00088					MRH153039					mixture(Ca:Fe:Pt:As=23:23:10:44) - (alumina crucible sealed in quartz tube) - heat(1100C ) - slow cool to 1050C for 40h					Superconductivity at 38K in Iron-Based Compound with Platinum-Arsenide Layers Ca10(Pt4As8)(Fe2-xPtxAs2)5			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)093704	Satomi KAKIYA,Kazutaka KUDO,Yoshihiro NISHIKUBO,Kenta OKU,Eiji NISHIBORI,Hiroshi SAWA,Takahisa YAMAMOTO,Toshio NOZAKA,Minoru NOHARA		
153040	JPS080094703	Tc and Hc2(0) shows for P=2.63 GPa. Hc2 for J//H//[001]. Neel-T depends on magnetic field	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2011								5																		ABC3		BaNiSn3																		K		1.6			0		1.6	MTC153040																			T	resistivity		45											MHC153040																																																														single crystals grown by Czochralski method in tetra-arc furnace					Field-Induced Antiferromagnetic State in Non-centrosymmetric Superconductor CeIrSi3			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 80(2011)094703	Rikio SETTAI,Rikio SETTAI,Dai AOKI,Ilya SHEIKIN,Georg KNEBEL,Jacques FLOUQUET,Yoshichika ONUKI		
153041	PRB084054541	defect introduced by n-irradiation 2E;19/cm2 (E>0.1MeV). defect control by isochronal ANN(0.5h) at various T. this sample : ANN(900C)	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		1	2011																										A2B3C5		Sc2Fe3Si5																		K		2.78					2.78	MTC153041																												T/K	resistivity, R=0.9Rn	0.93																																																																	arc-melting, then ANN(1200C,19h)					Superconductivity in iron silicide Lu2Fe3Si5 probed by radiation-induced disordering			Institute of Metal Physics UB RAS, 18 S. Kovalevskoi Street, Ekaterinburg 620219, Russia	Phys.Rev.B, 84(2011)054541	A. E. Karkin,M. R. Yangirov,M. R. Yangirov,B. N. Goshchitskii		
153042	PRL107057001	Tn=0 at P = 0.39 Gpa, where Tc(max) = 0.63 K. Hc2(0.24 K) = 2 T for H//c. (dTn/dT) = -1.17 K/GPa at P=0	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2011								0.69																		AB2C2		CeCu2Si2																		K		0.46					0.46	MTC153042		K/GPa	2.33																																																																																																	Pressure Tuning of the Interplay of Magnetism and Superconductivity in CeCu2Si2			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.Lett.,  107(2011)057001	E. Lengyel,M. Nicklas,H. S. Jeevan,H. S. Jeevan,F. Steglich		
153043	SSC1511504	hexagonal	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			2011																										ABC		Fe2P																		K		13.8					13.8																																																																																														FeP,RuP,Zr		arc-melting, then ANN(1000C,3d, in vac)					The effect of Fe doping on superconductivity in ZrRuP			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg - Universitat, 55099 Mainz, Germany	Solid State Commun., 151(2011)1504	Leslie M. Schoop,Vadim Ksenofontov,Teuta Gasi,R.J. Cava,Claudia Felser		
153044	SSC1511504	hexagonal	Zr(Ru,Fe)P	Zr1Ru0.95Fe0.05P1	Zr	1	Ru	0.95	Fe	0.05	P	1																	2011																										ABC		Fe2P																		K		10.3					10.3																																																																																														FeP,RuP,Zr		arc-melting, then ANN(1000C,3d, in vac)					The effect of Fe doping on superconductivity in ZrRuP			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg - Universitat, 55099 Mainz, Germany	Solid State Commun., 151(2011)1504	Leslie M. Schoop,Vadim Ksenofontov,Teuta Gasi,R.J. Cava,Claudia Felser		
153045	SSC1511504	two phaes(hexa + ortho ). impurity : ZrRu by XRD. no magnetic order from Mossbauer results.	Zr(Ru,Fe)P	Zr1Ru0.8Fe0.2P1	Zr	1	Ru	0.8	Fe	0.2	P	1																	2011																										ABC		Fe2P																	two phases (Fe2P+Co2P)	K		2.6					2.6																																																																																														FeP,RuP,Zr		arc-melting, then ANN(1000C,3d, in vac)					The effect of Fe doping on superconductivity in ZrRuP			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg - Universitat, 55099 Mainz, Germany	Solid State Commun., 151(2011)1504	Leslie M. Schoop,Vadim Ksenofontov,Teuta Gasi,R.J. Cava,Claudia Felser		
153046	SSC1511504	two phaes(hexa + ortho ). impurity : ZrRu by XRD. no magnetic order from Mossbauer results.	Zr(Ru,Fe)P	Zr1Ru0.6Fe0.4P1	Zr	1	Ru	0.6	Fe	0.4	P	1																	2011																										ABC		Fe2P																	two phases (Fe2P+Co2P)	K					1.8																																																																																																FeP,RuP,Zr		arc-melting, then ANN(1000C,3d, in vac)					The effect of Fe doping on superconductivity in ZrRuP			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg - Universitat, 55099 Mainz, Germany	Solid State Commun., 151(2011)1504	Leslie M. Schoop,Vadim Ksenofontov,Teuta Gasi,R.J. Cava,Claudia Felser		
153047	SSC1511504	ortho	ZrFeP	Zr1Fe1P1	Zr	1	Fe	1	P	1																			2011																										ABC		Co2P																		K					1.8																																																																																																FeP,RuP,Zr		arc-melting, then ANN(1000C,3d, in vac)					The effect of Fe doping on superconductivity in ZrRuP			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg - Universitat, 55099 Mainz, Germany	Solid State Commun., 151(2011)1504	Leslie M. Schoop,Vadim Ksenofontov,Teuta Gasi,R.J. Cava,Claudia Felser		
153048	JPC0139393	electron =  16 e/f.u	ZrRuSi	Zr1Ru1Si1	Zr	1	Ru	1	Si	1																		1	2001																										ABC		Fe2P			A	6.684		3.672												K		12.2					12.2																																																																																																high-P synthesis (1200-1600C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153049	JPC0139393	electron =  17 e/f.u  High T (1600C) synthesis.	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	2001									8.148																	ABC		Fe2P			A	6.459		3.778												K		13					13																																																																																																high-P synthesis (1200-1600C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153050	JPC0139393	electron =  17 e/f.u  Low T (1200C) synthesis.	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	2001									8.172																	ABC		Co2P			A	6.417	7.322	3.862												K		4					4																																																																																																high-P synthesis (1200-1600C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153051	JPC0139393	electron =  18 e/f.u	ZrRhP	Zr1Rh1P1	Zr	1	Rh	1	P	1																		1	2001																										ABC		Co2P			A	6.438	7.393	3.787												K		1.5					1.5																																																																																																high-P synthesis (1200-1600C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153052	JPC0139393		Zr(Ru,Rh)P	Zr1Ru0.99Rh0.01P1	Zr	1	Ru	0.99	Rh	0.01	P	1																	2001																										ABC		Fe2P																		K		10.1					10.1	MTC153052																																																																																															high-P synthesis (1300 C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153053	JPC0139393	Two step transition ( correspond to hexa and ortho-phases).	Zr(Ru,Rh)P	Zr1Ru0.95Rh0.05P1	Zr	1	Ru	0.95	Rh	0.05	P	1																	2001																										ABC		Fe2P																		K		9.3					9.3	MTC153052																																																																																															high-P synthesis (1300 C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153054	JPC0139393		Zr(Ru,Rh)P	Zr1Ru0.95Rh0.05P1	Zr	1	Ru	0.95	Rh	0.05	P	1																	2001																										ABC		Co2P																		K		3					3	MTC153052																																																																																															high-P synthesis (1300 C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153055	JPC0139393		Zr(Ru,Rh)P	Zr1Ru0.9Rh0.1P1	Zr	1	Ru	0.9	Rh	0.1	P	1																	2001																										ABC		Co2P																		K		2.9					2.9	MTC153052																																																																																															high-P synthesis (1300 C, P=4 GPa)					Superconductivity and crystal structure of ZrRu1-xRhxP alloys prepared at high pressure			Faculty of Engineering, Muroran Institute of Technology, Muroran-shi 050-8585, Japan	J.Phys.:Condens.Mater, 13(2001)9393	Ichimin Shirotani,Daisuke Kato,Atsuhito Nishimoto,Takehiko Yagi		
153056	LTP0550011	lattice term coeff.(beta) = 0.0207 mJ/gat.K4. DOS = N(0)= 0.72 sttes/eV.atom. e-ph = 0.48.	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			1984																										ABC		Co2P			A	6.43	3.861	7.334											TiNiSi type	K		3.76					3.76																																																					MSP153056			mJ/gat.K2	2.52	SP-heat	454	SP-heat																																				SIN(900C,1h) - reground - wrapped in Ta foil - ANN(1200C,3d)					Phonon Anomalies in ZrRuP?			Kernforschungszentrum Karlsruhe, Institut fiur Technische Physik, and Universitat Karlsruhe, Karlsruhe, Federal Republic of Germany	J.Low Temp.Phys., 55(1984)11	H. Keiber,H. Wuhl,G. P. Meisner,G. R. Stewart		
153057	MRB0391231	impurity: ZrRu	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																			2004																										ABC		Fe2P			A	6.445		3.765												K			10.1				10.1																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153058	MRB0391231	impurity: ZrRu	ZrRu(P,B)	Zr1Ru1P0.95B0.05	Zr	1	Ru	1	P	0.95	B	0.05																	2004																										ABC		Fe2P			A	6.466		3.753												K			8.4				8.4																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153059	MRB0391231	impurity: ZrRu	ZrRu(P,B)	Zr1Ru1P0.9B0.1	Zr	1	Ru	1	P	0.9	B	0.1																	2004																										ABC		Fe2P			A	6.471		3.737												K			8.1				8.1																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153060	MRB0391231	impurity: ZrRu	ZrRu(P,B)	Zr1Ru1P0.85B0.15	Zr	1	Ru	1	P	0.85	B	0.15																	2004																										ABC		Fe2P			A	6.481		3.686												K			6.4				6.4																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153061	MRB0391231	impurity: ZrRu	ZrRu(P,B)	Zr1Ru1P0.8B0.2	Zr	1	Ru	1	P	0.8	B	0.2																	2004																										ABC		Fe2P			A	6.487		3.66												K			5.4				5.4																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153062	MRB0391231	impurity: ZrRu	ZrRu(P,B)	Zr1Ru1P0.6B0.4	Zr	1	Ru	1	P	0.6	B	0.4																	2004																										ABC		Fe2P			A	6.494		3.601												K			5.6				5.6																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153063	MRB0391231		LaRu2P2	La1Ru2P2	La	1	Ru	2	P	2																			2004																										AB2C2		ThCr2Si2			A	4.032		10.632												K			4				4																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153064	MRB0391231		LaRu2(P,B)2	La1Ru2P1.6B0.4	La	1	Ru	2	P	1.6	B	0.4																	2004																										AB2C2		ThCr2Si2			A	4.037		10.477												K			2				2																																																																																																mixture - preheating (900C,1d) - arc melting with excess P					Boron substitution in ternary metal phosphide superconductors			Department of Chemistry and Princeton Materials Institute, Princeton University, Princeton, NJ 08544, USA	Mat.Res.Bull., 39(2004)1231	R.E. Schaak,R.J. Cava		
153065	PHC2920079	hydrostatic pressure. Debye-T calculated  using McMillan's equation. e-ph = 1.1	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	1997																										ABC		Fe2P																	hexagonal	K			10.3				10.3			K/GPa	-0.053																																																							180	calculated																																				arc melting					Effect of pressure on the superconductivity of ZrRuP	199712		Department of Physics, Brock University, St. Catharines, Ontario, Canada L2S 3AI	Physica.C,292(1997)79-82	F.S. Razavi,G. Quirion,H. Salamati		
153066	PCS0720434		Pr(Fe,Co)AsO	Pr1Fe0.95Co0.05As1O1	Pr	1	Fe	0.95	Co	0.05	As	1													O	1		1	2011																										ABCD		oxypnictide				3.9865		8.5988												K		4.96					4.96																																																																		uV/K	-36.9			MTP153066																								PrAs,SrAs,Pr6O11,CoAs,Fe,PrAs,FeAs,CoAs		mixture - pellet - (sealed in evacuated quartz tube) - heat(1173K,5h) - heat(1433K,40h) FC to RT					Superconductivity in Sr and Co co-doped PrFeAsO			State Key Laboratory of Silicon Materials and Department of  Physics , Zhejiang University, Hangzhou 310027, China	J.Phys.Chem.Solids, 72(2011)434	Xiao Lin,HanjieGuo,ChenyiShen,QianTao,GuanghanCao,Zhu-anXu		
153067	PCS0720434		Pr(Fe,Co)AsO	Pr1Fe0.8Co0.2As1O1	Pr	1	Fe	0.8	Co	0.2	As	1													O	1		1	2011																										ABCD		oxypnictide				3.986		8.5548												K					1.5																																																																				uV/K	-44.6			MTP153067																								PrAs,SrAs,Pr6O11,CoAs,Fe,PrAs,FeAs,CoAs		mixture - pellet - (sealed in evacuated quartz tube) - heat(1173K,5h) - heat(1433K,40h) FC to RT					Superconductivity in Sr and Co co-doped PrFeAsO			State Key Laboratory of Silicon Materials and Department of  Physics , Zhejiang University, Hangzhou 310027, China	J.Phys.Chem.Solids, 72(2011)434	Xiao Lin,HanjieGuo,ChenyiShen,QianTao,GuanghanCao,Zhu-anXu		
153068	PCS0720434		(Pr,Sr)FeAsO	Pr0.8Sr0.2Fe1As1O1	Pr	0.8	Sr	0.2	Fe	1	As	1													O	1		1	2011																										ABCD		oxypnictide																		K		15					15	MTC153068																																																																	uV/K	11			MTP153068																								PrAs,SrAs,Pr6O11,CoAs,Fe,PrAs,FeAs,CoAs		mixture - pellet - (sealed in evacuated quartz tube) - heat(1173K,5h) - heat(1433K,40h) FC to RT					Superconductivity in Sr and Co co-doped PrFeAsO			State Key Laboratory of Silicon Materials and Department of  Physics , Zhejiang University, Hangzhou 310027, China	J.Phys.Chem.Solids, 72(2011)434	Xiao Lin,HanjieGuo,ChenyiShen,QianTao,GuanghanCao,Zhu-anXu		
153069	PCS0720434		(Pr,Sr)(Fe,Co)AsO	Pr0.8Sr0.2Fe0.85Co0.15As1O1	Pr	0.8	Sr	0.2	Fe	0.85	Co	0.15	As	1											O	1		1	2011																										ABCD		oxypnictide				3.9922		8.6203												K		15.8					15.8	MTC153068																																																																	uV/K	-40.2			MTP153069																								PrAs,SrAs,Pr6O11,CoAs,Fe,PrAs,FeAs,CoAs		mixture - pellet - (sealed in evacuated quartz tube) - heat(1173K,5h) - heat(1433K,40h) FC to RT					Superconductivity in Sr and Co co-doped PrFeAsO			State Key Laboratory of Silicon Materials and Department of  Physics , Zhejiang University, Hangzhou 310027, China	J.Phys.Chem.Solids, 72(2011)434	Xiao Lin,HanjieGuo,ChenyiShen,QianTao,GuanghanCao,Zhu-anXu		
153070	PHC4710476	hydrostatic-P. AF. (dTn/dP) = 0.35 K/GPa	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2011								18.5																		AB2C2		ThCr2Si2			A			12.07												K					10																																																																																																		polycrystals - reground - pellet - (in Al2O3) - sealed in evacuated quartz tube) - heat(1190C,24h) cool to 1100 C within 100h					Dependence of magnetic ordering temperature of doped and undoped EuFe2As2 on hydrostatic pressure to 0.8 GPa			Department of Physics, Washington University, One Brookings Dr., St. Louis, MO 63130, USA	Physica C, 471(2011)476	H.B. Banks,W. Bi,L. Sun,G.F. Chen,X.H. Chen,J.S. Schilling		
153071	PHC4710476	hydrostatic-P. Ferro-mag, (dTm/dP) = 2.4 K/GPa	EuFe2(As,P)2	Eu1Fe2As1.4P0.6	Eu	1	Fe	2	As	1.4	P	0.6																3	2011							19																			AB2C2		ThCr2Si2			A			11.88												K					10																																																																																																		polycrystals - reground - pellet - (in Al2O3) - sealed in evacuated quartz tube) - heat(1190C,24h) cool to 1100 C within 100h					Dependence of magnetic ordering temperature of doped and undoped EuFe2As2 on hydrostatic pressure to 0.8 GPa			Department of Physics, Washington University, One Brookings Dr., St. Louis, MO 63130, USA	Physica C, 471(2011)476	H.B. Banks,W. Bi,L. Sun,G.F. Chen,X.H. Chen,J.S. Schilling		
153072	PHC4710476	hydrostatic-P. Ferro-mag, (dTm/dP) = 2.0 K/GPa	Eu(Fe,Co)2As2	Eu1Fe1.715Co0.285As2	Eu	1	Fe	1.715	Co	0.285	As	2																3	2011							17.7																			AB2C2		ThCr2Si2																		K					10																																																																																																		polycrystals - reground - pellet - (in Al2O3) - sealed in evacuated quartz tube) - heat(1190C,24h) cool to 1100 C within 100h					Dependence of magnetic ordering temperature of doped and undoped EuFe2As2 on hydrostatic pressure to 0.8 GPa			Department of Physics, Washington University, One Brookings Dr., St. Louis, MO 63130, USA	Physica C, 471(2011)476	H.B. Banks,W. Bi,L. Sun,G.F. Chen,X.H. Chen,J.S. Schilling		
153073	PHC4710528	second SC-Tc = 9.25 K (diamag appears). SC remained upto x = 0.15 for La1.85-1.5xSr0.15+1.5xCu1-xMnxO4	(La,Sr)2(Cu,Mn)O4	La1.76Sr0.24Cu0.94Mn0.06O4	La	1.76	Sr	0.24	Cu	0.94	Mn	0.06													O	4		1	2011																												T	I4/mmm		A	3.778		13.202												K				34			34																																																																																														La2O3,SrCO3,CuO,MnO2		mixture - heat(900C,36h, in air) - SIN(1120C - 1200C,24h)					The suppression of superconductivity by the localization of oxygen holes in the double-doped La1.85-1.5xSr0.15+1.5xCu1-xMnxO4 system			College of Physics Science and Technology, Yangzhou University, Yangzhou 225002, China	Physica C, 471(2011)528	Caixia Wang,Qibing Huang,Xiaobing Chen		
153074	PHC2920079	quasi-hydrostatic pressure upto 7 GPa.   e-ph = 0.92	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	1997																										ABC		Co2P																	ortho-	K			7.6				7.6			K/GPa	-0.098																																																																																												arc melting					Effect of pressure on the superconductivity of ZrRuP	199712		Department of Physics, Brock University, St. Catharines, Ontario, Canada L2S 3AI	Physica.C,292(1997)79-82	F.S. Razavi,G. Quirion,H. Salamati		
153075	PHC4710591	minor phase (second phase) : CsFeCl3(BaNiO3-phase) about 10%	(Tl,Cs)xFeySe2	Tl0.59Cs0.26Fe1.9Se2	Tl	0.59	Cs	0.26	Fe	1.9	Se	2																2	2011																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.881		14.057												K	28		32.6				30.3																																																																																														Tl(5N),CsCl(4N),Fe(4N),Se(6N)		mixture(Tl:Cs:Fe:Se:Cl=0.5:0.3:1.73:1.7:0.3) - heat(600C5-6h,  then 800C,9-12h) - Q to ice water					Synthesis and superconductivity in (Tl, Cs)1-xFe2-ySe2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 471(2011)591	K.J. Syu,H.H. Sung,W.H. Lee		
153076	PHC4710594	1st principle calculation. bulk and shear modulus from Voigt model. compressibility = 0.023	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																			2011															GPa		30	GPa		79						ABC		KZnAs	P6/mmm	194	A	4.2976		9.0884												K		2.4					2.4																																																																																																					Electronic bands, Fermi surface, and elastic properties of new 4.2 K superconductor SrPtAs with a honeycomb structure from first principles calculations			Institute of Solid State Chemistry, Ural Branch of the Russian Academy of Sciences, 620990 Ekaterinburg, Russia	Physica C, 471(2011)594	I.R. Shein,A.L. Ivanovskii		
153077	SSC1510130	impurity phases: delta-FeSe, Fe3O4. Debye-T estimated from isomer shift(Mossbauer). [TP300] = TP(?K).	Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																			2011																										AB	2	PbO	P4/nmm																	K				12.5			12.5																																																											460	isomer shift						uV/K				MTP153077																								Se(4N),Fe(3N),Te(2N)		mixture - sealed in quartz tube(vac) - heat(600C,20h) - reground - heat(650C,20h) - FC to RT					Observation of lattice softening at Tc in the FeSe0.5Te0.5 superconductor			Department of Physics, Abo Akademi, FI-20500 Turku, Finland	Solid State Commun., 151(2011)130	J. Linden,J.-P. Liback,M. Karppinen,E.-L. Rautama,H. Yamauchi		
153078	SSC1510404		Zr2Co	Co1Zr2	Co	1	Zr	2																				1	2011																										AB2	2		I4/mcm		A	6.366		5.511												K		5.47	5.74	5.38			5.47																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153079	SSC1510404		Zr2(Co,Ga)	Zr2Co0.95Ga0.05	Zr	2	Co	0.95	Ga	0.05																		1	2011																										AB2	2		I4/mcm		A	6.379		5.476												K		5.79	6.05	5.79			5.79																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153080	SSC1510404		Zr2(Co,Ga)	Zr2Co0.9Ga0.1	Zr	2	Co	0.9	Ga	0.1																		1	2011																										AB2	2		I4/mcm		A	6.409		5.462												K		5.72	6	5.71			5.72																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153081	SSC1510404		Zr2(Co,Ga)	Zr2Co0.85Ga0.15	Zr	2	Co	0.85	Ga	0.15																		1	2011																										AB2	2		I4/mcm		A	6.426		5.441												K		5.56	5.81	5.35			5.56																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153082	SSC1510404		Zr2(Co,Ga)	Zr2Co0.8Ga0.2	Zr	2	Co	0.8	Ga	0.2																		1	2011																										AB2	2		I4/mcm		A	6.46		5.441												K		5.29	5.55	4.92			5.29																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153083	SSC1510404		Zr2(Co,Ga)	Zr2Co0.75Ga0.25	Zr	2	Co	0.75	Ga	0.25																		1	2011																										AB2	2		I4/mcm		A	6.463		5.413												K		5.1	5.31	4.76			5.1																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153084	SSC1510404		Zr2(Co,Ga)	Zr2Co0.7Ga0.3	Zr	2	Co	0.7	Ga	0.3																		1	2011																										AB2	2		I4/mcm		A	6.463		5.403												K		4.97	5.18	4.74			4.97																																																																																														Zr(2N),C0(3N),Ga(6N)		arc-melting. ANN(820C,5d, in air) - Q to water(RT)					Substitute effects of Ga on Tc in superconducting Zr2(Co1-xGax)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Solid State Commun., 151(2011)404	K.J. Syu,C.H. Wu,S.C. Chen,W.H. Lee		
153085	SSC1510557		FeCrxSe	Fe1Cr0.01Se1	Fe	1	Cr	0.01	Se	1																			2011																										AB	2		P4/nmm																beta-FeSe	K				10.4			10.4																																																																																																mixture - sealed in quartz tube - heat(500C,24h) - reground - heat(1050C,24h) - ANN(360C,3h)					Enhanced superconducting properties in FeCrxSe			Department of Physics, IIT Bombay, Mumbai 400076, India	Solid State Commun., 151(2011)557	Anil K. Yadav,Ajay D. Thakur,C.V. Tomy		
153086	SSC1510557	impurity: alpha-FeSe(NiAs-type)	FeCrxSe	Fe1Cr0.01Se1	Fe	1	Cr	0.01	Se	1																			2011																										AB	2		P4/nmm																beta-FeSe	K				11.2			11.2																				T	resistivity 0.5Rn, WHH	23.66												MHC153086		A	from Hc2	37.3																																																										mixture - sealed in quartz tube - heat(500C,24h) - reground - heat(1050C,24h) - ANN(360C,3h)					Enhanced superconducting properties in FeCrxSe			Department of Physics, IIT Bombay, Mumbai 400076, India	Solid State Commun., 151(2011)557	Anil K. Yadav,Ajay D. Thakur,C.V. Tomy		
153087	JPS0290879		Zr2Co	Co1Zr2	Co	1	Zr	2																				1	1970																										AB2		CuAl2			A	6.4		5.5331											CuAl2, C16	K		5					5																																																											230	Lindeman eq.																																		Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153088	JPS0290879		Zr2(Co,Ni)	Zr2Co0.85Ni0.15	Zr	2	Co	0.85	Ni	0.15																		1	1970																										AB2		CuAl2			A	6.4106		5.4906											CuAl2, C16	K		5.92					5.92																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153089	JPS0290879		Zr2(Co,Ni)	Zr2Co0.75Ni0.25	Zr	2	Co	0.75	Ni	0.25																		1	1970																										AB2		CuAl2			A	6.4288		5.4469											CuAl2, C16	K		4.91					4.91																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153090	JPS0290879		Zr2(Co,Ni)	Zr2Co0.5Ni0.5	Zr	2	Co	0.5	Ni	0.5																		1	1970																										AB2		CuAl2			A	6.45		5.3925											CuAl2, C16	K		3.11					3.11																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153091	JPS0290879		Zr2(Co,Ni)	Zr2Co0.3Ni0.7	Zr	2	Co	0.3	Ni	0.7																		1	1970																										AB2		CuAl2			A	6.4794		5.3538											CuAl2, C16	K		1.87					1.87																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153092	JPS0290879		Zr2(Co,Ni)	Zr2Co0.15Ni0.85	Zr	2	Co	0.15	Ni	0.85																		1	1970																										AB2		CuAl2			A	6.495		5.3181											CuAl2, C16	K		1.4					1.4																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153093	JPS0290879		Zr2Ni	Ni1Zr2	Ni	1	Zr	2																				1	1970																										AB2		CuAl2			A	6.5163		5.2869											CuAl2, C16	K		1.56					1.56																																																																																														Co(4N),Ni(4N),Zr		melt in plasma jet furnace. ANN(900C,10d, in vac)					Superconductivity and magnetic susceptibility of Zr2Co-Zr2Ni system			Department of Physics, Faculty of Science, Hokkaido University, Sapporo	J.Phys.Soc.Jpn, 29(1970)879	K.Yamaya,T.Sambongi,T.Mitsui		
153094	SSC0940425		LaPtSi	La1Pt1Si1	La	1	Pt	1	Si	1																		1	1995																										ABC		LaPtSi	I4<1>md		A	4.25		14.52												K	5.2		3.4				4.3																																																																							mOhm.cm											0.625												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153095	SSC0940425		La(Pt,Ni)Si	La1Pt0.9Ni0.1Si1	La	1	Pt	0.9	Ni	0.1	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.247		14.483												K	3.18		3.28				3.23																																																																							mOhm.cm											0.195												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153096	SSC0940425		La(Pt,Ni)Si	La1Pt0.8Ni0.2Si1	La	1	Pt	0.8	Ni	0.2	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.241		14.442												K	2.81		2.83				2.82																																																																							mOhm.cm											0.28												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153097	SSC0940425		La(Pt,Ni)Si	La1Pt0.7Ni0.3Si1	La	1	Pt	0.7	Ni	0.3	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.232		14.392												K	2.71		2.84				2.775																																																																							mOhm.cm											0.285												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153098	SSC0940425		La(Pt,Ni)Si	La1Pt0.6Ni0.4Si1	La	1	Pt	0.6	Ni	0.4	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.228		14.348												K	2.56		2.7				2.63																																																																							mOhm.cm											0.19												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153099	SSC0940425		La(Pt,Ni)Si	La1Pt0.5Ni0.5Si1	La	1	Pt	0.5	Ni	0.5	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.219		14.306												K	2.2		2.37				2.285																																																																							mOhm.cm											0.32												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153100	SSC0940425		La(Pt,Ni)Si	La1Pt0.4Ni0.6Si1	La	1	Pt	0.4	Ni	0.6	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.211		14.245												K	1.9		1.99				1.945	MTC153100																																																																						mOhm.cm											0.205												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153101	SSC0940425		La(Pt,Ni)Si	La1Pt0.3Ni0.7Si1	La	1	Pt	0.3	Ni	0.7	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.203		14.199												K	1.62		1.69				1.655																																																																							mOhm.cm											0.15												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153102	SSC0940425		La(Pt,Ni)Si	La1Pt0.1Ni0.9Si1	La	1	Pt	0.1	Ni	0.9	Si	1																1	1995																										ABC		LaPtSi	I4<1>md		A	4.191		14.127												K	1.26		1.29				1.275																																																																							mOhm.cm											0.1												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153103	SSC0940425		LaNiSi	La1Ni1Si1	La	1	Ni	1	Si	1																		1	1995																										ABC		LaPtSi	I4<1>md		A	4.181		14.069												K	1.2		1.26				1.23																																																																							mOhm.cm											0.1												Pt(5N),Ni(3N),Si(9N),La(3N)		arc-melting. ANN(1200C,4d, in Ar) or ANN(1000C,7-10d) for Ni-rich compounds					SUPERCONDUCTIVITY OF Ni-DOPED LaPtSi			Department of Physics, National Chung Cheng University Ming-Hsiung, Chia-Yi 621. Taiwun, Republic of China	Solid State Commun., 94(1995)425	W.H.Lee		
153104	PRB05006523	RRR=7.2. (dC/gamma*Tc) = 1.46. lattice term in SP(beta) = 0.487 mJ/mol.K4.	LaNiSi	La1Ni1Si1	La	1	Ni	1	Si	1																			1994																										ABC		LaPtSi	I4<1>md		A	4.181		14.069												K	1.2		1.26			0.06	1.23																																																3.5	14				MSP153104			mJ/mol.K2	8.89	SP-heat	229	SP-heat											uOhm.cm							13.9																		See Phys.Rev.B, 79(2009)014522					Crystal structure and superconductivity in the Ni-based ternary compound LaNisi			Department of Physics, National Chung Cheng University, Ming Hsi-ung, Chia Yi -621, Taiwan, Republic of China	Phys.Rev.B, 50(1994)6523	W. H. Lee,F. A. Yang,C. R. Shih,H. D. Yang		
153105	NMT008L630	Tc(max) = 36.7 K at P = 8.9 GPa. (dTc/dP) = 3.2 and -1.7 K/GPa for 0<P<8.9 and for P>8.9 GPa, respectively. Mossbauer effect measured.	beta-Fe1.01Se	Fe1.01Se1	Fe	1.01	Se	1																				1	2009																										AB																				K			8				8	MTC153105		K/GPa	12.6																																																																																																	Electronic and magnetic phase diagram of beta-Fe1:01Se with superconductivity at 36.7 K under pressure			Institut fur Anorganische und Analytische Chemie, University Mainz, 55099 Mainz, Germany,	Nature Materials, 8(2009)L630	S. Medvedev,T. M. McQueen,I. A. Troyan,T. Palasyuk,M. I. Eremets,R. J. Cava,S. Naghavi,F. Casper,V. Ksenofontov,G.Wortmann,C. Felser		
153106	PRB084092505	Phase-I (P<8.2 GPa). not SC.	B4Te3-I	Bi4Te3	Bi	4	Te	3																					2011																		GPa		52						A3B4			R3[-]m		A	4.451		41.888											trigonal	K					1																																																																																																Bi,Te(4N)		mixture - (evacuated quartz tube) - melt(700C,5d) - Q to Liq.N2 - ANN(440C,14d)					Distinct superconducting states in the pressure-induced metallic structures of the nominal semimetal Bi4Te3			Condensed Matter and Materials Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 84(2011)092505	J. R. Jeffries,A. L. Lima Sharma,P. A. Sharma,C. D. Spataru,S. K. McCall,J. D. Sugar,S. T. Weir,Y. K. Vohra		
153107	PRB084092505	Phase-II (8.2 <P <12.8 GPa.	B4Te3-II	Bi4Te3	Bi	4	Te	3																					2011																										A3B4			C2/m		A	4.311	4.6052	6.2641											monoclinic, beta = 110.22	K			2.1				2.1	MTC153107																																																																																													Bi,Te(4N)		mixture - (evacuated quartz tube) - melt(700C,5d) - Q to Liq.N2 - ANN(440C,14d)					Distinct superconducting states in the pressure-induced metallic structures of the nominal semimetal Bi4Te3			Condensed Matter and Materials Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 84(2011)092505	J. R. Jeffries,A. L. Lima Sharma,P. A. Sharma,C. D. Spataru,S. K. McCall,J. D. Sugar,S. T. Weir,Y. K. Vohra		
153108	PRB084092505	Phase-IV (P>16.2 GPa.	B4Te3-IV	Bi4Te3	Bi	4	Te	3																					2011																				120						A3B4			Im3[-]4		A	3.6702													bcc	K			8.4				8.4	MTC153107																																																																																													Bi,Te(4N)		mixture - (evacuated quartz tube) - melt(700C,5d) - Q to Liq.N2 - ANN(440C,14d)					Distinct superconducting states in the pressure-induced metallic structures of the nominal semimetal Bi4Te3			Condensed Matter and Materials Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 84(2011)092505	J. R. Jeffries,A. L. Lima Sharma,P. A. Sharma,C. D. Spataru,S. K. McCall,J. D. Sugar,S. T. Weir,Y. K. Vohra		
153109	EPL09567002	compositions by EDXS. Anisotropy (Hc2) = 3.3	(Ca,La)Fe2As2	Ca0.8La0.2Fe2As2	Ca	0.8	La	0.2	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2																		K			42.7	40			40																				T	resistivity 0.9Rn, WHH		185	55.6					T/K	resistivity 0.5+AD919Rn		6.25	1.88	MHC153109																																																														FeAs self-flux method					Synthesis and properties of La-doped CaFe2As2 single crystals with Tc = 42.7K			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences Beijing 100190, China	EuroPhys. Lett., 95(2011)67002	Zhaoshun Gao,Yanpeng Qi,Lei Wang,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Yanwei Ma		
153110	PRB084094513	[gap], [penet] are from muon-SR analysis. Two gaps:  large gap in DB, small one = 3.2 meV, (2d/kTc) = 2.0	(Ba,Rb)Fe2As2	Ba0.7Rb0.3Fe2As2	Ba	0.7	Rb	0.3	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2																		K		36.9					36.9																																									A	muon-SR	2490			meV	9.2	5.8	16																																													BaAs,RbAs,Fe2As		solid state reaction. mixture - pellet - (alumina crucible) - ANN(650C, 100h)					Muon-spin rotation measurements of the magnetic penetration depth in the iron-based superconductor Ba1-xRbxFe2As2			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 84(2011)094513	Z. Guguchia,Z. Shermadini,A. Amato,A. Maisuradze,A. Shengelaya,Z. Bukowski,H. Luetkens,R. Khasanov,J. Karpinski,H. Keller		
153111	PRB084094513	[gap], [penet] are from muon-SR analysis. Two gaps:  large gap in DB, small one = 2.9 meV, (2d/kTc) = 1.9	(Ba,Rb)Fe2As2	Ba0.65Rb0.35Fe2As2	Ba	0.65	Rb	0.35	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2																		K		35.8					35.8																																									A	muon-SR	2500			meV	8.8	5.7	16																																													BaAs,RbAs,Fe2As		solid state reaction. mixture - pellet - (alumina crucible) - ANN(650C, 100h)					Muon-spin rotation measurements of the magnetic penetration depth in the iron-based superconductor Ba1-xRbxFe2As2			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 84(2011)094513	Z. Guguchia,Z. Shermadini,A. Amato,A. Maisuradze,A. Shengelaya,Z. Bukowski,H. Luetkens,R. Khasanov,J. Karpinski,H. Keller		
153112	PRB084094513	[gap], [penet] are from muon-SR analysis. Two gaps:  large gap in DB, small one = 1.1 meV, (2d/kTc) = 0.8	(Ba,Rb)Fe2As2	Ba0.6Rb0.4Fe2As2	Ba	0.6	Rb	0.4	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2																		K		34					34																																									A	muon-SR	2550			meV	7.5	5.1	16																																													BaAs,RbAs,Fe2As		solid state reaction. mixture - pellet - (alumina crucible) - ANN(650C, 100h)					Muon-spin rotation measurements of the magnetic penetration depth in the iron-based superconductor Ba1-xRbxFe2As2			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 84(2011)094513	Z. Guguchia,Z. Shermadini,A. Amato,A. Maisuradze,A. Shengelaya,Z. Bukowski,H. Luetkens,R. Khasanov,J. Karpinski,H. Keller		
153113	PRB084100501	hydrostatic pressure. Neel-T defined as T where magnetic volume fraction = 50%.	La(O,F)FeAs	La1Fe1As1F0.055O0.945	La	1	Fe	1	As	1	F	0.055													O	0.945			2011								44																		ABCD		oxypnictide																		K				7			7	TC153113																																																																																													LaAs,FeAs,Fe2O3,Fe,LaF3		high-P synthesis. mixture - (P=3GPa) - heat(1320C,5.5h,P=3 GPa) - Q to RT.					Tuning of competing magnetic and superconducting phase volumes in LaFeAsO0.945F0.055 by hydrostatic pressure			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)100501	R. Khasanov,S. Sanna,G. Prando,Z. Shermadini,M. Bendele,A. Amato,P. Carretta,R. De Renzi,J. Karpinski,S. Katrych,H. Luetkens,N. D. Zhigadlo		
153114	PRB084064518	RRR = 160.GL-parameter=7.6. thermodynamic Hc(0)=650 Oe. (dC/gamma*Tc) = 1.2. lattice term in SP(beta) = 0.8 mJ/mol.K4	alpha-BiPd	Bi1Pd1	Bi	1	Pd	1																				3	2011																										AB			P2<1>		A	5.6284	10.6615	5.6752											alpha-BiPd(monoclinic), beta=101 degree	K		3.8				0.01	3.8											Oe	gamma, Hc1,Hc2	123							T	resistivity 0.5Rn, parabolic	0.7							T/K	resistivity 0.5Rn	0.3			MHC153114		A	from Hc2	170			A	calculate from other data using GL-eq	1292													mJ/mol.K2	4	SP-heat, 1.9<T<5K	169	SP-heat, 1.9<T<5K											uOhm.cm							0.3				130												Bi(5N),Pd(4N)		modified Bridgeman method. heat(650C) - slow cool to RT (1C/h)					Superconductivity in noncentrosymmetric BiPd			Department of Condensed Matter Physics and Materials Science, Tata Institute of Fundamental Research, Mumbai 400005, India	Phys.Rev.B, 84(2011)064518	Bhanu Joshi,A. Thamizhavel,S. Ramakrishnan		
153115	PRB084104502	RRR=18.4. Hc2 extrapolation: Hc2(0)= 30 and 23T for H//ab and H//c. best fitting: makiparameter(alpha) = 0.9, PHc2(0)=30 T. Anisotropy= 3.0(Tc), 1.30(0K)	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2011																										ABC		PbFCl																		K		17.4				2.7	17.4																				T	resistivity 0.5Rn, WHH dirty limit		39.6	19.7					T/K	resistivity 0.5Rn		3.3	1.64	MHC153115		A	from Hc2		40.9	20.3																															uOhm.cm							29				540														Sn-flux method. LiFeAs:Sn = 1:10 in alumina crucible - sealed in evacuated quartz tube.					Pauli-limiting effects in the upper critical fields of a clean LiFeAs single crystal			CeNSCMR, Department of Physics and Astronomy, Seoul National University, Seoul 151-747, Republic of Korea	Phys.Rev.B, 84(2011)104502	Seunghyun Khim,Bumsung Lee,Jae Wook Kim,Eun Sang Choi,G. R. Stewart,Kee Hoon Kim		
153116	PRB084104520		Yb(Ga,Si)	Yb1Ga1.1Si0.9	Yb	1	Ga	1.1	Si	0.9																			2011																		GPa		41						AB2		AlB2	P6/mmm		A	4.1275		4.2357												K			2.4				2.4	MTC153116		K/GPa	-0.78																																																																																												arc-melting - ANN					Pressure effect on critical temperature for superconductivity and lattice parameters of AlB2-type ternary silicide YbGa1.1Si0.9			Center for Transdisciplinary Research, Niigata University, 8050 Ikarashi-Ninocho, Nishi-ku, Niigata, Niigata 950-2181, Japan	Phys.Rev.B, 84(2011)104520	Koji Fujimaki,Fumihiro Ishikawa,Yuh Yamada,Naohito Tsujii,Motoharu Imai		
153117	PRB084104520		CaGaSi	Ca1Ga1Si1	Ca	1	Ga	1	Si	1																			2011																		GPa		42						ABC		AlB2	P6/mmm		A	4.12		4.4401												K			4.3				4.3	MTC153117		K/GPa	-0.11																																																																																												Ca:Ga:Si = 1.03:1:1) - arc-melting - BN capsule - sealed in quartz tube (Ar) - remelt(1470K,6h) cool to 1270 K (4K/h)					Pressure effect on critical temperature for superconductivity and lattice parameters of AlB2-type ternary silicide YbGa1.1Si0.9			Center for Transdisciplinary Research, Niigata University, 8050 Ikarashi-Ninocho, Nishi-ku, Niigata, Niigata 950-2181, Japan	Phys.Rev.B, 84(2011)104520	Koji Fujimaki,Fumihiro Ishikawa,Yuh Yamada,Naohito Tsujii,Motoharu Imai		
153118	PRB084104523	structural transition T<STR> = 160 K. At T=2K, space-G: cmme, a = 5.7063, b = 5.6788 , c = 8.7094	LaOFeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1		1	2011								145																		ABCD		oxypnictide	P4/nmm		A	4.0322		8.7364												K					4																																																																																																		solid state reaction					Effect of the isoelectronic substitution of Sb for As on the magnetic and structural properties of LaFe(As1-xSbx)O			Institut Neel, CNRS and UJF, 38042 Grenoble, France	Phys.Rev.B, 84(2011)104523	F. Levy-Bertrand,C. Marcenat,A. Sulpice,J. Marcus,S. Pairis,T. Klein,M. Nunez-Regueiro,G. Garbarino,T. Hansen,V. Nassif,P. Toulemonde		
153119	PRB084104523	structural transition T<STR> = 150 K. At T=2K, space-G: cmme, a = 5.7482, b = 5.7185 , c = 8.7799	LaOFe(As,Sb)	La1Fe1As0.8Sb0.2O1	La	1	Fe	1	As	0.8	Sb	0.2													O	1		1	2011								140																		ABCD		oxypnictide	P4/nmm		A	4.0607		8.8133												K					4																																																																																																		solid state reaction					Effect of the isoelectronic substitution of Sb for As on the magnetic and structural properties of LaFe(As1-xSbx)O			Institut Neel, CNRS and UJF, 38042 Grenoble, France	Phys.Rev.B, 84(2011)104523	F. Levy-Bertrand,C. Marcenat,A. Sulpice,J. Marcus,S. Pairis,T. Klein,M. Nunez-Regueiro,G. Garbarino,T. Hansen,V. Nassif,P. Toulemonde		
153120	PRB084104523	structural transition T<STR> = 130 K. At T=2K, space-G: cmme, a = 5.7830, b = 5.7507 , c = 8.8606	LaOFe(As,Sb)	La1Fe1As0.6Sb0.4O1	La	1	Fe	1	As	0.6	Sb	0.4													O	1		1	2011								120																		ABCD		oxypnictide	P4/nmm		A	4.0835		8.9014												K					4																																																																																																		solid state reaction					Effect of the isoelectronic substitution of Sb for As on the magnetic and structural properties of LaFe(As1-xSbx)O			Institut Neel, CNRS and UJF, 38042 Grenoble, France	Phys.Rev.B, 84(2011)104523	F. Levy-Bertrand,C. Marcenat,A. Sulpice,J. Marcus,S. Pairis,T. Klein,M. Nunez-Regueiro,G. Garbarino,T. Hansen,V. Nassif,P. Toulemonde		
153121	PRB077144502		1H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2008																										ABC		AlB2																		K				6.5		0.1	6.5	MTC153121		K/GPa	-0.3																																																																																												single crystals grown by floating zone method					Pressure effects on the superconducting transition in nH-CaAlSi			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany	Phys.Rev.B, 77(2008)144502	L. Boeri,J. S. Kim,M. Giantomassi,F. S. Razavi,S. Kuroiwa,J. Akimitsu,R. K. Kremer		
153122	PRB077144502		5H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2008																										ABC		AlB2																		K				5.95		0.4	5.95	MTC153122		K/GPa	0.13																																																																																												single crystals grown by floating zone method					Pressure effects on the superconducting transition in nH-CaAlSi			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany	Phys.Rev.B, 77(2008)144502	L. Boeri,J. S. Kim,M. Giantomassi,F. S. Razavi,S. Kuroiwa,J. Akimitsu,R. K. Kremer		
153123	PRB077144502		6H-CaAlSi	Ca1Al1Si1	Ca	1	Al	1	Si	1																		3	2008																										ABC		AlB2																		K				7.89		0.1	7.89	MTC153123																																																																																															single crystals grown by floating zone method					Pressure effects on the superconducting transition in nH-CaAlSi			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany	Phys.Rev.B, 77(2008)144502	L. Boeri,J. S. Kim,M. Giantomassi,F. S. Razavi,S. Kuroiwa,J. Akimitsu,R. K. Kremer		
153124	SST022045017	RRR = 5.8.	La(O,F)Fe(As,Sb)	La1Fe1As0.95Sb0.05F0.2O0.8	La	1	Fe	1	As	0.95	Sb	0.05	F	0.2											O	0.8		1	2009																										ABCD		oxypnictide			A	4.02		8.701												K			30.1				30.1																				T	resistivity 0.9Rn, WHH	69							T/K	resistivity, 0.9Rn	3.34			HC153124		A	from Hc2	22																												uV/K	-25			TP153125	mOrm.cm											3.8										n/cm3	730000000000000000000	LaO3,LaF3,La,FeAs,FeSb,Fe		two step solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in silica ampules - ANN(1150C,48h) - cool to RT					Enhancement of the superconducting transition temperature and upper critical field of LaO0.8F0.2FeAs with antimony doping			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	Supercond.Sci.Technol., 22(2009)045017	S J Singh,J Prakash,S Patnaik,A K Ganguli		
153125	SST022045017	RRR = 3.9	La(O,F)Fe(As,Sb)	La1Fe1As0.9Sb0.1F0.2O0.8	La	1	Fe	1	As	0.9	Sb	0.1	F	0.2											O	0.8		1	2009																										ABCD		oxypnictide			A	4.023		8.719												K			28.6				28.6																				T	resistivity 0.9Rn, WHH	73							T/K	resistivity, 0.9Rn	3.7																																								mOrm.cm											5.9										n/cm3	650000000000000000000	LaO3,LaF3,La,FeAs,FeSb,Fe		two step solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in silica ampules - ANN(1150C,48h) - cool to RT					Enhancement of the superconducting transition temperature and upper critical field of LaO0.8F0.2FeAs with antimony doping			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	Supercond.Sci.Technol., 22(2009)045017	S J Singh,J Prakash,S Patnaik,A K Ganguli		
153126	PRL107137003	new formula: Rb2Fe4Se5. magnetic moment at 295 K. Fe vacancy order-disorder transition temperature T<STR> = 515 K.	Rb2Fe4Se5	Rb0.88Fe1.81Se2	Rb	0.88	Fe	1.81	Se	2																		3	2011					myu-B/Fe	3.3		502																		A2B4C5			I4/mmm		A	8.788		14.597												K		32					32																																																																																																					Common Crystalline and Magnetic Structure of Superconducting A2Fe4Se5 (A = K, Rb, Cs, Tl) Single Crystals Measured Using Neutron Diffraction			Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 107(2011)137003	F. Ye,S. Chi,Wei Bao,X. F. Wang,J. J. Ying,X. H. Chen,H. D. Wang,C. H. Dong,Minghu Fang		
153127	PRL107137003	new formula: Cs2Fe4Se5. magnetic moment at 295 K. Fe vacancy order-disorder transition temperature T<STR> = 500 K.	Cs2Fe4Se5	Cs0.86Fe1.66Se2	Cs	0.86	Fe	1.66	Se	2																		3	2011					myu-B/Fe	3.4		471																		A2B4C5			I4/mmm		A	8.865		15.289												K		29					29																																																																																																					Common Crystalline and Magnetic Structure of Superconducting A2Fe4Se5 (A = K, Rb, Cs, Tl) Single Crystals Measured Using Neutron Diffraction			Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 107(2011)137003	F. Ye,S. Chi,Wei Bao,X. F. Wang,J. J. Ying,X. H. Chen,H. D. Wang,C. H. Dong,Minghu Fang		
153128	PRL107137003	new formula: (Tl,K)2Fe4Se5. magnetic moment at 295 K. Fe vacancy order-disorder transition temperature T<STR> = 533 K.	(Tl,K)2Fe4Se5	Tl0.4K0.3Fe1.7Se2	Tl	0.4	K	0.3	Fe	1.7	Se	2																3	2011					myu-B/Fe	3.2		506																		A2B4C5			I4/mmm		A	8.645		14.061												K		28					28																																																																																																					Common Crystalline and Magnetic Structure of Superconducting A2Fe4Se5 (A = K, Rb, Cs, Tl) Single Crystals Measured Using Neutron Diffraction			Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 107(2011)137003	F. Ye,S. Chi,Wei Bao,X. F. Wang,J. J. Ying,X. H. Chen,H. D. Wang,C. H. Dong,Minghu Fang		
153129	PRL107137003	new formula: (Tl,Rb)2Fe4Se5. magnetic moment at 295 K. Fe vacancy order-disorder transition temperature T<STR> = 512 K.	(Tl,Rb)2Fe4Se5	Tl0.4Rb0.4Fe1.6Se2	Tl	0.4	Rb	0.4	Fe	1.6	Se	2																3	2011					myu-B/Fe	3.2		511																		A2B4C5			I4/mmm		A	8.683		14.388												K		32					32																																																																																																					Common Crystalline and Magnetic Structure of Superconducting A2Fe4Se5 (A = K, Rb, Cs, Tl) Single Crystals Measured Using Neutron Diffraction			Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 107(2011)137003	F. Ye,S. Chi,Wei Bao,X. F. Wang,J. J. Ying,X. H. Chen,H. D. Wang,C. H. Dong,Minghu Fang		
153130	PRL107137003	new formula: K2Fe4Se5. magnetic moment at 295 K. Fe vacancy order-disorder transition temperature T<STR> = 578 K.	K2Fe4Se5	K0.86Fe1.66Se2	K	0.86	Fe	1.66	Se	2																		3	2011					myu-B/Fe	3.31		559																		A2B4C5			I4/mmm		A	8.7306		14.1128												K		32					32																																																																																																					Common Crystalline and Magnetic Structure of Superconducting A2Fe4Se5 (A = K, Rb, Cs, Tl) Single Crystals Measured Using Neutron Diffraction			Neutron Scattering Science Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 107(2011)137003	F. Ye,S. Chi,Wei Bao,X. F. Wang,J. J. Ying,X. H. Chen,H. D. Wang,C. H. Dong,Minghu Fang		
153131	EPL09427008	Fe-content not given(estimated value). Fe-vacancy ordered temperture T<STR> = 551  K.	KxFeySe2	K0.8Fe1.7Se2	K	0.8	Fe	1.7	Se	2																		3	2011								540																		AB2C2		ThCr2Si2																		K	30.5		31.5				31																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153132	EPL09427008	Fe-content not given(estimated value). Fe-vacancy ordered temperture T<STR> = 540  K.	RbxFeySe2	Rb0.8Fe1.7Se2	Rb	0.8	Fe	1.7	Se	2																		3	2011								534																		AB2C2		ThCr2Si2																		K	31.5		32				31.75																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153133	EPL09427008	Fe-content not given(estimated value). Fe-vacancy ordered temperture T<STR> = 525  K.	CsxFeySe2	Cs0.8Fe1.7Se2	Cs	0.8	Fe	1.7	Se	2																		3	2011								504																		AB2C2		ThCr2Si2																		K	27.5		30.9				29.2																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153134	EPL09427008	Fe-content not given(estimated value). Fe-vacancy ordered temperture T<STR> =  515 K.	(Tl,K)xFeySe2	Tl0.4K0.3Fe1.7Se2	Tl	0.4	K	0.3	Fe	1.7	Se	2																3	2011								496																		AB2C2		ThCr2Si2																		K	24.8		27.7				26.25																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153135	EPL09427008	Fe-content not given(estimated value). Fe-vacancy ordered temperture T<STR> =  512 K.	(Tl,Rb)xFeySe2	Tl0.4Rb0.4Fe1.7Se2	Tl	0.4	Rb	0.4	Fe	1.7	Se	2																3	2011								500																		AB2C2		ThCr2Si2																		K	30.9		31.8				31.35																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153136	SSC1511455	GL-parameter = 4.8. lattice term in SP (beta) = 0.114 mJ/mol.K4. (dC/gamma*Tc) = 1.39	Mo5SiB2	Mo5Si1B2	Mo	5	Si	1	B	2																		1	2011																												Cr5B3			A	6.001		11.022												K			5.8	5.8			5.8										120	Oe	M-H curve	262			232			1.8	T	SUS. WHH	0.606			0.55			1.8						MHC153136		A	from Hc2	233			A	Hc1,Hc2,GL	1120										MSP153136			mJ/mol.K2	16.98	SP-heat	515	SP-heat																																				arc-melting  - ANN(1800C,24h, in vac)					Superconductivity in Mo5SiB2			Escola de Engenharia de Lorena, Universidade de Sao Paulo, P.O. Box 116, Lorena, SP, Brazil	Solid State Commum., 151(2011)1455	A.J.S. Machado,A.M.S. Costa,C.A. Nunes,C.A.M. dos Santos,T. Grant,Z. Fisk		
153137	PRB084064533	Anisotropy(Hc2) = 1.85. GL-parameter = 82.	(Ca,Na)Fe2As2	Ca0.5Na0.5Fe2As2	Ca	0.5	Na	0.5	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.87		12.049												K			19.4				19.4																													T/K	resistivity		4	2.2	MHC153137							A	penet(L)		1460																																																		NaAs,CaAs,FeAs,Fe2As		self-flux method. mixture - (alumina crucible) - Ta crucible, 1.6 atm Ar) - (quartz ampoule) - heat(1160C) - cool slowly(5C/h)					Effect of doping on structural and superconducting properties in Ca1-xNaxFe2As2 single crystals (x =0.5, 0.6, 0.75)			MPA-STC, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 84(2011)064533	N. Haberkorn,B. Maiorov,M. Jaime,I. Usov,M. Miura,G. F. Chen,W. Yu,L. Civale		
153138	PRB084064533		(Ca,Na)Fe2As2	Ca0.4Na0.6Fe2As2	Ca	0.4	Na	0.6	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.8496		12.147												K			25				25																																																																																														NaAs,CaAs,FeAs,Fe2As		self-flux method. mixture - (alumina crucible) - Ta crucible, 1.6 atm Ar) - (quartz ampoule) - heat(1160C) - cool slowly(5C/h)					Effect of doping on structural and superconducting properties in Ca1-xNaxFe2As2 single crystals (x =0.5, 0.6, 0.75)			MPA-STC, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 84(2011)064533	N. Haberkorn,B. Maiorov,M. Jaime,I. Usov,M. Miura,G. F. Chen,W. Yu,L. Civale		
153139	PRB084064533	Two step transition in R(T).  Anisotropy(Hc2) = 1.85. GL-parameter = 91.	(Ca,Na)Fe2As2	Ca0.25Na0.75Fe2As2	Ca	0.25	Na	0.75	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.84		12.248												K			33.4				33.4																													T/K	resistivity		7.15	4	MHC153139							A	penet(L)		1000																																																		NaAs,CaAs,FeAs,Fe2As		self-flux method. mixture - (alumina crucible) - Ta crucible, 1.6 atm Ar) - (quartz ampoule) - heat(1160C) - cool slowly(5C/h)					Effect of doping on structural and superconducting properties in Ca1-xNaxFe2As2 single crystals (x =0.5, 0.6, 0.75)			MPA-STC, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 84(2011)064533	N. Haberkorn,B. Maiorov,M. Jaime,I. Usov,M. Miura,G. F. Chen,W. Yu,L. Civale		
153140	PRB084064525	Two gaps: (2d/kTc) = 2.12 and 4.16 from best-fitting of SP-data. SP shows anomaly around 12 K (maybe 2nd gap). (dC/gamma*Tc) = 1.26	(Ba,Na)Fe2As2	Ba0.65Na0.35Fe2As2	Ba	0.65	Na	0.35	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2																		K		29.4		29.7			29.4																																																					MSP153140			mJ/mol.K2	57.5	SP-heat																																						self-flux method					Multigap superconductivity in single crystals of Ba0.65Na0.35Fe2As2: A calorimetric investigation			Institute for Solid State Research, IFW Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 84(2011)064525	A. K. Pramanik,M. Abdel-Hafiez,S. Aswartham,A. U. B. Wolter,S. Wurmehl,V. Kataev,B. Buchner		
153141	SSC1510778	R(T,H) shows Hc2(0) nearly equal to 500 Oe. SP shows bulk SP transition. (dC/gamma*Tc) = 0.50. compositions: Y1.3Ni0.9Ge2.8 from XRD.	YNiGe3	Y1Ni1Ge3	Y	1	Ni	1	Ge	3																		1	2011																										ABC3		SmNiGe3			A	4.06	21.529	4.063												K			0.46				0.46																																																																																																mixture - pellet - wrapped in Mo-foil - sealed in silica tube - ANN(800C,1w)					Superconducting phase transition in YNiGe3, a non-f -electron reference to the unconventional superconductor CeNiGe3			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-950 Wroc?aw 2, Poland	Solid State Commum., 151(2011)778	Adam P. Pikul,Daniel Gnida		
153142	SSC1510956	Hirr(0) = 146 T.  Hc1( 4.1K) = 1120 Oe	(Nd,Ba)(O,F)FeAs	Nd0.8Ba0.2Fe1As1F0.4O0.6	Nd	0.8	Ba	0.2	Fe	1	As	1	F	0.4											O	0.6			2011																										ABCD		oxypnictide	P4/nmm		A	3.962		8.536												K			50.03			1.86	50.03											Oe	M-H curve				1120			4.1	T	resistivity 0.9Rn, WHH	162.8							T/K	resistivity	0.85			HC153142																																																												Fe2As,NdAs,FeO		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(1160C)					Magnetization and characteristic fields in Nd0.8Ba0.2FeAsO0.6F0.4 with binary doping			Research Center for Superconductors and Applied Technologies, Physics Department, Shanghai University, Shanghai 200444, China	Solid State Commum., 151(2011)956	C.Q. Qu,C.B. Cai,M.F. Wang,C.Z. Chen,F.Q. Huang		
153143	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	GdBa2Cu3O7	Gd1Ba2Cu3O7-z	Gd	1	Ba	2	Cu	3															O	7-z		1	2011																												Y123			A	3.854	3.898	11.698												K		91.8					91.8																				T	resistivity, WHH	84																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153144	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	(Gd,Pr)Ba2Cu3O7	Gd0.95Pr0.05Ba2Cu3O7-z	Gd	0.95	Pr	0.05	Ba	2	Cu	3													O	7-z		1	2011																												Y123			A	3.844	3.904	11.675												K		86.5					86.5																				T	resistivity, WHH	95																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153145	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	(Gd,Pr)Ba2(Cu,Mn)3O7	Gd0.95Pr0.05Ba2Cu2.94Mn0.06O7-z	Gd	0.95	Pr	0.05	Ba	2	Cu	2.94	Mn	0.06											O	7-z		1	2011																												Y123			A	3.851	3.898	11.689												K		68					68																				T	resistivity, WHH	160																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153146	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	(Gd,Pr)Ba2(Cu,Fe)3O7	Gd0.95Pr0.05Ba2Cu2.94Fe0.06O7-z	Gd	0.95	Pr	0.05	Ba	2	Cu	2.94	Fe	0.06											O	7-z		1	2011																												Y123			A	3.863	3.895	11.679												K		54.5					54.5																				T	resistivity, WHH	140																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153147	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	(Gd,Pr)Ba2(Cu,Ni)3O7	Gd0.95Pr0.05Ba2Cu2.94Ni0.06O7-z	Gd	0.95	Pr	0.05	Ba	2	Cu	2.94	Ni	0.06											O	7-z		1	2011																												Y123			A	3.824	3.913	11.651												K		64					64																				T	resistivity, WHH	64																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153148	SSC1511117	thermal conductivity, thermo power, SP-heat were measured.	(Gd,Pr)Ba2(Cu,Zn)3O7	Gd0.95Pr0.05Ba2Cu2.94Zn0.06O7-z	Gd	0.95	Pr	0.05	Ba	2	Cu	2.94	Zn	0.06											O	7-z		1	2011																												Y123			A	3.834	3.913	11.675												K		46.2					46.2																				T	resistivity, WHH	48																																																																										mixture - CAL(930C,12h, in air) - cold press - SIN(930C,72h, in flowing O2) - cool to 450C and hold(6h) - slow cool to RT					Magneto-resistance, thermal conductivity, thermo-electric power and specific heat of superconductor Gd0.95Pr0.05Ba2Cu2.94M0.06O7-z (M = Fe, Ni, Zn and Mn)			Department of Electronics and Telecommunication Engineering, Jadavpur University, Kolkata-700032, India	Solid State Commum., 151(2011)1117	Tirthankar Chakraborty,Bhasker Gahtori,Ajay Soni,G.S. Okram,S.K. Agrawal,S.-Y. Chen,Y.-K. Kuo,M.A.H. Ahsan,Ashok Rao		
153149	SSC1511400	O-content not given	(Cu,Mo)Sr2(Y,Ce)5Cu2O15	Mo0.25Sr2Y1Ce4Cu2.75O15+z	Mo	0.25	Sr	2	Y	1	Ce	4	Cu	2.75											O	15+z		2	2011																												(Cu,Mo)1252																		K		55					55										20																																																																																						high-P oxygenation (500C,30 min, under 33 mol-% KClO3)					Homologous series of (Cu,Mo)Sr2(Y,Ce)sCu2O5+2s+z copper-oxide superconductors: Synthesis of members up to s = 6			Laboratory of Inorganic Chemistry, Department of Chemistry, School of Chemical Technology, Aalto University, P.O. Box 16100, FI-00076 AALTO, Finland	Solid State Commum., 151(2011)1400	Weibo Gao,Keiichiro Oishi,Hisayuki Suematsu,Hisao Yamauchi,Maarit Karppinen		
153150	SSC1511400	O-content not given	(Cu,Mo)Sr2(Y,Ce)6Cu2O17	Mo0.25Sr2Y1.002Ce4.998Cu2.75O17+z	Mo	0.25	Sr	2	Y	1.002	Ce	4.998	Cu	2.75											O	17+z		2	2011																												(Cu,Mo)1262																		K		55					55																																																																																																high-P oxygenation (500C,30 min, under 33 mol-% KClO3)					Homologous series of (Cu,Mo)Sr2(Y,Ce)sCu2O5+2s+z copper-oxide superconductors: Synthesis of members up to s = 6			Laboratory of Inorganic Chemistry, Department of Chemistry, School of Chemical Technology, Aalto University, P.O. Box 16100, FI-00076 AALTO, Finland	Solid State Commum., 151(2011)1400	Weibo Gao,Keiichiro Oishi,Hisayuki Suematsu,Hisao Yamauchi,Maarit Karppinen		
153151	APEX001081702	nominal compositions. impurity phases: FeAs, CaO, unknown	(Ca,Na)Fe2As2	Ca0.8Na0.2Fe2As2	Ca	0.8	Na	0.2	Fe	2	As	2																1	2008																										AB2C2		ThCr2Si2	I4/mmm		A	3.8931		11.771												K				14			14										4																																																																																				Ca,As,Fe,Na		mixture - heat(1100,2h, P=2 GPa, in BN crucible)					Superconductivity at 26K in (Ca1-xNax)Fe2As2			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Express, 1(2008)081702	Parasharam Maruti Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
153152	APEX001081702	nominal compositions. impurity phases: FeAs, CaO, unknown	(Ca,Na)Fe2As2	Ca0.6Na0.4Fe2As2	Ca	0.6	Na	0.4	Fe	2	As	2																1	2008																										AB2C2		ThCr2Si2	I4/mmm		A	3.8801		11.892												K		21	26	17.2			21										48																																																																																				Ca,As,Fe,Na		mixture - heat(1100,2h, P=2 GPa, in BN crucible)					Superconductivity at 26K in (Ca1-xNax)Fe2As2			Nanoelectronics Research Institute (NeRI), National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Central 2, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Appl.Phys.Express, 1(2008)081702	Parasharam Maruti Shirage,Kiichi Miyazawa,Hijiri Kito,Hiroshi Eisaki,Akira Iyo		
153153	APEX002063007	impurity phases: SrP, Sc2O3	Ni2P2(Sr4Sc2O6)	Ni2P2Sr4Sc2O6	Ni	2	P	2	Sr	4	Sc	2													O	6			2009																															A	4.044		15.23											Sc-42622	K	3.3		3.6				3.45										140										T					1.2			2																																																																		SrO,Sc2O3,Ni,P (or NiAs)		mixture - SIN(1100-1200C, 18-48h, in evacuated quaetz ampoule)					New Series of Nickel-Based Pnictide Oxide Superconductors (Ni2Pn2)(Sr4Sc2O6) (Pn = P, As)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Express, 2(2009)063007	Yutaka Matsumura,Hiraku Ogino,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
153154	APEX002063007	impurity phases: SrP, Sc2O3	Ni2As2(Sr4Sc2O6)	Ni2As2Sr4Sc2O6	Ni	2	As	2	Sr	4	Sc	2													O	6			2009																															A	4.078		15.41											Sc-42622	K	2.7		2.9				2.8										150										T					0.5			2																																																																		SrO,Sc2O3,Ni,P (or NiAs)		mixture - SIN(1100-1200C, 18-48h, in evacuated quaetz ampoule)					New Series of Nickel-Based Pnictide Oxide Superconductors (Ni2Pn2)(Sr4Sc2O6) (Pn = P, As)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Express, 2(2009)063007	Yutaka Matsumura,Hiraku Ogino,Shigeru Horii,Kohji Kishio,Jun-ichi Shimoyama		
153155	JPCM022125702	T<SDW> = 220 K estimated from R(T).	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.928		12.388												K					4																																																																																																Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153156	JPCM022125702	T<SDW> = 182 K estimated from R(T).	SrFe2(As,P)2	Sr1Fe2As1.8P0.2	Sr	1	Fe	2	As	1.8	P	0.2																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.927		12.292												K					4																																																																																																Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153157	JPCM022125702	T<SDW> = 134 K estimated from R(T).	SrFe2(As,P)2	Sr1Fe2As1.5P0.5	Sr	1	Fe	2	As	1.5	P	0.5																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.92		12.21												K					4																																																																																																Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153158	JPCM022125702		SrFe2(As,P)2	Sr1Fe2As1.4P0.6	Sr	1	Fe	2	As	1.4	P	0.6																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.909		12.122												K			25				25	MTC153159																																																																																													Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153159	JPCM022125702		SrFe2(As,P)2	Sr1Fe2As1.3P0.7	Sr	1	Fe	2	As	1.3	P	0.7																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.902		12.089												K			27				27	MTC153159																																																																																													Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153160	JPCM022125702		SrFe2(As,P)2	Sr1Fe2As1.2P0.8	Sr	1	Fe	2	As	1.2	P	0.8																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.898		12.043												K			27				27	MTC153159																																																																																													Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153161	JPCM022125702	T<SDW> = 145 K estimated from R(T).	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.889		11.701												K					4																																																																																																Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153162	JPCM022125702	R not to zero at 4 K.	CaFe2(As,P)2	Ca1Fe2As1.925P0.075	Ca	1	Fe	2	As	1.925	P	0.075																1	2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.898		11.691												K			13				13																																																																																														Ca(chunk) or Sr(chunk), Fe,As,P		mixture - pellet - (alumina in quartz) - heat(800C,24h) - cool to RT - reground - heat(850C,48h) cool to RT within 12h					Structural properties and superconductivity of SrFe2As2-xPx (0.0=< x =<1.0) and CaFe2As2-yPy (0.0 =< y =< 0.3)			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.Condens.Matter. 22(2010)125702	H L Shi,HX Yang,H F Tian,J B Lu,ZWWang,Y B Qin,Y J Song,J Q Li		
153163	JPCM020422201	T<SDW> = 165 K. Anisotropy (R) = 50.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2008																										AB2C2		ThCr2Si2	I4/mmm		A	3.872		11.73												K					4																																																																				uV/K	-5.47			MTP153163															m3/C	0.000000000553					MRH153163					self-flux method					Different resistivity response to spin-density wave and superconductivity at 20 K in Ca1-xNaxFe2As2			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.Condens.Matter. 20(2008)422201	GWu,H Chen,TWu,Y L Xie,Y J Yan,R H Liu,X FWang,J J Ying,X H Chen		
153164	JPCM020422201		(Ca,Na)Fe2As2	Ca0.5Na0.5Fe2As2	Ca	0.5	Na	0.5	Fe	2	As	2																1	2008																										AB2C2		ThCr2Si2	I4/mmm		A	3.829		11.862												K			20				20																																																																																																					Different resistivity response to spin-density wave and superconductivity at 20 K in Ca1-xNaxFe2As2			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.Condens.Matter. 20(2008)422201	GWu,H Chen,TWu,Y L Xie,Y J Yan,R H Liu,X FWang,J J Ying,X H Chen		
153165	JPCM023402201	impurity phase(0.8 % mass fraction): FeSe1.974 (a=3.7738, c=5.5235)	BaFe2Se3	Ba1Fe2Se3	Ba	1	Fe	2	Se	3																		3	2011								240																		AB2C3			Pnma		A	11.8903	5.4079	9.1375												K				11			11										1																																																																																				Fe(4N),Se(4N)		Bridgeman method. mixture(Fe2Se3) - press to rod - sealed in silica ampoule(Fe2Se3+Ba) - ANN(1150C,24h) - cool to 750C(6 C/h) - cool to RT(200C/h)					The synthesis, and crystal and magnetic structure of the iron selenide BaFe2Se3 with possible superconductivity at Tc = 11 K			Laboratory for Development and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.Condens.Matter. 23(2011)402201	A Krzton-Maziopa,E Pomjakushina,V Pomjakushin,D Sheptyakov,D Chernyshov,V Svitlyk,K Conder		
153166	EPL08717004	P-induced SC. Tc(max) = 35.4 at P=1.4 GPa.. T<SDW> = 139 (102) K at P = 0 (1.6) GPa obtained from the peak of (dR/dT).	BaFe2As2	Ba1Fe2As3	Ba	1	Fe	2	As	3																		3	2009																										AB2C2		ThCr2Si2	I4/mmm																	K			35.4		0		35.4	MTC153166																																																																																															self-flux method. heat(1100 C,27h) - cool (5C/min)					Pressure-induced superconductivity in BaFe2As2 single crystal			Materials Science Group, Indira Gandhi Centre for Atomic Research - Kalpakkam, 603102, Tamilnadu, India	EuroPhys.Lett., 87(2009)17004	Awadhesh Mani,Nilotpal Ghosh,S. Paulraj,A. Bharathi,C. S. Sundar		
153167	EPL08847008		NaxFeAs	Na0.86Fe1As1	Na	0.86	Fe	1	As	1																			2009																										ABC		Cu2Sb	P4/nmm																	K			26				26	MTC153167																																																																																													Na3As,Fe,As		solid state reaction. mixture(Na:Fe:As = 1.2:1:1)  - wrapped in Ta foil  - sealed in quartz tube - SIN(800C,20h)					"Superconductivity at 31K in the ""111""-type iron arsenide superconductor Na1-xFeAs induced by pressure"			Institute of Physics, Chinese Academy of Sciences - Beijing 100190, China	EuroPhys.Lett., 88(2009)47008	S. J. Zhang,X. C. Wang,Q. Q. Liu,Y. X. Lv,X. H. Yu,Z. J. Lin,Y. S. Zhao,L. Wang,Y. Ding,H. K. Mao,C. Q. Jin		
153168	EPL08927002		(Tb,Ca)FeAsO	Tb0.56Ca0.44Fe1As1O1	Tb	0.56	Ca	0.44	Fe	1	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9		8.423											ZrCuSiAs-type	K			15.6				15.6										50										T	resistivity, 0.95Rn, WHH	77							T/K	resistivity, 0.95Rn	7.1			MHC153168																																																			m3/C	0.00000000018				9						mixture - pellet - (sealed in quartz tube) - heat to (1150-1170 C) (120C/h) to hold(40h)					Superconductivity at 15.6K in calcium-doped Tb1-xCaxFeAsO: The structure requirement for achieving superconductivity in the hole-doped 1111 phase			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	EuroPhys.Lett.,89(2010)27002	Gang Mu,Bin Zeng,Peng Cheng,Xiyu Zhu,Fei Han,Bing Shen,Hai-Hu Wen		
153169	EPL08927002		(Pr,Ca)FeAsO	Pr0.6Ca0.4Fe1As1O1	Pr	0.6	Ca	0.4	Fe	1	As	1													O	1			2010																										ABCD		oxypnictide			A	3.9871		8.6275											ZrCuSiAs-type	K					1.8																																																																																							m3/C	-0.00000000104				9				TbAs,CaAs,Fe,Fe2O3							Superconductivity at 15.6K in calcium-doped Tb1-xCaxFeAsO: The structure requirement for achieving superconductivity in the hole-doped 1111 phase			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	EuroPhys.Lett.,89(2010)27002	Gang Mu,Bin Zeng,Peng Cheng,Xiyu Zhu,Fei Han,Bing Shen,Hai-Hu Wen		
153170	CC2009707	structural transformation(tetra- to orth-) at 115 K.	(Nd,Sr)FeAsO	Nd0.95Sr0.05Fe1As1O1	Nd	0.95	Sr	0.05	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9718		8.5733												K					1.8																																																																																																Fe,Fe2O3,SrO,FeAs,NdAs		mixture - pellet - heat(1100C,48h)					Structural and electronic response upon hole doping of rare-earth iron oxyarsenides Nd1-xSrxFeAsO (0 < x =< 0.2)			School of Chemistry, University of Edinburgh, Edinburgh, UK	Chem. Commun., (2009) 707	Karolina Kasperkiewicz,Jan-Willem G. Bos,Andrew N. Fitch,Kosmas Prassides,Serena Margadonna		
153171	CC2009707	structural transformation(tetra- to orth-) at 130 K.	(Nd,Sr)FeAsO	Nd0.9Sr0.1Fe1As1O1	Nd	0.9	Sr	0.1	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9733		8.5808												K					1.8																																																																																																Fe,Fe2O3,SrO,FeAs,NdAs		mixture - pellet - heat(1100C,48h)					Structural and electronic response upon hole doping of rare-earth iron oxyarsenides Nd1-xSrxFeAsO (0 < x =< 0.2)			School of Chemistry, University of Edinburgh, Edinburgh, UK	Chem. Commun., (2009) 707	Karolina Kasperkiewicz,Jan-Willem G. Bos,Andrew N. Fitch,Kosmas Prassides,Serena Margadonna		
153172	CC2009707	structural transformation(tetra- to orth-) at 130 K.	(Nd,Sr)FeAsO	Nd0.8Sr0.2Fe1As1O1	Nd	0.8	Sr	0.2	Fe	1	As	1													O	1			2009																										ABCD		oxypnictide			A	3.9777		8.6417												K				13.5			13.5										17																																																																																				Fe,Fe2O3,SrO,FeAs,NdAs		mixture - pellet - heat(1100C,48h)					Structural and electronic response upon hole doping of rare-earth iron oxyarsenides Nd1-xSrxFeAsO (0 < x =< 0.2)			School of Chemistry, University of Edinburgh, Edinburgh, UK	Chem. Commun., (2009) 707	Karolina Kasperkiewicz,Jan-Willem G. Bos,Andrew N. Fitch,Kosmas Prassides,Serena Margadonna		
153173	EPL09147008	residual-[gamma] = 9.8 mJ/mol.K2. (dC/gamma*Tc) = 0.27 . Two gap model: large one in DB, small one (2D/kTc) = 1.54.	Ba(Fe,Co)2As2	Ba1Fe1.92Co0.08As2	Ba	1	Fe	1.92	Co	0.08	As	2																3	2010																										AB2C2		ThCr2Si2																		K		5.8					5.8																																																3.49	14							mJ/mol.K2	14.9	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153174	EPL09147008	residual-[gamma] = 2.5 mJ/mol.K2. (dC/gamma*Tc) = 1.23 . Two gap model: large one in DB, small one (2D/kTc) = 1.60.	Ba(Fe,Co)2As2	Ba1Fe1.9Co0.1As2	Ba	1	Fe	1.9	Co	0.1	As	2																3	2010																										AB2C2		ThCr2Si2																		K		19.5					19.5																																																4.15	14							mJ/mol.K2	17.2	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153175	EPL09147008	residual-[gamma] = 2.1 mJ/mol.K2. (dC/gamma*Tc) = 1.52 . Two gap model: large one in DB, small one (2D/kTc) = 2.02.	Ba(Fe,Co)2As2	Ba1Fe1.89Co0.11As2	Ba	1	Fe	1.89	Co	0.11	As	2																3	2010																										AB2C2		ThCr2Si2																		K		21.5					21.5																																																4.77	14							mJ/mol.K2	19	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153176	EPL09147008	residual-[gamma] = 2.6 mJ/mol.K2. (dC/gamma*Tc) = 1.55 . Two gap model: large one in DB, small one (2D/kTc) = 1.85.	Ba(Fe,Co)2As2	Ba1Fe1.885Co0.115As2	Ba	1	Fe	1.885	Co	0.115	As	2																3	2010																										AB2C2		ThCr2Si2																		K		24.3					24.3	MTC153176																																															4.96	14							mJ/mol.K2	21.3	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153177	EPL09147008	residual-[gamma] = 2.9 mJ/mol.K2. (dC/gamma*Tc) = 1.25 . Two gap model: large one in DB, small one (2D/kTc) = 1.85.	Ba(Fe,Co)2As2	Ba1Fe1.85Co0.15As2	Ba	1	Fe	1.85	Co	0.15	As	2																3	2010																										AB2C2		ThCr2Si2																		K		22.9					22.9																																																4.18	14							mJ/mol.K2	22.1	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153178	EPL09147008	residual-[gamma] = 3.6 mJ/mol.K2. (dC/gamma*Tc) = 1.16 . Two gap model: large one in DB, small one (2D/kTc) = 1.81.	Ba(Fe,Co)2As2	Ba1Fe1.82Co0.18As2	Ba	1	Fe	1.82	Co	0.18	As	2																3	2010																										AB2C2		ThCr2Si2																		K		20.7					20.7																																																4.26	14							mJ/mol.K2	20	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153179	EPL09147008	residual-[gamma] = 7.9 mJ/mol.K2. (dC/gamma*Tc) = 0.48 . Two gap model: large one in DB, small one (2D/kTc) = 1.72	Ba(Fe,Co)2As2	Ba1Fe1.776Co0.224As2	Ba	1	Fe	1.776	Co	0.224	As	2																3	2010																										AB2C2		ThCr2Si2																		K		11.1					11.1																																																3.6	14							mJ/mol.K2	17	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153180	EPL09147008	residual-[gamma] = 10.4 mJ/mol.K2. (dC/gamma*Tc) = 0.22 . Two gap model: large one in DB, small one (2D/kTc) = 1.29.	Ba(Fe,Co)2As2	Ba1Fe1.76Co0.24As2	Ba	1	Fe	1.76	Co	0.24	As	2																3	2010																										AB2C2		ThCr2Si2																		K		5.1					5.1																																																3.26	14							mJ/mol.K2	14.6	SP-heat																																						self-flux method					Doping evolution of superconducting gaps and electronic densities of states in Ba(Fe1-xCox)2As2 iron pnictides			Karlsruher Institut fur Technologie, Institut fur Festkorperphysik - 76021 Karlsruhe, Germany, EU	EuroPhys.Lett.,91(2010)47008	F. Hardy,P. Burger,T. Wolf,R. A. Fisher,P. Schweiss,P. Adelmann,R. Heid,R. Fromknecht,R. Eder,D. Ernst,H. v. Lohneysen,C. Meingast		
153181	EPL09517011	Ni-content by EDS. T<CDW> = 41 K. anisotropy (Hc1) = 6.4 at 1.8 K. (dC/gamma*Tc) = 1.20. Hc() = 449 Oe. GL-parameter = 19.3(ab), =3.0 (c).	NixZrTe3	Ni0.05Zr1Te3	Ni	0.05	Zr	1	Te	3																		3	2011																															A	5.895	3.923	10.16											monoclinic, beta = 97.76	K		3.1	3.59				3.1											Oe	M-H curve		50	321					T	resistivity, 0.95Rn		1.2281	0.4862										MHC153181		A	from Hc2		260	100	A			780	12420			3	14				MSP153181			mJ/mol.K2	2.7	SP-heat	192.4	SP-heat																																				Chemical vapor transport (CVT) method. 720C(H) - 645C(L) for 10 days.					Raising Tc in charge density wave superconductor ZrTe3 by Ni intercalation			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory Upton, NY 11973, USA	EuroPhys.Lett.,95(2011)17011	Hechang Lei,Xiangde Zhu,C. Petrovic		
153182	EPL09157008		CeFeAs(O,F)	Ce1Fe1As1F0.16O0.84	Ce	1	Fe	1	As	1	F	0.16													O	0.84			2010																										ABCD		oxypnictide			A	3.989		8.631											ZrCuSiAs-type	K			41				41	TC153182																																																																																															solid state reaction					Pressure-induced competition between superconductivity and Kondo effect in CeFeAsO1-xFx (x = 0.16 and 0.3)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences Beijing 100190, China	EuroPhys.Lett.,91(2010)57008	Liling Sun,Xi Dai,Chao Zhang,Wei Yi,Genfu Chen,Nanlin Wang,Lirong Zheng,Zheng Jiang,Xiangjun Wei,Yuying Huang,Jie Yang,Zhian Ren,Wei Lu,Xiaoli Dong,Guangcan Che,Qi Wu,Hong Ding,Tiandou Hu,Zhongxian Zhao		
153183	EPL09157008		CeFeAs(O,F)	Ce1Fe1As1F0.3O0.7	Ce	1	Fe	1	As	1	F	0.3													O	0.7			2010																										ABCD		oxypnictide			A	3.985		8.598											ZrCuSiAs-type	K			46				46	TC153183																																																																																															high-P synthesis					Pressure-induced competition between superconductivity and Kondo effect in CeFeAsO1-xFx (x = 0.16 and 0.3)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences Beijing 100190, China	EuroPhys.Lett.,91(2010)57008	Liling Sun,Xi Dai,Chao Zhang,Wei Yi,Genfu Chen,Nanlin Wang,Lirong Zheng,Zheng Jiang,Xiangjun Wei,Yuying Huang,Jie Yang,Zhian Ren,Wei Lu,Xiaoli Dong,Guangcan Che,Qi Wu,Hong Ding,Tiandou Hu,Zhongxian Zhao		
153184	EPL09167002	RRR = 24. Tc = 16.8 K from SP. (dC/Tc) = 20.2 mJ/mol.K2. Anisotropy = 2.3 near Tc.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2010																										ABC		Cu2Sb	P4/nmm																	K		16.8	18.2				16.8																				T	resistivity, 0.5Rn		36.9	17.2					T/K	resistivity, 0.5Rn		2.99	1.39			A	from Hc2		440	20																mJ/mol.K2	35	SP-heat	300	SP-heat																																				Sn-flux method. (LiFeAs):Sn = 1:10. alumina crucible/quartz ampoule - heat to and hold at 850 C cool to 500C (3.5 C/h)					Single-crystal growth and superconducting properties of LiFeAs			CeNSCMR & Department of Physics and Astronomy, Seoul National University - Seoul 151-747, Republic of Korea	EuroPhys.Lett.,91(2010)67002	Bumsung Lee,Seunghyun Khim,Jung Soo Kim,G. R. Stewart,Kee Hoon Kim		
153185	EPL09257004	Anisotropy = 2.58	Fe(Te,Se)	Fe1.04Te0.6Se0.4	Fe	1.04	Te	0.6	Se	0.4																		3	2010																															A			6.014												K		14					14																				T	resistivity, 0.1Rn, WHH		91	35					T/K	resistivity, 0.1Rn		9.43	3.65	MHC153185														3.48	14							mJ/mol.K2	27.61	SP-heat																																						unidirectional solidification method. heat(970-1000C,for 12h) - slow cool to 400 C(2-4 C/h)					Superconductivity and vortex pinning in Fe1.04Te0.60Se0.40 single crystal			Max-Planck-Institut fur Festkorperforschung - Heisenbergstrasse 1, D-70569 Stuttgart, Germany, EU	EuroPhys.Lett.,92(2010)57004	Y. Liu,R. K. Kremer,C. T. Lin		
153186	EPL09427008	not SC. AFM due to Fe-site vacancy. vacancy content not given. STR transition at 540 K	KFe2Se2	K1Fe2Se2	K	1	Fe	2	Se	2																		3	2011								527																		AB2C2		ThCr2Si2																		K					5																																																																																																		Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153187	EPL09427008	AFM due to Fe-site vacancy. vacancy content not given. STR transition at 551 K. Resistivity shows maximum at 170 K.	KxFe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2011								540																		AB2C2		ThCr2Si2																		K	30.5		31.5				31																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153188	EPL09427008	AFM due to Fe-site vacancy. vacancy content not given. STR transition at 540 K. Resistivity shows maximum at 250 K.	RbxFe2Se2	Rb0.8Fe2Se2	Rb	0.8	Fe	2	Se	2																		3	2011								534																		AB2C2		ThCr2Si2																		K	31.5		32				31.75																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153189	EPL09427008	AFM due to Fe-site vacancy. vacancy content not given. STR transition at 525 K. Resistivity shows maximum at 270 K.	CsxFe2Se2	Cs0.8Fe2Se2	Cs	0.8	Fe	2	Se	2																		3	2011								504																		AB2C2		ThCr2Si2																		K	27.5		30.9				29.2																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153190	EPL09427008	AFM due to Fe-site vacancy. vacancy content not given. STR transition at 515 K. Resistivity shows maximum at 78 K.	(Tl,K)xFe2Se2	Tl0.4K0.3Fe2Se2	Tl	0.4	K	0.3	Fe	2	Se	2																3	2011								496																		AB2C2		ThCr2Si2																		K	24.8		27.7				26.25																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153191	EPL09427008	AFM due to Fe-site vacancy. vacancy content not given. STR transition at 512 K. Resistivity shows maximum at 180 K.	(Tl,Rb)xFe2Se2	Tl0.4Rb0.4Fe2Se2	Tl	0.4	Rb	0.4	Fe	2	Se	2																3	2011								500																		AB2C2		ThCr2Si2																		K	30.9		31.8				31.35																																																																																																Bridgeman method					Coexistence of superconductivity and antiferromagnetism in single crystals A0.8Fe2-ySe2 (A = K, Rb, Cs, Tl/K and Tl/Rb): Evidence from magnetization and resistivity			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China - Hefei, Anhui 230026, PRC	EuroPhys.Lett., 94(2011)27008	R. H. Liu,X. G. Luo,M. Zhang,A. F. Wang,J. J. Ying,X. F. Wang,Y. J. Yan,Z. J. Xiang,P. Cheng,G. J. Ye,Z. Y. Li,X. H. Chen		
153192	EPL09567007	chemical formula from EDX. SC apears for small range of Ru-content (around 25 %)	Eu(Fe,Ru)2As2	Eu1Fe1.5Ru0.5As2	Eu	1	Fe	1.5	Ru	0.5	As	2																3	2011					myu-B/f.u	7.9	17																			AB2C2		ThCr2Si2			A			11.79												K	20		23				21.5																																																																																																self flux method. (Eu:Fe:Ru:As = 0.5:0.73:0.27:1)  - melt(1473 K) - cool( 5 K/h) - ANN(973K,48h, in vac)					Anisotropic superconductivity in Eu(Fe0.75Ru0.25)2As2 ferromagnetic superconductor			Department of Physics, Zhejiang University - Hangzhou 310027, China	EuroPhys.Lett.,95(2011)67007	Wen-He Jiao,Qian Tao,Jin-Ke Bao,Yun-Lei Sun,Chun-Mu Feng,Zhu-An Xu1,I. Nowik,I. Felner,Guang-Han Cao		
153193	EPL09617007	not SC.	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2011								138																		ABCD		oxypnictide	P4/nmm		A	3.9391		8.5017											ZrCuSiAs-type	K					2																																																																																																Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153194	EPL09617007	not SC.	SmO(Fe,Co)As	Sm1Fe0.975Co0.025As1O1	Sm	1	Fe	0.975	Co	0.025	As	1													O	1		1	2011								85																		ABCD		oxypnictide	P4/nmm		A	3.9395		8.4965											ZrCuSiAs-type	K					2																																																																																																Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153195	EPL09617007	not SC.	SmO(Fe,Co)As	Sm1Fe0.95Co0.05As1O1	Sm	1	Fe	0.95	Co	0.05	As	1													O	1		1	2011								55																		ABCD		oxypnictide	P4/nmm		A	3.9397		8.4953											ZrCuSiAs-type	K					2																																																																																																Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153196	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.925Co0.075As1O1	Sm	1	Fe	0.925	Co	0.075	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9399		8.4864											ZrCuSiAs-type	K		11.6					11.6																																																																																														Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153197	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.9Co0.1As1O1	Sm	1	Fe	0.9	Co	0.1	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9402		8.4852											ZrCuSiAs-type	K		15					15																																																																																														Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153198	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.875Co0.125As1O1	Sm	1	Fe	0.875	Co	0.125	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9403		8.4637											ZrCuSiAs-type	K		12.8					12.8	TC153198																																																																																													Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153199	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.85Co0.15As1O1	Sm	1	Fe	0.85	Co	0.15	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9404		8.4586											ZrCuSiAs-type	K		10					10																																																																																														Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153200	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.825Co0.175As1O1	Sm	1	Fe	0.825	Co	0.175	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9406		8.4508											ZrCuSiAs-type	K		5.8					5.8																																																																																														Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153201	EPL09617007		SmO(Fe,Co)As	Sm1Fe0.8Co0.2As1O1	Sm	1	Fe	0.8	Co	0.2	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9411		8.4454											ZrCuSiAs-type	K					2																																																																																																Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153202	EPL09617007	not SC.	SmOCoAs	Sm1Co1As1O1	Sm	1	Co	1	As	1															O	1		1	2011							56	38																		ABCD		oxypnictide	P4/nmm		A	3.954		8.2533											ZrCuSiAs-type	K					2																																																																																																Sm,As,Fe,Co,Co2O3,Fe2O3		mixture - (sealed in Nb tube) - heat(1180C,45h, in flowing Ar)					Superconductivity and magnetic properties in SmFe1-xCoxAsO (x = 0 to 1)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 96(2011)17007	Yanpeng Qi,Lei Wang,Zhaoshun Gao,Dongliang Wang,Xianping Zhang,Chao Yao,Chunlei Wang,Chengduo Wang,Yanwei Ma		
153203	EPL08967007		SmO(Fe,Co)As	Sm1Fe0.9Co0.1As1O1	Sm	1	Fe	0.9	Co	0.1	As	1													O	1		1	2010																										ABCD		oxypnictide	P4/nmm		A	3.9391		8.497											ZrCuSiAs-type	K		15.6		15.6			15.6	TC153203																			T	resistivity, 0.9Rn, WHH	48							T/K	resistivity, 0.9Rn	4.5			HC153203																																																														solid state reaction. heat(1180C, 45h)					Superconductivity in SmFe1-xMxAsO (M= Co, Rh, Ir)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 89(2010)67007	Yan-Peng Qi,Lei Wang,Zhao-Shun Gao,Dong-Liang Wang,Xian-Ping Zhang,Zhi-Yu Zhang,Yan-Wei Ma		
153204	EPL08967007		SmO(Fe,Rh)As	Sm1Fe0.9Rh0.1As1O1	Sm	1	Fe	0.9	Rh	0.1	As	1													O	1		1	2010																										ABCD		oxypnictide	P4/nmm		A	3.9427		8.4501											ZrCuSiAs-type	K		9.6		9.6			9.6	TC153204																			T	resistivity, 0.9Rn, WHH	25.6							T/K	resistivity, 0.9Rn	3.6			HC153204																																																														solid state reaction. heat(1180C, 45h)					Superconductivity in SmFe1-xMxAsO (M= Co, Rh, Ir)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 89(2010)67007	Yan-Peng Qi,Lei Wang,Zhao-Shun Gao,Dong-Liang Wang,Xian-Ping Zhang,Zhi-Yu Zhang,Yan-Wei Ma		
153205	EPL08967007		SmO(Fe,Ir)As	Sm1Fe0.875Ir0.125As1O1	Sm	1	Fe	0.875	Ir	0.125	As	1													O	1		1	2010																										ABCD		oxypnictide	P4/nmm		A	3.9521		8.419											ZrCuSiAs-type	K		16.5		16.5			16.5	TC153205																			T	resistivity, 0.9Rn, WHH	51							T/K	resistivity, 0.9Rn	4.2			HC153205																																																														solid state reaction. heat(1180C, 45h)					Superconductivity in SmFe1-xMxAsO (M= Co, Rh, Ir)			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences P. O. Box 2703, Beijing 100190, China	EuroPhys.Lett., 89(2010)67007	Yan-Peng Qi,Lei Wang,Zhao-Shun Gao,Dong-Liang Wang,Xian-Ping Zhang,Zhi-Yu Zhang,Yan-Wei Ma		
153206	SSC1511767		Fe(Te,Se)	Fe1Te0.5Se0.5	Fe	1	Te	0.5	Se	0.5																			2011																												Fe-11	P4/nmm		A	3.7945		6.0311												K				13			13																																																																																																mixture - pellet - encapsulate in quartz(vac) - heat(750C) - cool to 300C - Q to RT					"Role of interstitial ""caged"" Fe in the superconductivity of FeTe1/2Se1/2"			Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. K. S. Krishnan Road, New Delhi-110012, India	Solid State Commun., 151(2011)1767	Anuj Kumar,Anand Pal,R.P. Tandon,V.P.S. Awana		
153207	SST024085017	impurity: Fe2P. RRR = 4.8(rab), =4.6(Rc). Anisotropy (R) = 1.1, (Hc2) = 1.25. Curie-T and moment = 18.95K and 8.59 myu-B/Eu for H//c.	(Eu,Na)Fe2(As,P)	Eu0.7Na0.3Fe2As1.4P0.6	Eu	0.7	Na	0.3	Fe	2	As	1.4	P	0.6														3	2011					myu-B/Eu	8.48	25.2																			AB2C2		ThCr2Si2	I4/mmm		A	3.871		11.924												K			25.2			3.3	25.2																				T	resistivity, 0.9Rn, WHH		36.6	29.2					T/K	resistivity, 0.9Rn		1.59	1.26			A	from Hc2		33.5	26.9														mJ/mol.K	300	mJ/mol.K2	503	SP-heat	376	SP-heat																																				Bridgeman nethod. Eu:Na:Fe2(As0.7P0.4)2.3 = 0.7:0.6:1,  melt(1650C) - cool slowly (melting point not known)					Interplay of the superconductivity and magnetism in Eu0.7Na0.3Fe2As1.4P0.6			Department of Physics, Sungkyunkwan University, Suwon 440-746, Republic of Korea	Supercond.Sci.Technol., 24(2011)085017	Y R Jang,J BHong,J BHong,M A Jung,Y Y Song,H J Oh,K J Lee,M H Jung,SKanematsu,K Imura,K Deguchi,NK Sato,Y S Kwon		
153208	SST024085020	new phase confirmed by XRD, STEM. single phase not obtained. Ti-concentration is tentative value,	(Ca8(Mg,Ti)6)O9.5Fe2As2	Ca8Mg1.5Ti4.5Fe2As2O9.5	Ca	8	Mg	1.5	Ti	4.5	Fe	2	As	2											O	9.5			2011																															A	3.86		30												K			40	40			40																																																																																														Fe,CaO,MgO,Ti,TiO2		nominal: Fe2As2(Ca8(Mg0.25Ti0.75)6O9.5). mixture - pellet - (sealed in quartz ampoule) - heat(1000-1200C,72-100h)					A new iron pnictide oxide (Fe2As2)(Ca5(Mg, Ti)4Oy) and a new phase in the Fe-As-Ca-Mg-Ti-O system			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Supercond.Sci.Technol., 24(2011)085020	Hiraku Ogino,Yasuaki Shimizu,Naoto Kawaguchi,Kohji Kishio,Jun-ichi Shimoyama,Tetsuya Tohei,Yuichi Ikuhara		
153209	SST024095006	not SC.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																1	2011								114																		ABCD		oxypnictide			A	3.879		8.597												K																																																																																																							solid state reaction. precursor(Fe2-xRhxAs) mixed with CaAs, CaF2. mixture - pellet - heat(900C,9h) - hold(900C,24h) - FC to RT					Superconductivity in Rh-doped CaFeAsF			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Supercond.Sci.Technol., 24(2011)095006	T-L Xia,T-S Zhao		
153210	SST024095006		Ca(Fe,Rh)AsF	Ca1Fe0.95Rh0.05As1F1	Ca	1	Fe	0.95	Rh	0.05	As	1	F	1														1	2011								51																		ABCD		oxypnictide			A	3.8852		8.5726												K		3.81					3.81																																																																																																solid state reaction. precursor(Fe2-xRhxAs) mixed with CaAs, CaF2. mixture - pellet - heat(900C,9h) - hold(900C,24h) - FC to RT					Superconductivity in Rh-doped CaFeAsF			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Supercond.Sci.Technol., 24(2011)095006	T-L Xia,T-S Zhao		
153211	SST024095006		Ca(Fe,Rh)AsF	Ca1Fe0.92Rh0.08As1F1	Ca	1	Fe	0.92	Rh	0.08	As	1	F	1														1	2011																										ABCD		oxypnictide			A	3.8923		8.5387												K	15	22.2	25				22.2	MTC153211																			T	resistivity, 0.9Rn, WHH	31							T/K	resistivity, 0.9Rn	3			MHC153211																																																														solid state reaction. precursor(Fe2-xRhxAs) mixed with CaAs, CaF2. mixture - pellet - heat(900C,9h) - hold(900C,24h) - FC to RT					Superconductivity in Rh-doped CaFeAsF			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Supercond.Sci.Technol., 24(2011)095006	T-L Xia,T-S Zhao		
153212	SST024095006		Ca(Fe,Rh)AsF	Ca1Fe0.85Rh0.15As1F1	Ca	1	Fe	0.85	Rh	0.15	As	1	F	1														1	2011																										ABCD		oxypnictide			A	3.9043		8.4951												K		18.4					18.4																																																																																																solid state reaction. precursor(Fe2-xRhxAs) mixed with CaAs, CaF2. mixture - pellet - heat(900C,9h) - hold(900C,24h) - FC to RT					Superconductivity in Rh-doped CaFeAsF			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Supercond.Sci.Technol., 24(2011)095006	T-L Xia,T-S Zhao		
153213	SST024095007	impuity phase: ThC2. lattice term in SP (beta) = 1.012 mJ/mol K4. (dC/gamma*Tc) = 1.1. GL parameter = 25.	Th3Ni5C5	Th3Ni5C5	Th	3	Ni	5	C	5																			2011																										A3B5C5			Cmcm		A	13.92	7.14	7.04											ortho-	K			5	5		0.2	5										85	Oe	M-H curve	80							T	resistivity, extrapolation	5.8												MHC153213		A	from Hc2	75			A		2070													mJ/mol.K2	38.84	SP-heat	293	SP-heat																																		Ni,Th,graphite		arc-melting. ANN(900C,2d) - Q to Liq.N2					Superconductivity in Th3Ni5C5			Escola de Engenharia de Lorena, Universidade de Sao Paulo, PO Box 116, Lorena, SP, Brazil	Supercond.Sci.Technol., 24(2011)095007	A J S Machado,T Grant,Z Fisk		
153214	CEM0700019	Tc measured by ac-induction.	Y2FeC4	Y2Fe1C4	Y	2	Fe	1	C	4																		1	1987																										AB2C4			Ibam		A	7.529	9.565	5.0406											ortho-	K		3.6					3.6																																																																																														R(chips),Fe(powder),graphite		arc-melting - ANN(900C,0d, in silica tube(vac))					Preparation and Crystal Structure of Superconducting Y2FeC4 and lsotypic Lanthanoid Iron Carbides			Anorganisch-Chemisches Institut, Universittat Munster, Corrensstrasse 36, D-4400 Munster, Federal Republic of Germany	J.solid State Chem., 70(1987)19	M. H. GERSS,W. JEITSCHKO,L. BOONK,J. NIENTIEDT,J. GROBE,E. MGRSEN,A. LESON		
153215	CEM0700019		Lu2FeC4	Lu2Fe1C4	Lu	2	Fe	1	C	4																		1	1987																										AB2C4			Ibam		A	7.494	9.249	4.9508											ortho-	K						1.8																																																																																															R(chips),Fe(powder),graphite		arc-melting - ANN(900C,0d, in silica tube(vac))					Preparation and Crystal Structure of Superconducting Y2FeC4 and lsotypic Lanthanoid Iron Carbides			Anorganisch-Chemisches Institut, Universittat Munster, Corrensstrasse 36, D-4400 Munster, Federal Republic of Germany	J.solid State Chem., 70(1987)19	M. H. GERSS,W. JEITSCHKO,L. BOONK,J. NIENTIEDT,J. GROBE,E. MGRSEN,A. LESON		
153216	CEM0700019		Tm2FeC4	Tm2Fe1C4	Tm	2	Fe	1	C	4																		1	1987									7.97																	AB2C4			Ibam		A	7.494	9.367	4.9792											ortho-	K						1.8																																																																																															R(chips),Fe(powder),graphite		arc-melting - ANN(900C,0d, in silica tube(vac))					Preparation and Crystal Structure of Superconducting Y2FeC4 and lsotypic Lanthanoid Iron Carbides			Anorganisch-Chemisches Institut, Universittat Munster, Corrensstrasse 36, D-4400 Munster, Federal Republic of Germany	J.solid State Chem., 70(1987)19	M. H. GERSS,W. JEITSCHKO,L. BOONK,J. NIENTIEDT,J. GROBE,E. MGRSEN,A. LESON		
153217	SST024105015	SP coeffic, (beta) = 0.657 mJ/mol.K2, (delta) = 0.001 mJ/mol.K6. e-ph = 0.58. (dC/gamma*Tc) = 2.68. gap = 0.9 meV assuming single gap model.  GL parameter = 150.	Rh7S15	Rh17S15	Rh	17	S	15																				1	2011																										A15B17			Pm3m																cubic	K		5.36					5.36											Oe	Hc2,GL	16							T	ac-SUS, extrapolation	20							T/K	ac-SUS	3.6			MHC153217		A	from Hc2	40			A		6000					4	14							mJ/mol.K2	108.41	SP-heat	456	SP-heat																																		Rh(4N),S(5N),Pd(3N),Se(5N)		mixture - heat to 1150C(8C/h) in alumina crucible - ANN(1050C,2d) - cool to 600C(8C/h) - cool to RT (30C/h)					Normal state and superconducting properties of Rh17S15 and Pd17Se15			Tata Institute of Fundamental Research, Mumbai, India	Supercond.Sci.Technol., 24(2011)105015	H RNaren,Arumugam Thamizhavel,Sushil Auluck,Rajendra Prasad,S Ramakrishnan		
153218	SST024105015	SP coeffic, (beta) = 4.9 mJ/mol.K2, (delta) = 0.11 uJ/mol.K6. e-ph = 0.54..	Pd17Se15	Pd17Se15	Pd	17	Se	15																				1	2011																										A15B17			Pm3m		A	10.604													cubic	K		2.2					2.2																				T	ac-SUS, extrapolation	3.3							T/K	ac-SUS	1.5			MHC153218		A	from Hc2	100																		mJ/mol.K2	22	SP-heat	233.3	SP-heat											mOhm.cm											0.0432												Rh(4N),S(5N),Pd(3N),Se(5N)		mixture - heat to 1150C(8C/h) in alumina crucible - ANN(1050C,2d) - cool to 600C(8C/h) - cool to RT (30C/h)					Normal state and superconducting properties of Rh17S15 and Pd17Se15			Tata Institute of Fundamental Research, Mumbai, India	Supercond.Sci.Technol., 24(2011)105015	H RNaren,Arumugam Thamizhavel,Sushil Auluck,Rajendra Prasad,S Ramakrishnan		
153219	PRB084132503	concentration: Se:Te = 1:2 by EDX. [penet] is London-P , measured by surface impedance.	Fe(Se,Te)	Fe1Se0.4Te0.6	Fe	1	Se	0.4	Te	0.6																			2011																										AB																				K				14			14																																									A	surface impedance	4700																																																					Bridgeman method					Anomalous temperature dependence of the superfluid density caused by a dirty-to-clean crossover in superconducting FeSe0.4Te0.6 single crystals			Department of Basic Science, the University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan	Phys.Rev.B, 84(2011)132503	Hideyuki Takahashi,Yoshinori Imai,Seiki Komiya,Ichiro Tsukada,Atsutaka Maeda		
153220	PRB084134525	P-induced SC. Pc=4.8 GPa. Tc(max) = 16.6 K at P=5.31 GPa. magnetic(para-AFM) and structural(tetra-ortho) transitions at T=134 K.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																		K	16.6				0		16.6	MTC153220																																																																																															self-flux method					Combined effects of pressure and Ru substitution on BaFe2As2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)134525	S. K. Kim,M. S. Torikachvili,E. Colombier,A. Thaler,S. L. Bud'ko,P. C. Canfield		
153221	PRB084134525	P-induced SC. Pc = 5.1 GPa. Tc(max) = 25.8 K at P = 4.94 GPa. magnetic(para-AFM) and structural(tetra-ortho) transitions at T = 98K.	Ba(Fe,Ru)2As2	Ba1Fe1.82Ru0.18As2	Ba	1	Fe	1.82	Ru	0.18	As	2																3	2011																										AB2C2		ThCr2Si2																		K	25.8				0		25.8	MTC153221																																																																																															self-flux method					Combined effects of pressure and Ru substitution on BaFe2As2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)134525	S. K. Kim,M. S. Torikachvili,E. Colombier,A. Thaler,S. L. Bud'ko,P. C. Canfield		
153222	PRB084134525	P-induced SC. Pc = 2.4 GPa. Tc(max) = 23.0 K at P = 3.58 GPa. magnetic(para-AFM) and structural(tetra-ortho) transitions at T = 71 K.	Ba(Fe,Ru)2As2	Ba1Fe1.68Ru0.32As2	Ba	1	Fe	1.68	Ru	0.32	As	2																3	2011																										AB2C2		ThCr2Si2																		K	23				0		23	MTC153222																																																																																															self-flux method					Combined effects of pressure and Ru substitution on BaFe2As2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)134525	S. K. Kim,M. S. Torikachvili,E. Colombier,A. Thaler,S. L. Bud'ko,P. C. Canfield		
153223	PRB084134525	magnetic(para-AFM) and structural(tetra-ortho) transitions at T = 45.2 K	Ba(Fe,Ru)2As2	Ba1Fe1.58Ru0.42As2	Ba	1	Fe	1.58	Ru	0.42	As	2																3	2011																										AB2C2		ThCr2Si2																		K	6.83						6.83	MTC153223																																																																																															self-flux method					Combined effects of pressure and Ru substitution on BaFe2As2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)134525	S. K. Kim,M. S. Torikachvili,E. Colombier,A. Thaler,S. L. Bud'ko,P. C. Canfield		
153224	PRB084134525		Ba(Fe,Ru)2As2	Ba1Fe1.44Ru0.56As2	Ba	1	Fe	1.44	Ru	0.56	As	2																3	2011																										AB2C2		ThCr2Si2																		K	15						15	MTC153224																																																																																															self-flux method					Combined effects of pressure and Ru substitution on BaFe2As2			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)134525	S. K. Kim,M. S. Torikachvili,E. Colombier,A. Thaler,S. L. Bud'ko,P. C. Canfield		
153225	PRB084134526		SmOFe(As,P)	Sm1Fe1As0.5P0.5O1	Sm	1	Fe	1	As	0.5	P	0.5													O	1		1	2011																										ABCD		oxypnictide			A	3.9066		8.3489											ZrCuSiAs-type	K				23.4			23.4																																																																																														SmAs,SmP,Fe2O3,Fe		mixture - pellet - alumina crucible in quartz ampoule. high pressure(P=3.5 GPa) synthesis.					Interplay of composition, structure, magnetism, and superconductivity in SmFeAs1-xPxO1-y			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 84(2011)134526	N. D. Zhigadlo,S. Katrych,M. Bendele,P. J. W. Moll,M. Tortello,S. Weyeneth,V. Yu. Pomjakushin,J. Kanter,R. Puzniak,Z. Bukowski,H. Keller,R. S. Gonnelli,R. Khasanov,J. Karpinski,B. Batlogg		
153226	PRB084134526		SmOFe(As,P)	Sm1Fe1As0.5P0.5O1	Sm	1	Fe	1	As	0.5	P	0.5													O	1		1	2011																										ABCD		oxypnictide			A	3.9042		8.3206											ZrCuSiAs-type	K					1.2																																																																																																SmAs,SmP,Fe2O3,Fe		mixture - pellet - alumina crucible in quartz ampoule - heat(660 C + 1060 C). ambient pressure synthesis					Interplay of composition, structure, magnetism, and superconductivity in SmFeAs1-xPxO1-y			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 84(2011)134526	N. D. Zhigadlo,S. Katrych,M. Bendele,P. J. W. Moll,M. Tortello,S. Weyeneth,V. Yu. Pomjakushin,J. Kanter,R. Puzniak,Z. Bukowski,H. Keller,R. S. Gonnelli,R. Khasanov,J. Karpinski,B. Batlogg		
153227	PRB084134526	Two gaps: small gap = 3.5 meV,  (2D/kTc) = 4. large gap in DB. These gap measured by Point contact Andreev reflection using Ag/SmFeAs0.5P0.5O junction	SmOFe(As,P)	Sm1Fe1As0.5P0.5O1	Sm	1	Fe	1	As	0.5	P	0.5													O	1		1	2011																										ABCD		oxypnictide																	ZrCuSiAs-type	K		20					20																																														meV	11.9	13	1																																													SmAs,SmP,Fe2O3,Fe		mixture - pellet - alumina crucible in quartz ampoule. high pressure(P=3.5 GPa) synthesis.					Interplay of composition, structure, magnetism, and superconductivity in SmFeAs1-xPxO1-y			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 84(2011)134526	N. D. Zhigadlo,S. Katrych,M. Bendele,P. J. W. Moll,M. Tortello,S. Weyeneth,V. Yu. Pomjakushin,J. Kanter,R. Puzniak,Z. Bukowski,H. Keller,R. S. Gonnelli,R. Khasanov,J. Karpinski,B. Batlogg		
153228	PRB084134526		SmOFe(As,P)	Sm1Fe1As0.5P0.5O0.85	Sm	1	Fe	1	As	0.5	P	0.5													O	0.85		3	2011									7.297																	ABCD		oxypnictide			A	3.9102		8.3367											ZrCuSiAs-type	K	17						17																																									A	from Hc1		2000																																																				NaCl/KCl flux method					Interplay of composition, structure, magnetism, and superconductivity in SmFeAs1-xPxO1-y			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 84(2011)134526	N. D. Zhigadlo,S. Katrych,M. Bendele,P. J. W. Moll,M. Tortello,S. Weyeneth,V. Yu. Pomjakushin,J. Kanter,R. Puzniak,Z. Bukowski,H. Keller,R. S. Gonnelli,R. Khasanov,J. Karpinski,B. Batlogg		
153229	PRB084134526		SmOFe(As,P)	Sm1Fe1As0.5P0.5O0.85	Sm	1	Fe	1	As	0.5	P	0.5													O	0.85		3	2011																										ABCD		oxypnictide																	ZrCuSiAs-type	K	21.7						21.7																													T/K	resistivity, R=0.9Rn		5.7	1.3	HC153229																																																														NaCl/KCl flux method					Interplay of composition, structure, magnetism, and superconductivity in SmFeAs1-xPxO1-y			Laboratory for Solid State Physics, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 84(2011)134526	N. D. Zhigadlo,S. Katrych,M. Bendele,P. J. W. Moll,M. Tortello,S. Weyeneth,V. Yu. Pomjakushin,J. Kanter,R. Puzniak,Z. Bukowski,H. Keller,R. S. Gonnelli,R. Khasanov,J. Karpinski,B. Batlogg		
153230	PRB084140507	SP heat measured for magnetic fields H//[001] and H/n [001]//c-axis	Ce2PdIn8	Ce2Pd1In8	Ce	2	Pd	1	In	8																		3	2011																										AB2C8		Ho2CoGa8																		K		0.68					0.68																				T			2.2	1.8										MHC153230																																																														self-flux method					Quantum criticality near the upper critical field of Ce2PdIn8			I. Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 84(2011)140507	Y. Tokiwa,P. Gegenwart,D. Gnida,D. Kaczorowski		
153231	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.85 mJ/mol.K2. lattice term (beta) = 0.96 mJ/mol.K4. (dC/gamma*Tc) = 1.0.	RbxFezSe2	Rb0.653Fe1.532Se2	Rb	0.653	Fe	1.532	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9285		14.6003												K			30.9			2.8	30.9																																																								mJ/mol.K2	10	SP-heat																																						self flux method. starting mixture(Rb+2.5FeSe) - heat to 1030C with soaking time (3h) - cooling (rate = 6 C/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153232	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.18 mJ/mol.K2. lattice term (beta) = 1.09 mJ/mol.K4. (dC/gamma*Tc) = 0.95.	RbxFezSe2	Rb0.796Fe1.596Se2	Rb	0.796	Fe	1.596	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9228		14.5909												K			32.4			1.5	32.4	MPH153232																			T	resistivity, 0.9Rn, WHH		63	25										MHC153232																						mJ/mol.K2	12	SP-heat																																											Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153233	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.46 mJ/mol.K2. lattice term (beta) = 1.04 mJ/mol.K4. (dC/gamma*Tc) = 0.96.	RbxFezSe2	Rb0.801Fe1.602Se2	Rb	0.801	Fe	1.602	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9304		14.605												K			32.4			1.6	32.4																																																								mJ/mol.K2	12	SP-heat																																						Bridgeman method. starting mixture(Rb+2.5FeSe) - heat to 1070C with soaking time (3h) - cooling (rate = 3 mm/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153234	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.33 mJ/mol.K2. lattice term (beta) = 0.90 mJ/mol.K4.	RbxFezSe2	Rb0.737Fe1.439Se2	Rb	0.737	Fe	1.439	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9117		14.6516												K					1.8																																																																																																		Bridgeman method. starting mixture(0.9Rb+2FeSe) - heat to 1070C with soaking time (3h) - cooling (rate = 3 mm/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153235	PRB084144520	[gamma] estimated from entropy constraint using SP-data.  lattice term (beta) = 0.95 mJ/mol.K4.	RbxFezSe2	Rb0.698Fe1.497Se2	Rb	0.698	Fe	1.497	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9379		14.5983												K					1.8																																																																																																		Bridgeman method. starting mixture(Rb+2FeSe+0.5Se) - heat to 1070C with soaking time (3h) - cooling (rate = 3 mm/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153236	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.3 mJ/mol.K2. lattice term (beta) = 1.36 mJ/mol.K4.	RbxFezSe2	Rb0.644Fe1.62Se2	Rb	0.644	Fe	1.62	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.9021		14.6484												K					1.8																																																																																																		Bridgeman method. starting mixture(Rb+2.5FeSe+0.5Se) - heat to 1070C with soaking time (5h) - cooling (rate = 3 mm/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153237	PRB084144520	[gamma] estimated from entropy constraint using SP-data. residual [gamma] = 0.34 mJ/mol.K2. lattice term (beta) = 0.94 mJ/mol.K4. (dC/gamma*Tc) = 2.2.	RbxFezSe2	Rb0.74Fe1.6Se2	Rb	0.74	Fe	1.6	Se	2																		3	2011																										AB2C2		ThCr2Si2			A	3.919		14.5515												K			32.4			1.5	32.4																																																								mJ/mol.K2	7.4	SP-heat																																						Bridgeman method. starting mixture(Rb+2.5FeSe) - heat to 1070C with soaking time (5h) - cooling (rate = 3 mm/h)					Anisotropic magnetism, superconductivity, and the phase diagram of Rb1-xFe2-ySe2			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, DE-86159, Augsburg, Germany	Phys.Rev.B, 84(2011)144520	V. Tsurkan,J. Deisenhofer,A. Gunther,H.-A. Krug von Nidda,S. Widmann,A. Loidl		
153238	PRL107177005	sample: mosaic of single crystals. Rb2Fe4Se5 = Rb0.796Fe1.596Se2	Rb2Fe4Se5	Rb2Fe4Se5	Rb	2	Fe	4	Se	5																		3	2011																										A2B4C5																				K				32			32																																																7.2																																																Bridgeman method					Magnetic Resonant Mode in the Low-Energy Spin-Excitation Spectrum of Superconducting Rb2Fe4Se5 Single Crystals			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, 70569 Stuttgart, Germany	Phys.Rev.Lett., 107(2011)177005	J. T. Park,G. Friemel,Yuan Li,J.-H. Kim,V. Tsurkan,J. Deisenhofer,H.-A. Krug von Nidda,A. Loidl,A. Ivanov,B. Keimer,D. S. Inosov		
153239	EPL08437002		Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																			2008																										AB		PbO	I4/nmm																	K		15.2					15.2	MTC153239																																																																																															mixture - pellet - heat(600C,20h) - SIN(650C,20h, in quartz tube)					Tellurium substitution effect on superconductivity of the alpha-phase iron selenide			Institute of Physics, Academia Sinica - Nankang, Taipei, Taiwan	EuroPhys Lett., 84(2008)37002	Kuo-Wei Yeh,Tzu-Wen Huang,Yi-lin Huang,Ta-Kun Chen,Fong-Chi Hsu,Phillip M. Wu,Yong-Chi Lee,Yan-Yi Chu,Chi-Lian Chen,Jiu-Yong Luo,Der-Chung Yan,Maw-Kuen Wu		
153240	PRB083184521	Rb-, and Fe-content by ICP. Semicon-Metal transition at 150 K. Anisotropy = 3.5.	RbxFeySe2	Rb0.76Fe1.62Se2	Rb	0.76	Fe	1.62	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K	28		31				29.5										42										T	resistivity, 0.9Rn, WHH		145	42					T/K	resistivity, R=0.9Rn		6.78	1.98	MHC153240																																																												Se(4N),Fe(3N),Rb(99.75%)		Bridgeman method. mixture - alumina crucible - sealed in silica ampoule(vac) - heat(1030C) - hold(3h) - cool to 730C(6 C/h) - FC to RT					Transport properties and anisotropy of Rb1-xFe2-ySe2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O.Box 603, Beijing 100190, China	Phys.Rev.B, 83(2011)184521	Chun-Hong Li,Bing Shen,Fei Han,Xiyu Zhu,Hai-Hu Wen		
153241	PRB083184521	Rb-, and Fe-content by ICP. RRR = 14. Semicon-Metal transition at 186 K. Anisotropy = 4.8.	RbxFeySe2	Rb0.8Fe1.68Se2	Rb	0.8	Fe	1.68	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K	31.5		32.5				32										80										T	resistivity, 0.9Rn, WHH		198	41					T/K	resistivity, R=0.9Rn		8.84	1.92	MHC153241																																																												Se(4N),Fe(3N),Rb(99.75%)		Bridgeman method. mixture - alumina crucible - sealed in silica ampoule(vac) - heat(1050C) - hold(8h) - cool to 700C(3.5 C/h) - FC to RT					Transport properties and anisotropy of Rb1-xFe2-ySe2 single crystals			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O.Box 603, Beijing 100190, China	Phys.Rev.B, 83(2011)184521	Chun-Hong Li,Bing Shen,Fei Han,Xiyu Zhu,Hai-Hu Wen		
153242	PRL106067001	[penet] measured by magnetic force microscopy(MFM). Two gaps obtained by fitting. large gap in DB. small one (2D/kTc) = 1.2	Ba(Fe,Co)2As	Ba1Fe1.902Co0.098As2	Ba	1	Fe	1.902	Co	0.098	As	2																	2011																										AB2C2		ThCr2Si2																		K		15.8					15.8																																									A	MFM		4000				4.4																																																self-flux method					Local Measurement of the Superfluid Density in the Pnictide Superconductor Ba(Fe1-xCox)2  across the Superconducting Dome			Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA, and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.Lett., 106(2011)067001	Lan Luan,Thomas M. Lippman,Clifford W. Hicks,Julie A. Bert,Ophir M. Auslaender,Jiun-Haw Chu,James G. Analytis,Ian R. Fisher,Kathryn A. Moler		
153243	PRL106067001	[penet] measured by magnetic force microscopy(MFM). Two gaps obtained by fitting. large gap in DB. small one (2D/kTc) = 1.4	Ba(Fe,Co)2As	Ba1Fe1.898Co0.102As2	Ba	1	Fe	1.898	Co	0.102	As	2																	2011																										AB2C2		ThCr2Si2																		K		18.6					18.6																																									A	MFM		3200				4.6																																																self-flux method					Local Measurement of the Superfluid Density in the Pnictide Superconductor Ba(Fe1-xCox)2  across the Superconducting Dome			Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA, and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.Lett., 106(2011)067001	Lan Luan,Thomas M. Lippman,Clifford W. Hicks,Julie A. Bert,Ophir M. Auslaender,Jiun-Haw Chu,James G. Analytis,Ian R. Fisher,Kathryn A. Moler		
153244	PRL106067001	[penet] measured by magnetic force microscopy(MFM). Two gaps obtained by fitting. large gap in DB. small one (2D/kTc) = 2.6	Ba(Fe,Co)2As	Ba1Fe1.86Co0.14As2	Ba	1	Fe	1.86	Co	0.14	As	2																	2011																										AB2C2		ThCr2Si2																		K		22.4					22.4																																									A	MFM		2510				6.6																																																self-flux method					Local Measurement of the Superfluid Density in the Pnictide Superconductor Ba(Fe1-xCox)2  across the Superconducting Dome			Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA, and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.Lett., 106(2011)067001	Lan Luan,Thomas M. Lippman,Clifford W. Hicks,Julie A. Bert,Ophir M. Auslaender,Jiun-Haw Chu,James G. Analytis,Ian R. Fisher,Kathryn A. Moler		
153245	PRL106067001	[penet] measured by magnetic force microscopy(MFM). Two gaps obtained by fitting. large gap in DB. small one (2D/kTc) = 1.2	Ba(Fe,Co)2As	Ba1Fe1.83Co0.17As2	Ba	1	Fe	1.83	Co	0.17	As	2																	2011																										AB2C2		ThCr2Si2																		K		19.6					19.6																																									A	MFM						3.8																																																self-flux method					Local Measurement of the Superfluid Density in the Pnictide Superconductor Ba(Fe1-xCox)2  across the Superconducting Dome			Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA, and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.Lett., 106(2011)067001	Lan Luan,Thomas M. Lippman,Clifford W. Hicks,Julie A. Bert,Ophir M. Auslaender,Jiun-Haw Chu,James G. Analytis,Ian R. Fisher,Kathryn A. Moler		
153246	PRL106067001	[penet] measured by magnetic force microscopy(MFM). Two gaps obtained by fitting. large gap in DB. small one (2D/kTc) = 1.2	Ba(Fe,Co)2As	Ba1Fe1.78Co0.22As2	Ba	1	Fe	1.78	Co	0.22	As	2																	2011																										AB2C2		ThCr2Si2																		K		13.5					13.5																																									A	MFM		2740				3.4																																																self-flux method					Local Measurement of the Superfluid Density in the Pnictide Superconductor Ba(Fe1-xCox)2  across the Superconducting Dome			Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA, and Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA	Phys.Rev.Lett., 106(2011)067001	Lan Luan,Thomas M. Lippman,Clifford W. Hicks,Julie A. Bert,Ophir M. Auslaender,Jiun-Haw Chu,James G. Analytis,Ian R. Fisher,Kathryn A. Moler		
153247	STAM009044206	Hall effect measured for H//ab and H//c.  Anisotropy (Hc2) = 2.0. Two gaps, large one in DB. small one (2D/kTc) = 1.1 measured by SP heat	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																			2008																										A2B3C5		Sc2Fe3Si5																		K		5.6					5.6																																																4.4	14																																				m3/C	-0.000000000334					MRH153247					floating zone method using image furnace. starting rod made from arc-melting.  ANN(1250C)					Two-gap superconductivity in R2Fe3Si5 (R= Lu, Sc) and Sc5Ir4Si10			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Sci.Technol.Adv.Mater., 9(2008)044206	Tsuyoshi Tamegai,Yasuyuki Nakajima,Tsuyoshi Nakagawa,Guoji Li,Hisatomo Harima		
153248	STAM009044206	Hc2 defined as Tc(SUS). Hc2//c>Hc2//ab. Anisotropy (Hc2) = 2.0. Two gaps, large one in DB. small one (2D/kTc) = 1.70  measured by SP heat	Sc2Fe3Si5	Sc2Fe3Si5	Sc	2	Fe	3	Si	5																			2008																										A2B3C5		Sc2Fe3Si5																		K		4.8					4.8																				T	SUS													MHC153248														3.53	14																																															floating zone method using image furnace. starting rod made from arc-melting.  ANN(1250C)					Two-gap superconductivity in R2Fe3Si5 (R= Lu, Sc) and Sc5Ir4Si10			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Sci.Technol.Adv.Mater., 9(2008)044206	Tsuyoshi Tamegai,Yasuyuki Nakajima,Tsuyoshi Nakagawa,Guoji Li,Hisatomo Harima		
153249	STAM009044206	Hc2 defined as Tc(SUS). Hc2//c>Hc2//ab. Two gaps, large one in DB. small one (2D/kTc) = 1.90  measured by SP heat	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																			2008																										A4B5C10		Sc5Co4Si10																		K		8.4					8.4																				T	SUS													MHC153249														4.1	14							mJ/mol.K2	30.5	SP-heat																																						floating zone method using image furnace. starting rod made from arc-melting.  ANN(1250C)					Two-gap superconductivity in R2Fe3Si5 (R= Lu, Sc) and Sc5Ir4Si10			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Sci.Technol.Adv.Mater., 9(2008)044206	Tsuyoshi Tamegai,Yasuyuki Nakajima,Tsuyoshi Nakagawa,Guoji Li,Hisatomo Harima		
153250	SST024045009	impurity phase: Fe7Se8(P63/mmc) 1.4%. Jc(2K) = 86 kA. residual gamma = 0.96 mJ/mol.K2. lattice term (beta) = 0.94 mJ/mol.K4 using Debye and Einstein model	Fe(Se,Te)	Fe1Se0.5Te0.5	Fe	1	Se	0.5	Te	0.5																		3	2011																										AB			P4/nmm			3.8025		6.03											Fe-11	K	13.6			13.9			13.9																				T	resistivity, 0.9Rn, WHH			37										MHC153250												meV	2.26	3.57	14							mJ/mol.K2	25	SP-heat																																				Fe(3N),Se(5N),Te(5N),Mn(4N)		self-flux method. crytals grown in double quartz ampoule. mixture - heat(650C,10h) - heat(700C,24h) - heat(1100C,72h) - cool to 400C(1 C/min) - ANN(100h) - Q to ice water					Improvement of superconducting properties of FeSe0.5Te0.5 single crystals by Mn substitution			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86159 Augsburg, Germany	Supercond.Sci.Technol., 24(2011)045009	AGunther,J Deisenhofer,Ch Kant,H-A Krug von Nidda,V Tsurkan,A Loidl		
153251	SST024045009	impurity phase: Fe7Se8(P63/mmc) 4.7%. Jc(2K) = 85 kA. residual gamma = 0.1.88 mJ/mol.K2. lattice term (beta) = 0.74 mJ/mol.K4 using Debye and Einstein model	(Fe,Mn)(Se,Te)	Fe0.98Mn0.02Se0.5Te0.5	Fe	0.98	Mn	0.02	Se	0.5	Te	0.5																3	2011																										AB			P4/nmm			3.8013		6.06											Fe-11	K	14.4			14.4			14.4																				T	resistivity, 0.9Rn, WHH			42										MHC153251												meV	2.7	4.47	14							mJ/mol.K2	30	SP-heat																																				Fe(3N),Se(5N),Te(5N),Mn(4N)		self-flux method. crytals grown in double quartz ampoule. mixture - heat(650C,10h) - heat(700C,24h) - heat(1100C,72h) - cool to 400C(1 C/min) - ANN(100h) - Q to ice water					Improvement of superconducting properties of FeSe0.5Te0.5 single crystals by Mn substitution			Experimental Physics 5, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86159 Augsburg, Germany	Supercond.Sci.Technol., 24(2011)045009	AGunther,J Deisenhofer,Ch Kant,H-A Krug von Nidda,V Tsurkan,A Loidl		
153252	JPS080114710	RRR = 5. hidden order temperature T<HO> = 17.5 K. RRR defined as R300/R2K for I//a.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K		0.95					0.95	MTC153252																																																																																															Czochralski method in tetra-arc furnace under Ar					Details of Sample Dependence and Transport Properties of URu2Si2			ASRC, JAEA, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 80(2011)114710	Tatsuma D. MATSUDA,Elena HASSINGER,Dai AOKI,Valentin TAUFOUR,Georg KNEBEL,Naoyuki TATEIWA,Etsuji YAMAMOTO,Yoshinori HAGA,Yoshichika ONUKI,Zachary FISK,Jacques FLOUQUET		
153253	JPS080114710	RRR = 46. hidden order temperature T<HO> = 17.6 K. RRR defined as R300/R2K for I//a.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K		1.42					1.42	MTC153252																																																																																															Czochralski method in tetra-arc furnace under Ar					Details of Sample Dependence and Transport Properties of URu2Si2			ASRC, JAEA, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 80(2011)114710	Tatsuma D. MATSUDA,Elena HASSINGER,Dai AOKI,Valentin TAUFOUR,Georg KNEBEL,Naoyuki TATEIWA,Etsuji YAMAMOTO,Yoshinori HAGA,Yoshichika ONUKI,Zachary FISK,Jacques FLOUQUET		
153254	JPS080114710	RRR = 270. hidden order temperature T<HO> = 17.7 K. RRR defined as R300/R2K for I//a.	URu2Si2	U1Ru2Si2	U	1	Ru	2	Si	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm	139																K		1.45					1.45	MTC153252																																																																																															Czochralski method in tetra-arc furnace under Ar					Details of Sample Dependence and Transport Properties of URu2Si2			ASRC, JAEA, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 80(2011)114710	Tatsuma D. MATSUDA,Elena HASSINGER,Dai AOKI,Valentin TAUFOUR,Georg KNEBEL,Naoyuki TATEIWA,Etsuji YAMAMOTO,Yoshinori HAGA,Yoshichika ONUKI,Zachary FISK,Jacques FLOUQUET		
153255	PRB080064506	lattice parameter shows for T=16 K, P=0.25 GPa. max-Tc(on) = 37 K at P=7 GPa. volume compressibility = 0.033	FeSe	Fe1Se1	Fe	1	Se	1																				1	2009																		GPa		30.7						AB		PbO	Cmma			5.2952	5.3066	5.4545											alpha-FeSe	K			13.4				13.4																																																																																																					Pressure evolution of the low-temperature crystal structure and bonding of the superconductor FeSe (Tc = 37 K)			School of Chemistry, University of Edinburgh, Edinburgh EH9 3JJ, United Kingdom	Phys.Rev.B, 80(2009)064506	S. Margadonna,Y. Takabayashi,Y. Ohishi,Y. Mizuguchi,Y. Takano,T. Kagayama,T. Nakagawa,M. Takata,K. Prassides		
153256	JPCM022222203	RRR = 6. Anisotropy = 2 at 0 K.	(Ca,Na)Fe2As2	Ca0.33Na0.66Fe2As2	Ca	0.33	Na	0.66	Fe	2	As	2																3	2010																										AB2C2		ThCr2Si2			A	3.841		12.2												K				33			33										30										T	resistivity, 0.5Rn, WHH		172	85					T/K	resistivity, 0.5Rn		7.53	3.73																							mJ/mol.K2	17.262																																					CaAs,Na3As,FeAs,Fe		self flux method					Superconductivity above 33 K in (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	J.Phys.: Condens.Matter, 22(2010)222203	K Zhao,Q Q Liu,X CWang,Z Deng,Y X Lv,J L Zhu,F Y Li,CQ Jin		
153257	PRB084174501	paramag ESR signal measured. R<ab> has the peak at 131 K	KFe2(Se,S)2	K0.74Fe1.67Se1.61S0.4	K	0.74	Fe	1.67	Se	1.61	S	0.4																3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.856		14.0344												K	31.2		32.8				32																																																																																																self flux method					Coexistence of superconductivity and magnetism in KxFe2-ySe2-zSz (z = 0,0.4)			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)174501	L. Li,Z. R. Yang,Z. T. Zhang,W. Tong,C. J. Zhang,S. Tan,Y. H. Zhang		
153258	NJP013033008	R<ab> has the peak at 275 K. Tc(max) = 30.6 K at P = 0.82 GPa	CsFe2Se2	Cs0.86Fe1.66Se2	Cs	0.86	Fe	1.66	Se	2																		3	2011																										AB2C2		ThCr2Si2																		K			30				30	MTC153258		K/GPa	1.3	1.64																																																																		mOhm.cm												117													self flux method					Pressure effect on superconductivity of AxFe2Se2 (A = K and Cs)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	New J.Phys., 13(2011)033008	J J Ying,X F Wang,X G Luo,Z Y Li,Y J Yan,M Zhang,A F Wang,P Cheng,G J Ye,Z J Xiang,R H Liu,X H Chen		
153259	NJP013033008	R<ab> has the peak at 245 K. Tc monotonicaly decreases with increasing P.	KFe2Se2	K0.85Fe2Se1.8	K	0.85	Fe	2	Se	1.8																		3	2011																										AB2C2		ThCr2Si2																		K			32.6				32.6	MTC153259		K/GPa		1.68																																																																		Ohm.cm												1.49													self flux method					Pressure effect on superconductivity of AxFe2Se2 (A = K and Cs)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	New J.Phys., 13(2011)033008	J J Ying,X F Wang,X G Luo,Z Y Li,Y J Yan,M Zhang,A F Wang,P Cheng,G J Ye,Z J Xiang,R H Liu,X H Chen		
153260	NJP013033008	R<ab> has the peak at 130 K. Tc(max) = 32.4 K at P = 0.48 GPa	KFe2Se2	K0.86Fe2Se1.82	K	0.86	Fe	2	Se	1.82																		3	2011																										AB2C2		ThCr2Si2																		K			31.1				31.1	MTC153260		K/GPa		1.68																																																																		mOhm.cm												59.6													self flux method					Pressure effect on superconductivity of AxFe2Se2 (A = K and Cs)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	New J.Phys., 13(2011)033008	J J Ying,X F Wang,X G Luo,Z Y Li,Y J Yan,M Zhang,A F Wang,P Cheng,G J Ye,Z J Xiang,R H Liu,X H Chen		
153261	PRB084174501	paramag ESR signal measured. R<ab> has the peak at 120 K	KFe2Se2	K0.79Fe1.64Se2	K	0.79	Fe	1.64	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9106		14.0663												K	28.4		31.2	30.4			30.4										92																																																																																						self flux method					Coexistence of superconductivity and magnetism in KxFe2-ySe2-zSz (z = 0,0.4)			High Magnetic Field Laboratory, University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)174501	L. Li,Z. R. Yang,Z. T. Zhang,W. Tong,C. J. Zhang,S. Tan,Y. H. Zhang		
153262	PRB084174502	London [penet] measured by tunnel diode resonator TDR. Two gaps obtained using gamma-model. large gap in DB. small one: gap = 1.1 meV, [gapene] = 1.8.	Fe(Te,Se)	Fe1Se0.42Te0.58	Fe	1	Se	0.42	Te	0.58																		3	2011																										AB		AlB2	P6/mmm																Fe-11	K		14.8					14.8																																									A	TDR	5600			meV	2.5	3.86	7																																															self flux method					Precision global measurements of London penetration depth in FeTe0.58Se0.42			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 84(2011)174502	K. Cho,H. Kim,M. A. Tanatar,J. Hu,B. Qian,Z. Q. Mao,R. Prozorov		
153263	SUP0180667	<10>B-isotope compounds. Tc defined as max-(dR/dT).	MgB2	B2Mg1	B	2	Mg	1																				1	2005																										AB2		AlB2	P6/mmm																hexagonal	K		40.5					40.5																																																																																														Sc,B or <10>B isotope(97.5%)		direct reaction					Tc as a Function of Electron Doping in Mg<10>B2 Using Sc for Mg Substitution			"Dipartimento di Fisica, Universita di Roma ""La Sapienza,"", P. le Aldo Moro 2, 00185 Rome, Italy"	J.Supercon.: Incorp.Novel Mag., 18(2005)667	M. Filippi,L. Simonelli,S. Agrestini,M. Fratini,V. Palmisano,G. Campi,C. Sanipoli,S. De Negri,M. Giovannini,A. Saccone,A. Bianconi		
153264	SUP0180667	<10>B-isotope compounds. Tc defined as max-(dR/dT). TCFIG shows  isotope effect.	(Mg,Sc)B2	B2Mg0.988Sc0.012	B	2	Mg	0.988	Sc	0.012																		1	2005																										AB2		AlB2	P6/mmm																hexagonal	K		41.4					41.4	MTC153264																																																																																													Sc,B or <10>B isotope(97.5%)		direct reaction					Tc as a Function of Electron Doping in Mg<10>B2 Using Sc for Mg Substitution			"Dipartimento di Fisica, Universita di Roma ""La Sapienza,"", P. le Aldo Moro 2, 00185 Rome, Italy"	J.Supercon.: Incorp.Novel Mag., 18(2005)667	M. Filippi,L. Simonelli,S. Agrestini,M. Fratini,V. Palmisano,G. Campi,C. Sanipoli,S. De Negri,M. Giovannini,A. Saccone,A. Bianconi		
153265	SSC1501483	interface SC. Interface composed of NaO2,Na2O2,Na2O,NaO3.  20 < Tc < 34 K, observed by ac-SUS.	Na/NaOx	Na1Ox	Na	1																			O	x			2010																																														K		28					28																																																																																														Na(4N)		tablets of Na(4N) in quartz ampoule - oxydize at RT - evacuated ampoule - ANN(473 K, 1-15 h) - rapid quench to 77 K (rate of 80K/s)					Superconductivity in the metallic oxidized sodium interface			Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka, Moscow District, 142432, Russia	Solid State Commun., 150(2010)1483	N.S. Sidorov,A.V. Palnichenko,S.S. Khasanov		
153266	PRB082214513	surface /n/ c-axisis. d = 45 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.85Sr0.15Cu1O4	La	1.85	Sr	0.15	Cu	1															O	4		5	2010																												T																		K	44					4	44																																									A	ac-resistivity	2400																												mOhm.cm					0.09																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153267	PRB082214513	surface /n/ c-axisis. d = 45 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.82Sr0.18Cu1O4	La	1.82	Sr	0.18	Cu	1															O	4		5	2010																												T																		K	41					6	41																																									A	ac-resistivity	2100																												mOhm.cm					0.054																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153268	PRB082214513	surface /n/ c-axisis. d = 45 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.79Sr0.21Cu1O4	La	1.79	Sr	0.21	Cu	1															O	4		5	2010																												T																		K	33					4	33																																									A	ac-resistivity	2200																												mOhm.cm					0.048																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153269	PRB082214513	surface /n/ c-axisis. d = 45 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.76Sr0.24Cu1O4	La	1.76	Sr	0.24	Cu	1															O	4		5	2010																												T																		K	19					3	19																																									A	ac-resistivity	3000																												mOhm.cm					0.037																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153270	PRB082214513	surface /n/ c-axisis. d = 45 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.73Sr0.27Cu1O4	La	1.73	Sr	0.27	Cu	1															O	4		5	2010																												T																		K	4					2	4																																									A	ac-resistivity	5800																												mOhm.cm					0.031																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153271	PRB082214513	surface /n/ c-axisis. d =905 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.73Sr0.27Cu1O4	La	1.73	Sr	0.27	Cu	1															O	4		5	2010																												T																		K	21					1.6	21																																									A	ac-resistivity	3800																												mOhm.cm					0.07																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153272	PRB082214513	surface /n/ c-axisis. d =905 nm. Tc measured by ac-resistivity (50 kHz). [penet] measured by superfluid density. [abres77] shows the valu at 50 K.	(La,Sr)2CuO4	La1.7Sr0.3Cu1O4	La	1.7	Sr	0.3	Cu	1															O	4		5	2010																												T																		K	9					0.2	9																																									A	ac-resistivity	7900																												mOhm.cm					0.056																				MBE method. substrates = (001)LaSrAlO4 (a = 3.754 A).					Anomalously sharp superconducting transitions in overdoped La2-xSrxCuO4 films			Department of Physics, The Ohio State University, Columbus, Ohio 43210, USA	Phys.Rev.B, 82(2010)214513	T. R. Lemberger,I. Hetel,A. Tsukada,M. Naito		
153273	PRB084174519	[resn] shows the value at T=0.5 K.	W(O,F)3	W1F0.45O2.55	W	1	F	0.45																	O	2.55		1	2011																										AB3			Pm3[-]m																cubic	K	0.373	0.38	0.4				0.38																				T	resistivity, 0.9Rn, WHH	0.53														A	from Hc2	250																																	mOhm.cm							4.66							cm3/C						RH153273					(WO3+excess PTFE powder) - (in evacuated quartz tube) - SIN(550C, 36h)					Superconductivity in WO2.6F0.4 synthesized by reaction of WO3 with teflon			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 84(2011)174519	D. Hirai,E. Climent-Pascual,R. J. Cava		
153274	PRB084174519	[resn] shows the value at T=0.5 K.	W(O,F)3	W1F0.41O2.59	W	1	F	0.41																	O	2.59		1	2011																										AB3			Pm3[-]m		A	3.8122													cubic	K	0.4	0.42	0.452				0.42																																		HC153274																																					mOhm.cm							22																		(WO3+excess PTFE powder) - (in evacuated quartz tube) - SIN(550C, 36h)					Superconductivity in WO2.6F0.4 synthesized by reaction of WO3 with teflon			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 84(2011)174519	D. Hirai,E. Climent-Pascual,R. J. Cava		
153275	PRB084174519	lattice term in SP (beta) = 0.197 mJ/mol.K4. [resn] shows the value at T=0.5 K.	W(O,F)3	W1F0.44O2.56	W	1	F	0.44																	O	2.56		1	2011																										AB3			Pm3[-]m		A	3.8143													cubic	K	0.39	0.41	0.43				0.41																																																								mJ/mol.K2	1.59	SP-heat	340	SP-heat											mOhm.cm							12.7																		(WO3+excess PTFE powder) - (in evacuated quartz tube) - SIN(550C, 36h)					Superconductivity in WO2.6F0.4 synthesized by reaction of WO3 with teflon			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 84(2011)174519	D. Hirai,E. Climent-Pascual,R. J. Cava		
153276	NJP011053008		LaO(Fe,Zn)As	La1Fe0.98Zn0.02As1O1	La	1	Fe	0.98	Zn	0.02	As	1													O	1		1	2009																										ABCD		oxypnictide	P4/nmm		A	4.036		8.7321											ZrCuSiAs	K					2																																																																				uV/K	-22			TP153276																								LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153277	NJP011053008		LaO(Fe,Zn)As	La1Fe0.95Zn0.05As1O1	La	1	Fe	0.95	Zn	0.05	As	1													O	1		1	2009																										ABCD		oxypnictide	P4/nmm		A	4.0364		8.7278											ZrCuSiAs	K					2																																																																				uV/K	-20.3			TP153277																								LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153278	NJP011053008		La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2009																										ABCD		oxypnictide	P4/nmm		A	4.0314		8.7134											ZrCuSiAs	K		23	26.8	22.2			23										100																																																								uV/K	-49.2			TP153278																								LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153279	NJP011053008		La(O,F)(Fe,Zn)As	La1Fe0.98Zn0.02As1F0.1O0.9	La	1	Fe	0.98	Zn	0.02	As	1	F	0.1											O	0.9		1	2009																										ABCD		oxypnictide	P4/nmm		A	4.0304		8.7174											ZrCuSiAs	K		25.5		24.1			25.5										100																																																																																				LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153280	NJP011053008		La(O,F)(Fe,Zn)As	La1Fe0.95Zn0.05As1F0.1O0.9	La	1	Fe	0.95	Zn	0.05	As	1	F	0.1											O	0.9		1	2009																										ABCD		oxypnictide	P4/nmm		A	4.0295		8.7192											ZrCuSiAs	K		25.4		24.1			25.4										100																																																																																				LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153281	NJP011053008		La(O,F)(Fe,Zn)As	La1Fe0.9Zn0.1As1F0.1O0.9	La	1	Fe	0.9	Zn	0.1	As	1	F	0.1											O	0.9			2009																										ABCD		oxypnictide	P4/nmm		A	4.0291		8.7191											ZrCuSiAs	K		19.9		16.3			19.9																																																																		uV/K	-50.4			TP153281																								LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153282	NJP011053008		La(O,F)(Fe,Zn)As	La1Fe0.85Zn0.15As1F0.1O0.9	La	1	Fe	0.85	Zn	0.15	As	1	F	0.1											O	0.9			2009																										ABCD		oxypnictide	P4/nmm		A	4.0292		8.7193											ZrCuSiAs	K		19.9		16.4			19.9																																																																																														LaAs,La2O3,FeAs,Fe2As,LaF3,ZnO		mixture - pellet - (sealed in quartz tube) - heat(1433K,40h)					Effect of Zn doping on magnetic order and superconductivity in LaFeAsO			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	New J.Phys., 11(2009)053008	Yuke Li,Xiao Lin,Qian Tao,Cao Wang,Tong Zhou,Linjun Li,Qingbo Wang,Mi He,Guanghan Cao,Zhu'an Xu		
153283	PHC4710618		Sm(O,F)(Fe,Zn)As	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9351		8.4861											ZrCuSiAs	K				52.5			52.5																																																																																														SmAs,Fe,ZnO,FeF3,Fe2O3		mixture - pellet - wrapped in Ta foil - (sealed in quartz tube) - ANN(1150C,36h, in Ar) - FC to RT					Suppression of superconductivity in Zn-doped SmFeAsO0.8F0.2 system			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)618	Y.J. Cui,Y.L. Chen,C.H. Cheng,Y. Yang,Y. Zhao		
153284	PHC4710618		Sm(O,F)(Fe,Zn)As	Sm1Fe0.95Zn0.05As1F0.2O0.8	Sm	1	Fe	0.95	Zn	0.05	As	1	F	0.2											O	0.8		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9399		8.4974											ZrCuSiAs	K				23.3			23.3																																																																																														SmAs,Fe,ZnO,FeF3,Fe2O3		mixture - pellet - wrapped in Ta foil - (sealed in quartz tube) - ANN(1150C,36h, in Ar) - FC to RT					Suppression of superconductivity in Zn-doped SmFeAsO0.8F0.2 system			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)618	Y.J. Cui,Y.L. Chen,C.H. Cheng,Y. Yang,Y. Zhao		
153285	PHC4710618		Sm(O,F)(Fe,Zn)As	Sm1Fe0.9Zn0.1As1F0.2O0.8	Sm	1	Fe	0.9	Zn	0.1	As	1	F	0.2											O	0.8		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.94		8.4979											ZrCuSiAs	K				18.2			18.2																																																																																														SmAs,Fe,ZnO,FeF3,Fe2O3		mixture - pellet - wrapped in Ta foil - (sealed in quartz tube) - ANN(1150C,36h, in Ar) - FC to RT					Suppression of superconductivity in Zn-doped SmFeAsO0.8F0.2 system			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)618	Y.J. Cui,Y.L. Chen,C.H. Cheng,Y. Yang,Y. Zhao		
153286	PHC4710618	R anomaly (SDW) at 140 K.	Sm(O,F)(Fe,Zn)As	Sm1Fe0.8Zn0.2As1F0.2O0.8	Sm	1	Fe	0.8	Zn	0.2	As	1	F	0.2											O	0.8		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9439		8.503											ZrCuSiAs	K					5																																																																																																SmAs,Fe,ZnO,FeF3,Fe2O3		mixture - pellet - wrapped in Ta foil - (sealed in quartz tube) - ANN(1150C,36h, in Ar) - FC to RT					Suppression of superconductivity in Zn-doped SmFeAsO0.8F0.2 system			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)618	Y.J. Cui,Y.L. Chen,C.H. Cheng,Y. Yang,Y. Zhao		
153287	PHC4710618	R anomaly (SDW) at 130 K. impurity phase: SmZnAsO	Sm(O,F)(Fe,Zn)As	Sm1Fe0.6Zn0.4As1F0.2O0.8	Sm	1	Fe	0.6	Zn	0.4	As	1	F	0.2											O	0.8		2	2011																										ABCD		oxypnictide	P4/nmm		A	3.9417		8.5006											ZrCuSiAs	K					5																																																																																																SmAs,Fe,ZnO,FeF3,Fe2O3		mixture - pellet - wrapped in Ta foil - (sealed in quartz tube) - ANN(1150C,36h, in Ar) - FC to RT					Suppression of superconductivity in Zn-doped SmFeAsO0.8F0.2 system			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)618	Y.J. Cui,Y.L. Chen,C.H. Cheng,Y. Yang,Y. Zhao		
153288	PHC4710711	(dC/gamma*Tc) = 2.11. GL parameter = 22. Thermodynamic Hc(0) = 117 mT.	Ca3Co4Sn13	Ca3Co4Sn13	Ca	3	Co	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.745													stannide	K		5.75		6			5.75											Oe	Hc(0), GL theory	110							T	resistivity, GL theory	3.72												MHC153288		A	from Hc2	130			A	Hc, GL theory	2370			meV	0.988	4.09	14							mJ/mol.K2	61.6	SP-heat	215	SP-heat																																				Sn-flux method					Superconducting state in the ternary stannide R3Co4Sn13 (R = Ca, La)			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	Physica C, 471(2011)711	N. Kase,H. Hayamizu,K. Inoue,J. Akimitsu		
153289	PHC4710711	(dC/gamma*Tc) = 1.75. GL parameter = 18. Thermodynamic Hc(0) = 39.8 mT.	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.755													stannide	K		2.7		2.7			2.7											Oe	Hc(0), GL theory	46							T	resistivity, GL theory	1.06												MHC153289		A	from Hc2	250			A	Hc, GL theory	3770			meV	0.436	3.61	14							mJ/mol.K2	33.2	SP-heat	286	SP-heat																																				Sn-flux method					Superconducting state in the ternary stannide R3Co4Sn13 (R = Ca, La)			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	Physica C, 471(2011)711	N. Kase,H. Hayamizu,K. Inoue,J. Akimitsu		
153290	PHC4710714	(dC/gamma*Tc) = 1.49.	W5SiB2	W5Si1B2	W	5	Si	1	B	2																		1	2011																										AB2C5		Mo5SiB2	I4/mcm		A	6.034		11.02												K				5.8			5.8																				T	resistivity, GL theory	0.52																										3.32	14																																															solid state reaction					Superconductivity in W5SiB2 with the T2-phase structure studied by the specific heat measurement and band structure calculation			Department of Physics and Mathematics, Aoyama Gakuin University, Fuchinobe 5-10-1, Chuo-ku, Sagamihara-shi, Kanagawa 229-8558, Japan	Physica C, 471(2011)714	M. Fukuma,K. Kawashima,M. Maruyama,J. Akimitsu		
153291	PRB084184529	a-Mn phase. RRR = 1.15. GL parameter = 50.	Re3W	Re3W1	Re	3	W	1																				1	2011																										AB3		a-Mn	I4[-]3m		A	9.5987													a-Mn type, noncentosymmetric	K			7.85	7.8		0.05	7.8											Oe	M-H curve	97							T	resistivity, 0.9Rn, WHH	12.5							T/K	resistivity, 0.9Rn	2.3			MHC153291		A	from Hc2	51.3			A	Hc1(0)	2570																												uOhm.cm											1.7														arc-melting. ANN(1500C, 5d, in Ar)					Structure and superconductivity of two different phases of Re3W			Physics Department, University of Warwick, Coventry, CV4 7AL, United Kingdom	Phys.Rev.B, 84(2011)184529	P. K. Biswas,M. R. Lees,A. D. Hillier,R. I. Smith,W. G. Marshall,D. McK. Paul		
153292	PRB084184529	hexagonal phase. RRR = 1.52. GL parameter = 30.	Re3W	Re3W1	Re	3	W	1																				1	2011																										AB3			P6<3>/mmc		A	2.77		4.5207											hexagonal, centrosymmetric	K			9.45	9.4		0.32	9.4											Oe	M-H curve	279							T	resistivity, 0.9Rn, WHH	14.7							T/K	resistivity, 0.9Rn	2.1			MHC153292		A	from Hc2	47.3			A	Hc1(0)	1410																												uOhm.cm											2.1														arc-melting. as-grown					Structure and superconductivity of two different phases of Re3W			Physics Department, University of Warwick, Coventry, CV4 7AL, United Kingdom	Phys.Rev.B, 84(2011)184529	P. K. Biswas,M. R. Lees,A. D. Hillier,R. I. Smith,W. G. Marshall,D. McK. Paul		
153293	PRB084184534	T<SDW> =  165 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8938		11.718												K					5																																																																																																							Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153294	PRB084184534	T<SDW> =  150 K.	(Ca,Na)Fe2As2	Ca0.9Na0.1Fe2As2	Ca	0.9	Na	0.1	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8825		11.83												K					5																																																																																																							Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153295	PRB084184534	T<SDW> =  135 K.	(Ca,Na)Fe2As2	Ca0.8Na0.2Fe2As2	Ca	0.8	Na	0.2	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8752		11.913												K					5																																																																																																							Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153296	PRB084184534	T<SDW> =  120 K.	(Ca,Na)Fe2As2	Ca0.7Na0.3Fe2As2	Ca	0.7	Na	0.3	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8664		11.981												K					5																																																																																																							Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153297	PRB084184534	RRR = 10	(Ca,Na)Fe2As2	Ca0.64Na0.36Fe2As2	Ca	0.64	Na	0.36	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.859		12.0155												K				17			17	MTC153297																																																																																																				Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153298	PRB084184534	RRR = 18	(Ca,Na)Fe2As2	Ca0.5Na0.5Fe2As2	Ca	0.5	Na	0.5	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.851		12.0874												K				22			22																																																																																																					Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153299	PRB084184534	RRR = 30. (dC/T) = 66 mJ/mol.K2	(Ca,Na)Fe2As2	Ca0.34Na0.66Fe2As2	Ca	0.34	Na	0.66	Fe	2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8423		12.212												K				34			34																				T	resistivity, 0.5Rn, WHH	106							T/K	resistivity, 0.5Rn	4.49																																																																						Doping dependence of the superconductivity of (Ca1-xNax)Fe2As2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 84(2011)184534	K. Zhao,Q. Q. Liu,X. C. Wang,Z. Deng,Y. X. Lv,J. L. Zhu,F. Y. Li,C. Q. Jin		
153300	PRB084214511	semiconductor-like. lattice term in C  (beta) = 1.357 mJ/mol.K4. SC maybe from beta-FeSe impurity phase.	BaFe2Se3	Ba1Fe1.9Se3	Ba	1	Fe	1.9	Se	3																		3	2011								255																		AB2C3			Pnma		A	11.94	5.444	9.174												K				11			11										0.15																																																	205	SP-heat											Ohm.cm												17													mixture - (put in carbon crucible) - (sealed in quartz tube) - ANN(1150C,24h) - slow cool to 750C(6C/h) - FC to RT					Anisotropy in BaFe2Se3 single crystals with double chains of FeSe tetrahedra			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 84(2011)214511	Hechang Lei,Hyejin Ryu,Anatoly I. Frenkel,C. Petrovic		
153301	PRB084214527	impurity: Ru.  SP = gamma*T + beta*T^3 + delta*T^5. beta = 0.1467 mJ/mol.K4, delta = 0.00465 mJ/mol.K6.	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	2011																										AB2C3					A	5.68		3.565											hexagonal	K	6.8		7.9	7.8			7.8										100										T	resistivity													MHC153301																						mJ/mol.K2	36.8	SP-heat	412	SP-heat																																				arc-melting					Anomalous properties in the normal and superconducting states of LaRu3Si2			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 84(2011)214527	Sheng Li,Bin Zeng,Xiangang Wan,Jian Tao,Fei Han,Huan Yang,Zhihe Wang,Hai-Hu Wen		
153302	PRB084220504	topological SC. Hall mobility(300K) = 1000 cm3/V.s. carrier(2K) = 2 E+18 / cm3.	YPtBi	Y1Pt1Bi1	Y	1	Pt	1	Bi	1																		3	2011																										ABC			F-43m	216	A	6.6522													cubic	K		0.77					0.77																				T	resistivity, 0.5Rn, extrapolation	1.5												MHC153302		A	from Hc2	150																																															cm3/C	0.339					MRH153302	n/cm3	20000000000000000000			single crystals prepared in excess molten Bi.					Superconductivity in the topological semimetal YPtBi			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 84(2011)220504	N. P. Butch,P. Syers,K. Kirshenbaum,A. P. Hope,J. Paglione		
153303	PRB084224506	ANN(270C, in air)	FeTe	Fe1Te1	Fe	1	Te	1																				3	2011								70																		AB		Fe-11																		K					2																																																																																																Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153304	PRB084224506	ANN(270C, in air)	Fe(Te,Se)	Fe1Te0.98Se0.02	Fe	1	Te	0.98	Se	0.02																		3	2011								62.6																		AB		Fe-11																		K					2																																																																																																Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153305	PRB084224506	ANN(270C, in air)	Fe(Te,Se)	Fe1Te0.95Se0.05	Fe	1	Te	0.95	Se	0.05																		3	2011								54																		AB		Fe-11																		K		6.7					6.7																																																																																														Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153306	PRB084224506	ANN(270C, in air)	Fe(Te,Se)	Fe1Te0.93Se0.07	Fe	1	Te	0.93	Se	0.07																		3	2011								46.8																		AB		Fe-11																		K	4	8.2					8.2	MTC153306																																																																																													Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153307	PRB084224506	ANN(270C, in air)	Fe(Te,Se)	Fe1Te0.9Se0.1	Fe	1	Te	0.9	Se	0.1																		3	2011								35.8																		AB		Fe-11			A	3.826		6.245												K	7.6	9.6					9.6										30																																																																																				Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153308	PRB084224506	ANN(270C, in air). not bulk SC for 0.3 =< x	Fe(Te,Se)	Fe1Te0.7Se0.3	Fe	1	Te	0.7	Se	0.3																		3	2011																										AB		Fe-11																		K		12.9					12.9																																																																																														Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153309	PRB084224506	ANN(270C, in air). not bulk SC for 0.3 =< x	Fe(Te,Se)	Fe1Te0.4Se0.4	Fe	1	Te	0.4	Se	0.4																		3	2011																										AB		Fe-11			A	3.804		6.069												K		14.4					14.4	MTC153306																																																																																													Fe(4N),Te(5N),Se(5N)		mixture - Bridgeman ampoule - (evacuated, sealed, heat(920C)) - slow cool to RT					Revised phase diagram for the FeTe1-xSex system with fewer excess Fe atoms			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 84(2011)220506	Chiheng Dong,Hangdong Wang,Zujuan Li,Jian Chen,H. Q. Yuan,Minghu Fang		
153310	PRB084224518	P4/mcc(80%), I4/mcm(10%), impurity phase: Nb3Ni2Si(2 vol%), NbNi3(5%), Nb(3%). (dC/gamma*Tc) = 0.93. lattice term in SP (beta) = 0.1615 mJ/mol.K4. e-ph = 0.60	Nb4NiSi	Nb4Ni1Si1	Nb	4	Ni	1	Si	1																		1	2011																										ABC4		CuAl2	P4/mcc	124	A	6.1948		5.039												K	7.3		7.7	7.7			7.7										42	Oe	M-H curve, GL theory	109							T	resistivity, 0.9Rn, GL theory	1.89																																		mJ/mol.K2	14.1	SP-heat	415	SP-heat											mOhm.cm											0.113												Nb(3N),Ni(4N),Co(4N),Fe(4N),Si(4N)		arc-melting - ANN(1373-1573, 96-144 h, in vac)					Superconductivity in Nb4MSi (M=Ni, Co, and Fe) with a quasi-two-dimensional Nb network			Materials and Structures Laboratory, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)224518	Gihun Ryu,Sung Wng Kim,Satoru Matsuishi,Hitoshi Kawaji,Hideo Hosono		
153311	PRB084224518	P4/mcc(84%), I4/mcm(13%), impurity phase: Nb(2%).	Nb4CoSi	Nb4Co1Si1	Nb	4	Co	1	Si	1																		1	2011																										ABC4		CuAl2	P4/mcc	124	A	6.1637		5.0563												K			6				6										7																																																																																				Nb(3N),Ni(4N),Co(4N),Fe(4N),Si(4N)		arc-melting - ANN(1373-1573, 96-144 h, in vac)					Superconductivity in Nb4MSi (M=Ni, Co, and Fe) with a quasi-two-dimensional Nb network			Materials and Structures Laboratory, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)224518	Gihun Ryu,Sung Wng Kim,Satoru Matsuishi,Hitoshi Kawaji,Hideo Hosono		
153312	PRB084224518	P4/mcc(84%), I4/mcm(2%), impurity phase: Nb(8%).	Nb4FeSi	Nb4Fe1Si1	Nb	4	Fe	1	Si	1																		1	2011																										ABC4		CuAl2	P4/mcc	124	A	6.1819		5.0364												K			6.8				6.8										78																																																																																				Nb(3N),Ni(4N),Co(4N),Fe(4N),Si(4N)		arc-melting - ANN(1373-1573, 96-144 h, in vac)					Superconductivity in Nb4MSi (M=Ni, Co, and Fe) with a quasi-two-dimensional Nb network			Materials and Structures Laboratory, Tokyo Institute of Technology, Mail Box S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)224518	Gihun Ryu,Sung Wng Kim,Satoru Matsuishi,Hitoshi Kawaji,Hideo Hosono		
153313	PHC4710600	not SC.  T<SDW> = 210 K.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9263		12.377												K					1.6																																																																																																		solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153314	PHC4710600	R not to zero at 1.6 K..  T<SDW> = 143 K.	Sr(Fe,Pt)2As2	Sr1Fe1.9Pt0.1As2	Sr	1	Fe	1.9	Pt	0.1	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9355		12.351												K		1.6	17.3				1.6																																																																																																solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153315	PHC4710600	T<SDW> = 94 K	Sr(Fe,Pt)2As2	Sr1Fe1.85Pt0.15As2	Sr	1	Fe	1.85	Pt	0.15	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9416		12.333												K	11.7						11.7																																																																																																solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153316	PHC4710600		Sr(Fe,Pt)2As2	Sr1Fe1.8Pt0.2As2	Sr	1	Fe	1.8	Pt	0.2	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.947		12.322												K	15.8						15.8																																																																																																solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153317	PHC4710600		Sr(Fe,Pt)2As2	Sr1Fe1.7Pt0.3As2	Sr	1	Fe	1.7	Pt	0.3	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9529		12.305												K	12.6						12.6																																																																																																solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153318	PHC4710600	R not to zero at 1.6 K.	Sr(Fe,Pt)2As2	Sr1Fe1.6Pt0.4As2	Sr	1	Fe	1.6	Pt	0.4	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9663		12.259												K			7				7																																																																																																solid state reaction. mixture (press in Ta capsule) - (sealed in quartz tube) - heat(1000C,48h)					Superconductivity of the platinum doped 122 iron arsenide SrFe2-xPtxAs2			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)600	S.B. Zhang,Y.F. Guo,J.J. Li,X.X. Wang,K. Yamaura,E. Takayama-Muromachi		
153319	PHC4710704	lattice parameter a = 4.3548 - 0.1743x for Ba1-xKxBiO3. Tc depends on x (see TCFIG)	(Ba,K)BiO3	Ba0.6K0.4O3	Ba	0.6	K	0.4																	O	3		1	2011																										ABC3		BKBO	Pm3[-]m		A	4.2856														K				30.6			30.6	TC153319																																																																																															molten salts method using KOH					Synthesis and superconductivity properties of Ba1-xKxBiO3			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)704	Y.L. Chen,Y.J. Cui,Y. Yang,Y. Zhang,Y. Zhao		
153320	PHC4710704	lattice parameter a = 4.3548 - 0.1743x for Ba1-xKxBiO3. Tc depends on x (see TCFIG)	(Ba,K)BiO3	Ba0.4K0.6O3	Ba	0.4	K	0.6																	O	3		1	2011																										ABC3		BKBO	Pm3[-]m		A	4.25														K				7			7																																																																																																molten salts method using KOH					Synthesis and superconductivity properties of Ba1-xKxBiO3			Key Laboratory of Advanced Technology of Materials (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	Physica C, 471(2011)704	Y.L. Chen,Y.J. Cui,Y. Yang,Y. Zhang,Y. Zhao		
153321	PHC4710717	films with various carrier concentration obtained by annealing at temperatures for 1h or 4h.	Zn-doped In2O3	Zn0.025In2O3	Zn	0.025	In	2																	O	3			2011																																														K		2.68					2.68	TC153321																																																																																															Zn-doped In2O3 films (350 nm thickness) were prepared by DC magnetron sputtering using (In2O3)1-x(ZnO)x target					Superconducting characteristics and microstructure of polycrystalline Zn-doped In2O3 films			Department of Physics, Kyushu University, Fukuoka 812-8581, Japan	Physica C, 471(2011)717	B. Shinozaki,S. Takada,N. Kokubo,K. Makise,K. Mitsuishi,K. Yamada,K. Yano,H. Nakamura		
153322	JPS079095002	Tc is almost independent of x	Sr(Fe,Pt)2As2	Sr1Fe1.75Pt0.25As2	Sr	1	Fe	1.75	Pt	0.25	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm																	K	15.6		17				16.3	MTC153322									57																																																																																						mixture - (wrapped in Ta foil) - heat(900C,in evacuated quartz tube)					Superconductivity in SrFe2As2 with Pt Doping			Department of Physics, Faculty of Science, Okayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 79(2010)095002	Yoshihiro NISHIKUBO,Satomi KAKIYA,Masataka DANURA,Kazutaka KUDO,Minoru NOHARA		
153323	PRB079214516	small amount of Ru1-xFexAs impurity. T<SDW> = 190 K.	Sr(Fe,Ru)2As2	Sr1Fe1.9Ru0.1As2	Sr	1	Fe	1.9	Ru	0.1	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9321		12.3446											Fe-122	K					2																																																																																																SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153324	PRB079214516	small amount of Ru1-xFexAs impurity. T<SDW> = 165 K.	Sr(Fe,Ru)2As2	Sr1Fe1.8Ru0.2As2	Sr	1	Fe	1.8	Ru	0.2	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9439		12.2905											Fe-122	K					2																																																																																																SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153325	PRB079214516	small amount of Ru1-xFexAs impurity. T<SDW> = 140 K.	Sr(Fe,Ru)2As2	Sr1Fe1.7Ru0.3As2	Sr	1	Fe	1.7	Ru	0.3	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9515		12.2551											Fe-122	K					2																																																																																																SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153326	PRB079214516	small amount of Ru1-xFexAs impurity. T<SDW> = 140 K.. not bulk SC(from SP)	Sr(Fe,Ru)2As2	Sr1Fe1.6Ru0.4As2	Sr	1	Fe	1.6	Ru	0.4	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9669		12.1772											Fe-122	K					2																																																																																																SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153327	PRB079214516	small amount of Ru1-xFexAs impurity.  not bulk SC(from SP)	Sr(Fe,Ru)2As2	Sr1Fe1.5Ru0.5As2	Sr	1	Fe	1.5	Ru	0.5	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9772		12.13											Fe-122	K	7						7																																																																																														SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153328	PRB079214516	small amount of Ru1-xFexAs impurity. ( dC/Tc) = 13.4 mJ/mol.K2	Sr(Fe,Ru)2As2	Sr1Fe1.4Ru0.6As2	Sr	1	Fe	1.4	Ru	0.6	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9918		12.0635											Fe-122	K	17.5	19.8	19.3				19.8																																																								mJ/mol.K2	6.2	SP-heat	232	SP-heat																																		SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153329	PRB079214516	small amount of Ru1-xFexAs impurity. ( dC/Tc) = 11.6 mJ/mol.K2	Sr(Fe,Ru)2As2	Sr1Fe1.3Ru0.7As2	Sr	1	Fe	1.3	Ru	0.7	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.0051		12.0087											Fe-122	K	16	20.1	19.3				20.1																																																								mJ/mol.K2	7.3	SP-heat	229	SP-heat																																		SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153330	PRB079214516	small amount of Ru1-xFexAs impurity. ( dC/Tc) = 13.6 mJ/mol.K2	Sr(Fe,Ru)2As2	Sr1Fe1.2Ru0.8As2	Sr	1	Fe	1.2	Ru	0.8	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.011		11.9835											Fe-122	K	18	17.2	17.6				17.2																																																								mJ/mol.K2	6.7	SP-heat	231	SP-heat																																		SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153331	PRB079214516		Sr(Fe,Ru)2As2	Sr1Fe1Ru1As2	Sr	1	Fe	1	Ru	1	As	2																1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.0444		11.8097											Fe-122	K					2																																																										mJ/mol.K2	6.9	SP-heat	243	SP-heat																																		SrAs,Fe2As,As,Ru		(mixture in glassy-carbon) - (Ta-crucible in evacuated quartz tube) - heat(900C, 24h-7d)					Substitution-induced superconductivity in SrFe2-xRuxAs2 (0=< x =<2)			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 79(2009)214516	W. Schnelle,A. Leithe-Jasper,R. Gumeniuk,U. Burkhardt,D. Kasinathan,H. Rosner		
153332	MAT0901.4582	RRR = 17. lattice term in SP (beta) = 0.49 mJ/mol.K4. SDW not observed.	BaRu2As2	Ba1Ru2As2	Ba	1	Ru	2	As	2																		1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.1525		12.2504												K					1.8																																																										mJ/mol.K2	4.9	SP-heat	271	SP-heat											uOhm.cm							9.7				170												Ba(5N),Sr(4N),Ru(6N),As(5N)		mixture - Al2O3 crucible - (heat(610,10h + 850C,20h) - (grind pelletize) - (wrapped in Ta) - heat(1000C)					Magnetic, Thermal, and Transport Properties of Layered Arsenides BaRu2As2 and SrRu2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	cond-mat/0901.4582	R. Nath,Yogesh Singh,D. C. Johnston		
153333	MAT0901.4582	RRR = 5. lattice term in SP (beta) = 0.49 mJ/mol.K4. SDW not observed.	SrRu2As2	Ba1Ru2As2	Ba	1	Ru	2	As	2																		1	2009																										AB2C2		ThCr2Si2	I4/mmm		A	4.1713		11.1545												K					1.8																																																										mJ/mol.K2	4.1	SP-heat	271	SP-heat											mOhm.cm							2.3				10.7												Ba(5N),Sr(4N),Ru(6N),As(5N)		mixture - Al2O3 crucible - (heat(610,10h + 850C,20h) - (grind pelletize) - (wrapped in Ta) - heat(1000C)					Magnetic, Thermal, and Transport Properties of Layered Arsenides BaRu2As2 and SrRu2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	cond-mat/0901.4582	R. Nath,Yogesh Singh,D. C. Johnston		
153334	APL096012507		BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.961		13.017											Fe-122	K					2																																																																																																BaAs,Fe1-xIrxAs		mixture - pellet - SIN(1100C,20h, in quartz tube)					Microstructure and superconductivity of Ir-doped BaFe2As2 superconductor			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Appl.Phys.Lett., 96(2010)012507	X. L. Wang,H. Y. Shi,X. W. Yan,Y. C. Yuan,Z.-Y. Lu,X. Q. Wang,T.-S. Zhao		
153335	APL096012507		Ba(Fe,Ir)2As2	Ba1Fe1.8Ir0.2As2	Ba	1	Fe	1.8	Ir	0.2	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.975		12.997											Fe-122	K		27.4	28.2	27.3		1.1	27.4																				T	resistivity, 0.5Rn, WHH	65.4							T/K	resistivity, 0.5Rn	3.46			MHC153335																																																												BaAs,Fe1-xIrxAs		mixture - pellet - SIN(1100C,20h, in quartz tube)					Microstructure and superconductivity of Ir-doped BaFe2As2 superconductor			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Appl.Phys.Lett., 96(2010)012507	X. L. Wang,H. Y. Shi,X. W. Yan,Y. C. Yuan,Z.-Y. Lu,X. Q. Wang,T.-S. Zhao		
153336	APL096012507		Ba(Fe,Ir)2As2	Ba1Fe1.7Ir0.3As2	Ba	1	Fe	1.7	Ir	0.3	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.989		12.985											Fe-122	K		27	28.2	27			27																																																																																														BaAs,Fe1-xIrxAs		mixture - pellet - SIN(1100C,20h, in quartz tube)					Microstructure and superconductivity of Ir-doped BaFe2As2 superconductor			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Appl.Phys.Lett., 96(2010)012507	X. L. Wang,H. Y. Shi,X. W. Yan,Y. C. Yuan,Z.-Y. Lu,X. Q. Wang,T.-S. Zhao		
153337	APL096012507		Ba(Fe,Ir)2As2	Ba1Fe1.6Ir0.4As2	Ba	1	Fe	1.6	Ir	0.4	As	2																1	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.987		12.981											Fe-122	K		24.5	26.4	24.7			24.5																																																																																														BaAs,Fe1-xIrxAs		mixture - pellet - SIN(1100C,20h, in quartz tube)					Microstructure and superconductivity of Ir-doped BaFe2As2 superconductor			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	Appl.Phys.Lett., 96(2010)012507	X. L. Wang,H. Y. Shi,X. W. Yan,Y. C. Yuan,Z.-Y. Lu,X. Q. Wang,T.-S. Zhao		
153338	JPCM022072204	H//c-axis. (dC/Tc) = 20 mJ/mol.K2 in SP measurements.	Ba(Fe,Pt)2As2	Ba1Fe1.9Pt0.1As2	Ba	1	Fe	1.9	Pt	0.1	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm		A	3.9772		12.988											Fe-122	K	21.5		23	23		1.5	23										100	mT	M-H curve						200	1.8	T	resistivity, 0.5Rn, WHH			45					T/K	resistivity, 0.5Rn			2.8	MHC153338																																																												Fe(5N),Pt(4N),As(4N),Ba(3N)		FeAs self-flux method. (FeAs:PtAs:Ba = 4-2x:2x:1 , in alumina crucible) - heat(1150C) - slow cool - Q to RT					Superconductivity at 23 K in Pt doped BaFe2As2 single crystals			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, MD 20742, USA	J.Phys.:Condens.Matter, 22(2010)072204	S R Saha,T Drye,K Kirshenbaum,N P Butch,P Y Zavalij,Johnpierre Paglione		
153339	PRB078020503	not SC. T<SDW>=139.9K, wherestructural transformation to Fmmm ( a=5.6146, b=5.5742, c=12.9453). Debye-T calculate from (beta)=2.0 mJ/mol.K4 (3.1<T<14K)	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		1	2008																										AB2C2		ThCr2Si2	I4/mmm		A	3.9625		13.0168												K					3																																																										mJ/mol.K2	16	SP-heat	134	SP-heat											mOhm.cm							0.2																		mixture - heat to 1123K at 50K/h - keep(1123K,10h) - cool to RT - ANN(1173K,25h) - pellet -ANN(973K)					Spin-density-wave anomaly at 140 K in the ternary iron arsenide BaFe2As2			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13, Haus D, Munchen 81377, Germany	Phys.Rev.B, 78(2008)020503	Marianne Rotter,Marcus Tegel,Dirk Johrendt,Inga Schellenberg,Wilfried Hermes,Rainer Pottgen		
153340	JPCM015S2175	Figure[HALLFIG] shows effective RH (=RH0 + anomalous term). Tc and [gamma] from num= 111252 data. Curie-T and moment for H//c.  For H//a, Curie-T = -14 K.	Ce2CoIn8	Ce2Co1In8	Ce	2	Co	1	In	8																		3	2003					myu-B/mol	2.3	3																			AB2C8		Ho2CoGa8																		K		0.4					0.4																																																								J/K2.Mol-C	0.5	SP-heat																											m3/C	-0.00000000042					MRH153340					In-flux method					Transport properties of the heavy-fermion superconductor Ce2CoIn8			Department of Electrical and Computer Engineering, Nagoya Institute of Technology, Nagoya 466-8555, Japan	J.Phys.:Condens.Matter,15(2003)S2175	Genfu Chen,Shigeo Ohara,Masato Hedo,Yoshiya Uwatoko,Isao Sakamoto		
153341	JPS081023702		Sr(Si,Ni)2	Sr1Si1.9Ni0.1	Sr	1	Si	1.9	Ni	0.1																		1	2012																										AB2		AlB2			A	4.0521		4.7341												K		2.3					2.3																																																																																																arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153342	JPS081023702		Sr(Si,Ni)2	Sr1Si1.8Ni0.2	Sr	1	Si	1.8	Ni	0.2																		1	2012																										AB2		AlB2			A	4.0595		4.7057												K		2.6					2.6										119																																														mJ/mol.K2	3.37	SP-heat													mOhm.cm											0.637														arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153343	JPS081023702	(dC/gamma*Tc) = 0.8. (dC/Tc) = 3.2 mJ/mol.K2	Sr(Si,Ni)2	Sr1Si1.7Ni0.3	Sr	1	Si	1.7	Ni	0.3																		1	2012																										AB2		AlB2			A	4.0611		4.6932												K		2.8					2.8										106										T	resistivity, 0.5Rn, WHH	1.58												MHC153343		A	from Hc2	144																		mJ/mol.K2	3.78	SP-heat																																						arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153344	JPS081023702	R shows zero but SC-volume < 0.1 %. not bulk SC.	Sr(Si,Ni)2	Sr1Si1.6Ni0.4	Sr	1	Si	1.6	Ni	0.4																		1	2012																										AB2		AlB2			A	4.063		4.6648												K					1.72												0.1																																														mJ/mol.K2	3.06	SP-heat																																						arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153345	JPS081023702	R shows SC-like drop.	Sr(Si,Ni)2	Sr1Si1.5Ni0.5	Sr	1	Si	1.5	Ni	0.5																		1	2012																										AB2		AlB2			A	4.0683		4.6602												K					1.72																																																										mJ/mol.K2	2.84	SP-heat																																						arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153346	JPS081023702	R shows SC-like drop.	Sr(Si,Ni)2	Sr1Si1.4Ni0.6	Sr	1	Si	1.4	Ni	0.6																		1	2012																										AB2		AlB2			A	4.0722		4.6455												K					1.72																																																										mJ/mol.K2	3.14	SP-heat													mOhm.cm											0.4														arc-melting. mixture - pellet - arc melting					Superconductivity in Pseudo-Binary Silicide SrNixSi2 x with AlB2-Type Structure			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)023702	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153347	JPS081023703	Al-doped V2Al20. Einstein-T = 23.7 K using Einstein model(delta=0.280). (dC/gamma*Tc) = 1.35	AlxV2Al20	Al20.3V2	Al	20.3	V	2																					2012																										AB2C20			Fd3[-]m		A	14.5157													cubic, Einstein solid	K	1.5	1.49					1.49																																																2.74	14							mJ/mol.K2	33	SP-heat																																						arc-melting - ANN(650C,80h, in evacuated quartz ampoule)					Superconductivity in the Einstein Solid AxV2Al20 (A = Al and Ga)			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)023703	Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Zenji HIROI		
153348	JPS081023703	Ga-doped V2Al20. Einstein-T = 8.1 K using Einstein model(delta=0.050). (dC/gamma*Tc) = 1.40	GaxV2Al20	Ga0.2V2Al20	Ga	0.2	V	2	Al	20																			2012																										AB2C20			Fd3[-]m		A	14.5171													cubic, Einstein solid	K	1.68	1.66					1.66																																																2.9	14				MSP153348			mJ/mol.K2	35	SP-heat																																						arc-melting - ANN(650C,80h, in evacuated quartz ampoule)					Superconductivity in the Einstein Solid AxV2Al20 (A = Al and Ga)			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)023703	Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Zenji HIROI		
153349	JPS081023703	Y-doped V2Al20. SP-heat analyzed by Debye and Einstein model. (dC/gamma*Tc) = 1.41	YV2Al20	Y1V2Al20	Y	1	V	2	Al	20																			2012																										AB2C20			Fd3[-]m		A	14.5386													cubic, Einstein solid	K	0.7	0.69					0.69																																																								mJ/mol.K2	27	SP-heat	420	SP-heat																																				arc-melting - ANN(650C,80h, in evacuated quartz ampoule)					Superconductivity in the Einstein Solid AxV2Al20 (A = Al and Ga)			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)023703	Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Zenji HIROI		
153350	JPS081023703	not SC. La-doped V2Al20. SP-heat analyzed by Debye and Einstein model.	LaV2Al20	La1V2Al20	La	1	V	2	Al	20																			2012																										AB2C20			Fd3[-]m		A	14.6222													cubic, Einstein solid	K					0.4																																																										mJ/mol.K2	20	SP-heat	430	SP-heat																																				arc-melting - ANN(650C,80h, in evacuated quartz ampoule)					Superconductivity in the Einstein Solid AxV2Al20 (A = Al and Ga)			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)023703	Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Zenji HIROI		
153358	PRB085064511	composition: Sr0.797Eu0.203(Fe0.888Co0.112)2As2 by WDS. Hc2 measured by ac(16Hz) freqency shift.	(Sr,Eu)(Fe,Co)2As2	Sr0.8Eu0.2Fe1.78Co0.22As2	Sr	0.8	Eu	0.2	Fe	1.78	Co	0.22	As	2														3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	18.3			18			18																				T	rf-freqency shift, two band model		31.6	30.4										MHC153358		A	from Hc2		33	32																																																								self flux method. ANN(500C,24h)					Upper critical fields and two-band superconductivity in Sr1−xEux(Fe0.89Co0.11)2As2 (x = 0.20 and 0.46)			Ames Laboratory, US Department of Energy and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)064511	Rongwei Hu,Eun Deok Mun,M. M. Altarawneh,C. H. Mielke,V. S. Zapf,S. L. Bud’ko,P. C. Canfield		
153359	PRB085064511	composition: Sr0.537Eu0.463(Fe0.885Co0.115)2As2 by WDS. Hc2 measured by ac(16Hz) freqency shift.	(Sr,Eu)(Fe,Co)2As2	Sr0.54Eu0.46Fe1.78Co0.22As2	Sr	0.54	Eu	0.46	Fe	1.78	Co	0.22	As	2														3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	16.8			16.2			16.2																				T	rf-freqency shift, two band model		22.4	20.4										MHC153359		A	from Hc2		40	37																																																								self flux method. ANN(500C,24h)					Upper critical fields and two-band superconductivity in Sr1−xEux(Fe0.89Co0.11)2As2 (x = 0.20 and 0.46)			Ames Laboratory, US Department of Energy and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)064511	Rongwei Hu,Eun Deok Mun,M. M. Altarawneh,C. H. Mielke,V. S. Zapf,S. L. Bud’ko,P. C. Canfield		
153360	PRB085064513	R(T) has the hump at 154 K. Hc2//ab good fittong by WHH with alpha=5.6, ramda(so) = 0.3. Hc2//c increases linearly with decreasing T (Hc2//c(0) = 66 T).	(Tl,Rb)Fe2As2	Tl0.58Rb0.42Fe1.72Se2	Tl	0.58	Rb	0.42	Fe	1.72	Se	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		33.5				0.5	33.5																				T	resistivity, 0.9Rn, WHH		273	45					T/K	resistivity, 0.9Rn		12	2	MHC153360																																																														Bridgeman method					Upper critical field and thermally activated flux flow in single-crystalline Tl0.58Rb0.42Fe1.72Se2			Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 85(2012)064513	L. Jiao,Y. Kohama,J. L. Zhang,H. D. Wang,B. Maiorov,F. F. Balakirev,Y. Chen,L. N. Wang,T. Shang,M. H. Fang,H. Q. Yuan		
153361	PRB085064517	coexistence of SC and AFM measured by zero-field muon-SR and NED.	FeSe0.98	Fe1Se0.98	Fe	1	Se	0.98																					2012																												PbO																	Fe-11	K				8			8	MTC153361																																																																																															solid state reaction. Slow cool from 400C to RT					Coexistence of superconductivity and magnetism in FeSe1-x under pressure				Phys.Rev.B, 85(2012)064517	M. Bendele,A. Ichsanow,Yu. Pashkevich,L. Keller,Th. Strassle,A. Gusev,E. Pomjakushina,K. Conder,R. Khasanov,H. Keller		
153362	PRL104087003	magnetic states measured by zero-field muon-SR .	FeSe0.94	Fe1Se0.94	Fe	1	Se	0.94																					2010																												PbO																	Fe-11	K				8.79			8.79	MTC153362																																																																																															solid state reaction. Mixture - press - sealed in double walled quartz ampoule - heat to 700C - ANN(400C)					Pressure Induced Static Magnetic Order in Superconducting FeSe1-x			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 104(2010)087003	M. Bendele,A. Amato,K. Conder,M. Elender,H. Keller,H.-H. Klauss,H. Luetkens,E. Pomjakushina,A. Raselli,R. Khasanov		
153363	SSC1520644	O-content determined from linear dependence of lattice constant a on x, which confirmed by Rietveld analysis of NED	(LaOx)FeAs	La1Fe1As1O0.89	La	1	Fe	1	As	1															O	0.89		1	2012																										ABCD		oxypnictide																	Fe-1111	K		27.8					27.8	TC153363																																																																																															high-P synthesis using cubic anvil. (1050-1150 C, 2h, P=2.0-5.5 Gpa, in BN crucible)					Relationship between crystal structure and superconductivity in iron-based superconductors			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Solid State Commun., 152(2012)644	C.H. Lee,K. Kihou,A. Iyo,H. Kito,P.M. Shirage,H. Eisaki		
153364	SSC1520644	O-content determined from linear dependence of lattice constant a on x, which confirmed by Rietveld analysis of NED	(PrOx)FeAs	Pr1Fe1As1O0.896	Pr	1	Fe	1	As	1															O	0.896		1	2012																										ABCD		oxypnictide																	Fe-1111	K		44.4					44.4	TC153364																																																																																															high-P synthesis using cubic anvil. (1050-1150 C, 2h, P=2.0-5.5 Gpa, in BN crucible)					Relationship between crystal structure and superconductivity in iron-based superconductors			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Solid State Commun., 152(2012)644	C.H. Lee,K. Kihou,A. Iyo,H. Kito,P.M. Shirage,H. Eisaki		
153365	SSC1520644	O-content determined from linear dependence of lattice constant a on x, which confirmed by Rietveld analysis of NED	(NdOx)FeAs	Nd1Fe1As1O0.9	Nd	1	Fe	1	As	1															O	0.9		1	2012																										ABCD		oxypnictide																	Fe-1111	K		46.9					46.9	TC153365																																																																																															high-P synthesis using cubic anvil. (1050-1150 C, 2h, P=2.0-5.5 Gpa, in BN crucible)					Relationship between crystal structure and superconductivity in iron-based superconductors			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Solid State Commun., 152(2012)644	C.H. Lee,K. Kihou,A. Iyo,H. Kito,P.M. Shirage,H. Eisaki		
153366	SSC1520644	O-content determined from linear dependence of lattice constant a on x, which confirmed by Rietveld analysis of NED	(TbOx)FeAs	Tb1Fe1As1O0.8	Tb	1	Fe	1	As	1															O	0.8		1	2012																										ABCD		oxypnictide																	Fe-1111	K		32					32	TC153366																																																																																															high-P synthesis using cubic anvil. (1050-1150 C, 2h, P=2.0-5.5 Gpa, in BN crucible)					Relationship between crystal structure and superconductivity in iron-based superconductors			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Solid State Commun., 152(2012)644	C.H. Lee,K. Kihou,A. Iyo,H. Kito,P.M. Shirage,H. Eisaki		
153420	JPS081124707	impurity phase:Al45V7. [gamma] from curve fitting of Cel(T). (dC/gamma*Tc) = 1.20	GaxV2Al20	Ga0.05V2Al20	Ga	0.05	V	2	Al	20																		1	2012																										AB2C20					A	14.5118														K		1.53					1.53																																																2.6	14							mJ/mol.K2	34	SP-heat																																				Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153421	JPS081124707	impurity phase:Al45V7. [gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 7.19 E-4cm3/mol. Hc2=Hc2(0)[1-a(T/Tc)^b] , (a=1,b=1.9). (dC/gamma*Tc) = 1.35	GaxV2Al20	Ga0.1V2Al20	Ga	0.1	V	2	Al	20																		1	2012																										AB2C20					A	14.5121														K		1.53					1.53																				T	SP, empirical eq.	0.065												MHC153421		A	from Hc2	700										2.9	14							mJ/mol.K2	35	SP-heat																																				Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153422	JPS081124707	(dC/gamma*Tc) = 1.35	GaxV2Al20	Ga0.15V2Al20	Ga	0.15	V	2	Al	20																		1	2012																										AB2C20					A	14.5144														K		1.53					1.53																																																2.8	14																																													Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153423	JPS081124707	[gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 6.00 E-4cm3/mol. Hc2=Hc2(0)[1-a(T/Tc)^b] , (a=0.99,b=1.7). (dC/gamma*Tc) = 1.35	GaxV2Al20	Ga0.2V2Al20	Ga	0.2	V	2	Al	20																		1	2012																										AB2C20					A	14.5203														K	1.64	1.65	1.76				1.65																				T	SP, empirical eq.	0.109												MHC153421		A	from Hc2	550										2.9	14							mJ/mol.K2	35	SP-heat	96	SP-heat																																		Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153424	JPS081124707	impurity phase: Al. Pauli para [Kai] at 10 K = 6.04 E-4cm3/mol.	GaxV2Al20	Ga0.3V2Al20	Ga	0.3	V	2	Al	20																		1	2012																										AB2C20					A	14.5202														K		1.6					1.6																																																																																														Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153425	JPS081124707	[gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 5.71 E-4cm3/mol. (dC/gamma*Tc) = 1.40	GaxV2Al20	Ga0.3V2Al20	Ga	0.3	V	2	Al	20																		1	2012																										AB2C20					A	14.5245														K		1.54					1.54																																																2.5	14							mJ/mol.K2	39	SP-heat	92	SP-heat																																		Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153426	JPS081124707	[gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 5.26 E-4cm3/mol.  (dC/gamma*Tc) = 1.45	GaxV2Al20	Ga0.3V2Al20	Ga	0.3	V	2	Al	20																		1	2012																										AB2C20					A	14.5196														K		1.5					1.5																																																3.3	14							mJ/mol.K2	38	SP-heat	86	SP-heat																																		Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153427	JPS081124707	[gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 5.01 E-4cm3/mol. Hc2=Hc2(0)[1-a(T/Tc)^b] , (a=0.994,b=1.8). (dC/gamma*Tc) = 1.35	GaxV2Al20	Ga0.3V2Al20	Ga	0.3	V	2	Al	20																		1	2012																										AB2C20					A	14.525														K		1.43					1.43																				T	SP, empirical eq.	0.137												MHC153421		A	from Hc2	500										2.7	14							mJ/mol.K2	40	SP-heat	88	SP-heat																																		Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153428	JPS081124707	[gamma] from curve fitting of Cel(T). Pauli para [Kai] at 10 K = 6.61 E-4cm3/mol.  (dC/gamma*Tc) = 1.40	AlxV2Al20	Al20.3V20	Al	20.3	V	20																				1	2012																										AB2C20					A	14.5157														K		1.49					1.49																																																2.7	14							mJ/mol.K2	33	SP-heat	420	SP-heat																																		Ga,V,Al		composite - melt in arc furnace - seal in evacuateed quartz ampoule - ANN(600-650C, 80 h)					Rattling and Superconducting Properties of the Cage Compound GaxV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)124707	Zenji HIROI,Atsushi ONOSAKA,Yoshihiko OKAMOTO,Jun-ichi YAMAURA,Hisatomo HARIMA		
153429	JPS081113708	RRR = 12. SP heat shows multi-gap SC. (dC/gamma*Tc) = 0.82. lattice term in SP: beta= 2.3 mJ/mol.K4, delta=0.02 mJ/mol.K6.	beta-Bi2Pd	Bi2Pd1	Bi	2	Pd	1																				3	2012																										AB2			I4/mmm	144	A	3.37		12.96												K	5.3		5.4				5.35																				T	resistivity, 0.5Rn, extrapolation		1.13	0.73										MHC153429		A	from Hc2		212	137													MSP153429	mJ/mol.K2	40	mJ/mol.K2	12	SP-heat	136	SP-heat																																		Bi(5N),Pd(3N)		mixture - sealed in evacuated quartz tube - heat(900C,24h) - coll to 600C and hold 72h - Q in cold water					Superconductivity at 5.4K in beta-Bi2Pd			Department of Basic Science, the University of Tokyo, Meguro, Tokyo 153-8902, Japan	J.Phys.Soc.Jpn, 81(2012)113708	Yoshinori IMAI,Fuyuki NABESHIMA,Taiki YOSHINAKA,Kosuke MIYATANI,Ryusuke KONDO,Seiki KOMIYA,Ichiro TSUKADA,Atsutaka MAEDA		
153430	JPS081113707	Hc2(0.9Rn) and Hirr(0.1Rn) were measured upto 7T. pHirr = 53.9T and nHirr = 27.7T. Anisotropy(Hc2) = 2.2.	FeTe1-xSex	Fe1Te0.65Se0.35	Fe	1	Te	0.65	Se	0.35																		3	2012																										AB		Fe-11																		K			15				15																				T	resistivity, 0.9Rn,WHH		87.9	39.2																																																																						Fe(3N),Te(5N),Se(6N)		self-flux method. heat(1100C,20h) - cool to 650C at a rate of 2C/h - furnace cool					Evidence of Inhomogeneous Superconductivity in FeTe1-xSex by Scotch-Tape Method			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 81(2012)113707	Hiroyuki OKAZAKI,Tohru WATANABE,Takahide YAMAGUCHI,Yasuna KAWASAKI,Keita DEGUCHI,Satoshi DEMURA,Toshinori OZAKI,Saleem. J. DENHOLME,Yoshikazu MIZUGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153431	JPS081113707	Film. thickness = 100nm. Hc2(0.9Rn) and Hirr(0.1Rn) were measured upto 7T. pHirr = 102.6T and nHirr = 45.6T. Anisotropy(Hc2) = 1.5.	FeTe1-xSex	Fe1Te0.65Se0.35	Fe	1	Te	0.65	Se	0.35																		5	2012																										AB		Fe-11																		K			15				15																				T	resistivity, 0.9Rn,WHH		134.3	90.6																																																																								single crystal ( #153430 sample). films made by using   scotch tape method .					Evidence of Inhomogeneous Superconductivity in FeTe1-xSex by Scotch-Tape Method			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 81(2012)113707	Hiroyuki OKAZAKI,Tohru WATANABE,Takahide YAMAGUCHI,Yasuna KAWASAKI,Keita DEGUCHI,Satoshi DEMURA,Toshinori OZAKI,Saleem. J. DENHOLME,Yoshikazu MIZUGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153432	JPS081104715	Tc defined as max of (dR/dT). SP shows Tc = 2.52K. (dC/gamma*Tc) = 1.38.	YIr2Si2	Y1Ir2Si2	Y	1	Ir	2	Si	2																		1	2012																										AB2C2	2	CaBa2Ge2			A	4.0938		9.6856												K		2.72				0.1	2.72																				T	SP, WHH	1.59												MHC153432		A	from Hc2	4550															MSP153432	mJ/mol.K2	27.9	mJ/mol.K2	8	SP-heat	145	SP-heat																																		Y(3N) or La(3N),Ir(4N),Si(6N)		arc melting.. as-cast sample.					Superconductivity in the YIr2Si2 and LaIr2Si2 Polymorphs			Faculty of Mathematics and Physics, Charles University, DCMP, Ke Karlovu 5, CZ-12116 Praha 2, Czech Republic	J.Phys.Soc.Jpn, 81(2012)104715	Michal VALISKA,Jiri POSPISIL,Jan PROKLESKA,Martin DIVIS,Alexandra RUDAJEVOVA,Vladimir SECHOVSKY		
153433	JPS081104715	not SC.	YIr2Si2	Y1Ir2Si2	Y	1	Ir	2	Si	2																		1	2012																										AB2C2	2	ThCr2Si2			A	4.0483		9.8152												K					0.4																																																										mJ/mol.K2	8	SP-heat	180	SP-heat																																		Y(3N) or La(3N),Ir(4N),Si(6N)		arc melting - ANN(800-900C) - slow cool (<1C/min)					Superconductivity in the YIr2Si2 and LaIr2Si2 Polymorphs			Faculty of Mathematics and Physics, Charles University, DCMP, Ke Karlovu 5, CZ-12116 Praha 2, Czech Republic	J.Phys.Soc.Jpn, 81(2012)104715	Michal VALISKA,Jiri POSPISIL,Jan PROKLESKA,Martin DIVIS,Alexandra RUDAJEVOVA,Vladimir SECHOVSKY		
153434	JPS081104715	Tc defined as max of (dR/dT). SP shows Tc = 1.24 K. (dC/gamma*Tc) = 0.67.	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																		1	2012																										AB2C2	2	CaBa2Ge2			A	4.1873		9.938												K		1.4				0.4	1.4																				T	SP, WHH	0.041												MHC153434		A	from Hc2	897															MSP153434	mJ/mol.K2	6.7	mJ/mol.K2	8.1	SP-heat	155	SP-heat																																		Y(3N) or La(3N),Ir(4N),Si(6N)		arc melting.. as-cast sample.					Superconductivity in the YIr2Si2 and LaIr2Si2 Polymorphs			Faculty of Mathematics and Physics, Charles University, DCMP, Ke Karlovu 5, CZ-12116 Praha 2, Czech Republic	J.Phys.Soc.Jpn, 81(2012)104715	Michal VALISKA,Jiri POSPISIL,Jan PROKLESKA,Martin DIVIS,Alexandra RUDAJEVOVA,Vladimir SECHOVSKY		
153435	JPS081104715	not SC.	LaIr2Si2	La1Ir2Si2	La	1	Ir	2	Si	2																		1	2012																										AB2C2	2	ThCr2Si2			A	4.1111		10.3001												K					0.4																																																										mJ/mol.K2	8.1	SP-heat	200	SP-heat																																		Y(3N) or La(3N),Ir(4N),Si(6N)		arc melting - ANN(800-900C) - slow cool (<1C/min)					Superconductivity in the YIr2Si2 and LaIr2Si2 Polymorphs			Faculty of Mathematics and Physics, Charles University, DCMP, Ke Karlovu 5, CZ-12116 Praha 2, Czech Republic	J.Phys.Soc.Jpn, 81(2012)104715	Michal VALISKA,Jiri POSPISIL,Jan PROKLESKA,Martin DIVIS,Alexandra RUDAJEVOVA,Vladimir SECHOVSKY		
153436	JPS081103706	T<CDW/SDW> = 50K. Tc defined based on entropy conservationusing SP. (dC/gamma*Tc) = 1.36. Wilson ratio R<W> = 2.21. lattice term in SP: beta = 0.857 mJ/mol.K4	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2012	emu/mol	0.00041																								ABC2D2	2		P4/mmm		A	4.1104		8.0864												K		1.2	2				1.2										58																																											MSP153436			mJ/mol.K2	13.5	SP-heat	239	SP-heat																																		BaO(4N),Ti(3N),Sb(3N)	1	mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat(1000C,40h) - cool to RT with 25C/h					Superconductivity in BaTi2Sb2O with a d1 Square Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 81(2012)103706	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Toshio ONO,Yuko HOSOKOSHI,Yoshitaka MATSUSHITA,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153437	JPS081084709	two phases: non-SC phase(delta-hexagonal phase, 24%) and SC phase(beta-tetragonal phase)	FeSe1-xClx	Fe1Se0.82Cl0.18	Fe	1	Se	0.82	Cl	0.18																		2	2012																										AB	2				A	3.609		5.899												K			11.5	10.5			10.5																																																																																														Fe(4N),FeCl(3N),Se(6N)		mixture - pellet - sealed in quartz tube(Ar) - slow heating to 680C - hold(16h) .					Chlorine-Doping Dependence of Crystal Structure and Superconductivity in FeSe1-xClx			Department of Physics, National Chung Cheng University, Minghsiung, Chiayi 62199, Taiwan, Republic of China	J.Phys.Soc.Jpn, 81(2012)084709	Hsin-Hsien SUNG,Ren-Ren HU,Shan-Chien CHEN,Wun-Hsin LEE		
153438	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.782 mJ/mol.K4, (dC/gamma*Tc) = 2.09 . thermodynamic Hc(0) = 0.4T	FeSe1-xTex	Fe1Se0.4Te0.6	Fe	1	Se	0.4	Te	0.6																		3	2012																										AB		Fe-11																		K		14.4					14.4																																														meV	2.53	4.16	14							mJ/mol.K2	26.5	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153439	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.782 mJ/mol.K4, (dC/gamma*Tc) = 2.76 . thermodynamic Hc(0) = 0.48 T.	FeSe1-xTex	Fe1Se0.3Te0.7	Fe	1	Se	0.3	Te	0.7																		3	2012																										AB		Fe-11																		K		14.8					14.8																																														meV	2.62	4.31	14							mJ/mol.K2	35.7	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153440	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.782 mJ/mol.K4, (dC/gamma*Tc) = 0.99 . thermodynamic Hc(0) = 0.28 T.	FeSe1-xTex	Fe1Se0.2Te0.8	Fe	1	Se	0.2	Te	0.8																		3	2012																										AB		Fe-11																		K		12.8					12.8																																														meV	1.19	1.97	14							mJ/mol.K2	57.2	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153441	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.782 mJ/mol.K4, (dC/gamma*Tc) = 0.738 . thermodynamic Hc(0) = 0.18 T.	FeSe1-xTex	Fe1Se0.1Te0.9	Fe	1	Se	0.1	Te	0.9																		3	2012																										AB		Fe-11																		K		9.1					9.1																																														meV	1.2	3.03	14							mJ/mol.K2	66.6	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153442	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.652 mJ/mol.K4.	FeSe1-xTex	Fe1Se0.05Te0.95	Fe	1	Se	0.05	Te	0.95																		3	2012																										AB		Fe-11																		K					2																																																										mJ/mol.K2	33.7	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153443	JPS081054708	C = aT+bT^3+cT^5+dT^7. b=0.643 mJ/mol.K4.	FeTe	Fe1Te1	Fe	1	Te	1																				3	2012																										AB		Fe-11																		K					2																																																										mJ/mol.K2	25.6	SP-heat																																						Bridgman method. heat(950-1050C) - cool to RT - ANN(400C,200h)					Specific-Heat Study of Superconducting and Normal States in FeSe1-xTex (0.6 =< x =< 1 Single Crystals: Strong-Coupling Superconductivity, Strong Electron-Correlation, and Inhomogeneity			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 81(2012)054708	Takashi NOJI,Masato IMAIZUMI,Takumi SUZUKI,Tadashi ADACHI,Masatsune KATO,Yoji KOIKE		
153444	PHC4750010	Epitaxial film, d=1000-1700A. Substrate= CaF2(a=5.463A). F introduced by diffusin process. F-content not given. impurity phases: SmOF, SmO0.7F1.6	Sm(O,F)FeAs	Sm1Fe1As1F0.5Ox	Sm	1	Fe	1	As	1	F	0.5													O	x		5	2012																												oxypnictide																		K	56.4		57.8				57.1																																																																																																MBE method. F-free SmFeAsO films at T<sub> = 650C. deposit SmF3 overlayer film (200A). F-diffusion (650C, 30min)					Substrate effect on structure and superconductivity in SmFeAs(O,F) epitaxial films			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 475(2012)10	S. Takano,S. Ueda,S. Takeda,H. Sugawara,M. Naito		
153445	PHC4750010	Epitaxial film, d=1000-1700A. Substrate= SrF2(a=5.800A). F introduced by diffusin process. F-content not given. impurity phases: SmOF, SmO0.7F1.6	Sm(O,F)FeAs	Sm1Fe1As1F0.5Ox	Sm	1	Fe	1	As	1	F	0.5													O	x		5	2012																												oxypnictide																		K	55.5		57.3				56.4																																																																																																MBE method. F-free SmFeAsO films at T<sub> = 650C. deposit SmF3 overlayer film (200A). F-diffusion (650C, 30min)					Substrate effect on structure and superconductivity in SmFeAs(O,F) epitaxial films			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 475(2012)10	S. Takano,S. Ueda,S. Takeda,H. Sugawara,M. Naito		
153446	PHC4750010	Epitaxial film, d=1000-1700A. Substrate= BaF2(a=6.200A). F introduced by diffusin process. F-content not given. impurity phases: SmOF, SmO0.7F1.6	Sm(O,F)FeAs	Sm1Fe1As1F0.5Ox	Sm	1	Fe	1	As	1	F	0.5													O	x		5	2012																												oxypnictide																		K	51.8		56.4				54.1																																																																																																MBE method. F-free SmFeAsO films at T<sub> = 650C. deposit SmF3 overlayer film (200A). F-diffusion (650C, 30min)					Substrate effect on structure and superconductivity in SmFeAs(O,F) epitaxial films			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 475(2012)10	S. Takano,S. Ueda,S. Takeda,H. Sugawara,M. Naito		
153447	PHC4750010	Epitaxial film, d=1000-1700A. Substrate= LaAlO3(rhombohedral, a=5.356, alpha= 60.06). F introduced by diffusin process. F-content not given. impurity phases: SmOF, SmO0.7F1.6	Sm(O,F)FeAs	Sm1Fe1As1F0.5Ox	Sm	1	Fe	1	As	1	F	0.5													O	x		5	2012																												oxypnictide																		K	49.3		50.3				49.8																																																																																																MBE method. F-free SmFeAsO films at T<sub> = 650C. deposit SmF3 overlayer film (200A). F-diffusion (650C, 30min)					Substrate effect on structure and superconductivity in SmFeAs(O,F) epitaxial films			Department of Applied Physics, Tokyo University of Agriculture and Technology, Naka-cho 2-24-16, Koganei, Tokyo 184-8588, Japan	Physica C, 475(2012)10	S. Takano,S. Ueda,S. Takeda,H. Sugawara,M. Naito		
153448	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.95La0.05Cu2.95Al0.05Oz	Y	1	Ba	1.95	La	0.05	Cu	2.95	Al	0.05											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8793	3.8282	11.662												K		90					90																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153449	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.9La0.1Cu2.9Al0.1Oz	Y	1	Ba	1.9	La	0.1	Cu	2.9	Al	0.1											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8665	3.8527	11.6478												K		84					84																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153450	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.85La0.15Cu2.85Al0.15Oz	Y	1	Ba	1.85	La	0.15	Cu	2.85	Al	0.15											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8647	3.8589	11.6336												K		83					83																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153451	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.8La0.2Cu2.8Al0.2Oz	Y	1	Ba	1.8	La	0.2	Cu	2.8	Al	0.2											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8655	3.85	11.63												K		82					82																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153452	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.75La0.25Cu2.75Al0.25Oz	Y	1	Ba	1.75	La	0.25	Cu	2.75	Al	0.25											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8612	3.8536	11.6107												K		81					81																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153453	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Al)3Oz	Y1Ba1.7La0.3Cu2.7Al0.3Oz	Y	1	Ba	1.7	La	0.3	Cu	2.7	Al	0.3											O	z		1	2012																										AB2C3D7	3	Y123			A	3.861	3.8554	11.5971												K		79					79																																																																																														Y2O3,BaCO3,La2O3,CuO,Al2O3	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153454	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.95La0.05Cu2.95Zn0.05Oz	Y	1	Ba	1.95	La	0.05	Cu	2.95	Zn	0.05											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8873	3.8239	11.6583												K		71.9					71.9																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153455	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.9La0.1Cu2.9Zn0.1Oz	Y	1	Ba	1.9	La	0.1	Cu	2.9	Zn	0.1											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8873	3.8276	11.6465												K		50.8					50.8																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153456	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.85La0.15Cu2.85Zn0.15Oz	Y	1	Ba	1.85	La	0.15	Cu	2.85	Zn	0.15											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8865	3.8284	11.6391												K		49.9					49.9																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153457	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.8La0.2Cu2.8Zn0.2Oz	Y	1	Ba	1.8	La	0.2	Cu	2.8	Zn	0.2											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8708	3.8495	11.6299												K		28.7					28.7																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153458	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.75La0.25Cu2.75Zn0.25Oz	Y	1	Ba	1.75	La	0.25	Cu	2.75	Zn	0.25											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8704	3.8544	11.6187												K		23.8					23.8																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153459	PHC4750028	co-doped Y123 materials	Y(Ba,La)2(Cu,Zn)3Oz	Y1Ba1.7La0.3Cu2.7Zn0.3Oz	Y	1	Ba	1.7	La	0.3	Cu	2.7	Zn	0.3											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8678	3.8571	11.5934												K		0					0																																																																																														Y2O3,BaCO3,La2O3,CuO,ZnO	1	mixture-CAL(930C,18h in air) - reground - pellet - SIN(940C,24h) - ANN(400C,24h, in flowing O2)					Structural and superconducting properties of co-doped YBa2-xLaxCu3-xMxOz and La-free YBa2Cu3-xMxOz (M = Al, Zn) high-TC superconductors			Materials Physics Laboratory, State Key Laboratory for Mesoscopic Physics, Department of Physics, Peking University, Beijing 100871, PR China	Physica C, 475(2012)28	S.J. Hao,,W.T. Jin,C.Q. Guo,,H. Zhang		
153460	PHC4770036	grain size = 8.1 micron by SEM.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.95Ca0.05Ba2Cu2.97Mg0.03Oz	Y	0.95	Ca	0.05	Ba	2	Cu	2.97	Mg	0.03											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8138	3.8771	11.666												K		76.6					76.6																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153461	PHC4770036	grain size = 6.5 micron by SEM. Tc not measured.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.9Ca0.1Ba2Cu2.97Mg0.03Oz	Y	0.9	Ca	0.1	Ba	2	Cu	2.97	Mg	0.03											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8111	3.872	11.665												K																																																																																																					Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153462	PHC4770036	grain size = 4.6 micron by SEM.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.85Ca0.15Ba2Cu2.97Mg0.03Oz	Y	0.85	Ca	0.15	Ba	2	Cu	2.97	Mg	0.03											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8131	3.8724	11.668												K		73.5					73.5																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153463	PHC4770036	grain size = 3.6 micron by SEM.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.8Ca0.2Ba2Cu2.97Mg0.03Oz	Y	0.8	Ca	0.2	Ba	2	Cu	2.97	Mg	0.03											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8132	3.8749	11.668												K		71.85					71.85																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153464	PHC4770036	grain size = 4.3 micron by SEM. atomic compo. O(53.98),Mg(0.89),Ca(0.37),Cu(22.27),Y(6.66),Ba(15.83)	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.95Ca0.05Ba2Cu2.94Mg0.06Oz	Y	0.95	Ca	0.05	Ba	2	Cu	2.94	Mg	0.06											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8179	3.8856	11.683												K		75.92					75.92																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153465	PHC4770036	grain size = 3.2 micron by SEM. Tc not measured.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.9Ca0.1Ba2Cu2.94Mg0.06Oz	Y	0.9	Ca	0.1	Ba	2	Cu	2.94	Mg	0.06											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8179	3.8789	11.673												K																																																																																																					Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153466	PHC4770036	grain size = 2.8 micron by SEM.	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.85Ca0.15Ba2Cu2.94Mg0.06Oz	Y	0.85	Ca	0.15	Ba	2	Cu	2.94	Mg	0.06											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8095	3.8522	11.629												K		72.6					72.6																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153467	PHC4770036	grain size = 1.7 micron by SEM. O(53.94),Mg(0.80),Ca(1.44),Cu(23.12),Y(5.40),Ba(15.30)	(Y,Ca)Ba2(Cu,Mg)3Oz	Y0.8Ca0.2Ba2Cu2.94Mg0.06Oz	Y	0.8	Ca	0.2	Ba	2	Cu	2.94	Mg	0.06											O	z		1	2012																										AB2C3D7	3	Y123			A	3.8068	3.8542	11.619												K		72.3					72.3																																																																																														Y2O3,CaCO3,BaCO3,MgO,CuO	1	mixture - heat(750C,900C,5h) - SIN(915,930C,24h) - heat(940C,6h,in flowing O2) - rapid cool to 400C - ANN(400C,24h) - FC to RT					Effect of double substitution on structural and magnetic properties of Y1-xCaxBa2(Cu1-yMgy)3O7-z			Universite Mentouri, Laboratoire de Couches Minces et Interfaces, Campus de Chaabet Erssas, 25017 Constantine, Algeria	Physica C, 477(2012)36	S. Attaf,M.F. Mosbah,R. Fittipaldi,D. Zola,S. Pace,A. Vecchione		
153468	PHC4770063	impurity phase: YNi2Ge2. AlB2 derived structure.	Y2NiGe3	Y2Ni1Ge3	Y	2	Ni	1	Ge	3																		1	2012																										AB2C3					A	4.066		4.025												K		0.533				0.037	0.533																																																											480	R(T), fitting Broch eq.																																		Y(4N) or La(4N),Ni(5N),Ge(4N)		arc-melting - wrapped in Ta foil - sealed in evacuated quartz tube - ANN(700C,1w)					Superconductivity of the Ni-based ternary compounds with AlB2-type structure Y2NiGe3 and La2NiGe3			Department of Physics, National Taiwan University, Taipei, Taiwan, ROC	Physica C, 477(2012)63	J.W. Chen,S.Y. Guan,C.H. Wang,S.P. Ho		
153469	PHC4770063	impurity phase: LaNi2Ge2. AlB2 derived structure.	La2NiGe3	La2Ni1Ge3	La	2	Ni	1	Ge	3																		1	2012																										AB2C3					A	4.18		4.334												K		0.394				0.091	0.394																																																											300	R(T), fitting Broch eq.																																		Y(4N) or La(4N),Ni(5N),Ge(4N)		arc-melting - wrapped in Ta foil - sealed in evacuated quartz tube - ANN(700C,1w)					Superconductivity of the Ni-based ternary compounds with AlB2-type structure Y2NiGe3 and La2NiGe3			Department of Physics, National Taiwan University, Taipei, Taiwan, ROC	Physica C, 477(2012)63	J.W. Chen,S.Y. Guan,C.H. Wang,S.P. Ho		
153470	PHC4780005	Two gap model: gap(0.19, 1.02 meV), Tc(4.1, 5.4K), penet(2050, 3210 A), (2D/kTc) = (1.08,  4.37). Hc2 and cohere from PRL100157001.	Lu2Fe3Si5	Lu2Fe3Si5	Lu	2	Fe	3	Si	5																		3	2012																										A2B3C5		Sc2Fe3Si5																		K		6.1				1	6.1											Oe	M-H curve, considering demag factor			121			32.5	2	T				13										MHC153470		A	from Hc2		50		A	Hc1, GL theory		2420				4.37																																																floating zone method. ANN for 2 weeks.					Two energy gaps in superconducting Lu2Fe3Si5 single crystal derived from the temperature dependence of lower critical field Hc1(T)			INPAC?Institute for Nanoscale Physics and Chemistry, KU Leuven, Celestijnenlaan 200D, B-3001 Leuven, Belgium	Physica C, 478(2012)5	J. Ge,J. Gutierrez,B. Raes,T. Watanabe,J. Koshio,V.V. Moshchalkov		
153471	PHC4780029		Ca2-xNaxCuO2Cl2	Ca1.875Na0.125Cu1Cl2O2	Ca	1.875	Na	0.125	Cu	1	Cl	2													O	2		3	2012																										AB2C4		T			A			15.1388												K				15			15																																																																																														Ca2CuO2Cl2,NaClO4,NaCl		mixture - sealed in Pt capsules - heat to 1200c with 10 min - keep for 40min - cool to 10toc for 6h					High-pressure growth of Ca2-xNaxCuO2Cl2 single crystals and pressure effect on superconductivity			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Physica C, 478(2012)29	Runze Yu,,Qingqing Liu,Sijia Zhang,Xiancheng Wang,Wei Han,Changqing Jin		
153472	PHC4780029		Ca2-xNaxCuO2Cl2	Ca1.867Na0.133Cu1Cl2O2	Ca	1.867	Na	0.133	Cu	1	Cl	2													O	2		3	2012																										AB2C4		T			A			15.1481												K				20			20	TC153472		K/GPa	-1.87																																																																																										Ca2CuO2Cl2,NaClO4,NaCl		mixture - sealed in Pt capsules - heat to 1200c with 10 min - keep for 40min - cool to 10toc for 6h					High-pressure growth of Ca2-xNaxCuO2Cl2 single crystals and pressure effect on superconductivity			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Physica C, 478(2012)29	Runze Yu,,Qingqing Liu,Sijia Zhang,Xiancheng Wang,Wei Han,Changqing Jin		
153473	PHC4780029		Ca2-xNaxCuO2Cl2	Ca1.843Na0.157Cu1Cl2O2	Ca	1.843	Na	0.157	Cu	1	Cl	2													O	2		3	2012																										AB2C4		T			A			15.1565												K				25			25																																																																																														Ca2CuO2Cl2,NaClO4,NaCl		mixture - sealed in Pt capsules - heat to 1200c with 10 min - keep for 40min - cool to 10toc for 6h					High-pressure growth of Ca2-xNaxCuO2Cl2 single crystals and pressure effect on superconductivity			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Physica C, 478(2012)29	Runze Yu,,Qingqing Liu,Sijia Zhang,Xiancheng Wang,Wei Han,Changqing Jin		
153474	PHC4790095	gap paameter obtained by BCS fitting of STS conductance (at T=0.42 K)	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		3	2012																										AB2C2		ThCr2Si2																		K		2.6					2.6																																														meV	0.43	3.84	1																																															high-T flux method using PdGe self flux.					Superconducting density of states and vortex studies on SrPd2Ge2			Centre of Low Temperature Physics, Institute of Experimental Physics SAS & Faculty of Science, P.J. Safarik University, Kosice, Slovakia	Physica C, 479(2012)95	T. Samuely,P. Szabo,J.G. Rodrigo,P. Samuely		
153475	PHC4800001	72h-reduction. grain size: several micron meter by SEM.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.06	Pr	2	Ba	4	Cu	7															O	15-z	14.06	1	2012																										A2B4C7D15		Y247																		K				30.5			30.5	TC153475																																																																	uV/K	29.2			TP153475																										sol-gel method. mixture - CAL(800C,24h,in air) - press to pellet - SIN(875-876C,180h, in O2) - ANN(500C,48 or 72h, in vac)					Magnetization and transport properties in the superconducting Pr2Ba4Cu7O15-z with metallic double-chain			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	Physica C, 480(2012)1	Shibuki Toshima,Michiaki Matsukawa,Taiji Chiba,Satoru Kobayashi,Sigeki Nimori,Makoto Hagiwara		
153476	PHC4800001	48h-reduction. grain size: several micron meter by SEM.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.3	Pr	2	Ba	4	Cu	7															O	15-z	14.3	1	2012																										A2B4C7D15		Y247																		K				21			21																																																																																																sol-gel method. mixture - CAL(800C,24h,in air) - press to pellet - SIN(875-876C,180h, in O2) - ANN(500C,48 or 72h, in vac)					Magnetization and transport properties in the superconducting Pr2Ba4Cu7O15-z with metallic double-chain			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	Physica C, 480(2012)1	Shibuki Toshima,Michiaki Matsukawa,Taiji Chiba,Satoru Kobayashi,Sigeki Nimori,Makoto Hagiwara		
153477	PHC4830162	grain size = 20 nm. Film thickness = 80 nm. Film compositions : 71.1 at % Pb, 28.9 at % Bi.  Hc2 for H perpendicular to film plane.	Pb7Bi3	Pb7Bi3	Pb	7	Bi	3																				4	2012																										A3B7			P63mmc		A	3.5058		5.7959												K		10.3					10.3																																																																																																electroplating on brass substrates. various electroplating parameters are tested					The superconducting properties of nanostructured Pb7Bi3 films obtained by pulse electroplating			Institute of Solid State Physics RAS, Academika Osipyana, 2, Chernogolovka, Moscow Reg., Russia	Physica C, 483(2012)162	G.V. Strukov,V.S. Stolyarov,G.K. Strukova,V.N. Zverev		
153478	PHC4830162	Film thickness = submicron. electroplating with no Ce(+3) ion in electrolyte.	Pb7Bi3	Pb7Bi3	Pb	7	Bi	3																				4	2012																										A3B7			P63mmc																	K		7.8					7.8																				T					0.7			4.2																																																																				electroplating on brass substrates. various electroplating parameters are tested					The superconducting properties of nanostructured Pb7Bi3 films obtained by pulse electroplating			Institute of Solid State Physics RAS, Academika Osipyana, 2, Chernogolovka, Moscow Reg., Russia	Physica C, 483(2012)162	G.V. Strukov,V.S. Stolyarov,G.K. Strukova,V.N. Zverev		
153479	PHC4830207	grain size = 100 um. Tc determind by sound velocity. longitudinal sound velocity decreases at Tc.	BaFe2-xNixAs2	Ba1Fe1.93Ni0.07As2	Ba	1	Fe	1.93	Ni	0.07	As	2																3	2012																										AB2C2																				K		17					17			K/GPa	9																																																																																												crystals grown using Fe/Ni -As self flux method					Elastic anomalies in BaFe2-xNixAs2 crystals			Institut Neel, CNRS et Universite Joseph Fourier BP 166, F 38042 Grenoble Cedex 9, France	Physica C, 483(2012)207	M. Saint-Paul,A. Abbassi,Zhao-Sheng Wang,Huinqian Luo,Xingye Lu,Cong Ren,Hai-Hu Wen,K. Hasselbach		
153480	PHC4830207	elastic constant  c<66> is minimum at Tc. (dTc/dP) is calculated from sonic velocity.	BaFe2-xNixAs2	Ba1Fe1.85Ni0.15As2	Ba	1	Fe	1.85	Ni	0.15	As	2																3	2012																										AB2C2																				K		13.5					13.5																																																																																																crystals grown using Fe/Ni -As self flux method					Elastic anomalies in BaFe2-xNixAs2 crystals			Institut Neel, CNRS et Universite Joseph Fourier BP 166, F 38042 Grenoble Cedex 9, France	Physica C, 483(2012)207	M. Saint-Paul,A. Abbassi,Zhao-Sheng Wang,Huinqian Luo,Xingye Lu,Cong Ren,Hai-Hu Wen,K. Hasselbach		
153481	SSC1520513	Tc = 0.825 K from SP-heat. There are three different Tc (SUS, Res, SP).	YIn3	Y1In3	Y	1	In	3																				3	2012																										AB3		AuCu3			A	4.593													triclinic, alpha=99.04, beta=108.21, gamma=90.0	K			1.08	0.96		0.1	0.96																																																																																														In(6N),Y(3N)		excess In flux(In:Y = 50:1) in Al-crucible. sealed in quartz( Ar) - heat an hold(1150C, 72h) - slow cool to 450 C.					Superconductivity in single-crystal YIn3			Physics Department, University of California Davis, Davis, CA 95616, United States	Solid State Commun., 152(2012)513	S.D. Johnson,J.R. Young,R.J. Zieve,J.C. Cooley		
153482	SSC1520635	alpha-phase. Hc2 defined as R/Rn = 0.5.	Ca10(Pt4As8)(Fe1.64Pt0.36As2)5	Ca10Pt5.8Fe8.2As18	Ca	10	Pt	5.8	Fe	8.2	As	18																3	2012																													P1[-]		A	8.719	8.727	11.161											triclinic, alpha=94.82, beta=99.62, gamma=89.99	K	32.7		34.6				33.65	MTC153482		K/GPa	-0.9																T	resistivity, WHH theory			35					T/K	resistivity			1.6																																																															See J.Phys.Soc.Jpn 80(2011)093704					Iron-platinum-arsenide superconductors Ca10(PtnAs8)(Fe2-xPtxAs2)5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Solid State Commun., 152(2012)635	Minoru Nohara,Satomi Kakiya,Kazutaka Kudo,Yoshihiro Oshiro,Shingo Araki,Tatsuo C. Kobayashi,Kenta Oku,Eiji Nishibori,Hiroshi Sawa		
153483	SSC1520635	beta-phase. Hc2 defined as R/Rn = 0.5.	Ca10(Pt4As8)(Fe1.84Pt0.16As2)5	Ca10Pt4.8Fe9.2As18	Ca	10	Pt	4.8	Fe	9.2	As	18																3	2012																													P1[-]		A	8.795	8.789	21.008												K	13.7						13.7																				T	resistivity, WHH theory			22					T/K	resistivity			2.3																																																															See J.Phys.Soc.Jpn 80(2011)093704					Iron-platinum-arsenide superconductors Ca10(PtnAs8)(Fe2-xPtxAs2)5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Solid State Commun., 152(2012)635	Minoru Nohara,Satomi Kakiya,Kazutaka Kudo,Yoshihiro Oshiro,Shingo Araki,Tatsuo C. Kobayashi,Kenta Oku,Eiji Nishibori,Hiroshi Sawa		
153484	SSC1520640	compositions are nominal values.	Fe2As2(Sr4V2O6)	Fe2As2Sr4V2O6	Fe	2	As	2	Sr	4	V	2													O	6		1	2012																												FA22426			A			15.7											XRD	K				27			27																																																																																															1	solid state reaction in sealed quartz ampoule. details are in Appl.Phys.Exp. 3(2010)63102					Irreversibility lines of layered Fe-based superconductors with thick blocking layers			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Solid State Commun., 152(2012)640	Jun-ichi Shimoyama,Hiraku Ogino,Akiyasu Yamamoto,Kohji Kishio		
153485	SSC1520640	compositions are nominal values. Tirr/Tc at H=100Oe = 0.95. Hirr(T=0.7Tc) = 123 mT . anisotropy  < 80.	Fe2As2(Ca4(Mg0.25Ti0.75)3O7.5)	Fe2As2Ca4Mg0.75Ti2.25O7.5	Fe	2	As	2	Ca	4	Mg	0.75	Ti	2.25											O	7.5		1	2012																												FA22438			A			16.7											XRD	K				42			42																																																																																															1	solid state reaction in sealed quartz ampoule. details are in Appl.Phys.Exp. 3(2010)63102					Irreversibility lines of layered Fe-based superconductors with thick blocking layers			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Solid State Commun., 152(2012)640	Jun-ichi Shimoyama,Hiraku Ogino,Akiyasu Yamamoto,Kohji Kishio		
153486	SSC1520640	compositions are nominal values. Tirr/Tc at H=100Oe = 0.72. Hirr(T=0.7Tc) = 16.9 mT . anisotropy  > 100.	Fe2As2(Ca5(Sc0.5Ti0.5)4O10.5)	Fe2As2Ca5Sc2Ti2O10.5	Fe	2	As	2	Ca	5	Sc	2	Ti	2											O	10.5		1	2012																												FA2254(11)			A			20.6											XRD	K				33			33																																																																																															1	solid state reaction in sealed quartz ampoule. details are in Appl.Phys.Exp. 3(2010)63102					Irreversibility lines of layered Fe-based superconductors with thick blocking layers			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Solid State Commun., 152(2012)640	Jun-ichi Shimoyama,Hiraku Ogino,Akiyasu Yamamoto,Kohji Kishio		
153487	SSC1520640	compositions are nominal values. Tirr/Tc at H=100Oe = 0.67. Hirr(T=0.7Tc) = 4.1 mT . anisotropy  > 100.	Fe2As2(Ca6(Al0.25Ti0.75)4O11)	Fe2As2Ca6Al1Ti3O11	Fe	2	As	2	Ca	6	Al	1	Ti	3											O	11		1	2012																												FA2264(12)			A			22.7											XRD	K				32			32																																																																																															1	solid state reaction in sealed quartz ampoule. details are in Appl.Phys.Exp. 3(2010)63102					Irreversibility lines of layered Fe-based superconductors with thick blocking layers			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Solid State Commun., 152(2012)640	Jun-ichi Shimoyama,Hiraku Ogino,Akiyasu Yamamoto,Kohji Kishio		
153488	SSC1520640	compositions are nominal values. Tirr/Tc at H=100Oe = 0.61. Hirr(T=0.7Tc) =  0.35 mT. anisotropy  > 100.	Fe2As2(Ca5(Mg0.25Ti0.75)4O9.5)	Fe2As2Ca5Mg1Ti3O9.5	Fe	2	As	2	Ca	5	Mg	1	Ti	3											O	9.5			2012																												FA2286(18)			A			30											XRD	K				36			36																																																																																															1	solid state reaction in sealed quartz ampoule. main phase (FA2286(18) ) formed by SIN(1125 C, 72h).					Irreversibility lines of layered Fe-based superconductors with thick blocking layers			Department of Applied Chemistry, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Solid State Commun., 152(2012)640	Jun-ichi Shimoyama,Hiraku Ogino,Akiyasu Yamamoto,Kohji Kishio		
153489	SSC1520671	single crystals were cleaved into thin slices. RH150 = -29.97 m3/C. carrier shows at 150 K.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.91Co0.09As2	Ba	1	Fe	1.91	Co	0.09	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		16.76					16.76																				T	resistivity, WHH			2.861					T/K	resistivity			0.252																																																				m3/C	-0.000000002044					MRH153491	n/cm3	2120000000000000000000			HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153490	SSC1520671	single crystals were cleaved into thin slices.	Ba(Fe,Co)2As2	Ba1Fe1.87Zn0.04Co0.09As2	Ba	1	Fe	1.87	Zn	0.04	Co	0.09	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		13.42					13.42																				T	resistivity, WHH			1.278					T/K	resistivity			0.123																																																															HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153491	SSC1520671	single crystals were cleaved into thin slices. RH150 = -31.33 m3/C. carrier shows at 150 K.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.83Zn0.08Co0.09As2	Ba	1	Fe	1.83	Zn	0.08	Co	0.09	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		7.54					7.54																																																																																					m3/C	-0.000000003474						n/cm3	2030000000000000000000			HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153492	SSC1520671	single crystals were cleaved into thin slices. RH150 = -71.53 m3/C. carrier shows at 150 K.	Ba(Fe,Co)2As2	Ba1Fe1.78Co0.22As2	Ba	1	Fe	1.78	Co	0.22	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		18.96					18.96																				T	resistivity, WHH			1.747					T/K	resistivity			0.135																																																				m3/C	-0.000000004292						n/cm3	887000000000000000000			HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153493	SSC1520671	single crystals were cleaved into thin slices.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.74Zn0.04Co0.22As2	Ba	1	Fe	1.74	Zn	0.04	Co	0.22	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		15.82					15.82																				T	resistivity, WHH			2.87					T/K	resistivity			0.265																																																															HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153494	SSC1520671	single crystals were cleaved into thin slices. RH150 = -65.40 m3/C. carrier shows at 150 K.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.7Zn0.08Co0.22As2	Ba	1	Fe	1.7	Zn	0.08	Co	0.22	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		8.77					8.77																																																																																					m3/C	-0.000000003951						n/cm3	960000000000000000000			HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153495	SSC1520671	single crystals were cleaved into thin slices.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.66Zn0.12Co0.22As2	Ba	1	Fe	1.66	Zn	0.12	Co	0.22	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		4.6					4.6																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153496	SSC1520671	single crystals were cleaved into thin slices.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.79Zn0.12Co0.09As2	Ba	1	Fe	1.79	Zn	0.12	Co	0.09	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		3.37					3.37																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153497	SSC1520671		Sr(Fe,Co)2As2	Sr1Fe1.8Co0.2As2	Sr	1	Fe	1.8	Co	0.2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		17.53					17.53																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153498	SSC1520671		Sr(Fe,Zn,Co)2As2	Sr1Fe1.76Zn0.04Co0.2As2	Sr	1	Fe	1.76	Zn	0.04	Co	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		12.1					12.1																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153499	SSC1520671		Sr(Fe,Zn,Co)2As2	Sr1Fe1.72Zn0.08Co0.2As2	Sr	1	Fe	1.72	Zn	0.08	Co	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		9.41					9.41																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153500	SSC1520671		Sr(Fe,Zn,Co)2As2	Sr1Fe1.68Zn0.12Co0.2As2	Sr	1	Fe	1.68	Zn	0.12	Co	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		6.22					6.22																																																																																																HP method. mixture in BN - Ta capsule - preheat(1900C,1h, in N2) -heat(1300C,2h, at P=3 GPa) - cool to 1100C within 1h					Impurity effects on the Fe-based superconductor A(Fe1-yCoy)2As2 (A = Ba and Sr)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)671	Jun Li,Yanfeng Guo,Shoubao Zhang,Yoshihiro Tsujimoto,Xia Wang,C.I. Sathish,Shan Yu,Kazunari Yamaura,Eiji Takayama-Muromachi		
153501	JPS081033701	P-content by EDX. T<STR> = 84.7 K, T<SDW> = 75.6 K.	BaFe2(As,P)2	Ba1Fe2As1.6P0.4	Ba	1	Fe	2	As	1.6	P	0.4																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		8.6					8.6																																																																																																See Phys.Rev.B, 81(2010)184519					Microscopic Evidence of Direct Coupling between Magnetic and Superconducting Order Parameters in BaFe2(As1-xPx)2			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 81(2012)033701	Tetsuya IYE,Yusuke NAKAI,Shunsaku KITAGAWA,Kenji ISHIDA,Shigeru KASAHARA,Takasada SHIBAUCHI,Yuji MATSUDA,Takahito TERASHIMA		
153502	JPS081033701	P-content by EDX. T<STR> = 61.6 K, T<SDW> = 53.4 K. not bulk SC. At P=2 GPa, sample shows bulk SC (Tc=13 K) from Meissner signal.	BaFe2(As,P)2	Ba1Fe2As1.5P0.5	Ba	1	Fe	2	As	1.5	P	0.5																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		29.9					29.9																																																																																																See Phys.Rev.B, 81(2010)184519					Microscopic Evidence of Direct Coupling between Magnetic and Superconducting Order Parameters in BaFe2(As1-xPx)2			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 81(2012)033701	Tetsuya IYE,Yusuke NAKAI,Shunsaku KITAGAWA,Kenji ISHIDA,Shigeru KASAHARA,Takasada SHIBAUCHI,Yuji MATSUDA,Takahito TERASHIMA		
153503	SSC1520849	Hc, Hc2 defined as SP using entropy conservation. (dC/gamma*Tc) = 1.89. e-ph coupling = 0.66. residual [gamma] = 0.4 mJ/mol.K2.	CuRh2S4	Cu1Rh2S4	Cu	1	Rh	2	S	4																		1	2012																										AB2C4		spinel																		K		4.72					4.72																				T	SP-heat	3.3												MHC153503																			MSP153503			mJ/mol.K2	26.9	SP-heat	258	SP-heat																																				solid state reaction in evacuated quartz tube					Heat capacity of the spinel superconductors CuRh2S4 and CuRh2Se4			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)849	Makoto Tachibana		
153504	SSC1520849	Hc, Hc2 defined as SP using entropy conservation. (dC/gamma*Tc) = 1.68. e-ph coupling = 0.63. residual [gamma] = 0.2 mJ/mol.K2.	CuRh2Se4	Cu1Rh2Se4	Cu	1	Rh	2	Se	4																		1	2012																										AB2C4		spinel																		K		3.38					3.38																				T	SP-heat	0.58												MHC153504																			MSP153504			mJ/mol.K2	21.4	SP-heat	218	SP-heat																																				solid state reaction in evacuated quartz tube					Heat capacity of the spinel superconductors CuRh2S4 and CuRh2Se4			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Solid State Commun., 152(2012)849	Makoto Tachibana		
153505	JPS081044704	InN[12[-]10] // substrate Al2O3[101[-]0]. Tc defined as 0.5 Rn.	InN	In1N1	In	1	N	1																				5	2012																										AB	7																		hexagonal. c-axis /n sapphire(0001)	K	0.25	0.47	1				0.47																																																																																																ga-source MBE with GaN & AlN buffer layers.					Superconducting Properties of InN with Low Carrier Density near the Mott Transition			Department of Electronics, Tokai University, Hiratsuka, Kanagawa 259-1292, Japan	J.Phys.Soc.Jpn, 81(2012)044704	Takashi INUSHIMA,Duncan K. MAUDE,Hai LU,William J. SCHAFF,Takuya IIZUKA,Shin-ichi KIMURA,Akio YAMAMOTO,Kazutoshi FUKUI		
153506	JPS081044704	InN[12[-]10] // substrate Al2O3[101[-]0]. Tc defined as 0.5 Rn.	InN	In1N1	In	1	N	1																				5	2012																										AB	7																		hexagonal. c-axis /n sapphire(0001)	K	1.8	2.4	3.5				2.4																																																																																																ga-source MBE with GaN & AlN buffer layers.					Superconducting Properties of InN with Low Carrier Density near the Mott Transition			Department of Electronics, Tokai University, Hiratsuka, Kanagawa 259-1292, Japan	J.Phys.Soc.Jpn, 81(2012)044704	Takashi INUSHIMA,Duncan K. MAUDE,Hai LU,William J. SCHAFF,Takuya IIZUKA,Shin-ichi KIMURA,Akio YAMAMOTO,Kazutoshi FUKUI		
153507	JPS081044704	InN[12[-]10] // substrate Al2O3[101[-]0]. Tc defined as 0.5 Rn. BCS-type SC. Hc2 measured by ac-SUS.	InN	In1N1	In	1	N	1																				5	2012																										AB	7																		hexagonal. c-axis /n sapphire(0001)	K		1.3					1.3																																				A	from Hc2	3100								meV	0.43																																																	rf-MBE					Superconducting Properties of InN with Low Carrier Density near the Mott Transition			Department of Electronics, Tokai University, Hiratsuka, Kanagawa 259-1292, Japan	J.Phys.Soc.Jpn, 81(2012)044704	Takashi INUSHIMA,Duncan K. MAUDE,Hai LU,William J. SCHAFF,Takuya IIZUKA,Shin-ichi KIMURA,Akio YAMAMOTO,Kazutoshi FUKUI		
153508	JPS081044704	InN[12[-]10] // substrate Al2O3[101[-]0]. Tc defined as 0.5 Rn.	InN	In1N1	In	1	N	1																				5	2012																										AB	7																		hexagonal. c-axis /n sapphire(0001)	K	2	2.7	3				2.7																																																																																																metalorganic vapor epitaxy with GaN buffer layer					Superconducting Properties of InN with Low Carrier Density near the Mott Transition			Department of Electronics, Tokai University, Hiratsuka, Kanagawa 259-1292, Japan	J.Phys.Soc.Jpn, 81(2012)044704	Takashi INUSHIMA,Duncan K. MAUDE,Hai LU,William J. SCHAFF,Takuya IIZUKA,Shin-ichi KIMURA,Akio YAMAMOTO,Kazutoshi FUKUI		
153509	SSC1521135	as-grown sample. not bulk SC. bulk SC for x >= 0.4	FeTe1-xSex	Fe1Te0.8Se0.2	Fe	1	Te	0.8	Se	0.2																		3	2012																										AB		Fe-11																		K				10.5			10.5	MTC153509																																																																																													Fe(3N),Te(5N),Se(5N)		self-flux method. mixture - evacuated double quartz tube - heat(1100C,20h) - cool to 650C (4-5 K/h) - FC to RT					Phase diagram and oxygen annealing effect of FeTe1-xSex iron-based superconductor			National Institute for Materials Science, 1-2-1Sengen, Tsukuba 305-0047, Japan	Solid State Commun., 152(2012)1135	Yasuna Kawasaki,Keita Deguchi,Satoshi Demura,Tohru Watanabe,Hiroyuki Okazaki,Toshinori  Ozaki,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
153510	SSC1521135	O2-anneald sample. typical O-content: Fe1+xTe0.9Se0.1O0.07. bulk SC for 0.1 =< x	FeTe1-xSex	Fe1Te0.6Se0.4	Fe	1	Te	0.6	Se	0.4																		3	2012																										AB		Fe-11																		K				14.3			14.3	MTC153510																																																																																													Fe(3N),Te(5N),Se(5N)		self-flux method. mixture - evacuated double quartz tube - heat(1100C,20h) - cool to 650C (4-5 K/h) - FC to RT					Phase diagram and oxygen annealing effect of FeTe1-xSex iron-based superconductor			National Institute for Materials Science, 1-2-1Sengen, Tsukuba 305-0047, Japan	Solid State Commun., 152(2012)1135	Yasuna Kawasaki,Keita Deguchi,Satoshi Demura,Tohru Watanabe,Hiroyuki Okazaki,Toshinori  Ozaki,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
153511	SSC1521076	Hc2 defined as STM tunneling spectroscopy, down to 0.1 K. Hc2 feature shows three phases at T= 2, 4, 6 K. H//a-axis.	ErNi2B2C	Er1Ni2B2C	Er	1	Ni	2	B	2	C																	3	2012																										ABC2D2		LuNi2B2C																		K		11					11																				T	STM													MHC153511																																																														sample was prepared by cutting a suitable needle out of single crystalline platelets of several mm thickness along tha basal plane.					Magnetic and superconducting phase diagrams in ErNi2B2C			Laboratorio de Bajas Temperaturas, Departamento de Fisica  de la Materia Condensada, Instituto de Ciencia de Materiales Nicolas Cabrera Facultad de Ciencias, Universidad Autonoma de Madrid, 28049 Madrid, Spain	Solid State Commun., 152(2012)1076	J.A. Galvis,M.Crespo,I.Guillamon,H.Suderow,S.Vieira,M.Garcia Hernandez,S.Bud'ko,P.C.Canfield		
153512	SSC1521678	Hc1=85 Oe (4K), = 35 Oe (6K).	Mg1.2(C,B)1.6Ni3	Mg1.2C1.6Ni3	Mg	1.2	C	1.6	Ni	3																			2012																										ABC3		CaTiO3	Pm3m		A	3.8106														K				7.3			7.3											Oe	M-H curve				150			2	T	M-H curve				9.17			2																																																																		Mg(2N),Ni(4N),amor-C,B(3N)		mixture - pellet - iron alloy capsule - heat(600C,2h, at 10C/min in Ar-flow) - heat(950C,3h) - cool to RT					Effect of Boron substitution on the superconductivity of non-oxide perovskite MgCNi3			Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Solid State Commun., 152(2012)1678	Anuj Kumar,Rajveer Jha,R.P. Tandon,V.P.S. Awana		
153513	SSC1521678	Hc1=95 Oe (4K), = 50 Oe (6K).	Mg1.2(C,B)1.6Ni3	Mg1.2C1.52B0.08Ni3	Mg	1.2	C	1.52	B	0.08	Ni	3																	2012																										ABC3		CaTiO3	Pm3m		A	3.8164														K				6.9			6.9											Oe	M-H curve				160			2	T	M-H curve				5.844			2																																																																		Mg(2N),Ni(4N),amor-C,B(3N)		mixture - pellet - iron alloy capsule - heat(600C,2h, at 10C/min in Ar-flow) - heat(950C,3h) - cool to RT					Effect of Boron substitution on the superconductivity of non-oxide perovskite MgCNi3			Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Solid State Commun., 152(2012)1678	Anuj Kumar,Rajveer Jha,R.P. Tandon,V.P.S. Awana		
153514	SSC1521678	Hc1=160 Oe (4K), = 70 Oe (6K).	Mg1.2(C,B)1.6Ni3	Mg1.2C1.44B0.16Ni3	Mg	1.2	C	1.44	B	0.16	Ni	3																	2012																										ABC3		CaTiO3	Pm3m		A	3.8173														K				6.6			6.6											Oe	M-H curve				200			2	T	M-H curve				4.25			2																																																																		Mg(2N),Ni(4N),amor-C,B(3N)		mixture - pellet - iron alloy capsule - heat(600C,2h, at 10C/min in Ar-flow) - heat(950C,3h) - cool to RT					Effect of Boron substitution on the superconductivity of non-oxide perovskite MgCNi3			Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Solid State Commun., 152(2012)1678	Anuj Kumar,Rajveer Jha,R.P. Tandon,V.P.S. Awana		
153515	PRB085014510	fresh sample (d=0 in Na1-dFeAs). TCFIG shows Na-deintercalated effect by air exposure	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																			2012																										ABC		PbFCl																		K	12		14				13	MTC153515																																																																																															mixture(Na,Fe,As) - seal in Ta tube - heat(950C) - cool to 900C with 5C/h - stored in sealed container(inert gas)					Evolution of normal and superconducting properties of single crystals of Na1-zFeAs upon interaction with environment			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)014510	M. A. Tanatar,N. Spyrison,Kyuil Cho,E. C. Blomberg,Guotai Tan,Pengcheng Dai,Chenglin Zhang,R. Prozorov		
153516	PRB085014510	stored in Apiezon greese for 8.5h.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																			2012																										ABC		PbFCl																		K			26				26																																																																																																mixture(Na,Fe,As) - seal in Ta tube - heat(950C) - cool to 900C with 5C/h - stored in sealed container(inert gas)					Evolution of normal and superconducting properties of single crystals of Na1-zFeAs upon interaction with environment			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)014510	M. A. Tanatar,N. Spyrison,Kyuil Cho,E. C. Blomberg,Guotai Tan,Pengcheng Dai,Chenglin Zhang,R. Prozorov		
153517	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.988Mo0.012As2	Ba	1	Fe	1.988	Mo	0.012	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9617		13.0195											Fe-122	K			16.3				16.3	MTC153517																																																																																															mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153518	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.982Mo0.018As2	Ba	1	Fe	1.982	Mo	0.018	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9613		13.0208											Fe-122	K			16.7				16.7	MTC153517																																																																																															mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153519	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.974Mo0.026As2	Ba	1	Fe	1.974	Mo	0.026	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9607		13.0298											Fe-122	K			12.5				12.5																																																																																																mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153520	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.948Mo0.052As2	Ba	1	Fe	1.948	Mo	0.052	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9612		13.0484											Fe-122	K			7.4				7.4																																																																																																mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153521	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.946Mo0.056As2	Ba	1	Fe	1.946	Mo	0.056	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9605		13.0517											Fe-122	K			4.9				4.9																																																																																																mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153522	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.91Mo0.09As2	Ba	1	Fe	1.91	Mo	0.09	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9602		13.074											Fe-122	K					0																																																																																																		mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153523	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.902Mo0.098As2	Ba	1	Fe	1.902	Mo	0.098	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9598		13.0948											Fe-122	K					0																																																																																																		mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153524	PRB085024503	Ba-content by EDS. Tn nearly equal to T<STR> measured by SUS and RES. Tc defined as sharp drop of R, but not to zero (maybe filamentary SC)	Ba(Fe,Mo)2As2	Ba1Fe1.868Mo0.132As2	Ba	1	Fe	1.868	Mo	0.132	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9612		13.12											Fe-122	K					0																																																																																																		mixture - heat(1200C,20h) - cool (2C/h) - decanting of flux at 1100C or 1120C					Effect of molybdenum 4d hole substitution in BaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 85(2012)024503	Athena S. Sefat,Karol Marty,Andrew D. Christianson,Bayrammurad Saparov,Michael A. McGuire,Mark D. Lumsden,Wei Tian,Brian C. Sales		
153525	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . T<STR> = 90 K. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.04Fe9.96As18	Ca	10	Pt	3.04	Fe	9.96	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K					0																																																																																																		See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153526	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . T<STR> = 50 K. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.18Fe9.82As18	Ca	10	Pt	3.18	Fe	9.82	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K					0																																																																																																		See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153527	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . no structural transition. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.28Fe9.72As18	Ca	10	Pt	3.28	Fe	9.72	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K		6					6																																																																																																See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153528	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . no structural transition. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.41Fe9.59As18	Ca	10	Pt	3.41	Fe	9.59	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K		7.38					7.38																																																																																																See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153529	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . no structural transition. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.42Fe9.58As18	Ca	10	Pt	3.42	Fe	9.58	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K		8.78					8.78																																																																																																See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153530	PRB085020504	In-plane London [penet] measured by TDR, but values not shown . no structural transition. At low temp, d[penet] = A*T^n.	Ca10(Pt3As8)[(Fe2-xPtx)As2]5	Ca10Pt3.97Fe9.03As18	Ca	10	Pt	3.97	Fe	9.03	As	18																3	2012																										Ca-10-3-8																			Ca-10-3-8	K		10.5					10.5																																																																																																See Angew.Chem.Int.Ed., 50(2011)9195					Doping-dependent superconducting gap anisotropy in the two-dimensional pnictide Ca10(Pt3As8)[(Fe1-xPtx)2As2]5			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)020504	K. Cho,M. A. Tanatar,H. Kim,W. E. Straszheim,N. Ni,R. J. Cava,R. Prozorov		
153531	PRB085024511	T<SDW> = 189K	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2012								19.4																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																				uV/K	6.87			MTP153531																								FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153532	PRB085024511	T<SDW> = 178 K	Eu1-xKxFe2As2	Eu0.887K0.113Fe2As2	Eu	0.887	K	0.113	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0			MPH153532																																																																																													FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153533	PRB085024511	T<SDW> = 162 K	Eu1-xKxFe2As2	Eu0.784K0.216Fe2As2	Eu	0.784	K	0.216	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																																																FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153534	PRB085024511		Eu1-xKxFe2As2	Eu0.64K0.36Fe2As2	Eu	0.64	K	0.36	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		27.6					27.6																																																																																														FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153535	PRB085024511		Eu1-xKxFe2As2	Eu0.56K0.44Fe2As2	Eu	0.56	K	0.44	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		28.7					28.7																																																																		uV/K	22.3			MTP153535																								FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153536	PRB085024511		Eu1-xKxFe2As2	Eu0.51K0.49Fe2As2	Eu	0.51	K	0.49	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		32.5					32.5	MPH153532																																																																																													FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153537	PRB085024511		Eu1-xKxFe2As2	Eu0.48K0.52Fe2As2	Eu	0.48	K	0.52	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		30					30																																																																																														FeAs,KAs,Fe,Eu		self flux method. mixture - sealed in Ta crucible (Ar) - heat to 1100C (50C/h) - hold (1100C,4h) - cool to 900C (3C/h) - quick cool to RT					Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153538	PRB085024511	T<SDW> = 150 K.	EuFe(As1-xPx)2	Eu1Fe2As1.89P0.11	Eu	1	Fe	2	As	1.89	P	0.11																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																				uV/K	3.94			MTP153538																															Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153539	PRB085024511	SC for 0.16 < x < 0.22 in EuFe2(As1-xPx)2	EuFe(As1-xPx)2	Eu1Fe2As1.58P0.42	Eu	1	Fe	2	As	1.58	P	0.42																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		29					29																																																																		uV/K	-0.24			MTP153539																															Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153540	PRB085024511		EuFe(As1-xPx)2	Eu1Fe2As1.48P0.52	Eu	1	Fe	2	As	1.48	P	0.52																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																				uV/K	-2.65			MTP153540																															Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153541	PRB085024511		EuFe(As1-xPx)2	Eu1Fe2As1.28P0.72	Eu	1	Fe	2	As	1.28	P	0.72																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																				uV/K	-7.1			MTP153541																															Signatures of quantum criticality in hole-doped and chemically pressurized EuFe2As2 single crystals			Physikalisches Institut, Georg-August-Universitat Gottingen, D-37077 Gottingen, Germany	Phys.Rev.B, 85(2012)024511	Jannis Maiwald,H. S. Jeevan,Philipp Gegenwart		
153542	PRB085024525	La-content by WDS. Tc, Tn measured by Res and SUS. Xc(AFM disappears) = 0.14.	Ca1-xLaxFe2As2	Ca0.895La0.105Fe2As2	Ca	0.895	La	0.105	Fe	2	As	2																3	2012								97																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																																																		self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153543	PRB085024525	La-content by WDS. Tc, Tn measured by Res and SUS. Xc(AFM disappears) = 0.14.	Ca1-xLaxFe2As2	Ca0.835La0.165Fe2As2	Ca	0.835	La	0.165	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		41.2					41.2	MPH153543																																																																																															self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153544	PRB085024525	La-content by WDS. Tc, Tn measured by Res and SUS. Xc(AFM disappears) = 0.14.	Ca1-xLaxFe2As2	Ca0.719La0.281Fe2As2	Ca	0.719	La	0.281	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		31.7					31.7																																																																																																self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153545	PRB085024525	Ce-content by WDS. Tc, Tn measured by Res and SUS. Xc(AFM disappears) = 0.14.	Ca1-xCexFe2As2	Ca0.88Ce0.12Fe2As2	Ca	0.88	Ce	0.12	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		33.2					33.2	MPH153545																																																																																															self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153546	PRB085024525	Ce-content by WDS. Tc, Tn measured by Res and SUS. Xc(AFM disappears) = 0.14.	Ca1-xCexFe2As2	Ca0.78Ce0.22Fe2As2	Ca	0.78	Ce	0.22	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		36.2					36.2																																																																																																self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153547	PRB085024525		Ca1-xPrxFe2As2	Ca0.956Pr0.044Fe2As2	Ca	0.956	Pr	0.044	Fe	2	As	2																3	2012								133																		AB2C2		ThCr2Si2	I4/mmm		A	3.9047		11.6557											Fe-122, XRD at 250 K.	K					0			MPH153547																																																																																															self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153548	PRB085024525		Ca1-xPrxFe2As2	Ca0.902Pr0.098Fe2As2	Ca	0.902	Pr	0.098	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		40					40																																																																																																self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153549	PRB085024525		Ca1-xPrxFe2As2	Ca0.858Pr0.142Fe2As2	Ca	0.858	Pr	0.142	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		45.3					45.3																																																																																																self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153550	PRB085024525		Ca1-xNdxFe2As2	Ca0.923Nd0.077Fe2As2	Ca	0.923	Nd	0.077	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		41.8					41.8	MPH153550																																																																																															self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153551	PRB085024525		Ca1-xNdxFe2As2	Ca0.906Nd0.094Fe2As2	Ca	0.906	Nd	0.094	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9022		11.5908											Fe-122, XRD at 250 K.	K		19.3					19.3																																																																																																self-flux method					Structural collapse and superconductivity in rare-earth-doped CaFe2As2			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 85(2012)024525	S. R. Saha,N. P. Butch,T. Drye,J. Magill,S. Ziemak,K. Kirshenbaum,P. Y. Zavalij,J. W. Lynn,J. Paglione		
153552	PRB085024526	RRR = 30. Thermopower measured for H//b upto 16 T.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2012							2.8																			ABC		TiNiSi																		K		0.6					0.6																																																																		uV/K				MTP153552																										Czhochralski method					Thermoelectricity of the ferromagnetic superconductor UCoGe			Laboratoire National des Champs Magnetiques Intenses, UPR 3228, CNRS-INSA-UJF-UPS, F-31400 Toulouse, France	Phys.Rev.B, 85(2012)024526	Liam Malone,Ludovic Howald,Alexandre Pourret,Dai Aoki,Valentin Taufour,Georg Knebel,Jacques Flouquet		
153553	PRB085024536	in-plane R and Hall effect measured.	BaFe2-xRuxAs2	Ba1Fe1.55Ru0.45As2	Ba	1	Fe	1.55	Ru	0.45	As	2																3	2012								37.8																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		8.18					8.18	MPH153553																																																																																															flux method using FeAs, RuAs flux.					Evolution of transport properties of BaFe2-xRuxAs2 in a wide range of isovalent Ru substitution			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B, 85(2012)024536	M. J. Eom,S. W. Na,C. Hoch,R. K. Kremer,J. S. Kim		
153554	PRB085024536	in-plane R and Hall effect measured.	BaFe2-xRuxAs2	Ba1Fe1.32Ru0.68As2	Ba	1	Fe	1.32	Ru	0.68	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		14.5					14.5																																																																																																flux method using FeAs, RuAs flux.					Evolution of transport properties of BaFe2-xRuxAs2 in a wide range of isovalent Ru substitution			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B, 85(2012)024536	M. J. Eom,S. W. Na,C. Hoch,R. K. Kremer,J. S. Kim		
153555	PRB085024536	in-plane R and Hall effect measured.	BaFe2-xRuxAs2	Ba1Fe1.2Ru0.8As2	Ba	1	Fe	1.2	Ru	0.8	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		5.02					5.02																																																																																																flux method using FeAs, RuAs flux.					Evolution of transport properties of BaFe2-xRuxAs2 in a wide range of isovalent Ru substitution			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B, 85(2012)024536	M. J. Eom,S. W. Na,C. Hoch,R. K. Kremer,J. S. Kim		
153556	PRB085024536	in-plane R and Hall effect measured.	BaFe2-xRuxAs2	Ba1Fe1.68Ru0.32As2	Ba	1	Fe	1.68	Ru	0.32	As	2																3	2012								74.2																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					0																																																																									uOhm.cm								26.5				120													flux method using FeAs, RuAs flux.					Evolution of transport properties of BaFe2-xRuxAs2 in a wide range of isovalent Ru substitution			Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.B, 85(2012)024536	M. J. Eom,S. W. Na,C. Hoch,R. K. Kremer,J. S. Kim		
153557	PRB085024538	(dC/gamma*Tc) = 1.20.	SrNi2Ge2	Sr1Ni2Ge2	Sr	1	Ni	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.181		10.251											Fe-122	K	0.87		0.92				0.895																																																					MSP153557			mJ/mol.K2	15.5	SP-heat	175	SP-heat																																				two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153558	PRB085024538	grain size (1-10 um), aligned along c-axis. H//c	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.42		10.104											Fe-122	K				3.12			3.12											Oe	M-H						44	2	T	M(T)						0.1	2																																																																				two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153559	PRB085024538		SrCo2Ge2	Sr1Co2Ge2	Sr	1	Co	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.071		10.683											Fe-122	K					2																																																																																																		two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153560	PRB085024538		SrRh2Ge2	Sr1Rh2Ge2	Sr	1	Rh	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.193		10.724											Fe-122	K					2																																																																																																		two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153561	PRB085024538	TCFIG shows Tc(x) for Sr(Pd1-xNix)2Ge2	Sr(Pd1-xNix)2Ge2	Sr1Pd1.8Ni0.2Ge2	Sr	1	Pd	1.8	Ni	0.2	Ge	2																1	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				3.1			3.1	MTC153561																																																																																															two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153562	PRB085024538	TCFIG shows Tc(x) for Sr(Pd1-xRhx)2Ge2	Sr(Pd1-xRhx)2Ge2	Sr1Pd1.8Rh0.2Ge2	Sr	1	Pd	1.8	Rh	0.2	Ge	2																1	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				2.92			2.92	MTC153561																																																																																															two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153563	PRB085024538	TCFIG shows Tc(x) for Sr(Pd1-xCox)2Ge2	Sr(Pd1-xCox)2Ge2	Sr1Pd1.94Co0.06Ge2	Sr	1	Pd	1.94	Co	0.06	Ge	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				2.58			2.58	MTC153561																																																																																															two step arc melting . 1st, (T,T')Ge were made by arc melting. 2nd, melted with Sr by arc melting					Superconductivity and structural variation of the electron-correlated layer systems Sr(Pd1-xTx)2Ge2 (T = Co, Ni, Rh; 0=< x =< 1)			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, Republic of China	Phys.Rev.B, 85(2012)024538	J. W. Wang,I. A. Chen,T. L. Hung,Y. B. You,H. C. Ku,Y. Y. Hsu,J. C. Ho,Y. Y. Chen		
153564	PRB085054507	atomic compositiond measured by ICP-AES. SUS for H//c	K0.8Fe1.7S2	K0.8Fe1.7S2	K	0.8	Fe	1.7	S	2																		3	2012								260																		AB2C2		ThCr2Si2	I4/mmm		A	3.7451		13.5782											Fe-122	K					4																																																																																																		Fe2-xS2 and FeSSe firstly prepared, then mixed with K.					Effect of doping on electrical, magnetic, and superconducting properties of KxFe2-yS2			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 85(2012)054507	Jiangang Guo,Xiaolong Chen,Gang Wang,Shifeng Jin,Tingting Zhou,Xiaofang Lai		
153565	PRB085054507	atomic compositiond measured by ICP-AES. Hc2 measured for H//c.	K0.8Fe1.7SSe	K0.8Fe1.7S1Se1	K	0.8	Fe	1.7	S	1	Se	1																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K	24.6		26.3	24.5			24.5										80										T	RES, WHH approx.			13.5					T/K	resistivity			0.74																																																															Fe2-xS2 and FeSSe firstly prepared, then mixed with K.					Effect of doping on electrical, magnetic, and superconducting properties of KxFe2-yS2			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 85(2012)054507	Jiangang Guo,Xiaolong Chen,Gang Wang,Shifeng Jin,Tingting Zhou,Xiaofang Lai		
153566	PRB085054507	atomic compositiond measured by ICP-AES. magnetic prop. for H//c	KFe1.5S2	K1Fe1.5S2	K	1	Fe	1.5	S	2																		3	2012	emu/g.Oe	0.0000261	emu.K/g.Oe	0.000256			-112	43																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					4																																																																																																		Fe2-xS2 and FeSSe firstly prepared, then mixed with K.					Effect of doping on electrical, magnetic, and superconducting properties of KxFe2-yS2			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 85(2012)054507	Jiangang Guo,Xiaolong Chen,Gang Wang,Shifeng Jin,Tingting Zhou,Xiaofang Lai		
153567	PRB085054517	lattice term in SP (beta=0.37 mJ/mol.K4). Debye-T(RES) = 148 K.	LaNi2Ge2	La1Ni2Ge2	La	1	Ni	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm			4.1859		9.9042											Fe-122	K					1.8																																																										mJ/mol.K2	12.4	SP-heat	297	SP-heat											uOhm.cm							6.8					85													stoichiometric (La,Ni,Ge) were melted in arc furnace, then thoroughly ground and mixed with P.  sealed in evacuated quartz tube, heat(990C,6d)					Structural, thermal, magnetic, and electronic transport properties of the LaNi2(Ge1-xPx)2 system			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)054517	R. J. Goetsch,V. K. Anand,Abhishek Pandey,D. C. Johnston		
153568	PRB085054517	lattice term in SP (beta=0.26 mJ/mol.K4). Debye-T(RES) = 119 K.	LaNi2(Ge1-xPx)2	La1Ni2Ge1.5P0.5	La	1	Ni	2	Ge	1.5	P	0.5																1	2012																										AB2C2		ThCr2Si2	I4/mmm			4.1353		9.8012											Fe-122	K					1.8																																																										mJ/mol.K2	11.27	SP-heat	333.9	SP-heat											uOhm.cm							95.9					189													stoichiometric (La,Ni,Ge) were melted in arc furnace, then thoroughly ground and mixed with P.  sealed in evacuated quartz tube, heat(990C,6d)					Structural, thermal, magnetic, and electronic transport properties of the LaNi2(Ge1-xPx)2 system			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)054517	R. J. Goetsch,V. K. Anand,Abhishek Pandey,D. C. Johnston		
153569	PRB085054517	lattice term in SP (beta=0.194 mJ/mol.K4). Debye-T(RES) = 208 K.	LaNi2(Ge1-xPx)2	La1Ni2Ge1P1	La	1	Ni	2	Ge	1	P	1																1	2012																										AB2C2		ThCr2Si2	I4/mmm			4.0813		9.7424											Fe-122	K					1.8																																																										mJ/mol.K2	9.3	SP-heat	369	SP-heat											uOhm.cm							249.79					401													stoichiometric (La,Ni,Ge) were melted in arc furnace, then thoroughly ground and mixed with P.  sealed in evacuated quartz tube, heat(990C,6d)					Structural, thermal, magnetic, and electronic transport properties of the LaNi2(Ge1-xPx)2 system			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)054517	R. J. Goetsch,V. K. Anand,Abhishek Pandey,D. C. Johnston		
153570	PRB085054517	lattice term in SP (beta=0.159 mJ/mol.K4). Debye-T(RES) = 242 K.	LaNi2(Ge1-xPx)2	La1Ni2Ge0.5P1.5	La	1	Ni	2	Ge	0.5	P	1.5																1	2012																										AB2C2		ThCr2Si2	I4/mmm			4.055		9.7289											Fe-122	K					1.8																																																										mJ/mol.K2	7.4	SP-heat	394	SP-heat											uOhm.cm							191.51					300													stoichiometric (La,Ni,Ge) were melted in arc furnace, then thoroughly ground and mixed with P.  sealed in evacuated quartz tube, heat(990C,6d)					Structural, thermal, magnetic, and electronic transport properties of the LaNi2(Ge1-xPx)2 system			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)054517	R. J. Goetsch,V. K. Anand,Abhishek Pandey,D. C. Johnston		
153571	PRB085054517	Annealed sample. lattice term in SP (beta=0.126 mJ/mol.K4). Debye-T(RES) = 265 K. Res and SUS show occurrence of SC, but not clear  bulk SC or impurity phase.	LaNi2P2	La1Ni2P2	La	1	Ni	2	P	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm			4.0145		9.6471											Fe-122	K			2.1	2.6			2.6																																																								mJ/mol.K2	5.87	SP-heat	426	SP-heat											uOhm.cm							36					1520													stoichiometric (La,Ni,Ge) were melted in arc furnace, then thoroughly ground and mixed with P.  sealed in evacuated quartz tube, heat(990C,6d)					Structural, thermal, magnetic, and electronic transport properties of the LaNi2(Ge1-xPx)2 system			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 85(2012)054517	R. J. Goetsch,V. K. Anand,Abhishek Pandey,D. C. Johnston		
153572	PRB085064504	non-SC Fe1.08Te0.55Se0.45 become SC after O2-annealing. O-content not given. O2-annealing inproved Jc value (maybe precipitates of hexagonal phase.	Fe1.08(Te,Se)Ox	Fe1.08Te0.55Se0.45Ox	Fe	1.08	Te	0.55	Se	0.45															O	x		3	2012																										AB		PbO	P4/nmm																Fe-11	K	11.5	14.5					14.5																																																																																																					Structure of the oxygen-annealed chalcogenide superconductor Fe1.08Te0.55Se0.45Ox			Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 85(2012)064504	Hefei Hu,Jian-Min Zuo,Mao Zheng,James N. Eckstein,Wan Kyu Park,Laura H. Greene,Jinsheng Wen,Zhijun Xu,Zhiwei Lin,Qiang Li,Genda Gu		
153573	PRB085092503	T<SDW> = 167.5 K	Eu1-xLaxFe2As2	Eu0.92La0.08Fe2As2	Eu	0.92	La	0.08	Fe	2	As	2																3	2012								20																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K								MPH153573																																																																																															self-flux method. mixture - alumina crucible - sealed in quartz tube - slow heat to 680C - hold(680C,12h) - heat(1190C,10h) - cool to 900C(4K/h) - FC to RT					Phase diagram as a function of doping level and pressure in the Eu1-xLaxFe2As2 system			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)092503	M. Zhang,J. J. Ying,Y. J. Yan,A. F. Wang,X. F. Wang,Z. J. Xiang,G. J. Ye,P. Cheng,X. G. Luo,Jiangping Hu,X. H. Chen		
153574	PRB085092503	T<SDW> = 102.0 K	Eu1-xLaxFe2As2	Eu0.78La0.22Fe2As2	Eu	0.78	La	0.22	Fe	2	As	2																3	2012								20																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K								MPH153574																																																																																															self-flux method. mixture - alumina crucible - sealed in quartz tube - slow heat to 680C - hold(680C,12h) - heat(1190C,10h) - cool to 900C(4K/h) - FC to RT					Phase diagram as a function of doping level and pressure in the Eu1-xLaxFe2As2 system			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)092503	M. Zhang,J. J. Ying,Y. J. Yan,A. F. Wang,X. F. Wang,Z. J. Xiang,G. J. Ye,P. Cheng,X. G. Luo,Jiangping Hu,X. H. Chen		
153575	PRB085092503	T<SDW> = 84.6 K	Eu1-xLaxFe2As2	Eu0.73La0.27Fe2As2	Eu	0.73	La	0.27	Fe	2	As	2																3	2012								20																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K								MPH153575																																																																																															self-flux method. mixture - alumina crucible - sealed in quartz tube - slow heat to 680C - hold(680C,12h) - heat(1190C,10h) - cool to 900C(4K/h) - FC to RT					Phase diagram as a function of doping level and pressure in the Eu1-xLaxFe2As2 system			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)092503	M. Zhang,J. J. Ying,Y. J. Yan,A. F. Wang,X. F. Wang,Z. J. Xiang,G. J. Ye,P. Cheng,X. G. Luo,Jiangping Hu,X. H. Chen		
153576	PRB085100501	Compositions by x-ray fluorescence. SC parameters obtained by fitting to muon-SR data using s-wave model.	Rb0.77Fe1.61Se2	Rb0.77Fe1.61Se2	Rb	0.77	Fe	1.61	Se	2																		3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				32.6			32.6										100																															A	muon-SR		2580		meV	7.7	5.5																																																Bridgman method					Superconducting properties of single-crystalline AxFe2-ySe2 (A=Rb, K) studied using muon spin spectroscopy			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 85(2012)100501	Z. Shermadini,H. Luetkens,R. Khasanov,A. Krzton-Maziopa,K. Conder,E. Pomjakushina,H-H. Klauss,A. Amato		
153577	PRB085100501	Compositions by x-ray fluorescence. SC parameters obtained by fitting to muon-SR data using s-wave model.	K0.74Fe1.66Se2	K0.74Fe1.66Se2	K	0.74	Fe	1.66	Se	2																		3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				31			31										100																															A	muon-SR		2250		meV	6.3	4.7																																																Bridgman method					Superconducting properties of single-crystalline AxFe2-ySe2 (A=Rb, K) studied using muon spin spectroscopy			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 85(2012)100501	Z. Shermadini,H. Luetkens,R. Khasanov,A. Krzton-Maziopa,K. Conder,E. Pomjakushina,H-H. Klauss,A. Amato		
153578	PRB085100502	(Pt4-0.246As8) sample. Hc2 using rf-[penet] measurement in pulsed field. Hc2 has upward curvature, not explained one-gap WHH. Anisotropy factor = 7(Tc), =1 (zero K).	Ca10(Pt3.754As8)((Fe1.94Pt0.06)2As2)5	Ca10Pt4.054Fe9.7As18	Ca	10	Pt	4.054	Fe	9.7	As	18																3	2012																											2		P4/n																Ca-10-4-8	K				26.5			26.5																				T	rf-penet, WHH		132	24										MHC153578																																																														See Proc.Natl.Acad.Sci.USA, 108(2011)E1019					Anisotropic Hc2 up to 92 T and the signature of multiband superconductivity in Ca10(Pt4As8)((Fe1-xPtx)2As2)5			National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 85(2012)100502	Eundeok Mun,Ni Ni,Jared M. Allred,Robert J. Cava,Oscar Ayala,Ross D. McDonald,Neil Harrison,Vivien S. Zapf		
153579	PRB085140509	pseudogap phase transition temperature T<PG> = 409 K.	Ru1-xRhxP	Ru0.7Rh0.3P1	Ru	0.7	Rh	0.3	P	1																		1	2012																										AB	3	MnP	Pnma																	K		1.13					1.13																																																																																																solid state reaction. mixture - SIN((580C,10h) + (1050C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153580	PRB085140509		Ru1-xRhxP	Ru0.55Rh0.45P1	Ru	0.55	Rh	0.45	P	1																		1	2012																										AB	3	MnP	Pnma																	K				3.6			3.6	MTC153580																																																																																															solid state reaction. mixture - SIN((580C,10h) + (1050C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153581	PRB085140509		Ru1-xRhxP	Ru0.4Rh0.6P1	Ru	0.4	Rh	0.6	P	1																		1	2012																										AB	3	MnP	Pnma																	K		1.27					1.27																																																																																																solid state reaction. mixture - SIN((580C,10h) + (1050C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153582	PRB085140509	pseudogap phase transition temperature T<PG> = 155 K.	Ru1-xRhxAs	Ru0.86Rh0.14As1	Ru	0.86	Rh	0.14	As	1																		1	2012																										AB	3	MnP	Pnma																	K		0.75					0.75																																																																																																solid state reaction. mixture - SIN((580C,10h) + (950C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153583	PRB085140509		Ru1-xRhxAs	Ru0.77Rh0.23As1	Ru	0.77	Rh	0.23	As	1																		1	2012																										AB	3	MnP	Pnma																	K		1.88					1.88	MTC153583																																																																																															solid state reaction. mixture - SIN((580C,10h) + (950C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153584	PRB085140509		Ru1-xRhxAs	Ru0.58Rh0.42As1	Ru	0.58	Rh	0.42	As	1																		1	2012																										AB	3	MnP	Pnma																	K		0.68					0.68																																																																																																solid state reaction. mixture - SIN((580C,10h) + (950C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153585	PRB085140509		RuSb	Ru1Sb1	Ru	1	Sb	1																				1	2012																										AB	3	MnP	Pnma																	K		1.2					1.2																																																																																																solid state reaction. mixture - SIN((580C,10h) + (900C,48h) , in quartz tube) - reground - pellet - SIN(72h)					Metal-insulator transition and superconductivity induced by Rh doping in the binary pnictides RuPn (Pn = P, As, Sb)			Department of Advanced Materials, University of Tokyo and JST-TRIP, Kashiwa 277-8561, Japan	Phys.Rev.B, 85(2012)140509	Daigorou Hirai,Tomohiro Takayama,Daisuke Hashizume,Hidenori Takagi		
153586	PRB085144513	lattice term in SP beta= 0.46 mJ/mol.K4	Eu0.5K0.5Fe2As2	Eu0.5K0.5Fe2As2	Eu	0.5	K	0.5	Fe	2	As	2																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.875		13.0309											Fe-122	K				33			33																																																								mJ/mol.K2	260	SP-heat	276	SP-heat											mOhm.cm							6.3																		solid state reaction. mixture - alumina crucible - sealed in Ta crucible in quartz - heat to 600C(50C/h) - keep 12h - reground - pellet - ANN(90C,5d)					Effect of Ni doping on magnetism and superconductivity in Eu0.5K0.5Fe2As2			Department of Physics, Indian Institute of Technology Kanpur, Kanpur 208016, India	Phys.Rev.B, 85(2012)144513	Anupam,V. K. Anand,P. L. Paulose,S. Ramakrishnan,C. Geibel,Z. Hossain		
153587	PRB085144513	lattice term in SP beta= 0.496 mJ/mol.K4. reentrant RES at 6 K.	Eu0.5K0.5(Fe1-xNix)2As2	Eu0.5K0.5Fe1.94Ni0.06As2	Eu	0.5	K	0.5	Fe	1.94	Ni	0.06	As	2														1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.8781		12.8472											Fe-122	K				23			23																																																								mJ/mol.K2	230	SP-heat	269	SP-heat											mOhm.cm							0.68																		solid state reaction. mixture - alumina crucible - sealed in Ta crucible in quartz - heat to 600C(50C/h) - keep 12h - reground - pellet - ANN(90C,5d)					Effect of Ni doping on magnetism and superconductivity in Eu0.5K0.5Fe2As2			Department of Physics, Indian Institute of Technology Kanpur, Kanpur 208016, India	Phys.Rev.B, 85(2012)144513	Anupam,V. K. Anand,P. L. Paulose,S. Ramakrishnan,C. Geibel,Z. Hossain		
153588	PRB085144513	lattice term in SP beta= 0.515 mJ/mol.K4	Eu0.5K0.5(Fe1-xNix)2As2	Eu0.5K0.5Fe1.9Ni0.1As2	Eu	0.5	K	0.5	Fe	1.9	Ni	0.1	As	2														1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.8791		12.8931											Fe-122	K				18			18																																																								mJ/mol.K2	187	SP-heat	265	SP-heat											mOhm.cm							0.42																		solid state reaction. mixture - alumina crucible - sealed in Ta crucible in quartz - heat to 600C(50C/h) - keep 12h - reground - pellet - ANN(90C,5d)					Effect of Ni doping on magnetism and superconductivity in Eu0.5K0.5Fe2As2			Department of Physics, Indian Institute of Technology Kanpur, Kanpur 208016, India	Phys.Rev.B, 85(2012)144513	Anupam,V. K. Anand,P. L. Paulose,S. Ramakrishnan,C. Geibel,Z. Hossain		
153589	PRB085144513	lattice term in SP beta= 0.532 mJ/mol.K4	Eu0.5K0.5(Fe1-xNix)2As2	Eu0.5K0.5Fe1.84Ni0.16As2	Eu	0.5	K	0.5	Fe	1.84	Ni	0.16	As	2														1	2012								8.5																		AB2C2		ThCr2Si2	I4/mmm		A	3.8907		12.6054											Fe-122	K					1.8													mT	M-H				8			1.8	T	resistivity(0.9Rn). WHH	39.3							T/K	resistivity	3.15			MHC153588		A	from Hc2	27																		mJ/mol.K2	236	SP-heat	263	SP-heat											mOhm.cm							54																		solid state reaction. mixture - alumina crucible - sealed in Ta crucible in quartz - heat to 600C(50C/h) - keep 12h - reground - pellet - ANN(90C,5d)					Effect of Ni doping on magnetism and superconductivity in Eu0.5K0.5Fe2As2			Department of Physics, Indian Institute of Technology Kanpur, Kanpur 208016, India	Phys.Rev.B, 85(2012)144513	Anupam,V. K. Anand,P. L. Paulose,S. Ramakrishnan,C. Geibel,Z. Hossain		
153590	PRB085144513	lattice term in SP beta= 0.562 mJ/mol.K4. T<SDW> = 200 K.	Eu0.5K0.5(Fe1-xNix)2As2	Eu0.5K0.5Fe1.76Ni0.24As2	Eu	0.5	K	0.5	Fe	1.76	Ni	0.24	As	2														1	2012								7																		AB2C2		ThCr2Si2	I4/mmm		A	3.8854		12.717											Fe-122	K					1.8																																																										mJ/mol.K2	206	SP-heat	258	SP-heat											mOhm.cm							46																		solid state reaction. mixture - alumina crucible - sealed in Ta crucible in quartz - heat to 600C(50C/h) - keep 12h - reground - pellet - ANN(90C,5d)					Effect of Ni doping on magnetism and superconductivity in Eu0.5K0.5Fe2As2			Department of Physics, Indian Institute of Technology Kanpur, Kanpur 208016, India	Phys.Rev.B, 85(2012)144513	Anupam,V. K. Anand,P. L. Paulose,S. Ramakrishnan,C. Geibel,Z. Hossain		
153591	PRB085144517	gap measured by STM using UHV-cleaved sample.	KxTiNCl	K0.5Ti1N1Cl1	K	0.5	Ti	1	N	1	Cl	1																1	2012																												FeOCl																	alpha-type	K		16					16																																														meV	10.2	15																																																react alpha-TiNCl with KN3					Nanoscale electronic structure of the layered nitride superconductors alpha-KxTiNCl and beta-HfNCly observed by scanning tunneling microscopy and spectroscopy			Graduate School of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Phys.Rev.B, 85(2012)144517	Akira Sugimoto,Kazuhiro Shohara,Toshikazu Ekino,Zhanfeng Zheng,Shoji Yamanaka		
153592	PRB085144517	gap measured by STM using UHV-cleaved sample.	HfNClx	Hf1N1Cl0.7	Hf	1	N	1	Cl	0.7																		1	2012																												SmSI																	beta-type	K		24					24																																														meV	7.5	7.2																																																sample prepared by reacting with K formed by the thermal decomposition of KN3					Nanoscale electronic structure of the layered nitride superconductors alpha-KxTiNCl and beta-HfNCly observed by scanning tunneling microscopy and spectroscopy			Graduate School of Integrated Arts and Sciences, Hiroshima University, Higashi-Hiroshima 739-8521, Japan	Phys.Rev.B, 85(2012)144517	Akira Sugimoto,Kazuhiro Shohara,Toshikazu Ekino,Zhanfeng Zheng,Shoji Yamanaka		
153593	PRB085174505	(dC/gamma*Tc) = 1.73. thermodynamic Hc = 62 mT. GL-parameter = 10. e-ph coupling = 0.70. Energy gap from SP-heat fitting.	YPd2Sn	Y1Pd2Sn1	Y	1	Pd	2	Sn	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.716													Fm3[-]m	K		4.7					4.7											mT	m-H, 2.5% deviate	10							T	resistivity(0.5Rn). WHH	0.9							T/K	resistivity	0.273			MHC153593		A	from Hc2	190			A	GL theory	1960			meV	0.83	4.1								mJ/mol.K2	9.2	SP-heat	210	SP-heat																																				arc-melting in Ar. ANN(750C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153594	PRB085174505	(dC/gamma*Tc) = 1.45.  e-ph coupling = 0.58	LuPd2Sn	Lu1Pd2Sn1	Lu	1	Pd	2	Sn	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.6401													Fm3[-]m	K		2.8					2.8																				T	resistivity(0.5Rn). WHH	0.45														A	from Hc2	270																		mJ/mol.K2	7.4	SP-heat	246	SP-heat																																				arc-melting in Ar. ANN(750C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153595	PRB085174505	e-ph coupling = 0.52	ScPd2Sn	Sc1Pd2Sn1	Sc	1	Pd	2	Sn	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.5021													Fm3[-]m	K		2					2																				T	resistivity(0.5Rn). WHH	0.26														A	from Hc2	360																		mJ/mol.K2	6.6	SP-heat	277	SP-heat																																				arc-melting in Ar. ANN(750C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153596	PRB085174505	(dC/gamma*Tc) = 1.50. thermodynamic Hc = 76 mT. GL-parameter = 17. e-ph coupling = 0.68. Energy gap from SP-heat fitting.	HfPd2Al	Hf1Pd2Al1	Hf	1	Pd	2	Al	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.3728													Fm3[-]m	K		3.66					3.66											mT	m-H, 2.5% deviate	9							T	resistivity(0.5Rn). WHH	1.81														A	from Hc2	130			A	GL theory	2250			meV	0.59	3.74								mJ/mol.K2	7.9	SP-heat	182	SP-heat																																				arc-melting in Ar. ANN(840C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153597	PRB085174505	(dC/gamma*Tc) = 1.02.  e-ph coupling = 0.65. Energy gap from SP-heat fitting.	ZrPd2Al	Zr1Pd2Al1	Zr	1	Pd	2	Al	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.3942													Fm3[-]m	K		3.4					3.4																				T	resistivity(0.5Rn). WHH	2.82														A	from Hc2	110								meV	0.51	3.48								mJ/mol.K2	9	SP-heat	189	SP-heat																																				arc-melting in Ar. ANN(840C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153598	PRB085174505	e-ph coupling = 0.58	HfPd2In	Hf1Pd2In1	Hf	1	Pd	2	In	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.5342													Fm3[-]m	K		2.86					2.86																				T	resistivity(0.5Rn). WHH	1														A	from Hc2	180																		mJ/mol.K2	8.5	SP-heat	243	SP-heat																																				arc-melting in Ar. ANN(840C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153599	PRB085174505	e-ph coupling = 0.55	ZrPd2Al	Zr1Pd2In1	Zr	1	Pd	2	In	1																		1	2012																										ABC2		Heusler	L2<1>	225	A	6.5534													Fm3[-]m	K		2.19					2.19																				T	resistivity(0.5Rn). WHH	0.63														A	from Hc2	230																		mJ/mol.K2	10.9	SP-heat	236	SP-heat																																				arc-melting in Ar. ANN(840C,2w, in evacuated quartz tube) - Q to (-13 K brine					Superconductivity in the Heusler family of intermetallics			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)174505	T. Klimczuk,C. H. Wang,K. Gofryk,F. Ronning,J. Winterlik,G. H. Fecher,J.-C. Griveau,E. Colineau,C. Felser,J. D. Thompson,D. J. Safarik,R. J. Cava		
153600	PRB085174514	Type-1 SC. RRR=14.0. GL(kappa) = 0.23. effective mass = 3.03 m0. (dC/gamma*Tc) = 1.44. e-ph coupling = 0.45. latticeterm in SP (beta)=0.027 mJ/mol.K2. H//a-axis.	ScGa3	Ga3Sc1	Ga	3	Sc	1																				3	2012																										AB3			Pm3[-]m		A	4.0919														K		2.1					2.1																				Oe	M(H), SP	209												MHC153600		um	effective mass	0.26			nm	effective mass	59			meV	0.18		14							mJ/mol.K2	7.03	SP-heat	660	SP-heat																																		Sc(6N),Lu(6N),Ga		self flux method. mixture(Sc(or Lu):Ga = 1:9) - alumina crucible - heat(930 C) - slow cool to 760 C - wrapped in Ta foil - ANN(800C, 1w)					Type-I superconductivity in ScGa3 and LuGa3 single crystals			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 85(2012)174514	E. Svanidze,E. Morosan		
153601	PRB085174514	Type-1 SC. RRR=6.5. GL(kappa) = 0.30. effective mass = 3.49 m0. (dC/gamma*Tc) = 1.44. e-ph coupling = 0.55. latticeterm in SP (beta)=0.621 mJ/mol.K2. H//a-axis.	LuGa3	Ga3Lu1	Ga	3	Lu	1																				3	2012																										AB3			Pm3[-]m		A	4.19														K		2.2					2.2																				Oe	M(H), SP	226												MHC153601		um	effective mass	0.21			nm	effective mass	63			meV	0.17		14							mJ/mol.K2	8.52	SP-heat	232	SP-heat																																		Sc(6N),Lu(6N),Ga		self flux method. mixture(Sc(or Lu):Ga = 1:9) - alumina crucible - heat(930 C) - slow cool to 760 C - wrapped in Ta foil - ANN(800C, 1w)					Type-I superconductivity in ScGa3 and LuGa3 single crystals			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 85(2012)174514	E. Svanidze,E. Morosan		
153602	PRB085174523	Actual composition: Rb0.74Fe1.7Se2 by ICP. Structurl transition at 556 K	Rb0.8Fe2Se2	Rb0.8Fe2Se2	Rb	0.8	Fe	2	Se	2																		3	2012								514																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K	30.7		31.4				31.05																																																																																																(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153603	PRB085174523	Actual composition: Rb0.78Fe1.67Se1.9Te0.095 by ICP	Rb0.8Fe2Se2-xTex	Rb0.8Fe2Se1.9Te0.1	Rb	0.8	Fe	2	Se	1.9	Te	0.1																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K	23		29.5				26.25	MPH153603																																																																																															(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153604	PRB085174523	Actual composition: Rb0.83Fe1.66Se1.8Te0.198 by ICP	Rb0.8Fe2Se2-xTex	Rb0.8Fe2Se1.8Te0.2	Rb	0.8	Fe	2	Se	1.8	Te	0.2																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K	21.6		28.5				25.05																																																																																																(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153605	PRB085174523	Actual composition: Rb0.79Fe1.63Se1.75Te0.210 by ICP	Rb0.8Fe2Se2-xTex	Rb0.8Fe2Se1.75Te0.25	Rb	0.8	Fe	2	Se	1.75	Te	0.25																3	2012								508																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K	17.2		27.2				22.2																																																																																																(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153606	PRB085174523	Actual composition: Rb0.82Fe1.63Se1.7Te0.272 by ICP	Rb0.8Fe2Se2-xTex	Rb0.8Fe2Se1.7Te0.3	Rb	0.8	Fe	2	Se	1.7	Te	0.3																3	2012								506																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			25.5				25.5																																																																																																(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153607	PRB085174523	Actual composition: Rb0.8Fe1.66Se1.6Te0.400 by ICP. Both SC and AFM not observed.	Rb0.8Fe2Se2-xTex	Rb0.8Fe2Se1.6Te0.4	Rb	0.8	Fe	2	Se	1.6	Te	0.4																3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					4																																																																																																		(FeSe,FeTe) mingled with Rb - alumina crucible - sealed in silica ampoule - slowly heat to 1000 C and keep for 5h - heat to 1100C, keep 5h - cool to 800C with 4C/h -FC to RT					Correlation between superconductivity and antiferromagnetism in Rb0.8Fe2-ySe2-xTex single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 85(2012)174523	Dachun Gu,Liling Sun,Qi Wu,Chao Zhang,Jing Guo,Peiwen Gao,Yue Wu,Xiaoli Dong,Xi Dai,Zhongxian Zhao		
153608	PRB085184501	P-induced SC. incomplete SC for P < 1.76 GPa. T<CT> in Fig. means Collapsed tetragonal transition temperature.	Ca0.67Sr0.33Fe2As2	Ca0.67Sr0.33Fe2As2	Ca	0.67	Sr	0.33	Fe	2	As	2																3	2012								200																		AB2C2		ThCr2Si2	I4/mmm		A	3.907		11.988											Fe-122	K		22			0		22	MPH153608																																																																																															flux method					Suppression of magnetism and development of superconductivity within the collapsed tetragonal phase of Ca0.67Sr0.33Fe2As2 under pressure			Condensed Matter and Materials Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 85(2012)184501	J. R. Jeffries,N. P. Butch,K. Kirshenbaum,S. R. Saha,G. Samudrala,S. T. Weir,Y. K. Vohra,J. Paglione		
153609	PRB085184513	filamentary SC(high T) and bulk-SC(low T). Tc in DB shows for R//b. For R//a, Tc(on) = 5K. lattice term inSP beta=0.985 mJ/mol.K4. (dC/gamma*Tc) = 0.99. T<CDW> = 63 K.	ZrTe3	Te3Zr1	Te	3	Zr	1																				3	2012																										AB3																				K	1.5		2.1			0.6	1.8																																																					MSP153609	mJ/mol.K	2.13	mJ/mol.K2	2.15														mOhm.cm												0.3											Zr(4N),Te(5N)		Iodine vapor transport method T-gradient (730 - 680 C)					Mixed bulk-filament nature in superconductivity of the charge-density-wave conductor ZrTe3			Center of Education and Research for Topological Science and Technology, Hokkaido University, Kita 13, Nishi 8 Kita-Ku, Sapporo 060-8628, Japan	Phys.Rev.B, 85(2012)184513	Kazuhiko Yamaya,Shigeru Takayanagi,Satoshi Tanda		
153610	PRB085205105	S, Rxy, SP measured for various P, T. H. Figure shows P-dependence of Tc(SP), Rxy(T=0.75K,H=8T), S(2K,8T) .	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2012																										AB2C2																				K	0.78	0.8					0.8	MTC153610																			T														MHC153610																																uV/K				MTP153610	uOhm.cm							8.3													MRH153610										Heavy fermion superconductor CeCu2Si2 under high pressure: Multiprobing the valence crossover			DPMC-Universite de Geneve, 24 Quai Ernest Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 85(2012)205105	G. Seyfarth,A.-S. Ruetschi,K. Sengupta,A. Georges,D. Jaccard,S. Watanabe,K. Miyake		
153611	PRB085214509	(dC/Tc) = 44.50 mJ/mol.K2. Tc defined as max of (dR/dT).	Ba0.5K0.5Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.014		13.298											Fe-122	K		37.78					37.78																																																																																					m3/C	0.000000001603					MRH153611	n/cm3	3750000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153612	PRB085214509	real conc. x = 0.039 in (Ba,K)(Fe1-xMx)2As2 by EPMA. Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xMnx)2As2	Ba0.5K0.5Fe1.9Mn0.1As2	Ba	0.5	K	0.5	Fe	1.9	Mn	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.984		13.196											Fe-122	K		9.53		13.1			9.53																																																																																					m3/C	0.000000001568					MRH153611	n/cm3	3890000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153613	PRB085214509	real conc. x = 0.032 in (Ba,K)(Fe1-xMx)2As2 by EPMA. (dC/Tc) = 73.49 mJ/mol.K2.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xRux)2As2	Ba0.5K0.5Fe1.9Ru0.1As2	Ba	0.5	K	0.5	Fe	1.9	Ru	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.051		13.419											Fe-122	K		37.14		36.1			37.14																																																																																					m3/C	-0.0000000005444					MRH153613	n/cm3	12100000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153614	PRB085214509	real conc. x = 0.052 in (Ba,K)(Fe1-xMx)2As2 by EPMA. (dC/Tc) = 39.26 mJ/mol.K2.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xCox)2As2	Ba0.5K0.5Fe1.9Co0.1As2	Ba	0.5	K	0.5	Fe	1.9	Co	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.038		13.383											Fe-122	K		30.31		30.1			30.31																																																																																					m3/C	0.0000000006095					MRH153611	n/cm3	9630000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153615	PRB085214509	real conc. x = 0.039 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xNix)2As2	Ba0.5K0.5Fe1.9Ni0.1As2	Ba	0.5	K	0.5	Fe	1.9	Ni	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.99		13.229											Fe-122	K		26.75		26.7			26.75																																																																																					m3/C	0.0000000002431					MRH153611	n/cm3	30600000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153616	PRB085214509	real conc. x = 0.044 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xCux)2As2	Ba0.5K0.5Fe1.9Cu0.1As2	Ba	0.5	K	0.5	Fe	1.9	Cu	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.97		13.05											Fe-122	K		22.29		26.2			22.29																																																																																					m3/C	0.0000000002899					MRH153613	n/cm3	22900000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153617	PRB085214509	real conc. x = 0.040 in (Ba,K)(Fe1-xMx)2As2 by EPMA. (dC/Tc) = 21.66 mJ/mol.K2.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xZnx)2As2	Ba0.5K0.5Fe1.9Zn0.1As2	Ba	0.5	K	0.5	Fe	1.9	Zn	0.1	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.102		13.322											Fe-122	K		30.15		31			30.15																																																																																					m3/C	-0.0000000005621					MRH153613	n/cm3	12100000000000000000000			high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153618	PRB085214509	real conc. x = 0.013 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xMnx)2As2	Ba0.5K0.5Fe1.96Mn0.04As2	Ba	0.5	K	0.5	Fe	1.96	Mn	0.04	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		23.3		20.1			23.3																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153619	PRB085214509	real conc. x = 0.087 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xCux)2As2	Ba0.5K0.5Fe1.8Cu0.2As2	Ba	0.5	K	0.5	Fe	1.8	Cu	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		11.83		13.04			11.83																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153620	PRB085214509	real conc. x = 0.089 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xNix)2As2	Ba0.5K0.5Fe1.8Ni0.2As2	Ba	0.5	K	0.5	Fe	1.8	Ni	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		11.1		12.1			11.1																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153621	PRB085214509	real conc. x = 0.149 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xNix)2As2	Ba0.5K0.5Fe1.7Ni0.3As2	Ba	0.5	K	0.5	Fe	1.7	Ni	0.3	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		5.1		5.01			5.1																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153622	PRB085214509	real conc. x = 0.079 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xZnx)2As2	Ba0.5K0.5Fe1.8Zn0.2As2	Ba	0.5	K	0.5	Fe	1.8	Zn	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		18.3		19.95			18.3																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153623	PRB085214509	real conc. x = 0.139 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xZnx)2As2	Ba0.5K0.5Fe1.7Zn0.3As2	Ba	0.5	K	0.5	Fe	1.7	Zn	0.3	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		7.86		9.07			7.86																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153624	PRB085214509	real conc. x = 0.092 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xCox)2As2	Ba0.5K0.5Fe1.8Co0.2As2	Ba	0.5	K	0.5	Fe	1.8	Co	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		19.95		22.89			19.95																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153625	PRB085214509	real conc. x = 0.147 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xCox)2As2	Ba0.5K0.5Fe1.7Co0.3As2	Ba	0.5	K	0.5	Fe	1.7	Co	0.3	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		13.56		14			13.56																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153626	PRB085214509	real conc. x = 0.063 in (Ba,K)(Fe1-xMx)2As2 by EPMA.  Tc defined as max of (dR/dT).	Ba0.5K0.5(Fe1-xRux)2As2	Ba0.5K0.5Fe1.8Ru0.2As2	Ba	0.5	K	0.5	Fe	1.8	Ru	0.2	As	2														3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		36.5		35.1			36.5																																																																																																high-P synthesis. cleaved in to thin slices along c-axis on MgO substrate					Superconductivity suppression of Ba0.5K0.5Fe2-2xM2xAs2 single crystals by substitution of transition metal (M = Mn, Ru, Co, Ni, Cu, and Zn)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 85(2012)214509	J. Li,Y. F. Guo,S. B. Zhang,J. Yuan,Y. Tsujimoto,X. Wang,C. I. Sathish,Y. Sun,S. Yu,W. Yi,K. Yamaura,E. Takayama-Muromachiu,Y. Shirako,M. Akaogi,H. Kontani		
153627	PRB085214519	sample has two paramag-regions and AFM phase. Abrupt decrease of Tc at around  5GPa related to tha change of hyperfine field (Mossbauer)	Rb0.8Fe2Se2	Rb0.8Fe1.6Se2	Rb	0.8	Fe	1.6	Se	2																		3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				32.4			32.4	MTC153627																																																																																															Bridgman method					Superconductivity and magnetism in Rb0.8Fe1.6Se2 under pressure			Institut fur Anorganische und Analytische Chemie, Johannes Gutenberg-Universitat, D-55099 Mainz, Germany	Phys.Rev.B, 85(2012)214519	Vadim Ksenofontov,Sergey A. Medvedev,Leslie M. Schoop,Gerhard Wortmann,Taras Palasyuk,Vladimir Tsurkan,Joachim Deisenhofer,Alois Loidl,Claudia Felser		
153628	PRB085014514	real H conc. = 0.07. Ce:Fe:As:O:H = 1.01:1:1.00:0.89:0.07 by EPMA.	Ce(O,H)FeAs	Ce1Fe1As1H0.07O0.93	Ce	1	Fe	1	As	1	H	0.07													O	0.93			2012																										ABCD		oxypnictide	P4/nmm																Fe-1111	K				31.3			31.3										2.94																																																																																				CeAs,Fe2As,CeO2,CeD2		CeD2 synthesized by heating Ce in D2. mixture of starting materials and  Ca(OD)2 , NaBD4(as excess D-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153629	PRB085014514	real H conc. = 0.22. Ce:Fe:As:O:H = 1.00:1:1.00:0.74:0.22  by EPMA.	Ce(O,H)FeAs	Ce1Fe1As1H0.2O0.8	Ce	1	Fe	1	As	1	H	0.2													O	0.8			2012																										ABCD		oxypnictide	P4/nmm																Fe-1111	K				45.6			45.6	TC153629									69																																																																																				CeAs,Fe2As,CeO2,CeD2		CeD2 synthesized by heating Ce in D2. mixture of starting materials and  Ca(OD)2 , NaBD4(as excess D-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153630	PRB085014514	real H conc. = 0.32. Ce:Fe:As:O:H = 1.01:1:0.99:0.73:0.32 by EPMA.	Ce(O,H)FeAs	Ce1Fe1As1H0.3O0.7	Ce	1	Fe	1	As	1	H	0.3													O	0.7			2012																										ABCD		oxypnictide	P4/nmm																Fe-1111	K				44.9			44.9										98																																																																																				CeAs,Fe2As,CeO2,CeD2		CeD2 synthesized by heating Ce in D2. mixture of starting materials and  Ca(OD)2 , NaBD4(as excess D-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153631	PRB085014514	real H conc. = 0.40. Ce:Fe:As:O:H = 1.01:1:1.01:0.60:0.40 by EPMA.	Ce(O,H)FeAs	Ce1Fe1As1H0.4O0.6	Ce	1	Fe	1	As	1	H	0.4													O	0.6			2012																										ABCD		oxypnictide	P4/nmm																Fe-1111	K				37.3			37.3										58																																																																																				CeAs,Fe2As,CeO2,CeD2		CeD2 synthesized by heating Ce in D2. mixture of starting materials and  Ca(OD)2 , NaBD4(as excess D-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153632	PRB085014514	real O-conc. = 0.721  by EPMA.	Ce(O,D)FeAs	Ce1Fe1As1D0.3O0.7	Ce	1	Fe	1	As	1	D	0.3													O	0.7			2012																										ABCD		oxypnictide	P4/nmm		A	3.9775		8.6091											Fe-1111	K				47.2			47.2	TC153629									44																																																																																				CeAs,Fe2As,CeO2,CeH2		CeH2 synthesized by heating Ce in H2. mixture of starting materials and  Ca(OH)2 , NaBH4(as excess H-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153633	PRB085014514	real O-conc. = 0.574  by EPMA.	Ce(O,D)FeAs	Ce1Fe1As1D0.4O0.6	Ce	1	Fe	1	As	1	D	0.4													O	0.6			2012																										ABCD		oxypnictide	P4/nmm		A	3.9538		8.5926											Fe-1111	K				43			43										27																																																																																				CeAs,Fe2As,CeO2,CeH2		CeH2 synthesized by heating Ce in H2. mixture of starting materials and  Ca(OH)2 , NaBH4(as excess H-sources) - heat(1473K, 30min, P=2 GPa)					Structural analysis and superconductivity of CeFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, S2-13, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)014514	Satoru Matsuishi,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Shin-ich Shamoto,Ronald I. Smith,Hideo Hosono		
153689	JAC2130509	RRR = 3.	UNi2Al3	U1Ni2.05Al2.98	U	1	Ni	2.05	Al	2.98																			1994																										AB2C3		PrNi2Al3																		K					0.4																																																																																																		arc-melting					Influence of off-stoichiometry on the properties of the heavy fermion superconductors UNi2A13 and UPd2AI3			Institut fur Festkorperphysik Technische Hochschule Darmstadt, D-64289 Darmstadt (Germany)	J.Alloys Compd., 213(1994)509	C. Schank,F. Jahrling,A. Grauel,R. Borth,R. Helfrich,T. Luhmann,P.H.P. Reinders,C. Geibel,F. Steglich		
153700	PRB085214526	remanent Sb-flux(5%). RRR = 186. Type-I SC (Hc2 = Hc). .(dC/gamma*Tc)= 0.85. GL = 0.05. e-ph = 0.51. Hc(by resonant freq) shows 2nd SC phase (Tc=0.41K, Hc=430 Oe)	YbSb2	Yb1Sb2	Yb	1	Sb	2																				3	2012																										AB2	3	ZrSi2	Cmcm		A	4.554	16.715	4.267												K		1.3					1.3										100										Oe	Type-1, Hc,SUS, SP	55												MHC153700		A	effective mass 1.39m0	8260			A	effective mass 1.39m0	400													mJ/mol.K2	3.18	SP	186	SP											uOhm.cm							0.53																Yb(5N),Sb(6N)		(Yb:Sb=1:9) - alumina crucible in quartz ampoule(Ar) - heat to 650 C - hold(650C,4h) - slow cool to 620 C - excess flux was removed.					Type-I superconductivity in YbSb2 single crystals			Department of Physics & Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 85(2012)214526	Liang L. Zhao,Stefan Lausberg,H. Kim,M. A. Tanatar,Manuel Brando,R. Prozorov,E. Morosan		
153701	PRB085224504	BCS-alpha-model. SC parameters calculated from C(T,H) and thermodynamic analysis(entropy conservation). Hc(0)=0.63T, GL=78. (dC/gamma*Tc) = 2.9. Hc2(0) = 224T from WHH.	(Ba,K)(Fe,Co)2As2	Ba0.55K0.45Fe1.95Co0.05As2	Ba	0.55	K	0.45	Fe	1.95	Co	0.05	As	2															2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		32.5					32.5											Oe	Hc2, GL	240							T	C(T,H) measurement,	70							T/K	SP-heat	10					A	Hc(0), GL-eq.	22			A	GL parameter	1700			meV	7.2	5.14	14				MSP153701	mJ/mol.K2	118	mJ/mol.K2	40.5	SP																																						powder metallurgical method					Fully-gapped superconductivity in Ba0.55K0.45Fe1.95Co0.05As2: A low-temperature specific heat study			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 85(2012)224504	K. Gofryk,J. C. Lashley,F. Ronning,D. J. Safarik,F. Weickert,J. L. Smith,A. Leithe-Jasper,W. Schnelle,M. Nicklas,H. Rosner		
153702	PRB085224521	T<STR>, T<SDW> measured by (dR/dT). Tc defined as R=0. no SP-jump at Tc.	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2012																										ABC		PbFCl			A			7.056											Fe-111	K	9.58						9.58																																																																																																NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153703	PRB085224521	T<STR>, T<SDW> measured by (dR/dT).	Na(Fe,Co)As	Na1Fe0.99Co0.01As1	Na	1	Fe	0.99	Co	0.01	As	1																3	2012																										ABC		PbFCl			A			7.0499											Fe-111	K	13.7						13.7																																																																																																NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153704	PRB085224521	T<STR>, T<SDW> measured by (dR/dT).	Na(Fe,Co)As	Na1Fe0.979Co0.021As1	Na	1	Fe	0.979	Co	0.021	As	1																3	2012																										ABC		PbFCl			A			7.0417											Fe-111	K	19.4						19.4																																																																																																NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153705	PRB085224521	SP-heat, beta - 0.23 mJ.mol.K4, delta = -0.0589 mJ/mol.K6. gamma(0) = 1.5 mJ/mol.K2. SP-heat shows two band s-wave SC. (gap size(L) = 3.56, (H) = 6.22 in DB)	Na(Fe,Co)As	Na1Fe0.972Co0.028As1	Na	1	Fe	0.972	Co	0.028	As	1																3	2012																										ABC		PbFCl			A			7.0376											Fe-111	K	20.1						20.1	MPH153705																																															6.22	14							mJ/mol.K2	10.1																																							NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153706	PRB085224521		Na(Fe,Co)As	Na1Fe0.939Co0.061As1	Na	1	Fe	0.939	Co	0.061	As	1																3	2012																										ABC		PbFCl			A			7.021											Fe-111	K	13.4						13.4	MPH153705																																																																																															NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153707	PRB085224521		Na(Fe,Co)As	Na1Fe0.925Co0.075As1	Na	1	Fe	0.925	Co	0.075	As	1																3	2012																										ABC		PbFCl			A			7.0132											Fe-111	K	10.6						10.6																																																																																																NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153708	PRB085224521	not SC	Na(Fe,Co)As	Na1Fe0.891Co0.109As1	Na	1	Fe	0.891	Co	0.109	As	1																3	2012																										ABC		PbFCl			A			6.9871											Fe-111	K					2																																																																																																		NaAs flux method. (NaAs:Fe:Co = 4:1-x:x) - alumina crucible - sealed in Fe crucible(Ar) - heat to 950C (60C/h) - keep(950C,10h) - cool to 600 C(3C/h)					Phase diagram and calorimetric properties of NaFe1-xCoxAs			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224521	A. F. Wang,X. G. Luo,Y. J. Yan,J. J. Ying,Z. J. Xiang,G. J. Ye,P. Cheng,Z. Y. Li,W. J. Hu,X. H. Chen		
153709	PRB085224527	not SC. Fe-plane distance d=10.066 A..	Ca10(Pt3As8)(Fe2As2)5	Ca10Pt3Fe10As18	Ca	10	Pt	3	Fe	10	As	18																3	2012																																													10-3-8 phase	K					2																																																																									mOhm.cm												1.92		cm3/C	0.00196						MRH153709		CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153710	PRB085224527	Fe-plane distance d=10.147 A.	Ca10(Pt3As8)((Fe1-xPtx)2As2)5	Ca10Pt3.213Fe9.787As18	Ca	10	Pt	3.213	Fe	9.787	As	18																3	2012																															A	8.7608	8.7551	10.6831											10-3-8 phase. triclinic, alpha=94.6823,beta=104.2267,gamma=89.9874	K				4.3			4.3										5																																																																											cm3/C	0.0054						MRH153710		CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153711	PRB085224527	Fe-plane distance d=10.221 A.	Ca10(Pt3As8)((Fe1-xPtx)2As2)5	Ca10Pt3.474Fe9.526As18	Ca	10	Pt	3.474	Fe	9.526	As	18																3	2012																																													10-3-8 phase	K	11.6	11.85	13.52	11.1			11.85										30																								MHC153711																																					mOhm.cm												1.11											CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153712	PRB085224527	anisotropy(Hc2) = 10. Fe-plane distance d=10.25 A.	Ca10(Pt3As8)((Fe1-xPtx)2As2)5	Ca10Pt3.53Fe9.47As18	Ca	10	Pt	3.53	Fe	9.47	As	18																3	2012																																													10-3-8 phase	K	13.6	15.8	20	13.6			15.8	MTC153712									80										T	RES (0.5Rn), WHH		143.4	14.13										MHC153712																																					mOhm.cm												0.882		cm3/C	0.00218						MRH153712		CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153713	PRB085224527	Fe-plane distance d=10.252 A.	Ca10(Pt3As8)((Fe1-xPtx)2As2)5	Ca10Pt3.617Fe9.383As18	Ca	10	Pt	3.617	Fe	9.383	As	18																3	2012																																													10-3-8 phase	K	13.6			13.6			13.6										100																																																																																				CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153714	PRB085224527		Ca10(Pt3As8)((Fe1-xPtx)2As2)5	Ca10Pt3.981Fe9.019As18	Ca	10	Pt	3.981	Fe	9.019	As	18																3	2012																																													10-3-8 phase	K				7.49			7.49																																																																							mOhm.cm												0.694		cm3/C	0.00201						MRH153714		CaAs,FeAs,Pt		mixture(CaAs:FeAs:Pt=2:2:(0.6+x)) - alumina crucible - sealed in quartz tube - heat(1323K,75h) - cool to 1173K (4.5K/h) - FC to RT					Transport properties and electronic phase diagram of single-crystalline Ca10(Pt3As8)((Fe1-xPtx)2As2)5			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 85(2012)224527	Z. J. Xiang,X. G. Luo,J. J. Ying,X. F. Wang,Y. J. Yan,A. F. Wang,P. Cheng,G. J. Ye,X. H. Chen		
153715	PRB086020501	not SC. Tn(from Fe and Ce moment) = 145 K and 4 K	CeFeAsO	Ce1Fe1As1O1	Ce	1	Fe	1	As	1															O	1		3	2012								145																		ABCD		oxypnictide																	Fe-1111	K					1.8																																																																																																		See Phys.Rev.B, 81(2010)134525					Ferromagnetism and superconductivity in CeFeAs1-xPxO (0 =< x =<40%)			Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B, 86(2012)020501	A. Jesche,T. Forster,J. Spehling,M. Nicklas,M. de Souza,R. Gumeniuk,H. Luetkens,T. Goltz,C. Krellner,M. Lang,J. Sichelschmidt,H.-H. Klauss,C. Geibel		
153716	PRB086020501	Tn(from Fe and Ce moment) = 40 K and 4 K. Curie-T ( from Ce-moment) = 5 K. dL(10-100K)/L(100K) = -6.9 E-4 by thermal expansion.	CeFe(As,P)O	Ce1Fe1As0.7P0.3O1	Ce	1	Fe	1	As	0.7	P	0.3													O	1		3	2012							5	40																		ABCD		oxypnictide																	Fe-1111	K		4					4																																																																																																See Phys.Rev.B, 81(2010)134525					Ferromagnetism and superconductivity in CeFeAs1-xPxO (0 =< x =<40%)			Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B, 86(2012)020501	A. Jesche,T. Forster,J. Spehling,M. Nicklas,M. de Souza,R. Gumeniuk,H. Luetkens,T. Goltz,C. Krellner,M. Lang,J. Sichelschmidt,H.-H. Klauss,C. Geibel		
153717	PRB086020501	not SC. Curie-T ( from Ce-moment) = 5 K.	CeFePO	Ce1Fe1P1O1	Ce	1	Fe	1	P	1															O	1		3	2012							1																			AB2C3		oxypnictide																	Fe-1111	K					1.8													Oe					70			2.6																																																																													See Phys.Rev.B, 81(2010)134525					Ferromagnetism and superconductivity in CeFeAs1-xPxO (0 =< x =<40%)			Max Planck Institute for Chemical Physics of Solids, D-01187 Dresden, Germany	Phys.Rev.B, 86(2012)020501	A. Jesche,T. Forster,J. Spehling,M. Nicklas,M. de Souza,R. Gumeniuk,H. Luetkens,T. Goltz,C. Krellner,M. Lang,J. Sichelschmidt,H.-H. Klauss,C. Geibel		
153718	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	2012			comment	0.00403	nyu-B/mol	0.12	-7.025																			AB2C3		LaRu3Si2			A	5.6748		3.5569												K		7.18					7.18																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153719	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	La(Ru,Fe)3Si2	La1Ru2.97Fe0.03Si2	La	1	Ru	2.97	Fe	0.03	Si	2																1	2012			comment	0.00613	nyu-B/mol	0.76	-4.553																			AB2C3		LaRu3Si2			A	5.6765		3.5595												K		6.22					6.22																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153720	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	La(Ru,Fe)3Si2	La1Ru2.94Fe0.06Si2	La	1	Ru	2.94	Fe	0.06	Si	2																1	2012			comment	0.0188	nyu-B/mol	1.4	-5.097																			AB2C3		LaRu3Si2			A	5.6755		3.5601												K		4.58					4.58	MTC153720																																																																																													La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153721	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	La(Ru,Fe)3Si2	La1Ru2.925Fe0.075Si2	La	1	Ru	2.925	Fe	0.075	Si	2																1	2012			comment	0.02304	nyu-B/mol	1.42	-4.89																			AB2C3		LaRu3Si2			A	5.6739		3.5577												K		3.12					3.12																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153722	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	La(Ru,Fe)3Si2	La1Ru2.9175Fe0.0825Si2	La	1	Ru	2.9175	Fe	0.0825	Si	2																1	2012			comment	0.02723	nyu-B/mol	1.51	-4.628																			AB2C3		LaRu3Si2			A	5.6747		3.5588												K		2.51					2.51																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153723	PRB086024513	magnetic properties using Curie-Weiss , Curie constant in emu.K/mol.Oe.	La(Ru,Fe)3Si2	La1Ru2.91Fe0.09Si2	La	1	Ru	2.91	Fe	0.09	Si	2																1	2012																										AB2C3		LaRu3Si2			A	5.6738		3.559												K		0					0																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153724	PRB086024513		La(Ru,Co)3Si2	La1Ru2.94Co0.06Si2	La	1	Ru	2.94	Co	0.06	Si	2																1	2012			comment	0.00883	nyu-B/mol	0.81	-5.596																			AB2C3		LaRu3Si2			A	5.6734		3.5568												K		6.62					6.62																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153725	PRB086024513		La(Ru,Co)3Si2	La1Ru2.85Co0.15Si2	La	1	Ru	2.85	Co	0.15	Si	2																1	2012			comment	0.01046	nyu-B/mol	0.59	-12.608																			AB2C3		LaRu3Si2			A	5.6722		3.5555												K		6.45					6.45	MTC153725																																																																																													La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153726	PRB086024513		La(Ru,Co)3Si2	La1Ru2.76Co0.24Si2	La	1	Ru	2.76	Co	0.24	Si	2																1	2012			comment	0.00984	nyu-B/mol	0.45	-9.307																			AB2C3		LaRu3Si2			A	5.6635		3.5536												K		6.04					6.04																																																																																														La(3N),Fe(4N),Co(4N),Ru(4N),Si(4N)		arc-melting. To avoid the formation of LaRu2Si2 phase, excess Ru (about 15 %) are added.					Distinct behaviors of suppression to superconductivity in LaRu3Si2 induced by Fe and Co dopants			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)024513	Sheng Li,Jian Tao,Xiangang Wan,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153727	PRB086024516	Basal plane distance d = 7.7979 A	alpha-TiNCl	Ti1N1Cl1	Ti	1	N	1	Cl	1																			2012																													Pmmm			3.937	3.2548	7.7979											alpha-ATiNCl	K					0																																																																																																		Alkali metal intercalation was carried out using 0.1 M alkali-metal naphthalene solutions in tetrahydrofuran (A-Naph/THF)					Superconductivity in electron-doped layered TiNCl with variable interlayer coupling			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Phys.Rev.B, 86(2012)024516	Shuai Zhang,Masashi Tanaka,Shoji Yamanaka		
153728	PRB086024516	Na-intercalated TiNCl. Na-content by ICP. Basal plane distance d = 8.442 A.  Anisotropy (cohere) = 1.2.	alpha-Na1.16TiNCl	Na0.16Ti1N1Cl1	Na	0.16	Ti	1	N	1	Cl	1																	2012																													Bmmb			4.0187	3.2738	16.884											alpha-ATiNCl	K	10		18				14										100																								MHC153728		A	from (dHc2/dT)		33	28																																																								Alkali metal intercalation was carried out using 0.1 M alkali-metal naphthalene solutions in tetrahydrofuran (A-Naph/THF)					Superconductivity in electron-doped layered TiNCl with variable interlayer coupling			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Phys.Rev.B, 86(2012)024516	Shuai Zhang,Masashi Tanaka,Shoji Yamanaka		
153729	PRB086024516	Na(THF) intercalated TiNCl. M=(THF)y: THF=tetrahydrofuran. Na-content by ICP. Basal plane distance d = 13.105 A.  Anisotropy (cohere) = 1.5.	alpha-Na1.16(THF)yTiNCl	Na0.16M1Ti1N1Cl1	Na	0.16	M	1	Ti	1	N	1	Cl	1															2012																													Immm			3.9687	3.2694	26.21											alpha-ATiNCl	K			10.2				10.2										60																								MHC153729		A	from (dHc2/dT)		55	35																																																								Alkali metal intercalation was carried out using 0.1 M alkali-metal naphthalene solutions in tetrahydrofuran (A-Naph/THF)					Superconductivity in electron-doped layered TiNCl with variable interlayer coupling			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Phys.Rev.B, 86(2012)024516	Shuai Zhang,Masashi Tanaka,Shoji Yamanaka		
153730	PRB086024516	Na(PC) intercalated TiNCl. M=(PC): PC= propylene carbonate. Na-content by ICP. Basal plane distance d = 20.53 A.	alpha-Na1.16(PC)yTiNCl	Na0.16M1Ti1N1Cl1	Na	0.16	M	1	Ti	1	N	1	Cl	1															2012																													Immm			3.982	3.273	41.07											alpha-ATiNCl	K			7.4				7.4										38																								MHC153730		A	from (dHc2/dT)		84																																																									Alkali metal intercalation was carried out using 0.1 M alkali-metal naphthalene solutions in tetrahydrofuran (A-Naph/THF)					Superconductivity in electron-doped layered TiNCl with variable interlayer coupling			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Phys.Rev.B, 86(2012)024516	Shuai Zhang,Masashi Tanaka,Shoji Yamanaka		
153731	PRB086024524	R not zero at 1.8K. T<CDW> = 202 K, cohere<CDW> = 5.4 A.	Lu2Ir3Si5	Lu2Ir3Si5	Lu	2	Ir	3	Si	5																		1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.915	11.287	5.722												K				5.55			5.55																																																								mJ/mol.K2	7.5	SP	376	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153732	PRB086024524	T<CDW> = 192 K, cohere<CDW> = 6.8 A. Two step SC transition in SUS and RES.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.98Ge0.02	Lu	2	Ir	3	Si	4.98	Ge	0.02																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.917	11.302	5.728												K				6.32			6.32																																																								mJ/mol.K2	8.7	SP	367	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153733	PRB086024524	T<CDW> = 174 K, cohere<CDW> = 9.66 A. Two step SC transition in SUS and RES.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.95Ge0.05	Lu	2	Ir	3	Si	4.95	Ge	0.05																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.924	11.302	5.732												K				6.75			6.75																																																								mJ/mol.K2	9.1	SP	367	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153734	PRB086024524	T<CDW> = 160 K, cohere<CDW> = 11.37 A. Two step SC transition in SUS and RES.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.9Ge0.1	Lu	2	Ir	3	Si	4.9	Ge	0.1																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.926	11.331	5.738												K				7.74			7.74																																																								mJ/mol.K2	9.7	SP	348	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153735	PRB086024524	T<CDW> = 181 K, cohere<CDW> = 13.54 A.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.75Ge0.25	Lu	2	Ir	3	Si	4.75	Ge	0.25																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.91	11.348	5.748												K				6.2			6.2																																																								mJ/mol.K2	8.5	SP	318	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153736	PRB086024524	T<CDW> = 204 K, cohere<CDW> = 14.85 A.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.5Ge0.5	Lu	2	Ir	3	Si	4.5	Ge	0.5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.909	11.389	5.759												K				5.2			5.2																																																								mJ/mol.K2	7.9	SP	299	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153737	PRB086024524	T<CDW> = 214 K, cohere<CDW> = 16.68 A.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4.25Ge0.75	Lu	2	Ir	3	Si	4.25	Ge	0.75																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.854	11.423	5.786												K				4.6			4.6																																																								mJ/mol.K2	6.9	SP	295	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153738	PRB086024524	T<CDW> = 231 K, cohere<CDW> = 23.67 A.	Lu2Ir3(Si,Ge)5	Lu2Ir3Si4Ge1	Lu	2	Ir	3	Si	4	Ge	1																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.709	11.562	5.984												K				3.6			3.6																																																								mJ/mol.K2	5.7	SP	284	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153739	PRB086024524	T<CDW> = 220 K, cohere<CDW> = 9.01 A.	Lu2(Ir,Rh)3Si5	Lu2Ir2.97Rh0.03Si5	Lu	2	Ir	2.97	Rh	0.03	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.881	11.264	5.709												K			4.6				4.6																																																								mJ/mol.K2	6.3	SP	310	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153740	PRB086024524	T<CDW> = 233 K, cohere<CDW> = 10 A.	Lu2(Ir,Rh)3Si5	Lu2Ir2.91Rh0.09Si5	Lu	2	Ir	2.91	Rh	0.09	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.76	11.251	5.661												K			3.8				3.8																																																								mJ/mol.K2	5.7	SP	3.9	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153741	PRB086024524	T<CDW> = 262 K, cohere<CDW> = 8.61 A.	Lu2(Ir,Rh)3Si5	Lu2Ir2.7Rh0.3Si5	Lu	2	Ir	2.7	Rh	0.3	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.711	11.173	5.652												K			3.1				3.1																																																								mJ/mol.K2	4.6	SP	297	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153742	PRB086024524	T<CDW> = 283 K, cohere<CDW> = 11.16 A.	Lu2(Ir,Rh)3Si5	Lu2Ir2.4Rh0.6Si5	Lu	2	Ir	2.4	Rh	0.6	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.666	11.171	5.645												K			2.5				2.5																																																								mJ/mol.K2	3.6	SP	3.9	SP																																		5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153743	PRB086024524	not SC above 1.8 K. no SDW	Lu2(Ir,Rh)3Si5	Lu2Ir2.1Rh0.9Si5	Lu	2	Ir	2.1	Rh	0.9	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.561	11.161	5.622												K					1.8																																																																																																5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153744	PRB086024524	T<CDW> = 182 K,	(Lu,Sc)2Ir3Si5	Lu1.96Sc0.04Ir3Si5	Lu	1.96	Sc	0.04	Ir	3	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.898	11.167	5.684												K			2.8				2.8																																																																																														5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153745	PRB086024524	T<CDW> = 174 K,	(Lu,Sc)2Ir3Si5	Lu1.92Sc0.08Ir3Si5	Lu	1.92	Sc	0.08	Ir	3	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.644	10.831	5.656												K			3.1				3.1																																																																																														5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153746	PRB086024524	T<CDW> = 163 K,	(Lu,Sc)2Ir3Si5	Lu1.9Sc0.1Ir3Si5	Lu	1.9	Sc	0.1	Ir	3	Si	5																1	2012																										A2B3C5		U2Co3Si5	Ibam	72	A	9.601	10.801	5.616												K			3.2				3.2																																																																																														5N-Lu,Si,Ge, 4N-Sc,Ir,Rh		arc-melting(seveal times) - wrapped in Ta foil - sealed in quartz tube - ANN(1000C, 10d)					Interplay of superconductivity and charge density wave ordering in pseudoternary alloy compounds: Lu2Ir3(Si1-xGex)5, Lu2(Ir1-xRhx)3Si5, and (Lu1-xScx)2Ir3Si5			Department of Physics, Indian Institute of Technology Guwahati, Guwahati, Assam 781039, India	Phys.Rev.B, 86(2012)024524	N. S. Sangeetha,A. Thamizhavel,C. V. Tomy,Saurabh Basu,A. M. Awasthi,S. Ramakrishnan,D. Pal		
153747	PRB086054502	RRR = 9.3. lattice term in C beta=22.39 mJ/mol.K4. Debye-T = 95.08 K by R(T). (dC/gammma*Tc) = 1.8. Anisotropy = 1.08. e-ph coupling = 0.74	Rh3Bi14	Rh3Bi14	Rh	3	Bi	14																					2012																										A3B14			Fddd		A	6.891	17.388	31.718												K	2.84	2.94	3.04	2.91		0.3	2.94										81	Oe	M-H curve		90	63					T	RES(onset), WHH		1.24	1.34					T/K	RES(onset)		0.601	0.647	MHC153747		A			157	169	A			2730	1660											mJ/mol.K2	8	SP	113.9	SP																																		Rh(3N),Bi(3N)		flux growth method. mixture - alumina crucible covered with quartz wool - sealed in quartz tube - heat(1000C,2h) - cool to 300C (3.5C/h)					Superconducting state in the metastable binary bismuthide Rh3Bi14 single crystals			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 86(2012)054502	Xiao Zhang,Hechang Lei,C. Petrovic		
153748	PRB086054512	Heavy fermion SC. Heavy fermion state for T< 20 K. lattice term in SP beta=1.03 mJ/mol.K4 and delta= 9.3 mJ/mol.K6 for 2 < T < 10K.	KNi2Se2	K1Ni2Se2	K	1	Ni	2	Se	2																		1	2012																										AB2C2		ThCr2Si2			A	3.9098		13.4145											Fe-122	K		0.8					0.8																				mT	SP, WHH	50												MHC153748		A	from Hc2	800																		mJ/mol.K2	44	SP	211	SP, 2 <T< 10 K											uOhm.cm							2																		See J.Amer.Chem.Soc.134(2012)7750					Mixed-valence-driven heavy-fermion behavior and superconductivity in KNi2Se2			Department of Chemistry, Johns Hopkins University, Baltimore, Maryland 21218, USA	Phys.Rev.B, 86(2012)054512	James R. Neilson,Anna Llobet,Andreas V. Stier,Liang Wu,Jiajia Wen,Jing Tao,Yimei Zhu,Zlatko B. Tesanovic,N. P. Armitage,Tyrel M. McQueen		
153749	PRB086054523	H-content x = 0  , measured by TG-MS. O-content = 0.86 by thermodynamic method	LaOFeAs	La1Fe1As1O0.85	La	1	Fe	1	As	1															O	0.85	0.85	1	2012																										ABCD		oxypnictide	P4/nmm		A	4.032		8.713											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 113.1 degree	K			26	25			25	MTC153749										mT	M-H curve	6.28							T	RES(R=0.5Rn), WHH	35							T/K	RES(R=0.5Rn)	0.25					A	from Hc2	30.6			A	From Hc1	3180													mJ/mol.K2	1.65	SP																																		n/cm3	3920000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153750	PRB086054523	H-content x = 0.14  , measured by TG-MS. O-content = 0.85 by thermodynamic method	La(O,H)FeAs	La1Fe1As1H0.15	La	1	Fe	1	As	1	H	0.15																1	2012																										ABCD		oxypnictide	P4/nmm		A	4.025		8.705											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 112.84 degree	K			28	27.5			27.5											mT	M-H curve	6.19							T	RES(R=0.5Rn), WHH	33.6																																		mJ/mol.K2	1.63	SP																																		n/cm3	4010000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153751	PRB086054523	H-content x = 0.33  , measured by TG-MS. O-content = 0.88 by thermodynamic method	La(O,H)FeAs	La1Fe1As1H0.35	La	1	Fe	1	As	1	H	0.35																1	2012																										ABCD		oxypnictide	P4/nmm		A	4.018		8.698											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 112.47 degree	K			29.5	29			29											mT	M-H curve	6.09							T	RES(R=0.5Rn), WHH	31.5																																		mJ/mol.K2	1.66	SP																																		n/cm3	3970000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153752	PRB086054523	H-content x = 0.52  , measured by TG-MS. O-content = 0.86 by thermodynamic method	La(O,H)FeAs	La1Fe1As1H0.55	La	1	Fe	1	As	1	H	0.55																1	2012																										ABCD		oxypnictide	P4/nmm		A	4.012		8.692											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 111.95 degree	K			30.5	30.5			30.5											mT	M-H curve	5.97							T	RES(R=0.5Rn), WHH	31.9																																		mJ/mol.K2	1.64	SP																																		n/cm3	4120000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153753	PRB086054523	H-content x = 0.66  , measured by TG-MS. O-content = 0.87 by thermodynamic method	La(O,H)FeAs	La1Fe1As1H0.7	La	1	Fe	1	As	1	H	0.7																1	2012																										ABCD		oxypnictide	P4/nmm		A	4.004		8.688											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 111.63 degree	K			32.5	32.5			32.5											mT	M-H curve	5.91							T	RES(R=0.5Rn), WHH	30.2																																		mJ/mol.K2	1.67	SP																																		n/cm3	4180000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153754	PRB086054523	H-content x = 0.82  , measured by TG-MS. O-content = 0.88 by thermodynamic method. Jc(2K) = 5200 A/cm2 using Been model.	La(O,H)FeAs	La1Fe1As1H0.85	La	1	Fe	1	As	1	H	0.85																1	2012																										ABCD		oxypnictide	P4/nmm		A	4.002		8.685											Fe-1111, ZrCuSiAstype, As-Fe-As bonding angle = 111.58 degree	K			35.5	35			35											mT	M-H curve	5.87							T	RES(R=0.5Rn), WHH	32.7							T/K	RES(R=0.5Rn)	0.22					A	from Hc2	31.7			A	From Hc1	3220													mJ/mol.K2	1.69	SP			mW/K				MTHC153755																											n/cm3	4290000000000000000000	LaAs,Fe2O3,La(OH)3,Fe		mixture sealed in Au capsule with h-BN tube inner, then heat (1300C,2h, P=6 GPa)					Continuous critical temperature enhancement with gradual hydrogen doping in LaFeAsO0.85Hx (x = 0-0.85)			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 86(2012)054523	Yanfeng Guo,Xia Wang,Jun Li,Ying Sun,Yoshihiro Tsujimoto,Alexei A. Belik,Yoshitaka Matsushita,Kazunari Yamaura,Eiji Takayama-Muromachi		
153755	PRB086064504	Thermal conductivity, k well fitted to (k/T) = a + b*T^(alpha-1), a=-3 uW/K2. alpha = 2.41. H perpendicular to the (100) plane.	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2012																										A3B4C13		Yb3Rh4Sn13																	Fe-122	K	7.25			6.9		0.2	6.9																				T	RES(zero),extrapolation		7													A	from Hc2	79																																	uOhm.cm								114																	flux method					Nodeless superconductivity in Ca3Ir4Sn13: Evidence from quasiparticle heat transport			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, P. R. China	Phys.Rev.B, 86(2012)064504	S. Y. Zhou,H. Zhang,X. C. Hong,B. Y. Pan,X. Qiu,W. N. Dong,X. L. Li,S. Y. Li		
153756	PRB086094521	not SC. Tc and T<SDW> are measured by thermal expansion coefficient. P-content by EDX.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2012																										AB2C2		ThCr2Si2																	Fe-122	K					0																																																										mJ/mol.K2	4.73	SP																																						self flux method. (Ba:FeP=1:5) - heat(1300C) - slow cool to 1200C (0.3 C/h)					Thermodynamic phase diagram, phase competition, and uniaxial pressure effects in BaFe2(As1-xPx)2 studied by thermal expansion			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 86(2012)094521	A. E. Bohmer,P. Burger,F. Hardy,T. Wolf,P. Schweiss,R. Fromknecht,H. v. Lohneysen,C. Meingast,H. K. Mak,R. Lortz,S. Kasahara,T. Terashima,T. Shibauchi,Y. Matsuda		
153757	PRB086094521	Tc and T<SDW> are measured by thermal expansion coefficient. P-content by EDX. T<SDW> = 48.5 K.	BaFe2(As,P)2	Ba1Fe2As1.5P0.5	Ba	1	Fe	2	As	1.5	P	0.5																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		15.9	19.4				15.9	MPH153757																																																																																															self flux method. (Ba:FeP=1:5) - heat(1300C) - slow cool to 1200C (0.3 C/h)					Thermodynamic phase diagram, phase competition, and uniaxial pressure effects in BaFe2(As1-xPx)2 studied by thermal expansion			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 86(2012)094521	A. E. Bohmer,P. Burger,F. Hardy,T. Wolf,P. Schweiss,R. Fromknecht,H. v. Lohneysen,C. Meingast,H. K. Mak,R. Lortz,S. Kasahara,T. Terashima,T. Shibauchi,Y. Matsuda		
153758	PRB086094521	Tc and T<SDW> are measured by thermal expansion coefficient. P-content by EDX. T<SDW> = 40.9 K.	BaFe2(As,P)2	Ba1Fe2As1.46P0.54	Ba	1	Fe	2	As	1.46	P	0.54																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		24.5	30.3				24.5	MPH153757																																																							mJ/mol.K2	22.4	SP																																						self flux method. (Ba:FeP=1:5) - heat(1300C) - slow cool to 1200C (0.3 C/h)					Thermodynamic phase diagram, phase competition, and uniaxial pressure effects in BaFe2(As1-xPx)2 studied by thermal expansion			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 86(2012)094521	A. E. Bohmer,P. Burger,F. Hardy,T. Wolf,P. Schweiss,R. Fromknecht,H. v. Lohneysen,C. Meingast,H. K. Mak,R. Lortz,S. Kasahara,T. Terashima,T. Shibauchi,Y. Matsuda		
153759	PRB086094521	Tc and T<SDW> are measured by thermal expansion coefficient. P-content by EDX. (dTc/dPa) = 1.4 K/GPa. (dTc/dPc) = -6.3 K/GPa. (dC/Tc) = 38 mJ/mol.K2	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		28.8	28.8				28.8			K/GPa	-3.5																																																				mJ/mol.K2	21.9	SP																																						self flux method. (Ba:FeP=1:5) - heat(1300C) - slow cool to 1200C (0.3 C/h)					Thermodynamic phase diagram, phase competition, and uniaxial pressure effects in BaFe2(As1-xPx)2 studied by thermal expansion			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 86(2012)094521	A. E. Bohmer,P. Burger,F. Hardy,T. Wolf,P. Schweiss,R. Fromknecht,H. v. Lohneysen,C. Meingast,H. K. Mak,R. Lortz,S. Kasahara,T. Terashima,T. Shibauchi,Y. Matsuda		
153760	PRB086100505	not SC. T<STR> = 791 K. lattice distortion due to Ge-Ge dimer.	BaNi2Ge2	Ba1Ni2Ge2	Ba	1	Ni	2	Ge	2																		1	2012																										AB2C2		ThCr2Si2	Pnma		A	8.3888	11.3217	4.293											Fe-122	K					0																																																										mJ/mol.K2	5.69	SP	255	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153761	PRB086100505	not SC.  lattice distortion due to Ge-Ge dimer.	BaNi2(Ge,P)2	Ba1Ni2Ge1.8P0.2	Ba	1	Ni	2	Ge	1.8	P	0.2																1	2012																										AB2C2		ThCr2Si2	Pnma		A	8.3912	11.29	4.2742											Fe-122	K					0																																																										mJ/mol.K2	6.35	SP	244	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153762	PRB086100505	not SC.  lattice distortion due to Ge-Ge dimer.	BaNi2(Ge,P)2	Ba1Ni2Ge1.6P0.4	Ba	1	Ni	2	Ge	1.6	P	0.4																1	2012																										AB2C2		ThCr2Si2	Pnma		A	8.356	11.3184	4.2472											Fe-122	K					0																																																										mJ/mol.K2	6.23	SP	242	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153763	PRB086100505	not SC. T<STR> = 320 K. lattice distortion due to Ge-Ge dimer. Two phases with spaceG (Pnma and I4/mmm)	BaNi2(Ge,P)2	Ba1Ni2Ge1.4P0.6	Ba	1	Ni	2	Ge	1.4	P	0.6																1	2012																										AB2C2		ThCr2Si2	Pnma		A	8.3067	11.3502	4.2038											Fe-122	K					0																																																										mJ/mol.K2	6.59	SP	226	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153764	PRB086100505	not SC. T<STR> = 352-160 K.	BaNi2(Ge,P)2	Ba1Ni2Ge1.2P0.8	Ba	1	Ni	2	Ge	1.2	P	0.8																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1228		11.4438											Fe-122	K					0																																																										mJ/mol.K2	8.52	SP	217	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153765	PRB086100505	T<STR> = 217-88.2 K. (dC/gamma*Tc) = 1.28	BaNi2(Ge,P)2	Ba1Ni2Ge1P1	Ba	1	Ni	2	Ge	1	P	1																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.0806		11.5191											Fe-122	K		0.68					0.68																																																								mJ/mol.K2	8.58	SP	220	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153766	PRB086100505	T<STR> = 140-43.7 K. (dC/gamma*Tc) = 1.44	BaNi2(Ge,P)2	Ba1Ni2Ge0.8P1.2	Ba	1	Ni	2	Ge	0.8	P	1.2																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.0419		11.6027											Fe-122	K		1.38					1.38																																																								mJ/mol.K2	9.61	SP	224	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153767	PRB086100505	(dC/gamma*Tc) = 1.59	BaNi2(Ge,P)2	Ba1Ni2Ge0.6P1.4	Ba	1	Ni	2	Ge	0.6	P	1.4																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.0102		11.8746											Fe-122	K		2.45					2.45																																																								mJ/mol.K2	11.6	SP	221	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153768	PRB086100505	(dC/gamma*Tc) = 1.63	BaNi2(Ge,P)2	Ba1Ni2Ge0.4P1.6	Ba	1	Ni	2	Ge	0.4	P	1.6																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9821		11.7381											Fe-122	K		2.84					2.84	MTC153768																																																							mJ/mol.K2	11.72	SP	253	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153769	PRB086100505	(dC/gamma*Tc) = 1.45	BaNi2(Ge,P)2	Ba1Ni2Ge0.2P1.8	Ba	1	Ni	2	Ge	0.2	P	1.8																1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9563		11.9967											Fe-122	K		2.59					2.59																																																								mJ/mol.K2	12.81	SP	291	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153770	PRB086100505	(dC/gamma*Tc) = 1.11	BaNi2P2	Ba1Ni2P2	Ba	1	Ni	2	P	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9457		11.8117											Fe-122	K		2.55					2.55																																																								mJ/mol.K2	14.43	SP	294	SP																																				2 step reaction. mixture(Ba:Ni:Ge(P) = 1.05:2:2) - SIN(550C,10h + 800C,48h) - mixture(BaNi2Ge2,BaNi2P2) - heat(800C,24h) -  reground - pellet - SIN(800C,24h)					Emergence of superconductivity in BaNi2(Ge1-xPx)2 at a structural instability			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 86(2012)100505	Daigorou Hirai,F. von Rohr,R. J. Cava		
153771	PRB086134501	spacing between HfNCl plane, d = 9.24 A.	beta-HfNCl	Hf1N1Cl1	Hf	1	N	1	Cl	1																			2012																												SmSI	R3[-]m		A	3.58		27.71												K					0																																																																																																		Co-intercalation of Yb and NH3 or THF by liquid ammonia method at RT					Superconductivity in YbxMyHfNCl (M = NH3 and THF)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 86(2012)134501	Guojun Ye,Jianjun Ying,Yajun Yan,Xigang Luo,Peng Cheng,Ziji Xiang,Aifeng Wang,Xianhui Chen		
153772	PRB086134501	M = NH3. spacing between HfNCl plane, d = 11.95 A.	Yb0.2(NH3)xHfNCl	Yb0.2M1Hf1N1Cl1	Yb	0.2	M	1	Hf	1	N	1	Cl	1															2012																												SmSI	P3[-]m		A	3.59		11.95												K		23					23										170										T	SUS,WHH	4							T/K	SUS	0.25			MHC153772																																																														Co-intercalation of Yb and NH3 or THF by liquid ammonia method at RT					Superconductivity in YbxMyHfNCl (M = NH3 and THF)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 86(2012)134501	Guojun Ye,Jianjun Ying,Yajun Yan,Xigang Luo,Peng Cheng,Ziji Xiang,Aifeng Wang,Xianhui Chen		
153773	PRB086134501	M = NH3. spacing between HfNCl plane, d = 13.20 A.	Yb0.3(NH3)xHfNCl	Yb0.3M1Hf1N1Cl1	Yb	0.3	M	1	Hf	1	N	1	Cl	1															2012																												SmSI	P3[-]m		A	3.59		13.2												K		24.8					24.8										145																																																																																						Co-intercalation of Yb and NH3 or THF by liquid ammonia method at RT					Superconductivity in YbxMyHfNCl (M = NH3 and THF)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 86(2012)134501	Guojun Ye,Jianjun Ying,Yajun Yan,Xigang Luo,Peng Cheng,Ziji Xiang,Aifeng Wang,Xianhui Chen		
153774	PRB086134501	M = THF. spacing between HfNCl plane, d = 15.05 A.	Yb0.2(THF)xHfNCl	Yb0.2M1Hf1N1Cl1	Yb	0.2	M	1	Hf	1	N	1	Cl	1															2012																												SmSI	P3[-]m		A	3.59		15.05												K		25.2					25.2	MTC153774		K/GPa	-0.6						160										T	SUS,WHH	6.6							T/K	SUS	0.38			MHC153774																																																														Ybx(NH3)HfNCl - immersing into THF solution for 1-2 days					Superconductivity in YbxMyHfNCl (M = NH3 and THF)			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 86(2012)134501	Guojun Ye,Jianjun Ying,Yajun Yan,Xigang Luo,Peng Cheng,Ziji Xiang,Aifeng Wang,Xianhui Chen		
153775	PRB086144509	[penet] measured by magnetic force microscopy. Anisotropy(H) = 1.85	(Ca,Na)Fe2As2	Ca0.5Na0.5Fe2As2	Ca	0.5	Na	0.5	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		19.4					19.4																													T/K			4	2.2			A	from (dHc2/dT)		28		nm	MFM(magnetic force microscopy)	260																																																										Magnetic penetration-depth measurements of a suppressed superfluid density of superconducting Ca0.5Na0.5Fe2As2 single crystals by proton irradiation			Los Alamos National Laboratory, Los Alamos, New Mexico 87545 USA	Phys.Rev.B, 86(2012)144509	Jeehoon Kim,N. Haberkorn,M. J. Graf,I. Usov,F. Ronning,L. Civale,E. Nazaretski,G. F. Chen,W. Yu,J. D. Thompson,R. Movshovich		
153776	PRB086144509	Proton(3.5 MeV)-irradiated sample. total proton dose = 2 E+16 /cm2. sample thickness = 28 um. [penet] measured by magnetic force microscopy. Anisotropy(H) = 1.65	(Ca,Na)Fe2As2	Ca0.5Na0.5Fe2As2	Ca	0.5	Na	0.5	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		17.8					17.8																													T/K			3.8	2.3	MHC153776		A	from (dHc2/dT)		28		nm	MFM(magnetic force microscopy)	430																																																										Magnetic penetration-depth measurements of a suppressed superfluid density of superconducting Ca0.5Na0.5Fe2As2 single crystals by proton irradiation			Los Alamos National Laboratory, Los Alamos, New Mexico 87545 USA	Phys.Rev.B, 86(2012)144509	Jeehoon Kim,N. Haberkorn,M. J. Graf,I. Usov,F. Ronning,L. Civale,E. Nazaretski,G. F. Chen,W. Yu,J. D. Thompson,R. Movshovich		
153777	PRB085180504		Ca10(Pt3As8)((Fe0.903Pt0.097)2As2)5	Ca10Pt3.97Fe9.03As18	Ca	10	Pt	3.97	Fe	9.03	As	18																3	2012																																													10-3-8 phase	K		11					11																																									nm	MFM(magnetic force microscopy)	1000																																																										Large magnetic penetration depth and thermal fluctuations in a superconducting Ca10(Pt3As8)[(Fe1-xPtx)2As2]5 (x=0.097) single crystal			Los Alamos	Phys.Rev.B, 85(2012)180504	Jeehoon Kim,Fillip Ronning,N.Haberkorm,L.Civale,E.Nazaretski,Ni Ni,R.Cava,J.D.Thompson,R.Movshovich		
153778	PRB086174522	R not to zero at 5 K. Tc defined by SUS. no structural transformation  upto 15 GPa. extrapolated Tc = 0 at P = 4.8 GPa. lattice parameters measured upto 15 GPa.	NaAlSi	Na1Al1Si1	Na	1	Al	1	Si	1																			2012																										ABC		PbFCl	P4/nmm	129	A	4.1247		7.368												K				7.4			7.4	MTC153778																																																																																															mixture(Na:Al:Si=3:1:1) - sealed in Ta tube - encapsuled in glass - heat to 970K with 50 K/h - ANN(970K,3d) - cool to RT with 50K/h - excess Na distilled off in vac.					Effect of pressure on superconductivity in NaAlSi			Graduate School Material Science in Mainz, 55099 Mainz, Germany	Phys.Rev.B, 86(2012)174522	Leslie Schoop,Lukas Muchler,Jennifer Schmitt,Vadim Ksenofontov,Sergey Medvedev,Jurgen Nuss,Frederick Casper,Martin Jansen,R. J. Cava,Claudia Felser		
153779	PRB086174522	not SC	NaAlGe	Na1Al1Ge1	Na	1	Al	1	Ge	1																			2012																										ABC		PbFCl	P4/nmm	129																K					1.8																																																																																																							Effect of pressure on superconductivity in NaAlSi			Graduate School Material Science in Mainz, 55099 Mainz, Germany	Phys.Rev.B, 86(2012)174522	Leslie Schoop,Lukas Muchler,Jennifer Schmitt,Vadim Ksenofontov,Sergey Medvedev,Jurgen Nuss,Frederick Casper,Martin Jansen,R. J. Cava,Claudia Felser		
153780	PRB086180501	K-content by EDX. NMR data shows microscopic coexistence of AFM and NMR. Tc = 16 K and 15.5 K for H//a = 12T and H//c =12T, respectively.	(Ba,K)Fe2As2	Ba0.77K0.23Fe2As2	Ba	0.77	K	0.23	Fe	2	As	2																3	2012								46																		AB2C2		ThCr2Si2																	Fe-122	K				16.5			16.5	MPH153780																																																																																															self flux method					Microscopic coexistence of antiferromagnetic order and superconductivity in Ba0.77K0.23Fe2As2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 86(2012)180501	Z. Li,R. Zhou,Y. Liu,D. L. Sun,J. Yang,C. T. Lin,Guo-qing Zheng		
153781	PRB086180501	K-content by EDX.	(Ba,K)Fe2As2	Ba0.68K0.32Fe2As2	Ba	0.68	K	0.32	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K				38.5			38.5	MPH153780																																																																																															self flux method					Microscopic coexistence of antiferromagnetic order and superconductivity in Ba0.77K0.23Fe2As2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 86(2012)180501	Z. Li,R. Zhou,Y. Liu,D. L. Sun,J. Yang,C. T. Lin,Guo-qing Zheng		
153782	PRB086180501	K-content by EDX.	(Ba,K)Fe2As2	Ba0.39K0.61Fe2As2	Ba	0.39	K	0.61	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K				24.5			24.5																																																																																																self flux method					Microscopic coexistence of antiferromagnetic order and superconductivity in Ba0.77K0.23Fe2As2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 86(2012)180501	Z. Li,R. Zhou,Y. Liu,D. L. Sun,J. Yang,C. T. Lin,Guo-qing Zheng		
153783	PRB086214517	hydrostatic P using He-gas. Tc by RES. (P,Tc) = (0.36,6.22), (0.67,5.29)	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		3	2012																										ABCD		oxypnictide																	ZrCuSiAs	K		7.32					7.32			K/GPa	-3																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153784	PRB086214517	hydrostatic P using He-gas. Tc by SUS. (P,Tc) = (0.24,6.03). (0.52,5.31), (0.76,4.79)	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		3	2012																										ABCD		oxypnictide																	ZrCuSiAs	K				6.72			6.72			K/GPa	-2.46																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153785	PRB086214517	hydrostatic P using He-gas. Tc by SUS. (P,Tc) = (0.36,3.30), (0.74,2.71)	PrOFeP	Pr1Fe1P1O1	Pr	1	Fe	1	P	1															O	1		3	2012																										ABCD		oxypnictide																	ZrCuSiAs	K				3.96			3.96			K/GPa	-1.7																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153786	PRB086214517	hydrostatic P using He-gas. Tc by SUS. (P,Tc) = (0.38,3.08), (0.76,2.35)	NdOFeP	Nd1Fe1P1O1	Nd	1	Fe	1	P	1															O	1		3	2012																										ABCD		oxypnictide																	ZrCuSiAs	K				3.83			3.83			K/GPa	-1.94																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153787	PRB086214517	poly crystal. unannealed sample.hydrostatic P using He-gas. Tc by SUS. (P,Tc) = (0.38,5.29), (0.73,4.23)	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2012																										ABCD		oxypnictide																	ZrCuSiAs	K				6.61			6.61			K/GPa	-3.24																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153788	PRB086214517	poly crystal. unannealed sample.hydrostatic P using He-gas. Tc by RES. (P,Tc) = (0.29,4.88), (0.56,4.39), (0.78,3.72)	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2012																										ABCD		oxypnictide																	ZrCuSiAs	K		5.63					5.63			K/GPa	-2.3																																																																																												(R:Fe2O3:P:Sn = 9:3:6:80.5) - quartz ampoules - heat to 1135 C with 35C/h - keep (1135C,96h) - rapid cool to 700C - remove excess flux. O2-annealing(700C,24h, in flowing O2)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153789	PRB086214517	Piston cylinder cell. P-medium = Fluorinert FC-70.	LaOFeP	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		3	2012																										ABCD		oxypnictide																	ZrCuSiAs	K				7.22			7.22	MTC153789		K/GPa	-4.5																																																																																										Ce,CeF3,CeO2,Bi2S3,S		solid state reaction. mixture - pellet - sealed in quartz - heat(700C,10h) - cool to RT. reground - pellet - ANN(600C,10h)					Intrinsic dependence of Tc on hydrostatic (He-gas) pressure for superconducting LaFePO, PrFePO, and NdFePO single crystals			Department of Physics, Washington University, CB 1105, One Brookings Dr., St. Louis, Missouri 63130, USA	Phys.Rev.B, 86(2012)214517	N. J. Hillier,N. Foroozani,D. A. Zocco,J. J. Hamlin,R. E. Baumbach,I. K. Lum,M. B. Maple,J. S. Schilling		
153790	PRB086214518	not SC. RES, Hall effect, magnetoresistance measured.	CeOBiS2	Ce1Bi1S2O1	Ce	1	Bi	1	S	2															O	1			2012																										ABCD2			P4/nmmz		A	4.016		13.607											CeOBiS2, 1112	K					1.8																																																																																																							Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153791	PRB086214518	not SC. RES, Hall effect, magnetoresistance measured.	Ce(O,F)BiS2	Ce1Bi1S2F0.25O0.75	Ce	1	Bi	1	S	2	F	0.25													O	0.75			2012																										ABCD2			P4/nmmz		A	4.0329		13.519											CeOBiS2, 1112	K					1.8																																																																																																							Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153792	PRB086214518	RES, Hall effect, magnetoresistance measured.	Ce(O,F)BiS2	Ce1Bi1S2F0.33O0.67	Ce	1	Bi	1	S	2	F	0.33													O	0.67			2012																										ABCD2			P4/nmmz		A	4.0361		13.465											CeOBiS2, 1112	K		2.25					2.25																																																																																																					Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153793	PRB086214518	RES, Hall effect, magnetoresistance measured.	Ce(O,F)BiS2	Ce1Bi1S2F0.4O0.6	Ce	1	Bi	1	S	2	F	0.4													O	0.6			2012																										ABCD2			P4/nmmz		A	4.0383		13.406											CeOBiS2, 1112	K		2.77					2.77																																																																																																					Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153794	PRB086214518	RES, Hall effect, magnetoresistance measured. FM below 5 K.	Ce(O,F)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5			2012																										ABCD2			P4/nmmz		A	4.0388		13.373											CeOBiS2, 1112	K		3					3	MTC153794																																																																																																				Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153795	PRB086214518	RES, Hall effect, magnetoresistance measured.	Ce(O,F)BiS2	Ce1Bi1S2F0.6O0.4	Ce	1	Bi	1	S	2	F	0.6													O	0.4			2012																										ABCD2			P4/nmmz		A	4.0371		13.341											CeOBiS2, 1112	K		2.96					2.96																																																																																																					Superconductivity appears in the vicinity of semiconducting-like behavior in CeO1-xFxBiS2			National Laboratory of Solid State Microstructures and Department of Physics, Center for Superconducting Physics and Materials, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 86(2012)214518	Jie Xing,Sheng Li,Xiaxin Ding,Huan Yang,Hai-Hu Wen		
153796	PRB086220509	Pressure by piston-sylinder using FC75 fluorinert medium. Energy gap by neutron spin resonance.	Fe(Te,Se)	Fe1Te0.6Se0.4	Fe	1	Te	0.6	Se	0.4																		3	2012																										AB		PbO			A	3.8023		6.069												K	11.5		13.6	11			11	MTC153796																																															4.6	8																																															Bridgman method					Effect of pressure on the neutron spin resonance in the unconventional superconductor FeTe0.6Se0.4			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 86(2012)220509	K. Marty,A. D. Christianson,A. M. dos Santos,B. Sipos,K. Matsubayashi,Y. Uwatoko,J. A. Fernandez-Baca,C. A. Tulk,T. A. Maier,B. C. Sales,M. D. Lumsden		
153797	JPS081114725	2nd annealing (800C,10h).	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5			2012																													P4/nmmz		A	4.0614		13.379											CeOBiS2, 1112	K				2.7			2.7										11																																																																																				LanO3(3N),LaF3(3N),La2S3(3N),Bi2S3,Bi		mixture - pellet - sealed in quartz tube - heat(800C,10h) - ground - mixture - pellet - ANN(800C,10h)					Superconductivity in Novel BiS2-Based Layered Superconductor LaO1-xFxBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 81(2012)114725	Yoshikazu MIZUGUCHI,Satoshi DEMURA,Keita DEGUCHI,Yoshihiko TAKANO,Hiroshi FUJIHISA,Yoshito GOTOH,Hiroki IZAWA,Osuke MIURA		
153798	JPS081114725	2nd annealing (700C,10h).	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5			2012																													P4/nmmz		A	4.0528		13.321											CeOBiS2, 1112	K				3			3										13.4																																																																																				LanO3(3N),LaF3(3N),La2S3(3N),Bi2S3,Bi		mixture - pellet - sealed in quartz tube - heat(800C,10h) - ground - mixture - pellet - ANN(800C,10h)					Superconductivity in Novel BiS2-Based Layered Superconductor LaO1-xFxBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 81(2012)114725	Yoshikazu MIZUGUCHI,Satoshi DEMURA,Keita DEGUCHI,Yoshihiko TAKANO,Hiroshi FUJIHISA,Yoshito GOTOH,Hiroki IZAWA,Osuke MIURA		
153799	JPS081114725	high-P annealing ANN(700C) and ANN(600C, P=2 GPa). Hc2 defined as R deviate from normal value.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5			2012																													P4/nmmz		A														CeOBiS2, 1112	K	7.58		10.6				9.09										100										T	RES(onset), WHH	10							T/K	RES(onset)	1.37			MHC153799																																																												LanO3(3N),LaF3(3N),La2S3(3N),Bi2S3,Bi		mixture - pellet - sealed in quartz tube - heat(800C,10h) - ground - mixture - pellet - ANN(800C,10h)					Superconductivity in Novel BiS2-Based Layered Superconductor LaO1-xFxBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 81(2012)114725	Yoshikazu MIZUGUCHI,Satoshi DEMURA,Keita DEGUCHI,Yoshihiko TAKANO,Hiroshi FUJIHISA,Yoshito GOTOH,Hiroki IZAWA,Osuke MIURA		
153800	PRB086220510	SC volume fraction at 2K = 100%.	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4			2012																										A3B4C4			I4/mmm		A	3.9592		41.241											another candidate of space G , I-42m	K	4.5		8.6				6.55										100										T	RES(onset), WHH	21							T/K	RES(onset)	3.54			MHC153800																																																												Bi2S3,Bi2O3,S		mixture - ground - pellet - sealed in quartz tube - heat(510C,10h) - reground - pellet - ANN(510C,10h in evacuated quartz tube)					BiS2-based layered superconductor Bi4O4S3			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1 Minami-osawa, Hachioji, Tokyo 192-0397, Japan	Phys.Rev.B, 86(2012)220510	Yoshikazu Mizuguchi,Hiroshi Fujihisa,Yoshito Gotoh,Katsuhiro Suzuki,Hidetomo Usui,Kazuhiko Kuroki,Satoshi Demura,Yoshihiko Takano,Hiroki Izawa,Osuke Miura		
153801	PRB086224507	isotropic magnetic behaviour. (dC/gamma*Tc) = 0.36. Lattice term in SP, beta=1.18 mJ/mol.K4, delta = 0.0103 mJ/mol.K6. Comp = La2.1Pt2.8Ge5.1 by EDX	La2Pt3Ge5	La2Pt3Ge5	La	2	Pt	3	Ge	5																		3	2012																										A2B3C5		U2Co3Si5	Ibam		A	10.1508	12.03	6.2709												K				8.1			8.1																																																								mJ/mol.K2	4.65	SP																																				La(3N),Pr(3N),Pt(4N),Ge(5N)		Pt-Ge mixture as flux. La(or Pr):Pt:Ge = 1:4:20, -alumina crucible - sealed in quartz tube(1/3 atm Ar) - heat to 1130C(200C/h) - keep(40h) - cool to 850C(3C/h)					Possible multigap superconductivity and magnetism in single crystals of superconducting La2Pt3Ge5 and Pr2Pt3Ge5			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	Phys.Rev.B, 86(2012)224507	N. H. Sung,C. J. Roh,K. S. Kim,B. K. Cho		
153802	PRB086224507	Curie-T = -54.63 K, Meff = 3.65 myu-B/Pr for H//ab. For H//c, data in DB. Comp = Pr2.1Pt2.9Ge5.0 by EDX	Pr2Pt3Ge5	Pr2Pt3Ge5	Pr	2	Pt	3	Ge	5																		3	2012					mB/Pr	3.65	-40.35																			A2B3C5		U2Co3Si5	Ibam		A	10.1333	11.86	6.2288												K				7.8			7.8																																																																																														La(3N),Pr(3N),Pt(4N),Ge(5N)		Pt-Ge mixture as flux. La(or Pr):Pt:Ge = 1:4:20, -alumina crucible - sealed in quartz tube(1/3 atm Ar) - heat to 1130C(200C/h) - keep(40h) - cool to 850C(3C/h)					Possible multigap superconductivity and magnetism in single crystals of superconducting La2Pt3Ge5 and Pr2Pt3Ge5			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	Phys.Rev.B, 86(2012)224507	N. H. Sung,C. J. Roh,K. S. Kim,B. K. Cho		
153803	PRB086224514	(dC/Tc) = 67 mJ/mol.K2. Thermal expansin jump at Tc = 1.2 E-6 /K. c-axis uniaxial P dependence of Tc: (dTc/dP<c>) = 1.1 K/GPa estimated from thermal expansion	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2012																										AB2C2		ThCr2Si2												0.0057					Fe-122, (dL/L)c = 0.0006 at 77K.	K		3.4		3.43			3.4	MTC153803		K/GPa	-1.04																																																				mJ/mol.K2	107	SP	224	SP																																				KAs flux method.. mixture(K:Fe:As=5:2:6) - alumina crucible - sealed fused silica ampule - heat to 920 C - slow cool to 620 C(1C/h)					Hydrostatic and uniaxial pressure dependence of superconducting transition temperature of KFe2As2 single crystals			The Ames Laboratory, US Department of Energy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 86(2012)224514	Sergey L. Bud'ko,Yong Liu,Thomas A. Lograsso,Paul C. Canfield		
153805	CIN039S257		(Tl,Bi)(Sr,Yb)2Ca(Cu,Fe)2O7	Tl0.9Bi0.1Sr1.8Yb0.2Ca1Cu1.99Fe0.01O7-z	Tl	0.9	Bi	0.1	Sr	1.8	Yb	0.2	Ca	1	Cu	1.99	Fe	0.01							O	7-z			2013																											2	Tl1212			A	3.797		12.126											Tl-1212	K	40		88.1				64.05																																																																																														SrCO3,CaO,CuO,CdO,A2O3(A=Yb,Fe,Tl,Bi)	1	Precursor(Sr-Yb-Ca-Cu-Fe-Cd-O) - heat(900C,24h), then mixed with Tl2O3 & Bi2O3 - pellet - heat(1000C, 5min) - FC to RT					Superconducting fluctuation and infrared absorption of Cd-substituted Tl0.9Bi0.1Sr1.8Yb0.2Ca1-xCdxCu1.99Fe0.01O7-d ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Malaysia	Ceramics International, 39(2013)S257	S. Ismail,A.K.Yahya,Nawazish A. Khan		
153806	CIN039S257	[cohere]c calculates from resistivity using LD model, Josephson coupling. Anisotropy(cohere) = 14.641 assuming [cohere]ab = 10 A.	(Tl,Bi)(Sr,Yb)2(Ca,Cd)(Cu,Fe)2O7	Tl0.9Bi0.1Sr1.8Yb0.2Ca0.9Cd0.1Cu1.99Fe0.01O7-z	Tl	0.9	Bi	0.1	Sr	1.8	Yb	0.2	Ca	0.9	Cd	0.1	Cu	1.99	Fe	0.01					O	7-z			2013																											2	Tl1212			A	3.796		12.121											Tl-1212	K	57.5		85.1				71.3																																				A	from resistivity, L-D model			0.683																																																						SrCO3,CaO,CuO,CdO,A2O3(A=Yb,Fe,Tl,Bi)	1	Precursor(Sr-Yb-Ca-Cu-Fe-Cd-O) - heat(900C,24h), then mixed with Tl2O3 & Bi2O3 - pellet - heat(1000C, 5min) - FC to RT					Superconducting fluctuation and infrared absorption of Cd-substituted Tl0.9Bi0.1Sr1.8Yb0.2Ca1-xCdxCu1.99Fe0.01O7-d ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Malaysia	Ceramics International, 39(2013)S257	S. Ismail,A.K.Yahya,Nawazish A. Khan		
153807	CIN039S257	[cohere]c calculates from resistivity using LD model, Josephson coupling. Anisotropy(cohere) = 17.699 assuming [cohere]ab = 10 A.	(Tl,Bi)(Sr,Yb)2(Ca,Cd)(Cu,Fe)2O7	Tl0.9Bi0.1Sr1.8Yb0.2Ca0.8Cd0.2Cu1.99Fe0.01O7-z	Tl	0.9	Bi	0.1	Sr	1.8	Yb	0.2	Ca	0.8	Cd	0.2	Cu	1.99	Fe	0.01					O	7-z			2013																											2	Tl1212			A	3.795		12.118											Tl-1212	K	68.2		88.5				78.35																																				A	from resistivity, L-D model			0.565																																																						SrCO3,CaO,CuO,CdO,A2O3(A=Yb,Fe,Tl,Bi)	1	Precursor(Sr-Yb-Ca-Cu-Fe-Cd-O) - heat(900C,24h), then mixed with Tl2O3 & Bi2O3 - pellet - heat(1000C, 5min) - FC to RT					Superconducting fluctuation and infrared absorption of Cd-substituted Tl0.9Bi0.1Sr1.8Yb0.2Ca1-xCdxCu1.99Fe0.01O7-d ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Malaysia	Ceramics International, 39(2013)S257	S. Ismail,A.K.Yahya,Nawazish A. Khan		
153808	CIN039S257	[cohere]c calculates from resistivity using LD model, Josephson coupling. Anisotropy(cohere) = 14.184 assuming [cohere]ab = 10 A.	(Tl,Bi)(Sr,Yb)2(Ca,Cd)(Cu,Fe)2O7	Tl0.9Bi0.1Sr1.8Yb0.2Ca0.7Cd0.3Cu1.99Fe0.01O7-z	Tl	0.9	Bi	0.1	Sr	1.8	Yb	0.2	Ca	0.7	Cd	0.3	Cu	1.99	Fe	0.01					O	7-z			2013																											2	Tl1212			A	3.794		12.116											Tl-1212	K	76.4		93.6				85																																				A	from resistivity, L-D model			0.705																																																						SrCO3,CaO,CuO,CdO,A2O3(A=Yb,Fe,Tl,Bi)	1	Precursor(Sr-Yb-Ca-Cu-Fe-Cd-O) - heat(900C,24h), then mixed with Tl2O3 & Bi2O3 - pellet - heat(1000C, 5min) - FC to RT					Superconducting fluctuation and infrared absorption of Cd-substituted Tl0.9Bi0.1Sr1.8Yb0.2Ca1-xCdxCu1.99Fe0.01O7-d ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Malaysia	Ceramics International, 39(2013)S257	S. Ismail,A.K.Yahya,Nawazish A. Khan		
153809	CIN039S257	[cohere]c calculates from resistivity using LD model, Josephson coupling. Anisotropy(cohere) = 14.038 assuming [cohere]ab = 10 A.	(Tl,Bi)(Sr,Yb)2(Ca,Cd)(Cu,Fe)2O7	Tl0.9Bi0.1Sr1.8Yb0.2Ca0.6Cd0.4Cu1.99Fe0.01O7-z	Tl	0.9	Bi	0.1	Sr	1.8	Yb	0.2	Ca	0.6	Cd	0.4	Cu	1.99	Fe	0.01					O	7-z			2013																											2	Tl1212			A	3.793		12.111											Tl-1212	K	74.8		91.9				83.35																																				A	from resistivity, L-D model			0.665																																																						SrCO3,CaO,CuO,CdO,A2O3(A=Yb,Fe,Tl,Bi)	1	Precursor(Sr-Yb-Ca-Cu-Fe-Cd-O) - heat(900C,24h), then mixed with Tl2O3 & Bi2O3 - pellet - heat(1000C, 5min) - FC to RT					Superconducting fluctuation and infrared absorption of Cd-substituted Tl0.9Bi0.1Sr1.8Yb0.2Ca1-xCdxCu1.99Fe0.01O7-d ceramics			Faculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Malaysia	Ceramics International, 39(2013)S257	S. Ismail,A.K.Yahya,Nawazish A. Khan		
153810	JPS082013703		BaTi2Bi2O	Ba1Ti2Bi2O1	Ba	1	Ti	2	Bi	2															O	1			2013																										A1B1C2D2			P4/mmm		A	4.1232		8.3447											oxybismuthide	K			4.6	4.6			4.6										60																																																																																				BaO(4N),Ti(3N),Bi(3N)		pellet - wrapped in Ta foil - sealed in quartz tube - heat(850C,50h)					Synthesis and Physical Properties of the New Oxybismuthides BaTi2Bi2O and (SrF)2Ti2Bi2O with a d1 Square Net			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)013703	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,James HESTER,Takafumi YAMAMOTO,Yoji KOBAYASHI,Naruki TSUJI,Jungeun KIM,Akihiko FUJIWARA,Hiroshi KAGEYAMA		
153811	JPS082013703	not SC	(SrF)2Ti2Bi2O	Sr1F1Ti2Bi2O1	Sr	1	F	1	Ti	2	Bi	2													O	1			2013																										A1B2C2D2			I4/mmm		A	4.1178		21.3703											oxybismuthide	K					1.85																																																																																																SrF2,SrO(3N),Ti(3N),Bi(3N)		pellet - wrapped in Ta foil - sealed in quartz tube - heat(900C,50h)					Synthesis and Physical Properties of the New Oxybismuthides BaTi2Bi2O and (SrF)2Ti2Bi2O with a d1 Square Net			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)013703	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,James HESTER,Takafumi YAMAMOTO,Yoji KOBAYASHI,Naruki TSUJI,Jungeun KIM,Akihiko FUJIWARA,Hiroshi KAGEYAMA		
153812	JPS082023711	impurity phases: Hg1234, HgO. (dTc/dP) = 2.5 K/GPa for P<5 GPa and  = 1.0 K/GPa for P > 10GPa	HgBa2Ca2Cu3O8	Hg1Ba2Ca2Cu3O8+z	Hg	1	Ba	2	Ca	2	Cu	3													O	8+z		1	2013																												Hg1223																		K	130.5	130.9	131.7				130.9	TC153812		K/GPa	2.5																																																																																												high P synthesis. mixture(HgO:precursor Ba2Ca2Cu3Oz = 0.75:1) - press - charged in Au capsule - heat(830C,0.5h,P=2 GPa using cubic-anvil HP apparatus)					Zero Resistivity above 150K in HgBa2Ca2Cu3O8t  at High Pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 82(2013)023711	Nao TAKESHITA,Ayako YAMAMOTO,Akira IYO,Hiroshi EISAKI		
153813	JPS082033705	T<SDW> = 203 K	BaTi2As2O	Ba1Ti2As2O1	Ba	1	Ti	2	As	2															O	1		1	2013																															A	4.0454		7.2776												K					1.85																																																																																																BaO(4N),Ti(3N),As(6N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153814	JPS082033705	T<SDW> = 160 K	BaTi2(As,Sb)2O	Ba1Ti2As1.2Sb0.8O1	Ba	1	Ti	2	As	1.2	Sb	0.8													O	1		1	2013																															A	4.0759		7.5589												K					1.85																																																																																																BaO(4N),Ti(3N),As(6N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153815	JPS082033705	T<SDW> = 95 K	BaTi2(As,Sb)2O	Ba1Ti2As0.4Sb1.6O1	Ba	1	Ti	2	As	0.4	Sb	1.6													O	1		1	2013																															A	4.1012		7.8953												K					1.85			TC153815																																																																																													BaO(4N),Ti(3N),As(6N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153816	JPS082033705	T<SDW> = 85 K	BaTi2(As,Sb)2O	Ba1Ti2As0.2Sb1.8O1	Ba	1	Ti	2	As	0.2	Sb	1.8													O	1		1	2013																															A	4.1066		7.9991												K		0.48					0.48										50																																																																																				BaO(4N),Ti(3N),As(6N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153817	JPS082033705	T<SDW> = 50 K	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2013																															A	4.1126		8.0804												K		1.48					1.48										50																																																																																				BaO(4N),Ti(3N),As(6N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153818	JPS082033705		BaTi2(Sb,Bi)2O	Ba1Ti2Sb1.6Bi0.4O1	Ba	1	Ti	2	Sb	1.6	Bi	0.4													O	1		1	2013																															A	4.1121		8.1252												K				3.47			3.47	TC153818									50																																																																																				BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153819	JPS082033705		BaTi2(Sb,Bi)2O	Ba1Ti2Sb1.4Bi0.6O1	Ba	1	Ti	2	Sb	1.4	Bi	0.6													O	1		1	2013																															A	4.1138		8.1617												K				2.59			2.59										50																																																																																				BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153820	JPS082033705	not bulk SC. but SC sign at 3.0 K	BaTi2(Sb,Bi)2O	Ba1Ti2Sb1.2Bi0.8O1	Ba	1	Ti	2	Sb	1.2	Bi	0.8													O	1		1	2013																															A	4.1169		8.1897												K					1.85																																																																																																BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153821	JPS082033705	not bulk SC. but SC sign at 2.0 K	BaTi2(Sb,Bi)2O	Ba1Ti2Sb1Bi1O1	Ba	1	Ti	2	Sb	1	Bi	1													O	1		1	2013																															A	4.1175		8.2093												K					1.85																																																																																																BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153822	JPS082033705		BaTi2(Sb,Bi)2O	Ba1Ti2Sb0.8Bi1.2O1	Ba	1	Ti	2	Sb	0.8	Bi	1.2													O	1		1	2013																															A	4.1199		8.2177												K				4.02			4.02	TC153818									50																																																																																				BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153823	JPS082033705		BaTi2(Sb,Bi)2O	Ba1Ti2Sb0.4Bi1.6O1	Ba	1	Ti	2	Sb	0.4	Bi	1.6													O	1		1	2013																															A	4.1211		8.2794												K				4.52			4.52										50																																																																																				BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153824	JPS082033705		BaTi2Bi2O	Ba1Ti2Bi2O1	Ba	1	Ti	2	Bi	2															O	1		1	2013																															A	4.1253		8.3439												K				4.6			4.6										50																																																																																				BaO(4N),Ti(3N),Bi(3N),Sb(3N)		solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 900 C(100C/h) - keep(900C,40h) - cool to RT(50C/h)					Two Superconducting Phases in the Isovalent Solid Solutions BaTi2Pn2O (Pn = As, Sb, and Bi)			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)033705	Takeshi YAJIMA,Kousuke NAKANO,Fumitaka TAKEIRI,Yasumasa NOZAKI,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
153825	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.1O0.9	Nd	1	Bi	1	S	2	F	0.1													O	0.9			2013																										ABCD2			P4/nmm		A	3.9999		13.583											CeOBiS2, 1112	K				4.24			4.24																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153826	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.2O0.8	Nd	1	Bi	1	S	2	F	0.2													O	0.8			2013																										ABCD2			P4/nmm		A	3.9981		13.581											CeOBiS2, 1112	K				5.12			5.12																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153827	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.3O0.7	Nd	1	Bi	1	S	2	F	0.3													O	0.7			2013																										ABCD2			P4/nmm		A	3.9976		13.4703											CeOBiS2, 1112	K	5.2		6.7	5.12			5.12	TC153827																			T	RES, WHH	3.3												HC153827																																																												Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153828	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.4O0.6	Nd	1	Bi	1	S	2	F	0.4													O	0.6			2013																										ABCD2			P4/nmm		A	4.0035		13.4423											CeOBiS2, 1112	K				5.25			5.25																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153829	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2			P4/nmm		A	3.9991		13.4067											CeOBiS2, 1112	K				4.7			4.7																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153830	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.6O0.4	Nd	1	Bi	1	S	2	F	0.6													O	0.4			2013																										ABCD2			P4/nmm		A	4.0016		13.4019											CeOBiS2, 1112	K				4.35			4.35																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153831	JPS082033708	impurity phases: NdOF, Bi2S3	Nd(O,F)Bi2S2	Nd1Bi1S2F0.7O0.3	Nd	1	Bi	1	S	2	F	0.7													O	0.3			2013																										ABCD2			P4/nmm		A	3.9953		13.4115											CeOBiS2, 1112	K				4.25			4.25																																																																																														Bi,Bi2S3,Nd2O3,Nd2S3,NdF3		mixture - ground - pelletize - sealed in evacuated quartz tube - heat(800 C,10h)					New Member of BiS2-Based Superconductor NdO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 82(2013)033708	Satoshi DEMURA,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Hiroyuki OKAZAKI,Hiroshi HARA,Tohru WATANABE,Saleem James DENHOLME,Masaya FUJIOKA,Toshinori OZAKI,Hiroshi FUJIHISA,Yoshito GOTOH,Osuke MIURA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
153832	JPS082034718	impurity phase: Bi2S3. as-grown and 400C-annealed samples show no SC. Hc1, Hc2 at 0 K estimate assuming Hc1, Hc2(t) = [(1-t^2)/(1+t^2)]Hc1(0),Hc2(0). GL(kappa) = 59.46	Bi6O8S5	Bi6S5O8	Bi	6	S	5																	O	8			2013																										A5B6C8			I4/mmm		A	3.9		39.91												K	0.6		4.2				2.4											Oe	M-H curve	2.69			2			2	kOe	M-H curve	4.565			3.4			2								nm	from Hc2(0)	26.86			um	Hc1, GL equation	1.6																																																			Bi,Bi2S3,Bi2O3,S		solid state reaction. mixture - pellet -sealed in evacuated quartz tube - heat (510C,18h) - ANN(200C,4h, in O2					Superconductivity in Vacuum Annealed Bi6O8S5			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	J.Phys.Soc.Jpn, 82(2013)034718	Yi YU,Jifeng SHAO,Shun TAN,Changjin ZHANG,Yuheng ZHANG		
153833	PHB4120119	impurity phases: Bi,Bi2S3	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4			2013																													I4/mmm		A	3.9753		41.4287												K	4.15		4.85	4.11			4.11																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in silica tube - heat(450C,10h) - heat(510C,10h) - one more process.					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
153834	PHB4120119	impurity phases: Bi,Bi2S3	(Bi,Cu)4O4S3	Bi3.99Cu0.01S3O4	Bi	3.99	Cu	0.01	S	3															O	4			2013																													I4/mmm		A	3.975		41.4083												K	3.91		4.51	3.93			3.93																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in silica tube - heat(450C,10h) - heat(510C,10h) - one more process.					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
153835	PHB4120119	impurity phases: Bi,Bi2S3	(Bi,Cu)4O4S3	Bi3.975Cu0.025S3O4	Bi	3.975	Cu	0.025	S	3															O	4			2013																													I4/mmm		A	3.9687		41.4009												K	3.1		3.91	2.99			2.99	TC153835																																																																																													Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in silica tube - heat(450C,10h) - heat(510C,10h) - one more process.					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
153836	PHB4120119	impurity phases: Bi,Bi2S3	(Bi,Cu)4O4S3	Bi3.95Cu0.05S3O4	Bi	3.95	Cu	0.05	S	3															O	4			2013																													I4/mmm		A	3.9668		41.3861												K	2.68		3.51	2.59			2.59																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in silica tube - heat(450C,10h) - heat(510C,10h) - one more process.					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
153837	PHB4120119	impurity phases: Bi,Bi2S3.  R not to zero at 2K.	(Bi,Cu)4O4S3	Bi3.9Cu0.1S3O4	Bi	3.9	Cu	0.1	S	3															O	4			2013																													I4/mmm		A	3.9655		41.3954												K			2.99				2.99																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in silica tube - heat(450C,10h) - heat(510C,10h) - one more process.					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
153838	PHB4130036	volume fraction: Tl2223:Tl1223 = 43.07:45.74 another phase=Ba2Cu3O5 (volume fraction not shown). lattice const. for Tl2223 phase.	Tl2Ba2Ca2Cu3Oz	Tl2Ba2Ca2Cu3Oz	Tl	2	Ba	2	Ca	2	Cu	3													O	z		2	2013																												Tl2223			A	3.83		35.01											Tl-1223(a=3.83, c=15.85)	K	102.1		113.3			11.2	107.7																																																																																																precursor(ba-Cu-Ca-V-O) synthsized by heating(880C,4h,O2-flow) - mixed with Tl2O3 - wrapped in Au foil - heat(880C,30min)					Effect of vanadium substitution on the microstructural and superconducting  properties  of Tl2Ba2Ca2-xVxCu3Oy superconductors			Superconductivity and Thermal Analysis Laboratory, Department of Physics, Faculty of Science, Gazi University, 06531 Ankara, Turkey	Physica B, 413(2013)36	E. Erbilen,S. Cavdar,H.Koralay,A.G unen		
153839	PHB4130036	volume fraction: Tl2223:Tl1223 = 41.83:43.24 another phase=Ba2Cu3O5 (volume fraction not shown). lattice const. for Tl2223 phase.	Tl2Ba2(Ca,V)2Cu3Oz	Tl2Ba2Ca1.9Cu0.1Cu3Oz	Tl	2	Ba	2	Ca	1.9	Cu	0.1	Cu	3											O	z		2	2013																												Tl2223			A	3.85		35.31											Tl-1223(a=3.84, c=15.93)	K	105.9		115.8			9.9	110.85																																																																																																precursor(ba-Cu-Ca-V-O) synthsized by heating(880C,4h,O2-flow) - mixed with Tl2O3 - wrapped in Au foil - heat(880C,30min)					Effect of vanadium substitution on the microstructural and superconducting  properties  of Tl2Ba2Ca2-xVxCu3Oy superconductors			Superconductivity and Thermal Analysis Laboratory, Department of Physics, Faculty of Science, Gazi University, 06531 Ankara, Turkey	Physica B, 413(2013)36	E. Erbilen,S. Cavdar,H.Koralay,A.G unen		
153840	PHB4130036	volume fraction: Tl2223:Tl1223 = 39.27:36.91 another phase=Ba2Cu3O5 (volume fraction not shown). lattice const. for Tl2223 phase.	Tl2Ba2(Ca,V)2Cu3Oz	Tl2Ba2Ca1.7Cu0.3Cu3Oz	Tl	2	Ba	2	Ca	1.7	Cu	0.3	Cu	3											O	z		2	2013																												Tl2223			A	3.84		35.38											Tl-1223(a=3.84, c=15.93)	K	107.6		115.4			7.8	111.5																																																																																																precursor(ba-Cu-Ca-V-O) synthsized by heating(880C,4h,O2-flow) - mixed with Tl2O3 - wrapped in Au foil - heat(880C,30min)					Effect of vanadium substitution on the microstructural and superconducting  properties  of Tl2Ba2Ca2-xVxCu3Oy superconductors			Superconductivity and Thermal Analysis Laboratory, Department of Physics, Faculty of Science, Gazi University, 06531 Ankara, Turkey	Physica B, 413(2013)36	E. Erbilen,S. Cavdar,H.Koralay,A.G unen		
153841	PHB4130036	volume fraction: Tl2223:Tl1223 = 33.88:29.68 another phase=Ba2Cu3O5 (volume fraction not shown). lattice const. for Tl2223 phase.	Tl2Ba2(Ca,V)2Cu3Oz	Tl2Ba2Ca1.5Cu0.5Cu3Oz	Tl	2	Ba	2	Ca	1.5	Cu	0.5	Cu	3											O	z		2	2013																												Tl2223			A	4.13		34.79											Tl-1223(a=3.83, c=15.89)	K	99		113.2			14.2	106.1																																																																																																precursor(ba-Cu-Ca-V-O) synthsized by heating(880C,4h,O2-flow) - mixed with Tl2O3 - wrapped in Au foil - heat(880C,30min)					Effect of vanadium substitution on the microstructural and superconducting  properties  of Tl2Ba2Ca2-xVxCu3Oy superconductors			Superconductivity and Thermal Analysis Laboratory, Department of Physics, Faculty of Science, Gazi University, 06531 Ankara, Turkey	Physica B, 413(2013)36	E. Erbilen,S. Cavdar,H.Koralay,A.G unen		
153842	PHB4130036	volume fraction: Tl2223:Tl1223 = 29.03:24.97 another phase=Ba2Cu3O5 (volume fraction not shown). lattice const. for Tl2223 phase.	Tl2Ba2(Ca,V)2Cu3Oz	Tl2Ba2Ca1.3Cu0.7Cu3Oz	Tl	2	Ba	2	Ca	1.3	Cu	0.7	Cu	3											O	z		2	2013																												Tl2223			A	3.85		35.48											Tl-1223(a=3.82, c=15.96)	K	102		112.1			10.1	107.05																																																																																																precursor(ba-Cu-Ca-V-O) synthsized by heating(880C,4h,O2-flow) - mixed with Tl2O3 - wrapped in Au foil - heat(880C,30min)					Effect of vanadium substitution on the microstructural and superconducting  properties  of Tl2Ba2Ca2-xVxCu3Oy superconductors			Superconductivity and Thermal Analysis Laboratory, Department of Physics, Faculty of Science, Gazi University, 06531 Ankara, Turkey	Physica B, 413(2013)36	E. Erbilen,S. Cavdar,H.Koralay,A.G unen		
153843	PHC4840012	As-Fe-As bond angle = 102.16 degree	Ca4Al2O6Fe2As2	Ca4Al2Fe2As2O6	Ca	4	Al	2	Fe	2	As	2													O	6			2013																												Fe-42622			A	3.713		15.407											Al-42622As	K			28.2				28.2																																																																																																HP synthesis. mixture((Ca4Al2O6-x)(Fe2Pn2) or (Ca3Al2O5-x)(Fe2Pn2) ) -pellet - heat(1150C(Pn=As) or 1300C(Pn=P), 1h, P=4.5 GPa)					"Discovery of the Ca4Al2O6Fe2Pn2  ""Al-42622(Pn)"" and Ca3Al2O5Fe2Pn2 ""Al-32522(Pn)""  (Pn = As, P) superconductors"			National Institute of Advanced Industrial Science and Technology (AIST), Central-2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 484(2013)12	P.M. Shirage,K. Kihou,C.H. Lee,H. Kito,H. Eisaki,A. Iyo		
153844	PHC4840012	As-Fe-As bond angle = 109.4 degree	Ca4Al2O6Fe2P2	Ca4Al2Fe2P2O6	Ca	4	Al	2	Fe	2	P	2													O	6			2013																												Fe-42622			A	3.692		14.934											Al-42622P	K			17.1				17.1																																																																																																HP synthesis. mixture((Ca4Al2O6-x)(Fe2Pn2) or (Ca3Al2O5-x)(Fe2Pn2) ) -pellet - heat(1150C(Pn=As) or 1300C(Pn=P), 1h, P=4.5 GPa)					"Discovery of the Ca4Al2O6Fe2Pn2  ""Al-42622(Pn)"" and Ca3Al2O5Fe2Pn2 ""Al-32522(Pn)""  (Pn = As, P) superconductors"			National Institute of Advanced Industrial Science and Technology (AIST), Central-2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 484(2013)12	P.M. Shirage,K. Kihou,C.H. Lee,H. Kito,H. Eisaki,A. Iyo		
153845	PHC4840012	As-Fe-As bond angle = 103.28 degree	Ca3Al2O5Fe2As2	Ca3Al2Fe2As2O5	Ca	3	Al	2	Fe	2	As	2													O	5			2013																												Fe-32522			A	4.742		26.078											Al-32522As	K			30.2				30.2																																																																																																HP synthesis. mixture((Ca4Al2O6-x)(Fe2Pn2) or (Ca3Al2O5-x)(Fe2Pn2) ) -pellet - heat(1150C(Pn=As) or 1300C(Pn=P), 1h, P=4.5 GPa)					"Discovery of the Ca4Al2O6Fe2Pn2  ""Al-42622(Pn)"" and Ca3Al2O5Fe2Pn2 ""Al-32522(Pn)""  (Pn = As, P) superconductors"			National Institute of Advanced Industrial Science and Technology (AIST), Central-2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 484(2013)12	P.M. Shirage,K. Kihou,C.H. Lee,H. Kito,H. Eisaki,A. Iyo		
153846	PHC4840012	As-Fe-As bond angle = 110.46 degree	Ca3Al2O5Fe2P2	Ca3Al2Fe2P2O5	Ca	3	Al	2	Fe	2	P	2													O	5			2013																												Fe-32522			A	3.715		25.236											Al-32522P	K			16.6				16.6																																																																																																HP synthesis. mixture((Ca4Al2O6-x)(Fe2Pn2) or (Ca3Al2O5-x)(Fe2Pn2) ) -pellet - heat(1150C(Pn=As) or 1300C(Pn=P), 1h, P=4.5 GPa)					"Discovery of the Ca4Al2O6Fe2Pn2  ""Al-42622(Pn)"" and Ca3Al2O5Fe2Pn2 ""Al-32522(Pn)""  (Pn = As, P) superconductors"			National Institute of Advanced Industrial Science and Technology (AIST), Central-2, 1-1-1, Umezono, Tsukuba, Ibaraki 305-8568, Japan	Physica C, 484(2013)12	P.M. Shirage,K. Kihou,C.H. Lee,H. Kito,H. Eisaki,A. Iyo		
153847	PHC4840052		Y2C3	C3Y2	C	3	Y	2																				1	2013																										A2B3		Pu2C3																		K	15.4		15.9			0.5	15.65																																																3.4	1																																															Polycrystals were prepared by arc-melting, followed by high-P(4-5.5 GPa) and high-T(1673-1873 K) treatment.					Tunneling break-junction measurements of the superconducting gap in Y2C3			Hiroshima University, Graduate School of Integrated Arts and Sciences, Higashi-Hiroshima 739-8521, Japan	Physica C, 484(2013)52	T. Ekino,A. Sugimoto,A.M. Gabovich,H. Kinoshita,J. Akimitsu		
153848	PHC4850160	impurity phase: PrGe2(1 %). Tc(0.58 GPa) = 7.83 K.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2013																										AB4C12		skutterudite			A	8.61														K				7.91			7.91	MTC153848		K/GPa	-0.19																																																																																												arc-melting(5 times) - sealed in quartz tube(200 Torr Ar) - ANN(800C,2w)					Dependence of the superconducting transition temperature of the filled skutterudite compound PrPt4Ge12 on hydrostatic pressure			Department of Physics, Washington University, St. Louis, MO 63130, United States	Physica C, 485(2013)160	N. Foroozani,J.J. Hamlin,J.S. Schilling,R.E. Baumbach,I.K. Lum,L. Shu,K. Huang,M.B. Maple		
153849	PHC4850168	6% MgB2C2 phase. Two gap model: gap(meV), gamma(mJ/mol.K2) are (1.68, 0.99) and (6.77, 0.51) for pai- and sigma- band electron, respectively. C(T,H) measured	Mg(B,C)2	Mg1B1.9C0.1	Mg	1	B	1.9	C	0.1																		1	2013																										AB2		AlB2																		K		31.4					31.4																																															6.77	5	14							mJ/mol.K2	1.5																																												Specific heat of Mg(B1-xCx)2, x = 0.05, 0.1			Lawrence Berkeley National Laboratory, USA	Physica C, 485(2013)168	R.A. Fisher,J.E. Gordon,F. Hardy,W.E. Mickelson,N. Oeschler,N.E. Phillips,A. Zettl		
153850	PHC4850168	10% MgB2C2 phase. Two gap model: gap(meV), gamma(mJ/mol.K2) are (1.39, 1.42) and (3.57, 0.35) for pai- and sigma- band electron, respectively. C(T,H) measured	Mg(B,C)2	Mg1B1.8C0.2	Mg	1	B	1.8	C	0.2																		1	2013																										AB2		AlB2																		K		19.7					19.7																																														meV	3.57	4.2	14							mJ/mol.K2	1.77																																												Specific heat of Mg(B1-xCx)2, x = 0.05, 0.1			Lawrence Berkeley National Laboratory, USA	Physica C, 485(2013)168	R.A. Fisher,J.E. Gordon,F. Hardy,W.E. Mickelson,N. Oeschler,N.E. Phillips,A. Zettl		
153851	PHC4890032	compositions by SEM. Fe-content = 1.03 - - 1.04. Hc2 defined as R=0.5Rn.	Fe1.03Te1-xSex	Fe1.03Te0.9Se0.1	Fe	1.03	Te	0.9	Se	0.1																		3	2013					myu-B/mol	4.1	85	34																				Fe-11																	Fe-11	K	11.5	11.9	12.4				11.9																													T/K	RES(0.5Rn)		14.4	5.33																																																															crystals grown by KCl/NaCl flux technique in evacuated quartz tube for 21 days. T-gradient: high-T(765 C) and low-T(720 C)					Coexistence of superconductivity and magnetism in Fe1+d Te1-xSex (x = 0.1, 0.2, 0.28, 0.4 and 0.45)			Low Temperature Physics and Superconductivity Department, M.V. Lomonosov Moscow State University, Moscow 119991, Russia	Physica C, 489(2013)32	Y.A. Ovchenkov,D.A. Chareev,E.S. Kozlyakova,O.S. Volkova,A.N. Vasiliev		
153852	PHC4890032	compositions by SEM. Fe-content = 1.03 - - 1.04. Hc2 defined as R=0.5Rn.	Fe1.03Te1-xSex	Fe1.03Te0.8Se0.2	Fe	1.03	Te	0.8	Se	0.2																		3	2013					myu-B/mol	3.67		22																				Fe-11																	Fe-11	K	12.8	13.5	13.8				13.5																													T/K	RES(0.5Rn)		13.5	5.29																																																															crystals grown by KCl/NaCl flux technique in evacuated quartz tube for 21 days. T-gradient: high-T(765 C) and low-T(720 C)					Coexistence of superconductivity and magnetism in Fe1+d Te1-xSex (x = 0.1, 0.2, 0.28, 0.4 and 0.45)			Low Temperature Physics and Superconductivity Department, M.V. Lomonosov Moscow State University, Moscow 119991, Russia	Physica C, 489(2013)32	Y.A. Ovchenkov,D.A. Chareev,E.S. Kozlyakova,O.S. Volkova,A.N. Vasiliev		
153853	PHC4890032	compositions by SEM. Fe-content = 1.03 - - 1.04. Hc2 defined as R=0.5Rn.	Fe1.03Te1-xSex	Fe1.03Te0.72Se0.28	Fe	1.03	Te	0.72	Se	0.28																		3	2013					myu-B/mol	3.72		18																				Fe-11																	Fe-11	K	13.3	13.9	14.1				13.9																													T/K	RES(0.5Rn)		12.6	4.4																																																															crystals grown by KCl/NaCl flux technique in evacuated quartz tube for 21 days. T-gradient: high-T(765 C) and low-T(720 C)					Coexistence of superconductivity and magnetism in Fe1+d Te1-xSex (x = 0.1, 0.2, 0.28, 0.4 and 0.45)			Low Temperature Physics and Superconductivity Department, M.V. Lomonosov Moscow State University, Moscow 119991, Russia	Physica C, 489(2013)32	Y.A. Ovchenkov,D.A. Chareev,E.S. Kozlyakova,O.S. Volkova,A.N. Vasiliev		
153854	PHC4890032	compositions by SEM. Fe-content = 1.03 - - 1.04. Hc2 defined as R=0.5Rn.	Fe1.03Te1-xSex	Fe1.03Te0.6Se0.4	Fe	1.03	Te	0.6	Se	0.4																		3	2013					myu-B/mol	4.27		16																				Fe-11																	Fe-11	K	13.7	14	14.3				14																													T/K	RES(0.5Rn)		12.5	3.77																																																															crystals grown by KCl/NaCl flux technique in evacuated quartz tube for 21 days. T-gradient: high-T(765 C) and low-T(720 C)					Coexistence of superconductivity and magnetism in Fe1+d Te1-xSex (x = 0.1, 0.2, 0.28, 0.4 and 0.45)			Low Temperature Physics and Superconductivity Department, M.V. Lomonosov Moscow State University, Moscow 119991, Russia	Physica C, 489(2013)32	Y.A. Ovchenkov,D.A. Chareev,E.S. Kozlyakova,O.S. Volkova,A.N. Vasiliev		
153855	PHC4890032	compositions by SEM. Fe-content = 1.03 - - 1.04. Hc2 defined as R=0.5Rn.	Fe1.03Te1-xSex	Fe1.03Te0.5Se0.5	Fe	1.03	Te	0.5	Se	0.5																		3	2013					myu-B/mol	4.1	250	15																				Fe-11																	Fe-11	K	11.9	12.9	13.6				12.9																													T/K	RES(0.5Rn)		8.8	3.76	MHC153855																																																														crystals grown by KCl/NaCl flux technique in evacuated quartz tube for 21 days. T-gradient: high-T(765 C) and low-T(720 C)					Coexistence of superconductivity and magnetism in Fe1+d Te1-xSex (x = 0.1, 0.2, 0.28, 0.4 and 0.45)			Low Temperature Physics and Superconductivity Department, M.V. Lomonosov Moscow State University, Moscow 119991, Russia	Physica C, 489(2013)32	Y.A. Ovchenkov,D.A. Chareev,E.S. Kozlyakova,O.S. Volkova,A.N. Vasiliev		
153856	PHC4920018	compositions by EDX. Bump in R(T) at 230 K( maybe I-M transition). Hc2 defined as R=0.9Rn. Anisotropy(Hc2) = 3.3. Jc(5K,0T) = 1.7E+4 A/cm2	K0.58Fe1.56Se2	K0.58Fe1.56Se2	K	0.58	Fe	1.56	Se	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K			31.9				31.9																				T	RES(0.9Rn), WHH		276	84					T/K	RES(0.9Rn)		12.5	3.8	MHC153856																	17000																																													mixture(K & (Fe+Se)) - alumina crucible - sealed in pure-Fe tube - heat(1050C) - hold(2h) - cool to780C (6C/h)					Upper fields and critical current density of K0.58Fe1.56Se2 single crystals grown by one step technique			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, Beijing 100190, China	Physica C, 492(2013)18	Zhaoshun Gao,Yanpeng Qi,Lei Wang,Chao Yao,Dongliang Wang,Xianping Zhang,Yanwei Ma		
153857	PHC4920090	I,H//[110]. (dC/gamma*Tc) = 0.85. thermodynamic Hc(0) = 218 Oe.[cohere],[penet] estimated from Hc(0) and GL theory. G-L = 12.6. e-ph = 0.53. dC at Tc = 17 mJ/mol.K	Y3Ru4Ge13	Y3Ru4Ge13	Y	3	Ru	4	Ge	13																		3	2013																										A3B4C13		Yb3Rh4Sn13	Pm3n		A	8.9723														K				2.85			2.85											Oe	estimated using GL.	31							T	RES(0.5Rn), WHH, for H//[110]	4.91							T/K	RES(0.5Rn)	2.49					nm	GL, Hc(0)	39.3			nm	GL, Hc(0)	495.1			meV	0.21	1.7	14							mJ/mol.K2	7.08	SP	222.9	SP											uOhm.cm		93										77											Y(3N),Ru(5N),Ge(5N)		Czochralski method using tetra-arc furnace. W-seeded rod, pulling rate 10 mm/h.					Superconductivity in a low carrier density system: A single crystal study of cubic Y3Ru4Ge13			Dept. of Condensed Matter Physics and Material Science, Tata Institute of Fundamental Research, Dr. Homi Bhabha Road, Colaba, Mumbai 400 005, India	Physica C, 492(2013)92	Om Prakash,A. Thamizhavel,A.K. Nigam,S. Ramakrishnan		
153858	PRB087020504	impurity phase : Bi2S3(15%)	SrFBiS2	Sr1F1Bi1S2	Sr	1	F	1	Bi	1	S	2																1	2013																										ABCD2	2		P4/nmm		A	4.082		13.8025											BiS2 layerd	K					2																																																																																																La,SrF2,Bi,S		two step solid state reaction. La2S3 firstly made ( mixture(La,S) - heat(873K,10h)). mixture(La2S3,SrS,SrF2,Bi,S) - pellet - heat(1073K,10h,in quartz tube) - FC to RT					Superconductivity induced by La doping in Sr1-xLaxFBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 87(2013)020504	Xi Lin,Xinxin Ni,Bin Chen,Xiaofeng Xu,Xuxin Yang,Jianhui Dai,Yuke Li,Xiaojun Yang,Yongkang Luo,Qian Tao,Guanghan Cao,Zhuan Xu		
153859	PRB087020504	impurity phase : Bi2S3(12%). Hc2(T) by GL theory. carrier concentration at 2K in DB. lattice term in SP (beta) = 0.414 mJ/mol.K4. (dC/gamma*Tc) = 1.4	(Sr,La)FBiS2	Sr0.5La0.5F1Bi1S2	Sr	0.5	La	0.5	F	1	Bi	1	S	2														1	2013																										ABCD2	2				A	4.0822		13.335											BiS2 layerd	K			2.8				2.8										20										T	RES(0.9Rn), Hc2(T) by GL	1.04												MHC153859																						mJ/mol.K2	1.42	SP	265	SP																									m3/C						MRH153859	n/cm3	10500000000000000000	La,SrF2,Bi,S		two step solid state reaction. La2S3 firstly made ( mixture(La,S) - heat(873K,10h)). mixture(La2S3,SrS,SrF2,Bi,S) - pellet - heat(1073K,10h,in quartz tube) - FC to RT					Superconductivity induced by La doping in Sr1-xLaxFBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 87(2013)020504	Xi Lin,Xinxin Ni,Bin Chen,Xiaofeng Xu,Xuxin Yang,Jianhui Dai,Yuke Li,Xiaojun Yang,Yongkang Luo,Qian Tao,Guanghan Cao,Zhuan Xu		
153860	PRB087024508	High-T synthesis.  Zr:Tl = 1:3 by EDS, WDS. T<CDW> = 61 K. SC due to disorder along a-c plane. Hc1(2K)//b-axis = 4 Oe. residual gamma = 1.1 mJ/mol.K2	Te3Zr	Te3Zr1	Te	3	Zr	1																				3	2013																										AB3	4	TiS3	P2<1>/m	11	A	5.917	3.948	10.155											monoclinic. alpha=90, beta=97.90, gamma=90	K			4	3			3										60	Oe	M-H curve, H//b-axis					4		2																																					mJ/mol.K2	2.4	SP																																						Chemical transport method using iodine as agent. Low-T synthesis: 735C(source)/660C(sink)					Disorder-induced bulk superconductivity in ZrTe3 single crystals via growth control			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 87(2013)024508	Xiyu Zhu,Bing Lv,Fengyan Wei,Yuyi Xue,Bernd Lorenz,Liangzi Deng,Yanyi Sun,Ching-Wu Chu		
153861	PRB087024508	Low-T synthesis. Zr:Tl = 1:3 by EDS, WDS.  not SC. T<CDW> = 72 K.	Te3Zr	Te3Zr1	Te	3	Zr	1																				3	2013																										AB3	4	TiS3	P2<1>/m	11	A	5.898	3.924	10.109											monoclinic. alpha=90, beta=97.88, gamma=90	K					2																																																																																																		Chemical transport method using iodine as agent. High-T synthesis: 950C(source)/850C(sink)					Disorder-induced bulk superconductivity in ZrTe3 single crystals via growth control			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 87(2013)024508	Xiyu Zhu,Bing Lv,Fengyan Wei,Yuyi Xue,Bernd Lorenz,Liangzi Deng,Yanyi Sun,Ching-Wu Chu		
153862	JPS076S0120	impurity phase: SrMoO4. Tc defined as Tc(on). Tm independent of P.	MoSr2YCu2O8	Mo1Sr2Y1Cu2O8-z	Mo	1	Sr	2	Y	1	Cu	2													O	8-z		1	2007								9.9																				M1212	P4/mmm																Mo-1212	K			39.8				39.8	TC153862		K/GPa	3.3																																																																																										Y2O3,CuO,SrCO3,Mo		solid state reaction					Pressure Effects on the Physical and Magnetic Properties of MoSr2YCu2O8-z Oxide Superconductor			Graduate School of Science and Technology, Niigata University, Ikarashi 2-8050, Niigata 950-2181	J.Phys.Soc.Jpn. Suppl.A, 76(2007)120	Ado Kaeriyama,Mitsuru Ueno,Kazunori Fukuda,Kenta Udagawa,Fumihiro Ishikawa,Yuh Yamada,Akiyuki Matsushita		
153863	JPS076S0120	impurity phase: SrMoO4. Tc defined as Tc(on)	MoSr2(Y,Ca)Cu2O8	Mo1Sr2Y0.93Ca0.07Cu2O8-z	Mo	1	Sr	2	Y	0.93	Ca	0.07	Cu	2											O	8-z		1	2007																												M1212	P4/mmm																Mo-1212	K			50.1				50.1	TC153862		K/GPa	3.5																																																																																										Y2O3,CuO,SrCO3,Mo		solid state reaction					Pressure Effects on the Physical and Magnetic Properties of MoSr2YCu2O8-z Oxide Superconductor			Graduate School of Science and Technology, Niigata University, Ikarashi 2-8050, Niigata 950-2181	J.Phys.Soc.Jpn. Suppl.A, 76(2007)120	Ado Kaeriyama,Mitsuru Ueno,Kazunori Fukuda,Kenta Udagawa,Fumihiro Ishikawa,Yuh Yamada,Akiyuki Matsushita		
153864	PRB087054504	residual [gamma] = 5 mJ/mol.K2. (dC/Tc) = 5.2 mJ/mol.K2.	LiFeP	Li1Fe1P1	Li	1	Fe	1	P	1																		1	2013																										ABC		PbFCl																	Fe-111	K		4.86					4.86																																																					MSP153864			mJ/mol.K2	9.2	SP																																						mixture(Li3P,Fe,P) - pellet - sealed in Nb tube(1 atm-Ar) - heat(700C,20h, in evacuated quartz tube)					LiFeP: A nodal superconductor with an unusually large (dC/Tc)			Department of Physics, University of Florida, Gainesville, Florida 32611-8440, USA	Phys.Rev.B, 87(2013)054504	J. S. Kim,L. Y. Xing,X. C. Wang,C. Q. Jin,G. R. Stewart		
153865	PRB087060501	not SC. Anomaly in R(T) at 150 K (= T<SDW>)	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9396		8.4921											ZrCuSiAs, Fe-1111	K					4																																																																																							m3/C						RH153865			SmAs,U3O8,FeAs,Fe,Fe2O3		mixture - pellet - sealed in evacuated quartz tube - heat(1180C,90h) - FC to RT					Superconductivity induced by U doping in the SmFeAsO system			Key Laboratory of Radiation Physics and Technology, Ministry of Education, Institute of Nuclear Science and Technology, Sichuan University, Chengdu 610064, People's Republic of China	Phys.Rev.B, 87(2013)060501	Bo Huang,Jijun Yang,Jun Tang,Jiali Liao,Yuanyou Yang,Ning Liu,Gang Mu,Tao Hu,Xiaoping Shen,Donglai Feng		
153866	PRB087060501	impurity phase: UO2	(Sm,U)OFeAs	Sm0.9U0.1Fe1As1O1	Sm	0.9	U	0.1	Fe	1	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9315		8.4654											ZrCuSiAs, Fe-1111	K			47				47																																																																																					m3/C						RH153865			SmAs,U3O8,FeAs,Fe,Fe2O3		mixture - pellet - sealed in evacuated quartz tube - heat(1180C,90h) - FC to RT					Superconductivity induced by U doping in the SmFeAsO system			Key Laboratory of Radiation Physics and Technology, Ministry of Education, Institute of Nuclear Science and Technology, Sichuan University, Chengdu 610064, People's Republic of China	Phys.Rev.B, 87(2013)060501	Bo Huang,Jijun Yang,Jun Tang,Jiali Liao,Yuanyou Yang,Ning Liu,Gang Mu,Tao Hu,Xiaoping Shen,Donglai Feng		
153867	PRB087060501	impurity phase: UO2	(Sm,U)OFeAs	Sm0.8U0.2Fe1As1O1	Sm	0.8	U	0.2	Fe	1	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9214		8.4165											ZrCuSiAs, Fe-1111	K			49	46			46																				T	RES(0.95Rn), WHH	250							T/K	RES(0.95Rn)	7.4																																																						m3/C						RH153865			SmAs,U3O8,FeAs,Fe,Fe2O3		mixture - pellet - sealed in evacuated quartz tube - heat(1180C,90h) - FC to RT					Superconductivity induced by U doping in the SmFeAsO system			Key Laboratory of Radiation Physics and Technology, Ministry of Education, Institute of Nuclear Science and Technology, Sichuan University, Chengdu 610064, People's Republic of China	Phys.Rev.B, 87(2013)060501	Bo Huang,Jijun Yang,Jun Tang,Jiali Liao,Yuanyou Yang,Ning Liu,Gang Mu,Tao Hu,Xiaoping Shen,Donglai Feng		
153868	PRB087060507		Ca10(Pt3As8)(Fe2As2)5	Ca10Pt3Fe10As18	Ca	10	Pt	3	Fe	10	As	18																3	2013																											5		P-1																10-3-8 phase	K					2																																																										mJ/mol.K2	4.8	SP	256	SP											mOhm.cm												0.57									n/cm3	8700000000000000000000			CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153869	PRB087060507	La-content x by WDS.two kink point in (dR/dT); 103 K (STR) and 95 K (MAG). lattice term in SP (beta) = 0.95 mJ/mol-Fe2.K4. [gamma] in mol-Fe2	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca9.79La0.21Pt3Fe10As18	Ca	9.79	La	0.21	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K					2																																																																																																		CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153870	PRB087060507	La-content x by WDS.	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca9.57La0.43Pt3Fe10As18	Ca	9.57	La	0.43	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K		13.3		14.6			13.3																																																																																																CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153871	PRB087060507	La-content x by WDS.	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca9.35La0.65Pt3Fe10As18	Ca	9.35	La	0.65	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K		19.7		21.4			19.7																																																																																																CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153872	PRB087060507	La-content x by WDS. [gamma] in mJ/mol-Fe2.K2. (dC/Tc) = 13 mJ/mol-Fe2.K	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca9.07La0.93Pt3Fe10As18	Ca	9.07	La	0.93	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K		22.2		22.7			22.2	MPH153872																																																							mJ/mol.K2	5.8	SP	257	SP																																				CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153873	PRB087060507	La-content x by WDS.	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca8.55La1.45Pt3Fe10As18	Ca	8.55	La	1.45	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K		26.1		26.5			26.1	MPH153872																			T	RES(0.95Rn), WHH		400	60										MHC153873																																																										n/cm3	10600000000000000000000			CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153874	PRB087060507	La-content x by WDS.	(Ca,La)10(Pt3As8)(Fe2As2)5	Ca8.18La1.82Pt3Fe10As18	Ca	8.18	La	1.82	Pt	3	Fe	10	As	18														3	2013																											5		P-1																10-3-8 phase	K		22.1		25.2			22.1																																																																																																CaAs-rich flux. CaAs, FeAs, and LaAs precursors were made using the solid state reaction. mixture(precursors+Pt) - pellet - Al2O3 crucible - quartz tube - heat(1150C,96h) - slow cool to 885C - quench					Transport and thermodynamic properties of (Ca1-xLax)10(Pt3As8)(Fe2As2)5 superconductors			Los Alamos National Laboratory, Los Alamos, New Mexico 87544, USA	Phys.Rev.B, 87(2013)060507	N. Ni,W. E. Straszheim,D. J. Williams,M. A. Tanatar,R. Prozorov,E. D. Bauer,F. Ronning,J. D. Thompson,R. J. Cava		
153875	PRB085085108	not SC. RRR = 1.35. <243>Am isotope, Am:Pd:Al = 1:5:1.70 by EDX. Hall coeff. = -2 E-10 m3/C for T>100K. Thermopower ; see Fig.5	AmPd5Al2	Am1Pd5Al2	Am	1	Pd	5	Al	2																		3	2012																										AB2C5		ZrNi2Al5	I4/mmm	139	A	4.1298		14.792												K					2																																																										mJ/mol.K2	19	SP	295	SP						uV/K	-1.2				uOhm.cm											16.8			m3/C	-0.0000000002								Pd(4N),Al(5N),Am(99.85)		arc-melting. Single crystal(50*50*20 um3 extracted from button					Crystal structure and physical properties of <243>AmPd5Al2			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, D-76125 Karlsruhe, Germany	Phys.Rev.B, 85(2012)085108	J.-C. Griveau,K. Gofryk,D. Bouexiiere,E. Colineau,J. Rebizant		
153876	PRB085060503	RRR = 150. GL(kappa) = 4.4. nodal energy gap.	LiFeP	Li1Fe1P1	Li	1	Fe	1	P	1																		3	2012																										ABC		PbFCl			A	3.6955		6.0411											Fe-111	K		4.9	5.3				4.9																				T	RES(0.5Rn), WHH		1.7	0.29					T/K	RES(0.5Rn)			0.085	MHC153876		nm	from Hc2		34	5.8	nm			150																											uOhm.cm											310												Li(ingot),FeAs/FeP(powder)		self-flux method. mixture in BN crucible - sealed in quartz tube - heat to 1100C - slow cool to 600C					Contrasts in electron correlations and inelastic scattering between LiFeP and LiFeAs revealed by charge transport			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 85(2012)060503	S. Kasahara,K. Hashimoto,H. Ikeda,T. Terashima,Y. Matsuda,T. Shibauchi		
153877	PRB085060503	RRR = 150. GL(kappa) = 51. nodeless energy gap.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2012																										ABC		PbFCl			A	3.7914		6.3639											Fe-111	K		17.3	17.8				17.3																				T	RES(0.5Rn), WHH		48	20					T/K	RES(0.5Rn)			1.6	MHC153877		nm	from Hc2		4.1	1.6	nm			210																											uOhm.cm											690												Li(ingot),FeAs/FeP(powder)		self-flux method. mixture in BN crucible - sealed in quartz tube - heat to 1100C - slow cool to 600C					Contrasts in electron correlations and inelastic scattering between LiFeP and LiFeAs revealed by charge transport			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 85(2012)060503	S. Kasahara,K. Hashimoto,H. Ikeda,T. Terashima,Y. Matsuda,T. Shibauchi		
153878	SST026075001	SP-heat coeff. (beta) = 1.58 mJ/mol.K4, (delta) = 0.14 mJ/mol.K6. (dC/gamma*Tc) = 1.29. R(T) has anomaly at 270 K (STR transition by XRD)	SrPt2Sb2	Sr1Pt2Sb2	Sr	1	Pt	2	Sb	2																		1	2013																										AB2C2		ThCr2Si2			A	4.603		10.565												K	2.1			2.1			2.1										114	Oe	M-H curve				6			1.8	T	M-H curve				0.1			1.8																												mJ/mol.K2	9.2	SP	183	SP																																		Sr(3N),Pt(3N),Sb(5N)		mixture(Sr:Pt:Sb=1.03:2:2) - arc-melting - remelt - sealed in BN - heat(1470C,2h) - cool to 1160C with 5 K/min					Superconductivity in 122 antimonide SrPt2Sb2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	Supercond.Sci.Technol., 26(2013)075001	Motoharu Imai,Satoshi Emura,Mitsuaki Nishio,Yoshitaka Matsushita,Soshi Ibuka,Naoya Eguchi,Fumihiro Ishikawa,Yuh Yamada,Takahiro Muranaka,Jun Akimitsu		
153879	PRB087064502	RRR = 19. Two gaps analysis of SP-data: D1(lower) = 0.8 kTc, D2(higher) = 2.0 kTc. [penet](T) = A*T^n , (n = 3.2).	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		3	2013																										AB4C12		skutterudite			A	8.6105														K	7.8			7.8			7.8																																									nm	muon-SR, TDO	114					4	14							mJ/mol.K2	69	SP	190	SP											uOhm.cm											3.5												Pr(3N),Pt(3N),Ge(6N)		arc-melting - glassy carbon crucible - heat(800C,120h in silica tube) - powdered - pellet - glassy carbon crucible - weld in Ta-container - heat(85-67C,60d)					Multiband superconductivity in PrPt4Ge12 single crystals			Department of Physics and Center for Correlated Matter, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 87(2013)064502	J. L. Zhang,Y. Chen,L. Jiao,R. Gumeniuk,M. Nicklas,Y. H. Chen,L. Yang,B. H. Fu,W. Schnelle,H. Rosner,A. Leithe-Jasper,Y. Grin,F. Steglich,H. Q. Yuan		
153880	PRB086060516		Ca10(Pt4As8)(FeAs)10	Ca10Pt4Fe10As18	Ca	10	Pt	4	Fe	10	As	18																1	2012																																													Ca-10-4-8 phase	K		38					38																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153881	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt4.1Fe9.9As18	Ca	10	Pt	4.1	Fe	9.9	As	18																1	2012																																													Ca-10-4-8 phase	K		32.2					32.2																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153882	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt4.3Fe9.7As18	Ca	10	Pt	4.3	Fe	9.7	As	18																1	2012																																													Ca-10-4-8 phase	K		33.9					33.9	MTC153882																																																																																															solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153883	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt4.6Fe9.4As18	Ca	10	Pt	4.6	Fe	9.4	As	18																1	2012																																													Ca-10-4-8 phase	K		22.5					22.5	MTC153882																																																																																															solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153884	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt5Fe9As18	Ca	10	Pt	5	Fe	9	As	18																1	2012																																													Ca-10-4-8 phase	K		9.78					9.78																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153885	PRB086060516		Ca10(Pt3As8)(Fe1-xPtxAs)10	Ca10Pt3.33Fe9.67As18	Ca	10	Pt	3.33	Fe	9.67	As	18																1	2012																																													Ca-10-3-8 phase	K		0					0																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153886	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt3.42Fe9.58As18	Ca	10	Pt	3.42	Fe	9.58	As	18																1	2012																																													Ca-10-3-8 phase	K		10.96					10.96																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153887	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt3.51Fe9.49As18	Ca	10	Pt	3.51	Fe	9.49	As	18																1	2012																																													Ca-10-3-8 phase	K		12.44					12.44	MTC153887																																																																																															solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153888	PRB086060516		Ca10(Pt4As8)(Fe1-xPtxAs)10	Ca10Pt3.72Fe9.28As18	Ca	10	Pt	3.72	Fe	9.28	As	18																1	2012																																													Ca-10-3-8 phase	K		14.9					14.9	MTC153887																																																																																															solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153889	PRB086060516	electron doped Ca-10-3-8 phase	(Ca0.8La0.2)10(Pt4As8)(Fe1-xPtxAs)10	Ca8La2Pt3.3Fe9.7As18	Ca	8	La	2	Pt	3.3	Fe	9.7	As	18														1	2012																																													Ca-10-3-8 phase	K		29.4					29.4																																																																																																solid state reaction. See Angew.Chem.Int.Ed., 50(2011)9195					Role of different negatively charged layers in Ca10(FeAs)10(Pt4As8) and superconductivity at 30 K in electron-doped (Ca0.8La0.2)10(FeAs)10(Pt3As8)			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany	Phys.Rev.B, 86(2012)060516	Tobias Sturzer,Gerald Derondeau,Dirk Johrendt		
153890	PRB087064512	SC parameters in DB calculated using Hc2(SUS). GL(kappa) = 55. [cohere](Pippard) = 181 nm. [penet](London) = 48.3 nm.	AgSnSe2	Ag1Sn1Se2	Ag	1	Sn	1	Se	2																		1	2013	emu/g	0.000000042																								ABC2		NaCl	Fm3m		A	5.675														K				4.55			4.55											mT	M-H curve	1.58							T	Tc(SUS), WHH	2.26												MHC153890		nm	from Hc2	12.5			nm	Hc1,Hc2,GL theory	685					3.85	14																																											n/cm3	20000000000000000000000	Ag(5N),Sn(4N),Se(5N)		mixture - sealed in quartz tube - melt(800C,48h) - quench to cold water - ANN(450C,2w) - quench to cold water					Anomalous metallic state above the upper critical field of the conventional three-dimensional superconductor AgSnSe2 with strong intrinsic disorder			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 87(2013)064512	Zhi Ren,M. Kriener,A. A. Taskin,Satoshi Sasaki,Kouji Segawa,Yoichi Ando		
153891	PRB087094503	RRR = 4.5. Anisotropy (Hc2) = 1.22(1.5K), 1.554(15K). Tc by TDR.	SrFe2(As,P)2	Sr1Fe2As1.3P0.7	Sr	1	Fe	2	As	1.3	P	0.7																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		23.3	25				23.3																																		MHC153891																																					uOhm.cm												300													Self-flux method.					Upper critical field of isoelectron substituted SrFe2(As1-xPx)2			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)094503	S. Yeninas,M. A. Tanatar,J. Murphy,C. P. Strehlow,O. E. Ayala-Valenzuela,R. D. McDonald,U. Welp,W. K. Kwok,T. Kobayashi,S. Miyasaka,S. Tajima,R. Prozorov		
153892	PRB087094503	E=1.4 GeV-Pb-ion irradiated sample. dose = 1.2 E+12 ion/cm2. Anisotropy (Hc2) = 1.22(1.5K), 1.354(15K). Tc by TDR.	SrFe2(As,P)2	Sr1Fe2As1.3P0.7	Sr	1	Fe	2	As	1.3	P	0.7																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		23.3					23.3																																		MHC153892																																																														Self-flux method.					Upper critical field of isoelectron substituted SrFe2(As1-xPx)2			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)094503	S. Yeninas,M. A. Tanatar,J. Murphy,C. P. Strehlow,O. E. Ayala-Valenzuela,R. D. McDonald,U. Welp,W. K. Kwok,T. Kobayashi,S. Miyasaka,S. Tajima,R. Prozorov		
153893	PRB087094505	slightly overdoped sample. angular dependence of Hc2 were measured at various temperatures.	Ba(Fe,Ni)2As2	Ba1Fe1.892Ni0.108As2	Ba	1	Fe	1.892	Ni	0.108	As	2																3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		16					16																																		MHC153893																																																														FeAs flux method					Angular-dependent upper critical field of overdoped Ba(Fe1-xNix)2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)094505	J. Murphy,M. A. Tanatar,D. Graf,J. S. Brooks,S. L. Bud'ko,P. C. Canfield,V. G. Kogan,R. Prozorov		
153894	PRB087094505	strongly overdoped sample. angular dependence of Hc2 were measured at various temperatures.	Ba(Fe,Ni)2As2	Ba1Fe1.856Ni0.144As2	Ba	1	Fe	1.856	Ni	0.144	As	2																3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		7.5					7.5																																		MHC153894																																																														FeAs flux method					Angular-dependent upper critical field of overdoped Ba(Fe1-xNix)2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)094505	J. Murphy,M. A. Tanatar,D. Graf,J. S. Brooks,S. L. Bud'ko,P. C. Canfield,V. G. Kogan,R. Prozorov		
153895	PRB087094508	broad hump at 180 K in R(T). No structural transition. Tc(H//ab) = 28 K, and Tc(H//c) = 25 K by TDO. difference between Tc(RES) and Tc(TDO) due to air degradation.	K0.83Fe1.83Se2	K0.83Fe1.83Se2	K	0.83	Fe	1.83	Se	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		32.5					32.5																				T	TDO, extrapolation		73.9	55.4										MHC153895																																																														Optical floating zone method					Upper critical magnetic field of KxFe2-ySe2 and Eu0.5K0.5Fe2As2 single crystals			Institute of Solid State Physics RAS, 142432 Chernogolovka, Moscow District Russian Federation	Phys.Rev.B, 87(2013)094508	Vitaly A. Gasparov,A. Audouard and L. Drigo,A. I. Rodigin,C. T. Lin,W. P. Liu,M. Zhang,A. F. Wang,X. H. Chen,H. S. Jeevan,J. Maiwald,P. Gegenwart		
153896	PRB087094508	Hc2//ab = 73.9, Hc2//c = 55.4 T obtained by extrapolation. Anisotropy = 2 near Tc.	K0.8Fe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		32.5					32.5																				T	TDO, WHH		120	36					T/K	TDO		5.5	1.68	MHC1538956		nm	from Hc2		2.83	1.2																																																								High temperature flux method					Upper critical magnetic field of KxFe2-ySe2 and Eu0.5K0.5Fe2As2 single crystals			Institute of Solid State Physics RAS, 142432 Chernogolovka, Moscow District Russian Federation	Phys.Rev.B, 87(2013)094508	Vitaly A. Gasparov,A. Audouard and L. Drigo,A. I. Rodigin,C. T. Lin,W. P. Liu,M. Zhang,A. F. Wang,X. H. Chen,H. S. Jeevan,J. Maiwald,P. Gegenwart		
153897	PRB087094508	Hc2//ab = 65.9, Hc2//c = 54.8 T obtained by extrapolation. Anisotropy nealy T-independent.	(Eu,K)Fe2As2	Eu0.5K0.5Fe2As2	Eu	0.5	K	0.5	Fe	2	As	2																3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		31.5					31.5																				T	TDO, WHH		115	75					T/K	TDO		5.3	3.5	MHC153897		nm	from Hc2		2.1	1.36																																																								self flux method					Upper critical magnetic field of KxFe2-ySe2 and Eu0.5K0.5Fe2As2 single crystals			Institute of Solid State Physics RAS, 142432 Chernogolovka, Moscow District Russian Federation	Phys.Rev.B, 87(2013)094508	Vitaly A. Gasparov,A. Audouard and L. Drigo,A. I. Rodigin,C. T. Lin,W. P. Liu,M. Zhang,A. F. Wang,X. H. Chen,H. S. Jeevan,J. Maiwald,P. Gegenwart		
153898	PRB087094515	Tc,[penet] by TDR measurements. London's [penet] = 50 nm using single gap model. Campbwll penetration depth also estimated.	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		2.7					2.7																				T	TDR, Helfand-Werthamer theory	0.4817																			nm	TDR, superfluid density		426																																																				self flux method					Magnetic penetration depth in single crystals of SrPd2Ge2 superconductor			The Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)094515	H. Kim,N. H. Sung,B. K. Cho,M. A. Tanatar,R. Prozorov		
153899	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.8K0.2Fe2As2	Ba	0.8	K	0.2	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		7.28					7.28			K/GPa	5.7																																																		mJ/mol.K	4.43																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153900	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.7K0.3Fe2As2	Ba	0.7	K	0.3	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		37.4					37.4	MTC153900		K/GPa	-0.29																																																		mJ/mol.K	4703																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153901	PRB087100509	Optimal sample. Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		38					38	MTC153900		K/GPa	-0.37																																																		mJ/mol.K	3054																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153902	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.4K0.6Fe2As2	Ba	0.4	K	0.6	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		28.7					28.7	MTC153900		K/GPa	-0.62																																																		mJ/mol.K	1760																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153903	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.3K0.7Fe2As2	Ba	0.3	K	0.7	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		19.4					19.4			K/GPa	-1.07																																																		mJ/mol.K	434																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153904	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.2K0.8Fe2As2	Ba	0.2	K	0.8	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		11.7					11.7			K/GPa	-2.01																																																		mJ/mol.K	559																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153905	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	(Ba,K)Fe2As2	Ba0.1K0.9Fe2As2	Ba	0.1	K	0.9	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		6.86					6.86			K/GPa	-1.6																																																		mJ/mol.K	317																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153906	PRB087100509	Tc(P) measured by DC-magnetization upto 1.2 GPa.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		1	2013																										AB2C2		ThCr2Si2																	Fe-122	K		3					3			K/GPa	-1.02																																																		mJ/mol.K	225																																							KAs,BaAs,Fe2As		mixture - load in alumina crucible - in Nb-tube sealed in quartz tube - preheat(600C,12h) - reground - pellet - heat(800-1100C, 24-48h, depends on compositions)					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xKxFe2As2 (0.2 =< x  =<  1.0) series			Ames Laboratory, US DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)100509	Sergey L. Bud'ko,Mihai Sturza,Duck Young Chung,Mercouri G. Kanatzidis,Paul C. Canfield		
153907	PRB087104515	STR transition at T<STR> = 53 K. Lattice term in SP (beta) = 0.64 mJ/mol.K2. e-ph = 0.59. N(0) = 8.5 stats/eV.f.u. Curie Weis law for 220 < T. (dC/gamma*Tc) = 1.49	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2013					Myu-B/Mo	1.67	-1078																			A3B7		Ir3Ge7	IM3[-]m	229															phase transition at 53 K(a=9.551, c=9.523	K		2.35		2.35			2.35																																																								mJ/mol.K2	31.8	SP, fitting for 2.8<T<6 K	248	SP, fitting for 2.8<T<6 K	W/m.K				MTHC153907	uV/K	16			MTP153907	uOhm.cm											160												Mo(5N),Sb(6N)		mixture(reduced Mo:Sb = 1:49) - in 2 ml Al2O3 crucible - sealed ampoule - heat(1000C,5h) - homogenize(12h) - cool to 700C over 100h - decant at 700C					Flux growth and physical properties of Mo3Sb7 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 87(2013)104515	J.-Q. Yan,M. A. McGuire,A. F. May,H. Cao,A. D. Christianson,D. G. Mandrus,B. C. Sales		
153908	PRB087134502	RRR = 10. Tc, Hc2 measured by SUS. (dTc/dP) = 0.22 K/GPa for 9<P<14 GPA, and = 0.16 K/GPa for P > 14 GPa..	2H-NbS2	Nb1S2	Nb	1	S	2																				3	2013																										AB2		2H-NbSe2																	2H-NbS2	K				6			6	MTC153908		K/GPa	0.09																T	SUS, extrapolation	2.6												MHC153908																																																														See Inorg.Chem., 19(1980)39					Pressure dependence of superconducting critical temperature and upper critical field of 2H-NbS2			Institute of Solid State Physics, Chernogolovka, 142432 Moscow Region, Russia	Phys.Rev.B, 87(2013)134502	V. G. Tissen,M. R. Osorio,J. P. Brison,N. M. Nemes,M. Garcia-Hernandez,L. Cario,P. Rodiere,S. Vieira,H. Suderow		
153909	PRB087134512	average composition: FeSe0.89-0.90.  85%-tetra-phase, minor phase: hexagonal (a=3.605, c=5.889 A).	FeSe	Fe1Se1	Fe	1	Se	1																				3	2013																										AB		PbO			A	3.78		5.49												K	8.65	9.9	12				9.9																				T	RES(0.9Rn), WHH		34	29					T/K	RES(0.9Rn)		5	3.65	MHC153909		A	from Hc2		33	28.5																																																								crystals grown by KCl-solution-mwlt free grown method					Temperature dependence of the upper critical field of FeSe single crystals			Laboratoire National des Champs Magnetiques Intenses, CNRS-UJF-UPS-INSA, 25 avenue des Martyrs, 38042 Grenoble, France	Phys.Rev.B, 87(2013)134512	S. I. Vedeneev,B. A. Piot,D. K. Maude,A. V. Sadakov		
153910	PRB087134513	RRR = 2500-3000.Hc2 criterion (Rn, 0.9Rn, 0.5Rn,R-0) discussed.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		3.8		3.5			3.8																				T	RES(0.5Rn), WHH			1.5										MHC153910		nm	from Hc2		20																																																									KAs flux method. mixture(K:Fe:As=5:2:6) - alumina crucible with Sn chunk on the bottom - sealed in quartz tube - heat - cool from 920C to 820C (4C/h) - cool to 620C (1C/h)					Upper critical field of high-quality single crystals of KFe2As2			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)134513	Yong Liu,M. A. Tanatar,V. G. Kogan,Hyunsoo Kim,T. A. Lograsso,R. Prozorov		
153911	PRB087094501	Na-content estimated from Tc(x). band dependent gaps. higher one(in DB) for inner <gamma> barrel, lower : (2d/kTc) = 3.15 for outer <gamma> barrel. gap by ARPES.	(Ca,Na)Fe2As2	Ca0.8Na0.2Fe2As2	Ca	0.8	Na	0.2	Fe	2	As	2																3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		14					14																																														meV	3.5	5.81	12																																																				Electronic band structure and momentum dependence of the superconducting gap in Ca1-xNaxFe2As2 from angle-resolved photoemission spectroscopy			Institute for Solid State Research, IFW Dresden, P. O. Box 270116, D-01171 Dresden, Germany	Phys.Rev.B, 87(2013)094501	D. V. Evtushinsky,V. B. Zabolotnyy,L. Harnagea,A. N. Yaresko,S. Thirupathaiah,A. A. Kordyuk,J. Maletz,S. Aswartham,S. Wurmehl,E. Rienks,R. Follath,B. Buchner,S. V. Borisenko		
153912	PRB087094501	energy gap measured by ARPES. band dependent gaps. higher one(in DB) for inner <gamma> barrel, lower : (2d/kTc) = 1.62 for outer <gamma> barrel.	(Ca,Na)Fe2As2	Ca0.32Na0.68Fe2As2	Ca	0.32	Na	0.68	Fe	2	As	2																3	2013																										AB2C2		ThCr2Si2																	Fe-122	K		33					33																																														meV	7.8	5.46	12																																																				Electronic band structure and momentum dependence of the superconducting gap in Ca1-xNaxFe2As2 from angle-resolved photoemission spectroscopy			Institute for Solid State Research, IFW Dresden, P. O. Box 270116, D-01171 Dresden, Germany	Phys.Rev.B, 87(2013)094501	D. V. Evtushinsky,V. B. Zabolotnyy,L. Harnagea,A. N. Yaresko,S. Thirupathaiah,A. A. Kordyuk,J. Maletz,S. Aswartham,S. Wurmehl,E. Rienks,R. Follath,B. Buchner,S. V. Borisenko		
153950	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.98Ru0.02As1F0.11O0.89	La	1	Fe	0.98	Ru	0.02	As	1	F	0.11											O	0.89			2013																										ABCD		oxypnictide																	Fe-1111	K		27.4					27.4																																																																																																					Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153951	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.9Ru0.1As1F0.11O0.89	La	1	Fe	0.9	Ru	0.1	As	1	F	0.11											O	0.89			2013																										ABCD		oxypnictide																	Fe-1111	K		23.7					23.7																																																																																																					Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153952	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.8Ru0.2As1F0.11O0.89	La	1	Fe	0.8	Ru	0.2	As	1	F	0.11											O	0.89			2013								0																		ABCD		oxypnictide																	Fe-1111	K		19.7					19.7	MPH153953																			T	SUS, WHH	49.7																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153953	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.75Ru0.25As1F0.11O0.89	La	1	Fe	0.75	Ru	0.25	As	1	F	0.11											O	0.89			2013								11																		ABCD		oxypnictide																	Fe-1111	K		17.6					17.6	MPH153953																			T	SUS, WHH	48.7																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153954	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.7Ru0.3As1F0.11O0.89	La	1	Fe	0.7	Ru	0.3	As	1	F	0.11											O	0.89			2013								0																		ABCD		oxypnictide																	Fe-1111	K		18.3					18.3	MPH153953																			T	SUS, WHH	42.1																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153955	PRB087134518		La(O,F)(Fe,Ru)As	La1Fe0.5Ru0.5As1F0.11O0.89	La	1	Fe	0.5	Ru	0.5	As	1	F	0.11											O	0.89			2013																										ABCD		oxypnictide																	Fe-1111	K		13.6					13.6																				T	SUS, WHH	26.4																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153956	PRB087134518		La(O,F)FeAs	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89			2013																										ABCD		oxypnictide																	Fe-1111	K		28					28																				T	SUS, WHH	88.7																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153957	PRB087134518		Nd(O,F)(Fe,Ru)As	Nd1Fe0.98Ru0.02As1F0.11O0.89	Nd	1	Fe	0.98	Ru	0.02	As	1	F	0.11											O	0.89			2013																										ABCD		oxypnictide																	Fe-1111	K		46.7					46.7																																																																																																					Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153958	PRB087134518		Nd(O,F)(Fe,Ru)As	Nd1Fe0.9Ru0.1As1F0.11O0.89	Nd	1	Fe	0.9	Ru	0.1	As	1	F	0.11											O	0.89			2013								0																		ABCD		oxypnictide																	Fe-1111	K		37.4					37.4	MPH153959																																																																																																				Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153959	PRB087134518		Nd(O,F)(Fe,Ru)As	Nd1Fe0.8Ru0.2As1F0.11O0.89	Nd	1	Fe	0.8	Ru	0.2	As	1	F	0.11											O	0.89			2013								6.9																		ABCD		oxypnictide																	Fe-1111	K		22.1					22.1	MPH153959																																																																																																				Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153960	PRB087134518		Nd(O,F)(Fe,Ru)As	Nd1Fe0.7Ru0.3As1F0.11O0.89	Nd	1	Fe	0.7	Ru	0.3	As	1	F	0.11											O	0.89			2013								6.7																		ABCD		oxypnictide																	Fe-1111	K		21.3					21.3	MPH153959																																																																																																				Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153961	PRB087134518		Nd(O,F)(Fe,Ru)As	Nd1Fe0.5Ru0.5As1F0.11O0.89	Nd	1	Fe	0.5	Ru	0.5	As	1	F	0.11											O	0.89			2013								0																		ABCD		oxypnictide																	Fe-1111	K		13.7					13.7																																																																																																					Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153962	PRB087134518		Sm(O,F)(Fe,Ru)As	Sm1Fe0.95Ru0.05As1F0.15O0.85	Sm	1	Fe	0.95	Ru	0.05	As	1	F	0.15											O	0.85			2013								0																		ABCD		oxypnictide																	Fe-1111	K		39.3					39.3																				T	SUS, WHH	140																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153963	PRB087134518		Sm(O,F)(Fe,Ru)As	Sm1Fe0.8Ru0.2As1F0.15O0.85	Sm	1	Fe	0.8	Ru	0.2	As	1	F	0.15											O	0.85			2013								27.5																		ABCD		oxypnictide																	Fe-1111	K		16.9					16.9	MPH153964																			T	SUS, WHH	37.6																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153964	PRB087134518		Sm(O,F)(Fe,Ru)As	Sm1Fe0.7Ru0.3As1F0.15O0.85	Sm	1	Fe	0.7	Ru	0.3	As	1	F	0.15											O	0.85			2013								29.5																		ABCD		oxypnictide																	Fe-1111	K		11.1					11.1	MPH153964																			T	SUS, WHH	21.8																																																																															Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153965	PRB087134518		Sm(O,F)(Fe,Ru)As	Sm1Fe0.5Ru0.5As1F0.15O0.85	Sm	1	Fe	0.5	Ru	0.5	As	1	F	0.15											O	0.85			2013								4.67																		ABCD		oxypnictide																	Fe-1111	K		4.26					4.26																																																																																																					Onset of magnetism in optimally electron-doped LFe1-xRuxAsO1-yFy (L = La, Nd, or Sm) superconductors around x = 1/4			Department of Physics, University of Pavia?CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 87(2013)134518	S. Sanna,P. Carretta,R. De Renzi,G. Prando,P. Bonf,M. Mazzani,G. Lamura,T. Shiroka,Y. Kobayashi,M. Sato		
153966	JPS081053701	STR transition (Trigonal to monoclinic) at Ts ( = 270 K(heating), =236 K(cooling)). lattice const. at RT. SP data for monoclinic phase.	IrTe2	Ir1Te2	Ir	1	Te	2																					2012																										AB2	6		P3[-]m1		A	3.9333		5.4017											STR transitin to monoclinic (C2/m) at Ts	K					0.32																																																										mJ/mol.K2	3.05	SP	212	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153967	JPS081053701	STR transition (Trigonal to monoclinic) at Ts ( = 226 K(heating), = 184 K(cooling)). lattice const. at RT. SP data for monoclinic phase. Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.99Pt0.01Te2	Ir	0.99	Pt	0.01	Te	2																			2012																										AB2	6		P3[-]m1		A	3.9333		5.3966											STR transitin to monoclinic (C2/m) at Ts	K			2.05				2.05																																																								mJ/mol.K2	3.05	SP	209	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153968	JPS081053701	STR transition (Trigonal to monoclinic) at Ts ( = 174 K(heating), = 118 K(cooling)). lattice const. at RT. SP data for monoclinic phase. Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.98Pt0.02Te2	Ir	0.98	Pt	0.02	Te	2																			2012																										AB2	6		P3[-]m1		A	3.9317		5.3915											STR transitin to monoclinic (C2/m) at Ts	K	2.78		2.93				2.855																																																								mJ/mol.K2	4.02	SP	203	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153969	JPS081053701	STR transition (Trigonal to monoclinic) at Ts ( = 157 K(heating), = 90.5 K(cooling)). lattice const. at RT. SP data for monoclinic phase. Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.97Pt0.03Te2	Ir	0.97	Pt	0.03	Te	2																			2012																										AB2	6		P3[-]m1		A	3.9383		5.3932											STR transitin to monoclinic (C2/m) at Ts	K	3.04		3.1				3.07	MPH153969																																																				MSP153969			mJ/mol.K2	5.69	SP	196	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153970	JPS081053701	STR transition for x =< 0.035. (dC/gamma*Tc) = 1.50. Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.96Pt0.04Te2	Ir	0.96	Pt	0.04	Te	2																			2012																										AB2	6		P3[-]m1		A	3.9383		5.3881												K	2.92		2.97				2.945	MPH153969																			T	RES(0.5Rn), WHH	0.17												MHC153970		nm		44															MSP153970			mJ/mol.K2	6.29	SP	195	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153971	JPS081053701	Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.94Pt0.06Te2	Ir	0.94	Pt	0.06	Te	2																			2012																										AB2	6		P3[-]m1		A	3.9417		5.3831												K	2.65		2.73				2.69																																																								mJ/mol.K2	5.88	SP	197	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153972	JPS081053701	Tc in Fig. shows bulk-Tc(SP).	Ir1-xPtxTe2	Ir0.92Pt0.08Te2	Ir	0.92	Pt	0.08	Te	2																			2012																										AB2	6		P3[-]m1		A	3.945		5.378												K	2.2		2.36				2.28																																																					MSP153972			mJ/mol.K2	5.32	SP	198	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153973	JPS081053701	not-SC	Ir1-xPtxTe2	Ir0.9Pt0.1Te2	Ir	0.9	Pt	0.1	Te	2																			2012																										AB2	6		P3[-]m1		A	3.95		5.3746												K					2																																																										mJ/mol.K2	4.76	SP	199	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153974	JPS081053701	not-SC	Ir1-xPtxTe2	Ir0.85Pt0.15Te2	Ir	0.85	Pt	0.15	Te	2																			2012																										AB2	6		P3[-]m1		A	3.955		5.3525												K					2																																																										mJ/mol.K2	4.65	SP	201	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153975	JPS081053701	not-SC	Ir1-xPtxTe2	Ir0.8Pt0.2Te2	Ir	0.8	Pt	0.2	Te	2																			2012																										AB2	6		P3[-]m1		A	3.96		5.3458												K					2																																																										mJ/mol.K2	3.61	SP	207	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153976	JPS081053701	not-SC	Ir1-xPtxTe2	Ir0.75Pt0.25Te2	Ir	0.75	Pt	0.25	Te	2																			2012																										AB2	6		P3[-]m1		A	3.965		5.3322												K					2																																																										mJ/mol.K2	3.16	SP	208	SP																																									Superconductivity Induced by Bond Breaking in the Triangular Lattice of IrTe2			Department of Physics, Faculty of Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 81(2012)053701	Sunseng PYON,Kazutaka KUDO,Minoru NOHARA		
153977	PRB087140507	RRR = 17.	SnTe	Sn1Te1	Sn	1	Te	1																					2013																										AB	1		Fm3[-]m		A	6.321														K					1.8																																																																																																Sn(4N),In(4N),Te(4N)		modified Bridgman method. mixture - sealed in evacuated quartz tube - heat(900C) - slow cool to 700C (2C/h) - fast cool to RT					Superconducting properties of the In-substituted topological crystalline insulator SnTe			Department of Physics, University of Warwick, Coventry, CV4 7AL, United Kingdom	Phys.Rev.B, 87(2013)140507	G. Balakrishnan,L. Bawden,S. Cavendish,M. R. Lees		
153978	PRB087140507	RRR = 1.3. GK(kappa) = 56.4. Lattice term in SP (beta) = 0.635 mJ/mol.K4, (delta) = 8.0 uJ/mol.K6. (dC/gamma*Tc) = 1.26. e-ph = 0.67.	Sn1-xInxTe	Sn0.6In0.4Te1	Sn	0.6	In	0.4	Te	1																			2013																										AB	1		Fm3[-]m		A	6.28														K	3.5		4.7	4.75		1	4.75										98	mT	M-H curve, parabolic T-dependency	0.9							T	RES(R=0), GL-approx.	1.42												MHC153978		nm	from Hc2	15.2			nm	Hc1,Hc2,GL theory	860													mJ/mol.K2	2.62	SP	183	SP																																		Sn(4N),In(4N),Te(4N)		modified Bridgman method. mixture - sealed in evacuated quartz tube - heat(900C) - slow cool to 700C (2C/h) - fast cool to RT					Superconducting properties of the In-substituted topological crystalline insulator SnTe			Department of Physics, University of Warwick, Coventry, CV4 7AL, United Kingdom	Phys.Rev.B, 87(2013)140507	G. Balakrishnan,L. Bawden,S. Cavendish,M. R. Lees		
153980	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 2.57. not SC.	Sn1-xInxTe	Sn0.98In0.008Te1	Sn	0.98	In	0.008	Te	1																		3	2010																										AB																				K					0.7																																																																									uOhm.cm							112														n/cm3	459000000000000000000			vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153981	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 2.60. not SC.	Sn1-xInxTe	Sn0.979In0.009Te1	Sn	0.979	In	0.009	Te	1																		3	2010																										AB																				K					0.7																																																										mJ/mol.K2	0.803	SP													uOhm.cm							87.5														n/cm3	377000000000000000000			vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153982	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.13. Tc(SP) = 0(not bulk SC).	Sn1-xInxTe	Sn0.961In0.027Te1	Sn	0.961	In	0.027	Te	1																		3	2010																										AB																				K			1.85		0.7		1.85																																																																							uOhm.cm							800																		vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153983	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.09. Tc(SP) = 0 (not bulk SC)	Sn1-xInxTe	Sn0.95In0.038Te1	Sn	0.95	In	0.038	Te	1																		3	2010																										AB																				K			1.9		0.7		1.9																																																								mJ/mol.K2	0.796	SP													uOhm.cm							1250														n/cm3	512000000000000000000			vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153984	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.09. Tc(SP) = 1.67. (dC/gamma*Tc) = 0.816.	Sn1-xInxTe	Sn0.927In0.061Te1	Sn	0.927	In	0.061	Te	1																		3	2010																										AB																				K			1.8				1.8																				T	RES.													MHC153984																						mJ/mol.K2	0.973	SP													uOhm.cm							793																		vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153985	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.66. Tc(SP) = 1.74 K. (dC/gamma*Tc) = 0.632	Sn1-xInxTe	Sn0.923In0.065Te1	Sn	0.923	In	0.065	Te	1																		3	2010																										AB																				K			1.8				1.8																				T	RES.													MHC153985																						mJ/mol.K2	1.11	SP													uOhm.cm							437														n/cm3	1140000000000000000000			vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153986	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.40. Tc(SP) = 1.86 K. (dC/gamma*Tc) = 1.14.	Sn1-xInxTe	Sn0.915In0.073Te1	Sn	0.915	In	0.073	Te	1																		3	2010																										AB																				K			1.9				1.9																																																								mJ/mol.K2	1.05	SP													uOhm.cm							687														n/cm3	1450000000000000000000			vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153987	MAT1009.0090	concentration by EPMA. Mother compound SnTe has 1.2% Sn vacancy from RH. RRR = 1.74. Tc(SP) = 1.94. (dC/gamma*Tc) = 1.16	Sn1-xInxTe	Sn0.904In0.084Te1	Sn	0.904	In	0.084	Te	1																		3	2010																										AB																				K			1.76				1.76																																																								mJ/mol.K2	1.19	SP													uOhm.cm							475																		vapor transport method. mixture - pellet - SIN(600C,36h) - once more - homogeneous mixture - evacuated quartz tube - heat(750C,9d under T-gradient (1 C/cm) - ANN(550C,12h)					Anomalous scattering in superconducting indium-doped tin telluride			Department of Applied Physics and Geballe Laboratory for Advanced Materials, Stanford University, CA 94305	Cond-Mat/1009.0090	A. S. Erickson,T. H. Geballe,I. R. Fisher,Y. Q. Wu,M. J. Kramer		
153988	ACS13110338	R(min)  at T=224 K. R(anomaly, max)  at T=151 K.	SmOFeAs	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2009																										ABCD	2	oxypnictide			A	3.936		8.503											Fe-1111, ZrCuSiAs-type	K					5																																																																																																SmAs(3N),Fe(4N),Ir(4N),Fe2O3(3N)		solid state reaction. mixture - pellet - wrapped with Ta foil - sealed in evacuated quartz tube - ANN(1150C,36h, in Ar)					Ir Doping-Induced Superconductivity in the SmFeAsO System			Key Laboratory of AdVanced Technology of Materials, Peking UniVersity, Beijing 100871, China	J.Am.Chem.Soc., 131(2009)10338	Yong Liang Chen,Cui Hua Cheng,Ya Jing Cui,Han Zhang,Yong Zhang,Ye Yang,Yong Zhao		
153989	ACS13110338	R(min)  at T=151 K	SmO(Fe,Ir)As	Sm1Fe0.85Ir0.15As1O1	Sm	1	Fe	0.85	Ir	0.15	As	1													O	1		1	2009																										ABCD	2	oxypnictide			A	3.953		8.434											Fe-1111, ZrCuSiAs-type	K		16	17.3	16			16	MTC153989									60																																																																																				SmAs(3N),Fe(4N),Ir(4N),Fe2O3(3N)		solid state reaction. mixture - pellet - wrapped with Ta foil - sealed in evacuated quartz tube - ANN(1150C,36h, in Ar)					Ir Doping-Induced Superconductivity in the SmFeAsO System			Key Laboratory of AdVanced Technology of Materials, Peking UniVersity, Beijing 100871, China	J.Am.Chem.Soc., 131(2009)10338	Yong Liang Chen,Cui Hua Cheng,Ya Jing Cui,Han Zhang,Yong Zhang,Ye Yang,Yong Zhao		
153990	CRY0510253	impurity phase: Fe7Se8. Tc defined as max of dR/dT. T<STR>(Tetra-to Ortho) = 90 K, defined as max of dR/dT.	FeSe0.92	Fe1Se0.92	Fe	1	Se	0.92																				1	2011																										AB			P4/nmm																Fe-11	K		7.6					7.6																																																																																														Fe(9N),Se(3N),Sb(4N)		mixture - sealed in evacuated quartz tube - heat(700C,13h) - reground - pellet - heat(680C,40h, in vac) - FC to RT					The transport properties in antimony doped iron selenide Fe(Se1-xSbx)0.92 system			Department of Physics, Shanghai University, Shanghai 200444, China	Cryogenics, 51(2011)253	Junyi Ge,Shixun Cao,Shaoxi Shen,Shujuan Yuan,Baojuan Kang,Jincang Zhang		
153991	CRY0510253	impurity phase: Fe7Se8. Tc defined as max of dR/dT. T<STR>(Tetra-to Ortho) = 100 K, defined as max of dR/dT.	Fe(Se,Sb)0.92	Fe1Se0.874Sb0.046	Fe	1	Se	0.874	Sb	0.046																		1	2011																										AB			P4/nmm																Fe-11	K		9.2					9.2																																																																																														Fe(9N),Se(3N),Sb(4N)		mixture - sealed in evacuated quartz tube - heat(700C,13h) - reground - pellet - heat(680C,40h, in vac) - FC to RT					The transport properties in antimony doped iron selenide Fe(Se1-xSbx)0.92 system			Department of Physics, Shanghai University, Shanghai 200444, China	Cryogenics, 51(2011)253	Junyi Ge,Shixun Cao,Shaoxi Shen,Shujuan Yuan,Baojuan Kang,Jincang Zhang		
153992	CRY0510253	impurity phase: Fe7Se8. Tc defined as max of dR/dT. T<STR>(Tetra-to Ortho) = 97 K, defined as max of dR/dT.	Fe(Se,Sb)0.92	Fe1Se0.828Sb0.092	Fe	1	Se	0.828	Sb	0.092																		1	2011																										AB			P4/nmm																Fe-11	K		8.3		7.2			8.3																																																																																														Fe(9N),Se(3N),Sb(4N)		mixture - sealed in evacuated quartz tube - heat(700C,13h) - reground - pellet - heat(680C,40h, in vac) - FC to RT					The transport properties in antimony doped iron selenide Fe(Se1-xSbx)0.92 system			Department of Physics, Shanghai University, Shanghai 200444, China	Cryogenics, 51(2011)253	Junyi Ge,Shixun Cao,Shaoxi Shen,Shujuan Yuan,Baojuan Kang,Jincang Zhang		
153993	CRY0510253	impurity phase: Fe7Se8. Tc defined as max of dR/dT. T<STR>(Tetra-to Ortho) = 98 K, defined as max of dR/dT.	Fe(Se,Sb)0.92	Fe1Se0.736Sb0.184	Fe	1	Se	0.736	Sb	0.184																		1	2011																										AB			P4/nmm																Fe-11	K		8.85					8.85																																																																																														Fe(9N),Se(3N),Sb(4N)		mixture - sealed in evacuated quartz tube - heat(700C,13h) - reground - pellet - heat(680C,40h, in vac) - FC to RT					The transport properties in antimony doped iron selenide Fe(Se1-xSbx)0.92 system			Department of Physics, Shanghai University, Shanghai 200444, China	Cryogenics, 51(2011)253	Junyi Ge,Shixun Cao,Shaoxi Shen,Shujuan Yuan,Baojuan Kang,Jincang Zhang		
153994	JPCONF215012035	Hydrostatic P (medium: Daphne 7373)	YbGa1.1Si0.9	Yb1Ga1.1Si0.9	Yb	1	Ga	1.1	Si	0.9																		1	2010																										ABC		AlB2	P6/mmm																	K			2.4			0.1	2.4	MTC153994		K/GPa	-0.78																																																				mJ/mol.K2	10																																							Ar-arcmelting - ANN. sample loaded in BN capsule. Sealed in quartz tube. Remelt(1470K,6h) - cool to 1270 K(4K/h).					Pressure dependence of superconducting-transition temperature of YbGa1.1Si0.9			Center for Transdisciplinary Research, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	J.Phys.Conf.Ser., 215(2010)012035	A Ohmura,K Fujimaki,M Einaga,F Ishikawa,A Nakayama,Yuh Yamada,M Imai,N Tsujii		
153995	JPCONF215012035	Hydrostatic P (medium: Daphne 7373)	CaGaSi	Ca1Ga1Si1	Ca	1	Ga	1	Si	1																		1	2010																										ABC		AlB2	P6/mmm																	K			4.2				4.2	MTC153995		K/GPa	-0.11																																																																																												Ar-arcmelting - ANN. sample loaded in BN capsule. Sealed in quartz tube. Remelt(1470K,6h) - cool to 1270 K(4K/h).					Pressure dependence of superconducting-transition temperature of YbGa1.1Si0.9			Center for Transdisciplinary Research, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	J.Phys.Conf.Ser., 215(2010)012035	A Ohmura,K Fujimaki,M Einaga,F Ishikawa,A Nakayama,Yuh Yamada,M Imai,N Tsujii		
153996	JPCONF215012036	P-induced SC. P<cr> = 9.0 GPa. For P > 11 GPa, 2nd SC phase ( dTc/dP = +0.3 K/GPa). R(P,RT)) shows the electrical topological transition at 2GPa	Bi2Te3	Bi2Te3	Bi	2	Te	3																				1	2010																										A2B3	7		R3[-]m		A	4.385		30.51											hexagonal	K	2.74		2.95		0		2.845	MTC153996		K/GPa	-0.3																																																																																												Polycrystalline Bi2Te3(99.99%) from Kojundo Chemical Lab., Ltd.					New superconducting phase of Bi2Te3 under pressure above 11 GPa			Graduate School of Science & Technology, Niigata University, Niigata 950-2181,Japan	J.Phys.Conf.Ser., 215(2010)012036	M Einaga,Y Tanabe,A Nakayama,A Ohmura,F Ishikawa,Yuh Yamada		
153997	JPCONF400022088	P-induce SC. P<cr> = 4.5 GPa. R(P,RT)shows transition from A7 to incommensurate host-guest composite at 3 GPa.	Bi0.85Sb0.15	Bi0.85Sb0.15	Bi	0.85	Sb	0.15																				1	2012																												A7	R-3m		A	4.5186		11.774											superspace group (gamma)4/mcm(00[gamma])0000 at P=3GPa.	K			6.79		0	0.2	6.79	MTC153997																																																																																													Bi(5N),Sb(5N)		mixture - loaded in quartz tube - sealed in vac - melt(420 C,24h) - Q in water - ANN(264 C,1w)					Pressure-induced superconductivity in Bi0.85Sb0.15 alloy			Center for Transdisciplinary Research, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	J.Phys.Conf.Ser., 400(2012)022088	A Ohmura,A Yamamura,M Einaga,F Ishikawa,A Nakayama,Yuh Yamada,S Nakano		
153998	PCS0520761	b-axis whisker. RRR = 114. Tc(R) depends on current density. small diamagnetism. Maybe, sample composed of isolated filament SCs with diameter less than [penet]	TaSe3	Ta1Se3	Ta	1	Se	3																					1991																										AB3			P2<1>/m		A	10.402	3.495	9.829											monoclinic, beta = 106.26 degree	K		2					2																																																																							uOhm.cm							7.91				898																			SUPERCONDUCTIVITY IN THE FILAMENTARY CONDUCTOR TaSe3			Department of Applied Materials Science,Muroran Institute of Technology, Muroran 050,Japan	J.Phys.Chem.Solids, 52(1991)761	S.Nagata,S.Ebisu,TAochi,Y.Kinoshita,S.Chikazawa,K.Yamaya		
153999	ACS1320908		LiCu2P2	Li1Cu2P2	Li	1	Cu	2	P	2																		1	2010																										AB2C2	2	CeAl2Ca2	I4/mmm		A	3.8888		9.562											Fe-122	K				3.7			3.7										15																																																																																						solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - ANN(650-850 C,24-48h)					A New Pnictide Superconductor without Iron			Texas Materials Institute, ETC 9.102, UniVersity of Texas at Austin, Austin, Texas 78712	J.Am.Chem.Soc., 132(2010)0908	Jian-Tao Han,Jian-Shi Zhou,Jin-Guang Cheng,John B. Goodenough		
154000	ACS1320908		LiFeP	Li1Fe1P1	Li	1	Fe	1	P	1																		1	2010																										ABC			P4/nmm		A	3.6992		6.0374											Fe-111	K				4.1			4.1										15																																																																																						solid state reaction. mixture - pellet - wrapped in Ta foil - sealed in quartz tube - ANN(650-850 C,24-48h)					A New Pnictide Superconductor without Iron			Texas Materials Institute, ETC 9.102, UniVersity of Texas at Austin, Austin, Texas 78712	J.Am.Chem.Soc., 132(2010)0908	Jian-Tao Han,Jian-Shi Zhou,Jin-Guang Cheng,John B. Goodenough		
154001	ACS1331751	impurity phase: Cu3P (5%). not SC	LiCu2P2	Li1Cu2P2	Li	1	Cu	2	P	2																		1	2011																										AB2C2	2	CeAl2Ca2	I4/mmm		A	3.89152		9.56114												K					2																																																																																							m3/C	0.0000000004287					MRH154001	n/m3	14579000000000000000000000000	Li(foil),CuP(powder)		mixture - pellet - in Ta boat - sealed in quartz tube(0.2 bar Ar) - heat(170C,20h) - RT - reground - pellet - ANN(675C,20h)					Absence of Superconductivity in LiCu2P2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	J.Am.Chem.Soc., 133(2011)1751	Fei Han,Xiyu Zhu,Gang Mu,Bin Zeng,Peng Cheng,Bing Shen,Hai-Hu Wen		
154002	ACS1331751	not SC	LiCu2P2	Li1Cu2P2	Li	1	Cu	2	P	2																		3	2011																										AB2C2	2	CeAl2Ca2	I4/mmm		A	3.89152		9.56114												K					2																																																																																																		Sn-flux method. (Li:Cu:P:Sn = 1:2:2:15) in alumina crucible - sealed in quartz tube(vac) - heat(900C,180h) - cool to 600C (3.5C/h)					Absence of Superconductivity in LiCu2P2			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	J.Am.Chem.Soc., 133(2011)1751	Fei Han,Xiyu Zhu,Gang Mu,Bin Zeng,Peng Cheng,Bing Shen,Hai-Hu Wen		
154003	JMC0192573	M = pyridine (C5H5N). Intercalated material	M0.25TiNCl	M0.25Ti1N1Cl1	M	0.25	Ti	1	N	1	Cl	1																	2009																										ABC		FeOCl	Bmmb	63	A	3.9787	3.283	27.014											alpha-MNX(metal nitride halides)	K				8.6			8.6																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154004	JMC0192573	Intercalated material. K-content, x not measured. DB value is tentative.	KxTiNCl	K0.5Ti1N1Cl1	K	0.5	Ti	1	N	1	Cl	1																	2009																										ABC		FeOCl	Immm	71	A	4.0605	3.2932	17.722											alpha-MNX(metal nitride halides)	K				16.3			16.3																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154005	JMC0192573		TiN	Ti1N1	Ti	1	N	1																					2009																										ABC		NaCl	Fm-3m	225	A	4.244														K				5.6			5.6																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154006	JMC0192573	Intercalated material. Li-content, x not measured. DB value is tentative.	LixTiNCl	Li0.5Ti1N1Cl1	Li	0.5	Ti	1	N	1	Cl	1																1	2009																										ABC		FeOCl	Pmmn	59	A	4.0114	3.2726	7.9211											alpha-MNX(metal nitride halides)	K				16.5			16.5																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154007	JMC0192573	Intercalated material. Na-content, x not measured. DB value is tentative.	NaxTiNCl	Na0.5Ti1N1Cl1	Na	0.5	Ti	1	N	1	Cl	1																1	2009																										ABC		FeOCl	Bmmb	63	A	4.017	3.2737	16.8835											alpha-MNX(metal nitride halides)	K				16.3			16.3																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154009	JMC0192573	Intercalated material. Rb-content, x not measured. DB value is tentative.	RbxTiNCl	Rb0.5Ti1N1Cl1	Rb	0.5	Ti	1	N	1	Cl	1																1	2009																										ABC		FeOCl	Immm	71	A	4.0375	3.2899	18.398											alpha-MNX(metal nitride halides)	K				16.3			16.3																																																																																																mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154010	JMC0192573		TiNCl	Ti1N1Cl1	Ti	1	N	1	Cl	1																		1	2009																										ABC			Pmmn	59	A	3.9382	3.2582	7.8												K					2																																																																																																		mixture(TiNCl + alkalimetal azide) loaded in BN cell. After decomposition(250-350 C) of azide, ANN(300C,7days)					Structure and superconductivity of the intercalation compounds of TiNCl with pyridine and alkali metals as intercalants			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Mater.Chem., 19(2009)2573	Shoji Yamanaka,Toshihiro Yasunaga,Kosuke Yamaguchi,Masahiro Tagawa		
154011	JPCONF150052079	O-content calculated from the weight change during ANN.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.74	Pr	2	Ba	4	Cu	7															O	15-z	14.74	1	2009																										A2B4C7D15		Y247																		K				15.5			15.5																																																																																														Pr6O11,CuO,Ba(NO3)2		precursor(decomposed at 800-880C in air for 24h. pellet - reaction(973C,18h in 5 atm-O2) - ANN(400C)					Pressure effects on the electrical resistivity of Pr2Ba4Cu7O15-z oxide superconductor			Graduate School of Science and Technology, Niigata University, Niigata, Japan	J.Phys.Conf.Ser., 150(2009)052079	Fumihiro Ishikawa,Kazunori Fukuda,Yasunori Hiura,Yusuke Onoda,Atsuko Nakayama,Yuh Yamada,Akiyuki Matsushita,Tomoko Kagayama		
154012	JPCONF150052079	O-content calculated from the weight change during ANN. R not zero for P>2 GPa. Tc(on) = 3.3 K at 2.5 GPa.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.36	Pr	2	Ba	4	Cu	7															O	15-z	14.36	1	2009																										A2B4C7D15		Y247																		K			22.7	20.6			20.6	MTC154012																																																																																													Pr6O11,CuO,Ba(NO3)2		precursor(decomposed at 800-880C in air for 24h. pellet - reaction(973C,18h in 5 atm-O2) - ANN(400C)					Pressure effects on the electrical resistivity of Pr2Ba4Cu7O15-z oxide superconductor			Graduate School of Science and Technology, Niigata University, Niigata, Japan	J.Phys.Conf.Ser., 150(2009)052079	Fumihiro Ishikawa,Kazunori Fukuda,Yasunori Hiura,Yusuke Onoda,Atsuko Nakayama,Yuh Yamada,Akiyuki Matsushita,Tomoko Kagayama		
154013	JPCONF150052079	O-content calculated from the weight change during ANN. Zero resistivity observed for P=<2.0 GPa. Tc(on) = 25.5 K at 2.5 GPa.	Pr2Ba4Cu7O15	Pr2Ba4Cu7O14.21	Pr	2	Ba	4	Cu	7															O	15-z	14.21	1	2009																										A2B4C7D15		Y247																		K			23				23	MTC154012									60																																																																																				Pr6O11,CuO,Ba(NO3)2		precursor(decomposed at 800-880C in air for 24h. pellet - reaction(973C,18h in 5 atm-O2) - ANN(400C)					Pressure effects on the electrical resistivity of Pr2Ba4Cu7O15-z oxide superconductor			Graduate School of Science and Technology, Niigata University, Niigata, Japan	J.Phys.Conf.Ser., 150(2009)052079	Fumihiro Ishikawa,Kazunori Fukuda,Yasunori Hiura,Yusuke Onoda,Atsuko Nakayama,Yuh Yamada,Akiyuki Matsushita,Tomoko Kagayama		
154014	JPCONF273012089		SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		1	2011																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.422		10.131											Fe-122	K				3			3																																																																																														Pd(4N),Ni(4N),Ge(6N),Sr(99.5%)		Two step arc melting. Stoichiometric (Pd-Ni-Ge) firstly arc melted. Then Sr rock was added and arc melted.					Superconductivity in Sr(Pd1-xNix)2Ge2			Department of Physics, National Taiwan Normal University, Taipei 11677, Taiwan	J.Phys.Conf.Ser., 273(2011)012089	C D Yang,H C Hsu,W Y Tseng,H C Chen,H C Ku,M N Ou,Y Y Chen,Y Y Hsu		
154015	JPCONF273012089		Sr(Pd1-xNix)2Ge2	Sr1Pd1.8Ni0.2Ge2	Sr	1	Pd	1.8	Ni	0.2	Ge	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm	139															Fe-122	K				3.2			3.2	MTC154015																																																																																													Pd(4N),Ni(4N),Ge(6N),Sr(99.5%)		Two step arc melting. Stoichiometric (Pd-Ni-Ge) firstly arc melted. Then Sr rock was added and arc melted.					Superconductivity in Sr(Pd1-xNix)2Ge2			Department of Physics, National Taiwan Normal University, Taipei 11677, Taiwan	J.Phys.Conf.Ser., 273(2011)012089	C D Yang,H C Hsu,W Y Tseng,H C Chen,H C Ku,M N Ou,Y Y Chen,Y Y Hsu		
154016	JPCONF273012089		Sr(Pd1-xNix)2Ge2	Sr1Pd1Ni1Ge2	Sr	1	Pd	1	Ni	1	Ge	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.292		10.179											Fe-122	K				2.1			2.1	MTC154015																																																																																													Pd(4N),Ni(4N),Ge(6N),Sr(99.5%)		Two step arc melting. Stoichiometric (Pd-Ni-Ge) firstly arc melted. Then Sr rock was added and arc melted.					Superconductivity in Sr(Pd1-xNix)2Ge2			Department of Physics, National Taiwan Normal University, Taipei 11677, Taiwan	J.Phys.Conf.Ser., 273(2011)012089	C D Yang,H C Hsu,W Y Tseng,H C Chen,H C Ku,M N Ou,Y Y Chen,Y Y Hsu		
154017	JPCONF273012089		SrNi2Ge2	Sr1Ni2Ge2	Sr	1	Ni	2	Ge	2																		1	2011																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.178		10.252											Fe-122	K	0.845	0.87	0.915			0.036	0.87																																																																																														Pd(4N),Ni(4N),Ge(6N),Sr(99.5%)		Two step arc melting. Stoichiometric (Pd-Ni-Ge) firstly arc melted. Then Sr rock was added and arc melted.					Superconductivity in Sr(Pd1-xNix)2Ge2			Department of Physics, National Taiwan Normal University, Taipei 11677, Taiwan	J.Phys.Conf.Ser., 273(2011)012089	C D Yang,H C Hsu,W Y Tseng,H C Chen,H C Ku,M N Ou,Y Y Chen,Y Y Hsu		
154018	JPC024475701	residual [gamma] due to normal volume fraction. (dC/Tc) = 16.7 mJ/mol.K2. residual [gamma] = 0.4 mJ/mol.K2. gamma(H) = 0.4 + 3.1*H^0.66.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2012																										ABC																			Fe-111	K		15.1				1	15.1																																																																																														LiAs,FeAs,As		self flux method. mixture - pellet - alumina-oxide tube in Nb-tube(1atm-air) - sealed in quartz tube - heat(1100C,10h) - cool to 700C (5c/h)					Specific heat versus field for LiFe1-xCuxAs			Department of Physics, University of Florida, Gainesville, FL 32611-8440, USA	J.Phys.:Condens.Matter, 24(2012)475701	J S Kim,G R Stewart,L Y Xing,X C Wang,C Q Jin		
154019	JPC024475701	residual [gamma] due to normal volume fraction. (dC/Tc) = 5.0 mJ/mol.K2. residual [gamma] = 0.31 mJ/mol.K2. gamma(H) = 0.31 + 4.16*H^0.57.	Li(Fe,Cu)As	Li1Fe0.98Cu0.02As1	Li	1	Fe	0.98	Cu	0.02	As	1																3	2012																										ABC																			Fe-111	K		9.3					9.3																																																																																														LiAs,FeAs,As		self flux method. mixture - pellet - alumina-oxide tube in Nb-tube(1atm-air) - sealed in quartz tube - heat(1100C,10h) - cool to 700C (5c/h)					Specific heat versus field for LiFe1-xCuxAs			Department of Physics, University of Florida, Gainesville, FL 32611-8440, USA	J.Phys.:Condens.Matter, 24(2012)475701	J S Kim,G R Stewart,L Y Xing,X C Wang,C Q Jin		
154020	JPC022075702	not SC. SUS-anomaly at 200K due to SDW/CDW. Lattice term in SP (beta) = 0.79 mJ/mol.K4 derived for 3.9 < T < 25 K.	BaTi2As2O	Ba1Ti2As2O1	Ba	1	Ti	2	As	2															O	1		1	2010																										ABC2D2			P4/nmm	123	A	4.0456		7.2723												K					0																																																										mJ/mol.K2	15.3	SP	223	SP																																		BaO(3N),Ti(4N),As(6N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - react(850C,40h)					Structure and physical properties for a new layered pnictide-oxide: BaTi2As2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter, 22(2010)075702	X F Wang,Y J Yan,J J Ying,Q J Li,M Zhang,N Xu,XH Chen		
154021	JPC022075702	not SC. BaLixTi2As2O were measured for x < 0.2.	BaLixTi2As2O	Ba1Li0.05Ti2As2O1	Ba	1	Li	0.05	Ti	2	As	2													O	1		1	2010																										ABC2D2			P4/nmm	123	A	4.038		7.2664											Lattice parameters in Fig.	K					0			MLAT154021																																																																																													LiAs,BaO,Ti,As		Firstly LiAs obtained by reacting Li and As at 500C for 10h. mixture - pellet - heat(800C,4h)					Structure and physical properties for a new layered pnictide-oxide: BaTi2As2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.:Condens.Matter, 22(2010)075702	X F Wang,Y J Yan,J J Ying,Q J Li,M Zhang,N Xu,XH Chen		
154022	JAP11107E117		Sr(Pd1-xPtx)2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		3	2012																										AB2C2		ThCr2Si2			A	4.4113		10.12											Fe-122	K		2.7					2.7																				Oe						1596		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154023	JAP11107E117	Pt-content (measured by WDS) = 0.015 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.99Pt0.01Ge2	Sr	1	Pd	1.99	Pt	0.01	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4099		10.1184											Fe-122	K		2.82					2.82																				Oe						1799		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154024	JAP11107E117	Pt-content (measured by WDS) = 0.0298 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.98Pt0.02Ge2	Sr	1	Pd	1.98	Pt	0.02	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4102		10.1162											Fe-122	K		2.96					2.96																				Oe						1995		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154025	JAP11107E117	Pt-content (measured by WDS) = 0.0543 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.96Pt0.04Ge2	Sr	1	Pd	1.96	Pt	0.04	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4075		10.1177											Fe-122	K		3.16					3.16																				Oe						2700		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154026	JAP11107E117	Pt-content (measured by WDS) = 0.0606 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.94Pt0.06Ge2	Sr	1	Pd	1.94	Pt	0.06	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4084		10.1162											Fe-122	K		3.22					3.22	MTC154026																			Oe						2896		2						MHC154026																																																														single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154027	JAP11107E117	Pt-content (measured by WDS) = 0.0617 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.93Pt0.07Ge2	Sr	1	Pd	1.93	Pt	0.07	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4099		10.1251											Fe-122	K		3.24					3.24																				Oe						3100		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154028	JAP11107E117	Pt-content (measured by WDS) = 0.0649 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.92Pt0.08Ge2	Sr	1	Pd	1.92	Pt	0.08	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.409		10.128											Fe-122	K		3.23					3.23																				Oe						3304		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154029	JAP11107E117	Pt-content (measured by WDS) = 0.1287 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.9Pt0.1Ge2	Sr	1	Pd	1.9	Pt	0.1	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4065		10.1268											Fe-122	K		2.89					2.89																				Oe						1494		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154030	JAP11107E117	Pt-content (measured by WDS) = 0.1457 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xPtx)2Ge2	Sr1Pd1.86Pt0.14Ge2	Sr	1	Pd	1.86	Pt	0.14	Ge	2																3	2012																										AB2C2		ThCr2Si2			A	4.4106		10.1358											Fe-122	K		2.6					2.6																				Oe						1007		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154031	JAP11107E117	Si-content (measured by WDS) = 0.0053 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	SrPd2(Ge1-x,Six)2	Sr1Pd2Si0.02Ge1.98	Sr	1	Pd	2	Si	0.02	Ge	1.98																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.76					2.76																				Oe						1596		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154032	JAP11107E117	Si-content (measured by WDS) = 0.0096 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	SrPd2(Ge1-x,Six)2	Sr1Pd2Si0.04Ge1.96	Sr	1	Pd	2	Si	0.04	Ge	1.96																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.72					2.72																				Oe						1589		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154033	JAP11107E117	Si-content (measured by WDS) = 0.0266 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	SrPd2(Ge1-x,Six)2	Sr1Pd2Si0.1Ge1.9	Sr	1	Pd	2	Si	0.1	Ge	1.9																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.7					2.7																				Oe						1589		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154034	JAP11107E117	Ag-content (measured by WDS) = 0.0564 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xAgx)2Ge2	Sr1Pd1.98Ag0.02Ge2	Sr	1	Pd	1.98	Ag	0.02	Ge	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.64					2.64																				Oe						1589		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154035	JAP11107E117	Ag-content (measured by WDS) = 0.0755 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xAgx)2Ge2	Sr1Pd1.9Ag0.1Ge2	Sr	1	Pd	1.9	Ag	0.1	Ge	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.62					2.62	MTC154026																			Oe						1487		2						MHC154026																																																														single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154036	JAP11107E117	Ag-content (measured by WDS) = 0.117 in Sr(Pd1-xPtx)2Ge2. Hc2// measured at 2 K.	Sr(Pd1-xAgx)2Ge2	Sr1Pd1.8Ag0.2Ge2	Sr	1	Pd	1.8	Ag	0.2	Ge	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		2.52					2.52																				Oe						1385		2																																																																				single crystals grown using high-T flux method					Chemical pressure and electron doping effects in SrPd2Ge2 single crystals			School of Materials Science and Engineering, Gwangju Institute of Science and Technology (GIST), Gwangju 500-712, Korea	J.Appl.Phys., 111(2012)07E117	N. H. Sung,C. J. Roh,B. Y. Kang,B. K. Cho		
154038	JPS078113709	Tc defined as R=0.5Rn.  Hc2(T)//b for sample #1(Tc=0.55 K), Hc2(T)//a and //c for sample #2 (Tc=0.71 K)	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2009							2.6																			ABC		TiNiSi																		K	0.48	0.55	0.72				0.55																				T	RES, R=0.5Rn			0.6										MHC154038																																																														Czochralski method					Extremely Large and Anisotropic Upper Critical Field and the Ferromagnetic Instability in UCoGe			INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn., 78(2009)113709	Dai AOKI,Tatsuma D. MATSUDA,Valentin TAUFOUR,Elena HASSINGER,Georg KNEBEL,Jacques FLOUQUET		
154039	JPS078113709	Curie-T(H) from SP and change of (dR/dT). Angular dependence of Hc2(T) measured for small deviation from b- and a-axis.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2009							2.6																			ABC		TiNiSi																		K	0.48	0.55	0.72				0.55	MPH154039																																	MHC154039																																																														Czochralski method					Extremely Large and Anisotropic Upper Critical Field and the Ferromagnetic Instability in UCoGe			INAC/SPSMS, CEA-Grenoble, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn., 78(2009)113709	Dai AOKI,Tatsuma D. MATSUDA,Valentin TAUFOUR,Elena HASSINGER,Georg KNEBEL,Jacques FLOUQUET		
154040	JPS079113705	magnetic properties for H//[110]. SUS(T) shows max at 45 K, but no anomaly in SP. Hc2(0) = 7 Tby extrapolation. (dC/gamma:Tc) = 2.78. Wilson ratio  R<W> = 1.7	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2010	emu/mol	-0.00013	emu.K/mol	0.18	Myu-B/mol	1.2	-211																			A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.7437														K	7		7.3	7		0.3	7										80										T	RES, R=0.5Rn, WHH	5.5												MHC154040		A	from Hc2	79																mJ/mol.K	798	mJ/mol.K2	41	SP	149.5																																					flux method					Coexistence of Superconductivity and Ferromagnetic Spin-Fluctuationin Ca3Ir4Sn13 Single Crystal			Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn., 79(2010)113705	Jinhu YANG,Bin CHEN,Chishiro MICHIOKA,Kazuyoshi YOSHIMURA		
154041	JPS080075002	Pressure medium , ( FC70:FC77= 1:1). R(T) has a hump around 200 K.. Tc(on) and Tc(zero)  measured for P < 2.0 GPa (See Fig.)	K0.82Fe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																		3	2011																										AB2C2		ThCr2Si2																	Fe-122	K	31.5		33				32.25	MTC154041		K/GPa																																																																																													crystals preoared by melting ( FeAs + K)					Pressure Study of the New Iron-Based Superconductor K0:8Fe2Se2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn.,80(2011)075002	Yasuna KAWASAKI,Yoshikazu MIZUGUCHI,Keita DEGUCHI,Tohru WATANABE,Toshinori OZAKI,Shunsuke TSUDA,Takahide YAMAGUCHI,Hiroyuki TAKEYA,Yoshihiko TAKANO		
154042	MTL0010071	SUS(300K) = 0.24 E-3 emu/mol. Tc(H=100Oe) = 0.55 K.	LaNi2Ge2	La1Ni2Ge2	La	1	Ni	2	Ge	2																		1	1982																										AB2C2		ThCr2Si2																		K		0.69				0.047	0.69										90																																																																																						induction melting (stoichiometric) in vitreous carbon crucible (1 atm-Ar) - ANN(750C,5days)					Superconductivity in LaNi2Ge2 and Related Intermetallics			Bell Laboratories, Murray Hill, New Jersey 07974, USA	Materials Letters, 1(1982)71	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
154043	MTL0010071	x=0.2 and 0.3 (in LaPd2(Ge1-xSnx)2 samples were multi-phase even after ANN(750C,5days).	LaPd2(Ge,Sn)2	La1Pd2Ge1.9Sn0.1	La	1	Pd	2	Ge	1.9	Sn	0.1																2	1982																										AB2C2		ThCr2Si2																		K		1.25				0.04	1.25										80																																																																																						induction melting (stoichiometric) in vitreous carbon crucible (1 atm-Ar) - ANN(750C,5days)					Superconductivity in LaNi2Ge2 and Related Intermetallics			Bell Laboratories, Murray Hill, New Jersey 07974, USA	Materials Letters, 1(1982)71	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
154044	MTL0010071	some second phases present.	LaPt2(Ge,Sn)2	La1Pt2Ge1.8Sn0.2	La	1	Pt	2	Ge	1.8	Sn	0.2																	1982																										AB2C2		ThCr2Si2																		K		1.3				0.22	1.3										90																																																																																						induction melting (stoichiometric) in vitreous carbon crucible (1 atm-Ar) - ANN(750C,5days)					Superconductivity in LaNi2Ge2 and Related Intermetallics			Bell Laboratories, Murray Hill, New Jersey 07974, USA	Materials Letters, 1(1982)71	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
154045	MTL0010071		LaPd2(Ge,Sn)2	La1Pd2Ge1.96Sn0.04	La	1	Pd	2	Ge	1.96	Sn	0.04																	1982																										AB2C2		ThCr2Si2																		K		0.82					0.82																																																																																																epitaxial growth on sapphire [101[-]0] substrate.					Superconductivity in LaNi2Ge2 and Related Intermetallics			Bell Laboratories, Murray Hill, New Jersey 07974, USA	Materials Letters, 1(1982)71	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
154046	MTL0010071		LaPd2(Ge,Sn)2	La1Pd2Ge1.92Sn0.08	La	1	Pd	2	Ge	1.92	Sn	0.08																	1982																										AB2C2		ThCr2Si2																		K		1.44					1.44																																																																																																epitaxial growth on sapphire [101[-]0] substrate.					Superconductivity in LaNi2Ge2 and Related Intermetallics			Bell Laboratories, Murray Hill, New Jersey 07974, USA	Materials Letters, 1(1982)71	J.H.Wernick,G.W.Hull,T.H.Geballe,J.E.Bernardini,J.V.Waszczak		
154047	PSS0071287	Thickness=0.4um. Tc=2.2 K for J//[112[-]0] and = 1.5 K for J//[101[-]0]. Figure shows Hc2(T), defined as ac-SUS(onset). R(J//[112[-]0] goes to infinite (insulator) down to 0 K for H=3mT.	InN	In1N1	In	1	N	1																				5	2010																										AB																				K	1.1		2.2	0.2			0.2																				mT	SUS, two fluid approx.		13.9	3.5										MHC154047		A	from Hc2		1500	3100						meV	0.43	3.9	17																																											n/cm3	7000000000000000000								Meissner effect of superconducting InN			Department of Electronics, Tokai University, 1117 Kitakaname, Hiratsuka 259-1292 Japan	Phys.Status Solidi, C7(2010)1287	Takashi Inushima,Duncan K. Maude,Daisuke Muto,Yasushi Nanishi		
154048	PHC4710213	residual resistivity at Tc(on)	Ba(Fe,Co)2As2	Ba1Fe1.87Co0.13As2	Ba	1	Fe	1.87	Co	0.13	As	2																1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.96		13											Fe-122	K				25			25																																																																							mOhm.cm							0.42																BaAs,FeAs,Fe(3N),Co(99.5%),Zn(4N)		stoichiometric mixture - (Pt capsule with h-BN inner) - sealed in evacuated quartz tube - heat(1100C,20h)					Non-magnetic impurity effect on the optimally carrier doped superconductor BaFe1.87Co0.13As2 prepared at ambient pressure			Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)213	J.J. Li,Y.F. Guo,S.B. Zhang,S. Yu,Y. Tsujimoto,K. Yamaura,E. Takayama-Muromachi		
154049	PHC4710213	residual resistivity at Tc(on)	Ba(Fe,Zn,Co)2As2	Ba1Fe1.83Zn0.04Co0.13As2	Ba	1	Fe	1.83	Zn	0.04	Co	0.13	As	2														1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9633		13											Fe-122	K				20			20																																																																							mOhm.cm							0.54																BaAs,FeAs,Fe(3N),Co(99.5%),Zn(4N)		stoichiometric mixture - (Pt capsule with h-BN inner) - sealed in evacuated quartz tube - heat(1100C,20h)					Non-magnetic impurity effect on the optimally carrier doped superconductor BaFe1.87Co0.13As2 prepared at ambient pressure			Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)213	J.J. Li,Y.F. Guo,S.B. Zhang,S. Yu,Y. Tsujimoto,K. Yamaura,E. Takayama-Muromachi		
154050	PHC4710213	residual resistivity at Tc(on)	Ba(Fe,Zn,Co)2As2	Ba1Fe1.81Zn0.06Co0.13As2	Ba	1	Fe	1.81	Zn	0.06	Co	0.13	As	2														1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9645		13.0352											Fe-122	K				19			19																																																																							mOhm.cm							0.66																BaAs,FeAs,Fe(3N),Co(99.5%),Zn(4N)		stoichiometric mixture - (Pt capsule with h-BN inner) - sealed in evacuated quartz tube - heat(1100C,20h)					Non-magnetic impurity effect on the optimally carrier doped superconductor BaFe1.87Co0.13As2 prepared at ambient pressure			Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)213	J.J. Li,Y.F. Guo,S.B. Zhang,S. Yu,Y. Tsujimoto,K. Yamaura,E. Takayama-Muromachi		
154051	PHC4710213	residual resistivity at Tc(on)	Ba(Fe,Zn,Co)2As2	Ba1Fe1.79Zn0.08Co0.13As2	Ba	1	Fe	1.79	Zn	0.08	Co	0.13	As	2														1	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.961		13.0446											Fe-122	K				19			19																																																																							mOhm.cm							0.73																BaAs,FeAs,Fe(3N),Co(99.5%),Zn(4N)		stoichiometric mixture - (Pt capsule with h-BN inner) - sealed in evacuated quartz tube - heat(1100C,20h)					Non-magnetic impurity effect on the optimally carrier doped superconductor BaFe1.87Co0.13As2 prepared at ambient pressure			Superconducting Materials Center, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Physica C, 471(2011)213	J.J. Li,Y.F. Guo,S.B. Zhang,S. Yu,Y. Tsujimoto,K. Yamaura,E. Takayama-Muromachi		
154052	PRB070064403	Tc(SP) = 2.8 K. (dC/gamma*Tc) = 0.85.	Y2Ir3Si5	Y2Ir3Si5	Y	2	Ir	3	Si	5																		1	2004	emu/mol.K	0.003371																								A2B3C5		U2Co3Si5	Ibam		A	9.918	11.472	5.795												K		2.96		2.85			2.96																																																					MSP154052			mJ/mol.K2	35																																					R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154053	PRB070064403	Tc(SP) = 1.96 K. (dC/gamma*Tc) = 0.41.	La2Ir3Si5	La2Ir3Si5	La	2	Ir	3	Si	5																		1	2004	emu/mol.K	0.002034																								A2B3C5		U2Co3Si5	Ibam		A	9.979	11.649	5.924												K		1.99		1.95			1.99																																																					MSP154053			mJ/mol.K2	19.4																																					R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154054	PRB070064403	not SC	Ce2Ir3Si5	Ce2Ir3Si5	Ce	2	Ir	3	Si	5																		1	2004	emu/mol.K	0.002115																								A2B3C5		U2Co3Si5	Ibam		A	9.96	11.629	5.879												K					1.5																																																										mJ/mol.K2	45																																					R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154055	PRB070064403	not SC	Pr2Ir3Si5	Pr2Ir3Si5	Pr	2	Ir	3	Si	5																		1	2004	emu/mol.K	-0.0001507			myu-B/mol	4.38	-21.4																			A2B3C5		U2Co3Si5	Ibam		A	9.947	11.615	5.872												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154056	PRB070064403	not SC	Nd2Ir3Si5	Nd2Ir3Si5	Nd	2	Ir	3	Si	5																		1	2004	emu/mol.K	0.0001557			myu-B/mol	3.79	-4.65	5																		A2B3C5		U2Co3Si5	Ibam		A	9.939	11.587	5.857												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154057	PRB070064403	not SC	Gd2Ir3Si5	Gd2Ir3Si5	Gd	2	Ir	3	Si	5																		1	2004	emu/mol.K	-0.0004762			myu-B/mol	8.14	-22.1	4.82																		A2B3C5		U2Co3Si5	Ibam		A	9.925	11.521	5.822												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154058	PRB070064403	not SC	Tb2Ir3Si5	Tb2Ir3Si5	Tb	2	Ir	3	Si	5																		1	2004	emu/mol.K	-0.000936			myu-B/mol	9.99	-31.5	3.21																		A2B3C5		U2Co3Si5	Ibam		A	9.916	11.487	5.799												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154059	PRB070064403	not SC	Dy2Ir3Si5	Dy2Ir3Si5	Dy	2	Ir	3	Si	5																		1	2004	emu/mol.K	0.002913			myu-B/mol	10.32	-11.81	6.35																		A2B3C5		U2Co3Si5	Ibam		A	9.897	11.406	5.779												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154060	PRB070064403	not SC	Ho2Ir3Si5	Ho2Ir3Si5	Ho	2	Ir	3	Si	5																		1	2004								5.38																		A2B3C5		U2Co3Si5	Ibam		A	9.883	11.371	5.759												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154061	PRB070064403	not SC	Er2Ir3Si5	Er2Ir3Si5	Er	2	Ir	3	Si	5																		1	2004	emu/mol.K	-0.000339			myu-B/mol	9.92	0.63	2.2																		A2B3C5		U2Co3Si5	Ibam		A	9.872	11.364	5.751												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154062	PRB070064403	not SC	Tm2Ir3Si5	Tm2Ir3Si5	Tm	2	Ir	3	Si	5																		1	2004	emu/mol.K	-0.002134			myu-B/mol	7.78	2.64																			A2B3C5		U2Co3Si5	Ibam		A	9.866	11.33	5.745												K					1.5																																																																																																R(3N),Ir(3N),Si(5N)		Ar-arcmelting.  wrapped in Zr-foil - ANN(900C,10d)					Low-temperature studies of the magnetic and superconducting properties of the R2Ir3Si5 (R=Y,La,Ce-Nd,Gd-Tm) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 70(2004)064403	Yogesh Singh,D. Pal,S. Ramakrishnan		
154063	PRB04810435	not SC. (dR/dT) = 1.20 uOhm.cm/K at 300 K.	Nd3Ru4Ge13	Nd3Ru4Ge13	Nd	3	Ru	4	Ge	13																			1993			emu/mol.K	4.4	myu-B/mol	3.4	2.7																			A3B4C13		Pr3Rh4Sn13	Pm3n		A	9.0535														K					1.5																																																																																																R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154064	PRB04810435	not SC. (dR/dT) = 0.66 uOhm.cm/K at 300 K.	Dy3Ru4Ge13	Dy3Ru4Ge13	Dy	3	Ru	4	Ge	13																			1993			emu/mol.K	39.5	myu-B/mol	10.3	2.3																			A3B4C13		Pr3Rh4Sn13	Pm3n		A	8.9548														K					1.5																																																																																																R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154065	PRB04810435	not SC. (dR/dT) = 0.348 uOhm.cm/K at 300 K.	Er3Ru4Ge13	Er3Ru4Ge13	Er	3	Ru	4	Ge	13																			1993			emu/mol.K	30.6	myu-B/mol	9.04	8.3																			A3B4C13		Pr3Rh4Sn13	Pm3n		A	8.9303														K					1.5																																																																																																R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154066	PRB04810435	not SC. (dR/dT) = 0.46 uOhm.cm/K at 300 K.	Ho3Ru4Ge13	Ho3Ru4Ge13	Ho	3	Ru	4	Ge	13																			1993			emu/mol.K	42.5	myu-B/mol	10.6	-6																			A3B4C13		Pr3Rh4Sn13	Pm3n		A	8.9444														K					1.5																																																																																																R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154067	PRB04810435	not SC. anomalous R(T) behaviour.	Yb3Ru4Ge13	Yb3Ru4Ge13	Yb	3	Ru	4	Ge	13																			1993	emu/mol	0.0013	emu/mol.K	2.6	myu-B/mol	2.6	-49.2																			A3B4C13		Pr3Rh4Sn13	Pm3n		A	8.9073														K					1.5																																																																																																R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154068	PRB04810435	SUS(T) nearly T-independent down to 2.3 K (diamag). (dR/dT) = 0.243 uOhm.cm/K at 300 K	Lu3Ru4Ge13	Lu3Ru4Ge13	Lu	3	Ru	4	Ge	13																			1993																										A3B4C13		Pr3Rh4Sn13	Pm3n		A	8.9068														K		2.3		2.3			2.3																																																																																														R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154069	PRB04810435	SUS(T) nearly T-independent down to 2 K (paramag). (dR/dT) = 0.897 uOhm.cm/K at 300 K	Y3Ru4Ge13	Y3Ru4Ge13	Y	3	Ru	4	Ge	13																			1993																										A3B4C13		Pr3Rh4Sn13	Pm3n																	K		1.8		1.8			1.8																																																																																														R(3N),Ru(4N),Ge(4N)		arc-melting - ANN(900C,2w, in sealed quartz tube with He)					Resistivity and magnetic-susceptibility studies in the R3Ru4Ge13 (R=Nd, Dy, Ho, Er, Yb, Lu, and Y) system			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 48(1993)104353	K. Ghosh,S. Ramakrishnan,Girish Chandra		
154070	PRB071045109	R not to zero  down to 1.8K. R(T) has huge thermal hysteresis : 208 K(warming), 164 K(cooling). CDW-like phase transition. SP heat also shows these anomalies.	Lu2Ir3Si5	Lu2Ir3Si5	Lu	2	Ir	3	Si	5																		1	2005																										A2B3C5		U2Co3Si5	Ibam		A	9.91457	11.2866	5.72191												K			3.3	3.3			3.3																																																																																														Lu(3N),Ir(3N),Si(5N)		arc-melting 6 times. wrapped in Zr foil - sealed in evacuated quartz tube - ANN(950C,8d)					Phase transitions in Lu2Ir3Si5			Tata Institute of Fundamental Research, Bombay-400005, India	Phys.Rev.B, 71(2005)045109	Yogesh Singh,Dilip Pal,S. Ramakrishnan,A. M. Awasthi,S. K. Malik		
154072	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2009								132	6.454																	AB2C2		ThCr2Si2	I4/mmm		A	3.9642		13.018											Fe-122	K					1.8																																																										mJ/mol.K2	6.1	SP																																						mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,13h) - cool (1.8 C/h) - decanting FeAs/CrAs flux at 1100C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154073	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe1.96Cr0.04As2	Ba	1	Fe	1.96	Cr	0.04	As	2																3	2009								118																		AB2C2		ThCr2Si2	I4/mmm		A	3.962		13.04											Fe-122	K					1.8																																																										mJ/mol.K2	6.1	SP																																	MRH154073					mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,13h) - cool (1.8 C/h) - decanting FeAs/CrAs flux at 1100C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154074	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe1.86Cr0.14As2	Ba	1	Fe	1.86	Cr	0.14	As	2																3	2009								88																		AB2C2		ThCr2Si2	I4/mmm		A	3.9618		13.085											Fe-122	K					1.8			MPH154074																																																							mJ/mol.K2	30	SP																																	MRH154074					mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,13h) - cool (1.8 C/h) - decanting FeAs/CrAs flux at 1100C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154075	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe1.8Cr0.2As2	Ba	1	Fe	1.8	Cr	0.2	As	2																3	2009								80																		AB2C2		ThCr2Si2	I4/mmm		A	3.9665		13.112											Fe-122	K					1.8																																																										mJ/mol.K2	38	SP																																						mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,13h) - cool (1.8 C/h) - decanting FeAs/CrAs flux at 1100C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154076	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe1.64Cr0.36As2	Ba	1	Fe	1.64	Cr	0.36	As	2																3	2009								58																		AB2C2		ThCr2Si2	I4/mmm		A	3.9657		13.165											Fe-122	K					1.8																																																										mJ/mol.K2	65.4	SP																																						mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,10h) - cool (2.0 C/h) - decanting FeAs/CrAs flux at 1120 C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154077	PRB079224524	not SC	Ba(Fe,Cr)2As2	Ba1Fe1.25Cr0.75As2	Ba	1	Fe	1.25	Cr	0.75	As	2																3	2009																										AB2C2		ThCr2Si2	I4/mmm		A	3.9792		13.26											Fe-122	K					1.8																																																										mJ/mol.K2	70	SP																																						mixture(Ba,FeAs,CrAs) - heat in alumina crucible(1230C,10h) - cool (2.0 C/h) - decanting FeAs/CrAs flux at 1120 C					Absence of superconductivity in hole-doped BaFe2-xCrxAs2 single crystals			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6114, USA	Phys.Rev.B, 79(2009)224524	Athena S. Sefat,David J. Singh,Lindsay H. VanBebber,Yurij Mozharivskyj,Michael A. McGuire,Rongying Jin,Brian C. Sales,Veerle Keppens,David Mandrus		
154078	PRB082180520	K:Fe:Se = 0.39:0.85:1 by ICP. Broad maximun in R(T) at 105 K.	KxFe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																			2010																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9136		14.0367											Fe-122	K	27.2	28.3	30.1	31			28.3											T	M-H curve				0.2			5																																																																									n/cm3	176000000000000000000000			Two step method. 1stly, precursor made by solid state reactin , then flux method. alumina crucible - sealed in silica ampoule - heat(1300K) - cool to 1000K with 4 K/h - FC					Superconductivity in the iron selenide KxFe2Se2 (0 =< x =<1.0)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 82(2010)180520	Jiangang Guo,Shifeng Jin,Gang Wang,Shunchong Wang,Kaixing Zhu,Tingting Zhou,Meng He,Xiaolong Chen		
154079	PRB080224522	Thermal conductivity k(H,T) were measured for H??[110]. Figure shows Hc2 and Hd , where the slope of k(H) changes significantly.	HoNi2B2C	Ho1Ni2B2C	Ho	1	Ni	2	B	2	C																	3	2009																										ABC2D2		LuNi2B2C																		K		8.6					8.6																				T	RES													MHC154079																																																														floating zone method. - ANN(1000C,72h)					Magnetic pair breaking in superconducting HoNi2B2C studied on a single crystal by thermal conductivity in magnetic fields			Institut fur Festkorper- und Werkstoffforschung Dresden (IFW), D-01171 Dresden, Germany	Phys.Rev.B, 80(2009)224522	M. Schneider,G. Fuchs,K.-H. Muller,K. Nenkov,G. Behr,D. Souptel,S.-L. Drechsler		
154080	PRB084020513	Tc(R) defined as max of (dR/dT). Hall const (150K) measured for H//c.	Ba(Fe,Co)2As2	Ba1Fe1.89Co0.11As2	Ba	1	Fe	1.89	Co	0.11	As	2																3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.955		12.976											Fe-122	K		25					25																																																																							mOhm.cm								0.26						m3/C		-0.00000000292							BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154081	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.008 by EPMA.Tc(R) defined as max of (dR/dT).	Ba(Fe,Zn,Co)2As2	Ba1Fe1.87Zn0.02Co0.11As2	Ba	1	Fe	1.87	Zn	0.02	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.957		12.98											Fe-122	K		20					20																																																																							mOhm.cm								0.42															BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154082	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.021 by EPMA.Tc(R) defined as max of (dR/dT). Hall const (150K) measured for H//c.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.85Zn0.04Co0.11As2	Ba	1	Fe	1.85	Zn	0.04	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.963		12.983											Fe-122	K		18.5					18.5																																																																							mOhm.cm								0.4						m3/C		-0.00000000282							BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154083	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.033 by EPMA.Tc(R) defined as max of (dR/dT).	Ba(Fe,Zn,Co)2As2	Ba1Fe1.83Zn0.06Co0.11As2	Ba	1	Fe	1.83	Zn	0.06	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.967		12.989											Fe-122	K		17					17																																																																							mOhm.cm								0.48															BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154084	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.044 by EPMA.Tc(R) defined as max of (dR/dT). Hall const (150K) measured for H//c.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.81Zn0.08Co0.11As2	Ba	1	Fe	1.81	Zn	0.08	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.968		13.002											Fe-122	K		11					11																																																																							mOhm.cm								0.57						m3/C		-0.00000000457							BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154085	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.052 by EPMA.Tc(R) defined as max of (dR/dT).	Ba(Fe,Zn,Co)2As2	Ba1Fe1.79Zn0.1Co0.11As2	Ba	1	Fe	1.79	Zn	0.1	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.968		13.001											Fe-122	K		8					8																																																																							mOhm.cm								0.59															BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154086	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.073 by EPMA.Tc(R) defined as max of (dR/dT). Hall const (150K) measured for H//c.	Ba(Fe,Zn,Co)2As2	Ba1Fe1.75Zn0.14Co0.11As2	Ba	1	Fe	1.75	Zn	0.14	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.972		13.026											Fe-122	K		5					5																																																																							mOhm.cm								0.76						m3/C		-0.00000000481							BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154087	PRB084020513	Zn-content x (in Ba(Fe1.89-2xCo2x)As2) = 0.082 by EPMA.Tc(R) defined as max of (dR/dT).	Ba(Fe,Zn,Co)2As2	Ba1Fe1.73Zn0.16Co0.11As2	Ba	1	Fe	1.73	Zn	0.16	Co	0.11	As	2														3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.977		13.033											Fe-122	K					2																																																																									mOhm.cm								1.02															BaAs,FeAs,Fe(3N),Co(99.5),Zn(4N)		mixture in BN - in Ta capsule - high-P synthesis: heat(1300C,2h, P=3 GPa) - slow cool to 1000C (2h) - Q to RT - keep in vac for 3-5 days.					Linear decrease of critical temperature with increasing Zn substitution in the iron-based superconductor BaFe1.89-2xZn2xCo0.11As2			Superconducting Properties Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 84(2011)020513	Jun Li,Yanfeng Guo,Shoubao Zhang,Shan Yu,Yoshihiro Tsujimoto,Hiroshi Kontani,Kazunari Yamaura,Eiji Takayama-Muromachi		
154088	PRB084014502	K:Fe:Se = 0.79:1.64:2 measured by EDX. broad hump at 115 K in R(T).	K0.8Fe2Se2	K0.8Fe2Se2	K	0.8	Fe	2	Se	2																			2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9106		14.0662											Fe-122	K			30.5				30.5																																																																							mOhm.cm								0.168																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154089	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xCrxSe2	K0.8Fe1.996Cr0.004Se2	K	0.8	Fe	1.996	Cr	0.004	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9111		14.0545											Fe-122	K			20				20																																																																							mOhm.cm								0.32																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154090	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xCrxSe2	K0.8Fe1.993Cr0.007Se2	K	0.8	Fe	1.993	Cr	0.007	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9114		14.0455											Fe-122	K			11				11																																																																							mOhm.cm								1.282																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154091	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xCoxSe2	K0.8Fe1.996Co0.004Se2	K	0.8	Fe	1.996	Co	0.004	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9108		14.0583											Fe-122	K			22				22																																																																							mOhm.cm								0.236																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154092	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xCoxSe2	K0.8Fe1.992Co0.008Se2	K	0.8	Fe	1.992	Co	0.008	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9116		14.0496											Fe-122	K			17				17																																																																							mOhm.cm								0.301																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154093	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xCoxSe2	K0.8Fe1.988Co0.012Se2	K	0.8	Fe	1.988	Co	0.012	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.912		14.0387											Fe-122	K			11				11																																																																							mOhm.cm								0.482																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154094	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xMnxSe2	K0.8Fe1.99Mn0.01Se2	K	0.8	Fe	1.99	Mn	0.01	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9122		14.058											Fe-122	K			31				31																																																																							mOhm.cm								0.185																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154095	PRB084014502	K:Fe:Mn:Se = 0.8:1.59:0.021:2 by EDX.	K0.8Fe2-xMnxSe2	K0.8Fe1.979Mn0.021Se2	K	0.8	Fe	1.979	Mn	0.021	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9133		14.0533											Fe-122	K			31				31																																																																							mOhm.cm								0.228																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154096	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xMnxSe2	K0.8Fe1.97Mn0.03Se2	K	0.8	Fe	1.97	Mn	0.03	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9141		14.0412											Fe-122	K			31.5				31.5																																																																							mOhm.cm								0.224																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154097	PRB084014502	K:Fe:Mn:Se = 0.8:1.61:0.049:2 by EDX	K0.8Fe2-xMnxSe2	K0.8Fe1.951Mn0.049Se2	K	0.8	Fe	1.951	Mn	0.049	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9153		14.0296											Fe-122	K			31.9				31.9																																																																							mOhm.cm								0.262																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154098	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xMnxSe2	K0.8Fe1.933Mn0.067Se2	K	0.8	Fe	1.933	Mn	0.067	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9158		14.0202											Fe-122	K			32				32																																																																							mOhm.cm								0.193																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154099	PRB084014502	compositions of K and Fe are nearly 0.8 and 1.65 , respectively by EDX.	K0.8Fe2-xZnxSe2	K0.8Fe1.995Zn0.005Se2	K	0.8	Fe	1.995	Zn	0.005	Se	2																	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.9103		14.0583											Fe-122	K					4																																																																									mOhm.cm								1.352																	mixture((Fe,M):Se=1:1) - heat(650C,12h). Stoichiometric mixture - sealed in quartz tube(vac) - put in bigger quartz tube - heat(1050C,4h) - slow cool to 700C(4C/h) - FC to RT					Different response of superconductivity to the transition-metal impurities in K0.8Fe2-y-xMxSe2 (M = Cr, Mn, Co, Zn)			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	Phys.Rev.B, 84(2011)014502	Dian Tan,Changjin Zhang,Chuanying Xi,Langsheng Ling,Lei Zhang,Wei Tong,Yi Yu,Guolin Feng,Hongyan Yu,Li Pi,Zhaorong Yang,Shun Tan,Yuheng Zhang		
154100	PRB085014520	London [penet] and [cohere] estimated from Fermiology(ARPES). GL(kappa) = 0.13. Energy gap from STS.	SrPd2Ge2	Sr1Pd2Ge2	Sr	1	Pd	2	Ge	2																		3	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			2.9	2.7			2.7																																				A	esitmated from Fermiology(ARPES)	2990			A	London, esitmated from Fermiology(ARPES)	400			meV	0.5	4	11																																															high-temperature flux method using PdGe self-flux.					Conventional superconductivity in SrPd2Ge2			Diamond Light Source Ltd., Didcot OX11 0DE, United Kingdom	Phys.Rev.B, 85(2012)014520	T. K. Kim,A. N. Yaresko,V. B. Zabolotnyy,A. A. Kordyuk,D. V. Evtushinsky,N. H. Sung,B. K. Cho,T. Samuely,P. Szab,J. G. Rodrigo,J. T. Park,D. S. Inosov,P. Samuely,B. Buchner,S. V. Borisenko		
154101	PRB085180505	multi-band s-wave SC. (beta) = 0.231 mJ/mol.K4 and (delta) = -0.0001 mJ/mol.K6 in SP. Hc(0) = 0.23 T from entropy analysis. GL parameter=29. (dC/Tc) = 7.65 mJ/mol.K2	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2012																										ABC		Cu2Sb	P4/nmm		A	3.7818		6.3463											Fe-111	K		15					15																				T	calculate from Hc(0),GL-parameter	9.4																																		mJ/mol.K2	17	SP	294	SP																																				Bridgman method using W-crucible.					Evidence for s+- - wave pairing symmetry in LiFeAs from its low-temperature specific heat			Department of Physics, Sungkyunkwan University, Suwon 440-746, Republic of Korea	Phys.Rev.B, 85(2012)180505	Dong-Jin Jang,J. B. Hong,Y. S. Kwon,T. Park,K. Gofryk,F. Ronning,D. Thompson,Yunkyu Bang		
154102	PRB085184507	T<STR> = 138.17 K	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																			2012					myu-B/mol	0.756		139																		AB2C2		b-SrRh2As2	Fmmm		A	5.6157	5.5718	12.9424											Fe-122. NPD(HRPD) results at 1.7 K	K					0																																																																																																BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154103	PRB085184507	T<STR> = 136.02 K	(Ba,K)Fe2As2	Ba0.9K0.1Fe2As2	Ba	0.9	K	0.1	Fe	2	As	2																	2012					myu-B/mol	0.741		136.5																		AB2C2		b-SrRh2As2	Fmmm		A	5.5997	5.5587	13.0031											Fe-122. NPD(HRPD) results at 1.7 K	K					0																																																																																																BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154104	PRB085184507	T<STR> = 128.29K	(Ba,K)Fe2As2	Ba0.875K0.125Fe2As2	Ba	0.875	K	0.125	Fe	2	As	2																	2012					myu-B/mol	0.697		130																		AB2C2		b-SrRh2As2	Fmmm		A	5.594	5.5551	13.0243											Fe-122. NPD(HRPD) results at 1.7 K	K					0																																																																																																BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154105	PRB085184507	T<STR> = 122.09 K	(Ba,K)Fe2As2	Ba0.85K0.15Fe2As2	Ba	0.85	K	0.15	Fe	2	As	2																	2012					myu-B/mol	0.702		122.1																		AB2C2		b-SrRh2As2	Fmmm		A	5.589	5.5517	13.0404											Fe-122. NPD(HRPD) results at 1.7 K	K		4					4																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154106	PRB085184507	T<STR> = 112.1 K	(Ba,K)Fe2As2	Ba0.825K0.175Fe2As2	Ba	0.825	K	0.175	Fe	2	As	2																	2012					myu-B/mol	0.683		113.9																		AB2C2		b-SrRh2As2	Fmmm		A	5.5842	5.5492	13.0563											Fe-122. NPD(HRPD) results at 1.7 K	K		10					10																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154107	PRB085184507	T<STR> = 102.00 K	(Ba,K)Fe2As2	Ba0.8K0.2Fe2As2	Ba	0.8	K	0.2	Fe	2	As	2																	2012					myu-B/mol	0.652		102																		AB2C2		b-SrRh2As2	Fmmm		A	5.5767	5.546	13.0736											Fe-122. NPD(HRPD) results at 1.7 K	K		17					17																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154108	PRB085184507	T<STR> = 96.0 K	(Ba,K)Fe2As2	Ba0.79K0.21Fe2As2	Ba	0.79	K	0.21	Fe	2	As	2																	2012					myu-B/mol	0.61		96																		AB2C2		b-SrRh2As2	Fmmm		A	5.575	5.5462	13.0749											Fe-122. NPD(HRPD) results at 1.7 K	K		18					18																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154109	PRB085184507	T<STR> = 93.93 K	(Ba,K)Fe2As2	Ba0.78K0.22Fe2As2	Ba	0.78	K	0.22	Fe	2	As	2																	2012					myu-B/mol	0.55		93.97																		AB2C2		b-SrRh2As2	Fmmm		A	5.5706	5.5461	13.0803											Fe-122. NPD(HRPD) results at 1.7 K	K		23.5					23.5																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154110	PRB085184507	T<STR> = 80.0 K	(Ba,K)Fe2As2	Ba0.76K0.24Fe2As2	Ba	0.76	K	0.24	Fe	2	As	2																	2012					myu-B/mol	0.572		79.9																		AB2C2		b-SrRh2As2	Fmmm		A	5.5672	5.5449	13.0888											Fe-122. NPD(HRPD) results at 1.7 K	K		26					26																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154111	PRB085184507	T<STR> = 74.8 K	(Ba,K)Fe2As2	Ba0.75K0.25Fe2As2	Ba	0.75	K	0.25	Fe	2	As	2																	2012					myu-B/mol	0.456		74.9																		AB2C2		b-SrRh2As2	Fmmm		A	5.5636	5.5476	13.1027											Fe-122. NPD(HRPD) results at 1.7 K	K		28.5					28.5																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154112	PRB085184507		(Ba,K)Fe2As2	Ba0.72K0.28Fe2As2	Ba	0.72	K	0.28	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122. NPD(HRPD) results at 1.7 K	K		34					34																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154113	PRB085184507	Tc(x) and Tn(x) shown in Fig.	(Ba,K)Fe2As2	Ba0.7K0.3Fe2As2	Ba	0.7	K	0.3	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.9165		13.1614											Fe-122. NPD(HRPD) results at 1.7 K	K		36					36	MPH154113																																																																																													BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154114	PRB085184507		(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122. NPD(HRPD) results at 1.7 K	K		38					38																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154115	PRB085184507		(Ba,K)Fe2As2	Ba0.5K0.5Fe2As2	Ba	0.5	K	0.5	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.8893		13.3242											Fe-122. NPD(HRPD) results at 1.7 K	K		34					34																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154116	PRB085184507		(Ba,K)Fe2As2	Ba0.3K0.7Fe2As2	Ba	0.3	K	0.7	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122. NPD(HRPD) results at 1.7 K	K		20					20																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154117	PRB085184507		(Ba,K)Fe2As2	Ba0.1K0.9Fe2As2	Ba	0.1	K	0.9	Fe	2	As	2																	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122. NPD(HRPD) results at 1.7 K	K		7					7																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154118	PRB085184507		KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																			2012																										AB2C2		ThCr2Si2	I4/mmm		A	3.8251		13.7846											Fe-122. NPD(HRPD) results at 1.7 K	K		3					3																																																																																														BaAs,KAs,Fe2As		mixture - ANN(1050C, in Nb-tube, sealed in quartz tube)					Phase diagram of Ba1-xKxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 85(2012)184507	S. Avci,O. Chmaissem,D. Y. Chung,S. Rosenkranz,E. A. Goremychkin,J. P. Castellan,I. S. Todorov,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,M. G. Kanatzidis,R. Osborn		
154119	PRB086140502	New phase appears at T0 K for P > 1.0 GPa, which defined as a peak of (dR/dT). shown in Fig.	(Ba,K)Fe2As2	Ba0.84K0.16Fe2As2	Ba	0.84	K	0.16	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	7.3						7.3	MPH154119																																																																																															self-flux method					Pressure-induced Fermi-surface reconstruction in the iron-arsenide superconductor Ba1-xKxFe2As2: Evidence of a phase transition inside the antiferromagnetic phase			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 86(2012)140502	E. Hassinger,G. Gredat,F. Valade,S. Rene de Cotret,A. Juneau-Fecteau,J.-Ph. Reid,H. Kim,M. A. Tanatar,R. Prozorov,B. Shen,H.-H. Wen,N. Doiron-Leyraud,Louis Taillefer		
154120	PRB086140502	New phase appears at T0 K for P > 1.0 GPa, which defined as a peak of (dR/dT). shown in Fig.	(Ba,K)Fe2As2	Ba0.82K0.18Fe2As2	Ba	0.82	K	0.18	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	10.5						10.5	MPH154120																																																																																															self-flux method					Pressure-induced Fermi-surface reconstruction in the iron-arsenide superconductor Ba1-xKxFe2As2: Evidence of a phase transition inside the antiferromagnetic phase			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 86(2012)140502	E. Hassinger,G. Gredat,F. Valade,S. Rene de Cotret,A. Juneau-Fecteau,J.-Ph. Reid,H. Kim,M. A. Tanatar,R. Prozorov,B. Shen,H.-H. Wen,N. Doiron-Leyraud,Louis Taillefer		
154121	PRB086140502	New phase appears at T0 K for P > 1.0 GPa, which defined as a peak of (dR/dT). shown in Fig.	(Ba,K)Fe2As2	Ba0.81K0.19Fe2As2	Ba	0.81	K	0.19	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	15						15	MPH154121																																																																																															self-flux method					Pressure-induced Fermi-surface reconstruction in the iron-arsenide superconductor Ba1-xKxFe2As2: Evidence of a phase transition inside the antiferromagnetic phase			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 86(2012)140502	E. Hassinger,G. Gredat,F. Valade,S. Rene de Cotret,A. Juneau-Fecteau,J.-Ph. Reid,H. Kim,M. A. Tanatar,R. Prozorov,B. Shen,H.-H. Wen,N. Doiron-Leyraud,Louis Taillefer		
154122	PRB086140502	New phase appears at T0 K for P > 1.0 GPa, which defined as a peak of (dR/dT). shown in Fig.	(Ba,K)Fe2As2	Ba0.79K0.21Fe2As2	Ba	0.79	K	0.21	Fe	2	As	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K	18						18	MPH154122																																																																																															self-flux method					Pressure-induced Fermi-surface reconstruction in the iron-arsenide superconductor Ba1-xKxFe2As2: Evidence of a phase transition inside the antiferromagnetic phase			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 86(2012)140502	E. Hassinger,G. Gredat,F. Valade,S. Rene de Cotret,A. Juneau-Fecteau,J.-Ph. Reid,H. Kim,M. A. Tanatar,R. Prozorov,B. Shen,H.-H. Wen,N. Doiron-Leyraud,Louis Taillefer		
154123	SST023115009	RRR = 12.4. demagnetising correction. PHirr(1.8K)=550 Oe, nHirr(1.8K) = 544 Oe. Isotropic SC, then Hc1//,Hc2// = Hc1/n/, Hc2/n/. GL)kappa) = 1.48.	LaRu2P2	La1Ru2P2	La	1	Ru	2	P	2																		3	2010																										AB2C2		ThCr2Si2	I4/mmm		A			10.67												K		3.7				0.1	3.7										80	Oe	M-H curve, linear approx.		230			114	100	1.8	Oe	RES, R=0.5Rn, WHH		1140	1140										MHC154123		A	from Hc2(0)	540			A	from Hc1(T)	800																												uOhm.cm								8.9				110		cm3/C						MRH154123	n/cm3	30000000000000000000000	La,Ru,P		Sn-flux method. mixture(La:Ru:P:Sn=1:2:2:20) - in alumina crucible - sealed in quartz tube(vac) heat to 1473K(100K/h) - hold (1473K,12h) - cool to 1173K(3K/h) - FC to RT					Isotropic superconductivity in LaRu2P2 with the ThCr2Si2-type structure			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Supercond.Sci.Technol., 23(2010)115009	J J Ying,Y J Yan,R H Liu,XFWang,A FWang,MZhang,Z J Xiang,X H Chen		
154124	SST023054001	not SC	SmFeAs(O,F)	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2010								131																		ABCD		oxypnictide																	Fe-1111	K					5																																																															W/m.K	11.9			THC154124	uV/K	-11.8			TP154125																					RH154125					See SST021095017(2008)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154125	SST023054001		SmFeAs(O,F)	Sm1Fe1As1F0.075O0.925	Sm	1	Fe	1	As	1	F	0.075													O	0.925		1	2010																										ABCD		oxypnictide																	Fe-1111	K			33				33																													T/K		5.36																																			uV/K	-36.1			TP154125																					RH154125					See SST021095017(2008)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154126	SST023054001		SmFeAs(O,F)	Sm1Fe1As1F0.15O0.85	Sm	1	Fe	1	As	1	F	0.15													O	0.85		1	2010																										ABCD		oxypnictide																	Fe-1111	K			51.5				51.5																													T/K		11.35																														W/m.K	2.11			THC154124	uV/K	-29.4			TP154125																					RH154125			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154127	SST023054001	not SC	Fe1+yTe	Fe1.05Te1	Fe	1.05	Te	1																				1	2010																										AB		PbO			A	3.8219		6.2851											Fe-11	K					5																																																																			MTHC154127	uV/K	-6.67			MTP154127															m3/C	0.00000000298					MRH154127			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154128	SST023054001		Fe1+yTe1-xSex	Fe1.04Te0.95Se0.05	Fe	1.04	Te	0.95	Se	0.05																		1	2010																										AB		PbO			A	3.8184		6.2617											Fe-11	K			11				11																																																																																					m3/C	0.00000000129					MRH154127			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154129	SST023054001		Fe1+yTe1-xSex	Fe0.03Te0.9Se0.1	Fe	0.03	Te	0.9	Se	0.1																		1	2010																										AB		PbO			A	3.816		6.2381											Fe-11	K			11.9				11.9																													T/K		16.3																																		MTHC154127	uV/K	-7.58			MTP154127															m3/C	0.0000000005					MRH154129			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154130	SST023054001		Fe1+yTe1-xSex	Fe0.02Te0.85Se0.15	Fe	0.02	Te	0.85	Se	0.15																		1	2010																										AB		PbO			A	3.8133		6.2116											Fe-11	K			12.7				12.7																																																																																					m3/C	0.00000000081					MRH154129			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154131	SST023054001		Fe1+yTe1-xSex	Fe0.02Te0.8Se0.2	Fe	0.02	Te	0.8	Se	0.2																		1	2010																										AB		PbO			A	3.8114		6.1843											Fe-11	K			13.6				13.6																													T/K		12.9																																		MTHC154131	uV/K	-4.77			MTP154131															m3/C	0.00000000136					MRH154131			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154132	SST023054001		Fe1+yTe1-xSex	Fe1Te0.5Se0.5	Fe	1	Te	0.5	Se	0.5																		1	2010																										AB		PbO			A	3.8041		6.053											Fe-11	K			15.6				15.6																													T/K		8.2																																		MTHC154131	uV/K	0.08			MTP154131															m3/C	0.00000000113					MRH154131			Fe(4N),Se(3N),Te(5N)		stoichiometric mixture - react(400-450C,1-2 days in Pyrex) - ground - pellet - heat(800C,7-8 days, in SiO2 tube)					Transport and superconducting properties of Fe-based superconductors: a comparison between SmFeAsO1-xFx and Fe1+yTe1-xSex			CNR/INFM-LAMIA Corso Perrone 24, 16152 Genova, Italy	Supercond.Sci.Technol., 23(2010)054001	MTropeano,I Pallecchi,M R Cimberle,C Ferdeghini,G Lamura,M Vignolo,A Martinelli,A Palenzona,M Putti		
154133	PRB086174516	P = 0 GPa. SC parameters were calculated from muon-SR data. Two gaps: lower gap, d=0.15 meV (2D/kTc) = 1.5. higher one in DB. GL(kappa) = 24	RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				2.55			2.55	MTC154133		K/GPa	-1.32																T														MHC154133							A	Myu-SR	2670			meV	0.49	4.5																																														RbAs,Fe2As		mixture - pellet - ANN(650C,several days, in sealed silica ampoule)					Superfluid density and superconducting gaps of RbFe2As2 as a function of hydrostatic pressure			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174516	Z. Shermadini,H. Luetkens,A. Maisuradze,R. Khasanov,Z. Bukowski,H.-H. Klauss,A. Amato		
154134	PRB086174516	P = 0.6  GPa. SC parameters were calculated from muon-SR data. Two gaps: lower gap, d=0.08 meV (2D/kTc) = 1.1.  higher one in DB. GL(kappa) = 17	RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		1	2012																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K				1.73			1.73																																		MHC154134							A	Myu-SR	2870			meV	0.3	4.1																																														RbAs,Fe2As		mixture - pellet - ANN(650C,several days, in sealed silica ampoule)					Superfluid density and superconducting gaps of RbFe2As2 as a function of hydrostatic pressure			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174516	Z. Shermadini,H. Luetkens,A. Maisuradze,R. Khasanov,Z. Bukowski,H.-H. Klauss,A. Amato		
154135	SST023054003	For P=1.56 GPa, Hc2/n/ = 48T, dHc2/dT = -1.93 T/K. For P=1.99 GPa, Hc2/n/ = 56T, dHc2/dT = -2.05 T/K	Ba(Fe,Co)2As2	Ba1Fe1.924Co0.076As2	Ba	1	Fe	1.924	Co	0.076	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			14.2				14.2	MTC154135																			T	RES, R=0.9Rn, linear approx.			35					T/K				2.38	MHC154135																																																														flux method using FeAs/CoAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154136	SST023054003		Ba(Fe,Co)2As2	Ba1Fe1.906Co0.094As2	Ba	1	Fe	1.906	Co	0.094	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			20				20	MTC154136																			T	RES, R=0.9Rn, linear approx.			46																																																																								flux method using FeAs/CoAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154137	SST023054003	For P=1.51 GPa, Hc2/n/ = 67T, dHc2/dT = -2.68 T/K. For P=1.92 GPa, Hc2/n/ = 57.6T, dHc2/dT = -2.36 T/K	Ba(Fe,Co)2As2	Ba1Fe1.852Co0.148As2	Ba	1	Fe	1.852	Co	0.148	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			23.4				23.4	MTC154137																			T	RES, R=0.9Rn, linear approx.			73					T/K				3.07	MHC154137																																																														flux method using FeAs/CoAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154138	SST023054003		Ba(Fe,Co)2As2	Ba1Fe1.8Co0.2As2	Ba	1	Fe	1.8	Co	0.2	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			18.9				18.9	MTC154138																																																																																															flux method using FeAs/CoAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154139	SST023054003	For P=2.04 GPa, Hc2/n/ = 35.8T, dHc2/dT = -2.01 T/K.	Ba(Fe,Co)2As2	Ba1Fe1.772Co0.228As2	Ba	1	Fe	1.772	Co	0.228	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K			16.4				16.4	MTC154139																			T	RES, R=0.9Rn, linear approx.			27.56					T/K				1.77	MHC154139																																																														flux method using FeAs/CoAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154140	SST023054003	not SC upto 6 GPa.	Ba(Fe,Cr)2As2	Ba1Fe1.946Cr0.054As2	Ba	1	Fe	1.946	Cr	0.054	As	2																3	2010																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					2																																																																																																		flux method using FeAs/CrAs flux.					Electrical transport measurements under pressure for BaFe2As2 compounds doped with Co, Cr, or Sn			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 23(2010)054003	E Colombier,M S Torikachvili,N Ni,A Thaler,S L Bud'ko,P C Canfield		
154141	SST024065006	compositions by WDS. R(ab) and R(c) have broad peak at 160 K and 180 K,respectively. RRR = 6. Anisotropy R(c)/R(ab)  = 4 at 300K.. (dC/gamma*Tc) = 1.33. L-[penet] measured by TDR method	K0.80Fe1.76Se2	K0.8Fe1.76Se2	K	0.8	Fe	1.76	Se	2																		3	2011																										AB2C2		ThCr2Si2	I4/mmm		A	3.8897		14.141											Fe-122	K	30.9		31.6	30.1		0.7	30.1																																																								mJ/mol.K2	5.8	SP								uV/K	-67																													precusor(FeAs) by reacting(1050C). mixture(K,FeAs) - alumina crucible - sealed in silica tube - heat(1050C) - hold(2h) - slow cool to 750C within 50h - FC to RT					Anisotropic magnetism, resistivity, London penetration depth and magneto-optical imaging of superconducting K0.80Fe1.76Se2 single crystals			Ames Laboratory, US DOE and Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	Supercond.Sci.Technol., 24(2011)065006	RHu,K Cho,H Kim,HHodovanets,W E Straszheim,M A Tanatar,R Prozorov,S L Bud'ko,P C Canfield		
154142	SST024065020		PrO(Fe0.9Co0.1)As	Pr1Fe0.9Co0.1As1O1	Pr	1	Fe	0.9	Co	0.1	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9867		8.5915											ZrCuSiAs-type. Fe-1111	K			14.5	13.8			13.8																				T	RES,R=0.9Rn, WHH	64																																																																								Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154143	SST024065020		PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.95P0.05O1	Pr	1	Fe	0.9	Co	0.1	As	0.95	P	0.05											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9817		8.563											ZrCuSiAs-type. Fe-1111	K			14.9	14.2			14.2																																																																																														Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154144	SST024065020	Hc2 defined as R=0.9Rn. Hirr defined as R= zero.	PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.9P0.1O1	Pr	1	Fe	0.9	Co	0.1	As	0.9	P	0.1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.981		8.5585											ZrCuSiAs-type. Fe-1111	K			15.9	14.7			14.7	TC154144																																	HC154144																																																												Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154145	SST024065020		PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.85P0.15O1	Pr	1	Fe	0.9	Co	0.1	As	0.85	P	0.15											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9764		8.5446											ZrCuSiAs-type. Fe-1111	K			12.9	12.2			12.2																																																																																														Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154146	SST024065020	Hc2 defined as R=0.9Rn. Hirr defined as R= zero.	PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.8P0.2O1	Pr	1	Fe	0.9	Co	0.1	As	0.8	P	0.2											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9756		8.5416											ZrCuSiAs-type. Fe-1111	K			11.5	10.9			10.9																																		HC154146																																																												Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154147	SST024065020	Hc2 defined as R=0.9Rn. Hirr defined as R= zero.	PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.7P0.3O1	Pr	1	Fe	0.9	Co	0.1	As	0.7	P	0.3											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9743		8.5197											ZrCuSiAs-type. Fe-1111	K			10.6	9.86			9.86																				T	RES,R=0.9Rn, WHH	29												HC154147																																																												Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154148	SST024065020	Fe2As2O12(5%), FePO4(5%)	PrO(Fe0.9Co0.1)As1-xPx	Pr1Fe0.9Co0.1As0.5P0.5O1	Pr	1	Fe	0.9	Co	0.1	As	0.5	P	0.5											O	1		1	2011																										ABCD		oxypnictide	P4/nmm		A	3.9637		8.4756											ZrCuSiAs-type. Fe-1111	K				7.46			7.46																																																																																														Pr,Pr6O11,Co3O4,FeAs,FeP,As		mixture - sealed in silica tube(vac) - heat(950C,24h) - ground - disc - wrapped in Ta foil - SIN(1100C,48h, in evacuated silica) - cool to RT					Superconducting and critical properties of PrOFe0.9Co0.1As: effect of P doping			Material Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, India	Supercond.Sci.Technol., 24(2011)065020	Shilpam Sharma,Jai Prakash,Gohil S Thakur,A T Satya,A Bharathi,A K Ganguli,C S Sundar		
154150	SST024065010	Film. Fe-content, x not given. gap measured by point contact Andreev reflection. contact resistance = 26 Ohm. gap(T) tend to zero at 21.6 K.(fitting parameter)	Sm(O1-xFx)FeAs	Sm1Fe1As1F0.2O0.8	Sm	1	Fe	1	As	1	F	0.2													O	0.8		4	2011																										ABCD		oxypnictide																	Fe-1111	K	25	29	34			3	29																																														meV	10	3.6	1																						uOhm.cm							100																		pulsed laser deposition					Point-contact study of ReFeAsO1-xFx (Re = La, Sm) superconducting films			B Verkin Institute for Low Temperature Physics and Engineering, National Academy of Sciences of Ukraine, 47 Lenin Avenue, 61103, Kharkiv, Ukraine	Supercond.Sci.Technol., 24(2011)065010	Yu G Naidyuk,O E Kvitnitskaya,I K Yanson,G Fuchs,S Haindl,M Kidszun,L Schultz,B Holzapfel		
154151	SST024065010	Film. Fe-content, x not given. gap measured by point contact Andreev reflection.  gap(T) tend to zero at 18 K. (fitting parameter). carrier < 1 E+21 /cm3 from Hall coeffic.	La(O1-xFx)FeAs	La1Fe1As1F0.2O0.8	La	1	Fe	1	As	1	F	0.2													O	0.8		4	2011																										ABCD		oxypnictide																	Fe-1111	K		25					25																																																3.5	1																																															pulsed laser deposition					Point-contact study of ReFeAsO1-xFx (Re = La, Sm) superconducting films			B Verkin Institute for Low Temperature Physics and Engineering, National Academy of Sciences of Ukraine, 47 Lenin Avenue, 61103, Kharkiv, Ukraine	Supercond.Sci.Technol., 24(2011)065010	Yu G Naidyuk,O E Kvitnitskaya,I K Yanson,G Fuchs,S Haindl,M Kidszun,L Schultz,B Holzapfel		
154152	PRL103147002	gap by muon-SR. C<el> = A*T + B*T^3 (A=1.31 mJ/mol.K2, B=2.88 mJ/mol.K4). (dC/Tc) = 130 mJ/mol.K2. (dC/gamma:Tc) = 2.06.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																			2009																										AB4C12		skutterudite																		K		7.9					7.9																				T	RES. extrapolation	1.82												MHC154152		A	from Hc2	181			A		1140					4.7	16							mJ/mol.K2	63	SP	189	SP																																				See PRL100017002					Superfluid Density and Energy Gap Function of Superconducting PrPt4Ge12			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 103(2009)147002	A. Maisuradze,M. Nicklas,R. Gumeniuk,C. Baines,W. Schnelle,H. Rosner,A. Leithe-Jasper,Yu. Grin,R. Khasanov		
154153	PRB087144502	RRR = 200. R<ab> =A*T^1.5 for T > 9 K. thermal conductivity THC<ab> = a + (ph-term). residual linear term, a = 1.27 mW/cm.K2. FIG shows k/T vs H	CsFe2As2	Cs1Fe2As2	Cs	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K	1.81						1.81																				T	RES(R= 0 ). extrapolation			1.4										MHC154153																															MTHC154153						uOhm.cm							1.8																		self-flux method. cleaved sample (3.5*10 mm, 30um thickness)					Nodal gap in iron-based superconductor CsFe2As2 probed by quasiparticle heat transport			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, P. R. China	Phys.Rev.B, 87(2013)144502	X. C. Hong,X. L. Li,B. Y. Pan,L. P. He,A. F. Wang,X. G. Luo,X. H. Chen,S. Y. Li		
154154	PRB087174502		Zr1-xVxB2	Zr0.99V0.01B2	Zr	0.99	V	0.01	B	2																		1	2013																										AB2		AlB2	P6/mmm		A	3.1647		3.529												K			6.4				6.4	MTC154154																																																																																															Ar-arc melting. 5 times for homogenizing					Evidence of multiband behavior in the superconducting alloy Zr0.96V0.04B2			Escola de Engenharia de Lorena, Universidade de Sao Paulo, P.O. Box 116, Lorena, SP, Brazil	Phys.Rev.B, 87(2013)174502	S. T. Renosto,H. Consoline,C. A. M. dos Santos,J. Albino Aguiar,Soon-Gil Jung,J. Vanacken,V. V. Moshchalkov,Z. Fisk,A. J. S. Machado		
154155	PRB087174502	optimal. lattice term in SP beta = 0.034 mJ/mol.K4.  (dC/gamma*T) = 0.42.	Zr1-xVxB2	Zr0.96V0.04B2	Zr	0.96	V	0.04	B	2																		1	2013																										AB2		AlB2	P6/mmm		A	3.1641		3.524												K			8.7				8.7											mT	M-H curve	2.5							T	RES, WHH	16.3			11.5			4.5						MHC154155		A	from Hc2	44.9															MSP154155			mJ/mol.K2	3.8	SP	555.6	SP																																				Ar-arc melting. 5 times for homogenizing					Evidence of multiband behavior in the superconducting alloy Zr0.96V0.04B2			Escola de Engenharia de Lorena, Universidade de Sao Paulo, P.O. Box 116, Lorena, SP, Brazil	Phys.Rev.B, 87(2013)174502	S. T. Renosto,H. Consoline,C. A. M. dos Santos,J. Albino Aguiar,Soon-Gil Jung,J. Vanacken,V. V. Moshchalkov,Z. Fisk,A. J. S. Machado		
154156	PRB087174502	secondary phase. solubility limit x = 0.04.	Zr1-xVxB2	Zr0.95V0.05B2	Zr	0.95	V	0.05	B	2																		1	2013																										AB2		AlB2	P6/mmm		A	3.1631		3.522												K			8.2				8.2																																																																																																Ar-arc melting. 5 times for homogenizing					Evidence of multiband behavior in the superconducting alloy Zr0.96V0.04B2			Escola de Engenharia de Lorena, Universidade de Sao Paulo, P.O. Box 116, Lorena, SP, Brazil	Phys.Rev.B, 87(2013)174502	S. T. Renosto,H. Consoline,C. A. M. dos Santos,J. Albino Aguiar,Soon-Gil Jung,J. Vanacken,V. V. Moshchalkov,Z. Fisk,A. J. S. Machado		
154157	PRB087174510	T<STR> = 350K. For T>350K, cubic, Pa3, #205, a=6.4152, alpha=90. (dC/gamma*Tc) - 1.0.	Ir3Te8	Ir3Te8	Ir	3	Te	8																				3	2013					uB/Ir	0.024	-0.7																			A3B8			R-3	148	A	6.4024													rhombohedral , alpha = 90.017 for T < 350 K.	K			1.8	1.8			1.8										16																																														mJ/mol.K2	11	SP	246	SP											uOhm.cm		45																							poly crystal(ir3Te8) made by slow heating to 1000C and hold 7 days. mixed with Te powder - heat(1050C, 48h , in quartz tube)  - slow cool to 700C.					Observation of superconductivity and anomalous electrical resistivity in single-crystal Ir3Te8			Department of Physics and Astronomy, Center for Advanced Materials, University of Kentucky, Lexington, Kentucky 40506, USA	Phys.Rev.B, 87(2013)174510	L. Li,T. F. Qi,L. S. Lin,X. X. Wu,X. T. Zhang,K. Butrouna,V. S. Cao,Y. H. Zhang,Jiangping Hu,S. J. Yuan,P. Schlottmann,L. E. De Long,G. Cao		
154158	PRB087174512	Tc= 1.42 K by ac-SUS. lattice term in SP (beta) = 0.82 mJ/mol.K4	(La,Hf)OBiS2	La0.8Hf0.2Bi1S2O1	La	0.8	Hf	0.2	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0589		13.818												K		2.36		2.81			2.36																				T	RES, R=0.5Rn													HC154158																						mJ/mol.K2	2.12	SP	228	SP																																				"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154159	PRB087174512		(La,Hf)OBiS2	La0.7Hf0.3Bi1S2O1	La	0.7	Hf	0.3	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		1.74					1.74																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154160	PRB087174512		(La,Hf)OBiS2	La0.6Hf0.4Bi1S2O1	La	0.6	Hf	0.4	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		1.74					1.74																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154161	PRB087174512		(La,Zr)OBiS2	La0.8Zr0.2Bi1S2O1	La	0.8	Zr	0.2	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0585		13.807												K		1.66					1.66																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154162	PRB087174512		(La,Ti)OBiS2	La0.8Ti0.2Bi1S2O1	La	0.8	Ti	0.2	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0524		13.804												K		2.35					2.35																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154163	PRB087174512		(La,Ti)OBiS2	La0.7Ti0.3Bi1S2O1	La	0.7	Ti	0.3	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		2.22					2.22																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154164	PRB087174512	not SC.	(La,Sr)OBiS2	La0.8Sr0.2Bi1S2O1	La	0.8	Sr	0.2	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0692		13.694												K					1.2																																																																																																		"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154165	PRB087174512	R(T) minimum at 220 K.	LaOBiS2	La1Bi1S2O1	La	1	Bi	1	S	2															O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0624		13.858												K					1.2																																																																																																		"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154166	PRB087174512	Tc= 2.05 K by ac-SUS. lattice term in SP (beta) = 0.91 mJ/mol.K4. (dC/gamma*Tc) = 0.91	(La,Th)OBiS2	La0.85Th0.15Bi1S2O1	La	0.85	Th	0.15	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		2.85		2.51			2.85																				T	RES, R=0.5Rn													HC154166																						mJ/mol.K2	0.58	SP	0.91	SP																																				"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154167	PRB087174512	Tc= 1.65 K by ac-SUS.	(La,Th)OBiS2	La0.8Th0.2Bi1S2O1	La	0.8	Th	0.2	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0506		13.774												K		2.046					2.046																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154168	PRB087174512	Tc= 1.73 K by ac-SUS.	(La,Th)OBiS2	La0.7Th0.3Bi1S2O1	La	0.7	Th	0.3	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		2.04					2.04																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154169	PRB087174512		(La,Th)OBiS2	La0.6Th0.4Bi1S2O1	La	0.6	Th	0.4	Bi	1	S	2													O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129																K		2.12					2.12																																																																																																"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154170	PRB087174512	R(T) minimum at 206 K.	ThOBiS2	Th1Bi1S2O1	Th	1	Bi	1	S	2															O	1		1	2013																										ABCD2		CeOBiS2	P4/nmm	129	A	3.9623		13.5062												K					1.2																																																																																																		"solid state metathesis reaction: details, see ""Solid State Commun., 152(2012)632"""					Superconductivity induced by electron doping in La1-xMxOBiS2 (M= Ti, Zr, Hf, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 87(2013)174512	D. Yazici,K. Huang,B. D. White,I. Jeon,V. W. Burnett,A. J. Friedman,I. K. Lum,M. Nallaiyan,S. Spagna,M. B. Maple		
154171	PRB087174515	not SC for x = < 0.2 in LaO(Fe1-xMnx)As	LaO(Fe,Mn)As	La1Fe0.9Mn0.1As1O1	La	1	Fe	0.9	Mn	0.1	As	1													O	1		1	2013																										ABCD		oxypnictide				4.0393		8.7739											Fe-1111	K					12			LAT154171																																																																																																				Short-range magnetic order and effective suppression of superconductivity by manganese doping in LaFe1-xMnxAsO1-yFy			Department Chemie, Ludwig-Maximilians Universitat Munchen, 81377 Munchen, Germany	Phys.Rev.B, 87(2013)174515	Rainer Frankovsky,Hubertus Luetkens,Frank Tambornino,Alexey Marchuk,Gwendolyne Pascua,Alex Amato,Hans-Henning Klauss,Dirk Johrendt		
154172	PRB087174515	not SC for y = < 0.5 in La(O1-yFy)(Fe0.9Mn0.1)As. Impurity: LaAs,Na1.5La1.5F6	La(O,F)(Fe0.9Mn0.1)As	La1Fe0.9Mn0.1As1F0.2O0.8	La	1	Fe	0.9	Mn	0.1	As	1	F	0.2											O	0.8		1	2013																										ABCD		oxypnictide				4.0287		8.7538											Fe-1111	K					12			LAT154172																																																																																																				Short-range magnetic order and effective suppression of superconductivity by manganese doping in LaFe1-xMnxAsO1-yFy			Department Chemie, Ludwig-Maximilians Universitat Munchen, 81377 Munchen, Germany	Phys.Rev.B, 87(2013)174515	Rainer Frankovsky,Hubertus Luetkens,Frank Tambornino,Alexey Marchuk,Gwendolyne Pascua,Alex Amato,Hans-Henning Klauss,Dirk Johrendt		
154173	PRB087174517	NMR of <75>As and <23>Na were measured at H//c = 6.4 T. gap (single isotropic) from Knight shift of <23>Na. (dC/gamma*Tc) = 1.14.	Na(Fe,Co)As	Na1Fe0.975Co0.025As1	Na	1	Fe	0.975	Co	0.025	As	1																3	2013																										ABC		PbFCl																	Fe-111	K				21			21																																									A	NMR of <23>Na		5327		meV	3.6	4	6																																															crystals were grown at Univ. of Tennessee					Spin pairing and penetration depth measurements from nuclear magnetic resonance in NaFe0.975Co0.025As			Department of Physics and Astronomy, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 87(2013)174517	Sangwon Oh,A. M. Mounce,Jeongseop A. Lee,W. P. Halperin,C. L. Zhang,S. Carr,Pengcheng Dai		
154174	PRB087180501	Tn = 203 and 116 K for heating and cooling proces, respectively,  measured by R(T). For IrTe2 , Tn = 268K and 238 K., respectively.	CuxIrTe2	Cu0.03Ir1Te2	Cu	0.03	Ir	1	Te	2																		1	2013								203																				CdI2	P-3m		A	3.9344		5.3974											1T-TaS2, trigonal at RT	K				2.53			2.53																																																																																																mixture(Ir,Te powder) - heat(900C,20h) - mixed with Cu powder - pellet - heat(300C,200h)					Superconductivity in CuxIrTe2 driven by interlayer hybridization			Department of Applied Physics and Quantum-Phase Electronics Center (QPEC), University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 87(2013)180501	M. Kamitani,M. S. Bahramy,R. Arita,S. Seki,T. Arima,Y. Tokura,S. Ishiwata		
154175	PRB087180501		CuxIrTe2	Cu0.05Ir1Te2	Cu	0.05	Ir	1	Te	2																		1	2013																												CdI2	P-3m		A	3.9408		5.3975											1T-TaS2, trigonal at RT	K				2.84			2.84																																																																																																mixture(Ir,Te powder) - heat(900C,20h) - mixed with Cu powder - pellet - heat(300C,200h)					Superconductivity in CuxIrTe2 driven by interlayer hybridization			Department of Applied Physics and Quantum-Phase Electronics Center (QPEC), University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 87(2013)180501	M. Kamitani,M. S. Bahramy,R. Arita,S. Seki,T. Arima,Y. Tokura,S. Ishiwata		
154176	PRB087180501		CuxIrTe2	Cu0.07Ir1Te2	Cu	0.07	Ir	1	Te	2																		1	2013																												CdI2	P-3m		A	3.9426		5.3975											1T-TaS2, trigonal at RT	K				2.71			2.71																																																																																																mixture(Ir,Te powder) - heat(900C,20h) - mixed with Cu powder - pellet - heat(300C,200h)					Superconductivity in CuxIrTe2 driven by interlayer hybridization			Department of Applied Physics and Quantum-Phase Electronics Center (QPEC), University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 87(2013)180501	M. Kamitani,M. S. Bahramy,R. Arita,S. Seki,T. Arima,Y. Tokura,S. Ishiwata		
154177	PRB087180501		CuxIrTe2	Cu0.1Ir1Te2	Cu	0.1	Ir	1	Te	2																		1	2013																												CdI2	P-3m		A	3.9503		5.3992											1T-TaS2, trigonal at RT	K				2.41			2.41																																																																																																mixture(Ir,Te powder) - heat(900C,20h) - mixed with Cu powder - pellet - heat(300C,200h)					Superconductivity in CuxIrTe2 driven by interlayer hybridization			Department of Applied Physics and Quantum-Phase Electronics Center (QPEC), University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 87(2013)180501	M. Kamitani,M. S. Bahramy,R. Arita,S. Seki,T. Arima,Y. Tokura,S. Ishiwata		
154178	PRB087180508	H//c. kappa(GL) = 80. calculated from Hc2/Hc1 = 2k^2*ln(k)	Pr4Fe2As2TexO4	Pr4Fe2As2Te0.88O4	Pr	4	Fe	2	As	2	Te	0.88													O	4		3	2013																												oxypnictide	I4/mmm	139	A	4.0165		29.8572											FeAs-42214 or Fe-22414	K	24.8	25.1	25.5	25			25.1										95	mT	M-H curve						2	5	T	SUS(on), WHH			6.5					T/K	SUS(on)			0.35	HC154178		A	from Hc2		70		A	cohere, kappa(GL)		5600																											mOhm.cm												1.84											PrAs,PrTe,FeO		precursor made from mixture(PeAs:PrTe:FeO=0.9:0.1:1) - high-P synthesis(3.5GPa,NaCl/KCl flux) - heat(1500C,1h) - keep(60h) - cool to 1050C(45C/h) - cool to RT					Pr4Fe2As2Te1-xO4: A layered FeAs-based superconductor			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 87(2013)180508	S. Katrych,K. Rogacki,A. Pisoni,S. Bosma,S. Weyeneth,R. Gaal,N. D. Zhigadlo,J. Karpinski,L. Forro		
154179	PRB087214504	RRR = 60. STM measured for various T, (0.15 < T < 1.2) and H. gap size and gap(T) well described by BCS.	LaSb2	La1Sb2	La	1	Sb	2																				3	2013																										AB2		SmSb2			A	6.319	6.1739	18.57												K		1.2					1.2																				T	STM		0.7	0.15												A	from Hc2		100	460						meV	0.182	3.52	11																																															Flux method using excess Sb-flux.					Scanning tunneling microscopy in the superconductor LaSb2			Laboratorio de Bajas Temperaturas, Departamento de F?sica de la Materia Condensada, Instituto de Ciencia de Materiales Nicolas Cabrera, Facultad de Ciencias, Universidad Autonoma de Madrid, E-28049 Madrid, Spain	Phys.Rev.B, 87(2013)214504	J. A. Galvis,H. Suderow,S. Vieira,S. L. Bud'ko,P. C. Canfield		
154180	PRB087184504	bulk SC. Half-Heusler compound. Topological SC. Hall const.(2K) = 256 mm3/C. n(2K) = 2.44E+19/cm3	LuPtBi	Lu1Pt1Bi1	Lu	1	Pt	1	Bi	1																		3	2013																										ABC					A	6.578													cubic.	K			1				1																				T	RES(0.9Rn). GL-theory			1.6										MHC154180		A	from Hc2		140																																uOhm.cm								74				137		cm3/C				0.256	10	MRH154180	n/cm3	24400000000000000000			flux method using Bi-flux.					Superconductivity in the noncentrosymmetric half-Heusler compound LuPtBi: A candidate for topological superconductivity			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 87(2013)184504	F. F. Tafti,Takenori Fujii,A. Juneau-Fecteau,S.Rene de Contret,N. Doiron-Leyraud,Atsushi Asamitsu,Louis Taillefer		
154200	PRB087214510	impurity phase: IrSe2(<5%). e-ph = 0.51.	Cu(Ir,Pt)2Se4	Cu1Ir1.8Pt0.2Se4	Cu	1	Ir	1.8	Pt	0.2	Se	4																1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3358														K			1.06			0.1	1.06																																																								mJ/mol.K2	13.1	SP	225	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154201	PRB087214510	impurity phase: IrSe2(<5%). e-ph = 0.57. (dC/gamma*Tc) = 1.58	Cu(Ir,Pt)2Se4	Cu1Ir1.6Pt0.4Se4	Cu	1	Ir	1.6	Pt	0.4	Se	4																1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3453														K			1.76				1.76	MTC154201																			T	RES. WHH	3.2							T/K	RES	2.6					A	from Hc2	101															MSP154201			mJ/mol.K2	16.5	SP	212	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154202	PRB087214510	impurity phase: IrSe2(<5%). e-ph = 0.56. (dC/gamma*Tc) = 1.44.	Cu(Ir,Pt)2Se4	Cu1Ir1.4Pt0.6Se4	Cu	1	Ir	1.4	Pt	0.6	Se	4																1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3625														K			1.64				1.64	MTC154201																			T	RES. WHH	3.6							T/K	RES	3.2					A	from Hc2	96																		mJ/mol.K2	15.7	SP	227	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154203	PRB087214510	impurity phase: IrSe2(<5%). not SC	Cu(Ir,Pt)2Se4	Cu1Ir1.2Pt0.8Se4	Cu	1	Ir	1.2	Pt	0.8	Se	4																1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3742														K					0.5																																																										mJ/mol.K2	10.9	SP	211	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154204	PRB087214510	not SC.	Cu(Ir,Pt)2Se4	Cu1Ir1Pt1Se4	Cu	1	Ir	1	Pt	1	Se	4																1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3864														K					0.5																																																										mJ/mol.K2	3	SP	249	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154205	PRB087214510	not SC. Semiconductor-like(dR/dT<0). R(T) = R0*exp(-T0/T)^(1/n), n=4.	Cu(Ir,Pt)2Se4	Cu1Ir2Se4	Cu	1	Ir	2	Se	4																		1	2013																										AB2C4		spinel	Fd-3m	229	A	10.3199														K					0.5																																																										mJ/mol.K2	7	SP	222	SP																																		Cu(99.5),Ir(99.95),Pt(99.95),Se(5N)		solid state reaction. mixture - pellet - sealed in quartz tube - heat(1123K,96h) - reground - pellet - SIN(1123K,48h)					Superconductivity in the Cu(Ir1-xPtx)2Se4 spinel			Department of Chemistry, Princeton University, Princeton, New Jersey, 08544, USA	Phys.Rev.B, 87(2013)214510	Huixia Luo,Tomasz Klimczuk,Lukas Muchler,Leslie Schoop,Daigorou Hirai,M. K. Fuccillo,C. Felser,R. J. Cava		
154206	SSC1570021	RH300 shows Hall const. at 10 K.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																										ABCD2			P4/nmm		A	4.069		13.366											ZrCuSiAs	K			2.7				2.7										6										T	RES. WHH	1.9							T/K	RES	1			HC154206		A	from Hc2	130																																															m3/C	0.0000000504036						n/cm3	124000000000000000000	La,Bi,S,LaF3,La2O3		mixture - pellet - sealed in quartz tube(vac) - heat to 800C(2C/min) - keep(800C,12h) - cool to RT within 6h					Appearance of superconductivity in layered LaO0.5F0.5BiS2			Quantum Phenomena and Applications Division, National  Physical Laboratory (CSIR), Dr.K.S.Krishnan Road, New Delhi 110012, India	Solid State Commun., 157(2013)21	V.P.S. Awana,AnujKumar,RajveerJha,ShivaKumarSingh,AnandPal,Shruti,J.Saha,S.Patnaik		
154207	SSC1570021	not SC	LaOBiS2	La1Bi1S2O1	La	1	Bi	1	S	2															O	1		1	2013																										ABCD2			P4/nmm		A	4.066		13.862											ZrCuSiAs	K					1.5																																																																																																La,Bi,S,LaF3,La2O3		mixture - pellet - sealed in quartz tube(vac) - heat to 800C(2C/min) - keep(800C,12h) - cool to RT within 6h					Appearance of superconductivity in layered LaO0.5F0.5BiS2			Quantum Phenomena and Applications Division, National  Physical Laboratory (CSIR), Dr.K.S.Krishnan Road, New Delhi 110012, India	Solid State Commun., 157(2013)21	V.P.S. Awana,AnujKumar,RajveerJha,ShivaKumarSingh,AnandPal,Shruti,J.Saha,S.Patnaik		
154208	PRB084184512	[RH300] shows RH200. RH100 = -4.48 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (71.78, 0.3662, 2.13)	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2011								137																		AB2C2		ThCr2Si2																	Fe-122	K					2																																																																																							m3/C	-0.000000000957										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154209	PRB084184512	[RH300] shows RH200. RH100 = 6.41 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (33.87, 0.1767, 2.32)	(Ba,K)Fe2As2	Ba0.9K0.1Fe2As2	Ba	0.9	K	0.1	Fe	2	As	2																3	2011								123																		AB2C2		ThCr2Si2																	Fe-122	K		5.5					5.5																																																																																					m3/C	0.000000000365										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154210	PRB084184512	[RH300] shows RH200. RH100 = 4.71 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (33.04, 0.2898, 2.20)	(Ba,K)Fe2As2	Ba0.88K0.12Fe2As2	Ba	0.88	K	0.12	Fe	2	As	2																3	2011								117																		AB2C2		ThCr2Si2																	Fe-122	K		10					10																																																																																					m3/C	0.000000000617										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154211	PRB084184512	[RH300] shows RH200. RH100 = 3.32 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (26.86, 1.168, 1.94)	(Ba,K)Fe2As2	Ba0.85K0.15Fe2As2	Ba	0.85	K	0.15	Fe	2	As	2																3	2011								100																		AB2C2		ThCr2Si2																	Fe-122	K		18					18																																																																																					m3/C	0.000000000554										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154212	PRB084184512	[RH300] shows RH200. RH100 = 2.44 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (26.82, 1.4735, 1.892)	(Ba,K)Fe2As2	Ba0.8K0.2Fe2As2	Ba	0.8	K	0.2	Fe	2	As	2																3	2011								90.5																		AB2C2		ThCr2Si2																	Fe-122	K		22					22																																																																																					m3/C	0.00000000068										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154213	PRB084184512	[RH300] shows RH200. RH100 = 2.32 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (16.51, 7.24, 1.56)	(Ba,K)Fe2As2	Ba0.75K0.25Fe2As2	Ba	0.75	K	0.25	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2																	Fe-122	K		31					31																																																																																					m3/C	0.00000000068										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154214	PRB084184512	[RH300] shows RH200. RH100 = 1.436 E-9 m3/C. Rab = R0 + A*T^n for Tc < T < Tn: R0(uOhm.cm), A, n are (-1.46, 104.68, 1.01)	(Ba,K)Fe2As2	Ba0.63K0.37Fe2As2	Ba	0.63	K	0.37	Fe	2	As	2																3	2011																										AB2C2		ThCr2Si2																	Fe-122	K		39					39																																																																																					m3/C	0.000000000743										self flux method using FeAs flux					Transport properties and asymmetric scattering in Ba1-xKxFe2As2 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, China	Phys.Rev.B, 84(2011)184512	Bing Shen,Huan Yang,Zhao-Sheng Wang,Fei Han,Bin Zeng,Lei Shan,Cong Ren,Hai-Hu Wen		
154215	PRL108237001	C = gamma*T + beta*T^3 + delta*T^5 : beta=1.29 mJ/mol.K4, delta= 0.00798 mJ/mol.K6. Gap from SP fitting using alpha-model	SrPt3P	Sr1Pt3P1	Sr	1	Pt	3	P	1																		1	2012																										ABC3			P4/nmm	129		5.8094		5.3833												K		8.4					8.4										97										T	RES(0.5Rn), linear approx.	5.7												MHC154215		A	from Hc2	76								meV	1.85	5.1	14							mJ/mol.K2	12.7	SP	190	SP																															MRH154215			Pt,P,Sr(Ca,La)		solid state reaction. mixture - sealed in quartz tube(Ar) - heat to 400 C - hold(400C,12h) - CAL(900C,12h) - ANN(900C,several days, in Ar)					Strong Coupling Superconductivity at 8.4 K in an Antiperovskite Phosphide SrPt3P			Department of Advanced Materials, University of Tokyo, and JST-TRIP, Kashiwa, Chiba 275-8651, Japan	Phys.Rev.Lett., 108(2012)237001	T. Takayama,K. Kuwano,D. Hirai,Y. Katsura,A. Yamamoto,H. Takagi		
154216	PRL108237001		CaPt3P	Ca1Pt3P1	Ca	1	Pt	3	P	1																		1	2012																										ABC3			P4/nmm	129		5.6673		5.4665												K		6.6					6.6																																																								mJ/mol.K2	17.7	SP																																				Pt,P,Sr(Ca,La)		solid state reaction. mixture - sealed in quartz tube(Ar) - heat to 400 C - hold(400C,12h) - CAL(900C,12h) - ANN(900C,several days, in Ar)					Strong Coupling Superconductivity at 8.4 K in an Antiperovskite Phosphide SrPt3P			Department of Advanced Materials, University of Tokyo, and JST-TRIP, Kashiwa, Chiba 275-8651, Japan	Phys.Rev.Lett., 108(2012)237001	T. Takayama,K. Kuwano,D. Hirai,Y. Katsura,A. Yamamoto,H. Takagi		
154217	PRL108237001		LaPt3P	La1Pt3P1	La	1	Pt	3	P	1																		1	2012																										ABC3			P4/nmm	129		5.7626		5.465												K		1.5					1.5																																																								mJ/mol.K2	6.7	SP																																				Pt,P,Sr(Ca,La)		solid state reaction. mixture - sealed in quartz tube(Ar) - heat to 400 C - hold(400C,12h) - CAL(900C,12h) - ANN(900C,several days, in Ar)					Strong Coupling Superconductivity at 8.4 K in an Antiperovskite Phosphide SrPt3P			Department of Advanced Materials, University of Tokyo, and JST-TRIP, Kashiwa, Chiba 275-8651, Japan	Phys.Rev.Lett., 108(2012)237001	T. Takayama,K. Kuwano,D. Hirai,Y. Katsura,A. Yamamoto,H. Takagi		
154218	PRL108187003	Anisotropy, R(a):R(b):R(c) = 80:1:1600(at 300K) and 150:1:1600(at 4.2 K). (-dHc2/dT) = 1.5, 19.5, 0.5 T/K for a, b, c axis , respectively. [cohere] = 100, 300, 25 A for a, b, c axis.	Li0.9Mo6O17	Li0.9Mo6O17	Li	0.9	Mo	6																	O	17		3	2012																										AB6C17		bronze																		K		2.2					2.2																													T/K	RES(max of dR/dT)		19.5	0.5	HC154218		A	from Hc2(extrapolation)		300	25																																																													Upper Critical Magnetic Field far above the Paramagnetic Pair-Breaking Limit of Superconducting One-Dimensional Li0:9Mo6O17 Single Crystals			H.H. Wills Physics Laboratory, University of Bristol, Tyndall Avenue, BS8 1TL, United Kingdom	Phys.Rev.Lett., 108(2012)187003	J.-F. Mercure,A. F. Bangura,Xiaofeng Xu,N. Wakeham,A. Carrington,P. Walmsley,M. Greenblatt,N. E. Hussey		
154219	MAT1209.4229	R = R0 + A*T^n (R0=4.34 uOhm.cm, n = 3.01) for 3.5 < T <31 K. Nodeless SC from thermal conductivity measurements	Ir0.5Pt0.5Te2	Ir0.5Pt0.5Te2	Ir	0.5	Pt	0.5	Te	2																		3	2012																										AB2		CdI2																		K			3				3										100										T	RES(zero), extrapolation)			0.09										MHC154219																			MSP154219			mJ/mol.K2	9.2	SP							MTHC154219																															self-flux method					Nodeless superconductivity in Ir1-xPtxTe2 with strong spin-orbital coupling			State Key Laboratory of Surface Physics, Department of Physics,and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, P. R. China	cond-mat/1209.4229	S. Y. Zhou,X. L. Li,B. Y. Pan,X. Qiu,J. Pan,X. C. Hong,Z. Zhang,A. F. Fang,N. L. Wang,S. Y. Li		
154220	DRM0201273	thickness = 3 um	B-doped diamond	C1	C	1																							2011																												diamond																		K			3.1				3.1																																																																																																1st: undoped diamond films on Si using MPCVD reactor, then pyramidal surface with [111], 2nd: B-doped films using MPCVD reactor, thickness = 3 um					Superconductivity in heavily B-doped diamond layers deposited on highly oriented diamond films			Aoyama-Gakuin University	Diamond Relat.Mater., 20(2011)1273	T. Nuranaka,K. Kobashi,H. Okabe,T. Tachibana,Y. Yokota,K. Hayashi,N. Mawakami,J. Akimitsu		
154221	DRM0201273	thickness = 2 um. Carrier density (n) estimated from Tc vs n curve	B-doped diamond	C1	C	1																							2011																												diamond																		K			4.1				4.1																				T	RES(on)	3.98							T/K	RES(on)	1.48					A		88																																																						n/cm3	2200000000000000000000			1st: Si[100] films by bias-nucleation method, then undoped diamond films with pyramidal surface. 2nd: B-doped films deposited. d = 2 um.					Superconductivity in heavily B-doped diamond layers deposited on highly oriented diamond films			Aoyama-Gakuin University	Diamond Relat.Mater., 20(2011)1273	T. Nuranaka,K. Kobashi,H. Okabe,T. Tachibana,Y. Yokota,K. Hayashi,N. Mawakami,J. Akimitsu		
154222	DRM0201273	thickness = 7 um. Carrier density (n) estimated from Tc vs n curve	B-doped diamond	C1	C	1																							2011																												diamond																		K			5				5																				T	RES(on)	3.4							T/K	RES(on)	1.12					A		80																																																						n/cm3	5000000000000000000000			High-oriented diamond films with ajimuthally aligned [100] surface by MPCVD. then pyramidal surface and B-doped diamond films. d = 7 um.					Superconductivity in heavily B-doped diamond layers deposited on highly oriented diamond films			Aoyama-Gakuin University	Diamond Relat.Mater., 20(2011)1273	T. Nuranaka,K. Kobashi,H. Okabe,T. Tachibana,Y. Yokota,K. Hayashi,N. Mawakami,J. Akimitsu		
154223	EPL08357001	Energy gaps measured by Knight shift using <75>As NMR. Two gap fitting with nodes: higher gap in DB, lower one is 1.1 kTc with weight of 0.6	Pr(O,F)FeAs	Pr1Fe1As1F0.11O0.89	Pr	1	Fe	1	As	1	F	0.11													O	0.89		1	2008																										ABCD		oxypnictide	P4/nmm																Fe-1111, ZrCuSiAs-type	K				45			45																																																3.5	6																																													PrAs,Fe,Fe2O3,FeF3		high pressure synthesis. mixture - grind - pellet - SIN(1250C,2h, P=6 GPa)					Spin-singlet superconductivity with multiple gaps in PrFeAsO0.89F0.11			Department of Physics, Okayama University - Okayama 700-8530, Japan	EuroPhys.Lett., 83(2008)57001	K. Matano,Z. A. Ren,X. L. Dong,L. L. Sun,Z. X. Zhao,Guo-qing Zheng		
154224	IMET0380088	not SC down to 300 mK. R measured for 0.3 < T < 300 K.	Ni2Zn11	Ni2Zn11	Ni	2	Zn	11																				3	2013												GPa		141	GPa		56.4	GPa		94		0.25				A2B11		Cu5Zn8	I4[-]3m		A	8.911													gamma-brass type	K					0.3																																																										mJ/mol.K2	4	SP													uOhm.cm							11																Zn(granules),Ni(powder)		mixture(14 at.%Ni) - compact in steel dia in quartz tube - heat to 870C - cool to 800C and keep for 4 days - water quench					Physical properties of non-centrosymmetric Ni2Zn11			Institute of Physical Chemistry, University of Vienna, Wahringerstrasse 42, A-1090 Vienna, Austria	Intermetallics, 38(2013)88	Z. Malik,F. Kneidinger,H. Michor,S. Puchegger,E. Bauer,G. Giester,P. Rogl		
154225	JAC5630261	Young's modulus by sound resonance method. Fracture toughness = 0.57 MPa.m^0.5.	La(O,F)(Fe,Zn)As	La1Fe1As1F0.15O0.85	La	1	Fe	1	As	1	F	0.15													O	0.85			2013										GPa	0.306	GPa		19.6												ABCD		oxypnictide	P4/nmm																Fe-1111, ZrCuSiAs-type	K			26.2				26.2																																																																																														LaAs,Fe2O3,FeF2,Zn,Fe		mixture - press(250 MPa) to bar - wrapped in Ta-foil - sealed in silica tube(Ar) - heat (1150C,50h)					Superconductivity and mechanical properties for LaFe1-xZnxAsO0.85F0.15			School of Materials Science and Engineering, Beihang University, Beijing 100191, China	J.Alloys & Compounds., 563(2013)261	Yanling Pei,David Berardan,Nita Dragoe,Celine Barreteau,Jiehe Sui,Li-Dong Zhao		
154226	JAC5630261	Young's modulus by sound resonance method. Fracture toughness = 0.625 MPa.m^0.5.	La(O,F)(Fe,Zn)As	La1Fe0.8Zn0.2As1F0.15O0.85	La	1	Fe	0.8	Zn	0.2	As	1	F	0.15											O	0.85			2013										GPa	0.345	GPa		22.5												ABCD		oxypnictide	P4/nmm																Fe-1111, ZrCuSiAs-type	K			25.5				25.5																																																																																														LaAs,Fe2O3,FeF2,Zn,Fe		mixture - press(250 MPa) to bar - wrapped in Ta-foil - sealed in silica tube(Ar) - heat (1150C,50h)					Superconductivity and mechanical properties for LaFe1-xZnxAsO0.85F0.15			School of Materials Science and Engineering, Beihang University, Beijing 100191, China	J.Alloys & Compounds., 563(2013)261	Yanling Pei,David Berardan,Nita Dragoe,Celine Barreteau,Jiehe Sui,Li-Dong Zhao		
154227	JAC5630261	Young's modulus by sound resonance method. Fracture toughness = 0.693 MPa.m^0.5.	La(O,F)(Fe,Zn)As	La1Fe0.4Zn0.6As1F0.15O0.85	La	1	Fe	0.4	Zn	0.6	As	1	F	0.15											O	0.85			2013										GPa	0.395	GPa		25.7												ABCD		oxypnictide	P4/nmm																Fe-1111, ZrCuSiAs-type	K			24.6				24.6																																																																																														LaAs,Fe2O3,FeF2,Zn,Fe		mixture - press(250 MPa) to bar - wrapped in Ta-foil - sealed in silica tube(Ar) - heat (1150C,50h)					Superconductivity and mechanical properties for LaFe1-xZnxAsO0.85F0.15			School of Materials Science and Engineering, Beihang University, Beijing 100191, China	J.Alloys & Compounds., 563(2013)261	Yanling Pei,David Berardan,Nita Dragoe,Celine Barreteau,Jiehe Sui,Li-Dong Zhao		
154228	JAC5630261	Young's modulus by sound resonance method. Fracture toughness = 0.699 MPa.m^0.5.	La(O,F)(Fe,Zn)As	La1Fe0.2Zn0.8As1F0.15O0.85	La	1	Fe	0.2	Zn	0.8	As	1	F	0.15											O	0.85			2013										GPa	0.42	GPa		26.7												ABCD		oxypnictide	P4/nmm																Fe-1111, ZrCuSiAs-type	K			23.9				23.9																																																																																														LaAs,Fe2O3,FeF2,Zn,Fe		mixture - press(250 MPa) to bar - wrapped in Ta-foil - sealed in silica tube(Ar) - heat (1150C,50h)					Superconductivity and mechanical properties for LaFe1-xZnxAsO0.85F0.15			School of Materials Science and Engineering, Beihang University, Beijing 100191, China	J.Alloys & Compounds., 563(2013)261	Yanling Pei,David Berardan,Nita Dragoe,Celine Barreteau,Jiehe Sui,Li-Dong Zhao		
154229	JAC5880418	multi-phases: beta(SC) = 27.80%, Fe7Se8=61.41%.	FeSe0.93	Fe1Se0.93	Fe	1	Se	0.93																				2	2014																										AB					A	3.772		5.522											Fe-11	K	4.5		9.5				7																																																																																														Fe(4N),Se(4N),Sn(3N)		solid state reaction.mixture(Fe+Se) - SIN(650C,24h) - ANN - mixed with Sn - mixture - press - SIN(600C,5h)					Influence of Sn doping on the phase formation and superconductivity of FeSe0.93			Tianjin Key Laboratory of Composite and Functional Materials, School of Materials Science & Engineering, Tianjin University, Tianjin 300072, People's Republic of China	J.Alloys & Compounds., 588(2014)418	Ning Chen,Zongqing Ma,Yongchang Liu,Xiaoting Li,Qi Cai,Huijun Li,Liming Yu		
154230	JAC5880418	Sn-doped(5wt%)-FeSe0.93. multi-phases: beta(SC) = 47.30%, Fe7Se8=33.27%. Sn-content in DB is tentative value.	Sn-doped FeSe0.93	Sn0.05Fe1Se0.93	Sn	0.05	Fe	1	Se	0.93																		2	2014																										AB																			Fe-11	K	4.5		9.5				7																																																																																														Fe(4N),Se(4N),Sn(3N)		solid state reaction.mixture(Fe+Se) - SIN(650C,24h) - ANN - mixed with Sn - mixture - press - SIN(600C,5h)					Influence of Sn doping on the phase formation and superconductivity of FeSe0.93			Tianjin Key Laboratory of Composite and Functional Materials, School of Materials Science & Engineering, Tianjin University, Tianjin 300072, People's Republic of China	J.Alloys & Compounds., 588(2014)418	Ning Chen,Zongqing Ma,Yongchang Liu,Xiaoting Li,Qi Cai,Huijun Li,Liming Yu		
154231	JAC5880418	Sn-doped(10wt%)-FeSe0.93. multi-phases: beta(SC) = 53.26%, Fe7Se8=25.02%. Sn-content in DB is tentative value.	Sn-doped FeSe0.93	Sn0.1Fe1Se0.93	Sn	0.1	Fe	1	Se	0.93																		2	2014																										AB																			Fe-11	K	4.5		9.5				7																																																																																														Fe(4N),Se(4N),Sn(3N)		solid state reaction.mixture(Fe+Se) - SIN(650C,24h) - ANN - mixed with Sn - mixture - press - SIN(600C,5h)					Influence of Sn doping on the phase formation and superconductivity of FeSe0.93			Tianjin Key Laboratory of Composite and Functional Materials, School of Materials Science & Engineering, Tianjin University, Tianjin 300072, People's Republic of China	J.Alloys & Compounds., 588(2014)418	Ning Chen,Zongqing Ma,Yongchang Liu,Xiaoting Li,Qi Cai,Huijun Li,Liming Yu		
154232	CEM1980445	sample obtained by thermal decomposition from CaAl2Si2 at high-T-high-P condition	Ca2Al3Si4	Ca2Al3Si4	Ca	2	Al	3	Si	4																		1	2013																										A2B3C4			Cmc2	36	A	5.8605	15.036	7.7659												K				6.2			6.2																																																																																																Zintl compound CaAl2Si2 is peritectically decomposed to a mixture of Ca2Al3Si4 and Al at T > 600C, under P=5 GPa.					High pressure synthesis and crystal structure of a ternary superconductor  Ca2Al3Si4  containing layer structured calcium sub-network isomorphous with black phosphorus			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527,Japan	J.Solid State Chem., 198(2013)445	Masashi Tanaka,Shuai Zhang,Yuki Tanaka,Kei Inumaru,Shoji Yamanaka		
154233	CEM1980445	sample obtained by thermal decomposition from CaAl2Si2 at high-T-high-P condition	Ca2Al3-xSi4+x	Ca2Al2.73Si4.27	Ca	2	Al	2.73	Si	4.27																		3	2013																										A2B3C4			Cmc2	36	A	5.8846	14.973	7.7966												K				6.4			6.4										22																																																																																						Zintl compound CaAl2Si2 is peritectically decomposed to a mixture of Ca2Al3Si4 and Al at T > 600C, under P=5 GPa.					High pressure synthesis and crystal structure of a ternary superconductor  Ca2Al3Si4  containing layer structured calcium sub-network isomorphous with black phosphorus			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527,Japan	J.Solid State Chem., 198(2013)445	Masashi Tanaka,Shuai Zhang,Yuki Tanaka,Kei Inumaru,Shoji Yamanaka		
154234	CEM1980445	sample obtained by thermal decomposition from CaAl2Si2 at high-T-high-P condition	Ca2Al3-xSi4+x	Ca2Al2.39Si4.61	Ca	2	Al	2.39	Si	4.61																		2	2013																										A2B3C4			Cmc2	36																K				5.4			5.4										80																																																																																						High pressure synthesis (1200C, P = 13 GPa)					High pressure synthesis and crystal structure of a ternary superconductor  Ca2Al3Si4  containing layer structured calcium sub-network isomorphous with black phosphorus			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527,Japan	J.Solid State Chem., 198(2013)445	Masashi Tanaka,Shuai Zhang,Yuki Tanaka,Kei Inumaru,Shoji Yamanaka		
154235	PHB4120119		Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4			2013																										A3B4C4			I4/mmm		A	3.9754		41.4286												K	4.16		4.85	4.11			4.11																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154236	PHB4120119	impurity phase: Bi, Bi2O3	Bi4-xCuxO4S3	Bi3.99Cu0.01S3O4	Bi	3.99	Cu	0.01	S	3															O	4			2013																										A3B4C4			I4/mmm		A	3.975		41.4082												K	3.93		4.51	3.94			3.94	MTC154236																																																																																													Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154237	PHB4120119	impurity phase: Bi, Bi2O3	Bi4-xCuxO4S3	Bi3.975Cu0.025S3O4	Bi	3.975	Cu	0.025	S	3															O	4			2013																										A3B4C4			I4/mmm		A	3.9688		41.401												K	3.11		3.92	2.99			2.99																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154238	PHB4120119	impurity phase: Bi, Bi2O3	Bi4-xCuxO4S3	Bi3.95Cu0.05S3O4	Bi	3.95	Cu	0.05	S	3															O	4			2013																										A3B4C4			I4/mmm		A	3.9669		41.3847												K	2.69		3.52	2.6			2.6																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154239	PHB4120119	impurity phase: Bi, Bi2O3	Bi4-xCuxO4S3	Bi3.9Cu0.1S3O4	Bi	3.9	Cu	0.1	S	3															O	4			2013																										A3B4C4			I4/mmm		A	3.9655		41.3959												K			3				3																																																																																														Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154240	PHB4120119	impurity phase: Bi, Bi2O3	Bi4-xCuxO4S3	Bi3.85Cu0.15S3O4	Bi	3.85	Cu	0.15	S	3															O	4			2013																										A3B4C4			I4/mmm		A	3.9577		41.4184												K					1.5																																																																																																Cu(4N),Bi(5N),S(3N),Bi2O3(3N)		mixture - pellet - sealed in evacuated silica tube - heat(450C,10h + 510C,10h)					The effects o fCu doping on the physical properties of the new layered  superconductor Bi4-xCuxO4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica B, 412(2013)119	Y. Liu,P.Tong,S.G.Tan,W.J.Lu,L.J.Li,B.C.Zhao,S.B.Zhang,Y.P.Sun		
154241	JAC5830151	Tc = 1.38K from SP. (dC/Tc) = 9.13 mJ/mol.K2.  (dC/gamma*Tc) = 1.325. lattice term in SP (beta) = 1.266 mJ/mol.K4. e-ph = 0.496. Hc2(0) = 0.86 T from linear approx.	LaPd2Sb2	La1Pd2Sb2	La	1	Pd	2	Sb	2																		1	2014																										AB2C2		CaBe2Ge2	P4/nmm		A	4.568		10.266											M-122	K	1.2		1.4				1.3										90										T	RES(R=0.5Rn). WHH	0.58							T/K	RES(R=0.5Rn).	0.6			MHC154241		A	from Hc2	233																		mJ/mol.K2	6.89	SP	210	SP																																		La(3N),Sb(3N),Pd(3N)		mixture - pellet - heat(900C,40h) - Q - reground - pellet - heat(900C,40h) - Q to RT					LaPd2Sb2: A pnictide superconductor with CaBe2Ge2 type structure			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Alloys & Compounds., 583(2014)151	Subodh Ganesanpotti,Takeshi Yajima,Takami Tohyama,Zhi Li,Kousuke Nakano,Yasumasa Nozaki,Cedric Tassel,Yoji Kobayashi,Hiroshi Kageyama		
154242	PHC4920165	not SC	EuSr2NbCu2O8-x	Eu1Sr2Nb1Cu2O8-z	Eu	1	Sr	2	Nb	1	Cu	2													O	8-z		1	2013																												M1212			A	3.874		11.631												K					2																																																																																																Eu2O3,SrCO3,CuO,Nb,Nb2O5,SnO2		mixture - CAL(1000C,12h,in air) -reground - pellet - SIN(1010C,24h,in air) - FC to RT					New superconductor EuSr2Cu2(Nb,Sn)O8-y with the RE-123 type structure			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physica C, 492(2013)165	Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154243	PHC4920165	R(T) is semiconductor-like for T < 200K.	EuSr2(Nb,Sn)Cu2O8-x	Eu1Sr2Nb0.8Sn0.2Cu2O8-z	Eu	1	Sr	2	Nb	0.8	Sn	0.2	Cu	2											O	8-z		1	2013																												M1212			A	3.874		11.663												K			40	40			40																																																																																														Eu2O3,SrCO3,CuO,Nb,Nb2O5,SnO2		mixture - CAL(1000C,12h,in air) -reground - pellet - SIN(1010C,24h,in air) - FC to RT					New superconductor EuSr2Cu2(Nb,Sn)O8-y with the RE-123 type structure			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physica C, 492(2013)165	Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154244	PHC4930075	P-induced SC. P<crit> = 8.5 GPa. Topological compound. Structural transition at P=9.8 GPa at RT.	Cu0.14Bi2Te3	Cu0.14Bi2Te3	Cu	0.14	Bi	2	Te	3																		3	2013																													R-3m		A	4.385		30.48											rhombohedral	K			6		0		6																																																																																														Bi(5N),Te(5N),Cu(4N)		single crystals were prepared by Bridgman method.					Superconductivity in copper intercalated topological compound  CuxBi2Te3 induced via high pressure			Institute of Physics, Chinese Academy of Sciences, Beijing, China	Physica C, 493(2013)75	J.L. Zhang,S.J. Zhang,P.P. Kong,J. Zhu,X.D. Li,J. Liu,L.Z. Cao,C.Q. Jin		
154245	PHC4930093	Major phase SrPt2Ge2 (not SC): SG=P2<1>, a=4.401, b=4.435, c=9.764 A, beta= 90.5degree. Minor phase SrPt2Ge2 shows SC.	SrPt2Ge2	Sr1Pt2Ge2	Sr	1	Pt	2	Ge	2																		2	2013																										AB2C2			I4/mmm		A	4.4		9.8											unstable	K				10.2			10.2																																																																																																PtGe firstly arc-melted. then, melted with Sr and extra-Sr for stoichiometly. Wrapped in Ta-foil - ANN(1000-1200C,5d) - rapid quench					New superconductor SrPt2Ge2 with Tc = 10.2 K			Department of Physics, National Tsing Hua University, Hsinchu 30013, Taiwan, ROC	Physica C, 493(2013)93	H.C. Ku,I.A. Chen,C.H. Huang,C.W. Chen,Y.B. You,M.F. Tai,Y.Y. Hsu		
154246	PHC4940057	R(60K) = 2.13  mOhm.cm	Sm(O,F)FeAs	Sm1Fe1As1F0.12O0.88	Sm	1	Fe	1	As	1	F	0.12													O	0.88		1	2013																										ABCD		oxypnictide			A	3.9307		8.4786											Fe-1111, ZrCuSiAs-type	K			50.1				50.1																																		HC154246																																uV/K	-33.6			TP154246																								SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154247	PHC4940057	R(60K) = 2.78  mOhm.cm	Sm(O,F)(Fe,Mn)As	Sm1Fe0.99Mn0.01As1F0.12O0.88	Sm	1	Fe	0.99	Mn	0.01	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9347		8.4912											Fe-1111, ZrCuSiAs-type	K			37.2				37.2																																		HC154246																																																												SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154248	PHC4940057	R(60K) = 4.41  mOhm.cm	Sm(O,F)(Fe,Mn)As	Sm1Fe0.97Mn0.03As1F0.12O0.88	Sm	1	Fe	0.97	Mn	0.03	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9373		8.4951											Fe-1111, ZrCuSiAs-type	K			31.3				31.3																																		HC154248																																uV/K	-19.4			TP154248																								SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154249	PHC4940057	R(60K) = 7.10  mOhm.cm	Sm(O,F)(Fe,Mn)As	Sm1Fe0.94Mn0.06As1F0.12O0.88	Sm	1	Fe	0.94	Mn	0.06	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9407		8.5005											Fe-1111, ZrCuSiAs-type	K			16				16																																		HC154248																																																												SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154250	PHC4940057	R(60K) = 11.27  mOhm.cm	Sm(O,F)(Fe,Mn)As	Sm1Fe0.92Mn0.08As1F0.12O0.88	Sm	1	Fe	0.92	Mn	0.08	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9429		8.5121											Fe-1111, ZrCuSiAs-type	K			0				0																																																																																														SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154251	PHC4940057	R(60K) = 23.38  mOhm.cm	Sm(O,F)(Fe,Mn)As	Sm1Fe0.9Mn0.1As1F0.12O0.88	Sm	1	Fe	0.9	Mn	0.1	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9458		8.5208											Fe-1111, ZrCuSiAs-type	K			0				0																																																																																														SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154254	PHC4940057	R(60K) = 2.18  mOhm.cm	Sm(O,F)(Fe,Ni)As	Sm1Fe0.99Ni0.01As1F0.12O0.88	Sm	1	Fe	0.99	Ni	0.01	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9323		8.4753												K			45.7				45.7																																		HC154255																																																												SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154255	PHC4940057	R(60K) =  2.27 mOhm.cm	Sm(O,F)(Fe,Ni)As	Sm1Fe0.97Ni0.03As1F0.12O0.88	Sm	1	Fe	0.97	Ni	0.03	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9361		8.4699												K			34.5				34.5																																		HC154255																																uV/K	-36.1			TP154255																								SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154256	PHC4940057	R(60K) =  2.78 mOhm.cm	Sm(O,F)(Fe,Ni)As	Sm1Fe0.94Ni0.06As1F0.12O0.88	Sm	1	Fe	0.94	Ni	0.06	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9391		8.4685												K			18.8				18.8																																		HC154255																																																												SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154257	PHC4940057	R(60K) =  2.69 mOhm.cm	Sm(O,F)(Fe,Ni)As	Sm1Fe0.9Ni0.1As1F0.12O0.88	Sm	1	Fe	0.9	Ni	0.1	As	1	F	0.12											O	0.88		1	2013																										ABCD		oxypnictide			A	3.9404		8.4622												K			5.6				5.6																																																																																														SmAs,Fe2O3,FeF2,Fe,Ma(or Ni)		mixture - pellet(40 MPa) - wrapped in Ta-foil - heat(900C,45h, in evacuated quartz ampoules)					Effects of Mn and Ni doping on the superconductivity of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)57	S.J. Singh,J. Shimoyama,A. Yamamoto,H. Ogino,K. Kishio		
154258	PHC4940065	RRR=1.65. Jc(2K) = 3E+5 A/cm2. Proton irradiation effect  were investigated, Anisotropy(Hc2) = 10. R(T) has minimum at 80 K.	Ca10(Pt3As8)(Fe1.79Pt0.21As2)5	Ca10Pt4.05Fe8.95As18	Ca	10	Pt	4.05	Fe	8.95	As	18																3	2013																																													Ca-10-3-8 phase	K				13			13																				T	RES(R=0.9Rn). WHH		65.1	15.3										MHC154258																																					uOhm.cm								300															Cu(99.5),Pt(3N),As(7N),FeAs		mixture - heat(700C,6h) - react(1065C,10h) - alumina crucible - sealed in quartz tube - heat(1100C,72h) - cool to 1050C(1C/h) - FC to RT					Superconducting properties of iron-platinum-arsenides Ca10(PtnAs8)(Fe2-xPtxAs2)5 (n = 3, 4)			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)65	T. Tamegai,Q.P. Ding,T. Taen,F. Ohtake,H. Inoue,Y. Tsuchiya,S. Mohan,Y. Sun,Y. Nakajima,S. Pyon,H. Kitamura		
154259	PHC4940065	RRR=2.15. Jc(2K) = 3E+5 A/cm2. Proton irradiation effect  were investigated, Anisotropy(Hc2) = 10.	Ca10(Pt4As8)(Fe1.96Pt0.04As2)5	Ca10Pt4.2Fe9.8As18	Ca	10	Pt	4.2	Fe	9.8	As	18																3	2013																																													Ca-10-4-8 phase	K				30			30																				T	RES(R=0.9Rn). WHH		115.4	33.9										MHC154259																																					uOhm.cm								100															Cu(99.5),Pt(3N),As(7N),FeAs		mixture - heat(700C,6h) - react(1065C,10h) - alumina crucible - sealed in quartz tube - heat(1000C,72h) - cool to 800C(3C/h) - FC to RT					Superconducting properties of iron-platinum-arsenides Ca10(PtnAs8)(Fe2-xPtxAs2)5 (n = 3, 4)			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physica C, 494(2013)65	T. Tamegai,Q.P. Ding,T. Taen,F. Ohtake,H. Inoue,Y. Tsuchiya,S. Mohan,Y. Sun,Y. Nakajima,S. Pyon,H. Kitamura		
154260	PHC4940077	impurity phase: Lu2O3,LuCx. Hc1(T), Hc2(T) have GL-type T-dependency. Hc(0) = 704 Oe. kappa(GL) = 9.2	Lu2SnC	Lu2Sn1C1	Lu	2	Sn	1	C	1																		1	2013																										ABC2	7	Cr2AlC	P6<3>/mmc		A	3.51		15.15											M2AX phase, hexagonal	K				5.2			5.2											Oe	M-H curve, GL	110							T	SUS(on), Hc2(T) by GL	0.45												MHC154260		A	from Hc2	270			A	from Hc1	2500																																																					arc-melting - ANN(1100C,several days)					Superconductivity in Lu2SnC			Department of Physics and Mathematics, Aoyama-Gakuin University, 5-10-1 Fuchinobe, Sagamihara, Kanagawa 252-5258, Japan	Physica C, 494(2013)77	S. Kuchida,T. Muranaka,K. Kawashima,K. Inoue,M. Yoshikawa,J. Akimitsu		
154261	PHC4940095	BCS coherence qsi-0 = 116 A. mean free pass = 637 A from residual -R ( = 8.32 uOhm.cm).	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																			2013																										AB2C3			P4<3>32																	K		8.29					8.29																				T	RES(R=0.5Rn)													MHC154262		A		110																																	uOhm.cm								8.32															Pd(3N),B(99.5),Li(3N)		Firstly Pd3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154262	PHC4940095	Al-doped Li2Pd3B. mean free pass = 83 A from residual -R ( = 64.6 uOhm.cm).	Li2Pd3(B,Al)	Li2Pd3B0.95Al0.05	Li	2	Pd	3	B	0.95	Al	0.05																	2013																										AB2C3			P4<3>32																	K		7.75					7.75																				T	RES(R=0.5Rn)													MHC154262		A		82																																	uOhm.cm								64.6															Pd(3N),B(99.5),Li(3N)		Firstly Pd3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154263	PHC4940095	Al-doped Li2Pd3B. mean free pass = 76 A from residual -R ( = 71.5 uOhm.cm).	Li2Pd3(B,Al)	Li2Pd3B0.9Al0.1	Li	2	Pd	3	B	0.9	Al	0.1																	2013																										AB2C3			P4<3>32																	K		7.49					7.49																				T	RES(R=0.5Rn)													MHC154262		A		77																																	uOhm.cm								71.5															Pd(3N),B(99.5),Li(3N)		Firstly Pd3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154264	PHC4940095	mean free pass = 491 A from residual -R ( = 30.2 uOhm.cm).	Li2Pt3B	Li2Pt3B1	Li	2	Pt	3	B	1																			2013																										AB2C3			P4<3>32																	K		3.19					3.19																				T	RES(R=0.5Rn)													MHC154265		A		135																																	uOhm.cm								30.2															Pt(3N),B(99.5),Li(3N)		Firstly Pt3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154265	PHC4940095	Al-doped Li2Pt3B.  mean free pass = 129 A from residual -R ( = 116 uOhm.cm).	Li2Pt3(B,Al)	Li2Pt3B0.99Al0.01	Li	2	Pt	3	B	0.99	Al	0.01																	2013																										AB2C3			P4<3>32																	K		2.86					2.86																				T	RES(R=0.5Rn)													MHC154265		A		142																																	uOhm.cm								116															Pt(3N),B(99.5),Li(3N)		Firstly Pt3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154266	PHC4940095	Al-doped Li2Pt3B.  mean free pass = 91 A from residual -R ( = 166 uOhm.cm).	Li2Pt3(B,Al)	Li2Pt3B0.95Al0.05	Li	2	Pt	3	B	0.95	Al	0.05																	2013																										AB2C3			P4<3>32																	K		2.12					2.12																				T	RES(R=0.5Rn)													MHC154265		A		166																																	uOhm.cm								166															Pt(3N),B(99.5),Li(3N)		Firstly Pt3B was synthesized by arc-melting, then arc-melted with 10% excess Li and Al.					Influence on superconductivity in the parity mixing superconductor Li2T3B(T:Pt,Pd) by non-magnetic impurity and defect doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	Physica C, 494(2013)95	G. Bao,Y. Inada,G. Eguchi,Y. Maeno,M. Ichioka,G.-q. Zheng		
154267	PHC4940080	Trigonal to monoclinic phase transition at 219K(heating) , 205K(cooling)	Ir1-xPtxTe2	Ir0.98Pt0.02Te2	Ir	0.98	Pt	0.02	Te	2																		3	2013																										AB2	6		P3[-]ml																trigonal	K					1.8																																																																																																		self-flux method. mixture(Ir:Pt:Te=0.18(1-x):0.18x:0.82) - alumina crucible - quartz tube - heat(950C,10h) - slow cool to 1160C - cool to 900C( (1 C/h) - Q to ice					Emergence of superconductivity near the structural phase boundary in Pt-doped IrTe2 single crystals			Department of Physics, Okayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan	Physica C, 494(2013)80	Sunseng Pyon,Kazutaka Kudo,Minoru Nohara		
154268	PHC4940080	Trigonal to monoclinic phase transition at 145K(heating) , 91K(cooling)	Ir1-xPtxTe2	Ir0.96Pt0.04Te2	Ir	0.96	Pt	0.04	Te	2																		3	2013																										AB2	6		P3[-]ml																trigonal	K				3			3	MTC154268																																																																																															self-flux method. mixture(Ir:Pt:Te=0.18(1-x):0.18x:0.82) - alumina crucible - quartz tube - heat(950C,10h) - slow cool to 1160C - cool to 900C( (1 C/h) - Q to ice					Emergence of superconductivity near the structural phase boundary in Pt-doped IrTe2 single crystals			Department of Physics, Okayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan	Physica C, 494(2013)80	Sunseng Pyon,Kazutaka Kudo,Minoru Nohara		
154269	PHC4940080		Ir1-xPtxTe2	Ir0.92Pt0.08Te2	Ir	0.92	Pt	0.08	Te	2																		3	2013																										AB2	6		P3[-]ml																trigonal	K				2.49			2.49																																																																																																self-flux method. mixture(Ir:Pt:Te=0.18(1-x):0.18x:0.82) - alumina crucible - quartz tube - heat(950C,10h) - slow cool to 1160C - cool to 900C( (1 C/h) - Q to ice					Emergence of superconductivity near the structural phase boundary in Pt-doped IrTe2 single crystals			Department of Physics, Okayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan	Physica C, 494(2013)80	Sunseng Pyon,Kazutaka Kudo,Minoru Nohara		
154270	PHC4940080		Ir1-xPtxTe2	Ir0.88Pt0.12Te2	Ir	0.88	Pt	0.12	Te	2																		3	2013																										AB2	6		P3[-]ml																trigonal	K				1.92			1.92																																																																																																self-flux method. mixture(Ir:Pt:Te=0.18(1-x):0.18x:0.82) - alumina crucible - quartz tube - heat(950C,10h) - slow cool to 1160C - cool to 900C( (1 C/h) - Q to ice					Emergence of superconductivity near the structural phase boundary in Pt-doped IrTe2 single crystals			Department of Physics, Okayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan	Physica C, 494(2013)80	Sunseng Pyon,Kazutaka Kudo,Minoru Nohara		
154271	PHC4940109	[penet] measured by surface impedance (f = 19 GHz)	Na(Fe,Co)As	Na1Fe0.97Co0.03As1	Na	1	Fe	0.97	Co	0.03	As	1																3	2013																										ABC																			Fe-111	K				22			22																				T	RES(R=0.9Rn and calc from Rn, viscous drag coeff.													MHC154271							A	surface impedance, f=19 GHz		3750																																																				self-flux method. mixture(Na:Fe:Co:As=2:0.95:0.05:2) - alumina crucible - qurtz tube - heat(950C) - slow cool (from 900 to 400 C, in 100h) - cool to RT in a day					Magnetic penetration depth and flux-flow resistivity measurements on NaFe0.97Co0.03As single crystals			Department of Basic Science, The University of Tokyo, Meguro, Tokyo 153-8902, Japan	Physica C, 494(2013)109	T. Okada,H. Takahashi,Y. Imai,K. Kitagawa,K. Matsubayashi,Y. Uwatoko,A. Maeda		
154272	PHC4950010		Zr2Co	Zr2Co1	Zr	2	Co	1																				1	2013																										AB2	2	CuAl2	I4/mcm		A	6.354		5.512											tetragonal	K		5.47	6.2	5.58			5.47																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154273	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.95Cu0.05	Zr	2	Co	0.95	Cu	0.05																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.371		5.483											tetragonal	K		6.52	6.69	6.01			6.52	MTC154273																																																																																													Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154274	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.9Cu0.1	Zr	2	Co	0.9	Cu	0.1																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.389		5.463											tetragonal	K		6.07	6.6	5.8			6.07																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154275	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.85Cu0.15	Zr	2	Co	0.85	Cu	0.15																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.407		5.443											tetragonal	K		5.88	6.4	5.69			5.88																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154276	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.8Cu0.2	Zr	2	Co	0.8	Cu	0.2																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.416		5.421											tetragonal	K		5.41	5.7	5.29			5.41																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154277	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.75Cu0.25	Zr	2	Co	0.75	Cu	0.25																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.428		5.402											tetragonal	K		4.89	5.3	4.79			4.89																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154278	PHC4950010		Zr2(Co1-xCux)	Zr2Co0.7Cu0.3	Zr	2	Co	0.7	Cu	0.3																		1	2013																										AB2	2	CuAl2	I4/mcm		A	6.452		5.386											tetragonal	K		4.39	4.89	4.49			4.39																																																																																														Zr(99.95),Co(3N),Cu(6N)		arc-melting - ANN(820C,5d, in quartz tube) - Q to RT					Superconductivity in Zr2(Co1-xCux)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 495(2013)10	K.J. Syu,S.C. Chen,H.H. Wu,H.H. Sung,W.H. Lee		
154279	PHC4980014	splat-cooled sample. alpha-(ortho) + gamma(bcc) phase. Hc2(0) = 0.3 T by using T^2 approx.	U	U1	U	1																							2014									18.06																	A																			alpha- & gamma-phase	K		1.24					1.24																				T	RES(R=0.5Rn), WHH	0.3							T/K	RES(R=0.5Rn)	0.35			MHC154280																						mJ/mol.K2	11	SP	179	SP											uOhm.cm								53																	(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154280	PHC4980014	splat-cooled sample. alpha-(ortho) + gamma(bcc) phase.	U1-xMox	U0.97Mo0.03	U	0.97	Mo	0.03																					2014																										A																			alpha- & gamma-phase	K		0.65					0.65																																																																																																(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154281	PHC4980014	splat-cooled sample. alpha-(ortho) + gamma(bcc) phase.	U1-xMox	U0.94Mo0.06	U	0.94	Mo	0.06																					2014																										A																			alpha- & gamma-phase	K		0.7					0.7																				T	RES(R=0.5Rn), WHH	1.3							T/K	RES(R=0.5Rn)	2.6			MHC154280																																																														(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154282	PHC4980014	splat-cooled sample. gamma(bcc) phase.	U1-xMox	U0.89Mo0.11	U	0.89	Mo	0.11																					2014																										A	2				A	3.4841		3.4041											gamma-phase	K		1.25					1.25																				T	RES(R=0.5Rn), WHH	3.3							T/K	RES(R=0.5Rn)	3.8			MHC154284																						mJ/mol.K2	13	SP	147	SP											uOhm.cm								105																	(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154283	PHC4980014	splat-cooled sample. gamma(bcc) phase. Hc2(0) = 6.0 T by using T^2 approx.	U1-xMox	U0.88Mo0.12	U	0.88	Mo	0.12																					2014																										A	2				A	3.4451		3.3966											gamma-phase	K		1.91					1.91																				T	RES(R=0.5Rn), WHH	5.2							T/K	RES(R=0.5Rn)	3.9			MHC154284																						mJ/mol.K2	15.8	SP	139	SP											uOhm.cm								80																	(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154284	PHC4980014	splat-cooled sample. gamma(bcc) phase. Hc2(0) = 6.7 T by using T^2 approx.	U1-xMox	U0.85Mo0.15	U	0.85	Mo	0.15																					2014																										A	2				A	3.4409		3.4409											gamma-phase	K		2.11					2.11																				T	RES(R=0.5Rn), WHH	5.3							T/K	RES(R=0.5Rn)	3.6			MHC154284																						mJ/mol.K2	16	SP	139	SP											uOhm.cm								89																	(natural-U + Mo) - arc melting - splatcooling on Cu (cooling rate = 1 E+6 K/s) to irregular disc( dia = 20mm, d = 1-2 mm)					Electronic properties of gamma-U and superconductivity of U-Mo alloys			Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 12116 Prague, Czech Republic	Physica C, 498(2014)14	I. Tkach,N.-T.H. Kim-Ngan,A. Warren,T. Scott,A.P. Goncalves,L. Havela		
154285	PHC4980045	impurity phases: Bi, Bi2S3	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2014																											2		I4/mmm		A	3.9708		41.357												K			4.5	4.4			4.4																				T	RES(R=0.9Rn), WHH	2.3												MHC154285																																																														solid state reaction. mixture - pellet - sealed in quartz ampoule - heat to 400C (2C/min) - keep(400C,10h) - slow cool to RT within 6h					Effect of Se doping in recently discovered layered Bi4O4S3 superconductor			CSIR-National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Physica C, 498(2014)45	Rajveer Jha,V.P.S. Awana		
154286	PHC4980045		Bi4O4(S,Se)3	Bi4S2.97Se0.03O4	Bi	4	S	2.97	Se	0.03															O	4		1	2014																											2		I4/mmm																	K				4.2			4.2																				T	RES(R=0.9Rn), WHH	2.1												MHC154286																																																														solid state reaction. mixture - pellet - sealed in quartz ampoule - heat to 400C (2C/min) - keep(400C,10h) - slow cool to RT within 6h					Effect of Se doping in recently discovered layered Bi4O4S3 superconductor			CSIR-National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Physica C, 498(2014)45	Rajveer Jha,V.P.S. Awana		
154287	PHC4980045		Bi4O4(S,Se)3	Bi4S2.91Se0.09O4	Bi	4	S	2.91	Se	0.09															O	4		1	2014																											2		I4/mmm																	K				3.7			3.7																																																																																																solid state reaction. mixture - pellet - sealed in quartz ampoule - heat to 400C (2C/min) - keep(400C,10h) - slow cool to RT within 6h					Effect of Se doping in recently discovered layered Bi4O4S3 superconductor			CSIR-National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Physica C, 498(2014)45	Rajveer Jha,V.P.S. Awana		
154288	PHC4980045		Bi4O4(S,Se)3	Bi4S2.85Se0.15O4	Bi	4	S	2.85	Se	0.15															O	4		1	2014																											2		I4/mmm		A	3.9717		41.419												K			4	3.5			3.5																				T	RES(R=0.9Rn), WHH	1.8												MHC154288																																																														solid state reaction. mixture - pellet - sealed in quartz ampoule - heat to 400C (2C/min) - keep(400C,10h) - slow cool to RT within 6h					Effect of Se doping in recently discovered layered Bi4O4S3 superconductor			CSIR-National Physical Laboratory (CSIR), Dr. K.S. Krishnan Road, New Delhi 110012, India	Physica C, 498(2014)45	Rajveer Jha,V.P.S. Awana		
154289	PHC4980050	RRR = 6.98. Hall coeffic. RH(25K) = 0.85 E-8 m3/C.	(Pr,Sr)Fe(As,Sb)O	Pr0.65Sr0.35Fe1As0.9Sb0.1O1	Pr	0.65	Sr	0.35	Fe	1	As	0.9	Sb	0.1											O	1		1	2014																										ABCD		oxypnictide																	ZrCuSiAs-type	K			21.87				21.87																				T	RES(R=0.95Rn), WHH	17.8							T/K	RES(R=0.95Rn)	1.3			HC154289																																																														Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154290	PHC4980050	RRR = 4.85. Hall coeffic. RH(25K) = 0.70 E-8 m3/C.	(Pr,Sr)Fe(As,Sb)O	Pr0.65Sr0.35Fe1As0.8Sb0.2O1	Pr	0.65	Sr	0.35	Fe	1	As	0.8	Sb	0.2											O	1		1	2014																										ABCD		oxypnictide																	ZrCuSiAs-type	K			22				22																				T	RES(R=0.95Rn), WHH	30.7							T/K	RES(R=0.95Rn)	2.1			HC154290																																																														Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154291	PHC4980050	RRR = 8.47. Hall coeffic. RH(25K) = 0.45 E-8 m3/C.	(Pr,Sr)Fe(As,Sb)O	Pr0.65Sr0.35Fe1As0.85Sb0.15O1	Pr	0.65	Sr	0.35	Fe	1	As	0.85	Sb	0.15											O	1		1	2014																										ABCD		oxypnictide			A	3.996		8.648											ZrCuSiAs-type	K			21.9				21.9																																																																																																Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154292	PHC4980050	RRR = 8.51. Hall coeffic. RH(25K) = 0.51 E-8 m3/C.	(Pr,Sr)Fe(As,P)O	Pr0.65Sr0.35Fe1As0.95P0.05O1	Pr	0.65	Sr	0.35	Fe	1	As	0.95	P	0.05											O	1		1	2014																										ABCD		oxypnictide																	ZrCuSiAs-type	K			15.4				15.4																																																																																																Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154293	PHC4980050	Hall coeffic. RH(25K) = 4.49 E-8 m3/C.	(Pr,Sr)Fe(As,P)O	Pr0.65Sr0.35Fe1As0.9P0.1O1	Pr	0.65	Sr	0.35	Fe	1	As	0.9	P	0.1											O	1		1	2014																										ABCD		oxypnictide			A	3.979		8.598											ZrCuSiAs-type	K			0		2		0																																																																																																Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154294	PHC4980050	RRR = 8.41	(Pr,Sr)Fe(As,Sb)O	Pr0.6Sr0.4Fe1As0.9Sb0.1O1	Pr	0.6	Sr	0.4	Fe	1	As	0.9	Sb	0.1											O	1		1	2014																										ABCD		oxypnictide			A	3.998		8.662												K			22				22																																																																																																Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154295	PHC4980050	RRR = 9.45. Hall coeffic. RH(25K) = 0.604 E-8 m3/C.	(Pr,Sr)FeAsO	Pr0.65Sr0.35Fe1As1O1	Pr	0.65	Sr	0.35	Fe	1	As	1													O	1		1	2014																										ABCD		oxypnictide			A	3.994		8.655												K			16.5				16.5																																																																																																Two step solid state reaction. 1st step: PrAs,SrAs,PrSb(or PrP) were prepared. 2nd step: mixture - pellet - ANN(1150C,40h) - FC to RT					Enhancement of superconductivity by Sb-doping in the hole-doped iron-pnictide superconductor Pr1-xSrxFeAsO			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Physica C, 498(2014)50	Qiucheng Ji,Bo Gao,Gang Mu,Tao Hu,Wei Li,Yinshang Liu,Yonghui Ma,Xiaoming Xie		
154296	PRB087180507	RRR=380. Tc(SP)=3.5K. (dC/Tc) = 46 mJ/mol.K2. Low-T SP represented by C=A*T+B*T^2+C*T^3. B=33.7 mJ/mol.K3 from cluster-glass phase.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2013																										AB2C2																			Fe-122	K	3.6						3.6																																																					MSP154296			mJ/mol.K2	44.8		262												uOhm.cm								1.44																	crystals grown using KAs as a flux.					Evidence of d-wave superconductivity in K1-xNaxFe2As2 (x = 0,0.1) single crystals from low-temperature specific-heat measurements			Leibniz Institute for Solid State and Materials Research, IFW-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 87(2013)180507	M. Abdel-Hafiez,V. Grinenko,S. Aswartham,I. Morozov,M. Roslova,O. Vakaliuk,S. Johnston,D. V. Efremov,J. van den Brink,H. Rosner,M. Kumar,C. Hess,S. Wurmehl,A. U. B. Wolter,B. Buchner,E. L. Green,J. Wosnitza,P. Vogt,A. Reifenberger,C. Enss		
154297	PRB087180507	RRR=120. Tc(SP)=2.75K. (dC/Tc) = 40 mJ/mol.K2. Low-T SP represented by C=A*T+B*T^2+C*T^3. B=35.4 mJ/mol.K3 from cluster-glass phase.	(K,Na)Fe2As2	K0.9Na0.1Fe2As2	K	0.9	Na	0.1	Fe	2	As	2																3	2013																										AB2C2																			Fe-122	K	2.9						2.9																																																					MSP154297			mJ/mol.K2	55.2		264												uOhm.cm								3.82																	crystals grown using KAs as a flux.					Evidence of d-wave superconductivity in K1-xNaxFe2As2 (x = 0,0.1) single crystals from low-temperature specific-heat measurements			Leibniz Institute for Solid State and Materials Research, IFW-Dresden, D-01171 Dresden, Germany	Phys.Rev.B, 87(2013)180507	M. Abdel-Hafiez,V. Grinenko,S. Aswartham,I. Morozov,M. Roslova,O. Vakaliuk,S. Johnston,D. V. Efremov,J. van den Brink,H. Rosner,M. Kumar,C. Hess,S. Wurmehl,A. U. B. Wolter,B. Buchner,E. L. Green,J. Wosnitza,P. Vogt,A. Reifenberger,C. Enss		
154298	PRB087224504	(dC/gamma*Tc) = 2.0. R(T) = R0 + A*T^n: n = 1.61	Ir0.95Te2	Ir0.95Te2	Ir	0.95	Te	2																				1	2013																										AB2		pyrite			A	6.4361														K		4.68					4.68																																																											260																																					mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154299	PRB087224504	(dC/gamma*Tc) = 1.92. R(T) = R0 + A*T^n: n = 1.65	Ir0.95-xRhxTe2	Ir0.85Rh0.1Te2	Ir	0.85	Rh	0.1	Te	2																		1	2013																										AB2		pyrite			A	6.44														K		4.49					4.49																																																											257																																					mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154300	PRB087224504	(dC/gamma*Tc) = 1.77. R(T) = R0 + A*T^n: n = 1.93	Ir0.95-xRhxTe2	Ir0.75Rh0.2Te2	Ir	0.75	Rh	0.2	Te	2																		1	2013																										AB2		pyrite			A	6.4433														K		4.33					4.33	MTC154300																																																							mJ/mol.K2	7.66		288																																					mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154301	PRB087224504	(dC/gamma*Tc) = 1.60. R(T) = R0 + A*T^n: n = 1.92	Ir0.95-xRhxTe2	Ir0.68Rh0.27Te2	Ir	0.68	Rh	0.27	Te	2																		1	2013																										AB2		pyrite			A	6.4447														K		4.02					4.02																																																								mJ/mol.K2	7.79		309																																					mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154302	PRB087224504	(dC/gamma*Tc) = 1.52. R(T) = R0 + A*T^n: n = 2.02	Ir0.95-xRhxTe2	Ir0.58Rh0.37Te2	Ir	0.58	Rh	0.37	Te	2																		1	2013																										AB2		pyrite			A	6.4464														K		3.76					3.76																																																											339																																					mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154303	PRB087224504	(dC/gamma*Tc) = 1.49. R(T) = R0 + A*T^n: n = 2.15	Ir0.95-xRhxTe2	Ir0.53Rh0.42Te2	Ir	0.53	Rh	0.42	Te	2																		1	2013																										AB2		pyrite			A	6.4463														K		3.2					3.2																																																								mJ/mol.K2	8.77																																							mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154304	PRB087224504	(dC/gamma*Tc) = 1.30. R(T) = R0 + A*T^n: n = 2.09	Ir0.95-xRhxTe2	Ir0.43Rh0.52Te2	Ir	0.43	Rh	0.52	Te	2																		1	2013																										AB2		pyrite			A	6.4462														K		2.82					2.82																																																																																																mixture - pelletized - h-BN capsule - heat(1573 K,2h, P=5 GPa)					Structure and superconductivity in pyrite Ir0.95-xRhxTe2: A comparison with analogous selenides			Frontier research center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 87(2013)224504	Jiangang Guo,Yanpeng Qi,Hideo Hosono		
154305	PRB087235111	optimal F-cintent sample. Tc(P) measured upto 8GPa. Tc defined as SUS(on)	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide																	Fe-1111	K				27			27	TC154305																																																																																													RAs,Fe,Fe2O3,FeF2		solid state reaction. mixture - heat(1100C,20h) - wrapped (Ta-foil) - silica tube - heat(250-1000C)					Superconductivity under pressure in RFeAsO1-xFx (R = La, Ce-Sm) by dc magnetization measurements			Department of Material Science, Shimane University, Matsue 690-8504, Japan	Phys.Rev.B, 87(2013)235111	Kiyotaka Miyoshi,Eiko Kojima,Saki Ogawa,Yuta Shimojo,Jun Takeuchi		
154306	PRB087235111	optimal F-cintent sample. Tc(P) measured upto 8GPa. Tc defined as SUS(on)	Ce(O,F)FeAs	Ce1Fe1As1F0.1O0.9	Ce	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide																	Fe-1111	K				38			38	TC154306																																																																																													RAs,Fe,Fe2O3,FeF2		solid state reaction. mixture - heat(1100C,20h) - wrapped (Ta-foil) - silica tube - heat(250-1000C)					Superconductivity under pressure in RFeAsO1-xFx (R = La, Ce-Sm) by dc magnetization measurements			Department of Material Science, Shimane University, Matsue 690-8504, Japan	Phys.Rev.B, 87(2013)235111	Kiyotaka Miyoshi,Eiko Kojima,Saki Ogawa,Yuta Shimojo,Jun Takeuchi		
154307	PRB087235111	optimal F-cintent sample. Tc(P) measured upto 8GPa. Tc defined as SUS(on)	Pr(O,F)FeAs	Pr1Fe1As1F0.1O0.9	Pr	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide																	Fe-1111	K				43			43	TC154307																																																																																													RAs,Fe,Fe2O3,FeF2		solid state reaction. mixture - heat(1100C,20h) - wrapped (Ta-foil) - silica tube - heat(250-1000C)					Superconductivity under pressure in RFeAsO1-xFx (R = La, Ce-Sm) by dc magnetization measurements			Department of Material Science, Shimane University, Matsue 690-8504, Japan	Phys.Rev.B, 87(2013)235111	Kiyotaka Miyoshi,Eiko Kojima,Saki Ogawa,Yuta Shimojo,Jun Takeuchi		
154308	PRB087235111	optimal F-cintent sample. Tc(P) measured upto 8GPa. Tc defined as SUS(on)	Nd(O,F)FeAs	Nd1Fe1As1F0.1O0.9	Nd	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide																	Fe-1111	K				48			48	TC154308																																																																																													RAs,Fe,Fe2O3,FeF2		solid state reaction. mixture - heat(1100C,20h) - wrapped (Ta-foil) - silica tube - heat(250-1000C)					Superconductivity under pressure in RFeAsO1-xFx (R = La, Ce-Sm) by dc magnetization measurements			Department of Material Science, Shimane University, Matsue 690-8504, Japan	Phys.Rev.B, 87(2013)235111	Kiyotaka Miyoshi,Eiko Kojima,Saki Ogawa,Yuta Shimojo,Jun Takeuchi		
154309	PRB087235111	optimal F-cintent sample. Tc(P) measured upto 8GPa. Tc defined as SUS(on)	Sm(O,F)FeAs	Sm1Fe1As1F0.1O0.9	Sm	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide																	Fe-1111	K				53			53	TC154309																																																																																													RAs,Fe,Fe2O3,FeF2		solid state reaction. mixture - heat(1100C,20h) - wrapped (Ta-foil) - silica tube - heat(250-1000C)					Superconductivity under pressure in RFeAsO1-xFx (R = La, Ce-Sm) by dc magnetization measurements			Department of Material Science, Shimane University, Matsue 690-8504, Japan	Phys.Rev.B, 87(2013)235111	Kiyotaka Miyoshi,Eiko Kojima,Saki Ogawa,Yuta Shimojo,Jun Takeuchi		
154310	PRB088024423	impurity phase: La2Pd3Si3. (dC/T) = 27 mJ/mol.K2. (dC/gamma*Tc) = 1.03. Debye-T = 155K calculated from R(T). Hc2(0) represented by two band model (a1=1.95, a2=1.1)	La3Pd4Si4	La3Pd4Si4	La	3	Pd	4	Si	4																		1	2013																										A3B4C4		U3Ni4Si4	Immm		A	4.2358	4.29	24.54												K		1.98					1.98																				T	RES,Two band model	0.6												MHC154310																			MSP154310			mJ/mol.K2	26	SP	280	SP																																		R(3N),Si(5N),Pd(4N)		arc-melting - ANN(800C,30days, in quartz tube) - Q to cold water					Superconductivity and non-Fermi-liquid behavior of La3Pd4Si4 and Ce3Pd4Si4			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 88(2013)024423	F. Kneidinger,H. Michor,E. Bauer,A. Gribanov,A. Lipatov,Y. Seropegin,J. Sereni,P. Rogl		
154311	PRB088024423	not SC. Kondo lattice system. R(T) has max around 8.5 K.	Ce3Pd4Si4	Ce3Pd4Si4	Ce	3	Pd	4	Si	4																		1	2013																										A3B4C4		U3Ni4Si4	Immm																	K					0.34																																																																																																R(3N),Si(5N),Pd(4N)		arc-melting - ANN(800C,30days, in quartz tube) - Q to cold water					Superconductivity and non-Fermi-liquid behavior of La3Pd4Si4 and Ce3Pd4Si4			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 88(2013)024423	F. Kneidinger,H. Michor,E. Bauer,A. Gribanov,A. Lipatov,Y. Seropegin,J. Sereni,P. Rogl		
154312	PRB088024508	SC for very narrow region of x (Pd-content): for 0.68=<x=<0.702. R(T) = A*T^n : n=2 (Fermi-liquid type). [phc2zero] is Hc2//b, [nhc2zero] is hc2//a, Hc2(0)//c = 7.16 T.	Nb3Pd0.7Se7	Nb3Pd0.7Se7	Nb	3	Pd	0.7	Se	7																		3	2013																													C2/m		A	12.7965	3.4059	21.037											beta=95.53, alpha and gammma = 90.0	K		2.1					2.1																				T	RES(R=0.5Rn),extrapolation.		14.1	3.47										MHC154312																																																												Nb(4N),Pd(4N),Se(5N)		mixture(Nb:Pd:Se = 4:1:10) - sealed in quartz tube - heat to 850C(100C/h) - keep(850C,48h) -Q to RT					Anomalous metallic state and anisotropic multiband superconductivity in Nb3Pd0.7Se7			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 88(2013)024508	Q. R. Zhang,D. Rhodes,B. Zeng,T. Besara,T. Siegrist,M. D. Johannes,L. Balicas		
154313	PRB088024508	SC for very narrow region of x (Pd-content): around x = 0.67. R(T) = A*T^n : n = 0.54 for T > 50K.	Nb2Pd0.67Se5	Nb2Pd0.67Se5	Nb	2	Pd	0.67	Se	5																		3	2013																													C2/m		A	12.8325	3.39327	15.3859											beta=101.471, alpha and gammma = 90.0	K		1.2					1.2																																																																																														Nb(4N),Pd(4N),Se(5N)		mixture(Nb:Pd:Se = 4:1:10) - sealed in quartz tube - heat to 850C(100C/h) - keep(850C,48h) -Q to RT					Anomalous metallic state and anisotropic multiband superconductivity in Nb3Pd0.7Se7			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA	Phys.Rev.B, 88(2013)024508	Q. R. Zhang,D. Rhodes,B. Zeng,T. Besara,T. Siegrist,M. D. Johannes,L. Balicas		
154314	PRB088064503	Tc(max) = 10.1 K (P=1.1 GPa). (dTc/dP) = -0.30 K/GPa for P>1.1 GPa.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																															A	4.0613		13.3157												K		3.34					3.34	TC154314																																																																																													La2O3(3N),LaF3(3N),La2S3(3N),Bi2S3(3N)		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Pressure-induced enhancement of superconductivity and suppression of semiconducting behavior in LnO0.5F0.5BiS2 (Ln = La,Ce) compounds			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 88(2013)064503	C. T. Wolowiec,D. Yazici,B. D. White,K. Huang,M. B. Maple		
154315	PRB088064503	Tc(max) = 6.7 K (P = 2 GPa). (dTc/dP) = -0.30 K/GPa for P > 2 GPa.	Ce(O,F)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																															A	4.0398		13.4513												K		2.27					2.27	TC154315																																																																																													CeF3(3N),CeO2(3N),Bi2S3(3N)		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Pressure-induced enhancement of superconductivity and suppression of semiconducting behavior in LnO0.5F0.5BiS2 (Ln = La,Ce) compounds			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 88(2013)064503	C. T. Wolowiec,D. Yazici,B. D. White,K. Huang,M. B. Maple		
154316	PRB088064510	e-ph coupling = 0.49	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2013																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide	K		1.2				0.2	1.2																				T	SP, WHH	0.08												HC154316		A	from Hc2	640								meV	0.15	2.91	14							mJ/mol.K2	10.9	SP	230	SP																																		BaO(4N),Ti(4N),Sb(5N)		mixture - pellet - in welded Nb container in quartz - heat to 900C(2C/min) - keep(900c3d) - slow cool to 200C(1C/min) - reground - pellet - ANN(900C,3d)					Weak coupling BCS-like superconductivity in the pnictide oxide Ba1-xNaxTi2Sb2O (x = 0 and 0.15)			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 88(2013)064510	Melissa Gooch,Phuong Doan,Zhongjia Tang,Bernd Lorenz,Arnold M. Guloy,Paul C. W. Chu		
154317	PRB088064510	Tc = 4.2 K from SP. e-ph coupling = 0.68	(Ba,Na)Ri2Sb2O	Ba0.85Na0.15Ti2Sb2O1	Ba	0.85	Na	0.15	Ti	2	Sb	2													O	1		1	2013																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide	K		5					5																				T	SP, WHH	1.7												HC154317		A	from Hc2	140								meV	0.65	3.6	14							mJ/mol.K2	13	SP	210	SP																																		BaO(4N),BaO2,Na2O,Na2O2,Ti(4N),Sb(5N)		mixture - pellet - in welded Nb container in quartz - heat to 900C(2C/min) - keep(900c3d) - slow cool to 200C(1C/min) - reground - pellet - ANN(900C,3d)					Weak coupling BCS-like superconductivity in the pnictide oxide Ba1-xNaxTi2Sb2O (x = 0 and 0.15)			TCSUH and Department of Physics, University of Houston, Houston, Texas 77204, USA	Phys.Rev.B, 88(2013)064510	Melissa Gooch,Phuong Doan,Zhongjia Tang,Bernd Lorenz,Arnold M. Guloy,Paul C. W. Chu		
154318	ZAAC5840150		Na2Ti2Sb2O	Na2Ti2Sb2O1	Na	2	Ti	2	Sb	2															O	1		1	1990																												oxypnictide	I4/mmm	139	A	4.144		16.561												K					4																																																																																																		solid stte reaction					Darstellung und Kristallstructur der Pnictidoxide Na2Ti2As2O und Na2Ti2Sb2O				Z.Anorg.Allg.Chem., 584(1990)150	A.Adam,H.-U.Schuster		
154319	PRB088094521	M = NH3. M-content (y)  not given. impurity phases are beta-FeSe(37%), alpha-FeSe(26%). Cs-content = Cs0.255 in this formula by XRD. R not to zero at5K.	(NH3)yCs0.4FeSe	M1Cs0.4Fe1Se1	M	1	Cs	0.4	Fe	1	Se	1																1	2013																													I4/mmm		A	3.8331		16.217												K		31.2	36				31.2	MTC154320		K/GPa	-4.33						31.2																																																																																						annealing method using liquid NH3 technique.					Superconductivity in (NH3)yCs0.4FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 88(2013)094521	Lu Zheng,Masanari Izumi,Yusuke Sakai,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kambe,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Jungeun Kim,Akihiko Fujiwara,Yoshihiro Kubozono		
154320	PRB088094521	beta-FeSe(80%) + alpha-FeSe(20%).	beta-FeSe	Fe1Se1	Fe	1	Se	1																				1	2013																													P4/mmm		A	3.771		5.5234												K		8.2		9			8.2										92																																																																																											Superconductivity in (NH3)yCs0.4FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 88(2013)094521	Lu Zheng,Masanari Izumi,Yusuke Sakai,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kambe,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Jungeun Kim,Akihiko Fujiwara,Yoshihiro Kubozono		
154321	PRB088094521	M = NH3. M-content (y)  not given. M(=NH3) intercalated sample.	(NH3)yK0.4FeSe	M1K0.4Fe1Se1	M	1	K	0.4	Fe	1	Se	1																1	2013																																														K		27.2		30			27.2																																																																																																annealing method using liquid NH3 technique.					Superconductivity in (NH3)yCs0.4FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 88(2013)094521	Lu Zheng,Masanari Izumi,Yusuke Sakai,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kambe,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Jungeun Kim,Akihiko Fujiwara,Yoshihiro Kubozono		
154322	PRB088094521	M = NH3. M-content (y)  not given. M(=NH3) intercalated sample.	(NH3)yRb0.4FeSe	M1Rb0.4Fe1Se1	M	1	Rb	0.4	Fe	1	Se	1																1	2013																																														K		29.9		31			29.9																																																																																																annealing method using liquid NH3 technique.					Superconductivity in (NH3)yCs0.4FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 88(2013)094521	Lu Zheng,Masanari Izumi,Yusuke Sakai,Ritsuko Eguchi,Hidenori Goto,Yasuhiro Takabayashi,Takashi Kambe,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Jungeun Kim,Akihiko Fujiwara,Yoshihiro Kubozono		
154323	SCIR0031446	needle like crystals(b-axis long). (dC/gamma) = 0.37. Anisotropy (Hc2//b)/(Hc2//ab) = 3 (Tc) and 1.5 (T<1 K).	Nb2Pd0.81S5	Nb2Pd0.81S5	Nb	2	Pd	0.81	S	5																		3	2013																											4		C2/m	12															monoclinic	K		6.6					6.6																				T	RES. extrapolation		37											MHC154323																						mJ/mol.K2	15																																												Superconductivity with extremely large upper critical fields in Nb2Pd0.81S5			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida, USA	Scientific Reports, 3(2013)1446	Q.Zhang,G.Li,D.Rhodes,A.Kiswondhi,T.Besara,B.Zeng,J.Sun,T.Siegrist,M.D.Johannes,L.Balicas		
154324	PRB088104507		Nb2Pd2S5	Nb2Pd1S5	Nb	2	Pd	1	S	5																		1	2013																										AB2C5	4		C2/m		A	12.2077	3.3797	15.0656											monoclinic	K			6.25				6.25																				T	RES(R=0.9Rn), WHH	20.8												MHC154324																																																												Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154325	PRB088104507	R(T) has minimum at 17.3 K. SP-heat coeffic.: (beta) = 2.97 mJ/mol.K4, (delta) = -0.00738 mJ/mol.K6.  (dC/gamma:Tc) = 1.2.	Nb2Pd2(S,Se)5	Nb2Pd1S4.5Se0.5	Nb	2	Pd	1	S	4.5	Se	0.5																1	2013																										AB2C5	4		C2/m		A	12.3	3.3753	15.092											monoclinic	K			4.27				4.27																				T	RES(R=0.9Rn), WHH	14.6												MHC154324																						mJ/mol.K2	19.2																																					Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154326	PRB088104507	R(T) has minimum at 24.7 K	Nb2Pd2(S,Se)5	Nb2Pd1S4.25Se0.75	Nb	2	Pd	1	S	4.25	Se	0.75																1	2013																										AB2C5	4		C2/m		A	12.3132	3.3792	15.1088											monoclinic	K			3.18				3.18																				T	RES(R=0.9Rn), WHH	10.4												MHC154326																																																												Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154327	PRB088104507	R(T) has minimum at 27.7 K	Nb2Pd2(S,Se)5	Nb2Pd1S4Se1	Nb	2	Pd	1	S	4	Se	1																1	2013																										AB2C5	4		C2/m		A	12.3527	3.3896	15.1568											monoclinic	K			2.76				2.76																				T	RES(R=0.9Rn), WHH	9.36												MHC154326																																																												Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154328	PRB088104507	R(T) has minimum at 44.9 K.	Nb2Pd2(S,Se)5	Nb2Pd1S3.75Se1.25	Nb	2	Pd	1	S	3.75	Se	1.25																1	2013																										AB2C5	4		C2/m		A	12.4758	3.3929	15.1712											monoclinic	K			2.23				2.23																																																																																														Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154329	PRB088104507	R(T) has minimum at 59.4 K.	Nb2Pd2(S,Se)5	Nb2Pd1S3.5Se1.5	Nb	2	Pd	1	S	3.5	Se	1.5																1	2013																										AB2C5	4		C2/m		A	12.4978	3.3885	15.2036											monoclinic	K			1.87				1.87																				T	RES(R=0.9Rn), WHH	6.49												MHC154329																																																												Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154330	PRB088104507	R(T) has minimum at 98.7 K.	Nb2Pd2(S,Se)5	Nb2Pd1S3Se2	Nb	2	Pd	1	S	3	Se	2																1	2013																										AB2C5	4		C2/m		A	12.5593	3.3808	15.2096											monoclinic	K			1.17				1.17																				T	RES(R=0.9Rn), WHH	4.04												MHC154329																																																												Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154331	PRB088104507	R(T) has minimum at 150.2 K.	Nb2Pd2(S,Se)5	Nb2Pd1S2Se3	Nb	2	Pd	1	S	2	Se	3																1	2013																										AB2C5	4		C2/m		A	12.6033	3.3863	15.2732											monoclinic	K					0.8																																																																																																Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154332	PRB088104507	R(T) has minimum at 179.5 K.	Nb2Pd2(S,Se)5	Nb2Pd1S1Se4	Nb	2	Pd	1	S	1	Se	4																1	2013																										AB2C5	4		C2/m		A	12.722	3.3907	15.3308											monoclinic	K					0.8																																																																																																Nb(4N),Pd(3N),S(4N),Se(4N)		solid state reaction. mixture(Nb:Pd:(S,Se) = 2:1:7.2) - pellet - sealed in quartz tube - heat(825C,48h) - Q to RT					Effect of selenium doping on the superconductivity of Nb2Pd(S1-xSex)5			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 88(2013)104507	C. Q. Niu,J. H. Yang,Y. K. Li,Bin Chen,N. Zhou,J. Chen,L. L. Jiang,B. Chen,X. X. Yang,Chao Cao,Jianhui Dai,Xiaofeng Xu		
154333	PRB088134520	minor phase(less than 5%) Y5Bi3-type Zr5Sb.	Zr5Sb	Sb3Zr5	Sb	3	Zr	5																				1	2013																										A3B5	7	Mo5Si3	P6<3>mcm		A	8.4053		5.764												K				2.3		0.2	2.3											Oe	M-H curve				5			1.9	T	SP, WHH	2.8																															MSP154333			mJ/mol.K2	24.1	SP	240	SP											mOhm.cm											0.36														arc-melting (Zr:Sb = 5:3+d, d=0.3)					Superconductivity in the Mn5Si3-type Zr5Sb3 system			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 88(2013)134520	B. Lv,X. Y. Zhu,B. Lorenz,F. Y. Wei,Y. Y. Xue,Z. P. Yin,G. Kotliar,C. W. Chu		
154334	PRB088134520	not SC.	Zr5Sn	Sn3Zr5	Sn	3	Zr	5																				1	2013																										A3B5	7	Mo5Si3	P6<3>mcm		A	8.4603		5.7771												K							1.9																																																								mJ/mol.K2	14	SP	280	SP																																				arc-melting (Zr:Sb = 5:3+d, d=0.3)					Superconductivity in the Mn5Si3-type Zr5Sb3 system			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 88(2013)134520	B. Lv,X. Y. Zhu,B. Lorenz,F. Y. Wei,Y. Y. Xue,Z. P. Yin,G. Kotliar,C. W. Chu		
154335	PRB088134520	5 % Hf- or Y-doped Zr5Sb3.	Zr5Sb	Sb3Zr5	Sb	3	Zr	5																				1	2013																										A3B5	7	Mo5Si3	P6<3>mcm		A															K				2.2			2.2																																																																																																arc-melting (Zr:Sb = 5:3+d, d=0.3)					Superconductivity in the Mn5Si3-type Zr5Sb3 system			Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 88(2013)134520	B. Lv,X. Y. Zhu,B. Lorenz,F. Y. Wei,Y. Y. Xue,Z. P. Yin,G. Kotliar,C. W. Chu		
154336	PRB088140501	Energy gap by muon-SR. Tc(x) in Ba1-xNaxTi2Sb2O [MTCFIG} festimated from  M(T) -graoh.	(Ba,Na)Ti2Sb2O	Ba0.75Na0.25Ti2Sb2O1	Ba	0.75	Na	0.25	Ti	2	Sb	2													O	1		1	2013																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide	K		4.5		5.1			4.5																				T					1.5			1.5													nm	muon-SR	307			meV	0.56	2.9	16																																													BaO2,Na2O2,Ti,Sb		mixture - pellet - sealed in Nb ampule - SIN(1000C, 24h) -redround - pellet - SIN(1000C,36h)					Conventional superconductivity and charge-density-wave ordering in Ba1-xNaxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 88(2013)140501	Fabian von Rohr,Andreas Schilling,Reinhard Nesper,Chris Baines,Markus Bendele		
154337	PRB088140502	BCS-alpha-model, alpha(= gap/Tc) = 1.77. rhombohedral for hole density < 4.8 E+20 /cm3	(Sn,In)Te	Sn0.975In0.025Te1	Sn	0.975	In	0.025	Te	1																		3	2013																																													rhombohedral	K		1.42				0.022	1.42																																																								mJ/mol.K2	0.87														mOhm.cm	0.46																				n/cm3	320000000000000000000	Sn(4N),In(4N),Te(5N)		vapor transport method. source materials - keep (( center(630C), T-gradient = 1.5K/cm), 1 week)					Unusual nature of fully gapped superconductivity in In-doped SnTe			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 88(2013)140502	Mario Novak,Satoshi Sasaki,Markus Kriener,Kouji Segawa,Yoichi Ando		
154338	PRB088140502	BCS-alpha-model, alpha(= gap/Tc) = 1.83	(Sn,In)Te	Sn0.96In0.04Te1	Sn	0.96	In	0.04	Te	1																		3	2013																											1																		cubic	K		1.22					1.22	MTC154338																																																																																											n/cm3	500000000000000000000	Sn(4N),In(4N),Te(5N)		vapor transport method. source materials - keep (( center(630C), T-gradient = 1.5K/cm), 1 week)					Unusual nature of fully gapped superconductivity in In-doped SnTe			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 88(2013)140502	Mario Novak,Satoshi Sasaki,Markus Kriener,Kouji Segawa,Yoichi Ando		
154339	PRB088140502	BCS-alpha-model, alpha(= gap/Tc) = 1.88	(Sn,In)Te	Sn0.95In0.05Te1	Sn	0.95	In	0.05	Te	1																		3	2013																											1																		cubic	K		1.41					1.41																																																																																												n/cm3	700000000000000000000	Sn(4N),In(4N),Te(5N)		vapor transport method. source materials - keep (( center(630C), T-gradient = 1.5K/cm), 1 week)					Unusual nature of fully gapped superconductivity in In-doped SnTe			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 88(2013)140502	Mario Novak,Satoshi Sasaki,Markus Kriener,Kouji Segawa,Yoichi Ando		
154340	PRB088140507	Compositions by EPMA. Structure analyzed by Ba3Rh4Ge16.  (dC/gamma*Tc) = 1.85	Ba3Ir4Ge16	Ba3Ir4Ge16	Ba	3	Ir	4	Ge	16																		1	2013																										A3B4C16	2		I4/mmm		A	6.5387		22.2834												K			6.1				6.1																				T	RES(R=0.9Rn), linear approx.	1.82							T/K	RES(R=0.9Rn)	0.315			MHC154340		A	from Hc2	134.5															MSP154340			mJ/mol.K2	21	SP	240	SP																																				arc-melting. ANN(1073K,10h) - ANN(1273K,10h)					Superconductivity in Ban+2Ir4nGe12n+4 (n = 1,2) with cage structure and softening of low-lying localized mode			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 88(2013)140507	Jiangang Guo,Jun-ichi Yamaura,Hechang Lei,Satoru Matsuishi,Yanpeng Qi,Hideo Hosono		
154341	PRB088140507	Compositions by EPMA. (dC/gamma*Tc) = 1.31	Ba4Ir8Ge28	Ba4Ir8Ge28	Ba	4	Ir	8	Ge	28																		3	2013																										A4B8C28	3		Pmna		A	37.737	6.4246	6.4567												K			3.2				3.2																				T	RES(R=0.9Rn), linear approx.	1.63							T/K	RES(R=0.9Rn)	0.492			MHC154340		A	from Hc2	142.1															MSP154341			mJ/mol.K2	36	SP	254	SP																																				IrGe-flux method: mixture - heat to 1373K - cool to 1173K(4K/h) - FC to RT					Superconductivity in Ban+2Ir4nGe12n+4 (n = 1,2) with cage structure and softening of low-lying localized mode			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 88(2013)140507	Jiangang Guo,Jun-ichi Yamaura,Hechang Lei,Satoru Matsuishi,Yanpeng Qi,Hideo Hosono		
154342	PRB088144510	(dC/gamma*Tc) = 1.86. gap(0) = 1.93Tc		Nb0.18Re0.82	Nb	0.18	Re	0.82																				1	2013																																													cubic, Ti5Re24 structure type	K		8.9		8.6			8.9																				T	RES(R=0.5Rn), linear approx.	23																			nm	TDO method	414													mJ/mol.K2	4.8	SP																																				Nb(4N),Re(4N)		arc-melting. ANN(800C,7d. in evacuated quartz tube)					BCS-like superconductivity in the noncentrosymmetric compounds NbxRe1-x (0.13 =< x =< 0.38)			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 88(2013)144510	J. Chen,L. Jiao,J. L. Zhang,Y. Chen,L. Yang,M. Nicklas,F. Steglich,H. Q. Yuan		
154343	PRB088144510			Nb0.25Re0.75	Nb	0.25	Re	0.75																				1	2013																																													cubic, Ti5Re24 structure type	K		6.75		6.52			6.75																				T	RES(R=0.5Rn), linear approx.	14.5																																		mJ/mol.K2	4.24	SP																																				Nb(4N),Re(4N)		arc-melting. ANN(800C,7d. in evacuated quartz tube)					BCS-like superconductivity in the noncentrosymmetric compounds NbxRe1-x (0.13 =< x =< 0.38)			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 88(2013)144510	J. Chen,L. Jiao,J. L. Zhang,Y. Chen,L. Yang,M. Nicklas,F. Steglich,H. Q. Yuan		
154344	PRB088144510			Nb0.29Re0.71	Nb	0.29	Re	0.71																				1	2013																																													cubic, Ti5Re24 structure type	K		5.62		5.03			5.62																				T	RES(R=0.5Rn), linear approx.	11.8																																		mJ/mol.K2	3.46	SP																																				Nb(4N),Re(4N)		arc-melting. ANN(800C,7d. in evacuated quartz tube)					BCS-like superconductivity in the noncentrosymmetric compounds NbxRe1-x (0.13 =< x =< 0.38)			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 88(2013)144510	J. Chen,L. Jiao,J. L. Zhang,Y. Chen,L. Yang,M. Nicklas,F. Steglich,H. Q. Yuan		
154345	PRB088144510	(dC/gamma*Tc) = 0.5		Nb0.31Re0.69	Nb	0.31	Re	0.69																				1	2013																																													cubic, Ti5Re24 structure type	K		4.92		4.3			4.92																				T	RES(R=0.5Rn), linear approx.	9																																		mJ/mol.K2	2.99	SP																																				Nb(4N),Re(4N)		arc-melting. ANN(800C,7d. in evacuated quartz tube)					BCS-like superconductivity in the noncentrosymmetric compounds NbxRe1-x (0.13 =< x =< 0.38)			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310027, China	Phys.Rev.B, 88(2013)144510	J. Chen,L. Jiao,J. L. Zhang,Y. Chen,L. Yang,M. Nicklas,F. Steglich,H. Q. Yuan		
154346	PRB088144511	Pd-content by X-ray analysis. RRR=2.45(in-plane). nearly T-independent Hall const.	LaPdxBi2	La1Pd0.85Bi2	La	1	Pd	0.85	Bi	2																		3	2013									10.068																		2	ZrCuSi2	P4/nmm		A	4.634		9.9436												K	2		4	2.1			2.1																				T	RES(R=0.9Rn), GL	3												MHC154346																																																			cm3/C	-0.00017								La(Ce),Pd,Bi		self-flux method. mixture(La/Ce:Pd:Bi = 1:1:12) - alumina crucible - evacuated silica tube - heat to 900C - keep(900C,10h) - slow cool to 500C - remove excess Bi					Superconductivity and strong intrinsic defects in LaPd1-xBi2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States	Phys.Rev.B, 88(2013)144511	Fei Han,Christos D. Malliakas,Constantinos C. Stoumpos,Mihai Sturza,Helmut Claus,Duck Young Chung,Mercouri G. Kanatzidis		
154347	PRB088144511	not SC. Tn(AFM) for H//c-axis.	CePdxBi2	Ce1Pd0.78Bi2	Ce	1	Pd	0.78	Bi	2																		3	2013					myu-B/Ce	2.86	-1.5	6	10.366																		2	ZrCuSi2	P4/nmm		A	4.6136		9.65												K					2																																																																																														n/cm3	37000000000000000000000	La(Ce),Pd,Bi		self-flux method. mixture(La/Ce:Pd:Bi = 1:1:12) - alumina crucible - evacuated silica tube - heat to 900C - keep(900C,10h) - slow cool to 500C - remove excess Bi					Superconductivity and strong intrinsic defects in LaPd1-xBi2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States	Phys.Rev.B, 88(2013)144511	Fei Han,Christos D. Malliakas,Constantinos C. Stoumpos,Mihai Sturza,Helmut Claus,Duck Young Chung,Mercouri G. Kanatzidis		
154348	PRB088174512	Hc1(T) well described by two gap model(lower 0.41 and higher 3.33 meV) or anisotropic s-wave model (1.663 meV in DB). Jc(2K) = 1.34 E+4 A/cm2 for H//c.	FeSe	Fe1Se1	Fe	1	Se	1																				3	2013																										AB																			Fe-11	K				9.4			9.4											Oe	M-H curve						25	2															MHC154348							nm	Hc1	445			meV	1.663	4.11																																																single crystals grown in evacuated quartz ampoule using AlCl3/KCl flux method. hot end(427C), cold end(380C, T-gradient(5C/cm.					Temperature dependence of lower critical field Hc1(T) shows nodeless superconductivity in FeSe			Departement de Physique, Universite de Liege, B-4000 Sart Tilman, Belgium	Phys.Rev.B, 88(2013)174512	M. Abdel-Hafiez,J. Ge,A. N. Vasiliev,D. A. Chareev,J. Van de Vondel,V. V. Moshchalkov,A. V. Silhanek		
154349	PRB088184508	impurity phase: rhombohedral Bi(0.5%). RRR = 15.3. C(T) has anomaly at 2K maybe FM origin. [gamma] estimated asuming (dC/gamma*Tc) = 1.43(BCS)	NiBi3	Bi3Ni1	Bi	3	Ni	1																				3	2013																										AB3	3	CaLiSi2	Pnma		A	8.877	4.097	11.48												K	3.9		4				3.95											Oe	M-H curve				120			1.8	T	M-H curve				0.35			1.8																												mJ/mol.K2	9	SP, BCS																																				Bi(4N),Ni(4N)		mixture(Bi:Ni = 9:1) - sealed in quartz ampoule - heat to 1100C(4h) - keep(1100C,100h) - cool to 300C within 300h - keep(100h) - remove Bi-flux.					Superconductivity and magnetism on flux-grown single crystals of NiBi3			Laboratorio de Bajas Temperaturas, Departamento de Fsica de la Materia Condensada, Instituto Nicolas Cabrera and Condensed Matter Physics Center (IFIMAC), Universidad Autonoma de Madrid, E-28049 Madrid, Spain	Phys.Rev.B, 88(2013)184508	B. Silva,R. F. Luccas,N. M. Nemes,J. Hanko,M. R. Osorio,P. Kulkarni,F. Mompean,M. Garcia-Hernandez,M. A. Ramos,S. Vieira,H. Suderow		
154350	PRB088195134		Ce(Co,Ru)In5	Ce1Co0.9Ru0.1In5	Ce	1	Co	0.9	Ru	0.1	In	5																3	2013																										ABC5		HoCoG5			A	4.6143		7.5529												K		2.25					2.25	MTC154350																																																																																															self-flux method in In solvent					Hole doping effect on superconductivity in Ce(Co1-xRux)In5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 88(2013)195134	M. N. Ou,K. Gofryk,R. E. Baumbach,S. S. Stoyko,J. D. Thompson,J. M. Lawrence,E. D. Bauer,F. Ronning,A. Mar,Y. Y. Chen		
154351	PRB088195134	Ru-content x = 0.055 in CeCo1-xRuxIn5 By EDX	Ce(Co,Ru)In5	Ce1Co0.8Ru0.2In5	Ce	1	Co	0.8	Ru	0.2	In	5																3	2013																										ABC5		HoCoG5			A	4.6195		7.5596												K		2.18					2.18																																																																																																self-flux method in In solvent					Hole doping effect on superconductivity in Ce(Co1-xRux)In5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 88(2013)195134	M. N. Ou,K. Gofryk,R. E. Baumbach,S. S. Stoyko,J. D. Thompson,J. M. Lawrence,E. D. Bauer,F. Ronning,A. Mar,Y. Y. Chen		
154352	PRB088195134	Ru-content x = 0.116 in CeCo1-xRuxIn5 By EDX	Ce(Co,Ru)In5	Ce1Co0.7Ru0.3In5	Ce	1	Co	0.7	Ru	0.3	In	5																3	2013																										ABC5		HoCoG5			A	4.619		7.5607												K		2.13					2.13																																																																																																self-flux method in In solvent					Hole doping effect on superconductivity in Ce(Co1-xRux)In5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 88(2013)195134	M. N. Ou,K. Gofryk,R. E. Baumbach,S. S. Stoyko,J. D. Thompson,J. M. Lawrence,E. D. Bauer,F. Ronning,A. Mar,Y. Y. Chen		
154353	PRB088195134	Ru-content x = 0.097 in CeCo1-xRuxIn5 By EDX	Ce(Co,Ru)In5	Ce1Co0.6Ru0.4In5	Ce	1	Co	0.6	Ru	0.4	In	5																3	2013																										ABC5		HoCoG5			A	4.6205		7.5606												K		1.8					1.8																																																																																																self-flux method in In solvent					Hole doping effect on superconductivity in Ce(Co1-xRux)In5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 88(2013)195134	M. N. Ou,K. Gofryk,R. E. Baumbach,S. S. Stoyko,J. D. Thompson,J. M. Lawrence,E. D. Bauer,F. Ronning,A. Mar,Y. Y. Chen		
154354	PRB088195134	Ru-content x = 0.097 in CeCo1-xRuxIn5 By EDX	Ce(Co,Ru)In5	Ce1Co0.5Ru0.5In5	Ce	1	Co	0.5	Ru	0.5	In	5																3	2013																										ABC5		HoCoG5			A	4.6184		7.5606												K		1.77					1.77																																																																																																self-flux method in In solvent					Hole doping effect on superconductivity in Ce(Co1-xRux)In5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 88(2013)195134	M. N. Ou,K. Gofryk,R. E. Baumbach,S. S. Stoyko,J. D. Thompson,J. M. Lawrence,E. D. Bauer,F. Ronning,A. Mar,Y. Y. Chen		
154355	PRB088224510	P-induced SC. Pcr = 2.5 GPa. RRR = 7. RH(31K) = -2 E-9 m3/C, where RH = (dRxy/dB) at B=0	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2																	Fe-122	K			31		0		31																				T	RES(R=0.5Rn)													MHC154355																																																			m3/C						MRH154355					Bridgman method					Pressure-induced superconductivity in EuFe2As2 without a quantum critical point: Magnetotransport and upper critical field measurements under high pressure			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan	Phys.Rev.B, 88(2013)224510	Nobuyuki Kurita,Motoi Kimata,Kota Kodama,Atsushi Harada,Megumi Tomita,Hiroyuki S. Suzuki,Takehiko Matsumoto,Keizo Murata,Shinya Uji,Taichi Terashima		
154356	PRB088224515	[penet] measured by muon-SR. penet(T) fitting shows two gap model is better: the lower d=0.09 meV (2d/kTc = 0.44), the higher(in DB) d=0.93 meV (2d/kTc = 4.76)	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2013																																														K	4.6		4.8				4.7																				T	RES(R=0.9Rn). charged boson model	1.53												HC154356		A	from Hc2	120			nm	muon-SR	861			meV	0.93	4.76	16																						mOhm.cm							2																		solid state reaction					Low superfluid density and possible multigap superconductivity in the BiS2-based layered superconductor Bi4O4S3			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 88(2013)224515	P. K. Biswas,A. Amato,C. Baines,R. Khasanov,H. Luetkens,Hechang Lei,C. Petrovic,E. Morenzoni		
154357	PRB089014512	FM layers ordered AFM along c-axis. The behaviou of Eu moment upon field wre investigated. (dC) = 350 mJ/mol.K, but [gamma] not determined because of magnetic effect.	EuFe2(As,P)2	Eu1Fe2As1.7P0.3	Eu	1	Fe	2	As	1.7	P	0.3																3	2014								19																		AB2C2		ThCr2Si2																	Fe-122	K				25			25																																																																																																FeAs-flux method					Coexistence of superconductivity and ferromagnetism in P-doped EuFe2As2			Julich Centre for Neutron Science JCNS and Peter Grunberg Institut PGI, JARA-FIT, Forschungszentrum Julich GmbH, D-52425 Julich, Germany	Phys.Rev.B, 89(2014)014512	S. Nandi,W. T. Jin,Y. Xiao,Y. Su,S. Price,D. K. Shukla,J. Strempfer,H. S. Jeevan,P. Gegenwart,Th. Bruckel		
154358	PRB089020507	LiFeO2(anti-PbO type)-intercalated Fe2Se2. annealed sample. Tc(P) shows T-dependence of Tc(SUS-on).	LiFeO2Fe2Se2	Li1Fe3Se2O2	Li	1	Fe	3	Se	2															O	2		1	2014																													P4/nmm	129	A	3.7926		9.2845											LiFeO2-intercalated Fe-122	K	20		42	42.8			42.8	MTC154358		K/GPa	-5.16							Oe	M-H curve				300		5																																																																														0.012?0.02 mol selenourea, 0.0075 mol Fe powder and 12 g LiOH H2O were put into a Teflon-lined steel autoclave (50 mL) and mixed together with 10 ml de ionized water and heated (160, 3?10 days).					Superconductivity in LiFeO2Fe2Se2 with anti-PbO-type spacer layers			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 89(2014)020507	X. F. Lu,N. Z. Wang,G. H. Zhang,X. G. Luo,Z. M. Ma,B. Lei,F. Q. Huang,X. H. Chen		
154359	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used.. Tc(SP) = 7.92 K. (gap/Tc) = 3.46 from SP(electron)- data-fitting.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2014					myu-B/R	3.68	-0.7																			AB4C12		skutterudite																		K		7.92					7.92																																																	14							mJ/mol.K2	47.6	SP	193	SP											uOhm.cm							1.88																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154360	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used.. Tc(SP) = 5.29 K. (gap/Tc) = 2.97 from SP(electron)- data-fitting.	(Pr,Ce)Pt4Ge12	Pr0.95Ce0.05Pt4Ge12	Pr	0.95	Ce	0.05	Pt	4	Ge	12																1	2014					myu-B/R	3.58	-18.5																			AB4C12		skutterudite			A	8.612														K		5.75		5.58			5.75	MTC154360																																																14							mJ/mol.K2	45.6	SP	192	SP											uOhm.cm							8.83																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154361	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used.. Tc(SP) = 4.76 K. (gap/Tc) = 3.49 from SP(electron)- data-fitting.	(Pr,Ce)Pt4Ge12	Pr0.94Ce0.06Pt4Ge12	Pr	0.94	Ce	0.06	Pt	4	Ge	12																1	2014							-51.9																			AB4C12		skutterudite			A	8.6117														K								MTC154360																																																14							mJ/mol.K2	53.7	SP	192	SP																																		Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154362	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used.. Tc(SP) = 4.37 K. (gap/Tc) = 3.38 from SP(electron)- data-fitting.	(Pr,Ce)Pt4Ge12	Pr0.93Ce0.07Pt4Ge12	Pr	0.93	Ce	0.07	Pt	4	Ge	12																1	2014					myu-B/R	3.57	-18.5																			AB4C12		skutterudite																		K		5.52		4.953			5.52	MTC154360																																																14							mJ/mol.K2	59.4	SP	195	SP											uOhm.cm							7.64																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154363	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..  (gap/Tc) = 3.47 from SP(electron)- data-fitting.	(Pr,Ce)Pt4Ge12	Pr0.915Ce0.085Pt4Ge12	Pr	0.915	Ce	0.085	Pt	4	Ge	12																1	2014					myu-B/R	3.62	-16.1																			AB4C12		skutterudite			A	8.6104														K		4.61		4.1			4.61																																																	14							mJ/mol.K2	58.9	SP	194	SP																																		Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154364	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used.. Tc(SP) = 3.13 K. (gap/Tc) = 2.92 from SP(electron)- data-fitting.	(Pr,Ce)Pt4Ge12	Pr0.9Ce0.1Pt4Ge12	Pr	0.9	Ce	0.1	Pt	4	Ge	12																1	2014					myu-B/R	3.63	-22.1																			AB4C12		skutterudite																		K		4.11					4.11																																																	14							mJ/mol.K2	53.7	SP	196	SP											uOhm.cm							9.67																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154365	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.86Ce0.14Pt4Ge12	Pr	0.86	Ce	0.14	Pt	4	Ge	12																1	2014					myu-B/R	3.62	-19.3																			AB4C12		skutterudite																		K		3.43		3.121			3.43																																																								mJ/mol.K2	82.1	SP	200	SP											uOhm.cm							17.6																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154366	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.8Ce0.2Pt4Ge12	Pr	0.8	Ce	0.2	Pt	4	Ge	12																1	2014					myu-B/R	3.61	-36.3																			AB4C12		skutterudite			A	8.612														K		1.767		2			1.767																																																								mJ/mol.K2	86.6	SP	209	SP											uOhm.cm							14.4																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154367	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.75Ce0.25Pt4Ge12	Pr	0.75	Ce	0.25	Pt	4	Ge	12																1	2014					myu-B/R	3.39	-8.1																			AB4C12		skutterudite			A	8.6124														K		1.015					1.015																																																								mJ/mol.K2	91.5	SP	194	SP											uOhm.cm							31.1																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154368	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.7Ce0.3Pt4Ge12	Pr	0.7	Ce	0.3	Pt	4	Ge	12																1	2014					myu-B/R	3.5	-41.2																			AB4C12		skutterudite																		K																																																															mJ/mol.K2	109.4	SP	197	SP											uOhm.cm							22.7																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154369	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.65Ce0.35Pt4Ge12	Pr	0.65	Ce	0.35	Pt	4	Ge	12																1	2014					myu-B/R	3.37	-30.8																			AB4C12		skutterudite																		K		0.29					0.29																																																								mJ/mol.K2	95.3	SP	2.9	SP											uOhm.cm							38.4																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154370	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.6Ce0.4Pt4Ge12	Pr	0.6	Ce	0.4	Pt	4	Ge	12																1	2014					myu-B/R	3.23	-25.3																			AB4C12		skutterudite			A	8.6127														K					0.05																																																										mJ/mol.K2	98.3	SP	204	SP											uOhm.cm							31																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154371	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.55Ce0.45Pt4Ge12	Pr	0.55	Ce	0.45	Pt	4	Ge	12																1	2014					myu-B/R	3.22	-35.3																			AB4C12		skutterudite			A	8.6133														K					0.05																																																										mJ/mol.K2	102.7	SP	209	SP																																		Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154372	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.5Ce0.5Pt4Ge12	Pr	0.5	Ce	0.5	Pt	4	Ge	12																1	2014					myu-B/R	3.19	-39.5																			AB4C12		skutterudite			A	8.6136														K					0.05																																																										mJ/mol.K2	119.1	SP	215	SP											uOhm.cm							36.9																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154373	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.375Ce0.625Pt4Ge12	Pr	0.375	Ce	0.625	Pt	4	Ge	12																1	2014					myu-B/R	3.05	-31.7																			AB4C12		skutterudite			A	8.6135														K					0.05																																																										mJ/mol.K2	113.8	SP	213	SP																																		Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154374	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.25Ce0.75Pt4Ge12	Pr	0.25	Ce	0.75	Pt	4	Ge	12																1	2014					myu-B/R	2.94	-44.1																			AB4C12		skutterudite			A	8.6149														K					0.05																																																										mJ/mol.K2	113.8	SP	213	SP											uOhm.cm							44.3																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154375	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	(Pr,Ce)Pt4Ge12	Pr0.125Ce0.875Pt4Ge12	Pr	0.125	Ce	0.875	Pt	4	Ge	12																1	2014					myu-B/R	2.63	-41.1																			AB4C12		skutterudite			A	8.6155														K					0.05																																																										mJ/mol.K2	113.8	SP	219	SP																																		Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154376	PRB089035145	R = R0+A*T^n, Curie-Weis law, Debye-model, are used..	CePt4Ge12	Ce1Pt4Ge12	Ce	1	Pt	4	Ge	12																		1	2014					myu-B/R	2.69	-84																			AB4C12		skutterudite			A	8.6149														K					0.05																																																										mJ/mol.K2	86.2	SP	217	SP											uOhm.cm							13.2																Ce(rod),Pr(3N),Pt(6N),Ge(6N)		arc-melting - ANN(800C,336h, in sealed quartz tube)					Probing the superconductivity of PrPt4Ge12 through Ce substitution			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 89(2014)035145	K. Huang,L. Shu,I. K. Lum,B. D. White,M. Janoschek,D. Yazici,J. J. Hamlin,D. A. Zocco,P.-C. Ho,R. E. Baumbach,M. B. Maple		
154377	PRB089054512	Ca11Bi9.88 by XRD analysis. RRR = 120. H-direction not shown.	Ca11Bi10	Ca10Bi9.88	Ca	10	Bi	9.88																				3	2014									6.175																	A11B10	2	Ho10Ge11	I4/mmm		A	12.2842		17.866												K	1.95		2.2				2.075										90										Oe	RES(onset), GL fitting	172												MHC154377																																					uOhm.cm												129.4		m3/C		0.0000000151			9		n/cm3	6500000000000000000			self-flux method using excess Bi. mixture(Ca:Bi = 1:5) - loaded(Nb-tube and weld(Ar)) - heat to 1373 K 10h - hold(100h) - slow cool to 773K (10K/h)					Superconductivity in the intermetallic pnictide compound Ca11Bi10-x			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B, 89(2014)054512	Mihai Sturza,Fei Han,Christos D. Malliakas,Duck Young Chung,Helmut Claus,Mercouri G. Kanatzidis		
154378	PRL111207001	RRR = 103. (Rc/Rab) = 1.57 (at RT). SP heat (beta) = 1.65 mJ/mol.K4, (delta) = 0.135 mJ/mol.K6. Two gaps from SP, the lower (d1) = 0.84 kTc, higher (d2) = 2.01 kTc(in DB)	TlNi2Se2	Tl1Ni2Se2	Tl	1	Ni	2	Se	2																		3	2013	emu/mol	0.0006064																								AB2C2	2	ThCr2Si2	I4/mmm		A	3.87		13.435											Fe-122	K	3.7					0.05	3.7											Oe	M-H curve			170					T	RES(R=0.5Rn), GL-fitting			0.802										MHC154378		A	from Hc2		203									4.02	14							mJ/mol.K2	40	SP	175	SP											uOhm.cm							0.615					68.69	108.1												self-flux method. mixture(Tl:Ni:Se = 1:2:2) - alumina crucible in sealed quartz tube - heat(950C,12h) - cool to700C (6C/h) - FC to RT					Multiband Superconductivity of Heavy Electrons in a TlNi2Se2 Single Crystal			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.Lett., 111(2013)207001	Hangdong Wang,Chiheng Dong,Qianhui Mao,Rajwali Khan,Xi Zhou,Chenxia Li,Bin Chen,Jinhu Yang,Qiping Su,Minghu Fang		
154379	SSC1570021	not SC.	LaOBiS2	La1Bi1S2O1	La	1	Bi	1	S	2															O	1			2013																										ABCD2	2	CeOBiS2	P4/nmm		A	4.066		13.862											ZrCuSiAs-type	K					1.8																																																																																																La,Bi,S,LaF3,La2O3		solid state reaction. mixture - pellet - sealed in quartz ampoule - heat(800C,12h) - cool to RT witin 6h					Appearance of superconductivity in layered LaO0.5F0.5BiS2			Quantum Phenomena and Applications Division, National  Physical Laboratory (CSIR), Dr.K.S.Krishnan Road, New Delhi 110012, India	Solid State Commun., 157(2013)21	V.P.S. Awana,AnujKumar,RajveerJha,ShivaKumarSingh,AnandPal,Shruti,J.Saha,S.Patnaik		
154380	SSC1570021	Hall coeff. RH(10K) = 5.04 E-8 m3/C. Carrier n(10K) = 1.24 E+20 /cm3	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2	2	CeOBiS2	P4/nmm		A	4.069		13.366											ZrCuSiAs-type	K	2.4		2.7	2.7			2.7										6										T	RES(R=0.9Rn), WHH	1.9							T/K	RES(R=0.9Rn)	1			MHC154380		A	from Hc2	130																																																								La,Bi,S,LaF3,La2O3		solid state reaction. mixture - pellet - sealed in quartz ampoule - heat(800C,12h) - cool to RT witin 6h					Appearance of superconductivity in layered LaO0.5F0.5BiS2			Quantum Phenomena and Applications Division, National  Physical Laboratory (CSIR), Dr.K.S.Krishnan Road, New Delhi 110012, India	Solid State Commun., 157(2013)21	V.P.S. Awana,AnujKumar,RajveerJha,ShivaKumarSingh,AnandPal,Shruti,J.Saha,S.Patnaik		
154381	SSC1590026	resistive transition foe P < 20 GPa.	Rb0.19WO3	Rb0.19W1O3	Rb	0.19	W	1																	O	3			2013																											3	bronze																		K		5.5					5.5	MTC154381																																																																																															The samples obtained by acid etching stoichiometric single crystal Rb0.33WO3.					Effect of pressure on the superconductivity of Rb0.19WO3			Institut Neel, Centre Nationale de la Recherche Scientifique - Universite Joseph Fourier, BP166 Cedex 09, 38042 Grenoble, France	Solid State Commun., 159(2013)26	M. Nunez-Regueiro,D.C.Freitas,R.Brusetti,J.Marcus		
154382	SSC1720001		Fe(Se,Br)	Fe1Se0.82Br0.18	Fe	1	Se	0.82	Br	0.18																			2013																										AB	2	PbO	P4/nmm		A	3.77		5.518											beta-FeSe phase	K				5			5										40																																																																																						mixture - pellet - sealed in quartz tube - heat(680C,16h) - reground - pellet - ANN(400C,4d) - q to ice water					Bromine-doping dependence of crystal structure and superconductivity in FeSe1-xBrx			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	Solid State Commun., 172(2013)1	K.J. Syu,Y.T.Shen,S.C.Chen,W.H.Lee		
154383	SSC1720001		Fe(Se,Br)	Fe1Se0.8Br0.2	Fe	1	Se	0.8	Br	0.2																			2013																										AB	2	PbO	P4/nmm		A	3.774		5.528											beta-FeSe phase	K				5			5										40																																																																																						mixture - pellet - sealed in quartz tube - heat(680C,16h) - reground - pellet - ANN(400C,4d) - q to ice water					Bromine-doping dependence of crystal structure and superconductivity in FeSe1-xBrx			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	Solid State Commun., 172(2013)1	K.J. Syu,Y.T.Shen,S.C.Chen,W.H.Lee		
154384	SSC1720001	small SC volume fraction	Fe(Se,Br)	Fe1Se0.7Br0.3	Fe	1	Se	0.7	Br	0.3																			2013																										AB	2	PbO	P4/nmm		A	3.773		5.528											beta-FeSe phase	K				5			5																																																																																																mixture - pellet - sealed in quartz tube - heat(680C,16h) - reground - pellet - ANN(400C,4d) - q to ice water					Bromine-doping dependence of crystal structure and superconductivity in FeSe1-xBrx			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	Solid State Commun., 172(2013)1	K.J. Syu,Y.T.Shen,S.C.Chen,W.H.Lee		
154385	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.23 by EPMA. R not to zero at 2 K.	La(O,F)BiS2	La1Bi1S2F0.3O0.77	La	1	Bi	1	S	2	F	0.3													O	0.7	0.77	3	2014																										ABCD2		CeOBiS2			A			13.57												K			3.1				3.1																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154386	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.46 by EPMA.	La(O,F)BiS2	La1Bi1S2F0.7O0.54	La	1	Bi	1	S	2	F	0.7													O	0.3	0.54	3	2014																										ABCD2		CeOBiS2			A			13.37												K			4.46				4.46																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154387	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.46 by EPMA.	La(O,F)BiS2	La1Bi1S2F0.9O0.54	La	1	Bi	1	S	2	F	0.9													O	0.1	0.54	3	2014																										ABCD2		CeOBiS2			A			13.39												K			4.55				4.55																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154388	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.53 by EPMA.	Ce(O,F)BiS2	Ce1Bi1S2F0.3O0.47	Ce	1	Bi	1	S	2	F	0.3													O	0.7	0.47	3	2014																										ABCD2		CeOBiS2			A			13.54												K					2																																																																																																R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154389	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.65 by EPMA.	Ce(O,F)BiS2	Ce1Bi1S2F0.7O0.35	Ce	1	Bi	1	S	2	F	0.7													O	0.3	0.35	3	2014																										ABCD2		CeOBiS2			A			13.39												K			4				4																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154390	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.66 by EPMA.	Ce(O,F)BiS2	Ce1Bi1S2F0.9O0.34	Ce	1	Bi	1	S	2	F	0.9													O	0.1	0.34	3	2014																										ABCD2		CeOBiS2			A			13.4												K			3.51				3.51																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154391	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.26 by EPMA.	Nd(O,F)BiS2	Nd1Bi1S2F0.3O0.74	Nd	1	Bi	1	S	2	F	0.3													O	0.7	0.74	3	2014																										ABCD2		CeOBiS2			A			13.56												K			3.51				3.51																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154392	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.37 by EPMA.	Nd(O,F)BiS2	Nd1Bi1S2F0.7O0.63	Nd	1	Bi	1	S	2	F	0.7													O	0.3	0.63	3	2014																										ABCD2		CeOBiS2			A			13.43												K			5.24				5.24																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154393	SSC1780033	F-content x in LaO1-xFx)BiS2 = 0.38 by EPMA.	Nd(O,F)BiS2	Nd1Bi1S2F0.9O0.62	Nd	1	Bi	1	S	2	F	0.9													O	0.1	0.62	3	2014																										ABCD2		CeOBiS2			A			13.01												K			5.44				5.44																																																																																														R2S2,Bi,Bi2S2,Bi2O3,BiF3,CsCl,KCl		CsCl/KCl flux method. mixture - heat(800C,10h) - slow cool to 600C (1C/h) - FC to RT					Growth and superconducting properties of F-substituted = ROBiS2 (R = La, Ce, Nd) singlecrystals			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 178(2014)33	Masanori Nagao,Akira Miura,Satoshi Demura,Keita Deguchi,Satoshi Watauchi,Takahiro Takei,YoshihikoTakano,Nobuhiro Kumada,Isao Tanaka		
154394	PRL112047005	inhomogeneity: gap=15 meV(2/3 volume) , gap=30 meV(1/3 volume) in the normal states by STM. SC(45K) comes from clover like defect around Pr atom.	(Ca,Pr)Fe2As2	Ca0.86Pr0.14Fe2As2	Ca	0.86	Pr	0.14	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																		K	20		45				32.5										5																																				meV	12	6.3	11							mJ/mol.K2	50																																							FeAs flux method					Local Inhomogeneity and Filamentary Superconductivity in Pr-Doped CaFe2As2			Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.Lett., 112(2014)047005	Krzysztof Gofryk,Minghu Pan,Claudia Cantoni,Bayrammurad Saparov,Jonathan E. Mitchell,Athena S. Sefat		
154395	PRL112067002	C<e> = A*exp(-d0/T) + gamma-0*T: d0 = 0.39 K and gamma-0 = 0.028 mJ/mol for T<0.15 K.. Hc2 measured for H//[100]	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2014																										AB2C2																				K		0.6					0.6																																		MHC154395																																																														See Phys.Status Solidi B, 247(2010)614					Multiband Superconductivity with Unexpected Deficiency of Nodal Quasiparticles in CeCu2Si2			Institute for Solid State Physics (ISSP), University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 112(2014)067002	Shunichiro Kittaka,Yuya Aoki,Yasuyuki Shimura,Toshiro Sakakibara,Silvia Seiro,Christoph Geibel,Frank Steglich,Hiroaki Ikeda,Kazushige Machida		
154400	PRB087224510	RRR = 3. SP-heat:(beta=0.463 mJ/mol.K4, (delta)=6.8 mJ/mol.K6. Debye-T(RES) = 135K. DOS(FL) = 2.76 states/eV.f.u. (dC/gamma*Tc) = 1.14. GL = 11.7 e-ph = 0.474	CaPd2As2	Ca1Pd2As2	Ca	1	Pd	2	As	2																		3	2013									7.23																	AB2C2	2	ThCr2Si2	I4/mmm		A	4.2824		10.088												K		1.27	1.8				1.27											Oe	GL	14							T	RES, SP	0.157												MHC154400		A	from Hc2	458			A		2100					3.16	14				MSP154400	mJ/mol.K	9.4	mJ/mol.K2	6.52	SP	276	SP											uOhm.cm							43																Ca(3N),Pd(4N),As(7N),Sr(3N),Ba(4N)		flux method(PdAs flux). Ca(or Sr, Ba):PdAs flux = 1:4(mol ratio). alumina crucible - sealed in fused silica tube - heat to 1100C (60-80 C/h) - keep(12h) - cool to 800C (2.5 C/h)					Superconducting and normal-state properties of APd2As2 (A=Ca, Sr, Ba) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)224510	V. K. Anand,H. Kim,M. A. Tanatar,R. Prozorov,D. C. Johnston		
154401	PRB087224510	RRR = 8. SP-heat:(beta=0.369 mJ/mol.K4, (delta)=3.7 mJ/mol.K6. Debye-T(RES) = 170K. DOS(FL) = 2.73 states/eV.f.u. (dC/gamma*Tc) = 1.03	SrPd2As2	Sr1Pd2As2	Sr	1	Pd	2	As	2																		3	2013									7.682																	AB2C2	2	ThCr2Si2	I4/mmm		A	4.3759		10.1671												K		0.92	1.5				0.92											Oe	SP	11.7							T	SP	0.07												MHC154401		A	from Hc2	690			A		1700					3	14				MSP154401			mJ/mol.K2	6.43	SP	298	SP											uOhm.cm							7.57																Ca(3N),Pd(4N),As(7N),Sr(3N),Ba(4N)		flux method(PdAs flux). Ca(or Sr, Ba):PdAs flux = 1:4(mol ratio). alumina crucible - sealed in fused silica tube - heat to 1100C (60-80 C/h) - keep(12h) - cool to 800C (2.5 C/h)					Superconducting and normal-state properties of APd2As2 (A=Ca, Sr, Ba) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)224510	V. K. Anand,H. Kim,M. A. Tanatar,R. Prozorov,D. C. Johnston		
154402	PRB087224510	RRR = 25. not bulk SC. SP-heat:(beta=0.638 mJ/mol.K4, (delta)=4.0 mJ/mol.K6. Debye-T(RES) = 114K. DOS(FL) = 2.03 states/eV.f.u.	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2013									7.648																	AB2C2	2	CeMg2Si2	P4/mmm		A	4.3438		5.7536												K			2				2																																																								mJ/mol.K2	4.79	SP	248	SP											uOhm.cm							1.02																Ca(3N),Pd(4N),As(7N),Sr(3N),Ba(4N)		flux method(PdAs flux). Ca(or Sr, Ba):PdAs flux = 1:4(mol ratio). alumina crucible - sealed in fused silica tube - heat to 1100C (60-80 C/h) - keep(12h) - cool to 800C (2.5 C/h)					Superconducting and normal-state properties of APd2As2 (A=Ca, Sr, Ba) single crystals			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 87(2013)224510	V. K. Anand,H. Kim,M. A. Tanatar,R. Prozorov,D. C. Johnston		
154403	SST022014003	Gap measured by Point Contact Andreev Reflection (PCAR ). Tc(PCAR=45 K. Two gaps: d1=5 meV (2d/kTc = 2.6) and d2 = 11 meV (=5.7)	NdFeAs)O,F)	Nd1Fe1As1F0.1O0.9	Nd	1	Fe	1	As	1	F	0.1													O	0.9		3	2009																										ABCD		oxypnictide																	Fe-1111	K			51				51																																														meV	11	5.7	1																																													Nd2O3,NdF3,Nd		High-P synthesis. mixture - pellet - BN crucible - P=3.4 GPa heat to 1300-1400C - hold(8h) - Q to RT					Possible two-gap superconductivity in NdFeAsO0.9F0.1 probed by point-contact Andreev-reflection spectroscopy			Centre of Low Temperature Physics, IEP Slovak Academy of Sciences and P J Safarik University, Watsonova 47, SK-04001 Kosice, Slovakia	Supercond.Sci.Technol., 22(2009)014003	P Samuely,P Szab,Z Pribulova,M E Tillman,S L Bud'ko2,P C Canfield		
154404	SST023054009	Gap measured by Point Contact Andreev Reflection (PCAR ), analyzed using single gap BTK model. Surface is sensitive to air exposure.	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2010																										AB2C2		ThCr2Si2																	Fe-122	K		32					32																																														meV	3.5	2.5	1																																															FeAs flux method					Point-contact spectroscopic studies on normal and superconducting AFe2As2-type iron pnictide single crystals			Department of Physics and Fredrick Seitz Materials Research Laboratory, University of Illinois at Urbana-Champaign, IL 61801, USA	Supercond.Sci.Technol., 23(2010)054009	Xin Lu,WKPark,HQYuan,G F Chen,GLLuo,NLWang,A S Sefat,M A McGuire,R Jin,B C Sales,D Mandrus,J Gillett,Suchitra E Sebastian,L H Greene		
154405	SST027025005	beta-Po type structure	AuxSb1-2xTex	Au0.05Sb0.9Te0.05	Au	0.05	Sb	0.9	Te	0.05																		1	2014																																													beta-Po type, rhombohedral	K					2			MTC154405																																																																																													Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154406	SST027025005	beta-Po type structure	AuxSb1-2xTex	Au0.075Sb0.85Te0.075	Au	0.075	Sb	0.85	Te	0.075																		1	2014																																													beta-Po type, rhombohedral	K				4.5			4.5																																																																																														Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154407	SST027025005		AuxSb1-2xTex	Au0.1Sb0.8Te0.1	Au	0.1	Sb	0.8	Te	0.1																		1	2014																											1				A	3.027													alpha-Po type, simple cubic	K				6			6																																																																																														Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154408	SST027025005		AuxSb1-2xTex	Au0.125Sb0.75Te0.125	Au	0.125	Sb	0.75	Te	0.125																		1	2014																											1				A	3.016													alpha-Po type, simple cubic	K				6.7			6.7																				T	SUS, extrapolation	1.17												MHC154408																																																												Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154409	SST027025005	multi-phase alpha-Po type structure.	AuxSb1-2xTex	Au0.2Sb0.6Te0.2	Au	0.2	Sb	0.6	Te	0.2																		1	2014																											1																		alpha-Po type, simple cubic	K				6.6			6.6																																																																																														Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154410	SST027025005		AuxSb1-x	Au0.1Sb0.9	Au	0.1	Sb	0.9																				1	2014																											1																		alpha-Po type, simple cubic	K				8			8																																																																																														Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154411	SST027025005		AuxSb1-x	Au0.1Sb0.9	Au	0.1	Sb	0.9																				1	2014																											1																		alpha-Po type, simple cubic	K				7			7																																																																																														Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154412	SST027025005		AuxSb1-x	Au0.15Sb0.85	Au	0.15	Sb	0.85																				1	2014																											1				A	3.0012													alpha-Po type, simple cubic	K				8.1			8.1	MTC154412																			T	SUS, extrapolation	1.36												MHC154412																																																												Sb(4N),Te(5N),AuSb2		mixture - pellet - BN vessel - heat(800C,25min, P=3.4 GPa) - cool to 200C within 10s					Superconductivity at the highest transition temperature of 8.1 K in a simple cubic AuxSb1-x-yTey alloy system synthesized under high pressure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)025005	A Iyo1,2,K Hira,K Tokiwa,Y Tanaka,I Hase,T Yanagisawa,N Takeshita,K Kihou,C H Lee,P M Shirage,P Raychaudhuri,H Eisaki		
154413	SST027072001	RRR = 27.3. e-ph = 1.0 using Debye-T = 75.9K( from R(T) analysis).	Ba2Bi3	Ba2Bi3	Ba	2	Bi	3																				1	2014																										A2B3			Immm	71	A	4.813	7.994	9.971												K			4.4			0.15	4.4	MTC154413		T/GPa	-0.56																T	RES(R=0.5Rn), extrapolation	1.23												MHC154413		A	from Hc2	164																					75.9	R(T) analysis											uOhm.cm							22.7				619														mixture( with 25%-excess Ba) - pellet - (solid state reaction) - BN crucible - heat(800C,1h, P= 1 GPa)					Superconductivity at 4.4 K in Ba2Bi3			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 27(2014)072001	A Iyo,Y Yanagi,S Ishida,K Oka,Y Yoshida,K Kihou,C H Lee,H Kito,N Takeshita,I Hase,T Yanagisawa,T Kinjo,T Nishio,H Eisaki		
154420	PRL101147003	gap measured by ARPES. nodeless SC gap observed. gap size calculated from gap=15 meV.	NdFeAs(O,F)	Nd1Fe1As1F0.1O0.9	Nd	1	Fe	1	As	1	F	0.1													O	0.9		3	2008																										ABCD		oxypnictide																		K		53					53																																														meV	15	6.58	12																																													NdFe3As3,Nd2O3,NdF3,Nd		high-P synthesis. mixture - pellet - BN crucible - heat to 1350-1400C (within 1h) - hold(8h, P=3.3 GPa) - Q to RT					Momentum Dependence of the Superconducting Gap in NdFeAsO0:9F0:1 Single Crystals Measured by Angle Resolved Photoemission Spectroscopy			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 101(2008)147003	Takeshi Kondo,A. F. Santander-Syro,O. Copie,Chang Liu,M. E. Tillman,E. D. Mun,J. Schmalian,S. L. Bud'ko,M. A. Tanatar,P. C. Canfield,A. Kaminski		
154421	ACS13416520	T<CDW>,T<SDW> = 54 K.	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1			2012																										ABC2D2		oxypnictide	P4/mmm		A	4.1196		8.0951											Ti-oxypnictide, BaTi2As2o	K					2																																																																																																BaO,BaO2,Na2O,Na2O2,Ti,Sb		mixture - weld in Nb container - heat(900C,3d) - cool to 200C(2C/min) - reground - SIN(900C,3d)					Ba1-xNaxTi2Sb2O (0.0<=x<=0.33): A Layered Titanium-Based Pnictide Oxide Superconductor			Department of Chemistry,  University of Houston, Houston, Texas 77204, United States	J.Am.Chem.Soc., 134(2012)16520	Phuong Doan,Melissa Gooch,Zhongjia Tang,Bernd Lorenz,Angela Moller,Joshua Tapp,Paul C. W. Chu,Arnold M. Guloy		
154422	ACS13416520	T<CDW>,T<SDW> = 45.3 K.	(Ba,Na)Ti2Sb2O	Ba0.95Na0.05Ti2Sb2O1	Ba	0.95	Na	0.05	Ti	2	Sb	2													O	1			2012																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide, CeCr2Si2C	K				3.14			3.14																																																																																														BaO,BaO2,Na2O,Na2O2,Ti,Sb		mixture - weld in Nb container - heat(900C,3d) - cool to 200C(2C/min) - reground - SIN(900C,3d)					Ba1-xNaxTi2Sb2O (0.0<=x<=0.33): A Layered Titanium-Based Pnictide Oxide Superconductor			Department of Chemistry,  University of Houston, Houston, Texas 77204, United States	J.Am.Chem.Soc., 134(2012)16520	Phuong Doan,Melissa Gooch,Zhongjia Tang,Bernd Lorenz,Angela Moller,Joshua Tapp,Paul C. W. Chu,Arnold M. Guloy		
154423	ACS13416520	T<CDW>,T<SDW> = 40.8 K.	(Ba,Na)Ti2Sb2O	Ba0.9Na0.1Ti2Sb2O1	Ba	0.9	Na	0.1	Ti	2	Sb	2													O	1			2012																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide, CeCr2Si2C	K				4.24			4.24	MTC154423																																																																																													BaO,BaO2,Na2O,Na2O2,Ti,Sb		mixture - weld in Nb container - heat(900C,3d) - cool to 200C(2C/min) - reground - SIN(900C,3d)					Ba1-xNaxTi2Sb2O (0.0<=x<=0.33): A Layered Titanium-Based Pnictide Oxide Superconductor			Department of Chemistry,  University of Houston, Houston, Texas 77204, United States	J.Am.Chem.Soc., 134(2012)16520	Phuong Doan,Melissa Gooch,Zhongjia Tang,Bernd Lorenz,Angela Moller,Joshua Tapp,Paul C. W. Chu,Arnold M. Guloy		
154424	ACS13416520	T<CDW>,T<SDW> = 34 K. (dC/Tc) = 8 mJ/mol.K2	(Ba,Na)Ti2Sb2O	Ba0.85Na0.15Ti2Sb2O1	Ba	0.85	Na	0.15	Ti	2	Sb	2													O	1			2012																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide, CeCr2Si2C	K				5.22			5.22	MTC154423																																																				MSP154424																																									BaO,BaO2,Na2O,Na2O2,Ti,Sb		mixture - weld in Nb container - heat(900C,3d) - cool to 200C(2C/min) - reground - SIN(900C,3d)					Ba1-xNaxTi2Sb2O (0.0<=x<=0.33): A Layered Titanium-Based Pnictide Oxide Superconductor			Department of Chemistry,  University of Houston, Houston, Texas 77204, United States	J.Am.Chem.Soc., 134(2012)16520	Phuong Doan,Melissa Gooch,Zhongjia Tang,Bernd Lorenz,Angela Moller,Joshua Tapp,Paul C. W. Chu,Arnold M. Guloy		
154425	ACS13416520	T<CDW>,T<SDW> = 31.1 K.	(Ba,Na)Ti2Sb2O	Ba0.75Na0.25Ti2Sb2O1	Ba	0.75	Na	0.25	Ti	2	Sb	2													O	1			2012																										ABC2D2		oxypnictide	P4/mmm																Ti-oxypnictide, CeCr2Si2C	K				5.53			5.53																																																																																														BaO,BaO2,Na2O,Na2O2,Ti,Sb		mixture - weld in Nb container - heat(900C,3d) - cool to 200C(2C/min) - reground - SIN(900C,3d)					Ba1-xNaxTi2Sb2O (0.0<=x<=0.33): A Layered Titanium-Based Pnictide Oxide Superconductor			Department of Chemistry,  University of Houston, Houston, Texas 77204, United States	J.Am.Chem.Soc., 134(2012)16520	Phuong Doan,Melissa Gooch,Zhongjia Tang,Bernd Lorenz,Angela Moller,Joshua Tapp,Paul C. W. Chu,Arnold M. Guloy		
154426	ACS13502951	M = NH3. K-intercalated sample. compositions: K0.28Fe1.97Se2M0.47 by ICP-AES. Tc not depends on M-content	KxFe2Se2(NH3)y	K0.3Fe2Se2M0.47	K	0.3	Fe	2	Se	2	M	0.47																1	2013																															A			15.56												K				44			44																																																																																																synthesized by a liquid NH3 method.					Superconducting Phases in Potassium-Intercalated Iron Selenides			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Am.Chem.Soc., 135(2013)02951	Tianping Ying,Xiaolong Chen,Gang Wang,Shifeng Jin,Xiaofang Lai,Tingting Zhou,Han Zhang,Shijie Shen,Wanyan Wang		
154427	ACS13502951	M = NH3. K-intercalated sample. compositions: K0.4Fe2Se2M0.5 by ICP-AES. sample composed of two Tc phases (Tc-44K and 30 K, correspond to x=0.3 and 0.6, respectively. Tc not depends on M-content	KxFe2Se2(NH3)y	K0.4Fe2Se2M0.47	K	0.4	Fe	2	Se	2	M	0.47																1	2013																																														K				36			36																																																																																																synthesized by a liquid NH3 method.					Superconducting Phases in Potassium-Intercalated Iron Selenides			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Am.Chem.Soc., 135(2013)02951	Tianping Ying,Xiaolong Chen,Gang Wang,Shifeng Jin,Xiaofang Lai,Tingting Zhou,Han Zhang,Shijie Shen,Wanyan Wang		
154428	ACS13502951	M = NH3. K-intercalated sample. compositions: K0.57Fe2.02Se2M0.34 by ICP-AES. Tc not depends on M-content	KxFe2Se2(NH3)y	K0.7Fe2Se2M0.47	K	0.7	Fe	2	Se	2	M	0.47																1	2013																															A			14.84												K				30			30																																																																																																synthesized by a liquid NH3 method.					Superconducting Phases in Potassium-Intercalated Iron Selenides			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Am.Chem.Soc., 135(2013)02951	Tianping Ying,Xiaolong Chen,Gang Wang,Shifeng Jin,Xiaofang Lai,Tingting Zhou,Han Zhang,Shijie Shen,Wanyan Wang		
154429	CEM2160091	impurity phases: FeAs(1.4 wt%), Sr3V2O7(5.7 wt%), SrFe2As2(9.1 wt%).	Sr2VO3FeAs	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3			2014																												22426	P4/nmm		A	3.93621		15.7047											STR = 21113 type	K		24.8					24.8										31																																																																																				SrO,CaO,V,Fe2O3,Fe,As		mixture - pellet - alumina crucible - sealed in silica ampoule - heat to 1100C(1C/min) - hold(48h) -cool to RT					Control of the superconducting properties of Sr2-xCaxVO3FeAs through isovalent substitution			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX13QR, UK	J.Solid State Chem., 216(2014)91	Alex J.Corkett,David G.Free,Simon J.Cassidy,Silvia Ramos,Simon J.Clarke		
154430	CEM2160091	impurity phases: FeAs(3.4 wt%), Sr3V2O7(1.78 wt%), SrFe2As2(0.79 wt%).	(Sr,Ca)VO3FeAs	Sr1.9Ca0.1V1Fe1As1O3	Sr	1.9	Ca	0.1	V	1	Fe	1	As	1											O	3			2014																												22426	P4/nmm		A	3.93561		15.6711											STR = 21113 type	K		25.8					25.8	MTC154430									32																																																																																				SrO,CaO,V,Fe2O3,Fe,As		mixture - pellet - alumina crucible - sealed in silica ampoule - heat to 1100C(1C/min) - hold(48h) -cool to RT					Control of the superconducting properties of Sr2-xCaxVO3FeAs through isovalent substitution			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX13QR, UK	J.Solid State Chem., 216(2014)91	Alex J.Corkett,David G.Free,Simon J.Cassidy,Silvia Ramos,Simon J.Clarke		
154431	CEM2160091	impurity phases: FeAs(3.2 wt%), Sr3V2O7(1.13 wt%), SrFe2As2(0.6 wt%).	(Sr,Ca)VO3FeAs	Sr1.8Ca0.2V1Fe1As1O3	Sr	1.8	Ca	0.2	V	1	Fe	1	As	1											O	3			2014																												22426	P4/nmm		A	3.93387		15.6611											STR = 21113 type	K		13.7					13.7	MTC154430									8.5																																																																																				SrO,CaO,V,Fe2O3,Fe,As		mixture - pellet - alumina crucible - sealed in silica ampoule - heat to 1100C(1C/min) - hold(48h) -cool to RT					Control of the superconducting properties of Sr2-xCaxVO3FeAs through isovalent substitution			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX13QR, UK	J.Solid State Chem., 216(2014)91	Alex J.Corkett,David G.Free,Simon J.Cassidy,Silvia Ramos,Simon J.Clarke		
154432	CEM2160091	impurity phases: FeAs(5.4 wt%), Sr3V2O7(1.2 wt%), SrFe2As2(1.4 wt%).	(Sr,Ca)VO3FeAs	Sr1.7Ca0.3V1Fe1As1O3	Sr	1.7	Ca	0.3	V	1	Fe	1	As	1											O	3			2014																												22426	P4/nmm		A	3.9312		15.6602											STR = 21113 type	K			0.8				0.8																																																																																														SrO,CaO,V,Fe2O3,Fe,As		mixture - pellet - alumina crucible - sealed in silica ampoule - heat to 1100C(1C/min) - hold(48h) -cool to RT					Control of the superconducting properties of Sr2-xCaxVO3FeAs through isovalent substitution			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford, OX13QR, UK	J.Solid State Chem., 216(2014)91	Alex J.Corkett,David G.Free,Simon J.Cassidy,Silvia Ramos,Simon J.Clarke		
154433	EPJB0850279	M = NH3	Li0.9Fe2As2(NH3)0.5	Li0.9Fe2Se2M0.5	Li	0.9	Fe	2	Se	2	M	0.5																	2012																															A	3.8273		16.518											SC phase: 245 structure	K				44			44																																																																																																LixFe2Se2 - NH3-intercalation(-75C,1-4h)					Superconductivity at Tc = 44 K in LixFe2Se2(NH3)y			CPM, Institute of Physics, University of Augsburg, 86157 Augsburg, Germany	Eur.Phys.J. B., 85(2012)279	E.-W. Scheidt,V.R. Hathwar,D. Schmitz,A. Dunbar,W. Scherer,F. Mayr,V. Tsurkan,J. Deisenhofer,A. Loidl		
154434	EPJB0850279	M = (NH3)[LiNH2]0.5	Li1.8Fe2Se2(NH3)[LiNH2]0.5	Li1.8Fe2Se2M1	Li	1.8	Fe	2	Se	2	M	1																	2012																															A	3.79607		16.998											SC phase: 245 structure	K				40			40																																																																																																Excess Li used for intercalation process					Superconductivity at Tc = 44 K in LixFe2Se2(NH3)y			CPM, Institute of Physics, University of Augsburg, 86157 Augsburg, Germany	Eur.Phys.J. B., 85(2012)279	E.-W. Scheidt,V.R. Hathwar,D. Schmitz,A. Dunbar,W. Scherer,F. Mayr,V. Tsurkan,J. Deisenhofer,A. Loidl		
154435	EPL10117004	High pressure annealing(600C, P=2 GPa).	La(O,F)BiS2	La1Bi1S2F0.2O0.8	La	1	Bi	1	S	2	F	0.2													O	0.8		1	2013																										ABCD2			P4/nmm		A	4.0574		13.5147											BiS2-layer	K	3.8		6.55	7.11			7.11																																																																																														Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h) - ground - ANN(600C,1h, P = 2 GPa)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154436	EPL10117004	High pressure annealing(600C, P=2 GPa).	La(O,F)BiS2	La1Bi1S2F0.4O0.6	La	1	Bi	1	S	2	F	0.4													O	0.6		1	2013																										ABCD2			P4/nmm		A	4.0616		13.4284											BiS2-layer	K	4.76		8.77	10.26			10.26																																																																																														Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h) - ground - ANN(600C,1h, P = 2 GPa)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154437	EPL10117004	High pressure annealing(600C, P=2 GPa).	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																										ABCD2			P4/nmm		A	4.062		13.2998											BiS2-layer	K	7.65		10.36	10.96			10.96	MTC154437																																																																																													Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h) - ground - ANN(600C,1h, P = 2 GPa)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154438	EPL10117004	High pressure annealing(600C, P=2 GPa).	La(O,F)BiS2	La1Bi1S2F0.6O0.4	La	1	Bi	1	S	2	F	0.6													O	0.4		1	2013																										ABCD2			P4/nmm		A	4.0598		13.1037											BiS2-layer	K	6.38		8.78	9.5			9.5																																																																																														Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h) - ground - ANN(600C,1h, P = 2 GPa)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154439	EPL10117004	High pressure annealing(600C, P=2 GPa).	La(O,F)BiS2	La1Bi1S2F0.7O0.3	La	1	Bi	1	S	2	F	0.7													O	0.3		1	2013																										ABCD2			P4/nmm		A	4.0546		13.0594											BiS2-layer	K	4.56		7.63	7.86			7.86																																																																																														Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h) - ground - ANN(600C,1h, P = 2 GPa)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154440	EPL10117004	No post annealing.. Tc data not shown.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																										ABCD2			P4/nmm		A	4.0721		13.4242											BiS2-layer	K																																																																																																					Bi2O3,BiF3,La2S3,Bi		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Evolution of superconductivity in LaO1-xFxBiS2 prepared by high-pressure technique			National Institute for Materials Science - 1-2-1, Sengen, Tsukuba, 305-0047, Ibaraki, Japan	Europhys.Lett., 101(2013)17004	K. Deguchi,Y. Mizuguchi,S. Demura,H. Hara,T. Watanabe,S. J. Denholme,M. Fujioka,H. Okazaki,T. Ozaki,H. Takeya,T. Yamaguchi,O. Miura,Y. Takano		
154441	EPL10427001	impurity phase: maybe alpha-Bi2Pd(Tc=1.72 K). Tn, Tc defined as max of (dR/dT).	ErPdBi	Er1Pd1Bi1	Er	1	Pd	1	Bi	1																		3	2013					myu-B/mol	3.54	-3.5																			ABC			F4[-]3m		A	6.595													cubic	K		1.24		1.22			1.24										15	Oe	preriminary	2							T	RES(max of (dR/dT). extrapolation	1.6												MHC154441		A	from Hc2	140			A	calc using Hc1,Hc2,GL eq.	4480																																																			Er(3N5),Pd(4N),Bi(5N)		arc-melting - alumina crucible with excess Bi-flux - heat to 1150C( in quartz tube, 0.3 bar-Ar-gas) - keep(36h) - slow cool to 500C(3C/h)					Superconductivity and magnetic order in the noncentrosymmetric half-Heusler compound ErPdBi			Van der Waals - Zeeman Institute, University of Amsterdam - Science Park 904, 1098 XH Amsterdam, The Netherlands	Europhys.Lett., 104(2013)27001	Y. Pan,A. M. Nikitin,T. V. Bay,Y. K. Huang,C. Paulsen,B. H. Yan,A. de Visser		
154442	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	LaNi1-xBi2+y	La1Ni0.84Bi2.04	La	1	Ni	0.84	Bi	2.04																		3	2013																													P4/nmm		A	4.56		9.78											ZrCuSi2-type	K			4.41				4.41										3										kOe	RES(on)													MHC154442																																																														crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154443	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	CeNi1-xBi2+y	Ce1Ni0.8Bi2.03	Ce	1	Ni	0.8	Bi	2.03																		3	2013	emu/mole	0.001			myu-B/mol	2.4	-17	4.8																					P4/nmm		A	4.54		9.64											ZrCuSi2-type	K			4.2				4.2										3										kOe	RES(on)													MHC154443																																																														crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154444	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	PrNi1-xBi2+y	Pr1Ni0.79Bi1.98	Pr	1	Ni	0.79	Bi	1.98																		3	2013	emu/mole	0.0001			myu-B/mol	3.6	-12	6.4																					P4/nmm		A	4.52		9.6001											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154445	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	NdNi1-xBi2+y	Nd1Ni0.72Bi2.14	Nd	1	Ni	0.72	Bi	2.14																		3	2013	emu/mole	0.0002			myu-B/mol	3.8	-16	3.8																					P4/nmm		A	4.52		9.53											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154446	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	SmNi1-xBi2+y	Sm1Ni0.78Bi2.08	Sm	1	Ni	0.78	Bi	2.08																		3	2013								3.3																					P4/nmm		A	4.5001		9.42											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154447	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	GdNi1-xBi2+y	Gd1Ni0.72Bi1.91	Gd	1	Ni	0.72	Bi	1.91																		3	2013	emu/mole	0.001			myu-B/mol	7.9	-51	9.8																					P4/nmm		A	4.49		9.37											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154448	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	TbNi1-xBi2+y	Tb1Ni0.74Bi1.9	Tb	1	Ni	0.74	Bi	1.9																		3	2013	emu/mole	-0.0012			myu-B/mol	10	-40	10.2																					P4/nmm		A	4.48		9.3001											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154449	JAC5540304	compositions by WDS, not bulk SC. SC maybe from Ni-Bi compounds (but not detected by XRD.	DyNi1-xBi2+y	Dy1Ni0.74Bi1.78	Dy	1	Ni	0.74	Bi	1.78																		3	2013	emu/mole	0.0028			myu-B/mol	10.8	-24	5.4																					P4/nmm		A	4.47		9.29											ZrCuSi2-type	K			4.2				4.2																																																																																																crystals grown from excess Bi-flux via high temperature solution method.					Anisotropic magnetization and resistivity of single crystalline RNi1-xBi2+-y (R = La-Nd, Sm, Gd-Dy)			Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Alloy Compd., 554(2013)304	Xiao Lin,Warren E. Straszheim,Sergey L. Bud'ko,Paul C. Canfield		
154450	JAP113056102	Lattice term in SP (beta) = 1.428 mJ/mol.K4	Nd(O,F)BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5		1	2013																										ABCD2			P4/nmm		A	3.9911		13.383											BiS2-layer, 1112 phase.	K	4.7		5.2				4.95																				T	RES(on). WHH	2.3							T/K	RES(on)	0.75			MHC154450																						mJ/mol.K2	26.23	SP	189.55	SP																																		Nd,Bi,S,NdF3,Nd2O3		mixture - solid state reaction					Superconductivity at 5K in NdO0.5F0.5BiS2			Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. K. S. Krishnan Road, New Delhi 110012, India	J.Appl.Phys., 113(2013)056102	Rajveer Jha,Anuj Kumar,Shiva Kumar Singh,V. P. S. Awana		
154451	JPCM01410759	Black-P. Tc measured for 0 < P < 160 GPa. Tc(max) = 9.5 K at 32 GPa.	Black-P	P1	P	1																							2002																										A																				K				9.5	0		9.5	MTC154451		K/GPa	0.58																																																																																																	The pressure effect on the superconducting transition temperature of black phosphorus			Research Centre for Materials Science at Extreme Conditions (KYOKUGEN), Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.: Condens.Matter, 14(2002)10759	M.Karuzawa,M.Ishizuka,S.Endo		
154452	JPCM020165207	RRR = 21	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2008																										ABC2		CeNiC2	Amm2		A	3.954	4.557	6.193												K	3.07		3.45	2.86			2.86																																																																							uOhm.cm											191														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154453	JPCM020165207		La(Ni,Cu)C2	La1Ni0.95Cu0.05C2	La	1	Ni	0.95	Cu	0.05	C	2																1	2008																										ABC2		CeNiC2	Amm2		A	3.954	4.557	6.195												K	3.15		4.05	3.15			3.15																																																																							uOhm.cm											168														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154454	JPCM020165207		La(Ni,Cu)C2	La1Ni0.9Cu0.1C2	La	1	Ni	0.9	Cu	0.1	C	2																1	2008																										ABC2		CeNiC2	Amm2		A	3.954	4.558	6.196												K	3.45		4.21	3.24			3.24	MTC154454																																																																						uOhm.cm											120														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154455	JPCM020165207		La(Ni,Cu)C2	La1Ni0.85Cu0.15C2	La	1	Ni	0.85	Cu	0.15	C	2																1	2008																										ABC2		CeNiC2	Amm2		A	3.955	4.559	6.199												K	3.72		4.25	3.31			3.31																																																																							uOhm.cm											107														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154456	JPCM020165207	RRR = 9.4	La(Ni,Cu)C2	La1Ni0.8Cu0.2C2	La	1	Ni	0.8	Cu	0.2	C	2																1	2008																										ABC2		CeNiC2	Amm2		A	3.956	4.56	6.201												K	4.02		4.61	3.45			3.45																																																																							uOhm.cm											90														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154457	JPCM020165207		La(Ni,Cu)C2	La1Ni0.75Cu0.25C2	La	1	Ni	0.75	Cu	0.25	C	2																1	2008																										ABC2		CeNiC2	Amm2		A	3.957	4.56	6.201												K	4.05		4.65	3.48			3.48																																																																							uOhm.cm											107														arc-melting					The antipressure effect of Cu on Tc in superconducting La(Ni1-xCux)C2 (0 =< x =<0.25)			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, Republic of China	J.Phys.: Condens.Matter, 20(2008)165207	H H Sung,S Y Chou,K J Syu,W H Lee		
154458	JPCM020385204	Lattice term in SP (beta)=0.393 mJ/mol.K4. (delta)=5.05 uJ/mol.K6. e-ph = 0.39-0.45. DOS =  1.69-1.63 states/ev.fu. (dC/gamma*Tc) = 1.05	LaPd2Ge2	La1Pd2Ge2	La	1	Pd	2	Ge	2																		1	2008																										AB2C2		ThCr2Si2																		K		0.96	1.1				0.96																																														meV	0.15	3.65	14				MSP154458			mJ/mol.K2	8.26	SP	291	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154459	JPCM020385204	Lattice term in SP (beta)=0.208 mJ/mol.K4. (delta)=1.97 uJ/mol.K6	LaNi2Si2	La1Ni2Si2	La	1	Ni	2	Si	2																		1	2008																										AB2C2		ThCr2Si2																		K					0.4																																																										mJ/mol.K2	11.3	SP	360	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154460	JPCM020385204	Lattice term in SP (beta)=0.273 mJ/mol.K4. (delta)=3.14 uJ/mol.K6	LaNi2Ge2	La1Ni2Ge2	La	1	Ni	2	Ge	2																		1	2008																										AB2C2		ThCr2Si2																		K					0.4																																																										mJ/mol.K2	14.5	SP	328	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154461	JPCM020385204	Lattice term in SP (beta)=1.27 mJ/mol.K4. (delta)=12.7 uJ/mol.K6. e-ph = 0.48-0.55. DOS =  3.86-3.69 states/ev.fu. (dC/gamma*Tc) = 1.24	La3Pd4Ge4	La3Pd4Ge4	La	3	Pd	4	Ge	4																		1	2008																										A3B4C4		U3Ni4Si4																		K		2.23	2.5				2.23																																														meV	0.3	3.08	14				MSP154461			mJ/mol.K2	27	SP	256	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154462	JPCM020385204	Lattice term in SP (beta)=0.645 mJ/mol.K4. (delta)=4.40 uJ/mol.K6. e-ph = 0.39-0.43. DOS =  5.43-5.32 states/ev.fu. (dC/gamma*Tc) = 1.32	La3Ni4Si4	La3Ni4Si4	La	3	Ni	4	Si	4																		1	2008																										A3B4C4		U3Ni4Si4																		K		0.96	1				0.96																																														meV	0.14	3.26	14				MSP154462			mJ/mol.K2	36.9	SP	321	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154463	JPCM020385204	Lattice term in SP (beta)=0.930 mJ/mol.K4. (delta)=2.76 uJ/mol.K6. e-ph = 0.38-0.43. DOS =  5.16-4.97 states/ev.fu. (dC/gamma*Tc) = 0.95	La3Ni4Ge4	La3Ni4Ge4	La	3	Ni	4	Ge	4																		1	2008																										A3B4C4		U3Ni4Si4																		K		0.74	0.76				0.74																																														meV	0.09	2.83	14				MSP154463			mJ/mol.K2	34.5	SP	284	SP																																				arc-melting - ANN(900-1100C, 1week, in vac)					Low temperature specific heat of superconducting ternary intermetallics La3Pd4Ge4, La3Ni4Si4, and La3Ni4Ge4 with U3Ni4Si4-type structure			SuperconductingMaterials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.: Condens.Matter, 20(2008)385204	S Kasahara,H Fujii,H Takeya,T Mochiku,A D Thakur,KHirata		
154464	JPCM022075702	not SC. Lattice term in SP (beta) = 0.79 mJ/mol.K4 for 3.9 < T < 25 K. T<SDW/CDW> = 200 K.	BaTi2As2O	Ba1Ti2As2O1	Ba	1	Ti	2	As	2															O	1		1	2010																										ABC2D2			P4/mmm	123	A	4.0456		7.2723												K					3.9																																																										mJ/mol.K2	15.3	SP	223	SP																																		BaO(3N),Ti(4N),As(6N)		solid state reaction. mixture - pellet - wrapped by Ta-foil - sealed in quartz tube - heat(850C, 40h)					Structure and physical properties for a new layered pnictide-oxide: BaTi2As2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.: Condens.Matter, 22(2010)075702	X F Wang,Y J Yan,J J Ying,Q J Li,M Zhang,N Xu,XH Chen		
154465	JPCM022075702	not SC. T<SDW> = 150 K. Interstitial site doping of Li.	BaLixTi2As2O	Ba1Li0.2Ti2As2O1	Ba	1	Li	0.2	Ti	2	As	2													O	1		1	2010																										ABC2D2			P4/mmm	123																K					3.9																																																																																																LiAs,BaO,Ti,As		mixture - react(500C,10h) - reground - pellet heat(800C,40h)					Structure and physical properties for a new layered pnictide-oxide: BaTi2As2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	J.Phys.: Condens.Matter, 22(2010)075702	X F Wang,Y J Yan,J J Ying,Q J Li,M Zhang,N Xu,XH Chen		
154467	JPCM023464203	impurity phases: Pr2O3, FeAs. R(T) shows hump around 150K.	(Pr,Sr)FeAsO	Pr0.8Sr0.2Fe1As1O1	Pr	0.8	Sr	0.2	Fe	1	As	1													O	1		1	2011																										ABCD		oxypnictide	P4/nmm																Fe-1111	K		13.6					13.6																																																																																											MRH154467			PrAs,SrAs,Pr6O11,FeAs,Fe,ZnO		mixture - pellet - ANN(1443K,40h, in evacuated quartz tube) - FC to RT					Effect of Zn doping in hole-type 1111 phase (Pr, Sr)FeAsO			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.: Condens.Matter, 23(2011)464203	Xiao Lin,Chenyi Shen,Chen Lv,Jianjian Miao,Hao Tan,Guanghan Cao,Zhu-An Xu		
154468	JPCM023464203	impurity phases: Pr2O3, FeAs. R(T) shows hump around 150K.	(Pr,Sr)(Fe,Zn)AsO	Pr0.8Sr0.2Fe0.97Zn0.03As1O1	Pr	0.8	Sr	0.2	Fe	0.97	Zn	0.03	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm																Fe-1111	K		13					13																																																																																														PrAs,SrAs,Pr6O11,FeAs,Fe,ZnO		mixture - pellet - ANN(1443K,40h, in evacuated quartz tube) - FC to RT					Effect of Zn doping in hole-type 1111 phase (Pr, Sr)FeAsO			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.: Condens.Matter, 23(2011)464203	Xiao Lin,Chenyi Shen,Chen Lv,Jianjian Miao,Hao Tan,Guanghan Cao,Zhu-An Xu		
154469	JPCM023464203	impurity phases: Pr2O3, FeAs. R(T) shows hump around 150K.	(Pr,Sr)(Fe,Zn)AsO	Pr0.8Sr0.2Fe0.94Zn0.06As1O1	Pr	0.8	Sr	0.2	Fe	0.94	Zn	0.06	As	1											O	1		1	2011																										ABCD		oxypnictide	P4/nmm																Fe-1111	K		12					12																																																																																											MRH154469			PrAs,SrAs,Pr6O11,FeAs,Fe,ZnO		mixture - pellet - ANN(1443K,40h, in evacuated quartz tube) - FC to RT					Effect of Zn doping in hole-type 1111 phase (Pr, Sr)FeAsO			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.: Condens.Matter, 23(2011)464203	Xiao Lin,Chenyi Shen,Chen Lv,Jianjian Miao,Hao Tan,Guanghan Cao,Zhu-An Xu		
154470	JPCM024382202	compositions by EDAX. M=C5H5N(pyridine). M-content not measured. (tentative value of 1)	Kx(C5H5N)yFe2Se2	K1.15M1Fe2.02Se2	K	1.15	M	1	Fe	2.02	Se	2																	2012																													I4/mmm																Fe-122	K			10				10																																																																																																appropriate amount of powdered FeAs precursor was placed into container filled with 0.2M solution of pure alkali metal dissoved in anhydrous pyridine.					Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc = 45 K			Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.: Condens.Matter, 24(2012)382202	A Krzton-Maziopa,E V Pomjakushina,V Yu Pomjakushin,F von Rohr,A Schilling,K Conder		
154471	JPCM024382202	compositions by EDAX. M=C5H5N(pyridine). M-content not measured. (tentative value of 1)	Nax(C5H5N)yFe2Se2	Na1.23M1Fe1.85Se2	Na	1.23	M	1	Fe	1.85	Se	2																	2012																													I4/mmm																Fe-122	K			35				35																																																																																																appropriate amount of powdered FeAs precursor was placed into container filled with 0.2M solution of pure alkali metal dissoved in anhydrous pyridine.					Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc = 45 K			Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.: Condens.Matter, 24(2012)382202	A Krzton-Maziopa,E V Pomjakushina,V Yu Pomjakushin,F von Rohr,A Schilling,K Conder		
154472	JPCM024382202	compositions by EDAX. M=C5H5N(pyridine). M-content not measured. (tentative value of 1)	Rbx(C5H5N)yFe2Se2	Rb1.21M1Fe1.85Se2	Rb	1.21	M	1	Fe	1.85	Se	2																	2012																													I4/mmm																Fe-122	K			15				15																																																																																																appropriate amount of powdered FeAs precursor was placed into container filled with 0.2M solution of pure alkali metal dissoved in anhydrous pyridine.					Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc = 45 K			Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.: Condens.Matter, 24(2012)382202	A Krzton-Maziopa,E V Pomjakushina,V Yu Pomjakushin,F von Rohr,A Schilling,K Conder		
154473	JPCM024382202	M = C5H5N(pyridine). M-content not measured. (tentative value of 1). compositions(Li,Fe,Se) not measured. R(T) shows 2 step transitions (45 and 31 K)	Lix(C5H5N)yFe2Se2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2012																													I4/mmm																Fe-122	K			45				45																																																																																																appropriate amount of powdered FeAs precursor was placed into container filled with 0.2M solution of pure alkali metal dissoved in anhydrous pyridine.					Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc = 45 K			Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.: Condens.Matter, 24(2012)382202	A Krzton-Maziopa,E V Pomjakushina,V Yu Pomjakushin,F von Rohr,A Schilling,K Conder		
154474	JPCM024382202	Anneald((215 C)-sample. M = C5H5N(pyridine). M-content not measured. (tentative value of 1). compositions not measured. sharp transitions.	Lix(C5H5N)yFe2Se2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2012																													P4/mmm																Fe-122	K			40				40										100																																																																																						appropriate amount of powdered FeAs precursor was placed into container filled with 0.2M solution of pure alkali metal dissoved in anhydrous pyridine.					Synthesis of a new alkali metal-organic solvent intercalated iron selenide superconductor with Tc = 45 K			Laboratory for Developments and Methods, Paul Scherrer Institute, 5232 Villigen PSI, Switzerland	J.Phys.: Condens.Matter, 24(2012)382202	A Krzton-Maziopa,E V Pomjakushina,V Yu Pomjakushin,F von Rohr,A Schilling,K Conder		
154475	JPCM025155701	RRR = 27. Hall const. at 2K. Lattice term in SP (beta) = 0.91 mJ/mol.K4. (dC/gamma*Tc) = 1.3. e-ph = 0.5. GL = 0.6	beta-IrSn4	Ir1Sn4	Ir	1	Sn	4																				3	2013																										AB4		MoSn4	I4<1>/acd		A	6.308		22.739											MoSn4-type	K	0.84	0.93	1	0.9		0.15	0.93											mT	M-H curve				3			0.5	mT	RES, WHH	8			6.8			0.15	mT/K		9.83			MHC154475		A	Hc2, spherical Fermi surface model	1930			A	Hc2, spherical Fermi surface model	1150					3.55	14				MSP154475			mJ/mol.K2	5.2	SP	221	SP											uOhm.cm							3				80			m3/C				0.000000000895			n/m3	6980000000000000000000000000	Ir(4N),Sn(5N)		self-flux method. mixture(Ir:Sn=1:80) - alumina crucible - sealed in quartz ampule - heat to 900C - cool to 600C(5C/h) - FC to 300C within 3h.					Observation of superconductivity in the intermetallic compound beta-IrSn4					Vinh Hung Tran,Zbigniew Bukowski		
154476	JPS077124702	RRR = 20. SUS(300K) = -9.79 E-5 emu/fu.	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																		1	2008																										AB4C12		skutterudite			A	8.618														K		8.2					8.2																																																																							uOhm.cm							18.3																		arc-melting - ANN(800C,200h, in vac)					Electrical, Magnetic and NMR Studies of Ge-Based Filled Skutterudites RPt4Ge12 (R = La, Ce, Pr, Nd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Tokushima 770-8502	J.Phys.Soc. Jpn, 77(2008)124702	Masatoshi TODA,Hitoshi SUGAWARA,Ko-ichi MAGISHI,Takahito SAITO,Kuniyuki KOYAMA,Yuji AOKI,Hideyuki SATO		
154477	JPS077124702	RRR = 24. Curie-Weis Law for T > 200K.	CePt4Ge12	Ce1Pt4Ge12	Ce	1	Pt	4	Ge	12																		1	2008					myu-B/fu	2.58	-62																			AB4C12		skutterudite			A	8.61														K					0.37																																																																									uOhm.cm							11.4																		arc-melting - ANN(800C,200h, in vac)					Electrical, Magnetic and NMR Studies of Ge-Based Filled Skutterudites RPt4Ge12 (R = La, Ce, Pr, Nd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Tokushima 770-8502	J.Phys.Soc. Jpn, 77(2008)124702	Masatoshi TODA,Hitoshi SUGAWARA,Ko-ichi MAGISHI,Takahito SAITO,Kuniyuki KOYAMA,Yuji AOKI,Hideyuki SATO		
154478	JPS077124702	RRR = 42. Curie-Weis Law for T > 100K.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2008					myu-B/fu	3.59	-16.8																			AB4C12		skutterudite			A	8.608														K		7.8					7.8																																																																							uOhm.cm							4.5																		arc-melting - ANN(800C,200h, in vac)					Electrical, Magnetic and NMR Studies of Ge-Based Filled Skutterudites RPt4Ge12 (R = La, Ce, Pr, Nd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Tokushima 770-8502	J.Phys.Soc. Jpn, 77(2008)124702	Masatoshi TODA,Hitoshi SUGAWARA,Ko-ichi MAGISHI,Takahito SAITO,Kuniyuki KOYAMA,Yuji AOKI,Hideyuki SATO		
154479	JPS077124702	RRR = 100. Curie-Weis Law for T > 100K.	NdPt4Ge12	Nd1Pt4Ge12	Nd	1	Pt	4	Ge	12																		1	2008					myu-B/fu	3.72	-31.1																			AB4C12		skutterudite			A	8.602														K			0.7				0.7																																																																							uOhm.cm							4.5																		arc-melting - ANN(800C,200h, in vac)					Electrical, Magnetic and NMR Studies of Ge-Based Filled Skutterudites RPt4Ge12 (R = La, Ce, Pr, Nd)			Faculty of Integrated Arts and Sciences, The University of Tokushima, Tokushima 770-8502	J.Phys.Soc. Jpn, 77(2008)124702	Masatoshi TODA,Hitoshi SUGAWARA,Ko-ichi MAGISHI,Takahito SAITO,Kuniyuki KOYAMA,Yuji AOKI,Hideyuki SATO		
154480	JPS081103702	Metallic R(T) for T > Tc	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2012																										A3B4C4																				K	4.34		4.6				4.47	MTC154480		K/GPa	-1.1																																																																																												solid state reaction					Pressure Study of BiS2-Based Superconductors Bi4O4S3 and La(O,F)BiS2			Department of Physics, Kobe University, Kobe 658-8530, Japan	J.Phys.Soc.Jpn, 81(2012)103702	Hisashi KOTEGAWA,Yusuke TOMITA,Hideki TOU,Hiroki IZAWA,Yoshikazu MIZUGUCHI,Osuke MIURA,Satoshi DEMURA,Keita DEGUCHI,Yoshihiko TAKANO		
154481	JPS081103702	Semiconductor-like R(T) for T > Tc. (dTc/dP) = -0.4 K/GPa for P > 1.0 GPa.	La(O0.5F0.5)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2012																										ABCD2		CeOBiS2																	CeOBiS2, BiS2 layer	K	7.63		9.67				8.65	MTC154481																																																																																															solid state reaction					Pressure Study of BiS2-Based Superconductors Bi4O4S3 and La(O,F)BiS2			Department of Physics, Kobe University, Kobe 658-8530, Japan	J.Phys.Soc.Jpn, 81(2012)103702	Hisashi KOTEGAWA,Yusuke TOMITA,Hideki TOU,Hiroki IZAWA,Yoshikazu MIZUGUCHI,Osuke MIURA,Satoshi DEMURA,Keita DEGUCHI,Yoshihiko TAKANO		
154482	JSNM0220343	120 K SC observed by SUS for reduced HxWO3 crystals (proton doped-WO3). H-dependence of Tc measured.	HxWO3	H1W1O3	H	1	W	1																	O	3			2009																																														K				120			120																																																																																																Crystals with HxWO3 surface were prepared by reduction of WO3 in 0.2N HCl in the presence of Zn metal chips at 90 C. Reduction (a few min)					A Possible 2D HxWO3 Superconductor with a T c of 120 K			Department of Materials and Interfaces, Weizmann Institute of Science, Rehovot 76100, Israel	J.Supercond. Nov. Magn., 22(2009)343	S. Reich,G. Leitus,R. Popovitz-Biro,A. Goldbourt,S. Vega		
154483	NATM0120015	M = (NH2)0.2(NH3)0.8, Substitution of H-to-D shows no effect for Tc.	Lix(NH2)y(NH3)1-yFe2Se2	Li0.6M1Fe2Se2	Li	0.6	M	1	Fe	2	Se	2																	2013																																														K				43			43																																																																																																					Enhancement of the superconducting transition temperature of FeSe by intercalation of a molecular spacer layer			Department of Chemistry, University of Oxford, Inorganic Chemistry Laboratory, South Parks Road, Oxford OX1 3QR, UK	Nature Mat., 12(2013)15	Matthew Burrard-Lucas,David G. Free,Stefan J. Sedlmaier,Jack D.Wright,Simon J. Cassidy,Yoshiaki Hara,Alex J. Corkett,Tom Lancaster,Peter J. Baker,Stephen J. Blundell,Simon J. Clarke		
154484	PHB4031119	Tc by SP. Lattice term in SP (beta)=1.27 mJ/mol.K4, (delta)=12.7 mJ/mol.K6, e-ph = 0.48-0.55. DOS = 3.86-3.69 states/eV.fu.  (dC/gamma*Tc) = 1.24.	La3Pd4Ge4	La3Pd4Ge4	La	3	Pd	4	Ge	4																			2008																										A3B4C4		U3Ni4Si4																		K			2.5				2.5																																														meV	0.3		14				MSP154484			mJ/mol.K2	27	SP	256	SP																																				arc-melting - ANN(900-1000C,1w)					Low temperature specific heat of ternary germanide superconductor La3Pd4Ge4			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica B, 403(2008)1119	Shigeru Kasahara,Hiroki Fujii,Takashi Mochiku,Hiroyuki Takeya,Kazuto Hirata		
154485	PHC4630182	impurity phase = LaPd2Ge2. Details of phases are investigated by NPD.	La3Pd4Ge4	La3Pd4Ge4	La	3	Pd	4	Ge	4																			2007																										A3B4C4		U3Ni4Si4			A	4.2293	4.3823	25.0109												K				2.75			2.75																																																																																																arc-melting - wrapped in Mo foil - ANN(900C,1w, in vac)					BaAl4-type derivative structure in superconducting La-Pd-Ge system			Superconducting Materials Center, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Physica C, 463(2007)182	T. Mochiku,H. Fujii,H. Takeya,T. Wuernisha,K. Mori,T. Ishigaki,T. Kamiyama,K. Hirata		
154486	PHC4970043	RRR = 1.44	MgB2	Mg1B2	Mg	1	B	2																					2014																												AlB2			A	3.0864		3.5255												K			33				33																																																																																																					Enhancing the superconducting temperature of MgB2 by SWCNT dilution			Department of Energy and Environmental Engineering, The Pennsylvania State University, University Park, PA 16802, USA	Physica C, 497(2014)43	Danhao Ma,Ruwantha Jayasingha,Dustin T. Hess,Kofi W. Adu,Gamini U. Sumanasekera,Mauricio Terrones		
154487	PHC4970043	composite material (MgB2+SWCNT). M = SWCNT(wt% in DB). charge transfer = 0.0023/carbon. RRR = 1.39	MgB2(SWCNT)x	Mg1B2M0.05	Mg	1	B	2	M	0.05																			2014																												AlB2			A	3.0871		3.5256												K			37.5				37.5																																																																																																purification of SWCNT - dispersion of SWCNT in MgB2 (ultrasonic bath, 3h,ethanol) - evaporation of ethanol(100C) - pellet					Enhancing the superconducting temperature of MgB2 by SWCNT dilution			Department of Energy and Environmental Engineering, The Pennsylvania State University, University Park, PA 16802, USA	Physica C, 497(2014)43	Danhao Ma,Ruwantha Jayasingha,Dustin T. Hess,Kofi W. Adu,Gamini U. Sumanasekera,Mauricio Terrones		
154488	PHC4970043	composite material (MgB2+SWCNT). M = SWCNT(wt% in DB). charge transfer = 0.0018/carbon. RRR = 1.27	MgB2(SWCNT)x	Mg1B2M0.5	Mg	1	B	2	M	0.5																			2014																												AlB2			A	3.0869		3.5257												K			37.8				37.8																																																																																																purification of SWCNT - dispersion of SWCNT in MgB2 (ultrasonic bath, 3h,ethanol) - evaporation of ethanol(100C) - pellet					Enhancing the superconducting temperature of MgB2 by SWCNT dilution			Department of Energy and Environmental Engineering, The Pennsylvania State University, University Park, PA 16802, USA	Physica C, 497(2014)43	Danhao Ma,Ruwantha Jayasingha,Dustin T. Hess,Kofi W. Adu,Gamini U. Sumanasekera,Mauricio Terrones		
154489	PHC4970043	composite material (MgB2+SWCNT). M = SWCNT(wt% in DB). charge transfer = 0.0008/carbon. RRR = 1.20	MgB2(SWCNT)x	Mg1B2M5	Mg	1	B	2	M	5																			2014																												AlB2			A	3.0869		3.5255												K			36.4				36.4																																																																																																purification of SWCNT - dispersion of SWCNT in MgB2 (ultrasonic bath, 3h,ethanol) - evaporation of ethanol(100C) - pellet					Enhancing the superconducting temperature of MgB2 by SWCNT dilution			Department of Energy and Environmental Engineering, The Pennsylvania State University, University Park, PA 16802, USA	Physica C, 497(2014)43	Danhao Ma,Ruwantha Jayasingha,Dustin T. Hess,Kofi W. Adu,Gamini U. Sumanasekera,Mauricio Terrones		
154490	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	Au25Sb75	Au25Sb75	Au	25	Sb	75																					1971																																													amorphous-like	K			6.7			0.5	6.7																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154491	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	Pd16.5Sb83.5	Pd16.5Sb83.5	Pd	16.5	Sb	83.5																					1971																																													amorphous-like	K			4.9				4.9																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154492	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	In25Sb75	In25Sb75	In	25	Sb	75																					1971																																													amorphous-like	K			4.1				4.1																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154493	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	In31.5Sb68.3	In31.5Sb68.5	In	31.5	Sb	68.5																					1971																																													amorphous-like	K			3.7				3.7																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154494	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	Au30Pd3.3Te66.6	Au30Pd3.3Te66.6	Au	30	Pd	3.3	Te	66.6																			1971																															A	2.85													amorphous-like	K			2.6				2.6																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154495	PLA0340080	metastable alloy made by liquid quenching. Tc measured by ac bridge.	Au16.7Pd16.6Te66.7	Au16.7Pd16.6Te66.7	Au	16.7	Pd	16.6	Te	66.7																			1971																															A	2.93													amorphous-like	K			4.6				4.6																																																																																																melt by induction under Ar atmosphere. Then quenched at a rate of 10E+7 C/sec.					SUPERCONDUCTING METASTABLE SIMPLE CUBIC ALLOYS			W. M. Keck Laboratory of Engineering Materials, California Institute of Technology, Pasadena, California 91109, USA	Phys.Lett., 34A(1971)80	C.C.Tsuei,Huan-Chun Yen,P.Duwez		
154496	PMB0930673	SP measured for 1.8 < T < 50 K. Tc(SP) = 2.93 K. Lattice term in SP (beta) = 0.904 mJ/mol.K4. (dC/gamma*Tc) = 0.94	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2		CeOBiS2	P4/nmm		A	4.0613		13.3157												K		3.1	3.6	2.8			3.1																				T		0.757																																		mJ/mol.K2	2.53	SP	221	SP																																		Ln2O3(or CeO2),LnF3,Ln2S3,Bi2S3		mixture - pellet - sealed in quartz tube(vac) - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds			Department of Physics, University of California, San Diego, La Jolla, CA 92093, USA	Philos.Magazine, 93(2013)673	D. Yazici,K. Huang,B.D. White,A.H. Chang,A.J. Friedman,M.B. Maple		
154497	PMB0930673	SP measured for 1.8 < T < 50 K.	Ce(O,F)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2		CeOBiS2	P4/nmm		A	4.0398		13.4513												K		1.89	2.2	5			1.89																																																								mJ/mol.K2	58.1	SP	224	SP																																		Ln2O3(or CeO2),LnF3,Ln2S3,Bi2S3		mixture - pellet - sealed in quartz tube(vac) - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds			Department of Physics, University of California, San Diego, La Jolla, CA 92093, USA	Philos.Magazine, 93(2013)673	D. Yazici,K. Huang,B.D. White,A.H. Chang,A.J. Friedman,M.B. Maple		
154498	PMB0930673		Pr(O,F)BiS2	Pr1Bi1S2F0.5O0.5	Pr	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2		CeOBiS2	P4/nmm		A	4.0192		13.4238												K		4.29	4.5	3.5			4.29																																																																																														Ln2O3(or CeO2),LnF3,Ln2S3,Bi2S3		mixture - pellet - sealed in quartz tube(vac) - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds			Department of Physics, University of California, San Diego, La Jolla, CA 92093, USA	Philos.Magazine, 93(2013)673	D. Yazici,K. Huang,B.D. White,A.H. Chang,A.J. Friedman,M.B. Maple		
154499	PMB0930673		LNdO,F)BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5			2013																										ABCD2		CeOBiS2	P4/nmm		A	4.0102		13.4468												K		4.37	4.4	4			4.37																																																																																														Ln2O3(or CeO2),LnF3,Ln2S3,Bi2S3		mixture - pellet - sealed in quartz tube(vac) - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds			Department of Physics, University of California, San Diego, La Jolla, CA 92093, USA	Philos.Magazine, 93(2013)673	D. Yazici,K. Huang,B.D. White,A.H. Chang,A.J. Friedman,M.B. Maple		
154500	PMB0930673	SP measured for 1.8 < T < 50 K. Neel-T by SP	Yb(O,F)BiS2	Yb1Bi1S2F0.5O0.5	Yb	1	Bi	1	S	2	F	0.5													O	0.5			2013								2.65																		ABCD2		CeOBiS2	P4/nmm		A	3.9851		13.5057												K		5.3	5.4	5			5.3																						1.38																																		mJ/mol.K2	30.1	SP	186	SP																																		Ln2O3(or CeO2),LnF3,Ln2S3,Bi2S3		mixture - pellet - sealed in quartz tube(vac) - ANN(800C,10h) - reground - pellet - ANN(800C,10h)					Superconductivity of F-substituted LnOBiS2 (Ln = La, Ce, Pr, Nd, Yb) compounds			Department of Physics, University of California, San Diego, La Jolla, CA 92093, USA	Philos.Magazine, 93(2013)673	D. Yazici,K. Huang,B.D. White,A.H. Chang,A.J. Friedman,M.B. Maple		
154501	PHC4630076	[penet] measured by dM/d(lnH). [penet](T) good fitting to BCS model. Jc(2K,0.5T) = 612 A/cm2.	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																		3	2007																										A4B5C10		Sc5Co4Si10																		K				8.4		0.4	8.4																				T	SUS, WHH		0.93	2.03					T/K	SUS		0.16	0.35	MHC154501		A	from Hc2		127	279	A	dM/d(lnH)		2100	840																																																			arc-melting. Crystals grown by floating zone method with growth rate = 2mm/h.					Anisotropic superconducting properties in Sc5Ir4Si10			Department of Applied Physics, The University of Tokyo, Hongo, Bunkyo-ku, Tokyo, Japan	Physica C, 463-465(2007)76	G.J.Li,M.Miura,Z.X.Shi,T.Tamegai		
154502	PRB082104513	RRR = 94. Lattice term in SP (beta) = 0.813 mJ/mol.K4. (dTc/gamma*Tc) = 1.53. Hc2(0) = 0.74 T, [cohere] = 210 A by WHH mobel,	PrRu4As12	Pr1Ru4As12	Pr	1	Ru	4	As	12																		3	2010					myu-B/Pr	3.52	-6.21																			AB4C12		skutterudite			A	8.508														K				2.5			2.5										100										T	SP. linear approx..	1.07							T/K	SP.	0.43			MHC154502		A	from (dHc2/dT), linear approx.	178																		mJ/mol.K2	70	SP	344	SP						uV/K	18			MTP154502	uOhm.cm							1.04				135														Crystals grown in a molten Cd:As flux. small crystals collected and etched in HCL acid to remove any impurities from surface					Superconductivity and crystalline electric field effects in the filled skutterudite PrRu4As12			Department of Physics, University of California?San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 82(2010)104513	T. A. Sayles,R. E. Baumbach,W. M. Yuhasz,M. B. Maple,L. Bochenek,R. Wawryk,T. Cichorek,A. Pietraszko,Z. Henkie,P.-C. Ho		
154503	PRB083214513	RRR = 7. P-induced SC. Tc(zero) appears for 2.5=<P =<3.0. Phase diagram shows two AFM temperature: T0 from Fe<2+> and Tn from Eu<2+>.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2																	Fe-122.	K		29	30		0		29	MPH154503																																																																																															Bridgman method					Phase diagram of pressure-induced superconductivity in EuFe2As2 probed by high-pressure resistivity up to 3.2 GPa			National Institute for Materials Science, Tsukuba, Ibaraki 305-0003, Japan	Phys.Rev.B, 83(2011)214513	Nobuyuki Kurita,Motoi Kimata,Kota Kodama,Atsushi Harada,Megumi Tomita,Hiroyuki S. Suzuki,Takehiko Matsumoto,Keizo Murata,Shinya Uji,Taichi Terashima		
154504	PRB085054503	T<STR> is transition temperature from P4/nmm to Cmma	NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2012																										ABC		PbFCl	P4/nmm																	K				8.94			8.94										7.8																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154505	PRB085054503	T<STR> is transition temperature from P4/nmm to Cmma	Na(Fe,Co)As	Na1Fe0.995Co0.005As1	Na	1	Fe	0.995	Co	0.005	As	1																3	2012																										ABC		PbFCl	P4/nmm																	K				9.81			9.81	MPH154505									35.6																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154506	PRB085054503	T<STR> is transition temperature from P4/nmm to Cmma	Na(Fe,Co)As	Na1Fe0.99Co0.01As1	Na	1	Fe	0.99	Co	0.01	As	1																3	2012																										ABC		PbFCl	P4/nmm																	K				17.8			17.8										79.4																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154507	PRB085054503	T<STR> is transition temperature from P4/nmm to Cmma	Na(Fe,Co)As	Na1Fe0.985Co0.015As1	Na	1	Fe	0.985	Co	0.015	As	1																3	2012																										ABC		PbFCl	P4/nmm																	K				19.9			19.9	MPH154505									94.1																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154508	PRB085054503		Na(Fe,Co)As	Na1Fe0.97Co0.03As1	Na	1	Fe	0.97	Co	0.03	As	1																3	2012																										ABC		PbFCl	P4/nmm																	K				21			21										100																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154509	PRB085054503		Na(Fe,Co)As	Na1Fe0.95Co0.05As1	Na	1	Fe	0.95	Co	0.05	As	1																3	2012																										ABC		PbFCl	P4/nmm																	K				15.9			15.9										100																																																																																						See Phys.Rev.Lett., 104(2010)057007					Gradual destruction of magnetism in the superconducting family NaFe1-xCoxAs			Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, United Kingdom	Phys.Rev.B, 85(2012)054503	J. D. Wright,T. Lancaster,I. Franke,A. J. Steele,J. S. Moller,M. J. Pitcher,A. J. Corkett,D. R. Parker,D. G. Free,F. L. Pratt,P. J. Baker,S. J. Clarke,S. J. Blundell		
154510	PRB086064516	RRR = 45. Tc and flux flow resistivity measured by surface impedance. Hc2 defined by R and flux flow. [penet]<L> measured.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2012																										ABC		PbFCl																		K			17				17																				T	RES, flux flow	22												MHC154510							A	surface impedance	3900																												uOhm.cm							30				1350														self-flux method					Microwave surface-impedance measurements of the electronic state and dissipation of magnetic vortices in superconducting LiFeAs single crystals			Department of Basic Science, The University of Tokyo, Meguro, Tokyo 153-8902, Japan	Phys.Rev.B, 86(2012)064516	T. Okada,H. Takahashi,Y. Imai,K. Kitagawa,K. Matsubayashi,Y. Uwatoko,A. Maeda		
154511	PRB086144525	[penet]<L> measured by nicro wave surface impedance.	SrFe2(As,P)2	Sr1Fe2As1.4P0.6	Sr	1	Fe	2	As	1.4	P	0.6																3	2012																										AB2C2		ThCr2Si2																		K	25						25																																									A	surface impedance	2700																												uOhm.cm							53.8				240														SrAs self-flux method					Investigation of the superconducting gap structure in SrFe2(As0.7P0.3)2 by magnetic penetration depth and flux flow resistivity analysis			Department of Basic Science, the University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan	Phys.Rev.B, 86(2012)144525	Hideyuki Takahashi,Tatsunori Okada,Yoshinori Imai,Kentaro Kitagawa,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Atsutaka Maeda		
154512	PRB087060510	<121/123>Sb-NQR measured. better fitting to s-wave full gap model. T<SDW>=T<CDW>= 40 K.from NMR-NQR.	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2013																										ABC2D2																				K		0.95					0.95																																																4.4	6																																															solid state reaction					s-wave superconductivity in superconducting BaTi2Sb2O revealed by <121/123>Sb-NMR/nuclear quadrupole resonance measurements			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 87(2013)060510	S. Kitagawa,K. Ishida,K. Nakano,T. Yajima,H. Kageyama		
154513	PRB089014510	dC at Tc = 16.9 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.85Na0.15Fe2As2	Ba	0.85	Na	0.15	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		5.3					5.3				-0.82																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154514	PRB089014510	dC at Tc = 206 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.8Na0.2Fe2As2	Ba	0.8	Na	0.2	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		11.8					11.8	MTC154514			5.44																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154515	PRB089014510	dC at Tc = 298 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.76Na0.24Fe2As2	Ba	0.76	Na	0.24	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		15.9					15.9	MTC154515			-3.5																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154516	PRB089014510	dC at Tc = 533 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.7Na0.3Fe2As2	Ba	0.7	Na	0.3	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		23.8					23.8	MTC154516			-2.62																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154517	PRB089014510	dC at Tc = 4537 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.65Na0.35Fe2As2	Ba	0.65	Na	0.35	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		33.1					33.1	MTC154516			-0.63																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154518	PRB089014510	dC at Tc = 4332 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.6Na0.4Fe2As2	Ba	0.6	Na	0.4	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		33.7					33.7	MTC154516			-0.87																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154519	PRB089014510	dC at Tc = 3789 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.5Na0.5Fe2As2	Ba	0.5	Na	0.5	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		32.8					32.8	MTC154516			-1.14																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154520	PRB089014510	dC at Tc = 2987 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.4Na0.6Fe2As2	Ba	0.4	Na	0.6	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		28.7					28.7	MTC154520			-1.07																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154521	PRB089014510	dC at Tc = 1397 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.3Na0.7Fe2As2	Ba	0.3	Na	0.7	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		24.2					24.2	MTC154520			-1.04																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154522	PRB089014510	dC at Tc = 868 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.2Na0.8Fe2As2	Ba	0.2	Na	0.8	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		19.2					19.2	MTC154520			-0.78																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154523	PRB089014510	dC at Tc = 150 mJ/mol.K extracted from Fig.2 (BNC-scaling)	(Ba,Na)Fe2As2	Ba0.1Na0.9Fe2As2	Ba	0.1	Na	0.9	Fe	2	As	2																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		18.4					18.4	MTC154520			-0.49																																																																																												mixture - sealed in Nb-tube - alumina crucible - sealed in fused silica tube - heat(800C,1-3 days) - heat(850C,1 day) - Q					Heat capacity jump at Tc and pressure derivatives of superconducting transition temperature in the Ba1-xNaxFe2As2 (0.1=< x  =< 0.9) series			Ames Laboratory, U.S. DOE and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)014510	Sergey L. Bud'ko,Duck Young Chung,Daniel Bugaris,Helmut Claus,Mercouri G. Kanatzidis,Paul C. Canfield		
154524	PRB089024517	Debye-T(RES) = 302K, Hc2(0) = 0.21Tby WHH, (dC/gamma*Tc) = 0.73, e-ph = 0.52, DOS = 2.95 states/eV.f.u from [gamma]	LaRhP	La1Rh1P1	La	1	Rh	1	P	1																		1	2014																										ABC	2	LaPtSi	I4<1>md		A	4.1846		14.9358												K			2.5			0.2	2.5																				T	RES(0.9Rn), GL	0.27												MHC154524		A	from Hc2	349																		mJ/mol.K2	6.95	SP	328	SP																																		LaP,LaAs,(Rh or Ir)		mixture - h-BN capsule - heat(1673 K,2h, P=5 GPa)					Superconductivity in noncentrosymmetric ternary equiatomic pnictides LaMP (M = Ir and Rh; P = P and As)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)024517	Yanpeng Qi,Jiangang Guo,Hechang Lei,Zewen Xiao,Toshio Kamiya,Hideo Hosono		
154525	PRB089024517	not SC. Debye-T(RES) = 237K, DOS = 3.27 states/eV.f.u from [gamma]	LaRhAs	La1Rh1As1	La	1	Rh	1	As	1																		1	2014																										ABC	2	LaPtSi	I4<1>md		A	4.1257		14.3839												K					1.9																																																										mJ/mol.K2	7.71	SP	263	SP																																		LaP,LaAs,(Rh or Ir)		mixture - h-BN capsule - heat(1673 K,2h, P=5 GPa)					Superconductivity in noncentrosymmetric ternary equiatomic pnictides LaMP (M = Ir and Rh; P = P and As)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)024517	Yanpeng Qi,Jiangang Guo,Hechang Lei,Zewen Xiao,Toshio Kamiya,Hideo Hosono		
154526	PRB089024517	Debye-T(RES) = 294K, Hc2(0) = 1.38 Tby WHH, (dC/gamma*Tc) = 0.65, e-ph = 0.67, DOS = 3.84 states/eV.f.u from [gamma]	LaIrP	La1Ir1P1	La	1	Ir	1	P	1																		1	2014																										ABC	2	LaPtSi	I4<1>md		A	4.2065		14.9379												K			5.3			0.2	5.3																				T	RES(0.9Rn), GL	1.64							T/K	RES(R=0.9Rn)	0.377			MHC154526		A	from Hc2	142																		mJ/mol.K2	9.07	SP	282	SP																																		LaP,LaAs,(Rh or Ir)		mixture - h-BN capsule - heat(1673 K,2h, P=5 GPa)					Superconductivity in noncentrosymmetric ternary equiatomic pnictides LaMP (M = Ir and Rh; P = P and As)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)024517	Yanpeng Qi,Jiangang Guo,Hechang Lei,Zewen Xiao,Toshio Kamiya,Hideo Hosono		
154527	PRB089024517	Debye-T(RES) = 240 K, Hc2(0) = 0.55 T by WHH, (dC/gamma*Tc) = 0.84, e-ph = 0.58, DOS = 3.74 states/eV.f.u from [gamma]	LaIrAs	La1Ir1As1	La	1	Ir	1	As	1																		1	2014																										ABC	2	LaPtSi	I4<1>md		A	4.1505		14.3277												K			3.1			0.2	3.1																				T	RES(0.9Rn), GL	0.64												MHC154527		A	from Hc2	227																		mJ/mol.K2	8.82	SP	261	SP																																		LaP,LaAs,(Rh or Ir)		mixture - h-BN capsule - heat(1673 K,2h, P=5 GPa)					Superconductivity in noncentrosymmetric ternary equiatomic pnictides LaMP (M = Ir and Rh; P = P and As)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)024517	Yanpeng Qi,Jiangang Guo,Hechang Lei,Zewen Xiao,Toshio Kamiya,Hideo Hosono		
154528	PRB089024518		Pr4Fe2As2TexO4	Pr4Fe2As2Te0.88O4	Pr	4	Fe	2	As	2	Te	0.88													O	4		3	2014																										AB2C2D4E4	2		I4/mmm		A	4.0165		29.8572											42214-type	K				25			25																																																																																																crystals grown at high pressure from precursor in NaCl/KCl flux. See Phys.Rev.B, 87(2013)180508					L4Fe2As2Te1-xO4-yFy (L = Pr, Sm, Gd): A layered oxypnictide superconductor with Tc up to 45 K			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 89(2014)024518	S. Katrych,A. Pisoni,S. Bosma,S. Weyeneth,N. D. Zhigadlo,R. Gaal,J. Karpinski,L. Forro		
154529	PRB089024518		Sm4Fe2As2TexO4	Sm4Fe2As2Te0.92O4	Sm	4	Fe	2	As	2	Te	0.92													O	4		3	2014																										AB2C2D4E4	2		I4/mmm		A	3.9642		29.509											42214-type	K				25			25																																																																																																crystals grown at high pressure from precursor in NaCl/KCl flux. See Phys.Rev.B, 87(2013)180508					L4Fe2As2Te1-xO4-yFy (L = Pr, Sm, Gd): A layered oxypnictide superconductor with Tc up to 45 K			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 89(2014)024518	S. Katrych,A. Pisoni,S. Bosma,S. Weyeneth,N. D. Zhigadlo,R. Gaal,J. Karpinski,L. Forro		
154530	PRB089024518		Gd4Fe2As2TexO4	Gd4Fe2As2Te0.9O4	Gd	4	Fe	2	As	2	Te	0.9													O	4		3	2014																										AB2C2D4E4	2		I4/mmm		A	3.9353		29.369											42214-type	K				25			25																																																																																																crystals grown at high pressure from precursor in NaCl/KCl flux. See Phys.Rev.B, 87(2013)180508					L4Fe2As2Te1-xO4-yFy (L = Pr, Sm, Gd): A layered oxypnictide superconductor with Tc up to 45 K			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 89(2014)024518	S. Katrych,A. Pisoni,S. Bosma,S. Weyeneth,N. D. Zhigadlo,R. Gaal,J. Karpinski,L. Forro		
154531	PRB089024518	F and O content by nominal value.	Sm4Fe2As2Tex(O,F)4	Sm4Fe2As2Te0.72F1.2O2.8	Sm	4	Fe	2	As	2	Te	0.72	F	1.2											O	2.8		3	2014																										AB2C2D4E4	2		I4/mmm		A	3.9597		29.268											42214-type	K			37	40			40																																																																																																crystals grown at high pressure from precursor in NaCl/KCl flux. See Phys.Rev.B, 87(2013)180508					L4Fe2As2Te1-xO4-yFy (L = Pr, Sm, Gd): A layered oxypnictide superconductor with Tc up to 45 K			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 89(2014)024518	S. Katrych,A. Pisoni,S. Bosma,S. Weyeneth,N. D. Zhigadlo,R. Gaal,J. Karpinski,L. Forro		
154532	PRB089024518	F and O content by nominal value.	Gd4Fe2As2Tex(O,F)4	Gd4Fe2As2Te0.92F0.8O3.2	Gd	4	Fe	2	As	2	Te	0.92	F	0.8											O	3.2		3	2014																										AB2C2D4E4	2		I4/mmm		A	3.9363		29.35											42214-type	K				45			45																																																																																																crystals grown at high pressure from precursor in NaCl/KCl flux. See Phys.Rev.B, 87(2013)180508					L4Fe2As2Te1-xO4-yFy (L = Pr, Sm, Gd): A layered oxypnictide superconductor with Tc up to 45 K			Institute of Condensed Matter Physics, EPFL, CH-1015 Lausanne, Switzerland	Phys.Rev.B, 89(2014)024518	S. Katrych,A. Pisoni,S. Bosma,S. Weyeneth,N. D. Zhigadlo,R. Gaal,J. Karpinski,L. Forro		
154533	PRB089035114	NMR of <75>As measured.	Ba(Fe,Co,Mn)2As2	Ba1Fe1.857Co0.13Mn0.013As2	Ba	1	Fe	1.857	Co	0.13	Mn	0.013	As	2														3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		18					18																																																																																																self flux method. mixture(Ba:FeAs:CoAs:MnAs = 1:4-x-y:x:y) - heat(1180C,6h, in evacuated quartz tube) - cool to 1000C(6C/h) - cool to RT.					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154534	PRB089035114	NMR of <75>As measured.	Ba(Fe,Co,Mn)2As2	Ba1Fe1.832Co0.15Mn0.018As2	Ba	1	Fe	1.832	Co	0.15	Mn	0.018	As	2														3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		13.5					13.5																																																																																																self flux method. mixture(Ba:FeAs:CoAs:MnAs = 1:4-x-y:x:y) - heat(1180C,6h, in evacuated quartz tube) - cool to 1000C(6C/h) - cool to RT.					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154535	PRB089035114	NMR of <75>As measured.	Ba(Fe,Co,Mn)2As2	Ba1Fe1.86Co0.12Mn0.02As2	Ba	1	Fe	1.86	Co	0.12	Mn	0.02	As	2														3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		12.5					12.5																																																																																																self flux method. mixture(Ba:FeAs:CoAs:MnAs = 1:4-x-y:x:y) - heat(1180C,6h, in evacuated quartz tube) - cool to 1000C(6C/h) - cool to RT.					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154536	PRB089035114	NMR of <75>As measured.	Ba(Fe,Co,Mn)2As2	Ba1Fe1.84Co0.13Mn0.03As2	Ba	1	Fe	1.84	Co	0.13	Mn	0.03	As	2														3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		8					8																																																																																																self flux method. mixture(Ba:FeAs:CoAs:MnAs = 1:4-x-y:x:y) - heat(1180C,6h, in evacuated quartz tube) - cool to 1000C(6C/h) - cool to RT.					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154537	PRB089035114	NMR of <75>As and (31>P measured.	BaFe2(As,P)2	Ba1Fe2As1.3P0.7	Ba	1	Fe	2	As	1.3	P	0.7																1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		30					30																																																																																														Ba,Fe,MnAs,P,As		solid state reaction. mixture - heat(950C,36h)					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154538	PRB089035114	NMR of <75>As and (31>P measured.	Ba(Fe,Mn)2(As,P)2	Ba1Fe1.97Mn0.03As1.3P0.7	Ba	1	Fe	1.97	Mn	0.03	As	1.3	P	0.7														1	2014																										AB2C2		ThCr2Si2																	Fe-122	K		16					16																																																																																														Ba,Fe,MnAs,P,As		solid state reaction. mixture - heat(950C,36h)					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154539	PRB089035114	NMR of <75>As and (31>P measured.	Ba(Fe,Mn)2(As,P)2	Ba1Fe1.94Mn0.06As1.3P0.7	Ba	1	Fe	1.94	Mn	0.06	As	1.3	P	0.7														1	2014																										AB2C2		ThCr2Si2																	Fe-122	K					2																																																																																																Ba,Fe,MnAs,P,As		solid state reaction. mixture - heat(950C,36h)					NMR study of electronic correlations in Mn-doped Ba(Fe1-xCox)2As2 and BaFe2(As1-xPx)2			Laboratoire de Physique des Solides, Universite Paris-Sud, UMR8502, CNRS - F-91405 Orsay Cedex, France	Phys.Rev.B, 89(2014)035114	D. LeBoeuf,Y. Texier,M. Boselli,A. Forget,D. Colson,J. Bobroff		
154540	PRB089041101	Actualconcentration of Hg (in DB value) is 20 % of nominal values.	CeIrIn5	Ce1Ir1In5	Ce	1	Ir	1	In	5																		3	2014																										ABC5	2	HoCoGa5																		K		1.273					1.273																																																								mJ/mol.K2	726	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154544	PHC4702040	major grain: Mo0.32Sn0.01Sr1.9Y1.2Cu2.9Oz by EDX position of Sn : Mo-site, grain boundary	Mo(Snx)Sr2YCu2O8	Mo1Sn0.03Sr2Y1Cu2O8-z	Mo	1	Sn	0.03	Sr	2	Y	1	Cu	2											O	8-z			2010																												M1212				3.82		11.459												K				26			26											Oe	M-H curve				70			2	T	R=0.5Rn	3.2																																																																								MoO3,SnO2,Y2O3,SrCO3,CuO	1	mixture - pellet - preheat(750C,24h, in air) - (grind & pellet) - SIN(950C,24h, in O2-flow) - (grid & pellet) - (1050C,48h, in O2-flow) - ANN(600C,48h + 400C,24h, in O2-flow)					Superconductivity and critical fields in undoped and Sn-doped MoSr2YCu2O8			Institute of Solid State Physics, Bulgarian Academy of Sciences, 1784 Sofia, Bulgaria	Physica C, 470(2010)2040	N. Balchev,K. Nenkov,V. Antonov,J. Pirov,B. Kunev		
154550	PRB089041101	Actualconcentration of Hg (in DB value) is 20 % of nominal values.	CeIrIn5-xHgx	Ce1Ir1In4.973Hg0.027	Ce	1	Ir	1	In	4.973	Hg	0.027																3	2014																										ABC5	2	HoCoGa5																		K		0.955					0.955																																																								mJ/mol.K2	769	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154551	PRB089041101	Actualconcentration of Hg (in DB value) is 20 % of nominal values.	CeIrIn5-xHgx	Ce1Ir1In4.955Hg0.045	Ce	1	Ir	1	In	4.955	Hg	0.045																3	2014								1.49																		ABC5	2	HoCoGa5																		K		0.993					0.993	MTC154551																																																							mJ/mol.K2	679	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154552	PRB089041101	Actualconcentration of Hg (in DB value) is 20 % of nominal values.	CeIrIn5-xHgx	Ce1Ir1In4.946Hg0.054	Ce	1	Ir	1	In	4.946	Hg	0.054																3	2014								1.77																		ABC5	2	HoCoGa5																		K		0.476					0.476	MTC154551																																																							mJ/mol.K2	629	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154553	PRB089041101	Actualconcentration of Hg (in DB value) is 20 % of nominal values.	CeIrIn5-xHgx	Ce1Ir1In4.775Hg0.225	Ce	1	Ir	1	In	4.775	Hg	0.225																3	2014								8.6																		ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	175	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154554	PRB089041101	Actualconcentration of Sn (in DB value) is 50 % of nominal values.	CeIrIn5-xSnx	Ce1Ir1In4.996Sn0.004	Ce	1	Ir	1	In	4.996	Sn	0.004																3	2014																										ABC5	2	HoCoGa5																		K		1.043					1.043																																																																																																single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154555	PRB089041101	Actualconcentration of Sn (in DB value) is 50 % of nominal values.	CeIrIn5-xSnx	Ce1Ir1In4.986Sn0.014	Ce	1	Ir	1	In	4.986	Sn	0.014																3	2014																										ABC5	2	HoCoGa5																		K		0.8					0.8	MTC154555																																																																																															single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154556	PRB089041101	Actualconcentration of Sn (in DB value) is 50 % of nominal values.	CeIrIn5-xSnx	Ce1Ir1In4.97Sn0.03	Ce	1	Ir	1	In	4.97	Sn	0.03																3	2014																										ABC5	2	HoCoGa5																		K		0.66					0.66	MTC154555																																																																																															single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154557	PRB089041101	Actualconcentration of Pt (in DB value) is 44 % of nominal values.	CeIr1-xPtxIn5	Ce1Ir0.987Pt0.013In5	Ce	1	Ir	0.987	Pt	0.013	In	5																3	2014																										ABC5	2	HoCoGa5																		K		0.897					0.897																																																								mJ/mol.K2	692	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154558	PRB089041101	Actualconcentration of Pt (in DB value) is 44 % of nominal values.	CeIr1-xPtxIn5	Ce1Ir0.978Pt0.022In5	Ce	1	Ir	0.978	Pt	0.022	In	5																3	2014																										ABC5	2	HoCoGa5																		K		0.734					0.734	MTC154558																																																																																															single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154559	PRB089041101	Actualconcentration of Pt (in DB value) is 44 % of nominal values.	CeIr1-xPtxIn5	Ce1Ir0.956Pt0.044In5	Ce	1	Ir	0.956	Pt	0.044	In	5																3	2014																										ABC5	2	HoCoGa5																		K		0.429					0.429	MTC154558																																																							mJ/mol.K2	633	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154560	PRB089041101	not SC. Actualconcentration of Sn (in DB value) is 50 % of nominal values. Fermi liquid temperature T<FL> = 1.0 K.	CeIrIn5-xSnx	Ce1Ir1In4.95Sn0.05	Ce	1	Ir	1	In	4.95	Sn	0.05																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	611	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154561	PRB089041101	not SC. Actualconcentration of Sn (in DB value) is 50 % of nominal values. Fermi liquid temperature T<FL> = 2.21 K.	CeIrIn5-xSnx	Ce1Ir1In4.9Sn0.1	Ce	1	Ir	1	In	4.9	Sn	0.1																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	519	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154562	PRB089041101	not SC. Actualconcentration of Sn (in DB value) is 50 % of nominal values. Fermi liquid temperature T<FL> = 2.79 K.	CeIrIn5-xSnx	Ce1Ir1In4.85Sn0.15	Ce	1	Ir	1	In	4.85	Sn	0.15																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	474	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154563	PRB089041101	not SC. Actualconcentration of Sn (in DB value) is 50 % of nominal values. Fermi liquid temperature T<FL> = 3.51 K.	CeIrIn5-xSnx	Ce1Ir1In4.8Sn0.2	Ce	1	Ir	1	In	4.8	Sn	0.2																3	2014																										ABC5	2	HoCoGa5																		K					0.2			MTC154555																																																							mJ/mol.K2	423	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154564	PRB089041101	not SC. Actualconcentration of Sn (in DB value) is 50 % of nominal values. Fermi liquid temperature T<FL> = 4.49 K.	CeIrIn5-xSnx	Ce1Ir1In4.65Sn0.35	Ce	1	Ir	1	In	4.65	Sn	0.35																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	298	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154565	PRB089041101	not SC. Actualconcentration of Pt (in DB value) is 44 % of nominal values. Fermi liquid temperature T<FL> = 1.21 K.	CeIr1-xPtxIn5	Ce1Ir0.932Pt0.068In5	Ce	1	Ir	0.932	Pt	0.068	In	5																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	532	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154566	PRB089041101	not SC. Actualconcentration of Pt (in DB value) is 44 % of nominal values. Fermi liquid temperature T<FL> = 2.84 K.	CeIr1-xPtxIn5	Ce1Ir0.828Pt0.172In5	Ce	1	Ir	0.828	Pt	0.172	In	5																3	2014																										ABC5	2	HoCoGa5																		K					0.2			MTC154558																																																							mJ/mol.K2	420	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154567	PRB089041101	not SC. Actualconcentration of Pt (in DB value) is 44 % of nominal values. Fermi liquid temperature T<FL> = 4.22 K.	CeIr1-xPtxIn5	Ce1Ir0.736Pt0.264In5	Ce	1	Ir	0.736	Pt	0.264	In	5																3	2014																										ABC5	2	HoCoGa5																		K					0.2																																																										mJ/mol.K2	255	SP																																						single crystals grown by In self-flux method.					CeIrIn5: Superconductivity on a magnetic instability			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 89(2014)041101	T. Shang,R. E. Baumbach,K. Gofryk,F. Ronning,Z. F. Weng,J. L. Zhang,X. Lu,E. D. Bauer,J. D. Thompson,H. Q. Yuan		
154568	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 2.83 at t=0.6. T<STR> = 53.6 K.	NsFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2014								44.4																		ABC		PbFCl																	Fe-111	K		11.1					11.1																				T	pulsed H, resonance,WHH		16.4	10.1					T/K	pulsed H, resonance		6		MHC154568		A	from Hc2		57.5	34.2	um	SC carrier density		1.36																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154569	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 1.96 at t=0.9. T<STR> = 30.8 K.	NaFe1-xCoxAs	Na1Fe0.99Co0.01As1	Na	1	Fe	0.99	Co	0.01	As	1																3	2014								27.6																		ABC		PbFCl																	Fe-111	K		13					13																				T	pulsed H, resonance,WHH		45.5	36.9					T/K	pulsed H, resonance		5.44		MHC154569		A	from Hc2		28.7	24.9	um	SC carrier density		0.544																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154570	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 2.78 at t=0.9. T<STR> = 29.8 K.	NaFe1-xCoxAs	Na1Fe0.98Co0.02As1	Na	1	Fe	0.98	Co	0.02	As	1																3	2014																										ABC		PbFCl																	Fe-111	K		18.8					18.8	MPH154570																			T	pulsed H, resonance,WHH		50.9	44.1					T/K	pulsed H, resonance		10		MHC154570		A	from Hc2		27	23.8	um	SC carrier density		0.402																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154571	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 6.77 at t=0.9.	NaFe1-xCoxAs	Na1Fe0.97Co0.03As1	Na	1	Fe	0.97	Co	0.03	As	1																3	2014																										ABC		PbFCl																	Fe-111	K		20.4					20.4																				T	pulsed H, resonance,WHH		61.9	55.9					T/K	pulsed H, resonance		10		MHC154571		A	from Hc2		24.2	22	um	SC carrier density		0.309																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154572	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 5.89 at t=0.9.	NaFe1-xCoxAs	Na1Fe0.95Co0.05As1	Na	1	Fe	0.95	Co	0.05	As	1																3	2014																										ABC		PbFCl																	Fe-111	K		17					17																				T	pulsed H, resonance,WHH		50.4	45					T/K	pulsed H, resonance		9.78		MHC154572		A	from Hc2		26.3	24.9	um	SC carrier density		0.517																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154573	PRB089054502	Hc2(0) by WHH for H//ab, Gurevich model for H//c. Anisotropy(Hc2) = 4.94 at t=0.9.	NaFe1-xCoxAs	Na1Fe0.92Co0.08As1	Na	1	Fe	0.92	Co	0.08	As	1																3	2014																										ABC		PbFCl																	Fe-111	K		7.53					7.53																				T	pulsed H, resonance,WHH		26	15.7					T/K	pulsed H, resonance		7.22		MHC154573		A	from Hc2		44.5	28	um	SC carrier density		0.667																																																				mixture(NaAs:Fe1-xCox=2:1) - alumina crucible - sealed in Nb tube - silica ampule - heat to 900C (1C/min) - slow cool to 400C (5C/h) - Q to RT					Upper critical field of NaFe1-xCoxAs superconductors			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 89(2014)054502	S. Ghannadzadeh,J. D. Wright,F. R. Foronda,S. J. Blundell,S. J. Clarke,P. A. Goddard		
154574	PRB089054514	not SC	Ba(Fe1-xCox)2As2	Ba1Fe1.93Co0.07As2	Ba	1	Fe	1.93	Co	0.07	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K					0.2																																																																																																		mixture(FeAs,CoAs,Ba) - in glassy carbon crucible - sealed in SiO2 ampoule - heat to 650C - heat (1200C,5h) - cool to 1000C (1C/h)					High-pressure evolution of the specific heat of a strongly underdoped Ba(Fe0.963Co0.037)As2 iron-based superconductor			Department of Physics, Hong Kong University of Science & Technology, Clear Water Bay, Kowloon, Hong Kong	Phys.Rev.B, 89(2014)054514	Y. Zheng,Y. Wang,F. Hardy,A. E. Bohmer,T. Wolf,C. Meingast,R. Lortz		
154575	PRB089054514	Tc(max) = 27.7  K (Cmid) at P = 2.3 GPa.	Ba(Fe1-xCox)2As2	Ba1Fe1.926Co0.074As2	Ba	1	Fe	1.926	Co	0.074	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		6.2					6.2	MTC154575																																																				MSP154575																																											mixture(FeAs,CoAs,Ba) - in glassy carbon crucible - sealed in SiO2 ampoule - heat to 650C - heat (1200C,5h) - cool to 1000C (1C/h)					High-pressure evolution of the specific heat of a strongly underdoped Ba(Fe0.963Co0.037)As2 iron-based superconductor			Department of Physics, Hong Kong University of Science & Technology, Clear Water Bay, Kowloon, Hong Kong	Phys.Rev.B, 89(2014)054514	Y. Zheng,Y. Wang,F. Hardy,A. E. Bohmer,T. Wolf,C. Meingast,R. Lortz		
154576	PRB089054514		Ba(Fe1-xCox)2As2	Ba1Fe1.92Co0.08As2	Ba	1	Fe	1.92	Co	0.08	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		6.7					6.7																																																																																																mixture(FeAs,CoAs,Ba) - in glassy carbon crucible - sealed in SiO2 ampoule - heat to 650C - heat (1200C,5h) - cool to 1000C (1C/h)					High-pressure evolution of the specific heat of a strongly underdoped Ba(Fe0.963Co0.037)As2 iron-based superconductor			Department of Physics, Hong Kong University of Science & Technology, Clear Water Bay, Kowloon, Hong Kong	Phys.Rev.B, 89(2014)054514	Y. Zheng,Y. Wang,F. Hardy,A. E. Bohmer,T. Wolf,C. Meingast,R. Lortz		
154577	PRB089094505	T<CDW> = 331. K.	Ba1-xRbxTi2Sb2O	Ba0.95Rb0.05Ti2Sb2O1	Ba	0.95	Rb	0.05	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C	P4/mmm		A	4.1065		8.0875												K		4.25					4.25																				T	RES(0.5Rn),WHH	1.3							T/K	RES(0.5Rn)	0.49			MHC154577		A	from Hc2	160																																																								BaO(4N),Rb2O,Ti(4N),TiO2,Sb(5N)		mixture - pellet - sealed in Nb ampoule(Ar) -SIN(1000C,72h) - reground - pellet -SIN(1000C,24h)					Superconductivity in rubidium-substituted Ba1-xRbxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)094505	Fabian von Rohr,Reinhard Nesper,Andreas Schilling		
154578	PRB089094505	T<CDW> = 12.2. K.	Ba1-xRbxTi2Sb2O	Ba0.9Rb0.1Ti2Sb2O1	Ba	0.9	Rb	0.1	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C	P4/mmm		A	4.1053		8.1011												K		5.33					5.33																																																																																														BaO(4N),Rb2O,Ti(4N),TiO2,Sb(5N)		mixture - pellet - sealed in Nb ampoule(Ar) -SIN(1000C,72h) - reground - pellet -SIN(1000C,24h)					Superconductivity in rubidium-substituted Ba1-xRbxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)094505	Fabian von Rohr,Reinhard Nesper,Andreas Schilling		
154579	PRB089094505	lattice term in SP (beta) = 1.63 mJ/mol.K4. (dC/gamma*Tc) = 1.6 Tc(SP) = 5.4 K.	Ba1-xRbxTi2Sb2O	Ba0.8Rb0.2Ti2Sb2O1	Ba	0.8	Rb	0.2	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C	P4/mmm		A	4.1016		8.1279												K		6.19					6.19	MPH154579																			T	RES(0.5Rn),WHH	2.3							T/K	RES(0.5Rn)	0.61			MHC154579		A	from Hc2	120															MSP154579			mJ/mol.K2	14	SP	193	SP																																		BaO(4N),Rb2O,Ti(4N),TiO2,Sb(5N)		mixture - pellet - sealed in Nb ampoule(Ar) -SIN(1000C,72h) - reground - pellet -SIN(1000C,24h)					Superconductivity in rubidium-substituted Ba1-xRbxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)094505	Fabian von Rohr,Reinhard Nesper,Andreas Schilling		
154580	PRB089094505		Ba1-xRbxTi2Sb2O	Ba0.7Rb0.3Ti2Sb2O1	Ba	0.7	Rb	0.3	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C	P4/mmm		A	4.0983		8.1386												K		5.93					5.93																																																																																														BaO(4N),Rb2O,Ti(4N),TiO2,Sb(5N)		mixture - pellet - sealed in Nb ampoule(Ar) -SIN(1000C,72h) - reground - pellet -SIN(1000C,24h)					Superconductivity in rubidium-substituted Ba1-xRbxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)094505	Fabian von Rohr,Reinhard Nesper,Andreas Schilling		
154581	PRB089094505		Ba1-xRbxTi2Sb2O	Ba0.6Rb0.4Ti2Sb2O1	Ba	0.6	Rb	0.4	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C	P4/mmm		A	4.0937		8.1773												K		5.71					5.71																																																																																														BaO(4N),Rb2O,Ti(4N),TiO2,Sb(5N)		mixture - pellet - sealed in Nb ampoule(Ar) -SIN(1000C,72h) - reground - pellet -SIN(1000C,24h)					Superconductivity in rubidium-substituted Ba1-xRbxTi2Sb2O			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)094505	Fabian von Rohr,Reinhard Nesper,Andreas Schilling		
154582	PRB089094509	impurity phase: LaSi2(5wt%). lattice term in SP (beta) = 0.155 mJ/mol.K4. e-ph = 0.51. (dC/gamma*Tc) = 1.37. type-I SC.	LaPdSi3	La1Pd1Si3	La	1	Pd	1	Si	3																		1	2014																										ABC3		BaNiSn3	I4/mm	107	A	4.3542		9.664												K	2.63	2.65	2.7	2.6			2.65										100										Oe	SP, muon-SR, extrapolation	182.7												MHC154582														3.514	14							mJ/mol.K2	4.67	SP	397	SP																																				arc-melting  -  wrapped in Ta foil - in quartz tube - ANN(900C,2w)					Investigations of the superconducting states of noncentrosymmetric LaPdSi3 and LaPtSi3			Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 89(2014)094509	M. Smidman,A. D. Hillier,D. T. Adroja,M. R. Lees,V. K. Anand,R. P. Singh,R. I. Smith,D. M. Paul,G. Balakrishnan		
154583	PRB089094509	lattice term in SP (beta) = 0.238 mJ/mol.K4. e-ph = 0.47. (dC/gamma*Tc) = 1.33. Hc2(0) = 526 G  from R(zero) and WHH.. GL-parameter=2.49.	LaPtSi3	La1Pt1Si3	La	1	Pt	1	Si	3																		1	2014																										ABC3		BaNiSn3	I4/mm	107	A	4.3474		9.6368												K	1.43	1.52	1.58	1.58			1.52																				Oe	muon-SR, extrapolation	360												MHC154583		A	from Hc2	960			A	muon-R	2390													mJ/mol.K2	4.41	SP	344	SP																																				arc-melting  -  wrapped in Ta foil - in quartz tube - ANN(900C,2w)					Investigations of the superconducting states of noncentrosymmetric LaPdSi3 and LaPtSi3			Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 89(2014)094509	M. Smidman,A. D. Hillier,D. T. Adroja,M. R. Lees,V. K. Anand,R. P. Singh,R. I. Smith,D. M. Paul,G. Balakrishnan		
154584	PRB089094514	not SC. MI(Mott insulator) to M'(intermediate metallic state) transition at T<H>. Reentrant to MI at T'. For P>10GPa, R(T) shows kink at T<K>.	(Tl,Rb)Fe2Se2	Tl0.36Rb0.44Fe1.56Se2	Tl	0.36	Rb	0.44	Fe	1.56	Se	2																3	2014																										AB2C2		ThCr2Si2																	245-phase	K					4			MPH154584																																																																																															Bridgeman method					Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 89(2014)094514	Peiwen Gao,Rong Yu,Liling Sun,Hangdong Wang,Zhen Wang,Qi Wu,Minghu Fang,Genfu Chen,Jing Guo,Chao Zhang,Dachun Gu,Huanfang Tian,Jianqi Li,Jing Liu,Yanchun Li,Xiaodong Li,Sheng Jiang,Ke Yang,Aiguo Li,Zhongxian Zhao		
154585	PRB089094514	not SC. MI(Mott insulator) to M'(intermediate metallic state) transition at T<H>. Reentrant to MI at T'. For P>10GPa, R(T) shows kink at T<K>.	KFe2Se2	K0.8Fe1.6Se2	K	0.8	Fe	1.6	Se	2																		3	2014																										AB2C2		ThCr2Si2																	245-phase	K					4			MPH154585																																																																																															Bridgeman method					Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 89(2014)094514	Peiwen Gao,Rong Yu,Liling Sun,Hangdong Wang,Zhen Wang,Qi Wu,Minghu Fang,Genfu Chen,Jing Guo,Chao Zhang,Dachun Gu,Huanfang Tian,Jianqi Li,Jing Liu,Yanchun Li,Xiaodong Li,Sheng Jiang,Ke Yang,Aiguo Li,Zhongxian Zhao		
154586	PRB089094514	MI(Mott insulator) to M'(intermediate metallic state) transition at T<H>. For P>10 GPa, second SC dome apperas (Tc(max) = 47 K at P=12.4 GPa)	(Tl,Rb)Fe2Se2	Tl0.4Rb0.4Fe1.67Se2	Tl	0.4	Rb	0.4	Fe	1.67	Se	2																3	2014																										AB2C2		ThCr2Si2																		K		31.8					31.8	MPH154586																																																																																															Bridgeman method					Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 89(2014)094514	Peiwen Gao,Rong Yu,Liling Sun,Hangdong Wang,Zhen Wang,Qi Wu,Minghu Fang,Genfu Chen,Jing Guo,Chao Zhang,Dachun Gu,Huanfang Tian,Jianqi Li,Jing Liu,Yanchun Li,Xiaodong Li,Sheng Jiang,Ke Yang,Aiguo Li,Zhongxian Zhao		
154587	PRB089094514	MI(Mott insulator) to M'(intermediate metallic state) transition at T<H>. For P>10 GPa, second SC dome apperas (Tc(max) = 48 K at P=12.5 GPa)	KFe2Se2	K0.8Fe1.7Se2	K	0.8	Fe	1.7	Se	2																		3	2014																										AB2C2		ThCr2Si2																		K		32					32	MPH154587																																																																																															Bridgeman method					Role of the 245 phase in alkaline iron selenide superconductors revealed by high-pressure studies			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 89(2014)094514	Peiwen Gao,Rong Yu,Liling Sun,Hangdong Wang,Zhen Wang,Qi Wu,Minghu Fang,Genfu Chen,Jing Guo,Chao Zhang,Dachun Gu,Huanfang Tian,Jianqi Li,Jing Liu,Yanchun Li,Xiaodong Li,Sheng Jiang,Ke Yang,Aiguo Li,Zhongxian Zhao		
154588	PRB089094520	RRR = 18.4. R(T) has a hump at 147 K, where thermal conductivity shows clear drop and SP-jump (dC = 20.2J/mol.K).	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2014																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.7964														K		5					5																																																													W/m.K	22.7				uV/K	2.94			MTP154588	uOhm.cm							1.93				35.5			cm3/C	-0.0000863				3	MRH154588					self-flux method. mixture(Sr:Ir:Sn = 2.5:1:25) - sealed in evacuated quartz tube - heat to 1323 K - cool to 773 K over 72h.					Characteristics of the phase transition near 147 K in Sr3Ir4Sn13			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 89(2014)094520	C. N. Kuo,H. F. Liu,C. S. Lue,L. M. Wang,C. C. Chen,Y. K. Kuo		
154589	PRB089100501	Anisotropy(Hc2) = 2.  Energy gap(0.4 K)  = 0.36 meV by STS tunneling.	(Ir,Pd)Te2	Ir0.95Pd0.05Te2	Ir	0.95	Pd	0.05	Te	2																		3	2014																										AB2			P3[-]ml		A			5.372												K	2		2.5	2.5			2.5										60										T	SUS,WHH		0.33	0.16												A	from Hc2		450	220						meV	0.39	3.6	1																																															crystals grown by chemical vapor transport method. T-gradient = 60 C (Hot-880C)					Fully gapped s-wave-like superconducting state and electronic structure in Ir0.95Pd0.05Te2 single crystals with strong spin-orbital coupling			Key Laboratory of Artificial Structures and Quantum Control (Ministry of Education), Department of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China	Phys.Rev.B, 89(2014)100501	D. J. Yu,F. Yang,Lin Miao,C. Q. Han,Meng-Yu Yao,Fengfeng Zhu,Y. R. Song,K. F. Zhang,J. F. Ge,X. Yao,Z. Q. Zou,Z. J. Li,B. F. Gao,Canhua Liu,D. D. Guan,C. L. Gao,Dong Qian,Jin-feng Jia		
154590	PRB089104520		KxWO3	K0.38W1O3	K	0.38	W	1																	O	3		1	2014																											2	bronze	P4/mbm	127	A	12.256		3.8247												K	2	2.09	2.19			0.2	2.09																																																																																														K2WO4,WO3,WO2		solid state reaction					Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 89(2014)104520	Neel Haldolaarachchige,Quinn Gibson,Jason Krizan,R. J. Cava		
154591	PRB089104520	(dC/gamma*Tc) = 1.03, Tc(SP) = 1.5 K. Lattice term in SP 8beta) = 0.59 mJ/mol.K2. e-ph coupling = 0.52. DOS = 0.27 states /eV.f.u fro [gamma]	KxWO3	K0.4W1O3	K	0.4	W	1																	O	3		1	2014																											2	bronze	P4/mbm	127	A	12.258		3.8252												K	1.65	1.74	1.81			0.2	1.74																				T	RES(0.5Rn), WHH	0.14							T/K	RES(0.5Rn)	0.12			MHC154591		A	from Hc2	485															MSP154591			mJ/mol.K2	4.15	SP	242	SP											mOhm.cm							0.27																K2WO4,WO3,WO2		solid state reaction					Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 89(2014)104520	Neel Haldolaarachchige,Quinn Gibson,Jason Krizan,R. J. Cava		
154592	PRB089104520		KxWO3	K0.42W1O3	K	0.42	W	1																	O	3		1	2014																											2	bronze	P4/mbm	127	A	12.264		3.8271												K	1.3	1.34	1.5			0.2	1.34																																																																																														K2WO4,WO3,WO2		solid state reaction					Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 89(2014)104520	Neel Haldolaarachchige,Quinn Gibson,Jason Krizan,R. J. Cava		
154593	PRB089104520		KxWO3	K0.45W1O3	K	0.45	W	1																	O	3		1	2014																											2	bronze	P4/mbm	127	A	12.272		3.829												K	0.811	0.885	1.1			0.2	0.885																																																																																														K2WO4,WO3,WO2		solid state reaction					Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 89(2014)104520	Neel Haldolaarachchige,Quinn Gibson,Jason Krizan,R. J. Cava		
154594	PRB089104520	not SC.	KxWO3	K0.5W1O3	K	0.5	W	1																	O	3		1	2014																											2	bronze	P4/mbm	127	A	12.279		3.831												K					0.4	0.2																																																																																															K2WO4,WO3,WO2		solid state reaction					Superconducting properties of the KxWO3 tetragonal tungsten bronze and the superconducting phase diagram of the tungsten bronze family			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 89(2014)104520	Neel Haldolaarachchige,Quinn Gibson,Jason Krizan,R. J. Cava		
154595	PRB089125111	Hc2(T) fitting to GL theory. Residual gamma = 9 mJ/mol.K2. Lattice term in SP (beta) = 2 mJ/mol.K2. (dC/gamma*Tc) = 1.5	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		1	2014																										A3B4C13		Yb3Co4Sn13																		K		1.95					1.95	MTC154595		K/GPa	0.03																T	RES(0.5Rn), GL	1.38												MHC154595		A	from Hc2	160								K	3.5	3.6	14							mJ/mol.K2	26	SP	268	SP																																				arc-melting. ANN(870C,12d)					Superconductivity of La3Co4Sn13 and La3Rh4Sn13: A comparative study			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	Phys.Rev.B, 89(2014)125111	A. Slebarski,M. Fija?kowski,M. M. Maska,M. Mierzejewski,B. D. White,M. B. Maple		
154596	PRB089125111	Two step SC transition (2.85 and 2.10 K)Hc2(T) fitting to GL theory. Residual gamma = 6 mJ/mol.K2. Lattice term in SP (beta) = 3 mJ/mol.K2. (dC/gamma*Tc) = 1.5	La3Rh4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		1	2014																										A3B4C13		Yb3Co4Sn13																		K		2.85					2.85	MTC154596		K/GPa	-0.05																T	RES(0.5Rn), GL	1.6												MHC154596		A	from Hc2	140								K	4.4	4.1	14							mJ/mol.K2	15	SP	234	SP																																				arc-melting. ANN(870C,12d)					Superconductivity of La3Co4Sn13 and La3Rh4Sn13: A comparative study			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	Phys.Rev.B, 89(2014)125111	A. Slebarski,M. Fija?kowski,M. M. Maska,M. Mierzejewski,B. D. White,M. B. Maple		
154597	PRB089174515	Hc2(T) for samples with randomly oriented powder sample, was discussed. Anisotropy = 7.4.	La(O,F)BiS2	La1F0.5Bi1S2O0.5	La	1	F	0.5	Bi	1	S	2													O	0.5		1	2014																										ABCD2		CeOBiS2	P4/nmm																	K	7.7		10.8				9.25																				T	RES(0.99Rn)													MHC154597																																																												La2S3,Bi2O3,BiF3,Bi2S3,Bi		High-P synthesis. mixture - pellet - sealed in BN crucible - high-P cell - heat(700C,1h, P=2 GPa)					Anisotropic upper critical field of the BiS2-based superconductor LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1 Minami-osawa, Hachioji, Tokyo 192-0397, Japan	Phys.Rev.B, 89(2014)174515	Yoshikazu Mizuguchi,Atsushi Miyake,Kazuto Akiba,Masashi Tokunaga,Joe Kajitani,Osuke Miura		
154598	PRB089205136	Magnetic phase diagram(T vs H) measured by torque, RES,tunnel diode method. Anisotropy(Hc2) = 10.	Ca10(Pt3As8)[(Fe0.922Pt0.078)2As2]5	Ca10Pt0.78Fe9.22As18	Ca	10	Pt	0.78	Fe	9.22	As	18																3	2014																																													Ca-10-3-8	K		9.96					9.96																				T	RES(R=0), WHH		30	20										MHC154598																																																														See Proc.Natl.Acad.Sci.USA, 108,E1019(2011)					Field-induced magnetic transitions in Ca10(Pt3As8)((Fe1-xPtx)2As2)5 compounds			Clarendon Laboratory, Department of Physics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kindom	Phys.Rev.B, 89(2014)205136	M. D. Watson,A. McCollam,S. F. Blake,D. Vignolles,L. Drigo,I. I. Mazin,D. Guterding,H. O. Jeschke,R. Valenti,N. Ni,R. Cava,A. I. Coldea		
154599	PRB089214516	slightly over-doped sample. Hc2(T) obtained from fluctuation conductivity for H > Tc(H).	Bi2Sr2CuO6	Bi2.15Sr1.9Cu1O6+z	Bi	2.15	Sr	1.9	Cu	1															O	6+z		3	2014																												Bi2201																		K		4					4																				T	RES,fluctuation													MHC154599																																																																			Low anisotropy of the upper critical field in a strongly anisotropic layered cuprate Bi2.15Sr1.9CuO6+z: Evidence for a paramagnetically limited superconductivity			Department of Physics, Stockholm University, AlbaNova University Center, SE-10691 Stockholm, Sweden	Phys.Rev.B, 89(2014)214516	S. O. Katterwe,Th. Jacobs,A. Maljuk,V. M. Krasnov		
154600	PRB089214516	optimally-doped sample. Hc2(T) obtained from fluctuation conductivity for H > Tc(H).	Bi2Sr2CuO6	Bi2.15Sr1.9Cu1O6+z	Bi	2.15	Sr	1.9	Cu	1															O	6+z		3	2014																												Bi2201																		K		4.3					4.3																				T	RES,fluctuation													MHC154600																																																																			Low anisotropy of the upper critical field in a strongly anisotropic layered cuprate Bi2.15Sr1.9CuO6+z: Evidence for a paramagnetically limited superconductivity			Department of Physics, Stockholm University, AlbaNova University Center, SE-10691 Stockholm, Sweden	Phys.Rev.B, 89(2014)214516	S. O. Katterwe,Th. Jacobs,A. Maljuk,V. M. Krasnov		
154601	PRB089224504	RRR = 10. (dC/Tc) = 38 mJ/mol.K2, (dC/gamma*Tc) = 1.52. DOS = 10.6 states/eV from [gamma]. R(T) = R0 + A*T^2 (A=1.94E-5 mOhm.cm/K2.	Ca3Ir4Ge4	Ca3Ir4Ge4	Ca	3	Ir	4	Ge	4																		1	2014									4.517																	A3B4C4		Na3Pt4Ge4	I4[-]3m	217	A	7.5689														K	1.4	1.7					1.7																																																					MSP154601			mJ/mol.K2	25	SP	235	SP											mOhm.cm							0.04				0.4												Ir(5N),Ge(5N),Ca(3N)		solid state reaction. IrGe by heating(600C,12h, in quartz tube). Then, mixture(IrGe+Ca) - pellet - in alumina crucible - sealed in quartz tube - heat to 800C(100C/h) - (800c,20h) - Q to water					Superconductivity and correlated Fermi liquid behavior in noncentrosymmetric Ca3Ir4Ge4			Physik-Institut der Universitat Zurich, Winterthurerstrasse 190, CH-8057 Zurich, Switzerland	Phys.Rev.B, 89(2014)224504	Fabian von Rohr,Huixia Luo,Ni Ni,Michael Worle,Robert J. Cava		
154602	PRB090020504	not SC	(PbSe)5(Bi2Se3)6	Pb5Bi12Se23	Pb	5	Bi	12	Se	23																		3	2014																											4		C2/m		A	21.551	4.1774	52.918											monoclinic, alpha=90.0, beta=107.224, gamma=90.0	K					1.2																																																																																																		self-flux method					Dirac fermions and superconductivity in the homologous structures (AgxPb1-xSe)5(Bi2Se3)3m (m = 1,2)			Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 90(2014)020504	L. Fang,C. C. Stoumpos,Y. Jia,A. Glatz,D. Y. Chung,H. Claus,U. Welp,W.-K. Kwok,M. G. Kanatzidis		
154603	PRB090020504	not SC	(Pb1-xAgxSe)5(Bi2Se3)6	Pb4Ag1Bi12Se23	Pb	4	Ag	1	Bi	12	Se	23																3	2014																											4		C2/m		A	21.521	4.1747	52.927											monoclinic, alpha=90.0, beta=107.423, gamma=90.0	K					1.2																																																																																																		self-flux method					Dirac fermions and superconductivity in the homologous structures (AgxPb1-xSe)5(Bi2Se3)3m (m = 1,2)			Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 90(2014)020504	L. Fang,C. C. Stoumpos,Y. Jia,A. Glatz,D. Y. Chung,H. Claus,U. Welp,W.-K. Kwok,M. G. Kanatzidis		
154604	PRB090020504	not SC	(PbSe)5(Bi2Se3)3	Pb5Bi6Se14	Pb	5	Bi	6	Se	14																		3	2014																											4		P21/m		A	21.4727	4.1915	15.984											monoclinic, alpha=90.0, beta=97.475, gamma=90.0	K					1.2																																																																																																		self-flux method					Dirac fermions and superconductivity in the homologous structures (AgxPb1-xSe)5(Bi2Se3)3m (m = 1,2)			Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 90(2014)020504	L. Fang,C. C. Stoumpos,Y. Jia,A. Glatz,D. Y. Chung,H. Claus,U. Welp,W.-K. Kwok,M. G. Kanatzidis		
154605	PRB090020504	Anisotropy(Hc2) = 1.5. Angular dependence of Hc2 measured.	(Pb1-xAgxSe)5(Bi2Se3)3	Pb4Ag1Bi6Se14	Pb	4	Ag	1	Bi	6	Se	14																3	2014																											4		P21/m																monoclinic	K	0.55		1.6				1.075																				T	RES(0.9Rn), WHH		1.1	0.74					T/K	RES(0.9Rn)		1.7	0.67	MHC154605		A	from Hc2		217																																																									self-flux method					Dirac fermions and superconductivity in the homologous structures (AgxPb1-xSe)5(Bi2Se3)3m (m = 1,2)			Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 90(2014)020504	L. Fang,C. C. Stoumpos,Y. Jia,A. Glatz,D. Y. Chung,H. Claus,U. Welp,W.-K. Kwok,M. G. Kanatzidis		
154606	PRB090020504		(Pb1-xAgxSe)5(Bi2Se3)3	Pb3.9Ag1.1Bi6Se14	Pb	3.9	Ag	1.1	Bi	6	Se	14																3	2014																											4		P21/m																monoclinic	K			1.7				1.7																																																																																																self-flux method					Dirac fermions and superconductivity in the homologous structures (AgxPb1-xSe)5(Bi2Se3)3m (m = 1,2)			Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA	Phys.Rev.B, 90(2014)020504	L. Fang,C. C. Stoumpos,Y. Jia,A. Glatz,D. Y. Chung,H. Claus,U. Welp,W.-K. Kwok,M. G. Kanatzidis		
154607	CEM2100238	sample: (Nb0.87Si0.09X0.04)(N0.87O0.13), where X is cationic vacancy	(Nb0.87Si0.09X0.04)(N0.87O0.13)	Nb0.87Si0.09N0.87O0.13	Nb	0.87	Si	0.09	N	0.87															O	0.13		1	2014																										AB		NaCl																		K	15.28	16.35	16.62				16.35																				T	RES(0.5Rn), Linear approx.	28.07												MHC154607		A	from Hc2	34.25																																																										amorphous oxide precursor - nitride in alumina boat with ammonia - ANN(1200 or 1500C,3h, under 0.5 MPa-N2 in graphite furnace					Local structure around the flux pinning centers in superconducting niobium silicon oxynitride (Nb0.87Si0.09X0.04)(N0.87O0.13)			Faculty of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo, Hokkaido 060-8628, Japan	J.Solid State Chem., 210(2014)238	Y.Ohashi,Y.Masubuchi,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi,T.Yoshida,S. Kikkawa		
154608	CEM2100238	Nb-oxynitrides	Nb(N0.87O0.13)	Nb1N0.87O0.13	Nb	1	N	0.87																	O	0.13		1	2014																										AB		NaCl																		K	16.76	17.2	17.72				17.2																				T	RES(0.5Rn), Linear approx.	19.8												MHC154608		A	from Hc2	40.78																																																										amorphous oxide precursor - nitride in alumina boat with ammonia - ANN(1200 or 1500C,3h, under 0.5 MPa-N2 in graphite furnace					Local structure around the flux pinning centers in superconducting niobium silicon oxynitride (Nb0.87Si0.09X0.04)(N0.87O0.13)			Faculty of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo, Hokkaido 060-8628, Japan	J.Solid State Chem., 210(2014)238	Y.Ohashi,Y.Masubuchi,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi,T.Yoshida,S. Kikkawa		
154609	PR06012467	compositions not given. Bi-2201	Bi2Sr2CuOz	Bi2Sr2Cu1O6+z	Bi	2	Sr	2	Cu	1															O	6+z		3	1999																												Bi2201																		K		6					6																				T	RES													MHC154609																																																														Sr-deficient Bi3Sr2CuOz crystals were grown in a gaseous phase in the large closed cavities of KCl solution melt.					Temperature dependence of the upper critical field of Bi2Sr2CuOx single crystals			High Magnetic Field Laboratory, Max-Planck-Institut fur Festkorperforschung and Centre National de la Recherche Scientifique, Boite Postale, Grenoble Cedex 9, France	Phys.Rev.B, 60(1999)12467	S.I.Vedeneev,A.G.M.Jansen,E.Haanappel,P.Wyder		
154610	PR06012467	compositions not given. Bi-2201	Bi2Sr2CuOz	Bi2Sr2Cu1O6+z	Bi	2	Sr	2	Cu	1															O	6+z		3	1999																												Bi2201																		K		9					9																				T	RES(0.5Rn), Linear approx.		43	16										MHC154610		A	from Hc2		45	15																																																								Sr-deficient Bi3Sr2CuOz crystals were grown in a gaseous phase in the large closed cavities of KCl solution melt.					Temperature dependence of the upper critical field of Bi2Sr2CuOx single crystals			High Magnetic Field Laboratory, Max-Planck-Institut fur Festkorperforschung and Centre National de la Recherche Scientifique, Boite Postale, Grenoble Cedex 9, France	Phys.Rev.B, 60(1999)12467	S.I.Vedeneev,A.G.M.Jansen,E.Haanappel,P.Wyder		
154611	PRB090020505		(Pb0.5Sn0.5)Te	Pb0.5Sn0.5Te1	Pb	0.5	Sn	0.5	Te	1																		3	2014																												NaCl	Fm3[-]m		A	6.329														K					1.75																																																																																																		modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154612	PRB090020505		(Pb0.5Sn0.5)1-xInxTe	Pb0.47Sn0.47In0.06Te1	Pb	0.47	Sn	0.47	In	0.06	Te	1																3	2014																												NaCl	Fm3[-]m		A	6.386														K					1.75																																																																																																		modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154613	PRB090020505		(Pb0.5Sn0.5)1-xInxTe	Pb0.445Sn0.445In0.13Te1	Pb	0.445	Sn	0.445	In	0.13	Te	1																3	2014																												NaCl	Fm3[-]m		A	6.378														K			3.2				3.2	MTC154615																			T	RES(on), WHH		4.86						T/K	RES(on)	2.2			MHC154614																																																														modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154614	PRB090020505		(Pb0.5Sn0.5)1-xInxTe	Pb0.42Sn0.42In0.16Te1	Pb	0.42	Sn	0.42	In	0.16	Te	1																3	2014																												NaCl	Fm3[-]m		A	6.375														K			3.4				3.4	MTC154615																			T	RES(on), WHH		5.07						T/K	RES(on)	2.16			MHC154614																																																														modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154615	PRB090020505		(Pb0.5Sn0.5)1-xInxTe	Pb0.4Sn0.4In0.2Te1	Pb	0.4	Sn	0.4	In	0.2	Te	1																3	2014																												NaCl	Fm3[-]m		A	6.372														K			4				4	MTC154615																			T	RES(on), WHH		5.11						T/K	RES(on)	1.85			MHC154614																																																														modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154616	PRB090020505	For x > 0.3, secondary phase appears.	(Pb0.5Sn0.5)1-xInxTe	Pb0.35Sn0.35In0.3Te1	Pb	0.35	Sn	0.35	In	0.3	Te	1																3	2014																												NaCl	Fm3[-]m		A	6.359														K			4.8				4.8	MTC154615																			T	RES(on), WHH		5.1						T/K	RES(on)	1.54			MHC154614																																																														modified floating zone method. (5N purity elements) - melt(900C) - cool to RT(100C/h) - floating zone furnace - pre-melt(200mm/h) - growth(1.0 mm/h)					Superconductivity induced by In substitution into the topological crystalline insulator Pb0.5Sn0.5Te			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020505	R. D. Zhong,J. A. Schneeloch,T. S. Liu,F. E. Camino,J. M. Tranquada,G. D. Gu		
154617	EPL10427001	Half Heusler SC. Tn(H) defined by (dR/dT). carrier: n(hole) = 7.4 E+18 /cm3 at 4 K from Hall coeffic.	ErPdBi	Er1Pd1Bi1	Er	1	Pd	1	Bi	1																		3	2013					myu-B/mol	3.54	-3.5	1.06																		ABC	1		F4[-]3m		A	6.595														K		1.24		1.22			1.24	MPH154617										mT		0.2							T	RES, Linear approx.		1.6													A	from Hc2		140																																																							Er(3N5),Pd(4N),Bi(5N)		Bi-flux method. melt(alumina crucible with excess Bi) - heat(1150C,36h, in quartz tube, 0.3 bar Ar) - slow cool to 500C(3C/h)					Superconductivity and magnetic order in the noncentrosymmetric half-Heusler compound ErPdBi			Van der Waals - Zeeman Institute, University of Amsterdam - Science Park 904, 1098 XH Amsterdam, The Netherlands	Europhys.Lett., 104(2013)27001	Y. Pan,A. M. Nikitin,T. V. Bay,Y. K. Huang,C. Paulsen,B. H. Yan,A. de Visser		
154618	JPCM025155701	RRR = 27. Debye-T = 216 K by R(T). Lattice term in SP (beta) = 0.91 mJ/mol.K4. (dC/gamma*Tc) = 1.29. e-ph = 0.5	beta-IrSn4	Ir1Sn4	Ir	1	Sn	4																				3	2013																										AB4		MoSn4	I4<1>/acd		A	6.308		22.739												K	0.84	0.93	1			0.15	0.93											mT	M-H curve				3			0.5	mT	SP,RES,WHH	8.1							mT/K	RES,SP	9.83																	3.55	14				MSP154618			mJ/mol.K2	5.2	SP	221	SP											uOhm.cm							3				80			m3/C	0.000000000895						n/m3	6980000000000000000000000000	Ir(4N),Sn(5N)		self-flux method. mixture(Ir:Sn=1:80) - alumina crucible in sealed quartz tube - heat(900C) - cool to 600 C(5C/h) - FC to 300 C within 3h.					Observation of superconductivity in the intermetallic compound beta-IrSn4					Vinh Hung Tran,Zbigniew Bukowski		
154619	PRB088014526	not SC. RRR=15.3. Debye-T = 167K from R(T). lattice term in SP (beta) = 0.611 mJ/mol.K2. Kadowaki-Woods = 5.7E-3 mOhm.cm.mol2/J2	ScCo2As2	Sc1Co2As2	Sc	1	Co	2	As	2																		3	2013			cm3K/mol	0.65	myu-B/Co	1.61	-102																			AB2C2		ThCr2Si2	I4/mmm		A	3.9471		11.801											Fe-122	K					3																																																										mJ/mol.K2	37.8	SP	251	SP											uOhm.cm								12															Sr(3N5),Co(4N8),As(7N),Sn(5N)		Sn-flux method. mixture(Sr:Co:As:Sn=1:2:2:45) - alumina crucible - sealed in evacuated silica tube - heat(600C,5h) - heat(1150C,8h) - cool to 700C within 160h					Crystallographic, electronic, thermal, and magnetic properties of single-crystal SrCo2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 88(2013)014526	Abhishek Pandey,D. G. Quirinale,W. Jayasekara,A. Sapkota,M. G. Kim,R. S. Dhaka,Y. Lee,T. W. Heitmann,P. W. Stephens,V. Ogloblichev,A. Kreyssig,R. J. McQueeney,A. I. Goldman,Adam Kaminski,B. N. Harmon,Y. Furukawa,D. C. Johnston		
154620	SSC1810001	as-grown sample	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																													P4/nmm		A	4.071		13.3495												K	2.54	2.65		2.4			2.65																																																																																														La2S3,Bi2O3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat(700C,10h)					Correlation between crystal structure and superconductivity in LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Solid State Commun., 181(2014)1	J. Kajitani,K.Deguchi,A.Omachi,T.Hiroi,Y.Takano,H.Takatsu,H.Kadowaki,O. Miura,Y.Mizuguchi		
154621	SSC1810001	as-grown - high-P annealing(600C,2 GPa)	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																													P4/nmm																	K	7	7.92		6.9			7.92																																																																																														La2S3,Bi2O3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat(700C,10h)					Correlation between crystal structure and superconductivity in LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Solid State Commun., 181(2014)1	J. Kajitani,K.Deguchi,A.Omachi,T.Hiroi,Y.Takano,H.Takatsu,H.Kadowaki,O. Miura,Y.Mizuguchi		
154622	SSC1810001	as-grown - high-P annealing(600C,2 GPa) - post annealing(300C,10h). Tc extracted from R(T) plot.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																													P4/nmm																	K		5.43					5.43																																																																																														La2S3,Bi2O3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat(700C,10h)					Correlation between crystal structure and superconductivity in LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Solid State Commun., 181(2014)1	J. Kajitani,K.Deguchi,A.Omachi,T.Hiroi,Y.Takano,H.Takatsu,H.Kadowaki,O. Miura,Y.Mizuguchi		
154623	SSC1810001	as-grown - high-P annealing(600C,2 GPa) - post annealing(500C,10h). Tc extracted from R(T) plot.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																													P4/nmm																	K		4.51					4.51																																																																																														La2S3,Bi2O3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat(700C,10h)					Correlation between crystal structure and superconductivity in LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Solid State Commun., 181(2014)1	J. Kajitani,K.Deguchi,A.Omachi,T.Hiroi,Y.Takano,H.Takatsu,H.Kadowaki,O. Miura,Y.Mizuguchi		
154624	SSC1810001	as-grown - high-P annealing(600C,2 GPa) - post annealing(700C,10h). Tc extracted from R(T) plot.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																													P4/nmm																	K		2.75					2.75																																																																																														La2S3,Bi2O3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat(700C,10h)					Correlation between crystal structure and superconductivity in LaO0.5F0.5BiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Solid State Commun., 181(2014)1	J. Kajitani,K.Deguchi,A.Omachi,T.Hiroi,Y.Takano,H.Takatsu,H.Kadowaki,O. Miura,Y.Mizuguchi		
154625	SSC1830013	[penet] measured by muon-SR. GL = 94 using [cohere] = 17 nm(DB-data). Tc(SUS) = 0.80 K for H = 0.026 mT)	YPtBi	Y1Pt1Bi1	Y	1	Pt	1	Bi	1																		3	2014																										ABC			F4[-]3m																half-Heusler, MgAgAs-type	K		0.98		0.8		0.36	0.98										67	mT	M-H curve	0.0087																					MHC154625							um	muon-SR	1.6																																																	n/cm3	1300000000000000000			Bi-flux method					Low field magnetic response of the non-centrosymmetric superconductor YPtBi			Van der Waals-Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Solid State Commun., 183(2014)13	T.V.Bay,M.Jackson,C.Paulsen,C.Baines,A.Amato,T.Orvis,M.C.Aronson,Y.K.Huang,A.deVisser		
154626	SST027035005	GL = 4.42. Lattice term in SP (beta) = 0.293 mJ/mol.K4. e-ph = 0.62.	Nb2BN	Nb2B1N1	Nb	2	B	1	N	1																		1	2014																										ABC2		Mo2BN	cmcm																	K		4.4		4.4		0.1	4.4										60	Oe	M-H curve, GL fitting	93							Oe	WHH	2082												MHC154626		A	from Hc2	425			nm	from Hc1	188					3.45	14							mJ/mol.K2	6.3	SP	298	SP																																		Nb(4N,powder),BN(5N)		solid state reaction. BN degassed(1000C,24h,in vac) - mixture(Nb:BN=2:1) - pellet - sealed in quartz tube - heat(1200C) - ANN - Q to RT - pellet - heat(1200C,28d)					Conventional superconductivity properties of the ternary boron-nitride Nb2BN			Escola de Engenharia de Lorena, Universidade de Sao Paulo, PO Box 116, Lorena-SP, Brazil	Supercond.Sci.Technol., 27(2014)035005	O V Cigarroa,S T Renosto,A J S Machado		
154627	SSC1520666	Tn by SP.	CeNixBi2	Ce1Ni0.8Bi2	Ce	1	Ni	0.8	Bi	2																		1	2012								5																		ABC2		HfCuSi2	P4/nmm																	K	4.2						4.2										95																																														mJ/mol.K2	400																																							solid state reaction					Superconducting compounds with metallic square net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 152(2012)666	Hiroshi Mizoguchi,Toshio Kamiya,Hideo Hosono		
154628	SSC1520666	not SC.	LaCo2B2	La1Co2B2	La	1	Co	2	B	2																		1	2012																										AB2C2		ThCr2Si2																		K					1.8																																																																				uV/K	-7.4				uOhm.cm											70														arc-melting					Superconducting compounds with metallic square net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 152(2012)666	Hiroshi Mizoguchi,Toshio Kamiya,Hideo Hosono		
154629	SSC1520666		(La,Y)Co2B2	La0.9Y0.1Co2B2	La	0.9	Y	0.1	Co	2	B	2																1	2012																										AB2C2		ThCr2Si2																		K	4.1						4.1										15																																																																																						arc-melting					Superconducting compounds with metallic square net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 152(2012)666	Hiroshi Mizoguchi,Toshio Kamiya,Hideo Hosono		
154630	SSC1520666		La2Sb	La2Sb1	La	2	Sb	1																				1	2012																										AB2																				K		5.3					5.3										130																																																																																						solid state reaction					Superconducting compounds with metallic square net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Solid State Commun., 152(2012)666	Hiroshi Mizoguchi,Toshio Kamiya,Hideo Hosono		
154631	SSS0150123	not SC. T<SDW> = 144 K.	SmFeAsO	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9373		8.4913											Fe-1111	K					3																																																																																																Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154632	SSS0150123	not SC. T<SDW> = 88 K.	Sm(Fe,Ni)AsO	Sm1Fe0.99Ni0.01As1O1	Sm	1	Fe	0.99	Ni	0.01	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9375		8.4868											Fe-1111	K					3																																																																																																Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154633	SSS0150123	not SC. T<SDW> = 56 K.	Sm(Fe,Ni)AsO	Sm1Fe0.98Ni0.02As1O1	Sm	1	Fe	0.98	Ni	0.02	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9375		8.4794											Fe-1111	K					3																																																																																																Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154634	SSS0150123		Sm(Fe,Ni)AsO	Sm1Fe0.96Ni0.04As1O1	Sm	1	Fe	0.96	Ni	0.04	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9383		8.4719											Fe-1111	K		7.5					7.5																				T	RES(0.5Rn), GL-approx.	17.8												MHC154634																																																												Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154635	SSS0150123		Sm(Fe,Ni)AsO	Sm1Fe0.94Ni0.06As1O1	Sm	1	Fe	0.94	Ni	0.06	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9339		8.46											Fe-1111	K		9					9																				T	RES(0.5Rn), GL-approx.	16.9												MHC154635																																																												Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154636	SSS0150123		Sm(Fe,Ni)AsO	Sm1Fe0.92Ni0.08As1O1	Sm	1	Fe	0.92	Ni	0.08	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.94		8.4496											Fe-1111	K		6					6																																																																																														Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154637	SSS0150123	Tc < 3.	Sm(Fe,Ni)AsO	Sm1Fe0.9Ni0.1As1O1	Sm	1	Fe	0.9	Ni	0.1	As	1													O	1		1	2013																										ABCD		oxypnictide	P4/nmm		A	3.9411		8.4422											Fe-1111	K					3																																																																																																Sm,Fe2O3,Fe,Ni		solid state reaction. mixture - pellet - sealed in quartz tube - heat(550C,12h + 850C,12h) - heat(1150C,33h) - slow cool to RT					Appearance and disappearance of superconductivity in SmFe1-xNixAsO (x = 0.0 - 1.0)			Quamtum Phenomenon and Applications (QPA) Division, National Physical Laboratory (CS/R). Dr.K .S. Krishnan Marg, New Delhi 110012, India	Solid State Science, 15(2013)123	Anand Pal,S.S. Mehdi,Mushahid Husain,V.P.S. Awana		
154638	SSS0280031	T<CDW> = 50K and T<STR> = 47.7 K  from SUS(T) at H=2T.	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.111		8.07												K				1.2			1.2										100																																																																																				Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154639	SSS0280031	T<CDW> = 33K and  from SUS(T) at H=2T.	(Ba,K)Ti2Sb2O	Ba0.96K0.04Ti2Sb2O1	Ba	0.96	K	0.04	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.1079		8.0937												K				3.88			3.88										100																																																																																				Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154640	SSS0280031	T<CDW> = 32.3K ,and T<STR> = 30.8 K  from SUS(T) at H=2T.	(Ba,K)Ti2Sb2O	Ba0.95K0.05Ti2Sb2O1	Ba	0.95	K	0.05	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.1067		8.0972												K				4.25			4.25										100																																																																																				Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154641	SSS0280031	T<CDW> = 25.5K ,and T<STR> = 24.9 K  from SUS(T) at H=2T.	(Ba,K)Ti2Sb2O	Ba0.9K0.1Ti2Sb2O1	Ba	0.9	K	0.1	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.1047		8.1112												K				5.13			5.13	MPH154642									100																																																																																				Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154642	SSS0280031		(Ba,K)Ti2Sb2O	Ba0.88K0.12Ti2Sb2O1	Ba	0.88	K	0.12	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.1042		8.1121												K				6.1			6.1	MPH154642									100																																																																																				Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154643	SSS0280031		(Ba,K)Ti2Sb2O	Ba0.85K0.15Ti2Sb2O1	Ba	0.85	K	0.15	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.1008		8.1313												K				5.86			5.86																																																																																														Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154644	SSS0280031		(Ba,K)Ti2Sb2O	Ba0.8K0.2Ti2Sb2O1	Ba	0.8	K	0.2	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.0974		8.1444												K				3			3																																																																																														Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154645	SSS0280031	not SC.	(Ba,K)Ti2Sb2O	Ba0.7K0.3Ti2Sb2O1	Ba	0.7	K	0.3	Ti	2	Sb	2													O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.0899		8.1768												K					1.76																																																																																																Ba(4N),BaO2(4N),K(3N5),Sb(5N),Ti(2N5),		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154646	SSS0280031	not SC.	KTi2Sb2O	K1Ti2Sb2O1	K	1	Ti	2	Sb	2															O	1		1	2014																										ABC2D2		CeCr2Si2C			A	4.0454		8.4843												K					1.76																																																																																																Ba(4N),K(3N5),Sb(5N),Ti(2N5),TiO2		solid state reaction					Superconductivity in Ba1-xl<xTi2Sb2O (0 =< x =< 1) controlled by the layer charge			Department Chemie, Ludwig-Maximilians-Univesitat Munchen,Butenandstrasse  5-13 (Hans D),  81377 Munchen, Germany	Solid State Science, 28(2014)31	Ursula Pachmayr,Dirk Johrendt		
154700	PHC5040001	impurity phase: SrSnO3.	EuSr2(Ta,Sn)Cu2O8-z	Eu1Sr2Ta0.8Sn0.2Cu2O8-z	Eu	1	Sr	2	Ta	0.8	Sn	0.2	Cu	2											O	8-z		1	2014																											2	M1212			A	3.872		11.674											Ta-1212	K	13		40	40			40																																																																							mOhm.cm											11.6												Eu2O3,SrCO3,CuO,Ta2O5,SnO2		mixture - SIN(1000C,12h, in air) - reground - pellet  - SIN(1030C,24h, in air) - cool to RT - ANN(200-400C,48h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154701	PHC5040001	impurity phase: SrSnO3. not SC	NdSr2(Ta,Sn)Cu2O8-z	Nd1Sr2Ta0.8Sn0.2Cu2O8-z	Nd	1	Sr	2	Ta	0.8	Sn	0.2	Cu	2											O	8-z		1	2014																											2	M1212																	Ta-1212	K					2																																																																																																Eu2O3,SrCO3,CuO,Ta2O5,SnO2		mixture - SIN(1000C,12h, in air) - reground - pellet  - SIN(1030C,24h, in air) - cool to RT - ANN(200-400C,48h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154702	PHC5040001	impurity phase: SrSnO3.	SmSr2(Ta,Sn)Cu2O8-z	Sm1Sr2Ta0.8Sn0.2Cu2O8-z	Sm	1	Sr	2	Ta	0.8	Sn	0.2	Cu	2											O	8-z		1	2014																											2	M1212																	Ta-1212	K				30			30																																																																																														Eu2O3,SrCO3,CuO,Ta2O5,SnO2		mixture - SIN(1000C,12h, in air) - reground - pellet  - SIN(1030C,24h, in air) - cool to RT - ANN(200-400C,48h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154703	PHC5040001	not SC	EuSr2(Ta,Sn)Cu2O8-z	Eu1Sr2Ta0.9Sn0.1Cu2O8-z	Eu	1	Sr	2	Ta	0.9	Sn	0.1	Cu	2											O	8-z		1	2014																											2	M1212																	Ta-1212	K					2																																																																																																Eu2O3,SrCO3,CuO,Ta2O5,SnO2		mixture - SIN(1000C,12h, in air) - reground - pellet  - SIN(1030C,24h, in air) - cool to RT - ANN(200-400C,48h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154704	PHC5040008	Intercalated sample. M=EDA(ethylenediamine) = C2H8N2). LixMyFe2Se2: (x,y) not measured. Tc(SUS) = 45 K and lower Tc = 8K from FeSe.	Lix(C2H8N2)yFe2Se2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																1	2014																															A	3.458		20.74												K	18		43	45			45																																																																																																FeSe powder - placed in beaker with 0.2M-Li or Na in ethylenediamine(EDA) - heat(100-500C, 60h, in evacuated glass tube)					Synthesis and post-annealing effects of alkaline-metal-ethylenediamine intercalated superconductors Ax(C2H8N2)yFe2-zSe2 (A = Li, Na) with Tc = 45 K			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	Physica C, 504(2014)8	Takashi Noji,Takehiro Hatakeda,Shohei Hosono,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
154705	PHC5040008	Intercalated sample. M=EDA(ethylenediamine) = C2H8N2). NaxMyFe2Se2: (x,y) not measured.	Nax(C2H8N2)yFe2Se2	Na1M1Fe2Se2	Na	1	M	1	Fe	2	Se	2																1	2014																															A			21.9												K				45			45																																																																																																FeSe powder - placed in beaker with 0.2M-Li or Na in ethylenediamine(EDA) - heat(100-500C, 60h, in evacuated glass tube)					Synthesis and post-annealing effects of alkaline-metal-ethylenediamine intercalated superconductors Ax(C2H8N2)yFe2-zSe2 (A = Li, Na) with Tc = 45 K			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	Physica C, 504(2014)8	Takashi Noji,Takehiro Hatakeda,Shohei Hosono,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
154706	CEM1831710	As-nitrided sample. cation vacancy observed, then compositions are Nb0.6Al0.08(vac)0.32O0.21N0.79 by XRD.	(Nb,Al)(O,N)	Nb0.6Al0.08N0.79O0.21	Nb	0.6	Al	0.08	N	0.79															O	0.21			2010																											2		I4/m		A	6.874		4.346											tetragonal	K				7			7										23																																																																																						Ammonolysis throufg a citrate precursor, using Nb0.89Al0.11 oxynitrides.					Crystal structure and superconductive characteristics of Nb0.89Al0.11 oxynitrides			Graduate School of Engineering, Hokkaido University, Sapporo 060-8628, Japan	J.Solid State Chem., 183(2010)1710	Yoshio Ohashi,Teruk Motohashi,Yuji Masubuchi,Shinichi Kikkawa		
154707	CEM1831710	post annealed sample.	(Nb,Al)(O,N)	Nb0.89Al0.11N0.85O0.17	Nb	0.89	Al	0.11	N	0.85															O	0.17			2010																											1	NaCl	Fm-3m		A	4.401													cubic	K				17.3			17.3										91																																																																																						Ammonolysis throufg a citrate precursor, using Nb0.89Al0.11 oxynitrides. After nitridation , post-annealing (1773 K,3h, under 0.5MPa N2)					Crystal structure and superconductive characteristics of Nb0.89Al0.11 oxynitrides			Graduate School of Engineering, Hokkaido University, Sapporo 060-8628, Japan	J.Solid State Chem., 183(2010)1710	Yoshio Ohashi,Teruk Motohashi,Yuji Masubuchi,Shinichi Kikkawa		
154708	CEM1842061		(Nb,Mg)(N,O)	Nb0.95Mg0.05N0.92O0.08	Nb	0.95	Mg	0.05	N	0.92															O	0.08			2011																											1	NaCl	Fm-3m																	K				15			15										89																																																																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Preparation, crystalstructure, and superconductive characteristics of new oxynitrides (Nb1-xMx)(N1-yOy)  where M=Mg, Si, and  x nealy y			Graduate School of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo 060-8628, Japan	J.Solid State Chem., 184(2011)2061	Yoshio Ohashi,Teruki Motohashi,Yuji Masubuchi,Toshihiro Moriga,Keiichiro Murai,Shinichi Kikkawa		
154709	CEM1842061	post annealing at 1500 C.	(Nb,Mg)(N,O)	Nb0.95Mg0.05N0.92O0.08	Nb	0.95	Mg	0.05	N	0.92															O	0.08			2011																											1	NaCl	Fm-3m		A	4.419														K				17.6			17.6										100																																																																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Preparation, crystalstructure, and superconductive characteristics of new oxynitrides (Nb1-xMx)(N1-yOy)  where M=Mg, Si, and  x nealy y			Graduate School of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo 060-8628, Japan	J.Solid State Chem., 184(2011)2061	Yoshio Ohashi,Teruki Motohashi,Yuji Masubuchi,Toshihiro Moriga,Keiichiro Murai,Shinichi Kikkawa		
154710	CEM1842061		(Nb,Si)(N,O)	Nb0.9Mg0.1N0.87O0.13	Nb	0.9	Mg	0.1	N	0.87															O	0.13			2011																											1	NaCl	Fm-3m		A	4.37														K				5			5										8																																																																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Preparation, crystalstructure, and superconductive characteristics of new oxynitrides (Nb1-xMx)(N1-yOy)  where M=Mg, Si, and  x nealy y			Graduate School of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo 060-8628, Japan	J.Solid State Chem., 184(2011)2061	Yoshio Ohashi,Teruki Motohashi,Yuji Masubuchi,Toshihiro Moriga,Keiichiro Murai,Shinichi Kikkawa		
154711	CEM1842061	post annealing at 1200 C.	(Nb,Si)(N,O)	Nb0.9Mg0.1N0.87O0.13	Nb	0.9	Mg	0.1	N	0.87															O	0.13			2011																											1	NaCl	Fm-3m		A	4.41														K				16.2			16.2										95																																																																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Preparation, crystalstructure, and superconductive characteristics of new oxynitrides (Nb1-xMx)(N1-yOy)  where M=Mg, Si, and  x nealy y			Graduate School of Engineering, Hokkaido University, N13W8, Kita-ku, Sapporo 060-8628, Japan	J.Solid State Chem., 184(2011)2061	Yoshio Ohashi,Teruki Motohashi,Yuji Masubuchi,Toshihiro Moriga,Keiichiro Murai,Shinichi Kikkawa		
154712	CEM1880066		Nb(N,O)	Nb1N0.98O0.02	Nb	1	N	0.98																	O	0.02			2012																												NaCl			A	4.42														K				17.7			17.7																																																																																																Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Superconductivity in quaternary niobium oxynitrides containing main group elements (M=Mg,Al,Si)			Faculty of Engineering Hokkaido University, N13W8, Kita-ku, Sapporo, 060-8628, Japan	J.Solid State Chem., 188(2012)66	Yoshio Ohashi,Shinichi Kikkawa,I.Felner,M.I.Tsindlekht,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi		
154713	CEM1880066	gap size = 4.63 - 2.22 from SP heat using BCS theory.. (dC/gamma*Tc) = 44.4-3.65.	(Nb,Mg)(N,O)	Nb0.95Mg0.05N0.92O0.08	Nb	0.95	Mg	0.05	N	0.92															O	0.08			2012																												NaCl			A	4.419														K				17			17																				T	SUS, BCS approx.	8.22												MHC154713														4.63	14				MSP154713			mJ/mol.K2	0.18	SP																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Superconductivity in quaternary niobium oxynitrides containing main group elements (M=Mg,Al,Si)			Faculty of Engineering Hokkaido University, N13W8, Kita-ku, Sapporo, 060-8628, Japan	J.Solid State Chem., 188(2012)66	Yoshio Ohashi,Shinichi Kikkawa,I.Felner,M.I.Tsindlekht,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi		
154714	CEM1880066	gap size = 3.97 - 2.37 from SP heat using BCS theory..(dC/gamma*Tc) = 1.94-0.89	(Nb,Al)(N,O)	Nb0.89Al0.11N0.84O0.16	Nb	0.89	Al	0.11	N	0.84															O	0.16			2012																												NaCl			A	4.401														K				16.7			16.7																				T	SUS, BCS approx.	7.29												MHC154713														3.92	14				MSP154714			mJ/mol.K2	2.944	SP																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Superconductivity in quaternary niobium oxynitrides containing main group elements (M=Mg,Al,Si)			Faculty of Engineering Hokkaido University, N13W8, Kita-ku, Sapporo, 060-8628, Japan	J.Solid State Chem., 188(2012)66	Yoshio Ohashi,Shinichi Kikkawa,I.Felner,M.I.Tsindlekht,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi		
154715	CEM1880066	cation site vacancy: compositions = Nb0.87Si0.09(vac)0.04N0.87O0.13.  gap size = 3.05 from SP heat. .(dC/gamma*Tc) = 0.19-0.07	(Nb,Si)(N,O)	Nb0.87Si0.09N0.13O0.13	Nb	0.87	Si	0.09	N	0.13															O	0.13			2012																												NaCl			A	4.399														K				16.8			16.8																				T	SUS, BCS approx.	19.5												MHC154713														3.05	14				MSP154715			mJ/mol.K2	25.269	SP																																						Samples prepared at 1000C by ammonia nitridation of oxide precursor.					Superconductivity in quaternary niobium oxynitrides containing main group elements (M=Mg,Al,Si)			Faculty of Engineering Hokkaido University, N13W8, Kita-ku, Sapporo, 060-8628, Japan	J.Solid State Chem., 188(2012)66	Yoshio Ohashi,Shinichi Kikkawa,I.Felner,M.I.Tsindlekht,D.Venkateshwarlu,V.Ganesan,J.V.Yakhmi		
154716	CM0221503	impurity phases: SrF2,SrTiO3. R(T) anomaly at 380K due to M-I transition	(SrF)2Ti2As2O	Sr2F2Ti2As2O1	Sr	2	F	2	Ti	2	As	2													O	1		1	2010																											2		I4/mmm		A	4.04865		19.4204												K					2																																																																				uV/K	-8.022			MTP154716															m3/C	-0.00000000154					MRH154716			PrAs(PrSb),SrF2,Sm2O3,TiO2,As,Ti		solid state reaction. mixture - pellet - wrapped with Ta foil - sealed in quartz tube - SIN(1000 C,50h or 1150 C,50h)					Structure and Physical Properties of the Layered Pnictide-Oxides: (SrF)2Ti2Pn2O (Pn=As, Sb) and (SmO)2Ti2Sb2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's of Republic of China	Chem.Mater, 22(2010)1503	R.H.Liu,Y.A.Song,Q.J.Li,J.J.Ying,Y.J.Yan,Y.He,X.H.Chen		
154717	CM0221503	impurity phases: SrF2,SrTiO3. R(T) anomaly at 200K due to M-I transition. SP anomaly at 198 K. SP fitting for 3.1<T<14 K. lattice term in SP (beta) = 1.13 mJ/mol.K4.	(SrF)2Ti2Sb2O	Sr2F2Ti2Sb2O1	Sr	2	F	2	Ti	2	Sb	2													O	1		1	2010																											2		I4/mmm		A	4.1095		20.8858												K					2																																																										mJ/mol.K2	7.73	SP	249	SP						uV/K	-10.4			MTP154717															m3/C	-0.000000000175					MRH154717			PrAs(PrSb),SrF2,Sm2O3,TiO2,As,Ti		solid state reaction. mixture - pellet - wrapped with Ta foil - sealed in quartz tube - SIN(1000 C,50h or 1150 C,50h)					Structure and Physical Properties of the Layered Pnictide-Oxides: (SrF)2Ti2Pn2O (Pn=As, Sb) and (SmO)2Ti2Sb2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's of Republic of China	Chem.Mater, 22(2010)1503	R.H.Liu,Y.A.Song,Q.J.Li,J.J.Ying,Y.J.Yan,Y.He,X.H.Chen		
154718	CM0221503	R(T) anomaly at 230K due to M-I transition. SP anomaly at 230 K. SP fitting for 12<T<24 K. lattice term in SP (beta) = 0.72 mJ/mol.K4.	(SmO)2Ti2Sb2O	Sm2Ti2Sb2O3	Sm	2	Ti	2	Sb	2															O	3		1	2010								3.2																			2		I4/mmm		A	4.032		20.153												K					2																																																										mJ/mol.K2	170.15	SP	289	SP																																		PrAs(PrSb),SrF2,Sm2O3,TiO2,As,Ti		solid state reaction. mixture - pellet - wrapped with Ta foil - sealed in quartz tube - SIN(1000 C,50h or 1150 C,50h)					Structure and Physical Properties of the Layered Pnictide-Oxides: (SrF)2Ti2Pn2O (Pn=As, Sb) and (SmO)2Ti2Sb2O			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's of Republic of China	Chem.Mater, 22(2010)1503	R.H.Liu,Y.A.Song,Q.J.Li,J.J.Ying,Y.J.Yan,Y.He,X.H.Chen		
154719	EPJB0870131	alpha-phase(<2%). (dC/gamma*Tc) = 2	TixV1-x	Ti0.4V0.6	Ti	0.4	V	0.6																				1	2014																															A	3.07													beta-phase	K		7.46		7.62			7.46																				T	SUS, WHH	10.64							T/K	SUS	2.9			MHC154719																						mJ/mol.K2	10.35	SP	304	SP											uOhm.cm							61.55																Ti(4N),V(2N)		Ar-arc melting - ANN(1573 K,10h) - cool to 1273 K - Q to water					The influence of electron-phonon coupling and spin fluctuations on the superconductivity of the Ti-V alloys			Magnetic and Superconducting Materials Section, Raja Ramanna Center for Advanced Technology, Indore, 452 013 Madhya Pradesh, India	Eur. Phys. J. B., 87(2014)131	Md. Matin,L.S. Sharath Chandra,Sudhir K. Pandey,Maulindu Kumar Chattopadhyay,Sindhunil Barman Roy		
154720	EPJB0870131	(dC/gamma*Tc) = 2	TixV1-x	Ti0.6V0.4	Ti	0.6	V	0.4																				1	2014																															A	3.19													beta-phase	K		7.15		7.05			7.15																				T	SUS, WHH	13.5							T/K	SUS	3.94			MHC154720																						mJ/mol.K2	9.52	SP	260	SP											uOhm.cm							98.98																Ti(4N),V(2N)		Ar-arc melting - ANN(1573 K,10h) - cool to 1273 K - Q to water					The influence of electron-phonon coupling and spin fluctuations on the superconductivity of the Ti-V alloys			Magnetic and Superconducting Materials Section, Raja Ramanna Center for Advanced Technology, Indore, 452 013 Madhya Pradesh, India	Eur. Phys. J. B., 87(2014)131	Md. Matin,L.S. Sharath Chandra,Sudhir K. Pandey,Maulindu Kumar Chattopadhyay,Sindhunil Barman Roy		
154721	EPJB0870131	(dC/gamma*Tc) = 2	TixV1-x	Ti0.7V0.3	Ti	0.7	V	0.3																				1	2014																															A	3.21													beta-phase	K		7		6.6			7																				T	SUS, WHH	11.6							T/K	SUS	3.87			MHC154721																						mJ/mol.K2	9.12	SP	257	SP											uOhm.cm							129.78																Ti(4N),V(2N)		Ar-arc melting - ANN(1573 K,10h) - cool to 1273 K - Q to water					The influence of electron-phonon coupling and spin fluctuations on the superconductivity of the Ti-V alloys			Magnetic and Superconducting Materials Section, Raja Ramanna Center for Advanced Technology, Indore, 452 013 Madhya Pradesh, India	Eur. Phys. J. B., 87(2014)131	Md. Matin,L.S. Sharath Chandra,Sudhir K. Pandey,Maulindu Kumar Chattopadhyay,Sindhunil Barman Roy		
154722	EPJB0870131	(dC/gamma*Tc) = 1.63	TixV1-x	Ti0.8V0.2	Ti	0.8	V	0.2																				1	2014																															A	3.235													beta-phase	K		4.15		4.48			4.15																				T	SUS, WHH	8.68							T/K	SUS	4.43			MHC154722																						mJ/mol.K2	7.46	SP	286	SP											uOhm.cm							157.3																Ti(4N),V(2N)		Ar-arc melting - ANN(1573 K,10h) - cool to 1273 K - Q to water					The influence of electron-phonon coupling and spin fluctuations on the superconductivity of the Ti-V alloys			Magnetic and Superconducting Materials Section, Raja Ramanna Center for Advanced Technology, Indore, 452 013 Madhya Pradesh, India	Eur. Phys. J. B., 87(2014)131	Md. Matin,L.S. Sharath Chandra,Sudhir K. Pandey,Maulindu Kumar Chattopadhyay,Sindhunil Barman Roy		
154723	JPCM025176002		CePdBi	Ce1Pd1Bi1	Ce	1	Pd	1	Bi	1																		1	2013					myu-B/mol	2.23	0.5	2																		ABC			F4[-]3m		A	6.817													MgAgAs type	K	1.26	1.3					1.3										8										T	RES(zero), BCS approx.	1.4												MHC154723																									226	SP																																				arc-melting in Ar with Al getter. ANN(600 C,2w) 11 wt% excess Bi was added after 1st melting.					Experimental and theoretical study of CePdBi			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J. Phys.: Condens. Matter, 25(2013)176002	Jerzy Goraus,Andrej Slebarski,Marcin Fijalkowski		
154724	JPCM026025701	nominal=La0.28C0.72. 2nd phase=graphite(4%). (dC/Tc) = 3.47 mJ/mol.K2. Lattice term in SP (beta) = 0.2234 mJ/mol.K4. e-ph = 0.49.	LaC2	La1C2	La	1	C	2																				1	2014																										AB2					A	3.9364		6.5783												K				1.695			1.695																																																3.64	14				MSP154724			mJ/mol.K2	2.97	SP	296	SP																																		La(4N),C(3N8)		arc melting. using outgassed(950 C, overnight)-C . ANN(1300 C,10h)					Structure and bonding of superconducting LaC2			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	J. Phys.: Condens. Matter, 26(2014)025701	V Babizhetskyy,O Jepsen,R K Kremer,A Simon,B Ouladdiaf,A Stolovits		
154725	JPCM026025701	nominal = La0.35C0.65. 2nd phase= La2C3(9%).	LaC2	La1C2	La	1	C	2																				1	2014																										AB2					A	3.9324		6.5745												K				1.8			1.8																																																																																														La(4N),C(3N8)		arc melting. using outgassed(950 C, overnight)-C . ANN(1300 C,10h)					Structure and bonding of superconducting LaC2			Max-Planck-Institut fur Festkorperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany	J. Phys.: Condens. Matter, 26(2014)025701	V Babizhetskyy,O Jepsen,R K Kremer,A Simon,B Ouladdiaf,A Stolovits		
154726	JPCONF273012078	Tc by SP.	SrPdGe3	Sr1Pd1Ge3	Sr	1	Pd	1	Ge	3																		1	2011																										ABC3		BaNiSn3	I4mm		A	4.4677		10.2863												K		1.5					1.5																																																								mJ/mol.K2	5	SP																																						arc-melting. ANN(900C,100h, in sealed quartz tube)					Platinum metal silicides and germanides: superconductivity in non-centrosymmetric intermetallics			Institute of Physical Chemistry, University of Vienna, A-1090 Wien, Austria	J.Phys.:Conf.Ser., 273(2011)012078	K. Miliyanchuk,F. Kneidinger,C. Blaas-Schenner,D. Reith,R.Podloucky,P. Rogl,T. Khan,L. Salamakha,G. Hilscher,H.Michor,E. Bauer,A. D. Hillier		
154727	JPCONF273012078	SC properties calculated from muon-SR measurements.	BaPtSi3	Ba1Pt1Si3	Ba	1	Pt	1	Si	3																		1	2011																										ABC3		BaNiSn3	I4mm																	K		1.75					1.75																				T	muon-SR.	0.064														A	muon-SR.	72			A	muon-SR.	188																																																					arc-melting. ANN(900C,100h, in sealed quartz tube)					Platinum metal silicides and germanides: superconductivity in non-centrosymmetric intermetallics			Institute of Physical Chemistry, University of Vienna, A-1090 Wien, Austria	J.Phys.:Conf.Ser., 273(2011)012078	K. Miliyanchuk,F. Kneidinger,C. Blaas-Schenner,D. Reith,R.Podloucky,P. Rogl,T. Khan,L. Salamakha,G. Hilscher,H.Michor,E. Bauer,A. D. Hillier		
154728	JPCONF273012078	Tc by SP.	SrPtGe3	Sr1Pt1Ge3	Sr	1	Pt	1	Ge	3																		1	2011																										ABC3		BaNiSn3	I4mm		A	4.4859		10.1364												K		1					1																																																								mJ/mol.K2	4	SP																																						arc-melting. ANN(900C,100h, in sealed quartz tube)					Platinum metal silicides and germanides: superconductivity in non-centrosymmetric intermetallics			Institute of Physical Chemistry, University of Vienna, A-1090 Wien, Austria	J.Phys.:Conf.Ser., 273(2011)012078	K. Miliyanchuk,F. Kneidinger,C. Blaas-Schenner,D. Reith,R.Podloucky,P. Rogl,T. Khan,L. Salamakha,G. Hilscher,H.Michor,E. Bauer,A. D. Hillier		
154729	JPS0662163	ANN(900C,1w)	LaPdSi3	La1Pd1Si3	La	1	Pd	1	Si	3																		1	1997																										ABC3		BsNiSn3	I4mm	107	A	4.352		9.661												K		2.6					2.6																																																								mJ/mol.K2	5.3	SP	354	SP																																				arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154730	JPS0662163	ANN(900C,10d)	LaPd2Ge	La1Pd2Ge1	La	1	Pd	2	Ge	1																		1	1997																										ABC2		YPd2Si	Pnma	62	A	7.713	6.973	5.822												K					0.5																																																										mJ/mol.K2	5.5	SP	226	SP																																				arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154731	JPS0662163	ANN(800C,1w)	La2Pd3Ge5	La2Pd3Ge5	La	2	Pd	3	Ge	5																		1	1997																										A2B3C5		U2Co3Si5	Ibam	72	A	10.187	12.205	6.194												K					0.5																																																										mJ/mol.K2	9	SP	326	SP																																				arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154732	JPS0662163	ANN(800C,1w)	LaPd0.6Ge0.14	La1Pd0.6Ge0.14	La	1	Pd	0.6	Ge	0.14																		1	1997																										AB2		AlB2	P6/mmm	191	A	4.301		4.273												K		2.8					2.8																																																								mJ/mol.K2	4.7	SP	300	SP																																				arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154733	JPS0662163	ANN(900C,1w)	La2Pd3Si5	La2Pd3Si5	La	2	Pd	3	Si	5																		1	1997																										A2B3C5		U2Co3Si5	Ibam	72	A	9.996	11.902	6.011												K					0.5																																																										mJ/mol.K2	7	SP	424	SP																																				arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154734	JPS0662163	ANN(800C,2w). C(mJ/mol.K) = 170*T + 90*T^3 for T<2.5.	Ce2Pd3Si5	Ce2Pd3Si5	Ce	2	Pd	3	Si	5																		1	1997					myu-B/mol	2.51	-30	8.4																		A2B3C5		U2Co3Si5	Ibam	72	A	9.953	11.81	5.976												K					0.5																																																										mJ/mol.K2	170																																							arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154735	JPS0662163	ANN(900C,1w). C(mJ/mol.K) = 57*T + 194*T^3 for T<2. Two magnetic ordering- Temp (3K and 5.2K)	CePdSi3	Ce1Pd1Si3	Ce	1	Pd	1	Si	3																		1	1997					myu-B/mol	2.48	-26	5.2																		ABC3		BsNiSn3	I4mm	107	A	4.33		9.631												K					0.5																																																										mJ/mol.K2	57																																							arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154736	JPS0662163	ANN(800C,1w). C(mJ/mol.K) = 60*T + 252*T^3 for T<1.5. Two magnetic ordering- Temp (2.1K and 3.5K)	CePd0.5Si1.5	Ce1Pd0.5Si1.5	Ce	1	Pd	0.5	Si	1.5																		1	1997					myu-B/mol	2.54	-20	3.5																		AB2		AlB2	P6/mmm	191	A	4.152		4.361												K					0.5																																																										mJ/mol.K2	60																																							arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154737	JPS0662163	ANN(700C,1w). Spi glass-T = 2.7 K.	CePd0.4Si1.6	Ce1Pd0.4Si1.6	Ce	1	Pd	0.4	Si	1.6																		1	1997					myu-B/mol	2.54	-21																			AB2		AlB2	P6/mmm	191	A	4.134		4.373												K					0.5																																																																																																		arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154738	JPS0662163	ANN(900C,10d). magnetic order at 1.7K and 2K	CePd2Ge	Ce1Pd2Ge1	Ce	1	Pd	2	Ge	1																		1	1997																										ABC2		YPd2Si	Pnma	62	A	7.663	6.97	5.754												K					0.5																																																																																																		arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154739	JPS0662163	ANN(800C,1w). magnetic order at 3.9K	Ce2Pd3Ge5	Ce2Pd3Ge5	Ce	2	Pd	3	Ge	5																		1	1997																										A2B3C5		U2Co3Si5	Ibam	72	A	10.165	12.129	6.159												K					0.5																																																																																																		arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154740	JPS0662163	ANN(800C,1w). magnetic order at 5K	CePd0.75Al3.25	Ce1Pd0.75Al3.25	Ce	1	Pd	0.75	Al	3.25																		1	1997																										ABC3		PrNiGa3	I4/mmm	139	A	4.318		10.791												K					0.5																																																																																																		arc melting -ANN in evacuated quartz tube)					Low-Temperature Magnetic Properties of Several Compounds in Ce-Pd-X (X=Si, Ge and Al) Ternary Systems			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo	J.Phys.Soc.Jpn, 66(1997)2163	Jiro Kitagawa,Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
154741	JPS082044712		FeSe0.3Te0.7	Fe1Se0.3Te0.7	Fe	1	Se	0.3	Te	0.7																		3	2013																															A	3.8069		6.1368											Fe-11	K		14.5		14.5			14.5																																																																																					cm3/C	0.00225					MRH154741					Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154742	JPS082044712		(Fe,Co)Se0.3Te0.7	Fe0.99Co0.01Se0.3Te0.7	Fe	0.99	Co	0.01	Se	0.3	Te	0.7																3	2013																															A	3.8077		6.1287											Fe-11	K		13.3		13.8			13.3																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154743	JPS082044712		(Fe,Co)Se0.3Te0.7	Fe0.98Co0.02Se0.3Te0.7	Fe	0.98	Co	0.02	Se	0.3	Te	0.7																3	2013																															A	3.8074		6.1295											Fe-11	K		10.3		12.4			10.3																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154744	JPS082044712		(Fe,Co)Se0.3Te0.7	Fe0.97Co0.03Se0.3Te0.7	Fe	0.97	Co	0.03	Se	0.3	Te	0.7																3	2013																															A	3.8084		6.129											Fe-11	K		9.24		13.6			9.24																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154745	JPS082044712		(Fe,Co)Se0.3Te0.7	Fe0.95Co0.05Se0.3Te0.7	Fe	0.95	Co	0.05	Se	0.3	Te	0.7																3	2013																															A	3.8053		6.1219											Fe-11	K		8.2		9.71			8.2																																																																																					cm3/C	0.00163					MRH154741					Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154746	JPS082044712		(Fe,Ni)Se0.3Te0.7	Fe0.99Ni0.01Se0.3Te0.7	Fe	0.99	Ni	0.01	Se	0.3	Te	0.7																3	2013																															A	3.8081		6.1345											Fe-11	K		9.5		11.6			9.5																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154747	JPS082044712		(Fe,Ni)Se0.3Te0.7	Fe0.98Ni0.02Se0.3Te0.7	Fe	0.98	Ni	0.02	Se	0.3	Te	0.7																3	2013																															A	3.8079		6.1252											Fe-11	K		2.1		5.24			2.1																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154748	JPS082044712		(Fe,Ni)Se0.3Te0.7	Fe0.97Ni0.03Se0.3Te0.7	Fe	0.97	Ni	0.03	Se	0.3	Te	0.7																3	2013																															A	3.8082		6.122											Fe-11	K					2																																																																																																		Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154749	JPS082044712		(Fe,Ni)Se0.3Te0.7	Fe0.95Ni0.05Se0.3Te0.7	Fe	0.95	Ni	0.05	Se	0.3	Te	0.7																3	2013																															A	3.8065		6.1095											Fe-11	K					2																																																																																							cm3/C	0.00101					MRH154749					Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154750	JPS082044712		(Fe,Zn)Se0.3Te0.7	Fe0.99Zn0.01Se0.3Te0.7	Fe	0.99	Zn	0.01	Se	0.3	Te	0.7																3	2013																															A	3.8101		6.143											Fe-11	K		13		14.5			13																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154751	JPS082044712		(Fe,Zn)Se0.3Te0.7	Fe0.98Zn0.02Se0.3Te0.7	Fe	0.98	Zn	0.02	Se	0.3	Te	0.7																3	2013																															A	3.8071		6.1433											Fe-11	K		12		14.4			12																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154752	JPS082044712		(Fe,Zn)Se0.3Te0.7	Fe0.97Zn0.03Se0.3Te0.7	Fe	0.97	Zn	0.03	Se	0.3	Te	0.7																3	2013																															A	3.8093		6.1548											Fe-11	K		11.8		14.4			11.8																																																																																																Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154753	JPS082044712		(Fe,Zn)Se0.3Te0.7	Fe0.95Zn0.05Se0.3Te0.7	Fe	0.95	Zn	0.05	Se	0.3	Te	0.7																3	2013																															A	3.8115		6.1601											Fe-11	K		13.5		14.3			13.5																																																																																					cm3/C	0.00144					MRH154749					Bridgman method. ampoule - heat(600C,100h) - heat(950-1050 C,30h) - cool to 650C (2-3 C/h) - FC to RT - ANN(400C,200h)					Superconducting Symmetry Studied from Impurity Effects in Single-Crystal Fe1-yMySe0.3Te0.7 (M = Co, Ni, Zn)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)044712	Takuya INABE,Takayuki KAWAMATA,Takashi NOJI,Tadashi ADACHI,Yoji KOIKE		
154754	JPS082063702	Cu-intercalated Bi2Se3. SC for 0.03 =< x =< 0.5 in CuxBi2Se3.	CuxBi2Se3	Cu0.1Bi2Se3	Cu	0.1	Bi	2	Se	3																			2013																																														K	2.7		3.2				2.95										15																																																																																		n/cm3	100000000000000000000			Two step method. CuSe fiestly made. Then, final stoichiometric mixture - heat(900C, overnight) - keep(700C) - Q to cold water					Reproducible Synthetic Method for the Topological Superconductor CuxBi2Se3			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)063702	Ryusuke KONDO,Taiki YOSHINAKA,Yoshinori IMAI,Atsutaka MAEDA		
154755	JPS082063704	Tc(SP) = 3.84 K. (dC/Tc) = 8.60 mJ/mol.K2. (dC/gamma*Tc) = 1.57.	(Au,Pt)Te2	Au0.65Pt0.35Te2	Au	0.65	Pt	0.35	Te	2																			2013																										AB2	6	CdI2	P3[-]ml	164	A	4.1341		5.1535												K	4		4.2			0.09	4.1										71										T	R(0.5Rn), WHH	1.29							T/K	R(0.5Rn)	0.46			MHC154755		A	from Hc2	160															MSP154755			mJ/mol.K2	5.48	SP	187	SP											uOhm.cm							80																Au(4N),Pt(4N),Te(4N)		mixture - heat(500C, in quartz tube) - pellet - heat(430-460 C) - cool to RT. heating and cooling rate = 20 C/h)					Superconductivity Induced by Breaking Te2 Dimers of AuTe2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)063704	Kazutaka KUDO,Hiroyuki ISHII,Masaya TAKASUGA,Keita IBA,Seiya NAKANO,Jungeun KIM,Akihiko FUJIWARA,Minoru NOHARA		
154756	JPS082063704		AuTe2	Au1Te2	Au	1	Te	2																					2013																										AB2		CdI2	C2/m	12																K							1.8																																																								mJ/mol.K2	1.1	SP	182.2	SP											uOhm.cm							2.9																Au(4N),Pt(4N),Te(4N)		mixture - heat(500C, in quartz tube) - pellet - heat(430-460 C) - cool to RT. heating and cooling rate = 20 C/h)					Superconductivity Induced by Breaking Te2 Dimers of AuTe2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)063704	Kazutaka KUDO,Hiroyuki ISHII,Masaya TAKASUGA,Keita IBA,Seiya NAKANO,Jungeun KIM,Akihiko FUJIWARA,Minoru NOHARA		
154757	JPS082065002		LaPt2Ge2	La1Pt2Ge2	La	1	Pt	2	Ge	2																			2013																										AB2C2	4	CaBe2Ge2	P2<1>/c		A	10.037	4.508	8.987											monoclinic, beta = 90.72	K				0.41			0.41																																																																																														La(3N),Pt(5N),Ge(5N)		arc melting in Ar(6N) atmosphere - wrapped in Ta-foil - sealed in quartz tube - ANN(1000 C,3d) - slow cool to RT					Superconductivity in Tetragonal LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)065002	Satoki MAEDA,Kazuaki MATANO,Hiroki SAWAOKA,Yoshihiko INADA,Guo-qing ZHENG		
154758	JPS082065002		LaPt1.85Ge2.15	La1Pt1.85Ge2.15	La	1	Pt	1.85	Ge	2.15																			2013																										AB2C2		CaBe2Ge2	P4/nmm		A	4.396		10.031												K				1.85			1.85																																																																																														La(3N),Pt(5N),Ge(5N)		arc melting in Ar(6N) atmosphere - wrapped in Ta-foil - sealed in quartz tube - ANN(1000 C,3d) - slow cool to RT					Superconductivity in Tetragonal LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)065002	Satoki MAEDA,Kazuaki MATANO,Hiroki SAWAOKA,Yoshihiko INADA,Guo-qing ZHENG		
154759	JPS082065002		LaPt1.8Ge2.2	La1Pt1.8Ge2.2	La	1	Pt	1.8	Ge	2.2																			2013																										AB2C2		CaBe2Ge2	P4/nmm		A	4.395		10.05												K				1.95			1.95																																																																																														La(3N),Pt(5N),Ge(5N)		arc melting in Ar(6N) atmosphere - wrapped in Ta-foil - sealed in quartz tube - ANN(1000 C,3d) - slow cool to RT					Superconductivity in Tetragonal LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)065002	Satoki MAEDA,Kazuaki MATANO,Hiroki SAWAOKA,Yoshihiko INADA,Guo-qing ZHENG		
154760	JPS082073709	CDW around 200 K from R(T) and SUS(T). gap from NMR. Tc(H=4T) = 8.2 K.	Mo3Al2C	Al2C1Mo3	Al	2	C	1	Mo	3																		1	2013																										AB2C3		beta-Mn																		K		8.2					8.2																																																2.8	6																																															sparc plasma sintering. mixture - in carbon die - heat(600C,10min) - heatto 1300C for 1h - cool to RT. heating and cooling rate = 100C/min in flowing Ar					Normal and Superconducting Properties of the Noncentrosymmetric Mo3Al2C			Graduate School of Material Science, University of Hyogo, Kamigori, Hyogo 678-1297, Japan	J.Phys.Soc.Jpn, 82(2013)073709	Takehide KOYAMA,Yoshitaka MAEDA,Tomoaki YAMAZAKI,Ko-ichi UEDA,Takeshi MITO,Takao KOHARA,Takeshi WAKI,Yoshikazu TABATA,Hiroshi TSUNEMI,Mikio ITO,Hiroyuki NAKAMURA		
154761	JPS082074706	reduction. ANN(500C,48h, in vac).	Pr2Ba4Cu7O15-z	Pr2Ba4Cu7O14.44	Pr	2	Ba	4	Cu	7															O	15	14.44	1	2013																												Y247																		K	15		26.5				20.75																				T	R(on)	21												MHC154761																																uV/K				MTP154761																										sol-gel method. precursor - pellet - CAL(875-887 C,120-180 h, in O2)					Effect of Magnetic Field on the Superconducting Phase in the Electron-Doped Metallic Double-Chain Compound Pr2Ba4Cu7O15-z			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	J.Phys.Soc.Jpn, 82(2013)074706	Taiji CHIBA,Michiaki MATSUKAWA,Junki TADA,Satoru KOBAYASHI,Makoto HAGIWARA,Tsuyoshi MIYAZAKI,Kazuhiro SANO,Yoshiaki ONO,Takahiko SASAKI,Jun-ichi ECHIGOYA		
154762	JPS082074706	as-synthesized. no O2-reduction. not SC	Pr2Ba4Cu7O15-z	Pr2Ba4Cu7O15-z	Pr	2	Ba	4	Cu	7															O	15-z		1	2013																												Y247																		K					2																																																																				uV/K				MTP154762																										sol-gel method. precursor - pellet - CAL(875-887 C,120-180 h, in O2)					Effect of Magnetic Field on the Superconducting Phase in the Electron-Doped Metallic Double-Chain Compound Pr2Ba4Cu7O15-z			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	J.Phys.Soc.Jpn, 82(2013)074706	Taiji CHIBA,Michiaki MATSUKAWA,Junki TADA,Satoru KOBAYASHI,Makoto HAGIWARA,Tsuyoshi MIYAZAKI,Kazuhiro SANO,Yoshiaki ONO,Takahiko SASAKI,Jun-ichi ECHIGOYA		
154763	JAC2190313		(Sn,In)Te	Sn0.95In0.05Te1	Sn	0.95	In	0.05	Te	1																			1995																												NaCl																		K		1.21					1.21																				T		0.348																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154764	JAC2190313		(Pb,Sn,In)Te	Pb0.2375Sn0.7125In0.05Te1	Pb	0.2375	Sn	0.7125	In	0.05	Te	1																	1995																												NaCl																		K		2.66					2.66	MTC154764																			T		2.57												MHC154764																																																														metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154765	JAC2190313		(Pb,Sn,In)Te	Pb0.3325Sn0.6175In0.05Te1	Pb	0.3325	Sn	0.6175	In	0.05	Te	1																	1995																												NaCl																		K		1.61					1.61																				T		0.922																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154766	JAC2190313		(Pb,Sn,In)Te	Sn0.84In0.16Te1	Sn	0.84	In	0.16	Te	1																			1995																												NaCl																		K		2.14					2.14																				T		0.796																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154767	JAC2190313		(Pb,Sn,In)Te	Pb0.252Sn0.588In0.16Te1	Pb	0.252	Sn	0.588	In	0.16	Te	1																	1995																												NaCl																		K		3.92					3.92	MTC154764																			T		2.75												MHC154767																																																														metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154768	JAC2190313		(Pb,Sn,In)Te	Pb0.42Sn0.42In0.16Te1	Pb	0.42	Sn	0.42	In	0.16	Te	1																	1995																												NaCl																		K		4.21					4.21																				T		4.43																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154769	JAC2190313		(Sn,In)Te	Sn0.975In0.025Te1	Sn	0.975	In	0.025	Te	1																			1995																																														K		0.84					0.84																				T		0.221																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154770	JAC2190313		(Sn,In)Te	Sn0.92In0.08Te1	Sn	0.92	In	0.08	Te	1																			1995																																														K		1.36					1.36	MTC154770																			T		0.415												MHC154770																																																														metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154771	JAC2190313		(Sn,In)Te	Sn0.84In0.16Te1	Sn	0.84	In	0.16	Te	1																			1995																																														K		2.12					2.12																				T		0.77																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154772	JAC2190313		(Pb,Sn,In)Te	Pb0.196Sn0.784In0.02Te1	Pb	0.196	Sn	0.784	In	0.02	Te	1																	1995																																														K		1.68					1.68																				T		0.685																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154773	JAC2190313		(Pb,Sn,In)Te	Pb0.184Sn0.736In0.08Te1	Pb	0.184	Sn	0.736	In	0.08	Te	1																	1995																																														K		2.84					2.84	MTC154773																			T		2.52												MHC154773																																																														metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154774	JAC2190313		(Pb,Sn,In)Te	Pb0.16Sn0.64In0.2Te1	Pb	0.16	Sn	0.64	In	0.2	Te	1																	1995																																														K		3.31					3.31																				T		1.78																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154775	JAC2190313		(Pb,Sn,In)Te	Pb0.38Sn0.57In0.05Te1	Pb	0.38	Sn	0.57	In	0.05	Te	1																	1995																																														K		0.68					0.68																				T		0.471																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154776	JAC2190313		(Pb,Sn,In)Te	Pb0.352Sn0.528In0.12Te1	Pb	0.352	Sn	0.528	In	0.12	Te	1																	1995																																														K		3.6					3.6	MTC154776																			T		5.23												MHC154776																																																														metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154777	JAC2190313		(Pb,Sn,In)Te	Pb0.32Sn0.48In0.2Te1	Pb	0.32	Sn	0.48	In	0.2	Te	1																	1995																																														K		4.19					4.19																				T		2.9																																																																										metallocermic technique. ANN(650C)					Superconductivity and magnetism in In-doped lead-tin tellurides			A.F.Ioffe Physical Technical Institute, Russian Academy of Sciences, St.Petersburg, Russia	J.Alloys & Compd., 219(1995)313	R.V.Parfeniev,D.V.Shamshur,M.A.Shakhov,Zb.Chrapkiewiez		
154778	JPS082064715	several % impurity phases.	YPt2Si2	Y1Pt2Si2	Y	1	Pt	2	Si	2																		1	2013																										AB2C2		CaBe2Ge2			A	4.16		9.805												K			1.5				1.5																																																																							uOhm.cm							12																R(3N),Pt(3N),Si(5N)		arc-melting - ANN(1000 C,1w)					Charge Density Wave and Superconductivity of RPt2Si2 (R = Y, La, Nd, and Lu)			Department of Physics, Kyushu University, Fukuoka 812-8581, Japan	J.Phys.Soc.Jpn, 82(2013)064715	Yutaro NAGANO,Nobutaka ARAOKA,Akihiro MITSUDA,Hideki YAYAMA,Hirofumi WADA,Masaki ICHIHARA,Masahiko ISOBE,Yutaka UEDA		
154779	JPS082064715	T<CDW> = 112 K. Two step SC transition. T-O transition at 112 K. Orth-phase has a=6.0529, b=6.0396 A at 10 K.	LaPt2Si2	La1Pt2Si2	La	1	Pt	2	Si	2																		1	2013																										AB2C2		CaBe2Ge2			A	4.288		9.833												K	1.2		1.8				1.5																																																																							uOhm.cm							40				90												R(3N),Pt(3N),Si(5N)		arc-melting - ANN(1000 C,1w)					Charge Density Wave and Superconductivity of RPt2Si2 (R = Y, La, Nd, and Lu)			Department of Physics, Kyushu University, Fukuoka 812-8581, Japan	J.Phys.Soc.Jpn, 82(2013)064715	Yutaro NAGANO,Nobutaka ARAOKA,Akihiro MITSUDA,Hideki YAYAMA,Hirofumi WADA,Masaki ICHIHARA,Masahiko ISOBE,Yutaka UEDA		
154780	JPS082064715	T<CDW> = 77 K	NdPt2Si2	Nd1Pt2Si2	Nd	1	Pt	2	Si	2																		1	2013					myu-B/mol	3.62	-2.96																			AB2C2		CaBe2Ge2			A	4.23		9.78												K					2																																																																																																R(3N),Pt(3N),Si(5N)		arc-melting - ANN(1000 C,1w)					Charge Density Wave and Superconductivity of RPt2Si2 (R = Y, La, Nd, and Lu)			Department of Physics, Kyushu University, Fukuoka 812-8581, Japan	J.Phys.Soc.Jpn, 82(2013)064715	Yutaro NAGANO,Nobutaka ARAOKA,Akihiro MITSUDA,Hideki YAYAMA,Hirofumi WADA,Masaki ICHIHARA,Masahiko ISOBE,Yutaka UEDA		
154781	JPS082064715	several % impurity phases.	LuPt2Si2	Lu1Pt2Si2	Lu	1	Pt	2	Si	2																		1	2013																										AB2C2		CaBe2Ge2			A	4.092		9.922												K			1.9				1.9																																																																							uOhm.cm							40																R(3N),Pt(3N),Si(5N)		arc-melting - ANN(1000 C,1w)					Charge Density Wave and Superconductivity of RPt2Si2 (R = Y, La, Nd, and Lu)			Department of Physics, Kyushu University, Fukuoka 812-8581, Japan	J.Phys.Soc.Jpn, 82(2013)064715	Yutaro NAGANO,Nobutaka ARAOKA,Akihiro MITSUDA,Hideki YAYAMA,Hirofumi WADA,Masaki ICHIHARA,Masahiko ISOBE,Yutaka UEDA		
154782	JPS082074707	Metal to CDW/SDW transition at T* (RES) = 55K	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.1104		8.0864												K		1.19					1.19	MPH154784																																																																																													BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154783	JPS082074707	Tc not given.	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.9Sn0.1O1	Ba	1	Ti	2	Sb	1.9	Sn	0.1													O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.108		8.0777												K								MPH154784																																																																																													BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154784	JPS082074707	Tc(SP) = 2.29 K.  Metal to CDW/SDW transition at T* (RES) = 44.5 K	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.8Sn0.2O1	Ba	1	Ti	2	Sb	1.8	Sn	0.2													O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.1045		8.073												K		2.2					2.2	MPH154784																																																																																													BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154785	JPS082074707	Metal to CDW/SDW transition at T* (RES) = 40 K	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.7Sn0.3O1	Ba	1	Ti	2	Sb	1.7	Sn	0.3													O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.1005		8.0681												K		2.2					2.2	MPH154784																																																																																													BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154786	JPS082074707	Metal to CDW/SDW transition at T* (RES) =36.8 5K	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.6Sn0.4O1	Ba	1	Ti	2	Sb	1.6	Sn	0.4													O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.0998		8.058												K		2.31					2.31	MPH154784										Oe					15			1.85																																																																											BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154787	JPS082074707	Metal to CDW/SDW transition at T* (RES) = 30.9 K	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.4Sn0.6O1	Ba	1	Ti	2	Sb	1.4	Sn	0.6													O	1		1	2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.0954		8.0518												K		2.49					2.49	MPH154784																																																																																													BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154788	JPS082074707	Tc not given. Solubility limit : x = 0.3 in BaTi2(Sb1-xSnx)2O	BaTi2(Sb,Sn)2O	Ba1Ti2Sb1.2Sn0.8O1	Ba	1	Ti	2	Sb	1.2	Sn	0.8													O	1			2013																										ABC2D2		BaTi2Sb2O	P4/mmm		A	4.0982		8.0592												K																																																																																																					BaO(4N),Ti(3N),Sb(3N),Sn(3N)		mixture - pellet - wrapped in Ta foil - sealed in quartz tube - heat to 1000 C(50C/h) - hold(50h) - cool to RT(20C/h)					Tc Enhancement by Aliovalent Anionic Substitution in Superconducting BaTi2(Sb1-xSnx)2O			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 82(2013)074707	Kousuke NAKANO,Takeshi YAJIMA,Fumitaka TAKEIRI,Mark A. GREEN,James HESTER,Yoji KOBAYASHI,Hiroshi KAGEYAMA		
154789	JPS082074713	textured sample. surface plane=(110)//c-axis. Anisotropic s-wave SC. Anisotropic factor (Hc2) = 0.45. (dC/gamma*Tc) = 1.75. e-ph = 0.63. (2D/kTc) = 3.80 for s-wave fitting.	Sc5Ir4Si10	Sc5Ir4Si10	Sc	5	Ir	4	Si	10																		1	2013																										A4B5C10		Sc5Co4Si10																		K				8		0.2	8																				T	SUS, WHH		1.17	2.78					T/K	SUS		0.2	0.4	MHC154789														3.8	14				MSP154789			mJ/mol.K2	32.4	SP	371.5	SP																																				arc-melting					Specific Heat and Upper Critical Field of Sc5Ir4Si10 Superconductor			Department of Physics, Southeast University, Nanjing 211189, People's Republic of China	J.Phys.Soc.Jpn, 82(2013)074713	Yue SUN,Yi DING,Dongmei GU,Jinchen ZHUANG,Zhixiang SHI,Tsuyoshi TAMEGAI		
154790	JPS082105003	As-synthesized. not SC	Pr2Ba4Cu7O15-z	Pr2Ba4Cu7O15-z	Pr	2	Ba	4	Cu	7															O	15-z		1	2013																												Y247																		K					2																																																																																							cm3/C					7	MRH154790										Hall Coefficient in the Superconducting and Non-Superconducting Pr2Ba4Cu7O15-z Compounds with Metallic Double Chains			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	J.Phys.Soc.Jpn, 82(2013)105003	Junki TADA,Michiaki MATSUKAWA,Takahisa KONNO,Satoru KOBAYASHI,Makoto HAGIWARA,Tsuyoshi MIYAZAKI,Kazuhiro SANO,Yoshiaki ONO,Akiyuki MATSUSHITA		
154791	JPS082105003	reduced(500C,48h, in vac)	Pr2Ba4Cu7O15-z	Pr2Ba4Cu7O15-z	Pr	2	Ba	4	Cu	7															O	15-z		1	2013																												Y247																		K				27			27																																																																																					cm3/C					7	MRH154791										Hall Coefficient in the Superconducting and Non-Superconducting Pr2Ba4Cu7O15-z Compounds with Metallic Double Chains			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	J.Phys.Soc.Jpn, 82(2013)105003	Junki TADA,Michiaki MATSUKAWA,Takahisa KONNO,Satoru KOBAYASHI,Makoto HAGIWARA,Tsuyoshi MIYAZAKI,Kazuhiro SANO,Yoshiaki ONO,Akiyuki MATSUSHITA		
154792	JPS082113701	Nd0.98O0.7F0.3Bi0.98S2 by EPMA. I//ab plane. Hirr//ab = 16T, Hirr//c = 0.64T. Anisotropy(Hc2) = 32.3	Nd(O,F)BiS2	Nd1Bi1S2F0.3O0.7	Nd	1	Bi	1	S	2	F	0.3													O	0.7		3	2013																										ABCD2			P4/nmm	129	A	3.996		13.464											BiS2-plane	K	5		5.5				5.25																				T	R(onset), linear approx.		42	1.3										MHC154792																																																														CsCl/KCl flux method. mixture(nominal NdO0.7F0.3BiS2 + flux) - sealed in quartz tube - heat (800C,10h) - cool to 600C(0.5C/h) - FC to RT					Structural Analysis and Superconducting Properties of F-Substituted NdOBiS2 Single Crystals			Center for Crystal Science and Technology, University of Yamanashi, Kofu 400-8511, Japan	J.Phys.Soc.Jpn, 82(2013)113701	Masanori NAGAO,Satoshi DEMURA,Keita DEGUCHI,Akira MIURA,Satoshi WATAUCHI,Takahiro TAKEI,Yoshihiko TAKANO,Nobuhiro KUMADA,Isao TANAKA		
154793	JPS082113704	P-induced SC. Pcr = 1.77 GPa. 1st order phase transition (broad) at 2.61 GPa. RRR = 350.	AuTe2	Au1Te2	Au	1	Te	2																				3	2013																										AB2		CdI2	C2/m																	K		2.3			0		2.3	MPH154793																																																																						uOhm.cm								0.78															Au(4N),Te(4N)		mixture - sealed in quartz tube - heat to 470 C(18C/h) - heat to 600 C(6.5C/h) - cool to RT(11.5C/h)					Pressure-Induced Superconductivity in Mineral Calaverite AuTe2			Department of Physics, Kobe University, Kobe 658-8530, Japan	J.Phys.Soc.Jpn, 82(2013)113704	Shunsaku KITAGAWA,Hisashi KOTEGAWA,Hideki TOU,Hiroyuki ISHII,Kazutaka KUDO,Minoru NOHARA,Hisatomo HARIMA		
154794	JPS082114702	RRR = 560. Hydrostatic P. (dTc/dP) = 1.04 K/GPa (Tc by M) in DB,  = 0.71K/GPa (Tc by R).	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																		3	2013																		GPa		150						AB4C12		skutterudite	Im3[-]	204	A	7.8311														K	4.5		4.9	4.1		0.5	4.1	MTC154794		K/GPa	1.04	7																																																																																											Sn-flux method. mixture(La:Fe:P:Sn = 1:4:20:50) - sealed in vac - heat(1050C) - cool to 600C(1C/h) -					Pressure Effect on the Structure and Superconducting Transition Temperature of Filled Skutterudites LaT4P12 (T = Fe, Ru)			Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J.Phys.Soc.Jpn, 82(2013)114702	Yukihiro KAWAMURA,Takuma KAWAAI,Junichi HAYASHI,Chihiro SEKINE,Hirotada GOTOU,Jinguang CHENG,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
154795	JPS082114702	RRR = 7. Hydrostatic P. (dTc/dP) = -0.07 K/GPa for 0 < P <2 GPa ,  = -0.29 K/GPa for 6 < P < 8 GPa (Tc by R).	LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																		1	2013																		GPa		170						AB4C12		skutterudite	Im3[-]	204	A	8.05645														K		6.57					6.57	MTC154795		K/GPa	-0.07																																																																																												HTHP reaction (1050C,0.5h, P=4.5h)					Pressure Effect on the Structure and Superconducting Transition Temperature of Filled Skutterudites LaT4P12 (T = Fe, Ru)			Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J.Phys.Soc.Jpn, 82(2013)114702	Yukihiro KAWAMURA,Takuma KAWAAI,Junichi HAYASHI,Chihiro SEKINE,Hirotada GOTOU,Jinguang CHENG,Kazuyuki MATSUBAYASHI,Yoshiya UWATOKO		
154796	JPS082123702	Ca0.84La0.16Fe1.03As2.37 by EDS. novel 112-type SC.	(Ca,La)FeAs2	Ca0.9La0.1Fe1As2	Ca	0.9	La	0.1	Fe	1	As	2																3	2013																										ABC2			P2<1>	4	A	3.9471	3.8724	10.321											monoclinic, alpha=90,beta=91.415, gamma=90. HfCuSi2-type, Fe-112	K	36		39	34		2.4	34										66																																																																																				Ca,La,FeAs,As		mixture - in Al crucible - sealed in quartz tube - heat(700C,3h) - heat to 1100C and cool to 1050C at 1.25C/h) - FC to RT					Superconductivity in Ca1-xLaxFeAs2: A Novel 112-Type Iron Pnictide with Arsenic Zigzag Bonds			Department of Applied Physics, Nagoya University, Nagoya 464-8603, Japan	J.Phys.Soc.Jpn, 82(2013)123702	Naoyuki KATAYAMA,Kazutaka KUDO,Seiichiro ONARI,Tasuku MIZUKAMI,Kento SUGAWARA,Yuki SUGIYAMA,Yutaka KITAHAMA,Keita IBA,Kazunori FUJIMURA,Naoki NISHIMOTO,Minoru NOHARA,Hiroshi SAWA		
154797	JPS082123702	Ca0.81La0.19Fe1.03As2.34 by EDS. High-Tc(45K) SC observed. Fe-112	(Ca,La)FeAs2	Ca0.79La0.21Fe1As2	Ca	0.79	La	0.21	Fe	1	As	2																3	2013																										ABC2			P2<1>	4															Fe-112	K	25		45	25			25																																																																																														Ca,La,FeAs,As		mixture - in Al crucible - sealed in quartz tube - heat(700C,3h) - heat to 1100C and cool to 1050C at 1.25C/h) - FC to RT					Superconductivity in Ca1-xLaxFeAs2: A Novel 112-Type Iron Pnictide with Arsenic Zigzag Bonds			Department of Applied Physics, Nagoya University, Nagoya 464-8603, Japan	J.Phys.Soc.Jpn, 82(2013)123702	Naoyuki KATAYAMA,Kazutaka KUDO,Seiichiro ONARI,Tasuku MIZUKAMI,Kento SUGAWARA,Yuki SUGIYAMA,Yutaka KITAHAMA,Keita IBA,Kazunori FUJIMURA,Naoki NISHIMOTO,Minoru NOHARA,Hiroshi SAWA		
154798	JPS082123705	M= C2H8N2: ethylenediamine(EDA). as-intercalated sample. compositions (x,y,z) not shown. lower Tc = 8 K from non-intercalated regin(FAs)	LixMyFe2-zSe2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2013																															A	3.458		20.74												K				45			45																																																																																																EDA-intercalation as follows. poly-FeAs powder - placed in beaker with 0.2M Li-metal dessolved in EDA. Li:FeAs = 1:2					New Li-Ethylenediamine-Intercalated Superconductor Lix(C2H8N2)yFe2-zSe2 with Tc = 45K			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)123705	Takehiro HATAKEDA,Takashi NOJI,Takayuki KAWAMATA,Masatsune KATO,Yoji KOIKE		
154799	JPS082123705	M= C2H8N2: Vethylenediamine(EDA). intercalated sample. post-ANN(150C,60h). compositions (x,y,z) not shown 8K and 18K Tc phase observed.	LixMyFe2-zSe2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2013																															A	3.438		20.92												K				41			41																																																																																																EDA-intercalation as follows. poly-FeAs powder - placed in beaker with 0.2M Li-metal dessolved in EDA. Li:FeAs = 1:2					New Li-Ethylenediamine-Intercalated Superconductor Lix(C2H8N2)yFe2-zSe2 with Tc = 45K			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)123705	Takehiro HATAKEDA,Takashi NOJI,Takayuki KAWAMATA,Masatsune KATO,Yoji KOIKE		
154800	JPS082123705	M= C2H8N2: ethylenediamine(EDA). intercalated sample. as sintered(200C,20h). compositions (x,y,z) not shown	LixMyFe2-zSe2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2013																															A	3.436		20.92												K	18		43	35			35																																																																																																EDA-intercalation as follows. poly-FeAs powder - placed in beaker with 0.2M Li-metal dessolved in EDA. Li:FeAs = 1:2					New Li-Ethylenediamine-Intercalated Superconductor Lix(C2H8N2)yFe2-zSe2 with Tc = 45K			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 82(2013)123705	Takehiro HATAKEDA,Takashi NOJI,Takayuki KAWAMATA,Masatsune KATO,Yoji KOIKE		
154801	JPS082124703	RR=10.9. Hc(0) = 389 Oe. GL(kappa) = 7.6. (dC/gamma*Tc) = 1.26. R=R0+A*T^2 (A=4.8 uOhm.cm/K). lattice term in SP (beta) = 0.373 mJ/mol.K4.	LuRu2	Lu1Ru2	Lu	1	Ru	2																				1	2013	emu/mol	0.000439																								AB2	7	Laves			A	5.211		8.73											Laves(C14, hexagonal)	K		2.23					2.23											Oe	M-H curve,parabolic.	80							T	RES, WHH	0.231							T/K	RES	0.149			MHC154801		A	from Hc2	378			A	from Hc1	2870			meV	0.322	3.35	14				MSP154801			mJ/mol.K2	17.5	SP	250	SP																																		Ru(4N),Lu(3N),Y(3N),Sc(3N)		arc-melting several times. ANN(1000C,2w, in evacuated silica)					Comprehensive Macroscopic Investigation on Hexagonal C14 Laves-Type Ru-Based Superconductors ARu2 (A = Lu, Y, Sc) with Effective Electron Correlation			RIKEN, Wako, Saitama 351-0198, Japan	J.Phys.Soc.Jpn, 82(2013)124703	Seiji NIITAKA,Emi MINAMITANI,Yousoo KIM,Hidenori TAKAGI,Kimitoshi KONO		
154802	JPS082124703	RR=10.3. Hc(0) = 460 Oe. GL(kappa) = 7.9. (dC/gamma*Tc) = 1.18. R=R0+A*T^2 (A=6.2 uOhm.cm/K). lattice term in SP (beta) = 0.220 mJ/mol.K4.	YRu2	Ru2Y1	Ru	2	Y	1																				1	2013	emu/mol	0.000458																								AB2	7	Laves			A	5.226		8.799											Laves(C14, hexagonal)	K		2.75					2.75											Oe	M-H curve,parabolic.	121							T	RES, WHH	0.375							T/K	RES	0.197			MHC154802		A	from Hc2	296			A	from Hc1	2330			meV	0.383	3.23	14				MSP154802			mJ/mol.K2	17.8	SP	298	SP																																		Ru(4N),Lu(3N),Y(3N),Sc(3N)		arc-melting several times. ANN(1000C,2w, in evacuated silica)					Comprehensive Macroscopic Investigation on Hexagonal C14 Laves-Type Ru-Based Superconductors ARu2 (A = Lu, Y, Sc) with Effective Electron Correlation			RIKEN, Wako, Saitama 351-0198, Japan	J.Phys.Soc.Jpn, 82(2013)124703	Seiji NIITAKA,Emi MINAMITANI,Yousoo KIM,Hidenori TAKAGI,Kimitoshi KONO		
154803	JPS082124703	RR=39.1. Hc(0) = 413 Oe. GL(kappa) = 4.1. (dC/gamma*Tc) = 1.28. R=R0+A*T^2 (A=1.6 uOhm.cm/K). lattice term in SP (beta) = 0.067 mJ/mol.K4.	ScRu2	Ru2Sc1	Ru	2	Sc	1																				1	2013	emu/mol	0.000455																								AB2	7	Laves			A	5.115		8.54											Laves(C14, hexagonal)	K		2.36					2.36											Oe	M-H curve,parabolic.	166							T	RES, WHH	0.139							T/K	RES	0.085			MHC154803		A	from Hc2	486			A	from Hc1	1990			meV	0.345	3.39	14				MSP154803			mJ/mol.K2	16.3	SP	442	SP																																		Ru(4N),Lu(3N),Y(3N),Sc(3N)		arc-melting several times. ANN(1000C,2w, in evacuated silica)					Comprehensive Macroscopic Investigation on Hexagonal C14 Laves-Type Ru-Based Superconductors ARu2 (A = Lu, Y, Sc) with Effective Electron Correlation			RIKEN, Wako, Saitama 351-0198, Japan	J.Phys.Soc.Jpn, 82(2013)124703	Seiji NIITAKA,Emi MINAMITANI,Yousoo KIM,Hidenori TAKAGI,Kimitoshi KONO		
154804	JPS083013707	Tc  > Tn. Tc(SP) = 1.84 K.  Tn measured by specific heat(SP) and neutron scattering.	(Ce,Nd)CoIn5	Ce0.95Nd0.05Co1In5	Ce	0.95	Nd	0.05	Co	1	In	5																3	2014								0.9																		ABC5		HoCoGa5																		K			1.9				1.9																																																					MSP154804																																											self-flux method					Magnetic Order in Ce0.95Nd0.05CoIn5: The Q-Phase at Zero Magnetic Field			SPSMS, UMR-E 9001, CEA-INAC/UJF-Grenoble 1, 38054 Grenoble, France	J.Phys.Soc.Jpn, 83(2014)013707	Stephane Raymond,Scheilla M. Ramos,Dai Aoki,Georg Knebel,Vladimir P. Mineev,Gerard Lapertot		
154805	JPS083013707	no magnetic order.	(Ce,La)CoIn5	Ce0.965La0.035Co1In5	Ce	0.965	La	0.035	Co	1	In	5																3	2014																										ABC5		HoCoGa5																		K		1.84					1.84																																																					MSP154805																																											self-flux method					Magnetic Order in Ce0.95Nd0.05CoIn5: The Q-Phase at Zero Magnetic Field			SPSMS, UMR-E 9001, CEA-INAC/UJF-Grenoble 1, 38054 Grenoble, France	J.Phys.Soc.Jpn, 83(2014)013707	Stephane Raymond,Scheilla M. Ramos,Dai Aoki,Georg Knebel,Vladimir P. Mineev,Gerard Lapertot		
154806	JPS083014709	not SC	SrFBiS2	Sr1Bi1S2F1	Sr	1	Bi	1	S	2	F	1																1	2014																										ABCD2			P4/nmm		A	4.0833		13.808												K					1.8																																																																																																SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154807	JPS083014709	not SC	(Sr,La)FBiS2	Sr0.75La0.25Bi1S2F1	Sr	0.75	La	0.25	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0753		13.4994												K					1.8																																																																																																SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154808	JPS083014709	not SC	(Sr,La)FBiS2	Sr0.6La0.4Bi1S2F1	Sr	0.6	La	0.4	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0811		13.3587												K					1.8																																																																																																SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154809	JPS083014709	R(1.8K) not zero.	(Sr,La)FBiS2	Sr0.58La0.42Bi1S2F1	Sr	0.58	La	0.42	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0819		13.3344												K	1.71	2.13					2.13																																																																																														SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154810	JPS083014709	RH(4K)= positive value(hole). gamma = 1.2 mJ/mol.K2 after SC volume correction.  (dC/gamma*Tc) = 1.1.	(Sr,La)FBiS2	Sr0.55La0.45Bi1S2F1	Sr	0.55	La	0.45	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0851		13.3269												K	3	3.1					3.1	MTC154810									75																																														mJ/mol.K2	1.6	SP																											cm3/C						MRH154810			SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154811	JPS083014709	impurity phase: Bi. RH(4K)= positive value(hole).	(Sr,La)FBiS2	Sr0.5La0.5Bi1S2F1	Sr	0.5	La	0.5	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0839		13.3219												K	2.85	3.04					3.04																																																								mJ/mol.K2	1.3	SP																											cm3/C									SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154812	JPS083014709	impurity phase: Bi. RH(4K) = -8.3 E-2 cm3/C.	(Sr,La)FBiS2	Sr0.4La0.6Bi1S2F1	Sr	0.4	La	0.6	Bi	1	S	2	F	1														1	2014																										ABCD2			P4/nmm		A	4.0815		13.3025												K	2.67	2.96					2.96																																																																																														SrF2,SrS,LaF3,LaS3,Bi,S		mixture - pellet - heat(600C,10h, in evacuated quartz)					Insulator-to-Superconductor Transition upon Electron Doping in a BiS2-Based Superconductor Sr1-xLaxFBiS2			Department of Applied Physics, University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 83(2014)014709	Hideaki Sakai,Daichi Kotajima,Kosuke Saito,Hiroki Wadati,Yuki Wakisaka,Masaichiro Mizumaki,Kiyofumi Nitta,Yoshinori Tokura,Shintaro Ishiwata		
154813	JPS083033705	not SC. R(T) anomaly at 95.8 K. La-content = 0 by EPMA. H-content = 1.0 by TDS. O-content = 0.06 by EPMA.	CaFeAsH	Ca1Fe1As1H1	Ca	1	Fe	1	As	1	H	1																	2014																										ABCD		oxypnictide	P4/nmm		A	3.8785		8.2551											ZrCuSiAs-type. Fe-1111	K					5																																																																																																		mixture(CaH2,LaH2,FeAs,Ca(OH)2,NaBH4) - in BN capsule - in stainless capsule - heat(1173K,30min, P=2.5 GPa)					La-Substituted CaFeAsH Superconductor with Tc = 47K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Phys.Soc.Jpn, 83(2014)033705	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
154814	JPS083033705	La-content = 0.85 by EPMA. H-content = 0.952 by TDS. O-content = 0.081 by EPMA.	(Ca,La)FeAsH	Ca0.9La0.1Fe1As1H1	Ca	0.9	La	0.1	Fe	1	As	1	H	1															2014																										ABCD		oxypnictide	P4/nmm		A	3.8918		8.2671											ZrCuSiAs-type. Fe-1111	K			47	28.2		10	28.2																																																																																																mixture(CaH2,LaH2,FeAs,Ca(OH)2,NaBH4) - in BN capsule - in stainless capsule - heat(1173K,30min, P=2.5 GPa)					La-Substituted CaFeAsH Superconductor with Tc = 47K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Phys.Soc.Jpn, 83(2014)033705	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
154815	JPS083033705	La-content = 0.203 by EPMA. H-content = 0.937 by TDS. O-content = 0.099 by EPMA.	(Ca,La)FeAsH	Ca0.8La0.2Fe1As1H1	Ca	0.8	La	0.2	Fe	1	As	1	H	1															2014																										ABCD		oxypnictide	P4/nmm		A	3.9075		8.2728											ZrCuSiAs-type. Fe-1111	K			47.4	40.6			40.6																																																																																																mixture(CaH2,LaH2,FeAs,Ca(OH)2,NaBH4) - in BN capsule - in stainless capsule - heat(1173K,30min, P=2.5 GPa)					La-Substituted CaFeAsH Superconductor with Tc = 47K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Phys.Soc.Jpn, 83(2014)033705	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
154816	JPS083033705	La-content = 313 by EPMA. H-content = 0.944 by TDS. O-content = 0.1 by EPMA.	(Ca,La)FeAsH	Ca0.7La0.3Fe1As1H1	Ca	0.7	La	0.3	Fe	1	As	1	H	1															2014																										ABCD		oxypnictide	P4/nmm		A	3.9177		8.3067											ZrCuSiAs-type. Fe-1111	K			47	35.7			35.7																																																																																																mixture(CaH2,LaH2,FeAs,Ca(OH)2,NaBH4) - in BN capsule - in stainless capsule - heat(1173K,30min, P=2.5 GPa)					La-Substituted CaFeAsH Superconductor with Tc = 47K			Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Phys.Soc.Jpn, 83(2014)033705	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
154817	JPS083044702	RRR=1.5. not-SC hexagonal Cr-Re alloy phase(30 mol%) by XRD. gamma = 11.2 mJ/mol.K2 using alpha-model. (dC/gamma*Tc) = 2.11. GL = 62.5. beta in SP = 0.51 mJ/mol.K4	Cr2Re3B	Cr2Re3B1	Cr	2	Re	3	B	1																		1	2014																										AB2C3		beta-Mn	P4<1>32	213	A	6.61														K	4.8		5.3	4.8			4.8										15	Oe	M-H curve,parabolic.	52							T	R(zero), Hc2=Hc2(0)(1-t^(1.5))^(1.5)	10												MHC154817		A	from Hc2	57			A	from Hc1. Hc1(0)=fai0/(pai*penet^2)	3560					3.66	14							mJ/mol.K2	18	SP																																				Cr(4N),Re(4N),B(2N)		arc-melting					Superconductivity in the Ternary Boride Cr2Re3B with the beta-Mn-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 83(2014)044702	Haru Niimura,Kenji Kawashima,Keigo Inoue,Masaaki Yoshikawa,Jun Akimitsu		
154818	JPS083073703	P-induced SC. Tc(max) = 14.7 K at P=3.0 GPa.. Pcr = 1.8 GPa. Tn measured by SUS for H//c.	SrCa13Cu24O41	Sr1Ca13Cu24O41	Sr	1	Ca	13	Cu	24															O	41		3	2014								4.2																				LAD																	two-leg ladder	K			14.7	11.8			11.8	MTC154818																																																																																															single crysta grown with 63.2% powder of four 300W halogen lamps using modified mirror floating zone furnace(35 bar O2)					Superconductivity on a Crossover Phenomenon of Spin-Ladder System SrCa13Cu24O41 Single Crystals			Institute of Socio-Arts and Sciences, The University of Tokushima, Tokushima 770-8502, Japan	J.Phys.Soc.Jpn, 83(2014)073703	Akihiko Hisada,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Naoki Fujiwara,Guochu Deng,Ekaterina Pomjakushina,Kazimierz Conder,Dinadhayalane Mohan Radheep,Raman Thiyagarajan,Sankaran Esakkimuthu,Sonachalam Arumugam		
154819	JPS083073705	T<CDW> measured by R(T). Ortho to monoclinic transition at 230 K.	Ba2Bi(Sb1-xBix)2	Ba2Bi1Sb2	Ba	2	Bi	1	Sb	2																			2014																											3				A	4.8067	7.6717	9.8968												K					1.8																																																																																																Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154820	JPS083073705	T<CDW> measured by R(T).	Ba2Bi(Sb1-xBix)2	Ba2Bi1.25Sb1.75	Ba	2	Bi	1.25	Sb	1.75																			2014																											3				A	4.8091	7.6903	9.9027												K					1.8																																																																																																Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154821	JPS083073705	T<CDW> measured by R(T).	Ba2Bi(Sb1-xBix)2	Ba2Bi1.5Sb1.5	Ba	2	Bi	1.5	Sb	1.5																			2014																											3				A	4.8115	7.7325	9.9095												K					1.8																																																																																																Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154822	JPS083073705	T<CDW> measured by R(T).	Ba2Bi(Sb1-xBix)2	Ba2Bi1.75Sb1.25	Ba	2	Bi	1.75	Sb	1.25																			2014																											3				A	4.8115	7.7723	9.9126												K		3.51					3.51																																																																																														Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154823	JPS083073705	T<CDW> measured by R(T).	Ba2Bi(Sb1-xBix)2	Ba2Bi2Sb1	Ba	2	Bi	2	Sb	1																			2014																											3				A	4.8125	7.8117	9.9158												K		3.92					3.92	MTC154823																																																																																													Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154824	JPS083073705		Ba2Bi(Sb1-xBix)2	Ba2Bi2.25Sb0.75	Ba	2	Bi	2.25	Sb	0.75																			2014																											3				A	4.8139	7.8656	9.9339												K		4.06					4.06																																																																																														Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154825	JPS083073705		Ba2Bi(Sb1-xBix)2	Ba2Bi2.5Sb0.5	Ba	2	Bi	2.5	Sb	0.5																			2014																											3				A	4.8148	7.9151	9.9452												K		4.25					4.25																																																																																														Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154826	JPS083073705		Ba2Bi(Sb1-xBix)2	Ba2Bi2.75Sb0.25	Ba	2	Bi	2.75	Sb	0.25																			2014																											3				A	4.816	7.9579	9.9615												K		4.46					4.46																																																																																														Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154827	JPS083073705		Ba2Bi(Sb1-xBix)2	Ba2Bi3	Ba	2	Bi	3																					2014																											3				A	4.8188	7.9991	9.9756												K		4.48					4.48																																																																																														Ba(2N),Bi(3N),Sb(3N)		solid state rection. mixture(Bi+Sb) - pellet - (pellet+Ba) - sealed in quartz tube - heat to 800C(100C/h) - keep (72h) - cool to RT (100C/h)					Superconductivity in the Hypervalent Compound Ba2Bi(Sb1-xBix)2 with a Square-Honeycomb Lattice			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Phys.Soc.Jpn, 83(2014)073705	Takeshi Yajima,Fumitaka Takeiri,Yasumasa Nozaki,Zhi Li,Takami Tohyama,Mark A. Green,Yoji Kobayashi,Hiroshi Kageyama		
154828	JPS083074713		ZrP2-xSex	Zr1P1.5Se0.5	Zr	1	P	1.5	Se	0.5																		1	2014																										ABC	2	PbFCl	P4/nmm		A	3.626		7.906												K				5.76			5.76																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154829	JPS083074713		ZrP2-xSex	Zr1P1.35Se0.65	Zr	1	P	1.35	Se	0.65																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				6.24			6.24	MTC154829																																																																																															mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154830	JPS083074713		ZrP2-xSex	Zr1P1.25Se0.75	Zr	1	P	1.25	Se	0.75																		1	2014																										ABC	2	PbFCl	P4/nmm																	K	6.5			6.3			6.3	MTC154829									129	Oe	M-H curve				210			2	T	R(onset), WHH	2.92							T/K	R(onset)	0.65			MHC154830																																					mOhm.cm							0.23																		mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154831	JPS083074713		ZrP2-xSex	Zr1P1.1Se0.9	Zr	1	P	1.1	Se	0.9																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				5.34			5.34																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154832	JPS083074713		ZrP2-xSex	Zr1P0.6Se1.4	Zr	1	P	0.6	Se	1.4																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				4.11			4.11																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154833	JPS083074713		ZrP2-xSx	Zr1P1.6S0.4	Zr	1	P	1.6	S	0.4																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				4.36			4.36																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154834	JPS083074713		ZrP2-xSx	Zr1P1.4S0.6	Zr	1	P	1.4	S	0.6																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				4.99			4.99	MTC154834																																																																																															mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154835	JPS083074713		ZrP2-xSx	Zr1P1.25S0.75	Zr	1	P	1.25	S	0.75																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				4.85			4.85																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154836	JPS083074713		ZrP2-xSx	Zr1P1S1	Zr	1	P	1	S	1																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				3.6			3.6																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154837	JPS083074713		HfP2-xSx	Hf1P1.5S0.5	Hf	1	P	1.5	S	0.5																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				4.63			4.63																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154838	JPS083074713		HfP2-xSex	Hf1P1.7S0.3	Hf	1	P	1.7	S	0.3																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				3.71			3.71																																																																																																mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154839	JPS083074713		HfP2-xSex	Hf1P1.5S0.5	Hf	1	P	1.5	S	0.5																		1	2014																										ABC	2	PbFCl	P4/nmm																	K				5.31			5.31	MTC154839																																																																																															mixture - pellet - BN crucible - heat(1300-1400C, 1-2h, P=2 GPa)					New Intermetallic Ternary Phosphide Chalcogenide AP2-xXx (A = Zr, Hf; X = S, Se) Superconductors with PbFCl-Type Crystal Structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Soc.Jpn, 83(2014)074713	Hijiri Kito,Yousuke Yanagi,Shigeyuki Ishida,Kunihiko Oka,Yoshito Gotoh,Hiroshi Fujihisa,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki		
154840	JPS083093702	P induced SC. Pcr = 0.73 GPa. RRR=290 for P=0.73 GPa.. SC properties in DB for P=1.0 GPa(Tcmax). (Tc,Hc2(0), cohere) = (2.1,1.6,164) and (1.88,0.79,197) in(K,T,A) unit for P=1.40 and .88 GPa.	CrAs	As1Cr1	As	1	Cr	1																				3	2014								265																		AB		MnP	Pmma																	K	2.17				0		2.17	MTC154840																			T	WHH		1.37						T/K			0.91		MHC154840																																																														Sn-flux method. (Cr:As:Sn = 1:1:10) - in alumina crucible - sealed in quartz tube - heat to 1050C - hold(2h) - cool to 600C(5 C/h)					Superconductivity of 2.2K under Pressure in Helimagnet CrAs			Department of Physics, Kobe University, Kobe 658-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093702	Hisashi Kotegawa,Shingo Nakahara,Hideki Tou,Hitoshi Sugawara		
154841	JPS083103703	mixed phase: IrSi3 and unknown phase. Lattice term in SP (beta) = 0.101 mJ/mol.K4. (dC/gamma*Tc) = 1.40. e-ph = 0.52	Li2IrSi3	Li2Ir1Si3	Li	2	Ir	1	Si	3																			2014																										AB2C3			P6<3>	194	A	5.01762		7.84022												K	3.7		3.7				3.7										80										T	R(mid)	0.21												MHC154841		A	from Hc2	400										3.26	14							mJ/mol.K2	5.37	SP	486	SP																																				solid stae reaction. mixture(Si+Ir) - mixed with Li - pellet - sealed in Ti tube(arc-welded) - SIN(850C,48h in carbon coeted quartz tube)					Superconductivity at 3.7K in Ternary Silicide Li2IrSi3			Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	J.Phys.Soc.Jpn, 83(2014)103703	Daigorou Hirai,Rui Kawakami,Oxana V. Magdysyuk,Robert E. Dinnebier,Alexander Yaresko,Hidenori Takagi		
154842	NAT4830067	2nd high-TC SC phase appears for high-P region. no-structure change upto 15 GPa. Tc defines as intersection of (dR/dT)max to normal line.	KFe2Se2	K0.8Fe1.7Se2	K	0.8	Fe	1.7	Se	2																		3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		32					32	MTC154842																																																																																															Bridgman method					Re-emerging superconductivity at 48 kelvin in iron chalcogenides			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Nature, 483(2012)67	Liling Sun,Xiao-Jia Chen,Jing Guo,Peiwen Gao,Qing-Zhen Huang,Hangdong Wang,Minghu Fang,Xiaolong Chen,Genfu Chen,Qi Wu,Chao Zhang,Dachun Gu,Xiaoli Dong,LinWang,Ke Yang,Aiguo Li,Xi Dai,Ho-kwang Mao,Zhongxian Zhao		
154843	NAT4830067	2nd high-TC SC phase appears for high-P region. no-structure change upto 15 GPa. Tc defines as intersection of (dR/dT)max to normal line.	KFe2Se2	K0.8Fe1.78Se2	K	0.8	Fe	1.78	Se	2																		3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		32					32	MTC154843																																																																																															Bridgman method					Re-emerging superconductivity at 48 kelvin in iron chalcogenides			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Nature, 483(2012)67	Liling Sun,Xiao-Jia Chen,Jing Guo,Peiwen Gao,Qing-Zhen Huang,Hangdong Wang,Minghu Fang,Xiaolong Chen,Genfu Chen,Qi Wu,Chao Zhang,Dachun Gu,Xiaoli Dong,LinWang,Ke Yang,Aiguo Li,Xi Dai,Ho-kwang Mao,Zhongxian Zhao		
154844	NAT4830067	2nd high-TC SC phase appears for high-P region. no-structure change upto 15 GPa. Tc defines as intersection of (dR/dT)max to normal line.	(Tl,Rb)Fe2Se2	Tl0.6Rb0.4Fe1.67Se2	Tl	0.6	Rb	0.4	Fe	1.67	Se	2																3	2012																										AB2C2		ThCr2Si2																	Fe-122	K		32					32	MTC154844																																																																																															Bridgman method					Re-emerging superconductivity at 48 kelvin in iron chalcogenides			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Nature, 483(2012)67	Liling Sun,Xiao-Jia Chen,Jing Guo,Peiwen Gao,Qing-Zhen Huang,Hangdong Wang,Minghu Fang,Xiaolong Chen,Genfu Chen,Qi Wu,Chao Zhang,Dachun Gu,Xiaoli Dong,LinWang,Ke Yang,Aiguo Li,Xi Dai,Ho-kwang Mao,Zhongxian Zhao		
154845	NATCOM0030943	Fermi liquid. R(T): expornent = 1.92. Tc(P) defined as Tc(on)	La(O,H)FeAs	La1Fe1As1H0.08O0.92	La	1	Fe	1	As	1	H	0.08													O	0.92		1	2012																										ABCD		oxypnictide																	Fe-1111	K			28.7				28.7	MTC154845																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154846	NATCOM0030943	Fermi liquid. R(T): expornent = 2.25. Tc(P) defined as Tc(on)	La(O,H)FeAs	La1Fe1As1H0.21O0.79	La	1	Fe	1	As	1	H	0.21													O	0.79		1	2012																										ABCD		oxypnictide																	Fe-1111	K			17.8				17.8	MTC154846																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154847	NATCOM0030943		La(O,H)FeAs	La1Fe1As1H0.3O0.7	La	1	Fe	1	As	1	H	0.3													O	0.7		1	2012																										ABCD		oxypnictide																	Fe-1111	K			38				38	MTC154847																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154848	NATCOM0030943	R(T): expornent = 0.7. Tc(P) defined as Tc(on)	La(O,H)FeAs	La1Fe1As1H0.46O0.54	La	1	Fe	1	As	1	H	0.46													O	0.54		1	2012																										ABCD		oxypnictide																	Fe-1111	K			36.2				36.2	MTC154848																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154849	NATCOM0030943	R(T): expornent = 1.14. Tc(P) defined as Tc(on)	La(O,H)FeAs	La1Fe1As1H0.24O0.76	La	1	Fe	1	As	1	H	0.24													O	0.76		1	2012																										ABCD		oxypnictide																	Fe-1111	K			30.1				30.1	MTC154849																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154850	NATCOM0030943	R(T): expornent = 1.1.	Gd(O,H)FeAs	Gd1Fe1As1H0.1O0.9	Gd	1	Fe	1	As	1	H	0.1													O	0.9		1	2012																										ABCD		oxypnictide																	Fe-1111	K			55				55	MTC154850																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154851	NATCOM0030943	R(T): expornent = 0.81.	Gd(O,H)FeAs	Gd1Fe1As1H0.3O0.7	Gd	1	Fe	1	As	1	H	0.3													O	0.7		1	2012																										ABCD		oxypnictide																	Fe-1111	K			45.9				45.9																																																																																																					Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154852	NATCOM0030943	R(T): expornent = 0.93.	Sm(O,H)FeAs	Sm1Fe1As1H0.066O0.934	Sm	1	Fe	1	As	1	H	0.066													O	0.934		1	2012																										ABCD		oxypnictide																	Fe-1111	K			43.3				43.3																																																																																																					Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154853	NATCOM0030943		Sm(O,H)FeAs	Sm1Fe1As1H0.25O0.75	Sm	1	Fe	1	As	1	H	0.25													O	0.75		1	2012																										ABCD		oxypnictide																	Fe-1111	K			54.7				54.7	MTC154853																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154854	NATCOM0030943		Sm(O,H)FeAs	Sm1Fe1As1H0.4O0.6	Sm	1	Fe	1	As	1	H	0.4													O	0.6		1	2012																										ABCD		oxypnictide																	Fe-1111	K			46.4				46.4																																																																																																					Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154855	NATCOM0030943		Ce(O,H)FeAs	Ce1Fe1As1H0.065O0.935	Ce	1	Fe	1	As	1	H	0.065													O	0.935		1	2012																										ABCD		oxypnictide																	Fe-1111	K			41.1				41.1																																																																																																					Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154856	NATCOM0030943	R(T): expornent = 1.46.	Ce(O,H)FeAs	Ce1Fe1As1H0.22O0.78	Ce	1	Fe	1	As	1	H	0.22													O	0.78		1	2012																										ABCD		oxypnictide																	Fe-1111	K			48				48	MTC154856																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154857	NATCOM0030943	R(T): expornent = 0.53.	Ce(O,H)FeAs	Ce1Fe1As1H0.4O0.6	Ce	1	Fe	1	As	1	H	0.4													O	0.6		1	2012																										ABCD		oxypnictide																	Fe-1111	K			43.1				43.1																																																																																																					Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
154858	NJP012123003	R<ab> measured. Energy gap measured by time-resolved optical reflection.	Ba(Fe,Ni)2As2	Ba1Fe1.9Ni0.1As2	Ba	1	Fe	1.9	Ni	0.1	As	2																3	2010																										AB2C2		ThCr2Si2																	Fe-122	K		20				0.7	20																																																6.6	15																																															self flux method					Distinct quasiparticle relaxation dynamics in an electron-doped superconductor, BaFe1.9Ni0.1As2			Department of Physics and Astronomy, Hunter College, the City University of New York, 695 Park Avenue, New York, NY 10065, USA	New J.Phys., 12(2010)123003	Y Gong,W Lai,T Nosach,L J Li,G H Cao,Z A Xu,Y H Ren		
154859	PHC5020010	impurity phase : Fe3O4(NiAs type phase)	Fe(Te,Se)	Fe1.02Te0.5Se0.5	Fe	1.02	Te	0.5	Se	0.5																			2014																										AB		PbO			A	3.7879		5.9833											Fe-11	K	12.2	13.6	15				13.6																																																																							mOhm.cm				1							1.1												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154860	PHC5020010	impurity phase : Fe3O4(NiAs type phase)	Fe(Te,Se,S)	Fe1.02Te0.5Se0.4S0.1	Fe	1.02	Te	0.5	Se	0.4	S	0.1																	2014																										AB		PbO			A	3.7915		6.0265											Fe-11	K	11.8	13	14.3				13																																																																							mOhm.cm				1.38							1.16												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154861	PHC5020010	impurity phase : Fe3O4(NiAs type phase)	Fe(Te,Se,S)	Fe1.02Te0.5Se0.3S0.2	Fe	1.02	Te	0.5	Se	0.3	S	0.2																	2014																										AB		PbO			A	3.796		6.0643											Fe-11	K	10.41	11.64	12.9				11.64	MTC154862																																																																						mOhm.cm				2.14							1.54												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154862	PHC5020010	impurity phase : Fe3O4(NiAs type phase)	Fe(Te,Se,S)	Fe1.02Te0.5Se0.2S0.3	Fe	1.02	Te	0.5	Se	0.2	S	0.3																	2014																										AB		PbO			A	3.7968		6.11											Fe-11	K	8.79	10.16	11.5				10.16	MTC154862																																																																						mOhm.cm				4.18							2.38												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154863	PHC5020010	impurity phase : Fe3O4(NiAs type phase)	Fe(Te,Se,S)	Fe1.02Te0.5Se0.1S0.4	Fe	1.02	Te	0.5	Se	0.1	S	0.4																	2014																										AB		PbO			A	3.8008		6.1702											Fe-11	K	7.31	8.45	10.02				8.45																																																																							mOhm.cm				6.94							4.48												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154864	PHC5020010	not SC. impurity phase : Fe3O4(NiAs type phase)	Fe(Te,S)	Fe1.02Te0.5S0.5	Fe	1.02	Te	0.5	S	0.5																			2014																										AB		PbO			A	3.8013		6.2295											Fe-11	K					2																																																																									mOhm.cm				18.3							10.1												Fe(3N8),Te(4N),Se(4N),S(4N)		solid state reaction. mixture - sealed in quartz tube - heat(700C,24h) - reground - ANN(500C,10h) - ANN(700C,38h) - ANN(700C,120h)					Properties of FeSe-type superconductors with ternary mixture of chalcogens			Institute of Natural Sciences, Ural Federal University, 620083 Ekaterinburg, Russia	Physca C, 502(2014)10	A.S. Abouhaswa,A.I. Merentsov,N.V. Selezneva,N.V. Baranov		
154865	PHC5040001	Impurity phase: SrSnO3. SC volume increases by high P ANN process.	EuSr2(Ta,Sn)Cu2O8-z	Eu1Sr2Ta0.8Sn0.2O8-z	Eu	1	Sr	2	Ta	0.8	Sn	0.2													O	8-z			2014																												M1212			A	3.872		11.674											Ta-1212	K	13		40	40			40																																																																																																mixture - SIN(1000C,12h,in air) - reground - pellet - SIN(1030C,24h in air) - cool to RT - ANN(200-400C,40h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154866	PHC5040001		SmSr2(Ta,Sn)Cu2O8-z	Sm1Sr2Ta0.8Sn0.2O8-z	Sm	1	Sr	2	Ta	0.8	Sn	0.2													O	8-z			2014																												M1212																	Ta-1212	K				30			30																																																																																																mixture - SIN(1000C,12h,in air) - reground - pellet - SIN(1030C,24h in air) - cool to RT - ANN(200-400C,40h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154867	PHC5040001	not SC	NdSr2(Ta,Sn)Cu2O8-z	Nd1Sr2Ta0.8Sn0.2O8-z	Nd	1	Sr	2	Ta	0.8	Sn	0.2													O	8-z			2014																												M1212																	Ta-1212	K					2																																																																																																		mixture - SIN(1000C,12h,in air) - reground - pellet - SIN(1030C,24h in air) - cool to RT - ANN(200-400C,40h, in flowing O2)					Synthesis of a new superconductor EuSr2Cu2(Ta,Sn)O8-z			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)1	Shinnosuke Sato,Keon Kim,Masatsune Kato,Takashi Noji,Yoji Koike		
154868	PHC4690370	(dHc2/dT) depends on Tc-criterion. Energy gap by PCAR. two gaps: d1 = 6.45 me,V(2d1/kTc) = 2.8-3.1, d2=16.6 meV, (2d2/kTc) = 6.8-8.5. Anisotropy(Hc2) = 7-7.5	Sm(O,F)FeAs	Sm1Fe1As1F0.25O0.7	Sm	1	Fe	1	As	1	F	0.25													O	0.7		3	2009																										ABCD	2	oxypnictide	P4/nmm																Fe-1111	K		49.6					49.6																				T	R(0.5Rn)								T/K	R(0.5Rn)		8	3.3	MHC154868												meV	16.6	6.8	1																																															cubic anvil high pressure method					Single crystals of LnFeAsO1-xFx (Ln = La, Pr, Nd, Sm, Gd) and Ba1-xRbxFe2As2: Growth, structure and superconducting properties			Laboratory for Solid State Physics, ETH Zurich, 8093 Zurich, Switzerland	Physca C, 469(2009)370	J. Karpinski,N.D. Zhigadlo,S. Katrych,Z. Bukowski,P. Moll,S. Weyeneth,H. Keller,R. Puzniak,M. Tortello,D. Daghero,R. Gonnelli,I. Maggio-Aprile,Y. Fasano,F. Fischer,K. Rogacki,B. Batlogg		
154869	PHC4690370	Anisotropy(Hc2) = 2.5-3.2 near Tc.	(Ba,Rb)Fe2As2	Ba0.9Rb0.1Fe2As2	Ba	0.9	Rb	0.1	Fe	2	As	2																3	2009																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.925		13.2096											Fe-122	K		23.3					23.3																				T	R(0.5Rn)								T/K	R(0.5Rn)		7.1	4.2	MHC154869																																																														Sn-flux method. Fe:Sn=1:24. mixture - alumina crucible in sealed quartz tube - heat(850C,3h) - cool to 500C over 50h.					Single crystals of LnFeAsO1-xFx (Ln = La, Pr, Nd, Sm, Gd) and Ba1-xRbxFe2As2: Growth, structure and superconducting properties			Laboratory for Solid State Physics, ETH Zurich, 8093 Zurich, Switzerland	Physca C, 469(2009)370	J. Karpinski,N.D. Zhigadlo,S. Katrych,Z. Bukowski,P. Moll,S. Weyeneth,H. Keller,R. Puzniak,M. Tortello,D. Daghero,R. Gonnelli,I. Maggio-Aprile,Y. Fasano,F. Fischer,K. Rogacki,B. Batlogg		
154870	PHC5040016	Energy gap measured by SP using two band model. Large & Small gaps are (d1,d2) = (4.09, 2.60) meV for H = 0 T.	Fe(Se,Te)	Fe1Se0.4Te0.6	Fe	1	Se	0.4	Te	0.6																			2014																										AB		Fe-11																	Fe-11	K		14.2					14.2																																														meV	4.09		14																																															Bridgman method. as-grown sample - ANN(400C,200h, in vac)					Specific heat in magnetic fields and superconducting gap structure in FeSe1-xTex (0.6 =< x =<1)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	Physca C, 504(2014)16	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
154871	PHC5040019	impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K. Carrier conc. = 7.8 E+22 /cm3 at 60 K.	Sm(O,F)FeAs	Sm1Fe1As1F0.12O0.88	Sm	1	Fe	1	As	1	F	0.12													O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9301		8.4781											ZrCuSiAs type. Fe-1111	K	48.4		50.3				49.35																				T	R(0.9Rn), WHH	292							T/K	R(0.9Rn)	8.4			MHC154871		A	from Hc2	10.6																												uV/K	-34			MTP154871	mOhm.cm				3.25										m3/C	-0.00000000252					MRH154871			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154872	PHC5040019	impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K. Carrier conc. = 5.8 E+22 /cm3 at 60 K.	Sm(O,F)Fe(As,P)	Sm1Fe1As0.95P0.05F0.12O0.88	Sm	1	Fe	1	As	0.95	P	0.05	F	0.12											O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9306		8.4747											ZrCuSiAs type. Fe-1111	K	44.4		49.2				46.8	MTC154872																			T	R(0.9Rn), WHH	194							T/K	R(0.9Rn)	6			MHC154872																																uV/K	-28.6			MTP154872	mOhm.cm				2.32										m3/C	-0.00000000355					MRH154872			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154873	PHC5040019	impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K. Carrier conc. = 4.8 E+22 /cm3 at 60 K.	Sm(O,F)Fe(As,P)	Sm1Fe1As0.9P0.1F0.12O0.88	Sm	1	Fe	1	As	0.9	P	0.1	F	0.12											O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9307		8.4714											ZrCuSiAs type. Fe-1111	K	33.5		39.2				36.35																				T	R(0.9Rn), WHH	116							T/K	R(0.9Rn)	4.5			MHC154873																																uV/K	-26.5			MTP154873	mOhm.cm				6.7										m3/C	-0.00000000366					MRH154873			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154874	PHC5040019	impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K.	Sm(O,F)Fe(As,P)	Sm1Fe1As0.85P0.15F0.12O0.88	Sm	1	Fe	1	As	0.85	P	0.15	F	0.12											O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9311		8.4664											ZrCuSiAs type. Fe-1111	K	14.9		20.7				17.8																				T	R(0.9Rn), WHH	36							T/K	R(0.9Rn)	2.7			MHC154874																																uV/K	-24.1			MTP154874	mOhm.cm				9.9																			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154875	PHC5040019	impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K. Carrier conc. = 7.8 E+22 /cm3 at 60 K.	Sm(O,F)Fe(As,P)	Sm1Fe1As0.8P0.2F0.12O0.88	Sm	1	Fe	1	As	0.8	P	0.2	F	0.12											O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9316		8.4604											ZrCuSiAs type. Fe-1111	K	13.1		18.1				15.6																				T	R(0.9Rn), WHH	31							T/K	R(0.9Rn)	2.6			MHC154875																																					mOhm.cm				10.5																			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154876	PHC5040019	not SC. impurity phases(SmAs,SmOF,Fe2P) are observed by XRD. [RES77] shows RES at 60 K. Carrier conc. = 7.8 E+22 /cm3 at 60 K.	Sm(O,F)Fe(As,P)	Sm1Fe1As0.75P0.25F0.12O0.88	Sm	1	Fe	1	As	0.75	P	0.25	F	0.12											O	0.88		1	2014																										ABCD		oxypnictide	P4/nmm																ZrCuSiAs type. Fe-1111	K					2																																																																									mOhm.cm				11.6																			SmAs,Fe2O3,FeF2,Fe,FeP		solid state reaction. mixture - pellet - wrapped in Ta foil - SIN(900C,45h, in evacuated quartz tube)					Effects of phosphorous doping on the superconducting properties of SmFeAs(O,F)			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Physca C, 504(2014)19	Shiv Jee Singh,Jun-ichi Shimoyama,Akiyasu Yamamoto,Hiraku Ogino,Kohji Kishio		
154877	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.6Nd0.4F0.5Bi1S2O0.5	Ce	0.6	Nd	0.4	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		3					3	MTC154877																																																																																													Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154878	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.5Nd0.5F0.5Bi1S2O0.5	Ce	0.5	Nd	0.5	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		3.46					3.46	MTC154877																																																																																													Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154879	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.4Nd0.6F0.5Bi1S2O0.5	Ce	0.4	Nd	0.6	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		3.94					3.94																																																																																														Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154880	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.3Nd0.7F0.5Bi1S2O0.5	Ce	0.3	Nd	0.7	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		4.07					4.07																																																																																														Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154881	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.2Nd0.8F0.5Bi1S2O0.5	Ce	0.2	Nd	0.8	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		4.42					4.42																																																																																														Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154882	PHC5040033		(Ce,Nd)(O,F)BiS2	Ce0.1Nd0.9F0.5Bi1S2O0.5	Ce	0.1	Nd	0.9	F	0.5	Bi	1	S	2											O	0.5		1	2014																													P4/nmm																BiS2 layer	K		4.68					4.68																																																																																														Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154883	PHC5040033		Nd(O,F)BiS2	Nd1F0.5Bi1S2O0.5	Nd	1	F	0.5	Bi	1	S	2													O	0.5		1	2014																													P4/nmm																BiS2 layer	K		4.79					4.79																																																																																														Bi,Ce2S3,Nd2S3,BiF3,Bi2O3,Bi2S3		mixture - pellet - sealed in quartz tube - heat(700C,10h) - reground - heat(700C,10h)					Chemical pressure effect on Tc in BiS2-based Ce1-xNdxO0.5F0.5BiS2			Tokyo Metropolitan University, 1-1 Minami-Osawa, Hachioji, Tokyo 192-0397, Japan	Physca C, 504(2014)33	Joe Kajitani,Atsushi Omachi,Takafumi Hiroi,Osuke Miura,Yoshikazu Mizuguchi		
154884	PHC5040036	DOS estimated to be 5.7 states/eV/f.u.	BaTi2Sb2O	Ba1Ti2Sb2O1	Ba	1	Ti	2	Sb	2															O	1		1	2014																										ABC2D2																				K		1.2					1.2																				T	R(0.5Rn), Linear approx.	1.32												MHC154884		A	from Hc2	158																																																								BaO(4N),Ti(3N),Sb(3N)		mixture - pellet - wrapped with Ta foil - sealed in quartz tube - heat(1000C,50h) - cool to RT(25C/h)					Superconducting properties of BaTi2Pn2O (Pn = Sb, Bi)			Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Physca C, 504(2014)36	Takeshi Yajima,Kousuke Nakano,Yasumasa Nozaki,Hiroshi Kageyama		
154885	PHC5040036	impurity phases: Bi, BaO.  GL(kappa) = 20.8. DOS estimated to be 4.79 states/eV/f.u.	BaTi2Bi2O	Ba1Ti2Bi2O1	Ba	1	Ti	2	Bi	2															O	1		1	2014																										ABC2D2																				K		4.6					4.6											Oe	M-H curve	60							T	R(0.5Rn), Linear approx.	1.7												MHC154885		A	from Hc2	139			A	from Hc1, GL theory	2900																																																			BaO(4N),Ti(3N),Bi(3N)		mixture - pellet - wrapped with Ta foil - sealed in quartz tube - heat(850C,50h) - cool to RT(25C/h)					Superconducting properties of BaTi2Pn2O (Pn = Sb, Bi)			Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Physca C, 504(2014)36	Takeshi Yajima,Kousuke Nakano,Yasumasa Nozaki,Hiroshi Kageyama		
154886	PHC5060040	K0.63Fe1.37Mn0.028Se2 by EDX. Three step SC transitions. Tc=31.9, 36.8, 42.5 K. DB shows for 2nd transition. Tc defined as R=0.5Rn.	K0.8(Fe,Mn)2Se2	K0.8Fe1.97Mn0.03Se2	K	0.8	Fe	1.97	Mn	0.03	Se	2																3	2014																										AB2C2		ThCr2Si2																		K	32.1	37.4	39.6	36.8			37.4																				T	RES, WHH		137.4	51.8					T/K	RES		5.3	2	MHC154886		A	from Hc2	25.2	9.5																																																									melting process					Anisotropic characteristics and critical behaviors in Mn doped K0.8Fe2Se2 single crystal			Department of Physics, Shanghai University, 200444 Shanghai, China	Physca C, 506(2014)40	M.T. Li,L. Chen,Z.J. Feng,D.M. Deng,B.J. Kang,S.X. Cao,C.T. Lin,J.C. Zhang		
154887	PHC5060040	K0.38Fe1.68Mn0.023Se2 by EDX. Three step SC transitions. Tc=31.9, 36.8, 42.5 K. DB shows for 3rd transition. Tc defined as R=0.9Rn.	K0.8(Fe,Mn)2Se2	K0.8Fe1.97Mn0.03Se2	K	0.8	Fe	1.97	Mn	0.03	Se	2																3	2014																										AB2C2		ThCr2Si2																		K		42.2	46.1	42.5			42.2																				T	RES, WHH		178.4	52.6					T/K	RES		6.1	1.8	MHC154887		A	from Hc2	25	7.4																																																									melting process					Anisotropic characteristics and critical behaviors in Mn doped K0.8Fe2Se2 single crystal			Department of Physics, Shanghai University, 200444 Shanghai, China	Physca C, 506(2014)40	M.T. Li,L. Chen,Z.J. Feng,D.M. Deng,B.J. Kang,S.X. Cao,C.T. Lin,J.C. Zhang		
154888	PHC5060094	Al-content = 2.89 by EDS.	Ba8(Si,Al)46	Ba8Si44Al2	Ba	8	Si	44	Al	2																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.40759														K				5.85			5.85																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154889	PHC5060094	Al-content = 3.79 by EDS.	Ba8(Si,Al)46	Ba8Si43Al3	Ba	8	Si	43	Al	3																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.41768														K				5.75			5.75																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154890	PHC5060094	Al-content = 5.39 by EDS.	Ba8(Si,Al)46	Ba8Si41Al5	Ba	8	Si	41	Al	5																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.44446														K				6			6																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154891	PHC5060094	Al-content = 6.51 by EDS.	Ba8(Si,Al)46	Ba8Si40Al6	Ba	8	Si	40	Al	6																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.45573														K				5.6			5.6																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154892	PHC5060094	Al-content = 7.24 by EDS.	Ba8(Si,Al)46	Ba8Si39Al7	Ba	8	Si	39	Al	7																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.47502														K				4			4																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154893	PHC5060094	Al-content = 8.06 by EDS.	Ba8(Si,Al)46	Ba8Si38Al8	Ba	8	Si	38	Al	8																			2014																										A8B46		clathrate	Pm3[-]n	223	A	10.49473														K				3			3																																																																																														Ba(4N),Si(5N),Al(5N)		arc-melting with extra Ba (5%)					The effect of Al-substitution on superconducting type-I clathrate Ba8Si46			Department of Physics, School of Mathematics and Physics, University of Science and Technology Beijing, Beijing 100083, China	Physca C, 506(2014)94	Lihua Liu,Shanli Bi,Ning Chen,Feng Li,Yang Liu,Guohui Cao,Yang Li		
154894	PHC5070085	O-content by mass change during ANN. Mossbauer effect measured.	FeSr2YCu2O6+z	Fe1Sr2Y1Cu2O7.51	Fe	1	Sr	2	Y	1	Cu	2													O	6+z	7.51		2014	cm3/g	0.0000024			myu-B/Y	3.6	-56																				2	M1212																	Fe-1212	K	42		65			23	53.5																																																																																														R2O3,SrCO3,CuO,Fe2O3		mixture - CAL(850C,24h, in air) - ground - pellet - SIN(950C,24h, in air) - ANN(790C,24h, in flowing N2) - ANN(270C,24h, in flowing O2) - ANN(270C,24h, in O2)					Fe ion distribution and superconductivity of FeSr2RECu2O6ty (RE = Eu, Er, Gd, Nd and Y)			Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686, Japan	Physca C, 507(2014)85	Yoshiaki Hata,Kazuhiro Yamaugchi,Kazuki Kinoshita,Eiji Kita,Takashi Mochiku,Hiroshi Yasuoka		
154895	PHC5070085	R not zero down to 4.2 K. O-content by mass change during ANN. Mossbauer effect measured.	FeSr2EuCu2O6+z	Fe1Sr2Eu1Cu2O7.51	Fe	1	Sr	2	Eu	1	Cu	2													O	6+z	7.51		2014	cm3/g	0.0000368			myu-B/Eu	2.87	-330																				2	M1212																	Fe-1212	K			22				22																																																																																														R2O3,SrCO3,CuO,Fe2O3		mixture - CAL(850C,24h, in air) - ground - pellet - SIN(950C,24h, in air) - ANN(790C,24h, in flowing N2) - ANN(270C,24h, in flowing O2) - ANN(270C,24h, in O2)					Fe ion distribution and superconductivity of FeSr2RECu2O6ty (RE = Eu, Er, Gd, Nd and Y)			Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686, Japan	Physca C, 507(2014)85	Yoshiaki Hata,Kazuhiro Yamaugchi,Kazuki Kinoshita,Eiji Kita,Takashi Mochiku,Hiroshi Yasuoka		
154896	PHC5070085	O-content by mass change during ANN. Mossbauer effect measured.	FeSr2GdCu2O6+z	Fe1Sr2Gd1Cu2O7.58	Fe	1	Sr	2	Gd	1	Cu	2													O	6+z	7.58		2014	cm3/g	0.00000191			myu-B/Gd	7.77	1																				2	M1212																	Fe-1212	K	26		47			21	36.5																																																																																														R2O3,SrCO3,CuO,Fe2O3		mixture - CAL(850C,24h, in air) - ground - pellet - SIN(950C,24h, in air) - ANN(790C,24h, in flowing N2) - ANN(270C,24h, in flowing O2) - ANN(270C,24h, in O2)					Fe ion distribution and superconductivity of FeSr2RECu2O6ty (RE = Eu, Er, Gd, Nd and Y)			Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686, Japan	Physca C, 507(2014)85	Yoshiaki Hata,Kazuhiro Yamaugchi,Kazuki Kinoshita,Eiji Kita,Takashi Mochiku,Hiroshi Yasuoka		
154897	PHC5070085	not SC. O-content by mass change during ANN. Mossbauer effect measured.	FeSr2NdCu2O6+z	Fe1Sr2Nd1Cu2O7.54	Fe	1	Sr	2	Nd	1	Cu	2													O	6+z	7.54		2014	cm3/g	0.000000471			myu-B/Nd	4.4	-11.7																				2	M1212																	Fe-1212	K							4.2																																																																																														R2O3,SrCO3,CuO,Fe2O3		mixture - CAL(850C,24h, in air) - ground - pellet - SIN(950C,24h, in air) - ANN(790C,24h, in flowing N2) - ANN(270C,24h, in flowing O2) - ANN(270C,24h, in O2)					Fe ion distribution and superconductivity of FeSr2RECu2O6ty (RE = Eu, Er, Gd, Nd and Y)			Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686, Japan	Physca C, 507(2014)85	Yoshiaki Hata,Kazuhiro Yamaugchi,Kazuki Kinoshita,Eiji Kita,Takashi Mochiku,Hiroshi Yasuoka		
154898	PHC5070085	O-content by mass change during ANN. Mossbauer effect measured.	FeSr2ErCu2O6+z	Fe1Sr2Er1Cu2O7.5	Fe	1	Sr	2	Er	1	Cu	2													O	6+z	7.5		2014	cm3/g	0.00000314			myu-B/Er	9.5	-10.2																				2	M1212																	Fe-1212	K	42		62			20	52																																																																																														R2O3,SrCO3,CuO,Fe2O3		mixture - CAL(850C,24h, in air) - ground - pellet - SIN(950C,24h, in air) - ANN(790C,24h, in flowing N2) - ANN(270C,24h, in flowing O2) - ANN(270C,24h, in O2)					Fe ion distribution and superconductivity of FeSr2RECu2O6ty (RE = Eu, Er, Gd, Nd and Y)			Department of Applied Physics, National Defense Academy, 1-10-20 Hashirimizu, Yokosuka 239-8686, Japan	Physca C, 507(2014)85	Yoshiaki Hata,Kazuhiro Yamaugchi,Kazuki Kinoshita,Eiji Kita,Takashi Mochiku,Hiroshi Yasuoka		
154899	PHC5070055	M(H//ab)  shows 3 step transition at 4K (H=0.78, 1.0, 1.25 T). For T < 2 K, (dHc2/dT) = 0.031 T/K, then Hc2//ab = 0.13 T by WHH.	DyNi2B2C	Dy1Ni2B2C1	Dy	1	Ni	2	B	2	C	1																3	2014								10.3																		ABC2D2		LuNi2B2C																		K	6.2		6.4			0.2	6.3																				T	RES,WHH		0.55						T/K	RES, (2<T<4)		0.108																																							uOhm.cm	113												113												flux method using Ni2B solvent.					Transport properties along c-axis of DyNi2B2C			Department of Physics, Sookmyung Women's University, Seoul 140-742, Republic of Korea	Physca C, 507(2014)55	W.C. Lee		
154900	PHSS0431845	Hc2 defined as R=0.5Rn. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.776Pb0.194In0.03Te1	Sn	0.776	Pb	0.194	In	0.03	Te	1																	2001																										AB																				K		2.25					2.25																				T	RES(R=0.5Rn), GL		1.5						T/K	RES(R=0.5Rn)																																									mOhm.cm	1.79																				n/cm3	239000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154901	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 3.23E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.768Pb0.192In0.04Te1	Sn	0.768	Pb	0.192	In	0.04	Te	1																	2001																										AB																				K		2.57					2.57																				T	RES(R=0.5Rn), GL		2.13						T/K	RES(R=0.5Rn)	1.2																																								mOhm.cm	2.07																				n/cm3	269000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154902	PHSS0431845	Hc2 defined as R=0.5Rn. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.576Pb0.384In0.04Te1	Sn	0.576	Pb	0.384	In	0.04	Te	1																	2001																										AB																				K		0.4					0.4																				T	RES(R=0.5Rn), GL		0.249																																																mOhm.cm	5.12																				n/cm3	171000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154903	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 4.71E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.9025Pb0.0475In0.05Te1	Sn	0.9025	Pb	0.0475	In	0.05	Te	1																	2001																										AB																				K		1.79					1.79																				T	RES(R=0.5Rn), GL		0.676																																																mOhm.cm	0.683																				n/cm3	603000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154904	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 4.89E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.8549Pb0.0951In0.05Te1	Sn	0.8549	Pb	0.0951	In	0.05	Te	1																	2001																										AB																				K		2.06					2.06																				T	RES(R=0.5Rn), GL		0.863						T/K	RES(R=0.5Rn)	0.61																																								mOhm.cm	0.734																				n/cm3	551000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154905	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 5.22E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.8075Pb0.1425In0.05Te1	Sn	0.8075	Pb	0.1425	In	0.05	Te	1																	2001																										AB																				K		2.81					2.81																				T	RES(R=0.5Rn), GL		2.04						T/K	RES(R=0.5Rn)	1.1																																								mOhm.cm	1.18																				n/cm3	561000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154906	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 4.70E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.7598Pb0.1902In0.05Te1	Sn	0.7598	Pb	0.1902	In	0.05	Te	1																	2001																										AB																				K		2.77					2.77																				T	RES(R=0.5Rn), GL		1.71						T/K	RES(R=0.5Rn)	0.9																																								mOhm.cm	1.09																				n/cm3	4760000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154907	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 3.93E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.7127Pb0.2373In0.05Te1	Sn	0.7127	Pb	0.2373	In	0.05	Te	1																	2001																										AB																				K		2.62					2.62	MTC154907																			T	RES(R=0.5Rn), GL		2.57						T/K	RES(R=0.5Rn)	1.42																																								mOhm.cm	2.07																				n/cm3	433000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154908	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 2.69E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.6646Pb0.2854In0.05Te1	Sn	0.6646	Pb	0.2854	In	0.05	Te	1																	2001																										AB																				K		2.28					2.28																				T	RES(R=0.5Rn), GL		2.15						T/K	RES(R=0.5Rn)	1.35																																								mOhm.cm	2.84																				n/cm3	403000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154909	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 0.985E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.6175Pb0.3325In0.05Te1	Sn	0.6175	Pb	0.3325	In	0.05	Te	1																	2001																										AB																				K		1.6					1.6																				T	RES(R=0.5Rn), GL		0.935						T/K	RES(R=0.5Rn)	0.84																																								mOhm.cm	4.77																				n/cm3	362000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154910	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 0.546E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.57Pb0.38In0.05Te1	Sn	0.57	Pb	0.38	In	0.05	Te	1																	2001																										AB																				K		0.703					0.703																				T	RES(R=0.5Rn), GL		0.486						T/K	RES(R=0.5Rn)	1.01																																								mOhm.cm	10.2																				n/cm3	287000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154911	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 3.31E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.92In0.08Te1	Sn	0.92	In	0.08	Te	1																			2001																										AB																				K		1.35					1.35																				T	RES(R=0.5Rn), GL		0.371						T/K	RES(R=0.5Rn)	0.413																																								mOhm.cm	0.67																				n/cm3	1350000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154912	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 8.23E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.736Pb0.184In0.08Te1	Sn	0.736	Pb	0.184	In	0.08	Te	1																	2001																										AB																				K		2.82					2.82																				T	RES(R=0.5Rn), GL		2.47						T/K	RES(R=0.5Rn)	1.28																																								mOhm.cm	0.835																				n/cm3	1240000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154913	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 1.47E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.552Pb0.368In0.08Te1	Sn	0.552	Pb	0.368	In	0.08	Te	1																	2001																										AB																				K		2.16					2.16																				T	RES(R=0.5Rn), GL		2.26						T/K	RES(R=0.5Rn)	1.5																																								mOhm.cm	5.4																				n/cm3	916000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154914	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 6.95E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.8798Pb0.0002In0.12Te1	Sn	0.8798	Pb	0.0002	In	0.12	Te	1																	2001																										AB																				K		1.76					1.76																				T	RES(R=0.5Rn), GL		0.578						T/K	RES(R=0.5Rn)	0.493																																								mOhm.cm	0.362																				n/cm3	2440000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154915	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 9.12E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.704Pb0.176In0.12Te1	Sn	0.704	Pb	0.176	In	0.12	Te	1																	2001																										AB																				K		2.98					2.98																				T	RES(R=0.5Rn), GL		1.92																																																mOhm.cm	0.541																				n/cm3	2240000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154916	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 9.13E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.5277Pb0.3523In0.12Te1	Sn	0.5277	Pb	0.3523	In	0.12	Te	1																	2001																										AB																				K		3.58					3.58																				T	RES(R=0.5Rn), GL		5.22						T/K	RES(R=0.5Rn)	2.11																																								mOhm.cm	1.18																				n/cm3	4180000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154917	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 8.26E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.84In0.16Te1	Sn	0.84	In	0.16	Te	1																			2001																										AB																				K		2.13					2.13																				T	RES(R=0.5Rn), GL		0.764						T/K	RES(R=0.5Rn)	0.524																																																													n/cm3	5480000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154918	PHSS0431845	Hc2 defined as R=0.5Rn.  Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.6723Pb0.1677In0.16Te1	Sn	0.6723	Pb	0.1677	In	0.16	Te	1																	2001																										AB																				K		3.11					3.11																													T/K	RES(R=0.5Rn)	0.8																																																													n/cm3	4960000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154919	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 1.1E+22 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.5883Pb0.2517In0.16Te1	Sn	0.5883	Pb	0.2517	In	0.16	Te	1																	2001																										AB																				K		3.88					3.88																				T	RES(R=0.5Rn), GL		2.75						T/K	RES(R=0.5Rn)	1.03																																								mOhm.cm	0.525																				n/cm3	5260000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154920	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 1.05E+22 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.504Pb0.336In0.16Te1	Sn	0.504	Pb	0.336	In	0.16	Te	1																	2001																										AB																				K		4.01					4.01																				T	RES(R=0.5Rn), GL		4.43						T/K	RES(R=0.5Rn)	1.6																																								mOhm.cm	0.818																				n/cm3	5140000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154921	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 6.45E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.4197Pb0.4203In0.16Te1	Sn	0.4197	Pb	0.4203	In	0.16	Te	1																	2001																										AB																				K		4.18					4.18	MTC154921																			T	RES(R=0.5Rn), GL		4.05						T/K	RES(R=0.5Rn)	1.41																																								mOhm.cm	1.18																				n/cm3	5130000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154922	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 0.43E+20 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.3361Pb0.5039In0.16Te1	Sn	0.3361	Pb	0.5039	In	0.16	Te	1																	2001																										AB																				K		2.49					2.49																				T	RES(R=0.5Rn), GL		2.67						T/K	RES(R=0.5Rn)	1.54																																								mOhm.cm	194																				n/cm3	5960000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154923	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 9.71E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.6001Pb0.1999In0.2Te1	Sn	0.6001	Pb	0.1999	In	0.2	Te	1																	2001																										AB																				K		3.59					3.59																				T	RES(R=0.5Rn), GL		2.09						T/K	RES(R=0.5Rn)	0.848																																																													n/cm3	7520000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154924	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 7.97E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.56Pb0.24In0.2Te1	Sn	0.56	Pb	0.24	In	0.2	Te	1																	2001																										AB																				K		3.87					3.87																				T	RES(R=0.5Rn), GL		2.64						T/K	RES(R=0.5Rn)	0.96																																								mOhm.cm	0.71																				n/cm3	6240000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154925	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 1.42E+22 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.4797Pb0.3203In0.2Te1	Sn	0.4797	Pb	0.3203	In	0.2	Te	1																	2001																										AB																				K		4.16					4.16																				T	RES(R=0.5Rn), GL		3.95						T/K	RES(R=0.5Rn)	1.37																																								mOhm.cm	0.493																				n/cm3	5950000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154926	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 8.74E+21 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.3997Pb0.4003In0.2Te1	Sn	0.3997	Pb	0.4003	In	0.2	Te	1																	2001																										AB																				K		4.23					4.23	MTC154926																			T	RES(R=0.5Rn), GL		5.31						T/K	RES(R=0.5Rn)	1.81																																								mOhm.cm	1.12																				n/cm3	6090000000000000000000			ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154927	PHSS0431845	Hc2 defined as R=0.5Rn. DOS = 1.54E+20 /eV.cm3, calculated from [RESN] and [dHc2/dT].. Carrier from Hall coeffic.	(Sn,Pb)1-xInxTe	Sn0.32Pb0.48In0.2Te1	Sn	0.32	Pb	0.48	In	0.2	Te	1																	2001																										AB																				K		3.35					3.35																				T	RES(R=0.5Rn), GL		1.29						T/K	RES(R=0.5Rn)	0.539																																								mOhm.cm	18.2																								ceramic technology. Samples quenched to RT. Crashed to grain size of nearly 0.1 mm. Hot-pressed(2000 kg/cm2) - ANN(600C,200h)					Superconductivity of (Sn1-zPbz)1-xInxTe Alloys			Ioffe Physicotechnical Institute, Russian Academy of Sciences, ul. Politekhnicheskaya 26, St. Petersburg, 194021 Russia	Phys.Solid State, 43(2001)1845	R. V. Parfen'ev,D. V. Shamshur,S. A. Nemov		
154928	PLA2500439	a few % impurity phase. Energy gap from <139>La-NQR.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	1998																										ABC2	3	CeNiC2			A	3.96	4.565	6.207												K		3					3																																																3.34	6																																													La(3N),Ni(3N),C(5N)		arc-melting					Microscopic measurements in <139>La-NQR of the ternary carbide superconductor LaNiC2			Department of Material Science. Faculty of Science, Hirneji Institute of Technogy, Ako-gun, Hyogo 678.1297, Japan	Phys.Lett. A, 250(1998)439	Y. Iwamoto,Y. Iwasaki,K. Ueda,T. Kohara		
154929	PRB081144414	R(T) shows SC transition at 3.7 K, maybe filamentary Sn impurity incorporated during growth. Two successive magnetic transition , Tn = 17K and 16K in SP.	EuPtSi3	Eu1Pt1Si3	Eu	1	Pt	1	Si	3																		3	2010								17																		ABC3			I4mm		A	4.266		9.8768												K		3.7					3.7																																																																																																High-T solution growth using Sn solvent					Magnetic properties of EuPtSi3 single crystals			Department of Condensed Matter Physics and Material Sciences, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India	Phys.Rev.B, 81(2010)144414	Neeraj Kumar,S. K. Dhar,A. Thamizhavel,P. Bonville,P. Manfrinetti		
154930	PRB081220501	[penet]^2 = (1-t^n): n=1.13. Thermal cond. k/T = T^2 + b, b = 25 mW/K2m for low T region. sign changing line node SC.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																3	2010																										AB2C2		ThCr2Si2																	Fe-122	K	29.8	30	30.5				30																				T	SP, Torque			51.6										MHC154930							nm	tunnel diode		200																	W/K.m				MTHC154930													62			30															self-flux method					Line nodes in the energy gap of superconducting BaFe2(As1-xPx)2 single crystals as seen via penetration depth and thermal conductivity			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.B, 81(2010)220501	K. Hashimoto,M. Yamashita,S. Kasahara,Y. Senshu,N. Nakata,S. Tonegawa,K. Ikada,A. Serafin,A. Carrington,T. Terashima,H. Ikeda,T. Shibauchi,Y. Matsuda1		
154931	PRB086064515	RRR = 1.4 for P=0 GPa. Tc defined as max of (dR/dT). HCFIG shows Hc2(T) for various P.	YPtBi	Y1Pt1Bi1	Y	1	Pt	1	Bi	1																		3	2012																										ABC			F4[-]3m		A	6.65													Half Heusler compd.	K		0.77				0.06	0.77	MTC154931		K/GPa	0.044																T	Max of (dR/dT), extraporation	1.23							T/K	Max of (dR/dT)	1.9			MHC154931																																					uOhm.cm							160			4	230										n/cm3	22000000000000000000			Y:Pt:Bi=1:1:1.4. melt(Y,Pt) with Bi - in alumina crucible - in quartz tube(Ar) - heat(1250C,24h) -cool to 900C(1C/h)					Superconductivity in noncentrosymmetric YPtBi under pressure			Van der Waals - Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Phys.Rev.B, 86(2012)064515	T. V. Bay,T. Naka,Y. K. Huang,A. de Visser		
154932	PRB090035115	T<str> = 147 K (Fm3[-]n to I4[-]3d observed in R(T9, C(T), and SUS(T).	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2014																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.8156														K		5					5																																																					MSP154932			mJ/mol.K2	40																																							self-flux method using Sn-flux.					Unconventional charge-density wave in Sr3Ir4Sn13 cubic superconductor revealed by optical spectroscopy study			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Phys.Rev.B, 90(2014)035115	A. F. Fang,X. B. Wang,P. Zheng,N. L. Wang		
154933	PRB090014513	RRR=31. Tc(SP)=0.72 K. DOS=1.95 states/eV.mol. GL = 0.55(Type-1 SC). e-ph = 0.41. (dC/gamma*Tc) = 1.09. cohere(L) = 2081nm. penet(clean) = 33.7 nm	LaIrSi3	La1Ir1Si3	La	1	Ir	1	Si	3																		1	2014																										ABC3		BaNiSn3	I4mm	107	A	4.2784		9.8308												K	1.3	1.45	1.6				1.45																				mT	Hc(0) estimated from Ce(T) using entropy	6.1							mT					MHC154933	Hc from RES, Hc from C(T)	nm		373			nm	dirty limit	205					3.08	14				MSP154933	mJ/mol.K	3.6	mJ/mol.K2	4.6	SP	385	SP											uOhm.cm							2.7			1.6	83.7												La(3N),Ir(4N),Si(5N)		arc-melting - ANN(900C,1w, in vac)					Physical properties of noncentrosymmetric superconductor LaIrSi3: A muon-SR study			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, Oxon OX11 0QX, United Kingdom	Phys.Rev.B, 90(2014)014513	V. K. Anand,D. Britz,A. Bhattacharyya,D. T. Adroja,A. D. Hillier,A. M. Strydom,W. Kockelmann,B. D. Rainford,K. A. McEwen		
154934	PRB090054510	La2O2S,Y2O2S impurity phases(total less than 1% in mass fraction) . lattice term in SP (beta)=0.88 mJ/mol.K4. (dC/gamma*Tc) = 0.8	(La,Y)(O,F)BiS2	La0.95Y0.05F0.5Bi1S2O0.5	La	0.95	Y	0.05	F	0.5	Bi	1	S	2											O	0.5		1	2014																												CeOBiS2	P4/nmm																	K		2.5		2.5			2.5	MTC154934																																																							mJ/mol.K2	3.22	SP	222	SP																																		La,Y,S,LaF3,Bi2O3,Bi2S3		mixture - pellet - in evacuated quartz tube - ANN(800C,2d)					Effect of yttrium substitution on the superconducting properties of La1-xYxO0.5F0.5BiS2			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 90(2014)054510	I. Jeon,D. Yazici,B. D. White,A. J. Friedman,M. B. Maple		
154935	PRB090054510	La2O2S,Y2O2S impurity phases(total nearly 8% in mass fraction) . lattice term in SP (beta)=0.83 mJ/mol.K4. (dC/gamma*Tc) = 0.9	(La,Y)(O,F)BiS2	La0.75Y0.25F0.5Bi1S2O0.5	La	0.75	Y	0.25	F	0.5	Bi	1	S	2											O	0.5		1	2014																												CeOBiS2	P4/nmm																	K		3.1		3.1			3.1	MTC154934																																																							mJ/mol.K2	2.21	SP	227	SP																																		La,Y,S,LaF3,Bi2O3,Bi2S3		mixture - pellet - in evacuated quartz tube - ANN(800C,2d)					Effect of yttrium substitution on the superconducting properties of La1-xYxO0.5F0.5BiS2			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 90(2014)054510	I. Jeon,D. Yazici,B. D. White,A. J. Friedman,M. B. Maple		
155000	JPCM025362204	P-induced SC. Pcr = 12 GPa. Tc(max) = 8.2 K(P=17.2 GPa). Low-P phase for P < 12 GPa. High-P phase for P > 12 GPa. lattice C at P=0.35 GPa. SC properties for P=23 GPa.	Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2013																										A2B3			R3[-]m																values for P<12 GPa:  rhombohedral	K			8.2		0		8.2	MTC155000																			T	RES(onset), WHH			4.7					T/K	RES(onset)			1.02	MHC155000																																																										n/cm3	2000000000000000000	Bi(5N),Se(5N)		Bridgman method. mixture(Bi:Se=2:3) - pellet - sealed in quartz ampule) - heat to 800C for 2 days - cool to 550 C(3 C/h) - hold(3d) - slow cool to RT					Superconductivity of the topological insulator Bi2Se3 at high pressure			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, People's Republic of China	J.Phys:Condens.Matter, 25(2013)362204	P P Kong,J L Zhang,S J Zhang,J Zhu,Q Q Liu,R C Yu,Z Fang,C Q Jin,W G Yang,X H Yu,J L Zhu,Y S Zhao		
155001	PRB084184523	SC properties at P = 0 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	z	6.98	1	2011																												Y123																		K		89.6					89.6																																																3.87	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155002	PRB084184523	SC properties at P = 1.4 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.98	Y	1	Ba	2	Cu	3															O	z	6.98	1	2011																												Y123																		K		89.5					89.5																																																3.6	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155003	PRB084184523	SC properties at P = 0 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	1	2011																												Y123																		K		77.1					77.1																																																3.02	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155004	PRB084184523	SC properties at P = 1.1 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	z	6.8	1	2011																												Y123																		K		83.2					83.2																																																3.48	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155005	PRB084184523	SC properties at P = 0 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	z	6.66	1	2011																												Y123																		K		58.9					58.9																																																3.02	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155006	PRB084184523	SC properties at P = 1.1 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.66	Y	1	Ba	2	Cu	3															O	z	6.66	1	2011																												Y123																		K		62.6					62.6																																																3.27	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155007	PRB084184523	SC properties at P = 0 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	z	6.45	1	2011																												Y123																		K		45.4					45.4																																																3	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155008	PRB084184523	SC properties at P = 1.1 GPa. Tc, gap measured by muon-SR at H=0.1 T. [penet] not given explicitly	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	z	6.45	1	2011																												Y123																		K		49.5					49.5																																																3	16																																													Y2O3,CuO,BaCO3	1	solid state reaction method					Muon spin rotation investigation of the pressure effect on the magnetic penetration depth in YBa2Cu3Ox			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut , CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 84(2011)184523	A.Maisuradze,A.Shengelaya,A.Amato,E.Pomjakshina,H.Keller		
155009	MAT1208.5873	Lattice term in SP (beta) = 0.764 mJ/mol.K4	Pr(O,F)BiS2	Pr1Bi1S2F0.5O0.5	Pr	1	Bi	1	S	2	F	0.5													O	0.5		1	2012																										ABCD2		CeOBiS2	P4/nmm		A	4.015		13.362												K	3.1		3.7	3.7			3.7											Oe	M-H curve				8			2.1	T	peak of (dR/dT),  WHH	6.4							T/K	peak of (dR/dT)	3																									mJ/mol.K2	286.36	SP																																				Pr,Bi,S,PrF3,Pr6O11		solid state reaction. mixture - pellet - sealed in quartzampule - heat(780C,12h, at a rate of 2C/min) - cool to RT (6h)					Synthesis and superconductivity of new BiS2 based superconductor PrO0.5F0.5BiS2			Quantum Phenomena and Applications Division, National Physical Laboratory (CSIR), Dr. K.S. Krishnan Marg, New Delhi-110012, India	cond-mat/1208.5873	Rajveer Jha,Anuj Kumar,Shiva Kumar Singh,V.P. S. Awana		
155010	NJP013123022	[penet] measured by diode method. Absolute value of [penet] estimated from [gamma] and Hc2(0).	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2011																										ABC2		CeNiC2	Amm2																	K		3					3																				T		0.125																			A	diode method	1230													mJ/mol.K2	7																																					La(3N),C(5N5),Ni(4N5)		arc-melting - ANN(1273C,10d, in quartz tube(Ar)) - Q to water(RT)					Nodal gap structure in the noncentrosymmetric superconductor LaNiC2 from magnetic-penetration-depth measurements			Centro de Fisica, Instituto Venezolano de Investigaciones Cientificas, Apartado 20632, Caracas 1020-A, Venezuela	J.New Phys., 13(2011)123022	I Bonalde,R L Ribeiro,K J Syu,H H Sung,W H Lee		
155011	PHC5030132	Film(100nm thickness) on Fe film(20nm). Energy gap measured by reflectivity. Reflectivity change could be influenced by SDW.	Ba(Fe,Co)2As2	Ba1Fe1.84Co0.16As2	Ba	1	Fe	1.84	Co	0.16	As	2																4	2014																												ThCr2Si2																		K			26.3				26.3																																														meV	3.67	3.4	17																																															Laser deposition on substrate (001)[100]MgO.					Evaluation of superconducting gaps in optimally doped Ba(Fe1-xCox)2As2/Fe bilayers by ultrafast time-resolved spectroscopy			Dipartimento Scienze Fisiche, Universita di Napoli Federico II, Facolta di Ingegneria, I-80125 Napoli, Italy	Physica C, 503(2014)132	C. Bonavolonta,C. de Lisio,M. Valentino,L. Parlato,G.P. Pepe,F. Kurth,K. Iida		
155012	PRB090054505	not SC	Mo2As3	As3Mo2	As	3	Mo	2																				1	2014																										A2B3	4		C2/m		A	13.3684	3.2347	9.642											monoclinic, beta = 124.593	K					2																																																										mJ/mol.K2	7.2	SP																																						mixture(Mo:As=2:3) - heat to 350C(50C/h,hold 5h) - heat to 600C(30C/h,hold 20h) - heat to 650C(20C/h,hold 40h) - pellet - ANN(875C,45h) - ANN(1080C,80h)					Evidence for superconductivity at Tc = 12 K in oxygen-deficient MoO2-z and properties of molybdenum arsenide and oxide binaries			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 90(2014)054505	D. Parker,J. C. Idrobo,C. Cantoni,A. S. Sefat		
155013	PRB090054505	not SC	Mo5As4	As4Mo5	As	4	Mo	5																				1	2014																										A4B5	2		I4/m		A	9.5957		3.2273											tetragonal	K					2																																																										mJ/mol.K2	13.4	SP																																						mixture(Mo:As=5:4) - heat to 350C(50C/h,hold 5h) - heat to 600C(30C/h,hold 20h) - heat to 650C(20C/h,hold 40h) - pellet - ANN(875C,45h) - ANN(975C,50h)					Evidence for superconductivity at Tc = 12 K in oxygen-deficient MoO2-z and properties of molybdenum arsenide and oxide binaries			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 90(2014)054505	D. Parker,J. C. Idrobo,C. Cantoni,A. S. Sefat		
155014	PRB090054505	mixture of Mo2As3, Mo5As4, MoO2. Then SC comes from MoO2(4% difficient-O)	MoO2-z	Mo1O2-z	Mo	1																			O	2-z			2014																										AB2	4		P2<1>/c		A	5.5397	4.8566	5.626											monoclinic, beta = 119.70	K				12			12										8	Oe	M-H curve				900		2																																																																																			Evidence for superconductivity at Tc = 12 K in oxygen-deficient MoO2-z and properties of molybdenum arsenide and oxide binaries			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 90(2014)054505	D. Parker,J. C. Idrobo,C. Cantoni,A. S. Sefat		
155015	ACS13014428	T<STR> = 120 K, where structural and/or magnetic transitions, measured by R-anomaly.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																	2008																										ABCD			P4/nmm		A	3.878		8.593											ZrCuSiAs-type	K					2																																																																																																CaF2(4N),CaAs,Fe2As,Co2As		mixture - press - heat(1000C,10h, in evacuated silica tube)					Superconductivity Induced by Co-Doping in Quaternary Fluoroarsenide CaFeAsF			Frontier Research Center, Materials and Structures Laboratory, and ERATO-SORST, JST, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 130(2008)14428	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Hiroshi Yanagi,Masahiro Hirano,Hideo Hosono		
155016	ACS13014428		Ca(Fe,Co)AsF	Ca1Fe0.9Co0.1As1F1	Ca	1	Fe	0.9	Co	0.1	As	1	F	1															2008																										ABCD					A	3.881		8.552											ZrCuSiAs-type	K		22	23				22	MTC155016																																																																																													CaF2(4N),CaAs,Fe2As,Co2As		mixture - press - heat(1000C,10h, in evacuated silica tube)					Superconductivity Induced by Co-Doping in Quaternary Fluoroarsenide CaFeAsF			Frontier Research Center, Materials and Structures Laboratory, and ERATO-SORST, JST, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 130(2008)14428	Satoru Matsuishi,Yasunori Inoue,Takatoshi Nomura,Hiroshi Yanagi,Masahiro Hirano,Hideo Hosono		
155017	ACS1360846	not SC. CaFe2As2, PrAs detected.	(Ca,Pr)Fe1.9As2.1	Ca0.9Pr0.1Fe1.9As2.1	Ca	0.9	Pr	0.1	Fe	1.9	As	2.1																	2014																										AB2C2																			122-type	K					2																																																																																																FeAs(3N),PrAs(3N),Ca(2N),As(4N),CaO(3N)		mixture - pellet - sealed in evacuated quartz ampules with alumina crucible - heat(1000-1200C,24h)					A New Layered Iron Arsenide Superconductor: (Ca,Pr)FeAs2			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Am.Chem.Soc., 136(2014)846	Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Tetsuya Tohei,Yuichi Ikuhara,Yoshito Gotoh,Hiroshi Fujihisa,Kunimitsu Kataoka,Hiroshi Eisaki,Jun-ichi Shimoyama		
155018	ACS1360846	CaFe2As2, PrAs detected. Plate like single crystals(112-phase)	(Ca,Pr)Fe1.3As1.8O0.2	Ca0.9Pr0.1Fe1.3As1.8O0.2	Ca	0.9	Pr	0.1	Fe	1.3	As	1.8													O	0.2		3	2014																										ABC2			P2<1>/m		A	3.9163	3.8953	10.311											112-phase. monoclinic, beta=90.788	K	12		24	20			20																																																																																														FeAs(3N),PrAs(3N),Ca(2N),As(4N),CaO(3N)		mixture - pellet - sealed in evacuated quartz ampules with alumina crucible - heat(1000-1200C,24h)					A New Layered Iron Arsenide Superconductor: (Ca,Pr)FeAs2			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Am.Chem.Soc., 136(2014)846	Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Tetsuya Tohei,Yuichi Ikuhara,Yoshito Gotoh,Hiroshi Fujihisa,Kunimitsu Kataoka,Hiroshi Eisaki,Jun-ichi Shimoyama		
155019	ACS1360846	FeAs2 detected. 112-phase.	(Ca,Pr)FeAs2	Ca0.9Pr0.1Fe1As2	Ca	0.9	Pr	0.1	Fe	1	As	2																	2014																										ABC2																			112-type phase	K				20			20																																																																																														FeAs(3N),PrAs(3N),Ca(2N),As(4N),CaO(3N)		mixture - pellet - sealed in evacuated quartz ampules with alumina crucible - heat(1000-1200C,24h)					A New Layered Iron Arsenide Superconductor: (Ca,Pr)FeAs2			Department of Applied Chemistry, The University of Tokyo, 7-3-1 Hongo, Bunkyo, Tokyo 113-8656, Japan	J.Am.Chem.Soc., 136(2014)846	Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Tetsuya Tohei,Yuichi Ikuhara,Yoshito Gotoh,Hiroshi Fujihisa,Kunimitsu Kataoka,Hiroshi Eisaki,Jun-ichi Shimoyama		
155020	EPL08467007	not SC. T<SDW> = 175 K = T<STR>. SDW induced structural transition . lattice term in SP (beta) = 0.2 mJ/mol.K4	SrFeAsF	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																1	2008																										ABCD	2		P4/nmm		A	3.993		8.9546											ZrCuSiAs-type. For T<175, space-G = Cmme, a=5.6155, b=5.6602, c=8.9173 at T=10 K.	K					4.2																																																										mJ/mol.K2	1.5	SP	339	SP																																				mixture(SrF2:Sr:Fe:As=1:1:2:2) - heat to 1173 K(50K/h) - keep(40h) - cool to RT - reground - press to pellet - SIN(1273K,48h)					Synthesis, crystal structure and spin-density-wave anomaly of the iron arsenide-fluoride SrFeAsF			Department Chemie und Biochemie, Ludwig-Maximilians-Universitat Munchen - Butenandtstrasse 5-13 (Haus D), 81377 Munchen, Germany, EU	EuroPhys.Lett., 84(2008)67007	M. Tegel,S. Johansson,V. Weiss,I. Schellenberg,W. Hermes,R. Pottgen,D. Johrendt		
155021	EPL08517011	T<STR> = T<SDW> = 173 K determined by R(T)	SrFeAsF	Sr1Fe1As1F1	Sr	1	Fe	1	As	1	F	1																	2009																										ABCD	2				A	4.004		8.971											ZrCuSiAs-type	K					2																																																																																																LaAs,SrAs,FeF3(2N),Fe(4N)		mixture - pellet - sealed in silica tube(0.2 bar(Ar) - heat(950C,60h) - slow cool to RT - reground - SIN(1000C,30h)					Superconductivity in fluoride-arsenide Sr1-xLaxFeAsF compounds			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	Europhys.Lett., 85(2009)17011	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Lei Fang,Hai-Hu Wen		
155022	EPL08517011	T<STR> = T<SDW> = 60 K determined by R(T)	(Sr,La)FeAsF	Sr0.8La0.2Fe1As1F1	Sr	0.8	La	0.2	Fe	1	As	1	F	1															2009																										ABCD	2				A	3.976		8.96											ZrCuSiAs-type	K			24.4				24.4																																																																																														LaAs,SrAs,FeF3(2N),Fe(4N)		mixture - pellet - sealed in silica tube(0.2 bar(Ar) - heat(950C,60h) - slow cool to RT - reground - SIN(1000C,30h)					Superconductivity in fluoride-arsenide Sr1-xLaxFeAsF compounds			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	Europhys.Lett., 85(2009)17011	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Lei Fang,Hai-Hu Wen		
155023	EPL08517011		(Sr,La)FeAsF	Sr0.6La0.4Fe1As1F1	Sr	0.6	La	0.4	Fe	1	As	1	F	1															2009																										ABCD	2																		ZrCuSiAs-type	K	24.6		29.5				27.05																																																																																														LaAs,SrAs,FeF3(2N),Fe(4N)		mixture - pellet - sealed in silica tube(0.2 bar(Ar) - heat(950C,60h) - slow cool to RT - reground - SIN(1000C,30h)					Superconductivity in fluoride-arsenide Sr1-xLaxFeAsF compounds			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	Europhys.Lett., 85(2009)17011	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Lei Fang,Hai-Hu Wen		
155024	EPL08517011	T<STR> = T<SDW> = 153 K determined by R(T)	EuFeAsF	Eu1Fe1As1F1	Eu	1	Fe	1	As	1	F	1																	2009																										ABCD	2				A	3.974		8.929											ZrCuSiAs-type	K					2																																																																																																EuAs,FeF3(2N),Fe(4N)		mixture - pellet - sealed in silica tube(0.2 bar(Ar) - heat(950C,60h) - slow cool to RT - reground - SIN(1000C,30h)					Superconductivity in fluoride-arsenide Sr1-xLaxFeAsF compounds			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	Europhys.Lett., 85(2009)17011	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Lei Fang,Hai-Hu Wen		
155025	EPL08517011	T<STR> = T<SDW> = 118 K determined by R(T)	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																	2009																										ABCD	2				A	3.88		8.594											ZrCuSiAs-type	K					2																																																																																																CaAs,FeF3(2N),Fe(4N)		mixture - pellet - sealed in silica tube(0.2 bar(Ar) - heat(950C,60h) - slow cool to RT - reground - SIN(1000C,30h)					Superconductivity in fluoride-arsenide Sr1-xLaxFeAsF compounds			National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - P. O. Box 603, Beijing 100190, PRC	Europhys.Lett., 85(2009)17011	Xiyu Zhu,Fei Han,Peng Cheng,Gang Mu,Bing Shen,Lei Fang,Hai-Hu Wen		
155026	JAC6220640	impurity: 7 wt%Sn. not SC. R(T), C(T) shows anomaly at 0.9 K due to AFM short range order (maybe). RRR = 3. Debye-T = 81.3K from R(T).	TmSnGe	Tm1Sn1Ge1	Tm	1	Sn	1	Ge	1																			2015					myu-B/mol	7.61	0	0.9																		ABC	3		Cmcm	63	A	4.2029	15.9695	4.0211												K					0.35																																																																									uOhm.cm							23				67												Tm(or Lu),Sn(4N),Ge(4N)		arcmelting - ANN(773K,1W, in evacuated silica tube)					Low-temperature physical properties of TmSnGe and LuSnGe			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	J.Alloys Compd., 622(2015)640	Dariusz Kaczorowski,Andrzej Szytu?a		
155027	JAC6220640	impurity= 5 wt%-Sn. RRR = 3. Debye-T = 119.9 K from R(T). lattice term in SP: beta = 2.12E-4 mJ/mol.K4. (dC) = 3.5 mJ/K at Tc(=0.74K). (dC/gamma*Tc) = 1.28	LuSnGe	Lu1Sn1Ge1	Lu	1	Sn	1	Ge	1																			2015																										ABC	3		Cmcm	63	A	4.1791	15.858	4.013												K	0.4		0.74				0.57																				T	SP	0.04														A	from Hc2	910			A	GL eq.	2830													mJ/mol.K2	3.7	SP	302	SP											uOhm.cm							8				25												Tm(or Lu),Sn(4N),Ge(4N)		arcmelting - ANN(773K,1W, in evacuated silica tube)					Low-temperature physical properties of TmSnGe and LuSnGe			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O. Box 1410, 50-950 Wroc?aw, Poland	J.Alloys Compd., 622(2015)640	Dariusz Kaczorowski,Andrzej Szytu?a		
155028	JPS083063704	Low-P phase for P < 0.7 GPa. Phase transition to high-P phase at P=0.7 GPa.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																											2		P4/nmm		A	4.0877		13.4703												K			2.5				2.5			K/GPa	-0.28																																																																																																	Pressure-Induced Enhancement of Superconductivity and Structural Transition in BiS2-Layered LaO1-xFxBiS2			Department of Physics, College of Humanities and Sciences, Nihon University, Setagaya, Tokyo 156-8550, Japan	J.Phys.Soc.Jpn, 83(2014)063704	Takahiro Tomita,Masaya Ebata,Hideto Soeda,Hiroki Takahashi,Hiroshi Fujihisa,Yoshito Gotoh,Yoshikazu Mizuguchi,Hiroki Izawa,Osuke Miura,Satoshi Demura,Keita Deguchi,Yoshihiko Takano		
155029	JPS083063704	High-P phase for P > 0.7 GPa.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2014																											4		P2<1>/m		A	4.046	4.025	13.022											monoclinic. beta = 97.902	K			10.7				10.7																																																																																																					Pressure-Induced Enhancement of Superconductivity and Structural Transition in BiS2-Layered LaO1-xFxBiS2			Department of Physics, College of Humanities and Sciences, Nihon University, Setagaya, Tokyo 156-8550, Japan	J.Phys.Soc.Jpn, 83(2014)063704	Takahiro Tomita,Masaya Ebata,Hideto Soeda,Hiroki Takahashi,Hiroshi Fujihisa,Yoshito Gotoh,Yoshikazu Mizuguchi,Hiroki Izawa,Osuke Miura,Satoshi Demura,Keita Deguchi,Yoshihiko Takano		
155030	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)Fe(As,Sb)2	Ca0.88La0.12Fe1As1.8Sb0.2	Ca	0.88	La	0.12	Fe	1	As	1.8	Sb	0.2														3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9738	3.896	10.3495											monoclinic. beta = 91.72  Fe-112 type	K	47		49	47.2			47.2										100																																																													mOhm.cm												0.454											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155031	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)Fe(As,Sb)2	Ca0.85La0.15Fe1As1.98Sb0.02	Ca	0.85	La	0.15	Fe	1	As	1.98	Sb	0.02														3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9516	3.8895	10.3466											monoclinic. beta = 91.44  Fe-112 type	K				43			43																																																																							mOhm.cm												0.349											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155032	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.85La0.15Fe1As2	Ca	0.85	La	0.15	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9523	3.8762	10.3505											monoclinic. beta = 91.18  Fe-112 type	K				35.1			35.1																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155033	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.84La0.16Fe1As2	Ca	0.84	La	0.16	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9525	3.8797	10.3505											monoclinic. beta = 91.19  Fe-112 type	K				34			34																																																																							mOhm.cm												0.251											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155034	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.81La0.19Fe1As2	Ca	0.81	La	0.19	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A														monoclinic. Fe-112 type	K				28.1			28.1																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155035	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.79La0.21Fe1As2	Ca	0.79	La	0.21	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9489	3.8816	10.3522											monoclinic. beta = 91.33  Fe-112 type	K				28			28																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155036	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.78La0.22Fe1As2	Ca	0.78	La	0.22	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9497	3.8793	10.3452											monoclinic. beta =  91.20 Fe-112 type	K				21.8			21.8																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155037	JPS083093705	plate like single crystals obtained from samples.	(Ca,La)FeAs2	Ca0.75La0.25Fe1As2	Ca	0.75	La	0.25	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>		A	3.9577	3.8781	10.3693											monoclinic. beta = 91.37  Fe-112 type	K				0			0																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155038	JPS083093705	not bulk SC.plate like single crystals obtained from samples.	(Ca,Ce)FeAs2	Ca0.81Ce0.19Fe1As2	Ca	0.81	Ce	0.19	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				0			0																																																																							mOhm.cm												0.488											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155039	JPS083093705	plate like single crystals obtained from samples.	(Ca,Ce)Fe(As,Sb)2	Ca0.84Ce0.16Fe1As1.98Sb0.02	Ca	0.84	Ce	0.16	Fe	1	As	1.98	Sb	0.02														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				21			21																																																																							mOhm.cm												0.36											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155040	JPS083093705	plate like single crystals obtained from samples.	(Ca,Ce)Fe(As,Sb)2	Ca0.76Ce0.24Fe1As1.8Sb0.2	Ca	0.76	Ce	0.24	Fe	1	As	1.8	Sb	0.2														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				43			43																																																																																														Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155041	JPS083093705	plate like single crystals obtained from samples.	(Ca,Pr)FeAs2	Ca0.8Pr0.2Fe1As2	Ca	0.8	Pr	0.2	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				10			10										5																																																													mOhm.cm												0.423											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155042	JPS083093705	plate like single crystals obtained from samples.	(Ca,Pr)Fe(As,Sb)2	Ca0.82Pr0.18Fe1As1.98Sb0.02	Ca	0.82	Pr	0.18	Fe	1	As	1.98	Sb	0.02														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				26			26																																																																							mOhm.cm												0.499											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155043	JPS083093705	plate like single crystals obtained from samples.	(Ca,Pr)Fe(As,Sb)2	Ca0.76Pr0.24Fe1As0.9Sb0.1	Ca	0.76	Pr	0.24	Fe	1	As	0.9	Sb	0.1														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K	43			43			43																																																																							mOhm.cm												0.55											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155044	JPS083093705	plate like single crystals obtained from samples.	(Ca,Nd)FeAs2	Ca0.81Nd0.19Fe1As2	Ca	0.81	Nd	0.19	Fe	1	As	2																3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				11			11										5																																																													mOhm.cm												0.336											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155045	JPS083093705	plate like single crystals obtained from samples.	(Ca,Nd)Fe(As,Sb)2	Ca0.81Nd0.19Fe1As1.98Sb0.02	Ca	0.81	Nd	0.19	Fe	1	As	1.98	Sb	0.02														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K				24			24																																																																							mOhm.cm												0.689											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155046	JPS083093705	plate like single crystals obtained from samples.	(Ca,Nd)Fe(As,Sb)2	Ca0.84Nd0.16Fe1As0.9Sb0.1	Ca	0.84	Nd	0.16	Fe	1	As	0.9	Sb	0.1														3	2014																										ABC2	4	Fe-112	P2<1>																monoclinic. Fe-112 type	K	37			43			43																																																																							mOhm.cm												0.328											Ca,R,FeAs,As,Sb		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Superconducting Transition Temperatures of up to 47K from Simultaneous Rare-Earth Element and Antimony Doping of 112-Type CaFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093705	Kazutaka Kudo,Yutaka Kitahama,Kazunori Fujimura,Tasuku Mizukami,Hiromi Ota,Minoru Nohara		
155047	JPS083093706	Li-vacancy(x=1.8 in LixIrSi3). RRR = 11. Tc(SP) = 3.75 K. (dC/Tc) = 7.4 mJ/mol.K2. (dC/gamma*Tc)  = 1.41. Debye-T = 330 K from R(T).	Li2IrSi3	Li2Ir1Si3	Li	2	Ir	1	Si	3																		1	2014																										AB2C3			P31c	159	A	5.0139		7.8397												K	3.7		3.9	3.8		0.1	3.8										72										T	RES(0.5Rn), Linear approx.	0.3												MHC155047		A	from Hc2	330																		mJ/mol.K2	5.3	SP	484	SP											uOhm.cm							9.8																		arc-melting (IrSi3) . Then, arc-melting (Li + IrSi3)					Superconductivity in Noncentrosymmetric Iridium Silicide Li2IrSi3			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093706	Sunseng Pyon,Kazutaka Kudo,Jun-ichi Matsumura,Hiroyuki Ishii,Genta Matsuo,Minoru Nohara,Hajime Hojo,Kengo Oka,Masaki Azuma,V. Ovidiu Garlea,Katsuaki Kodama,Shin-ichi Shamoto		
155048	JPS083093706	RRR = 1.3. Debye-T = 397 K from R(T).	IrSi3	Ir1Si3	Ir	1	Si	3																				1	2014																										AB3																				K					2																																																										mJ/mol.K2	0.73	SP	516	SP											uOhm.cm							234																		arc-melting (IrSi3) . Then, arc-melting (Li + IrSi3)					Superconductivity in Noncentrosymmetric Iridium Silicide Li2IrSi3			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)093706	Sunseng Pyon,Kazutaka Kudo,Jun-ichi Matsumura,Hiroyuki Ishii,Genta Matsuo,Minoru Nohara,Hajime Hojo,Kengo Oka,Masaki Azuma,V. Ovidiu Garlea,Katsuaki Kodama,Shin-ichi Shamoto		
155049	JPS083104702	RRR = 3. not SC. as-grown sample	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2014								197																		AB2C2	2	ThCr2Si2			A	3.9214		12.3431											Fe-122	K					1.8																																																																																							cm3/C						MRH155049					self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155050	JPS083104702	as-grown sample	SrFe2(As,P)2	Sr1Fe2As1.4P0.6	Sr	1	Fe	2	As	1.4	P	0.6																3	2014								49.5																		AB2C2	2	ThCr2Si2			A	3.9054		12.1034											Fe-122	K	27.9						27.9																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155051	JPS083104702	as-grown sample	SrFe2(As,P)2	Sr1Fe2As1.3P0.7	Sr	1	Fe	2	As	1.3	P	0.7																3	2014																										AB2C2	2	ThCr2Si2			A	3.9028		12.0974											Fe-122	K	29.6						29.6																																																																																					cm3/C						MRH155051					self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155052	JPS083104702	as-grown sample	SrFe2(As,P)2	Sr1Fe2As1.22P0.78	Sr	1	Fe	2	As	1.22	P	0.78																3	2014																										AB2C2	2	ThCr2Si2			A	3.8975		12.0077											Fe-122	K	24.9						24.9	MTC155052																																																																																															self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155053	JPS083104702	as-grown sample	SrFe2(As,P)2	Sr1Fe2As1.08P0.92	Sr	1	Fe	2	As	1.08	P	0.92																3	2014																										AB2C2	2	ThCr2Si2			A	3.8932		11.9221											Fe-122	K	19.2						19.2																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155054	JPS083104702	as-grown sample	SrFe2(As,P)2	Sr1Fe2As1P1	Sr	1	Fe	2	As	1	P	1																3	2014																										AB2C2	2	ThCr2Si2			A	3.8842		11.932											Fe-122	K	3.69						3.69																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155055	JPS083104702	not SC. as-grown sample	SrFe2(As,P)2	Sr1Fe2As0.8P1.2	Sr	1	Fe	2	As	0.8	P	1.2																3	2014																										AB2C2	2	ThCr2Si2			A	3.8667		11.8307											Fe-122	K					1.8																																																																																																		self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155056	JPS083104702	RRR = 10. not SC. post-annealed(500C,1w) sample.	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K					1.8																																																																																							cm3/C						MRH155056					self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155057	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As1.4P0.6	Sr	1	Fe	2	As	1.4	P	0.6																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	33.9						33.9																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155058	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As1.3P0.7	Sr	1	Fe	2	As	1.3	P	0.7																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	34						34																																																																																					cm3/C						MRH155058					self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155059	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As1.22P0.78	Sr	1	Fe	2	As	1.22	P	0.78																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	29.8						29.8	MTC155059																																																																																															self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155060	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As1.08P0.92	Sr	1	Fe	2	As	1.08	P	0.92																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	26.8						26.8																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155061	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As1P1	Sr	1	Fe	2	As	1	P	1																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	14.5						14.5																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155062	JPS083104702	post-annealed(500C,1w) sample.	SrFe2(As,P)2	Sr1Fe2As0.8P1.2	Sr	1	Fe	2	As	0.8	P	1.2																3	2014																										AB2C2	2	ThCr2Si2																	Fe-122	K	6.26						6.26																																																																																																self-flux method. molar ratio(Sr:FeP:Sn=1:2:20) - alumina crucible - sealed in silica tube - heat to 1300C - slow cool to 650C - decanted in centrifuge					Electronic Phase Diagram of SrFe2(As1-xPx)2: Effect of Structural Dimensionality			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 83(2014)104702	Tatsuya Kobayashi,Shigeki Miyasaka,Setsuko Tajima,Noriko Chikumoto		
155063	JPS084023705	"quasi crystal. Tsai-type cluster. mol means ""mol-cluster"". (dC/Tc) = 138 mJ/mol-cluster.K2. (dC/gamma*Tc) = 1.26. Hc(0) = 78.7 Oe. GL = 28.6. Wilson ratio = 1."	Au-Ge-Yb	Au0.64Ge0.22Yb0.14	Au	0.64	Ge	0.22	Yb	0.14																			2015																																													Tsai-type-cluster	K	0.63		0.68				0.655											Oe		6.7							T	SUS, WHH	0.318							T/K	SUS	0.584			MHC155063		A	from Hc2	322			A		9200													mJ/mol.K2	109	SP	160	SP											uOhm.cm	150.8			150.8			150.8																Au(4N),Ge(5N),Yb(3N)		mixture - in alumina crucible - sealed in quartz tube - heat to 1000C - cool to 800C - slow cool to 450C - Q to water					Superconductivity of Au-Ge-Yb Approximants with Tsai-Type Clusters			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)023705	Kazuhiko Deguchi,Mika Nakayama,Shuya Matsukawa,Keiichiro Imura,Katsumasa Tanaka,Tsutomu Ishimasa,Noriaki K. Sato		
155064	JPS084023705	"quasi crystal. Tsai-type cluster. mol means ""mol-cluster"". (dC/Tc) = 218 mJ/mol-cluster.K2. (dC/gamma*Tc) = 0.54. Hc(0) = 50.0 Oe. GL = 25.9. Wilson ratio = 3."	Au-Ge-Yb	Au0.635Ge0.205Yb0.16	Au	0.635	Ge	0.205	Yb	0.16																			2015	emu/mol	0.0048					104																																						Tsai-type-cluster	K	0.29		0.36				0.325											Oe		4.5							T	SUS, WHH	0.183							T/K	SUS	0.675			MHC155064		A	from Hc2	424			A		11000													mJ/mol.K2	251	SP	157	SP											uOhm.cm	135.8			135.8			135.8																Au(4N),Ge(5N),Yb(3N)		mixture - in alumina crucible - sealed in quartz tube - heat to 1000C - cool to 800C - slow cool to 450C - FC to RT					Superconductivity of Au-Ge-Yb Approximants with Tsai-Type Clusters			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)023705	Kazuhiko Deguchi,Mika Nakayama,Shuya Matsukawa,Keiichiro Imura,Katsumasa Tanaka,Tsutomu Ishimasa,Noriaki K. Sato		
155065	JPS084024723	filamentary SC	La(O,F)Bi(S,Se)	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0516		13.4315											BiS2-layerd SC	K	2.49			2.49			2.49																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155066	JPS084024723	filamentary SC	La(O,F)Bi(S,Se)	La1Bi1S1.8Se0.2F0.5O0.5	La	1	Bi	1	S	1.8	Se	0.2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0654		13.4472											BiS2-layerd SC	K	2.19			2.19			2.19																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155067	JPS084024723	bulk SC	La(O,F)Bi(S,Se)	La1Bi1S1.6Se0.4F0.5O0.5	La	1	Bi	1	S	1.6	Se	0.4	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0799		13.4678											BiS2-layerd SC	K	2.5			2.5			2.5																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155068	JPS084024723		La(O,F)Bi(S,Se)	La1Bi1S1.4Se0.6F0.5O0.5	La	1	Bi	1	S	1.4	Se	0.6	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0934		13.4954											BiS2-layerd SC	K	3			3			3																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155069	JPS084024723		La(O,F)Bi(S,Se)	La1Bi1S1.2Se0.8F0.5O0.5	La	1	Bi	1	S	1.2	Se	0.8	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.1032		13.4998											BiS2-layerd SC	K	3.7			3.7			3.7																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155070	JPS084024723		La(O,F)Bi(S,Se)	La1Bi1S1Se1F0.5O0.5	La	1	Bi	1	S	1	Se	1	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.1136		13.537											BiS2-layerd SC	K	3.78			3.78			3.78	MTC155070																																																																																													Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155071	JPS084024723		La(O,F)Bi(S,Se)	La1Bi1S0.8Se1.2F0.5O0.5	La	1	Bi	1	S	0.8	Se	1.2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.1247		13.606											BiS2-layerd SC	K	3.6			3.6			3.6																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155072	JPS084024723		La(O,F)Bi(S,Se)	La1Bi1S0.6Se1.4F0.5O0.5	La	1	Bi	1	S	0.6	Se	1.4	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.1306		13.741											BiS2-layerd SC	K	3.01			3.01			3.01																																																																																														Bi2Se3,La2O3,LaF3,La2S3,Bi,S		solid state reaction. mixture - pellet - sealed in quartz tube - ANN(700C,15h)					Evolution of Superconductivity in BiS2-Based Superconductor LaO0.5F0.5Bi(S1-xSex)2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)024723	Takafumi Hiroi,Joe Kajitani,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155073	JPS084044712	Tm = 7.5 K (FM order by Ce)	(Ce,Nd)O0.3F0.7BiS2	Ce1Bi1S2F0.7O0.3	Ce	1	Bi	1	S	2	F	0.7													O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0493		13.4368											BiS2-layerd SC	K				2.68			2.68										25																																																																																				Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155074	JPS084044712	Tm = 7.5 K (FM order by Ce)	(Ce,Nd)O0.3F0.7BiS2	Ce0.8Nd0.2Bi1S2F0.7O0.3	Ce	0.8	Nd	0.2	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0381		13.4235											BiS2-layerd SC	K				3.145			3.145																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155075	JPS084044712	Tm = 7.5 K (FM order by Ce)	(Ce,Nd)O0.3F0.7BiS2	Ce0.6Nd0.4Bi1S2F0.7O0.3	Ce	0.6	Nd	0.4	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0246		13.3939											BiS2-layerd SC	K				3.256			3.256																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155076	JPS084044712	Tm = 7.5 K (FM order by Ce)	(Ce,Nd)O0.3F0.7BiS2	Ce0.4Nd0.6Bi1S2F0.7O0.3	Ce	0.4	Nd	0.6	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0187		13.4124											BiS2-layerd SC	K				3.67			3.67	MTC155076									52																																																																																				Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155077	JPS084044712	Tm = 7.5 K (FM order by Ce)	(Ce,Nd)O0.3F0.7BiS2	Ce0.2Nd0.8Bi1S2F0.7O0.3	Ce	0.2	Nd	0.8	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0102		13.4225											BiS2-layerd SC	K				4.31			4.31																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155078	JPS084044712		(Ce,Nd)O0.3F0.7BiS2	Nd1Bi1S2F0.7O0.3	Nd	1	Bi	1	S	2	F	0.7													O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	4.0009		13.4227											BiS2-layerd SC	K				4.75			4.75																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155079	JPS084044712		(Ce,Nd)O0.3F0.7BiS2	Nd0.8Sm0.2Bi1S2F0.7O0.3	Nd	0.8	Sm	0.2	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	3.9893		13.3729											BiS2-layerd SC	K				4.65			4.65	MTC155079									2																																																																																				Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155080	JPS084044712		(Ce,Nd)O0.3F0.7BiS2	Nd0.6Sm0.4Bi1S2F0.7O0.3	Nd	0.6	Sm	0.4	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	3.9843		13.1612											BiS2-layerd SC	K				4.58			4.58										16																																																																																				Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155081	JPS084044712		(Ce,Nd)O0.3F0.7BiS2	Nd0.4Sm0.6Bi1S2F0.7O0.3	Nd	0.4	Sm	0.6	Bi	1	S	2	F	0.7											O	0.3		1	2015																											2	CeOBiS2	P4/nmm		A	3.98		13.1645											BiS2-layerd SC	K					2																																																																																																Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155082	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.7Nd0.3Bi1S2F0.5O0.5	Ce	0.7	Nd	0.3	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0325		13.5387											BiS2-layerd SC	K					2																																																																																																Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155083	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.6Nd0.4Bi1S2F0.5O0.5	Ce	0.6	Nd	0.4	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0316		13.5125											BiS2-layerd SC	K				3			3																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155084	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.5Nd0.5Bi1S2F0.5O0.5	Ce	0.5	Nd	0.5	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0289		13.468											BiS2-layerd SC	K				3.48			3.48																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155085	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.4Nd0.6Bi1S2F0.5O0.5	Ce	0.4	Nd	0.6	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0236		13.4674											BiS2-layerd SC	K				3.93			3.93	MTC155085																																																																																													Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155086	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.3Nd0.7Bi1S2F0.5O0.5	Ce	0.3	Nd	0.7	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0181		13.463											BiS2-layerd SC	K				4.07			4.07																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155087	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.2Nd0.8Bi1S2F0.5O0.5	Ce	0.2	Nd	0.8	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0188		13.4881											BiS2-layerd SC	K				4.48			4.48																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155088	JPS084044712		(Ce,Nd)O0.5F0.5BiS2	Ce0.1Nd0.9Bi1S2F0.5O0.5	Ce	0.1	Nd	0.9	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0146		13.488											BiS2-layerd SC	K				4.68			4.68																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155089	JPS084044712		(Nd,Sm)O0.5F0.5BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0037		13.4629											BiS2-layerd SC	K				4.78			4.78																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155090	JPS084044712		(Nd,Sm)O0.5F0.5BiS2	Nd0.8Sm0.2Bi1S2F0.5O0.5	Nd	0.8	Sm	0.2	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	3.9985		13.4629											BiS2-layerd SC	K				5.11			5.11																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155091	JPS084044712		(Nd,Sm)O0.5F0.5BiS2	Nd0.6Sm0.4Bi1S2F0.5O0.5	Nd	0.6	Sm	0.4	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	3.9887		13.5345											BiS2-layerd SC	K				5.32			5.32	MTC155091																																																																																													Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155092	JPS084044712		(Nd,Sm)O0.5F0.5BiS2	Nd0.4Sm0.6Bi1S2F0.5O0.5	Nd	0.4	Sm	0.6	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	3.9811		13.5375											BiS2-layerd SC	K				5.51			5.51																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155093	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Ce0.4Nd0.6Bi1S2F0.3O0.7	Ce	0.4	Nd	0.6	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	4.0196		13.6446											BiS2-layerd SC	K					2																																																																																																Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155094	JPS084044712		(Ce,Nd)O0.7F0.3BiS2	Ce0.2Nd0.8Bi1S2F0.3O0.7	Ce	0.2	Nd	0.8	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	4.0146		13.6351											BiS2-layerd SC	K				2.33			2.33																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155095	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Nd1Bi1S2F0.3O0.7	Nd	1	Bi	1	S	2	F	0.3													O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	4.0104		13.5743											BiS2-layerd SC	K				3.55			3.55																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155096	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Nd0.8Sm0.2Bi1S2F0.3O0.7	Nd	0.8	Sm	0.2	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	4.011		13.5735											BiS2-layerd SC	K				4.9			4.9																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155097	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Nd0.6Sm0.4Bi1S2F0.3O0.7	Nd	0.6	Sm	0.4	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	3.9786		13.4577											BiS2-layerd SC	K				5.19			5.19	MTC155097																																																																																													Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155098	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Nd0.4Sm0.6Bi1S2F0.3O0.7	Nd	0.4	Sm	0.6	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	3.9787		13.4484											BiS2-layerd SC	K				5.38			5.38																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155099	JPS084044712		(Nd,Sm)O0.7F0.3BiS2	Nd0.2Sm0.8Bi1S2F0.3O0.7	Nd	0.2	Sm	0.8	Bi	1	S	2	F	0.3											O	0.7		1	2015																											2	CeOBiS2	P4/nmm		A	3.9818		13.4878											BiS2-layerd SC	K				5.58			5.58																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,Bi2S3,Bi(5N)		mixture - pellet - sealed in quartz tube - heat(700C,10h)					Chemical Pressure Effect on Superconductivity of BiS2-Based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 84(2015)044712	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155100	MAT1312.5818		CaH(Fe,Co)As	Ca1Fe0.98Co0.02As1H1	Ca	1	Fe	0.98	Co	0.02	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8786		8.259											Fe-1111	K					2																																																																																																CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155101	MAT1312.5818		CaH(Fe,Co)As	Ca1Fe0.96Co0.04As1H1	Ca	1	Fe	0.96	Co	0.04	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8791		8.246											Fe-1111	K					2												1.3																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155102	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (6.58 %)	CaH(Fe,Co)As	Ca1Fe0.93Co0.07As1H1	Ca	1	Fe	0.93	Co	0.07	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8803		8.241											Fe-1111	K		23					23										14.7																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155103	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (7.76 %)	CaH(Fe,Co)As	Ca1Fe0.91Co0.09As1H1	Ca	1	Fe	0.91	Co	0.09	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8803		8.253											Fe-1111	K		22.7					22.7										25.8																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155104	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (9.1 %)	CaH(Fe,Co)As	Ca1Fe0.88Co0.12As1H1	Ca	1	Fe	0.88	Co	0.12	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8811		8.2247											Fe-1111	K		23.2					23.2										58.3																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155105	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (14.9 %)	CaH(Fe,Co)As	Ca1Fe0.83Co0.17As1H1	Ca	1	Fe	0.83	Co	0.17	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8816		8.2023											Fe-1111	K		19					19										34.1																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155106	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (18.1 %)	CaH(Fe,Co)As	Ca1Fe0.78Co0.22As1H1	Ca	1	Fe	0.78	Co	0.22	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8824		8.1936											Fe-1111	K		13.3					13.3										54																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155107	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (22.8 %)	CaH(Fe,Co)As	Ca1Fe0.74Co0.26As1H1	Ca	1	Fe	0.74	Co	0.26	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.8825		8.1798											Fe-1111	K		8.95					8.95										32.3																																																																																				CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155108	MAT1312.5818	impurity phase = CaFe1.85Co1.03As1.82 (27.5 %)	CaH(Fe,Co)As	Ca1Fe0.69Co0.31As1H1	Ca	1	Fe	0.69	Co	0.31	As	1	H	1															2013																										ABCD	2	oxypnictide	P4/nmm		A	3.884		8.1619											Fe-1111	K					2																																																																																																CaAs,CaH2,Fe2As,Co2As		mixture with Ca(OH)2 & NaBH4 in BN capsule - heat(1273 K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H-substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuda-cho, Midori-ku, Yokohama 226-8503, Japan	cond-mat/1312.5818	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155109	PRB090020502	PHc2(0) = 150-160 T, NHc2(0) = 38-48 T . Values in DB shows the best fitting values using two-band BCS model.	(K,Na)Fe2Se2	K0.5Na0.24Fe1.52Se2	K	0.5	Na	0.24	Fe	1.52	Se	2																3	2014																										AB2C2	2		I4/mmm		A	3.87		14.16											vacancy-type, Fe-122	K	14.1	20	26				20										72										T	RES(R=0.1Rn), Two band BCS mocel		160	48					T/K	RES(R=0.1Rn)		4.3	1.1			A	from Hc2		26.2	7.5																																																								nominal (K:Na:Fe:Se=0.6:0.2:2:2). as-grown crystals - sealed in Pyrex tube - ANN(400C,3h) - Q in air.					Multiband transport and nonmetallic low-temperature state of K0.50Na0.24Fe1.52Se2			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 90(2014)020502	Hyejin Ryu,F. Wolff-Fabris,J. B. Warren,M. Uhlarz,J. Wosnitza,C. Petrovic		
155120	PRB090024519	thickness d=3000A. Hc2 defined R=zero (Hirr). T<min> in FIg. shows T where R is min in R(T). Nernst effect measured and analysed for Hc2.	(Pr,Ce)CuO4	Pr1.87Ce0.13Cu1O4	Pr	1.87	Ce	0.13	Cu	1															O	4		5	2014																												T'																	PCCO, Pr-214	K	8.8						8.8																				T	RES(R=zero). extraporation			3.4																																																																								epitaxial films with[001]. pulsed laser deposition. substrate = LSAT [(LaAlO3)0.3(Sr2AlTaO6)0.7]					Nernst effect in the electron-doped cuprate superconductor Pr2-xCexCuO4: Superconducting fluctuations, upper critical field Hc2, and the origin of the Tc dome			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 90(2014)024519	F. F. Tafti,F. Laliberte,M. Dion,J. Gaudet,P. Fournier,Louis Taillefer		
155121	PRB090024519	thickness d=3000A. Hc2 defined R=zero (Hirr). T<min> in FIg. shows T where R is min in R(T). Nernst effect measured and analysed for Hc2.	(Pr,Ce)CuO4	Pr1.86Ce0.14Cu1O4	Pr	1.86	Ce	0.14	Cu	1															O	4		5	2014																												T'																	PCCO, Pr-214	K	17.7						17.7																				T	RES(R=zero). extraporation			10.1										MHC155121																																																														epitaxial films with[001]. pulsed laser deposition. substrate = LSAT [(LaAlO3)0.3(Sr2AlTaO6)0.7]					Nernst effect in the electron-doped cuprate superconductor Pr2-xCexCuO4: Superconducting fluctuations, upper critical field Hc2, and the origin of the Tc dome			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 90(2014)024519	F. F. Tafti,F. Laliberte,M. Dion,J. Gaudet,P. Fournier,Louis Taillefer		
155122	PRB090024519	thickness d=3000A. Hc2 defined R=zero (Hirr). T<min> in FIg. shows T where R is min in R(T). Nernst effect measured and analysed for Hc2.	(Pr,Ce)CuO4	Pr1.85Ce0.15Cu1O4	Pr	1.85	Ce	0.15	Cu	1															O	4		5	2014																												T'																	PCCO, Pr-214	K	19.5						19.5	MPH155122																			T	RES(R=zero). extraporation			8.9																																					mW/K.m				MTHC155122																															epitaxial films with[001]. pulsed laser deposition. substrate = LSAT [(LaAlO3)0.3(Sr2AlTaO6)0.7]					Nernst effect in the electron-doped cuprate superconductor Pr2-xCexCuO4: Superconducting fluctuations, upper critical field Hc2, and the origin of the Tc dome			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 90(2014)024519	F. F. Tafti,F. Laliberte,M. Dion,J. Gaudet,P. Fournier,Louis Taillefer		
155123	PRB090024519	thickness d=3000A. Hc2 defined R=zero (Hirr). T<min> in FIg. shows T where R is min in R(T). Nernst effect measured and analysed for Hc2.	(Pr,Ce)CuO4	Pr1.83Ce0.17Cu1O4	Pr	1.83	Ce	0.17	Cu	1															O	4		5	2014																												T'																	PCCO, Pr-214	K	13.4						13.4																				T	RES(R=zero). extraporation			3																																																																								epitaxial films with[001]. pulsed laser deposition. substrate = LSAT [(LaAlO3)0.3(Sr2AlTaO6)0.7]					Nernst effect in the electron-doped cuprate superconductor Pr2-xCexCuO4: Superconducting fluctuations, upper critical field Hc2, and the origin of the Tc dome			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 90(2014)024519	F. F. Tafti,F. Laliberte,M. Dion,J. Gaudet,P. Fournier,Louis Taillefer		
155124	PRB090064518	T<CDW> = 280K by R(T) anomaly, not detected by XRD. Hall number = 0.24 electron/f.u.. Lattice term in SP (beta) = 1.19 mJ/mol.K4.	EuFBiS2	Eu1Bi1S2F1	Eu	1	Bi	1	S	2	F	1																	2014	emu/mol	0.0032			myu-B/mole	7.2																				ABCD2	2	CeBiS2O	P4/nmm	129	A	4.0508		13.5338												K	0.3						0.3																				T	RES(0.9Rn). Extraporation	0.16			0.16			0.018						MHC155124																						mJ/mol.K2	73.3	SP	201	SP																									m3/C	-0.0000000023					MRH155124	n/m3	2100000000000000000000000000	Eu(3N),S(5N),EuF3(3N),Bi2F3(4N5)		mixture - in evacuated quartz tube - heat(1053 K,20h, in muffle furnace) - ground - pellet - SIN(1053 K,20h)					Possible charge-density wave, superconductivity, and f -electron valence instability in EuBiS2F			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 90(2014)064518	Hui-Fei Zhai,Zhang-Tu Tang,Hao Jiang,Kai Xu,Ke Zhang,Pan Zhang,Jin-Ke Bao,Yun-Lei Sun,Wen-He Jiao,I. Nowik,I. Felner,Yu-Ke Li,Xiao-Feng Xu,Qian Tao,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
155125	PRB090094507	High-Tc phase for P > 1.5 GPa. RRR < 2.	La(O,F)BiSe2	La1Bi1Se2F0.5O0.5	La	1	Bi	1	Se	2	F	0.5													O	0.5		3	2014																										ABCD2	2	CeBiS2O	P4/nmm		A			14.05												K			3.43				3.43	MTC155125																			T	RES(0.9Rn)													MHC155125																																																												La2O3,LaF3,Bi2Se3,Se,La		flux method. mixture(CsCl:KCl:(LaO0.5F0.5BiSe2) = 12:8:1) - sealed in quartz tube - heat(800C,50h) - cool to 600C (3C/h)					Pressure-tuned enhancement of superconductivity and change of ground state properties in LaO0.5F0.5BiSe2 single crystals			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, National Center of Microstructures and Quantum Manipulation, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 90(2014)094507	Jianzhong Liu,Sheng Li,Yufeng Li,Xiyu Zhu,Hai-Hu Wen		
155126	PRB090094507	R(T) shows upturn behavior in low T . High -Tc phase for P > 1.95 GPa. RESN minimum at P = 1.95 GPa.	La(O,F)BiSe2	La1Bi1Se2F0.5O0.5	La	1	Bi	1	Se	2	F	0.5													O	0.5		3	2014																										ABCD2																				K			3.57				3.57	MTC155126																																																																																													La2O3,LaF3,Bi2Se3,Se,La		flux method. mixture(CsCl:KCl:(LaO0.5F0.5BiSe2) = 12:8:1) - sealed in quartz tube - heat(800C,50h) - cool to 600C (3C/h)					Pressure-tuned enhancement of superconductivity and change of ground state properties in LaO0.5F0.5BiSe2 single crystals			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, National Center of Microstructures and Quantum Manipulation, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 90(2014)094507	Jianzhong Liu,Sheng Li,Yufeng Li,Xiyu Zhu,Hai-Hu Wen		
155127	PRB090104511	Tn, magnetic exchange interaction J measured by Raman. O-content by iodometric titration	(Ca,La)(Ba,La)Cu3Oz	La1.25Ba1.65Ca0.1Cu3O7.15	La	1.25	Ba	1.65	Ca	0.1	Cu	3													O	z	7.15	3	2014																										AB2C3D7	2	Y123	P4/mmm																	K		57.3					57.3	MPH155127																																																																																															Floating zone method					Relation between cuprate superconductivity and magnetism: A Raman study of (CaLa)1(BaLa)2Cu3Oy			Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science, 77 Cheongam-Ro, Nam-Gu, Pohang 790-784, Korea	Phys.Rev.B, 90(2014)104511	Dirk Wulferding,Meni Shay,Gil Drachuck,Rinat Ofer,Galina Bazalitsky,Zaher Salman,Peter Lemmens,Amit Keren		
155128	PRB090104511	Tn, magnetic exchange interaction J measured by Raman. O-content by iodometric titration	(Ca,La)(Ba,La)Cu3Oz	La1.25Ba1.55Ca0.2Cu3O7.16	La	1.25	Ba	1.55	Ca	0.2	Cu	3													O	z	7.16	3	2014																										AB2C3D7	2	Y123	P4/mmm																	K		68.5					68.5	MPH155128																																																																																															Floating zone method					Relation between cuprate superconductivity and magnetism: A Raman study of (CaLa)1(BaLa)2Cu3Oy			Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science, 77 Cheongam-Ro, Nam-Gu, Pohang 790-784, Korea	Phys.Rev.B, 90(2014)104511	Dirk Wulferding,Meni Shay,Gil Drachuck,Rinat Ofer,Galina Bazalitsky,Zaher Salman,Peter Lemmens,Amit Keren		
155129	PRB090104511	Tn, magnetic exchange interaction J measured by Raman. O-content by iodometric titration	(Ca,La)(Ba,La)Cu3Oz	La1.25Ba1.45Ca0.3Cu3O7.15	La	1.25	Ba	1.45	Ca	0.3	Cu	3													O	z	7.15	3	2014																										AB2C3D7	2	Y123	P4/mmm																	K		75.2					75.2	MPH155129																																																																																															Floating zone method					Relation between cuprate superconductivity and magnetism: A Raman study of (CaLa)1(BaLa)2Cu3Oy			Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science, 77 Cheongam-Ro, Nam-Gu, Pohang 790-784, Korea	Phys.Rev.B, 90(2014)104511	Dirk Wulferding,Meni Shay,Gil Drachuck,Rinat Ofer,Galina Bazalitsky,Zaher Salman,Peter Lemmens,Amit Keren		
155130	PRB090104511	Tn, magnetic exchange interaction J measured by Raman. O-content by iodometric titration	(Ca,La)(Ba,La)Cu3Oz	La1.25Ba1.35Ca0.4Cu3O7.16	La	1.25	Ba	1.35	Ca	0.4	Cu	3													O	z	7.16	3	2014																										AB2C3D7	2	Y123	P4/mmm																	K		79.8					79.8	MPH155130																																																																																															Floating zone method					Relation between cuprate superconductivity and magnetism: A Raman study of (CaLa)1(BaLa)2Cu3Oy			Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science, 77 Cheongam-Ro, Nam-Gu, Pohang 790-784, Korea	Phys.Rev.B, 90(2014)104511	Dirk Wulferding,Meni Shay,Gil Drachuck,Rinat Ofer,Galina Bazalitsky,Zaher Salman,Peter Lemmens,Amit Keren		
155131	PRB090104514	Absolute value of [penet] estimated from d-[penet] usind tunnel diode method assuming [penet] (optimal sample) = 200 nm. T<STR> = 103 K by R(T) anomaly	(Ba,K)Fe2As2	Ba0.81K0.19Fe2As2	Ba	0.81	K	0.19	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K	14						14																																									nm	tunnel diode resonator	356																																																					High-T FeAs flux method. Compositions measured by WDS.					Effects of electron irradiation on resistivity and London penetration depth of Ba1-xKxFe2As2 (x =< 0.34) iron-pnictide superconductor			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 90(2014)104514	K. Cho,M. Konczykowski,J. Murphy,H. Kim,M. A. Tanatar,W. E. Straszheim,B. Shen,H. H. Wen,R. Prozorov		
155132	PRB090104514	electron (2.5MeV) irradiation to nominal single crystal. dose = 1.12E+19 el/cm2. T<STR> = 97.9 K by R(T)	(Ba,K)Fe2As2	Ba0.81K0.19Fe2As2	Ba	0.81	K	0.19	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	k	9.2						9.2																																									nm	tunnel diode resonator	427																																																					High-T FeAs flux method. Compositions measured by WDS.					Effects of electron irradiation on resistivity and London penetration depth of Ba1-xKxFe2As2 (x =< 0.34) iron-pnictide superconductor			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 90(2014)104514	K. Cho,M. Konczykowski,J. Murphy,H. Kim,M. A. Tanatar,W. E. Straszheim,B. Shen,H. H. Wen,R. Prozorov		
155133	PRB090104514	[penet] = 226, 237, 242 nm for dose = 0, 9.36, 16.2 E+18 e/cm2 samples, respectively.	(Ba,K)Fe2As2	Ba0.74K0.26Fe2As2	Ba	0.74	K	0.26	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K	32						32																																									nm	tunnel diode resonator	226																																																					High-T FeAs flux method. Compositions measured by WDS.					Effects of electron irradiation on resistivity and London penetration depth of Ba1-xKxFe2As2 (x =< 0.34) iron-pnictide superconductor			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 90(2014)104514	K. Cho,M. Konczykowski,J. Murphy,H. Kim,M. A. Tanatar,W. E. Straszheim,B. Shen,H. H. Wen,R. Prozorov		
155134	PRB090104514	[penet] = 205, 238 nm for dose = 0, 5.18 E+19 e/cm2, respectively.	(Ba,K)Fe2As2	Ba0.68K0.32Fe2As2	Ba	0.68	K	0.32	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K	37						37																																									nm	tunnel diode resonator	205																																																					High-T FeAs flux method. Compositions measured by WDS.					Effects of electron irradiation on resistivity and London penetration depth of Ba1-xKxFe2As2 (x =< 0.34) iron-pnictide superconductor			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 90(2014)104514	K. Cho,M. Konczykowski,J. Murphy,H. Kim,M. A. Tanatar,W. E. Straszheim,B. Shen,H. H. Wen,R. Prozorov		
155135	PRB090104514	[penet] = 200, 212 nm for dose = 0, 1.25 E+19 e/cm2, respectively.	(Ba,K)Fe2As2	Ba0.64K0.34Fe2As2	Ba	0.64	K	0.34	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K	39						39																																									nm	tunnel diode resonator	200																																																					High-T FeAs flux method. Compositions measured by WDS.					Effects of electron irradiation on resistivity and London penetration depth of Ba1-xKxFe2As2 (x =< 0.34) iron-pnictide superconductor			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 90(2014)104514	K. Cho,M. Konczykowski,J. Murphy,H. Kim,M. A. Tanatar,W. E. Straszheim,B. Shen,H. H. Wen,R. Prozorov		
155136	PRB090125126	Hydrostatic pressure. SC induced for P > 7GPa, where structure is monoclinic. Tc(max) =  K at P= 8 GPa.	Bi2Te3	Bi2Te3	Bi	2	Te	3																				3	2014																										A2B3																			rhombohedral	K					0			MTC155136																																																																																				m3/C	0.00000041					MRH155136					flux method					Superconductivity in the topological insulator Bi2Te3 under hydrostatic pressure			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 90(2014)125126	K. Matsubayashi,T. Terai,J. S. Zhou,Y. Uwatoko		
155137	PRB090144508	Intergrowth(BaFe2As2 + BaTi2As2O).Optical reflectance measured. Density wave(SDW or CDW) at 125 K. [penet] estimated from plasma freqency. Two gaps(3.4 and 7.9 meV)	Ba2Ti2Fe2As4O	Ba2Ti2Fe2As4O1	Ba	2	Ti	2	Fe	2	As	4													O	1		3	2014																																														K		21.5					21.5																																									A	Optical reflectance	2900			meV	7.9	8.7	15																																															Ba2As3 flux method					Coexistence of superconductivity and density wave in Ba2Ti2Fe2As4O: An optical spectroscopy study			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 90(2014)144508	H. P. Wang,Y. L. Sun,X. B. Wang,Y. Huang,T. Dong,R. Y. Chen,G. H. Cao,N. L. Wang		
155138	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.501 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se1H1O1	Li	0.8	Fe	1.2	Se	1	H	1													O	1		1	2014								8.67																			2		P4/nmm	129	A	3.7924		9.2824											FeSe-derived SC	K				40.9			40.9																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155139	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.92S0.08H1O1	Li	0.8	Fe	1.2	Se	0.92	S	0.08	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.789		9.2559											FeSe-derived SC	K																																																																																																							hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155140	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.456 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.84S0.16H1O1	Li	0.8	Fe	1.2	Se	0.84	S	0.16	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7752		9.2467											FeSe-derived SC	K				38.6			38.6										69																																																																																						hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155141	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.438 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.78S0.22H1O1	Li	0.8	Fe	1.2	Se	0.78	S	0.22	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7672		9.221											FeSe-derived SC	K				35.6			35.6	MPH155140																																																																																															hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155142	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.431 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.72S0.28H1O1	Li	0.8	Fe	1.2	Se	0.72	S	0.28	H	1											O	1		1	2014								8.45																			2		P4/nmm	129	A	3.7618		9.1972											FeSe-derived SC	K				35			35																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155143	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.411 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.59S0.41H1O1	Li	0.8	Fe	1.2	Se	0.59	S	0.41	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7538		9.1656											FeSe-derived SC	K				32			32																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155144	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.397 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.47S0.53H1O1	Li	0.8	Fe	1.2	Se	0.47	S	0.53	H	1											O	1		1	2014								8.48																			2		P4/nmm	129	A	3.7455		9.1351											FeSe-derived SC	K				24.2			24.2	MPH155140																																																																																															hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155145	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.370 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.34S0.66H1O1	Li	0.8	Fe	1.2	Se	0.34	S	0.66	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7325		9.0979											FeSe-derived SC	K				18.4			18.4																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155146	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.23S0.77H1O1	Li	0.8	Fe	1.2	Se	0.23	S	0.77	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7197		9.0339											FeSe-derived SC	K				11			11																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155147	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.288 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2Se0.1S0.9H1O1	Li	0.8	Fe	1.2	Se	0.1	S	0.9	H	1											O	1		1	2014																											2		P4/nmm	129	A	3.7124		8.9678											FeSe-derived SC	K				0	0		0																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155148	PRB090214520	AFM order from (Li0.8Fe0.2)OH layers. Tn measured by SP-heat. Anion hight from Fe(2)  layers = 1.263 A.	(Li,Fe)OH(Se,S)	Li0.8Fe1.2S0.41H1O1	Li	0.8	Fe	1.2	S	0.41	H	1													O	1		1	2014								8.51																			2		P4/nmm	129	A	3.7067		8.9104											FeSe-derived SC	K				0	0		0																																																																																																hydrothermal reaction method. stoichiometric mixture in 10mL water - mixed with Fe powder & LiOH/H2O - sealed in Teflon autoclave - heat(150-160C,3-10 days)					Superconductivity and phase diagram of (Li0.8Fe0.2)OHFeSe1-xSx			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 90(2014)214520	X. F. Lu,N. Z. Wang,X. G. Luo,G. H. Zhang,X. L. Gong,F. Q. Huang,X. H. Chen		
155149	PRB090220510	Tc increases with P. High-Tc and low-Tc phases exist. For P>1.1 GPa, H-Tc phase appears. At P=2.26 GPa, H-Tc phase only.	Eu3Bi2S4F4	Eu3Bi2S4F4	Eu	3	Bi	2	S	4	F	4																1	2014																										A2B3C4D4	2		I4/mmm	139															Eu3F4-layer + BiS2-bilayer	K			1.43	1.45			1.45	MPH155149																			T	RES(on)													MHC155149																																					mOhm.cm	2.41			2.16							2.27														solid state reaction. See J.Am.Chem.Soc. 136(2014)15386					Pressure-enhanced superconductivity in Eu3Bi2S4F4			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 90(2014)220510	Yongkang Luo,Hui-Fei Zhai,Pan Zhang,Zhu-An Xu,Guang-Han Cao,J. D. Thompson		
155150	PRB090224410	FM ordering along c-axis below Tm=7 K.. Tm = 6.54 K from neutron diffraction. Lattice const. at 20 K. SC & FM coexist below Tc.	Ce(O,F)BiS2	Ce1Bi1S2F0.7O0.3	Ce	1	Bi	1	S	2	F	0.7													O	0.3		1	2014					myu-B/Ce	0.52	7																			ABCD2	2		P4/nmm		A	4.039		13.566											BiS2-layer-SC	K	4.5						4.5																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		mixture - pellet - sealed in quartz tube - heat(800C,10h) - reground - ANN(600C,1h, under P=3 GPa)					Coexistence of ferromagnetism and superconductivity in CeO0.3F0.7BiS2			Department of Physics, University of Virginia, Charlottesville, Virginia 22904, USA	Phys.Rev.B, 90(2014)224410	J. Lee,S. Demura,M. B. Stone,K. Iida,G. Ehlers,C. R. dela Cruz,M. Matsuda,K. Deguchi,Y. Takano,Y. Mizuguchi,O. Miura,D. Louca,S.-H. Lee		
155151	PRB091014508	Impurity phase: Bi2S3(6%). Ce-moment order FM below Tm = 7.5 K. Pauli limit = 1.84Tc = 5T. SP data analyzed for 10 < T < 15 K.	(Sr,Ce)FBiS2	Sr0.5Ce0.5Bi1S2F1	Sr	0.5	Ce	0.5	Bi	1	S	2	F	1														1	2015			emu.K/Ce	0.8	myu-B/Ce	2.53	-19.2																			ABCD2	2		P4/nmm		A	4.0695		13.3491											BiS2-layer-SC	K			2.8				2.8																				T	RES(0.9Rn), GL theory	1.16												MHC155151																						mJ/mol.K2	58.6	SP	220	SP																																		Ce2S3,SrF2,CeF3,Bi2S3,S		mixture - pellet - sealed in quartz tube - heat(1073K,24h) - Q to RT - ANN(973K,10h)					Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 91(2015)014508	Lin Li,Yuke Li,Yuefeng Jin,Haoran Huang,Bin Chen,Xiaofeng Xu,Jianhui Dai,Li Zhang,Xiaojun Yang,Huifei Zhai,Guanghan Cao,Zhuan Xu		
155152	PRB091014513	RRR=4.04.SP (beta=2.32 mJ/mol.K4, delta=0.11 mJ/mol.K6). (dC/Tc) = 11.8 where Tc= 1.66K(SP-mid), then (dC/gamma*Tc) = 1.37.	BaPt2Sb2	Ba1Pt2Sb2	Ba	1	Pt	2	Sb	2																		1	2015																										AB2C2	4	CaBa2Ge2	C2/m	12	A	6.7015	6.7524	10.4744											monoclinic, beta=91.227. Fe-122	K	1.82		1.85				1.835										100										T	RES(on), extraporation	0.27												MHC155152		A	from Hc2	350																		mJ/mol.K2	8.6	SP	146	SP																																		Ba(3N),Pt(3N5),Sb(5N)		nominal (Ba:Pt:Sb = 1.05:2:2),  arc-mwlting. Sample compositions: (Ba:Pt:Sb = 20.2:40.6:39.3) by EPMA					Superconductivity in 122-type antimonide BaPt2Sb2			Superconducting Properties Unit, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 91(2015)014513	Motoharu Imai,Soshi Ibuka,Naoki Kikugawa,Taichi Terashima,Shinya Uji,Takeshi Yajima,Hiroshi Kageyama,Izumi Hase		
155153	PRB091020506	Hp = 9.0 T. Hc2(0) = 32 T using WHH theory.  (dC/gamma*Tc) = 1.8. Lattice term in SP: beta = 2.9 mJ/mol.K4.	Rb2Cr3As3	Rb2Cr3As3	Rb	2	Cr	3	As	3																		1	2015																										A2B3C3	7	K2Cr3As3	P6[-]m2	187	A	10.281		4.2421											Hexagonal	K			4.8	4.8		0.44	4.8										91										T	RES(0.9Rn), GL theory	20							T/K	RES(0.9Rn)	5.08			MHC155153																			MSP155153			mJ/mol.K2	55.1	SP	175	SP																																		Rb,Cr,As		nominal(3% excess-Rb). mixture - sealed in quartz ampoule - heat(523K, 15h) - grind - pellet - in alumina tube - sealed in Ta tube - SIN(973K, 24h)					Unconventional superconductivity in quasi-one-dimensional Rb2Cr3As3			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 91(2015)020506	Zhang-Tu Tang,Jin-Ke Bao,Yi Liu,Yun-Lei Sun,Abduweli Ablimit,Hui-Fei Zhai,Hao Jiang,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
155154	MAT1412.0067	Hp = 11 T. Hc2(0) = 32 T using WHH theory.. (dC/gamma*Tc) = 2.4. Lattice term in SP: beta = 1.51 mJ/mol.K4. R=R0 + A*T, where R0=0.195 mOhm.cm, A=0.0067 mOhm.cm/K	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		1	2014																										A2B3C3	7	K2Cr3As3	P6[-]m2	187	A	9.9832		4.2304											Hexagonal	K			6.1			0.24	6.1										100										T	RES(0.9Rn), Linear approx.	44.7							T/K	RES(0.9Rn)	7.43			MHC155154																			MSP155154			mJ/mol.K2	75	SP	218	SP											mOhm.cm							0.195																		solid state reaction. After initial reaction, mixture - ground - pellet - SIN(973K + 1173K, 24h)					Superconductivity in quasi-one-dimensional K2Cr3As3 with significant electron correlations			Department of Physics, Zhejiang University, Hangzhou 310027, China	cond-mat/1412.0067	Jin-Ke Bao,Ji-Yong Liu,Cong-Wei Ma,Zhi-Hao Meng,Zhang-Tu Tang,Yun-Lei Sun,Hui-Fei Zhai,Hao Jiang,Hua Bai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
155155	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Rh1C2	U	2	Rh	1	C	2																		1	2015	emu/g	0.0000037	emu/g.K	0.00028	myu-B/U	2.8	44	22.5																		AB2C2		Na2HgO2			A	3.4662		12.5206												K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155156	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Pt0.1Rh0.9C2	U	2	Pt	0.1	Rh	0.9	C	2																1	2015								23																		AB2C2		Na2HgO2																		K					0.38			MPH155155																																																																																															arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155157	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Pt0.2Rh0.8C2	U	2	Pt	0.2	Rh	0.8	C	2																1	2015								21.1																		AB2C2		Na2HgO2																		K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155158	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Pt0.3Rh0.7C2	U	2	Pt	0.3	Rh	0.7	C	2																1	2015								18.4																		AB2C2		Na2HgO2																		K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155159	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Pt0.4Rh0.6C2	U	2	Pt	0.4	Rh	0.6	C	2																1	2015								15.1																		AB2C2		Na2HgO2			A	3.4868		12.552												K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155160	PRB091024408	SP-heat measured down to 2 K	U2(Pt,Rh)C2	U2Pt0.5Rh0.5C2	U	2	Pt	0.5	Rh	0.5	C	2																1	2015								9.96																		AB2C2		Na2HgO2																		K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155161	PRB091024408		U2(Pt,Rh)C2	U2Pt0.6Rh0.4C2	U	2	Pt	0.6	Rh	0.4	C	2																1	2015								4.33																		AB2C2		Na2HgO2			A	3.5036		12.5697												K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155162	PRB091024408	Tn < 0.38 K. SP-heat measured down to 0.38 K	U2(Pt,Rh)C2	U2Pt0.7Rh0.3C2	U	2	Pt	0.7	Rh	0.3	C	2																1	2015																										AB2C2		Na2HgO2			A	3.5086		12.5684												K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155163	PRB091024408	SP-heat measured down to 0.38 K	U2(Pt,Rh)C2	U2Pt0.8Rh0.2C2	U	2	Pt	0.8	Rh	0.2	C	2																1	2015																										AB2C2		Na2HgO2			A	3.5175		12.5766												K					0.38																																																																																																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155164	PRB091024408	SP-heat measured down to 0.38 K	U2(Pt,Rh)C2	U2Pt0.9Rh0.1C2	U	2	Pt	0.9	Rh	0.1	C	2																1	2015																										AB2C2		Na2HgO2			A	3.5247		12.5763												K		1.09					1.09																																																																							uOhm.cm							42																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155165	PRB091024408	SP-heat measured down to 0.38 K	U2(Pt,Rh)C2	U2Pt0.95Rh0.05C2	U	2	Pt	0.95	Rh	0.05	C	2																1	2015																										AB2C2		Na2HgO2			A	3.5243		12.5687												K		1.41					1.41	MPH155155																																																																																															arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155166	PRB091024408	spin triplet SC. SP-heat measured down to 0.38 K	U2(Pt,Rh)C2	U2Pt1C2	U	2	Pt	1	C	2																		1	2015																										AB2C2		Na2HgO2			A	3.5288		12.5729												K		1.45					1.45																																																																							uOhm.cm							5																		arc-melting(U:Pt:Rh:C = 2:1.1x:1.1(1-x):2.2) - wrapped in Ta foil - sealed in quartz tube - ANN(1050C, 2 month)					Magnetism and superconductivity in U2PtxRh1-xC2			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)024408	N. Wakeham,Ni Ni,E. D. Bauer,J. D. Thompson,E. Tegtmeier,F. Ronning		
155167	PRB091024509	Tc=3.53 K(SP). Thermal expansion (alpha) = 1.40 E-5 /K for 300 < T <700 K. SP-fitting for 2 < T < 5 K.  (dC/gamma*Tc) = 1.59. e-ph = 0.657	HfPd2Al	Pd2Hf1Al1	Pd	2	Hf	1	Al	1																		1	2015																		GPa		97						ABC2		Heusler			A	6.367														K		3.55					3.55	MTC155167		K/GPa	-0.13																																																	MSP155167			mJ/mol.K2	7.6	SP	177	SP																																		Hf(2N5),Pd(3N5),Al(3N)		arc-melting. as-grown(not ANN) sample					Pressure effects on the superconductivity of the HfPd2Al Heusler compound: Experimental and theoretical study			AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, Aleja Mickiewicza 30, 30-059 Krakow, Poland	Phys.Rev.B, 91(2015)024509	B. Wiendlocha,M. J. Winiarski,M. Muras,C. Zvoriste-Walters,J.-C. Griveau,S. Heathman,M. Gazda,T. Klimczuk		
155168	PRB091045108	Antiferrodistortive phase transition at 104  K by SP. Hall mobility = 9000 cm3/V.sec. mean free path = 1380 A.	SrTiO3-d	Sr1Ti1O3-d	Sr	1	Ti	1																	O	3-d		3	2015																										ABC3		ABO3																		K		0.085					0.085	MTC155168																																			A	from (dhc2/dT)	990																																																						n/cm3	520000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155169	PRB091045108	Antiferrodistortive phase transition at 104  K by SP. Hall mobility = 10000 cm3/V.sec. mean free path = 1860 A.	SrTiO3-d	Sr1Ti1O3-d	Sr	1	Ti	1																	O	3-d		3	2015																										ABC3		ABO3																		K		0.175					0.175																																				A	from (dhc2/dT)	790																																																						n/cm3	1080000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155170	PRB091045108	Antiferrodistortive phase transition at 104  K by SP. Hall mobility = 8000 cm3/V.sec. mean free path = 1800 A.	SrTiO3-d	Sr1Ti1O3-d	Sr	1	Ti	1																	O	3-d		3	2015																										ABC3		ABO3																		K		0.201					0.201																																				A	from (dhc2/dT)	580																																																						n/cm3	2200000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155171	PRB091045108	Antiferrodistortive phase transition at 110  K by SP. Hall mobility = 6100 cm3/V.sec. mean free path = 1080 A.	(Sr,Ca)TiO3-d	Sr0.9978Ca0.0022Ti1O3-d	Sr	0.9978	Ca	0.0022	Ti	1															O	3-d		3	2015																										ABC3		ABO3																		K		0.067					0.067																																				A	from (dhc2/dT)	3740																																																						n/cm3	520000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155172	PRB091045108	Antiferrodistortive phase transition at 104  K by SP. Hall mobility = 3900 cm3/V.sec. mean free path = 810 A.	(Sr,Ca)TiO3-d	Sr0.9978Ca0.0022Ti1O3-d	Sr	0.9978	Ca	0.0022	Ti	1															O	3-d		3	2015																										ABC3		ABO3																		K		0.132					0.132	MTC155171																																			A	from (dhc2/dT)	1080																																																						n/cm3	1080000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155173	PRB091045108	Antiferrodistortive phase transition at 104  K by SP. Hall mobility = 3000 cm3/V.sec. mean free path = 800 A.	(Sr,Ca)TiO3-d	Sr0.9978Ca0.0022Ti1O3-d	Sr	0.9978	Ca	0.0022	Ti	1															O	3-d		3	2015																										ABC3		ABO3																		K		0.182					0.182																																				A	from (dhc2/dT)	840																																																						n/cm3	2200000000000000000			Commercial SrTiO3:Ca single crystals. O-deficient samples obtained by ANN (700 - 1000 C, 2h, in vac)					Interplay between antiferrodistortive, ferroelectric, and superconducting instabilities in Sr1-x Cax TiO3-z			Universidade de Sao Paulo, Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 91(2015)045108	B. S. de Lima,M. S. da Luz,F. S. Oliveira,L. M. S. Alves,C. A. M. dos Santos,F. Jomard,Y. Sidis,P. Bourges,S. Harms,C. P. Grams,J. Hemberger,X. Lin,B. Fauque,K. Behnia		
155175	PRB091060510	Coexistence of two CDW and SC. <75>As-NMR/NQR and <195>Pt-NMR measured. T<CDW> = 410 K and 255 K for As-Pt-As layer and Pt-As-Pt layer, respectively. Gap from NMR	SrPt2As2	Sr1Pt2As2	Sr	1	Pt	2	As	2																		1	2015																										AB2C2		CaBe2Ge2																	Fe-122	K		5.2					5.2																																																3.1	6																																															solid state reaction					Coexistence of multiple charge-density waves and superconductivity in SrPt2As2 revealed by <75>As-NMR/NQR and <195>Pt-NMR			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)060510	Shinji Kawasaki,Yoshihiko Tani,Tomosuke Mabuchi,Kazutaka Kudo,Yoshihiro Nishikubo,Daisuke Mitsuoka,Minoru Nohara,Guo-qing Zheng		
155176	NATCOM0030943		GdFeAs(O,H)	Gd1Fe1As1H0.1O0.9	Gd	1	Fe	1	As	1	H	0.1													O	0.9		1	2012																										ABCD		oxypnictide																	Fe-1111	K			56.2				56.2	MTC155176																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
155177	NATCOM0030943		SmFeAs(O,H)	Sm1Fe1As1H0.25O0.75	Sm	1	Fe	1	As	1	H	0.25													O	0.75		1	2012																										ABCD		oxypnictide																	Fe-1111	K			55				55	MTC155177																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
155178	NATCOM0030943		CeFeAs(O,H)	Ce1Fe1As1H0.21O0.79	Ce	1	Fe	1	As	1	H	0.21													O	0.79		1	2012																										ABCD		oxypnictide																	Fe-1111	K			48				48	MTC155178																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
155179	NATCOM0030943		LaFeAs(O,H)	La1Fe1As1H0.36O0.64	La	1	Fe	1	As	1	H	0.36													O	0.64		1	2012																										ABCD		oxypnictide																	Fe-1111	K			36				36	MTC155179																																																																																																				Two-dome structure in electron-doped iron arsenide superconductors			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Nature Commun., 3(2012)943	Soshi Iimura,Satoru Matsuishi,Hikaru Sato,Taku Hanna,Yoshinori Muraba,Sung Wng Kim,Jung Eun Kim,Masaki Takata,Hideo Hosono		
155180	PRB091064509	SC and AF are segregated in electronic phase diagram. T<STR> = 156 K. Pseudogap Temp (defined as deviation from Curie-Weis law) = 69.6 K. H-content by TDS (not nominal)	LaFeAs(O,H)	La1Fe1As1H0.44O0.56	La	1	Fe	1	As	1	H	0.44													O	0.56			2015																										ABCD		oxypnictide																	Fe-1111	K		21					21																																																																																																					Quantum critical behavior in heavily doped LaFeAsO1-xHx pnictide superconductors analyzed using nuclear magnetic resonance			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 91(2015)064509	R. Sakurai,N. Fujiwara,N. Kawaguchi,Y. Yamakawa,H. Kontani,S. Iimura,S. Matsuishi,H. Hosono		
155181	PRB091064509	Pseudogap Temp (defined as deviation from Curie-Weis law) = 81 K. H-content by TDS (not nominal)	LaFeAs(O,H)	La1Fe1As1H0.49O0.51	La	1	Fe	1	As	1	H	0.49													O	0.51			2015								60																		ABCD		oxypnictide																	Fe-1111	K					4																																																																																																							Quantum critical behavior in heavily doped LaFeAsO1-xHx pnictide superconductors analyzed using nuclear magnetic resonance			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 91(2015)064509	R. Sakurai,N. Fujiwara,N. Kawaguchi,Y. Yamakawa,H. Kontani,S. Iimura,S. Matsuishi,H. Hosono		
155182	PRB091064509	Pseudogap Temp (defined as deviation from Curie-Weis law) = 90 K. H-content by TDS (not nominal)	LaFeAs(O,H)	La1Fe1As1H0.51O0.49	La	1	Fe	1	As	1	H	0.51													O	0.49			2015								70																		ABCD		oxypnictide																	Fe-1111	K					4																																																																																																							Quantum critical behavior in heavily doped LaFeAsO1-xHx pnictide superconductors analyzed using nuclear magnetic resonance			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 91(2015)064509	R. Sakurai,N. Fujiwara,N. Kawaguchi,Y. Yamakawa,H. Kontani,S. Iimura,S. Matsuishi,H. Hosono		
155183	PRB091064509	H-content by TDS (not nominal)	LaFeAs(O,H)	La1Fe1As1H0.6O0.4	La	1	Fe	1	As	1	H	0.6													O	0.4			2015								110																		ABCD		oxypnictide																	Fe-1111	K					4																																																																																																							Quantum critical behavior in heavily doped LaFeAsO1-xHx pnictide superconductors analyzed using nuclear magnetic resonance			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 91(2015)064509	R. Sakurai,N. Fujiwara,N. Kawaguchi,Y. Yamakawa,H. Kontani,S. Iimura,S. Matsuishi,H. Hosono		
155184	PRB091064509	H-content by TDS (not nominal)	LaFeAs(O,H)	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2015								138																		ABCD		oxypnictide																	Fe-1111	K					4																																																																																																							Quantum critical behavior in heavily doped LaFeAsO1-xHx pnictide superconductors analyzed using nuclear magnetic resonance			Graduate School of Human and Environmental Studies, Kyoto University, Yoshida-Nihonmatsu-cyo, Sakyo-ku, Kyoto 606-8501, Japan	Phys.Rev.B, 91(2015)064509	R. Sakurai,N. Fujiwara,N. Kawaguchi,Y. Yamakawa,H. Kontani,S. Iimura,S. Matsuishi,H. Hosono		
155186	PRB091064510	ANN(800 C). Schottky anomaly below 3.7 K in SP. SP-FIG shows C<el> obtainedby extracted C<ph> and C<Sch> from C. (dC/gamma*Tc) = 0.21	(La,Sm)(O,F)BiS2	La0.9Sm0.1Bi1S2F0.5O0.5	La	0.9	Sm	0.1	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0563		13.333											BiS2-layer SC	K		2.93		2.76			2.93																																																					MSP155186			mJ/mol.K2	9	SP																																						solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155187	PRB091064510	ANN(800 C).	(La,Sm)(O,F)BiS2	La0.7Sm0.3Bi1S2F0.5O0.5	La	0.7	Sm	0.3	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0317		13.3686											BiS2-layer SC	K		3.11		2.87			3.11																																																																																																solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155188	PRB091064510	ANN(800 C)	(La,Sm)(O,F)BiS2	La0.6Sm0.4Bi1S2F0.5O0.5	La	0.6	Sm	0.4	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0266		13.3804											BiS2-layer SC	K		3.26		3			3.26	MTC155188																																																																																															solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155189	PRB091064510	ANN(750C)	(La,Sm)(O,F)BiS2	La0.5Sm0.5Bi1S2F0.5O0.5	La	0.5	Sm	0.5	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0155		13.407											BiS2-layer SC	K		4.05		3.86			4.05																																																																																																solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155190	PRB091064510	ANN(750C)	(La,Sm)(O,F)BiS2	La0.4Sm0.6Bi1S2F0.5O0.5	La	0.4	Sm	0.6	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.0077		13.4096											BiS2-layer SC	K		4.21		4.95			4.21	MTC155188																																																																																															solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155191	PRB091064510	ANN(750C)	(La,Sm)(O,F)BiS2	La0.3Sm0.7Bi1S2F0.5O0.5	La	0.3	Sm	0.7	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	4.3996		13.4129											BiS2-layer SC	K		5.14		5.22			5.14																																																																																																solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155192	PRB091064510	ANN(710C). Schottky anomaly below 3.7 K in SP. SP-FIG shows C<el> obtainedby extracted C<ph> and C<Sch> from C. (dC/gamma*Tc) = 3.6	(La,Sm)(O,F)BiS2	La0.2Sm0.8Bi1S2F0.5O0.5	La	0.2	Sm	0.8	Bi	1	S	2	F	0.5											O	0.5		1	2015																											2	CeOBiS2	P4/nmm		A	3.9831		13.434											BiS2-layer SC	K		5.42		5.17			5.42																																																					MSP155192			mJ/mol.K2	18	SP																																						solid state reaction					Enhancement of superconductivity in La1-xSmxO0.5F0.5BiS2			Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 91(2015)064510	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155193	PRB091094427	Magnetic order: long range FM , Tm = 19 K by muon-SR. Volume fractin = 100 % for FM and SC. Coexistence of FM and SC.	Eu(Fe,Ir)2As2	Eu1Fe1.72Ir0.28As2	Eu	1	Fe	1.72	Ir	0.28	As	2																1	2015																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.9365		12.027											Fe-122. ND results, a=(3.9326, 3.9287), c=(11.897, 11.884) at T=25 and 1.8 K, respectively	K		21.5					21.5										100																																																																																				Eu(3N),Fe(5N),Ir(4N),As(5N)		solid state reaction. Eu mixed with (Fe,Ir,As-powder) - pellet - heat(900C,30h, in evacuated quartz tube) -reground - pellet -SIN(900C,5d, in quartz tube)					muon-SR and neutron diffraction investigations on the reentrant ferromagnetic superconductor Eu(Fe0.86Ir0.14)2As2			Helmholtz-Zentrum Berlin fur Materialien und Energie, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 91(2015)094427	V. K. Anand,D. T. Adroja,A. Bhattacharyya,U. B. Paramanik,P. Manuel,A. D. Hillier,D. Khalyavin,Z. Hossain		
155194	PRB091094515	P-induced SC. magnetic order (Tm1 and Tm2). R(T) peak at T*-1,T*-2. RR=1.8 uOhm.cm (P=0). Tc(in DB) for P=21.2 GPa.	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K			2.55				2.55	MPH155194																																																																																															Sn-flux method					Effect of disorder on the pressure-induced superconducting state of CeAu2Si2			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 91(2015)094515	Z. Ren,G. Giriat,G. W. Scheerer,G. Lapertot,D. Jaccard		
155195	PRB091094515	P-induced SC. magnetic order (Tm1 and Tm2). R(T) peak at T*-1,T*-2. RR=12.2  (P=0), =43.0 uOhm.cm (P=21.2 GPa). Tc(in DB) for P=21.2 GPa.	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K			1.15				1.15	MPH155195																																																																																															Au-Si self flux method					Effect of disorder on the pressure-induced superconducting state of CeAu2Si2			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 91(2015)094515	Z. Ren,G. Giriat,G. W. Scheerer,G. Lapertot,D. Jaccard		
155196	PRB091100504	[penet] & [gap] measured by muon-SR. nodeless SC. GL parameter = 183.	Nb2PdS5	Nb2Pd1S5	Nb	2	Pd	1	S	5																		1	2015																										AB2C5	4		C2/m																monoclinic	K	6.05			6			6											Oe	estimated from penet and cohere	14							T	#154324, GL fitting	17.6														A	from Hc2	43			A	muon-SR, fitting parameter	7850			meV	1.07	4.04	16																																															solid state reaction					Nodeless superconductivity in quasi-one-dimensional Nb2PdS5: A muon-SR study			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 91(2015)100504	P. K. Biswas,H. Luetkens,Xiaofeng Xu,J. H. Yang,C. Baines,A. Amato,E. Morenzoni		
155197	PRB091104506	STM measured on the cleaved surface (1[-]03) plane. Hc2 along C' axis. CDW-like modulation observed along the stripe. Gap from STM using BCS fitting.	Ta4Pd3Te16	Ta4Pd3Te16	Ta	4	Pd	3	Te	16																		3	2015																										A3B4C16																				K		4.3					4.3																				T		2.9														A	from Hc2	110								meV	0.66	3.56	11																																															self-flux method					Scanning tunneling microscopy study of superconductivity, magnetic vortices, and possible charge-density wave in Ta4Pd3Te16			State Key Laboratory of Surface Physics, Department of Physics, and Advanced Materials Laboratory, Fudan University, Shanghai 200433, China	Phys.Rev.B, 91(2015)104506	Q. Fan,W. H. Zhang,X. Liu,Y. J. Yan,M. Q. Ren,M. Xia,H. Y. Chen,D. F. Xu,Z. R. Ye,W. H. Jiao,G. H. Cao,B. P. Xie,T. Zhang,D. L. Feng		
155198	PRB091104511	Impurity: Bi2OS2,Bi2O3,Bi (total < 8%). Thermopower S(T) shows semimetallic behaviour. Tc(SUS) = 3.3 K for P = 0.6 GPa.	Bi3O2S3	Bi3S3O2	Bi	3	S	3																	O	2		1	2015																										A2B3C3					A	3.9645		41.3165												K	4.03		5.75	4.1			4.1																																																													W/m.K	3.07			MTHC155198	uV/K	-29.2			MTP155198																								Bi2O3,S		mixture - pellet - sealed in silica tube - heat(430C,4h) - Q to ice water - reground -pellet - sealed in quartz tube - heat(430C,14h) - reground - heat (520C,17h) - Q					Superconductivity in semimetallic Bi3O2S3			Materials Science & Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 91(2015)104511	L. Li,D. Parker,P. Babkevich,L. Yang,H. M. Ronnow,A. S. Sefat		
155199	MAT1404.0371	sample #1. R=R0+A*T^n (R0=3.96 uOhm.cm, n=2.26). Hc2//C*-axis. There exist nodes in SC-gaps from thermal conductivity.	Ta4Pd3Te16	Ta4Pd3Te16	Ta	4	Pd	3	Te	16																		3	2014																										A3B4C16																				K	4.3			4.3			4.3																				T	RES(zero), extrapolation	2.9												MHC155199																																																														self flux method					Nodal superconductivity and superconducting dome in new layered superconductor Ta4Pd3Te16			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, China	cond-mat/1404.0371	J. Pan,W. H. Jiao,X. C. Hong,Z. Zhang,L. P. He,P. L. Cai,J. Zhang,G. H. Cao,S. Y. Li1		
155200	MAT1404.0371	sample #6. Hc2(0) and -(dHc2/dT) = (7.9, 4.8, 3.2) in T and (1.16, 0.85, 0.53) inT/K for H//b, H//a', and H//c*, respectively.	Ta4Pd3Te16	Ta4Pd3Te16	Ta	4	Pd	3	Te	16																		3	2014																										A3B4C16																				K	4.3						4.3																				T	RES(zero), extrapolation	3.2												MHC155200																																																														self flux method					Nodal superconductivity and superconducting dome in new layered superconductor Ta4Pd3Te16			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, China	cond-mat/1404.0371	J. Pan,W. H. Jiao,X. C. Hong,Z. Zhang,L. P. He,P. L. Cai,J. Zhang,G. H. Cao,S. Y. Li1		
155201	MAT1404.0371	Tc(max) = 6.7 K at P=0.31 GPa. R(T)-exponent (n) depends on P. n(min) = 2.1 at P=0.31 GPa.	Ta4Pd3Te16	Ta4Pd3Te16	Ta	4	Pd	3	Te	16																		3	2014																										A3B4C16																				K	4.3						4.3	MPH155201																																																																																															self flux method					Nodal superconductivity and superconducting dome in new layered superconductor Ta4Pd3Te16			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, China	cond-mat/1404.0371	J. Pan,W. H. Jiao,X. C. Hong,Z. Zhang,L. P. He,P. L. Cai,J. Zhang,G. H. Cao,S. Y. Li1		
155202	APL101162602	Epitaxial thin films. CeNixBi2[100]//MgO[110]. CeNixBi2 is SC for 0.75< x <0.93 with Tc = 3.7 - 4.05.	CeNixBi2	Ce1Ni0.86Bi2	Ce	1	Ni	0.86	Bi	2																		5	2012																										ABC2					A	4.565														K	4.05		4.15				4.1																																																																							uOhm.cm							282				426												Ce(3N),Ni(4N5),Bi(5N)		Epitaxial thin films by MBE using e-gan. Substrate= (100)MgO. T<sub> = 410-440 C. growth rate = 0.5 A/s.					Superconducting epitaxial thin films of CeNixBi2 with a bismuth square net structure			Institute of Materials Science, Technische Universitat Darmstadt, 64287 Darmstadt, Germany	Appl.Phys.Lett., 101(2012)162602	Alexander Buckow,Katharina Kupka,Reiner Retzlaff,Jose Kurian,Lambert Alff		
155203	SST026015014		LaNixBi2	La1Ni0.72Bi2	La	1	Ni	0.72	Bi	2																		5	2013																										ABC2		ZrCuSiAs	P4/nmm		A	4.57		9.76												K			4.05			0.1	4.05	MTC155203																																																																						uOhm.cm							545				589												La(5N),Ni(4N5),Bi(5N)		Epitaxial films grown by RMBE using La,Ni,Bi targets om (100)MgO substrate. T<sub> = 430 C. growth rate = 0.5 A/s					Growth of superconducting epitaxial LaNixBi2 pnictide thin films with a Bi square net layer by reactive molecular beam epitaxy			Institute of Materials Science, Technische Universitat Darmstadt, Petersenstr. 23, D-64287 Darmstadt,Germany	Supercond.Sci.Technol., 26(2013)015014	A Buckow,R Retzlaff,J Kurian,L Alff		
155204	PRB091104519	Pd-content shows tentative value. Optimum Pd conc. (not measured). RRR = 1.58. R(T) = R0+A*T^2, where R0=57.4 uOhm.cm, A=2.54 nOhm.cm/K2 for 5< T <30 K	LaPdxSb2	La1Pd0.8Sb2	La	1	Pd	0.8	Sb	2																		5	2015																										ABC2																				K	3.23		3.27			0.03	3.25											Oe	M-H curve						10	1.8	T	RES(R=0.5Rn), extrapolation			1.1																																															uOhm.cm							57.4				91.5												La(3N),Pd(3N5),Sb(5N) or Bi(5N)		Epitaxial films grown by RMBE using La,Ni,Sb or Bi targets on (100)MgO substrate. T<sub> = 440 - 520 C. growth rate = 0.5 A/s					Superconductivity and role of pnictogen and Fe substitution in 112-LaPdx Pn2 (Pn = Sb, Bi)			Institute of Materials Science, Technische Universitat Darmstadt, Alarich-Weiss-Strasse 2, 64287 Darmstadt, Germany	Phys.Rev.B, 91(2015)104519	Reiner Retzlaff,Alexander Buckow,Philipp Komissinskiy,Soumya Ray,Stefan Schmidt,Holger Muhlig,Frank Schmidl,Paul Seidel,Jose Kurian,Lambert Alff		
155205	PRB091104519	Pd-content shows tentative value. Optimum Pd conc. (not measured). RRR = 1.70. R(T) = R0+A*T^2, where R0=86.6 uOhm.cm, A=2.64 nOhm.cm/K2 for 5< T <30 K	LaPdxBi2	La1Pd0.8Bi2	La	1	Pd	0.8	Bi	2																		5	2015																										ABC2					A	4.55		9.7												K	2.7		3.03				2.865																																																																							uOhm.cm							86.6				150												La(3N),Pd(3N5),Sb(5N) or Bi(5N)		Epitaxial films grown by RMBE using La,Ni,Sb or Bi targets on (100)MgO substrate. T<sub> = 440 - 520 C. growth rate = 0.5 A/s					Superconductivity and role of pnictogen and Fe substitution in 112-LaPdx Pn2 (Pn = Sb, Bi)			Institute of Materials Science, Technische Universitat Darmstadt, Alarich-Weiss-Strasse 2, 64287 Darmstadt, Germany	Phys.Rev.B, 91(2015)104519	Reiner Retzlaff,Alexander Buckow,Philipp Komissinskiy,Soumya Ray,Stefan Schmidt,Holger Muhlig,Frank Schmidl,Paul Seidel,Jose Kurian,Lambert Alff		
155206	PRB091165109	Anisotropy(H) = 2. (dC/gamma*Tc)=2.14. Energy gap from SP. 2gap-model, large one in in DB, small (2d/kTc) = 1.76. SP heat (beta)=0.000434 mJ/mol.K4. Hc1(T) measured by M vs H.	FeSe1-xSx	Fe1Se1	Fe	1	Se	1																				3	2015																										AB	2	PbO	P4/nmm		A	3.77		5.52											beta-FeSe	K				8.5			8.5											Oe	M-H curve						28.1	2	T	RES(0.9Rn), extrapolation			14.8										MHC155206							nm	SP analysis		446				4.44	14							mJ/mol.K2	5.3	SP																																						single crystals grown in quartz ampoule using AlCl3/KCl flux (hot 400C-cold 350C) for 45 days.					Superconducting properties of sulfur-doped iron selenide			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 91(2015)165109	Mahmoud Abdel-Hafiez,Yuan-Yuan Zhang,Zi-Yu Cao,Chun-Gang Duan,G. Karapetrov,V. M. Pudalov,V. A. Vlasenko,A. V. Sadakov,D. A. Knyazev,T. A. Romanova,D. A. Chareev,O. S. Volkova,A. N. Vasiliev,Xiao-Jia Chen		
155207	PRB091165109	Anisotropy(H) = 4. (dC/gamma*Tc)=2.43. Energy gap from SP. 2gap-model, large one in in DB, small (2d/kTc) = 3.8. SP heat (beta)=0.00048 mJ/mol.K4. Hc1(T) measured by M vs H.	FeSe1-xSx	Fe1Se0.96S0.04	Fe	1	Se	0.96	S	0.04																		3	2015																										AB	2	PbO	P4/nmm																beta-FeSe	K				9.58			9.58											Oe	M-H curve						40.4	2	T	RES(0.9Rn), extrapolation			17.5										MHC155207							nm	SP analysis		372				5	14							mJ/mol.K2	5.1	SP																																						single crystals grown in quartz ampoule using AlCl3/KCl flux (hot 400C-cold 350C) for 45 days.					Superconducting properties of sulfur-doped iron selenide			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 91(2015)165109	Mahmoud Abdel-Hafiez,Yuan-Yuan Zhang,Zi-Yu Cao,Chun-Gang Duan,G. Karapetrov,V. M. Pudalov,V. A. Vlasenko,A. V. Sadakov,D. A. Knyazev,T. A. Romanova,D. A. Chareev,O. S. Volkova,A. N. Vasiliev,Xiao-Jia Chen		
155208	PRB091165109	Anisotropy(H) = 3.5. (dC/gamma*Tc)=2.2. Energy gap from SP. 2gap-model, large one in in DB, small (2d/kTc) = 4.4. SP heat (beta)=0.00036 mJ/mol.K4. Hc1(T) measured by M vs H.	FeSe1-xSx	Fe1Se0.91S0.09	Fe	1	Se	0.91	S	0.09																		3	2015																										AB	2	PbO	P4/nmm																beta-FeSe	K				10.1			10.1											Oe	M-H curve						54.5	2	T	RES(0.9Rn), extrapolation			18.8										MHC155208							nm	SP analysis		433				4.7	14							mJ/mol.K2	4.9	SP																																						single crystals grown in quartz ampoule using AlCl3/KCl flux (hot 400C-cold 350C) for 45 days.					Superconducting properties of sulfur-doped iron selenide			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 91(2015)165109	Mahmoud Abdel-Hafiez,Yuan-Yuan Zhang,Zi-Yu Cao,Chun-Gang Duan,G. Karapetrov,V. M. Pudalov,V. A. Vlasenko,A. V. Sadakov,D. A. Knyazev,T. A. Romanova,D. A. Chareev,O. S. Volkova,A. N. Vasiliev,Xiao-Jia Chen		
155209	PRB091165109	Anisotropy(H) = 3.5. (dC/gamma*Tc)=1.95. Energy gap from SP. 2gap-model, large one in in DB, small (2d/kTc) = 3.92. SP heat (beta)=0.00041 mJ/mol.K4. Hc1(T) measured by M vs H.	FeSe1-xSx	Fe1Se0.89S0.11	Fe	1	Se	0.89	S	0.11																		3	2015																										AB	2	PbO	P4/nmm																beta-FeSe	K				10.7			10.7																				T	RES(0.9Rn), extrapolation			20.2																	nm	SP analysis		415				4.78	14							mJ/mol.K2	4.95	SP																																						single crystals grown in quartz ampoule using AlCl3/KCl flux (hot 400C-cold 350C) for 45 days.					Superconducting properties of sulfur-doped iron selenide			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 91(2015)165109	Mahmoud Abdel-Hafiez,Yuan-Yuan Zhang,Zi-Yu Cao,Chun-Gang Duan,G. Karapetrov,V. M. Pudalov,V. A. Vlasenko,A. V. Sadakov,D. A. Knyazev,T. A. Romanova,D. A. Chareev,O. S. Volkova,A. N. Vasiliev,Xiao-Jia Chen		
155210	PRL109217002	Se-Se bond length = 2.652 A. SP (beta) = 0.376 mJ/mol.K4. (dC/gamma*Tc) = 3.1	IrxSe2	Ir0.91Se2	Ir	0.91	Se	2																					2012																										AB2			Pa3[-]		A	5.98													pyrite	K	6.4		6.5				6.45																				T	estimation, not measured	14.3														A	from Hc2	48																		mJ/mol.K2	6.8	SP	249	SP																																		Ir(3N wt%),Se(3N wt%) or Te		mixture - in h-BN capsule - heat(1673 K,2h, 5GPa)					Superconductivity in Defective Pyrite-Type Iridium Chalcogenides IrxCh2 (Ch = Se and Te)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.Lett., 109(2012)217002	Yanpeng Qi,Satoru Matsuishi,Jiangang Guo,Hiroshi Mizoguchi,Hideo Hosono		
155211	PRL109217002		IrxSe2	Ir0.77Se2	Ir	0.77	Se	2																					2012																										AB2			Pa3[-]																pyrite	K	3.2		3.8				3.5	MTC155211																																																																																													Ir(3N wt%),Se(3N wt%) or Te		mixture - in h-BN capsule - heat(1673 K,2h, 5GPa)					Superconductivity in Defective Pyrite-Type Iridium Chalcogenides IrxCh2 (Ch = Se and Te)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.Lett., 109(2012)217002	Yanpeng Qi,Satoru Matsuishi,Jiangang Guo,Hiroshi Mizoguchi,Hideo Hosono		
155212	PRL109217002	(dC/gamma*Tc) = 2.0	IrxTe2	Ir0.93Te2	Ir	0.93	Te	2																					2012																										AB2																			pyrite	K	4.7						4.7																				T	estimation, not measured	4.58														A	from Hc2	69																					262	SP																																		Ir(3N wt%),Se(3N wt%) or Te		mixture - in h-BN capsule - heat(1673 K,2h, 5GPa)					Superconductivity in Defective Pyrite-Type Iridium Chalcogenides IrxCh2 (Ch = Se and Te)			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori, Yokohama 226-8503, Japan	Phys.Rev.Lett., 109(2012)217002	Yanpeng Qi,Satoru Matsuishi,Jiangang Guo,Hiroshi Mizoguchi,Hideo Hosono		
155213	SSC0530119	Hydrostatic P. Tc measured by as-SUS.	LaFe4P12	La1Fe4P12	La	1	Fe	4	P	12																			1985																										AB4C12		skutterudite			A	7.8316														K				4.1			4.1	MTC155213		K/GPa	0.72																																																																																												High purity elements in molten Sn (1050C). Cool to 500C over 10 days.- Q to RT					THE PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF LaT4PI2 (T = Fe, Ru, Os)			Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40502	Solid State Commun., 53(1985)119	L..E..DeLong,G.P.Meisner		
155214	SSC0530119	RuP2 phase (5-10%).  Hydrostatic P. Tc measured by as-SUS.	LaRu4P12	La1Ru4P12	La	1	Ru	4	P	12																			1985																										AB4C12		skutterudite			A	8.0561														K				7.2			7.2	MTC155213		K/GPa	-0.16																																																																																												High purity elements in molten Sn (1050C). Cool to 500C over 10 days.- Q to RT					THE PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF LaT4PI2 (T = Fe, Ru, Os)			Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40502	Solid State Commun., 53(1985)119	L..E..DeLong,G.P.Meisner		
155215	SSC0530119	OsP2 phase (5-10%).  Hydrostatic P. Tc measured by as-SUS.	LaOs4P12	La1Os4P12	La	1	Os	4	P	12																			1985																										AB4C12		skutterudite			A	8.0844														K				1.8			1.8	MTC155213		K/GPa	-0.095																																																																																												OsP2 prepared by sintering. Then added to a melt that was cooled from 1250C.					THE PRESSURE DEPENDENCE OF THE SUPERCONDUCTING TRANSITION TEMPERATURE OF LaT4PI2 (T = Fe, Ru, Os)			Department of Physics and Astronomy, University of Kentucky, Lexington, KY 40502	Solid State Commun., 53(1985)119	L..E..DeLong,G.P.Meisner		
155216	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca9La1Pt3Fe10As18	Ca	9	La	1	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				27.9			27.9	MTC155216																																																																																															See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155217	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca8.87La1.13Pt3Fe10As18	Ca	8.87	La	1.13	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				32.8			32.8																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155218	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca8.85La1.15Pt3Fe10As18	Ca	8.85	La	1.15	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				35.1			35.1																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155219	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca8.6La1.4Pt3Fe10As18	Ca	8.6	La	1.4	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				34.5			34.5																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155220	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca8.44La1.56Pt3Fe10As18	Ca	8.44	La	1.56	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				32.3			32.3																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155221	SSC2010036		(Ca1-xLax)(Pt3As8)(FeAs)10	Ca7.62La2.38Pt3Fe10As18	Ca	7.62	La	2.38	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				26			26																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155222	SSC2010036		(Ca1-xCex)(Pt3As8)(FeAs)10	Ca9.26Ce0.74Pt3Fe10As18	Ca	9.26	Ce	0.74	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				22.6			22.6	MTC155216																																																																																															See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155223	SSC2010036		(Ca1-xCex)(Pt3As8)(FeAs)10	Ca8.38Ce1.62Pt3Fe10As18	Ca	8.38	Ce	1.62	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				30.5			30.5																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155224	SSC2010036		(Ca1-xCex)(Pt3As8)(FeAs)10	Ca8.32Ce1.68Pt3Fe10As18	Ca	8.32	Ce	1.68	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				30.4			30.4																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155225	SSC2010036		(Ca1-xCex)(Pt3As8)(FeAs)10	Ca7.16Ce2.84Pt3Fe10As18	Ca	7.16	Ce	2.84	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				18.9			18.9																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155226	SSC2010036		(Ca1-xPrx)(Pt3As8)(FeAs)10	Ca9.39Pr0.61Pt3Fe10As18	Ca	9.39	Pr	0.61	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				19.5			19.5																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155227	SSC2010036		(Ca1-xPrx)(Pt3As8)(FeAs)10	Ca8.77Pr1.23Pt3Fe10As18	Ca	8.77	Pr	1.23	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				26.9			26.9	MTC155216																																																																																															See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155228	SSC2010036		(Ca1-xPrx)(Pt3As8)(FeAs)10	Ca8.48Pr1.52Pt3Fe10As18	Ca	8.48	Pr	1.52	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				31.8			31.8																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155229	SSC2010036		(Ca1-xPrx)(Pt3As8)(FeAs)10	Ca8.03Pr1.97Pt3Fe10As18	Ca	8.03	Pr	1.97	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				25			25																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155230	SSC2010036		(Ca1-xPrx)(Pt3As8)(FeAs)10	Ca6.85Pr3.15Pt3Fe10As18	Ca	6.85	Pr	3.15	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				20.5			20.5																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155231	SSC2010036		(Ca1-xNdx)(Pt3As8)(FeAs)10	Ca8.77Nd1.23Pt3Fe10As18	Ca	8.77	Nd	1.23	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				28.4			28.4																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155232	SSC2010036		(Ca1-xNdx)(Pt3As8)(FeAs)10	Ca8.41Nd1.59Pt3Fe10As18	Ca	8.41	Nd	1.59	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				28.1			28.1																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155233	SSC2010036		(Ca1-xNdx)(Pt3As8)(FeAs)10	Ca7.65Nd2.35Pt3Fe10As18	Ca	7.65	Nd	2.35	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				18.9			18.9																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155234	SSC2010036		(Ca1-xSmx)(Pt3As8)(FeAs)10	Ca9.29Sm0.71Pt3Fe10As18	Ca	9.29	Sm	0.71	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				26.2			26.2																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155235	SSC2010036		(Ca1-xSmx)(Pt3As8)(FeAs)10	Ca8.45Sm1.55Pt3Fe10As18	Ca	8.45	Sm	1.55	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				28			28																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155236	SSC2010036		(Ca1-xGdx)(Pt3As8)(FeAs)10	Ca9.06Gd0.94Pt3Fe10As18	Ca	9.06	Gd	0.94	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				25			25																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155237	SSC2010036		(Ca1-xTbx)(Pt3As8)(FeAs)10	Ca9.16Tb0.84Pt3Fe10As18	Ca	9.16	Tb	0.84	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				23.7			23.7																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155238	SSC2010036		(Ca1-xDyx)(Pt3As8)(FeAs)10	Ca9.35Dy0.65Pt3Fe10As18	Ca	9.35	Dy	0.65	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				20.9			20.9																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155239	SSC2010036		(Ca1-xHox)(Pt3As8)(FeAs)10	Ca9.68Ho0.32Pt3Fe10As18	Ca	9.68	Ho	0.32	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				19.5			19.5																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155240	SSC2010036		(Ca1-xErx)(Pt3As8)(FeAs)10	Ca9.75Er0.25Pt3Fe10As18	Ca	9.75	Er	0.25	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				17.6			17.6																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155241	SSC2010036		(Ca1-xTmx)(Pt3As8)(FeAs)10	Ca9.72Tm0.28Pt3Fe10As18	Ca	9.72	Tm	0.28	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				14.8			14.8																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155242	SSC2010036		(Ca1-xYbx)(Pt3As8)(FeAs)10	Ca9.5Yb0.5Pt3Fe10As18	Ca	9.5	Yb	0.5	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				11.6			11.6																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155243	SSC2010036		(Ca1-xLux)(Pt3As8)(FeAs)10	Ca9.75Lu0.25Pt3Fe10As18	Ca	9.75	Lu	0.25	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				10.9			10.9																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155244	SSC2010036		(Ca1-xYx)(Pt3As8)(FeAs)10	Ca9.58Y0.42Pt3Fe10As18	Ca	9.58	Y	0.42	Pt	3	Fe	10	As	18														1	2015																																													Ca-10-3-8 phase	K				18.6			18.6																																																																																																See Phys.Rev.B., 86(2012)060516					Superconductivity by rare earth doping in the 1038-type compounds (Ca1-xREx)10(FeAs)10(Pt3As8) with RE = Y, La-Nd, Sm-Lu			Department Chemie, Ludwig-Maximilians-Universitat Munchen, Butenandtstr. 5-13 (Haus D), 81377 Munchen, Germany	Solid State Commun., 201(2015)36	Tobias Sturzer,Gerald Derondeau,Eva-Maria Bertschler,Dirk Johrendt		
155245	JPS083054706	impurity phase: Cu3As(10%), FeAs(1%). not SC. R(40K) = 0.10 mOhm.cm	CuFeAs	Cu1Fe1As1	Cu	1	Fe	1	As	1																		1	2014								9																		ABC	2	Cu2Sb	P4/nmm		A	3.7442		5.8925											As-Fe-As bond angle (alpha=94.23, beta=117.59)	K					2																																																																									mOhm.cm											0.32												Cu2As,Fe2As		mixture - heat(700C,24h in quartz ampoule) - regrond - pellet - heat(700C,4d, in quartz ampoule)					CuFeAs: A New Member in the 111-Family of Iron-Pnictides			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	J.Phys.Soc,Jpn, 83(2014)054706	Gohil S. Thakur,Zeba Haque,L. C. Gupta,A. K. Ganguli		
155246	JPS084024709	As-grown sample. Two type of FM(Tm= 4.5 & 7.5 K) for x >= 0.45. Lattice const. given in Fig. MPH155246 for 0=<x=<1.	Ce(O,F)BiS2	Ce1Bi1S2F0.45O0.55	Ce	1	Bi	1	S	2	F	0.45													O	0.55		1	2015							4.78																			ABCD2	2	CeOBiS2	P4/nmm		A	4.036		13.4056											BiS2 layer SC	K	2.18		2.41				2.295	MPH155246																																																																																													Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		solid state reaction. mixture - pellet - sealed in quartz tube - heat(800C,10h)					Coexistence of Bulk Superconductivity and Magnetism in CeO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc,Jpn, 84(2015)024709	Satoshi Demura,Keita Deguchi,Yoshikazu Mizuguchi,Kazuki Sato,Ryota Honjyo,Aichi Yamashita,Takuma Yamaki,Hiroshi Hara,Tohru Watanabe,Saleem J. Denholme,Masaya Fujioka,Hiroyuki Okazaki,Toshinori Ozaki,Osuke Miura,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155247	JPS084024709		Ce(O,F)BiS2	Ce1Bi1S2F0.7O0.3	Ce	1	Bi	1	S	2	F	0.7													O	0.3		1	2015							7.62																			ABCD2	2	CeOBiS2	P4/nmm		A	4.0393		13.3663											BiS2 layer SC	K	2.82		3.02				2.92																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		solid state reaction. mixture - pellet - sealed in quartz tube - heat(800C,10h)					Coexistence of Bulk Superconductivity and Magnetism in CeO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc,Jpn, 84(2015)024709	Satoshi Demura,Keita Deguchi,Yoshikazu Mizuguchi,Kazuki Sato,Ryota Honjyo,Aichi Yamashita,Takuma Yamaki,Hiroshi Hara,Tohru Watanabe,Saleem J. Denholme,Masaya Fujioka,Hiroyuki Okazaki,Toshinori Ozaki,Osuke Miura,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155248	JPS084024709	High-P-ANN  sample. Two type of FM(Tm= 4.5 & 7.5 K) for x >= 0.45. Lattice const. given in Fig. MPH155248 for 0=<x=<1. SC and FM coexist for x > 0.6.	Ce(O,F)BiS2	Ce1Bi1S2F0.6O0.4	Ce	1	Bi	1	S	2	F	0.6													O	0.4		1	2015							7.69																			ABCD2	2	CeOBiS2	P4/nmm		A	4.0423		13.3513											BiS2 layer SC	K	3.72		5.2				4.46	MPH155248																																																																																													Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		solid state reaction. mixture - pellet - sealed in quartz tube - heat(800C,10h) reground - ANN(600C,1h､P=3 GPa)					Coexistence of Bulk Superconductivity and Magnetism in CeO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc,Jpn, 84(2015)024709	Satoshi Demura,Keita Deguchi,Yoshikazu Mizuguchi,Kazuki Sato,Ryota Honjyo,Aichi Yamashita,Takuma Yamaki,Hiroshi Hara,Tohru Watanabe,Saleem J. Denholme,Masaya Fujioka,Hiroyuki Okazaki,Toshinori Ozaki,Osuke Miura,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155249	JPS084024709		Ce(O,F)BiS2	Ce1Bi1S2F0.9O0.1	Ce	1	Bi	1	S	2	F	0.9													O	0.1		1	2015							7.6																			ABCD2	2	CeOBiS2	P4/nmm		A	4.0322		13.3637											BiS2 layer SC	K	5.96		7.75				6.855																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		solid state reaction. mixture - pellet - sealed in quartz tube - heat(800C,10h) reground - ANN(600C,1h､P=3 GPa)					Coexistence of Bulk Superconductivity and Magnetism in CeO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc,Jpn, 84(2015)024709	Satoshi Demura,Keita Deguchi,Yoshikazu Mizuguchi,Kazuki Sato,Ryota Honjyo,Aichi Yamashita,Takuma Yamaki,Hiroshi Hara,Tohru Watanabe,Saleem J. Denholme,Masaya Fujioka,Hiroyuki Okazaki,Toshinori Ozaki,Osuke Miura,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155250	JPS084024709		Ce(O,F)BiS2	Ce1Bi1S2F0.4O0.6	Ce	1	Bi	1	S	2	F	0.4													O	0.6		1	2015																										ABCD2	2	CeOBiS2	P4/nmm		A	4.0339		13.4688											BiS2 layer SC	K			2.85				2.85																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Ce2S3		solid state reaction. mixture - pellet - sealed in quartz tube - heat(800C,10h) reground - ANN(600C,1h､P=3 GPa)					Coexistence of Bulk Superconductivity and Magnetism in CeO1-xFxBiS2			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc,Jpn, 84(2015)024709	Satoshi Demura,Keita Deguchi,Yoshikazu Mizuguchi,Kazuki Sato,Ryota Honjyo,Aichi Yamashita,Takuma Yamaki,Hiroshi Hara,Tohru Watanabe,Saleem J. Denholme,Masaya Fujioka,Hiroyuki Okazaki,Toshinori Ozaki,Osuke Miura,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155251	PHB4590021	Anomaly in V(P) appears around P=15 GPa. Lat-a = 4.9284 A at P=41 GPa.	Nb3Ga	Ga1Nb3	Ga	1	Nb	3																				3	2015																		GPa		198						AB3		A15			A	5.1673														K			16.5				16.5	MTC155251																																																																																															mixture(Nb:Ga=3:1) - pellet - arc melting					High pressure transport and structural studies on Nb3Ga  superconductor			High Pressure Science and Engineering Center and Department of Physics and Astronomy, University of Nevada Las Vegas, Las Vegas, NV89154 USA	Physica B, 459(2015)21	Vahe Mkrtcheyan,Ravhi Kumar,Jason Baker,Anthony Connolly,Daniel Antonio,Andrew Cornelius,Yusheng Zhao		
155252	PHC5090008	SC(Tc= 18-20 K) for 0.05 =< x < 0.2 in Ba1-xYbxFe2As2. Tc measured by dc-SUS. Cleaved crystals were brittle, R(T) not measured.	(Ba,Yb)Fe2As2	Ba0.9Yb0.1Fe2As2	Ba	0.9	Yb	0.1	Fe	2	As	2																3	2015																										AB2C2		ThCr2Si2			A			13.0213											Fe-122	K				20			20																																																																																														Ba,Yb(3N),Fe(5N),As(4N)		FeAs self-flux method. mixture - in alumina oxide crucible - sealed in quartz tube(Ar) - heat to 1150C(70C/h) - hold(8h) - cool to 1000C(2C/h) - FC to RT					Superconductivity in Yb-doped BaFe2As2			Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 62199, Taiwan, ROC	Physica C, 509(2015)8	S.C. Chen,W.H. Lee,M.D. Lan		
155253	SSC0520797	ANN(900C,6d)	LaRh2Si2	La1Rh2Si2	La	1	Rh	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.1109		10.289												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155254	SSC0520797	ANN(1200C,2d) (700C,9d)	LaIr2Si2(LT)	La1Ir2Si2	La	1	Ir	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.094		10.248												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155255	SSC0520797	as-cast	LaIr2Si2(HT)	La1Ir2Si2	La	1	Ir	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.19		9.944												K	1.52		1.58				1.55																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155256	SSC0520797	ANN(1200C2d) (700C,9d)	LaPt2Si2	La1Pt2Si2	La	1	Pt	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.277		9.798												K	1.31		1.42				1.365																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155257	SSC0520797	as-cast	YRu2Si2	Y1Ru2Si2	Y	1	Ru	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.157		9.522												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155258	SSC0520797	ANN(1000C,6d)	YRh2Si2	Y1Rh2Si2	Y	1	Rh	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.023		9.9												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155259	SSC0520797	ANN(1000C,6d)	YPd2Si2	Y1Pd2Si2	Y	1	Pd	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.125		9.842												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155260	SSC0520797	as-cast	YOs2Si2	Y1Os2Si2	Y	1	Os	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.128		9.667												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155261	SSC0520797	ANN(1300C,2d) (700C,7d)	YIr2Si2(LT)	Y1Ir2Si2	Y	1	Ir	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.047		9.914												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155262	SSC0520797	ANN(1300C,2d)	YIr2Si2(HT)	Y1Ir2Si2	Y	1	Ir	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.081		9.754												K	2.72		2.83				2.775																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155263	SSC0520797	ANN(1250C,2d) (1000C,6d) (700C,7d)	YPt2Si2	Y1Pt2Si2	Y	1	Pt	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.162		9.817												K	1.58		1.7				1.64																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155264	SSC0520797	ANN(1000C,4d)	ThRu2Si2	Th1Ru2Si2	Th	1	Ru	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.188		9.736												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155265	SSC0520797	as-cast	ThRh2Si2	Th1Rh2Si2	Th	1	Rh	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.089		10.018												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155266	SSC0520797	ANN(1000C,4d)	ThPd2Si2	Th1Pd2Si2	Th	1	Pd	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.187		9.92												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155267	SSC0520797	ANN(1000C,4d)	ThOs2Si2	Th1Os2Si2	Th	1	Os	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.189		9.798												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155268	SSC0520797	ANN(1300C,2d) (1000C,2d) (700C,4d)	ThIr2Si2	Th1Ir2Si2	Th	1	Ir	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.15		9.887												K	2.16		2.27				2.215																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155269	SSC0520797	as-cast	ThPt2Si2	Th1Pt2Si2	Th	1	Pt	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.238		9.713												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155270	SSC0520797	as-cast	URh2Si2	U1Rh2Si2	U	1	Rh	2	Si	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.994		9.993												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155271	SSC0520797	as-cast	UIr2Si2	U1Ir2Si2	U	1	Ir	2	Si	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.088		9.938												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155272	SSC0520797	ANN(1250C,2d)	ThRu2Ge2	Th1Ru2Ge2	Th	1	Ru	2	Ge	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.264		9.942												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155273	SSC0520797	ANN(100C,4d) (700C,7d)	ThRh2Ge2	Th1Rh2Ge2	Th	1	Rh	2	Ge	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.23		10.042												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155274	SSC0520797	ANN(1000C,4d)	ThPd2Ge2	Th1Pd2Ge2	Th	1	Pd	2	Ge	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.295		10.104												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155275	SSC0520797	ANN(1300C,2d) (1000C,7d) (700C,9d)	ThOs2Ge2	Th1Os2Ge2	Th	1	Os	2	Ge	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.266		9.954												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155276	SSC0520797	ANN(1000C,4d) (700C,9d)	ThIr2Ge2	Th1Ir2Ge2	Th	1	Ir	2	Ge	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.222		10.087												K	1.46		1.56				1.51																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155277	SSC0520797	as-cast	ThPt2Ge2	Th1Pt2Ge2	Th	1	Pt	2	Ge	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.342		9.803												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155278	SSC0520797	as-cast	URh2Ge2	U1Rh2Ge2	U	1	Rh	2	Ge	2																		1	1984																										AB2C2	2	ThCr2Si2	I4/mmm		A	4.141		9.696												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155279	SSC0520797	as-cast	UIr2Ge2	U1Ir2Ge2	U	1	Ir	2	Ge	2																		1	1984																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.165		9.833												K							1.1																																																																																														T(3N),Si(7N5),Ge(6N5)		arc melting - ANN using Zr, Mo, Ta foil					Superconductivity and rerative phase stability in 1:2:2 ternary transition metal silisides and germanides			Departement de Physique de la Matiere Condensee, Unversite de Geneve	Solid State Commun., 52(1984)797	R.N.Shelton,H.F.Braun,K.Musick		
155280	PHB1690687		(Pb,Sn,In)Te	Pb0.19Sn0.76In0.05Te1	Pb	0.19	Sn	0.76	In	0.05	Te	1																1	1991																										AB		NaCl																		K	2.76						2.76	MTC155280																																																																																															Metalloceramic method. ANN(650C,100h)					Superconducting Properties of the SnTe-PbTe System Doped with Indium			A.F.Ioffe Physical-Technical Institute, USSR Academy of Sciences, Leningrad, USSR	Physica B, 169(1991)687	G.S.Bushmarina,I.A.Drabkin,D.V.Mashovets,R.V.Parfeniev,D.V.Shamshur,M.A.Shachov		
155281	PHB1690687		(Pb,Sn,In)Te	Pb0.18Sn0.74In0.08Te1	Pb	0.18	Sn	0.74	In	0.08	Te	1																1	1991																										AB		NaCl																		K	2.85						2.85	MTC155284																																																																																															Metalloceramic method. ANN(650C,100h)					Superconducting Properties of the SnTe-PbTe System Doped with Indium			A.F.Ioffe Physical-Technical Institute, USSR Academy of Sciences, Leningrad, USSR	Physica B, 169(1991)687	G.S.Bushmarina,I.A.Drabkin,D.V.Mashovets,R.V.Parfeniev,D.V.Shamshur,M.A.Shachov		
155282	PHB1690687		(Pb,Sn,In)Te	Pb0.35Sn0.53In0.12Te1	Pb	0.35	Sn	0.53	In	0.12	Te	1																1	1991																										AB		NaCl																		K	3.5						3.5	MTC155284																																																																																															Metalloceramic method. ANN(650C,100h)					Superconducting Properties of the SnTe-PbTe System Doped with Indium			A.F.Ioffe Physical-Technical Institute, USSR Academy of Sciences, Leningrad, USSR	Physica B, 169(1991)687	G.S.Bushmarina,I.A.Drabkin,D.V.Mashovets,R.V.Parfeniev,D.V.Shamshur,M.A.Shachov		
155283	PHB1690687		(Pb,Sn,In)Te	Pb0.43Sn0.43In0.16Te1	Pb	0.43	Sn	0.43	In	0.16	Te	1																1	1991																										AB		NaCl																		K	4.17						4.17	MTC155280																																																																																															Metalloceramic method. ANN(650C,100h)					Superconducting Properties of the SnTe-PbTe System Doped with Indium			A.F.Ioffe Physical-Technical Institute, USSR Academy of Sciences, Leningrad, USSR	Physica B, 169(1991)687	G.S.Bushmarina,I.A.Drabkin,D.V.Mashovets,R.V.Parfeniev,D.V.Shamshur,M.A.Shachov		
155284	PHB1690687		(Pb,Sn,In)Te	Pb0.4Sn0.4In0.2Te1	Pb	0.4	Sn	0.4	In	0.2	Te	1																1	1991																										AB		NaCl																		K	4.24						4.24	MTC155284																																																																																															Metalloceramic method. ANN(650C,100h)					Superconducting Properties of the SnTe-PbTe System Doped with Indium			A.F.Ioffe Physical-Technical Institute, USSR Academy of Sciences, Leningrad, USSR	Physica B, 169(1991)687	G.S.Bushmarina,I.A.Drabkin,D.V.Mashovets,R.V.Parfeniev,D.V.Shamshur,M.A.Shachov		
155300	MAT1412.0460	P-induced SC. P and T cycle: (P=100 GPa) - (cool to 4 K) - warm to 100-150 K and apply next P) - (cool to 4K). Tc increases with increasind P from 60 K phase (P<160 GPa)	H2S	H2S1	H	2	S	1																					2014																																														K			60				60	MTC155300																			T	RES(R-on)	25												MHC155301																																																																			Conventional superconductivity at 190 K at high pressures			Max-Planck Institut fur Chemie, Chemistry and Physics at High Pressures Group, Postfach 3060, 55020 Mainz, Germany	cond-mat/1412.0460	A.P.Drozdov,M.I.Eremets,I.A.Troyan		
155301	MAT1412.0460	P-induced SC. P and T cycle: (P applied at 220-300 K.) -  (cool to 4K.).  Two phases appears: Tc=190 K and 30 K. 30 K-phase is unstable.	H2S	H2S1	H	2	S	1																					2014																																														K			185				185	MTC155301																			T	RES(R-on)	70												MHC155301																																																																			Conventional superconductivity at 190 K at high pressures			Max-Planck Institut fur Chemie, Chemistry and Physics at High Pressures Group, Postfach 3060, 55020 Mainz, Germany	cond-mat/1412.0460	A.P.Drozdov,M.I.Eremets,I.A.Troyan		
155302	MAT1412.0460	P-induced SC. P and T cycle: (P=100 GPa) - (cool to 4 K) - warm to 100-150 K and apply next P) - (cool to 4K)	D2S	D2S1	D	2	S	1																					2014																																														K			30				30	MTC155302																																																																																																				Conventional superconductivity at 190 K at high pressures			Max-Planck Institut fur Chemie, Chemistry and Physics at High Pressures Group, Postfach 3060, 55020 Mainz, Germany	cond-mat/1412.0460	A.P.Drozdov,M.I.Eremets,I.A.Troyan		
155303	ACS1342516	nominal compositions (LaN:Ni:B = 0.9:1:1)	(LaN)2(Ni2B2)	La1Ni1B1N1	La	1	Ni	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.7266		7.5759												K	3.69	3.92	4.43	3.82			3.92																																																																																																high-pressure synthesis. (1200C, 0.5h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155304	ACS1342516	nominal compositions (RN:Ni:B = 0.9:1:1)	(LaN)2(Ru2B2)	La1Ru1B1N1	La	1	Ru	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.7646		7.9514												K					1.8																																																																																																		high-pressure synthesis. (1200C, 1h, P=2 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155305	ACS1342516	nominal compositions (RN:Ni:B = 0.9:1:1)	(LaN)2(Rh2B2)	La1Rh1B1N1	La	1	Rh	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.867		7.489												K					1.8																																																																																																		high-pressure synthesis. (1400C, 1h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155306	ACS1342516	nominal compositions (RN:Ni:B = 0.9:1:1)	(LaN)2(Ir2B2)	La1Ir1B1N1	La	1	Ir	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.8458		7.639												K					1.8																																																																																																		high-pressure synthesis. (1400C, 1h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155307	ACS1342516	nominal compositions (RN:Ni:B = 0.9:1:1)	(LaN)2(Pt2B2)	La1Pt1B1N1	La	1	Pt	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.824		7.8649												K	6.54	6.7	7.58	6.97			6.7																																																																																																high-pressure synthesis. (1400C, 1h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155308	ACS1342516		(LaN)3(Co2B2)	La3Co2B2N3	La	3	Co	2	B	2	N	3																1	2012																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7152		20.399												K					1.8																																																																																																		high-pressure synthesis. (1400C, 2h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155309	ACS1342516		(LaN)3(Ni2B2)	La3Ni2B2N3	La	3	Ni	2	B	2	N	3																1	2012																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7123		20.538												K				14.9			14.9																																																																																																high-pressure synthesis. (1400C, 2h, P=5 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155310	ACS1342516	nominal compositions (LaN:Ru:B = 3.3:1.9:1)	(LaN)3(Ru2B2)	La3Ru2B2N3	La	3	Ru	2	B	2	N	3																1	2012																										A2B2C3D3		La3Ni2B2N3	I4/mmm		A	3.7454		21.222												K					1.8																																																																																																		high-pressure synthesis. (1600C, 1h, P=2 GPa)					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155311	ACS1342516		(CaN)2(Ni2B2)	Ca1Ni1B1N1	Ca	1	Ni	1	B	1	N	1																1	2012																										ABCD		LuNiBC	P4/nmm		A	3.5359		7.6394												K		2.08		2.12			2.08																																																																																																nominal mixture(Ca3N2,Ni,B,BN) - pellet - high pressure synthesis					Superconductivity in LaTMBN and La3TM2B2N3 (TM = Transition Metal) Synthesized under High Pressure			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)2516	Naoki Imamura,Hiroshi Mizoguchi,Hideo Hosono		
155312	ACS1355372		Bi3O2S3	Bi3S3O2	Bi	3	S	3																	O	2			2013																															A			41.4											Bi-O-S system	K				4.5			4.5																																																																																																					Stacking Variants and Superconductivity in the Bi-O-S System			Department of Chemistry, Department of Physics and Astronomy, Institute for Quantum Matter, and Department of Earth andPlanetary Sciences, Johns Hopkins University, Baltimore, Maryland 21218, United State	J.Am.Chem.Soc., 135(2013)5372	W. Adam Phelan,David C. Wallace,Kathryn E. Arpino,James R. Neilson,Kenneth J. Livi,Che R. Seabourne,Andrew J. Scott,Tyrel M. McQueen		
155313	ACS1355372		Bi2OS2	Bi2S2O1	Bi	2	S	2																	O	1			2013																															A	4		13.8											Bi-O-S system	K					2																																																																																																							Stacking Variants and Superconductivity in the Bi-O-S System			Department of Chemistry, Department of Physics and Astronomy, Institute for Quantum Matter, and Department of Earth andPlanetary Sciences, Johns Hopkins University, Baltimore, Maryland 21218, United State	J.Am.Chem.Soc., 135(2013)5372	W. Adam Phelan,David C. Wallace,Kathryn E. Arpino,James R. Neilson,Kenneth J. Livi,Che R. Seabourne,Andrew J. Scott,Tyrel M. McQueen		
155314	ACS1355372	sample sypws nominal composisions. Bi2OS2 intercalated in Bi3O2S3. Tc decreases with increasing Bi2OS2 intercalant.	Bi12O18S11	Bi12S11O18	Bi	12	S	11																	O	18			2013																																													Bi-O-S system	K				4			4																																																																																																					Stacking Variants and Superconductivity in the Bi-O-S System			Department of Chemistry, Department of Physics and Astronomy, Institute for Quantum Matter, and Department of Earth andPlanetary Sciences, Johns Hopkins University, Baltimore, Maryland 21218, United State	J.Am.Chem.Soc., 135(2013)5372	W. Adam Phelan,David C. Wallace,Kathryn E. Arpino,James R. Neilson,Kenneth J. Livi,Che R. Seabourne,Andrew J. Scott,Tyrel M. McQueen		
155315	ACS13420001	R(T)-exponent = 0.03. (dC/gamma*Tc) = 3.0)	Ir0.94-xRhxSe2	Ir0.94Se2	Ir	0.94	Se	2																					2012																										AB2	1		Pa3[-]	205	A	5.9824														K			6.24				6.24																																																								mJ/mol.K2	6.41	SP	253	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155316	ACS13420001	R(T)-exponent = 0.21. (dC/gamma*Tc) = 3.25)	Ir0.94-xRhxSe2	Ir0.85Rh0.09Se2	Ir	0.85	Rh	0.09	Se	2																			2012																										AB2	1		Pa3[-]	205	A	5.9875														K			7.61				7.61																																																											250	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155317	ACS13420001	R(T)-exponent = 0.37.	Ir0.94-xRhxSe2	Ir0.82Rh0.12Se2	Ir	0.82	Rh	0.12	Se	2																			2012																										AB2	1		Pa3[-]	205	A															K			7.96				7.96																																																																																														Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155318	ACS13420001	R(T)-exponent = 0.55.	Ir0.94-xRhxSe2	Ir0.76Rh0.18Se2	Ir	0.76	Rh	0.18	Se	2																			2012																										AB2	1		Pa3[-]	205	A	5.9947														K			8.09				8.09																																																																																														Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155319	ACS13420001	R(T)-exponent = 0.75. (dC/gamma*Tc) = 3.29)	Ir0.94-xRhxSe2	Ir0.64Rh0.3Se2	Ir	0.64	Rh	0.3	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.0001														K			8.77				8.77																																																											250	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155320	ACS13420001	R(T)-exponent = 1.10. (dC/gamma*Tc) = 3.55). Hc2(0) = 24.5 T from GL approx.	Ir0.94-xRhxSe2	Ir0.58Rh0.36Se2	Ir	0.58	Rh	0.36	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.005														K			9.6				9.6	MTC155320										Oe	M-H curve, linear approx.	200							T	R(on), WHH	28.5												MHC155320														5.95	14							mJ/mol.K2	8.02	SP	242	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155321	ACS13420001	R(T)-exponent = 1.08. (dC/gamma*Tc) = 3.24)	Ir0.94-xRhxSe2	Ir0.44Rh0.5Se2	Ir	0.44	Rh	0.5	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.0068														K			9.24				9.24																																																											247	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155322	ACS13420001	R(T)-exponent = 1.27. (dC/gamma*Tc) = 3.14)	Ir0.94-xRhxSe2	Ir0.37Rh0.57Se2	Ir	0.37	Rh	0.57	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.0077														K			9.09				9.09																																																											251	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155323	ACS13420001	R(T)-exponent = 1.39.	Ir0.94-xRhxSe2	Ir0.3Rh0.64Se2	Ir	0.3	Rh	0.64	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.0097														K			8.39				8.39																																																																																														Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155324	ACS13420001	R(T)-exponent = 1.56. (dC/gamma*Tc) = 3.06)	Ir0.94-xRhxSe2	Ir0.19Rh0.75Se2	Ir	0.19	Rh	0.75	Se	2																			2012																										AB2	1		Pa3[-]	205	A	6.0084														K			7.49				7.49																																																											276	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155325	ACS13420001	R(T)-exponent = 2.10. (dC/gamma*Tc) = 2.80)	Ir0.94-xRhxSe2	Rh0.94Se2	Rh	0.94	Se	2																					2012																										AB2	1		Pa3[-]	205	A	6.0093														K			5.19				5.19																																																								mJ/mol.K2	3.57	SP	293	SP																																		Ir,Rh,Se-powder		mixture - (h-BN capsule) - heat(1773K, 3h, P=5 GPa)					Tc Maximum in Solid Solution of Pyrite IrSe2-RhSe2 Induced by Destabilization of Anion Dimers			Frontier Research Center, and Materials and Structures Laboratory, Tokyo Institute of Technology, Yokohama 226-8503, Japan	J.Am.Chem.Soc., 134(2012)20001	Jiangang Guo,Yanpeng Qi,Satoru Matsuishi,Hideo Hosono		
155326	ACS13412893	Annealed ( 773K,40h, in vac) sample. impurity phases: BaFe2As2,Fe2As, BaTi2As2O. R(T) anomaly at 125 K, corresponding to CDW/SDW order.	Ba2Ti2Fe2As4O	Ba2Ti2Fe2As4O1	Ba	2	Ti	2	Fe	2	As	4													O	1			2012																											2		I4/mmm		A	4.0276		27.3441											intergrowth of BaFe2As2 and BaTi2As2O	K	16		21.5				18.75										23																																																													mOhm.cm							0.834			21.5	1.415												Ba,Ti,Fe,As,TiO2		mixture - alumina tube - sealed in quartz ampule - heat(1173K,24h) - reground - SIN(1373K,40h) - FC to RT					Ba2Ti2Fe2As4O: A New Superconductor Containing Fe2As2 Layers and Ti2O Sheets			Department of Physics, State Key Lab of Silicon Materials, and Center of Electron Microscope, Zhejiang University, Hangzhou 310027, China	J.Am.Chem.Soc., 134(2012)12893	Yun-Lei Sun,Hao Jiang,Hui-Fei Zhai,Jin-Ke Bao,Wen-He Jiao,Qian Tao,Chen-Yi Shen,Yue-Wu Zeng,Zhu-An Xu,Guang-Han Cao		
155327	ACS1361284	RRR = 26. (dC<el>/Tc) = 54 mJ/mol.K2. (dC/gamma*Tc) = 1.4. e-ph = 0.77. lattice term in SP (beta) = 11.11 mJ/mol.K4. DOS = 18.1 /ev.fu.	Ta4Pd3Te16	Ta4Pd3Te16	Ta	4	Pd	3	Te	16																		3	2014																										S3B4C16	4		I2/m		A	17.687	3.735	19.51											beta=110.42. structural data at 111 K from A. Mar et al	K	4.11	4.46	4.62	4.6			4.46										90																																											MSP155327			mJ/mol.K2	42.8	SP	159	SP											uOhm.m							2.34			6	61												Ta(3N7),Pd(4N5),Te(4N)		self flux method. mixture(Ta:Pd:Te = 2:3:15) - sealed in quartz ampule - heat to 1223 K - hold(24h) - cool to 923 K(5K/h) - cool to RT					Superconductivity in a Layered Ta4Pd3Te16 with PdTe2 Chains			Department of Physics, State Key Lab of Silicon Materials and Center of Electron Microscope, Zhejiang University, Hangzhou 310027, China	J.Am.Chem.Soc., 136(2014)1284	Wen-He Jiao,Zhang-Tu Tang,Yun-Lei Sun,Yi Liu,Qian Tao,Chun-Mu Feng,Yue-Wu Zeng,Zhu-An Xu,Guang-Han Cao		
155328	ACS13615386	Pauli limit = 2.76 T. Hc2(0) = 0.59 T for R(0.9Rn) definition and GL fitting. lattice term in SP (beta) = 3.00 mJ/mol.K4. DOS = 65 /eV.fu.	Eu3Bi2S4F4	Eu3Bi2S4F4	Eu	3	Bi	2	S	4	F	4																1	2014					myu-B/Eu	7.28		2.3	6.6413																	A2B3C4D4	2		I4/mmm	139	A	4.077		32.433											Eu-3244	K	1.4						1.4																				T	R(onset), GL fitting	2.34																																		mJ/mol.K2	159	SP	203	SP																																		EuS,EuF2(3N),Bi2S3(5N)		solid state reaction. mixture - sealed in evacuatedd quartz ampule - SIN(1123K, 35h)					Anomalous Eu Valence State and Superconductivity in Undoped Eu3Bi2S4F4			Department of Physics, State Key Lab of Silicon Materials and Center of Electron Microscope, Zhejiang University, Hangzhou 310027, China	J.Am.Chem.Soc., 136(2014)15386	Hui-Fei Zhai,Pan Zhang,Si-Qi Wu,Chao-Yang He,Zhang-Tu Tang,Hao Jiang,Yun-Lei Sun,Jin-Ke Bao,Israel Nowik,Israel Felner,Yue-Wu Zeng,Yu-Ke Li,Xiao-Feng Xu,Qian Tao,Zhu-An Xu,Guang-Han Cao		
155329	APL103142601	As-prepared sample. compositions: Ca:Fe:As:F:H:O = 1.00:1.00:0.95:0.73:0.24:0.07. not SC. R(T) anomaly around 100K.	CaFeAs(F,H)	Ca1Fe1As1F0.8H0.2	Ca	1	Fe	1	As	1	F	0.8	H	0.2															2013																										ABCD	2	oxypnictide																	ZrCuSiAs-type. Fe-1111	K					2																																																																																																CaAs,Fe2As,CaH2		mixture - in BN capsule - added LiAlH4 for supplementary H source - heat(1273 K, 1h, P=2GPa)					Superconductivity in 1111-type CaFeAsF1-xHx induced by selective hydrogen elimination			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259-S2-13 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Appl.Phys.Lett., 103(2013)142601	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155330	APL103142601	As-annealed (553K,72h,in He-flow) sample. compositions: Ca:Fe:As:F:H:O = 0.99:1.00:0.96:0.69:0.03:0.06. Annealing results in the formation of F vacancy.	CaFeAs(F,H)	Ca1Fe1As1F0.8H0.2	Ca	1	Fe	1	As	1	F	0.8	H	0.2															2013																										ABCD	2	oxypnictide			A	3.896		8.669											ZrCuSiAs-type. Fe-1111	K				29			29										31																																																																																				CaAs,Fe2As,CaH2		mixture - in BN capsule - added LiAlH4 for supplementary H source - heat(1273 K, 1h, P=2GPa)					Superconductivity in 1111-type CaFeAsF1-xHx induced by selective hydrogen elimination			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259-S2-13 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Appl.Phys.Lett., 103(2013)142601	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155331	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. La-content = 25 % (x=0.25) by EDX.	(Ca,La)FeAs2	Ca0.85La0.15Fe1As2	Ca	0.85	La	0.15	Fe	1	As	2																3	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		16.2	22.7				16.2																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155332	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Ce-content = 26 % (x=0.26) by EDX.	(Ca,Ce)FeAs2	Ca0.85Ce0.15Fe1As2	Ca	0.85	Ce	0.15	Fe	1	As	2																3	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K																																																																																																					FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155333	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Pr-content not given	(Ca,Pr)FeAs2	Ca0.85Pr0.15Fe1As2	Ca	0.85	Pr	0.15	Fe	1	As	2																3	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		21	24.6	24.5			21																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155334	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Nd-content = 23 % (x=0.23) by EDX.	(Ca,Nd)FeAs2	Ca0.85Nd0.15Fe1As2	Ca	0.85	Nd	0.15	Fe	1	As	2																3	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		14	17.9		2		14																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155335	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Sm-content = 11 % (x=0.11) by EDX.	(Ca,Sm)FeAs2	Ca0.85Sm0.15Fe1As2	Ca	0.85	Sm	0.15	Fe	1	As	2																1	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		17.6	23.2	13.2			17.6																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155336	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Eu-content = 17 % (x=0.17) by EDX.	(Ca,Eu)FeAs2	Ca0.85Eu0.15Fe1As2	Ca	0.85	Eu	0.15	Fe	1	As	2																3	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		12.2	13.2	11.9			12.2																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155337	APE007073102	x = 0.15(in Ca1-xRxFeAs2) is the best for SC. Gd-content not measured by EDX	(Ca,Gd)FeAs2	Ca0.85Gd0.15Fe1As2	Ca	0.85	Gd	0.15	Fe	1	As	2																1	2014																										ABC2		Fe-112	P2<1>/m																Fe-112 type.	K		19.5	22.8	11.6			19.5																																																																																														FeAs(3N),RAs(3N),Ca(2N),As(4N)		Powder mixture - pelletize - react(1000C,1h, P=2 GPa, in BN crucible)					Synthesis and physical properties of Ca1-xRExFeAs2 with RE = La-Gd			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys.Exp., 7(2014)073102	Alberto Sala,Hiroyuki Yakita,Hiraku Ogino,Tomoyuki Okada,Akiyasu Yamamoto,Kohji Kishio,Shigeyuki Ishida,Akira Iyo,Hiroshi Eisaki,Masaya Fujioka,Yoshihiko Takano,Marina Putti,Jun-ichi Shimoyama		
155338	CEM1960579	(dC/gamma*Tc) = 1.1. e-ph = 1.09.  GL parameter = 25.	delta-MoC0.681	C0.681Mo1	C	0.681	Mo	1																					2012									8.907																	AB	1		Fm-3m	225	A	4.26647														K		12		12			12											Oe	M-H curve	310							T	SP, WHH	11.2							T/K	SP	1.45			MHC155338		A	from Hc2	52.2			A	from Hc1	1320					2.95	14							mJ/mol.K2	5	SP																																				Mo(4N),C		powder mixture - (flat belt-type high P apparatus) - heat(2000C,10-30 min, P=6 GPa) - Q to RT					Superconducting and structural properties of delta-MoC0.681 cubic molybdenum carbide phase			Graduate School of Chemical Science sand Engineering, Hokkaido University, Sapporo, Hokkaido0 60-0810, Japan	J.Solid State Chem., 196(2012)579	C.I. Sathish,Yanfeng Guo,Xia Wang,Yoshihiro Tsujimoto,Jun  Li,Shoubao Zhang,Yoshitaka Matsushita,Youguo Shi,Huanfang Tian,Huaixin Yang,Jianqi Li,Kazunari Yamaura		
155339	CEM2190168	target material = La(O0.5F0.5)BiSe2. resultant  = La(O0.82F0.18)BiSe2 by EDX.	La(O,F)BiSe2	La1Bi1Se2F0.5O0.5	La	1	Bi	1	Se	2	F	0.5													O	0.5		3	2014																										ABCD2		CeOBiS2	P4/nmm	192	A	4.1408		14.1096												K	3.2	3.48	3.6	3.6			3.48																																																																							mOhm.cm							0.136			3.6													La(3N),Bi2O3,Se,BiF3,Bi,Bi2Se3		CsCl-flux method. mixture(La:Bi2O3:BiF3:Bi:Bi2Se3:Se = 6:1:1:1:1:3) - sealed in quartz tube - heat(880C,10h) heat(900C,10h) - cool to 650C(1C/h) - FC to RT					First single crystal growth and structural analysis of superconducting  layered bismuth oxyselenide; La(O,F)BiSe2			National Institute for Materials Science, 1-2-1Sengen, Tsukuba, Ibaraki 305-0047, Japan	J.Solid State Chem., 219(2014)168	Masashi Tanaka,Masanori Nagao,Yoshitaka Matsushita,Masaya Fujioka,Saleem J. Denholme,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155340	CHM0262155	molar volume: SrAuSi3:SrAu2Si2 = 0.823:0.177. VOLS nearly equal to volume of SrAuSi3. (dC/gamma*Tc)=1.92. (dC<el>/Tc) = 11.6 mJ/mol.K2.GL = 11. C<el>(T) has a kink at 1.3K. Hc(0) = 0.014T.	SrAuSi3	Sr1Au1Si3	Sr	1	Au	1	Si	3																			2014									6.3346																	ABC3		BaNiSn3	I4mm	107	A	4.409		9.9475												K	1.61	1.65	1.74	1.6			1.65										75										T	R(mid), Linear approx.	0.22												MHC155340		A	from Hc2	390			A		4400										MSP155340			mJ/mol.K2	6	SP	410	SP											mOhm.cm							0.1			2													SrSi(3N),Au(4N),Si(4N)		mixture - pellet - high-P(h-BN) - heat(1500C,1h, P= 6 GPa) - Q to RT					SrAuSi3: A Noncentrosymmetric Superconductor			Superconducting Properties Unit, National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Chem.Materials, 26(2014)2155	Masaaki Isobe,Hiroyuki Yoshida,Koji Kimoto,Masao Arai,Eiji Takayama-Muromachi		
155341	CHM0231558	K-intercalated.	K0.08ZrNCl	K0.08Zr1N1Cl1	K	0.08	Zr	1	N	1	Cl	1																	2011																													P3[-]m	164	A															K				13			13																																																																																																					Preparation and Superconductivity of New Stage and Polytypic Phases in Potassium-Intercalated Zirconium Nitride Chloride(KxZrNCl)			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Chem.Materials, 23(2011)1558	Zhanfeng Zheng,Shoji Yamanaka		
155342	CHM0231558	M = THF. M-content not given. co-intercalated (K, and M) sample	K0.08(THF)yZrNCl	K0.08M1Zr1N1Cl1	K	0.08	M	1	Zr	1	N	1	Cl	1															2011																													P3[-]m	164	A	3.6143		13.1449												K				15			15																																																																																																					Preparation and Superconductivity of New Stage and Polytypic Phases in Potassium-Intercalated Zirconium Nitride Chloride(KxZrNCl)			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Chem.Materials, 23(2011)1558	Zhanfeng Zheng,Shoji Yamanaka		
155343	CHM0231558	K-intercalated.	K0.26ZrNCl	K0.26Zr1N1Cl1	K	0.26	Zr	1	N	1	Cl	1																	2011																													P3[-]m	164	A	3.6295		10.965												K				11.5			11.5																																																																																																					Preparation and Superconductivity of New Stage and Polytypic Phases in Potassium-Intercalated Zirconium Nitride Chloride(KxZrNCl)			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Chem.Materials, 23(2011)1558	Zhanfeng Zheng,Shoji Yamanaka		
155344	CHM0231558	M = PC (propylene carbonate).  M-content not given. co-intercalated (K, and M) sample	K0.26(PC)ZrNCl	K0.26M1Zr1N1Cl1	K	0.26	M	1	Zr	1	N	1	Cl	1															2011																													P3[-]m	164	A	3.625		21.83												K				11.5			11.5																																																																																																					Preparation and Superconductivity of New Stage and Polytypic Phases in Potassium-Intercalated Zirconium Nitride Chloride(KxZrNCl)			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Chem.Materials, 23(2011)1558	Zhanfeng Zheng,Shoji Yamanaka		
155345	EPL09927002	compositions: Nb:Si:As = 32.7:34.4:32.9 by EPMA. Tc = 7.6 K  defined as (dC/2). (dC<el>/gamma*Tc) = 1.95. lattice term in SP (beta) = 0.178 mJ/mol.K4. e-ph = 0.66.	NbSiAs	Nb1Si1As1	Nb	1	Si	1	As	1																		1	2012																										ABC		PbFCl	P4/nmm	129	A	3.4914		7.9005												K			8.2				8.2										40										T	M-H curve				0.88			2																												mJ/mol.K2	8.8	SP	324	SP																																		Nb(4N),Si(5N),As(4N)		mixture - sealed in silica tube - heat(1023K, 277h)-reground - heat again					Superconductivity in a PbFCl-type pnictide: NbSiAs			Materials and Structures Laboratory, Tokyo Institute of Technology - 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Europhys.Lett., 99(2012)27002	Gihun Ryu,Sung Wng Kim,Hiroshi Mizoguchi,Satoru Matsuishi,Hideo Hosono		
155346	EPL10417003	SC from impurity phases. RRR = 4.6. DOS = 15.03 states/eV.fu	LaRu2B2	La1Ru2B2	La	1	Ru	2	B	2																		1	2013																										AB2C2		F222			A	6.4401	9.2222	10.1574												K					1.8																																																										mJ/mol.K2	6.8	SP	343	SP																																				arc-melting					Superconductivity and physical properties of strongly electron correlated compounds LanRu3n-1B2n (n = 1, 2, and 3)			Frontier Research Center, Tokyo Institute of Technology - Yokohama 226-8503, Japan	Europhys.Lett., 104(2013)17003	Hechang Lei,Hideo Hosono		
155347	EPL10417003	SC from impurity phases. RRR = 7.1. DOS = 35.26 states/eV.fu	La2Ru5B4	La2Ru5B4	La	2	Ru	5	B	4																		1	2013																										A2B4C5		Fmmm			A	5.6259	9.7464	11.562												K					1.8																																																										mJ/mol.K2	6.9	SP	369	SP																																				arc-melting					Superconductivity and physical properties of strongly electron correlated compounds LanRu3n-1B2n (n = 1, 2, and 3)			Frontier Research Center, Tokyo Institute of Technology - Yokohama 226-8503, Japan	Europhys.Lett., 104(2013)17003	Hechang Lei,Hideo Hosono		
155348	EPL10417003	RRR = 1.8. DOS = 68.49 states/eV.fu. Tc = 3.21 K from SP.  GL = 17.8. Hc(0) = 852 Oe, (dC/gamma*Tc) = 0.89. e-ph = 0.56 Hp = 6.1 T.	La3Ru8B6	La3Ru8B6	La	3	Ru	8	B	6																		1	2013																										A3B6C8		Fmmm			A	5.5678	9.8106	17.5181												K			3.31	3.15		0.37	3.15										100	Oe	M-H curve	100							T	RES(0.9Rn), WHH	2.15							T/K	RES(0.9Rn)	0.97			MHC155348		A	from Hc2	124			A	from Hc1	2210										MSP155348			mJ/mol.K2	48	SP	307	SP																																				arc-melting					Superconductivity and physical properties of strongly electron correlated compounds LanRu3n-1B2n (n = 1, 2, and 3)			Frontier Research Center, Tokyo Institute of Technology - Yokohama 226-8503, Japan	Europhys.Lett., 104(2013)17003	Hechang Lei,Hideo Hosono		
155349	INO0523953		Mg4AlSi3	Mg4Al1Si3	Mg	4	Al	1	Si	3																		3	2013																											2		P4/ncc	130	A	6.7225		13.515											tetragonal	K				5.2			5.2										40																																																																																						High-P-high-T synthesis (950-1000C, 5GPa) - cool to RT					Structural Characterization of Magnesium-Based Compounds Mg9Si5 and Mg4Si3Al (Superconductor) Synthesized under High Pressure and High Temperature Conditions			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)3953	Shidong Ji,,Motoharu Imai,Haikui Zhu,Shoji Yamanaka		
155350	INO0523953	Mg9-xAlxSi5 hexagonal phase  ( x < 0.4) not SC.	Mg9-xAlxSi5	Mg8.8Al0.2Si5	Mg	8.8	Al	0.2	Si	5																		3	2013																																													hexagonal	K					1.9																																																																																																		High-P-high-T synthesis (950-1000C, 5GPa) - cool to RT					Structural Characterization of Magnesium-Based Compounds Mg9Si5 and Mg4Si3Al (Superconductor) Synthesized under High Pressure and High Temperature Conditions			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)3953	Shidong Ji,,Motoharu Imai,Haikui Zhu,Shoji Yamanaka		
155351	INO0523953	Mg(Mg1-xAlx)Si,  ortho-phase (x > 0.5) is SC.	Mg(Mg1-xAlx)Si	Mg1.4Al0.6Si1	Mg	1.4	Al	0.6	Si	1																		3	2013																											3																		ortho	K				6			6																																																																																																High-P-high-T synthesis (950-1000C, 5GPa) - cool to RT					Structural Characterization of Magnesium-Based Compounds Mg9Si5 and Mg4Si3Al (Superconductor) Synthesized under High Pressure and High Temperature Conditions			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)3953	Shidong Ji,,Motoharu Imai,Haikui Zhu,Shoji Yamanaka		
155352	INO0526039		Ca(Al,Si)2	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2013																										AB2					A	7.8112													Laves phase	K				2.6			2.6	MTC155352									37	Oe	M-H curve				5			1.9	T	SUS, WHH	0.27							T/K	SUS	0.15			MHC155352																																																														High-P-high-T synthesis (1000C, 13 GPa)					High-Pressure Synthesis and Superconductivity of the Laves Phase Compound Ca(Al,Si)2 Composed of Truncated Tetrahedral Cages Ca@(Al,Si)12			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)6039	Masashi Tanaka,Shuai Zhang,Kei Inumaru,Shoji Yamanaka		
155353	INO0526039		Ca(Al,Si)2	Ca1Al0.74Si1.26	Ca	1	Al	0.74	Si	1.26																			2013																										AB2			Fd3[-]m	227	A	7.754													Laves phase	K				2.46			2.46	MTC155352									2.4																																																																																						High-P-high-T synthesis (1000C, 13 GPa)					High-Pressure Synthesis and Superconductivity of the Laves Phase Compound Ca(Al,Si)2 Composed of Truncated Tetrahedral Cages Ca@(Al,Si)12			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)6039	Masashi Tanaka,Shuai Zhang,Kei Inumaru,Shoji Yamanaka		
155354	JAC2570023		LaNiSb2	La1Ni1Sb2	La	1	Ni	1	Sb	2																		1	1997																										ABC2	2	ZrCuSi2	P4/nmm	129	A	4.415		9.9												K		1					1																																																								mJ/mol.K2	9.27	SP	336	SP																																				ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155355	JAC2570023	T(Rmax) = 5 K.	CeNiSb2	Ce1Ni1Sb2	Ce	1	Ni	1	Sb	2																		1	1997					myu-B/mol	2.54	-36																			ABC2	2	ZrCuSi2	P4/nmm	129	A	4.403		9.761												K					2																																																										mJ/mol.K2	500	SP																																						ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155356	JAC2570023		LaCuSb2	La1Cu1Sb2	La	1	Cu	1	Sb	2																		1	1997																										ABC2	2	ZrCuSi2	P4/nmm	129	A	4.363		10.317												K		0.9					0.9																																																								mJ/mol.K2	2.92	SP	151	SP																																				ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155357	JAC2570023	T(Rmax) = 5 K.	CeCuSb2	Ce1Cu1Sb2	Ce	1	Cu	1	Sb	2																		1	1997					myu-B/mol	2.56	-12	8																		ABC2	2	ZrCuSi2	P4/nmm	129	A	4.33		10.202												K					2																																																										mJ/mol.K2	94	SP																																						ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155358	JAC2570023		LaPdSb2	La1Pd1Sb2	La	1	Pd	1	Sb	2																		1	1997																										ABC2	2	ZrCuSi2	P4/nmm	129	A	4.522		9.982												K		2.7					2.7																																																								mJ/mol.K2	7.48	SP	227	SP																																				ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155359	JAC2570023	T(Rmax) = 50 K.	CePdSb2	Ce1Pd1Sb2	Ce	1	Pd	1	Sb	2																		1	1997					myu-B/mol	2.58	-66																			ABC2	2	ZrCuSi2	P4/nmm	129	A	4.486		9.879												K					2																																																										mJ/mol.K2	150	SP																																						ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155360	JAC2570023		LaAgSb2	La1Ag1Sb2	La	1	Ag	1	Sb	2																		1	1997																										ABC2	2	ZrCuSi2	P4/nmm	129	A	4.393		10.855												K					2																																																										mJ/mol.K2	2.62	SP	249	SP																																				ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155361	JAC2570023	T(Rmax) = 15 K.	CeAgSb2	Ce1Ag1Sb2	Ce	1	Ag	1	Sb	2																		1	1997					myu-B/mol	2.47	-6	10																		ABC2	2	ZrCuSi2	P4/nmm	129	A	4.37		10.714												K					2																																																										mJ/mol.K2	75	SP																																						ar-arc-melting with excess Sb (about 3 %) - ANN(800C,1w, in evacuated quartz tube)					Magnetic and transport properties of dense Kondo systems, CeTSb 2 (T=Ni, Cu, Pd and Ag)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106, Japan	J.Alloys Compd., 257(1997)23	Yuji Muro,Naoya Takeda,Masayasu Ishikawa		
155362	JAC6130370	Hc2(0) = 0.402T, (dHc2/dT) = 0.52 T/K, [cohere] = 137 A for RES(0.9Rn), WHH definition. (dC/gamma*Tc) = 1.17 using Tc(SP) = 0.90 K. e-ph = 0.45. DOS = 0.97 states/eV.fu.	LaPd2As2	La1Pd2As2	La	1	Pd	2	As	2																			2014																										AB2C2		ThCr2Si2	I4/mmm		A	4.3027		10.268											collapsed tetragonal ( stable)	K	0.75	0.97	1.13				0.97										40										T	RES(0.5Rn),Linear approx.	0.334							T/K	RES(0.5Rn)	0.34			MHC155362		A	from Hc2	421																		mJ/mol.K2	5.56	SP	261	SP																																				mixture (in N2 atmosphere) - pellet - heat(850C,20h) - reground - pellet - heat(850C,40h) cool to RT					Superconductivity in LaPd2As2 with a collapsed 122 structure			Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Kyoto 615-8510, Japan	J.Alloys Compd., 613(2014)370	Subodh Ganesanpotti,Takeshi Yajima,Kousuke Nakano,Yasumasa Nozaki,Takafumi Yamamoto,Cedric Tassel,Yoji Kobayashi,Hiroshi Kageyama		
155363	JAP112073923	Tm(FM) = 70 K. ferromag.  (Tm/Tc) = 7. kappa(GL) = 4.1. weak ferro-(not conventional ferro-)	KxMoO2	K0.05Mo1O2-z	K	0.05	Mo	1																	O	2-z			2012							70																				4		P2<1>/c																	K				9.5			9.5										0.4	Oe	M-H curve				1170			2	T	M-H curve				1			2																																																																		Mo,MoO3,K2MoO4		mixture - pellet - in quartz tube - heat(400C,1d) - heat(700C,3d)					Superconductivity and magnetism in the KxMoO2-d			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP 12602-810, Brazil	J.Appl.Phys., 112(2012)073923	L.M.Alves,C.A.M.dos Santos,S.S.Benaion,A.J.S.Machado,B.S.de Lima,J.J.Neumeier,M.D.R.Marques,J.Albino Aguiar,R.J.O.Mossanek,M.Abbate		
155364	JAP112073923	Tm(FM) = 70 K. ferromag.  (Tm/Tc) = 18	KxMoO2	K0.3Mo1O2-z	K	0.3	Mo	1																	O	2-z			2012							70																				4		P2<1>/c																	K			4	4			4	MTC155364									1																																																																																				Mo,MoO3,K2MoO4		mixture - pellet - in quartz tube - heat(400C,1d) - heat(700C,3d)					Superconductivity and magnetism in the KxMoO2-d			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP 12602-810, Brazil	J.Appl.Phys., 112(2012)073923	L.M.Alves,C.A.M.dos Santos,S.S.Benaion,A.J.S.Machado,B.S.de Lima,J.J.Neumeier,M.D.R.Marques,J.Albino Aguiar,R.J.O.Mossanek,M.Abbate		
155365	JMC02210752	M = EDA (ethylene diamine). sample prepared by reaction (75 C, 10 days)	MxTiNCl	M0.23Ti1N1Cl1	M	0.23	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.999	3.264	22.23											M-intercalated TiNCl structure	K				10.5			10.5										16.3																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155366	JMC02210752	M = PDA (propylene diamine). sample prepared by reaction (75 C, 5 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Immm		A	3.975	3.274	23.34											M-intercalated TiNCl structure	K				3.8			3.8										0.1																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155367	JMC02210752	M = TMDA . sample prepared by reaction (75 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.97	3.2761	23.349											M-intercalated TiNCl structure	K				6.8			6.8										3.5																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155368	JMC02210752	M = PMDA  sample prepared by reaction (75 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Immm		A	4.0138	3.269	23.283											M-intercalated TiNCl structure	K				10.5			10.5										5.4																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155369	JMC02210752	M = HMDA (heptamethylene diamine). sample prepared by reaction (75 C, 15 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.982	3.28	23.34											M-intercalated TiNCl structure	K				15.5			15.5										17.4																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155370	JMC02210752	M = HPMDA . sample prepared by reaction (150 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Immm		A	3.98	3.276	24.16											M-intercalated TiNCl structure	K				7			7										1.6																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155371	JMC02210752	M = OMDA . sample prepared by reaction (150 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.972	3.271	23.66											M-intercalated TiNCl structure	K				15.2			15.2										20.7																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155372	JMC02210752	M = NMDA (nonamethylene diamine) . sample prepared by reaction (150 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Immm		A	3.981	3.275	24.14											M-intercalated TiNCl structure	K				15.5			15.5										6.5																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155373	JMC02210752	M = DMDA (decaamethylene diamine) . sample prepared by reaction (200 C, 15 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.98	3.274	24.59											M-intercalated TiNCl structure	K				17.1			17.1										54.1																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155374	JMC02210752	M = UDMDA . sample prepared by reaction (200 C, 15 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Immm		A	3.979	3.286	24.63											M-intercalated TiNCl structure	K				16			16										10.6																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155375	JMC02210752	M = DDMDA ( dodecamethylene diamine). sample prepared by reaction (150 C, 10 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.976	3.247	24.72											M-intercalated TiNCl structure	K				16.4			16.4										13.9																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155376	JMC02210752	M = pyridine . sample prepared by reaction (250 C, 1 days). M-content x not given.	MxTiNCl	M1Ti1N1Cl1	M	1	Ti	1	N	1	Cl	1																	2012																													Bmmb		A	3.9787	3.283	17.014											M-intercalated TiNCl structure	K				8.6			8.6										18.8																																																																																						mixed(TiNCl + various alkylene diamine: H2N-(cH2)n-NH2 (3=<n=<12) )  - heat(50-200C, 5-15 days, in Pyrex(vac) )					Preparation and superconductivity of intercalation compounds of TiNCl with aliphatic amines			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.	J.Mater.Chem., 22(2012)10752	Shoji Yamanaka,Keita Umemoto,Zhanfeng Zheng,Yuta Suzuki,Hiroshi Matsui,Naoki Toyota,Kei Inumaru		
155377	JPCM026215702	impurity phase = Bi2Se3(25 wt %)	La(O,F)BiSe2	La1Bi1Se2F0.5O0.5	La	1	Bi	1	Se	2	F	0.5													O	0.5			2014																												ZrCuSiAs	P4/nmm		A	4.15941		14.01567												K			2.7	2.6			2.6										70	Oe	M-H curve				5			1.8	T	M-H curve				0.06			1.8																																											mOhm.cm							0.12			4													La2O3,LaF3,Se		solid state reaction. mixture - pellet - preheat(800C,15h,in quartz(vac)) - reground - pellet - heat(800C,48h) - cool to 300C - Q to RT in air					Superconductivity in a new layered bismuth oxyselenide: LaO0.5F0.5BiSe2			Faculty of Chemistry, Warsaw University of Technology, Noakowskiego 3, 00-664 Warsaw, Poland	J.Phys.:Condens.Matter, 26(2014)215702	A Krzton-Maziopa,Z Guguchia2,,E Pomjakushina,V Pomjakushin,R Khasanov,H Luetkens,P K Biswas,A Amato,H Keller,K Conder		
155378	JPCM026215702	not SC	La(O,F)BiTe2	La1Bi1Te2F0.5O0.5	La	1	Bi	1	Te	2	F	0.5													O	0.5			2014																												ZrCuSiAs																		K					1.7																																																																																																La2O3,LaF3,Se		solid state reaction. mixture - pellet - preheat(800C,15h,in quartz(vac)) - reground - pellet - heat(800C,48h) - cool to 300C - Q to RT in air					Superconductivity in a new layered bismuth oxyselenide: LaO0.5F0.5BiSe2			Faculty of Chemistry, Warsaw University of Technology, Noakowskiego 3, 00-664 Warsaw, Poland	J.Phys.:Condens.Matter, 26(2014)215702	A Krzton-Maziopa,Z Guguchia2,,E Pomjakushina,V Pomjakushin,R Khasanov,H Luetkens,P K Biswas,A Amato,H Keller,K Conder		
155379	JPCM026215702	not SC	La(O,F)SbS2	La1Sb1S2F0.5O0.5	La	1	Sb	1	S	2	F	0.5													O	0.5			2014																												ZrCuSiAs																		K					1.7																																																																																																La2O3,LaF3,Se		solid state reaction. mixture - pellet - preheat(800C,15h,in quartz(vac)) - reground - pellet - heat(800C,48h) - cool to 300C - Q to RT in air					Superconductivity in a new layered bismuth oxyselenide: LaO0.5F0.5BiSe2			Faculty of Chemistry, Warsaw University of Technology, Noakowskiego 3, 00-664 Warsaw, Poland	J.Phys.:Condens.Matter, 26(2014)215702	A Krzton-Maziopa,Z Guguchia2,,E Pomjakushina,V Pomjakushin,R Khasanov,H Luetkens,P K Biswas,A Amato,H Keller,K Conder		
155380	JPCM023464204	Two AFM transition, 196 K, and 20 K corresponding to Fe- and Eu- order, respectively.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		1	2011								196																		AB2C2		ThCr2Si2			A	3.9122		12.1315												K					2																																																																																																EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155381	JPCM023464204		EuFe2(As,P)2	Eu1Fe1.8As2P0.2	Eu	1	Fe	1.8	As	2	P	0.2																1	2011								153																		AB2C2		ThCr2Si2			A	3.9067		12.0532												K					2																																																																																																EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155382	JPCM023464204	SC coexists with FM order of Eu.	EuFe2(As,P)2	Eu1Fe1.6As2P0.4	Eu	1	Fe	1.6	As	2	P	0.4																1	2011								34																		AB2C2		ThCr2Si2			A	3.8981		11.916												K			23.5				23.5																																																																																														EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155383	JPCM023464204	SC coexists with FM order of Eu.	EuFe2(As,P)2	Eu1Fe1.4As2P0.6	Eu	1	Fe	1.4	As	2	P	0.6																1	2011																										AB2C2		ThCr2Si2			A	3.8898		11.916												K			28.7				28.7	MPH155383																																																																																													EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155384	JPCM023464204	SC coexists with FM order of Eu.	EuFe2(As,P)2	Eu1Fe1.2As2P0.8	Eu	1	Fe	1.2	As	2	P	0.8																1	2011							19.7																			AB2C2		ThCr2Si2			A	3.8808		11.7569												K			21.5				21.5																																																																																														EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155385	JPCM023464204		EuFe2(As,P)2	Eu1Fe1As2P1	Eu	1	Fe	1	As	2	P	1																1	2011							21.8																			AB2C2		ThCr2Si2			A	3.8704		11.686												K					2																																																																																																EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155386	JPCM023464204		EuFe2(As,P)2	Eu1Fe0.5As2P1.5	Eu	1	Fe	0.5	As	2	P	1.5																1	2011							25.1																			AB2C2		ThCr2Si2			A	3.8173		11.4451												K					2																																																																																																EuAs,Fe2As,Eu2P		mixture - pellet - ANN(1273K,20h, in silica tube(vac))					Superconductivity and ferromagnetism in EuFe2(As1-xPx)2			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.:Condens.Matter, 23(2011)464204	Guanghan Cao,Shenggao Xu,Zhi Ren,Shuai Jiang,Chunmu Feng,Zhu'an Xu		
155387	JPCM025265701	T<SDW/STR> = 196 K. Tn(Eu) = 19 K.	Eu(Fe,Ir)2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		1	2013								19																		AB2C2		ThCr2Si2	I4/mmm		A	3.9113		12.136												K					2																																																																																																Eu(3N),Fe(5N),As(5N)		solid state reaction					Reentrant superconductivity in Eu(Fe1-xIrx)2As2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.:Condens.Matter, 25(2013)265701	U B Paramanik,Debarchan Das,R Prasad,Z Hossain		
155388	JPCM025265701	T<SDW/STR> = 170	Eu(Fe,Ir)2As2	Eu1Fe1.9Ir0.1As2	Eu	1	Fe	1.9	Ir	0.1	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.9163		12.122												K					2																																																																																																Eu(3N),Fe(5N),As(5N)		solid state reaction					Reentrant superconductivity in Eu(Fe1-xIrx)2As2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.:Condens.Matter, 25(2013)265701	U B Paramanik,Debarchan Das,R Prasad,Z Hossain		
155389	JPCM025265701	T<SDW/STR> = 90. Tm(FM) = 15K  reentrant behavior in R(T)	Eu(Fe,Ir)2As2	Eu1Fe1.78Ir0.22As2	Eu	1	Fe	1.78	Ir	0.22	As	2																1	2013							15																			AB2C2		ThCr2Si2	I4/mmm		A	3.9257		12.079												K			21				21																																																																																														Eu(3N),Fe(5N),As(5N)		solid state reaction					Reentrant superconductivity in Eu(Fe1-xIrx)2As2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.:Condens.Matter, 25(2013)265701	U B Paramanik,Debarchan Das,R Prasad,Z Hossain		
155390	JPCM025265701	Tm(FM) = 8.94. reentrant behavior in R(T)	Eu(Fe,Ir)2As2	Eu1Fe1.72Ir0.28As2	Eu	1	Fe	1.72	Ir	0.28	As	2																1	2013	emu/mol	0.000186	emu.K/mol	8.23	myu-B/mol	8.1	22.8																			AB2C2		ThCr2Si2	I4/mmm		A	3.9328		12.056												K			21.6				21.6																				T	RES(0.9Rn), WHH	15							T/K	RES(0.9Rn)	0.95			MHC155390																																																												Eu(3N),Fe(5N),As(5N)		solid state reaction					Reentrant superconductivity in Eu(Fe1-xIrx)2As2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.:Condens.Matter, 25(2013)265701	U B Paramanik,Debarchan Das,R Prasad,Z Hossain		
155391	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.80. compositions of O & F by EPMA.	LaFeAs(O,H)	La1Fe1As1F0.08O0.9	La	1	Fe	1	As	1	F	0.08													O		0.9		2014																										ABCD	2	oxypnictide			A	4.0224		8.7136											Fe-1111	K			28.4	25.9			25.9										22.2																																																													mOhm.cm							0.134							cm3/C						MRH155391			LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155392	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 2.17. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.991Zn0.009As1F0.08O0.9	La	1	Fe	0.991	Zn	0.009	As	1	F	0.08											O		0.9		2014																										ABCD	2	oxypnictide			A	4.0291		8.7231											Fe-1111	K			20.4	15.6			15.6	MTC155392									9.2																																																													mOhm.cm							1.39							cm3/C						MRH155391			LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155393	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.92. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.985Zn0.015As1F0.08O0.9	La	1	Fe	0.985	Zn	0.015	As	1	F	0.08											O		0.9		2014																										ABCD	2	oxypnictide			A	4.0242		8.7189											Fe-1111	K			11.2	0.2			0.2										1																																																													mOhm.cm							1.56																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155394	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 2.15. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.973Zn0.027As1F0.08O0.9	La	1	Fe	0.973	Zn	0.027	As	1	F	0.08											O		0.9		2014																										ABCD	2	oxypnictide			A	4.0258		8.7278											Fe-1111	K			8.6	0			0										1																																																													mOhm.cm							2.76																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155395	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 2.09. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.959Zn0.041As1F0.08O0.9	La	1	Fe	0.959	Zn	0.041	As	1	F	0.08											O		0.9		2014																										ABCD	2	oxypnictide			A	4.0277		8.7315											Fe-1111	K					2																																																																									mOhm.cm							1.33																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155396	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.20. compositions of O & F by EPMA.	LaFeAs(O,H)	La1Fe1As1F0.28O0.68	La	1	Fe	1	As	1	F	0.28													O		0.68		2014																										ABCD	2	oxypnictide			A	3.8044		8.6933											Fe-1111	K			36.5	33.5			33.5										27.2																																																													mOhm.cm							0.202							cm3/C						MRH155396			LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155397	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.12. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.982Zn0.018As1F0.28O0.68	La	1	Fe	0.982	Zn	0.018	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	3.8298		8.6998											Fe-1111	K			21.1	19.6			19.6	MTC155397									12.7																																																													mOhm.cm							0.344							cm3/C						MRH155396			LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155398	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.18. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.973Zn0.027As1F0.28O0.68	La	1	Fe	0.973	Zn	0.027	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	3.8224		8.7059											Fe-1111	K			16.8	12.2			12.2										5																																																													mOhm.cm							0.825																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155399	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.17. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.951Zn0.049As1F0.28O0.68	La	1	Fe	0.951	Zn	0.049	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	3.8835		8.7146											Fe-1111	K			10.3	1			1										1																																																													mOhm.cm							1																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155400	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.15. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.918Zn0.082As1F0.28O0.68	La	1	Fe	0.918	Zn	0.082	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	3.9331		8.7193											Fe-1111	K			8.2				8.2																																																																							mOhm.cm							2.91																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155401	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.13. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.905Zn0.095As1F0.28O0.68	La	1	Fe	0.905	Zn	0.095	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	3.9331		8.7256											Fe-1111	K			3.5				3.5																																																																							mOhm.cm							1.48																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155402	JPCM026435702	TCFIG shows Tc(SUS). R(T)-exponent = 1.08. compositions of O & F by EPMA.	La(Fe,Zn)As(O,H)	La1Fe0.887Zn0.113As1F0.28O0.68	La	1	Fe	0.887	Zn	0.113	As	1	F	0.28											O		0.68		2014																										ABCD	2	oxypnictide			A	4.0561		8.7331											Fe-1111	K					2																																																																									mOhm.cm							2.97																LaAs,Fe2As,FeAs,La2O3,LaH2,ZnO		solid state reaction using a belt-type high pressure anvil cell to prevent the evaporation of volatile Zn atom during the synthesis.					Comparison of impurity effect between two Tc domes in LaFeAsO1-xHx			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	J.Phys.:Condens.Matter, 26(2014)435702	Junichi Ishida,Soshi Iimura,Satoru Matsuishi,Hideo Hosono		
155403	JPS082085001	STR/electronic phase transition: T<STR> = 150 (heating), 107 (cooling) K.	Ir1-xRhxTe2	Ir0.9Rh0.1Te2	Ir	0.9	Rh	0.1	Te	2																		1	2013																										AB2		CdI2	P3[-]m1		A	3.9264		5.3969												K				2.61			2.61	MTC155403																																																																																															solid state reaction					Suppression of Structural Phase Transition in IrTe2 by Isovalent Rh Doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)085001	Kazutaka KUDO,Masakazu KOBAYASHI,Sunseng PYON,Minoru NOHARA		
155404	JPS082085001		Ir1-xRhxTe2	Ir0.85Rh0.15Te2	Ir	0.85	Rh	0.15	Te	2																		1	2013																										AB2		CdI2	P3[-]m1		A	3.9264		5.3959												K				2.39			2.39																																																																																																solid state reaction					Suppression of Structural Phase Transition in IrTe2 by Isovalent Rh Doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)085001	Kazutaka KUDO,Masakazu KOBAYASHI,Sunseng PYON,Minoru NOHARA		
155405	JPS082085001	RH-solubility limit at 0.3< x < 0.5.	Ir1-xRhxTe2	Ir0.7Rh0.3Te2	Ir	0.7	Rh	0.3	Te	2																		1	2013																										AB2		CdI2	P3[-]m1		A	3.9248		5.3955												K				2.09			2.09																																																																																																solid state reaction					Suppression of Structural Phase Transition in IrTe2 by Isovalent Rh Doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)085001	Kazutaka KUDO,Masakazu KOBAYASHI,Sunseng PYON,Minoru NOHARA		
155406	JPS082085001	not SC. STR/electronic phase transition: T<STR> = 261 (heating), 236 (cooling) K.	IrTe2	Ir1Te2	Ir	1	Te	2																				1	2013																										AB2		CdI2	P3[-]m1		A	3.9317		5.3966												K					2																																																																																																		solid state reaction					Suppression of Structural Phase Transition in IrTe2 by Isovalent Rh Doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)085001	Kazutaka KUDO,Masakazu KOBAYASHI,Sunseng PYON,Minoru NOHARA		
155407	JPS082085001	not SC. STR/electronic phase transition: T<STR> = 235 (heating), 200 (cooling) K.	Ir1-xRhxTe2	Ir0.96Rh0.04Te2	Ir	0.96	Rh	0.04	Te	2																		1	2013																										AB2		CdI2	P3[-]m1		A	3.9265		5.3945												K					2																																																																																																		solid state reaction					Suppression of Structural Phase Transition in IrTe2 by Isovalent Rh Doping			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 82(2013)085001	Kazutaka KUDO,Masakazu KOBAYASHI,Sunseng PYON,Minoru NOHARA		
155408	JPS083025001		(Ca,La)Fe(As,P)2	Ca0.84La0.16Fe1As1.99P0.01	Ca	0.84	La	0.16	Fe	1	As	1.99	P	0.01														3	2014																										ABC2					A	3.952	3.8727	10.3364											112-phase	K			43.8	41			41																																																																							mOhm.cm												0.482													mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155409	JPS083025001		(Ca,La)Fe(As,P)2	Ca0.82La0.18Fe1As1.99P0.01	Ca	0.82	La	0.18	Fe	1	As	1.99	P	0.01														3	2014																										ABC2					A	3.9492	3.8768	10.3442											112-phase	K			41	39			39	MTC155409																																																																						mOhm.cm												0.482													mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155410	JPS083025001		(Ca,La)Fe(As,P)2	Ca0.77La0.23Fe1As1.99P0.01	Ca	0.77	La	0.23	Fe	1	As	1.99	P	0.01														3	2014																										ABC2					A	3.9487	3.8785	10.3589											112-phase	K			30.1	28			28																																																																																																mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155411	JPS083025001		(Ca,La)FeAs2	Ca0.85La0.15Fe1As2	Ca	0.85	La	0.15	Fe	1	As	2																3	2014																										ABC2					A	3.9522	3.8765	10.346											112-phase	K			40	35			35																																																																							mOhm.cm												0.593													mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155412	JPS083025001		(Ca,La)FeAs2	Ca0.81La0.19Fe1As2	Ca	0.81	La	0.19	Fe	1	As	2																3	2014																										ABC2																			112-phase	K			45	28			28	MTC155412																																																																						mOhm.cm												0.378													mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155413	JPS083025001		(Ca,La)FeAs2	Ca0.78La0.22Fe1As2	Ca	0.78	La	0.22	Fe	1	As	2																3	2014																										ABC2					A	3.9492	3.8788	10.3456											112-phase	K			30	22			22																																																																																																mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155414	JPS083025001		(Ca,La)Fe(As,Sb)2	Ca0.85La0.15Fe1As1.98Sb0.02	Ca	0.85	La	0.15	Fe	1	As	1.98	Sb	0.02														3	2014																										ABC2					A	3.9502	3.8888	10.346											112-phase	K			44	43			43																																																																							mOhm.cm												0.354													mixture - (alumina crucible) - sealed in quartz tube - heat(700C,3h) - heat to 1100C (46C/h) - cool to 1050C (1.25 C/h) - FC to RT					Enhanced Superconductivity up to 43K by P/Sb Doping of Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 83(2014)025001	Kazutaka Kudo,Tasuku Mizukami,Yutaka Kitahama,Daisuke Mitsuoka,Keita Iba,Kazunori Fujimura,Naoki Nishimoto,Yuji Hiraoka,Minoru Nohara		
155415	MAT1407.3105	R not to zero down to 2K at ambient pressure. Hc2 data for P = 2.5 GPa.	Sr0.5Ce0.5FBiS2	Sr0.5Ce0.5F1Bi1S2	Sr	0.5	Ce	0.5	F	1	Bi	1	S	2														1	2014					Myu-B/f.u	2.97	-216.31	8																		ABCD2		CeOBiS2	P4/nmm		A	4.065		13.35											BiS2-layered SC	K			2.7				2.7	MTC155415																			T	RES(0.9Rn), WHH	13.8												MHC155415																																																														solid state reaction. mixture - pellet - sealed in quartz tube - SIN(650C,12h) (heating rate, 2C/min)					Appearance of bulk Superconductivity under Hydrostatic Pressure in Sr0.5RE0.5FBiS2 (RE=Ce, Nd, Pr and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	cond-mat/1407.3105	Rajveer Jha,Brajesh Tiwari,V.P.S. Awana		
155416	MAT1407.3105	P-induced SC. Hc2 data for P = 2.5 GPa.	Sr0.5Nd0.5FBiS2	Sr0.5Nd0.5F1Bi1S2	Sr	0.5	Nd	0.5	F	1	Bi	1	S	2														1	2014					Myu-B/f.u	2.87	-72.61																			ABCD2		CeOBiS2	P4/nmm		A	4.056		13.38											BiS2-layered SC	K					2			MTC155416																			T	RES(0.9Rn), WHH	11.6												MHC155416																																																														solid state reaction. mixture - pellet - sealed in quartz tube - SIN(650C,12h) (heating rate, 2C/min)					Appearance of bulk Superconductivity under Hydrostatic Pressure in Sr0.5RE0.5FBiS2 (RE=Ce, Nd, Pr and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	cond-mat/1407.3105	Rajveer Jha,Brajesh Tiwari,V.P.S. Awana		
155417	MAT1407.3105	P-induced SC. Hc2 data for P = 2.5 GPa.	Sr0.5Pr0.5FBiS2	Sr0.5Pr0.5F1Bi1S2	Sr	0.5	Pr	0.5	F	1	Bi	1	S	2														1	2014					Myu-B/f.u	3.14	-59.18																			ABCD2		CeOBiS2	P4/nmm		A	4.061		13.36											BiS2-layered SC	K					2			MTC155417																			T	RES(0.9Rn), WHH	13.5												MHC155417																																																														solid state reaction. mixture - pellet - sealed in quartz tube - SIN(650C,12h) (heating rate, 2C/min)					Appearance of bulk Superconductivity under Hydrostatic Pressure in Sr0.5RE0.5FBiS2 (RE=Ce, Nd, Pr and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	cond-mat/1407.3105	Rajveer Jha,Brajesh Tiwari,V.P.S. Awana		
155418	MAT1407.3105	P-induced SC. Hc2 data for P = 2.5 GPa.	Sr0.5Sm0.5FBiS2	Sr0.5Sm0.5F1Bi1S2	Sr	0.5	Sm	0.5	F	1	Bi	1	S	2														1	2014					Myu-B/f.u	3.24	-160.9																			ABCD2		CeOBiS2	P4/nmm		A	4.053		13.4											BiS2-layered SC	K					2			MTC155418																			T	RES(0.9Rn), WHH	14.5												MHC155418																																																														solid state reaction. mixture - pellet - sealed in quartz tube - SIN(650C,12h) (heating rate, 2C/min)					Appearance of bulk Superconductivity under Hydrostatic Pressure in Sr0.5RE0.5FBiS2 (RE=Ce, Nd, Pr and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi-110012, India	cond-mat/1407.3105	Rajveer Jha,Brajesh Tiwari,V.P.S. Awana		
155419	MAT1410.0061	ANN(800 C). (dC/gamma*Tc) = 0.21. Schottky type anomaly in low T.	(La,Sm)(O,F)BiS2	La0.9Sm0.1Bi1S2F0.5O0.5	La	0.9	Sm	0.1	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	4.056		13.333											BiS2-layered SC	K		2.93		2.64			2.93										7.3																																											MSP155419			mJ/mol.K2	8.9	SP																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155420	MAT1410.0061	ANN(800 C)	(La,Sm)(O,F)BiS2	La0.7Sm0.3Bi1S2F0.5O0.5	La	0.7	Sm	0.3	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	4.0317		13.369											BiS2-layered SC	K		3.11		2.85			3.11										26.7																																																																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155421	MAT1410.0061	ANN(800 C)	(La,Sm)(O,F)BiS2	La0.6Sm0.4Bi1S2F0.5O0.5	La	0.6	Sm	0.4	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	4.0264		13.38											BiS2-layered SC	K		3.25		3			3.25																																																																																																solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155422	MAT1410.0061	ANN(750 C)	(La,Sm)(O,F)BiS2	La0.5Sm0.5Bi1S2F0.5O0.5	La	0.5	Sm	0.5	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	4.0155		13.407											BiS2-layered SC	K		4.05		2.95			4.05	MTC155422									69.4																																																																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155423	MAT1410.0061	ANN(750 C)	(La,Sm)(O,F)BiS2	La0.4Sm0.6Bi1S2F0.5O0.5	La	0.4	Sm	0.6	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	4.0075		13.41											BiS2-layered SC	K		4.2		3.75			4.2										80																																																																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155424	MAT1410.0061	ANN(750 C)	(La,Sm)(O,F)BiS2	La0.3Sm0.7Bi1S2F0.5O0.5	La	0.3	Sm	0.7	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	3.9957		13.413											BiS2-layered SC	K		5.1		4.95			5.1										108																																																																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155425	MAT1410.0061	ANN(750 C). Sm solubility limit  X > 0.8. (dC/gamma*Tc) = 3.32	(La,Sm)(O,F)BiS2	La0.2Sm0.8Bi1S2F0.5O0.5	La	0.2	Sm	0.8	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2			A	3.3983		13.434											BiS2-layered SC	K		5.44		5.18			5.44	MTC155422									87																																											MSP155425			mJ/mol.K2	25																																							solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155426	MAT1410.0061	ANN(710 C)  Sm solubility limit  X > 0.8	(La,Sm)(O,F)BiS2	La0.1Sm0.9Bi1S2F0.5O0.5	La	0.1	Sm	0.9	Bi	1	S	2	F	0.5											O	0.5		1	2014																										ABCD2		CeOBiS2																	BiS2-layered SC	K		5.2		4.4			5.2										17.8																																																																																						solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155427	MAT1410.0061	lattice term in SP beta=0.655 mJ/mol.K4,  delta = 4.27 uJ/mol.K6.	LaOBiS2	La1Bi1S2O1	La	1	Bi	1	S	2															O	1		1	2014																										ABCD2		CeOBiS2																	BiS2-layered SC	K					1.1																																																																																																		solid state reaction. ANN(800C or 750 C) optimal condition					Enhancement of Superconductivity in La1-xSmxO0.5F0.5BiS2			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	cond-mat/1410.0061	Y. Fang,D. Yazici,B. D. White,M. B. Maple		
155428	NATCOM0053280	hole doping p = 0.078 estimated from Tc(p) in RRB073180505(2006).	YBa2Cu3Oz	Y1Ba2Cu3O6.45	Y	1	Ba	2	Cu	3															O	7-z	6.45	3	2014																												Y123																		K	45						45																				T	RES or Thermal conduc.	50																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155429	NATCOM0053280	hole doping p = 0.135 estimated from Tc(p) in RRB073180505(2006).	YBa2Cu3Oz	Y1Ba2Cu3O6.8	Y	1	Ba	2	Cu	3															O	7-z	6.8	3	2014																												Y123																		K	78.5						78.5																				T	RES or Thermal conduc.	35																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155430	NATCOM0053280	hole doping p = 0.180 estimated from Tc(p) in RRB073180505(2006).	YBa2Cu3Oz	Y1Ba2Cu4O6.998	Y	1	Ba	2	Cu	4															O	7-z	6.998	3	2014																												Y123																		K	90.5						90.5	MTC155430																			T	RES or Thermal conduc.	150												MHC155430																																																														Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155431	NATCOM0053280	hole doping p = 0.140 estimated from Tc(p) in RRB073180505(2006).	YBa2Cu4O8	Y1Ba2Cu3O8	Y	1	Ba	2	Cu	3															O	8		3	2014																												Y124																		K	80						80																				T	RES or Thermal conduc.	45																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155432	NATCOM0053280	hole doping p = 0.190 estimated from Ca-content.	Y(Ba,Ca)2Cu3Oz	Y1Ba1.972Ba0.028Cu3O7-z	Y	1	Ba	1.972	Ba	0.028	Cu	3													O	7-z		3	2014																												Y123																		K	87						87																				T	RES or Thermal conduc.	140																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155433	NATCOM0053280	hole doping p = 0.225 estimated using (Tc/Tcmax) = 1-82.6(p-0.16)^2 with Tcmax = 90 K.	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	2014																												Tl2201																		K	59						59																				T	RES or Thermal conduc.	63																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155434	NATCOM0053280	hole doping p = 0.248 estimated using (Tc/Tcmax) = 1-82.6(p-0.16)^2 with Tcmax = 90 K.	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	2014																												Tl2201																		K	33						33																				T	RES or Thermal conduc.	20																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155435	NATCOM0053280	hole doping p = 0.257 estimated using (Tc/Tcmax) = 1-82.6(p-0.16)^2 with Tcmax = 90 K.	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	2014																												Tl2201																		K	20						20																				T	RES or Thermal conduc.	14																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155436	NATCOM0053280	hole doping p = 0.260 estimated using (Tc/Tcmax) = 1-82.6(p-0.16)^2 with Tcmax = 90 K.	Tl2Ba2CuO6	Tl2Ba2Cu1O6	Tl	2	Ba	2	Cu	1															O	6		3	2014																												Tl2201																		K	15						15																				T	RES or Thermal conduc.	10																																																																										Flux growth method					Direct measurement of the upper critical field in cuprate superconductors			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1.	Nat.Commun., 5(2014)3280	G. Grissonnanche,O. Cyr-Choiniere,F. Laliberte,S. Rene de Cotret,A. Juneau-Fecteau,S. Dufour-Beausejour,M.-E. Delage,D. LeBoeuf,J. Chang,B.J. Ramshaw,D.A. Bonn,W.N. Hardy,R. Liang,S. Adachi,N.E. Hussey,B. Vignolle,C. Proust,M. Sutherland,S. Kramer,J.-H. Park		
155437	NATCOM0054756		Na0.65Fe1.93(Se,S)2	Na0.65Fe1.93Se2	Na	0.65	Fe	1.93	Se	2																		1	2014																												ThCr2Si2	I4/mmm		A	3.787		13.6678											Fe-122	K				37.5			37.5																																																																																														FeSe(3N8),Se(4N),S(4N)		mixture - alumina crucible - sealed in silica capsule - heat(1300K,30h) - ANN(673 K,50h) - FC to RT					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155438	NATCOM0054756		Na0.65Fe1.93(Se,S)2	Na0.65Fe1.93Se1.8S0.2	Na	0.65	Fe	1.93	Se	1.8	S	0.2																1	2014																												ThCr2Si2	I4/mmm		A	3.7797		13.5302											Fe-122	K				36			36	MTC155438																																																																																													FeSe(3N8),Se(4N),S(4N)		mixture - alumina crucible - sealed in silica capsule - heat(1300K,30h) - ANN(673 K,50h) - FC to RT					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155439	NATCOM0054756		Na0.65Fe1.93(Se,S)2	Na0.65Fe1.93Se1.6S0.4	Na	0.65	Fe	1.93	Se	1.6	S	0.4																1	2014																												ThCr2Si2	I4/mmm		A	3.7716		13.4365											Fe-122	K				32			32																																																																																														FeSe(3N8),Se(4N),S(4N)		mixture - alumina crucible - sealed in silica capsule - heat(1300K,30h) - ANN(673 K,50h) - FC to RT					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155440	NATCOM0054756		Na0.65Fe1.93(Se,S)2	Na0.65Fe1.93Se1.4S0.6	Na	0.65	Fe	1.93	Se	1.4	S	0.6																1	2014																												ThCr2Si2	I4/mmm		A	3.7598		13.2808											Fe-122. CaAl2Si2 for x > 0.3	K				25.1			25.1																																																																																														FeSe(3N8),Se(4N),S(4N)		mixture - alumina crucible - sealed in silica capsule - heat(1300K,30h) - ANN(673 K,50h) - FC to RT					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155441	NATCOM0054756	M = NH3 intercalated sample.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se2	Na	0.8	M	0.6	Fe	1.86	Se	2																1	2014																												ThCr2Si2	I4/mmm		A	3.799		17.4165											Fe-122	K				45.2			45.2																																																																																																Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155442	NATCOM0054756	M = NH3 intercalated sample.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se1.8S0.2	Na	0.8	M	0.6	Fe	1.86	Se	1.8	S	0.2														1	2014																												ThCr2Si2	I4/mmm		A	3.7907		17.2089											Fe-122	K				43.7			43.7	MTC155442																																																																																															Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155443	NATCOM0054756	M = NH3 intercalated sample.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se1.6S0.4	Na	0.8	M	0.6	Fe	1.86	Se	1.6	S	0.4														1	2014																												ThCr2Si2	I4/mmm		A	3.7848		17.0303											Fe-122	K				42.2			42.2																																																																																																Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155444	NATCOM0054756	M = NH3 intercalated sample.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se1.4S0.6	Na	0.8	M	0.6	Fe	1.86	Se	1.4	S	0.6														1	2014																												ThCr2Si2	I4/mmm		A	3.7752		16.9039											Fe-122	K				39.2			39.2																																																																																																Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155445	NATCOM0054756	M = NH3 intercalated sample.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se1.2S0.8	Na	0.8	M	0.6	Fe	1.86	Se	1.2	S	0.8														1	2014																												ThCr2Si2	I4/mmm		A	3.763		16.799											Fe-122	K				35.3			35.3																																																																																																Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155446	NATCOM0054756	M = NH3 intercalated sample. x = 0.5: hexagonal phase solubility limit.	Na0.80M0.6Fe1.86(Se,S)2	Na0.8M0.6Fe1.86Se1S1	Na	0.8	M	0.6	Fe	1.86	Se	1	S	1														1	2014																												ThCr2Si2	I4/mmm		A	3.7563		16.6896											Fe-122.	K				25.3			25.3																																																																																																Using (Na/NH3) concentration solution. After intercalated procedure, solutions were evaporated.					Superconductivity and phase instability of NH3-free Na-intercalated FeSe1-zSz			Frontier Research Center, Tokyo Institute of Technology, Yokohama 226-8503, Japan.	Nat.Commun., 5(2014)4756	Jiangang Guo,Hechang Lei,Fumitaka Hayashi,Hideo Hosono		
155447	NATM0070367	A15-type Cs3C60.  P-induced SC. Pcr = 4 kbar	Cs3C60	Cs3C60	Cs	3	C	60																					2008																		GPa		18.5						A3B60		fullerene																		K				38	0		38	MTC155447																																																																																															reaction of Cs metal or Cs6C60 in methylamine at -65C using a dual manifold high vacuum line. Warm to RT, solvent removed.					Bulk superconductivity at 38K in a molecular system			Department of Chemistry, University of Liverpool, Liverpool L69 7ZD, UK	Nat. Mater., 7(2008)367	ALEXEY Y. GANIN,YASUHIRO TAKABAYASHI,YAROSLAV Z. KHIMYAK,SERENA MARGADONNA,ANNA TAMAI,MATTHEW J. ROSSEINSKY,KOSMAS PRASSIDES		
155448	NATM0080305	Not SC. Structural transition (T to O) T<STR> = 158 K. Tc and Tn from muon-SR. T<STR> from XRD and SUS. Local moment = 171 mT at 0 K.	La(O,F)FeAs	La1Fe1As1O1	La	1	Fe	1	As	1															O	1			2009								134																		ABCD		oxypnictide																		K					0																																																																																																							The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155449	NATM0080305	Not SC. Structural transition (T to O) T<STR> = 150 K. .  Tc and Tn from muon-SR. T<STR> from XRD and SUS. Local moment = 171 mT at 0 K.	La(O,F)FeAs	La1Fe1As1F0.02O0.98	La	1	Fe	1	As	1	F	0.02													O	0.98			2009								131																		ABCD		oxypnictide																		K					0																																																																																																							The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155450	NATM0080305	Not SC. Structural transition (T to O) T<STR> = 145 K. Tc and Tn from muon-SR. T<STR> from XRD and SUS. Local moment = 164 mT at 0 K.	La(O,F)FeAs	La1Fe1As1F0.04O0.96	La	1	Fe	1	As	1	F	0.04													O	0.96			2009								120																		ABCD		oxypnictide																		K					0																																																																																																							The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155451	NATM0080305	Tc and Tn  from muon-SR.	La(O,F)FeAs	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95			2009																										ABCD		oxypnictide																		K		20					20																																									nm	muon-SR		396																																																									The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155452	NATM0080305	Tc and Tn  from muon-SR.	La(O,F)FeAs	La1Fe1As1F0.075O0.925	La	1	Fe	1	As	1	F	0.075													O	0.925			2009																										ABCD		oxypnictide																		K		21.2					21.2	MPH155452																																								nm	muon-SR		366																																																									The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155453	NATM0080305	Tc and Tn  from muon-SR.	La(O,F)FeAs	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9			2009																										ABCD		oxypnictide																		K		25.1					25.1	MPH155452																																								nm	muon-SR		254																																																									The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155454	NATM0080305	Tc and Tn  from muon-SR.	La(O,F)FeAs	La1Fe1As1F0.15O0.85	La	1	Fe	1	As	1	F	0.15													O	0.85			2009																										ABCD		oxypnictide																		K		10.5					10.5																																									nm	muon-SR		295																																																									The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155455	NATM0080305	Tc and Tn  from muon-SR.	La(O,F)FeAs	La1Fe1As1F0.2O0.8	La	1	Fe	1	As	1	F	0.2													O	0.8			2009																										ABCD		oxypnictide																		K		11.1					11.1																																									nm	muon-SR		289																																																									The electronic phase diagram of the LaO1-xFxFeAs superconductor			Laboratory for Muon-Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Nat. Mater., 8(2009)305	H. Luetkens,H.-H. Klauss,M. Kraken,F. J. Litterst,T. Dellmann,R. Klingeler,C. Hess,R. Khasanov,A. Amato,C. Baines,M. Kosmala,O. J. Schumann,M. Braden,J. Hamann-Borrero,N. Leps,A. Kondrat,G. Behr,J.Werner,B. Buchner		
155456	NATM0140325	absolute H content is 60 wt% in (Li0.8Fe0.2)OHFeSe. SC and AFM coexist. FM also observed by NPD.	(Li,Fe)OHFeSe	Li0.8Fe1.2Se1H1O1	Li	0.8	Fe	1.2	Se	1	H	1													O	1			2015								8.6																					I4/nmm	129	A	3.77871		9.1604												K				40			40										60																																																								uV/K	-6.27			MTP155456																								SeC(NH2)2,Fe,LiOH/H2O		mixed with 10ml de ionized water - Teflon-lined autoclave - sealed and heat(160C,3-10days) - washed and dried					Coexistence of superconductivity and antiferromagnetism in (Li0.8Fe0.2)OHFeSe			Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Nat. Mater., 14(2015)325	X. F. Lu,N. Z.Wang,H.Wu,Y. P.Wu,D. Zhao,X. Z. Zeng,X. G. Luo,T.Wu,W. Bao,G. H. Zhang,F. Q. Huang,Q. Z. Huang,X. H. Chen		
155457	NJP015073019	Thicknwss=150-250 nm. not SC. R(T) anomaly at 130 K	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		5	2013																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.9638		13.02											Fe-122	K					2																																																																																																		Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155458	NJP015073019	Thicknwss=150-250 nm. R(T) anomaly at 70 K.	(Ba,Ce)Fe2As2	Ba0.91Ce0.09Fe2As2	Ba	0.91	Ce	0.09	Fe	2	As	2																5	2013																										AB2C2	2	ThCr2Si2	I4/mmm																Fe-122	K			4.12				4.12																																																																																																Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155459	NJP015073019	Thicknwss=150-250 nm. optimal Ce-content.	(Ba,Ce)Fe2As2	Ba0.85Ce0.15Fe2As2	Ba	0.85	Ce	0.15	Fe	2	As	2																5	2013																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.962		12.866											Fe-122	K			13.4				13.4	MPH155459																																																																																															Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155460	NJP015073019	Thicknwss=150-250 nm. optimal La-content.	(Ba,La)Fe2As2	Ba0.88La0.12Fe2As2	Ba	0.88	La	0.12	Fe	2	As	2																5	2013																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.97		12.872											Fe-122	K			22.4				22.4	MPH155460																																																																																															Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155461	NJP015073019	Thicknwss=150-250 nm. optimal Pr-content.	(Ba,Pr)Fe2As2	Ba0.82Pr0.18Fe2As2	Ba	0.82	Pr	0.18	Fe	2	As	2																5	2013																										AB2C2	2	ThCr2Si2	I4/mmm		A	3.952		12.879											Fe-122	K			6.2				6.2	MPH155461																																																																																															Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155462	NJP015073019	Thicknwss=150-250 nm. optimal Nd-content.. R(T) anomary at 79 K.. For x=0.071, R(T) anomaly at 109 K.	(Ba,Nd)Fe2As2	Ba0.87Nd0.13Fe2As2	Ba	0.87	Nd	0.13	Fe	2	As	2																5	2013																										AB2C2	2	ThCr2Si2	I4/mmm																Fe-122	K			4.76				4.76																																																																																																Epitaxial films grown on MgO(001) substrates (Ts=850C) using pulsed laser deposition(PLD)					Magnetic scattering and electron pair breaking by rare-earth-ion substitution in BaFe2As2 epitaxial films			Frontier Research Center, Tokyo Institute of Technology, S2-6F East, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	New J.Phys., 15(2013)073019	Takayoshi Katase,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155463	PRC0270300	polycrystal films (d=500A) on MgO substrates (Ts=480C), with growth rate of 0.7 A/s. R not to zero down to 4 K.	LaNiBiO	La1Ni1Bi1O1	La	1	Ni	1	Bi	1															O	1		4	2012																										ABCD		oxypnictide																	Fe-1111	K			5.5				5.5																																																																																														La(3N),Ni(4N5),Bi(5N)		Reactive MBE method. Films were grown by simultaneous evaporation of elemental sources. Oxidation by  activated oxygen source.					MBE growth of LaNiBiO1-x thin films			Technische Universitut Darmstadt, Institute for Material Science, Petersenstr, 23, 64287 Darmstadt, Germany	Physics Procedia, 27(2012300, ISS2011	A.Buckow,R.Retzlaff,J.Kurian,L.Alff		
155464	PRB081174532	No drop in R(T) near Tc(SUS). R-exponent = 0.59. GL-parameter = 1.89.	KxMoO2-z	K0.05Mo1O1.63	K	0.05	Mo	1																	O	2-z	1.63	1	2010																											4		P2<1>/c		A	5.58	4.84	5.61											monoclinic, beta = 121 degree	K				7.25			7.25											Oe	M-H curve	450							Oe	M-H curve	802												MHC155464		A	from Hc2	641			A	from Hc1	1210																																																			K2CO3,MoO3,Mo		mixture - pellet - SIN(650-750C,3days, in quartz tube). K- and O-contents depend on sintering conditions					Unconventional metallic behavior and superconductivity in the K-Mo-O system			Escola de Engenharia de Lorena, University of Sao Paulo, P.O. Box 116, 12602-810 Lorena, SP, Brazil	Phys.Rev.B, 81(2010)174532	L. M. S. Alves,V. I. Damasceno,C. A. M. dos Santos,A. D. Bortolozo,P. A. Suzuki,H. J. Izario Filho,A. J. S. Machado,Z. Fisk		
155465	PRB083054501		CeFeAsO0.95F0.05	Ce1Fe1As1F0.05O0.95	Ce	1	Fe	1	As	1	F	0.05													O	0.95		1	2011					myu-B/Ce	2.47		2.61																		ABCD	2	oxypnictide	P4/nmm	129	A	3.9988		8.6243											Fe-1111, ZrCuSiAs-type	K			13.2	11.9			11.9																																																								mJ/mol.K2	22.7	SP																																				CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155466	PRB083054501	C(T) analyzed by Debye and Einstein model. gamma= 15.3 mJ/mol.K2, Debye-T = 270.6 K, Einstein-T = 351.4 K, (dC/Tc) = 5 mJ/mol.K2	CeFe(As,P)O0.95F0.05	Ce1Fe1As0.85P0.15F0.05O0.95	Ce	1	Fe	1	As	0.85	P	0.15	F	0.05											O	0.95		1	2011								3.3																		ABCD	2	oxypnictide	P4/nmm	129															Fe-1111, ZrCuSiAs-type	K			21.3	21.7			21.7	MPH155466																																																							mJ/mol.K2	11.3	SP	270	SP																																		CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155467	PRB083054501		CeFe(As,P)O0.95F0.05	Ce1Fe1As0.7P0.3F0.05O0.95	Ce	1	Fe	1	As	0.7	P	0.3	F	0.05											O	0.95		1	2011					myu-B/Ce	2.53		3.66																		ABCD	2	oxypnictide	P4/nmm	129	A	3.9826		8.5376											Fe-1111, ZrCuSiAs-type	K			18.2	18.1			18.1																																																																																														CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155468	PRB083054501		CeFe(As,P)O0.95F0.05	Ce1Fe1As0.55P0.45F0.05O0.95	Ce	1	Fe	1	As	0.55	P	0.45	F	0.05											O	0.95		1	2011							2.57																			ABCD	2	oxypnictide	P4/nmm	129															Fe-1111, ZrCuSiAs-type	K			15.1	15			15																																																																																														CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155469	PRB083054501		CeFe(As,P)O0.95F0.05	Ce1Fe1As0.47P0.53F0.05O0.95	Ce	1	Fe	1	As	0.47	P	0.53	F	0.05											O	0.95		1	2011							4.36																			ABCD	2	oxypnictide	P4/nmm	129															Fe-1111, ZrCuSiAs-type	K			7.32	5.84			5.84	MPH155466																																																							mJ/mol.K2	47.3	SP																																				CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155470	PRB083054501		CeFe(As,P)O0.95F0.05	Ce1Fe1As0.3P0.7F0.05O0.95	Ce	1	Fe	1	As	0.3	P	0.7	F	0.05											O	0.95		1	2011					myu-B/Ce	2.58	8.74																			ABCD	2	oxypnictide	P4/nmm	129	A	3.9493		8.4194											Fe-1111, ZrCuSiAs-type	K					1.2																																																										mJ/mol.K2	95.9	SP																																				CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155471	PRB083054501		CeFe(As,P)O0.95F0.05	Ce1Fe1P1F0.05O0.95	Ce	1	Fe	1	P	1	F	0.05													O	0.95		1	2011					myu-B/Ce	2.57	1.81																			ABCD	2	oxypnictide	P4/nmm	129	A	3.9205		8.3439											Fe-1111, ZrCuSiAs-type	K					1.2																																																										mJ/mol.K2	121	SP																																				CeAs,CeP,CeO2,CeF3,FeAs,FeP		mixture - pellet - sealed in evacuated quartz tube - heat to 1430-1470K - keep for 50h					Interplay of superconductivity and Ce 4 f magnetism in CeFeAs1-xPxO0.95F0.05			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 83(2011)054501	Yongkang Luo,Han Han,Shuai Jiang,Xiao Lin,Yuke Li,Jianhui Dai,Zhu-an Xu		
155472	PRB084024521	not SC. T<STR> = 144 K.	SmFeAsO	Sm1Fe1As1O1	Sm	1	Fe	1	As	1															O	1		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.9387		8.4985											Fe-1111, ZrCuSiAs-type	K					2																																																																									mOhm.cm							1.35																SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155473	PRB084024521	T<STR> = 114 K. R(T) exponent = 1.83	SmFeAs(O,H)	Sm1Fe1As1H0.03O0.97	Sm	1	Fe	1	As	1	H	0.03													O	0.97		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.9373		8.4836											Fe-1111, ZrCuSiAs-type	K			5	0.2			0.2	MPH155473									1.3																																																													mOhm.cm							0.75																SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155474	PRB084024521	R(T) exponent = 1.15	SmFeAs(O,H)	Sm1Fe1As1H0.19O0.81	Sm	1	Fe	1	As	1	H	0.19													O	0.81		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.9183		8.453											Fe-1111, ZrCuSiAs-type	K			55.4	55.3			55.3										60																																																																																				SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155475	PRB084024521	R(T) exponent = 0.87	SmFeAs(O,H)	Sm1Fe1As1H0.34O0.64	Sm	1	Fe	1	As	1	H	0.34													O	0.64		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.8974		8.4324											Fe-1111, ZrCuSiAs-type	K			51	51.8			51.8										77																																																																																				SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155476	PRB084024521		SmFeAs(O,H)	Sm1Fe1As1H0.43O0.57	Sm	1	Fe	1	As	1	H	0.43													O	0.57		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.8838		8.4053											Fe-1111, ZrCuSiAs-type	K			47	45			45										45																																																																																				SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155477	PRB084024521	Tc(x)  from J.Supercond.Novel Magn., 22(2009)565	SmFeAs(O,H)	Sm1Fe1As1F0.06O0.94	Sm	1	Fe	1	As	1	F	0.06													O	0.94		1	2011																										ABCD	2	oxypnictide	P4/nmm	129	A														Fe-1111, ZrCuSiAs-type	K			36.4				36.4	MPH155477																																																																																													SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155478	PRB084024521	R(T) anomaly at 100K due to T-to-O transition.	CaFeAsH	Ca1Fe1As1H1	Ca	1	Fe	1	As	1	H	1																	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.8787		8.26											Fe-1111, ZrCuSiAs-type. Below 100K, Ortho- (a = 5.4921, b = 5.4566, c = 8.2115 A)	K					2																																																																									mOhm.cm											2.74												SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155479	PRB084024521	R(T) anomaly at 100K due to T-to-O transition.	CaFeAsD	Ca1Fe1As1D1	Ca	1	Fe	1	As	1	D	1																	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.876		8.257											Fe-1111, ZrCuSiAs-type	K					2																																																																									mOhm.cm											3.1												SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155480	PRB084024521	R(T) anomaly at 120K due to T-to-O transition.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																	2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.879		8.5945											Fe-1111, ZrCuSiAs-type	K					2																																																																									mOhm.cm											4.1												SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155481	PRB084024521	H-content by TG-MS method. Not SC for 0 =< x =< 1 in CaFeAsF1-xHx.	CaFeAs(F,H)	Ca1Fe1As1F0.29H0.71	Ca	1	Fe	1	As	1	F	0.29	H	0.71															2011																										ABCD	2	oxypnictide	P4/nmm	129	A	3.8808		8.4064											Fe-1111, ZrCuSiAs-type	K					2			MLAT155481																																																																																													SmAs,FeAs,Fe2As,Sm2O3,SmH2		High-P synthesis. mixture - heat(1200C, P = 2GPa)					Hydrogen in layered iron arsenides: Indirect electron doping to induce superconductivity			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 84(2011)024521	Taku Hanna,Yoshinori Muraba,Satoru Matsuishi,Naoki Igawa,Katsuaki Kodama,Shin-ichi Shamoto,Hideo Hosono		
155482	PRB085140516	Thick film (d = 150-250 nm). R(T) anomaly at 131 K (structure/magnetic transition)	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		4	2012																										AB2C2	2	ThCr2Si2			A	3.9741		13.0015											Fe-122	K					2																																																																																																		Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155483	PRB085140516	Thick film (d = 150-250 nm). R(T) anomaly at 120 K (structure/magnetic transition)	(Ba,La)Fe2As2	Ba0.98La0.02Fe2As2	Ba	0.98	La	0.02	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9861		12.9819											Fe-122	K					2																																																																																																		Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155484	PRB085140516	Thick film (d = 150-250 nm). R(T) anomaly at 72.8 K (structure/magnetic transition). Coexistence of SC and AFM.	(Ba,La)Fe2As2	Ba0.91La0.09Fe2As2	Ba	0.91	La	0.09	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9648		12.9392											Fe-122	K				7.76			7.76																																																																																																Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155485	PRB085140516	Thick film (d = 150-250 nm).	(Ba,La)Fe2As2	Ba0.86La0.14Fe2As2	Ba	0.86	La	0.14	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9765		12.872											Fe-122	K				22.7			22.7	MPH155485																																																																																				cm3/C	-0.000184					MRH155485					Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155486	PRB085140516	Thick film (d = 150-250 nm).	(Ba,La)Fe2As2	Ba0.82La0.18Fe2As2	Ba	0.82	La	0.18	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9462		12.8175											Fe-122	K				14.8			14.8																																																																																																Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155487	PRB085140516	Thick film (d = 150-250 nm).	(Ba,La)Fe2As2	Ba0.76La0.24Fe2As2	Ba	0.76	La	0.24	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9662		12.7784											Fe-122	K				5.02			5.02																																																																																																Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155488	PRB085140516	Thick film (d = 150-250 nm).	(Ba,La)Fe2As2	Ba0.7La0.3Fe2As2	Ba	0.7	La	0.3	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9696		12.658											Fe-122	K					2																																																																																																		Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155489	PRB085140516	Thick film (d = 150-250 nm).	(Ba,La)Fe2As2	Ba0.56La0.44Fe2As2	Ba	0.56	La	0.44	Fe	2	As	2																4	2012																										AB2C2	2	ThCr2Si2			A	3.9619		12.5472											Fe-122	K					2																																																																																																		Thick films were fabricated on MgO(001) single crystal ( Ts= 850C) by PLD method. La-added Ba-122 synthesized by solid state reaction					Identical effects of indirect and direct electron doping of superconducting BaFe2As2 thin films			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 85(2012)140516	Takayoshi Katase,Soshi Iimura,Hidenori Hiramatsu,Toshio Kamiya,Hideo Hosono		
155490	PRB087020504	impurity phase: Bi2S3(15%). Semiconductor (gap = 38.2 meV from R(T) analysis)	SrFBiS2	Sr1Bi1S2F1	Sr	1	Bi	1	S	2	F	1																1	2013																										ABCD2		CeOBiS2			A	4.082		13.8025											BiS2-layered SC	K					0.4																																																																																																La2S3,SrS,SrF2,Bi,S		mixture - pellet - heat(1073K,10h, in evacuated quartz tube) - FC to RT					Superconductivity induced by La doping in Sr1-xLaxFBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 87(2013)020504	Xi Lin,Xinxin Ni,Bin Chen,Xiaofeng Xu,Xuxin Yang,Jianhui Dai,Yuke Li,Xiaojun Yang,Yongkang Luo,Qian Tao,Guanghan Cao,Zhuan Xu		
155491	PRB087020504	impurity phase: Bi2S3(25%). Lattice term in SP (beta) = 0.414 mJ/mol.K4.  (dC/gamma*Tc) = 1.4.	(Sr,La)FBiS2	Sr0.5La0.5Bi1S2F1	Sr	0.5	La	0.5	Bi	1	S	2	F	1														1	2013																										ABCD2		CeOBiS2				4.0822		13.335											BiS2-layered SC	K				2.8			2.8										30										T	RES(R=0.9Rn), GL theory	1.04												MHC155491																						mJ/mol.K2	1.42	SP	265	SP																															MRH155491			La2S3,SrS,SrF2,Bi,S		mixture - pellet - heat(1073K,10h, in evacuated quartz tube) - FC to RT					Superconductivity induced by La doping in Sr1-xLaxFBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 87(2013)020504	Xi Lin,Xinxin Ni,Bin Chen,Xiaofeng Xu,Xuxin Yang,Jianhui Dai,Yuke Li,Xiaojun Yang,Yongkang Luo,Qian Tao,Guanghan Cao,Zhuan Xu		
155492	PRB087224507	SP data, best fitting to two gap model. [gamma-1] = 3.44, [gamma-2] = 6.35, totall [gamma] = 12.5 mJ/mol.K2. (dC/gamma*Tc) = 1.6. R(T) = R(0) + AT^2 A=3.2 nOhm.cm for T<32K.	SrPt2As2	Sr1Pt2As2	Sr	1	Pt	2	As	2																		3	2013																										AB2C2		CaBe2Ge2																		K		4.6					4.6																				T	RES(0.9Rn)								T/K	RES(0.9Rn)		0.92		MHC155492																																					mOhm.cm								0.078																	Single crystals synthesized by self-melting technique.					Evidence for two energy gaps and Fermi liquid behavior in the SrPt2As2 superconductor			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 87(2013)224507	Xiaofeng Xu,B. Chen,W. H. Jiao,Bin Chen,C. Q. Niu,Y. K. Li,J. H. Yang,A. F. Bangura,Q. L. Ye,C. Cao,J. H. Dai,Guanghan Cao,N. E. Hussey		
155493	PRB073180505	Tc(lat-c) and Tc(p) measured. hole density as a function of lattice const. c,  p = 11.491y + 5.17E+9*y^6 where y = 1-c/c0, c0 = 1.18447 nm	YBa2Cu3O6+z	Y1Ba2Cu3O6	Y	1	Ba	2	Cu	3															O	6+z	6	3	2006																										AB2C3D7		Y123																		K					0																																																																																																		High-purity(4N5) YBCO crystals grown in Ba-zirconate crucible.					Evaluation of CuO2 plane hole doping in YBa2Cu3O6+x single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia V6T 1Z1, Canada	Phys.Rev.B, 73(2006)180505	Ruixing Liang,D. A. Bonn,W. N. Hardy		
155494	PRB073180505	Tc(lat-c) and Tc(p) measured. hole density as a function of lattice const. c,  p = 11.491y + 5.17E+9*y^6 where y = 1-c/c0, c0 = 1.18447 nm	YBa2Cu3O6+z	Y1Ba2Cu3O6.5	Y	1	Ba	2	Cu	3															O	6+z	6.5	3	2006																										AB2C3D7		Y123																		K				54.1			54.1	MTC155494																																																																																															High-purity(4N5) YBCO crystals grown in Ba-zirconate crucible.					Evaluation of CuO2 plane hole doping in YBa2Cu3O6+x single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia V6T 1Z1, Canada	Phys.Rev.B, 73(2006)180505	Ruixing Liang,D. A. Bonn,W. N. Hardy		
155495	PRB073180505	Tc(lat-c) and Tc(p) measured. hole density as a function of lattice const. c,  p = 11.491y + 5.17E+9*y^6 where y = 1-c/c0, c0 = 1.18447 nm	YBa2Cu3O6+z	Y1Ba2Cu3O6.67	Y	1	Ba	2	Cu	3															O	6+z	6.67	3	2006																										AB2C3D7		Y123																		K				60.6			60.6	MTC155494																																																																																															High-purity(4N5) YBCO crystals grown in Ba-zirconate crucible.					Evaluation of CuO2 plane hole doping in YBa2Cu3O6+x single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia V6T 1Z1, Canada	Phys.Rev.B, 73(2006)180505	Ruixing Liang,D. A. Bonn,W. N. Hardy		
155496	PRB073180505	Tc(lat-c) and Tc(p) measured. hole density as a function of lattice const. c,  p = 11.491y + 5.17E+9*y^6 where y = 1-c/c0, c0 = 1.18447 nm	YBa2Cu3O6+z	Y1Ba2Cu3O6.75	Y	1	Ba	2	Cu	3															O	6+z	6.75	3	2006																										AB2C3D7		Y123																		K				75.3			75.3																																																																																																High-purity(4N5) YBCO crystals grown in Ba-zirconate crucible.					Evaluation of CuO2 plane hole doping in YBa2Cu3O6+x single crystals			Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia V6T 1Z1, Canada	Phys.Rev.B, 73(2006)180505	Ruixing Liang,D. A. Bonn,W. N. Hardy		
155497	PRB081134422	Not SC for 0 =< x =< 1 in CeFeAs1-xPxO. Tn = 134 K for Fe-AFM.	CeFe(As,P)O	Ce1Fe1As0.9P0.1O1	Ce	1	Fe	1	As	0.9	P	0.1													O	1		1	2010								134																		ABCD	2	oxypnictide	P4/nmm	129	A	3.9967		8.5995											Fe-1111, ZrCuSiAs-type	K					2																																																																																																CeAs,CeP,CeO2,FeAs,FeP		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat to 1448 K -keep(50h)					Phase diagram of CeFeAs1-xPxO obtained from electrical resistivity, magnetization, and specific heat measurements			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 81(2010)134422	Yongkang Luo,Yuke Li,Shuai Jiang,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
155498	PRB081134422	Not SC for 0 =< x =< 1 in CeFeAs1-xPxO.  Tn = 4.12 K for Ce-AFM. Tm = 4.49 K for Ce-FM.	CeFe(As,P)O	Ce1Fe1As0.63P0.37O1	Ce	1	Fe	1	As	0.63	P	0.37													O	1		1	2010								44.1																		ABCD	2	oxypnictide	P4/nmm	129															Fe-1111, ZrCuSiAs-type	K					2			MPH155498																																																																																													CeAs,CeP,CeO2,FeAs,FeP		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat to 1448 K -keep(50h)					Phase diagram of CeFeAs1-xPxO obtained from electrical resistivity, magnetization, and specific heat measurements			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 81(2010)134422	Yongkang Luo,Yuke Li,Shuai Jiang,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
155499	PRB081134422	Not SC for 0 =< x =< 1 in CeFeAs1-xPxO. Tn = 44.1 K for Fe-AFM.Tm = 10.8 K for Ce-FM	CeFe(As,P)O	Ce1Fe1As0.4P0.6O1	Ce	1	Fe	1	As	0.4	P	0.6													O	1		1	2010																										ABCD	2	oxypnictide	P4/nmm	129	A	3.9586		8.4456											Fe-1111, ZrCuSiAs-type	K					2			MPH155498																																																																																													CeAs,CeP,CeO2,FeAs,FeP		solid state reaction. mixture - pellet - sealed in evacuated quartz tube - heat to 1448 K -keep(50h)					Phase diagram of CeFeAs1-xPxO obtained from electrical resistivity, magnetization, and specific heat measurements			State Key Laboratory of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 81(2010)134422	Yongkang Luo,Yuke Li,Shuai Jiang,Jianhui Dai,Guanghan Cao,Zhu-an Xu		
155500	PRB089094501	R not zero down to 0K. Tanom = 80 K.	Ce(Fe,Co)AsH	Ce1Fe0.98Co0.02As1H1	Ce	1	Fe	0.98	Co	0.02	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8788		8.2601											Fe-1111, ZrCuSiAs-type	K				2			2										0																																																													mOhm.cm				3.8			3.59																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155501	PRB089094501	R not zero down to 0K. Tanom = 55 K.	Ce(Fe,Co)AsH	Ce1Fe0.96Co0.04As1H1	Ce	1	Fe	0.96	Co	0.04	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8793		8.249											Fe-1111, ZrCuSiAs-type	K				2			2										0																																																													mOhm.cm				4.32			4.61																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155502	PRB089094501	Co-rich phase 7.3%	Ce(Fe,Co)AsH	Ce1Fe0.93Co0.07As1H1	Ce	1	Fe	0.93	Co	0.07	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8804		8.2395											Fe-1111, ZrCuSiAs-type	K				23			23	MPH155502									15																																																													mOhm.cm				3.53			4.03																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155503	PRB089094501	Co-rich phase 7.9%	Ce(Fe,Co)AsH	Ce1Fe0.91Co0.09As1H1	Ce	1	Fe	0.91	Co	0.09	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8806		8.2317											Fe-1111, ZrCuSiAs-type	K				23			23										25																																																													mOhm.cm				3.24			3.06																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155504	PRB089094501	Co-rich phase: 9.54 %	Ce(Fe,Co)AsH	Ce1Fe0.88Co0.12As1H1	Ce	1	Fe	0.88	Co	0.12	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.881		8.2254											Fe-1111, ZrCuSiAs-type	K				23			23	MPH155502									58																																																													mOhm.cm				3.52			3.4																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155505	PRB089094501	Co-rich phase: 15.8 %	Ce(Fe,Co)AsH	Ce1Fe0.83Co0.17As1H1	Ce	1	Fe	0.83	Co	0.17	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8816		8.2015											Fe-1111, ZrCuSiAs-type	K				19.5			19.5										34																																																													mOhm.cm				4.67			4.3																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155506	PRB089094501	Co-rich phase: 19.2 %	Ce(Fe,Co)AsH	Ce1Fe0.78Co0.22As1H1	Ce	1	Fe	0.78	Co	0.22	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8825		8.1935											Fe-1111, ZrCuSiAs-type	K				13.5			13.5										54																																																													mOhm.cm				2.73			2.4																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155507	PRB089094501	Co-rich phase: 23.0 %	Ce(Fe,Co)AsH	Ce1Fe0.74Co0.26As1H1	Ce	1	Fe	0.74	Co	0.26	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8827		8.1792											Fe-1111, ZrCuSiAs-type	K				10			10										32																																																													mOhm.cm				3.4			3.14																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155508	PRB089094501	Co-rich phase: 27.7 %	Ce(Fe,Co)AsH	Ce1Fe0.69Co0.31As1H1	Ce	1	Fe	0.69	Co	0.31	As	1	H	1														1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8841		8.1618											Fe-1111, ZrCuSiAs-type	K				0			0										0																																																													mOhm.cm				2.01			1.93																CaAs,CaH2,Fe2As,Co2As		starting material mixture - in BN capsule with Ca(OH)2, NaBH4 as a excess H source - heat (1273K,30min, P=2 GPa)					Enhancing the three-dimensional electronic structure in 1111-type iron arsenide superconductors by H substitution			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094501	Yoshinori Muraba,Satoru Matsuishi,Hideo Hosono		
155509	PRB089094510		SmFeAsO1-xHx	Sm1Fe1As1H0.22O0.78	Sm	1	Fe	1	As	1	H	0.22													O	0.78		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.9112		8.4412											Fe-1111, ZrCuSiAs-type	K				50			50	MTC155509																																																																																													SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155510	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.77P0.23H0.11O0.89	Sm	1	Fe	1	As	0.77	P	0.23	H	0.11											O	0.89		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.9143		8.3763											Fe-1111, ZrCuSiAs-type	K			31	28			28	MTC155510																																																																																													SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155511	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.77P0.23H0.2O0.8	Sm	1	Fe	1	As	0.77	P	0.23	H	0.2											O	0.8		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8943		8.3527											Fe-1111, ZrCuSiAs-type	K			44.5	36			36																																																																																														SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155512	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.55P0.45H0.08O0.92	Sm	1	Fe	1	As	0.55	P	0.45	H	0.08											O	0.92		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.9034		8.3253											Fe-1111, ZrCuSiAs-type	K			22.5	19			19	MTC155512																																																																																													SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155513	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.55P0.45H0.16O0.84	Sm	1	Fe	1	As	0.55	P	0.45	H	0.16											O	0.84		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8947		8.3107											Fe-1111, ZrCuSiAs-type	K			18	11			11																																																																																														SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155514	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.55P0.45H0.26O0.74	Sm	1	Fe	1	As	0.55	P	0.45	H	0.26											O	0.74		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8774		8.2804											Fe-1111, ZrCuSiAs-type	K			24	17			17																																																																																														SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155515	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.47P0.53H0.09O0.91	Sm	1	Fe	1	As	0.47	P	0.53	H	0.09											O	0.91		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.896		8.2938											Fe-1111, ZrCuSiAs-type	K			13.5	10.5			10.5	MTC155515																																																																																													SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155516	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.47P0.53H0.15O0.85	Sm	1	Fe	1	As	0.47	P	0.53	H	0.15											O	0.85		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8843		8.2671											Fe-1111, ZrCuSiAs-type	K			4	0			0																																																																																														SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155517	PRB089094510		SmFeAs1-yPyO1-xHx	Sm1Fe1As0.47P0.53H0.24O0.76	Sm	1	Fe	1	As	0.47	P	0.53	H	0.24											O	0.76		1	2014																										ABCD	2	oxypnictide	P4/nmm		A	3.8726		8.2479											Fe-1111, ZrCuSiAs-type	K			12.5	5.5			5.5																																																																																														SmAs,FeAs,Fe2As,Fe2P,Sm2O3,SmH2		Samples synthesized by solid state reaction using belt-type high-P anvil. H-content evaluated by thermal desorption spectroscopy.					Controlling factors of Tc dome structure in 1111-type iron arsenide superconductors			Materials Research Center for Element Strategy, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.B, 89(2014)094510	Satoru Matsuishi,Takuya Maruyama,Soshi Iimura,Hideo Hosono		
155518	PRB089220509	Tc and Hc2 measured for P < 7.1 GPa. R(T)= R0 +A*T^2. A decreases with P. (dHc2/dT) has linear dependence of A. .	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2014																										AB2C2		ThCr2Si2																	Fe-122	K			3.58	3.5			3.5	MTC155518																			T	RES(zero)						1.6	0.5						MHC155518																																																														single crystals grown by KAs flux method.					Upper critical field of KFe2As2 under pressure: A test for the change in the superconducting gap structure			Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)220509	Valentin Taufour,Neda Foroozani,Makariy A. Tanatar,Jinhyuk Lim,Udhara Kaluarachchi,Stella K. Kim,Yong Liu,Thomas A. Lograsso,Vladimir G. Kogan,Ruslan Prozorov,Sergey L. Bud'ko,James S. Schilling,Paul C. Canfield		
155519	PRB091054511	Pc(critical P where the sign of (dTc/dP) change to plus) = 11 kbar. RH = RH(0) + A*T^2 for T^2 < 12 K2.	RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2			A	3.86		14.45											Fe-122	K	2.5						2.5	MTC155519																			T	RES(zero)													MHC155519																																					uOhm.cm							0.8							mm3/C				0.72		MRH155519					single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155520	PRB091054511	RESN = 0.2 uOhm.cm. Pc(critical P where the sign of (dTc/dP) change to plus) = 17.5 kbar. RH = RH(0) + A*T^2 for T^2 < 12 K2.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2			A	3.84		13.84											Fe-122	K	3.6						3.6	MTC155520																																																																						uOhm.cm							0.2							mm3/C				0.4		MRH155519					single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155521	PRB091054511	RESN = 1.3 uOhm.cm. Pc(critical P where the sign of (dTc/dP) change to plus) = 17.5 kbar.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K	3.1						3.1	MTC155521																			T	RES(zero)													MHC155521																																					uOhm.cm							1.3																		single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155522	PRB091054511	Pc(critical P where the sign of (dTc/dP) change to plus) = 14 kbar.  RH = RH(0) + A*T^2 for T^2 < 12 K2.	CsFe2As2	Cs1Fe2As2	Cs	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2			A	3.89		15.07											Fe-122	K	1.8						1.8	MTC155522																																																																						uOhm.cm							1.5							mm3/C				0.27		MRH155519					single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155523	PRB091054511		KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K																																																																																																							single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155524	PRB091054511		RbFe2As2	Rb1Fe2As2	Rb	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K																																																																																																							single crystals grown by self flux method.					Universal V-shaped temperature-pressure phase diagram in the iron-based superconductors KFe2As2, RbFe2As2, and CsFe2As2			Departement de physique & RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada	Phys.Rev.B, 91(2015)054511	F. F. Tafti,A. Ouellet,A. Juneau-Fecteau,S. Faucher,M. Lapointe-Major,N. Doiron-Leyraud,A. F. Wang,X.-G. Luo,X. H. Chen,Louis Taillefer		
155525	PRB089220509		KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2014																										AB2C2		ThCr2Si2																	Fe-122	K			3.58	3.5			3.5																				T	RES(zero)						1.6	0.5						MHC155525																																																														single crystals grown by KAs flux method.					Upper critical field of KFe2As2 under pressure: A test for the change in the superconducting gap structure			Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)220509	Valentin Taufour,Neda Foroozani,Makariy A. Tanatar,Jinhyuk Lim,Udhara Kaluarachchi,Stella K. Kim,Yong Liu,Thomas A. Lograsso,Vladimir G. Kogan,Ruslan Prozorov,Sergey L. Bud'ko,James S. Schilling,Paul C. Canfield		
155526	PRL106057002	Samples decomposed at ambient atmosphere, then stored in deciccate(vac).	LaNi0.65Bi2	La1Ni0.65Bi2	La	1	Ni	0.65	Bi	2																		1	2011																										ABC2		ZrCuSiAs			A	4.5599		9.7544												K			4				4										1	Oe	M-H curve				90			2																																																																											La(Ce or Nd or Y),Ni,Bi		solid state reaction. mixture - heat(773K,10h, in silica ampoule) - heat(1023K,20h) - reground - pellet - heat(1073K,10h)					Coexistence of Light and Heavy Carriers Associated with Superconductivity and Antiferromagnetism in CeNi0.8Bi2 with a Bi Square Net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)057002	Hiroshi Mizoguchi,Satoru Matsuishi,Masahiro Hirano,Makoto Tachibana,Eiji Takayama-Muromachi,Hitoshi Kawaji,Hideo Hosono		
155527	PRL106057002	Samples decomposed at ambient atmosphere, then stored in deciccate(vac). . [gamma] comtains two contributions of SC and AFM electrons	CeNi0.80Bi2	Ce1Ni0.8Bi2	Ce	1	Ni	0.8	Bi	2																		1	2011																										ABC2		ZrCuSiAs			A	4.5439		9.6414												K	4		4.2				4.1										96	Oe	M-H curve				65			2																																																																											La(Ce or Nd or Y),Ni,Bi		solid state reaction. mixture - heat(773K,10h, in silica ampoule) - heat(1023K,20h) - reground - pellet - heat(1073K,10h)					Coexistence of Light and Heavy Carriers Associated with Superconductivity and Antiferromagnetism in CeNi0.8Bi2 with a Bi Square Net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)057002	Hiroshi Mizoguchi,Satoru Matsuishi,Masahiro Hirano,Makoto Tachibana,Eiji Takayama-Muromachi,Hitoshi Kawaji,Hideo Hosono		
155528	PRL106057002	Samples decomposed at ambient atmosphere, then stored in deciccate(vac).	NdNi0.89Bi2	Nd1Ni0.89Bi2	Nd	1	Ni	0.89	Bi	2																		1	2011																										ABC2		ZrCuSiAs			A	4.519		9.532												K			4.1				4.1										14	Oe	M-H curve				55			2																																																																											La(Ce or Nd or Y),Ni,Bi		solid state reaction. mixture - heat(773K,10h, in silica ampoule) - heat(1023K,20h) - reground - pellet - heat(1073K,10h)					Coexistence of Light and Heavy Carriers Associated with Superconductivity and Antiferromagnetism in CeNi0.8Bi2 with a Bi Square Net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)057002	Hiroshi Mizoguchi,Satoru Matsuishi,Masahiro Hirano,Makoto Tachibana,Eiji Takayama-Muromachi,Hitoshi Kawaji,Hideo Hosono		
155529	PRL106057002	Samples decomposed at ambient atmosphere, then stored in deciccate(vac).	YNi0.82Bi2	Y1Ni0.82Bi2	Y	1	Ni	0.82	Bi	2																		1	2011																										ABC2		ZrCuSiAs			A	4.4835		9.3003												K			4.1				4.1										17	Oe	M-H curve				67			2																																					J/mol.K2	0.4	SP																																				La(Ce or Nd or Y),Ni,Bi		solid state reaction. mixture - heat(773K,10h, in silica ampoule) - heat(1023K,20h) - reground - pellet - heat(1073K,10h)					Coexistence of Light and Heavy Carriers Associated with Superconductivity and Antiferromagnetism in CeNi0.8Bi2 with a Bi Square Net			Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta, Midori-ku, Yokohama 226-8503, Japan	Phys.Rev.Lett., 106(2011)057002	Hiroshi Mizoguchi,Satoru Matsuishi,Masahiro Hirano,Makoto Tachibana,Eiji Takayama-Muromachi,Hitoshi Kawaji,Hideo Hosono		
155530	PRL109097002	T<STR>=138(heating), 132(cooling) K. (dC/gamma*Tc) = 1.3.	BaNi2As2	Ba1Ni2As2	Ba	1	Ni	2	As	2																		3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1478		11.6184											tetra-to-triclinic transition at 132 K.	K	0.575						0.575																																																																																														Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155531	PRL109097002	T<STR>=123(heating), 118(cooling) K. (dC/gamma*Tc) = 1.3.	BaNi2(As1-x,Px)2	Ba1Ni2As1.972P0.028	Ba	1	Ni	2	As	1.972	P	0.028																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1394		11.6195											tetra-to-triclinic transition at 118 K.	K	0.634						0.634																																																																																														Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155532	PRL109097002	T<STR>=84(heating), 76(cooling) K.  (dC/gamma*Tc) = 1.3.	BaNi2(As1-x,Px)2	Ba1Ni2As1.902P0.098	Ba	1	Ni	2	As	1.902	P	0.098																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1358		11.6302											tetra-to-triclinic transition at 76 K.	K	0.763						0.763	MPH155533																																																																																													Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155533	PRL109097002	(dC/gamma*Tc) = 1.9. Logarithmic averaged phonon frequency = 53.4 K.	BaNi2(As1-x,Px)2	Ba1Ni2As1.846P0.154	Ba	1	Ni	2	As	1.846	P	0.154																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1339		11.6274												K	3.28						3.28	MPH155533																																																				MSP155533																																									Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155534	PRL109097002	(dC/gamma*Tc) = 11.78. Logarithmic averaged phonon frequency = 66.8 K.	BaNi2(As1-x,Px)2	Ba1Ni2As1.816P0.184	Ba	1	Ni	2	As	1.816	P	0.184																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1248		11.6412												K	3.27						3.27																																																					MSP155534																																									Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155535	PRL109097002	(dC/gamma*Tc) = 11.60. Logarithmic averaged phonon frequency = 103.8 K. Solubility limit x = 0.13 for BaNi2(As1-xPx)2	BaNi2(As1-x,Px)2	Ba1Ni2As1.792P0.208	Ba	1	Ni	2	As	1.792	P	0.208																3	2012																										AB2C2		ThCr2Si2	I4/mmm		A	4.1242		11.6386												K	3.24						3.24																																																																																														Ba,NiAs,Ni,P		self-flux method. mixture - alumina crucible - sealed in quartz tube - heat(700C,3h) - slow heating to 1150C - cool to 1000C(2 C/h) - FC to RT.					Giant Phonon Softening and Enhancement of Superconductivity by Phosphorus Doping of BaNi2As2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.Lett., 109(2012)097002	K. Kudo,M. Takasuga,Y. Okamoto,Z. Hiroi,M. Nohara		
155536	PRX004031055	P-induced SC. Tc  shows Tc(max) at P=21.7 GPa.. For every pressures, R(T) = R0 + A*T^n* R0, A, n are in Fig -data MPH155536.	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2014																										AB2C2		ThCr2Si2																	Fe-122	K	2.33		2.58		0		2.455	MPH155536																																																																																													Ce(4N),Au(5N),Si(6N)		Au-Si self-flux method. Ce0.05Au0.475Si0.475 are melted in alumina crucible - hold(1120C,6h) cool to 850C (1.2 C/h)					Giant Overlap between the Magnetic and Superconducting Phases of CeAu2Si2 under Pressure			DPMC-University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.X, 4(2014)031055	Z. Ren,L. V. Pourovskii,G. Giriat,G. Lapertot,A. Georges,D. Jaccard		
155537	PSS0080845	Lattice term in SP (beta)  = 2.6 mJ/mol.K4. (dC/gamma*Tc) = 1.42. GL (kappa) = 56.5 from Hc1.  Compositions by EDX. Hall coeff. independent of H for H<1T.	Bi3O2S3	Bi3S3O3	Bi	3	S	3																	O	3		1	2014																										A2B3C3			I4/mmm		A	3.9674		41.2825												K			5.8	5.1			5.1										96.5	Oe	M-H curve, GL theory	30.5			25			2	T	RES(on), WHH	4.84												MHC155537		A	from Hc2	82.4			A	GL parameter, cohere	4660										MSP155537			mJ/mol.K2	1.65	SP	182	SP											mOhm.cm											3			m3/C	-0.000000395				1	MRH155537					mixture - pellet - sealed in quartz tube - heat(430C,2h) -Q to ice - (repeat) - heat(430C,15h) - Q - (repeat) - SIN(520C,17H)					Bulk superconductivity in single-phase Bi3O2S3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, P.R. China	Phys.Status Solidi PRL, 8(2014)845	Jifeng Shao,Zhongheng Liu,Xiong Yao,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
155538	SCI3231585	A15-type Cs3C60. P-induced SC. Pc = 2.6 kbar. AFI(antiferromag-insulator) state at ambient-P. Tc(max) = 38 K at 7 kbar. Compressibility(14.6 K) = 0.054 GPa(-1)	Cs3C60	Cs3C60	Cs	3	C	60																					2009								46										GPa	18.5							A3B60		fullerene	Pm3[-]n																	K				38	0		38	MPH155538																																																																																																				The Disorder-Free Non-BCS Superconductor Cs3C60 Emerges from an Antiferromagnetic Insulator Parent State			Department of Chemistry, University of Durham, Durham DH1 3LE, UK	Science, 323(2009)1585	Yasuhiro Takabayashi,Alexey Y. Ganin,Peter Jeglic,Denis Arcon,Takumi Takano,Yoshihiro Iwasa,Yasuo Ohishi,Masaki Takata,Nao Takeshita,Kosmas Prassides,Matthew J. Rosseinsky		
155539	SCIR0033101	Single crystals separated from the mixture. R(T) measured for ab plane.	Ca10(Ir4As8)(Fe2As2)5	Ca10Ir4Fe10As18	Ca	10	Ir	4	Fe	10	As	18																3	2013																													P4/n	85															Ca-10-4-8	K	17		20	16		2	16										83																																																													mOhm.cm					0.454			0.284				0.613		cm3/C	-0.000328					MRH155539			Ca,FeAs,IrAs2,Ir		mixture - in alumina crucible - sealed in quartz tube - heat(700C,3h) - heat(1100-1150C,10-40h) - Q to ice					Superconductivity in Ca10(Ir4As8)(Fe2As2)5 with Square-Planar Coordination of Iridium			Department of Physics, Okayama University, Okayama 700-8530, Japan	Science Peports, 3(2013)3101	Kazutaka Kudo,Daisuke Mitsuoka,Masaya Takasuga,Yuki Sugiyama,Kento Sugawara,Naoyuki Katayama,Hiroshi Sawa,Hiroaki S. Kubo,Kenta Takamori,Masanori Ichioka,Tatsuo Fujii,Takashi Mizokawa,Minoru Nohara		
155540	SSC1940006	P = 0 GPa. Impurity phase: Bi, hydrostatic pressure.	Ce(O,F)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5			2014																										ABCD2		CeOBiS2	P4/nmm		A	4.037		13.407											BiS2 layer-SC	K	2.2		2.7				2.45	MTC155540																			T	RES(0.9Rn), WHH	1.5							T/K	RES(0.9Rn)	0.79			MHC155540																																																												Ce,Bi,S,CeF3,CeO2		mixture - pellet - sealed in quartz tube - heat to 700 C(2 C/h) - keep(700C,12h) - slow cool to RT (within 6h)					Significant enhancement of superconductivity under Hydrostatic pressure in CeO0.5F0.5BiS2 superconductor			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	Solid State Commun., 194(2014)6	Rajveer Jha,H. Kishan,V.P.S. Awana		
155541	SSC1940006	P = 1.97 GPa. Impurity phase: Bi, hydrostatic pressure.	Ce(O,F)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5			2014																										ABCD2		CeOBiS2	P4/nmm																BiS2 layer-SC	K	6.96		8.28				7.62	MTC155540																			T	RES(0.9Rn), WHH	4.8							T/K	RES(0.9Rn)	0.83			MHC155540																																																												Ce,Bi,S,CeF3,CeO2		mixture - pellet - sealed in quartz tube - heat to 700 C(2 C/h) - keep(700C,12h) - slow cool to RT (within 6h)					Significant enhancement of superconductivity under Hydrostatic pressure in CeO0.5F0.5BiS2 superconductor			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	Solid State Commun., 194(2014)6	Rajveer Jha,H. Kishan,V.P.S. Awana		
155542	SST023054013	Samples exposed to the air for several days (high Tc sample).  Anion hight dependence of Tc measured.	Fe(Te,S)	Fe1Te0.8S0.2	Fe	1	Te	0.8	S	0.2																			2010																										AB																			Fe-11	K	6.6		9.2				7.9	MTC155542																																																																																															solid state reaction. as-grown sample exposed to the air for several days					Anion height dependence of Tc for the Fe-based superconductor			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba 305-0047, Japan	Supercond.Sci.Technol., 23(2010)054013	Y Mizuguchi,YHara,K Deguchi,S Tsuda,T Yamaguchi,K Takeda,H Kotegawa,H Tou,Y Takano		
155543	SST025084017	H-content x in LaNiAsO1-xHx measure by EPM	LaNiAs(O,H)	La1Ni1As1H0.08O0.92	La	1	Ni	1	As	1	H	0.08													O	0.92			2012																										ABCD					A	4.1192		8.1787												K			3.76				3.76	MTC155543									78																																																													mOhm.cm											2.26												LnAs,NiAs,Ni2As,LnO3,LnH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155544	SST025084017	H-content x in LaNiAsO1-xHx measure by EPM	LaNiAs(O,H)	La1Ni1As1H0.17O0.83	La	1	Ni	1	As	1	H	0.17													O	0.83			2012																										ABCD					A	4.1086		8.1453												K			3.68				3.68	MTC155543									67																																																													mOhm.cm											1.02												LnAs,NiAs,Ni2As,LnO3,LnH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155545	SST025084017	H-content x in CeNiAsO1-xHx measure by EPM. not SC for x  < 0.14.	CeNiAs(O,H)	Ce1Ni1As1H0.06O0.94	Ce	1	Ni	1	As	1	H	0.06													O	0.94			2012																										ABCD					A	4.0928		8.0441												K					0.5																																																																																																CeAs,NiAs,Ni2As,CeO2,CeH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155546	SST025084017	H-content x in PrNiAsO1-xHx measure by EPM	PrNiAsO	Pr1Ni1As1O1	Pr	1	Ni	1	As	1															O	1			2012																										ABCD																				K					0.5																																																																																																LnAs,NiAs,Ni2As,LnO3,LnH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155547	SST025084017	H-content x in PrNiAsO1-xHx measure by EPM	PrNiAs(O,H)	Pr1Ni1As1H0.06O0.94	Pr	1	Ni	1	As	1	H	0.06													O	0.94			2012																										ABCD					A	4.0818		8.0259												K			1.6				1.6																																																																																														LnAs,NiAs,Ni2As,LnO3,LnH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155548	SST025084017	H-content x in NdNiAsO1-xHx measure by EPM.  Not SC for x < 0.19	NdNiAs(O,H)	Nd1Ni1As1H0.05O0.95	Nd	1	Ni	1	As	1	H	0.05													O	0.95			2012																										ABCD					A	4.0586		7.9977												K					0.5																																																																																																LnAs,NiAs,Ni2As,LnO3,LnH2		mixture - in BN crucible - added Ca(OH)2 and NaBH4 as excess H sources - heat(1273-1373 K,30min, P=2 GPa)					Hydrogen substitution effect on the superconductivity of LnNiAsO (Ln D La-Nd)			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan	Supercond.Sci.Technol., 25(2012)084017	Satoru Matsuishi,Atsushi Nakamura,Yoshinori Muraba,Hideo Hosono		
155549	SST026045017	M=NH3, y not measured. co-intercalation of Eu and NH3 into ZrNCl.	Eu0.16(NH3)yZrNCl	Eu0.16M1Zr1N1Cl1	Eu	0.16	M	1	Zr	1	N	1	Cl	1															2013																												SmSI	P3[-]m			3.6113		11.889											interlayer distance , d = 11.889	K			13.5	12.7		1.2	12.7											Oe	M-H curve, GL			46																																																																																	RE dissolved in liquid ammonia. MNCl (M=Zr,Hf) ws dispersed into (Re+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155550	SST026045017	M=NH3, y not measured. co-intercalation of Yb and NH3 into ZrNCl.	Yb0.31(NH3)yZrNCl	Yb0.31M1Zr1N1Cl1	Yb	0.31	M	1	Zr	1	N	1	Cl	1															2013																												SmSI	P3[-]m			3.599		11.859											interlayer distance , d = 11.859	K			13.1	12.5		1.5	12.5											Oe	M-H curve, GL			46																																																																																	RE dissolved in liquid ammonia. MNCl (M=Zr,Hf) ws dispersed into (Re+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155551	SST026045017	M=NH3, y not measured. co-intercalation of Eu and NH3 into HfNCl.	Eu0.08(NH3)yHfNCl	Eu0.08M1Hf1N1Cl1	Eu	0.08	M	1	Hf	1	N	1	Cl	1															2013					myu-B/mol	7.56																						SmSI	P3[-]m			3.582		11.914											interlayer distance , d = 11.914	K			24.7	24.3		2.5	24.3											Oe	M-H curve, GL		18	72					T	RES(on), WHH		37	9					T/K	RES(on)		2.1	0.5	MHC155551		A	from Hc2		60.5	14.8	A	Hc1, GL theory		2980	12240																																																			RE dissolved in liquid ammonia. MNCl (M=Zr,Hf) ws dispersed into (Re+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155552	SST026045017	M=NH3, y not measured. co-intercalation of Eu and NH3 into HfNCl.	Eu0.13(NH3)yHfNCl	Eu0.13M1Hf1N1Cl1	Eu	0.13	M	1	Hf	1	N	1	Cl	1															2013					myu-B/mol	7.42																						SmSI	P3[-]m			3.58		11.9											interlayer distance , d = 11.90	K				24.1			24.1																																																																																																RE dissolved in liquid ammonia. MNCl (M=Zr,Hf) ws dispersed into (Re+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155553	SST026045017	M=NH3, y not measured. co-intercalation of Eu and NH3 into HfNCl.	Yb0.11(NH3)yHfNCl	Yb0.11M1Hf1N1Cl1	Yb	0.11	M	1	Hf	1	N	1	Cl	1															2013					myu-B/mol	4.64																						SmSI	P3[-]m			3.5876		12.007											interlayer distance , d = 12.007	K			23.3	23		2.7	23											Oe	M-H curve, GL			74																																																																																	RE dissolved in liquid ammonia. MNCl (M=Zr,Hf) ws dispersed into (Re+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155554	SST026045017	M = THF (tetrahydrofuran). co-intercalation of Eu and THF	Eu0.13(THF)HfNCl	Eu0.13M1Hf1N1Cl1	Eu	0.13	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																	K				25.8			25.8																																																																																																					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155555	SST026045017	M = PC (propylene carbonate).  co-intercalation of Eu and PC	Eu0.13(PC)HfNCl	Eu0.13M1Hf1N1Cl1	Eu	0.13	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																	K				25.6			25.6																																																																																																					Superconductivity of metal nitride chloride beta-MNCl (M = Zr, Hf) with rare-earth metal RE (RE = Eu, Yb) doped by intercalation			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)045017	Shuai Zhang,Masashi Tanaka,Takahiro Onimaru,Toshiro Takabatake,Yosikazu Isikawa,Shoji Yamanaka		
155556	SST026085015		Ba0.33HfNCl	Ba0.33Hf1N1Cl1	Ba	0.33	Hf	1	N	1	Cl	1																	2013																												SmSI	P3[-]m																interlayer distance , d = 10.3931	K				20.2			20.2																																																																																																AE dissolved in liquid ammonia. HfNCl  ws dispersed into (AE+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155557	SST026085015		Sr0.38HfNCl	Sr0.33Hf1N1Cl1	Sr	0.33	Hf	1	N	1	Cl	1																	2013																												SmSI	P3[-]m																interlayer distance , d = 10.2564	K				20.3			20.3																																																																																																AE dissolved in liquid ammonia. HfNCl  ws dispersed into (AE+liq.NH3) for 2 h to complete intercalation in dry ice bath.					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155558	SST026085015	M=NH3, y not measured. co-intercalation of Ca and NH3 into HfNCl.	Cax(NH3)yHfNCl	Ca0.4M1Hf1N1Cl1	Ca	0.4	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 11.814	K				22.4			22.4	MTC155558																																																																																																				Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155559	SST026085015	M=NH3, y not measured. co-intercalation of Ca and NH3 into HfNCl.	Cax(NH3)yHfNCl	Ca0.29M1Hf1N1Cl1	Ca	0.29	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 11.859	K				22.7			22.7																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155560	SST026085015	M=NH3, y not measured. co-intercalation of Ca and NH3 into HfNCl.	Cax(NH3)yHfNCl	Ca0.24M1Hf1N1Cl1	Ca	0.24	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 11.937	K				22.8			22.8	MTC155560																																																																																																				Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155561	SST026085015	M=NH3, y not measured. co-intercalation of Ca and NH3 into HfNCl.	Cax(NH3)yHfNCl	Ca0.11M1Hf1N1Cl1	Ca	0.11	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 12.045	K				23.3			23.3																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155562	SST026085015	M=NH3, y not measured. co-intercalation of Sr and NH3 into HfNCl.	Srx(NH3)yHfNCl	Sr0.09M1Hf1N1Cl1	Sr	0.09	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 12.244	K				24.1			24.1	MTC155562																																																																																																				Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155563	SST026085015	M=NH3, y not measured. co-intercalation of Sr and NH3 into HfNCl.	Srx(NH3)yHfNCl	Sr0.24M1Hf1N1Cl1	Sr	0.24	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																	K				24.1			24.1																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155564	SST026085015	M=NH3, y not measured. co-intercalation of Ba and NH3 into HfNCl.	Bax(NH3)yHfNCl	Ba0.1M1Hf1N1Cl1	Ba	0.1	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 12.174	K				24.5			24.5	MTC155564																																																																																																				Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155565	SST026085015	M = THF (tetrahydrofuran). co-intercalation of Ba and THF	Bax(THF)HfNCl	Ba0.1M1Hf1N1Cl1	Ba	0.1	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 14.439	K				25.7			25.7																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155566	SST026085015	M = THF (tetrahydrofuran). co-intercalation of Ca and THF	Cax(THF)HfNCl	Ca0.11M1Hf1N1Cl1	Ca	0.11	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 15.047	K				26			26	MTC155566																			T	SUS, WHH		61	15					T/K	SUS		3.3	0.8	MHC155566		A	from Hc2		46.8	11.5																																																													Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155567	SST026085015	M = THF (tetrahydrofuran). co-intercalation of Sr and THF.  Anisotropy(Hc2) = 4.1	Srx(THF)HfNCl	Sr0.24M1Hf1N1Cl1	Sr	0.24	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 15.396	K				25.6			25.6																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155568	SST026085015	M = PC (propylene carbonate).  co-intercalation of Ca and PC	Cax(PC)HfNCl	Ca0.11M1Hf1N1Cl1	Ca	0.11	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 18.768	K				25.6			25.6																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155569	SST026085015	M = PC (propylene carbonate).  co-intercalation of Sr and PC	Srx(PC)HfNCl	Sr0.24M1Hf1N1Cl1	Sr	0.24	M	1	Hf	1	N	1	Cl	1															2013																												SmSI	P3[-]m																interlayer distance , d = 18.955	K				25.1			25.1																																																																																																					Superconductivity of layered  beta-HfNCl with varying electron-doping concentrations and interlayer spacings			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)085015	Shuai Zhang,Masashi Tanaka,Haikui Zhu,Shoji Yamanaka		
155600	SST026122001	interlayer distance d = 9.464 A. Anisotropy (Hc2) = 1.3	alpha-K0.21TiNBr	K0.21Ti1N1Br1	K	0.21	Ti	1	N	1	Br	1																	2013																												FeOCl	Immm		A	4.0259	3.3769	18.927											alpha-type	K				17.2			17.2	MTC155600									49																								MHC155600		A		53	41		A		3045																																																					TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155601	SST026122001	interlayer distance d = 8.942	alpha-Na0.23TiNBr	Na0.23Ti1N1Br1	Na	0.23	Ti	1	N	1	Br	1																	2013																													Bmmb		A	4.01	3.37	17.884											alpha-type	K				15.2			15.2										32																																																																																						TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155602	SST026122001	interlayer distance d = 9.691 A	alpha-Rb0.22TiNBr	Rb0.22Ti1N1Br1	Rb	0.22	Ti	1	N	1	Br	1																	2013																													Immm		A	4.0187	3.3803	19.382											alpha-type	K				16.3			16.3										20																																																																																						TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155603	SST026122001	interlayer distance d = 8.296 A	TiNBr	Ti1N1Br1	Ti	1	N	1	Br	1																			2013																													Pmmn		A	3.9287	3.3508	8.2961											alpha-type	K					0																																																																																																		TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155604	SST026122001	M=THF. interlayer distance d = 14.186 A	alpha-Li0.37(THF)yTiNBr	Li0.37M1Ti1N1Br1	Li	0.37	M	1	Ti	1	N	1	Br	1															2013																													Immm		A	3.995	3.362	28.371											alpha-type	K				7.5			7.5										7.5																																																																																						TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155605	SST026122001	M=THF.  interlayer distance d = 12.9 A	Na0.23(THF)TiNBr	Na0.23M1Ti1N1Br1	Na	0.23	M	1	Ti	1	N	1	Br	1															2013																																													alpha-type	K				11			11																																																																																																TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155606	SST026122001	M=PC.  interlayer distance d = 15.7 A	Na0.23(PC)TiNBr	Na0.23M1Ti1N1Br1	Na	0.23	M	1	Ti	1	N	1	Br	1															2013																																													alpha-type	K				8.6			8.6																																																																																																TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155607	SST026122001	interlayer distance	alpha-K0.46TiNBr	K0.46Ti1N1Br1	K	0.46	Ti	1	N	1	Br	1																	2013																															A	4.0329	3.3774	18.9332											alpha-type	K				16.3			16.3										12																																																																																						TiBr4 - (ammonia steam at 100C for a few hours) - heat(250C,3h) - sealed in Pyrex with NH4Br - heat(270-360C gradient,1w). Intercalation(0.1M A-naphthalene + THF)					Superconductivity of alkali metal intercalated TiNBr with alpha-type nitride layers			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8527, Japan	Supercond.Sci.Technol., 26(2013)122001	Shuai Zhang,Masashi Tanaka,ErikaWatanabe,Haikui Zhu,Kei Inumaru,Shoji Yamanaka		
155608	SST027025012	RRR = 4.7. SP-heat, beta=0.279 mJ/mol.K4, delta=0.0011 mJ/mol.K6. (dC/gamma:Tc) = 1.54. Tc(P) = -0.16P^2 + 0.06P + 6.02.	Zr2Ru3Si4	Zr2Ru3Si4	Zr	2	Ru	3	Si	4																		1	2014																										A2B3C4		Hf2Ru3Si4	C2/c		A	18.98	5.348	13.28											monoclinic, beta = 127.73 degree	K	5.5		6	5.7			5.7	MTC155608									100	Oe	M-H curve	100							T	RES(0.5Rn), linear approx.	10							T/K	RES(0.5Rn)	1			MHC155608		A	from Hc2	60										3.5	14				MSP155608			mJ/mol.K2	13.1	SP	191	SP											uOhm.cm											240												Zr(3N),Ru(3N),Si(10N)		arc-melting. (Zr:Ru:Si = 20:35:45) - ANN(1270K,100h, in alumina crucible, sealed in quartz tube(Ar)) - FC to RT					Superconducting properties of the ternary transition-metal silicide Zr2Ru3Si4			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	Supercond.Sci.Technol., 27(2014)025012	Soshi Ibuka,Motoharu Imai,Takashi Naka,Mitsuaki Nishio		
155609	SST027025012	not SC	Hf2Ru3Si4	Hf2Ru3Si4	Hf	2	Ru	3	Si	4																		1	2014																										A2B3C4		Hf2Ru3Si4	C2/c																	K					1.8																																																																																																							Superconducting properties of the ternary transition-metal silicide Zr2Ru3Si4			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	Supercond.Sci.Technol., 27(2014)025012	Soshi Ibuka,Motoharu Imai,Takashi Naka,Mitsuaki Nishio		
155610	SST027025012	not SC	Yb2Ru3Ge3	Yb2Ru3Ge4	Yb	2	Ru	3	Ge	4																		1	2014																										A2B3C4		Hf2Ru3Si4	C2/c																	K					1.8																																																																																																							Superconducting properties of the ternary transition-metal silicide Zr2Ru3Si4			National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	Supercond.Sci.Technol., 27(2014)025012	Soshi Ibuka,Motoharu Imai,Takashi Naka,Mitsuaki Nishio		
155611	SST027055005	R(T) measured on a cleaved surface. Tc(SP) = 0.6 K. Lattice term in SP (beta) = 1.39 mJ/mol.K4	Ca2InN	Ca2In1N1	Ca	2	In	1	N	1																			2014																										ABC2			Cmcm		A	3.52	20.2	4.96											Ca2 intercalated InN	K		0.6	0.7				0.6										78																																											MSP155611	mJ/mol.K	2.85	mJ/mol.K2	4.24	SP	322	SP											mOhm.cm											27														mixture(Ca2N+In) - pellet - wrapped in Mo-foil - sealed in silica ampoule(Ar) - heat(873K,50h)					Superconductivity of Ca2InN with a layered structure embedding an anionic indium chain array			Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Japan	Supercond.Sci.Technol., 27(2014)055005	Sehoon Jeong,Satoru Matsuishi,Kimoon Lee,Yoshitake Toda,Sung Wng Kim,Hideo Hosono		
155612	SST027075012	FM order Tm = 16.5 K. SC Tc(on) = 22.5K, Tc(zero) = 10K. reentrant SC. Eu(2+)-AFM order coexists with SC.	Eu(Fe,Ir)2As2	Eu1Fe1.72Ir0.28As2	Eu	1	Fe	1.72	Ir	0.28	As	2																3	2014							16.5																			AB2C2		ThCr2Si2			A	3.932		12.056												K			21.9				21.9																																																					MSP155612			mJ/mol.K2	35	SP	307	SP																																		FeAs,IrAs		self-flux method. Eu:[(FeAs)1-x(IrAs)x] = 1:4  - in alumina crucible - sealed in Ta tube - heat(1200C,5h) - cool to 1030C (3C/h) - FC to RT					Magnetic and superconducting properties of Ir-doped EuFe2As2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	Supercond.Sci.Technol., 27(2014)075012	U B Paramanik,P L Paulose,S Ramakrishnan,A K Nigam,C Geibel,Z Hossain		
155613	PLA3792498	GL(kappa) = 4.04. Lattice term in SP beta=0.22 mJ/mol.K4.	(Th,Zr)B12	Th0.93Zr0.07B12	Th	0.93	Zr	0.07	B	12																		1	2015																										AB12	1	UB12	Fm-3m		A	7.465													cubic	K			5.5	5.5			5.5											mT	M-H curve	6							T	RES(0.5Rn), WHH	0.098												MHC155613		A	from Hc2	579			A	from Hc1	2340			meV	0.8						MSP155613			mJ/mol.K2	17.1	SP	486	SP																																				arc-mwlting					Superconductivity in the Th0.93Zr0.07B12 compound with UB12 prototype structure			Departamento de Engenharia de Materiais, Escola de Engenharia de Lorena, Universidade de Sao Paulo-Lorena, SP 12602-810, Brazil	Phys.Lett.A, 379(2015)2498	S.T.Renosto,L.E.Correa,M.S.daLuz,P.F.S.Rosa,Z.Fisk,J.Albino-Aguiar,A.J.S.Machado		
155614	ACS13413558	meta-stable at AP. e-ph = 0.6, (dC/gamma*Tc) = 1.05-1.17	CaSi3	Ca1Si3	Ca	1	Si	3																					2012									2.76																	AB3	2		I4/mmm	139	A	7.2676		11.3501												K		4.25	4.5	4.5			4.25										1.4										T	SP(mid),WHH	0.048																															MSP155614			mJ/mol.K2	4.81	SP	514	SP																																		CaSi2(YSi2 or LuSi2),Si(6N)		High-T-High-P synthesis (900-1400 C, 12-15 GPa)					Dumbbells of Five-Connected Silicon Atoms and Superconductivity in the Binary Silicides MSi3 (M = Ca, Y, Lu)			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	J.Am.Chem.Soc., 134(2012)13558	Ulrich Schwarz,Aron Wosylus,Helge Rosner,Walter Schnelle,Alim Ormeci,Katrin Meier,Alexey Baranov,Michael Nicklas,Susann Leipe,Carola J. Muller,Yuri Grin		
155615	ACS13413558	meta-stable at AP. e-ph = 0.6, (dC/Tc) = 7.6, (dC/gamma*Tc) = 1.42	YSi3	Si3Y1	Si	3	Y	1																					2012									4.07																	AB3	2		I4/mmm	139	A	7.231		10.792												K		4.63	5				4.63										1.4										T	SP(mid),WHH	0.08																															MSP155615			mJ/mol.K2	5.16	SP	451	SP																																		CaSi2(YSi2 or LuSi2),Si(6N)		High-T-High-P synthesis (900-1400 C, 12-15 GPa)					Dumbbells of Five-Connected Silicon Atoms and Superconductivity in the Binary Silicides MSi3 (M = Ca, Y, Lu)			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	J.Am.Chem.Soc., 134(2012)13558	Ulrich Schwarz,Aron Wosylus,Helge Rosner,Walter Schnelle,Alim Ormeci,Katrin Meier,Alexey Baranov,Michael Nicklas,Susann Leipe,Carola J. Muller,Yuri Grin		
155616	ACS13413558	nominal = LuSi3 + 2Si(cI16). meta-stable at AP. e-ph = 0.65, (dC/Tc) = 9.4, (dC/gamma*Tc) = 1.50	LuSi3	Lu1Si3	Lu	1	Si	3																					2012									6.37																	AB3	2		I4/mmm	139	A	7.1835		10.471												K		6.78	7.1	7			6.78										2.1										T	SP(mid),WHH	0.234																															MSP155616			mJ/mol.K2	6.26	SP	365	SP																																		CaSi2(YSi2 or LuSi2),Si(6N)		High-T-High-P synthesis (900-1400 C, 12-15 GPa)					Dumbbells of Five-Connected Silicon Atoms and Superconductivity in the Binary Silicides MSi3 (M = Ca, Y, Lu)			Max-Planck-Institut fur Chemische Physik fester Stoffe, 01187 Dresden, Germany	J.Am.Chem.Soc., 134(2012)13558	Ulrich Schwarz,Aron Wosylus,Helge Rosner,Walter Schnelle,Alim Ormeci,Katrin Meier,Alexey Baranov,Michael Nicklas,Susann Leipe,Carola J. Muller,Yuri Grin		
155617	IJIM0020581	Zn-intercalated beta-ZrNCl. Volume fraction varies with synthesis conditions. Max = 75 %.	beta-Zn0.04ZrNCl	Zn0.04Zr1N1Cl1	Zn	0.04	Zr	1	N	1	Cl	1																	2000																										ABC	7				A	3.58													hexagonal	K				15			15										75																																																																																						Zn intercalation by electrochemical method					Novel superconductors obtained by electrochemical Zn intercalation of beta-ZrNCl and related compounds			Departmento de Quimica Inorganica, Facultad de Ciencias Quimicas, Universidad Complutense, 28040, Madrid, Spain	Int.J.Inorg.Mater., 2(2000)581	M.E. Arroyo y de Dompablo,E. Morana,M.A . Alario-Franco,F. Drymiotis,A.D. Bianchi,Z. Fisk		
155618	IJIM0020581	Zn-intercalated beta-ZrNBr. Volume fraction decreases with the time of air exposure (from 86 to 66 %)	beta-Zn0.035ZrNBr	Zn0.035Zr1N1Br1	Zn	0.035	Zr	1	N	1	Br	1																	2000																										ABC	7				A	3.552													hexagonal	K				14			14										86																																																																																						Zn intercalation by electrochemical method					Novel superconductors obtained by electrochemical Zn intercalation of beta-ZrNCl and related compounds			Departmento de Quimica Inorganica, Facultad de Ciencias Quimicas, Universidad Complutense, 28040, Madrid, Spain	Int.J.Inorg.Mater., 2(2000)581	M.E. Arroyo y de Dompablo,E. Morana,M.A . Alario-Franco,F. Drymiotis,A.D. Bianchi,Z. Fisk		
155619	CEM2260024	not SC. Mg3+xNi7-xB2 prepared and measured magnetic properties. Spin freezing temperature = 33 K.	Mg3Ni7B2	Mg4Ni6B2	Mg	4	Ni	6	B	2																			2015																										A2B4C6			R-3m	166																K							4																																																																																														Mg(3N),Ni(3N5),B(2N5)		Solid state reaction					Preparation and properties of a new ternary phase Mg3+xNi7-xB2 (0.17 =< x =< 0.66) and its Cu-doping effect			Institute of Physics, Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics, Beijing 100190, China	J.Solid State Chem., 226(2015)24	Chang-Zhong  Liao,Cheng Dong,Kaimin Shih,Lingmin Zeng,Bing He,Wenhuan Cao,Lihong Yang		
155620	INO05110300	Compositions are nominal values. multi-phase: Mg(Mg0.25Al0.75)Si (major phase) + Mg9Si5 + Al + Si by EPMA.	MgAlSi	Mg1Al1Si1	Mg	1	Al	1	Si	1																			2012																										ABC			Pnma		A	6.9242	4.138	7.9618												K			5.7	6			6																																																																																																High-P-High-T synthesis (5 GPa, 1000 C) - Q to RT					High Pressure Synthesis and Superconductivity of the Ternary Compounds Mg(Mg1-xAlx)Si with the Anticotunnite Structure			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 51(2012)10300	Shidong Ji,Masashi Tanaka,Shuai Zhang,Shoji Yamanaka		
155621	INO0526039	Laves phase composed of truncated tetragonal cages.	Ca(Al,Si)2	Ca1Al1Si1	Ca	1	Al	1	Si	1																			2013																										AB2		Laves			A	7.8112														K				2.6			2.6	MTC155621										Oe	M-H curve				5			1.9	T	SUS, WHH	0.27							T/K	SUS	0.15			MHC155621		A	from Hc2	350																																																										High-P-High-T synthesis (13 GPa, 1000C)					High-Pressure Synthesis and Superconductivity of the Laves Phase Compound Ca(Al,Si)2 Composed of Truncated Tetrahedral Cages Ca@(Al,Si)12			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorg. Chem., 52(2013)6039	Masashi Tanaka,Shuai Zhang,Kei Inumaru,Shoji Yamanaka		
155622	JAC6340208		(Ba,K)(Bi,Pb)O3	Ba0.82K0.18Bi0.53Pb0.47	Ba	0.82	K	0.18	Bi	0.53	Pb	0.47																	2015									7.91																	ABC3	1		Pm-3[-]m	221	A	4.28877													cubic	K			15	22.8			22.8										64																																																																																						Hydrothermal reaction at 240 C.					Hydrothermal synthesis of a new Bi-based (Ba0.82K0.18)(Bi0.53Pb0.47)O3 superconductor			Center for Crystal Science and Technology, University of Yamanashi, 7-32 Miyamae-cho, Kofu 400-8511, Japan	J.Alloys Compd., 634(2015)208	Mirza H.K. Rubel,Takahiro Takei,Nobuhiro Kumada,M.M. Ali,Akira Miura,Kiyoharu Tadanaga,K. Oka,M. Azuma,E. Magomae,C. Moriyoshi,Y. Kuroiwa		
155623	JPS084023705	Tsai-type approximant. gamma in mJ/k2.mol-cluster. kappa(GL)=28.6. (dC/Tc) = 138 mJ/K2.mol-cluster. (dC/gamma*Tc) = 1.26. Hc(0) = 78.7 Oe.	Au64Ge22Yb14	Au64Ge22Yb14	Au	64	Ge	22	Yb	14																			2015																															A	14.724													Tsai-type approximant	K		0.68		0.68			0.68											Oe		6.7							T	RES,WHH	0.276							T/K	RES	0.584			MHC155623		A	from Hc2	322			A	from Hc1	9200										MSP155623			mJ/mol.K2	109	SP	160	SP											uOhm.cm							150																Au(4N),Ge(5N),Yb(3N)		mixture - alumina crucible - sealed in quartz tube - heat to 1000C - cool to 800C- cool to 450C - Q to water					Superconductivity of Au-Ge-Yb Approximants with Tsai-Type Clusters			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)023705	Kazuhiko Deguchi,Mika Nakayama,Shuya Matsukawa,Keiichiro Imura,Katsumasa Tanaka,Tsutomu Ishimasa,Noriaki K. Sato		
155624	JPS084023705	Tsai-type approximant. gamma in mJ/k2.mol-cluster. kappa(GL)=25.9. (dC/Tc) = 218 mJ/K2.mol-cluster. (dC/gamma*Tc) = 0.54. Hc(0) = 50.0 Oe.	Au63.5Ge20.5Yb16.0	Au63.5Ge20.5Yb16	Au	63.5	Ge	20.5	Yb	16																			2015																															A	14.605													Tsai-type approximant	K		0.36		0.36			0.36													4.5							T	RES,WHH	0.165							T/K	RES	0.675			MHC155624		A	from Hc2	424			A	from Hc1	11000										MSP155624			mJ/mol.K2	251	SP	157	SP											uOhm.cm							134.9																Au(4N),Ge(5N),Yb(3N)		mixture - alumina crucible - sealed in quartz tube - heat to 1000C - cool to 800C- cool to 450C - slow cool to RT					Superconductivity of Au-Ge-Yb Approximants with Tsai-Type Clusters			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)023705	Kazuhiko Deguchi,Mika Nakayama,Shuya Matsukawa,Keiichiro Imura,Katsumasa Tanaka,Tsutomu Ishimasa,Noriaki K. Sato		
155625	MAT1408.2625	filamentary SC.	(Ce,Nd)(O,F)BiS2	Ce0.2Nd0.8F0.3Bi1S2O0.7	Ce	0.2	Nd	0.8	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	4.0143		13.6366											BiS2-layer SC	K				2.35			2.35																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155626	MAT1408.2625		(Ce,Nd)(O,F)BiS2	Nd1F0.3Bi1S2O0.7	Nd	1	F	0.3	Bi	1	S	2													O	0.7			2014																										ABCD2			P4/nmm		A	4.0104		13.5751											BiS2-layer SC	K				3.52			3.52																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155627	MAT1408.2625		(Ce,Nd)(O,F)BiS2	Ce0.6Nd0.4F0.5Bi1S2O0.5	Ce	0.6	Nd	0.4	F	0.5	Bi	1	S	2											O	0.5			2014																										ABCD2			P4/nmm		A	4.0313		13.5133											BiS2-layer SC	K				2.98			2.98																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155628	MAT1408.2625		(Ce,Nd)(O,F)BiS2	Ce0.2Nd0.8F0.5Bi1S2O0.5	Ce	0.2	Nd	0.8	F	0.5	Bi	1	S	2											O	0.5			2014																										ABCD2			P4/nmm		A	4.0187		13.4881											BiS2-layer SC	K				4.46			4.46																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155629	MAT1408.2625		(Ce,Nd)(O,F)BiS2	Nd1F0.5Bi1S2O0.5	Nd	1	F	0.5	Bi	1	S	2													O	0.5			2014																										ABCD2			P4/nmm		A	4.0034		13.4639											BiS2-layer SC	K				4.78			4.78																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155630	MAT1408.2625	filamentary SC. not bulk SC	(Ce,Nd)(O,F)BiS2	Ce1F0.7Bi1S2O0.7	Ce	1	F	0.7	Bi	1	S	2													O	0.7			2014																										ABCD2			P4/nmm		A	4.0496		13.4378											BiS2-layer SC	K				2.68			2.68																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155631	MAT1408.2625	filamentary SC. not bulk SC	(Ce,Nd)(O,F)BiS2	Ce0.6Nd0.4F0.7Bi1S2O0.7	Ce	0.6	Nd	0.4	F	0.7	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	4.0246		13.3937											BiS2-layer SC	K				3.25			3.25																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155632	MAT1408.2625	filamentary SC. not bulk SC	(Ce,Nd)(O,F)BiS2	Ce0.2Nd0.8F0.7Bi1S2O0.7	Ce	0.2	Nd	0.8	F	0.7	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	4.0103		13.4216											BiS2-layer SC	K				4.29			4.29																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155633	MAT1408.2625	filamentary SC. not bulk SC	(Ce,Nd)(O,F)BiS2	Nd1F0.7Bi1S2O0.7	Nd	1	F	0.7	Bi	1	S	2													O	0.7			2014																										ABCD2			P4/nmm		A	4.0013		13.4231											BiS2-layer SC	K				4.78			4.78																																																																																														Ce2S3,Nd2S3,Bi2O3,BiF3,BiF3,Bi2S3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155634	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.8Sm0.2F0.3Bi1S2O0.7	Nd	0.8	Sm	0.2	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	4.011		13.5727											BiS2-layer SC	K				4.9			4.9																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155635	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.6Sm0.4F0.3Bi1S2O0.7	Nd	0.6	Sm	0.4	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	3.9784		13.4572											BiS2-layer SC	K				5.21			5.21																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155636	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.2Sm0.8F0.3Bi1S2O0.7	Nd	0.2	Sm	0.8	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	3.9817		13.4877											BiS2-layer SC	K				5.58			5.58																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155637	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.8Sm0.2F0.3Bi1S2O0.5	Nd	0.8	Sm	0.2	F	0.3	Bi	1	S	2											O	0.5			2014																										ABCD2			P4/nmm		A	3.9986		13.4627											BiS2-layer SC	K				5.1			5.1																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155638	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.8Sm0.2F0.3Bi1S2O0.5	Nd	0.8	Sm	0.2	F	0.3	Bi	1	S	2											O	0.5			2014																										ABCD2			P4/nmm		A	3.9885		13.5351											BiS2-layer SC	K				5.3			5.3																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155639	MAT1408.2625		(Nd,Sm)(O,F)BiS2	Nd0.6Sm0.4F0.3Bi1S2O0.5	Nd	0.6	Sm	0.4	F	0.3	Bi	1	S	2											O	0.5			2014																										ABCD2			P4/nmm		A	3.9809		13.54											BiS2-layer SC	K				5.52			5.52																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155640	MAT1408.2625	not bulk SC	(Nd,Sm)(O,F)BiS2	Nd0.4Sm0.6F0.3Bi1S2O0.7	Nd	0.4	Sm	0.6	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	3.9893		13.3738											BiS2-layer SC	K				4.66			4.66																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155641	MAT1408.2625	not bulk SC	(Nd,Sm)(O,F)BiS2	Nd0.8Sm0.2F0.3Bi1S2O0.7	Nd	0.8	Sm	0.2	F	0.3	Bi	1	S	2											O	0.7			2014																										ABCD2			P4/nmm		A	3.9844		13.1607											BiS2-layer SC	K				4.59			4.59																																																																																														Nd2S3,Sm2S3,Bi2O3,BiF3,Bi2S3,Bi,		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,10h) - redround - sealed in quartz tube - hea again					Chemical pressure effect on superconductivity of BiS2-based Ce1-xNdxO1-yFyBiS2 and Nd1-zSmzO1-yFyBiS2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, 192-0397	cond-mat/1408.2625	Joe Kajitani,Takafumi Hiroi,Atsushi Omachi,Osuke Miura,Yoshikazu Mizuguchi		
155642	MRB0660231	as-synthesized (not oxygenated)  sample has Tc = 151.00 K. R(T) metallic.	RuSr2GdCu2Oz	Ru1Sr2Gd1Cu2Oz	Ru	1	Sr	2	Gd	1	Cu	2													O	z		1	2015								139.63																		ABC2D2E8		Ru1212	P4/mmm	123	A	3.845		11.571												K		33.1	39.2				33.1																																																																																																solid state reaction with excess CuO. mixture - pellet - heat(1050C,45h). then oxygennated in quartz tube					Magnetic, electrical and structural properties of the Re-doped ruthenocuprate Ru1-xRexSr2GdCu2Oy			Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Mater.Res.Bull., 66(2015)231	L.T. Corredor,J. Albino Aguiar,D.A. Landinez Tellez,P. Pureur,F. Mesquita,J. Roa-Rojas		
155643	MRB0660231	as-synthesized (not oxygenated)  sample has Tc = 143.45 K. R(T) semicond-like	(Ru,Re)Sr2GdCu2Oz	Ru0.97Re0.03Sr2Gd1Cu2Oz	Ru	0.97	Re	0.03	Sr	2	Gd	1	Cu	2											O	z		1	2015								123.47																		ABC2D2E8		Ru1212	P4/mmm	123	A	3.834		11.548												K			9.96				9.96																																																																																																solid state reaction with excess CuO. mixture - pellet - heat(1050C,45h). then oxygennated in quartz tube					Magnetic, electrical and structural properties of the Re-doped ruthenocuprate Ru1-xRexSr2GdCu2Oy			Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Mater.Res.Bull., 66(2015)231	L.T. Corredor,J. Albino Aguiar,D.A. Landinez Tellez,P. Pureur,F. Mesquita,J. Roa-Rojas		
155644	MRB0660231	as-synthesized (not oxygenated)  sample has Tc = 150.98 K. R(T) semicond-like	(Ru,Re)Sr2GdCu2Oz	Ru0.94Re0.06Sr2Gd1Cu2Oz	Ru	0.94	Re	0.06	Sr	2	Gd	1	Cu	2											O	z		1	2015								119.7																		ABC2D2E8		Ru1212	P4/mmm	123	A	3.835		11.531												K			9.86				9.86																																																																																																solid state reaction with excess CuO. mixture - pellet - heat(1050C,45h). then oxygennated in quartz tube					Magnetic, electrical and structural properties of the Re-doped ruthenocuprate Ru1-xRexSr2GdCu2Oy			Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Mater.Res.Bull., 66(2015)231	L.T. Corredor,J. Albino Aguiar,D.A. Landinez Tellez,P. Pureur,F. Mesquita,J. Roa-Rojas		
155645	MRB0660231	not SC. as-synthesized (not oxygenated)  sample has Tc = 146.99 K. R(T) semicond-like	(Ru,Re)Sr2GdCu2Oz	Ru0.91Re0.09Sr2Gd1Cu2Oz	Ru	0.91	Re	0.09	Sr	2	Gd	1	Cu	2											O	z		1	2015								146.41																		ABC2D2E8		Ru1212	P4/mmm	123	A	3.837		11.493												K					4																																																																																																		solid state reaction with excess CuO. mixture - pellet - heat(1050C,45h). then oxygennated in quartz tube					Magnetic, electrical and structural properties of the Re-doped ruthenocuprate Ru1-xRexSr2GdCu2Oy			Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Mater.Res.Bull., 66(2015)231	L.T. Corredor,J. Albino Aguiar,D.A. Landinez Tellez,P. Pureur,F. Mesquita,J. Roa-Rojas		
155646	MRB0660231	not SC. as-synthesized (not oxygenated)  sample has Tc = 153.90 K. R(T) semicond-like	(Ru,Re)Sr2GdCu2Oz	Ru0.88Re0.12Sr2Gd1Cu2Oz	Ru	0.88	Re	0.12	Sr	2	Gd	1	Cu	2											O	z		1	2015								153.95																		ABC2D2E8		Ru1212	P4/mmm	123	A	3.836		11.515												K					4																																																																																																		solid state reaction with excess CuO. mixture - pellet - heat(1050C,45h). then oxygennated in quartz tube					Magnetic, electrical and structural properties of the Re-doped ruthenocuprate Ru1-xRexSr2GdCu2Oy			Departamento de Fisica, Universidade Federal de Pernambuco, 50670-901 Recife, PE, Brazil	Mater.Res.Bull., 66(2015)231	L.T. Corredor,J. Albino Aguiar,D.A. Landinez Tellez,P. Pureur,F. Mesquita,J. Roa-Rojas		
155647	NATP0090349	(dTc/dP) = -0.106 K/kbar for P < Pc(= 16.1kbar) change to +0.04 K/kbar for P > Pc.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2																		K	2.74		3.41				3.075	MTC155647		K/GPa	-1.06																																																																																	m3/C	0.0000000004															Sudden reversal in the pressure dependence of Tc in the iron-based superconductor KFe2As2			Departement de physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, J1K 2R1, Canada	Nature Phys., 9(2013)349	F. F. Tafti,A. Juneau-Fecteau,M-E.. Delage,S. Rene de Cotret,J-Ph. Reid,A. F.Wang,X-G. Luo,X. H. Chen,N. Doiron-Leyraud,Louis Taillefer		
155648	NATP0090349	(dTc/dP) = -0.29 K/kbar (only 2 Tc point)	K(Fe,Co)2As2	K1Fe1.932Co0.068As2	K	1	Fe	1.932	Co	0.068	As	2																3	2013																										AB2C2		ThCr2Si2																		K	1.7		1.99				1.845																																																																							uOhm.cm							3.8																							Sudden reversal in the pressure dependence of Tc in the iron-based superconductor KFe2As2			Departement de physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, J1K 2R1, Canada	Nature Phys., 9(2013)349	F. F. Tafti,A. Juneau-Fecteau,M-E.. Delage,S. Rene de Cotret,J-Ph. Reid,A. F.Wang,X-G. Luo,X. H. Chen,N. Doiron-Leyraud,Louis Taillefer		
155649	PRB090045136	RRR = 4.3. dH3/dP = -4.64 mT/kbar. Hc3(0) = 450 mT(=1.6 Hc2). Hc3 defined as surface Hc2 //plane. Tc defined as thepeak of dR/dT or d(SUS)/dT.	YB6	B6Y1	B	6	Y	1																				3	2014																		GPa		166						AB6		CaB6	Pm3m																	K		7.5					7.5	MTC155649		K/GPa	-0.44							mT		36							T		0.28							T/K					MHC155649																																					uOhm.cm							10																		Floating zone method. melting in 5bar-Ar					High-pressure effect on the superconductivity of YB6			Centre of Low Temperature Physics, Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 90(2014)045136	S. Gabani,I. Takacova,G. Pristas,E. Gazo,K. Flachbart,T. Mori,D. Braithwaite,M. Misek,K. V. Kamenev,M. Hanfland,P. Samuely		
155650	PRB090045136	RRR = 2.5. (dTc/dP) = -0.44 K/GPa for P < 5GPa and = -0.15 K/GPa for P > 8 GPa.	YB6	B6Y1	B	6	Y	1																				3	2014																										AB6		CaB6	Pm3m																	K		5.9					5.9	MTC155650		K/GPa	-0.44																																																																			uOhm.cm							21																		Floating zone method. melting in 5bar-Ar					High-pressure effect on the superconductivity of YB6			Centre of Low Temperature Physics, Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 90(2014)045136	S. Gabani,I. Takacova,G. Pristas,E. Gazo,K. Flachbart,T. Mori,D. Braithwaite,M. Misek,K. V. Kamenev,M. Hanfland,P. Samuely		
155651	PRB090060504	multiple nodeless gap SC. RRR = 120. the ratio of small to large gap = 0.6 from thermal conductivity. k/T = k0/T + b*T^2 for T^2 < 0.16, k0/T = 0.18 mW/K2.cm.	TlNi2Se2	Tl1Ni2Se2	Tl	1	Ni	2	Se	2																		3	2014																										AB2C2		ThCr2Si2																		K				3.7			3.7																				T	thermal conductivity	0.8																																											MTHC155651																															self-flux method					Multigap nodeless superconductivity in nickel chalcogenide TlNi2Se2			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 90(2014)060504	X. C. Hong,Z. Zhang,S. Y. Zhou,J. Pan,Y. Xu,Hangdong Wang,Qianhui Mao,Minghu Fang,J. K. Dong,S. Y. Li		
155652	PRB090224513	SC appears in only low-T phase (orthorhombic). Filamentary SC for P > 0.5 GPa	Ca10(Ir4As8)(Fe2-xIrxAs2)5	Ca10Ir4Fe10As18	Ca	10	Ir	4	Fe	10	As	18																	2014								106																																					Ortho-, Ca-10-4-8	K	18.2		19.2				18.7	MPH155652																																																																						mOhm.cm								0.275															Ca,FeAs,IrAs2,Ir		mixture - in alumina crucible - sealed in quartz tube - heat(700C,3h) - heat(1100-1150C,10-40h) - Q to ice					Simultaneous suppression of superconductivity and structural phase transition under pressure in Ca10(Ir4As8)(Fe2-xIrxAs2)5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 90(2014)224513	Shunsaku Kitagawa,Shingo Araki,Tatsuo C. Kobayashi,Hiroyuki Ishii,Kazunori Fujimura,Daisuke Mitsuoka,Kazutaka Kudo,Minoru Nohara		
155653	PRB091125107	static magnetic order (FM-like) observed for T < 5.5 K. by NMR. Thermally intercalated into FeSe layer	(Li0.8Fe0.2)OHFeSe	Li0.8Fe1.2H1Se1	Li	0.8	Fe	1.2	H	1	Se	1																1	2015																																														K			34				34																																		MHC155653																																																														Hydrothermal reaction method					NMR evidence for field-induced ferromagnetism in (Li0.8Fe0.2)OHFeSe superconductor			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 91(2015)125107	Y. P. Wu,D. Zhao,X. R. Lian,X. F. Lu,N. Z. Wang,X. G. Luo,X. H. Chen,T. Wu		
155654	SSC1870018	AFM comes from Eu-moment. Fe-agnetic freezing of moments around 15 K from Mossbauer, muon-SR.	EuFe2(As0.7P0.3)2	Eu1Fe2As1.4P0.6	Eu	1	Fe	2	As	1.4	P	0.6																3	2014								18																		AB2C2		ThCr2Si2																		K		10					10										100										T	RES(0.5Rn), extrapolation			10										MHC155654																																																														See Phys.Rev.b, 82(2010)134509					Magnetism in superconducting EuFe2As1.4P0.6 single crystals studied by local probes			Centro Brasileiro de Pesquisas Fisicas, Rua Xavier Sigaud 150, Riode Janeiro, Brazil	Solid State Commun., 187(2014)18	J. Munevar,H.Micklitz,M.Alzamora,C.Arguello,T.Goko,F.L.Ning,T.Munsie,T.J.Williams,A.A.Aczel,G.M.Luke,G.F.Chen,W.Yu,Y.J.Uemura,E.Baggio-Saitovitch		
155655	PRB091174514		MgPtSi	Mg1Pt1Si1	Mg	1	Pt	1	Si	1																		1	2015																										ABC			Pnma	62	A	6.5324	4.1005	7.1752											TiNiSi-type	K	2.52		2.97	2.5		0.2	2.5										86										T	RES(0.5Rn), linear extrapolation	0.636												MHC155655		A	from Hc2	230																																																								Mg2Si,Pt,Si		mixture (Mg:Pt:Si = 10:7:25) - in alumina crucible - sealed in quartz tube - heat(1000C,12h) - FC to RT					Superconductivity in MgPtSi: An orthorhombic variant of MgB2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174514	Kazutaka Kudo,Kazunori Fujimura,Seiichiro Onari,Hiromi Ota,Minoru Nohara		
155656	PRB091174514		Mg(Pt,Au)Si	Mg1Pt0.5Au0.5Si1	Mg	1	Pt	0.5	Au	0.5	Si	1																1	2015																										ABC			Pnma	62															TiNiSi-type	K		2.9					2.9																																																																																														Mg2Si,Pt,Si		mixture (Mg:Pt:Si = 10:7:25) - in alumina crucible - sealed in quartz tube - heat(1000C,12h) - FC to RT					Superconductivity in MgPtSi: An orthorhombic variant of MgB2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174514	Kazutaka Kudo,Kazunori Fujimura,Seiichiro Onari,Hiromi Ota,Minoru Nohara		
155657	PRB091174514	not SC down to 1.8 K	MgRhSi	Mg1Rh1Si1	Mg	1	Rh	1	Si	1																		1	2015																										ABC			Pnma	62	A	6.5719	4.011	6.9798											TiNiSi-type	K					1.8																																																																																																Mg2Si,Pt,Si		mixture (Mg:Pt:Si = 10:7:25) - in alumina crucible - sealed in quartz tube - heat(1000C,12h) - FC to RT					Superconductivity in MgPtSi: An orthorhombic variant of MgB2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174514	Kazutaka Kudo,Kazunori Fujimura,Seiichiro Onari,Hiromi Ota,Minoru Nohara		
155658	PRB091174514	not SC down to 1.8 K	MgIrSi	Mg1Ir1Si1	Mg	1	Ir	1	Si	1																		1	2015																										ABC			Pnma	62	A	6.574	4.0149	6.9693											TiNiSi-type	K					1.8																																																																																																Mg2Si,Pt,Si		mixture (Mg:Pt:Si = 10:7:25) - in alumina crucible - sealed in quartz tube - heat(1000C,12h) - FC to RT					Superconductivity in MgPtSi: An orthorhombic variant of MgB2			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174514	Kazutaka Kudo,Kazunori Fujimura,Seiichiro Onari,Hiromi Ota,Minoru Nohara		
155659	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Li = 0.0843g, FeAs = 0.3001g, Liq. ammonia = 15ml, reaction duration = 10 days.	LiFe2Se2	Li1Fe2Se2	Li	1	Fe	2	Se	2																			2012																										AB2C2					A	3.775		17.04												K			44				44										32																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155660	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Na = 0.258g, FeAs = 0.3002g, Liq. ammonia = 15ml, reaction duration = 3 days.	NaFe2Se2	Na1Fe2Se2	Na	1	Fe	2	Se	2																			2012																										AB2C2					A	3.7846		17.432												K			46				46										40																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155661	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: K = 0.0290g, FeAs = 0.3999g, Liq. ammonia = 15ml, reaction duration = 2.5 days.	KFe2Se2	K1Fe2Se2	K	1	Fe	2	Se	2																			2012																										AB2C2																				K			40				40										11																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155662	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Ca = 0.0226g, FeAs = 0.3000g, Liq. ammonia = 10ml, reaction duration = 2 days.	Ca0.5Fe2Se2	Ca0.5Fe2Se2	Ca	0.5	Fe	2	Se	2																			2012																										AB2C2																				K			40				40										4																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155663	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Sr = 0.0814g, FeAs = 0.3131g, Liq. ammonia = 15ml, reaction duration = 13 days.	Sr0.8Fe2Se2	Sr0.8Fe2Se2	Sr	0.8	Fe	2	Se	2																			2012																										AB2C2																				K			38				38										60																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155664	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Ba = 0.1219g, FeAs = 0.3000g, Liq. ammonia = 10ml, reaction duration = 4 days. Lattice term in SP,  beta=0.36 uJ/g.K4	Ba0.8Fe2Se2	Ba0.8Fe2Se2	Ba	0.8	Fe	2	Se	2																			2012																										AB2C2					A	3.7781		16.8427												K			39				39										62	mT		150							T		36.5																																		uJ/g.K2	3.47	SP																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155665	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Eu = 0.0843g, FeAs = 0.3001g, Liq. ammonia = 15ml, reaction duration = 10 days.	EuFe2Se2	Eu1Fe2Se2	Eu	1	Fe	2	Se	2																			2012																										AB2C2																				K			40				40										8																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155666	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: Yb = 0.1365g, FeAs = 0.2658g, Liq. ammonia = 10ml, reaction duration = 10 days.	Yb0.8Fe2Se2	Yb0.8Fe2Se2	Yb	0.8	Fe	2	Se	2																			2012																										AB2C2																				K			42				42										5																																																																																						nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155667	SCIR0020426	metal intercalated-FeAs. Synthetic conditions: FeAs = 0.2000g, Liq. ammonia = 10ml, reaction duration = 17 days.	FeSe(soaked in LA)	Fe1Se1	Fe	1	Se	1																					2012																																														K			8.5				8.5																																																																																																nominal(metal/beta-FeAs = 0.5 - 1.0) - loaded in autoclave - placed in Liq.N2 ( a few min.) - Liq. ammonia filled upto a half volume of autoclave - react(2-17 days at RT)					Observation of superconductivity at 30, 46K in AxFe2Se2 (A = Li, Na, Ba, Sr, Ca, Yb, and Eu)			Research & Development Center for Functional Crystals, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Scientific Reports, 2(2012)426	T. P. Ying,X. L. Chen,G. Wang,S. F. Jin,T. T. Zhou,X. F. Lai,H. Zhang,W. Y. Wang		
155668	SSC1850062	P-induced SC. T<STR>=T<SDW> = 139 K.	Ba(Fe1-xRux)2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2014																										AB2C2		ThCr2Si2																		K					4			MTC155668																																																																																													Ba,FeAs,RuAs		mixture - (melt) - slow cooling without using any flux					Unification of the pressure and composition dependence of superconductivity in Ru substituted BaFe2As2			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 185(2014)62	T.R.Devidas,AwadheshMani,ShilpamSharma,K.Vinod,A.Bharathi,C.S.Sundar		
155669	SSC1850062	P-induced SC. T<STR>=T<SDW> = 103 K.	Ba(Fe1-xRux)2As2	Ba1Fe1.76Ru0.24As2	Ba	1	Fe	1.76	Ru	0.24	As	2																3	2014																										AB2C2		ThCr2Si2																		K					4			MTC155669																																																																																													Ba,FeAs,RuAs		mixture - (melt) - slow cooling without using any flux					Unification of the pressure and composition dependence of superconductivity in Ru substituted BaFe2As2			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 185(2014)62	T.R.Devidas,AwadheshMani,ShilpamSharma,K.Vinod,A.Bharathi,C.S.Sundar		
155670	SSC1850062		Ba(Fe1-xRux)2As2	Ba1Fe1.48Ru0.52As2	Ba	1	Fe	1.48	Ru	0.52	As	2																3	2014																										AB2C2		ThCr2Si2																		K		21.2					21.2	MTC155670																																																																																													Ba,FeAs,RuAs		mixture - (melt) - slow cooling without using any flux					Unification of the pressure and composition dependence of superconductivity in Ru substituted BaFe2As2			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 185(2014)62	T.R.Devidas,AwadheshMani,ShilpamSharma,K.Vinod,A.Bharathi,C.S.Sundar		
155671	SSC1850062		Ba(Fe1-xRux)2As2	Ba1Fe1.3Ru0.7As2	Ba	1	Fe	1.3	Ru	0.7	As	2																3	2014																										AB2C2		ThCr2Si2																		K		20					20	MTC155671		K/GPa	-10																																																																																										Ba,FeAs,RuAs		mixture - (melt) - slow cooling without using any flux					Unification of the pressure and composition dependence of superconductivity in Ru substituted BaFe2As2			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 185(2014)62	T.R.Devidas,AwadheshMani,ShilpamSharma,K.Vinod,A.Bharathi,C.S.Sundar		
155672	SSC1850062		Ba(Fe1-xRux)2As2	Ba1Fe1.58Ru0.42As2	Ba	1	Fe	1.58	Ru	0.42	As	2																3	2014																										AB2C2		ThCr2Si2																		K		19.2					19.2	MTC155672																																																																																													Ba,FeAs,RuAs		mixture - (melt) - slow cooling without using any flux					Unification of the pressure and composition dependence of superconductivity in Ru substituted BaFe2As2			Materials Science Group, Indira Gandhi Centre for Atomic Research, Kalpakkam 603102, Tamil Nadu, India	Solid State Commun., 185(2014)62	T.R.Devidas,AwadheshMani,ShilpamSharma,K.Vinod,A.Bharathi,C.S.Sundar		
155673	PRB079094426	not SC. impurity phase Eu2O3, Fe0.985Ni0.015As	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		1	2009																										AB2C2	2	ThCr2Si2																		K					2																																																																				uV/K			-2.71	MTP155673																								EuAs,Fe2As,Ni2As		mixture - pellet - sealed in quartz tube - ANN(1173K, 24h) - FC to RT					Suppression of spin-density-wave transition and emergence of ferromagnetic ordering of Eu2+ moments in EuFe2-xNixAs2			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 79(2009)094426	Zhi Ren,Xiao Lin,Qian Tao,Shuai Jiang,Zengwei Zhu,Cao Wang,Guanghan Cao,Zhu'an Xu		
155674	PRB079094426	not SC. impurity phase Eu2O3, Fe0.985Ni0.015As	Eu(Fe,Ni)2As2	Eu1Fe1.91Ni0.09As2	Eu	1	Fe	1.91	Ni	0.09	As	2																1	2009																										AB2C2	2	ThCr2Si2																		K					2			MPH155674																																																																	uV/K			-18.4	MTP155674																								EuAs,Fe2As,Ni2As		mixture - pellet - sealed in quartz tube - ANN(1173K, 24h) - FC to RT					Suppression of spin-density-wave transition and emergence of ferromagnetic ordering of Eu2+ moments in EuFe2-xNixAs2			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 79(2009)094426	Zhi Ren,Xiao Lin,Qian Tao,Shuai Jiang,Zengwei Zhu,Cao Wang,Guanghan Cao,Zhu'an Xu		
155675	PRB079094426	not SC. impurity phase Eu2O3, Fe0.985Ni0.015As	Eu(Fe,Ni)2As2	Eu1Fe1.8Ni0.2As2	Eu	1	Fe	1.8	Ni	0.2	As	2																1	2009																										AB2C2	2	ThCr2Si2																		K					2																																																																				uV/K			-31.1	MTP155675																								EuAs,Fe2As,Ni2As		mixture - pellet - sealed in quartz tube - ANN(1173K, 24h) - FC to RT					Suppression of spin-density-wave transition and emergence of ferromagnetic ordering of Eu2+ moments in EuFe2-xNixAs2			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 79(2009)094426	Zhi Ren,Xiao Lin,Qian Tao,Shuai Jiang,Zengwei Zhu,Cao Wang,Guanghan Cao,Zhu'an Xu		
155676	PRB091014508	Tm = 7.5 K, Curie=Weis law for T>100K.	Sr0.5Ce0.5FBiS2	Sr0.5Ce0.5F1Bi1S2	Sr	0.5	Ce	0.5	F	1	Bi	1	S	2														1	2015			emu.K/mol	0.8	myu-B/Ce	2.53	-19.2																						P4/nmm		A	4.069		13.349											BiS2-layer SC	K		2.81					2.81																				T	RES(0.9Rn), GL eq.	1.16												MHC155676																						mJ/mol.K2	58.6	SP	220	SP																																		Ce2S3,SrF2,CeF2,CeF3,Bi2S3,S		mixture - pellet - sealed in quartz tube - heat(1073K,24h) - Q to RT - ANN(973K,10h)					Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2			Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 91(2015)014508	Lin Li,Yuke Li,Yuefeng Jin,Haoran Huang,Bin Chen,Xiaofeng Xu,Jianhui Dai,Li Zhang,Xiaojun Yang,Huifei Zhai,Guanghan Cao,Zhuan Xu		
155677	PRB091020506	air-snsitive. (dC/gamma*Tc) = 1.8. (residual gamma) = 5.3 mJ/mol.K2. Lattice term in SP beta = 2.9 mJ/mol.K4	Rb2Cr3As3	Rb2Cr3As3	Rb	2	Cr	3	As	3																			2015																										A2B3C3	2	K2Cr3As3	P6[-]m2		A	10.281		4.2421												K			4.8			0.44	4.8										91										T	RES(0.9Rn), GL-eq.	20							T/K	RES(0.9Rn)	5.08			MHC155677																			MSP155677			mJ/mol.K2	55	SP	175	SP																																				(mixture+3% excess Rb) - preheat(523K, in quartz ampoule) - grind - pellet - alumina tube - Ta tube -quartz tube - heat(973K, 24h)					Unconventional superconductivity in quasi-one-dimensional Rb2Cr3As3			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 91(2015)020506	Zhang-Tu Tang,Jin-Ke Bao,Yi Liu,Yun-Lei Sun,Abduweli Ablimit,Hui-Fei Zhai,Hao Jiang,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
155678	CEM1821991		alpha-LaSi5	La1Si5	La	1	Si	5																					2009																										AB5			C2/m		A	15.19	4.01	8.2											beta = 109.44	K	10.7		11.7	11.4			11.4										100																																																																																				LaSi2,Si(powder)		mixture -(High-P-high-T synthesis using Kawai-type anvils P=13 GPa). (LaSi2 + 3Si) - heat(700C,1h) - rapid cool to 600C					Phase diagram of the La-Si binary system under high pressure and the structures of superconducting LaSi5 and LaSi10			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 182(2009)1991	Shoji Yamanaka,Satoshi Izumi,Shoichi Maekawa,Keita Umemoto		
155679	CEM1821991	not SC down to 2K	beta-LaSi5	La1Si5	La	1	Si	5																					2009																										AB5			C2/m		A	14.922	3.906	8.807											beta=107.19	K					2																																																																																																LaSi2,Si(powder)		mixture -(High-P-high-T synthesis using Kawai-type anvils P=13 GPa). (LaSi2 + 3Si) - heat(700C,1h) - slow cool to 600C					Phase diagram of the La-Si binary system under high pressure and the structures of superconducting LaSi5 and LaSi10			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 182(2009)1991	Shoji Yamanaka,Satoshi Izumi,Shoichi Maekawa,Keita Umemoto		
155680	CEM1821991		LaSi10	La1Si10	La	1	Si	10																					2009																										AB10			P6<3>/mmc		A	9.623		4.723												K				6.7			6.7																																																																																																mixture -(High-P-high-T synthesis using Kawai-type anvils P=13 GPa).					Phase diagram of the La-Si binary system under high pressure and the structures of superconducting LaSi5 and LaSi10			Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	J.Solid State Chem., 182(2009)1991	Shoji Yamanaka,Satoshi Izumi,Shoichi Maekawa,Keita Umemoto		
155681	CEM2290124		Sn0.8In0.2Te	Sn0.8In0.2Te1	Sn	0.8	In	0.2	Te	1																		1	2015																													Fm3[-]m		A	6.2832														K			3.1				3.1											Oe	M-H curve				10			1.8	T	RES(0.9Rn), WHH	1.33							T/K	RES(0.9Rn)	0.62			MHC155681		A	from Hc2	111																																																								Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155682	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.95Se0.05	Sn	0.8	In	0.2	Te	0.95	Se	0.05																1	2015																													Fm3[-]m		A	6.273														K			3.3				3.3																																																																																														Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155683	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.9Se0.1	Sn	0.8	In	0.2	Te	0.9	Se	0.1																1	2015																													Fm3[-]m		A	6.2677														K			3.7				3.7																																																																																														Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155684	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.85Se0.15	Sn	0.8	In	0.2	Te	0.85	Se	0.15																1	2015																													Fm3[-]m		A	6.2535														K			3.9				3.9	MTC155684									85.9						30			1.8	T	RES(0.9Rn), WHH	2.81							T/K	RES(0.9Rn)	1.04			MHC155684		A	from Hc2	77																																																								Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155685	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.8Se0.2	Sn	0.8	In	0.2	Te	0.8	Se	0.2																1	2015																													Fm3[-]m		A	6.2398														K			3.8				3.8																																																																																														Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155686	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.75Se0.25	Sn	0.8	In	0.2	Te	0.75	Se	0.25																1	2015																													Fm3[-]m		A	6.2298														K			3.7				3.7																																																																																														Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155687	CEM2290124		Sn0.8In0.2(Te1-xSex)	Sn0.8In0.2Te0.7Se0.3	Sn	0.8	In	0.2	Te	0.7	Se	0.3																1	2015																													Fm3[-]m		A	6.2174														K			3.5				3.5																																																																																														Sn(3N),In(5N),Te(5N),Se(5N)		mixture - sealed in carbon coated quartz tube - heat(1223K,12h) - FC to RT - reground - pellet - sealed - ANN(973K,12h) - FC to RT					Selenium doping in potential topological superconductor Sn0.8In0.2Te			CAS Key Laboratory of Materials for Energy Conversion and State Key Laboratory of High Performance Ceramics and Superfine  Microstructures, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 229(2015)124	HaijieChen,Ganghua Zhang,Hui Zhang,Gang Mu,Fuqiang Huang		
155688	CEM2320050	compositions = Cs0.96Pb0.25Bi3.75Te6.04 by EDS. SP heat: beta = 10.11 mJ/mol.K4, delta = 0.16 mJ/mol.K6. (dCel/Tc) = 11.51 mJ/mol.K2, (dCel/gamma*Tc) =1.32	CsPbxBi4-xTe6	Cs1Pb0.3Bi3.7Te6	Cs	1	Pb	0.3	Bi	3.7	Te	6																1	2015																										AB4C6	3				A	6.327	28.648	4.359											orthorhombic	K	2.3	2.9	3.1	3.1			2.9	MTC155688																			T	RES(0.9Rn), GL theory	1.5																															MSP155688			mJ/mol.K2	8.75	SP	128.4	SP																																		Bi2Te3,Pb,Te,Cs		(mixture with small excess Cs) - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air Q to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
155689	CEM2320050	compositions = Cs0.94Pb0.99Bi3.00Te6.07 by EDS.	CsPbxBi4-xTe6	Cs1Pb1Bi3Te6	Cs	1	Pb	1	Bi	3	Te	6																1	2015																										AB4C6	3				A	6.345	28.68	4.377											orthorhombic	K				2.7			2.7																																																																							mOhm.cm							7																Bi2Te3,Pb,Te,Cs		(mixture with small excess Cs) - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air Q to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
155690	INO0506372	R(T) is metallic. synthesis condition (1200C,10GPa)	BaGe3	Ba1Ge3	Ba	1	Ge	3																					2011																										AB3	7		P6<3>/mmc	194	A	6.814		5.027											hexagonal	K	4			4			4										146																																																																																				Ba(2N),Ge(5N)		BaGe2 by arc-mwlting. mixture(BaGe2:Ge = 1:1) in h-BN cell - placed in MgO octahedral pressure medium - heat(500-1200C, 3-13GPa)					High-Pressure Synthesis and Superconductivity of a New Binary Barium Germanide BaGe3			Department of Applied Chemistry, Faculty of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan	Inorganic Chem., 50(2011)6372	Hiroshi Fukuoka,Yusuke Tomomitsu,Kei Inumaru		
155691	INO0515509	SP fitting: C/T = gamma + beta*T^2 + delta*T^4 for 4.0 =<T=<8.0.  (d/kTc) = 1.94 using alpha-model in SP. e-ph = 0.72 from McMillan's eq.	CaGe3	Ca1Ge3	Ca	1	Ge	3																					2012																										AB3	2		I4/mmm	139	A	7.692		11.3314												K	6.2			6.8			6.8																				T	SP, WHH	0.29																										3.88	14				MSP155691			mJ/mol.K2	6.31	SP	330	SP											uOhm.cm							86				136														High-T-High-T synthesis. Mixture(aGe2 + Ge) - ANN(1200C,1h, 10 GPa) - Quench					Dumbbells of Five-Connected Ge Atoms and Superconductivity in CaGe3			Max-Planck-Institut fuur Chemische Physik fester Stoffe, Dresden, Germany	Inorganic Chem., 51(2012)5509	Walter Schnelle,Alim Ormeci,Aron Wosylus,Katrin Meier,Yuri Grin,Ulrich Schwarz		
155692	JAC6460517	Kink feature observed around 195K in R(T). Multi phases(tetra & ortho).	(Nb0.9-xTi0.1Cux)Sr2EuCu2Oz	Nb0.9Ti0.1Sr2Eu1Cu2Oz	Nb	0.9	Ti	0.1	Sr	2	Eu	1	Cu	2											O	z		1	2015																												M1212			A	3.8718		11.6303												K					10																																																																				uV/K	146																											Nb2O5,TiO2,SrCO3,Eu2O3,CuO		mixture - heat(1010C,7-10h, in air) - redround - pellet - ANN(1050C,12h, in O2) - SIN(1060C,15h, i O2 flow) - slow cool to 200C and RT					Structure and superconductivity in new Nb-based cuprates (Nb,Ti,Cu) Sr2EuCu2Oz			Department of Physics, Kangwon National University, Chuncheon 200-701, Republic of Korea	J.Alloys compds, 646(2015)517	H.K. Lee,Y.I. Kim		
155693	JAC6460517	Kink feature observed around 195K in R(T). Multi phases(tetra & ortho). Ortho-phase: 7.7 wt %	(Nb0.9-xTi0.1Cux)Sr2EuCu2Oz	Nb0.8Ti0.1Sr2Eu1Cu2.1Oz	Nb	0.8	Ti	0.1	Sr	2	Eu	1	Cu	2.1											O	z		1	2015																												M1212			A	3.8663		11.617												K				28			28										0.04																																																								uV/K	120				mOhm.cm											86.7												Nb2O5,TiO2,SrCO3,Eu2O3,CuO		mixture - heat(1010C,7-10h, in air) - redround - pellet - ANN(1050C,12h, in O2) - SIN(1060C,15h, i O2 flow) - slow cool to 200C and RT					Structure and superconductivity in new Nb-based cuprates (Nb,Ti,Cu) Sr2EuCu2Oz			Department of Physics, Kangwon National University, Chuncheon 200-701, Republic of Korea	J.Alloys compds, 646(2015)517	H.K. Lee,Y.I. Kim		
155694	JAC6460517	Kink feature observed around 195K in R(T). Multi phases(tetra & ortho).	(Nb0.9-xTi0.1Cux)Sr2EuCu2Oz	Nb0.7Ti0.1Sr2Eu1Cu2.2Oz	Nb	0.7	Ti	0.1	Sr	2	Eu	1	Cu	2.2											O	z		1	2015																												M1212			A	3.866		11.6193												K				30			30										0.68																																																								uV/K	95				mOhm.cm											45.5												Nb2O5,TiO2,SrCO3,Eu2O3,CuO		mixture - heat(1010C,7-10h, in air) - redround - pellet - ANN(1050C,12h, in O2) - SIN(1060C,15h, i O2 flow) - slow cool to 200C and RT					Structure and superconductivity in new Nb-based cuprates (Nb,Ti,Cu) Sr2EuCu2Oz			Department of Physics, Kangwon National University, Chuncheon 200-701, Republic of Korea	J.Alloys compds, 646(2015)517	H.K. Lee,Y.I. Kim		
155695	JAC6460517	Kink feature observed around 195K in R(T). Multi phases(tetra & ortho). Ortho-phase: 59 %.	(Nb0.9-xTi0.1Cux)Sr2EuCu2Oz	Nb0.5Ti0.1Sr2Eu1Cu2.4Oz	Nb	0.5	Ti	0.1	Sr	2	Eu	1	Cu	2.4											O	z		1	2015																												M1212			A	3.8672		11.6192												K	24			30			30										1.97																																																								uV/K	56				mOhm.cm											39.4												Nb2O5,TiO2,SrCO3,Eu2O3,CuO		mixture - heat(1010C,7-10h, in air) - redround - pellet - ANN(1050C,12h, in O2) - SIN(1060C,15h, i O2 flow) - slow cool to 200C and RT					Structure and superconductivity in new Nb-based cuprates (Nb,Ti,Cu) Sr2EuCu2Oz			Department of Physics, Kangwon National University, Chuncheon 200-701, Republic of Korea	J.Alloys compds, 646(2015)517	H.K. Lee,Y.I. Kim		
155696	JAC6460866	single phase.	La3(Co,Ru)4Sn13	La3Co1Ru3Sn13	La	3	Co	1	Ru	3	Sn	13																1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		5	5.58				5	MTC155696		K/GPa	-0.32																T	RES(0.5Rn), GL	5.28							T/K	RES(0.5Rn)	1.3			MHC155696		A	from Hc2	80																																																										arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155697	JAC6460866	single phase. (dC/gamma*Tc) = 1.7 from SP heat measurements.	La3(Co,Ru)4Sn13	La3Co3.5Ru0.5Sn13	La	3	Co	3.5	Ru	0.5	Sn	13																1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		2.41					2.41	MTC155697		K/GPa	-0.12																T	RES(0.5Rn), GL	2.24							T/K	RES(0.5Rn)	1.34			MHC155697		A	from Hc2	110																																																										arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155698	JAC6460866	Two phases different Tc (Tc(R) and Tc(SP))	La3(Co,Ru)4Sn13	La3Co2Ru2Sn13	La	3	Co	2	Ru	2	Sn	13																1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		4					4	MTC155698																																																																																															arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155699	JAC6460866		La3Rh4Sn13	La3Rh2Sn13	La	3	Rh	2	Sn	13																		1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		3					3																																		MHC155699																																																														arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155700	JAC6460866		La3(Co,Ru)4Sn13	La3Co2Sn13	La	3	Co	2	Sn	13																		1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		1.95					1.95	MTC155700		K/GPa	0.05																T	RES(0.5Rn), GL	1.38							T/K	RES(0.5Rn)	0.904			MHC155700		A	from Hc2	160																																																										arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155701	JAC6460866		La3Ru4Sn13	La3Ru2Sn13	La	3	Ru	2	Sn	13																		1	2015																										A3B4C13		Yb3Rh4Sn13	Pm3n																	K		1.58	3.76				1.58	MTC155701		K/GPa	-0.03																T	RES(0.5Rn), GL	1.34							T/K	RES(0.5Rn)	1.33			MHC155701		A	from Hc2	189																																																										arc-melting.  ANN(870C,2w)					Superconductivity in the presence of disorder in skutterudite-related La3Co4Sn13 and La3Ru4Sn13 compounds: Electrical transport and magnetic studies			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys compds, 646(2015)866	A. Slebarski,M.M. Maska,M. Fijaikowski,C.A. McElroy,M.B. Maple		
155702	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe1.15Te0.72S0.28  by EDX.  Filamentary SC.  R=R0*exp[(T0/T)^n], T0 = 2294 K.	FeTe1-x-ySexSy	Fe1Te0.88S0.12	Fe	1	Te	0.88	S	0.12																		1	2015																										AB		PbO	P4/nmm		A	3.8		6.1												K	6.8						6.8																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155703	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe0.88Te0.82Se0.09S0.09  by EDX.   R = R0*exp[(T0/T)^n], T0 = 403 K.	FeTe1-x-ySexSy	Fe1Te0.8Se0.1S0.1	Fe	1	Te	0.8	Se	0.1	S	0.1																1	2015																										AB		PbO	P4/nmm		A	3.802		6.16												K	9.9			6.6			6.6																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155704	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe1.25Te0.67Se0.27S0.06  by EDX.  R = R0*exp[(T0/T)^n], T0 = 853 K.	FeTe1-x-ySexSy	Fe1Te0.69Se0.25S0.06	Fe	1	Te	0.69	Se	0.25	S	0.06																1	2015																										AB		PbO	P4/nmm		A	3.807		6.23												K	12.3			11.3			11.3																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155705	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe1.18Te0.66Se0.28S0.06  by EDX.  R = R0*exp[(T0/T)^n], T0 = 435 K	FeTe1-x-ySexSy	Fe1Te0.65Se0.3S0.05	Fe	1	Te	0.65	Se	0.3	S	0.05																1	2015																										AB		PbO	P4/nmm		A	3.802		6.08												K	13			12.2			12.2																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155706	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe0.92Te0.50Se0.46S0.04  by EDX.  R = R0*exp[(T0/T)^n], T0 = 337 K.	FeTe1-x-ySexSy	Fe1Te0.58Se0.4S0.02	Fe	1	Te	0.58	Se	0.4	S	0.02																1	2015																										AB		PbO	P4/nmm		A	3.798		6.03												K	13.5			13.1			13.1																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155707	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe1.13Te0.51Se0.47S0.02  by EDX.  R = R0*exp[(T0/T)^n], T0 = 297 K	FeTe1-x-ySexSy	Fe1Te0.54Se0.45S0.01	Fe	1	Te	0.54	Se	0.45	S	0.01																1	2015																										AB		PbO	P4/nmm		A	3.798		6.01												K	13.5			13.3			13.3																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155708	JAC6491031	Impurity phase: Fe7Se8(less than 8%). Compositions = Fe0.99Te0.42Se0.58  by EDX.  R=R0*exp[(T0/T)^n], T0 = 524 K.	FeTe1-x-ySexSy	Fe1Te0.5Se0.5	Fe	1	Te	0.5	Se	0.5																		1	2015																										AB		PbO	P4/nmm		A	3.801		6												K	14			14.3			14.3																																																																																																solid state reaction.					Influence of substitutional disorder on the electrical transport and the superconducting properties of Fe1+zTe1-x-ySexSy			Laboratorio de Bajas Temperaturas, Departamento de Fisica, FCEyNUBA and IFIBA-CONICET, Buenos Aires, Argentina	J.Alloys compds, 649(2015)1031	M.G. Rodriguez,G. Polla,C.P. Ramos,C. Acha		
155709	JJP049020210	M = PC (propylene carbonate). PC-content not given. co-intercalation of Mg and PC.	Mgx(PC)yZrNCl	Mg0.3M1Zr1N1Cl1	Mg	0.3	M	1	Zr	1	N	1	Cl	1															2010																															A			66.7												K				15			15																																																																																																using 1M Mg(ClO4)2 dissolved in propylene carbonate.					A New Intercalation Superconductor Mgx(PC)yZrNCl			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	Jpn.J.Appl.Phys.,49(2010)020210	Hiroto Tezuka,Masatsune Kato,Takashi Noji,Shoji Yamanaka,Yoji Koike		
155710	JPS083033706	R(T) shows max at 47 K. effective moment = 2.57 and 2.58 myu-B/Ce, Curie-T = -97 and -31 K for H//a and H//c-axis, respectively. (dC/gamma*Tc) = 4.6	CeCo(In,Zn)5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2014					myu-B/Ce	2.57	-97																			ABC5		HoCoGa5																		K	2.23		2.27	2.29			2.29																				T	SUS, WHH						4.79	0.27																																																																				In-flux method. Ce:Co:In:Zn = 1:1:F*(1-x):F*x, F=20-25. mixture melt in quartz tube (0.02 MPa Ar)					Possible Evolution of Antiferromagnetism in Zn-Doped Heavy-Fermion Superconductor CeCoIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 83(2014)033706	Makoto Yokoyama,Kenji Fujimura,Sara Ishikawa,Masashi Kimura,Takeshi Hasegawa,Ikuto Kawasaki,Kenichi Tenya,Yohei Kono,Toshiro Sakakibara		
155711	JPS083033706	(dC/gamma*Tc) = 3.8	CeCo(In,Zn)5	Ce1Co1In4.875Zn0.125	Ce	1	Co	1	In	4.875	Zn	0.125																3	2014																										ABC5		HoCoGa5																		K	2.07		2.1	2.14			2.14																				T	SUS, WHH						5.05	0.27																									MSP155711																																											In-flux method. Ce:Co:In:Zn = 1:1:F*(1-x):F*x, F=20-25. mixture melt in quartz tube (0.02 MPa Ar)					Possible Evolution of Antiferromagnetism in Zn-Doped Heavy-Fermion Superconductor CeCoIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 83(2014)033706	Makoto Yokoyama,Kenji Fujimura,Sara Ishikawa,Masashi Kimura,Takeshi Hasegawa,Ikuto Kawasaki,Kenichi Tenya,Yohei Kono,Toshiro Sakakibara		
155712	JPS083033706	(dC/gamma*Tc) = 1.7	CeCo(In,Zn)5	Ce1Co1In4.75Zn0.25	Ce	1	Co	1	In	4.75	Zn	0.25																3	2014																										ABC5		HoCoGa5																		K	1.8	1.82	1.92	1.91			1.82																				T	SUS, WHH			15.6			4.8	0.27	T/K	SUS			12.8	MHC155712																			MSP155712																																											In-flux method. Ce:Co:In:Zn = 1:1:F*(1-x):F*x, F=20-25. mixture melt in quartz tube (0.02 MPa Ar)					Possible Evolution of Antiferromagnetism in Zn-Doped Heavy-Fermion Superconductor CeCoIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 83(2014)033706	Makoto Yokoyama,Kenji Fujimura,Sara Ishikawa,Masashi Kimura,Takeshi Hasegawa,Ikuto Kawasaki,Kenichi Tenya,Yohei Kono,Toshiro Sakakibara		
155713	JPS083033706	R(T) shows max at 37 K.	CeCo(In,Zn)5	Ce1Co1In7.65Zn0.35	Ce	1	Co	1	In	7.65	Zn	0.35																3	2014																										ABC5		HoCoGa5																		K	1.76		1.78	1.78			1.78																				T	SUS, WHH						4.2	0.27																																																																				In-flux method. Ce:Co:In:Zn = 1:1:F*(1-x):F*x, F=20-25. mixture melt in quartz tube (0.02 MPa Ar)					Possible Evolution of Antiferromagnetism in Zn-Doped Heavy-Fermion Superconductor CeCoIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 83(2014)033706	Makoto Yokoyama,Kenji Fujimura,Sara Ishikawa,Masashi Kimura,Takeshi Hasegawa,Ikuto Kawasaki,Kenichi Tenya,Yohei Kono,Toshiro Sakakibara		
155714	JPS083023707	Tn measured from T-dependence of <31>P-NMR. Curie-T obtained from (1/T1*T).	LsFe(As1-xPx)O	La1Fe1As0.9P0.1O1	La	1	Fe	1	As	0.9	P	0.1													O	1		1	2014							65.2	65.7																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K	0				0		0																																																																																																solid state reaction. Powdered samples used for NMR					Relationship between Superconductivity and Antiferromagnetism in LaFe(As1-xPx)O Revealed by <31>P-NMR			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 83(2014)023707	Shunsaku Kitagawa,Tetsuya Iye,Yusuke Nakai,Kenji Ishida,Cao Wang,Guang-Han Cao,Zhu-An Xu		
155715	JPS083023707	Tn measured from T-dependence of <31>P-NMR. Curie-T obtained from (1/T1*T).	LsFe(As1-xPx)O	La1Fe1As0.8P0.2O1	La	1	Fe	1	As	0.8	P	0.2													O	1		1	2014							38.9	37.3																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K	0				0		0																																																																																																solid state reaction. Powdered samples used for NMR					Relationship between Superconductivity and Antiferromagnetism in LaFe(As1-xPx)O Revealed by <31>P-NMR			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 83(2014)023707	Shunsaku Kitagawa,Tetsuya Iye,Yusuke Nakai,Kenji Ishida,Cao Wang,Guang-Han Cao,Zhu-An Xu		
155716	JPS083023707	Tn measured from T-dependence of <31>P-NMR. Curie-T obtained from (1/T1*T).	LsFe(As1-xPx)O	La1Fe1As0.7P0.3O1	La	1	Fe	1	As	0.7	P	0.3													O	1		1	2014							10.6																			ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K				10.6			10.6	MPH155716																																																																																															solid state reaction. Powdered samples used for NMR					Relationship between Superconductivity and Antiferromagnetism in LaFe(As1-xPx)O Revealed by <31>P-NMR			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 83(2014)023707	Shunsaku Kitagawa,Tetsuya Iye,Yusuke Nakai,Kenji Ishida,Cao Wang,Guang-Han Cao,Zhu-An Xu		
155717	JPS083023707	Tn measured from T-dependence of <31>P-NMR. Curie-T obtained from (1/T1*T).	LsFe(As1-xPx)O	La1Fe1As0.6P0.4O1	La	1	Fe	1	As	0.6	P	0.4													O	1		1	2014							20.7	17.6																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K				7.73			7.73																																																																																																solid state reaction. Powdered samples used for NMR					Relationship between Superconductivity and Antiferromagnetism in LaFe(As1-xPx)O Revealed by <31>P-NMR			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 83(2014)023707	Shunsaku Kitagawa,Tetsuya Iye,Yusuke Nakai,Kenji Ishida,Cao Wang,Guang-Han Cao,Zhu-An Xu		
155718	JPS083023707	Tn measured from T-dependence of <31>P-NMR. Curie-T obtained from (1/T1*T).	LsFe(As1-xPx)O	La1Fe1As0.5P0.5O1	La	1	Fe	1	As	0.5	P	0.5													O	1		1	2014							14.7	16.5																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K	0				0		0																																																																																																solid state reaction. Powdered samples used for NMR					Relationship between Superconductivity and Antiferromagnetism in LaFe(As1-xPx)O Revealed by <31>P-NMR			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 83(2014)023707	Shunsaku Kitagawa,Tetsuya Iye,Yusuke Nakai,Kenji Ishida,Cao Wang,Guang-Han Cao,Zhu-An Xu		
155719	JPS083083702	Tn by <31>P-NMR.	LsFe(As1-xPx)O	La1Fe1As0.6P0.4O1	La	1	Fe	1	As	0.6	P	0.4													O	1		1	2014								16																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K				4.8			4.8																																																																																																solid state reaction					Emergence of Novel Antiferromagnetic Order Intervening between Two Superconducting Phases in LaFe(As1-xPx)O: <31>P-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 83(2014)083702	Hidekazu Mukuda,Fuko Engetsu,Takayoshi Shiota,Kwing To Lai,Mitsuharu Yashima,Yoshio Kitaoka,Shigeki Miyasaka,Setsuko Tajima		
155720	JPS083083702	Tn by <31>P-NMR. Figure shows 2nd AFM phase in LaFe(As1-xPx)O along with the results of PRB090064504(2014) and EPL08647002(2009)	LsFe(As1-xPx)O	La1Fe1As0.5P0.5O1	La	1	Fe	1	As	0.5	P	0.5													O	1		1	2014								13.7																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K					0			MPH155720																																																																																															solid state reaction					Emergence of Novel Antiferromagnetic Order Intervening between Two Superconducting Phases in LaFe(As1-xPx)O: <31>P-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 83(2014)083702	Hidekazu Mukuda,Fuko Engetsu,Takayoshi Shiota,Kwing To Lai,Mitsuharu Yashima,Yoshio Kitaoka,Shigeki Miyasaka,Setsuko Tajima		
155721	JPS083083702	Tn by <31>P-NMR.	LsFe(As1-xPx)O	La1Fe1As0.4P0.6O1	La	1	Fe	1	As	0.4	P	0.6													O	1		1	2014								35																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K					0			MPH155720																																																																																															solid state reaction					Emergence of Novel Antiferromagnetic Order Intervening between Two Superconducting Phases in LaFe(As1-xPx)O: <31>P-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 83(2014)083702	Hidekazu Mukuda,Fuko Engetsu,Takayoshi Shiota,Kwing To Lai,Mitsuharu Yashima,Yoshio Kitaoka,Shigeki Miyasaka,Setsuko Tajima		
155722	JPS083083702	Tn by <31>P-NMR.	LsFe(As1-xPx)O	La1Fe1As0.3P0.7O1	La	1	Fe	1	As	0.3	P	0.7													O	1		1	2014								15.5																		ABCD		oxypnictide																	Fe-1111, ZrCuSiAs-type	K					0																																																																																																		solid state reaction					Emergence of Novel Antiferromagnetic Order Intervening between Two Superconducting Phases in LaFe(As1-xPx)O: <31>P-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 83(2014)083702	Hidekazu Mukuda,Fuko Engetsu,Takayoshi Shiota,Kwing To Lai,Mitsuharu Yashima,Yoshio Kitaoka,Shigeki Miyasaka,Setsuko Tajima		
155723	JPS083094721	Energy gap obtained by SP using two gap model. Large and small gaps are 4.11 and 2.60 meV.	FeSe1-xTex	Fe1Se0.4Te0.6	Fe	1	Se	0.4	Te	0.6																		3	2014																										AB																			Fe-11	K		13.8					13.8																																														meV	4.11		14				MSP155723																																											Single crystals grown by Bridgman method. As-grown sample - ANN(400C, 200h in vac)					Superconducting Gap and Symmetry in FeSe1-xTex Studied by Specific Heat in Magnetic Fields			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)094721	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
155724	JPS083094721	Energy gap obtained by SP using two gap model. Large and small gaps are 4.60 and 3.10 meV.	FeSe1-xTex	Fe1Se0.3Te0.7	Fe	1	Se	0.3	Te	0.7																		3	2014																										AB																			Fe-11	K		13.7					13.7																																														meV	4.6		14				MSP155724																																											Single crystals grown by Bridgman method. As-grown sample - ANN(400C, 200h in vac)					Superconducting Gap and Symmetry in FeSe1-xTex Studied by Specific Heat in Magnetic Fields			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)094721	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
155725	JPS083094721	Energy gap obtained by SP using two gap model. Large and small gaps are 5.01 and 3.00 meV.	FeSe1-xTex	Fe1Se0.2Te0.8	Fe	1	Se	0.2	Te	0.8																		3	2014																										AB																			Fe-11	K		13					13																																														meV	5.01		14				MSP155725																																											Single crystals grown by Bridgman method. As-grown sample - ANN(400C, 200h in vac)					Superconducting Gap and Symmetry in FeSe1-xTex Studied by Specific Heat in Magnetic Fields			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)094721	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
155726	JPS083094721	Energy gap obtained by SP using two gap model. Large and small gaps are 2.51 and 1.81 meV.	FeSe1-xTex	Fe1Se0.1Te0.9	Fe	1	Se	0.1	Te	0.9																		3	2014																										AB																			Fe-11	K		11					11																																														meV	2.51		14				MSP155726																																											Single crystals grown by Bridgman method. As-grown sample - ANN(400C, 200h in vac)					Superconducting Gap and Symmetry in FeSe1-xTex Studied by Specific Heat in Magnetic Fields			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)094721	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
155727	JPS083094721	not SC. gamma from SP-heat.	FeSe1-xTex	Fe1Te1	Fe	1	Te	1																				3	2014																										AB																			Fe-11	K		0			0		0																																																								mJ/mol.K2	29.43																																							Single crystals grown by Bridgman method. As-grown sample - ANN(400C, 200h in vac)					Superconducting Gap and Symmetry in FeSe1-xTex Studied by Specific Heat in Magnetic Fields			Department of Applied Physics, Graduate School of Engineering, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)094721	Takuya Konno,Tadashi Adachi,Masato Imaizumi,Takashi Noji,Takayuki Kawamata,Yoji Koike		
155728	JPS083113704	co-intercalated (Li,M)-sample. M is HMDA (C6H16N2). compositions: Li1.25M0.64Fe2.05Se2 by IPS-OES. R(T) not to zero down to 5K. FeSe layer distance d=16.225 A	LixMyFe2-zSe2	Li1.25M0.64Fe2.05Se2	Li	1.25	M	0.64	Fe	2.05	Se	2																1	2014																															A	3.453		32.45												K				38			38	MTC155728																																																																																															FeSe made by solid state reaction. mixture(Fe:Se=1.02:1) - pellet - sealed in quartz - heat(800C,40h). FeSe powder - placed in beaker(0.2-0.8 M solution of Li desolved HMDA reaction(45C,5d)					New Intercalation Superconductor Lix(C6H16N2)yFe2-zSe2 with a Very Large Interlayer-Spacing and Tc = 38K			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 83(2014)113704	Shohei Hosono,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
155729	JPS083114709	R(T) anomaly at 50 K.. Anisotropy = (Hc2//ab)/(Hc2//c) = 49.	La(,O,F)BiSe2	La1Bi1Se2F0.5O0.5	La	1	Bi	1	Se	2	F	0.5													O	0.5		1	2014																												CeOBiS2																	BiS2-layer SC	K	3.05		3.75				3.4																				T	RES(on), Linear approx.		28	0.57										MHC155729																																																												La,Bi,Se,Bi2Se3,BiF3		High-T flux method. (mixture 0.8g) - mixed with CsCl flux(5g) - sealed in quartz tube - heat(900C,10h) - cool to 650C (1 C/h) - FC to RT					Superconducting Anisotropies of F-Substituted LaOBiSe2 Single Crystals			University of Yamanashi, Kofu 400-8511, Japan	J.Phys.Soc.Jpn, 83(2014)114709	Masanori Nagao,Masashi Tanaka,Satoshi Watauchi,Isao Tanaka,Yoshihiko Takano		
155730	JPS084063703	RRR = 54. AF-quadrupole order Temp = 0.11K	Pr1-xLaxIr2Zn20	Pr1Ir2Zn20	Pr	1	Ir	2	Zn	20																		1	2015					Myu-B/Pr	3.5																				AB2C20		CeCr2Al20			A	14.2729														K		0.07					0.07																				mT	RES, WHH	0.8							mT/K	RES	16			MHC155730		A	from Hc2	6600																																	uOhm.cm							1.93																Pr(4N),La(4N),Ir(3N),Zn(6N)		melt-grown method					Effect of La Substitution in PrIr2Zn20 on the Superconductivity and Antiferro-Quadrupole Order			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 84(2015)063703	Keisuke T. Matsumoto,Takahiro Onimaru,Kazuhei Wakiya,Kazunori Umeo,Toshiro Takabatake		
155731	JPS084063703		Pr1-xLaxIr2Zn20	Pr0.73La0.27Ir2Zn20	Pr	0.73	La	0.27	Ir	2	Zn	20																1	2015					Myu-B/Pr	3.4																				AB2C20		CeCr2Al20																		K		0.093					0.093																																																																							uOhm.cm							8.55																Pr(4N),La(4N),Ir(3N),Zn(6N)		melt-grown method					Effect of La Substitution in PrIr2Zn20 on the Superconductivity and Antiferro-Quadrupole Order			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 84(2015)063703	Keisuke T. Matsumoto,Takahiro Onimaru,Kazuhei Wakiya,Kazunori Umeo,Toshiro Takabatake		
155732	JPS084063703		Pr1-xLaxIr2Zn20	Pr0.25La0.75Ir2Zn20	Pr	0.25	La	0.75	Ir	2	Zn	20																1	2015					Myu-B/Pr	3.2																				AB2C20		CeCr2Al20																		K		0.28					0.28	MTC155732																																																																						uOhm.cm							22.9																Pr(4N),La(4N),Ir(3N),Zn(6N)		melt-grown method					Effect of La Substitution in PrIr2Zn20 on the Superconductivity and Antiferro-Quadrupole Order			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 84(2015)063703	Keisuke T. Matsumoto,Takahiro Onimaru,Kazuhei Wakiya,Kazunori Umeo,Toshiro Takabatake		
155733	JPS084063703	AF-quadrupole order Temp = 0.067 K	Pr1-xLaxIr2Zn20	Pr0.96La0.04Ir2Zn20	Pr	0.96	La	0.04	Ir	2	Zn	20																1	2015																										AB2C20		CeCr2Al20																		K		0.07					0.07	MTC155733																																																																						uOhm.cm							2.2																Pr(4N),La(4N),Ir(3N),Zn(6N)		melt-grown method					Effect of La Substitution in PrIr2Zn20 on the Superconductivity and Antiferro-Quadrupole Order			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 84(2015)063703	Keisuke T. Matsumoto,Takahiro Onimaru,Kazuhei Wakiya,Kazunori Umeo,Toshiro Takabatake		
155734	JPS084063703	RRR = 12	Pr1-xLaxIr2Zn20	La1Ir2Zn20	La	1	Ir	2	Zn	20																		1	2015																										AB2C20		CeCr2Al20			A	14.3535														K		0.58					0.58																				mT	RES, WHH	11							mT/K	RES	26			MHC155734		A	from Hc2	1800																																	uOhm.cm							7.61																Pr(4N),La(4N),Ir(3N),Zn(6N)		melt-grown method					Effect of La Substitution in PrIr2Zn20 on the Superconductivity and Antiferro-Quadrupole Order			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 84(2015)063703	Keisuke T. Matsumoto,Takahiro Onimaru,Kazuhei Wakiya,Kazunori Umeo,Toshiro Takabatake		
155735	JPS084075001	Nominal  Co-content x = 0.025. Tc defined as coset of M/H.	Ca0.8La0.2Fe1-xCoxAs2	Ca0.8La0.2Fe0.978Co0.022As2	Ca	0.8	La	0.2	Fe	0.978	Co	0.022	As	2														1	2015																										ABC2		Fe-112	P2<1>																Fe-112 phase	K				37.8			37.8																																																																																														CaO,Ca,La,FeAs,CoAs,As		self-flux method					Co-co-doping Effect on Superconducting Properties of 112-Type Ca0.8La0.2FeAs2 Single Crystals			Department of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Phys.Soc.Jpn, 84(2015)075001	Xiangzhuo Xing,Baozhang Xu,Na Li,Yiran Sun,Yufeng Zhang,Zhixiang Shi		
155736	JPS084075001	Nominal  Co-content x = 0.0375. Tc defined as coset of M/H.	Ca0.8La0.2Fe1-xCoxAs2	Ca0.8La0.2Fe0.9671Co0.0329As2	Ca	0.8	La	0.2	Fe	0.9671	Co	0.0329	As	2														1	2015																										ABC2		Fe-112	P2<1>																Fe-112 phase	K				36.5			36.5																																																																																														CaO,Ca,La,FeAs,CoAs,As		self-flux method					Co-co-doping Effect on Superconducting Properties of 112-Type Ca0.8La0.2FeAs2 Single Crystals			Department of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Phys.Soc.Jpn, 84(2015)075001	Xiangzhuo Xing,Baozhang Xu,Na Li,Yiran Sun,Yufeng Zhang,Zhixiang Shi		
155737	JPS084075001	Nominal  Co-content x = 0.05. Tc defined as coset of M/H.	Ca0.8La0.2Fe1-xCoxAs2	Ca0.8La0.2Fe0.9558Co0.0442As2	Ca	0.8	La	0.2	Fe	0.9558	Co	0.0442	As	2														1	2015																										ABC2		Fe-112	P2<1>																Fe-112 phase	K				35.1			35.1																																																																																														CaO,Ca,La,FeAs,CoAs,As		self-flux method					Co-co-doping Effect on Superconducting Properties of 112-Type Ca0.8La0.2FeAs2 Single Crystals			Department of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Phys.Soc.Jpn, 84(2015)075001	Xiangzhuo Xing,Baozhang Xu,Na Li,Yiran Sun,Yufeng Zhang,Zhixiang Shi		
155738	JPS084084703	As-synthesized. SC disappears for P > 2 GPa. R(T) has two anomalies at T1 =  and T2 = for P > 2GPa, due to Bi metal. For P=8 GPa, T1=5.83 K, T2=8.38 K.	Bi(O,F)BiS2	Bi2S2F0.5O0.5	Bi	2	S	2	F	0.5															O	0.5		1	2015																										AB2C2					A	3.97		13.723											BiS2-layer SC	K			5.1	5.1			5.1	MTC155738		K/GPa	-1.2																																																																																												Topotactic reaction (Bi2OS2 + 0.5 XeF2 at 400C, 72H in evacuated quartz ampoule					Pressure Effects on Superconducting Properties of the BiS2-Based Superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 84(2015)084703	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio,Nao Takeshita,Naoki Shirakawa,Akira Iyo,Hiroshi Eisaki		
155739	JPS084084703	HP-annealed (470C,2 GPa,1h) sample	Bi(O,F)BiS2	Bi2S2F0.5O0.5	Bi	2	S	2	F	0.5															O	0.5		1	2015																										AB2C2					A	3.979		13.693											BiS2-layer SC	K				4.9			4.9																																																																																																Topotactic reaction (Bi2OS2 + 0.5 XeF2 at 400C, 72H in evacuated quartz ampoule					Pressure Effects on Superconducting Properties of the BiS2-Based Superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 84(2015)084703	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio,Nao Takeshita,Naoki Shirakawa,Akira Iyo,Hiroshi Eisaki		
155740	JPS084084703		Bi(O,F)BiS2	Bi2S2F0.1O0.9	Bi	2	S	2	F	0.1															O	0.9		1	2015																										AB2C2					A	3.964		13.761											BiS2-layer SC	K				2.92			2.92																																																																																																Topotactic reaction (Bi2OS2 + 0.1 XeF2 at 470C, 72H in evacuated quartz ampoule					Pressure Effects on Superconducting Properties of the BiS2-Based Superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 84(2015)084703	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio,Nao Takeshita,Naoki Shirakawa,Akira Iyo,Hiroshi Eisaki		
155741	JPS084084703		Bi(O,F)BiS2	Bi2S2F0.1O0.9	Bi	2	S	2	F	0.1															O	0.9		3	2015																										AB2C2					A	3.969		13.736											BiS2-layer SC	K				4.43			4.43																																																																																																Topotactic reaction (Bi2OS2 + 0.1 XeF2 at 470C, 72H in evacuated quartz ampoule					Pressure Effects on Superconducting Properties of the BiS2-Based Superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	J.Phys.Soc.Jpn, 84(2015)084703	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio,Nao Takeshita,Naoki Shirakawa,Akira Iyo,Hiroshi Eisaki		
155742	JPS084095001	Tc, Hc2 data for P=0.4 GPa.. Hc2(T) figure by DB staff from Fig.3. Tc(onset) = 5.7 K for P=1.9 GPa.	La(O,F)BiSeS	La1Bi1Se1S1F0.5O0.5	La	1	Bi	1	Se	1	S	1	F	0.5											O	0.5		3	2015																												P4/nmm			A			13.54											BiS2-layer SC	K	2.3		4.9				3.6																				T	RES(0.9Rn)													MHC155742																																																														CsCl flux method					Observation of a Pressure-Induced Phase Transition for Single Crystalline LaO0.5F0.5BiSeS Using a Diamond Anvil Cell			Laboratory of Nano-Structure Physics, Research Institute for Electronic Science, University of Hokkaido, Sapporo 001-0020, Japan	J.Phys.Soc.Jpn, 84(2015)095001	Masaya Fujioka,Ryo Matsumoto,Takuma Yamaki,Saleem J. Denholme,Masashi Tanaka,Hiroyuki Takeya,Takahide Yamaguchi,Hiroki Takahashi,Yoshihiko Takano		
155743	JPS084095001	Tc data for P=5.1 GPa (high-Tc phase). space group = P2<1>/m for P>3 GPa. Tc = 5.0 K (low Tc phase)	La(O,F)BiSeS	La1Bi1Se1S1F0.5	La	1	Bi	1	Se	1	S	1	F	0.5														1	2015																												P2<1>/m																	BiS2-layer SC	K	3.48		7				5.24																																																																																																CsCl flux method					Observation of a Pressure-Induced Phase Transition for Single Crystalline LaO0.5F0.5BiSeS Using a Diamond Anvil Cell			Laboratory of Nano-Structure Physics, Research Institute for Electronic Science, University of Hokkaido, Sapporo 001-0020, Japan	J.Phys.Soc.Jpn, 84(2015)095001	Masaya Fujioka,Ryo Matsumoto,Takuma Yamaki,Saleem J. Denholme,Masashi Tanaka,Hiroyuki Takeya,Takahide Yamaguchi,Hiroki Takahashi,Yoshihiko Takano		
155744	JPS084104706		BNx	N0.7V1	N	0.7	V	1																				1	2015																										AB		NaCl	Fm3m		A	4.08														K				2.03			2.03																																																																																																mixture(V, VN powder) - pressed into pellet - ANN(1100C,24h, under 0.1 Pa-Ar, in quartz tube)					High Pressure Effect on the Superconductivity in VN			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 84(2015)104706	Bosen Wang,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Kenya Ohgushi		
155745	JPS084104706		BNx	N0.8V1	N	0.8	V	1																				1	2015																										AB		NaCl	Fm3m		A	4.1152														K				4.54			4.54																																																																																																mixture(V, VN powder) - pressed into pellet - ANN(1100C,24h, under 0.1 Pa-Ar, in quartz tube)					High Pressure Effect on the Superconductivity in VN			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 84(2015)104706	Bosen Wang,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Kenya Ohgushi		
155746	JPS084104706	Lattice term in SP (beta) = 0.04 mJ/mol.K4. (dC/gamma*Tc) = 1.65. e-ph = 0.75	BNx	N1V1	N	1	V	1																					2015	emu/mol	0.00027	emu.K/mol	0.0101			-13.5																			AB		NaCl	Fm3m		A	4.1427														K	7.98		9.23	8.32			8.32			K/GPa	0.14																T	RES(onset), WHH	10.32							T/K	RES(onset)	1.66			MHC155746														4.05	14				MSP155746			mJ/mol.K2	9.82	SP	458	SP											uOhm.cm							163.6																		mixture(V, VN powder) - pressed into pellet - ANN(1100C,24h, under 0.1 Pa-Ar, in quartz tube)					High Pressure Effect on the Superconductivity in VN			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 84(2015)104706	Bosen Wang,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Kenya Ohgushi		
155747	JPS084115003	P-induced SC. Eu:F:Bi:S = 1:0.9:0.9:1.7 by EDX. R(T) anomaly at 230 K, which decreases with increasing P. I to M transition at 0.3 GPa. Tc and Hc2 for P = 1.8 GPa., where Tc(max).	EuFBiS2	Eu1Bi1S2F1	Eu	1	Bi	1	S	2	F	1																1	2015																											2	CeOBiS2			A	4.0478		13.52											BiS2-layer SC	K	7.8		8.6		2		8.2	MTC155747																			T	RES(onset), extrapolation	3												MHC155747																																																												EuS,BiF3,Bi2S3		mixture - pellet - sealed in quartz tube - heat (700C,20h)					Pressure-Induced Superconductivity in BiS2-Based EuFBiS2			1National Institute for Materials Science, Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 84(2015)115003	Kouji Suzuki,Masashi Tanaka,Saleem J. Denholme,Masaya Fujioka,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
155748	NATM0070953	T<STR> = 154 K ( P4/nmm to Cmma). Tn(Ce) = 3.75 K. AFM moment, data shows at 40 K. M(Fe) = 0.94 and M(Ce) = 0.83 Myu-B at T = 1.7 K.	Ce(O,F)FeAs	Ce1Fe1As1O1	Ce	1	Fe	1	As	1															O	1			2008					Myu-B/Fe	0.8		138																		ABCD		oxypnictide	P4/nmm		A	3.9959		8.6522											data , at T=175K.  For T=1.4K, SG=Cmma, a=5.6626, b=5.6327, c=8.6445	K					1.4																																																																																																							Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155749	NATM0070953	T<STR> = 138 K ( P4/nmm to Cmma). Tn(Ce) = 3.91 K. AFM moment, data shows at 40 K.	Ce(O,F)FeAs	Ce1Fe1As1F0.02O0.98	Ce	1	Fe	1	As	1	F	0.02													O	0.98			2008					Myu-B/Fe	0.67		127																		ABCD		oxypnictide	Cmma		A	5.6586	5.6315	8.6382											data at T=1.4 K	K					1.4																																																																																																							Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155750	NATM0070953	T<STR> = 118 K ( P4/nmm to Cmma). Tn(Ce) = 3.71 K. AFM moment, data shows at 40 K.	Ce(O,F)FeAs	Ce1Fe1As1F0.04O0.96	Ce	1	Fe	1	As	1	F	0.04													O	0.96			2008					Myu-B/Fe	0.4		97.6																		ABCD		oxypnictide	Cmma		A	5.6553	5.6325	8.6355											data at T=1.4 K	K					1.4			MPH155754																																																																																																				Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155751	NATM0070953	T<STR> = 92 K ( P4/nmm to Cmma). Tn(Ce) = 2.89 K. AFM moment, data shows at 40 K.	Ce(O,F)FeAs	Ce1Fe1As1F0.06O0.94	Ce	1	Fe	1	As	1	F	0.06													O	0.94			2008					Myu-B/Fe	0		10.8																		ABCD		oxypnictide	Cmma		A	5.6511	5.6346	8.6335											data at T=1.4 K	K				0			0																																																																																																					Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155752	NATM0070953	T<STR> = 60 K ( P4/nmm to Cmma).	Ce(O,F)FeAs	Ce1Fe1As1F0.08O0.92	Ce	1	Fe	1	As	1	F	0.08													O	0.92			2008																										ABCD		oxypnictide	Cmma		A	5.645	5.6352	8.6287											data at T=1.4 K	K				27.6			27.6																																																																																																					Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155753	NATM0070953		Ce(O,F)FeAs	Ce1Fe1As1F0.1O0.9	Ce	1	Fe	1	As	1	F	0.1													O	0.9			2008																										ABCD		oxypnictide	Cmma		A	5.6386	5.6364	8.6258											data at T=1.4 K	K				32.8			32.8																																																																																																					Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155754	NATM0070953		Ce(O,F)FeAs	Ce1Fe1As1F0.16O0.84	Ce	1	Fe	1	As	1	F	0.16													O	0.84			2008																										ABCD		oxypnictide	P4/nmm		A	3.9847		8.6032											data at T=60 K	K				40.7			40.7	MPH155754																																																																																																				Structural and magnetic phase diagram of CeFeAsO1-xFx and its relation to high-temperature superconductivity			Department of Physics and Astronomy, The University of Tennessee, Knoxville, Tennessee 37996-1200, USA	Nature Mater., 7(2008)953	JUN ZHAO,Q. HUANG,CLARINA DE LA CRUZ,SHILIANG LI,J. W. LYNN,Y. CHEN,M. A. GREEN,G. F. CHEN,G. LI,Z. LI,J. L. LUO,N. L. WANG,PENGCHENG DAI		
155755	PCS0840017	max-(dTc/dP) = 8.25 K/GPa at P=0.97 GPa). For P = 1.68GPa,  Tc(on) = 10.4 K, Hc2(0) =15.9 T	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																												CeOBiS2	P4/nmm		A	4.06		13.38											BiS2-layer SC	K	2.1						2.1	MTC155755																			T	RES(0.9Rn), WHH	1.4												MHC155755																																																												La,La2O3,LaF3,Bi,S		mixture - pellet - sealed in quartz tube(vac) - SIN(650C,12h) - slow cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
155756	PCS0840017	For P = 1.79 GPa,  Tc(on) = 7.33 K, Hc2(0) = 8.8 T	Pr(O,F)BiS2	Pr1Bi1S2F0.5O0.5	Pr	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																												CeOBiS2	P4/nmm		A	4.03		13.42											BiS2-layer SC	K	3.2						3.2	MTC155756																			T	RES(0.9Rn), WHH	2.6												MHC155756																																																												Pr,Pr6O11PrF3,Bi,S		mixture - pellet - sealed in quartz tube(vac) - SIN(650C,12h) - slow cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
155757	PCS0840017	For P = 1.79 GPa,  Tc(on) = 7.33 K, Hc2(0) = 8.2 T	Nd(O,F)BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																												CeOBiS2	P4/nmm		A	3.99		13.38											BiS2-layer SC	K	4.2						4.2	MTC155757																			T	RES(0.9Rn), WHH	2.86												MHC155757																																																												Nd,Nd2O3,NdF3,Bi,S		mixture - pellet - sealed in quartz tube(vac) - SIN(650C,12h) - slow cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
155758	PHB4790051	<119>Sn NMR. Two gaps, (2d/kTc) = 7 and 1.5) from two gap model using T-dependence of (1/T1). (1/T1) vs T shows Tc = 4.5 K for f=33 MHz, H=2.06 T.	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7					7																																																7	6																																															single crystal - crushed - mixed powders in paraffin - NMR sample					<119>Sn-NMR investigations on superconducting Ca3Ir4Sn13:  Evidence for multigap superconductivity			Institute for Solid State Physics, TU Dresden, D-01069 Dresden, Germany	Physica B, 479(2015)51	R. Sarkar,F.Bruckner,M.Gunther,Kefeng Wang,C.Petrovic,P.K.Biswas,H. Luetkens,E.Morenzoni,A. Amato,H-H. Klauss		
155759	PHC470S760	Tc = 15K for 0.01 =< x =<0.8. almost independent of x  in MgxZrNCl, Mg-content x estimated from the total charge during intercalation process.	beta-MgxZrNCl	Mg0.16Zr1N1Cl1	Mg	0.16	Zr	1	N	1	Cl	1																	2010																																														K				15			15																																																																																																Mg-intercalation into beta-Zr(or Hf)NCl was carried out under constant current in an Ar-filled glove box.					A new family of superconducting intercalation compound of MgxMNCl (M = Zr, Hf)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	Physica C, 470(2010)S760	Hotaka Yagyu,Masatsune Kato,Hiroto Tezuka,Takashi Noji,Shoji Yamanaka,Yoji Koike		
155760	PHC470S760	Tc=25 K for 0.1=< x =<0.3 , almost independent of x in MgxHfNCl, Mg-content x estimated from the total charge during intercalation process.	beta-MgxHfNCl	Mg0.3Hf1N1Cl1	Mg	0.3	Hf	1	N	1	Cl	1																	2010																																														K				25			25																																																																																																Mg-intercalation into beta-Zr(or Hf)NCl was carried out under constant current in an Ar-filled glove box.					A new family of superconducting intercalation compound of MgxMNCl (M = Zr, Hf)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	Physica C, 470(2010)S760	Hotaka Yagyu,Masatsune Kato,Hiroto Tezuka,Takashi Noji,Shoji Yamanaka,Yoji Koike		
155761	PHC5190104	M = PC(= C4H6O3). Pc-content not given. Na-content by Faraday's law. Sample contains Fe7Se8(FM) and FeSe(Tc=8 K). SC volume fraction (max) = 5 % for x=0.3. Tc independent of x.	Nax(PC)yFe2Se2	Na0.3M1Fe2Se2	Na	0.3	M	1	Fe	2	Se	2																	2015																																														K				43			43										5																																																																																						electrode(FeSe covered with Ni mesh), counter electrode(Na-metal) in liquid (NaPF6 in PC). Electrochemical intercalation at RT.					Electrochemical  Na-intercalation-induced high-temperature superconductivity in FeSe			Frontier Research Institute for Interdisciplinary Sciences (FRIS), Tohoku University, 6-3 Aoba, Aramaki, Aoba-ku Sendai 980-8579, Japan	Physica C, 519(2015)104	Tetsuya Kajita,Takayuki Kawamata,Takashi Noji,Takehiro Hatakeda,Masatsune Kato,Yoji Koike,Takashi Itoh		
155762	PMB0933680	Pd-10-3-8 structure. SC volume fraction = 20 % at 3.5 K.	(Ca,La)10(Fe,Pd,As)10Pd2.8As8	Ca0.92La0.08Fe8.6Pd4.2As18	Ca	0.92	La	0.08	Fe	8.6	Pd	4.2	As	18															2013																													P1[-]		A	8.8057	8.8134	10.639											Pd10-3-8. triclinic, alpha=85.239, beta=75.653, gamma=89.879	K	10		17				13.5										20																																																																																						solid state reaction. mixture - heat(1000C, in alumina crucible sealed in silica tube under Ar)					Superconductivity and crystal structure of the palladium-iron-arsenides Ca10(Fe1-x PdxAs)10Pd3As8			Department Chemie der Ludwig-Maximilians-Universitat, Butenandtstr. 5-13 (Haus D), 81377, Munchen, Germany	Philo.Mag., 93(2013)3680	C. Hieke,J. Lippmann,T. Sturzer,G. Friederichs,F. Nitsche,F. Winter,R. Pottgen,D. Johrendt		
155765	PRB091174513	RRR = 6.4.(dC/gamma*Tc) = (52.4/22*1.7) = 1.39, Tc = 1.7K(SP). kappa(GL) = 50. Lattice term in SP (beta) = 1.94 mJ/mol.K4.	Bi2Rh3.5S2	Bi2Rh3.5S2	Bi	2	Rh	3.5	S	2																		3	2015									9.861																	A2B2C3	4		C2/m		A	11.5212	7.9408	7.873											monoclinic, beta= 128.033 data at 293 K.	K	2.1						2.1																				T	(dR/dT)max to zero, extrapolation	1.5												MHC155765		A	from Hc2	150			A	from Hc(0) using entropy, GL theory	7450										MSP155765			mJ/mol.K2	22	SP	196	SP																																				mixture(Rh:Bi:S = 55:22.5:22.5) - alumina crucible - sealed in silica ampule(Ar) - heatto 1150C,12 h - keep(1150C,3h) - cool to 700C over 70h)					Superconductivity versus structural phase transition in the closely related Bi2Rh3.5S2 and Bi2Rh3S2			Ames Laboratory, U.S. DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 91(2015)174513	Udhara S. Kaluarachchi,Weiwei Xie,Qisheng Lin,Valentin Taufour,Sergey L. Bud'ko,Gordon J. Miller,Paul C. Canfield		
155766	PRB091174513	not SC. R(T) anomaly at 165 K due to structural transition, not CDW.	Bi2Rh3S3	Bi2Rh3.5S2	Bi	2	Rh	3.5	S	2																		3	2015									9.605																	A2B2C3	4		C2/m		A	11.29	8.378	7.932											monoclinic, beta = 133.286 at 293 K. At 120K, monoclinic, C2/m, a=11.542, b=8.341, c=17.768, beta=107.614	K					0.5																																																										mJ/mol.K2	9.41	SP	209	SP																																				mixture(Rh:Bi:S = 42.6:28.2:29.2) - alumina crucible - sealed in silica ampule(Ar) - heatto 1150C,12 h - keep(1150C,3h) - cool to 700C over 70h)					Superconductivity versus structural phase transition in the closely related Bi2Rh3.5S2 and Bi2Rh3S2			Ames Laboratory, U.S. DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 91(2015)174513	Udhara S. Kaluarachchi,Weiwei Xie,Qisheng Lin,Valentin Taufour,Sergey L. Bud'ko,Gordon J. Miller,Paul C. Canfield		
155768	PRB091174516	Tetra-to-monoclinic structural transition T<STR> = 395 K	LaPt2-xGe2+x	La1Pt2Ge2	La	1	Pt	2	Ge	2																		1	2015																										AB2C2	4	CaBe2Ge2			A	4.4445	4.429	9.894											monoclinic below T<STR> = 354	K		0.41		0.41			0.41																																																																																														La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155769	PRB091174516	Tetra-to-monoclinic structural transition T<STR> = 354 K	LaPt2-xGe2+x	La1Pt1.97Ge2.03	La	1	Pt	1.97	Ge	2.03																		1	2015																										AB2C2	4	CaBe2Ge2			A	4.431	4.4195	9.9203												K		0.83		0.85			0.83																																																																																														La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155770	PRB091174516	Tetra-to-monoclinic structural transition T<STR> = 275 K	LaPt2-xGe2+x	La1Pt1.94Ge2.06	La	1	Pt	1.94	Ge	2.06																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.396		9.9466												K		0.95		0.96			0.95																																																																																														La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155771	PRB091174516	Tetra-to-monoclinic structural transition T<STR> = 210 K	LaPt2-xGe2+x	La1Pt1.9Ge2.1	La	1	Pt	1.9	Ge	2.1																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.3881		9.9752												K		1.67		1.63			1.67	MPH155771																																																																																													La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155772	PRB091174516		LaPt2-xGe2+x	La1Pt1.85Ge2.15	La	1	Pt	1.85	Ge	2.15																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.3881		10.0131												K		1.87					1.87																																																																																														La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155773	PRB091174516	solubility limit Tetra-to-monoclinic structural transition T<STR> = 50 K	LaPt2-xGe2+x	La1Pt1.8Ge2.2	La	1	Pt	1.8	Ge	2.2																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.3929		10.044												K		1.95		1.95			1.95	MPH155771																																																																																													La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155774	PRB091174516	over solubility limit, Tc not measured	LaPt2-xGe2+x	La1Pt1.75Ge2.25	La	1	Pt	1.75	Ge	2.25																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.3928		10.0523												K																																																																																																					La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
155775	PRB091174516	over solubility limit, Tc not measured	LaPt2-xGe2+x	La1Pt1.7Ge2.3	La	1	Pt	1.7	Ge	2.3																		1	2015																										AB2C2	2	CaBe2Ge2	P4/nmm		A	4.3922		10.0527												K																																																																																																					La(3N),Pt(5N),Ge(5N)		arc-melting - wrapped in Ta foil - sealed in quartz tube (He) - ANN(1000C,3d) - cool to RT over 3 days					Superconductivity and the electronic phase diagram of LaPt2-xGe2+x			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 91(2015)174516	S. Maeda,K. Matano,R. Yatagai,T. Oguchi,Guo-qing Zheng		
156000	JPS084014707	Tc defined by onset of ac-SUS. Tc depends on in-plane uniaxial pressure, P//[10], P//[110], P//[001]. Tc(max) = 3.3 K for high Tc phase.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2015																										AB2C4		Sr2RuO4																		K				1.5			1.5	MTC156000																																																																																															Floating zone method using Ru self flux					Higher-Tc Superconducting Phase in Sr2RuO4 Induced by In-Plane Uniaxial Pressure			Department of Materials Science and Engineering, Iwate University, Morioka 020-8551, Japan	J.Phys.Soc.Jpn, 84(2015)014707	Haruka Taniguchi,Keigo Nishimura,Swee K. Goh,Shingo Yonezawa,Yoshiteru Maeno		
156001	JPS084044710	Two phases: SC phase ( 16.4 wt % in DB) and AFM phase(83.6 wt %), SG=I4/m, a=8.77540, c=14.57582 A	RbxFe2-ySe2	Rb0.8Fe1.7Se2	Rb	0.8	Fe	1.7	Se	2																		3	2015																										AB2C2			I4/mmm		A	3.84702		14.768											Two phases, onother phase: SG=I4/m (83.6 wt %)	K	31.4			32			32																																																																							Ohm.cm								0.012				0.771													flux method. mixture((Fe2-y):Rb = x:1) sealed in quartz tube - heat to 1030C - hold(4h) - cool to 750C (6C/h) - FC to RT					Identification of Various Coexisting Phases in Superconducting and Non-superconducting Samples of RbxFe2-ySe2			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)044710	Yoshiaki Kobayashi,Shohei Kototani,Kazuki Ohishi,Masayuki Itoh,Akinori Hoshikawa,Toru Ishigaki,Masatoshi Sato		
156002	JPS084044710	Three phases: not SC phase(68wt % in DB) and AFM-1 phase(22 wt %) SG=I4/m, a=8.7672, c=14.6058 and AFM-2 phase(10 wt %), SG=Pmna, a=5.4416, b=5.4699, c=14.328A	RbxFe2-ySe2	Rb0.7Fe1.9Se2	Rb	0.7	Fe	1.9	Se	2																		3	2015																										AB2C2			I4/mmm		A	3.85792		14.7583											Three phases, AFM-1 phase (22wt %, SG=I4/m, a=8.7672, c=14.6058), AFM-2 phase(10 wt %, SG=Pmna, a=5.4416, b=5.4699, c=14.328)	K					4.2																																																																									Ohm.cm												1.26													flux method. mixture((Fe2-y):Rb = x:1) sealed in quartz tube - heat to 1050C - hold(4h) - cool to 750C (6C/h) - FC to RT					Identification of Various Coexisting Phases in Superconducting and Non-superconducting Samples of RbxFe2-ySe2			Department of Physics, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan	J.Phys.Soc.Jpn, 84(2015)044710	Yoshiaki Kobayashi,Shohei Kototani,Kazuki Ohishi,Masayuki Itoh,Akinori Hoshikawa,Toru Ishigaki,Masatoshi Sato		
156003	NAP0100300	not SC. H-content x , determined by thermal desorption spectroscopy. nominal x = 0.63. Structural transition (T-O) at 95 K. Tn(AF-2 phase) = 92 K	LaFeAs(O,H)	La1Fe1As1H0.51O0.49	La	1	Fe	1	As	1	H	0.51													O	0.49		3	2014								92																		ABCD		oxypnictide	P4/nmm		A	3.97565		8.65241											T-O transition at 95 K. At 43K, SG = Aem2, a=8.6365, b=5.6243, c=5.6004A.	K					2																																																																																																							Bipartite magnetic parent phases in the iron oxypnictide superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Nature Physics, 10(2014)300	M. Hiraishi,S. Iimura,K. M. Kojima,J. Yamaura,H. Hiraka,K. Ikeda,P. Miao,Y. Ishikawa,S. Torii,M. Miyazaki,I. Yamauchi,A. Koda,K. Ishii,M. Yoshida,J. Mizuki,R. Kadono,R. Kumai,T. Kamiyama,T. Otomo,Y. Murakami		
156004	NAP0100300	H-content x , determined by thermal desorption spectroscopy. nominal x = 0.53. Structural transition (T-O) at 79.5 K. Tn(AF-2 phase) = 76  K	LaFeAs(O,H)	La1Fe1As1H0.45O0.55	La	1	Fe	1	As	1	H	0.45													O	0.55		3	2014								76																		ABCD		oxypnictide	P4/nmm		A	3.9788		9.0324												K		0					0										3																																																																																											Bipartite magnetic parent phases in the iron oxypnictide superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Nature Physics, 10(2014)300	M. Hiraishi,S. Iimura,K. M. Kojima,J. Yamaura,H. Hiraka,K. Ikeda,P. Miao,Y. Ishikawa,S. Torii,M. Miyazaki,I. Yamauchi,A. Koda,K. Ishii,M. Yoshida,J. Mizuki,R. Kadono,R. Kumai,T. Kamiyama,T. Otomo,Y. Murakami		
156005	NAP0100300	H-content x , determined by thermal desorption spectroscopy. nominal x = 0.53. Tn(AF-2 phase) = 43  K. Coexist of SC and AF-2 (volume fractin 61%)	LaFeAs(O,H)	La1Fe1As1H0.42O0.58	La	1	Fe	1	As	1	H	0.42													O	0.58		3	2014								43																		ABCD		oxypnictide	P4/nmm																	K		20.3					20.3	MPH156005									32																																																																																											Bipartite magnetic parent phases in the iron oxypnictide superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Nature Physics, 10(2014)300	M. Hiraishi,S. Iimura,K. M. Kojima,J. Yamaura,H. Hiraka,K. Ikeda,P. Miao,Y. Ishikawa,S. Torii,M. Miyazaki,I. Yamauchi,A. Koda,K. Ishii,M. Yoshida,J. Mizuki,R. Kadono,R. Kumai,T. Kamiyama,T. Otomo,Y. Murakami		
156006	NAP0100300	H-content x , determined by thermal desorption spectroscopy. nominal x = 0.53. Tn(AF-2 phase) = 35  K. Coexist of SC and AF-2 (volume fractin 30%)	LaFeAs(O,H)	La1Fe1As1H0.41O0.59	La	1	Fe	1	As	1	H	0.41													O	0.59		3	2014								35																		ABCD		oxypnictide	P4/nmm																	K		19.5					19.5										34																																																																																											Bipartite magnetic parent phases in the iron oxypnictide superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Nature Physics, 10(2014)300	M. Hiraishi,S. Iimura,K. M. Kojima,J. Yamaura,H. Hiraka,K. Ikeda,P. Miao,Y. Ishikawa,S. Torii,M. Miyazaki,I. Yamauchi,A. Koda,K. Ishii,M. Yoshida,J. Mizuki,R. Kadono,R. Kumai,T. Kamiyama,T. Otomo,Y. Murakami		
156007	NAP0100300	H-content x , determined by thermal desorption spectroscopy. nominal x = 0.53. Tn(AF-2 phase) = 12  K. Coexist of SC and AF-2 (volume fractin 22%)	LaFeAs(O,H)	La1Fe1As1H0.4O0.6	La	1	Fe	1	As	1	H	0.4													O	0.6		3	2014								12																		ABCD		oxypnictide	P4/nmm																	K		23.9					23.9										107																																																																																											Bipartite magnetic parent phases in the iron oxypnictide superconductor			Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Nature Physics, 10(2014)300	M. Hiraishi,S. Iimura,K. M. Kojima,J. Yamaura,H. Hiraka,K. Ikeda,P. Miao,Y. Ishikawa,S. Torii,M. Miyazaki,I. Yamauchi,A. Koda,K. Ishii,M. Yoshida,J. Mizuki,R. Kadono,R. Kumai,T. Kamiyama,T. Otomo,Y. Murakami		
156008	JPS084114701	Analyzed by alpha-model. Two bands ( alpha = (3.30, 0.86), gap = (10.41, 2.73) meV, gamma = (31.0, 9.1 ) mJ/mol.K2). Tc defined by mid point of SP transition. C(T,H) measured.	(Ba,K)Fe2As2	Ba0.59K0.41Fe2As2	Ba	0.59	K	0.41	Fe	2	As	2																3	2015																										AB2C2		ThCr2Si2																		K		36.9					36.9																																																					MSP156008			mJ/mol.K2	40.1																																							self-flux method. compositions by ICP					Specific Heat of Ba0.59K0.41Fe2As2, an Fe-Pnictide Superconductor with Tc = 36.9 K, and a New Method for Identifying the Electron Contribution			Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, U.S.A.	J.Phys.Soc.Jpn, 84(2015)114701	Costel R. Rotundu,Thomas R. Forrest,Norman E. Phillips,Robert J. Birgeneau		
156009	CEM2320050	Compositions: Cs0.96Pb0.25Bi3.75Te0.604. Lattice term in SP beta=8.75 mJ/mol.K4, delta=0.16 mJ/mol.K6. Tc(SP-mid) = 2.92 K. (dCe/Tc) = 11.51 mJ/mol.K2. (dC/gamma*Tc) = 1.32	Cs(Bi,Pb)4Te6	Ce1Bi3.7Pb0.3Te6	Ce	1	Bi	3.7	Pb	0.3	Te	6																1	2015																										A3B4C6	3		Cmcm		A	6.327	28.648	4.359												K	2.3	2.9	3.1	3.1			2.9										100																																											MSP156009			mJ/mol.K2	8.75	SP	128.4	SP											mOhm.cm							7																Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156010	CEM2320050	Compositions: Cs0.91Pb0.35Bi3.70Te0.604	Cs(Bi,Pb)4Te6	Ce1Bi3.6Pb0.4Te6	Ce	1	Bi	3.6	Pb	0.4	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				3			3																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156011	CEM2320050	Compositions: Cs0.95Pb0.42Bi3.62Te0.601	Cs(Bi,Pb)4Te6	Ce1Bi3.5Pb0.5Te6	Ce	1	Bi	3.5	Pb	0.5	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				3			3																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156012	CEM2320050	Compositions: Cs0.94Pb0.53Bi3.51Te0.602	Cs(Bi,Pb)4Te6	Ce1Bi3.4Pb0.6Te6	Ce	1	Bi	3.4	Pb	0.6	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				3			3																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156013	CEM2320050	Compositions: Cs0.94Pb0.68Bi3.37Te0.601	Cs(Bi,Pb)4Te6	Ce1Bi3.3Pb0.7Te6	Ce	1	Bi	3.3	Pb	0.7	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				2.9			2.9																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156014	CEM2320050	Compositions: Cs0.93Pb0.78Bi3.23Te0.606	Cs(Bi,Pb)4Te6	Ce1Bi3.2Pb0.8Te6	Ce	1	Bi	3.2	Pb	0.8	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				2.9			2.9																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156015	CEM2320050	Compositions: Cs0.92Pb0.85Bi3.20Te0.603	Cs(Bi,Pb)4Te6	Ce1Bi3.1Pb0.9Te6	Ce	1	Bi	3.1	Pb	0.9	Te	6																1	2015																										A3B4C6	3		Cmcm																	K				2.8			2.8																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156016	CEM2320050	Compositions: Cs0.94Pb0.99Bi3.00Te0.607	Cs(Bi,Pb)4Te6	Ce1Bi3Pb1Te6	Ce	1	Bi	3	Pb	1	Te	6																1	2015																										A3B4C6	3		Cmcm		A	6.345	28.68	4.377												K				2.7			2.7																																																																																														Bi2Te3,Pb,Te,Cs		mixture with 1% excess Cs - alumina crucible - sealed in silica tube - preheat(200C,10h) - hold(700C,40h) - cool to RT - heat(700C,40h) - air quench to RT					Superconductivity in the orthorhombic phase of thermoelectric CsPbxBi4-xTe6 with 0.3 =< x =< 1.0			Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 232(2015)50	R.X. Zhang,H.X. Yang,H.F. Tian,G.F. Chen,S.L. Wu,L.L .Wei,J.Q. Li		
156017	JAC6150921	Susceptibility obeys the modified Curie-Weis law for T > 120 K. R(0.4K) = 702 uOhm.cm.	Ce3Ru4Sn13	Ce3Ru4Sn13	Ce	3	Ru	4	Sn	13																		1	2014																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K					0.4																																																																									uOhm.cm											943														arc-melting several times. ANN(870C,12days)					Crystal electric field and the ground state properties of heavy fermion Ce3Ru4Sn13			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys Compd., 615(2014)921	A. Slebarski,M. Fijalkowski,J. Goraus,L. Kalinowski,P. Witas		
156018	JAC6150921	High-Tc phase. Tc defined at R = 0.5Rn. R(4K) = 206 uOhm.cm	La3Ru4Sn13	La3Ru4Sn13	La	3	Ru	4	Sn	13																		1	2014					Myu-B/mol	0.75																				A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K		3.75					3.75																				T	RES(0.5Rn, GL approx.	3.05												MHC156018		A	from Hc2	90																																	uOhm.cm							206				363														arc-melting several times. ANN(870C,12days)					Crystal electric field and the ground state properties of heavy fermion Ce3Ru4Sn13			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys Compd., 615(2014)921	A. Slebarski,M. Fijalkowski,J. Goraus,L. Kalinowski,P. Witas		
156019	JAC6150921	bulk-Tc = 1.55 K, defined as mid point of SP-transition. Gap = 1.5 K from SP. (dC/gamma*Tc) = 1.6	La3Ru4Sn13	La3Ru4Sn13	La	3	Ru	4	Sn	13																		1	2014																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K		1.55					1.55																				T	SP.	1.45												MHC156018		A	from Hc2	180										2.1	14							mJ/mol.K2	9.9	SP	150	SP																																				arc-melting several times. ANN(870C,12days)					Crystal electric field and the ground state properties of heavy fermion Ce3Ru4Sn13			Institute of Physics, University of Silesia, 40-007 Katowice, Poland	J.Alloys Compd., 615(2014)921	A. Slebarski,M. Fijalkowski,J. Goraus,L. Kalinowski,P. Witas		
156020	JAC6450158	Tc(SP) = 0.65 K.	U	U1	U	1																							2015																																													alpha-U type	K		1.24				0.2	1.24																				T	RES(0.5Rn),extrapolation	0.3							T/K	RES(0.5Rn)	0.35			MHC156023																																					uOhm.cm	14										53												U(2N8),T(3N5)		arc-melting-remelt 3 times - splat cooled system (cooling rate= 10^6 K/s) - resultant sample(20mm dia x (100-200) micro-m thickness)					Structure and superconducting transition in splat-cooled U-T alloys (T = Mo, Pd, Pt)			Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	J. Alloys Compd., 645(2015)158	N.-T.H. Kim-Ngan,M. Paukov,S. Sowa,M. Krupska,I. Tkach,L. Havela		
156021	JAC6450158	Tc(SP) = 2.1 K.	U1-xMox	U0.85Mo0.15	U	0.85	Mo	0.15																					2015																																													gamma-U type	K		2.1				0.02	2.1																				T	RES(0.5Rn),extrapolation	6.7							T/K	RES(0.5Rn)	3.6																																								uOhm.cm	95										89												U(2N8),T(3N5)		arc-melting-remelt 3 times - splat cooled system (cooling rate= 10^6 K/s) - resultant sample(20mm dia x (100-200) micro-m thickness)					Structure and superconducting transition in splat-cooled U-T alloys (T = Mo, Pd, Pt)			Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	J. Alloys Compd., 645(2015)158	N.-T.H. Kim-Ngan,M. Paukov,S. Sowa,M. Krupska,I. Tkach,L. Havela		
156022	JAC6450158	Tc(SP) = 0.72 K.. R(T) shows two step like behaviour.	U1-xMox	U0.94Mo0.06	U	0.94	Mo	0.06																					2015																																													(alpha+gamma)-U type	K		0.78				0.56	0.78																				T	RES(0.5Rn),extrapolation	2.2							T/K	RES(0.5Rn)	3.6			MHC156023																			MSP156022																		uOhm.cm	82										91												U(2N8),T(3N5)		arc-melting-remelt 3 times - splat cooled system (cooling rate= 10^6 K/s) - resultant sample(20mm dia x (100-200) micro-m thickness)					Structure and superconducting transition in splat-cooled U-T alloys (T = Mo, Pd, Pt)			Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	J. Alloys Compd., 645(2015)158	N.-T.H. Kim-Ngan,M. Paukov,S. Sowa,M. Krupska,I. Tkach,L. Havela		
156023	JAC6450158		U1-xPdx	U0.95Pd0.05	U	0.95	Pd	0.05																					2015																																														K		0.69				0.08	0.69																				T	RES(0.5Rn),extrapolation	1.9							T/K	RES(0.5Rn)	3.2			MHC156023																																					uOhm.cm	36										60												U(2N8),T(3N5)		arc-melting-remelt 3 times - splat cooled system (cooling rate= 10^6 K/s) - resultant sample(20mm dia x (100-200) micro-m thickness)					Structure and superconducting transition in splat-cooled U-T alloys (T = Mo, Pd, Pt)			Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	J. Alloys Compd., 645(2015)158	N.-T.H. Kim-Ngan,M. Paukov,S. Sowa,M. Krupska,I. Tkach,L. Havela		
156024	JAC6450158	Tc(SP) = 0.68 K.	U1-xPtx	U0.95Pt0.05	U	0.95	Pt	0.05																					2015																																														K		0.69				0.02	0.69																				T	RES(0.5Rn),extrapolation	1.8							T/K	RES(0.5Rn)	3.3			MHC156023																			MSP156024																		uOhm.cm	162										175												U(2N8),T(3N5)		arc-melting-remelt 3 times - splat cooled system (cooling rate= 10^6 K/s) - resultant sample(20mm dia x (100-200) micro-m thickness)					Structure and superconducting transition in splat-cooled U-T alloys (T = Mo, Pd, Pt)			Institute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	J. Alloys Compd., 645(2015)158	N.-T.H. Kim-Ngan,M. Paukov,S. Sowa,M. Krupska,I. Tkach,L. Havela		
156025	JAC6600044	(dC/gamma*Tc) = 1.4. Energy gap obtained from SP-fitting.	Ta5GeB2	Ta5Ge1B2	Ta	5	Ge	1	B	2																			2016																										AB2C5		Cr5B3	I4/mcm		A	6.239		11.578												K	3.5		3.8	3.8			3.8										80										T	RES(onset), WHH	0.519														A	from Hc2	252								meV	0.968	3.45	14				MSP156025			mJ/mol.K2	10.5	SP	348	SP																																									Ta5GeB2: New T2 superconductor phase			Escola de Engenharia de Lorena e USP, Lorena 12602-810, SP, Brazil	J. Alloys Compd., 660(2016)44	L.E. Correa,M.S. da Luz,B.S. de Lima,O.V. Cigarroa,A.A.A.P. da Silva,G.C. Coelho,Z. Fisk,A.J.S. Machado		
156026	JAC6650333	RRR = 2.18.  R(T) = R0 + A*T^2, R0 in DB, A = 5.482 E-6 mOhm.cm/K^2	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		1	2016									8.2																	A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.636														K	1.77		2.5	2.2			2.2																																																																							uOhm.cm							644																La(4N),In(5N),Sn(5N),Co(5N)		arc-melting - (pellet) - sealed in quartz ampoule - ANN(870C,12h)					Improved superconducting properties of La3Co4Sn13 with indium substitution			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	J. Alloys Compd., 665(2016)333	P. Neha,P. Srivastava,R. Jha,Shruti,V.P.S. Awana,S. Patnaik		
156027	JAC6650333	concentrations: La:Co:Sn:In = 14.09:20.74:62.0:3.1  by EDX. RRR = 1.37. R(T) = R0 + A*T^2, R0 in DB, A = 4.542 E-4 microOhm.cm/K^2	La3Co4(Sn,In)13	La3Co4Sn12.35In0.65	La	3	Co	4	Sn	12.35	In	0.65																1	2016																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.637														K	3.2		4.7	5.1			5.1																																				A		195																																	uOhm.cm							31.3																La(4N),In(5N),Sn(5N),Co(5N)		arc-melting - (pellet) - sealed in quartz ampoule - ANN(870C,12h)					Improved superconducting properties of La3Co4Sn13 with indium substitution			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	J. Alloys Compd., 665(2016)333	P. Neha,P. Srivastava,R. Jha,Shruti,V.P.S. Awana,S. Patnaik		
156028	JAC6650333	concentrations: La:Co:Sn:In = 15.1:20.21:58.32:6.37  by EDX. RRR =2.15. GL(kappa) = 1.53. (dTc/dP) = -0.331, -0.267 for Tc(on) and Tc(zero), respectively.	La3Co4(Sn,In)13	La3Co4Sn11.7In1.3	La	3	Co	4	Sn	11.7	In	1.3																1	2016																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.639														K			5.1	4.6		0.1	4.6	MTC156028		K/GPa	-0.311							Oe	M-H curve	28							T	RES(onset), extrapolation	0.68												MHC156028		A	from Hc2	216			A	Hc1, GL theory	332																												uOhm.cm							16.45																La(4N),In(5N),Sn(5N),Co(5N)		arc-melting - (pellet) - sealed in quartz ampoule - ANN(870C,12h)					Improved superconducting properties of La3Co4Sn13 with indium substitution			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	J. Alloys Compd., 665(2016)333	P. Neha,P. Srivastava,R. Jha,Shruti,V.P.S. Awana,S. Patnaik		
156029	JJP043L1480	bulc SC. SC-volume fraction  = 6 % at 2K. Li-doping, x = 0.15 by ICP. carrier = electron.	LixSr2CuO2Br2	Li0.15Sr2Cu1Br2O2	Li	0.15	Sr	2	Cu	1	Br	2													O	2			2004																															A	3.99													tetragonal	K				8			8										6																																																																																						SrCuO2 mixed with SrBr2 - SIN(825C,24h) - Sr2CuO2Br2 - mixed with naphthalene(30 wt%) - Li-intercalation using PC as an electrolyte					New Electron-Doped Superconducting Cuprate LixSr2CuO2Br2			Department of Applied Physics, Graduate School of Engineering, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	Jpn J.Appl.Phys., 43(2004)L1480	Tetsuya KAJITA,Masatsune KATO,Takashi SUZUKI,Takashi ITOH,Takashi NOJI,Yoji KOIKE		
156030	JPS0711134	Elastic modulus measured by ultrasonic measurements. (dTc/dP) = -1.16 (in DB), +0.96 K/GPa for //a and //c uniaxial P are estimated.	Sr2RuO4	Sr2Ru1O4	Sr	2	Ru	1																	O	4		3	2002																												T																		K		1.37					1.37			K/GPa	-1.16																																																																																																	Unconventional Strain Dependence of Superconductivity in Spin-Triplet Superconductor Sr2RuO4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8530	J.Phys.Soc.Jpn, 71(2002)1134	Noriki OKUDA,Takashi SUZUKI,Zhiqiang MAO,Yoshiteru MAENO,Toshizo FUJITA		
156031	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 2.31E-8 Ohm.cm/K^2.	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2011																										ABCD		oxypnictide																		K		5.8					5.8																																																																		uV/K	-23			MTP156031	uOhm.cm							67.6				1500												LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156032	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 2.78E-8 Ohm.cm/K^2.	LaFeP(O,F)	La1Fe1P1F0.03O0.97	La	1	Fe	1	P	1	F	0.03													O	0.97		1	2011																										ABCD		oxypnictide																		K		7.8					7.8																																																													W/K.m	2.53			MTHC156032	uV/K	-34.2			MTP156032	uOhm.cm							77.1																LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156033	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 2.43E-8 Ohm.cm/K^2.	LaFeP(O,F)	La1Fe1P1F0.05O0.95	La	1	Fe	1	P	1	F	0.05													O	0.95		1	2011																										ABCD		oxypnictide																		K		8					8																																																																		uV/K	-36			MTP156033	uOhm.cm							78.8																LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156034	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 3.31E-8 Ohm.cm/K^2.	LaFeP(O,F)	La1Fe1P1F0.08O0.92	La	1	Fe	1	P	1	F	0.08													O	0.92		1	2011																										ABCD		oxypnictide																		K		7.8					7.8																																																													W/K.m	2.92			MTHC156034	uV/K	-35.6			MTP156034	uOhm.cm							117																LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156035	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 3.14E-8 Ohm.cm/K^2.	LaFeP(O,F)	La1Fe1P1F0.1O0.9	La	1	Fe	1	P	1	F	0.1													O	0.9		1	2011																										ABCD		oxypnictide																		K		6.2					6.2																																																																		uV/K	-34.2			MTP156035	uOhm.cm																							LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156036	JPS080044704		LaFeAs(O,F)	La1Fe1As1F0.02O0.98	La	1	Fe	1	As	1	F	0.02													O	0.98		1	2011																										ABCD		oxypnictide																		K					4																																																																				uV/K	-33.1			MTP156036																								LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156037	JPS080044704		LaFeAs(O,F)	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95		1	2011																										ABCD		oxypnictide																		K		14.5					14.5																																																																		uV/K	-39.2			MTP156037																								LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156038	JPS080044704		LaFeAs(O,F)	La1Fe1As1F0.08O0.92	La	1	Fe	1	As	1	F	0.08													O	0.92		1	2011																										ABCD		oxypnictide																		K		22.8					22.8																																																													W/K.m	1.94			MTHC156038	uV/K	-49.3			MTP156038																								LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156039	JPS080044704		LaFeAs(O,F)	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2011																										ABCD		oxypnictide																		K		25.2					25.2																																																																		uV/K	-39.4			MTP156039																								LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156040	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 1.75E-8 Ohm.cm/K^2.	LaFeAs(O,F)	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2011																										ABCD		oxypnictide																		K		22.9					22.9																																																																		uV/K	-45.9			MTP156040	uOhm.cm							50.1																LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156041	JPS080044704	R(T) = R0 +A*T^2, R0 in DB, A = 1.66E-8 Ohm.cm/K^2.	LaFeAs(O,F)	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86		1	2011																										ABCD		oxypnictide																		K		12.9					12.9																																																													W/K.m	2.52			MTHC156041	uV/K	-42.4			MTP156041	uOhm.cm							48.1																LaP,LaAs,Fe2O3,FeF2		Two step solid state reaction. First step: raw materials prepared.  mixture - pellet - ANN(1100C,40h, in silica tube)					Thermoelectric Properties of LaFePO1-xFx and LaFeAsO1-xFx : Possibility of the Hidden Mass Enhancement of LaFeAsO1-xFx			Department of Nano-Structures and Advanced Materials, Kagoshima University, 1-21-40 Korimoto, Kagohisma 890-0065, Japan	J.Phys.Soc.Jpn, 80(2011)044704	Tetsuji OKUDA,Wataru HIRATA,Akira TAKEMORI,Shinnosuke SUZUKI,Satoshi SAIJO,Shigeki MIYASAKA,Setsuko TAJIMA		
156042	JPS081114717	Hc2(T) = Hc2(0)*(1-t^(1.5))^(1.5).	BaPdxSi2-x	Ba1Pd0.3Si1.7	Ba	1	Pd	0.3	Si	1.7																		1	2012																										AB2		AlB2	P6/mmm	191	A	4.154		5.009												K				2.9			2.9											Oe	M-H curve. GL-approx.	16							T	RES(mid). GL-approx..	2.2												MHC156042		A	from Hc2	12			A	From Hc, Hc1	640																																																			Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156043	JPS081114717	Impurity phase = BaSi2. Hc2(T) = Hc2(0)*(1-t^(1.5))^(1.5).	BaPtxSi2-x	Ba1Pt0.3Si1.7	Ba	1	Pt	0.3	Si	1.7																		1	2012																										AB2		AlB2	P6/mmm	191	A	4.142		5.02												K				2.6			2.6											Oe	M-H curve. GL-approx.	8							T	RES(mid). GL-approx..	2.4												MHC156043		A	from Hc2	12			A	From Hc, Hc1	910																																																			Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156044	JPS081114717	Hc2(T) = Hc2(0)*(1-t^(1.5))^(1.5). Lattice term in SP (beta) = 0.15 mJ/mol.K4. (dC/gamma*Tc) = 1.38	BaCuxSi2-x	Ba1Cu0.3Si1.7	Ba	1	Cu	0.3	Si	1.7																		1	2012																										AB2		AlB2	P6/mmm	191	A	4.114		5.042												K				3			3											Oe	M-H curve. GL-approx.	21							T	RES(mid). GL-approx..	2.2												MHC156044		A	from Hc2	12			A	From Hc, Hc1	560										MSP156044			mJ/mol.K2	4.13	SP																																				Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156045	JPS081114717	Hc2(T) = Hc2(0)*(1-t^(1.5))^(1.5).	BaAgxSi2-x	Ba1Ag0.3Si1.7	Ba	1	Ag	0.3	Si	1.7																		1	2012																										AB2		AlB2	P6/mmm	191	A	4.218		4.993												K				3.2			3.2											Oe	M-H curve. GL-approx.	18							T	RES(mid). GL-approx..	3.3												MHC156045		A	from Hc2	10			A	From Hc, Hc1	600																																																			Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156046	JPS081114717	Hc2(T) = Hc2(0)*(1-t^(1.5))^(1.5).	BaAuxSi2-x	Ba1Au0.3Si1.7	Ba	1	Au	0.3	Si	1.7																		1	2012																										AB2		AlB2	P6/mmm	191	A	4.189		5.001												K				3.2			3.2											Oe	M-H curve. GL-approx.	15									3.7												MHC156046		A	from Hc2	10			A	From Hc, Hc1	660																																																			Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156047	JPS081114717		BaAgxSi2-x	Ba1Ag0.2Si1.8	Ba	1	Ag	0.2	Si	1.8																			2012																										AB2		AlB2	P6/mmm	191																K				3.2			3.2																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156048	JPS081114717		BaCuxSi2-x	Ba1Cu0.2Si1.8	Ba	1	Cu	0.2	Si	1.8																			2012																										AB2		AlB2	P6/mmm	191	A	4.1125		5.0244												K				3.02			3.02																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156049	JPS081114717		BaPdxSi2-x	Ba1Pd0.2Si1.8	Ba	1	Pd	0.2	Si	1.8																			2012																										AB2		AlB2	P6/mmm	191																K				2.91			2.91																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156050	JPS081114717		BaAgxSi2-x	Ba1Ag0.4Si1.6	Ba	1	Ag	0.4	Si	1.6																			2012																										AB2		AlB2	P6/mmm	191																K				2.79			2.79	MTC156051																																																																																													Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156051	JPS081114717		BaCuxSi2-x	Ba1Cu0.4Si1.6	Ba	1	Cu	0.4	Si	1.6																			2012																										AB2		AlB2	P6/mmm	191	A	4.1247		5.012												K				2.11			2.11	MTC156051																																																																																													Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156052	JPS081114717		BaPdxSi2-x	Ba1Pd0.4Si1.6	Ba	1	Pd	0.4	Si	1.6																			2012																										AB2		AlB2	P6/mmm	191																K				1.11			1.11	MTC156051																																																																																													Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156053	JPS081114717		BaAgxSi2-x	Ba1Ag0.5Si1.5	Ba	1	Ag	0.5	Si	1.5																			2012																										AB2		AlB2	P6/mmm	191																K				1.21			1.21																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156054	JPS081114717	Lattice term in SP (beta) = 0.14 mJ/mol.K4	BaCuxSi2-x	Ba1Cu0.5Si1.5	Ba	1	Cu	0.5	Si	1.5																			2012																										AB2		AlB2	P6/mmm	191	A	4.1204		5.006												K				2.53			2.53																																																								mJ/mol.K2	3.87	SP																																				Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156055	JPS081114717		BaPdxSi2-x	Ba1Pd0.5Si1.5	Ba	1	Pd	0.5	Si	1.5																			2012																										AB2		AlB2	P6/mmm	191																K				0.6			0.6																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156056	JPS081114717		BaCuxSi2-x	Ba1Cu0.6Si1.4	Ba	1	Cu	0.6	Si	1.4																			2012																										AB2		AlB2	P6/mmm	191	A	4.1332		4.9859												K				1.74			1.74																																																																																														Ba(2N5),Si(5N),(3N)-Pd,Pt,Cu,Ag,Au		arc-melting					Superconductivity in Ba(TM,Si)2 (TM = Pd, Pt, Cu, Ag, and Au) with the AlB2-Type Structure			Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	J.Phys.Soc.Jpn, 81(2012)114717	Kenji KAWASHIMA,Keigo INOUE,Takuya ISHIKAWA,Michinori FUKUMA,Masaaki YOSHIKAWA,Jun AKIMITSU		
156057	NJP010123003	impurity phase: FeAs. RRR = 4.87. T<SDW> = 200K defined as R(T) anomaly. Hc2, Hirr defined as 0.9Rn and 0.1Rn, respectively.	(Eu,Na)Fe2As2	Eu0.7Na0.3Fe2As2	Eu	0.7	Na	0.3	Fe	2	As	2																1	2008																										AB2C2		ThCr2Si2			A	3.8978		12.2623												K			34.7	32			32										90										T	RES(0.9Rn), WHH	90							T/K	RES(0.9Rn)	3.87			MHC156057		A	from Hc2	19																																																								Eu(4N),Na(2N/5),Fe(4N),As(5N)		mixture - in Nb tube - sealed in Fe-tube - slow heat to 850 C - keep (35h) - ANN ( in Ar)					Superconductivity at 34.7K in the iron arsenide Eu0.7Na0.3Fe2As2			Key Laboratory of Applied Superconductivity, Institute of Electrical Engineering, Chinese Academy of Sciences, P O Box 2703, Beijing 100190, People's Republic of China	New J.Phys., 10(2008)123003	Yanpeng Qi,Zhaoshun Gao,Lei Wang,Dongliang Wang,Xianping Zhang,Yanwei Ma		
156058	PHB1630131	not SC. Ferromag-order at 3.9 K by SP peak. Lattice term in SP (beta) = 2.41 mJ/mol.K4	Ce4Sb3	Ce4Sb3	Ce	4	Sb	3																				3	1990																										A3B4																				K					1.8																																																										mJ/mol.K2	644	SP																																											Ce4Sb3: A ferromagnetic system with Kondo behavior			Department of Physics, Faculty of Science, Tohoku University, Sendai 980, Japan	Physica B, 163(1990)131	T.Tuzuki,O.Nakamura,N.Tomonaga,S.Ozeki,Y.S.Kwon,A.Ochiai,T.Takeda,T.Kasuya		
156059	PHC5190137	grain size = 423 nm, RRR = R300/R40 = 2.53. pinning force(max) = 2.97E+9 N/m3. Jc measured using Bean's model.	MgB2	B2Mg1	B	2	Mg	1																					2015																										AB2		AlB2			A	3.0816														K		37					37																				T	RES(0.9Rn)				11.8			20						MHC156059																																					uOhm.cm							4.82																B(4N),Mg(2N6),glucose(3N)		ball milled using 6 ball of ZrO2 - pelletaize - wrapped in Ta foil - heat to 650 C(5C/min) - hold (650C,2h, in Ar)					Effects of glucose doping on the MgB2 superconductors using cheap crystalline boron			Department of Physics and Astronomy, College of Science, PO Box 2455, King Saud University, Riyadh 11451, Saudi Arabia	Physica C, 519(2015)137	Jafar Meethale Parakkandy,Mohammed Shahabuddin,M. Shahabuddin Shah,Nasser S. Alzayed,Salem A.S. Qaid,Niyaz Ahmad Madhar,Shahid M. Ramay,Muhammad Ali Shar		
156060	PHC5190137	2%-glucose(C6H12O6) doped sample. grain size = 413 nm, RRR = R300/R40 = 2.18. pinning force(max) = 2.10E+9 N/m3. Jc measured using Bean's model.	Mg(B,C)2	Mg1B1.98C0.02	Mg	1	B	1.98	C	0.02																			2015																										AB2		AlB2			A	3.0783														K		37					37																				T	RES(0.9Rn)				12.5			20																																											uOhm.cm							6.52																B(4N),Mg(2N6),glucose(3N)		ball milled using 6 ball of ZrO2 - pelletaize - wrapped in Ta foil - heat to 650 C(5C/min) - hold (650C,2h, in Ar)					Effects of glucose doping on the MgB2 superconductors using cheap crystalline boron			Department of Physics and Astronomy, College of Science, PO Box 2455, King Saud University, Riyadh 11451, Saudi Arabia	Physica C, 519(2015)137	Jafar Meethale Parakkandy,Mohammed Shahabuddin,M. Shahabuddin Shah,Nasser S. Alzayed,Salem A.S. Qaid,Niyaz Ahmad Madhar,Shahid M. Ramay,Muhammad Ali Shar		
156061	PHC5190137	4%-glucose(C6H12O6) doped sample. grain size = 387 nm, RRR = R300/R40 = 1.91. pinning force(max) = 1.43E+9 N/m3. Jc measured using Bean's model.	Mg(B,C)2	Mg1B1.968C0.032	Mg	1	B	1.968	C	0.032																			2015																										AB2		AlB2			A	3.0766														K		37					37																				T	RES(0.9Rn)				13.9			20																																											uOhm.cm							8.52																B(4N),Mg(2N6),glucose(3N)		ball milled using 6 ball of ZrO2 - pelletaize - wrapped in Ta foil - heat to 650 C(5C/min) - hold (650C,2h, in Ar)					Effects of glucose doping on the MgB2 superconductors using cheap crystalline boron			Department of Physics and Astronomy, College of Science, PO Box 2455, King Saud University, Riyadh 11451, Saudi Arabia	Physica C, 519(2015)137	Jafar Meethale Parakkandy,Mohammed Shahabuddin,M. Shahabuddin Shah,Nasser S. Alzayed,Salem A.S. Qaid,Niyaz Ahmad Madhar,Shahid M. Ramay,Muhammad Ali Shar		
156062	PHC5190137	6%-glucose(C6H12O6) doped sample. grain size = 297 nm, RRR = R300/R40 = 1.72. pinning force(max) = 1.27E+9 N/m3. Jc measured using Bean's model.	Mg(B,C)2	Mg1B1.938C0.062	Mg	1	B	1.938	C	0.062																			2015																										AB2		AlB2			A	3.0719														K		37					37																				T	RES(0.9Rn)				14.6			20						MHC156062																																					uOhm.cm							10.51																B(4N),Mg(2N6),glucose(3N)		ball milled using 6 ball of ZrO2 - pelletaize - wrapped in Ta foil - heat to 650 C(5C/min) - hold (650C,2h, in Ar)					Effects of glucose doping on the MgB2 superconductors using cheap crystalline boron			Department of Physics and Astronomy, College of Science, PO Box 2455, King Saud University, Riyadh 11451, Saudi Arabia	Physica C, 519(2015)137	Jafar Meethale Parakkandy,Mohammed Shahabuddin,M. Shahabuddin Shah,Nasser S. Alzayed,Salem A.S. Qaid,Niyaz Ahmad Madhar,Shahid M. Ramay,Muhammad Ali Shar		
156063	PRB082104518	R(T) anomaly at 150 K due to AFM along c-axis. Curie-Weis law for 150<T<300 K.  Weak FM below 52 K .	Sr2VFeAsO3	Sr2V1Fe1As1O3	Sr	2	V	1	Fe	1	As	1													O	3		1	2010					myu-B/V	1.2	52																						P4/nmm		A	3.9352		15.6823											STR = 22426 or 21113 type. As-Fe-As angle = 109.1 deg.	K			24				24																																																																							mOhm.cm							4.05				7.05												SrO,MgO,V,Fe,Fe2O3,As		mixture(powder) - alumina tube - sealed in quartz ampoule - heat to 1273K - hold(24h) - ground - pellet - SIN(1350K,48h)					Self-doping effect and successive magnetic transitions in superconducting Sr2VFeAsO3			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 82(2010)104518	Guang-Han Cao,Zhifeng Ma,Cao Wang,Yunlei Sun,Jinke Bao,Shuai Jiang,Yongkang Luo,Chunmu Feng,Yi Zhou,Zhi Xie,Fengchun Hu,Shiqiang Wei,I. Nowik,I. Felner,Lei Zhang,Zhu'an Xu,Fu-Chun Zhang		
156064	PRB082104518	no anomaly in R(T).	Sr2(V,Mg)FeAsO3	Sr2V0.9Mg0.1Fe1As1O3	Sr	2	V	0.9	Mg	0.1	Fe	1	As	1											O	3		1	2010																													P4/nmm		A	3.9334		15.7488											STR = 22426 or 21113 type. As-Fe-As angle = 109.7 deg.	K			30				30																																																																							mOhm.cm							3.12				6.61												SrO,MgO,V,Fe,Fe2O3,As		mixture(powder) - alumina tube - sealed in quartz ampoule - heat to 1273K - hold(24h) - ground - pellet - SIN(1350K,48h)					Self-doping effect and successive magnetic transitions in superconducting Sr2VFeAsO3			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 82(2010)104518	Guang-Han Cao,Zhifeng Ma,Cao Wang,Yunlei Sun,Jinke Bao,Shuai Jiang,Yongkang Luo,Chunmu Feng,Yi Zhou,Zhi Xie,Fengchun Hu,Shiqiang Wei,I. Nowik,I. Felner,Lei Zhang,Zhu'an Xu,Fu-Chun Zhang		
156065	PRB087045124	Impurity phases: K2Ni3S3(3 wt.%), Ni3S2(1 wt.%). Volume anomaly at 8.9 and 13 K.	KNi2S2	K1Ni2S2	K	1	Ni	2	S	2																		1	2013																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.7922		12.8193												K		0.46					0.46																				T	SP	0.04														A	from Hc2	900																		mJ/mol.K2	67.6	SP	219	SP											mOhm.cm							60																		See J.Am.Chem.Soc., 134(2012)7750					Charge density wave fluctuations, heavy electrons, and superconductivity in KNi2S2			Department of Chemistry, Johns Hopkins University, Baltimore, Maryland 21218, USA	Phys.Rev.B, 87(2013)045124	James R. Neilson,Tyrel M. McQueen,Anna Llobet,Jiajia Wen,Matthew R. Suchomel		
156066	PRB088014517	kappa-1(GL) = 87, 15 for H//ab and H//c, respectively. Hc(0) = 73 mT from SP. Hp(Pauli limit) = 6.7 T. Hc2 measured by SUS, thermal expansion, magnetostriction.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2	I4/mmm																	K		3.4					3.4																				T	SUS, WHH		5	1.5					T/K	SUS		3.7	0.6	MHC156066																						mJ/mol.K2	103	SP																																						Flux method.. mixture(K:Fe:As = 0.3:0.1:0.6) - alumina crucible - sealed in Fe cylinder(Ar) - heat to 980 C - slow cool (0.5C/h)					Strong Pauli-limiting behavior of Hc2 and uniaxial pressure dependencies in KFe2As2			Institut fur Festkorperphysik, Karlsruher Institut fur Technologie, 76021 Karlsruhe, Germany	Phys.Rev.B, 88(2013)014517	P. Burger,F. Hardy,D. Aoki,A. E. Bohmer,R. Eder,R. Heid,T. Wolf,P. Schweiss,R. Fromknecht,M. J. Jackson,C. Paulsen,C. Meingast		
156067	MAT1302.1696	RRR = 1150. (dC/gamma*Tc) = 0.53. Lattice term in SP (beta) = 0.35 mJ/mol.K4.A=0.025 uOhm.cm/K2 in R(T) = R0 + A*T^2.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																			2013																										AB2C2		ThCr2Si2	I4/mmm																	K		3.4				0.5	3.4																																																					MSP156067			mJ/mol.K2	102	SP	177	SP											uOhm.cm							0.39				450																			Evidence of Strong Correlations and Coherence-Incoherence Crossover in the Iron Pnictide Superconductor KFe2As2			Institut fur Festkorperphysik, Karlsruher Institut fur Technologie, 76021 Karlsruhe, Germany	cond-mat/1302.1696	F. Hardy,A. E. Bohmer,D. Aoki,P. Burger,T. Wolf,P. Schweiss,R. Heid,P.Adelmann,Y.X.Yao,G.Kotliar,J.Schmalian,C.Meingast		
156068	PRB089064511	The hight of pnictogen from the Fe plane h<pn> = 1.24 A. As-Fe-As bonding angle alpha = 116.3 degree.	LaFe(As,P)(O,F)	La1Fe1As0.6P0.4F0.1O0.9	La	1	Fe	1	As	0.6	P	0.4	F	0.1											O	0.9		1	2014																										ABCD		oxypnictide			A	4.002													Fe-1111	K		27					27	MTC156068																																																																																															solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156069	PRB089064511		LaFe(As,P)(O,F)	La1Fe1As0.2P0.8F0.1O0.9	La	1	Fe	1	As	0.2	P	0.8	F	0.1											O	0.9		1	2014																										ABCD		oxypnictide																	Fe-1111	K		8.8					8.8																																																																																																solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156070	PRB089064511	The hight of pnictogen from the Fe plane h<pn> = 1.15 A. As-Fe-As bonding angle alpha = 119.7 degree.	LaFeP(O,F)	La1Fe1P1F0.1O0.9	La	1	Fe	1	P	1	F	0.1													O	0.9		1	2014																										ABCD		oxypnictide			A	3.951													Fe-1111	K		5.4					5.4																																																																																																solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156071	PRB089064511	The hight of pnictogen from the Fe plane h<pn> = 1.25 A. As-Fe-As bonding angle alpha = 116.0 degree.	LaFe(As,P)(O,F)	La1Fe1As0.6P0.4F0.05O0.95	La	1	Fe	1	As	0.6	P	0.4	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide			A	4.011													Fe-1111	K		19					19																																																																																																solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156072	PRB089064511		LaFe(As,P)(O,F)	La1Fe1As0.4P0.6F0.05O0.95	La	1	Fe	1	As	0.4	P	0.6	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide																	Fe-1111	K		24					24	MTC156072																																																																																															solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156073	PRB089064511	The hight of pnictogen from the Fe plane h<pn> = 1.12 A. As-Fe-As bonding angle alpha = 121.1 degree.	LaFeP(O,F)	La1Fe1P1F0.05O0.95	La	1	Fe	1	P	1	F	0.05													O	0.95		1	2014																										ABCD		oxypnictide			A	3.959													Fe-1111	K		6.7					6.7																																																																																																solid state reaction. See Physica C, 470(2010)S298					Enhancement of superconducting transition temperature due to antiferromagnetic spin fluctuations in iron pnictides LaFe(As1-xPx)(O1-yFy): <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.B, 89(2014)064511	H. Mukuda,F. Engetsu,K. Yamamoto,K. T. Lai,M. Yashima,Y. Kitaoka,A. Takemori,S. Miyasaka,S. Tajima		
156074	PRB090064504	n = 1.96 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -4.75E-3 cm3/C.	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9653		8.5252											Fe-1111	K		5.42		6.23			5.42																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156075	PRB090064504	n = 1.75 where R(T) = R0 + A*T^n for Tc < T < 100K.	LaFe(As,P)O	La1Fe1As0.1P0.9O1	La	1	Fe	1	As	0.1	P	0.9													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9778		8.5419											Fe-1111	K		5.96		6.39			5.96																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156076	PRB090064504	n = 1.72 where R(T) = R0 + A*T^n for Tc < T < 100K.	LaFe(As,P)O	La1Fe1As0.15P0.85O1	La	1	Fe	1	As	0.15	P	0.85													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9819		8.5493											Fe-1111	K		11.67		11.2			11.67																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156077	PRB090064504	n = 1.69 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -6.26E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.2P0.8O1	La	1	Fe	1	As	0.2	P	0.8													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9846		8.556											Fe-1111	K		11.42		11.78			11.42	MPH156077																																																																																				cm3/C						MRH156077			LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156078	PRB090064504	n = 1.80 where R(T) = R0 + A*T^n for Tc < T < 100K.	LaFe(As,P)O	La1Fe1As0.25P0.75O1	La	1	Fe	1	As	0.25	P	0.75													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9875		8.5684											Fe-1111	K		7.52		7.07			7.52																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156079	PRB090064504	n = 1.63 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -28.84E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.3P0.7O1	La	1	Fe	1	As	0.3	P	0.7													O	1		1	2014								16.2																		ABCD		oxypnictide	P4/nmm		A	3.9891		8.5758											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156080	PRB090064504	n = 1.25 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -43.3E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.4P0.6O1	La	1	Fe	1	As	0.4	P	0.6													O	1		1	2014								35.2																		ABCD		oxypnictide	P4/nmm		A	3.9987		8.6011											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156081	PRB090064504	As content (EDX) same as nominal value	LaFe(As,P)O	La1Fe1As0.5P0.5O1	La	1	Fe	1	As	0.5	P	0.5													O	1		1	2014								12.4																		ABCD		oxypnictide	P4/nmm		A	4.006		8.6089											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156082	PRB090064504	n = 1.30 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -50.9E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.6P0.4O1	La	1	Fe	1	As	0.6	P	0.4													O	1		1	2014								15.1																		ABCD		oxypnictide	P4/nmm		A	4.0174		8.6472											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156083	PRB090064504	n = 0.99 where R(T) = R0 + A*T^n for Tc < T < 100K. Hall coeffic. RH(50K) = -33.8E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.7P0.3O1	La	1	Fe	1	As	0.7	P	0.3													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0232		8.6638											Fe-1111	K		7.83					7.83	MPH156077																																																																																				cm3/C						MRH156083			LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156084	PRB090064504	Hall coeffic. RH(50K) = -41.3E-3 cm3/C.	LaFe(As,P)O	La1Fe1As0.8P0.2O1	La	1	Fe	1	As	0.8	P	0.2													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0318		8.6932											Fe-1111	K		2.31		6.7			2.31																																																																																					cm3/C						MRH156084			LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156085	PRB090064504		LaFe(As,P)O	La1Fe1As0.9P0.1O1	La	1	Fe	1	As	0.9	P	0.1													O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0354		8.7258											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156086	PRB090064504		LaFeAsO	La1Fe1As1O1	La	1	Fe	1	As	1															O	1		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0404		8.749											Fe-1111	K					2																																																																																																LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156087	PRB090064504	F content not measured by EDX. n = 1.79 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFeP(O,F)	La1Fe1P1F0.05O0.95	La	1	Fe	1	P	1	F	0.05													O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9636		8.5251											Fe-1111	K		6.93		6.69			6.93																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156088	PRB090064504	n = 1.50 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.2P0.8F0.05O0.95	La	1	Fe	1	As	0.2	P	0.8	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9821		8.5512											Fe-1111	K		10.87		10.41			10.87																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156089	PRB090064504	n = 1.29 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.4P0.6F0.05O0.95	La	1	Fe	1	As	0.4	P	0.6	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	3.9995		8.5953											Fe-1111	K		24.24		24.03			24.24	MTC156089																																																																																													LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156090	PRB090064504	n = 1.04 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.5P0.5F0.05O0.95	La	1	Fe	1	As	0.5	P	0.5	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.006		8.607											Fe-1111	K		21.2		18.14			21.2																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156091	PRB090064504	n = 1.12 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.6P0.4F0.05O0.95	La	1	Fe	1	As	0.6	P	0.4	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0133		8.6229											Fe-1111	K		19.08		18.86			19.08	MTC156089																																																																																													LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156092	PRB090064504	n = 1.30 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.7P0.3F0.05O0.95	La	1	Fe	1	As	0.7	P	0.3	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0212		8.6443											Fe-1111	K		15.75		15.62			15.75																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156093	PRB090064504	n = 1.58 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.75P0.25F0.05O0.95	La	1	Fe	1	As	0.75	P	0.25	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0232		8.6767											Fe-1111	K		22.38		20.22			22.38																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156094	PRB090064504	n = 1.33 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.8P0.2F0.05O0.95	La	1	Fe	1	As	0.8	P	0.2	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0252		8.6971											Fe-1111	K		25.61		25.75			25.61																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156095	PRB090064504	n = 1.52 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.9P0.1F0.05O0.95	La	1	Fe	1	As	0.9	P	0.1	F	0.05											O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0312		8.7088												K		23.6		17.25			23.6																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156096	PRB090064504	n = 2.03 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFeAs(O,F)	La1Fe1As1F0.05O0.95	La	1	Fe	1	As	1	F	0.05													O	0.95		1	2014																										ABCD		oxypnictide	P4/nmm		A	4.0386		8.7399												K		27.84		27.17			27.84																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156097	PRB090064504	n = 1.40 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.4P0.6F0.1O0.9	La	1	Fe	1	As	0.4	P	0.6	F	0.1											O	0.9		1	2014																										ABCD		oxypnictide	P4/nmm																	K		21.14		21.67			21.14																																																																																														LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156098	PRB090064504	n = 1.16 where R(T) = R0 + A*T^n for Tc < T < 100K	LaFe(As,P)(O,F)	La1Fe1As0.6P0.4F0.1O0.9	La	1	Fe	1	As	0.6	P	0.4	F	0.1											O	0.9		1	2014																										ABCD		oxypnictide	P4/nmm																	K		27		23			27	MTC156098																																																																																													LaAs,LaP,Fe2O3,Fe,LaF3		mixture - pellet - sealed in quartz tube - heat(1100C,4d)					Evolution of the phase diagram of LaFeP1-xAsxO1- yFy ( y = 0-0.1)			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 90(2014)064504	K. T. Lai,A. Takemori,S. Miyasaka,F. Engetsu,H. Mukuda,S. Tajima		
156099	PRB091220505	Cr chain //rod direction. Hc2 measured by R(T) for H<14T, and proximity detector oscilator for H > 14 T. Anisotropy (Hc2) = 0.35 at Tc and = 1.7 at 0.7 K.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2015																										A2B3C3		K2Cr3As3																		K			6.1				6.1																				T	RES(on), extrapolation.		37	23					T/K	RES(on)		7	12	MHC156099		A		22																																																										K:Cr:As = 6:1:7 - alumina crucible - welded in Ta tube - slow heat to 1000C - cool to 700C within 3 days.					Anisotropy reversal of the upper critical field at low temperatures and spin-locked superconductivity in K2Cr3As3			National High Magnetic Field Laboratory, Los Alamos National Laboratory, MS-E536, Los Alamos, New Mexico 87545, USA	Phys.Rev.B, 91(2015)220505	F. F. Balakirev,T. Kong,M. Jaime,R. D. McDonald,C. H. Mielke,A. Gurevich,P. C. Canfield,S. L. Bud'ko		
156100	PRB092014517	[penet] measured by magnetic force microscope (MFM). [penet varies locally for T < T<wFM> (weak FM) = 2.3 K.	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	2015																										ABC2D2		LuNi2B2C																	borocarbide	K				10			10																																									A	MFM	1900																																																					Ni2B flux method					Spatially resolved penetration depth measurements and vortex manipulation in the ferromagnetic superconductor ErNi2B2C			Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science, 77 Cheongam-Ro, Nam-Gu, Pohang 790-784, Korea	Phys.Rev.B, 92(2015)014517	Dirk Wulferding,Ilkyu Yang,Jinho Yang,Minkyung Lee,Hee Cheul Choi,Sergey L. Bud'ko,Paul C. Canfield,Han Woong Yeom,Jeehoon Kim		
156101	PRB092020505		La(Fe,Mn)As(O,F)	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		27					27																																																																																																					Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156102	PRB092020505	Mn-content =0.025% (x = 0.00025 in Fe1-xMnx)	La(Fe,Mn)As(O,F)	La1Fe0.9997Mn0.00025As1F0.11O0.89	La	1	Fe	0.9997	Mn	0.00025	As	1	F	0.11											O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		22.8					22.8	MTC156102																																																																																																				Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156103	PRB092020505		La(Fe,Mn)As(O,F)	La1Fe0.999Mn0.001As1F0.11O0.89	La	1	Fe	0.999	Mn	0.001	As	1	F	0.11											O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		9.84					9.84																																																																																																					Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156104	PRB092020505		(La,Y)(Fe,Mn)As(O,F)	La0.8Y0.2Fe1As1F0.11O0.89	La	0.8	Y	0.2	Fe	1	As	1	F	0.11											O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		30.3					30.3																																																																																																					Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156105	PRB092020505		(La,Y)(Fe,Mn)As(O,F)	La0.8Y0.2Fe0.997Mn0.003As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.997	Mn	0.003	As	1	F	0.11									O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		29.3					29.3																																																																																																					Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156106	PRB092020505		(La,Y)(Fe,Mn)As(O,F)	La0.8Y0.2Fe0.995Mn0.005As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		25.7					25.7	MTC156106																																																																																																				Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156107	PRB092020505		(La,Y)(Fe,Mn)As(O,F)	La0.8Y0.2Fe0.99Mn0.01As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.99	Mn	0.01	As	1	F	0.11									O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		25.3					25.3																																																																																																					Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156108	PRB092020505		Sm(Fe,Mn)As(O,F)	Sm1Fe0.965Mn0.035As1F0.11O0.89	Sm	1	Fe	0.965	Mn	0.035	As	1	F	0.11											O	0.89		1	2015																										ABCD		oxypnictide																	Fe-1111	K		31.3					31.3	MTC156108																																																																																																				Enhancement of low-frequency fluctuations and superconductivity breakdown in Mn-doped La1-yYyFeAsO0.89F0.11 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 92(2015)020505	F. Hammerath,M. Moroni,L. Bossoni,S. Sanna,R. Kappenberger,S. Wurmehl,A. U. B. Wolter,M. A. Afrassa,Y. Kobayashi,M. Sato,B. Buchner,P. Carretta		
156109	PRB092020506	Sr0.1Bi2Se3(90.97%),BiSe(7.05%), SrBi2Se4(1.98%). RRR = 1.95. Anisotropy (penet) = 1.5. GL(kappa)//ab = 119.2. TP(50K) = -19.4 uV/K. carrier n(200K) = 1.24E+19/cm3	SrxBi2Se3	Sr0.1Bi2Se3	Sr	0.1	Bi	2	Se	3																		3	2015																													R3[-]m		A	4.14		28.65											topological SC	K	2.8		2.94			0.16	2.87											Oe	M-H curve		3.9						T	RES(on), GL-fitting		2.1	1.4										MHC156109		A	from Hc2		153	102	um			1.22																						uV/K	-34.1				uOhm.cm								3.68						cm3/C						MRH156109			Bi(5N),Se(5N),Sr(2N)		mixture - melt(850C.8d, in sealed quartz tube) - cool to 650C (10 C/h) - Q to ice water					Superconductivity by Sr intercalation in the layered topological insulator Bi2Se3			School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, India	Phys.Rev.B, 92(2015)020506	Shruti, V. K. Maurya,P. Neha,P. Srivastava,S. Patnaik		
156110	MAT1502.01105		Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2015																															A	4.1328		28.573											topological SC	K					1.9																																																																																																		SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with topological surface state in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	cond-mat/1502.01105	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156111	MAT1502.01105	nominal compositions = Sr0.17Bi2Se3. DB values by EDX. carrier n = 2.02 (300K) and = 2.65 (10K) E+19 /cm3.  SC-volume fraction = 88%(bulk SC)	SrxBi2Se3	Sr0.062Bi2Se3	Sr	0.062	Bi	2	Se	3																		3	2015																															A	4.1369		28.598											topological SC	K	2.39		2.57				2.48	MTC156111									88																																																													mOh..cm								0.24						cm3/C	0.31					MRH156111	n/cm3	20200000000000000000			SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with topological surface state in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	cond-mat/1502.01105	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156112	MAT1502.01105	nominal compositions = Sr0.19Bi2Se3. DB values by EDX. SC-volume fraction = 91.5 %(bulk SC)	SrxBi2Se3	Sr0.065Bi2Se3	Sr	0.065	Bi	2	Se	3																		3	2015																																													topological SC	K			2.6				2.6										91.5																																																																																						SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with topological surface state in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	cond-mat/1502.01105	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156113	MAT1502.01105	not SC for x =< 0.25 in Bi2-xSrxSe3. x values(EDX) are nearly equal to nominal ones.	Bi2-xSrxSe3	Bi1.85Sr0.15Se3	Bi	1.85	Sr	0.15	Se	3																		3	2015																															A	4.146		28.559											topological SC	K					1.9																																																																																																		SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with topological surface state in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People's Republic of China	cond-mat/1502.01105	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156114	PRB092024511	not SC. R(T) = R0 + A*T^n , n= 1.6	UPt3B	U1Pt3B1	U	1	Pt	3	B	1																		1	2015																										ABC3		CePt3B	P4mm		A	3.8906		5.2241												K					0.34																																																										mJ/mol.K2	221	SP																																						arc-melting(Ar) - sealed in quartz tube - ANN (800c,500h), (600C,1000h), (400C,2500h)					Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th,U}Pt3B			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 92(2015)024511	E. Bauer,E. Royanian,H. Michor,O. Sologub,E.-W. Scheidt,A. P. Gonc,alves,J. Bursik,W. Wolf,D. Reith,C. Blaas-Schenner,R. Moser,R. Podloucky,P. Rogl		
156115	PRB092024511	Thermodynamic Hc(0) = 6 mT. (dC/Tc) = 5 mJ/mol.K2. GL(kappa) = 43. [penet](London) = 1.3 microm-m.	ThPt3B	Th1Pt3B1	Th	1	Pt	3	B	1																		1	2015																										ABC3		CePt3B	Pm3[-]m		A	4.383														K		0.75					0.75																				T	RES(0.5Rn), WHH	0.42							T/K	RES(0.5Rn)	0.83			MHC156115		A	from Hc2	280			um		1.3										MSP156115			mJ/mol.K2	6.5	SP	220	SP											uOhm.cm							196																		arc-melting(Ar) - sealed in quartz tube - ANN (800c,500h), (600C,1000h), (400C,2500h)					Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th,U}Pt3B			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 92(2015)024511	E. Bauer,E. Royanian,H. Michor,O. Sologub,E.-W. Scheidt,A. P. Gonc,alves,J. Bursik,W. Wolf,D. Reith,C. Blaas-Schenner,R. Moser,R. Podloucky,P. Rogl		
156116	PRB092054507	No trace of alpha-Bi2Pd. gap measured by STM. Samples show a single-gap multiband SC.	beta-Bi2Pd	Bi2Pd1	Bi	2	Pd	1																				3	2015																										AB2			I4/mmm		A	3.36		12.97												K		5.07				0.03	5.07	MGAP156116																			T	RES(on)						0.45	2						MHC156116		A			230							meV	0.76	3.49	11							mJ/mol.K2	13	SP													uOhm.cm								18															Bi(4N),Pd(3N5)		mixture - quartz ampoule - sealed (140 mbar He) - heat to 900 C in 3h - hold(24h) - cool to 490 c in 96h - cool to 395 C in 200h - Q to cold water					Magnetic field dependence of the density of states in the multiband superconductor betha-Bi2Pd	8	Bi2Pd, vortex, STM, multiband, single gap	Laboratorio de Bajas Temperaturas y Altos Campos Magneticos, Departamento de Fisico de la Materia Condensada, Instituto Nicolas Cabrera and Condensed Matter Physics Center (IFIMAC), Universidad Autonoma de Madrid, E-28049 Madrid, Spain	Physical Review B, 92(2015)054507	E. Herrera,I. Guillamon,J. A. Galvis,A. Correa,A. Fente,R. F. Luccas,F. J. Mompean,M. Garcia-Hernandez,S. Viera,J.P. Brison,H. Suderow	Bi2Pd	betha-Bi2Pd is a single-gap multiband superconductor, measured by STM.
156117	PRB092064515	Anisotropy facter = (R<C>/R<ab>) = 2500 at 50 K. R(T) anomaly at 120 K. Hall coeff. RH = -9.66E-3 cm3/C at 50 K.	(Li0.84Fe0.16)OHFe0.98Se	Li0.84H1Fe1.14Se1O1	Li	0.84	H	1	Fe	1.14	Se	1													O	1		3	2015					myu-B/Fe	4.2	-6.6																			ABCDE			P4/nmm		A	3.7827		9.3184											Fe-11111	K				42		1	42																				T	RES(mid), WHH		313	79										MHC156117																																																			cm3/C					9	MRH156117					Crystals synthesized by hydrothermal ion-exchange method using K0.8Fe1.6Se2 crystal as a matrix.					(Li0.84Fe0.16)OHFe0.98Se superconductor: Ion-exchange synthesis of large single-crystal and highly two-dimensional electron properties			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys.Rev.B, 92(2015)064515	Xiaoli Dong,Kui Jin,Dongna Yuan,Huaxue Zhou,Jie Yuan,Yulong Huang,Wei Hua,Junliang Sun,Ping Zheng,Wei Hu,Yiyuan Mao,Mingwei Ma,Guangming Zhang,Fang Zhou,Zhongxian Zhao		
156118	PRB092064515	not SC.	K0.8Fe1.6Se2	K0.8Fe1.6Se2	K	0.8	Fe	1.6	Se	2																		3	2015								538																		A2B4C5			I4/m		A	8.7248		14.1339											K:Fe:Se = 2:4:5	K					4																																																																																																		Crystals synthesized by hydrothermal ion-exchange method using K0.8Fe1.6Se2 crystal as a matrix.					(Li0.84Fe0.16)OHFe0.98Se superconductor: Ion-exchange synthesis of large single-crystal and highly two-dimensional electron properties			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys.Rev.B, 92(2015)064515	Xiaoli Dong,Kui Jin,Dongna Yuan,Huaxue Zhou,Jie Yuan,Yulong Huang,Wei Hua,Junliang Sun,Ping Zheng,Wei Hu,Yiyuan Mao,Mingwei Ma,Guangming Zhang,Fang Zhou,Zhongxian Zhao		
156119	PRB092134517	Sr3M-intercalated, M=(NH2)y(NH3)1-y, 0.2=<y=<0.6. Hc2 measured by resonant frequency (LCR) for pulsed magnetic field.	Sr0.3(NH2)y(NH3)1-yFe2Se2	Sr0.3M1Fe2Se2	Sr	0.3	M	1	Fe	2	Se	2																3	2015																																														K		36.3		36			36.3																				T	LCR, Two band Gurevich model	33												MHC156119							A	muon-SR	2920																																																			FeSe powder,Sr		mixture - glass Schlenk tube - cool to (-78 C) with an isopropanol/dry ice bath - Liq.ammonia,					Robustness of superconductivity to structural disorder in Sr0.3(NH2)y(NH3)1-yFe2Se2			Oxford University Department of Physics, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 92(2015)134517	F. R. Foronda,S. Ghannadzadeh,S. J. Sedlmaier,J. D. Wright,K. Burns,S. J. Cassidy,P. A. Goddard,T. Lancaster,S. J. Clarke,J. Blundell		
156120	PRB092161114	Heavy Fermion SC. Having two AFM temp. Tn1=2.2K, Tn2=2.0K corresponding  to two Ce sites. (dC/gamma*Tc) = 0.7. SP(beta) = 5.58 mJ/mol.K4.	Ce3PtIn11	Ce3Pt1In11	Ce	3	Pt	1	In	11																		3	2015					myu-B/Ce	2.6	-64	2																		AB3C11			P4/mmm		A	4.6874		16.8422											Ce3PdIn11 type	K		0.32					0.32	MPH156120																			T	R(mid), (1-t2)-dependency	1.4							T/K	RES(mid)	7.24			MHC156120																						mJ/mol.K2	520	SP	174	SP											uOhm.cm												40	60												Flux method using excess In.					Magnetism, superconductivity, and quantum criticality in the multisite cerium heavy-fermion compound Ce3PtIn11			Charles University in Prague, Faculty of Mathematics and Physics, Ke Karlovu 5, 121 16 Prague 2, Czech Republic	Phys.Rev.B, 92(2015)161114	J. Prokleska,M. Kratochvilova,K. Uhlirova,V.Sechovsky,J.Custers		
156121	PRB092174509	Hc2(WHH) = 31.0 T(//ab),  20.0 T(//c), Maki-parameter:  (alpha) = 0.33 , (s-o) = 0 , Anisotropy (Hc2) =  1.08 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.935Ni0.065As2	Ba	1	Fe	1.935	Ni	0.065	As	2																3	2015																										AB2C2		ThCr2Si2																		K			11.3				11.3																				T	RES(on), Maki-theory		29.6	27.3					T/K	RES(on)		3.98		MHC156121																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156122	PRB092174509	Hc2(WHH) = 40.7 T(//ab),  25.3 T(//c), Maki-parameter:  (alpha) = 0.38 , (s-o) = 0 , Anisotropy (Hc2) =  1.04 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.925Ni0.075As2	Ba	1	Fe	1.925	Ni	0.075	As	2																3	2015																										AB2C2		ThCr2Si2																		K			13.7				13.7																				T	RES(on), Maki-theory		38.3	36.7					T/K	RES(on)		4.31		MHC156122																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156123	PRB092174509	Hc2(WHH) = 57.6 T(//ab),  33.9 T(//c), Maki-parameter:  (alpha) = 0.70 , (s-o) = 0.05 , Anisotropy (Hc2) =  1.07 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.915Ni0.085As2	Ba	1	Fe	1.915	Ni	0.085	As	2																3	2015																										AB2C2		ThCr2Si2																		K			18.2				18.2																				T	RES(on), Maki-theory		46.6	43.5					T/K	RES(on)		4.59		MHC156123																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156124	PRB092174509	Hc2(WHH) = 83.2 T(//ab),  37.0 T(//c), Maki-parameter:  (alpha) = 1.69 , (s-o) = 0.12 , Anisotropy (Hc2) =  1.06 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.908Ni0.092As2	Ba	1	Fe	1.908	Ni	0.092	As	2																3	2015																										AB2C2		ThCr2Si2																		K			19.3				19.3																				T	RES(on), Maki-theory		47.6	44.9					T/K	RES(on)		6.25		MHC156124																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156125	PRB092174509	Hc2(WHH) = 98.9 T(//ab),  40.9 T(//c), Maki-parameter:  (alpha) = 2.58 , (s-o) = 0.18 , Anisotropy (Hc2) =  1.05 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.904Ni0.096As2	Ba	1	Fe	1.904	Ni	0.096	As	2																3	2015																										AB2C2		ThCr2Si2																		K			19.9				19.9																				T	RES(on), Maki-theory		48	45.7					T/K	RES(on)		7.2		MHC156125																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156126	PRB092174509	Hc2(WHH) = 107.7 T(//ab),  44.4 T(//c), Maki-parameter:  (alpha) = 2.77 , (s-o) = 0.28 , Anisotropy (Hc2) =  1.02 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.9Ni0.1As2	Ba	1	Fe	1.9	Ni	0.1	As	2																3	2015																										AB2C2		ThCr2Si2																		K			20.3				20.3																				T	RES(on), Maki-theory		48.2	47.5					T/K	RES(on)		7.69		MHC156126																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156127	PRB092174509	Hc2(WHH) = 117.9 T(//ab),  45.2 T(//c), Maki-parameter:  (alpha) = 3.09 , (s-o) = 0.33 , Anisotropy (Hc2) =  1.05 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.892Ni0.108As2	Ba	1	Fe	1.892	Ni	0.108	As	2																3	2015																										AB2C2		ThCr2Si2																		K			20.3				20.3																				T	RES(on), Maki-theory		50	47.6					T/K	RES(on)		8.42		MHC156127																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156128	PRB092174509	Hc2(WHH) = 99.7 T(//ab),  38.2 T(//c), Maki-parameter:  (alpha) = 2.62 , (s-o) = 0.40 , Anisotropy (Hc2) =  1.16 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.88Ni0.12As2	Ba	1	Fe	1.88	Ni	0.12	As	2																3	2015																										AB2C2		ThCr2Si2																		K			18.6				18.6																				T	RES(on), Maki-theory		49.4	42.6					T/K	RES(on)		7.77		MHC156128																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156129	PRB092174509	Hc2(WHH) = 52.7 T(//ab),  22.7 T(//c), Maki-parameter:  (alpha) = 1.20 , (s-o) = 0.06 , Anisotropy (Hc2) =  1.37 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.85Ni0.15As2	Ba	1	Fe	1.85	Ni	0.15	As	2																3	2015																										AB2C2		ThCr2Si2																		K			14.5				14.5																				T	RES(on), Maki-theory		35.1	25.6					T/K	RES(on)		5.2		MHC156129																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156130	PRB092174509	Hc2(WHH) = 32.8 T(//ab),  15.3 T(//c), Maki-parameter:  (alpha) = 0.68 , (s-o) = 0.04 , Anisotropy (Hc2) =  1.55 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.82Ni0.18As2	Ba	1	Fe	1.82	Ni	0.18	As	2																3	2015																										AB2C2		ThCr2Si2																		K			10.9				10.9																				T	RES(on), Maki-theory		27.6	17.8					T/K	RES(on)		4.36		MHC156130																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156131	PRB092174509	Hc2(WHH) = 19.2 T(//ab),  6.5 T(//c), Maki-parameter:  (alpha) = 0 , (s-o) = 0 , Anisotropy (Hc2) =  2.09 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.8Ni0.2As2	Ba	1	Fe	1.8	Ni	0.2	As	2																3	2015																										AB2C2		ThCr2Si2																		K			6.4				6.4																				T	RES(on), Maki-theory		19.3	9.2					T/K	RES(on)		4.35		MHC156131																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156132	PRB092174509	Hc2(WHH) = 10.0 T(//ab),  2.6 T(//c), Maki-parameter:  (alpha) = 0 , (s-o) = 0 , Anisotropy (Hc2) =  2.43 at 0 K.	Ba(Fe,Ni)2As2	Ba1Fe1.78Ni0.22As2	Ba	1	Fe	1.78	Ni	0.22	As	2																3	2015																										AB2C2		ThCr2Si2																		K			3.4				3.4																				T	RES(on), Maki-theory		10.1	4.2					T/K	RES(on)		4.25		MHC156132																																																														Self flux method					Electron doping dependence of the anisotropic superconductivity in BaFe2-xNixAs2			Hochfeld-Magnetlabor Dresden (HLD-EMFL), Helmholtz-Zentrum Dresden-Rossendorf, D-01314 Dresden, Germany	Phys.Rev.B, 92(2015)174509	Zhaosheng Wang,Tao Xie,E. Kampert,T. Forster,Xingye Lu,Rui Zhang,Dongliang Gong,Shiliang Li,T. Herrmannsdorfer,J. Wosnitza,Huiqian Luo		
156133	PRB092180508	Tn(AFM) measured by <75>As-NMR, NQR.	(Ca,La)FeAs2	Ca0.85La0.15Fe1As2	Ca	0.85	La	0.15	Fe	1	As	2																3	2015								62																		ABC2		Fe-112																		K				35			35																																																																																																See J.Phys.Soc.Jpn,  83(2014)025001					Doping-enhanced antiferromagnetism in Ca1-xLaxFeAs2			Department of Physics, and Research Center of New Functional Materials for Energy Production, Storage and Transport, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 92(2015)180508	Shinji Kawasaki,Tomosuke Mabuchi,Satoki Maeda,Tomoki Adachi,Tasuku Mizukami,Kazutaka Kudo,Minoru Nohara,Guo-qing Zheng		
156134	PRB092180508	Tn(AFM) measured by <75>As-NMR, NQR.	(Ca,La)FeAs2	Ca0.81La0.19Fe1As2	Ca	0.81	La	0.19	Fe	1	As	2																3	2015								63																		ABC2		Fe-112																		K				34			34																																																																																																See J.Phys.Soc.Jpn,  83(2014)025001					Doping-enhanced antiferromagnetism in Ca1-xLaxFeAs2			Department of Physics, and Research Center of New Functional Materials for Energy Production, Storage and Transport, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 92(2015)180508	Shinji Kawasaki,Tomosuke Mabuchi,Satoki Maeda,Tomoki Adachi,Tasuku Mizukami,Kazutaka Kudo,Minoru Nohara,Guo-qing Zheng		
156135	PRB092180508	not SC.  Tn(AFM) measured by <75>As-NMR, NQR.	(Ca,La)FeAs2	Ca0.76La0.24Fe1As2	Ca	0.76	La	0.24	Fe	1	As	2																3	2015								70																		ABC2		Fe-112																		K					4																																																																																																		See J.Phys.Soc.Jpn,  83(2014)025001					Doping-enhanced antiferromagnetism in Ca1-xLaxFeAs2			Department of Physics, and Research Center of New Functional Materials for Energy Production, Storage and Transport, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 92(2015)180508	Shinji Kawasaki,Tomosuke Mabuchi,Satoki Maeda,Tomoki Adachi,Tasuku Mizukami,Kazutaka Kudo,Minoru Nohara,Guo-qing Zheng		
156136	PRB092214508	Compositions = Ba6.00Nb9.57O28.05 by EPMA. SP (beta) = 0.37 mJ/molK4. (dC/gamma*Tc) = 1.31 Thermal diffusivity (300K) = 0.6 mm2/g.	Ba6Nb10O30	Ba6Nb10O30	Ba	6	Nb	10																	O	30		1	2015																										A6B10C30			P4/mbm		A	12.6173		3.9835												K			1.65				1.65										15																																				meV	0.382	5.38	14				MSP156136			mJ/mol.K2	17.09	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156137	PRB092214508	Compositions = Ba4.99Sr1.01Nb9.91O29.16.  SP (beta) = 1.15 mJ/molK4. (dC/gamma*Tc) = 1.56	(Ba,Sr)6Nb10O30	Ba5Sr1Nb10O30	Ba	5	Sr	1	Nb	10															O	30		1	2015																										A6B10C30			P4/mbm		A	12.5848		3.9726												K			0.96				0.96																																														meV	0.236	5.7	14							mJ/mol.K2	15.75	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156138	PRB092214508	Compositions = Ba4.03Sr1.97Nb10.01O29.26.  SP (beta) = 1.04 mJ/molK4. (dC/gamma*Tc) = 1.60	(Ba,Sr)6Nb10O30	Ba4Sr2Nb10O30	Ba	4	Sr	2	Nb	10															O	30		1	2015																										A6B10C30			P4/mbm		A	12.5551		3.9576												K			0.98				0.98										30																																				meV	0.227	5.38	14							mJ/mol.K2	16.82	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156139	PRB092214508	Compositions = Ba3.12Sr2.88Nb10.11O29.79.	(Ba,Sr)6Nb10O30	Ba3Sr3Nb10O30	Ba	3	Sr	3	Nb	10															O	30		1	2015																										A6B10C30			P4/mbm		A	12.5168		3.9436												K					0.4																																																										mJ/mol.K2	8.13	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156140	PRB092214508	Compositions = Ba2.10Sr3.90Nb10.22O29.69	(Ba,Sr)6Nb10O30	Ba2Sr4Nb10O30	Ba	2	Sr	4	Nb	10															O	30		1	2015																										A6B10C30			P4/mbm		A	12.4652		3.9301												K					0.4																																																										mJ/mol.K2	1.7	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156141	PRB092214508	Compositions = Ba1.05Sr4.95Nb10.41O31.37	(Ba,Sr)6Nb10O30	Ba1Sr5Nb10O30	Ba	1	Sr	5	Nb	10															O	30		1	2015																										A6B10C30			P4/mbm		A	12.4149		3.9157												K					0.4																																																										mJ/mol.K2	0.82	SP																																				BaCO3(4N),SrCO3(4N),Nb2O5(4N8)		mixture - heat(1000C,10h, in flowing H2/Ar) - two intermwdiate regrindings - SIN(1360C,10-12h, in flowing H2/Ar)					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156142	PRB092214508	Compositions = Ba6.00Nb9.26Mg0.41O28.67by EPMA	Ba6Nb10O30	Ba6Nb10O30	Ba	6	Nb	10																	O	30		3	2015																										A6B10C30			P4/mbm		A	12.5842		3.9995											a = 12.5672, c = 3.9980 at 100K.	K				1.6			1.6																																																																																														BaCO3,Nb2O5		addition of 1 wt% MgO - in Mo crucuble - heat(1400C) - cool to 1200C(10C/h) - FC to RT					Superconductivity and crystal structural origins of the metal-insulator transition in Ba6-xSrxNb10O30 tetragonal tungsten bronzes			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev.B, 92(2015)214508	Taras Kolodiazhnyi,Hiroya Sakurai,Masaaki Isobe,Yoshitaka Matsushita,Scott Forbes,Yurij Mozharivskyj,Timothy J. S. Munsie,Graeme M. Luke,Mary Gurak,David R. Clarke		
156143	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 138 K (T-to-O).	(Ba,Na)Fe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2016																										AB2C2		ThCr2Si2																		K					2																																																																																																		self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156144	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 134 K (T-to-O).	(Ba,Na)Fe2As2	Ba0.907Na0.093Fe2As2	Ba	0.907	Na	0.093	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K					2																																																																																																		self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156145	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 111 K (T-to-O).	(Ba,Na)Fe2As2	Ba0.818Na0.182Fe2As2	Ba	0.818	Na	0.182	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		6.4					6.4																																																																																																self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156146	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 100 K (T-to-O)., 21 K (O-to-T)	(Ba,Na)Fe2As2	Ba0.779Na0.221Fe2As2	Ba	0.779	Na	0.221	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		8					8	MPH156146																																																																																															self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156147	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 58 K (T-to-O),  49.4 K (O-to-O'), 36.2 K (O'-to- T).	(Ba,Na)Fe2As2	Ba0.698Na0.302Fe2As2	Ba	0.698	Na	0.302	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		18					18																																																																																																self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156148	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 49.3 K (T-to-O').	(Ba,Na)Fe2As2	Ba0.68Na0.32Fe2As2	Ba	0.68	Na	0.32	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		23.8					23.8																																																																																																self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156149	PRB093014514	Phase transitions measured  by thermal expansion and SP.	(Ba,Na)Fe2As2	Ba0.64Na0.36Fe2As2	Ba	0.64	Na	0.36	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		31					31																																																																																																self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156150	PRB093014514	Phase transitions measured  by thermal expansion and SP.	(Ba,Na)Fe2As2	Ba0.6Na0.4Fe2As2	Ba	0.6	Na	0.4	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		34					34																																																																																																self-flux method, (Ba1-xNax):FeAs = 1:4 or 1:5. melt(1150-1170 C) - cool to (940 -  1020 C) at 0.5 C/h.					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156151	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 118 K (T-to-O).	(Ba,K)Fe2As2	Ba0.84K0.16Fe2As2	Ba	0.84	K	0.16	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		5.54					5.54																																																																																																					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156152	PRB093014514	Phase transitions measured  by thermal expansion and SP. T<STR> = 54 K (T-to-O), 34.6 K (ortho-to-tetra)	(Ba,K)Fe2As2	Ba0.737K0.263Fe2As2	Ba	0.737	K	0.263	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		24					24	MPH156152																																																																																																				Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156153	PRB093014514	Phase transitions measured  by thermal expansion and SP.	(Ba,K)Fe2As2	Ba0.65K0.35Fe2As2	Ba	0.65	K	0.35	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		38					38																																																																																																					Complex phase diagram of Ba1-xNaxFe2As2: A multitude of phases striving for the electronic entropy			Institut fur Festkorperphysik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Phys.Rev.B, 93(2016)014514	L. Wang,F. Hardy,A. E. Bohmer,T. Wolf,P. Schweiss,C. Meingast		
156154	PRB093045118	Au2Pb0.95. RRR = 9. Tc(P=1GPa) = 1.1 K.  Structural phase transitions at T1 = 97, T2 = 51, T3 = 40 K from R(T).	Au2Pb	Au2Pb1	Au	2	Pb	1																				3	2016																										AB2		MgCu2(Laves)	Fd3[-]m	227	A	7.9141													unit volume = 495.69 A3	K		1.2					1.2																																																					MSP156154			mJ/mol.K2	1.9	SP	133	SP											uOhm.cm											35.9														Pb flux method. mixture(Au:Pb = 2:3) - sealed in quartz tube - heat to 600C (50 C/h) - hold(24h) - cool to 300 C(3 C/h)					Temperature-pressure phase diagram of cubic Laves phase Au2Pb			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32306, USA	Phys.Rev.B, 93(2016)045118	K. W. Chen,D. Graf,T. Besara,A. Gallagher,N. Kikugawa,L. Balicas,T. Siegrist,A. Shekhter,R. E. Baumbach		
156155	PRB093045118	RRR = 20. No anomaly in R(T). SP-heat (beta) = 1.6 mJ/mol.K4	Au2Bi	Au2Bi1	Au	2	Bi	1																				3	2016																										AB2		MgCu2(Laves)	Fd3[-]m	227																K		1.7					1.7																																																					MSP156155			mJ/mol.K2	2.3	SP	153	SP																																				Pb flux method. mixture(Au:Pb = 2:3) - sealed in quartz tube - heat to 600C (50 C/h) - hold(24h) - cool to 300 C(3 C/h)					Temperature-pressure phase diagram of cubic Laves phase Au2Pb			National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32306, USA	Phys.Rev.B, 93(2016)045118	K. W. Chen,D. Graf,T. Besara,A. Gallagher,N. Kikugawa,L. Balicas,T. Siegrist,A. Shekhter,R. E. Baumbach		
156156	PRB093054508	RRR = 200. Optical conductivity measured. Two isotropic gaps: d1 = 2.9, d2 = 5.5 meV (2d/kTc = 3.7 and 7.1). coexist of clean and dirty-limit SC.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2016																										ABC		PbFCl																		K		18					18																																									A	plasma frequency	2040			meV	5.5	7.1	15																						uOhm.cm							1.45																		self-flux method					Coexistence of clean- and dirty-limit superconductivity in LiFeAs			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 93(2016)054508	Y. M. Dai,H. Miao,L. Y. Xing,X. C. Wang,C. Q. Jin,H. Ding,C. C. Homes		
156157	PRB093054513	(Ca,Pr)Fe2.07As1.948	(Ca,Pr)Fe2As2	Ca0.941Pr0.059Fe2As2	Ca	0.941	Pr	0.059	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																	Fe-122	K			28.9				28.9	MTC156157									0.2																																																																																				Fe(5N),As(6N),Ca(4N),Pr(3N),La(3N)		self-flux method. mixture((Ca+R):FeAs = 1:4) - alumina crucible in silica tube - heat(1200C,8h) - cool to 980 C (2 C/h)					Evidence for defect-induced superconductivity up to 49 K in (Ca1-x Rx)Fe2As2			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 93(2016)054513	L. Z. Deng,B. Lv,K. Zhao,F. Y. Wei,Y. Y. Xue,Z. Wu,C. W. Chu		
156158	PRB093054513	(Ca,Pr)Fe2.068As1.948. Two-step SC-transition, lower Tc = 23.9 K.	(Ca,Pr)Fe2As2	Ca0.875Pr0.125Fe2As2	Ca	0.875	Pr	0.125	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																	Fe-122	K			49				49										3																																																																																				Fe(5N),As(6N),Ca(4N),Pr(3N),La(3N)		self-flux method. mixture((Ca+R):FeAs = 1:4) - alumina crucible in silica tube - heat(1200C,8h) - cool to 980 C (2 C/h)					Evidence for defect-induced superconductivity up to 49 K in (Ca1-x Rx)Fe2As2			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 93(2016)054513	L. Z. Deng,B. Lv,K. Zhao,F. Y. Wei,Y. Y. Xue,Z. Wu,C. W. Chu		
156159	PRB093054513	(Ca,La)Fe2.00As1.970. Two-step SC-transition, lower Tc = 20.0 K.	(Ca,La)Fe2As2	Ca0.891La0.109Fe2As2	Ca	0.891	La	0.109	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																	Fe-122	K			45.4				45.4	MTC156159									18.6																																																																																				Fe(5N),As(6N),Ca(4N),Pr(3N),La(3N)		self-flux method. mixture((Ca+R):FeAs = 1:4) - alumina crucible in silica tube - heat(1200C,8h) - cool to 980 C (2 C/h)					Evidence for defect-induced superconductivity up to 49 K in (Ca1-x Rx)Fe2As2			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 93(2016)054513	L. Z. Deng,B. Lv,K. Zhao,F. Y. Wei,Y. Y. Xue,Z. Wu,C. W. Chu		
156160	PRB093054513	(Ca,La)Fe2.075As1.970,  Two-step SC-transition, lower Tc = 26.3 K.  SP-heat (beta) = 0.66 mJ/mol.K4	(Ca,La)Fe2As2	Ca0.857La0.143Fe2As2	Ca	0.857	La	0.143	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																	Fe-122	K			44				44										20																																														mJ/mol.K2	31	SP																																				Fe(5N),As(6N),Ca(4N),Pr(3N),La(3N)		self-flux method. mixture((Ca+R):FeAs = 1:4) - alumina crucible in silica tube - heat(1200C,8h) - cool to 980 C (2 C/h)					Evidence for defect-induced superconductivity up to 49 K in (Ca1-x Rx)Fe2As2			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 93(2016)054513	L. Z. Deng,B. Lv,K. Zhao,F. Y. Wei,Y. Y. Xue,Z. Wu,C. W. Chu		
156161	PRB093054520	RRR = 107. Hc2(0)=0.87T(//ab), = 0.24T(//c) for GL-approx. Hc2(0) = 0.53 T(//ab), = 0.17 T(//c) for WHH-approx. using (dHc2/dT).  (dC/gamma*Tc) = 1.71.	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2016																										ABC2			P6[-]m2																	K			3.8				3.8											Oe	M-H curve. (1-t^2) approx.	90							T	R(mid). T-sweep					1.25	0.32	0.2	T/K	R(mid)		0.19	0.061	MHC156161		A	from Hc2	162																		mJ/mol.K2	6.01	SP	161	SP											uOhm.cm							3.8																		CVD method. source zone(900C,PbTaSe2 powder), sink zone(800C) in three zone furnace for 1 week using PbCl2 agent.					Superconducting properties in single crystals of the topological nodal semimetal PbTaSe2			International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China	Phys.Rev.B, 93(2016)054520	Cheng-Long Zhang,Zhujun Yuan,Guang Bian,Su-Yang Xu,Xiao Zhang,M. Zahid Hasan,Shuang Jia		
156162	PRB093060506	RRR = 220. [penet] estimated using Hc1(0) = 120 A and [cohere] = 162 A	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2016																										ABC2			P6[-]m2																	K			3.9				3.9											Oe	M-H curve. (1-t^2) approx.		120																				MHC156162		A	from Hc2	162			A	from Hc1, cohere,	2040																												uOhm.cm							0.14																		CVD method					Nodeless superconductivity in noncentrosymmetric PbTaSe2 single crystals			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 93(2016)060506	G. M. Pang,M. Smidman,L. X. Zhao,Y. F. Wang,Z. F. Weng,L. Q. Che,Y. Chen,X. Lu,G. F. Chen,H. Q. Yuan		
156163	PRB093064502	nodal d-wave SC. [resn] = R(0), R(T) = R(0) + A*T for T < 4 K. (k0/T) = 1.22 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	(Ce,Yb)CoIn5	Ce0.987Yb0.013Co1In5	Ce	0.987	Yb	0.013	Co	1	In	5																3	2016																										ABC5		HoCoGa5																		K		2.13					2.13																				T	R(mid), extrapolation		5.4											MHC156163																											mW/K.cm										uOhm.cm								7.9																	In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156164	PRB093064502	nodal d-wave SC. [resn] = R(0), R(T) = R(0) + A*T for T < 4 K. (k0/T) = 1.19 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	(Ce,Yb)CoIn5	Ce0.916Yb0.084Co1In5	Ce	0.916	Yb	0.084	Co	1	In	5																3	2016																										ABC5		HoCoGa5																		K		1.84					1.84																				T	R(mid), extrapolation		5.2											MHC156163																											mW/K.cm										uOhm.cm								11.2																	In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156165	PRB093064502	nodal d-wave SC. [resn] = R(0), R(T) = R(0) + A*T for T < 4 K. (k0/T) = 1.08 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	(Ce,Yb)CoIn5	Ce0.837Yb0.163Co1In5	Ce	0.837	Yb	0.163	Co	1	In	5																3	2016																										ABC5		HoCoGa5																		K		1.4					1.4																				T	R(mid), extrapolation		5.1											MHC156163																											mW/K.cm										uOhm.cm								20.2																	In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156166	PRB093064502	nodal d-wave SC. (k0/T) = 1.03 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	CeCo(In,Cd)5	Ce1Co1In4.98Cd0.02	Ce	1	Co	1	In	4.98	Cd	0.02																3	2016																										ABC5		HoCoGa5																		K		2.14					2.14																																																													mW/K.cm																																			In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156167	PRB093064502	nodal d-wave SC. (k0/T) = 0.90 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	CeCo(In,Cd)5	Ce1Co1In4.96Cd0.04	Ce	1	Co	1	In	4.96	Cd	0.04																3	2016																										ABC5		HoCoGa5																		K		2.05					2.05																																																													mW/K.cm																																			In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156168	PRB093064502	nodal d-wave SC. (k0/T) = 0.93 mW/K2.cm ,  (k/T) = (k0/T) + A*T for T < 0.5 K.	CeCo(In,Cd)5	Ce1Co1In4.945Cd0.055	Ce	1	Co	1	In	4.945	Cd	0.055																3	2016																										ABC5		HoCoGa5																		K		1.92					1.92																																																													mW/K.cm																																			In-self flux method					Universal heat conduction in Ce1-xYbxCoIn5: Evidence for robust nodal d-wave superconducting gap			State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 93(2016)064502	Y. Xu,J. K. Dong,I. K. Lum,J. Zhang,X. C. Hong,L. P. He,K. F. Wang,Y. C. Ma,C. Petrovic,M. B. Maple,L. Shu,S. Y. Li		
156170	PRB093064507	Compositions: Mo5P1.07B1.93.	Mo5P0.9B2.1	Mo5P0.9B2.1	Mo	5	P	0.9	B	2.1																		1	2016																										AB2C5			I4/mcm		A	5.9726		11.074												K	8.7			8.9			8.9																																		MHC156172																																																												Mo(5N),P(5N),B(2N5)		mixture - react(1050C,16-24h) - press into pellet - heat(1100-1150 C,5days)					Superconductivity at 9 K in Mo5PB2 with evidence for multiple gaps			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 93(2016)064507	Michael A. McGuire,David S. Parker		
156171	PRB093064507	Compositions: Mo5P1.07B1.93.  (dC/gamma*Tc) = 1.30	Mo5PB2	Mo5P1B2	Mo	5	P	1	B	2																		1	2016																										AB2C5			I4/mcm		A	5.97303		11.076												K	8.8			8.7			8.7																				T	R(zero),extrapolation	1.7												MHC156172																						mJ/mol.K2	24.56	SP	501	SP																																		Mo(5N),P(5N),B(2N5)		mixture - react(1050C,16-24h) - press into pellet - heat(1100-1150 C,5days)					Superconductivity at 9 K in Mo5PB2 with evidence for multiple gaps			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 93(2016)064507	Michael A. McGuire,David S. Parker		
156172	PRB093064507	Compositions: Mo5P1.12B1.88.  RRR = 11. (dC/gamma*Tc) = 1.39. Hc2(0) = 1.3 T using (dHc2/dT) and WHH theory.	Mo5P1.1PB1.9	Mo5P1.1B1.9	Mo	5	P	1.1	B	1.9																		1	2016									8.97																	AB2C5			I4/mcm		A	5.97633		11.0813												K	9.2			9.2			9.2										120										T	R(zero),extrapolation	1.7							T/K	R(zero)	0.21																									mJ/mol.K2	24.96	SP	494	SP																																		Mo(5N),P(5N),B(2N5)		mixture - react(1050C,16-24h) - press into pellet - heat(1100-1150 C,5days)					Superconductivity at 9 K in Mo5PB2 with evidence for multiple gaps			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 93(2016)064507	Michael A. McGuire,David S. Parker		
156173	PRB093064507	Tc = 5.5 K by SP measurements.	Mo3P	Mo3P1	Mo	3	P	1																				1	2016																										AB3																				K			5.5				5.5																																																					MSP156173																																									Mo,P(red)		mixture - het(850C, in silica) - reground - pellet - hat(1150C)					Superconductivity at 9 K in Mo5PB2 with evidence for multiple gaps			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 93(2016)064507	Michael A. McGuire,David S. Parker		
156174	PRB093085130		ZrB12	Zr1B12	Zr	1	B	12																				3	2016																										AB12		UB12																		K		6.09		5.95			6.09																																																																																					cm3/C	-0.000256				9	MRH156174					grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156175	PRB093085130		(Zr,Lu)B12	Zr0.993Lu0.007B12	Zr	0.993	Lu	0.007	B	12																		3	2016	myu-B/kOe	0.000023																								AB12		UB12																		K		5.97		5.54			5.97																																																																																																grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156176	PRB093085130		(Zr,Lu)B12	Zr0.985Lu0.015B12	Zr	0.985	Lu	0.015	B	12																		3	2016	myu-B/kOe	-0.000044																								AB12		UB12																		K		5.67					5.67	MTC156176																																																																																				cm3/C	-0.00025				9	MRH156176					grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156177	PRB093085130		(Zr,Lu)B12	Zr0.984Lu0.016B12	Zr	0.984	Lu	0.016	B	12																		3	2016	myu-B/kOe	0.000112																								AB12		UB12																		K		5.65					5.65																																																																																																grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156178	PRB093085130		(Zr,Lu)B12	Zr0.935Lu0.065B12	Zr	0.935	Lu	0.065	B	12																		3	2016	myu-B/kOe	0.000114																								AB12		UB12																		K		4.77		4.53			4.77																																																																																																grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156179	PRB093085130		(Zr,Lu)B12	Zr0.926Lu0.074B12	Zr	0.926	Lu	0.074	B	12																		3	2016	myu-B/kOe	0.000033																								AB12		UB12																		K		4.78		4.54			4.78																																																																																																grown by vertical crucible-free inductive floating zone melting in an inert gas atmosphere.					Suppression of superconductivity in LuxZr1-xB12: Evidence of static magnetic moments induced by nonmagnetic impurities			A. M. Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)085130	N. E. Sluchanko,A. N. Azarevich,M. A. Anisimov,A. V. Bogach,S. Yu. Gavrilkin,M. I. Gilmanov,V. V. Glushkov,S. V. Demishev,A. L. Khoroshilov,A. V. Dukhnenko,K. V. Mitsen,N. Yu. Shitsevalova,V. B. Filippov,V. V. Voronov,K. Flachbart		
156180	PRB093094511	P-induced SC. Tc(max) = 8.6 K  at P=14.5 GPa), Phase-I (hexagonal, P<7 GPa), phase-II(intermediate phase)  and phase-III (bcc, complete for P>17 GPa.). (dtc/dP) at P=14.5 GPa	Bi2Te	Bi2Te1	Bi	2	Te	1																				3	2016																										AB2					A	3.747													P=8.8 GPa.. III-phase, bcc	K		8.6			0		8.6	MTC156180		K/GPa	-0.34																T	R(mid), WHH, P=14.5 GPa	1.94				2.12		1.36						MHC156180																																																			cm3/C						MRH156180			Bi(5N),Te(5N)		(Bi:Te = 88:12) - in alumina crucible - sealed in quartz tube(Ar) - melt(420C,2 days) - cool to 318 C, over 4 days)					Superconducting Bi2Te: Pressure-induced universality in the (Bi2)m(Bi2Te3)n series			Materials Science Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 93(2016)094511	Ryan L. Stillwell,Zsolt Jenei,Samuel T. Weir,Yogesh K. Vohra,Jason R. Jeffries		
156182	PRB093104507	R(T) = R0 + A*T^2, R0=1.93 uOhm.cm, A = 4.94 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2016					myu-B/Pr	3.65	7.26																			AB4C12		skutterudite			A	8.8102														K		7.85					7.85																																																								mJ/mol.K2	104.4	SP	238	SP											uOhm.cm	1.93																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156183	PRB093104507	R(T) = R0 + A*T^2, R0=28.3 uOhm.cm, A = 2.44 uOhm.cm/K2 for Tc^2 < T^2 < 250. Energy gap d, (d/Tc) = 1.3 from SP	PrPt4(Ge,Sb)12	Pr1Pt4Ge11.5Sb0.5	Pr	1	Pt	4	Ge	11.5	Sb	0.5																1	2016					myu-B/Pr	3.6	-11																			AB4C12		skutterudite			A	8.6479														K		4.43					4.43																				T	R(mid), WHH	1.16							T/K	R(mid)	0.39			MHC156183																						mJ/mol.K2	46.1	SP	244	SP											uOhm.cm	28.3																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156184	PRB093104507	R(T) = R0 + A*T^2, R0=71.9 uOhm.cm, A = 2.17 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge11Sb1	Pr	1	Pt	4	Ge	11	Sb	1																1	2016					myu-B/Pr	3.48	-17.7																			AB4C12		skutterudite			A	8.6756														K		2.68					2.68	MTC156184																			T	R(mid), WHH	0.61							T/K	R(mid)	0.39			MHC156183																						mJ/mol.K2	33.4	SP	250	SP											uOhm.cm	71.9																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156185	PRB093104507	R(T) = R0 + A*T^2, R0=62.4 uOhm.cm, A = 3.80 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge10.5Sb1.5	Pr	1	Pt	4	Ge	10.5	Sb	1.5																1	2016					myu-B/Pr	3.63	-15.4																			AB4C12		skutterudite			A	8.6849														K		1.71					1.71																				T	R(mid), WHH	0.53							T/K	R(mid)	0.39			MHC156183																																					uOhm.cm	62.4																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156186	PRB093104507	R(T) = R0 + A*T^2, R0=143 uOhm.cm, A = 5.29 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge10Sb2	Pr	1	Pt	4	Ge	10	Sb	2																1	2016					myu-B/Pr	3.32	-3.82																			AB4C12		skutterudite			A	8.7472														K		1.27					1.27																				T	R(mid), WHH	0.35							T/K	R(mid)	0.39			MHC156183																						mJ/mol.K2	10.9	SP	251	SP											uOhm.cm	143																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156187	PRB093104507	R(T) = R0 + A*T^2, R0=177 uOhm.cm, A = 1.82 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge9.5Sb2.5	Pr	1	Pt	4	Ge	9.5	Sb	2.5																1	2016					myu-B/Pr	3.53	-11.7																			AB4C12		skutterudite			A	8.7571														K		0.69					0.69																				T	R(mid), WHH	0.15							T/K	R(mid)	0.39			MHC156183																						mJ/mol.K2	2.4	SP	252	SP											uOhm.cm	177																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156188	PRB093104507		PrPt4(Ge,Sb)12	Pr1Pt4Ge9Sb3	Pr	1	Pt	4	Ge	9	Sb	3																1	2016					myu-B/Pr	3.34	-2.88																			AB4C12		skutterudite			A	8.7918														K			1.4				1.4																																																								mJ/mol.K2	0.594	SP	256	SP																																		PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156189	PRB093104507	Major = PtSb4, minor = PrPtGe7Sb5. R(T) = R0 + A*T^2, R0=114.6 uOhm.cm, A = 10.9 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge8Sb4	Pr	1	Pt	4	Ge	8	Sb	4																2	2016					myu-B/Pr	3.79	-24.9																			AB4C12		skutterudite			A	8.8602														K			1.4				1.4																																																								mJ/mol.K2	46.9	SP	262	SP											uOhm.cm	114.6																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156190	PRB093104507	Major = PtSb4, minor = PrPtGe7Sb5.  R(T) = R0 + A*T^2, R0=216.6 uOhm.cm, A = 30.5 uOhm.cm/K2 for Tc^2 < T^2 < 250.	PrPt4(Ge,Sb)12	Pr1Pt4Ge7Sb5	Pr	1	Pt	4	Ge	7	Sb	5																2	2016																										AB4C12		skutterudite			A	8.9028														K					1.4																																																										mJ/mol.K2	182	SP	267	SP											uOhm.cm	216.6																						PR(3N),Pt(6N),Ge(6N),Sb(2N)		arc-melting - ANN (750C,336h, in sealed quartz ampoule (Ar))					Investigation of superconducting and normal-state properties of the filled-skutterudite system PrPt4Ge12-xSbx			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 93(2016)104507	I. Jeon,K. Huang,D. Yazici,N. Kanchanavatee,B. D. White,P.-C. Ho,S. Jang,N. Pouse,M. B. Maple		
156191	PRB093104516	resistivity, Hall effect, specific heat, Nernst and Seebeck coefficient were measured up to 5.5 GPa.	(Ba,K)Fe2As2	Ba0.85K0.15Fe2As2	Ba	0.85	K	0.15	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																	Fe-122	K	10		14				12	MPH156191																																																																																															self-flux method. (Ba,K,FeAs) in Al2O3 crucible - sealed in steel container - heat (1151 C) - slow cool to 1051 C(0.2-0.5 C/h)					Absence of nematic order in the pressure-induced intermediate phase of the iron-based superconductor Ba0.85K0.15Fe2As2			Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China	Phys.Rev.B, 93(2016)104516	Yan Zheng,Pok Man Tam,Jianqiang Hou,Anna E. Bohmer,Thomas Wolf,Christoph Meingast,Rolf Lortz		
156192	SST028015008	nominal=Bi2O3S2.2. 89%-Bi(O,F)BiS2 phase	BiOBiS2	Bi2.14S2O1	Bi	2.14	S	2																	O	1		1	2015																										ABCD2			I4/nmm		A	3.9744		13.7497											BiS2 layer SC.	K					2																																																																																																Bi2O3(4N),S(2N5),Bi(2N5),BiF3(2N)		mixture - pellet - sealed in quartz tube - heat(430C,2h) - Q to ice water - reground - pellet -ANN(430C,15h) - q to ice water					Superconductivity in BiO1-xFxBiS2 and possible parent phase of Bi4O4S3 superconductor			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People?s Republic of China	Supercond.Sci.Technol., 28(2015)015008	Jifeng Shao,Xiong Yao,Zhongheng Liu,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156193	SST028015008	nominal=Bi2(O0.94F0.06)3S2.2. 90%-Bi(O,F)BiS2 phase	Bi(O,F)BiS2	Bi2.13F0.17S2O0.83	Bi	2.13	F	0.17	S	2															O	0.83		1	2015																										ABCD2			I4/nmm		A	3.97688		13.7114											BiS2 layer SC.	K			3.2				3.2																																																																																														Bi2O3(4N),S(2N5),Bi(2N5),BiF3(2N)		mixture - pellet - sealed in quartz tube - heat(430C,2h) - Q to ice water - reground - pellet -ANN(430C,15h) - q to ice water					Superconductivity in BiO1-xFxBiS2 and possible parent phase of Bi4O4S3 superconductor			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People?s Republic of China	Supercond.Sci.Technol., 28(2015)015008	Jifeng Shao,Xiong Yao,Zhongheng Liu,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156194	SST028015008	nominal=Bi2(O0.9F0.1)3S2.2.  89%-Bi(O,F)BiS2 phase	Bi(O,F)BiS2	Bi2.14F0.27S2O0.73	Bi	2.14	F	0.27	S	2															O	0.73		1	2015																										ABCD2			I4/nmm		A	3.9642		13.6961											BiS2 layer SC.	K			2.7				2.7																																																																																														Bi2O3(4N),S(2N5),Bi(2N5),BiF3(2N)		mixture - pellet - sealed in quartz tube - heat(430C,2h) - Q to ice water - reground - pellet -ANN(430C,15h) - q to ice water					Superconductivity in BiO1-xFxBiS2 and possible parent phase of Bi4O4S3 superconductor			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People?s Republic of China	Supercond.Sci.Technol., 28(2015)015008	Jifeng Shao,Xiong Yao,Zhongheng Liu,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156195	SST028015008	nominal=Bi2(O0.91F0.09)3S2.2. Hc1(0) and Hc2(0) from Hc1(2K) and Hc2(2K) using GL eq.  GL-parameter = 9.6	Bi(O,F)BiS2	Bi2.14F0.24S2O0.76	Bi	2.14	F	0.24	S	2															O	0.76		1	2015																										ABCD2			I4/nmm																BiS2 layer SC.	K			3.5				3.5	MTC156195										mT	M-H, GL approx.	2.22			1.44			2	T	R(on), GL approx.	0.178			0.115			2								A	from Hc2	429			A		4120																																																			Bi2O3(4N),S(2N5),Bi(2N5),BiF3(2N)		mixture - pellet - sealed in quartz tube - heat(430C,2h) - Q to ice water - reground - pellet -ANN(430C,15h) - q to ice water					Superconductivity in BiO1-xFxBiS2 and possible parent phase of Bi4O4S3 superconductor			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, People?s Republic of China	Supercond.Sci.Technol., 28(2015)015008	Jifeng Shao,Xiong Yao,Zhongheng Liu,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
156196	PRB093064504	delta-[penet](T) measured by TDO(tunnel diode oscilator). Energi gap from penetration depth analysis.	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																		1	2016																										ABC		KZnAs																		K		2.45					2.45																																									A	TDO	3390					3																																																					High-resolution magnetic penetration depth and inhomogeneities in locally noncentrosymmetric SrPtAs			Centro de Fisica, Instituto Venezolano de Investigaciones Cientificas, Apartado 20632, Caracas 1020-A, Venezuela	Phys.Rev.B, 93(2016)064504	J. F. Landaeta,S. V. Taylor,I. Bonalde,C. Rojas,Y. Nishikubo,K. Kudo,M. Nohara		
156197	PRB087180503	disk shaped pellet (12 mm dia.). [penet] measured by muon-SR using Brandt's eq.	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																		1	2013																										ABC		KZnAs																		K		2.45					2.45																																									A	muon-SR	339																																																										Evidence for superconductivity with broken time-reversal symmetry in locally noncentrosymmetric SrPtAs			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 87(2013)180503	P. K. Biswas,H. Luetkens,T. Neupert,T. Sturzer,C. Baines,G. Pascua,A. P. Schnyder,M. H. Fischer,J. Goryo,M. R. Lees,H. Maeter,F. Bruckner,H.-H. Klauss,M. Nicklas,P. J. Baker,A. D. Hillier,M. Sigrist,A. Amato,D. Johrendt		
156198	PRB087180503	powder sample.  [penet] measured by muon-SR using Brandt's eq.	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																		1	2013																										ABC		KZnAs																		K		2.45					2.45																																									A	muon-SR	239																																																										Evidence for superconductivity with broken time-reversal symmetry in locally noncentrosymmetric SrPtAs			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 87(2013)180503	P. K. Biswas,H. Luetkens,T. Neupert,T. Sturzer,C. Baines,G. Pascua,A. P. Schnyder,M. H. Fischer,J. Goryo,M. R. Lees,H. Maeter,F. Bruckner,H.-H. Klauss,M. Nicklas,P. J. Baker,A. D. Hillier,M. Sigrist,A. Amato,D. Johrendt		
156200	STAM014035003	8 fu in unit cell. not SC	SrRh2B2	Sr1Rh2B2	Sr	1	Rh	2	B	2																		1	2013																										AB2C2			Fddd		A	5.9826	9.3906	10.6682												K					1.8																																																																																																		solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156201	STAM014035003	8 fu in unit cell. not SC. SP fitting for 2 < T < 10K.	SrIr2B3	Sr1Ir2B2	Sr	1	Ir	2	B	2																		1	2013																										AB2C2			Fddd		A	6.0221	9.3983	10.7123												K					1.8																																																										mJ/mol.K2	3.1	SP	282	SP																																				solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156202	STAM014035003	4 fu in unit cell. SP fitting for 2 < T < 10K. Hc2(0) = 0.385 T using quadratic T-dependency	Sr3Rh8B6	Sr3Rh8B6	Sr	3	Rh	8	B	6																		1	2013																										A3B6C8			Fmmm	69	A	5.5655	9.9042	17.1186												K			3.4				3.4																				T	R(onset), WHH	0.27												MHC156202																						mJ/mol.K2	19	SP	325	SP																																				solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156203	STAM014035003	8 fu in unit cell. not SC	CaIr2B2	Ca1Ir2B2	Ca	1	Ir	2	B	2																		1	2013																										AB2C2			Fddd		A	5.8741	9.2544	10.7267												K					1.8																																																										mJ/mol.K2	3.1	SP	298	SP																																				solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156204	STAM014035003	8 fu in unit cell. not SC	CaRh2B2	Ca1Rh2B2	Ca	1	Rh	2	B	2																		1	2013																										AB2C2			Fddd		A	5.8396	9.2535	10.6071												K					1.8																																																										mJ/mol.K2	3.4	SP	350	SP																																				solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156205	STAM014035003	4 fu in unit cell. Impurity phase = CaRh2(Tc=6.4 K), unidentified phase (Tc=8.7 K). SP fitting for 2 < T < 10K. Hc2(0) = 1.2 T using quadratic T-dependency	Ca3Rh8B6	Ca3Rh8B2	Ca	3	Rh	8	B	2																			2013																										A3B6C8			Fmmm	69	A	5.4872	9.7035	16.9683												K				4			4																				T	R(onset), WHH	1												MHC156205																						mJ/mol.K2	14	SP	325	SP																																				solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Probing the electronic properties of ternary AnM3n-1B2n (n = 1: A = Ca, Sr; M= Rh, Ir and n = 3: A = Ca, Sr;M= Rh) phases: observation of superconductivity			National Institute for Materials Science,1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Sci. Technol. Adv. Mater., 14 (2013) 035003	Hiroyuki Takeya,Mohammed ElMassalami,Luis A Terrazos,Raul E Rapp,Rodrigo B Capaz,Hiroki Fujii,Yoshihiko Takano,Mathias Doerr,Sergey A Granovsky		
156206	PROC2007	4 fu in unit cell. not SC SC data from ref.22 in STAM014035003	Y3Os8B6	Y3Os8B6	Y	3	Os	8	B	6																			2007																										A3B6C8			Fmmm	69																K			5.8				5.8																				T		2																																																																										solid state reaction using BN or Ta crucible. as-prepared samples - ANN(850C,18-20h, in Ta crucible					Superconductivity in the new Y3Os8B6 boride				Proc. Actinides(sesmbra,Portugal (2007)	Lopes E B,Sologub O L,Casaca A,Havela L,Sebek J,Santava E,Janu Z,Gon,calves A		
156207	PRL108116402	T<CDW> = 262 K.	IrTe2	Ir1Te2	Ir	1	Te	2																				1	2012																												CdI2	P3[-]m1																	K					0.32																																																																																																Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156208	PRL108116402	Pd-intercalated between IrTe2 layers. T<CDW> = 187 K.	PdxIrTe2	Pd0.02Ir1Te2	Pd	0.02	Ir	1	Te	2																		1	2012																																														K		2.15					2.15																																																																																														Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156209	PRL108116402	Pd-intercalated between IrTe2 layers. T<CDW> = (70 -150) K.  GL-parameter (kappa) = 1.53 calculated from M-H curve.	PdxIrTe2	Pd0.03Ir1Te2	Pd	0.03	Ir	1	Te	2																		1	2012																																														K		2.68					2.68	MTC156209																																																																																													Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156210	PRL108116402	Ir in IrTe2 layer replaced by Pd. T<CDW> = 235 K.	PdxIr1-xTe2	Pd0.01Ir0.99Te2	Pd	0.01	Ir	0.99	Te	2																		1	2012																										AB2																				K					1.8																																																																																																Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156211	PRL108116402	Ir in IrTe2 layer replaced by Pd. T<CDW> = 176 K.	PdxIr1-xTe2	Pd0.03Ir0.97Te2	Pd	0.03	Ir	0.97	Te	2																		1	2012																										AB2																				K		2.7					2.7																																																																																														Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156212	PRL108116402	Ir in IrTe2 layer replaced by Pd.  GL-parameter (kappa) = 1.50 calculated from M-H curve.	PdxIr1-xTe2	Pd0.04Ir0.96Te2	Pd	0.04	Ir	0.96	Te	2																		1	2012																										AB2																				K		2.99					2.99	MTC156209																																																																																													Ir(3N5),Te(4N),Pd(4N)		mixture - pellet - sealed in quartz tube - SIN(1000C,15h) - FC to RT - repeat twice with intermediate grinding					Charge-Orbital Density Wave and Superconductivity in the Strong Spin-Orbit Coupled IrTe2:Pd			Laboratory for Pohang Emergent Materials, Pohang University of Science and Technology, Pohang 790-784, Korea	Phys.Rev.Lett., 108(2012)116402	J. J. Yang,Y. J. Choi,Y. S. Oh,A. Hogan,Y. Horibe,K. Kim,B. I. Min,S-W. Cheong		
156213	PRL116127001	(97.5-99.5) % phase pure samples. RRR = 211.  R(T) = R0 + A*T^(3/2). bulk-SC confirmed by SP and SUS.	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		1	2016																										AB2C2					A	3.964		10.457												K		1.83					1.83	MTC156213																			T	R(mid), WHH	2.24							T/K	R(mid)	1.75			MHC156213		A	from Hc2	120																		mJ/mol.K2	100	SP																																						melt by induction furnace. (YFe2 + Ge) - melt - quench  - ANN(1250C,1h) - ANN(800C, 8 days)					Unconventional Superconductivity in the Layered Iron Germanide YFe2Ge2			Cavendish Laboratory, University of Cambridge, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett., 116(2016)127001	Jiasheng Chen,Konstantin Semeniuk,Zhuo Feng,Pascal Reiss,Philip Brown,Yang Zou,Peter W. Logg,Giulio I. Lampronti,F. Malte Grosche		
156300	ACS13514540	not SC. carrier n = 6.93E+19 /cm3 at 5 K.	CsBi4Te6	Cs1Bi4Te6	Cs	1	Bi	4	Te	6																			2013																										AB4C6	4		C2/m		A	51.9205	4.4025	14.5118											monoclinic. beta = 101.480 deg.	K					2																																																																																																		react(Bi2Te3 + Cs vapor, at 670C) - slow cooling - needle like crystals - cleaved samples					Superconductivity in the Narrow-Gap Semiconductor CsBi4Te6			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States	J.Am.Chem.Soc., 135(2013)14540	Christos D. Malliakas,Duck Young Chung,Helmut Claus,Mercouri G. Kanatzidis		
156301	ACS13514540	p-type semicond. n = 0.96E+19 /cm3 at 5 K. Hc2(0) = 9.7 T using GL approx.	Cs0.96Bi4Te6	Cs0.96Bi4Te6	Cs	0.96	Bi	4	Te	6																			2013																										AB4C6	4		C2/m																monoclinic	K			4.4				4.4										14										T	RES(0.9Rn),WHH	8.2												MHC156301																																																														react(Bi2Te3 + Cs vapor, at 670C) - slow cooling - needle like crystals - cleaved samples					Superconductivity in the Narrow-Gap Semiconductor CsBi4Te6			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States	J.Am.Chem.Soc., 135(2013)14540	Christos D. Malliakas,Duck Young Chung,Helmut Claus,Mercouri G. Kanatzidis		
156302	ACS13514540	p-type semicond. n = 1.21E+19 /cm3 at 5 K.	CsBi4.1Te65.9	Cs1Bi4.1Te5.9	Cs	1	Bi	4.1	Te	5.9																			2013																										AB4C6	4		C2/m																monoclinic	K			4.4				4.4										20																																																																																						react(Bi2Te3 + Cs vapor, at 670C) - slow cooling - needle like crystals - cleaved samples					Superconductivity in the Narrow-Gap Semiconductor CsBi4Te6			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, United States	J.Am.Chem.Soc., 135(2013)14540	Christos D. Malliakas,Duck Young Chung,Helmut Claus,Mercouri G. Kanatzidis		
156303	EPL10837010	RRR = 1.31. d[penet](T) measured by TDO and ARPES. As a fitting parameter, [penet] = 8320 A and energy gap  are obtained.. Jc(H=0,T=2K) = 3.4E+2 A/cm2	(Sn,In)Te	Sn0.5In0.5Te1	Sn	0.5	In	0.5	Te	1																		3	2014																										AB		NaCl	Fm3m		A	6.265														K	4.3		4.5			0.2	4.4											mT	M -H curve				1			2	T	RES(0.9Rn),WHH	1.6							T/K	RES(0.9Rn)	0.496			MHC156303		A	from Hc2	143.5			A	from Hc1, GL eq.	8530			meV	1.247	6.4																							mOhm.cm	0.67										0.88												Sn(4N),Te(5N),In(5N)		melt(900C,5days, in quartz tube) - slow cool to 770C over72 h - ANN(770C, 48h) - cool to RT					Superconducting properties of indium-doped topological crystalline insulator SnTe			School of Physical Sciences, Jawaharlal Nehru University - New Delhi, India	EuroPhys.Lett., 108(2014)37010	V. K. Maurya,Shruti,P. Srivastava,S. Patnaik		
156304	JAP0483998	single crystals	Nb5Ge3	Ge3Nb5	Ge	3	Nb	5																				3	1977																										A3B5			I4/mcm		A	10.146		5.136												K	0.32	0.46	0.59				0.46																																																																																																single crystals produced by peritectic melting					Superconductivity of Nb5Ge3			Physics Department, Chalmers University of Technology, Fack, S-402 20 Goreborg 5, Sweden	J.Appl.Phys., 48(1977)3998	T.Claeson,J.Ivarsson,S.E.Rasmuussen		
156305	JAP0483998	poly crystals with large single crystals	Nb5Ge3	Ge3Nb5	Ge	3	Nb	5																				1	1977																										A3B5																				K	0.33	0.45	1				0.45																																																																																																single crystals produced by peritectic melting					Superconductivity of Nb5Ge3			Physics Department, Chalmers University of Technology, Fack, S-402 20 Goreborg 5, Sweden	J.Appl.Phys., 48(1977)3998	T.Claeson,J.Ivarsson,S.E.Rasmuussen		
156306	JPCONF391012090	RRR = 6.5. Impurity phase = WSi2.Solution limit x = 0.2 in W5-xTaxSiB2.	(W,Ta)5SiB2	W4.8Ta0.2Si1B2	W	4.8	Ta	0.2	Si	1	B	2																1	2012																										AB2C5		Mo5SiB2	I4/mcm	140															T2 phase. Mo5SiB2-type	K	6.4		6.6	6.5		0.15	6.5										15																																																																																						See J.Phys.Soc.Jpn 80(2011)024702					Substitution effect on the superconductivity in W5-xTaxSiB2 with the T2 phase structure			Department of Physics and Mathematics, Aoyama Gakuin University, Fuchinobe 5-10-1, Chuo-ku, Sagamihara-shi, Kanagawa 252-5258, Japan	J.Phys. Conf. Ser., 391(2012)012090	M. Fukuma,K. Kawashima,J. Akimitsu		
156307	JPS0683074	Tc defined as R(ab) = 0. (dTc/dP) = 1.7 K/GPa at P = 0 (ortho-), = -0.3 K/GPa at Pc ( = 3.3 GPa (tetragonal)	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1999																												T																		K	22.9						22.9	MTC156307		K/GPa	1.7																																																																																												Single crystals grown by TSFZ method. - ANN ((915C,50h) + (500C,50h), in flowing O2)					Reduction of Superconducting Transition Temperature due to Orthorhombic Distortion in La2-xSrxCuO4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526	J.Phys.Soc.Jpn, 68(1999)3074	Tatsuo Goko,Fumihiko Nakamura,Toshizo Fujita		
156308	JPS0683074	Tc defined as R(c) = 0  (dTc/dP) = 0.8 K/GPa at P = 0 (ortho-), = -3.0 K/GPa at Pc ( = 3.3 GPa (tetragonal)	(La,Sr)2CuO4	La1.9Sr0.1Cu1O4	La	1.9	Sr	0.1	Cu	1															O	4		3	1999																												T																		K	22.9						22.9	MTC156307		K/GPa	-0.8																																																																																												Single crystals grown by TSFZ method. - ANN ((915C,50h) + (500C,50h), in flowing O2)					Reduction of Superconducting Transition Temperature due to Orthorhombic Distortion in La2-xSrxCuO4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526	J.Phys.Soc.Jpn, 68(1999)3074	Tatsuo Goko,Fumihiko Nakamura,Toshizo Fujita		
156309	JPS0683074	Tc defined as R(ab) = 0  (dTc/dP) = 3.0 K/GPa at P = 0 (ortho-), = 0.0 K/GPa at Pc ( = 1.6 GPa (tetragonal)	(La,Sr)2CuO4	La1.855Sr0.145Cu1O4	La	1.855	Sr	0.145	Cu	1															O	4		3	1999																												T																		K	32.2						32.2	MTC156309		K/GPa	3																																																																																												Single crystals grown by TSFZ method. - ANN ((915C,50h) + (500C,50h), in flowing O2)					Reduction of Superconducting Transition Temperature due to Orthorhombic Distortion in La2-xSrxCuO4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526	J.Phys.Soc.Jpn, 68(1999)3074	Tatsuo Goko,Fumihiko Nakamura,Toshizo Fujita		
156310	JPS0683074	Tc defined as R(c) = 0  (dTc/dP) = -0.5 K/GPa at P = 0 (ortho-), = -4.4 K/GPa at Pc ( = 1.6 GPa (tetragonal)	(La,Sr)2CuO4	La1.855Sr0.145Cu1O4	La	1.855	Sr	0.145	Cu	1															O	4		3	1999																												T																		K	32.2						32.2	MTC156309		K/GPa	-0.5																																																																																												Single crystals grown by TSFZ method. - ANN ((915C,50h) + (500C,50h), in flowing O2)					Reduction of Superconducting Transition Temperature due to Orthorhombic Distortion in La2-xSrxCuO4			Department of Quantum Matter, ADSM, Hiroshima University, Higashi-Hiroshima 739-8526	J.Phys.Soc.Jpn, 68(1999)3074	Tatsuo Goko,Fumihiko Nakamura,Toshizo Fujita		
156311	JPS078114712	(dC/gamma*Tc) = 0.32	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2009																										ABCD		oxypnictide				3.956		8.4942											Fe-1111	K				5.8			5.8																				T	RES(0.95Rn), extrapolation		7	1										MHC156311																																																			m3/C	-0.00000000399					MRH156311			Fe,Fe2O3,LaF3,P,LaP		mixture - pressed into pellet - ANN(1100C,40h, in silica tube)					Systematic Study on Fluorine-Doping Dependence of Superconducting and Normal State Properties in LaFePO1-xFx			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043 2JST, TRIP, Chiyoda, Tokyo 102-0075	J.Phys.Soc.Jpn, 78(2009)114712	Shinnosuke SUZUKI,Shigeki MIYASAKA,Setsuko TAJIMA,Takanori KIDA,Masayuki HAGIWARA		
156312	JPS078114712	(dC/gamma*Tc) = 0.42	LaFeP(O,F)	La1Fe1P1F0.03O0.97	La	1	Fe	1	P	1	F	0.03													O	0.97		1	2009																										ABCD		oxypnictide				3.9545		8.4909											Fe-1111	K				7.8			7.8																																		MHC156312																																																			m3/C	-0.00000000381					MRH156311			Fe,Fe2O3,LaF3,P,LaP		mixture - pressed into pellet - ANN(1100C,40h, in silica tube)					Systematic Study on Fluorine-Doping Dependence of Superconducting and Normal State Properties in LaFePO1-xFx			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043 2JST, TRIP, Chiyoda, Tokyo 102-0075	J.Phys.Soc.Jpn, 78(2009)114712	Shinnosuke SUZUKI,Shigeki MIYASAKA,Setsuko TAJIMA,Takanori KIDA,Masayuki HAGIWARA		
156313	JPS078114712	(dC/gamma*Tc) = 0.46	LaFeP(O,F)	La1Fe1P1F0.05O0.95	La	1	Fe	1	P	1	F	0.05													O	0.95		1	2009																										ABCD		oxypnictide				3.955		8.4919											Fe-1111	K				8			8																																		MHC156313																																																			m3/C	-0.00000000372					MRH156311			Fe,Fe2O3,LaF3,P,LaP		mixture - pressed into pellet - ANN(1100C,40h, in silica tube)					Systematic Study on Fluorine-Doping Dependence of Superconducting and Normal State Properties in LaFePO1-xFx			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043 2JST, TRIP, Chiyoda, Tokyo 102-0075	J.Phys.Soc.Jpn, 78(2009)114712	Shinnosuke SUZUKI,Shigeki MIYASAKA,Setsuko TAJIMA,Takanori KIDA,Masayuki HAGIWARA		
156314	JPS078114712		LaFeP(O,F)	La1Fe1P1F0.08O0.92	La	1	Fe	1	P	1	F	0.08													O	0.92		1	2009																										ABCD		oxypnictide				3.954		8.4939											Fe-1111	K				7.8			7.8																																																																																														Fe,Fe2O3,LaF3,P,LaP		mixture - pressed into pellet - ANN(1100C,40h, in silica tube)					Systematic Study on Fluorine-Doping Dependence of Superconducting and Normal State Properties in LaFePO1-xFx			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043 2JST, TRIP, Chiyoda, Tokyo 102-0075	J.Phys.Soc.Jpn, 78(2009)114712	Shinnosuke SUZUKI,Shigeki MIYASAKA,Setsuko TAJIMA,Takanori KIDA,Masayuki HAGIWARA		
156315	JPS078114712		LaFeP(O,F)	La1Fe1P1F0.1O0.9	La	1	Fe	1	P	1	F	0.1													O	0.9		1	2009																										ABCD		oxypnictide				3.9531		8.496											Fe-1111	K				62			62																																																																																														Fe,Fe2O3,LaF3,P,LaP		mixture - pressed into pellet - ANN(1100C,40h, in silica tube)					Systematic Study on Fluorine-Doping Dependence of Superconducting and Normal State Properties in LaFePO1-xFx			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043 2JST, TRIP, Chiyoda, Tokyo 102-0075	J.Phys.Soc.Jpn, 78(2009)114712	Shinnosuke SUZUKI,Shigeki MIYASAKA,Setsuko TAJIMA,Takanori KIDA,Masayuki HAGIWARA		
156316	JPS079103703	Fe-As-Fe(in plane) angle = 112.3 deg. energy gap measured by NMR. Y(3+) substitution does not change the doping level.	(La,Y)FeAsO0.7	La0.8Y0.2Fe1As1O0.7	La	0.8	Y	0.2	Fe	1	As	1													O	0.7		1	2010																										ABCD		oxypnictide			A	4.004													Fe-1111	K				34			34																																																6.9	6																																															High-P synthesis					Origin of Tc Enhancement Induced by Doping Yttrium and Hydrogen into LaFeAsO-Based Superconductors: <57>Fe-, <75>As-, <139>La-, and <1>H-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 79(2010)103703	Hiroki YAMASHITA,Hidekazu MUKUDA,Mitsuharu YASHIMA,Satoshi FURUKAWA,Yoshio KITAOKA,Kiichi MIYAZAWA,Parasharam M. SHIRAGE,Hiroshi EISAKI,Akira IYO		
156317	JPS079103703	Fe-As-Fe(in plane) angle = 111.7 deg. energy gap measured by NMR. H-doping decreases the carrier density.	LaFeAsO0.58H0.58	La1Fe1As1H0.58O0.58	La	1	Fe	1	As	1	H	0.58													O	0.58		1	2010																										ABCD		oxypnictide			A	3.989													Fe-1111	K				32			32																																																4.7	6																																															High-P synthesis					Origin of Tc Enhancement Induced by Doping Yttrium and Hydrogen into LaFeAsO-Based Superconductors: <57>Fe-, <75>As-, <139>La-, and <1>H-NMR Studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc.Jpn, 79(2010)103703	Hiroki YAMASHITA,Hidekazu MUKUDA,Mitsuharu YASHIMA,Satoshi FURUKAWA,Yoshio KITAOKA,Kiichi MIYAZAWA,Parasharam M. SHIRAGE,Hiroshi EISAKI,Akira IYO		
156318	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.41, A = 0.21E-5 Ohm.cm/K^n.  RH(50K) = -5.50E-3 cm3/C.	LaFe(As,P)(O,F)	La1Fe1As0.4P0.6F0.1O0.9	La	1	Fe	1	As	0.4	P	0.6	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9708		8.5458											Fe-1111	K			21.4				21.4	MTC156318																																																																																				m3/C						MRH156318					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156319	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.31, A = 0.45E-5 Ohm.cm/K^n.  RH(50K) = -8.26E-3 cm3/C.	LaFe(As,P)(O,F)	La1Fe1As0.8P0.2F0.1O0.9	La	1	Fe	1	As	0.8	P	0.2	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	4.0092		8.6463											Fe-1111	K			26				26																																																																																					m3/C						MRH156319					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156320	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 2.04, A = 0.01E-5 Ohm.cm/K^n.  RH(50K) = -3.22E-3 cm3/C.	PrFeP(O,F)	Pr1Fe1P1F0.1O0.9	Pr	1	Fe	1	P	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide			A	3.9099		8.3452											Fe-1111	K			2.34				2.34																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156321	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.83, A = 0.01E-5 Ohm.cm/K^n.  RH(50K) = -2.56E-3 cm3/C.	PrFe(As,P)(O,F)	Pr1Fe1As0.2P0.8F0.1O0.9	Pr	1	Fe	1	As	0.2	P	0.8	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9292		8.3812											Fe-1111	K			8.71				8.71																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156322	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.51, A = 0.06E-5 Ohm.cm/K^n.  RH(50K) = -10.5E-3 cm3/C.	PrFe(As,P)(O,F)	Pr1Fe1As0.4P0.6F0.1O0.9	Pr	1	Fe	1	As	0.4	P	0.6	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9384		8.4071											Fe-1111	K			17.4				17.4	MTC156322																																																																																				m3/C						MRH156322					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156323	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.21, A = 0.40E-5 Ohm.cm/K^n.  RH(50K) = -24.3E-3 cm3/C.	PrFe(As,P)(O,F)	Pr1Fe1As0.6P0.4F0.1O0.9	Pr	1	Fe	1	As	0.6	P	0.4	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9608		8.4763											Fe-1111	K			23.4				23.4																																																																																					m3/C						MRH156323					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156324	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.13, A = 0.34E-5 Ohm.cm/K^n.  RH(50K) = -11.4E-3 cm3/C.	PrFe(As,P)(O,F)	Pr1Fe1As0.8P0.2F0.1O0.9	Pr	1	Fe	1	As	0.8	P	0.2	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9723		8.5284											Fe-1111	K			29.2				29.2																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156325	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.31, A = 0.098E-5 Ohm.cm/K^n.  RH(50K) = -2.72E-3 cm3/C.	PrFe(As,P)(O,F)	Pr1Fe1As0.9P0.1F0.1O0.9	Pr	1	Fe	1	As	0.9	P	0.1	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9801		8.5603											Fe-1111	K			35.2				35.2																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156326	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.38, A = 0.1E-5 Ohm.cm/K^n.  RH(50K) = -5.93E-3 cm3/C.	PrFeAs(O,F)	Pr1Fe1As1F0.1O0.9	Pr	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide			A	3.9811		8.5958											Fe-1111	K			44				44																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156327	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 2.05, A = 0.03E-5 Ohm.cm/K^n.  RH(50K) = -3.06E-3 cm3/C.	NdFeP(O,F)	Nd1Fe1P1F0.1O0.9	Nd	1	Fe	1	P	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide			A	3.8805		8.2682											Fe-1111	K			2.9				2.9																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156328	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.89, A = 0.008E-5 Ohm.cm/K^n.  RH(50K) = -2.72E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.2P0.8F0.1O0.9	Nd	1	Fe	1	As	0.2	P	0.8	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.893		8.3017											Fe-1111	K			6.98				6.98																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156329	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.43, A = 0.26E-5 Ohm.cm/K^n.  RH(50K) = -8.23E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.4P0.6F0.1O0.9	Nd	1	Fe	1	As	0.4	P	0.6	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9065		8.3521											Fe-1111	K			22.6				22.6																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156330	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.29, A = 0.46E-5 Ohm.cm/K^n.  RH(50K) = -10.9E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.5P0.5F0.1O0.9	Nd	1	Fe	1	As	0.5	P	0.5	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.917		8.4027											Fe-1111	K			25.2				25.2	MTC156330																																																																																				m3/C						MRH156330					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156331	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.09, A = 1.71E-5 Ohm.cm/K^n.  RH(50K) = -12.1E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.6P0.4F0.1O0.9	Nd	1	Fe	1	As	0.6	P	0.4	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9245		8.4126											Fe-1111	K			28				28																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156332	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.23, A = 0.58E-5 Ohm.cm/K^n.  RH(50K) = -13.9E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.7P0.3F0.1O0.9	Nd	1	Fe	1	As	0.7	P	0.3	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9279		8.4368											Fe-1111	K			29.5				29.5																																																																																					m3/C						MRH156332					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156333	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.25, A = 0.35E-5 Ohm.cm/K^n.  RH(50K) = -12.7E-3 cm3/C.	NdFe(As,P)(O,F)	Nd1Fe1As0.8P0.2F0.1O0.9	Nd	1	Fe	1	As	0.8	P	0.2	F	0.1											O	0.9		1	2013																										ABCD		oxypnictide			A	3.9394		8.4596											Fe-1111	K			34.1				34.1																																																																																																solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156334	JPS082124706	R(T) = R0 + A*T^n for Tc < T < 100K, n = 1.09, A = 0.82E-5 Ohm.cm/K^n.  RH(50K) = -4.31E-3 cm3/C.	NdFeAs(O,F)	Nd1Fe1As1F0.1O0.9	Nd	1	Fe	1	As	1	F	0.1													O	0.9		1	2013																										ABCD		oxypnictide			A	3.9395		8.4961											Fe-1111	K			50.1				50.1																																																																																					m3/C						MRH156334					solid state reaction					Two Fermi Surface States and Two Tc-Rising Mechanisms Revealed by Transport Properties in RFeP1-xAsxO0.9F0.1 (R = La, Pr, and Nd)			Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 82(2013)124706	Shigeki MIYASAKA,Akira TAKEMORI,Tatsuya KOBAYASHI,Shinnosuke SUZUKI,Satoshi SAIJO,Setsuko TAJIMA		
156335	JPS085013702	M-intercalated materials. M = HMDA (hexamethylenediamine).  As-grown(phase I). Interlayer spacing, d= 16.17 A. contents(x,y) not given	Lix(HMDA)yFe2Se2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2016																												Thcr2Si2			A			32.33												K				38			38																																																																																																powder mixture (Li:FeSe=1:2) -put into HMDA - reaction(45C, 2days) - separation from residual HMDA					New Superconducting Phase of Lix(C6H16N2)yFe2-zSe2 with Tc = 41K Obtained through the Post-Annealing			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 85(2016)013702	Shohei Hosono,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
156336	JPS085013702	M-intercalated materials. M = HMDA (hexamethylenediamine).  Post annealing(150C)-sample(phase III). Interlayer spacing, d= 16.17 A. contents(x,y) not given	Lix(HMDA)yFe2Se2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2016																												Thcr2Si2			A			20.59												K				41			41																																																																																																powder mixture (Li:FeSe=1:2) -put into HMDA - reaction(45C, 2days) - separation from residual HMDA					New Superconducting Phase of Lix(C6H16N2)yFe2-zSe2 with Tc = 41K Obtained through the Post-Annealing			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 85(2016)013702	Shohei Hosono,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
156337	JPS085013704	Tc(SP) = 3.5K. Lattice term in SP (beta) = 0.372 mJ/mol.K4. (dCel)/k = 4.7 mJ/mol.K2. (dCel/kTc) = 1.55.	ScIrP	Sc1Ir1P1	Sc	1	Ir	1	P	1																		1	2016																										ABC		ZrNiAl	P6[-]2m		A	6.3309		3.8854											hexagonal	K	3.3	3.46	3.65	3.4			3.46										220										T	RES(0.5Rn), GL	5.11												MHC156337		A	from Hc2	80.3										3.1	14				MSP156337			mJ/mol.K2	4.11	SP																																				Sc(chip),Ir(powder),P(black)		solid state reaction. mixture - sealed in quaerz tube - heat(673K,12h +1173K,96h) - reground - pellet - wrapped un Ta-foil - sealed in quartz tube - heat(1423K,44h)					Superconductivity in the Hexagonal Ternary Phosphide ScIrP			Department of Applied Physics, Nagoya University, Nagoya 464-8603, Japan	J.Phys.Soc.Jpn, 85(2016)013704	Yoshihiko Okamoto,Takumi Inohara,Youichi Yamakawa,Ai Yamakage,Koshi Takenaka		
156338	JPS085024715		LaRhSi3	La1Rh1Si3	La	1	Rh	1	Si	3																		3	2016																										ABC3		BaNiSn3	I4mm	107																K		2.3					2.3																																		MHC156338																																																																			Type II/I Superconductivity with Extremely High Hc3 in Noncentrosymmetric LaRhSi3			Department of Physics, Tohoku University, Sendai 980-8578, Japan	J.Phys.Soc.Jpn, 85(2016)024715	Noriaki Kimura,Noriyuki Kabeya,Kohsuke Saitoh,Kazunori Satoh,Hajime Ogi,Kohki Ohsaki,Haruyoshi Aoki		
156339	JPS085034706	RRR = 31, Rn = 3.4 uOhm.cm for J//[001]. (dCel/gamma*Tc) = 1.30. Hc(0) = 0.1T. Tc in Tc(P) -Fig. defined as Tc(zero).	Zr2Co	Co1Zr2	Co	1	Zr	2																				3	2016																										AB2		CuAl2	I4/mcm	140																K	5.2	5	6				5	MTC156339									100	Oe	M-H,		112	112					T	RES,SP, WHH		1.3	1.1					T/K			0.38		MHC156339		A	from Hc2		160		A	Hc1		1900				3.36	14				MSP156339			mJ/mol.K2	22.5	SP	235	SP											uOhm.cm		3.4	3.8																				Zr(3N),Co(4N)		Bridgman method. poly(Zr2Co) by arc-melting - crushed - yttria crucible - quartz tube -heat to 1150C - slow cool to 1050C 84days) - cool to RT					Superconducting and Fermi Surface Properties of Single Crystal Zr2Co			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa 903-0213, Japan	J.Phys.Soc.Jpn, 85(2016)034706	Atsushi Teruya,Masashi Kakihana,Tetsuya Takeuchi,Dai Aoki,Fuminori Honda,Ai Nakamura,Yoshinori Haga,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hisatomo Harima,Masato Hedo,Takao Nakama,Yoshichika Onuki		
156340	JPS085043701	no CDW. RRR = 1.65.  GL(kappa) = 31.7. e-ph = 0.554. DOS = 2.28 states/eV.f.u. Hc(0) = 13.4 mT. (beta) in SP = 2.35 mJ/mol.K4	LT-SrPd2Sb2	Sr1Pd2Sb2	Sr	1	Pd	2	Sb	2																			2016																										AB2C2		CaBa2Ge2	P4/nmm	129	A	4.637		10.629												K	1.9					0.1	1.9											Oe		10.6							T	RES(0.5Rn),Linear approx.	0.6												MHC156340		A	from Hc2	234			A	Hc(0),Hc1	7890										MSP156340			mJ/mol.K2	8.36	SP	161	SP																																				mixture - sealed in quartz tube - heat(900C,20h + 720C,72h) - cool to RT					Superconductivity in Ternary Pnictide SrPd2Sb2 Polymorphs			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 85(2016)043701	Naoki Kase,Harufumi Suzuki,Takenori Tsukamoto,Tomohito Nakano,Naoya Takeda		
156341	JPS085043701	no CDW. RRR = 1.7.  e-ph = 0.453. DOS = 1.54 states/eV.f.u.  (beta) in SP = 3.75 mJ/mol.K4 [gamma] in SP = 5.27 mJ/mol.K2 for normal state	HT-SrPd2Sb2	Sr1Pd2Sb2	Sr	1	Pd	2	Sb	2																			2016																										AB2C2		Thcr2Si2	I4/mmm	139	A	4.621		10.776												K	0.6					0.15	0.6																				T	RES(0.5Rn),Linear approx.	0.06												MHC156341		A	from Hc2	741																		mJ/mol.K2	7.27	SP	137	SP																																				mixture - ampule - heat(900C.20h) - Q to ice water					Superconductivity in Ternary Pnictide SrPd2Sb2 Polymorphs			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 85(2016)043701	Naoki Kase,Harufumi Suzuki,Takenori Tsukamoto,Tomohito Nakano,Naoya Takeda		
156342	JPS085053702	Ag-content x = 0.18 by EDX. Tc(SUS) defined as T where SUS become negative.	Sn1-xAgxTe	Sn0.85Ag0.15Te1	Sn	0.85	Ag	0.15	Te	1																		1	2016																										AB		NaCl			A	6.2136														K			2.4	2.15			2.15																																																																																														Ag(3N),Sn(4N),Te(6N)		High-P synthesis using cubic anvil type system. mixture - pressed into pellet - BN-capsule - heat(500C,30min, P=2 GPa)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156343	JPS085053702	Ag-content x = 0.23 by EDX. Tc(SUS) defined as T where SUS become negative. Hc2(0) = 1.04 T using linear approx.	Sn1-xAgxTe	Sn0.8Ag0.2Te1	Sn	0.8	Ag	0.2	Te	1																		1	2016																										AB		NaCl			A	6.1768														K			2.4	2.29			2.29	MTC156343																			T	SUS(negative point), WHH	0.72												MHC156343																																																												Ag(3N),Sn(4N),Te(6N)		High-P synthesis using cubic anvil type system. mixture - pressed into pellet - BN-capsule - heat(500C,30min, P=2 GPa)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156344	JPS085053702	Ag-content x = 0.34 by EDX. Tc(SUS) defined as T where SUS become negative.	Sn1-xAgxTe	Sn0.75Ag0.25Te1	Sn	0.75	Ag	0.25	Te	1																		1	2016																										AB		NaCl			A	6.1407														K			2.4	2.2			2.2																																																																																														Ag(3N),Sn(4N),Te(6N)		High-P synthesis using cubic anvil type system. mixture - pressed into pellet - BN-capsule - heat(500C,30min, P=2 GPa)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156345	JPS085053702	Ag-content x = 0.40 by EDX. Tc(SUS) defined as T where SUS become negative.	Sn1-xAgxTe	Sn0.67Ag0.33Te1	Sn	0.67	Ag	0.33	Te	1																		1	2016																										AB		NaCl			A	6.1089														K			2.4	1.95			1.95																																																																																														Ag(3N),Sn(4N),Te(6N)		High-P synthesis using cubic anvil type system. mixture - pressed into pellet - BN-capsule - heat(500C,30min, P=2 GPa)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156346	JPS085053702	Ag-content x = 0.39 by EDX. Tc(SUS) defined as T where SUS become negative.	Sn1-xAgxTe	Sn0.5Ag0.5Te1	Sn	0.5	Ag	0.5	Te	1																		1	2016																										AB		NaCl			A	6.0823														K					1.8																																																																																																Ag(3N),Sn(4N),Te(6N)		High-P synthesis using cubic anvil type system. mixture - pressed into pellet - BN-capsule - heat(500C,30min, P=2 GPa)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156347	JPS085053702	Synthesis at ambient pressure. Two phases: phase-1(Sn-rich phase a = 6.2225 A) and phase-2(Sn0.5Ag0.5Te phase. a = 6.0789A)	Sn1-xAgxTe	Sn0.6Ag0.4Te1	Sn	0.6	Ag	0.4	Te	1																		2	2016																										AB		NaCl			A	6.2225													Phase-2 (a = 6.0789 A)	K				1.95			1.95																																																																																														Ag(3N),Sn(4N),Te(6N)		solid state reaction at ambient pressure (600C,10h)					High-Pressure Synthesis and Superconductivity of Ag-Doped Topological Crystalline Insulator SnTe (Sn1-xAgxTe with x = 0-0.5)			Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)053702	Yoshikazu Mizuguchi,Osuke Miura		
156348	JPS085064710	impurity phase = RbFe2As2. RRR = 11.2. Anomaly appears around 15 K ( due to magnetic order of Eu(2+) ) in SUS(T)	EuRbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																1	2016																										ABC4D4			P4/mmm	123	A	3.889		13.3											Fe-1144 type	K	35.8		36.2	36			36																				T	RES(mid),WHH	92							T/K	RES(0.5Rn)	3.692			MHC156348		A	from Hc2	18																																																										See J.Am.Chem.Soc., 138(2016)3410					Superconductivity in Fe-Based Compound EuAFe4As4 (A = Rb and Cs)			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys.Soc.Jpn, 85(2016)064710	Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida,Akira Iyo		
156349	JPS085064710	impurity phase = CsFe2As2. RRR = 14.5. Anomaly appears around 15 K ( due to magnetic order of Eu(2+) ) in SUS(T)	EuCsFe4As4	Eu1Cs1Fe4As4	Eu	1	Cs	1	Fe	4	As	4																1	2016																										ABC4D4			P4/mmm	123	A	3.901		13.63											Fe-1144 type	K	34.9		35.1	35			35																				T	RES(mid),WHH	87.5							T/K	RES(0.5Rn)	3.612			MHC156349		A	from Hc2	19																																																										See J.Am.Chem.Soc., 138(2016)3410					Superconductivity in Fe-Based Compound EuAFe4As4 (A = Rb and Cs)			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys.Soc.Jpn, 85(2016)064710	Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida,Akira Iyo		
156350	JPS085073707	Thermal conductivity k measured down to 100 mK. k/T =  0.1 mW/K2.m when T tends to 0 K. Thermal conductivity shows fully gapped SC.	Nd(O,F)BiS2	Nd1Bi1S2F0.29O0.71	Nd	1	Bi	1	S	2	F	0.29													O	0.71		3	2016																										ABCD2																			BiS2 type	K			5.2				5.2										100	Oe			30						T				1												A			180		A			4470																	mW/K.m				MTHC156350																															Flux method using CsCl/KCl as flux					Conventional s-Wave Superconductivity in BiS2-Based NdO0.71F0.29BiS2 Revealed by Thermal Transport Measurements			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 85(2016)073707	Takuya Yamashita,Yoshifumi Tokiwa,Daiki Terazawa,Masanori Nagao,Satoshi Watauchi,Isao Tanaka,Takahito Terashima,Yuji Matsuda		
156351	JPS085073713	H// = H//[001], H/n = H//[110]. gamma in mJ/U-mol.K2. (dC/gamma*Tc) = 1.58. Hc(0) = 0.065T. A = 0.012 uOhm.cm/K2 R0 = 54 uOhm.cm for R = R0 + A*T2.	U6Co	Co1U6	Co	1	U	6																				3	2016																										AB6	2	U5Mn	I4/mcm	140	A	10.36		5.21												K	2.33	2.36	2.8				2.36																				T	RES(mid). Linear approx.		7.85	6.56					T/K	RES(mid)	4.3	3.4		MHC156351		A			65	71						K	3.97	3.7	14				MSP156351			mJ/mol.K2	20	SP																																						self-flux method. (U:Co = 76:24) - put in alumina crucible - sealed in quartz ampoule - heat(830C,300h) - cool to 740C with 0.4C/h.					Large Upper Critical Field of Superconductivity in the Single Crystal U6Co			IMR, Tohoku University, Oarai, Ibaraki 311-1313, Japan	J.Phys.Soc.Jpn, 85(2016)073713	Dai Aoki,Ai Nakamura,Fuminori Honda,DeXin Li,Yoshiya Homma		
156352	MMM4000066	RRR = 19. R(T) has a steep drop at T0 (= 0.67 K)  due to multipolar ordering	PrV2Al20	Pr1V2Al20	Pr	1	V	2	Al	20																		3	2016																										AB2C20																				K			0.05				0.05																																																																																																Al-self-flux method					Strong orbital fluctuations in multipolar ordered states of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Japan	J.Mag.Mag.Mat., 400(2016)66	Yosuke Matsumoto,Masaki Tsujimoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
156353	MMM4000066	RRR = 18	PrV2Al20	Pr1V2Al20	Pr	1	V	2	Al	20																		3	2016																										AB2C20																				K			0.039				0.039																																																																																																Al-self-flux method					Strong orbital fluctuations in multipolar ordered states of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Japan	J.Mag.Mag.Mat., 400(2016)66	Yosuke Matsumoto,Masaki Tsujimoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
156354	MMM4000066	RRR = 4. not SC. R(T) has a steep drop at T0 (= 0.5 K) due to multipolar ordering	PrV2Al20	Pr1V2Al20	Pr	1	V	2	Al	20																		3	2016																										AB2C20																				K					0.038																																																																																																		Al-self-flux method					Strong orbital fluctuations in multipolar ordered states of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Japan	J.Mag.Mag.Mat., 400(2016)66	Yosuke Matsumoto,Masaki Tsujimoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
156355	MMM4000066	RRR = 7. not SC.	PrV2Al20	Pr1V2Al20	Pr	1	V	2	Al	20																		3	2016																										AB2C20																				K					0.043																																																																																																		Al-self-flux method					Strong orbital fluctuations in multipolar ordered states of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Japan	J.Mag.Mag.Mat., 400(2016)66	Yosuke Matsumoto,Masaki Tsujimoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
156356	MMM4000066	RRR = 150. R(T) has a steep drop at T0 (= 2.0 K) due to multipolar ordering	PrTi2Al20	Pr1Ti2Al20	Pr	1	Ti	2	Al	20																		3	2016																										AB2C20																				K			0.19				0.19																																																																																																Al-self-flux method					Strong orbital fluctuations in multipolar ordered states of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Japan	J.Mag.Mag.Mat., 400(2016)66	Yosuke Matsumoto,Masaki Tsujimoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
156357	MMM4170420	RRR = 2.4. unit volume = 161.4 A^3.	YPd2P2	Y1Pd2P2	Y	1	Pd	2	P	2																		3	2016																										AB2C2		ThCr2Si2	I4/mmm		A	4.05		9.84												K				0.96			0.96																																																																																																Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156358	MMM4170420	RRR = 7.8. unit volume = 174.1 A^3.	LaPd2P2	La1Pd2P2	La	1	Pd	2	P	2																		3	2016																										AB2C2		ThCr2Si2	I4/mmm		A	4.12		9.89												K				0.75			0.75																																																																																																Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156359	MMM4170420	not SC. RRR = 12.4. unit volume = 171.1 A^3. Curie-T = -344K(H//ab), 64 K(H//c). Tm(ferromag) = 28.4 K.	CePd2P2	Ce1Pd2P2	Ce	1	Pd	2	P	2																		3	2016					myu-B/R	2.44	-344																			AB2C2		ThCr2Si2	I4/mmm		A	4.16		9.9												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156360	MMM4170420	not SC. RRR = 7. unit volume = 169.5 A^3. Curie-T = -55K(H//ab), 32 K(H//c). Tm(ferromag) = 8.3 K.	YPrPd2P2	Pr1Pd2P2	Pr	1	Pd	2	P	2																		3	2016					myu-B/R	3.52	-55																			AB2C2		ThCr2Si2	I4/mmm		A	4.14		9.88												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156361	MMM4170420	not SC. RRR = 5.4. unit volume = 168.1 A^3. Curie-T = -25K(H//ab), -2 K(H//c). Tm(AFM) = 6.0 K.	NdPd2P2	Nd1Pd2P2	Nd	1	Pd	2	P	2																		3	2016					myu-B/R	3.64	-25	6																		AB2C2		ThCr2Si2	I4/mmm		A	4.12		9.88												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156362	MMM4170420	not SC. RRR = 3.8. unit volume = 165.8 A^3. Tm(AFM) = 3.3 K.	SmPd2P2	Sm1Pd2P2	Sm	1	Pd	2	P	2																		3	2016								3.3																		AB2C2		ThCr2Si2	I4/mmm		A	4.1		9.87												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156363	MMM4170420	not SC. RRR = 10. unit volume = 170.8 A^3. Curie-T = -30K(H//ab),  -31 K(H//c). At least, 4 magnetic  transitions (T1=18.2, T2=12.4, T3=9.8, T4 = 5.8 K in R(T) and SUS(T).Tm(AFM) = 18.2 K.	EuPd2P2	Eu1Pd2P2	Eu	1	Pd	2	P	2																		3	2016					myu-B/R	7.6	-30	18.2																		AB2C2		ThCr2Si2	I4/mmm		A	4.16		9.74												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R5Pd60P35) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156364	MMM4170420	not SC. RRR = 3. unit volume = 164.2 A^3. Curie-T = -25K(H//ab), -27 K(H//c). Tm(AFM) = 10.0 and 7.0  K.	GdPd2P2	Gd1Pd2P2	Gd	1	Pd	2	P	2																		3	2016					myu-B/R	8.01	-25	10.1																		AB2C2		ThCr2Si2	I4/mmm		A	4.08		9.86												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R10Pd54P36) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156365	MMM4170420	not SC. RRR = 2.5. unit volume = 162.5 A^3. Curie-T = -10.7K(H//ab),  4.3 K(H//c). Three magnetic transitions (T1= 12.0 K(AFM), T2 = 7.5 K(AFM) T3 = 4.6 K, in R(T).	TbPd2P2	Tb1Pd2P2	Tb	1	Pd	2	P	2																		3	2016					myu-B/R	9.71	-107	12																		AB2C2		ThCr2Si2	I4/mmm		A	4.06		9.86												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R10Pd54P36) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156366	MMM4170420	not SC. RRR = 2.5. unit volume = 161.2 A^3. Curie-T = -37K(H//ab),  16 K(H//c). Two magnetic transitions (T1= 6.2 K(AFM), T2 = 2.5 K , in R(T).	DyPd2P2	Dy1Pd2P2	Dy	1	Pd	2	P	2																		3	2016					myu-B/R	10.62	-37	6.3																		AB2C2		ThCr2Si2	I4/mmm		A	4.02		9.85												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R10Pd54P36) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156367	MMM4170420	not SC. RRR = 2. unit volume = 159.8 A^3. Curie-T = -10K(H//ab),  2 K(H//c). magnetic transition Tn = 5.2 K in R(T).	HoPd2P2	Ho1Pd2P2	Ho	1	Pd	2	P	2																		3	2016					myu-B/R	1.64	-10	5.2																		AB2C2		ThCr2Si2	I4/mmm		A	4.03		9.84												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R10Pd54P36) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156368	MMM4170420	not SC. RRR = 5. unit volume = 163.0 A^3.  broad magnetic transition around 5.2 K.	YbPd2P2	Yb1Pd2P2	Yb	1	Pd	2	P	2																		3	2016																										AB2C2		ThCr2Si2	I4/mmm		A	4.1		8.72												K					0.03																																																																																																		Crystals grown from self flux by adding 5-10% R in to Pd67P33. resultant(R10Pd54P36) -  alumina crucible - silica ampules - heat (300C,3h + 6h) - heat(1180C,12h) - cool to 930C (90-120h)					Magnetization and transport properties of single crystalline  RPd2P2 (R=Y, La-Nd, Sm-Ho, Yb)			Department of Physics and  Astronomy, Iowa State University, Ames, IA50011, USA	J.Mag.Mag.Mat., 417(2016)66	Gil Drachuck,Anna E. Bohmer,Sergey L. Bud'ko,Paul C. Canfield		
156369	NATCOM0055508	RRR = 240. SC properties at P = 9.5 kbar are in DB. Coexistence of AFM and SC for 3 < P < 8 kbar	CrAs	As1Cr1	As	1	Cr	1																				3	2014																										AB		MnP			A	5.649	3.463	6.2084												K		1.506			0		1.506	MPH156369																			T	RES(mid), T^2 approx.	0.96												MHC156369		A	from Hc2	185																																																										Flux method using Sn-flux					Superconductivity in the vicinity of antiferromagnetic order in CrAs			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Nature Commun., 5(2014)5508	Wei Wu,Jinguang Cheng,Kazuyuki Matsubayashi,Panpan Kong,Fukun Lin,Changqing Jin,Nanlin Wang,Yoshiya Uwatoko,Jianlin Luo		
156370	NATM0120605	Annealing step= 15. Tc and gap size ( measured by photoemission) depend on annealing conditions.	FeSe monolayer	Fe1Se1	Fe	1	Se	1																					2013																										AB																				K		65					65	MGAP156370																																													meV	19																																																	FeSe monolayers grown on SrTiO3 sibstrate by MBE method.					Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films			National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Nature Materials, 12(2013)605	Shaolong He,Junfeng He,Wenhao Zhang,Lin Zhao,Defa Liu,Xu Liu,Daixiang Mou,Yun-Bo Ou,Qing-YanWang,Zhi Li,LiliWang,Yingying Peng,Yan Liu,Chaoyu Chen,Xi Chen,Xucun Ma		
156371	NATM0120605	Annealing step= 13. Tc and gap size ( measured by photoemission) depend on annealing conditions.	FeSe monolayer	Fe1Se1	Fe	1	Se	1																					2013																										AB																				K		60					60	MGAP156371																																													meV	16																																																	FeSe monolayers grown on SrTiO3 sibstrate by MBE method.					Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films			National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Nature Materials, 12(2013)605	Shaolong He,Junfeng He,Wenhao Zhang,Lin Zhao,Defa Liu,Xu Liu,Daixiang Mou,Yun-Bo Ou,Qing-YanWang,Zhi Li,LiliWang,Yingying Peng,Yan Liu,Chaoyu Chen,Xi Chen,Xucun Ma		
156372	NATM0120605	Annealing step= 12. Tc and gap size ( measured by photoemission) depend on annealing conditions.	FeSe monolayer	Fe1Se1	Fe	1	Se	1																					2013																										AB																				K		55					55	MGAP156372																																													meV	14																																																	FeSe monolayers grown on SrTiO3 sibstrate by MBE method.					Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films			National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Nature Materials, 12(2013)605	Shaolong He,Junfeng He,Wenhao Zhang,Lin Zhao,Defa Liu,Xu Liu,Daixiang Mou,Yun-Bo Ou,Qing-YanWang,Zhi Li,LiliWang,Yingying Peng,Yan Liu,Chaoyu Chen,Xi Chen,Xucun Ma		
156373	NATM0120605	Annealing step= 10. Tc and gap size ( measured by photoemission) depend on annealing conditions.	FeSe monolayer	Fe1Se1	Fe	1	Se	1																					2013																										AB																				K		40					40	MGAP156373																																													meV	10																																																	FeSe monolayers grown on SrTiO3 sibstrate by MBE method.					Phase diagram and electronic indication of high-temperature superconductivity at 65 K in single-layer FeSe films			National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Nature Materials, 12(2013)605	Shaolong He,Junfeng He,Wenhao Zhang,Lin Zhao,Defa Liu,Xu Liu,Daixiang Mou,Yun-Bo Ou,Qing-YanWang,Zhi Li,LiliWang,Yingying Peng,Yan Liu,Chaoyu Chen,Xi Chen,Xucun Ma		
156374	PCS0840017	Impurity phase: Bi2S3,Bi. unit volume =221.71A^3. Hc2(0) = 15.9 T at P=1.68 GPa.	La(O0.5F0.5)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																										ABCD2	2		P4/nmm		A	4.06		13.38												K			2.7				2.7	MTC156374																			T	RES(on),WHH	1.64												MHC156374																																																												La,La2O3,LaF3,Bi,S		mixture - pellet - sealed in quartz tube - SIN(650C,12h) cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
156375	PCS0840017	Impurity phase: Bi2S3,Bi. unit volume =216.33A^3. Hc2(0) = 8.8 T at P=1.97 GPa	Pr(O0.5F0.5)BiS2	Pr1Bi1S2F0.5O0.5	Pr	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																										ABCD2	2		P4/nmm		A	4.03		13.42												K			3.5				3.5	MTC156374																			T	RES(on),WHH	2.65												MHC156375																																																												Pr,Pr6O11,PrF3,Bi,S		mixture - pellet - sealed in quartz tube - SIN(650C,12h) cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
156376	PCS0840017	Impurity phase: Bi2S3,Bi. unit volume =214.60A^3. Hc2(0) = 8.2 T at P=1.97 GPa.	Nd(O0.5F0.5)BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5		1	2015																										ABCD2	2		P4/nmm		A	3.99		13.38												K			4.5				4.5	MTC156374																			T	RES(on),WHH	2.84												MHC156376																																																												Nd,Nd2O3,NdF3,Bi,S		mixture - pellet - sealed in quartz tube - SIN(650C,12h) cool to RT					Effect of hydrostatic pressures on the superconductivity of new BiS2 based REO0.5F0.5BiS2 (RE = La, Pr and Nd) superconductors			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Chem.Solids, 84(2015)17	Rajveer Jha,H. Kishan,V.P.S. Awana		
156377	PHC2620249	Weak FM component of 0.33 mhi-B/Er for T<2.3 K. M vs H measured for H//[100], H//[110], and H//[001].	ErNi2B2C	Er1Ni2B2C1	Er	1	Ni	2	B	2	C	1																3	1996							2.3	6																		ABC2D2		LuNi2B2C																		K		10.5					10.5																				T		1.2																															MSP156377																																											flux method					Possible co-existence of superconductivity and weak ferromagnetism in ErNi2B2C	05		Ames Laboratory and Department of Physics and Astronomy, lowa State University, Ames, IA 50011, USA	Physica.C,262(1996)249-254	B.K. Cho,P.C. Canfield,S.L. Bud'ko	Er, Ni, B, C	
156378	PHC470S298		LaFeP(O,F)	La1Fe1P1F0.1O0.9	La	1	Fe	1	P	1	F	0.1													O	0.9		1	2010																										ABCD		oxypnictide																	Fe-1111	K	5.25						5.25																																																																																														LaAs,LaP,Fe2O3,LaF3,Fe		mixture - pellet-ANN(1000C,40h , in evacuated quartz tube)					Non-monotonic change of electronic properties by As substitution in LaFeP(O,F)			a Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan	Physica C, 470(2010)S298	S. Saijo,S. Suzuki,S. Miyasaka,S. Tajima		
156379	PHC470S298		LaFe(P,As)O0.9F0.1	La1Fe1P0.6As0.4F0.1O0.9	La	1	Fe	1	P	0.6	As	0.4	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide																	Fe-1111	K	20.86						20.86																																																																																														LaAs,LaP,Fe2O3,LaF3,Fe		mixture - pellet-ANN(1000C,40h , in evacuated quartz tube)					Non-monotonic change of electronic properties by As substitution in LaFeP(O,F)			a Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan	Physica C, 470(2010)S298	S. Saijo,S. Suzuki,S. Miyasaka,S. Tajima		
156380	PHC470S298		LaFe(P,As)O0.9F0.1	La1Fe1P0.6As0.6F0.1O0.9	La	1	Fe	1	P	0.6	As	0.6	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide																	Fe-1111	K	26.9						26.9	MTC156380																																																																																													LaAs,LaP,Fe2O3,LaF3,Fe		mixture - pellet-ANN(1000C,40h , in evacuated quartz tube)					Non-monotonic change of electronic properties by As substitution in LaFeP(O,F)			a Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan	Physica C, 470(2010)S298	S. Saijo,S. Suzuki,S. Miyasaka,S. Tajima		
156381	PHC470S298		LaFe(P,As)O0.9F0.1	La1Fe1P0.6As0.8F0.1O0.9	La	1	Fe	1	P	0.6	As	0.8	F	0.1											O	0.9		1	2010																										ABCD		oxypnictide																	Fe-1111	K	25.3						25.3																																																																																														LaAs,LaP,Fe2O3,LaF3,Fe		mixture - pellet-ANN(1000C,40h , in evacuated quartz tube)					Non-monotonic change of electronic properties by As substitution in LaFeP(O,F)			a Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan	Physica C, 470(2010)S298	S. Saijo,S. Suzuki,S. Miyasaka,S. Tajima		
156382	PHC470S298		LaFeAs(O,F)	La1Fe1As1F0.1O0.9	La	1	Fe	1	As	1	F	0.1													O	0.9		1	2010																										ABCD		oxypnictide																	Fe-1111	K	24.3						24.3																																																																																														LaAs,LaP,Fe2O3,LaF3,Fe		mixture - pellet-ANN(1000C,40h , in evacuated quartz tube)					Non-monotonic change of electronic properties by As substitution in LaFeP(O,F)			a Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan	Physica C, 470(2010)S298	S. Saijo,S. Suzuki,S. Miyasaka,S. Tajima		
156383	PHC5240024	gap=1.11 meV(2d/kTc = 4.1) from s-wavw fitting of d(penet)(T) measured by TDO. [penet] estimated from Hc1, cohere (literature data)	Nb2PdS5	Nb2Pd1S5	Nb	2	Pd	1	S	5																		1	2016																										AB2C5			C2/m		A	12.132	3.2774	15.024												K	6	6.25	6.4	6			6.25										90																															nm	Hc1,cohere,GL-eq.,	225			meV	1.11	4.1																																																solid state reaction					Single gap s-wave superconductivity in Nb2PdS5			School of Physical Sciences, JNU, New Delhi, India	Physica C, 524(2016)24	Shruti,R. Goyal,V.P.S. Awana,S. Patnaik		
156384	PHC5280012	Hirr = [(1-Tirr)/Tc(0)]^n, where n = 2.49 for H > 400 Oe.	(Hg,La)Ba2Ca3(Cu,Ag)4O10-z	Hg0.3La0.7Ba2Ca3Cu3.6Ag0.4O10-z	Hg	0.3	La	0.7	Ba	2	Ca	3	Cu	3.6	Ag	0.4									O	10-z		1	2016																										AB2C3D4E10		Hg1234																		K				121.6			121.6																																		MHC156384																																																														solid state reaction					AC susceptibility of the Hg0.3La0.7Ba2Ca3(Cu0.95Ag0.5)4O10+z superconductor			Department of Physics, Faculty of Science, University of Cairo, Giza, Egypt	Physica C, 528(2016)12	M.F. Mostafa,A Hassen		
156385	PHC5280012	Hirr = [(1-Tirr)/Tc(0)]^n, where n = 2.57 for H > 400 Oe.	(Hg,La)Ba2Ca3(Cu,Ag)4O10-z	Hg0.3La0.7Ba2Ca3Cu3.2Ag0.8O10-z	Hg	0.3	La	0.7	Ba	2	Ca	3	Cu	3.2	Ag	0.8									O	10-z		1	2016																										AB2C3D4E10		Hg1234																		K				126.8			126.8																																		MHC156384																																																														solid state reaction					AC susceptibility of the Hg0.3La0.7Ba2Ca3(Cu0.95Ag0.5)4O10+z superconductor			Department of Physics, Faculty of Science, University of Cairo, Giza, Egypt	Physica C, 528(2016)12	M.F. Mostafa,A Hassen		
156386	PHC5280012	Hirr = [(1-Tirr)/Tc(0)]^n, where n = 2.59 for H > 400 Oe.	(Hg,La)Ba2Ca3(Cu,Ag)4O10-z	Hg0.3La0.7Ba2Ca3Cu2.8Ag1.2O10-z	Hg	0.3	La	0.7	Ba	2	Ca	3	Cu	2.8	Ag	1.2									O	10-z		1	2016																										AB2C3D4E10		Hg1234																		K				126.9			126.9																																		MHC156386																																																														solid state reaction					AC susceptibility of the Hg0.3La0.7Ba2Ca3(Cu0.95Ag0.5)4O10+z superconductor			Department of Physics, Faculty of Science, University of Cairo, Giza, Egypt	Physica C, 528(2016)12	M.F. Mostafa,A Hassen		
156387	PHC5280012	Hirr = [(1-Tirr)/Tc(0)]^n, where n = 2.74 for H > 400 Oe.	(Hg,La)Ba2Ca3(Cu,Ag)4O10-z	Hg0.3La0.7Ba2Ca3Cu2Ag2O10-z	Hg	0.3	La	0.7	Ba	2	Ca	3	Cu	2	Ag	2									O	10-z		1	2016																										AB2C3D4E10		Hg1234																		K				106.7			106.7																																		MHC156386																																																														solid state reaction					AC susceptibility of the Hg0.3La0.7Ba2Ca3(Cu0.95Ag0.5)4O10+z superconductor			Department of Physics, Faculty of Science, University of Cairo, Giza, Egypt	Physica C, 528(2016)12	M.F. Mostafa,A Hassen		
156388	PHC5280023		(Bi,Co)4O4S3	Bi3.925Co0.075S3O4	Bi	3.925	Co	0.075	S	3															O	4		1	2016																										A3B4C4					A	3.9619		41.296												K	3.95		4.83				4.39																																																																							uOhm.cn	4.41																						Bi(4N),Bi2O3(4N), S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube - heat to 510C - keep(510C,10h) - cool to RT					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156389	PHC5280023	M-H curves below Tc, show coexistence of SC and FM	(Bi,Co)4O4S3	Bi3.9Co0.1S3O4	Bi	3.9	Co	0.1	S	3															O	4		1	2016																										A3B4C4					A	3.9595		41.286												K	4.96		5.5				5.23																																																																							uOhm.cn	3.1																						Bi(4N),Bi2O3(4N), S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube - heat to 510C - keep(510C,10h) - cool to RT					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156390	PHC5280023		(Bi,Co)4O4S3	Bi3.875Co0.125S3O4	Bi	3.875	Co	0.125	S	3															O	4		1	2016																										A3B4C4					A	3.9578		41.272												K	3.95		4.57				4.26																																																																							uOhm.cn	2.42																						Bi(4N),Bi2O3(4N), S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube - heat to 510C - keep(510C,10h) - cool to RT					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156391	PHC5280023		(Bi,Co)4O4S3	Bi3.85Co0.15S3O4	Bi	3.85	Co	0.15	S	3															O	4		1	2016																										A3B4C4					A	3.9571		41.265												K	3.65		4.26				3.955																																																																							uOhm.cn	1.61																						Bi(4N),Bi2O3(4N), S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube - heat to 510C - keep(510C,10h) - cool to RT					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156392	PMB0950804	decant  at 550 C. As-grown sample.   RRR = 30. not SC	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K					0.05																																																																																																		Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156393	PMB0950804	decant  at 550 C.ANN(500 C, 7days).  RRR = 36	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K		0.6					0.6																																																																																																Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156394	PMB0950804	decant  at 550 C. ANN(600 C, 10days).  RRR = 38	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K		0.9					0.9																																																																																																Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156395	PMB0950804	decant  at 550 C. ANN(800 C, 7days).  RRR = 20.  not SC	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K					0.05																																																																																																		Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156396	PMB0950804	decant  at 400 C. ANN(600 C, 7days).  RRR = 57	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K		1					1																																																																																																Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156397	PMB0950804	decant  at 300 C. ANN(600 C, 7days).  RRR = 57	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2015																										AB2C2		ThCr2Si2																		K		1.2	1.4				1.2																																																																							uOhm.cm	3.38																								Flux method (Sn-flux). mixture(Y:Fe:Ge:Sn = 1:2.4:2:95) - inAl2O3 crucible - sealed in silica ampoule heat (1190C,2h) - cool to 300 - 500 C(decant)  for 4 days.					Crystal growth and annealing study of fragile, non-bulk superconductivity in YFe2Ge2			Department of Physics & Astronomy, Iowa State University, Ames 50011, USA; bAmes Laboratory, Iowa State University, Ames 50011, USA	Phil.Magazine, 95(2015)804	"H. Kim,S. Ran,E.D. Mun,H. Hodovanets,M.A. Tanatar,R. Prozorov,S.L.. Bud'ko
,P.C. Canfield"		
156398	PPROC0810057	RRR = 3.4. not SC.	NbIrSi	Nb1Ir1Si1	Nb	1	Ir	1	Si	1																		1	2016																										ABC	3		Pnma		A	6.408	3.794	7.273												K					0.28																																																																									uOhm.cm	301																						Nb(3N),Ta(3N),Ir(3N),Pt(3N),Si(5N)		arc-melting					Superconducting and Normal State Properties in the Ternary Silicide NbIrSi, TaIrSi and NbPtSi			Graduate School of Science and Technology, Niigata University, 8050 Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	Phys.Procedia, 81(2016)57	Harufumi Suzuki,Naoki Kase,Tomohito Nakano,Naoya Takeda		
156399	PPROC0810057	RRR = 2.0.  R(T) not to zero at T=0.28 K.	TaIrSi	Ta1Ir1Si1	Ta	1	Ir	1	Si	1																		1	2016																										ABC	3		Pnma		A	6.378	3.786	7.27												K			0.5				0.5																																																																							uOhm.cm	94																						Nb(3N),Ta(3N),Ir(3N),Pt(3N),Si(5N)		arc-melting					Superconducting and Normal State Properties in the Ternary Silicide NbIrSi, TaIrSi and NbPtSi			Graduate School of Science and Technology, Niigata University, 8050 Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	Phys.Procedia, 81(2016)57	Harufumi Suzuki,Naoki Kase,Tomohito Nakano,Naoya Takeda		
156400	PPROC0810057		NbPtSi	Nb1Pt1Si1	Nb	1	Pt	1	Si	1																		1	2016																										ABC	3		Pnma		A	6.424	3.823	7.381												K		1.24	1.27			0.07	1.24																				T	R(mid), T^2 extrapolation	1.15												MHC156400		A	from Hc2	169																																	uOhm.cm	82																						Nb(3N),Ta(3N),Ir(3N),Pt(3N),Si(5N)		arc-melting					Superconducting and Normal State Properties in the Ternary Silicide NbIrSi, TaIrSi and NbPtSi			Graduate School of Science and Technology, Niigata University, 8050 Ikarashi 2-no-cho, Nishi-ku, Niigata, 950-2181, Japan	Phys.Procedia, 81(2016)57	Harufumi Suzuki,Naoki Kase,Tomohito Nakano,Naoya Takeda		
156401	PRB078064516	Tc = 4.75 K , Hc(0) = 50 mT from SP and entropy balance, kappa(GL) = 3. (dC/gamma*Tc) = 1.75.	ThPt4Ge4	Th1Pt4Ge12	Th	1	Pt	4	Ge	12																		1	2008																										AB4C12		skutterudite			A	8.5931													LaFe4Sb12-type	K		4.8					4.8																				T	SP, WHH	0.21							T/K	SP	0.064					A	Hc(0), GL theoru	4			A	Hc(0), GL theoru	12			meV	0.72	3.6	14							mJ/mol.K2	35	SP													uOhm.cm	3																								arc-melting - in quartz capsule - ANN(800C,2w)					Superconductivity and spin fluctuations in {Th,U}Pt4Ge12 skutterudites			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 78(2008)064516	E. Bauer,Xing-Qiu Chen,P. Rogl,G. Hilscher,H. Michor,E. Royanian,R. Podloucky,G. Giester,O. Sologub,A. P. Goncalves		
156402	PRB078064516	not SC.  R(T) = R0 + A*T^n (R0 = 14.5 uOhm.cm, A = 0.42 uOhm.cm/K^(-1.5), n = 1.5	UPt4Ge4	U1Pt4Ge12	U	1	Pt	4	Ge	12																		1	2008																										AB4C12		skutterudite			A	8.5887													LaFe4Sb12-type	K					1.9																																																										mJ/mol.K2	156	SP													uOhm.cm	14.5																								arc-melting - in quartz capsule - ANN(800C,2w)					Superconductivity and spin fluctuations in {Th,U}Pt4Ge12 skutterudites			Institute of Solid State Physics, Vienna University of Technology, A-1040 Wien, Austria	Phys.Rev.B, 78(2008)064516	E. Bauer,Xing-Qiu Chen,P. Rogl,G. Hilscher,H. Michor,E. Royanian,R. Podloucky,G. Giester,O. Sologub,A. P. Goncalves		
156403	PRB078024521	not SC For stoichiometric sample. SP contains Shottky type anomaly. Impure sampe contains FeP impurity ( Curie-T = 215 K)	LaFePO	La1Fe1P1O1	La	1	Fe	1	P	1															O	1		1	2008																										ABCD		oxypnictide	P4/nmm	129	A	3.96306		8.5087												K					0.35																																																										mJ/mol.K2	12.5	SP	340	SP						uV/K	-18.9			MTP156403	mOhm.cm	0.64										1.51												LaP,Fe,Fe3O4		mixture - pellet - (pellet + 5%-excess P) - alimina crucible - heat to 1200C(180C/h) - keep(48h) - cool to RT(180C/h) - reground - ( with 5%-excess P) - same heat treatment					Intrinsic properties of stoichiometric LaFePO			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 78(2008)024521	T. M. McQueen,M. Regulacio,A. J. Williams,Q. Huang,J. W. Lynn,Y. S. Hor,D. V. West,M. A. Green,R. J. Cava		
156404	PRB083184509	Thermodynamic Hc calculated from SP-data. Hc(0) = 37.0 mT.  kappa(GL) = 19.5. (dC/gamma*Tc) = 1.84.	La3Rh4Sn13	La3Rh4Sn13	La	3	Rh	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.7457														K		3.1		3.1			3.1											mT	from Hc, Hc2	2.5							T	R(mid), polynominal fn fitting	1.02												MHC156404		nm	from Hc2	18			nm	Hc(0),Hc2, GL-eq.	401			meV	0.505	3.78	14							mJ/mol.K2	22.2	SP	284	SP																																		La(3N),Sr(3N),Rh(3N),Ir(3N),Sn(5N)		Sn-flux method. starting((La or Sr):(Rh orIr):Sn = 1:1.33:10) - alumina crucible in quartz tube - heat(105C,3h) - cool to 200C (5C/h)					Superconducting state in the ternary stannide superconductors R3T4Sn13 (R = La, Sr; T = Rh, Ir) with a quasiskutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 83(2011)184509	N. Kase,H. Hayamizu,J. Akimitsu		
156405	PRB083184509	Thermodynamic Hc calculated from SP-data. Hc(0) = 37.1 mT.  kappa(GL) = 25.9. (dC/gamma*Tc) = 1.67.	La3Ir4Sn13	La3Ir4Sn13	La	3	Ir	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.755														K		2.5		2.5			2.5											mT	from Hc, Hc2	4.1							T	R(mid), polynominal fn fitting	1.02												MHC156405		nm	from Hc2	18			nm	Hc(0),Hc2, GL-eq.	509			meV	0.389	3.61	14							mJ/mol.K2	19.2	SP	296	SP																																		La(3N),Sr(3N),Rh(3N),Ir(3N),Sn(5N)		Sn-flux method. starting((La or Sr):(Rh orIr):Sn = 1:1.33:10) - alumina crucible in quartz tube - heat(105C,3h) - cool to 200C (5C/h)					Superconducting state in the ternary stannide superconductors R3T4Sn13 (R = La, Sr; T = Rh, Ir) with a quasiskutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 83(2011)184509	N. Kase,H. Hayamizu,J. Akimitsu		
156406	PRB083184509	Thermodynamic Hc calculated from SP-data. Hc(0) = 60.1 mT. kappa(GL) = 29.4. (dC/gamma*Tc) = 1.78.	Sr3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.8048														K		4.15		4.15			4.15											mT	from Hc, Hc2	4.7							T	R(mid), polynominal fn fitting	2.5												MHC156404		nm	from Hc2	11.5			nm	Hc(0),Hc2, GL-eq.	363			meV	0.692	3.87	14							mJ/mol.K2	31	SP	252	SP																																		La(3N),Sr(3N),Rh(3N),Ir(3N),Sn(5N)		Sn-flux method. starting((La or Sr):(Rh orIr):Sn = 1:1.33:10) - alumina crucible in quartz tube - heat(105C,3h) - cool to 200C (5C/h)					Superconducting state in the ternary stannide superconductors R3T4Sn13 (R = La, Sr; T = Rh, Ir) with a quasiskutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 83(2011)184509	N. Kase,H. Hayamizu,J. Akimitsu		
156407	PRB083184509	Thermodynamic Hc calculated from SP-data. Hc(0) = 78.2 mT. kappa(GL) = 32.0. (dC/gamma*Tc) = 2.09.	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2011																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n	223	A	9.8159														K		4.95		4.95			4.95											mT	from Hc, Hc2	9.7							T	R(mid), polynominal fn fitting	3.54												MHC156405		nm	from Hc2	9.65			nm	Hc(0),Hc2, GL-eq.	328			meV	0.87	4.08	14							mJ/mol.K2	39.3	SP	184	SP																																		La(3N),Sr(3N),Rh(3N),Ir(3N),Sn(5N)		Sn-flux method. starting((La or Sr):(Rh orIr):Sn = 1:1.33:10) - alumina crucible in quartz tube - heat(105C,3h) - cool to 200C (5C/h)					Superconducting state in the ternary stannide superconductors R3T4Sn13 (R = La, Sr; T = Rh, Ir) with a quasiskutterudite structure			Department of Physics and Mathematics, Aoyama-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 83(2011)184509	N. Kase,H. Hayamizu,J. Akimitsu		
156408	PRB086144526		CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		5	2012																										ABC5		HoCoGa5			A	4.6199		7.5324												K		1.95					1.95																																																																							uOhm.cm								4.91						m3/C						MRH156408					MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156409	PRB086144526		(Ce,Yb)CoIn5	Ce0.98Yb0.02Co1In5	Ce	0.98	Yb	0.02	Co	1	In	5																5	2012																										ABC5		HoCoGa5			A			7.5322												K		1.89					1.89	MTC156409																																																																						uOhm.cm								6.09						m3/C						MRH156409					MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156410	PRB086144526		(Ce,Yb)CoIn5	Ce0.95Yb0.05Co1In5	Ce	0.95	Yb	0.05	Co	1	In	5																5	2012																										ABC5		HoCoGa5			A	4.6218		7.5309												K		1.73					1.73																																																																							uOhm.cm								8.27						m3/C						MRH156410					MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156411	PRB086144526		(Ce,Yb)CoIn5	Ce0.9Yb0.1Co1In5	Ce	0.9	Yb	0.1	Co	1	In	5																5	2012																										ABC5		HoCoGa5			A	4.6186		7.5292												K		1.47					1.47																																																																							uOhm.cm								13.8						m3/C						MRH156411					MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156412	PRB086144526		(Ce,Yb)CoIn5	Ce0.85Yb0.15Co1In5	Ce	0.85	Yb	0.15	Co	1	In	5																5	2012																										ABC5		HoCoGa5			A	4.6214		7.5218												K		1.19					1.19																																																																							uOhm.cm								16.8																	MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156413	PRB086144526		(Ce,Yb)CoIn5	Ce0.8Yb0.2Co1In5	Ce	0.8	Yb	0.2	Co	1	In	5																5	2012																										ABC5		HoCoGa5			A	4.6216		7.5146												K		0.92					0.92																																																																							uOhm.cm								22.5																	MBE method. Substrate = MgF2(001). T<sub> = 530-550 C. Evap. rate = 0.01 - 0.02 nm/s. Thickness = 120 nm. Compositions by EDX.					Strong suppression of superconductivity by divalent ytterbium Kondo holes in CeCoIn5			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 86(2012)144526	M. Shimozawa,T. Watashige,S. Yasumoto,Y. Mizukami,M. Nakamura,H. Shishido,S. K. Goh,T. Terashima,T. Shibauchi,Y. Matsuda		
156414	PRB088020505		(Sn,In)Te	Sn0.8In0.2Te1	Sn	0.8	In	0.2	Te	1																		3	2013																										AB					A	6.2976														K			2.71	2.97			2.97																				T	RES(onset), WHH	1.08							T/K	RES(onset)	0.58			MHC156414																																																														poly crystal samples - set in floating zone system in 1 bar Ar.  growth velocity = 0.5-1.0 mm/h.					Optimizing the superconducting transition temperature and upper critical field of Sn1-xInxTe			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 88(2013)020505	R. D. Zhong,J. A. Schneeloch,X. Y. Shi,Z. J. Xu,C. Zhang,J. M. Tranquada,Q. Li,G. D. Gu		
156415	PRB088020505		(Sn,In)Te	Sn0.7In0.3Te1	Sn	0.7	In	0.3	Te	1																		3	2013																										AB					A	6.2887														K			3.22	3.68			3.68																				T	RES(onset), WHH	1.18							T/K	RES(onset)	0.55			MHC156414																																																														poly crystal samples - set in floating zone system in 1 bar Ar.  growth velocity = 0.5-1.0 mm/h.					Optimizing the superconducting transition temperature and upper critical field of Sn1-xInxTe			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 88(2013)020505	R. D. Zhong,J. A. Schneeloch,X. Y. Shi,Z. J. Xu,C. Zhang,J. M. Tranquada,Q. Li,G. D. Gu		
156416	PRB088020505		(Sn,In)Te	Sn0.6In0.4Te1	Sn	0.6	In	0.4	Te	1																		3	2013																										AB					A	6.2772														K			4.18	4.27			4.27	MTC156416																			T	RES(onset), WHH	1.42							T/K	RES(onset)	0.49			MHC156416																																																														poly crystal samples - set in floating zone system in 1 bar Ar.  growth velocity = 0.5-1.0 mm/h.					Optimizing the superconducting transition temperature and upper critical field of Sn1-xInxTe			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 88(2013)020505	R. D. Zhong,J. A. Schneeloch,X. Y. Shi,Z. J. Xu,C. Zhang,J. M. Tranquada,Q. Li,G. D. Gu		
156417	PRB088020505	small amount of 2nd phase by XRD	(Sn,In)Te	Sn0.55In0.45Te1	Sn	0.55	In	0.45	Te	1																		3	2013																										AB					A	6.2743														K			4.5	4.46			4.46																				T	RES(onset), WHH	1.49							T/K	RES(onset)	0.48			MHC156416																																																														poly crystal samples - set in floating zone system in 1 bar Ar.  growth velocity = 0.5-1.0 mm/h.					Optimizing the superconducting transition temperature and upper critical field of Sn1-xInxTe			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 88(2013)020505	R. D. Zhong,J. A. Schneeloch,X. Y. Shi,Z. J. Xu,C. Zhang,J. M. Tranquada,Q. Li,G. D. Gu		
156418	PRB088020505		(Sn,In)Te	Sn0.7In0.3Te1	Sn	0.7	In	0.3	Te	1																		1	2013																										AB					A	6.2875														K				3.51			3.51	MTC156418																																																																																													Sn(4N),In(4N),Te(5N)		mixture - sealed in quartz ampoule - heat (850C) - cool to RT over 24h					Optimizing the superconducting transition temperature and upper critical field of Sn1-xInxTe			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 88(2013)020505	R. D. Zhong,J. A. Schneeloch,X. Y. Shi,Z. J. Xu,C. Zhang,J. M. Tranquada,Q. Li,G. D. Gu		
156419	PRB089020505	RRR = 6. Tc(SP) = 3.72 K. Hc(0) = 57.4 mT from Hc1/Hc2. Lattice term in SP (beta) = 2.67 mJ/mol.K4.  (dC/gamma*Tc) = 1.41. e-ph = 0.74.kappa(GL) = 17. Hc2(0) = 1.47 T from Hc2=Hc2(0)(1-t^1.5)^1.5	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		1	2014																										ABC2																			layer sequence, TaSe2-Pb-TaSe2-	K		3.7	3.79	3.7		0.15	3.7											mT	M-H curve, (1-t^2) dependence	7.5							T	RES(onset), WHH	1.19							T/K	RES(onset)	0.46			MHC156419		nm	from Hc2	15			nm	calc. from Hc1	248													mJ/mol.K2	6.9	SP	112	Debye & Einstein model																																		PbSe,TaSe2.Ta		mixture(PbSe,TaSe2,Ta) - sealed in quartz tube in PbSe atmosphere - heat(800C,1w)					Noncentrosymmetric superconductor with a bulk three-dimensional Dirac cone gapped by strong spin-orbit coupling			Department of Chemistry, Princeton University, Princeton New Jersey, 08544, USA	Phys.Rev.B, 89(2014)020505	Mazhar N. Ali,Quinn D. Gibson,T. Klimczuk,R. J. Cava		
156420	PRB089140504	<195>Pt-NMR, <75>As-NQR measured. [penet] calculated from NMR fitting.. Tc(H=0.0842 T) = 1.43 K.	SrPtAs	Sr1Pt1As1	Sr	1	Pt	1	As	1																		1	2014																										ABC		KZnAs																		K		2.4					2.4																																									nm	NMR																																																				Sr,Pt,PtAs2		mixture - alumina crucible - heat(700C,3h + 1000C,24h) - reground - pellet - wrapped in Ta foil - heat(800C,2h)					Spin-singlet superconductivity with a full gap in locally noncentrosymmetric SrPtAs			Department of Physics, and Research Center of New Functional Materials for Energy Production, Storage and Transport, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 89(2014)140504	K. Matano,K. Arima,S. Maeda,Y. Nishikubo,K. Kudo,M. Nohara,Guo-qing Zheng		
156421	PRB091020507	RRR = 50.Pauli limit = 11T. (dC/gamma*Tc) = 2.2. kappa(GL) = 100. H-direction : // means H//rod direction. C/T vs T graph in Fig.4.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2015	emu/mol	0.0007			myu-B/f.u	0.36	-40																			A2B3C3		K2Cr3As3			A	9.983		4.23												K	6.1						6.1	MTC156421		K/GPa	-0.34							mT	M-T curve				7			2	T	RES(offset), WHH		534	312					T/K	RES(offset)		12	7	MHC156421																						mJ/mol.K2	73	SP,For 7<T<10 K	220																																					Matryoshika-like assembly. mixture(K:Cr:As=6:1:7) - weld into Ta tube - silica ampoule - heat to 1000C over 2 days - cool to 700C over 100h.					Anisotropic Hc2, thermodynamic and transport measurements, and pressure dependence of Tc in K2Cr3As3 single crystals			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 91(2015)020507	Tai Kong,Sergey L. Bud'ko,Paul C. Canfield		
156422	PRB089134503		LaFeAsO0.89F0.11	La1Fe1As1F0.11O0.89	La	1	Fe	1	As	1	F	0.11													O	0.89		1	2014																										ABCD		oxypnictide																		K				29			29																																																																																																See J.Phys.Soc. Jpn, 77(2008)103704					Poisoning effect of Mn in LaFe1-xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductors			Dipartimento di Fisica and Unita CNISM di Pavia, I-27100 Pavia, Italy	Phys.Rev.B, 89(2014)134503	F. Hammerath,P. Bonfa,S. Sanna,G. Prando,R. De Renzi,Y. Kobayashi,M. Sato,P. Carretta		
156423	PRB089134503		La(Fe,Mn)AsO0.89F0.11	La1Fe0.99975Mn0.00025As1F0.11O0.89	La	1	Fe	0.99975	Mn	0.00025	As	1	F	0.11											O	0.89		1	2014																										ABCD		oxypnictide																		K				25			25																																																																																																See J.Phys.Soc. Jpn, 77(2008)103704					Poisoning effect of Mn in LaFe1-xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductors			Dipartimento di Fisica and Unita CNISM di Pavia, I-27100 Pavia, Italy	Phys.Rev.B, 89(2014)134503	F. Hammerath,P. Bonfa,S. Sanna,G. Prando,R. De Renzi,Y. Kobayashi,M. Sato,P. Carretta		
156424	PRB089134503		La(Fe,Mn)AsO0.89F0.11	La1Fe0.99925Mn0.00075As1F0.11O0.89	La	1	Fe	0.99925	Mn	0.00075	As	1	F	0.11											O	0.89		1	2014																										ABCD		oxypnictide																		K				16.3			16.3	MPH156424																																																																																															See J.Phys.Soc. Jpn, 77(2008)103704					Poisoning effect of Mn in LaFe1-xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductors			Dipartimento di Fisica and Unita CNISM di Pavia, I-27100 Pavia, Italy	Phys.Rev.B, 89(2014)134503	F. Hammerath,P. Bonfa,S. Sanna,G. Prando,R. De Renzi,Y. Kobayashi,M. Sato,P. Carretta		
156425	PRB089134503	Tm(magnetic order) measured by ZF-muon-SR(zero field)	La(Fe,Mn)AsO0.89F0.11	La1Fe0.999Mn0.001As1F0.11O0.89	La	1	Fe	0.999	Mn	0.001	As	1	F	0.11											O	0.89		1	2014																										ABCD		oxypnictide																		K				11.5			11.5																																																																																																See J.Phys.Soc. Jpn, 77(2008)103704					Poisoning effect of Mn in LaFe1-xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductors			Dipartimento di Fisica and Unita CNISM di Pavia, I-27100 Pavia, Italy	Phys.Rev.B, 89(2014)134503	F. Hammerath,P. Bonfa,S. Sanna,G. Prando,R. De Renzi,Y. Kobayashi,M. Sato,P. Carretta		
156426	PRB089134503	Tm(magnetic order) measured by ZF-muon-SR(zero field)	La(Fe,Mn)AsO0.89F0.11	La1Fe0.998Mn0.002As1F0.11O0.89	La	1	Fe	0.998	Mn	0.002	As	1	F	0.11											O	0.89		1	2014																										ABCD		oxypnictide																		K					2			MPH156424																																																																																															See J.Phys.Soc. Jpn, 77(2008)103704					Poisoning effect of Mn in LaFe1-xMnxAsO0.89F0.11: Unveiling a quantum critical point in the phase diagram of iron-based superconductors			Dipartimento di Fisica and Unita CNISM di Pavia, I-27100 Pavia, Italy	Phys.Rev.B, 89(2014)134503	F. Hammerath,P. Bonfa,S. Sanna,G. Prando,R. De Renzi,Y. Kobayashi,M. Sato,P. Carretta		
156427	PRB091214517	Structural data at 6.76 K.  (dC/gamma*Tc) = 1.95. e-ph = 0.58. DOS = 0.6 states/eV.f.u.from [gamma.]	Au2Pb	Au2Pb1	Au	2	Pb	1																				3	2015																										AB2			Pbnc		A	7.904	5.5786	11.1905											data at T=6.76 K. RT-structure is cubic Laves	K			1.3				1.3																				T	RES(on), WHH	0.083							T/K	RES(on)	0.0928					A	from Hc2	629																		mJ/mol.K2	2.2	SP , For 1.3<T<2.5 K	139.6	SP																																				crystals grown by Pb-flux method					Dirac metal to topological metal transition at a structural phase change in Au2Pb and prediction of Z2 topology for the superconductor			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 91(2015)214517	Leslie M. Schoop,Lilia S. Xie,Ru Chen,Quinn D. Gibson,Saul H. Lapidus,Itamar Kimchi,Max Hirschberger,Neel Haldolaarachchige,Mazhar N. Ali,Carina A. Belvin,Tian Liang,Jeffrey B. Neaton,N. P. Ong,Ashvin Vishwanath,R. J. Cava		
156428	PRB091220502	needle-like crystals. T(sus, mid) = 5.6 K. d-[penet] measured by tunnel diode oscilator(TDO). penet(0) calculated using Hc2(0) = 31.2 T and gamma = 73 mJ/mol.K2.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		1	2015																										A2B3C3		K2Cr3As3																		K				6.1			6.1																																									nm	Hc2(0), gamma	646																																																					solid state reaction					Evidence for nodal superconductivity in quasi-one-dimensional K2Cr3As3			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China and Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China	Phys.Rev.B, 91(2015)220502	G. M. Pang,M. Smidman,W. B. Jiang,J. K. Bao,Z. F. Weng,Y. F. Wang,L. Jiao,J. L. Zhang,G. H. Cao,H. Q. Yuan		
156429	PRX005011013	R(T)= R0 + A*T, where R0 = 0.195 mOhm.cm, A=0.0067 mOhm,cm/K.  (dC/gamma*Tc) = 2.4. Hc2(0) = 44 T for linear approx.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		1	2015																										A2B3C3	7	K2Cr3As3	P6[-]m2	187	A	9.9832		4.2304											hexagonal	K				6.1			6.1										100										T	RES(0.9Rn), WHH	32							T/K	RES(0.9Rn)	7.43			MHC156429																			MSP156429			mJ/mol.K2	75	SP	218	SP											mOhm.cm							0.216				2.22														mixture(CrAs + KAs, K:Cr:As = 6:1:7) - alumina crucible - Ta tube - sealed in quartz tube - heat (1273K, 24h) - cool to 923K (2K/h)					Superconductivity in Quasi-One-Dimensional K2Cr3As3 with Significant Electron Correlations			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.X., 5(2015)011013	Jin-Ke Bao,Ji-Yong Liu,Cong-Wei Ma,Zhi-Hao Meng,Zhang-Tu Tang,Yun-Lei Sun,Hui-Fei Zhai,Hao Jiang,Hua Bai,Chun-Mu Feng,Chun-Mu Feng,Guang-Han Cao		
156430	PRB092134505	effective mass m*=1.75 me, carrier n, [penet], are estimated from muSR measurement. d-wave SC.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		1	2015																										A2B3C3	7	K2Cr3As3	P6[-]m2	187																K				5.8			5.8										100																															nm	muSR	432					6.4	16																																											n/m3	2700000000000000000000000000			See Phys.Rev.X5 (2015)011013					Superconducting ground state of quasi-one-dimensional K2Cr3As3 investigated using myu-on-SR measurements			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom	Phys.Rev.B, 92(2015)134505	D. T. Adroja,A. Bhattacharyya,M. Telling,Yu. Feng,M. Smidman,B. Pan,J. Zhao,A. D. Hillier,F. L. Pratt,A. M. Strydom		
156431	PRL109157001	Impurity: YAs. Small amount of H added to stabilize homogeneous samples. nominal O-content = 0.75-0.8. <75>As-NMR measured. multiple fully gapped SC.	(Y,La)FeAsO1-z	Y0.95La0.05Fe1As1H0.15O1-z	Y	0.95	La	0.05	Fe	1	As	1	H	0.15											O	1-z		1	2012																												oxypnictide			A	3.863		8.337											Fe-1111, or La-1111	K				50			50																																																																																																High-pressure synthesis					High-Tc Nodeless s<+-> -wave Superconductivity in (Y,La)FeAsO1-y with Tc = 50 K: <75>As-NMR Study			Graduate School of Engineering Science, Osaka University, Osaka 560-8531, Japan	Phys.Rev.Lett., 109(2012)157001	H. Mukuda,S. Furukawa,H. Kinouchi,M. Yashima,Y. Kitaoka,P. M. Shirage,H. Eisaki,A. Iyo		
156432	PRL111087001	Topological insulator. P = 5.5 GPa. not SC	Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2013																										A2B3			R-3m																	K					0																																																																																														n/cm3	24000000000000000000			Modified Bridgman method using excess Se.					Pressure-Induced Unconventional Superconducting Phase in the Topological Insulator Bi2Se3			Department of Physics, Center for Nanophysics and Advanced Materials, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.Lett., 111(2013)087001	Kevin Kirshenbaum,P. S. Syers,A. P. Hope,N. P. Butch,J. R. Jeffries,S. T. Weir,J. J. Hamlin,M. B. Maple,Y. K. Vohra,J. Paglione		
156433	PRL111087001	Topological SC. SC-properties at P = 20.8 GPa.	Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2013																										A2B3			C2/m																monoclinic	K		2.42			0		2.42																				T	RES(mid), WHH			2.28										MHC156433																																																									MRH156433	n/cm3	1680000000000000000000			Modified Bridgman method using excess Se.					Pressure-Induced Unconventional Superconducting Phase in the Topological Insulator Bi2Se3			Department of Physics, Center for Nanophysics and Advanced Materials, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.Lett., 111(2013)087001	Kevin Kirshenbaum,P. S. Syers,A. P. Hope,N. P. Butch,J. R. Jeffries,S. T. Weir,J. J. Hamlin,M. B. Maple,Y. K. Vohra,J. Paglione		
156434	PRL111087001	Topological SC. SC-properties at P = 34.4 GPa.	Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2013																										A2B3			C2/m																bcc-like	K		6.86			0		6.86	MTC156434																			T	RES(mid), WHH			3.84																																																																				n/cm3	21400000000000000000000			Modified Bridgman method using excess Se.					Pressure-Induced Unconventional Superconducting Phase in the Topological Insulator Bi2Se3			Department of Physics, Center for Nanophysics and Advanced Materials, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.Lett., 111(2013)087001	Kevin Kirshenbaum,P. S. Syers,A. P. Hope,N. P. Butch,J. R. Jeffries,S. T. Weir,J. J. Hamlin,M. B. Maple,Y. K. Vohra,J. Paglione		
156435	PRL111087001	Topological SC. SC-properties at P = 50.1 GPa.	Bi2Se3	Bi2Se3	Bi	2	Se	3																				3	2013																										A2B3			C2/m																bcc-like	K		7.01			0		7.01																				T	RES(mid), WHH			3.38										MHC156435																																																										n/cm3	26000000000000000000000			Modified Bridgman method using excess Se.					Pressure-Induced Unconventional Superconducting Phase in the Topological Insulator Bi2Se3			Department of Physics, Center for Nanophysics and Advanced Materials, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.Lett., 111(2013)087001	Kevin Kirshenbaum,P. S. Syers,A. P. Hope,N. P. Butch,J. R. Jeffries,S. T. Weir,J. J. Hamlin,M. B. Maple,Y. K. Vohra,J. Paglione		
156436	PSSL0080928	RRR = 41. Hc2(0) = 1.7 T from extrapolation. Polycrystals with RRR=30-50, show fully SC transitions.	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		1	2014																										AB2C2		ThCr2Si2			A	3.964		10.457												K		1.4	1.8	1.5			1.4										80										T	WHH	2.8							T/K	RES(on)	2.4			MHC156436		A	from Hc2	108															MSP156436																																									Y(3N),Fe(4N),Ge(6N)		mixture - melt in water cooled Cu-boat - ANN(800C,7 days)					Fermi liquid breakdown and evidence for superconductivity in YFe2Ge2			Cavendish Laboratory, University of Cambridge, J. J. Thomson Ave, Cambridge CB3 0HE, UK	Phys.Status Solidi RRL, 8(2014)928	Y. Zou,Z. Feng,P. W. Logg,J. Chen,G. Lampronti,F. M. Grosche		
156437	SCIR0032016	Topological insulator, not SC SC-critical P = 4 GPa.	Sb2Te3	Sb2Te3	Sb	2	Te	3																				3	2013																										A2B3			R-3m		A	4.3225		30.8679												K					1.5																																																																																																Sb(5N).Te(5N)		mixture - press into pills - quartz Bridgman ampoule - heat(800C,3d) - cool to 300C with 5C/h					Superconductivity in Topological Insulator Sb2Te3 Induced by Pressure			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Sci. Rep., 3(2013)2016	J. Zhu,J. L. Zhang,P. P. Kong,S. J. Zhang,X. H. Yu1,J. L. Zhu1,Q. Q. Liu,X. Li,R. C. Yu,R. Ahuja,W.G. Yang,G. Y. Shen,H. K.Mao,H.M. Weng,X. Dai,Z. Fang,Y. S. Zhao,C.Q. Jin		
156438	SCIR0032016	P = 6.7 GPa. P-induced  SC. carrier conc. shows at 218 K.	Sb2Te3	Sb2Te3	Sb	2	Te	3																				3	2013																										A2B3			R-3m		A	4.1143		29.17												K		4.3			1.5		4.3	MTC156438		K/GPa	0.45																T	RES(on), WHH			2.6										MHC156438																																																										n/cm3	1380000000000000000000	Sb(5N).Te(5N)		mixture - press into pills - quartz Bridgman ampoule - heat(800C,3d) - cool to 300C with 5C/h					Superconductivity in Topological Insulator Sb2Te3 Induced by Pressure			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Sci. Rep., 3(2013)2016	J. Zhu,J. L. Zhang,P. P. Kong,S. J. Zhang,X. H. Yu1,J. L. Zhu1,Q. Q. Liu,X. Li,R. C. Yu,R. Ahuja,W.G. Yang,G. Y. Shen,H. K.Mao,H.M. Weng,X. Dai,Z. Fang,Y. S. Zhao,C.Q. Jin		
156439	SCIR0032016	P = 8.6 GPa. P-induced SC.	Sb2Te3	Sb2Te3	Sb	2	Te	3																				3	2013																										A2B3			R-3m																	K		6.2			1.5		6.2																																																																																														Sb(5N).Te(5N)		mixture - press into pills - quartz Bridgman ampoule - heat(800C,3d) - cool to 300C with 5C/h					Superconductivity in Topological Insulator Sb2Te3 Induced by Pressure			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Sci. Rep., 3(2013)2016	J. Zhu,J. L. Zhang,P. P. Kong,S. J. Zhang,X. H. Yu1,J. L. Zhu1,Q. Q. Liu,X. Li,R. C. Yu,R. Ahuja,W.G. Yang,G. Y. Shen,H. K.Mao,H.M. Weng,X. Dai,Z. Fang,Y. S. Zhao,C.Q. Jin		
156440	SCIR0032016	P = 19.6 GPa. P-induced SC.	Sb2Te3	Sb2Te3	Sb	2	Te	3																				3	2013																										A2B3			C2/m																	K		6.97			1.5		6.97	MTC156440																																																																																													Sb(5N).Te(5N)		mixture - press into pills - quartz Bridgman ampoule - heat(800C,3d) - cool to 300C with 5C/h					Superconductivity in Topological Insulator Sb2Te3 Induced by Pressure			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Sci. Rep., 3(2013)2016	J. Zhu,J. L. Zhang,P. P. Kong,S. J. Zhang,X. H. Yu1,J. L. Zhu1,Q. Q. Liu,X. Li,R. C. Yu,R. Ahuja,W.G. Yang,G. Y. Shen,H. K.Mao,H.M. Weng,X. Dai,Z. Fang,Y. S. Zhao,C.Q. Jin		
156441	SCIR0032016	P = 30.6 GPa. P-induced SC.	Sb2Te3	Sb2Te3	Sb	2	Te	3																				3	2013																										A2B3			Im-3m																	K		7.24			1.5		7.24																																																																																														Sb(5N).Te(5N)		mixture - press into pills - quartz Bridgman ampoule - heat(800C,3d) - cool to 300C with 5C/h					Superconductivity in Topological Insulator Sb2Te3 Induced by Pressure			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China,	Sci. Rep., 3(2013)2016	J. Zhu,J. L. Zhang,P. P. Kong,S. J. Zhang,X. H. Yu1,J. L. Zhu1,Q. Q. Liu,X. Li,R. C. Yu,R. Ahuja,W.G. Yang,G. Y. Shen,H. K.Mao,H.M. Weng,X. Dai,Z. Fang,Y. S. Zhao,C.Q. Jin		
156442	SCM0580016	R(T) = 0.657 + 0.00524*T(mOhm.cm).  Hp = 4.0 T. SC-vol = 6%(T=1.9K), Lattice term in SP (beta) = 3.8 mJ/mol.K4	Cs2Cr3As3	Cs2Cr3As3	Cs	2	Cr	3	As	3																		1	2015	emu/mol	0.002			myu-B/Cr	0.14	-5.5																			A2B3C3		K2Cr3As3	P6[-]m2	187	A	10.605		4.2478												K			2.2				2.2																				T	RES(on),GL-fitting	6.45			6			0.44						MHC156442																			MSP156442			mJ/mol.K2	39	SP	160	SP																																		Cs,Cr,As		solid state reaction. mixture(with 3%-excess of Cs) - sealed in quartz ampoule - homogenize(423K,15h) - pellet - sealed in Ta tube) - heat(973K,24h)					Superconductivity in quasi-one-dimensional Cs2Cr3As3 with large interchain distance			Department of Physics, Zhejiang University, Hangzhou 310027, China	Sci.China Mater., 58(2015)16	Zhang-Tu Tang,Jin-Ke Bao,Zhen Wang,Hua Bai,Hao Jiang,Yi Liu,Hui-Fei Zhai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
156443	SNM0283173	Tc(onset) = 3.75 K. Upward curvature of Hc2(T) fitting by modified two band calculation.	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		1	2015																										ABC2																				K	3.26	3.38	3.53				3.38	MTC156443																			T	RES(0.9Rn), two band fitting	3.05												MHC156443																																uV/K	-6.44			MTP156443																										solid state reaction. See Phys.Rev.B 89(2014)020505					Upward Curvature of the Upper Critical Field and the V-Shaped Pressure Dependence of Tc in the Noncentrosymmetric Superconductor PbTaSe2			Department of Physics and Hangzhou Key Laboratory of Quantum Matters, Hangzhou Normal University, Hangzhou 310036, China	J.Supercond.Nov.Magn., 28(2015)3173	JianruiWang,Xiaofeng Xu,Nan Zhou,Lin Li,Xiaozhi Cao,Jinhu Yang,Yuke Li,Chao Cao,Jianhui Dai,Jinglei Zhang,Zhixiang Shi,Bin Chen,Zhihua Yang		
156444	SSC2230040		Nd(O,F)Bi1-xPbxS2	Nd1Bi0.99Pb0.01S2F0.3O0.7	Nd	1	Bi	0.99	Pb	0.01	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A			13.53											BiS2 layered SC	K				4.85			4.85																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156445	SSC2230040	R(T) = R(0) + A*T^n, where R(0) = 0.049 mOhm.cm, A=1.20E-4, n=0.98	Nd(O,F)Bi1-xPbxS2	Nd1Bi0.98Pb0.02S2F0.3O0.7	Nd	1	Bi	0.98	Pb	0.02	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A	3.9732		13.5219											BiS2 layered SC	K	5.27		5.62	5.17			5.17																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156446	SSC2230040		Nd(O,F)Bi1-xPbxS2	Nd1Bi0.97Pb0.03S2F0.3O0.7	Nd	1	Bi	0.97	Pb	0.03	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A			13.5168											BiS2 layered SC	K				5.37			5.37																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156447	SSC2230040	R(T) = R(0) + A*T^n, where R(0) = 0.173 mOhm.cm, A = 0.94E-4, n = 1.15	Nd(O,F)Bi1-xPbxS2	Nd1Bi0.96Pb0.04S2F0.3O0.7	Nd	1	Bi	0.96	Pb	0.04	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A	3.9742		13.5123											BiS2 layered SC	K	5.4		5.98	5.35			5.35																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156448	SSC2230040	R(T) = R(0) + A*T^n, where R(0) = 0.431 mOhm.cm, A = 1.76E-4, n = 1.27	Nd(O,F)Bi1-xPbxS2	Nd1Bi0.94Pb0.06S2F0.3O0.7	Nd	1	Bi	0.94	Pb	0.06	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A	3.9757		13.5038											BiS2 layered SC	K	5.65		6	5.56			5.56	MTC156448																																																																																													Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156449	SSC2230040	R(T) = R(0) + A*T^n, where R(0) = 0.3.5 mOhm.cm, A = 1.08E-4, n = 1.28	Nd(O,F)Bi1-xPbxS2	Nd1Bi0.9Pb0.1S2F0.3O0.7	Nd	1	Bi	0.9	Pb	0.1	S	2	F	0.3											O	0.7		3	2015																													P4/nmm		A	3.9797		13.5008											BiS2 layered SC	K	5.85		5.52	4.83			4.83																																																																																														Bi,Bi2S3,Bi2O3,BiF3,Nd2S3,PbO		Crystals grown by CsCl-flux method. Nominal mixture mixed with CsCl powder - sealed in quartz tube - heat(800C,10h) - cool to 630C,0.5 or 1.0 C/h - remove the flux.					Enhancement of Tc in BiS2-based superconductors NdO0.7F0.3BiS2  by substitution of Pb for Bi			Tokyo University of Science, Department of Physics, Kagurazaka, Shinjyuku-ku, Tokyo 162-8601, Japan	Solid State Commun., 223(2015)40	S. Demura,Y.Fujisawa,S.Otsuki,R.Ishio,Y.Takano,H.Sakata		
156450	SSC2420006	impurity phases: BiNi, Bi	Bi3Ni	Bi3Ni1	Bi	3	Ni	1																				1	2016																										AB3		CaLiSi2	Pnma		A	8.8832	4.0997	11.4839												K				4.05			4.05										83	Oe	M-H curve				50			3																																																																											Bi,Ni,Fe		mixture - sealed in quartz tube - heat(1000C,24h) - slow cool to RT					Superconductivity and magnetism in intermetallic Bi3Ni1-xFex  superconductor			Departamento de Fisica, Universidade Estadual de Ponta Grossa, Av. Gen. Carlos Cavalcanti 4748, 84.030-000, Ponta Grossa, Parana, Brazil	Solid State Commun., 242(2016)6	Silvio Henrique Gonsalves,Yuri Aparecido Opata,Pinheiro,Da Silva Leal,Monteiro,Siqueira,Andrade,Alcione Roberto Jurelo		
156451	SSC2420006	impurity phases: BiNi, Bi	Bi3Ni1-xFex	Bi3Ni0.95Fe0.05	Bi	3	Ni	0.95	Fe	0.05																		1	2016																										AB3		CaLiSi2	Pnma		A	8.8819	4.1002	11.483												K				4.08			4.08																																																																																														Bi,Ni,Fe		mixture - sealed in quartz tube - heat(1000C,24h) - slow cool to RT					Superconductivity and magnetism in intermetallic Bi3Ni1-xFex  superconductor			Departamento de Fisica, Universidade Estadual de Ponta Grossa, Av. Gen. Carlos Cavalcanti 4748, 84.030-000, Ponta Grossa, Parana, Brazil	Solid State Commun., 242(2016)6	Silvio Henrique Gonsalves,Yuri Aparecido Opata,Pinheiro,Da Silva Leal,Monteiro,Siqueira,Andrade,Alcione Roberto Jurelo		
156452	SSC2420006	impurity phases: BiNi, Bi. At 4K, M-H curve shows FM behavior (M = 0.08 emu/g)	Bi3Ni1-xFex	Bi3Ni0.9Fe0.1	Bi	3	Ni	0.9	Fe	0.1																		1	2016																										AB3		CaLiSi2	Pnma		A	8.8837	4.10283	11.4876												K				4.06			4.06										79																																																																																				Bi,Ni,Fe		mixture - sealed in quartz tube - heat(1000C,24h) - slow cool to RT					Superconductivity and magnetism in intermetallic Bi3Ni1-xFex  superconductor			Departamento de Fisica, Universidade Estadual de Ponta Grossa, Av. Gen. Carlos Cavalcanti 4748, 84.030-000, Ponta Grossa, Parana, Brazil	Solid State Commun., 242(2016)6	Silvio Henrique Gonsalves,Yuri Aparecido Opata,Pinheiro,Da Silva Leal,Monteiro,Siqueira,Andrade,Alcione Roberto Jurelo		
156453	SST025112001	single crystal. Tc by specific heat. [penet] measured by magnetic force microscopy MFM.	Ba(Fe,Co)2As2	Ba1Fe1.84Co0.16As2	Ba	1	Fe	1.84	Co	0.16	As	2																3	2012																										AB2C2		ThCr2Si2																		K		22					22																																									nm	MFM	310																																																					FeAs-flux method					Direct measurement of the magnetic penetration depth by magnetic force microscopy			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Supercond.Sci.Technol., 25(2012)112001	Jeehoon Kim,L Civale,E Nazaretski,N Haberkorn,F Ronning,A S Sefat,T Tajima,B H Moeckly,J D Thompson,R Movshovich		
156454	SST025112001	film, d = 300nm. [penet] measured by magnetic force microscopy MFM.	Nb	Nb1	Nb	1																						4	2012																										A																				K	8.8						8.8																																									nm	MFM	110																																																					electron beam deposition					Direct measurement of the magnetic penetration depth by magnetic force microscopy			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Supercond.Sci.Technol., 25(2012)112001	Jeehoon Kim,L Civale,E Nazaretski,N Haberkorn,F Ronning,A S Sefat,T Tajima,B H Moeckly,J D Thompson,R Movshovich		
156455	SST025112001	Film, d = 500nm. [penet] measured by magnetic force microscopy MFM.	MgB2	B2Mg1	B	2	Mg	1																				4	2012																										AB2		AlB2																		K	38.3						38.3																																									nm	MFM	200																																																					reactive evaporation					Direct measurement of the magnetic penetration depth by magnetic force microscopy			Los Alamos National Laboratory, Los Alamos, NM 87545, USA	Supercond.Sci.Technol., 25(2012)112001	Jeehoon Kim,L Civale,E Nazaretski,N Haberkorn,F Ronning,A S Sefat,T Tajima,B H Moeckly,J D Thompson,R Movshovich		
156456	PRB093104508	M = NH3, intercalated materials which can be assigned to the on-center structure.	(NH3)yCsxFeSe	M0.37Cs0.268Fe1Se1	M	0.37	Cs	0.268	Fe	1	Se	1																	2016																													I4/mmm		A	3.8272		16.243											At 30 K, a=3.8082,  c=16.2442 A.	K		33.5	35	33.5			33.5	MTC156456									25																																																																																						Using Liq.-NH3 technique with nominal x = 0.4 in (NH3)yCsxFeAs					Correlation of superconductivity with crystal structure in (NH3)yCsxFeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 93(2016)104508	Lu Zheng,Xiao Miao,Yusuke Sakai,Hidenori Goto,Eri Uesugi,Ritsuko Eguchi,Saki Nishiyama,Kunihisa Sugimoto,Akihiko Fujiwara,Yoshihiro Kubozono		
156500	PRB093104522	Dielectric const, and optical conduct. are measured for THz E-field //ab. T<IM>= 90 K (I-M transition defined as isosbestic point ). T<gap> = 61 K (means gap appears).	Rb0.75Fe1.6(Se,S)2	Rb0.75Fe1.6Se2	Rb	0.75	Fe	1.6	Se	2																		3	2016																										AB2C2		ThCr2Si2																		K		32					32																																																																																																single crystals grown by Bridgman method					Tuning orbital-selective correlations in superconducting Rb0.75Fe1.6Se2-zSz			Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B, 93(2016)104522	Zhe Wang,V. Tsurkan,M. Schmidt,A. Loidl,J. Deisenhofer		
156501	PRB093104522	Dielectric const, and optical conduct. are measured for THz E-field //ab. T<IM>= 80 K (I-M transition defined as isosbestic point ). T<gap> = 24 K (means gap appears).	Rb0.75Fe1.6(Se,S)2	Rb0.75Fe1.6Se1.75S0.25	Rb	0.75	Fe	1.6	Se	1.75	S	0.25																3	2016																										AB2C2		ThCr2Si2																		K		24					24																																																																																																single crystals grown by Bridgman method					Tuning orbital-selective correlations in superconducting Rb0.75Fe1.6Se2-zSz			Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B, 93(2016)104522	Zhe Wang,V. Tsurkan,M. Schmidt,A. Loidl,J. Deisenhofer		
156502	PRB093104522	Dielectric const, and optical conduct. are measured for THz E-field //ab. T<IM>= 105 K (I-M transition defined as isosbestic point ). T<gap> = 28 K (means gap appears).	Rb0.75Fe1.6(Se,S)2	Rb0.75Fe1.6Se1.5S0.5	Rb	0.75	Fe	1.6	Se	1.5	S	0.5																3	2016																										AB2C2		ThCr2Si2																		K		28					28	MTC156502																																																																																															single crystals grown by Bridgman method					Tuning orbital-selective correlations in superconducting Rb0.75Fe1.6Se2-zSz			Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B, 93(2016)104522	Zhe Wang,V. Tsurkan,M. Schmidt,A. Loidl,J. Deisenhofer		
156503	PRB093104522	Dielectric const, and optical conduct. are measured for THz E-field //ab. T<IM>= 120 K (I-M transition defined as isosbestic point ). T<gap> = 22 K (means gap appears).	Rb0.75Fe1.6(Se,S)2	Rb0.75Fe1.6Se1S1	Rb	0.75	Fe	1.6	Se	1	S	1																3	2016																										AB2C2		ThCr2Si2																		K		22					22																																																																																																single crystals grown by Bridgman method					Tuning orbital-selective correlations in superconducting Rb0.75Fe1.6Se2-zSz			Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B, 93(2016)104522	Zhe Wang,V. Tsurkan,M. Schmidt,A. Loidl,J. Deisenhofer		
156504	PRB093104522	Dielectric const, and optical conduct. are measured for THz E-field //ab. T<IM>= 170 K (I-M transition defined as isosbestic point ).	Rb0.75Fe1.6(Se,S)2	Rb0.75Fe1.6Se0.6S1.4	Rb	0.75	Fe	1.6	Se	0.6	S	1.4																3	2016																										AB2C2		ThCr2Si2																		K					8																																																																																																		single crystals grown by Bridgman method					Tuning orbital-selective correlations in superconducting Rb0.75Fe1.6Se2-zSz			Experimental Physics V, Center for Electronic Correlations and Magnetism, Institute of Physics, University of Augsburg, D-86135 Augsburg, Germany	Phys.Rev.B, 93(2016)104522	Zhe Wang,V. Tsurkan,M. Schmidt,A. Loidl,J. Deisenhofer		
156505	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.866		12.817											CaK-1144	K			33.4	33.1			33.1																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156506	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	CaRbFe4As4	Ca1Rb1Fe4As4	Ca	1	Rb	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.8757		13.104											CaRb-1144	K			34.6	35			35																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156507	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	CaCsFe4As4	Ca1Cs1Fe4As4	Ca	1	Cs	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.891		13.414											CaCs-1144	K			32	31.6			31.6																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156508	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	SrRbFe4As4	Sr1Rb1Fe4As4	Sr	1	Rb	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.897		13.417											SrRb-1144	K			35.7	35.1			35.1																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156509	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	SrCsFe4As4	Sr1Cs1Fe4As4	Sr	1	Cs	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.91		13.729											SrCs-1144	K			37	36.8			36.8																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156510	ACS1383410	Conditions for CaRb-1144 phase formation discussed.	BaCsFe4As4	Ba1Cs1Fe4As4	Ba	1	Cs	1	Fe	4	As	4																1	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.927		14.136											BaCs-1144	K				26			26																																																																																														(Ca,Sr)As,(K,Rb,Cs)As,FeAs,Fe2As		starting materials - ground - pellet - placed in SUS pipe - sealed with caps - heat(860-920C, 2-6h) - rapid cool to RT. Repeat process with addition of excess As (15-20 at.%)					New-Structure-Type Fe-Based Superconductors: CaAFe4As4 (A = K, Rb, Cs) and SrAFe4As4 (A = Rb, Cs)			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 138(2016)3410	Akira Iyo,Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida		
156511	APA0310201	prepared by sintering at T < 1200C, LT phase	TiRuP	Ti1Ru1P1	Ti	1	Ru	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.303		3.567												K		1.3					1.3																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156512	APA0310201	prepared by arc melting. HT phase	TiRuP	Ti1Ru1P1	Ti	1	Ru	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.325		3.542												K		1.3					1.3																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156513	APA0310201	prepared by sintering at T < 1250C LT phase	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.426		3.856												K		3.89					3.89																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156514	APA0310201	prepared by arc melting.  HT phase	ZrRuP	Zr1Ru1P1	Zr	1	Ru	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.459		3.778												K		12.93					12.93																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156515	APA0310201	prepared by sintering at T > 1250C	HfRuP	Hf1Ru1P1	Hf	1	Ru	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.414		3.753												K		10.8					10.8																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156516	APA0310201	prepared by sintering at T = 1250C	TiOsP	Ti1Os1P1	Ti	1	Os	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.285		3.625												K					0.35																																																																																																							The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156517	APA0310201	prepared by sintering at T < 1200C. LT phase	ZrOsP	Zr1Os1P1	Zr	1	Os	1	P	1																		1	1983																										ABC	3	TiNiSi	Pnma	62	A	6.432	3.895	7.327												K					0.35																																																																																																							The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156518	APA0310201	prepared by sintering at T > 1200C. HT phase	ZrOsP	Zr1Os1P1	Zr	1	Os	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.46		3.842												K		7.4					7.4																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156519	APA0310201	prepared by sintering at T = 1000C	HfOsP	Hf1Os1P1	Hf	1	Os	1	P	1																		1	1983																										ABC	2	ZrRuSi			A	6.417		3.792												K		6.1					6.1																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156520	APA0310201	prepared by sintering at T = 900C	TiRuAs	Ti1Ru1As1	Ti	1	Ru	1	As	1																		1	1983																										ABC	3	TiFeSi			A	7.287	11.227	6.515												K					0.35																																																																																																							The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156521	APA0310201	prepared by Cu-flux method.	ZrRuAs	Zr1Ru1As1	Zr	1	Ru	1	As	1																		1	1983																										ABC	2	ZrRuSi			A	6.624		3.823												K		3.2					3.2																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156522	APA0310201	prepared by sintering at T = 900C	ZrRuAs	Zr1Ru1As1	Zr	1	Ru	1	As	1																		1	1983																										ABC	2	ZrRuSi			A	6.586		3.891												K		11.9					11.9																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156523	APA0310201	prepared by sintering at T < 1000C LT phase	HfRuAs	Hf1Ru1As1	Hf	1	Ru	1	As	1																		1	1983																										ABC	3	TiFeSi			A	7.527	11.416	6.631												K					1																																																																																																							The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156524	APA0310201	prepared by sintering at T > 1000C HT phase	HfRuAs	Hf1Ru1As1	Hf	1	Ru	1	As	1																		1	1983																										ABC	2	ZrRuSi			A	6.568		3.842												K		4.93					4.93																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156525	APA0310201	TiOsAs<2/3>P<1/3>	TiOs(As,P)	Ti1Os1As0.67P0.33	Ti	1	Os	1	As	0.67	P	0.33																1	1983																										ABC	2	ZrRuSi			A	6.366		3.574												K					1																																																																																																							The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156526	APA0310201	prepared by sintering at T = 1200C	ZrOsAs	Zr1Os1As1	Zr	1	Os	1	As	1																		1	1983																										ABC	2	ZrRuSi			A	6.602		3.794												K		8					8																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156527	APA0310201	prepared by sintering at T = 1200C	HfOsAs	Zr1Hf1As1	Zr	1	Hf	1	As	1																		1	1983																										ABC	2	ZrRuSi			A	6.569		3.808												K		3.2					3.2																																																																																																					The Superconductivity and Structure of Equiatomic Ternary Transition Metal Pnictides			Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	Appl.Phys. A, 31(1983)201	G. P. Meisner,H. C. Ku		
156528	APE008023102		Bi2(O,F)S2	Bi2F0.6S2O0.4	Bi	2	F	0.6	S	2															O	0.4		1	2015																										AB2C2					A	3.969		13.729												K				5.1			5.1																																																																		uV/K	-33.2			MTP156528																										Topotactic reaction. Bi2OS2 + (x/2)XeFe2 = Bi2(O1-xFx)S2 + (x/2)Xe + (x/2)O2 at 400C for 72 h.					Topotactic synthesis of a new BiS2-based superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys. Express, 8(2015)023102	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio		
156529	APE008023102		Bi2(O,F)S2	Bi2F0.2S2O0.8	Bi	2	F	0.2	S	2															O	0.8		1	2015																										AB2C2					A	3.964		13.761												K				3			3																																																																																																Topotactic reaction. Bi2OS2 + (x/2)XeFe2 = Bi2(O1-xFx)S2 + (x/2)Xe + (x/2)O2 at 400C for 72 h.					Topotactic synthesis of a new BiS2-based superconductor Bi2(O,F)S2			Department of Applied Chemistry, The University of Tokyo, Bunkyo, Tokyo 113-8656, Japan	Appl.Phys. Express, 8(2015)023102	Tomoyuki Okada,Hiraku Ogino,Jun-ichi Shimoyama,Kohji Kishio		
156530	ASS3800237	impurity phase:CuO. small grain size, growth direction along a-axis. coercive force = 48.8 Oe at 300K	Cu(Cr,Fe)O2	Cu1Cr0.95Fe0.05O2	Cu	1	Cr	0.95	Fe	0.05															O	2			2016																										ABC2					A	2.976		17.103											delafossite structure	K	97		138				117.5																																																																							Ohm.cm											38														materials prepared using a self-combustion urea process. small					Characterization of transparent superconductivity Fe-doped CuCrO2 delafossite oxide			Materials Science and Nanotechnology Program, Faculty of Science, Khon Kaen University, Khon Kaen 40002, Thailand	Appl.Surface Sci., 380(2016)237	Chutirat Taddee,Teerasak Kamwanna,Vittaya Amornkitbamrung		
156531	ASS3800237	impurity phase:CuO. small grain size, growth direction along a-axis. coercive force = 72.5 Oe at 300K	Cu(Cr,Fe)O2	Cu1Cr0.9Fe0.1O2	Cu	1	Cr	0.9	Fe	0.1															O	2			2016																										ABC2					A	2.981		17.111											delafossite structure	K	89		107				98																																																																							Ohm.cm											24														materials prepared using a self-combustion urea process. small					Characterization of transparent superconductivity Fe-doped CuCrO2 delafossite oxide			Materials Science and Nanotechnology Program, Faculty of Science, Khon Kaen University, Khon Kaen 40002, Thailand	Appl.Surface Sci., 380(2016)237	Chutirat Taddee,Teerasak Kamwanna,Vittaya Amornkitbamrung		
156532	ASS3800237	impurity phase:CuO. small grain size, growth direction along a-axis	Cu(Cr,Fe)O2	Cu1Cr1O2	Cu	1	Cr	1																	O	2			2016																										ABC2					A	2.973		17.093											delafossite structure	K	118	132	150				132																																																																							Ohm.cm											104														materials prepared using a self-combustion urea process. small					Characterization of transparent superconductivity Fe-doped CuCrO2 delafossite oxide			Materials Science and Nanotechnology Program, Faculty of Science, Khon Kaen University, Khon Kaen 40002, Thailand	Appl.Surface Sci., 380(2016)237	Chutirat Taddee,Teerasak Kamwanna,Vittaya Amornkitbamrung		
156533	EPL10667002	Energy gaps measured by scanning tunnelig spectroscopy. Two gap-model (gap = 3.5 and 7.5 meV). Anisotropy = 30-50.	Nd(O,F)BiS2	Nd1F0.5Bi0.84S2O0.5	Nd	1	F	0.5	Bi	0.84	S	2													O	0.5		3	2014																										ABCD2																			BiS2-layer	K				4.5			4.5																				T	RES(0.9Rn), WHH		40	0.833										MHC156533												meV	3.5	16.8	1																																															polycrystal by solid state reaction - flux method using KCl/LiCL flux. (KCl:LiCl:(Nd(O,F)BiS2 = 15:10:1) - heat(750C,5d) - cool to 450C (5C/h)					Giant superconducting fluctuation and anomalous semiconducting normal state in NdO1-xFxBi1-yS2 single crystals			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, National Center of Microstructures and Quantum Manipulation, Nanjing University Nanjing 210093, China	EuroPhys.Lett., 106(2014)67002	Jianzhong Liu,Delong Fang,Zhenyu Wang,Jie Xing,Zengyi Du,Sheng Li,Xiyu Zhu,Huan Yang,Hai-Hu Wen		
156534	INT0710073	Curie-T measured by real part of ac-susceptibility. T<Curie> = 4.2 K from another method.	Co7Y9	Co7Y9	Co	7	Y	9																				1	2016							5.13																			A7B9					A	4.0471		11.517												K				3			3																																																																																														Y,Co,Pd		arc-melting - wrapped in Ta-foil - sealed in quartz ampoule - ANN(620 c, 520 C, 420 C for a week at each temperature)					Superconductivity and ferromagnetism in Pd doped Y9Co7			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Intermetallics, 71(2016)73	Judyta Strychalska,Joe D. Thompson,Robert J. Cava,Tomasz Klimczuk		
156535	JPCM027022202	impurity phase = BaPt4As6. Tetra-to-ortho phase transition at 272 K. Two step SC transitions. high-Tc(=1.69K) phase.	BaPt2As2	Ba1Pt2As2	Ba	1	Pt	2	As	2																		3	2015																										AB2C2		CeBe2Ge2	P4/nmm		A	4.564		10.02												K	1.35		1.69				1.52																				T	RES(on), WHH		0.85	0.52					T/K	RES(on)		0.76	0.52	MHC156535		A	from Hc2		197	252													MSP156535																																											self-flux method. mixture(PtAs2,Ba,Pt) - alumina crucible - sealed in quartz ampule heat to 1100C - keep (12h) - cool to 950C at 1.5 C/h - FC to RT					Superconductivity and structural distortion in BaPt2As2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.Condens.Matter, 27(2015)022202	W B Jiang,C Y Guo,Z F Weng,Y F Wang,Y H Chen,Y Chen,G M Pang,T Shang,X Lu,H Q Yuan		
156536	JPCM027022202	impurity phase = BaPt4As6. Tetra-to-ortho phase transition at 272 K. Two step SC transitions. Low-Tc(=1.35K) phase.  (dC/gamma*Tc) = 1.27. e-ph = 0.496	BaPt2As2	Ba1Pt2As2	Ba	1	Pt	2	As	2																		3	2015																										AB2C2		CeBe2Ge2	P4/nmm		A	4.564		10.02												K	1.35		1.69				1.52																				T	RES(zero), WHH		0.58	0.33					T/K	RES(zero)		0.62	0.35	MHC156535		A	from Hc2		238	316								3.46	14				MSP156535			mJ/mol.K2	7.42	SP	227	SP																																				self-flux method. mixture(PtAs2,Ba,Pt) - alumina crucible - sealed in quartz ampule heat to 1100C - keep (12h) - cool to 950C at 1.5 C/h - FC to RT					Superconductivity and structural distortion in BaPt2As2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.Condens.Matter, 27(2015)022202	W B Jiang,C Y Guo,Z F Weng,Y F Wang,Y H Chen,Y Chen,G M Pang,T Shang,X Lu,H Q Yuan		
156537	INT0710073	Curie-T measured by real part of ac-susceptibility.	Y9(Co,Pd)7	Y9Co6.95Pd0.05	Y	9	Co	6.95	Pd	0.05																		1	2016							9.4																			A7B9					A	4.0432		11.521												K					1.8																																																																																																Y,Co,Pd		arc-melting - wrapped in Ta-foil - sealed in quartz ampoule - ANN(620 c, 520 C, 420 C for a week at each temperature)					Superconductivity and ferromagnetism in Pd doped Y9Co7			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Intermetallics, 71(2016)73	Judyta Strychalska,Joe D. Thompson,Robert J. Cava,Tomasz Klimczuk		
156538	INT0710073	Curie-T measured by real part of ac-susceptibility.	Y9(Co,Pd)7	Y9Co6.9Pd0.1	Y	9	Co	6.9	Pd	0.1																		1	2016							9.8																			A7B9					A	4.0473		11.525												K					1.8																																																																																																Y,Co,Pd		arc-melting - wrapped in Ta-foil - sealed in quartz ampoule - ANN(620 c, 520 C, 420 C for a week at each temperature)					Superconductivity and ferromagnetism in Pd doped Y9Co7			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Intermetallics, 71(2016)73	Judyta Strychalska,Joe D. Thompson,Robert J. Cava,Tomasz Klimczuk		
156539	INT0710073	Curie-T measured by real part of ac-susceptibility.	Y9(Co,Pd)7	Y9Co6.8Pd0.2	Y	9	Co	6.8	Pd	0.2																		1	2016							10.5																			A7B9					A	4.0412		11.534												K					1.8																																																																																																Y,Co,Pd		arc-melting - wrapped in Ta-foil - sealed in quartz ampoule - ANN(620 c, 520 C, 420 C for a week at each temperature)					Superconductivity and ferromagnetism in Pd doped Y9Co7			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Intermetallics, 71(2016)73	Judyta Strychalska,Joe D. Thompson,Robert J. Cava,Tomasz Klimczuk		
156540	JPCM027225701	[penet] measured by TDO. Energy gap estimated from [penet] (in DB) using fitting process and superfluid density (gap = 2.14 kTc)	Nd(O,F)BiS2	Nd1F0.3Bi1S2O0.7	Nd	1	F	0.3	Bi	1	S	2													O	0.7		3	2015			K	0.0076	myu-B/mol	1.97	-0.73																			ABCD2																			BiS2-layer SC	K		4.7					4.7										100																															nm	TDO	447			kTc	1.95	3.9	1																																															Single crystals grown by flux method using CsCl/KCl as a flux.					Evidence for nodeless superconductivity in NdO1-xFxBiS2 (x = 0.3 and 0.5) single crystals			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310058, People's Republic of China	J.Phys.Condens.Matter, 27(2015)225701	Lin Jiao,Zongfa Weng,Jianzhong Liu,Jinglei Zhang,Guiming Pang,Chunyu Guo,Fei Gao,Xiyu Zhu,Hai-Hu Wen,H Q Yuan		
156541	JPCM027225701	[penet] measured by TDO. Energy gap estimated from [penet] (in DB) using fitting process and superfluid density (gap = 2.15 kTc)	Nd(O,F)BiS2	Nd1F0.5Bi1S2O0.5	Nd	1	F	0.5	Bi	1	S	2													O	0.5		3	2015			K	0.0154	myu-B/mol	2.8	-1.02																			ABCD2																			BiS2-layer SC	K		4.4					4.4										70																															nm	TDO	480			kTc	1.92	3.84	1																																															Single crystals grown by flux method using CsCl/KCl as a flux.					Evidence for nodeless superconductivity in NdO1-xFxBiS2 (x = 0.3 and 0.5) single crystals			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310058, People's Republic of China	J.Phys.Condens.Matter, 27(2015)225701	Lin Jiao,Zongfa Weng,Jianzhong Liu,Jinglei Zhang,Guiming Pang,Chunyu Guo,Fei Gao,Xiyu Zhu,Hai-Hu Wen,H Q Yuan		
156542	JPS085064705	Pb and Sn content measured by EDX: (Pb/Ti) = 0.42  , (Sn/Ti) = 0.002	(Pb1-xSnxSe)1.6(TiSe2)2	Pb1.16Ti2Se5.16	Pb	1.16	Ti	2	Se	5.16																		3	2016																																														K		3.25					3.25																																																																																														Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156543	JPS085064705	Pb and Sn content measured by EDX: (Pb/Ti) = 0.52, (Sn/Ti) = 0.059	(Pb1-xSnxSe)1.6(TiSe2)2	Pb1.044Sn0.116Ti2Se5.16	Pb	1.044	Sn	0.116	Ti	2	Se	5.16																3	2016																																														K		4.19					4.19																																																																																														Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156544	JPS085064705	Pb and Sn content measured by EDX: (Pb/Ti) =   0.38, (Sn/Ti) = 0.132	(Pb1-xSnxSe)1.6(TiSe2)2	Pb0.928Sn0.232Ti2Se5.16	Pb	0.928	Sn	0.232	Ti	2	Se	5.16																3	2016																																														K		4.53					4.53																																																																																														Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156545	JPS085064705		(Pb1-xSnxSe)1.6(TiSe2)2	Pb0.812Sn0.348Ti2Se5.16	Pb	0.812	Sn	0.348	Ti	2	Se	5.16																3	2016																																														K		4.02					4.02																																																																																														Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156546	JPS085064705	Pb and Sn content measured by EDX: (Pb/Ti) =  0.37 , (Sn/Ti) = 0.13. Lattice term in SP (beta) = 3.89 mJ/mol.K4. (dC/gamma*Tc) = 1.38. e-ph = 0.72. DOS = 2.73 states/eV.fu from gamma.	(Pb1-xSnxSe)1.6(TiSe2)2	Pb0.696Sn0.464Ti2Se5.16	Pb	0.696	Sn	0.464	Ti	2	Se	5.16																3	2016																																														K		3.82					3.82	MTC156546																																																				MSP156546			mJ/mol.K2	11.06	SP	161	SP																																		Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156547	JPS085064705		(Pb1-xSnxSe)1.6(TiSe2)2	Pb0.58Sn0.58Ti2Se5.16	Pb	0.58	Sn	0.58	Ti	2	Se	5.16																3	2016																																														K		3.6					3.6																																																																																														Pb(3N),Sn(2N5),Ti(3N),Se(5N)		mixture(stoichiometric) - heat to 700C(1C/min) - keep(48h) - reground - heat to 900C(3C/min) - keep(16h). Single crystals grown by CVD method using SeCl4 as transport agent					Superconductivity in a Misfit Phase That Combines the Topological Crystalline Insulator Pb1-xSnxSe with the CDW-Bearing Transition Metal Dichalcogenide TiSe2			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 85(2016)064705	Huixia Luo,Kai Yan,Ivo's Pletikosic,Weiwei Xie,Brendan F. Phelan,Tonica Valla,Robert J. Cava		
156548	JPS085064710	RRR = 11.2. Minor impurity phase:  Fe-122(ThCr2Si2) type phase. magnetic order appears at 15 K.	EuRbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																1	2016																										ABC4D4			P4/mmm	123	A	3.889		13.3											Fe-1144	K	35.8		36.2	36			36																				T	RES(0.9Rn), WHH	92							T/K	RES(0.9Rn)	3.692			MHC156548		A	from Hc2	18																																																										Solid state reaction. See J.Am.Chem.Soc., 138(2016)3410					Superconductivity in Fe-Based Compound EuAFe4As4 (A = Rb and Cs)			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys.Soc.Jpn, 85(2016)064710	Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida,Akira Iyo		
156549	JPS085064710	RRR = 11.2. Minor impurity phase:  Fe-122(ThCr2Si2) type phase. magnetic order appears at 15 K.	EuCsFe4As4	Eu1Cs1Fe4As4	Eu	1	Cs	1	Fe	4	As	4																1	2016																										ABC4D4			P4/mmm	123	A	3.901		13.63											Fe-1144	K	34.9		35.1	35			35																				T	RES(0.9Rn), WHH	87.5							T/K	RES(0.9Rn)	3.612			MHC156548		A	from Hc2	19																																																										Solid state reaction. See J.Am.Chem.Soc., 138(2016)3410					Superconductivity in Fe-Based Compound EuAFe4As4 (A = Rb and Cs)			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys.Soc.Jpn, 85(2016)064710	Kenji Kawashima,Tatsuya Kinjo,Taichiro Nishio,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Hiroshi Eisaki,Yoshiyuki Yoshida,Akira Iyo		
156550	JPS085073708	"P-induced SC. P<cr> = 2.1 GPa. Figure captuon: polishe ""P"" and polished and ANN(900c,2w) ""P+A. Tc defined as R(end). Surface polishing affects Tc. Tn defined as kink in R(T)."	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2016																										ABC3		BaNiSn3																		K	1.6				0		1.6	MPH156550																																																																																													Ce(3N),Ir(3N),Si(5N)		Czochralski- method - single crystal - ANN(900C,1w, in vac)					Superconductivity Induced by Surface Polishing in CeIrSi3			Department of Physics, Tohoku University, Sendai 980-8578, Japan	J.Phys.Soc.Jpn, 85(2016)073708	Hiroki Iida,Masashi Sato,Noriaki Kimura		
156551	JPS085094713	R(T)max at T=47 K. R-exponent n=0.95. (dC/Tc) = 1.6 J/mol.K2	CeCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2016																										ABC5		HoCoGa5																		K	2.25						2.25																				T	R(zero), WHH			15.5					T/K	RES(zero)			10	MHC156552																																																														In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156552	JPS085094713	R(T)max at T=47 K. R-exponent n=0.69	Ce(Co,Ni)In5	Ce1Co0.95Ni0.05In5	Ce	1	Co	0.95	Ni	0.05	In	5																3	2016																										ABC5		HoCoGa5																		K	1.86						1.86																				T	R(zero), WHH			12.3					T/K	RES(zero)			9.58	MHC156552																																																														In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156553	JPS085094713	R(T)max at T=48 K. R-exponent n=0.64	Ce(Co,Ni)In5	Ce1Co0.925Ni0.075In5	Ce	1	Co	0.925	Ni	0.075	In	5																3	2016																										ABC5		HoCoGa5																		K	1.69						1.69	MTC156554																			T	R(zero), WHH			9.8					T/K	RES(zero)			8.44	MHC156552																																																														In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156554	JPS085094713	R(T)max at T=50 K. R-exponent n=0.65. (dC/Tc) = 1.2 J/mol.K2	Ce(Co,Ni)In5	Ce1Co0.875Ni0.125In5	Ce	1	Co	0.875	Ni	0.125	In	5																3	2016					myu-B/Ce	2.5	-87																			ABC5		HoCoGa5																		K	1.41						1.41	MTC156554																			T	R(zero), WHH			7.8					T/K	RES(zero)			7.99	MHC156554																																																														In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156555	JPS085094713	R(T)max at T=53.5 K. R-exponent n=0.71. (dC/Tc) = 0.34 J/mol.K2	Ce(Co,Ni)In5	Ce1Co0.8Ni0.2In5	Ce	1	Co	0.8	Ni	0.2	In	5																3	2016																										ABC5		HoCoGa5																		K	0.88						0.88																				T	R(zero), WHH			5.5					T/K	RES(zero)			9.06	MHC156554																																																														In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156556	JPS085094713	R(T)max at T=59.7 K. R-exponent n=0.85	Ce(Co,Ni)In5	Ce1Co0.75Ni0.25In5	Ce	1	Co	0.75	Ni	0.25	In	5																3	2016																										ABC5		HoCoGa5																		K	0				0.5		0																																																																																																In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156557	JPS085094713	R(T)max at T=67.9 K. R-exponent n=1.0	Ce(Co,Ni)In5	Ce1Co0.7Ni0.3In5	Ce	1	Co	0.7	Ni	0.3	In	5																3	2016																										ABC5		HoCoGa5																		K					0.5																																																																																																		In-flux method. (Ce,Co,Ni,In with excess flux) - quartz tube(Ar) - heat(1050 C) - cool by two stage process.					Superconductivity and Non-Fermi-Liquid Behavior in the Heavy-Fermion Compound CeCo1-xNixIn5			Faculty of Science, Ibaraki University, Mito 310-8512, Japan	J.Phys.Soc.Jpn, 85(2016)094713	Ryo Otaka,Makoto Yokoyama,Hiroaki Mashiko,Takeshi Hasegawa,Yusei Shimizu,Yoichi Ikeda,Kenichi Tenya,Shota Nakamura,Daichi Ueta,Hideki Yoshizawa,Toshiro Sakakibara		
156558	JPS085103701	HP-synthesis. Lattice term in sp (beta) = 0.813 mJ/mol.K4. (dC/gamma*Tc) = 1.54. dC<el> = 9.6 mJ/mol.K	HP-Sn0.8Ag0.2Te	Sn0.8Ag0.2Te1	Sn	0.8	Ag	0.2	Te	1																		1	2016																										AB			Fm3[-]m		A	6.1767														K		2.1					2.1																				T	RES(0.9Rn), extrapolation	0.9												MHC156558		A	from Hc2	200															MSP156558			mJ/mol.K2	2.95	SP	169	SP																																		Ag(3N),Sn(4N),Te(6N)		High P synthesis.  mixture - press to pellet - heat(500C,30min, P=2 GPa)					Specific Heat and Electrical Transport Properties of Sn0.8Ag0.2Te Superconductor			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)103701	Yoshikazu Mizuguchi,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Osuke Miura,Masanori Nagao		
156559	JPS085105001	RRR = 8.1. Tc(SP) = 0.72 K. Lattice term in SP (beta) = 3.00 mJ/mol.K4. [gamma]n  = [gamma](in DB) - gamma(0) = 65.5 - 16 = 50 mJ/mol.K2	Y6Nb4Al43	Y6Nb4Al43	Y	6	Nb	4	Al	43																		1	2016																										A4B6C43			P63<3>/mcm	193	A	11.06		17.758											cage structure	K		0.86					0.86																				T	RES(0.5Rn), WHH	0.22												MHC156559		A	from Hc2	387															MSP156559			mJ/mol.K2	65.5	SP	325	SP											uOhm.cm							5.5																Y(3N),Nb(3N),Mo(3N),Ta(3M),Al(5N)		mixture - arc-melting several times - ANN(1000C,7d, in quartz tube(vac)					Superconductivity in Y6Tr4Al43 (Tr = Nb, Mo, Ta) with Peanut-Shaped Cage Structure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 85(2016)105001	Naoki Kase,Ryoh Satoh,Tomohito Nakano,Naoya Takeda		
156560	JPS085105001	RRR = 13.8. Tc(SP) = 0.75 K. Lattice term in SP (beta) = 1.47 mJ/mol.K4. [gamma]n  = [gamma](in DB) - gamma(0) = 77.0 - 32 = 45 mJ/mol.K2	Y6Mo4Al43	Y6Mo4Al43	Y	6	Mo	4	Al	43																		1	2016																										A4B6C43			P63<3>/mcm	193	A	10.997		17.734											cage structure	K		0.75					0.75																				T	RES(0.5Rn), WHH	0.175												MHC156560		A	from Hc2	434															MSP156560			mJ/mol.K2	77	SP	412	SP											uOhm.cm							2.5																Y(3N),Nb(3N),Mo(3N),Ta(3M),Al(5N)		mixture - arc-melting several times - ANN(1000C,7d, in quartz tube(vac)					Superconductivity in Y6Tr4Al43 (Tr = Nb, Mo, Ta) with Peanut-Shaped Cage Structure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 85(2016)105001	Naoki Kase,Ryoh Satoh,Tomohito Nakano,Naoya Takeda		
156561	JPS085105001	RRR = 5.5. Tc(SP) = 0.53 K. Lattice term in SP (beta) = 2.00 mJ/mol.K4. [gamma]n  = [gamma](in DB) - gamma(0) = 60.8 - 10 = 51 mJ/mol.K2	Y6Ta4Al43	Y6Ta4Al43	Y	6	Ta	4	Al	43																		1	2016																										A4B6C43			P63<3>/mcm	193	A	11.087		17.895											cage structure	K		0.68					0.68																				T	RES(0.5Rn), WHH	0.15												MHC156561		A	from Hc2	468															MSP156561			mJ/mol.K2	60.8	SP	372	SP											uOhm.cm							10.3																Y(3N),Nb(3N),Mo(3N),Ta(3M),Al(5N)		mixture - arc-melting several times - ANN(1000C,7d, in quartz tube(vac)					Superconductivity in Y6Tr4Al43 (Tr = Nb, Mo, Ta) with Peanut-Shaped Cage Structure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 85(2016)105001	Naoki Kase,Ryoh Satoh,Tomohito Nakano,Naoya Takeda		
156562	JPS085103701	Ambient pressure synthesis. sample did not show bulk SC above 1.8 K.	AP-Sn0.8Ag0.2Te	Sn0.8Ag0.2Te1	Sn	0.8	Ag	0.2	Te	1																		1	2016																										AB			Fm3[-]m		A	6.2365														K		1.2					1.2																																																					MSP156562																																											Ambient pressure synthesis.  mixture - heat in evacuated quartz tube)					Specific Heat and Electrical Transport Properties of Sn0.8Ag0.2Te Superconductor			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)103701	Yoshikazu Mizuguchi,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Osuke Miura,Masanori Nagao		
156563	JPSCP003015011	RRR = 120 for I//a and 66 for I//c. Tc = 2.30 K for I//c. Hc2(T) by SUS is isotropic. Hc2(T) measured by R(zero) is much higher than Hc2 by SUS.	LaRhSi3	La1Rh1Si3	La	1	Rh	1	Si	3																		3	2014																										ABC3		BaNiSn3	I4mm	107																K	2.32						2.32																				T	RES(zero), extrapolation		0.126											MHC156563																																					uOhm.cm								0.21	0.48														La(3N),Rh(3N),Si(5N)		Czochrarski method - ANN(900C,1w, in vac)					Robust Zero Resistance under Magnetic Fields in Non-centrosymmetric Superconductor LaRhSi3			Department of Physics, Tohoku University, Sendai 980-8578, Japan	J.Phys.Soc.Jpn, Conf.Proc., 3(2014)015011	Noriaki KIMURA,Hajime OGI,Kazunori SATOH,Gohki OHSAKI,Kohsuke SAITOH,Hihoki IIDA,Haruyoshi AOKI		
156564	JPS085104710	Sample(La-Bi2201). Details of samples not given. described only by hole concentration calculated from Seebeck coeff. S(290K). Gaps measured by ARPES.	Bi2(Sr,La)2CuO6	Bi2Sr1.6La0.4Cu1O6+z	Bi	2	Sr	1.6	La	0.4	Cu	1													O	6+z		3	2016																												Bi2201																		K		32					32	MTC156564																																														13.6	9.85																																																single crystals grown by floating zone method					Carrier Concentration Dependence of Superconducting Gap of Bi2(Sr,La)2CuO6+z			Department of Crystalline Materials Science, Nagoya University, Nagoya 464-8603, Japan	J.Phys.Soc.Jpn, 85(2016)104710	Hideki Sakamoto,Koto Ogawa,Takeshi Kondo,Shik Shin,Masaharu Matsunami,Hiroshi Ikuta,Tsunehiro Takeuchi		
156565	MAT1502.04304	dTc/dP = -0.38 K/GPa for hydrostatic P < 2 GPa. (dTc/dP) = -0.76 K/GPa at P = 2.1 GPa.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2015																										A2B3C3		K2Cr3As3																		K		6.1					6.1	MTC156565		K/GPa	-0.38																																																																																												flux method					Reversible tuning of superconductivity in pressurized qausi-one-dimensional K2Cr3As3 (A=K and Rb)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/1502.04304	Zhe Wang,Vladimir Sidorov,Qi Wu,Jinke Bao,Zhangtu Tang,Wei Yi,Jing Guo,Yazhou Zhou,Shan Zhang,Chao Zhang,Guanghan Cao,Liling Sun,Zhongxian Zhao		
156566	MAT1502.04304		Rb2Cr3As3	Rb2Cr3As3	Rb	2	Cr	3	As	3																		3	2015																										A2B3C3		K2Cr3As3																		K		4.8					4.8	MTC156566			-0.814																																																																																												flux method					Reversible tuning of superconductivity in pressurized qausi-one-dimensional K2Cr3As3 (A=K and Rb)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	cond-mat/1502.04304	Zhe Wang,Vladimir Sidorov,Qi Wu,Jinke Bao,Zhangtu Tang,Wei Yi,Jing Guo,Yazhou Zhou,Shan Zhang,Chao Zhang,Guanghan Cao,Liling Sun,Zhongxian Zhao		
156567	MMM2700051	not SC. RRR = 32	YFe2Ge2	Y1Fe2Ge2	Y	1	Fe	2	Ge	2																		3	2004	emu/mol	0.003																								AB2C2		ThCr2Si2	I4/mmm		A	3.968		10.463											Fe-122	K					1.8																																																										mJ/mol.K2	60	SP	280	SP											uOhm.cm							5.4																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156568	MMM2700051	not SC. RRR = 23	LuFe2Ge2	Lu1Fe2Ge2	Lu	1	Fe	2	Ge	2																		3	2004	emu/mol	0.003																								AB2C2		ThCr2Si2	I4/mmm		A	3.914		10.395											Fe-122	K					1.8																																																										mJ/mol.K2	60	SP	240	SP											uOhm.cm							9																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156569	MMM2700051	not SC. RRR = 60. 2nd magnetic phase at 8.3 K.	PrFe2Ge2	Pr1Fe2Ge2	Pr	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0053			myu-B/R	3.5		14.6																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156570	MMM2700051	not SC. RRR = 53.2nd magnetic phase at 13.5 K	NdFe2Ge2	Nd1Fe2Ge2	Nd	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0042			myu-B/R	3.4		16.4																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156571	MMM2700051	not SC. RRR = 83. 2nd magnetic phase at 4.9 K	SmFe2Ge2	Sm1Fe2Ge2	Sm	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0039			myu-B/R	0.46		5.9																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																													250	SP																																				Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156572	MMM2700051	not SC. RRR = 68. 2nd magnetic phase at 9.6 K	GdFe2Ge2	Gd1Fe2Ge2	Gd	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0026			myu-B/R	7.6		10.8																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156573	MMM2700051	not SC. RRR = 32	TbFe2Ge2	Tb1Fe2Ge2	Tb	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0058			myu-B/R	9.6		7.4																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156574	MMM2700051	not SC. RRR = 31	DyFe2Ge2	Dy1Fe2Ge2	Dy	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0043			myu-B/R	10.6		2.1																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156575	MMM2700051	not SC. RRR = 34	HoFe2Ge2	Ho1Fe2Ge2	Ho	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0024			myu-B/R	11		1.1																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156576	MMM2700051	not SC. RRR = 38	ErFe2Ge2	Er1Fe2Ge2	Er	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0025			myu-B/R	9.5		2.5																		AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156577	MMM2700051	not SC. RRR = 21	TmFe2Ge2	Tm1Fe2Ge2	Tm	1	Fe	2	Ge	2																		3	2004	emu/mol	0.0049			myu-B/R	7.8																				AB2C2		ThCr2Si2	I4/mmm																Fe-122	K					1.8																																																																																																		Flux method using Sn-flux					Anisotropic magnetization, specific heat and resistivity of RFe2Ge2 single crystals			Ames Laboratory Condensed Matter Physics, Department of Physics and Astronomy, Iowa State University, Ames, IA 50011, USA	J.Magn.Magn.Mater., 270(2004)51	M.A. Avila,S.L. Bud'ko,P.C. Canfield		
156578	NATCOM0030931	Energy gpps measured by photoemission and ARPES.	FeSe	Fe1Se1	Fe	1	Se	1																					2012																										AB																				K		55					55	MGAP156578																																													meV	15	6.34																																																					Electronic origin of high-temperature superconductivity in single-layer FeSe superconductor			National Lab for Superconductivity, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences , Beijing 100190, China.	Nature Commun., 3(2012)931	Defa Liu,Wenhao Zhang,Daixiang Mou,Junfeng He,Yun-Bo Ou,Qing-Yan Wang,Zhi Li,Lili Wang,Lin Zhao,Shaolong He,Yingying Peng,Xu Liu,Chaoyu Chen,Li Yu,Guodong Liu,Xiaoli Dong,Jun Zhang,Chuangtian Chen,Zuyan Xu,X.J. Zhou		
156579	PCS0611591	RRR = R(280)/R(8K) = 3.3. Demag. factor = 0.1173 for Hc1. Hc1=Hc1(0)(1-t^2). -(dHc2/dT) = 0.415 and  0.336 T/K for 3<T<3.4 and for T<3 K, respectively.	TaPtSi	Ta1Pt1Si1	Ta	1	Pt	1	Si	1																		1	2000	emu/mol	0.0000392	emu/K/mol	0.0012			-34.6		15.02																	ABC	3	Co2Si	Pnma		A	6.388	3.808	7.353												K	3.45	3.54	3.8	3.6			3.54											Oe	M-H curve	56.8			44			1.7	T	RES(0.5Rn), WHH	1.02							T/K	RES(0.5Rn)	0.336			MHC156579		A	from Hc2	180			nm	GL theory using k(GL) and Hc1	315													mJ/mol.K2	1.18	calc from R0																																				Ta(4N),Pt(4N),Si(6N)		arc-melting - sealed in quartz ampoule(155 Torr Ar) - heat(1200C,3d) - Q to water					Superconductivity of the new intermetallic compound TaPtSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Phys.Chem.Solids, 61(2000)1591	S. Yashiro,R. Kasai,A. Kasahi,Y. Nagata,H. Samata,T. Uchida,M.D. Lan		
156580	PHB2840475	Specific heat(SP) measured for 0.5 < T < 20 K. Energy gap obtained from SP fitting.	Zr2Co	Co1Zr2	Co	1	Zr	2																				1	2000																										AB2																				K		5.5					5.5																																																3.02	14							mJ/mol.K2	19.3	SP																																											Superconductivity in an itinerant nearly antiferromagnetic Zr2(Co1-xNix)			Department of Physics, Faculty of Science, Kobe University, Nada, Kobe 657-8501, Japan	Physica B, 284-288(2000)475	Tomoyuki Matsuo,Hiroshi Sugita,Shinji Wada,Masayasu Ishikawa		
156581	PHB2840475	Specific heat(SP) measured for 0.5 < T < 20 K. Energy gap obtained from SP fitting.	Zr2Co1-xNix	Zr2Co0.85Ni0.15	Zr	2	Co	0.85	Ni	0.15																		1	2000																										AB2																				K		6					6																																																3.34	14							mJ/mol.K2	23.7	SP																																											Superconductivity in an itinerant nearly antiferromagnetic Zr2(Co1-xNix)			Department of Physics, Faculty of Science, Kobe University, Nada, Kobe 657-8501, Japan	Physica B, 284-288(2000)475	Tomoyuki Matsuo,Hiroshi Sugita,Shinji Wada,Masayasu Ishikawa		
156582	PHB2840475	Specific heat(SP) measured for 0.5 < T < 20 K. Energy gap obtained from SP fitting.	Zr2Co1-xNix	Zr2Co0.6Ni0.4	Zr	2	Co	0.6	Ni	0.4																		1	2000																										AB2																				K		4.2					4.2																																																3.62	14							mJ/mol.K2	20.5	SP																																											Superconductivity in an itinerant nearly antiferromagnetic Zr2(Co1-xNix)			Department of Physics, Faculty of Science, Kobe University, Nada, Kobe 657-8501, Japan	Physica B, 284-288(2000)475	Tomoyuki Matsuo,Hiroshi Sugita,Shinji Wada,Masayasu Ishikawa		
156583	PHB2841111		Zr2Co	Co1Zr2	Co	1	Zr	2																				1	2000																										AB2																				K		5.2					5.2																																		MHC156583														3.67	14							mJ/mol.K2	8.39	SP																																											Low-temperature specfic heat of Zr2(Co1-xNix) under magnetic fields			Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930-8555, Japan	Physica B, 284-288(2000)1111	Katushiko Nishimura,Yuzuru Tsurugiya,Shixun Cao,Seiichi Rengakuji,Katsunori Mori		
156584	PHB2841111		Zr2Co1-xNix	Zr2Co0.9Ni0.1	Zr	2	Co	0.9	Ni	0.1																		1	2000																										AB2																				K		5.94					5.94																																		MHC156584														4.72	14							mJ/mol.K2	8.62	SP																																											Low-temperature specfic heat of Zr2(Co1-xNix) under magnetic fields			Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930-8555, Japan	Physica B, 284-288(2000)1111	Katushiko Nishimura,Yuzuru Tsurugiya,Shixun Cao,Seiichi Rengakuji,Katsunori Mori		
156585	PHB2841111		Zr2Co1-xNix	Zr2Co0.8Ni0.2	Zr	2	Co	0.8	Ni	0.2																		1	2000																										AB2																				K		5.83					5.83																																		MHC156585														4.64	14							mJ/mol.K2	9.84	SP																																											Low-temperature specfic heat of Zr2(Co1-xNix) under magnetic fields			Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930-8555, Japan	Physica B, 284-288(2000)1111	Katushiko Nishimura,Yuzuru Tsurugiya,Shixun Cao,Seiichi Rengakuji,Katsunori Mori		
156586	PHB2841111		Zr2Co1-xNix	Zr2Co0.7Ni0.3	Zr	2	Co	0.7	Ni	0.3																		1	2000																										AB2																				K		5.14					5.14																																		MHC156586														4.41	14							mJ/mol.K2	7.73	SP																																											Low-temperature specfic heat of Zr2(Co1-xNix) under magnetic fields			Faculty of Engineering, Toyama University, 3190 Gofuku, Toyama 930-8555, Japan	Physica B, 284-288(2000)1111	Katushiko Nishimura,Yuzuru Tsurugiya,Shixun Cao,Seiichi Rengakuji,Katsunori Mori		
156587	PHC5280023	impurity phases: Bi2O3, Bi.	Bi4-xCoxO4S3	Bi3.925Co0.075S3O4	Bi	3.925	Co	0.075	S	3															O	4		1	2016																										A3B4C4			I4/mmm		A	3.9619		41.296											BiS2-layer SC	K	3.94		4.79				4.365																																																																							mOhm.cm							4.64																Bi(4N),Bi2O3(4N),S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube(vac) - heat(510C,10h) - reground - pellet - ANN(510C,10h)					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156588	PHC5280023	impurity phases: Bi2O3, Bi.  M-H curves show ferromag- and SC- diamag- behaviour at T-3 and 4 K.	Bi4-xCoxO4S3	Bi3.9Co0.1S3O4	Bi	3.9	Co	0.1	S	3															O	4		1	2016							14																			A3B4C4			I4/mmm		A	3.9595		41.2857											BiS2-layer SC	K	4.9		5.5				5.2																																																																							mOhm.cm							3.16																Bi(4N),Bi2O3(4N),S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube(vac) - heat(510C,10h) - reground - pellet - ANN(510C,10h)					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156589	PHC5280023	impurity phases: Bi2O3, Bi.	Bi4-xCoxO4S3	Bi3.875Co0.125S3O4	Bi	3.875	Co	0.125	S	3															O	4		1	2016																										A3B4C4			I4/mmm		A	3.9578		41.2716											BiS2-layer SC	K	3.94		4.56				4.25																																																																							mOhm.cm							2.56																Bi(4N),Bi2O3(4N),S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube(vac) - heat(510C,10h) - reground - pellet - ANN(510C,10h)					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156590	PHC5280023	impurity phases: Bi2O3, Bi.	Bi4-xCoxO4S3	Bi3.85Co0.15S3O4	Bi	3.85	Co	0.15	S	3															O	4		1	2016																										A3B4C4			I4/mmm		A	3.957		41.2657											BiS2-layer SC	K	3.66		4.28				3.97																																																																							mOhm.cm							1.84																Bi(4N),Bi2O3(4N),S(5N),Co3O4(4N)		mixture - pellet - sealed in quartz tube(vac) - heat(510C,10h) - reground - pellet - ANN(510C,10h)					Co-doping induced coexistence of superconductivity and ferromagnetism in Bi3.9Co0.1O4S3			Department of Physics, Shanghai University, Shanghai 2004 4 4, China	Physica C, 528(2016)23	Chuan Yu,Zhenjie Feng,Xunqing Yin,Qing Li,Baojuan Kang,Bo Lu,Shixun Cao,Jincang Zhang		
156591	PLA3791057	kappa(GL) = 39.7.  (dC/gamma*Tc) = 1.9	ZrVGe	Zr1V1Ge1	Zr	1	V	1	Ge	1																		1	2015																										ABC			I4/mmm		A	3.754		14.488												K				6			6										97	mT	M-H curve. dM-0.05 emu/g	3.5							T	RES(0.9Rn), WHH	5.5												MHC156591		A	from Hc2	77			nm	GL theory using k(GL) and Hc1	306										MSP156591			mJ/mol.K2	8.6	SP	289	SP																																		Zr,V,Ge		arc-melting					Superconductivity in the ternary ZrVGe compound			Escola de Engenharia de Lorena ? USP, P.O. Box 116, Lorena, 12602-810, Brazil	Phys.Lett. A, 379(2015)1057	A.J.S.Machado,F.B.Santos,B.S.deLima,S.T.Renosto,L.E.Correa,O.V.Cigarroa,M.S.daLuz,Z.Fisk		
156592	PRB093115119	proton irradiation (4MeV) effect. Samples are nearly optimal (x=0.33) three samples with Tc=28.7, 28.7, 29.6. proton creates cascades of point defect along with isolated point defects.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																3	2016																										AB2C2		ThCr2Si2	I4/mmm																Fe-122	K		25		28.7			25	MTC156592																																																																						uOhm.cm											120														self-flux method. crystal size = 200*400 um^2 * 20 um thickness					Effect of proton irradiation on superconductivity in optimally doped BaFe2(As1-xPx)2 single crystals			Materials Science Division, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, Illinois 60439, USA	Phys.Rev.B, 93(2016)115119	M. P. Smylie,M. Leroux,V. Mishra,L. Fang,K. M. Taddei,O. Chmaissem,H. Claus,A. Kayani,A. Snezhko,U. Welp,W.-K. Kwok		
156593	PRB089144509	M = NH3, intercalated materials. M-content y not given.	Na0.5(NH3)yFeSe	Na0.5M1Fe1Se1	Na	0.5	M	1	Fe	1	Se	1																1	2014																																														K		31					31	MTC156593		K/GPa	-7.7																																																																																												annealing method					Superconducting phases in (NH3)yMxFeSe1-zTez (M = Li, Na, and Ca)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 89(2014)144509	Yusuke Sakai,Lu Zheng,Masanari Izumi,Kazuya Teranishi,Ritsuko Eguchi,Hidenori Goto,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Yoshihiro Kubozono		
156595	PRB089144509	M = NH3, intercalated materials. M-content y not given. Hc2 measured for H < 4 T using Tc(on)  and Tc(mid).	Na0.4(NH3)yFeSe0.5Te0.5	Na0.4M1Fe1Se0.5Te0.5	Na	0.4	M	1	Fe	1	Se	0.5	Te	0.5														1	2014																													I4/mmm	139	A	3.9822		17.798												K		22	24				22	MTC156595		K/GPa	-11.7							Oe	M-H curve				100	5			T	RES(on), curve fitting	17												MHC156595																																																														annealing method					Superconducting phases in (NH3)yMxFeSe1-zTez (M = Li, Na, and Ca)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 89(2014)144509	Yusuke Sakai,Lu Zheng,Masanari Izumi,Kazuya Teranishi,Ritsuko Eguchi,Hidenori Goto,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Yoshihiro Kubozono		
156596	PRB089144509	M = NH3, intercalated materials. M-content y not given.	Li0.5(NH3)yFeSe0.5Te0.5	Li0.5M1Fe1Se0.5Te0.5	Li	0.5	M	1	Fe	1	Se	0.5	Te	0.5														1	2014																																														K		26	29				26																																																																																																annealing method					Superconducting phases in (NH3)yMxFeSe1-zTez (M = Li, Na, and Ca)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 89(2014)144509	Yusuke Sakai,Lu Zheng,Masanari Izumi,Kazuya Teranishi,Ritsuko Eguchi,Hidenori Goto,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Yoshihiro Kubozono		
156597	PRB089144509	M = NH3, intercalated materials. M-content y not given.	Ca0.4(NH3)yFeSe0.5Te0.5	Ca0.4M1Fe1Se0.5Te0.5	Ca	0.4	M	1	Fe	1	Se	0.5	Te	0.5														1	2014																																														K		17	18				17																																																																																																annealing method					Superconducting phases in (NH3)yMxFeSe1-zTez (M = Li, Na, and Ca)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 89(2014)144509	Yusuke Sakai,Lu Zheng,Masanari Izumi,Kazuya Teranishi,Ritsuko Eguchi,Hidenori Goto,Taiki Onji,Shingo Araki,Tatsuo C. Kobayashi,Yoshihiro Kubozono		
156598	PRB092020508	RRR = 15. for I//[001]. Anisotropy <1 for LT.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2015																										A2B3C3		K2Cr3As3	P6[-]m2		A	9.9832		4.2304												K		6.1					6.1										90	mT	M-H curve					9		1.8										T/K	RES(on)		16.1	5	MHC156598																																					uOhm.cm							53.7																K(or Rb)(2N8),Cr(5N),As(4N)		self flux method. mixture - alumina crucible - stainless tube-swagelok cap configuration - heat(1000C,1 day) - slow cool to 650C					Tunable electronic anisotropy in single-crystal A2Cr3As3 (A=K, Rb) quasi-one-dimensional superconductors			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 92(2015)020508	X. F. Wang,C. Roncaioli,C. Eckberg,H. Kim,J. Yong,Y. Nakajima,S. R. Saha,P. Y. Zavalij,J. Paglione		
156599	PRB092020508	RRR = 50. for I//[001]. Anisotropy <1 for LT. Lattice term in SP (beta) = 2.8 mJ/mol.K4. (dC/gamma*Tc) = 0.62	Rb2Cr3As3	Rb2Cr3As3	Rb	2	Cr	3	As	3																		3	2015																										A2B3C3		K2Cr3As3	P6[-]m2		A	10.304		4.2514											a=10.251, c=4.227 at 90 K	K		4.8					4.8										30	mT	M-H curve					6		1.8										T/K	RES(on)		14	4.4	MHC156599																						mJ/mol.K2	39.5	SP													uOhm.cm							1.75																K(or Rb)(2N8),Cr(5N),As(4N)		self flux method. mixture - alumina crucible - stainless tube-swagelok cap configuration - heat(1000C,1 day) - slow cool to 650C					Tunable electronic anisotropy in single-crystal A2Cr3As3 (A=K, Rb) quasi-one-dimensional superconductors			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 92(2015)020508	X. F. Wang,C. Roncaioli,C. Eckberg,H. Kim,J. Yong,Y. Nakajima,S. R. Saha,P. Y. Zavalij,J. Paglione		
156600	PRB092220503	RRR = 16.3. Superfluid density measured by mu-SR and TDO. [penet] from mu-SR. Energy gaps are (D/kTc) =1.31 and 1.80(in DB) from TDO results using two gap r- model (r = 0.4).	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																		1	2015																										AB4C12		skutterudite																		K		8.2					8.2																																									nm	mu-SR	120					3.6																																																See Phys.Rev.Lett., 100()017002					Weak interband-coupling superconductivity in the filled skutterudite LaPt4Ge12			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 92(2015)220503	J. L. Zhang,G. M. Pang,L. Jiao,M. Nicklas,Y. Chen,Z. F. Weng,M. Smidman,W. Schnelle,A. Leithe-Jasper,A. Maisuradze,C. Baines,R. Khasanov,A. Amato,F. Steglich,R. Gumeniuk,H. Q. Yuan		
156601	PRB093115133	CDW-gap size = 290 and 140 meV measured by ARPES.	PdxHoTe3	Ho1Te3	Ho	1	Te	3																				3	2016																										AB3	3				A		25.327												ortho-	K					1.8																																																																																																		flux method					Interplay between multiple charge-density waves and the relationship with superconductivity in PdxHoTe3			Department of Physics, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 93(2016)115133	Rui Lou,Yipeng Cai,Zhonghao Liu,Tian Qian,Lingxiao Zhao,Yu Li,Kai Liu,Zhiqing Han,Dandan Zhang,Junbao He,Genfu Chen,Hong Ding,Shancai Wang		
156602	PRB093115133	Pd-intercalated HoTe3. CDW-gap size = 274 and 271 meV measured by ARPES.	PdxHoTe3	Pd0.1Ho1Te3	Pd	0.1	Ho	1	Te	3																		3	2016																										AB3	3				A		25.341												ortho-	K					1.8																																																																																																		flux method					Interplay between multiple charge-density waves and the relationship with superconductivity in PdxHoTe3			Department of Physics, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 93(2016)115133	Rui Lou,Yipeng Cai,Zhonghao Liu,Tian Qian,Lingxiao Zhao,Yu Li,Kai Liu,Zhiqing Han,Dandan Zhang,Junbao He,Genfu Chen,Hong Ding,Shancai Wang		
156603	PRB093115133	Pd-intercalated HoTe3.  CDW-gap size = 240 and 235 meV measured by ARPES.	PdxHoTe3	Pd0.2Ho1Te3	Pd	0.2	Ho	1	Te	3																		3	2016																										AB3	3				A		25.37												ortho-	K			2				2																																																																																																flux method					Interplay between multiple charge-density waves and the relationship with superconductivity in PdxHoTe3			Department of Physics, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 93(2016)115133	Rui Lou,Yipeng Cai,Zhonghao Liu,Tian Qian,Lingxiao Zhao,Yu Li,Kai Liu,Zhiqing Han,Dandan Zhang,Junbao He,Genfu Chen,Hong Ding,Shancai Wang		
156604	PRB093115133	Pd-intercalated HoTe3. No CDW Gaps.	PdxHoTe3	Pd0.4Ho1Te3	Pd	0.4	Ho	1	Te	3																		3	2016																										AB3	3				A		25.406												ortho-	K			2.8				2.8																																																																																																flux method					Interplay between multiple charge-density waves and the relationship with superconductivity in PdxHoTe3			Department of Physics, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 93(2016)115133	Rui Lou,Yipeng Cai,Zhonghao Liu,Tian Qian,Lingxiao Zhao,Yu Li,Kai Liu,Zhiqing Han,Dandan Zhang,Junbao He,Genfu Chen,Hong Ding,Shancai Wang		
156605	PRB093214503	FM(Curie-T) =  15 K  from SUS and SP. (dC) = 7.5 J/mol.K, [gamma] = 145 mJ/mol.K2 assuming BCS value (dC/gamma*Tc) = 1.43.	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																1	2016	emu/mol	0.00178	emu.K/mol	7.91	myu-B/f.u	7.95	23.6																			ABC4D4			P4/mmm	123	A	3.8896		13.3109											Fe-1144	K	36		36.5	36.5			36.5										100										T	RES(0.9Rn)								T/K	RES(0.9Rn)	5.6			MHC156605																			MSP156605			mJ/mol.K2	145	SP													uOhm.cm							40				468			cm3/C	0.000247					MRH156605			FeAs,EuAs,RbAs,Fe		mixture - pellet - alumina crucible - sealed in Ta tube - quartz ampoule - heat to 1123-1173 K - hold(6h) - quench					Superconductivity and ferromagnetism in hole-doped RbEuFe4As4			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 93(2016)214503	Yi Liu,Ya-Bin Liu,Zhang-Tu Tang,Hao Jiang,Zhi-Cheng Wang,Abduweli Ablimit,Wen-He Jiao,Qian Tao,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
156606	PRB092220503	Superfluid density measured by mu-SR and TDO. [penet] from mu-SR. Energy gaps are (D/kTc) = 0.88 and 2.17 (in DB) from TDO results using two gap r- model (r = 0.15).	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2015																										AB4C12		skutterudite																		K		7.8					7.8																																									nm	mu-SR	122					4.34																																																See Phys.Rev.Lett., 100()017002					Weak interband-coupling superconductivity in the filled skutterudite LaPt4Ge12			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 92(2015)220503	J. L. Zhang,G. M. Pang,L. Jiao,M. Nicklas,Y. Chen,Z. F. Weng,M. Smidman,W. Schnelle,A. Leithe-Jasper,A. Maisuradze,C. Baines,R. Khasanov,A. Amato,F. Steglich,R. Gumeniuk,H. Q. Yuan		
156607	PRB092220503	[penet from mu-SR	SrPt4Ge12	Sr1Pt4Ge12	Sr	1	Pt	4	Ge	12																		1	2015																										AB4C12		skutterudite																		K		5.1					5.1																																									nm	mu-SR	238																																																					See Phys.Rev.Lett., 100()017002					Weak interband-coupling superconductivity in the filled skutterudite LaPt4Ge12			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 92(2015)220503	J. L. Zhang,G. M. Pang,L. Jiao,M. Nicklas,Y. Chen,Z. F. Weng,M. Smidman,W. Schnelle,A. Leithe-Jasper,A. Maisuradze,C. Baines,R. Khasanov,A. Amato,F. Steglich,R. Gumeniuk,H. Q. Yuan		
156608	PRB092220503	[penet from mu-SR	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																		1	2015																										AB4C12		skutterudite																		K		5.3					5.3																																									nm	mu-SR	203																																																					See Phys.Rev.Lett., 100()017002					Weak interband-coupling superconductivity in the filled skutterudite LaPt4Ge12			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 92(2015)220503	J. L. Zhang,G. M. Pang,L. Jiao,M. Nicklas,Y. Chen,Z. F. Weng,M. Smidman,W. Schnelle,A. Leithe-Jasper,A. Maisuradze,C. Baines,R. Khasanov,A. Amato,F. Steglich,R. Gumeniuk,H. Q. Yuan		
156610	PRB093214510	R = R0 + A*T^2 for T<30 K, A = 3.1E-2 uOhm.cm/K^2	SrPt3P	Sr1Pt3P1	Sr	1	Pt	3	P	1																		1	2016																										ABC3			P4/nmm		A	5.809		5.3834												K			8.98	8.35			8.35																																																																																														Pt(3N7),P(3N),Sr(98%),Pd(3N5)		mixture - pellet - sealed in quartz tube - heat(400C,10h) - CAL(900C,2d) - reground - ANN(900C, 3d, in quartz tube(Ar)					Effects of electron correlation, electron-phonon coupling, and spin-orbit coupling on the isovalent Pd-substituted superconductor SrPt3P			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Phys.Rev.B, 93(2016)214510	Kangkang Hu,Bo Gao,Qiucheng Ji,Yonghui Ma,Wei Li,Xuguang Xu,Hui Zhang,Gang Mu,Fuqiang Huang,Chuanbing Cai,Xiaoming Xie,Mianheng Jiang		
156611	PRB093214510		Sr(Pt1-xPdx)3P	Sr1Pt2.7Pd0.3P1	Sr	1	Pt	2.7	Pd	0.3	P	1																1	2016																										ABC3			P4/nmm		A	5.8138		5.3697												K			8.1	7.54			7.54	MTC156611																																																																																													Pt(3N7),P(3N),Sr(98%),Pd(3N5)		mixture - pellet - sealed in quartz tube - heat(400C,10h) - CAL(900C,2d) - reground - ANN(900C, 3d, in quartz tube(Ar)					Effects of electron correlation, electron-phonon coupling, and spin-orbit coupling on the isovalent Pd-substituted superconductor SrPt3P			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Phys.Rev.B, 93(2016)214510	Kangkang Hu,Bo Gao,Qiucheng Ji,Yonghui Ma,Wei Li,Xuguang Xu,Hui Zhang,Gang Mu,Fuqiang Huang,Chuanbing Cai,Xiaoming Xie,Mianheng Jiang		
156612	PRB093214510		Sr(Pt1-xPdx)3P	Sr1Pt2.4Pd0.6P1	Sr	1	Pt	2.4	Pd	0.6	P	1																1	2016																										ABC3			P4/nmm		A	5.8212		5.3595												K			7.34	6.57			6.57																																																																																														Pt(3N7),P(3N),Sr(98%),Pd(3N5)		mixture - pellet - sealed in quartz tube - heat(400C,10h) - CAL(900C,2d) - reground - ANN(900C, 3d, in quartz tube(Ar)					Effects of electron correlation, electron-phonon coupling, and spin-orbit coupling on the isovalent Pd-substituted superconductor SrPt3P			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Phys.Rev.B, 93(2016)214510	Kangkang Hu,Bo Gao,Qiucheng Ji,Yonghui Ma,Wei Li,Xuguang Xu,Hui Zhang,Gang Mu,Fuqiang Huang,Chuanbing Cai,Xiaoming Xie,Mianheng Jiang		
156613	PRB093214510	R = R0 + A*T^2 for T<40 K, A = 4.5E-2 uOhm.cm/K^2	Sr(Pt1-xPdx)3P	Sr1Pt2.1Pd0.9P1	Sr	1	Pt	2.1	Pd	0.9	P	1																1	2016																										ABC3			P4/nmm		A	5.8355		5.3343												K			6.38	5.78			5.78	MTC156611																																																																																													Pt(3N7),P(3N),Sr(98%),Pd(3N5)		mixture - pellet - sealed in quartz tube - heat(400C,10h) - CAL(900C,2d) - reground - ANN(900C, 3d, in quartz tube(Ar)					Effects of electron correlation, electron-phonon coupling, and spin-orbit coupling on the isovalent Pd-substituted superconductor SrPt3P			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Phys.Rev.B, 93(2016)214510	Kangkang Hu,Bo Gao,Qiucheng Ji,Yonghui Ma,Wei Li,Xuguang Xu,Hui Zhang,Gang Mu,Fuqiang Huang,Chuanbing Cai,Xiaoming Xie,Mianheng Jiang		
156614	PRB093214510		Sr(Pt1-xPdx)3P	Sr1Pt1.8Pd1.2P1	Sr	1	Pt	1.8	Pd	1.2	P	1																1	2016																										ABC3			P4/nmm		A	5.8409		5.3394												K			5.61	4.82			4.82																																																																																														Pt(3N7),P(3N),Sr(98%),Pd(3N5)		mixture - pellet - sealed in quartz tube - heat(400C,10h) - CAL(900C,2d) - reground - ANN(900C, 3d, in quartz tube(Ar)					Effects of electron correlation, electron-phonon coupling, and spin-orbit coupling on the isovalent Pd-substituted superconductor SrPt3P			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050, China	Phys.Rev.B, 93(2016)214510	Kangkang Hu,Bo Gao,Qiucheng Ji,Yonghui Ma,Wei Li,Xuguang Xu,Hui Zhang,Gang Mu,Fuqiang Huang,Chuanbing Cai,Xiaoming Xie,Mianheng Jiang		
156615	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.833K0.167Fe2As2	Ba	0.833	K	0.167	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		7					7																				T	Linear extrapolation			8.55										MHC156615																											W/K.m				MTHC156615																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156616	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.823K0.177Fe2As2	Ba	0.823	K	0.177	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		10					10																				T	Linear extrapolation			16										MHC156616																											W/K.m				MTHC156616																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156617	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.805K0.195Fe2As2	Ba	0.805	K	0.195	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		15					15																																																													W/K.m				MTHC156617																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156618	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.677K0.323Fe2As2	Ba	0.677	K	0.323	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		37					37																																																													W/K.m				MTHC156618																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156619	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.83K0.17Fe2As2	Ba	0.83	K	0.17	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		8					8																																																													W/K.m				MTHC156619																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156620	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.812K0.188Fe2As2	Ba	0.812	K	0.188	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		13					13																																																													W/K.m				MTHC156620																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156621	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.797K0.203Fe2As2	Ba	0.797	K	0.203	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		17					17																																																													W/K.m				MTHC156621																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156622	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.663K0.337Fe2As2	Ba	0.663	K	0.337	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		38					38																																																													W/K.m				MTHC156622																															self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156623	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.816K0.184Fe2As2	Ba	0.816	K	0.184	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		12					12																				T	Linear extrapolation			20.1										MHC156623																																																														self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156624	PRB093214519	K-content, x estimated from Tc using Tc = 38.5 -54(0.345-x) - 690(0.345-x)^2. Thermal conductivity measured for heat current//a and //c.	(Ba,K)Fe2As2	Ba0.788K0.212Fe2As2	Ba	0.788	K	0.212	Fe	2	As	2																3	2016																										AB2C2		ThCr2Si2																		K		19					19																				T	Linear extrapolation			35.4										MHC156624																																																														self-flux method					Doping evolution of the superconducting gap structure in the underdoped iron arsenide Ba1-xKxFe2As2 revealed by thermal conductivity			Departement de Physique and RQMP, Universite de Sherbrooke, Sherbrooke, Quebec, Canada J1K 2R1	Phys.Rev.B, 93(2016)214519	J.-Ph. Reid,M. A. Tanatar,X. G. Luo,H. Shakeripour,S. Rene de Cotret,A. Juneau-Fecteau,J. Chang,1 B. Shen,H.-H. Wen,H. Kim,R. Prozorov,N. Doiron-Leyraud,Louis Taillefer		
156625	PRB093220504	[penet], [gap] obtained from muon-SR fitting	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2016																										AB2																				K		4.84					4.84											Oe	cohere, GL theory	61																												nm	mu-SR	263			meV	0.78	3.74	16																																															single crystals grown from a melt. See Nature Commun., 6(2015)8595					Fully gapped superconductivity in the topological superconductor beta-PdBi2			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 93(2016)220504	P. K. Biswas,D. G. Mazzone,R. Sibille,E. Pomjakushina,K. Conder,H. Luetkens,C. Baines,J. L. Gavilano,M. Kenzelmann,A. Amato,E. Morenzoni		
156626	PRB093224516	RRR = 413. Diamag-signal observed at 13K by torque and C(T). Pseudogap 2d1 = 2.4 and 2d2 = 8.4 meV(2d/kTc = 11.6, 2d2/kTc = 45) by STS.	CsFe2As2	Cs1Fe2As2	Cs	1	Fe	2	As	2																		3	2016																										AB2C2		ThCr2Si2																	Fe-122	K	2.11						2.11																																																																							uOhm.cm							1.43				590														self-flux method. mixture(Cs:Fe:As = 6:1:6) - alumina crucible - sealed in Ta crucible(ar) - in quartz tube - heat to 200C - hold(6h) - heat (950C,10h) - cool to 550C(3C/h( - FC to RT					Possible superconducting fluctuation and pseudogap state above Tc in CsFe2As2			National Laboratory of Solid State Microstructures, Center for Superconducting Physics and Materials, School of Physics, Collaborative Innovation Center for Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 93(2016)224516	Huan Yang,Jie Xing,Zengyi Du,Xiong Yang,Hai Lin,Delong Fang,Xiyu Zhu,Hai-Hu Wen		
156627	PRB093245126	Tc depends on homogeneity. bulk Tc = 4.6 K(SP), Tc(on) = 4.97 K defined as R(onset).	Ca3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																		1	2016																										A3B4C13	1	Yb3Rh4Sn13	Pm3[-]n																	K		4.71	4.97				4.71			K/GPa	-0.2																T	SP, GL fitting	3.1												MHC156627		A	from Hc2	103																		mJ/mol.K2	6.1	SP	213	SP																																				arc-melting - ANN(870C,2w)					Effect of atomic disorder and Ce doping on superconductivity of Ca3Rh4Sn13: Electric transport properties under high pressure			Institute of Physics, University of Silesia, Uniwersytecka 4, 40-007 Katowice, Poland	Phys.Rev.B, 93(2016)245126	A. Slebarski,J. Goraus,M. M. Maska,P. Witas,M. Fija?kowski,C. T. Wolowiec,Y. Fang,M. B. Maple		
156628	PRB093245126	Hc2 defined as Tc(onset)	Ca3-xCoxRh4Sn13	Ca2.8Co0.2Rh4Sn13	Ca	2.8	Co	0.2	Rh	4	Sn	13																1	2016	emu/mol-Ce	0.00037	emu.K/mol	0.807			31																			A3B4C13	1	Yb3Rh4Sn13	Pm3[-]n																	K			7.73				7.73	MTC156628		K/GPa	-0.3																T	RES(on), GL-fitting	3.6												MHC156628		A	from Hc2	90																																																										arc-melting - ANN(870C,2w)					Effect of atomic disorder and Ce doping on superconductivity of Ca3Rh4Sn13: Electric transport properties under high pressure			Institute of Physics, University of Silesia, Uniwersytecka 4, 40-007 Katowice, Poland	Phys.Rev.B, 93(2016)245126	A. Slebarski,J. Goraus,M. M. Maska,P. Witas,M. Fija?kowski,C. T. Wolowiec,Y. Fang,M. B. Maple		
156629	PRB093245126	Hc2 defined as Tc(onset)	Ca3-xCoxRh4Sn13	Ca2.5Co0.5Rh4Sn13	Ca	2.5	Co	0.5	Rh	4	Sn	13																1	2016																										A3B4C13	1	Yb3Rh4Sn13	Pm3[-]n																	K		6.41					6.41																				T	RES(on), GL-fitting	4												MHC156629		A	from Hc2	96																																																										arc-melting - ANN(870C,2w)					Effect of atomic disorder and Ce doping on superconductivity of Ca3Rh4Sn13: Electric transport properties under high pressure			Institute of Physics, University of Silesia, Uniwersytecka 4, 40-007 Katowice, Poland	Phys.Rev.B, 93(2016)245126	A. Slebarski,J. Goraus,M. M. Maska,P. Witas,M. Fija?kowski,C. T. Wolowiec,Y. Fang,M. B. Maple		
156630	PRB094014509	T<STR> = 46.2 K from R(T). R(T) = R(0) + A*T^n : n= 1.55.	NaFe1-xCoxAs	Na1Fe0.99Co0.01As1	Na	1	Fe	0.99	Co	0.01	As	1																3	2016																										ABC		PbFCl																		K		0					0																																																																							mOhm.cm							0.417				0.778																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156631	PRB094014509	T<STR> = 43.2 K from NRD and 45.2 K from R(T).  R(T) = R(0) + A*T^n : n= 1.38.	NaFe1-xCoxAs	Na1Fe0.9875Co0.0125As1	Na	1	Fe	0.9875	Co	0.0125	As	1																3	2016								30.1																		ABC		PbFCl																		K			13.9				13.9																																																																							mOhm.cm							0.371				0.789																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156632	PRB094014509	T<STR> = 44.1  K from NRD.  R(T) = R(0) + A*T^n : n= 1.32.	NaFe1-xCoxAs	Na1Fe0.985Co0.015As1	Na	1	Fe	0.985	Co	0.015	As	1																3	2016								30.6																		ABC		PbFCl																		K		12.6	13.4				12.6	MPH156632																																																																						mOhm.cm							0.46				1.015																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156633	PRB094014509	T<STR> = 41.2 K from R(T).  R(T) = R(0) + A*T^n : n= 1.28.	NaFe1-xCoxAs	Na1Fe0.9825Co0.0175As1	Na	1	Fe	0.9825	Co	0.0175	As	1																3	2016								28.5																		ABC		PbFCl																		K			15.8				15.8																																																																							mOhm.cm							0.526				1.144																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156634	PRB094014509	R(T) = R(0) + A*T^n : n= 1.20.	NaFe1-xCoxAs	Na1Fe0.981Co0.019As1	Na	1	Fe	0.981	Co	0.019	As	1																3	2016																										ABC		PbFCl																		K		19.3	16.1				19.3																																																																							mOhm.cm							0.732				1.6																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156635	PRB094014509	R(T) = R(0) + A*T^n : n= 1.35.	NaFe1-xCoxAs	Na1Fe0.977Co0.023As1	Na	1	Fe	0.977	Co	0.023	As	1																3	2016								28																		ABC		PbFCl																		K			15.7				15.7																																																																							mOhm.cm							0.546				1.1																			Electron doping evolution of structural and antiferromagnetic phase transitions in NaFe1-xCoxAs iron pnictides			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 94(2016)014509	Guotai Tan,Yu Song,Chenglin Zhang,Lifang Lin,Zhuang Xu,Tingting Hou,Wei Tian,Huibo Cao,Shiliang Li,Shiping Feng,Pengcheng Dai		
156636	PRB094024106	magnetic moment shows coexistence of SC and FM.	NiSm	Ni1Sm1	Ni	1	Sm	1																				4	2016							27																																							K	0.7		2.5				1.6																																																																																												n/cm3	2000000000000000000000			Films prepared by MBE method. High purity Sm evaporated in 3E-4 mbar N2. Epitaxial films on aluminium nitride(AIN) substrate (400-500C)					Superconductivity in the ferromagnetic semiconductor samarium nitride			MacDiarmid Institute for Advanced Materials and Nanotechnology, School of Chemical and Physical Sciences, Victoria University of Wellington, P. O. Box 600, Wellington 6140, New Zealand	Phys.Rev.B, 94(2016)024106	E.-M. Anton,S. Granville,A. Engel,S. V. Chong,M. Governale,U. Zulicke,A. G. Moghaddam,H. J. Trodahl,F. Natali,S. Vezian,B. J. Ruck		
156637	PRB094024106	Superlattice films (10 nm-GdN/5 nm SmN)*12Tc increases and Curie-T increases higher than SmN films	GdSmN2	Gd1Sm1Ni2	Gd	1	Sm	1	Ni	2																		5	2016							70																																							K	4.2		4.8				4.5																				T	RES													MHC156637																																																														Films prepared by MBE method. High purity Sm evaporated in 3E-4 mbar N2. Epitaxial films on aluminium nitride(AIN) substrate (400-500C)					Superconductivity in the ferromagnetic semiconductor samarium nitride			MacDiarmid Institute for Advanced Materials and Nanotechnology, School of Chemical and Physical Sciences, Victoria University of Wellington, P. O. Box 600, Wellington 6140, New Zealand	Phys.Rev.B, 94(2016)024106	E.-M. Anton,S. Granville,A. Engel,S. V. Chong,M. Governale,U. Zulicke,A. G. Moghaddam,H. J. Trodahl,F. Natali,S. Vezian,B. J. Ruck		
156638	PRB094024518	RRR = 1.08, demag-factor = 0.14. kappa(GL) = 50.2. Hc(0) = 1.26 kOe. Lattice term in SP (beta) = 0.43 mJ/mol.K4, (delta) = 0.9 mJ/mol.K6. (dC/Tc) = 41.3 mJ/mol.K2. (dC/gamma*Tc = 1.63	Re6Hf	Hf1Re6	Hf	1	Re	6																				1	2016																										AB6		alpha-Mn	I4[-]3m		A	9.678														K	6.2		6.4	6.2		0.2	6.2											Oe	M-H curve, 1-t^2 fitting	74							T	RES(0.9Rn), WHH	8.9							T/K	RES(0.9Rn)	2.09			MHC156638		A	from Hc2	61.2			nm	Hc1, GL eq.	306										MSP156638			mJ/mol.K2	25.3	SP	316	SP																																		Re(3N),Hf(3N)		arc-melting - ANN in quartz tube (1123 K, 1w, in vac) - cool to RT within 24h					Superconductivity in the noncentrosymmetric compound Re6Hf			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, China	Phys.Rev.B, 94(2016)024518	Bin Chen,Yang Guo,Hangdong Wang,Qiping Su,Qianhui Mao,Jianhua Du,Yuxing Zhou,Jinhu Yang,Minghu Fang		
156639	PRB094035130	Compositions Y:Pt:Bi = 28.3:38:33.7 by EDX. Carrier = 5.6E+18 /cm3 for T<50K. Hall mobility = 1100 cm2/V.s for T<50K. Schottky term in SP = 0.052/T2 mJ/mol.K	YPtBi	Y1Pt1Bi1	Y	1	Pt	1	Bi	1																		3	2016																										ABC		MgAgAs	F4[-]3m		A	6.65													MgAgAs-type, Halh Heusler	K	0.85	0.97		0.86		0.45	0.97																				T	RES(0.9Rn), extrapolation	1.6			0.9			0.4								A	from Hc2	140																		mJ/mol.K2	0.69	SP	222	SP											mOhm.cm							0.88				0.52										n/cm3	340000000000000000000			Bi-flux method. YBi by arc-melting - crush - mixed with Pt and Bi - alumina crucible - sealed in quartz tube - heat(1130C,12h) - cool to 925C(3C/h) - keep(12h) - cool to 550C(1C/h) - remove Bi					Superconductivity and Shubnikov-de Haas oscillations in the noncentrosymmetric half-Heusler compound YPtBi			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P. O. Box 1410, 50-950 Wroc?aw, Poland	Phys.Rev.B, 94(2016)035130	Orest Pavlosiuk,Dariusz Kaczorowski,Piotr Wisniewski		
156640	PRB094041114	Carrier from Hall effect. Multiple Fermi pockets observed using torque magnetometry upto H = 45 T.	NbxBi2Se3	Nb0.25Bi2Se3	Nb	0.25	Bi	2	Se	3																		3	2016																																														K	3		3.55				3.275										90																																																													mOhm.cm							0.075														n/cm3	240000000000000000000								Multiple Fermi surfaces in superconducting Nb-doped Bi2Se3			Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, USA	Phys.Rev.B, 94(2016)041114	B. J. Lawson,Paul Corbae,Gang Li,Fan Yu,Tomoya Asaba,Colin Tinsman,Y. Qiu,J. E. Medvedeva,Y. S. Hor,Lu Li		
156641	PRB094041114	Carrier from Hall effect. Multiple Fermi pockets observed using torque magnetometry upto H = 45 T.	NbxBi2Se3	Nb0.28Bi2Se3	Nb	0.28	Bi	2	Se	3																		3	2016																																														K	3.13		3.57				3.35										60																																																													mOhm.cm							0.131														n/cm3	180000000000000000000								Multiple Fermi surfaces in superconducting Nb-doped Bi2Se3			Department of Physics, University of Michigan, Ann Arbor, Michigan 48109, USA	Phys.Rev.B, 94(2016)041114	B. J. Lawson,Paul Corbae,Gang Li,Fan Yu,Tomoya Asaba,Colin Tinsman,Y. Qiu,J. E. Medvedeva,Y. S. Hor,Lu Li		
156642	PRB094045131	not SC. RRR = 17.4. T<CDW> = 470 K.	1T-TaSe2-xTex	Se2Ta1	Se	2	Ta	1																				3	2016																										AB2		TX2			A	3.4737		6.2381											1T-TaX2 type	K																																																																																																					Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156643	PRB094045131	T<CDW> = 354 K.	1T-TaSe2-xTex	Ta1Se1.7Te0.3	Ta	1	Se	1.7	Te	0.3																		3	2016																										AB2		TX2			A	3.4941		6.3479											1T-TaX2 type	K	0		1.57				0.785																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156644	PRB094045131	T<CDW> = 329 K.	1T-TaSe2-xTex	Ta1Se1.6Te0.4	Ta	1	Se	1.6	Te	0.4																		3	2016																										AB2		TX2			A	3.5019		6.3883											1T-TaX2 type	K	0		2.4				1.2																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156645	PRB094045131	T<CDW> = 276 K.	1T-TaSe2-xTex	Ta1Se1.5Te0.5	Ta	1	Se	1.5	Te	0.5																		3	2016																										AB2		TX2																	1T-TaX2 type	K	0		2.4				1.2																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156646	PRB094045131	optimal concentration	1T-TaSe2-xTex	Ta1Se1.4Te0.6	Ta	1	Se	1.4	Te	0.6																		3	2016																										AB2		TX2			A	3.5273		6.4611											1T-TaX2 type	K	1.6		2.5				2.05	MTC156646																																																																																													Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156647	PRB094045131		1T-TaSe2-xTex	Ta1Se1.2Te0.8	Ta	1	Se	1.2	Te	0.8																		3	2016																										AB2		TX2			A	3.5473		6.5049											1T-TaX2 type	K	0.78		2.39				1.585																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156648	PRB094045131	RRR = 0.85	1T-TaSe2-xTex	Ta1Se1Te1	Ta	1	Se	1	Te	1																		3	2016																										AB2		TX2			A	3.5678		6.5441											1T-TaX2 type	K	0.66		2.23				1.445																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156649	PRB094045131		1T-TaSe2-xTex	Ta1Se0.8Te1.2	Ta	1	Se	0.8	Te	1.2																		3	2016																										AB2		TX2			A	3.5958		6.5996											1T-TaX2 type	K	0.5		1.83				1.165																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156650	PRB094045131		1T-TaSe2-xTex	Ta1Se0.7Te1.3	Ta	1	Se	0.7	Te	1.3																		3	2016																										AB2		TX2			A	3.602		6.6185											1T-TaX2 type	K	0		0.54				0.27																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156651	PRB094045131	not SC.	1T-TaSe2-xTex	Ta1Se0.6Te1.4	Ta	1	Se	0.6	Te	1.4																		3	2016																										AB2		TX2			A	3.6143		6.6472											1T-TaX2 type	K			0				0																																																																																														Ta(4N),Se(4N),Te(4N)		CVT method. Mixture - heat(900C,4d,in quartz tube. (TaSe2-xTex powder + Iodine(5mg/cm3)) - heat(950C(H) - 850C(L), two zone furnace)					Nature of charge density waves and superconductivity in 1T-TaSe2-xTex			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.B, 94(2016)045131	Y. Liu,D. F. Shao,L. J. Li,W. J. Lu,X. D. Zhu,P. Tong,R. C. Xiao,L. S. Ling,C. Y. Xi,L. Pi,H. F. Tian,H. X. Yang,J. Q. Li,W. H. Song,X. B. Zhu,Y. P. Sun2		
156652	PRB094054508		La(Fe,Mn)AsO0.89F0.11	La1Fe0.99975Mn0.00025As1F0.11O0.89	La	1	Fe	0.99975	Mn	0.00025	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		22.6					22.6																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156653	PRB094054508		La(Fe,Mn)AsO0.89F0.11	La1Fe0.99925Mn0.00075As1F0.11O0.89	La	1	Fe	0.99925	Mn	0.00075	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		14.4					14.4																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156654	PRB094054508	magnetic order not observed, Tm = 0 K.	La(Fe,Mn)AsO0.89F0.11	La1Fe0.999Mn0.001As1F0.11O0.89	La	1	Fe	0.999	Mn	0.001	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		9.67					9.67	MTC156654																																																																																															Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156655	PRB094054508	magnetic order Tm = 7.1 K.	La(Fe,Mn)AsO0.89F0.11	La1Fe0.998Mn0.002As1F0.11O0.89	La	1	Fe	0.998	Mn	0.002	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156656	PRB094054508	magnetic order Tm = 81.5 K.	La(Fe,Mn)AsO0.89F0.11	La1Fe0.995Mn0.005As1F0.11O0.89	La	1	Fe	0.995	Mn	0.005	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156657	PRB094054508	magnetic order Tm = 64.3 K.	La(Fe,Mn)AsO0.89F0.11	La1Fe0.9924Mn0.0076As1F0.11O0.89	La	1	Fe	0.9924	Mn	0.0076	As	1	F	0.11											O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156658	PRB094054508		La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.997Mn0.003As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.997	Mn	0.003	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		28.5					28.5																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156659	PRB094054508		La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.992Mn0.008As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.992	Mn	0.008	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		22.7					22.7	MTC156659																																																																																															Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156660	PRB094054508		La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.98Mn0.02As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.98	Mn	0.02	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		14.1					14.1																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156661	PRB094054508		La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.975Mn0.025As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.975	Mn	0.025	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		10.1					10.1																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156662	PRB094054508	magnetic order Tm = 0 K. from muon-SR	La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.96Mn0.06As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.96	Mn	0.06	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156663	PRB094054508	magnetic order Tm = 4.6 K. from muon-SR	La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.9Mn0.1As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.9	Mn	0.1	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156664	PRB094054508	magnetic order Tm = 8.2 K.  from muon-SR	La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.85Mn0.15As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.85	Mn	0.15	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156665	PRB094054508	magnetic order Tm = 18.9 K.  from muon-SR	La0.8Y0.2(Fe,Mn)AsO0.89F0.11	La0.8Y0.2Fe0.8Mn0.2As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.8	Mn	0.2	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K					0																																																																																																		Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156666	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.995Y0.005Fe0.995Mn0.005As1F0.11O0.89	La	0.995	Y	0.005	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		2.89					2.89																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156667	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.99Y0.01Fe0.995Mn0.005As1F0.11O0.89	La	0.99	Y	0.01	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		7.5					7.5																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156668	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.95Y0.05Fe0.995Mn0.005As1F0.11O0.89	La	0.95	Y	0.05	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		18.6					18.6	MTC156668																																																																																															Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156669	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.9Y0.1Fe0.995Mn0.005As1F0.11O0.89	La	0.9	Y	0.1	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		24.1					24.1																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156670	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.8Y0.2Fe0.995Mn0.005As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		26.6					26.6																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156671	PRB094054508		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.77Y0.23Fe0.995Mn0.005As1F0.11O0.89	La	0.77	Y	0.23	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2016																										ABCD		oxypnictide																	Fe-1111	K		27.9					27.9																																																																																																Two step solid state reaction					Competing effects of Mn and Y doping on the low-energy excitations and phase diagram of La1-yYyFe1-xMnxAsO0.89F0.11 iron-based superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B, 94(2016)054508	M. Moroni,S. Sanna,G. Lamura,T. Shiroka,R. De Renzi,R. Kappenberger,M. A. Afrassa,S. Wurmehl,A. U. B. Wolter,B. Buchner,P. Carretta		
156672	PRB094144515	RRR = 1.1. Lattice term in SP (beta) = 0.451 mJ/mol.K4. (dC/gamma*Tc) = 1.62. penet(London) = 2200 A.  kappa(GL) = 69.3	Re6Zr	Re6Zr1	Re	6	Zr	1																				1	2016																										AB6	1	alpha-Mn	I4[-]3m	217	A	9.6989													non-centrosymmetry	K		6.7		6.6		0.05	6.7			K/GPa	-0.07							mT		8							T	RES(0.5Rn), WHH	11.6												MHC156672		A	from Hc2	53.3			A	Hc1, GL theory	3696										MSP156672			mJ/mol.K2	27.5	SP			W/K.m	8.5			MTHC156672						uOhm.cm							135				150												Re(4N),Zr(4N)		arc-melting					Complex superconductivity in the noncentrosymmetric compound Re6Zr			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70808, USA	Phys.Rev.B, 94(2016)144515	Mojammel A. Khan,A. B. Karki,T. Samanta,D. Browne,S. Stadler,I. Vekhter,Abhishek Pandey,P. W. Adams,D. P. Young,S. Teknowijoyo,K. Cho,R. Prozorov,D. E. Graf		
156673	PRB094144516	RRR = 1.8(P=0) to 2.3(P=1.7GPa).  Hc2(T,P) measured for H//a-axis , I along a-axis. Anisotropy (Hc2(a)/Hc2(a*) = 5.36 for P=1.72 GPa, T=0.5 K)	Sr0.15Bi2Se3	Sr0.15Bi2Se3	Sr	0.15	Bi	2	Se	3																		3	2016																																														K		3.05					3.05	MTC156673																			T	RES(0.5Rn)													MHC156673																																																														stoichiometric mixture - melt(850C, in sealed quartz) - slow cool to 650C (3C/h)					High-pressure study of the basal-plane anisotropy of the upper critical field of the topological superconductor SrxBi2Se3			Van der Waals - Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Phys.Rev.B, 94(2016)144516	A. M. Nikitin,Y. Pan,Y. K. Huang,T. Naka,A. de Visser		
156674	PRB094144516	RRR = 1.8(P=0) to 3.72(P=2.1GPa). Hc2(T,P) measured for H//a*-axis , I along a-axis. Anisotropy (Hc2(a)/Hc2(a*) = 4.77 for P=1.72 GPa, T=0.84 K)	Sr0.15Bi2Se3	Sr0.15Bi2Se3	Sr	0.15	Bi	2	Se	3																		3	2016																																														K		3.06					3.06	MTC156674																																	MHC156674																																																														stoichiometric mixture - melt(850C, in sealed quartz) - slow cool to 650C (3C/h)					High-pressure study of the basal-plane anisotropy of the upper critical field of the topological superconductor SrxBi2Se3			Van der Waals - Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Phys.Rev.B, 94(2016)144516	A. M. Nikitin,Y. Pan,Y. K. Huang,T. Naka,A. de Visser		
156675	PRB094174505	Low-Tc phase R not to zero at 2K. M = NH3 intercalated. M0.03Na0.7Fe1.33Se0.48Te0.52 by EDX	(NH3)yNaxFeSe0.5Te0.5	M1Na0.3Fe1Se0.5Te0.5	M	1	Na	0.3	Fe	1	Se	0.5	Te	0.5														1	2016																													I4/mmm		A	3.9824		17.789												K		21	23				21										100	Oe		100							T	RES(on), WHH	34							T/K		1.76			MHC156675		A	from Hc2	31			nm	Hc1, GL theory	260																																																					beta-FeSe0.5Te0.5 prepared using liquid NH3 technique.					Superconductivity in (NH3)yNaxFeSe0.5Te0.5			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 94(2016)174505	Lu Zheng,Yusuke Sakai,Xiao Miao,Saki Nishiyama,Takahiro Terao,Ritsuko Eguchi,Hidenori Goto,Yoshihiro Kubozono		
156676	PRB094174505	High-Tc phase. R not to zero at 2K. M = NH3 intercalated. M0.63Na0.63Fe0.85Se0.55Te0.44 by EDX.	(NH3)yNaxFeSe0.5Te0.5	M1Na0.3Fe1Se0.5Te0.5	M	1	Na	0.3	Fe	1	Se	0.5	Te	0.5														1	2016																													I4/mmm		A	4.029		16.84												K		27	31				27										84	Oe	M-H curve				200			10	T	RES(on), WHH	20							T/K		0.94			MHC156676		A	from Hc2	41			nm	Hc1, GL theory	180																																																					beta-FeSe0.5Te0.5 prepared using liquid NH3 technique.					Superconductivity in (NH3)yNaxFeSe0.5Te0.5			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 94(2016)174505	Lu Zheng,Yusuke Sakai,Xiao Miao,Saki Nishiyama,Takahiro Terao,Ritsuko Eguchi,Hidenori Goto,Yoshihiro Kubozono		
156677	PRB094184504	[penet]  from M-H curve analysis for H//c-axis. Energy gap  obtained from curve fitting superfluid density using fully gap model.	Ir0.95Pt0.05Te2	Ir0.95Pt0.05Te2	Ir	0.95	Pt	0.05	Te	2																		3	2016																										AB2																				K				2.92			2.92																																									nm	Magnetization analysis			91		0.463	3.7																																																self-flux method					mu-SR and magnetometry study of superconducting 5% Pt-doped IrTe2			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada	Phys.Rev.B, 94(2016)184504	M. N. Wilson,T. Medina,T. J. Munsie,S. C. Cheung,B. A. Frandsen,L. Liu,J. Yan,D. Mandrus,Y. J. Uemura,G. M. Luke		
156678	PRB094184504	[penet]  from M-H curve analysis for H perpendicular to c-axis. Energy gap  obtained from curve fitting superfluid density using fully gap model.	Ir0.95Pt0.05Te2	Ir0.95Pt0.05Te2	Ir	0.95	Pt	0.05	Te	2																		3	2016																										AB2																				K				2.84			2.84																																									nm	Magnetization analysis		125			0.463	3.9																																																self-flux method					mu-SR and magnetometry study of superconducting 5% Pt-doped IrTe2			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada	Phys.Rev.B, 94(2016)184504	M. N. Wilson,T. Medina,T. J. Munsie,S. C. Cheung,B. A. Frandsen,L. Liu,J. Yan,D. Mandrus,Y. J. Uemura,G. M. Luke		
156679	PRB094184504	poly crystal. [penet] from muon-SR. Energy gap  obtained from curve fitting superfluid density using fully gap model.	Ir0.95Pt0.05Te2	Ir0.95Pt0.05Te2	Ir	0.95	Pt	0.05	Te	2																		1	2016																										AB2																				K				2.29			2.29																				mT	SUS				135			0.46													nm	muon analysis	154				0.467	4.7																																																					mu-SR and magnetometry study of superconducting 5% Pt-doped IrTe2			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario L8S 4M1, Canada	Phys.Rev.B, 94(2016)184504	M. N. Wilson,T. Medina,T. J. Munsie,S. C. Cheung,B. A. Frandsen,L. Liu,J. Yan,D. Mandrus,Y. J. Uemura,G. M. Luke		
156680	PRB094180509	Impurity phases: KCl(4.5%), KClO3(0.5%). hole conc. = 0.46 (overdoped sample. (dC/Tc) = 20 mJ/mol.K2. (dC) = 1.6 J/mol.K	(Cu,Mo)Sr2YCu2O7.54	Y1Sr2Mo0.25Cu2.75O7.54	Y	1	Sr	2	Mo	0.25	Cu	2.75													O	z	7.54	1	2016																												Cu1212			A			11.455											(Cu,Mo)-1212	K		78					78																																																																																														Y2O3,CuO,SrCO3,MoO3		sol-gel method. - CAL(600C,12h) - pellet - ANN(980C,2x24h). oxidation: mixed powder sample with KClO3(35 mol%) - heat(500C, P = 4 GPa)					Bulk superconductivity at 84 K in the strongly overdoped regime of cuprates			IMPMC, Sorbonne Universites-UPMC, CNRS, IRD, MNHN, 4, place Jussieu, F-75005 Paris, France	Phys.Rev.B, 94(2016)180509	A. Gauzzi,Y. Klein,M. Nisula,M. Karppinen,P. K. Biswas,H. Saadaoui,E. Morenzoni,P. Manuel,D. Khalyavin,M. Marezio,T. H. Geballe		
156681	PRB094184506	Hydrostatic P = 0 kbar. P-dependence of T<STR> shown in FIG-data. T<STR> = 275 K. T<CDW> > 300K.	BaPt2As2	Ba1Pt2As2	Ba	1	Pt	2	As	2																		3	2016																										AB2C2		CaBe2Ge2	P4/nmm		A	4.5608	4.5643	10.042											at 100K, a = 4.5489, b = 4.5700, c = 10.0192	K		1.6					1.6	MTC156681																			T	RES(mid)													MHC156681																																					uOhm.cm							174																		self-flux method					Superconductivity and multiple pressure-induced phases in BaPt2As2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 94(2016)184506	C. Y. Guo,W. B. Jiang,M. Smidman,F. Han,C. D. Malliakas,B. Shen,Y. F. Wang,Y. Chen,X. Lu,M. G. Kanatzidis,H. Q. Yuan		
156682	PRB094184506	Hydrostatic P = 7 kbar. P-dependence of T<STR> shown in FIG-data. T<STR> = 217 K.	BaPt2As2	Ba1Pt2As2	Ba	1	Pt	2	As	2																		3	2016																										AB2C2		CaBe2Ge2	P4/nmm																	K		2.13					2.13																																																																														160																		self-flux method					Superconductivity and multiple pressure-induced phases in BaPt2As2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 94(2016)184506	C. Y. Guo,W. B. Jiang,M. Smidman,F. Han,C. D. Malliakas,B. Shen,Y. F. Wang,Y. Chen,X. Lu,M. G. Kanatzidis,H. Q. Yuan		
156683	PRB094184506	Hydrostatic P = 19 kbar. P-dependence of T<STR> shown in FIG-data. T<STR> = 101 K. 2nd T<STR> = 270 K appears.	BaPt2As2	Ba1Pt2As2	Ba	1	Pt	2	As	2																		3	2016																										AB2C2		CaBe2Ge2	P4/nmm																	K		3.8					3.8																																																																														78.1																		self-flux method					Superconductivity and multiple pressure-induced phases in BaPt2As2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 94(2016)184506	C. Y. Guo,W. B. Jiang,M. Smidman,F. Han,C. D. Malliakas,B. Shen,Y. F. Wang,Y. Chen,X. Lu,M. G. Kanatzidis,H. Q. Yuan		
156684	PRL100017002	RRR = 33. (dC/gamma*Tc) = 1.49. T<Einstain> = 96 K.  Energy gap estimated from SP.	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																		1	2008																										AB4C12		akutterudite	Im3[-]		A	8.6235													LaFe4P12 type	K				8.29			8.29																				T	SP-jump(mid), extrapolation	1.6												MHC156684														1.94	14							mJ/mol.K2	75.8	SP	209	SP											uOhm.cm							5.3				177														arc-melting - sealed in Ta ampoule - ANN(800C,7d)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156685	PRL100017002	RRR = 42. (dC/gamma*Tc) = 1.56. Energy gap estimated from SP.	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2008					myu-B/Pr	3.67	-16.4																			AB4C12		akutterudite	Im3[-]		A	8.6111													LaFe4P12 type	K				7.92			7.92																				T	SP-jump(mid), extrapolation	2.06												MHC156685														2.35	14							mJ/mol.K2	87.1	SP	198	SP											uOhm.cm							2.6				110														arc-melting - sealed in Ta ampoule - ANN(800C,7d)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156686	PRL100017002	RRR = 4.78. (dC/gamma*Tc) = 1.13.	SrPt4Ge12	Sr1Pt4Ge12	Sr	1	Pt	4	Ge	12																		1	2008																										AB4C12		akutterudite	Im3[-]		A	8.6509													LaFe4P12 type	K				5.4			5.4																																																								mJ/mol.K2	39.9	SP	198	SP											uOhm.cm							50				239														arc-melting - sealed in Ta ampoule - ANN(800C,7d)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156687	PRL100017002	RRR = 5.3. (dC/gamma*Tc) = 1.17.	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																		1	2008																										AB4C12		akutterudite	Im3[-]		A	8.6838													LaFe4P12 type	K				4.98			4.98																																																								mJ/mol.K2	34	SP	209	SP											uOhm.cm							36				191														arc-melting - sealed in Ta ampoule - ANN(800C,7d)					Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156688	PRL100017002	data from ref. 16 ( R.Gumeniuk et al unpublished) in PRL100017002	EuPt4Ge12	Eu1Pt4Ge12	Eu	1	Pt	4	Ge	12																		1	2008								1.7																		AB4C12		akutterudite	Im3[-]		A	8.6363													LaFe4P12 type	K					0.48																																																																																																							Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156689	PRL100017002	data from ref. 16 ( R.Gumeniuk et al unpublished) in PRL100017002	NdPt4Ge12	Nd1Pt4Ge12	Nd	1	Pt	4	Ge	12																		1	2008								0.67																		AB4C12		akutterudite	Im3[-]		A	8.6074													LaFe4P12 type	K					0.48																																																																																																							Superconductivity in the Platinum Germanides MPt4Ge12 (M = Rare-Earth or Alkaline-Earth Metal) with Filled Skutterudite Structure			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Str. 40, 01187 Dresden, Germany	Phys.Rev.Lett., 100(2008)017002	R. Gumeniuk,W. Schnelle,H. Rosner,M. Nicklas,A. Leithe-Jasper,Yu. Grin		
156690	SCIR00512774	NaxMy-intercalated FeSe. M = NH3. Low Tc phase (y = 0.2 - 0.6).	Nax(NH3)yFeSe	Na0.1M0.3Fe1Se1	Na	0.1	M	0.3	Fe	1	Se	1																	2015																												I4/mmm			A	3.912		14.145												K			35	32.5			32.5										30.5																																																																																											Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156691	SCIR00512774	High-Tc (single phase) phase.	Nax(NH3)yFeSe	Na1M0.3Fe1Se1	Na	1	M	0.3	Fe	1	Se	1																	2015																												I4/mmm			A	3.8266		17.565												K			47	46			46										26																																																																																											Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156692	SCIR00512774	Two phases : high-Tc phase (Tc= 45 K) and low-Tc phase (Tc = 32 K).	Nax(NH3)yFeSe	Na0.7M0.3Fe1Se1	Na	0.7	M	0.3	Fe	1	Se	1																	2015																												I4/mmm																		K			45				45	MTC156692																																																																																																				Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156693	SCIR00512774	LixMy-intercalated FeSe. M = NH3. y-value not given.	Lix(NH3)yFeSe	Li0.1M0.3Fe1Se1	Li	0.1	M	0.3	Fe	1	Se	1																	2015																																														K			42	39.5			39.5																																																																																																					Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156694	SCIR00512774	LixMy-intercalated FeSe. M = NH3. y-value not given.	Lix(NH3)yFeSe	Li0.3M0.3Fe1Se1	Li	0.3	M	0.3	Fe	1	Se	1																	2015																																														K																																																																																																												Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156695	SCIR00512774	LixMy-intercalated FeSe. M = NH3. y-value not given.	Lix(NH3)yFeSe	Li0.5M0.3Fe1Se1	Li	0.5	M	0.3	Fe	1	Se	1																	2015																																														K								MTC156695																																																																																																				Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156696	SCIR00512774	LixMy-intercalated FeSe. M = NH3. y-value not given.	Lix(NH3)yFeSe	Li0.7M0.3Fe1Se1	Li	0.7	M	0.3	Fe	1	Se	1																	2015																																														K																																																																																																												Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156697	SCIR00512774	LixMy-intercalated FeSe. M = NH3. y-value not given.	Lix(NH3)yFeSe	Li0.9M0.3Fe1Se1	Li	0.9	M	0.3	Fe	1	Se	1																	2015																																														K																																																																																																												Emergence of Multiple Superconducting Phases in (NH3)yMxFeSe (M: Na and Li)			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Reports, 5(2015)12774	Lu Zheng,Xiao Miao,Yusuke Sakai,Masanari Izumi,Hidenori Goto,Saki Nishiyama,Eri Uesugi,Yuichi Kasahara,Yoshihiro Iwasa,Yoshihiro Kubozono		
156698	SCM0580016	Lattice term in SP (beta) = 3.8 mJ/fu.K4	Cs2Cr3As3	Cs2Cr3As3	Cs	2	Cr	3	As	3																		1	2015	emu/fu	0.002			myu-B/Cr	0.14	-5.5																			A2B3C3		K2Cr3As3	P6[-]m2		A	10.605		4.2478												K	1.5		2.2			0.43	1.85										6										T	RES(0.9Rn), GL	6.45			6			0.44						MHC156698																						mJ/f.u.K2	39	SP	160	SP																																									Superconductivity in quasi-one-dimensional Cs2Cr3As3 with large interchain distance			Department of Physics, Zhejiang University, Hangzhou 310027, China	Sci.China Mater., 58(2015)16	Zhang-Tu Tang,Jin-Ke Bao,Zhen Wang,Hua Bai,Hao Jiang,Yi Liu,Hui-Fei Zhai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
156699	SSC2450011		LaOBiS2	La1Bi1S2O1	La	1	Bi	1	S	2															O	1		1	2016																												CeOBiS2																		K					1.3																																																																																																R2S3,Bi2S3,Bi2O3(3N)		mixture - sealed in quartz tube(vac) - heat(700C,10h) - reground - pellet - sealed in quartz tube(vac) - heat(700C,20h)  - FC to RT					Superconductivity in CeOBiS2 with cerium valence fluctuation			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 245(2016)11	Masanori Nagao,Akira Miura,Ikuo Ueta,Satoshi Watauch,Isao Tanaka		
156700	SSC2450011		CeOBiS2	Ce1Bi1S2O1	Ce	1	Bi	1	S	2															O	1		1	2016																												CeOBiS2																		K	1.3		1.9				1.6																																																																																														R2S3,Bi2S3,Bi2O3(3N)		mixture - sealed in quartz tube(vac) - heat(700C,10h) - reground - pellet - sealed in quartz tube(vac) - heat(700C,20h)  - FC to RT					Superconductivity in CeOBiS2 with cerium valence fluctuation			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 245(2016)11	Masanori Nagao,Akira Miura,Ikuo Ueta,Satoshi Watauch,Isao Tanaka		
156701	SSC2450011		PrOBiS2	Pr1Bi1S2O1	Pr	1	Bi	1	S	2															O	1		1	2016																												CeOBiS2																		K					1.3																																																																																																R2S3,Bi2S3,Bi2O3(3N)		mixture - sealed in quartz tube(vac) - heat(700C,10h) - reground - pellet - sealed in quartz tube(vac) - heat(700C,20h)  - FC to RT					Superconductivity in CeOBiS2 with cerium valence fluctuation			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 245(2016)11	Masanori Nagao,Akira Miura,Ikuo Ueta,Satoshi Watauch,Isao Tanaka		
156702	SSC2450011	R(T) measured at 2.0 =< T =< 5.0 K, for H//ab and H//c ( H =< 0.3 T). R(onset) around 3K, but R not to zero at T=2 K.	CeOBiS2	Ce1Bi1S2O1	Ce	1	Bi	1	S	2															O	1		3	2016																												CeOBiS2																		K			3				3																																																																																																single crystals grown by CsCl flux method					Superconductivity in CeOBiS2 with cerium valence fluctuation			University of Yamanashi, 7-32 Miyamae, Kofu, Yamanashi 400-8511, Japan	Solid State Commun., 245(2016)11	Masanori Nagao,Akira Miura,Ikuo Ueta,Satoshi Watauch,Isao Tanaka		
156703	SST029035011	RRR = 22. lattice term in SP (beta) = 0.127 mJ/mol.K4. (dC/gamma*Tc) = 1.4. Hc(0) = 9.95 mT. e-ph = 0.441. DOS = 3.18 states/eV.f.u.	TiIrSi	Ti1Ir1Si1	Ti	1	Ir	1	Si	1																		1	2016																										ABC		TiNiSi	Pnma	62	A	6.249	3.858	7.202												K		1.42				0.25	1.42											mT	calc from Hc(0)	0.535							T	RES(0.5Rn), empirical	0.751												MHC156703		A	from Hc2	209			nm	Hc1, GL	1110													mJ/mol.K2	10.8	SP	358	SP											uOhm.cm							11				240												Ir(3N),Si(5N),Ti(3N),Zr(2N),Hf(2N)		mixture - arc melting - remelt several times - ANN(950-1000 C,7 days)					Superconductivity in the ternary silicide TrIrSi (Tr = Ti, Zr, and Hf)			Graduate School of Science and Technology, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata 950?2181, Japan	Supercond. Sci. Technol., 29(2016)035011	Naoki Kase,Harufumi Suzuki,Tomohito Nakano,Naoya Takeda		
156704	SST029035011	RRR = 6.5. lattice term in SP (beta) = 0.117 mJ/mol.K4. (dC/gamma*Tc) = 1.4. Hc(0) = 10.8 mT. e-ph = 0.464. DOS = 2.21 states/eV.f.u.	ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																		1	2016																										ABC		TiNiSi	Pnma	62	A	6.537	3.952	7.393												K		1.85				0.1	1.85											mT	calc from Hc(0)	0.713							T	RES(0.5Rn), empirical	0.618												MHC156704		A	from Hc2	231			nm	Hc1, GL	960													mJ/mol.K2	7.63	SP	368	SP											uOhm.cm							40				260												Ir(3N),Si(5N),Ti(3N),Zr(2N),Hf(2N)		mixture - arc melting - remelt several times - ANN(950-1000 C,7 days)					Superconductivity in the ternary silicide TrIrSi (Tr = Ti, Zr, and Hf)			Graduate School of Science and Technology, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata 950?2181, Japan	Supercond. Sci. Technol., 29(2016)035011	Naoki Kase,Harufumi Suzuki,Tomohito Nakano,Naoya Takeda		
156705	SST029035011	RRR = 2.9. lattice term in SP (beta) = 0.127 mJ/mol.K4. (dC/gamma*Tc) = 1.4. Hc(0) = 21.8 mT. e-ph = 0.545. DOS = 1.79 states/eV.f.u.	HfIrSi	Hf1Ir1Si1	Hf	1	Ir	1	Si	1																		1	2016									14.1																	ABC		TiNiSi	Pnma	62	A	6.463	3.93	7.376												K		3.43				0.14	3.43										80	mT	calc from Hc(0)	0.929							T	RES(0.5Rn), empirical	2.23												MHC156705		A	from Hc2	121			nm	Hc1, GL	841													mJ/mol.K2	12.7	SP	304	SP											uOhm.cm							79.5				230												Ir(3N),Si(5N),Ti(3N),Zr(2N),Hf(2N)		mixture - arc melting - remelt several times - ANN(950-1000 C,7 days)					Superconductivity in the ternary silicide TrIrSi (Tr = Ti, Zr, and Hf)			Graduate School of Science and Technology, Niigata University, 8050, Ikarashi 2-no-cho, Nishi-ku, Niigata 950?2181, Japan	Supercond. Sci. Technol., 29(2016)035011	Naoki Kase,Harufumi Suzuki,Tomohito Nakano,Naoya Takeda		
156800	ANN3580248	C=a*T + b*T^3 + c*T^5 + d*T~7, b=1.906mJ/mol.K4, c=0.097mJ/mol.K6, d=-0.00007mJ/mol.K8. gap = 0.93 meV, (dC/gamma*Tc) = 1.7  from SP fitting.	Ba0.67Pt3B2	Ba0.67Pt3B2	Ba	0.67	Pt	3	B	2																		1	2015																										A1B2C3		CeCo3B2	P6<3>/mmc		A	6.16		5.27											hexagonal	K	5.53	5.65	5.74	5.45			5.65										100										T														MHC156800												meV	0.93	3.53	14							mJ/mol.K2	5.93	SP	175																																			Ba(4N),Pt(3N),B		arc-melting. mixture - pellet - arc-melting , several times.					Superconductivity in Ba2/3Pt3B2 with the Kagome lattice			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University,Nanjing 210093, China,	Anals of Physics, 358(2015)248	Sheng Li,Jie Xing,Jian Tao,Huan Yang,Hai-Hu Wen		
156801	CPL029037402	one unit cell FeSe films on Se-etched STO(001) substrate by MBE method. Tc estimates from STM gap measurement assuming 2*gap = 5.5 kTc(bulk )	FeSe(film)	Fe1Se1	Fe	1	Se	1																				5	2012																										AB																			beta-phase FeSe	K		80					80																																														meV	20.1	5.5	11																																															one unit cell FeSe films on Se-etched STO(001) substrates by MBE method (co-evaporation)					Interface-Induced High-Temperature Superconductivity in Single Unit-Cell FeSe Films on SrTiO3			State Key Lab of Low-Dimensional Quantum Physics, Department of Physics, Tsinghua University, Beijing 100084	Chin.Phys.Lett., 29(2012)037402	WANG Qing-Yan,LI Zhi,ZHANG Wen-Hao,ZHANG Zuo-Cheng,ZHANG Jin-Song,LI Wei,DING Hao,OU Yun-Bo,DENG Peng,CHANG Kai,WEN Jing,SONG Can-Li,HE Ke,JIA Jin-Feng,JI Shuai-Hua,WANG Ya-Yu,WANG Li-Li,CHEN Xi,MA Xu-Cun,XUE Qi-Kun		
156802	JAC6770057	RRR = R(250)/R(5) = 9 , R(T) along b-axis. AFM below 247K(T-decreasing) and  258 K(T-increasing) R0 = 28.4 uOhm.cm and A = 0.00241 uOhm.cm/K2 for R(T) = R0 + A*T^2	CrAs	As1Cr1	As	1	Cr	1																				3	2016								258																		AB		MnP	Pnma	62	A	5.651	3.465	6.209												K					2																																																																																																Cr(3N),As(4N),I(4N)		CVT method. using iodine agent. mixture - sealed in quartz tube - slow heating  to 800 C - source zone heating to 900C - hold one week- cool to RT					Single crystal growth of the new pressure-induced-superconductor CrAs via chemical vapor transport			High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei, 230031, PR China	J.Alloys Compd., 677(2016)57	Xiangde Zhu,Langsheng Ling,Yuyan Han,Junmin Xu,Yongjian Wang,Hongwei Zhang,Changjin Zhang,Li Pi,Yuheng Zhang		
156803	JAC6860431	metastable at P=AP. Tm = 140 K(ferro-mag).(dC/gamma*Tc) = 0.16. gamma fitting for 4 < T < 7K. gap measured by point contact, gap1 = 0.46(singlet), gap2 = 0.93meV(triplet)	RhGe0.989	Ge0.989Rh1	Ge	0.989	Rh	1																				1	2016							140																			AB		FeSi	P2<1>3	198	A	4.85954													B20-type	K	2.6		4.5	4.1			4.1																													T/K	onset	0.065															meV	0.46		1							mJ/mol.K2	2.9	SP													uOhm.cm							28																Rh(4N),Ge(5N)		polycrystalline of RhGe cubic phase synthesized at P=8GPa, 1700K using toroidal high-P apparatus by melting Rh and Ge					Superconductivity and magnetism in noncentrosymmetric RhGe			L. F. Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190, Moscow, Troitsk, Russia	J.Alloys Compd., 686(2016)431	A.V. Tsvyashchenko,V.A. Sidorov,A.E. Petrova,L.N. Fomicheva,I.P. Zibrov,V.E. Dmitrienko		
156804	JAC6860431		RhGe1.003	Ge1.003Rh1	Ge	1.003	Rh	1																				1	2016																										AB		FeSi	P2<1>3	198															B20-type	K	2.9		4				3.45	MTC156804		K/GPa	0.15																																																																																										Rh(4N),Ge(5N)		polycrystalline of RhGe cubic phase synthesized at P=8GPa, 1700K using toroidal high-P apparatus by melting Rh and Ge					Superconductivity and magnetism in noncentrosymmetric RhGe			L. F. Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190, Moscow, Troitsk, Russia	J.Alloys Compd., 686(2016)431	A.V. Tsvyashchenko,V.A. Sidorov,A.E. Petrova,L.N. Fomicheva,I.P. Zibrov,V.E. Dmitrienko		
156805	JAC6860431		RhGe4	Ge4Rh1	Ge	4	Rh	1																				1	2016																										AB4																				K	2.27	2.56	2.66				2.56	MTC156805																																																																						mOhm.cm							0.8																Rh(4N),Ge(5N)		polycrystalline of RhGe cubic phase synthesized at P=8GPa, 1700K using toroidal high-P apparatus by melting Rh and Ge					Superconductivity and magnetism in noncentrosymmetric RhGe			L. F. Vereshchagin Institute for High Pressure Physics, Russian Academy of Sciences, 142190, Moscow, Troitsk, Russia	J.Alloys Compd., 686(2016)431	A.V. Tsvyashchenko,V.A. Sidorov,A.E. Petrova,L.N. Fomicheva,I.P. Zibrov,V.E. Dmitrienko		
156806	JAC6880206	k(GL) = 32. Hc(0) = 983 Oe. beta(SP) = 3.9E-4 J/mol.K^4. (dC/gamma*Tc) = 1.26. gamma = 6.8 mJ/mol.K2, Debye-T = 455K,, Ein-T = 110K  from SP(0 < T< 300K)	ThCoSi	Th1Co1Si1	Th	1	Co	1	Si	1																		1	2016	emu/mol	0.0004																								ABC		LaPtSi	I4<1>md		A	4.081		14.003											LaPtSi-type	K	2.95						2.95											Oe	M-H curve, Hc1(T)=A*(1-t^2)	74							T	defined as R=0.1Rn	4.5												MHC156806		nm	from Hc2	8.55			nm	Hc1, GL theory	277											mJ/mol.K	22.12	mJ/mol.K2	15.5	SP	392	SP											uOhm.cm	90										221												Th(98wt%),Co(99.95wt%),Si(5N-wt%)		arc-melting					Superconductivity in a non-centrosymmetric compound ThCoSi			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O.Box 1410, 50-950 Wroc?aw, Poland	J.Alloys Compd., 688(2016)206	Krzysztof Domieracki,Dariusz Kaczorowski		
156807	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT). T<STR> same as Tn	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2014								135																		AB2C2		ThCr2Si2																	Fe-122	K					0																																																																																																		FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156808	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT). T<STR> same as Tn	(Ba,K)Fe2As2	Ba0.892K0.108Fe2As2	Ba	0.892	K	0.108	Fe	2	As	2																3	2014								126																		AB2C2		ThCr2Si2																	Fe-122	K					0			MPH156808																																																																																															FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156809	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT). T<STR> same as Tn	(Ba,K)Fe2As2	Ba0.832K0.168Fe2As2	Ba	0.832	K	0.168	Fe	2	As	2																3	2014								120																		AB2C2		ThCr2Si2																	Fe-122	K		7.74					7.74	MTC156809																																																																																															FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156810	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT). T<STR> same as Tn	(Ba,K)Fe2As2	Ba0.807K0.193Fe2As2	Ba	0.807	K	0.193	Fe	2	As	2																3	2014								102																		AB2C2		ThCr2Si2																	Fe-122	K		17.2					17.2																																																																																																FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156811	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT). T<STR> same as Tn	(Ba,K)Fe2As2	Ba0.765K0.235Fe2As2	Ba	0.765	K	0.235	Fe	2	As	2																3	2014								90																		AB2C2		ThCr2Si2																	Fe-122	K		20.5					20.5																																																																																																FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156812	PRB089144514	K-content measured by WDS. Tc defined as max of (dR/dT).	(Ba,K)Fe2As2	Ba0.66K0.34Fe2As2	Ba	0.66	K	0.34	Fe	2	As	2																3	2014																										AB2C2		ThCr2Si2																	Fe-122	K		37.5					37.5																																																																																																FeAs flux method. cleaved samples are a:b:c = 0.5:0.5:0.02 mm3					Interplane resistivity of underdoped single crystals (Ba1-xKx)Fe2As2 (0 =< x =< 0.34)			Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)144514	M. A. Tanatar,W. E. Straszheim,Hyunsoo Kim,J. Murphy,N. Spyrison,E. C. Blomberg,K. Cho,J.-Ph. Reid,Bing Shen,Louis Taillefer,Hai-Hu Wen,R. Prozorov		
156813	PRB091060508	RRR = 1900. Tc defined as R=0 and R=onset for SC1 and SC2 phases , respectively. Tetra-to-collapsed tetra transition at 16.4 GPa. (dTc/dP) = 2.1 K/GPa estimated for P//[001].	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2015																										AB2C2		ThCr2Si2																	Fe-122	K	3.6		4.2				3.9	MTC156813																																																																																				cm3/C						MRH156813					KAs flux method					High-temperature superconductivity stabilized by electron-hole interband coupling in collapsed tetragonal phase of KFe2As2 under high pressure			Center for Nanophysics and Advanced Materials, Department of Physics, University of Maryland, College Park, Maryland 20742, USA	Phys.Rev.B, 91(2015)060508	Yasuyuki Nakajima,Renxiong Wang,Tristin Metz,Xiangfeng Wang,Limin Wang,Hyunchae Cynn,Samuel T. Weir,Jason R. Jeffries,Johnpierre Paglione		
156814	PRB094054514	Two band full-gap model. 2d/kTc) = 1.4(small in DB), =3.52(large). small gap is nodeless. from SP. (dC/gamma*Tc) = 1.25. Cel(H)/T = 0.012J/mol.K2.kOe(H//a)	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2016																										AB2C2		ThCr2Si2																	Fe-122	K	0.6						0.6																				T	SP, WHH		10	14.7					T/K	SP		24	35	MHC156814												K	0.39	1.4	14																																															Flux method					Thermodynamic study of gap structure and pair-breaking effect by magnetic field in the heavy-fermion superconductor CeCu2Si2			Institute for Solid State Physics (ISSP), University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.B, 94(2016)054514	Shunichiro Kittaka,Yuya Aoki,Yasuyuki Shimura,Toshiro Sakakibara,Silvia Seiro,Christoph Geibel,Frank Steglich,Yasumasa Tsutsumi,Hiroaki Ikeda,Kazushige Machida		
156815	PRB094054515	RRR=1.47. SP(beta)=0.28 mJ/mol.K4, SP(delta)=0.004 mJ/mol.K6. (dC/gamma*Tc) = 1.53. Hc2(0) = 9.77 T from WHH. Hc(0) = 126.7 mT. GL = 68. e-Ph = 0.63.	Re6Hf	Hf1Re6	Hf	1	Re	6																				1	2016																										AB6		alpha-Mn	I4[-]3m	217	A	9.685														K			5.96	5.94		0.41	5.94											mT	M-H curve, Hc1(T)=A*(1-t^2)	5.6			5.2			1.8	T	M and SP, GL-eq.	12.2							T/K	SP	2.36			MHC156815		A	from Hc2	52			A	Hc1, GL theory	3538			meV	0.94	3.64	14				MSP156815			mJ/mol.K2	27.2	SP	364	SP											uOhm.cm							106.12																Hf(4N),Re(4N)		arc-melting					Superconducting properties of the noncentrosymmetric superconductor Re6Hf			Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India	Phys.Rev.B, 94(2016)054515	D. Singh,A. D. Hillier,A. Thamizhavel,R. P. Singh		
156816	PRB094054517	P-induced SC. Tc(max) = 4.8 K at P=20 GPa.. Pcr = 5 GPa. gamma = 0, Debye model, CDW not detected. SC properties (in DB) at P=19.5 GPa. . Hc2(0) = 4.5 T from GL	HfTe5	Hf1Te5	Hf	1	Te	5																				3	2016																										AB5			Cmcm		A	3.974	14.481	13.72												K			4.8		0		4.8	MPH156816																			T	RES(0.9Rn), WHH	3.6							T/K	RES(0.9Rn)	1.08					nm	from Hc2	8.5																																																										Flux method. (Hf0.0025Te99.9975) - alumina crucible - quartz tube - heat(900C,1d) - rapid cool to 580C - slow cool to 470 C (0.5K/h)					Pressure-driven superconductivity in the transition-metal pentatelluride HfTe5			Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany	Phys.Rev.B, 94(2016)054517	Yanpeng Qi,Wujun Shi,Pavel G. Naumov,Nitesh Kumar,Walter Schnelle,Oleg Barkalov,Chandra Shekhar,Horst Borrmann,Claudia Felser,Binghai Yan,Sergey A. Medvedev		
156817	PRB094054523	RRR = 17. SP (beta) = 3.7 mJ/mol.K4. Einstain-T = 95.5 K from C(T) fitting for 0.3<T<10 K. Gap from C<e>  analysis.. Hc2 determined by thermal conductivity measurements.	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																		3	2016																										AB4C12		skutterudite																		K		8					8																				T	thermal cond.	1.4														A	from Hc2	200										4.06	14							mJ/mol.K2	56	SP	208	SP											uOhm.cm							3.8																		(bulk sample) - in glassy-C crucible - sealed in Ta-tube in quartz tube - heat(870C within 5h and hold 10h) - cool to 845C, hold 30d) - furnace cool to RT					Superconducting gap structure of the skutterudite LaPt4Ge12 probed by specific heat and thermal transport			Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany	Phys.Rev.B, 94(2016)054523	H. Pfau,M. Nicklas,U. Stockert,R. Gumeniuk,W. Schnelle,A. Leithe-Jasper,Y. Grin,F. Steglich		
156818	PRB094064501	RRR = 15 for R<ab>, = 7 for R<c>. Carrier = 0.74 (40K) and 1.3 (200K)  E+22/cm^3 from Hall coefficient.	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2016																										ABC4D4		CaRb1144	P4/mmm		A	3.8696		12.837											CaK-1144. a=3.8609, c=12.674 at T=6.7 K	K	35			35			35	MTC156818																			T	RES(onset)		92	71					T/K	RES(on)		10.9	4.4	MHC156818																			MSP156818													uV/K	27.3			MTP156818	uOhm.cm												300	1500								n/cm3	13000000000000000000000			K:Ca:(Fe0.512As0.488) = 1.2:0.8:20. welded in Ta crucible - in alumina ampoule - heat(650C,1h) - hold(3h) - heat(1180C,2h) - hold(5h) - cool to 1050C over5h - slow cool to 930C					Anisotropic thermodynamic and transport properties of single-crystalline CaKFe4As4			Ames Laboratory US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 94(2016)064501	W. R. Meier,T. Kong,U. S. Kaluarachchi,V. Taufour,N. H. Jo,G. Drachuck,A. E. Bohmer,S. M. Saunders,A. Sapkota,A. Kreyssig,M. A. Tanatar,R. Prozorov,A. I. Goldman,Fedor F. Balakirev,Alex Gurevich,S. L. Bud'ko,P. C. Canfield		
156819	PRB094064522	(dC/dT) vs T curve shows the step corresponding to the hidden SC at 15 K. coexistence of SC and FM(below 50K)	(Bi,Mn)4O4S3	Bi3.925Mn0.075S3O4	Bi	3.925	Mn	0.075	S	3															O	4		1	2016							50																			A3B4C4			I4/mmm		A	3.9652		41.3563												K			6.04	4.67			4.67	MTC156819																																																																																													Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156820	PRB094064522	(dC/dT) vs T curve shows the step corresponding to the hidden SC at 15 K. coexistence of SC and FM(below 50K)	(Bi,Mn)4O4S3	Bi3.9Mn0.1S3O4	Bi	3.9	Mn	0.1	S	3															O	4		1	2016							50																			A3B4C4			I4/mmm		A	3.9631		41.3562												K			6.28	4.75			4.75																																																																																														Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156821	PRB094064522	(dC/dT) vs T curve shows the step corresponding to the hidden SC at 15 K. coexistence of SC and FM(below 50K). R(T) minimum at 55 K.	(Bi,Mn)4O4S3	Bi3.875Mn0.125S3O4	Bi	3.875	Mn	0.125	S	3															O	4		1	2016							50	125																		A3B4C4			I4/mmm		A	3.9464		40.9695												K			6.43	4.77			4.77	MTC156819																																																																																				m3/C	0.00003716						n/m3	168800000000000000000000	Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156822	PRB094064522	(dC/dT) vs T curve shows the step corresponding to the hidden SC at 15 K. coexistence of SC and FM(below 50K). R(T) minimum at 23 K.	(Bi,Mn)4O4S3	Bi3.85Mn0.15S3O4	Bi	3.85	Mn	0.15	S	3															O	4		1	2016							50	125																		A3B4C4			I4/mmm		A	3.9368		40.9544												K			5.53	4.02			4.02																																																																																														Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156823	PRB094064522		(Bi,Co)4O4S3	Bi3.875Co0.125S3O4	Bi	3.875	Co	0.125	S	3															O	4		1	2016																										A3B4C4			I4/mmm		A	3.9614		41.2995												K			5.93	4.79			4.79																																																																																														Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156824	PRB094064522		(Bi,Ni)4O4S3	Bi3.875Ni0.125S3O4	Bi	3.875	Ni	0.125	S	3															O	4		1	2016																										A3B4C4			I4/mmm		A	3.953		41.0972												K			6.09	4.87			4.87																																																																																														Bi(4N),Bi2O3(4N),S(5N),MnO2(4N)		solid state reaction. mixture - pressed to pellet - sealed in quartz tube - heat to 510 C - hold(10h)					Mn-doping induced ferromagnetism and enhanced superconductivity in Bi4-xMnxO4S3 (0.075 =< x =< 0.15)			Department of Physics, Shanghai University, Shanghai 200444, China	Phys.Rev.B, 94(2016)064522	Zhenjie Feng,Xunqing Yin,Yiming Cao,Xianglian Peng,Tian Gao,Chuan Yu,Jingzhe Chen,Baojuan Kang,Bo Lu,Juan Guo,Qing Li,Wei-Shiuan Tseng,Zhongquan Ma,Chao Jing,Shixun Cao,Jincang Zhang,N.-C. Yeh		
156825	PRB094094501	RRR = 28.3.	LaPt4Ge12	La1Pt4Ge12	La	1	Pt	4	Ge	12																		1	2016	cm3/mol	390					-19.2																			AB4C12		skutterudite	Im3[-]		A	8.6145														K	8.33	8.54	9.3				8.54																																																																																														La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156826	PRB094094501	RRR = 8.75. (dTc/dx) = -0.4 K/at%Ce. Energy gap  D/Tc = 1.52 rom SP analysis.	(La,Ce)Pt4Ge12	La0.95Ce0.05Pt4Ge12	La	0.95	Ce	0.05	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	6.6159														K	5.42	5.73	6.32				5.73																																																					MSP156826			mJ/mol.K2	51.2	SP	204	SP																																		La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156827	PRB094094501	Energy gap  D/Tc = 1.38 from SP analysis.	(La,Ce)Pt4Ge12	La0.9Ce0.1Pt4Ge12	La	0.9	Ce	0.1	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.6141														K	3.14	5.61	4.53				5.61	MTC156826																																																							mJ/mol.K2	67.6	SP	210	SP																																		La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156828	PRB094094501	RRR = 5.85	(La,Ce)Pt4Ge12	La0.85Ce0.15Pt4Ge12	La	0.85	Ce	0.15	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.6139														K	1.59	2.17	2.99				2.17																																																								mJ/mol.K2	81.3	SP	210.3	SP																																		La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156829	PRB094094501	RRR = 4.59. T*(broad max point in M/H vs T curve) = 41.3 K	(La,Ce)Pt4Ge12	La0.8Ce0.2Pt4Ge12	La	0.8	Ce	0.2	Pt	4	Ge	12																1	2016	cm3/mol	1580			myu-B/Ce	3.16	-69.8																			AB4C12		skutterudite	Im3[-]		A	8.613														K			1.57				1.57																																																																																														La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156830	PRB094094501	RRR = 3.54. T*(broad max point in M/H vs T curve) = 51.3 K	(La,Ce)Pt4Ge12	La0.6Ce0.4Pt4Ge12	La	0.6	Ce	0.4	Pt	4	Ge	12																1	2016	cm3/mol	2340			myu-B/Ce	2.77	-57.9																			AB4C12		skutterudite	Im3[-]		A	8.6128														K					0																																																																																																La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156831	PRB094094501	RRR = 2.7. T*(broad max point in M/H vs T curve) = 64.9 K	(La,Ce)Pt4Ge12	La0.4Ce0.6Pt4Ge12	La	0.4	Ce	0.6	Pt	4	Ge	12																1	2016	cm3/mol	2840			myu-B/Ce	2.59	-64.1																			AB4C12		skutterudite	Im3[-]		A	8.6163														K					0																																																																																																La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156832	PRB094094501	RRR = 3.91. T*(broad max point in M/H vs T curve) = 74.7 K	(La,Ce)Pt4Ge12	La0.4Ce0.8Pt4Ge12	La	0.4	Ce	0.8	Pt	4	Ge	12																1	2016	cm3/mol	3980			myu-B/Ce	3.03	-98																			AB4C12		skutterudite	Im3[-]		A	8.6104														K					0																																																																																																La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156833	PRB094094501	RRR = 20.8. T*(broad max point in M/H vs T curve) = 80.3 K	(La,Ce)Pt4Ge12	Ce1Pt4Ge12	Ce	1	Pt	4	Ge	12																		1	2016	cm3/mol	3640			myu-B/Ce	2.71	-84																			AB4C12		skutterudite	Im3[-]		A	8.6145														K					0																																																																																																La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156834	PRB094094501	RRR = 12.3	(La,Th)Pt4Ge12	La0.8Th0.2Pt4Ge12	La	0.8	Th	0.2	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.627														K	7.78	8.06	8.29				8.06																																																								mJ/mol.K2	30.7	SP	201	SP																																		La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156835	PRB094094501	RRR = 10.4	(La,Th)Pt4Ge12	La0.6Th0.4Pt4Ge12	La	0.6	Th	0.4	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.6113														K	7.03	7.55	7.41				7.55																																																																																														La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156836	PRB094094501	RRR = 10.6. (dTc/dx) = -0.04 K/at%Th	(La,Th)Pt4Ge12	La0.4Th0.6Pt4Ge12	La	0.4	Th	0.6	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.6141														K	6.22	6.77	7.13				6.77	MTC156836																																																																																													La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156837	PRB094094501	RRR = 26.8	(La,Th)Pt4Ge12	La0.2Th0.8Pt4Ge12	La	0.2	Th	0.8	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite	Im3[-]		A	8.6081														K	5.36	5.67	6.2				5.67																																																																																														La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156838	PRB094094501	RRR = 38.5	(La,Th)Pt4Ge12	Th1Pt4Ge12	Th	1	Pt	4	Ge	12																		1	2016																										AB4C12		skutterudite	Im3[-]		A	8.5995														K	4.35	4.56	4.97				4.56																																																																																														La(3N),Ce(3N),Th(3N),Pt(6N),Ge(6N)		arc-melting.  ANN(800C,336h, in quartz tube(vac))					Superconducting and normal state properties of the systems La1-xMxPt4Ge12 (M = Ce, Th)			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 94(2016)094501	K. Huang,D. Yazici,B. D. White,I. Jeon,A. J. Breindel,N. Pouse,M. B. Maple		
156839	PRB094094523		(La,Ce)Ru3Si2	La0.9Ce0.1Ru3Si2	La	0.9	Ce	0.1	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	5.12			5.12			5.12																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156840	PRB094094523		(La,Ce)Ru3Si2	La0.8Ce0.2Ru3Si2	La	0.8	Ce	0.2	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	4.62			4.62			4.62	MTC156840																																																																																															arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156841	PRB094094523		(La,Ce)Ru3Si2	La0.6Ce0.4Ru3Si2	La	0.6	Ce	0.4	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	3.35			3.35			3.35																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156842	PRB094094523		(La,Ce)Ru3Si2	La0.4Ce0.6Ru3Si2	La	0.4	Ce	0.6	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	2.47			2.47			2.47																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156843	PRB094094523		CeRu3Si2	Ce1Ru3Si2	Ce	1	Ru	3	Si	2																		1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K					2																																																																																																		arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156844	PRB094094523		(La,Lu)Ru3Si2	La0.95Lu0.05Ru3Si2	La	0.95	Lu	0.05	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	6.19			6.19			6.19																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156845	PRB094094523		(La,Y)Ru3Si2	La0.92Y0.08Ru3Si2	La	0.92	Y	0.08	Ru	3	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	6.13			6.13			6.13																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156846	PRB094094523	RRR = 4.76	LaRu3Si2	La1Ru3Si2	La	1	Ru	3	Si	2																		1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.675		3.5574												K	6.89			6.89			6.89																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156847	PRB094094523	RRR = 5.40	La(Ru,Cr)3Si2	La1Ru2.94Cr0.06Si2	La	1	Ru	2.94	Cr	0.06	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.6737		3.5568												K	6.23			6.23			6.23																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156848	PRB094094523	RRR = 2.96	La(Ru,Cr)3Si2	La1Ru1Cr0.21Si2	La	1	Ru	1	Cr	0.21	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.6694		3.5517												K	4.88			4.88			4.88																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156849	PRB094094523	RRR = 2.14	La(Ru,Ni)3Si2	La1Ru2.919Ni0.081Si2	La	1	Ru	2.919	Ni	0.081	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.672		3.5556												K	5.42			5.42			5.42																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156850	PRB094094523	RRR = 1.67	La(Ru,Ni)3Si2	La1Ru2.865Ni0.135Si2	La	1	Ru	2.865	Ni	0.135	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.669		3.554												K	5.02			5.02			5.02																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156851	PRB094094523	RRR = 1.40	La(Ru,Ni)3Si2	La1Ru2.814Ni0.186Si2	La	1	Ru	2.814	Ni	0.186	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm		A	5.6672		3.5514												K	4.8			4.8			4.8																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156852	PRB094094523		La(Ru,Cu)3Si2	La1Ru2.94Cu0.06Si2	La	1	Ru	2.94	Cu	0.06	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	6.44						6.44																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156853	PRB094094523		La(Ru,Cu)3Si2	La1Ru2.88Cu0.12Si2	La	1	Ru	2.88	Cu	0.12	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	5.93						5.93																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156854	PRB094094523		La(Ru,Fe)3Si2	La1Ru2.97Fe0.03Si2	La	1	Ru	2.97	Fe	0.03	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	6.16						6.16																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156855	PRB094094523		La(Ru,Fe)3Si2	La1Ru2.94Fe0.06Si2	La	1	Ru	2.94	Fe	0.06	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	4.51						4.51	MTC156855																																																																																															arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156856	PRB094094523		La(Ru,Fe)3Si2	La1Ru2.925Fe0.075Si2	La	1	Ru	2.925	Fe	0.075	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	3						3																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156857	PRB094094523		La(Ru,Fe)3Si2	La1Ru2.9175Fe0.0825Si2	La	1	Ru	2.9175	Fe	0.0825	Si	2																1	2016																										AB2C3		LaRu2Si2	P6/mmm																	K	2.49						2.49																																																																																																arc-melting.Excess Ru added in nominal compositions to avoid LaRu2Si2 phase formation.					Chemical doping effect in the LaRu3Si2 superconductor with a kagome lattice			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 94(2016)094523	Baoxuan Li, Sheng Li,Hai-Hu Wen		
156858	PRB094094524	RH(250K) = -0.29E-3 cm3/C.	LiFeAs	Li1Fe1As1	Li	1	Fe	1	As	1																		3	2016																										ABC					A			6.3641												K	17			16.2			16.2																																																																																					cm3/C						MRH156858			Li3As,Fe1-xVxAs		self-flux method. mixture(Li3As:Fe1-xVxAs:As = 1:0.9:1.1) - alumina crucible - sealed in Nb tube - in quartz tube - heat(1100C,50h) - slow cool to 750 C(2C/h)					Observation of non-Fermi liquid behavior in hole-doped LiFe1-xVxAs			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)094524	L. Y. Xing,X. Shi,P. Richard,X. C. Wang,Q. Q. Liu,B. Q. Lv,J.-Z. Ma,B. B. Fu,L.-Y. Kong,H. Miao,T. Qian,T. K. Kim,M. Hoesch,H. Ding,C. Q. Jin		
156859	PRB094094524	dTc/dx = 7 K/at%V	Li(Fe,V)As	Li1Fe0.993V0.007As1	Li	1	Fe	0.993	V	0.007	As	1																3	2016																										ABC					A															K	12.6			12.2			12.2																																																																																														Li3As,Fe1-xVxAs		self-flux method. mixture(Li3As:Fe1-xVxAs:As = 1:0.9:1.1) - alumina crucible - sealed in Nb tube - in quartz tube - heat(1100C,50h) - slow cool to 750 C(2C/h)					Observation of non-Fermi liquid behavior in hole-doped LiFe1-xVxAs			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)094524	L. Y. Xing,X. Shi,P. Richard,X. C. Wang,Q. Q. Liu,B. Q. Lv,J.-Z. Ma,B. B. Fu,L.-Y. Kong,H. Miao,T. Qian,T. K. Kim,M. Hoesch,H. Ding,C. Q. Jin		
156860	PRB094094524		Li(Fe,V)As	Li1Fe0.986V0.014As1	Li	1	Fe	0.986	V	0.014	As	1																3	2016																										ABC					A			6.3625												K	7.77			5.7			5.7																																																																																														Li3As,Fe1-xVxAs		self-flux method. mixture(Li3As:Fe1-xVxAs:As = 1:0.9:1.1) - alumina crucible - sealed in Nb tube - in quartz tube - heat(1100C,50h) - slow cool to 750 C(2C/h)					Observation of non-Fermi liquid behavior in hole-doped LiFe1-xVxAs			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)094524	L. Y. Xing,X. Shi,P. Richard,X. C. Wang,Q. Q. Liu,B. Q. Lv,J.-Z. Ma,B. B. Fu,L.-Y. Kong,H. Miao,T. Qian,T. K. Kim,M. Hoesch,H. Ding,C. Q. Jin		
156861	PRB094094524		Li(Fe,V)As	Li1Fe0.981V0.019As1	Li	1	Fe	0.981	V	0.019	As	1																3	2016																										ABC					A			6.366												K				3			3																																																																																														Li3As,Fe1-xVxAs		self-flux method. mixture(Li3As:Fe1-xVxAs:As = 1:0.9:1.1) - alumina crucible - sealed in Nb tube - in quartz tube - heat(1100C,50h) - slow cool to 750 C(2C/h)					Observation of non-Fermi liquid behavior in hole-doped LiFe1-xVxAs			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)094524	L. Y. Xing,X. Shi,P. Richard,X. C. Wang,Q. Q. Liu,B. Q. Lv,J.-Z. Ma,B. B. Fu,L.-Y. Kong,H. Miao,T. Qian,T. K. Kim,M. Hoesch,H. Ding,C. Q. Jin		
156862	PRB094094524	n = 1.25 in R = A*T^n. RH(260K) = +0.24E-3 cm3/C.	Li(Fe,V)As	Li1Fe0.958V0.042As1	Li	1	Fe	0.958	V	0.042	As	1																3	2016																										ABC					A			6.3881												K					0																																																																																							cm3/C						MRH156862			Li3As,Fe1-xVxAs		self-flux method. mixture(Li3As:Fe1-xVxAs:As = 1:0.9:1.1) - alumina crucible - sealed in Nb tube - in quartz tube - heat(1100C,50h) - slow cool to 750 C(2C/h)					Observation of non-Fermi liquid behavior in hole-doped LiFe1-xVxAs			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)094524	L. Y. Xing,X. Shi,P. Richard,X. C. Wang,Q. Q. Liu,B. Q. Lv,J.-Z. Ma,B. B. Fu,L.-Y. Kong,H. Miao,T. Qian,T. K. Kim,M. Hoesch,H. Ding,C. Q. Jin		
156863	PRB094104507	R(T) has quadratic dependence of T for all P-range RRR = 1.3. (dR/dT) has two peaks in SC transition, Tc1(lower) and Tc2(higher ones). See TCFIG.	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2016																										A8B46	3	clathrate																		K		7.31	8				7.31	MTC156863																																																																																															mixed(BaSi2 + Si) - in h=BN cell - high-P synthesis(1000K,P=1-5 GPa) - Quench to RT - P release					Enhanced high-pressure superconductivity and local structure of the Ba8Si46 clathrate			Instituto de Investigaciones en Materiales, Universidad Nacional Autonoma de Mexico, Mexico, D.F. 04510, Mexico	Phys.Rev.B, 94(2016)104507	F. Morales,M. Nunez-Regueiro,P. Toulemonde,D. Machon,S. Le Floch,V. Pischedda,P. Lagarde,A.-M. Flank,J. P. Itie,A. San-Miguel		
156864	PRB094125110	RRR = 28. Hc2//b measured	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2016																										ABC	3	TiNiSi																		K		0.76				0.15	0.76	MPH156864																			T	RES(0.5Rn)													MHC156864																																					uOhm.cm							10.6																		crystals grown in a tetra-arc furnace by Chzochralski method.					Quantum criticality in the ferromagnetic superconductor UCoGe under pressure and magnetic field			Universite Grenoble Alpes, CEA, INAC-PHELIQS, F-38000 Grenoble, France	Phys.Rev.B, 94(2016)125110	Gael Bastien,Daniel Braithwaite,Dai Aoki,Georg Knebel,Jacques Flouquet		
156865	PRB094125110	Hc2//c measured	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2016																										ABC	3	TiNiSi																		K		0.76					0.76																				T	RES(0.5Rn)													MHC156865																																																														crystals grown in a tetra-arc furnace by Chzochralski method.					Quantum criticality in the ferromagnetic superconductor UCoGe under pressure and magnetic field			Universite Grenoble Alpes, CEA, INAC-PHELIQS, F-38000 Grenoble, France	Phys.Rev.B, 94(2016)125110	Gael Bastien,Daniel Braithwaite,Dai Aoki,Georg Knebel,Jacques Flouquet		
156866	PRB094134507	Trigonal(H) to monoclinic(L) phase transition, T<STR> = 249 K. Hall const in DB shows ones at 2 K.	IrTe2	Ir1Te2	Ir	1	Te	2																				1	2016																										AB2		CdI2			A	3.9317		5.3995											c/a = 1.374	K					1.8																																																										mJ/mol.K2	1.82	SP	204	SP																									cm3/C	-0.000041										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156867	PRB094134507	Trigonal(H) to monoclinic(L) phase transition, T<STR> = 290 K.  Hall const in DB shows ones at 2 K.	Ir(Te,Se)2	Ir1Te1.9Se0.1	Ir	1	Te	1.9	Se	0.1																		1	2016																										AB2		CdI2			A	3.9017		5.378											c/a = 1.378	K					1.8																																																																																							cm3/C	-0.000312										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156868	PRB094134507	Trigonal(H) to monoclinic(L) phase transition, T<STR> = 314 K. Hall const in DB shows ones at 2 K.	Ir(Te,Se)2	Ir1Te1.8Se0.2	Ir	1	Te	1.8	Se	0.2																		1	2016																										AB2		CdI2			A	3.8889		5.429											c/a = 1.397	K					1.8																																																										mJ/mol.K2	1.8	SP	204	SP																									cm3/C	-0.000416										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156869	PRB094134507	Trigonal(H) to monoclinic(L) phase transition, T<STR> = 342 K. Hall const in DB shows ones at 2 K.	Ir(Te,Se)2	Ir1Te1.7Se0.3	Ir	1	Te	1.7	Se	0.3																		1	2016																										AB2		CdI2			A	3.8885		5.3968											c/a = 1.388	K					1.8																																																										mJ/mol.K2	1.61	SP	204	SP																									cm3/C	-0.000844										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156870	PRB094134507	Trigonal(H) to monoclinic(L) phase transition, T<STR> = 408 K. Hall const in DB shows ones at 2 K.	Ir(Te,Se)2	Ir1Te1.5Se0.5	Ir	1	Te	1.5	Se	0.5																		1	2016																										AB2		CdI2			A	3.8446		5.3992											c/a = 1.404	K					1.8																																																										mJ/mol.K2	1.52	SP	208	SP																									cm3/C	-0.000942										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156871	PRB094134507	Hall const in DB shows ones at 2 K.	Ir(Te,Se)2	Ir1Te1.3Se0.7	Ir	1	Te	1.3	Se	0.7																		1	2016																										AB2		CdI2			A	3.7311		5.377											c/a = 1.441	K					1.8																																																										mJ/mol.K2	1.39	SP	215	SP																									cm3/C	-0.001186										solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156872	PRB094134507		IrTe2	Ir1Te2	Ir	1	Te	2																				1	2016																										AB2					A	3.93		5.3995												K					1.8																																																																																																		solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156873	PRB094134507		CuxIrTe2	Cu0.05Ir1Te2	Cu	0.05	Ir	1	Te	2																		1	2016																										AB2					A	3.9408		5.3941												K			2.85				2.85	MTC156873																																																																																															solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156874	PRB094134507		CuxIrTe2	Cu0.1Ir1Te2	Cu	0.1	Ir	1	Te	2																		1	2016																										AB2					A	3.9504		5.3992												K			2.6				2.6																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156875	PRB094134507		CuxIr(Te,Se)2	Cu0.05Ir1Te1.8Se0.2	Cu	0.05	Ir	1	Te	1.8	Se	0.2																1	2016																										AB2					A	3.9166		5.3825												K			2.8				2.8	MTC156873																																																																																															solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156876	PRB094134507		CuxIr(Te,Se)2	Cu0.2Ir1Te1.8Se0.2	Cu	0.2	Ir	1	Te	1.8	Se	0.2																1	2016																										AB2					A	3.9395		5.3873												K			2.21				2.21																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156877	PRB094134507		CuxIr(Te,Se)2	Cu0.05Ir1Te1.7Se0.3	Cu	0.05	Ir	1	Te	1.7	Se	0.3																1	2016																										AB2					A	3.9039		5.377												K			2.45				2.45																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156878	PRB094134507		CuxIr(Te,Se)2	Cu0.125Ir1Te1.7Se0.3	Cu	0.125	Ir	1	Te	1.7	Se	0.3																1	2016																										AB2					A	3.9174		5.3764												K			2.71				2.71																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156879	PRB094134507		CuxIr(Te,Se)2	Cu0.2Ir1Te1.7Se0.3	Cu	0.2	Ir	1	Te	1.7	Se	0.3																1	2016																										AB2					A	3.9312		5.378												K			1.68				1.68																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156880	PRB094134507		CuxIr(Te,Se)2	Cu0.1Ir1Te1.5Se0.5	Cu	0.1	Ir	1	Te	1.5	Se	0.5																1	2016																										AB2					A	3.8907		5.3606												K			1.95				1.95																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156881	PRB094134507		CuxIr(Te,Se)2	Cu0.15Ir1Te1.5Se0.5	Cu	0.15	Ir	1	Te	1.5	Se	0.5																1	2016																										AB2					A	3.8946		5.3606												K			2.35				2.35																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156882	PRB094134507		CuxIr(Te,Se)2	Cu0.2Ir1Te1.5Se0.5	Cu	0.2	Ir	1	Te	1.5	Se	0.5																1	2016																										AB2					A	3.9022		5.3611												K			2.3				2.3																																																																																																solid state reaction					Relation between the structural phase transition and superconductivity in CuxIrTe2-ySey			Department of Applied Physics, University of Tokyo, Hongo, Tokyo 113-8656, Japan	Phys.Rev.B, 94(2016)134507	M. Kamitani,H. Sakai,Y. Tokura,S. Ishiwata		
156883	PRB094144502	gaps composed of nodeless (in DB) and nodal (d=1.73 meV) component for x < 0.07. nodal component = 79%. gaps obtained from electronic SP analysis. beta (in SP) = 5.2 mJ/mol.K4	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2016																										AB4C12		skutterudite																		K		7.77					7.77																																														meV	1.09		14				MSP156883			mJ/mol.K2	73.7	SP																																						arc-melting					Multiband superconductivity in the correlated electron filled skutterudite system Pr1-xCexPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 94(2016)144502	Y. P. Singh,R. B. Adhikari,S. Zhang,K. Huang,D. Yazici,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
156884	PRB094144502	gaps composed of nodeless (in DB) and nodal (d = 1.47 meV) component for x < 0.07. nodal component = 40%. gaps obtained from electronic SP analysis.	(Pr,Ce)Pt4Ge12	Pr0.98Ce0.02Pt4Ge12	Pr	0.98	Ce	0.02	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite																		K		6.63					6.63																																														meV	0.98		14																																															arc-melting					Multiband superconductivity in the correlated electron filled skutterudite system Pr1-xCexPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 94(2016)144502	Y. P. Singh,R. B. Adhikari,S. Zhang,K. Huang,D. Yazici,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
156885	PRB094144502	gaps composed of nodeless (in DB) and nodal (d = 1.23 meV) component for x < 0.07. nodal component = 30%. gaps obtained from electronic SP analysis.	(Pr,Ce)Pt4Ge12	Pr0.96Ce0.04Pt4Ge12	Pr	0.96	Ce	0.04	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite																		K		5.59					5.59	MTC156885																																													meV	0.83		14																																															arc-melting					Multiband superconductivity in the correlated electron filled skutterudite system Pr1-xCexPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 94(2016)144502	Y. P. Singh,R. B. Adhikari,S. Zhang,K. Huang,D. Yazici,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
156886	PRB094144502	nodeless gap for  0.07 < x.  gaps obtained from electronic SP analysis.	(Pr,Ce)Pt4Ge12	Pr0.915Ce0.085Pt4Ge12	Pr	0.915	Ce	0.085	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite																		K		3.62					3.62	MGAP156886																																													meV	0.55		14				MSP156886																																											arc-melting					Multiband superconductivity in the correlated electron filled skutterudite system Pr1-xCexPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 94(2016)144502	Y. P. Singh,R. B. Adhikari,S. Zhang,K. Huang,D. Yazici,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
156887	PRB094144502	nodeless gap for  0.07 < x.  gaps obtained from electronic SP analysis.	(Pr,Ce)Pt4Ge12	Pr0.9Ce0.1Pt4Ge12	Pr	0.9	Ce	0.1	Pt	4	Ge	12																1	2016																										AB4C12		skutterudite																		K		3.03					3.03																																														meV	0.44		14																																															arc-melting					Multiband superconductivity in the correlated electron filled skutterudite system Pr1-xCexPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 94(2016)144502	Y. P. Singh,R. B. Adhikari,S. Zhang,K. Huang,D. Yazici,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
156888	CHM0281927		Ti1-xTaxSe2	Ti0.98Ta0.02Se2	Ti	0.98	Ta	0.02	Se	2																			2016																										AB2		1T-MX2																		K		1.02					1.02																																																																																														Ta'2N8),Nb(2N8),Ti(3N),Se(5N9		mixture - pellet - heat to 700C(1C/min) - hold(120h) - reground - pellet - heat to 700C(3C/min) - hold(129h), CVD method (725C(H) and 675C(L).					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
156889	CHM0281927		Ti1-xTaxSe2	Ti0.85Ta0.15Se2	Ti	0.85	Ta	0.15	Se	2																			2016																										AB2		1T-MX2																		K		2.29					2.29	MPH156889																			T	RES(0.5Rn), WHH	2.21							T/K	RES(0.5Rn)	1.4			MHC156889																																																												Ta'2N8),Nb(2N8),Ti(3N),Se(5N9		mixture - pellet - heat to 700C(1C/min) - hold(120h) - reground - pellet - heat to 700C(3C/min) - hold(129h), CVD method (725C(H) and 675C(L).					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
156890	CHM0281927	beta (SP) = 0.701 mJ/mol.K4. (dC/T) = 3.78, (dC/gamma:Tc) = 1.9. e-ph = 0.61, N(0) = 0.53 states/eV.f.u.	Ti1-xTaxSe2	Ti0.8Ta0.2Se2	Ti	0.8	Ta	0.2	Se	2																			2016																										AB2		1T-MX2																		K		2.29					2.29																				T	RES(0.5Rn), WHH	2.23							T/K	RES(0.5Rn)	1.4			MHC156890		A	from Hc2	120																		mJ/mol.K2	1.99	SP	202	SP																									Ohm.cm	-0.00019								Ta'2N8),Nb(2N8),Ti(3N),Se(5N9		mixture - pellet - heat to 700C(1C/min) - hold(120h) - reground - pellet - heat to 700C(3C/min) - hold(129h), CVD method (725C(H) and 675C(L).					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
156891	CHM0281927		Ti1-xTaxSe2	Ti0.6Ta0.4Se2	Ti	0.6	Ta	0.4	Se	2																			2016																										AB2		1T-MX2																		K		1.22					1.22																																																																																														Ta'2N8),Nb(2N8),Ti(3N),Se(5N9		mixture - pellet - heat to 700C(1C/min) - hold(120h) - reground - pellet - heat to 700C(3C/min) - hold(129h), CVD method (725C(H) and 675C(L).					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
156892	CHM0281927	not SC for x < 0.4 in Ti1-xNbxSe2. beta (SP) = 0.475  mJ/mol.K4. no CDW  (T<CDW> <89 K.).	Ti1-xNbxSe2	Ti0.8Nb0.2Se2	Ti	0.8	Nb	0.2	Se	2																			2016																										AB2		1T-MX2																		K					0.3																																																										mJ/mol.K2	0.45	SP	230	SP																									Ohm.cm	-0.0025					MRH156892			Ta'2N8),Nb(2N8),Ti(3N),Se(5N9		mixture - pellet - heat to 700C(1C/min) - hold(120h) - reground - pellet - heat to 700C(3C/min) - hold(129h), CVD method (725C(H) and 675C(L).					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
156893	JAC2810112	not SC.	Hf3Ni4Ge4	Hf3Ni4Ge4	Hf	3	Ni	4	Ge	4																		1	1998	eum/mol	0.000123	emu/mol	3.38			-0.29		10.845																	A3B4C4			Immm		A	12.873	6.484	3.892											ortho-. Hf3Cu4Si4 type	K					2																																																																									uOhm.cm							16.3																Hf(3N),Ni(3N),Ge(5N),Pt(5N)		arc-melting - in quartz ampoule (Ar) - heat(900C,3days) - Q to water					New intermetallic compounds found in Hf-Ni-Ge and Hf-Pt-Ge systems			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 281(1998)112	Y. Nagata,K. Sodeyama,S. Yashiro,H. Sasaki,H. Samata,T. Uchida,M.D. Lan		
156894	JAC2810112	not SC. Diamagnetic for T < 250 K	HfPtGe	Hf1Pt1Ge1	Hf	1	Pt	1	Ge	1																		1	1998									14.917																	ABC			Pnma		A	6.603	3.95	7.617											ortho-. Co2Si type	K					2																																																																									mOhm.cm							1.59																Hf(3N),Ni(3N),Ge(5N),Pt(5N)		arc-melting - in quartz ampoule (Ar) - heat(900C,3days) - Q to water					New intermetallic compounds found in Hf-Ni-Ge and Hf-Pt-Ge systems			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 281(1998)112	Y. Nagata,K. Sodeyama,S. Yashiro,H. Sasaki,H. Samata,T. Uchida,M.D. Lan		
156895	JAC2980051		HfPtSi	Hf1Pt1Si1	Hf	1	Pt	1	Si	1																		1	2000	emu/mol	-0.000133	emu/mol	0.000288	myu-B/mol	0.00482	-1.82		13.98																	ABC	3	Co2Si	Pnma		A	6.549	3.883	7.506											ortho	K					1.5																																																																																																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156896	JAC2980051		HfPdSi	Hf1Pd1Si1	Hf	1	Pd	1	Si	1																		1	2000	emu/mol	-0.000051	emu/mol	0.0000717	myu-B/mol	0.00482	-1.23		10																	ABC	3	Co2Si	Pnma		A	6.57	3.874	7.565											ortho	K					1.5																																																																																																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156897	JAC2980051		HfPdSi	Hf1Rh1Si1	Hf	1	Rh	1	Si	1																		1	2000	emu/mol	0.00013																								ABC					A	6.4697	3.8995	7.4061												K				2.18			2.18											Oe	M-H curve, Linear approx.	57			10			1.7	T	Linear approx.	0.54												MHC156897																																					uOhm.cm							67																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156898	JAC2980051		Hf(Rh,Pd)Si	Hf1Rh0.9Pd0.1Si1	Hf	1	Rh	0.9	Pd	0.1	Si	1																1	2000	emu/mol	0.000127																								ABC					A	6.4851	3.8985	7.434												K				1.95			1.95																																																																							uOhm.cm							344																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156899	JAC2980051		Hf(Rh,Pd)Si	Hf1Rh0.8Pd0.2Si1	Hf	1	Rh	0.8	Pd	0.2	Si	1																1	2000	emu/mol	0.000122																								ABC					A	6.4984	3.8938	7.4598												K				1.85			1.85	MLAT156899																																																																						uOhm.cm							392																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156900	JAC2980051		Hf(Rh,Pd)Si	Hf1Rh0.7Pd0.3Si1	Hf	1	Rh	0.7	Pd	0.3	Si	1																1	2000	emu/mol	0.000113																								ABC					A	6.4897	3.8756	7.4606												K				1.75			1.75																																																																							uOhm.cm							901																Hf(3N),Si(6N),Pt(4N),Pd(3N)		arc-melting - sealed in quartz ampoule (Ar) - heat(700C,3days) - Q to water					Magnetism and transport properties of HfMSi (M = Pt, Pd) and HfRh1-xPdxSi			College of Science and Engineering, Aoyama Gakuin University, Chitosedai, Setagaya, Tokyo 157-8572, Japan	J.Alloys Compd., 298(2000)51	S. Yashiro,Y. Nagata,H. Samata,S. Abe		
156901	JAC6940459	Compositions: Ba8.00Al6.31Si39.69 By EDS	Ba8Al5Si41	Ba8Al5Si41	Ba	8	Al	5	Si	41																		1	2017																										A8B46		clathrate	Pm3[-]n		A	10.4423														K				6.8			6.8										20.4	Oe	M-H cuve, (1-t2) approx.	58																					MHC156901																																																												Ba(4N),Eu(4N),Al(5N),Si(5N)		arc-melting ((8-x)*1.05:x:5:41) - ground and washed with dilute NaOH solution and HCl in order to remove impurity phases					Magnetic moment of Eu-dopant and superconductivity in Eu-substitutional Ba8Al5Si41 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	J.Alloys Compd., 694(2017)459	Lihua Liu,Yueting Ren,Bensheng Song,Jose Garcia,Hengyi Du,Xingqiao Ma,Yang Li		
156902	JAC6940459	Compositions: Ba7.91Eu0.09Al6.21Si39.79  By EDS	(Ba,Eu)8Al5Si41	Ba7.9Eu0.1Al5Si41	Ba	7.9	Eu	0.1	Al	5	Si	41																1	2017							3.89																			A8B46		clathrate	Pm3[-]n		A	10.4413														K				5.9			5.9																																																																																														Ba(4N),Eu(4N),Al(5N),Si(5N)		arc-melting ((8-x)*1.05:x:5:41) - ground and washed with dilute NaOH solution and HCl in order to remove impurity phases					Magnetic moment of Eu-dopant and superconductivity in Eu-substitutional Ba8Al5Si41 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	J.Alloys Compd., 694(2017)459	Lihua Liu,Yueting Ren,Bensheng Song,Jose Garcia,Hengyi Du,Xingqiao Ma,Yang Li		
156903	JAC6940459	Compositions: Ba7.77Eu0.23Al5.87Si40.13 By EDS	(Ba,Eu)8Al5Si41	Ba7.8Eu0.2Al5Si41	Ba	7.8	Eu	0.2	Al	5	Si	41																1	2017					myu-B/mol	7.45	5.58																			A8B46		clathrate	Pm3[-]n		A	10.4413														K				5.2			5.2																																																																																														Ba(4N),Eu(4N),Al(5N),Si(5N)		arc-melting ((8-x)*1.05:x:5:41) - ground and washed with dilute NaOH solution and HCl in order to remove impurity phases					Magnetic moment of Eu-dopant and superconductivity in Eu-substitutional Ba8Al5Si41 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	J.Alloys Compd., 694(2017)459	Lihua Liu,Yueting Ren,Bensheng Song,Jose Garcia,Hengyi Du,Xingqiao Ma,Yang Li		
156904	JAC6940459	Compositions: Ba7.75Eu0.25Al5.45Si40.55  By EDS	(Ba,Eu)8Al5Si41	Ba7.7Eu0.3Al5Si41	Ba	7.7	Eu	0.3	Al	5	Si	41																1	2017							5.71																			A8B46		clathrate	Pm3[-]n		A	10.4405														K				4.5			4.5																																																																																														Ba(4N),Eu(4N),Al(5N),Si(5N)		arc-melting ((8-x)*1.05:x:5:41) - ground and washed with dilute NaOH solution and HCl in order to remove impurity phases					Magnetic moment of Eu-dopant and superconductivity in Eu-substitutional Ba8Al5Si41 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	J.Alloys Compd., 694(2017)459	Lihua Liu,Yueting Ren,Bensheng Song,Jose Garcia,Hengyi Du,Xingqiao Ma,Yang Li		
156905	JAC6940459	Compositions: Ba7.63Eu0.37Al5.59Si40.41  By EDS	(Ba,Eu)8Al5Si41	Ba7.6Eu0.4Al5Si41	Ba	7.6	Eu	0.4	Al	5	Si	41																1	2017							7																			A8B46		clathrate	Pm3[-]n		A	10.4376														K					2																																																																																																Ba(4N),Eu(4N),Al(5N),Si(5N)		arc-melting ((8-x)*1.05:x:5:41) - ground and washed with dilute NaOH solution and HCl in order to remove impurity phases					Magnetic moment of Eu-dopant and superconductivity in Eu-substitutional Ba8Al5Si41 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	J.Alloys Compd., 694(2017)459	Lihua Liu,Yueting Ren,Bensheng Song,Jose Garcia,Hengyi Du,Xingqiao Ma,Yang Li		
156906	JAP111123912	C: interstitial sites by ND analysis.. Lattice term in SP (beta) = 0.395 mJ/mol.K4. (dC) = 120 mJ/mol.K. (dC/gamma*Tc) = 0.231(maybe small SC volume)	Nb5Ge3Cx	Nb5Ge3C0.3	Nb	5	Ge	3	C	0.3																		1	2012																										A3B5			P6<3>/mcm		A	7.65		5.307												K	15		15.3	15.3			15.3										25										T	(dR/dT), GL eq.	10.6												MHC156906		A	from Hc2	55																		mJ/mol.K2	34	SP	343	SP																																		graphite,Nb,Ge		mixture - press to 10*10*2 mm3 - sealed in quartz ampoule - heat(1200C,48h) - reground - press - sealed in quartz - SIN(1200C,96h) - rapid quench					Interstitial doping induced superconductivity at 15.3 K in Nb5Ge3 compound			Escola de Engenharia de Lorena?Universidade de Sao Paulo, P. O. Box 116, Lorena?SP 12600-970, Brazil	J.Appl.Phys., 111(2012)123912	A. D. Bortolozo,C. A. M. dos Santos,R. F. Jardim,C. Ritter,A. Devishvili,M. Rotter,F. G. Gandra,A. J. S. Machado		
156907	JPS085114708	not SC.RRR = 21. R(T) = A*T2 for T < 16 K, A = 1.0E-8 ohm.cm/K2. Kadowaki-Woods ratio (A/gamma^2) = 7.3E-6 uOhm.cm.mol2/mJ2. R0 at 2 K.	YbOs4Sb12	Yb1Os4Sb12	Yb	1	Os	4	Sb	12																		3	2016																										AB4C12		skutterudite			A	9.3193														K					2																																																										mJ/mol.K2	37	SP	226	SP											uOhm.cm				75.6			8.89				191			m3/C	0.00000000128					MRH156907			Yb(3N),Os(4N),Sb(6N)		(Yb:Os:Sb = 2:4:20) - sealed in silica tube - heat to 900C(60C/h) - keep(1day) - cool to 600C(60C/h) - ANN(600C, 1w) - furnace cool to RT					First Report on the Electronic, Magnetic, and Thermal Properties of Filled Skutterudite YbOs4Sb12			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)114708	Hiromu Kunitoshi,Tatsuma D. Matsuda,Ryo Midorikawa,Ryuji Higashinaka,Keitaro Kuwahara,Yuji Aoki,Hideyuki Sato		
156908	JPS085123703	SC island (x > 0.91) in SC matrix (x < 0.80). D (SC) escape slower than D (not SC). Ic defined as finite V in I-V characteristics. x = 0.80 from R(T) anomaly (T= 78K)	PdDx	D0.92Pd1	D	0.92	Pd	1																					2016																										AB																				K		6.8					6.8	MIV156908																																																																																													Pd(3N)-wire		D charged by electrolytic at RT. R(T) meaured immediately ater charging					Effect of Deuterium Interactions with Lattice Defects on Superconducting PdDx System			Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan	J.Phys.Soc.Jpn, 85(2016)123703	Syuma Yasuzuka,Norio Ogita,Daichi Anzai,Noriyuki Hatakenaka		
156909	JPS085123703	SC island (x > 0.91) in SC matrix (x < 0.80). D (SC) escape slower than D (not SC). Ic defined as finite V in I-V characteristics. x = 0.65 from R(T) anomaly (T= 62K)	PdDx	D0.91Pd1	D	0.91	Pd	1																					2016																										AB																				K		6.4					6.4	MIV156908																																																																																													Pd(3N)-wire		D charged by electrolytic at RT. R(T) measured after one month annealing at RT					Effect of Deuterium Interactions with Lattice Defects on Superconducting PdDx System			Research Center for Condensed Matter Physics, Hiroshima Institute of Technology, Hiroshima 731-5193, Japan	J.Phys.Soc.Jpn, 85(2016)123703	Syuma Yasuzuka,Norio Ogita,Daichi Anzai,Noriyuki Hatakenaka		
156910	JPS085124708	BiF3(<5%). fillamentary SC	Eu0.5La0.5FBiS2	Eu0.5La0.5F1Bi1S2	Eu	0.5	La	0.5	F	1	Bi	1	S	2														1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	1.2		2.2				1.7																																																																																														EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156911	JPS085124708	Two step SC-transitions.	Eu0.5La0.5FBi(S,Se)2	Eu0.5La0.5F1Bi1S1.8Se0.2	Eu	0.5	La	0.5	F	1	Bi	1	S	1.8	Se	0.2												1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	0.5		2.7				1.6																																																																																														EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156912	JPS085124708		Eu0.5La0.5FBi(S,Se)2	Eu0.5La0.5F1Bi1S1.6Se0.4	Eu	0.5	La	0.5	F	1	Bi	1	S	1.6	Se	0.4												1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	3						3	MTC156912																																																																																													EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156913	JPS085124708		Eu0.5La0.5FBi(S,Se)2	Eu0.5La0.5F1Bi1S1.4Se0.6	Eu	0.5	La	0.5	F	1	Bi	1	S	1.4	Se	0.6												1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	3.5						3.5																				T	RES													MHC156913																																																												EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156914	JPS085124708	Bi2Se3(12%). Two step SC transitions, Hc2 defined as R(on) for each transitions	Eu0.5La0.5FBi(S,Se)2	Eu0.5La0.5F1Bi1S1.2Se0.8	Eu	0.5	La	0.5	F	1	Bi	1	S	1.2	Se	0.8												1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	3.8		6.2				5																				T	RES													MHC156914																																																												EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156915	JPS085124708	Two step SC transitions, Hc2 defined as R(on) for each transitions	Eu0.5La0.5FBi(S,Se)2	Eu0.5La0.5F1Bi1S1Se1	Eu	0.5	La	0.5	F	1	Bi	1	S	1	Se	1												1	2016																										ABCD2			P4/nmm																BiS2-layered SC	K	3.69						3.69																																																																																														EuS,La2S3,BiF3,LaF3,Bi,S,Se		mixture - pelletize - sealed in quartz tube - heat(780C or 700C or 650C, 20h). one more process.					Bulk Superconductivity Induced by In-Plane Chemical Pressure Effect in Eu0.5La0.5FBiS2-xSex			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 85(2016)124708	Gen Jinno,Rajveer Jha,Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Masanori Nagao,Osuke Miura,Yoshikazu Mizuguchi		
156916	PRB084052509	<93>Nb-NMR measured. gap (d) = 10.3 K at Tc(H) = 5.8 K.	Re24Nb5	Nb5Re24	Nb	5	Re	24																				1	2011																										A5B24			I4[-]3m	217	A	9.6076													Re24Ti5 type	K				8.7			8.7																																																3.55	6																																													Re(4N7),Nb(3N5)		arc-melting - ANN(800C,5d, in quartz tube) - furnace cool to RT					Evidence for s-wave superconductivity in noncentrosymmetric Re24Nb5 from <93>Nb NMR measurements			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 84(2011)052509	C. S. Lue,T. H. Su,H. F. Liu,Ben-Li Young		
156917	PRB086174513	RRR = 6.1. penet = 213nm, Tc = 4.45K from muon-SR.. G-L = 8.0	BaPt4Ge12	Ba1Pt4Ge12	Ba	1	Pt	4	Ge	12																			2012																										AB4C12		skutterudite																		K				4.9			4.9											Oe	M-H curve				60			1.85	T	RES(mid), GL-eq.	1.46												MHC156917		A	M-H curve(1.7K)	255			nm	M-H curve(1.7K)	2.4			meV	0.65	3.4	16																						uOhm.m							15.1				90																			Superconducting parameters of BaPt4-xAuxGe12 filled skutterudite			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174513	A. Maisuradze,R. Gumeniuk,W. Schnelle,M. Nicklas,C. Baines,R. Khasanov,A. Amato,A. Leithe-Jasper		
156918	PRB086174513	penet = 241 nm, Tc = 4.93K from muon-SR.. G-L = 12.7	Ba(Pt,Au)4Ge12	Ba1Pt3.5Au0.5Ge12	Ba	1	Pt	3.5	Au	0.5	Ge	12																	2012																										AB4C12		skutterudite																		K				5.3			5.3																				T	muon-SR				0.84			1.7								A	M-H curve(1.7K)	188			nm	M-H curve(1.7K)	239			meV	0.88	4.14	16																						uOhm.m							33.6																							Superconducting parameters of BaPt4-xAuxGe12 filled skutterudite			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174513	A. Maisuradze,R. Gumeniuk,W. Schnelle,M. Nicklas,C. Baines,R. Khasanov,A. Amato,A. Leithe-Jasper		
156919	PRB086174513	penet = 243nm, Tc = 6.10 K from muon-SR.. G-L = 16.0	Ba(Pt,Au)4Ge12	Ba1Pt3.25Au0.75Ge12	Ba	1	Pt	3.25	Au	0.75	Ge	12																	2012																										AB4C12		skutterudite																		K				6.25			6.25																				T	muon-SR				1.68			1.7								A	M-H curve(1.7K)	150			nm	M-H curve(1.7K)	240			meV	1.13	4.3	16																						uOhm.m							36.8																							Superconducting parameters of BaPt4-xAuxGe12 filled skutterudite			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174513	A. Maisuradze,R. Gumeniuk,W. Schnelle,M. Nicklas,C. Baines,R. Khasanov,A. Amato,A. Leithe-Jasper		
156920	PRB086174513	penet = 210nm, Tc = 6.86 K from muon-SR.. G-L = 15.7	Ba(Pt,Au)4Ge12	Ba1Pt3Au1Ge12	Ba	1	Pt	3	Au	1	Ge	12																	2012																										AB4C12		skutterudite																		K				6.95			6.95											Oe	M-H curve				117				T	muon-SR				1.93			1.7								A	M-H curve(1.7K)	134			nm	M-H curve(1.7K)	210			meV	1.2	4.04	16																						uOhm.m							31.5																							Superconducting parameters of BaPt4-xAuxGe12 filled skutterudite			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 86(2012)174513	A. Maisuradze,R. Gumeniuk,W. Schnelle,M. Nicklas,C. Baines,R. Khasanov,A. Amato,A. Leithe-Jasper		
156921	PRB087214509	RRR = 200. residual-gamma = 108 mJ/mol.K2. beta(SP) = 0.466 mJ/mol.K4, delta(SP) = 0.00474 mJ/mol.K6. (dC/gamma*Tc) = 0.35. (dC/Tc) = 64 mJ/mol.K2	CsFe2As2	Cs1Fe2As2	Cs	1	Fe	2	As	2																		3	2013																										AB2C2		ThCr2Si2			A			15.13											Fe-122	K	1.8		1.88				1.84																				T	SP(mid)	1.65																																		mJ/mol.K2	184.01	SP	275	SP											uOhm.cm							1.8																		(Cs:Fe:As = 6:1:6) - alumina crucible - sealed in stainless container - sealed in quartz tube - heat(200C,400min) - heat to 950 C within 10h - keep(10h) - cool to 550c (3C/h)					Calorimetric study of single-crystal CsFe2As2			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China,n Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 87(2013)214509	A. F. Wang,B. Y. Pan,X. G. Luo,F. Chen,Y. J. Yan,J. J. Ying,G. J. Ye,P. Cheng,X. C. Hong,S. Y. Li,X. H. Chen		
156922	PRB088180509	Hc2(0) from reference data. effective-[penet] (1.7K) = 637 nm from muon-SR. [penet](1.7K) //ab obtained from [penet]eff. G-L = 85.	LaOs0.5F0.5BiS2	La0.5Bi1S2F0.5O0.5	La	0.5	Bi	1	S	2	F	0.5													O	0.5		1	2013																																													BiS2-layered	K		10					10																				T		10														A	from Hc2	57			nm	muon-SR		484																																																				High-P synthesis. mixture - pellet - ANN(600C, P=2 GPa)					s-wave pairing in the optimally doped LaO0.5F0.5BiS2 superconductor			CNR-SPIN and Universita di Genova, via Dodecaneso 33, I-16146 Genova, Italy	Phys.Rev.B, 88(2013)180509	G. Lamura,T. Shiroka,P. Bonf`,S. Sanna,R. De Renzi,C. Baines,H. Luetkens,J. Kajitani,Y. Mizuguchi,O. Miura,K. Deguchi,S. Demura,Y. Takano,M. Putti		
156923	PRB088224514	under doped sample. point defect introduced by H+-ion irradiation. dR0(in Fig) = R0(irrad) - R0. dR0<cr>(Tc tends to 0 K) = 376 uOhm.cm	(Ba,K)Fe2As2	Ba0.77K0.23Fe2As2	Ba	0.77	K	0.23	Fe	2	As	2																3	2013																										AB2C2																			Fe-122	K		24.4					24.4	MTC156924																																																																																															FeAs flux method. Other flux for x=0.69. cleaved samples with thickness less than 25 micron meter					Pair-breaking effects induced by 3-MeV proton irradiation in Ba1-xKxFe2As2			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 88(2013)224514	Toshihiro Taen,Fumiaki Ohtake,Hiroki Akiyama,Hiroshi Inoue,Yue Sun,Sunseng Pyon,Tsuyoshi Tamegai,Hisashi Kitamura		
156924	PRB088224514	Optimaly doped sample. point defect introduced by H+-ion irradiation. dR0(in Fig) = R0(irrad) - R0. dR0<cr>(Tc tends to 0 K) = 396 uOhm.cm	(Ba,K)Fe2As2	Ba0.58K0.42Fe2As2	Ba	0.58	K	0.42	Fe	2	As	2																3	2013																										AB2C2																			Fe-122	K		37.4					37.4	MTC156924																																																																																															FeAs flux method. Other flux for x=0.69. cleaved samples with thickness less than 25 micron meter					Pair-breaking effects induced by 3-MeV proton irradiation in Ba1-xKxFe2As2			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 88(2013)224514	Toshihiro Taen,Fumiaki Ohtake,Hiroki Akiyama,Hiroshi Inoue,Yue Sun,Sunseng Pyon,Tsuyoshi Tamegai,Hisashi Kitamura		
156925	PRB088224514	Over doped sample. point defect introduced by H+-ion irradiation. dR0(in Fig) = R0(irrad) - R0. dR0<cr>(Tc tends to 0 K) = 110 uOhm.cm	(Ba,K)Fe2As2	Ba0.31K0.69Fe2As2	Ba	0.31	K	0.69	Fe	2	As	2																3	2013																										AB2C2																			Fe-122	K		17.8					17.8	MTC156925																																																																																															FeAs flux method. Other flux for x=0.69. cleaved samples with thickness less than 25 micron meter					Pair-breaking effects induced by 3-MeV proton irradiation in Ba1-xKxFe2As2			Department of Applied Physics, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan	Phys.Rev.B, 88(2013)224514	Toshihiro Taen,Fumiaki Ohtake,Hiroki Akiyama,Hiroshi Inoue,Yue Sun,Sunseng Pyon,Tsuyoshi Tamegai,Hisashi Kitamura		
156926	PRB089134504	RRR = 6.96  . Anisotropy = 2.09 (onset),  2.07 (off). K-content x from WDS.	(Ba,K)Fe2As2	Ba0.78K0.22Fe2As2	Ba	0.78	K	0.22	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.1673											Fe-122	K				24.8			24.8																				T	R(on),R(off), WHH		92.6	43.9					T/K	R(on), R(off)		5.36	2.55	MHC156926																																					uOhm.cm											364														starting (Ba:K:Fe:As = 1-x:x:6:6), soaking temperature = 1453 K, soaking time = 2h, cooling rate = 2K/h to 1313 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156927	PRB089134504	RRR = 10.2  . Anisotropy = 2.09 (onset),  2.06 (off). K-content x from WDS.	(Ba,K)Fe2As2	Ba0.66K0.34Fe2As2	Ba	0.66	K	0.34	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.273											Fe-122	K				38.9			38.9																				T	R(on),R(off), WHH		253	124.7					T/K	R(on), R(off)		9.48	4.79	MHC156927																																					uOhm.cm											300														starting (Ba:K:Fe:As = 1-x:2x:4:5), soaking temperature = 1413 K, soaking time = 2h, cooling rate = 1K/h to 1293 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156928	PRB089134504	RRR = 9.69  . Anisotropy = 1.90 (onset),  2.09 (off). K-content x from WDS	(Ba,K)Fe2As2	Ba0.61K0.39Fe2As2	Ba	0.61	K	0.39	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.2796											Fe-122	K				38.6			38.6																				T	R(on),R(off), WHH		282	142.5					T/K	R(on), R(off)		10.35	5.23	MHC156928																																					uOhm.cm											340														starting (Ba:K:Fe:As = 1-x:2x:4:5), soaking temperature = 1413 K, soaking time = 2h, cooling rate = 1K/h to 1293 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156929	PRB089134504	RRR = 10.9  . Anisotropy = 1.65 (onset),  2.00 (off). K-content x from WDS	(Ba,K)Fe2As2	Ba0.53K0.47Fe2As2	Ba	0.53	K	0.47	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.3201											Fe-122	K																											T	R(on),R(off), WHH		238	156					T/K	R(on), R(off)		8059	5.68	MHC156929																																					uOhm.cm											327														starting (Ba:K:Fe:As = 1-x:2x:4:5), soaking temperature = 1413 K, soaking time = 2h, cooling rate = 1K/h to 1293 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156930	PRB089134504	RRR = 12.2  . Anisotropy = 2.44 (onset),  2.45 (off). K-content x from WDS	(Ba,K)Fe2As2	Ba0.47K0.53Fe2As2	Ba	0.47	K	0.53	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.4235											Fe-122	K				34.3			34.3	MTC156930																			T	R(on),R(off), WHH		193	83.6					T/K	R(on), R(off)		7.88	3.42	MHC156930																																					uOhm.cm																									starting (Ba:K:Fe:As = 1-x:2x:4:5), soaking temperature = 1413 K, soaking time = 2h, cooling rate = 1K/h to 1293 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156931	PRB089134504	RRR = 11.56  . Anisotropy = 2.13 (onset),  2.56 (off).  K-content x from WDS	(Ba,K)Fe2As2	Ba0.45K0.55Fe2As2	Ba	0.45	K	0.55	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.4275											Fe-122	K				33.1			33.1																				T	R(on),R(off), WHH		183	88.6					T/K	R(on), R(off)		8.04	3.97	MHC156931																																					uOhm.cm											397														starting (Ba:K:Fe:As = 1-x:3x:4:5), soaking temperature = 1393 K, soaking time = 2h, cooling rate = 0.5K/h to 1293 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156932	PRB089134504	RRR =  11.6 .  Anisotropy = 2.71 (onset), 2.89  (off)). K-content x from WDS	(Ba,K)Fe2As2	Ba0.35K0.65Fe2As2	Ba	0.35	K	0.65	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.5102											Fe-122	K				24.8			24.8																				T	R(on),R(off), WHH		99	37.2					T/K	R(on), R(off)		5.84	2.09	MHC156932																																					uOhm.cm											370														starting (Ba:K:Fe:As = y:4:2:5 and Ba:y  for y = 0.2-0.3), soaking temperature = 1273 K, soaking time = 6h, cooling rate = 4K/h to 1173,then 1K/h to 973 K K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156933	PRB089134504	RRR =  12.0 .  Anisotropy = 3.04 (onset), 3.22  (off)).  K-content x from WDS	(Ba,K)Fe2As2	Ba0.2K0.8Fe2As2	Ba	0.2	K	0.8	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.5633											Fe-122	K				14.5			14.5																				T	R(on),R(off), WHH		61.8	19.8					T/K	R(on), R(off)		5.11	1.61	MHC156933																																																														starting (Ba:K:Fe:As = y:4:2:5 and Ba:y  for y = 0.2-0.3), soaking temperature = 1273 K, soaking time = 6h, cooling rate = 4K/h to 1173,then 1K/h to 973 K K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156934	PRB089134504	RRR = 9.73  .  Anisotropy = 2.33 (onset),  2.56 (off)).  K-content x from WDS	(Ba,K)Fe2As2	Ba0.18K0.82Fe2As2	Ba	0.18	K	0.82	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.6403											Fe-122	K				10			10																				T	R(on),R(off), WHH		24.9	10.3					T/K	R(on), R(off)		3.86	1.53	MHC156934																																					uOhm.cm											338														starting (Ba:K:Fe:As = y:4:2:5 and Ba:y  for y = 0.2-0.3), soaking temperature = 1273 K, soaking time = 6h, cooling rate = 4K/h to 1173,then 1K/h to 973 K K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156935	PRB089134504	RRR =  12.3 .  Anisotropy = 3.93 (onset), 3.93  (off)).  K-content x from WDS	(Ba,K)Fe2As2	Ba0.1K0.9Fe2As2	Ba	0.1	K	0.9	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.767											Fe-122	K				7.39			7.39																				T	R(on),R(off), WHH		21.1	7.84					T/K	R(on), R(off)		4.12	1.07	MHC156935																																																														Starting (Ba:K:Fe:As = y:4:2:5, y = 0.1). soaking temperature = 1273K, soaking time = 2h, cooling rate = 3K/h to 1173K, then 1K/h to 973 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156936	PRB089134504	RRR = 12.5  .  Anisotropy = 3.83 (onset), 3.85 (off)).   K-content x from WDS	(Ba,K)Fe2As2	Ba0.08K0.92Fe2As2	Ba	0.08	K	0.92	Fe	2	As	2																3	2014																										AB2C2	2	ThCr2Si2			A			13.7716											Fe-122	K				6.37			6.37																				T	R(on),R(off), WHH		17.8	5.94					T/K	R(on), R(off)		3.61	1.03	MHC156936																																					uOhm.cm											308														Starting (Ba:K:Fe:As = y:4:2:5, y = 0.1). soaking temperature = 1273K, soaking time = 2h, cooling rate = 3K/h to 1173K, then 1K/h to 973 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156937	PRB089134504	RRR =  12.5 .  Anisotropy = 5.02 (onset),  6.48 (off)).  K-content x from WDS	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		3	2014																										AB2C2	2	ThCr2Si2			A			13.8629											Fe-122	K				3.94			3.94																				T	R(on),R(off), WHH		10.1	3.24					T/K	R(on), R(off)		3.06	0.52	MHC156937																																					uOhm.cm											284														Starting (Ba:K:Fe:As = y:5:2:6,  y=0). soaking temperature = 1193K, soaking time = 1h, cooling rate = 4K/h to 1093K, then 1K/h to 893 K.					Comprehensive scenario for single-crystal growth and doping dependence of resistivity and anisotropic upper critical fields in (Ba1-xKx)Fe2As2 (0.22 =< x =< 1)			Division of Materials Sciences and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.B, 89(2014)134504	Y. Liu,M. A. Tanatar,W. E. Straszheim,B. Jensen,K. W. Dennis,R. W. McCallum,V. G. Kogan,R. Prozorov,T. A. Lograsso		
156938	PRB090140507	muon-SR. [penet](1.7K) = 134 nm using two band (gap1=gap2 but different Fermi velocity). (dHc2/dT) = -0.77 T/K for T < 6K.	SrPt3P	Sr1Pt3P1	Sr	1	Pt	3	P	1																		1	2014																										ABC3																				K				8.4			8.4																				T	SUS								T/K	SUS	0.49			MHC156938							nm	muon-SR	162			meV	1.55	4.29	16																																													Sr,Pt,P purity all 4N		High-T-High-P synthesis using cubic anvil. mixture - in BN - heat to 1050C at P=2 GPa - keep(20-40h) - cool to RT in 1h					SrPt3P: A two-band single-gap superconductor			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 90(2014)140507	R. Khasanov,A. Amato,P. K. Biswas,H. Luetkens,N. D. Zhigadlo,B. Batlogg		
156939	PRB090214508	M = NH3. x and y not given.	LixMyFe2Se2	Li0.45M0.3Fe2Se2	Li	0.45	M	0.3	Fe	2	Se	2																	2014																															A	3.8287		16.452											LiM-122, phase1	K				41.2			41.2																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156940	PRB090214508	M = NH3. x and y not given.	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se1.8Te0.2	Li	0.45	M	0.3	Fe	2	Se	1.8	Te	0.2															2014																															A	3.8309		16.699											LiM-122. phase1	K				42.3			42.3																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156941	PRB090214508	M = NH3. x and y not given. Two phase-SC, Tc = 25.5 K for phase2.	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se1.6Te0.4	Li	0.45	M	0.3	Fe	2	Se	1.6	Te	0.4															2014																															A	3.8398		16.762											LiM-122. Two phses, for phase2, a=3.8545, c=17.685	K				41.5			41.5																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156942	PRB090214508	M = NH3. x and y not given. Two phase-SC, Tc = 22.8 K for phase2.	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se1.4Te0.6	Li	0.45	M	0.3	Fe	2	Se	1.4	Te	0.6															2014																															A	3.837		16.893											LiM-122.Two phases,  for phase 2, a=3.8558, c=17.782	K				38.8			38.8	MPH156942																																																																																															samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156943	PRB090214508	M = NH3. x and y not given.  Two phase-SC, Tc = 25.2 K for phase2.	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se1.2Te0.8	Li	0.45	M	0.3	Fe	2	Se	1.2	Te	0.8															2014																															A	3.8418		17.031											LiM-122. Two phases, for phase2 a=3.8613, c=17.813	K				36.6			36.6																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156944	PRB090214508	M = NH3. x and y not given.	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se1Te1	Li	0.45	M	0.3	Fe	2	Se	1	Te	1															2014																															A	3.8591		17.845											LiM-122. phase2	K				21.7			21.7	MPH156942																																																																																															samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156945	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 26.7 K	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se0.8Te1.2	Li	0.45	M	0.3	Fe	2	Se	0.8	Te	1.2															2014																															A	3.8666		17.869											LiM-122. phase2	K				16.5			16.5																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156946	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 32.9 K	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se0.6Te1.4	Li	0.45	M	0.3	Fe	2	Se	0.6	Te	1.4															2014																															A	3.8764		17.985											LiM-122. phase2	K				8.1			8.1																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156947	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 29.1 K	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se0.4Te1.6	Li	0.45	M	0.3	Fe	2	Se	0.4	Te	1.6															2014																															A	3.8893		18.168											LiM-122. phase2	K				0			0																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156948	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 38.1 K	LixMyFe2(Se,Te)2	Li0.45M0.3Fe2Se0.2Te1.8	Li	0.45	M	0.3	Fe	2	Se	0.2	Te	1.8															2014																															A	3.8959		18.359											LiM-122. phase2	K				0			0																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156949	PRB090214508	M = NH3. x and y not given. AFM at 30.0 K	LixMyFe2Te2	Li0.45M0.3Fe2Te2	Li	0.45	M	0.3	Fe	2	Te	2																	2014																															A	3.894		18.371											LiM-122. phase2	K				0			0																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156950	PRB090214508	M = NH3. x and y not given.	NaxMyFe2Se2	Na0.45M0.3Fe2Se2	Na	0.45	M	0.3	Fe	2	Se	2																	2014																															A	3.8012		17.435											NaM-122. phase1	K				45.6			45.6																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156951	PRB090214508	M = NH3. x and y not given.	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se1.8Te0.2	Na	0.45	M	0.3	Fe	2	Se	1.8	Te	0.2															2014																															A	3.8174		17.5											NaM-122. phase1	K				44.2			44.2																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156952	PRB090214508	M = NH3. x and y not given. Two phase-SC, Tc = 25.7 K for phase2.	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se1.6Te0.4	Na	0.45	M	0.3	Fe	2	Se	1.6	Te	0.4															2014																															A	3.8271		17.535											NaM-122. Two phases, for phase2, a=3.8413, c=18.089	K				43.2			43.2																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156953	PRB090214508	M = NH3. x and y not given. Two phase-SC, Tc = 22.0 K for phase2.	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se1.4Te0.6	Na	0.45	M	0.3	Fe	2	Se	1.4	Te	0.6															2014																															A	3.8283		17.599											NaM-122. Two phases, for phase2, a=3.8531, c=18.211	K				42.5			42.5	MPH156953																																																																																															samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156954	PRB090214508	M = NH3. x and y not given. Two phase-SC, Tc = 23.1 K for phase2.	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se1.2Te0.8	Na	0.45	M	0.3	Fe	2	Se	1.2	Te	0.8															2014																															A	3.8319		17.666											NaM-122. Two phases, for phase2, a=3.8541, c=18.302	K				39.6			39.6																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156955	PRB090214508	M = NH3. x and y not given.	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se1Te1	Na	0.45	M	0.3	Fe	2	Se	1	Te	1															2014																															A	3.8647		18.259											NaM-122. phase2	K				23.1			23.1	MPH156953																																																																																															samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156956	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 31.7 K	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se0.8Te1.2	Na	0.45	M	0.3	Fe	2	Se	0.8	Te	1.2															2014																															A	3.8622		18.401											NaM-122. phase2	K				17.4			17.4																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156957	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 33.3 K	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se0.6Te1.4	Na	0.45	M	0.3	Fe	2	Se	0.6	Te	1.4															2014																															A	3.8742		18.438											NaM-122. phase2	K				9.5			9.5																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156958	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 34.3 K	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se0.4Te1.6	Na	0.45	M	0.3	Fe	2	Se	0.4	Te	1.6															2014																															A	3.8703		18.697											NaM-122. phase2	K				0			0																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156959	PRB090214508	M = NH3. x and y not given. T<spin-glass > = 38.0 K	NaxMyFe2(Se,Te)2	Na0.45M0.3Fe2Se0.2Te1.8	Na	0.45	M	0.3	Fe	2	Se	0.2	Te	1.8															2014																															A	3.8724		18.78											NaM-122. phase2	K				0			0																																																																																																samples prepared by solid state reaction. reaction vessel(sample with NH3) stirred (223-243K, 3-10h). after intercalation, vessel opened and NH3 evaporated					Emergence of magnetism and controlling factors of superconductivity in Li/Na-ammonia cointercalated FeSe1-zTez			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 90(2014)214508	Hechang Lei,Jiangang Guo,Fumitaka Hayashi,Hideo Hosono		
156960	PRB091094514	Tc(max) = 8.49 K(P = 9.90 kbar). gap from SP using alpha-model. (dC/gamma*Tc) = 1.87.	SrPt3P	Sr1Pt3P1	Sr	1	Pt	3	P	1																		1	2015																										ABC3																				K		8.35	8.4			0.5	8.35	MTC156960																																													meV	1.65	4.8	14							mJ/mol.K2	6.31	SP																																											High-pressure and doping studies of the superconducting antiperovskite SrPt3P			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 91(2015)094514	BenMaan I. Jawdat,Bing Lv,Xiyu Zhu,Yuyi Xue,Ching-wu Chu		
156961	PRB091094514	gap from SP using alpha-model.  (dC/gamma*Tc) = 1.28.	SrPt3P1-xSix	Sr1Pt3P0.8Si0.2	Sr	1	Pt	3	P	0.8	Si	0.2																1	2015																										ABC3																				K			7.8			1	7.8																																														meV	1.28	4.4	14							mJ/mol.K2	7.77	SP																																											High-pressure and doping studies of the superconducting antiperovskite SrPt3P			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 91(2015)094514	BenMaan I. Jawdat,Bing Lv,Xiyu Zhu,Yuyi Xue,Ching-wu Chu		
156962	PRB091094514		SrPt3P1-xSix	Sr1Pt3P0.6Si0.4	Sr	1	Pt	3	P	0.6	Si	0.4																1	2015																										ABC3																				K			7.5				7.5																																																																																																					High-pressure and doping studies of the superconducting antiperovskite SrPt3P			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 91(2015)094514	BenMaan I. Jawdat,Bing Lv,Xiyu Zhu,Yuyi Xue,Ching-wu Chu		
156963	PRB091094514		SrPt3P1-xSix	Sr1Pt3P0.4Si0.6	Sr	1	Pt	3	P	0.4	Si	0.6																1	2015																										ABC3																				K			7				7																																																																																																					High-pressure and doping studies of the superconducting antiperovskite SrPt3P			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 91(2015)094514	BenMaan I. Jawdat,Bing Lv,Xiyu Zhu,Yuyi Xue,Ching-wu Chu		
156964	PRB091134508	RRR= R300/R10K) = 1.14 (ab-plane). SP heat, (beta) = 0.039 mJ/mol.K4, (delta) = 2.6E-4 mJ/mol.K6. Two band gap analysis D1 = 1.86meV (in DB), D2  = 1.36 meV.	Nb0.18Re0.82	Nb0.18Re0.82	Nb	0.18	Re	0.82																				3	2015																																														K		8.5					8.5																																														meV	1.86		14							mJ/mol.K2	6.1	SP																																						Floating zone method					Evidence of double-gap superconductivity in noncentrosymmetric Nb0.18Re0.82 single crystals			"CNR-SPIN and Dipartimento di Fisica ""E. R. Caianiello"", Universita di Salerno, I-84084 Fisciano (Salerno), Italy"	Phys.Rev.B, 91(2015)134508	C. Cirillo,R. Fittipaldi,M. Smidman,G. Carapella,C. Attanasio,A. Vecchione,R. P. Singh,M. R. Lees,G. Balakrishnan,M. Cuoco		
156965	PRB093144502	RRR = 2.8. Anisotropy (Hc2) = 1.25. Anisotropy = 1.14(Hc1), = 1.25(Hc2,penet). GL(kappa) = 5.7. Hc2(R-mid) corresponts to Hc3, not shown in Fig.	beta-Bi2Pd	Bi2Pd1	Bi	2	Pd	1																				3	2016																										AB2																				K		4.93				0.1	4.93											mT	Hall probe, demag-correction		19.7	22.5					T	SP(mid), extrapolation.		0.76	0.61										MHC156965		nm	from Hc2		23.2	18.5	nm	Hc1,GL(kappa), GL-eq.		132	105			4.1	14																																													Bi,Pd		melt-growth technique (quartz ampoule, 140 mbar-He gas)					Single-gap superconductivity in beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics, Slovak Academy of Sciences, and P. J. Safarik University, 040 01 Kosice, Slovakia	Phys.Rev.B, 93(2016)144502	J. Kacmarcik,Z. Pribulova,T. Samuely,P. Szabo,V. Cambel,J. Soltys,,E. Herrera,H. Suderow,A. Correa-Orellana,D. Prabhakaran,P. Samuely		
156966	PRB093144514	There are three phases depending on pressure. SG(spacegroup) = R-3m for P < 10GPa.	Sr0.065Bi2Se3	Sr0.065Bi2Se3	Sr	0.065	Bi	2	Se	3																		3	2016																													R-3m		A	4.1132		28.622											topological insulator	K			3				3	MLAT156966																																																																																															See ACS13710512					Pressure-induced reemergence of superconductivity in topological insulator Sr0.065Bi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B, 93(2016)144514	Yonghui Zhou,Xuliang Chen,Ranran Zhang,Jifeng Shao,Xuefei Wang,Chao An,Ying Zhou,Changyong Park,Wei Tong,Li Pi,Zhaorong Yang,Changjin Zhang,Yuheng Zhang		
156967	PRB093144514	There are three phases depending on pressure. SG(spacegroup) = C2/m for 10 < P < 30GPa. Reemerging SC. Fig-Hc2(T) at P = 19.5 GPa.	Sr0.065Bi2Se3	Sr0.065Bi2Se3	Sr	0.065	Bi	2	Se	3																		3	2016																													C2/m		A	13.784	3.7419	16.465											topological insulator	K			7.78				7.78	MTC156967																			T	RES(0.9Rn)													MHC156967																																																														See ACS13710512					Pressure-induced reemergence of superconductivity in topological insulator Sr0.065Bi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B, 93(2016)144514	Yonghui Zhou,Xuliang Chen,Ranran Zhang,Jifeng Shao,Xuefei Wang,Chao An,Ying Zhou,Changyong Park,Wei Tong,Li Pi,Zhaorong Yang,Changjin Zhang,Yuheng Zhang		
156968	PRB093144514	There are three phases depending on pressure. SG(spacegroup) = I4/mmm for 30 GPa < P  Reemerging SC.	Sr0.065Bi2Se3	Sr0.065Bi2Se3	Sr	0.065	Bi	2	Se	3																		3	2016																													I4/mmm		A	3.3615		16.636											topological insulator	K			7.07				7.07	MTC156967																																																																																															See ACS13710512					Pressure-induced reemergence of superconductivity in topological insulator Sr0.065Bi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, China	Phys.Rev.B, 93(2016)144514	Yonghui Zhou,Xuliang Chen,Ranran Zhang,Jifeng Shao,Xuefei Wang,Chao An,Ying Zhou,Changyong Park,Wei Tong,Li Pi,Zhaorong Yang,Changjin Zhang,Yuheng Zhang		
156969	PRB094214513	non-stoichiometric. Re:Zr = 85.7:14.3.  gap derived from 1/T1 of NQR.	Re6Zr1	Re6Zr1	Re	6	Zr	1																				1	2016																												alpha-Mn	I4[-]3m		A	9.714														K				6.72			6.72																																																3.58	6																																													Re(4N),Zr(3N)		arc-melting					Full-gap superconductivity in noncentrosymmetric Re6Zr, Re27Zr5, and Re24Zr5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 94(2016)214513	K. Matano,R. Yatagai,S. Maeda,Guo-qing Zheng		
156970	PRB094214513	non-stoichiometric.  Re:Zr = 84.4:15.6.  gap derived from 1/T1 of NQR	Re27Zr5	Re27Zr5	Re	27	Zr	5																				1	2016																												alpha-Mn	I4[-]3m		A	9.726														K				6.53			6.53																																																3.55	6																																													Re(4N),Zr(3N)		arc-melting					Full-gap superconductivity in noncentrosymmetric Re6Zr, Re27Zr5, and Re24Zr5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 94(2016)214513	K. Matano,R. Yatagai,S. Maeda,Guo-qing Zheng		
156971	PRB094214513	stoichiometric. Re:Zr = 82.8:17.2.  gap derived from 1/T1 of NQR	Re24Zr5	Re24Zr5	Re	24	Zr	5																				1	2016																												alpha-Mn	I4[-]3m		A	9.762														K				5			5																																																3.51	6																																													Re(4N),Zr(3N)		arc-melting					Full-gap superconductivity in noncentrosymmetric Re6Zr, Re27Zr5, and Re24Zr5			Department of Physics, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 94(2016)214513	K. Matano,R. Yatagai,S. Maeda,Guo-qing Zheng		
156972	PRB094224508	RRR=1.77. T<STR>=46.9K (cubic-Tetra). A(T-linear term coeff. in R(T)) = 4.2E-8 Ohm.cm/K.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2016																										A3B7																				K		2.37					2.37	MPH156972																																																																						uOhm.cm							99.8																		Sb-flux method					Competition of superconductivity with the structural transition in Mo3Sb7			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)224508	G. Z. Ye,J.-G. Cheng,J.-Q. Yan,J. P. Sun,K. Matsubayashi,T. Yamauchi,T. Okada,Q. Zhou,D. S. Parker,B. C. Sales,Y. Uwatoko		
156973	PRB094224508	RRR=2.37. T<STR>=46.6 K (cubic-Tetra). A(T-linear term coeff. in R(T)) = 11.7E-8 Ohm.cm/K.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2016																										A3B7																				K		2.36					2.36	MPH156973																																																																													95																		Sb-flux method					Competition of superconductivity with the structural transition in Mo3Sb7			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)224508	G. Z. Ye,J.-G. Cheng,J.-Q. Yan,J. P. Sun,K. Matsubayashi,T. Yamauchi,T. Okada,Q. Zhou,D. S. Parker,B. C. Sales,Y. Uwatoko		
156974	PRB094224508	RRR = 1.94. T<STR>=45.9K (cubic-Tetra). -(dHc2/dT) = 1.33, 1.42, 1.52, 1.57, 1.57, 1.54 T/K and Hc2(0) = 4.0, 5.1, 6.1, 8.9, 8.7, 8.5 T for P = 3.5, 6, 8.5, 12, 14, 15 GPa, respectively.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2016																										A3B7																				K		2.35					2.35	MPH156974																			T	RES(0.5Rn), linear fitting	2.96							T/K	RES(0.5Rn)	1.25			MHC156974																																												79.6																		Sb-flux method					Competition of superconductivity with the structural transition in Mo3Sb7			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 94(2016)224508	G. Z. Ye,J.-G. Cheng,J.-Q. Yan,J. P. Sun,K. Matsubayashi,T. Yamauchi,T. Okada,Q. Zhou,D. S. Parker,B. C. Sales,Y. Uwatoko		
156975	PRB095014502	RRR = 60. Anisotropy = (Hc2//c)/(Hc2/n/c) = 3.3(5.8K), = 0.82(1.68K). Angular dependence of Hc2 measured. (//c) means (//rod axis), current direction.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2017																										A2B3C3		K2Cr3As3																		K		6.2					6.2																				T	max of dR/dt					26	19.6	1.68	T/K	max of dR/dT		4.2	10.3	MHC156975																																																														self flux method					Temperature and angular dependence of the upper critical field in K2Cr3As3			Wuhan National High Magnetic Field Center, School of Physics, Huazhong University of Science and Technology, Wuhan 430074, China	Phys.Rev.B, 95(2017)014502	Huakun Zuo,Jin-Ke Bao,Yi Liu,Jinhua Wang,Zhao Jin,Zhengcai Xia,Liang Li,Zhuan Xu,Jian Kang,Zengwei Zhu,Guang-Han Cao		
156976	PRB095014507	P-induced SC. P<cr> = 3.6 GPa. Hc2-FIG shows Hc2/Tc vs P. Tc in TC-FIG. Structural transition (fcc-to-tetra) at 11 GPa.	LaBi	Bi1La1	Bi	1	La	1																				3	2017																										AB			Fm3[-]m																phase transition(fcc-to-tetra) to P4/mmm at P=11 GPa.	K	4.1				0		4.1	MTC156976																			T	R(zero), GL fitting													MHC156976																																																			mm3/C						MRH156976					In-flux method					Tuning the electronic and the crystalline structure of LaBi by pressure: From extreme magnetoresistance to superconductivity			Department of Physics, Boston College, Boston, Massachusetts, 02467 USA	Phys.Rev.B, 95(2017)014507	F. F. Tafti,M. S. Torikachvili,R. L. Stillwell,B. Baer,E. Stavrou,S. T. Weir,Y. K. Vohra,H.-Y. Yang,E. F. McDonnell,S. K. Kushwaha,Q. D. Gibson,R. J. Cava,J. R. Jeffries		
156977	PRB095014507	P-induced SC. data shows at P = 5.6 GPa.	LaBi(P=5.6GPa)	Bi1La1	Bi	1	La	1																				3	2017																										AB			Fm3[-]m																phase transition(fcc-to-tetra) to P4/mmm at P=11 GPa.	K	6.12						6.12																				T	R(zero), GL fitting	11.5												MHC156977																																																														In-flux method					Tuning the electronic and the crystalline structure of LaBi by pressure: From extreme magnetoresistance to superconductivity			Department of Physics, Boston College, Boston, Massachusetts, 02467 USA	Phys.Rev.B, 95(2017)014507	F. F. Tafti,M. S. Torikachvili,R. L. Stillwell,B. Baer,E. Stavrou,S. T. Weir,Y. K. Vohra,H.-Y. Yang,E. F. McDonnell,S. K. Kushwaha,Q. D. Gibson,R. J. Cava,J. R. Jeffries		
156978	PRB095014507	P-induced SC. data shows at P = 17.9 GPa. Space G = P4/mmm for P > 11 GPa.	LaBi(P=17.9GPa)	Bi1La1	Bi	1	La	1																				3	2017																										AB			P4/mmm																	K	7.2						7.2																				T	R(zero), GL fitting	6.1												MHC156977																																																														In-flux method					Tuning the electronic and the crystalline structure of LaBi by pressure: From extreme magnetoresistance to superconductivity			Department of Physics, Boston College, Boston, Massachusetts, 02467 USA	Phys.Rev.B, 95(2017)014507	F. F. Tafti,M. S. Torikachvili,R. L. Stillwell,B. Baer,E. Stavrou,S. T. Weir,Y. K. Vohra,H.-Y. Yang,E. F. McDonnell,S. K. Kushwaha,Q. D. Gibson,R. J. Cava,J. R. Jeffries		
156979	PRB095024510	P-induced SC. P<cr> = 2.55 GPa. Bi-I(P<2.55 GPa), Bi-II(2.55<P<2.70 GPa), Bi-III(2.70<P<7.7 GPa), Bi-V(P.8 GPa, Bi-IV phase at T.450 K. Hc2(0) = 0.073 and 3.71 T for II and III phase.	Bi	Bi1	Bi	1																							2017																										A																			many phases	K			3.9		0		3.9	MTC156979																			T	R(on)	0.073												MHC156979																																																														commercial Bi(4N7)					Pressure-induced superconductivity in Bi single crystals			Center for Superconducting Physics and Materials, National Laboratory of Solid State Microstructures and Department of Physics, National Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 95(2017)024510	Yufeng Li,Enyu Wang,Xiyu Zhu,Hai-Hu Wen		
156980	PRB095035148	T<STR>-1 = 283 K, T<STR>-2 = 167 K, At 300K, monoclinic. At 250K, triclinic. (beta) in SP = 0.60 mJ/mol.K4, (dC/gamma*Tc) = 0.83	IrTe2	Ir1Te2	Ir	1	Te	2																				3	2017																										AB2			P3[-]m1	164	A	3.94	3.94	5.406											alpha=beta=90, gamma=120 at 300K. At 250K, SG = P1[-], a=3.954, b=6.649, c=14.458, alpha=98.11,beta=92.53,gamma=107.10	K			2.5				2.5																																																								mJ/mol.K2	1.8	SP	213	SP											uOhm.cm								2.97	2440					cm3/C	-0.000112					MRH156980					self-flux method					Electrical anisotropy and coexistence of structural transitions and superconductivity in IrTe2			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 95(2017)035148	Guixin Cao,Weiwei Xie,W. Adam Phelan,J. F. DiTusa,Rongying Jin		
156981	PRB095054501	T<STR> = 47.0 K, R-expornent, n = 1.76  in R = R0 + A*T^n	Na(Fe,Cu)As	Na1Fe0.996Cu0.004As1	Na	1	Fe	0.996	Cu	0.004	As	1																3	2017								35.1																		ABC		PbFCl																		K		10.14					10.14	MPH156983																																																																																															self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156982	PRB095054501	T<STR> = 27.2 K, R-expornent, n = 1.12  in R = R0 + A*T^n	Na(Fe,Cu)As	Na1Fe0.986Cu0.014As1	Na	1	Fe	0.986	Cu	0.014	As	1																3	2017																										ABC		PbFCl																		K		12.25					12.25																																																																																																self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156983	PRB095054501	R-expornent, n = 1.17  in R = R0 + A*T^n. optimal doping x = 0.02 (Tc=11.8 K)	Na(Fe,Cu)As	Na1Fe0.982Cu0.018As1	Na	1	Fe	0.982	Cu	0.018	As	1																3	2017																										ABC		PbFCl																		K		12.6					12.6	MPH156983																																																																																															self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156984	PRB095054501	R-expornent, n = 1.16  in R = R0 + A*T^n	Na(Fe,Cu)As	Na1Fe0.978Cu0.022As1	Na	1	Fe	0.978	Cu	0.022	As	1																3	2017																										ABC		PbFCl																		K		11.6					11.6																																																																																																self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156985	PRB095054501	R-expornent, n = 1.61  in R = R0 + A*T^n	Na(Fe,Cu)As	Na1Fe0.975Cu0.025As1	Na	1	Fe	0.975	Cu	0.025	As	1																3	2017																										ABC		PbFCl																		K		11.3					11.3																																																																																																self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156986	PRB095054501	R-expornent, n = 1.97  in R = R0 + A*T^n	Na(Fe,Cu)As	Na1Fe0.968Cu0.032As1	Na	1	Fe	0.968	Cu	0.032	As	1																3	2017																										ABC		PbFCl																		K		10.8					10.8																																																																																																self-flux method					Phase diagram and neutron spin resonance of superconducting NaFe1-xCuxAs			Department of Physics, Beijing Normal University, Beijing 100875, China	Phys.Rev.B, 95(2017)054501	Guotai Tan,Yu Song,Rui Zhang,Lifang Lin,Zhuang Xu,Long Tian,Songxue Chi,M. K. Graves-Brook,Shiliang Li,Pengcheng Dai		
156989	PRB095060505	not SC. In-plane uniaxial pressure effect measured by NED, muon-SR. Tn(P) measured. (dTn/dP) = 0.22 K/MPa	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2017								140																		AB2C2																				K					0			MTN156989																																																																																																				Uniaxial pressure effect on the magnetic ordered moment and transition temperatures in BaFe2-xTxAs2 (T = Co,Ni)			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 95(2017)060505	David W. Tam,Yu Song,Haoran Man,Sky C. Cheung,Zhiping Yin,Xingye Lu,Weiyi Wang,Benjamin A. Frandsen,Lian Liu,Zizhou Gong,Takashi U. Ito,Yipeng Cai,Murray N. Wilson,Shengli Guo,Keisuke Koshiishi,Yasutomo J. Uemura,Jeffrey W. Lynn,Graeme M. Luke,Tom Berlijn,Pengcheng Dai		
156990	PRB095060505	In-plane uniaxial pressure effect measured by NED, muon-SR. Tn(P) measured. (dTn/dP) = 0.26 K/MPa	Ba(Fe,Ni)2As2	Ba1Fe1.915Ni0.085As2	Ba	1	Fe	1.915	Ni	0.085	As	2																3	2017								35																		AB2C2																				K		18					18	MTN156990																																																																																																				Uniaxial pressure effect on the magnetic ordered moment and transition temperatures in BaFe2-xTxAs2 (T = Co,Ni)			Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA	Phys.Rev.B, 95(2017)060505	David W. Tam,Yu Song,Haoran Man,Sky C. Cheung,Zhiping Yin,Xingye Lu,Weiyi Wang,Benjamin A. Frandsen,Lian Liu,Zizhou Gong,Takashi U. Ito,Yipeng Cai,Murray N. Wilson,Shengli Guo,Keisuke Koshiishi,Yasutomo J. Uemura,Jeffrey W. Lynn,Graeme M. Luke,Tom Berlijn,Pengcheng Dai		
156991	PRB095064514	P-induced SC. As p increases, amorphous - high density amor - (high density amor + bcc) - bcc, phase change. SC appears for P > 10 GPa. Tc(in DB) = 6K for Amor, P=30 GPa	Amor-GeSb2Te4	Ge1Sb2Te4	Ge	1	Sb	2	Te	4																			2017																										AB2C4																			amorphous. bcc for P>32 GPa.	K					0			MTC156991																			T	R(0.5Rn)				2.8			2						MHC156991																																																																			Superconductivity in multiple phases of compressed GeSb2Te4			Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel	Phys.Rev.B, 95(2017)064514	E. Greenberg,B. Hen,Samar Layek,I. Pozin,R. Friedman,V. Shelukhin,Y. Rosenberg,M. Karpovski,M. P. Pasternak,E. Sterer,Y. Dagan,G. Kh. Rozenberg,A. Palevski		
156992	PRB095064514	P-induced SC. Crystalline sample. Phase transition (hexa , ortho , bcc) with increasing P. See MTC156992. Tc(in DB) = 8.1 K at P=30 GPa, bcc	GwSb2Te4	Ge1Sb2Te4	Ge	1	Sb	2	Te	4																			2017																										AB2C4																			hexagonal to ortho transition  at P=28 GPa	K		8.1			0		8.1	MTC156992																																																																																																				Superconductivity in multiple phases of compressed GeSb2Te4			Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel	Phys.Rev.B, 95(2017)064514	E. Greenberg,B. Hen,Samar Layek,I. Pozin,R. Friedman,V. Shelukhin,Y. Rosenberg,M. Karpovski,M. P. Pasternak,E. Sterer,Y. Dagan,G. Kh. Rozenberg,A. Palevski		
156993	PRB095064515	Eu-valence measured by XAS and XPS. Eu<av> = 2.24. Effective Eu valence decreases with increasing Se-content, lead to mobility, metallicity, and Tc increasing.	Eu0.5La0.5FBi(S,Se)	Eu0.5La0.5F1Bi1S1.8Se0.2	Eu	0.5	La	0.5	F	1	Bi	1	S	1.8	Se	0.2													2017																												CeOBiS2																	BiS2-layer SC	K	0.5		2.7				1.6	MTC156993																																																																						mOhm.cm							6.19																							Evolution of Eu valence and superconductivity in layered Eu0.5La0.5FBiS2-xSex system			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1 Minami-osawa, Hachioji, Tokyo, 192-0397, Japan	Phys.Rev.B, 95(2017)064515	Y. Mizuguchi,E. Paris,T. Wakita,G. Jinno,A. Puri,K. Terashima,B. Joseph,O. Miura,T. Yokoya,N. L. Saini		
156994	PRB095064515	Eu-valence measured by XAS and XPS. Eu<av> = 2.18. Effective Eu valence decreases with increasing Se-content, lead to mobility, metallicity, and Tc increasing.	Eu0.5La0.5FBi(S,Se)	Eu0.5La0.5F1Bi1S1.2Se0.8	Eu	0.5	La	0.5	F	1	Bi	1	S	1.2	Se	0.8													2017																												CeOBiS2																	BiS2-layer SC	K	3.8		6.2				5	MVAL156994																																																																						mOhm.cm							2.17																							Evolution of Eu valence and superconductivity in layered Eu0.5La0.5FBiS2-xSex system			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1 Minami-osawa, Hachioji, Tokyo, 192-0397, Japan	Phys.Rev.B, 95(2017)064515	Y. Mizuguchi,E. Paris,T. Wakita,G. Jinno,A. Puri,K. Terashima,B. Joseph,O. Miura,T. Yokoya,N. L. Saini		
157000	SSC0350091		La0.9Ru3B2	La0.9Ru3B2	La	0.9	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.605		3.006												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157001	SSC0350091		CeRu3B2	Ce1Ru3B2	Ce	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.527		2.991												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157002	SSC0350091		PrRu3B2	Pr1Ru3B2	Pr	1	Ru	3	B	2																		1	1980							6.85																			AB2C3		CeCo3B2	P6/mmm		A	5.554		3.006												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157003	SSC0350091		NdRu3B2	Nd1Ru3B2	Nd	1	Ru	3	B	2																		1	1980							33.2																			AB2C3		CeCo3B2	P6/mmm		A	5.544		3.01												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157004	SSC0350091	Tm > 45 K. magnetic hardness = 100 kOe at 4.2K	SmRu3B2	Sm1Ru3B2	Sm	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.536		2.997												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157005	SSC0350091	Tm > 45 K	GdRu3B2	Gd1Ru3B2	Gd	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.508		3.018												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157006	SSC0350091	Tm > 45 K	TbRu3B2	Tb1Ru3B2	Tb	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.495		3.01												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157007	SSC0350091		DyRu3B2	Dy1Ru3B2	Dy	1	Ru	3	B	2																		1	1980							40.1																			AB2C3		CeCo3B2	P6/mmm		A	5.485		3.011												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157008	SSC0350091		HoRu3B2	Ho1Ru3B2	Ho	1	Ru	3	B	2																		1	1980							16.1																			AB2C3		CeCo3B2	P6/mmm		A	5.474		3.017												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157009	SSC0350091	magnetic hardness = 10 kOe	ErRu3B2	Er1Ru3B2	Er	1	Ru	3	B	2																		1	1980							27.3																			AB2C3		CeCo3B2	P6/mmm		A	5.467		3.017												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157010	SSC0350091		TmRu3B2	Tm1Ru3B2	Tm	1	Ru	3	B	2																		1	1980							18.3																			AB2C3		CeCo3B2	P6/mmm		A	5.461		3.012												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157011	SSC0350091		YbRu3B2	Yb1Ru3B2	Yb	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.464		3.006												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157012	SSC0350091		LuRu3B2	Lu1Ru3B2	Lu	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.454		3.004												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157013	SSC0350091		YRu3B2	Y1Ru3B2	Y	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.481		3.028												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157014	SSC0350091	Tc = 1.79--1.60	ThRu3B2	Th1Ru3B2	Th	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.526		3.07												K		1.79					1.79																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157015	SSC0350091		URu3B2	U1Ru3B2	U	1	Ru	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.476		2.96												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157016	SSC0350091	Tc = 1.53--1.40	Y0.5Th0.5Ru3B2	Y0.5Th0.5Ru3B2	Y	0.5	Th	0.5	Ru	3	B	2																1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.499		3.048												K		1.53					1.53																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157017	SSC0350091	Tc = 2.82--2.60	LaRh3B2	La1Rh3B2	La	1	Rh	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.48		3.137												K		2.82					2.82																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157018	SSC0350091		CeRh3B2	Ce1Rh3B2	Ce	1	Rh	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.474		3.085												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157019	SSC0350091		PrRh3B2	Pr1Rh3B2	Pr	1	Rh	3	B	2																		1	1980							1.68																			AB2C3		CeCo3B2	P6/mmm		A	5.461		3.105												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157020	SSC0350091		NdRh3B2	Nd1Rh3B2	Nd	1	Rh	3	B	2																		1	1980							13.5																			AB2C3		CeCo3B2	P6/mmm		A	5.466		3.109												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157021	SSC0350091	Tm > 45 K	SmRh3B2	Sm1Rh3B2	Sm	1	Rh	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.437		3.09												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157022	SSC0350091		EuRh3B2	Eu1Rh3B2	Eu	1	Rh	3	B	2																		1	1980							41.7																			AB2C3		CeCo3B2	P6/mmm		A	5.601		2.906												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157023	SSC0350091	Tm > 45 K	GdRh3B2	Gd1Rh3B2	Gd	1	Rh	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.404		3.115												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157024	SSC0350091	Tc = 1.88--1.56	Y0.5La0.5Rh3B2	Y0.5La0.5Rh3B2	Y	0.5	La	0.5	Rh	3	B	2																1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.434		3.127												K		1.88					1.88																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157025	SSC0350091	Tc = 4.62--4.45	LuOs3B2	Lu1Os3B2	Lu	1	Os	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.457		3.052												K		4.62					4.62																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157026	SSC0350091		UOs3B2	U1Os3B2	U	1	Os	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.523		2.976												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157027	SSC0350091	Tc = 4.14--3.84	Lu0.5Th0.5Os3B2	U0.5Th0.5Os3B2	U	0.5	Th	0.5	Os	3	B	2																1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.523		3.062												K		4.14					4.14																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157028	SSC0350091	Tc = 1.65--1.39	LaIr3B2	La1Ir3B2	La	1	Ir	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.543		3.116												K		1.65					1.65																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157029	SSC0350091	Tc = 2.09--1.90	ThIr3B2	Th1Ir3B2	Th	1	Ir	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.449		3.23												K		2.09					2.09																																																																																																					Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157030	SSC0350091		UIr3B2	U1Ir3B2	U	1	Ir	3	B	2																		1	1980																										AB2C3		CeCo3B2	P6/mmm		A	5.369		3.181												K					1.2																																																																																																							Superconducting and magnetic properties of new ternary borides with the CeCo3B2-type structure			Institute for Pure and Applied Physical Sciences University of California, San Diego, La Jolla, CA 92093	Solid State Commun., 35(1980)91	H.C.Ku,G.P.Meisner,F.Acker,D.C.Johnston		
157032	SST026055011	RRR = 1.3. Debye model, (beta) = 1.47 mJ/mol.K4, (delta) = 0.0049 mJ/mol.K6. (dC/gamma*Tc) = 1.51. e-ph = 0.6. DOS = 14.85 states/eV.f.u.	Re24Ti5	Re24Ti5	Re	24	Ti	5																				1	2013																										A5B24		alpha-Mn	I$[-]3m	217	A	9.6076														K				5.8			5.8										100										T	SP(mid), WHH	10.75																								k<B>T	10.6	3.68	14				MSP157032	gamma*Tc	1.51	mJ/mol.K2	111.8	SP	428	SP	W/m.K	7.29			MTHC157032	uV/K	10.1			MTP157032	uOhm.cm							214.8				279.2												Re(4N7),Ti(3N5)		arc-melting - ANN (800C, 5days, in quartz tube, vac)					Investigation of normal and superconducting states in noncentrosymmetric Re24Ti5			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Supercond. Sci. Technol., 26(2013)055011	C S Lue,H F Liu,C N Kuo,P S Shih,J-Y Lin,Y K Kuo,M W Chu,T-L Hung,Y Y Chen		
157033	SCIB0620218	not SC. AFM order, Tn= 41 K (Eu<2+> and Tn = 110K (Fe<2+., and STR transition).	EuFeAs2	Eu1Fe1As2	Eu	1	Fe	1	As	2																		1	2017								41																		ABC2		Fe-112	P2<1>/m	11	A	3.98	3.9	10.643											Fe-112, alpfa = 90, beta = 90.035, gamma = 90	K					0																																																																																																EuAs,LaAs,FeAs		solid state reaction. mixture - pellet - in alumina crucuble - in quartz tube - heat to 1123 K - hold(2days) - reground - heat to 1073 K - hold(1 week)					Discovery of a novel 112-type iron-pnictide and La-doping induced superconductivity in Eu1-xLaxFeAs2 (x = 0-0.15)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 62(2017)218	Jia Yu,Tong Liu,Bo-Jin Pan,Bin-Bin Ruan,Xiao-Chuan Wang,Qing-Ge Mu,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
157034	SCIB0620218	impurity phase: Eu2O3, FeAs2. AFM order, Tn= 27 K (Eu<2+>. Coexistence of SC and AFM(Eu<2+>.	(Eu,La)FeAs2	Eu0.85La0.15Fe1As2	Eu	0.85	La	0.15	Fe	1	As	2																1	2017																										ABC2		Fe-112	P2<1>/m	11															Fe-112	K	7.4		11.2				9.3																																																																																														EuAs,LaAs,FeAs		solid state reaction. mixture - pellet - in alumina crucuble - in quartz tube - heat to 1123 K - hold(2days) - reground - heat to 1073 K - hold(1 week)					Discovery of a novel 112-type iron-pnictide and La-doping induced superconductivity in Eu1-xLaxFeAs2 (x = 0-0.15)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 62(2017)218	Jia Yu,Tong Liu,Bo-Jin Pan,Bin-Bin Ruan,Xiao-Chuan Wang,Qing-Ge Mu,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
157035	SCIB0620218	SC 91% at T=1.8 K.	(Eu,La)FeAs2	Eu0.9La0.1Fe1As2	Eu	0.9	La	0.1	Fe	1	As	2																3	2017																										ABC2		Fe-112	P2<1>/m	11	A	3.982	3.8986	10.666											Fe-112, alpfa = 90, beta = 90.240, gamma = 90	K				6			6										91																																																																																						flux method					Discovery of a novel 112-type iron-pnictide and La-doping induced superconductivity in Eu1-xLaxFeAs2 (x = 0-0.15)			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 62(2017)218	Jia Yu,Tong Liu,Bo-Jin Pan,Bin-Bin Ruan,Xiao-Chuan Wang,Qing-Ge Mu,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
157036	SCIB0610921	SC-volume 80% (2K)	LaRu2As2	La1Ru2As2	La	1	Ru	2	As	2																		1	2016																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.182		10.59												K	6.8		7.8	7		1	7										80										T	RES(0.5Rn), Linear extrapolation	1.6												MHC157036																																																												La,Ru(powfer),As(powder)		solid state reaction. mixture - pellet - in quartz tube - SIN (between 900 and 1100C, 100h, repeat 3 times)					Superconductivity at 7.8 K in the ternary LaRu2As2 compound			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 61(2016)921	Qi Guo,Bo-Jin Pan,Jia Yu,Bin-Bin Ruan,Dong-Yun Chen,Xiao-Chuan Wang,Qing-Ge Mu,Gen-Fu Chen,Zhi-An Ren		
157037	SCIR0059158	RRR = 1.8. SP (beta) = 0.8 mJ/mol.K4, (delta) = 0.02 mJ/mol.K6. carrier n=1.2E+19 /cm3 for T<50K from RH. Large magnetoresistance , not saturates upto 9T	LuPdBi	Lu1Pd1Bi1	Lu	1	Pd	1	Bi	1																		3	2015																										ABC																				K	1.8		1.9				1.85																				T	RES(0.9Rn),(1-t^2)^1.496	2.3												MHC157037		nm	from Hc2	17			nm	from Hc1	3629													mJ/mol.K2	0.75	SP	194	SP											mOhm.cm	0.21										0.387										n/cm3	28000000000000000000								Shubnikov - de Haas oscillations, weak antilocalization effect and large linear magnetoresistance in the putative topological superconductor LuPdBi			Institute for Low Temperatures and Structure Research, Polish Academy of Sciences, P. O. Box 1410, 50-950 Wroc aw, Poland	Sci.Report, 5(2015)9158	Orest Pavlosiuk,Dariusz Kaczorowski,Piotr Wisniewski		
157038	SCIR00628632	In-plane anisotropy (Hc2//a)/(Hc2//a*) measured for I//a. Hc2 defined as R(mid). ANI(aa*) = Hc2(a)/Hc2(a*) = 6.8 at 1.9 K.	SrxBi2Se3	Sr0.1Bi2Se3	Sr	0.1	Bi	2	Se	3																		3	2016																										AB2C3			R3[-]m																	K		2.84					2.84																				T	RES(0.5Rn)					2.86	0.397	1.9						MHC157038																																																																			Rotational symmetry breaking in the topological superconductor SrxBi2Se3 probed by upper-critical field experiments			Van der Waals - Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands.	Sci.Report, 6(2016)28632	Y. Pan,A. M. Nikitin,G. K. Araizi,Y. K. Huang,Y. Matsushita,T. Naka,A. de Visser		
157039	SCIR00628632	In-plane anisotropy (Hc2//a)/(Hc2//a*) measured for I//a. Hc2 defined as R(mid). ANI(aa*) = Hc2(a)/Hc2(a*) = 2.6 at 0.3 K. [cohere] = 19.6,7.6, 5.4 nm for a, a*, c axis, respectively at t=0.1	SrxBi2Se3	Sr0.15Bi2Se3	Sr	0.15	Bi	2	Se	3																		3	2016																										AB2C3			R3[-]m																	K		3.05					3.05																				T	RES(0.5Rn)					7.71	2.41	0.3						MHC157039		nm	from Hc2		19.6	5.4																																																													Rotational symmetry breaking in the topological superconductor SrxBi2Se3 probed by upper-critical field experiments			Van der Waals - Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands.	Sci.Report, 6(2016)28632	Y. Pan,A. M. Nikitin,G. K. Araizi,Y. K. Huang,Y. Matsushita,T. Naka,A. de Visser		
157040	PRL108057001	Tc goto zero at P<cr> = 6.3 GPa.. Anisotropy (Hc2) = 2.9.  For P=2.31 GPa, anisotropy (cohere) = (15 nm/7 nm ) = 2.1	CuxBi2Se3	Cu0.3Bi2.1Se3	Cu	0.3	Bi	2.1	Se	3																		3	2012																										AB2C3			R3[-]m																	K		3.38				0.25	3.38	MTC157040																			T	RES(0.5Rn)		5.6	1.9					T/K	RES(0.5Rn)		2	0.6	MHC157040		nm	from Hc2		13	4																															mOhm.cm	0.15						0.15														n/cm3	120000000000000000000			melt in sealed quartz tube (850C) - slow cool to (500-600C) and ANN (60-100h)					Superconductivity in the Doped Topological Insulator CuxBi2Se3 under High Pressure			Van der Waals?Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Phys.Rev.Lett.,108(2012)057001	T.V. Bay,T. Naka,Y. K. Huang,H. Luigjes,M. S. Golden,A. de Visser		
157100	ACS13710512	topological SC. Sr-intercalation. Sr-content by EDX. Carrier n(10K) = 2.65E19 /cm3	SrxBi2Se3	Sr0.062Bi2Se3	Sr	0.062	Bi	2	Se	3																		3	2015																															A	4.1369		28.598												K	2.39		2.57				2.48										88																																																													mOhm.cm								0.24						cm3/C	0.31					MRH157100	n/cm3	20200000000000000000			SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with Topological Surface State in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, PR China	J.Am.Chem.Soc., 137(2015)10512	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
157101	ACS13710512	topological SC. Sr-intercalation. Sr-content by EDX.	SrxBi2Se3	Sr0.058Bi2Se3	Sr	0.058	Bi	2	Se	3																		3	2015																																														K	1.98		2.14				2.06										34																																																																																						SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with Topological Surface State in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, PR China	J.Am.Chem.Soc., 137(2015)10512	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
157102	ACS13710512	topological SC. Sr-intercalation. Sr-content by EDX. Nominal x = 0.19.	SrxBi2Se3	Sr0.065Bi2Se3	Sr	0.065	Bi	2	Se	3																		3	2015																																														K	2.35		2.59				2.47										91																																																																																						SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with Topological Surface State in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, PR China	J.Am.Chem.Soc., 137(2015)10512	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
157103	ACS13710512	Sr-doped Bi2Se3. not SC for x =< 025 in Bi2-xSrxSe3	Bi2-xSrxSe3	Sr0.15Bi1.85Se3	Sr	0.15	Bi	1.85	Se	3																			2015																										A2B3					A	4.146		28.559												K					1.9																																																																																																		SrxBi2Se3(nominal Sr-content x =<0.3) were grown. Cleaved crystals were used.					Superconductivity with Topological Surface State in SrxBi2Se3			High Magnetic Field Laboratory, Chinese Academy of Sciences and University of Science and Technology of China, Hefei 230026, PR China	J.Am.Chem.Soc., 137(2015)10512	Zhongheng Liu,Xiong Yao,Jifeng Shao,Ming Zuo,Li Pi,Shun Tan,Changjin Zhang,Yuheng Zhang		
157104	ACS1387856	Impurity phases: KFe2As2(3.0%),FeAs(2%),CaF2(1.8%). Tc(SP) = 32 K. (dC/Tc) = 150 mJ/mol.K2. gamma = 105 mJ/mol.K2 assuming BCS (dC/gamma*Tc) = 1.43	KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2															2016																													I4/mmm	139	A	3.8684		31.007											12442-structure	K	32.3	32.8	33.1	33			32.8										100										T	RES(0.9Rn)								T/K	SP	16			MHC157104																						mJ/mol.K2	104	SP																																				KAs,CaF2,CaAs,Fe2As		mixture - pellet - in alumina tube - sealed in Ta tube in quartz tube - SIN(930C, 36h) , reground and repeat reaction process					Superconductivity in KCa2Fe4As4F2 with Separate Double Fe2As2 Layers			Department of Physics and State Key Lab of Silicon Materials, Zhejiang University, Hangzhou 310027, China	J.Am.Chem.Soc., 138(2016)7856	Zhi-Cheng Wang,Chao-Yang He,Si-Qi Wu,Zhang-Tu Tang,Yi Liu,Abduweli Ablimit,Chun-Mu Feng,Guang-Han Cao		
157105	CEM2520106		SnAs	As1Sn1	As	1	Sn	1																					2017																										AB		NaCl			A	5.722														K				3.8			3.8											Oe	M-H curve				70			2																																																																											Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157106	CEM2520106		SnAs1-xSex	Sn1As0.99Se0.01	Sn	1	As	0.99	Se	0.01																			2017																										AB		NaCl			A	5.725														K			39	3.8			3.8											Oe	M-H curve				80			2	Oe	RES(0.9Rn),WHH	294							Oe/K	RES(0.9Rn)	109																																								uOhm.cm							3.03																Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157107	CEM2520106		SnAs1-xSex	Sn1As0.97Se0.03	Sn	1	As	0.97	Se	0.03																			2017																										AB		NaCl			A	5.727														K				4			4											Oe	M-H curve				110			2																																																																											Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157108	CEM2520106		SnAs1-xSex	Sn1As0.95Se0.05	Sn	1	As	0.95	Se	0.05																			2017																										AB		NaCl			A	5.729														K			4.3	4.3			4.3											Oe	M-H curve				70			2	Oe	RES(0.9Rn),WHH	649							Oe/K	RES(0.9Rn)	217																																								uOhm.cm							3.53																Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157109	CEM2520106		SnAs1-xSex	Sn1As0.93Se0.07	Sn	1	As	0.93	Se	0.07																			2017																										AB		NaCl			A	5.732														K				4.3			4.3											Oe	M-H curve				90			2																																																																											Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157110	CEM2520106		SnAs1-xSex	Sn1As0.9Se0.1	Sn	1	As	0.9	Se	0.1																			2017																										AB		NaCl			A	5.734														K			4.3	4.5			4.5											Oe	M-H curve				80			2	Oe	RES(0.9Rn),WHH	1011							Oe/K	RES(0.9Rn)	328																																								uOhm.cm							19.55																Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157111	CEM2520106		SnAs1-xSex	Sn1As0.87Se0.13	Sn	1	As	0.87	Se	0.13																			2017																										AB		NaCl			A	5.729														K				4.4			4.4											Oe	M-H curve				115			2																																																																											Sn,As,Se		mixture - ground - sealed in silica tube - heat to 973K in 10h - keap(973K,10h) - furnace cool to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157112	CHM0280779	Tl content by ICP. Tl not intercalated. Carrier = 1.8E+20 /cm3, mobility = 175 cm3/V.s at 2.5 K. SP (beta) = 4.4 mJ/mol.K4. Hc2 using SP data.	Tl0.6Bi2Te3	Tl0.6Bi2Te3	Tl	0.6	Bi	2	Te	3																		3	2016																													R3[-]m		A	4.385		30.438											gamma = 120 degree	K	2.15		2.42	2.35			2.35										83										T	SP(mid), WHH			1.06										MHC157112		nm	from Hc2	17.6																		mJ/mol.K2	4.8	SP													mOhm.cm								0.2															Tl(4N),Bi(6N),Te(6N)		mixture - sealed in quartz tube - heat to 1123 K - keep (48h) - cool to 823 K(5K/h) - Q to ice water					Superconductivity in Tl0.6Bi2Te3 Derived from a Topological Insulator			Institute of Physics II, University of Cologne, D-50937 Cologne, Germany	Chem.Mater. 28(2016)779	Zhiwei Wang,A. A. Taskin,Tobias Frolich,Markus Braden,Yoichi Ando		
157113	CHM0281927	not SC. T<CDW> = 221 K.	TiSe2	Se2Ti1	Se	2	Ti	1																				3	2016																													P3[-]m	164	A	3.5387		6.0118												K					0.4																																																																																																Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157114	CHM0281927	T<CDW> = 201 K.	Ti1-xTaxSe2	Ti0.95Ta0.05Se2	Ti	0.95	Ta	0.05	Se	2																		3	2016																													P3[-]m	164	A	3.537		6.019												K		1.75					1.75																																																																																														Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157115	CHM0281927	T<CDW> = 189 K.	Ti1-xTaxSe2	Ti0.9Ta0.1Se2	Ti	0.9	Ta	0.1	Se	2																		3	2016																													P3[-]m	164	A	3.5335		6.0297												K		2.23					2.23																																																																																														Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157116	CHM0281927	T<CDW> = 199 K. SP (beta) = 0.70 mJ/mol.K4  (dC/gamm*Tc) = 1.9. DOS = 0.53 states/eV from gmma.	Ti1-xTaxSe2	Ti0.8Ta0.2Se2	Ti	0.8	Ta	0.2	Se	2																		3	2016																													P3[-]m	164	A	3.518		6.0093												K		2.28					2.28	MTC157116																			T	R(0.5Rn), WHH	2.33							T/K	RES(0.5Rn)	1.4			MHC157116		A	from Hc2	120																		mJ/mol.K2	1.99	SP	202	SP																																		Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157117	CHM0281927	T<CDW> = 200 K.	Ti1-xTaxSe2	Ti0.85Ta0.15Se2	Ti	0.85	Ta	0.15	Se	2																		3	2016																													P3[-]m	164	A	3.529		6.0405												K		2.3					2.3																				T	R(0.5Rn), WHH	2.21							T/K	RES(0.5Rn)	1.4			MHC157117																																																												Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157118	CHM0281927	not SC for x < 0.4 in Ti1-xNbxSe2. SP (beta) = 0.48 mJ/mol.K4	Ti1-xNbxSe3	Ti0.8Nb0.2Se2	Ti	0.8	Nb	0.2	Se	2																			2016																													P3[-]m	164	A	3.5217		6.0443												K					0.4																																																										mJ/mol.K2	0.45	SP	230	SP																																		Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157119	CHM0281927		CuxTiSe2	Cu0.05Ti1Se2	Cu	0.05	Ti	1	Se	2																			2016																															A	3.5423		6.0246												K		1.52					1.52																																																																																														Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157120	CHM0281927		CuxTiSe2	Cu0.08Ti1Se2	Cu	0.08	Ti	1	Se	2																			2016																															A	3.544		6.0359												K		4.18					4.18	MTC157120																																																																																													Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157121	CHM0281927		PdxTiSe2	Pd0.12Ti1Se2	Pd	0.12	Ti	1	Se	2																			2016																																														K		2.18					2.18																																																																																														Ta(2N8) or Nb(2N8),Ti(3N),Se(5N)		mixture - pellet - heat to 700C (1C/min) - hold(120h) - repeat reactions. Single crystals grown by CTV (675K(L)-725K(H))					Differences in Chemical Doping Matter: Superconductivity in Ti1-xTaxSe2 but Not in Ti1-xNbxSe2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States	Chem.Mater., 28(2016)1927	Huixia Luo,Weiwei Xie,Jing Tao,Ivo Pletikosic,Tonica Valla,Girija S. Sahasrabudhe,Gavin Osterhoudt,Erin Sutton,Kenneth S. Burch,Elizabeth M. Seibel,Jason W. Krizan,Yimei Zhu,Robert J. Cava		
157122	EPJ0850414	TP300 in DB shows the value at 320 K.	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2012																										A3B4C4			I4/mmm		A	3.9687		41.324												K			4.6	4.41			4.41																																																																		uV/K	-33.1			MTP157122																								Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157123	EPJ0850414		Bi4-xAgxO4S3	Bi3.99Ag0.01S3O4	Bi	3.99	Ag	0.01	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9654		41.2982												K			4.39	4.31			4.31																																																																																														Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157124	EPJ0850414		Bi4-xAgxO4S3	Bi3.97Ag0.03S3O4	Bi	3.97	Ag	0.03	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9637		41.2376												K			4.24	4.2			4.2																																																																																														Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157125	EPJ0850414	TP300 in DB shows the value at 320 K.	Bi4-xAgxO4S3	Bi3.95Ag0.05S3O4	Bi	3.95	Ag	0.05	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.964		41.2211												K			3.52				3.52	MTC157125																																																																	uV/K	-33.8																											Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157126	EPJ0850414		Bi4-xAgxO4S3	Bi3.93Ag0.07S3O4	Bi	3.93	Ag	0.07	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9635		41.2132												K			3.01	2.1			2.1																																																																																														Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157127	EPJ0850414	TP300 in DB shows the value at 320 K.	Bi4-xAgxO4S3	Bi3.9Ag0.1S3O4	Bi	3.9	Ag	0.1	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9622		41.1662												K			1.99				1.99																																																																		uV/K	-40.4			MTP157127																								Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157128	EPJ0850414	TP300 in DB shows the value at 320 K.	Bi4-xAgxO4S3	Bi3.85Ag0.15S3O4	Bi	3.85	Ag	0.15	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9617		41.1648												K					2																																																																				uV/K	-43.4																											Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157129	EPJ0850414	TP300 in DB shows the value at 320 K.	Bi4-xAgxO4S3	Bi3.8Ag0.2S3O4	Bi	3.8	Ag	0.2	S	3															O	4		1	2012																										A3B4C4			I4/mmm		A	3.9616		41.0652												K					2																																																																				uV/K	-45.2			MTP157129																								Ag(4N),Bi(3N),S(3N),Ni2O3(>4N)		mixture - pellet - sealed in quartz tube - heat(450C, 10h) - heat(510C,10h) - repeat again					Suppression of superconductivity in layered Bi4O4S3 by Ag doping			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, P.R. China	Eur.Phys.J.B, 85(2012)414	S.G. Tan,P. Tong,Y. Liu,W.J. Lu,L.J. Li,B.C. Zhao,Y.P. Sun		
157130	JAC2910066	Only structural data. SC not measured.	SrFe4Sb12	Sr1Fe4Sb12	Sr	1	Fe	4	Sb	12																		1	1999																										AB4C12		skutterudite	Im3[-]		A	9.1812													a = 9.176 for Sr0.935Fe4Sb12																																																																																																								mixture - pellet - alumina crucible - sealed in silica crucible - heat to 900C (60C/h) - ANN(900C, between 1day and 1week) - Q to water					The antimony-rich parts of the ternary systems calcium, strontium, barium and cerium with iron and antimony; structure refinements of theLaFe4Sb12-type compounds SrFe4Sb12 and CeFe4Sb12 ; the new compounds CaOs4Sb12 and YbOs4Sb			Anorganisch-Chemisches Institut, Universitat Munster, Wilhelm-Klemm-Strasse 8, D-48149 Munster, Germany	J.Alloys Compd, 252(1999)66	Joachim W. Kaiser,Wolfgang Jeitschko		
157131	JAC2910066	Only structural data. SC not measured.	CeFe4Sb12	Ce1Fe4Sb12	Ce	1	Fe	4	Sb	12																		1	1999																										AB4C12		skutterudite	Im3[-]		A	9.136													a = 9.126 for Ce0.892Fe4Sb12																																																																																																								mixture - pellet - alumina crucible - sealed in silica crucible - heat to 900C (60C/h) - ANN(900C, between 1day and 1week) - Q to water					The antimony-rich parts of the ternary systems calcium, strontium, barium and cerium with iron and antimony; structure refinements of theLaFe4Sb12-type compounds SrFe4Sb12 and CeFe4Sb12 ; the new compounds CaOs4Sb12 and YbOs4Sb			Anorganisch-Chemisches Institut, Universitat Munster, Wilhelm-Klemm-Strasse 8, D-48149 Munster, Germany	J.Alloys Compd, 252(1999)66	Joachim W. Kaiser,Wolfgang Jeitschko		
157132	JAC2910066	Only structural data. SC not measured.	CaOs4Sb12	Ca1Os4Sb12	Ca	1	Os	4	Sb	12																		1	1999																										AB4C12		skutterudite			A	9.321																																																																																																																					mixture - pellet - alumina crucible - sealed in silica crucible - heat to 900C (60C/h) - ANN(900C, between 1day and 1week) - Q to water					The antimony-rich parts of the ternary systems calcium, strontium, barium and cerium with iron and antimony; structure refinements of theLaFe4Sb12-type compounds SrFe4Sb12 and CeFe4Sb12 ; the new compounds CaOs4Sb12 and YbOs4Sb			Anorganisch-Chemisches Institut, Universitat Munster, Wilhelm-Klemm-Strasse 8, D-48149 Munster, Germany	J.Alloys Compd, 252(1999)66	Joachim W. Kaiser,Wolfgang Jeitschko		
157133	JAC2910066	Only structural data. SC not measured.	YbOs4Sb12	Yb1Os4Sb12	Yb	1	Os	4	Sb	12																		1	1999																										AB4C12		skutterudite			A	9.316																																																																																																																					mixture - pellet - alumina crucible - sealed in silica crucible - heat to 900C (60C/h) - ANN(900C, between 1day and 1week) - Q to water					The antimony-rich parts of the ternary systems calcium, strontium, barium and cerium with iron and antimony; structure refinements of theLaFe4Sb12-type compounds SrFe4Sb12 and CeFe4Sb12 ; the new compounds CaOs4Sb12 and YbOs4Sb			Anorganisch-Chemisches Institut, Universitat Munster, Wilhelm-Klemm-Strasse 8, D-48149 Munster, Germany	J.Alloys Compd, 252(1999)66	Joachim W. Kaiser,Wolfgang Jeitschko		
157134	JAC6940439	(dC/gamma*Tc) = 0.59 ,  (2d/kTc) = 2.0 .	SrRhGe3	Sr1Rh1Ge3	Sr	1	Rh	1	Ge	3																		3	2017																										ABC3		BaNiSn3			A	4.4399		10.1321												K		0.71					0.71																																																								mJ/mol.K2	5.1	SP	200	SP																																		Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157135	JAC6940439	RRR = 150.  (dC/gamma*Tc) = 1.9 ,  (2d/kTc) = 5.6 .	SrIrGe3	Sr1Ir1Ge3	Sr	1	Ir	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K		0.53					0.53																																																								mJ/mol.K2	5.3	SP	230	SP											uOhm.cm							0.3																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157136	JAC6940439	(dC/gamma*Tc) = 0.93 ,  (2d/kTc) = 3.5 .	SrNiGe3	Sr1Ni1Ge3	Sr	1	Ni	1	Ge	3																		3	2017																										ABC3		BaNiSn3			A	4.3785		10.0231												K		0.46					0.46																																																								mJ/mol.K2	5.6	SP	280	SP																																		Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157137	JAC6940439	(dC/gamma*Tc) = 1.2 ,  (2d/kTc) = 3.1 .	SrPdGe3	Sr1Pd1Ge3	Sr	1	Pd	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K	1.47	1.38					1.38																																																								mJ/mol.K2	5.3	SP	250	SP																																		Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157138	JAC6940439	(dC/gamma*Tc) = 1.1 ,  (2d/kTc) = 2.8 .	SrPtGe3	Sr1Pt1Ge3	Sr	1	Pt	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K		0.84					0.84																																																								mJ/mol.K2	4.7	SP	260	SP																																		Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157139	JAC6940439	2nd Tn = 13.4 K. magnetic properties: DB values for H//[100]. For H//[001, moment = 7.33 my-B/Eu, Curie-T = -14.8 K.	EuCoGe3	Eu1Co1Ge3	Eu	1	Co	1	Ge	3																		3	2017					My-B/Eu	7.7	-20.7	15.4																		ABC3		BaNiSn3				4.3191		9.8847												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157140	JAC6940439	magnetic properties: DB values for H//[100]. For H//[001, moment = 7.94 my-B/Eu, Curie-T = -19.8 K.	EuRhGe3	Eu1Rh1Ge3	Eu	1	Rh	1	Ge	3																		3	2017					My-B/Eu	7.8	-16	11.6																		ABC3		BaNiSn3				4.4129		10.0906												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157141	JAC6940439	2nd Tn = 7.0 K. magnetic properties: DB values for H//[100]. For H//[001, moment = 7.85 my-B/Eu, Curie-T = -20.2 K.	EuIrGe3	Eu1Ir1Ge3	Eu	1	Ir	1	Ge	3																		3	2017					My-B/Eu	7.92	-19.6	12.2																		ABC3		BaNiSn3				4.4358		10.0581												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157142	JAC6940439	magnetic properties: DB values for H//[100]. For H//[001, moment = 7.97 my-B/Eu, Curie-T = -5.8 K.	EuNiGe3	Eu1Ni1Ge3	Eu	1	Ni	1	Ge	3																		3	2017					My-B/Eu	7.88	-2.81	13.3																		ABC3		BaNiSn3				4.349		9.9087												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157143	JAC6940439	magnetic properties: DB values for H//[100]. For H//[001, moment = 7.91 my-B/Eu, Curie-T = -2.8 K.	EuPdGe3	Eu1Pd1Ge3	Eu	1	Pd	1	Ge	3																		3	2017					My-B/Eu	7.78	-3	12.2																		ABC3		BaNiSn3				4.4606		10.2324												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157144	JAC6940439	magnetic properties: DB values for H//[100]. For H//[001, moment = 7.95 my-B/Eu, Curie-T = -6.4 K.	EuPtGe3	Eu1Pt1Ge3	Eu	1	Pt	1	Ge	3																		3	2017					My-B/Eu	7.96	-6	10.8																		ABC3		BaNiSn3				4.4758		10.0887												K					0.5																																																																																																Sr(3N),T(4N),Ge(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - in alumina crucible - in quartz tube - heat(1130C, 3d) - cool to 500C within 15 days. Flux removed at 250C.					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157145	JAC7210261	small SC volume fraction, Anomaly in R(T) are 69 K, 02 K(maybe SC)	(Ca,Ce)FeAs2	Ca0.82Ce0.18Fe1As2	Ca	0.82	Ce	0.18	Fe	1	As	2																3	2017																										ABC2		Fe-112																		K	6.2		20				13.1																																																																							mOhm.cm												0.418		cm3/C	-0.0000000226					MRH157145			Ca,Ce,FeAs,CoAs,As		self-flux method. Mixture - sealed in aluminum crucible - sealed in quartz tube - heat to 1000C - hold(15h) - cool to 1050C (1.25C/h) - furnace cool					Synthesis and transport properties of 112-type iron pnictide superconductors Ca1-xCexFe1-yCoyAs2			School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Alloys Compd, 721(2017)261	Xiangzhuo Xing,Zhanfeng Li,Chunqiang Xu,Wei Zhou,Xiaofeng Xu,Bin Chen,Haijun Zhao,Mingxiang Xu,Zhixiang Shi		
157146	JAC7210261	Anomaly in R(T) are 72 K, 22 K(maybe SC). R not to zero at T=2.8 K.	(Ca,Ce)FeAs2	Ca0.76Ce0.24Fe1As2	Ca	0.76	Ce	0.24	Fe	1	As	2																3	2017																										ABC2		Fe-112																		K			22				22																																																																							mOhm.cm												0.434		cm3/C	-0.00000000955					MRH157145			Ca,Ce,FeAs,CoAs,As		self-flux method. Mixture - sealed in aluminum crucible - sealed in quartz tube - heat to 1000C - hold(15h) - cool to 1050C (1.25C/h) - furnace cool					Synthesis and transport properties of 112-type iron pnictide superconductors Ca1-xCexFe1-yCoyAs2			School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Alloys Compd, 721(2017)261	Xiangzhuo Xing,Zhanfeng Li,Chunqiang Xu,Wei Zhou,Xiaofeng Xu,Bin Chen,Haijun Zhao,Mingxiang Xu,Zhixiang Shi		
157147	JAC7210261	Anomali in R(T) appears at 81 K. not SC	(Ca,Ce)FeAs2	Ca0.73Ce0.27Fe1As2	Ca	0.73	Ce	0.27	Fe	1	As	2																3	2017																										ABC2		Fe-112																		K					2.8																																																																									mOhm.cm												0.437		cm3/C	-0.00000000135					MRH157145			Ca,Ce,FeAs,CoAs,As		self-flux method. Mixture - sealed in aluminum crucible - sealed in quartz tube - heat to 1000C - hold(15h) - cool to 1050C (1.25C/h) - furnace cool					Synthesis and transport properties of 112-type iron pnictide superconductors Ca1-xCexFe1-yCoyAs2			School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Alloys Compd, 721(2017)261	Xiangzhuo Xing,Zhanfeng Li,Chunqiang Xu,Wei Zhou,Xiaofeng Xu,Bin Chen,Haijun Zhao,Mingxiang Xu,Zhixiang Shi		
157148	JAC7210261	stable Fe-112 phase.	(Ca,Ce)(Fe,Co)As2	Ca0.8Ce0.2Fe0.975Co0.025As2	Ca	0.8	Ce	0.2	Fe	0.975	Co	0.025	As	2														3	2017																										ABC2		Fe-112																		K	33	34.5	38	33			34.5										80										T	RES(0.5Rn), WHH		151	48.77					T/K	RES(0.5Rn)		6.32	2.04	MHC157148																																					mOhm.cm												0.472		cm3/C	-0.0000000192					MRH157148			Ca,Ce,FeAs,CoAs,As		self-flux method. Mixture - sealed in aluminum crucible - sealed in quartz tube - heat to 1000C - hold(15h) - cool to 1050C (1.25C/h) - furnace cool					Synthesis and transport properties of 112-type iron pnictide superconductors Ca1-xCexFe1-yCoyAs2			School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	J.Alloys Compd, 721(2017)261	Xiangzhuo Xing,Zhanfeng Li,Chunqiang Xu,Wei Zhou,Xiaofeng Xu,Bin Chen,Haijun Zhao,Mingxiang Xu,Zhixiang Shi		
157149	JAP117213912	RRR = 1.1. Ba8Si38.83Al3.47 by EPMA.  Hc2 defined as R=0.5Rn (H-sweep) and R=zero (T-sweep), SC properties calculated using T-sweep Hc2.	Ba8Si42Al4	Ba8Si42Al4	Ba	8	Si	42	Al	4																		1	2015																										A8B46		clathrate			A	10.39														K				5.7			5.7										30	Oe	M-H curve, (1-t^2)	40.2							T	R=zero, T-sweep, GL	6.64												MHC157149		A	from Hc2	70			A	Hc1, GL	4360																																																					Ba8Si46-xAlx prepared based on the multistep melting of Ba, Al, and Si under Ar atmosphere and subsequent solid state reaction					Critical magnetic fields of superconducting aluminum-substituted Ba8Si42Al4 clathrate			School of Engineering, University of Puerto Rico at Mayaguez, Mayaguez, Puerto Rico 00681-9000, USA	J.Appl.Phys., 117(2015)213912	Yang L,Jose Garcia,Giovanni Franco,Junqiang Lu,Kejie Lu,Bo Rong,Basir Shafiq,Ning Chen,Yang Liu,Lihua Liu,Bensheng Song,Yuping Wei,Zhiping Luo,Zhaosheng Feng		
157150	JPCM027385701	Impurity phases: Bi2S3,CeS. Tn (in phase diagram) obtained from hump in R(T,H) at H constant.	(Eu,Ce)BiS2F	Eu0.5Ce0.5Bi1S2F1	Eu	0.5	Ce	0.5	Bi	1	S	2	F	1														1	2015																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0697		13.3286											BiS2 layer SC	K		2.2					2.2																				T	RES(on), WHH	0.75																																		mJ/mol.K2	127	SP	212	SP																																		EuF2(3N),Bi2S3(4N5),S(5N5),Ce(2N8)		solid state reaction. Mixture - alumina tube in quartz ampoule - heat(1000K, 10h) - ground - pellet - SIN(1000K, 10h)					Coexistence of superconductivity and complex 4 f magnetism in Eu0.5Ce0.5BiS2F			Department of Physics, Zhejiang University, Hangzhou 310027, People's Republic of China	J.Phys.Condens.Matter, 27(2015)385701	Hui-Fei Zhai,Pan Zhang,Zhang-Tu Tang,Jin-Ke Bao,Hao Jiang,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
157151	JPS081113703	RRR = 41 for J//b-axis. Hc2 = 2 kOe for bulk (SP).  Hc2 measured also for H//a-,b-,c-axis for J//b-axis defined as R=0. SP (beta) = 0.15 mJ/mol.K4. (2gap/k) = 7.8 K from SP.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		3	2012																										ABC2		CeNiC2	Amm2		A	3.959	4.564	6.204												K	2.7						2.7																				T	SP	0.2												MHC157151														2.9	14				MSP157151			mJ/mol.K2	6.7	SP													uOhm.cm								2.9				120											La(3N),Ni(4N),C(4N)		single crystals grown by Czochralsky method in tetra-arc furnace using (La:Ni:C = 1:1:2004-2.08)					Fermi Surface and Superconducting Properties of Non-centrosymmetric LaNiC2			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 81(2012)113703	Yusuke HIROSE,Toshihiko KISHINO,Jyunya SAKAGUCHI,Yasunao MIURA,Fuminori HONDA,Tetsuya TAKEUCHI,Etsuji YAMAMOTO,Yoshinori HAGA,Hisatomo HARIMA,Rikio SETTAI,Yoshichika ONUKI		
157152	JPS086014704	RRR = 18. Curie-Weiss for T > 150K. Gamma(SP) = 145 mJ/mol-Ce.K2 from fitting for T < 1.0 K. lambda-type anomaly at around 1.0 K  in C(T)	Ce2Pt8P	Ce2Pt8P1	Ce	2	Pt	8	P	1																		1	2017					My-B/Ce	2.3	12																			AB2C8			Amm2	38	A	4.242	17.38	5.39											CePt5 intergrowth in CePt3P	K																																																															mJ/mol.K2	145	SP																																				Ce(3N),La(3N),Pt(3N),P(5N)		solid state reaction. CePt2(or LaPt2) - arcmelting - crush & ground to powder - mixture(CePt2 + P) - sealed in quartz tube - heat(1100C, 48h) - slow cool to RT					Heavy-Fermion Compound of the Ternary Phosphide Ce2Pt8P with a Non-Centrosymmetric Structure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 86(2017)014704	Naoki Kase,Shoh Furukawa,Tomohito Nakano,Naoya Takeda		
157153	JPS086014704	RRR = 56. gamma(SP) = 26.8 mJ/mol-La.K2. beta(SP) = 18.4 mJ/mol-La.K2	La2Pt8P	La2Pt8P1	La	2	Pt	8	P	1																		1	2017								9.6																		AB2C8			Amm2	38	A	4.248	17.382	5.394											LaPt5 intergrowth in CePt3P	K					0.28																																																										mJ/mol.K2	26.8	SP	200	SP																																		Ce(3N),La(3N),Pt(3N),P(5N)		solid state reaction. CePt2(or LaPt2) - arcmelting - crush & ground to powder - mixture(CePt2 + P) - sealed in quartz tube - heat(1100C, 48h) - slow cool to RT					Heavy-Fermion Compound of the Ternary Phosphide Ce2Pt8P with a Non-Centrosymmetric Structure			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	J.Phys.Soc.Jpn, 86(2017)014704	Naoki Kase,Shoh Furukawa,Tomohito Nakano,Naoya Takeda		
157154	JPS086023704	SP measured for unannealed sample. SP anomaly appears at around 36 K due to Einstein-phonon with T(Ein) = 177 K.	La3Be13	Be13La1	Be	13	La	1																				3	2017																										AB13		MnZn13	Fm3[-]c	226	A	10.506														K	0.53						0.53																																																								mJ/mol.K2	9.1	SP	950	SP																																		La(3N),Be(3N)		Al-flux method. Mixture(La:Be:Al(4N) = 1:13:35) - in Al2O3 crucible - sealed in quartz tube - heat(1050C, 72h) - cool (2C/h) -flux remove - ANN(700C, 2weeks)					Observation of Low-Energy Einstein Phonon and Superconductivity in Single-Crystalline LaBe13			Graduate School of Science, Hokkaido University, Sapporo 060-0810, Japan	J.Phys.Soc.Jpn, 86(2017)023704	Hiroyuki Hidaka,Yusei Shimizu,Seigo Yamazaki,Naoyuki Miura,Ryoma Nagata,Chihiro Tabata,Shota Mombetsu,Tatsuya Yanagisawa,Hiroshi Amitsuka		
157155	JPS086034707	T<STR> = 151 K. SP(lattice) has Debye and two Einstein temperature, Debye= 258 K for T < 3 K. Ein(1) = 34, Ein(2) = 76 K.	LaOs2Zn20	La1Os2Zn20	La	1	Os	2	Zn	20																		1	2017																										AB2C20		CeCr2Al20	Fd3[-]m		A	14.4223														K	0.07						0.07																				T	RES(R=zero)								T/K	RES(R=zero)	0.057			MHC157155																						mJ/mol.K2	10.4	SP	258	SP																																				Zn-flux method					Structural, Magnetic, and Superconducting Properties of Caged Compounds ROs2Zn20 (R = La, Ce, Pr, and Nd)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 86(2017)034707	Kazuhei Wakiya,Takahiro Onimaru,Keisuke T. Matsumoto,Yu Yamane,Naohiro Nagasawa,Kazunori Umeo,Shunichiro Kittaka,Toshiro Sakakibara,Yoshitaka Matsushita,Toshiro Takabatake		
157156	JPS086034707	T<STR> = 109 K.	CeOs2Zn20	Ce1Os2Zn20	Ce	1	Os	2	Zn	20																		1	2017	emu/mol	0.0027																								AB2C20		CeCr2Al20	Fd3[-]m		A	14.3865														K					0.04																																																																																																		Zn-flux method					Structural, Magnetic, and Superconducting Properties of Caged Compounds ROs2Zn20 (R = La, Ce, Pr, and Nd)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 86(2017)034707	Kazuhei Wakiya,Takahiro Onimaru,Keisuke T. Matsumoto,Yu Yamane,Naohiro Nagasawa,Kazunori Umeo,Shunichiro Kittaka,Toshiro Sakakibara,Yoshitaka Matsushita,Toshiro Takabatake		
157157	JPS086034707	T<STR> = 87 K.	PrOs2Zn20	Pr1Os2Zn20	Pr	1	Os	2	Zn	20																		1	2017																										AB2C20		CeCr2Al20	Fd3[-]m		A	14.3494														K	0.06						0.06																				T	RES(R=zero)								T/K	RES(R=zero)	0.2			MHC157155																																																														Zn-flux method					Structural, Magnetic, and Superconducting Properties of Caged Compounds ROs2Zn20 (R = La, Ce, Pr, and Nd)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 86(2017)034707	Kazuhei Wakiya,Takahiro Onimaru,Keisuke T. Matsumoto,Yu Yamane,Naohiro Nagasawa,Kazunori Umeo,Shunichiro Kittaka,Toshiro Sakakibara,Yoshitaka Matsushita,Toshiro Takabatake		
157158	JPS086034707	T<STR> = 62 K.	NdOs2Zn20	Nd1Os2Zn20	Nd	1	Os	2	Zn	20																		1	2017																										AB2C20		CeCr2Al20	Fd3[-]m		A	14.329														K					0.04																																																																																																		Zn-flux method					Structural, Magnetic, and Superconducting Properties of Caged Compounds ROs2Zn20 (R = La, Ce, Pr, and Nd)			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashihiroshima, Hiroshima 739-8530, Japan	J.Phys.Soc.Jpn, 86(2017)034707	Kazuhei Wakiya,Takahiro Onimaru,Keisuke T. Matsumoto,Yu Yamane,Naohiro Nagasawa,Kazunori Umeo,Shunichiro Kittaka,Toshiro Sakakibara,Yoshitaka Matsushita,Toshiro Takabatake		
157159	JPS086035001	P-P dimer distance, P(1)-P(1) = 3.2328 A, P(2)-P(2) = 2.7097 A.	SrNi2P2	Sr1Ni2P2	Sr	1	Ni	2	P	2																		1	2017																										AB2C2		ThCr2Si2	Immm		A	3.9552	11.87	10.4889												K		1.41					1.41																																																																																																solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157160	JPS086035001	P-P dimer distance, P(1)-P(1) = 3.3936 A, P(2)-P(2) = 2.7518 A. not bulk SC(SC and non-SC regions)	Sr1-xBaxNi2P2	Sr0.8Ba0.2Ni2P2	Sr	0.8	Ba	0.2	Ni	2	P	2																1	2017																										AB2C2		ThCr2Si2	Immm		A	3.9422	11.825	10.8652												K				2.87			2.87										48																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157161	JPS086035001	P-P dimer distance, P(1)-P(1) = 3.4594 A, P(2)-P(2) = 2.7892 A. not bulk SC(SC and non-SC regions)	Sr1-xBaxNi2P2	Sr0.6Ba0.4Ni2P2	Sr	0.6	Ba	0.4	Ni	2	P	2																1	2017																										AB2C2		ThCr2Si2	Immm		A	3.9432	11.8354	11.0662												K				2.84			2.84	MTC157161									73																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157162	JPS086035001	P-P dimer distance, P(1)-P(1) = 3.3919 A, P(2)-P(2) = 2.6347 A.	Sr1-xBaxNi2P2	Sr0.5Ba0.5Ni2P2	Sr	0.5	Ba	0.5	Ni	2	P	2																1	2017																										AB2C2		ThCr2Si2	Immm		A	3.9379	11.8053	10.9835												K				2.76			2.76										80																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157163	JPS086035001	P-P dimer distance = 3.5301A uncollapsed tetragonal structure	Sr1-xBaxNi2P2	Sr0.3Ba0.7Ni2P2	Sr	0.3	Ba	0.7	Ni	2	P	2																1	2017																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9521		11.5448											uncolapsed tetragonal	K				2.55			2.55	MTC157161									75																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157164	JPS086035001	P-P dimer distance = 3.5600A   uncollapsed tetragonal structure	Sr1-xBaxNi2P2	Sr0.15Ba0.85Ni2P2	Sr	0.15	Ba	0.85	Ni	2	P	2																1	2017																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9485		11.7116											uncolapsed tetragonal	K				2.53			2.53										72																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157165	JPS086035001	P-P dimer distance = 3.6760A  uncollapsed tetragonal structure	BaNi2P2	Ba1Ni2P2	Ba	1	Ni	2	P	2																		1	2017																										AB2C2		ThCr2Si2	I4/mmm	139	A	3.9454		11.8183											uncolapsed tetragonal	K				2.53			2.53										73																																																																																						solid state reaction. Mixture - ground - in alumina clucible - sealed in quartz tube - heat(300C,5h), (700C,3h), (1000C,24h) - natural cooling					Enhanced Superconductivity in Close Proximity to the Structural Phase Transition of Sr1-xBaxNi2P2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)035001	Kazutaka Kudo,Yutaka Kitahama,Keita Iba,Masaya Takasuga,Minoru Nohara		
157166	JPS086044710	[penet]London, and SC carrier density = 4.98E+26 /m3 derived from muon-SR. e-ph = 0.75.	Cs2Cr3As3	Cs2Cr3As3	Cs	2	Cr	3	As	3																		1	2017																										A2B3C3		K2Cr3As3	P6[-]m2	187																K				2.1			2.1										10	Oe	M-H curve				10			0.5																	A	from Hc2=6.45T	71.4			nm	muon-SR, London theory	954					3	16																																															See Sci.China Mater., 58(2015)16 (SCM0580016)					Nodal Superconducting Gap Structure in the Quasi-One-Dimensional Cs2Cr3As3 Investigated Using muon-SR Measurements			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon, OX11 0QX, U.K.	J.Phys.Soc.Jpn, 86(2017)044710	Devashibhai Adroja,Amitava Bhattacharyya,Michael Smidman,Adrian Hillier,Yu Feng,Bingying Pan,Jun Zhao,Martin R. Lees,Andre Strydom,Pabitra K. Biswas		
157167	JPS086054711	irreversible temperature defined as ZFC & FC curves split, T(irr) = 4.4 K .Impurity phase:  SnSe2(3%), Ag8SnSe6(1%)	AgSnSe2	Ag1Sn1Se2	Ag	1	Sn	1	Se	2																		1	2017																										ABC2		NaCl	Fm3[-]m	225	A	5.6749														K	4.5		5.7	4.7			4.7																																																																							mOhm.cm							2.12																Ag(3N),Sn(4N),Bi(5N),Se(5N)		solid state reaction. Ground - mixture - pellet - sealed in quartz tube - SIN(400C,20h) - reground - repeat one more process					Bi Substitution Effects on Superconductivity of Valence-Skip Superconductor AgSnSe2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 193-0397, Japan	J.Phys.Soc.Jpn, 86(2017)054711	Yudai Hijikata,Atsuhiro Nishida,Kohei Nagasaka,Osuke Miura,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshikazu Mizuguchi		
157168	JPS086054711	irreversible temperature defined as ZFC & FC curves split, T(irr) = 4.8 K. Impurity phase:  SnSe2(3%), Ag8SnSe6(1%)	Ag(Sn,Bi)Se2	Ag1Sn0.9Bi0.1Se2	Ag	1	Sn	0.9	Bi	0.1	Se	2																1	2017																										ABC2		NaCl	Fm3[-]m	225	A	5.6953														K	5		6.3	5.2			5.2																																																																							mOhm.cm							0.985																Ag(3N),Sn(4N),Bi(5N),Se(5N)		solid state reaction. Ground - mixture - pellet - sealed in quartz tube - SIN(400C,20h) - reground - repeat one more process					Bi Substitution Effects on Superconductivity of Valence-Skip Superconductor AgSnSe2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 193-0397, Japan	J.Phys.Soc.Jpn, 86(2017)054711	Yudai Hijikata,Atsuhiro Nishida,Kohei Nagasaka,Osuke Miura,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshikazu Mizuguchi		
157169	JPS086054711	irreversible temperature defined as ZFC & FC curves split, T(irr) = 4.9 K. Impurity phase:  SnSe2(4%), Ag8SnSe6(2%)	Ag(Sn,Bi)Se2	Ag1Sn0.8Bi0.2Se2	Ag	1	Sn	0.8	Bi	0.2	Se	2																1	2017																										ABC2		NaCl	Fm3[-]m	225	A	5.7176														K	4.8		9.7	5.1			5.1	MTC157169																																																																						mOhm.cm							4.71																Ag(3N),Sn(4N),Bi(5N),Se(5N)		solid state reaction. Ground - mixture - pellet - sealed in quartz tube - SIN(400C,20h) - reground - repeat one more process					Bi Substitution Effects on Superconductivity of Valence-Skip Superconductor AgSnSe2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 193-0397, Japan	J.Phys.Soc.Jpn, 86(2017)054711	Yudai Hijikata,Atsuhiro Nishida,Kohei Nagasaka,Osuke Miura,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshikazu Mizuguchi		
157170	JPS086054711	irreversible temperature defined as ZFC & FC curves split, T(irr) = 3.3 K.	Ag(Sn,Bi)Se2	Ag1Sn0.7Bi0.3Se2	Ag	1	Sn	0.7	Bi	0.3	Se	2																1	2017																										ABC2		NaCl	Fm3[-]m	225	A															K	0			4			4																																																																																														Ag(3N),Sn(4N),Bi(5N),Se(5N)		solid state reaction. Ground - mixture - pellet - sealed in quartz tube - SIN(400C,20h) - reground - repeat one more process					Bi Substitution Effects on Superconductivity of Valence-Skip Superconductor AgSnSe2			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 193-0397, Japan	J.Phys.Soc.Jpn, 86(2017)054711	Yudai Hijikata,Atsuhiro Nishida,Kohei Nagasaka,Osuke Miura,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshikazu Mizuguchi		
157171	JPS086063704	(dC/gamma*Tc) = 2.3.  Lattice paraeter not given	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2017																										AB2C2		ThCr2Si2	I4/mmm	139																K				3.85			3.85																																																								mJ/mol.K2	6.1	SP	144	SP																																				Two-step process. firstly PdAs2 prepared by solisd state reaction.  mixture(Ba,Pd,PdAs2) - alumina crucible - sealed in quartz tube - heat(900C,48h)					Strong-Coupling Superconductivity in BaPd2As2 Induced by Soft Phonons in the ThCr2Si2-Type Polymorph			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)063704	Kazutaka Kudo,Yoshiaki Yamada,Takaaki Takeuchi,Takumi Kimura,Satoshi Ioka,Genta Matsuo,Yutaka Kitahama,Minoru Nohara		
157172	JPS086063704	not bulk SC.down to 1.8 K. Lattice paraeter not given	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2017																										AB2C2		CeMgSi2	P4/mmm	123																K					1.8																																																										mJ/mol.K2	5.4	SP	259	SP																																				mixture(Ba,Pd,PdAs2) in alumina crucible - saled in quartz tube - heat(700 - 1150C) - Q to iced water					Strong-Coupling Superconductivity in BaPd2As2 Induced by Soft Phonons in the ThCr2Si2-Type Polymorph			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)063704	Kazutaka Kudo,Yoshiaki Yamada,Takaaki Takeuchi,Takumi Kimura,Satoshi Ioka,Genta Matsuo,Yutaka Kitahama,Minoru Nohara		
157173	JPS086064710	P-induced SC. P<cr> = 11.7 GPa for Tc(on). Tc (DB) shows Tc(max)  at P = 20.3 GPa. Tm<mod> in TCFIG shows R(T) anomaly due to reconstruction of magnetic order.	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2017																										AB2C2		ThCr2Si2	I4/mmm																	K		2.24	2.54		0		2.24	MPH157173																			T	P = 13.0 GPa			3										MHC157173																																uV/K				MTP157173																										Sn-flux method. Details in Phys.Rev.X4(2014)031055					High-Pressure Study of the Ground- and Superconducting-State Properties of CeAu2Si2			DQMP?University of Geneva, 1211 Geneva 4, Switzerland	J.Phys.Soc.Jpn, 86(2017)064710	Gernot W. Scheerer,Gaetan Giriat,Zhi Ren,Gerard Lapertot,Didier Jaccard		
157174	JPS086064710	Data shows for P = 18.3 GPa	CeAu2Si2 (P=18.3GPa)	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2017																										AB2C2		ThCr2Si2	I4/mmm																	K					0																																																																				uV/K				MTP157174																										Sn-flux method. Details in Phys.Rev.X4(2014)031055					High-Pressure Study of the Ground- and Superconducting-State Properties of CeAu2Si2			DQMP?University of Geneva, 1211 Geneva 4, Switzerland	J.Phys.Soc.Jpn, 86(2017)064710	Gernot W. Scheerer,Gaetan Giriat,Zhi Ren,Gerard Lapertot,Didier Jaccard		
157175	JPS086064710	Data shows for P = 21.5 GPa	CeAu2Si2 (P=21.5GPa)	Ce1Au2Si2	Ce	1	Au	2	Si	2																		3	2017																										AB2C2		ThCr2Si2	I4/mmm																	K					0																																																																				uV/K				MTP157175																										Sn-flux method. Details in Phys.Rev.X4(2014)031055					High-Pressure Study of the Ground- and Superconducting-State Properties of CeAu2Si2			DQMP?University of Geneva, 1211 Geneva 4, Switzerland	J.Phys.Soc.Jpn, 86(2017)064710	Gernot W. Scheerer,Gaetan Giriat,Zhi Ren,Gerard Lapertot,Didier Jaccard		
157176	LES098L1	Tc = 3.7K(in DB)  maybe due to beta-Sn (impurity phase)	IrSn4	Ir1Sn4	Ir	1	Sn	4																					1984									5.4																	AB4			Aba2		A	6.274	6.337	11.352											PtSn4-type	K		3.7					3.7																																																																																																mixture - compress - placed in graphite ampoule - heat (900 - 1100K, p = 6.0 GPa)					The new phases IrSn4 and RhGe4 formed by high pressure treatment			Institute of High Pressure Physics of the U.S.S.R. Academy of Sciences, 142092 Troitsk, Moscow Region (U.S.S.R.)	J.Less-Common Metals, 98(1984)L1	V.I.Larchev,S.V.Popova		
157177	LES098L1		RhGe4	Ge4Rh1	Ge	4	Rh	1																					1984									7.5																	AB4					A	6.19		7.802											hexagonal, IrGe4-type	K		2.5					2.5																																																																																																mixture - compress - placed in graphite ampoule - heat( 1000 - 1300K, p = 2.5 GPa)					The new phases IrSn4 and RhGe4 formed by high pressure treatment			Institute of High Pressure Physics of the U.S.S.R. Academy of Sciences, 142092 Troitsk, Moscow Region (U.S.S.R.)	J.Less-Common Metals, 98(1984)L1	V.I.Larchev,S.V.Popova		
157178	MCP1940219	main phase: Nb2GeC(94 wt%). SP (beta) = 0.095 mJ/mol.K4. (dC/gamma*Tc) = 1.3	Nb2GeC	Nb2Ge1C1	Nb	2	Ge	1	C	1																			2017																										ABC2		Cr2AlC	P6<3>/mmc	194	A	3.23		12.54												K	8.8		10	10			10										80										T	RES(0.5Rn), WHH	7.4												MHC157178		A	from Hc2	66.7																		mJ/mol.K2	3.89	SP	434	SP																																		graphite,Nb,Ge		mixture - pellet - sealed in quartz ampoule - heat(1200C,300h in microwave furnace)					Superconducting evidence of a processed Nb2GeC compound under a microwave heating			School of Applied Sciences/FCA, Research Group in Manufacturing of Advanced Materials, University of Campinas, UNICAMP, Campus Limeira, 1300, Pedro Zaccaria St., 13484-350, Limeira, SP, Brazil	Mat.Chem.Phys., 194(2017)219	Ausdinir D. Bortolozo,Wislei R. Osorio,Bruno S. de Lima,Carlos Alberto M. Dos Santos,Antonio Jefferson S. Machado		
157179	MRB0201229		Si2Th	Si2Th1	Si	2	Th	1																				1	1985																										AB2		alpha-ThSi2			A	4.127		14.194												K		3.16					3.16																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157180	MRB0201229		ThSi2-xCox	Th1Si1.95Co0.05	Th	1	Si	1.95	Co	0.05																		1	1985																										AB2		alpha-ThSi2			A	4.119		14.121												K		2.38					2.38																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157181	MRB0201229		ThSi2-xCox	Th1Si1.9Co0.1	Th	1	Si	1.9	Co	0.1																		1	1985																										AB2		alpha-ThSi2			A	4.107		14.061												K		2.18					2.18																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157182	MRB0201229		ThSi2-xCox	Th1Si1.85Co0.15	Th	1	Si	1.85	Co	0.15																		1	1985																										AB2		alpha-ThSi2			A	4.114		14.019												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157183	MRB0201229		ThSi2-xCox	Th1Si1.7Co0.3	Th	1	Si	1.7	Co	0.3																		1	1985																										AB2		alpha-ThSi2			A	4.117		14.976												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157184	MRB0201229		ThSi2-xCox	Th1Si1.65Co0.35	Th	1	Si	1.65	Co	0.35																		1	1985																										AB2		alpha-ThSi2			A	4.11		13.999												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157185	MRB0201229	There exists trace of beta-Thsi2	ThSi2-xCox	Th1Si1.6Co0.4	Th	1	Si	1.6	Co	0.4																		1	1985																										AB2		alpha-ThSi2			A	4.091		13.985												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157186	MRB0201229	Two phases: alpha- and beta-ThSi2	ThSi2-xCox	Th1Si1.58Co0.42	Th	1	Si	1.58	Co	0.42																		1	1985																										AB2		alpha-ThSi2			A	4.204		14.003											alpha- and beta-ThSi2(a=4.031, c=4.200)	K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157187	MRB0201229	There exists trace of alpha-Thsi2	ThSi2-xCox	Th1Si1.55Co0.45	Th	1	Si	1.55	Co	0.45																		1	1985																										AB2		beta-ThSi2			A	4.03		4.197												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157188	MRB0201229	Broad SC transition around 2 K.	ThSi2-xCox	Th1Si1.5Co0.5	Th	1	Si	1.5	Co	0.5																		1	1985																										AB2		beta-ThSi2			A	4.043		4.189												K		2					2																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157189	MRB0201229		ThSi2-xCox	Th1Si1.45Co0.55	Th	1	Si	1.45	Co	0.55																		1	1985																										AB2		beta-ThSi2			A	4.05		4.162												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157190	MRB0201229		ThSi2-xCox	Th1Si1.35Co0.65	Th	1	Si	1.35	Co	0.65																		1	1985																										AB2		beta-ThSi2			A	4.056		4.136												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157191	MRB0201229	Two phases: alpha- and beta-ThSi2	ThSi2-xCox	Th1Si1.3Co0.7	Th	1	Si	1.3	Co	0.7																		1	1985																										AB2		beta-ThSi2			A	4.068		14.091											alpha- and beta-ThSi2(a=4.070, c=4.100)	K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157192	MRB0201229	There exists trace of beta-Thsi2	ThSi2-xCox	Th1Si1.25Co0.75	Th	1	Si	1.25	Co	0.75																		1	1985																										AB2		alpha-ThSi2			A	4.074		14.094												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157193	MRB0201229	There exists trace of beta-Thsi2	ThSi2-xCox	Th1Si1.2Co0.8	Th	1	Si	1.2	Co	0.8																		1	1985																										AB2		alpha-ThSi2			A	4.078		14.119												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157194	MRB0201229	There exists trace of beta-Thsi2	ThSi2-xCox	Th1Si1.15Co0.85	Th	1	Si	1.15	Co	0.85																		1	1985																										AB2		alpha-ThSi2			A	4.078		14.122												K					1.7																																																																																																		arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157195	MRB0201229		ThSi2-xCox	Th1Si1.075Co0.925	Th	1	Si	1.075	Co	0.925																		1	1985																										AB2		alpha-ThSi2			A	4.084		14.133												K		2.7			1.7		2.7																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157196	MRB0201229		ThCoSi	Th1Si1Co1	Th	1	Si	1	Co	1																		1	1985																										ABC		alpha-ThSi2			A	4.077		14.115												K		2.84			1.7		2.84																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157197	MRB0201229		ThSi2-xRhx	Th1Rh0.96Si1.04	Th	1	Rh	0.96	Si	1.04																		1	1985																										ABC					A	4.129		14.28												K		6.45					6.45																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157198	MRB0201229		ThIrSi	Th1Ir1Si1	Th	1	Ir	1	Si	1																		1	1985																										ABC					A	4.143		14.27												K		6.5					6.5																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157199	MRB0201229		ThNiSi	Th1Ni1Si1	Th	1	Ni	1	Si	1																		1	1985																										ABC					A	4.073		14.099												K		2					2																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157200	MRB0201229		ThPtSi	Th1Pt1Si1	Th	1	Pt	1	Si	1																		1	1985																										ABC					A	4.154		14.582												K		2.98					2.98																																																																																																arc-melting using tri-arc furnace.  ANN(950C, 8 days)					Structural and Electrical Properties of Silisides: ThCoxSi2-x (0 =< x =<1) and ThTSi (T = Ni, Pt)			Laboratoire de Chemie du Solide du C.N.R..S. 351cours de la Liberation, 33405 Talence cedex, France	Mat.Res.Bull., 20(1985)1229	Wang Xian Zhong,Wee Lam Ng,B.Chevalier,J.Etourneau,P.Hagenmuller		
157201	NATCOM0067805	P-induced SC. SC appears Tc(on) = 3.1K at P=2.5 GPa. Tc(max) = 7 K (in DB) at P=16.8 GPa. Hc2 measured at P = 24.6 GPa. TCFIG for three runs for different samples.	WTe2	Te2W1	Te	2	W	1																				3	2015																										AB2			Pnm2<1>		A	3.53	6.201	14.015												K			7		1.8		7	MTC157201																			T	RES(on), WHH	2.72												MHC157201																																																														CVT method. (W & Te powder, TeBr4 as a transport agent) - quartz tube (800C(H) and 700C(L) zone, for 8 days)					Pressure-driven dome-shaped superconductivity and electronic structural evolution in tungsten ditelluride			National Laboratory of Solid State Microstructures, College of Physics, Nanjing University, Nanjing 210093, China	Nat.Cmmun., 6(2015)7805	Xing-Chen Pan,Xuliang Chen,Huimei Liu,Yanqing Feng,Zhongxia Wei,Yonghui Zhou,Zhenhua Chi,Li Pi,Fei Yen,Fengqi Song,Xiangang Wan,Zhaorong Yang,Baigeng Wang,Guanghou Wang,Yuheng Zhang		
157202	NATCOM0067804	P-induced SC. P<cr> = 10.8 GPa where Tc = 2.8 K. LMR(large magnetoresistance) below T*. Tc(max) = 6.5 K (in DB) at 13.0 GPa. Hc2(0) in Fig from GL fitting.	WTe2	Te2W1	Te	2	W	1																				3	2015																										AB2					A	3.5965	6.0401	13.6948											P = 0.8 GPa from Fig of T-dependence of lattice const.	K			6.5		0		6.5	MTC157202																			T	RES(on), GL-fitting, P=13.7 GPa	1.86												MHC157202																																																			cm3/C						MRH157202			W(3N),Te(5N)		mixture(W + excess Te) - alumina ampoule - sealed in quartz tube - heat to 1000C(100C/h) - keep(1000C,5h) - cool to 800C(1C/h) - cool to 700C(5C/h)					Superconductivity emerging from a suppressed large magnetoresistant state in tungsten ditelluride			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Nat.Cmmun., 6(2015)7804	Defen Kang,Yazhou Zhou,Wei Yi,Chongli Yang,Jing Guo,Youguo Shi,Shan Zhang,Zhe Wang,Chao Zhang,Sheng Jiang,Aiguo Li,Ke Yang,Qi Wu,Guangming Zhang,Liling Sun,Zhongxian Zhao		
157203	NATCOM00711038	RRR = 36. Phase transition, monoclinic 1T' to ortho-Td phase at 250 K. Tc(on) = 0.25 k for Td-phase.	MoTe2	Mo1Te2	Mo	1	Te	2																				3	2016																										AB2			P2<1>/m		A	6.32	3.469	13.86											1T'- MoTe2 phase at RT, beta = 93.91. phase transition to Td-phase around 250 K	K	0.1		0.25				0.175	MTC157203																																																																																													Mo(4N),Te(4N)		CVT method. (Mo & Te pellet + TeCl4 as transport agent) - quartz tube - two zone furnace (1000C(H) and 900C(L))					Superconductivity in Weyl semimetal candidate MoTe2			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Cmmun., 7(2016)11038	Yanpeng Qi,Pavel G. Naumov,Mazhar N. Ali,Catherine R. Rajamathi,Walter Schnelle,Oleg Barkalov,Michael Hanfland,Shu-Chun Wu,Chandra Shekhar,Yan Sun,Vicky Suss,Marcus Schmidt,Ulrich Schwarz,Eckhard Pippel,Peter Werner,Reinald Hillebrand,Tobias Forster,Erik Kampert,Stuart Parkin,Sergey A. Medvedev		
157204	NATCOM00711038	P = 1.1 GPa. no structural transition.	MoTe2	Mo1Te2	Mo	1	Te	2																				3	2016																										AB2																				K			6.1				6.1																				T	RES(0.9Rn), GL fitting	1.67												MHC157204																																																												Mo(4N),Te(4N)		CVT method. (Mo & Te pellet + TeCl4 as transport agent) - quartz tube - two zone furnace (1000C(H) and 900C(L))					Superconductivity in Weyl semimetal candidate MoTe2			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Cmmun., 7(2016)11038	Yanpeng Qi,Pavel G. Naumov,Mazhar N. Ali,Catherine R. Rajamathi,Walter Schnelle,Oleg Barkalov,Michael Hanfland,Shu-Chun Wu,Chandra Shekhar,Yan Sun,Vicky Suss,Marcus Schmidt,Ulrich Schwarz,Eckhard Pippel,Peter Werner,Reinald Hillebrand,Tobias Forster,Erik Kampert,Stuart Parkin,Sergey A. Medvedev		
157205	NATCOM00711038	P = 11.7 GPa.  no structural transition.	MoTe2	Mo1Te2	Mo	1	Te	2																				3	2016																										AB2																				K			8.1				8.1																				T	RES(0.9Rn), GL fitting	4												MHC157205																																																												Mo(4N),Te(4N)		CVT method. (Mo & Te pellet + TeCl4 as transport agent) - quartz tube - two zone furnace (1000C(H) and 900C(L))					Superconductivity in Weyl semimetal candidate MoTe2			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Cmmun., 7(2016)11038	Yanpeng Qi,Pavel G. Naumov,Mazhar N. Ali,Catherine R. Rajamathi,Walter Schnelle,Oleg Barkalov,Michael Hanfland,Shu-Chun Wu,Chandra Shekhar,Yan Sun,Vicky Suss,Marcus Schmidt,Ulrich Schwarz,Eckhard Pippel,Peter Werner,Reinald Hillebrand,Tobias Forster,Erik Kampert,Stuart Parkin,Sergey A. Medvedev		
157206	NATM0141008	P-induced SC. P<cr> = 10 GPa. Tc(max) = 17 K (in DB) at 13.5 GPa. (dTc/dH) = -3.8 K/T at 11.5 GPa.	BaFe2S3	Ba1Fe2S3	Ba	1	Fe	2	S	3																		3	2015					myu-B/Fe	1.2		119																		AB2C3																			ladder type	K	17				0		17	MTC157206																																																																																															solid state reaction. mixture(various nominal compositions) - carbon crucible - in quartz tube - heat(1100C, 40h) - slow cool to 750C over 24h.					Pressure-induced superconductivity in the iron-based ladder material BaFe2S3			College of Humanities & Sciences, Nihon University, Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan	Nat.Mater., 14(2015)1008	Hiroki Takahashi,Akira Sugimoto,Yusuke Nambu,Touru Yamauchi,Yasuyuki Hirata,Takateru Kawakami,Maxim Avdeev,Kazuyuki Matsubayashi,Fei Du,Chizuru Kawashima,Hideto Soeda,Satoshi Nakano,Yoshiya Uwatoko,Yutaka Ueda,Taku J. Sato,Kenya Ohgushi		
157207	NJP015053005	RRR = 26. Tc(SP) = 2.75 K. Hc2(0) = 0.48 T from SP measurements. Two-gap model (d1 - 2.0 and d2 = 1.2Tc) is better from [penet] and SP data.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2013																										ABC2	3	CeNiC2	Amm2	38	A	3.9599	4.5636	6.2031											At 8K, beta-SrRh2As2(Fmmm)	K		3.5		2.95			3.5																				T	RES, extrapolation	1.67												MHC157207							A	TDO measurement	3940					4					MSP157207			mJ/mol.K2	7.7	SP	450	SP											uOhm.cm	6										121												La(3N),Ni(2N),graphite(3N)		arc-melting several times - ANN(1050C, 7days, insealed quartz tube(vac)  - Q to RT					Evidence for two-gap superconductivity in the non-centrosymmetric compound LaNiC2			Department of Physics and Center for Correlated Matter, Zhejiang University, Hangzhou, Zhejiang 310027, People's Republic of China	New J.Phys., 15(2013)053005	J Chen,L Jiao,J L Zhang,Y Chen,L Yang,M Nicklas,F Steglich,H Q Yuan		
157208	PRB0586287	not SC. RRR = 13.8.  Curie-Weiss for 120<T<300K.  SP (gamma) = 140 mJ/mol.k2 derived from  T-dependence of (gamma) in SP-figure. (gamma) = 75 mJ/mol.K2 (in DB)  for 5<T<15 K.	YbFe4Sb12	Yb1Fe4Sb8	Yb	1	Fe	4	Sb	8																		1	1998	cm3/mol	0.0345			myu-B/f.u	3.09	40																			AB4C12	1	skutterudite			A	9.158													LaFe4P12-type	K					0.4																																																							MSP157208			mJ/mol.K2	75	SP	190	SP											uOhm.cm	9										125														mixture(Yb:Fe:Sb = 1.05:4:12) - in graphite crucible - sealed in quartz tube - heat(950C) - ANN(600C,20h, in Ar) - nearly single phase					Intermediate valence in the filled skutterudite compound YbFe4Sb12			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, California 92093	Phys.Rev.B, 58(1998)6287	N. R. Dilley,E. J. Freeman,E. D. Bauer,M. B. Maple		
157209	PRB079144509	RRR = 28. SP (beta)=0.3732 mJ/mol.K4. (dC/gamma*Tc) = 1.31. Hc(0) = 612 Oe from entropy analysis. e-ph = 0.48. Hc1(T) in Fig-data. Hall coeff.(DB) at 200K.	Ru7B3	B3Ru7	B	3	Ru	7																				1	2009																										A3B7			P6<3>mc		A	7.4629		4.7141											hexagonal	K	3.3			3.3	0.3		3.3											Oe	M-H curve	90							T	RES(zero)	1.1							T/K	RES(zero)	0.277			MHC157209		A	from Hc2	172			A	carrier density	2140			meV	0.5	3.6	14				MSP157209			mJ/mol.K2	80.15	SP	470.175	SP											uOhm.cm	9													m3/C	0.000000000447				9				Ru(3N), B(3N5)		Solid state reaction. mixture - pellet - wrapped with Ta-foil - sealed in silicon tube(95%Ar, 5%H2) - heat to 1000C(100C/h) - SIN(100h) - FC to RT.					Physical properties of the noncentrosymmetric superconductor Ru7B3			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, P.O. Box 603, Beijing 100190, People's Republic of China	Phys.Rev.B, 79(2009)144509	Lei Fang,Huan Yang,Xiyu Zhu,Gang Mu,Zhao-Sheng Wang,Lei Shan,Cong Ren,Hai-Hu Wen		
157210	PRB088094510	T<STR> = Tn = 136.6 K. Tn defined by NED and peak of (dM/dT).	(Ba,Na)Fe2As2	Ba0.9Na0.1Fe2As2	Ba	0.9	Na	0.1	Fe	2	As	2																1	2013					myu-B/f.u	0.73		137																		AB2C2		ThCr2Si2	I4/mmm		A	3.9417		13.0563											At 8K, beta-SrRh2As2(Fmmm), a=5.58558, b=5.5454, c=12.9669	K																																																																																																					Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157211	PRB088094510	T<STR> = Tn = 128.1 K. Tn defined by NED and peak of (dM/dT).	(Ba,Na)Fe2As2	Ba0.85Na0.15Fe2As2	Ba	0.85	Na	0.15	Fe	2	As	2																1	2013					myu-B/f.u	0.728		128																		AB2C2		ThCr2Si2	I4/mmm		A	3.9378		13.0759											At 8K, beta-SrRh2As2(Fmmm), a=5.5793, c=5.5397, c=12.9773	K				1.4			1.4																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157212	PRB088094510	T<STR> = Tn = 107.0 K. Tn defined by NED and peak of (dM/dT).	(Ba,Na)Fe2As2	Ba0.8Na0.2Fe2As2	Ba	0.8	Na	0.2	Fe	2	As	2																1	2013					myu-B/f.u	0.669		107																		AB2C2		ThCr2Si2	I4/mmm		A	3.9262		13.0988											At 8K, beta-SrRh2As2(Fmmm), a=5.5611, b=5.5302, c=12.9838	K				15.2			15.2																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157213	PRB088094510		(Ba,Na)Fe2As2	Ba0.7Na0.3Fe2As2	Ba	0.7	Na	0.3	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.9108		13.1222											At 8K, ThCr2Si2(I4/mmm, a=3.9031, c=13.0126	K				25.8			25.8																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157214	PRB088094510		(Ba,Na)Fe2As2	Ba0.6Na0.4Fe2As2	Ba	0.6	Na	0.4	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.8959		13.1313											At 8K, ThCr2Si2(I4/mmm, a=3.8867, c=13.0282	K				34.2			34.2	MTC157214																																																																																													Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157215	PRB088094510		(Ba,Na)Fe2As2	Ba0.5Na0.5Fe2As2	Ba	0.5	Na	0.5	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.8809		13.1208											At 8K, ThCr2Si2(I4/mmm, a=3.8692, c=13.0171	K				33.2			33.2																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157216	PRB088094510		(Ba,Na)Fe2As2	Ba0.4Na0.6Fe2As2	Ba	0.4	Na	0.6	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.8649		13.0893											At 8K, ThCr2Si2(I4/mmm, a=3.8533, c=12.9791	K				28.7			28.7																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157217	PRB088094510		(Ba,Na)Fe2As2	Ba0.3Na0.7Fe2As2	Ba	0.3	Na	0.7	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A	3.8515		13.0244											At 8K, ThCr2Si2(I4/mmm, a=3.8361, c=12.9217	K				24			24																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157218	PRB088094510		(Ba,Na)Fe2As2	Ba0.2Na0.8Fe2As2	Ba	0.2	Na	0.8	Fe	2	As	2																1	2013																										AB2C2		ThCr2Si2	I4/mmm		A															K				18.6			18.6																																																																																														Ba,Na,FeAs		mixture - in alumina tube - sealed in Nb tube(Ar) - quartz tube(vac) - heat(850C,1d) - ground to powder - heat(850C,3d)					Structural, magnetic, and superconducting properties of Ba1-xNaxFe2As2			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439-4845, USA	Phys.Rev.B, 88(2013)094510	S. Avci,J. M. Allred,O. Chmaissem,D. Y. Chung,S. Rosenkranz,J. A. Schlueter,H. Claus,A. Daoud-Aladine,D. D. Khalyavin,P. Manuel,A. Llobet,M. R. Suchomel,M. G. Kanatzidis,R. Osborn		
157219	PRB088094516		NaFeAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2013																										ABC																				K	9.6						9.6																																																																																					m3/C						MRH157219			NaAs,Fe,Cu		NaAs-flux method. mixture(NaAs:Fe:Cu = 4:(1-x):x) - wrapped in alumina crucible - sealed in Fe crucible(ar) - heat(950 C,10h) - cool to 600 C(3C/h)					Phase diagram and physical properties of NaFe1-xCuxAs single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 88(2013)094516	A. F. Wang,J. J. Lin,P. Cheng,G. J. Ye,F. Chen,J. Q. Ma,X. F. Lu,B. Lei,X. G. Luo,X. H. Chen		
157220	PRB088094516	Anisotropy (Hc2) = 1.88	Na(Fe,Cu)As	Na1Fe0.994Cu0.006As1	Na	1	Fe	0.994	Cu	0.006	As	1																3	2013																										ABC																				K	10.2						10.2	MTC157220																			T	RES(off), WHH		30	16					T/K	RES(off)		4.23	2.24																																																										MRH157220			NaAs,Fe,Cu		NaAs-flux method. mixture(NaAs:Fe:Cu = 4:(1-x):x) - wrapped in alumina crucible - sealed in Fe crucible(ar) - heat(950 C,10h) - cool to 600 C(3C/h)					Phase diagram and physical properties of NaFe1-xCuxAs single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 88(2013)094516	A. F. Wang,J. J. Lin,P. Cheng,G. J. Ye,F. Chen,J. Q. Ma,X. F. Lu,B. Lei,X. G. Luo,X. H. Chen		
157221	PRB088094516	Anisotropy (Hc2) = 2.22.  SP (beta) = 0.238 mJ/mol.K4, (delta) = -5.0E-5 mJ/mol.K6,  (dC/Tc) = 9.85. (dC/gamma*Tc) = 1.32.	Na(Fe,Cu)As	Na1Fe0.981Cu0.019As1	Na	1	Fe	0.981	Cu	0.019	As	1																3	2013																										ABC																				K	11.5						11.5	MTC157221																			T	RES(off), WHH		49	22					T/K	RES(off)		6.33	2.55																							mJ/mol.K2	7.44	SP	290	SP																															MRH157221			NaAs,Fe,Cu		NaAs-flux method. mixture(NaAs:Fe:Cu = 4:(1-x):x) - wrapped in alumina crucible - sealed in Fe crucible(ar) - heat(950 C,10h) - cool to 600 C(3C/h)					Phase diagram and physical properties of NaFe1-xCuxAs single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 88(2013)094516	A. F. Wang,J. J. Lin,P. Cheng,G. J. Ye,F. Chen,J. Q. Ma,X. F. Lu,B. Lei,X. G. Luo,X. H. Chen		
157222	PRB088094516		Na(Fe,Cu)As	Na1Fe0.963Cu0.037As1	Na	1	Fe	0.963	Cu	0.037	As	1																3	2013																										ABC																				K	2.6						2.6	MTC157222																																																																																										MRH157222			NaAs,Fe,Cu		NaAs-flux method. mixture(NaAs:Fe:Cu = 4:(1-x):x) - wrapped in alumina crucible - sealed in Fe crucible(ar) - heat(950 C,10h) - cool to 600 C(3C/h)					Phase diagram and physical properties of NaFe1-xCuxAs single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 88(2013)094516	A. F. Wang,J. J. Lin,P. Cheng,G. J. Ye,F. Chen,J. Q. Ma,X. F. Lu,B. Lei,X. G. Luo,X. H. Chen		
157223	PRB088094516		Na(Fe,Cu)As	Na1Fe0.976Cu0.024As1	Na	1	Fe	0.976	Cu	0.024	As	1																3	2013																										ABC																				K	11.1						11.1	MPH157223																																																																																													NaAs,Fe,Cu		NaAs-flux method. mixture(NaAs:Fe:Cu = 4:(1-x):x) - wrapped in alumina crucible - sealed in Fe crucible(ar) - heat(950 C,10h) - cool to 600 C(3C/h)					Phase diagram and physical properties of NaFe1-xCuxAs single crystals			Hefei National Laboratory for Physical Science at Microscale and Department of Physics, University of Science and Technology of China, Hefei, Anhui 230026, People's Republic of China	Phys.Rev.B, 88(2013)094516	A. F. Wang,J. J. Lin,P. Cheng,G. J. Ye,F. Chen,J. Q. Ma,X. F. Lu,B. Lei,X. G. Luo,X. H. Chen		
157224	PRB091060503	SP (delta) = 0.32 mJ/mol.K6.  (dC/gamma*Tc) = 2.06. Energy gap measured by muon-SR (in DB). (2d/kTc) = 4.26 from SP analysis. From muon-SR, m* = 1.32m, n = 2.6E+28 /m3.	Lu5Rh6Sn18	Lu5Rh6Sn18	Lu	5	Rh	6	Sn	18																		3	2015																										A5B6C18	2		I4<1>/acd																	K				4			4										53	Oe		20																																	meV	0.75	4.4	16					mJ/mol.K	397	mJ/mol.K2	48.1	SP	152	SP																																				Sn-flux method. nominal composition (Lu:Rh:Sn = 1:2:20). See Solid State Commun., 34(1980)923					Broken time-reversal symmetry probed by muon spin relaxation in the caged type superconductor Lu5Rh6Sn18			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom	Phys.Rev.B, 91(2015)060503	A. Bhattacharyya,D. T. Adroja,J. Quintanilla,A. D. Hillier,N. Kase,A. M. Strydom,J. Akimitsu		
157225	PNAS1132904	P-induced SC. SC-1 for P > Pc=6.7 GPa. Data for P = 14.6 GPa. R-anomaly at 128 K (P=0) where phase transition to C2/m.	ZrTe5	Te5Zr1	Te	5	Zr	1																				3	2016																										AB5			C2/m																Low temperature phase	K			4				4	MTC157225																			T	RES(0.9Rn), WHH	1.54												MHC157225																																																												Zr(4N),Te(4N)		Crystals grown by vapor transport method in two zone furnace using iodine as a transport agent					Pressure-induced superconductivity in a three-dimensional topological material ZrTe5			High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Proc.Natl,Acad.Sci.USA, 113(2016)2904	Yonghui Zhou,Juefei Wu,Wei Ning,Nana Li,Yongping Du,Xuliang Chen,Ranran Zhang,Zhenhua Chi,Xuefei Wang,Xiangde Zhu,Pengchao Lu,Cheng Ji,Xiangang Wan,Zhaorong Yang,Jian Sun,Wenge Yang,Mingliang Tian,Yuheng Zhang,Ho-kwang Mao		
157226	PNAS1132904	P-induced SC. Two SC phases, SC-1(for P > 6.7 GPa) and Sc2 ( for P > 21.2 GPa. SC-data for P = 30.0 GPa. no phase transition. SC-2 shows no zero resistivity at 1.8 K. maybe topological surface SC	ZrTe5	Te5Zr1	Te	5	Zr	1																				3	2016																										AB5			P-1																Low temperature phase	K			6				6	MTC157225																			T	RES(0.9Rn), WHH	0.46												MHC157226																																																												Zr(4N),Te(4N)		Crystals grown by vapor transport method in two zone furnace using iodine as a transport agent					Pressure-induced superconductivity in a three-dimensional topological material ZrTe5			High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Proc.Natl,Acad.Sci.USA, 113(2016)2904	Yonghui Zhou,Juefei Wu,Wei Ning,Nana Li,Yongping Du,Xuliang Chen,Ranran Zhang,Zhenhua Chi,Xuefei Wang,Xiangde Zhu,Pengchao Lu,Cheng Ji,Xiangang Wan,Zhaorong Yang,Jian Sun,Wenge Yang,Mingliang Tian,Yuheng Zhang,Ho-kwang Mao		
157227	PRB093100504	Space-G = P6<3>mc for RT, P=0. normal state: Insulator, semiconductor for P < 5 GPa. SC data for P = 24.1GPa. Hall const. at 10 K.	BiTeCl	Bi1Te1Cl1	Bi	1	Te	1	Cl	1																		3	2016																										ABC			Pnma																normal state STR from Raman	K			6.93				6.93	MTC157227																			T	RES(0.9Rn), WHH	8												MHC157227																																																			mm3/C	-94.3					MRH157227					Crystals grown by self-flux method. See New J. Phys., 15(2013)085022					Realization of insulating state and superconductivity in the Rashba semiconductor BiTeCl			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 93(2016)100504	Jian-Jun Ying,Viktor V. Struzhkin,Zi-Yu Cao,Alexander F. Goncharov,Ho-Kwang Mao,Fei Chen,Xian-Hui Chen,Alexander G. Gavriliuk,Xiao-Jia Chen		
157228	PRB093100504	Normal state: metallic. SC data for P = 50.1 GPa. Hall const. at 10K.	BiTeCl	Bi1Te1Cl1	Bi	1	Te	1	Cl	1																		3	2016																										ABC																			cubic from Raman	K			4.52				4.52	MTC157227																			T	RES(0.9Rn), WHH	3.5												MHC157227																																																			mm3/C	-0.3					MRH157227					Crystals grown by self-flux method. See New J. Phys., 15(2013)085022					Realization of insulating state and superconductivity in the Rashba semiconductor BiTeCl			Center for High Pressure Science and Technology Advanced Research, Shanghai 201203, China	Phys.Rev.B, 93(2016)100504	Jian-Jun Ying,Viktor V. Struzhkin,Zi-Yu Cao,Alexander F. Goncharov,Ho-Kwang Mao,Fei Chen,Xian-Hui Chen,Alexander G. Gavriliuk,Xiao-Jia Chen		
157229	PRB092064507	T<STR> = 53 K from C(T) measurement.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2015																										A3B7																				K			2.35	2.35			2.35																																																																																																Sb-flux method. (Te or Ru-doped sample):Sb = 1:49, crystals separated from residual flux after decanting at 700 C					Fragile structural transition in Mo3Sb7			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 92(2015)064507	J.-Q. Yan,M. A. McGuire,A. F. May,D. Parker,D. G. Mandrus,B. C. Sales		
157230	PRB092064507	Te-content = nominal.  no structural transition	Mo3(Sb,Te)7	Mo3Sb6.975Te0.025	Mo	3	Sb	6.975	Te	0.025																		3	2015																										A3B7																				K		2.05		2.05			2.05																																																																																																Sb-flux method. (Te or Ru-doped sample):Sb = 1:49, crystals separated from residual flux after decanting at 700 C					Fragile structural transition in Mo3Sb7			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 92(2015)064507	J.-Q. Yan,M. A. McGuire,A. F. May,D. Parker,D. G. Mandrus,B. C. Sales		
157231	PRB092064507	Ru-content by EDX.  no structural transition	(Mo,Ru)3Sb7	Mo2.91Ru0.09Sb7	Mo	2.91	Ru	0.09	Sb	7																		3	2015																										A3B7																				K			2.15	2.15			2.15																																																																																																Sb-flux method. (Te or Ru-doped sample):Sb = 1:49, crystals separated from residual flux after decanting at 700 C					Fragile structural transition in Mo3Sb7			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 92(2015)064507	J.-Q. Yan,M. A. McGuire,A. F. May,D. Parker,D. G. Mandrus,B. C. Sales		
157232	PRB092064507	T<STR> = 48 K from C(T) measurement. SUS shows Curie-Weiss law for T < 40 K. Effective moment = 1.1 myu-B/Cr.	(Mo,Cr)3Sb7	Mo2.9Co0.1Sb7	Mo	2.9	Co	0.1	Sb	7																		3	2015																										A3B7																				K					1.8																																																																																																		Sb-flux method. (Te or Ru-doped sample):Sb = 1:49, crystals separated from residual flux after decanting at 700 C					Fragile structural transition in Mo3Sb7			Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev.B, 92(2015)064507	J.-Q. Yan,M. A. McGuire,A. F. May,D. Parker,D. G. Mandrus,B. C. Sales		
157233	PRB095094505	not SC.  SUS and R(T) shows SC-transition due to impurity phase (0.5 % ZrB12) at 5.5 K.	ZrB2	B2Zr1	B	2	Zr	1																				1	2017																										AB2		AlB2																		K					2																																																																																																							Doping-induced superconductivity of ZrB2 and HfB2			Laboratorium fur Festkorperphysik, ETH Zurich, CH-8093, Zurich, Switzerland	Phys.Rev.B, 95(2017)094505	N. Barbero,T. Shiroka,B. Delley,T. Grant,A. J. S. Machado,Z. Fisk,H.-R. Ott,J. Mesot		
157234	PRB095094505	not SC.	HfB2	B2Hf1	B	2	Hf	1																				1	2017																										AB2		AlB2																		K					2																																																																																																							Doping-induced superconductivity of ZrB2 and HfB2			Laboratorium fur Festkorperphysik, ETH Zurich, CH-8093, Zurich, Switzerland	Phys.Rev.B, 95(2017)094505	N. Barbero,T. Shiroka,B. Delley,T. Grant,A. J. S. Machado,Z. Fisk,H.-R. Ott,J. Mesot		
157235	PRB095094505	GL(kappa) = 125	(Zr,V)B2	Zr0.96V0.04B2	Zr	0.96	V	0.04	B	2																		1	2017																										AB2		AlB2																		K				8.33			8.33											mT	H-V curve	2.5							T	RES, WHH	16.4												MHC157235		A	from Hc2	45			A	from GL(kappa)	5700																												uOhm.cm							0.7																							Doping-induced superconductivity of ZrB2 and HfB2			Laboratorium fur Festkorperphysik, ETH Zurich, CH-8093, Zurich, Switzerland	Phys.Rev.B, 95(2017)094505	N. Barbero,T. Shiroka,B. Delley,T. Grant,A. J. S. Machado,Z. Fisk,H.-R. Ott,J. Mesot		
157236	PRB095094505	GL(kappa) = 80	(Hf,V)B2	Hf0.97V0.03B2	Hf	0.97	V	0.03	B	2																		1	2017																										AB2		AlB2																		K				7.31			7.31											mT	H-V curve	3.6							T	RES, WHH	10.8												MHC157236		A	from Hc2	55			A	from GL(kappa)	4450																												uOhm.cm							0.8																							Doping-induced superconductivity of ZrB2 and HfB2			Laboratorium fur Festkorperphysik, ETH Zurich, CH-8093, Zurich, Switzerland	Phys.Rev.B, 95(2017)094505	N. Barbero,T. Shiroka,B. Delley,T. Grant,A. J. S. Machado,Z. Fisk,H.-R. Ott,J. Mesot		
157237	PRB095094510	Energy gap measured by optical conductivity. Two gaps: large gap in DB. small gap d2=4.9 meV, (2d2/kTc) = 3.6.	(C8.5La1.5)(Pt3As8)(Fe2As2)5	Ca8.5La1.5Pt3Fe10As18	Ca	8.5	La	1.5	Pt	3	Fe	10	As	18															2017																																													Ca-10-3-8	K	32.8		35.2				34																																														meV	14.2	10.2	15																																													CaAs,LaAs,FeAs		Bridgman method with a Mo-crucible at 1250 C					Optical properties of optimally doped single-crystal Ca8.5La1.5(Pt3As8)(Fe2As2)5			Department of Emerging Materials Science, Daegu Gyeongbuk Institute of Science and Technology (DGIST), Daegu 711-873, Republic of Korea	Phys.Rev.B, 95(2017)094510	Yu-il Seo,Woo-Jae Choi,Shin-ichi Kimura,Yunkyu Bang,Yong Seung Kwon		
157238	PRB095100501	RRR = 60. T<STR> = 250 K where (P2<1>/m)1T' phase to (Pnm2<1> Td phase transition. Pc (T<STR> = 0) = 0.75 GPa. (dTc/dP) = 4 K/GPa near Pc	MoTe2	Mo1Te2	Mo	1	Te	2																				3	2017																										AB2																			P2<1>/m to Pnm2<1> Td transition at 250 K	K	0.1						0.1	MTC157238																																																																																															single crystals grown by chemical vapor transport method (CVT)					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157239	PRB095100501	SP (beta) = 0.923 mJ/mol.K4	MoTe2	Mo1Te2	Mo	1	Te	2																				1	2017																										AB2																			LT phase = Td(polar)	K	0.3						0.3																																																								mJ/mol.K2	3.7	SP	180	SP						uV/K	34.4			MTP157239																										solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157240	PRB095100501		Mo(Te,Se)2	Mo1Te1.94Se0.06	Mo	1	Te	1.94	Se	0.06																		1	2017																										AB2																			LT phase = Td(polar)	K	0.46						0.46																																																																		uV/K	24.4																													solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157241	PRB095100501		Mo(Te,Se)2	Mo1Te1.9Se0.1	Mo	1	Te	1.9	Se	0.1																		1	2017																										AB2																			LT phase = Td(polar)	K	0.49						0.49																																																																		uV/K	26.6																													solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157242	PRB095100501		Mo(Te,Se)2	Mo1Te1.8Se0.2	Mo	1	Te	1.8	Se	0.2																		1	2017																										AB2																			1T'(nonpolar) phase	K	1.12						1.12	MTC157242																																																																	uV/K	23.4																													solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157243	PRB095100501		Mo(Te,Se)2	Mo1Te1.7Se0.3	Mo	1	Te	1.7	Se	0.3																		1	2017																										AB2																			1T'(nonpolar) phase	K	1.91						1.91																																																																		uV/K	12.8																													solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157244	PRB095100501	SP (beta) = 0.923 mJ/mol.K4	Mo(Te,Se)2	Mo1Te1.6Se0.4	Mo	1	Te	1.6	Se	0.4																		1	2017																										AB2																			1T'(nonpolar) phase	K	2.14						2.14																				T	RES(zero)													MHC157244																						mJ/mol.K2	3.7	SP	180	SP						uV/K	7.98			MTP157244																										solid state reaction in evacuated quartz tube					Anticorrelation between polar lattice instability and superconductivity in the Weyl semimetal candidate MoTe2			Department of Applied Physics and Quantum Phase Electronics Center (QPEC), University of Tokyo, Tokyo 113-8656, Japan	Phys.Rev.B, 95(2017)100501	H. Takahashi,T. Akiba,K. Imura,T. Shiino,K. Deguchi,N. K. Sato,H. Sakai,M. S. Bahramy,S. Ishiwata		
157245	PRB095100502	RRR = 15. energy gap measured by tunneling. Two gaps , large 5.70 meV (DB) and small 1.97 meV obtained from superfluid density analysis with penet = 239 nm.	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2017																										ABC4D4		CaRb1144																		K		35.8					35.8																																									A		2390			meV	5.7	3.76	1																																															FeAs-flux method					Nodeless multiband superconductivity in stoichiometric single-crystalline CaKFe4As4			Ames Laboratory, Ames and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 95(2017)100502	Kyuil Cho,A. Fente,S. Teknowijoyo,M. A. Tanatar,K. R. Joshi,N. M. Nusran,T. Kong,W. R. Meier,U. Kaluarachchi,I. Guillamon,H. Suderow,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
157246	PRB095100502	[penet] is average of two values obtained from Hc2 and Hc1	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2017																										ABC4D4		CaRb1144																		K		35.8					35.8																				T		71														A		21.5			A	average	1330																																																					FeAs-flux method					Nodeless multiband superconductivity in stoichiometric single-crystalline CaKFe4As4			Ames Laboratory, Ames and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 95(2017)100502	Kyuil Cho,A. Fente,S. Teknowijoyo,M. A. Tanatar,K. R. Joshi,N. M. Nusran,T. Kong,W. R. Meier,U. Kaluarachchi,I. Guillamon,H. Suderow,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
157247	PRB095115151	RRR=40. Tc, Hc2, T<FM> measured by thermal expansion <alpha>. Fig, shows Hc2-anisotropy. TCFIG shows pressure effect.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2017																										ABC		TiNiSi	Pnma																	K		0.53					0.53																				T	thermal expansion													MHC157247																																																														Tetra-arc furnace using Czochoralski method					Superconducting and ferromagnetic phase diagram of UCoGe probed by thermal expansion			Van der Waals?Zeeman Institute, University of Amsterdam, Science Park 904, NL-1098 XH Amsterdam, The Netherlands	Phys.Rev.B, 95(2017)115151	A. M. Nikitin,J. J. Geldhof,Y. K. Huang,D. Aoki,A. de Visser		
157248	PRB095115151	RRR=40. Tc, Hc2, T<FM> measured by thermal expansion <alpha>. Fig, shows Hc2- and T<FM>-anisotropy.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2017																										ABC		TiNiSi	Pnma																	K		0.53					0.53	MTC157248																			T	thermal expansion													MHC157248																																																														Tetra-arc furnace using Czochoralski method					Superconducting and ferromagnetic phase diagram of UCoGe probed by thermal expansion			Van der Waals?Zeeman Institute, University of Amsterdam, Science Park 904, NL-1098 XH Amsterdam, The Netherlands	Phys.Rev.B, 95(2017)115151	A. M. Nikitin,J. J. Geldhof,Y. K. Huang,D. Aoki,A. de Visser		
157249	PRB095125102	T<STR> = 53 K.(cubic to tetra). Two SC phases for 10.4 < P < 12.5 GPa by ac-SUS.  (dT<STR>/dP) = 2.5 K/GPa. Curie-Weiss for 230<T<700K.	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2017																										A3B7																			cubic(RT) to tetra(T<53 K)	K				2.3			2.3	MTC157249																																																																																															Sb self-flux method					Multiple superconducting states induced by pressure in Mo3Sb7			Okinawa Institute of Science and Technology Graduate University, Onna, Okinawa 904-0495, Japan	Phys.Rev.B, 95(2017)125102	Yejun Feng,Yishu Wang,A. Palmer,Ling Li,D. M. Silevitch,S. Calder,T. F. Rosenbaum		
157250	PRB095125102	P = 13.7 GPa. High-Tc phase	Mo3Sb7	Mo3Sb7	Mo	3	Sb	7																				3	2017																										A3B7																			cubic	K				6			6																																																																																																Sb self-flux method					Multiple superconducting states induced by pressure in Mo3Sb7			Okinawa Institute of Science and Technology Graduate University, Onna, Okinawa 904-0495, Japan	Phys.Rev.B, 95(2017)125102	Yejun Feng,Yishu Wang,A. Palmer,Ling Li,D. M. Silevitch,S. Calder,T. F. Rosenbaum		
157251	PRL112107002	SP (dC/gamma*Tc) = 1.62.  Pauli limit (1.83Tc) = 12.35 T. Energy gap: single isotropic s-wave SC from muon-SR.	Re6Zr	Re6Zr1	Re	6	Zr	1																				1	2014																										AB6		alpha-Mn	I4[-]3m	217																K				6.75			6.75											mT		8							T		12.2																										4.2	16				MSP157251			mJ/mol.K2	26	SP	319	SP																																		Zr(5N),Re(5N)		arc-melting. tetra-arc furnace					Detection of Time-Reversal Symmetry Breaking in the Noncentrosymmetric Superconductor Re6Zr Using Muon-Spin Spectroscopy			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.Lett., 112(2014)107002	R. P. Singh,A. D. Hillier,B. Mazidian,J. Quintanilla,J. F. Annett,D. McK. Paul,G. Balakrishnan,M. R. Lees		
157252	PRL115267001	muon-SR measurement. m*/me = 139, SC-carrier density = 0.169E+28 /m3	La7Ir3	Ir3La7	Ir	3	La	7																				1	2015																										A3B7			P6<3>mc		A	10.2376		6.4692												K				2.25			2.25																																									nm	muon-SR, s-wave fitting	482			meV	0.369	3.81	16							mJ/mol.K2	47	SP																																				La(3N),Ir(4N)		arc melting. For muon-SR, sample was ground to powder in high purity Ar - sealed in evacuated quartz tube					Unconventional Superconductivity in La7Ir3 Revealed by Muon Spin Relaxation: Introducing a New Family of Noncentrosymmetric Superconductor That Breaks Time-Reversal Symmetry			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.Lett., 115(2015)267001	J. A. T. Barker,D. Singh,A. Thamizhavel,A. D. Hillier,M. R. Lees,G. Balakrishnan,D. McK. Paul,R. P. Singh		
157253	PRL117277001	SC gap: (gap(meV), gap size) = (10.5, 7.4), (13, 9.1), (8, 5.6), (12, 8.4) for alpha-sheet, beta-hole, gamma-sheet, delta-sheet in Fermi surface, respectively. Largest (beta) in DB	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2016																										ABC4D4		CaRb1144																		K		35					35																																														meV	13	9.1	16																																															flux method					Enhancement of the Superconducting Gap by Nesting in CaKFe4As4: A New High Temperature Superconductor			Division of Materials Science and Engineering, Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.Lett., 117(2016)277001	Daixiang Mou,Tai Kong,William R. Meier,Felix Lochner,Lin-Lin Wang,Qisheng Lin,Yun Wu,S. L. Bud'ko,Ilya Eremin,D. D. Johnson,P. C. Canfield,Adam Kaminski		
157254	PRL118107002	T<STR> = 177K. Strain induced by gluind to glass substrate. The strain size not clear (See text). For strain free sample, T<STR> = 166 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																			2017																										AB2C2		ThCr2Si2																		K					0																																																																																																		FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157255	PRL118107002	T<STR> = 123 K. Strain induced by gluind to glass substrate. The strain size not clear (See text). For strain free sample, T<STR> = 76.6 K.	Ca(Fe,Co)2As2	Ca1Fe1.948Co0.052As2	Ca	1	Fe	1.948	Co	0.052	As	2																	2017																										AB2C2		ThCr2Si2																		K					0																																																																																																		FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157256	PRL118107002	T<STR> = 118 K. Strain induced by gluind to glass substrate. The strain size not clear (See text).  Tc = 15.1K due to strain free phase fraction in the strained sample.	Ca(Fe,Co)2As2	Ca1Fe1.94Co0.06As2	Ca	1	Fe	1.94	Co	0.06	As	2																	2017																										AB2C2		ThCr2Si2																		K				15.1			15.1																																																																																																FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157257	PRL118107002	T<STR> = 102 K. Strain induced by gluind to glass substrate. The strain size not clear (See text).  Tc = 17.4 K due to strain free phase fraction in the strained sample.	Ca(Fe,Co)2As2	Ca1Fe1.93Co0.07As2	Ca	1	Fe	1.93	Co	0.07	As	2																	2017																										AB2C2		ThCr2Si2																		K				17.4			17.4																																																																																																FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157258	PRL118107002	T<STR> = 98.8 K. Strain induced by gluind to glass substrate. The strain size not clear (See.text). For strain free sample, Tc = 12.1 K.	Ca(Fe,Co)2As2	Ca1Fe1.926Co0.074As2	Ca	1	Fe	1.926	Co	0.074	As	2																	2017																										AB2C2		ThCr2Si2																		K				16.9			16.9																																																																																																FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157259	PRL118107002	Strain induced by gluind to glass substrate. The strain size not clear (See text).  For strain free sample, Tc = 6.88  K.	Ca(Fe,Co)2As2	Ca1Fe1.902Co0.098As2	Ca	1	Fe	1.902	Co	0.098	As	2																	2017																										AB2C2		ThCr2Si2																		K				15.8			15.8																																																																																																FeAs flux method. ANN(400C). To create strain, samples were glued with epoxy to thin(160 um) borosilicate glass					Effect of Biaxial Strain on the Phase Transitions of CadFe1-xCoxT2As2			Ames Laboratory, US DOE, Ames, Iowa 50011, USA	Phys.Rev.Lett., 118(2017)107002	A. E. Bohmer,A. Sapkota,A. Kreyssig,S. L. Bud'ko,G. Drachuck,S. M. Saunders,A. I. Goldman,P. C. Canfield		
157260	SCIB0620857	P-induced SC. P<cr> = 2.88 GPa, Tc (onset) = 26.02 K at P<cr>. Tn = 53.6 K and T<STR> = 57.1 K are at P = 1 bar.	(Ca,La)FeAs2	Ca0.73La0.27Fe1As2	Ca	0.73	La	0.27	Fe	1	As	2																3	2017								53.6																		ABC2		Fe-112																		K					0			MPH157260																																																																																															Flux method					Observation of a bi-critical point between antiferromagnetic and superconducting phases in pressurized single crystal Ca0.73La0.27FeAs2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 62(2017)857	Yazhou Zhou,Shan Jiang,Qi Wu,Vladimir A. Sidorov,Jing Guo,Wei Yi,Shan Zhang,Zhe Wang,Honghong Wang,Shu Cai,Ke Yang,Sheng Jiang,Aiguo Li,Ni Ni,Guangming Zhang,Liling Sun,Zhongxian Zhao		
157261	SCIB0620857	P = 4.95 GPa	(Ca,La)FeAs2	Ca0.73La0.27Fe1As2	Ca	0.73	La	0.27	Fe	1	As	2																3	2017																										ABC2		Fe-112																		K	21		29.1		0		25.05																				T	RES(on)				8			25.6																																																																				Flux method					Observation of a bi-critical point between antiferromagnetic and superconducting phases in pressurized single crystal Ca0.73La0.27FeAs2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Bull., 62(2017)857	Yazhou Zhou,Shan Jiang,Qi Wu,Vladimir A. Sidorov,Jing Guo,Wei Yi,Shan Zhang,Zhe Wang,Honghong Wang,Shu Cai,Ke Yang,Sheng Jiang,Aiguo Li,Ni Ni,Guangming Zhang,Liling Sun,Zhongxian Zhao		
157262	SCIR0045709	Carrier = 4.9E+25 /m3, hole mobility = 300cm2/Vs at Tc.  SP (beta) = 1.0 mJ/mol.k2, (delta) = 0.36 mJ/mol.K6. Energy gap from SP using modified BCS	LuPdBi	Lu1Pd1Bi1	Lu	1	Pd	1	Bi	1																		3	2014																										ABC		MgAgAs			A	6.63													MgAgAs-type	K			1.7				1.7																				T	RES(on), GL fitting	2.2												MHC157262		A	from Hc2	120								meV	0.32	5.2	14							mJ/mol.K2	11.9	SP	295	SP											mOhm.cm							0.42														n/m3	100000000000000000000000000								Weak Antilocalization Effect and Noncentrosymmetric Superconductivity in a Topologically Nontrivial Semimetal LuPdBi			State Key Laboratory for Magnetism, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Sci.Rep., 4(2014)5709	Guizhou Xu,Wenhong Wang,Xiaoming  Zhang,Yin Du,Enke Liu,Shouguo Wang,Guangheng Wu,Zhongyuan Liu,Xi Xiang Zhang		
157263	SST021125014	not SC. T<SDW> = T<STR> = 135 K	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2008																										AB2C2		ThCr2Si2			A															K					0																																																																																																FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157264	SST021125014	not SC. compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.94K0.06Fe2As2	Ba	0.94	K	0.06	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.065												K					0																																																																																																FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157265	SST021125014	not SC. compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.92K0.08Fe2As2	Ba	0.92	K	0.08	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.077												K					0																																																																																																FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157267	SST021125014	compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.77K0.23Fe2As2	Ba	0.77	K	0.23	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.189												K			24.5	23.4		0.4	23.4																																																																																														FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157268	SST021125014	compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.75K0.25Fe2As2	Ba	0.75	K	0.25	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.196												K			28.7	27.5		0.71	27.5																																																																																														FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157269	SST021125014	compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.72K0.28Fe2As2	Ba	0.72	K	0.28	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.226												K			31.4	31.8		0.49	31.8																																																																																														FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157270	SST021125014	compositions by EDX, cleaved sample	(Ba,K)Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2008																										AB2C2		ThCr2Si2			A			13.344												K			36.6	36.3		0.44	36.3																																																																																														FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157271	SST021125014	not SC. T<SDW> = T<STR> = 173 K	SrFe2As2	Sr1Fe2As2	Sr	1	Fe	2	As	2																		3	2008																										AB2C2		ThCr2Si2			A			12.58												K					0																																																																																																FeAs,Ba,K		FeAs self-flux method. mixture - sealed in alumina crucible - sealed in quartz tube in muffle furnace - heat(1000-1150 C) - cool to 800 C(<10 C/h) - FC to RT					Growth and characterization of A1-xKxFe2As2 (A = Ba, Sr) single crystals with x = 0-0.4			National Laboratory for Superconductivity, Institute of Physics and National Laboratory for Condensed Matter Physics, PO Box 603, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 21(2008)125014	Huiqian Luo,Zhaosheng Wang,Huan Yang,Peng  Cheng,Xiyu Zhu,Hai-Hu Wen		
157272	SST028115010	Impurity phases: Bi2S3, EuF2.4. R not to zero at 2.0 K. Semicon-like down to Tc.	(Eu,La)BiS2F	Eu0.5La0.5F1Bi1S2	Eu	0.5	La	0.5	F	1	Bi	1	S	2														1	2015																										ABCD2		CeOBiS2	P4/nmm	129	A	4.0744		13.3336												K			2.2				2.2	MTC157272																			T	RES(on), WHH	10												MHC157272																																																												EuF3,La2S3,Bi2S3,Eu		mixture - sealed in quartz tube - heat(800C,24h) - reground - pellet - heat(800C,24h)					Pressure enhanced superconductivity at 10K in La doped EuBiS2F			Department of Chemistry, Indian Institute of Technology, New Delhi110016, India	Supercond.Sci.Technol., 28(2015)115010	Gohil S Thakur,Rajveer Jha,Zeba Haque,V P S Awana,L C Gupta,A K Ganguli		
157273	PRB095134517	RRR = 47.5. n = 4.56, A = 0.248 uOhm.cm/K in R(T) = R0 + A*T^n	PrPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2017					My-B/mol	3.64	-20.8																			AB4C12		skutterudite	Im3[-]		A	8.6205														K		8.13		7.8			8.13																																																								mJ/mol.K2	43	SP	191.6	SP											uOhm.cm							2.31																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157274	PRB095134517	RRR = 25.0. n = 4.19 , A = 0.097 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.95Eu0.05Pt4Ge12	Pr	0.95	Eu	0.05	Pt	4	Ge	12																1	2017					My-B/mol	4.16	-19.6																			AB4C12		skutterudite	Im3[-]		A	8.6219														K		7.78		7.7			7.78																																																								mJ/mol.K2	45.6	SP	194.6	SP											uOhm.cm							2.89																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157275	PRB095134517	RRR = 14.8. n = 4.74 , A = 0.248 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.9Eu0.1Pt4Ge12	Pr	0.9	Eu	0.1	Pt	4	Ge	12																1	2017					My-B/mol	4.29	-14.2																			AB4C12		skutterudite	Im3[-]		A	8.623														K		7.62		7.6			7.62	MPH157275																																																							mJ/mol.K2	43.7	SP	193.2	SP											uOhm.cm							8.39																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157276	PRB095134517	RRR = 11.4. n = 3.90 , A = 0.248 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.85Eu0.15Pt4Ge12	Pr	0.85	Eu	0.15	Pt	4	Ge	12																1	2017					My-B/mol	4.6	-14.7																			AB4C12		skutterudite	Im3[-]		A	8.6236														K		7.28		7.01			7.28																																																								mJ/mol.K2	51.4	SP	193.7	SP											uOhm.cm							14.3																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157277	PRB095134517	RRR = 9.32. n = 3.32 , A = 0.248 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.8Eu0.2Pt4Ge12	Pr	0.8	Eu	0.2	Pt	4	Ge	12																1	2017					My-B/mol	4.86	-12.6																			AB4C12		skutterudite	Im3[-]		A	8.6271														K		6.54		6.52			6.54																																																								mJ/mol.K2	52.3	SP	196.9	SP											uOhm.cm							12.03																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157278	PRB095134517	RRR = 9.06. n =3.07  , A = 0.248 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.7Eu0.3Pt4Ge12	Pr	0.7	Eu	0.3	Pt	4	Ge	12																1	2017					My-B/mol	5.17	-11.5																			AB4C12		skutterudite	Im3[-]		A	8.6275														K		5.28		4.9			5.28																																																								mJ/mol.K2	53.2	SP	199.3	SP											uOhm.cm							9.05																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157279	PRB095134517	RRR = 6.02 . n =2.46  , A = 1.074 uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.62Eu0.38Pt4Ge12	Pr	0.62	Eu	0.38	Pt	4	Ge	12																1	2017					My-B/mol	5.55	-9	0.58																		AB4C12		skutterudite	Im3[-]		A	8.6334														K		5.12		4.5			5.12																																																								mJ/mol.K2	65.7	SP	199.4	SP											uOhm.cm							15.1																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157280	PRB095134517	RRR =6.33 . n = 2.74 , A =0.602  uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.55Eu0.45Pt4Ge12	Pr	0.55	Eu	0.45	Pt	4	Ge	12																1	2017					My-B/mol	5.57	-9.2																			AB4C12		skutterudite	Im3[-]		A	8.6356														K		2.72		2.98			2.72																																																								mJ/mol.K2	61.7	SP	204.1	SP											uOhm.cm							18.2																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157281	PRB095134517	RRR = 5.14. n = 2.64 , A = 0.753  uOhm.cm/K in R(T) = R0 + A*T^n	(Pr,Eu)Pt4Ge12	Pr0.5Eu0.5Pt4Ge12	Pr	0.5	Eu	0.5	Pt	4	Ge	12																1	2017					My-B/mol	6.03	-8.9	0.78																		AB4C12		skutterudite	Im3[-]		A	8.6374														K		2.12					2.12																																																								mJ/mol.K2	74.9	SP	200.6	SP											uOhm.cm							17.03																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157282	PRB095134517	RRR = 5.70 . n =1.04 (2.59)  , A = 13.5  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	(Pr,Eu)Pt4Ge12	Pr0.4Eu0.6Pt4Ge12	Pr	0.4	Eu	0.6	Pt	4	Ge	12																1	2017					My-B/mol	6.31	-10.9																			AB4C12		skutterudite	Im3[-]		A	8.6379														K					2																																																										mJ/mol.K2	99.8	SP	205.4	SP											uOhm.cm							14.47																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157283	PRB095134517	RRR = 5.22. n = 1.39 (2.64) , A = 9.27  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	(Pr,Eu)Pt4Ge12	Pr0.3Eu0.7Pt4Ge12	Pr	0.3	Eu	0.7	Pt	4	Ge	12																1	2017					My-B/mol	6.74	-10.6	1																		AB4C12		skutterudite	Im3[-]		A	8.6405														K					2																																																										mJ/mol.K2	124.9	SP	203.8	SP											uOhm.cm							14.43																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157284	PRB095134517	RRR = 4.80. n = 0.79(2.51) , A = 27.6  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	(Pr,Eu)Pt4Ge12	Pr0.2Eu0.8Pt4Ge12	Pr	0.2	Eu	0.8	Pt	4	Ge	12																1	2017					My-B/mol	6.9	-11.9	1.19																		AB4C12		skutterudite	Im3[-]		A	8.6435														K					2			MPH157275																																																							mJ/mol.K2	123.6	SP	206.3	SP											uOhm.cm							11.42																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157285	PRB095134517	RRR = 8.28 . n =0.88 (3.03  , A = 9.78  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	(Pr,Eu)Pt4Ge12	Pr0.1Eu0.9Pt4Ge12	Pr	0.1	Eu	0.9	Pt	4	Ge	12																1	2017					My-B/mol	7.23	-14.2	1.58																		AB4C12		skutterudite	Im3[-]		A	8.644														K					2																																																										mJ/mol.K2	132.1	SP	211.1	SP											uOhm.cm							6.33																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157286	PRB095134517	RRR = 8.65 . n = 0.90 (2.68) , A = 16.8  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	(Pr,Eu)Pt4Ge12	Pr0.05Eu0.95Pt4Ge12	Pr	0.05	Eu	0.95	Pt	4	Ge	12																1	2017					My-B/mol	7.43	-14.5	1.63																		AB4C12		skutterudite	Im3[-]		A	8.6459														K					2																																																																									uOhm.cm							7.77																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157287	PRB095134517	RRR = 13.3. n = 0.96 (2.22) , A = 29.8  uOhm.cm/K in R(T) = R0 + A*T^n. () for T > T* where kink temperature in R(T).	EuPt4Ge12	Eu1Pt4Ge12	Eu	1	Pt	4	Ge	12																		1	2017					My-B/mol	7.9	-16.3	1.73																		AB4C12		skutterudite	Im3[-]		A	8.6489														K					2																																																										mJ/mol.K2	225.1	SP	219.4	SP											uOhm.cm							5.14																Pr(3N),Eu(3N),Pt(3N5),Ge(6N)		arc-melting - ANN					Crossover and coexistence of superconductivity and antiferromagnetism in the filled-skutterudite system Pr1-xEuxPt4Ge12			Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 95(2017)134517	I. Jeon,S. Ran,A. J. Breindel,P.-C. Ho,R. B. Adhikari,C. C. Almasan,B. Luong,M. B. Maple		
157288	PRB095140505	s + s wave two gap model gives best fitting. gap = 8.6 meV ( in DB) and  2.5 meV (2d/kTc) = 1.69	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																1	2017																										ABC4D4		CaRb1144																		K		34.3					34.3																																									nm	muon-SR	289			meV	8.6	5.83	16																																															Poly crystals synthesized using the stainless steel pipe and cap method					Signature of multigap nodeless superconductivity in CaKFe4As4			ISIS Pulsed Neutron and Muon Source, STFC Rutherford Appleton Laboratory, Harwell Campus, Didcot, Oxfordshire OX11 0QX, United Kingdom	Phys.Rev.B, 95(2017)140505	P. K. Biswas,A. Iyo,Y. Yoshida,H. Eisaki,K. Kawashima,A. D. Hillier		
157289	PRB095144505	not bulk SC.	Cu0.3ZrTe2	Cu0.3Zr1Te2	Cu	0.3	Zr	1	Te	2																		1	2017																												CdI2	P3[-]ml		A	3.959		6.656												K			10				10																																																																																														high purity powder of Zr,Cu,Te		mixture - pellet - in quartz tube(Ar) - heat(850C,48h) - reground - pellet - in quartz tube - heat(1000C,48h) - Q to ice water					Evidence for topological behavior in superconducting CuxZrTe2-y			Universidade de Sao Paulo Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 95(2017)144505	A. J. S. Machado,N. P. Baptista,B. S. de Lima,N. Chaia,T. W. Grant,L. E. Correa,S. T. Renosto,A. C. Scaramussa,R. F. Jardim,M. S. Torikachvili,J. Albino Aguiar,O. C. Cigarroa,L. T. F. Eleno,Z. Fisk		
157290	PRB095144505	Tc is completely insensitive to pressure for P < 1.3 GPa. n-type carrier	Cu0.3ZrTe1.2	Cu0.3Zr1Te1.2	Cu	0.3	Zr	1	Te	1.2																		1	2017																												CdI2	P3[-]ml																	K	8.43	9.07	9.7	9.7		1.2	9.07											Oe	M-H curve				11			2	T	RES(on)				0.9			2.4						MHC157290							um	London	0.5																							uV/K	-13.5			MTP157290	mOhm.cm							1.52												6		n/cm3	8100000000000000000	high purity powder of Zr,Cu,Te		mixture - pellet - in quartz tube(Ar) - heat(850C,48h) - reground - pellet - in quartz tube - heat(1000C,48h) - Q to ice water					Evidence for topological behavior in superconducting CuxZrTe2-y			Universidade de Sao Paulo Escola de Engenharia de Lorena, Lorena, Brazil	Phys.Rev.B, 95(2017)144505	A. J. S. Machado,N. P. Baptista,B. S. de Lima,N. Chaia,T. W. Grant,L. E. Correa,S. T. Renosto,A. C. Scaramussa,R. F. Jardim,M. S. Torikachvili,J. Albino Aguiar,O. C. Cigarroa,L. T. F. Eleno,Z. Fisk		
157291	PRB095174521	Tc(SP) = 3.5 K. Hc(0) = 70 mT from Hc1/Hc2. Lattice term in SP (beta) = 0.173 mJ/mol.K4. (dC/gamma*Tc) = 1.55. e-ph = 0.56. kappa(GL) = 20. Hc2(0) = 1.95 T from Hc2=Hc2(0)(1-t^1.5)^1.5	TaIr2Ge2	Ta1Ir2Ge2	Ta	1	Ir	2	Ge	2																		1	2017																										AB2C2		CaBe2Ge2	Pnnm	58	A	8.515	12.553	2.9247											Samples decompose to TaIrGe and TaIr3 by ANN(1000-1450,30min-2days)	K		3.9					3.9											Oe	M-H curve	72							T	RES(0.5Rn)	1.95			1			2.02	T/K	SP(mid)	0.6			MHC157291		nm	from Hc2	13			nm	from Hc1	262										MSP157291			mJ/mol.K2	11	SP	355	SP																																		Ta(3N5),Ir(3N5),Ge(6N)		arc-melting. pellet(Ir,Ge) - arc-melt firstly, then with Ta foil. Annealed below 1150C in quartz tube and in Ar-backfilled induction furnace (1150-1450C)					Superconductivity in a new intermetallic structure type based on endohedral Ta@Ir7Ge4 clusters			Department of Chemistry, Princeton University, Princeton New Jersey 08544, USA	Phys.Rev.B, 95(2017)174521	Laura C. Srivichitranond,Elizabeth M. Seibel,Weiwei Xie,Zuzanna Sobczak,Tomasz Klimczuk,R. J. Cava		
157292	NATCOM0055657	x = 0.33 - 0.36 in BaFe(2As1-xPx)2. Tc=28 K sample.  e-irradiation effect investigated by TDO measurements. e-dose = 2.0 C/cm2. Value of penetration depth not given.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																	2014																										AB2C2		ThCr2Si2																		K			24.6				24.6																																																1.1																																																					Disorder-induced topological change of the superconducting gap structure in iron pnictides			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan.	Nat.Cmmun., 5(2014)5657	Y. Mizukami,M. Konczykowski,Y. Kawamoto,S. Kurata,S. Kasahara,K. Hashimoto,V. Mishra,A. Kreisel,Y. Wang,P.J. Hirschfeld,Y. Matsuda,T. Shibauchi		
157293	NATCOM0055657	x = 0.33 - 0.36 in BaFe(2As1-xPx)2.Tc = 29 K sampl.   e-irradiation effect investigated by TDO measurements. e-dose = 2.7 C/cm2. Value of penetration depth not given.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																	2014																										AB2C2		ThCr2Si2																		K			23.2				23.2																																																1.3																																																					Disorder-induced topological change of the superconducting gap structure in iron pnictides			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan.	Nat.Cmmun., 5(2014)5657	Y. Mizukami,M. Konczykowski,Y. Kawamoto,S. Kurata,S. Kasahara,K. Hashimoto,V. Mishra,A. Kreisel,Y. Wang,P.J. Hirschfeld,Y. Matsuda,T. Shibauchi		
157294	NATCOM0055657	x = 0.33 - 0.36 in BaFe(2As1-xPx)2.Tc = 30 K sample.  e-irradiation effect investigated by TDO measurements. TCFIG shows Tc vs e-dose. Value of penetration depth not given.	BaFe2(As,P)2	Ba1Fe2As1.34P0.66	Ba	1	Fe	2	As	1.34	P	0.66																	2014																										AB2C2		ThCr2Si2																		K			30				30	MTC157294																																																																																																				Disorder-induced topological change of the superconducting gap structure in iron pnictides			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan.	Nat.Cmmun., 5(2014)5657	Y. Mizukami,M. Konczykowski,Y. Kawamoto,S. Kurata,S. Kasahara,K. Hashimoto,V. Mishra,A. Kreisel,Y. Wang,P.J. Hirschfeld,Y. Matsuda,T. Shibauchi		
157295	AIPC8500535	Li-intercalated sample. SC-volume fraction = 2% at 2 K, independent of Li-content.	LixSr2CuO2I2	Li0.25Sr2Cu1I2O2	Li	0.25	Sr	2	Cu	1	I	2													O	2			2006																												T																	K2NiF4-type	K				4.5			4.5										2																																																																																						electrochemical Li-intercalation carried out at RT using three-electrode cell. with constant potencial of 500 mV (vs Li/Li+) using potentiostat					Synthesis of New Electron-Doped Cuprates LixSr2CuO2X2 (X= Cl, Br, I)			Department of Applied Physics, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	AIP conf. Proc., 850(2006)0535	Tetsuya Kajita,Masatsune Kato,Takashi Noji,Yoji Koike		
157296	AIPC8500535		LixSr2CuO2Br2	Li0.15Sr2Cu1Br2O2	Li	0.15	Sr	2	Cu	1	Br	2													O	2			2006																												T																	K2NiF4-type	K				8			8																																																																																																electrochemical Li-intercalation carried out at RT using three-electrode cell. with constant potencial of 500 mV (vs Li/Li+) using potentiostat					Synthesis of New Electron-Doped Cuprates LixSr2CuO2X2 (X= Cl, Br, I)			Department of Applied Physics, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	AIP conf. Proc., 850(2006)0535	Tetsuya Kajita,Masatsune Kato,Takashi Noji,Yoji Koike		
157297	JPS081125002	bulk SC observed in SP measurements. SP (beta) = 3.0 mJ/mol.K4.	Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2012																																													BiS2-layer	K	4.4			4.7			4.7																																																								mJ/mol.K2	2.8	SP	192	SP											mOhm.cm							0.8																		solid state reaction					Bulk Superconductivity in Bi4O4S3 Revealed by Specific Heat Measurement			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo, Japan	J.Phys.Soc.Jpn, 81(2012)125002	Hiroshi Takatsu,Yoshikazu Mizoguchi,Hiroki Izawa,Osuke Mura,Hiroaki Kadowaki		
157298	PRB095144502	Tc from R(T) graph. N(0) calculated from SP{gamma} data, which in not given.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2017																										ABC2		CeNiC2																		K	2.92						2.92																																																																																														La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157299	PRB095144502	Tc from R(T) graph.  N(0) calculated from SP{gamma} data, which in not given.	(La,Ce)NiC2	La0.995Ce0.005Ni1C2	La	0.995	Ce	0.005	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K	2.41						2.41	MTC157299																																																				MDOS157299																																									La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157300	PRB095144502	Tc from Tc/Tc0 vs x graph using Tc0 = 2.92 K.N(0) calculated from SP{gamma} data, which in not given.	(La,Ce)NiC2	La0.99Ce0.01Ni1C2	La	0.99	Ce	0.01	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K	2						2																																																																																														La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157301	PRB095144502	Tc from R(T) graph.  N(0) calculated from SP{gamma} data, which in not given.	(La,Ce)NiC2	La0.985Ce0.015Ni1C2	La	0.985	Ce	0.015	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K	1.4						1.4																																																																																														La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157302	PRB095144502	R(T) not to zero at 0.4 K. Tc obtained from extrapolation to R=0.  N(0) calculated from SP{gamma} data, which in not given.	(La,Ce)NiC2	La0.98Ce0.02Ni1C2	La	0.98	Ce	0.02	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K	0.1						0.1																																																																																														La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157303	PRB095144502	not SC. x<cr> for SC = 0.022 in La1-xCexNiC2. N(0) calculated from SP{gamma} data, which in not given.	(La,Ce)NiC2	La0.975Ce0.025Ni1C2	La	0.975	Ce	0.025	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K					0.4																																																																																																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting, several times					Magnetic impurity effects on the superconductivity of noncentrosymmetric LaNiC2: Ce substitution for La			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 95(2017)144502	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Yohei Matsubara		
157400	ADV0262346	P-induced SC. Tc(max) in DB at P = 4.1 GPa. T' (semicon-transition) and Tn (AFM) obtained by R(T) measurements in TC-FIG.	Ca10(Pt3As8)(Fe1.996Pt0.004As2)5	Ca10Pt3.02As18Fe9.98	Ca	10	Pt	3.02	As	18	Fe	9.98																3	2014								90																																					Ca-10-3-8 phase	K			8.4	7.62	0		7.62	MTC157400																																																																																				cm3/C						MRH157400					single crystals grown by flux method					Pressure-Induced Superconductivity and Its Scaling with Doping-Induced Superconductivity in the Iron Pnictide with Skutterudite Intermediary Layers			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics Chinese Academy of Sciences Beijing 100190 , China	Adv.Mater., 26(2014)2346	Peiwen Gao,Liling Sun,Ni Ni,Jing Guo,Qi Wu,Chao Zhang,Dachun Gu,Ke Yang,Aiguo Li,Sheng Jiang,Robert Joseph Cava,Zhongxian Zhao		
157401	AIPC8500535	Li-intercalated (electron doped cuprates). SC volume nearly 2% independent of Li-content.	Li0.25Sr2CuO2I2	Li0.25Sr2Cu1I2O2	Li	0.25	Sr	2	Cu	1	I	2													O	2			2006																																													K2NiF4 structure	K				4.5			4.5										2																																																																																						(SrCuO2 + SrI2) - pellet - SIN(580 C, 24h) - Sr2CuO2I2. Li-intercalation using three electrode cell. 1.0M-LiClO4 dissolved in PC is used as electrolyte.					Synthesis of New Electron-Doped Cuprates LixSr2CuO2X2 (X= Cl, Br, I)			Department of Applied Physics, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	AIP conf. Proc., 850(2006)0535	Tetsuya Kajita,Masatsune Kato,Takashi Noji,Yoji Koike		
157402	AIPC8500535	Li-intercalated (electron doped cuprates).	Li0.15Sr2CuO2Br2	Li0.15Sr2Cu1Br2O2	Li	0.15	Sr	2	Cu	1	Br	2													O	2			2006																																													K2NiF4 structure	K				8			8																																																																																																(SrCuO2 + SrI2) - pellet - SIN(580 C, 24h) - Sr2CuO2I2. Li-intercalation using three electrode cell. 1.0M-LiClO4 dissolved in PC is used as electrolyte.					Synthesis of New Electron-Doped Cuprates LixSr2CuO2X2 (X= Cl, Br, I)			Department of Applied Physics, Tohoku University, 6-6-05 Aoba, Aramaki, Aoba-ku, Sendai 980-8579, Japan	AIP conf. Proc., 850(2006)0535	Tetsuya Kajita,Masatsune Kato,Takashi Noji,Yoji Koike		
157403	APL108162601	T<STR> = 240 K (Td - 1T'). R(min) = 8 K. R(T) = R0 +A*T2 for T < 50 K, R0=0.136 mOhm.cm, A=0.00238 uOhm.cm. SP (beta) = 0.635 mJ/mol.K4, e-ph = 0.49	MoTe1.8S0.2	Mo1Te1.8S0.2	Mo	1	Te	1.8	S	0.2																			2016																										AB2			Pmn2<1>																Td phase	K	1.3						1.3	MTC157403									60																																														mJ/mol.K2	2.07	SP	143	SP											mOhm.cm	0.136																													Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157404	APL108162601	SP (beta) = 0.758 mJ/mol.K4, e-ph = 0.32	MoTe2	Mo1Te2	Mo	1	Te	2																					2016																										AB2																			Td phase	K	0.1						0.1																																																								mJ/mol.K2	3.06	SP	135	SP																																									Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157405	APL108162601	T<STR> = 295 K	Mo(Te,S)2	Mo1Te1.88S0.12	Mo	1	Te	1.88	S	0.12																			2016																										AB2																			Td phase	K	0.832						0.832																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157406	APL108162601	T<STR> = 230 K	Mo(Te,S)2	Mo1Te1.84S0.16	Mo	1	Te	1.84	S	0.16																			2016																										AB2																			Td phase	K	0.893						0.893																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157407	APL108162601	R(min) = 3.86 K.	Mo(Te,S)2	Mo1Te1.82S0.18	Mo	1	Te	1.82	S	0.18																			2016																										AB2																			Td phase	K	0.981						0.981																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157408	APL108162601	R(min) = 11.9 K.	Mo(Te,S)2	Mo1Te1.78S0.22	Mo	1	Te	1.78	S	0.22																			2016																										AB2																			Td phase	K	1.143						1.143																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157409	APL108162601	R(min) = 31.4 K.	Mo(Te,S)2	Mo1Te1.72S0.28	Mo	1	Te	1.72	S	0.28																			2016																										AB2																			Td phase	K	0.736						0.736																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157410	APL108162601	R(min) = 28.3 K.	Mo(Te,S)2	Mo1Te1.63S0.37	Mo	1	Te	1.63	S	0.37																			2016																										AB2																			Td phase	K	0.04						0.04																																																																																																					Superconductivity enhancement in the S-doped Weyl semimetal candidate MoTe2			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, China	Appl.Phys.Lett., 108(2016)162601	F. C. Chen,X. Luo,R. C. Xiao,W. J. Lu,B. Zhang,H. X. Yang,J. Q. Li,Q. L. Pei,D. F. Shao,R. R. Zhang,L. S. Ling,C. Y. Xi,W. H. Song,Y. P. Sun		
157411	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.1M0.05Mo1S2	Ca	0.1	M	0.05	Mo	1	S	2																	2018																										AB2					A	3.186		18.51												K				6.31			6.31																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157412	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.15M0.15Mo1S2	Ca	0.15	M	0.15	Mo	1	S	2																	2018																										AB2					A	3.184		18.512												K				7.53			7.53																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157413	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.2M0.17Mo1S2	Ca	0.2	M	0.17	Mo	1	S	2																	2018																										AB2					A	3.191		18.518												K				8.55			8.55	MTC157413																			T	SUS, GL theory	0.098												MHC157413		nm	from Hc2	58																																																								Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157414	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.25M0.2Mo1S2	Ca	0.25	M	0.2	Mo	1	S	2																	2018																										AB2					A	3.188		18.517												K				5.75			5.75																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157415	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.3M0.31Mo1S2	Ca	0.3	M	0.31	Mo	1	S	2																	2018																										AB2					A	3.186		18.526												K				5.37			5.37																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157416	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.35M0.33Mo1S2	Ca	0.35	M	0.33	Mo	1	S	2																	2018																										AB2					A	3.19		18.522												K				5.12			5.12																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157417	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.4M0.41Mo1S2	Ca	0.4	M	0.41	Mo	1	S	2																	2018																										AB2					A	3.194		18.523												K				0	2		0																																																																																														Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157418	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.45M0.38Mo1S2	Ca	0.45	M	0.38	Mo	1	S	2																	2018																										AB2					A	3.193		18.527												K					2																																																																																																Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157419	CEM2580131	M = NH3, M-content measured therm gravimetric method	Cax(NH3)yMoS2	Ca0.5M0.4Mo1S2	Ca	0.5	M	0.4	Mo	1	S	2																	2018																										AB2			P-3m1		A	3.198		18.543												K					2																																																																																																Ca(2N5),MoS2,NH3(5N)		Ca-intercalation using low temperature reaction bath (213K, 3days), using high purity ammonia(99.999%)					Synthesis, crystal structure and superconducting properties of calcium intercalates of MoS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Solid State Chem., 258(2018)131	Menghu Zhou,Xiaochuan Li,Lihong Yang,Cheng Dong		
157420	CEM2520106		SnAs	As1Sn1	As	1	Sn	1																				1	2017																										AB		NaCl			A	5.722														K				3.8			3.8											Oe	M-H curve				70			2																																																																											Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157421	CEM2520106		SnAs1-xSex	Sn1As0.99Se0.01	Sn	1	As	0.99	Se	0.01																		1	2017																										AB		NaCl			A	5.725														K			3.9	3.8		0.15	3.8											Oe	M-H curve				80			2	Oe	RES(0.9Rn),WHH	294							Oe/K	RES(0.9Rn)	109																																								uOhm.cm							3.03																Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157422	CEM2520106		SnAs1-xSex	Sn1As0.97Se0.03	Sn	1	As	0.97	Se	0.03																		1	2017																										AB		NaCl			A	5.727														K				4			4											Oe	M-H curve				110			2																																																																											Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157423	CEM2520106		SnAs1-xSex	Sn1As0.95Se0.05	Sn	1	As	0.95	Se	0.05																		1	2017																										AB		NaCl			A	5.729														K			4.3	4.3		0.22	4.3											Oe	M-H curve				70			2	Oe	RES(0.9Rn),WHH	649							Oe/K	RES(0.9Rn)	217																																								uOhm.cm							3.53																Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157424	CEM2520106		SnAs1-xSex	Sn1As0.93Se0.07	Sn	1	As	0.93	Se	0.07																		1	2017																										AB		NaCl			A	5.732														K				4.3			4.3											Oe	M-H curve				90			2																																																																											Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157425	CEM2520106		SnAs1-xSex	Sn1As0.9Se0.1	Sn	1	As	0.9	Se	0.1																		1	2017																										AB		NaCl			A	5.734														K			4.5	4.5		0.23	4.5											Oe	M-H curve				80			2	Oe	RES(0.9Rn),WHH	1011							Oe/K	RES(0.9Rn)	328																																								uOhm.cm							19.55																Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157426	CEM2520106		SnAs1-xSex	Sn1As0.87Se0.13	Sn	1	As	0.87	Se	0.13																		1	2017																										AB		NaCl			A	5.729														K				4.4			4.4											Oe	M-H curve				115			2																																																																											Sn,As,Se		mixture - in silica tube - heat(973 K,10h) - FC to RT					Selenium doping NaCl-type superconductor: SnAs1-xSex (x = 0-0.13)			State Key Laboratory of High Performance Ceramics and Superfine Microstructure and CAS Key Laboratory of Materials for Energy Conversion, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 200050, PR China	J.Solid State Chem., 252(2017)106	Jianqiao He,Xian Zhang,Xiaofang Lai,Fuqiang Huang		
157427	CHM0267209	RRR = 30.8. Type-1 SC. SP (beta) = 0.30 mJ/mol.K4. (dC/gamma*Tc) = 1.42. GL = 0.05. e-ph = 0.62	AsSn	As1Sn1	As	1	Sn	1																				1	2014																										AB		NaCl	Fm3[-]m	225	A	5.72513														K			3.58			0.27	3.58										84										Oe	type-1,Hc, BCS	178												MHC157427		nm	BCS, from gamma	454.4			nm	London	23.2										MSP157427			mJ/mol.K2	2.18	SP	235	SP											uOhm.cm							5.42							cm3/C	-0.0000921					MRH157427			Sn(5N),As(4N)		mixture - sealed in silica ampule - heat(500C,10h) - press to pellet - heat(500C,5h, in silica ampule). For Hall effect, 70 nm SnAs films grown on silica substrates by laser deposition					SnAs with the NaCl-type Structure: Type-I Superconductivity and Single Valence State of Sn			Materials and Structures Laboratory, Tokyo Institute of Technology, Mailbox R3-1, 4259 Nagatsuta-cho, Midori-ku, Yokohama, Kanagawa 226-8503, Japan	Chem.Mater., 26(2014)7209	Yue Wang,Hikaru Sato,Yoshitake Toda,Shigenori Ueda,Hidenori Hiramatsu,Hideo Hosono		
157428	EPL11317002	RRR = 12.5	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2016																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.489		10.322												K	3.8		3.85	3.85			3.85										87										T	RES(0.5Rn), Linear approx.	0.21												MHC157428																			MSP157428																																											self flux method. mixture(Ba:Pd:As = 1:2:2) - alumina clucible sealed in quartz tube - heat to 1100 C(50 C/h) - keep(20h) - slow cool to 800 C(2 C/h) - cool to RT					Superconductivity at 3.85 K in BaPd2As2 with the ThCr2Si2-type structure			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - Beijing 100190, China	Europhys.Lett., 113(2016)17002	Qi Guo,Jia Yu,Bin-Bin Ruan,Dong-Yun Chen,Xiao-Chuan Wang,Qing-Ge Mu,Bo-Jin Pan,Gen-Fu Chen,Zhi-An Ren		
157429	JAC6940439	not SC. successive magnetic transition at 13.4 K. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.33 uB/Eu and Curie-T = -14.8 K.	EuCoGe3	Eu1Co1Ge3	Eu	1	Co	1	Ge	3																		3	2017					my-B/Eu	7.7	-20.7	15.4																		ABC3		BaNiSn3			A	4.3191		9.8847												K					0			MTN157429																																																																																													Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157430	JAC6940439	not SC. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.94 uB/Eu and Curie-T = -19.8 K.	EuRhGe3	Eu1Rh1Ge3	Eu	1	Rh	1	Ge	3																		3	2017					my-B/Eu	7.8	-16	11.6																		ABC3		BaNiSn3			A	4.4129		10.0906												K					0			MTN157430																																																																																													Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157431	JAC6940439	not SC. successive magnetic transition at 7.0 K. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.85 uB/Eu and Curie-T = -20.2 K.	EuIrGe3	Eu1Ir1Ge3	Eu	1	Ir	1	Ge	3																		3	2017					my-B/Eu	7.92	-19.6	12.2																		ABC3		BaNiSn3			A	4.4358		10.0581												K					0			MTN157431																																																																																													Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157432	JAC6940439	not SC. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.97 uB/Eu and Curie-T = -5.8 K.	EuNiGe3	Eu1Ni1Ge3	Eu	1	Ni	1	Ge	3																		3	2017					my-B/Eu	7.88	-2.81	13.3																		ABC3		BaNiSn3			A	4.349		9.9087												K					0																																																																																																Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157433	JAC6940439	not SC. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.91 uB/Eu and Curie-T = -2.8 K.	EuPdGe3	Eu1Pd1Ge3	Eu	1	Pd	1	Ge	3																		3	2017					my-B/Eu	7.78	-3	12.2																		ABC3		BaNiSn3			A	4.4606		10.2324												K					0																																																																																																Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157434	JAC6940439	not SC. magnetic data for H//[100] in DB, for H//[00], effective moment = 7.95 uB/Eu and Curie-T = -6.4 K.	EuPtNi3	Eu1Pt1Ge3	Eu	1	Pt	1	Ge	3																		3	2017					my-B/Eu	7.96	-6	10.8																		ABC3		BaNiSn3			A	4.4758		10.0887												K					0																																																																																																Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157435	JAC6940439	(dC/gamma*Tc) = 0.59	SrRhGe3	Sr1Rh1Ge3	Sr	1	Rh	1	Ge	3																		3	2017																										ABC3		BaNiSn3			A	4.4399		10.1321												K		0.71					0.71																																																2								mJ/mol.K2	5.1	SP	200	SP																																		Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157436	JAC6940439	(dC/gamma*Tc) = 0.93	SrNiGe3	Sr1Ni1Ge3	Sr	1	Ni	1	Ge	3																		3	2017																										ABC3		BaNiSn3			A	4.3785		10.0231												K		0.46					0.46																																																3.5								mJ/mol.K2	5.6	SP	280	SP																																		Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157437	JAC6940439	(dC/gamma*Tc) = 1.9	SrIrGe3	Sr1Ir1Ge3	Sr	1	Ir	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K		0.53					0.53																																																5.6								mJ/mol.K2	5.3	SP	230	SP																																		Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157438	JAC6940439	RRR = 150.  (dC/gamma*Tc) = 1.2	SrPdGe3	Sr1Pd1Ge3	Sr	1	Pd	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K		1.38					1.38																																																3.1								mJ/mol.K2	5.3	SP	250	SP											uOhm.cm							0.3																Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157439	JAC6940439	(dC/gamma*Tc) = 1.1	SrPtGe3	Sr1Pt1Ge3	Sr	1	Pt	1	Ge	3																		3	2017																										ABC3		BaNiSn3																		K		0.84					0.84																																																2.8								mJ/mol.K2	4.7	SP	260	SP																																		Sr(3N),T(4N),Ge(5N),In(5N)		(Sr:T:Ge:In = 1.2:1:(3-4):30) - alumina crucible - quartz tube - heat(1130 C,3d) - cool to 500C within 15 days - remove flux at 250C by spinning method					Superconducting, Fermi surface, and magnetic properties in SrTGe3 and EuTGe3 (T: transition metal) with the Rashba-type tetragonal structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa, 903-0213, Japan	J.Alloys Compd, 694(2017)439	Masashi Kakihana,Hiromu Akamine,Keisuke Tomori,Kengo Nishimura,Atsushi Teruya,Ai Nakamura,Fuminori Honda,Dai Aoki,Miho Nakashima,Yasushi Amako,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Tetsuya Takeuchi,Takanori Kida,Masayuki Hagiwara,Yoshinori Haga,Etsuji Yamamoto,Masato Hedo,Takao Nakama,Yoshichika Onuki		
157440	EPL0060659	P-induced SC. Tc(max) = 8.68 K(in DB) at P=8 GPa. many phases depending P. See TCFIG(Tc vs P)	Bi	Bi1	Bi	1																							1988																										A																				K		8.68			0		8.68	MTC157440		K/GPa	-0.3																																																																																										Bi(5N5)							Evidence for an Electronic Phase Transition in Bismuth under Pressure			Institut fur Festkorperforschung - KFA Julich, D-5170 Julich	Europhys.Lett., 6(1988)659	N.Lotter,J.Wittig		
157441	JPS080103701		Ca(Fe,Rh)2As2	Ca1Fe1.958Rh0.042As2	Ca	1	Fe	1.958	Rh	0.042	As	2																3	2011																										AB2C2		ThCr2Si2																		K				11.9			11.9																																																																																																Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157442	JPS080103701	uncollapsed-tetra to collapsed tetra transition at T<STR> = 54.2 K.	Ca(Fe,Rh)2As2	Ca1Fe1.952Rh0.048As2	Ca	1	Fe	1.952	Rh	0.048	As	2																3	2011																										AB2C2		ThCr2Si2																		K				12.8			12.8																																																																																																Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157443	JPS080103701	uncollapsed-tetra to collapsed tetra transition at T<STR> = 64.3 K.	Ca(Fe,Rh)2As2	Ca1Fe1.94Rh0.06As2	Ca	1	Fe	1.94	Rh	0.06	As	2																3	2011																										AB2C2		ThCr2Si2																		K				0	0		0																																																																																																Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157444	JPS080103701	uncollapsed-tetra to collapsed tetra transition at T<STR> = 154 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2011								154																		AB2C2		ThCr2Si2			A	3.8953		11.7153												K					0																																																																																																		Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157445	JPS080103701	uncollapsed-tetra to collapsed tetra transition at T<STR> = 108 K.	Ca(Fe,Rh)2As2	Ca1Fe1.968Rh0.032As2	Ca	1	Fe	1.968	Rh	0.032	As	2																3	2011								107																		AB2C2		ThCr2Si2			A	3.8997		11.713												K					0																																																																																																		Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157446	JPS080103701	uncollapsed-tetra to collapsed tetra transition at T<STR> = 79.3 K.	Ca(Fe,Rh)2As2	Ca1Fe1.96Rh0.04As2	Ca	1	Fe	1.96	Rh	0.04	As	2																3	2011								77.2																		AB2C2		ThCr2Si2			A	3.9012		11.692												K				10.8			10.8																																																																																																Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157447	JPS080103701		Ca(Fe,Rh)2As2	Ca1Fe1.956Rh0.044As2	Ca	1	Fe	1.956	Rh	0.044	As	2																3	2011																										AB2C2		ThCr2Si2			A	3.8996		11.6742												K				11.4			11.4																																																																																																Flux method. mixture(Ca:FeAs:RhAs = 1:(4-4x):4x) - alumina crucible in sealed quartz tube - heat(1100C) - cool to 1050 C(1.25 C/h) - cool to RT - remove flux mechanically					Interplay of Superconductivity and Fermi-Liquid Transport in Rh-Doped CaFe2As2 with Lattice-Collapse Transition			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 80(2011)103701	Masataka DANURA,Kazutaka KUDO,Yoshihiro OSHIRO,Shingo ARAKI,Tatsuo C. KOBAYASHI,Minoru NOHARA		
157448	JPS083063707	P=0 GPa. semiconductor like resistivity.	Sr0.5La0.5FBiS2	Sr0.5La0.5F1Bi1S2	Sr	0.5	La	0.5	F	1	Bi	1	S	2														1	2014																													P4/nmm		A	4.077		13.388											BiS2-plane SC	K	2		2.2				2.1																																																																																														La,SrF2,Bi,S		mixture - pellet - sealed in quartz tube - heat to 650 C(2 C/min) - SIN(650 C,12h) - cool to RT, one more process					Impact of Hydrostatic Pressure on Superconductivity of Sr0.5La0.5FBiS2			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Soc.Jpn, 83(2014)063707	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157449	JPS083063707	P = 1.97 GPa where Tc(max). R(T) = R0 + A*T for 20 < T < 240 K, where A = 1.57 uOhmcm/K.	Sr0.5La0.5FBiS2	Sr0.5La0.5F1Bi1S2	Sr	0.5	La	0.5	F	1	Bi	1	S	2														1	2014																																													BiS2-plane SC	K								MTC157449																			T	RES(0.9Rn), WHH	20												MHC157449																																					mOhm.cm							0.134																La,SrF2,Bi,S		mixture - pellet - sealed in quartz tube - heat to 650 C(2 C/min) - SIN(650 C,12h) - cool to RT, one more process					Impact of Hydrostatic Pressure on Superconductivity of Sr0.5La0.5FBiS2			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Phys.Soc.Jpn, 83(2014)063707	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157450	JETP0341263	not SC. Tc (in DB) = 8.4 K at 100 kbar for Bi-IV phase.	Bi	Bi1	Bi	1																							1972																										A																			Bi-IV phase	K		8.4					8.4	MTC157450																																																																																																				Superconductivity of Bismuth, Barium, and Lead at Pressures Exceeding 100 kbar			Institute of the Physics of High Pressures, USSR Academy of Sciences	oviet hysics JETP, 34(1972)1263	M.A.Il'ina,E.S.Itskevich,E.M.Dizhur		
157451	JETP0341263	not SC. Tc (in DB) = 4.85 K at 164 kbar for Ba-IV phase.	Ba	Ba1	Ba	1																							1972																										A																			Ba-IV phase	K		4.85					4.85	MTC157451																																																																																																				Superconductivity of Bismuth, Barium, and Lead at Pressures Exceeding 100 kbar			Institute of the Physics of High Pressures, USSR Academy of Sciences	oviet hysics JETP, 34(1972)1263	M.A.Il'ina,E.S.Itskevich,E.M.Dizhur		
157452	JETP0341263	Phase boundary at P = 160 kbar (Pb-I and Pb-II)	Pb	Pb1	Pb	1																							1972																										A																				K								MTC157452																																																																																																				Superconductivity of Bismuth, Barium, and Lead at Pressures Exceeding 100 kbar			Institute of the Physics of High Pressures, USSR Academy of Sciences	oviet hysics JETP, 34(1972)1263	M.A.Il'ina,E.S.Itskevich,E.M.Dizhur		
157453	JPS086063704	(dC/gamma*Tc) = 2.3.  gap size (2D/kTc) = 4.58 from SP-alpha model.	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		1	2017																										AB2C2		ThCr2Si2	I4/mmm	139																K				3.85			3.85																																																4.58	14				MSP157453			mJ/mol.K2	6.1	SP	144	SP																																				(Ba,Pd,PdAs2 powder) - alumina crucible in quartz tube - heat(900C,48h) - Q to iced water. preparatin condition is very strict.					Strong-Coupling Superconductivity in BaPd2As2 Induced by Soft Phonons in the ThCr2Si2-Type Polymorph			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)063704	Kazutaka Kudo,Yoshiaki Yamada,Takaaki Takeuchi,Takumi Kimura,Satoshi Ioka,Genta Matsuo,Yutaka Kitahama,Minoru Nohara		
157454	JPS086063704	not SC.	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		1	2017																										AB2C2		CeMg2Si2	P4/mmm	123																K					1.8																																																							MSP157453			mJ/mol.K2	5.4	SP	259	SP																																				(Ba,Pd,PdAs2 powder) - alumina crucible in quartz tube - heat(700 - 1150 C)) - Q to iced water or furnace cool to RT. very stable.					Strong-Coupling Superconductivity in BaPd2As2 Induced by Soft Phonons in the ThCr2Si2-Type Polymorph			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)063704	Kazutaka Kudo,Yoshiaki Yamada,Takaaki Takeuchi,Takumi Kimura,Satoshi Ioka,Genta Matsuo,Yutaka Kitahama,Minoru Nohara		
157455	JPS086074701	not SC	LaOBiSSe	La1Bi1S1Se1O1	La	1	Bi	1	S	1	Se	1													O	1		1	2017																													P2<1>/m		A	4.1159	4.1159	14.091											BiS2-layer SC	K					0																																																																				uV/K	-47.6				mOhm.cm																							Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157456	JPS086074701	SC suddenly induced by a small amount of electron doping  of 0.05-0.1per Bi	La(O,F)BiSSe	La1F0.1Bi1S1Se1O0.9	La	1	F	0.1	Bi	1	S	1	Se	1											O	0.9		1	2017																													P4/nmm		A	4.12		13.8576											BiS2-layer SC	K	3.2			3.5			3.5										85																																																								uV/K	-25.3				mOhm.cm							1.58																Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157457	JPS086074701		La(O,F)BiSSe	La1F2Bi1S1Se1O0.8	La	1	F	2	Bi	1	S	1	Se	1											O	0.8		1	2017																													P4/nmm		A	4.1337		13.7472											BiS2-layer SC	K	3.8			3.8			3.8																																																																		uV/K	-24.9				mOhm.cm							1.38																Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157458	JPS086074701		La(O,F)BiSSe	La1F0.3Bi1S1Se1O0.7	La	1	F	0.3	Bi	1	S	1	Se	1											O	0.7		1	2017																													P4/nmm		A	4.1349		13.6963											BiS2-layer SC	K	3.8			3.9			3.9	MTC157458																																																																	uV/K	-23.5				mOhm.cm							0.744																Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157459	JPS086074701		La(O,F)BiSSe	La1F0.4Bi1S1Se1O0.6	La	1	F	0.4	Bi	1	S	1	Se	1											O	0.6		1	2017																													P4/nmm		A	4.1363		13.6389											BiS2-layer SC	K	3.8			3.9			3.9																																																																		uV/K	-20.2				mOhm.cm							0.867																Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157460	JPS086074701		La(O,F)BiSSe	La1F0.5Bi1S1Se1O0.5	La	1	F	0.5	Bi	1	S	1	Se	1											O	0.5		1	2017																													P4/nmm		A	4.1375		13.6272											BiS2-layer SC	K	3.8			3.9			3.9																																																																		uV/K	-19.9				mOhm.cm							0.714																Bi2S3,La2S3,BiF3,Bi2S3,Bi2Se3,Bi		solid state reaction. mixture - pellet - sealed in quartz tube - heat(700C,20h)					Intrinsic Phase Diagram of Superconductivity in the BiCh2-Based System Without In-Plane Disorder			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)074701	Kouhei Nagasaka,Atsuhiro Nishida,Rajveer Jha,Joe Kajitani,Osuke Miura,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Hidetomo Usui,Kazuhiko Kuroki,Yoshikazu Mizuguchi		
157461	JPS086083706	Effect of disorder (induced by e-irradiation) on Tc, Tn	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2017																										AB2C2		ThCr2Si2																		K					0			MPH157461																																																																																				cm3/C						MRH157461					single crystals synthesized by self-flux method					Impact of Disorder on the Superconducting Phase Diagram in BaFe2(As1-xPx)2			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 86(2017)083706	Yuta Mizukami,Marcin Konczykowski,Kohei Matsuura,Tatsuya Watashige,Shigeru Kasahara,Yuji Matsuda,Takasada Shibauchi		
157462	JPS086083706	Effect of disorder (induced by e-irradiation) on Tc, Tn	BaFe2(As,P)2	Ba1Fe2As1.52P0.48	Ba	1	Fe	2	As	1.52	P	0.48																3	2017																										AB2C2		ThCr2Si2																		K		23.3					23.3	MPH157462																																																																																				cm3/C						MRH157462					single crystals synthesized by self-flux method					Impact of Disorder on the Superconducting Phase Diagram in BaFe2(As1-xPx)2			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 86(2017)083706	Yuta Mizukami,Marcin Konczykowski,Kohei Matsuura,Tatsuya Watashige,Shigeru Kasahara,Yuji Matsuda,Takasada Shibauchi		
157463	JPS086083706	Effect of disorder (induced by e-irradiation) on Tc, Tn	BaFe2(As,P)2	Ba1Fe2As1.44P0.56	Ba	1	Fe	2	As	1.44	P	0.56																3	2017																										AB2C2		ThCr2Si2																		K		30					30																																																																																																single crystals synthesized by self-flux method					Impact of Disorder on the Superconducting Phase Diagram in BaFe2(As1-xPx)2			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 86(2017)083706	Yuta Mizukami,Marcin Konczykowski,Kohei Matsuura,Tatsuya Watashige,Shigeru Kasahara,Yuji Matsuda,Takasada Shibauchi		
157464	JPS086083706	Effect of disorder (induced by e-irradiation) on Tc, Tn	BaFe2(As,P)2	Ba1Fe2As1.4P0.6	Ba	1	Fe	2	As	1.4	P	0.6																3	2017																										AB2C2		ThCr2Si2																		K		21.7					21.7	MTC157464																																																																																															single crystals synthesized by self-flux method					Impact of Disorder on the Superconducting Phase Diagram in BaFe2(As1-xPx)2			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 86(2017)083706	Yuta Mizukami,Marcin Konczykowski,Kohei Matsuura,Tatsuya Watashige,Shigeru Kasahara,Yuji Matsuda,Takasada Shibauchi		
157465	JPS086104704	DOS = 26.4 states/eV.spin , obtained from [gamma]	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2017	emu/mol	0.00003																								ABC2	3	CeNiC2			A	3.9521	4.5571	6.1929												K	2.8						2.8																																																								mJ/mol.K2	7.8														uOhm.cm							13.1																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157466	JPS086104704	DOS = 29.6 states/eV.spin , obtained from [gamma]	(La,Ce)NiC2	La0.995Ce0.005Ni1C2	La	0.995	Ce	0.005	Ni	1	C	2																1	2017	emu/mol	0.0005	emu/K/mol	3.2	myu-B/Ce	2.27																				ABC2	3	CeNiC2			A	3.9547	4.5578	6.1956												K	2.4						2.4	MTC157466																																																							mJ/mol.K2	8.7														uOhm.cm							17.6																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157467	JPS086104704	DOS = 26.2 states/eV.spin , obtained from [gamma]	(La,Ce)NiC2	La0.99Ce0.01Ni1C2	La	0.99	Ce	0.01	Ni	1	C	2																1	2017	emu/mol	0.0006	emu/K/mol	6.6	myu-B/Ce	2.3																				ABC2	3	CeNiC2			A		4.5553	6.1919												K	1.9						1.9																																																								mJ/mol.K2	7.7														uOhm.cm							15.4																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157468	JPS086104704	DOS = 28.2 states/eV.spin , obtained from [gamma]	(La,Ce)NiC2	La0.985Ce0.015Ni1C2	La	0.985	Ce	0.015	Ni	1	C	2																1	2017	emu/mol	0.001	emu/K/mol	10.1	myu-B/Ce	2.32																				ABC2	3	CeNiC2			A															K	1.5						1.5																																																								mJ/mol.K2	8.3														uOhm.cm							14.2																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157469	JPS086104704	DOS = 30.5 states/eV.spin , obtained from [gamma]	(La,Ce)NiC2	La0.98Ce0.02Ni1C2	La	0.98	Ce	0.02	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	14.1	myu-B/Ce	2.38																				ABC2	3	CeNiC2			A	3.9507		6.1934												K	0.1						0.1																																																								mJ/mol.K2	9														uOhm.cm							17.6																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157470	JPS086104704	not SC	(La,Ce)NiC2	La0.975Ce0.025Ni1C2	La	0.975	Ce	0.025	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	15.6	myu-B/Ce	2.24																				ABC2	3	CeNiC2			A		4.5549	6.1909												K					0.4																																																										mJ/mol.K2	8.5														uOhm.cm							23																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157471	JPS086104704	not SC	(La,Ce)NiC2	La0.97Ce0.03Ni1C2	La	0.97	Ce	0.03	Ni	1	C	2																1	2017	emu/mol	0.001	emu/K/mol	15.7	myu-B/Ce	2.05																				ABC2	3	CeNiC2			A	3.9521	4.5564	6.1923												K					0.4																																																										mJ/mol.K2	9.3														uOhm.cm							17.1																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157472	JPS086104704	not SC	(La,Ce)NiC2	La0.95Ce0.05Ni1C2	La	0.95	Ce	0.05	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	28.3	myu-B/Ce	2.13	-0.4																			ABC2	3	CeNiC2			A	3.9497	4.5536	6.1904												K					0.4																																																										mJ/mol.K2	8.3														uOhm.cm							30																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157473	JPS086104704	not SC	(La,Ce)NiC2	La0.9Ce0.1Ni1C2	La	0.9	Ce	0.1	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	73.1	myu-B/Ce	2.42	-0.8																			ABC2	3	CeNiC2			A	3.9447	4.5549	6.1891												K					0.4																																																										mJ/mol.K2	9														uOhm.cm							30.7																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157474	JPS086104704	not SC	(La,Ce)NiC2	La0.8Ce0.2Ni1C2	La	0.8	Ce	0.2	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	177	myu-B/Ce	2.66	-0.4																			ABC2	3	CeNiC2			A	3.9372	4.5549	6.1877												K					0.4																																																										mJ/mol.K2	16.6														uOhm.cm							45.5																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157475	JPS086104704	not SC	(La,Ce)NiC2	La0.5Ce0.5Ni1C2	La	0.5	Ce	0.5	Ni	1	C	2																1	2017	emu/mol	0.002	emu/K/mol	417	myu-B/Ce	2.58	-16.4																			ABC2	3	CeNiC2			A	3.9178	4.5565	6.1833												K					0.4																																																										mJ/mol.K2	62.3														uOhm.cm							51.9																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157476	JPS086104704	not SC	(La,Ce)NiC2	La0.35Ce0.65Ni1C2	La	0.35	Ce	0.65	Ni	1	C	2																1	2017	emu/mol	0.003	emu/K/mol	415	myu-B/Ce	2.26	-24.4																			ABC2	3	CeNiC2			A	3.9084	4.556	6.182												K					0.4																																																										mJ/mol.K2	79.2														uOhm.cm							50.7																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157477	JPS086104704	not SC. AFIC = incommensurate AFM state, AFC= commensurate AFM state, F = FM or Ferrimag state, in TC-fig.	(La,Ce)NiC2	La0.25Ce0.75Ni1C2	La	0.25	Ce	0.75	Ni	1	C	2																1	2017	emu/mol	0.003	emu/K/mol	534	myu-B/Ce	2.39	-16.2																			ABC2	3	CeNiC2			A	3.8992	4.5556	6.1792												K					0.4			MPH157477																																																							mJ/mol.K2	152														uOhm.cm							46.4																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157478	JPS086104704	not SC	(La,Ce)NiC2	La0.15Ce0.85Ni1C2	La	0.15	Ce	0.85	Ni	1	C	2																1	2017	emu/mol	0.004	emu/K/mol	539	myu-B/Ce	2.25	-15.1																			ABC2	3	CeNiC2			A	3.8942	4.556	6.1773												K					0.4																																																										mJ/mol.K2	166														uOhm.cm							40.6																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157479	JPS086104704	not SC. Ferro- or Ferrimag-state in low temperature.	CeNiC2	Ce1Ni1C2	Ce	1	Ni	1	C	2																		1	2017	emu/mol	0.006	emu/K/mol	654	myu-B/Ce	2.29	-17.5																			ABC2	3	CeNiC2			A	3.8821	4.556	6.1724												K					0.4																																																										mJ/mol.K2	292														uOhm.cm							15.7																La(3N),Ce(3N),Ni(4N8),C(5N5)		arc-melting with 4 at% excess C. several times.					Competition between Superconductivity and Magnetism in Non-centrosymmetric (La1-xCex)NiC2			Department of Physics, Graduate School of Science and Engineering, Saitama University, Saitama 338-8570, Japan	J.Phys.Soc.Jpn, 86(2017)104704	Susumu Katano,Kohei Shibata,Kotaro Nakashima,Hideaki Yoshimura,Yohei Matsubara		
157480	JPS086104712	R(T) not zero down to 1.9 K.	Eu0.5Ce0.5FBiS2	Eu0.5Ce0.5F1Bi1S2	Eu	0.5	Ce	0.5	F	1	Bi	1	S	2														1	2017																										ABCD2	2	CeOBiS2				4.0702		13.3418											BiS2-layer SC, EuFBiS2-type	K			2.3				2.3																																																																																														EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157481	JPS086104712		Eu0.5Ce0.5FBiS2-xSex	Eu0.5Ce0.5F1Bi1S1.8Se0.2	Eu	0.5	Ce	0.5	F	1	Bi	1	S	1.8	Se	0.2												1	2017																										ABCD2	2	CeOBiS2			A	4.0774		13.3626											BiS2-layer SC, EuFBiS2-type	K	2.68						2.68																																																																																														EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157482	JPS086104712		Eu0.5Ce0.5FBiS2-xSex	Eu0.5Ce0.5F1Bi1S1.6Se0.4	Eu	0.5	Ce	0.5	F	1	Bi	1	S	1.6	Se	0.4												1	2017																										ABCD2	2	CeOBiS2			A	4.0916		13.3996											BiS2-layer SC, EuFBiS2-type	K	3.02						3.02																																																																																														EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157483	JPS086104712		Eu0.5Ce0.5FBiS2-xSex	Eu0.5Ce0.5F1Bi1S1.4Se0.6	Eu	0.5	Ce	0.5	F	1	Bi	1	S	1.4	Se	0.6												1	2017																										ABCD2	2	CeOBiS2			A	4.1036		13.4153											BiS2-layer SC, EuFBiS2-type	K	3.53						3.53	MTC157483																																																																																													EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157484	JPS086104712		Eu0.5Ce0.5FBiS2-xSex	Eu0.5Ce0.5F1Bi1S1.2Se0.8	Eu	0.5	Ce	0.5	F	1	Bi	1	S	1.2	Se	0.8												1	2017																										ABCD2	2	CeOBiS2			A	4.1203		13.4416											BiS2-layer SC, EuFBiS2-type	K	3.61						3.61																																																																																														EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157485	JPS086104712		Eu0.5Ce0.5FBiS2-xSex	Eu0.5Ce0.5F1Bi1S1Se1	Eu	0.5	Ce	0.5	F	1	Bi	1	S	1	Se	1												1	2017																										ABCD2	2	CeOBiS2			A	4.1375		13.4786											BiS2-layer SC, EuFBiS2-type	K	3.36						3.36																																																																																														EuS,Ce2S3,BiF3,Bi(5N),S(4N),Se(5N)		mxture - pellet - sealed in quartz tube - heat(20h, 780C(x=0), 700C(x=0.2, 0.4), 650C(x=0.6,0.8), 600C(x=1))					Bulk Superconductivity Induced by Se Substitution in BiCh2-Based Layered Compounds Eu0.5Ce0.5FBiS2-xSex			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)104712	Yosuke Goto,Ryota Sogabe,Yoshikazu Mizuguchi		
157486	MMM0150042	Specific heat of ErxLa1-xBe13 (x = 0-0.09) were measured. SP (beta = 0.16 mJ/mol.K4. SC properties not described	LaBe13	Be13La1	Be	13	La	1																					1980																										AB13																				K					0																																																										mJ/mol.K2	11	SP																																											SPECIFIC HEAT AND ELECTRON SPIN RESONANCE OF ErxLa1-xBe13			Kamerlingh Onnes Laboratorium der Rijks-Universiteit, Leiden, The Netherlands	J.Mag.Mag.Mat., 15(1980)42	H.W.M. van Der Linden,G.J.Nieuwenhuys,H.D.Dokter,D.Davidov,I.Felner		
157487	PRB0110440	not SC above 0.45 K	LaBe13	Be13La1	Be	13	La	1																					1975	cm3/mole	-0.0000241																								AB13		NaZn13			A	10.451														K					0.45																																																										mJ/gat.K2	0.58	SP	820	SP																																									Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157488	PRB0110440	SC properties not investigated	CeBe13	Be13Ce1	Be	13	Ce	1																					1975	cm3/mole	0.00164																								AB13		NaZn13			A	10.372														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157489	PRB0110440	SC properties not investigated	PrBe13	Be13Pr1	Be	13	Pr	1																					1975	cm3/mole	0.047					-8																			AB13		NaZn13			A	10.369														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157490	PRB0110440	SC properties not investigated	NdBe13	Be13Nd1	Be	13	Nd	1																					1975							2.5	2.63																		AB13		NaZn13			A	10.348														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157491	PRB0110440	SC properties not investigated.  rambda-type SP anomaly at 9.05 K	SmBe13	Be13Sm1	Be	13	Sm	1																					1975								8.8																		AB13		NaZn13			A	10.304														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157492	PRB0110440	SC properties not investigated	EuBe13	Be13Eu1	Be	13	Eu	1																					1975	cm3/mole	0.00647																								AB13		NaZn13			A	10.286														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157493	PRB0110440	SC properties not investigated	GdBe13	Be13Gd1	Be	13	Gd	1																					1975							25	25.7																		AB13		NaZn13			A	10.273														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157494	PRB0110440	SC properties not investigated	TbBe13	Be13Tb1	Be	13	Tb	1																					1975							14	15.3																		AB13		NaZn13			A	10.247														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157495	PRB0110440	SC properties not investigated	DyBe13	Be13Dy1	Be	13	Dy	1																					1975							13	9.3																		AB13		NaZn13			A	10.233														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157496	PRB0110440	SC properties not investigated	HoBe13	Be13Ho1	Be	13	Ho	1																					1975							6	5.45																		AB13		NaZn13			A	10.219														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157497	PRB0110440	SC properties not investigated	ErBe13	Be13Er1	Be	13	Er	1																					1975							6	2.37																		AB13		NaZn13			A	10.203														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157498	PRB0110440	SC properties not investigated	TmBe13	Be13Tm1	Be	13	Tm	1																					1975							1																			AB13		NaZn13			A	10.189														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157499	PRB0110440	SC properties not investigated	YbBe13	Be13Yb1	Be	13	Yb	1																					1975																										AB13		NaZn13			A	10.18														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157500	PRB0110440	not SC above 0.45 K	LuBe13	Be13Lu1	Be	13	Lu	1																					1975																										AB13		NaZn13			A	10.17														K					0.45																																																										mJ/gat.K2	0.6	SP	930	SP																																									Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157501	PRB0110440	SC properties not investigated	(La,Tm)Be13	Be13La0.75Tm0.25	Be	13	La	0.75	Tm	0.25																			1975																										AB13		NaZn13			A	10.394														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157502	PRB0110440	not SC above 0.45 K	ThBe13	Be13Th1	Be	13	Th	1																					1975																										AB13		NaZn13			A	10.383														K					0.45																																																										mJ/gat.K2	507	SP	618	SP																																									Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157503	PRB0110440	SC properties not investigated.  no ordering down to 0.65 K.	UBe13	Be13U1	Be	13	U	1																					1975							-98																			AB13		NaZn13			A	10.257														K					0																																																																																																							Electronic properties of beryllides of the rare earth and some actinides			Bell Laboratories,Murry Hill, New Jersey 07974	Phys.Rev. B, 11(1975)440	E.Bucher,P.Maita,G.W.Hull,R.C.Fulton,A.S.Cooper		
157504	SSC0480835	SC properties not investigated	CeBe13	Be13Ce1	Be	13	Ce	1																					1983	cm3/mol	2050																								AB13		NaZn13																		K																																																															mJ/Mol.K2	58.6	SP	895	SP																																									ON THE VALENCE REGIME 1N THE (CexLa1-x)Be13 SYSTEM			L.M.S.E.S., Institut de Physique, 3, rue de I'Universite, 6084 Strasbourg, France	Solid State Commun., 48(1983)835	M.J.Besnus,J.P.Kappler,A.Meyer		
157505	SSC0480835	SC properties not investigated	(Ce,La)Be13	Be13Ce0.648La352	Be	13	Ce	0.648	La	352																			1983	cm3/mol	2860																								AB13		NaZn13																		K																																																															mJ/Mol.K2	74	SP	815	SP																																									ON THE VALENCE REGIME 1N THE (CexLa1-x)Be13 SYSTEM			L.M.S.E.S., Institut de Physique, 3, rue de I'Universite, 6084 Strasbourg, France	Solid State Commun., 48(1983)835	M.J.Besnus,J.P.Kappler,A.Meyer		
157506	SSC0480835	SC properties not investigated	(Ce,La)Be13	Be13Ce0.307La0.693	Be	13	Ce	0.307	La	0.693																			1983	cm3/mol	5010																								AB13		NaZn13																		K																																																															mJ/Mol.K2	126.6	SP	705	SP																																									ON THE VALENCE REGIME 1N THE (CexLa1-x)Be13 SYSTEM			L.M.S.E.S., Institut de Physique, 3, rue de I'Universite, 6084 Strasbourg, France	Solid State Commun., 48(1983)835	M.J.Besnus,J.P.Kappler,A.Meyer		
157507	SSC0480835	SC properties not investigated	(Ce,La)Be13	Be13Ce0.115La0.885	Be	13	Ce	0.115	La	0.885																			1983	cm3/mol	7270																								AB13		NaZn13																		K																																																															mJ/Mol.K2	214	SP	720	SP																																									ON THE VALENCE REGIME 1N THE (CexLa1-x)Be13 SYSTEM			L.M.S.E.S., Institut de Physique, 3, rue de I'Universite, 6084 Strasbourg, France	Solid State Commun., 48(1983)835	M.J.Besnus,J.P.Kappler,A.Meyer		
157508	SSC0480835	SC properties not investigated	LaBe13	Be13La1	Be	13	La	1																					1983	cm3/mol	-290																								AB13		NaZn13																		K																																																															mJ/Mol.K2	7.8	SP	865	SP																																									ON THE VALENCE REGIME 1N THE (CexLa1-x)Be13 SYSTEM			L.M.S.E.S., Institut de Physique, 3, rue de I'Universite, 6084 Strasbourg, France	Solid State Commun., 48(1983)835	M.J.Besnus,J.P.Kappler,A.Meyer		
157509	MSP0300092	matrix(Ti2GeC) , minor phase (Ti2C)	T12GeC	Ti2Ge1C1	Ti	2	Ge	1	C	1																		1	2012																										ABC2		Cr2AlC	P6<3>/mmc		A	3.078		12.92											hexagonal	K				9.5			9.5																				T	R(onset), GL	8.1												MHC157509		A	from Hc2	64																																																								Ti,Ge,graphite		mixture - compact (8*8*2 mm3) - sealed in quartz ampoule - heat(1000C,24h) - reground - compact - heat(1200C,120h) - ANN(1500C,30min)					Superconductivity at 9.5 K in the Ti2GeC compound			Departamento de Engenharia de Materiais, Escola de Engenharia de Lorena ? USP, P.O. BOX 116, Lorena ? SP, 12600-970 Brazil	Mat.Sci. Poland, 30(2012)92	A.D. BORTOLOZO,O.H. SANT'ANNA,C.A.M. DOS SANTOS,A.J.S. MACHADO		
157510	NAT5250073	P-induced SC.  High-Tc phase obtained by initial P loading at 200 K. Tc(max) = 203 K at P = 155 GPa.	H2S	H2S1	H	2	S	1																					2015																										AB2																				K			203				203	MTC157510																			T	R(onset), GL	70												MHC157510																																																																			Conventional superconductivity at 203 kelvin at high pressures in the sulfur hydride system			Max-Planck-Institut fur Chemie, Hahn-Meitner-Weg 1, 55128 Mainz, Germany. 2Institut fur Anorganische Chemie und Analytische Chemie, Johannes Gutenberg-Universitat Mainz, Staudingerweg 9, 55099 Mainz, Germany.	Nature, 525(2015)73	A. P. Drozdov1,M. I. Eremets,I. A. Troyan,V. Ksenofontov,S. I. Shylin		
157511	NAT5250073	P-induced SC.  High-Tc phase obtained by initial P loading at 200 K. Isotope ffect by deutorium.  Tc(max) = 153 K at P = 173 GPa.	D2S	D2S1	D	2	S	1																					2015																										AB2																				K			53				53	MTC157511																																																																																																				Conventional superconductivity at 203 kelvin at high pressures in the sulfur hydride system			Max-Planck-Institut fur Chemie, Hahn-Meitner-Weg 1, 55128 Mainz, Germany. 2Institut fur Anorganische Chemie und Analytische Chemie, Johannes Gutenberg-Universitat Mainz, Staudingerweg 9, 55099 Mainz, Germany.	Nature, 525(2015)73	A. P. Drozdov1,M. I. Eremets,I. A. Troyan,V. Ksenofontov,S. I. Shylin		
157512	NAT5250073	P-induced SC.  High-Tc phase obtained by initial P loading at 200 K. Tc(max) = 135 K at P = 200 GPa.	H2S	H2S1	H	2	S	1																					2015																										AB2																				K			135				135	MTC157512																																																																																																				Conventional superconductivity at 203 kelvin at high pressures in the sulfur hydride system			Max-Planck-Institut fur Chemie, Hahn-Meitner-Weg 1, 55128 Mainz, Germany. 2Institut fur Anorganische Chemie und Analytische Chemie, Johannes Gutenberg-Universitat Mainz, Staudingerweg 9, 55099 Mainz, Germany.	Nature, 525(2015)73	A. P. Drozdov1,M. I. Eremets,I. A. Troyan,V. Ksenofontov,S. I. Shylin		
157513	PHB4850084	Compositions: Ba7.4(vacancy)0.6Si46 by EDS	Ba8Si46	Ba8Si46	Ba	8	Si	46																					2016																										A8B46		clathrate			A	10.32056														K				7.5			7.5										30	Oe	M-H curve				155			2																																																																											Si,BaSi2,EuSi2		High-T-High-P method (P=3GPa, 840C, 1h)					High-pressure synthesis and properties of the Eu-substituted Ba8-xEuxSi46 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Physica B, 485(2016)84	Lihua Liu,Bensheng Song,Bing Sun,Hongan Ma,Xingqiao Ma,Yang Li		
157514	PHB4850084	Compositions: Ba7.47Eu0.53Si46 by EDS. no diamag signal down to 2K	(Ba,Eu)8Si46	Ba7.5Eu0.5Si46	Ba	7.5	Eu	0.5	Si	46																			2016					myu-B/Eu	7.74	2.3																			A8B46		clathrate			A	10.313														K					2																																																																																																Si,BaSi2,EuSi2		High-T-High-P method (P=3GPa, 840C, 1h)					High-pressure synthesis and properties of the Eu-substituted Ba8-xEuxSi46 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Physica B, 485(2016)84	Lihua Liu,Bensheng Song,Bing Sun,Hongan Ma,Xingqiao Ma,Yang Li		
157515	PHB4850084	Compositions: Ba6.91Eu1.09Si46 by EDS.  no diamag signal down to 2K	(Ba,Eu)8Si46	Ba7Eu1Si46	Ba	7	Eu	1	Si	46																			2016					myu-B/Eu	6.6	4																			A8B46		clathrate			A	10.30913														K					2																																																																																																Si,BaSi2,EuSi2		High-T-High-P method (P=3GPa, 840C, 1h)					High-pressure synthesis and properties of the Eu-substituted Ba8-xEuxSi46 clathrates			Department of Physics, University of Science and Technology Beijing, Beijing 100083, China	Physica B, 485(2016)84	Lihua Liu,Bensheng Song,Bing Sun,Hongan Ma,Xingqiao Ma,Yang Li		
157516	PHB5210013	Tc = 3 K at P = 3 GPa for phase I. Phase transition observed between 8 and 45 K. Topological SC due to interface state from proximity effect. Bulk modulus from lattice const.	Bi2Te3	Bi2Te3	Bi	2	Te	3																				3	2017																		GPa	45							A2B3			R-3m		A	4.3674		30.0228											P = 1 GPa, T=8 K. See FIG-MLAT157516	K			7				7	MLAT157516																																																																																													Bi(5N),Te(5N)		Bridgman method. mixture - pellet - sealed in quartz ampoule - heat(1000C,3days) - cool to 500C (5 C/h) - FC to RT					Structural stability and phase transition of Bi2Te3 under high pressure and low temperature			Faculty of Electrical Engineering and Computer Science, Ningbo University, Ningbo 315211, China	Physica B, 521(2017)13	J.L. Zhang,S.J. Zhang,J.L. Zhu,Q.Q. Liu,X.C. Wang,C.Q.,Jin,J.C. Yu		
157517	PHC4830094		Bi4O4S3	Bi4S3O4	Bi	4	S	3																	O	4		1	2012																										A3B4C4			I4/mmm		A	3.978		41.07												K	4.02		4.5	4.02		0.3	4.02										33	Oe	M-H curve				7.04			2																																										W/K.m	4.84			MTHC157517	uV/K	-54.3			MTP157517	mOhm.cm				0.431							0.678												Bi2S3,Bi2O3,S		solid state reaction. mixture - pellet - sealed in silica tube - heat(510 C,10h) - reground - one more heat process					Superconducting and thermoelectric properties of new layered superconductor Bi4O4S3			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Physica C, 483(2012)94	S.G. Tan,L.J. Li,Y. Liu,P. Tong,B.C. Zhao,W.J. Lu,Y.P. Sun		
157518	PCS1110070	M = NH3.  Increased hybridization between 4p(Se) and 4d(Mo), by intercalation, induce SC.	Nax(NH3)yMoSe2	Na0.55M0.41Mo1Se2	Na	0.55	M	0.41	Mo	1	Se	2																	2017																																													MX2 layered material	K		5					5																																																																																																					Effect of molecular intercalation on the local structure of superconducting Nax(NH3)yMoSe2 system			CELLS - ALBA Synchrotron Radiation Facility, Carrer de la Llum 2-26, 08290, Cerdanyola del Valles, Barcelona, Spain	J.Phys.Chem.Solids, 111(2017)70	L. Simonelli,E. Paris,T. Wakita,C. Marini,K. Terashima,X. Miao,W. Olszewski,N. Ramanan,D. Heinis,Y. Kubozono,T. Yokoya,N.L. Saini		
157519	PHC5420001	RRR = 57.6. RH(200K) = 1.05 cm3/C. DB value for 100K. SP (beta) = 2.54 mJ/mol.K4. (dC/gamma*Tc) = 1.05. GL(kappa) = 0.6. SUS(300K) = 1.18E-4 cm3/mol.	BaNbS3	Ba1Nb1S3	Ba	1	Nb	1	S	3																		1	2017									3.93																	ABC3			P6<3>/mmc		A	6.825		5.761											hexagonal	K		1.89				0.01	1.89																				Oe	R(0.9Rn), R(0.1Rn)		1640	338					K/kOe	R=0.5,0.9,0.1Rn used	1.02	3.46	0.68	MHC157519		A	from Hc2		987	204	A	London	2340										MSP157519			mJ/Mol.K2	1.35	SP	91.4	SP																									cm3/C	0.01067						n/cm3	586000000000000000000	BaCO3,Nb2O5		solid state reaction. (mixture-pellet-heat) - process several times using several heat conditions					Superconductivity in quasi-one-dimensional BaNbS3			Physics Department, Montana State University, Bozeman, MT 59717-3840, USA	Physica C, 542(2017)1	J.J. Neumeier,M.G. Smith		
157520	PHC5430058	RRR = R250/R4 = 6. Tc(P) measured by Tc(SUS)  at H=2 Oe.	Nb0.25Bi2Se3	Nb0.25Bi2Se3	Nb	0.25	Bi	2	Se	3																		3	2017																													R3[-]m																	K	3.25			3.4		0.5	3.4	MTC157520		K/GPa	0.47																																																																			mOhm.cm	0.25																				n/cm3	150000000000000000000			sample crystals cleaved naturally along the ab plane of the R3[-]m lattice					An increase in Tc under hydrostatic pressure in the superconducting doped topological insulator Nb0.25Bi2Se3			Materials Science Division, Argonne National Laboratory, Argonne, IL 60439, United States	Physica C, 543(2017)58	M.P. Smylie,K. Willa,K. Ryan,H. Claus,W.-K. Kwok,Y. Qiu,Y.S. Hor,U. Welp		
157521	PRB082052502	crystals with a-axis long. RRR=30. Anisotropic thermal expansion. TCFIG shows volumetric expansion. (dTc/dP) calculated from thermal expansion using Ehrenfest relation. FM at 2.6 K.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2010							2.6																			ABC		TiNiSi																		K	0.42						0.42	MEXP157521		K/GPa	0.98																																																																																												single crystals grown bu Czochralski method					Thermal expansion of the superconducting ferromagnet UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev. B, 82(2010)052502	A. Gasparini,Y. K. Huang,J. Hartbaum,H. v. Lohneysen,A. de Visser		
157522	PRB082052502	crystals with b-axis long. RRR=40. SP (gamma-0) = 0.04 J/mol.K2, which suggest two band SC. (dC/gamma*Tc) = 0.7.	UCoGe	U1Co1Ge1	U	1	Co	1	Ge	1																		3	2010																										ABC		TiNiSi																		K	0.35						0.35																																																					MSP157522			J/mol.K2	0.062	SP																																						single crystals grown bu Czochralski method					Thermal expansion of the superconducting ferromagnet UCoGe			Van der Waals-Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018 XE Amsterdam, The Netherlands	Phys.Rev. B, 82(2010)052502	A. Gasparini,Y. K. Huang,J. Hartbaum,H. v. Lohneysen,A. de Visser		
157523	PRB083060505	Tetra-to-ortho transiton at T<STR> = 164 K, T<SDW> = 152 K.	CaFe2As2	Ca1Fe2As2	Ca	1	Fe	2	As	2																		3	2011																										AB2C2		ThCr2Si2			A	3.8977		11.755											Tetra-to-orth transition	K					4																																																																																							cm3/C						MRH157523										Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157524	PRB083060505	Coexist of SC and SDW.	CaFe2(As,P)2	Ca1Fe2As1.94P0.06	Ca	1	Fe	2	As	1.94	P	0.06																3	2011																										AB2C2		ThCr2Si2			A	3.9048		11.6493											Tetra-to-orth transition	K			11				11	MPH157524																																																																																				cm3/C						MRH157524										Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157525	PRB083060505		CaFe2(As,P)2	Ca1Fe2As1.9P0.1	Ca	1	Fe	2	As	1.9	P	0.1																3	2011																										AB2C2		ThCr2Si2																	Tetra-to-orth transition	K			12.6				12.6	MTC157525																																																																																				cm3/C						MRH157523										Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157526	PRB083060505	SC disappers. Collapsed tetragonal phase for x >= 0.055.	CaFe2(As,P)2	Ca1Fe2As1.89P0.11	Ca	1	Fe	2	As	1.89	P	0.11																3	2011																										AB2C2		ThCr2Si2			A	3.9008		11.6585											Tetra-to-cllapsed tetra transition	K					4			MPH157524																																																																																				cm3/C						MRH157524										Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157527	PRB083060505	Tetra-to-collapsed tetra transition has thermal hysteress (cooling and warming).	CaFe2(As,P)2	Ca1Fe2As1.86P0.14	Ca	1	Fe	2	As	1.86	P	0.14																3	2011																										AB2C2		ThCr2Si2			A	3.9258		11.5769											Tetra-to-cllapsed tetra transition	K			20				20	MPH157524																																																																																																				Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157528	PRB083060505	Tetra-to-collapsed tetra transition has thermal hysteress (cooling and warming).	CaFe2(As,P)2	Ca1Fe2As1.83P0.17	Ca	1	Fe	2	As	1.83	P	0.17																3	2011																										AB2C2		ThCr2Si2			A	3.8728		11.4703											Tetra-to-cllapsed tetra transition	K			28.8				28.8																																																																																																					Abrupt recovery of Fermi-liquid transport following the collapse of the c axis in CaFe2(As1-xPx)2 single crystals			Research Center for Low Temperature and Materials Sciences, Kyoto University, Kyoto 606-8501, Japan	Phys.Rev. B, 83(2011)060505	S. Kasahara,K. Hashimoto,Y. Nakai,H. Ikeda,T. Terashima,Y. Matsuda		
157529	PLA3812040	Bicrystal of Bi0.93Sn0.07 with 0.01 % Sn. bicrystal has 4.6 and 1 degree interface (small disorientation angle). Two step SC transitions (T1 and T3).	Bi1-xSbx	Bi0.93Sb0.07	Bi	0.93	Sb	0.07																					2017																																													bicrystal with small angle interface	K	4.35		8.48				6.415																				kOe	R(onset)													MHC157529																																																														Compound bicrystal seeds were prepared by cutting a single crystalline block into two parts					Coexistence of superconductivity and weak ferromagnetism at the interface of twisting bicrystals of 3D topological insulator Bi1-xSbx(0.07 <x <0.2)			Institute of Electronic Engineering and Industrial Technologies, Academy of Sciences of Moldova, 2028 Chisinau, Moldova	Phys.Lett.A, 381(2017)2040	F.M.Muntyanu,A.Gilewski,A.J.Zaleski,V.Chistol,K.Rogacki		
157530	PLA3812040	Bicrystal of Bi0.93Sn0.07 with 0.01 % Sn.  bicrystal has 75 and 4 degree interface (large disorientation angle). single step SC transition	Bi1-xSbx	Bi0.93Sb0.07	Bi	0.93	Sb	0.07																					2017																																													bicrystal with large angle interface	K			3.67				3.67																																																																																																Compound bicrystal seeds were prepared by cutting a single crystalline block into two parts					Coexistence of superconductivity and weak ferromagnetism at the interface of twisting bicrystals of 3D topological insulator Bi1-xSbx(0.07 <x <0.2)			Institute of Electronic Engineering and Industrial Technologies, Academy of Sciences of Moldova, 2028 Chisinau, Moldova	Phys.Lett.A, 381(2017)2040	F.M.Muntyanu,A.Gilewski,A.J.Zaleski,V.Chistol,K.Rogacki		
157531	PLA3812040	Bicrystal of Bi0.85Sb0.15 with Te doping.. bicrystal has 19 and 2 degree interface.	Bi1-xSbx	Bi0.85Sb0.15	Bi	0.85	Sb	0.15																					2017																																													bicrystal	K			3.45				3.45																				kOe	R(onset), WHH	3.7							kOe/K	R(onset)	1.5			MHC157531		nm	from Hc2	30																																																										Compound bicrystal seeds were prepared by cutting a single crystalline block into two parts					Coexistence of superconductivity and weak ferromagnetism at the interface of twisting bicrystals of 3D topological insulator Bi1-xSbx(0.07 <x <0.2)			Institute of Electronic Engineering and Industrial Technologies, Academy of Sciences of Moldova, 2028 Chisinau, Moldova	Phys.Lett.A, 381(2017)2040	F.M.Muntyanu,A.Gilewski,A.J.Zaleski,V.Chistol,K.Rogacki		
157532	PRB084035208	not SC. Semicond. like gap = 94 meV. Carrier shows at 0 K. DOS = 5.96 /eV.	ErPdBi	Er1Pd1Bi1	Er	1	Pd	1	Bi	1																		1	2011																										ABC		MgAgAs	F4[-]3m		A	6.5952														K					1.2																																																																				uV/K	80				uOhm.cm											900										n/f.u	0.07	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157533	PRB084035208	not SC. Semicond. like gap = 32 meV. Carrier shows at 0 K. DOS = 8.01 /eV.	HoPdBi	Ho1Pd1Bi1	Ho	1	Pd	1	Bi	1																		1	2011								2																		ABC		MgAgAs	F4[-]3m		A	6.6012														K					1.2																																																																				uV/K	50				uOhm.cm											234										n/f.u	0.17	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157534	PRB084035208	not SC. Semicond. like gap = 35 meV. Carrier shows at 0 K. DOS =24.5  /eV.	DyPdBi	Dy1Pd1Bi1	Dy	1	Pd	1	Bi	1																		1	2011								3.5																		ABC		MgAgAs	F4[-]3m		A	6.6343														K					1.2																																																																				uV/K	92				uOhm.cm											422										n/f.u	0.16	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157535	PRB084035208	not SC. Semicond. like gap = 44.5 meV. Carrier shows at 0 K. DOS = 7.85 /eV.	YPdBi	Y1Pd1Bi1	Y	1	Pd	1	Bi	1																		1	2011																										ABC		MgAgAs	F4[-]3m		A	6.6391														K					1.2																																																																				uV/K	44				uOhm.cm											293										n/f.u	0.27	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157536	PRB084035208	not SC. Semicond. like gap = 43 meV. Carrier shows at 0 K. DOS = 8.1 /eV.	GdPdBi	Gd1Pd1Bi1	Gd	1	Pd	1	Bi	1																		1	2011								13																		ABC		MgAgAs	F4[-]3m		A	6.6906														K					1.2																																																																				uV/K	79				uOhm.cm											533										n/f.u	0.13	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157537	PRB084035208	not SC. Semicond. like gap = 34.5 meV. Carrier shows at 0 K. DOS = 9.65 /eV.	NdPdBi	Nd1Pd1Bi1	Nd	1	Pd	1	Bi	1																		1	2011								4																		ABC		MgAgAs	F4[-]3m		A	6.7257														K					1.2																																																																				uV/K	69				uOhm.cm											442										n/f.u	0.12	R(3N),Pd(5N),Bi(5N)		arc-melting					Magnetic and transport properties of rare-earth-based half-Heusler phases RPdBi: Prospective systems for topological quantum phenomena			Condensed Matter and Thermal Physics, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev. B, 84(2011)035208	K. Gofryk,D. Kaczorowski,T. Plackowski,A. Leithe-Jasper,Yu. Grin		
157538	PRB086184426	impurity: RhZn6.4, Pr14Zn, total < 5 %. TCFIG shows magnetic phase diagram. Antiferroquadrupole transition T<Q> depends on B-direction (see TCFIG). Hc2(T) not given. Tc = 0.06 K  same as T<Q> at H=0.	PrRh2Zn20	Pr1Rh2Zn20	Pr	1	Rh	2	Zn	20																		3	2012					Myu-B/f.u.	3.55	-4.8																			AB2C20		CeCr2Al20			A	14.2702														K	0.06						0.06	MPH157538									50																																																																																				Pr(4N),Rh(3N),Zn(6N)		Zn-self flux method					Simultaneous superconducting and antiferroquadrupolar transitions in PrRh2Zn20			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Phys.Rev. B, 86(2012)184426	T. Onimaru,N. Nagasawa,K. T. Matsumoto,K. Wakiya,K. Umeo,S. Kittaka,T. Sakakibara,Y. Matsushita,T. Takabatake		
157539	PRB087180502	1.4 GeV <208>Pb ion irradiation. [penet] measured by TDR, absolute value not given. gap size (d/kTc) = 0.99 and 0.81 for irradiation 2T and 4T, obtained by analysis of T-dependence of d[penet].	Ba0.6K0.4Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2013																										AB2C2		ThCr2Si2																		K		39					39																																									nm	TDR						1.98	1																																																				Effect of heavy-ion irradiation on superconductivity in Ba0.6K0.4Fe2As2			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 87(2013)180502	N. W. Salovich,Hyunsoo Kim,Ajay K. Ghosh,R. W. Giannetta,W. Kwok,U. Welp,B. Shen,S. Zhu,H.-H. Wen,M. A. Tanatar,R. Prozorov		
157540	PRB087180502	1.4 GeV <208>Pb ion irradiation. columnar distance = 10 nm, fluence = 1.0E+12 ions/cm2.s (columnar defect density = 21 T) not change Tc. [penet] not given, only d[penet](T)	Ba0.6K0.4Fe2As2	Ba0.6K0.4Fe2As2	Ba	0.6	K	0.4	Fe	2	As	2																3	2013																										AB2C2		ThCr2Si2																		K		36.8					36.8																																									nm	TDR																																																											Effect of heavy-ion irradiation on superconductivity in Ba0.6K0.4Fe2As2			Loomis Laboratory of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801, USA	Phys.Rev.B, 87(2013)180502	N. W. Salovich,Hyunsoo Kim,Ajay K. Ghosh,R. W. Giannetta,W. Kwok,U. Welp,B. Shen,S. Zhu,H.-H. Wen,M. A. Tanatar,R. Prozorov		
157541	PRB088054514	d[penet] measured by TDR, [penet] values not given. d[penet] = A*T^n, n(Tc/3) = 2.59, 2.39, for before and after Pb-ion irradiation. small but clear decrease inTc after irradiation	Ba(Fe,Co)2As2	Ba1Fe1.784Co0.216As2	Ba	1	Fe	1.784	Co	0.216	As	2																3	2013																										AB2C2		ThCr2Si2																		K		16					16																				T	R(mid), Linear approx.			30										MHC157541																																																														FeAs-flux method					Effect of heavy-ion irradiation on London penetration depth in overdoped Ba(Fe1-xCox)2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev. B, 88(2013)054514	J. Murphy,M. A. Tanatar,Hyunsoo Kim,W. Kwok,U. Welp,D. Graf,J. S. Brooks,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
157542	PRB088054514	d[penet] measured by TDR, [penet] values not given. d[penet] = A*T^n, n(Tc/3) = 2.04, 1.94, for before and after Pb-ion irradiation. small but clear decrease inTc after irradiation	Ba(Fe,Co)2As2	Ba1Fe1.746Co0.254As2	Ba	1	Fe	1.746	Co	0.254	As	2																3	2013																										AB2C2		ThCr2Si2																		K		8					8																				T	R(mid), Linear approx.			10										MHC157542																																																														FeAs-flux method					Effect of heavy-ion irradiation on London penetration depth in overdoped Ba(Fe1-xCox)2As2			Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev. B, 88(2013)054514	J. Murphy,M. A. Tanatar,Hyunsoo Kim,W. Kwok,U. Welp,D. Graf,J. S. Brooks,S. L. Bud'ko,P. C. Canfield,R. Prozorov		
157543	PRB093134507	RRR = 1.1. SP (beta) = 0.29 mJ/mol.K4, (delta) = 4.96 uJ/mol.K6. (dC/gamma*Tc) = 1.46. e-ph = 0.41	ScV2Al20	Sc1V2Al20	Sc	1	V	2	Al	20																		1	2016									2.993																	AB2C20		CeCr2Al20			A	14.4978														K		1.03		1			1.03																				T	R(mid), WHH	0.333							T/K	R(mid)	0.482					A	from Hc2	314															MSP157543			mJ/mol.K2	29.6	SP	536																																			R(3N),V(2N8),Al(5N)		arc-melting(R:V:Al = 1:2:20/3) - 2nd arc-melting with addition of remaining Al - sealed in quartz tube - ANN(650C, 3w) - Q to water(RT)					Rattling-enhanced superconductivity in MV2Al20 (M = Sc, Lu, Y) intermetallic cage compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev. B, 93(2016)134507	M. J. Winiarski,B. Wiendlocha,M. Sternik,P. Wisniewski,J. R. O'Brien,D. Kaczorowski,T. Klimczuk		
157544	PRB093134507	RRR = 7.2. SP (beta) = 0.32 mJ/mol.K4, (delta) = 0.33 uJ/mol.K6. (dC/gamma*Tc) = 1.24. e-ph = 0.39	YV2Al20	Y1V2Al20	Y	1	V	2	Al	20																		1	2016									3.158																	AB2C20		CeCr2Al20			A	14.5378														K		0.61		0.6			0.61																				T	R(mid), WHH	0.028							T/K	R(mid)	0.067					A	from Hc2	1084															MSP157544			mJ/mol.K2	26.5	SP	516																																			R(3N),V(2N8),Al(5N)		arc-melting(R:V:Al = 1:2:20/3) - 2nd arc-melting with addition of remaining Al - sealed in quartz tube - ANN(650C, 3w) - Q to water(RT)					Rattling-enhanced superconductivity in MV2Al20 (M = Sc, Lu, Y) intermetallic cage compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev. B, 93(2016)134507	M. J. Winiarski,B. Wiendlocha,M. Sternik,P. Wisniewski,J. R. O'Brien,D. Kaczorowski,T. Klimczuk		
157545	PRB093134507	RRR = 12.2. SP (beta) = 0.3 mJ/mol.K4, (delta) = 0.525 uJ/mol.K6.	LaV2Al20	La1V2Al20	La	1	V	2	Al	20																		1	2016									3.316																	AB2C20		CeCr2Al20			A	14.6212														K					0.48																																																										mJ/mol.K2	19.6	SP	525																																			R(3N),V(2N8),Al(5N)		arc-melting(R:V:Al = 1:2:20/3) - 2nd arc-melting with addition of remaining Al - sealed in quartz tube - ANN(650C, 3w) - Q to water(RT)					Rattling-enhanced superconductivity in MV2Al20 (M = Sc, Lu, Y) intermetallic cage compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev. B, 93(2016)134507	M. J. Winiarski,B. Wiendlocha,M. Sternik,P. Wisniewski,J. R. O'Brien,D. Kaczorowski,T. Klimczuk		
157546	PRB093134507	RRR = 3.6. SP (beta) = 0.31 mJ/mol.K4, (delta) = 0.64 uJ/mol.K6. (dC/gamma*Tc) = 1.29. e-ph = 0.39	LuV2Al20	Lu1V2Al20	Lu	1	V	2	Al	20																		1	2016									3.548																	AB2C20		CeCr2Al20			A	14.513														K		0.6		0.57			0.6																				T	R(mid), WHH	0.207							T/K	R(mid)	0.501					A	from Hc2	399															MSP157546			mJ/mol.K2	30.1	SP	502																																			R(3N),V(2N8),Al(5N)		arc-melting(R:V:Al = 1:2:20/3) - 2nd arc-melting with addition of remaining Al - sealed in quartz tube - ANN(650C, 3w) - Q to water(RT)					Rattling-enhanced superconductivity in MV2Al20 (M = Sc, Lu, Y) intermetallic cage compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev. B, 93(2016)134507	M. J. Winiarski,B. Wiendlocha,M. Sternik,P. Wisniewski,J. R. O'Brien,D. Kaczorowski,T. Klimczuk		
157547	PRB093174513	La-content =0.27 by WDS. T<STR>(monoclinic-to-triclinic) = 58 K.	Ca0.74La0.26FeAs2	Ca0.74La26Fe1As2	Ca	0.74	La	26	Fe	1	As	2																3	2016								54																		ABC2		Fe-112			A			10.3897												K					2																																																																																																		self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157548	PRB093174513	La-content =0.25 by WDS.  T<STR>(monoclinic-to-triclinic) = 48.3 K.	Ca0.74La0.26(Fe,Co)As2	Ca0.74La26Fe0.992Co0.008As2	Ca	0.74	La	26	Fe	0.992	Co	0.008	As	2														3	2016								44.4																		ABC2		Fe-112			A			10.3818												K					2																																																																																																		self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157549	PRB093174513	La-content =0.269 by WDS. T<STR>(monoclinic-to-triclinic) = 36.3 K.	Ca0.74La0.26(Fe,Co)As2	Ca0.74La26Fe0.975Co0.025As2	Ca	0.74	La	26	Fe	0.975	Co	0.025	As	2														3	2016								30.2																		ABC2		Fe-112			A			10.3845												K		11.2		11.1			11.2																																																																							mOhm.cm							0.134																		self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157550	PRB093174513	La-content =0.249 by WDS. Anisotropy (Hc2) = 4.7, SP (dC/Tc) = 6.7 mJ/mol-Fe.K2.	Ca0.74La0.26(Fe,Co)As2	Ca0.74La26Fe0.954Co0.046As2	Ca	0.74	La	26	Fe	0.954	Co	0.046	As	2														3	2016																										ABC2		Fe-112			A			10.3693												K		21.5		19.3			21.5	MPH157550																			T	R(mid)													MHC157550																																																														self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157551	PRB093174513	La-content =0.270 by WDS.	Ca0.74La0.26(Fe,Co)As2	Ca0.74La26Fe0.935Co0.065As2	Ca	0.74	La	26	Fe	0.935	Co	0.065	As	2														3	2016																										ABC2		Fe-112			A			10.3667												K		16.2		16.4			16.2																																																																																																self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157552	PRB093174513	La-content =0.259 by WDS.	Ca0.74La0.26(Fe,Co)As2	Ca0.74La26Fe0.967Co0.033As2	Ca	0.74	La	26	Fe	0.967	Co	0.033	As	2														3	2016					myu-B/Fe	0.6																				ABC2		Fe-112			A			10.377												K		15.6		18.6			15.6																																																																																																self-flux (CaAs:LaAs:FeAs:CoAs:As = 1.3:0.5:(1-x):x:0.7) method					Effect of interlayer coupling on the coexistence of antiferromagnetism and superconductivity in Fe pnictide superconductors: A study of Ca0.74(1)La0.26(1)(Fe1-xCox)As2 single crystals			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev. B, 93(2016)174513	Shan Jiang,Lian Liu,Michael Schutt,Alannah M. Hallas,Bing Shen,Wei Tian,Eve Emmanouilidou,Aoshuang Shi,Graeme M. Luke,Yasutomo J. Uemura,Rafael M. Fernandes,Ni Ni		
157553	PRB095174522	optical Ir-doped sample. Two gaps (d1 = 0.97 meV and d2 in DB) obtained by optical reflectivity measurements.	Eu(Fe,Ir)2As2	Eu1Fe1.82Ir0.18As2	Eu	1	Fe	1.82	Ir	0.18	As	2																3	2017																										AB2C2		ThCr2Si2																		K	18.9		21				19.95																																														meV	1.18		15																						uOhm.cm								92.7				237													self-flux method					Reentrant phases in electron-doped EuFe2As2: Spin glass and superconductivity			I. Physikalisches Institut, Universitut Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany	Phys.Rev. B, 95(2017)174522	A. Baumgartner,D. Neubauer,S. Zapf,A. V. Pronin,W. H. Jiao,G. H. Cao,M. Dressel		
157554	PRB095174522	Reentrant SC in R(T) measurement. R(max) at 15K below Tc(=19.6 K. Two gaps (d1 = 2.3 meV and d2 in DB) obtained by optical reflectivity measurements.	Eu(Fe,Rh)2As2	Eu1Fe1.86Rh0.14As2	Eu	1	Fe	1.86	Rh	0.14	As	2																3	2017																										AB2C2		ThCr2Si2																		K	9.1		19.6				14.35																																														meV	2.65		15																						uOhm.cm								92.7				204													self-flux method					Reentrant phases in electron-doped EuFe2As2: Spin glass and superconductivity			I. Physikalisches Institut, Universitut Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart, Germany	Phys.Rev. B, 95(2017)174522	A. Baumgartner,D. Neubauer,S. Zapf,A. V. Pronin,W. H. Jiao,G. H. Cao,M. Dressel		
157555	PRB095180503	Impurity phase = BiNb2Se3	NbxBi2Se3	Nb0.05Bi2Se3	Nb	0.05	Bi	2	Se	3																		3	2017																													R-3m																rhombohedral Bi2Se3 structure	K			2.57				2.57																				T	ARPES, WHH			0.75																																																																						Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157556	PRB095180503		NbxBi2Se3	Nb0.2Bi2Se3	Nb	0.2	Bi	2	Se	3																		3	2017																													R-3m																rhombohedral Bi2Se3 structure	K			3.27				3.27																				T	ARPES, WHH			0.63																																																																						Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157557	PRB095180503	(Bi2)m(Bi2Se3)n structure Nb dope in (Bi2) layer. Two set of Hc2(T) shown in HCFIG.	NbxBi2Se3	Nb0.25Bi2Se3	Nb	0.25	Bi	2	Se	3																		3	2017																																														K			3.31				3.31																					ARPES, WHH			1.8										MHC157557																																																												Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157558	PRB095180503		NbxBi2Se3	Nb0.3Bi2Se3	Nb	0.3	Bi	2	Se	3																		3	2017																																														K			3.47	3.27			3.27																																																																							uOhm.cm								219															Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157559	PRB095180503	(Bi2)m(Bi2Se3)n structure Nb dope in (Bi2) layer	NbxBi2Se3	Nb0.4Bi2Se3	Nb	0.4	Bi	2	Se	3																		3	2017																																														K			3.52				3.52																				T	ARPES, WHH													MHC157559																																																												Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157560	PRB095180503	(Bi2)m(Bi2Se3)n structure Nb dope in (Bi2) layer	NbxBi2Se3	Nb1Bi2Se3	Nb	1	Bi	2	Se	3																		3	2017																																														K			2.9				2.9																				T	ARPES, WHH													MHC157560																																																												Nb(4N),Bi,Se		mixture - sealed in quartz tube - heat(800C) - slow cool to 650C for 5h - Q to ice water					Unusual upper critical field behavior in Nb-doped bismuth selenides			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev. B, 95(2017)180503	Kaya Kobayashi,T. Ueno,H. Fujiwara,T. Yokoya,J. Akimitsu		
157561	PRB095184501	[penet] measured by TDO. gap size obtained using two gap model (small d(0) = 1.25 kTc, large (inDB) ) analysis of [penet](T).	Lu3Os4Ge13	Lu3Os4Ge13	Lu	3	Os	4	Ge	13																		3	2017																										A3B4C12		Yb3Rh4Ge13	Pm3[-]n																	K		3.2		3.05			3.2																				T	RES(mid), extrapolation	4.8												MHC157561							A	TDO, s-wave model	4736					5																																																Crystals grown using Czochralski method in tetra-arc furnace underAr atmosphere					Nodeless superconductivity and the peak effect in the quasiskutterudites Lu3Os4Ge13 and Y3Ru4Ge13			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev. B, 95(2017)184501	Z. F. Weng,M. Smidman,G. M. Pang,O. Prakash,Y. Chen,Y. J. Zhang,S. Ramakrishnan,H. Q. Yuan		
157562	PRB095184501	[penet] measured by TDO. gap size obtained using two gap model (small d(0) = 1.4 kTc, large (inDB) ) analysis of [penet](T).	Y3Ru4Ge13	Y3Ru4Ge13	Y	3	Ru	4	Ge	13																		3	2017																										A3B4C12		Yb3Rh4Ge13	Pm3[-]n																	K		2.8		2.3			2.8																				T	RES(mid), extrapolation	3.4												MHC157562							A	TDO, s-wave model	4951					4.3																																																Crystals grown using Czochralski method in tetra-arc furnace underAr atmosphere					Nodeless superconductivity and the peak effect in the quasiskutterudites Lu3Os4Ge13 and Y3Ru4Ge13			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev. B, 95(2017)184501	Z. F. Weng,M. Smidman,G. M. Pang,O. Prakash,Y. Chen,Y. J. Zhang,S. Ramakrishnan,H. Q. Yuan		
157563	PRB095184514	RRR=5.  SP (beta) = 0.96 mJ/mol.K4. gamma(8.55) = gamma(n) in DB * gamma(0) (1.53mJ/mol.K2). (dC/gamma(n)*Tc) = 1.50. Hc(0) = 18mT. kappa(GL) = 25. e-ph = 0.48	Ag2Pd3S	Ag2Pd3S1	Ag	2	Pd	3	S	1																		3	2017																										AB2C3		beta-Mn	P4<1>32		A	7.2292														K			2.25				2.25										40	Oe	M-H curve				3.5			1.8	T	RES(onset), linear approx.	0.63												MHC157563		nm	from Hc2	23			nm	Hc, GL model	568					3.48	14				MSP157563			mJ/mol.K2	7.02	SP	230	SP											uOhm.cm	62.1																						Ag2S,Pd		self-flux method. mixture(Ag2S:Pd = 1:3) - pellet - sealed in quartz tube - heat(1000C,48h) - slow cool to 500 C(5C/h) - Q to RT					Superconductivity in noncentrosymmetric Ag2Pd3S			National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan	Phys.Rev. B, 95(2017)184514	H. Yoshida,H. Okabe,Y. Matsushita,M. Isobe,E. Takayama-Muromachi		
157564	PRB095195146	RRR = 2.2. spin-glass, T<SG> = 14.1 K. T<SG> goes to zero at H = 250 Oe.  Hc2(T) shows for H//ab.	Eu(Fe0.93Rh0.07)2As2	Eu1Fe1.86Rh0.14As2	Eu	1	Fe	1.86	Rh	0.14	As	2																3	2017								16.6																		AB2C2		ThCr2Si2																		K	5.4		19.8				12.6																				T	RES(onset), linear approx.		12											MHC157564																																																														self-flux method					Effects of pressure and magnetic field on the reentrant superconductor Eu(Fe0.93Rh0.07)2As2			1. Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, D-70569 Stuttgart, Germany	Phys.Rev. B, 95(2017)195146	A. Lohle,A. Baumgartner,S. Zapf,M. Dressel,W. H. Jiao,G. H. Cao		
157565	PRB095195146	RRR = 2.2. spin-glass, T<SG> = 14.1 K. T<SG> goes to zero at H = 250 Oe.  Hc2(T) shows for H//c.	Eu(Fe0.93Rh0.07)2As2	Eu1Fe1.86Rh0.14As2	Eu	1	Fe	1.86	Rh	0.14	As	2																3	2017								16.6																		AB2C2		ThCr2Si2																		K	5.4		19.8				12.6																				T	RES(onset), linear approx.			10										MHC157565																																																														self-flux method					Effects of pressure and magnetic field on the reentrant superconductor Eu(Fe0.93Rh0.07)2As2			1. Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, D-70569 Stuttgart, Germany	Phys.Rev. B, 95(2017)195146	A. Lohle,A. Baumgartner,S. Zapf,M. Dressel,W. H. Jiao,G. H. Cao		
157566	PRB095195146	Pressure effects measured. For low T, coexistence of SC and c-axis FM components. For low T, n (R(T) = R0 + A*T^n) shown in MTC157566(dat)	Eu(Fe0.93Rh0.07)2As2	Eu1Fe1.86Rh0.14As2	Eu	1	Fe	1.86	Rh	0.14	As	2																3	2017								16.6																		AB2C2		ThCr2Si2																		K	5.4		19.8				12.6	MPH157566																																																																																															self-flux method					Effects of pressure and magnetic field on the reentrant superconductor Eu(Fe0.93Rh0.07)2As2			1. Physikalisches Institut, Universitat Stuttgart, Pfaffenwaldring 57, D-70569 Stuttgart, Germany	Phys.Rev. B, 95(2017)195146	A. Lohle,A. Baumgartner,S. Zapf,M. Dressel,W. H. Jiao,G. H. Cao		
157567	PRB095224506	[penet] = 140 nm(in DB) at H=250Oe, = 180 nm at H=400 Oe. Two-gap model, d1 = 0.399 meV (n DB) and d2 = 0.109 meV (2d2/kTc) = 0.71. From muon-SR.	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																			2017																										ABC2			P6[-]m2																	K				3.6			3.6										77	Oe	M-H curve				40			0.5	T	M-H curve				0.1			0.5													nm	muon-SR	140			meV	0.399	2.57	16																																															(preheated-PbTaSe2 + PbCl2) - CVT(850 C)					Muon-SR study of the noncentrosymmetric superconductor PbTaSe2			Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1	Phys.Rev. B, 95(2017)224506	M. N. Wilson,A. M. Hallas,Y. Cai,S. Guo,Z. Gong,R. Sankar,F. C. Chou,Y. J. Uemura,G. M. Luke		
157568	PRB095220501	data for H//ab. Commensurate-incommensurate transition at 473K. T<CDW> =   dTc/dP shows for Tc(onset). Tc(on) = 5.3, Tc(zero) = 4.6 K at P = 15 GPa. T<CDW> = 472 K.	1T-TaSe2	Se2Ta1	Se	2	Ta	1																				3	2017																										AB2		TX2	P3[-]m1	164															1T-TaSe2	K								MPH157568		K/GPa	0.148																																																																																												single crystals grown by chemical vapor transport using iodine agent.					Pressure-induced bulk superconductivity in a layered transition-metal dichalcogenide 1T-tantalum selenium			Institute for Solid State Physics, University of Tokyo, Kashiwanoha 5-1-5, Kashiwa, Chiba 277-8581, Japan	Phys.Rev. B, 95(2017)220501	Bosen Wang,Yu Liu,Kento Ishigaki,Kazuyuki Matsubayashi,Jinguang Cheng,Wenjian Lu,Yuping Sun,Yoshiya Uwatoko		
157569	PRB095220501	data for H//c	1T-TaSe2	Se2Ta1	Se	2	Ta	1																				3	2017																										AB2		TX2	P3[-]m1	164															1T-TaSe2	K								MPH157569		K/GPa	0.231																																																																																												single crystals grown by chemical vapor transport using iodine agent.					Pressure-induced bulk superconductivity in a layered transition-metal dichalcogenide 1T-tantalum selenium			Institute for Solid State Physics, University of Tokyo, Kashiwanoha 5-1-5, Kashiwa, Chiba 277-8581, Japan	Phys.Rev. B, 95(2017)220501	Bosen Wang,Yu Liu,Kento Ishigaki,Kazuyuki Matsubayashi,Jinguang Cheng,Wenjian Lu,Yuping Sun,Yoshiya Uwatoko		
157570	PRB095224508	RRR = 115-120. (Hc2/dT) defined as R(onset)	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2017																										ABC2			P6[-]m2		A	3.415		9.382												K	3.9		3.96	3.79			3.79	MTC157570																												kOe/K	R(on)			96	MHC157570																									204	R(T)																																				Sngle crystals grown by chemical vapor transport using PbCl2 as  agent					Highly responsive ground state of PbTaSe2: Structural phase transition and evolution of superconductivity under pressure			Ames Laboratory, US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev. B, 95(2017)224508	Udhara S. Kaluarachchi,Yuhang Deng,Matthew F. Besser,Kewei Sun,Lin Zhou,Manh Cuong Nguyen,Zhujun Yuan,Chenglong Zhang,James S. Schilling,Matthew J. Kramer,Shuang Jia,Cai-Zhuang Wang,Kai-Ming Ho,Paul C. Canfield,Sergey L. Bud'ko		
157571	PRB095224508	(Hc2/dT) defined as R(onset). Phase boundary. sample has two Tc, Tc(zero) = 3.75 and 2.81 K.	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2017																										ABC2			P6[-]m2																	K	3.75		3.78	3.11			3.11	MPH157571																												kOe/K	R(on)			0.45	MHC157571																									215	R(T)																																				Sngle crystals grown by chemical vapor transport using PbCl2 as  agent					Highly responsive ground state of PbTaSe2: Structural phase transition and evolution of superconductivity under pressure			Ames Laboratory, US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev. B, 95(2017)224508	Udhara S. Kaluarachchi,Yuhang Deng,Matthew F. Besser,Kewei Sun,Lin Zhou,Manh Cuong Nguyen,Zhujun Yuan,Chenglong Zhang,James S. Schilling,Matthew J. Kramer,Shuang Jia,Cai-Zhuang Wang,Kai-Ming Ho,Paul C. Canfield,Sergey L. Bud'ko		
157572	PRB095224508	MDEB157572 shows P-dependence of Debye-T obtained from R(T).	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2017																										ABC2			P6[-]m2																	K	2.07		2.21				2.14	MDEB157572																												kOe/K	R(on)			1.65																										220	R(T)																																				Sngle crystals grown by chemical vapor transport using PbCl2 as  agent					Highly responsive ground state of PbTaSe2: Structural phase transition and evolution of superconductivity under pressure			Ames Laboratory, US DOE, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev. B, 95(2017)224508	Udhara S. Kaluarachchi,Yuhang Deng,Matthew F. Besser,Kewei Sun,Lin Zhou,Manh Cuong Nguyen,Zhujun Yuan,Chenglong Zhang,James S. Schilling,Matthew J. Kramer,Shuang Jia,Cai-Zhuang Wang,Kai-Ming Ho,Paul C. Canfield,Sergey L. Bud'ko		
157573	PRB095235149	P-induced SC. optimal P = 16 GPa(Tc(max) = 4.2 K). T<CDW> = 80 K(P=0). P-dependence of T<CDW> in MTC157573. R(T), s(T), k(T) are measured.	beta-Bi4I4	Bi4I4	Bi	4	I	4																				3	2017																										A4B4																				K			4.2		0		4.2	MTC157573																																																																																															Single crystals obtained by chemical reaction method using (Bi + HgI2) powders as a starting materials					Pressure effect and superconductivity in the beta-Bi4I4 topological insulator			Institute of Physics, Ecole Polytechnique Federale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland	Phys.Rev. B, 95(2017)235149	A. Pisoni,R. Gaal,A. Zeugner,V. Falkowski,A. Isaeva,H. Huppertz,G. Autes,O. V. Yazyev,L. Forro		
157575	PRB095241109	P-induced SC. P<cr> = 12.7GPa, SC for 12.7 =< P < 15 GPa.	BaFe2S3	Ba1Fe2S3	Ba	1	Fe	2	S	3																		3	2017																										AB2C3			Pnma																CsAg2I3 type structure,  Fe ladder compound	K			11.2		0		11.2	MTC157575																			T	RES(onset), WHH	15.5							T/K	R(onset)	2.16			MHC157575																																																														Singe crystals grown by self-flux method					Interplay of magnetism and superconductivity in the compressed Fe-ladder compound BaFe2Se3			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, USA	Phys.Rev. B, 95(2017)241109	Jianjun Ying,Hechang Lei,Cedomir Petrovic,Yuming Xiao,Viktor V. Struzhkin		
157576	PRB096014504	d[penet](T) measured by TDO for H//ab. exponent of [penet] = 2.83. Analysis of d[penet](T) shows good fit to two gap model (gap size = 1.6 and 3.8 , alpha = 0.13)	(Li0.8Fe0.2)OHFeSe	Li0.8Fe1.2H1Se1O1	Li	0.8	Fe	1.2	H	1	Se	1													O	1			2017																																														K				40			40										100										T		79														nm	from Hc2	2			A	d[penet](T) analysis for T < 0.2Tc	636					174																							mOhm.cm								0.1																						Probing the superconducting gap structure of (Li1-xFex)OHFeSe			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev. B, 96(2017)014504	M. Smidman,G. M. Pang,H. X. Zhou,N. Z. Wang,W. Xie,Z. F. Weng,Y. Chen,X. L. Dong,X. H. Chen,Z. X. Zhao,H. Q. Yuan		
157577	PRB096014504	some inhomogeneity. d[penet](T) measured by TDO for H//ab. exponent of [penet] = 2.46.	(Li0.8Fe0.2)OHFeSe	Li0.8Fe1.2H1Se1O1	Li	0.8	Fe	1.2	H	1	Se	1													O	1			2017																																														K				37			37										100	mT	M-H curve				4.5			2																						A	d[penet](T) analysis for T < 0.2Tc	1228					156																																												n/cm3	1040000000000000000000								Probing the superconducting gap structure of (Li1-xFex)OHFeSe			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev. B, 96(2017)014504	M. Smidman,G. M. Pang,H. X. Zhou,N. Z. Wang,W. Xie,Z. F. Weng,Y. Chen,X. L. Dong,X. H. Chen,Z. X. Zhao,H. Q. Yuan		
157578	PRB096014507	(dC/gamma*Tc) = 0.86. e-ph = 0.493. DOS = 2.38 /eV.fu.	ThCoC2	Th1Co1C2	Th	1	Co	1	C	2																		1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8044	4.5275	6.1401												K		2.47	2.63	2.59			2.47	MTC157582																			T	RES(onset),													MHC157579																			MSP157578			mJ/mol.K2	8.38	SP	449	SP																																				Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157579	PRB096014507	(dC/gamma*Tc) = 0.36. e-ph = 0.553. DOS = 2.92 /eV.fu.	Th(Co,Ni)C2	Th1Co0.9Ni0.1C2	Th	1	Co	0.9	Ni	0.1	C	2																1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8194	4.5268	6.1396												K		4.38	4.22	4.51			4.38																				T	RES(onset),													MHC157579																			MSP157579			mJ/mol.K2	10.7	SP	454	SP											uOhm.cm							29				159														Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157580	PRB096014507	(dC/gamma*Tc) = 0.95. e-ph = 0.610. DOS = 3.08 /eV.fu.	Th(Co,Ni)C2	Th1Co0.8Ni0.2C2	Th	1	Co	0.8	Ni	0.2	C	2																1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8209	4.5242	6.1383												K		7.65	7.76	7.82			7.65																				T	RES(onset),													MHC157582																			MSP157580			mJ/mol.K2	11.7	SP	542	SP											uOhm.cm							48.1				137.4														Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157581	PRB096014507	(dC/gamma*Tc) = 1.25. e-ph = 0.677. DOS = 3.16 /eV.fu.	Th(Co,Ni)C2	Th1Co0.7Ni0.3C2	Th	1	Co	0.7	Ni	0.3	C	2																1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8229	4.52	6.1402												K		10.34	10.24	10.53			10.34																				T	RES(onset),													MHC157582																			MSP157581			mJ/mol.K2	12.5	SP	520	SP											uOhm.cm							90.9				188														Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157582	PRB096014507	(dC/gamma*Tc) = 1.23. e-ph = 0.681. DOS = 3.46 /eV.fu.	Th(Co,Ni)C2	Th1Co0.6Ni0.4C2	Th	1	Co	0.6	Ni	0.4	C	2																1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8379	4.5167	6.1414												K		11.83	12.08	11.93			11.83	MTC157582																			T	RES(onset),													MHC157582																			MSP157582			mJ/mol.K2	13.7	SP	584	SP											uOhm.cm							90.9				247.5														Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157583	PRB096014507		Th(Co,Ni)C2	Th1Co0.5Ni0.5C2	Th	1	Co	0.5	Ni	0.5	C	2																1	2017																										ABC2	3	CeNiC2	Amm2		A	3.8462	4.5115	6.1431												K		10.96	11.82	11.31			10.96																																																																							uOhm.cm							68.1				147.8														Arc-melting several times. ANN(1100C,2w, in evacuated quartz tube)					Tuning of superconductivity by Ni substitution into noncentrosymmetric ThCo1-xNixC2			Department of Physics and Astronomy, University of California?Irvine, Irvine, California 92697, USA	Phys.Rev. B, 96(2017)014507	T. W. Grant,O. V. Cigarroa,P. F. S. Rosa,A. J. S. Machado,Z. Fisk		
157584	PRL093247004	Li:Pd:B = 1.90:2.97:1 by ICP. Hc2(0) = 6.2T using linear approx.	Li2Pd3B	Li2Pd3B1	Li	2	Pd	3	B	1																		1	2004																										AB2C3					A	6.7523													cubic, 6.7436 A at 7.6 K. composd of distorted Pd6B octahedron	K			8.2	8		0.6	8																				T	RES(on),WHH	4.8							T/K	R(on), T<7 K.	0.84			MHC157584																																																														arc melting					Superconductivity in the Metal Rich Li-Pd-B Ternary Boride			Institute for Materials Research, Tohoku University, 2-1-1, Katahira, Aoba-ku, Sendai 980-8577, Japan	Phys.Rev.Lett., 93(2004)247004	K. Togano,P. Badica,Y. Nakamori,S. Orimo,H. Takeya,K. Hirata		
157585	SSS0680032	Compositions, Nb:Os:Si = 32:33:35 by EDX,  SUS(300) = 6.0E-5 emu/mol. molar weight = 311.2g/mol. unit cell = 0.1781 nm3	NbOsSi	Nb1Os1Si1	Nb	1	Os	1	Si	1																		1	2017									11.61																	ABC		TiNiSi	Pnma		A	6.2978	3.8872	7.2748												K	3.2			3.3			3.3											Oe	M-H curve				35			2.5																																																				uOhm.cm											0.617														arc-melting method. mixture(1:1:1) - pellet  - arc melting (several times) - ANN(1223K, 2days, in muffle furnace) - slow cool to RT (5K/h)					NbOsSi and TaOsSi - Two new superconducting ternary osmium silicides			Institut fur Anorganische und Analytische Chemie, Universitat Munster, Corrensstrasse 30, D-48149 Munster, Germany	Solid State Science, 68(2017)32	Christopher Benndorf,Lukas Heletta,Gunter Heymann,Hubert Huppertz,Hellmut Eckert,Rainer Pottgen		
157586	SSS0680032	Compositions, Ta:Os:Si = 31:34:25 by EDX,  SUS(300) = 8.9 E-5 emu/mol. molar weight = 399.2g/mol. unit cell = 0.1772 nm3	TaOsSi	Ta1Os1Si1	Ta	1	Os	1	Si	1																		1	2017									14.96																	ABC		TiNiSi	Pnma		A	6.268	3.8936	7.2922												K	5.4			5.5			5.5											Oe	M-H curve				67			2.5																																																																													arc-melting method. mixture(1:1:1) - pellet  - arc melting (several times) - ANN(1223K, 2days, in muffle furnace) - slow cool to RT (5K/h)					NbOsSi and TaOsSi - Two new superconducting ternary osmium silicides			Institut fur Anorganische und Analytische Chemie, Universitat Munster, Corrensstrasse 30, D-48149 Munster, Germany	Solid State Science, 68(2017)32	Christopher Benndorf,Lukas Heletta,Gunter Heymann,Hubert Huppertz,Hellmut Eckert,Rainer Pottgen		
157587	SSS0680032	SC not measured. Compositions, Zr:Os:Si = 29:34:35 by EDX,  molar weight = 309.5 g/mol. unit cell = 0.1925 nm3	ZrOsSi	Zr1Os1Si1	Zr	1	Os	1	Si	1																		1	2017									10.68																	ABC		TiNiSi	Pnma		A	6.4046	4.0407	7.4366												K																																																																																																							arc-melting method. mixture(1:1:1) - pellet  - arc melting (several times) - ANN(1223K, 2days, in muffle furnace) - slow cool to RT (5K/h)					NbOsSi and TaOsSi - Two new superconducting ternary osmium silicides			Institut fur Anorganische und Analytische Chemie, Universitat Munster, Corrensstrasse 30, D-48149 Munster, Germany	Solid State Science, 68(2017)32	Christopher Benndorf,Lukas Heletta,Gunter Heymann,Hubert Huppertz,Hellmut Eckert,Rainer Pottgen		
157588	SSS0680032	SC not measured. Compositions, Zr:Ir:Si = 30:32:?  by EDX,  molar weight = 311.5 g/mol. unit cell = 0.1910 nm3	ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																		1	2017									10.84																	ABC		TiNiSi	Pnma		A	6.5348	3.9535	7.3919												K																																																																																																							arc-melting method. mixture(1:1:1) - pellet  - arc melting (several times) - ANN(1223K, 2days, in muffle furnace) - slow cool to RT (5K/h)					NbOsSi and TaOsSi - Two new superconducting ternary osmium silicides			Institut fur Anorganische und Analytische Chemie, Universitat Munster, Corrensstrasse 30, D-48149 Munster, Germany	Solid State Science, 68(2017)32	Christopher Benndorf,Lukas Heletta,Gunter Heymann,Hubert Huppertz,Hellmut Eckert,Rainer Pottgen		
157589	SSS0680032	SC not measured. Compositions, Hf:Ir:Si = 27:48:38 by EDX,  molar weight = 398.8 g/mol. unit cell = 0.1874 nm3	HfIrSi	Hf1Ir1Si1	Hf	1	Ir	1	Si	1																		1	2017									14.13																	ABC		TiNiSi	Pnma		A	6.4634	3.9357	7.368												K																																																																																																							arc-melting method. mixture(1:1:1) - pellet  - arc melting (several times) - ANN(1223K, 2days, in muffle furnace) - slow cool to RT (5K/h)					NbOsSi and TaOsSi - Two new superconducting ternary osmium silicides			Institut fur Anorganische und Analytische Chemie, Universitat Munster, Corrensstrasse 30, D-48149 Munster, Germany	Solid State Science, 68(2017)32	Christopher Benndorf,Lukas Heletta,Gunter Heymann,Hubert Huppertz,Hellmut Eckert,Rainer Pottgen		
157590	SST027035004	RRR (R300/R4) = 218. SP (beta)= 0.0856 mJ/mol.K4. (delta) = 5.59E-4 mJ/mol.K6. (dC<e>/gamma*Tc) = 0.86	ThCoC2	Th1Co1C2	Th	1	Co	1	C	2																		1	2014																										ABC2		CeNiC2	Amm2	38	A	3.8053	4.5321	6.1424												K	2.55	2.65		2.55		0.2	2.65										110										T	RES(mid)													MHC157590																			MSP157590			mJ/mol.K2	8.38	SP	449	SP											uOhm.cm	0.37																						Th(3N),Co(4N),C(5N)		arc-melting 5times - wrapped in Ta foil - sealed in quartz tube - ANN(1100C,14 days)					Superconductivity in non-centrosymmetric ThCoC2			Department of Physics and Astronomy, University of California-Irvine, Irvine, CA 92697, USA	Supercond.Sci.Technol., 27(2014)035004	T Grant,A J S Machado,D J Kim,Z Fisk		
157591	SST030035007	Impurity phase: Ir. SP (beta) = 1.17 mJ/mol.K4, (delta) = 10.7 uJ/mol.K6. (dC<e>/gamma*Tc) = 1.36	BaIr2As2	Ba1Ir2As2	Ba	1	Ir	2	As	2																		1	2017																										AB2C2		ThCr2Si2	I4/mmm	139	A	4.052		12.787												K	2.35		2.45			0.1	2.4										92										T	RES(on), GL fitting	0.2			0.08			1.8																												mJ/mol.K2	14.6	SP	202	SP																																		BaAs,IrAs,Ir		High-T-High-P synthesis.  mixture(BaAs:IrAs:Ir=1:1:1) - ground - pellet - put in BN capsule - SIN(950 C, 2GPa, 2h).					Superconductivity in the ternary iridium-arsenide BaIr2As2			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 30(2017)035007	Xiao-Chuan Wang,Bin-Bin Ruan,Jia Yu,Bo-Jin Pan,Qing-Ge Mu,Tong Liu,Gen-Fu Chen,Zhi-An Ren		
157592	SST027104006	[penet] measured by TDR for Hac //c-axis. [penet] in DB shows the value of d[penet] at 0.3Tc	(Ca1-xLax)10(Pt3As8)(Fe2As2)5	Ca9.6La0.4Pt3Fe10As18	Ca	9.6	La	0.4	Pt	3	Fe	10	As	18														1	2014																																													10-3-8 phase	K		12.7					12.7																																									nm	d[penet](0.3Tc)	133																																																					single crystals grown by CaAs-flux method					Doping-evolution of the superconducting gap in single crystals of (Ca1-xLax)10(Pt3As8) (Fe2As2)5 superconductor from London penetration depth measurements			The Ames Laboratory, Ames, IA 50011, USA	Supercond.Sci.Technol., 27(2014)104006	K Cho,M A Tanatar,N Ni,R Prozorov		
157593	SST027104006	[penet] measured by TDR for Hac //c-axis. [penet] in DB shows the value of d[penet] at 0.3Tc	(Ca1-xLax)10(Pt3As8)(Fe2As2)5	Ca8.9La1.1Pt3Fe10As18	Ca	8.9	La	1.1	Pt	3	Fe	10	As	18														1	2014																																													10-3-8 phase	K		23.3					23.3																																									nm	d[penet](0.3Tc)	51.5																																																					single crystals grown by CaAs-flux method					Doping-evolution of the superconducting gap in single crystals of (Ca1-xLax)10(Pt3As8) (Fe2As2)5 superconductor from London penetration depth measurements			The Ames Laboratory, Ames, IA 50011, USA	Supercond.Sci.Technol., 27(2014)104006	K Cho,M A Tanatar,N Ni,R Prozorov		
157594	SST027104006	[penet] measured by TDR for Hac //c-axis. [penet] in DB shows the value of d[penet] at 0.3Tc	(Ca1-xLax)10(Pt3As8)(Fe2As2)5	Ca8.2La1.8Pt3Fe10As18	Ca	8.2	La	1.8	Pt	3	Fe	10	As	18														1	2014																																													10-3-8 phase	K		21.9					21.9																																									nm	d[penet](0.3Tc)	49																																																					single crystals grown by CaAs-flux method					Doping-evolution of the superconducting gap in single crystals of (Ca1-xLax)10(Pt3As8) (Fe2As2)5 superconductor from London penetration depth measurements			The Ames Laboratory, Ames, IA 50011, USA	Supercond.Sci.Technol., 27(2014)104006	K Cho,M A Tanatar,N Ni,R Prozorov		
157595	SST027104006	[penet] measured by TDR for Hac //c-axis. [penet] in DB shows the value of d[penet] at 0.3Tc	(Ca1-xLax)10(Pt3As8)(Fe2As2)5	Ca9.4La0.6Pt3Fe10As18	Ca	9.4	La	0.6	Pt	3	Fe	10	As	18														1	2014																																													10-3-8 phase	K		18.2					18.2																																									nm	d[penet](0.3Tc)	129																																																					single crystals grown by CaAs-flux method					Doping-evolution of the superconducting gap in single crystals of (Ca1-xLax)10(Pt3As8) (Fe2As2)5 superconductor from London penetration depth measurements			The Ames Laboratory, Ames, IA 50011, USA	Supercond.Sci.Technol., 27(2014)104006	K Cho,M A Tanatar,N Ni,R Prozorov		
157596	SST027104006	[penet] measured by TDR for Hac //c-axis. [penet] in DB shows the value of d[penet] at 0.3Tc	(Ca1-xLax)10(Pt3As8)(Fe2As2)5	Ca9.1La0.9Pt3Fe10As18	Ca	9.1	La	0.9	Pt	3	Fe	10	As	18														1	2014																																													10-3-8 phase	K		22.2					22.2																																									nm	d[penet](0.3Tc)	41																																																					single crystals grown by CaAs-flux method					Doping-evolution of the superconducting gap in single crystals of (Ca1-xLax)10(Pt3As8) (Fe2As2)5 superconductor from London penetration depth measurements			The Ames Laboratory, Ames, IA 50011, USA	Supercond.Sci.Technol., 27(2014)104006	K Cho,M A Tanatar,N Ni,R Prozorov		
157600	JAP117013901	Curie-Weiss for T>2 K. R not to zero at P = 0.  Hc2(T) at P = 2.5 GPa. Ferro-Mag hysteresis loop in M-H at 2K.	Sr0.5Ce0.5FBiS2	Sr0.5Ce0.5F1Bi1S2	Sr	0.5	Ce	0.5	F	1	Bi	1	S	2														1	2015			emu/mol.Oe	1.19	My-B/f.u	2.97	-216.31																			ABCD2			P4/nmm		A	4.065		13.35											BiS2 layer SC	K			2.7				2.7	MTC157600																			T	RES(0.9Rn), WHH, P=2.5 GPa	13.8												MHC157600																																					mOhm.cm											9.3												R(Ce,Nd,Pr,Sm),F,Bi,S		solid statereaction. stoichiometric powder mixture - in quartz tube(vac) - heat to 650C(2C/min) - SIN(650C,12h) - slow cool to RT					Appearance of bulk superconductivity under hydrostatic pressure in Sr0.5RE0.5FBiS2 (RE = Ce, Nd, Pr, and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Appl.Phys., 117(2015)013901	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157601	JAP117013901	P-induced SC. Curie-Weiss for T>2 K. Hc2(T) at P = 2.5 GPa.	Sr0.5Nd0.5FBiS2	Sr0.5Nd0.5F1Bi1S2	Sr	0.5	Nd	0.5	F	1	Bi	1	S	2														1	2015			emu/mol.Oe	1.429	My-B/f.u	2.87	-72.61																			ABCD2			P4/nmm		A	4.056		13.38											BiS2 layer SC	K					2			MTC157601																			T	RES(0.9Rn), WHH, P=2.5 GPa	11.6												MHC157601																																					mOhm.cm											8.81												R(Ce,Nd,Pr,Sm),F,Bi,S		solid statereaction. stoichiometric powder mixture - in quartz tube(vac) - heat to 650C(2C/min) - SIN(650C,12h) - slow cool to RT					Appearance of bulk superconductivity under hydrostatic pressure in Sr0.5RE0.5FBiS2 (RE = Ce, Nd, Pr, and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Appl.Phys., 117(2015)013901	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157602	JAP117013901	P-induced SC. Curie-Weiss for T>2 K. Hc2(T) at P = 2.5 GPa.	Sr0.5Pr0.5FBiS2	Sr0.5Pr0.5F1Bi1S2	Sr	0.5	Pr	0.5	F	1	Bi	1	S	2														1	2015			emu/mol.Oe	1.24	My-B/f.u	3.14	-59.18																			ABCD2			P4/nmm		A	4.061		13.36											BiS2 layer SC	K					2			MTC157602																			T	RES(0.9Rn), WHH, P=2.5 GPa	13.5												MHC157602																																					mOhm.cm											6.43												R(Ce,Nd,Pr,Sm),F,Bi,S		solid statereaction. stoichiometric powder mixture - in quartz tube(vac) - heat to 650C(2C/min) - SIN(650C,12h) - slow cool to RT					Appearance of bulk superconductivity under hydrostatic pressure in Sr0.5RE0.5FBiS2 (RE = Ce, Nd, Pr, and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Appl.Phys., 117(2015)013901	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157603	JAP117013901	P-induced SC. Curie-Weiss for T>2 K. Hc2(T) at  P= 2.5 GPa. Ferro-Mag hysteresis loop in M-H at 2K.	Sr0.5Sm0.5FBiS2	Sr0.5Sm0.5F1Bi1S2	Sr	0.5	Sm	0.5	F	1	Bi	1	S	2														1	2015			emu/mol.Oe	1.31	My-B/f.u	3.24	-160.9																			ABCD2			P4/nmm		A	4.053		13.4											BiS2 layer SC	K					2			MTC157603																			T	RES(0.9Rn), WHH, P=2.5 GPa	14.5												MHC157603																																					mOhm.cm											10.8												R(Ce,Nd,Pr,Sm),F,Bi,S		solid statereaction. stoichiometric powder mixture - in quartz tube(vac) - heat to 650C(2C/min) - SIN(650C,12h) - slow cool to RT					Appearance of bulk superconductivity under hydrostatic pressure in Sr0.5RE0.5FBiS2 (RE = Ce, Nd, Pr, and Sm) compounds			CSIR-National Physical Laboratory, Dr. K.S. Krishnan Marg, New Delhi 110012, India	J.Appl.Phys., 117(2015)013901	Rajveer Jha,Brajesh Tiwari,V. P. S. Awana		
157604	JPCM0165095	not SC. Curie-Weiss Law for T > 200 K. Einstein T = 82 K by SUS.	EuFe4Sb12	Eu1Fe4Sb12	Eu	1	Fe	4	Sb	12																		3	2004					My-B/Eu	7.7	89		7.903																	AB4C12		skutterudite	Im3[-]		A	9.1725													LaFe4Sb12-type	K					1.8																																																										mJ/mol.K2	85	SP	348	SP																																		Eu(4N),T(3N),Sb(6N)		Sb-flux method. (Eu:T:Sb=1:4:20) - in carbon coated quartz tube - heat to 950 C for 24h - cool to 650 C (3 C/h) - Q to RT					Investigation of ferromagnetic filled skutterudite compounds EuT4Sb12 (T = Fe, Ru, Os)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	J.Phys.:Condens.Matter, 16(2004)5095	E D Bauer,A  Slebarski,N A Frederick,W M Yuhasz,M B Maple,D Cao,F Bridges,G Giester,P Rogl		
157605	JPCM0165095	not SC. Curie-Weiss Law for T > 20 K. Einstein T = 78 K by SUS.	EuRu4Sb12	Eu1Ru4Sb12	Eu	1	Ru	4	Sb	12																		3	2004					My-B/Eu	8	3		8.362																	AB4C12		skutterudite	Im3[-]		A	9.2877													LaFe4Sb12-type	K					1.8																																																										mJ/mol.K2	73	SP	262	SP																																		Eu(4N),T(3N),Sb(6N)		Sb-flux method. (Eu:T:Sb=1:4:20) - in carbon coated quartz tube - heat to 950 C for 24h - cool to 650 C (3 C/h) - Q to RT					Investigation of ferromagnetic filled skutterudite compounds EuT4Sb12 (T = Fe, Ru, Os)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	J.Phys.:Condens.Matter, 16(2004)5095	E D Bauer,A  Slebarski,N A Frederick,W M Yuhasz,M B Maple,D Cao,F Bridges,G Giester,P Rogl		
157606	JPCM0165095	not SC. Curie-Weiss Law for T > 20 K. Einstein T = 74 K by SUS.	EuOs4Sb12	Eu1Os4Sb12	Eu	1	Os	4	Sb	12																		3	2004					My-B/Eu	7.3	8		9.721																	AB4C12		skutterudite	Im3[-]		A	9.3255													LaFe4Sb12-type	K					1.8																																																										mJ/mol.K2	135	SP	304	SP																																		Eu(4N),T(3N),Sb(6N)		Sb-flux method. (Eu:T:Sb=1:4:20) - in carbon coated quartz tube - heat to 950 C for 24h - cool to 650 C (3 C/h) - Q to RT					Investigation of ferromagnetic filled skutterudite compounds EuT4Sb12 (T = Fe, Ru, Os)			Department of Physics and Institute for Pure and Applied Physical Sciences, University of California, San Diego, La Jolla, CA 92093, USA	J.Phys.:Condens.Matter, 16(2004)5095	E D Bauer,A  Slebarski,N A Frederick,W M Yuhasz,M B Maple,D Cao,F Bridges,G Giester,P Rogl		
157607	PHB2810308	not SC. RRR = 30.  FM ordering at 18 K. Effective moment(my-B) and Curie-T(K)  are (7.75, 20), (7.81, 21), (7.69, 21) for H//[100], [110], [111], respectively.	EuRu4P12	Eu1Ru4P12	Eu	1	Ru	4	P	12																		3	2000					My-B/Eu	7.75	20																			AB4C12		skutterudite			A	8.0516														K					1.7																																																																																																		Sn-flux method. mixture(Eu:Ru:P:Sn = 1:4:20:50) - in quartz tube(150mHg-Ar) - heat to 1000 C -hold(1w) - cool to 600C(2 C/h) - Q to water					Magnetic and electrical properties of the filled skutterudite-type compound EuRu4P12			Department of Electrical and Electronic Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050-8585, Japan	Physica B, 281&282(2000)308	C. Sekine,M. Inoue,T. Inaba,I. Shirotani		
157608	PRB096060509	P-induced SC. Tc shows Tc(max) at 23 GPa. (dTc/dP) for 7 < P < 13 GPa. R(Tc) = 3.54, 5.66, 6.41, 10.9 uOhm.cm for P = 7.2, 8.4, 21.2, 32.7 GPa,respectively	PdSe2	Pd1Se2	Pd	1	Se	2																				3	2017																										AB2																			PdS2-type at P - 0. pyrite(NiSe2) for 6 < P < 38 GPa, gamma phase for P > 38 GPa	K			13.1		0		13.1	MTC157608		K/GPa	-1.2																																																																																												Chemical vapor transport (CVT) method using poly-PdSe2, Iodine agent. thickness= 5 micron meter					Pressure-induced superconductivity up to 13.1 K in the pyrite phase of palladium diselenide PdSe2			Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany	Phys.Rev.B, 96(2017)060509	Moaz A. ElGhazali,Pavel G. Naumov,Hossein Mirhosseini,Vicky Suss,Lukas Muchler,Walter Schnelle,Claudia Felser,Sergey A. Medvedev		
157609	PRB096064512	M=NH3. LiM intercalated SC. RRR=( = 12. R300/R50). Anisotropy(R300) = 900. Anisotropy(Hc2(0.5Rn)) = 12.	Li0.36(NH3)yFe2Se2	Li0.36M1Fe2Se2	Li	0.36	M	1	Fe	2	Se	2																3	2017																													I4/mmm		A	3.7704		16.973												K			44.56			1.1	44.56										100										T	RES(0.5Rn), WHH		208.7	29.5					T/K	RES(0.5Rn)		6.83	0.97	MHC157609																																																			cm3/C	-0.000264				14	MRH157609	n/cm3	23740000000000000000000			FeSe grown by CVT					Extreme anisotropy and anomalous transport properties of heavily electron doped Lix(NH3)yFe2Se2 single crystals			Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China, Beijing 100872, China	Phys.Rev.B, 96(2017)064512	Shanshan Sun,Shaohua Wang,Rong Yu,Hechang Lei		
157610	JPS086124802	Impurity phase: La2O2S, AgBiS2. The sample is not SC, will be non-SC upon carrier doping. Seebeck effect measured for 300 < T <800 K.	La2O2Bi3AgS6	La2Bi3Ag1S6O2	La	2	Bi	3	Ag	1	S	6													O	2		1	2017																										AB2C2D3E6			P4/nmm	129	A	4.0644		19.412												K					2																																																																				uV/K	-23			MTP157610																								Bi2O3(3N),La2S3(3N),Ag(3N),Bi(5N),S(4N)		Solid state reaction. mixture - pelletize - sealed in quartz tube - heat(700C,15h) - reground - in quartz tube - heat(720C,15h)					Synthesis, Crystal Structure, and Physical Properties of New Layered Oxychalcogenide La2O2Bi3AgS6			Graduate School of Science and Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)124802	Yudai Hijikata,Tomohiro Abe,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yosuke Goto,Akira Miura,Kiyoharu Tadanaga,Yongming Wang,Osuke Miura,Yoshikazu Mizuguchi		
157611	PRB096064528	1 st order phase transition at Ts (=425 K at P=0 GPa). For  P > 0.25 GPa, no phase transition.	PbTaSe2	Pb1Ta1Se2	Pb	1	Ta	1	Se	2																		3	2017																										ABC2			P6[-]m2																For T>Ts, P6[-]m2, For T<Ts, SG = P6[-]m2	K			4.02				4.02	MPH157611																																																																						uOhm.cm							0.733																		CVT method.  See J.Phys.: Condens.Matter 29(2017)095601  for detail					Topological phase transition under pressure in the topological nodal-line superconductor PbTaSe2			Advanced Functional Materials Lab and Department of Physics, Changshu Institute of Technology, Changshu 215500, China	Phys.Rev.B, 96(2017)064528	C. Q. Xu,R. Sankar,W. Zhou,Bin Li,Z. D. Han,B. Qian,J. H. Dai,Hengbo Cui,A. F. Bangura,F. C. Chou,Xiaofeng Xu		
157612	APL101042603	Electric-field induced SC. SC appears for V(G), gate voltage, >= 3V. Tc(onset) = 9.4 K for V(G) = 4V.  Hc2(onset) = 3 T for (V(G) = 3 V,  H//(001).	MoS2	Mo1S2	Mo	1	S	2																				3	2012																										AB2			P6<3>/mmc																2H-type	K			9.4		0		9.4																																																																																																MoS2 crystal. 6-electrodes on (001) surface. Final treatment: channel area & Pt-electrode immersed  in ionic liquid (DEME-TFSI)					Electric-field-induced superconductivity at 9.4K in a layered transition metal disulphide MoS2			Department of Physics, The University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Appl.Phys.Lett., 101(2012)042603	Kouji Taniguchi,Akiyo Matsumoto,Hidekazu Shimotani,Hidenori Takagi		
157613	CEM1420057	not SC. seminon-like R(T). DOS = 0.99 states/eV.  from susceptibility. samples BaNbS3+z for  2.93 <(3+z) < 3.06	BaNbS2.93	Ba1Nb1S2.93	Ba	1	Nb	1	S	2.93																		1	1999					My-B/Nb	0.04																				ABC3			P6<3>mmc		A	6.862		5.742											Fe-22241	K					4.2																																																																																																BaCO3(4N),Nb2O5(3N)		mixture - in alumina boat - in quartz tube - heat to 700 C(30C/min) - sulfurization using CS2 by flowing Ar gas					Resistance Anomaly in Quasi-One-Dimensional Sulfide BaNbS3+z			Department of Materials Science and Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050-8585, Japan	J.Solid State Chem., 142(1999)57	Norihito Kijima,Kenichi Morie,Susumu Chikazawa,Hironori Nishihara,Shoichi Nagata		
157614	JAC7310064	RRR = 7. energy gap from SP-alpha-model. Hc(0) = 167 Oe. kappa(GL) = 6.2. e-ph = 0.44. SP also measured for 0.3 < T < 300K	ThNiSi	Th1Ni1Si1	Th	1	Ni	1	Si	1																		1	2018																										ABC	2	LaPtSi	I4<1>md		A	4.0697		14.0891											Fe-22241	K	0.85		0.9				0.875											Oe	M-H curve, (1-t^2)	30			20			0.48	T	RES(zero), GL	0.126			0.09			0.37						MHC157614		nm	from Hc2	53.6			nm	from Hc1	316.2					3.528	14				MSP157614			mJ/mol.K2	8.54	SP	285	SP											uOhm.cm							63				458												Th(98 wt%),Ni(4N wt%),Si(5N wt%)		arc-melting - wrapped in Mo foil - sealed in quartz ampoule - ANN(1173K,14 days)					Superconductivity in non-centrosymmetric ThNiSi			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O.Box 1410, 50-950 Wroc?aw, Poland	J.Alloys Compd., 731(2018)64	Krzysztof Domieracki,Dariusz Kaczorowski		
157615	JAC7450460	Tc by M(T) at H=10 Oe.	Ba2Ti2Fe2As4O	Ba2Ti2Fe2As4O1	Ba	2	Ti	2	Fe	2	As	4													O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0296		27.345											Fe-22241	K				21.1			21.1																																																																							mOhm.cm							0.558																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157616	JAC7450460	Tc by M(T) at H=10 Oe. Tc(x) obeys A-G theory.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.98Cr0.02As4O1	Ba	2	Ti	2	Fe	1.98	Cr	0.02	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0297		27.3484											Fe-22241	K				19.1			19.1	MTC157616																																																																						mOhm.cm							0.747																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157617	JAC7450460	Tc by M(T) at H=10 Oe.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.96Cr0.04As4O1	Ba	2	Ti	2	Fe	1.96	Cr	0.04	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0296		27.3585											Fe-22241	K				15.7			15.7																																																																							mOhm.cm							0.893																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157618	JAC7450460	Tc by M(T) at H=10 Oe.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.94Cr0.06As4O1	Ba	2	Ti	2	Fe	1.94	Cr	0.06	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0299		27.359											Fe-22241	K				11.8			11.8																																																																							mOhm.cm							1.02																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157619	JAC7450460	Tc by M(T) at H=10 Oe.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.92Cr0.08As4O1	Ba	2	Ti	2	Fe	1.92	Cr	0.08	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0301		27.3617											Fe-22241	K				8.21			8.21																																																																							mOhm.cm							1.11																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157620	JAC7450460	Tc by M(T) at H=10 Oe.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.9Cr0.1As4O1	Ba	2	Ti	2	Fe	1.9	Cr	0.1	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0302		27.365											Fe-22241	K				5.29			5.29	MTC157616																																																																						mOhm.cm							1.24																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157621	JAC7450460	Tc by M(T) at H=10 Oe. Tc(x) obeys A-G theory.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.88Cr0.12As4O1	Ba	2	Ti	2	Fe	1.88	Cr	0.12	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0305		27.3819											Fe-22241	K				2.89			2.89																																																																							mOhm.cm							1.32																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157622	JAC7450460	not SC. Tc by M(T) at H=10 Oe. R(T) not to zero down to 1.8 K.	Ba2Ti2(Fe1-xCrx)2As4O	Ba2Ti2Fe1.84Cr0.16As4O1	Ba	2	Ti	2	Fe	1.84	Cr	0.16	As	4											O	1		1	2018																										AB2C2D2E4			I4/mmm		A	4.0306		27.3841											Fe-22241	K					1.8																																																																									mOhm.cm							1.46																Ba,Ti,Fe,Cr,TiO2,CeO3(>=3N)		solid state reaction. mixture - sealed in quartz ampule - heat to 900 C - hold(1day) - reground - SIN(1050C,3days) - ANN(500C,2days, in vac)					Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157623	JPS086084710	not SC down to 0.14 K. RRR = 22. AFM order (Tn=1.9K) decreases with H, desappear at H=3T.	CePt(In,Zn)4	Ce1Pt1In3.6Zn0.4	Ce	1	Pt	1	In	3.6	Zn	0.4																3	2017					My-B/Ce	2.49		1.9																		ABC4		YNiAl4	Cmcm	63	A	4.5175	16.757	7.3668												K					0.14																																																																									uOhm.cm	2.6										58												Ce(3N),Pt(3N),In(3N),Zn(3N)		Flux method. mixture(Ce:Pt:Zn:In = 2:2:2:94) - C-coated quartz tube - heat to 1000C(60C/h) - hold(0.3h) - cool to 750C(over 4h) -cool to 450C(over150h) - hold(48h)					Growth, Crystal Structure and Magnetic Characterization of Zn-Stabilized CePtIn4			Department of Chemistry, Princeton University, Princeton, NJ 08544, U.S.A.	J.Phys.Soc.Jpn, 86(2017)084710	Elizabeth M. Carnicom,Tomasz Klimczuk,Fabian von Rohr,Michal J. Winiarski,Tai Kong,Karoline Stolze,Weiwei Xie,Satya K. Kushwaha,Robert J. Cava		
157624	JPS086104701	M-content y not given.	MyTiSe2	M1Ti1Se2	M	1	Ti	1	Se	2																		1	2017																													P3[-]m1		A			10.107											phase-II	K			2.15	2.8			2.8																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157625	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given.	LixMyTiSe2	Li0.02M1Ti1Se2	Li	0.02	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			11.44											phase-III	K			2.73	4			4																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157626	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.57, Tc(SUS) = 4.0 K.	LixMyTiSe2	Li0.04M1Ti1Se2	Li	0.04	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			10.117											phase-II, phase-III (c=11.57 A)	K			2.42	2.8			2.8																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157627	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.62, Tc(SUS) = ?? K.	LixMyTiSe2	Li0.06M1Ti1Se2	Li	0.06	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			10.12											phase-II, phase-III (c=11.62 A)	K			1.51	2.7			2.7																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157628	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.58, Tc(SUS) = 4.2 K.	LixMyTiSe2	Li0.08M1Ti1Se2	Li	0.08	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			10.1											phase-II, phase-III (c=11.58 A)	K			1.38	2.7			2.7																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157629	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.53, Tc(SUS) = 4.2 K.	LixMyTiSe2	Li0.1M1Ti1Se2	Li	0.1	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			9.97											phase-II, phase-III (c=11.53 A)	K			0.97	2.7			2.7																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157630	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.59, Tc(SUS) = 4.2 K.	LixMyTiSe2	Li0.15M1Ti1Se2	Li	0.15	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			9.94											phase-II, phase-III(c=11.59A)	K			0.78	2.7			2.7																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157631	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.55, Tc(SUS) = 4.2 K.	LixMyTiSe2	Li0.2M1Ti1Se2	Li	0.2	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			6.11											phase-I,  phase-III(c=11.55A)	K				2.4			2.4																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157632	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.52, Tc(SUS) = ?? K.	LixMyTiSe2	Li0.3M1Ti1Se2	Li	0.3	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			9.96											phase-II, phase-III (c=11.52A)	K			0.7	2.8			2.8																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157633	JPS086104701	M=EDA(ethylenediamine, C2H8N2), M-content y not given. For phase-III, c = 11.43, Tc(SUS) = ?? K.	LixMyTiSe2	Li1M1Ti1Se2	Li	1	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			10.12											phase-II, phase-III (c=11.43 A)	K				2.8			2.8																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157634	JPS086104701	M=HMDA(hexamethylenediamine, C6H16N2), M-content y not given.	LixMyTiSe2	Li0.1M1Ti1Se2	Li	0.1	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			14.07												K			2.57	4.2			4.2																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157635	JPS086104701	M=HMDA(hexamethylenediamine, C6H16N2), M-content y not given.	LixMyTiSe2	Li0.2M1Ti1Se2	Li	0.2	M	1	Ti	1	Se	2																1	2017																													P3[-]m1		A			14.08												K			2.66	4.2			4.2																																																																																																1T-TiSe2 by solid state reaction. co-intercalation Li & EDA or HEDA prepared by reaction (50C 2 weeks) in 0.01M solution of Li desolved in  EDA or HMDA					New Lithium- and Diamines-Intercalated Superconductors Lix(C2H8N2)yTiSe2 and Lix(C6H16N2)yTiSe2			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 86(2017)104701	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157636	JPS086113705	Tc(max) = 36.2 K at P=1.3 GPa.  Tn defined as a peak of (dR/dT).	(Ca,La)FeAs2	Ca0.82La0.18Fe1As2	Ca	0.82	La	0.18	Fe	1	As	2																3	2017								47																		ABC2			P2<1>	4															Fe-112	K	20.5		41.4				30.95	MPH157636																																																																																													Ca,La,FeAs,As		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Pressure-Induced Superconductivity from Doping-Induced Antiferromagnetic Phase of 112-type Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)113705	Shunsaku Kitagawa,Taishi Sekiya,Yo Fujiyoshi,Shingo Araki,Tatsuo C. Kobayashi,Naoki Nishimoto,Tasuku Mizukami,Satoshi Ioka,Kazunori Fujimura,Kazutaka Kudo,Minoru Nohara		
157637	JPS086113705	P-induced SC. P<cr> = 1.48 GPa. Tc shows Tc(max)  at P = 3.82 GPa. Tn defined as a peak of (dR/dT).	(Ca,La)FeAs2	Ca0.79La0.21Fe1As2	Ca	0.79	La	0.21	Fe	1	As	2																3	2017								63																		ABC2			P2<1>	4															Fe-112	K	31.8		40.9		0		36.35	MPH157637																																																																																													Ca,La,FeAs,As		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Pressure-Induced Superconductivity from Doping-Induced Antiferromagnetic Phase of 112-type Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)113705	Shunsaku Kitagawa,Taishi Sekiya,Yo Fujiyoshi,Shingo Araki,Tatsuo C. Kobayashi,Naoki Nishimoto,Tasuku Mizukami,Satoshi Ioka,Kazunori Fujimura,Kazutaka Kudo,Minoru Nohara		
157638	JPS086113705	P-induced SC. P<cr> = 3.4 GPa. Tc shows Tc(max)  at P = 3.4 GPa. Tn defined as a peak of (dR/dT).	(Ca,La)FeAs2	Ca0.74La0.26Fe1As2	Ca	0.74	La	0.26	Fe	1	As	2																3	2017								63																		ABC2			P2<1>	4															Fe-112	K	14		38.2		0		26.1	MPH157638																																																																																													Ca,La,FeAs,As		mixture(x=0.1, 0=<y=<0.1 in Ca1-xRxFe(As1-ySny)2) - alumina crucible - sealed in quartz tube) - heat(700C,3h) - heat to 1100C(46C/h) - cool to 1050C(1.25C/h) - FC					Pressure-Induced Superconductivity from Doping-Induced Antiferromagnetic Phase of 112-type Ca1-xLaxFeAs2			Department of Physics, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 86(2017)113705	Shunsaku Kitagawa,Taishi Sekiya,Yo Fujiyoshi,Shingo Araki,Tatsuo C. Kobayashi,Naoki Nishimoto,Tasuku Mizukami,Satoshi Ioka,Kazunori Fujimura,Kazutaka Kudo,Minoru Nohara		
157639	JPS086123701	compositions(Na:Sn:As = 1:1.89:2.12). sample size = 0.06*0.1*0.07 mm^3. SP (beta) = 1.120 mJ/mol.K4. (dC/gamma*Tc) = 1.52	NaSn2As2	Na1Sn2As2	Na	1	Sn	2	As	2																		3	2017																										AB2C2			R3[-]m	166	A	4.01		27.56											gamma =120 degree	K	1.1		1.3				1.2																				T	RES(0.9Rn), WHH	0.2												MHC157639		A	from Hc2	410															MSP157639	mJ/mol.K	7.82	mJ/mol.K2	3.97	SP	205	SP																																		Na(3N),Sn(4N),As(6N)		mixture - in evacuated quartz tube - heat(750C,20h) - cool to 350C in 10h.					SnAs-Based Layered Superconductor NaSn2As2			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 86(2017)123701	Yosuke Goto,Akira Yamada,Tatsuma D. Matsuda,Yuji Aoki,Yoshikazu Mizuguchi		
157640	MRB0390561	not SC for 0.8 < x < 1.0, in BaNbxS3. Semicon-to-metal transition at 170 K.	BaNb0.95S3	Ba1Nb0.95S3	Ba	1	Nb	0.95	S	3																		1	2004																										ABC3			P6<3>mmc		A														BaVS3-type	K					2			MLAT157640																																																																	uV/K				MTP157640	Ohm.cm	1.29										2.05														mixture - in C-coated silica tube(vac) - heat to 1073 K(100K/h) - ANN(1073K, 7days) - reground - pelletize - in sealed silica tube - SIN(1073 K, 7days) - slow cool to RT					Phase transitions in quasi-one-dimensional chalcogenides of BaNbxS3 and BaTaxSe3			Laboratory for Solid State Chemistry, Okayama University of Science, Ridai-cho 1-1, Okayama 700-0005, Japan	Mater.Res.Bull., 39(2004)561	T. Ohtani,H. Sawada,M. Chikamori		
157641	MRB0390561	not SC for 0.8 < x < 1.0, in BaNbxS3. Semicon-to-semicon(2)  at 140 K.	BaTa0.95Se3	Ba1Ta0.95Se3	Ba	1	Ta	0.95	Se	3																		1	2004																										ABC3			P6<3>mmc		A	7.118		6.009											BaVS3-type	K					2																																																																				uV/K				MTP157641																										mixture - in C-coated silica tube(vac) - heat to 1073 K(100K/h) - ANN(1073K, 7days) - reground - pelletize - in sealed silica tube - SIN(1073 K, 7days) - slow cool to RT					Phase transitions in quasi-one-dimensional chalcogenides of BaNbxS3 and BaTaxSe3			Laboratory for Solid State Chemistry, Okayama University of Science, Ridai-cho 1-1, Okayama 700-0005, Japan	Mater.Res.Bull., 39(2004)561	T. Ohtani,H. Sawada,M. Chikamori		
157642	PHB2810308	not SC. RRR = 30. Curie-Weiss law for T > 50 K. (Curie-T, moment) = (20,7.75), (21,7.81), (21,7.69) for H//[100], [110], [111] direction, respectively. magnetic order = FM.	EuRu4P12	Eu1Ru2P12	Eu	1	Ru	2	P	12																		3	2000					My-B/Eu	7.75	20																			AB4C12		skutterudite			A	8.0516														K					1.7																																																																																																		Flux method. mixture(Eu:Ru:P:Sn = 1:4:20:50) - in quartz tube(Ar) - heat to 1000 C - keep (1 week) - cool to 600 C (2C/h) - Q to water - remove Sn-flux					Magnetic and electrical properties of the filled skutterudite-type compound EuRu4P12			Department of Electrical and Electronic Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido 050-8585, Japan	Physica B, 281&282(2000)308	C. Sekine,M. Inoue,T. Inaba,I. Shirotani		
157643	PHC3880445	not SC	LixCsSr2Nb3O10	Cs1Sr2Nb3O10	Cs	1	Sr	2	Nb	3															O	10		1	2003																										AB2C3D10																			Layered perovskite	K					2																																																																																																		host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157644	PHC3880445	Li-intercalated sample. SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.05Cs1Sr2Nb3O10	Li	0.05	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5.43					5.43										0.06																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157645	PHC3880445	Li-intercalated sample.. SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.1Cs1Sr2Nb3O10	Li	0.1	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5.43					5.43										3.11																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157646	PHC3880445	Li-intercalated sample.  SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.2Cs1Sr2Nb3O10	Li	0.2	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5.21					5.21										0.33																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157647	PHC3880445	Li-intercalated sample.  SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.3Cs1Sr2Nb3O10	Li	0.3	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5.22					5.22										0.1																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157648	PHC3880445	Li-intercalated sample.  SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.5Cs1Sr2Nb3O10	Li	0.5	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5					5										0.03																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157649	PHC3880445	Li-intercalated sample.  SC volume by measuring M. Tc does not depend on Li-content (x>0.05)	LixCsSr2Nb3O10	Li0.6Cs1Sr2Nb3O10	Li	0.6	Cs	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10																			Layered perovskite	K		5.01					5.01										0.02																																																																																						host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157650	PHC3880445	Li-intercalated sample. Li-content not given	LixRbCa2Nb3O10	Li0.1Rb1Ca2Nb3O10	Li	0.1	Rb	1	Ca	2	Nb	3													O	10		1	2003																										AB2C3D10					A	7.721													Layered perovskite	K		3.51					3.51																																																																																																host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157651	PHC3880445	Li-intercalated sample. Li-content not given	LixKCa2Nb3O10	Li0.1K1Ca2Nb3O10	Li	0.1	K	1	Ca	2	Nb	3													O	10		1	2003																										AB2C3D10					A	7.7326													Layered perovskite	K		5.51					5.51	MTC157651																																																																																															host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157652	PHC3880445	Li-intercalated sample. Li-content not given	LixCsCa2Nb3O10	Li0.1Cs1Ca2Nb3O10	Li	0.1	Cs	1	Ca	2	Nb	3													O	10		1	2003																										AB2C3D10					A	7.7404													Layered perovskite	K		5.62					5.62																																																																																																host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157653	PHC3880445	Li-intercalated sample. Li-content not given	LixRbSr2Nb3O10	Li0.1Rb1Sr2Nb3O10	Li	0.1	Rb	1	Sr	2	Nb	3													O	10		1	2003																										AB2C3D10					A	7.7891													Layered perovskite	K		6.02					6.02																																																																																																host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157654	PHC3880445	Li-intercalated sample. Li-content not given	LixCsBa2Nb3O10	Li0.1Cs1Ba2Nb3O10	Li	0.1	Cs	1	Ba	2	Nb	3													O	10		1	2003																										AB2C3D10					A	7.9743													Layered perovskite	K					2																																																																																																		host sample by solid state reaction. (sample + 25% napfthalene) - pelletize - SIN - Li-intercalation(1.0M LiClO4/PC/Pt, three electrode cell)					Superconductivity in the electrochemically Li-intercalated niobates with the layered perovskite structure			Department of Applied Physics, Tohoku University, Aoba-yama 08, Aoba-ku, Sendai 980-8579, Japan	Physica C, 388-389(2003)445	Masatsune Kato,Akira Inoue,Ichiro Nagai,Masato Kakihana,Arthur W. Sleight,Yoji Koike		
157655	PRB065064504	P-induced SC. P<cr> = 93 GPa. Tc(max) = 17.4 K at P = 185 GPa ( beta-Po structure	S	S1	S	1																							2002																										A																				K		17.4			0		17.4	MTC157655																																																																																															S(5N5) were loaded in Mao-Bell cell.  Tc measured by ac-SUS.					Superconductivity in the chalcogens up to multimegabar pressures			Geophysical Laboratory and Center for High Pressure Research, Carnegie Institution of Washington, 5251 Broad Branch Road NW, Washington, D.C. 20015	Phys.Rev.B,  65(2002)064504	Eugene Gregoryanz,Viktor V. Struzhkin,Russell J. Hemley,Mikhail I. Eremets,Ho-kwang Mao,Yuri A. Timofeev		
157656	PRB093224512	Energy gap = 10.5 meV for [penet]ab analysis  using s-wave model. Anisotropy(T=0) = [penet]c/[penet]ab = 5.6.	(Li1.84Fe0.16)OHFe0.98Se	Li1.84H1Fe1.14Se1O1	Li	1.84	H	1	Fe	1.14	Se	1													O	1			2016																										ABCDE			P4/nmm																	K			40.5				40.5																																									nm	muon-SR		286	1830	meV	10.5																																																	(0.012 mol selenourea, 0.00375 mol Fe, 4g LiOH H2O, K0.8Fe1.6Se2) - mixed with 5 ml deionized water - stainles autoclave - heat(1100 C, 3days)					Proximity-induced superconductivity within the insulating (Li0.84Fe0.16)OH layers in (Li0.84Fe0.16)OHFe0.98Se			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B,  93(2016)224512	Rustem Khasanov,Huaxue Zhou,Alex Amato,Zurab Guguchia,Elvezio Morenzoni,Xiaoli Dong,Guangming Zhang,Zhongxian Zhao		
157657	PRB094180510	SC properties measured by TDO method. d[penet](T) = A*T^2, indicate the presence of point node in SC order parameter.	Nb0.25Bi2Se3	Nb0.25Bi2Se3	Nb	0.25	Bi	2	Se	3																		3	2016																																														K				3.5			3.5										100	Oe	TDO, GL		75						T	TDO, Extrapolation		1.8	0.9										MHC157657		nm	from Hc2		19	9.5	nm	Hc1, GL		237																																																				Details,  See arXiv:1512.04554v2					Evidence of nodes in the order parameter of the superconducting doped topological insulator NbxBi2Se3 via penetration depth measurements			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.B,  94(2016)180510	M. P. Smylie,H. Claus,U. Welp,W.-K. Kwok,Y. Qiu,Y. S. Hor,A. Snezhko		
157658	PRB096094523	optimal doping. Irradiation(5.5 MeV proton. fluence = 4E+16 /cm2) effect. point defect, interdefect distance = 2.8 nm. dTc/d(phi) = 0.3E+16 K/cm2.	Ba(Fe,Rh)2As2	Ba1Fe1.864Rh0.136As2	Ba	1	Fe	1.864	Rh	0.136	As	2																3	2017																										AB2C2		ThCr2Si2																		K	23.3			23.3			23.3	MTC157658																																																																						uOhm.cm							106				230																			Effect of proton irradiation on the normal-state low-energy excitations of Ba(Fe1-xRhx)2As2 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B,  96(2017)094523	M. Moroni,L. Gozzelino,G. Ghigo,M. A. Tanatar,R. Prozorov,P. C. Canfield,P. Carretta		
157659	PRB096094523	over doped. Irradiation(5.5 MeV proton. fluence = 4E+16 /cm2) effect. point defect, interdefect distance = 2.8 nm. dTc/d(phi) = 0.2E+16 K/cm2.	Ba(Fe,Rh)2As2	Ba1Fe1.786Rh0.214As2	Ba	1	Fe	1.786	Rh	0.214	As	2																3	2017																										AB2C2		ThCr2Si2																		K				13.3			13.3	MTC157658																																																																						uOhm.cm							100				230																			Effect of proton irradiation on the normal-state low-energy excitations of Ba(Fe1-xRhx)2As2 superconductors			Department of Physics, University of Pavia-CNISM, I-27100 Pavia, Italy	Phys.Rev.B,  96(2017)094523	M. Moroni,L. Gozzelino,G. Ghigo,M. A. Tanatar,R. Prozorov,P. C. Canfield,P. Carretta		
157660	PRB096134503	M=NH3. LiM-intercalate to FeTe0.6Se0.4. (-dHc2/dT) is 11.5(onset) and 5.9(zero) for H//ab, 5.1(on) and 2.1(zero) for H//c. Anisotropy(RES) = 92 at 50K, (Hc2) = 6.5 at 19K.	Lix(NH3)yFe2Te1.2Se0.8	Li0.32M1Fe2Se0.8Te1.2	Li	0.32	M	1	Fe	2	Se	0.8	Te	1.2														3	2017																										AB2C2	2		I4/mmm	139															LiM-intercalated Fe(Te,Se)	K			20.84	21		2.97	21																				T	RES(0.5Rn), WHH		119.8	42.8					T/K	RES(0.5Rn)		9	3.2	MHC157660																																					mOhm.cm								1.77	169			4.36	294	cm3/C	0.00926				9	MRH157660					Low temperature ammonothermal technique					Enhanced superconductivity and anisotropy of FeTe0.6Se0.4 single crystals with Li-NH3 intercalation			Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials & Micro-nano Devices, Renmin University of China, Beijing 100872, China	Phys.Rev.B,  96(2017)134503	Chenghe Li,Shanshan Sun,Shaohua Wang,Hechang Lei		
157661	PRB096134503		FeTe0.6Se0.4	Fe1Se0.4Te0.6	Fe	1	Se	0.4	Te	0.6																			2017																										AB	2		P4/nmm	129																K			8				8																																																																																					cm3/C	0.00068				9	MRH157661										Enhanced superconductivity and anisotropy of FeTe0.6Se0.4 single crystals with Li-NH3 intercalation			Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials & Micro-nano Devices, Renmin University of China, Beijing 100872, China	Phys.Rev.B,  96(2017)134503	Chenghe Li,Shanshan Sun,Shaohua Wang,Hechang Lei		
157662	PRB096134504	Energy gap and [penet] obtained by TF-muon-SR analysis. Two-band gaps , d1 = 4.3 (in DB) and d2=1.76 meV.	Ga41Mo8	Ga41Mo8	Ga	41	Mo	8																				3	2017																										A8B41																				K		9.8					9.8																				T	muon-SR				3.77			3						MHC157662							nm	muon-SR	216.2			meV	4.3		16																																															Crystals grown by Ga flux method					Two-gap superconductivity in Mo8Ga41 and its evolution upon vanadium substitution			Department of Chemistry, Lomonosov Moscow State University, 119991 Moscow, Russia	Phys.Rev.B,  96(2017)134504	V. Yu. Verchenko,R. Khasanov,Z. Guguchia,A. A. Tsirlin,A. V. Shevelkov		
157663	PRB096134504	Energy gap and [penet] obtained by TF-muon-SR analysis.	Ga41Mo7V	Ga41Mo7V1	Ga	41	Mo	7	V	1																		3	2017																										A8B41																				K		9.2					9.2																				T	muon-SR													MHC157663							nm	muon-SR	292			meV	1.87	4.72	16																																															Crystals grown by Ga flux method					Two-gap superconductivity in Mo8Ga41 and its evolution upon vanadium substitution			Department of Chemistry, Lomonosov Moscow State University, 119991 Moscow, Russia	Phys.Rev.B,  96(2017)134504	V. Yu. Verchenko,R. Khasanov,Z. Guguchia,A. A. Tsirlin,A. V. Shevelkov		
157664	PRB096144502	R(T) exponent n=1.3 for T < 150 K. From muon-SR analysis, two-gap model (larger in DB, lower d2=0.3 meV, 2d2/kTc = 0.25). carrier = 4.97E+27  /m^3. SP (dC/Tc) = 25 mJ/mol.K2	ThAsFeN	Th1As1Fe1N1	Th	1	As	1	Fe	1	N	1																1	2017																										ABCD	2	oxypnictide	P4/nmm	129	A	4.0367		8.5262											ZrCuSiAs-type	K			30	30			30											Oe	M-H curve				30			5	T					8			26	T/K		2.4										nm	muon-SR, London	375			meV	5.2	4.29	16				MSP157664																																											solid state reaction method					Multigap superconductivity in ThAsFeN investigated using muon-SR measurements			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom	Phys.Rev.B,  96(2017)144502	Devashibhai Adroja,Amitava Bhattacharyya,Pabitra Kumar Biswas,Michael Smidman,Adrian D. Hillier,Huican Mao,Huiqian Luo,Guang-Han Cao,Zhicheng Wang,Cao Wang		
157665	PRB096184503	P = 0 GPa. Tc(max) at P = 3.9 GPa. Tc goes to zero at P = 17 GPa.	(Ca,La)(Fe,Co)As2	Ca0.8La0.2Fe0.98Co0.02As2	Ca	0.8	La	0.2	Fe	0.98	Co	0.02	As	2														3	2017																										ABC2		Fe-112																		K		37.5					37.5	MTC157665																																																																																				mm3/C	-0.0000000247					MRH157665					self-flux method					Correlation between non-Fermi-liquid behavior and superconductivity in (Ca, La)(Fe,Co)As2 iron arsenides: A high-pressure study			Advanced Functional Materials Laboratory and Department of Physics, Changshu Institute of Technology, Changshu 215500, China	Phys.Rev.B,  96(2017)184503	W. Zhou,F. Ke,Xiaofeng Xu,R. Sankar,X. Xing,C. Q. Xu,X. F. Jiang,B. Qian,N. Zhou,Y. Zhang,M. Xu,B. Li,B. Chen,Z. X. Shi		
157666	PRB096184503	P= 14.1 GPa. Hc2(0) = 5.31 T using two band fitting.	(Ca,La)(Fe,Co)As2	Ca0.8La0.2Fe0.98Co0.02As2	Ca	0.8	La	0.2	Fe	0.98	Co	0.02	As	2														3	2017																										ABC2		Fe-112																		K		8.95					8.95																				T	RES, WHH			5.24					T/K	RES			0.85	MHC157666																																																														self-flux method					Correlation between non-Fermi-liquid behavior and superconductivity in (Ca, La)(Fe,Co)As2 iron arsenides: A high-pressure study			Advanced Functional Materials Laboratory and Department of Physics, Changshu Institute of Technology, Changshu 215500, China	Phys.Rev.B,  96(2017)184503	W. Zhou,F. Ke,Xiaofeng Xu,R. Sankar,X. Xing,C. Q. Xu,X. F. Jiang,B. Qian,N. Zhou,Y. Zhang,M. Xu,B. Li,B. Chen,Z. X. Shi		
157667	PRB096184503	P = 12.1 GPa.   Hc2(0) = 13.92 T using two band fitting.	(Ca,La)(Fe,Co)As2	Ca0.8La0.2Fe0.98Co0.02As2	Ca	0.8	La	0.2	Fe	0.98	Co	0.02	As	2														3	2017																										ABC2		Fe-112																		K		16.08					16.08																				T	RES, WHH			11.81					T/K	RES			1.05	MHC157667																																																														self-flux method					Correlation between non-Fermi-liquid behavior and superconductivity in (Ca, La)(Fe,Co)As2 iron arsenides: A high-pressure study			Advanced Functional Materials Laboratory and Department of Physics, Changshu Institute of Technology, Changshu 215500, China	Phys.Rev.B,  96(2017)184503	W. Zhou,F. Ke,Xiaofeng Xu,R. Sankar,X. Xing,C. Q. Xu,X. F. Jiang,B. Qian,N. Zhou,Y. Zhang,M. Xu,B. Li,B. Chen,Z. X. Shi		
157668	PRB096184503	P = 9.8 GPa.   Hc2(0) = 30.61 T using two band fitting.	(Ca,La)(Fe,Co)As2	Ca0.8La0.2Fe0.98Co0.02As2	Ca	0.8	La	0.2	Fe	0.98	Co	0.02	As	2														3	2017																										ABC2		Fe-112																		K		23.89					23.89																				T	RES, WHH			17.79					T/K	RES			1.08	MHC157668																																																														self-flux method					Correlation between non-Fermi-liquid behavior and superconductivity in (Ca, La)(Fe,Co)As2 iron arsenides: A high-pressure study			Advanced Functional Materials Laboratory and Department of Physics, Changshu Institute of Technology, Changshu 215500, China	Phys.Rev.B,  96(2017)184503	W. Zhou,F. Ke,Xiaofeng Xu,R. Sankar,X. Xing,C. Q. Xu,X. F. Jiang,B. Qian,N. Zhou,Y. Zhang,M. Xu,B. Li,B. Chen,Z. X. Shi		
157669	PRB096214505	Tc(0.99Rn) = 3.5 K. Tc(max) = 3.7 K at P=0.95 GPa.	(La,Ti)OBiS2	La0.8Ti0.2Bi1S2O1	La	0.8	Ti	0.2	Bi	1	S	2													O	1		1	2017																										ABCD2		CeOBiS2																	BiS2-layer SC	K	2.19	2.48	2.76				2.48	MTC157669																																																																						mOhm.cm	12.3																								solid state reaction method					High-pressure effects on nonfluorinated BiS2-based superconductors La1-xMxOBiS2 (M =Ti and Th)			1Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B,  96(2017)214505	Y. Fang,D. Yazici,I. Jeon,M. B. Maple		
157670	PRB096214505	Tc(0.99Rn) = 2.88 K. Tc(max) = 3.14 K at P=0.42 GPa.	(La,Th)OBiS2	La0.85Th0.15Bi1S2O1	La	0.85	Th	0.15	Bi	1	S	2													O	1		1	2017																										ABCD2		CeOBiS2																	BiS2-layer SC	K	2.46	2.64	2.8				2.64	MTC157670																																																																						mOhm.cm	7.32																								solid state reaction method					High-pressure effects on nonfluorinated BiS2-based superconductors La1-xMxOBiS2 (M =Ti and Th)			1Materials Science and Engineering Program, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B,  96(2017)214505	Y. Fang,D. Yazici,I. Jeon,M. B. Maple		
157671	PRB096214506	no SP jump at Tc. maybe not bulk SC. Semicond-like R(T).	La(O,F)BiS2	La1F0.5Bi1S2O0.5	La	1	F	0.5	Bi	1	S	2													O	0.5		3	2017																										ABCD2		CeOBiS2			A	4.0512		13.41											BiS2-layer SC	K		2.2				0.7	2.2																																																																							mOhm.cm							5.8																		CsCl/NaCl-flux method. typical crystal size = 1 x 1 mm2					Superconducting gap symmetry of the BiS2-based superconductor LaO0.5F0.5BiSSe elucidated through specific heat measurements			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	Phys.Rev.B,  96(2017)214506	Naoki Kase,Yusuke Terui,Tomohito Nakano,Naoya Takeda		
157672	PRB096214506	SP (beta)=1.34 mJ/mol.K4, (delta)=0.0198 mJ/mol.K6. gamma(0) = 0.60 mJ/mol.K2. (dC/gamma*Tc) = 2.31	La(O,F)BiSe2	La1F0.5Bi1Se2O0.5	La	1	F	0.5	Bi	1	Se	2													O	0.5		3	2017																										ABCD2		CeOBiS2			A	4.1074		13.486											BiS2-layer SC	K		3.95				0.02	3.95																				T	RES, GL		18.5	0.572										MHC157672		nm	from Hc2		24	0.742								4.5	14							mJ/mol.K2	3.59	SP	194	SP											mOhm.cm							0.47																		CsCl/NaCl-flux method. typical crystal size = 1 x 1 mm2					Superconducting gap symmetry of the BiS2-based superconductor LaO0.5F0.5BiSSe elucidated through specific heat measurements			Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan	Phys.Rev.B,  96(2017)214506	Naoki Kase,Yusuke Terui,Tomohito Nakano,Naoya Takeda		
157673	PRB096220506	Type-I SC. Surface layer SC(Tc=1.33 K <bulk SC Tc = 1.64 K. Hc defined by M(T), ac-SUS(H = 0.0005 mT), R(T). GL = 0.34 (type-I)	PdTe2	Pd1Te2	Pd	1	Te	2																				3	2017																										AB2		CdI2	P3[-]m1																	K				1.64			1.64																				mT	M(T), Type-I SC	13.6												MHC157673		nm	from Hc	114			nm	London	39																																																	n/m^3	5500000000000000000000000000			Modified Bridgman method					Type-I superconductivity in the Dirac semimetal PdTe2			1Van der Waals?Zeeman Institute, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, The Netherlands	Phys.Rev.B,  96(2017)220506	H. Leng,C. Paulsen,Y. K. Huang,A. de Visser		
157674	PRB096220510		CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2017																										ABC4D4		CaRb1144																	CaK-1144	K		35.1					35.1																																																																																																NMR sample grown out of high-temperature solution rich in transition metals and arsenic					NMR study of the new magnetic superconductor CaK(Fe0.951Ni0.049)4As4: Microscopic coexistence of the hedgehog spin-vortex crystal and superconductivity			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B,  96(2017)220510	Q.-P. Ding,W. R. Meier,A. E. Bohmer,S. L. Bud'ko,P. C. Canfield,Y. Furukawa		
157675	PRB096220510		CaK(Fe,Ni)4As4	Ca1K1Fe3.932Ni0.068As4	Ca	1	K	1	Fe	3.932	Ni	0.068	As	4														3	2017								0																		ABC4D4		CaRb1144																	CaK-1144	K		29.3					29.3																																																																																																NMR sample grown out of high-temperature solution rich in transition metals and arsenic					NMR study of the new magnetic superconductor CaK(Fe0.951Ni0.049)4As4: Microscopic coexistence of the hedgehog spin-vortex crystal and superconductivity			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B,  96(2017)220510	Q.-P. Ding,W. R. Meier,A. E. Bohmer,S. L. Bud'ko,P. C. Canfield,Y. Furukawa		
157676	PRB096220510		CaK(Fe,Ni)4As4	Ca1K1Fe3.872Ni0.128As4	Ca	1	K	1	Fe	3.872	Ni	0.128	As	4														3	2017								44																		ABC4D4		CaRb1144																	CaK-1144	K		20.4					20.4																																																																																																NMR sample grown out of high-temperature solution rich in transition metals and arsenic					NMR study of the new magnetic superconductor CaK(Fe0.951Ni0.049)4As4: Microscopic coexistence of the hedgehog spin-vortex crystal and superconductivity			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B,  96(2017)220510	Q.-P. Ding,W. R. Meier,A. E. Bohmer,S. L. Bud'ko,P. C. Canfield,Y. Furukawa		
157677	PRB096220510	hedgehog spin-vortex crystal(SVC) coexist with SC below Tc. Anisotropy(Hc2) = 2 near Tc. Tn by NMR. Hc2(7.4K) = 5.9 T for H//c.	CaK(Fe,Ni)4As4	Ca1K1Fe3.804Ni0.196As4	Ca	1	K	1	Fe	3.804	Ni	0.196	As	4														3	2017								53																		ABC4D4		CaRb1144																	CaK-1144	K		10.5					10.5	MTC157677																			T	NMR					5.9		8.7																																																																				NMR sample grown out of high-temperature solution rich in transition metals and arsenic					NMR study of the new magnetic superconductor CaK(Fe0.951Ni0.049)4As4: Microscopic coexistence of the hedgehog spin-vortex crystal and superconductivity			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B,  96(2017)220510	Q.-P. Ding,W. R. Meier,A. E. Bohmer,S. L. Bud'ko,P. C. Canfield,Y. Furukawa		
157678	PRB096220510		CaK(Fe,Ni)4As4	Ca1K1Fe3.748Ni0.252As4	Ca	1	K	1	Fe	3.748	Ni	0.252	As	4														3	2017								53.7																		ABC4D4		CaRb1144																	CaK-1144	K		0					0																																																																																																NMR sample grown out of high-temperature solution rich in transition metals and arsenic					NMR study of the new magnetic superconductor CaK(Fe0.951Ni0.049)4As4: Microscopic coexistence of the hedgehog spin-vortex crystal and superconductivity			Ames Laboratory, U.S. DOE, and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B,  96(2017)220510	Q.-P. Ding,W. R. Meier,A. E. Bohmer,S. L. Bud'ko,P. C. Canfield,Y. Furukawa		
157679	PRB096224433	not SC. Ferromag. below 2 K measured by zero-field muon-SR.	(Sm,La)NiC2	Sm0.15La0.85Ni1C2	Sm	0.15	La	0.85	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K					0.03																																																																																																		arc-melting					Ferromagnetic quantum criticality in Sm1-xLaxNiC2 (x = 0.85, 0.92, and 0.96)			Department of Physics, Chung-Ang University, Seoul 06974, Republic of Korea	Phys.Rev.B,  96(2017)224433	Wonjun Lee,S. Lee,K.-Y. Choi,K.-J. Lee,B.-J. Kim,B. J. Suh,S. Shin,T. Park		
157680	PRB096224433	not SC. Tm(FM) = 23 mK.	(Sm,La)NiC2	Sm0.08La0.92Ni1C2	Sm	0.08	La	0.92	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K					0.03																																																																																																		arc-melting					Ferromagnetic quantum criticality in Sm1-xLaxNiC2 (x = 0.85, 0.92, and 0.96)			Department of Physics, Chung-Ang University, Seoul 06974, Republic of Korea	Phys.Rev.B,  96(2017)224433	Wonjun Lee,S. Lee,K.-Y. Choi,K.-J. Lee,B.-J. Kim,B. J. Suh,S. Shin,T. Park		
157681	PRB096224433	microscopic coexistence of SC and FM below Tm = 250 mK from muon-SR	(Sm,La)NiC2	Sm0.04La0.96Ni1C2	Sm	0.04	La	0.96	Ni	1	C	2																1	2017																										ABC2		CeNiC2																		K		1.01					1.01																																																																																																arc-melting					Ferromagnetic quantum criticality in Sm1-xLaxNiC2 (x = 0.85, 0.92, and 0.96)			Department of Physics, Chung-Ang University, Seoul 06974, Republic of Korea	Phys.Rev.B,  96(2017)224433	Wonjun Lee,S. Lee,K.-Y. Choi,K.-J. Lee,B.-J. Kim,B. J. Suh,S. Shin,T. Park		
157682	PRB096224510	Tm(FM) = 15.0 K. FSC(ferromagnetic superconductor) below Tc	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																1	2017					My-B/Eu	7.95	23.6																			ABC4D4		CaRb1144			A	3.889		13.304											RbEu-1144	K		36.4		36.7			36.4																																																																																														Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157683	PRB096224510	Tm(FM) = 15.0 K. FSC(ferromagnetic superconductor) below Tc	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.9Ni0.1As4	Rb	1	Eu	1	Fe	3.9	Ni	0.1	As	4														1	2017					My-B/Eu	7.88	24.3																			ABC4D4		CaRb1144			A	3.89		13.284											RbEu-1144	K		30.3		30.6			30.3																																																																																														Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157684	PRB096224510	T<SDW> = 28.9 K. Tm(FM) = 15.0 K. FSC(ferromagnetic superconductor) below Tc	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.8Ni0.2As4	Rb	1	Eu	1	Fe	3.8	Ni	0.2	As	4														1	2017					My-B/Eu	8	24.5																			ABC4D4		CaRb1144			A	3.8909		13.274											RbEu-1144	K		23		22.1			23	MPH157684																																																																																													Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157685	PRB096224510	T<SDW> = 31.1 K. Tm(FM) = 15.0 K. FSC(ferromagnetic superconductor) below Tc	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.76Ni0.24As4	Rb	1	Eu	1	Fe	3.76	Ni	0.24	As	4														1	2017					My-B/Eu	7.65	24.3																			ABC4D4		CaRb1144			A	3.8878		13.268											RbEu-1144	K		18.1		15.9			18.1																																																																																														Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157686	PRB096224510	T<SDW> = 35.0 K. Tm(FM) = 15.1 K. SFM(superconducting ferromagnet) below Tc.	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.72Ni0.28As4	Rb	1	Eu	1	Fe	3.72	Ni	0.28	As	4														1	2017					My-B/Eu	7.46	24.2																			ABC4D4		CaRb1144			A	3.8889		13.263											RbEu-1144	K		11.2					11.2																																																																																														Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157687	PRB096224510	T<SDW> = 33.6 K. Tm(FM) = 14.7 K. SFM(superconducting ferromagnet) below Tc.	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.68Ni0.32As4	Rb	1	Eu	1	Fe	3.68	Ni	0.32	As	4														1	2017					My-B/Eu	7.85	24.4																			ABC4D4		CaRb1144			A	3.8877		13.261											RbEu-1144	K		2.1					2.1																																																																																														Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157688	PRB096224510	T<SDW> = 31.3 K. Tm(FM) = 14.7 K.	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.64Ni0.36As4	Rb	1	Eu	1	Fe	3.64	Ni	0.36	As	4														1	2017					My-B/Eu	7.79	24.8																			ABC4D4		CaRb1144			A	3.8892		13.256											RbEu-1144	K																																																																																																					Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157689	PRB096224510	T<SDW> = 29.4 K. Tm(FM) = 14.8 K.	RbEu(Fe,Ni)4As4	Rb1Eu1Fe3.6Ni0.4As4	Rb	1	Eu	1	Fe	3.6	Ni	0.4	As	4														1	2017					My-B/Eu	7.74	24.4																			ABC4D4		CaRb1144			A	3.8877		13.25											RbEu-1144	K																																																																																																					Rb(2N75),As(5N),Eu(3N),Fe(4N8),Ni(2N75)		precrsor(EuAs,FeAs,NiAs,RbFe2As2 with 5%excess Rb) + Fe powder - mixture - sealed in Ta tube in quartz ampoule - heat(1133 K, 20h)					RbEu(Fe1-xNix)4As4: From a ferromagnetic superconductor to a superconducting ferromagnet			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B,  96(2017)224510	Yi Liu,Ya-Bin Liu,Ya-Long Yu,Qian Tao,Chun-Mu Feng,Guang-Han Cao		
157690	MAT1503.05331	P-induced SC. Pc = 90 GPa. SC properties in DB shows for P=200 GPa.  Cell volume V(P) , See HallFig = MLAT157690	2H-MoS2	Mo1S2	Mo	1	S	2																				3	2015																										AB2		TX2																		K			12.2		0		12.2	MTC157690																			T	RES(0.9Rn), GL fitting	7.33												MHC157690																																																									MLAT157690										Ultrahigh Pressure Superconductivity in Molybdenum Disulfide			Key Laboratory of Materials Physics, Institute of Solid State Physics, Hefei Institutes of Physical Science, Chinese Academy of Sciences, Hefei 230031, China	cond-mat/1503.05331	Zhenhua Chi,Feihsiang Yen,Feng Peng,Jinlong Zhu,Yijin Zhang,Xuliang Chen,Zhaorong Yang,Xiaodi Liu,Yanming Ma,Yusheng Zhao,Tomoko Kagayama,Yoshihiro Iwasa		
157691	PRB097014501	RRR = 38. SP (beta) = 66.4 uJ/mol.K4. (dC<e>/gamma*Tc) = 1.26. e-ph = 0.5. GL(kappa) = 2.34. Debye-T = 398 K from R(T).	BeAu	Au1Be1	Au	1	Be	1																				1	2018																										AB		FeSi	P2<1>3	198	A	4.6699													For 860K < T, CsCl-type, Pm3[-]m, #221	K		3.3		3.3			3.3										100	Oe	M-H curve, GL fitting	32							Oe	See FIG, GL fitting	335												MHC157691		nm	from Hc2	99.1			nm	Hc1	231.7			meV	0.26	3.72	14				MSP157691			mJ/mol.K2	1.94	SP	388	SP											uOhm.cm							0.97				37												Be(3N),Au(3N5)		arc melting. mixture(Be:Au = 51:49). Sealed in Ta-tube in alumina crucible - ANN(400C, 48h)					Noncentrosymmetric superconductor BeAu			Max-Planck-Institut fur Chemische Physik fester Stoffe, Nothnitzer Strasse 40, 01187 Dresden, Germany	Phys.Rev.B, 97(2018)014501	A. Amon,E. Svanidze,R. Cardoso-Gil,M. N. Wilson,H. Rosner,M. Bobnar,W. Schnelle,J. W. Lynn,R. Gumeniuk,C. Hennig,G. M. Luke,H. Borrmann,A. Leithe-Jasper,Yu. Grin		
157692	PRB097014514	STS measured. gap vanishes at about 3.2 K. Tc = 3.05 K and Hc2 = 0.45 T assuming (2d/kTc) = 3.528(BCS) and BCS type T-dependence .	TlNi2Se2	Tl1Ni2Se2	Tl	1	Ni	2	Se	2																		3	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.87		13.435											Ni-based SC	K		3.7					3.7																																																																																														Tl,Ni,Se		self-flux method. stoichiometric(Tl,Ni,Se) - sealed in alumina crucible - heat(950C,12h) - cool to 700C(6 C/h). cleaved suface (001) under vac(1E-9 mbar)					Scanning tunneling microscopy and spectroscopy studies of the heavy-electron superconductor TlNi2Se2			Physikalisches Institut, Experimentelle Physik II, Universitat Wurzburg, Am Hubland, D-97074 Wurzburg, Germany	Phys.Rev.B, 97(2018)014514	Stefan Wilfert,Martin Schmitt,Henrik Schmidt,Tobias Mauerer,Paolo Sessi,Hangdong Wang,Qianhui Mao,Minghu Fang,Matthias Bode		
157693	PRB097014523	RRR = 75. Inhomogeneneity on surface. majority of Hc = 250 G at T=385 mK. Hc2(in DB) shows the field where STS signal deisapperes. gap = 326 uV at 385mK	PdTe2	Pd1Te2	Pd	1	Te	2																				3	2018																										AB2		CdI2	P3[-]m1	164																K		1.78					1.78	MGAP157693																			T	STS, (1-t^2)			1.6										MHC157693		nm	from Hc2		14									2	1				MSP157693																																									Pd(4N),Te(6N)		mixture(Pd:Te=1:2.2) - sealed in quartz tube - heat(790C,15h) - hold(48h) - cool to 500C over 7 days - ANN(500C,5d)					Conventional superconductivity in the type-II Dirac semimetal PdTe2			Department of Physical Sciences, Indian Institute of Science Education and Research (IISER), Mohali, Sector 81, S. A. S. Nagar, Manauli, PO: 140306, India	Phys.Rev.B, 97(2018)014523	Shekhar Das,Amit,Anshu Sirohi,Lalit Yadav,Sirshendu Gayen,Yogesh Singh,Goutam Sheet		
157694	PRB097020502	GL(kappa) = 53. [penet] = 298 nm from muon-SR. Gap size(2d/kTc) from SP analysis. (dC/gamma*Tc) = 1.4. Hc2(T)-FIG assuming Tc=6K (definition not described)	Re24Ti5	Re24Ti5	Re	24	Ti	5																				1	2018																										A5B24		alpha-Mn																		K	6		6.8	6			6											mT	M-H curve, GL fitting	8.3							T	RES, SP, WHH	11.2												MHC157694		nm	from Hc2	5.41			nm	Hc1	286					3.8	14							mJ/mol.K2	26.4	SP																																						arc-melting - ANN(900C,2w)					Nodeless superconductivity and time-reversal symmetry breaking in the noncentrosymmetric superconductor Re24Ti5			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.B, 97(2018)020502	T. Shang,G. M. Pang,C. Baines,W. B. Jiang,W. Xie,A. Wang,M. Medarde,E. Pomjakushina,M. Shi,J. Mesot,H. Q. Yuan,T. Shiroka		
157695	PRB097020508	M=NH3. intercalated sample. M-content not shown. compositions by ICP. measuements under hydrostatic-P.  Hall effect measured at 50 K. 2nd SC phase appears at P = 2 GPa.	Li0.36(NH3)yFe2As2	Li0.36M1Fe2As2	Li	0.36	M	1	Fe	2	As	2																3	2018																													I4/mmm	139	A	3.7704		16.973												K	42		44.3				43.15	MTC157695																																																																																				m3/C						MRH157695					See PREPID = 157609					High-Tc superconductivity up to 55 K under high pressure in a heavily electron doped Li0.36(NH3)yFe2Se2 single crystal			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 97(2018)020508	P. Shahi,J. P. Sun,S. H. Wang,Y. Y. Jiao,K. Y. Chen,S. S. Sun,H. C. Lei,Y. Uwatoko,B. S. Wang,J.-G. Cheng		
157696	PRB097024501	NMR, muon-SR measured. [penet](T) nearly const. for T < (Tc/3). penet(London) and energy gap obtained from muon-SR fitting. nodeless SC.	SrAuSi3	Sr1Au1Si3	Sr	1	Au	1	Si	3																		1	2018																										ABC3		BaNiS3	I4mm	107																K		1.54					1.54																																									nm	muon-SR	398			meV	0.213	3.3	16																																															solid state reaction method. Heat (1000-1200 C, P=6 GPa)					Microscopic investigation of the weakly correlated noncentrosymmetric superconductor SrAuSi3			Laboratorium fur Festkorperphysik, ETH Zurich, CH-8093 Zurich, Switzerland	Phys.Rev.B, 97(2018)024501	N. Barbero,P. K. Biswas,M. Isobe,A. Amato,E. Morenzoni,A. D. Hillier,H.-R. Ott,J. Mesot,T. Shiroka		
157697	PRB097024516	Structurally homogeneous material. X-ray coherence = 91 nm. Co-exist-phase(FM&SC) has Tc(17K) and Hc2(120T), 2nd SC-phase(Tc=41K, Hc2=9T). DB shows higher values. Tm(ferromag) = 12 K.	(Li,Fe)OHFeSe	Li0.8Fe1.2Se1H1O1	Li	0.8	Fe	1.2	Se	1	H	1													O	1		1	2018																											2		P4/nmm	129	A	3.7881		9.2714												K				40			40											mT	M-H curve, GL fitting	8.3							T	Mag-field-microwave-spectroscopy	120												MHC157697		nm	from Hc2	1.63																																																										(Fe + selenourea ; LiOH/H2O) -mixed with distilled water(10 ml) -sealed in Teflon-lined autoclave - heat (155 C, 6d) - washed - dry under vac.					Coexistence of multiphase superconductivity and ferromagnetism in lithiated iron selenide hydroxide [(Li1-xFex)OH]FeSe			Department of Physics and Center for Advanced Nanoscience, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)024516	Christian Urban,Ilya Valmianski,Ursula Pachmayr,Ali C. Basaran,Dirk Johrendt,Ivan K. Schuller		
157698	PRB097054506	RRR=21. SP (beta) = 0.014 mJ/mol.K4. Two gap model, large(in DB), small (d2/kTc = 1.13) from SP analysis. (dC/gamma*Tc) = 1.42. Thermodynamic Hc(0) = 114Oe. e-ph = 0.37.GL(kappa) = 0.1. Type-I SC.	RuB2	B2Ru1	B	2	Ru	1																				1	2018																										AB2		RuB2	Pmmn		A	4.6457	2.8657	4.0442											STR data same as PRB076214510	K		1.5		1.55			1.5										90	Oe	Type-I, M-H	122																					MHC157698		nm	effective mass	450			nm	London, effective mass	47					3.76	14				MSP157698			mJ/mol.K2	1.65	SP	720	SP											uOhm.cm							1.1				22.5												Ru(5N),B(6N)		ac-melting					Possible multigap type-I superconductivity in the layered boride RuB2			Department of Physical Sciences, Indian Institute of Science Education and Research (IISER) Mohali, Knowledge City, Sector 81, Mohali 140306, India	Phys.Rev.B, 97(2018)054506	Jaskaran Singh,Anooja Jayaraj,D. Srivastava,S. Gayen,A. Thamizhavel,Yogesh Singh		
157699	PRB097054515	RRR = 75. Tc(SP) = 1.72 k. SP (beta) = 0.66 mJ/mol.K4. (dC/gamma*Tc) =1.52	PdTe2	Pd1Te2	Pd	1	Te	2																				3	2018																										AB2		CdI2	P3m1	164																K	1.75						1.75																				Oe	SP, Entropy correction	195																															MSP157699			mJ/mol.K2	6.01	SP													uOhm.cm								0.94				70											Pd(4N),Te(6N)		Modified Bridgman method. mixture(Pd:Te = 1:2.2) - in quartz tube - heat(790C, 15h) - keep(48h) - cool to 500C over 7 days - ANN(500C,5d) - cool to RT naturally					Heat capacity evidence for conventional superconductivity in the type-II Dirac semimetal PdTe2			Department of Physical Sciences, Indian Institute of Science Education and Research (IISER) Mohali, Knowledge City, Sector 81, Mohali 140306, India	Phys.Rev.B, 97(2018)054515	Amit,Yogesh Singh		
157700	PRB097054522		La(Fe,Mn)AsO0.89F0.11	La1Fe0.995Mn0.005As1F0.11O0.89	La	1	Fe	0.995	Mn	0.005	As	1	F	0.11											O	0.89		1	2018																												oxypnictide			A			8.7098											Fe-1111	K		15					15																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157701	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.99Y0.01Fe0.995Mn0.005As1F0.11O0.89	La	0.99	Y	0.01	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.7126											Fe-1111	K		10.9					10.9																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157702	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.97Y0.03Fe0.995Mn0.005As1F0.11O0.89	La	0.97	Y	0.03	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.697											Fe-1111	K		19					19																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157703	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.95Y0.05Fe0.995Mn0.005As1F0.11O0.89	La	0.95	Y	0.05	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.7075											Fe-1111	K		21					21	MTC157703																																																																																																				Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157704	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.9Y0.1Fe0.995Mn0.005As1F0.11O0.89	La	0.9	Y	0.1	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.6978											Fe-1111	K		25					25																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157705	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.85Y0.15Fe0.995Mn0.005As1F0.11O0.89	La	0.85	Y	0.15	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.6735											Fe-1111	K		26					26																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157706	PRB097054522		(La,Y)Fe0.995Mn0.005AsO0.89F0.11	La0.8Y0.2Fe0.995Mn0.005As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.995	Mn	0.005	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A			8.6686											Fe-1111	K		29.1					29.1																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157707	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe1As1F0.11O0.89	La	0.8	Y	0.2	Fe	1	As	1	F	0.11											O	0.89		1	2018																												oxypnictide			A														Fe-1111	K		33.2					33.2																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157708	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.999Mn0.001As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.999	Mn	0.001	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	3.9956		8.6539											Fe-1111	K		31.8		33.3			31.8																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157709	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.998Mn0.002As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.998	Mn	0.002	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0041		8.6688											Fe-1111	K		31.2		32.1			31.2																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157710	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.992Mn0.008As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.992	Mn	0.008	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0039		8.6722											Fe-1111	K		25		25			25	MTC157710																																																																																																				Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157711	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.985Mn0.015As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.985	Mn	0.015	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0016		8.6694											Fe-1111	K		20.2		18.9			20.2																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157712	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.98Mn0.02As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.98	Mn	0.02	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0052		8.6795											Fe-1111	K				11			11																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157713	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.975Mn0.025As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.975	Mn	0.025	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0052		8.6817											Fe-1111	K		10.1		8.9			10.1																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157714	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.97Mn0.03As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.97	Mn	0.03	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0035		8.6717											Fe-1111	K		10.8		9.1			10.8																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157715	PRB097054522		La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.965Mn0.035As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.965	Mn	0.035	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0015		8.6803											Fe-1111	K		4.7		0			4.7																																																																																																					Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157716	PRB097054522	not SC	La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.95Mn0.05As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.95	Mn	0.05	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0009		8.6835											Fe-1111	K					0																																																																																																							Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157717	PRB097054522	not SC	La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.9Mn0.1As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.9	Mn	0.1	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0092		8.7227											Fe-1111	K					0																																																																																																							Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157718	PRB097054522	not SC	La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.85Mn0.15As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.85	Mn	0.15	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.012		8.7304											Fe-1111	K					0																																																																																																							Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157719	PRB097054522	not SC	La0.8Y0.2Fe1-xMnxAsO0.89F0.11	La0.8Y0.2Fe0.8Mn0.2As1F0.11O0.89	La	0.8	Y	0.2	Fe	0.8	Mn	0.2	As	1	F	0.11									O	0.89		1	2018																												oxypnictide			A	4.0181		8.751											Fe-1111	K					0																																																																																																							Impact of concomitant Y and Mn substitution on superconductivity in La1-yYyFe1-xMnxAsO0.89F0.11			Leibniz Institute for Solid State and Materials Research, 01069 Dresden, Germany	Phys.Rev.B, 97(2018)054522	Rhea Kappenberger,Franziska Hammerath,Pierre Rousse,Mesfin Asfaw Afrassa,M. Hossein Haghighi,Sirko Kamusella,Giacomo Prando,Gianrico Lamura,Anja U. B. Wolter,Matteo Moroni,Samuele Sanna,Pietro Carretta,Christian Hess,Hans-Joachim Grafe,Hans-Henning Klauss,Sabine Wurmehl,Bernd Buchner		
157720	PRB097060503	P-induced SC. quasi-hydrostatic P. P releasing at 7GPa, Tc(on) = 3.2 k and Tc(zero) = 1.6 K at P = 0.5 GPa,  P-quenching. (dTc/dP) shows at P<cr>(=5 GPa)	1T-TiTe2	Te2Ti1	Te	2	Ti	1																				3	2018																										AB2																			1T-TiTe2	K			2.5		0		2.5	MTC157720		K/GPa	0.35																T	RES(0.9Rn)													MHC157720																																																			m3/C	0.00083					MRH157720					vapor transport method using iodine as a transport agent.					Pressure-induced superconductivity in semimetallic 1T-TiTe2 and its persistence upon decompression			High Pressure & Synchrotron Radiation Physics Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400085, India	Phys.Rev.B, 97(2018)060503	U. Dutta,P. S. Malavi,S. Sahoo,B. Joseph,S. Karmakar		
157721	PRB097060503	P-induced SC. non-hydrostatic P. Semimetal for P < 1.8 GPa.  (dTc/dP) shows at P<cr>(=6 GPa)	1T-TiTe2	Te2Ti1	Te	2	Ti	1																				3	2018																										AB2																			1T-TiTe2	K			2.98		0		2.98	MTC157721		K/GPa	0.06																																																																																												vapor transport method using iodine as a transport agent.					Pressure-induced superconductivity in semimetallic 1T-TiTe2 and its persistence upon decompression			High Pressure & Synchrotron Radiation Physics Division, Bhabha Atomic Research Centre, Trombay, Mumbai 400085, India	Phys.Rev.B, 97(2018)060503	U. Dutta,P. S. Malavi,S. Sahoo,B. Joseph,S. Karmakar		
157722	PRB097060506	SC poperties obtained by muon-SR analysis. two gap fitting : large gap in DB, small one ( d2=1.5 meV), weight of d1/d2  = 0.73)	CsCa2Fe4As4F2	Cs1Ca2Fe4As4F2	Cs	1	Ca	2	Fe	4	As	4	F	2														1	2018																										AB2C2D4E4																			12442-structure	K		28.31					28.31																																		PENE157722							nm	muon-SR		244		meV	7.5	3.1	16																																															solid state reaction metod. Details , See J.Am.Chem.Soc., 138(2016)7856					Two-gap superconductivity with line nodes in CsCa2Fe4As4F2			Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 97(2018)060506	Franziska K. K. Kirschner,Devashibhai T. Adroja,Zhi-Cheng Wang,Franz Lang,Michael Smidman,Peter J. Baker,Guang-Han Cao,Stephen J. Blundell		
157723	PRB097060509	SC poperties obtained by muon-SR analysis. two gap fitting : large gap in DB, small one ( d2=1.84 meV, 2d2/kTc = 1.29).	KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2														1	2018																										AB2C2D4E4																			12442-structure	K		33.36		33			33.36																																									nm	muon-SR		229.5		meV	10.12	7.11	16																																															solid state reaction metod. Details , See J.Am.Chem.Soc., 138(2016)7856					Nodal multigap superconductivity in KCa2Fe4As4F2			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 97(2018)060509	M. Smidman,F. K. K. Kirschner,D. T. Adroja,A. D. Hillier,F. Lang,Z. C. Wang,G. H. Cao,S. J. Blundell		
157724	PRB097064514	P-induced SC. P<cr> = 19.7 GPa. RRR = 13. SC-properties shows for P=21.5 GPa. For P < 13.6 GPa, two Tn(AFM). At P = 0, Tn1=14.7K, Tn2=7.51K. bulk modulas = 115 GPa.	CeRhGe3	Ce1Rh1Ge3	Ce	1	Rh	1	Ge	3																		3	2018								14.7																		ABC3			I4mm		A	4.3977		10.0345												K			1.33		0		1.33	MPH157724																			T	RES, linear approx.	15							T/K	RES	11.5			MHC157724																																																														(Ce:Rh:Ge = 1:3.5:13.5, CeRhGe6 + 10Rh0.25Ge0.75) - arc melting - alumina crucible - sealed in quartz tube - heat(1150C,12h) - cool to 875C(2C/h) - remove flux					Superconductivity in pressurized CeRhGe3 and related noncentrosymmetric compounds			Institute of Physics, National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 97(2018)064514	Honghong Wang,Jing Guo,Eric D. Bauer,Vladimir A. Sidorov,Hengcan Zhao,Jiahao Zhang,Yazhou Zhou,Zhe Wang,Shu Cai,Ke Yang,Aiguo Li,Xiaodong Li,Yanchun Li,Peijie Sun,Yi-feng Yang,Qi Wu,Tao Xiang,J. D. Thompson,Liling Sun		
157725	PRB097064514	Lattice const measured for P < 30 GPa.	CeRhGe3	Ce1Rh1Ge3	Ce	1	Rh	1	Ge	3																		3	2018																										ABC3			I4mm		A	4.3977		10.0345												K								MLAT157725																																																																																															(Ce:Rh:Ge = 1:3.5:13.5, CeRhGe6 + 10Rh0.25Ge0.75) - arc melting - alumina crucible - sealed in quartz tube - heat(1150C,12h) - cool to 875C(2C/h) - remove flux					Superconductivity in pressurized CeRhGe3 and related noncentrosymmetric compounds			Institute of Physics, National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 97(2018)064514	Honghong Wang,Jing Guo,Eric D. Bauer,Vladimir A. Sidorov,Hengcan Zhao,Jiahao Zhang,Yazhou Zhou,Zhe Wang,Shu Cai,Ke Yang,Aiguo Li,Xiaodong Li,Yanchun Li,Peijie Sun,Yi-feng Yang,Qi Wu,Tao Xiang,J. D. Thompson,Liling Sun		
157726	PRB097094505	M=(NH3). Low-Tc phase(contains 3 phases: low-Tc + beta-FeSe + Fe7Se8). NH3 content not shown	(NH3)yNaxFeAs(x=0.4)	Na0.4M1Fe1As1	Na	0.4	M	1	Fe	1	As	1																	2018																															A	3.8697		13.5451												K			38	35			35	MTC157726									48																																																																																											Pressure dependence of superconductivity in low- and high-Tc phases of (NH3)yNaxFeSe			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 97(2018)094505	Takahiro Terao,Xiaofan Yang,Xiao Miao,Lu Zheng,Hidenori Goto,Takafumi Miyazaki,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Yoshihiro Kubozono		
157727	PRB097094505	M=(NH3). High-Tc phase(contains 3 phases: High-Tc +  low-Tc + Fe7Se8).  NH3 content not shown.	(NH3)yNaxFeAs(x=0.6)	Na0.6M1Fe1As1	Na	0.6	M	1	Fe	1	As	1																	2018																															A	3.7836		17.0834												K			45	44			44	MTC157727									33																																																																																											Pressure dependence of superconductivity in low- and high-Tc phases of (NH3)yNaxFeSe			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 97(2018)094505	Takahiro Terao,Xiaofan Yang,Xiao Miao,Lu Zheng,Hidenori Goto,Takafumi Miyazaki,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Yoshihiro Kubozono		
157728	PRB097094506	[penet], energy gap, carrier obtained from muon-SR analysis. Fully gaped s-wave gap. effective mass = 9.8m<e> estimated.	LuRuB2	Lu1Ru1B2	Lu	1	Ru	1	B	2																		1	2018																										ABC2	3	LuRuB2	Pnma		A	5.8075	5.2323	6.279												K				9.8			9.8																																									nm	muon-SR	221			meV	1.36	3.3	16																																											n/m3	27300000000000000000000000000			arc-melting using tri-arc furnace(Ar) - ANN(1050C, 1 week, in evacuated quartz tube)					Probing the superconducting ground state of the rare-earth ternary boride superconductors RRuB2 (R = Lu,Y) using muon-spin rotation and relaxation			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 97(2018)094506	J. A. T. Barker,R. P. Singh,A. D. Hillier,D. McK. Paul		
157729	PRB097094506	[penet], energy gap, carrier obtained from muon-SR analysis. Fully gaped s-wave gap. effective mass = 15.0m<e> estimated.	YRuB2	Y1Ru1B2	Y	1	Ru	1	B	2																		1	2018																										ABC2	3	LuRuB2	Pnma		A	5.9071	5.2971	6.3535												K				7.8			7.8																																									nm	muon-SR	190			meV	1.1	3.4	16																																											n/m3	21700000000000000000000000000			arc-melting using tri-arc furnace(Ar) - ANN(1050C, 1 week, in evacuated quartz tube)					Probing the superconducting ground state of the rare-earth ternary boride superconductors RRuB2 (R = Lu,Y) using muon-spin rotation and relaxation			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 97(2018)094506	J. A. T. Barker,R. P. Singh,A. D. Hillier,D. McK. Paul		
157730	PRB097094509	Isotope effect dTc < 0.01 K for sample with <76>Se and <80>Se, then isotope exponent = 0.	LaO0.6F0.4Bi(S,Se)2	La1F0.4Bi1S0.899Se1.101O0.6	La	1	F	0.4	Bi	1	S	0.899	Se	1.101											O	0.6		1	2018																													P4/nmm		A	4.13711		13.6022											BiS2-layer SC	K	3.73		3.75	3.77			3.77						0	Se	99.8	0																																																																																					La2S3,La2O3,BiF3(3N),Bi2O3(4N),Bi(5N)		mixture - pellet - sealed in quartz tube -heat(700C,20h) - ground - pellet - ANN(700C,20h, in quartz tube)					Selenium isotope effect in the layered bismuth chalcogenide superconductor LaO0.6F0.4Bi(S,Se)2			Department of Physics, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan	Phys.Rev.B, 97(2018)094509	Kazuhisa Hoshi,Yosuke Goto,Yoshikazu Mizuguchi		
157731	PRB097094509	Isotope effect dTc < 0.01 K for sample with <76>Se and <80>Se, then isotope exponent = 0.	LaO0.6F0.4Bi(S,Se)2	La1F0.4Bi1S0.906Se1.094O0.6	La	1	F	0.4	Bi	1	S	0.906	Se	1.094											O	0.6		1	2018																													P4/nmm		A	4.13887		13.6031											BiS2-layer SC	K				3.76			3.76						0	Se	99.8	0																																																																																					La2S3,La2O3,BiF3(3N),Bi2O3(4N),Bi(5N)		mixture - pellet - sealed in quartz tube -heat(700C,20h) - ground - pellet - ANN(700C,20h, in quartz tube)					Selenium isotope effect in the layered bismuth chalcogenide superconductor LaO0.6F0.4Bi(S,Se)2			Department of Physics, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan	Phys.Rev.B, 97(2018)094509	Kazuhisa Hoshi,Yosuke Goto,Yoshikazu Mizuguchi		
157732	PRB097094509	Isotope effect dTc < 0.01 K for sample with <76>Se and <80>Se, then isotope exponent = 0.	LaO0.6F0.4Bi(S,Se)2	La1F0.4Bi1S0.872Se1.128O0.6	La	1	F	0.4	Bi	1	S	0.872	Se	1.128											O	0.6		1	2018																													P4/nmm		A	4.13567		13.6014											BiS2-layer SC	K	3.73		3.75	3.76			3.76						0	Se	99.91	0																																																																																					La2S3,La2O3,BiF3(3N),Bi2O3(4N),Bi(5N)		mixture - pellet - sealed in quartz tube -heat(700C,20h) - ground - pellet - ANN(700C,20h, in quartz tube)					Selenium isotope effect in the layered bismuth chalcogenide superconductor LaO0.6F0.4Bi(S,Se)2			Department of Physics, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan	Phys.Rev.B, 97(2018)094509	Kazuhisa Hoshi,Yosuke Goto,Yoshikazu Mizuguchi		
157733	PRB097094509	Isotope effect dTc < 0.01 K for sample with <76>Se and <80>Se, then isotope exponent = 0.	LaO0.6F0.4Bi(S,Se)2	La1F0.4Bi1S0.863Se1.137O0.6	La	1	F	0.4	Bi	1	S	0.863	Se	1.137											O	0.6		1	2018																													P4/nmm		A	4.13917		13.6333											BiS2-layer SC	K	3.72			3.77			3.77						0	Se	99.91	0																																																																																					La2S3,La2O3,BiF3(3N),Bi2O3(4N),Bi(5N)		mixture - pellet - sealed in quartz tube -heat(700C,20h) - ground - pellet - ANN(700C,20h, in quartz tube)					Selenium isotope effect in the layered bismuth chalcogenide superconductor LaO0.6F0.4Bi(S,Se)2			Department of Physics, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan	Phys.Rev.B, 97(2018)094509	Kazuhisa Hoshi,Yosuke Goto,Yoshikazu Mizuguchi		
157734	PRB097100504	Structure, SG= Cmme (#67) at T=15 K. R(T) shows Fermi liquid type above Tc.	LaFeSiH	La1Fe1Si1H1	La	1	Fe	1	Si	1	H	1																1	2018																										ABCD			P4/nmm	129	A	4.027		8.0374											At 15K, SG = Cmme, #67, a= 5.6831, b=5.7039, c=7.9728	K		9.7	11				9.7	MTC157734									64	mT	M-H curve				0.3			2	T	RES(0.5Rn), WHH		17						T/K	RES(0.5Rn)				MHC157734		nm	from Hc2	4.3																																																															Iron-based superconductivity extended to the novel silicide LaFeSiH			Dipartimento di Fisica, Universita di Cagliari, IT-09042 Monserrato, Italy	Phys.Rev.B, 97(2018)100504	F. Bernardini,G. Garbarino,A. Sulpice,M. Nunez-Regueiro,E. Gaudin,B. Chevalier,M.-A. Measson,A. Cano,S. Tence		
157735	PRB097100505	muon-SR fitting: Tc=5.98 K, gap(d) = 0.95 meV, d(0)/kTc = 1.84.  SP (dC<e>/gamma*Tc) = 1.58	Re6Ti	Re6Ti1	Re	6	Ti	1																				1	2018																										AB6		alpha-Mn	I4[-]3m	217	A	9.58														K				6			6																																									A	muon-SR	4937			meV	0.95	3.68	16				MSP157735																																									Re(3N5),Ti(3N5)		arc-melting - ANN(850C,1week, in quartz tube)					Time-reversal symmetry breaking in the noncentrosymmetric superconductor Re6Ti			Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India	Phys.Rev.B, 97(2018)100505	D. Singh,Sajilesh K. P,J. A. T. Barker,D. McK. Paul,A. D. Hillier,R. P. Singh		
157736	PRB097104503	Phase-I(P <8.8 GPa). not SC. Ag replaced Bi, not intercalated.	AgxBi2-xSe3	Ag0.05Bi1.95Se3	Ag	0.05	Bi	1.95	Se	3																		3	2018																													R3[-]m	166	A	4.146		28.66												K					0																																																																																																		stoichiometric(Ag,Bi,Se) powder - sealed in quartz tube - heat(800C,12h) - slow cool to 650C(30C/h) - Q to ice water					Pressure-induced superconductivity in AgxBi2-xSe3			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 97(2018)104503	Tong He,Xiaofan Yang,Takahiro Terao,Takaki Uchiyama,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Takafumi Miyazaki,Takumi Nishioka,Koji Kimura,Kouichi Hayashi,Naohisa Happo,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Yoshihiro Kubozono		
157737	PRB097104503	Phase-II(8.8 <P<21 GPa). P-induced SC. Tc & Hc2 for P=11 GPa.	AgxBi2-xSe3	Ag0.05Bi1.95Se3	Ag	0.05	Bi	1.95	Se	3																		3	2018																													C2/m	12	A	13.637	3.9252	16.251											monoclinic, beta = 148.87	K					0			MTC157737																																	MHC157737																																																														stoichiometric(Ag,Bi,Se) powder - sealed in quartz tube - heat(800C,12h) - slow cool to 650C(30C/h) - Q to ice water					Pressure-induced superconductivity in AgxBi2-xSe3			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 97(2018)104503	Tong He,Xiaofan Yang,Takahiro Terao,Takaki Uchiyama,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Takafumi Miyazaki,Takumi Nishioka,Koji Kimura,Kouichi Hayashi,Naohisa Happo,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Yoshihiro Kubozono		
157738	PRB097104503	Phase-III(P>21 GPa). P-induced SC. Tc & Hc2 for P=20.5 GPa.	AgxBi2-xSe3	Ag0.05Bi1.95Se3	Ag	0.05	Bi	1.95	Se	3																		3	2018																													I4/mmm	139	A	3.461		16.628												K					0			MTC157737																																	MHC157738																																																														stoichiometric(Ag,Bi,Se) powder - sealed in quartz tube - heat(800C,12h) - slow cool to 650C(30C/h) - Q to ice water					Pressure-induced superconductivity in AgxBi2-xSe3			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 97(2018)104503	Tong He,Xiaofan Yang,Takahiro Terao,Takaki Uchiyama,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Takafumi Miyazaki,Takumi Nishioka,Koji Kimura,Kouichi Hayashi,Naohisa Happo,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Yoshihiro Kubozono		
157739	PRB097104509	Anisotropy(Hc2)= 16 at 0 K. Hc2(T) measured by H-sweep and T-sweep. Hc2(0) by using two gap model. Angular dependence of Hc2 also measured.	La(O,F)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		3	2018																										ABCD2		CeOBiS2	P4/nmm		A	4.0585		13.324												K		3.7	5				3.7																				T	RES(0.5Rn),two gap model		16.2	1										MHC157739		nm	from Hc2		21.7	1.13																																																						La2S3,Bi2S3,BiF3,Bi,BiS3		CsCl-flux method. sealed in quartz tube(vac) - ANN(900C,12h) - cool to 500C(2.4C/h) - remove flux by H2O					Anisotropic two-gap superconductivity and the absence of a Pauli paramagnetic limit in single-crystalline LaO0.5F0.5BiS2			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 97(2018)104509	Y. C. Chan,K. Y. Yip,Y. W. Cheung,Y. T. Chan,Q. Niu,J. Kajitani,R. Higashinaka,T. D. Matsuda,Y. Yanase,Y. Aoki,K. T. Lai,Swee K. Goh		
157740	PRL102207001	[penet] measured by surface impedance. [penet](0) not shown. Energy gap obtained by d{penet] using 2 gap model, large in DB, small (d1) = 1.17 kTc.	(Ba,K)Fe2As2	Ba0.45K0.55Fe2As2	Ba	0.45	K	0.55	Fe	2	As	2																3	2009																										AB2C2		ThCr2Si2																		K				32.7			32.7																																																4.8	7																																															self-flux method. mixture - heat(1190C) - cool to 850C(4C/h) - quench. cleaved surface were used.					Microwave Surface-Impedance Measurements of the Magnetic PenetrationDepth in Single Crystal Ba1-xKxFe2As2 Superconductors: Evidence for a Disorder-Dependent Superfluid Density			Department of Physics, Kyoto University, Sakyo-ku, Kyoto 606-8502, Japan	Phys.Rev.Lett., 102(2009)207001	K. Hashimoto,T. Shibauchi,S. Kasahara,K. Ikada,S. Tonegawa,T. Kato,R. Okazaki,C. J. van der Beek,M. Konczykowski,H. Takeya,K. Hirata,T. Terashima,Y. Matsuda		
157741	PRL109187004	P-induced SC. data for P = 8.7 GPa. RRR=76. Tmax(max of Rmag(T)) = 27.9 K. Tq(quadrupole order) = 2.1 K. m*/m0 = 106.	PrTi2Al20	Pr1Ti2Al20	Pr	1	Ti	2	Al	20																		3	2012																										AB2C20		CeCr2Al20	Fd3[-]m																	K	1.08			1.12	0		1.12																				T	RES(zero), WHH	4.7							T/K	RES(zero)	6			MHC157742		A	from Hc2	84																																	uOhm.cm							3.28																		Al-flux method					Pressure-Induced Heavy Fermion Superconductivity in the Nonmagnetic Quadrupolar System PrTi2Al20			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 109(2012)187004	K. Matsubayashi,T. Tanaka,A. Sakai,S. Nakatsuji,Y. Kubo,Y. Uwatoko		
157742	PRL109187004	P-induced SC. P<cr> = 6.7 GPa. Tc(DB) shows for P = P<cr>. Hc2(T)  for P=6.7, 7.7, 8.7 GPa.	PrTi2Al20	Pr1Ti2Al20	Pr	1	Ti	2	Al	20																		3	2012																										AB2C20		CeCr2Al20	Fd3[-]m																	K	0.5			0.61	0		0.61	MTC157742																																	MHC157742																																																														Al-flux method					Pressure-Induced Heavy Fermion Superconductivity in the Nonmagnetic Quadrupolar System PrTi2Al20			Institute for Solid State Physics, The University of Tokyo, Kashiwanoha, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 109(2012)187004	K. Matsubayashi,T. Tanaka,A. Sakai,S. Nakatsuji,Y. Kubo,Y. Uwatoko		
157743	PRL113267001	RRR = 19. Tc depends on RRR.   SP (dC/Tc) = 0.3 J/mol.K2, (dC/gamma*Tc) = 0.3. effective mass m* = 140 m0.	PrV2Al20	Pr1V2Al20	Pr	1	V	2	Al	20																		3	2014																										AB2C20		CeCr2Al20																		K	0.046		0.05				0.048										82										mT	RES(zero), WHH			14.3					T/K	RES(zero)			0.41	MHC157743		nm	from Hc2		150																	mJ/mol.K2	900																																												Heavy-Fermion Superconductivity in the Quadrupole Ordered State of PrV2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 113(2014)267001	Masaki Tsujimoto,Yosuke Matsumoto,Takahiro Tomita,Akito Sakai,Satoru Nakatsuji		
157744	PRL120037002	P-induced SC. phase transition (Hc-to-Ha) at P=25 GPa. P<cr> = 90 GPa. Tc & Hc2 for P = 220 GPa. R-exponent n = 3 for 0<T<50 K at P=220 GPa. bulk modulus = 50, 110 GPa for Hc and Ha phase.	2Ha-MoS2	Mo1S2	Mo	1	S	2																				3	2018																										AB2		2H-MoS2																	2Hc- to 2Ha-MoS2 phase transition at P=25 GPa	K			12		0		12	MTC157744																			T	RES(onset), WHH	7.5												MHC157744																																																														2Hc-MoS2 grown by chemical vapor transport method					Superconductivity in Pristine 2Ha-MoS2 at Ultrahigh Pressure			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.Lett., 120(2018)037002	Zhenhua Chi,Xuliang Chen,Fei Yen,Feng Peng,Yonghui Zhou,Jinlong Zhu,Yijin Zhang,Xiaodi Liu,Chuanlong Lin,Shengqi Chu,Yanchun Li,Jinggeng Zhao,Tomoko Kagayama,Yanming Ma,Zhaorong Yang		
157745	PRL120037002	TCFIG syows P-dependence of lattice const	2Ha-MoS2	Mo1S2	Mo	1	S	2																				3	2018																										AB2		2H-MoS2																	2Hc- to 2Ha-MoS2 phase transition at P=25 GPa	K					0			MLAT157745																																																																																															2Hc-MoS2 grown by chemical vapor transport method					Superconductivity in Pristine 2Ha-MoS2 at Ultrahigh Pressure			Key Laboratory of Materials Physics, Institute of Solid State Physics, Chinese Academy of Sciences, Hefei 230031, People's Republic of China	Phys.Rev.Lett., 120(2018)037002	Zhenhua Chi,Xuliang Chen,Fei Yen,Feng Peng,Yonghui Zhou,Jinlong Zhu,Yijin Zhang,Xiaodi Liu,Chuanlong Lin,Shengqi Chu,Yanchun Li,Jinggeng Zhao,Tomoko Kagayama,Yanming Ma,Zhaorong Yang		
157746	SCI3381193	Mo-based EDLT device. Tc(DB) shows Tc(max). Tc(seet resistance) depens on carrier density n<2D> (measured by the Hall effect at 20 K), controlled by voltage of liquid gate(LG) and back gate(BG).	e-doped MoS2	Mo1S2	Mo	1	S	2																					2012																										AB2																				K			10.8		0		10.8	MTC157746																																																																																															To make, we isolated thin flakes of MoS2 from a bulk 2H-type single crystal by Scotch tape method and transferred them onto the surface of HfO2 grown by atomic layer deposition on a Nb-doped SrTiO3					Superconducting Dome in a Gate-Tuned Band Insulator			Quantum-Phase Electronics Center and Department of Applied Physics, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan.	Science, 338(2012)1193	J. T. Ye,Y. J. Zhang,R. Akashi,M. S. Bahramy,R. Arita,Y. Iwasa		
157800	CHPL6920249	2H-phase. volume=128.5 A3. bulk modulus , compressbility from X-ray analysis.	2H-NbSe2	Nb1Se2	Nb	1	Se	2																				1	2018																		GPa		52						AB2	7	MX2	P6<3>mmc	194	A	3.442		12.539							k0/GPa	0.0033		0.0174	k0 = a0 or c0 at ambient P	K				7			7																																																																																														Nb,Se,Te,powder(4N5 all)		mixture - pellet - sealed in quartz tube in furnace - heat to 750C (10K/min) - keep (750C,16h) - ANN(600C,96h)					Effect of pressure on crystal structure and superconductivity of NbSexTe2-x (x = 2, 1.5)			High Pressure Science and Engineering Center and Department of Physics and Astronomy, University of Nevada Las Vegas, Las Vegas, NV 89154, USA	Chem.Phys.Lett., 692(2018)249	Vahe Mkrtchyan,Ravhi Kumar,Melanie White,Howard Yanxon,Andrew Cornelius		
157801	CHPL6920249	2H-phase. volume=132 A3. bulk modulus , compressbility from X-ray analysis. (dTc/dP)  for P < 1.8 GPa	2H-Nb(Se,Te)2	Nb1Se1.5Te0.5	Nb	1	Se	1.5	Te	0.5																		1	2018																		GPa		61.7						AB2	7	MX2	P6<3>mmc	194	A	3.461		12.728							k0/GPa	0.0029		0.0115	k0 = a0 or c0 at ambient P	K			3.35				3.35	MTC157801		K/GPa	0.6																																																																																										Nb,Se,Te,powder(4N5 all)		mixture - pellet - sealed in quartz tube in furnace - heat to 750C (10K/min) - keep (750C,16h) - ANN(600C,96h)					Effect of pressure on crystal structure and superconductivity of NbSexTe2-x (x = 2, 1.5)			High Pressure Science and Engineering Center and Department of Physics and Astronomy, University of Nevada Las Vegas, Las Vegas, NV 89154, USA	Chem.Phys.Lett., 692(2018)249	Vahe Mkrtchyan,Ravhi Kumar,Melanie White,Howard Yanxon,Andrew Cornelius		
157802	JAC7410840	YGe1.5+z, vacancy z = 0.17	YGe1.5+z	Ge1.67Y1Ge2	Ge	1.67	Y	1	Ge	2																		1	2018																													Cmmm	63	A															K				3.9			3.9																																																																																														Y(3N),Ge(6N),T(2N8-3N8)		arc-melting. (Y:T:Ge = 1:x:2(with 3% excess Ge)					Electron counts, structural stability, and magnetism in BaCuSn2-CeNi1- xSi2-type YTxGe2 (T =  Cr, Mn, Fe, Co, and Ni)			Department of Chemistry, Louisiana State University, Baton Rouge, LA 70803, USA	J.Alloys Compd., 741(2018)840	Lea Gustin,Lingyi Xing,Max T. Pan,Rongying Jin,Weiwei Xie		
157803	JAC7410840	not SC. Ferro-mag at low-T. YMnxGe2, YGe1.5+x(minor phase)	YMnxGe2	Y1Mn0.24Ge2	Y	1	Mn	0.24	Ge	2																		1	2018			emu.K/mol	0.093	my-B/f.u	0.86	273																						Cmmm	63	A	4.1063	15.863	3.9571												K					0																																																																																																Y(3N),Ge(6N),T(2N8-3N8)		arc-melting. (Y:T:Ge = 1:x:2(with 3% excess Ge)					Electron counts, structural stability, and magnetism in BaCuSn2-CeNi1- xSi2-type YTxGe2 (T =  Cr, Mn, Fe, Co, and Ni)			Department of Chemistry, Louisiana State University, Baton Rouge, LA 70803, USA	J.Alloys Compd., 741(2018)840	Lea Gustin,Lingyi Xing,Max T. Pan,Rongying Jin,Weiwei Xie		
157804	JAC7410840	not SC. Para-mag at low-T. YCrxGe2, YGe1.5+x(minor phase)	YCrxGe2	Y1Cr0.23Ge2	Y	1	Cr	0.23	Ge	2																		1	2018			emu.K/mol	0.00056	my-B/f.u	0.07	-3.58																						Cmmm	63	A	4.119	15.861	3.997												K					0																																																																																																Y(3N),Ge(6N),T(2N8-3N8)		arc-melting. (Y:T:Ge = 1:x:2(with 3% excess Ge)					Electron counts, structural stability, and magnetism in BaCuSn2-CeNi1- xSi2-type YTxGe2 (T =  Cr, Mn, Fe, Co, and Ni)			Department of Chemistry, Louisiana State University, Baton Rouge, LA 70803, USA	J.Alloys Compd., 741(2018)840	Lea Gustin,Lingyi Xing,Max T. Pan,Rongying Jin,Weiwei Xie		
157805	JAC7410840	not SC. Para-mag at low-T. YFexGe2, YGe1.5+x(minor phase)	YFexGe2	Y1Fe0.282Ge2	Y	1	Fe	0.282	Ge	2																		1	2018			emu.K/mol	0.003	my-B/f.u	0.15	-22																						Cmmm	63	A	4.0974	15.839	3.9774												K					0																																																																																																Y(3N),Ge(6N),T(2N8-3N8)		arc-melting. (Y:T:Ge = 1:x:2(with 3% excess Ge)					Electron counts, structural stability, and magnetism in BaCuSn2-CeNi1- xSi2-type YTxGe2 (T =  Cr, Mn, Fe, Co, and Ni)			Department of Chemistry, Louisiana State University, Baton Rouge, LA 70803, USA	J.Alloys Compd., 741(2018)840	Lea Gustin,Lingyi Xing,Max T. Pan,Rongying Jin,Weiwei Xie		
157806	JAC7410840	not SC. Para-mag at low-T. YCoxGe2, YGe1.5+x(minor phase)	YCoxGe2	Y1Co0.493Ge2	Y	1	Co	0.493	Ge	2																		1	2018			emu.K/mol	0.00081	my-B/f.u	0.08	-0.25																						Cmmm	63	A	4.103	16.034	4.006												K					0																																																																																																Y(3N),Ge(6N),T(2N8-3N8)		arc-melting. (Y:T:Ge = 1:x:2(with 3% excess Ge)					Electron counts, structural stability, and magnetism in BaCuSn2-CeNi1- xSi2-type YTxGe2 (T =  Cr, Mn, Fe, Co, and Ni)			Department of Chemistry, Louisiana State University, Baton Rouge, LA 70803, USA	J.Alloys Compd., 741(2018)840	Lea Gustin,Lingyi Xing,Max T. Pan,Rongying Jin,Weiwei Xie		
157807	JPS087023704	Bi-S(1) interplane distance = 3.2996, Bi-S(1) in plane distance = 2.8760, Bi-S(2) distance = 2.5242 A. Tc(bulk)  depends on R-ion radius.	La(O0.5F0.5)BiS2	La1Bi1S2F0.5O0.5	La	1	Bi	1	S	2	F	0.5													O	0.5		1	2018																										ABCD2		CeOBiS2	P4/nmm		A	4.0674		13.431												K				2.2			2.2																																																																																																solid state reaction. mixture - pellet - ANN(700C,20h, in quartz tube)					Evolution of Anisotropic Displacement Parameters and Superconductivity with Chemical Pressure in BiS2-Based REO0.5F0.5BiS2 (RE = La, Ce, Pr, and Nd)			Graduate School of Science and Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn. 87(2018)023704	Yoshikazu Mizuguchi,Kazuhisa Hoshi,Yosuke Goto,Akira Miura,Kiyoharu Tadanaga,Chikako Moriyoshi,Yoshihiro Kuroiw		
157808	JPS087023704	Bi-S(1) interplane distance = 3.3201, Bi-S(1) in plane distance = 2.8540, Bi-S(2) distance = 2.5186 A. Tc(bulk)  depends on R-ion radius.	Ce(O0.5F0.5)BiS2	Ce1Bi1S2F0.5O0.5	Ce	1	Bi	1	S	2	F	0.5													O	0.5		1	2018																										ABCD2		CeOBiS2	P4/nmm		A	4.0331		13.4802												K						2																																																																																																	solid state reaction. mixture - pellet - ANN(700C,20h, in quartz tube)					Evolution of Anisotropic Displacement Parameters and Superconductivity with Chemical Pressure in BiS2-Based REO0.5F0.5BiS2 (RE = La, Ce, Pr, and Nd)			Graduate School of Science and Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn. 87(2018)023704	Yoshikazu Mizuguchi,Kazuhisa Hoshi,Yosuke Goto,Akira Miura,Kiyoharu Tadanaga,Chikako Moriyoshi,Yoshihiro Kuroiw		
157809	JPS087023704	Bi-S(1) interplane distance = 3.3067, Bi-S(1) in plane distance = 2.8426, Bi-S(2) distance = 2.5457 A. Tc(bulk)  depends on R-ion radius.	Pr(O0.5F0.5)BiS2	Pr1Bi1S2F0.5O0.5	Pr	1	Bi	1	S	2	F	0.5													O	0.5		1	2018																										ABCD2		CeOBiS2	P4/nmm		A	4.0164		13.4006												K				3.4			3.4	MTC157809																																																																																															solid state reaction. mixture - pellet - ANN(700C,20h, in quartz tube)					Evolution of Anisotropic Displacement Parameters and Superconductivity with Chemical Pressure in BiS2-Based REO0.5F0.5BiS2 (RE = La, Ce, Pr, and Nd)			Graduate School of Science and Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn. 87(2018)023704	Yoshikazu Mizuguchi,Kazuhisa Hoshi,Yosuke Goto,Akira Miura,Kiyoharu Tadanaga,Chikako Moriyoshi,Yoshihiro Kuroiw		
157810	JPS087023704	Bi-S(1) interplane distance = 3.3538, Bi-S(1) in plane distance = 2.8272, Bi-S(2) distance = 2.5632 A. Tc(bulk)  depends on R-ion radius.	Nd(O0.5F0.5)BiS2	Nd1Bi1S2F0.5O0.5	Nd	1	Bi	1	S	2	F	0.5													O	0.5		1	2018																										ABCD2		CeOBiS2	P4/nmm		A	3.997		13.4119												K				4.8			4.8																																																																																																solid state reaction. mixture - pellet - ANN(700C,20h, in quartz tube)					Evolution of Anisotropic Displacement Parameters and Superconductivity with Chemical Pressure in BiS2-Based REO0.5F0.5BiS2 (RE = La, Ce, Pr, and Nd)			Graduate School of Science and Engineering, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn. 87(2018)023704	Yoshikazu Mizuguchi,Kazuhisa Hoshi,Yosuke Goto,Akira Miura,Kiyoharu Tadanaga,Chikako Moriyoshi,Yoshihiro Kuroiw		
157811	PRB095214515		La0.9Sr0.1FeAsO	La0.9Sr0.1Fe1As1O1	La	0.9	Sr	0.1	Fe	1	As	1													O	1		1	2017								142																		ABCD		oxypnictide	P4/nmm		A	4.0498		8.7909											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157812	PRB095214515		La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.2O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.2											O	1		1	2017								40																		ABCD		oxypnictide	P4/nmm		A	4.0382		8.7247											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157813	PRB095214515		La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.3O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.3											O	1		1	2017								30																		ABCD		oxypnictide	P4/nmm		A	4.0285		8.6971											Fe-1111	K			6.72				6.72																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157814	PRB095214515	AFM2 observed only by NMR.	La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.4O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.4											O	1		1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0279		8.666											Fe-1111	K	11.14						11.14	MTC157814																																																																																													LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157815	PRB095214515	AFM2 observed only by NMR.	La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.5O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.5											O	1		1	2017								20.4																		ABCD		oxypnictide	P4/nmm		A	4.0172		8.6451											Fe-1111	K			6.38				6.38																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157816	PRB095214515	AFM2 observed only by NMR.	La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.6O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.6											O	1		1	2017								22.9																		ABCD		oxypnictide	P4/nmm		A	4.0098		8.6284											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157817	PRB095214515	AFM2 observed only by NMR.	La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.7O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.7											O	1		1	2017								22.3																		ABCD		oxypnictide	P4/nmm		A	3.992		8.5764											Fe-1111	K			5.04				5.04																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157818	PRB095214515		La0.9Sr0.1FeAs1-xPxO	La0.9Sr0.1Fe1As0.8P0.8O1	La	0.9	Sr	0.1	Fe	1	As	0.8	P	0.8											O	1		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9819		8.574											Fe-1111	K	11.76		16				13.88	MTC157814																																																																																													LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157819	PRB095214515		La0.9Sr0.1FePO	La0.9Sr0.1Fe1P1O1	La	0.9	Sr	0.1	Fe	1	P	1													O	1		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.963		8.5098											Fe-1111	K	5.6		6.79				6.195																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157820	PRB095214515	R-exponent n=1.99, pnivctogen hight =1.324 A, bond-angle = 113.5 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As1F0.14O0.86	La	1	Fe	1	As	1	F	0.14													O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0262		8.7155											Fe-1111	K	11.9						11.9																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157821	PRB095214515	R-exponent n=1.82, pnivctogen hight =1.305 A, bond-angle = 114.2 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.8P0.2F0.14O0.86	La	1	Fe	1	As	0.8	P	0.2	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0233		8.6795											Fe-1111	K	11.1						11.1																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157822	PRB095214515	R-exponent n=1.48, pnivctogen hight =1.294 A, bond-angle = 114.4 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.7P0.3F0.14O0.86	La	1	Fe	1	As	0.7	P	0.3	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0172		8.6478											Fe-1111	K	12.9						12.9																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157823	PRB095214515	R(T) = R0 + A*T^n where A = 4.8 uOhm.cm/K^n, n=1.12.  pnivctogen hight =1.278 A, bond-angle = 115.2 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.6P0.4F0.14O0.86	La	1	Fe	1	As	0.6	P	0.4	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0066		8.6222											Fe-1111	K	26.1						26.1	MTC157823																																																																						mOhm.cm							0.16																LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157824	PRB095214515	R(T) = R0 + A*T^n where A = 2.8 uOhm.cm/K^n, n=1.14. pnivctogen hight =1.249 A, bond-angle = 116.0 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.5P0.5F0.14O0.86	La	1	Fe	1	As	0.5	P	0.5	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9984		8.606											Fe-1111	K	26.1						26.1																																																																							mOhm.cm							0.1																LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157825	PRB095214515	R-exponent n=1.51, pnivctogen hight =1.225 A, bond-angle = 116.8 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.4P0.6F0.14O0.86	La	1	Fe	1	As	0.4	P	0.6	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.986		8.5796											Fe-1111	K	21.1						21.1																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157826	PRB095214515	R-exponent n=2.04, pnivctogen hight =1.205 A, bond-angle = 117.6 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1As0.2P0.8F0.14O0.86	La	1	Fe	1	As	0.2	P	0.8	F	0.14											O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9624		8.5505											Fe-1111	K	10.1						10.1																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157827	PRB095214515	R-exponent n=2.07, pnivctogen hight =1.190 A, bond-angle = 118.0 degree	LaFeAs1-xPxO0.86F0.14	La1Fe1P1F0.14O0.86	La	1	Fe	1	P	1	F	0.14													O	0.86		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9451		8.4849											Fe-1111	K	2.98						2.98																																																																																														LaAs,LaP,Fe2O3,Fe,SrAs		solid state reaction. mixture - pellet - ANN(1130C,40h, in evacuated silica tube)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157828	PRB095214515	R-exponent n=1.90, pnivctogen hight =1.326 A, bond-angle = 113.0 degree	LaFeAsO0.75H0.25	La1Fe1As1H0.25O0.75	La	1	Fe	1	As	1	H	0.25													O	0.75		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9949		8.6676											Fe-1111	K	15.4						15.4																																																																																														LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157829	PRB095214515	R-exponent n=2.13, pnivctogen hight =1.316 A, bond-angle = 113.4 degree	LaFeAs1-xPxO0.75H0.25	La1Fe1As0.9P0.1H0.25O0.75	La	1	Fe	1	As	0.9	P	0.1	H	0.25											O	0.75		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9868		8.6392											Fe-1111	K	7.6						7.6																																																																																														LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157830	PRB095214515	R-exponent n=2.15, pnivctogen hight =1.271 A, bond-angle = 115.2 degree	LaFeAs1-xPxO0.75H0.25	La1Fe1As0.8P0.2H0.25O0.75	La	1	Fe	1	As	0.8	P	0.2	H	0.25											O	0.75		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.984		8.6154											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157831	PRB095214515	R-exponent n=2.12, pnivctogen hight =1.259 A, bond-angle = 115.3 degree	LaFeAs1-xPxO0.75H0.25	La1Fe1As0.6P0.4H0.25O0.75	La	1	Fe	1	As	0.6	P	0.4	H	0.25											O	0.75		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9719		8.5689											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157832	PRB095214515	R-exponent n=2.24, pnivctogen hight =1.193 A, bond-angle = 117.6 degree	LaFePO0.75H0.25	La1Fe1P1H0.25O0.75	La	1	Fe	1	P	1	H	0.25													O	0.75		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9212		8.4886											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157833	PRB095214515	R(T) = R0 + A*T^n where A = 2.14 uOhm.cm/K^n, n=1.08.  pnivctogen hight =1.359 A, bond-angle = 111.8 degree	LaFeAsO0.7H0.3	La1Fe1As1H0.3O0.3	La	1	Fe	1	As	1	H	0.3													O	0.3		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9812		8.6782											Fe-1111	K	35						35																																																																							mOhm.cm							0.05																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157834	PRB095214515		LaFeAs1-xPxO0.7H0.3	La1Fe1As0.9P0.1H0.3O0.3	La	1	Fe	1	As	0.9	P	0.1	H	0.3											O	0.3		1	2017																										ABCD		oxypnictide	P4/nmm		A														Fe-1111	K	20						20																																																																																														LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157835	PRB095214515	not SC. R-exponent n=1.51, pnivctogen hight =1.304 A, bond-angle = 112.7 degree	LaFeAs1-xPxO0.7H0.3	La1Fe1As0.8P0.2H0.3O0.3	La	1	Fe	1	As	0.8	P	0.2	H	0.3											O	0.3		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9803		8.6232											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157836	PRB095214515	not SC.  R-exponent n=2.70, pnivctogen hight =1.259 A, bond-angle = 114.9 degree	LaFeAs1-xPxO0.7H0.3	La1Fe1As0.6P0.4H0.3O0.3	La	1	Fe	1	As	0.6	P	0.4	H	0.3											O	0.3		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9648		8.5677											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157837	PRB095214515	not SC.  R-exponent n=2.71, pnivctogen hight =1.196 A, bond-angle = 117.1 degree	LaFePO0.7H0.3	La1Fe1P1H0.3O0.3	La	1	Fe	1	P	1	H	0.3													O	0.3		1	2017																										ABCD		oxypnictide	P4/nmm		A	3.9061		8.4741											Fe-1111	K					0																																																																																																LaAs,LaP,Fe2O3,Fe,LaH2		High-P synthesis. mixture - press into BN capsule - heat(1100C,2h, P=4 GPa)					Three superconducting phases with different categories of pairing in holeand electron-doped LaFeAs1-xPxO			Department of Physics, Osaka University, Osaka 560-0043, Japan	Phys.Rev.B, 95(2017)214515	S. Miyasaka,M. Uekubo,H. Tsuji,M. Nakajima,S. Tajima,T. Shiota,H. Mukuda,H. Sagayama,H. Nakao,R. Kumai,Y. Murakami		
157838	ACS1373622	not SC for 0.2 < x < 0.4 in Li1-xSn2+xAs2. R(T), thermal conductivity measured.	Li0.65Sn2.35As2	Li0.65Sn2.35As2	Li	0.65	Sn	2.35	As	2																		1	2015																										AB2C2			R3[-]m	166																K					0																																																																																																Sn(2N7),As(6N),Li(2N)		solid state reaction. mixture(with excess Li) - sealed in silica ampule - heat(973K,10h)  - ANN(973K,2h) - cool to 423 K over 30h					Intricate Short-Range Ordering and Strongly Anisotropic Transport Properties of Li1-xSn2+xAs2			Department of Chemistry and Department of Chemical Engineering and Materials Science, University of California Davis, Davis, California 95616, United States	J.Am.Chem.Soc., 137(2015)3622	Kathleen Lee,Derrick Kaseman,Sabyasachi Sen,Ivan Hung,Zhehong Gan,Birgit Gerke,Rainer Pottgen,Mikhail Feygenson,Jorg Neuefeind,Oleg I. Lebedev,Kirill Kovnir		
157839	ACS1382170	No anomaly in R(T).	ThFeAsN	Th1Fe1As1	Th	1	Fe	1	As	1																		1	2016																										ABCD		oxypnictide	P4/nmm		A	4.0367		8.5262											Fe-1111, volume = 138.937 A3	K	28		30				29										100																																																																																				Th3N4,Th,FeAs		mixture(Th3N4,Th,FeAs) - heat(1000C,20h) - pellet - SIN(1150C,50h)					A New ZrCuSiAs-Type Superconductor: ThFeAsN			Department of Physics, Shandong University of Technology, Zibo 255049, China	J.Am.Chem.Soc., 137(2016)2170	Cao Wang,Zhi-Cheng Wang,Yu-Xue Mei,Yu-Ke Li,Lin Li,Zhang-Tu Tang,Yi Liu,Pan Zhang,Hui-Fei Zhai,Zhu-An Xu,Guang-Han Cao		
157840	ANG0540293	(Li1-xFex)OH(Fe1-yLiy)Se, x=0.205,y=0.085 by XRD.  Coexist (SC,F) below Tm (=10 K). FM-layer (Li1-Fex)OH and SC-layer (Fe1-yLiy)Se. Mossbauer measured.	(Li,Fe)OH(Fe,Li)Se	Li0.88Fe1.12Se1H1O1	Li	0.88	Fe	1.12	Se	1	H	1													O	1		1	2015																																														K			43	40			40																																																																																																polycrystalline synthesized under hydrothermal conditions					Coexistence of 3d-Ferromagnetism and Superconductivity in [(Li1-xFex)OH](Fe1-yLiy)Se			Department Chemie, Ludwig-Maximilians-Universitat Munchen Butenandtstrasse 5?13, Munchen, Germany	Angew.Chem.Int.Ed., 54(2015)293	Ursula Pachmayr,Fabian Nitsche,Hubertus Luetkens,Sirko Kamusella,Felix Bruckner,Rajib Sarkar,Hans-Henning Klauss,Dirk Johrendt		
157841	APL106112601	composition: La,Bi:S:Se:O:F = 1:0.95:0.92:0.9:0.32:0.19 by XRD. Anisotropy = (Hc2//ab/Hc2//c)  = 34	La(O,F)BiSSe	La1Bi1S1Se1F0.5O0.5	La	1	Bi	1	S	1	Se	1	F	0.5											O	0.5		3	2015																										ABCD2			P4/nmm		A	4.1102		13.601											bond length, angle shown in table	K			3.8	4.1			4.1																				T	RES(on), wHH		24.3	0.7										MHC157841																																																														single crystals were prepared by an alkali metal chloride flux method					Site selectivity on chalcogen atoms in superconducting La(O,F)BiSSe			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Appl.Phys.Lett., 106(2015)112601	Masashi Tanaka,Takuma Yamaki,Yoshitaka Matsushita,Masaya Fujioka,Saleem J. Denholme,Takahide Yamaguchi,Hiroyuki Takeya,Yoshihiko Takano		
157842	EPL11757005	R(T)-exponnt n=1.30 for 40 < T < 150. structure, h(Th-As) =1.7858, h(Fe-As) = 1.2964, d(Th-As) = 2.3700, d(Fe-As) = 2.4010	ThFeAsN	Th1Fe1As1N1	Th	1	Fe	1	As	1	N	1																1	2017																										ABCD		oxypnictide	P4/nmm		A	4.0414		8.5152											ZrCuSiAs-type. alpha(Fe-As-Fe) = 114.65, beta(Fe-As-Fe) = 106.95	K	30						30																																																																																					m3/C						MRH157842					Solid state reaction					Neutron powder diffraction study on the iron-based nitride superconductor ThFeAsN			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of SciencesBeijing 100190, China	Europhys.Lett., 117(2017)57005	Huican Mao,Cao Wang,Helen E. Maynard-Casely,Qingzhen Huang,Zhicheng Wang,Guanghan Cao,Shiliang Li1,Huiqian Luo		
157843	HPST0070589		Li-RbCaNb3O10	Li0.1Rb1Ca2Nb3O10	Li	0.1	Rb	1	Ca	2	Nb	3													O	10		1	1998																																													Li-intercalation	K				5			5	MTC157843																																																																																													K2CO3,Rb2CO3,CaCO3,Nb2O3		solid state reaction. mixture - SIN(1150C, in air)					High pressure studies of the non-copper superconductors KCa2Nb3O10 and RbCa2Nb3O10			Institute for Solid State Physics, Univ. of Tokyo, Roppongi, Minato-ku 106, Japan	Rev.High Pressure Sci.Technol., 7(1998)589	Yoshihiko Takano,Yoshihide Kimishima,Tokio Yamadaya,Nobuo Mori		
157844	HPST0070589	Li-intercalated RbCa2Nb3O10. Intercalation using n-butyllithium hexane solution. Li-intercalation content not measured.	Li-KCa2Nb3O10	Li0.1K1Ca2Nb3O10	Li	0.1	K	1	Ca	2	Nb	3													O	10		1	1998																																													Li-intercalation	K				5			5																																																																																														K2CO3,Rb2CO3,CaCO3,Nb2O3		solid state reaction. mixture - SIN(1150C, in air)					High pressure studies of the non-copper superconductors KCa2Nb3O10 and RbCa2Nb3O10			Institute for Solid State Physics, Univ. of Tokyo, Roppongi, Minato-ku 106, Japan	Rev.High Pressure Sci.Technol., 7(1998)589	Yoshihiko Takano,Yoshihide Kimishima,Tokio Yamadaya,Nobuo Mori		
157845	JAC7430547	Bond distance: d(Bi-S1) = 2.552 , d(Bi-S2) = 2.888, where S1(in plane S), S2(out-of plane S), angle (S1-Bi-S1) = 173 deg. Eu-valence = .2.23	Eu3Bi2S4F4	Eu3Bi2S4F4	Eu	3	Bi	2	S	4	F	4																1	2018																										A2B3C4D4					A	4.077														K			1.5				1.5																																																																																														Ba,Ti,Fe,Cr,As,TiO2,CrO3		solid state reaction. mixture - sealed in quartz tube - heat(900C,1d) - cool to RT - reground - pellet - SIN(1050C,3d) -cool to RT - ANN(500C,2d)					Role of local structure distortion in the suppression of superconductivity for Eu3-xSrxBi2S4F4 system			College of Science, New Energy Technology Engineering Laboratory of Jiangsu Province, Nanjing University of Posts and Telecommunications, Nanjing, Jiangsu, 210023, China	J.Alloys Compd., 743(2018)547	Jie Cheng,Pan Zhang,Peng Dong,Xiangfu Wang,Yu Wang,Xing'ao Li,Shengli Liu,Yuke Li,Zhu'an Xu		
157846	JAC7430547	Bond distance: d(Bi-S1) = 2.583, d(Bi-S2) = 2.886 , where S1(in plane S), S2(out-of plane S), angle (S1-Bi-S1) = 172 deg. Eu-valence = .2.49	(Eu,Sr)3Bi2S4F4	Eu2.5Sr0.5Bi2S4F4	Eu	2.5	Sr	0.5	Bi	2	S	4	F	4														1	2018																										A2B3C4D4					A	4.0725														K			0.87				0.87																																																																																														Ba,Ti,Fe,Cr,As,TiO2,CrO3		solid state reaction. mixture - sealed in quartz tube - heat(900C,1d) - cool to RT - reground - pellet - SIN(1050C,3d) -cool to RT - ANN(500C,2d)					Role of local structure distortion in the suppression of superconductivity for Eu3-xSrxBi2S4F4 system			College of Science, New Energy Technology Engineering Laboratory of Jiangsu Province, Nanjing University of Posts and Telecommunications, Nanjing, Jiangsu, 210023, China	J.Alloys Compd., 743(2018)547	Jie Cheng,Pan Zhang,Peng Dong,Xiangfu Wang,Yu Wang,Xing'ao Li,Shengli Liu,Yuke Li,Zhu'an Xu		
157847	JAC7430547	Bond distance: d(Bi-S1) = 2.606 , d(Bi-S2) = 2.885 , where S1(in plane S), S2(out-of plane S), angle (S1-Bi-S1) = 170 deg. Eu-valence = 2.70.  Tc from SST030015005.	(Eu,Sr)3Bi2S4F4	Eu2Sr1Bi2S4F4	Eu	2	Sr	1	Bi	2	S	4	F	4														1	2018																										A2B3C4D4					A	4.071														K			0.48				0.48																																																																																														Ba,Ti,Fe,Cr,As,TiO2,CrO3		solid state reaction. mixture - sealed in quartz tube - heat(900C,1d) - cool to RT - reground - pellet - SIN(1050C,3d) -cool to RT - ANN(500C,2d)					Role of local structure distortion in the suppression of superconductivity for Eu3-xSrxBi2S4F4 system			College of Science, New Energy Technology Engineering Laboratory of Jiangsu Province, Nanjing University of Posts and Telecommunications, Nanjing, Jiangsu, 210023, China	J.Alloys Compd., 743(2018)547	Jie Cheng,Pan Zhang,Peng Dong,Xiangfu Wang,Yu Wang,Xing'ao Li,Shengli Liu,Yuke Li,Zhu'an Xu		
157848	JAC7430547	Bond distance: d(Bi-S1) = 2.634, d(Bi-S2) = 2.882 , where S1(in plane S), S2(out-of plane S), angle (S1-Bi-S1) = 168 deg. Eu-valence = 2.89. Tc from SST030015005.	(Eu,Sr)3Bi2S4F4	Eu1Sr2Bi2S4F4	Eu	1	Sr	2	Bi	2	S	4	F	4														1	2018																										A2B3C4D4					A	4.065														K					0.3																																																																																																Ba,Ti,Fe,Cr,As,TiO2,CrO3		solid state reaction. mixture - sealed in quartz tube - heat(900C,1d) - cool to RT - reground - pellet - SIN(1050C,3d) -cool to RT - ANN(500C,2d)					Role of local structure distortion in the suppression of superconductivity for Eu3-xSrxBi2S4F4 system			College of Science, New Energy Technology Engineering Laboratory of Jiangsu Province, Nanjing University of Posts and Telecommunications, Nanjing, Jiangsu, 210023, China	J.Alloys Compd., 743(2018)547	Jie Cheng,Pan Zhang,Peng Dong,Xiangfu Wang,Yu Wang,Xing'ao Li,Shengli Liu,Yuke Li,Zhu'an Xu		
157849	JAC7450460	h(As) =  1.3450A. Angle(As-Fe-As) = 112.139 deg.	Ba2Ti2Fe2As4O	Ba2Ti2Fe2As4O1	Ba	2	Ti	2	Fe	2	As	4													O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0296		27.3448											22241-phase	K				21			21																																																																							mOhm.cm							0.564																							Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157850	JAC7450460	h(As) =  1.3451 A. Angle(As-Fe-As) = 112.137 deg.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.98Cr0.02As4O1	Ba	2	Ti	2	Fe	1.98	Cr	0.02	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0297		27.3489											Cr-doped 22241-phase	K				19.1			19.1	MTC157850																																																																						mOhm.cm							0.747																							Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157851	JAC7450460	h(As) = 1.3453 A . Angle(As-Fe-As) = 112.131 deg.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.96Cr0.04As4O1	Ba	2	Ti	2	Fe	1.96	Cr	0.04	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0296		27.3585											Cr-doped 22241-phase	K				15.7			15.7																																																																							mOhm.cm							0.896																							Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157852	JAC7450460	h(As) = 1.3453 A . Angle(As-Fe-As) = 112.131 deg.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.94Cr0.06As4O1	Ba	2	Ti	2	Fe	1.94	Cr	0.06	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0299		27.359											Cr-doped 22241-phase	K				11.8			11.8																																																																							mOhm.cm							1.029																							Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157853	JAC7450460	h(As) = 1.3453 A . Angle(As-Fe-As) = 112.13 deg. R(T) not to zero at 1.8 K.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.92Cr0.08As4O1	Ba	2	Ti	2	Fe	1.92	Cr	0.08	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0301		27.361											Cr-doped 22241-phase	K				8.16			8.16																																																																							mOhm.cm							1.098																							Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157854	JAC7450460	h(As) = 1.3454 A . Angle(As-Fe-As) = 112.127 deg. R(T) not to zero at 1.8 K.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.9Cr0.1As4O1	Ba	2	Ti	2	Fe	1.9	Cr	0.1	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0302		27.3649											Cr-doped 22241-phase	K																																																																																																												Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157855	JAC7450460	h(As) = 1.3458 A . Angle(As-Fe-As) = 112.116 deg. R(T) not to zero at 1.8 K.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.88Cr0.12As4O1	Ba	2	Ti	2	Fe	1.88	Cr	0.12	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0305		27.3821											Cr-doped 22241-phase	K																																																																																																												Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157856	JAC7450460	h(As) = 1.3458 A . Angle(As-Fe-As) = 112.115 deg.  R(T) not to zero at 1.8 K.	Ba2Ti2(Fe,Cr)2As4O	Ba2Ti2Fe1.84Cr0.16As4O1	Ba	2	Ti	2	Fe	1.84	Cr	0.16	As	4											O	1		1	2018																										AB2C2D2E4			P4/mmm		A	4.0306		27.3839											Cr-doped 22241-phase	K																																																																																																												Cr doping effects on structure and superconductivity of Ba2Ti2Fe2As4O			Key Laboratory of Levitation Technology and Maglev (Ministry of Education of China), Superconductivity R&D Center (SRDC), Mail Stop 165#, Southwest Jiaotong University, Chengdu, Sichuan 610031, China	J.Alloys Compd., 745(2018)460	C.C. Hsieh,C. Ke,D.J. Zhou,C.H. Cheng,H. Zhang,Y. Zhao		
157857	JPCM027395701	RRR = 100 . Tc(SP) = 3.46 K. SP (beta) = 1.65 mJ/mol.K4, (delta) = 0.135  mJ/mol.K6.	TlNi2Se2	Tl1Ni2Se2	Tl	1	Ni	2	Se	2																		3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.87		13.438												K			3.6	3.69			3.69																																																								mJ/mol.K2	40	SP																																						self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157858	JPCM027395701	RRR = 9.3 . Tc(SP) = 2.96  K. SP (beta) = 1.32  mJ/mol.K4, (delta) = 0.104  mJ/mol.K6.	TlNi2(Se,S)2	Tl1Ni2Se1.8S0.2	Tl	1	Ni	2	Se	1.8	S	0.2																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8571		13.332												K			2.85	2.83			2.83																																																					MSP157858			mJ/mol.K2	35.68	SP																																						self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157859	JPCM027395701	RRR = 6.3	TlNi2(Se,S)2	Tl1Ni2Se1.6S0.4	Tl	1	Ni	2	Se	1.6	S	0.4																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8518		13.2698												K			2.59	2.65			2.65																																																																																																self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157860	JPCM027395701	RRR = 5.6	TlNi2(Se,S)2	Tl1Ni2Se1.4S0.6	Tl	1	Ni	2	Se	1.4	S	0.6																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8432		13.193												K			2.03	2.2			2.2	MTC157860																																																																																															self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157861	JPCM027395701	RRR = 4.9 . Tc(SP) = 2.05 K. SP (beta) = 0.744 mJ/mol.K4, (delta) = 0.093  mJ/mol.K6.	TlNi2(Se,S)2	Tl1Ni2Se1.2S0.8	Tl	1	Ni	2	Se	1.2	S	0.8																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8397		13.146												K			2.06	2.16			2.16																																																					MSP157861			mJ/mol.K2	31.13	SP																																						self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157862	JPCM027395701	RRR = 4.1	TlNi2(Se,S)2	Tl1Ni2Se1S1	Tl	1	Ni	2	Se	1	S	1																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.832		13.0758												K			1.93	1.96			1.96																																																																																																self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157863	JPCM027395701	RRR = 4.7 . Tc(SP) = 2.02 K. SP (beta) = 0.511 mJ/mol.K4, (delta) =  0.090 mJ/mol.K6.	TlNi2(Se,S)2	Tl1Ni2Se0.8S1.2	Tl	1	Ni	2	Se	0.8	S	1.2																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8245		13.0305												K			1.99	2.03			2.03																																																					MSP157863			mJ/mol.K2	29.66	SP																																						self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157864	JPCM027395701	RRR = 4.9	TlNi2(Se,S)2	Tl1Ni2Se0.6S1.4	Tl	1	Ni	2	Se	0.6	S	1.4																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.815		12.9547												K			1.89	1.98			1.98																																																																																																self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157865	JPCM027395701	RRR = 4.7	TlNi2(Se,S)2	Tl1Ni2Se0.4S1.6	Tl	1	Ni	2	Se	0.4	S	1.6																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.8052		12.8907												K			1.94	1.99			1.99	MTC157860																																																																																															self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157867	JPCM027395701	RRR = 6.9	TlNi2(Se,S)2	Tl1Ni2Se0.2S1.8	Tl	1	Ni	2	Se	0.2	S	1.8																3	2015																										AB2C2		ThCr2Si2	I4/mmm		A	3.7982		12.8296												K			2.11	2.09			2.09																																																																																																self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157868	JPCM027395701	RRR = 8.3 . Tc(SP) = 2.15 K. SP (beta) = 1.14 mJ/mol.K4, (delta) = 0.094  mJ/mol.K6. (dC/gamma*Tc) = 1.55. Curie-Weiss for T < 100 K. Two gaps (large in DB, small = 0.95 kTc) from SP.	TlNi2S2	Tl1Ni2S2	Tl	1	Ni	2	S	2																		3	2015	emu/mol	0.00053																								AB2C2		ThCr2Si2	I4/mmm		A	3.7919		12.7809												K			2.25	2.3			2.3																				T	RES. GL-fitting	0.53												MHC157868		nm	from Hc2	24.9															MSP157868			mJ/mol.K2	30.57	SP	197	SP											uOh.cm												68	92												self-flux method. mixture(Tl:NiSe:NiS = 1:2-x:x) - placed in alumina crucible - sealed in quartz tube - heat(950C,12h) - cool to 650C(6 C/h) - FC to RT					Superconductivity and disorder effect in TlNi2Se2-xSx compounds			Hangzhou Key Laboratory of Quantum Matter, Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	J.Phys.Condens.Matter, 27(2015)395701	Hangdong Wang,Qianhui Mao,Huimin Chen,Qiping Su,Chiheng Dong,Rajwali Khan,Jinhu Yang,Bin Chen,Minghu Fang		
157869	JPCM028085701	RRR = 72.5. type-I SC. kappa(GL) = 0.611. Tc(SP) = 3.573 K. SP (beta) = 3.1 mJ/mol.K4. (dC<el>/gamma*Tc) = 6.06. e-ph = 0.774.	KBi2	Bi2K1	Bi	2	K	1																				3	2016																										AB2		MgCu2(Laves)			A	9.5233														K			3.549	3.517			3.517										100										Oe	type-I SC	234.3												MHC157869		nm	GL	133.7			nm	See text, GL	81.7										MSP157869			mJ/mol.K2	1.3	SP	123.4	SP																																				Flux method.  (K:Bi = 1:9) - mixed - alumina crucible covered with quartz wool - sealed in quartz tube - heat(580C, 12 h) - slow cool to 280C					Type-I superconductivity in KBi2 single crystals			Department of Physics, Renmin University of China, Beijing 100872, People's Republic of China	J.Phys.Condens.Matter, 28(2016)085701	Shanshan Sun,Kai Liu,Hechang Lei		
157870	JPS081083702	RRR = 150. Ferroquadrupole order T<Q> = 2.0 K. R=R0 + A*T^2exp(-d/T),  A=5.6 uOhm.cm/K2, d=2.1 K. cohere(0)= 280 nm penet = 330 nm from gamma(SP). GL = 1.2	PrTi2Al20	Pr1Ti2Al20	Pr	1	Ti	2	Al	20																		3	2012																										AB2C20		CeCr2Al20	Fd3[-]m																	K			0.2				0.2										60										Oe	SUS, WHH	63							mT/K	WHH fitting	47			MHC157870		nm	from Hc2	230			nm	from gamma(SP)	280													mJ/mol.K2	100														uOh.cm							0.38																Pr(4N),La(3N),Ti(3N),Al(5N)		Al-self flux method					Superconductivity in the Ferroquadrupolar State in the Quadrupolar Kondo Lattice PrTi2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)083702	Akito SAKAI,Kentaro KUGA,Satoru NAKATSUJI		
157871	JPS081083702	RRR = 60. Ferroquadrupole order T<Q> = 2.0 K. R=R0 + A*T^2exp(-d/T),  A = 5.1 uOhm.cm/K2, d = 2.0 K.	PrTi2Al20	Pr1Ti2Al20	Pr	1	Ti	2	Al	20																		3	2012																										AB2C20		CeCr2Al20	Fd3[-]m																	K			0.14				0.14																																																																							uOh.cm							0.93																Pr(4N),La(3N),Ti(3N),Al(5N)		Al-self flux method					Superconductivity in the Ferroquadrupolar State in the Quadrupolar Kondo Lattice PrTi2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)083702	Akito SAKAI,Kentaro KUGA,Satoru NAKATSUJI		
157872	JPS081083702	not SC down to 0.03 K.	LaTi2Al20	La1Ti2Al20	La	1	Ti	2	Al	20																		3	2012																										AB2C20		CeCr2Al20	Fd3[-]m																	K					0.03																																																										mJ/mol.K2	23																																					Pr(4N),La(3N),Ti(3N),Al(5N)		Al-self flux method					Superconductivity in the Ferroquadrupolar State in the Quadrupolar Kondo Lattice PrTi2Al20			Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc.Jpn, 81(2012)083702	Akito SAKAI,Kentaro KUGA,Satoru NAKATSUJI		
157873	JPS0673601	not SC	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		1	1998							-128	1.8																		ABC3		BaNiSn3			A	4.269		9.738												K					0.5																																																										mJ/mol.K2	120																																							arc-melting  - ANN(900 - 950 C,10d)					Contrasting Kondo-Lattice Behavior in CeTSi3 and CeTGe3 (T = Rh and Ir)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.Jpn, 67(1998)3601	Yuji Muro,Duhwa Eom,Naoya Takeda,Masayasu Ishikawa		
157874	JPS0673601	not SC	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		1	1998							-142	5																		ABC3		BaNiSn3			A	4.252		9.715												K					0.5																																																										mJ/mol.K2	125																																							arc-melting  - ANN(900 - 950 C,10d)					Contrasting Kondo-Lattice Behavior in CeTSi3 and CeTGe3 (T = Rh and Ir)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.Jpn, 67(1998)3601	Yuji Muro,Duhwa Eom,Naoya Takeda,Masayasu Ishikawa		
157875	JPS0673601	not SC. Curie-Weiss for T > 100 K.	CeRhGe3	Ce1Rh1Ge3	Ce	1	Rh	1	Ge	3																		1	1998					My-B/mol	2.53	-28	14.6																		ABC3		BaNiSn3			A	4.402		9.993												K					0.5																																																										mJ/mol.K2	40																																							arc-melting  - ANN(900 - 950 C,10d)					Contrasting Kondo-Lattice Behavior in CeTSi3 and CeTGe3 (T = Rh and Ir)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.Jpn, 67(1998)3601	Yuji Muro,Duhwa Eom,Naoya Takeda,Masayasu Ishikawa		
157876	JPS0673601	not SC. Curie-Weiss for T > 100 K.	CeIrGe3	Ce1Ir1Ge3	Ce	1	Ir	1	Ge	3																		1	1998					My-B/mol	2.39	-21	8.7																		ABC3		BaNiSn3			A	4.409		10.032												K					0.5																																																										mJ/mol.K2	80																																							arc-melting  - ANN(900 - 950 C,10d)					Contrasting Kondo-Lattice Behavior in CeTSi3 and CeTGe3 (T = Rh and Ir)			Institute for Solid State Physics, University of Tokyo, Roppongi, Minato-ku, Tokyo 106-8666	J.Phys.Soc.Jpn, 67(1998)3601	Yuji Muro,Duhwa Eom,Naoya Takeda,Masayasu Ishikawa		
157877	JPS0760166	P-induced SC. Tc = 0.986, 1.12, 1.06 K for P = 2.0, 2.2, 2.8 GPa, respectively	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		1	2007																										ABC3		BaNiSn3																		K					0.5																																																																																																		arc-melt using tetra-arc furnace. Wrapped in Ta-foil - sealed in quartz tube - ANN(850-950 C, 5d)					Pressure Effect of Electronic States in Antiferromagnets CeTX3 (T: Transition metal, X: Si and Ge)			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 76(2007)Suppl.A 166	Tomoya Kawai,Miho Nakashima,Yusuke Okuda,Hiroaki Shishido,Tetsuya Shimoda,Tatsuma D. Matsuda,Yoshinori Haga,Tetsuya Takeuchi,Masato Hedo,Yoshiya Uwatoko,Rikio Settai,Yoshichika Onuki		
157878	JPS0760166	not SC for P < 8 GPa. Fig shows Tn(P).	CePtSi3	Ce1Pt1Si3	Ce	1	Pt	1	Si	3																		1	2007																										ABC3		BaNiSn3																		K					0.5			MTN157878																																																																																															arc-melt using tetra-arc furnace. Wrapped in Ta-foil - sealed in quartz tube - ANN(850-950 C, 5d)					Pressure Effect of Electronic States in Antiferromagnets CeTX3 (T: Transition metal, X: Si and Ge)			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan	J.Phys.Soc.Jpn, 76(2007)Suppl.A 166	Tomoya Kawai,Miho Nakashima,Yusuke Okuda,Hiroaki Shishido,Tetsuya Shimoda,Tatsuma D. Matsuda,Yoshinori Haga,Tetsuya Takeuchi,Masato Hedo,Yoshiya Uwatoko,Rikio Settai,Yoshichika Onuki		
157879	JPS077064716	not SC for P = 0 GPa	CeRuSi3	Ce1Ru1Si3	Ce	1	Ru	1	Si	3																		3	2008								1.8																		ABC3		BaNiSn3	I4/mm	107	A	4.21577		9.9271												K					0																																																																																																		Czochralski mehod					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
157880	JPS077064716	not SC for P = 0 GPa	CeRhGe3	Ce1Rh1Ge3	Ce	1	Rh	1	Ge	3																		3	2008								15.3																		ABC3		BaNiSn3	I4/mm	107	A	4.3976		10.0322												K					0			MPH157880																																																							mJ/mol.K2	40.1																																							Bi-flux method					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
157881	JPS077064716	not SC for P = 0 GPa	CeIrGe3	Ce1Ir1Ge3	Ce	1	Ir	1	Ge	3																		3	2008								8.75																		ABC3		BaNiSn3	I4/mm	107	A	4.401		10.024												K					0			MPH157881																																																							mJ/mol.K2	80.3																																							Bi-flux method					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
157882	JPS077064716	not SC for P = 0 GPa	CeCoSi3	Ce1Co1Si3	Ce	1	Co	1	Si	3																		3	2008																										ABC3		BaNiSn3	I4/mm	107																K					0																																																										mJ/mol.K2	36.8																																							Bi-flux method					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
157883	JPS077064716	P-induced SC. P<cr> = 6.5 GPa. SC data shows for P = 6.5 GPa.	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		3	2008								21																		ABC3		BaNiSn3	I4/mm	107																K			0.69		0		0.69	MPH157883																												T/K	RES(on)	20																									mJ/mol.K2	32.6																																							Bi-flux method					Magnetic and Superconducting Properties of CeTX3 (T: Transition Metal and X: Si and Ge) with Non-centrosymmetric Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)064716	Tomoya KAWAI,Hiroshi MURANAKA,Marie-Aude MEASSON,Tetsuya SHIMODA,Yusuke DOI,Tatsuma D. MATSUDA,Yoshinori HAGA,Georg KNEBEL,Gerard LAPERTOT,Dai AOKI,Jacques FLOUQUET,Tetsuya TAKEUCHI,Rikio SETTAI,Yoshichika Onuki		
157884	JPS077114704	P = 0 GPa. RRR = 200.	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K					0																																																																																																							The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157885	JPS077114704	P = 1.7 GPa. RRR = 200. Hc2(WHH) = 25.7 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			2.124				2.124	MPH157884																			T	RES(on). extrapolation	10.19							T/K	RES(on)	17.28			MHC157885		A	BCS, Fermi velocity	41.2																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157886	JPS077114704	P = 2.4 GPa. RRR = 200. Hc2(WHH) = 36.1 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			2.258				2.258																				T	RES(on). extrapolation	10.62							T/K	RES(on)	22.83			MHC157886		A	BCS, Fermi velocity	36.9																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157887	JPS077114704	P = 2.6 GPa. RRR = 200. Hc2(WHH) = 31.4 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			2.207				2.207																				T	RES(on). extrapolation	9.34							T/K	RES(on)	20.34			MHC157887		A	BCS, Fermi velocity	38.5																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157888	JPS077114704	P = 2.8 GPa. RRR = 200. Hc2(WHH) = 30.8 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			2.21				2.21																				T	RES(on). extrapolation	9.35							T/K	RES(on)	19.93			MHC157888		A	BCS, Fermi velocity	38.43																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157889	JPS077114704	P = 3.7 GPa. RRR = 200. Hc2(WHH) = 17.3 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			1.82				1.82																				T	RES(on). extrapolation	5.7							T/K	RES(on)	13.6			MHC157887		A	BCS, Fermi velocity	47.35																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157890	JPS077114704	P = 4.5 GPa. RRR = 200. Hc2(WHH) = 5.9 T	CeRhIn5	Ce1Rh1In5	Ce	1	Rh	1	In	5																		3	2008																										ABC5		HoCoGa5																		K			1.16				1.16																				T	RES(on). extrapolation	2.76							T/K	RES(on)	7.25			MHC157887		A	BCS, Fermi velocity	74.75																																																															The Quantum Critical Point in CeRhIn5: A Resistivity Study			Commissariat a l Energie Atomic, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 77(2008)114704	Georg KNEBEL,Dai AOKI,Jean-Pascal BRISON,Jacques FLOUQUET		
157891	JPS087025003		Bi3O2S3	Bi3S3O2	Bi	3	S	3																	O	2		1	2018																										A2B3C3					A			41.2825												K	4.64		6				5.32																																																																							mOhm.cm							2.58				4.56																			Superconducting Properties in Y-doped Semimetallic Bi3O2S3 Superconductors			Department of Physics, Pusan National University, Busan 46241, Korea	J.Phys.Soc.Jpn, 87(2018)025003	Gun Cheol Kim,Miyeon Cheon,Dawood Ahmad,Yong Seung Kwon,Rock Kil Ko,Young Cheol Kim		
157892	JPS087025003		(Bi,La)3O2S3	Bi2.95La0.05S3O2	Bi	2.95	La	0.05	S	3															O	2		1	2018																										A2B3C3					A			41.3152												K	4.44						4.44																																																																							mOhm.cm							5.85																							Superconducting Properties in Y-doped Semimetallic Bi3O2S3 Superconductors			Department of Physics, Pusan National University, Busan 46241, Korea	J.Phys.Soc.Jpn, 87(2018)025003	Gun Cheol Kim,Miyeon Cheon,Dawood Ahmad,Yong Seung Kwon,Rock Kil Ko,Young Cheol Kim		
157893	JPS087025003		(Bi,Y)3O2S3	Bi2.95Y0.05S3O2	Bi	2.95	Y	0.05	S	3															O	2		1	2018																										A2B3C3					A			41.2428												K	4.93						4.93																																																																							mOhm.cm							0.82				1.65																			Superconducting Properties in Y-doped Semimetallic Bi3O2S3 Superconductors			Department of Physics, Pusan National University, Busan 46241, Korea	J.Phys.Soc.Jpn, 87(2018)025003	Gun Cheol Kim,Miyeon Cheon,Dawood Ahmad,Yong Seung Kwon,Rock Kil Ko,Young Cheol Kim		
157894	JPS087033707	RRR = 41.2. Tc(SP) = 0.46 K. e-ph = 0.376. (dC/gamma*Tc) = 1.26. Thermodynamic Hc(0) =25 Oe.	LaTi2Al20	La1Ti2Al20	La	1	Ti	2	Al	20																		3	2018																										AB2C20		CeCr2Al20	Fd3[-]m	227	A	14.7946														K		0.3					0.3										100																								MHC157894														3.34	14				MSP157894			mJ/mol.K2	22	SP	510	SP																																		La(3N),Al(4N)<Ti,V,Nb,Ta		Al-self flux method. mixture(La:T:Al = 1:2:90) - in alumina crucible - in quartz tube - heat(1050 C) - slow cool					Superconductivity in Cage Compounds LaTr2Al20 with Tr = Ti, V, Nb, and Ta			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 87(2018)033707	Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki		
157895	JPS087033707	RRR = 5.4.  e-ph = 0.34.	LaV2Al20	La1V2Al20	La	1	V	2	Al	20																		3	2018																										AB2C20		CeCr2Al20	Fd3[-]m	227	A	14.6125														K		0.15					0.15																																																								mJ/mol.K2	19.6	SP	525	SP																																		La(3N),Al(4N)<Ti,V,Nb,Ta		Al-self flux method. mixture(La:T:Al = 1:2:90) - in alumina crucible - in quartz tube - heat(1050 C) - slow cool					Superconductivity in Cage Compounds LaTr2Al20 with Tr = Ti, V, Nb, and Ta			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 87(2018)033707	Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki		
157896	JPS087033707	RRR = 9.5. Tc(SP) = 1.05 K. e-ph = 0.414. (dC/gamma*Tc) = 1.25. Thermodynamic Hc(0) = 57 Oe. kappa(GL) = 3.2	LaNb2Al20	La1Nb2Al20	La	1	Nb	2	Al	20																		3	2018																										AB2C20		CeCr2Al20	Fd3[-]m	227	A	14.818														K		1.15					1.15										100	Oe		15							Oe	SUS,extrapolation	449							Oe/K	SUS	586			MHC157896		A	from Hc2	856			A	cohere,kappa	2760					3.24	14				MSP157896			mJ/mol.K2	23.4	SP	505	SP																																		La(3N),Al(4N)<Ti,V,Nb,Ta		Al-self flux method. mixture(La:T:Al = 1:2:90) - in alumina crucible - in quartz tube - heat(1050 C) - slow cool					Superconductivity in Cage Compounds LaTr2Al20 with Tr = Ti, V, Nb, and Ta			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 87(2018)033707	Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki		
157897	JPS087033707	RRR = 9.2. Tc(SP) = 1.03 K. e-ph = 0.418. (dC/gamma*Tc) = 1.36. Thermodynamic Hc(0) = 56 Oe. kappa(GL) = 2.2	LaTa2Al20	La1Ta2Al20	La	1	Ta	2	Al	20																		3	2018																										AB2C20		CeCr2Al20	Fd3[-]m	227	A	14.8231														K		1.1					1.1										100	Oe		14							Oe	SUS,extrapolation	292							Oe/K	SUS	390			MHC157897		A	from Hc2	1060			A	cohere,kappa	2310					3.4	14				MSP157897			mJ/mol.K2	22.1	SP	480	SP																																		La(3N),Al(4N)<Ti,V,Nb,Ta		Al-self flux method. mixture(La:T:Al = 1:2:90) - in alumina crucible - in quartz tube - heat(1050 C) - slow cool					Superconductivity in Cage Compounds LaTr2Al20 with Tr = Ti, V, Nb, and Ta			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 87(2018)033707	Akira Yamada,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki		
157898	JPS087053704	Thermodynamic Hc(0) - 430 Oe. kappa(GL) = 40. Hc2(0) at T= 40 mK. (dC/gamma*Tc) = 1.39. e-ph = 0.69.	CeIr3	Ce1Ir3	Ce	1	Ir	3																				3	2018																										AB3			R3[-]m	166															PuNi3-type, Rhombohedral	K	3.2	3.4	3.5	3			3.4										100	Oe	M-H ccurve			51					T	RES(0.5Rn), extrapolation			4.65					T/K	RES(0.5Rn)			1.23	MHC157898		A	from Hc2		84		A	Hc1		3400				3.83	14							mJ/mol.K2	23	SP	144	SP											uOhm.cm							55																Ce(3N),Ir(3N5)		Czochralski method in tetra-arc furnace, Ce:In = 21.5:78.5					Superconducting Properties of CeIr3 Single Crystal			Graduate School of Engineering, Tohoku University, Sendai 980-8577, Japan	J.Phys.Soc.Jpn, 87(2018)053704	Yoshiki J. Sato,Ai Nakamura,Yusei Shimizu,Arvind Maurya,Yoshiya Homma,Dexin Li,Fuminori Honda,Dai Aoki		
157899	JPS087054704	not SC down to 18 K. SUS(300K) = -11.53 emu/g.	2H-Mose2	Mo1Se2	Mo	1	Se	2																				1	2018																													P6<3>/mmc		A	3.289		12.92											2H-type	K					1.8																																																																																																		2H-MoSe2 made by solid state reaction. Mixture(Li:MoSe2 = x:1) - heat(50C,2w). 0.2 M solution of Li, EDA					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157900	JPS087054704	Cointercalated(Li, M) sample. M = EDA(C2H8N2). M-content not known. Li-content x is nominal value..SUS(300K) = -0.97 emu/g.	Lix(C2H8N2)yMoSe2	Li0.25M1Mo1Se2	Li	0.25	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			23.7												K			4	4.2			4.2																																																																																																2H-MoSe2 made by solid state reaction. Mixture(Li:MoSe2 = x:1) - heat(50C,2w). 0.2 M solution of Li, EDA					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157901	JPS087054704	Cointercalated(Li, M) sample. M = EDA(C2H8N2). M-content not known. Li-content x is nominal value. SUS(300K) = -0.94 emu/g.	Lix(C2H8N2)yMoSe2	Li0.5M1Mo1Se2	Li	0.5	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			23.7											phase-II (c = 20.49)	K			4	4.2			4.2																																																																																																2H-MoSe2 made by solid state reaction. Mixture(Li:MoSe2 = x:1) - heat(50C,2w). 0.2 M solution of Li, EDA					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157902	JPS087054704	Cointercalated(Li, M) sample. M = EDA(C2H8N2). M-content not known. Li-content x is nominal value. SUS(300K) = -0.73 emu/g.	Lix(C2H8N2)yMoSe2	Li1M1Mo1Se2	Li	1	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			23.6											phase-II (c = 20.56)	K			3.9	4.2			4.2																																																																																																2H-MoSe2 made by solid state reaction. Mixture(Li:MoSe2 = x:1) - heat(50C,2w). 0.2 M solution of Li, EDA					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157903	JPS087054704	Cointercalated(Li, M) sample. M = HMDA(= C6H16N2). M-content not known. Li-content x is nominal value. SUS(300K) = -1.60 emu/g.	Lix(C6H16N2)yMoSe2	Li0.25M1Mo1Se2	Li	0.25	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			30.8												K				3.8			3.8																																																																																																					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157904	JPS087054704	Cointercalated(Li, M) sample. M = HMDA(= C6H16N2). M-content not known. Li-content x is nominal value. SUS(300K) = -1.11 emu/g.	Lix(C6H16N2)yMoSe2	Li0.5M1Mo1Se2	Li	0.5	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			37.4												K				4.2			4.2																																																																																																					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157905	JPS087054704	Cointercalated(Li, M) sample. M = HMDA(= C6H16N2). M-content not known. Li-content x is nominal value. SUS(300K) = -0.88 emu/g.	Lix(C6H16N2)yMoSe2	Li1M1Mo1Se2	Li	1	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			37.5												K				6			6																																																																																																					New Lithium- and Diamine-Intercalated Superconductors Lix(CnH2n+4N2)yMoSe2 (n = 2,6)			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)054704	Kazuki Sato,Takashi Noji,Takehiro Hatakeda,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
157906	JPS087054705	ANN(200C,100H,in O2). Tc(P)-FIG shows inflection point in M(T). hydrostatic (HSP) and uniaxial pressure. (dTc/dP) value in DB for HSP.	Fe1+yTe1-xSx	Fe1.07Te0.88S0.12	Fe	1.07	Te	0.88	S	0.12																		3	2018																										AB																			Fe-11	K	8.2		9	8.4			8.4	MTC157906		K/GP	-3.8																																																																																												crystals made by Tammann method. nominal(x=0.2,y=0) sealed in quartz ampule - heat(1050C,20h) -  ground -  furnace( T- gradient = 3C/cm) - heated(950 C,20h) - cool to 650( 3C/h) - kept( 650C,20 h)					Anisotropic Pressure Effects on Superconductivity in Fe1+yTe1-xSx			Department of Physics, Faculty of Science and Technology, Tokyo University of Science, Noda, Chiba 278-8510, Japan	J.Phys.Soc.Jpn, 87(2018)054705	Kazunori Yamamoto,Teruo Yamazaki,Takayoshi Yamanaka,Daichi Ueta,Hideki Yoshizawa,Hiroshi Yaguchi		
157907	JPS087063702	Tc by SP measurements. (dC/Tc) = 9.80 mJ/mol.K2. (dC/gamma*Tc) = 1.43.	BaPtSb	Ba1Pt1Sb1	Ba	1	Pt	1	Sb	1																		3	2018																										ABC		SrPtAs	P6[-]m2	187																K		1.64					1.64																																																					MSP157907			mJ/mol.K2	6.86	SP	186	SP											uOhm.cm							13				150												Ba,Pt,Sb powder		mixture(Ba:Pt:Sb=1.5:1:1.2) - alumina crucible - sealed in quartz tube (Ar) - heat(1150 C) - cool to 1100C (2.08 C/h) - FC to RT					Superconductivity in BaPtSb with an Ordered Honeycomb Network			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 87(2018)063702	Kazutaka Kudo,Yuki Saito,Takaaki Takeuchi,Shin-ya Ayukawa,Takayuki Kawamata,Shinichiro Nakamura,Yoji Koike,Minoru Nohara		
157908	JPS087073708	decomposed in air within several days.	BaPtAs	Ba1Pt1As1	Ba	1	Pt	1	As	1																		3	2018																										ABC		SrPtSb	P6[-]m2	187	A	4.308		4.761												K	2.75		2.82	2.8			2.8																				T	RES(0.5Rn), extrapolation	0.55												MHC157908		A	from Hc2	245																																																								Ba,Pt,PtAs2 powder		mixture - in alumina crucible - sealed in quartz tube - heat(1150 C,24-27 h) - furnace cool					Superconductivity in Hexagonal BaPtAs: SrPtSb- and YPtAs-type Structures with Ordered Honeycomb Network			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 87(2018)073708	Kazutaka Kudo,Takaaki Takeuchi,Hiromi Ota,Yuki Saito,Shin-ya Ayukawa,Kazunori Fujimura,Minoru Nohara		
157909	JPS087073708	decomposed in air within several days. (dC/Tc) = 8.40 mJ/mol.K2. (dC/gamma*Tc) = 1.46	BaPtAs	Ba1Pt1As1	Ba	1	Pt	1	As	1																		3	2018																										ABC		YPtAs	P6<3>/mmc	194	A	4.324		19.101												K	2.87		2.92				2.895																				T	RES(0.5Rn), extrapolation	3												MHC157909		A	from Hc2	105															MSP157909			mJ/mol.K2	5.74	SP	211	SP																																		Ba,Pt,PtAs2 powder		mixture - in alumina crucible - sealed in quartz tube - heat(1150 C,24-27 h) - rapid cooling to iced water					Superconductivity in Hexagonal BaPtAs: SrPtSb- and YPtAs-type Structures with Ordered Honeycomb Network			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 87(2018)073708	Kazutaka Kudo,Takaaki Takeuchi,Hiromi Ota,Yuki Saito,Shin-ya Ayukawa,Kazunori Fujimura,Minoru Nohara		
157910	JPS087073708	decomposed in air within several days.	BaPtAs	Ba1Pt1As1	Ba	1	Pt	1	As	1																		3	2018																										ABC		YPtAs	P6<3>/mmc	194	A	4.324		19.101												K	2.17		2.22				2.195																				T	RES(0.5Rn), extrapolation	0.5												MHC157909		A	from Hc2	256															MSP157909			mJ/mol.K2	4.77	SP	213	SP																																		Ba,Pt,PtAs2 powder		mixture - in alumina crucible - sealed in quartz tube - heat(1150 C,24-27 h) - rapid cooling to iced water					Superconductivity in Hexagonal BaPtAs: SrPtSb- and YPtAs-type Structures with Ordered Honeycomb Network			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 87(2018)073708	Kazutaka Kudo,Takaaki Takeuchi,Hiromi Ota,Yuki Saito,Shin-ya Ayukawa,Kazunori Fujimura,Minoru Nohara		
157911	JPS087073708	not SC above 0.1 K.	BaPtAs	Ba1Pt1As1	Ba	1	Pt	1	As	1																		3	2018																										ABC		LaIrSi	P2<1>3	198																K					0.1																																																																																																Ba,Pt,PtAs2 powder		mixture - in alumina crucible - sealed in quartz tube - heat(1100 C,24-27 h) - furnace cool					Superconductivity in Hexagonal BaPtAs: SrPtSb- and YPtAs-type Structures with Ordered Honeycomb Network			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	J.Phys.Soc.Jpn, 87(2018)073708	Kazutaka Kudo,Takaaki Takeuchi,Hiromi Ota,Yuki Saito,Shin-ya Ayukawa,Kazunori Fujimura,Minoru Nohara		
157912	JPS087073703	not SC. M-I transition at 255 K and 200 K.	RuAs	As1Ru1	As	1	Ru	1																				3	2018																										AB			P2<1>/c		A	5.723	3.3276	6.3206												K					1.4			MLAT157913																																																																																															Bi-flux method.  (Ru:Rh:As:Bi = (1-x):x:1:10) - sealed in silica tube - heat to 1100 C - cool to 500 C (2 C/h)					<75>As-NQR Investigation of the Relationship between the Instability of Metal-Insulator Transition and Superconductivity in Ru1-xRhxAs			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 87(2018)073703	Yoshiki Kuwata,Hisashi Kotegawa,Hitoshi Sugawara,Takahiro Sakurai,Hitoshi Ohta,Hideki Tou		
157913	JPS087073703		Ru1-xRhxAs	Ru0.75Rh0.25As1	Ru	0.75	Rh	0.25	As	1																		3	2018																										AB			P2<1>/c		A	5.6296	3.4572	6.197												K				1.8			1.8																																																																																																Bi-flux method.  (Ru:Rh:As:Bi = (1-x):x:1:10) - sealed in silica tube - heat to 1100 C - cool to 500 C (2 C/h)					<75>As-NQR Investigation of the Relationship between the Instability of Metal-Insulator Transition and Superconductivity in Ru1-xRhxAs			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 87(2018)073703	Yoshiki Kuwata,Hisashi Kotegawa,Hitoshi Sugawara,Takahiro Sakurai,Hitoshi Ohta,Hideki Tou		
157914	JPS087073703	SC-volume  is max for x = 0.4 in Ru1-xRhxAs. gap estimated from NMR measurements.	Ru1-xRhxAs	Ru0.6Rh0.4As1	Ru	0.6	Rh	0.4	As	1																		3	2018																										AB			P2<1>/c		A	5.5965	3.5256	6.1545												K				1.8			1.8																																																2	6																																															Bi-flux method.  (Ru:Rh:As:Bi = (1-x):x:1:10) - sealed in silica tube - heat to 1100 C - cool to 500 C (2 C/h)					<75>As-NQR Investigation of the Relationship between the Instability of Metal-Insulator Transition and Superconductivity in Ru1-xRhxAs			Department of Physics, Kobe University, Kobe 657-8501, Japan	J.Phys.Soc.Jpn, 87(2018)073703	Yoshiki Kuwata,Hisashi Kotegawa,Hitoshi Sugawara,Takahiro Sakurai,Hitoshi Ohta,Hideki Tou		
157915	LES1100321	not SC. (dR(T)/dT) = 1.4 uOhm.cm/K) for T <  25 K.	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		1	1985																										ABC3		BaNiSn3																		K					0																																																																									uOhm.cm											145														arc-melting - ANN(800-850 C, 6-8 days)					LOW-TEMPERATURE MAGNETIC AND ELECTRICAL PROPERTIES OF THE NEW TERNARY SILICIDES LaMSi AND CeMSi, WITH M = Co, Rh, Ir, Ru, OS			CRTBT-CNRS, BP 166 X, F-38042 Grenoble Cedex (France)	J.Less-Common Metals, 110(1985)321	P.Haen,P.Lejay,B.Chevalier,B.Lloret,J.Etourneau,M.Sera		
157916	LES1100321	not SC. (dR(T)/dT) = 1.5 uOhm.cm/K) for T < 12 K.	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		1	1985																										ABC3		BaNiSn3																		K					0																																																																									uOhm.cm											130														arc-melting - ANN(800-850 C, 6-8 days)					LOW-TEMPERATURE MAGNETIC AND ELECTRICAL PROPERTIES OF THE NEW TERNARY SILICIDES LaMSi AND CeMSi, WITH M = Co, Rh, Ir, Ru, OS			CRTBT-CNRS, BP 166 X, F-38042 Grenoble Cedex (France)	J.Less-Common Metals, 110(1985)321	P.Haen,P.Lejay,B.Chevalier,B.Lloret,J.Etourneau,M.Sera		
157917	LES1100321	not SC. T(T)-exponent, n = 2 for T < 100 K.	CeRuSi3	Ce1Ru1Si3	Ce	1	Ru	1	Si	3																		1	1985																										ABC3		BaNiSn3																		K					0																																																																									uOhm.cm											190														arc-melting - ANN(800-850 C, 6-8 days)					LOW-TEMPERATURE MAGNETIC AND ELECTRICAL PROPERTIES OF THE NEW TERNARY SILICIDES LaMSi AND CeMSi, WITH M = Co, Rh, Ir, Ru, OS			CRTBT-CNRS, BP 166 X, F-38042 Grenoble Cedex (France)	J.Less-Common Metals, 110(1985)321	P.Haen,P.Lejay,B.Chevalier,B.Lloret,J.Etourneau,M.Sera		
157918	LES1100321	not SC. T(T)-exponent, n = 2 for T < 100 K.	CeOsSi3	Ce1Os1Si3	Ce	1	Os	1	Si	3																		1	1985																										ABC3		BaNiSn3																		K					0																																																																									uOhm.cm											210														arc-melting - ANN(800-850 C, 6-8 days)					LOW-TEMPERATURE MAGNETIC AND ELECTRICAL PROPERTIES OF THE NEW TERNARY SILICIDES LaMSi AND CeMSi, WITH M = Co, Rh, Ir, Ru, OS			CRTBT-CNRS, BP 166 X, F-38042 Grenoble Cedex (France)	J.Less-Common Metals, 110(1985)321	P.Haen,P.Lejay,B.Chevalier,B.Lloret,J.Etourneau,M.Sera		
157919	LES1100321	T(T)-exponent, n = 2.5 for T < 100 K.	CeCoSi3	Ce1Co1Si3	Ce	1	Co	1	Si	3																		1	1985																										ABC3		BaNiSn3																		K				1.4			1.4																																																																							uOhm.cm											160														arc-melting - ANN(800-850 C, 6-8 days)					LOW-TEMPERATURE MAGNETIC AND ELECTRICAL PROPERTIES OF THE NEW TERNARY SILICIDES LaMSi AND CeMSi, WITH M = Co, Rh, Ir, Ru, OS			CRTBT-CNRS, BP 166 X, F-38042 Grenoble Cedex (France)	J.Less-Common Metals, 110(1985)321	P.Haen,P.Lejay,B.Chevalier,B.Lloret,J.Etourneau,M.Sera		
157920	MAT1704.07194	RRR = 10. Debye-T = 116 K from R(T). SP (beta) = 2.10 mJ/mol.K4. (dS/dT) = 0.00298 uV/K2 for 150<T<300K. carrier n = 3.78E+22 /cm3 from S (thermopower)	PdTe2	Pd1Te2	Pd	1	Te	2																				1	2017																										AB		CdI2	P-3m1																	K					1.8																																																										mJ/mol.K2	5.84	SP	140	SP	W/m.K	15.1			MTHC157920	uV/K	0.51			MTP157920	uOhm.cm	5.32										60														solid state reaction. mixture - sealed in quartz tube - heat(800 C,24h) - heat(500 C,7d) - reground - pellet - SIN(500 C,24h)					Electronic transport properties of intermediately coupled superconductors: PdTe2 and Cu0.04PdTe2			School of Basic Sciences, Indian Institute of Technology Mandi, Mandi-175005 (H.P.) India	cond-mat/1704.07194	M. K. Hooda,C. S. Yadav		
157921	MAT1704.07194	RRR = 30. Debye-T = 108 K from R(T). SP (beta) = 3.05 mJ/mol.K4. (dS/dT) = 0.00288 uV/K2 for 150<T<300K. carrier n = 3.78E+22 /cm3 from S (thermopower)	Cu0.04PdTe2	Cu0.04Pd1Te2	Cu	0.04	Pd	1	Te	2																		1	2017																										AB		CdI2	P-3m1																	K		2.4					2.4																																																								mJ/mol.K2	6.32	SP	136	SP	W/m.K	15.4			MTHC157921	uV/K	-0.64			MTP157921	uOhm.cm	1.45										51.4														solid state reaction. mixture - sealed in quartz tube - heat(800 C,24h) - heat(500 C,7d) - reground - pellet - SIN(500 C,24h)					Electronic transport properties of intermediately coupled superconductors: PdTe2 and Cu0.04PdTe2			School of Basic Sciences, Indian Institute of Technology Mandi, Mandi-175005 (H.P.) India	cond-mat/1704.07194	M. K. Hooda,C. S. Yadav		
157922	PHB5360150	P-induced SC. RRR = 4.55 (P=0).  SC properties for P = 15.8 GPa, where Tc(max). Hc2(0) = 5.75 T, -(dHc2/dT) = 11 T/K for R=zero definition.	CeAg2Si2	Ce1Ag2Si2	Ce	1	Ag	2	Si	2																		3	2018								8.6																		AB2C2		ThCr2Si2	I4/mmm																	K	1.25		1.57		0		1.41	MPH157922																			T	RES(onset), WHH			7.5					T/K	RES(onset)			25																																																															Bridgman method					Heavy-fermion superconductivity in CeAg2Si2 - Interplay of spin and valence fluctuations			DQMP ? University of Geneva, 1211 Geneva 4, Switzerland	Physica B, 536(2018)150	Gernot W. Scheerera,Zhi Ren,Gerard Lapertot,Gaston Garbarino,Didier Jaccard		
157923	PHB5360516	maybe Type-I SC	ThBe13	Be13Th1	Be	13	Th	1																				3	2018																										AB13		NaZn13			A	10.395														K	0.135		0.18	0.135			0.135																				T	RES(zero), BCS	0.003												MHC157923																																																												Th(2N5),Lu(3N),Be(3N5),Al(5N)		Crystals grown by Al-flux method.  mixture(R:Be:Al=1:13:45) - in al2O3 crucible - heat(1050 C,3d) - cool to 800C (2 C/h)					Superconductivity in single crystalline ThBe13 and LuBe13			Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 121 16 Prague 2, Czech Republic	Physica B, 536(2018)516	Klara Uhlirova,Naoyuki Miura,Vladimir Tkac,Jan Prokleska,Maciej Chrobak,Zbigniew Tarnawski,Hiroki Hidaka,Tatsuya Yanagisawa,Vladimir Sechovsky,Hiroshi Amitsuka		
157924	PHB5360516	maybe Type-I SC	LuBe13	Be13Lu1	Be	13	Lu	1																				3	2018																										AB13		NaZn13			A	10.184														K				0.62			0.62																																																																																														Th(2N5),Lu(3N),Be(3N5),Al(5N)		Crystals grown by Al-flux method.  mixture(R:Be:Al=1:13:45) - in al2O3 crucible - heat(1050 C,3d) - cool to 800C (2 C/h)					Superconductivity in single crystalline ThBe13 and LuBe13			Department of Condensed Matter Physics, Faculty of Mathematics and Physics, Charles University, Ke Karlovu 5, 121 16 Prague 2, Czech Republic	Physica B, 536(2018)516	Klara Uhlirova,Naoyuki Miura,Vladimir Tkac,Jan Prokleska,Maciej Chrobak,Zbigniew Tarnawski,Hiroki Hidaka,Tatsuya Yanagisawa,Vladimir Sechovsky,Hiroshi Amitsuka		
157925	PHB5360734	RRR = 8. SP (beta) = 0.549 mJ/mol.K4. (dC/Tc) = 6.0 mJ/mol.K2, (dC/gamma*Tc) = 0.9. kappa(GL) = 2.14.  e-ph = 0.42	ThPd2Ge2	Th1Pd2Ge2	Th	1	Pd	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.2935		10.0944												K	0.63			0.62			0.62																				mT	RES(mid),GL approx..	32												MHC157925		nm	from Hc2	102			nm	kappa(GL)	218					2.814	14				MSP157925			mJ/mol.K2	6.64	SP	260	SP											uOhm.cm	19.4																						Th(98%),Pd(4N),Ge(5N)		arc-melting					Superconductivity in ThPd2Ge2			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P.O.Box 1410, 50-950 Wroc?aw, Poland	Physica B, 536(2018)734	Krzysztof Domieracki,Piotr Wisniewski,Konrad Wochowski,Tetiana Romanova,Alicja Hackemer,Roman Gorzelniak,Adam Pikul,Dariusz Kaczorowski		
157926	PHB5360761		YPd2Ge2	Y1Pd2Ge2	Y	1	Pd	2	Ge	2																		3	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.2347		10.0374												K				1.14			1.14											mT	M-H curve		6.9						mT	SP and SUS		19.3	34.5										MHC157926		nm	from Hc2		127	101	nm			227	287								MSP157926			mJ/mol.K2	7.8	SP	289	SP											uOhm.cm		8.6	7.8																						PdGe-flux. Firstly PdGe prepared by arc-melting - remelt with Y (Y:Pd:Ge = 1:4:4) - sealed in quartz ampoule - heat (1200 C, 48 h) - slow cool to 1070 C.					Superconductivity in single crystalline YPd2Ge2			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50?590 Wroc?aw 2, Poland	Physica B, 536(2018)761	G. Chajewski,P.Wisniewski,A.Hackemer,A.P.Pikul,D.Kaczorowski		
157927	PHC5490011	alpha-pyrochlore.	Cd2Re2O7	Cd2Re2O7	Cd	2	Re	2	O	7																		3	2018																										A2B2C7		pyrochlore	Fd3m																	K		0.99					0.99																																																3.3	1																																													Re(4N),Cd(4N75),O		Firstly prepared Re2O7 from Re and O or <18>O(enriched 98% isotope,  addition with Cd or <116>Cd(enriched 88.7 %), then CVT method					Isotope effect on superconductivity and Raman phonons of Pyrochlore Cd2Re2O7			Department of Physics, Brock University, St. Catharines, Ontario L2S 3A1, Canada	Physica C, 549(2018)11	F.S. Razavi,M. Hajialamdari,M. Reedyk,R.K. Kremer		
157928	PHC5490011	SP (beta) = 0.223 mJ/mol.K4. isotope effect of <18>O , alpha =< 0.04	Cd2Re2<18>O7	Cd2Re2O7	Cd	2	Re	2	O	7																		3	2018																										A2B2C7		pyrochlore	Fd3m																	K														O	98																																													MSP157928																																									Re(4N),Cd(4N75),O		Firstly prepared Re2O7 from Re and O or <18>O(enriched 98% isotope,  addition with Cd or <116>Cd(enriched 88.7 %), then CVT method					Isotope effect on superconductivity and Raman phonons of Pyrochlore Cd2Re2O7			Department of Physics, Brock University, St. Catharines, Ontario L2S 3A1, Canada	Physica C, 549(2018)11	F.S. Razavi,M. Hajialamdari,M. Reedyk,R.K. Kremer		
157929	PHC5490011	isotope effect of <116>Cd , alpha = 0.04	<116>Cd2Re2<18>O7	Cd2Re2O7	Cd	2	Re	2	O	7																		3	2018																										A2B2C7		pyrochlore	Fd3m																	K								MGAP157929					0.04	Cd	88.7																																													MSP157928			mJ/mol.K2	30.4	SP																																				Re(4N),Cd(4N75),O		Firstly prepared Re2O7 from Re and O or <18>O(enriched 98% isotope,  addition with Cd or <116>Cd(enriched 88.7 %), then CVT method					Isotope effect on superconductivity and Raman phonons of Pyrochlore Cd2Re2O7			Department of Physics, Brock University, St. Catharines, Ontario L2S 3A1, Canada	Physica C, 549(2018)11	F.S. Razavi,M. Hajialamdari,M. Reedyk,R.K. Kremer		
157930	PHC5490088	RRR = 8.0. - (dHc2/dT) = 5.77 and 4.44 for R(0.9Rn) and R(0.1Rn). SP (beta) = 1.14 mJ/mol.K4. (dC/gamma*Tc) = 1.04. SUS(300K) = 3.21E-4 cm3/mol.	BaNb2S5	Ba1Nb2S5	Ba	1	Nb	2	S	5																			2018																										AB2C5						3.318		24.65											hexagonal	K		1.09					1.09																													T/K	RES(mid)	0.5			MHC157930		A		62.1			A	London	2090			meV	0.184		14							mJ/mol.K2	9.02	SP	119.3	SP																																		BaCO3,Nb2O5		mixture quartz tube - solid state reaction, several times using CS2/N2 gas flow.					Observation of superconductivity in BaNb2S5			Physics Department, Montana State University, Bozeman, MT 59717-3840, USA	Physica C, 549(2018)88	M.G. Smith,J.J. Neumeier		
157931	PHC5490088	RRR = 17.  -(dHc2/dT) = 7.64 and 4.86 for R(0.9Rn) and R(0.1Rn). SP (beta) = 0.963 mJ/mol.K4. (dC/gamma*Tc) = 0.993. SUS(300K) = 3.25E-4 cm3/mol.	BaNb2S5	Ba1Nb2S5	Ba	1	Nb	2	S	5																			2018																										AB2C5						3.316		24.77											hexagonal	K		0.95					0.95																													T/K	RES(mid)	0.576																						MSP157931			mJ/mol.K2	11.2	SP	126	SP																									cm3/C	-0.0015					MRH157931	n/cm3	2400000000000000000000			solid state reaction using elements of Ba, Nb metal s and S, details in text.					Observation of superconductivity in BaNb2S5			Physics Department, Montana State University, Bozeman, MT 59717-3840, USA	Physica C, 549(2018)88	M.G. Smith,J.J. Neumeier		
157932	PRB087121101	nodeless SC for x =< 0.4 in (Ca4Al2O6)Fe2(As1-xPx)2.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As2O6	Ca	4	Al	2	Fe	2	As	2													O	6		1	2013																												Fe-42622																	Al-42622As	K		26.8					26.8																																																																																																High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157933	PRB087121101	nodeless SC for x =< 0.4 in (Ca4Al2O6)Fe2(As1-xPx)2.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As1.6P0.4O6	Ca	4	Al	2	Fe	2	As	1.6	P	0.4											O	6		1	2013																												Fe-42622																	Al-42622As	K		22.5					22.5	MPH157933																																																																																															High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157934	PRB087121101	open symbol in Figure, means Tn of minority phase.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As1.2P0.8O6	Ca	4	Al	2	Fe	2	As	1.2	P	0.8											O	6		1	2013								0																				Fe-42622																	Al-42622As	K		0			0		0																																																																																																High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157935	PRB087121101	AFM occures for 1.32 < h<Pn> (pnictide hight) < 1.42. open symbol in Figure, means Tc of minority phase.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As1P1O6	Ca	4	Al	2	Fe	2	As	1	P	1											O	6		1	2013								45.3																				Fe-42622																	Al-42622As	K		0			0		0																																																																																																High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157936	PRB087121101	AFM occures for 1.32 < h<Pn> (pnictide hight) < 1.42.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As0.5P1.5O6	Ca	4	Al	2	Fe	2	As	0.5	P	1.5											O	6		1	2013								62																				Fe-42622																	Al-42622As	K		0			0		0	MPH157933																																																																																															High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157937	PRB087121101	AFM occures for 1.32 < h<Pn> (pnictide hight) < 1.42.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2As0.1P1.9O6	Ca	4	Al	2	Fe	2	As	0.1	P	1.9											O	6		1	2013								50																				Fe-42622																	Al-42622As	K		0			0		0																																																																																																High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157938	PRB087121101	nodal SC for x > 0.95 in (Ca4Al2O6)Fe2(As1-xPx)2.	(Ca4Al2O6)Fe2(As1-xPx)2	Ca4Al2Fe2P2O6	Ca	4	Al	2	Fe	2	P	2													O	6		1	2013																												Fe-42622																	Al-42622As	K		16.6					16.6																																																																																																High-P, solid state reaction method. O-content = nearly 6					Emergent phases of nodeless and nodal superconductivity separated by antiferromagnetic order in iron-based superconductor (Ca4Al2O6)Fe2(As1-xPx)2: <75>As- and <31>P-NMR studies			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	Phys.Rev.B, 87(2013)121101	H. Kinouchi,H. Mukuda,Y. Kitaoka,P. M. Shirage,H. Fujihisa,Y. Gotoh,H. Eisaki,A. Iyo		
157939	PRB093064501	Mo8.1Ga40.9 by EDX. SP (beta) = 11.76 mJ/mol.K4.  (dC/gamma*Tc) = 2.83.  DOS = 22.36 state/eV.fu from gamma. Hc3(0) =12.3 T. Hc3/Hc2 = 1.5	Mo8Ga41	Ga41Mo8	Ga	41	Mo	8																				3	2016																										A8B41			R3[-]	148																K			9.8				9.8											Oe	M-H curve	131							T	SP, SUS, GL fitting	8.3							T/K	SP,SUS	1			MHC157939		A	from Hc2	158																																																								Mo(3N),V(3N),Ga(5N)		(Mo:V:Ga = (8-x:x:400) - quartz ampoule - ANN(830 C,55h) - slow cool to 170 C(4 C/h) - remove excess of liquid Ga - 0.5M Hcl (24h) - washed by water					Strong electron-phonon coupling in the intermetallic superconductor Mo8Ga41			Department of Chemistry, Lomonosov Moscow State University, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)064501	Valeriy Yu. Verchenko,Alexander A. Tsirlin,Alexander O. Zubtsovskiy,Andrei V. Shevelkov		
157940	PRB093064501		Mo8-xVxGa41	Ga41Mo7V1	Ga	41	Mo	7	V	1																		3	2016																										A8B41			R3[-]	148																K			9.2				9.2																																																																																														Mo(3N),V(3N),Ga(5N)		(Mo:V:Ga = (8-x:x:400) - quartz ampoule - ANN(830 C,55h) - slow cool to 170 C(4 C/h) - remove excess of liquid Ga - 0.5M Hcl (24h) - washed by water					Strong electron-phonon coupling in the intermetallic superconductor Mo8Ga41			Department of Chemistry, Lomonosov Moscow State University, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)064501	Valeriy Yu. Verchenko,Alexander A. Tsirlin,Alexander O. Zubtsovskiy,Andrei V. Shevelkov		
157941	PRB093064501		Mo8-xVxGa41	Ga41Mo6V2	Ga	41	Mo	6	V	2																		3	2016																										A8B41			R3[-]	148																K			8.7				8.7																																																								mJ/mol.K2	99.1	SP	201	SP											mOhm.cm							0.221																Mo(3N),V(3N),Ga(5N)		(Mo:V:Ga = (8-x:x:400) - quartz ampoule - ANN(830 C,55h) - slow cool to 170 C(4 C/h) - remove excess of liquid Ga - 0.5M Hcl (24h) - washed by water					Strong electron-phonon coupling in the intermetallic superconductor Mo8Ga41			Department of Chemistry, Lomonosov Moscow State University, 119991 Moscow, Russia	Phys.Rev.B, 93(2016)064501	Valeriy Yu. Verchenko,Alexander A. Tsirlin,Alexander O. Zubtsovskiy,Andrei V. Shevelkov		
157942	PNAS112E7048	SP (beta) = 4.68 mJ/mol.K4. (dC/gamma*Tc) = 1.6. e-ph = 0.51. DOS = 1.3 states/eV.fu from gamma.	ReGa5	Ga5Re1	Ga	5	Re	1																					2015																										AB5			Cmce																PdGa5-type, ortho-	K		2.1		2.3			2.1																																																					MSP157942			mJ/mol.K2	4.7	SP	314	SP																																		Re(5N),Ga(4N5)		(Re1.5Ga98.5,Re3Ga97) - sealed in SiO2 jackets - heat to 900 C for 24h at 3 C/min - cool to 500 C (4 C/h) - ANN(2days)					Endohedral gallide cluster superconductors and superconductivity in ReGa5			Department of Chemistry, Princeton University, Princeton, NJ 08540; and bFaculty of Applied Physics and Mathematics, Gdansk University of Technology, 80-233 Gdansk, Poland	Proc.Natl.Acad.Sci. (PNAS). (2015)112E7048	Weiwei Xie,Huixia Luo,Brendan F. Phelan,Tomasz Klimczuk,Francois Alexandre Cevallos,Robert Joseph Cava		
157943	PRB097104513	P-induced SC. RRR = 120. Tc(P) and Tn(P)  measured.  Tc(DB) shows Tc(max) at P = 2.52 GPa	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2018																										ABC3		BaNiSn3																		K				1.52	0		1.52	MPH157943																																																																																															Czochralski method. crystals - sealed in quartz tube - ANN(950 C, 5 days, in vac					Unconventional superconductivity and quantum criticality in the heavy fermions CeIrSi3 and CeRhSi3			Centro de Fisica, Instituto Venezolano de Investigaciones Cientificas, Apartado 20632, Caracas 1020-A, Venezuela	Phys.Rev.B, 97(2018)104513	J. F. Landaeta,D. Subero,D. Catala,S. V. Taylor,N. Kimura,R. Settai,Y. Onuki,M. Sigrist,I. Bonalde		
157944	PRB097104513	P-induced SC. RRR = 180. Tc(P) and Tn(P)  measured.  Tc(DB) shows Tc(max) at P = 2.45 GPa	CeRhSi3	Ce1Rh1Si3	Ce	1	Rh	1	Si	3																		3	2018																										ABC3		BaNiSn3																		K				0.92	0		0.92	MPH157944																																																																																															Czochralski method. crystals - sealed in quartz tube - ANN(950 C, 5 days, in vac					Unconventional superconductivity and quantum criticality in the heavy fermions CeIrSi3 and CeRhSi3			Centro de Fisica, Instituto Venezolano de Investigaciones Cientificas, Apartado 20632, Caracas 1020-A, Venezuela	Phys.Rev.B, 97(2018)104513	J. F. Landaeta,D. Subero,D. Catala,S. V. Taylor,N. Kimura,R. Settai,Y. Onuki,M. Sigrist,I. Bonalde		
157945	PRB097134508	Gap measured by Andreev reflection. gap size = 4.76 by SP analysis. SP (beta) = 1.16 mJ/mol.K4. Isotropic Hc2 (Hc2//ab = Hc2//c).	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2018																										AB2C2		ThCr2Si2	I4/mmm																	K		3.5		3.75			3.5	MGAP157945										Oe	M-H curve		43						T	M-H, RES, WHH		0.18	0.18										MHC157945		nm	from Hc2	42.7			nm	cohere, kappa	26.4			meV	0.85	5.4								mJ/mol.K2	5.9	SP	144	SP																																				self-flux method					High-pressure effects on isotropic superconductivity in the iron-free layered pnictide superconductor BaPd2As2			Center for High Pressure Science and Technology Advanced Research, Beijing, 100094, China	Phys.Rev.B, 97(2018)134508	M. Abdel-Hafiez,Y. Zhao,Z. Huang,C.-w. Cho,C. H. Wong,A. Hassen,M. Ohkuma,Y.-W. Fang,B.-J. Pan,Z.-A. Ren,A. Sadakov,A. Usoltsev,V. Pudalov,M. Mito,R. Lortz,C. Krellner,W. Yang		
157946	PRB097134508	Lattice const measured up to 30 GPa by angle dispersive XRD. bulk modulus= 40 (in DB) and 142 GPa for P < 12 and for P < 30 GPa, respectively.	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		3	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.474		10.331											lattice const measured for P < 30.2 GPa	K								MTC157946		K/GPa	-0.25																																																																																												self-flux method					High-pressure effects on isotropic superconductivity in the iron-free layered pnictide superconductor BaPd2As2			Center for High Pressure Science and Technology Advanced Research, Beijing, 100094, China	Phys.Rev.B, 97(2018)134508	M. Abdel-Hafiez,Y. Zhao,Z. Huang,C.-w. Cho,C. H. Wong,A. Hassen,M. Ohkuma,Y.-W. Fang,B.-J. Pan,Z.-A. Ren,A. Sadakov,A. Usoltsev,V. Pudalov,M. Mito,R. Lortz,C. Krellner,W. Yang		
157947	PRB097174516	Sn-content not shown.  P = 0. volume=153.7 A3. SG = R-3m for P < 19.1 GPa	Sn-doped Bi1.1Sb0.9Te2S	Sn0.1Bi1.1Sb0.9Te2S1	Sn	0.1	Bi	1.1	Sb	0.9	Te	2	S	1														3	2018																		GPa		51.4									R-3m		A	4.219		29.672												K					0																																																																																																		single crystals grown by modified Bridgman method					Pressure-induced topological insulator-to-metal transition and superconductivity in Sn-doped Bi1.1Sb0.9Te2S			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 97(2018)174516	Chao An,Xuliang Chen,Bin Wu,Yonghui Zhou,Ying Zhou,Ranran Zhang,Changyong Park,Fengqi Song,Zhaorong Yang		
157948	PRB097174516	Sn-content not shown.  P = 14.3 GPa. SG = C2/c for P > 11.7 GPa	Sn-doped Bi1.1Sb0.9Te2S	Sn0.1Bi1.1Sb0.9Te2S1	Sn	0.1	Bi	1.1	Sb	0.9	Te	2	S	1														3	2018																		GPa		97.2						AB2C2			C2/c																Two phases(R-3m + C2/c)	K			4.31				4.31	MTC157948																			T	RES(0.9Rn), WHH	2.31												MHC157948																																																														single crystals grown by modified Bridgman method					Pressure-induced topological insulator-to-metal transition and superconductivity in Sn-doped Bi1.1Sb0.9Te2S			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 97(2018)174516	Chao An,Xuliang Chen,Bin Wu,Yonghui Zhou,Ying Zhou,Ranran Zhang,Changyong Park,Fengqi Song,Zhaorong Yang		
157949	PRB097174516	Sn-content not shown.  P = 31.6 GPa. SG = Im-3m for P > 24 GPa	Sn-doped Bi1.1Sb0.9Te2S	Sn0.1Bi1.1Sb0.9Te2S1	Sn	0.1	Bi	1.1	Sb	0.9	Te	2	S	1														3	2018																		GPa		122.9						AB2C2			Im-3m		A	6.1885	12.92	18.083											Two phases(C2/c + Im-3m)	K			9.62				9.62																																																																																																single crystals grown by modified Bridgman method					Pressure-induced topological insulator-to-metal transition and superconductivity in Sn-doped Bi1.1Sb0.9Te2S			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 97(2018)174516	Chao An,Xuliang Chen,Bin Wu,Yonghui Zhou,Ying Zhou,Ranran Zhang,Changyong Park,Fengqi Song,Zhaorong Yang		
157950	PRB097184517	summary data of alpha-Ga(MP = 302.9 K). Type-I SC.  (dC/gamma*Tc) = 1.41. N(0) = 0.25 states/eV.atom from gamma.	alpha-Ga	Ga1	Ga	1																							2018																										A			Cmca																ortho-	K		1.08					1.08																				mT		5.03																								meV	0.18	3.94	14							mJ/mol.K2	0.6	SP	350	SP																																									Raising the superconducting Tc of gallium: In situ characterization of the transformation of alpha-Ga into beta-Ga			Department of Physics, Stockholm University, SE-106 91 Stockholm, Sweden	Phys.Rev.B, 97(2018)184517	D. Campanini,Z. Diao,A. Rydh		
157951	PRB097184517	beta-Ga(MP = 255 K). (dC/gamma*Tc) = 1.83. N(0) = 0.65 states/eV.atom from gamma.	beta-Ga	Ga1	Ga	1																							2018																										A			C2/c																monoclinic	K		6.04					6.04																				mT	SP(mid)	57												MHC157951												meV	1.04	4	14							mJ/mol.K2	1.53	SP	120	SP																																				heat to 317 K - supercooling at 255 K to beta-Ga.					Raising the superconducting Tc of gallium: In situ characterization of the transformation of alpha-Ga into beta-Ga			Department of Physics, Stockholm University, SE-106 91 Stockholm, Sweden	Phys.Rev.B, 97(2018)184517	D. Campanini,Z. Diao,A. Rydh		
157952	PRB097224506	SP (beta)=0.39mJ/mol.K4, (delta) = 1 microJ/mol.K6. (dC/gamma*Tc) = 1.76. [penet] measured using tuuel diode oscillator(TDO) and SP analysis. gap from SP and [penet]	Re6Zr	Re6Zr1	Re	6	Zr	1																				3	2018																										AB6																				K		6.8		6.8		0.2	6.8																																				nm	from Hc2	5.5			nm	TDO	200					3.9	14				MSP157952			mJ/mol.K2	27.4	SP													mOhm.cm							0.3																		Czochralski method					Fully gapped superconductivity in single crystals of noncentrosymmetric Re6Zr with broken time-reversal symmetry			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 97(2018)224506	G. M. Pang,Z. Y. Nie,A. Wang,D. Singh,W. Xie,W. B. Jiang,Y. Chen,R. P. Singh,M. Smidman,H. Q. Yuan		
157953	PRB097224508	T-O transition, Ts = 58.0 K,	NaFe1-xNixAs	Na1Fe1As1	Na	1	Fe	1	As	1																		3	2018								44.7																		ABC		PbFCl																	tetra-to-ortho transition at Ts	K				8.64			8.64										10																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157954	PRB097224508	T-O transition, Ts = 44.8 K,	NaFe1-xNixAs	Na1Fe1Ni0.004As1	Na	1	Fe	1	Ni	0.004	As	1																3	2018								32.9																		ABC		PbFCl																	tetra-to-ortho transition at Ts	K				8.42			8.42	MPH157954									70																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157955	PRB097224508	inhomogeneous magnetic order for 0.004 < x =< 0.13.	NaFe1-xNixAs	Na1Fe1Ni0.006As1	Na	1	Fe	1	Ni	0.006	As	1																3	2018								31.6																		ABC		PbFCl																	tetra-to-ortho transition at Ts	K				12.6			12.6										100																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157956	PRB097224508	inhomogeneous magnetic order for 0.004 < x =< 0.13.	NaFe1-xNixAs	Na1Fe1Ni0.008As1	Na	1	Fe	1	Ni	0.008	As	1																3	2018																										ABC		PbFCl																	tetra-to-ortho transition at Ts	K				17.4			17.4										100																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157957	PRB097224508	inhomogeneous magnetic order for 0.004 < x =< 0.13.	NaFe1-xNixAs	Na1Fe1Ni0.01As1	Na	1	Fe	1	Ni	0.01	As	1																3	2018								24.1																		ABC		PbFCl																	tetra-to-ortho transition at Ts	K				17.8			17.8										100																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157958	PRB097224508	T-O transition, Ts = 33.1 K. Energy gap, two gaps (large in DB, small ( D=1.8 meV, gap size = 2.8)) from muon-SR. Another Tn = 10 K. inhomogeneous magnetic order for 0.004 < x =< 0.13.	NaFe1-xNixAs	Na1Fe1Ni0.013As1	Na	1	Fe	1	Ni	0.013	As	1																3	2018								18.4																		ABC		PbFCl																	tetra-to-ortho transition at Ts	K				17.7			17.7										100																																				meV	4.5	6.9	16																																															self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157959	PRB097224508	magnetic order completely suppressed.	NaFe1-xNixAs	Na1Fe1Ni0.015As1	Na	1	Fe	1	Ni	0.015	As	1																3	2018																										ABC		PbFCl																		K				18.6			18.6										100																																																																																						self-flux method					Disentangling superconducting and magnetic orders in NaFe1-xNixAs using muon spin rotation			Department of Physics, Columbia University, New York, New York 10027, USA	Phys.Rev.B, 97(2018)224508	Sky C. Cheung,Zurab Guguchia,Benjamin A. Frandsen,Zizhou Gong,Kohtaro Yamakawa,Dalson E. Almeida,Ifeanyi J. Onuorah,Pietro Bonfa,Eduardo Miranda,Weiyi Wang,David W. Tam,Yu Song,Chongde Cao,Yipeng Cai,Alannah M. Hallas,Murray N. Wilson,Timothy J. S. Munsie,Graeme Luke,Bijuan Chen,Roberto De Renzi		
157960	PRB097224511	SP-heat shows no clear jump at Tc. carrier from Hall effect at RT. Tn obtained from kink in R(T).	TbPdBi	Tb1Pd1Bi1	Tb	1	Pd	1	Bi	1																		3	2018								5.5																		ABC		MgAgAs	F4[-]3m	216	A	6.653														K	1.58		1.7				1.64																				T	RES(on), Linear approx.	2.36							T/K	RES(on)	1.53			MHC157960		A	from Hc2	120																																																						n/cm3	9430000000000000000			Flux method using Bi-flux					Superconductivity in the half-Heusler compound TbPdBi			Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China	Phys.Rev.B, 97(2018)224511	H. Xiao,T. Hu,W. Liu,Y. L. Zhu,P. G. Li,G. Mu,J. Su,K. Li,Z. Q. Mao		
157961	PRB097235149		Ce1-xSmxCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2018																										ABC5		HoCoGa5	P4/mmm		A	4.6122		7.5606												K	2.3						2.3																																																																																																single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157962	PRB097235149		Ce1-xSmxCoIn5	Ce0.95Sm0.05Co1In5	Ce	0.95	Sm	0.05	Co	1	In	5																3	2018																										ABC5		HoCoGa5	P4/mmm																	K	1.78						1.78																																																																																																single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157963	PRB097235149		Ce1-xSmxCoIn5	Ce0.9Sm0.1Co1In5	Ce	0.9	Sm	0.1	Co	1	In	5																3	2018																										ABC5		HoCoGa5	P4/mmm		A	4.611		7.5483												K	1.44						1.44																																																																																																single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157964	PRB097235149		Ce1-xSmxCoIn5	Ce0.85Sm0.15Co1In5	Ce	0.85	Sm	0.15	Co	1	In	5																3	2018																										ABC5		HoCoGa5	P4/mmm		A	4.6114		7.5512												K	0.59						0.59																																																																																																single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157965	PRB097235149		Ce1-xSmxCoIn5	Ce0.82Sm0.18Co1In5	Ce	0.82	Sm	0.18	Co	1	In	5																3	2018								1.2																		ABC5		HoCoGa5	P4/mmm		A	4.6091		7.5507												K	0				0.025		0																																																																																																single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157966	PRB097235149	T2 in TCFIG shows another peak in C(T), corresponding to some magnetic order	Ce1-xSmxCoIn5	Ce0.3Sm0.7Co1In5	Ce	0.3	Sm	0.7	Co	1	In	5																3	2018								832																		ABC5		HoCoGa5	P4/mmm		A	4.5953		7.5134												K					0.025																																																																																																		single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157967	PRB097235149	T2 and T3 in TCFIG show another peak in C(T), corresponding to some magnetic order	Ce1-xSmxCoIn5	Sm1Co1In5	Sm	1	Co	1	In	5																		3	2018							-73	11.7																		ABC5		HoCoGa5	P4/mmm		A	4.5872		7.4951												K					0.025																																																																																																		single crystals grown by In-flux method					Temperature versus Sm concentration phase diagram and quantum criticality in the correlated electron system Ce1-xSmxCoIn5			Department of Physics, University of California, San Diego, La Jolla, California 92093, USA	Phys.Rev.B, 97(2018)235149	N. Pouse,S. Jang,B. D. White,S. Ran,R. B. Adhikari,C. C. Almasan,M. B. Maple		
157968	PRB098014502	(dC/gamma*Tc) = 1.57. SP data best fit to s-s two gap model, large one in DB, small (d0 =0.14 meV, gap size = 0.54). [penet] measured by muon-SR. GL (kappa)= 139.	TaRh2B2	Ta1Rh2B2	Ta	1	Rh	2	B	2																		1	2018																										AB2C2	6		P3<1>		A	4.6984		8.7338											trigonal	K		6					6											mT	H-H curve, GL approx.	3.8							T	RES(mid), GL approx.	15.2							T/K	RES(mid)	3.1			MHC157968		nm	from Hc2	4.67			nm	muon-SR	648			meV	1.16	4.56	14				MSP157968			mJ/mol.K2	4.29	SP	374	SP											mOhm.cm							2																Ta(3N),Rh(3N),B(2N)		mixture(Ta:Rh:B = 1:1.9:2.1) - pellet - wrapped in Ta foil - heat to 1200 C(150 C/h) - react (6h) - FC to RT					Multigap superconductivity in chiral noncentrosymmetric TaRh2B2	7		Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom; ISIS Facility, STFC Rutherford Appleton Laboratory, Harwell Science and Innovation Campus, Oxfordshire OX11 0QX, United Kingdom	Phys.Rev.B, 98(2018)014502	D. A. Mayoh,A. D. Hillier,K. Gotze,D. McK. Paul,G. Balakrishnan,M. R. Lees		
157969	PRB098020503	van der Waals layered structure. [penet] measured using TDO system. [penet](London) = 44 nm from calc.	NaSn2As2	Na1Sn2As2	Na	1	Sn	2	As	2																		3	2018																										AB2C2																				K		1.18					1.18																				T	RES(zero), WHH		0.567	0.241										MHC157969		A	from Hc2//c		380		nm	TDO	960					4.2																							uOhm.cm							122																		Melt synthesis. (Na:Sn:As = 1:2:2)					Evidence for s-wave pairing with atomic scale disorder in the van der Waals superconductor NaSn2As2			Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Phys.Rev.B, 98(2018)020503	K. Ishihara,T. Takenaka,Y. Miao,O. Tanaka,Y. Mizukami,H. Usui,K. Kuroki,M. Konczykowski,Y. Goto,Y. Mizuguchi,T. Shibauchi		
157970	PRB098024511	SP (beta) = 0.13 mJ/mol.K4, (delta) = 0.32 mJ/mol.K6. GL(kappa) = 51.7. C<el> fitting well by alpha model(= 2.65).	Sc5Rh6Sn18	Sc5Rh6Sn18	Sc	5	Rh	6	Sn	18																		3	2018																										A5B6C18			I4<1>/acd																	K				4.4			4.4																				T		7.24														nm	from Hc2	6.74			nm	Hc1, Hc(0)	34.2					5.3	14				MSP157970			mJ/mol.K2	51.1	SP	271	SP																																				(Sc:Rh:Sn = 1:2:20) - placed in quartz tube - heat(1050 C, 3h) - cool to 200 C(5 C/h) - removed excess flux					Unconventional superconductivity in the cage-type compound Sc5Rh6Sn18			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon OX11 0QX, United Kingdom	Phys.Rev.B, 98(2018)024511	A. Bhattacharyya,D. T. Adroja,N. Kase,A. D. Hillier,A. M. Strydom,J. Akimitsu		
157971	PRL121037003	nominal x = 7% Hg. Tc and Tn measured by C(T). (dC/gamma*Tc) = 0.8.  magnetic order below Tc measured by neutron diffraction.	CeCo(In1-xHgx)5	Ce1Co1In4.95Hg0.05	Ce	1	Co	1	In	4.95	Hg	0.05																3	2018								3.41																		ABC5		HoCoGa5																		K		1.73					1.73																																																																																																crystals grown by In/Hg flux method.					From Ising Resonant Fluctuations to Static Uniaxial Order in Antiferromagnetic and Weakly Superconducting CeCodIn1-xHgxT5dx=0.01T			School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.Lett.,121(2018)037003	C. Stock,J. A. Rodriguez-Rivera,K. Schmalzl,F. Demmel,D. K. Singh,F. Ronning,J. D. Thompson,E. D. Bauer		
157972	PRL121037003	nominal x = 9% Hg.  Tc and Tn measured by C(T). magnetic order below Tc measured by neutron diffraction.	CeCo(In1-xHgx)5	Ce1Co1In4.935Hg0.065	Ce	1	Co	1	In	4.935	Hg	0.065																3	2018								3.51																		ABC5		HoCoGa5																		K		1.37					1.37																																																																																																crystals grown by In/Hg flux method.					From Ising Resonant Fluctuations to Static Uniaxial Order in Antiferromagnetic and Weakly Superconducting CeCodIn1-xHgxT5dx=0.01T			School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.Lett.,121(2018)037003	C. Stock,J. A. Rodriguez-Rivera,K. Schmalzl,F. Demmel,D. K. Singh,F. Ronning,J. D. Thompson,E. D. Bauer		
157973	PRL121037003	Tc  measured by C(T)	CeCo(In1-xHgx)5	Ce1Co1In4.9625Hg0.0375	Ce	1	Co	1	In	4.9625	Hg	0.0375																3	2018					My-B/mol	0.98																				ABC5		HoCoGa5																		K		2.19					2.19																																																																																																crystals grown by In/Hg flux method.					From Ising Resonant Fluctuations to Static Uniaxial Order in Antiferromagnetic and Weakly Superconducting CeCodIn1-xHgxT5dx=0.01T			School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3JZ, United Kingdom	Phys.Rev.Lett.,121(2018)037003	C. Stock,J. A. Rodriguez-Rivera,K. Schmalzl,F. Demmel,D. K. Singh,F. Ronning,J. D. Thompson,E. D. Bauer		
157974	SCIR00512926	(dC/gamma*Tc) = 1.95. C<el> well fitting to T^3 dependence(alpha = 2.93). muon-SR measured at H=0 and transverse field.	Y5Rh6Sn18	Y5Rh6Sn18	Y	5	Rh	6	Sn	18																		3	2015																										A5B6C18			I4<1>/acd		A	13.75		27.45												K				3			3																																																					MSP157974	mJ/mol.K	223	mJ/mol.K2	38.13	SP	183	SP											uOhm.cm							350																		Sn-flux method. mixture(Y:Rh:Sn = 1:2:20) - quartz tube - heat to 1323 K - keep(1323K,3h) - cool to 473 K(5 K/h) - excess flux was detached					Unconventional superconductivity in Y5Rh6Sn18 probed by muon spin relaxation			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon, OX11 0QX, UK.	Sci,Rep., 5(2015)12926	Amitava Bhattacharyya,Devashibhai Adroja,Naoki Kase,Adrian Hillier,Jun Akimitsu,Andre Strydom		
157975	PRX004041032	electron(2.5 MeV) irradiation effect. irradiation rate = 3E-5 C/s.cm2. (dTc/dR0) = -350 mK/uOhm.cm	Ba(Fe1-xRux)2As2	Ba1Fe1.52Ru0.48As2	Ba	1	Fe	1.52	Ru	0.48	As	2																3	2014																										AB2C2		ThCr2Si2																		K		17.8					17.8	MTC157975																																																																						uOhm.cm							866																		sel-flux method					Effect of Electron Irradiation on Superconductivity in Single Crystals of Ba(Fe1-xRux)2As2 (x = 0.24)			The Ames Laboratory, Ames, Iowa 50011, USA	Phys.Rev.X, 4(2014)041032	R. Prozorov,M. Konczykowski,M. A. Tanatar,A. Thaler,S. L. Bud'ko,P. C. Canfield,V. Mishra,P. J. Hirschfeld		
157976	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text), =1.0081.	Ce1-xNdxO0.5F0.5BiS2	Ce1F0.5Bi1S2O0.5	Ce	1	F	0.5	Bi	1	S	2													O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0414		13.4752											S-Bi-S angle = 176.28, Bi-S(in-plane) distance = 3.2881 A	K		0					0																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157977	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text), = 1.0101	Ce1-xNdxO0.5F0.5BiS2	Ce0.8Nd0.2F0.5Bi1S2O0.5	Ce	0.8	Nd	0.2	F	0.5	Bi	1	S	2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0327		13.4524											S-Bi-S angle = 176.45 , Bi-S(in-plane) distance = 3.2883 A	K		0					0																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157978	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text), =1.0119	Ce1-xNdxO0.5F0.5BiS2	Ce0.6Nd0.4F0.5Bi1S2O0.5	Ce	0.6	Nd	0.4	F	0.5	Bi	1	S	2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.027		13.4508											S-Bi-S angle = 177.74, Bi-S(in-plane) distance = 3.3050 A	K		3					3																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157979	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text), =1.0151	Ce1-xNdxO0.5F0.5BiS2	Ce0.4Nd0.6F0.5Bi1S2O0.5	Ce	0.4	Nd	0.6	F	0.5	Bi	1	S	2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.015		13.4026											S-Bi-S angle = 178.10, Bi-S(in-plane) distance = 3.2931 A	K		3.94					3.94																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157980	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text), = 1.0169	Ce1-xNdxO0.5F0.5BiS2	Ce0.2Nd0.8F0.5Bi1S2O0.5	Ce	0.2	Nd	0.8	F	0.5	Bi	1	S	2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0069		13.3982											S-Bi-S angle = 178.48 , Bi-S(in-plane) distance = 3.3086 A	K		4.48					4.48	MTC157980																																																																																																				In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157981	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0184	Ce1-xNdxO0.5F0.5BiS2	Nd1F0.5Bi1S2O0.5	Nd	1	F	0.5	Bi	1	S	2													O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0018		13.4153											S-Bi-S angle = 179.44 , Bi-S(in-plane) distance = 3.3352 A	K		4.79					4.79																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157982	SCIR00514968		LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S2O0.5	La	1	F	0.5	Bi	1	S	2													O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0699		13.4828											S-Bi-S angle = 178.16 , Bi-S(in-plane) distance =  3.2890A	K		2.48					2.48																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157983	SCIR00514968		LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S1.8Se0.2O0.5	La	1	F	0.5	Bi	1	S	1.8	Se	0.2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0792		13.4902											S-Bi-S angle = 178.60 , Bi-S(in-plane) distance = 3.3226 A	K		2.18					2.18																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157984	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0135	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S1.6Se0.4O0.5	La	1	F	0.5	Bi	1	S	1.6	Se	0.4											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.0913		13.5069											S-Bi-S angle = 177.52 , Bi-S(in-plane) distance = 3.3352 A	K		2.48					2.48																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157985	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0180	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S1.4Se0.6O0.5	La	1	F	0.5	Bi	1	S	1.4	Se	0.6											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.1071		13.5416											S-Bi-S angle = 177.50 , Bi-S(in-plane) distance = 3.3662 A	K		2.99					2.99																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157986	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0221	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S1.2Se0.8O0.5	La	1	F	0.5	Bi	1	S	1.2	Se	0.8											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.1273		13.5821											S-Bi-S angle = 176.95 , Bi-S(in-plane) distance = 3.3885 A	K		3.69					3.69																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157987	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0270	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S1Se1O0.5	La	1	F	0.5	Bi	1	S	1	Se	1											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.1349		13.6074											S-Bi-S angle = 176.06 , Bi-S(in-plane) distance = 3.3856 A	K		3.79					3.79	MTC157980																																																																																																				In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157988	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0303	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1S0.8Se1.2O0.5	La	1	F	0.5	Bi	1	S	0.8	Se	1.2											O	0.5		1	2015																										ABCD2		CeOBiS2			A	4.1406		13.6625											S-Bi-S angle = 176.12 , Bi-S(in-plane) distance = 3.3728 A	K		3.59					3.59																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157989	SCIR00514968	Tc depends on in-plane chemical pressure (definition , See text),  = 1.0308	LaO0.5F0.5Bi(S1-xSex)2	La1F0.5Bi1Se2O0.5	La	1	F	0.5	Bi	1	Se	2													O	0.5		1	2015																										ABCD2		CeOBiS2			A														S-Bi-S angle =  , Bi-S(in-plane) distance =  A	K		3.59					3.59																																																																																																					In-plane chemical pressure essential for superconductivity in BiCh2-based (Ch: S, Se) layered structure			Department of Electrical and Electronic Engineering, Tokyo Metropolitan University, 1-1, Minami-osawa, Hachioji 192-0397, Japan.	Sci,Rep., 5(2015)14968	Yoshikazu Mizuguchi,Akira Miura,Joe Kajitani,Takafumi Hiroi,Osuke Miura,Kiyoharu Tadanaga,Nobuhiro Kumada,Eisuke Magome,Chikako Moriyoshi,Yoshihiro Kuroiwa		
157990	SCIR00626530	not SC, T<CDW> = 148 K. Tm(FM) = 17.2 K	Sm1-xLaxNiC2	Sm1Ni1C2	Sm	1	Ni	1	C	2																		1	2016							17.2																			ABC2		CeNiC2	Amm2	38															cell volume = 102.1 A^3	K					1.8																																																																																																		arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157991	SCIR00626530	not SC, T<CDW> = 80 K. Tm(FM) = 17.8 K	Sm1-xLaxNiC2	Sm0.8La0.2Ni1C2	Sm	0.8	La	0.2	Ni	1	C	2																1	2016							17.8																			ABC2		CeNiC2	Amm2	38															cell volume = 104.0 A^3	K					1.8																																																																																																		arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157992	SCIR00626530	not SC, T<CDW> = 34 K. Tm(FM) = 17.8 K	Sm1-xLaxNiC2	Sm0.7La0.3Ni1C2	Sm	0.7	La	0.3	Ni	1	C	2																1	2016							17.82																			ABC2		CeNiC2	Amm2	38															cell volume = 105.0 A^3	K					1.8																																																																																																		arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157993	SCIR00626530	not SC, Tm(FM) = 5.2 K. T<CDW> not observed for x > 0.3.	Sm1-xLaxNiC2	Sm0.2La0.8Ni1C2	Sm	0.2	La	0.8	Ni	1	C	2																1	2016							5.2																			ABC2		CeNiC2	Amm2	38															cell volume = 110.3 A^3	K					1.8																																																																																																		arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157994	SCIR00626530	R not to zero. maybe filamentary SC. T<CDW> not observed for x > 0.3.	Sm1-xLaxNiC2	Sm0.05La0.95Ni1C2	Sm	0.05	La	0.95	Ni	1	C	2																1	2016																										ABC2		CeNiC2	Amm2	38															cell volume = 102.1 A^3	K			1.8				1.8																																																																																																arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157995	SCIR00626530	R not to zero. maybe filamentary SC	Sm1-xLaxNiC2	Sm0.03La0.97Ni1C2	Sm	0.03	La	0.97	Ni	1	C	2																1	2016																										ABC2		CeNiC2	Amm2	38															cell volume = 112.0 A^3	K			1.8				1.8	MPH157995																																																				MSP157995																																											arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157996	SCIR00626530		Sm1-xLaxNiC2	Sm0.02La0.98Ni1C2	Sm	0.02	La	0.98	Ni	1	C	2																1	2016																										ABC2		CeNiC2	Amm2	38																K	2						2																																																																																																arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157997	SCIR00626530	(dC/gamma*Tc) = 1.33. Tc(SP) = 2.9 K.	Sm1-xLaxNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2016																										ABC2		CeNiC2	Amm2	38															cell volume = 112.2 A^3	K	3.4						3.4																																																					MSP157997			mJ/mol.K2	7.3	SP	445	SP																																				arc-melting. weight loss less than 1%.  ANN(1173 K, 10 days in sealed quartz tube) - Q to NaCl-ice water mixture					Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157998	SCIR00626530	not SC. T<CDW> = 152 K.  FM for T < Tm = 10.4 K.	Sm1-xLuxNiC2	Sm0.2Lu0.2Ni1C2	Sm	0.2	Lu	0.2	Ni	1	C	2																1	2016							10.4																			ABC2		CeNiC2	Amm2	38															cell volume = 101.42 A^3	K					1.8																																																																																																							Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
157999	SCIR00626530	not SC. FM for T < Tm = 8.9 K.	Sm1-xLuxNiC2	Sm0.6Lu0.4Ni1C2	Sm	0.6	Lu	0.4	Ni	1	C	2																1	2016							8.9																			ABC2		CeNiC2	Amm2	38															cell volume = 98.42 A^3	K					1.8																																																																																																							Tuning the ferromagnetic phase in the CDW compound SmNiC2 via chemical alloying			Department of Physics, Sungkyunkwan University, Suwon 440-746, Korea.	Sci,Rep., 6(2016)26530	G. Prathiba,I. Kim,S. Shin,J. Strychalska,T. Klimczuk,T. Park		
158000	MAT1805.07847	van der Waals material. SP (beta) = 0.73 mJ/mol.K4, T(Ein) = 34 K. (dC/Tc) = 9.15 mJ/mol.K2. (dC/gamma*Tc) = 1.0. e-ph = 0.4	Na1-xSn2P2	Na0.926Sn2P2	Na	0.926	Sn	2	P	2																		1	2018																										AB2C2	6		R3[-]m	166	A	3.8847		27.1766											trigonal. gamma = 120 degree	K	1.9		2				1.95																				T	RES(0.9Rn), Linear approx.	1.6							T/K					MHC158000		nm	from Hc2	15															MSP158000			mJ/mol.K2	5.31	SP	237	SP																																		Na3P,Sn(4N),P(6N)		solid state reaction. mixture(Na3P:Sn:P = 1:3:2) - pellet - heat(400C, 20h, in quartz tube) - reground - pellet - heat(400C,20h)					Na1-xSn2P2 as a new member of van der Waals-type layered tin pnictide superconductors			Department of Physics, Tokyo Metropolitan University, 1-1 Minami-osawa, Hachioji, Tokyo 192-0397, Japan	cond-mat/1805.07847	Yosuke Goto,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Tatsuma D. Matsuda,Yuji Aoki,Yoshikazu Mizuguchi		
158050	JPS077073705	P-induced SC.  H//[001]. SC properties shows for P = 2.65 GPa. Hc2(0)//[001]  for various P are shown in figure MHC158050	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2008																										ABC3		BaNiSn3																		K	1.56				0		1.56	MTC158050																			T	RES(zero),		45						T/K	RES(zero)		17		MHC158050																																																														tetra-arc furnace.					Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)073705	Rikio SETTAI,Yuichiro MIYAUCHI,Tetsuya TAKEUCHI,Florence LEVY,Ilya SHEIKIN,Yoshichika ONUKI		
158051	JPS077073705	P-induced SC.  H//[110].  SC properties shows for P = 2.65 GPa.	CeIrSi3	Ce1Ir1Si3	Ce	1	Ir	1	Si	3																		3	2008																										ABC3		BaNiSn3																		K	1.5				0		1.5	MTC158050																			T	RES(zero),			9.5					T/K	RES(zero)			14.5	MHC158051																																																														tetra-arc furnace.					Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)073705	Rikio SETTAI,Yuichiro MIYAUCHI,Tetsuya TAKEUCHI,Florence LEVY,Ilya SHEIKIN,Yoshichika ONUKI		
158052	JPS077073705		LaIrSi3	La1Ir1Si3	La	1	Ir	1	Si	3																		3	2008																										ABC3		BaNiSn3																		K	0.9						0.9																				T			0.125	0.17					T/K			0.19	0.26	MHC158052																																																														tetra-arc furnace.					Huge Upper Critical Field and Electronic Instability in Pressure-induced Superconductor CeIrSi3 without Inversion Symmetry in the Crystal Structure			Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043	J.Phys.Soc.Jpn, 77(2008)073705	Rikio SETTAI,Yuichiro MIYAUCHI,Tetsuya TAKEUCHI,Florence LEVY,Ilya SHEIKIN,Yoshichika ONUKI		
158053	PRB098161103	T*(anomaly in R(T)) = 129 K (= T<STR>) from inelastic x-ray scattering data.	Sr3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																		3	2018																										A3B4C13			Pm3[-]m																	K		4.18					4.18																																																																																																Sn-flux method					Evidence of a structural quantum critical point in (CaxSr1-x)3Rh4Sn13 from a lattice dynamics study			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 98(2018)161103	Y. W. Cheung,Y. J. Hu,M. Imai,Y. Tanioku,H. Kanagawa,J. Murakawa,K. Moriyama,W. Zhang,K. T. Lai,K. Yoshimura,F. M. Grosche,K. Kaneko,S. Tsutsui,Swee K. Goh		
158054	PRB098161103	T*(anomaly in R(T)) = 48.6 K (= T<STR>) from inelastic x-ray scattering data.	(CaxSr1-x)3Rh4Sn13	Ca1.5Sr1.5Rh4Sn13	Ca	1.5	Sr	1.5	Rh	4	Sn	13																3	2018																										A3B4C13			Pm3[-]m																	K		6.41					6.41																																																																																																Sn-flux method					Evidence of a structural quantum critical point in (CaxSr1-x)3Rh4Sn13 from a lattice dynamics study			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 98(2018)161103	Y. W. Cheung,Y. J. Hu,M. Imai,Y. Tanioku,H. Kanagawa,J. Murakawa,K. Moriyama,W. Zhang,K. T. Lai,K. Yoshimura,F. M. Grosche,K. Kaneko,S. Tsutsui,Swee K. Goh		
158055	PRB098161103	T*(anomaly in R(T)) = 13.3 K (= T<STR>) from inelastic x-ray scattering data.	(CaxSr1-x)3Rh4Sn13	Ca2.25Sr0.75Rh4Sn13	Ca	2.25	Sr	0.75	Rh	4	Sn	13																3	2018																										A3B4C13			Pm3[-]m																	K		7.32					7.32																																																																																																Sn-flux method					Evidence of a structural quantum critical point in (CaxSr1-x)3Rh4Sn13 from a lattice dynamics study			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 98(2018)161103	Y. W. Cheung,Y. J. Hu,M. Imai,Y. Tanioku,H. Kanagawa,J. Murakawa,K. Moriyama,W. Zhang,K. T. Lai,K. Yoshimura,F. M. Grosche,K. Kaneko,S. Tsutsui,Swee K. Goh		
158056	PRB098161103	T*(anomaly in R(T)) = -5.8 K (= T<STR>) from inelastic x-ray scattering data. From this extrapolation, structural QCP occurs near x=0.86.	(CaxSr1-x)3Rh4Sn13	Ca2.55Sr0.45Rh4Sn13	Ca	2.55	Sr	0.45	Rh	4	Sn	13																3	2018																										A3B4C13			Pm3[-]m																	K		7.6					7.6																																																																																																Sn-flux method					Evidence of a structural quantum critical point in (CaxSr1-x)3Rh4Sn13 from a lattice dynamics study			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 98(2018)161103	Y. W. Cheung,Y. J. Hu,M. Imai,Y. Tanioku,H. Kanagawa,J. Murakawa,K. Moriyama,W. Zhang,K. T. Lai,K. Yoshimura,F. M. Grosche,K. Kaneko,S. Tsutsui,Swee K. Goh		
158057	PRB098140506	RRR = 15.7. FM(ab plane EU moment) below Tm = 15 K. energy gap measured by infrared reflectivity.	EuRbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																3	2018							15																			ABC4D4																			Fe-1144	K	36.25		36.5				36.375	MGAP158057																																								nm	optical conductivity	420			cm(-1)	40	3.17	15																						mOhm.cm												0.23													See PRB093214503. shiny ab face with 1 mm size					Unique interplay between superconducting and ferromagnetic orders in EuRbFe4As4			Moscow Institute of Physics and Technology, Dolgoprudny, Moscow 141700, Russia	Phys.Rev.B, 98(2018)140506	V. S. Stolyarov,A. Casano,M. A. Belyanchikov,A. S. Astrakhantseva,S. Yu. Grebenchuk,D. S. Baranov,I. A. Golovchanskiy,I. Voloshenko,E. S. Zhukova,B. P. Gorshunov,A. V. Muratov,V. V. Dremov,L. Ya. Vinnikov,D. Roditchev,Y. Liu,G.-H. Cao,M. Dressel,E. Uykur		
158058	PHB1350434	Tc measured inductively, defined as mid point in transition.	LaRu2	La1Ru2	La	1	Ru	2																				1	1985																										AB2		MgCu2(Laves)																		K		4.3					4.3																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158059	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxRu2	La0.94Th0.06Ru2	La	0.94	Th	0.06	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		3.44					3.44	MTC158059																																																																																															RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158060	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxRu2	La0.9Th0.1Ru2	La	0.9	Th	0.1	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		2.62					2.62																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158061	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxRu2	La0.47Th0.53Ru2	La	0.47	Th	0.53	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		1.73					1.73																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158062	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxRu2	La0.3Th0.7Ru2	La	0.3	Th	0.7	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		3.61					3.61																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158063	PHB1350434	Tc measured inductively, defined as mid point in transition.	ThRu2	Ru2Th1	Ru	2	Th	1																				1	1985																										AB2		MgCu2(Laves)																		K		3.4					3.4																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method.					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158064	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxRu2	Ce0.93Th0.07Ru2	Ce	0.93	Th	0.07	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		5.6					5.6																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158065	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxRu2	Ce0.7Th0.3Ru2	Ce	0.7	Th	0.3	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		4.89					4.89	MTC158065																																																																																															RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158066	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxRu2	Ce0.6Th0.4Ru2	Ce	0.6	Th	0.4	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		4.5					4.5																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158067	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxRu2	Ce0.3Th0.7Ru2	Ce	0.3	Th	0.7	Ru	2																		1	1985																										AB2		MgCu2(Laves)																		K		4.12					4.12																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158068	PHB1350434	Tc measured inductively, defined as mid point in transition.	ThRu2	Ru2Th1	Ru	2	Th	1																				1	1985																										AB2		MgCu2(Laves)																		K		3.5					3.5																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158069	PHB1350434	Tc measured inductively, defined as mid point in transition.	LaIr3	Ir3Th1	Ir	3	Th	1																				1	1985																										AB3																				K		2.47					2.47																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158070	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxIr3	La0.9Th0.1Ir3	La	0.9	Th	0.1	Ir	3																		1	1985																										AB3																				K		3.18					3.18																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158071	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxIr3	La0.6Th0.4Ir3	La	0.6	Th	0.4	Ir	3																		1	1985																										AB3																				K		3.63					3.63	MTC158071																																																																																															RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158072	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxIr3	La0.4Th0.6Ir3	La	0.4	Th	0.6	Ir	3																		1	1985																										AB3																				K		4.03					4.03																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158073	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxIr3	La0.2Th0.8Ir3	La	0.2	Th	0.8	Ir	3																		1	1985																										AB3																				K		4.48					4.48																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158074	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xThxIr3	Ir3Th1	Ir	3	Th	1																				1	1985																										AB3																				K		4.99					4.99																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158075	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xCexIr3	La0.9Ce0.1Ir3	La	0.9	Ce	0.1	Ir	3																		1	1985																										AB3																				K		2.82					2.82																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158076	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xCexIr3	La0.71Ce0.29Ir3	La	0.71	Ce	0.29	Ir	3																		1	1985																										AB3																				K		3.08					3.08	MTC158076																																																																																															RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158077	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xCexIr3	La0.39Ce0.61Ir3	La	0.39	Ce	0.61	Ir	3																		1	1985																										AB3																				K		2.74					2.74																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158078	PHB1350434	Tc measured inductively, defined as mid point in transition.	La1-xCexIr3	La0.2Ce0.8Ir3	La	0.2	Ce	0.8	Ir	3																		1	1985																										AB3																				K		2.79					2.79																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158079	PHB1350434	Tc measured inductively, defined as mid point in transition.	ThIr3	Ir3Th1	Ir	3	Th	1																				1	1985																										AB3																				K		3.05					3.05																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158080	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxIr3	Ce0.52Th0.48Ir3	Ce	0.52	Th	0.48	Ir	3																		1	1985																										AB3																				K		3.83					3.83	MTC158080																																																																																															RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158081	PHB1350434	Tc measured inductively, defined as mid point in transition.	Ce1-xThxIr3	Ce0.32Th0.68Ir3	Ce	0.32	Th	0.68	Ir	3																		1	1985																										AB3																				K		4.22					4.22																																																																																																RRu2,RIr2, firstly arc-melted. Then, pseudobinary samples made by arc-melting method. ANN(1000C, 5d, in quartz tube (He))					The valence of Ce in CeRu2 and CeIr3 THRU superconductivity				Physica B, 135(1985)434	M.HAKIMI,J.G. HUBER		
158082	JPS086114605	not SC. S-intercalated Nd3.5Sm0.5Ni3O8.	Nd3.5Sm0.5Ni3O8Sx	Nd3.5Sm0.5Ni3S0.26O8	Nd	3.5	Sm	0.5	Ni	3	S	0.26													O	8		1	2017																													I4/mmm	139	A	3.8518		26.825												K																																																																																																							Nd3.5Sm0.5Ni3O10 by solid state reaction - ANN(350C,5h, in flowing O2. S-intercalation by heating (300C,60h) with pellet of S.					Synchrotron X-ray Diffraction and High-Pressure Electrical Resistivity Studies for High-Tc Candidate Nd3.5Sm0.5Ni3O8			Department of Physics, Yokohama National University, Yokohama 240-8501, Japan	J.Phys.Soc.Jpn, 86(2017)114605	Masatomo Uehara,Kai Kobayashi,Hiroki Yamamoto,Akitoshi Nakata,Kazuhei Wakiya,Izuru Umehara,Jun Gouchi,Yoshiya Uwatoko		
158083	JPS086114605	not SC for P =< 8 GPa. S-deintercalated Nd3.5Sm0.5Ni3O8Sx. R(T) shows metallic for T > 60 K, semicond. for T < 60 K at P = 0.	Nd3.5Sm0.5Ni3O8Sx	Nd3.5Sm0.5Ni3O8	Nd	3.5	Sm	0.5	Ni	3															O	8		1	2017																													I4/mmm	139	A	3.9137		25.287												K																																																																																																							deintercalation performed by heating (290C, 20h, in flowing H2 gas)					Synchrotron X-ray Diffraction and High-Pressure Electrical Resistivity Studies for High-Tc Candidate Nd3.5Sm0.5Ni3O8			Department of Physics, Yokohama National University, Yokohama 240-8501, Japan	J.Phys.Soc.Jpn, 86(2017)114605	Masatomo Uehara,Kai Kobayashi,Hiroki Yamamoto,Akitoshi Nakata,Kazuhei Wakiya,Izuru Umehara,Jun Gouchi,Yoshiya Uwatoko		
158084	JPS087013701	<27>Al-NMR measured for H//c. Linewidth of NMR supports to be [penet]//ab = 4600 A.	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																		3	2018								14.5																		AB2C3		PrNi2Al3	P6/mmm																hexagonal	K		2					2																																									A	NMR(Al)		4600																																																				Chochralski method in triarc furnace					Spatially Inhomogeneous Superconducting State near Hc2 in UPd2Al3			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc.Jpn, 87(2018)013701	Shunsaku Kitagawa,Ryoichi Takaki,Masahiro Manago,Kenji Ishida,Noriaki K. Sato		
158085	PRB080165107	not SC. P-P and Co-Co distance, Co-P-Co angle were measured	Sr1-xCaxCo2P2	Sr1Co2P2	Sr	1	Co	2	P	2																		1	2009																										AB2C2		ThCr2Si2			A	3.7885		11.601												K					1.8																																																										mJ/m-Co.K2	21.9																																					P,Sr,Ca,CoP							Lattice collapse and the magnetic phase diagram of Sr1-xCaxCo2P2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 80(2009)165107	Shuang Jia,A. J. Williams,P. W. Stephens,R. J. Cava		
158086	PRB080165107	not SC. P-P and Co-Co distance, Co-P-Co angle were measured	Sr1-xCaxCo2P2	Sr0.56Ca0.44Co2P2	Sr	0.56	Ca	0.44	Co	2	P	2																1	2009																										AB2C2		ThCr2Si2			A	3.7867		11.202												K					1.8			MLAT158086																																																				MSP158086			mJ/m-Co.K2	18.2																																					P,Sr,Ca,CoP							Lattice collapse and the magnetic phase diagram of Sr1-xCaxCo2P2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 80(2009)165107	Shuang Jia,A. J. Williams,P. W. Stephens,R. J. Cava		
158087	PRB080165107	not SC. P-P and Co-Co distance, Co-P-Co angle were measured. T<FL> in TCFIG shows Fermi Liquid temperature.	Sr1-xCaxCo2P2	Sr0.46Ca0.54Co2P2	Sr	0.46	Ca	0.54	Co	2	P	2																1	2009																										AB2C2		ThCr2Si2			A	3.7909		11.0736												K					1.8			MPH158087																																																							mJ/m-Co.K2	20																																					P,Sr,Ca,CoP							Lattice collapse and the magnetic phase diagram of Sr1-xCaxCo2P2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 80(2009)165107	Shuang Jia,A. J. Williams,P. W. Stephens,R. J. Cava		
158088	PRB080165107	not SC. P-P and Co-Co distance, Co-P-Co angle were measured	Sr1-xCaxCo2P2	Ca1Co2P2	Ca	1	Co	2	P	2																		1	2009																										AB2C2		ThCr2Si2			A	3.8552		9.5686												K					1.8																																																																																																P,Sr,Ca,CoP							Lattice collapse and the magnetic phase diagram of Sr1-xCaxCo2P2			Department of Chemistry, Princeton University, Princeton, New Jersey 08544, USA	Phys.Rev.B, 80(2009)165107	Shuang Jia,A. J. Williams,P. W. Stephens,R. J. Cava		
158089	PRB082060518	[penet]London measured by TDR. but absolut value not shown. d[penet] = T^n, n = 2.78	Ba(Fe1-xCox)2As2	Ba1Fe1.86Co0.14As2	Ba	1	Fe	1.86	Co	0.14	As	2																3	2010																										AB2C2																				K			22.5				22.5																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158090	PRB082060518	Irradiation (1.4 GeV, <208>Pb-ion) effect. Density of deffect expressed by matching field B (T-unit). B = 0.5 T.  d[penet] = T^n, n = 2.66	Ba(Fe1-xCox)2As2	Ba1Fe1.86Co0.14As2	Ba	1	Fe	1.86	Co	0.14	As	2																3	2010																										AB2C2																				K			22.3				22.3																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158091	PRB082060518	Irradiation (1.4 GeV, <208>Pb-ion) effect. Density of deffect expressed by matching field B (T-unit). B = 1.0 T. d[penet] = T^n, n = 2.49	Ba(Fe1-xCox)2As2	Ba1Fe1.86Co0.14As2	Ba	1	Fe	1.86	Co	0.14	As	2																3	2010																										AB2C2																				K			22				22																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158092	PRB082060518	B = 0 T. d[penet] = T^n, n = 2.47	BaFe1-xNix)2As2	Ba1Fe1.91Ni0.09As2	Ba	1	Fe	1.91	Ni	0.09	As	2																3	2010																										AB2C2																				K			18.9				18.9																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158093	PRB082060518	Irradiation (1.4 GeV, <208>Pb-ion) effect. Density of deffect expressed by matching field B (T-unit). B = 1.0 T.  d[penet] = T^n, n = 2.30	BaFe1-xNix)2As2	Ba1Fe1.91Ni0.09As2	Ba	1	Fe	1.91	Ni	0.09	As	2																3	2010																										AB2C2																				K			18.27				18.27																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158094	PRB082060518	Irradiation (1.4 GeV, <208>Pb-ion) effect. Density of deffect expressed by matching field B (T-unit). B = 2.0 T.  d[penet] = T^n, n = 2.08	BaFe1-xNix)2As2	Ba1Fe1.91Ni0.09As2	Ba	1	Fe	1.91	Ni	0.09	As	2																3	2010																										AB2C2																				K			17.86				17.86																																																																																																FeAs flux method					London penetration depth in Ba(Fe1-xTx)2As2 (T= Co, Ni) superconductors irradiated with heavy ions			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 82(2010)060518	H. Kim,R. T. Gordon,M. A. Tanatar,J. Hua,U. Welp,W. K. Kwok,N. Ni,S. L. Bud'ko,P. C. Canfield,A. B. Vorontsov,R. Prozorov		
158095	JPCM0145067	not SC. T<CDW> = 151 K for both commensurate and incommensurate superstructures. CDW and AFM states coexist below Tn(=2.8 K)	Er5Ir4Si10	Er5Ir4Si10	Er	5	Ir	4	Si	10																		3	2002								2.8																		A4B5C10		Sc5Co4Si10	P4/mbm		A	12.543		4.203												K					1.8																																																																																																		single crystals grown by tri-arc Czochralski method					Coexistence of charge density wave and antiferromagnetism in Er5Ir4Si10			Kamerlingh Onnes Laboratory, Leiden University, NL-2300 RA Leiden, The Neitherlands	J.Phys.: Condens.Matter, 14(2002)5067	F. Galli,R.Feyerherm,R.W. Hendrikx,E.Dudzik,G.J.Nieuwenhuys,S.Ramakrishnan,S.D.Brown,S van Smaalen,J.A.Mydosh		
158096	JPS078074714	P-induced SC. Many AFM phases appear with increasing pressure. SC phase for 4 < P < 8 GPa. Figure shows magnetic (AFM) phase diagram for P < 8 GPa	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		3	2009								21.5																		ABC3		BaNiSn3	I4mm																	K					0			MPH158096																																																							mJ/mol.K2	32																																							Bi-flux method					High Pressure Phase Diagram of the Non-centrosymmetric Antiferromagnet CeCoGe3			Commissariat a l'Energie Atomique, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 78(2009)074714	Georg KNEBEL,Dai AOKI,Gerard LAPERTOT,Bernard SALCE,Jacques FLOUQUET,Tomoya KAWAI,Hiroshi MURANAKA,Rikio SETTAI,Yoshichika ONUKI		
158097	JPS078074714	P-induced SC. SC poperties (Tc, Hc2) are for P = 5.7 GPa.	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		3	2009																										ABC3		BaNiSn3	I4mm																	K		0.65			0		0.65	MPH158097																												T/K		73			MHC158097																																																														Bi-flux method					High Pressure Phase Diagram of the Non-centrosymmetric Antiferromagnet CeCoGe3			Commissariat a l'Energie Atomique, INAC, SPSMS, 17 rue des Martyrs, 38054 Grenoble, France	J.Phys.Soc.Jpn, 78(2009)074714	Georg KNEBEL,Dai AOKI,Gerard LAPERTOT,Bernard SALCE,Jacques FLOUQUET,Tomoya KAWAI,Hiroshi MURANAKA,Rikio SETTAI,Yoshichika ONUKI		
158098	JPS080SA112	(dC/gamma*Tc) = 1.96. C<e>: T^3 (anisotropic gap with point node. gamma(H) = H^(0.5) dependency at T = 0.63 K.	Y5Rh6Sn18	Y5Rh6Sn18	Y	5	Rh	6	Sn	18																		3	2011																										A5B6C18			I4<1>/acd		A	13.74		27.48												K				3			3																																																					MSP158098	mJ/mol.K	222	mJ/mol.K2	37.8	SP	185	SP																																		Y(3N) or Lu(3N),Rh(3N),Sn(5N)		Sn-flux method					Highly Anisotropic Gap Function in a Nonmagnetic Superconductor Y5Rh6Sn18			Department of Physics and Mathematics, Aoyana-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011) SA 112	Naoki KASE,Keigo INOUE,Hiroki HAYAMIZU,Jun AKIMITSU		
158099	JPS080SA112	(dC/gamma*Tc) = 2.02.  gamma(H) = linear H dependency at T = 0.63 K. Energy gap obtained from SP measurements	Lu5Rh6Sn18	Lu5Rh6Sn18	Lu	5	Rh	6	Sn	18																		3	2011																										A5B6C18			I4<1>/acd		A	13.63		27.26												K				4			4																																																4.26	14				MSP158099	mJ/mol.K	397	mJ/mol.K2	49.1	SP	158	SP																																		Y(3N) or Lu(3N),Rh(3N),Sn(5N)		Sn-flux method					Highly Anisotropic Gap Function in a Nonmagnetic Superconductor Y5Rh6Sn18			Department of Physics and Mathematics, Aoyana-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011) SA 112	Naoki KASE,Keigo INOUE,Hiroki HAYAMIZU,Jun AKIMITSU		
158100	JPS080SA112		(Y1-xLux)5Rh6Sn18	Y4Lu1Rh6Sn18	Y	4	Lu	1	Rh	6	Sn	18																3	2011																										A5B6C18			I4<1>/acd																	K				3.58			3.58																																																																																														Y(3N) or Lu(3N),Rh(3N),Sn(5N)		Sn-flux method					Highly Anisotropic Gap Function in a Nonmagnetic Superconductor Y5Rh6Sn18			Department of Physics and Mathematics, Aoyana-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011) SA 112	Naoki KASE,Keigo INOUE,Hiroki HAYAMIZU,Jun AKIMITSU		
158101	JPS080SA112		(Y1-xLux)5Rh6Sn18	Y3Lu2Rh6Sn18	Y	3	Lu	2	Rh	6	Sn	18																3	2011																										A5B6C18			I4<1>/acd																	K				3.75			3.75	MTC158101																																																																																													Y(3N) or Lu(3N),Rh(3N),Sn(5N)		Sn-flux method					Highly Anisotropic Gap Function in a Nonmagnetic Superconductor Y5Rh6Sn18			Department of Physics and Mathematics, Aoyana-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011) SA 112	Naoki KASE,Keigo INOUE,Hiroki HAYAMIZU,Jun AKIMITSU		
158102	JPS080SA112		(Y1-xLux)5Rh6Sn18	Y1Lu4Rh6Sn18	Y	1	Lu	4	Rh	6	Sn	18																3	2011																										A5B6C18			I4<1>/acd																	K				3.93			3.93																																																																																														Y(3N) or Lu(3N),Rh(3N),Sn(5N)		Sn-flux method					Highly Anisotropic Gap Function in a Nonmagnetic Superconductor Y5Rh6Sn18			Department of Physics and Mathematics, Aoyana-Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 252-5258, Japan	J.Phys.Soc.Jpn, 80(2011) SA 112	Naoki KASE,Keigo INOUE,Hiroki HAYAMIZU,Jun AKIMITSU		
158103	JPS083023702	Tc depends on Pd-content. Tc(x=0.94) = 5.56, Tc(x=0.89) = 317K.	Ta2PdxS5	Ta2Pd0.97S5	Ta	2	Pd	0.97	S	5																		1	2014																										AB2C5					A	12.273	3.28	15.294											alpha = gamma = 90, beta = 105.20 degree	K	6.05		6.53	5.91			5.91																																																					MSP158103			mJ/mol.K2	27.6	SP	231	SP											mOhm.cm								4.2																	solid state reaction					Superconductivity at 6K and the Violation of Pauli Limit in Ta2PdxS5			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 83(2014)023702	Yangfan Lu,Tomohiro Takayama,Alimamy F. Bangura,Yukari Katsura,Daisuke Hashizume,Hidenori Takagi		
158104	JPS083023702	Pauli limit = 10.2 T. Maki parameter = 4.4.	Ta2PdxS5	Ta2Pd0.92S5	Ta	2	Pd	0.92	S	5																		3	2014																										AB2C5																				K				5.4			5.4																				T	RES(0.5Rn),WHH		32	14					T/K	RES(0.5Rn)		8.5	3.7	MHC158104		nm	from Hc2		3.2	4.8																															mOhm.cm								0.32																	Chemical vapor transport (CVT) method					Superconductivity at 6K and the Violation of Pauli Limit in Ta2PdxS5			Department of Advanced Materials, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	J.Phys.Soc.Jpn, 83(2014)023702	Yangfan Lu,Tomohiro Takayama,Alimamy F. Bangura,Yukari Katsura,Daisuke Hashizume,Hidenori Takagi		
158105	JPS087083704	slightly high Ag conc. by EDS. Anomaly in R(T) at 180 K due to CDW. R(T) starts to deviate from normal value at 2.5 K	La2O2Bi3AgS6	La2Bi3Ag1S6O2	La	2	Bi	3	Ag	1	S	6													O	2		1	2018																													P4/nmm		A	4.0568		19.348											stacking of (BiAg)S and LaO(BiAg)S2	K	0.5						0.5																																																																																														Bi2O3(3N),La2S3(3N),AgO(3N),Bi(5N),S(4N)		Solid state reaction. mixture - pellet - sealed in quartz tube - heat(720C, 15h)					Superconductivity in Layered Oxychalcogenide La2O2Bi3AgS6			Department of Physics, Tokyo Metropolitan University, Hachioji, Tokyo 192-0397, Japan	J.Phys.Soc.Jpn, 87(2018)083704	Rajveer Jha,Yosuke Goto,Ryuji Higashinaka,Tatsuma D. Matsuda,Yuji Aoki,Yoshikazu Mizuguchi		
158106	JPS087094717	not SC. as-grown sample. muonSR measured.	T'-La1.8Eu0.2Cu1-xNixO4	La1.8Eu0.2Cu1O4	La	1.8	Eu	0.2	Cu	1															O	4		1	2018								50																				T'																		K					0																																																																																																		low temperature synthesis					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158107	JPS087094717	reduced sample.muonSR measured.	T'-La1.8Eu0.2Cu1-xNixO3.5	La1.8Eu0.2Cu1O3.5	La	1.8	Eu	0.2	Cu	1															O	3.5		1	2018								22																				T'																		K		20					20																																																																																																T-type materials - reduced sample(solid state reaction with CaH2) - N-type materials - react(400C,12h flowing O2) - reduction annealing					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158108	JPS087094717	reduced sample.  muonSR measured.	T'-La1.8Eu0.2Cu1-xNixO3.5	La1.8Eu0.2Cu0.995Ni0.005O3.5	La	1.8	Eu	0.2	Cu	0.995	Ni	0.005													O	3.5		1	2018								20																				T'																		K		17					17																																																																																																T-type materials - reduced sample(solid state reaction with CaH2) - N-type materials - react(400C,12h flowing O2) - reduction annealing					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158109	JPS087094717	reduced sample.  muonSR measured.	T'-La1.8Eu0.2Cu1-xNixO3.5	La1.8Eu0.2Cu0.99Ni0.01O3.5	La	1.8	Eu	0.2	Cu	0.99	Ni	0.01													O	3.5		1	2018								37																				T'																		K		15					15																																																																																																T-type materials - reduced sample(solid state reaction with CaH2) - N-type materials - react(400C,12h flowing O2) - reduction annealing					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158110	JPS087094717	reduced sample.  muonSR measured.	T'-La1.8Eu0.2Cu1-xZnxO3.5	La1.8Eu0.2Cu0.995Zn0.005O3.5	La	1.8	Eu	0.2	Cu	0.995	Zn	0.005													O	3.5		1	2018								20																				T'																		K		16					16																																																																																																T-type materials - reduced sample(solid state reaction with CaH2) - N-type materials - react(400C,12h flowing O2) - reduction annealing					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158111	JPS087094717	reduced sample.  muonSR measured.	T'-La1.8Eu0.2Cu1-xZnxO3.5	La1.8Eu0.2Cu0.99Zn0.01O3.5	La	1.8	Eu	0.2	Cu	0.99	Zn	0.01													O	3.5		1	2018								17																				T'																		K		14					14																																																																																																T-type materials - reduced sample(solid state reaction with CaH2) - N-type materials - react(400C,12h flowing O2) - reduction annealing					Impurity Effects on the Electronic State in the Undoped (Ce-free) Superconductor T'-La1.8Eu0.2CuO4 Studied by Muon Spin Relaxation			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)094717	Takayuki Kawamata,Koki Ohashi,Tomohisa Takamatsu,Tadashi Adachi,Masatsune Kato,Isao Watanabe,Yoji Koike		
158112	JPS087105001	coexistence of Sc and weak FM. remanence = 0.002 my-B/f.u at 50 K. Magnetic state studied by x-ray magnetic circular dichroism.	Sr2VFeAsO3-z	Sr2V1Fe1As1O2.75	Sr	2	V	1	Fe	1	As	1													O	3-z	2.75	3	2018							210																			ABCD2E3		21113																	stacking of FeAs and SrVO3	K				20			20																																																																																																self flux method					Local Magnetic States of the Weakly Ferromagnetic Iron-Based Superconductor Sr2VFeAsO3-z  Studied by X-ray Magnetic Circular Dichroism			Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	J.Phys.Soc.Jpn, 87(2018)105001	Masafumi Horio,Yukiharu Takeda,Hiromasa Namiki,Takao Katagiri,Yuki K. Wakabayashi,Shoya Sakamoto,Yosuke Nonaka,Goro Shibata,Keisuke Ikeda,Yuji Saitoh,Hiroshi Yamagami,Takao Sasagawa,Atsushi Fujimori		
158113	JPS087113702	M = EDA. co-intercalated (Ca and EDA) to 2H-MoSe2. lattice const (a) and EDA content x not measured. SC-volume fraction = 2 % at 2K. Tc depends on EDOS.	Ca(EDA)xMoSe2	Ca1M1Mo1Se2	Ca	1	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			24.13											2H-Mose2	K				6			6																																																																																														Mo(3N),Se(5N)		mixture(2H-MoSe2 and alkaline-earth metal) -  placed in a Teflon-lined steel autoclave together with EDA. (molar ratio of A:2H-MoSe2 = 1 : 1) - sealed in Teflonlined autoclave -  heat (120 C for 7 d)					New Intercalation Superconductors Ax(C2H8N2)yMoSe2 (A = Ca, Sr, Ba) Synthesized by Solvothermal Method			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)113702	Kazuki Sato,Takashi Noji,Shota Ueno,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
158114	JPS087113702	M = EDA. co-intercalated (Ca and EDA) to 2H-MoSe2. lattice const (a) and EDA content x not measured. SC-volume fraction = 2 % at 2K. Tc depends on EDOS.	Sr(EDA)xMoSe2	Sr1M1Mo1Se2	Sr	1	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			24.16											2H-Mose2	K				6.4			6.4																																																																																														Mo(3N),Se(5N)		mixture(2H-MoSe2 and alkaline-earth metal) -  placed in a Teflon-lined steel autoclave together with EDA. (molar ratio of A:2H-MoSe2 = 1 : 1) - sealed in Teflonlined autoclave -  heat (120 C for 7 d)					New Intercalation Superconductors Ax(C2H8N2)yMoSe2 (A = Ca, Sr, Ba) Synthesized by Solvothermal Method			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)113702	Kazuki Sato,Takashi Noji,Shota Ueno,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
158115	JPS087113702	M = EDA. co-intercalated (Ca and EDA) to 2H-MoSe2. lattice const (a) and EDA content x not measured. SC-volume fraction = 2 % at 2K. Tc depends on EDOS.	Ba(EDA)xMoSe2	Ba1M1Mo1Se2	Ba	1	M	1	Mo	1	Se	2																1	2018																													P6<3>/mmc		A			24.07											2H-Mose2	K				7.2			7.2																																																																																														Mo(3N),Se(5N)		mixture(2H-MoSe2 and alkaline-earth metal) -  placed in a Teflon-lined steel autoclave together with EDA. (molar ratio of A:2H-MoSe2 = 1 : 1) - sealed in Teflonlined autoclave -  heat (120 C for 7 d)					New Intercalation Superconductors Ax(C2H8N2)yMoSe2 (A = Ca, Sr, Ba) Synthesized by Solvothermal Method			Department of Applied Physics, Tohoku University, Sendai 980-8579, Japan	J.Phys.Soc.Jpn, 87(2018)113702	Kazuki Sato,Takashi Noji,Shota Ueno,Takayuki Kawamata,Masatsune Kato,Yoji Koike		
158116	JPS087114712	not SC	UPd5Al2	U1Pd5Al2	U	1	Pd	5	Al	2																		1	2018							-12.7																			AB2C5		ZrNi2Al5	I4/mmm		A	4.0893		14.628												K					0																																																										mJ/mol.K2	20														uOhm.cm	26.3			55.5							129.3														arc-melting					Localized 5f<2> States in UPd5Al2 and Valence Crossover in the Vicinity of Heavy-Fermion Superconductivity			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 87(2018)114712	Naoto Metoki,Yoshinori Haga,Etsuji Yamamoto,Masaaki Matsuda		
158117	JPS087114712	not SC	ThPd5Al2	Th1Pd5Al2	Th	1	Pd	5	Al	2																		1	2018																										AB2C5		ZrNi2Al5	I4/mmm		A	4.1971		14.682												K					0																																																																																																		arc-melting					Localized 5f<2> States in UPd5Al2 and Valence Crossover in the Vicinity of Heavy-Fermion Superconductivity			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 87(2018)114712	Naoto Metoki,Yoshinori Haga,Etsuji Yamamoto,Masaaki Matsuda		
158118	JPS087114712	not SC	PuPd5Al2	Pu1Pd5Al2	Pu	1	Pd	5	Al	2																		1	2018							-12	5.6																					I4/mmm		A	4.1309		14.803												K					0																																																																																																		arc-melting					Localized 5f<2> States in UPd5Al2 and Valence Crossover in the Vicinity of Heavy-Fermion Superconductivity			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 87(2018)114712	Naoto Metoki,Yoshinori Haga,Etsuji Yamamoto,Masaaki Matsuda		
158119	JPS087114712	not SC	AmPd5Al2	Am1Pd5Al2	Am	1	Pd	5	Al	2																		1	2018							-0.7																						I4/mmm		A	4.1303		14.615												K					0																																																																																																		arc-melting					Localized 5f<2> States in UPd5Al2 and Valence Crossover in the Vicinity of Heavy-Fermion Superconductivity			Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 87(2018)114712	Naoto Metoki,Yoshinori Haga,Etsuji Yamamoto,Masaaki Matsuda		
158120	MSE0310289	SC for 0.3 =< x =< 0.6 in NaxMoS2	Na0.3MoS2	Na0.3Mo1S2	Na	0.3	Mo	1	S	2																		1	1977																											2				A			14.97											A-intercalated MoS2	K		3.6					3.6																				T			5	0.76					T/K			2																																																																					Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158121	MSE0310289	SC for 0.05 =< x =< 0.07 in CaxMoS2	Ca0.05MoS2	Ca0.05Mo1S2	Ca	0.05	Mo	1	S	2																		1	1977																											3				A			18.64											A-intercalated MoS2	K		4					4																				T			2.1	0.65					T/K			1.8																																																																					Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158122	MSE0310289	SC for 0.06 =< x =< 0.1 in SrxMoS2	Sr0.06MoS2	Sr0.06Mo1S2	Sr	0.06	Mo	1	S	2																		1	1977																											2				A			18.62											A-intercalated MoS2	K		5.6					5.6																				T			4.6	1.36					T/K			1.6																																																																					Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158123	MSE0310289		K0.4MoS2	K0.4Mo1S2	K	0.4	Mo	1	S	2																		1	1977																											7				A			16.58											A-intercalated MoS2	K		6.9					6.9																				T				4					T/K			4																																																																					Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158124	MSE0310289		Rb0.3MoS2	Rb0.3Mo1S2	Rb	0.3	Mo	1	S	2																		1	1977																											7				A			17.19											A-intercalated MoS2	K		6.9					6.9																				T				4					T/K			3																																																																					Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158125	MSE0310289		Cs0.3MoS2	Cs0.3Mo1S2	Cs	0.3	Mo	1	S	2																		1	1977																											7				A			19.61											A-intercalated MoS2	K		6.9					6.9																				T			22	3.3					T/K			5		MHC158125																																																																			Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158126	MSE0310289	2H-type MoS2.  not SC	2H-MoS2	Mo1S2	Mo	1	S	2																				1	1977																											7				A			12.29											2H-Mos2	K					0																																																																																																							Physics and Chemistry of MoS2 Intercalation Compounds			NASA Lewis Research Center, Cleveland, Ohio 44135, USA	Mat.Res.Engineering, 31(1977)289	John A. Woollam,Robert B. Somoano		
158127	SST030015005		Eu3-xSrxBi2S4F4	Eu3Bi2S4F4	Eu	3	Bi	2	S	4	F	4																1	2017					my-B/Eu	7.28		2.14																		A2B3C4D4			I4/mmm	139	A	4.0769		32.4358												K			1.5				1.5																																																								mJ/mol.K2	159	SP	203	SP											mOhm.cm	2.406										2.284												EuS,SrS,Bi2S3,EuF2,SrF2		mixture - ground - pellet - sealed in quartz ampoule - heat(1123K, 35h)					Effect of Sr doping in layered Eu3Bi2S4F4 superconductor			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People?s Republic of China	Supercond.Sci.Technol., 30(2017)015005	Pan Zhang,Hui-Fei Zhai,Zhen Wang,Jian Chen,Chun-Mu Feng,Guang-Han Cao,Zhu-An Xu		
158128	SST030015005	SP (beta) = 3.27 mJ/mol.K4	Eu3-xSrxBi2S4F4	Eu2.5Sr0.5Bi2S4F4	Eu	2.5	Sr	0.5	Bi	2	S	4	F	4														1	2017					my-B/Eu	7.19		2.07																		A2B3C4D4			I4/mmm	139	A	4.0724		32.5594												K			0.87				0.87																																																					MSP158128			mJ/mol.K2	214.7	SP	213	SP											mOhm.cm	3.404										3.423												EuS,SrS,Bi2S3,EuF2,SrF2		mixture - ground - pellet - sealed in quartz ampoule - heat(1123K, 35h)					Effect of Sr doping in layered Eu3Bi2S4F4 superconductor			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People?s Republic of China	Supercond.Sci.Technol., 30(2017)015005	Pan Zhang,Hui-Fei Zhai,Zhen Wang,Jian Chen,Chun-Mu Feng,Guang-Han Cao,Zhu-An Xu		
158129	SST030015005		Eu3-xSrxBi2S4F4	Eu2Sr1Bi2S4F4	Eu	2	Sr	1	Bi	2	S	4	F	4														1	2017					my-B/Eu	7.02		1.62																		A2B3C4D4			I4/mmm	139	A	4.0705		32.6309												K			0.48				0.48																																																								mJ/mol.K2	302.3	SP	221	SP											mOhm.cm	1.902										2.178												EuS,SrS,Bi2S3,EuF2,SrF2		mixture - ground - pellet - sealed in quartz ampoule - heat(1123K, 35h)					Effect of Sr doping in layered Eu3Bi2S4F4 superconductor			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People?s Republic of China	Supercond.Sci.Technol., 30(2017)015005	Pan Zhang,Hui-Fei Zhai,Zhen Wang,Jian Chen,Chun-Mu Feng,Guang-Han Cao,Zhu-An Xu		
158130	SST030015005	not SC	Eu3-xSrxBi2S4F4	Eu1Sr2Bi2S4F4	Eu	1	Sr	2	Bi	2	S	4	F	4														1	2017					my-B/Eu	6.58		1.41																		A2B3C4D4			I4/mmm	139	A	4.0681		32.8011												K					0																																																										mJ/mol.K2	338.2	SP	245	SP																																		EuS,SrS,Bi2S3,EuF2,SrF2		mixture - ground - pellet - sealed in quartz ampoule - heat(1123K, 35h)					Effect of Sr doping in layered Eu3Bi2S4F4 superconductor			State Key Lab of Silicon Materials and Department of Physics, Zhejiang University, Hangzhou 310027, People?s Republic of China	Supercond.Sci.Technol., 30(2017)015005	Pan Zhang,Hui-Fei Zhai,Zhen Wang,Jian Chen,Chun-Mu Feng,Guang-Han Cao,Zhu-An Xu		
158131	JPCM0068585	not SC. Tn measured by resistivity anomaly	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		1	1994								9.4																		AB2C2		ThCr2Si2	I4/mmm		A	4.318		10.223												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158132	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xLaxAu2Si2	Ce0.85La0.15Au2Si2	Ce	0.85	La	0.15	Au	2	Si	2																1	1994								7.8																		AB2C2		ThCr2Si2	I4/mmm		A	4.321		10.219												K					0			MLAT158132																																																																																																				Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158133	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xLaxAu2Si2	Ce0.3La0.7Au2Si2	Ce	0.3	La	0.7	Au	2	Si	2																1	1994								4																		AB2C2		ThCr2Si2	I4/mmm		A	4.333		10.225												K					0			MTN158133																																																																																																				Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158134	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xYxSu2Si2	Ce0.95Y0.05Au2Si2	Ce	0.95	Y	0.05	Au	2	Si	2																1	1994								9																		AB2C2		ThCr2Si2	I4/mmm		A	4.317		10.223												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158135	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xYxSu2Si2	Ce0.6Y0.4Au2Si2	Ce	0.6	Y	0.4	Au	2	Si	2																1	1994								6.6																		AB2C2		ThCr2Si2	I4/mmm		A	4.296		10.204												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158136	JPCM0068585	not SC. Tn measured by resistivity anomaly	CeAg2Si2	Ce1Ag2Si2	Ce	1	Ag	2	Si	2																		1	1994								7.3																		AB2C2		ThCr2Si2	I4/mmm		A	4.285		10.552												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158137	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xLaxAg2Si2	Ce0.6La0.4Ag2Si2	Ce	0.6	La	0.4	Ag	2	Si	2																1	1994								4.3																		AB2C2		ThCr2Si2	I4/mmm		A	4.307		10.547												K					0			MLAT158137																																																																																																				Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158138	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xLaxAg2Si2	Ce0.3La0.7Ag2Si2	Ce	0.3	La	0.7	Ag	2	Si	2																1	1994								2.7																		AB2C2		ThCr2Si2	I4/mmm		A	4.312		10.543												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158139	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xYxAg2Si2	Ce0.95Y0.05Ag2Si2	Ce	0.95	Y	0.05	Ag	2	Si	2																1	1994								7.6																		AB2C2		ThCr2Si2	I4/mmm		A	4.28		10.549												K					0																																																																																																							Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158140	JPCM0068585	not SC. Tn measured by resistivity anomaly	Ce1-xYxAg2Si2	Ce0.3Y0.7Ag2Si2	Ce	0.3	Y	0.7	Ag	2	Si	2																1	1994								4.1																		AB2C2		ThCr2Si2	I4/mmm		A	4.247		10.502												K					0			MTN158140																																																																																																				Antiferromagnetis in CeAu2Si2- and CeAg2Si2-based Kondo-lattice systems			Low Temperature Physics Group, Tata Institute of Fundamental Research, Road, Colaba. Bombay400 005, India	J.Phys.: Condens.Matte, 6(1994)8585	C S Garde,J Ray		
158141	NAL0160629	For 0 =< x =<0.4, 2H-phase.	2H-KxMoS2	K0.4Mo1S2	K	0.4	Mo	1	S	2																			2016																																													2H-phase	K				6.9			6.9																																																																																																Liquid ammonia method. Intercalation achieved by immersion of 2H-MoS2 powder in a solution inliquid ammonia at -78 C, various time					Superconductivity in Potassium-Doped Metallic Polymorphs of MoS2			School of Physics and Astronomy, Atmospheric, and Environmental Sciences, University of Manchester, Oxford Road, Manchester M13 9PL, United Kingdom	Nano Lett., 16(2016) 629	Renyan Zhang,I-Ling Tsai,James Chapman,Ekaterina Khestanova,John Waters,Irina V. Grigorieva		
158142	NAL0160629	For 0.4 =< x < 1.0, coexistence of 2H-phase and 1T-KxMoS2. K-concentration x not shown explicitly.	1T-KxMoS2	K0.6Mo1S2	K	0.6	Mo	1	S	2																			2016																																													1T-phase	K				2.8			2.8																																																																																																Liquid ammonia method. Intercalation achieved by immersion of 2H-MoS2 powder in a solution inliquid ammonia at -78 C, various time					Superconductivity in Potassium-Doped Metallic Polymorphs of MoS2			School of Physics and Astronomy, Atmospheric, and Environmental Sciences, University of Manchester, Oxford Road, Manchester M13 9PL, United Kingdom	Nano Lett., 16(2016) 629	Renyan Zhang,I-Ling Tsai,James Chapman,Ekaterina Khestanova,John Waters,Irina V. Grigorieva		
158143	NAL0160629	For 0.8 < x, coexistence of 2H-phase and 1T'-KxMoS2. These two phases continue to higher concentration of 50 at.% K (average ).	1T'-KMoS2	K1Mo1S2	K	1	Mo	1	S	2																			2016																																													1T'-phase	K				4.6			4.6																																																																																																Liquid ammonia method. Intercalation achieved by immersion of 2H-MoS2 powder in a solution inliquid ammonia at -78 C, various time					Superconductivity in Potassium-Doped Metallic Polymorphs of MoS2			School of Physics and Astronomy, Atmospheric, and Environmental Sciences, University of Manchester, Oxford Road, Manchester M13 9PL, United Kingdom	Nano Lett., 16(2016) 629	Renyan Zhang,I-Ling Tsai,James Chapman,Ekaterina Khestanova,John Waters,Irina V. Grigorieva		
158144	PHC5520027	Tc defined as R-onset. T1(R=0) = 91 K estimated from R(T) fig.	H3S	H3S1	H	3	S	1																					2018																										AB3			Im-3m																H3S-phase	K	91		203				147	MTC158144																																																																																															H2S transforms to H3S under high-P(150GPa)  by 3H2S = 2H3S + S process.					Superconductivity and structural studies of highly compressed hydrogen sulfide			KYOKUGEN, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531, Japan	Physica C, 552(2018)27	Mikhail Eremets,Alexander Drozdov,Ivan Troyan,Naohisa Hirao,Saori Kawaguchi,Yasuo Ohishi		
158145	PHC5520027	Tc defined as R-onset.	D3S	D3S1	D	3	S	1																					2018																										AB3			Im-3m																H3S-phase	K			148				148	MTC158144																																																																																															H2S transforms to H3S under high-P(150GPa)  by 3H2S = 2H3S + S process.					Superconductivity and structural studies of highly compressed hydrogen sulfide			KYOKUGEN, Osaka University, 1-3 Machikaneyama, Toyonaka, Osaka 560-8531, Japan	Physica C, 552(2018)27	Mikhail Eremets,Alexander Drozdov,Ivan Troyan,Naohisa Hirao,Saori Kawaguchi,Yasuo Ohishi		
158146	PHI0944219	RRR = 5.64. Yb content of sngle crystals(Ce1-xYbxCoIn5) were corrected by EDS,WDS,TXAS analysis. Tc vs x phse diagram revised using correctef x values	Ce1-xYbxCoIn5	Ce0.95Yb0.05Co1In5	Ce	0.95	Yb	0.05	Co	1	In	5																3	2014																										ABC5		HoCoGa5																		K		2.14					2.14	MTC158146																																																																																															In-flux method in alumina crucible					Resolution of the discrepancy between the variation of the physical properties of Ce1-xYbxCoIn5 single crystals and thin films with Yb composition			Materials Science and Engineering Program, University of California, La Jolla, San Diego, CA 92093, USA	Philos.Mag., 94(2014)4219	S. Jang,B.D. White,I.K. Lum,H. Kim,M.A. Tanatar,W.E. Straszheim,R. Prozorov,T. Keiber,F. Bridges,L. Shu,R.E. Baumbach,M. Janoschek,M.B. Maple		
158147	PHI0944219	RRR = 2.34. Yb content of sngle crystals(Ce1-xYbxCoIn5) were corrected by EDS,WDS,TXAS analysis.  Tc-x phase diagram of previous paper revised after correction of x.	Ce1-xYbxCoIn5	Ce0.8Yb0.2Co1In5	Ce	0.8	Yb	0.2	Co	1	In	5																3	2014																										ABC5		HoCoGa5																		K		1.92					1.92	MTC158147																																																																																															In-flux method in alumina crucible					Resolution of the discrepancy between the variation of the physical properties of Ce1-xYbxCoIn5 single crystals and thin films with Yb composition			Materials Science and Engineering Program, University of California, La Jolla, San Diego, CA 92093, USA	Philos.Mag., 94(2014)4219	S. Jang,B.D. White,I.K. Lum,H. Kim,M.A. Tanatar,W.E. Straszheim,R. Prozorov,T. Keiber,F. Bridges,L. Shu,R.E. Baumbach,M. Janoschek,M.B. Maple		
158148	PHI0944219	RRR = 1.23.	Ce1-xYbxCoIn5	Ce0.6Yb0.4Co1In5	Ce	0.6	Yb	0.4	Co	1	In	5																3	2014																										ABC5		HoCoGa5																		K		1.2					1.2																																																																																																In-flux method in alumina crucible					Resolution of the discrepancy between the variation of the physical properties of Ce1-xYbxCoIn5 single crystals and thin films with Yb composition			Materials Science and Engineering Program, University of California, La Jolla, San Diego, CA 92093, USA	Philos.Mag., 94(2014)4219	S. Jang,B.D. White,I.K. Lum,H. Kim,M.A. Tanatar,W.E. Straszheim,R. Prozorov,T. Keiber,F. Bridges,L. Shu,R.E. Baumbach,M. Janoschek,M.B. Maple		
158149	PRB0292664	not SC. AFM for T < Tn	CeAu2Si2	Ce1Au2Si2	Ce	1	Au	2	Si	2																		1	1984					my-B/mol	1.29		10																		AB2C2		ThCr2Si2	I4/mmm		A	4.32		10.19											a=4.3002, c=10.2106 at T=15 K, a=4.3005, c=10.2116 at T=5K	K					0																																																																																																		arc-melting - ANN(800C, 4-5 days, in vac)					Magnetic ordering in CeMzSiz (M =Ag, Au, Pd, Rh) compounds as studied by neutron diffraction			Physics Department, Brookhaven National Laboratory, Upton, Pew York 11973	Phys.Rev.B, 29(1984)2664	B. H. Grier,J. M. Lawrence,V. Murgai,D. Parks		
158150	PRB0292664	not SC. AFM for T < Tn	CePd2Si2	Ce1Pd2Si2	Ce	1	Pd	2	Si	2																		1	1984					my-B/mol	0.62		10																		AB2C2		ThCr2Si2	I4/mmm		A	4.24		9.88											a=4.2235, c=9.8971 at 15 K, a=4.2231, c=9.8962 at T= 5 K	K					0																																																																																																		arc-melting - ANN(800C, 4-5 days, in vac)					Magnetic ordering in CeMzSiz (M =Ag, Au, Pd, Rh) compounds as studied by neutron diffraction			Physics Department, Brookhaven National Laboratory, Upton, Pew York 11973	Phys.Rev.B, 29(1984)2664	B. H. Grier,J. M. Lawrence,V. Murgai,D. Parks		
158151	PRB0292664	not SC. AFM for T < Tn	CeAg2Si2	Ce1Ag2Si2	Ce	1	Ag	2	Si	2																		1	1984								10																		AB2C2		ThCr2Si2	I4/mmm		A	4.25		10.66											a=4.2330, c=10.6342 at T=15 K	K					0																																																																																																		arc-melting - ANN(800C, 4-5 days, in vac)					Magnetic ordering in CeMzSiz (M =Ag, Au, Pd, Rh) compounds as studied by neutron diffraction			Physics Department, Brookhaven National Laboratory, Upton, Pew York 11973	Phys.Rev.B, 29(1984)2664	B. H. Grier,J. M. Lawrence,V. Murgai,D. Parks		
158152	PRB0292664	not SC. there are two Tn, higher 39 K, lower 27 K.	CeRh2Si2	Ce1Rh2Si2	Ce	1	Rh	2	Si	2																		1	1984								39																		AB2C2		ThCr2Si2	I4/mmm		A	4.09		10.18											a=4.0840, c=1693 at 47.5 K, a=4.0834,c=10.1713 at 32 K, a=4.0828, c=10.1705 at 10K	K					0																																																																																																		arc-melting - ANN(800C, 4-5 days, in vac)					Magnetic ordering in CeMzSiz (M =Ag, Au, Pd, Rh) compounds as studied by neutron diffraction			Physics Department, Brookhaven National Laboratory, Upton, Pew York 11973	Phys.Rev.B, 29(1984)2664	B. H. Grier,J. M. Lawrence,V. Murgai,D. Parks		
158153	MPL0213238	P-induced SC. Two Tn (= 21K and 13.5 K). RRR = 54.  SC properties for P = 5.6 GPa. Tc= 0.696, 0.69, 0.693, 0.646 for P = 5.6, 5.5, 5.4, 4.9 GPa, respectively.	CeCoGe3	Ce1Co1Ge3	Ce	1	Co	1	Ge	3																		1	2007								21																		ABC3	2	BaNiSn3			A	4.319		9.829												K			0.75		0		0.75	MPH158153																			T	RES(onset)	7							T/K	RES(onset)	18			MHC158153		A	from Hc2	70																																	uOhm.cm	1.68																						Ce(3N),Co(4N),Ge(6N)		arc-melting - wrapped in Ta-foil - sealed in quartz tube - ANN(850C,1w)					Non-centrosymmetric heavy Fermion superconductivity in CeCoGe3			Graduate School of Science, Osaka University, Toyonaka, Osaka, Japan	Int'l J.Mod.Phys., 21(2007)3238	R.Settai,Y.Okuda,Y.Haga,H.Harima		
158155	PRB097174505	P-induced SC. Pcr = 8.6 GPa, where Tc(onset) = 25.7 K. T<STR> = 118 K, T<c> = 9.6 GPa. (dT<STR>/dP) = -6.25 K/GPa, P dependence of Hall coeff. measured at 40K	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																3	2018																										ABCD		oxypnictide																	Fe-1111, Tetra- to Ortho- transition at 118 K	K			25.7		0		25.7	MPH158155																																																																																				m3/C						MRH158155					self-flux method					Pressure-induced superconductivity in parent CaFeAsF single crystals			Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China	Phys.Rev.B, 97(2018)174505	Bo Gao,Yonghui Ma,Gang Mu,Hong Xiao		
158156	PRB097174505	P = 21.6 GPa. Hc2(T) = Hc2(0)(1-t)^n, Hc2 = 15-20 T for 18.5 < P < 27.7 GPa.	CaFeAsF	Ca1Fe1As1F1	Ca	1	Fe	1	As	1	F	1																3	2018																										ABCD		oxypnictide																	Fe-1111	K			15.5				15.5																				T	RES(0.9Rn)		15											MHC158156																																																														self-flux method					Pressure-induced superconductivity in parent CaFeAsF single crystals			Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China	Phys.Rev.B, 97(2018)174505	Bo Gao,Yonghui Ma,Gang Mu,Hong Xiao		
158157	PRB098014518	bulk modulus obtained from lattice const. SC, FM , and SC+FM phases investigated using loading and unloading conditions	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																1	2018																		GPa		50.7						ABC4D4		CaRb1144	P4/mmm		A	3.889		13.3213												K		26.6	36.4				26.6	MPH158157																																																																																															See Phys.Rev.B, 93(2016)214503					Superconducting and magnetic phase diagram of RbEuFe4As4 and CsEuFe4As4 at high pressure			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 98(2018)014518	Daniel E. Jackson,Derrick VanGennep,Wenli Bi,Dongzhou Zhang,Philipp Materne,Yi Liu,Guang-Han Cao,Samuel T. Weir,Yogesh K. Vohra,James J. Hamlin		
158158	PRB098014518	bulk modulus obtained from lattice const. SC, FM , and SC+FM phases investigated using loading and unloading conditions	CsEuFe4As4	Cs1Eu1Fe4As4	Cs	1	Eu	1	Fe	4	As	4																1	2018																		GPa		46.3						ABC4D4		CaRb1144	P4/mmm		A	3.9004		13.6357												K		287	33.5				287	MPH158158																																																																																															See Phys.Rev.B, 93(2016)214503					Superconducting and magnetic phase diagram of RbEuFe4As4 and CsEuFe4As4 at high pressure			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 98(2018)014518	Daniel E. Jackson,Derrick VanGennep,Wenli Bi,Dongzhou Zhang,Philipp Materne,Yi Liu,Guang-Han Cao,Samuel T. Weir,Yogesh K. Vohra,James J. Hamlin		
158159	PRB098014518	P-dependence of CsEuFe4As4(#158158) shown in MLAT158159	CsEuFe4As4	Cs1Eu1Fe4As4	Cs	1	Eu	1	Fe	4	As	4																1	2018																										ABC4D4																				K		287	33.5				287	MLAT158159																																																																																															See Phys.Rev.B, 93(2016)214503					Superconducting and magnetic phase diagram of RbEuFe4As4 and CsEuFe4As4 at high pressure			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 98(2018)014518	Daniel E. Jackson,Derrick VanGennep,Wenli Bi,Dongzhou Zhang,Philipp Materne,Yi Liu,Guang-Han Cao,Samuel T. Weir,Yogesh K. Vohra,James J. Hamlin		
158160	PRB098014518	P-dependence of RbEuFe4As4(#158157) shown in MLAT158160	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																1	2018																										ABC4D4																				K		26.6	36.4				26.6	MLAT158160																																																																																															See Phys.Rev.B, 93(2016)214503					Superconducting and magnetic phase diagram of RbEuFe4As4 and CsEuFe4As4 at high pressure			Department of Physics, University of Florida, Gainesville, Florida 32611, USA	Phys.Rev.B, 98(2018)014518	Daniel E. Jackson,Derrick VanGennep,Wenli Bi,Dongzhou Zhang,Philipp Materne,Yi Liu,Guang-Han Cao,Samuel T. Weir,Yogesh K. Vohra,James J. Hamlin		
158161	PRB098024520	P-induced SC.needle crystal. RRR = 330. Hc2(T) = Hc2(0)(1-t^n), n = 1.36. SC data at P = 1.3 GPa. Hc2 has 6-fold angular dependence in bc-plane	CrAs	As1Cr1	As	1	Cr	1																				3	2018																										AB		MnP																	distorted NiAs type at RT	K		1.85			0		1.85																				T	RES(0.5Rn), WHH		1.03						T/K	RES(0.5Rn)		0.77		MHC158161																																					uOhm.cm		1.5																							crystals by Sn-flux method. (Cr:As:Sn = 3:3:20) - in alumina crucible - in quartz tube - heat(650C,8h) - heat(1000C,15h)					Evidence for triplet superconductivity near an antiferromagnetic instability in CrAs			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.B, 98(2018)024520	C. Y. Guo,M. Smidman,B. Shen,W. Wu,F. K. Lin,X. L. Han,Y. Chen,F. Wu,Y. F. Wang,W. B. Jiang,X. Lu,J. P. Hu,J. L. Luo,H. Q. Yuan		
158162	PRB098064506		Pr1-xEuxPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2018																										AB4C12		skutterudite																		K			8.11	7.91			7.91																																																								mJ/mol.K2	73.1	SP	185.2	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158163	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.427 K. SP (beta) = 4.97 mJ/mol.K4	Pr1-xEuxPt4Ge12	Pr0.95Eu0.05Pt4Ge12	Pr	0.95	Eu	0.05	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			7.81	7.41			7.41	MPH158163																																																				MSP158163			mJ/mol.K2	76.39	SP	188.1	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158164	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.488 K.	Pr1-xEuxPt4Ge12	Pr0.9Eu0.1Pt4Ge12	Pr	0.9	Eu	0.1	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			7.62	7.12			7.12																																																								mJ/mol.K2	78.82	SP	187.1	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158165	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.488 K.	Pr1-xEuxPt4Ge12	Pr0.85Eu0.15Pt4Ge12	Pr	0.85	Eu	0.15	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			7.26	6.45			6.45																																																								mJ/mol.K2	75.21	SP	190.2	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158166	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.521 K.	Pr1-xEuxPt4Ge12	Pr0.8Eu0.2Pt4Ge12	Pr	0.8	Eu	0.2	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			6.48	5.77			5.77																																																								mJ/mol.K2	78.39	SP	190.2	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158167	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.613 K.	Pr1-xEuxPt4Ge12	Pr0.7Eu0.3Pt4Ge12	Pr	0.7	Eu	0.3	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			5.28				5.28																																																								mJ/mol.K2	79.7	SP	191	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158168	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.662 K.	Pr1-xEuxPt4Ge12	Pr0.62Eu0.38Pt4Ge12	Pr	0.62	Eu	0.38	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K																																																															mJ/mol.K2	97.83	SP	192	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158169	PRB098064506	Tn = T of SP-peak. Schottky peak = peak-T of Schottky term = 0.645 K.	Pr1-xEuxPt4Ge12	Pr0.5Eu0.5Pt4Ge12	Pr	0.5	Eu	0.5	Pt	4	Ge	12																1	2018																										AB4C12		skutterudite																		K			2.09				2.09																																																								mJ/mol.K2	99.34	SP	195.1	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158170	PRB098064506	Tn = T of SP-peak. second AFM peak appears.	Pr1-xEuxPt4Ge12	Pr0.3Eu0.7Pt4Ge12	Pr	0.3	Eu	0.7	Pt	4	Ge	12																1	2018								1																		AB4C12		skutterudite																		K					0.5			MPH158163																																																							mJ/mol.K2	105.8	SP	198.5	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158171	PRB098064506	Tn = T of SP-peak. second AFM peak appears.	Pr1-xEuxPt4Ge12	Pr0.2Eu0.8Pt4Ge12	Pr	0.2	Eu	0.8	Pt	4	Ge	12																1	2018								1.214																		AB4C12		skutterudite																		K					0.5																																																										mJ/mol.K2	125.9	SP	203.3	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158172	PRB098064506	Tn = T of SP-peak. second AFM peak appears.	Pr1-xEuxPt4Ge12	Pr0.1Eu0.9Pt4Ge12	Pr	0.1	Eu	0.9	Pt	4	Ge	12																1	2018								1.472																		AB4C12		skutterudite																		K					0.5																																																										mJ/mol.K2	131.5	SP	208.5	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158173	PRB098064506	Tn = T of SP-peak. second AFM peak appears.	Pr1-xEuxPt4Ge12	Eu1Pt4Ge12	Eu	1	Pt	4	Ge	12																		1	2018								1.731																		AB4C12		skutterudite																		K					0.5																																																										mJ/mol.K2	216.8	SP	207.6	SP																																				arc-melting, ANN					Short-range antiferromagnetic correlations in the superconducting state of filled skutterudite alloys Pr1-xEuxPt4Ge12			Department of Physics, Kent State University, Kent, Ohio 44242, USA	Phys.Rev.B, 98(2018)064506	R. B. Adhikari,D. L. Kunwar,I. Jeon,M. B. Maple,M. Dzero,C. C. Almasan		
158174	PRB098094504	P<cr> = 21 GPa(Tc goes to zero). R = R0 + AT^n, n = 2.0(P=0), n= 1.5(P=Pc=21 GPa), n=2.0(P=50 GPa)	NdFeAsO0.9F0.1	Nd1Fe1As1F0.1O0.9	Nd	1	Fe	1	As	1	F	0.1													O	0.9		3	2018																										ABCD		oxypnictide																	Fe-1111	K			45.4				45.4	MPH158174		K/GPa	-2.2																																																																			uOhm.cm												448.5		m3/C						MRH158174					single crystals grown from NaCl/KCl flux using  molar ratio of sample:flux = 1:7. crystal size = 70*70*10 micron-m					High-pressure phase diagram of NdFeAsO0.9F0.1: Disappearance of superconductivity on the verge of ferromagnetism from Nd moments			Center for High Pressure Science and Technology Advanced Research, Beijing, 100094, China	Phys.Rev.B, 98(2018)094504	M. Abdel-Hafiez,M. Mito,K. Shibayama,S. Takagi,M. Ishizuka,A. N. Vasiliev,C. Krellner,H. K. Mao		
158175	PRB098094505	TF-muon-SR used for SC properties measurements. Two gaps ( large one in DB, small one is 0.11 meV). large (86%),  small(14%)	LuxZr1-xB12	Lu0.04Zr0.96B12	Lu	0.04	Zr	0.96	B	12																		1	2018																										AB2		AlB2																		K		4.09					4.09																																									um	muon-SR	0.198			meV	0.76		16																																															mixture(amorphous B, Lu2O3, ZrO2) - press into tablets - heat(1650C, in vac) - crush - tablets - heat(1650C) - crush - tablets - SIN(1750C, 1h)					Observation of a crossover from nodal to gapped superconductivity in LuxZr1-xB12			Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 98(2018)094505	Franziska K. K. Kirschner,Nikolay E. Sluchanko,Vladimir B. Filipov,Francis L. Pratt,Chris Baines,Natalya Yu. Shitsevalova,Stephen J. Blundell		
158176	PRB098094505	TF-muon-SR used for SC properties measurements. Two gaps ( large one in DB, small one is 0.135 meV). large (88%),  small(12%)	LuxZr1-xB12	Lu0.07Zr0.93B12	Lu	0.07	Zr	0.93	B	12																		1	2018																										AB2		AlB2																		K		3.64					3.64																																									um	muon-SR	261			meV	0.78		16																																															(crushedsingle crystals of LuB12 & ZrB12) - mix - SIN(1750C, in vac)					Observation of a crossover from nodal to gapped superconductivity in LuxZr1-xB12			Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 98(2018)094505	Franziska K. K. Kirschner,Nikolay E. Sluchanko,Vladimir B. Filipov,Francis L. Pratt,Chris Baines,Natalya Yu. Shitsevalova,Stephen J. Blundell		
158177	PRB098094505	TF-muon-SR used for SC properties measurements. Two gaps ( large one in DB, small one is 0.151 meV). large (90%),  small(10%)	LuxZr1-xB12	Lu0.17Zr0.83B12	Lu	0.17	Zr	0.83	B	12																		1	2018																										AB2		AlB2																		K		3.41					3.41																																									um	muon-SR	0.366			meV	0.66		16																																															mixture(amorphous B, Lu2O3, ZrO2) - press into tablets - heat(1650C, in vac) - crush - tablets - heat(1650C) - crush - tablets - SIN(1750C, 1h)					Observation of a crossover from nodal to gapped superconductivity in LuxZr1-xB12			Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 98(2018)094505	Franziska K. K. Kirschner,Nikolay E. Sluchanko,Vladimir B. Filipov,Francis L. Pratt,Chris Baines,Natalya Yu. Shitsevalova,Stephen J. Blundell		
158178	PRB098094505	TF-muon-SR used for SC properties measurements. Two gaps ( large one in DB, small one is 0.006 meV). large (10%),  small(90%)	LuxZr1-xB12	Lu0.8Zr0.2B12	Lu	0.8	Zr	0.2	B	12																		1	2018																										AB2		AlB2																		K		0.55					0.55																																									um	muon-SR	0.621			meV	0.087		16																																															mixture(amorphous B, Lu2O3, ZrO2) - press into tablets - heat(1650C, in vac) - crush - tablets - heat(1650C) - crush - tablets - SIN(1750C, 1h)					Observation of a crossover from nodal to gapped superconductivity in LuxZr1-xB12			Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 98(2018)094505	Franziska K. K. Kirschner,Nikolay E. Sluchanko,Vladimir B. Filipov,Francis L. Pratt,Chris Baines,Natalya Yu. Shitsevalova,Stephen J. Blundell		
158179	PRB098094519	Thermopower and Thermal conductivity has thermal hysteresis due to structural transition from P3[-]1 to P1[-] at 250 K	Ir1-xRhxTe2	Ir1Te2	Ir	1	Te	2																				1	2018																										AB2		CdI2	P3[-]m1		A	3.9294		5.3974											trigonal symmetry	K					2																																																										mJ/mol.K2	3.77	SP	215	SP	W/K.m	18			MTHC158179	uV/K	2.37			MTP158179																										solid state reaction method					Thermoelectric studies of Ir1-xRhxTe2 (0 =< x =< 0.3)			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)094519	Yu Liu,Hechang Lei,Kefeng Wang,Milinda Abeykoon,J. B. Warren,Emil Bozin,C. Petrovic		
158180	PRB098094519	Thermopower and Thermal conductivity has thermal hysteresis due to structural transition from P3[-]1 to P1[-] at 180 K	Ir1-xRhxTe2	Ir0.9Rh0.1Te2	Ir	0.9	Rh	0.1	Te	2																		1	2018																										AB2		CdI2	P3[-]m1		A	3.9284		5.3945											trigonal symmetry	K					2																																																										mJ/mol.K2	6.47	SP	210	SP	W/K.m	11.6			MTHC158180	uV/K	2.74			MTP158180																										solid state reaction method					Thermoelectric studies of Ir1-xRhxTe2 (0 =< x =< 0.3)			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)094519	Yu Liu,Hechang Lei,Kefeng Wang,Milinda Abeykoon,J. B. Warren,Emil Bozin,C. Petrovic		
158181	PRB098094519		Ir1-xRhxTe2	Ir0.8Rh0.2Te2	Ir	0.8	Rh	0.2	Te	2																		1	2018																										AB2		CdI2	P3[-]m1		A	3.9272		5.3962											trigonal symmetry	K	2.45		2.6				2.525																																																								mJ/mol.K2	8.06	SP	201	SP	W/K.m	15.4			MTHC158181	uV/K	2.95			MTP158181																										solid state reaction method					Thermoelectric studies of Ir1-xRhxTe2 (0 =< x =< 0.3)			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)094519	Yu Liu,Hechang Lei,Kefeng Wang,Milinda Abeykoon,J. B. Warren,Emil Bozin,C. Petrovic		
158182	PRB098094519	not SC for T > 2 K.	Ir1-xRhxTe2	Ir0.7Rh0.3Te2	Ir	0.7	Rh	0.3	Te	2																		1	2018																										AB2		CdI2	P3[-]m1		A	3.9255		5.3927											trigonal symmetry	K					2																																																										mJ/mol.K2	8.6	SP	198	SP	W/K.m	13.5			MTHC158182	uV/K	3.12			MTP158182																										solid state reaction method					Thermoelectric studies of Ir1-xRhxTe2 (0 =< x =< 0.3)			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)094519	Yu Liu,Hechang Lei,Kefeng Wang,Milinda Abeykoon,J. B. Warren,Emil Bozin,C. Petrovic		
158183	PRB098094525	Einstein T of As-Pd atomic pairs = 220 K.  SC in BaPd2As2 comes from structural instability. CeMg2Si2 type sample not SC.	BaPd2As2	Ba1Pd2As2	Ba	1	Pd	2	As	2																		1	2018																										AB2C2		ThCr2Si2																		K			3.85				3.85	MLAT158183																																																																																															heat treatment in quartz tube					Temperature-dependent local structure and superconductivity of BaPd2As2 and SrPd2As2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 98(2018)094525	K. Terashima,E. Paris,L. Simonelli,E. Salas-Colera,A. Puri,T. Wakita,Y. Yamada,S. Nakano,H. Idei,K. Kudo,M. Nohara,Y. Muraoka,T. Mizokawa,T. Yokoya,N. L. Saini		
158184	PRB098094525	Einstein T = 265 K from EXAFS analysis	SrPd2As2	Sr1Pd2As2	Sr	1	Pd	2	As	2																		1	2018																										AB2C2		ThCr2Si2																		K			0.92				0.92	MLAT158184																																																										265	EXAFS																																				heat treatment in quartz tube					Temperature-dependent local structure and superconductivity of BaPd2As2 and SrPd2As2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 98(2018)094525	K. Terashima,E. Paris,L. Simonelli,E. Salas-Colera,A. Puri,T. Wakita,Y. Yamada,S. Nakano,H. Idei,K. Kudo,M. Nohara,Y. Muraoka,T. Mizokawa,T. Yokoya,N. L. Saini		
158185	PRB098094525	Einstein T = 276 K from EXAFS analysis	CaPd2As2	Ca1Pd2As2	Ca	1	Pd	2	As	2																		1	2018																										AB2C2		ThCr2Si2																		K			1.27				1.27																																																											276	EXAFS																																				heat treatment in quartz tube					Temperature-dependent local structure and superconductivity of BaPd2As2 and SrPd2As2			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan	Phys.Rev.B, 98(2018)094525	K. Terashima,E. Paris,L. Simonelli,E. Salas-Colera,A. Puri,T. Wakita,Y. Yamada,S. Nakano,H. Idei,K. Kudo,M. Nohara,Y. Muraoka,T. Mizokawa,T. Yokoya,N. L. Saini		
158186	PRB098104503	(dC/Tc) = 0.21 J/mol.K2. gama estimated assuming  (dC/gamma*Tc) = 1.43(BCS). k<GL> = 108, 67 for <ab> and <c> direction, Anisotropy = 1.7. magnetic data  shows for H//ab.	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																3	2018	emu/mol.G	0.034	K/mol.G	7.476	my-B/Eu	7.75	24.18	15																		ABC4D4		CaRb1144	P4/mmm		A	3.882		13.273												K			36.8	36.8			36.8																				T	RES(0.9Rn), linear approx.		250	160					T/K	RES(0.9Rn)		7	4.2	MHC158186		nm	from Hc2		1.4	0.92													MSP158186			mJ/mol.K2	147	SP																																						single crystals grown using RbAs flux method. crystal sze= 0.8*0.8*60 micron-m					Anisotropic superconductivity and magnetism in single-crystal RbEuFe4As4			Materials Science Division, Argonne National Laboratory, 9700 S. Cass Avenue, Argonne, Illinois 60439, USA	Phys.Rev.B, 98(2018)104503	M. P. Smylie,K. Willa,J.-K. Bao,K. Ryan,Z. Islam,H. Claus,Y. Simsek,Z. Diao,A. Rydh,A. E. Koshelev,W.-K. Kwok,D. Y. Chung,M. G. Kanatzidis,U. Welp		
158187	PRB098104506	demag(N = 0.25), RRR =1.04, Debye-T = 300K from R(T). SP (beta) = 0.232 mJ/mol.K4, (delta) = 0.44 uJ/mol.K6. Energy gap = 0.72 meV, penet = 599 nm, M* = 14.5 m<e>  from muon-SR. Hc(0) = 58.9 mT.	Re3Ta	Re3Ta1	Re	3	Ta	1																				1	2018																										AB3		alpha-Mn	I4[-]3m		A	9.6907														K	4.6	4.65	4.7	4.68			4.65											mT	M-H curve	2.13							T	WHH,	7.3							T/K	RES	2.25			MHC158187		nm	from Hc2	6.71			nm	from Hc1	588			meV	0.742	3.68	14				MSP158187			mJ/mol.K2	13.1	SP	321	SP											uOhm.cm	248.52																						Re(4N),Ta(5N)		arc-melting(tri-arc furnace) - ANN(800C,1w, in quartz tube, vac)					Superconducting and normal-state properties of the noncentrosymmetric superconductor Re3Ta			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 98(2018)104506	J. A. T. Barker,B. D. Breen,R. Hanson,A. D. Hillier,M. R. Lees,G. Balakrishnan,D. McK. Paul,R. P. Singh		
158188	PRB098134506	Two phases (nondimerized ( P3[-]m1) and dimerized(P1[-] phaseusing atomic pair distribution function (PDF) method. dimerized phase (SG = P1[1]) = 25%.	Ir1-xRhxTe2	Ir0.88Rh0.12Te2	Ir	0.88	Rh	0.12	Te	2																		1	2018																										AB2			P3[-m1																space group = P1[-]	K								MPH158188																																																																																															mixture - pellet - alumina crucible - sealed in quartz tube - SIN(1000C,15h)					Phase separation at the dimer-superconductor transition in Ir1-xRhxTe2			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)134506	R. Yu,S. Banerjee,H. Lei,M. Abeykoon,C. Petrovic,Z. Guguchia,E. S. Bozin		
158189	PRB098134506		Ir1-xRhxTe2	Ir0.8Rh0.2Te2	Ir	0.8	Rh	0.2	Te	2																		1	2018																										AB2			P3[-m1																	K								MTC158188																																																																																															mixture - pellet - alumina crucible - sealed in quartz tube - SIN(1000C,15h)					Phase separation at the dimer-superconductor transition in Ir1-xRhxTe2			Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA	Phys.Rev.B, 98(2018)134506	R. Yu,S. Banerjee,H. Lei,M. Abeykoon,C. Petrovic,Z. Guguchia,E. S. Bozin		
158190	PRB098134512	SP (dC/Tc) = 10 mJ/mol.K. Spin fluctuation effect disappears at x<cr> = 0.17 and conventional SC appears for x > X<cr>.	Cr0.8Ru0.2	Cr0.8Ru0.2	Cr	0.8	Ru	0.2																				3	2018																										A																				K		1.35	1.54				1.35	MPH158190																																																				MSP158190			mJ/mol.K2	6.2																																							arc-zoning method. as-cast ingot - alumina Bridgman crucible - heat(1700C, in vac) - heat(1900C9. withdrawn from heat zone at a rate of 5mm/h					Suppression of antiferromagnetic spin fluctuations in superconducting Cr0.8Ru0.2			Physics Engineering Department, Istanbul Technical University, 34469, Maslak, Istanbul, Turkey	Phys.Rev.B, 98(2018)134512	M. Ramazanoglu,B. G. Ueland,D. K. Pratt,L. W. Harriger,J. W. Lynn,G. Ehlers,G. E. Granroth,S. L. Bud'ko,P. C. Canfield,D. L. Schlagel,A. I. Goldman,T. A. Lograsso,R. J. McQueeney		
158191	PRB098140506	T<CDW> = 490 K. CDW anomaly = 20 J/mol.K.	EuRbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																3	2018																										ABC4D4		CaRb1144																		K			36.5				36.5	MGAP158191																																								nm	far infrared reflectivity	420			cm(-1)	80	3.17	2																																																				Unique interplay between superconducting and ferromagnetic orders in EuRbFe4As4			Moscow Institute of Physics and Technology, Dolgoprudny, Moscow 141700, Russia	Phys.Rev.B, 98(2018)140506	V. S. Stolyarov,A. Casano,M. A. Belyanchikov,A. S. Astrakhantseva,S. Yu. Grebenchuk,D. S. Baranov,I. A. Golovchanskiy,I. Voloshenko,E. S. Zhukova,B. P. Gorshunov,A. V. Muratov,V. V. Dremov,L. Ya. Vinnikov,D. Roditchev,Y. Liu,G.-H. Cao,M. Dressel,E. Uykur		
158193	NATP0130967	T<CDW> = 318 K. SP (beta) = 1.13 mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt2In1	Lu	1	Pt	2	In	1																		1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.45					0.45																																																					MSP158195			mJ/mol.K2	4.29	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158194	NATP0130967	T<CDW> = 155 K. SP (beta) = 1.02 mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt1.6Pd0.4In1	Lu	1	Pt	1.6	Pd	0.4	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.42					0.42	MCDW158193																																																							mJ/mol.K2	4.43	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158195	NATP0130967	T<CDW> = 80.3 K. SP (beta) = 1.12 mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt1.2Pd0.8In1	Lu	1	Pt	1.2	Pd	0.8	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.67					0.67																																																					MSP158195			mJ/mol.K2	5.09	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158196	NATP0130967	T<CDW> = 68.6 K. SP (beta) = 1.55 mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt0.96Pd1.04In1	Lu	1	Pt	0.96	Pd	1.04	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		1					1	MGAM158196																																																				MSP158195			mJ/mol.K2	5.63	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158197	NATP0130967	SP (beta) = 1.54 mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt0.92Pd1.08In1	Lu	1	Pt	0.92	Pd	1.08	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		1.103					1.103	MTC158197																																																				MSP158195			mJ/mol.K2	5.89	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158198	NATP0130967	SP (beta) = 1.46  mJ/mol.K4. T<CDW> = 0 for x = 0.58 where Tc = 1.10 K (max) and SC volume fraction = 80 %.	Lu(Pt1-xPdx)2In	Lu1Pt0.88Pd1.12In1	Lu	1	Pt	0.88	Pd	1.12	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		1.109					1.109	MBET158198																																																				MSP158199			mJ/mol.K2	5.96	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158199	NATP0130967	SP (beta) = 0.667  mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt0.72Pd1.28In1	Lu	1	Pt	0.72	Pd	1.28	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.903					0.903																																																					MSP158199			mJ/mol.K2	6.37	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158200	NATP0130967	SP (beta) = 0.857  mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt0.6Pd1.4In1	Lu	1	Pt	0.6	Pd	1.4	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.822					0.822																																																					MSP158199			mJ/mol.K2	6.07	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158201	NATP0130967	SP (beta) = 0.634  mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pt0.4Pd1.6In1	Lu	1	Pt	0.4	Pd	1.6	In	1																1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K		0.399					0.399																																																								mJ/mol.K2	6.29	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158202	NATP0130967	not SC down to 0.35 K (Tc < 0.35 K).  SP (beta) = 0.462  mJ/mol.K4.	Lu(Pt1-xPdx)2In	Lu1Pd2In1	Lu	1	Pd	2	In	1																		1	2017																										ABC2			L2<1>																cubic Heusler, RT2X type	K					0.35																																																							MSP158199			mJ/mol.K2	6.18	SP																																						arc-melting					Charge density wave quantum critical point with strong enhancement of superconductivity			Max Planck Institute for Chemical Physics of Solids, Nothnitzer Strasse 40, 01187 Dresden, Germany	Nat.Physics, 13(2017)967	Thomas Gruner,Dongjin Jang,Zita Huesges,Raul Cardoso-Gil,Gerhard H. Fecher,Michael M. Koza,Oliver Stockert,Andrew P. Mackenzie,Manuel Brando,Christoph Geibel		
158203	PRL109186402		CeCo(In,Sn,Hg)5	Ce1Co1In4.91Sn0.09	Ce	1	Co	1	In	4.91	Sn	0.09																1	2012																										ABC5		HoCoGa5																		K		1.19					1.19																																																																																																					Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158204	PRL109186402		CeCo(In,Sn,Hg)5	Ce1Co1In4.9095Sn0.0899Hg0.025	Ce	1	Co	1	In	4.9095	Sn	0.0899	Hg	0.025														1	2012																										ABC5		HoCoGa5																		K		1.24					1.24	MPH158204																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158205	PRL109186402		CeCo(In,Sn,Hg)5	Ce1Co1In4.8488Sn0.0889Hg0.062	Ce	1	Co	1	In	4.8488	Sn	0.0889	Hg	0.062														1	2012								1.27																		ABC5		HoCoGa5																		K		0.77					0.77																																																																																																					Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158206	PRL109186402		CeCo(In,Sn,Hg)5	Ce1Co1In4.7867Sn0.0877Hg0.126	Ce	1	Co	1	In	4.7867	Sn	0.0877	Hg	0.126														1	2012								2.88																		ABC5		HoCoGa5																		K					0																																																																																																							Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158207	PRL109186402		Ce(Co,Pt)(In,Hg)5	Ce1Co0.91Pt0.09In5	Ce	1	Co	0.91	Pt	0.09	In	5																1	2012																										ABC5		HoCoGa5																		K		1.11					1.11																																																																																																					Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158208	PRL109186402		Ce(Co,Pt)(In,Hg)5	Ce1Co0.91Pt0.09In4.975Hg0.025	Ce	1	Co	0.91	Pt	0.09	In	4.975	Hg	0.025														1	2012																										ABC5		HoCoGa5																		K		1.41					1.41																																																																																																					Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158209	PRL109186402		Ce(Co,Pt)(In,Hg)5	Ce1Co0.91Pt0.09In4.962Hg0.038	Ce	1	Co	0.91	Pt	0.09	In	4.962	Hg	0.038														1	2012																										ABC5		HoCoGa5																		K		1.36					1.36	MPH158209																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158210	PRL109186402		Ce(Co,Pt)(In,Hg)5	Ce1Co0.91Pt0.09In4.938Hg0.062	Ce	1	Co	0.91	Pt	0.09	In	4.938	Hg	0.062														1	2012								1.42																		ABC5		HoCoGa5																		K		1.56					1.56																																																																																																					Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158211	PRL109186402		Ce(Co,Pt)(In,Hg)5	Ce1Co0.91Pt0.09In4.85Hg0.15	Ce	1	Co	0.91	Pt	0.09	In	4.85	Hg	0.15														1	2012								4.13																		ABC5		HoCoGa5																		K					0																																																																																																							Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158212	PRL109186402		CeCo(In,Sn)5	Ce1Co1In4.972Sn0.028	Ce	1	Co	1	In	4.972	Sn	0.028																1	2012																										ABC5		HoCoGa5																		K			1.93				1.93																																																																							uOhm.cm	3																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158213	PRL109186402		CeCo(In,Sn)5	Ce1Co1In4.91Sn0.09	Ce	1	Co	1	In	4.91	Sn	0.09																1	2012																										ABC5		HoCoGa5																		K			1.22				1.22																																																																							uOhm.cm	5.52																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158214	PRL109186402		CeCo(In,Sn)5	Ce1Co1In4.85Sn0.15	Ce	1	Co	1	In	4.85	Sn	0.15																1	2012																										ABC5		HoCoGa5																		K			0.44				0.44																																																																							uOhm.cm	8.62																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158215	PRL109186402		CeCo(In,Sn)5	Ce1Co1In4.821Sn0.179	Ce	1	Co	1	In	4.821	Sn	0.179																1	2012																										ABC5		HoCoGa5																		K					0																																																																									uOhm.cm	9.73																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158216	PRL109186402	T2 shows Tc from C(T).	Ce(Co,Pt)In5	Ce1Co1In5	Ce	1	Co	1	In	5																		1	2012																										ABC5		HoCoGa5																		K		2.31	2.29				2.31																																																																							uOhm.cm	1.83																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158217	PRL109186402	T2 shows Tc from C(T).	Ce(Co,Pt)In5	Ce1Co0.96Pt0.04In5	Ce	1	Co	0.96	Pt	0.04	In	5																1	2012																										ABC5		HoCoGa5																		K		1.76	1.74				1.76																																																																							uOhm.cm	2.49																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158218	PRL109186402	T2 shows Tc from C(T).	Ce(Co,Pt)In5	Ce1Co0.91Pt0.09In5	Ce	1	Co	0.91	Pt	0.09	In	5																1	2012																										ABC5		HoCoGa5																		K		1.05	1.09				1.05																																																																							uOhm.cm	5																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158219	PRL109186402		Ce(Co,Pt)In5	Ce1Co0.83Pt0.17In5	Ce	1	Co	0.83	Pt	0.17	In	5																1	2012																										ABC5		HoCoGa5																		K			0.28				0.28																																																																							uOhm.cm	7.51																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158220	PRL109186402		Ce(Co,Pt)In5	Ce1Co0.78Pt0.22In5	Ce	1	Co	0.78	Pt	0.22	In	5																1	2012																										ABC5		HoCoGa5																		K					0																																																																									uOhm.cm	8.33																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158221	PRL109186402		Ce(Co,Pt)In5	Ce1Co0.74Pt0.26In5	Ce	1	Co	0.74	Pt	0.26	In	5																1	2012																										ABC5		HoCoGa5																		K					0																																																																									uOhm.cm	11.2																													Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158222	PRL109186402		CeCoIn-xCdx	Ce1Co1In5	Ce	1	Co	1	In	5																		1	2012																										ABC5		HoCoGa5																		K		2.26					2.26	MTC158222																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158223	PRL109186402		CeCoIn-xCdx	Ce1Co1In4.95Cd0.05	Ce	1	Co	1	In	4.95	Cd	0.05																1	2012																										ABC5		HoCoGa5																		K		1.83					1.83	MTC158223																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158224	PRL109186402		CeCoIn-xCdx	Ce1Co1In4.925Cd0.075	Ce	1	Co	1	In	4.925	Cd	0.075																1	2012																										ABC5		HoCoGa5																		K		0.44					0.44	MTC158224																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158225	PRL109186402		CeCoIn-xCdx	Ce1Co1In4.9Cd0.1	Ce	1	Co	1	In	4.9	Cd	0.1																1	2012																										ABC5		HoCoGa5																		K					0.4			MTC158225																																																																																																				Electronic Tuning and Uniform Superconductivity in CeCoIn5			Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA	Phys.Rev.Lett., 109(2012)186402	K. Gofryk,F. Ronning,J.-X. Zhu,,M. N. Ou,P. H. Tobash,S. S. Stoyko,X. Lu,A. Mar,T. Park,E. D. Bauer,J. D. Thompson,Z. Fisk		
158226	PRL114027003	T-dependence of penet(London) measured by tunnel diode resonator (TDR). penet(0) not given. d[penet] = A*T^n, n = 2 for all doping	Ce1-xLaxCoIn5	Ce0.98La0.02Co1In5	Ce	0.98	La	0.02	Co	1	In	5																3	2015																										ABC5		HoCoGa5																		K				2.1			2.1	MTC158226																																																																																															single crystals grown by In-flux method.,					Nodal to Nodeless Superconducting Energy-Gap Structure Change Concomitant with Fermi-Surface Reconstruction in the Heavy-Fermion Compound CeCoIn5			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 114(2015)027003	Hyunsoo Kim,M. A. Tanatar,R. Flint,C. Petrovic,Rongwei Hu,B. D. White,I. K. Lum,M. B. Maple,R. Prozorov		
158227	PRL114027003	T-dependence of penet(London) measured by tunnel diode resonator (TDR). penet(0) not given. d[penet] = A*T^n, n = 2 for all doping	Ce1-xNdxCoIn5	Ce0.98Nd0.02Co1In5	Ce	0.98	Nd	0.02	Co	1	In	5																3	2015																										ABC5		HoCoGa5																		K				2.01			2.01	MTC158227																																																																																															single crystals grown by In-flux method.,					Nodal to Nodeless Superconducting Energy-Gap Structure Change Concomitant with Fermi-Surface Reconstruction in the Heavy-Fermion Compound CeCoIn5			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 114(2015)027003	Hyunsoo Kim,M. A. Tanatar,R. Flint,C. Petrovic,Rongwei Hu,B. D. White,I. K. Lum,M. B. Maple,R. Prozorov		
158228	PRL114027003	T-dependence of penet(London) measured by tunnel diode resonator (TDR). penet(0) not given. d[penet] = A*T^n, n = 2 for x =< 0.002, n>2 for x >=0.015	Ce1-xYbxCoIn5	Ce0.985Yb0.015Co1In5	Ce	0.985	Yb	0.015	Co	1	In	5																3	2015																										ABC5		HoCoGa5																		K				2.03			2.03	MTC158228																																																																																															single crystals grown by In-flux method.,					Nodal to Nodeless Superconducting Energy-Gap Structure Change Concomitant with Fermi-Surface Reconstruction in the Heavy-Fermion Compound CeCoIn5			Ames Laboratory and Department of Physics & Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.Lett., 114(2015)027003	Hyunsoo Kim,M. A. Tanatar,R. Flint,C. Petrovic,Rongwei Hu,B. D. White,I. K. Lum,M. B. Maple,R. Prozorov		
158229	PRL121037004	P-induced SC. Tc = 1.04 K at Pc= 86 GPa.Tc measured by R(T) (dR/dT)-max to zero line, and SUS(real part of ac-SUS. dTc/dH = 1.3 mK/Oe for 116 GPa.	Yb	Yb1	Yb	1																						1	2018																										A	1																		fcc, at RT, P=0. for P = 202 GPa, hexagonal	K	1.04				0		1.04	MTC158229																																																																																															thin square shaped Yb (3N)					Pressure-Induced Superconductivity in Elemental Ytterbium Metal			Department of Physics, Washington University, St. Louis, Missouri 63130, USA	Phys.Rev.Lett., 121(2018)037004	J. Song,G. Fabbris,W. Bi,D. Haskel,J. S. Schilling		
158230	PRX008031017	P-induced SC. Tc(max) = 1.62 K (DB) atP =  9.4 kbar. P<cr> = 10 kbar (Tn = 0). R(T)-R0= A*T^1.5, A=1.55E-3 uOhm.cm/K2 & n = 1.91.	CrAs1-xPx	As1Cr1	As	1	Cr	1																				3	2018								265																		AB		MnP			A		3.4591	6.189											a-axis value not given	K					0			MPH158230																																																							mJ/mol.K2	8.21	SP																																						Sn-flux method					Evolution of Magnetic Double Helix and Quantum Criticality near a Dome of Superconductivity in CrAs			Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev. X, 8(2018)031017	M. Matsuda,F. K. Lin,R. Yu,J.-G. Cheng,W. Wu,J. P. Sun,J. H. Zhang,P. J. Sun,K. Matsubayashi,T. Miyake,T. Kato,J.-Q. Yan,M. B. Stone,Qimiao Si,J. L. Luo,Y. Uwatoko		
158231	PRX008031017	R(T)-R0= A*T^1.5, A=4.93E-3 uOhm.cm/K2 & n = 1.63.	CrAs1-xPx	Cr1As0.965P0.035	Cr	1	As	0.965	P	0.035																		3	2018								244																		AB		MnP			A		3.4367	6.2075											a-axis value not given	K					10																																																										mJ/mol.K2	7.59	SP																																						Sn-flux method					Evolution of Magnetic Double Helix and Quantum Criticality near a Dome of Superconductivity in CrAs			Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev. X, 8(2018)031017	M. Matsuda,F. K. Lin,R. Yu,J.-G. Cheng,W. Wu,J. P. Sun,J. H. Zhang,P. J. Sun,K. Matsubayashi,T. Miyake,T. Kato,J.-Q. Yan,M. B. Stone,Qimiao Si,J. L. Luo,Y. Uwatoko		
158232	PRX008031017	no anomaly in R(T), AFM not appears.  R(T)-R0= A*T^1.5, A=12.8E-3 uOhm.cm/K2 & n = 1.58.	CrAs1-xPx	Cr1As0.95P0.05	Cr	1	As	0.95	P	0.05																		3	2018																										AB		MnP			A		3.416	6.2158											a-axis value not given	K					10																																																										mJ/mol.K2	32.2	SP																																						Sn-flux method					Evolution of Magnetic Double Helix and Quantum Criticality near a Dome of Superconductivity in CrAs			Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev. X, 8(2018)031017	M. Matsuda,F. K. Lin,R. Yu,J.-G. Cheng,W. Wu,J. P. Sun,J. H. Zhang,P. J. Sun,K. Matsubayashi,T. Miyake,T. Kato,J.-Q. Yan,M. B. Stone,Qimiao Si,J. L. Luo,Y. Uwatoko		
158233	PRX008031017	R(T)-R0= A*T^1.5, A=18.4E-3 uOhm.cm/K2 & n = 1.79.	CrAs1-xPx	Cr1As0.9P0.1	Cr	1	As	0.9	P	0.1																		3	2018																										AB		MnP																		K					10																																																										mJ/mol.K2	29.6	SP																																						Sn-flux method					Evolution of Magnetic Double Helix and Quantum Criticality near a Dome of Superconductivity in CrAs			Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev. X, 8(2018)031017	M. Matsuda,F. K. Lin,R. Yu,J.-G. Cheng,W. Wu,J. P. Sun,J. H. Zhang,P. J. Sun,K. Matsubayashi,T. Miyake,T. Kato,J.-Q. Yan,M. B. Stone,Qimiao Si,J. L. Luo,Y. Uwatoko		
158234	PRX008031017	R(T)-R0= A*T^1.5, A=26.7E-3 uOhm.cm/K2 & n = 1.95.	CrAs1-xPx	Cr1As0.8P0.2	Cr	1	As	0.8	P	0.2																		3	2018																										AB		MnP																		K					10																																																										mJ/mol.K2	26.7	SP																																						Sn-flux method					Evolution of Magnetic Double Helix and Quantum Criticality near a Dome of Superconductivity in CrAs			Neutron Scattering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA	Phys.Rev. X, 8(2018)031017	M. Matsuda,F. K. Lin,R. Yu,J.-G. Cheng,W. Wu,J. P. Sun,J. H. Zhang,P. J. Sun,K. Matsubayashi,T. Miyake,T. Kato,J.-Q. Yan,M. B. Stone,Qimiao Si,J. L. Luo,Y. Uwatoko		
158235	SCIA0047969	demag N = 0.504. Hc(0) = 169 mT. H(P) = 10.7 T.  GL(kappa) = 48. beta(SP) = 0.178 mJ/mol.K4. (dC/gamma*Tc) = 1.56. DOS = 1.52 states/eV.fu	TaRh2B2	Ta1Rh2B2	Ta	1	Rh	2	B	2																		1	2018																										AB2C2			P3<1>	144	A	4.6994		8.766												K				5.8			5.8											mT	M-H curve, demag-correction	9.56							T	RES(0.5Rn), WHH	11.7							T/K	RES(0.5Rn)	2.91			MHC158235		A	from Hc2	53			A	Hc1	2580			meV	0.98	3.98	14							mJ/mol.K2	5.8	SP	379	SP																																		Ta(3N),Nb(3N),Rh(3N),B		mixture(Ta(Nb):Rh:B=1:1.9:2.1) - pellet - heat(1200C,6h) - arc-melting - ANN(1100C,1w, in silica tube)					TaRh2B2 and NbRh2B2: Superconductors with a chiral noncentrosymmetric crystal structure			Department of Chemistry, Princeton University, Princeton, NJ 08544, USA.	Sci.Advances, 4(2018)7969	Elizabeth M. Carnicom,Weiwei Xie,Tomasz Klimczuk,Jingjing Lin,Karolina Gornicka,Zuzanna Sobczak,Nai Phuan Ong,Robert J. Cava		
158236	SCIA0047969	demag N = 0.448. Hc(0) = 248 mT. H(P) = 14.1 T.  GL(kappa) = 51. beta(SP) = 0.203 mJ/mol.K4. (dC/gamma*Tc) = 1.60. DOS = 2.21 states/eV.fu	NbRh2B2	Nb1Rh2B2	Nb	1	Rh	2	B	2																		1	2018																										AB2C2			P3<1>	144	A	4.716		8.749												K				7.6			7.6											mT	M-H curve, demag-correction	13.5							T	RES(0.5Rn), WHH	18							T/K	RES(0.5Rn)	3.42			MHC158236		A	from Hc2	43			A	Hc1	2190			meV	1.4	4.28	14							mJ/mol.K2	8.8	SP	362	SP																																		Ta(3N),Nb(3N),Rh(3N),B		mixture(Ta(Nb):Rh:B=1:1.9:2.1) - pellet - heat(1200C,6h) - arc-melting - ANN(1100C,1w, in silica tube)					TaRh2B2 and NbRh2B2: Superconductors with a chiral noncentrosymmetric crystal structure			Department of Chemistry, Princeton University, Princeton, NJ 08544, USA.	Sci.Advances, 4(2018)7969	Elizabeth M. Carnicom,Weiwei Xie,Tomasz Klimczuk,Jingjing Lin,Karolina Gornicka,Zuzanna Sobczak,Nai Phuan Ong,Robert J. Cava		
158237	SCICM0600083	Jc(2 K, H=0) = 2.2E+5 A/cm2 from M-H hysteresis and Bean's model	RbCa2Fe4As4F2	Rb1Ca2Fe4As4F2	Rb	1	Ca	2	Fe	4	As	4	F	2														1	2017																										AB2C2D4E4			I4/mmm	139	A	3.8716		31.667											12442-structure type	K			30.5	30.5			30.5										90										T	RES(0.9Rn)								T/K	RES(0.9Rn)	13.9			MHC158237																																																												Rb(2N),Cs(2N),Ca(2N),Fe(4N8),As(5N),CaF2		solid state reaction. mixture - alumina tube, Ta-tube - quartz ampoule - heat(1203 K,5h)					Crystal structure and superconductivity at about 30 K in ACa2Fe4As4F2 (A = Rb, Cs)			Department of Physics and Stat Key Lab of Silicon Materials, Zhejiang University, Hangzhou 310027, China	Sci.China Mater., 60(2017)83	ZhichengWang,Chaoyang He,Zhangtu Tang,Siqi Wu,Guanghan Cao		
158238	SCICM0600083	Jc(2 K, H=0) = 5.2E+5 A/cm2 from M-H hysteresis and Bean's model	CsCa2Fe4As4F2	Cs1Ca2Fe4As4F2	Cs	1	Ca	2	Fe	4	As	4	F	2														1	2017																										AB2C2D4E4			I4/mmm	139	A	3.8807		32.363											12442-structure type	K			28.5	28.2			28.2										65										T	RES(0.9Rn)								T/K	RES(0.9Rn)	14.2			MHC158238																																																												Rb(2N),Cs(2N),Ca(2N),Fe(4N8),As(5N),CaF2		solid state reaction. mixture - alumina tube, Ta-tube - quartz ampoule - heat(1203 K,5h)					Crystal structure and superconductivity at about 30 K in ACa2Fe4As4F2 (A = Rb, Cs)			Department of Physics and Stat Key Lab of Silicon Materials, Zhejiang University, Hangzhou 310027, China	Sci.China Mater., 60(2017)83	ZhichengWang,Chaoyang He,Zhangtu Tang,Siqi Wu,Guanghan Cao		
158239	SCICM0600083		KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2														1	2017																										AB2C2D4E4			I4/mmm	139	A	3.8684		31.007											12442-structure type	K																																																																																																					Rb(2N),Cs(2N),Ca(2N),Fe(4N8),As(5N),CaF2		solid state reaction. mixture - alumina tube, Ta-tube - quartz ampoule - heat(1203 K,5h)					Crystal structure and superconductivity at about 30 K in ACa2Fe4As4F2 (A = Rb, Cs)			Department of Physics and Stat Key Lab of Silicon Materials, Zhejiang University, Hangzhou 310027, China	Sci.China Mater., 60(2017)83	ZhichengWang,Chaoyang He,Zhangtu Tang,Siqi Wu,Guanghan Cao		
158240	SST031055012	Sr3SnO shows Tc = 3.7 K , due to excess Sn	Sr3-xSnO	Sr3Sn1O1	Sr	3	Sn	1																	O	1		1	2018																										ABC3																				K					2																																																																																																Sr(3N)		starting composition (3.0Sn + SnO) using Sr(3N), alumina crucible -  heat(800C,3h, in quartz tube(vac))					Controlled synthesis of the antiperovskite oxide superconductor Sr3-xSnO			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Supercond.Sci.Technol., 31(2018)055012	J N Hausmann,M Oudah,A Ikeda,S Yonezawa,Y Maeno		
158241	SST031055012	using 99.9 % Sn	Sr3-xSnO	Sr2.5Sn1O1	Sr	2.5	Sn	1																	O	1		1	2018																										ABC3																				K				4.7			4.7																																																																																														Sr(3N)		starting composition (2.5Sn + SnO) using Sr(3N), alumina crucible -  heat(825C,3h, in quartz tube(30 kPa-Ar))					Controlled synthesis of the antiperovskite oxide superconductor Sr3-xSnO			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Supercond.Sci.Technol., 31(2018)055012	J N Hausmann,M Oudah,A Ikeda,S Yonezawa,Y Maeno		
158242	SST031055012	using 99.99 % Sn	Sr3-xSnO	Sr2.5Sn1O1	Sr	2.5	Sn	1																	O	1		1	2018																										ABC3					A	5.137		12.097											Sr2.5SnO phase	K				5.4			5.4																																																																																														Sr(4N)		starting composition (2.5Sn + SnO) using Sr(4N), alumina crucible -  heat(825C,3h, in quartz tube(30 kPa-Ar))					Controlled synthesis of the antiperovskite oxide superconductor Sr3-xSnO			Department of Physics, Graduate School of Science, Kyoto University, Kyoto 606-8502, Japan	Supercond.Sci.Technol., 31(2018)055012	J N Hausmann,M Oudah,A Ikeda,S Yonezawa,Y Maeno		
158243	SST031065001	e-ph = 0.67. DOS = 3.02 states/eV. T<CDW> = 73.1 K from R(T) anomaly.	2H-PdxTaS2	Pd0.01Ta1S2	Pd	0.01	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3142		12.113											hexagonal , distorted 2H-structure	K				3.02			3.02																																																								mJ/mol.K2	12.62	SP	192.2	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158244	SST031065001	e-ph = 0.71. DOS = 3.70 states/eV. T<CDW> = 72.7 K from R(T) anomaly.	2H-PdxTaS2	Pd0.02Ta1S2	Pd	0.02	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3149		12.1214											hexagonal , distorted 2H-structure	K			3.93	3.95			3.95																																																								mJ/mol.K2	14.94	SP	210.8	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158245	SST031065001	e-ph = 0.72. DOS = 4.06 states/eV. T<CDW> = 71.4 K from R(T) anomaly.	2H-PdxTaS2	Pd0.03Ta1S2	Pd	0.03	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3143		12.1249											hexagonal , distorted 2H-structure	K			4.14	4.12			4.12																																																					MSP158245			mJ/mol.K2	16.47	SP	210.3	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158247	SST031065001	e-ph = 0.70. DOS = 3.93 states/eV. T<CDW> = 65.5 K from R(T) anomaly.	2H-PdxTaS2	Pd0.05Ta1S2	Pd	0.05	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3151		12.1343											hexagonal , distorted 2H-structure	K			3.87	3.89			3.89																																																					MSP158247			mJ/mol.K2	15.85	SP	212.8	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158248	SST031065001	e-ph = 0.69. DOS = 3.86 states/eV.	2H-PdxTaS2	Pd0.06Ta1S2	Pd	0.06	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3154		12.1465											hexagonal , distorted 2H-structure	K			3.67	3.73			3.73	MPH158246																																																							mJ/mol.K2	15.41	SP	214.9	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158249	SST031065001	e-ph = 0.65. DOS = 3.84 states/eV.	2H-PdxTaS2	Pd0.08Ta1S2	Pd	0.08	Ta	1	S	2																		1	2018																										AB2			P31c	159	A	3.3155													hexagonal , distorted 2H-structure	K			2.97	3			3																																																								mJ/mol.K2	14.98	SP	215.1	SP																																		Pd(4N),Ta(3N),S(2N5)		mixture - pellet - sealed in quartz tube(vac) - heat(923K,2d) - air quenched to RT - reground - pellet - sealed in quartz tube - heat(1023K, 2d) - ANN(923K,2w) - Q to RT					Superconductivity in palladium-doped 2H-TaS2			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)065001	M H Zhou,X C Li,C Dong		
158250	PHB5360767	Debye-T = 256 K from R(T) anlysis.  (dC/gamma*Tc) = 1.6	YCo2Ge2	Y1Co2Ge2	Y	1	Co	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.9705		10.098												K			0.4				0.4																																																								mJ/mol.K2	11.7	SP	331	SP											uOhm.cm	53.1						53.1																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158251	PHB5360767	Debye-T = 173 K from R(T) anlysis.	YNi2Ge2	Y1Ni2Ge2	Y	1	Ni	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.04504		9.7978												K					0.4																																																										mJ/mol.K2	13.7	SP	295	SP											uOhm.cm	18.8						18.8																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158252	PHB5360767	Debye-T = 224 K from R(T) anlysis.	YRu2Ge2	Y1Ru2Ge2	Y	1	Ru	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.2289		9.8372												K					0.4																																																										mJ/mol.K2	7.9	SP	298	SP											uOhm.cm	57.2						57.2																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158253	PHB5360767	Debye-T = 235 K from R(T) anlysis.	YRh2Ge2	Y1Rh2Ge2	Y	1	Rh	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.10212		10.2618												K					0.4																																																										mJ/mol.K2	6.9	SP	305	SP											uOhm.cm	63						63																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158254	PHB5360767	Debye-T = 169 K from R(T) anlysis.  (dC/gamma*Tc) = 1.7	YPd2Ge2	Y1Pd2Ge2	Y	1	Pd	2	Ge	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.2387		10.0305												K	1.1						1.1																																																					MSP158254			mJ/mol.K2	6.6	SP	231	SP											uOhm.cm	13.7						13.7																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158255	PHB5360767	Debye-T = 123 K from R(T) anlysis.  (dC/gamma*Tc) = 1.6	YPt2Ge2	Y1Pt2Ge2	Y	1	Pt	2	Ge	2																		1	2018																										AB2C2		CaBe2Ge2	P4/mmm		A	4.27		9.906												K	1.6						1.6																																																					MSP158255			mJ/mol.K2	5.9	SP	195	SP											uOhm.cm	26.2						26.2																		arc-melting. pellet - wrapped in Mo-foil - ANN(1273 K, 2w, in silica tube)					Superconductivity in YTE Ge 2 2 compounds (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)767	G. Chajewski,M. Samsel?Czeka?a,A. Hackemer,P. Wisniewski,A.P. Pikul,D. Kaczorowski		
158256	SCIB0630952	Pauli limit Hp = 19.1 T. (dC/gamma*Tc) = 1.54	K2Mo3As3	K2Mo3As3	K	2	Mo	3	As	3																		1	2018																										A2B3C3			P-6m2	187	A	10.145		4.453											Cr-233 type	K	10.1		10.4			0.3	10.25																				T	RES(on), GL approx.	22												MHC158256																						mJ/mol.K2	13	SP	234	SP											mOhm.cm							2.26				4.1												K(2N),M0(3N5),As(5N)		mixture(K:Mo:As = 2.5:3:3) - alumina crucible - heat(523 K,20h) - cool to RT - reground - pellet - (Ta-tube with cap (welding))  - sealed in quartz tube - SIN(1123K,50h) - furnace cool  to RT					Superconductivity at 10.4 K in a novel quasi-one-dimensional ternary molybdenum pnictide K2Mo3As3			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Science Bulletin, 63(2018)952	Qing-Ge Mu,Bin-Bin Ruan,Kang Zhao,Bo-Jin Pan,Tong Liu,Lei Shan,Gen-Fu Chen,Zhi-An Ren		
158257	JPS087084708	Isostructure of NpPd5Al2. Crystalline electric field (CEF) measured by neutron inelastic scattering(NIS)	NdPd5Al2	Nd1Pd5Al2	Nd	1	Pd	5	Al	2																		1	2018					Myu-B	2.7		1.2																		AB2C5		ZrNi2Al5	I4/mmm																Isostructure of NpPd5Al2	K					0.3																																																																																																Nd(3N),Pd(3N5),Al(5N)		arc-melting. As-grown sample - sandwiched between Al-foil and fixed in Al can.					Neutron Inelastic Scattering Study of the f-Electron States in NdPd5Al2			Materials Sciences Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Phys.Soc.Jpn, 87(2018)084708	Naoto Metoki,Hiroki Yamauchi,Hiroyuki S. Suzuki,Hideaki Kitazawa,Kazuya Kamazawa,Kazuhiko Ikeuchi,Ryoichi Kajimoto,Mitsutaka Nakamura,Yasuhiro Inamura		
158300	PRL106177001	SP measured for 0.04 < T < 300 K. AFQ ordering T = 0.11 K  defined as peak in C(T). Curie-Weiss for T > 20 K. M measured for H//[110], H//[100]	PrIr2Zn20	Pr1Ir2Zn20	Pr	1	Ir	2	Zn	20																		3	2011					my-B/f.u	3.49																				AB2C20		CeCr2Al20	Fd3[-]m																	K				0.05			0.05	MPH158300																																																				MSP158300																																											melt growth method					Antiferroquadrupolar Ordering in a Pr-Based Superconductor PrIr2Zn20			Department of Quantum Matter, Graduate School of Advanced Sciences of Matter, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Phys.Rev.Lett., 106(2011)177001	T. Onimaru,K. T. Matsumoto,Y. F. Inoue,K. Umeo,T. Sakakibara,Y. Karaki,M. Kubota,T. Takabatake		
158301	JAC6941149	RRR = 1.4. Curie-Weiss for T < 200 K. SP (beta) = 0.995 mJ/mol.K4	Ba2Ti2Cr2As4O	Ba2Ti2Cr2As4O1	Ba	2	Ti	2	Cr	2	As	4													O	1			2017	emu/mol	0.0016	emu.K/mol	0.0758	my-B/f.u	0.778	-5.7	350																		AB2C2D2E4		oxypnictide	I4/mmm	139	A	4.0391		27.8474											22241-type	K					2																																																										mJ/mol.K2	99.6	SP	277.78	SP											mOhm.cm							0.304				0.43												Ba,Ti,As,Cr,TiO2,all 3N		mixture - in alumina ampoule - heat(1253K,1500 min, in quartz tube - cool to RT - SIN(1273K,1500 min)					Synthesis, crystal structure and physical properties of a new oxypnictide Ba2Ti2Cr2As4O containing [Ti2As2O]<2-> and [Cr2As2]<2-> layers			Department of Physics, Zhejiang University, Hangzhou 310027, China	J.Alloys Compd., 694(2017)1149	Abduweli Ablimit,Yun-Lei Sun,Hao Jiang,Jin-Ke Bao,Hui-Fei Zhai,Zhang-Tu Tang,Yi Liu,Zhi-Cheng Wang,Chun-Mu Feng,Guang-Han Cao		
158302	ACTM1660543	heat(1370 K,4.0 GPa, 2 h)	LaxRh4P12	La0.59Rh4P12	La	0.59	Rh	4	P	12																			2019																										AB4C12		skutterudite			A	8.0569														K	3.55	4.58	5.87				4.58																																																																																														La(3N),Rh(3N),P(5N)		mixture(La:Rh:P = 1:4:12) - loaded in BN capsule - pressurize to 4.0 - 9.4 Gpa at RT - heat(1370 K,2h)					Superconductivity in filled skutterudite LaxRh4P12 (0.5 < x =< 1): Experimental and computational studies			Research Center for Functional Materials, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0048, Japan	Acta Materialia, 166(2019)543	Motoharu Imai,Masao Arai,Takashi Taniguchi		
158303	ACTM1660543	heat(1470 K,4.0 GPa, 2 h)	LaxRh4P12	La0.69Rh4P12	La	0.69	Rh	4	P	12																			2019																										AB4C12		skutterudite			A	8.0621														K	6.15	8.07	10.37				8.07	MTC158303																																																																																													La(3N),Rh(3N),P(5N)		mixture(La:Rh:P = 1:4:12) - loaded in BN capsule - pressurize to 4.0 - 9.4 Gpa at RT - heat(1370 K,2h)					Superconductivity in filled skutterudite LaxRh4P12 (0.5 < x =< 1): Experimental and computational studies			Research Center for Functional Materials, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0048, Japan	Acta Materialia, 166(2019)543	Motoharu Imai,Masao Arai,Takashi Taniguchi		
158304	ACTM1660543	heat(1370 K, 5.5 GPa, 2 h)	LaxRh4P12	La0.75Rh4P12	La	0.75	Rh	4	P	12																			2019																										AB4C12		skutterudite			A	8.0719														K	7.84	8.71	9.65				8.71																																																																																														La(3N),Rh(3N),P(5N)		mixture(La:Rh:P = 1:4:12) - loaded in BN capsule - pressurize to 4.0 - 9.4 Gpa at RT - heat(1370 K,2h)					Superconductivity in filled skutterudite LaxRh4P12 (0.5 < x =< 1): Experimental and computational studies			Research Center for Functional Materials, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0048, Japan	Acta Materialia, 166(2019)543	Motoharu Imai,Masao Arai,Takashi Taniguchi		
158305	ACTM1660543	heat(1470 K,7.7 GPa, 2 h)	LaxRh4P12	La0.81Rh4P12	La	0.81	Rh	4	P	12																			2019																										AB4C12		skutterudite			A	8.0737														K	9.25	9.81	10.39				9.81																																																																																														La(3N),Rh(3N),P(5N)		mixture(La:Rh:P = 1:4:12) - loaded in BN capsule - pressurize to 4.0 - 9.4 Gpa at RT - heat(1370 K,2h)					Superconductivity in filled skutterudite LaxRh4P12 (0.5 < x =< 1): Experimental and computational studies			Research Center for Functional Materials, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0048, Japan	Acta Materialia, 166(2019)543	Motoharu Imai,Masao Arai,Takashi Taniguchi		
158306	ACTM1660543	heat(1470 K, 9.4 GPa, 2 h)	LaxRh4P12	La0.99Rh4P12	La	0.99	Rh	4	P	12																			2019																										AB4C12		skutterudite			A	8.0787														K	16.19	16.41	16.49				16.41																																																																																														La(3N),Rh(3N),P(5N)		mixture(La:Rh:P = 1:4:12) - loaded in BN capsule - pressurize to 4.0 - 9.4 Gpa at RT - heat(1370 K,2h)					Superconductivity in filled skutterudite LaxRh4P12 (0.5 < x =< 1): Experimental and computational studies			Research Center for Functional Materials, National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki, 305-0048, Japan	Acta Materialia, 166(2019)543	Motoharu Imai,Masao Arai,Takashi Taniguchi		
158307	APP1311036	Lu behaves like non-magnetic impurities. (dTc/dx) = 0.12 K/at% Lu.	Zr1-xLuxB12	Zr0.96Lu0.04B12	Zr	0.96	Lu	0.04	B	12																		3	2017																												UB12																		K				5.47			5.47	MTC158307																																																																																															single crystals made by floating zone method in an inert gas atmosphere					Superconductivity in LuxZr1-xB12 Dodecaborides with Cage-Glass Crystal Structure			Prokhorov General Physics Institute, RAS, Vavilov Str. 38, 119991 Moscow, Russia	ACTA Phys.Polonica A, 131(2017)1036	N. Sluchanko,A. Azarevich,A. Bogach,S. Gavrilkin,V. Glushkov,S. Demishev,K. Mitsen,N. Shitsevalova,V. Filippov,S. Gabani,K. Flachbart		
158308	APP1311036		Zr1-xLuxB12	Zr0.8Lu0.2B12	Zr	0.8	Lu	0.2	B	12																		3	2017																												UB12																		K				3.9			3.9																																																																																																single crystals made by floating zone method in an inert gas atmosphere					Superconductivity in LuxZr1-xB12 Dodecaborides with Cage-Glass Crystal Structure			Prokhorov General Physics Institute, RAS, Vavilov Str. 38, 119991 Moscow, Russia	ACTA Phys.Polonica A, 131(2017)1036	N. Sluchanko,A. Azarevich,A. Bogach,S. Gavrilkin,V. Glushkov,S. Demishev,K. Mitsen,N. Shitsevalova,V. Filippov,S. Gabani,K. Flachbart		
158309	APP1311036	Lu behaves like magnetic impurities. (dTc/dx) = 0.21 K/at% Lu.	Zr1-xLuxB12	Zr0.993Lu0.007B12	Zr	0.993	Lu	0.007	B	12																		3	2017																												UB12																		K				5.81			5.81	MTC158307																																																																																															single crystals made by floating zone method in an inert gas atmosphere					Superconductivity in LuxZr1-xB12 Dodecaborides with Cage-Glass Crystal Structure			Prokhorov General Physics Institute, RAS, Vavilov Str. 38, 119991 Moscow, Russia	ACTA Phys.Polonica A, 131(2017)1036	N. Sluchanko,A. Azarevich,A. Bogach,S. Gavrilkin,V. Glushkov,S. Demishev,K. Mitsen,N. Shitsevalova,V. Filippov,S. Gabani,K. Flachbart		
158310	APP1311036		Zr1-xLuxB12	Zr0.926Lu0.074B12	Zr	0.926	Lu	0.074	B	12																		3	2017																												UB12																		K				4.49			4.49																																																																																																single crystals made by floating zone method in an inert gas atmosphere					Superconductivity in LuxZr1-xB12 Dodecaborides with Cage-Glass Crystal Structure			Prokhorov General Physics Institute, RAS, Vavilov Str. 38, 119991 Moscow, Russia	ACTA Phys.Polonica A, 131(2017)1036	N. Sluchanko,A. Azarevich,A. Bogach,S. Gavrilkin,V. Glushkov,S. Demishev,K. Mitsen,N. Shitsevalova,V. Filippov,S. Gabani,K. Flachbart		
158313	EPL12027006	RRR = 2.3. Centrosymmetric. Hc2 = 57.4 T from WHH fitting.	RbCr3As3	Rb1Cr3As3	Rb	1	Cr	3	As	3																		3	2017																										AB3C3			P6<3>/m	176	A	9.373		4.203											hexagonal	K			7.3	6.2			6.2										100										T	RES(on), GL fitting			72.4										MHC158313																																																												RbAs,CrAs		single crystal Rb2Cr3As3 by high-T solution growth method. Deintercalating Rb by immersing in dehydrated ethanol (1 week) - ANN(273 K, 10h)					Superconductivity at 7.3 K in the 133-type Cr-based RbCr3As3 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences - Beijing 100190, China	Europhys.Lett., 120(2017)27006	Tong Liu,Qing-Ge Mu,Bo-Jin Pan,Jia Yu,Bin-Bin Ruan,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
158314	EPL12347004	RRR = 3.7. Anomaly in R(T) at 193 K, maybe CDW. S-wave full gaped SC from thermal conductivity.  R = R0 + A*T^n where n = 3.5  for 2 < T<10K	NaSn2As2	Na1Sn2As2	Na	1	Sn	2	As	2																		3	2018																										AB2C2	2		R3[-]/m																	K	1.48		1.6				1.54																				T	RES(on), GL fitting		0.54	0.22										MHC158314																			MSP158314			mJ/mol.K2	1.9	SP	218	SP	mW/cm.K2				MTHC158314						uOhm.cm							60.3																As(5N),Na(4N),Sn(5N)		Sn-flux method. Mixture(Na:Sn:As = 1:10:2) - im alumina crucible in quartz tube - heat(750C, 3d) - cool (1.5 K/h) - remove Sn flux at 350 C					Nodeless superconductivity in the SnAs-based van der Waals-type superconductor NaSn2As2			State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University - Shanghai 200433, China	Europhys.Lett., 123(2018)47004	E. J. Cheng,J. M. Ni,F. Q. Meng,T. P. Ying,B. L. Pan,Y. Y. Huang,Darren C. Peets,Q. H. Zhang,S. Y. Li		
158315	EPL12357001	H dependence of  C<e> obtained by subtract lattice and Schottky type SP terms. SP (beta = 1.45 mJ/mol.K4. (dC/gamma*Tc) = 2.5.	K2Cr3As3	K2Cr3As3	K	2	Cr	3	As	3																		3	2018																										A2B3C3		K2Cr3As3																		K				6.1			6.1																				T	SP, WHH fitting	32.2												MHC158315														15.7	14				MSP158315			mJ/mol.K2	71	SP	221	SP																																				self-flux method					Evidence of line nodes in superconducting gap function in K2Cr3As3 from specific-heat measurements			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences Beijing 100190, China	Europhys.Lett., 123(2018)57001	Y. T. Shao,X. X. Wu,L. Wang,Y. G. Shi,J. P. Hu,J. L. Luo		
158316	JAC4640047	not SCCurie-Weiss law for T > 200 K.	UPd5Al2	U1Pd5Al2	U	1	Pd	5	Al	2																		2	2008					my-B/U	3.4	-13																			AB2C5		ZrNi2Al5	I4/mmm	123	A	4.1693		14.629												K					4																																																																																																		poly crystal. Arc melting					Crystal structure and magnetic properties of the new ternary actinide compounds AnPd5Al2 (An =U, Np)			Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Alloys Compd., 464(2008)47	Y. Haga,D. Aoki,Y. Homma,S. Ikeda,T.D. Matsuda,E. Yamamoto,H. Sakai,N. Tateiwa,N.D. Dung,A. Nakamura,Y. Shiokawa,Y. Onuki		
158317	JAC4640047	Curie-Weiss law for T > 50 K. H//[110]	NpPd5Al2	Np1Pd5Al2	Np	1	Pd	5	Al	2																		2	2008					my-B/Np	3.22	-42																			AB2C5		ZrNi2Al5	I4/mmm	123	A	4.148		14.716												K				5			5																																																																																																Pb flux method					Crystal structure and magnetic properties of the new ternary actinide compounds AnPd5Al2 (An =U, Np)			Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan	J.Alloys Compd., 464(2008)47	Y. Haga,D. Aoki,Y. Homma,S. Ikeda,T.D. Matsuda,E. Yamamoto,H. Sakai,N. Tateiwa,N.D. Dung,A. Nakamura,Y. Shiokawa,Y. Onuki		
158318	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Gd0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7Gd0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	Gd	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.799		12.046												K	75		102	61		27	61																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158319	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Er0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7Er0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	Er	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.791		12.022												K	60		98	50		38	50																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158320	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7La0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7La0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	La	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.774		12.051												K	50		83	50		33	50																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158321	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Li0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7Li0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	Li	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.766		12.081												K	89		100	92		11	92																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158322	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Na0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7Na0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	Na	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.757		12.092												K	72		93	93		21	93																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158323	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7K0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7K0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	K	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.761		12.095												K	81		94	86		13	86																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158324	JAC7720745	Major= CSCO , Minor = 1212  , Minor = 1201  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Rb0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl0.7Rb0.3Sr2Ca0.8Cr0.2Cu2O7	Tl	0.7	Rb	0.3	Sr	2	Ca	0.8	Cr	0.2	Cu	2									O	7			2019																										Tl-1212		Tl1212			A	3.785		12.056												K	82		100	84		18	84																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158325	JAC7720745	Major= 1212 , Minor = 1201  , Minor = CSCO  , CSCO = Ca0.3Sr0.7CuO2	(Tl0.7Tl0.3)Sr2Ca0.8Cr0.2Cu2O7	Tl1Sr2Ca0.8Cr0.2Cu2O7	Tl	1	Sr	2	Ca	0.8	Cr	0.2	Cu	2											O	7			2019																										Tl-1212		Tl1212			A	3.787		12.086												K	96		104	102		8	102																																																																																																An appropriate ammount of Tl2O3 (excess 10%) was added to the precursor, mixed, pressed.  Heat(1000C, 5min, in flowing O2) - furnace cool to RT.					Effects of rare-earth elements and alkali metals on the superconductivity of (Tl0.7M0.3)Sr2Ca0.8Cr0.2Cu2O7 with M = Gd, Er, La, Li, Na, K, and Rb			School of Applied Physics, Universiti Kebangsaan Malaysia, 43600, Bangi, Selangor, Malaysia	J.Alloys Compd., 772(2019)745	Ilhamsyah Putra Abu Bakar,R. Abd-Shukor		
158326	JAC7730034	There are two humps in R(T). T'(low), T''(high).. They depend on P. T' depends on heating or cooling	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		3	2019																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K	2.7						2.7	MTC158326		K/Gpa	0.07																T	RES(zero), WHH	1.03							T/K	RES(zero)	0.55			MHC158326																																																														single crystals grown by using flux (Sn-excess)					Pressure effects on the structural and superconducting transitions in La3Co4Sn13			Centro de Ciencias Naturais e Humanas, Universidade Federal do ABC, 09210-170, Santo Andre, SP, Brazil	J.Alloys Compd., 773(2019)34	L. Mendonca-Ferreira,F.B. Carneiro,M.B. Fontes,E. Baggio-Saitovitch,L.S.I. Veiga,J.R.L. Mardegan,J. Strempfer,M.M. Piva,R.D. dos Reis,E.M. Bittar		
158327	JAC7730034	P = 2.53 G Pa	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		3	2019																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K	2.87						2.87	MTST158327																			T	RES(zero), WHH	1.04							T/K	RES(zero)	0.52			MHC158326																																																														single crystals grown by using flux (Sn-excess)					Pressure effects on the structural and superconducting transitions in La3Co4Sn13			Centro de Ciencias Naturais e Humanas, Universidade Federal do ABC, 09210-170, Santo Andre, SP, Brazil	J.Alloys Compd., 773(2019)34	L. Mendonca-Ferreira,F.B. Carneiro,M.B. Fontes,E. Baggio-Saitovitch,L.S.I. Veiga,J.R.L. Mardegan,J. Strempfer,M.M. Piva,R.D. dos Reis,E.M. Bittar		
158328	JAC7820170	Tn by C(T).. dC = 170 mJ/mol.K. (beta) = 3.66 mJ/mol.K4. Curie-Weis law for T>75 K. Curie-T = 19.1 K, moment = 4.17 my-B, for H//c. DB for H//ab.  Anisotropy(hc2) = 2.6 at 0 K.	NdPdxBi2	Nd1Pd0.77Bi2	Nd	1	Pd	0.77	Bi	2																		3	2019					my-B	3.23	-148	4																		ABC2			P4/nmm	129	A	4.515		9.509												K		3.2					3.2																				T	RES(0.9Rn), WHH		6.2	2.4										MHC158328		nm	from Hc2		18.6	7.3													MSP158328			mJ/mol.K2	300	SP	127	SP																																		La,Pd,Bi		mixture(La:Pd:Bi) = 1:1:10) - in alumina crucible - sealed in quartz tube - heat(1273 K,10 h, in vac) - cool to 973 K (5K/h) - cool to RT - remove flux at 673 K.					Synthesis and thermodynamic properties of superconducting NdPd1- dBi2 (d~0.23) single crystals			Department of Physics, Soochow University, Suzhou, 215006, China	J.Alloys Compd.,782(2019)170	F.M. Zhang,W. Zhou,C.Q. Xu,S.W. Liu,J.Y. Zhang,M. Xia,Xiaofeng Xu,B. Qian		
158329	JPCL0090868	vol = 197.67 A3. RRR = 5.8	(La,Na)RbFe4As4	La0.4Na0.6Rb1Fe4As4	La	0.4	Na	0.6	Rb	1	Fe	4	As	4															2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8606		13.2624												K	25		26.4	25.5			25.5																				T	RES(mid), WHH	98							T/K	RES(mid)	5.464			MHC158329		A	from Hc2	18																																																								LaAs,Aas(A=Na,Rb,Cs),FeAs,Fe2As		mixture with 5% excess Aas using stainless steel pipe - heat(860-890 C, 2h) - quench to RT					Superconductivity in a New 1144-Type Family of (La,Na)AFe4As4 (A = Rb or Cs)			IMRA Material R&D Co., Ltd., 2-1 Asahi-machi, Kariya, Aichi 448-0032, Japan	J.Phys.Chem.Lett., 9(2018)868	Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Yoshiyuki Yoshida,Hiroshi Eisaki,Hiraku Ogino,Akira Iyo		
158330	JPCL0090868	RRR = 5.6	(La,Na)CsFe4As4	La0.4Cs0.6Rb1Fe4As4	La	0.4	Cs	0.6	Rb	1	Fe	4	As	4															2018																										ABC4D4		CaRb1144	P4/mmm	123																K	23		24.8	24			24																				T	RES(mid), WHH	82							T/K	RES(mid)	4.841			MHC158329		A	from Hc2	20																																																								LaAs,Aas(A=Na,Rb,Cs),FeAs,Fe2As		mixture with 5% excess Aas using stainless steel pipe - heat(860-890 C, 2h) - quench to RT					Superconductivity in a New 1144-Type Family of (La,Na)AFe4As4 (A = Rb or Cs)			IMRA Material R&D Co., Ltd., 2-1 Asahi-machi, Kariya, Aichi 448-0032, Japan	J.Phys.Chem.Lett., 9(2018)868	Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Kunihiro Kihou,Yoshiyuki Yoshida,Hiroshi Eisaki,Hiraku Ogino,Akira Iyo		
158331	JPCM030475603	T<CDW> = 106.7 K from Tthermo power, = 109.8 K from thermal cond..	LaPt2Si2	La1Pt2Si2	La	1	Pt	2	Si	2																		1	2018																										AB2C2		CaBe2Ge2	P4/nmm																	K		1.22					1.22																																																													W/m.K	2.87			MTHC158331	uV/K	-8.52			MTP158331																								La(3N),Pr(3N),Pt(3N),Si(6N)		arc-melting - ANN(1000C,7 d, in vac)					Thermal transport studies on charge density wave materials LaPt2Si2 and PrPt2Si2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.Condens.Matter, 30(2018)475603	Ritu Gupta,K P Rajeev,Z Hossain		
158332	JPCM030475603	T<CDW> = 86.9 K  from thermal cond..	PrPt2Si2	Pr1Pt2Si2	Pr	1	Pt	2	Si	2																		1	2018																										AB2C2		CaBe2Ge2	P4/nmm																	K					0																																																															W/m.K	3.05			MTHC158332	uV/K	-10.15			MTP158332																								La(3N),Pr(3N),Pt(3N),Si(6N)		arc-melting - ANN(1000C,7 d, in vac)					Thermal transport studies on charge density wave materials LaPt2Si2 and PrPt2Si2			Department of Physics, Indian Institute of Technology, Kanpur 208016, India	J.Phys.Condens.Matter, 30(2018)475603	Ritu Gupta,K P Rajeev,Z Hossain		
158333	JPCM030475802	ThO2 less than 3.2 wt%. SP (beta) = 1.65 mJ/mol.K4. (dC) = 108 mJ/mol.K at Tc.  (dC/gamma*Tc) = 1.23. e-ph = 0.53. k(GL) = 20.	Th7Ni3	Ni3Th7	Ni	3	Th	7																				1	2018	cm3/mol	0.00176			my-B/mol	0.018	-1.4																			A3B7		Fe3Th7			A	9.89		6.23												K		1.94		1.96		0.04	1.94										97	Oe					30			1.73	T	SP, GL fitting	1.24			0.08			1.73						MHC158333		nm	from Hc2	16.3			nm		32.6					2.69	14				MSP158333			mJ/mol.K2	45.3	SP	227.8	SP																																		Th(2N8),Ni(4N)		arc-melting - stoichiometric ratio (Th:Ni = 7:3) - arc melting  several times					Superconducting-state properties and electronic band structure calculations of a noncentrosymmetric Th7Ni3 compound			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, PO Box 1410, 50-422 Wroc?aw, Poland	J.Phys.Condens.Matter, 30(2018)475802	R Idczak,M Sahakyan,V H Tran		
158334	JPCS969012027	magnetic transition Tm = 15 K defined as  kink in SUS(T).	(Eu,Ca)RbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																1	2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8899		13.307												K				36.78			36.78																																																																																																solid state reaction using stainless steel pipe and cap method					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type Structure			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys: Conf.Ser., 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y.Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo		
158335	JPCS969012027	magnetic transition Tm = 12 K defined as  kink in SUS(T).	(Eu,Ca)RbFe4As4	Eu0.75Ca0.25Rb1Fe4As4	Eu	0.75	Ca	0.25	Rb	1	Fe	4	As	4														1	2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8874		13.279												K				36.54			36.54	MTC158335																																																																																															solid state reaction using stainless steel pipe and cap method					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type Structure			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys: Conf.Ser., 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y.Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo		
158336	JPCS969012027	magnetic transition Tm = 7 K defined as  kink in SUS(T).	(Eu,Ca)RbFe4As4	Eu0.5Ca0.5Rb1Fe4As4	Eu	0.5	Ca	0.5	Rb	1	Fe	4	As	4														1	2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8846		13.231												K				36.49			36.49																																																																																																solid state reaction using stainless steel pipe and cap method					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type Structure			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys: Conf.Ser., 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y.Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo		
158337	JPCS969012027		(Eu,Ca)RbFe4As4	Eu0.25Ca0.75Rb1Fe4As4	Eu	0.25	Ca	0.75	Rb	1	Fe	4	As	4														1	2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8811		13.181												K				36			36																																																																																																solid state reaction using stainless steel pipe and cap method					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type Structure			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys: Conf.Ser., 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y.Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo		
158338	JPCS969012027		(Eu,Ca)RbFe4As4	Ca1Rb1Fe4As4	Ca	1	Rb	1	Fe	4	As	4																1	2018																										ABC4D4		CaRb1144	P4/mmm	123	A	3.8773		13.109												K				36.26			36.26																																																																																																solid state reaction using stainless steel pipe and cap method					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type Structure			IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J.Phys: Conf.Ser., 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y.Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo		
158339	JPS0720017	not SC	Cr1-xRux	Cr0.841Ru0.159	Cr	0.841	Ru	0.159																				1	2003								283																																						K					0.45																																																																									uOhm.cm							42.4							m3/C						MRH158339					arc-melting - ANN(1500C, 150 h, in sealed W crucible					Competition of Antiferromagnetism and Superconductivity in Cr-Ru Alloys			Department of Physics, Tohoku University Aoba, Aoba-ku, Sendai 980-8578	J.Phys.Soc.Jpn, 72(2003)17	K. CHATANI,Y. ENDOH		
158340	JPS0720017		Cr1-xRux	Cr0.808Ru0.182	Cr	0.808	Ru	0.182																				1	2003																																														K		1.27					1.27	MTC158340																																	MHC158341																			MSP158340																		uOhm.cm							33.8																		arc-melting - ANN(1500C, 150 h, in sealed W crucible					Competition of Antiferromagnetism and Superconductivity in Cr-Ru Alloys			Department of Physics, Tohoku University Aoba, Aoba-ku, Sendai 980-8578	J.Phys.Soc.Jpn, 72(2003)17	K. CHATANI,Y. ENDOH		
158341	JPS0720017		Cr1-xRux	Cr0.797Ru0.203	Cr	0.797	Ru	0.203																				1	2003																																														K		1.69					1.69																																		MHC158341																			MSP158341																		uOhm.cm							39.3																		arc-melting - ANN(1500C, 150 h, in sealed W crucible					Competition of Antiferromagnetism and Superconductivity in Cr-Ru Alloys			Department of Physics, Tohoku University Aoba, Aoba-ku, Sendai 980-8578	J.Phys.Soc.Jpn, 72(2003)17	K. CHATANI,Y. ENDOH		
158342	JPS0720017		Cr1-xRux	Cr0.774Ru0.226	Cr	0.774	Ru	0.226																				1	2003																																														K		2.06					2.06																																		MHC158341																			MSP158342																		uOhm.cm							42.1																		arc-melting - ANN(1500C, 150 h, in sealed W crucible					Competition of Antiferromagnetism and Superconductivity in Cr-Ru Alloys			Department of Physics, Tohoku University Aoba, Aoba-ku, Sendai 980-8578	J.Phys.Soc.Jpn, 72(2003)17	K. CHATANI,Y. ENDOH		
158343	JPS087123705	Compositions:  Lu:Nd:Ba:Cu = 0.89:0.14:1.98:4 by EDX. Tc increases with increasing  c (lattice constant) in Y124 phase.	(Lu,Nd)Ba2Cu4O8	Lu0.8Nd0.2Ba2Cu4O8	Lu	0.8	Nd	0.2	Ba	2	Cu	4													O	8		3	2018																										AB2C4D8	3	Y124	Ammm		A	3.835	3.879	27.195												K	65		75	75			75																																																																																														Lu2O3,Nd2O3,Ba(OH)2,CuO		KOH flux method. Mixture with 70 wt% KOH - Al2O3 crucible with lid - heat(700 -730 C, 15-40 h) - FC to RT - remove flux - dried at 110C, 30 min.					Single Crystal Growth of Cuprate Superconductor (Lu0.8Nd0.2)Ba2Cu4O8 by KOH Flux Method			MANA, National Institute for Materials Science (NIMS), Tsukuba, Ibaraki 305-0047, Japan	J.Phys.Soc.Jpn, 87(2018)123705	Hiroshi Hara,Shintaro Adachi,Ryo Matsumoto,Aichi Yamashita,Hiroyuki Takeya,Yoshihiko Takano		
158344	JPS087124705	ZF-muon-SR. s+d wave model. Two gaps (higher in DB, lower = 0.92 meV). (dC/Tc) = 94.6 mJ/mol.K2  effective mass m* = 2.45 m<e>	RbCa2Fe4As4F2	Rb1Ca2Fe4As4F2	Rb	1	Ca	2	Fe	4	As	4	F	2														1	2018																										AB2C2D4E4			I4/mmm	139	A	3.8716		31.667											12442-type	K				30			30										100	mT	M-H curve				20			3	T	WHH	300							T/K		13.9					nm	from Hc2	1.04			nm	muon-SR	231			meV	8.08	6.42	16				MSP158344																																																Multigap Superconductivity in RbCa2Fe4As4F2 InvestigatedUsing muon-SR Measurements			ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot Oxon, OX11 0QX, United Kingdom	J.Phys.Soc.Jpn, 87(2018)124705	Devashibhai T. Adroja,Franziska K. K. Kirschner,Franz Lang,Michael Smidman,Adrian D. Hillier,Zhi-Cheng Wang,Guang-Han Cao,Gavin B. G. Stenning,Stephen J. Blundell		
158345	MCP2170451	Autoclave heating (180C, 3days)  Fe/S = 1.31 by EDX.   Hall coehh. RH(0 K) = 0.06 cm3/C. SP (beta) = 0.11 mJ/mol.K4	Li1-xFexOHFeS	Li0.69Fe1.31S1H1O1	Li	0.69	Fe	1.31	S	1	H	1													O	1			2018								8																					P4/nmm	129	A	3.70087		8.88824												K		2.71				0.15	2.71										80										Oe	RES(mid), WHH	386.6												MHC158345																			MSP158345			mJ/mol.K2	130	SP													mOhm.cm							0.17																							Effect of hydrothermal conditions on superconductivity and magnetism in [Li1-xFexOH]FeS			Department of Physics, Boston College, Chestnut Hill, MA 02467, USA	Mat.Chem.Phys., 217(2018)451	E. McDonnell,S. Jaszewski,H.-Y. Yang,M. Abramchuk,Fazel Tafti		
158346	MCP2170451	Autoclave heating (150C, 3days): Fe/S = 1.52 by EDX.	Li1-xFexOHFeS	Li0.48Fe1.52S1H1O1	Li	0.48	Fe	1.52	S	1	H	1													O	1			2018																													P4/nmm	129																K		2.51					2.51										10																																																													mOhm.cm							0.36																							Effect of hydrothermal conditions on superconductivity and magnetism in [Li1-xFexOH]FeS			Department of Physics, Boston College, Chestnut Hill, MA 02467, USA	Mat.Chem.Phys., 217(2018)451	E. McDonnell,S. Jaszewski,H.-Y. Yang,M. Abramchuk,Fazel Tafti		
158347	MCP2170451	Autoclave heating (110C, 3days):  Fe/S = 1.71 by EDX.	Li1-xFexOHFeS	Li0.29Fe1.71S1H1O1	Li	0.29	Fe	1.71	S	1	H	1													O	1			2018					my-B	3	67.1																						P4/nmm	129																K		2.18					2.18																																																																							mOhm.cm							0.6																							Effect of hydrothermal conditions on superconductivity and magnetism in [Li1-xFexOH]FeS			Department of Physics, Boston College, Chestnut Hill, MA 02467, USA	Mat.Chem.Phys., 217(2018)451	E. McDonnell,S. Jaszewski,H.-Y. Yang,M. Abramchuk,Fazel Tafti		
158348	MCP2260095	Nb-Nb chain//c-axis. NbTe4 :Te = 0.8:0.2 (weight fraction). T<CDW> = 208 K  another anomaly at 50 K in R(T). Not SC	NbTe4-x	Nb1Te4	Nb	1	Te	4																					2018																										AB4	2		P4/mcc	124	A	6.4965		6.8232											NbTe4 phase	K					2																																																																																																Nb(2N8),Te(4N8)		solid state reaction. Mixture - pellet - sealed in quartz tube - heat(400C, 72h) - Q to iced water - reground - one more same process					Large enhancement of the CDW resistivity anomaly and traces of superconductivity in imperfect samples of NbTe4			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP, 12600-970, Brazil	Mat.Chem.Phys., 226(2018)95	B.S. de Lima,N. Chaia,T.W. Grant,L.R. de Faria,J.C. Canova,F.S. de Oliveira,F. Abud,A.J.S. Machado		
158349	MCP2260095	Nb-Nb chain//c-axis. NbTe4 :Te = 0.9:0.1 (weight fraction). SC not detected	NbTe4-x	Nb1Te3.4	Nb	1	Te	3.4																					2018																										AB4	2		P4/mcc	124	A	6.5017		6.8326											NbTe4 phase	K					2																																																																																																Nb(2N8),Te(4N8)		solid state reaction. Mixture - pellet - sealed in quartz tube - heat(400C, 72h) - Q to iced water - reground - one more same process					Large enhancement of the CDW resistivity anomaly and traces of superconductivity in imperfect samples of NbTe4			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP, 12600-970, Brazil	Mat.Chem.Phys., 226(2018)95	B.S. de Lima,N. Chaia,T.W. Grant,L.R. de Faria,J.C. Canova,F.S. de Oliveira,F. Abud,A.J.S. Machado		
158350	MCP2260095	Nb-Nb chain//c-axis. NbTe4 :Te = 1:0 (weight fraction). SC not detected	NbTe4-x	Nb1Te3	Nb	1	Te	3																					2018																										AB4	2		P4/mcc	124	A	6.5025		6.8338											NbTe4 phase	K					2																																																																																																Nb(2N8),Te(4N8)		solid state reaction. Mixture - pellet - sealed in quartz tube - heat(400C, 72h) - Q to iced water - reground - one more same process					Large enhancement of the CDW resistivity anomaly and traces of superconductivity in imperfect samples of NbTe4			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP, 12600-970, Brazil	Mat.Chem.Phys., 226(2018)95	B.S. de Lima,N. Chaia,T.W. Grant,L.R. de Faria,J.C. Canova,F.S. de Oliveira,F. Abud,A.J.S. Machado		
158351	MCP2260095	Nb-Nb chain//c-axis. NbTe4 :Te = 1:0 (weight fraction)	NbTe4-x	Nb1Te2	Nb	1	Te	2																					2018																										AB4	2		P4/mcc	124	A	6.5025		6.8338											NbTe4 phase	K			5.5	5.5			5.5										45																																																																																				Nb(2N8),Te(4N8)		solid state reaction. Mixture - pellet - sealed in quartz tube - heat(400C, 72h) - Q to iced water - reground - one more same process					Large enhancement of the CDW resistivity anomaly and traces of superconductivity in imperfect samples of NbTe4			Escola de Engenharia de Lorena, Universidade de Sao Paulo, Lorena, SP, 12600-970, Brazil	Mat.Chem.Phys., 226(2018)95	B.S. de Lima,N. Chaia,T.W. Grant,L.R. de Faria,J.C. Canova,F.S. de Oliveira,F. Abud,A.J.S. Machado		
158352	MRB1120384		Bi1-xPbxPd	Bi1Pd1	Bi	1	Pd	1																					2019																										AB4			P2<1>		A	7.231	10.607	8.722											monoclinic, alpha-BiPd structure	K			3.7	3.8			3.8																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158353	MRB1120384		Bi1-xPbxPd	Bi0.9Pb0.1Pd1	Bi	0.9	Pb	0.1	Pd	1																		1	2019																										AB			P2<1>		A	7.214	10.628	8.722											monoclinic, alpha-BiPd structure	K			3.3	3.2			3.2																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158354	MRB1120384		Bi1-xPbxPd	Bi0.8Pb0.2Pd1	Bi	0.8	Pb	0.2	Pd	1																		1	2019																										AB			P2<1>		A	7.218	10.579	8.73											monoclinic, alpha-BiPd structure	K			2.7	2.6			2.6																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158355	MRB1120384		Bi1-xPbxPd	Bi0.7Pb0.3Pd1	Bi	0.7	Pb	0.3	Pd	1																		1	2019																										AB			P2<1>		A	7.208	10.503	8.742											monoclinic, alpha-BiPd structure	K					2																																																																																																Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158356	MRB1120384		Bi1-xPbxPd	Bi0.6Pb0.4Pd1	Bi	0.6	Pb	0.4	Pd	1																		1	2019																										AB			P2<1>		A	7.19	10.494	8.725											monoclinic, alpha-BiPd structure	K					2																																																																																																Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158357	MRB1120384		Bi1-xPbxPd	Bi0.5Pb0.5Pd1	Bi	0.5	Pb	0.5	Pd	1																		1	2019																										AB			P2<1>		A	7.243	10.42	8.685											monoclinic, alpha-BiPd structure	K					2																																																																																																Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158358	MRB1120384		Bi2-xPbxPd	Bi2Pd1	Bi	2	Pd	1																				1	2019																										AB2			I4/mmm		A	3.348		12.983											beta-Bi2Pd	K			5.3	5.3			5.3																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158359	MRB1120384		Bi2-xPbxPd	Bi1.8Pb0.2Pd1	Bi	1.8	Pb	0.2	Pd	1																		1	2019																										AB2			I4/mmm		A	3.336		12.971											beta-Bi2Pd	K			4.5	4.4			4.4																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158360	MRB1120384		Bi2-xPbxPd	Bi1.6Pb0.4Pd1	Bi	1.6	Pb	0.4	Pd	1																		1	2019																										AB2			I4/mmm		A	3.339		12.941											beta-Bi2Pd	K			3.1	3.1			3.1																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158361	MRB1120384		Bi2-xPbxPd	Bi1.5Pb0.5Pd1	Bi	1.5	Pb	0.5	Pd	1																		1	2019																										AB2			I4/mmm		A	3.336		12.958											beta-Bi2Pd	K			2.4	2.5			2.5																																																																																														Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158362	MRB1120384		Bi2-xPbxPd	Bi1.4Pb0.6Pd1	Bi	1.4	Pb	0.6	Pd	1																		1	2019																										AB2			I4/mmm		A	3.341		12.917											beta-Bi2Pd	K					2																																																																																																Bi(4N),Pb(3N),Pd(3N)		mixture - sealed in quartz tube(vac) - SIN(1273 K, 34 h) - quench					Influence of Pb doping on superconductivity of alpha-BiPd and beta-Bi2Pd alloys			Department of Chemistry, University of Science and Technology of China, Hefei, 230026, China	Mater.Res.Bull., 112(2019)384	Miao Wang,Suyuan Zeng,Baichuan Zhu,Dake Wang,Dan Lin,Yi Ren,Lulu Tang,Kaibin Tang		
158363	PHB1990103	muon-SR measured at H = 350 Oe (Tc = 1.65 K). Penetration depth for H//ab and H//c  measured.	UPd2Al3	U1Pd2Al3	U	1	Pd	2	Al	3																		3	1994																										AB2C3		PrNi2Al3																		K		2					2																																									A	muon-SR		4600	4200																																																								muon +SR studies of magnetism and superconductivity of the heavy fermion superconductor UPd2A13			Institute for Intermediate Energy Physics (ETH Zurich), CH-3232 Villigen, Switzerland	Physica B, 199&200(2014)103	R. Feyerherm,A. Amato,C. Geibel,F.N. Gygax,T. Komatsubara,N. Sato,A.Schenck,F.Steglich		
158364	PHB4042946	R(200K) = 15.05 uOhm.cm	YPd5Al2	Y1Pd5Al2	Y	1	Pd	5	Al	2																		1	2009																										AB2C5		ZrNi2Al5	I4/mmm		A	4.121		14.823												K					0.3																																																										mJ/mol.K2	5	SP													uOhm.cm	4.53																								arc-melting - sealed in quartz tube -ANN(800 C, 7 days)					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158365	PHB4042946	Tn = 3.9 K for poly crystal. Second Tn  = 2.9 K for poly and single crystal. R(200K) = 17.76 uOhm.cm	CePd5Al2	Ce1Pd5Al2	Ce	1	Pd	5	Al	2																		3	2009					my-B/f.u	2.5		4.1																		AB2C5		ZrNi2Al5	I4/mmm		A	4.168		14.941												K					0.3																																																																									uOhm.cm	3.1																								single crystals made by Czochralski method					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158366	PHB4042946	no magnetic order down to 0.3 K. R(200K) = 8.07 uOhm.cm	PrPd5Al2	Pr1Pd5Al2	Pr	1	Pd	5	Al	2																		1	2009					my-B/f.u	3.79																				AB2C5		ZrNi2Al5	I4/mmm		A	4.156		14.938												K					0.3																																																																									uOhm.cm	2.01																								arc-melting - sealed in quartz tube -ANN(800 C, 7 days)					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158367	PHB4042946	Tn from SP measurement. R(200K) = 21.04 uOhm.cm	NdPd5Al2	Nd1Pd5Al2	Nd	1	Pd	5	Al	2																		1	2009					my-B/f.u	3.7		1.2																		AB2C5		ZrNi2Al5	I4/mmm		A	4.149		14.905												K					0.3																																																																									uOhm.cm	6.39																								arc-melting - sealed in quartz tube -ANN(800 C, 7 days)					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158368	PHB4042946	Tn from SP measurement,	SmPd5Al2	Sm1Pd5Al2	Sm	1	Pd	5	Al	2																		1	2009								1.7																		AB2C5		ZrNi2Al5	I4/mmm		A	4.136		14.86												K					0.3																																																																																																		arc-melting - sealed in quartz tube -ANN(800 C, 7 days)					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158369	PHB4042946	R(200K) = 9.31 uOhm.cm	GdPd5Al2	Gd1Pd5Al2	Gd	1	Pd	5	Al	2																		1	2009																										AB2C5		ZrNi2Al5	I4/mmm		A	4.125		14.801												K					0.3																																																																									uOhm.cm	2.245																								arc-melting - sealed in quartz tube -ANN(800 C, 7 days)					Magnetic propertiesof RPd5Al2 (R = Y,Ce,Pr,Nd,Sm,Gd)			Institute for Advanced Materials Research, Hiroshima University, Higashi-Hiroshima 739-8530, Japan	Physica B, 404(2009)2946	R.A.Ribeiro,Y.F.Inoue,T.Onimaru,M.A.Avila,K.Shigetoh,T.Takabatake		
158370	PHC5560019	RRR = 4.6. SP (beta) = 2.72 mJ/mol.K4. (dC/gamma*Tc) = 1.20,  Tc(SP mid) = 2.27 K	SrTa2S5	Sr1Ta2S5	Sr	1	Ta	2	S	5																			2019																										AB2C5	7				A	3.318		24.03											hexagonal	K		2.4					2.4																				T	RES(0.5Rn), (1-t^2) fitting	2.32			2.17			0.6	T/K	RES(0.5Rn)	1.435			MHC158370		A	from Hc2	3.3			A		3200			meV	0.288	2.95	14				MSP158370			mJ/mol.K2	7.62	SP	89.4	SP											mOhm.cm	0.445										2.136			cm3/C	0.0168						n/cm3	372000000000000000000			several heat process in CS2/N2 gas flow. Details see text.					Physical properties and superconductivity of SrTa2S5			Physics Department, Montana State University, Bozeman, MT 59717-3840, USA	Physica C, 556(2019)19	Alisa K. Drenner,S.M. Benjamin,M.G. Smith,J.J. Neumeier		
158371	PRB0133843	Na-intercalated MoS2. 0.3 =< x =< 0.6 in NaxMoS2.	NaxMoS2	Na0.4Mo1S2	Na	0.4	Mo	1	S	2																			1976																											2																		tetra-	K		3.6					3.6																				T			5	0.76					T/K			2	0.3	MHC158371																																																														Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158372	PRB0133843	Ca-intercalated MoS2. 0.05 =< x =< 0.07 in CaxMoS2.	CaxMoS2	Ca0.06Mo1S2	Ca	0.06	Mo	1	S	2																			1976																											3																		ortho-	K		4					4																				T			2.1	0.65					T/K			1.8	0.3	MHC158372																																																														Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158373	PRB0133843	Sr-intercalated MoS2. 0.06 =< x =< 0.1 in SrxMoS2.	SrxMoS2	Sr0.08Mo1S2	Sr	0.08	Mo	1	S	2																			1976																											2																		tetra-	K		5.6					5.6																				T			4.6	1.36					T/K			1.6	0.3	MHC158373																																																														Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158374	PRB0133843	K-intercalated MoS2	K0.4MoS2	K0.4Mo1S2	K	0.4	Mo	1	S	2																			1976																											7																		hexagonal	K		6.9					6.9																				T				4					T/K			4	0.7																																																															Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158375	PRB0133843	Rb-intercalated MoS2	Rb0.3MoS2	Rb0.3Mo1S2	Rb	0.3	Mo	1	S	2																			1976																											7																		hexagonal	K		6.9					6.9																				T				4					T/K			3	0.8																																																															Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158376	PRB0133843	Cs-intercalated MoS2	Cs0.3MoS2	Cs0.3Mo1S2	Cs	0.3	Mo	1	S	2																			1976																											7																		hexagonal	K		6.9					6.9																				T			22	3.3					T/K			5	0.6	MHC158376																																																														Alkali or alkaline-earth metals dissolved in liquid ammonia with MoS2 for intercalated materials					Superconducting critical fields of alkali and alkalne-earth intercalates of MoS2			NASA Levvis Research Center, Cleveland, Ohio 44135	Phys.Rev.B, 13(1976)3843	John A. Woollam,Robert B. Somoano		
158377	PRB0315775	As-arc melted sample.	Cr1-xRex	Cr0.82Re0.18	Cr	0.82	Re	0.18																				1	1985																											1				A	2.9342													cubic	K		0.49					0.49																				kOe	RES(0.5Rn), extrapolation	1.67												MHC158377																						mJ/mol.K2	2.48																																					Cr(4N),Re(4N)		arc-melting					Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 31(1985)5775	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto		
158378	PRB0315775	As-arc melted sample.	Cr1-xRex	Cr0.74Re0.26	Cr	0.74	Re	0.26																				1	1985																											1				A	2.9511													cubic	K		2.69					2.69																				kOe	RES(0.5Rn), extrapolation	5.8												MHC158377																						mJ/mol.K2	5.39																																					Cr(4N),Re(4N)		arc-melting					Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 31(1985)5775	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto		
158379	PRB0315775	As-arc melted sample.	Cr1-xRex	Cr0.66Re0.34	Cr	0.66	Re	0.34																				1	1985																											1				A	2.9697													cubic	K		4.19					4.19	MTC158379																			kOe	RES(0.5Rn), extrapolation	13.6												MHC158377																						mJ/mol.K2	5.58																																					Cr(4N),Re(4N)		arc-melting					Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 31(1985)5775	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto		
158380	PRB0315775	As-arc melted sample.	Cr1-xRex	Cr0.6Re0.4	Cr	0.6	Re	0.4																				1	1985																											1				A	2.9817													cubic	K		5.49					5.49	MTC158380																			kOe	RES(0.5Rn), extrapolation	24.1												MHC158377																						mJ/mol.K2	5.96																																					Cr(4N),Re(4N)		arc-melting					Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 31(1985)5775	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto		
158381	PRB0315775	Annealed sample.  FIG shows annealing effect of Tc and Hc2	Cr1-xRex	Cr0.74Re0.26	Cr	0.74	Re	0.26																				3	1985																											1																		cubic	K		2.75					2.75	MTC158381																																	MHC158381																																																												Cr(4N),Re(4N)		arc-melting					Itinerant-electron antiferromagnetism and superconductivity in bcc Cr-Re alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 31(1985)5775	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto		
158383	PRB0343446	Tn appears for x =< 0.14.	Cr1-xRux	Cr0.86Ru0.14	Cr	0.86	Ru	0.14																				1	1986																															A	2.9145													bcc	K					0.5																																																																																																Cr(4N),Ru(3N)		arc-melting					Superconductivity and magnetism of bcc Cr-Ru alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 34(1986)3446	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto,K. Takeda,K. Fukamichi		
158384	PRB0343446		Cr1-xRux	Cr0.82Ru0.18	Cr	0.82	Ru	0.18																				1	1986																															A	2.9244													bcc	K		1.42					1.42																				T	RES(0.5Rn)				0.88			0.5						MHC158384																																																												Cr(4N),Ru(3N)		arc-melting					Superconductivity and magnetism of bcc Cr-Ru alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 34(1986)3446	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto,K. Takeda,K. Fukamichi		
158385	PRB0343446	(C/gamma*Tc) = 1.28,  Tc(peak)  = 1.87 K.	Cr1-xRux	Cr0.75Ru0.25	Cr	0.75	Ru	0.25																				1	1986																															A	2.9357													bcc	K		2.4				0.05	2.4											Oe	M-H curve				143			0.51	T	RES(0.5Rn)				2.9			0.5						MHC158385																			MSP158385			mJ/mol.K2																																						Cr(4N),Ru(3N)		arc-melting					Superconductivity and magnetism of bcc Cr-Ru alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 34(1986)3446	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto,K. Takeda,K. Fukamichi		
158386	PRB0343446	Tc not given	Cr1-xRux	Cr0.72Ru0.28	Cr	0.72	Ru	0.28																				1	1986																															A	2.9426													bcc	K																																																																																																					Cr(4N),Ru(3N)		arc-melting					Superconductivity and magnetism of bcc Cr-Ru alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 34(1986)3446	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto,K. Takeda,K. Fukamichi		
158387	PRB0343446	A15 compound. ANN(800C, 2 weeks)	Cr3Ru	Cr3Ru1	Cr	3	Ru	1																				1	1986																												A15			A	4.677														K		3.25					3.25																				T	RES(0.5Rn)				4.2			1						MHC158387																																																												Cr(4N),Ru(3N)		arc-melting					Superconductivity and magnetism of bcc Cr-Ru alloys			Electrotechnical Laboratory, Sakura-mura, Ibaraki 305, Japan	Phys.Rev.B, 34(1986)3446	Y. Nishihara,Y. Yamaguchi,T. Kohara,M. Tokumoto,K. Takeda,K. Fukamichi		
158388	PRB077092405	modified Curie-Weiss law for T > 10 K.. not SC.	PuPd5Al2	Pu1Pd5Al2	Pu	1	Pd	5	Al	2																		3	2008	emu/mol	0.00069			myu-B	1.05	-12.5	5.6																		AB2C5		ZrNi2Al5	I4/mmm		A	4.1302		14.8428												K					2																																																							MSP158388			mJ/mol.K2	67									uV/K	-7			MTP158388	uOhm.cm	6.36																								arc-melting. small single crystals (0.03*0.2*0.05 mm3) obtained from as arc-melted sample					Magnetic and electronic properties of antiferromagnetic PuPd5Al2			European Commission, Joint Research Centre, Institute for Transuranium Elements, Postfach 2340, 76125 Karlsruhe, Germany	Phys.Rev.B, 77(2008)092405	K. Gofryk,J-C. Griveau,E. Colineau,J. Rebizant		
158389	PRB077165129	not SC. Tn measured by SP and SUS. Tn = 9.0 K in text.	Nd1-xCexCoIn5	Nd1Co1In5	Nd	1	Co	1	In	5																		3	2008								8.6																		ABC5		HoCoGa5				4.591		7.5126												K					0.5																																																																																																		flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158390	PRB077165129	not SC. Tn measured by SP and SUS	Nd1-xCexCoIn5	Ce0.2Nd0.8Co1In5	Ce	0.2	Nd	0.8	Co	1	In	5																3	2008								8.4																		ABC5		HoCoGa5				4.5938		7.5292												K					0.5																																																																																																		flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158391	PRB077165129	not SC. Tn measured by SP and SUS	Nd1-xCexCoIn5	Ce0.4Nd0.6Co1In5	Ce	0.4	Nd	0.6	Co	1	In	5																3	2008								4.5																		ABC5		HoCoGa5				4.6004		7.5331												K					0.5			MPH158391																																																																																															flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158392	PRB077165129	not SC. Tn measured by SP and SUS. Tcoh (in FIg shows coherence T of Kondo lattice )  = 27 K.	Nd1-xCexCoIn5	Ce0.6Nd0.4Co1In5	Ce	0.6	Nd	0.4	Co	1	In	5																3	2008								1.81																		ABC5		HoCoGa5				4.6053		7.5407												K					0.5			MLAT158392																																																																																															flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158393	PRB077165129	Tcoh (in FIg shows coherence T of Kondo lattice )  = 36 K. Tm(in Fig shows anomaly in C/T below Tc) = 1.31 K	Nd1-xCexCoIn5	Ce0.83Nd0.17Co1In5	Ce	0.83	Nd	0.17	Co	1	In	5																3	2008																										ABC5		HoCoGa5																		K		0.74					0.74																																																																																																flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158394	PRB077165129	Tm(in Fig shows anomaly in C/T below Tc) = 0.6 K	Nd1-xCexCoIn5	Ce0.95Nd0.05Co1In5	Ce	0.95	Nd	0.05	Co	1	In	5																3	2008																										ABC5		HoCoGa5																		K		1.97					1.97																																																																																																flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158395	PRB077165129	Tcoh (in FIg shows coherence T of Kondo lattice )  = 45.6K.	Nd1-xCexCoIn5	Ce1Co1In5	Ce	1	Co	1	In	5																		3	2008																										ABC5		HoCoGa5				4.6128		7.5514												K		2.26					2.26																																																																																																flux method using excess In					Composition and field-tuned magnetism and superconductivity in Nd1-xCexCoIn5			Condensed Matter Physics, Brookhaven National Laboratory, Upton, New York 11973-5000, USA	Phys.Rev.B, 77(2008)165129	Rongwei Hu,Y. Lee,J. Hudis,V. F. Mitrovic,C. Petrovic		
158396	PRB091180404	not bulk SC. Cluster spin glass state below 5 K. Semicon-like R(T) for T* < 60 K.  Curie-Weiss law for T > 60 K.	KCr3As3	K1Cr3As3	K	1	Cr	3	As	3																			2015	emu/mol-Cr	0.0003			my-B/Cr	0.68	-83																			AB3C3		AlFe3Te3	P6<3>/m	176	A	9.0909		4.1806											133-phase	K					4																																																							MSP158396																		mOhm.cm	3.5										1																			Cluster spin-glass ground state in quasi-one-dimensional KCr3As3			Department of Physics, Zhejiang University, Hangzhou 310027, China	Phys.Rev.B, 91(2015)180404	Jin-Ke Bao,Lin Li,Zhang-Tu Tang,Yi Liu,Yu-Ke Li,Hua Bai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
158397	PRB092195122	.P = 0.15 GPa. For P = 0, Tc = 6.79 K from (dTc/dP).	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		6.97					6.97	MTC158397		K/GPa	0.592																																					um	muon-SR	0.344					2.48	16																																															See Phys.Rev.B, 86(2012)024522					Strong enhancement of s-wave superconductivity near a quantum critical point of Ca3Ir4Sn13			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 92(2015)195122	P. K. Biswas,Z. Guguchia,R. Khasanov,M. Chinotti,L. Li,Kefeng Wang,C. Petrovic,E. Morenzoni		
158398	PRB092195122	P = 1.13 GPa. d(1/pen^2)/dP  = 2.84 um^(-2)/Gpa for P =< Pc . Pc = 1.6 GPa	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.69					7.69	MPEN158398																																								um	muon-SR	0.302					2.24	16																																															See Phys.Rev.B, 86(2012)024522					Strong enhancement of s-wave superconductivity near a quantum critical point of Ca3Ir4Sn13			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 92(2015)195122	P. K. Biswas,Z. Guguchia,R. Khasanov,M. Chinotti,L. Li,Kefeng Wang,C. Petrovic,E. Morenzoni		
158399	PRB092195122	P = 2.18 Gpa. d(1/pen^2)/dP  = 10.17 um^(-2)/Gpa for P >= Pc . Pc = 1.6 GPa	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		8.09					8.09	MGAP158399																																								um	muon-SR	0.233					3.41	16																																															See Phys.Rev.B, 86(2012)024522					Strong enhancement of s-wave superconductivity near a quantum critical point of Ca3Ir4Sn13			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.B, 92(2015)195122	P. K. Biswas,Z. Guguchia,R. Khasanov,M. Chinotti,L. Li,Kefeng Wang,C. Petrovic,E. Morenzoni		
158400	PRB093241112	Structural phase transition at 152 K from R(T) & C(T). SP (beta) = 3.53 mJ/mol.K4. (dC/gamma*Tc) = 1.93. R = R0 + A*T^2, R0=24.9 uOhm.cm, A = 0.026 uOhm.cm/T^2	La3Co4Sn13	La3Co4Sn13	La	3	Co	4	Sn	13																		3	2016																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K		2.7					2.7																																																								mJ/mol.K2	27.87																																					La(3N),Co(3N),Sn(3N)		Flux method. Mixture(La:Co:Sn = 2:1:30) - sealed in quartz tube - heat(1050 C) - cool to 600 C(3 C/h) - remove excess Sn after reheating to 500 C					Second-order structural transition in the superconductor La3Co4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.B, 93(2016)241112	Y. W. Cheung,J. Z. Zhang,J. Y. Zhu,W. C. Yu,Y. J. Hu,D. G. Wang,Yuka Otomo,Kazuaki Iwasa,Koji Kaneko,Masaki Imai,Hibiki Kanagawa,Kazuyoshi Yoshimura,Swee K. Goh		
158401	PRB093245119	T*(=T<STR>) = 135.2 K from SP data. Below T*, CDW appears. (dT*/dP) =  -1.9 K/kbar from linear thermal expansion coefficient.	Sr3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																		3	2016																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K																																																												MSP158401																																											self-flux method					Comparative study of thermodynamic properties near the structural phase transitions in Sr3Rh4Sn13 and Sr3Ir4Sn13			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 93(2016)245119	C. S. Lue,C. N. Kuo,C. W. Tseng,K. K. Wu,Y.-H. Liang,C.-H. Du,Y. K. Kuo		
158402	PRB093245119	T*(=T<STR>) = 146.3 K from SP data. Below T*, CDW appears. (dT*/dP) =  -1.6 K/kbar from linear thermal expansion coefficient.	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2016																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																	K																																																												MSP158402																																											self-flux method					Comparative study of thermodynamic properties near the structural phase transitions in Sr3Rh4Sn13 and Sr3Ir4Sn13			Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan	Phys.Rev.B, 93(2016)245119	C. S. Lue,C. N. Kuo,C. W. Tseng,K. K. Wu,Y.-H. Liang,C.-H. Du,Y. K. Kuo		
158403	PRB096064521	RRR = 1.09. Debye-T = 237 K from R(T). SP (beta) = 0.35 mJ/mol.K4, (delta) = 1.2 uJ/mol.K6.  (dC/gamma*Tc) = 1.60. GL = 46.2.	Re6Zr	Re6Zr1	Re	6	Zr	1																				1	2017																										AB6		alpha-Mn	I4[-]3m																	K		6.75		6.7		0.2	6.75											mT	M-H curve, (1-t^2)	10.3							T	SUS. WHH	11.2							T/K	SUS	2.44			MHC158403		nm	from Hc2	5.37			nm		247					3.72	14				MSP158403			mJ/mol.K2	26.9	SP	338	SP											uOhm.cm							142																Re(4N),Zr(4N)		arc-melting. Several times.					Superconducting and normal-state properties of the noncentrosymmetric superconductor Re6Zr			Physics Department, University of Warwick, Coventry CV4 7AL, United Kingdom	Phys.Rev.B, 96(2017)064521	D. A. Mayoh,J. A. T. Barker,R. P. Singh,G. Balakrishnan,D. McK. Paul,M. R. Lees		
158404	PRB096140504	R(T)  shows semiconducting behaviour below 100 K.	KCr3As3	K1Cr3As3	K	1	Cr	3	As	3																		3	2017																										AB3C3		AlFe3Te3	P6<3>/m	176	A	9.09		4.182											133-phase	K	3		4.5				3.75										9																																																													mOhm.cm											0.765														133-type single crystals prepared by intercalation of K from 233-type crystals ( immersing in dehydrated ethanol)					Superconductivity at 5 K in quasi-one-dimensional Cr-based KCr3As3 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 96(2017)140504	Qing-Ge Mu,Bin-Bin Ruan,Bo-Jin Pan,Tong Liu,Jia Yu,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
158405	PRB096140504	RRR = 3. SP (dC/gamma*Tc) = 0.47.	KCr3As3	K1Cr3As3	K	1	Cr	3	As	3																		3	2017																										AB3C3		AlFe3Te3	P6<3>/m	176															133-phase	K	4.54		5				4.77										98										T	RES(0.5Rn), GL fitting		20.8											MHC158405																			MSP158405			mJ/mol.K2	81.31	SP	319	SP											mOhm.cm							0.16				0.492														(#158404 sample) - ANN(373 K, 12 h, in evacuated quartz tube)					Superconductivity at 5 K in quasi-one-dimensional Cr-based KCr3As3 single crystals			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 96(2017)140504	Qing-Ge Mu,Bin-Bin Ruan,Bo-Jin Pan,Tong Liu,Jia Yu,Kang Zhao,Gen-Fu Chen,Zhi-An Ren		
158406	PRB096140501	Structural phase transition  Tetra-to-hcT (half collapsed tetra) at 4 GPa. For P >= 4 Gpa, hcT phase stabilized and not bulk SC.	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2017																										ABC4D4		CaRb1144	P4/mmm																	K	35		35	35.6		0.2	35.6	MTC158406																																																																																															single crystals grown using high-T solution growth technique					Pressure-induced half-collapsed-tetragonal phase in CaKFe4As4			Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 96(2017)140501	Udhara S. Kaluarachchi,Valentin Taufour,Aashish Sapkota,Vladislav Borisov,Tai Kong,William R. Meier,Karunakar Kothapalli,Benjamin G. Ueland,Andreas Kreyssig,Roser Valenti,Robert J. McQueeney,Alan I. Goldman,Sergey L. Bud'ko,Paul C. Canfield		
158407	PRB098214505	SP (beta) = 1.83 mJ/mol.K4. (delta) = 0.49 uJ/mol.K6. GL(kappa) = 23. (dC/gamma*Tc) = 1.17.  Hc(0) = 21 mT. gap d = 0.46 meV,  2d  = 3.58 kTc from muon-SR	LaPtGe	La1Pt1Ge1	La	1	Pt	1	Ge	1																		1	2018																										ABC		LaPtSi	I4<1>md	109	A	4.2655		14.9654												K			3.05	3.05			3.05										100	mT	M-H curve, (1-t^2)	2.1							T	RES(on), GL fitting	0.69							T/K	RES(on)	0.67			MHC158407		A	from Hc2	218			A	from Hc1	5047					3.2	14				MSP158407			mJ/mol.K2	6.6	SP	147	SP											uOhm.cm							195				400												La(4N),Pt(4N),Ge(4N)		arc-melting , several times					Superconducting properties of the noncentrosymmetric superconductor LaPtGe			Department of Physics, Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India	Phys.Rev.B, 98(2018)214505	Sajilesh K. P,D. Singh,P. K. Biswas,A. D. Hillier,R. P. Singh		
158408	PRB098214509	Three phases,  alpha-(P =< 0.33), beta-(0.33 < P  =<1.05), gamma-(1.05 < P  < 2.13 GPa). Hc2(T) measured for three phases	BaBi3	Ba1Bi3	Ba	1	Bi	3																				3	2018																										AB3			P4/mmm		A	5.06		5.13												K								MTC158408																																																																																															Bi-self flux method					Pressure-induced multiple phase transformations of the BaBi3 superconductor			Ames Laboratory, Iowa State University, Ames, Iowa 50011, USA	Phys.Rev.B, 98(2018)214509	Li Xiang,Raquel A. Ribeiro,Udhara S. Kaluarachchi,Elena Gati,Manh Cuong Nguyen,Cai-Zhuang Wang,Kai-Ming Ho,Sergey L. Bud'ko,Paul C. Canfield		
158409	PRB098214517	RRR = 1.1. SP (beta) = 0.169 mJ/mol.K4. dC<e> = 8.14 mJ/mol.K. (dC<e>/gamma*Tc) = 1.42. e-ph = 0.49. GL = 111.	Ru0.75Rh0.25As	Ru0.75Rh0.25As1	Ru	0.75	Rh	0.25	As	1																		1	2018																										AB	3	MnP	Pnma		A	5.6322	3.473	6.2065												K	1.63		1.8	1.6			1.6										100	mT	M-H curve	5.4							T	R(T), extrapolation	2.6							T/K		1.72			MHC158409		nm	from Hc2	11			nm	muon-SR	487			meV	0.25	3.62	16				MSP158409			mJ/mol.K2	3.79	SP	284	SP											mOhm.cm							7.25																Ru(3N),Rh(4N),P(3N5),As(5N)		mixture - pellet  -  sealed in quartz tube -  SIN(1100 C for P, 1000 C for AS, 60 h) - reground -  SIN(1100 C for P, 1000 C for AS, 80 h)					Superconductivity in Ru0.55Rh0.45P and Ru0.75Rh0.25As probed by muon spin relaxation and rotation measurements			Helmholtz-Zentrum Berlin fur Materialien und Energie GmbH, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 98(2018)214517	V. K. Anand,D. T. Adroja,M. R. Lees,P. K. Biswas,A. D. Hillier,B. Lake		
158410	PRB098214517	RRR = 1.2. SP (beta) = 0.078 mJ/mol.K4. dC<e> = 5.4 mJ/mol.K. (dC<e>/gamma*Tc) = 1.42. e-ph = 0.56. GL = 93.	Ru0.55Rh0.45P	Ru0.55Rh0.45P1	Ru	0.55	Rh	0.45	P	1																		1	2018																										AB	3	MnP	Pnma		A	5.423	3.3891	5.9255												K	3.8		3.9	3.7			3.7										100	mT	M-H curve	5.6							T	R(T), extrapolation	3.3							T/K		1.08			MHC158410		nm	from Hc2	10			nm	muon-SR	309			meV	0.57	3.56	16				MSP158410			mJ/mol.K2	1.03	SP	368	SP											mOhm.cm							0.55																Ru(3N),Rh(4N),P(3N5),As(5N)		mixture - pellet  -  sealed in quartz tube -  SIN(1100 C for P, 1000 C for AS, 60 h) - reground -  SIN(1100 C for P, 1000 C for AS, 80 h)					Superconductivity in Ru0.55Rh0.45P and Ru0.75Rh0.25As probed by muon spin relaxation and rotation measurements			Helmholtz-Zentrum Berlin fur Materialien und Energie GmbH, Hahn-Meitner Platz 1, D-14109 Berlin, Germany	Phys.Rev.B, 98(2018)214517	V. K. Anand,D. T. Adroja,M. R. Lees,P. K. Biswas,A. D. Hillier,B. Lake		
158411	PRB098220507	nematic transition at about 45 K observed in asymmetry factor measured by NQR.	BaTi2Bi2O	Ba1Ti2Bi2O1	Ba	1	Ti	2	Bi	2															O	1			2018																										ABC2D2			P4/mmm	123															nematic	K				4.6			4.6																																																																																														BaO,Ti,Bi		solid state reaction. mixture - pellet - wrapped in Ta-foil - sealed in quartz tube - heat (850 C). poly sample mixed with Araldite adhesive					Nematic transition and highly two-dimensional superconductivity in BaTi2Bi2O revealed by <209>Bi-nuclear magnetic resonance/nuclear quadrupole resonance measurements			Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Phys.Rev.B, 98(2018)220507	Shunsaku Kitagawa,Kenji Ishida,Wataru Ishii,Takeshi Yajima,Zenji Hiroi		
158412	PRB098224505	SC gaps measured by infrared spectroscopy. There are three gaps. 2d/kTc = 1.97, 3.63, 5.44. The largest one , 5.44 in DB. gap-origin discussed in text.	BaFe1.9Pt0.1As2	Ba1Fe1.9Pt0.1As2	Ba	1	Fe	1.9	Pt	0.1	As	2																3	2018																										AB2C2		ThCr2Si2																		K		23					23																																														meV	5.1	5.44	2																																															single crystals grown using FeAs self-flux method					Strong electron-boson coupling in the iron-based superconductor BaFe1.9Pt0.1As2 revealed by infrared spectroscopy			Department of Physics, College of William & Mary, Williamsburg, Virginia 23187-8795, USA	Phys.Rev.B, 98(2018)224505	Zhen Xing,Shanta Saha,J. Paglione,M. M. Qazilbash		
158413	PRB098220512	In-plane anisotropy of Hc2, C<e> are measured. C<e> depends on H-direction (H//a or H//b)	Cu1.5(PbSe)5(Bi2Se3)6	Cu1.5Pb5Bi6Se23	Cu	1.5	Pb	5	Bi	6	Se	23																3	2018																																														K		2.7					2.7										75										T	RES(0.5Rn)													MHC158413																																																														Modified Bridgman method					Nematic superconductivity in Cu1.5(PbSe)5(Bi2Se3)6			Physics Institute II, University of Cologne, 50937 Koln, Germany	Phys.Rev.B, 98(2018)220512	Lionel Andersen,Zhiwei Wang,Thomas Lorenz,Yoichi Ando		
158414	PRB098220512	same as #158413, only different of SC volume fraction.	Cu1.5(PbSe)5(Bi2Se3)6	Cu1.5Pb5Bi6Se23	Cu	1.5	Pb	5	Bi	6	Se	23																3	2018																																														K		2.7					2.7										104										T	RES(0.5Rn)													MHC158414																			MSP158414																																											Modified Bridgman method					Nematic superconductivity in Cu1.5(PbSe)5(Bi2Se3)6			Physics Institute II, University of Cologne, 50937 Koln, Germany	Phys.Rev.B, 98(2018)220512	Lionel Andersen,Zhiwei Wang,Thomas Lorenz,Yoichi Ando		
158415	PRB098220506	RRR = 90.SP (beta) = 13.86 mJ/mol.K4. C<e>/gamma*Tc) = 0.67. e-ph = 0.98. kappa(GL) = 10.35. (dTc/dP) = -0.55 for P < Pc(0.88 GPa, = -0.73 K/GPa for P>Pc	BaBi3	Ba1Bi3	Ba	1	Bi	3																					2018																										AB3	2		I4/mmm																	K	5.95		6				5.975	MTC158415		K/GPa	-0.55						100	Oe	M-H curve, (1-t^2)	237.8							T	WHH	21.8												MHC158415		nm	from Hc2	12.3			nm	London	127.3					3.28	14				MSP158415			mJ/mol.K2	49.19	SP	149	SP											uOhm.cm							356																							Two distinct superconducting phases and pressure-induced crossover from type-II to type-I superconductivity in the spin-orbit-coupled superconductors BaBi3 and SrBi3			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 98(2018)220506	Bosen Wang,Xuan Luo,Kento Ishigaki,Kazuyuki Matsubayashi,Jinguang Cheng,Yuping Sun,Yoshiya Uwatoko		
158416	PRB098220506	RRR = 549.SP (beta) = 5.84 mJ/mol.K4. C<e>/gamma*Tc) = 2.41. e-ph = 0.93. kappa(GL) = 0.76	SrBi3	Bi3Sr1	Bi	3	Sr	1																					2018																										AB3																				K	5.5		5.6				5.55	MTC158416		K/GPa	-0.49						85	Oe	M-H curve, (1-t^2)	488.7							T	WHH	1.9												MHC158416		nm	from Hc2	42.28			nm	London	31.79					6.09	14				MSP158416			mJ/mol.K2	11.03	SP	180	SP											uOhm.cm							0.11																							Two distinct superconducting phases and pressure-induced crossover from type-II to type-I superconductivity in the spin-orbit-coupled superconductors BaBi3 and SrBi3			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 98(2018)220506	Bosen Wang,Xuan Luo,Kento Ishigaki,Kazuyuki Matsubayashi,Jinguang Cheng,Yuping Sun,Yoshiya Uwatoko		
158417	PRB098235130	RRR = 18. not SC down to 2 K. For hydrostatic P upto 2.13 GP, SC not observed in R(T), C(T) and Hall effect.	SrAg4As2	Sr1Ag4As2	Sr	1	Ag	4	As	2																		3	2018																										AB2C4			R3[-]m																	K					2																																																													140	SP											uOhm.cm							3																Sr,Ag2As		Single crystals grown  by self-flux method. mixture(Sr:Ag2As = 1:4) - in alumina crucible - sealed in quartz tube - heat to 1100 C - slow cool to 650 C(5 C/h)					Significant change in the electronic behavior associated with structural distortions in monocrystalline SrAg4As2			Department of Physics and Astronomy and California NanoSystems Institute, University of California, Los Angeles, California 90095, USA	Phys.Rev.B, 98(2018)235130	Bing Shen,Eve Emmanouilidou,Xiaoyu Deng,Alix McCollam,Jie Xing,Gabriel Kotliar,Amalia I. Coldea,Ni Ni		
158418	PRB099014501	T*(cohere-incohere crossover temp) = 150 K. R(T) = R0 + A*T^n  for Tc < T 80 K, n =1.05	KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2														1	2019																										AB2C2D4E4			I4/mmm	139	A	3.8785		31.282											12442-type structure. 2(CaFeAs +KFe2As2	K	32.2		33.5	33.2			33.2	MTC158418																																																																						mOhm.cm							0.257																		solid state reaction					Pressure-induced enhancement of superconductivity and quantum criticality in the 12442-type hybrid-structure superconductor KCa2Fe4As4F2			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 99(2019)014501	Bosen Wang,Zhi-Cheng Wang,Kento Ishigaki,Kazuyuki Matsubayashi,Tetsujiro Eto,Jianping Sun,Jin-Guang Cheng,Guang-Han Cao,Yoshiya Uwatoko		
158419	PRB099014501	Data for P = 9.5 GPa. T*(cohere-incohere crossover temp) = 224 K. R(T) = R0 + A*T^n  for Tc < T 80 K, n =1.8	KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2														1	2019																										AB2C2D4E4					A	3.736		29.0388											12442-type structure. 2(CaFeAs +KFe2As2	K	18		28.6				23.3	MLAT158419																																																																						mOhm.cm							0.06																		solid state reaction					Pressure-induced enhancement of superconductivity and quantum criticality in the 12442-type hybrid-structure superconductor KCa2Fe4As4F2			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 99(2019)014501	Bosen Wang,Zhi-Cheng Wang,Kento Ishigaki,Kazuyuki Matsubayashi,Tetsujiro Eto,Jianping Sun,Jin-Guang Cheng,Guang-Han Cao,Yoshiya Uwatoko		
158420	PRB099020503	P-induced SC. Pc = 23.8 GPa. SC properties (in DB) are for P = 45 GPa.	TaIrTe4	Ta1Ir1Te4	Ta	1	Ir	1	Te	4																		3	2019																										ABC4	3				A	3.8	12.47	13.24												K			1.752		0		1.752	MTC158420																			T	RES(on), WHH	0.83												MHC158420																																																														flux method using Te as a flux..  (Ta:Ir:Te = 3:3:94) - alumina crucible - sealed in quartz tube - heat(1200 C, 3 h) - cool to 550 C (2 C/h)					Observation of superconductivity in the pressurized Weyl-semimetal candidate TaIrTe4			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 99(2019)020503	Shu Cai,Eve Emmanouilidou,Jing Guo,Xiaodong Li,Yanchun Li,Ke Yang,Aiguo Li,Qi Wu,Ni Ni,Liling Sun		
158421	PRB099020503	Data for P = 23.8 GPa. Hall coeff. (FIG) shows RH(P) at T= 10 K. Lattice const.(FIG) shows pressure dependence.	TaIrTe4	Ta1Ir1Te4	Ta	1	Ir	1	Te	4																		3	2019																										ABC4	3				A	3.6078	11.8057	11.8933												K			0.54		0		0.54	MLAT158421																																																																																				cm3/C						MRH158421					flux method using Te as a flux..  (Ta:Ir:Te = 3:3:94) - alumina crucible - sealed in quartz tube - heat(1200 C, 3 h) - cool to 550 C (2 C/h)					Observation of superconductivity in the pressurized Weyl-semimetal candidate TaIrTe4			Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 99(2019)020503	Shu Cai,Eve Emmanouilidou,Jing Guo,Xiaodong Li,Yanchun Li,Ke Yang,Aiguo Li,Qi Wu,Ni Ni,Liling Sun		
158422	PRB099024508	P-induced SC. Pc = 90 GPa. lattice const. at P = 0	Li5MoH11	Li5Mo1H11	Li	5	Mo	1	H	11																			2019																										AB5C11			P6<3>cm		A															K					0			MLAT158422																																																																																															High-P-High-T synthesis. Annealing at RT under high pressure					Superconductivity of the hydrogen-rich metal hydride Li5MoH11 under high pressure			KYOKUGEN, Graduate School of Engineering Science, Osaka University, 1?3 Machikaneyama, Toyonaka, Osaka 560?8531, Japan	Phys.Rev.B, 99(2019)024508	Dezhong Meng,Masafumi Sakata,Katsuya Shimizu,Yuki Iijima,Hiroyuki Saitoh,Toyoto Sato,Shigeyuki Takagi,Shin-ichi Orimo		
158423	PRB099024508	P-induced SC. Pc = 90 GPa. Data for P = 160 GPa. Tc defined as inflection point in R(T). For P = 160 GPa, three point , three different Hc2(T)	Li5MoH11	Li5Mo1H11	Li	5	Mo	1	H	11																			2019																										AB5C11																				K					0			MTC158423																			T	RES(on)													MHC158423																																																														High-P-High-T synthesis. Annealing at RT under high pressure					Superconductivity of the hydrogen-rich metal hydride Li5MoH11 under high pressure			KYOKUGEN, Graduate School of Engineering Science, Osaka University, 1?3 Machikaneyama, Toyonaka, Osaka 560?8531, Japan	Phys.Rev.B, 99(2019)024508	Dezhong Meng,Masafumi Sakata,Katsuya Shimizu,Yuki Iijima,Hiroyuki Saitoh,Toyoto Sato,Shigeyuki Takagi,Shin-ichi Orimo		
158424	PRL109237008	Substitution Ca to Sr induces negative pressure effect. x =0 (Ca3Ir4Sn13) equal to P = -52 kbar for Sr3Ir4Sn13. Tc-Fig shows Tc vs P. T* = 147 K.	(CaxSr1-x)3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2012																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.7968													I phase	K		5					5	MTC158424																																																																																															single crystals grown by flux method					Pressure- and Composition-Induced Structural Quantum Phase Transition in the Cubic Superconductor dSr; CaT3Ir4Sn13			Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett., 109(2012)237008	Lina E. Klintberg,Swee K. Goh,Patricia L. Alireza,Paul J. Saines,David A. Tompsett,Peter W. Logg,Jinhu Yang,Bin Chen,Kazuyoshi Yoshimura,F. Malte Grosche		
158425	PRL109237008	T* (superlattice transition) = 82 K.	(CaxSr1-x)3Ir4Sn13	Ca1.5Sr1.5Ir4Sn13	Ca	1.5	Sr	1.5	Ir	4	Sn	13																3	2012																										A3B4C13		Yb3Rh4Sn13																		K		5.75					5.75	MTC158425																																																																																															single crystals grown by flux method					Pressure- and Composition-Induced Structural Quantum Phase Transition in the Cubic Superconductor dSr; CaT3Ir4Sn13			Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett., 109(2012)237008	Lina E. Klintberg,Swee K. Goh,Patricia L. Alireza,Paul J. Saines,David A. Tompsett,Peter W. Logg,Jinhu Yang,Bin Chen,Kazuyoshi Yoshimura,F. Malte Grosche		
158426	PRL109237008	T* (superlattice transition) = 44 K.	(CaxSr1-x)3Ir4Sn13	Ca2.25Sr0.75Ir4Sn13	Ca	2.25	Sr	0.75	Ir	4	Sn	13																3	2012																										A3B4C13		Yb3Rh4Sn13																		K		6.36					6.36																																																																																																single crystals grown by flux method					Pressure- and Composition-Induced Structural Quantum Phase Transition in the Cubic Superconductor dSr; CaT3Ir4Sn13			Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom	Phys.Rev.Lett., 109(2012)237008	Lina E. Klintberg,Swee K. Goh,Patricia L. Alireza,Paul J. Saines,David A. Tompsett,Peter W. Logg,Jinhu Yang,Bin Chen,Kazuyoshi Yoshimura,F. Malte Grosche		
158427	PRL114097002	T*(phase transition measured by R(T)) = 138 K. Chemical P (x=0) correspond to -68 kbar of x=1 in (CaxSr1-x)3Rh4Sn13.	(CaxSr1-x)3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n		A	9.8061													Phase transition (I to I' phase at T*)	K		4.65					4.65																																																																																																Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158428	PRL114097002	T* = 87 K	(CaxSr1-x)3Rh4Sn13	Ca0.75Sr2.25Rh4Sn13	Ca	0.75	Sr	2.25	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																	Phase transition (I to I' phase at T*)	K		4.86					4.86																																																																																																Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158429	PRL114097002	T* = 55 K	(CaxSr1-x)3Rh4Sn13	Ca1.5Sr1.5Rh4Sn13	Ca	1.5	Sr	1.5	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																	Phase transition (I to I' phase at T*)	K		6.42					6.42	MTC158429																																																																																															Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158430	PRL114097002	T* = 28 K	(CaxSr1-x)3Rh4Sn13	Ca2.25Sr0.75Rh4Sn13	Ca	2.25	Sr	0.75	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																	Phase transition (I to I' phase at T*)	K		7.34					7.34																																																																																																Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158431	PRL114097002	T* = 0 K. Pc = -6.8 kbar	(CaxSr1-x)3Rh4Sn13	Ca2.7Sr0.3Rh4Sn13	Ca	2.7	Sr	0.3	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.65					7.65																																																																																																Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158432	PRL114097002		(CaxSr1-x)3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.76					7.76	MTC158432																																																																																															Sn-flux method					Ambient Pressure Structural Quantum Critical Point in the Phase Diagram of  (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 114(2015)097002	S. K. Goh,D. A. Tompsett,P. J. Saines,H. C. Chang,T. Matsumoto,M. Imai,K. Yoshimura,F. M. Grosche		
158433	PRL114146403	P-induced SC. Pc(Tn=0 K) at  P = 3.2 GPa	CeIrIn4.95Cd0.05	Ce1Ir1In4.95Cd0.05	Ce	1	Ir	1	In	4.95	Cd	0.05																3	2015																										ABC5		HoCoGa5																		K	1.05			0.99	0		0.99	MTC158433																																																																																															self-flux method					Reemergent Superconductivity and Avoided Quantum Criticality in Cd-Doped CeIrIn5 under Pressure			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou 310058, China	Phys.Rev.Lett., 114(2015)146403	Y. Chen,W. B. Jiang,C. Y. Guo,F. Ronning,E. D. Bauer,Tuson Park,H. Q. Yuan,Z. Fisk,J. D. Thompson,Xin Lu		
158434	PRL115207003	T*(phase transition measured by R(T)) = 138. (dC/gamma*Tc) = 1.48. Einstein-T = 47.1 K.	(CaxSr1-x)3Rh4Sn13	Sr3Rh4Sn13	Sr	3	Rh	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13	Pm3[-]n																for T > T*	K		4.15					4.15																																																3.47	14							mJ/mol.K2	35.1	SP	244.3	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158435	PRL115207003	T*(phase transition measured by R(T)) = 92.2. (dC/gamma*Tc) = 1.87. Einstein-T = 43.9 K.	(CaxSr1-x)3Rh4Sn13	Ca0.75Sr2.25Rh4Sn13	Ca	0.75	Sr	2.25	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		4.84					4.84																																																4.11	14							mJ/mol.K2	36.8	SP	234.3	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158436	PRL115207003	T*(phase transition measured by R(T)) = 57.7. (dC/gamma*Tc) = 3.08. Einstein-T = 43.8 K.	(CaxSr1-x)3Rh4Sn13	Ca1.5Sr1.5Rh4Sn13	Ca	1.5	Sr	1.5	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		6.46					6.46																																																5.56	14							mJ/mol.K2	40.5	SP	199.7	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158437	PRL115207003	T*(phase transition measured by R(T)) = 22.4. (dC/gamma*Tc) = 3.31. Einstein-T = 33.3 K.	(CaxSr1-x)3Rh4Sn13	Ca2.25Sr0.75Rh4Sn13	Ca	2.25	Sr	0.75	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.5					7.5																																																6.04	14							mJ/mol.K2	48.2	SP	162.6	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158438	PRL115207003	(dC/gamma*Tc) = 2.91. Einstein-T = 32.1 K.	(CaxSr1-x)3Rh4Sn13	Ca2.7Sr0.3Rh4Sn13	Ca	2.7	Sr	0.3	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.76					7.76																																																6.36	14				MSP158438			mJ/mol.K2	49.7	SP	162.9	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158439	PRL115207003	(dC/gamma*Tc) = 3.46. Einstein-T = 31.6 K.	(CaxSr1-x)3Rh4Sn13	Ca2.85Sr0.15Rh4Sn13	Ca	2.85	Sr	0.15	Rh	4	Sn	13																3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.9					7.9																																																6.66	14							mJ/mol.K2	51.5	SP	161.3	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158440	PRL115207003	(dC/gamma*Tc) = 2.71. Einstein-T = 32.7 K.	(CaxSr1-x)3Rh4Sn13	Ca3Rh4Sn13	Ca	3	Rh	4	Sn	13																		3	2015																										A3B4C13		Yb3Rh4Sn13																		K		7.94					7.94																																																5.71	14							mJ/mol.K2	59.6	SP	166.9	SP																																				Sn-flux method					Strong Coupling Superconductivity in the Vicinity of the Structural Quantum Critical Point in (CaxSr1-x)3Rh4Sn13			Department of Physics, The Chinese University of Hong Kong, Shatin, New Territories, Hong Kong, China	Phys.Rev.Lett., 115(2015)207003	Wing Chi Yu,Yiu Wing Cheung,Paul J. Saines,Masaki Imai,Takuya Matsumoto,Chishiro Michioka,Kazuyoshi Yoshimura,Swee K. Goh		
158441	SST031015003	M = NH3. x and y in LixMyFe2(TezSe1-z)2 not given. compositions = (Li:Fe:Se = 0.18:1:0.9 ) by ICP-AES. H*= unpinned to pinned vortex transition. Hg= transition to vortex glass state	Lix(NH3)yFe2(TezSe1-z)2	Li1M1Fe2Se2	Li	1	M	1	Fe	2	Se	2																	2018																																													M-intercalated material	K		44.36					44.36																				T	RES(0.9Rn)					14		43.7						MHC158441		nm	from Hc2			0.27																																																								single crystals of LiFeSe-122 and LiFeTeSe-122 were synthesized via low temperature ammonothermal technique.					Transport properties of Lix(NH3)yFe2(TezSe1-z)2 single crystals in the mixed state			Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials & Micro-nano Devices, Renmin University of China, Beijing 100872, People?s Republic of China	Supercond.Sci.Technol., 31(2018)015003	Shanshan Sun,Shaohua Wang,Chenghe Li,Hechang Lei		
158442	SST031015003	M = NH3. x and y in LixMyFe2(TezSe1-z)2 not given. compositions = (Li:Fe:Te:Se= 0.16:1:0.60:0.38 ) by ICP-AES. H*= unpinned to pinned vortex transition. Hg= transition to vortex glass state	Lix(NH3)yFe2(TezSe1-z)2	Li1M1Fe2Se0.4Te0.6	Li	1	M	1	Fe	2	Se	0.4	Te	0.6															2018																																													M-intercalated material	K		20.28					20.28																				T	RES(0.9Rn)					14		19.7						MHC158442		nm	from Hc2			0.9																																																								single crystals of LiFeSe-122 and LiFeTeSe-122 were synthesized via low temperature ammonothermal technique.					Transport properties of Lix(NH3)yFe2(TezSe1-z)2 single crystals in the mixed state			Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials & Micro-nano Devices, Renmin University of China, Beijing 100872, People?s Republic of China	Supercond.Sci.Technol., 31(2018)015003	Shanshan Sun,Shaohua Wang,Chenghe Li,Hechang Lei		
158443	SST031015020	Compositions by XRD and ICP. RRR = 1.5. SP (beta) = 1.3 mJ/mol.K4. (dC) at Tc = 8.02 mJ/mol.K.  Anisotropy (Hc2) = 1.8.	HfAs1.67Te0.12	Hf1As1.67Te0.12	Hf	1	As	1.67	Te	0.12																		3	2018																										ABC		PbFCl	P4/nmm	129	A	3.6695		8.1395												K	1.67			1.7		0.04	1.7										100										T	RES(zero),SP,SUS, WHH		0.5	0.28										MHC158443		A	from Hc2		342	194													MSP158443			mJ/mol.K2	4	SP													uOhm.cm							62				93														single crystals grown using chemical transport method ( agent : Iodine). 1123 K(sink) - 1223 K(source)					Superconductivity and valence state in layered single-crystal HfAs1.67Te0.12			Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People?s Republic of China	Supercond.Sci.Technol., 31(2018)015020	Jian Peng,Jia Yu,Shuai Zhang,Genfu Chen		
158444	SST031034007	as-grown crystal. e-ph = 0.6. strong coupling correction factor = 1.14. Anisotropy (dHc2/dT) = 5.6	NdFeAsO0.7F0.3	Nd1Fe1As1F0.3O0.7	Nd	1	Fe	1	As	1	F	0.3													O	0.7		3	2018																										ABCD		oxypnictide																		K			46.4				46.4																													T/K			7.3	1.3	MHC158444																																																																			Clean to dirty limit and Tc suppression in NdFeAsO0.7F0.3 studied by Hc2 analysis			CNR-SPIN, c/o Department of Physics, via Dodecaneso 33, 16146, Genoa, Italy	Supercond.Sci.Technol., 31(2018)034007	I Pallecchi,C Tarantini,Y Shen,R K Singh,N Newman,P Cheng,Y Jia,H-H Wen,M Putti		
158445	SST031034007	2MeV alpha-particle irradiation effect . Tc = 11.5 K . Tc depends on irradiation dose and disorder parameter, not shown explicitely.  Anisotropy (dHc2/dT) = 2.5	NdFeAsO0.7F0.3	Nd1Fe1As1F0.3O0.7	Nd	1	Fe	1	As	1	F	0.3													O	0.7		3	2018																										ABCD		oxypnictide																		K			11.5				11.5																													T/K			5.7	2.3	MHC158445																																					uOhm.cm											775																			Clean to dirty limit and Tc suppression in NdFeAsO0.7F0.3 studied by Hc2 analysis			CNR-SPIN, c/o Department of Physics, via Dodecaneso 33, 16146, Genoa, Italy	Supercond.Sci.Technol., 31(2018)034007	I Pallecchi,C Tarantini,Y Shen,R K Singh,N Newman,P Cheng,Y Jia,H-H Wen,M Putti		
158446	SST031034007	2MeV alpha-particle irradiation effect . Tc = 41.4 K . Tc depends on irradiation dose and disorder parameter, not shown explicitely. Anisotropy (dHc2/dT) = 3.1	NdFeAsO0.7F0.3	Nd1Fe1As1F0.3O0.7	Nd	1	Fe	1	As	1	F	0.3													O	0.7		3	2018																										ABCD		oxypnictide																		K			41.4				41.4																													T/K			6.75	2	MHC158446																																																																			Clean to dirty limit and Tc suppression in NdFeAsO0.7F0.3 studied by Hc2 analysis			CNR-SPIN, c/o Department of Physics, via Dodecaneso 33, 16146, Genoa, Italy	Supercond.Sci.Technol., 31(2018)034007	I Pallecchi,C Tarantini,Y Shen,R K Singh,N Newman,P Cheng,Y Jia,H-H Wen,M Putti		
158447	PRB099014516	RRR = 1.02. Hc(0) = 51 mT. kappa(GL) = 46.5. SP (beta) = 0.123 mJ/mol.K4. (dC<el>/gamma*Tc) = 1.45. e-ph = 0.52.	NbOs2	Nb1Os2	Nb	1	Os	2																				1	2019																										AB2		alpha-Mn	I4[-]3m		A	9.654														K			2.7	2.7			2.7										100	mT	M-H curve, (1-t^2)	2.98							T	RES(onset),WHH	3.36							T/K	RES(onset)	1.8			MHC158447		A	from Hc2	99			A	Hc1, GL analysis	4608					3.54	14				MSP158447			mJ/mol.K2	8.58	SP	362	SP																																		Nb(3N5),Os(3N5)		arc-melting several times - sealed in quartz tube - ANN( 1 week)					Superconducting and normal state properties of the noncentrosymmetric superconductor NbOs2 investigated by muon spin relaxation and rotation			Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India	Phys.Rev.B, 99(2019)014516	D. Singh,Sajilesh K. P,Sourav Marik,A. D. Hillier,R. P. Singh		
158448	PRB099014516	muon-SR measurements.  [ penet]<L> = 3720 A.  [cohere]0 - 90 A	NbOs2	Nb1Os2	Nb	1	Os	2																				1	2019																										AB2		alpha-Mn	I4[-]3m		A	9.654														K			2.7	2.7			2.7																																									A	muon-SR	6190																																																	n/m3	2740000000000000000000000000	Nb(3N5),Os(3N5)		arc-melting several times - sealed in quartz tube - ANN( 1 week)					Superconducting and normal state properties of the noncentrosymmetric superconductor NbOs2 investigated by muon spin relaxation and rotation			Indian Institute of Science Education and Research Bhopal, Bhopal 462066, India	Phys.Rev.B, 99(2019)014516	D. Singh,Sajilesh K. P,Sourav Marik,A. D. Hillier,R. P. Singh		
158500	CEM1802670	not SC. T-independent Pauli paramagnetic. SUS(300 K) = 6E-4 emu/mol. XPS,PES measured for band structure.	Hf(SixAs1-x)As	Hf1Si0.5As1.5	Hf	1	Si	0.5	As	1.5																		3	2007	emu/mol	0.0008																								ABC	2	PbFCl	P4/nmm	129	A	3.641		8.155											ZrSiS -type structure	K					2																																																																									mOhm.cm												0.19											Hf(2N6),Si(4N),As(5N8)		mixture (Hf:Si:As = 1:0.5:1.5) - sealed in silica tube - heat(873 K, 12 h) - hold (3 days) - heat (1173 K,24 h) - ANN ( 1-4 weeks) - Q to water					Analysis of the electronic structure of Hf(Si0.5As0.5)As by X-ray photoelectron and photoemission spectroscopy			Department of Chemistry, University of Alberta, Edmonton, Alberta, Canada T6G 2G2	J.Solid State Chem., 180(2007)2670	Andrew P. Grosvenor,Ronald G. Cavell,Arthur Mar,Robert I.R. Blyth		
158501	CPC0112639	Compositions were quantatively measured by ICP-OES. Anisotropy (Rc/Rab) = 3 at Tc. RRR = 1.1. SP (beta = 0.161 J/mol.K4.	HfAs1.7Se0.2	Hf1As1.7Se0.2	Hf	1	As	1.7	Se	0.2																		3	2010																										ABC	2	PbFCl			A	3.7084		8.0496											Hf-(As,Se)-As , three layers	K		0.52				0.04	0.52																																																					MSP158501			mJ/mol.K2	2.7	SP	330	SP	W/K.m				MTHC158501	uV/K	11.5			MTP158501	uOhm.cm		143	426																						Chemical transport method using iodine as agent. 1073 K(source) and 1173 K(sink)					Crystal Chemistry and Physical Properties of the Nonmagnetic Kondo Compound HfAs1.7Se0.2			Max-Planck-Institut fur Chemische Physik fester Stoffe Ncthnitzer Strasse 40, Dresden , Germany	Chem.Phys.Chem., 11(2010)2639	Andreas Czulucki,Gudrun Auffermann,Michal Bednarski,Lukasz Bochenek,Maik Bohme,Tomasz Cichorek,Rainer Niewa,Niels Oeschler,Marcus Schmidt,Frank Steglich,Rudiger Kniep		
158502	JAC7930393	RRR = 4.3. Hc1:after demag-correction (N = 0.65). GL(kappa) = 9.5. Hc(0) = 250 mT. e-ph = 0.63. (dC/gamma*Tc) =1.78. DOS = 6.44 eV/fu	CaRh2	Ca1Rh2	Ca	1	Rh	2																				1	2019																										AB2		MgCu2(Laves)	Fd-3m	227	A	7.5326													C15	K	5.2			5.16			5.16										100	Oe	M-H curve, demag = 0.65	418							T	RES(0.5Rn), GL approx.	3.37												MHC158502		A	from Hc2	98			A	Hc1, GL equation	942										MSP158502			mJ/mol.K2	24.7	SP	322	SP											uOhm.cm	56.3						56.3																Ca(4N),Rh(3N8)		Two step solid state reaction. mixture (25% excess Ca) - alumina crucible - in quartz tube - heat (870 C,12h) - slow cool to 800 C, keep 2h - reground - pellet - heat (800 C, 12h)					The electronic characterization of the cubic Laves-phase superconductor CaRh2			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, ul. Narutowicza 11/12, 80-233, Gdansk, Poland	J.Alloy.Compound, 793(2019)393	Karolina Gornicka,Robert J. Cava,Tomasz Klimczuk		
158503	JAC7960287	not SC	Zr4Rh2Ox	Zr4Rh2O0.4	Zr	4	Rh	2																	O	0.4		1	2019																										AB2C4			Fd3[-]m		A	12.4127													eta-carbide structure	K					1.75																																																																																																Zr(sponge, 2N5),ZrO2(4N5),Rh(2N8)		mixture - pellet - (arc melting) - ground to powder - pellet - sealed in quartz tube - heat in furnace (10 days) - ANN (1000C)					Superconductivity in the eta-carbide-type oxides Zr4Rh2Ox			Department of Chemistry and Department of Physics, University of Zurich, CH-8057 Zurich, Switzerland	J.Alloys Compd., 796(2019)287	KeYuan Ma,Jorge Lago,Fabian O. von Rohr		
158504	JAC7960287	not SC	Zr4Rh2Ox	Zr4Rh2O0.5	Zr	4	Rh	2																	O	0.5		1	2019																										AB2C4			Fd3[-]m		A	12.4061													eta-carbide structure	K					1.75																																																																																																Zr(sponge, 2N5),ZrO2(4N5),Rh(2N8)		mixture - pellet - (arc melting) - ground to powder - pellet - sealed in quartz tube - heat in furnace (10 days) - ANN (1000C)					Superconductivity in the eta-carbide-type oxides Zr4Rh2Ox			Department of Chemistry and Department of Physics, University of Zurich, CH-8057 Zurich, Switzerland	J.Alloys Compd., 796(2019)287	KeYuan Ma,Jorge Lago,Fabian O. von Rohr		
158505	JAC7960287	not SC	Zr4Rh2Ox	Zr4Rh2O0.6	Zr	4	Rh	2																	O	0.6		1	2019																										AB2C4			Fd3[-]m		A	12.4014													eta-carbide structure	K					1.75																																																																																																Zr(sponge, 2N5),ZrO2(4N5),Rh(2N8)		mixture - pellet - (arc melting) - ground to powder - pellet - sealed in quartz tube - heat in furnace (10 days) - ANN (1000C)					Superconductivity in the eta-carbide-type oxides Zr4Rh2Ox			Department of Chemistry and Department of Physics, University of Zurich, CH-8057 Zurich, Switzerland	J.Alloys Compd., 796(2019)287	KeYuan Ma,Jorge Lago,Fabian O. von Rohr		
158506	JAC7960287	highest phase purity. RRR = 1.08. SP (beta) = 1.43 mJ/mol.K4. (dC/gamma*Tc) = 2.25.  Hp = 5.18 T. e-ph = 0.60	Zr4Rh2Ox	Zr4Rh2O0.7	Zr	4	Rh	2																	O	0.7		1	2019																										AB2C4			Fd3[-]m		A	12.41014													eta-carbide structure	K		2.8		2.6			2.8											mT	M-H curve								T	RES(0.5Rn), WHH	4.89							T/K	RES(0.5Rn)	2.51			MHC158506		A	from Hc2	8.3			A	Hc1, GL equation				meV	0.47	4.2	14				MSP158506			mJ/mol.K2	14.5	SP	209	SP											mOhm.cm												0.11											Zr(sponge, 2N5),ZrO2(4N5),Rh(2N8)		mixture - pellet - (arc melting) - ground to powder - pellet - sealed in quartz tube - heat in furnace (10 days) - ANN (1000C)					Superconductivity in the eta-carbide-type oxides Zr4Rh2Ox			Department of Chemistry and Department of Physics, University of Zurich, CH-8057 Zurich, Switzerland	J.Alloys Compd., 796(2019)287	KeYuan Ma,Jorge Lago,Fabian O. von Rohr		
158507	JAC7960287	RRR = 1.62. SP (beta) = 2.01 mJ/mol.K4. (dC/gamma*Tc) = 1.74. Hc(0) = 101 mT. Hp = 8.70 T. GL(kappa) = 44. e-ph = 0.73	Zr4Rh2Ox	Zr4Rh2O1	Zr	4	Rh	2																	O	1		1	2019																										AB2C4			Fd3[-]m		A	12.38112													eta-carbide structure	K		4.7		4.3			4.7											mT	M-H curve	8.8							T	RES(0.5Rn), WHH	6.08							T/K	RES(0.5Rn)	1.95			MHC158507		A	from Hc2	72			A	Hc1, GL equation	3199			meV	0.64	3.46	14				MSP158507			mJ/mol.K2	17.9	SP	189	SP											mOhm.cm												0.23											Zr(sponge, 2N5),ZrO2(4N5),Rh(2N8)		mixture - pellet - (arc melting) - ground to powder - pellet - sealed in quartz tube - heat in furnace (10 days) - ANN (800)C					Superconductivity in the eta-carbide-type oxides Zr4Rh2Ox			Department of Chemistry and Department of Physics, University of Zurich, CH-8057 Zurich, Switzerland	J.Alloys Compd., 796(2019)287	KeYuan Ma,Jorge Lago,Fabian O. von Rohr		
158508	JAC8030597		Ta1-xZrxB	Ta1B1	Ta	1	B	1																				1	2019																										AB																			CrB proto-type	K		4					4																																																																																																mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158509	JAC8030597		Ta1-xZrxB	Ta0.9Zr0.1B1	Ta	0.9	Zr	0.1	B	1																		1	2019																										AB																			FeB prototype	K		4.62					4.62																																																																																																mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158510	JAC8030597		Ta1-xZrxB	Ta0.85Zr0.15B1	Ta	0.85	Zr	0.15	B	1																		1	2019																										AB																			FeB prototype	K		6.01					6.01																																																																																																mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158511	JAC8030597	SP (beta) = 0.1511 mJ/mol.K4.  (dC/gamma*Tc) = 1.44.	Ta1-xZrxB	Ta0.8Zr0.2B1	Ta	0.8	Zr	0.2	B	1																		1	2019																										AB					A	6.14	3.159	4.62											FeB prototype	K		7.51	7.8	7.8			7.51	MTC158511									95	Oe	M-H curve. Hc1(T), Fig.								T	RES(0.5Rn), two-band model	8.8												MHC158511																			MSP158511			mJ/mol.K2	3.067	SP	295	SP																																				mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158512	JAC8030597		Ta1-xZrxB	Ta0.75Zr0.25B1	Ta	0.75	Zr	0.25	B	1																		1	2019																										AB																			FeB prototype	K		6					6																																																																																																mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158513	JAC8030597		Ta1-xZrxB	Ta0.7Zr0.3B1	Ta	0.7	Zr	0.3	B	1																		1	2019																										AB																			FeB prototype	K		5					5																																																																																																mixture - arc-melting . weight loss during arc melting less than 0.2 %					Evidence of multiband behavior in a new superconductor Ta0.8Zr0.2B with FeB-prototype structure			Escola de Engenharia de Lorena, University of Sao Paulo, P. O. Box 116, Lorena, 12602-810, Brazil	J.Alloy.Compound, 803(2019)597	L.E. Correa,J.C.C. Nova,L.R. de Faria,F.B. Santos,B.S. de Lima,C.A. Nunes,G.C. Coelho,P. Rogl,Z. Fisk,A.J.S. Machado		
158514	JPCC11918007	P-induced SC.. Phase diagram from run-1,run-2, run-3 pressure experiments. SC observed by R(T).	BaReH9	Ba1Re1H9	Ba	1	Re	1	H	9																			2015																										ABC9		NiAs	P6<3>/mmc																	K			7				7	MPH158514																																																																																															Sample synthesized through the reduction of perrhnate in aqueous ethylenediamiine solutions					Metallization and Superconductivity in the Hydrogen-Rich Ionic Salt BaReH9			Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC 20015, United States	J.Phys.Chem.C, 119(2015)18007	Takaki Muramatsu,Wilson K. Wanene,Maddury Somayazulu,Eugene Vinitsky,Dhanesh Chandra,Timothy A. Strobel,Viktor V. Struzhkin,Russell J. Hemley		
158515	JPS088035001	Film. prepared under P(O2) = 1 E-7 Torr . not SC. Fig. shows M-I transition temperature vs P.	Ti4O7	Ti4O7	Ti	4																			O	7			2019																										A4B7					A	5.52	7.12	20.43											alpha = 67.5, beta = 57.3, gamma = 108.8.	K					0			MPH158515																																																																																															Pulsed laser deposition. deposition under P(O2)  = 1 E-7 Torr (oxidative condition).  Substrates = LSAT and  LaAlO3					High-pressure Study of Superconductivity in Ti4O7 Film			Department of Physics, College of Humanities and Sciences, Nihon University, Setagaya, Tokyo 156-8550, Japan	J.Phys.Soc.Jpn, 88(2019)035001	Shuhei Sekiguchi,Takuya Shiraishi,Kyota Miura,Chizuru Kawashima,Kohei Yoshimatsu,Akira Ohtomo,Hayato Kamioka,Hiroki Takahashi		
158516	JPS088035001	Film. deposited under P(Ar) = 1 E-3 Torr (less oxidative condition). Fig shows P-dependence of Tc.	Ti4O7	Ti4O7	Ti	4																			O	7			2019																										A4B7					A	5.52	7.11	20.46											alpha = 67.5, beta = 57.2, gamma = 108.8.	K	2.07		2.56				2.315	MTC158516		K/GPa	-0.7																																																																																												Pulsed laser deposition. deposition under P(Ar)  = 1 E-3 Torr (less oxidative condition). Substrate = LaAlO3					High-pressure Study of Superconductivity in Ti4O7 Film			Department of Physics, College of Humanities and Sciences, Nihon University, Setagaya, Tokyo 156-8550, Japan	J.Phys.Soc.Jpn, 88(2019)035001	Shuhei Sekiguchi,Takuya Shiraishi,Kyota Miura,Chizuru Kawashima,Kohei Yoshimatsu,Akira Ohtomo,Hayato Kamioka,Hiroki Takahashi		
158517	JPS088043702	Oarai sample (CVT). RRR = 35.  (dC<el>/gamma*Tc) = 1.51	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2			Immm	71	A	4.161	6.122	13.955											UTe2-type	K		1.65					1.65																				T	RES(0.5Rn)													MHC158517																			MSP158517			J/mol.K2	0.117	SP													uOhm.cm	18.5																								single crystals grown using chemical vapor transport method (CVT) in Oarai					Unconventional Superconductivity in Heavy Fermion UTe2			IMR, Tohoku University, Oarai, Ibaraki 311-1313, Japan	J.Phys.Soc.Jpn, 88(2019)043702	Dai Aoki,Ai Nakamura,Fuminori Honda,DeXin Li,Yoshiya Homma,Yusei Shimizu,Yoshiki J. Sato,Georg Knebel,Jean-Pascal Brison,Alexandre Pourret,Daniel Braithwaite,Gerard Lapertot,Qun Niu,Michal Vali?ka,Hisatomo Harima,Jacques Flouquet		
158518	JPS088043702	Self-flux sample. RRR = 4.	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2																			UTe2-type	K		1.1					1.1																																																																							uOhm.cm	340																								Self-flux method. starting material with the ratio,  U:Te = 22:78, in alumina crucible in double sealed (Ta/quartz) ampoule.					Unconventional Superconductivity in Heavy Fermion UTe2			IMR, Tohoku University, Oarai, Ibaraki 311-1313, Japan	J.Phys.Soc.Jpn, 88(2019)043702	Dai Aoki,Ai Nakamura,Fuminori Honda,DeXin Li,Yoshiya Homma,Yusei Shimizu,Yoshiki J. Sato,Georg Knebel,Jean-Pascal Brison,Alexandre Pourret,Daniel Braithwaite,Gerard Lapertot,Qun Niu,Michal Vali?ka,Hisatomo Harima,Jacques Flouquet		
158519	JPS088043702	Grenoble sample (CVT)	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2																			UTe2-type	K		1.4					1.4																				T	RES(0.5Rn)													MHC158519																			MSP158519																																											single crystals grown using chemical vapor transport method (CVT) in Grenoble					Unconventional Superconductivity in Heavy Fermion UTe2			IMR, Tohoku University, Oarai, Ibaraki 311-1313, Japan	J.Phys.Soc.Jpn, 88(2019)043702	Dai Aoki,Ai Nakamura,Fuminori Honda,DeXin Li,Yoshiya Homma,Yusei Shimizu,Yoshiki J. Sato,Georg Knebel,Jean-Pascal Brison,Alexandre Pourret,Daniel Braithwaite,Gerard Lapertot,Qun Niu,Michal Vali?ka,Hisatomo Harima,Jacques Flouquet		
158520	JPS088063707	HCFIG shows angular dependence of Hc2(T = 30 mK) for b-to a-axis and b-to c-axiis angle direction.	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2			Immm																Ortho-, UTe2-type	K		1.5					1.5																				T														MHC158520																																																														single crystals grown using chemical vapor transport method (CVT) in Grenoble					Field-Reentrant Superconductivity Close to a Metamagnetic Transition in the Heavy-Fermion Superconductor UTe2			Univ. Grenoble Alpes, CEA, IRIG-Pheliqs, 38000 Grenoble, France	J.Phys.Soc.Jpn, 88(2019)063707	Georg Knebel,William Knafo,Alexandre Pourret,Qun Niu,Michal Vali?ka,Daniel Braithwaite,Gerard Lapertot,Marc Nardone,Abdelaziz Zitouni,Sanu Mishra,Ilya Sheikin,Gabriel Seyfarth,Jean-Pascal Brison,Dai Aoki,Jacques Flouquet		
158521	JPS088063707	HCFIG shows Hc2 (T) for several H-direction , angle (theta) from b- to a- direction	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2			Immm																Ortho-, UTe2-type	K		1.5					1.5																				T	RES(0)													MHC158521																																																														single crystals grown using chemical vapor transport method (CVT) in Grenoble					Field-Reentrant Superconductivity Close to a Metamagnetic Transition in the Heavy-Fermion Superconductor UTe2			Univ. Grenoble Alpes, CEA, IRIG-Pheliqs, 38000 Grenoble, France	J.Phys.Soc.Jpn, 88(2019)063707	Georg Knebel,William Knafo,Alexandre Pourret,Qun Niu,Michal Vali?ka,Daniel Braithwaite,Gerard Lapertot,Marc Nardone,Abdelaziz Zitouni,Sanu Mishra,Ilya Sheikin,Gabriel Seyfarth,Jean-Pascal Brison,Dai Aoki,Jacques Flouquet		
158522	SCIR0059477	M = NH3. y not given. High Tc phase (SC-2) appears above 8 GPa. For  low Tc phase (SC-1) , Tc  linearly decreases with P.	(NH3)yCs0.4FeSe	M1Cs0.4Fe1Se1	M	1	Cs	0.4	Fe	1	Se	1																	2015																													I4/mmm		A	3.8331		16.217												K			33	31			31	MTC158522																																																																																															Liquid ammonia method					Emergence of double-dome superconductivity in ammoniated metal-doped FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Report, 5(2015)9477	Masanari Izumi,Lu Zheng,Yusuke Sakai,Hidenori Goto,Masafumi Sakata,Yuki Nakamoto,Huyen L. T. Nguyen,Tomoko Kagayama,Katsuya Shimizu,Shingo Araki,Tatsuo C. Kobayashi,Takashi Kambe,Dachun Gu,Jing Guo,Jing Liu,Yanchun Li,Liling Sun,Kosmas Prassides,Yoshihiro Kubozono		
158523	SCIR0059477	M = NH3. y not given. Lattice constant measured by XRD and SPring - 8.	(NH3)yCs0.4FeSe	M1Cs0.4Fe1Se1	M	1	Cs	0.4	Fe	1	Se	1																	2015																													I4/mmm																	K			33	31			31	MLAT158523																																																																																															Liquid ammonia method					Emergence of double-dome superconductivity in ammoniated metal-doped FeSe			Research Laboratory for Surface Science, Okayama University, Okayama 700-8530, Japan	Sci.Report, 5(2015)9477	Masanari Izumi,Lu Zheng,Yusuke Sakai,Hidenori Goto,Masafumi Sakata,Yuki Nakamoto,Huyen L. T. Nguyen,Tomoko Kagayama,Katsuya Shimizu,Shingo Araki,Tatsuo C. Kobayashi,Takashi Kambe,Dachun Gu,Jing Guo,Jing Liu,Yanchun Li,Liling Sun,Kosmas Prassides,Yoshihiro Kubozono		
158524	PCS1280211	P-induced SC. Tc = 3.4 K at  Pcr = 6.8 GPa. SC properties for P = 14 GPa.	BiTeCl	Bi1Te1Cl1	Bi	1	Te	1	Cl	1																		3	2019																										ABC	7		P6<3>mc																Phase transition P6<3>/mc to Pnma at P=6.7 GPa.	K			3.6		0		3.6	MTC158524																			T	RES(onset), WHH		5.63											MHC158524																																																			cm3/C						MRH158524	n/cm3	389000000000000000000	Te(powder),Bi  & Cl (reagent)		Bridgeman method. mixture - sealed in quartz tube(1E-4 Pa) - heat (660 C, 24 h) - slow cool to 100C (12 C/h) - Q to RT					Pressure-induced superconductivity and quantum phase transitions in the Rashba material BiTeCl			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Phys.Chem.Solids, 128(2019)211	M.L. Jin,S.J. Zhang,L.Y. Xing,W.M. Li,G.Q. Zhao,X.C. Wang,Y.W. Long,X.D. Li,H.Y. Bai,C.Z. Gu,C.Q. Jin		
158525	PCS1280211	P-induced SC. Tc = 3.4 K at  Pcr = 6.8 GPa. SC properties for P = 28 GPa.	BiTeCl	Bi1Te1Cl1	Bi	1	Te	1	Cl	1																		3	2019																										ABC																				K			4.12		0		4.12																				T	RES(onset), WHH		4.44											MHC158524																																																										n/cm3	9100000000000000000000	Te(powder),Bi  & Cl (reagent)		Bridgeman method. mixture - sealed in quartz tube(1E-4 Pa) - heat (660 C, 24 h) - slow cool to 100C (12 C/h) - Q to RT					Pressure-induced superconductivity and quantum phase transitions in the Rashba material BiTeCl			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Phys.Chem.Solids, 128(2019)211	M.L. Jin,S.J. Zhang,L.Y. Xing,W.M. Li,G.Q. Zhao,X.C. Wang,Y.W. Long,X.D. Li,H.Y. Bai,C.Z. Gu,C.Q. Jin		
158526	PCS1280211	P-induced SC. Pcr = 8.0 GPa. Tc = 5.39 K (in DB)  at Pcr.  topological phase transition at about 2 GPa.	BiTeI	Bi1Te1I1	Bi	1	Te	1	I	1																			2019																										ABC			P3m1																	K			5.39		0		5.39	MTC158526																																																																																																				Pressure-induced superconductivity and quantum phase transitions in the Rashba material BiTeCl			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	J.Phys.Chem.Solids, 128(2019)211	M.L. Jin,S.J. Zhang,L.Y. Xing,W.M. Li,G.Q. Zhao,X.C. Wang,Y.W. Long,X.D. Li,H.Y. Bai,C.Z. Gu,C.Q. Jin		
158527	PHB5360816	not SC. Debye-T = 332 K   from R(T) analysis.	LuFe2Si2	Lu1Fe2Si2	Lu	1	Fe	2	Si	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8726		9.8698												K					0																																																										mJ/mol.K2	40.4	SP	323	SP											uOhm.cm	6.2						6.2																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158528	PHB5360816	not SC. Debye-T = 259 K   from R(T) analysis.	LuCo2Si2	Lu1Co2Si2	Lu	1	Co	2	Si	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8494		9.6765												K					0																																																										mJ/mol.K2	8.5	SP	355	SP											uOhm.cm	51.4						51.4																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158529	PHB5360816	not SC. Debye-T = 236 K   from R(T) analysis.	LuNi2Si2	Lu1Ni2Si2	Lu	1	Ni	2	Si	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.9085		9.5035												K					0																																																										mJ/mol.K2	12.6	SP	360	SP											uOhm.cm	5.2						5.2																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158530	PHB5360816	not SC. Debye-T = 243 K  from R(T) analysis.	LuRu2Si2	Lu1Ru2Si2	Lu	1	Ru	2	Si	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.138		9.4199												K					0																																																										mJ/mol.K2	7.7	SP	359	SP											uOhm.cm	3.2						3.2																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158531	PHB5360816	Debye-T = 150 K   from R(T) analysis. (dC/gamma*Tc) = 1.7	LuPd2Si2	Lu1Pd2Si2	Lu	1	Pd	2	Si	2																		1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	4.0898		9.8513												K		0.6					0.6																																																								mJ/mol.K2	6.9	SP	290	SP											uOhm.cm	3						3																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158532	PHB5360816	Debye-T = 144 K   from R(T) analysis.   (dC/gamma*Tc) = 1.5	LuPt2Si2	Lu1Pt2Si2	Lu	1	Pt	2	Si	2																		1	2018																										AB2C2		CaBe2Ge2	P4/nmm		A	4.0998		9.9463												K		1.8					1.8																																																					MSP158532			mJ/mol.K2	4.7	SP	198	SP											uOhm.cm	51.6						51.6																		arc melting (Ar) - wrapped in Mo-foil - ANN(1173 K,2w, in silica tube)					Electronic structures and superconductivity in LuTE2Si2 phases (TE = d-electron transition metal)			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, P Nr 1410, 50-590 Wroc?aw 2, Poland	Physica B, 536(2018)816	M. Samsel?Czeka?a,G. Chajewski,P.Wisniewski,T.Romanova,A.Hackemer,R.Gorzelniak,A.P.Pikul,D.Kaczorwski		
158533	PHB5360830	Li-intercalated KSr2Nb3O10 (LT phase). Li-content by electro-chemical method.	LixKSr2Nb3O10	Li1.3K1Sr2Nb3O10	Li	1.3	K	1	Sr	2	Nb	3													O	10		3	2018																													P2<1>/m		A	7.831	7.801	15.292											monoclinic, beta = 97.44. LT-phase	K				4			4																																																																																														K2SO3,SrCoO3,Nb2O5		mixture (K2SO3:SrCoO3:Nb2O5 = 10:2:3) - heat (1350 C, 30h, in pt crucible) slow cool to 1000 C (4 C/h) - rapid cool to RT					Crystal structure and superconducting properties of KSr2Nb3O10			Graduate School of Natural Science and Technology, Okayama University, Okayama, Japan	Physica B, 536(2018)830	T. Kawaguchi,K. Horigane,Y. Itoh,K. Kobayashi,R. Horie,T. Kambe,J. Akimitsu		
158534	PHB5450152	splat cooled alloy	U0.85Nb0.15	U0.85Nb0.15	U	0.85	Nb	0.15																					2018																															A	3.435		3.565											distorted gamma-U structure	K		1.9	1.9			0.18	1.9																				T	RES(mid), GL	5.4							T/K	RES(mid)	3.2			MHC158534																						mJ/mol.K2	13.5	SP	154	SP											uOhm.cm							86				84														arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158535	PHB5450152	splat cooled alloy	U0.85Mo0.15	U0.85Mo0.15	U	0.85	Mo	0.15																					2018																																													gamma-phase	K		2.11	2.11			0.02	2.11																				T	RES(mid), GL	6.7							T/K	RES(mid)	3.6			MHC158535																						mJ/mol.K2	16	SP	139	SP											uOhm.cm							95				89														arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158536	PHB5450152	splat cooled alloy	U0.85Pt0.15	U0.85Pt0.15	U	0.85	Pt	0.15																					2018																																													gamma + alpha phase	K		0.75				0.08	0.75																				T	RES(mid), GL	2.5							T/K	RES(mid)	3.8																									mJ/mol.K2	19.5	SP	145	SP											uOhm.cm							166				164														arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158537	PHB5450152	splat cooled alloy	U0.85Ru0.15	U0.85Ru0.15	U	0.85	Ru	0.15																					2018																																													gamma-phase	K		1.4				0.09	1.4																				T	RES(mid), GL	4.5							T/K	RES(mid)	4.3																									mJ/mol.K2	13.2	SP	142	SP											uOhm.cm							214				220														arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158538	PHB5450152	splat cooled alloy	U0.85Ti0.15	U0.85Ti0.15	U	0.85	Ti	0.15																					2018																																													gamma + alpha phase	K		0.45	1.9			0.3	0.45																				T	RES(mid), GL	1.5							T/K	RES(mid)	2.7																									mJ/mol.K2	13.4	SP	157	SP											uOhm.cm							166				167														arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158539	PHB5450152	splat cooled alloy	U0.89Mo0.11	U0.89Mo0.11	U	0.89	Mo	0.11																					2018																																														K																																																												MSP158539																																											arc-melting - splat cooling apparatus - cool with cooling rate of  E+6 K/s.					Superconductivity in U-Nb alloys with gamma-U phase and ferromagnetism of their hydrides			aInstitute of Physics, Pedagogical University, Podchorazych 2, 30-084 Krakow, Poland	Physica B, 545(2018)152	N.-T.H. Kim-Ngan,S. Sowa,M. Krupska,V. Buturlim,M. Paukov,D. Drozdenko,P. Minarik,L. Havela		
158540	PHB5700296	SP shows two  AFM peaks,  Tn = 3.5 K and  4.3 K (in DB).  SP (beta) = 1.76 mJ/mol.K4.	Pr2Pt3Ge5	Pr2Pt3Ge5	Pr	2	Pt	3	Ge	5																		1	2019								4.3																				U2Co3Si5	Ibam		A	10.156	11.894	6.247												K			6.7				6.7																				T	RES(mid), WHH	2.1												MHC158540		A	from Hc2	126																		mJ/mol.K2	170	SP	222.6	SP											uOhm.cm							20																		arc-melting					Robust superconductivity against the antiferromagnetic ordering in Pr2Pt3Ge5			UGC-DAE CSR, University Campus, Khandwa Road, Indore, 452001, Madhya Pradesh, India	Physica B, 570(2019)296	Vinay Kaushik,D. Venkateshwarlu,A.K. Mishra,M. Krishnan,R. Venkatesh,M.M. Patidar,V. Ganesan		
158542	PHC5630007	hexagonal MoC + zeta-Mo2C + unknown phase. MoCx, x not given. x=1 (DB) is tentative. R(T) not to zero down to 3 K.	MoCx	Mo1C1	Mo	1	C	1																					2019																																														K				5.8			5.8																				T	RES(0.9Rn), GL	1.7																																																	uOhm.cm	4.1						22				127												Mo(4N),C(3N5)		arc-melting. mixture (Mo:C = 1:1) - press to pellet - arc-melting ( 4 times). weight loss = 6.73%					Superconductivity in an arc melted MoCx			College of Science, Henan University of Engineering, Zhengzhou 451191, China	Physica C, 563(2019)7	Qianhui Mao,Jinfeng Yang,Ruixue Li,Haoshan Hao,Zhefeng Lou,Yuxing Zhou,Minghu Fang		
158543	PRB090220504	Cu intercalated - (PbSe)5(Bi2Se3)6	Cux(PbSe)5(Bi2Se3)6	C1.36Pb5Bi12Se23	C	1.36	Pb	5	Bi	12	Se	23																	2014																																														K		2.9		2.9			2.9	MTC158543										mT	M-H		0.34						T	RES(0.5Rn), extrapolation		4.3	2.6					T/K	RES(0.5Rn)		0.936	1.615	MHC158543		nm	from Hc2		6.8	11.3	um			1.3	2.2								MSP158543																																											Cu-intercalation					Superconductor derived from a topological insulator heterostructure			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 90(2014)220504	Satoshi Sasaki,Kouji Segawa,Yoichi Ando		
158544	PRB090220504	Cu intercalated - (PbSe)5(Bi2Se3)6	Cux(PbSe)5(Bi2Se3)6	C1.66Pb5Bi12Se23	C	1.66	Pb	5	Bi	12	Se	23																	2014																																														K																																																												MSP158544																																											Cu-intercalation					Superconductor derived from a topological insulator heterostructure			Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka 567-0047, Japan	Phys.Rev.B, 90(2014)220504	Satoshi Sasaki,Kouji Segawa,Yoichi Ando		
158545	PRB096144501	Tc = 7.55 K sample. dC(at Tc) = 62.1 mJ/mol.K. (dC/gamma*Tc) = 2.21. Hc(0) = 615 Oe	YB6	B6Y1	B	6	Y	1																				3	2017																												CaB6			A	4.1001														K		7.55				0.3	7.55											Oe	M-H curve		267						Oe			2850						Oe/K			559		MHC158545		A	from Hc2		340		A			1109		K	14.8	4.01	14							mJ/mol.K2	3.73														uOhm.cm							8.28																Y2O3(5N),amorphous B (2N5)		Induction zone melting using sintered rod, which are synthesized by thermal reaction					Lattice instability and enhancement of superconductivity in YB6			Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia and Moscow Institute of Physics and Technology, 9 Institutskiy Lane, 141700 Dolgoprudny, Moscow Region, Russia	Phys.Rev.B, 96(2017)144501	N. Sluchanko,V. Glushkov,S. Demishev,A. Azarevich,M. Anisimov,A. Bogach,V. Voronov,S. Gavrilkin,K. Mitsen,A. Kuznetsov,I. Sannikov,N. Shitsevalova,V. Filipov,M. Kondrin,S. Gabani,K. Flachbart		
158546	PRB096144501	Tc = 7.4 K sample. dC(at Tc) = 59 mJ/mol.K. (dC/gamma*Tc) = 2.1. Hc(0) = 610 Oe	YB6	B6Y1	B	6	Y	1																				3	2017																												CaB6			A	4.1001														K		7.4				0.12	7.4											Oe	M-H curve		267						Oe			2912						Oe/K			575				A	from Hc2		336.4		A			1130		K	14.6	3.99	14							mJ/mol.K2	3.79														uOhm.cm							9.68																Y2O3(5N),amorphous B (2N5)		Induction zone melting using sintered rod, which are synthesized by thermal reaction					Lattice instability and enhancement of superconductivity in YB6			Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia and Moscow Institute of Physics and Technology, 9 Institutskiy Lane, 141700 Dolgoprudny, Moscow Region, Russia	Phys.Rev.B, 96(2017)144501	N. Sluchanko,V. Glushkov,S. Demishev,A. Azarevich,M. Anisimov,A. Bogach,V. Voronov,S. Gavrilkin,K. Mitsen,A. Kuznetsov,I. Sannikov,N. Shitsevalova,V. Filipov,M. Kondrin,S. Gabani,K. Flachbart		
158547	PRB096144501	Tc = 6.6 K sample. dC(at Tc) = 29.3 mJ/mol.K. (dC/gamma*Tc) = 1.23. Hc(0) = 470 Oe	YB6	B6Y1	B	6	Y	1																				3	2017																												CaB6			A	4.1001														K		6.6				0.2	6.6											Oe	M-H curve		147						Oe			2927						Oe/K			623		MHC158547		A	from Hc2		335.5		A			1618		K	12.1	3.91	14							mJ/mol.K2	3.58														uOhm.cm							13.35																Y2O3(5N),amorphous B (2N5)		Induction zone melting using sintered rod, which are synthesized by thermal reaction					Lattice instability and enhancement of superconductivity in YB6			Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia and Moscow Institute of Physics and Technology, 9 Institutskiy Lane, 141700 Dolgoprudny, Moscow Region, Russia	Phys.Rev.B, 96(2017)144501	N. Sluchanko,V. Glushkov,S. Demishev,A. Azarevich,M. Anisimov,A. Bogach,V. Voronov,S. Gavrilkin,K. Mitsen,A. Kuznetsov,I. Sannikov,N. Shitsevalova,V. Filipov,M. Kondrin,S. Gabani,K. Flachbart		
158548	PRB096144501	Tc = 5.2 K sample. Tc(SP) = 4.2 K.  dC(at Tc) = 15.1 mJ/mol.K. (dC/gamma*Tc) = 1.39. Hc(0) = 211 Oe	YB6	B6Y1	B	6	Y	1																				3	2017																												CaB6			A	4.1001														K		5.2				0.45	5.2											Oe	M-H curve		50						Oe			2840						Oe/K			980				A	from Hc2		340.6		A			3242		K	6.2	2.65	14				MSP158548			mJ/mol.K2	2.09														uOhm.cm							25.6																Y2O3(5N),amorphous B (2N5)		Induction zone melting using sintered rod, which are synthesized by thermal reaction					Lattice instability and enhancement of superconductivity in YB6			Prokhorov General Physics Institute of RAS, 38 Vavilov Street, 119991 Moscow, Russia and Moscow Institute of Physics and Technology, 9 Institutskiy Lane, 141700 Dolgoprudny, Moscow Region, Russia	Phys.Rev.B, 96(2017)144501	N. Sluchanko,V. Glushkov,S. Demishev,A. Azarevich,M. Anisimov,A. Bogach,V. Voronov,S. Gavrilkin,K. Mitsen,A. Kuznetsov,I. Sannikov,N. Shitsevalova,V. Filipov,M. Kondrin,S. Gabani,K. Flachbart		
158549	PRB099054501	unit volume = 75.58 A^3. RRR = 27.1.	alpha-PdBi2	Bi2Pd1	Bi	2	Pd	1																				1	2019																													C2/m		A	12.557	4.1989	5.6553											monoclinic	K			1.6	1.6		0.17	1.6											Oe	M-H curve				40			0.5	Oe	RES8onset), WHH	290			260			0.5																																																																		Pd(5N),Bi(5N)		flux method. mixture - sealed in quartz tube - SIN(900 C, 24h) - cool to RT with the cooling rate of (2-3) C/h					Pressure-induced irreversible evolution of superconductivity in PdBi2			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 99(2019)054501	Ying Zhou,Xuliang Chen,Chao An,Yonghui Zhou,Langsheng Ling,Jiyong Yang,Chunhua Chen,Lili Zhang,Mingliang Tian,Zhitao Zhang,Zhaorong Yang		
158550	PRB099054501	data for P  = 17.1 GPa. Hc2 = 2.2 an d = 5.6 kOe for P = 3.3 and 42.8 GPa,respectively. For P>8 GPa, alpha- and beta- phase coexist.	PdBi2	Bi2Pd1	Bi	2	Pd	1																				1	2019																													I4/mmm		A	3.2037		11.937											alpha- phase + beta-phase	K			2.78				2.78	MTC158550																			kOe	RES8onset), WHH	6.2												MHC158550																																																												Pd(5N),Bi(5N)		flux method. mixture - sealed in quartz tube - SIN(900 C, 24h) - cool to RT with the cooling rate of (2-3) C/h					Pressure-induced irreversible evolution of superconductivity in PdBi2			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 99(2019)054501	Ying Zhou,Xuliang Chen,Chao An,Yonghui Zhou,Langsheng Ling,Jiyong Yang,Chunhua Chen,Lili Zhang,Mingliang Tian,Zhitao Zhang,Zhaorong Yang		
158551	PRB099054503	STM measurement. Two gaps. gap = 1.6 meV(in DB) and 0.9 meV, (2d/kTc) 3.72 (in DB)  and 2.09. magnetic field dependence of gap also measured.	MoGa41	Ga41Mo1	Ga	41	Mo	1																					2019																										AB41			R3[-]	148	A	9.5788													rhombohedral, alpha = beta = gamma = 94.974	K			10	10			10	MGAP158551																																													meV	1.6	3.72	11																																															solid state reaction. stoichiometric mixture - in quartz ampoule - heat(850C, in vac) - cool down slowly					Multiband superconductivity in Mo8Ga41 driven by a site-selective mechanism			1Department of Physical Sciences, Indian Institute of Science Education and Research (IISER) Mohali, Sector 81, S. A. S. Nagar, Manauli, PO 140306, India	Phys.Rev.B, 99(2019)054503	Anshu Sirohi,Surabhi Saha,Prakriti Neha,Shekhar Das,Satyabrata Patnaik,Tanmoy Das,Goutam Sheet		
158552	PRB099094512	Film. thickness = 40-50 nm. Tc and Hc not given explicitly in the text. DB value is tentative from R(T) figure. polycrystal of alpha- and alpha' phase.	Cd3As2 film	As2Cd3	As	2	Cd	3																					2019																										A2B3			I4<1>acd		A	12.6461	25.4378												alpha-phase	K		0.186					0.186																				Oe	RES(0.5Rn)													MHC158552																																																														magnetron nonreactive sputtering.using single crystal Cd3As2 on polished p-Si substrate at Ts = RT. deposition time = 20 min.					Observation of subkelvin superconductivity in Cd3As2 thin films			National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA	Phys.Rev.B, 99(2019)094512	A. V. Suslov,A. B. Davydov,L. N. Oveshnikov,L. A. Morgun,K. I. Kugel,V. S. Zakhvalinskii,E. A. Pilyuk,A. V. Kochura,A. P. Kuzmenko,V. M. Pudalov,B. A. Aronzon		
158553	PRB099094512	Film. thickness = 80 nm. Tc and Hc not given explicitly in the text. DB value is tentative from R(T) figure. polycrystal of alpha- and alpha' phase.	Cd3As2 film	As2Cd3	As	2	Cd	3																					2019																										A2B3			P4<2>nbc		A	12.6848	25.4887												alpha'-phase	K		0.185					0.185																				Oe	RES(0.5Rn)													MHC158553																																																														magnetron nonreactive sputtering.using single crystal Cd3As2 on Al2O3 substrate at Ts = RT. deposition time = 40 min.					Observation of subkelvin superconductivity in Cd3As2 thin films			National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA	Phys.Rev.B, 99(2019)094512	A. V. Suslov,A. B. Davydov,L. N. Oveshnikov,L. A. Morgun,K. I. Kugel,V. S. Zakhvalinskii,E. A. Pilyuk,A. V. Kochura,A. P. Kuzmenko,V. M. Pudalov,B. A. Aronzon		
158554	PRB099094512	Film. thickness = 40-50 nm. Tc and Hc not given explicitly in the text. DB value is tentative from R(T) figure. polycrystal of alpha- and alpha' phase.	Cd3As2 film	As2Cd3	As	2	Cd	3																					2019																										A2B3			I4<1>acd		A	12.6461	25.4378												alpha-phase	K		0.186					0.186																				Oe	RES(0.5Rn)													MHC158554																																																														magnetron nonreactive sputtering.using single crystal Cd3As2 on polished p-Si substrate at Ts = RT. deposition time = 20 min.					Observation of subkelvin superconductivity in Cd3As2 thin films			National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA	Phys.Rev.B, 99(2019)094512	A. V. Suslov,A. B. Davydov,L. N. Oveshnikov,L. A. Morgun,K. I. Kugel,V. S. Zakhvalinskii,E. A. Pilyuk,A. V. Kochura,A. P. Kuzmenko,V. M. Pudalov,B. A. Aronzon		
158555	NPJ00116014	P-induced SC. Pc = 8.5 GPa. Tc and Hc2 shows the values at P = 13.5 GPa. Hc2 measured for H perpendicular to (112) plane.	Cd3As2	As2Cd3	As	2	Cd	3																				3	2016																										A2B3																				K			3.55		0		3.55	MPH158555																			T	RES(0.9Rn), linear approx.			4.29																																																																								single crystals grown by CD flux method					Pressure-induced superconductivity in the three-dimensional topological Dirac semimetal Cd3As2			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai, China	NJP Quantum Materials, 1(2016)16014	Lanpo He,Yating Jia,Sijia Zhang,Xiaochen Hong,Changqing Jin,Shiyan Li		
158556	PRB099100501	P-induced SC . SC for 10.5 < P < 11.5. SC properties (DB) are for P = 11.4 GPa.	CeNiC2	Ce1Ni1C2	Ce	1	Ni	1	C	2																		1	2019																										ABC2	3		Amm2		A	3.882	4.556	6.172											orthorhombic	K	2.5		3.5		0		3	MPH158556																			T	RES(onset), GL	20							T/K	RES(onset)	7.1			MHC158556		A	from Hc2	42																																	uOhm.cm							23																Ce(3N),Ni(4N8),C(5N5)		Ar-arc furnace melting					Exotic superconductivity in noncentrosymmetric and magnetic CeNiC2 revealed under high pressure			Department of Physics, Graduate School of Science and Engineering, Saitama University, Sakura-ku, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 99(2019)100501	Susumu Katano,Masayuki Ito,Kohei Shibata,Jun Gouchi,Yoshiya Uwatoko,Kazuyuki Matsubayashi,Hideto Soeda,Hiroki Takahashi		
158557	PRB099134509	Type-I SC. RRR = 83.  (dC/gamma*Tc) = 1.51. SP (beta) = 0.076 mJ/mol.K4. kappa(GL) = 0.4. e-ph = 0.54. penet(L) = 450 A. Hc  defined as M(H) = 0 in M-H curve.	AuBe	Au1Be1	Au	1	Be	1																				1	2019																										AB		FeSi			A	4.6684														K	3.15	3.2	3.15	3.2			3.2										100										Oe	Type-I SC	259												MHC158557		A		2052			A		821					3.76	14				MSP158557			mJ/mol.K2	2.35	SP	370	SP											uOhm.cm	1.35										112												Au(5N),Be(5N)		arc-melting					Type-I superconductivity in the noncentrosymmetric superconductor BeAu			Indian Institute of Science Education and Research Bhopal, Bhopal, 462066, India	Phys.Rev.B, 99(2019)134509	D. Singh,A. D. Hillier,R. P. Singh		
158558	PRB099144511	Two phases: PtH-I  phase(SG = P321), and PtH-II phase (SG = P6<3>/mmc). PtH-II exhibit P-induced SC. Tc = 6.7 K(P = 32 GPa) , Tc = 4.8 K (P = 36 GPa)	PTH - II	H1Pt1	H	1	Pt	1																					2019																										AB			P6<3>/mmc		A	2.776		4.718											P = 41 GPa	K			6.7		0		6.7																																																																																														Pt foil(3N5), H2		(Pt + NH3BH3) - heat (1800C using IR laser, P = 30 GPa)					Superconductivity of platinum hydride			Department of Electrical, Electronic and Computer Engineering, Faculty of Engineering, Gifu University, Gifu 501-1193, Japan	Phys.Rev.B, 99(2019)144511	Takahiro Matsuoka,Masahiro Hishida,Keiji Kuno,Naohisa Hirao,Yasuo Ohishi,Shigeo Sasaki,Kazushi Takahama,Katsuya Shimizu		
158559	PRB099144519	R(T) = T^3.67 for T < 23 K. RRR = 375. Type-I SC. Hc not depends on H-direction. SP (dC<el>/gamma*Tc) = 1.37. Thermodynamic Hc(0) = 43 Oe.	Al6Re	Al6Re1	Al	6	Re	1																				3	2019																										AB6			Cmcm	63	A	7.599	6.602	9.04											T = 203 K.	K		0.74					0.74										95										Oe	Type-I SC	48												MHC158559																			MSP158559			mJ/mol.K2	3.9	SP	400	SP																																		Al(wire),Re(powder)		Al-flux method. (Al:Re = 200:1) - alumina crucible with Al2O3 lid - sealed under inside quartz tube - heat to 975 C - cool to 830 C (5 days)					Type-I superconductivity in Al6Re			State Key Laboratory of Surface Physics, Department of Physics; and Advanced Materials Laboratory, Fudan University, Shanghai 200438, China	Phys.Rev.B, 99(2019)144519	Darren C. Peets,Erjian Cheng,Tianping Ying,Markus Kriener,Xiaoping Shen,Shiyan Li,Donglai Feng		
158560	PRB099174513	gap measured by TF-muonSR. s-wave model analysis.	ZrIrSi	Zr1Ir1Si1	Zr	1	Ir	1	Si	1																		1	2019																										ABC	3		Pnma		A	6.557	3.942	7.413												K	1.7						1.7											mT		0.7							T		0.6																								meV	0.37	5.1	16																																													Zr(4N),Ir(4N),Si(5N)		arc-melting several times. ANN(1000 C,1week) in sealed quartz tube.					Probing the superconducting ground state of ZrIrSi: A muon spin rotation and relaxation study			Department of Physics, Ramakrishna Mission Vivekananda Educational and Research Institute, Howrah 711202, India	Phys.Rev.B, 99(2019)174513	K. Panda,A. Bhattacharyya,D. T. Adroja,N. Kase,P. K. Biswas,Surabhi Saha,Tanmoy Das,M. R. Lees,A. D. Hillier		
158561	PRB099184502	P-induced SC. Pcr = 47.8 GPa. SC data( in DB)  show for P = 47.8 GPa. RRR = 1.46 at Pcr.  Debye-T = 202 K from R(T) analysis	SnS	S1Sn1	S	1	Sn	1																				3	2019																										AB			Pnma																P = 0. beta-SnS(Cmcm) for P < 8.1 GPa, gamma-SnS(Pm-3m) for P > 18 GPa.	K			5.8		0		5.8																				T	RES(on), WHH	1.6														A	from Hc2	14																					202	R(T)																																		Sn(4N),S(4N)		stoichiometric composition - in ampoule - heat(350C,4 h) - heat (900 C,20 h) - cool to 830 C for 20 h - FC to RT.					Pressure-induced superconductivity in tin sulfide			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 99(2019)184502	Ryo Matsumoto,Peng Song,Shintaro Adachi,Yoshito Saito,Hiroshi Hara,Aichi Yamashita,Kazuki Nakamura,Sayaka Yamamoto,Hiromi Tanaka,Tetsuo Irifune,Hiroyuki Takeya,Yoshihiko Takano		
158562	PRB099184502	P-induced SC. Pcr = 30 GPa. Tc = 4.2 K (in DB) for P = 30 GPa. Insulator-to metal transition at 14 GPa.	SnSe	Se1Sn1	Se	1	Sn	1																				3	2019																										AB																				K			4.2		0		4.2																																																											92	R(T)																																				See J.Phys.Soc.Jpn. 87(2018)065001					Pressure-induced superconductivity in tin sulfide			International Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 99(2019)184502	Ryo Matsumoto,Peng Song,Shintaro Adachi,Yoshito Saito,Hiroshi Hara,Aichi Yamashita,Kazuki Nakamura,Sayaka Yamamoto,Hiromi Tanaka,Tetsuo Irifune,Hiroyuki Takeya,Yoshihiko Takano		
158563	PRB099184509	RRR = 37. (dC/gamma*Tc) = 1.54. e-ph = 0.453. Debye-T from R(T) analysis.	WP	P1W1	P	1	W	1																				3	2019																										AB	3	MnP	Pnma	62	A	5.722	3.2434	6.211												K		0.834	0.85			0.02	0.834																				mT	RES(mid), WHH	12.5												MHC158563		A	from Hc2	1642															MSP158563			mJ/mol.K2	1.355	SP	238	R(T)											uOhm.cm											40														CVT method. WP poly crystal in quartz tube, two zone furnace, 1100 C(source end), 1050 C (sink  end),  for 1 week, using iodine agent					Superconductivity in WP single crystals			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.B, 99(2019)184509	Ziyi Liu,Wei Wu,Zhenzheng Zhao,Hengcan Zhao,Jian Cui,Pengfei Shan,Jiahao Zhang,Changli Yang,Peijie Sun,Yuan Wei,Shiliang Li,Jinggeng Zhao,Yu Sui,Jinguang Cheng,Li Lu,Jianlin Luo,Guangtong Liu		
158564	PRB099184513	RRR = 45. SP (beta) = 0.67 mJ/mol.K4. e-ph = 0.72. (dC/gamma*Tc) = 1.44. Hc2(0) = 1.09 T from R(T) measurements, Debye-T = 251 K from R(T). kappa(GL) = 6.04	Mo3P	Mo3P1	Mo	3	P	1																				1	2019																										AB3	2		I4[-]2m	121	A	9.79094		4.826099											alpha-V3S type structure	K	5.5		5.7	5.5		0.2	5.5											mT	M-H curve, (1-t^2) fitting	29.4							T	SUS, SP, GL	0.94												MHC158564		nm	from Hc2	18.7			nm	Hc1,GL-eq.	113			meV	0.82	3.47	14				MSP158564			mJ/mol.K2	10.3	SP	225	SP											uOhm.cm							5.92																Mo(5N) powder,P pieces		solid state reaction. mixture - heat(1100 C,48 h) - reground - pellet - SIN(1100 C,48 h)					Nodeless superconductivity and preserved time-reversal symmetry in the noncentrosymmetric Mo3P superconductor			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.B, 99(2019)184513	T. Shang,J. Philippe,J. A. T. Verezhak,Z. Guguchia,J. Z. Zhao,L.-J. Chang,M. K. Lee,D. J. Gawryluk,E. Pomjakushina,M. Shi,M. Medarde,H.-R. Ott,T. Shiroka		
158565	PRB099224505	Y0.96Ni1.00Si3.09 by EPMA.  RRR = 54. SP (beta) = 0.096 mJ/mol.K4.. e-ph = 0.43. (dC/gamma*Tc) = 1.14. GL(kappa) = 0.113.	YNiSi3	Y1Ni1Si3	Y	1	Ni	1	Si	3																		3	2019																										ABC3																				K			1.42	1.36			1.36																				mT	M(T),(1-t^2) dependence	9.6												MHC158565		nm	BCS, xi(0)	780			nm	London	34													mJ/mol.K2	4.04	SP	466	SP											uOhm.cm							0.33																		Sn-flux method. (Y/Lu:Ni:Si:Sn = 1:1:3.5:45)					Superconductivity in monocrystalline YNiSi3 and LuNiSi3			CCNH, Universidade Federal do ABC (UFABC), Santo Andre, Sao Paulo, Brazil	Phys.Rev.B, 99(2019)224505	Fabiana R. Arantes,Deisy Aristizabal-Giraldo,Daniel A. Mayoh,Yu Yamane,Chongli Yang,Martin R. Lees,Jorge M. Osorio-Guillen,Toshiro Takabatake,Marcos A. Avila		
158567	PRB099224505	Lu1.00Ni0.68Si3.13 by EPMA.  RRR = 38. SP (beta) = 0.091 mJ/mol.K4.. e-ph = 0.44. (dC/gamma*Tc) = 0.71. GL(kappa) = 0.42.	LuNiSi3	Lu1Ni1Si3	Lu	1	Ni	1	Si	3																		3	2019																										ABC3																				K			1.63	1.63			1.63																				mT	M(T),(1-t^2) dependence	10.4												MHC158565		nm	BCS, xi(0)	690			nm	London	33													mJ/mol.K2	3.97	SP	474	SP											uOhm.cm							1.6																		Sn-flux method. (Y/Lu:Ni:Si:Sn = 1:1:3.5:45)					Superconductivity in monocrystalline YNiSi3 and LuNiSi3			CCNH, Universidade Federal do ABC (UFABC), Santo Andre, Sao Paulo, Brazil	Phys.Rev.B, 99(2019)224505	Fabiana R. Arantes,Deisy Aristizabal-Giraldo,Daniel A. Mayoh,Yu Yamane,Chongli Yang,Martin R. Lees,Jorge M. Osorio-Guillen,Toshiro Takabatake,Marcos A. Avila		
158568	PRB099245152	T<CDW> = 106.5 K	Nd1-xLaxNiC2	Nd0.9La0.1Ni1C2	Nd	0.9	La	0.1	Ni	1	C	2																1	2019					myu-B/f.u	3.56	-4.6	16.1																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158569	PRB099245152	T<CDW> = 83.0 K	Nd1-xLaxNiC2	Nd0.8La0.2Ni1C2	Nd	0.8	La	0.2	Ni	1	C	2																1	2019					myu-B/f.u	3.49	-16.3	15.2																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158570	PRB099245152	T<CDW> = 53.7 K	Nd1-xLaxNiC2	Nd0.7La0.3Ni1C2	Nd	0.7	La	0.3	Ni	1	C	2																1	2019					myu-B/f.u	3.15	-8	13.2																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8			MPH158570																																																																																													C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158571	PRB099245152		Nd1-xLaxNiC2	Nd0.6La0.4Ni1C2	Nd	0.6	La	0.4	Ni	1	C	2																1	2019					myu-B/f.u	2.72	-3	11.1																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158572	PRB099245152	SUS(T) shows sharp peak at Tn for x =< 0.5.	Nd1-xLaxNiC2	Nd0.5La0.5Ni1C2	Nd	0.5	La	0.5	Ni	1	C	2																1	2019					myu-B/f.u	2.56	-3.7	9.7																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158573	PRB099245152	SUS(T) shows broad peak at Tn for 0.6 =< x =< 0.8.	Nd1-xLaxNiC2	Nd0.4La0.6Ni1C2	Nd	0.4	La	0.6	Ni	1	C	2																1	2019					myu-B/f.u	2.31	-7.2	6.02																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158574	PRB099245152		Nd1-xLaxNiC2	Nd0.3La0.7Ni1C2	Nd	0.3	La	0.7	Ni	1	C	2																1	2019					myu-B/f.u	2.02	-121	3.68																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158575	PRB099245152		Nd1-xLaxNiC2	Nd0.2La0.8Ni1C2	Nd	0.2	La	0.8	Ni	1	C	2																1	2019					myu-B/f.u	1.68	-17.2	1.92																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158576	PRB099245152		Nd1-xLaxNiC2	Nd0.1La0.9Ni1C2	Nd	0.1	La	0.9	Ni	1	C	2																1	2019					myu-B/f.u	1.24	-29.8																			ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158577	PRB099245152		Nd1-xLaxNiC2	Nd0.04La0.96Ni1C2	Nd	0.04	La	0.96	Ni	1	C	2																1	2019					myu-B/f.u	0.65	-4.3																			ABC2		CeNiC2	Amm2																relative value a/a0 only	K		2.16	2.28	1.99			2.16	MTC158577																																																																																													C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158578	PRB099245152		Nd1-xLaxNiC2	Nd0.03La0.97Ni1C2	Nd	0.03	La	0.97	Ni	1	C	2																1	2019					myu-B/f.u	0.6	-8.1																			ABC2		CeNiC2	Amm2																relative value a/a0 only	K		2.36	2.46	2.16			2.36																																																																																														C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158579	PRB099245152		Nd1-xLaxNiC2	Nd0.02La0.98Ni1C2	Nd	0.02	La	0.98	Ni	1	C	2																1	2019							-1.1																			ABC2		CeNiC2	Amm2																relative value a/a0 only	K		2.66	2.8	2.75			2.66																																																																																														C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158580	PRB099245152		Nd1-xLaxNiC2	Nd0.01La0.99Ni1C2	Nd	0.01	La	0.99	Ni	1	C	2																1	2019																										ABC2		CeNiC2	Amm2																relative value a/a0 only	K		3.25	3.34	2.83			3.25																																																																																														C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158581	PRB099245152		LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2019																										ABC2		CeNiC2	Amm2																relative value a/a0 only	K		3.25	3.41	3			3.25																																																																																														C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158582	PRB099245152	T<CDW> = 120 K	NdNiC2	Nd1Ni1C2	Nd	1	Ni	1	C	2																		1	2019					myu-B/f.u	4.07	-23	16.7																		ABC2		CeNiC2	Amm2																relative value a/a0 only	K					1.8																																																																																																C(4N),Ni(5N),Nd(3N).La(4N)		arc-melting.  ANN(900 C,12 h)					Crossover from charge density wave stabilized antiferromagnetism to superconductivity in Nd1-xLaxNiC2 compounds			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland	Phys.Rev.B, 99(2019)245152	Marta Roman,Leszek Litzbarski,Tomasz Klimczuk,Kamil K. Kolincio		
158583	PRB100014507	P-induced SC. Pcr = 20.7 GPa. SC properties show for P = Pcr(20.7 GPa). Semicond -to-metal at 7 GPa. PdS2-type to pyrite at 16 GPa. SC in pyrite	PdS2	Pd1S2	Pd	1	S	2																				3	2019																										AB2		pyrite																	PdS2 type ,SG = Pbca at P = 0 GPa	K			2		0		2	MTC158583		K/GPa	0.35																																																																																										Pd(3N5),S(5N)		CVT method.  (Pd + S) - heat(550C,10d in silica tube), - CVT (600C(source)  to 500C(sink)  with PdCl2 as additive)					Pressure-induced metallization, transition to the pyrite-type structure, and superconductivity in palladium disulfide PdS2			Max Planck Institute for Chemical Physics of Solids, Dresden 01187, Germany	Phys.Rev.B, 100(2019)014507	M. A. ElGhazali,P. G. Naumov,Q. Mu,V. Suss,A. O. Baskakov,C. Felser,S. A. Medvedev		
158584	PRB100014507	not SC upto 50 GPa.	NiSe2	Ni1Se2	Ni	1	Se	2																				3	2019																										AB2		pyrite																	PdS2 type ,SG = Pbca at P = 0 GPa	K					1.4																																																																																																Ni(4N6),Se(5N)		CVT method.  (Pd + S) - heat(800C,10d in silica tube), - CVT (800C(source)  to 700C(sink)  with SeCl4 as additive)					Pressure-induced metallization, transition to the pyrite-type structure, and superconductivity in palladium disulfide PdS2			Max Planck Institute for Chemical Physics of Solids, Dresden 01187, Germany	Phys.Rev.B, 100(2019)014507	M. A. ElGhazali,P. G. Naumov,Q. Mu,V. Suss,A. O. Baskakov,C. Felser,S. A. Medvedev		
158585	PRB100024508	(dC/gamma*Tc) = 1.56	Pr1-xLaxPt4Ge12	Pr1Pt4Ge12	Pr	1	Pt	4	Ge	12																		1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6111														K		7.91					7.91																				T	SUS, H-sweep(onset)	2.07																																		mJ/mol.K2	87.1	SP	198	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158586	PRB100024508	(dC/gamma*Tc) = 1.56	Pr1-xLaxPt4Ge12	Pr0.9La0.1Pt4Ge12	Pr	0.9	La	0.1	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6134														K		7.85					7.85																				T	SUS, H-sweep(onset)	2.2												MHC158586																						mJ/mol.K2	76.3	SP	201.3	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158587	PRB100024508	(dC/gamma*Tc) = 1.67	Pr1-xLaxPt4Ge12	Pr0.7La0.3Pt4Ge12	Pr	0.7	La	0.3	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.615														K		7.87					7.87																				T	SUS, H-sweep(onset)	2.13												MHC158587														2.66	14							mJ/mol.K2	67.9	SP	203.7	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158588	PRB100024508	(dC/gamma*Tc) = 1.55	Pr1-xLaxPt4Ge12	Pr0.5La0.5Pt4Ge12	Pr	0.5	La	0.5	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6198														K		7.97					7.97																																																								mJ/mol.K2	70.5	SP	203.1	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158589	PRB100024508	(dC/gamma*Tc) = 1.54	Pr1-xLaxPt4Ge12	Pr0.3La0.7Pt4Ge12	Pr	0.3	La	0.7	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6213														K		8.02					8.02																				T	SUS, H-sweep(onset)	2.04												MHC158589														2.26	14							mJ/mol.K2	68.8	SP	216.4	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158590	PRB100024508	(dC/gamma*Tc) = 1.53	Pr1-xLaxPt4Ge12	Pr0.2La0.8Pt4Ge12	Pr	0.2	La	0.8	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6229														K		8.07					8.07																																																								mJ/mol.K2	67.2	SP	208.1	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158591	PRB100024508	(dC/gamma*Tc) = 1.53	Pr1-xLaxPt4Ge12	Pr0.1La0.9Pt4Ge12	Pr	0.1	La	0.9	Pt	4	Ge	12																1	2019																										AB4C12		skutterudite	Im3[-]		A	8.6222														K		8.22					8.22																																																								mJ/mol.K2	64.6	SP	207.9	SP																																									Broken time-reversal symmetry in superconducting Pr1-xLaxPt4Ge12			State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People's Republic of China	Phys.Rev.B, 100(2019)024508	J. Zhang,Z. F. Ding,K. Huang,C. Tan,A. D. Hillier,P. K. Biswas,D. E. MacLaughlin,L. Shu		
158592	PRB100041109	P-induced SC. Pcr = 56 GPa. Hc(0) = 1370 Oe (in DB) for P = 71 GPa. Tc = 2.1 K (DB) for P = 56 GPa. SC observed for  oC16 phase.	Rb	Rb1	Rb	1																						1	2019																										A			oC16																tI4 phase for  P < 50 GPa	K		2.1			0		2.1	MTC158592		K/GPa	-0.039																Oe	P = 71 GPa	1370												MHC158592																																																														Rb(2N75)  from Alfa Aesar					Evidence for superconductivity in Rb metal above 55 GPa pressure			Department of Physics, Washington University, St. Louis, Missouri 63130, USA	Phys.Rev.B, 100(2019)041109	Yuhang Deng,James S. Schilling		
158594	PRB100014503	NED measured. Lattice const. shows anomaly at Tc via strong e-ph interaction. Tc = 27 K (DB) for P = 24.7 kbar.	EuFe2As2	Eu1Fe2As2	Eu	1	Fe	2	As	2																		3	2019																										AB2C2		ThCr2Si2	I4/mmm																	K		27			0		27	MLAT158594																																																																																																				Coexistence of Eu antiferromagnetism and pressure-induced superconductivity in single-crystal EuFe2As2			Julich Centre for Neutron Science JCNS at Heinz Maier-Leibnitz Zentrum (MLZ), Forschungszentrum Julich GmbH, Lichtenbergstrasse 1, D-85747 Garching, Germany	Phys.Rev.B, 100(2019)014503	W. T. Jin,Y. Xiao,S. Nandi,S. Price,Y. Su,K. Schmalzl,W. Schmidt,T. Chatterji,A. Thamizhavel,Th. Bruckel		
158595	PRL117106601	Two channel Kondo material. vacancy in the Se-site.	ZrAs1.58Se0.39	Zr1As1.58Se0.39	Zr	1	As	1.58	Se	0.39																			2016																										ABC		PbFCl	P4/nmm																	K			0.14	0.14			0.14																																																					MSP158595			mJ/mol.K2	1.7	SP																																											Two-Channel Kondo Physics due to As Vacancies in the Layered Compound ZrAs1.58Se0.39			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, 50-950 Wroclaw, Poland	Phys.Rev.Lett., 117(2016)106601	T. Cichorek,L. Bochenek,M. Schmidt,A. Czulucki,G. Auffermann,R. Kniep,R. Niewa,F. Steglich,S. Kirchner		
158596	PRL117106601		ZrP1.54S0.46	Zr1P1.54S0.46	Zr	1	P	1.54	S	0.46																			2016																										ABC		PbFCl	P4/nmm																	K			3.9	3.9			3.9																																																					MSP158596			mJ/mol.K2	1.7	SP																																											Two-Channel Kondo Physics due to As Vacancies in the Layered Compound ZrAs1.58Se0.39			Institute of Low Temperature and Structure Research, Polish Academy of Sciences, 50-950 Wroclaw, Poland	Phys.Rev.Lett., 117(2016)106601	T. Cichorek,L. Bochenek,M. Schmidt,A. Czulucki,G. Auffermann,R. Kniep,R. Niewa,F. Steglich,S. Kirchner		
158597	PRL122067001		UBe13	Be13U1	Be	13	U	1																					2019																										AB13		NaZn13																		K			0.96	0.88			0.88	MTC158597																			T	various method													MHC158597																																																																			Spin-Triplet p-Wave Superconductivity Revealed under High Pressure in UBe13			Universite Grenoble Alpes, INAC/PHELIQS, CEA-Grenoble, F-38000 Grenoble, France	Phys.Rev.Lett., 122(2019)067001	Yusei Shimizu,Daniel Braithwaite,Dai Aoki,Bernard Salce,Jean-Pascal Brison		
158598	PRL122067001		UBe13	Be13U1	Be	13	U	1																					2019																										AB13		NaZn13																		K			0.96	0.88			0.88																				T	various method													MHC158598																																																																			Spin-Triplet p-Wave Superconductivity Revealed under High Pressure in UBe13			Universite Grenoble Alpes, INAC/PHELIQS, CEA-Grenoble, F-38000 Grenoble, France	Phys.Rev.Lett., 122(2019)067001	Yusei Shimizu,Daniel Braithwaite,Dai Aoki,Bernard Salce,Jean-Pascal Brison		
158600	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.30  . e-ph = 0.46  .	Re	Re1	Re	1																						1	2019																												Mg	P6<3>/mmc	194															hexagonal	K		1.69					1.69																																														kTc	1.71	3.42	14							mJ/mol.K2	2.3	SP	415	SP											uOhm.cm											20.1												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158601	PRM003024801	Composition: x = 0.18 by XRF.  Energy gap from SP analysis. (dC/gamma*Tc) =  1.18  . e-ph = 0.66  .	Re1-xMox	Re0.88Mo0.12	Re	0.88	Mo	0.12																				1	2019																												Mg	P6<3>/mmc	194	A	2.76798		4.48728											hexagonal	K		7.45					7.45																																														kTc	1.85	3.7	14							mJ/mol.K2	3.8	SP	402.9	SP																						40.1												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158602	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) = 0.98   . e-ph = 0.72  .	Re1-xMox	Re0.8Mo0.2	Re	0.8	Mo	0.2																				1	2019																												Mg	P6<3>/mmc	194															hexagonal	K		9.02					9.02																																														kTc	1.8	3.6	14							mJ/mol.K2	3.77	SP	363.7	SP																						49.9												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158603	PRM003024801	Composition: x = 0.29 by XRF.  centrosymmetric.  Energy gap from SP analysis. (dC/gamma*Tc) = 1.07   . e-ph = 0.77 .	Re1-xMox	Re0.77Mo0.23	Re	0.77	Mo	0.23																				1	2019																												alpha-Mn	I4[-]3m	217	A	9.58476													cubic	K		9.43					9.43																																														kTc	1.8	3.6	14							mJ/mol.K2	3.53	SP	333	SP																						69.1												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158604	PRM003024801	non-centrosymmetric.   Energy gap from SP analysis. (dC/gamma*Tc) = 1.90   . e-ph = 0.76 .	Re1-xMox	Re0.77Mo0.23	Re	0.77	Mo	0.23																				1	2019																												alpha-Mn	I4[-]3m	217	A	9.58476													cubic	K		8.65					8.65	MTC158608																																													kTc	2	4	14							mJ/mol.K2	3.66	SP	311.4	SP																																		Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158605	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) = 1.51  . e-ph = 0.63  .	Re1-xMox	Re0.65Mo0.35	Re	0.65	Mo	0.35																				1	2019																												alpha-Mn	I4[-]3m																	K		6.3					6.3																																														kTc	1.9	3.8	14							mJ/mol.K2	3.2	SP	391.1	SP																						63.6												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158606	PRM003024801	Composition: x = 0.47 by XRF.  Energy gap from SP analysis. (dC/gamma*Tc) = 1.44   . e-ph =  0.58 .	Re1-xMox	Re0.6Mo0.4	Re	0.6	Mo	0.4																				1	2019																												beta-CrFe	P4<2>/mnm	136	A	9.58514		4.9789											tetragonal	K		6.07					6.07																																														kTc	1.82	3.64	14				MSP158606			mJ/mol.K2	3.01	SP	520	SP																						60.4												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158607	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.59  . e-ph = 0.64  .	Re1-xMox	Re0.55Mo0.45	Re	0.55	Mo	0.45																				1	2019																												beta-CrFe	P4<2>/mnm																	K		6.6					6.6																																														kTc	1.85	3.7	14							mJ/mol.K2	3.45	SP	397.2	SP																						54.2												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158608	PRM003024801	Composition: x = 0.66 by XRF.  Energy gap from SP analysis. (dC/gamma*Tc) = 2.00  . e-ph = 0.87  .	Re1-xMox	Re0.4Mo0.6	Re	0.4	Mo	0.6																				1	2019																												W	Im3[-]m	229	A	3.12627													cubic	K		13					13	MTC158608																																													kTc	2.14	4.28	14				MSP158608			mJ/mol.K2	4.05	SP	341.8	SP																						26.9												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158609	PRM003024801	Composition: x = 0.70 by XRF.   Energy gap from SP analysis. (dC/gamma*Tc) =   1.96 . e-ph =  0.79 .	Re1-xMox	Re0.35Mo0.65	Re	0.35	Mo	0.65																				1	2019																												W	Im3[-]m																	K		12.05					12.05																																														kTc	2.1	4.2	14							mJ/mol.K2	3.89	SP	397.3	SP																						23.5												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158610	PRM003024801	Composition: x = 0.80 by XRF.   Energy gap from SP analysis. (dC/gamma*Tc) =  1.64  . e-ph = 0.69  .	Re1-xMox	Re0.25Mo0.75	Re	0.25	Mo	0.75																				1	2019																												W	Im3[-]m																	K		10.3					10.3																																														kTc	1.9	3.8	14							mJ/mol.K2	3.69	SP	480.6	SP																						27.1												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158611	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.51  . e-ph = 0.68  .	Re1-xMox	Re0.2Mo0.8	Re	0.2	Mo	0.8																				1	2019																												W	Im3[-]m																	K		8.5					8.5																																														kTc	1.87	3.74	14							mJ/mol.K2	3.65	SP	420.7	SP																						16.01												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158612	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.50  . e-ph =  0.62 .	Re1-xMox	Re0.15Mo0.85	Re	0.15	Mo	0.85																				1	2019																												W	Im3[-]m																	K		6.74					6.74																																														kTc	1.85	3.7	14							mJ/mol.K2	3.41	SP	436.2	SP																						14.1												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158613	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.35  . e-ph = 0.51  .	Re1-xMox	Re0.1Mo0.9	Re	0.1	Mo	0.9																				1	2019																												W	Im3[-]m																	K		3.02					3.02	MTC158608																																													kTc	1.8	3.6	14							mJ/mol.K2	2.39	SP	429.9	SP																						11.47												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158614	PRM003024801	Energy gap from SP analysis. (dC/gamma*Tc) =  1.25  . e-ph =  0.41 .	Mo	Mo1	Mo	1																						1	2019																												W	Im3[-]m																	K		0.92					0.92																																														kTc	1.7	3.4	14							mJ/mol.K2	1.83	SP	460	SP																						5.98												Mo,Re		arc-melting several times to homogeneity. ANN(900 C, 2 weeks)					Structure and superconductivity in the binary Re1-xMox alloys			Laboratory for Multiscale Materials Experiments, Paul Scherrer Institut, Villigen CH-5232, Switzerland	Phys.Rev.Mater.,3(2019)024801	T. Shang,D. J. Gawryluk,J. A. T. Verezhak,E. Pomjakushina,M. Shi,M. Medarde,J. Mesot,T. Shiroka		
158615	PRM003024802	Compositions = Y7Ru3.67In0.86Ge11.2 by EDS. RRR = 3. Anisotropy(Hc2) = 2.2. (dC/gamma*Tc) = 2.4.  SP (beta) = 3.55 mJ/mol.K4, (delta) = 7.48 uJ/mol.K6. e-ph = 0.73	Y7Ru4InGe12	Y7Ru4In1Ge12	Y	7	Ru	4	In	1	Ge	12																3	2019	emu/mol	0.00088							7.129																	AB4C7D12	2		P4/m		A	10.5348		4.2239											tetragonal, volume = 468.78 A^3	K	5.6		5.8	5.8			5.8											Oe	H-M curve						33	2	T	RES(0.9Rn), WHH		2.4	5.3					T/K	RES(0.9Rn)		0.62	1.35	MHC158615		A	from Hc2		78.8	174								4.36	14							mJ/f.u.K2	43	SP	236	SP											mOhm.cm							0.026				0.079												Ru(5N),Y(3N8),Ge(5N),In(5N)		(Y:Ru:Ge:In = 7:4:12:63) - alumina crucible - covered stailess frit - fused silica tube - heat(1000C,10 h) - hold (1000 C, 12h) - cool to 500 C with 2 C/h					Superconductivity in Y7Ru4InGe12			Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys.Rev.Mater.,3(2019)024802	Jin-Ke Bao,Daniel E. Bugaris,Huihuo Zheng,Kristin Willa,Ulrich Welp,Duck Young Chung,Mercouri G. Kanatzidis		
158616	PRM003074201	TF muSR shows nodeless SC. [penet] and energy gap are obtained.   ZF muSR shows triplet paring	Sr0.1Bi2Se3	Sr0.1Bi2Se3	Sr	0.1	Bi	2	Se	3																		3	2019																																														K		2.5					2.5																																									nm	muSR	1622			meV	0.49	4.36	16																																															single crystals grown by modified Bridgeman method. mixture - in quartz ampoule(vac) - heat(850 C,8 d) -slow cool to 650 C (10 C/h) - Q to ices water					Time-reversal symmetry breaking in topological superconductor Sr0.1Bi2Se3			School of Physical Sciences, Jawaharlal Nehru University, New Delhi-110067, India	Phys.Rev.Mater.,3(2019)074201	P. Neha,P. K. Biswas,Tanmoy Das,S. Patnaik		
158617	SCM0580543	R(T) anomaly at about 50 K. Curie-Weiss for 100 < T < 280 K. cluster spin glass below 6 K.  R(4K)/R(300K) = 8.64	RbCr3As3	Rb1Cr3As3	Rb	1	Cr	3	As	3																		1	2015	emu/mol-Cr	0.00067			myu-B/Cr	1.22	-79																			AB3C3			P6<3>/m	176	A	9.334		4.1775												K					2																																																										mJ/mol.K2	89	SP													mOhm.cm											2														single crystals grown using chemical vapor transport method (CVT) in Oarai					Synthesis, crystal structure and physical properties of quasi-one-dimensional ACr3As3 (A = Rb, Cs)			Department of Physics, Zhejiang University, Hangzhou 310027, China	Sci. China Mater.,  58(2015)543	Zhang-Tu Tang,Jin-Ke Bao,Yi Liu,Hua Bai,Hao Jiang,Hui-Fei Zhai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
158618	SCM0580543	R(T) anomaly at about 50 K. cluster spin glass below 5 K.  R(4K)/R(300K) = 19.9	CsCr3As3	Cs1Cr3As3	Cs	1	Cr	3	As	3																		1	2015					myu-B/Cr	1.59	-80																			AB3C3			P6<3>/m	176	A	9.632		4.1814												K					2																																																										mJ/mol.K2	185	SP													mOhm.cm											60														single crystals grown using chemical vapor transport method (CVT) in Oarai					Synthesis, crystal structure and physical properties of quasi-one-dimensional ACr3As3 (A = Rb, Cs)			Department of Physics, Zhejiang University, Hangzhou 310027, China	Sci. China Mater.,  58(2015)543	Zhang-Tu Tang,Jin-Ke Bao,Yi Liu,Hua Bai,Hao Jiang,Hui-Fei Zhai,Chun-Mu Feng,Zhu-An Xu,Guang-Han Cao		
158619	SST02903LT02	RRR = 16.9	LaBi3	Bi3La1	Bi	3	La	1																				1	2016																										AB3		AuCu3			A	4.99														K	7.4			7.3			7.3	MTC158619		K/GPa	-0.26						111										T	R(mid), Linear approx.	1.7							T/K	R(mid)	0.238			MHC158619		A	from Hc2	139																																																								LaBi,Bi		starting compositions (La:Bi = 1.3:3) - press into pellet - in BN crucible - heat(450C, 1 h, P = 3.4 GPa)					Superconductivity in LaBi3 with AuCu3-type structure			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)03LT02	Tatsuya Kinjo,Saori Kajino,Taichiro Nishio,Kenji Kawashima,Yousuke Yanagi,Izumi Hase,Takashi Yanagisawa,Shigeyuki Ishida,Hijiri Kito,Nao Takeshita,Kunihiko Oka,Hiroshi Eisaki,Yoshiyuki Yoshida,Akira Iyo		
158620	SST029055004	RH(20K) = -0.861 E-3 cm^3/C.	ZrP2-xSex	Zr1P1.6Se0.4	Zr	1	P	1.6	Se	0.4																		1	2016																												PBFCl			A	3.6216		7.9127												K		3.98		3.5			3.98																				T	RES(0.9Rn), GL	0.99												MHC158622																																					mOhm.cm							0.127																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158621	SST029055004	RH(20K) = -0.673 E-3 cm^3/C.	ZrP2-xSex	Zr1P1.5Se0.5	Zr	1	P	1.5	Se	0.5																		1	2016																												PBFCl			A	3.629		7.9151												K		5.19		5.33			5.19																				T	RES(0.9Rn), GL	1.39												MHC158622																																					mOhm.cm							0.112																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158622	SST029055004	RH(20K) = -0.594 E-3 cm^3/C.	ZrP2-xSex	Zr1P1.4Se0.6	Zr	1	P	1.4	Se	0.6																		1	2016																												PBFCl			A	3.6396		7.9209												K		6.28		6.2			6.28	MTC158622																			T	RES(0.9Rn), GL	1.93												MHC158622																																					mOhm.cm							0.186																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158623	SST029055004	RH(20K) = -0.193 E-3 cm^3/C.	ZrP2-xSex	Zr1P1.3Se0.7	Zr	1	P	1.3	Se	0.7																		1	2016																												PBFCl			A	3.6503		7.9347												K		6.22		5.99			6.22																				T	RES(0.9Rn), GL	2.46												MHC158624																																					mOhm.cm							0.343																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158624	SST029055004	RH(20K) = -0.136 E-3 cm^3/C.	ZrP2-xSex	Zr1P1.2Se0.8	Zr	1	P	1.2	Se	0.8																		1	2016																												PBFCl			A	3.6562		7.9572												K		5		5			5																				T	RES(0.9Rn), GL	1.72												MHC158624																																					mOhm.cm							0.399																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158625	SST029055004		ZrP2-xSex	Zr1P1.1Se0.9	Zr	1	P	1.1	Se	0.9																		1	2016																																														K		4.61		4.19			4.61																				T	RES(0.9Rn), GL	1.68												MHC158624																																					mOhm.cm							0.439																Zr(3N),P(5N),Se(5N)		mixture(Zr:P:Se = 1:(2-x):x) - SIN(1300-1400 C, P = 2 GPa)					Superconductivity in layered ZrP2-xSex with PbFCl-type structure			National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Ibaraki 305-8568, Japan	Supercond.Sci.Technol., 29(2016)055004	Shigeyuki Ishida,Hiroshi Fujihisa,Izumi Hase,Yousuke Yanagi,Kenji Kawashima,Kunihiko Oka,Yoshito Gotoh,Yoshiyuki Yoshida,Akira Iyo,Hiroshi Eisaki,Hijiri Kito		
158626	SST030025015	Hc(0) = 5.015 kOe. Hc2(0) = 22 kOe from RES(0.9Rn) and WHH.  (dC<el>/gamma*Tc) = 1.05.  kappa(GL) = 2.074.	BaBi3	Ba1Bi3	Ba	1	Bi	3																				3	2017																										AB3		AuCu3	P4/mmm		A	5.06		5.13											tetragonal distorted AuCu3 phase	K			6				6	MTC158626		K/GPa	1.22						100	Oe	H-M curve	1710							T	M-H curve, (1-t^2)	1.47												MHC158626		A	from Hc2	149			A	GL(kappa)	309													mJ/mol.K2	3.2	SP	171	SP											mOhm.cm							0.15																Ba(3N5),Sr(3N5),Bi(4N)		Bi-self flux method. Ba(or Sr):Bi = 1:4,  sealed in quartz tube (vac) - heat slowly to 600C and keep 10 h - cool to 350 C with 2 C/h - remove excess Bi					Hydrostatic pressure effect on the superconducting properties of BaBi3 and SrBi3 single crystals			CCNH, Universidade Federal do ABC (UFABC), Santo Andre, SP, 09210-580 Brazil	Supercond.Sci.Technol., 30(2017)025015	Rajveer Jha,Marcos A Avila,Raquel A Ribeiro		
158627	SST030025015	Hc(0) = 357 Oe. Hc2(0) = 2.9 kOe from RES(0.9Rn) and WHH.  (dC<el>/gamma*Tc) = 2.08.   kappa(GL) = 1.76.	SrBi3	Bi3Sr1	Bi	3	Sr	1																				3	2017																										AB3		AuCu3	Pm-3m		A	5.05													cubic phase	K			5.6				5.6	MTC158627		K/GPa	-0.41						80	Oe	H-M curve	210							T	M-H curve, (1-t^2)	0.089												MHC158627		A	from Hc2	608			A	GL(kappa)	1070													mJ/mol.K2	6.5	SP	180	SP											uOhm.cm							5.3																Ba(3N5),Sr(3N5),Bi(4N)		Bi-self flux method. Ba(or Sr):Bi = 1:4,  sealed in quartz tube (vac) - heat slowly to 600C and keep 10 h - cool to 350 C with 2 C/h - remove excess Bi					Hydrostatic pressure effect on the superconducting properties of BaBi3 and SrBi3 single crystals			CCNH, Universidade Federal do ABC (UFABC), Santo Andre, SP, 09210-580 Brazil	Supercond.Sci.Technol., 30(2017)025015	Rajveer Jha,Marcos A Avila,Raquel A Ribeiro		
158628	SST031085001		Zr5Ge3	Ge3Zr5	Ge	3	Zr	5																				1	2018																										A3B5		Mn5Si3																		K					1.8																																																																																																Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158629	SST031085001		Zr5Ge2.5Pd0.5	Zr5Ge2.5Pd0.5	Zr	5	Ge	2.5	Pd	0.5																		1	2018																										A3B5		Mn5Si3																		K					1.8																																																																																																Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158630	SST031085001	R(T) shows small drop at 1.8 K due to SC of Zr-Ir alloy (SEM)	Zr5Ge2.5Ir0.5	Zr5Ge2.5Ir0.5	Zr	5	Ge	2.5	Ir	0.5																		1	2018																										A3B5		Mn5Si3																		K					1.8																																																																																																Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158631	SST031085001	Tc(SP) = 2.5 K. SP (beta) = 0.48 mJ/mol.K4. (dC/gamma*Tc) = 0.72	Zr5Ge2.5Pt0.5	Zr5Ge2.5Pt0.5	Zr	5	Ge	2.5	Pt	0.5																		1	2018																										A3B5		Mn5Si3																		K			2.8			0.1	2.8										70		H-M curve				20			1.8	T	RES(0.9Rn), WHH	4.3												MHC158631																						mJ/mol.K2	16.15	SP	325	SP																																		Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158632	SST031085001	SC might already be induced  for x < 0.2 with Tc  < 2K, in Zr5Ge3-xPtx	Zr5Ge2.8Pt0.2	Zr5Ge2.8Pt0.2	Zr	5	Ge	2.8	Pt	0.2																		1	2018																										A3B5		Mn5Si3																		K			2.6			0.1	2.6																																																																																														Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158633	SST031085001	For x > 1, phase separation appears in Zr5Ge3-xPtx	Zr5Ge2Pt	Zr5Ge2Pt1	Zr	5	Ge	2	Pt	1																		1	2018																										A3B5		Mn5Si3																		K			3.5			0.5	3.5																																																																																														Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158634	SST031085001	Pt in Zr site. not SC	Zr4.5Pt0.5Ge3	Zr4.5Ge3Pt0.5	Zr	4.5	Ge	3	Pt	0.5																		1	2018																										A3B5		Mn5Si3																		K					1.8																																																																																																Zr(2N8),Ge(4N),Pt(3N)		arc-melting with Zr-getter. remelt several times (weight loss (<1%) - into Nb tube - in quartz tube - ANN (1000 C, 1 w)					Superconductivity and phase diagram in a transition metal doped Zr5Ge3 compound			Department of Physics, The University of Texas at Dallas, Richardson, TX 75080, United States of America	Supercond.Sci.Technol., 31(2018)085001	Sheng Li,Xiaoyuan Liu,Varun Anand,Bing Lv		
158635	SST031105002	P-induced SC. Pc = 9 GPa. The large shrinkage of the Fe-ladder unit.	BaFe2S3	Ba1Fe2S3	Ba	1	Fe	2	S	3																		1	2018																		GPa		46						AB2C3		LAD													(dL/L)/GPa	0.00552	0.0113	0.00362	two leg ladder structure	K			24		0		24																																																																																																solid state reaction					Crystal structure determination under high pressure in the iron-based ladder superconductor BaFe2S3			Condensed Matter Research Center, Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK), Tsukuba, Ibaraki 305-0801, Japan	Supercond.Sci.Technol., 31(2018)105002	Kensuke Kobayashi,Sachiko Maki,Youichi Murakami,Yasuyuki Hirata,Kenya Ohgushi,Jun-ichi Yamaura		
158636	SST031125008	Tn = 106 K. T<STR> = 106 K by R(T) measurement.	(La,Na)Fe2As2	La0.34Na0.66Fe2As2	La	0.34	Na	0.66	Fe	2	As	2																3	2018								106																		AB2C2		ThCr2Si2	I4/m		A	3.8676		12.287												K	26.9		27.3	27			27																				T	RES(0.9Rn),WHH		128	67					T/K	RES(0.9Rn)		6.8	3.6	MHC158636																																																			m3/C	0.000000000154										starting material = LaFeAs(O,F):NaAs:NaF = 1:17:11. mixture - sealed in Ta tube(ar) - sealed in quartz tube(vac) - heat(1150C,10h) - cool to 700C with 2 C/h					Single-crystal growth of the iron-based superconductor La0.34Na0.66Fe2As2			Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 31(2018)125008	Yanhong Gu,Jia-Ou Wang,Xiaoyan Ma,Huiqian Luo,Youguo Shi,Shiliang Li		
158700	SCIR00739699	P-induced SC. Pcr = 8 GPa. Tc(14 GPa) = 4.5 K. (dTc/dP) = -0.14 K/Gpa at Pcr. Hc2(0)//c = 2.9 T (P = 14 GPa) and = 2.8 T (26 GPa).	BiTeI	Bi1Te1I1	Bi	1	Te	1	I	1																		3	2017																										ABC			P3m1		A	4.3392		6.854											trigonal	K			5.3		0		5.3	MTC158700		K/GPa	-0.14																T	RES(on), WHH, P=14 GPa			2.9										MHC158700																																																														Bridgeman method. stoichiometric mixture - sealed in quartz(vac) - heat (600 C,24h) - cool to 100 C (12 C/h) - q to RT					Superconductivity Bordering Rashba Type Topological Transition			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.	Sci.Rep., 7(2017)39699	M. L. Jin,F. Sun,L. Y. Xing,S. J. Zhang,S. M. Feng,P. P. Kong,W. M. Li,X. C. Wang,J. L. Zhu,Y. W. Long,H. Y. Bai,C. Z. Gu,R. C. Yu,W. G. Yang,G. Y. Shen,Y. S. Zhao,H. K. Mao,C. Q. Jin		
158701	PRB095184503	R(T) = R0 + A*T^2.  Tc(zero) depends linearly on root(A). coeff. = 170 K/(uOhm.cm)^(0.5)	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				1	2017																										AB3		Cr3Si(A15)																		K	17.49	17.75	17.9				17.75	MTC158701																																																																						uOhm.cm							9.7																		HIP (hot isostatic pressure) synthesis. react (1250 C, 24 h, at 250 MPa) - cool to 0 C with 30 C/h					Evolution of T2 resistivity and superconductivity in Nb3Sn under pressure			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 95(2017)184503	Z. Ren,L. Gamperle,A. Fete,C. Senatore,D. Jaccard		
158702	PRB095184503	R(T) = R0 + A*T^2.  Tc(zero) depends linearly on root(A). coeff. = 51 K/(uOhm.cm)^(0.5)	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				3	2017																										AB3		Cr3Si(A15)																		K	17.06	17.29	17.48				17.29	MTC158702																																																																						uOhm.cm							0.71																		single crystals grown by Iodine vapor transport method					Evolution of T2 resistivity and superconductivity in Nb3Sn under pressure			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 95(2017)184503	Z. Ren,L. Gamperle,A. Fete,C. Senatore,D. Jaccard		
158704	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 280 K.	Eu3Bi2S4-xSexF4	Eu3Bi2S4F4	Eu	3	Bi	2	S	4	F	4																1	2015					myu-B/Eu	7.28		2.16																		A2B3C4D4			I4/mmm	139	A	4.0774		32.4328												K		1.45					1.45																																																																																					m3/C	-0.00000000303					MRH158708										Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158705	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 269 K.	Eu3Bi2S4-xSexF4	Eu3Bi2S3.8Se0.2F4	Eu	3	Bi	2	S	3.8	Se	0.2	F	4														1	2015					myu-B/Eu	7.23																				A2B3C4D4			I4/mmm	139	A	4.0838		32.4528												K		1.78					1.78																																																																																																					Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158706	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 209 K.	Eu3Bi2S4-xSexF4	Eu3Bi2S3.4Se0.6F4	Eu	3	Bi	2	S	3.4	Se	0.6	F	4														1	2015					myu-B/Eu	7.02																				A2B3C4D4			I4/mmm	139	A	4.0929		32.4826												K		2.17					2.17	MTC158706																																																																																																				Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158707	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 175 K.  Tn1 = 2.15 K, Tn2 = 1.48 K.	Eu3Bi2S4-xSexF4	Eu3Bi2S3Se1F4	Eu	3	Bi	2	S	3	Se	1	F	4														1	2015					myu-B/Eu	6.96		2.15																		A2B3C4D4			I4/mmm	139	A	4.1017		32.5035												K		2.39					2.39																																																																																																					Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158708	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 118 K.  Tn1 = 2.3 K, Tn2 = 0.6 K. SP (beta) = 3.44 mJ/mol.K4.	Eu3Bi2S4-xSexF4	Eu3Bi2S2.5Se1.5F4	Eu	3	Bi	2	S	2.5	Se	1.5	F	4														1	2015					myu-B/Eu	6.92	-2.67	2.3																		A2B3C4D4			I4/mmm	139	A	4.1171		32.5477												K		2.72					2.72																																																					MSP158708			mJ/mol.K2	18.1	SP	194.2	SP																									m3/C	-0.000000000272					MRH158708										Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158709	EPL11127002	T*(dR/dT anomaly, maybe CDW transition) = 64 K.	Eu3Bi2S4-xSexF4	Eu3Bi2S2Se2F4	Eu	3	Bi	2	S	2	Se	2	F	4														1	2015					myu-B/Eu	6.77																				A2B3C4D4			I4/mmm	139	A	4.1295		32.6263												K		3.26					3.26										100																																																																																											Superconductivity enhanced by Se doping in Eu3Bi2(S,Se)4F4			Department of Physics and State Key Laboratory of Silicon Materials, Zhejiang University Hangzhou 310027, China	Europhys.Lett., 111(2015)27002	P. Zhang,H. F. Zhai,Z. J. Tang,L. Li,Y. K. Li,Q. Chen,J. Chen,Z. Wang,C. M. Feng,G. H. Cao,Z. A. Xu		
158710	INO0570037	not SC above 0.3 K. broad hump appears  at 250 K in R(T).	EuSr2Bi2S4-xSexF4	Eu1Sr2Bi2S3.5Se0.5F4	Eu	1	Sr	2	Bi	2	S	3.5	Se	0.5	F	4												1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158711	INO0570037	not SC above 0.3 K.	EuSr2Bi2S4-xSexF4	Eu1Sr2Bi2S3Se1F4	Eu	1	Sr	2	Bi	2	S	3	Se	1	F	4												1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158712	INO0570037	not SC above 0.3 K.	EuSr2Bi2S4-xSexF4	Eu1Sr2Bi2S2.5Se1.5F4	Eu	1	Sr	2	Bi	2	S	2.5	Se	1.5	F	4												1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158713	INO0570037	bulk SC. broad hump  in R(T) disappears.	EuSr2Bi2S4-xSexF4	Eu1Sr2Bi2S2Se2F4	Eu	1	Sr	2	Bi	2	S	2	Se	2	F	4												1	2018																										A2B3C4D4			I4/mmm																	K	2.46	2.94	2.3				2.94																				T	RES(0.9Rn), WHH	0.585							T/K	RES(0.9Rn)	0.287																																																															EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158714	INO0570037	not SC above 0.3 K.	Eu2SrBi2S4-xSexF4	Eu2Sr1Bi2S4F4	Eu	2	Sr	1	Bi	2	S	4	F	4														1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158715	INO0570037	not SC above 0.3 K.	Eu2SrBi2S4-xSexF4	Eu2Sr1Bi2S3.5Se0.5F4	Eu	2	Sr	1	Bi	2	S	3.5	Se	0.5	F	4												1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158716	INO0570037	not SC above 0.3 K.	Eu2SrBi2S4-xSexF4	Eu2Sr1Bi2S3Se1F4	Eu	2	Sr	1	Bi	2	S	3	Se	1	F	4												1	2018																										A2B3C4D4			I4/mmm																	K					0.3																																																																																																EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158717	INO0570037	not bulk SC (diamagnetic signal not observed).	Eu2SrBi2S4-xSexF4	Eu2Sr1Bi2S2.5Se1.5F4	Eu	2	Sr	1	Bi	2	S	2.5	Se	1.5	F	4												1	2018																										A2B3C4D4			I4/mmm																	K	2.1		2.6				2.35																				T	RES(0.9Rn), WHH	0.8							T/K	RES(0.9Rn)	0.45																																																															EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158718	INO0570037	not bulk SC (diamagnetic signal not observed).	Eu2SrBi2S4-xSexF4	Eu2Sr1Bi2S2Se2F4	Eu	2	Sr	1	Bi	2	S	2	Se	2	F	4												1	2018																										A2B3C4D4			I4/mmm																	K	2.35		2.8				2.575																																																																																														EuF3,EuF2,SrF2,BiS3,BiSe3,Bi		solid state reaction.  mixture - pellet - heat(1123 K,30 h, in quartz ampule). Impurity phases are Bi2S3, Bi2Se3, EuF2.4					Valence State of Eu and Superconductivity in Se-Substituted EuSr2Bi2S4F4 and Eu2SrBi2S4F4			Department of Chemistry, Indian Institute of Technology, New Delhi 110016, India	Inorganic Chem.,57(2018)37	Zeba Haque,Gohil Singh Thakur,Ganesan Kalai Selvan,Theresa Block,Oliver Janka,Rainer Pottgen,Amish G. Joshi,Rangasamy Parthasarathy,Sonachalam Arumugam,Laxmi Chand Gupta,Ashok Kumar Ganguli		
158719	INO0575364	Volume fraction of tetra-phase = 100 %	Ce1-xPrxOBiS2	Ce1Bi1S2O1	Ce	1	Bi	1	S	2															O	1		1	2018																										ABCD2	2		P4/nmm		A	4.01002		13.5602											at 100K, a = 4.00018, c = 13.5422	K	1.3						1.3																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158720	INO0575364	Volume fraction of tetra-phase = 100 %	Ce1-xPrxOBiS2	Ce0.9Pr0.1Bi1S2O1	Ce	0.9	Pr	0.1	Bi	1	S	2													O	1		1	2018																										ABCD2																				K	1.4						1.4																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158721	INO0575364	Volume fraction of tetra-phase = 76 %	Ce1-xPrxOBiS2	Ce0.7Pr0.3Bi1S2O1	Ce	0.7	Pr	0.3	Bi	1	S	2													O	1		1	2018																										ABCD2																				K	2.12						2.12																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158722	INO0575364	Volume fraction of tetra-phase = 55 %	Ce1-xPrxOBiS2	Ce0.5Pr0.5Bi1S2O1	Ce	0.5	Pr	0.5	Bi	1	S	2													O	1		1	2018																										ABCD2	2		P4/nmm		A	4.00363		13.6088											at 100K, a = 3.99299, c = 13.5831 A	K	2.21						2.21																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158723	INO0575364	Volume fraction of tetra-phase = 37 %	Ce1-xPrxOBiS2	Ce0.3Pr0.7Bi1S2O1	Ce	0.3	Pr	0.7	Bi	1	S	2													O	1		1	2018																										ABCD2																				K	1.92						1.92																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158724	INO0575364	Volume fraction of tetra-phase = 9 %. R(T) not to zero down to 0.1 K.	Ce1-xPrxOBiS2	Ce0.1Pr0.9Bi1S2O1	Ce	0.1	Pr	0.9	Bi	1	S	2													O	1		1	2018																										ABCD2																				K			2				2																																																																																														Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158725	INO0575364	monoclinic not  SC.	Ce1-xPrxOBiS2	Pr1Bi1S2O1	Pr	1	Bi	1	S	2															O	1		1	2018																										ABCD2			P2<1>/m		A	4.01269	4.00837	13.8371											monoclinic beta = 90.276 deg. At 100K, monoclinic, a=4.01231, b=3.99363, c=13.8371, beta = 90.200 drg	K					0.1																																																																																																Bi2O3,Bi2S3,Ce2S3,Pr2S3		mixture - ground - press to pellet - sealed in quartz tube - heat(700 C, 20 h) - FC to RT					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158726	INO0575364	single crystal. Bi:Ce:Pr = 1:0.5:0.5, distributed homogeneously by SEM and EDX	Ce0.5Pr0.5OBiS2	Ce0.5Pr0.5Bi1S2O1	Ce	0.5	Pr	0.5	Bi	1	S	2													O	1		3	2018																										ABCD2	2		P4/nmm																	K		2.4		2.4			2.4																																																																																																single crystal grown by CsCl flux method. mixture with CsCl flux - sealed in quartz tube - heat(950 C, 10 h) - cool to 650 C (1 C/h) - remove flux					Crystal Structure and Superconductivity of Tetragonal and Monoclinic Ce1-xPrxOBiS2			Faculty of Engineering, Hokkaido University, Kita 13, Nishi 8, Sapporo 060-8628, Japan	Inorganic Chem.,57(2018)5364	Akira Miura,Masanori Nagao,Yosuke Goto,Yoshikazu Mizuguchi,Tatsuma D. Matsuda,Yuji Aoki,Chikako Moriyoshi,Yoshihiro Kuroiwa,Yoshihiko Takano,Satoshi Watauchi,Isao Tanaka,Nataly Carolina Rosero-Navarro,Kiyoharu Tadanaga		
158727	JAC7870414	SP (beta) = 0.022 mJ/mol.K4. e-ph = 0.36.	Nb1-xNixB2	B2Nb1	B	2	Nb	1																				1	2019																										AB2	7	AlB2	P6/mmm		A	3.1125		3.2653											hexagonal	K				1.3			1.3																																																								mJ/mol.K2	2.217	SP	642	SP																																		Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158728	JAC7870414		Nb1-xNixB2	Nb0.99Ni0.01B2	Nb	0.99	Ni	0.01	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.1042		3.2475											hexagonal	K				3.9			3.9																																																																																														Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158729	JAC7870414		Nb1-xNixB2	Nb0.97Ni0.03B2	Nb	0.97	Ni	0.03	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.0991		3.2379											hexagonal	K				4.3			4.3																																																																																														Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158730	JAC7870414		Nb1-xNixB2	Nb0.95Ni0.05B2	Nb	0.95	Ni	0.05	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.0956		3.2272											hexagonal	K				4.6			4.6	MTC158730																																																																																													Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158731	JAC7870414		Nb1-xNixB2	Nb0.93Ni0.07B2	Nb	0.93	Ni	0.07	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.0897		3.2254											hexagonal	K				5.1			5.1																																																																																														Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158732	JAC7870414	SP (beta) = 0.046 mJ/mol.K4	Nb1-xNixB2	Nb0.91Ni0.09B2	Nb	0.91	Ni	0.09	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.0869		3.2226											hexagonal	K			6.5	6			6											Oe	M-H curve, linear	116							kOe	RES(on), M(T), linear fitting	8.2																																		mJ/mol.K2	3.602	SP	500	SP																																		Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158733	JAC7870414		Nb1-xNixB2	Nb0.9Ni0.1B2	Nb	0.9	Ni	0.1	B	2																		1	2019																										AB2	7	AlB2	P6/mmm		A	3.0882		3.2237											hexagonal	K				5.4			5.4																																																																																														Nb(4N),Ni(4N),B(4N)		arc-melting					Evidence of unconventional superconductivity in the Ni-doped NbB2 system			Universidad de Salamanca - Departamento de Fisica Fundamental, Nanolab - Grupo de Nanotecnologia, Salamanca, 37008, Spain	J.Alloys Compd., 787(2019)414	S.T. Renosto,R. Lang,E. Diez,L.E. Correa,M.S. da Luz,Z. Fisk,A.J.S. Machado		
158734	JPCM026212201	RRR = 50. SP (beta) = 1.44 mJ/mol.K4.  (dC/Tc) = 2.6 mJ/mol.K2. (dC/gamma*Tc) = 0.78. e-ph = 0.62. DOS = 0.88 states/eV.fu.	NaBi	Bi1Na1	Bi	1	Na	1																				1	2014																										AB	2		P4/mmm																	K		2.15		2.15		0.15	2.15											Oe	M-H curve				30			0.4	Oe	RES(mid), H-sweep, WHH	250												MHC158734		nm	from Hc2	115															MSP158734			mJ/mol.K2	3.4	SP	140	SP																																		Bi(5N),Na(3N5)		mixture(Bi:Na = 1:1) - sealed in metallic tube(arc-welded) - heat to 600 C(60 C/h) - hold(12 h) - Q to iced water - ANN(400 C, 24 h)					Superconducting properties and electronic structure of NaBi			Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	J.Phys.Condens.Matter,  26(2014)212201	S K Kushwaha,J W Krizan,J Xiong,T Klimczuk,Q D Gibson,T Liang,N P Ong,N P Ong		
158735	JPCM026395701	SP measured for 0.35<T<3.0 K . SP (beta) = 2.6 mJ/mol.K4, (delta) = 0.32 mJ/mol.K6. (dC/Tc) = 21.7 mJ/mol.K2. (dC/gamma*Tc) = 1.30.  Tc(SP) = 0.46 K.	CoBi3	Bi3Co1	Bi	3	Co	1																				1	2014																										AB3			Pnma	62	A	8.8464	4.0697	11.5604												K			0.48			0.03	0.48																				kOe	RES(0.9Rn), WHH	2.25							kOe/K	RES(0.9Rn)	6.72					nm	from Hc2	39																		mJ/mol.K2	17.9	SP	144	SP											uOhm.cm	225						225				800												Bi(5N),Co(4N)		High-T-high-P synthesis, (370 - 1200 C) (5.0 - 10 GPa),					CoBi3-the first binary compound of cobalt with bismuth: high-pressure synthesis and superconductivity			CNRS, ICMCB, UPR 9048, F-33600 Pessac, France	J.Phys.Condens.Matter,  26(2014)395701	S Tence,O Janson,C Krellner,H Rosner,U Schwarz,Y Grin,F Steglich		
158736	JPCM027185701	SP (beta) = 0.32 mJ/mol.K4.  (dC/gamma*Tc) = 0.89. Hc(0) = 0.06 T.kappa(GL) = 10.6. e-ph = 0.79. N(ef) = 3.49 stats /ev.fu.	CaIr2	Ca1Ir2	Ca	1	Ir	2																				1	2015																										AB2		MgCu2(Laves)																	C15. Ir atoms have pyrochlore lattice.	K		5.8		5.8			5.8											Oe	M-H curve, (1-t^2) fitting	381							T	RES(mid), empirical	4							T/K	RES(mid)	0.81			MHC158736		A	from Hc2	90.7			A		960										MSP158736			mJ/mol.K2	8.36	SP	160	SP											mOhm.cm											9.6												Ca(4N),Ir(4N)		Two step reaction. starting(200% excess Ca) - in alumina crucible(Ar) - sealed in quartz tube - heat (850 C, 20h) - ground with excess Ca - pellet - heat (700 C,12h)					Characterization of the heavy metal pyrochlore lattice superconductor CaIr2			Department of Chemistry, Princeton University, Princeton, NJ 08544, USA	J.Phys.Condens.Matter,  27(2015)185701	Neel Haldolaarachchige,Quinn Gibson,Leslie M Schoop,Huixia Luo,R J Cava		
158737	JPCM030075601	Hc(0) = 62.4 mT. kappa(GL) = 61.1. SP (beta) = 0.039 mJ/mol.K4. (dC/gamma*Tc) = 1.48. [penet] = 6538 A from muSR.	Nb0.5Os0.5	Nb0.5Os0.5	Nb	0.5	Os	0.5																				1	2018																												alpha-Mn	I4[-]3m	217	A	9.765														K	3.1			3.07			3.07										100	mT	M-H curve, (1-t^2) fitting	3.06							T	SP, M(T), GL fitting	5.4							T/K	SP,M(T)	2.1			MHC158737		A	from Hc2	78.12			A	Hc1,GL eq.	4774					3.62	14				MSP158737			mJ/mol.K2	3.42	SP	367	SP																																		Nb(3N5),Os(3N5)		arc-melting. ANN(1000 C, 5 d, in evacuated quartz tube)					Superconducting properties and muon-SR study of the noncentrosymmetric superconductor Nb0.5Os0.5			Indian Institute of Science Education and Research Bhopal, Bhopal, 462066, India	J.Phys.Condens.Matter,  30(2018)075601	D Singh,J A T Barker,A Thamizhavel,A D Hillier,D McK Paul,R P Singh		
158738	JPCM031035701	RRR = 16.4. (dTc/dP) = -0.55 K/GPa at P=2 GPa. For P=0 in DB. Hc2 data for H perpendicular to b-axis.	NiBi3	Bi3Ni1	Bi	3	Ni	1																				1	2019																										AB3	3	NiBi3	Pnma																orthorhombic	K	4.1			4.1			4.1	MTC158738		K/GPa	-0.35																T	H normal to b-axis								T/K	RES, H normal to b-axis	0.105			MHC158738																																																												Ni(4N),Bi(4N)		mixture(Ni:Bi = 1:9 mol-ratio) - alumina crucible - sealed in silica ampule - heat to 1000C(3h) - hold(1000 C,3h) - rapid cool to 600 C(3h) - hold(600 C,3h) - slow cool to 320 C over 40h					Effect of pressure on the physical properties of the superconductor NiBi3			Ames Laboratory, Iowa State University, Ames, IA 50011, United States of America	J.Phys.Condens.Matter,  31(2019)035701	Elena Gati,Li Xiang,Lin-Lin Wang,Soham Manni,Paul C Canfield,Sergey L Bud'ko		
158739	JPS0644849	RRR = 8. H*  shows peak effect field  in M(H) curve. Anisotropy, Hc2//<100> = 6.48 T, Hc2//<110> = 6.56 T at 1.5 K. penet = 1100 ~ 1400 A.	CeRu2	Ce1Ru2	Ce	1	Ru	2																				3	1995																										AB2		MgCu2(Laves)																		K		6.18					6.18																				T	RES. H//<110>		7.4			2.8		4.25						MHC158739		A	from Hc2		67		A	Hc1, cohere, GL		1100																																																		Ce(4N),Ru(3N)		zone melting method.					Superconducting Properties of CeRu2 Single Crystal			Faculty of Science, Tokyo Metropolitan University, Minami-Osawa 1-1 Hachioji, Tokyo 192-03	J.Phys.Soc. Jpn, 64(1995)4849	Hitoshi Sugawara,Hideyuki Sato,Tsuyoshi Yamazaki,Noriaki Kimura,Rikio Settai,Yoshichika Onuki		
158740	JPS0644849	Fig shows  H* is peak effect field in M(H) curve.  H* appears for T < 5.0 K.Hc2 and H* of for #158740.	CeRu2	Ce1Ru2	Ce	1	Ru	2																				3	1995																										AB2		MgCu2(Laves)																		K		6.17					6.17																																		MHC158740																																																												Ce(4N),Ru(4N)		zone melting method. ANN at melting point - q uench					Superconducting Properties of CeRu2 Single Crystal			Faculty of Science, Tokyo Metropolitan University, Minami-Osawa 1-1 Hachioji, Tokyo 192-03	J.Phys.Soc. Jpn, 64(1995)4849	Hitoshi Sugawara,Hideyuki Sato,Tsuyoshi Yamazaki,Noriaki Kimura,Rikio Settai,Yoshichika Onuki		
158741	JPS084124702	RRR = 350, where J//<100>.  (dC) = 120 mJ/mol.K. (dC/gamma*Tc) = 1.56 where Tc(SP) = 5.5 K. Several dHvA branches are observed.	SrBi3	Bi3Sr1	Bi	3	Sr	1																				3	2015																										AB3		AuCu3			A	5.042														K		5.9					5.9																																																								mJ/mol.K2	14	SP													uOhm.cm							0.21																Sr(3N),Bi(6N)		Bi-self flux method. starting(Sr:Bi = 14:86) - alumina crucible - in quartz tube - heat(800 C) - slow cool from 560 to 300 C(total 10 days) - remove excess Bi.					Fermi Surface Properties Based on the Relativistic Effect in SrBi3 with AuCu3-Type Cubic Structure			Graduate School of Engineering and Science, University of the Ryukyus, Nishihara, Okinawa 903-0213, Japan	J.Phys.Soc. Jpn, 84(2015)124702	Masashi Kakihana,Hiromu Akamine,Tomoyuki Yara,Atsushi Teruya,Ai Nakamura,Tetsuya Takeuchi,Masato Hedo,Takao Nakama,Yoshichika ?nuki,Hisatomo Harima		
158742	JPS088083705	SP (beta = 2.81 mJ/mol.K2. residual (gamma) = 53.0 mJ/mol.K2. (dC/gamma*Tc) = 1.6. SP anomaly detected upto 36 T for magnetic hard axis (H//b)	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2																			UTe2-type	K		1.65					1.65																																																					MSP158742			mJ/mol.K2	123.5	SP																																						CVT method					Thermodynamic Investigation of Metamagnetism in Pulsed High Magnetic Fields on Heavy Fermion Superconductor UTe2			The Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan	J.Phys.Soc. Jpn, 88(2019)083705	Shusaku Imajo,Yoshimitsu Kohama,Atsushi Miyake,Chao Dong,Masashi Tokunaga,Jacques Flouquet,Koichi Kindo,Dai Aoki		
158743	JPS088093709	vols = 39 % at 0.07 K. SP (beta) = 0.346 mJ/mol.K4 for 2 < T < 4.5K.	PtSbS	Pt1Sb1S1	Pt	1	Sb	1	S	1																		1	2019																										ABC		FeS2(pyrite)	P2<1>3		A	6.17													ullmannite-type structure. ordered pyrite	K	0.15		0.18	0.12			0.12										39										Oe	RES(zero), GL	620												MHC158743		nm	from Hc2	73																		mJ/mol.K2	4.22	SP	256	SP											mOhm.cm							0.27																Pt(3N),Sb(3N),S(4N)		solid state reaction. mixture - press - sealed in quartz tube - heat (400 C,24 h) - heat (750 C,3 h) - hold (500 C,24 h) - FC to RT					Superconductivity in PtSbS with a Noncentrosymmetric Cubic Crystal Structure			Department of Applied Physics, Nagoya University, Nagoya 464-8603, Japan	J.Phys.Soc. Jpn, 88(2019)093709	Ryosuke Mizutani,Yoshihiko Okamoto,Hayate Nagaso,Youichi Yamakawa,Hiroshi Takatsu,Hiroshi Kageyama,Shunichiro Kittaka,Yohei Kono,Toshiro Sakakibara,Koshi Takenaka		
158744	JPS088113702	not SC. <75>As-NMR measured. Fig shows (1/T1*T) vs T.	La0.5-xNa0.5+xFe2As2	La0.5Na0.5Fe2As2	La	0.5	Na	0.5	Fe	2	As	2																1	2019								130																		AB2C2		ThCr2Si2																		K					4																																																																																																		polycrystals synthesized using a cubic-anvil-type high pressure apparatus.					Unconventional Multi-gap Superconductivity and Antiferromagnetic Spin Fluctuations in New Iron-arsenide LaFe2As2 in Heavily Electron-doped Regime			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc. Jpn, 88(2019)113702	Takayoshi Kouchi,Mitsuharu Yashima,Hidekazu Mukuda,Shigeyuki Ishida,Hiroshi Eisaki,Yoshiyuki Yoshida,Kenji Kawashima,Akira Iyo		
158745	JPS088113702	<75>As-NMR measured. Fig shows (1/T1*T) vs T.	La0.5-xNa0.5+xFe2As2	La1Fe2As2	La	1	Fe	2	As	2																		1	2019																										AB2C2		ThCr2Si2																		K				9.4			9.4	TNMR158745																																																																																															polycrystals synthesized using a cubic-anvil-type high pressure apparatus.					Unconventional Multi-gap Superconductivity and Antiferromagnetic Spin Fluctuations in New Iron-arsenide LaFe2As2 in Heavily Electron-doped Regime			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc. Jpn, 88(2019)113702	Takayoshi Kouchi,Mitsuharu Yashima,Hidekazu Mukuda,Shigeyuki Ishida,Hiroshi Eisaki,Yoshiyuki Yoshida,Kenji Kawashima,Akira Iyo		
158746	JPS088113702	<75>As-NMR measured. Fig shows (1/T1*T) vs T.	La0.5-xNa0.5+xFe2As2	La0.2Na0.8Fe2As2	La	0.2	Na	0.8	Fe	2	As	2																1	2019																										AB2C2		ThCr2Si2																		K				27			27																																																																																																polycrystals synthesized using a cubic-anvil-type high pressure apparatus.					Unconventional Multi-gap Superconductivity and Antiferromagnetic Spin Fluctuations in New Iron-arsenide LaFe2As2 in Heavily Electron-doped Regime			Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan	J.Phys.Soc. Jpn, 88(2019)113702	Takayoshi Kouchi,Mitsuharu Yashima,Hidekazu Mukuda,Shigeyuki Ishida,Hiroshi Eisaki,Yoshiyuki Yoshida,Kenji Kawashima,Akira Iyo		
158747	JPS088113703	<125>Te-NMR. Knight shift shows two gap model of two point nodes is better. d1 = 3.8 kTc (in DB) and d2 = 0.28 kTc.	UTe2	Te2U1	Te	2	U	1																				3	2019																										AB2																			UTe2-type	K				1.65			1.65																				T	SUS.					5	1.34							MHC158747														7.6	6																																															cubic anvil type HP apparatus. mixture(la1.1Fe2As2.1) - press to pellet - in BN crucible - heat(960C,15h,P=3.4 GPa) - rapid cooling (100 C/min)					Superconducting Properties of Heavy Fermion UTe2 Revealed by <125>Te-nuclear Magnetic Resonance			Depertment of Phisics, Kyoto University, Kyoto 606-8502, Japan	J.Phys.Soc. Jpn, 88(2019)113703	Genki Nakamine,Shunsaku Kitagawa,Kenji Ishida,Yo Tokunaga,Hironori Sakai,Shinsaku Kambe,Ai Nakamura,Yusei Shimizu,Yoshiya Homma,Dexin Li,Fuminori Honda,Dai Aoki		
158748	JPCL0101018	Collapsed tetragonal(as-synthesized). Impurity phase: LaAs. Compositions : La:Fe:As = 1.02:1.80:2.0.  RRR = 15.5	LaFe2As2	La1Fe2As2	La	1	Fe	2	As	2																		1	2019																										AB2C2		ThCr2Si2	I4/mmm		A	4.0035		11.0144												K				7.4			7.4										40																																																																																				LaAs,FeAs		cubic anvil type HP apparatus. mixture(la1.1Fe2As2.1) - press to pellet - in BN crucible - heat(960C,15h,P=3.4 GPa) - rapid cooling (100 C/min)					Superconductivity in Uncollapsed Tetragonal LaFe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Chem.Lett., 10(2019)1018	Akira Iyo,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Izumi Hase,Yoshiyuki Yoshida,Hiroshi Eisaki,Kenji Kawashima		
158749	JPCL0101018	Uncollapsed tetragonal(as-annealed). Impurity phase: LaAs increased.  Compositions : La:Fe:As = 1.01:1.94:2.0.  RRR = 2.3	LaFe2As2	La1Fe2As2	La	1	Fe	2	As	2																		1	2019																										AB2C2		ThCr2Si2	I4/mmm		A	3.9376		11.7317												K		12.2	13	12.1			12.2										100										T	RES(mid), WHH	15							T/K	RES(mid)	1.77			MHC158749																																																												LaAs,FeAs		cubic anvil type HP apparatus. mixture(la1.1Fe2As2.1) - press to pellet - in BN crucible - heat(960C,15h,P=3.4 GPa) - rapid cooling (100 C/min)- ANN					Superconductivity in Uncollapsed Tetragonal LaFe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Phys.Chem.Lett., 10(2019)1018	Akira Iyo,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Izumi Hase,Yoshiyuki Yoshida,Hiroshi Eisaki,Kenji Kawashima		
158750	ACS1400369	not SC	La0.5-xNa0.5+xFe2As2	La0.7Na0.3Fe2As2	La	0.7	Na	0.3	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8745		12.134												K					5			MLAT158750																																																																						mOhm.cm											2.91												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 940 C for  x < 0).					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158751	ACS1400369	not SC	La0.5-xNa0.5+xFe2As2	La0.6Na0.4Fe2As2	La	0.6	Na	0.4	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8724		12.141												K					5																																																																									mOhm.cm											1.45												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 940 C for  x < 0).					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158752	ACS1400369	T<STR> = Tn = 131 K (tetra-to-ortho)	La0.5-xNa0.5+xFe2As2	La0.5Na0.5Fe2As2	La	0.5	Na	0.5	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8744		12.1631												K					5																																																																									mOhm.cm											1.74												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158753	ACS1400369	T<STR> = Tn = 112.9 K (tetra-to-ortho). SC trace below 15 K.	La0.5-xNa0.5+xFe2As2	La0.4Na0.6Fe2As2	La	0.4	Na	0.6	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8621		12.2082												K					5																																																																									mOhm.cm											2.1												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158754	ACS1400369	bulk-Tc for x >=0.15 in La0.5-xNa0.5+xFe2As2.	La0.5-xNa0.5+xFe2As2	La0.3Na0.7Fe2As2	La	0.3	Na	0.7	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8515		12.2604												K				22.1			22.1																																																																							mOhm.cm											2.21												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158755	ACS1400369		La0.5-xNa0.5+xFe2As2	La0.2Na0.8Fe2As2	La	0.2	Na	0.8	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8439		12.3149												K				27			27	MPH158755									122																																																													mOhm.cm											2.16												LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158756	ACS1400369		La0.5-xNa0.5+xFe2As2	La0.15Na0.85Fe2As2	La	0.15	Na	0.85	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8382		12.3305												K				26			26																																																																																														LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158757	ACS1400369		La0.5-xNa0.5+xFe2As2	La0.1Na0.9Fe2As2	La	0.1	Na	0.9	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8421		12.3393												K					5																																																																																																LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158758	ACS1400369		La0.5-xNa0.5+xFe2As2	La0.05Na0.95Fe2As2	La	0.05	Na	0.95	Fe	2	As	2																1	2018																										AB2C2		ThCr2Si2	I4/mmm		A	3.8397		12.3445												K					5																																																																																																LaAs,NaAs,Fe2As,FeAs		mixture - ground in N2 - (5 at% excess As added) - pellet - wrapped in Ta foil - in SUS pipe with cap - heat at Ts ( = 900 - 200x for 0 =< x =<0.5.					Superconductivity on Hole-Doping Side of (La0.5-xNa0.5+x)Fe2As2			National Institute of Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J.Am.Chem.Soc., 140(2018)369	Akira Iyo,Kenji Kawashima,Shigeyuki Ishida,Hiroshi Fujihisa,Yoshito Gotoh,Hiroshi Eisaki,Yoshiyuki Yoshida		
158759	PCCP01821737	RRR = 200.  SP (beta) = 1.21 mJ/mol.K4. (dC/Tc) = 6.4 mJ/mol.K2. gamma(residual) = 0.5 mJ/mol.K2. Type-I SC. Hc defined as M goes to normal value ( H/n/b-axis). e-ph = 0.59. DOS = 1.07 states/eV.fu	CaBi2	Bi2Ca1	Bi	2	Ca	1																				1	2016									8.225																	AB2	3	ZrSi2	Cmcm		A	4.696	17.081	4.611											orthorhombic, ZrSi2 type. cell vol = 369.9 A^3	K		2		1.95			2																				Oe	SUS, (1-t^2 fitting	124												MHC158759												meV	0.23		14				MSP158759			mJ/mol.K2	4.6	SP	157	SP																																		Ca(2N5),Bi(4N)		(Ca:Bi = 3:17) - carbon coated quartz tube (Ar) - heat(550 C,8h) - slow cool to 310 C  (3 C/h) - remove the excess Bi					Superconductivity in CaBi2			Faculty of Applied Physics and Mathematics, Gdansk University of Technology, Narutowicza 11/12, 80-233 Gdansk, Poland.	Phys.Chem.Chem.Phys., 18(2016)21737	M. J. Winiarski,B. Wiendlocha,S. Gotab,S. K. Kushwaha,P. Wisniewski,D. Kaczorowski,J. D. Thompson,R. J. Cava,T. Klimczuk		
158760	PHB2370068	The sample of 4 month intercalation has Tc = 2 K(onset) and shows mwtallic behavior below 60 K. Li-content not given.	LixKCaNb3O10	Li0.1K1Ca1Nb3O10	Li	0.1	K	1	Ca	1	Nb	3													O	10			1997																																													triple layered NbO6 octahedra	K	1.5		2				1.75																																																																																														K2CO3,CaCO3,Nb2O5		mixture with 10%-excess K2CO3 - pellet - CAL(1150 C,10 h, in air. Li-intercalation using n-butyl lithium n-hexane solution					Transport properties of Li intercalated KCa2Nb3O10			Institute for Solid State Physics, University of Tokyo, Minato-ku, Japan	Physica B, 237-238(1997)68	Yoshihiko Takano,Hiroyuki Taketomi,Haruto Tsurumi,Tokio Yamadaya,Nobuo Mori		
158761	PHC3000067	Average ompositions of 10 grains  are Eu:Nb:S = 17.2:22:61 by EDX .	EuNb2S5	Eu1Nb2S5	Eu	1	Nb	2	S	5																			1998																										AB2C5																				K				3			3										80																																																																																						samples synthesized by heating (1100 C, 48 h) in silica tube					A new superconducting sulfide-EuNb2S5	199805		Chemical Department, Moscow State University, 119899 Moscow, Russian Federation	Physica.C,300(1998)67-70	A. Yu. Grippa,E.V. Antipov,G. Svensson,J.L. Tholence,O.G. D'yachenko,S.Ya. Istomin		
158762	PHC5651353518		Pb2-xBixPd	Pb2Pd1	Pb	2	Pd	1																				1	2019																										AB2	2	CuAl2			A	6.873		5.834											cell volume = 275.587 A^3	K			3	3			3																																																																																														Pb,Bi,Pd		mixture - ground - encapsulated into quartz tube - SIN(1273 K, 24 h) - cool to RT					Bi substitution effect on superconductivity of novel Pb2Pd alloy			Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, 230026, China	Physica C, 565(2019)1353518	Wang Miao,Tang Kaibin		
158763	PHC5651353518		Pb2-xBixPd	Pb1.8Bi0.2Pd1	Pb	1.8	Bi	0.2	Pd	1																		1	2019																										AB2	2	CuAl2			A	6.881		5.85											cell volume = 276.986 A^3	K			3.3	3.3			3.3																																																																																														Pb,Bi,Pd		mixture - ground - encapsulated into quartz tube - SIN(1273 K, 24 h) - cool to RT					Bi substitution effect on superconductivity of novel Pb2Pd alloy			Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, 230026, China	Physica C, 565(2019)1353518	Wang Miao,Tang Kaibin		
158764	PHC5651353518		Pb2-xBixPd	Pb1.6Bi0.4Pd1	Pb	1.6	Bi	0.4	Pd	1																		1	2019																										AB2	2	CuAl2			A	6.884		5.875											cell volume = 278.413 A^3	K			2.8	2.8			2.8																																																																																														Pb,Bi,Pd		mixture - ground - encapsulated into quartz tube - SIN(1273 K, 24 h) - cool to RT					Bi substitution effect on superconductivity of novel Pb2Pd alloy			Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, 230026, China	Physica C, 565(2019)1353518	Wang Miao,Tang Kaibin		
158765	PHC5651353518		Pb2-xBixPd	Pb1.4Bi0.6Pd1	Pb	1.4	Bi	0.6	Pd	1																		1	2019																										AB2	2	CuAl2			A	6.876		5.891											cell volume = 278.523 A^3	K			3.3	3.3			3.3																																																																																														Pb,Bi,Pd		mixture - ground - encapsulated into quartz tube - SIN(1273 K, 24 h) - cool to RT					Bi substitution effect on superconductivity of novel Pb2Pd alloy			Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, 230026, China	Physica C, 565(2019)1353518	Wang Miao,Tang Kaibin		
158766	PRB082094517	RRR = 13. SP (beta) = 0.83 mJ/mol.K4,  (delta) = 0.01 mJ/mol.K6, (dC/gamma*Tc) = 2.19. kappa(GL) = 4.1	YSn3	Sn3Y1	Sn	3	Y	1																				1	2010																										AB3		AuCu3	Pm3[-]m		A	4.667														K	7		7.3	7			7											Oe	M-H curve, (1-t^2) fitting	90							Oe	RES(mid), WHH	3000							Oe/K	RES(mid)	600			MHC158766		nm	from Hc2	66			nm	from Hc1	270										MSP158766			mJ/mol.K2	7.57	SP	210	SP																																		Y(3N),Sn(5N)		mixture - encapsuled in hBN.  High-T-High-P synthesis, (700 C, 2-10 min, P=5.5 GPa) - (470 C, 10-30 min, P = 5.5 GPa) - Q to RT					Superconducting state in YSn3 with a AuCu3-type structure			Department of Physics and Mathematics, Aoyama Gakuin University, Fuchinobe 5-10-1, Sagamihara, Kanagawa 229-8558, Japan	Phys.Rev.B, 82(2010)094517	K. Kawashima,M. Maruyama,M. Fukuma,J. Akimitsu		
158767	PRB090220508	RRR = 20. Hydrostatic P. (dTc/dP) for P < 4 GPa. For P > 4 GPa, P-induced phase (PI-phase) appears , then Tc decreases  and goes to zero below 8GPa. dT<PI>/dP = 51.5 K/GPa.	LaNiC2	La1Ni1C2	La	1	Ni	1	C	2																		1	2014																										ABC2	3	CeNiC2	Amm2		A	3.952	4.557	6.193												K	2.8						2.8	MTC158767		K/GPa	0.25																																																																			uOhm.cm	8.5																						La(3N),Ni(4N7),C(5N5)		arc-melting					Anomalous pressure dependence of the superconductivity in noncentrosymmetric LaNiC2: Evidence of strong electronic correlations			Department of Physics, Graduate School of Science and Engineering, Saitama University, Sakura-ku, Saitama, Saitama 338-8570, Japan	Phys.Rev.B, 90(2014)220508	Susumu Katano,Hideya Nakagawa,Kazuyuki Matsubayashi,Yoshiya Uwatoko,Hideto Soeda,Takahiro Tomita,Hiroki Takahashi		
158768	PRB091214512	P = 0.3 GPa. T<CDW> = 260 K.	EuBiS2F	Eu1Bi1S2F1	Eu	1	Bi	1	S	2	F	1																1	2015																										ABCD2	2	CeOBiS2	P4/nmm																	K		0.35					0.35																																																																							mOhm.cm							0.762																		solid state reaction method					Evidence for two distinct superconducting phases in EuBiS2F under pressure			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310058, China	Phys.Rev.B, 91(2015)214512	C. Y. Guo,Y. Chen,M. Smidman,S. A. Chen,W. B. Jiang,H. F. Zhai,Y. F. Wang,G. H. Cao,J. M. Chen,X. Lu,H. Q. Yuan		
158769	PRB091214512	P = 2.4 GPa.  monoclinic for P > 1.4 GPa.  Hc2 = 1.8 T (defined as R=0.1Rn).	EuBiS2F	Eu1Bi1S2F1	Eu	1	Bi	1	S	2	F	1																1	2015																										ABCD2		CeOBiS2	P2<1>/m																	K		8.61					8.61	MTC158769																			T	RES(0.9Rn), extrapolation	3.1												MHC158769		A	from Hc2	103										4.5	14																						mOhm.cm							0.263																		solid state reaction method					Evidence for two distinct superconducting phases in EuBiS2F under pressure			Center for Correlated Matter and Department of Physics, Zhejiang University, Hangzhou, Zhejiang 310058, China	Phys.Rev.B, 91(2015)214512	C. Y. Guo,Y. Chen,M. Smidman,S. A. Chen,W. B. Jiang,H. F. Zhai,Y. F. Wang,G. H. Cao,J. M. Chen,X. Lu,H. Q. Yuan		
158770	PRB093134505	structural anomaly T* = 38 K. SP (beta) = 12.0 mJ/mol.K4.  (dC/Tc) = 100 mJ/mol.K2, (dC/gamma*Tc) = 2.5. Hc(0) = 78 mT from C(T).	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2016																										A3B4C13		Yb3Rh4Sn12	Pm3[-]n																	K		6.8					6.8	MTC158770																																															4.9	14				MSP158770			mJ/mol.K2	40	SP	150	SP																																		Ca(4N),Ir(3N),Sn(5N)							Strong-coupling phonon-mediated scenario of superconductivity in Ca3Ir4Sn13 and Ca3(Ir0.91Co0.09)4Sn13			Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong	Phys.Rev.B, 93(2016)134505	Jianqiang Hou,Chi Ho Wong,Rolf Lortz,Romain Sibille,Michel Kenzelmann		
158771	PRB093134505	SP (beta) = 12.0 mJ/mol.K4.  (dC/Tc) = 160 mJ/mol.K2, (dC/gamma*Tc) = 2.7. Hc(0) = 100 mT from C(T).	Ca3(Ir0.91Co0.09)4Sn13	Ca3Ir3.64Co0.36Sn13	Ca	3	Ir	3.64	Co	0.36	Sn	13																3	2016																										A3B4C13		Yb3Rh4Sn12	Pm3[-]n																	K		75					75																																																					MSP158771			mJ/mol.K2	60	SP	149	SP											uOhm.cm							25.6																Ca(4N),Ir(3N),Co(3N),Sn(5N)		starting(Ca:Ir:Co:Sn = 3:2.2:1.8:90) - heat (1050 C,2h, in sealed quartz tube) - cool to 500 C (3 C/h) - Q to RT - remove excess Sn using HCl					Strong-coupling phonon-mediated scenario of superconductivity in Ca3Ir4Sn13 and Ca3(Ir0.91Co0.09)4Sn13			Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong	Phys.Rev.B, 93(2016)134505	Jianqiang Hou,Chi Ho Wong,Rolf Lortz,Romain Sibille,Michel Kenzelmann		
158772	PRB095184503	poly crystal. TCFIG shows Tc vs P.  A = 6.9 nOhm.cm/K^2. Tc(bulk) = Tc(zero) = Tc(SP). structural transition (cubic-to-tetra)  at  41 K.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				1	2017																										AB3		Cr3Si(A15)																		K	17.5	17.8	17.9				17.8	MTC158772																																																				MSP158772																		uOhm.cm							9.7																		HIP (hot isostatic pressure) furnace (200 MPa, 1250 C, 24 h) - cool to 0 C with 30 C/h					Evolution of T2 resistivity and superconductivity in Nb3Sn under pressure			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 95(2017)184503	Z. Ren,L. Gamperle,A. Fete,C. Senatore,D. Jaccard		
158773	PRB095184503	single crystal. TCFIG shows Tc vs root(A) where R = R0 + A*T^2.  A = 7.7 nOhm.cm/K^2. Tc(bulk) = Tc(zero) = Tc(SP).	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				3	2017																										AB3		Cr3Si(A15)																		K	17.1	17.3	17.5				17.3	MTC158773																																																																						uOhm.cm							0.71																		Tiny single crystals by vapor transport method					Evolution of T2 resistivity and superconductivity in Nb3Sn under pressure			DQMP - University of Geneva, 24 Quai Ernest-Ansermet, 1211 Geneva 4, Switzerland	Phys.Rev.B, 95(2017)184503	Z. Ren,L. Gamperle,A. Fete,C. Senatore,D. Jaccard		
158774	PRB096165123	P-induced SC. Pc = 27 GPa. SC properties (in DB) for P = 39.0 GPa. phase transition: alpha-to-beta SnSe (15 GPa) and to CsCl-type (26 GPa). semicond-metal (10 GPa)	SnSe	Se1Sn1	Se	1	Sn	1																					2017																										AB			Pnma	62	A	11.4447	4.3825	4.1616											At 39 GPa, CsCl type, a = 3.2060 A.	K			3.25		0		3.25	MTC158774																			T	RES(0.9Rn), linear approx.	1.12												MHC158774																																																																			Topological Dirac line nodes and superconductivity coexist in SnSe at high pressure			Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei 230031, China	Phys.Rev.B, 96(2017)165123	Xuliang Chen,Pengchao Lu,Xuefei Wang,Yonghui Zhou,Chao An,Ying Zhou,Cong Xian,Hao Gao,Zhaopeng Guo,Changyong Park,Binyang Hou,Kunling Peng,Xiaoyuan Zhou,Jian Sun,Yimin Xiong,Zhaorong Yang,Dingyu Xing,Yuheng Zhang		
158775	PRB100045152	half collapsed phase (hcT)  for 6 < P < 22 GPa. fully collapsed phase (fcT) for P > 22 GPa. for P = 3.1 GPa, dTc/dH = -0.3 K/T.	CaRbFe4As4	Ca1Rb1Fe4As4	Ca	1	Rb	1	Fe	4	As	4																3	2019																										ABC4D4		CaRb1144			A	3.8762		13.093												K								MTC158775																			T	RES(0.9Rn)													MHC158775																																																			cm3/C					10	MRH158775					(ca:Rb:FeAs = 0.8:1.2:10) - crucible in capped stainless tube - heat to 560C, hold 3h - heat to 1180 C, hold2 h - cool to 1030 C(30h) - 900 C(30h) - FC to RT					Observation of two collapsed phases in CaRbFe4As4			Lawrence Livermore National Laboratory, Livermore, California 94550, USA	Phys.Rev.B, 100(2019)045152	Ryan L. Stillwell,Xiangfeng Wang,Limin Wang,Daniel J. Campbell,Johnpierre Paglione,Samuel T. Weir,Yogesh K. Vohra,Jason R. Jeffries		
158776	PRB100060103	HCFIG shows h* vs t for P = 6.5 GPa, where h* = [Hc(T)/Tc]/[dHc2/dT at Tc].	Au2Pb	Au2Pb1	Au	2	Pb	1																				3	2019																										AB2			Fd3[-]m																cubic Laves. For low-T (SC states ), SG = I4[-]2d	K			3.61				3.61	MTC158776																			T	RES(0.9Rn), WHH	0.16							T/K	RES(0.9Rn)	0.0645			MHC158776																																																														Au2Pb powder in scre-pressure-type diamond-anvil cell					Ground states of Au2Pb and pressure-enhanced superconductivity			National Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 100(2019)060103	Juefei Wu,Zili Feng,Jinghui Wang,Qun Chen,Chi Ding,Tong Chen,Zhaopeng Guo,Jinsheng Wen,Youguo Shi,Dingyu Xing,Jian Sun		
158777	PRB100064516	Hc2,Hc1 for H//ab. demag-correction. Anisotropy (Hc2) = 14.9.  kappa(GL) = 7.58. SP  (dC/gamma*Tc) = 1.23. e-ph = 0.66.  N(0) = 1.14 states/eV.fu.	SnTaS2	Sn1Ta1S2	Sn	1	Ta	1	S	2																		3	2019																										ABC2			P6<3>/mmc		A	3.309		17.45												K		3		2.97			3										100	Oe	M-H cuve(5% deviation, (1-t^2) fitting		53.5	81.7					Oe	RES(0.5Rn). two band model fitting		3034	203.6										MHC158777		nm	from Hc2		127	8.5	nm			64.4	962.4								MSP158777			mJ/mol.K2	4.45	SP	154.4	SP																																		Sn0.33TaS2,Sn		crystals grown by CVT method using iodine agent. mixture(Sn:Ta:S = 1.2:1:2) - two zone furnace (1000 C(H) and 970 C(L) in quartz tube for 2weeks					Superconducting properties in a candidate topological nodal line semimetal SnTaS2 with a centrosymmetric crystal structure			College of Physics, Qingdao University, Qingdao 266071, China	Phys.Rev.B, 100(2019)064516	Dong-Yun Chen,Yuelong Wu,Lei Jin,Yongkai Li,Xiaoxiong Wang,JunXi Duan,Junfeng Han,Xiang Li,Yun-Ze Long,Xiaoming Zhang,Dong Chen,Bing Teng		
158778	PRB100064516	Hc2,Hc1 for H//c. demag-correction. Anisotropy (Hc2) = 14.9.  kappa(GL) = 5.07.  SP  (dC/gamma*Tc) = 1.23. e-ph = 0.66.  N(0) = 1.14 states/eV.fu.	SnTaS2	Sn1Ta1S2	Sn	1	Ta	1	S	2																		3	2019																										ABC2			P6<3>/mmc		A	3.309		17.45												K		3		2.97			3										100	Oe	M-H cuve(5% deviation, (1-t^2) fitting		53.5	81.7					Oe	RES(0.5Rn), GL fitting		3034	203.6										MHC158778		nm	from Hc2		127	8.5	nm			64.4	962.4								MSP158777			mJ/mol.K2	4.45	SP	154.4	SP																																		Sn0.33TaS2,Sn		crystals grown by CVT method using iodine agent. mixture(Sn:Ta:S = 1.2:1:2) - two zone furnace (1000 C(H) and 970 C(L) in quartz tube for 2weeks					Superconducting properties in a candidate topological nodal line semimetal SnTaS2 with a centrosymmetric crystal structure			College of Physics, Qingdao University, Qingdao 266071, China	Phys.Rev.B, 100(2019)064516	Dong-Yun Chen,Yuelong Wu,Lei Jin,Yongkai Li,Xiaoxiong Wang,JunXi Duan,Junfeng Han,Xiang Li,Yun-Ze Long,Xiaoming Zhang,Dong Chen,Bing Teng		
158779	PRB100094103	Anisotropy (Rc/Rab) = 55 (40 K), = 16 (30 K). Thermal conductivity K,ab> shows with K<el> via Wiedemann-Franz law.	Ca10Pt4As8((Fe1-xPtx)2As2)5, x=0.05	Ca10Pt4.5Fe9.5As18	Ca	10	Pt	4.5	Fe	9.5	As	18																3	2019																													P2<1>/n		A	8.76	8.76	20.18											gamma-1048 phase. monoclinic. alpha= beta = 90, gamma = 90.5.	K	32			32			32																																																													W/K.m			1.18	MTHC158779						mOhm.cm								0.26	14.2			0.62	9.85																	Atomically imaged crystal structure and normal-state properties of superconducting Ca10Pt4As8((Fe1-xPtx)2As2 )5			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 100(2019)094103	Zhen Wang,R. Jin,Lijun Wu,Jing Tao,A. B. Karki,J. Y. Pan,Yimei Zhu,E. W. Plummer		
158780	PRB100094103	data from Angew.Chem.Int.Ed., 50(2011)9195.	Ca10Pt4As8((Fe1-xPtx)2As2)5, x=0	Ca10Pt4Fe10As18	Ca	10	Pt	4	Fe	10	As	18																	2019																													P4/n		A	8.716		10.462											alpha-1048 phase. tetra-. alpha = beta = gamma = 90	K		35					35																																																																																																					Atomically imaged crystal structure and normal-state properties of superconducting Ca10Pt4As8((Fe1-xPtx)2As2 )5			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 100(2019)094103	Zhen Wang,R. Jin,Lijun Wu,Jing Tao,A. B. Karki,J. Y. Pan,Yimei Zhu,E. W. Plummer		
158781	PRB100094103	data from Proc.Natl.Acad.Sci.USA, 108(2011)E1019	Ca10Pt4As8((Fe1-xPtx)2As2)5, x=0.03	Ca10Pt4.3Fe9.7As18	Ca	10	Pt	4.3	Fe	9.7	As	18																	2019																													P4/n		A	8.733		10.481											alpha-1048 phase. tetra-. alpha = beta = gamma = 90	K		27					27																																																																																																					Atomically imaged crystal structure and normal-state properties of superconducting Ca10Pt4As8((Fe1-xPtx)2As2 )5			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 100(2019)094103	Zhen Wang,R. Jin,Lijun Wu,Jing Tao,A. B. Karki,J. Y. Pan,Yimei Zhu,E. W. Plummer		
158782	PRB100094103	data from Angew.Chem.Int.Ed., 50(2011)9195.	Ca10Pt4As8((Fe1-xPtx)2As2)5, x=0.13	Ca10Pt4.3Fe8.7As18	Ca	10	Pt	4.3	Fe	8.7	As	18																	2019																													P1[-]		A	8.7382	8.7887	11.225											beta-1048 phase. triclinic.  alpha=81.049, beta=71.915, gamma=89.980	K		13					13																																																																																																					Atomically imaged crystal structure and normal-state properties of superconducting Ca10Pt4As8((Fe1-xPtx)2As2 )5			Department of Physics and Astronomy, Louisiana State University, Baton Rouge, Louisiana 70803, USA	Phys.Rev.B, 100(2019)094103	Zhen Wang,R. Jin,Lijun Wu,Jing Tao,A. B. Karki,J. Y. Pan,Yimei Zhu,E. W. Plummer		
158784	PRB100094511	needle like crystals. RRR = 2.17.  Energy gap measured by PCAR, STS.  Two gaps , 1.8  and 5 meV (2d/kTc = 5.83 and 16) obtained  from PCAR measurements	RbCr3As3	Rb1Cr3As3	Rb	1	Cr	3	As	3																		3	2019																										AB3C3			P6<3>/m																hexagonal	K			7.17			0.64	7.17																																														meV	5	16	1																						uOhm.cm							249				540														single crystals grown by deintercalation process of  Rb ions from Rb2Cr3As3 precursors.					Multiband superconductivity and possible nodal gap in RbCr3As3 revealed by Andreev reflection and single-particle tunneling measurements			National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China	Phys.Rev.B, 100(2019)094511	Zhixin Liu,Mingyang Chen,Ying Xiang,Xiaoyu Chen,Huan Yang,Tong Liu,Qing-Ge Mu,Kang Zhao,Zhi-An Ren,Hai-Hu Wen		
158785	PRB100094513	[penet]<L> measured by TDR, MWR, NV center method. n = 2.5, where d[penet] = a + b*(T/Tc)^n.	CaK(Fe1-xNix)4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2019																										ABC4D4		CaRb1144																		K		36					36																																									nm	microwave resonator	196.4																																																					Single crystals grown by high-T solution growth out of FeAs flux.					Analysis of the London penetration depth in Ni-doped CaKFe4As4			Politecnico di Torino, Department of Applied Science and Technology, Torino 10129, Italy	Phys.Rev.B, 100(2019)094513	D. Torsello,K. Cho,K. R. Joshi,S. Ghimire,G. A. Ummarino,N. M. Nusran,M. A. Tanatar,W. R. Meier,M. Xu,S. L. Bud'ko,P. C. Canfield,G. Ghigo,R. Prozorov		
158786	PRB100094513	[penet]<L> measured by TDR, MWR, NV center method. n = 2.5, where d[penet] = a + b*(T/Tc)^n.	CaK(Fe1-xNix)4As4	Ca1K1Fe3.932Ni0.068As4	Ca	1	K	1	Fe	3.932	Ni	0.068	As	4														3	2019																										ABC4D4		CaRb1144																		K		28.2					28.2																																									nm	microwave resonator	227																																																					Single crystals grown by high-T solution growth out of FeAs flux.					Analysis of the London penetration depth in Ni-doped CaKFe4As4			Politecnico di Torino, Department of Applied Science and Technology, Torino 10129, Italy	Phys.Rev.B, 100(2019)094513	D. Torsello,K. Cho,K. R. Joshi,S. Ghimire,G. A. Ummarino,N. M. Nusran,M. A. Tanatar,W. R. Meier,M. Xu,S. L. Bud'ko,P. C. Canfield,G. Ghigo,R. Prozorov		
158787	PRB100094513	[penet]<L> measured by TDR, MWR, NV center method. n = 1.9, where d[penet] = a + b*(T/Tc)^n.	CaK(Fe1-xNix)4As4	Ca1K1Fe3.864Ni0.136As4	Ca	1	K	1	Fe	3.864	Ni	0.136	As	4														3	2019																										ABC4D4		CaRb1144																		K		19.3					19.3																																									nm	microwave resonator	285.2																																																					Single crystals grown by high-T solution growth out of FeAs flux.					Analysis of the London penetration depth in Ni-doped CaKFe4As4			Politecnico di Torino, Department of Applied Science and Technology, Torino 10129, Italy	Phys.Rev.B, 100(2019)094513	D. Torsello,K. Cho,K. R. Joshi,S. Ghimire,G. A. Ummarino,N. M. Nusran,M. A. Tanatar,W. R. Meier,M. Xu,S. L. Bud'ko,P. C. Canfield,G. Ghigo,R. Prozorov		
158788	PRB100094522	W3Al1.78C0.8 by ICP-AES.  SP (beta) = 0.62 mJ/mol.K4. (dC/gamma*Tc) = 2.7.  Hc2(0) = 15.4 T using (1-t^2)/(1+t^2) fitting. N(Ef) = 2.37 state/eV.fu.	W3Al2C	W3Al2C1	W	3	Al	2	C	1																		1	2019																										AB2C3		beta-Mn	P4<1>32	213	A	6.8757														K	7.5		7.6	7.5		0.1	7.5											A	M-H curve, linear	100							T	RES(mid), WHH	13.1							T/K	RES(mid)	2.5			MHC158788		nm	from Hc2	5.7			nm	from Hc1	320					5.43	14							mJ/mol.K2	7.3	SP	266	SP											uOhm.cm							215																		mixture(W:Al:C = 3:1.8:0.8) - pellet - in h-BN capsule - heat(2173 K, 24 h, P=5 GPa) - slow cool to RT within 1 day					Superconductivity with strong electron-phonon coupling in noncentrosymmetric W3Al2C			Materials Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan	Phys.Rev.B, 100(2019)094522	T. P. Ying,Y. P. Qi,H. Hosono		
158789	PRB100094525	P-induced SC. Pc = 2.69 GPa.Tc(max) = 5.45 K(P = 13.5 GPa). Tc defined as R = 0.99Rn. R not to zero down to 1.4 K. structural phase transition shows in num = 158790.	Bi2Te2Se	Bi2Te2Se1	Bi	2	Te	2	Se	1																			2019																										A2B3			R3[-]m	166	A	4.2609		29.766											rhombohedral	K			5.45		0		5.45	MTC158789																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158790	PRB100094525	Bi2.1Te1.8Se1.2 from EDX. Phase I (rhombohedral, SG = R3[-]m, #166), Phase-II (monoclinic, SG = C2/m, #12), PhaseIII (9/10-fold monoclinic, SG = C2/m, #12)	Bi2Te2Se	Bi2Te2Se1	Bi	2	Te	2	Se	1																			2019																													R3[-]m	166	A	4.2609		29.766											phase transition	K			5.45		0		5.45	MPH158790																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158791	PRB100094525	P-induced SC. Pc = 5.15 GPa.Tc(max) = 3.90 K(P = 11.9 GPa). Tc defined as R = 0.99Rn. R not to zero down to 1.4 K. structural phase transition shows in num = 158792.	Bi1.75Sb0.25Te2Se	Bi1.75Sb0.25Te2Se1	Bi	1.75	Sb	0.25	Te	2	Se	1																	2019																													R3[-]m	166	A	4.2695		29.869											rhombohedral	K			3.9		0		3.9	MTC158791																			T	RES(0.99Rn)													MHC158791																																																																			Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158792	PRB100094525	Bi1.75Sb0.25Te1.89Se1.11 from EDX. Phase I (rhombohedral, SG = R3[-]m, #166), Phase-II (monoclinic, SG = C2/m, #12), PhaseIII (9/10-fold monoclinic, SG = C2/m, #12)	Bi1.75Sb0.25Te2Se	Bi1.75Sb0.25Te2Se1	Bi	1.75	Sb	0.25	Te	2	Se	1																	2019																													R3[-]m	166	A	4.2695		29.869											phase transition	K			3.9		0		3.9	MPH158792																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158793	PRB100094525	P-induced SC. Pc = 5.02 GPa.Tc(max) = 5.28 K(P = 14.2 GPa). Tc defined as R = 0.99Rn. R not to zero down to 1.4 K. structural phase transition shows in num = 158792.	Bi1.5Sb0.5Te2Se	Bi1.5Sb0.5Te2Se1	Bi	1.5	Sb	0.5	Te	2	Se	1																	2019																													R3[-]m	166	A	4.263		29.99											rhombohedral	K			5.28		0		5.28	MTC158793																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158794	PRB100094525	Bi1.50Sb0.50Te1.68Se1.32 from EDX. Phase I (rhombohedral, SG = R3[-]m, #166), Phase-II (monoclinic, SG = C2/m, #12), PhaseIII (9/10-fold monoclinic, SG = C2/m, #12)	Bi1.5Sb0.5Te2Se	Bi1.5Sb0.5Te2Se1	Bi	1.5	Sb	0.5	Te	2	Se	1																	2019																													R3[-]m	166	A	4.263		29.99											phase transition	K			5.28		0		5.28	MPH158794																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158795	PRB100094525	P-induced SC. Pc = 8.49 GPa.Tc(max) = 2.40 K(P = 11.2 GPa). Tc defined as R = 0.99Rn. R not to zero down to 1.4 K. structural phase transition shows in num = 158792.	BiSbTe2Se	Bi1Sb1Te2Se1	Bi	1	Sb	1	Te	2	Se	1																	2019																													R3[-]m	166	A	4.2212		29.9869											rhombohedral	K			2.4		0		2.4	MTC158795																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158796	PRB100094525	Bi1.089Sb0.911Te1.81Se1.19  from EDX. Phase I (rhombohedral, SG = R3[-]m, #166), Phase-II (monoclinic, SG = C2/m, #12), PhaseIII (9/10-fold monoclinic, SG = C2/m, #12)	BiSbTe2Se	Bi1Sb1Te2Se1	Bi	1	Sb	1	Te	2	Se	1																	2019																													R3[-]m	166	A	4.2212		29.9869											phase transition	K			2.4		0		2.4	MPH158796																																																																																																				Pressure-induced superconductivity in Bi2-xSbxTe3-ySey			Research Institute for Interdisciplinary Science, Okayama University, Okayama 700?8530, Japan	Phys.Rev.B, 100(2019)094525	Tong He,Xiaofan Yang,Tomoya Taguchi,Teppei Ueno,Kaya Kobayashi,Jun Akimitsu,Hitoshi Yamaoka,Hirofumi Ishii,Yen-Fa Liao,Hiromi Ota,Hidenori Goto,Ritsuko Eguchi,Kensei Terashima,Takayoshi Yokoya,Harald O. Jeschke,Xianxin Wu,Yoshihiro Kubozono1		
158797	PRB100094527	gap (d--wave)	Fe1-xVxSe, x=0.005	Fe0.995V0.005Se1	Fe	0.995	V	0.005	Se	1																			2019																										AB					A	3.77076		5.52137												K		8.6					8.6																																									um	muon-SR		0.36		meV	1.72																																															Fe(4N8),Se(5N),V(4N)		mixture - ground - sealed in silica tube - heat to 700 C(2 C/min) - hold(36 h) - cool to 400 C - ANN(400 C,10 d) Q to 0 C.					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158798	PRB100094527	gap (d--wave)	Fe1-xVxSe, x=0.01	Fe0.99V0.01Se1	Fe	0.99	V	0.01	Se	1																			2019																										AB					A	3.77129		5.52105												K		8.5					8.5																																									um	muon-SR		0.39		meV	1.71																																															Fe(4N8),Se(5N),V(4N)		mixture - ground - sealed in silica tube - heat to 700 C(2 C/min) - hold(36 h) - cool to 400 C - ANN(400 C,10 d) Q to 0 C.					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158799	PRB100094527	gap (d--wave)	Fe1-xVxSe, x=0.02	Fe0.98V0.02Se1	Fe	0.98	V	0.02	Se	1																			2019																										AB					A	3.77152		5.52164												K		8.5					8.5																																									um	muon-SR		0.38		meV	1.83																																															Fe(4N8),Se(5N),V(4N)		mixture - ground - sealed in silica tube - heat to 700 C(2 C/min) - hold(36 h) - cool to 400 C - ANN(400 C,10 d) Q to 0 C.					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158800	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.61 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 0.62 meV(s-wave), d2 =0.14 meV(d)	Li0.6MFe1-xVxSe, x=0.005	Li0.6M1Fe0.995V0.005Se1	Li	0.6	M	1	Fe	0.995	V	0.005	Se	1															2019																															A	3.8315		16.3968												K		41.1					41.1																																									um	muon-SR		0.2		meV	0.62																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158801	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.64 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 1.1 meV(s-wave), d2 =0.18 meV(d)	Li0.6MFe1-xVxSe, x=0.005	Li0.6M1Fe0.995V0.005Se1	Li	0.6	M	1	Fe	0.995	V	0.005	Se	1															2019																															A	3.8315		16.3968												K		40.2					40.2																																									um	muon-SR		0.19		meV	1.1																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158802	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.45 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 1.23 meV(s-wave), d2 =0.14 meV(d)	Li0.6MFe1-xVxSe, x=0.01	Li0.6M1Fe0.995V0.01Se1	Li	0.6	M	1	Fe	0.995	V	0.01	Se	1															2019																															A	3.8336		16.3429												K		41.7					41.7																																									um	muon-SR		0.18		meV	1.23																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158803	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.53 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 2.1 meV(s-wave), d2 =0.16 meV(d)	Li0.6MFe1-xVxSe, x=0.01	Li0.6M1Fe0.995V0.01Se1	Li	0.6	M	1	Fe	0.995	V	0.01	Se	1															2019																															A	3.8336		16.3429												K		40.9					40.9																																									um	muon-SR		0.18		meV	2.1																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158804	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.46 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 1.17 meV(s-wave), d2 =0.14 meV(d)	Li0.6MFe1-xVxSe, x=0.02	Li0.6M1Fe0.995V0.02Se1	Li	0.6	M	1	Fe	0.995	V	0.02	Se	1															2019																															A	3.8295		16.4504												K		40.7					40.7																																									um	muon-SR		0.19		meV	1.17																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158805	PRB100094527	M-intercalated material. M = (NH2)0.2(NH3)0.8. two gaps, w = 0.55 where gap<av> = d1(1-w) + d2*w, d1(in DB) = 2.3 meV(s-wave), d2 =0.16 meV(d)	Li0.6MFe1-xVxSe, x=0.02	Li0.6M1Fe0.995V0.02Se1	Li	0.6	M	1	Fe	0.995	V	0.02	Se	1															2019																															A	3.8295		16.4504												K		40					40																																									um	muon-SR		0.2		meV	2.3																																																	(Fe,V,Se) - in Schlenk tube  with Li and stirred bar - evacuate  - cool to -78 C. NH3 condenced in flusk,  stirred (-78 C, 4h) - warm to RT  ( NH3 intercalated)					Robustness of superconducting properties to transition metal substitution and impurity phases in Fe1-xVxSe			1Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU, United Kingdom	Phys.Rev.B, 100(2019)094527	Franziska K. K. Kirschner,Daniel N. Woodruff,Matthew J. Bristow,Franz Lang,Peter J. Baker,Simon J. Clarke,Stephen J. Blundell		
158808	PRB100094528	not SC.  Insulator	NdO0.8F0.2SbSe2	Nd1F0.2Sb1Se2O0.8	Nd	1	F	0.2	Sb	1	Se	2													O	0.8			2019																												CeOBiS2	P4/nmm		A	4.0478		14.0568											impurity phase	K					0																																																																																																Nd2O3,NdSe,NdSe2,Sb(3N),Bi(5N),Se(5N)		mixture - pellet - heat(700 C,15 h, in evacuated silica tube) - ground - pelletize - heat(700 C,15 h)					Pressure-induced superconductivity in the layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0.3 and 0.7)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 100(2019)094528	Ryo Matsumoto,Yosuke Goto,Sayaka Yamamoto,Kenta Sudo,Hidetomo Usui,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Shintaro Adachi,Tetsuo Irifune,Hiroyuki Takeya,Hiromi Tanaka,Kazuhiko Kuroki,Yoshikazu Mizuguchi,Yoshihiko Takano		
158809	PRB100094528	Impurity phase: Nd2O2Se(4.1 wt%), NdOF(1.9 wt%), Bi2Se3(0.8 wt%). P-induced SC.  Tc(on) = 7.68 K at 70.6 GPa, but R not to zero down to 2 K.	NdO0.8F0.2Sb1-xBixSe2, x=0.3	Nd1F0.2Sb0.7Bi0.3Se2O0.8	Nd	1	F	0.2	Sb	0.7	Bi	0.3	Se	2											O	0.8			2019																												CeOBiS2	P4/nmm		A	4.0568		14.1322											impurity phase	K					0			MTC158809																			T	RES(onset), WHH	6.7												MHC158809																																																												Nd2O3,NdSe,NdSe2,Sb(3N),Bi(5N),Se(5N)		mixture - pellet - heat(650 C,15 h, in evacuated silica tube) - ground - pelletize - heat(650 C,15 h)					Pressure-induced superconductivity in the layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0.3 and 0.7)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 100(2019)094528	Ryo Matsumoto,Yosuke Goto,Sayaka Yamamoto,Kenta Sudo,Hidetomo Usui,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Shintaro Adachi,Tetsuo Irifune,Hiroyuki Takeya,Hiromi Tanaka,Kazuhiko Kuroki,Yoshikazu Mizuguchi,Yoshihiko Takano		
158810	PRB100094528	P-induced SC. SC data not given.	NdO0.8F0.2Sb1-xBixSe2, x=0.5	Nd1F0.2Sb0.5Bi0.5Se2O0.8	Nd	1	F	0.2	Sb	0.5	Bi	0.5	Se	2											O	0.8			2019																												CeOBiS2	P4/nmm		A	4.0625		14.2284											impurity phase	K					0			MLAT158810																																																																																													Nd2O3,NdSe,NdSe2,Sb(3N),Bi(5N),Se(5N)		mixture - pellet - heat(650 C,15 h, in evacuated silica tube) - ground - pelletize - heat(650 C,15 h)					Pressure-induced superconductivity in the layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0.3 and 0.7)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 100(2019)094528	Ryo Matsumoto,Yosuke Goto,Sayaka Yamamoto,Kenta Sudo,Hidetomo Usui,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Shintaro Adachi,Tetsuo Irifune,Hiroyuki Takeya,Hiromi Tanaka,Kazuhiko Kuroki,Yoshikazu Mizuguchi,Yoshihiko Takano		
158811	PRB100094528	Impurity phase: Nd2O2Se(4.1 wt%), NdOF(1.9 wt%), Bi2Se3(0.8 wt%). P-induced SC.  Tc(on) = 5.76 K at  52 GPa, but R not to zero down to 2 K.	NdO0.8F0.2Sb1-xBixSe2, x=0.7	Nd1F0.2Sb0.3Bi0.7Se2O0.8	Nd	1	F	0.2	Sb	0.3	Bi	0.7	Se	2											O	0.8			2019																												CeOBiS2	P4/nmm		A	4.0701		14.2224											impurity phase	K					0			MTC158811																			T	RES(onset), WHH	10.9												MHC158811																																																												Nd2O3,NdSe,NdSe2,Sb(3N),Bi(5N),Se(5N)		mixture - pellet - heat(650 C,15 h, in evacuated silica tube) - ground - pelletize - heat(650 C,15 h)					Pressure-induced superconductivity in the layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0.3 and 0.7)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 100(2019)094528	Ryo Matsumoto,Yosuke Goto,Sayaka Yamamoto,Kenta Sudo,Hidetomo Usui,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Shintaro Adachi,Tetsuo Irifune,Hiroyuki Takeya,Hiromi Tanaka,Kazuhiko Kuroki,Yoshikazu Mizuguchi,Yoshihiko Takano		
158812	PRB100094528	Nd2O2Se(13.2 wt%), Bi2Se3(12.9 wt%), solubility limit around x = 0.8.	NdO0.8F0.2Sb1-xBixSe2, x=0.8	Nd1F0.2Sb0.2Bi0.8Se2O0.8	Nd	1	F	0.2	Sb	0.2	Bi	0.8	Se	2											O	0.8			2019																												CeOBiS2	P4/nmm		A	4.0728		14.2502											impurity phase	K					0																																																																																																Nd2O3,NdSe,NdSe2,Sb(3N),Bi(5N),Se(5N)		mixture - pellet - heat(650 C,15 h, in evacuated silica tube) - ground - pelletize - heat(650 C,15 h)					Pressure-induced superconductivity in the layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0.3 and 0.7)			National Institute for Materials Science, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan	Phys.Rev.B, 100(2019)094528	Ryo Matsumoto,Yosuke Goto,Sayaka Yamamoto,Kenta Sudo,Hidetomo Usui,Akira Miura,Chikako Moriyoshi,Yoshihiro Kuroiwa,Shintaro Adachi,Tetsuo Irifune,Hiroyuki Takeya,Hiromi Tanaka,Kazuhiko Kuroki,Yoshikazu Mizuguchi,Yoshihiko Takano		
158813	PRB100134503	RRR = 5.9. SP (beta)= 0.027 mJ/mol.K2. (dC/gamma*Tc) = 1.3, (delta) = 0.0015 mJ/mol.K6.  Two gaps ,  (2d/kTc) = 1.06 and 3.74 (in DB) from SP analysis.	TaOsSi	Ta1Os1Si1	Ta	1	Os	1	Si	1																		1	2019																										ABC	3	TiNiSi	Pnma	62	A	6.26	3.89	7.25											ortho-	K	4.2		5.51				4.855	MTC158813																			T	RES(0.9Rn), two band model.	4.52												MHC158813														3.74	14				MSP158813			mJ/mol.K2	8.52	SP	595	SP											uOhm.cm							4.9				28.9												Ta(4N),Os(4N),Si(4N)		arc-melting. starting(Ta:Os:Si = 1:1:1, molar volume ratio) - arc-melting 10 times  -  ANN (1273 K, 9 days, in sealed quartz tube)					Two-gap superconductivity and topological surface states in TaOsSi			School of Physics and Key Laboratory of MEMS of the Ministry of Education, Southeast University, Nanjing 211189, China	Phys.Rev.B, 100(2019)134503	C. Q. Xu,B. Li,J. J. Feng,W. H. Jiao,Y. K. Li,S. W. Liu,Y. X. Zhou,R. Sankar,Nikolai D. Zhigadlo,H. B. Wang,Z. D. Han,B. Qian,W. Ye,W. Zhou,T. Shiroka,Pabitra K. Biswas,Xiaofeng Xu,Z. X. Shi		
158815	PRB100144505	penetration depth and anisotropy measured by torque method.  [ppenet] =  0.33 um at  25 K (in DB).  Anisotropy (penet) = 17.4  independent of T.	KCa2Fe4As4F2	K1Ca2Fe4As4F2	K	1	Ca	2	Fe	4	As	4	F	2														3	2019																										AB2C2D4E4																			12442-type structure	K				33			33	MPEN158815																																								um	torque, 25 K		0.33																																																				self-flux method using  KAs-flux.					Probing superconducting anisotropy of single crystal KCa2Fe4As4F2 by magnetic torque measurements			State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Chinese Academy of Sciences, Shanghai 200050,China	Phys.Rev.B, 100(2019)144505	A. B. Yu,T. Wang,Y. F. Wu,Z. Huang,H. Xiao,G. Mu,T. Hu		
158816	PRB092174404	Hall coeff. at 10 K ( in DB).	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2015																										AB2					A			12.963											beta-phase	K			5.4			0.3	5.4	MTC158816		K/GPa	-0.28																																																																																	cm3/C		-0.000424			5	MRH158816	n/cm3	14700000000000000000000			melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158817	PRB092174404	impurity phase: alpha-PdBi2.	beta-PdBi2-xPbx	Pd1Bi1.92Pb0.08	Pd	1	Bi	1.92	Pb	0.08																		3	2015																										AB2																			beta-phase	K			4.9			0.3	4.9																																																																																																melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158818	PRB092174404		beta-PdBi2-xPbx	Pd1Bi1.85Pb0.15	Pd	1	Bi	1.85	Pb	0.15																		3	2015																										AB2																			beta-phase	K			4.4			0.3	4.4																																																																																																melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158819	PRB092174404	Hall coeff. at 10 K ( in DB).	beta-PdBi2-xPbx	Pd1Bi1.8Pb0.2	Pd	1	Bi	1.8	Pb	0.2																		3	2015																										AB2																			beta-phase	K			3.8			0.3	3.8	MTC158819																																																																																				cm3/C		-0.000112					n/cm3	5560000000000000000000			melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158820	PRB092174404		beta-PdBi2-xPbx	Pd1Bi1.72Pb0.28	Pd	1	Bi	1.72	Pb	0.28																		3	2015																										AB2																			beta-phase	K			2.5			0.3	2.5																																																																																																melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158821	PRB092174404		beta-PdBi2-xPbx	Pd1Bi1.65Pb0.35	Pd	1	Bi	1.65	Pb	0.35																		3	2015																										AB2																			beta-phase	K			2.2			0.3	2.2																																																																																																melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158822	PRB092174404	Tc eventually above 2 K. For x > 0.6, alpha-phase increases with increasing x.  For x = 1, only alpha-phase.	beta-PdBi2-xPbx	Pd1Bi1.6Pb0.4	Pd	1	Bi	1.6	Pb	0.4																		3	2015																										AB2					A			12.94											beta-phase	K			2			0.3	2																																																																																																melt-grown method. (Pd + Bi) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158823	PRB092174404	nominal Na  x = 0.1.  Na-concentration x = 0.044 in NaxPdBi2 by WDS.  impurity phase : NaBi and Pd  (total 10 %) in beta-PdBi2 phase.	beta-NaxPdBi2	Na0.044Pd1Bi2	Na	0.044	Pd	1	Bi	2																		3	2015																										AB2																			beta-phase	K			4.1				4.1																																																																																																melt-grown method. (Na + PdBi2) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158824	PRB092174404	nominal Na  x = 0.4.  Na-concentration x = 0.057 in NaxPdBi2 by WDS.  impurity phase : NaBi and Pd  (total 10 %) in beta-PdBi2 phase.	beta-NaxPdBi2	Na0.044Pd1Bi2	Na	0.044	Pd	1	Bi	2																		3	2015																										AB2																			beta-phase	K			3.9				3.9																																																																																					cm3/C						MRH158824	n/cm3	30900000000000000000000			melt-grown method. (Na + PdBi2) - sealed in evacuated quartz tube - heat to 700 C - keep(700C,10h) - slow cool to 450 C over 30 h - Q to iced water					Chemical doping and high-pressure studies of layered beta-PdBi2 single crystals			Texas Center for Superconductivity and Department of Physics, University of Houston, Houston, Texas 77204-5002, USA	Phys.Rev.B, 92(2015)174404	Kui Zhao,Bing Lv,Yu-Yi Xue,Xi-Yu Zhu,L. Z. Deng,Zheng Wu,C. W. Chu		
158825	PRB097134505	P = 0.001 kbar.  SP  (beta) = 2.37 mJ/mol.K4,  e-ph = 0.97	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.98				0.08	4.98	MTC158825		K/GPa	-0.25																T	RES(0.5Rn), WHH			0.6										MHC158825		nm	from Hc2	23.4																		mJ/mol.K2	13.23	SP	91	SP											uOhm.cm							24.23	22															Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158826	PRB097134505	P = 6.8 kbar. e-ph = 0.85	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.81					4.81																				T	RES(0.5Rn), WHH			0.52										MHC158826		nm	from Hc2	25.1																																	uOhm.cm							23.23																Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158827	PRB097134505	P = 10.6 kbar. e-ph = 0.83	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.72					4.72																				T	RES(0.5Rn), WHH			0.49										MHC158825		nm	from Hc2	25.9																																	uOhm.cm							22.79																Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158828	PRB097134505	P = 13.3 kbar.  e-ph = 0.81	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.62					4.62	MTC158825																			T	RES(0.5Rn), WHH			0.47										MHC158826		nm	from Hc2	26.4																																	uOhm.cm							22.47																Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158829	PRB097134505	P = 21.4 kbar.  e-ph = 0.78	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.47					4.47	MTC158829																			T	RES(0.5Rn), WHH			0.42										MHC158825		nm	from Hc2	27.9																																	uOhm.cm							21.85																Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158830	PRB097134505	P = 24.0 kbar.   e-ph = 0.77	beta-PdBi2	Bi2Pd1	Bi	2	Pd	1																				3	2018																										AB2																				K		4.36					4.36																				T	RES(0.5Rn), WHH			0.39										MHC158826		nm	from Hc2	28.9																																	uOhm.cm							21.74																Bi(4N),Pd(3N5)		melt-growth method. stoichiometric (Bi,Pd) - sealed in 14 mbar He in quartz ampoules					Pressure effect on the superconducting and the normal state of beta-Bi2Pd			Centre of Low Temperature Physics, Institute of Experimental Physics SAS, Watsonova 47, 040 01 Kosice, Slovakia	Phys.Rev.B, 97(2018)134505	G. Pristas,Mat. Orendac,S. Gabani,J. Kacmarcik,E. Gazo,Z. Pribulova,A. Correa-Orellana,E. Herrera,H. Suderow,P. Samuely		
158831	PRL0820169	P = 0. single crystal.  Hc2(T) shows best fitting to strong coupling model	UBe13	Be13U1	Be	13	U	1																				3	1999																										AB13																				K			0.956				0.956																				T	RES(0.9Rn), strong coupling model	13.9							T/K	R(0.9Rn),	55			MHC158831																																																																			Pressure Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UBe13			Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble-Cedex 9, France	Phys.Rev.Lett., 82(1999)0169	L. Glemot,J. P. Brison,J. Flouquet,A. I. Buzdin,I. Sheikin,D. Jaccard,C. Thessieu,F. Thomas		
158832	PRL0820169	P = 4 kbar.  Hc2(T) shows best fitting to strong coupling model	UBe13	Be13U1	Be	13	U	1																				1	1999																										AB13																				K			0.911				0.911																				T	RES(0.9Rn), strong coupling model	11.5							T/K	R(0.9Rn),	42																																																																						Pressure Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UBe13			Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble-Cedex 9, France	Phys.Rev.Lett., 82(1999)0169	L. Glemot,J. P. Brison,J. Flouquet,A. I. Buzdin,I. Sheikin,D. Jaccard,C. Thessieu,F. Thomas		
158833	PRL0820169	P = 6 kbar. Hc2(T) shows best fitting to strong coupling model	UBe13	Be13U1	Be	13	U	1																				1	1999																										AB13																				K			0.865				0.865																				T	RES(0.9Rn), strong coupling model	10.2							T/K	R(0.9Rn),	32			MHC158831																																																																			Pressure Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UBe13			Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble-Cedex 9, France	Phys.Rev.Lett., 82(1999)0169	L. Glemot,J. P. Brison,J. Flouquet,A. I. Buzdin,I. Sheikin,D. Jaccard,C. Thessieu,F. Thomas		
158834	PRL0820169	P = 10 kbar. Hc2(T) shows best fitting to strong coupling model	UBe13	Be13U1	Be	13	U	1																				1	1999																										AB13																				K			0.786				0.786																				T	RES(0.9Rn), strong coupling model	8.2							T/K	R(0.9Rn),	21																																																																						Pressure Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UBe13			Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble-Cedex 9, France	Phys.Rev.Lett., 82(1999)0169	L. Glemot,J. P. Brison,J. Flouquet,A. I. Buzdin,I. Sheikin,D. Jaccard,C. Thessieu,F. Thomas		
158835	PRL0820169	P = 20 kbar. Hc2(T) shows best fitting to strong coupling model	UBe13	Be13U1	Be	13	U	1																				1	1999																										AB13																				K			0.65				0.65																				T	RES(0.9Rn), strong coupling model	4.2							T/K	R(0.9Rn),	8.5			MHC158831																																																																			Pressure Dependence of the Upper Critical Field of the Heavy Fermion Superconductor UBe13			Centre de Recherches sur les Tres Basses Temperatures, CNRS, BP 166, 38042 Grenoble-Cedex 9, France	Phys.Rev.Lett., 82(1999)0169	L. Glemot,J. P. Brison,J. Flouquet,A. I. Buzdin,I. Sheikin,D. Jaccard,C. Thessieu,F. Thomas		
158836	PRL0814476	MSP158837 shows C/T vs B at T = 208 mK for UBe13. Tc = 0.898 K from SP.  (dC/gamma*Tc) = 1.26. T<L> (thermal expansion anomaly) = 0.77 K.	UBe13	Be13U1	Be	13	U	1																				3	1998																										AB13																				K		0.92				0.025	0.92			K/GPa	-0.13																T	SP, Thermal expansion													MHC158836																			MSP158836																																																Revision of the Phase Diagram of Superconducting U1-xThxBe13			Max-Planck Institute for Chemical Physics of Solides, D-01187 Dresden, Germany	Phys.Lev.Lett.,81(1998)4476	A. Bach,C. Langhammer,F. Koromer,F. Steglich,G.R. Stewart,J.S. Kim,M. Lang,R. Helfrich,T. Michels		
158837	PRL0814476	MTEX158838 shows T-dependence of thermal expansion coeffic. of U1-xThxBe13.  T<L> (thermal expansion anomaly) = 0.50 K.	U1-xThxBe13	U0.99Th0.01Be13	U	0.99	Th	0.01	Be	13																			1998																										AB13																				K		0.63					0.63			K/GPa	-0.19																																																	MSP158837																																																Revision of the Phase Diagram of Superconducting U1-xThxBe13			Max-Planck Institute for Chemical Physics of Solides, D-01187 Dresden, Germany	Phys.Lev.Lett.,81(1998)4476	A. Bach,C. Langhammer,F. Koromer,F. Steglich,G.R. Stewart,J.S. Kim,M. Lang,R. Helfrich,T. Michels		
158838	PRL0814476	MTEX158838 shows T-dependence of thermal expansion coeffic. of U1-xThxBe13.  T<L> (thermal expansion anomaly) = 0.43 K.	U1-xThxBe13	U0.983Th0.017Be13	U	0.983	Th	0.017	Be	13																			1998																										AB13																				K		0.51					0.51	MTEX158838		K/GPa	-0.3																																																																																																	Revision of the Phase Diagram of Superconducting U1-xThxBe13			Max-Planck Institute for Chemical Physics of Solides, D-01187 Dresden, Germany	Phys.Lev.Lett.,81(1998)4476	A. Bach,C. Langhammer,F. Koromer,F. Steglich,G.R. Stewart,J.S. Kim,M. Lang,R. Helfrich,T. Michels		
158839	PRL114117001	needle like single crystals.  not SC.  P-induced SC for 7.6=< P =<8.3 GPa. Tm(FM) = 291 K. Tm = 250 K for P = 2.8 GPa.	MnP	Mn1P1	Mn	1	P	1																				3	2015																										AB																				K					0																																																																																																		crystals grown  using Sn-flux					Pressure Induced Superconductivity on the border of Magnetic Order in MnP			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.Lett., 114(2015)117001	J.-G. Cheng,K. Matsubayashi,W. Wu,J. P. Sun,F. K. Lin,J. L. Luo,Y. Uwatoko		
158840	PRL114117001	not SC  under P =0.   SC data for 7.8 GPa.	MnP, P=7.8 GPa)	Mn1P1	Mn	1	P	1																				3	2015																										AB					A	5.26	3.17	5.92											ortho-.  B31-type	K	0.68	0.94	1.04		0		0.94	MTC158840																			T	RES(0.5Rn), linear fitting)	0.33							T/K	RES(0.5Rn)	0.34			MHC158840		A	from Hc2	315																																																										crystals grown  using Sn-flux					Pressure Induced Superconductivity on the border of Magnetic Order in MnP			Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China	Phys.Rev.Lett., 114(2015)117001	J.-G. Cheng,K. Matsubayashi,W. Wu,J. P. Sun,F. K. Lin,J. L. Luo,Y. Uwatoko		
158841	PRL122067001	Tc shows for P = 0. Hc2 measured for various P.	UBe13	Be13U1	Be	13	U	1																				1	2019																										AB13																				K		0.89					0.89																				T	RES													MHC158841																																																																			Spin-Triplet p-Wave Superconductivity Revealed under High Pressure in UBe13			Universite Grenoble Alpes, INAC/PHELIQS, CEA-Grenoble, F-38000 Grenoble, France	Phys.Rev.Lett., 122(2019)067001	Yusei Shimizu,Daniel Braithwaite,Dai Aoki,Bernard Salce,Jean-Pascal Brison		
158842	PRL122067001	Tc sdhows for P = 2.1 GPa.  Hc2 measured for various P.	UBe13	Be13U1	Be	13	U	1																				1	2019																										AB13																				K		0.53					0.53	MPH158842																			T	RES													MHC158842																																																																			Spin-Triplet p-Wave Superconductivity Revealed under High Pressure in UBe13			Universite Grenoble Alpes, INAC/PHELIQS, CEA-Grenoble, F-38000 Grenoble, France	Phys.Rev.Lett., 122(2019)067001	Yusei Shimizu,Daniel Braithwaite,Dai Aoki,Bernard Salce,Jean-Pascal Brison		
158843	PRL122067001	Tc shows for P = 4.3 GPa.  Hc2 measured for various P.	UBe13	Be13U1	Be	13	U	1																				1	2019																										AB13																				K		0.22					0.22																				T	RES													MHC158843																																																																			Spin-Triplet p-Wave Superconductivity Revealed under High Pressure in UBe13			Universite Grenoble Alpes, INAC/PHELIQS, CEA-Grenoble, F-38000 Grenoble, France	Phys.Rev.Lett., 122(2019)067001	Yusei Shimizu,Daniel Braithwaite,Dai Aoki,Bernard Salce,Jean-Pascal Brison		
158844	PRL123027002	Nematic single crystal x = 0.1 in SrxBi2Se3. Specific heat (dC/T) exhibits two-fold symmetry in azimuthal angle behavior. Anisotropy Hc2<x>/Hc2<y> =  2.5.	SrxBi2Se3	Sr0.1Bi2Se3	Sr	0.1	Bi	2	Se	3																		3	2019																																													hexagonal. x-axis defined as Se-Bi bond direction in hexagonal plane	K	3.1			3.1			3.1										80										T	RES													MHC158844																																																														single crystal (nematic state) grownn by flux method					Quasiparticle Evidence for the Nematic State above Tc in SrxBi2Se3			Institute for Solid State Physics (ISSP), The University of Tokyo, Kashiwa, Chiba 277-8581, Japan	Phys.Rev.Lett., 123(2019)027002	Yue Sun,Shunichiro Kittaka,Toshiro Sakakibara,Kazushige Machida,Jinghui Wang,Jinsheng Wen,Xiangzhuo Xing,Zhixiang Shi,Tsuyoshi Tamegai		
158845	PRL123147001	x = 0.11(av). AFM order for x = 0.11(av) sample for P > 0.6 GPa.. MTC158845 shows phase diagram from muSR and ac-SUS. Ts shows nematic order.	FeSe1-xSx	Fe1Se0.89S0.11	Fe	1	Se	0.89	S	0.11																		1	2019																																														K				10			10	MTC158845																																																																																																				Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-xSx			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 123(2019)147001	S. Holenstein,J. Stahl,Z. Shermadini,G. Simutis,V. Grinenko,D. A. Chareev,R. Khasanov,J.-C. Orain,A. Amato,H.-H. Klauss,E. Morenzoni,D. Johrendt,H. Luetkens		
158846	PRL123147001	Tc(max) at P = 0.68 GPa.	FeSe1-xSx, x=0	Fe1Se1	Fe	1	Se	1																				3	2019																																														K				8.91			8.91	MTC158847																																																																																																				Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-xSx			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 123(2019)147001	S. Holenstein,J. Stahl,Z. Shermadini,G. Simutis,V. Grinenko,D. A. Chareev,R. Khasanov,J.-C. Orain,A. Amato,H.-H. Klauss,E. Morenzoni,D. Johrendt,H. Luetkens		
158847	PRL123147001	Tc(max) at P = 0.49 GPa.	FeSe1-xSx,  x=0.05	Fe1Se0.95S0.05	Fe	1	Se	0.95	S	0.05																		3	2019																																														K				9.86			9.86	MTC158847																																																																																																				Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-xSx			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 123(2019)147001	S. Holenstein,J. Stahl,Z. Shermadini,G. Simutis,V. Grinenko,D. A. Chareev,R. Khasanov,J.-C. Orain,A. Amato,H.-H. Klauss,E. Morenzoni,D. Johrendt,H. Luetkens		
158848	PRL123147001	Tc(max) at P = 0.30 GPa.	FeSe1-xSx, x = 0.09	Fe1Se0.91S0.09	Fe	1	Se	0.91	S	0.09																		3	2019																																														K				10.33			10.33	MTC158847																																																																																																				Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-xSx			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 123(2019)147001	S. Holenstein,J. Stahl,Z. Shermadini,G. Simutis,V. Grinenko,D. A. Chareev,R. Khasanov,J.-C. Orain,A. Amato,H.-H. Klauss,E. Morenzoni,D. Johrendt,H. Luetkens		
158849	PRL123147001	Tc(max) at P = 0.24 GPa.	FeSe1-xSx, x=0.14	Fe1Se0.86S0.14	Fe	1	Se	0.86	S	0.14																		3	2019																																														K				10.52			10.52	MTC158847																																																																																																				Extended Magnetic Dome Induced by Low Pressures in Superconducting FeSe1-xSx			Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland	Phys.Rev.Lett., 123(2019)147001	S. Holenstein,J. Stahl,Z. Shermadini,G. Simutis,V. Grinenko,D. A. Chareev,R. Khasanov,J.-C. Orain,A. Amato,H.-H. Klauss,E. Morenzoni,D. Johrendt,H. Luetkens		
158850	SCIR00637527	semicond-like R(T)	Sr0.5Ce0.5FBiS2	Sr0.5Ce0.5F1Bi1S2	Sr	0.5	Ce	0.5	F	1	Bi	1	S	2														1	2016							7.5																				2	CeOBiS2	P4/nmm																SrFBiS2-type	K	2		2.4				2.2																																																																							mOhm.cm							42.5				4.12																			Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex (x = 0.5 and 1.0), a non-U material with Tc < T-FM			Department of Chemistry, Indian Institute of Technology, New Delhi, 110016, India	Sci.Rep., 6(2016)37527	Gohil S. Thakur,G. Fuchs,K. Nenkov,Zeba Haque,L. C. Gupta,A. K. Ganguli		
158851	SCIR00637527	impurity phase: Bi2Se3, Bi2S3.  semicond-like R(T)	Sr0.5Ce0.5FBiS1.7Se0.3	Sr0.5Ce0.5F1Bi1S1.7Se0.3	Sr	0.5	Ce	0.5	F	1	Bi	1	S	1.7	Se	0.3												1	2016							4.1																				2	CeOBiS2	P4/nmm																SrFBiS2-type	K	2.5		2.7				2.6																																																																							mOhm.cm							8.51				3.96																			Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex (x = 0.5 and 1.0), a non-U material with Tc < T-FM			Department of Chemistry, Indian Institute of Technology, New Delhi, 110016, India	Sci.Rep., 6(2016)37527	Gohil S. Thakur,G. Fuchs,K. Nenkov,Zeba Haque,L. C. Gupta,A. K. Ganguli		
158852	SCIR00637527	impurity phase: Bi2Se3, Bi2S3.  SP-FIG shows  (C-C<Schottky>) vs T.  (beta) = 1.48 mJ/mol.K4. Itinerant FM and SC coexist below Tc. Magnetic data from C-W law.	Sr0.5Ce0.5FBiS1.5Se0.5	Sr0.5Ce0.5F1Bi1S1.5Se0.5	Sr	0.5	Ce	0.5	F	1	Bi	1	S	1.5	Se	0.5												1	2016					myu-B/Ce	2.22	3.6																				2	CeOBiS2	P4/nmm		A	4.0886		13.4143											SrFBiS2-type	K	2.6		2.9	2.65			2.65										95										T	RES(0.9Rn), WHH	2.6							T/K	RES(0.9Rn)	1.3			MHC158852																			MSP158852			mJ/mol.K2	12	SP	187	SP											mOhm.cm							1.09				0.88																			Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex (x = 0.5 and 1.0), a non-U material with Tc < T-FM			Department of Chemistry, Indian Institute of Technology, New Delhi, 110016, India	Sci.Rep., 6(2016)37527	Gohil S. Thakur,G. Fuchs,K. Nenkov,Zeba Haque,L. C. Gupta,A. K. Ganguli		
158853	SCIR00637527	impurity phase: Bi2Se3, Bi2S3.  metallic R(T).   Itinerant FM and SC coexist below Tc. Magnetic data from C-W law.	Sr0.5Ce0.5FBiSSe	Sr0.5Ce0.5F1Bi1S1Se1	Sr	0.5	Ce	0.5	F	1	Bi	1	S	1	Se	1												1	2016					myu-B/Ce	2.29																					2	CeOBiS2	P4/nmm		A	4.1057		13.4756											SrFBiS2-type	K	3.1		3.3	3.12		0.2	3.12										95										T	RES(0.9Rn), WHH	3.3							T/K	RES(0.9Rn)	1.45			MHC158852																																					mOhm.cm							1.51				1.7																			Coexistence of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex (x = 0.5 and 1.0), a non-U material with Tc < T-FM			Department of Chemistry, Indian Institute of Technology, New Delhi, 110016, India	Sci.Rep., 6(2016)37527	Gohil S. Thakur,G. Fuchs,K. Nenkov,Zeba Haque,L. C. Gupta,A. K. Ganguli		
158854	SCIR00717370	Tm(FM) = 3.5 K. spontaneous moment = 0.09 myu-B/Ce from M(H) and muSR.  volume fraction of FM = 8 % from muSR.	Sr0.5Ce0.5FBiS1.5Se0.5	Sr0.5Ce0.5F1Bi1S1.5Se0.5	Sr	0.5	Ce	0.5	F	1	Bi	1	S	1.5	Se	0.5												1	2017					myu-B/Ce	0.09	3.5																				2	CeOBiS2	P4/nmm																SrFBiS2-type	K			2.7				2.7																																																																																																					Macroscopic phase separation of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex revealed by muSR			Van der Waals-Zeeman Institute, University of Amsterdam, 1098 XH, Amsterdam, The Netherlands	Sci.Rep., 7(2017)17370	A. M. Nikitin,V. Grinenko,R. Sarkar,J.-C. Orain,M. V. Salis,J. Henke,Y. K. Huang,H.-H. Klauss,A. Amato,A. de Visser		
158855	SCIR00717370	Tm(FM) = 3.3 K. spontaneous moment = 0.2 myu-B/Ce from M(H) and muSR. Volume fractions of SC and FM plotted in FIG from muSR analysis.	Sr0.5Ce0.5FBiSSe	Sr0.5Ce0.5F1Bi1S1Se1	Sr	0.5	Ce	0.5	F	1	Bi	1	S	1	Se	1												1	2017					myu-B/Ce	0.2	3.3																				2	CeOBiS2	P4/nmm																SrFBiS2-type	K			2.9				2.9	MVOL158855										mT		0.6							T		2.9																			nm	muSR	390																																																										Macroscopic phase separation of superconductivity and ferromagnetism in Sr0.5Ce0.5FBiS2-xSex revealed by muSR			Van der Waals-Zeeman Institute, University of Amsterdam, 1098 XH, Amsterdam, The Netherlands	Sci.Rep., 7(2017)17370	A. M. Nikitin,V. Grinenko,R. Sarkar,J.-C. Orain,M. V. Salis,J. Henke,Y. K. Huang,H.-H. Klauss,A. Amato,A. de Visser		
158856	SST028095016	RRR = 1.3. TaB-phase increass with x for 0.05 =< x =< 0.45. SP  (beta) = 0.11222 mJ/mol.K4.  (dC/gamma*Tc) = 1.11.	Ta0.7Hf0.3B	Ta0.7Hf0.3B1	Ta	0.7	Hf	0.3	B	1																		1	2015																										AB	3	FeB	Pnma		A	6.2462	3.1513	4.7496												K	6.2		6.7	6.7			6.7										55										T	RES(0.5Rn), WHH	10.5																															MSP158856			mJ/mol.K2	2	Sp	325.93	SP																																				arc-melting 5 times for 0=< x =< 0.45.  sealed in furnace - ANN(2000 C, 8h)					Ta1-xHfxB: a new FeB-prototype superconductor			Escola de Engenharia de Lorena?USP, P. O. Box 116, Lorena, 12602-810, Brazil	Supercond.Sci.Technol., 28(2015)095016	A J S Machado,L E Correa,M S da Luz,F B Santos,B S de Lima,S T Renosto,O V Cigarroa,M R Custodio,C A Nunes,G C Coelho,P F Rogl,P F S Rosa,D J Kim,Z Fisk		
158857	SST028095016		TaB	B1Ta1	B	1	Ta	1																				1	2015																										AB	3	FeB	Pnma																	K			4				4																																																																																																arc-melting 5 times for 0=< x =< 0.45.  sealed in furnace - ANN(2000 C, 8h)					Ta1-xHfxB: a new FeB-prototype superconductor			Escola de Engenharia de Lorena?USP, P. O. Box 116, Lorena, 12602-810, Brazil	Supercond.Sci.Technol., 28(2015)095016	A J S Machado,L E Correa,M S da Luz,F B Santos,B S de Lima,S T Renosto,O V Cigarroa,M R Custodio,C A Nunes,G C Coelho,P F Rogl,P F S Rosa,D J Kim,Z Fisk		
158858	SST028095016		Ta0.85Hf0.15B	Ta0.85Hf0.15B1	Ta	0.85	Hf	0.15	B	1																		1	2015																										AB	3	FeB	Pnma																	K								MTC158858																																																																																															arc-melting 5 times for 0=< x =< 0.45.  sealed in furnace - ANN(2000 C, 8h)					Ta1-xHfxB: a new FeB-prototype superconductor			Escola de Engenharia de Lorena?USP, P. O. Box 116, Lorena, 12602-810, Brazil	Supercond.Sci.Technol., 28(2015)095016	A J S Machado,L E Correa,M S da Luz,F B Santos,B S de Lima,S T Renosto,O V Cigarroa,M R Custodio,C A Nunes,G C Coelho,P F Rogl,P F S Rosa,D J Kim,Z Fisk		
158859	SST028095016	secondary FeB-phase  appears for x > 0.4.  FeB phase is stable.	Ta0.6Hf0.4B	Ta0.6Hf0.4B1	Ta	0.6	Hf	0.4	B	1																		1	2015																										AB	3	FeB	Pnma																	K																																																																																																							arc-melting 5 times for 0=< x =< 0.45.  sealed in furnace - ANN(2000 C, 8h)					Ta1-xHfxB: a new FeB-prototype superconductor			Escola de Engenharia de Lorena?USP, P. O. Box 116, Lorena, 12602-810, Brazil	Supercond.Sci.Technol., 28(2015)095016	A J S Machado,L E Correa,M S da Luz,F B Santos,B S de Lima,S T Renosto,O V Cigarroa,M R Custodio,C A Nunes,G C Coelho,P F Rogl,P F S Rosa,D J Kim,Z Fisk		
158860	SST030115011	P-induced SC. Pc = 2.37 GPa.  SC properties(DB) for P = 2.9 GPa. RRR = 89.4. Activation energy Eg = 6.08 meV from R(T) fitting.	Eu2SrBi2S4F4	Eu2Sr1Bi2S4F4	Eu	2	Sr	1	Bi	2	S	4	F	4														1	2017																										A2B3C4D4			I4/nmm																BiS2-plane SC	K			9.8		0	2.2	9.8																				T	RES(0.9Rn), WHH	3.04							T/K	RES(0.9Rn)	0.45			MHC158860		A	from Hc2	104																																	mOhm.cm							1.4				1.27																			Superconductivity induced by external pressure in Eu3-xSrxBi2S4F4 (x = 1, 2) compounds			Centre for High Pressure Research, School of Physics, Bharathidasan University, Tiruchirapalli-620024, India	Supercond.Sci.Technol., 30(2017)115011	M Kannan,G Kalai Selvan,Z Haque,Gohil S Thakur,B Wang,K Ishigaki,Y Uwatoko,L C Gupta,A K Ganguli,S Arumugam		
158861	SST030115011	P-induced SC. Pc = 2.37 GPa.  SC properties(DB) for P = 2.9 GPa. RRR = 85.9.  Activation energy Eg = 13.6 meV from R(T) fitting.	EuSr2Bi2S4F4	Eu1Sr2Bi2S4F4	Eu	1	Sr	2	Bi	2	S	4	F	4														1	2017																										A2B3C4D4			I4/nmm																BiS2-plane SC	K			8.2		0		8.2																				T	RES(0.9Rn), WHH	1.17							T/K	RES(0.9Rn)	0.21			MHC158861		A	from Hc2	167																																	mOhm.cm							2.69				2.31																			Superconductivity induced by external pressure in Eu3-xSrxBi2S4F4 (x = 1, 2) compounds			Centre for High Pressure Research, School of Physics, Bharathidasan University, Tiruchirapalli-620024, India	Supercond.Sci.Technol., 30(2017)115011	M Kannan,G Kalai Selvan,Z Haque,Gohil S Thakur,B Wang,K Ishigaki,Y Uwatoko,L C Gupta,A K Ganguli,S Arumugam		
158862	SST031115005	RRR = 1.3. SP  (beta) = 0.02 mJ/mol.K4. (dC/gamma*Tc) = 1.56.  e-ph = 0.43. Gap from SP analysis.  Hc2 = 0.47 T from WHH using dHc2/dT.	WB4.2	B4.2W1	B	4.2	W	1																				3	2018																										AB4.2			P6<3>/mmc	194	A	5.191		6.345												K	2	2.1					2.1											Oe	M-H curve				10			0.5	T	RES(0.5Rn), Linear approx.	0.71							T/K	RES(0.5Rn)	0.33			MHC158862		A	from Hc2	260								meV	0.22	2.44	14				MSP158862			mJ/mol.K2	2.07	SP	780	SP																																		B(2N5),W(3N)		mixture(W:B = 1:10) - arc-melting three times(600 mbar-Ar). single crystals obtained from arc-melted samples					Superconductivity in the superhard boride WB4.2			Department of Chemistry, Princeton University, Princeton, NJ 08544, United States of America	Supercond.Sci.Technol., 31(2018)115005	Elizabeth M Carnicom,Judyta Strychalska-Nowak,P Wi?niewski,D Kaczorowski,W Xie,T Klimczuk,R J Cava		
158863	SST031125005	needle-like (b-axis) crystals. Energy gap measured by Andreev reflection method. isotropic gap.	NiBi3	Bi3Ni1	Bi	3	Ni	1																				3	2018																										AB3		NiBi3																		K		4.07					4.07	MGAP158863																																															3.51	16																																															self-flux method. mixture(Ni:Bi = 1:10) - sealed in quartz tube - heat to 1150 C and soaked 2 h  - cool to 400 C with 5 C/h - remove the excess flux.					Singlet superconductivity in a single-crystal NiBi3 superconductor			Institute for Quantum Science and Engineering and Department of Physics of Southern University of Science and Technology, Shenzhen 518055, People's Republic of China	Supercond.Sci.Technol., 31(2018)125005	G J Zhao,X X Gong,P C Xu,B C Li,Z Y Huang,X F Jin,X D Zhu,T Y Chen		
158864	SST032035001	T<CDW> = 122 K.	Ta1+xSe2	Se2Ta1	Se	2	Ta	1																				1	2019																										AB2		MX2			A	3.432		12.76											mixed phase of 2H<b> + 3R	K					2																																																																																																Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158865	SST032035001		Ta1+xSe2	Se2Ta1.02	Se	2	Ta	1.02																				1	2019																										AB2		MX2			A	3.432		12.74											mixed phase of 2H<b> + 3R	K					2																																																																																																Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158866	SST032035001		Ta1+xSe2	Se2Ta1.04	Se	2	Ta	1.04																				1	2019																										AB2		MX2			A	3.432		12.748											mixed phase of 2H<b> + 3R	K					2																																																																																																Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158867	SST032035001	SP  (beta) = 0.7131 mJ/mol.K4. N(Ef) = 2.51 states/eV.fu.  e-ph = 0.675. (dC/gamma*Tc) = 0.517	Ta1+xSe2	Se2Ta1.06	Se	2	Ta	1.06																				1	2019																										AB2		MX2			A	3.434		12.732											mixed phase of 2H<b> + 3R	K		3.2					3.2																				kOe	SUS(on), GL fitting	10.14												MHC158867		nm	from Hc2	18															MSP158867			mJ/mol.K2	9.88	SP	201.5	SP																																		Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158868	SST032035001	N(Ef) = 2.35 states/eV.fu.  e-ph = 0.675. (dC/gamma*Tc) = 0.507	Ta1+xSe2	Se2Ta1.08	Se	2	Ta	1.08																				1	2019																										AB2		MX2			A	3.432		12.65											3R-phase	K		2.95					2.95																																																								mJ/mol.K2	9.27	SP	182.3	SP																																		Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158869	SST032035001	Tc(SUS) < 2.0 K. maybe small SC volume.	Ta1+xSe2	Se2Ta1.1	Se	2	Ta	1.1																				1	2019																										AB2		MX2			A	3.432		12.62											3R-phase	K		2.1					2.1																																																																																														Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158870	SST032035001	M-I transition at about 25 K from R(T).	Ta1+xSe2	Se2Ta1.12	Se	2	Ta	1.12																				1	2019																										AB2		MX2																	3R-phase	K					2																																																																																																Ta(3N),Se(4N)		mixture - sealed in quartz tube - heat(1173 K, 24 h) - FC to RT - reground - pellet - sealed in quartz tube - ANN(1173 K, 240 h) - cool to RT					Superconductivity enhancement in Ta1+xSe2 with a randomly stacked structure			Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China	Supercond.Sci.Technol., 32(2019)035001	X C Li,M H Zhou,C Dong		
158871	SST032115014	SP (beta) = 0.085 mJ/mol.K4. (dC/gamma*Tc) = 1.72. e-ph = 0.58. kappa(GL) = 6.6. DOS = 5.4 states/eV.fu from gamma. Anisotropy(R) = 14(300C)	Mo3P	Mo3P1	Mo	3	P	1																				3	2019																										AB3			I4[-]2m		A	9.8084		4.8352												K				5.6			5.6											Oe	M-H curve, (1-t^2)	190							kOe	RES(0.5Rn), GL fitting		41.2	13.7					kOe/K	RES(0.5Rn)		5	2.5	MHC158871		A	from Hc2	183			A	from Hc1, Hc2	1210					3.42	14				MSP158871			mJ/mol.K2	12.8	SP	454	SP											uOhm.cm								2.94				166																		Superconductivity in noncentrosymmetric Mo3P single crystal			Department of Physics, Hangzhou Normal University, Hangzhou 310036, People's Republic of China	Supercond.Sci.Technol., 32(2019)115014	Wuzhang Yang,Zhefeng Lou,Qinqing Zhu,Bin Chen,Hangdong Wang,Qianhui Mao,Jianhua Du,Jinhu Yang,Minghu Fang		
158872	SST032045010	SP  (beta) = 0.396 mJ/mol.K4.  (dC/gamma*Tc) = 0.86.  e-ph = 0.46.  kappa(GL) = 15.6.  carrier = electron	Nb5Sn2Al	Nb5Sn2Al1	Nb	5	Sn	2	Al	1																		1	2019																										AB2C5	2	W5Si3			A	10.638		5.225												K	2			2			2										85	mT	M-H curve, demag-correction	2							T	RES(zero), WHH	0.3												MHC158872		nm	from Hc2	32.8			nm	from Hc1, Hc2	516										MSP158872			mJ/mol.K2	19	SP	340	SP																																n/cm3	13000000000000000000000								Type-II superconductivity in W5Si3-type Nb5Sn2Al			Department of Physics, Fudan University, Shanghai 200433, People?s Republic of China	Supercond.Sci.Technol., 32(2019)045010	Jifeng Wu,Bin Liu,Yanwei Cui,Hangdong Wang,Zhicheng Wang,Zhi Ren,Guanghan Cao		
158873	SST032045010	SP  (beta) = 0.270 mJ/mol.K4. carrier = hole	Ti5Sn2Al	Ti5Sn2Al1	Ti	5	Sn	2	Al	1																		1	2019																										AB2C5	2	W5Si3			A	10.558		5.262												K					0.5																																																							MSP158872			mJ/mol.K2	31.5	SP	386	SP																																n/cm3	15000000000000000000000								Type-II superconductivity in W5Si3-type Nb5Sn2Al			Department of Physics, Fudan University, Shanghai 200433, People?s Republic of China	Supercond.Sci.Technol., 32(2019)045010	Jifeng Wu,Bin Liu,Yanwei Cui,Hangdong Wang,Zhicheng Wang,Zhi Ren,Guanghan Cao		
158874	NAT05720624	Possibility of nickelate superconducors; GL coherence length 3.25+-0.01 nm, Jc(2K)~ 170kAcm-2.	Nd0.8Sr0.2NiO2	Nd0.8Sr0.2Ni1O2	Nd	0.8	Sr	0.2	Ni	1	O	2																2	2019																											2		P4/mmm		A	3.92		3.34											SrFBiS2-type	K				7.5		2	7.5	158874Fig4																																	158874fig3		nm		3.25			micrometer		2.2							170000		158874Fig2																																										NdNiO3, NdSrNiO3	3	PLD method; stoichiometric targets of NdNiO3 and Nd0.8Sr0.2NiO3 were used. After the deposition, the films were reduced to Nd0.8Sr0.2NiO2 with CaH2 powders.		SrTiO3			Superconductivity in an infinite-layer nickalate	8	infinite-layer, nickalate	Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, Menlo Park, CA, USA	Nature, 572(2019)624	Danfeng Li,Kyuho Lee,Bai Yang Wang,Motoki Osada,Samuel Crossley,Hye Ryoung Lee,Yi Cui,Yasuyuki Hikita,Harold H. Wang		
158875	COMSMA01016	Absence of superconductivity in bulk Nd1-xSrxNiO2, even in high pressures up to 50.2GPa. Superconductivity happens in interface or stress-related effects in thin films.	Nd1-xSrxNiO2 (x=0,0.2,0.4)	Nd0.8Sr0.2Ni1O2	Nd	0.8	Sr	0.2	Ni	1	O	2																1	2020			muB/f.u.	2.32	emu mol-1	0.001																					2		P4/mmm		A	3.914		3.239											SrFBiS2-type																																																																																																						Nd0.8Sr0.2NiO2	1	solid state reaction of Nd2O3, NiO, and SrO at 1200C for 24 hrs, and the precursor of Nd2-2xSr2xNiO4, NiO, and KClO4 to synthesize Nd1-xSrxNiO3 with Oxygen sealed in a gold capsule at 1000C and 2GPa					Absence of superconductivity in bilk Nd1-xSrxNiO2	4	nickelate, superconductivity	National Laboratory of Solid State Microstructures and Depeartment of Physics, Center for Superconducting Physics and Naterials, Collaborative Innovation Center for Advanced Microstructures, Nanjing University, Nanjing 210093, China	Communications Materials, 1(2020)16	Qing Li,Chengpin He,Jin Si,Xiyu Zhu,Yue Zhang,Hai-Hu Wen		
158876	NATCOM01910233	Proximity-induced surface superconductivity of Dirac semi-metal Cd3As2 between Nb strands, Josephson coherent length x = 228-424 nm. Fraunhofer-like pattern was observed.	Cd3As2	Cd3As2	Cd	3	As	2																				2	2019																											2		I41/acd		A	12.67		25.48											tetragonal, 158876fig1	K	2.1					1	2.1	158876Fig2																																								nm		50			meV	0.2					158876Fig3																																										Cd3As2	3	Argon gas transport of Cd3As2 powders on Nb thin films		Nb			Proximity-induced surface superconductivity in Dirac semimetal Cd3As2	5	Dirac semimetal, surface superconductivity	State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, China	Nature Communications, 10(2019)10233	Ce Huang,Benjamin T. Zhou,Huiqin Zhang,Bingjia Yang,Ran Liu,Hanwen Wang,Yimin Wan,Ke Huang,Zhiming Liao,Enze Zhang,Shanshan Liu,Qingsong Deng,Yanhui Chen,Xiaodong Han,Jin Zou,Xi Lin,Zheng Han,Yihua Wang,Kam Tuen Law,Faxian Xiu		
158877	NATCOM110990	By X-ray diffraction method, F-CDW and AF-CDW coupling modify the electronic structure, in which F-CDW dominates in the superconducting and normal state properties of YBCO	YBa2Cu3O6.7	Y1Ba2Cu3O6.7	Y	1	Ba	2	Cu	3	O	6.7																3	2020																											3				A	3.82	3.87	11.7											T' phase	K	67						67																																																																																														YBa2Cu3O7	3	self-flux method					Spatially inhomogeneous competetion between superconductivity and the charge density wave in YBa2Cu36.67	2	YBaCuO, CDW, superconductivity	Physik-Institut, Universitaet Zuerich, Winterthuresrstrasse 190, CH-8057, Switzerland	Nature Communications, 11(2020)0990	J. Hoi,O. Ivashko,E. Blackburn,R. Liang,D.A. Bonn,W.N. Hardy,A.T. Holmes,N.B. Christensen,M. Huecker,S. Gerber,O. Gutouski,U. Ruett,M.v. Zimmermann,E.M. Forgan,S.M. Hayden,J. Chang		
158878	PRM3093601	smectic-nematic transition in perpendicular direction to Cu-O plane	Tb2Cu0.83Pd0.17O4	Tb2Cu0.83Pd0.17O4	Tb	2	Cu	0.83	Pd	0.17															O	4		1	2019																											2	K2NiO4	Pbca																	K	0	0	0				0																																		158878fig1																																																												Gd2O3, Tb4O7, Dy2O3, PdO, CuO	1	Tb4O7 was reduced to Tb2O3 at 700C for 24hrs. Mixture with intermediate grinding heated in a alumina crucible at 1000C under air for 36hrs, and at 1050C for 36hrs.					Smectic and nematic phase modulations and transitions under electron beam in Tb2Cu0.83Pd0.17O4	12	214, Tb, Pd, smectic, nematic	Beijing National Laboratory of Condenced Matter, Insitute of Physics, Chinese Academy of Science, Beijing 100190, China	Physical Review Materials 3(2019)093601	Wei Wang,Kai Sun,Yuzki M. Oey,Robert J. Cava,Lijun Wu,Yimei Zhu,Richeng Yu,Jing Tao		
158879	PRM3091401R	Ferroelectric fluctuations may be a origin of superconductivity in SrTiO3	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		4	2019																											2	Perovskite	4/mmm, 4mm																	K	0	0	0				0																																		158879fig1																																																									158879fig2			SrTiO3	17	Sm-doped SrTiO3 film was epitaxially grown on (LaAlO3)0.3(Sa2AlTaO6)0.7(LAST) substrate at 900C by MBE.					Ferroelectric enhancement of superconductivity in compressively strained SrTiO3 films	9	SrTiO3, strained, ferroelectric	Materials Department, University of California, Santa Barbara, California 93106, USA	Physical Review Materials 3(2019)091401(R)	Ryan Russell,Noah Ratecliff,Kaveh Ahadi,Lianyang Dong,Susanne Stemmer,John W. Harter		
158880	SADEAAW0120	Enhancing superconductivity in SrTiO3 films with strain	SrTiO3	Sr1Ti1O3	Sr	1	Ti	1																	O	3		5	2019																											2	Perovskite	4/mmm, 4mm																	K							0.67	158880fig1																			T					0.91									158880fig3		nm		19								micro-eV	100																																												158880fig2			SrTiO3	17	Sm-doped SrTiO3 film was epitaxially grown on (LaAlO3)0.3(Sa2AlTaO6)0.7(LAST) substrate at 900C by MBE.					Enhancing superconductivity in SrTiO3 films with strain	4	SrTiO, strain, ferroelectric	Materials Department, University of California, Santa Barbara, California 93106, USA	Science Advances,5(2019)eaaw0120	Kaveh Ahadi,Luca Gilletti,Yuntian Li,Salva Salmani-Rezie,Wangzhou Wu,Susanne Stemmer		
158881	NAT5690528	highest critical temperature of around 250K was achieved in a high pressure as around 150GPa, isotope effect observed	LaH	La1H10	La	1	H	10																				1	2019																											1	fcc	Fm3m		A	5.1019														K							250	158881fig1							0.46												T					136									158881fig2																																				158881fig3																								La, H2	1	synthesized from La+H2 mixture, heated at high pressure as 145GPa					Superconductivity at 250K in lanthanaum hydride under high pressures	5	LaH10,high pressure	Maxplanck Institut fuer Chemie, Mainz, Germany	Nature 569(2019)528	A.P. Drozdov,P.P. Kong,V.S. Minkov,S.P. Besedin,M.A. Kuzovnikov,S. Mozaffari,L. Balicas,F.F. Balakirev,D.E. Graf,V.B. Prakapenka,E. Greenberg,D.A. Knyazev,M. Tkacz,M.I. Eremets		
158882	NCT110569	In the overdoped Bi2Sr2Cu2O8+d, superconductivity disappears due to vanishing copupling, eliminating phononic mechanism and originating the spin-fluctuation.	Bi2Sr2CuO2O8+d	Bi2Sr2Cu1O8+d	Bi	2	Sr	2	Cu	1															O	8+d		3	2020																											3																			K							91	158882fig1																																														16		9			158882fig2																																										Bi2O3, Sr2O, CuO, CaO	7	as-grown single crystal is overdoped, and by annealing in ozone atomosphere at 350-480C					Disappearance of superconductivity due to vanishing coupling in the overdoped Bi2Sr2CaCu2O8+deltha	1	Bi2Sr2CaCu2O8+deltha, ARPES, overdoped	Condensed Matter Physics and Materials Science Department, Brookhaven Lab., Upton, NY 11973, USA	Nature Communications 11(2020)569	T. Vella,I.K. Drozdov,G.D. Gu		
158883	SAD3E1601667	heavy-fermion of CeCu2Si2 has a fully-gapped superconductivity with no sign change and nodes in Fermi surface.	CeCu2Si2	Ce1Cu2Si2	Ce	1	Cu	2	Si	2																		3	2017																											2	ThCr2Si2																		K							0.71	158883fig1	1									mT	Hall sensor			1.2			0.32																		nm			4.7	6.9	nm	tunnel diode oscillator tech		700		K	0.39		3							mJ/K2mol	15	C/T			W/K2m				158883fig2																													CeCu2Si2	5	self-flux method combined with a Bridgman cooling technique in an Al2O3 crucible together with a 40 mol% excess Cu as self flux					Fully gapped supercondcutivity with no sign change in the prototypical heavy-fermion CeCu2Si2	6	heavy-fermion, CeCu2Si2	Department of Physics, Kyoto University, Kyoto 606-8502, Japan	Science Advances 3(2017)e160667	T. Yamashita,T. Takenaka,Y. Tokiwa,J. Wilcox,Y. Mizukami,D. Terazawa,Y. Kasahara,S. Kittaka,T. Sakakibara,M. Konczykowski,S. Seiro,H. S. Jeeven,C. Geibel,C. Putzke,T. Onishi,H. Ikeda,A. Carrington,T. Shibauchi,Y. Matsuda		
158884	SADEABB8570	Transparent p-type superconductor Li1-xNbO2 was epitaxially grown on MgAl2O4 substrate with Tc of about 4K.	Li1-xNbO2	Li1Nb1O2	Li	1	Nb	1																	O	2		5	2020																											2	MoS2			A	2.914		10.468	1											K							3.9	158884fig1	1																																158884fig2																																																												Li3NbO4	17	After growing by a PLD in vacuum, in-situ annealing was made at 800C with Ar/H2 atomosphare of 0.1mTorr, and then, Li deintercalation was made with 0.02Ml2/CH3CN in air.	17	MgAl2O4	Li3NbO4		p-type transparent superconductivity in a layered oxide	7	superconductivity, LiNbO2, two-dimmensional	Department of Chemical Science and Engineering, Tokyo Institute of Technology, 2-12-1 Ookayama, Megro, Tokyo 152-8552, Japan	Science Advances 6(2020)eabb8570	T. Soma,K. Yoshimatsu,A. Ohtomo		
158885	STA190909	For data-driven approach, pressure-induced superconductivity was found in PbBi2Te4	Pb0.9Bi2Te3.8	Pb0.9Bi2Te3.8	Pb	0.9	Bi	2	Te	3.8																		3	2018																											6		R-3m		A	4.42	4.42	41.57	1											K							7.9	158885fig1	1	GPa		50.8															T	resistivity	5.8	21.7			0								158885fig2																											W/K.m	1.54				microW/mK2			100																									PbBi2Te4	9	In the stoichiometric composition of Pb grains, Bi ones, and Te chips was melted and slow-cooling to grow single crystals in a evacuated quartz tube from 100C to 800C.					Data-driven exploaration of new pressure-induced superconductivity in PbBi2Te4	11	data-driven, supercnductivity, high-ressure	MA, National Institute for Materials Science, Sengen 1-2-1, Tsukuba 305-0047, Japan	Science and Technology of Advanced Materials 19(2018)909	R. Matsumoto,Zh. Hou,M. Nagao,S. Adachi,H. Hara,H. Tanaka,K. Nakamura,R. Murakami,S. Yamamoto,H. Takeya,T. Irifune,K. Terakura,Y. Takano		
158886	TSF1280275	The influence of film thickness and annealing temperature in Li1+xTi2-x4thin films was examined on the electrical resistivity and the superconducting transition temperature.	Li1+xTi2-xO4	Li1Ti2O4	Li	1	Ti	2																	O	4		4	1985																												spinel																		K							13.6	158886fig1	1																																																800000		158886fig2																			ohmcm											0.0013			cm3C-1	-61						cm3C-1	11000000000000000000000	LiTi2O4	16	LTO films were deposited onto suppire(1102) substrates at 200-300C by r.f. magnetron sputtering. The films were annealed at 750-1000C in a hydrongen flow for 6 hrs.		Al2O3	LiTi2O4	r.f.hot pressing mixed Li2Ti2O5 and Ti2O3 powders	Influence of film thickness and annealing temperature on superconducting Li1+xTi2-xO4	2	LiTi2O4, superconductivity, thin films	Ibaraki Electrical Communication Laboratory, Nippon Telegraph and Telephone Public Corporation, Tokai, Ibaraki^ken, 319-11, Japan	Thin Solid Films, 128(1985)275	T. Inukai,T. Murakami		
158887	APL1010123103	The epitxial thin film growth of LiTi2O4 superconductor has been achieved with the highest Tc of 12K on the substrate of MgAl2O4 (111).	LiTi2O4	Li1Ti2O4	Li	1	Ti	2																	O	4		4	2012																												spinel			nm															K				12			12	158887fig1	2																																																																					ohmcm											0.00033									158887fig2			Li4Ti5O12	17	By PLD method, Li4Ti5O12 and LiTi2O4 epitaxial thin films were obtained with varyong the Oxygen partial pressure between 1 x 10-3 and 1 x 10-7 Torr.		MgAl2O4	Li4Ti5O12		Growth processes of lithium titanate thin films deposited by using pulsed laser deposition	9	PLD, LiTi2O4, superconductivity	Advanced Institute for Materials Research, Tohoku University, 980-8577 Sendai, Japan	Applied Physics Letters 101(2012)123103	A. Kumatani,T. Ohsawa,R. Shimizu,Y. Takagi,S. Shiraki,T. Hitosugi		
158888	PRR02013373	From a Raman scattering study, a distinct pair-breaking excitation was detected across the gap. Analyzing the phonon self-energy effects, the e-p coupling constant is too small to explain SC.	Fe1+yTe0.6Se0.4	Fe1Te0.6Se0.4	Fe	1	Te	0.6	Se	0.4																		3	2020																											2	PbO	P4/nmm																	K				14			14	158888fig1	2																																												meV	2.8		4			158888Tab1																																										Fe1+yTe0.6Se0.4	10	modified Bridgeman method.					Superconductivity and phonon self-energy effects in Fe(1+y)Te0.6Se0.4	3	superconductivity, FeTeSe, Raman spectroscopy, electron-phonon coupling	Department of Physics and Astronomy, Ruttgers University, Piscataway, New Jersey 08854, USA	Physical Review Research, 2(2020)013373	S.-F. Wu,A. Almoalem,I. Feldman,A. Lee,A. Kanigel,G. Blumberg		
158889	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.25) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se1S0	Fe1Se1S0	Fe	1	Se	1	S	0																		3	2019																											2	PbO	P4/nmm																	K							8.75	158889fig1	2																																158889fig2																																					microohmcm		5.3																	350000				Fe1Se1S0	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-200C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158890	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.26) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.95S0.05	Fe1Se0.95S0.05	Fe	1	Se	0.95	S	0.05																		3	2019																											2	PbO	P4/nmm																	K							9.12	158890fig1	2																																																																					microohmcm		16.9																	350000				Fe1Se0.95Se0.05	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-201C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158891	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.27) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.90S0.10	Fe1Se0.9S0.1	Fe	1	Se	0.9	S	0.1																		3	2019																											2	PbO	P4/nmm																	K							8.91	158891fig1	2																																																																					microohmcm		11.3																	350000				Fe1Se0.90Se0.10	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-202C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158892	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.28) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.87S0.13	Fe1Se0.87S0.13	Fe	1	Se	0.87	S	0.13																		3	2019																											2	PbO	P4/nmm																	K							8.7	158892fig1	2																																																																					microohmcm		17.46																	350000				Fe1Se0.87Se0.13	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-203C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158893	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.29) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.84S0.16	Fe1Se0.84S0.16	Fe	1	Se	0.84	S	0.16																		3	2019																											2	PbO	P4/nmm																	K							8.91	158893fig1	2																																																																					microohmcm		17.08																	350000				Fe1Se0.84Se0.16	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-204C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158894	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.30) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.82S0.18	Fe1Se0.82S0.18	Fe	1	Se	0.82	S	0.18																		3	2019																											2	PbO	P4/nmm																	K							7.96	158894fig1	2																																																																					microohmcm		13.56																	350000				Fe1Se0.82Se0.18	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-205C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158895	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.31) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.80S0.20	Fe1Se0.8S0.2	Fe	1	Se	0.8	S	0.2																		3	2019																											2	PbO	P4/nmm																	K							5.99	158895fig1	2																																																																					microohmcm		13.06																	350000				Fe1Se0.80Se0.20	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-206C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158896	NAT56700213	Electronic nematicity was clarified around the quantum critical point(x=0.16) of FeSe(1-x)Sx(x=0-0.32) in the normal state of resistivity, braeking the superconductivity in high magnetic fields.	Fe1Se0.75S0.25	Fe1Se0.75S0.25	Fe	1	Se	0.75	S	0.25																		3	2019																											2	PbO	P4/nmm																	K							7.39	158896fig1	2																																																																					microohmcm		8.37																	350000				Fe1Se0.75Se0.25	18	chemical vapour transport technique. Fe, Se and S powders with KCL and AlCl3 was sealed in an evacuated quartz tube heated at 390-450C on one end, while the other end was kept at 140-207C.					Electrical resistivity across a nematic quantum critical point	3	FeSeS, quantum critical point, nematic phase	High Field Magnet Laboratory(HFML-EMFL) and institute for Molecules and Materials, Radboud University, Nijimegen, The netherlands	Nature 567(2019)213	S. Licciardello,J. Buhot,J. Lu,J. Ayres,S. Kasahara,Y. Matsuda,T. Shibauchi,N. E. Hussey		
158897	PRR01033154	Direct evidence for the coupling between nematicity and superconductivity has been confirmed. The nematic fluctuations is important for the superconductivity in iron-based superconductors.	BaFe1.9Ni0.1As2	Ba1Fe1.9Ni0.1As2	Ba	1	Fe	1.9	Ni	0.1	As	2																12	2019																											2	ThCr2Si2																		K							19.2	158897fig1	1	mK/MPa	4	15																																															158897fig3																																											5	self-flux method					Nonlinear uniaxial pressure dependence of Tc in iron-based superconductor	12	iron-based superconductors, pressure, Tc	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Physical Review Research 1(2019)033154	Z. Liu,Y. Gu,W. Hong,T, Xie,D. Gong,X, Ma,J. Liu,C. Hu,L. Zhao,X. Zhou,R. M. Fernandes,Y-f. Yang,H. Luo,S. Li		
158898	PRR01033154	Direct evidence for the coupling between nematicity and superconductivity has been confirmed. The nematic fluctuations is important for the superconductivity in iron-based superconductors.	Ba0.67Fe2K0.33As2	Ba0.67Fe2K0.33As2	Ba	0.67	Fe	2	K	0.33	As	2																12	2019																											2	ThCr2Si2																		K								158897fig2	1	mK/MPa	-1	15																																															158897fig3																																											5	self-flux method					Nonlinear uniaxial pressure dependence of Tc in iron-based superconductor	12	iron-based superconductors, pressure, Tc	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Physical Review Research 1(2019)033154	Z. Liu,Y. Gu,W. Hong,T, Xie,D. Gong,X, Ma,J. Liu,C. Hu,L. Zhao,X. Zhou,R. M. Fernandes,Y-f. Yang,H. Luo,S. Li		
158899	PRR01033154	Direct evidence for the coupling between nematicity and superconductivity has been confirmed. The nematic fluctuations is important for the superconductivity in iron-based superconductors.	KFe2As2	K1Fe2As2	K	1	Fe	2	As	2																		12	2019																											2	ThCr2Si2																		K									1	mK/MPa	-2	15																																															158897fig3																																											5	self-flux method					Nonlinear uniaxial pressure dependence of Tc in iron-based superconductor	12	iron-based superconductors, pressure, Tc	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Physical Review Research 1(2019)033154	Z. Liu,Y. Gu,W. Hong,T, Xie,D. Gong,X, Ma,J. Liu,C. Hu,L. Zhao,X. Zhou,R. M. Fernandes,Y-f. Yang,H. Luo,S. Li		
158900	PRR01033154	Direct evidence for the coupling between nematicity and superconductivity has been confirmed. The nematic fluctuations is important for the superconductivity in iron-based superconductors.	LaFeAsO0.74F0.26	La1Fe1As1F0.26O0.74	La	1	Fe	1	As	1	F	0.26													O	0.74		12	2019																											2	ThCr2Si2																		K									1	mK/MPa	4	15																																															158897fig3																																											5	self-flux method					Nonlinear uniaxial pressure dependence of Tc in iron-based superconductor	12	iron-based superconductors, pressure, Tc	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Physical Review Research 1(2019)033154	Z. Liu,Y. Gu,W. Hong,T, Xie,D. Gong,X, Ma,J. Liu,C. Hu,L. Zhao,X. Zhou,R. M. Fernandes,Y-f. Yang,H. Luo,S. Li		
158901	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.096.	BaFe2As2	Ba1Fe2As2As2	Ba	1	Fe	2	As	2	As	2																3	2011								134																			2	ThCr2Si2			nm			1.303											Structual transition at around 134K	K								158901fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158902	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.097.	BaFe1.97Ni0.03As2	Ba1Fe1.97Ni0.03As2	Ba	1	Fe	1.97	Ni	0.03	As	2																3	2011								105																			2	ThCr2Si2																	Structual transition at around 110K	K								158902fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158903	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.098.	BaFe1.935Ni0.065As2	Ba1Fe1.935Ni0.065As2	Ba	1	Fe	1.935	Ni	0.065	As	2																3	2011								64																			2	ThCr2Si2																	Structual transition at around 74K	K				7.8			7.8	158903fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158904	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.099.	BaFe1.925Ni0.075As2	Ba1Fe1.925Ni0.075As2	Ba	1	Fe	1.925	Ni	0.075	As	2																3	2011								52																			2	ThCr2Si2																	Structual transition at around 62K	K				13.2			13.2	158904fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158905	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.100.	BaFe1.915Ni0.085As2	Ba1Fe1.915Ni0.085As2	Ba	1	Fe	1.915	Ni	0.085	As	2																3	2011								41																			2	ThCr2Si2																	Structual transition at around 42K	K				16.9			16.9	158905fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158906	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.101.	BaFe1.908Ni0.092As2	Ba1Fe1.908Ni0.082As2	Ba	1	Fe	1.908	Ni	0.082	As	2																3	2011								43																			2	ThCr2Si2																	Structual transition at around 40K	K				18.5			18.5	158906fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158907	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.102.	BaFe1.90Ni0.10As2	Ba1Fe1.9Ni0.1As2	Ba	1	Fe	1.9	Ni	0.1	As	2																3	2011																											2	ThCr2Si2																		K				20.1			20.1	158907fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158908	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.103.	BaFe1.88Ni0.12As2	Ba1Fe1.88Ni0.12As2	Ba	1	Fe	1.88	Ni	0.12	As	2																3	2011																											2	ThCr2Si2																		K				19			19	158908fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158909	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.104.	BaFe1.85Ni0.15As2	Ba1Fe1.85Ni0.15As2	Ba	1	Fe	1.85	Ni	0.15	As	2																3	2011																											2	ThCr2Si2																		K				14.1			14.1	158909fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158910	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.105.	BaFe1.82Ni0.18As2	Ba1Fe1.82Ni0.18As2	Ba	1	Fe	1.82	Ni	0.18	As	2																3	2011																											2	ThCr2Si2																		K				8.7			8.7	158910fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158911	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.106.	BaFe1.80Ni0.20As2	Ba1Fe1.8Ni0.2As2	Ba	1	Fe	1.8	Ni	0.2	As	2																3	2011																											2	ThCr2Si2																		K				5.2			5.2	158911fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158912	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.107.	BaFe1.75Ni0.25As2	Ba1Fe1.75Ni0.25As2	Ba	1	Fe	1.75	Ni	0.25	As	2																3	2011																											2	ThCr2Si2																		K								158912fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158913	SST024065004	High-quality large single crystals of Ni-doped Ba2Fe2As2 were grown, and the phase diagram was established with QCP point of x=0.108.	BaFe1.70Ni0.30As2	Ba1Fe1.7Ni0.3As2	Ba	1	Fe	1.7	Ni	0.3	As	2																3	2011																											2	ThCr2Si2			nm			1.297												K								158913fig1	1																																																		158901fig2																																										Fe/Ni-As powders	5	self-flux method with Fe/Ni-As powders as precursor sealed in an evacuated quartz tube(BFNA in aluminum oxide crucible).					Systemtic growth of BaFe2-xNixAs2 large crystals	2	iron-based superconductors, Ni doping, Tc, crystal growth	Institute of Physics and National Laboratory for Condenced Matter Physics, Chinese Academy of Science, Beijing 100191, China	Supercond. Sci. Technol. 24(2011)065004	Y. Chen,X. Lu,M. Wang,H. Luo,S. Li		
158914	PRB101104504	magnetic-flux evolution in the magnetic superconductor RbEuFe4As4 was confirmed with magneto-optical imaging.	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																3	2020																											2		P4/mmm		nm	3.88825	3.8825	13.273												K						0.5	37	158914fig1	2																																158914fig2		nm	magnetization		1.4	0.92	nm		160		94																																																		5	large single crystal growth by RbAs flux with an alumina crucible emcapseled in a silica tube, using prereacted binary precursors RbAs, EuAs, and Fe2As powders.					Cooperative response of magnetism and superconductivity in the magnetic superconductor RbEuFe4As4	3	RbEuFe4As4, magnetic superconductor	Materials Science Divisio, Argonne National Laboratory, Argonne, Illinois 60439, USA	Phys. Rev, B101 (2020)104504	V.K. Vlasko-Vlasov,U. Welp,A,E. Koshelev,M. Smylie,J.-K. Bao,D.Y. Chung,M.G. Kanatzidis,W.-K. Kwok		
158915	CGD01803517	large single crystal growth of RbEuFe4As4, and the results of Tc and heat capacity measurements.	RbEuFe4As4	Rb1Eu1Fe4As4	Rb	1	Eu	1	Fe	4	As	4																4	2018	emu/mol	0.0128					17																				2		P4/mmm		nm	3.88825	3.8825	13.273												K							37.8	158915fig1	2																																																					37										158915fig2																														5	large single crystal growth by RbAs flux with an alumina crucible emcapseled in a silica tube, using prereacted binary precursors RbAs, EuAs, and Fe2As powders.					Single crystal growth and study of the ferromagnetic superconductor RbEuFe4As4	4	RbEuFe4As4, ferromagnetic superconductor, crystal growth	Materials Science Divisio, Argonne National Laboratory, Argonne, Illinois 60440, USA	Cryst. Growth Des. 18(2018)3517	J.-K. Bao,K. Willa,M. Smylie,H. Chen,U. Welp,D.Y. Chung,M.G. Kanatzidis		
158916	NAC01201462	Enhancement of in-plane upper critical magnetic field, caused by spin-orbit coupling locking measured by in-situ electron transport measurements.	In	In1	In	1																						3	2021																																													atomic layer on Si(111)	K							3.14	158916fig1	3																		T														158916fig2		nm				41.3												158916Tab1																			ohm							35.9																In	17	atomic layer of In on Si(111)				Due to the Si surface, causing the out-of-plane inversion symmetry and leading to the Rashbatype SOC.	Atomic-layer Rashba-type superconductor protected by dynamic spin-momentum locjing	3	atomic layer, Rashba-tyoe, superconductor, spin-orbit coupling	Research Center for Advnced Measurement and Characterization, National Institute for Materials Science, Tsukuba, Ibaraki, JAPAN	Nature Commun. 12(2021)1462	S. Yoshizawa,T. Kobayashi,Y. Nakata,K. Yaji,F. Komori,K. Sakamoto,T. Uchihashi		
158917	PRB101104511	By high-energy X-ray diffraction measurements at high pressures and low temperatures, a rapid suppression of the superlattice transition is associated with the emergency of quantum fluctuations.	Ca3Ir4Sn13	Ca3Ir4Sn13	Ca	3	Ir	4	Sn	13																		3	2020																													Pm3n																	K							5	158917fig1	3																																158917fig1																																																												Ca, Ir, Sn	5	Sn-flux method					Possible quantum fluctuations in the vicinity of the quantum critical point of (Sr,Ca)3Ir4Sn13 revealed by high-energy x-ray diffraction	5	(Sr,Ca)3Ir4Sn13, quantum fluctuation, quantum critical point, x-ray	Deutches Elektronen-Synchrotron(DESY), Hamburg 22607, Germany	Phys. Rev. B101 (2020)104511	L.S.I. Veiga,J.R.L. Mardegan,M.v. Zimmermann,D.T. Maimone,F.B.Carneiro,M.B. Fontes,J. Strempfer,E. Granado,P.G. Pagliuso,E.M. Bittar		
158918	PRB101104511	By high-energy X-ray diffraction measurements at high pressures and low temperatures, a rapid suppression of the superlattice transition is associated with the emergency of quantum fluctuations.	Sr3Ir4Sn13	Sr3Ir4Sn13	Sr	3	Ir	4	Sn	13																		3	2020																													Pm3n																	K							7	158917fig1	3																																158917fig1																																																												Ca, Ir, Sn	5	Sn-flux method					Possible quantum fluctuations in the vicinity of the quantum critical point of (Sr,Ca)3Ir4Sn13 revealed by high-energy x-ray diffraction	5	(Sr,Ca)3Ir4Sn13, quantum fluctuation, quantum critical point, x-ray	Deutches Elektronen-Synchrotron(DESY), Hamburg 22607, Germany	Phys. Rev. B101 (2020)104511	L.S.I. Veiga,J.R.L. Mardegan,M.v. Zimmermann,D.T. Maimone,F.B.Carneiro,M.B. Fontes,J. Strempfer,E. Granado,P.G. Pagliuso,E.M. Bittar		
158919	PRB101134502	The upper critical field of multiband superconductor CaKFe4As4 was mapped out up to 90T for different orientations and at temperature down to 4.K.	CaKFe4As4	Ca1K1Fe4As4	Ca	1	K	1	Fe	4	As	4																3	2020																												ThCr2Si2-type	I4/mmm																	K	34.94	34.97	35.01			0.07	34.97	158919fig1	2																		T														158919fig2																		158919fig3																																										Sr, Ir, Sn	5	Sn-flux method					Competing pairing interactions responsible for the large upper critical field in a stoichiometric iron-based superconductor CaKFe4As4	4	CaKFe4As4, upper critical field, FFLO state	Clarendon Laboratory, Department of Phusics, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom	Phys. Rev. B101 (2020)134502	M. Bristow,W. Knafo,P. Reiss,W. Meier,P. C. Canfield,S. J. Blundell,A. I. Colda		
158920	PRB101115422	The transport characteristics in 2D superconductor NbC are understood in terms of coupled Josephson junctions, forming between isolated NbC crystals.	NbC	Nb1C1	Nb	1	C	1																				4	2020																											1	NaCl	Pm3m		nm	0.45	0.45	0.45	1											K							7	158920fig1	3																																158920fig2																																																												CH4	18	Nb atoms are diffused to Cu foil, become the high nucleation density, and NbC samples have the thickness of 10 to 20 nm.			Cu/Nb foil	NbC islands grow along (111) perpendicular to the substrate.	Transport through a network of two-dimensional NbC superconducting crystals connected via weak links	3	NbC, weak link	Key Laboratory for the Physics and Chemistry of Nanodevices and Department of Electronics, Peking University, Beijing 100871, China	Phys. Rev. B101 (2020)115422	M. Hao,Ch. Xu,Zh. Liu,Ch. Wang,Zh. Liu,S. Sun,H-M. Cheng,W. Ren,N. Kang		
158921	PRB101134506	By measuring resistivity, Hall coefficient, and Raman scattering at high pressures on TaS2, CDW  was observed to disappear at 7.3 Gpa, and reveals characeristics of distinct pressure-tunable.	TaS	Ta1S2	Ta	1	S	2																				3	2020																											7		R3c		nm	0.33	0.33	0.6	1											K							0.8	158921fig3	3																																																																																												Ta, S		2H-TaS was systhesized at HQ-Graphene.					Pressure tuning of the charge density wave and superconductivity in 2H-TaS2	4	TaS2, charge density wave, pressure	College of Materials Science and Engineering, Henan University of Technology, Zhengzhou, Zhengzhou 450001, China	Phys. Rev. B101 (2020)134506	X-M. Zhao,K. Zhang+A19,Z-Y. Cao,Z-W. Zhao,V. V. Struzhkin,A. F. Gonchanov,H-K. Wang,A. G. Gavrikiuk,H-K. Mao,X-J. Chen		
158922	PRB101134513	By extensive measurements of muon-spin technique, electrical resistivity, magnetizatio, and specific heat, a multiple- to single gap SC is suggested in the Nb5Ir3-xPtxO family.	Nb5Ir3O	Nb5Ir3O1	Nb	5	Ir	3																	O	1		3	2020																											2	Ti5Ga4-type	P4/mmm		nm	0.7861		0.5092	1											K							10.5	158922fig1	5																		T	MH	11.2												158922fig2		nm		5.4			nm	TF-mueSR	230										158922fig3	Jmol-1K-2	0.075	mJmol-1K-2	37		380	sp-heat																																		Nb, Ir, O	9	Nb5Ir3-xO was prepared by arc-melting with a mixture of Nb, Nb2O5 and Ir poaders.				arc-melting method.	Crossover from multiple- to single-gap superconductivity in Nb5Ir3-PtxO alloys	4	Nb5Ir3-PtxO, mu-SR, nodeless	Physik-Institut, Universitat Zurich, Winterthureerstrasse 190, CH-8057 Zurich, Switzerland	Phys. Rev. B101 (2020)134513	Y. Xu,S. Johr,L. Das,J. Kitagawa,M. Medarde,T. Shiroka,J. Chang,T. Shang		
158923	PRB101134513	By extensive measurements of muon-spin technique, electrical resistivity, magnetizatio, and specific heat, a multiple- to single gap SC is suggested in the Nb5Ir3-xPtxO family.	Nb5Ir1.4Pt1.6O	Nb5Ir1.4Pt1.6O1	Nb	5	Ir	1.4	Pt	1.6															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7916		0.5065	1											K							9.1	158922fig1	5																		T	MH	12.7												158922fig2		nm		5.1			nm	TF-mueSR	314										158922fig3	Jmol-1K-2	0.05	mJmol-1K-2	42		365	sp-heat																																		Nb, Ir, Pt, O	9	Nb5Ir1.4Pt1.6O was prepared by remelting the Nb5Ir3-xO with Pt wire.				arc-melting method.	Crossover from multiple- to single-gap superconductivity in Nb5Ir3-PtxO alloys	4	Nb5Ir3-PtxO, mu-SR, nodeless	Physik-Institut, Universitat Zurich, Winterthureerstrasse 190, CH-8057 Zurich, Switzerland	Phys. Rev. B101 (2020)134513	Y. Xu,S. Johr,L. Das,J. Kitagawa,M. Medarde,T. Shiroka,J. Chang,T. Shang		
158924	PRB101134516	Measuring the c-axis Jc current in Fe1+yTe1-xSex single crystals, depairing limit along the c-axis is investigated, based on the GL theory.	FeTeSe	Fe1Te0.8Se0.2	Fe	1	Te	0.8	Se	0.2																		3	2020																											2		P4/mmm		nm	0.39744		0.50219												K							8.6	158924fig3	3																																																																																												Fe, Te, Se	10	The powders of Fe, Te, and Se are doubly sealed in the fused quartz tube.				Gradient freezing method.	Achieving the depairing limit along the c axis in Fe1+yTe1-xSex single crystals	4	Fe1+yTe1-xSex, depairing, Jc	Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	Phys. Rev. B101 (2020)134516	Y. Sun,H. Ohnuma,S. Ayukawa,T. Noji,Y. Koike,T. Tamegai,H. Kitano		
158925	PRB101134516	Measuring the c-axis Jc current in Fe1+yTe1-xSex single crystals, depairing limit along the c-axis is investigated, based on the GL theory.	FeTeSe	Fe1Te0.7Se0.3	Fe	1	Te	0.7	Se	0.3																		3	2020																											2		P4/mmm																	K							11.9	158924fig3	3																																																																																												Fe, Te, Se	10	The powders of Fe, Te, and Se are doubly sealed in the fused quartz tube.				Gradient freezing method.	Achieving the depairing limit along the c axis in Fe1+yTe1-xSex single crystals	4	Fe1+yTe1-xSex, depairing, Jc	Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	Phys. Rev. B101 (2020)134516	Y. Sun,H. Ohnuma,S. Ayukawa,T. Noji,Y. Koike,T. Tamegai,H. Kitano		
158926	PRB101134516	Measuring the c-axis Jc current in Fe1+yTe1-xSex single crystals, depairing limit along the c-axis is investigated, based on the GL theory.	FeTeSe	Fe1Te0.6Se0.4	Fe	1	Te	0.6	Se	0.4																		3	2020																											2		P4/mmm																	K							13.7	158924fig1	3																																		nm	Jc	3			um	Jc	1.32							13000000		158924fig3																																										Fe, Te, Se	10	The powders of Fe, Te, and Se are doubly sealed in the fused quartz tube.				Gradient freezing method.	Achieving the depairing limit along the c axis in Fe1+yTe1-xSex single crystals	4	Fe1+yTe1-xSex, depairing, Jc	Department of Physics and Mathematics, Aoyama Gakuin University, Sagamihara 252-5258, Japan	Phys. Rev. B101 (2020)134516	Y. Sun,H. Ohnuma,S. Ayukawa,T. Noji,Y. Koike,T. Tamegai,H. Kitano		
158927	PRB101134521	The cooperative electronic phenomena of charge density wave and superconductivity are demonstrated to coexist in the cluster compound K2Mo15Se19.	K2Mo15Se19	K1Mo15Se19	K	1	Mo	15	Se	19																		3	2020																											7		R3c		nm	0.97093		5.81385	1											K				2.8			2.8	158927fig1	2									mT		12						0	T		2.9												158927fig2		nm		11			nm		200			meV	0.4									mJmol-1K-2	63		183																																			K, Mo, Se	1	Synthsizing MoSe2, K2Mo6Se6 and Mo powders (K2Mo6Se6 was synthsized with In2Mo6Se6 and KCl chemical reaction), single crystal is obatined from polycrystalline K2Mo15Se19 with furnace-cooled process.				During the crystal growth process, contamination by oxygen and moisture must be avoided.	Coexistence of a charge density wave and superconductivity in the cluster compound K2Mo15Se19	4	K2Mo15Se19, charege density wave	Institut Jean La, mour, UMR 7198 CNRS-Universite de Lorraine, Campus ARTEM, 2 allee Andre Guinier, Boite Postale 50840, 54013 Nancy, France	Phys. Rev. B101 (2020)134521	C. Candolfi,M. Misek,P. Gougeon,R. AL R. Al Orabi,P. Gall,R. Gautier,S. Migot,J. Ghanbaja,J. Kastil,P. Levinsky,J. Hejtmanek,A. Dauscher,B. Malaman,B. Lenoir		
158928	PRB101134523	Using a SANS, empirical fittings to the temperature dependence of the form factor and penetration depth rule out a simple s-wave model, but support the nodes in the gap function.	TlNi2Se2	Tl1Ni2Se2	Tl	1	Ni	2	Se	2																		3	2020																											2	ThCr2Si2-type	I4/mmm		nm	0.387		1.3435	1											K							3.55	158928fig1	3																		T		0.48												158928fig2		nm		26.1			nm		71.2									158928fig3																																										Fe, Te, Se	10	The powders of Fe, Te, and Se are doubly sealed in the fused quartz tube.				Gradient freezing method.	Unconventional superconductivity in the nickel chalcogenide superconductor TlNi2Se2	4	TlNi2Se2, two-gap superconductor, node	School of Physics and Astronomy, University of Birmingham, Birmingham B15 4TT, United Kingdom	Phys. Rev. B101 (2020)134523	E. Jellyman,P. Jefferies,S. Pollard,E. M. Forgan,E. Blackburn,E. Campillo,A. T. Holmes,R. Cubit,J. Gavilano,H. Wang,J. Du,M. Fang		
158929	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaNi2As2	Ba1Ni2As2	Ba	1	Ni	2	As	2																		3	2016																											2	ThCr2Si2-type	I4/mmm		nm			1.303	1										structual transition x<0.10									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158930	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.97Ni0.03As2	Ba1Fe1.97Ni0.03As2	Ba	1	Fe	1.97	Ni	0.03	As	2																3	2016																											2		I4/mmm						1										structual transition x<0.11									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158931	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.935Ni0.065As2	Ba1Fe1.935Ni0.065As2	Ba	1	Fe	1.935	Ni	0.065	As	2																3	2016																											2		I4/mmm						1										structual transition x<0.12	K							7.8	158929fig1	5																																																																																												Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158932	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.915Ni0.085As2	Ba1Fe1.915Ni0.085As2	Ba	1	Fe	1.915	Ni	0.085	As	2																3	2016																											2		I4/mmm						1										structual transition x<0.13	K							16.9	158929fig1	5																																																																																												Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158933	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.87Ni0.13As2	Ba1Fe1.87Ni0.13As2	Ba	1	Fe	1.87	Ni	0.13	As	2																3	2016																											2		I4/mmm						1										nematic transition above x > 0.10									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158934	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe185Ni0.15As2	Ba1Fe1.85Ni0.15As2	Ba	1	Fe	1.85	Ni	0.15	As	2																3	2016																											2		I4/mmm						1										nematic transition above x > 0.11	K							14.1	158929fig1	5																																																																																												Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158935	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.84Ni0.16As2	Ba1Fe1.84Ni0.16As2	Ba	1	Fe	1.84	Ni	0.16	As	2																3	2016																											2		I4/mmm						1										nematic transition above x > 0.12									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158936	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.82Ni0.18As2	Ba1Fe1.82Ni0.18As2	Ba	1	Fe	1.82	Ni	0.18	As	2																3	2016																											2		I4/mmm						1										nematic transition above x > 0.13	K							8.7	158929fig1	5																																																																																												Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158937	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.75Ni0.25As2	Ba1Fe1.75Ni0.25As2	Ba	1	Fe	1.75	Ni	0.25	As	2																3	2016																											2		I4/mmm		nm			1.297	1										nematic transition above x > 0.14									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158938	PRL117157002	The nematic fluctuations are systematically studied by the uniaxis pressure-dependent resistivity in the electron-doped iron-based superconductor BaFe2-xNixAs2.	BaFe1.70Ni0.30As2	Ba1Fe1.7Ni0.3As2	Ba	1	Fe	1.7	Ni	0.3	As	2																3	2016																																													nematic transition above x > 0.15									158929fig1																																																																																													Ba, Fe, As	5	Extra Fe-As is used as a flux				The mixture in an aulminium oxide cruicible is sealed in an evacuated quartz tube.	Nematic quantum critical fluctuations in BaFe2-xNixAs2	10	BaFe2-xNixAs2, nematic phase, quantum critical fluctuations	Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Science, Beijing 100190, China	Phys. Rev.Lett. 117 (2016)157002	Zh. Liu,Y. Gu,W. Zhang,D. Gong,W. Zhang,T. Xie,X. Lu,X. Ma,X. Zhang,R. Zhang,J. Zhu,C. Ren,L. Shan,X. Qiu,P. Dai,Y-F. Yang,H. Luo,S. Li		
158939	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir3O	Nb5Ir3O1	Nb	5	Ir	3																	O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7808		0.5091	1										158939fig1	K							10.84	158939fig2	2																																																		158939Tab1																			microohm							271													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158940	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir2.4Pt0.6O	Nb5Ir2.4Pt0.6O1	Nb	5	Ir	2.4	Pt	0.6															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7879		0.5081	1										158939fig1	K							10.27	158939fig2	2																																																		158939Tab1			37																microohm							186													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158941	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir2.2Pt0.8O	Nb5Ir2.2Pt0.8O1	Nb	5	Ir	2.2	Pt	0.8															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.78906		0.50785	1										158939fig1	K							10.44	158939fig2	2																																																		158939Tab1																																										Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158942	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir2.0Pt1.0O	Nb5Ir2Pt1O1	Nb	5	Ir	2	Pt	1															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7891		0.50734	1										158939fig1	K							9.01	158939fig2	2																																																		158939Tab1																																										Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158943	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir1.4Pt1.6O	Nb5Ir1.4Pt1.6O1	Nb	5	Ir	1.4	Pt	1.6															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7915		0.5065	1										158939fig1	K							8.56	158939fig2	2																																																		158939Tab1																			microohm							162													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158944	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir1.2Pt1.8O	Nb5Ir1.2Pt1.8O1	Nb	5	Ir	1.2	Pt	1.8															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7922		0.50618	1										158939fig1	K							7.98	158944fig1	2																																																		158939Tab1																																										Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158945	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir1.0Pt2.0O	Nb5Ir1Pt2O1	Nb	5	Ir	1	Pt	2															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7926		0.50935	1										158939fig1	K							7.41	158944fig1	2																																																		158939Tab1																																										Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158946	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir0.8Pt2.2O	Nb5Ir0.8Pt2.2O1	Nb	5	Ir	0.8	Pt	2.2															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7933		0.5053	1										158939fig1	K							6.69	158944fig1	2																																																		158939Tab1																			micro-ohm							337													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158947	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir0.4Pt2.6O	Nb5Ir0.4Pt2.6O1	Nb	5	Ir	0.4	Pt	2.6															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7945		0.50441	1										158939fig1	K							6.42	158944fig1	2																																																		158939Tab1																			micro-ohm							150													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158948	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Ir0.2Pt2.8O	Nb5Ir0.2Pt2.8O1	Nb	5	Ir	0.2	Pt	2.8															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7953		0.503884	1										158939fig1	K							4.89	158944fig1	2																																																		158939Tab1																																										Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158949	JPS30011055	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.	Nb5Pt3O	Nb5Ir0Pt3O1	Nb	5	Ir	0	Pt	3															O	1		3	2020																											2	Ti5Ga5-type	P4/mmm		nm	0.7958		0.5034	1										158939fig1	K							5.03	158944fig1	2																																																		158939Tab1																			micro-ohm							503													158939fig3			Nb, Ir, Pt	1	Nb5Ir3-xO was initially prepared by arc-melting, and Pt wires are added to the Nb5Ir3-xO pellet to form stoichiometric composition.					Superconductivity in Nb5Ir3-xPtxO	3	Nb5Ir3-xPtxO, superconductivity, Mathias rule	Department og Electrical Engineering, Faculty of Engineering, Fukuoka Institute of Technology, 3-30-1 Wajiro-higashi, Higashi-ku, Fukuoka 811-0295, Japan	Jap. J. Phys. Soc. 30(2020)011055	J. Kitagawa,S. Hamamoto	Nb5Pt3O	The lattice parameters show a linear x-dependence in Nb5Ir3-xPtxO, but Tc shows nonlinear x-dependency.
158950	PRB101134503	Bulk superconductivity was induced at point contacts on t-TaAs in this topological semimetal.	TaAs	Ta1As1	Ta	1	As	1																				4	2020																											7	NbAS-type	I41md																	K							3	158950fig1	5																		T		4.2					2.5	1.8						158950fig2																																																																			Two superconducting phase induced at point contacts on the Weyl semimetal TaAs	4	TaAs, Weyl semimetal, point contact	Key Laboratory of Structure and Functional Regulation of Hybrid Materials of Ministry of Education, Institute of Physical Science and Information Technology, Anhui University, Hefei 230601, China	Phys. Rev. B 101(2020)134503	X-Y. Hou,Ya-D. Gu,Shu-J. Li,L-X. Zhao,W-L. Zhu,Z. Wang,M-D. Zhang,F. Zhang,L. Zhang,H. Zi,Y-W. Wu,H-X. Yang,Z-A. Ren,P. Zhang,G-F. Chen,N. Hao,L. Shan	TaAs	Bulk superconductivity was induced at point contacts on h-TaAs of the topological semimetal.
158951	PRB101134503	Bulk superconductivity was induced at point contacts on h-TaAs in this topological semimetal.	TaAs	Ta1As1	Ta	1	As	1																				4	2020																											7	WC-type	P6m2 I41md																								7.3	158950fig2	5																		T		1.1					1	1.8						158950fig2																																																																			Two superconducting phase induced at point contacts on the Weyl semimetal TaAs	4	TaAs, Weyl semimetal, point contact	Key Laboratory of Structure and Functional Regulation of Hybrid Materials of Ministry of Education, Institute of Physical Science and Information Technology, Anhui University, Hefei 230601, China	Phys. Rev. B 101(2020)134503	X-Y. Hou,Ya-D. Gu,Shu-J. Li,L-X. Zhao,W-L. Zhu,Z. Wang,M-D. Zhang,F. Zhang,L. Zhang,H. Zi,Y-W. Wu,H-X. Yang,Z-A. Ren,P. Zhang,G-F. Chen,N. Hao,L. Shan	TaAs	Bulk superconductivity was induced at point contacts on h-TaAs of the topological semimetal.
158952	NAM01401135	Large-area high-quality 2D ultrathin Mo2C superconducting crystals	Mo2C	Mo2C1	Mo	2	C	1																				3	2015																											1	orthrhombic			A	4.77	5.98	5.21	1										alpha-Mo2C	K	2.76		3.3				3.03	158952fig1	3																		T						8.35	0.327	1.8						158952fig2			resistivity			22																															ohm								4.85		10											cm-2	48000000000000000	Mo, C	18	With methane as the carbon source on a Cu foil sitting ona Mo foil as the substrate at temperature above 1085C	18	Mo foil			Large-area high-quality 2D ultrathin Mo2C superconducting crystals	8	2D superconductor, Mo2C, ultrathin crystal			Ch. Xu,L. Wang,Zh. Liu,L. Chen,J. Guo,N. Kang,X-L. Ma,H-M. Cheng,W. Ren	Mo2C	High-quality 2D ultrathin Mo2C crystals have been successfully grown by CVD with a few nanometer thick and over 100 micrmeter.
158953	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe	Fe1Se1	Fe	1	Se	1																				3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158954	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.95S0.05	Fe1Se0.95S0.05	Fe	1	Se	0.95	S	0.05																		3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158955	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.9S0.10	Fe1Se0.9S0.1	Fe	1	Se	0.9	S	0.1																		3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158956	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.87S0.13	Fe1Se0.87S0.13	Fe	1	Se	0.87	S	0.13																		3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158957	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.84S0.16	Fe1Se0.84S0.16	Fe	1	Se	0.84	S	0.16																		3	2019																											2	tetragonal																		K			8.2				8.2	158953fig2	3																																158953fig3																																																									158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158958	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.82S0.18	Fe1Se0.82S0.18	Fe	1	Se	0.82	S	0.18																		3	2019																											2	tetragonal																		K	7.4	8.1	8.3				8.1	158953fig1	3																																																																																									158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158959	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.80S0.20	Fe1Se0.8S0.2	Fe	1	Se	0.8	S	0.2																		3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158960	PRR001023011	The coexistence of two independent charge sectors in a quantum critical system of nonmagnetic FeSe1-xSx.	FeSe0.75S0.25	Fe1Se0.75S0.25	Fe	1	Se	0.75	S	0.25																		3	2019																											2	tetragonal																																																																																																																				158953fig4			Fe, Se,S	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Coexixtence of orbital and quantum critical magnetoresistance in FeSe1-xSx	9	FeSeS, quantum critical point, nematicity, magnetiresistance	High Field Magnetic Laboratory(HFML-EMFL) and Institute for Molecules and Materials, Radboud University, Toernooiveld 7, 6525 ED Nijmegen, The Neatherlands	Phys. Rev. Research, 1(2019)023011	S. Licciardello,N. Maksimovic,J. Ayres,J. Buhot,M. Culo,B. Bryant,S. Kasahara,Y. Matsuda,T. Shibauchi,V. Nagarajan,J. G. Analytis,N. E. Hussey	FeSe0.80S0.25	The coexistence of two independent charge sectors in a quantum critical system.
158961	PRR002013211	Determination of the electromechanical limits of high-performance Nb3Sn Rutherford cables under transverse stress(up to 210MPa) from a single-wire experiments with variuous impregnants.	Nb3Sn	Nb3Sn1	Nb	3	Sn	1																				1	2020																																																																									T	resistivity				4.2		24.9																							337		158961fig1																																										Nb, Sn	1	PIT(Powder-In-Tube) method.					Determination of the electromechanical limits of high-performance Nb3Sn Rutherford cables under transverse stress from a single-wire experiments with variuous impregnants.	2	Nb3Sn, Rutherford cable, stress, single-wire	Dep. Of Quantum Matter Physics, University of Geneva, 1211 Geneva, Switzerland	Phys. Rev. Research, 2(2020)013211	L. Gaemperle,J. Ferradas,C. Barth,B. Bordini,D. Tommasini,C. Senatore	Nb3Sn	
158962	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe	Fe1Se1	Fe	1	Se	1																				3	2016					K		30.9																				2	tetragonal																		K							8.7	158962fig1	3																																158962fig7																																																									158962fig2			Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158963	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.96S0.04	Fe1Se0.96S0.04	Fe	1	Se	0.96	S	0.04																		3	2016																											2	tetragonal																		K							9.6	158962fig1	3																																158962fig7																																																												Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158964	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.92S0.08	Fe1Se0.92S0.08	Fe	1	Se	0.92	S	0.08																		3	2016					K		20.6																				2	tetragonal																		K							10.3	158962fig1	3																																158962fig7																																																									158962fig3			Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158965	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.88S0.12	Fe1Se0.88S0.12	Fe	1	Se	0.88	S	0.12																		3	2016					K		14.7																				2	tetragonal																		K							9.4	158962fig1	3																																158962fig7																																																												Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158966	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.85S0.15	Fe1Se0.85S0.15	Fe	1	Se	0.85	S	0.15																		3	2016																											2	tetragonal																		K							7.5	158962fig1	3																																158962fig7																																																									158962fig4			Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158967	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.83S0.17	Fe1Se0.83S0.17	Fe	1	Se	0.83	S	0.17																		3	2016					K		0																				2	tetragonal																		K							7.2	158962fig1	3																																158962fig7																																																									158962fig5			Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158968	PNA113008139	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.	FeSe0.79S0.21	Fe1Se0.79S0.21	Fe	1	Se	0.79	S	0.21																		3	2016					K		-31.2																				2	tetragonal																		K							5.6	158962fig1	3																																158962fig7																																																									158962fig6			Fe, Se	20	A mixture of Fe, Se, and S powders with KCL and AlCl3 sealed in an evacuated quartz tube was put in the furnace with temperature gradieant at 140-200C one end and 390-450C the others.					Nematic quantum critical point without magnetism in FeSe1-xSx superconductors	5	FeSeS, quantum critical point, nematicity	Dep. Of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan	Proc. Natl. Acad. Sci. USA 113(2016)8139	S. Hosoi,K. Matsuura,K. Ishida,H. Wang,Y. Mizukami,T. Watashige,S. Kasahara,Y. Matsuda,T. Shibauchi	FeSe1-xSx	Nematic fluctuations are divergently enhanced at the nematic QCP in FeSe1-xSx superconductors without accompanying other orders.
158969	PRR002013311	Measuring upper critical fields on LaAlO3/SrTiO3 with applying a gate voltage to the interface, Elliot-Yafet type spin relaxation is suggested dominantly to the spin-orbit scattering lifetime.	LaAlO3/SrTiO3	La1Al1O3	La	1	Al	1																	O	3		5	2020																											2	tetragonal																									0.36	158969fig1	3																		T	resistivity	1.32	1.32			0.74	0.09	0.72								nm	GL theory		90																																														cm2/Vs				10	2.5	158969fig3	cm-2	19000000000000	La, Al, O3	21	During the LAO layer-by-layer film growth, a highly concentrated ozone was supplied at a pressure of 1x10-6 torr at 800C on Atomically-flat TiO2-terminated (100)SrTiO3 substrates.		SrTiO3		Films were prepared by an oxige molecular beam epitaxy on atomically flat TiO2-terminated (100) SrTiO3.	Determination of spi-orbit scattering lifetime at the interface of LaAlO3/SrTiO3 from the superconducting upper critical fields	3	LaAlO3, spin-orbit coupling, gates device	Institute of Physics, Academia Sinica, Nankang, Teipei 11529, Taiwan	Phys. Rev. Research, 2(2020)013311	A. Kr. Singh,T-C. Wu,M-Y. Song,M-C. Chen,C-S. Li,S.-K. Yip,W-L. Lee	LaAlO3/SrTiO3	Measuring upper critical fields on LaAlO3/SrTiO3 with applying a gate voltageto the interface, Elliot-Yafet type spin relaxation is suggested dominantly to the spin-orbit scattering lifetime.
158970	PRR002013311	Measuring upper critical fields on LaAlO3/SrTiO3 with applying a gate voltage to the interface, Elliot-Yafet type spin relaxation is suggested dominantly to the spin-orbit scattering lifetime.	LaAlO3/SrTiO3	La1Al1O3	La	1	Al	1																	O	3		5	2020																											2	tetragonal																	Ts=90K(PM Tetragonal to PM Orthorhombic transition)	K							0.296	158970fig1	3																		T	resistivity		0.4	2.5										158970fig2		nm	GL theory		90																																														cm2/Vs				200	0.4	158970fig3	cm-2	23000000000000	La, Al, O3	21	During the LAO layer-by-layer film growth, a highly concentrated ozone was supplied at a pressure of 1x10-6 torr at 800C on Atomically-flat TiO2-terminated (100)SrTiO3 substrates.		SrTiO3		Films were prepared by an oxige molecular beam epitaxy on atomically flat TiO2-terminated (100) SrTiO3.	Determination of spi-orbit scattering lifetime at the interface of LaAlO3/SrTiO3 from the superconducting upper critical fields	3	LaAlO3, spin-orbit coupling, gates device	Institute of Physics, Academia Sinica, Nankang, Teipei 11529, Taiwan	Phys. Rev. Research, 2(2020)013311	A. Kr. Singh,T-C. Wu,M-Y. Song,M-C. Chen,C-S. Li,S.-K. Yip,W-L. Lee	LaAlO3/SrTiO3	Measuring upper critical fields on LaAlO3/SrTiO3 with applying a gate voltageto the interface, Elliot-Yafet type spin relaxation is suggested dominantly to the spin-orbit scattering lifetime.
158971	SCI373001122	Electronic nematicity shows peculiar sinusoidal waves in real-space with wavelength more than 1000 times as long as unit cell.	FeSe	Fe1Se1	Fe	1	Se	1																				9	2021																											2	tetragonal																	Ts,n=93K(PM Tetragonal to AFM Orthorhombic transition)								9		3																																158971fig2																																																									158971fig1				20	Fe and Se powders were sealed in an evacuated SiO2 ampoule together with KCl and AlCl3 powders.				The ampoule was heated to 390C on one end while the other end was kept at 240C for 28.5 days.	Discovery of mesoscopic nematicity wave in iron-based superconductivity	9	iron-base superconductors, mesoscopic, nematicity	RIKEN Center for Emergent Matter Science(CEMS), Wako 351-0199, Japan	Science373(2021)1123	T. Shimojima,Y. Motoyui,T. Taniuchi,C. Bareille,S. Onari,H. Kontani,M. Nakajima,S. Kasahara,T. Shibauchi,Y. Matsuda,S. Shin	BaFe2(As0.87P0.13)2	Electronic nematicity shows peculiar sinusoidal waves in real-space with wavelength more than 1000 times as long as the unit cell.
158972	SCI373001122	Electronic nematicity shows peculiar sinusoidal waves in real-space with wavelength more than 1000 times as long as unit cell.	BaFe2(As0.87P0.13)2	Ba1Fe2As1.74P0.26	Ba	1	Fe	2	As	1.74	P	0.26																9	2021																											2	tetragonal																											3																																158972fig2																																																									158972fig1				5	Ba2As3, Ba2P3, FeAs, and FeP were adopted as a atarting materials.				The quartz tube with the compositional materials was heated at 1150C for 10 h, and slowly colled to 900Cat a rate of 1C/h.	Discovery of mesoscopic nematicity wave in iron-based superconductivity	9	iron-base superconductors, mesoscopic, nematicity	RIKEN Center for Emergent Matter Science(CEMS), Wako 351-0199, Japan	Science373(2021)1123	T. Shimojima,Y. Motoyui,T. Taniuchi,C. Bareille,S. Onari,H. Kontani,M. Nakajima,S. Kasahara,T. Shibauchi,Y. Matsuda,S. Shin	BaFe2(As0.87P0.13)2	Electronic nematicity shows peculiar sinusoidal waves in real-space with wavelength more than 1000 times as long as the unit cell.
158973	PRR002012064	Unifying the origins of the upper critical field with the orbital and the paramagnetic effect, comprehensive understanding of Hc2 has been proposed on 2D NbSe2.	NbSe2	Nb1Se2	Nb	1	Se	2																				3	2020																																														K							6.2	158973fig1	3																		T						30		2						158973fig2		nm		7.85														158973fig3																																											5	Ba2As3, Ba2P3, FeAs, and FeP were adopted as a atarting materials.				The quartz tube with the compositional materials was heated at 1150C for 10 h, and slowly colled to 900Cat a rate of 1C/h.	Angle dependence of Hc2 with crossover between the orbital and paramagnetic limits	3	iron-base superconductors, high-magnetic field, nematicity	Department of Applied Physics, The University of Tokyo, Tokyo 113-8657, Japan	Physical Review Research2(2020)012065	H. Matsuoka,M. Nakano,T. Shitaokoshi,T. Ouchi,Y. Wang,Y. Kashiwabara,S. Yoshida,K. Ishizaka,M. Kawasaki,Y. Kohama,T. Nojima,Y. Iwasa	NbSe2	Unifying the origins of the upper critical field with the orbital and the paramagnetic effect, comprehensive understanding of Hc2 has been proposed on 2D NbSe2
158974	PRR002013309	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.	FeSe	Fe1Se1S0	Fe	1	Se	1	S	0																		3	2020																																														K							9.01	158974fig1	3																																158974fig3																																																			m3C-1(20K)	-0.000000025				1	158974fig2			Nb, Se	21	molecular-beam epitaxy with observing RHEED for getting a layer-by-layer growth of NbSe2.		Al2O3	Nb, Se	Atomically flat surface of Al2O3 was obtained by annealing the substrate.	Anomalous high-magnetic field electronic state of the nematic superconductors FeSe1-xSx	3	iron-base superconductors, high-magnetic field, nematicity	Clarendon Laboratory, Department of Physics, University of Oxford, Parks aroad, Oxford OX1 3PU, United Kingdom	Physical Review Research2(2020)013309	M. Bristow,P. Reiss,A.A. Haghighirad,Z. Zajicek,S.J. Singh,T. Wolf,D. Graf,W. Knafo,A. McCollam,A.I. Coldea	FeSe0.75S0.25	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.
158975	PRR002013309	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.	FeSe0.93S0.07	Fe1Se0.93S0.07	Fe	1	Se	0.93	S	0.07																		3	2020																																														K							10.42	158975fig1	3																																																																																			m3C-1(20K)	-0.000000002				1	158974fig2			Fe, Se							Anomalous high-magnetic field electronic state of the nematic superconductors FeSe1-xSx	3	iron-base superconductors, high-magnetic field, nematicity	Clarendon Laboratory, Department of Physics, University of Oxford, Parks aroad, Oxford OX1 3PU, United Kingdom	Physical Review Research2(2020)013309	M. Bristow,P. Reiss,A.A. Haghighirad,Z. Zajicek,S.J. Singh,T. Wolf,D. Graf,W. Knafo,A. McCollam,A.I. Coldea	FeSe0.75S0.25	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.
158976	PRR002013309	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.	FeSe0.89S0.11	Fe1Se0.89S0.11	Fe	1	Se	0.89	S	0.11																		3	2020																																														K							10.64	158976fig1	3																																																																																			m3C-1(20K)	0.000000007				1	158974fig2			Fe, Se, S							Anomalous high-magnetic field electronic state of the nematic superconductors FeSe1-xSx	3	iron-base superconductors, high-magnetic field, nematicity	Clarendon Laboratory, Department of Physics, University of Oxford, Parks aroad, Oxford OX1 3PU, United Kingdom	Physical Review Research2(2020)013309	M. Bristow,P. Reiss,A.A. Haghighirad,Z. Zajicek,S.J. Singh,T. Wolf,D. Graf,W. Knafo,A. McCollam,A.I. Coldea	FeSe0.75S0.25	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.
158977	PRR002013309	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.	FeSe0.83S0.17	Fe1Se0.83S0.17	Fe	1	Se	0.83	S	0.17																		3	2020																																														K							10.33	158977fig1	3																																																																																			m3C-1(20K)	0.000000011				1	158974fig2			Fe, Se, S							Anomalous high-magnetic field electronic state of the nematic superconductors FeSe1-xSx	3	iron-base superconductors, high-magnetic field, nematicity	Clarendon Laboratory, Department of Physics, University of Oxford, Parks aroad, Oxford OX1 3PU, United Kingdom	Physical Review Research2(2020)013309	M. Bristow,P. Reiss,A.A. Haghighirad,Z. Zajicek,S.J. Singh,T. Wolf,D. Graf,W. Knafo,A. McCollam,A.I. Coldea	FeSe0.75S0.25	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.
158978	PRR002013309	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.	FeSe0.75S0.25	Fe1Se0.75S0.25	Fe	1	Se	0.75	S	0.25																		3	2020																																														K							6.09	158978fig1	3																																																																																			m3C-1(20K)	0				1	158974fig2			Fe, Se, S							Anomalous high-magnetic field electronic state of the nematic superconductors FeSe1-xSx	3	iron-base superconductors, high-magnetic field, nematicity	Clarendon Laboratory, Department of Physics, University of Oxford, Parks aroad, Oxford OX1 3PU, United Kingdom	Physical Review Research2(2020)013309	M. Bristow,P. Reiss,A.A. Haghighirad,Z. Zajicek,S.J. Singh,T. Wolf,D. Graf,W. Knafo,A. McCollam,A.I. Coldea	FeSe0.75S0.25	Anomalous transport inside the nematic phase has been observed, influenced by both changes in the electronic structure and the scattering with the lattice and spin fluctuations.
158979	RRR002013329	A novel vortex distribution in betha-Bi2Pd has been observed with SOT and MFM, influenced by the defects.	betha-Bi2Pd	Bi2Pd1	Bi	2	Pd	1																				3	2020																											2	tetragonal	I4/mmm		nm	0.336	0.336	1.297	1											K						0.03	5											gauss		225							gauss		6000												158979fig1		nm		23.5			nm		132									158979fig2																																										Bi, Pd	9	High-purity Bi and Pd in quartz ampoule with 140mbar of He was heated at 900C, cooled down to 490C, and to 395C, and was quenched by immersion in cold water.				To avoid the formation of alpha-Bi2Pd, the sibgle crystals were quenched from 395C(15C higher than the temperature of alpha-Bi2Pd) to room temperature/	Observation of a gel of quantum vortices in a superconductor at very low magnetic fields	3	Bi2Pd, vortex	Laboratorio de Bajas Temperaturas y Altos Campos Magneticos, Departamento de Fisico de la Materia Condensada, Instituto Nicolas Cabrera and Condensed Matter Physics Center (IFIMAC), Universidad Autonoma de Madrid, E-28049 Madrid, Spain	Physical Review Research2(2020)013310	J. B. Llorens,L. Embon,A. Correa,J. D. Gonzalez,E. Herrera,I. Guillamon,R. F. Luccas,J. Azpeitia,F. J. Mompean,M. Garcia-Hernandez,C. Munuera,J. A. Sanchez,Y. Fasano,M. V. Milosevic,H. Suderow,Y. Anahory	Bi2Pd	A novel vortex distribution in betha-Bi2Pd has been observed with SOT and MFM, influenced by the defects..
158980	PRB092054507	betha-Bi2Pd is a single-gap multiband superconductor, measured by STM.	betha-Bi2Pd	Bi2Pd1	Bi	2	Pd	1																				3	2015																											2	tetragonal	I4/mmm		nm	0.336	0.336	1.297	1											K						0.03	5.07																																		158980fig3		nm		23								meV	0.75		1			158980fig1				mJ/K2mol	13														microohmcm								18												158980fig2			Bi, Pd	9	High-purity Bi and Pd in quartz ampoule with 140mbar of He was heated at 900C, cooled down to 490C, and to 395C, and was quenched by immersion in cold water.				To avoid the formation of alpha-Bi2Pd, the sibgle crystals were quenched from 395C(15C higher than the temperature of alpha-Bi2Pd) to room temperature/	Magnetic field dependence of the density of states in the multiband superconductor betha-Bi2Pd	8	Bi2Pd, vortex, STM, multiband, single gap	Laboratorio de Bajas Temperaturas y Altos Campos Magneticos, Departamento de Fisico de la Materia Condensada, Instituto Nicolas Cabrera and Condensed Matter Physics Center (IFIMAC), Universidad Autonoma de Madrid, E-28049 Madrid, Spain	Physical Review B, 92(2015)054507	E. Herrera,I. Guillamon,J. A. Galvis,A. Correa,A. Fente,R. F. Luccas,F. J. Mompean,M. Garcia-Hernandez,S. Viera,J.P. Brison,H. Suderow	Bi2Pd	betha-Bi2Pd is a single-gap multiband superconductor, measured by STM.
158981	PRB102165125	Superconductivity in La2Ni2O shows a dirty type-II superconductor with likely s-wave gap symmetry.	La2Ni2In	La2Ni2In1	La	2	Ni	2	In	1																		3	2020																											2	tetragonal	P4/mbm		nm	0.76448		0.389149												K							0.89	158981fig1	1									Oe		11.2							Oe		1918												158981fig4		nm		34.4			nm		250									158981fig2	158981fig3			mJ/K2mol	13.01		226																																			La, Ni, O	5	Single crystals of La2Ni2In were sythsized using a LaNi self-flux.				LaNi, sealed under ~250mBar argon atomosphere in a quartz tube. The precursor of powdered LaNi with In in a ratio of 6:1set on Al2O3 crucible were heated in open furnace to 770C and down to 725C.	Superconductivity in La2Ni2In	10	La2Ni2In, specific heat, superconductivity	Quntum Matter Institute, University of British Columbia, Vancouver, BC, Canada V6T IZ1	Physical Review B, 102(2020)165125	J. Maiwald,I. I. Mazin,A. Gulvich,M. Aronson	La2Ni2In	Superconductivity in La2Ni2O shows a dirty type-II superconductor with likely s-wave gap symmetry.
158982	PRB087180505	Superconductivity does not reduce the orthorhombicity below Tc, instead superconductivity couples strongly to the in-plane area.	FeSe	Fe1Se1	Fe	1	Se	1																				3	2013																											2	tetragonal	I4/mmm	158982fig3	nm	0.37707		0.5521												K				7.75			7.75	158982fig1	1																																158982fig2																															158982fig4																													Fe, Se	20	vapor-grown single crystal with temperature difference 390C at one end and 240C at the other end for 28.5 days..				Stoichiometric Fe and Se powders are mixed and sealed in an evacuated SiO2 ampoule together with a eutectic mixture of KCl and AlCl3.	Lack of coupling between superconductivity and orthorhombic distortion in stoichiometric single-crystalline FeSe		FeSe, superconductivity, distortion	Institute fuer Physik, Karlsruhe Institute of Technology, 76021 Karlsruhe, Germany	Physical Review B, 87(2013)180505	A.E. Boehmer,F. Hardy,F. Eilers,D. Ernst,P. Adelmann,P. Schweiss,T. Wolf,C. Meingast	FeSe	Superconductivity does not reduce the orthorhombicity below Tc, instead superconductivity couples strongly to the in-plane area.
158983	PRB102184502	By ARPES measurements on LiFeAs, a spontaneous breaking of rotational symmetry in the gap amplitude on all Fermi surfaces, as well as unidirectional distortion of the Fermi pockets.	LiFeAS	Li1Fe1As1	Li	1	Fe	1	As	1																			2020																											2	tetragonal	C4/mmm																	K				18			18																																														meV	3.57		9			158983fig1																																										Li, Fe, As	5	All preparation steps were made in an argon box.				Li/Fe/As = 3:2:3 molar ratio for the raw materials.	Nematic superconductivity in LiFeAs	11	LiFeAs, nematicity, ARPES, superconductivity	IFW Dresden, Helmholtzstrasse 20, 01069 Dresden, Germany	Physical Review B, 102(2020)184502	Y.S. Kushnirenko,D.V. Evetushinsky,T.K. Kim,I. Morovov,L. Harnagea,S. Wurmehl,S. Aswartham,B. Buechner,A.V. Chubukov,S.V. Borisenko	LiFeAs	By ARPES measurements on LiFeAs, a spontaneous breaking of rotational symmetry in the gap amplitude on all Fermi surfaces, as well as unidirectional distortion of the Fermi pockets.
158984	PNA117007645	Identification of superconducting phases in Mundrabilla, by MFMMS, VSM, and EDX.	Mundrabilla(a typical sample)	In74.72Sn15.36Pb8.75Si1.17	In	74.72	Sn	15.36	Pb	8.75	Si	1.17																4	2020																																			1										Iron IAB	K							6	158984fig1	13																																158984fig2																																																												In, Sn, Pb, Si		Extreme environments found in space(Field Museum of Chicago)				After MFMMS measurements, superconducting samples were separated and taken as MUND-1 and -2.	Superconductivity found in meteorites	4	meteorites, MFMMS, astronomy, superconductivity	Department of Physics, University of California San Diego, La Jolla, CA 92093, USA	Proceedings of the National Academy of Sciences	J. Wampler,M. Thiemens,S. Cheng,Y. Zhu,I.K. Schuller	GRA 95205	Identification of superconducting phases in Mundrabilla, by MFMMS, VSM, and EDX
158985	PNA117007645	Identification of superconducting phases in GRA 95205, by MFMMS, VSM, and EDX.	GRA 95205(a typical sample)	Mg1C1Na1Sn1Ca1Al1Si1Ni1In1Pb1	Mg	1	C	1	Na	1	Sn	1	Ca	1	Al	1	Si	1	Ni	1	In	1	Pb	1				4	2020																																			1										Ureilite	K							5.5	158985fig1	13																																																																																												In, Sn, Pb, Si		Extreme environments found in space(Field Museum of Chicago)				After MFMMS measurements, superconducting samples were separated and taken as MUND-1 and -2.	Superconductivity found in meteorites	4	meteorites, MFMMS, astronomy, superconductivity	Department of Physics, University of California San Diego, La Jolla, CA 92093, USA	Proceedings of the National Academy of Sciences	J. Wampler,M. Thiemens,S. Cheng,Y. Zhu,I.K. Schuller	GRA 95205	Identification of superconducting phases in Mundrabilla, by MFMMS, VSM, and EDX
158986	NAT586000373	Using a photochemically transformed carbonaceous sulfur hydride system, a maximum superconducting transition temperature of 287.7±1.2K was achieved at 267±10GPa.	C-S-H	C1S1	C	1	S	1																				4	2020																																														K							287.7	158986fig1	3																																158986fig2																		158986fig3																																							158986fig4			Mg, C, Na, Sn, Ca, Al, Si, Ni, In		Extreme environments found in space(Antarctic meteorite collection, curated at Johns Space Center)				After MFMMS measurements, superconducting samples were separated.	Room-temperature superconductivity in a carbonaceous sulfur hydride	10	room-temperature, high pressure, superconductivity, C-S-H	Department of Mechanical Engineering, School of Engineering and Applied Sciences, University of Rochester, Rochester, NY, USA	Nature, 586(2020)373	E. Snider,N. Dasenbrock-Gammon,R. McBride,M. Dedebessal,H. Vindana,K. Vencatasamy,K.V. Lawler,A. Salamat,R.P. Dias	C-S-H	Using a photochemically transformed carbonaceous sulfur hydride system, a maximum superconducting transition temperature of 287.7±1.2K was achieved at 267±10GPa.
158987	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2As2	Ba1Fe2As2	Ba	1	Fe	2	As	2																		3	2012																												tetragonal			nm			1.301	1										After antiferromagnetic transition at 142K, structure changes to orthrhombic.									158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158988	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.93P0.07)2	Ba1Fe2As0.14P1.86	Ba	1	Fe	2	As	0.14	P	1.86																3	2012																												tetragonal			nm			1.296	1										After antiferromagnetic transition, structure changes to orthrhombic.									158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158989	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.87P0.13)2	Ba1Fe2As0.26P1.74	Ba	1	Fe	2	As	0.26	P	1.74																3	2012																												tetragonal			nm			1.293	1										After antiferromagnetic transition at 100K, structure changes to orthrhombic.									158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158990	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.80P0.20)2	Ba1Fe2As0.4P1.6	Ba	1	Fe	2	As	0.4	P	1.6																3	2012																												tetragonal			nm			1.289	1										After antiferromagnetic transition at 77K, structure changes to orthrhombic.	K							9.1	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158991	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.76P0.24)2	Ba1Fe2As0.48P1.52	Ba	1	Fe	2	As	0.48	P	1.52																3	2012																												tetragonal			nm			1.286	1										After antiferromagnetic transition at 62K, structure changes to orthrhombic.	K							17.1	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158992	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.68P0.32)2	Ba1Fe2As0.64P1.36	Ba	1	Fe	2	As	0.64	P	1.36																3	2012																												tetragonal			nm			1.283	1											K							32	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158993	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.62P0.38)2	Ba1Fe2As0.76P1.24	Ba	1	Fe	2	As	0.76	P	1.24																3	2012																												tetragonal			nm			1.278	1											K							26.7	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158994	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.55P0.45)2	Ba1Fe2As0.9P1.1	Ba	1	Fe	2	As	0.9	P	1.1																3	2012																												tetragonal			nm			1.276	1											K							24.3	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158995	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.48P0.52)2	Ba1Fe2As1.04P0.96	Ba	1	Fe	2	As	1.04	P	0.96																3	2012																												tetragonal			nm			1.27	1											K							15.2	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158996	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.39P0.61)2	Ba1Fe2As1.22P0.78	Ba	1	Fe	2	As	1.22	P	0.78																3	2012																												tetragonal			nm			1.266	1											K							9.1	158987fig2	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158997	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.34P0.66)2	Ba1Fe2As1.32P0.68	Ba	1	Fe	2	As	1.32	P	0.68																3	2012																												tetragonal			nm			1.262	1																			158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158998	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.26P0.74)2	Ba1Fe2As1.48P0.52	Ba	1	Fe	2	As	1.48	P	0.52																3	2012																												tetragonal			nm			1.258	1																			158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
158999	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2(As0.13P0.87)2	Ba1Fe2As1.74P0.26	Ba	1	Fe	2	As	1.74	P	0.26																3	2012																												tetragonal			nm			1.251	1																			158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
159000	JPS081104710	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.	BaFe2P2	Ba1Fe2P2	Ba	1	Fe	2	P	2																		3	2012																												tetragonal			nm			1.244	1																			158987fig1	3																																158987fig3																																																												Ba, Fe, As	5	Prepared pieces of Ba2As3, Ba2P3, FeAs and FeP in molar ratio were placed in an alumina cruicible, and sealed in a quartz tube.				The tube was heated at 1150C(x≦0.15)　or 1200C(0.15＜x) for 10 hrs, followed by decanting the flux.	Growth of BaFe2(As1-xPx)2 single crystals (0 ≦ x ≦ 1) by Ba2As3/Ba2P3-flux method	9	iron-based superconductor, isovalent chemical substitution, BaFe2(As1-xPx)2, single crystal growth, transport properties, annealing effect	Department of Physics, University of Tokyo, Bunkyo, Tokyo 113-0033, Japan	Journal of the Physical Society of Japan, 81(2012)104710	M. Nakajima,S. Uchida,K. Kihou,Ch-H. Lee,A. Iyo,H. Eisaki	BaFe2P2	Single crystal of  BaFe2(As1-xPx)2 has been grown successfully by a Ba2As3/Ba2P3 self-flux.
159001	NAP0120139	Observation of the in-plane upper critical field is six times larger than Pauli paramegnetic limit in the monolayer NbSe2.	NbSe2	Nb1Se2	Nb	1	Se	2																				5	2016																												trigonal																		K							3	159001fig1	3																		T								0.3				31.5		159001fig2																																																												Nb, Se	5	Atomically-thin layers of the sample were fabricated by exfoliating mechanically 2H-NbSe2.				The layer thickness was measured by using Raman measurements.	Ising pairing in superconducting NbSe2 atomic layers	2	NbSe2, atomic layers, Ising pairing, superconductors	Department of Physics and Center for 2-dimensional and Layered Materials, The Pennsylvania State University, University Park, Pennsilvania 16802-6300, USA	Nature Physics, 12(2016)139	X. Xi,Z. Wang,W. Zhao,J-H. Park,K. T. Law,H. Berger,L. Forro,J. Shan,K. F. Mak	NbSe2	Observation of the in-plane upper critical field is six times larger than Pauli paramegnetic limit in the monolayer NbSe2.
159002	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	ZrPS	Zr1Pd1S1	Zr	1	Pd	1	S	1																		2	2020																												tetragonal			nm	0.3584		0.7674	3											K							3.64	159002fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159003	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.5Lu0.5PS	Zr0.5Lu0.5P1S1	Zr	0.5	Lu	0.5	P	1	S	1																2	2020																												tetragonal			nm	0.3575		0.7379	3											K							5.78	159002fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159004	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.6Lu0.4PS	Zr0.6Lu0.4P1S1	Zr	0.6	Lu	0.4	P	1	S	1																2	2020																												tetragonal			nm	0.3575		0.7446	3											K							6.41	159002fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159005	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.675Lu0.325PS	Zr0.675Lu0.325P1S1	Zr	0.675	Lu	0.325	P	1	S	1																2	2020																												tetragonal			nm	0.3578		0.7467	3											K							5.9	159002fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159006	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.75Lu0.25PS	Zr0.75Lu0.25P1S1	Zr	0.75	Lu	0.25	P	1	S	1																2	2020																												tetragonal			nm	0.3581		0.7592	3											K							5.81	159002fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159007	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.4Y0.6PS	Zr0.4Y0.6P1S1	Zr	0.4	Y	0.6	P	1	S	1																2	2020																												tetragonal			nm	0.3562		0.7181	3											K							5.35	159002fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159008	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.5Y0.5PS	Zr0.5Y0.5P1S1	Zr	0.5	Y	0.5	P	1	S	1																2	2020																												tetragonal			nm	0.3559		0.7184	3											K							5.34	159002fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159009	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.6Y0.4PS	Zr0.6Y0.4P1S1	Zr	0.6	Y	0.4	P	1	S	1																2	2020																												tetragonal			nm	0.3562		0.7385	3											K							4.88	159002fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159010	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Zr0.75Y0.25PS	Zr0.75Y0.25P1S1	Zr	0.75	Y	0.25	P	1	S	1																2	2020																												tetragonal			nm	0.3572		0.7382	3											K							4.97	159002fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159011	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	HfPS	Hf1P1.55S0.45	Hf	1	P	1.55	S	0.45																		2	2020																												tetragonal			nm	0.3603		0.7816	3											K							4.9	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159012	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Lu0.2P1.55S0.45	Hf0.8Lu0.2P1.55S0.45	Hf	0.8	Lu	0.2	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.3579		0.7816	3											K							4.81	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159013	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.7Lu0.3P1.55S0.45	Hf0.7Lu0.3P1.55S0.45	Hf	0.7	Lu	0.3	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.3575		0.7834	3											K							4.75	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159014	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.6Lu0.4P1.55S0.45	Hf0.6Lu0.4P1.55S0.45	Hf	0.6	Lu	0.4	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.3574		0.7881	3											K							5.91	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159015	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.5Lu0.5P1.55S0.45	Hf0.5Lu0.5P1.55S0.45	Hf	0.5	Lu	0.5	P	1.55	S	0.45																2	2020																												tetragonal			nm				3											K							5.68	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159016	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Y0.2P1.55S0.45	Hf0.8Y0.2P1.55S0.45	Hf	0.8	Y	0.2	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.357		0.7824	3											K							5.01	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159017	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.7Y0.3P1.55S0.45	Hf0.7Y0.3P1.55S0.45	Hf	0.7	Y	0.3	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.356		0.7829	3											K							4.52	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159018	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.6Y0.4P1.55S0.45	Hf0.6Y0.4P1.55S0.45	Hf	0.6	Y	0.4	P	1.55	S	0.45																2	2020																												tetragonal			nm	0.355		0.7827	3											K							4.81	159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159019	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.5Y0.5P1.55S0.45	Hf0.5Y0.5P1.55S0.45	Hf	0.5	Y	0.5	P	1.55	S	0.45																2	2020																												tetragonal			nm				3											K								159002fig3	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159020	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	ZrP1.25Se0.75	Zr1P1.25Se0.75	Zr	1	P	1.25	Se	0.75																		2	2019																												PbFCl-type			nm	3.65958		7.95654	3											K							5.907	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159021	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.85Sc0.15P1.25Se0.75	Zr1.85Sc0.15P1.25Se0.75	Zr	1.85	Sc	0.15	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm	3.65564		7.95052	3											K							7.333	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159022	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.75Sc0.25P1.25Se0.75	Zr1.75Sc0.25P1.25Se0.75	Zr	1.75	Sc	0.25	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm	3.65591		7.95366	3											K							7.574	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159023	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.70Sc0.30P1.25Se0.75	Zr1.7Sc0.3P1.25Se0.75	Zr	1.7	Sc	0.3	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm	3.65696		7.97042	3											K							7.352	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159024	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.60Sc0.40P1.25Se0.75	Zr1.6Sc0.4P1.25Se0.75	Zr	1.6	Sc	0.4	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm	3.64882		7.96021	3											K							7.315	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159025	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.30Sc0.70P1.25Se0.75	Zr1.3Sc0.7P1.25Se0.75	Zr	1.3	Sc	0.7	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm	3.65249		7.97042	3											K							3.444	159020fig1	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159026	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.85La0.15P1.25Se0.75	Zr1.85La0.15P1.25Se0.75	Zr	1.85	La	0.15	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							5.889	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159027	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.75La0.25P1.25Se0.75	Zr1.75La0.25P1.25Se0.75	Zr	1.75	La	0.25	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							5.185	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159028	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.60La0.40P1.25Se0.75	Zr1.6La0.4P1.25Se0.75	Zr	1.6	La	0.4	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							5.185	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159029	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.85Y0.15P1.25Se0.75	Zr1.85Y0.15P1.25Se0.75	Zr	1.85	Y	0.15	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							6.37	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159030	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.75Y0.25P1.25Se0.75	Zr1.75Y0.25P1.25Se0.75	Zr	1.75	Y	0.25	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							6.056	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159031	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.60Y0.40P1.25Se0.75	Zr1.6Y0.4P1.25Se0.75	Zr	1.6	Y	0.4	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							5.09	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159032	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.50Y0.50P1.25Se0.75	Zr1.5Y0.5P1.25Se0.75	Zr	1.5	Y	0.5	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							5.63	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159033	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.85Lu0.15P1.25Se0.75	Zr1.85Lu0.15P1.25Se0.75	Zr	1.85	Lu	0.15	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							6.278	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159034	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.75Lu0.25P1.25Se0.75	Zr1.75Lu0.25P1.25Se0.75	Zr	1.75	Lu	0.25	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							7.093	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159035	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.60Lu0.40P1.25Se0.75	Zr1.6Lu0.4P1.25Se0.75	Zr	1.6	Lu	0.4	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							7.241	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159036	JPC12930012003	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.	Zr1.50Lu0.50P1.25Se0.75	Zr1.5Lu0.5P1.25Se0.75	Zr	1.5	Lu	0.5	P	1.25	Se	0.75																2	2019																												PbFCl-type			nm				3											K							6.778	159020fig2	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors II	10	Zr(P,Se)2, superconductor, rare earth, substituition	Department of Physics, Tokyo University of Science, 1-3 Kagrazaka, Shinjuku-ku, Tokyo 162-8601, Japan	Journal of Physics:Conf. Series 1293(2019)012003	K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,I. Hase,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida,H. Kito	Zr1.50Lu0.50P1.25Se0.75	Effect of non-magnetic rare earth substitution for Zr on mixed anion Zr(P,Se)2 superconductors.
159037	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	HfPS	Hf1P1.45S0.55	Hf	1	P	1.45	S	0.55																			2020																												tetragonal			nm	0.3559		0.7715	3											K							3.13	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159038	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Lu0.2P1.45S0.55	Hf0.8Lu0.2P1.45S0.55	Hf	0.8	Lu	0.2	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3562		0.7769	3											K							4.09	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159039	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.7Lu0.3P1.45S0.55	Hf0.7Lu0.3P1.45S0.55	Hf	0.7	Lu	0.3	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3557		0.7772	3											K							4.85	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159040	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Lu0.4P1.45S0.55	Hf0.6Lu0.4P1.45S0.55	Hf	0.6	Lu	0.4	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3555		0.7794	3											K							4.48	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159041	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.7Lu0.5P1.45S0.55	Hf0.5Lu0.5P1.45S0.55	Hf	0.5	Lu	0.5	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3556		0.7802	3											K							5.87	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159042	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Lu0.6P1.45S0.55	Hf0.4Lu0.6P1.45S0.55	Hf	0.4	Lu	0.6	P	1.45	S	0.55																	2020																												tetragonal			nm				3											K							5	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159043	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.8Y0.2P1.55S0.45	Hf0.8Y0.2P1.45S0.55	Hf	0.8	Y	0.2	P	1.45	S	0.55																	2020																												tetragonal			nm	0.356		0.7519	3											K								159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159044	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.6Y0.3P1.55S0.45	Hf0.7Y0.3P1.45S0.55	Hf	0.7	Y	0.3	P	1.45	S	0.55																	2020																												tetragonal			nm	0.356		0.776	3											K							4.53	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159045	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.5Y0.4P1.55S0.45	Hf0.6Y0.4P1.45S0.55	Hf	0.6	Y	0.4	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3562		0.777	3											K							4.74	159002fig4	1																																																																																												Zr, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159046	JPC1590012007	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.	Hf0.5Y0.5P1.55S0.45	Hf0.5Y0.5P1.45S0.55	Hf	0.5	Y	0.5	P	1.45	S	0.55																	2020																												tetragonal			nm	0.3559		0.7799	3											K							4.42	159002fig4	1																																																																																												Zr, Lu, P, S	1	Polycrystalline samples were synthsized by using a cubic-anvil high pressure apparatus, heated at ~1425C~1651C under a pressure of ~2 Gpa for 1 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	Effect of non-magnetic rare earth substitution for A site in mixed anion APX superconductors	8	APX, superconductors, non-magnetic, rare earth, substitution	National Institute for Advanced Industrial Science and Technology (AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	Journal of Physics:Conf. Series 1590(2020)012007	H. Kito,K. Kawashima,S. Ishida,K. Oka,H. Fujishima,Y. Gotoh,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	Hf0.5Y0.5P1.45S0.55	Effect on superconducting transition temperature of non-magnetic rare earth atoms was studied to substitute A-atom into APX-based superconductors.
159047	JPC1054012003	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.	ZrP1.25Se0.75	Zr1P1.25Se0.75	Zr	1	P	1.25	Se	0.75																		3	2018																											2	PbFCl-type																		K				6.2			6.2	159047fig1	1																																159047fig2																																																												Zr,P,Se	1	Single crystal samples were synthsized by using a cubic-anvil apparatus at ~2050C under a pressure of ~4 Gpa for 3 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	single crystal growth of mixed anion Zr(P,Se)2 superconductor and related materials	7	Zr(P,Se)2, superconductor, single crystal	National Institute of Advanced Industrial Science and Technology(AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J. of Physics, Conf. Series 1054(2018)012003	H. Kito,K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujihisa,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	ZrP1.25Se0.75	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.
159048	JPC1054012003	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.	Zr0.5Y0.5PSe	Zr0.5Y0.5P1Se1	Zr	0.5	Y	0.5	P	1	Se	1																3	2018																											2	PbFCl-type																		K				6.66			6.66	159047fig1	1																																159047fig2																					37																																							Zr,P,Se	1	Single crystal samples were synthsized by using a cubic-anvil apparatus at ~2050C under a pressure of ~4 Gpa for 3 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	single crystal growth of mixed anion Zr(P,Se)2 superconductor and related materials	7	Zr(P,Se)2, superconductor, single crystal	National Institute of Advanced Industrial Science and Technology(AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J. of Physics, Conf. Series 1054(2018)012003	H. Kito,K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujihisa,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	ZrP1.25Se0.75	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.
159049	JPC1054012003	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.	Zr0.5Lu0.5PSe	Zr0.5Lu0.5P1Se1	Zr	0.5	Lu	0.5	P	1	Se	1																3	2018																											2	PbFCl-type																		K				6.91			6.91	159047fig1	1																																159047fig2																																					ohm							35.9																Zr,P,Se	1	Single crystal samples were synthsized by using a cubic-anvil apparatus at ~2050C under a pressure of ~4 Gpa for 3 hr to quench to room rapidly temperature.				The metal powders were mixed and pelletized in a nitrogen-filled glove box, were put into BN crucible.	single crystal growth of mixed anion Zr(P,Se)2 superconductor and related materials	7	Zr(P,Se)2, superconductor, single crystal	National Institute of Advanced Industrial Science and Technology(AIST), 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, Japan	J. of Physics, Conf. Series 1054(2018)012003	H. Kito,K. Iwakiri,T. Nishio,K. Kawashima,S. Ishida,K. Oka,H. Fujihisa,A. Iyo,H. Ogino,H. Eisaki,Y. Yoshida	ZrP1.25Se0.75	New method for growing single crystal of AP2-xXx (A=Zr, Hf, X=S,Se) with a wedge-tyoe cubis-anvil under a pressure of 2GPa.
159050	APM007121103	NaAlSi with a critical temperature of TC ~7K is found to be a nodal-line semimetal with s+s-wave symmetry full-gap, unprecedented topological quantum phases.	NaAlSi	Na1Al1Si1	Na	1	Al	1	Si	1																		3	2019																													P4/nmm																	K				7			7																																									micrometer	14	0.67			meV	1.39		14			159050fig1																																											22	The elements in a ratio of Na:Al:Si=3:1:1 were sealed in a argon-filled tantalum tube, and thean were sealed ina quartz tube at 700C for three days.				To increase the crystallinity, the samples were slowly cooled(5C/h) to 600C, held for three days at this temp., and cooled to r.t.(5C/h).	Superconducting order parameters of the nodal-line semimetal NaAlSi	12	NaAlSi, semimetal, nodal line	Center for Computational Quantum Physics, The Flation Institute, New York, New York 10010, USA	Applied Physics Letters Materials, 7(2019)121103	L. Muechler,Z. Cuguchia,J-Ch. Orain,J. Nuss,L.M. Scoop,R. Thomale,F.O. van Rohr	NaAlSi	NaAlSi with a critical temperature of TC ~7K is found to be a nodal-line semimetal with s+s-wave symmetry full-gap, unprecedented topological quantum phases.
159051	JPC969012027	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.	EuRbFe4As4	Eu1Rb1Fe4As4	Eu	1	Rb	1	Fe	4	As	4																1	2018																											2		P4/mmm		A	3.8898		13.307												K				36.78			36.78	159051fig1	1																																159051fig2																		159051fig3																																										Eu, Rb, Fe, As	22	Polycrystalline samples of Eu1-xCaxRbFe4As4 (x=0.0, 0.25, 0.50, 0.75, 1.0) was synthsized bya conventional sokid state reaction using stainless steel pipe capped with quartz tube.					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type structure	7	(Eu1-xCax)RbFe4As4, superconductor, magnetic order, single crystal	IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J. of Physics, Conf. Series 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y. Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo	EuRbFe4As4	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.
159052	JPC969012027	Ca substitution effect in Fe-based superconductor EuRbFe4As4; magnetic order was suppressed to 12.0K, but Tc is almost unchanged with substitution.	Eu0.75Ca0.25RbFe4As4	Eu0.75Ca0.25Rb1Fe4As4	Eu	0.75	Ca	0.25	Rb	1	Fe	4	As	4														1	2018																											2		P4/mmm		A	3.8874		13.28												K				36.5			36.5	159051fig1	1																																159051fig2																		159051fig3																																										Eu, Rb, Fe, As	22	Polycrystalline samples of Eu1-xCaxRbFe4As4 (x=0.0, 0.25, 0.50, 0.75, 1.0) was synthsized bya conventional sokid state reaction using stainless steel pipe capped with quartz tube.					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type structure	7	(Eu1-xCax)RbFe4As4, superconductor, magnetic order, single crystal	IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J. of Physics, Conf. Series 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y. Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo	EuRbFe4As4	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.
159053	JPC969012027	Ca substitution effect in Fe-based superconductor EuRbFe4As4; magnetic order was suppressed to 5K, but Tc is almost unchanged.	Eu0.50Ca0.50RbFe4As4	Eu0.5Ca0.5Rb1Fe4As4	Eu	0.5	Ca	0.5	Rb	1	Fe	4	As	4														1	2018																											2		P4/mmm		A	3.8847		13.2289												K				36.5			36.5	159051fig1	1																																159051fig2																		159051fig3																																										Eu, Rb, Fe, As	22	Polycrystalline samples of Eu1-xCaxRbFe4As4 (x=0.0, 0.25, 0.50, 0.75, 1.0) was synthsized bya conventional sokid state reaction using stainless steel pipe capped with quartz tube.					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type structure	7	(Eu1-xCax)RbFe4As4, superconductor, magnetic order, single crystal	IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J. of Physics, Conf. Series 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y. Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo	EuRbFe4As4	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.
159054	JPC969012027	Ca substitution effect in Fe-based superconductor EuRbFe4As4; magnetic order was suppressed, but Tc is almost unchanged with substitution.	Eu0.25Ca0.75RbFe4As4	Eu0.25Ca0.75Rb1Fe4As4	Eu	0.25	Ca	0.75	Rb	1	Fe	4	As	4														1	2018																											2		P4/mmm		A	3.8812		13.1805												K				35.94			35.94	159051fig1	1																																159051fig2																		159051fig3																																										Eu, Rb, Fe, As	22	Polycrystalline samples of Eu1-xCaxRbFe4As4 (x=0.0, 0.25, 0.50, 0.75, 1.0) was synthsized bya conventional sokid state reaction using stainless steel pipe capped with quartz tube.					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type structure	7	(Eu1-xCax)RbFe4As4, superconductor, magnetic order, single crystal	IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J. of Physics, Conf. Series 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y. Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo	EuRbFe4As4	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.
159055	JPC969012027	Ca substitution effect in Fe-based superconductor EuRbFe4As4; magnetic order was suppressed, but Tc is almost unchanged with substitution.	CaRbFe4As4	Ca1Rb1Fe1As4	Ca	1	Rb	1	Fe	1	As	4																1	2018																											2		P4/mmm		A	3.8774		13.1105												K				35.24			35.24	159051fig1	1																																159051fig2																		159051fig3																																										Eu, Rb, Fe, As	22	Polycrystalline samples of Eu1-xCaxRbFe4As4 (x=0.0, 0.25, 0.50, 0.75, 1.0) was synthsized bya conventional sokid state reaction using stainless steel pipe capped with quartz tube.					Superconducting state in (Eu1-xCax)RbFe4As4 with 1144-type structure	7	(Eu1-xCax)RbFe4As4, superconductor, magnetic order, single crystal	IMRA Material R&D Co., Ltd., Kariya, Aichi 448-0032, Japan	J. of Physics, Conf. Series 969(2018)012027	K. Kawashima,S. Ishida,K. Oka,H. Kito,N. Takeshita,H. Fujihisa,Y. Gotoh,K. Kihou,H. Eisaki,Y. Yoshida,A. Iyo	EuRbFe4As4	In Fe-based superconductor EuRbFe4As4; re-entrant magnetic order was observed below 15.1K.
159056	NAT586000424	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor NbSe2, 2D topological superconductivity was observed.	CrBr3	Cr1Br3	Cr	1	Br	3																				5	2020					muB	6																									A	6.37													3.455A layer-layer distance from the top Se atoms to botom Br atoms.																																																												159056fig1																																										Cr, Br	21	Anhydroous CrBr3 powderof99% purity was evaporated from a Knudsen cell on the cleaved NbSe2 substrate at 350 C( optimal subatrate temperaturre for monolayer growth is 270 C).		NbSe2	CrBr3		Topological superconductivity in a van der Waals heterostructure	12	topolofical superconductivity, NbSe2, CrBr3, STM	Department of Applied Physics, Aalto University, Espoo, Finland	Nature, 586(2020)424	S. Kezilebieke,Md N. Huda,V. Vano,M. Aspro,S. C. Ganguli,O. J. Silveira,S. Gtodzik,A. S. Foster,T. Ojanen,P. Liljeroth	CrBr3	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor, 2D topological superconductivity was observed.
159057	NAT586000424	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor NbSe2, 2D topological superconductivity was observed.	CrNb	Cr1Nb1	Cr	1	Nb	1																				5	2020																															A	6.775													3.275A layer-layer distance from the top Se atoms to botom Br atoms.																																																																																																						Cr, Br	21	Anhydroous CrBr3 powderof99% purity was evaporated from a Knudsen cell on the cleaved NbSe2 substrate at 350 C( optimal subatrate temperaturre for monolayer growth is 270 C).		NbSe2	CrBr3		Topological superconductivity in a van der Waals heterostructure	12	topolofical superconductivity, NbSe2, CrBr3, STM	Department of Applied Physics, Aalto University, Espoo, Finland	Nature, 586(2020)424	S. Kezilebieke,Md N. Huda,V. Vano,M. Aspro,S. C. Ganguli,O. J. Silveira,S. Gtodzik,A. S. Foster,T. Ojanen,P. Liljeroth	CrBr3	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor, 2D topological superconductivity was observed.
159058	NAT586000424	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor NbSe2, 2D topological superconductivity was observed.	CrNbSe	Cr1Nb1Se1	Cr	1	Nb	1	Se	1																		5	2020																															A	6.78													3.255A layer-layer distance from the top Se atoms to botom Br atoms.																																																																																																						Cr, Br	21	Anhydroous CrBr3 powderof99% purity was evaporated from a Knudsen cell on the cleaved NbSe2 substrate at 350 C( optimal subatrate temperaturre for monolayer growth is 270 C).		NbSe2	CrBr3		Topological superconductivity in a van der Waals heterostructure	12	topolofical superconductivity, NbSe2, CrBr3, STM	Department of Applied Physics, Aalto University, Espoo, Finland	Nature, 586(2020)424	S. Kezilebieke,Md N. Huda,V. Vano,M. Aspro,S. C. Ganguli,O. J. Silveira,S. Gtodzik,A. S. Foster,T. Ojanen,P. Liljeroth	CrBr3	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor, 2D topological superconductivity was observed.
159059	NAT586000424	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor NbSe2, 2D topological superconductivity was observed.	CrSe	Cr1Se1	Cr	1	Se	1																				5	2020					muB	6.097																									A	6.774													3.501A layer-layer distance from the top Se atoms to botom Br atoms.																																																																																																						Cr, Br	21	Anhydroous CrBr3 powderof99% purity was evaporated from a Knudsen cell on the cleaved NbSe2 substrate at 350 C( optimal subatrate temperaturre for monolayer growth is 270 C).		NbSe2	CrBr3		Topological superconductivity in a van der Waals heterostructure	12	topolofical superconductivity, NbSe2, CrBr3, STM	Department of Applied Physics, Aalto University, Espoo, Finland	Nature, 586(2020)424	S. Kezilebieke,Md N. Huda,V. Vano,M. Aspro,S. C. Ganguli,O. J. Silveira,S. Gtodzik,A. S. Foster,T. Ojanen,P. Liljeroth	CrBr3	Designing van der Waals heterostructure to combine a 2D ferromagnetic CrBr3 with superconductor, 2D topological superconductivity was observed.
159060	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(CTA)0.50SnSe2	Ct0.5Sn1Se2	Ct	0.5	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			14.74											c-axis lattice length is unchanged with the intercalation.	K				7.1	7.46	0.71	7.1	159060fig1	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159061	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(CTA)0.25SnSe2	Ct0.25Sn1Se2	Ct	0.25	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			14.74											c-axis lattice length is unchanged with the intercalation.	K				7.1			7.1	159060fig4	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159062	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(CTA)0.75SnSe2	Ct0.75Sn1Se2	Ct	0.75	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			14.74											c-axis lattice length is unchanged with the intercalation.	K				7.1			7.1	159060fig4	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159063	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(TBA)0.5SnSe2	Tb0.5Sn1Se2	Tb	0.5	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			18.62											c-axis lattice length is unchanged with the intercalation.	K				6.4			6.4	159060fig3	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159064	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(TBA)0.75SnSe2	Tb0.75Sn1Se2	Tb	0.75	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			18.62											c-axis lattice length is unchanged with the intercalation.	K				6.4			6.4	159060fig3	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159065	PRM004124803	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	(TBA)1.0SnSe2	Tb1Sn1Se2	Tb	1	Sn	1	Se	2																		3	2020																											7	CdI2	Pm1		A			18.62											c-axis lattice length is unchanged with the intercalation.	K				6.4			6.4	159060fig3	1																																																		159060fig2																																																	Quasi-two-dimensional superconductivity in SnSe2 via organic ion intercalation	12	SnSe2, intercalation, organic, CTA	Hefei National Laboratory for Physical Sciences at Microscale and Department of Physics, and CAS Key laboratory of Strongly-coupled Quantum Matter Physics, University of Science and Technology of China, Hefei, Anhui 230026, China	Phys. Rev. Materials 4(2020)124803	L.K. Ma,M.Z. Shi,B.L.Kang,K.L. Peng,F.B. Meng,C.S.Zhu,J.H.Cui,Z.L.Sun,D.H.Ma,H.H. Wang,B. Lei,T. Wu,X.H. Chen	(CTA)0.5SnSe2	To explore 2D superconductivity, organic-ion-intercalation can induce a quasi-two-dimensional superconductivity in (CTA)xSnSe2
159066	NAL002200328	A moire pattern between van der Waals superconductor and a monolayer ferromagnet creates aperiodic potetial moduration to realize a topological superconducting state.	CrBr3/NbSe2	Cr1Br3	Cr	1	Br	3																				5	2022																																																																																																			d(Nb)	0.3		1			159066fig1																																										Cr, Br	21	Anhydroous CrBr3 powderof99% purity was evaporated from a Knudsen cell on the cleaved NbSe2 substrate at 350 C( optimal subatrate temperaturre for monolayer growth is 270 C).		NbSe2	CrBr3		Moire-enabled topological superconductivity	1	STM, topological superconductivity, moire pattern, 2D ferromagnet	Department of Applied Physics, Aalto University, 00076 Aalto, Finland	Nano Lett. 22(2022)328	S. Kezilebieke,V. Vano,Md N. Huda,M. Aapro,S. C. Ganguli,P. Liljeroth,J.L. Lado	CrBr3/NbSe2	A moire pattern between van der Waals superconductor and a monolayer ferromagnet creates aperiodic potetial moduration to realize a topological superconducting state.
159067	MAT000302055	BY the systematic investgations of electronic structure on a quasi-1D superconductor TaSe3, non-trivial topological surface states was identified.	TaSe3	Ta1Se3	Ta	1	Se	3																				3	2020																											4		P21/m		A	3.48	3.49	12.18												K						0.5	2	159067fig1	3																																												meV	0.27		1			159067fig2																																																	Observation of topological electronic structure in quasi-1D superconductor TaSe3	12	topological superconductivity, quasi-1D, TaSe3, electronic structure	School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, P.R. China	Matter 3(2020)2055	Ch. Chen,A. Liang,Sh. Liu,S. Nie,J. Huang,M. Wang,Y. Li,D. Pei,H. Yang,H. Zheng,Y. Zhang,D. Lu,M. Hashimoto,A. Barinov,Ch. Jozwick,A. Bostwick,E. Rotenberg,X. Kou,L. Yang,Zh. Wang	TaSe3	BY the systematic investgations of electronic structure on a quasi-1D superconductor TaSe3, non-trivial topological surface states was identified.
159068	NAL002100136	Employing ultrathin PFS-molecular monolayer adlayers, Tc is enhanced about +55% of NbSe2 by generating a macroscopic electrostatic field on NbSe2.	PFS/NbSe2	Pf1Nb1Se2	Pf	1	Nb	1	Se	2																		5	2020																																													Ultrathin monomolecule of PFS was formed on monolayer of NbSe2.	K							1.55	159068fig1	3																																																																																																			Tailoring superconductivity in large-area single-layer NbSe2 via self-assembled molecular adlayers	12	NbSe2, tunable superconductivity, self-assembly, monolayer TMD	CIC nanoGUNE BRTA, Donostia-San Sebastian, Basque Country 20018, Spain	Nano Lett. 21(2020)136	F. Calavalle,P. Drecher,A.P. Surdendran,W. Wan,M. Timpel,R. Verucchi,C. Rogero,T. Bauch,F. Lombardi,F. Casanova,M.V. Nardi,M.M. Ugeda,L.E. Hueso,M. Gobbi	PFS/NbSe2	Employing ultrathin PFS-molecular monolayer adlayers, Tc is enhanced about +55% of NbSe2 by generating a macroscopic electrostatic field on NbSe2.
159069	NAL002100136	Employing ultrathin AHAPS-molecular monolayer adlayers, Tc is decreased about -70% of NbSe2 by generating a macroscopic electrostatic field on NbSe2.	AHAPS/NbSe2	Ah1Nb1Se2	Ah	1	Nb	1	Se	2																		5	2020																																													Ultrathin monomolecule of AHAPS was formed on monolayer of NbSe2.	K							0.29	159069fig1	3																																																																																																			Tailoring superconductivity in large-area single-layer NbSe2 via self-assembled molecular adlayers	12	NbSe2, tunable superconductivity, self-assembly, monolayer TMD	CIC nanoGUNE BRTA, Donostia-San Sebastian, Basque Country 20018, Spain	Nano Lett. 21(2020)136	F. Calavalle,P. Drecher,A.P. Surdendran,W. Wan,M. Timpel,R. Verucchi,C. Rogero,T. Bauch,F. Lombardi,F. Casanova,M.V. Nardi,M.M. Ugeda,L.E. Hueso,M. Gobbi	PFS/NbSe2	Employing ultrathin PFS-molecular monolayer adlayers, Tc is enhanced about +55% of NbSe2 by generating a macroscopic electrostatic field on NbSe2.
159070	NAL002100288	Re-entrance of the dissipationless state in quasi-one-dimensional superconducting Ta2PdS5 nanostrips was observed in magnetic fields, which attributes to thegeometrical effect analyzed with TDGL..	Ta2PdS5	Ta2Pd1S5	Ta	2	Pd	1	S	5																		3	2020																													C2/m																	K							3.2	159070fig1	3																		T		6.5																														159070fig2																																																	Manetic-field-induced re-entrance of superconductivity in Ta2PdS5 nanostrips	12	magnetic field, vortex, re-entrance of superconductivity	State Key Laboratory of Surface Physics and Department of Physics, Fudan University, Shanghai 200433, China	Nano Lett. 21(2020)288	E. Zhang,X. Xu,C. Huang,Y-Ch. Zou,L. Ai,Sh. Liu,P. Leng,Z. Jia,Y. Zhang,M. Zzhao,Z. Li,Y. Yang,J. Liu,S. J. Haigh,Zh. Mao,F. Xiu	Ta2PdS5	Re-entrance of the dissipationless state in quasi-one-dimensional superconducting Ta2PdS5 nanostrips, which attributes to the geometrical effect analyzed with TDGL..
159071	NAL02100583	Vortex mobility and dissipation in the clean-limit atomically thin 2H-NbSe2 were proposed with a qualitatively two-fluid vortex model with a thermal fluctuation	NbSe2	Nb1Se2	Nb	1	Se	2																				5	2020																																														K							5.2	159071fig3	3																																159071fig2		nm	1		2.7													159071fig1																																										Nb, Se	20	Samples for the meas. are prepared by cleaving the single crystals. electrodes are attached					Nonmonotonic temperature-dependent dissipation at nonequilibrium in atomically thin clean-limit superconductors	12	superconductivity, clean limit, two-dimensional, vortex physics, 2H-NbSe2	Department of Mechanical Engineering, Columbia University, New York 10027, United States	Nano Lett. 21(2020)583	A. Benyamini,D.M. Kennes,E.J. Telford,K. Watanabe,T. Taniguchi,A.J. Millis,J. Hone,C.R. Dean,A.N. Pasupathy	2H-NbSe2	Vortex mobility and dissipation in the clean-limit atomically thin 2H-NbSe2 were pooroposed with a qualitatively two-fluid vortex model with a thermal fluctuation.
159072	PRL02800299	The superconducting transition temperature was studied for NbSe2 crystals of afew layers thick. Tc of 3.8K was predicted for a single layer.	NbSe2	Nb1Se2	Nb	1	Se	2																				5	1972																																														K							3.8	159072fig1	3																																159072fig2																					37																																							Nb, Se	20	A few layers of NbSe2 samples were prepared to fix on the substrates of an epoxy, mica, and fused quartz, and to cleaved the single crystal.					Superconductivity in ultrathin NbSe2 layers	12	superconductivity, ultrathin layers, NbSe2	Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada	Phys. Rev. Letters, 28(1972)299	R.F. Frindt	2H-NbSe2	The superconducting transition temperature was studied for NbSe2 crystals of a few layers thick. Tc of 3.8K was predicted for a single layer.
159073	AIP01115007	Interdiffused layer between YBCO/LSMO and the sustrates of STO and LSAT is largely attributed to a modified YBCO layer.	YBa2Cu3O7-d, LSMO	Y1Ba2Cu3La0.67Sr0.33Mn1O3OO7	Y	1	Ba	2	Cu	3	La	0.67	Sr	0.33	Mn	1	O	3							O	O7		5	2021																																														K							80.3	159073fig1	3																		kA/m							240	20						159073fig2																		159073fig3																			ohm							35.9																YBa2CuO7, La0.67Sr0.33MnO3	23	All films were deposited at 750C in 320mTorr O2 at a target/substrate distance of 75mm by a pulsed laser deposition system.		SrTiO3(001), LSAT	YBCO/LSMO		Growth and characterization of La0.67Sr0.33MnO3/YBa2Cu3O7-d bilayers	1	La0.67Sr0.33MnO3, YBa2Cu3O7-d, ferromagnetic	Department of Applied Physics, Stanford University, Stanford, California 94305, USA	AIP Advances, 11(2021)015007	J. J. Wisser,Y. Suzuki	La0.67Sr0.33MnO3/YBa2Cu3O7-d	Interdiffused layer between YBCO/LSMO and the sustrates of STO and LSAT is largely attributed to a modified YBCO layer.
159074	MAD00305375	A new member of the Bi-Pd based compounds is reported with Tc of 4.0(1)K in the moderate coupling limit.	Bi2PdPt	Bi2Pd1Pt1	Bi	2	Pd	1	Pt	1																		3	2022																											7		P63/mmc		A	4.294	4.294	5.567	2											K				3.98			3.98	159074fig1	3									mT	1	2.96							T	1.08													159074fig2																			159074fig3			mJmol-1K-2	5.1		165	Debye model																																		Bi2PdPt	10	The polycrystalline sample was prepared using solid state reaction method, and the single crystal was grown by the modified Bridgeman method.					Superconductivity in Bi based Bi2PdPt	5	Bi2PdPt, Bi-based, topological superconductivity	Department of Physics, Indian Institute of Science Education and Research Bhopal, Bhopal, 462066, India	Mater. Adv., 3(2022)5375	A. Kataria,T. Agarwal,S. Sharma,D. Singh,S. Marik,R.P.Singh	Bi2PdPt	A new member of the Bi-Pd based compounds is reported with Tc of 4.0(1)K in the moderate coupling limit.
159075	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.4F0.6BiS2	La1F0.6Bi1S2O0.4	La	1	F	0.6	Bi	1	S	2													O	0.4		3	2020																											2		P4/nmm																								2.45	159075fig1	4																																																			159079fig1			mJmol-1K-2	1.1		220																																			LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159076	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5BiS2	La1F0.5Bi1S2O0.5	La	1	F	0.5	Bi	1	S	2													O	0.5		3	2020																											2		P4/nmm																	K							2.5	159077fig2	3																																																			159076fig1			mJmol-1K-2	1.5		210																																			LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159077	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.98Sb0.02S2	La1F0.5Bi0.98S2Sb0.02O0.5	La	1	F	0.5	Bi	0.98	S	2	Sb	0.02											O	0.5		3	2020																											2		P4/nmm		A	4.034	4.034	13.384											159077fig1								2.55	159077fig2	3																																																																																												LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159078	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.96Sb0.04S2	La1F0.5Bi0.94S2Sb0.04O0.5	La	1	F	0.5	Bi	0.94	S	2	Sb	0.04											O	0.5		3	2020																											2		P4/nmm		A	4.098	4.098	13.386											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159079	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.84Sb0.06S2	La1F0.5Bi0.9S2Sb0.06O0.5	La	1	F	0.5	Bi	0.9	S	2	Sb	0.06											O	0.5		3	2020																											2		P4/nmm		A	4.022	4.022	13.384											159077fig1								2.19	159077fig2	4																																																			159079fig1																																									LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159080	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.92Sb0.08S2	La1F0.5Bi0.88S2Sb0.08O0.5	La	1	F	0.5	Bi	0.88	S	2	Sb	0.08											O	0.5		3	2020																											2		P4/nmm		A	4.892	4.892	13.385											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159081	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.90Sb0.10S2	La1F0.5Bi0.8S2Sb0.1O0.5	La	1	F	0.5	Bi	0.8	S	2	Sb	0.1											O	0.5		3	2020																											2		P4/nmm		A	4.037	4.037	13.382											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159082	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.88Sb0.12S2	La1F0.5Bi0.72S2Sb0.12O0.6	La	1	F	0.5	Bi	0.72	S	2	Sb	0.12											O	0.6		3	2020																											2		P4/nmm		A	4.025	4.025	13.384											159077fig1								1.71	159077fig2	4																																																			159082fig1																																									LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159083	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.86Sb0.14S2	La1F0.5Bi0.64S2Sb0.14O0.5	La	1	F	0.5	Bi	0.64	S	2	Sb	0.14											O	0.5		3	2020																											2		P4/nmm		A	4.048	4.048	13.384											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159084	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.84Sb0.16S2	La1F0.5Bi0.56S2Sb0.16O0.5	La	1	F	0.5	Bi	0.56	S	2	Sb	0.16											O	0.5		3	2020																											2		P4/nmm		A	4.008	4.008	13.385											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159085	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.82Sb0.18S2	La1F0.5Bi0.48S2Sb0.18O0.5	La	1	F	0.5	Bi	0.48	S	2	Sb	0.18											O	0.5		3	2020																											2		P4/nmm		A	4.021	4.021	13.385											159077fig1																																																																																																						LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159086	JPS089094708	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.	LaO0.5F0.5Bi0.80Sb0.20S2	La1F0.5Bi0.4S2Sb0.2O0.5	La	1	F	0.5	Bi	0.4	S	2	Sb	0.2											O	0.5		3	2020																											2		P4/nmm		A	4.007	4.007	13.386											159077fig1								0	159086fig1	3																																																			159082fig1																																									LaFBiS	5	Single-crystals were fabricated by the CsCl/KCl flux method in vacuum quartz tubes, being heated at 950C for 12 hrs and cooled to 600C at a rate of 1.0C/h.					Impurity effect on superconductivity of LaO1-xFxBi1-ySbyS2 through specic heat measurements	8	LaOFBiSbS, specific heat, superconductivity, impurity effect	Muroran Institute of Technology, Muroran, Hokkaido 050-8585, Japan	J. Phys. Soc. Japan, 89(2020)094708	Y. Wang,S. Takahashi,T. Suda,T. Tamura,H. Ohta,T. Kurosawa,M. Oda,M. Ido,N. Nomono	LaO0.4F0.6BiS2	The effect of Sb substitution on a single crystal of layered superconductor LaO1-xFxBi1-ySbyS2 has been studied by specific heat measurement.
159087	AIP01115011	Coincident of the onset of the magnetic interactions with the superconducting critical temperatureis suggested by the muSR measurements.	FeSr2YCu2O7.57	Fe1Sr2Y1Cu2O7.57	Fe	1	Sr	2	Y	1	Cu	2													O	7.57		1	2021																											2		P4/nmm		A	3.81908	3.81908	11.3446											159087fig3	K							30	159087fig1	1																																																		159087fig2																																																	Coexistence of magnetism and superconductivity in the iron containing FeSr2YCu2O7.57 cuprate as studied by the muSR	1	FeSr2YCu2O7.57, magnetism, superconductivity, muSR	Inorganic Chemistry Department, Universidad Complutense de Madrid, Plaza de Cienas 2, 28040 Madrid, Spain	AIP Advances, 11(2021)015011	S. A. Lopez-Paz,D. P. Sari,A. D. Hiller,M.A. Alario-Franco	FeSr2YCu2O7.57	Coincident of the onset of the magnetic interactions with the superconducting critical temperatureis suggested by the muSR measurements.
159088	NAL02003808	In an atomically ultrathin of TaS2, incorporation of oxygen into TaS2 crystal lattice is energitically favorable and heals sulpher vacancies, enhancing the electron-phonon coupling.	TaS2	Ta1S2	Ta	1	S	2																				5	2020																																													159088fig3	K							2.75	159088fig1	3																		T	3						1.23	0.27						159088fig2																																																																			Enhanced superconductivity in few-layer TaS2 due to healing by oxygenation	4	2D materials, superconductivity, oxygenation	Department of Physics, University of Antwerp, B-2020 Antwerp, Belgium	Nano Lett. 20(2020)3808	J. Bekaert,E. Khestanova,D.G. Hopkinson,J. Birbeck,N. Clerk,M. Zhu,D.A. Bandrin,R. Gorbachev,S. Fairclough,Y. Zou,M. Harmer,D.J. Terry,J.J.P. Peters,A.M. Sanchez,B. Partoens,S.J. Haigh,M.V. Milosevic,I. Grigorieva	TaS2	In an atomically ultrathin of TaS2, incorporation of oxygen into TaS2 crystal lattice is energitically favorable and heals sulpher vacancies, enhancing the electron-phonon coupling.
159089	MAT00302055	By an angle-resolved photoemission spectropy, the electronic structure of a quasi-1D superconductor TaSe3 was systematically investigated to identify the non-trivial topological surface states.	TaSe3	Ta1Se3	Ta	1	Se	3																				3	2020																											4		P21/m																								2	159089fig1	3																																												meV	0.27		5																																																				Observation of topological electronic structure in quasi-1D superconductor TaSe3	12	topological superconductivity, quasi-1D materials, Majorana mode	School of Physical Science and Technology, Shanghai Tech University, Shanghai 201210, R.P. China	Matter, 3(2020)2055	C. Chen,A. Liang,S. Liu,S. Nie,J. Huang,M. Wang,Y. Li,D. Pei,H. Yang,H. Zheng,Y. Zhang,D. Lu,M. Hashimoto,A. Barinov,C. Jpzwiak,A. Bostwick,E. Rotenberg,X. Kou,L. Yang,Y. Chen	TaSe3	By an angle-resolved photoemission spectropy, the electronic structure of a quasi-1D superconductor TaSe3 was systematically investigated to identify the non-trivial topological surface states.
159090	AFM0312007960	New superconductor NbIr2B2 shows Tc of 7.2K with unconventional superconductivity (exceeding the Pauli limit) in magnetic fields.	NbIr2B2	Nb1Ir2B2	Nb	1	Ir	2	B	2																		11	2020																											4		P31		A	8.1586	4.7746	6.0067																			7.2	159090fig1	1									mT	1	6.5							T	3	16.3												159090fig2		A	3	45			A		2230									159090fig3	159090fig4			mJmol-1K-2	4.9		274						159090fig4																																				NbIr2B2 and TaIr2B2 - New low symmetry noncentrosymmetric superconductors with strong spin-orbit coupling	6	crystal structure, noncentrosymmetric superconductors, spin-orbit coupling	Faculty of Applied Physics and Mathematics, Gdansk Universuty of Technology, ul. Narutowiczka 11/12, Gdansk 80-233, Poland	Advance Functional Materials, 31(2020)2007960	K. Gornicka,X. Gui,B. Wiendlocha,L. T. Nguyen,W. Xie,R.J. Cava,T. Klimczuk	NbIr2B2	New superconductor NbIr2B2 shows Tc of 7.2K with unconventional superconductivity (exceeding the Pauli limit) in magnetic fields.
159091	AFM0312007960	New superconductor TaIr2B22 shows Tc of 5.11K with unconventional superconductivity (exceeding the Pauli limit) in magnetic fields.	TaIr2B2	Ta1Ir2B2	Ta	1	Ir	2	B	2																		11	2020																											4		P31																								5.1	159091fig1	1									mT	1	2.71							T	3	14.7												159094fig2		A	3	47			A		3420									159091fig3	159091fig4			mJmol-1K-2	5.2		230						159091fig4																																				NbIr2B2 and TaIr2B2 - New low symmetry noncentrosymmetric superconductors with strong spin-orbit coupling	6	crystal structure, noncentrosymmetric superconductors, spin-orbit coupling	Faculty of Applied Physics and Mathematics, Gdansk Universuty of Technology, ul. Narutowiczka 11/12, Gdansk 80-233, Poland	Advance Functional Materials, 31(2020)2007960	K. Gornicka,X. Gui,B. Wiendlocha,L. T. Nguyen,W. Xie,R.J. Cava,T. Klimczuk	NbIr2B2	New superconductor NbIr2B2 shows Tc of 7.2K with unconventional superconductivity (exceeding the Pauli limit) in magnetic fields.
159092	NAT0615000244	Evidence of superconductivity on a nitrogen-doped lutetium hydride with a maximum Tc of 394K at 10 kBar.	N-doped Lu-hydride	Lu1H	Lu	1	H																					2	2023																													Fm3m		A	5.0289																					294	159092fig1	3																																159092fig2																		159092fig3	159092fig4																																																Evidence of near-ambient superconductivity in a N-doped lutetium hydride	3	N-doped Lu-hydride, ambient superconductivity, high pressure	Department of Physics and Astronomy, University of Rochester, New York 10027, United States	Nature, 244(2023)244	N. Dasenbrock-Gammon,E. Snider,R. McBride,H. Pasan,D. Durkee,N. Khalvashi-Sutter,S. Munasinghe,S. Dissanayake,K. V. Lawler,A. Salamat,R. P. Dias	Na-doped Lu-H	Evidence of superconductivity on a nitrogen-doped lutetium hydride with a maximum Tc of 394K at 10 kBar.